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diff --git a/.hgtags b/.hgtags
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diff --git a/ChangeLog b/ChangeLog
--- a/ChangeLog
+++ b/ChangeLog
@@ -1,6445 +1,6509 @@
+2019-01-29 Andy Buckley <andy.buckley@cern.ch>
+
+ * Add real CMS Run 1 and Run 2 MET resolution smearing functions, based on 8 TeV paper and 13 TeV PAS.
+
2019-01-07 Leif Lönnblad <Leif.Lonnblad@thep.lu.se>
* Reintroduced the PXCONE option in FastJets using a local version
of the Fortran based pxcone algorithm converted to c++ with f2c
and slightly hacked to avoid dependency on Fortran runtime libraries.
* Introduced rivet-merge for statistically correct merging of YODA
files produced by Rivet. Only works on analysis with reentrant
finalize.
* Introduced --dump flag to the rivet script to periodically run
finalize and write out the YODA file for anayses with reentrant
finalize.
* Introduced reentrant finalize. Rivet now produces YODA files
where all analysis objects are stored in two version. One is
prefixed by "/RAW" and gives the state of the object before
finalize was run, and the other is the properly finalized object.
Analyses must be flagged "Reentrant: True" in the .info file to
properly use this feature.
* Added an option system. Analyses can now be added to rivet with
options. Adding eg. "MyAnalysis:Opt1=val1:Opt2=val2" will create
and add a MyAnalysis object making the options available through
the Analysis::getOption() function. Several objects of MyAnalysis
with different options can be added in the same run. Allowed
options must be specified in the MyAnalysis.info file.
* Added several utilities for heavy ions.
+2019-01-03 Andy Buckley <andy.buckley@cern.ch>
+
+ * Add setting of cross-section error in AnalysisHandler and Run.
+
+2018-12-21 Andy Buckley <andy.buckley@cern.ch>
+
+ * Add hasNoTag jet-classification functor, to complement hasBTag and hasCTag.
+
+2018-12-20 Andy Buckley <andy.buckley@cern.ch>
+
+ * Rework VetoedFinalState to be based on Cuts, and to be constructible from Cut arguments.
+
+ * Pre-emptively exclude all hadrons and partons from returning true in isDirect computations.
+
+ * Cache the results of isDirect calculations on Particle (a bit awkwardly... roll on C++17).
+
+ * Add a default-FinalState version of the DressedLeptons constructor.
+
+2018-12-19 Andy Buckley <andy.buckley@cern.ch>
+
+ * Add a FIRST/LAST enum switch for PartonicTops, to choose which top quark clone to use.
+
+2018-12-14 Andy Buckley <andy.buckley@cern.ch>
+
+ * Add a FastJet clustering mode for DressedLeptons.
+
+2018-12-10 Andy Buckley <andy.buckley@cern.ch>
+
+ * Release 2.6.2
+
+ * Info file bugfixes for LHCF_2016_I1385877, from Eugenio Berti.
+
+ * Update references in three CMS analysis .info files.
+
+2018-12-05 Andy Buckley <andy.buckley@cern.ch>
+
+ * Rework doc directory no-build by default to be compatible with 'make dist' packaging.
+
+ * Add fjcontrib RecursiveTools to Rivet/Tools/fjcontrib set.
+
+2018-11-21 Andy Buckley <andy.buckley@cern.ch>
+
+ * Add CMS_2018_I1653948, CMS_2018_I1653948, CMS_2018_I1682495, and CMS_2018_I1690148 analyses.
+
+ * Add FastJet EnergyCorrelator and rejig the internal fjcontrib bundle a little.
+
+2018-11-15 Andy Buckley <andy.buckley@cern.ch>
+
+ * Merge ATLAS_2017_I1517194_MU and ATLAS_2018_I1656578.
+
+ * Add signed calculation optional bool argument on all deltaPhi functions.
+
+2018-11-12 Andy Buckley <andy.buckley@cern.ch>
+
+ * Fix CMS_2012_I1102908 efficiency calculation. Thanks to Anton Karneyeu!
+
+2018-11-09 Andy Buckley <andy.buckley@cern.ch>
+
+ * Remove doc dir from default top-level make
+
2018-09-20 Andy Buckley <andy.buckley@cern.ch>
* Use updated ATLAS R2 muon efficiencies.
* Use proper ATLAS photon efficiency functions for Runs 1 and 2, from arXiv:1606.01813 and ATL-PHYS-PUB-2016-014.
2018-08-31 Andy Buckley <andy.buckley@cern.ch>
* Update embedded yaml-cpp to v0.6.0.
2018-08-29 Andy Buckley <andy.buckley@cern.ch>
* Add RIVET_WEIGHT_INDEX=-1 -> ignore event weights behaviour. Slow, but sometimes useful for debug.
2018-08-29 Christian Gutschow <chris.g@cern.ch>
* Allow reference data file name to be different from plugin name
via setRefDataName(fname) method, aiming to unify HepData records.
2018-08-14 Andy Buckley <andy.buckley@cern.ch>
* Version 2.6.1 release.
2018-08-08 Andy Buckley <andy.buckley@cern.ch>
* Add a RIVET_RANDOM_SEED variable to fix the smearing random-seed engine for validation comparisons.
2018-07-19 Andy Buckley <andy.buckley@cern.ch>
* Merge in ATLAS_2017_I1604029 (ttbar+gamma), ATLAS_2017_I1626105
(dileptonic ttbar), ATLAS_2017_I1644367 (triphotons), and
ATLAS_2017_I1645627 (photon + jets).
* Postpone Particles enhancement now, since the required C++11 isn't supported on lxplus7 = CentOS7.
* Add MC_DILEPTON analysis.
2018-07-10 Andy Buckley <andy.buckley@cern.ch>
* Fix HepData tarball download handling: StringIO is *not* safe anymore
2018-07-08 Andy Buckley <andy.buckley@cern.ch>
* Add LorentzTransform factory functions direct from FourMomentum, and operator()s
2018-06-20 Andy Buckley <andy.buckley@cern.ch>
* Add FinalState(fs, cut) augmenting constructor, and PrevFS projection machinery. Validated for a abscharge > 0 cut.
* Add hasProjection() methods to ProjectionHandler and ProjectionApplier.
* Clone MC_GENERIC as MC_FSPARTICLES and deprecate the badly-named original.
* Fix Spires -> Inspire ID for CMS_2017_I1518399.
2018-06-04 Andy Buckley <andy.buckley@cern.ch>
* Fix installation of (In)DirectFinalState.hh
2018-05-31 Andy Buckley <andy.buckley@cern.ch>
* Add init-time setting of a single weight-vector index from the
RIVET_WEIGHT_INDEX environment variable. To be removed in v3, but
really we should have done this years ago... and we don't know how
long the handover will be.
2018-05-22 Neil Warrack <neil.warrack@cern.ch>
* Include 'unphysical' photon parents in PartonicTops' veto of prompt leptons from photon conversions.
2018-05-20 Andy Buckley <andy.buckley@cern.ch>
* Make Particles and Jets into actual specialisations of
std::vector rather than typedefs, and update surrounding classes
to use them. The specialisations can implicitly cast to vectors of
FourMomentum (and maybe Pseudojet).
2018-05-18 Andy Buckley <andy.buckley@cern.ch>
* Make CmpAnaHandle::operator() const, for GCC 8 (thanks to CMS)
2018-05-07 Andy Buckley <andy.buckley@cern.ch>
* CMS_2016_I1421646.cc: Add patch from CMS to veto if leading jets
outside |y| < 2.5, rather than only considering jets in that
acceptance. Thanks to CMS and Markus Seidel.
2018-04-27 Andy Buckley <andy.buckley@cern.ch>
* Tidy keywords and luminosity entries, and add both to BSM search .info files.
* Add Luminosity_fb and Keywords placeholders in mkanalysis output.
2018-04-26 Andy Buckley <andy.buckley@cern.ch>
* Add pairMass and pairPt functions.
* Add (i)discardIfAnyDeltaRLess and (i)discardIfAnyDeltaPhiLess functions.
* Add normalize() methods to Cutflow and Cutflows.
* Add DirectFinalState and IndirectFinalState alias headers, for forward compatibility. 'Prompt' is confusing.
2018-04-24 Andy Buckley <andy.buckley@cern.ch>
* Add initializer_list overload for binIndex. Needed for other util functions operating on vectors.
* Fix function signature bug is isMT2 overload.
* Add isSameSign, isOppSign, isSameFlav, isOppFlav, and isOSSF etc. functions on PIDs and Particles.
2018-03-27 Andy Buckley <andy.buckley@cern.ch>
* Add RatioPlotLogY key to make-plots. Thanks to Antonin Maire.
2018-02-22 Andy Buckley <andy.buckley@cern.ch>
* Adding boolean operator syntactic sugar for composition of bool functors.
* Copy & paste error fixes in implementation of BoolJetAND,OR,NOT.
2018-02-01 Andy Buckley <andy.buckley@cern.ch>
* Make the project() and compare() methods of projections public.
* Fix a serious bug in the SmearedParticles and SmearedJets compare methods.
* Add string representations and streamability to the Cut objects, for debugging.
2018-01-08 Andy Buckley <andy.buckley@cern.ch>
* Add highlighted source to HTML analysis metadata listings.
2017-12-21 Andy Buckley <andy.buckley@cern.ch>
* Version 2.6.0 release.
2017-12-20 Andy Buckley <andy.buckley@cern.ch>
* Typo fix in TOTEM_2012_I1220862 data -- thanks to Anton Karneyeu.
2017-12-19 Andy Buckley <andy.buckley@cern.ch>
* Adding contributed analyses: 1 ALICE, 6 ATLAS, 1 CMS.
* Fix bugged PID codes in MC_PRINTEVENT.
2017-12-13 Andy Buckley <andy.buckley@cern.ch>
* Protect Run methods and rivet script against being told to run from a missing or unreadable file.
2017-12-11 Andy Buckley <andy.buckley@cern.ch>
* Replace manual event count & weight handling with a YODA Counter object.
2017-11-28 Andy Buckley <andy.buckley@cern.ch>
* Providing neater & more YODA-consistent sumW and sumW2 methods on AnalysisHandler and Analysis.
* Fix to Python version check for >= 2.7.10 (patch submitted to GNU)
2017-11-17 Andy Buckley <andy.buckley@cern.ch>
* Various improvements to DISKinematics, DISLepton, and the ZEUS 2001 analysis.
2017-11-06 Andy Buckley <andy.buckley@cern.ch>
* Extend AOPath regex to allow dots and underscores in weight names.
2017-10-27 Andy Buckley <andy.buckley@cern.ch>
* Add energy to the list of cuts (both as Cuts::E and Cuts::energy)
* Add missing pT (rather than Et) functions to SmearedMET,
although they are just copies of the MET functions for now.
2017-10-09 Andy Buckley <andy.buckley@cern.ch>
* Embed zstr and enable transparent reading of gzipped HepMC streams.
2017-10-03 Andy Buckley <andy.buckley@cern.ch>
* Use Lester MT2 bisection header, and expose a few more mT2 function signatures.
2017-09-26 Andy Buckley <andy.buckley@cern.ch>
* Use generic YODA read and write functions -- enables zipped yoda.gz output.
* Add ChargedLeptons enum and mode argument to ZFinder and WFinder
constructors, to allow control over whether the selected charged
leptons are prompt. This is mostly cosmetic/for symmetry in the
case of ZFinder, since the same can be achieved by passing a
PromptFinalState as the fs argument, but for WFinder it's
essential since passing a prompt final state screws up the MET
calculation. Both are slightly different in the treatment of the
lepton dressing, although conventionally this is an area where
only prompt photons are used.
2017-09-25 Andy Buckley <andy.buckley@cern.ch>
* Add deltaR2 functions for squared distances.
2017-09-10 Andy Buckley <andy.buckley@cern.ch>
* Add white backgrounds to make-plots main and ratio plot frames.
2017-09-05 Andy Buckley <andy.buckley@cern.ch>
* Add CMS_2016_PAS_TOP_15_006 jet multiplicity in lepton+jets ttbar at 8 TeV analysis.
* Add CMS_2017_I1467451 Higgs -> WW -> emu + MET in 8 TeV pp analysis.
* Add ATLAS_2017_I1609448 Z->ll + pTmiss analysis.
* Add vectorMissingEt/Pt and vectorMET/MPT convenience methods to MissingMomentum.
* Add ATLAS_2017_I1598613 J/psi + mu analysis.
* Add CMS SUSY 0-lepton search CMS_2017_I1594909 (unofficial implementation, validated vs. published cutflows)
2017-09-04 Andy Buckley <andy.buckley@cern.ch>
* Change license explicitly to GPLv3, cf. MCnet3 agreement.
* Add a better jet smearing resolution parametrisation, based on GAMBIT code from Matthias Danninger.
2017-08-16 Andy Buckley <andy.buckley@cern.ch>
* Protect make-plots against NaNs in error band values (patch from Dmitry Kalinkin).
2017-07-20 Andy Buckley <andy.buckley@cern.ch>
* Add sumPt, sumP4, sumP3 utility functions.
* Record truth particles as constituents of SmearedParticles output.
* Rename UnstableFinalState -> UnstableParticles, and convert
ZFinder to be a general ParticleFinder rather than FinalState.
2017-07-19 Andy Buckley <andy.buckley@cern.ch>
* Add implicit cast from FourVector & FourMomentum to Vector3, and tweak mT implementation.
* Add rawParticles() to ParticleFinder, and update DressedLeptons, WFinder, ZFinder and VetoedFinalState to cope.
* Add isCharged() and isChargedLepton() to Particle.
* Add constituents() and rawConstituents() to Particle.
* Add support for specifying bin edges as braced initializer lists rather than explicit vector<double>.
2017-07-18 Andy Buckley <andy.buckley@cern.ch>
* Enable methods for booking of Histo2D and Profile2D from Scatter3D reference data.
* Remove IsRef annotation from autobooked histogram objects.
2017-07-17 Andy Buckley <andy.buckley@cern.ch>
* Add pair-smearing to SmearedJets.
2017-07-08 Andy Buckley <andy.buckley@cern.ch>
* Add Event::centrality(), for non-HepMC access to the generator
value if one has been recorded -- otherwise -1.
2017-06-28 Andy Buckley <andy.buckley@cern.ch>
* Split the smearing functions into separate header files for
generic/momentum, Particle, Jet, and experiment-specific smearings
& efficiencies.
2017-06-27 Andy Buckley <andy.buckley@cern.ch>
* Add 'JetFinder' alias for JetAlg, by analogy with ParticleFinder.
2017-06-26 Andy Buckley <andy.buckley@cern.ch>
* Convert SmearedParticles to a more general list of combined
efficiency+smearing functions, with extra constructors and some
variadic template cleverness to allow implicit conversions from
single-operation eff and smearing function. Yay for C++11 ;-)
This work based on a macro-based version of combined eff/smear
functions by Karl Nordstrom -- thanks!
* Add *EffFn, *SmearFn, and *EffSmearFn types to SmearingFunctions.hh.
2017-06-23 Andy Buckley <andy.buckley@cern.ch>
* Add portable OpenMP enabling flags to AM_CXXFLAGS.
2017-06-22 Andy Buckley <andy.buckley@cern.ch>
* Fix the smearing random number seed and make it thread-specific
if OpenMP is available (not yet in the build system).
* Remove the UNUSED macro and find an alternative solution for the
cases where it was used, since there was a risk of macro clashes
with embedding codes.
* Add a -o output directory option to make-plots.
* Vector4.hh: Add mT2(vec,vec) functions.
2017-06-21 Andy Buckley <andy.buckley@cern.ch>
* Add a full set of in-range kinematics functors: ptInRange,
(abs)etaInRange, (abs)phiInRange, deltaRInRange, deltaPhiInRange,
deltaEtaInRange, deltaRapInRange.
* Add a convenience JET_BTAG_EFFS functor with several constructors to handle mistag rates.
* Add const efficiency functors operating on Particle, Jet, and FourMomentum.
* Add const-efficiency constructor variants for SmearedParticles.
2017-06-21 Jon Butterworth <jmb@hep.ucl.ac.uk>
* Fix normalisations in CMS_2016_I1454211.
* Fix analysis name in ref histo paths for ATLAS_2017_I1591327.
2017-06-18 Andy Buckley <andy.buckley@cern.ch>
* Move all standard plugin files into subdirs of src/Analyses,
with some custom make rules driving rivet-buildplugin.
2017-06-18 David Grellscheid <david.grellscheid@durham.ac.uk>
* Parallelise rivet-buildplugin, with source-file cat'ing and use
of a temporary Makefile.
2016-06-18 Holger Schulz <holger.schulz@durham.ac.uk>
* Version 2.5.4 release!
2016-06-17 Holger Schulz <holger.schulz@durham.ac.uk>
* Fix 8 TeV DY (ATLAS_2016_I1467454), EL/MU bits were bissing.
* Add 13 TeV DY (ATLAS_2017_I1514251) and mark
ATLAS_2015_CONF_2015_041 obsolete
* Add missing install statement for ATLAS_2016_I1448301.yoda/plot/info leading to
segfault
2017-06-09 Andy Buckley <andy.buckley@cern.ch>
* Slight improvements to Particle constructors.
* Improvement to Beam projection: before falling back to barcodes
1 & 2, try a manual search for status=4 particles. Based on a
patch from Andrii Verbytskyi.
2017-06-05 Andy Buckley <andy.buckley@cern.ch>
* Add CMS_2016_I1430892: dilepton channel ttbar charge asymmetry analysis.
* Add CMS_2016_I1413748: dilepton channel ttbar spin correlations and polarisation analysis.
* Add CMS_2017_I1518399: leading jet mass for boosted top quarks at 8 TeV.
* Add convenience constructors for ChargedLeptons projection.
2017-06-03 Andy Buckley <andy.buckley@cern.ch>
* Add FinalState and Cut (optional) constructor arguments and
usage to DISFinalState. Thanks to Andrii Verbytskyi for the idea
and initial patch.
2017-05-23 Andy Buckley <andy.buckley@cern.ch>
* Add ATLAS_2016_I1448301, Z/gamma cross section measurement at 8 TeV.
* Add ATLAS_2016_I1426515, WW production at 8 TeV.
2016-05-19 Holger Schulz <holger.schulz@durham.ac.uk>
* Add BELLE measurement of semileptonic B0bar -> D*+ ell nu decays. I
took the liberty to correct the data in the sense that I take the bin
widhts into account in the normalisation. BELLE_2017_I1512299.
This is a nice analysis as it probes the hadronic and the leptonic
side of the decay so very valuable for model building and of course it
is rare as it is an unfolded B measurement.
2016-05-17 Holger Schulz <holger.schulz@durham.ac.uk>
* Add ALEPH measurement of hadronic tau decays, ALEPH_2014_I1267648.
* Add ALEPH dimuon invariant mass (OS and SS) analysis, ALEPH_2016_I1492968
* The latter needed GENKTEE FastJet algorithm so I added that FastJets
* Protection against logspace exception in histobooking of
MC_JetAnalysis
* Fix compiler complaints about uninitialised variable in OPAL_2004.
2016-05-16 Holger Schulz <holger.schulz@durham.ac.uk>
* Tidy ALEPH_1999 charm fragmentation analysis and normalise to data
integral. Added DSTARPLUS and DSTARMINUS to PID.
2017-05-16 Andy Buckley <andy.buckley@cern.ch>
* Add ATLAS_2016_CONF_2016_092, inclusive jet cross sections using early 13 TeV data.
* Add ATLAS_2017_I1591327, isolated diphoton + X differential cross-sections.
* Add ATLAS_2017_I1589844, ATLAS_2017_I1589844_EL, ATLAS_2017_I1589844_MU: kT splittings in Z events at 8 TeV.
* Add ATLAS_2017_I1509919, track-based underlying event at 13 TeV in ATLAS.
* Add ATLAS_2016_I1492320_2l2j and ATLAS_2016_I1492320_3l, the WWW cross-section at 8 TeV.
2017-05-12 Andy Buckley <andy.buckley@cern.ch>
* Add ATLAS_2016_I1449082, charge asymmetry in top quark pair production in dilepton channel.
* Add ATLAS_2015_I1394865, inclusive 4-lepton/ZZ lineshape.
2017-05-11 Andy Buckley <andy.buckley@cern.ch>
* Add ATLAS_2013_I1234228, high-mass Drell-Yan at 7 TeV.
2017-05-10 Andy Buckley <andy.buckley@cern.ch>
* Add CMS_2017_I1519995, search for new physics with dijet angular distributions in proton-proton collisions at sqrt{(s) = 13 TeV.
* Add CMS_2017_I1511284, inclusive energy spectrum in the very forward direction in proton-proton collisions at 13 TeV.
* Add CMS_2016_I1486238, studies of 2 b-jet + 2 jet production in proton-proton collisions at 7 TeV.
* Add CMS_2016_I1454211, boosted ttbar in pp collisions at sqrtS = 8 TeV.
* Add CMS_2016_I1421646, CMS azimuthal decorrelations at 8 TeV.
2017-05-09 Andy Buckley <andy.buckley@cern.ch>
* Add CMS_2015_I1380605, per-event yield of the highest transverse
momentum charged particle and charged-particle jet.
* Add CMS_2015_I1370682_PARTON, a partonic-top version of the CMS
7 TeV pseudotop ttbar differential cross-section analysis.
* Adding EHS_1988_I265504 from Felix Riehn: charged-particle
production in K+ p, pi+ p and pp interactions at 250 GeV/c.
* Fix ALICE_2012_I1116147 for pi0 and Lambda feed-down.
2017-05-08 Andy Buckley <andy.buckley@cern.ch>
* Add protection against leptons from QED FSR photon conversions
in assigning PartonicTop decay modes. Thanks to Markus Seidel for
the report and suggested fix.
* Reimplement FastJets methods in terms of new static helper functions.
* Add new mkClusterInputs, mkJet and mkJets static methods to
FastJets, to help with direct calls to FastJet where particle
lookup for constituents and ghost tags are required.
* Fix Doxygen config and Makefile target to allow working with
out-of-source builds. Thanks to Christian Holm Christensen.
* Improve DISLepton for HERA analyses: thanks to Andrii Verbytskyi for the patch!
2017-03-30 Andy Buckley <andy.buckley@cern.ch>
* Replace non-template Analysis::refData functions with C++11 default T=Scatter2D.
2017-03-29 Andy Buckley <andy.buckley@cern.ch>
* Allow yes/no and true/false values for LogX, etc. plot options.
* Add --errs as an alias for --mc-errs to rivet-mkhtml and rivet-cmphistos.
2017-03-08 Peter Richardson <peter.richardson@durham.ac.uk>
* Added 6 analyses AMY_1990_I295160, HRS_1986_I18502, JADE_1983_I190818,
PLUTO_1980_I154270, TASSO_1989_I277658, TPC_1987_I235694 for charged multiplicity
in e+e- at CMS energies below the Z pole
* Added 2 analyses for charged multiplicity at the Z pole DELPHI_1991_I301657,
OPAL_1992_I321190
* Updated ALEPH_1991_S2435284 to plot the average charged multiplcity
* Added analyses OPAL_2004_I631361, OPAL_2004_I631361_qq, OPAL_2004_I648738 for
gluon jets in e+e-, most need fictitious e+e- > g g process
2017-03-29 Andy Buckley <andy.buckley@cern.ch>
* Add Cut and functor selection args to HeavyHadrons accessor methods.
2017-03-03 Andy Buckley <andy.buckley@cern.ch>
* bin/rivet-mkanalysis: Add FastJets.hh include by default -- it's almost always used.
2017-03-02 Andy Buckley <andy.buckley@cern.ch>
* src/Analyses/CMS_2016_I1473674.cc: Patch from CMS to use partonic tops.
* src/Analyses/CMS_2015_I1370682.cc: Patch to inline jet finding from CMS.
2017-03-01 Andy Buckley <andy.buckley@cern.ch>
* Convert DressedLeptons use of fromDecay to instead veto photons
that match fromHadron() || fromHadronicTau() -- meaning that
electrons and muons from leptonic taus will now be dressed.
* Move Particle and Jet std::function aliases to .fhh files, and
replace many uses of templates for functor arguments with
ParticleSelector meta-types instead.
* Move the canonical implementations of hasAncestorWith, etc. and
isLastWith, etc. from ParticleUtils.hh into Particle.
* Disable the event-to-event beam consistency check if the
ignore-beams mode is active.
2017-02-27 Andy Buckley <andy.buckley@cern.ch>
* Add BoolParticleAND, BoolJetOR, etc. functor combiners to
Tools/ParticleUtils.hh and Tools/JetUtils.hh.
2017-02-24 Andy Buckley <andy.buckley@cern.ch>
* Mark ATLAS_2016_CONF_2016_078 and CMS_2016_PAS_SUS_16_14
analyses as validated, since their cutflows match the documentation.
2017-02-22 Andy Buckley <andy.buckley@cern.ch>
* Add aggregate signal regions to CMS_2016_PAS_SUS_16_14.
2017-02-18 Andy Buckley <andy.buckley@cern.ch>
* Add getEnvParam function, for neater use of environment variable
parameters with a required default.
2017-02-05 Andy Buckley <andy.buckley@cern.ch>
* Add HasBTag and HasCTag jet functors, with lower-case aliases.
2017-01-18 Andy Buckley <andy.buckley@cern.ch>
* Use std::function in functor-expanded method signatures on JetAlg.
2017-01-16 Andy Buckley <andy.buckley@cern.ch>
* Convert FinalState particles() accessors to use std::function
rather than a template arg for sorting, and add filtering functor
support -- including a mix of filtering and sorting functors. Yay
for C++11!
* Add ParticleEffFilter and JetEffFilter constructors from a double (encoding constant efficiency).
* Add Vector3::abseta()
2016-12-13 Andy Buckley <andy.buckley@cern.ch>
* Version 2.5.3 release.
2016-12-12 Holger Schulz <holger.schulz@cern.ch>
* Add cut in BZ calculation in OPAL 4 jet analysis. Paper is not clear
about treatment of parallel vectors, leads to division by zero and
nan-fill and subsequent YODA RangeError (OPAL_2001_S4553896)
2016-12-12 Andy Buckley <andy.buckley@cern.ch>
* Fix bugs in SmearedJets treatment of b & c tagging rates.
* Adding ATLAS_2016_I1467454 analysis (high-mass Drell-Yan at 8 TeV)
* Tweak to 'convert' call to improve the thumbnail quality from rivet-mkhtml/make-plots.
2016-12-07 Andy Buckley <andy.buckley@cern.ch>
* Require Cython 0.24 or later.
2016-12-02 Andy Buckley <andy.buckley@cern.ch>
* Adding L3_2004_I652683 (LEP 1 & 2 event shapes) and
LHCB_2014_I1262703 (Z+jet at 7 TeV).
* Adding leading dijet mass plots to MC_JetAnalysis (and all
derived classes). Thanks to Chris Gutschow!
* Adding CMS_2012_I1298807 (ZZ cross-section at 8 TeV),
CMS_2016_I1459051 (inclusive jet cross-sections at 13 TeV) and
CMS_PAS_FSQ_12_020 (preliminary 7 TeV leading-track underlying
event).
* Adding CDF_2015_1388868 (ppbar underlying event at 300, 900, and 1960 GeV)
* Adding ATLAS_2016_I1467230 (13 TeV min bias),
ATLAS_2016_I1468167 (13 TeV inelastic pp cross-section), and
ATLAS_2016_I1479760 (7 TeV pp double-parton scattering with 4
jets).
2016-12-01 Andy Buckley <andy.buckley@cern.ch>
* Adding ALICE_2012_I1116147 (eta and pi0 pTs and ratio) and
ATLAS_2011_I929691 (7 TeV jet frag)
2016-11-30 Andy Buckley <andy.buckley@cern.ch>
* Fix bash bugs in rivet-buildplugin, including fixing the --cmd mode.
2016-11-28 Andy Buckley <andy.buckley@cern.ch>
* Add LHC Run 2 BSM analyses ATLAS_2016_CONF_2016_037 (3-lepton
and same-sign 2-lepton), ATLAS_2016_CONF_2016_054 (1-lepton +
jets), ATLAS_2016_CONF_2016_078 (ICHEP jets + MET),
ATLAS_2016_CONF_2016_094 (1-lepton + many jets), CMS_2013_I1223519
(alphaT + b-jets), and CMS_2016_PAS_SUS_16_14 (jets + MET).
* Provide convenience reversed-argument versions of apply and
declare methods, to allow presentational choice of declare syntax
in situations where the projection argument is very long, and
reduce requirements on the user's memory since this is one
situation in Rivet where there is no 'most natural' ordering
choice.
2016-11-24 Andy Buckley <andy.buckley@cern.ch>
* Adding pTvec() function to 4-vectors and ParticleBase.
* Fix --pwd option of the rivet script
2016-11-21 Andy Buckley <andy.buckley@cern.ch>
* Add weights and scaling to Cutflow/s.
2016-11-19 Andy Buckley <andy.buckley@cern.ch>
* Add Et(const ParticleBase&) unbound function.
2016-11-18 Andy Buckley <andy.buckley@cern.ch>
* Fix missing YAML quote mark in rivet-mkanalysis.
2016-11-15 Andy Buckley <andy.buckley@cern.ch>
* Fix constness requirements on ifilter_select() and Particle/JetEffFilter::operator().
* src/Analyses/ATLAS_2016_I1458270.cc: Fix inverted particle efficiency filtering.
2016-10-24 Andy Buckley <andy.buckley@cern.ch>
* Add rough ATLAS and CMS photon reco efficiency functions from
Delphes (ATLAS and CMS versions are identical, hmmm)
2016-10-12 Andy Buckley <andy.buckley@cern.ch>
* Tidying/fixing make-plots custom z-ticks code. Thanks to Dmitry Kalinkin.
2016-10-03 Holger Schulz <holger.schulz@cern.ch>
* Fix SpiresID -> InspireID in some analyses (show-analysis pointed to
non-existing web page)
2016-09-29 Holger Schulz <holger.schulz@cern.ch>
* Add Luminosity_fb to AnalysisInfo
* Added some keywords and Lumi to ATLAS_2016_I1458270
2016-09-28 Andy Buckley <andy.buckley@cern.ch>
* Merge the ATLAS and CMS from-Delphes electron and muon tracking
efficiency functions into generic trkeff functions -- this is how
it should be.
* Fix return type typo in Jet::bTagged(FN) templated method.
* Add eta and pT cuts to ATLAS truth b-jet definition.
* Use rounding rather than truncation in Cutflow percentage efficiency printing.
2016-09-28 Frank Siegert <frank.siegert@cern.ch>
* make-plots bugfix in y-axis labels for RatioPlotMode=deviation
2016-09-27 Andy Buckley <andy.buckley@cern.ch>
* Add vector and scalar pT (rather than Et) to MissingMomentum.
2016-09-27 Holger Schulz <holger.schulz@cern.ch>
* Analysis keyword machinery
* rivet -a @semileptonic
* rivet -a @semileptonic@^bdecays -a @semileptonic@^ddecays
2016-09-22 Holger Schulz <holger.schulz@cern.ch>
* Release version 2.5.2
2016-09-21 Andy Buckley <andy.buckley@cern.ch>
* Add a requirement to DressedLeptons that the FinalState passed
as 'bareleptons' will be filtered to only contain charged leptons,
if that is not already the case. Thanks to Markus Seidel for the
suggestion.
2016-09-21 Holger Schulz <holger.schulz@cern.ch>
* Add Simone Amoroso's plugin for hadron spectra (ALEPH_1995_I382179)
* Add Simone Amoroso's plugin for hadron spectra (OPAL_1993_I342766)
2016-09-20 Holger Schulz <holger.schulz@cern.ch>
* Add CMS ttbar analysis from contrib, mark validated (CMS_2016_I1473674)
* Extend rivet-mkhtml --booklet to also work with pdfmerge
2016-09-20 Andy Buckley <andy.buckley@cern.ch>
* Fix make-plots automatic YMax calculation, which had a typo from code cleaning (mea culpa!).
* Fix ChargedLeptons projection, which failed to exclude neutrinos!!! Thanks to Markus Seidel.
* Add templated FN filtering arg versions of the Jet::*Tags() and
Jet::*Tagged() functions.
2016-09-18 Andy Buckley <andy.buckley@cern.ch>
* Add CMS partonic top analysis (CMS_2015_I1397174)
2016-09-18 Holger Schulz <holger.schulz@cern.ch>
* Add L3 xp analysis of eta mesons, thanks Simone (L3_1992_I336180)
* Add D0 1.8 TeV jet shapes analysis, thanks Simone (D0_1995_I398175)
2016-09-17 Andy Buckley <andy.buckley@cern.ch>
* Add has{Ancestor,Parent,Child,Descendant}With functions and
HasParticle{Ancestor,Parent,Child,Descendant}With functors.
2016-09-16 Holger Schulz <holger.schulz@cern.ch>
* Add ATLAS 8TeV ttbar analysis from contrib (ATLAS_2015_I1404878)
2016-09-16 Andy Buckley <andy.buckley@cern.ch>
* Add particles(GenParticlePtr) to RivetHepMC.hh
* Add hasParent, hasParentWith, and hasAncestorWith to Particle.
2016-09-15 Holger Schulz <holger.schulz@cern.ch>
* Add ATLAS 8TeV dijet analysis from contrib (ATLAS_2015_I1393758)
* Add ATLAS 8TeV 'number of tracks in jets' analysis from contrib (ATLAS_2016_I1419070)
* Add ATLAS 8TeV g->H->WW->enumunu analysis from contrib (ATLAS_2016_I1444991)
2016-09-14 Holger Schulz <holger.schulz@cern.ch>
* Explicit std::toupper and std::tolower to make clang happy
2016-09-14 Andy Buckley <andy.buckley@cern.ch>
* Add ATLAS Run 2 0-lepton SUSY and monojet search papers (ATLAS_2016_I1452559, ATLAS_2016_I1458270)
2016-09-13 Andy Buckley <andy.buckley@cern.ch>
* Add experimental Cutflow and Cutflows objects for BSM cut tracking.
* Add 'direct' versions of any, all, none to Utils.hh, with an
implicity bool() transforming function.
2016-09-13 Holger Schulz <holger.schulz@cern.ch>
* Add and mark validated B+ to omega analysis (BABAR_2013_I1116411)
* Add and mark validated D0 to pi- analysis (BABAR_2015_I1334693)
* Add a few more particle names and use PID names in recently added
analyses
* Add Simone's OPAL b-frag analysis (OPAL_2003_I599181) after some
cleanup and heavy usage of new features
* Restructured DELPHI_2011_I890503 in the same manner --- picks up
a few more B-hadrons now (e.g. 20523 and such)
* Clean up and add ATLAS 8TeV MinBias (from contrib ATLAS_2016_I1426695)
2016-09-12 Andy Buckley <andy.buckley@cern.ch>
* Add a static constexpr DBL_NAN to Utils.hh for convenience, and
move some utils stuff out of MathHeader.hh
2016-09-12 Holger Schulz <holger.schulz@cern.ch>
* Add count function to Tools/Utils.h
* Add and mark validated B0bar and Bminus-decay to pi analysis (BELLE_2013_I1238273)
* Add and mark validated B0-decay analysis (BELLE_2011_I878990)
* Add and mark validated B to D decay analysis (BELLE_2011_I878990)
2016-09-08 Andy Buckley <andy.buckley@cern.ch>
* Add C-array version of multi-target Analysis::scale() and normalize(), and fix (semantic) constness.
* Add == and != operators for cuts applied to integers.
* Add missing delta{Phi,Eta,Rap}{Gtr,Less} functors to ParticleBaseUtils.hh
2016-09-07 Andy Buckley <andy.buckley@cern.ch>
* Add templated functor filtering args to the Particle parent/child/descendent methods.
2016-09-06 Andy Buckley <andy.buckley@cern.ch>
* Add ATLAS Run 1 medium and tight electron ID efficiency functions.
* Update configure scripts to use newer (Py3-safe) Python testing macros.
2016-09-02 Andy Buckley <andy.buckley@cern.ch>
* Add isFirstWith(out), isLastWith(out) functions, and functor
wrappers, using Cut and templated function/functor args.
* Add Particle::parent() method.
* Add using import/typedef of HepMC *Ptr types (useful step for HepMC 2.07 and 3.00).
* Various typo fixes (and canonical renaming) in ParticleBaseUtils functor collection.
* Add ATLAS MV2c10 and MV2c20 b-tagging effs to SmearingFunctions.hh collection.
2016-09-01 Andy Buckley <andy.buckley@cern.ch>
* Add a PartonicTops projection.
* Add overloaded versions of the Event::allParticles() method with
selection Cut or templated selection function arguments.
2016-08-25 Andy Buckley <andy.buckley@cern.ch>
* Add rapidity scheme arg to DeltaR functor constructors.
2016-08-23 Andy Buckley <andy.buckley@cern.ch>
* Provide an Analysis::bookCounter(d,x,y, title) function, for
convenience and making the mkanalysis template valid.
* Improve container utils functions, and provide combined
remove_if+erase filter_* functions for both select- and
discard-type selector functions.
2016-08-22 Holger Schulz <holger.schulz@cern.ch>
* Bugfix in rivet-mkhtml (NoneType: ana.spiresID() --> spiresid)
* Added <numeric> include to Rivet/Tools/Utils.h to make gcc6 happy
2016-08-22 Andy Buckley <andy.buckley@cern.ch>
* Add efffilt() functions and Particle/JetEffFilt functors to SmearingFunctions.hh
2016-08-20 Andy Buckley <andy.buckley@cern.ch>
* Adding filterBy methods for Particle and Jet which accept
generic boolean functions as well as the Cut specialisation.
2016-08-18 Andy Buckley <andy.buckley@cern.ch>
* Add a Jet::particles(Cut&) method, for inline filtering of jet constituents.
* Add 'conjugate' behaviours to container head and tail functions
via negative length arg values.
2016-08-15 Andy Buckley <andy.buckley@cern.ch>
* Add convenience headers for including all final-state and
smearing projections, to save user typing.
2016-08-12 Andy Buckley <andy.buckley@cern.ch>
* Add standard MET functions for ATLAS R1 (and currently copies
for R2 and CMS).
* Add lots of vector/container helpers for e.g. container slicing,
summing, and min/max calculation.
* Adapt SmearedMET to take *two* arguments, since SET is typically
used to calculate MET resolution.
* Adding functors for computing vector & ParticleBase differences
w.r.t. another vector.
2016-08-12 Holger Schulz <holger.schulz@cern.ch>
* Implemented a few more cuts in prompt photon analysis
(CDF_1993_S2742446) but to no avail, the rise of the data towards
larger costheta values cannot be reproduced --- maybe this is a
candidate for more scrutiny and using the boosting machinery such that
the c.m. cuts can be done in a non-approximate way
2016-08-11 Holger Schulz <holger.schulz@cern.ch>
* Rename CDF_2009_S8383952 to CDF_2009_I856131 due to invalid Spires
entry.
* Add InspireID to all analysis known by their Spires key
2016-08-09 Holger Schulz <holger.schulz@cern.ch>
* Release 2.5.1
2016-08-08 Andy Buckley <andy.buckley@cern.ch>
* Add a simple MC_MET analysis for out-of-the-box MET distribution testing.
2016-08-08 Holger Schulz <holger.schulz@cern.ch>
* Add DELPHI_2011_I890503 b-quark fragmentation function measurement,
which superseded DELPHI_2002_069_CONF_603. The latter is marked
OBSOLETE.
2016-08-05 Holger Schulz <holger.schulz@cern.ch>
* Use Jet mass and energy smearing in CDF_1997_... six-jet analysis,
mark validated.
* Mark CDF_2001_S4563131 validated
* D0_1996_S3214044 --- cut on jet Et rather than pT, fix filling of
costheta and theta plots, mark validated. Concerning the jet
algorithm, I tried with the implementation of fastjet
fastjet/D0RunIConePlugin.hh but that really does not help.
* D0_1996_S3324664 --- fix normalisations, sorting jets properly now,
cleanup and mark validated.
2016-08-04 Holger Schulz <holger.schulz@cern.ch>
* Use Jet mass and energy smearing in CDF_1996_S310 ... jet properties
analysis. Cleanup analysis and mark validated. Added some more run info.
The same for CDF_1996_S334... (pretty much the same cuts, different
observables).
* Minor fixes in SmearedJets projection
2016-08-03 Andy Buckley <andy.buckley@cern.ch>
* Protect SmearedJets against loss of tagging information if a
momentum smearing function is used (rather than a dedicated Jet
smearing fn) via implicit casts.
2016-08-02 Andy Buckley <andy.buckley@cern.ch>
* Add SmearedMET projection, wrapping MissingMomentum.
* Include base truth-level projections in SmearedParticles/Jets compare() methods.
2016-07-29 Andy Buckley <andy.buckley@cern.ch>
* Rename TOTEM_2012_002 to proper TOTEM_2012_I1220862 name.
* Remove conditional building of obsolete, preliminary and
unvalidated analyses. Now always built, since there are sufficient
warnings.
2016-07-28 Holger Schulz <holger.schulz@cern.ch>
* Mark D0_2000... W pT analysis validated
* Mark LHCB_2011_S919... phi meson analysis validated
2016-07-25 Andy Buckley <andy.buckley@cern.ch>
* Add unbound accessors for momentum properties of ParticleBase objects.
* Add Rivet/Tools/ParticleBaseUtils.hh to collect tools like functors for particle & jet filtering.
* Add vector<ptr> versions of Analysis::scale() and ::normalize(), for batched scaling.
* Add Analysis::scale() and Analysis::divide() methods for Counter types.
* Utils.hh: add a generic sum() function for containers, and use auto in loop to support arrays.
* Set data path as well as lib path in scripts with --pwd option, and use abs path to $PWD.
* Add setAnalysisDataPaths and addAnalysisDataPath to RivetPaths.hh/cc and Python.
* Pass absolutized RIVET_DATA_PATH from rivet-mkhtml to rivet-cmphistos.
2016-07-24 Holger Schulz <holger.schulz@cern.ch>
* Mark CDF_2008_S77... b jet shapes validated
* Added protection against low stats yoda exception
in finalize for that analysis
2016-07-22 Andy Buckley <andy.buckley@cern.ch>
* Fix newly introduced bug in make-plots which led to data point
markers being skipped for all but the last bin.
2016-07-21 Andy Buckley <andy.buckley@cern.ch>
* Add pid, abspid, charge, abscharge, charge3, and abscharge3 Cut
enums, handled by Particle cut targets.
* Add abscharge() and abscharge3() methods to Particle.
* Add optional Cut and duplicate-removal flags to Particle children & descendants methods.
* Add unbound versions of Particle is* and from* methods, for easier functor use.
* Add Particle::isPrompt() as a member rather than unbound function.
* Add protections against -ve mass from numerical precision errors in smearing functions.
2016-07-20 Andy Buckley <andy.buckley@cern.ch>
* Move several internal system headers into the include/Rivet/Tools directory.
* Fix median-computing safety logic in ATLAS_2010_S8914702 and
tidy this and @todo markers in several similar analyses.
* Add to_str/toString and stream functions for Particle, and a bit
of Particle util function reorganisation.
* Add isStrange/Charm/Bottom PID and Particle functions.
* Add RangeError exception throwing from MathUtils.hh stats
functions if given empty/mismatched datasets.
* Add Rivet/Tools/PrettyPrint.hh, based on https://louisdx.github.io/cxx-prettyprint/
* Allow use of path regex group references in .plot file keyed values.
2016-07-20 Holger Schulz <holger.schulz@cern.ch>
* Fix the --nskip behaviour on the main rivet script.
2016-07-07 Andy Buckley <andy.buckley@cern.ch>
* Release version 2.5.0
2016-07-01 Andy Buckley <andy.buckley@cern.ch>
* Fix pandoc interface flag version detection.
2016-06-28 Andy Buckley <andy.buckley@cern.ch>
* Release version 2.4.3
* Add ATLAS_2016_I1468168 early ttbar fully leptonic fiducial
cross-section analysis at 13 TeV.
2016-06-21 Andy Buckley <andy.buckley@cern.ch>
* Add ATLAS_2016_I1457605 inclusive photon analysis at 8 TeV.
2016-06-15 Andy Buckley <andy.buckley@cern.ch>
* Add a --show-bibtex option to the rivet script, for convenient
outputting of a BibTeX db for the used analyses.
2016-06-14 Andy Buckley <andy.buckley@cern.ch>
* Add and rename 4-vector boost calculation methods: new methods
beta, betaVec, gamma & gammaVec are now preferred to the
deprecated boostVector method.
2016-06-13 Andy Buckley <andy.buckley@cern.ch>
* Add and use projection handling methods declare(proj, pname) and
apply<PROJ>(evt, pname) rather than the longer and explicitly
'projectiony' addProjection & applyProjection.
* Start using the DEFAULT_RIVET_ANALYSIS_CTOR macro (newly created
preferred alias to long-present DEFAULT_RIVET_ANA_CONSTRUCTOR)
* Add a DEFAULT_RIVET_PROJ_CLONE macro for implementing the
clone() method boiler-plate code in projections.
2016-06-10 Andy Buckley <andy.buckley@cern.ch>
* Add a NonPromptFinalState projection, and tweak the
PromptFinalState and unbound Particle functions a little in
response. May need some more finessing.
* Add user-facing aliases to ProjectionApplier add, get, and apply
methods... the templated versions of which can now be called
without using the word 'projection', which makes the function
names a bit shorter and pithier, and reduces semantic repetition.
2016-06-10 Andy Buckley <andy.buckley@cern.ch>
* Adding ATLAS_2015_I1397635 Wt at 8 TeV analysis.
* Adding ATLAS_2015_I1390114 tt+b(b) at 8 TeV analysis.
2016-06-09 Andy Buckley <andy.buckley@cern.ch>
* Downgrade some non-fatal error messages from ERROR to WARNING
status, because *sigh* ATLAS's software treats any appearance of
the word 'ERROR' in its log file as a reason to report the job as
failed (facepalm).
2016-06-07 Andy Buckley <andy.buckley@cern.ch>
* Adding ATLAS 13 TeV minimum bias analysis, ATLAS_2016_I1419652.
2016-05-30 Andy Buckley <andy.buckley@cern.ch>
* pyext/rivet/util.py: Add pandoc --wrap/--no-wrap CLI detection
and batch conversion.
* bin/rivet: add -o as a more standard 'output' option flag alias to -H.
2016-05-23 Andy Buckley <andy.buckley@cern.ch>
* Remove the last ref-data bin from table 16 of
ATLAS_2010_S8918562, due to data corruption. The corresponding
HepData record will be amended by ATLAS.
2016-05-12 Holger Schulz <holger.schulz@durham.ac.uk>
* Mark ATLAS_2012_I1082009 as validated after exhaustive tests with
Pythia8 and Sherpa in inclusive QCD mode.
2016-05-11 Andy Buckley <andy.buckley@cern.ch>
* Specialise return error codes from the rivet script.
2016-05-11 Andy Buckley <andy.buckley@cern.ch>
* Add Event::allParticles() to provide neater (but not *helpful*)
access to Rivet-wrapped versions of the raw particles in the
Event::genEvent() record, and hence reduce HepMC digging.
2016-05-05 Andy Buckley <andy.buckley@cern.ch>
* Version 2.4.2 release!
* Update SLD_2002_S4869273 ref data to match publication erratum,
now updated in HepData. Thanks to Peter Skands for the report and
Mike Whalley / Graeme Watt for the quick fix and heads-up.
2016-04-27 Andy Buckley <andy.buckley@cern.ch>
* Add CMS_2014_I1305624 event shapes analysis, with standalone
variable calculation struct embedded in an unnamed namespace.
2016-04-19 Andy Buckley <andy.buckley@cern.ch>
* Various clean-ups and fixes in ATLAS analyses using isolated
photons with median pT density correction.
2016-04-18 Andy Buckley <andy.buckley@cern.ch>
* Add transformBy(LT) methods to Particle and Jet.
* Add mkObjectTransform and mkFrameTransform factory methods to LorentzTransform.
2016-04-17 Andy Buckley <andy.buckley@cern.ch>
* Add null GenVertex protection in Particle children & descendants methods.
2016-04-15 Andy Buckley <andy.buckley@cern.ch>
* Add ATLAS_2015_I1397637, ATLAS 8 TeV boosted top cross-section vs. pT
2016-04-14 Andy Buckley <andy.buckley@cern.ch>
* Add a --no-histos argument to the rivet script.
2016-04-13 Andy Buckley <andy.buckley@cern.ch>
* Add ATLAS_2015_I1351916 (8 TeV Z FB asymmetry) and
ATLAS_2015_I1408516 (8 TeV Z phi* and pT) analyses, and their _EL,
_MU variants.
2016-04-12 Andy Buckley <andy.buckley@cern.ch>
* Patch PID utils for ordering issues in baryon decoding.
2016-04-11 Andy Buckley <andy.buckley@cern.ch>
* Actually implement ZEUS_2001_S4815815... only 10 years late!
2016-04-08 Andy Buckley <andy.buckley@cern.ch>
* Add a --guess-prefix flag to rivet-config, cf. fastjet-config.
* Add RIVET_DATA_PATH variable and related functions in C++ and
Python as a common first-fallback for RIVET_REF_PATH,
RIVET_INFO_PATH, and RIVET_PLOT_PATH.
* Add --pwd options to rivet-mkhtml and rivet-cmphistos
2016-04-07 Andy Buckley <andy.buckley@cern.ch>
* Remove implicit conventional event rotation for HERA -- this
needs to be done explicitly from now.
* Add comBoost functions and methods to Beam.hh, and tidy
LorentzTransformation.
* Restructure Beam projection functions for beam particle and
sqrtS extraction, and add asqrtS functions.
* Rename and improve PID and Particle Z,A,lambda functions ->
nuclZ,nuclA,nuclNlambda.
2016-04-05 Andy Buckley <andy.buckley@cern.ch>
* Improve binIndex function, with an optional argument to allow
overflow lookup, and add it to testMath.
* Adding setPE, setPM, setPtEtaPhiM, etc. methods and
corresponding mk* static methods to FourMomentum, as well as
adding more convenience aliases and vector attributes for
completeness. Coordinate conversion functions taken from
HEPUtils::P4. New attrs also mapped to ParticleBase.
2016-03-29 Andy Buckley <andy.buckley@cern.ch>
* ALEPH_1996_S3196992.cc, ATLAS_2010_S8914702.cc,
ATLAS_2011_I921594.cc, ATLAS_2011_S9120807.cc,
ATLAS_2012_I1093738.cc, ATLAS_2012_I1199269.cc,
ATLAS_2013_I1217867.cc, ATLAS_2013_I1244522.cc,
ATLAS_2013_I1263495.cc, ATLAS_2014_I1307756.cc,
ATLAS_2015_I1364361.cc, CDF_2008_S7540469.cc,
CMS_2015_I1370682.cc, MC_JetSplittings.cc, STAR_2006_S6870392.cc:
Updates for new FastJets interface, and other cleaning.
* Deprecate 'standalone' FastJets constructors -- they are
misleading.
* More improvements around jets, including unbound conversion and
filtering routines between collections of Particles, Jets, and
PseudoJets.
* Place 'Cut' forward declaration in a new Cuts.fhh header.
* Adding a Cuts::OPEN extern const (a bit more standard- and
constant-looking than Cuts::open())
2016-03-28 Andy Buckley <andy.buckley@cern.ch>
* Improvements to FastJets constructors, including specification
of optional AreaDefinition as a constructor arg, disabling dodgy
no-FS constructors which I suspect don't work properly in the
brave new world of automatic ghost tagging, using a bit of
judicious constructor delegation, and completing/exposing use of
shared_ptr for internal memory management.
2016-03-26 Andy Buckley <andy.buckley@cern.ch>
* Remove Rivet/Tools/RivetBoost.hh and Boost references from
rivet-config, rivet-buildplugin, and configure.ac. It's gone ;-)
* Replace Boost assign usage with C++11 brace initialisers. All
Boost use is gone from Rivet!
* Replace Boost lexical_cast and string algorithms.
2016-03-25 Andy Buckley <andy.buckley@cern.ch>
* Bug-fix in semi-leptonic top selection of CMS_2015_I1370682.
2016-03-12 Andy Buckley <andy.buckley@cern.ch>
* Allow multi-line major tick labels on make-plots linear x and y
axes. Linebreaks are indicated by \n in the .dat file.
2016-03-09 Andy Buckley <andy.buckley@cern.ch>
* Release 2.4.1
2016-03-03 Andy Buckley <andy.buckley@cern.ch>
* Add a --nskip flag to the rivet command-line tool, to allow
processing to begin in the middle of an event file (useful for
batched processing of large files, in combination with --nevts)
2016-03-03 Holger Schulz <holger.schulz@durham.ac.uk>
* Add ATLAS 7 TeV event shapes in Z+jets analysis (ATLAS_2016_I1424838)
2016-02-29 Andy Buckley <andy.buckley@cern.ch>
* Update make-plots to use multiprocessing rather than threading.
* Add FastJets::trimJet method, thanks to James Monk for the
suggestion and patch.
* Add new preferred name PID::charge3 in place of
PID::threeCharge, and also convenience PID::abscharge and
PID::abscharge3 functions -- all derived from changes in external
HEPUtils.
* Add analyze(const GenEvent*) and analysis(string&) methods to
AnalysisHandler, plus some docstring improvements.
2016-02-23 Andy Buckley <andy.buckley@cern.ch>
* New ATLAS_2015_I1394679 analysis.
* New MC_HHJETS analysis from Andreas Papaefstathiou.
* Ref data updates for ATLAS_2013_I1219109, ATLAS_2014_I1312627,
and ATLAS_2014_I1319490.
* Add automatic output paging to 'rivet --show-analyses'
2016-02-16 Andy Buckley <andy.buckley@cern.ch>
* Apply cross-section unit fixes and plot styling improvements to
ATLAS_2013_I1217863 analyses, thanks to Christian Gutschow.
* Fix to rivet-cmphistos to avoid overwriting RatioPlotYLabel if
already set via e.g. the PLOT pseudo-file. Thanks to Johann Felix
v. Soden-Fraunhofen.
2016-02-15 Andy Buckley <andy.buckley@cern.ch>
* Add Analysis::bookCounter and some machinery in rivet-cmphistos
to avoid getting tripped up by unplottable (for now) data types.
* Add --font and --format options to rivet-mkhtml and make-plots,
to replace the individual flags used for that purpose. Not fully
cleaned up, but a necessary step.
* Add new plot styling options to rivet-cmphistos and
rivet-mkhtml. Thanks to Gavin Hesketh.
* Modify rivet-cmphistos and rivet-mkhtml to apply plot hiding if
*any* path component is hidden by an underscore prefix, as
implemented in AOPath, plus other tidying using new AOPath
methods.
* Add pyext/rivet/aopaths.py, containing AOPath object for central
& standard decoding of Rivet-standard analysis object path
structures.
2016-02-12 Andy Buckley <andy.buckley@cern.ch>
* Update ParticleIdUtils.hh (i.e. PID:: functions) to use the
functions from the latest version of MCUtils' PIDUtils.h.
2016-01-15 Andy Buckley <andy.buckley@cern.ch>
* Change rivet-cmphistos path matching logic from match to search
(user can add explicit ^ marker if they want match semantics).
2015-12-20 Andy Buckley <andy.buckley@cern.ch>
* Improve linspace (and hence also logspace) precision errors by
using multiplication rather than repeated addition to build edge
list (thanks to Holger Schulz for the suggestion).
2015-12-15 Andy Buckley <andy.buckley@cern.ch>
* Add cmphistos and make-plots machinery for handling 'suffix'
variations on plot paths, currently just by plotting every line,
with the variations in a 70% faded tint.
* Add Beam::pv() method for finding the beam interaction primary
vertex 4-position.
* Add a new Particle::setMomentum(E,x,y,z) method, and an origin
position member which is automatically populated from the
GenParticle, with access methods corresponding to the momentum
ones.
2015-12-10 Andy Buckley <andy.buckley@cern.ch>
* make-plots: improve custom tick attribute handling, allowing
empty lists. Also, any whitespace now counts as a tick separator
-- explicit whitespace in labels should be done via ~ or similar
LaTeX markup.
2015-12-04 Andy Buckley <andy.buckley@cern.ch>
* Pro-actively use -m/-M arguments when initially loading
histograms in mkhtml, *before* passing them to cmphistos.
2015-12-03 Andy Buckley <andy.buckley@cern.ch>
* Move contains() and has_key() functions on STL containers from std to Rivet namespaces.
* Adding IsRef attributes to all YODA refdata files; this will be
used to replace the /REF prefix in Rivet v3 onwards. The migration
has also removed leading # characters from BEGIN/END blocks, as
per YODA format evolution: new YODA versions as required by
current Rivet releases are able to read both the old and new
formats.
2015-12-02 Andy Buckley <andy.buckley@cern.ch>
* Add handling of a command-line PLOT 'file' argument to rivet-mkhtml, cf. rivet-cmphistos.
* Improvements to rivet-mkhtml behaviour re. consistency with
rivet-cmphistos in how muti-part histo paths are decomposed into
analysis-name + histo name, and removal of 'NONE' strings.
2015-11-30 Andy Buckley <andy.buckley@cern.ch>
* Relax rivet/plotinfo.py pattern matching on .plot file
components, to allow leading whitespace and around = signs, and to
make the leading # optional on BEGIN/END blocks.
2015-11-26 Andy Buckley <andy.buckley@cern.ch>
* Write out intermediate histogram files by default, with event interval of 10k.
2015-11-25 Andy Buckley <andy.buckley@cern.ch>
* Protect make-plots against lock-up due to partial pstricks command when there are no data points.
2015-11-17 Andy Buckley <andy.buckley@cern.ch>
* rivet-cmphistos: Use a ratio label that doesn't mention 'data' when plotting MC vs. MC.
2015-11-12 Andy Buckley <andy.buckley@cern.ch>
* Tweak plot and subplot sizing defaults in make-plots so the
total canvas is always the same size by default.
2015-11-10 Andy Buckley <andy.buckley@cern.ch>
* Handle 2D histograms better in rivet-cmphistos (since they can't be overlaid)
2015-11-05 Andy Buckley <andy.buckley@cern.ch>
* Allow comma-separated analysis name lists to be passed to a single -a/--analysis/--analyses option.
* Convert namespace-global const variables to be static, to suppress compiler warnings.
* Use standard MAX_DBL and MAX_INT macros as a source for MAXDOUBLE and MAXINT, to suppress GCC5 warnings.
2015-11-04 Holger Schulz <holger.schulz@durham.ac.uk>
* Adding LHCB inelastic xsection measurement (LHCB_2015_I1333223)
* Adding ATLAS colour flow in ttbar->semileptonic measurement (ATLAS_2015_I1376945)
2015-10-07 Chris Pollard <cpollard@cern.ch>
* Release 2.4.0
2015-10-06 Holger Schulz <holger.schulz@durham.ac.uk>
* Adding CMS_2015_I1327224 dijet analysis (Mjj>2 TeV)
2015-10-03 Holger Schulz <holger.schulz@durham.ac.uk>
* Adding CMS_2015_I1346843 Z+gamma
2015-09-30 Andy Buckley <andy.buckley@cern.ch>
* Important improvement in FourVector & FourMomentum: new reverse()
method to return a 4-vector in which only the spatial component
has been inverted cf. operator- which flips the t/E component as
well.
2015-09-28 Holger Schulz <holger.schulz@durham.ac.uk>
* Adding D0_2000_I503361 ZPT at 1800 GeV
2015-09-29 Chris Pollard <cpollard@cern.ch>
* Adding ATLAS_2015_CONF_2015_041
2015-09-29 Chris Pollard <cpollard@cern.ch>
* Adding ATLAS_2015_I1387176
2015-09-29 Chris Pollard <cpollard@cern.ch>
* Adding ATLAS_2014_I1327229
2015-09-28 Chris Pollard <cpollard@cern.ch>
* Adding ATLAS_2014_I1326641
2015-09-28 Holger Schulz <holger.schulz@durham.ac.uk>
* Adding CMS_2013_I1122847 FB assymetry in DY analysis
2015-09-28 Andy Buckley <andy.buckley@cern.ch>
* Adding CMS_2015_I1385107 LHA pp 2.76 TeV track-jet underlying event.
2015-09-27 Andy Buckley <andy.buckley@cern.ch>
* Adding CMS_2015_I1384119 LHC Run 2 minimum bias dN/deta with no B field.
2015-09-25 Andy Buckley <andy.buckley@cern.ch>
* Adding TOTEM_2014_I1328627 forward charged density in eta analysis.
2015-09-23 Andy Buckley <andy.buckley@cern.ch>
* Add CMS_2015_I1310737 Z+jets analysis.
* Allow running MC_{W,Z}INC, MC_{W,Z}JETS as separate bare lepton
analyses.
2015-09-23 Andy Buckley <andy.buckley@cern.ch>
* FastJets now allows use of FastJet pure ghosts, by excluding
them from the constituents of Rivet Jet objects. Thanks to James
Monk for raising the issue and providing a patch.
2015-09-15 Andy Buckley <andy.buckley@cern.ch>
* More MissingMomentum changes: add optional 'mass target'
argument when retrieving the vector sum as a 4-momentum, with the
mass defaulting to 0 rather than sqrt(sum(E)^2 - sum(p)^2).
* Require Boost 1.55 for robust compilation, as pointed out by
Andrii Verbytskyi.
2015-09-10 Andy Buckley <andy.buckley@cern.ch>
* Allow access to MissingMomentum projection via WFinder.
* Adding extra methods to MissingMomentum, to make it more user-friendly.
2015-09-09 Andy Buckley <andy.buckley@cern.ch>
* Fix factor of 2 in LHCB_2013_I1218996 normalisation, thanks to
Felix Riehn for the report.
2015-08-20 Frank Siegert <frank.siegert@cern.ch>
* Add function to ZFinder to retrieve all fiducial dressed
leptons, e.g. to allow vetoing on a third one (proposed by
Christian Gutschow).
2015-08-18 Andy Buckley <andy.buckley@cern.ch>
* Rename xs and counter AOs to start with underscores, and modify
rivet-cmphistos to skip AOs whose basenames start with _.
2015-08-17 Andy Buckley <andy.buckley@cern.ch>
* Add writing out of cross-section and total event counter by
default. Need to add some name protection to avoid them being
plotted.
2015-08-16 Andy Buckley <andy.buckley@cern.ch>
* Add templated versions of Analysis::refData() to use data types
other than Scatter2DPtr, and convert the cached ref data store to
generic AnalysisObjectPtrs to make it possible.
2015-07-29 Andy Buckley <andy.buckley@cern.ch>
* Add optional Cut arguments to all the Jet tag methods.
* Add exception handling and pre-emptive testing for a
non-writeable output directory (based on patch from Lukas
Heinrich).
2015-07-24 Andy Buckley <andy.buckley@cern.ch>
* Version 2.3.0 release.
2015-07-02 Holger Schulz <holger.schulz@durham.ac.uk>
* Tidy up ATLAS higgs combination analysis.
* Add ALICE kaon, pion analysis (ALICE_2015_I1357424)
* Add ALICE strange baryon analysis (ALICE_2014_I1300380)
* Add CDF ZpT measurement in Z->ee events analysis (CDF_2012_I1124333)
* Add validated ATLAS W+charm measurement (ATLAS_2014_I1282447)
* Add validated CMS jet and dijet analysis (CMS_2013_I1208923)
2015-07-01 Andy Buckley <andy.buckley@cern.ch>
* Define a private virtual operator= on Projection, to block
'sliced' accidental value copies of derived class instances.
* Add new muon-in-jet options to FastJet constructors, pass that
and invisibles enums correctly to JetAlg, tweak the default
strategies, and add a FastJets constructor from a
fastjet::JetDefinition (while deprecating the plugin-by-reference
constructor).
2015-07-01 Holger Schulz <holger.schulz@durham.ac.uk>
* Add D0 phi* measurement (D0_2015_I1324946).
* Remove WUD and MC_PHOTONJETUE analyses
* Don't abort ATLAS_2015_I1364361 if there is no stable Higgs
print a warning instead and veto event
2015-07-01 Andy Buckley <andy.buckley@cern.ch>
* Add all, none, from-decay muon filtering options to JetAlg and
FastJets.
* Rename NONPROMPT_INVISIBLES to DECAY_INVISIBLES for clarity &
extensibility.
* Remove FastJets::ySubJet, splitJet, and filterJet methods --
they're BDRS-paper-specific and you can now use the FastJet
objects directly to do this and much more.
* Adding InvisiblesStrategy to JetAlg, using it rather than a bool
in the useInvisibles method, and updating FastJets to use this
approach for its particle filtering and to optionally use the enum
in the constructor arguments. The new default invisibles-using
behaviour is to still exclude _prompt_ invisibles, and the default
is still to exclude them all. Only one analysis
(src/Analyses/STAR_2006_S6870392.cc) required updating, since it
was the only one to be using the FastJets legacy seed_threshold
constructor argument.
* Adding isVisible method to Particle, taken from
VisibleFinalState (which now uses this).
2015-06-30 Andy Buckley <andy.buckley@cern.ch>
* Marking many old & superseded ATLAS analyses as obsolete.
* Adding cmpMomByMass and cmpMomByAscMass sorting functors.
* Bump version to 2.3.0 and require YODA > 1.4.0 (current head at
time of development).
2015-06-08 Andy Buckley <andy.buckley@cern.ch>
* Add handling of -m/-M flags on rivet-cmphistos and rivet-mkhtml,
moving current rivet-mkhtml -m/-M to -a/-A (for analysis name
pattern matching). Requires YODA head (will be YODA 1.3.2 of
1.4.0).
* src/Analyses/ATLAS_2015_I1364361.cc: Now use the built-in prompt
photon selecting functions.
* Tweak legend positions in MC_JETS .plot file.
* Add a bit more debug output from ZFinder and WFinder.
2015-05-24 Holger Schulz <holger.schulz@durham.ac.uk>
* Normalisation discussion concerning ATLAS_2014_I1325553
is resolved. Changed YLabel accordingly.
2015-05-19 Holger Schulz <holger.schulz@durham.ac.uk>
* Add (preliminary) ATLAS combined Higgs analysis
(ATLAS_2015_I1364361). Data will be updated and more
histos added as soon as paper is published in journal.
For now using data taken from public ressource
https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/HIGG-2014-11/
2015-05-19 Peter Richardson <peter.richardson@durham.ac.uk>
* Fix ATLAS_2014_I1325553 normalisation of histograms was wrong by
factor of two |y| vs y problem
2015-05-01 Andy Buckley <andy.buckley@cern.ch>
* Fix MC_HJETS/HINC/HKTSPLITTINGS analyses to (ab)use the ZFinder
with a mass range of 115-135 GeV and a mass target of 125 GeV (was
previously 115-125 and mass target of mZ)
2015-04-30 Andy Buckley <andy.buckley@cern.ch>
* Removing uses of boost::assign::list_of, preferring the existing
comma-based assign override for now, for C++11 compatibility.
* Convert MC_Z* analysis finalize methods to use scale() rather than normalize().
2015-04-01 Holger Schulz <holger.schulz@durham.ac.uk>
* Add CMS 7 TeV rapidity gap analysis (CMS_2015_I1356998).
* Remove FinalState Projection.
2015-03-30 Holger Schulz <holger.schulz@durham.ac.uk>
* Add ATLAS 7 TeV photon + jets analysis (ATLAS_2013_I1244522).
2015-03-26 Andy Buckley <andy.buckley@cern.ch>
* Updates for HepMC 2.07 interface constness improvements.
2015-03-25 Holger Schulz <holger.schulz@durham.ac.uk>
* Add ATLAS double parton scattering in W+2j analysis (ATLAS_2013_I1216670).
2015-03-24 Andy Buckley <andy.buckley@cern.ch>
* 2.2.1 release!
2015-03-23 Holger Schulz <holger.schulz@durham.ac.uk>
* Add ATLAS differential Higgs analysis (ATLAS_2014_I1306615).
2015-03-19 Chris Pollard <cpollard@cern.ch>
* Add ATLAS V+gamma analyses (ATLAS_2013_I1217863)
2015-03-20 Andy Buckley <andy.buckley@cern.ch>
* Adding ATLAS R-jets analysis i.e. ratios of W+jets and Z+jets
observables (ATLAS_2014_I1312627 and _EL, _MU variants)
* include/Rivet/Tools/ParticleUtils.hh: Adding same/oppSign and
same/opp/diffCharge functions, operating on two Particles.
* include/Rivet/Tools/ParticleUtils.hh: Adding HasAbsPID functor
and removing optional abs arg from HasPID.
2015-03-19 Andy Buckley <andy.buckley@cern.ch>
* Mark ATLAS_2012_I1083318 as VALIDATED and fix d25-x01-y02 ref data.
2015-03-19 Chris Pollard <cpollard@cern.ch>
* Add ATLAS W and Z angular analyses (ATLAS_2011_I928289)
2015-03-19 Andy Buckley <andy.buckley@cern.ch>
* Add LHCb charged particle multiplicities and densities analysis (LHCB_2014_I1281685)
* Add LHCb Z y and phi* analysis (LHCB_2012_I1208102)
2015-03-19 Holger Schulz <holger.schulz@durham.ac.uk>
* Add ATLAS dijet analysis (ATLAS_2014_I1325553).
* Add ATLAS Z pT analysis (ATLAS_2014_I1300647).
* Add ATLAS low-mass Drell-Yan analysis (ATLAS_2014_I1288706).
* Add ATLAS gap fractions analysis (ATLAS_2014_I1307243).
2015-03-18 Andy Buckley <andy.buckley@cern.ch>
* Adding CMS_2014_I1298810 and CMS_2014_I1303894 analyses.
2015-03-18 Holger Schulz <holger.schulz@durham.ac.uk>
* Add PDG_TAUS analysis which makes use of the TauFinder.
* Add ATLAS 'traditional' Underlying Event in Z->mumu analysis (ATLAS_2014_I1315949).
2015-03-18 Andy Buckley <andy.buckley@cern.ch>
* Change UnstableFinalState duplicate resolution to use the last
in a chain rather than the first.
2015-03-17 Holger Schulz <holger.schulz@durham.ac.uk>
* Update Taufinder to use decaytyoe (can be HADRONIC, LEPTONIC or
ANY), in FastJet.cc --- set TauFinder mode to hadronic for tau-tagging
2015-03-16 Chris Pollard <cpollard@cern.ch>
* Removed fuzzyEquals() from Vector3::angle()
2015-03-16 Andy Buckley <andy.buckley@cern.ch>
* Adding Cuts-based constructor to PrimaryHadrons.
* Adding missing compare() method to HeavyHadrons projection.
2015-03-15 Chris Pollard <cpollard@cern.ch>
* Adding FinalPartons projection which selects the quarks and
gluons immediately before hadronization
2015-03-05 Andy Buckley <andy.buckley@cern.ch>
* Adding Cuts-based constructors and other tidying in UnstableFinalState and HeavyHadrons
2015-03-03 Andy Buckley <andy.buckley@cern.ch>
* Add support for a PLOT meta-file argument to rivet-cmphistos.
2015-02-27 Andy Buckley <andy.buckley@cern.ch>
* Improved time reporting.
2015-02-24 Andy Buckley <andy.buckley@cern.ch>
* Add Particle::fromHadron and Particle::fromPromptTau, and add a
boolean 'prompt' argument to Particle::fromTau.
* Fix WFinder use-transverse-mass property setting. Thanks to Christian Gutschow.
2015-02-04 Andy Buckley <andy.buckley@cern.ch>
* Add more protection against math domain errors with log axes.
* Add some protection against nan-valued points and error bars in make-plots.
2015-02-03 Andy Buckley <andy.buckley@cern.ch>
* Converting 'bitwise' to 'logical' Cuts combinations in all analyses.
2015-02-02 Andy Buckley <andy.buckley@cern.ch>
* Use vector MET rather than scalar VET (doh...) in WFinder
cut. Thanks to Ines Ochoa for the bug report.
* Updating and tidying analyses with deprecation warnings.
* Adding more Cuts/FS constructors for Charged,Neutral,UnstableFinalState.
* Add &&, || and ! operators for without-parens-warnings Cut
combining. Note these don't short-circuit, but this is ok since
Cut comparisons don't have side-effects.
* Add absetaIn, absrapIn Cut range definitions.
* Updating use of sorted particle/jet access methods and cmp
functors in projections and analyses.
2014-12-09 Andy Buckley <andy.buckley@cern.ch>
* Adding a --cmd arg to rivet-buildplugin to allow the output
paths to be sed'ed (to help deal with naive Grid
distribution). For example BUILDROOT=`rivet-config --prefix`;
rivet-buildplugin PHOTONS.cc --cmd | sed -e
"s:$BUILDROOT:$SITEROOT:g"
2014-11-26 Andy Buckley <andy.buckley@cern.ch>
* Interface improvements in DressedLeptons constructor.
* Adding DEPRECATED macro to throw compiler deprecation warnings when using deprecated features.
2014-11-25 Andy Buckley <andy.buckley@cern.ch>
* Adding Cut-based constructors, and various constructors with
lists of PDG codes to IdentifiedFinalState.
2014-11-20 Andy Buckley <andy.buckley@cern.ch>
* Analysis updates (ATLAS, CMS, CDF, D0) to apply the changes below.
* Adding JetAlg jets(Cut, Sorter) methods, and other interface
improvements for cut and sorted ParticleBase retrieval from JetAlg
and ParticleFinder projections. Some old many-doubles versions
removed, syntactic sugar sorting methods deprecated.
* Adding Cuts::Et and Cuts::ptIn, Cuts::etIn, Cuts::massIn.
* Moving FastJet includes, conversions, uses etc. into Tools/RivetFastJet.hh
2014-10-07 Andy Buckley <andy.buckley@cern.ch>
* Fix a bug in the isCharmHadron(pid) function and remove isStrange* functions.
2014-09-30 Andy Buckley <andy.buckley@cern.ch>
* 2.2.0 release!
* Mark Jet::containsBottom and Jet::containsCharm as deprecated
methods: use the new methods. Analyses updated.
* Add Jet::bTagged(), Jet::cTagged() and Jet::tauTagged() as
ghost-assoc-based replacements for the 'contains' tagging methods.
2014-09-17 Andy Buckley <andy.buckley@cern.ch>
* Adding support for 1D and 3D YODA scatters, and helper methods
for calling the efficiency, asymm and 2D histo divide functions.
2014-09-12 Andy Buckley <andy.buckley@cern.ch>
* Adding 5 new ATLAS analyses:
ATLAS_2011_I921594: Inclusive isolated prompt photon analysis with full 2010 LHC data
ATLAS_2013_I1263495: Inclusive isolated prompt photon analysis with 2011 LHC data
ATLAS_2014_I1279489: Measurements of electroweak production of dijets + $Z$ boson, and distributions sensitive to vector boson fusion
ATLAS_2014_I1282441: The differential production cross section of the $\phi(1020)$ meson in $\sqrt{s}=7$ TeV $pp$ collisions measured with the ATLAS detector
ATLAS_2014_I1298811: Leading jet underlying event at 7 TeV in ATLAS
* Adding a median(vector<NUM>) function and fixing the other stats
functions to operate on vector<NUM> rather than vector<int>.
2014-09-03 Andy Buckley <andy.buckley@cern.ch>
* Fix wrong behaviour of LorentzTransform with a null boost vector
-- thanks to Michael Grosse.
2014-08-26 Andy Buckley <andy.buckley@cern.ch>
* Add calc() methods to Hemispheres as requested, to allow it to
be used with Jet or FourMomentum inputs outside the normal
projection system.
2014-08-17 Andy Buckley <andy.buckley@cern.ch>
* Improvements to the particles methods on
ParticleFinder/FinalState, in particular adding the range of cuts
arguments cf. JetAlg (and tweaking the sorted jets equivalent) and
returning as a copy rather than a reference if cut/sorted to avoid
accidentally messing up the cached copy.
* Creating ParticleFinder projection base class, and moving
Particles-accessing methods from FinalState into it.
* Adding basic forms of MC_ELECTRONS, MC_MUONS, and MC_TAUS
analyses.
2014-08-15 Andy Buckley <andy.buckley@cern.ch>
* Version bump to 2.2.0beta1 for use at BOOST and MCnet school.
2014-08-13 Andy Buckley <andy.buckley@cern.ch>
* New analyses:
ATLAS_2014_I1268975 (high mass dijet cross-section at 7 TeV)
ATLAS_2014_I1304688 (jet multiplicity and pT at 7 TeV)
ATLAS_2014_I1307756 (scalar diphoton resonance search at 8 TeV -- no histograms!)
CMSTOTEM_2014_I1294140 (charged particle pseudorapidity at 8 TeV)
2014-08-09 Andy Buckley <andy.buckley@cern.ch>
* Adding PromptFinalState, based on code submitted by Alex
Grohsjean and Will Bell. Thanks!
2014-08-06 Andy Buckley <andy.buckley@cern.ch>
* Adding MC_HFJETS and MC_JETTAGS analyses.
2014-08-05 Andy Buckley <andy.buckley@cern.ch>
* Update all analyses to use the xMin/Max/Mid, xMean, xWidth,
etc. methods on YODA classes rather than the deprecated lowEdge
etc.
* Merge new HasPID functor from Holger Schulz into
Rivet/Tools/ParticleUtils.hh, mainly for use with the any()
function in Rivet/Tools/Utils.hh
2014-08-04 Andy Buckley <andy.buckley@cern.ch>
* Add ghost tagging of charms, bottoms and taus to FastJets, and
tag info accessors to Jet.
* Add constructors from and cast operators to FastJet's PseudoJet
object from Particle and Jet.
* Convert inRange to not use fuzzy comparisons on closed
intervals, providing old version as fuzzyInRange.
2014-07-30 Andy Buckley <andy.buckley@cern.ch>
* Remove classifier functions accepting a Particle from the PID
inner namespace.
2014-07-29 Andy Buckley <andy.buckley@cern.ch>
* MC_JetAnalysis.cc: re-enable +- ratios for eta and y, now that
YODA divide doesn't throw an exception.
* ATLAS_2012_I1093734: fix a loop index error which led to the
first bin value being unfilled for half the dphi plots.
* Fix accidental passing of a GenParticle pointer as a PID code
int in HeavyHadrons.cc. Effect limited to incorrect deductions
about excited HF decay chains and should be small. Thanks to
Tomasz Przedzinski for finding and reporting the issue during
HepMC3 design work!
2014-07-23 Andy Buckley <andy.buckley@cern.ch>
* Fix to logspace: make sure that start and end values are exact,
not the result of exp(log(x)).
2014-07-16 Andy Buckley <andy.buckley@cern.ch>
* Fix setting of library paths for doc building: Python can't
influence the dynamic loader in its own process by setting an
environment variable because the loader only looks at the variable
once, when it starts.
2014-07-02 Andy Buckley <andy.buckley@cern.ch>
* rivet-cmphistos now uses the generic yoda.read() function rather
than readYODA() -- AIDA files can also be compared and plotted
directly now.
2014-06-24 Andy Buckley <andy.buckley@cern.ch>
* Add stupid missing <string> include and std:: prefix in Rivet.hh
2014-06-20 Holger Schulz <hschulz@physik.hu-berlin.de>
* bin/make-plots: Automatic generation of minor xtick labels if LogX is requested
but data resides e.g. in [200, 700]. Fixes m_12 plots of, e.g.
ATLAS_2010_S8817804
2014-06-17 David Grellscheid <David.Grellscheid@durham.ac.uk>
* pyext/rivet/Makefile.am: 'make distcheck' and out-of-source
builds should work now.
2014-06-10 Andy Buckley <andy.buckley@cern.ch>
* Fix use of the install command for bash completion installation on Macs.
2014-06-07 Andy Buckley <andy.buckley@cern.ch>
* Removing direct includes of MathUtils.hh and others from analysis code files.
2014-06-02 Andy Buckley <andy.buckley@cern.ch>
* Rivet 2.1.2 release!
2014-05-30 Andy Buckley <andy.buckley@cern.ch>
* Using Particle absrap(), abseta() and abspid() where automatic conversion was feasible.
* Adding a few extra kinematics mappings to ParticleBase.
* Adding p3() accessors to the 3-momentum on FourMomentum, Particle, and Jet.
* Using Jet and Particle kinematics methods directly (without momentum()) where possible.
* More tweaks to make-plots 2D histo parsing behaviour.
2014-05-30 Holger Schulz <hschulz@physik.hu-berlin.de>
* Actually fill the XQ 2D histo, .plot decorations.
* Have make-plots produce colourmaps using YODA_3D_SCATTER
objects. Remove the grid in colourmaps.
* Some tweaks for the SFM analysis, trying to contact Martin Wunsch
who did the unfolding back then.
2014-05-29 Holger Schulz <hschulz@physik.hu-berlin.de>
* Re-enable 2D histo in MC_PDFS
2014-05-28 Andy Buckley <andy.buckley@cern.ch>
* Updating analysis and project routines to use Particle::pid() by
preference to Particle::pdgId(), and Particle::abspid() by
preference to abs(Particle::pdgId()), etc.
* Adding interfacing of smart pointer types and booking etc. for
YODA 2D histograms and profiles.
* Improving ParticleIdUtils and ParticleUtils functions based on
merging of improved function collections from MCUtils, and
dropping the compiled ParticleIdUtils.cc file.
2014-05-27 Andy Buckley <andy.buckley@cern.ch>
* Adding CMS_2012_I1090423 (dijet angular distributions),
CMS_2013_I1256943 (Zbb xsec and angular correlations),
CMS_2013_I1261026 (jet and UE properties vs. Nch) and
D0_2000_I499943 (bbbar production xsec and angular correlations).
2014-05-26 Andy Buckley <andy.buckley@cern.ch>
* Fixing a bug in plot file handling, and adding a texpand()
routine to rivet.util, to be used to expand some 'standard'
physics TeX macros.
* Adding ATLAS_2012_I1124167 (min bias event shapes),
ATLAS_2012_I1203852 (ZZ cross-section), and ATLAS_2013_I1190187
(WW cross-section) analyses.
2014-05-16 Andy Buckley <andy.buckley@cern.ch>
* Adding any(iterable, fn) and all(iterable, fn) template functions for convenience.
2014-05-15 Holger Schulz <holger.schulz@cern.ch>
* Fix some bugs in identified hadron PIDs in OPAL_1998_S3749908.
2014-05-13 Andy Buckley <andy.buckley@cern.ch>
* Writing out [UNVALIDATED], [PRELIMINARY], etc. in the
--list-analyses output if analysis is not VALIDATED.
2014-05-12 Andy Buckley <andy.buckley@cern.ch>
* Adding CMS_2013_I1265659 colour coherence analysis.
2014-05-07 Andy Buckley <andy.buckley@cern.ch>
* Bug fixes in CMS_2013_I1209721 from Giulio Lenzi.
* Fixing compiler warnings from clang, including one which
indicated a misapplied cut bug in CDF_2006_S6653332.
2014-05-05 Andy Buckley <andy.buckley@cern.ch>
* Fix missing abs() in Particle::abspid()!!!!
2014-04-14 Andy Buckley <andy.buckley@cern.ch>
* Adding the namespace protection workaround for Boost described
at http://www.boost.org/doc/libs/1_55_0/doc/html/foreach.html
2014-04-13 Andy Buckley <andy.buckley@cern.ch>
* Adding a rivet.pc template file and installation rule for pkg-config to use.
* Updating data/refdata/ALEPH_2001_S4656318.yoda to corrected version in HepData.
2014-03-27 Andy Buckley <andy.buckley@cern.ch>
* Flattening PNG output of make-plots (i.e. no transparency) and other tweaks.
2014-03-23 Andy Buckley <andy.buckley@cern.ch>
* Renaming the internal meta-particle class in DressedLeptons (and
exposed in the W/ZFinders) from ClusteredLepton to DressedLepton
for consistency with the change in name of its containing class.
* Removing need for cmake and unportable yaml-cpp trickery by
using libtool to build an embedded symbol-mangled copy of yaml-cpp
rather than trying to mangle and build direct from the tarball.
2014-03-10 Andy Buckley <andy.buckley@cern.ch>
* Rivet 2.1.1 release.
2014-03-07 Andy Buckley <andy.buckley@cern.ch>
* Adding ATLAS multilepton search (no ref data file), ATLAS_2012_I1204447.
2014-03-05 Andy Buckley <andy.buckley@cern.ch>
* Also renaming Breit-Wigner functions to cdfBW, invcdfBW and bwspace.
* Renaming index_between() to the more Rivety binIndex(), since that's the only real use of such a function... plus a bit of SFINAE type relaxation trickery.
2014-03-04 Andy Buckley <andy.buckley@cern.ch>
* Adding programmatic access to final histograms via AnalysisHandler::getData().
* Adding CMS 4 jet correlations analysis, CMS_2013_I1273574.
* Adding CMS W + 2 jet double parton scattering analysis, CMS_2013_I1272853.
* Adding ATLAS isolated diphoton measurement, ATLAS_2012_I1199269.
* Improving the index_between function so the numeric types don't
have to exactly match.
* Adding better momentum comparison functors and sortBy, sortByX
functions to use them easily on containers of Particle, Jet, and
FourMomentum.
2014-02-10 Andy Buckley <andy.buckley@cern.ch>
* Removing duplicate and unused ParticleBase sorting functors.
* Removing unused HT increment and units in ATLAS_2012_I1180197 (unvalidated SUSY).
* Fixing photon isolation logic bug in CMS_2013_I1258128 (Z rapidity).
* Replacing internal uses of #include Rivet/Rivet.hh with
Rivet/Config/RivetCommon.hh, removing the MAXRAPIDITY const, and
repurposing Rivet/Rivet.hh as a convenience include for external
API users.
* Adding isStable, children, allDescendants, stableDescendants,
and flightLength functions to Particle.
* Replacing Particle and Jet deltaX functions with generic ones on
ParticleBase, and adding deltaRap variants.
* Adding a Jet.fhh forward declaration header, including fastjet::PseudoJet.
* Adding a RivetCommon.hh header to allow Rivet.hh to be used externally.
* Fixing HeavyHadrons to apply pT cuts if specified.
2014-02-06 Andy Buckley <andy.buckley@cern.ch>
* 2.1.0 release!
2014-02-05 Andy Buckley <andy.buckley@cern.ch>
* Protect against invalid prefix value if the --prefix configure option is unused.
2014-02-03 Andy Buckley <andy.buckley@cern.ch>
* Adding the ATLAS_2012_I1093734 fwd-bwd / azimuthal minbias correlations analysis.
* Adding the LHCB_2013_I1208105 forward energy flow analysis.
2014-01-31 Andy Buckley <andy.buckley@cern.ch>
* Checking the YODA minimum version in the configure script.
* Fixing the JADE_OPAL analysis ycut values to the midpoints,
thanks to information from Christoph Pahl / Stefan Kluth.
2014-01-29 Andy Buckley <andy.buckley@cern.ch>
* Removing unused/overrestrictive Isolation* headers.
2014-01-27 Andy Buckley <andy.buckley@cern.ch>
* Re-bundling yaml-cpp, now built as a mangled static lib based on
the LHAPDF6 experience.
* Throw a UserError rather than an assert if AnalysisHandler::init
is called more than once.
2014-01-25 David Grellscheid <david.grellscheid@durham.ac.uk>
* src/Core/Cuts.cc: New Cuts machinery, already used in FinalState.
Old-style "mineta, maxeta, minpt" constructors kept around for ease of
transition. Minimal set of convenience functions available, like EtaIn(),
should be expanded as needed.
2014-01-22 Andy Buckley <andy.buckley@cern.ch>
* configure.ac: Remove opportunistic C++11 build, until this
becomes mandatory (in version 2.2.0?). Anyone who wants C++11 can
explicitly set the CXXFLAGS (and DYLDFLAGS for pre-Mavericks Macs)
2014-01-21 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* src/Core/Analysis.cc: Fixed bug in Analysis::isCompatible where
an 'abs' was left out when checking that beam energes does not
differ by more than 1GeV.
* src/Analyses/CMS_2011_S8978280.cc: Fixed checking of beam energy
and booking corresponding histograms.
2013-12-19 Andy Buckley <andy.buckley@cern.ch>
* Adding pid() and abspid() methods to Particle.
* Adding hasCharm and hasBottom methods to Particle.
* Adding a sorting functor arg version of the ZFinder::constituents() method.
* Adding pTmin cut accessors to HeavyHadrons.
* Tweak to the WFinder constructor to place the target W (trans) mass argument last.
2013-12-18 Andy Buckley <andy.buckley@cern.ch>
* Adding a GenParticle* cast operator to Particle, removing the
Particle and Jet copies of the momentum cmp functors, and general
tidying/improvement/unification of the momentum properties of jets
and particles.
2013-12-17 Andy Buckley <andy.buckley@cern.ch>
* Using SFINAE techniques to improve the math util functions.
* Adding isNeutrino to ParticleIdUtils, and
isHadron/isMeson/isBaryon/isLepton/isNeutrino methods to Particle.
* Adding a FourMomentum cast operator to ParticleBase, so that
Particle and Jet objects can be used directly as FourMomentums.
2013-12-16 Andy Buckley <andy@duality>
* LeptonClusters renamed to DressedLeptons.
* Adding singular particle accessor functions to WFinder and ZFinder.
* Removing ClusteredPhotons and converting ATLAS_2010_S8919674.
2013-12-12 Andy Buckley <andy.buckley@cern.ch>
* Fixing a problem with --disable-analyses (thanks to David Hall)
* Require FastJet version 3.
* Bumped version to 2.1.0a0
* Adding -DNDEBUG to the default build flags, unless in --enable-debug mode.
* Adding a special treatment of RIVET_*_PATH variables: if they
end in :: the default search paths will not be appended. Used
primarily to restrict the doc builds to look only inside the build
dirs, but potentially also useful in other special circumstances.
* Adding a definition of exec_prefix to rivet-buildplugin.
* Adding -DNDEBUG to the default non-debug build flags.
2013-11-27 Andy Buckley <andy.buckley@cern.ch>
* Removing accidentally still-present no-as-needed linker flag from rivet-config.
* Lots of analysis clean-up and migration to use new features and W/Z finder APIs.
* More momentum method forwarding on ParticleBase and adding
abseta(), absrap() etc. functions.
* Adding the DEFAULT_RIVET_ANA_CONSTRUCTOR cosmetic macro.
* Adding deltaRap() etc. function variations
* Adding no-decay photon clustering option to WFinder and ZFinder,
and replacing opaque bool args with enums.
* Adding an option for ignoring photons from hadron/tau decays in LeptonClusters.
2013-11-22 Andy Buckley <andy.buckley@cern.ch>
* Adding Particle::fromBottom/Charm/Tau() members. LHCb were
aready mocking this up, so it seemed sensible to add it to the
interface as a more popular (and even less dangerous) version of
hasAncestor().
* Adding an empty() member to the JetAlg interface.
2013-11-07 Andy Buckley <andy.buckley@cern.ch>
* Adding the GSL lib path to the library path in the env scripts
and the rivet-config --ldflags output.
2013-10-25 Andy Buckley <andy.buckley@cern.ch>
* 2.0.0 release!!!!!!
2013-10-24 Andy Buckley <andy.buckley@cern.ch>
* Supporting zsh completion via bash completion compatibility.
2013-10-22 Andy Buckley <andy.buckley@cern.ch>
* Updating the manual to describe YODA rather than AIDA and the new rivet-cmphistos script.
* bin/make-plots: Adding paths to error messages in histogram combination.
* CDF_2005_S6217184: fixes to low stats errors and final scatter plot binning.
2013-10-21 Andy Buckley <andy.buckley@cern.ch>
* Several small fixes in jet shape analyses, SFM_1984, etc. found
in the last H++ validation run.
2013-10-18 Andy Buckley <andy.buckley@cern.ch>
* Updates to configure and the rivetenv scripts to try harder to discover YODA.
2013-09-26 Andy Buckley <andy.buckley@cern.ch>
* Now bundling Cython-generated files in the tarballs, so Cython
is not a build requirement for non-developers.
2013-09-24 Andy Buckley <andy.buckley@cern.ch>
* Removing unnecessary uses of a momentum() indirection when
accessing kinematic variables.
* Clean-up in Jet, Particle, and ParticleBase, in particular
splitting PID functions on Particle from those on PID codes, and
adding convenience kinematic functions to ParticleBase.
2013-09-23 Andy Buckley <andy.buckley@cern.ch>
* Add the -avoid-version flag to libtool.
* Final analysis histogramming issues resolved.
2013-08-16 Andy Buckley <andy.buckley@cern.ch>
* Adding a ConnectBins flag in make-plots, to decide whether to
connect adjacent, gapless bins with a vertical line. Enabled by
default (good for the step-histo default look of MC lines), but
now rivet-cmphistos disables it for the reference data.
2013-08-14 Andy Buckley <andy.buckley@cern.ch>
* Making 2.0.0beta3 -- just a few remaining analysis migration
issues remaining but it's worth making another beta since there
were lots of framework fixes/improvements.
2013-08-11 Andy Buckley <andy.buckley@cern.ch>
* ARGUS_1993_S2669951 also fixed using scatter autobooking.
* Fixing remaining issues with booking in BABAR_2007_S7266081
using the feature below (far nicer than hard-coding).
* Adding a copy_pts param to some Analysis::bookScatter2D methods:
pre-setting the points with x values is sometimes genuinely
useful.
2013-07-26 Andy Buckley <andy.buckley@cern.ch>
* Removed the (officially) obsolete CDF 2008 LEADINGJETS and
NOTE_9351 underlying event analyses -- superseded by the proper
versions of these analyses based on the final combined paper.
* Removed the semi-demo Multiplicity projection -- only the
EXAMPLE analysis and the trivial ALEPH_1991_S2435284 needed
adaptation.
2013-07-24 Andy Buckley <andy.buckley@cern.ch>
* Adding a rejection of histo paths containing /TMP/ from the
writeData function. Use this to handle booked temporary
histograms... for now.
2013-07-23 Andy Buckley <andy.buckley@cern.ch>
* Make rivet-cmphistos _not_ draw a ratio plot if there is only one line.
* Improvements and fixes to HepData lookup with rivet-mkanalysis.
2013-07-22 Andy Buckley <andy.buckley@cern.ch>
* Add -std=c++11 or -std=c++0x to the Rivet compiler flags if supported.
* Various fixes to analyses with non-zero numerical diffs.
2013-06-12 Andy Buckley <andy.buckley@cern.ch>
* Adding a new HeavyHadrons projection.
* Adding optional extra include_end args to logspace() and linspace().
2013-06-11 Andy Buckley <andy.buckley@cern.ch>
* Moving Rivet/RivetXXX.hh tools headers into Rivet/Tools/.
* Adding PrimaryHadrons projection.
* Adding particles_in/out functions on GenParticle to RivetHepMC.
* Moved STL extensions from Utils.hh to RivetSTL.hh and tidying.
* Tidying, improving, extending, and documenting in RivetSTL.hh.
* Adding a #include of Logging.hh into Projection.hh, and removing
unnecessary #includes from all Projection headers.
2013-06-10 Andy Buckley <andy.buckley@cern.ch>
* Moving htmlify() and detex() Python functions into rivet.util.
* Add HepData URL for Inspire ID lookup to the rivet script.
* Fix analyses' info files which accidentally listed the Inspire
ID under the SpiresID metadata key.
2013-06-07 Andy Buckley <andy.buckley@cern.ch>
* Updating mk-analysis-html script to produce MathJax output
* Adding a version of Analysis::removeAnalysisObject() which takes
an AO pointer as its argument.
* bin/rivet: Adding pandoc-based conversion of TeX summary and
description strings to plain text on the terminal output.
* Add MathJax to rivet-mkhtml output, set up so the .info entries should render ok.
* Mark the OPAL 1993 analysis as UNVALIDATED: from the H++
benchmark runs it looks nothing like the data, and there are some
outstanding ambiguities.
2013-06-06 Andy Buckley <andy.buckley@cern.ch>
* Releasing 2.0.0b2 beta version.
2013-06-05 Andy Buckley <andy.buckley@cern.ch>
* Renaming Analysis::add() etc. to very explicit
addAnalysisObject(), sorting out shared_pointer polymorphism
issues via the Boost dynamic_pointer_cast, and adding a full set
of getHisto1D(), etc. explicitly named and typed accessors,
including ones with HepData dataset/axis ID signatures.
* Adding histo booking from an explicit reference Scatter2D (and
more placeholders for 2D histos / 3D scatters) and rewriting
existing autobooking to use this.
* Converting inappropriate uses of size_t to unsigned int in Analysis.
* Moving Analysis::addPlot to Analysis::add() (or reg()?) and
adding get() and remove() (or unreg()?)
* Fixing attempted abstraction of import fallbacks in rivet.util.import_ET().
* Removing broken attempt at histoDir() caching which led to all
histograms being registered under the same analysis name.
2013-06-04 Andy Buckley <andy.buckley@cern.ch>
* Updating the Cython version requirement to 0.18
* Adding Analysis::integrate() functions and tidying the Analysis.hh file a bit.
2013-06-03 Andy Buckley <andy.buckley@cern.ch>
* Adding explicit protection against using inf/nan scalefactors in
ATLAS_2011_S9131140 and H1_2000_S4129130.
* Making Analysis::scale noisly complain about invalid
scalefactors.
2013-05-31 Andy Buckley <andy.buckley@cern.ch>
* Reducing the TeX main memory to ~500MB. Turns out that it *can*
be too large with new versions of TeXLive!
2013-05-30 Andy Buckley <andy.buckley@cern.ch>
* Reverting bookScatter2D behaviour to never look at ref data, and
updating a few affected analyses. This should fix some bugs with
doubled datapoints introduced by the previous behaviour+addPoint.
* Adding a couple of minor Utils.hh and MathUtils.hh features.
2013-05-29 Andy Buckley <andy.buckley@cern.ch>
* Removing Constraints.hh header.
* Minor bugfixes and improvements in Scatter2D booking and MC_JetAnalysis.
2013-05-28 Andy Buckley <andy.buckley@cern.ch>
* Removing defunct HistoFormat.hh and HistoHandler.{hh,cc}
2013-05-27 Andy Buckley <andy.buckley@cern.ch>
* Removing includes of Logging.hh, RivetYODA.hh, and
ParticleIdUtils.hh from analyses (and adding an include of
ParticleIdUtils.hh to Analysis.hh)
* Removing now-unused .fhh files.
* Removing lots of unnecessary .fhh includes from core classes:
everything still compiling ok. A good opportunity to tidy this up
before the release.
* Moving the rivet-completion script from the data dir to bin (the
completion is for scripts in bin, and this makes development
easier).
* Updating bash completion scripts for YODA format and
compare-histos -> rivet-cmphistos.
2013-05-23 Andy Buckley <andy.buckley@cern.ch>
* Adding Doxy comments and a couple of useful convenience functions to Utils.hh.
* Final tweaks to ATLAS ttbar jet veto analysis (checked logic with Kiran Joshi).
2013-05-15 Andy Buckley <andy.buckley@cern.ch>
* Many 1.0 -> weight bugfixes in ATLAS_2011_I945498.
* yaml-cpp v3 support re-introduced in .info parsing.
* Lots of analysis clean-ups for YODA TODO issues.
2013-05-13 Andy Buckley <andy.buckley@cern.ch>
* Analysis histo booking improvements for Scatter2D, placeholders
for 2D histos, and general tidying.
2013-05-12 Andy Buckley <andy.buckley@cern.ch>
* Adding configure-time differentiation between yaml-cpp API versions 3 and 5.
2013-05-07 Andy Buckley <andy.buckley@cern.ch>
* Converting info file reading to use the yaml-cpp 0.5.x API.
2013-04-12 Andy Buckley <andy.buckley@cern.ch>
* Tagging as 2.0.0b1
2013-04-04 Andy Buckley <andy.buckley@cern.ch>
* Removing bundling of yaml-cpp: it needs to be installed by the
user / bootstrap script from now on.
2013-04-03 Andy Buckley <andy.buckley@cern.ch>
* Removing svn:external m4 directory, and converting Boost
detection to use better boost.m4 macros.
2013-03-22 Andy Buckley <andy.buckley@cern.ch>
* Moving PID consts to the PID namespace and corresponding code
updates and opportunistic clean-ups.
* Adding Particle::fromDecay() method.
2013-03-09 Andy Buckley <andy.buckley@cern.ch>
* Version bump to 2.0.0b1 in anticipation of first beta release.
* Adding many more 'popular' particle ID code named-consts and
aliases, and updating the RapScheme enum with ETA -> ETARAP, and
fixing affected analyses (plus other opportunistic tidying / minor
bug-fixing).
* Fixing a symbol misnaming in ATLAS_2012_I1119557.
2013-03-07 Andy Buckley <andy.buckley@cern.ch>
* Renaming existing uses of ParticleVector to the new 'Particles' type.
* Updating util classes, projections, and analyses to deal with
the HepMC return value changes.
* Adding new Particle(const GenParticle*) constructor.
* Converting Particle::genParticle() to return a const pointer
rather than a reference, for the same reason as below (+
consistency within Rivet and with the HepMC pointer-centric coding
design).
* Converting Event to use a different implementation of original
and modified GenParticles, and to manage the memory in a more
future-proof way. Event::genParticle() now returns a const pointer
rather than a reference, to signal that the user is leaving the
happy pastures of 'normal' Rivet behind.
* Adding a Particles typedef by analogy to Jets, and in preference
to the cumbersome ParticleVector.
* bin/: Lots of tidying/pruning of messy/defunct scripts.
* Creating spiresbib, util, and plotinfo rivet python module
submodules: this eliminates lighthisto and the standalone
spiresbib modules. Util contains convenience functions for Python
version testing, clean ElementTree import, and process renaming,
for primary use by the rivet-* scripts.
* Removing defunct scripts that have been replaced/obsoleted by YODA.
2013-03-06 Andy Buckley <andy.buckley@cern.ch>
* Fixing doc build so that the reference histos and titles are
~correctly documented. We may want to truncate some of the lists!
2013-03-06 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added ATLAS_2012_I1125575 analysis
* Converted rivet-mkhtml to yoda
* Introduced rivet-cmphistos as yoda based replacement for compare-histos
2013-03-05 Andy Buckley <andy.buckley@cern.ch>
* Replacing all AIDA ref data with YODA versions.
* Fixing the histograms entries in the documentation to be
tolerant to plotinfo loading failures.
* Making the findDatafile() function primarily find YODA data
files, then fall back to AIDA. The ref data loader will use the
appropriate YODA format reader.
2013-02-05 David Grellscheid <David.Grellscheid@durham.ac.uk>
* include/Rivet/Math/MathUtils.hh: added BWspace bin edge method
to give equal-area Breit-Wigner bins
2013-02-01 Andy Buckley <andy.buckley@cern.ch>
* Adding an element to the PhiMapping enum and a new mapAngle(angle, mapping) function.
* Fixes to Vector3::azimuthalAngle and Vector3::polarAngle calculation (using the mapAngle functions).
2013-01-25 Frank Siegert <frank.siegert@cern.ch>
* Split MC_*JETS analyses into three separate bits:
MC_*INC (inclusive properties)
MC_*JETS (jet properties)
MC_*KTSPLITTINGS (kT splitting scales).
2013-01-22 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fix TeX variable in the rivetenv scripts, especially for csh
2012-12-21 Andy Buckley <andy.buckley@cern.ch>
* Version 1.8.2 release!
2012-12-20 Andy Buckley <andy.buckley@cern.ch>
* Adding ATLAS_2012_I1119557 analysis (from Roman Lysak and Lily Asquith).
2012-12-18 Andy Buckley <andy.buckley@cern.ch>
* Adding TOTEM_2012_002 analysis, from Sercan Sen.
2012-12-18 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added CMS_2011_I954992 analysis
2012-12-17 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added CMS_2012_I1193338 analysis
* Fixed xi cut in ATLAS_2011_I894867
2012-12-17 Andy Buckley <andy.buckley@cern.ch>
* Adding analysis descriptions to the HTML analysis page ToC.
2012-12-14 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added CMS_2012_PAS_FWD_11_003 analysis
* Added LHCB_2012_I1119400 analysis
2012-12-12 Andy Buckley <andy.buckley@cern.ch>
* Correction to jet acceptance in CMS_2011_S9120041, from Sercan Sen: thanks!
2012-12-12 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added CMS_2012_PAS_QCD_11_010 analysis
2012-12-07 Andy Buckley <andy.buckley@cern.ch>
* Version number bump to 1.8.2 -- release approaching.
* Rewrite of ALICE_2012_I1181770 analysis to make it a bit more sane and acceptable.
* Adding a note on FourVector and FourMomentum that operator- and
operator-= invert both the space and time components: use of -=
can result in a vector with negative energy.
* Adding particlesByRapidity and particlesByAbsRapidity to FinalState.
2012-12-07 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added ALICE_2012_I1181770 analysis
* Bump version to 1.8.2
2012-12-06 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added ATLAS_2012_I1188891 analysis
* Added ATLAS_2012_I1118269 analysis
* Added CMS_2012_I1184941 analysis
* Added LHCB_2010_I867355 analysis
* Added TGraphErrors support to root2flat
2012-11-27 Andy Buckley <andy.buckley@cern.ch>
* Converting CMS_2012_I1102908 analysis to use YODA.
* Adding XLabel and YLabel setting in histo/profile/scatter booking.
2012-11-27 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fix make-plots png creation for SL5
2012-11-23 Peter Richardson <peter.richardson@durham.ac.uk>
* Added ATLAS_2012_CONF_2012_153 4-lepton SUSY search
2012-11-17 Andy Buckley <andy.buckley@cern.ch>
* Adding MC_PHOTONS by Steve Lloyd and AB, for testing general
unisolated photon properties, especially those associated with
charged leptons (e and mu).
2012-11-16 Andy Buckley <andy.buckley@cern.ch>
* Adding MC_PRINTEVENT, a convenient (but verbose!) analysis for
printing out event details to stdout.
2012-11-15 Andy Buckley <andy.buckley@cern.ch>
* Removing the long-unused/defunct autopackage system.
2012-11-15 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added LHCF_2012_I1115479 analysis
* Added ATLAS_2011_I894867 analysis
2012-11-14 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added CMS_2012_I1102908 analysis
2012-11-14 Andy Buckley <andy.buckley@cern.ch>
* Converting the argument order of logspace, clarifying the
arguments, updating affected code, and removing Analysis::logBinEdges.
* Merging updates from the AIDA maintenance branch up to r4002
(latest revision for next merges is r4009).
2012-11-11 Andy Buckley <andy.buckley@cern.ch>
* include/Math/: Various numerical fixes to Vector3::angle and
changing the 4 vector mass treatment to permit spacelike
virtualities (in some cases even the fuzzy isZero assert check was
being violated). The angle check allows a clean-up of some
workaround code in MC_VH2BB.
2012-10-15 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added CMS_2012_I1107658 analysis
2012-10-11 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added CDF_2012_NOTE10874 analysis
2012-10-04 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added ATLAS_2012_I1183818 analysis
2012-07-17 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Cleanup and multiple fixes in CMS_2011_S9120041
* Bugfixed in ALEPH_2004_S5765862 and ATLAS_2010_CONF_2010_049
(thanks to Anil Pratap)
2012-08-09 Andy Buckley <andy.buckley@cern.ch>
* Fixing aida2root command-line help message and converting to TH*
rather than TGraph by default.
2012-07-24 Andy Buckley <andy.buckley@cern.ch>
* Improvements/migrations to rivet-mkhtml, rivet-mkanalysis, and
rivet-buildplugin.
2012-07-17 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Add CMS_2012_I1087342
2012-07-12 Andy Buckley <andy.buckley@cern.ch>
* Fix rivet-mkanalysis a bit for YODA compatibility.
2012-07-05 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Version 1.8.1!
2012-07-05 Holger Schulz <holger.schulz@physik.hu-berlin.de>
* Add ATLAS_2011_I945498
2012-07-03 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Bugfix for transverse mass (thanks to Gavin Hesketh)
2012-06-29 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Merge YODA branch into trunk. YODA is alive!!!!!!
2012-06-26 Holger Schulz <holger.schulz@physik.hu-berlin.de>
* Add ATLAS_2012_I1091481
2012-06-20 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added D0_2011_I895662: 3-jet mass
2012-04-24 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* fixed a few bugs in rivet-rmgaps
* Added new TOTEM dN/deta analysis
2012-03-19 Andy Buckley <andy.buckley@cern.ch>
* Version 1.8.0!
* src/Projections/UnstableFinalState.cc: Fix compiler warning.
* Version bump for testing: 1.8.0beta1.
* src/Core/AnalysisInfo.cc: Add printout of YAML parser exception error messages to aid debugging.
* bin/Makefile.am: Attempt to fix rivet-nopy build on SLC5.
* src/Analyses/LHCB_2010_S8758301.cc: Add two missing entries to the PDGID -> lifetime map.
* src/Projections/UnstableFinalState.cc: Extend list of vetoed particles to include reggeons.
2012-03-16 Andy Buckley <andy.buckley@cern.ch>
* Version change to 1.8.0beta0 -- nearly ready for long-awaited release!
* pyext/setup.py.in: Adding handling for the YAML library: fix for
Genser build from Anton Karneyeu.
* src/Analyses/LHCB_2011_I917009.cc: Hiding lifetime-lookup error
message if the offending particle is not a hadron.
* include/Rivet/Math/MathHeader.hh: Using unnamespaced std::isnan
and std::isinf as standard.
2012-03-16 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Improve default plot behaviour for 2D histograms
2012-03-15 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Make ATLAS_2012_I1084540 less verbose, and general code
cleanup of that analysis.
* New-style plugin hook in ATLAS_2011_I926145,
ATLAS_2011_I944826 and ATLAS_2012_I1084540
* Fix compiler warnings in ATLAS_2011_I944826 and CMS_2011_S8973270
* CMS_2011_S8941262: Weights are double, not int.
* disable inRange() tests in test/testMath.cc until we have a proper
fix for the compiler warnings we see on SL5.
2012-03-07 Andy Buckley <andy.buckley@cern.ch>
* Marking ATLAS_2011_I919017 as VALIDATED (this should have
happened a long time ago) and adding more references.
2012-02-28 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* lighthisto.py: Caching for re.compile(). This speeds up aida2flat
and flat2aida by more than an order of magnitude.
2012-02-27 Andy Buckley <andy.buckley@cern.ch>
* doc/mk-analysis-html: Adding more LaTeX/text -> HTML conversion
replacements, including better <,> handling.
2012-02-26 Andy Buckley <andy.buckley@cern.ch>
* Adding CMS_2011_S8973270, CMS_2011_S8941262, CMS_2011_S9215166,
CMS_QCD_10_024, from CMS.
* Adding LHCB_2011_I917009 analysis, from Alex Grecu.
* src/Core/Analysis.cc, include/Rivet/Analysis.hh: Add a numeric-arg version of histoPath().
2012-02-24 Holger Schulz <holger.schulz@physik.hu-berlin.de>
* Adding ATLAS Ks/Lambda analysis.
2012-02-20 Andy Buckley <andy.buckley@cern.ch>
* src/Analyses/ATLAS_2011_I925932.cc: Using new overflow-aware
normalize() in place of counters and scale(..., 1/count)
2012-02-14 Andy Buckley <andy.buckley@cern.ch>
* Splitting MC_GENERIC to put the PDF and PID plotting into
MC_PDFS and MC_IDENTIFIED respectively.
* Renaming MC_LEADINGJETS to MC_LEADJETUE.
2012-02-14 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* DELPHI_1996_S3430090 and ALEPH_1996_S3486095:
fix rapidity vs {Thrust,Sphericity}-axis.
2012-02-14 Andy Buckley <andy.buckley@cern.ch>
* bin/compare-histos: Don't attempt to remove bins from MC histos
where they aren't found in the ref file, if the ref file is not
expt data, or if the new --no-rmgapbins arg is given.
* bin/rivet: Remove the conversion of requested analysis names to
upper-case: mixed-case analysis names will now work.
2012-02-14 Frank Siegert <frank.siegert@cern.ch>
* Bugfixes and improvements for MC_TTBAR:
- Avoid assert failure with logspace starting at 0.0
- Ignore charged lepton in jet finding (otherwise jet multi is always
+1).
- Add some dR/deta/dphi distributions as noted in TODO
- Change pT plots to logspace as well (to avoid low-stat high pT bins)
2012-02-10 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* rivet-mkhtml -c option now has the semantics of a .plot
file. The contents are appended to the dat output by
compare-histos.
2012-02-09 David Grellscheid <david.grellscheid@durham.ac.uk>
* Fixed broken UnstableFS behaviour
2012-01-25 Frank Siegert <frank.siegert@cern.ch>
* Improvements in make-plots:
- Add PlotTickLabels and RatioPlotTickLabels options (cf.
make-plots.txt)
- Make ErrorBars and ErrorBands non-exclusive (and change
their order, such that Bars are on top of Bands)
2012-01-25 Holger Schulz <holger.schulz@physik.hu-berlin.de>
* Add ATLAS diffractive gap analysis
2012-01-23 Andy Buckley <andy.buckley@cern.ch>
* bin/rivet: When using --list-analyses, the analysis summary is
now printed out when log level is <= INFO, rather than < INFO.
The effect on command line behaviour is that useful identifying
info is now printed by default when using --list-analyses, rather
than requiring --list-analyses -v. To get the old behaviour,
e.g. if using the output of rivet --list-analyses for scripting,
now use --list-analyses -q.
2012-01-22 Andy Buckley <andy.buckley@cern.ch>
* Tidying lighthisto, including fixing the order in which +- error
values are passed to the Bin constructor in fromFlatHisto.
2012-01-16 Frank Siegert <frank.siegert@cern.ch>
* Bugfix in ATLAS_2012_I1083318: Include non-signal neutrinos in
jet clustering.
* Add first version of ATLAS_2012_I1083318 (W+jets). Still
UNVALIDATED until final happiness with validation plots arises and
data is in Hepdata.
* Bugfix in ATLAS_2010_S8919674: Really use neutrino with highest
pT for Etmiss. Doesn't seem to make very much difference, but is
more correct in principle.
2012-01-16 Peter Richardson <peter.richardson@durham.ac.uk>
* Fixes to ATLAS_20111_S9225137 to include reference data
2012-01-13 Holger Schulz <holger.schulz@physik.hu-berlin.de>
* Add ATLAS inclusive lepton analysis
2012-01-12 Hendrik Hoeth <hendrik.hoeth@durham.ac.uk>
* Font selection support in rivet-mkhtml
2012-01-11 Peter Richardson <peter.richardson@durham.ac.uk>
* Added pi0 to list of particles.
2012-01-11 Andy Buckley <andy.buckley@cern.ch>
* Removing references to Boost random numbers.
2011-12-30 Andy Buckley <andy.buckley@cern.ch>
* Adding a placeholder rivet-which script (not currently
installed).
* Tweaking to avoid a very time-consuming debug printout in
compare-histos with the -v flag, and modifying the Rivet env vars
in rivet-mkhtml before calling compare-histos to eliminate
problems induced by relative paths (i.e. "." does not mean the
same thing when the directory is changed within the script).
2011-12-12 Andy Buckley <andy.buckley@cern.ch>
* Adding a command line completion function for rivet-mkhtml.
2011-12-12 Frank Siegert <frank.siegert@cern.ch>
* Fix for factor of 2.0 in normalisation of CMS_2011_S9086218
* Add --ignore-missing option to rivet-mkhtml to ignore non-existing
AIDA files.
2011-12-06 Andy Buckley <andy.buckley@cern.ch>
* Include underflow and overflow bins in the normalisation when
calling Analysis::normalise(h)
2011-11-23 Andy Buckley <andy.buckley@cern.ch>
* Bumping version to 1.8.0alpha0 since the Jet interface changes
are quite a major break with backward compatibility (although the
vast majority of analyses should be unaffected).
* Removing crufty legacy stuff from the Jet class -- there is
never any ambiguity between whether Particle or FourMomentum
objects are the constituents now, and the jet 4-momentum is set
explicitly by the jet alg so that e.g. there is no mismatch if the
FastJet pt recombination scheme is used.
* Adding default do-nothing implementations of Analysis::init()
and Analysis::finalize(), since it is possible for analysis
implementations to not need to do anything in these methods, and
forcing analysis authors to write do-nothing boilerplate code is
not "the Rivet way"!
2011-11-19 Andy Buckley <andy.buckley@cern.ch>
* Adding variant constructors to FastJets with a more natural
Plugin* argument, and decrufting the constructor implementations a
bit.
* bin/rivet: Adding a more helpful error message if the rivet
module can't be loaded, grouping the option parser options,
removing the -A option (this just doesn't seem useful anymore),
and providing a --pwd option as a shortcut to append "." to the
search path.
2011-11-18 Andy Buckley <andy.buckley@cern.ch>
* Adding a guide to compiling a new analysis template to the
output message of rivet-mkanalysis.
2011-11-11 Andy Buckley <andy.buckley@cern.ch>
* Version 1.7.0 release!
* Protecting the OPAL 2004 analysis against NaNs in the
hemispheres projection -- I can't track the origin of these and
suspect some occasional memory corruption.
2011-11-09 Andy Buckley <andy@insectnation.org>
* Renaming source files for EXAMPLE and
PDG_HADRON_MULTIPLICITIES(_RATIOS) analyses to match the analysis
names.
* Cosmetic fixes in ATLAS_2011_S9212183 SUSY analysis.
* Adding new ATLAS W pT analysis from Elena Yatsenko (slightly adapted).
2011-10-20 Frank Siegert <frank.siegert@cern.ch>
* Extend API of W/ZFinder to allow for specification of input final
state in which to search for leptons/photons.
2011-10-19 Andy Buckley <andy@insectnation.org>
* Adding new version of LHCB_2010_S8758301, based on submission
from Alex Grecu. There is some slightly dodgy-looking GenParticle*
fiddling going on, but apparently it's necessary (and hopefully robust).
2011-10-17 Andy Buckley <andy@insectnation.org>
* bin/rivet-nopy linker line tweak to make compilation work with
GCC 4.6 (-lHepMC has to be explicitly added for some reason).
2011-10-13 Frank Siegert <frank.siegert@cern.ch>
* Add four CMS QCD analyses kindly provided by CMS.
2011-10-12 Andy Buckley <andy@insectnation.org>
* Adding a separate test program for non-matrix/vector math
functions, and adding a new set of int/float literal arg tests for
the inRange functions in it.
* Adding a jet multiplicity plot for jets with pT > 30 GeV to
MC_TTBAR.
2011-10-11 Andy Buckley <andy@insectnation.org>
* Removing SVertex.
2011-10-11 James Monk <jmonk@cern.ch>
* root2flat was missing the first bin (plus spurious last bin)
* My version of bash does not understand the pipe syntax |& in rivet-buildplugin
2011-09-30 James Monk <jmonk@cern.ch>
* Fix bug in ATLAS_2010_S8817804 that misidentified the akt4 jets
as akt6
2011-09-29 Andy Buckley <andy@insectnation.org>
* Converting FinalStateHCM to a slightly more general
DISFinalState.
2011-09-26 Andy Buckley <andy@insectnation.org>
* Adding a default libname argument to rivet-buildplugin. If the
first argument doesn't have a .so library suffix, then use
RivetAnalysis.so as the default.
2011-09-19 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* make-plots: Fixing regex for \physicscoor. Adding "FrameColor"
option.
2011-09-17 Andy Buckley <andy@insectnation.org>
* Improving interactive metadata printout, by not printing
headings for missing info.
* Bumping the release number to 1.7.0alpha0, since with these
SPIRES/Inspire changes and the MissingMomentum API change we need
more than a minor release.
* Updating the mkanalysis, BibTeX-grabbing and other places that
care about analysis SPIRES IDs to also be able to handle the new
Inspire system record IDs. The missing link is getting to HepData
from an Inspire code...
* Using the .info file rather than an in-code declaration to
specify that an analysis needs cross-section information.
* Adding Inspire support to the AnalysisInfo and Analysis
interfaces. Maybe we can find a way to combine the two,
e.g. return the SPIRES code prefixed with an "S" if no Inspire ID
is available...
2011-09-17 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added ALICE_2011_S8909580 (strange particle production at 900 GeV)
* Feed-down correction in ALICE_2011_S8945144
2011-09-16 Andy Buckley <andy@insectnation.org>
* Adding ATLAS track jet analysis, modified from the version
provided by Seth Zenz: ATLAS_2011_I919017. Note that this analysis
is currently using the Inspire ID rather than the Spires one:
we're clearly going to have to update the API to handle Inspire
codes, so might as well start now...
2011-09-14 Andy Buckley <andy@insectnation.org>
* Adding the ATLAS Z pT measurement at 7 TeV (ATLAS_2011_S9131140)
and an MC analysis for VH->bb events (MC_VH2BB).
2011-09-12 Andy Buckley <andy@insectnation.org>
* Removing uses of getLog, cout, cerr, and endl from all standard
analyses and projections, except in a very few special cases.
2011-09-10 Andy Buckley <andy@insectnation.org>
* Changing the behaviour and interface of the MissingMomentum
projection to calculate vector ET correctly. This was previously
calculated according to the common definition of -E*sin(theta) of
the summed visible 4-momentum in the event, but that is incorrect
because the timelike term grows monotonically. Instead, transverse
2-vectors of size ET need to be constructed for each visible
particle, and vector-summed in the transverse plane.
The rewrite of this behaviour made it opportune to make an API
improvement: the previous method names scalarET/vectorET() have
been renamed to scalar/vectorEt() to better match the Rivet
FourMomentum::Et() method, and MissingMomentum::vectorEt() now
returns a Vector3 rather than a double so that the transverse
missing Et direction is also available.
Only one data analysis has been affected by this change in
behaviour: the D0_2004_S5992206 dijet delta(phi) analysis. It's
expected that this change will not be very significant, as it is
a *veto* on significant missing ET to reduce non-QCD
contributions. MC studies using this analysis ~always run with QCD
events only, so these contributions should be small. The analysis
efficiency may have been greatly improved, as fewer events will
now fail the missing ET veto cut.
* Add sorting of the ParticleVector returned by the ChargedLeptons
projection.
* configure.ac: Adding a check to make sure that no-one tries to
install into --prefix=$PWD.
2011-09-04 Andy Buckley <andy@insectnation.org>
* lighthisto fixes from Christian Roehr.
2011-08-26 Andy Buckley <andy@insectnation.org>
* Removing deprecated features: the setBeams(...) method on
Analysis, the MaxRapidity constant, the split(...) function, the
default init() method from AnalysisHandler and its test, and the
deprecated TotalVisibleMomentum and PVertex projections.
2011-08-23 Andy Buckley <andy@insectnation.org>
* Adding a new DECLARE_RIVET_PLUGIN wrapper macro to hide the
details of the plugin hook system from analysis authors. Migration
of all analyses and the rivet-mkanalysis script to use this as the
standard plugin hook syntax.
* Also call the --cflags option on root-config when using the
--root option with rivet-biuldplugin (thanks to Richard Corke for
the report)
2011-08-23 Frank Siegert <frank.siegert@cern.ch>
* Added ATLAS_2011_S9126244
* Added ATLAS_2011_S9128077
2011-08-23 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added ALICE_2011_S8945144
* Remove obsolete setBeams() from the analyses
* Update CMS_2011_S8957746 reference data to the official numbers
* Use Inspire rather than Spires.
2011-08-19 Frank Siegert <frank.siegert@cern.ch>
* More NLO parton level generator friendliness: Don't crash or fail when
there are no beam particles.
* Add --ignore-beams option to skip compatibility check.
2011-08-09 David Mallows <dave.mallows@gmail.com>
* Fix aida2flat to ignore empty dataPointSet
2011-08-07 Andy Buckley <andy@insectnation.org>
* Adding TEXINPUTS and LATEXINPUTS prepend definitions to the
variables provided by rivetenv.(c)sh. A manual setting of these
variables that didn't include the Rivet TEXMFHOME path was
breaking make-plots on lxplus, presumably since the system LaTeX
packages are so old there.
2011-08-02 Frank Siegert <frank.siegert@cern.ch>
Version 1.6.0 release!
2011-08-01 Frank Siegert <frank.siegert@cern.ch>
* Overhaul of the WFinder and ZFinder projections, including a change
of interface. This solves potential problems with leptons which are not
W/Z constituents being excluded from the RemainingFinalState.
2011-07-29 Andy Buckley <andy@insectnation.org>
* Version 1.5.2 release!
* New version of aida2root from James Monk.
2011-07-29 Frank Siegert <frank.siegert@cern.ch>
* Fix implementation of --config file option in make-plots.
2011-07-27 David Mallows <dave.mallows@gmail.com>
* Updated MC_TTBAR.plot to reflect updated analysis.
2011-07-25 Andy Buckley <andy@insectnation.org>
* Adding a useTransverseMass flag method and implementation to
InvMassFinalState, and using it in the WFinder, after feedback
from Gavin Hesketh. This was the neatest way I could do it :S Some
other tidying up happened along the way.
* Adding transverse mass massT and massT2 methods and functions
for FourMomentum.
2011-07-22 Frank Siegert <frank.siegert@cern.ch>
* Added ATLAS_2011_S9120807
* Add two more observables to MC_DIPHOTON and make its isolation cut
more LHC-like
* Add linear photon pT histo to MC_PHOTONJETS
2011-07-20 Andy Buckley <andy@insectnation.org>
* Making MC_TTBAR work with semileptonic ttbar events and generally
tidying the code.
2011-07-19 Andy Buckley <andy@insectnation.org>
* Version bump to 1.5.2.b01 in preparation for a release in the
very near future.
2011-07-18 David Mallows <dave.mallows@gmail.com>
* Replaced MC_TTBAR: Added t,tbar reconstruction. Not yet working.
2011-07-18 Andy Buckley <andy@insectnation.org>
* bin/rivet-buildplugin.in: Pass the AM_CXXFLAGS
variable (including the warning flags) to the C++ compiler when
building user analysis plugins.
* include/LWH/DataPointSet.h: Fix accidental setting of errorMinus
= scalefactor * error_Plus_. Thanks to Anton Karneyeu for the bug
report!
2011-07-18 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added CMS_2011_S8884919 (charged hadron multiplicity in NSD
events corrected to pT>=0).
* Added CMS_2010_S8656010 and CMS_2010_S8547297 (charged
hadron pT and eta in NSD events)
* Added CMS_2011_S8968497 (chi_dijet)
* Added CMS_2011_S8978280 (strangeness)
2011-07-13 Andy Buckley <andy@insectnation.org>
* Rivet PDF manual updates, to not spread disinformation about
bootstrapping a Genser repo.
2011-07-12 Andy Buckley <andy@insectnation.org>
* bin/make-plots: Protect property reading against unstripped \r
characters from DOS newlines.
* bin/rivet-mkhtml: Add a -M unmatch regex flag (note that these
are matching the analysis path rather than individual histos on
this script), and speed up the initial analysis identification and
selection by avoiding loops of regex comparisons for repeats of
strings which have already been analysed.
* bin/compare-histos: remove the completely (?) unused histogram
list, and add -m and -M regex flags, as for aida2flat and
flat2aida.
2011-06-30 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* fix fromFlat() in lighthistos: It would ignore histogram paths
before.
* flat2aida: preserve histogram order from .dat files
2011-06-27 Andy Buckley <andy@insectnation.org>
* pyext/setup.py.in: Use CXXFLAGS and LDFLAGS safely in the Python
extension build, and improve the use of build/src directory
arguments.
2011-06-23 Andy Buckley <andy@insectnation.org>
* Adding a tentative rivet-updateanalyses script, based on
lhapdf-getdata, which will download new analyses as requested. We
could change our analysis-providing behaviour a bit to allow this
sort of delivery mechanism to be used as the normal way of getting
analysis updates without us having to make a whole new Rivet
release. It is nice to be able to identify analyses with releases,
though, for tracking whether bugs have been addressed.
2011-06-10 Frank Siegert <frank.siegert@cern.ch>
* Bugfixes in WFinder.
2011-06-10 Andy Buckley <andy@insectnation.org>
* Adding \physicsxcoor and \physicsycoor treatment to make-plots.
2011-06-06 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Allow for negative cross-sections. NLO tools need this.
* make-plots: For RatioPlotMode=deviation also consider the MC
uncertainties, not just data.
2011-06-04 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Add support for goodness-of-fit calculations to make-plots.
The results are shown in the legend, and one histogram can
be selected to determine the color of the plot margin. See
the documentation for more details.
2011-06-04 Andy Buckley <andy@insectnation.org>
* Adding auto conversion of Histogram2D to DataPointSets in the
AnalysisHandler _normalizeTree method.
2011-06-03 Andy Buckley <andy@insectnation.org>
* Adding a file-weight feature to the Run object, which will
optionally rescale the weights in the provided HepMC files. This
should be useful for e.g. running on multiple differently-weighted
AlpGen HepMC files/streams. The new functionality is used by the
rivet command via an optional weight appended to the filename with
a colon delimiter, e.g. "rivet fifo1.hepmc fifo2.hepmc:2.31"
2011-06-01 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Add BeamThrust projection
2011-05-31 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fix LIBS for fastjet-3.0
* Add basic infrastructure for Taylor plots in make-plots
* Fix OPAL_2004_S6132243: They are using charged+neutral.
* Release 1.5.1
2011-05-22 Andy Buckley <andy@insectnation.org>
* Adding plots of stable and decayed PID multiplicities to
MC_GENERIC (useful for sanity-checking generator setups).
* Removing actually-unused ProjectionApplier.fhh forward
declaration header.
2011-05-20 Andy Buckley <andy@insectnation.org>
* Removing import of ipython shell from rivet-rescale, having just
seen it throw a multi-coloured warning message on a student's
lxplus Rivet session!
* Adding support for the compare-histos --no-ratio flag when using
rivet-mkhtml. Adding --rel-ratio, --linear, etc. is an exercise
for the enthusiast ;-)
2011-05-10 Andy Buckley <andy@insectnation.org>
* Internal minor changes to the ProjectionHandler and
ProjectionApplier interfaces, in particular changing the
ProjectionHandler::create() function to be called getInstance and
to return a reference rather than a pointer. The reference change
is to make way for an improved singleton implementation, which
cannot yet be used due to a bug in projection memory
management. The code of the improved singleton is available, but
commented out, in ProjectionManager.hh to allow for easier
migration and to avoid branching.
2011-05-08 Andy Buckley <andy@insectnation.org>
* Extending flat2aida to be able to read from and write to
stdin/out as for aida2flat, and also eliminating the internal
histo parsing representation in favour of the one in
lighthisto. lighthisto's fromFlat also needed a bit of an
overhaul: it has been extended to parse each histo's chunk of
text (including BEGIN and END lines) in fromFlatHisto, and for
fromFlat to parse a collection of histos from a file, in keeping
with the behaviour of fromDPS/fromAIDA. Merging into Professor is
now needed.
* Extending aida2flat to have a better usage message, to accept
input from stdin for command chaining via pipes, and to be a bit
more sensibly internally structured (although it also now has to
hold all histos in memory before writing out -- that shouldn't be
a problem for anything other than truly huge histo files).
2011-05-04 Andy Buckley <andy@insectnation.org>
* compare-histos: If using --mc-errs style, prefer dotted and
dashdotted line styles to dashed, since dashes are often too long
to be distinguishable from solid lines. Even better might be to
always use a solid line for MC errs style, and to add more colours.
* rivet-mkhtml: use a no-mc-errors drawing style by default,
to match the behaviour of compare-histos, which it calls. The
--no-mc-errs option has been replaced with an --mc-errs option.
2011-05-04 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Ignore duplicate files in compare-histos.
2011-04-25 Andy Buckley <andy@insectnation.org>
* Adding some hadron-specific N and sumET vs. |eta| plots to MC_GENERIC.
* Re-adding an explicit attempt to get the beam particles, since
HepMC's IO_HERWIG seems to not always set them even though it's
meant to.
2011-04-19 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added ATLAS_2011_S9002537 W asymmetry analysis
2011-04-14 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* deltaR, deltaPhi, deltaEta now available in all combinations of
FourVector, FourMomentum, Vector3, doubles. They also accept jets
and particles as arguments now.
2011-04-13 David Grellscheid <david.grellscheid@durham.ac.uk>
* added ATLAS 8983313: 0-lepton BSM
2011-04-01 Andy Buckley <andy@insectnation.org>
* bin/rivet-mkanalysis: Don't try to download SPIRES or HepData
info if it's not a standard analysis (i.e. if the SPIRES ID is not
known), and make the default .info file validly parseable by YAML,
which was an unfortunate gotcha for anyone writing a first
analysis.
2011-03-31 Andy Buckley <andy@insectnation.org>
* bin/compare-histos: Write more appropriate ratio plot labels
when not comparing to data, and use the default make-plots labels
when comparing to data.
* bin/rivet-mkhtml: Adding a timestamp to the generated pages, and
a -t/--title option to allow setting the main HTML page title on
the command line: otherwise it becomes impossible to tell these
pages apart when you have a lot of them, except by URL!
2011-03-24 Andy Buckley <andy@insectnation.org>
* bin/aida2flat: Adding a -M option to *exclude* histograms whose
paths match a regex. Writing a negative lookahead regex with
positive matching was far too awkward!
2011-03-18 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* src/Core/AnalysisHandler.cc (AnalysisHandler::removeAnalysis):
Fixed strange shared pointer assignment that caused seg-fault.
2011-03-13 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* filling of functions works now in a more intuitive way (I hope).
2011-03-09 Andy Buckley <andy@insectnation.org>
* Version 1.5.0 release!
2011-03-08 Andy Buckley <andy@insectnation.org>
* Adding some extra checks for external packages in make-plots.
2011-03-07 Andy Buckley <andy@insectnation.org>
* Changing the accuracy of the beam energy checking to 1%, to make
the UI a bit more forgiving. It's still best to specify exactly the right
energy of course!
2011-03-01 Andy Buckley <andy@insectnation.org>
* Adding --no-plottitle to compare-histos (+ completion).
* Fixing segfaults in UA1_1990_S2044935 and UA5_1982_S875503.
* Bump ABI version numbers for 1.5.0 release.
* Use AnalysisInfo for storage of the NeedsCrossSection analysis flag.
* Allow field setting in AnalysisInfo.
2011-02-27 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Support LineStyle=dashdotted in make-plots
* New command line option --style for compare-histos. Options are
"default", "bw" and "talk".
* cleaner uninstall
2011-02-26 Andy Buckley <andy@insectnation.org>
* Changing internal storage and return type of Particle::pdgId()
to PdgId, and adding Particle::energy().
* Renaming Analysis::energies() as Analysis::requiredEnergies().
* Adding beam energies into beam consistency checking:
Analysis::isCompatible methods now also require the beam energies
to be provided.
* Removing long-deprecated AnalysisHandler::init() constructor and
AnalysisHandler::removeIncompatibleAnalyses() methods.
2011-02-25 Andy Buckley <andy@insectnation.org>
* Adding --disable-obsolete, which takes its value from the value
of --disable-preliminary by default.
* Replacing RivetUnvalidated and RivetPreliminary plugin libraries
with optionally-configured analysis contents in the
experiment-specific plugin libraries. This avoids issues with
making libraries rebuild consistently when sources were reassigned
between libraries.
2011-02-24 Andy Buckley <andy@insectnation.org>
* Changing analysis plugin registration to fall back through
available paths rather than have RIVET_ANALYSIS_PATH totally
override the built-in paths. The first analysis hook of a given
name to be found is now the one that's used: any duplicates found
will be warned about but unused. getAnalysisLibPaths() now returns
*all* the search paths, in keeping with the new search behaviour.
2011-02-22 Andy Buckley <andy@insectnation.org>
* Moving the definition of the MSG_* macros into the Logging.hh
header. They can't be used everywhere, though, as they depend on
the existence of a this->getLog() method in the call scope. This
move makes them available in e.g. AnalysisHandler and other bits
of framework other than projections and analyses.
* Adding a gentle print-out from the Rivet AnalysisHandler if
preliminary analyses are being used, and strengthening the current
warning if unvalidated analyses are used.
* Adding documentation about the validation "process" and
the (un)validated and preliminary analysis statuses.
* Adding the new RivetPreliminary analysis library, and the
corresponding --disable-preliminary configure flag. Analyses in
this library are subject to change names, histograms, reference
data values, etc. between releases: make sure you check any
dependences on these analyses when upgrading Rivet.
* Change the Python script ref data search behaviours to use Rivet
ref data by default where available, rather than requiring a -R
option. Where relevant, -R is still a valid option, to avoid
breaking legacy scripts, and there is a new --no-rivet-refs option
to turn the default searching *off*.
* Add the prepending and appending optional arguments to the path
searching functions. This will make it easier to combine the
search functions with user-supplied paths in Python scripts.
* Make make-plots killable!
* Adding Rivet version to top of run printout.
* Adding Run::crossSection() and printing out the cross-section in
pb at the end of a Rivet run.
2011-02-22 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Make lighthisto.py aware of 2D histograms
* Adding published versions of the CDF_2008 leading jets and DY
analyses, and marking the preliminary ones as "OBSOLETE".
2011-02-21 Andy Buckley <andy@insectnation.org>
* Adding PDF documentation for path searching and .info/.plot
files, and tidying overfull lines.
* Removing unneeded const declarations from various return by
value path and internal binning functions. Should not affect ABI
compatibility but will force recompilation of external packages
using the RivetPaths.hh and Utils.hh headers.
* Adding findAnalysis*File(fname) functions, to be used by Rivet
scripts and external programs to find files known to Rivet
according to Rivet's (newly standard) lookup rule.
* Changing search path function behaviour to always return *all*
search directories rather than overriding the built-in locations
if the environment variables are set.
2011-02-20 Andy Buckley <andy@insectnation.org>
* Adding the ATLAS 2011 transverse jet shapes analysis.
2011-02-18 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Support for transparency in make-plots
2011-02-18 Frank Siegert <frank.siegert@cern.ch>
* Added ATLAS prompt photon analysis ATLAS_2010_S8914702
2011-02-10 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Simple NOOP constructor for Thrust projection
* Add CMS event shape analysis. Data read off the plots. We
will get the final numbers when the paper is accepted by
the journal.
2011-02-10 Frank Siegert <frank.siegert@cern.ch>
* Add final version of ATLAS dijet azimuthal decorrelation
2011-02-10 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* remove ATLAS conf note analyses for which we have final data
* reshuffle histograms in ATLAS minbias analysis to match Hepdata
* small pT-cut fix in ATLAS track based UE analysis
2011-01-31 Andy Buckley <andy@insectnation.org>
* Doc tweaks and adding cmp-by-|p| functions for Jets, to match
those added by Hendrik for Particles.
* Don't sum photons around muons in the D0 2010 Z pT analysis.
2011-01-27 Andy Buckley <andy@insectnation.org>
* Adding ATLAS 2010 min bias and underlying event analyses and data.
2011-01-23 Andy Buckley <andy@insectnation.org>
* Make make-plots write out PDF rather than PS by default.
2011-01-12 Andy Buckley <andy@insectnation.org>
* Fix several rendering and comparison bugs in rivet-mkhtml.
* Allow make-plots to write into an existing directory, at the
user's own risk.
* Make rivet-mkhtml produce PDF-based output rather than PS by
default (most people want PDF these days). Can we do the same
change of default for make-plots?
* Add getAnalysisPlotPaths() function, and use it in compare-histos
* Use proper .info file search path function internally in AnalysisInfo::make.
2011-01-11 Andy Buckley <andy@insectnation.org>
* Clean up ATLAS dijet analysis.
2010-12-30 Andy Buckley <andy@insectnation.org>
* Adding a run timeout option, and small bug-fixes to the event
timeout handling, and making first event timeout work nicely with
the run timeout. Run timeout is intended to be used in conjunction
with timed batch token expiry, of the type that likes to make 0
byte AIDA files on LCG when Grid proxies time out.
2010-12-21 Andy Buckley <andy@insectnation.org>
* Fix the cuts in the CDF 1994 colour coherence analysis.
2010-12-19 Andy Buckley <andy@insectnation.org>
* Fixing CDF midpoint cone jet algorithm default construction to
have an overlap threshold of 0.5 rather than 0.75. This was
recommended by the FastJet manual, and noticed while adding the
ATLAS and CMS cones.
* Adding ATLAS and CMS old iterative cones as "official" FastJets
constructor options (they could always have been used by explicit
instantiation and attachment of a Fastjet plugin object).
* Removing defunct and unused ClosestJetShape projection.
2010-12-16 Andy Buckley <andy@insectnation.org>
* bin/compare-histos, pyext/lighthisto.py: Take ref paths from
rivet module API rather than getting the environment by hand.
* pyext/lighthisto.py: Only read .plot info from the first
matching file (speed-up compare-histos).
2010-12-14 Andy Buckley <andy@insectnation.org>
* Augmenting the physics vector functionality to make FourMomentum
support maths operators with the correct return type (FourMomentum
rather than FourVector).
2010-12-11 Andy Buckley <andy@insectnation.org>
* Adding a --event-timeout option to control the event timeout,
adding it to the completion script, and making sure that the init
time check is turned OFF once successful!
* Adding an 3600 second timeout for initialising an event file. If
it takes longer than (or anywhere close to) this long, chances are
that the event source is inactive for some reason (perhaps
accidentally unspecified and stdin is not active, or the event
generator has died at the other end of the pipe. The reason for
not making it something shorter is that e.g. Herwig++ or Sherpa
can have long initialisation times to set up the MPI handler or to
run the matrix element integration. An timeout after an hour is
still better than a batch job which runs for two days before you
realise that you forgot to generate any events!
2010-12-10 Andy Buckley <andy@insectnation.org>
* Fixing unbooked-histo segfault in UA1_1990_S2044935 at 63 GeV.
2010-12-08 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixes in ATLAS_2010_CONF_083, declaring it validated
* Added ATLAS_2010_CONF_046, only two plots are implemented.
The paper will be out soon, and we don't need the other plots
right now. Data is read off the plots in the note.
* New option "SmoothLine" for HISTOGRAM sections in make-plots
* Changed CustomTicks to CustomMajorTicks and added CustomMinorTicks
in make-plots.
2010-12-07 Andy Buckley <andy@insectnation.org>
* Update the documentation to explain this latest bump to path
lookup behaviours.
* Various improvements to existing path lookups. In particular,
the analysis lib path locations are added to the info and ref
paths to avoid having to set three variables when you have all
three file types in the same personal plugin directory.
* Adding setAnalysisLibPaths and addAnalysisLibPath
functions. rivet --analysis-path{,-append} now use these and work
correctly. Hurrah!
* Add --show-analyses as an alias for --show-analysis, following a
comment at the ATLAS tutorial.
2010-12-07 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Change LegendXPos behaviour in make-plots. Now the top left
corner of the legend is used as anchor point.
2010-12-03 Andy Buckley <andy@insectnation.org>
* 1.4.0 release.
* Add bin-skipping to compare-histos to avoid one use of
rivet-rmgaps (it's still needed for non-plotting post-processing
like Professor).
2010-12-03 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fix normalisation issues in UA5 and ALEPH analyses
2010-11-27 Andy Buckley <andy@insectnation.org>
* MathUtils.hh: Adding fuzzyGtrEquals and fuzzyLessEquals, and
tidying up the math utils collection a bit.
* CDF 1994 colour coherence analysis overhauled and
correction/norm factors fixed. Moved to VALIDATED status.
* Adding programmable completion for aida2flat and flat2aida.
* Improvements to programmable completion using the neat _filedir
completion shell function which I just discovered.
2010-11-26 Andy Buckley <andy@insectnation.org>
* Tweak to floating point inRange to use fuzzyEquals for CLOSED
interval equality comparisons.
* Some BibTeX generation improvements, and fixing the ATLAS dijet
BibTeX key.
* Resolution upgrade in PNG make-plots output.
* CDF_2005_S6217184.cc, CDF_2008_S7782535.cc: Updates to use the
new per-jet JetAlg interface (and some other fixes).
* JetAlg.cc: Changed the interface on request to return per-jet
rather than per-event jet shapes, with an extra jet index argument.
* MathUtils.hh: Adding index_between(...) function, which is handy
for working out which bin a value falls in, given a set of bin edges.
2010-11-25 Andy Buckley <andy@insectnation.org>
* Cmp.hh: Adding ASC/DESC (and ANTISORTED) as preferred
non-EQUIVALENT enum value synonyms over misleading
SORTED/UNSORTED.
* Change of rapidity scheme enum name to RapScheme
* Reworking JetShape a bit further: constructor args now avoid
inconsistencies (it was previously possible to define incompatible
range-ends and interval). Internal binning implementation also
reworked to use a vector of bin edges: the bin details are
available via the interface. The general jet pT cuts can be
applied via the JetShape constructor.
* MathUtils.hh: Adding linspace and logspace utility
functions. Useful for defining binnings.
* Adding more general cuts on jet pT and (pseudo)rapidity.
2010-11-11 Andy Buckley <andy@insectnation.org>
* Adding special handling of FourMomentum::mass() for computed
zero-mass vectors for which mass2 can go (very slightly) negative
due to numerical precision.
2010-11-10 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Adding ATLAS-CONF-2010-083 conference note. Data is read from plots.
When I run Pythia 6 the bins close to pi/2 are higher than in the note,
so I call this "unvalidated". But then ... the note doesn't specify
a tune or even just a version for the generators in the plots. Not even
if they used Pythia 6 or Pythia 8. Probably 6, since they mention AGILe.
2010-11-10 Andy Buckley <andy@insectnation.org>
* Adding a JetAlg::useInvisibles(bool) mechanism to allow ATLAS
jet studies to include neutrinos. Anyone who chooses to use this
mechanism had better be careful to remove hard neutrinos manually
in the provided FinalState object.
2010-11-09 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Adding ATLAS-CONF-2010-049 conference note. Data is read from plots.
Fragmentation functions look good, but I can't reproduce the MC lines
(or even the relative differences between them) in the jet cross-section
plots. So consider those unvalidated for now. Oh, and it seems ATLAS
screwed up the error bands in their ratio plots, too. They are
upside-down.
2010-11-07 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Adding ATLAS-CONF-2010-081 conference note. Data is read from plots.
2010-11-06 Andy Buckley <andy@insectnation.org>
* Deprecating the old JetShape projection and renaming to
ClosestJetShape: the algorithm has a tenuous relationship with
that actually used in the CDF (and ATLAS) jet shape analyses. CDF
analyses to be migrated to the new JetShape projection... and some
of that projection's features, design elements, etc. to be
finished off: we may as well take this opportunity to clear up
what was one of our nastiest pieces of code.
2010-11-05 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Adding ATLAS-CONF-2010-031 conference note. Data is read from plots.
2010-10-29 Andy Buckley <andy@insectnation.org>
* Making rivet-buildplugin use the same C++ compiler and CXXFLAGS
variable as used for the Rivet system build.
* Fixing NeutralFinalState projection to, erm, actually select
neutral particles (by Hendrik).
* Allow passing a general FinalState reference to the JetShape
projection, rather than requiring a VetoedFS.
2010-10-07 Andy Buckley <andy@insectnation.org>
* Adding a --with-root flag to rivet-buildplugin to add
root-config --libs flags to the plugin build command.
2010-09-24 Andy Buckley <andy@insectnation.org>
* Releasing as Rivet 1.3.0.
* Bundling underscore.sty to fix problems with running make-plots
on dat files generated by compare-histos from AIDA files with
underscores in their names.
2010-09-16 Andy Buckley <andy@insectnation.org>
* Fix error in N_effective definition for weighted profile errors.
2010-08-18 Andy Buckley <andy@insectnation.org>
* Adding MC_GENERIC analysis. NB. Frank Siegert also added MC_HJETS.
2010-08-03 Andy Buckley <andy@insectnation.org>
* Fixing compare-histos treatment of what is now a ref file, and
speeding things up... again. What a mess!
2010-08-02 Andy Buckley <andy@insectnation.org>
* Adding rivet-nopy: a super-simple Rivet C++ command line
interface which avoids Python to make profiling and debugging
easier.
* Adding graceful exception handling to the AnalysisHandler event
loop methods.
* Changing compare-histos behaviour to always show plots for which
there is at least one MC histo. The default behaviour should now
be the correct one in 99% of use cases.
2010-07-30 Andy Buckley <andy@insectnation.org>
* Merging in a fix for shared_ptrs not being compared for
insertion into a set based on raw pointer value.
2010-07-16 Andy Buckley <andy@insectnation.org>
* Adding an explicit library dependency declaration on libHepMC,
and hence removing the -lHepMC from the rivet-config --libs
output.
2010-07-14 Andy Buckley <andy@insectnation.org>
* Adding a manual section on use of Rivet (and AGILe) as
libraries, and how to use the -config scripts to aid compilation.
* FastJets projection now allows setting of a jet area definition,
plus a hacky mapping for getting the area-enabled cluster
sequence. Requested by Pavel Starovoitov & Paolo Francavilla.
* Lots of script updates in last two weeks!
2010-06-30 Andy Buckley <andy@insectnation.org>
* Minimising amount of Log class mapped into SWIG.
* Making Python ext build checks fail with error rather than
warning if it has been requested (or, rather, not explicitly
disabled).
2010-06-28 Andy Buckley <andy@insectnation.org>
* Converting rivet Python module to be a package, with the dlopen
flag setting etc. done around the SWIG generated core wrapper
module (rivet.rivetwrap).
* Requiring Python >= 2.4.0 in rivet scripts (and adding a Python
version checker function to rivet module)
* Adding --epspng option to make-plots (and converting to use subprocess.Popen).
2010-06-27 Andy Buckley <andy@insectnation.org>
* Converting JADE_OPAL analysis to use the fastjet
exclusive_ymerge_*max* function, rather than just
exclusive_ymerge: everything looks good now. It seems that fastjet
>= 2.4.2 is needed for this to work properly.
2010-06-24 Andy Buckley <andy@insectnation.org>
* Making rivet-buildplugin look in its own bin directory when
trying to find rivet-config.
2010-06-23 Andy Buckley <andy@insectnation.org>
* Adding protection and warning about numerical precision issues
in jet mass calculation/histogramming to the MC_JetAnalysis
analysis.
* Numerical precision improvement in calculation of
Vector4::mass2.
* Adding relative scale ratio plot flag to compare-histos
* Extended command completion to rivet-config, compare-histos, and
make-plots.
* Providing protected log messaging macros,
MSG_{TRACE,DEBUG,INFO,WARNING,ERROR} cf. Athena.
* Adding environment-aware functions for Rivet search path list access.
2010-06-21 Andy Buckley <andy@insectnation.org>
* Using .info file beam ID and energy info in HTML and LaTeX documentation.
* Using .info file beam ID and energy info in command-line printout.
* Fixing a couple of references to temporary variables in the
analysis beam info, which had been introduced during refactoring:
have reinstated reference-type returns as the more efficient
solution. This should not affect API compatibility.
* Making SWIG configure-time check include testing for
incompatibilities with the C++ compiler (re. the recurring _const_
char* literals issue).
* Various tweaks to scripts: make-plots and compare-histos
processes are now renamed (on Linux), rivet-config is avoided when
computing the Rivet version,and RIVET_REF_PATH is also set using
the rivet --analysis-path* flags. compare-histos now uses multiple
ref data paths for .aida file globbing.
* Hendrik changed VetoedFinalState comparison to always return
UNDEFINED if vetoing on the results of other FS projections is
being used. This is the only simple way to avoid problems
emanating from the remainingFinalState thing.
2010-06-19 Andy Buckley <andy@insectnation.org>
* Adding --analysis-path and --analysis-path-append command-line
flags to the rivet script, as a "persistent" way to set or extend
the RIVET_ANALYSIS_PATH variable.
* Changing -Q/-V script verbosity arguments to more standard
-q/-v, after Hendrik moaned about it ;)
* Small fix to TinyXML operator precendence: removes a warning,
and I think fixes a small bug.
* Adding plotinfo entries for new jet rapidity and jet mass plots
in MC_JetAnalysis derivatives.
* Moving MC_JetAnalysis base class into a new
libRivetAnalysisTools library, with analysis base class and helper
headers to be stored in the reinstated Rivet/Analyses include
directory.
2010-06-08 Andy Buckley <andy@insectnation.org>
* Removing check for CEDARSTD #define guard, since we no longer
compile against AGILe and don't have to be careful about
duplication.
* Moving crappy closest approach and decay significance functions
from Utils into SVertex, which is the only place they have ever
been used (and is itself almost entirely pointless).
* Overhauling particle ID <-> name system to clear up ambiguities
between enums, ints, particles and beams. There are no more enums,
although the names are still available as const static ints, and
names are now obtained via a singleton class which wraps an STL
map for name/ID lookups in both directions.
2010-05-18 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixing factor-of-2 bug in the error calculation when scaling
histograms.
* Fixing D0_2001_S4674421 analysis.
2010-05-11 Andy Buckley <andy@insectnation.org>
* Replacing TotalVisibleMomentum with MissingMomentum in analyses
and WFinder. Using vector ET rather than scalar ET in some places.
2010-05-07 Andy Buckley <andy@insectnation.org>
* Revamping the AnalysisHandler constructor and data writing, with
some LWH/AIDA mangling to bypass the stupid AIDA idea of having to
specify the sole output file and format when making the data
tree. Preferred AnalysisHandler constructor now takes only one arg
-- the runname -- and there is a new AH.writeData(outfile) method
to replace AH.commitData(). Doing this now to begin migration to
more flexible histogramming in the long term.
2010-04-21 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixing LaTeX problems (make-plots) on ancient machines, like lxplus.
2010-04-29 Andy Buckley <andy@insectnation.org>
* Fixing (I hope!) the treatment of weighted profile bin errors in LWH.
2010-04-21 Andy Buckley <andy@insectnation.org>
* Removing defunct and unused KtJets and Configuration classes.
* Hiding some internal details from Doxygen.
* Add @brief Doxygen comments to all analyses, projections and
core classes which were missing them.
2010-04-21 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* remove obsolete reference to InitialQuarks from DELPHI_2002
* fix normalisation in CDF_2000_S4155203
2010-04-20 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* bin/make-plots: real support for 2-dim histograms plotted as
colormaps, updated the documentation accordingly.
* fix misleading help comment in configure.ac
2010-04-08 Andy Buckley <andy@insectnation.org>
* bin/root2flat: Adding this little helper script, minimally
modified from one which Holger Schulz made for internal use in
ATLAS.
2010-04-05 Andy Buckley <andy@insectnation.org>
* Using spiresbib in rivet-mkanalysis: analysis templates made
with rivet-mkanalysis will now contain a SPIRES-dumped BibTeX key
and entry if possible!
* Adding BibKey and BibTeX entries to analysis metadata files, and
updating doc build to use them rather than the time-consuming
SPIRES screen-scraping. Added SPIRES BibTeX dumps to all analysis
metadata using new (uninstalled & unpackaged) doc/get-spires-data
script hack.
* Updating metadata files to add Energies, Beams and PtCuts
entries to all of them.
* Adding ToDo, NeedsCrossSection, and better treatment of Beams
and Energies entries in metadata files and in AnalysisInfo and
Analysis interfaces.
2010-04-03 Andy Buckley <andy@insectnation.org>
* Frank Siegert: Update of rivet-mkhtml to conform to improved
compare-histos.
* Frank Siegert: LWH output in precision-8 scientific notation, to
solve a binning precision problem... the first time weve noticed a
problem!
* Improved treatment of data/reference datasets and labels in
compare-histos.
* Rewrite of rivet-mkanalysis in Python to make way for neat
additions.
* Improving SWIG tests, since once again the user's biuld system
must include SWIG (no test to check that it's a 'good SWIG', since
the meaning of that depends on which compiler is being used and we
hope that the user system is consistent... evidence from Finkified
Macs and bloody SLC5 notwithstanding).
2010-03-23 Andy Buckley <andy@insectnation.org>
* Tag as patch release 1.2.1.
2010-03-22 Andy Buckley <andy@insectnation.org>
* General tidying of return arguments and intentionally unused
parameters to keep -Wextra happy (some complaints remain from
TinyXML, FastJet, and HepMC).
* Some extra bug fixes: in FastJets projection with explicit
plugin argument, removing muon veto cut on FoxWolframMoments.
* Adding UNUSED macro to help with places where compiler warnings
can't be helped.
* Turning on -Wextra warnings, and fixing some violations.
2010-03-21 Andy Buckley <andy@insectnation.org>
* Adding MissingMomentum projection, as replacement for ~all uses
of now-deprecated TotalVisibleMomentum projection.
* Fixing bug with TotalVisibleMomentum projection usage in MC_SUSY
analysis.
* Frank Siegert fixed major bug in pTmin param passing to FastJets
projection. D'oh: requires patch release.
2010-03-02 Andy Buckley <andy@insectnation.org>
* Tagging for 1.2.0 release... at last!
2010-03-01 Andy Buckley <andy@insectnation.org>
* Updates to manual, manual generation scripts, analysis info etc.
* Add HepData URL to metadata print-out with rivet --show-analysis
* Fix average Et plot in UA1 analysis to only apply to the tracker
acceptance (but to include neutral particle contributions,
i.e. the region of the calorimeter in the tracker acceptance).
* Use Et rather than pT in filling the scalar Et measure in
TotalVisibleMomentum.
* Fixes to UA1 normalisation (which is rather funny in the paper).
2010-02-26 Andy Buckley <andy@insectnation.org>
* Update WFinder to not place cuts and other restrictions on the
neutrino.
2010-02-11 Andy Buckley <andy@insectnation.org>
* Change analysis loader behaviour to use ONLY RIVET_ANALYSIS_PATH
locations if set, otherwise use ONLY the standard Rivet analysis
install path. Should only impact users of personal plugin
analyses, who should now explicitly set RIVET_ANALYSIS_PATH to
load their analysis... and who can now create personal versions of
standard analyses without getting an error message about duplicate
loading.
2010-01-15 Andy Buckley <andy@insectnation.org>
* Add tests for "stable" heavy flavour hadrons in jets (rather
than just testing for c/b hadrons in the ancestor lists of stable
jet constituents)
2009-12-23 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* New option "RatioPlotMode=deviation" in make-plots.
2009-12-14 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* New option "MainPlot" in make-plots. For people who only want
the ratio plot and nothing else.
* New option "ConnectGaps" in make-plots. Set to 1 if you
want to connect gaps in histograms with a line when ErrorBars=0.
Works both in PLOT and in HISTOGRAM sections.
* Eliminated global variables for coordinates in make-plots and
enabled multithreading.
2009-12-14 Andy Buckley <andy@insectnation.org>
* AnalysisHandler::execute now calls AnalysisHandler::init(event)
if it has not yet been initialised.
* Adding more beam configuration features to Beam and
AnalysisHandler: the setRunBeams(...) methods on the latter now
allows a beam configuration for the run to be specified without
using the Run class.
2009-12-11 Andy Buckley <andy@insectnation.org>
* Removing use of PVertex from few remaining analyses. Still used
by SVertex, which is itself hardly used and could maybe be
removed...
2009-12-10 Andy Buckley <andy@insectnation.org>
* Updating JADE_OPAL to do the histo booking in init(), since
sqrtS() is now available at that stage.
* Renaming and slightly re-engineering all MC_*_* analyses to not
be collider-specific (now the Analysis::sqrtS/beams()) methods
mean that histograms can be dynamically binned.
* Creating RivetUnvalidated.so plugin library for unvalidated
analyses. Unvalidated analyses now need to be explicitly enabled
with a --enable-unvalidated flag on the configure script.
* Various min bias analyses updated and validated.
2009-12-10 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Propagate SPECIAL and HISTOGRAM sections from .plot files
through compare-histos
* STAR_2006_S6860818: <pT> vs particle mass, validate analysis
2009-12-04 Andy Buckley <andy@insectnation.org>
* Use scaling rather than normalising in DELPHI_1996: this is
generally desirable, since normalizing to 1 for 1/sig dsig/dx
observables isn't correct if any events fall outside the histo
bounds.
* Many fixes to OPAL_2004.
* Improved Hemispheres interface to remove unnecessary consts on
returned doubles, and to also return non-squared versions
of (scaled) hemisphere masses.
* Add "make pyclean" make target at the top level to make it
easier for developers to clean their Python module build when the
API is extended.
* Identify use of unvalidated analyses with a warning message at
runtime.
* Providing Analysis::sqrtS() and Analysis::beams(), and making
sure they're available by the time the init methods are called.
2009-12-02 Andy Buckley <andy@insectnation.org>
* Adding passing of first event sqrt(s) and beams to analysis handler.
* Restructuring running to only use one HepMC input file (no-one
was using multiple ones, right?) and to break down the Run class
to cleanly separate the init and event loop phases. End of file is
now neater.
2009-12-01 Andy Buckley <andy@insectnation.org>
* Adding parsing of beam types and pairs of energies from YAML.
2009-12-01 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixing trigger efficiency in CDF_2009_S8233977
2009-11-30 Andy Buckley <andy@insectnation.org>
* Using shared pointers to make I/O object memory management
neater and less error-prone.
* Adding crossSectionPerEvent() method [==
crossSection()/sumOfWeights()] to Analysis. Useful for histogram
scaling since numerator of sumW_passed/sumW_total (to calculate
pass-cuts xsec) is cancelled by dividing histo by sumW_passed.
* Clean-up of Particle class and provision of inline PID::
functions which take a Particle as an argument to avoid having to
explicitly call the Particle::pdgId() method.
2009-11-30 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixing division by zero in Profile1D bin errors for
bins with just a single entry.
2009-11-24 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* First working version of STAR_2006_S6860818
2009-11-23 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Adding missing CDF_2001_S4751469 plots to uemerge
* New "ShowZero" option in make-plots
* Improving lots of plot defaults
* Fixing typos / non-existing bins in CDF_2001_S4751469 and
CDF_2004_S5839831 reference data
2009-11-19 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixing our compare() for doubles.
2009-11-17 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Zeroth version of STAR_2006_S6860818 analysis (identified
strange particles). Not working yet for unstable particles.
2009-11-11 Andy Buckley <andy@insectnation.org>
* Adding separate jet-oriented and photon-oriented observables to
MC PHOTONJETUE analysis.
* Bug fix in MC leading jets analysis, and general tidying of
leading jet analyses to insert units, etc. (should not affect any
current results)
2009-11-10 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixing last issues in STAR_2006_S6500200 and setting it to
VALIDATED.
* Noramlise STAR_2006_S6870392 to cross-section
2009-11-09 Andy Buckley <andy@insectnation.org>
* Overhaul of jet caching and ParticleBase interface.
* Adding lists of analyses' histograms (obtained by scanning the
plot info files) to the LaTeX documentation.
2009-11-07 Andy Buckley <andy@insectnation.org>
* Adding checking system to ensure that Projections aren't
registered before the init phase of analyses.
* Now that the ProjHandler isn't full of defunct pointers (which
tend to coincidentally point to *new* Projection pointers rather
than undefined memory, hence it wasn't noticed until recently!),
use of a duplicate projection name is now banned with a helpful
message at runtime.
* (Huge) overhaul of ProjectionHandler system to use shared_ptr:
projections are now deleted much more efficiently, naturally
cleaning themselves out of the central repository as they go out
of scope.
2009-11-06 Andy Buckley <andy@insectnation.org>
* Adding Cmp<double> specialisation, using fuzzyEquals().
2009-11-05 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixing histogram division code.
2009-11-04 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* New analysis STAR_2006_S6500200 (pion and proton pT spectra in
pp collisions at 200 GeV). It is still unclear if they used a cut
in rapidity or pseudorapidity, thus the analysis is declared
"UNDER DEVELOPMENT" and "DO NOT USE".
* Fixing compare() in NeutralFinalState and MergedFinalState
2009-11-04 Andy Buckley <andy@insectnation.org>
* Adding consistence checking on beam ID and sqrt(s) vs. those
from first event.
2009-11-03 Andy Buckley <andy@insectnation.org>
* Adding more assertion checks to linear algebra testing.
2009-11-02 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixing normalisation issue with stacked histograms in
make-plots.
2009-10-30 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* CDF_2009_S8233977: Updating data and axes labels to match final
paper. Normalise to cross-section instead of data.
2009-10-23 Andy Buckley <andy@insectnation.org>
* Fixing Cheese-3 plot in CDF 2004... at last!
2009-10-23 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fix muon veto in CDF_1994_S2952106, CDF_2005_S6217184,
CDF_2008_S7782535, and D0_2004_S5992206
2009-10-19 Andy Buckley <andy@insectnation.org>
* Adding analysis info files for MC SUSY and PHOTONJETUE analyses.
* Adding MC UE analysis in photon+jet events.
2009-10-19 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Adding new NeutralFinalState projection. Note that this final
state takes E_T instead of p_T as argument (makes more sense for
neutral particles). The compare() method does not yet work as
expected (E_T comparison still missing).
* Adding new MergedFinalState projection. This merges two final
states, removing duplicate particles. Duplicates are identified by
looking at the genParticle(), so users need to take care of any
manually added particles themselves.
* Fixing most open issues with the STAR_2009_UE_HELEN analysis.
There is only one question left, regarding the away region.
* Set the default split-merge value for SISCone in our FastJets
projection to the recommended (but not Fastjet-default!) value of
0.75.
2009-10-17 Andy Buckley <andy@insectnation.org>
* Adding parsing of units in cross-sections passed to the "-x"
flag, i.e. "-x 101 mb" is parsed internally into 1.01e11 pb.
2009-10-16 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Disabling DELPHI_2003_WUD_03_11 in the Makefiles, since I don't
trust the data.
* Getting STAR_2009_UE_HELEN to work.
2009-10-04 Andy Buckley <andy@insectnation.org>
* Adding triggers and other tidying to (still unvalidated)
UA1_1990 analysis.
* Fixing definition of UA5 trigger to not be intrinscally
different for pp and ppbar: this is corrected for (although it
takes some readng to work this out) in the 1982 paper, which I
think is the only one to compare the two modes.
* Moving projection setup and registration into init() method for
remaining analyses.
* Adding trigger implementations as projections for CDF Runs 0 &
1, and for UA5.
2009-10-01 Andy Buckley <andy.buckley@cern.ch>
* Moving projection setup and registration into init() method for
analyses from ALEPH, CDF and the MC_ group.
* Adding generic SUSY validation analysis, based on plots used in
ATLAS Herwig++ validation.
* Adding sorted particle accessors to FinalState (cf. JetAlg).
2009-09-29 Andy Buckley <andy@insectnation.org>
* Adding optional use of args as regex match expressions with
-l/--list-analyses.
2009-09-03 Andy Buckley <andy.buckley@cern.ch>
* Passing GSL include path to compiler, since its absence was
breaking builds on systems with no GSL installation in a standard
location (such as SLC5, for some mysterious reason!)
* Removing lib extension passing to compiler from the configure
script, because Macs and Linux now both use .so extensions for the
plugin analysis modules.
2009-09-02 Andy Buckley <andy@insectnation.org>
* Adding analysis info file path search with RIVET_DATA_PATH
variable (and using this to fix doc build.)
* Improvements to AnalysisLoader path search.
* Moving analysis sources back into single directory, after a
proletarian uprising ;)
2009-09-01 Andy Buckley <andy@insectnation.org>
* Adding WFinder and WAnalysis, based on Z proj and analysis, with
some tidying of the Z code.
* ClusteredPhotons now uses an IdentifiedFS to pick the photons to
be looped over, and only clusters photons around *charged* signal
particles.
2009-08-31 Andy Buckley <andy@insectnation.org>
* Splitting analyses by directory, to make it easier to disable
building of particular analysis group plugin libs.
* Removing/merging headers for all analyses except for the special
MC_JetAnalysis base class.
* Exit with an error message if addProjection is used twice from
the same parent with distinct projections.
2009-08-28 Andy Buckley <andy@insectnation.org>
* Changed naming convention for analysis plugin libraries, since
the loader has changed so much: they must now *start* with the
word "Rivet" (i.e. no lib prefix).
* Split standard plugin analyses into several plugin libraries:
these will eventually move into separate subdirs for extra build
convenience.
* Started merging analysis headers into the source files, now that
we can (the plugin hooks previously forbade this).
* Replacement of analysis loader system with a new one based on
ideas from ThePEG, which uses dlopen-time instantiation of
templated global variables to reduce boilerplate plugin hooks to
one line in analyses.
2009-07-14 Frank Siegert <frank.siegert@durham.ac.uk>
* Replacing in-source histo-booking metadata with .plot files.
2009-07-14 Andy Buckley <andy@insectnation.org>
* Making Python wrapper files copy into place based on bundled
versions for each active HepMC interface (2.3, 2.4 & 2.5), using a
new HepMC version detector test in configure.
* Adding YAML metadata files and parser, removing same metadata
from the analysis classes' source headers.
2009-07-07 Andy Buckley <andy@insectnation.org>
* Adding Jet::hadronicEnergy()
* Adding VisibleFinalState and automatically using it in JetAlg
projections.
* Adding YAML parser for new metadata (and eventually ref data)
files.
2009-07-02 Andy Buckley <andy@insectnation.org>
* Adding Jet::neutralEnergy() (and Jet::totalEnergy() for
convenience/symmetry).
2009-06-25 Andy Buckley <andy@insectnation.org>
* Tidying and small efficiency improvements in CDF_2008_S7541902
W+jets analysis (remove unneeded second stage of jet storing,
sorting the jets twice, using foreach, etc.).
2009-06-24 Andy Buckley <andy@insectnation.org>
* Fixing Jet's containsBottom and containsCharm methods, since B
hadrons are not necessarily to be found in the final
state. Discovered at the same time that HepMC::GenParticle defines
a massively unhelpful copy constructor that actually loses the
tree information; it would be better to hide it entirely!
* Adding RivetHepMC.hh, which defines container-type accessors to
HepMC particles and vertices, making it possible to use Boost
foreach and hence avoiding the usual huge boilerplate for-loops.
2009-06-11 Andy Buckley <andy@insectnation.org>
* Adding --disable-pdfmanual option, to make the bootstrap a bit
more robust.
* Re-enabling D0IL in FastJets: adding 10^-10 to the pTmin removes
the numerical instability!
* Fixing CDF_2004 min/max cone analysis to use calo jets for the
leading jet Et binning. Thanks to Markus Warsinsky
for (re)discovering this bug: I was sure it had been fixed. I'm
optimistic that this will fix the main distributions, although
Swiss Cheese "minus 3" is still likely to be broken. Early tests
look okay, but it'll take more stats before we can remove the "do
not trust" sign.
2009-06-10 Andy Buckley <andy@insectnation.org>
* Providing "calc" methods so that Thrust and Sphericity
projections can be used as calculators without having to use the
projecting/caching system.
2009-06-09 Andy Buckley <andy@insectnation.org>
* 1.1.3 release!
* More doc building and SWIG robustness tweaks.
2009-06-07 Andy Buckley <andy@insectnation.org>
* Make doc build from metadata work even before the library is
installed.
2009-06-07 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fix phi rotation in CDF_2008_LEADINGJETS.
2009-06-07 Andy Buckley <andy@insectnation.org>
* Disabling D0 IL midpoint cone (using CDF modpoint instead),
since there seems to be a crashing bug in FastJet's
implementation: we can't release that way, since ~no D0 analyses
will run.
2009-06-03 Andy Buckley <andy@insectnation.org>
* Putting SWIG-generated source files under SVN control to make
life easier for people who we advise to check out the SVN head
version, but who don't have a sufficiently modern copy of SWIG to
* Adding the --disable-analyses option, for people who just want
to use Rivet as a framework for their own analyses.
* Enabling HepMC cross-section reading, now that HepMC 2.5.0 has
been released.
2009-05-23 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Using gsl-config to locate libgsl
* Fix the paths for linking such that our own libraries are found
before any system libraries, e.g. for the case that there is an
outdated fastjet version installed on the system while we want to
use our own up-to-date version.
* Change dmerge to ymerge in the e+e- analyses using JADE or
DURHAM from fastjet. That's what it is called in fastjet-2.4 now.
2009-05-18 Andy Buckley <andy@insectnation.org>
* Adding use of gsl-config in configure script.
2009-05-16 Andy Buckley <andy@insectnation.org>
* Removing argument to vetoEvent macro, since no weight
subtraction is now needed. It's now just an annotated return, with
built-in debug log message.
* Adding an "open" FinalState, which is only calculated once per
even, then used by all other FSes, avoiding the loop over
non-status 1 particles.
2009-05-15 Andy Buckley <andy@insectnation.org>
* Removing incorrect setting of DPS x-errs in CDF_2008 jet shape
analysis: the DPS autobooking already gets this bit right.
* Using Jet rather than FastJet::PseudoJet where possible, as it
means that the phi ranges match up nicely between Particle and the
Jet object. The FastJet objects are only really needed if you want
to do detailed things like look at split/merge scales for
e.g. diff jet rates or "y-split" analyses.
* Tidying and debugging CDF jet shape analyses and jet shape
plugin... ongoing, but I think I've found at least one real bug,
plus a lot of stuff that can be done a lot more nicely.
* Fully removing deprecated math functions and updating affected
analyses.
2009-05-14 Andy Buckley <andy@insectnation.org>
* Removing redundant rotation in DISKinematics... this was a
legacy of Peter using theta rather than pi-theta in his rotation.
* Adding convenience phi, rho, eta, theta, and perp,perp2 methods
to the 3 and 4 vector classes.
2009-05-12 Andy Buckley <andy@insectnation.org>
* Adding event auto-rotation for events with one proton... more
complete approach?
2009-05-09 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Renaming CDF_2008_NOTE_9337 to CDF_2009_S8233977.
* Numerous small bug fixes in ALEPH_1996_S3486095.
* Adding data for one of the Rick-Field-style STAR UE analyses.
2009-05-08 Andy Buckley <andy@insectnation.org>
* Adding rivet-mkanalysis script, to make generating new analysis
source templates easier.
2009-05-07 Andy Buckley <andy@insectnation.org>
* Adding null vector check to Vector3::azimuthalAngle().
* Fixing definition of HCM/Breit frames in DISKinematics, and
adding asserts to check that the transformation is doing what it
should.
2009-05-05 Andy Buckley <andy@insectnation.org>
* Removing eta and Et cuts from CDF 2000 Z pT analysis, based on
our reading of the paper, and converting most of the analysis to a
call of the ZFinder projection.
2009-05-05 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Support non-default seed_threshold in CDF cone jet algorithms.
* New analyses STAR_2006_S6870392 and STAR_2008_S7993412. In
STAR_2008_S7993412 only the first distribution is filled at the
moment. STAR_2006_S6870392 is normalised to data instead of the
Monte Carlo cross-section, since we don't have that available in
the HepMC stream yet.
2009-05-05 Andy Buckley <andy@insectnation.org>
* Changing Event wrapper to copy whole GenEvents rather than
pointers, use std units if supported in HepMC, and run a
placeholder function for event auto-orientation.
2009-04-28 Andy Buckley <andy@insectnation.org>
* Removing inclusion of IsolationTools header by analyses that
aren't actually using the isolation tools... which is all of
them. Leaving the isolation tools in place for now, as there might
still be use cases for them and there's quite a lot of code there
that deserves a second chance to be used!
2009-04-24 Andy Buckley <andy@insectnation.org>
* Deleting Rivet implementations of TrackJet and D0ILConeJets: the
code from these has now been incorporated into FastJet 2.4.0.
* Removed all mentions of the FastJet JADE patch and the HAVE_JADE
preprocessor macro.
* Bug fix to D0_2008_S6879055 to ensure that cuts compare to both
electron and positron momenta (was just comparing against
electrons, twice, probably thanks to the miracle of cut and
paste).
* Converting all D0 IL Cone jets to use FastJets. Involved tidying
D0_2004 jet azimuthal decorrelation analysis and D0_2008_S6879055
as part of migration away from using the getLorentzJets method,
and removing the D0ILConeJets header from quite a few analyses
that weren't using it at all.
* Updating CDF 2001 to use FastJets in place of TrackJet, and
adding axis labels to its plots.
* Note that ZEUS_2001_S4815815 uses the wrong jet definition: it
should be a cone but curently uses kT.
* Fixing CDF_2005_S6217184 to use correct (midpoint, R=0.7) jet
definition. That this was using a kT definition with R=1.0 was
only made obvious when the default FastJets constructor was
removed.
* Removing FastJets default constructor: since there are now
several good (IRC safe) jet definitions available, there is no
obvious safe default and analyses should have to specify which
they use.
* Moving FastJets constructors into implementation file to reduce
recompilation dependencies, and adding new plugins.
* Ensuring that axis labels actually get written to the output
data file.
2009-04-22 Andy Buckley <andy@insectnation.org>
* Adding explicit FastJet CDF jet alg overlap_threshold
constructor param values, since the default value from 2.3.x is
now removed in version 2.4.0.
* Removing use of HepMC ThreeVector::mag method (in one place
only) since this has been removed in version 2.5.0b.
* Fix to hepmc.i (included by rivet.i) to ignore new HepMC 2.5.0b
GenEvent stream operator.
2009-04-21 Andy Buckley <andy@insectnation.org>
* Dependency on FastJet now requires version 2.4.0 or later. Jade
algorithm is now native.
* Moving all analysis constructors and Projection headers from the
analysis header files into their .cc implementation files, cutting
header dependencies.
* Removing AIDA headers: now using LWH headers only, with
enhancement to use axis labels. This facility is now used by the
histo booking routines, and calling the booking function versions
which don't specify axis labels will result in a runtime warning.
2009-04-07 Andy Buckley <andy@insectnation.org>
* Adding $(DESTDIR) prefix to call to Python module "setup.py
install"
* Moving HepMC SWIG mappings into Python Rivet module for now:
seems to work-around the SL type-mapping bug.
2009-04-03 Andy Buckley <andy@insectnation.org>
* Adding MC analysis for LHC UE: higher-pT replica of Tevatron
2008 leading jets study.
* Adding CDF_1990 pseudorapidity analysis.
* Moving CDF_2001 constructor into implementation file.
* Cleaning up CDF_2008_LEADINGJETS a bit, e.g. using foreach
loops.
* Adding function interface for specifying axis labels in histo
bookings. Currently has no effect, since AIDA doesn't seem to have
a mechanism for axis labels. It really is a piece of crap.
2009-03-18 Andy Buckley <andy@insectnation.org>
* Adding docs "make upload" and other tweaks to make the doc files
fit in with the Rivet website.
* Improving LaTex docs to show email addresses in printable form
and to group analyses by collider or other metadata.
* Adding doc script to include run info in LaTeX docs, and to make
HTML docs.
* Removing WZandh projection, which wasn't generator independent
and whose sole usage was already replaced by ZFinder.
* Improvements to constructors of ZFinder and InvMassFS.
* Changing ExampleTree to use real FS-based Z finding.
2009-03-16 Andy Buckley <andy@insectnation.org>
* Allow the -H histo file spec to give a full name if wanted. If
it doesn't end in the desired extension, it will be added.
* Adding --runname option (and API elements) to choose a run name
to be prepended as a "top level directory" in histo paths. An
empty value results in no extra TLD.
2009-03-06 Andy Buckley <andy@insectnation.org>
* Adding R=0.2 photon clustering to the electrons in the CDF 2000
Z pT analysis.
2009-03-04 Andy Buckley <andy@insectnation.org>
* Fixing use of fastjet-config to not use the user's PATH
variable.
* Fixing SWIG type table for HepMC object interchange.
2009-02-20 Andy Buckley <andy@insectnation.org>
* Adding use of new metadata in command line analysis querying
with the rivet command, and in building the PDF Rivet manual.
* Adding extended metadata methods to the Analysis interface and
the Python wrapper. All standard analyses comply with this new
interface.
2009-02-19 Andy Buckley <andy@insectnation.org>
* Adding usefully-scoped config headers, a Rivet::version()
function which uses them, and installing the generated headers to
fix "external" builds against an installed copy of Rivet. The
version() function has been added to the Python wrapper.
2009-02-05 Andy Buckley <andy@insectnation.org>
* Removing ROOT dependency and linking. Woo! There's no need for
this now, because the front-end accepts no histo format switch and
we'll just use aida2root for output conversions. Simpler this way,
and it avoids about half of our compilation bug reports from 32/64
bit ROOT build confusions.
2009-02-04 Andy Buckley <andy@insectnation.org>
* Adding automatic generation of LaTeX manual entries for the
standard analyses.
2009-01-20 Andy Buckley <andy@insectnation.org>
* Removing RivetGun and TCLAP source files!
2009-01-19 Andy Buckley <andy@insectnation.org>
* Added psyco Python optimiser to rivet, make-plots and
compare-histos.
* bin/aida2root: Added "-" -> "_" mangling, following requests.
2009-01-17 Andy Buckley <andy@insectnation.org>
* 1.1.2 release.
2009-01-15 Andy Buckley <andy@insectnation.org>
* Converting Python build system to bundle SWIG output in tarball.
2009-01-14 Andy Buckley <andy@insectnation.org>
* Converting AIDA/LWH divide function to return a DPS so that bin
width factors don't get all screwed up. Analyses adapted to use
the new division operation (a DPS/DPS divide would also be
nice... but can wait for YODA).
2009-01-06 Andy Buckley <andy@insectnation.org>
* bin/make-plots: Added --png option for making PNG output files,
using 'convert' (after making a PDF --- it's a bit messy)
* bin/make-plots: Added --eps option for output filtering through
ps2eps.
2009-01-05 Andy Buckley <andy@insectnation.org>
* Python: reworking Python extension build to use distutils and
newer m4 Python macros. Probably breaks distcheck but is otherwise
more robust and platform independent (i.e. it should now work on
Macs).
2008-12-19 Andy Buckley <andy@insectnation.org>
* make-plots: Multi-threaded make-plots and cleaned up the LaTeX
building a bit (necessary to remove the implicit single global
state).
2008-12-18 Andy Buckley <andy@insectnation.org>
* make-plots: Made LaTeX run in no-stop mode.
* compare-histos: Updated to use a nicer labelling syntax on the
command line and to successfully build MC-MC plots.
2008-12-16 Andy Buckley <andy@insectnation.org>
* Made LWH bin edge comparisons safe against numerical errors.
* Added Particle comparison functions for sorting.
* Removing most bad things from ExampleTree and tidying up. Marked
WZandh projection for removal.
2008-12-03 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added the two missing observables to the CDF_2008_NOTE_9337 analysis,
i.e. track pT and sum(ET). There is a small difference between our MC
output and the MC plots of the analysis' author, we're still waiting
for the author's comments.
2008-12-02 Andy Buckley <andy@insectnation.org>
* Overloading use of a std::set in the interface, since the
version of SWIG on Sci Linux doesn't have a predefined mapping for
STL sets.
2008-12-02 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixed uemerge. The output was seriously broken by a single line
of debug information in fillAbove(). Also changed uemerge output
to exponential notation.
* Unified ref and mc histos in compare-histos. Histos with one
bin are plotted linear. Option for disabling the ratio plot.
Several fixes for labels, legends, output directories, ...
* Changed rivetgun's fallback directory for parameter files to
$PREFIX/share/AGILe, since that's where the steering files now are.
* Running aida2flat in split mode now produces make-plots compatible
dat-files for direct plotting.
2008-11-28 Andy Buckley <andy@insectnation.org>
* Replaced binreloc with an upgraded and symbol-independent copy.
2008-11-25 Andy Buckley <andy@insectnation.org>
* Added searching of $RIVET_REF_PATH for AIDA reference data
files.
2008-11-24 Andy Buckley <andy@insectnation.org>
* Removing "get"s and other obsfucated syntax from
ProjectionApplier (Projection and Analysis) interfaces.
2008-11-21 Andy Buckley <andy@insectnation.org>
* Using new "global" Jet and V4 sorting functors in
TrackJet. Looks like there was a sorting direction problem before...
* Verbose mode with --list-analyses now shows descriptions as well
as analysis names.
* Moved data/Rivet to data/refdata and moved data/RivetGun
contents to AGILe (since generator steering is no longer a Rivet
thing)
* Added unchecked ratio plots to D0 Run II jet + photon analysis.
* Added D0 inclusive photon analysis.
* Added D0 Z rapidity analysis.
* Tidied up constructor interface and projection chain
implementation of InvMassFinalState.
* Added ~complete set of Jet and FourMomentum sorting functors.
2008-11-20 Andy Buckley <andy@insectnation.org>
* Added IdentifiedFinalState.
* Moved a lot of TrackJet and Jet code into .cc files.
* Fixed a caching bug in Jet: cache flag resets should never be
conditional, since they are then sensitive to initialisation
errors.
* Added quark enum values to ParticleName.
* Rationalised JetAlg interfaces somewhat, with "size()" and
"jets()" methods in the interface.
* Added D0 W charge asymmetry and D0 inclusive jets analyses.
2008-11-18 Andy Buckley <andy@insectnation.org>
* Adding D0 inclusive Z pT shape analysis.
* Added D0 Z + jet pT and photon + jet pT spectrum analyses.
* Lots of tidying up of particle, event, particle name etc.
* Now the first event is used to detect the beam type and remove
incompatible analyses.
2008-11-17 Andy Buckley <andy@insectnation.org>
* Added bash completion for rivetgun.
* Starting to provide stand-alone call methods on projections so
they can be used without the caching infrastructure. This could
also be handy for unit testing.
* Adding functionality (sorting function and built-in sorting
schemes) to the JetAlg interface.
2008-11-10 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fix floating point number output format in aida2flat and flat2aida
* Added CDF_2002_S4796047: CDF Run-I charged multiplicity distribution
* Renamed CDF_2008_MINBIAS to CDF_2008_NOTE_9337, since the
note is publicly available now.
2008-11-10 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added DELPHI_2003_WUD_03_11: Delphi 4-jet angular distributions.
There is still a problem with the analysis, so don't use it yet.
But I need to commit the code because my laptop is broken ...
2008-11-06 Andy Buckley <andy@insectnation.org>
* Code review: lots of tidying up of projections and analyses.
* Fixes for compatibility with the LLVM C & C++ compiler.
* Change of Particle interface to remove "get"-prefixed method
names.
2008-11-05 Andy Buckley <andy@insectnation.org>
* Adding ability to query analysis metadata from the command line.
* Example of a plugin analyis now in plugindemo, with a make check
test to make sure that the plugin analysis is recognised by the
command line "rivet" tool.
* GCC 4.3 fix to mat-vec tests.
2008-11-04 Andy Buckley <andy@insectnation.org>
* Adding native logger control from Python interface.
2008-11-03 Andy Buckley <andy@insectnation.org>
* Adding bash_completion for rivet executable.
2008-10-31 Andy Buckley <andy@insectnation.org>
* Clean-up of histo titles and analysis code review.
* Added momentum construction functions from FastJet PseudoJets.
2008-10-28 Andy Buckley <andy@insectnation.org>
* Auto-booking of histograms with a name, rather than the HepData
ID 3-tuple is now possible.
* Fix in CDF 2001 pT spectra to get the normalisations to depend
on the pT_lead cutoff.
2008-10-23 Andy Buckley <andy@insectnation.org>
* rivet handles signals neatly, as for rivetgun, so that premature
killing of the analysis process will still result in an analysis
file.
* rivet now accepts cross-section as a command line argument and,
if it is missing and is required, will prompt the user for it
interactively.
2008-10-22 Andy Buckley <andy@insectnation.org>
* rivet (Python interface) now can list analyses, check when
adding analyses that the given names are valid, specify histo file
name, and provide sensibly graded event number logging.
2008-10-20 Andy Buckley <andy@insectnation.org>
* Corrections to CDF 2004 analysis based on correspondance with
Joey Huston. M bias dbns now use whole event within |eta| < 0.7,
and Cheese plots aren't filled at all if there are insufficient
jets (and the correct ETlead is used).
2008-10-08 Andy Buckley <andy@insectnation.org>
* Added AnalysisHandler::commitData() method, to allow the Python
interface to write out a histo file without having to know
anything about the histogramming API.
* Reduced SWIG interface file to just map a subset of Analysis and
AnalysisHandler functionality. This will be the basis for a new
command line interface.
2008-10-06 Andy Buckley <andy@insectnation.org>
* Converted FastJets plugin to use a Boost shared_pointer to the
cached ClusterSequence. The nullness of the pointer is now used to
indicate an empty tracks (and hence jets) set. Once FastJet
natively support empty CSeqs, we can rewrite this a bit more
neatly and ditch the shared_ptr.
2008-10-02 Andy Buckley <andy@insectnation.org>
* The CDF_2004 (Acosta) data file now includes the full range of
pT for the min bias data at both 630 and 1800 GeV. Previously,
only the small low-pT insert plot had been entered into HepData.
2008-09-30 Andy Buckley <andy@insectnation.org>
* Lots of updates to CDF_2004 (Acosta) UE analysis, including
sorting jets by E rather than Et, and factorising transverse cone
code into a function so that it can be called with a random
"leading jet" in min bias mode. Min bias histos are now being
trial-filled just with tracks in the transverse cones, since the
paper is very unclear on this.
* Discovered a serious caching problem in FastJets projection when
an empty tracks vector is passed from the
FinalState. Unfortunately, FastJet provides no API way to solve
the problem, so we'll have to report this upstream. For now, we're
solving this for CDF_2004 by explicitly vetoing events with no
tracks.
* Added Doxygen to the build with target "dox"
* Moved detection of whether cross-section information is needed
into the AnalysisHandler, with dynamic computation by scanning
contained analyses.
* Improved robustness of event reading to detect properly when the
input file is smaller than expected.
2008-09-29 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* New analysis: CDF_2000_S4155203
2008-09-23 Andy Buckley <andy@insectnation.org>
* rivetgun can now be built and run without AGILe. Based on a
patch by Frank Siegert.
2008-09-23 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Some preliminary numbers for the CDF_2008_LEADINGJETS analysis
(only transverse region and not all observables. But all we have now.)
2008-09-17 Andy Buckley <andy@insectnation.org>
* Breaking up the mammoth "generate" function, to make Python
mapping easier, among other reasons.
* Added if-zero-return-zero checking to angle mapping functions,
to avoid problems where 1e-19 gets mapped on to 2 pi and then
fails boundary asserts.
* Added HistoHandler singleton class, which will be a central
repository for holding analyses' histogram objects to be accessed
via a user-chosen name.
2008-08-26 Andy Buckley <andy@insectnation.org>
* Allowing rivet-config to return combined flags.
2008-08-14 Andy Buckley <andy@insectnation.org>
* Fixed some g++ 4.3 compilation bugs, including "vector" not
being a valid name for a method which returns a physics vector,
since it clashes with std::vector (which we globally import). Took
the opportunity to rationalise the Jet interface a bit, since
"particle" was used to mean "FourMomentum", and "Particle" types
required a call to "getFullParticle". I removed the "gets" at the
same time, as part of our gradual migration to a coherent naming
policy.
2008-08-11 Andy Buckley <andy@insectnation.org>
* Tidying of FastJets and added new data files from HepData.
2008-08-10 James Monk <jmonk@hep.ucl.ac.uk>
* FastJets now uses user_index property of fastjet::PseudoJet to
reconstruct PID information in jet contents.
2008-08-07 Andy Buckley <andy@insectnation.org>
* Reworking of param file and command line parsing. Tab characters
are now handled by the parser, in a way equivalent to spaces.
2008-08-06 Andy Buckley <andy@insectnation.org>
* Added extra histos and filling to Acosta analysis - all HepData
histos should now be filled, depending on sqrt{s}. Also trialling
use of LaTeX math mode in titles.
2008-08-05 Andy Buckley <andy@insectnation.org>
* More data files for CDF analyses (2 x 2008, 1 x 1994), and moved
the RivetGun AtlasPythia6.params file to more standard
fpythia-atlas.params (and added to the install list).
2008-08-04 Andy Buckley <andy@insectnation.org>
* Reduced size of available options blocks in RivetGun help text
by removing "~" negating variants (which are hardly ever used in
practice) and restricting beam particles to
PROTON, ANTIPROTON,ELECTRON and POSITRON.
* Fixed Et sorting in Acosta analysis.
2008-08-01 Andy Buckley <andy@insectnation.org>
* Added AIDA headers to the install list, since
external (plugin-type) analyses need them to be present for
compilation to succeed.
2008-07-29 Andy Buckley <andy@insectnation.org>
* Fixed missing ROOT compile flags for libRivet.
* Added command line repetition to logging.
2008-07-29 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Included the missing numbers and three more observables
in the CDF_2008_NOTE_9351 analysis.
2008-07-29 Andy Buckley <andy@insectnation.org>
* Fixed wrong flags on rivet-config
2008-07-28 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Renamed CDF_2008_DRELLYAN to CDF_2008_NOTE_9351. Updated
numbers and cuts to the final version of this CDF note.
2008-07-28 Andy Buckley <andy@insectation.org>
* Fixed polar angle calcuation to use atan2.
* Added "mk" prefixes and x/setX convention to math classes.
2008-07-28 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Fixed definition of FourMomentum::pT (it had been returning pT2)
2008-07-27 Andy Buckley <andy@insectnation.org>
* Added better tests for Boost headers.
* Added testing for -ansi, -pedantic and -Wall compiler flags.
2008-07-25 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* updated DELPHI_2002_069_CONF_603 according to information
from the author
2008-07-17 Andy Buckley <andy@insectnation.org>
* Improvements to aida2flat: now can produce one output file per
histo, and there is a -g "gnuplot mode" which comments out the
YODA/make_plot headers to make the format readable by gnuplot.
* Import boost::assign namespace contents into the Rivet namespace
--- provides very useful intuitive collection initialising
functions.
2008-07-15 Andy Buckley <andy.buckley@dur.ac.uk>
* Fixed missing namespace in vector/matrix testing.
* Removed Boost headers: now a system dependency.
* Fixed polarRadius infinite loop.
2008-07-09 Andy Buckley <andy@insectnation.org>
* Fixed definitions of mapAngleMPiToPi, etc. and used them to fix
the Jet::getPhi method.
* Trialling use of "foreach" loop in CDF_2004: it works! Very nice.
2008-07-08 Andy Buckley <andy@insectnation.org>
* Removed accidental reference to an "FS" projection in
FinalStateHCM's compare method. rivetgun -A now works again.
* Added TASSO, SLD and D0_2008 reference data. The TASSO and SLD
papers aren't installed or included in the tarball since there are
currently no plans to implement these analyses.
* Added Rivet namespacing to vector, matrix etc. classes. This
required some re-writing and the opportunity was taken to move
some canonical function definitions inside the classes and to
improve the header structure of the Math area.
2008-07-07 Andy Buckley <andy@insectnation.org>
* Added Rivet namespace to Units.hh and Constants.hh.
* Added Doxygen "@brief" flags to analyses.
* Added "RIVET_" namespacing to all header guards.
* Merged Giulio Lenzi's isolation/vetoing/invmass projections and
D0 2008 analysis.
2008-06-23 Jon Butterworth <J.Butterworth@ucl.ac.uk>
* Modified FastJet to fix ysplit and split and filter.
* Modified ExampleTree to show how to call them.
2008-06-19 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added first version of the CDF_2008_DRELLYAN analysis described on
http://www-cdf.fnal.gov/physics/new/qcd/abstracts/UEinDY_08.html
There is a small difference between the analysis and this
implementation, but it's too small to be visible.
The fpythia-cdfdrellyan.params parameter file is for this analysis.
* Added first version of the CDF_2008_MINBIAS analysis described on
http://www-cdf.fnal.gov/physics/new/qcd/abstracts/minbias_08.html
The .aida file is read from the plots on the web and will change.
I'm still discussing some open questions about the analysis with
the author.
2008-06-18 Jon Butterworth <J.Butterworth@ucl.ac.uk>
* Added First versions of splitJet and filterJet methods to
fastjet.cc. Not yet tested, buyer beware.
2008-06-18 Andy Buckley <andy@insectnation.org>
* Added extra sorted Jets and Pseudojets methods to FastJets, and
added ptmin argument to the JetAlg getJets() method, requiring a
change to TrackJet.
2008-06-13 Andy Buckley <andy@insectnation.org>
* Fixed processing of "RG" parameters to ensure that invalid
iterators are never used.
2008-06-10 Andy Buckley <andy@insectnation.org>
* Updated AIDA reference files, changing "/HepData" root path to
"/REF". Still missing a couple of reference files due to upstream
problems with the HepData records.
2008-06-09 Andy Buckley <andy@insectnation.org>
* rivetgun now handles termination signals (SIGTERM, SIGINT and
SIGHUP) gracefully, finishing the event loop and finalising
histograms. This means that histograms will always get written
out, even if not all the requested events have been generated.
2008-06-04 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added DELPHI_2002_069_CONF_603 analysis
2008-05-30 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added InitialQuarks projection
* Added OPAL_1998_S3780481 analysis
2008-05-29 Andy Buckley <andy@insectnation.org>
* distcheck compatibility fixes and autotools tweaks.
2008-05-28 Andy Buckley <andy@insectnation.org>
* Converted FastJet to use Boost smart_ptr for its plugin
handling, to solve double-delete errors stemming from the heap
cloning of projections.
* Added (a subset of) Boost headers, particularly the smart
pointers.
2008-05-24 Andy Buckley <andy@insectnation.org>
* Added autopackage spec files.
* Merged these changes into the trunk.
* Added a registerClonedProjection(...) method to
ProjectionHandler: this is needed so that cloned projections will
have valid pointer entries in the ProjectHandler repository.
* Added clone() methods to all projections (need to use this,
since the templated "new PROJ(proj)" approach to cloning can't
handle object polymorphism.
2008-05-19 Andy Buckley <andy@insectnation.org>
* Moved projection-applying functions into ProjectionApplier base
class (from which Projection and Analysis both derive).
* Added Rivet-specific exceptions in place of std::runtime_error.
* Removed unused HepML reference files.
* Added error handling for requested analyses with wrong case
convention / missing name.
2008-05-15 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* New analysis PDG_Hadron_Multiplicities
* flat2aida converter
2008-05-15 Andy Buckley <andy@insectnation.org>
* Removed unused mysterious Perl scripts!
* Added RivetGun.HepMC logging of HepMC event details.
2008-05-14 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* New analysis DELPHI_1995_S3137023. This analysis contains
the xp spectra of Xi+- and Sigma(1385)+-.
2008-05-13 Andy Buckley <andy@insectnation.org>
* Improved logging interface: log levels are now integers (for
cross-library compatibility and level setting also applies to
existing loggers.
2008-05-09 Andy Buckley <andy@insectnation.org>
* Improvements to robustness of ROOT checks.
* Added --version flag on config scripts and rivetgun.
2008-05-06 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* New UnstableFinalState projection which selects all hadrons,
leptons and real photons including unstable particles.
* In the DELPHI_1996_S3430090 analysis the multiplicities for
pi+/pi- and p0 are filled, using the UnstableFinalState projection.
2008-05-06 Andy Buckley <andy@insectnation.org>
* FastJets projection now protects against the case where no
particles exist in the final state (where FastJet throws an
exception).
* AIDA file writing is now separated from the
AnalysisHandler::finalize method... API users can choose what to
do with the histo objects, be that writing out or further
processing.
2008-04-29 Andy Buckley <andy@insectnation.org>
* Increased default tolerances in floating point comparisons as
they were overly stringent and valid f.p. precision errors were
being treated as significant.
* Implemented remainder of Acosta UE analysis.
* Added proper getEtSum() to Jet.
* Added Et2() member and function to FourMomentum.
* Added aida2flat conversion script.
* Fixed ambiguity in TrackJet algorithm as to how the iteration
continues when tracks are merged into jets in the inner loop.
2008-04-28 Andy Buckley <andy@insectnation.org>
* Merged in major "ProjectionHandler" branch. Projections are now
all stored centrally in the singleton ProjectionHandler container,
rather than as member pointers in projections and analyses. This
also affects the applyProjection mechanism, which is now available
as a templated method on Analysis and Projection. Still a few
wrinkles need to be worked out.
* The branch changes required a comprehensive review of all
existing projections and analyses: lots of tidying up of these
classes, as well as the auxiliary code like math utils, has taken
place. Too much to list and track, unfortunately!
2008-03-28 Andy Buckley <buckley@pc54.hep.ucl.ac.uk>
* Started second CDF UE analysis ("Acosta"): histograms defined.
* Fixed anomalous factor of 2 in LWH conversion from Profile1D
to DataPointSet.
* Added pT distribution histos to CDF 2001 UE analysis.
2008-03-26 Andy Buckley <andy@insectnation.org>
* Removed charged+neutral versions of histograms and projections
from DELPHI analysis since they just duplicate the more robust
charged-only measurements and aren't really of interest for
tuning.
2008-03-10 Andy Buckley <andy@insectnation.org>
* Profile histograms now use error computation with proper
weighting, as described here:
http://en.wikipedia.org/wiki/Weighted_average
2008-02-28 Andy Buckley <andy@insectnation.org>
* Added --enable-jade flag for Professor studies with patched
FastJet.
* Minor fixes to LCG tag generator and gfilt m4 macros.
* Fixed projection slicing issues with Field UE analysis.
* Added Analysis::vetoEvent(e) function, which keeps track of the
correction to the sum of weights due to event vetoing in analysis
classes.
2008-02-26 Andy Buckley <andy@insectnation.org>
* Vector<N> and derived classes now initialise to have zeroed
components when the no-arg constructor is used.
* Added Analysis::scale() function to scale 1D
histograms. Analysis::normalize() uses it internally, and the
DELPHI (A)EEC, whose histo weights are not pure event weights, and
normalised using scale(h, 1/sumEventWeights).
2008-02-21 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Added EEC and AEEC to the DELPHI_1996_S3430090 analysis. The
normalisation of these histograms is still broken (ticket #163).
2008-02-19 Hendrik Hoeth <hendrik.hoeth@cern.ch>
* Many fixes to the DELPHI_1996_S3430090 analysis: bugfix in the
calulation of eigenvalues/eigenvectors in MatrixDiag.hh for the
sphericity, rewrite of Thrust/Major/Minor, fixed scaled momentum,
hemisphere masses, normalisation in single particle events,
final state slicing problems in the projections for Thrust,
Sphericity and Hemispheres.
2008-02-08 Andy Buckley <andy@insectnation.org>
* Applied fixes and extensions to DIS classes, based on
submissions by Dan Traynor.
2008-02-06 Andy Buckley <andy@insectnation.org>
* Made projection pointers used for cut combining into const
pointers. Required some redefinition of the Projection* comparison
operator.
* Temporarily added FinalState member to ChargedFinalState to stop
projection lifetime crash.
2008-02-01 Andy Buckley <andy@insectnation.org>
* Fixed another misplaced factor of bin width in the
Analysis::normalize() method.
2008-01-30 Andy Buckley <andy@insectnation.org>
* Fixed the conversion of IHistogram1D to DPS, both via the
explicit Analysis::normalize() method and the implicit
AnalysisHandler::treeNormalize() route. The root of the problem is
the AIDA choice of the word "height" to represent the sum of
weights in a bin: i.e. the bin width is not taken into account
either in computing bin height or error.
2008-01-22 Andy Buckley <andy@insectnation.org>
* Beam projection now uses HepMC GenEvent::beam_particles() method
to get the beam particles. This is more portable and robust for
C++ generators, and equivalent to the existing "first two" method
for Fortran generators.
2008-01-17 Andy Buckley <andy@insectnation.org>
* Added angle range fix to pseudorapidity function (thanks to
Piergiulio Lenzi).
2008-01-10 Andy Buckley <andy@insectnation.org>
* Changed autobooking plot codes to use zero-padding (gets the
order right in JAS, file browser, ROOT etc.). Also changed the
'ds' part to 'd' for consistency. HepData's AIDA output has been
correspondingly updated, as have the bundled data files.
2008-01-04 Andy Buckley <andy@insectnation.org>
* Tidied up JetShape projection a bit, including making the
constructor params const references. This seems to have sorted the
runtime segfault in the CDF_2005 analysis.
* Added caching of the analysis bin edges from the AIDA file -
each analysis object will now only read its reference file once,
which massively speeds up the rivetgun startup time for analyses
with large numbhers of autobooked histos (e.g. the
DELPHI_1996_S3430090 analysis).
2008-01-02 Andy Buckley <andy@insectnation.org>
* CDF_2001_S4751469 now uses the LossyFinalState projection, with
an 8% loss rate.
* Added LossyFinalState and HadronicFinalState, and fixed a
"polarity" bug in the charged final state projection (it was
keeping only the *uncharged* particles).
* Now using isatty(1) to determine whether or not color escapes
can be used. Also removed --color argument, since it can't have an
effect (TCLAP doesn't do position-based flag toggling).
* Made Python extension build optional (and disabled by default).
2008-01-01 Andy Buckley <andy@insectnation.org>
* Removed some unwanted DEBUG statements, and lowered the level of
some infrastructure DEBUGs to TRACE level.
* Added bash color escapes to the logger system.
2007-12-21 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* include/LWH/ManagedObject.h: Fixed infinite loop in
encodeForXML cf. ticket #135.
2007-12-20 Andy Buckley <andy@insectnation.org>
* Removed HepPID, HepPDT and Boost dependencies.
* Fixed XML entity encoding in LWH. Updated CDF_2007_S7057202
analysis to not do its own XML encoding of titles.
2007-12-19 Andy Buckley <andy@insectnation.org>
* Changed units header to set GeV = 1 (HepMC convention) and using
units in CDF UE analysis.
2007-12-15 Andy Buckley <andy@insectnation.org>
* Introduced analysis metadata methods for all analyses (and made
them part of the Analysis interface).
2007-12-11 Andy Buckley <andy@insectnation.org>
* Added JetAlg base projection for TrackJet, FastJet etc.
2007-12-06 Andy Buckley <andy@insectnation.org>
* Added checking for Boost library, and the standard Boost test
program for shared_ptr.
* Got basic Python interface running - required some tweaking
since Python and Rivet's uses of dlopen collide (another
RTLD_GLOBAL issue - see
http://muttley.hates-software.com/2006/01/25/c37456e6.html )
2007-12-05 Andy Buckley <andy@insectnation.org>
* Replaced all use of KtJets projection with FastJets
projection. KtJets projection disabled but left undeleted for
now. CLHEP and KtJet libraries removed from configure searches and
Makefile flags.
2007-12-04 Andy Buckley <andy@insectnation.org>
* Param file loading now falls back to the share/RivetGun
directory if a local file can't be found and the provided name has
no directory separators in it.
* Converted TrackJet projection to update the jet centroid with
each particle added, using pT weighting in the eta and phi
averaging.
2007-12-03 Andy Buckley <andy@insectnation.org>
* Merged all command line handling functions into one large parse
function, since only one executable now needs them. This removes a
few awkward memory leaks.
* Removed rivet executable - HepMC file reading functionality will
move into rivetgun.
* Now using HepMC IO_GenEvent format (IO_Ascii and
IO_ExtendedAscii are deprecated). Now requires HepMC >= 2.3.0.
* Added forward declarations of GSL diagonalisation routines,
eliminating need for GSL headers to be installed on build machine.
2007-11-27 Andy Buckley <andy@insectnation.org>
* Removed charge differentiation from Multiplicity projection (use
CFS proj) and updated ExampleAnalysis to produce more useful numbers.
* Introduced binreloc for runtime path determination.
* Fixed several bugs in FinalState, ChargedFinalState, TrackJet
and Field analysis.
* Completed move to new analysis naming scheme.
2007-11-26 Andy Buckley <andy@insectnation.org>
* Removed conditional HAVE_FASTJET bits: FastJet is now compulsory.
* Merging appropriate RivetGun parts into Rivet. RivetGun currently broken.
2007-11-23 Andy Buckley <andy@insectnation.org>
* Renaming analyses to Spires-ID scheme: currently of form
S<SpiresID>, to become <Expt>_<YYYY>_<SpiresID>.
2007-11-20 Andy Buckley <andy@insectnation.org>
* Merged replacement vectors, matrices and boosts into trunk.
2007-11-15 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* src/Analysis.cc, include/Rivet/Analysis.hh: Introduced normalize
function. See ticket #126.
2007-10-31 Andy Buckley <andy@insectnation.org>
* Tagging as 1.0b2 for HERA-LHC meeting.
2007-10-25 Andy Buckley <andy@insectnation.org>
* Added AxesDefinition base interface to Sphericity and Thrust,
used by Hemispheres.
* Exposed BinaryCut class, improved its interface and fixed a few
bugs. It's now used by VetoedFinalState for momentum cuts.
* Removed extra output from autobooking AIDA reader.
* Added automatic DPS booking.
2007-10-12 Andy Buckley <andy@insectnation.org>
* Improved a few features of the build system
2007-10-09 James Monk
* Fixed dylib dlopen on Mac OS X.
2007-10-05 Andy Buckley <andy@insectnation.org>
* Added new reference files.
2007-10-03 Andy Buckley <andy@insectnation.org>
* Fixed bug in configure.ac which led to explicit CXX setting
being ignored.
* Including Logging.hh in Projection.hh, hence new transitive
dependency on Logging.hh being installed. Since this is the normal
behaviour, I don't think this is a problem.
* Fixed segfaulting bug due to use of addProjection() in
locally-scoped contained projections. This isn't a proper fix,
since the whole framework should be designed to avoid the
possibility of bugs like this.
* Added newly built HepML and AIDA reference files for current
analyses.
2007-10-02 Andy Buckley <andy@insectnation.org>
* Fixed possible null-pointer dereference in Particle copy
constructor and copy assignment: this removes one of two blocker
segfaults, the other of which is related to the copy-assignment of
the TotalVisMomentum projection in the ExampleTree analysis.
2007-10-01 Andy Buckley <andy@insectnation.org>
* Fixed portable path to Rivet share directory.
2007-09-28 Andy Buckley <andy@insectnation.org>
* Added more functionality to the rivet-config script: now has
libdir, includedir, cppflags, ldflags and ldlibs options.
2007-09-26 Andy Buckley <andy@insectnation.org>
* Added the analysis library closer function to the
AnalysisHandler finalize() method, and also moved the analysis
delete loop into AnalysisHandler::finalize() so as not to try
deleting objects whose libraries have already closed.
* Replaced the RivetPaths.cc.in method for portable paths with
something using -D defines - much simpler!
2007-09-21 Lars Sonnenschein <sonne@mail.cern.ch>
* Added HepEx0505013 analysis and JetShape projection (some fixes
by AB.)
* Added GetLorentzJets member function to D0 RunII cone jet projection
2007-09-21 Andy Buckley <andy@insectnation.org>
* Fixed lots if bugs and bad practice in HepEx0505013 (to make it
compile-able!)
* Downclassed the log messages from the Test analysis to DEBUG
level.
* Added isEmpty() method to final state projection.
* Added testing for empty final state and useful debug log
messages to sphericity projection.
2007-09-20 Andy Buckley <andy@insectnation.org>
* Added Hemispheres projection, which calculates event hemisphere
masses and broadenings.
2007-09-19 Andy Buckley <andy@insectnation.org>
* Added an explicit copy assignment operator to Particle: the
absence of one of these was responsible for the double-delete
error.
* Added a "fuzzy equals" utility function for float/double types
to Utils.hh (which already contains a variety of handy little
functions).
* Removed deprecated Beam::operator().
* Added ChargedFinalState projection and de-pointered the
contained FinalState projection in VetoedFinalState.
2007-09-18 Andy Buckley <andy@insectnation.org>
* Major bug fixes to the regularised version of the sphericity
projection (and hence the Parisi tensor projection). Don't trust
C & D param results from any previous version!
* Added extra methods to thrust and sphericity projections to get
the oblateness and the sphericity basis (currently returns dummy
axes since I can't yet work out how to get the similarity
transform eigenvectors from CLHEP)
2007-09-14 Andy Buckley <andy@insectnation.org>
* Merged in a branch of pluggable analysis mechanisms.
2007-06-25 Jon Butterworth <jmb@hep.ucl.ac.uk>
* Fixed some bugs in the root output for DataPoint.h
2007-06-25 Andy Buckley <andy@insectnation.org>
* include/Rivet/**/Makefile.am: No longer installing headers for
"internal" functionality.
* include/Rivet/Projections/*.hh: Removed the private restrictions
on copy-assignment operators.
2007-06-18 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* include/LWH/Tree.h: Fixed minor bug in listObjectNames.
* include/LWH/DataPointSet.h: Fixed setCoordinate functions so
that they resize the vector of DataPoints if it initially was
empty.
* include/LWH/DataPoint.h: Added constructor taking a vector of
measuremts.
2007-06-16 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* include/LWH/Tree.h: Implemented the listObjectNames and ls
functions.
* include/Rivet/Projections/FinalStateHCM.hh,
include/Rivet/Projections/VetoedFinalState.hh: removed
_theParticles and corresponding access function. Use base class
variable instead.
* include/Rivet/Projections/FinalState.hh: Made _theParticles
protected.
2007-06-13 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* src/Projections/FinalStateHCM.cc,
src/Projections/DISKinematics.cc: Equality checks using
GenParticle::operator== changed to check for pointer equality.
* include/Rivet/Analysis/HepEx9506012.hh: Uses modified DISLepton
projection.
* include/Rivet/Particle.hh: Added member function to check if a
GenParticle is associated.
* include/Rivet/Projections/DISLepton.hh,
src/Projections/DISLepton.cc: Fixed bug in projection. Introduced
final state projection to limit searching for scattered
lepton. Still not properly tested.
2007-06-08 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* include/Rivet/Projections/PVertex.hh,
src/Projections/PVertex.cc: Fixed the projection to simply get the
signal_process_vertex from the GenEvent. This is the way it should
work. If the GenEvent does not have a signal_process_vertex
properly set up in this way, the problem is with the class that
fills the GenEvent.
2007-06-06 Jon Butterworth <jmb@hep.ucl.ac.uk>
* Merged TotalVisibleMomentum and CalMET
* Added pT ranges to Vetoed final state projection
2007-05-27 Jon Butterworth <jmb@hep.ucl.ac.uk>
* Fixed initialization of VetoedFinalStateProjection in ExampleTree
2007-05-27 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* include/Rivet/Projections/KtJets.*: Make sure the KtEvent is
deleted properly.
2007-05-26 Jon Butterworth <jmb@hep.ucl.ac.uk>
* Added leptons to the ExampleTree.
* Added TotalVisibleEnergy projection, and added output to ExampleTree.
2007-05-25 Jon Butterworth <jmb@hep.ucl.ac.uk>
* Added a charged lepton projection
2007-05-23 Andy Buckley <andy@insectnation.org>
* src/Analysis/HepEx0409040.cc: Changed range of the histograms to
the "pi" range rather than the "128" range.
* src/Analysis/Analysis.cc: Fixed a bug in the AIDA path building.
Histogram auto-booking now works.
2007-05-23 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* src/Analysis/HepEx9506012.cc: Now uses the histogram booking
function in the Analysis class.
2007-05-23 Jon Butterworth <jmb@hep.ucl.ac.uk>
* Fixed bug in PRD65092002 (was failing on zero jets)
2007-05-23 Andy Buckley <andy@insectnation.org>
* Added (but haven't properly tested) a VetoedFinalState projection.
* Added normalize() method for AIDA 1D histograms.
* Added configure checking for Mac OS X version, and setting the
development target flag accordingly.
2007-05-22 Andy Buckley <andy@insectnation.org>
* Added an ostream method for AnalysisName enums.
* Converted Analyses and Projections to use projection lists, cuts
and beam constraints.
* Added beam pair combining to the BeamPair sets of Projections
by finding set meta-intersections.
* Added methods to Cuts, Analysis and Projection to make Cut
definition easier.
* Fixed default fall-through in cut handling switch statement and
now using -numeric_limits<double>::max() rather than min()
* Added more control of logging presentation via static flag
methods on Log.
2007-05-13 Andy Buckley <andy@insectnation.org>
* Added self-consistency checking mechanisms for Cuts and Beam
* Re-implemented the cut-handling part of RivetInfo as a Cuts class.
* Changed names of Analysis and Projection name() and handler()
methods to getName() and getHandler() to be more consistent with
the rest of the public method names in those classes.
2007-05-02 Andy Buckley <andy@insectnation.org>
* Added auto-booking of histogram bins from AIDA XML files. The
AIDA files are located via a C++ function which is generated from
RivetPaths.cc.in by running configure.
2007-04-18 Andy Buckley <andy@insectnation.org>
* Added a preliminary version of the Rick Field UE analysis, under
the name PRD65092002.
2007-04-19 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* src/Analysis/HepEx0409040.cc: The reason this did not compile
under gcc-4 is that some iterators into a vector were wrongly
assued to be pointers and were initialized to 0 and later compared
to 0. I've changed this to initialize to end() of the
corresponding vector and to compare with the same end() later.
2007-04-05 Andy Buckley <andy@insectnation.org>
* Lots of name changes in anticipation of the MCNet
school. RivetHandler is now AnalysisHandler (since that's what it
does!), BeamParticle has become ParticleName, and RivetInfo has
been split into Cut and BeamConstraint portions.
* Added BeamConstraint mechanism, which can be used to determine
if an analysis is compatible with the beams being used in the
generator. The ParticleName includes an "ANY" wildcard for this
purpose.
2006-03-19 Andy Buckley <andy@insectnation.org>
* Added "rivet" executable which can read in HepMC ASCII dump
files and apply Rivet analyses on the events.
2007-02-24 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* src/Projections/KtJets.cc: Added comparison of member variables
in compare() function
* all: Merged changes from polymorphic-projections branch into
trunk
2007-02-17 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* all: projections and analysis handlers: All projections which
uses other projctions now has a pointer rather than a copy of
those projections to allow for polymorphism. The constructors has
also been changed to require the used projections themselves,
rather than the arguments needed to construct them.
2007-02-17 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* src/Projections/FinalState.cc,
include/Rivet/Projections/FinalState.icc (Rivet),
include/Rivet/Projections/FinalState.hh: Added cut in transverse
momentum on the particles to be included in the final state.
2007-02-06 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* include/LWH/HistogramFactory.h: Fixed divide-by-zero in divide
function. Also fixed bug in error calculation in divide
function. Introduced checkBin function to make sure two histograms
are equal even if they have variable bin widths.
* include/LWH/Histogram1D.h: In normalize(double), do not do anything
if the sum of the bins are zero to avoid dividing by zero.
2007-01-20 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* src/Test/testLWH.cc: Modified to output files using the Tree.
* configure.ac: Removed AC_CONFIG_AUX_DIR([include/Rivet/Config])
since the directory does not exist anymore.
2006-12-21 Andy Buckley <andy@insectnation.org>
* Rivet will now conditionally install the AIDA and LWH headers if
it can't find them when configure'ing.
* Started integrating Leif's LWH package to fulfill the AIDA
duties.
* Replaced multitude of CLHEP wrapper headers with a single
RivetCLHEP.h header.
2006-11-20 Andy Buckley <andy@insectnation.org>
* Introduced log4cpp logging.
* Added analysis enum, which can be used as input to an analysis
factory by Rivet users.
2006-11-02 Andy Buckley <andy@insectnation.org>
* Yet more, almost pointless, administrative moving around of
things with the intention of making the structure a bit
better-defined:
* The RivetInfo and RivetHandler classes have been
moved from src/Analysis into src as they are really the main Rivet
interface classes. The Rivet.h header has also been moved into the
"header root".
* The build of a single shared library in lib has been disabled,
with the library being built instead in src.
2006-10-14 Andy Buckley <andy@insectnation.org>
* Introduced a minimal subset of the Sherpa math tools, such as
Vector{3,4}D, Matrix, etc. The intention is to eventually cut the
dependency on CLHEP.
2006-07-28 Andy Buckley <andy@insectnation.org>
* Moving things around: all sources now in directories under src
2006-06-04 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* Analysis/Examples/HZ95108.*: Now uses CentralEtHCM. Also set GeV
units on the relevant histograms.
* Projections/CentralEtHCM.*: Making a special class just to get
out one number - the summed Et in the central rapidity bin - may
seem like an overkill. But in case some one else might nees it...
2006-06-03 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* Analysis/Examples/HZ95108.*: Added the hz95108 energy flow
analysis from HZtool.
* Projections/DISLepton.*: Since many HERA measurements do not
care if we have electron or positron beam, it is now possible to
specify lepton or anti-lepton.
* Projections/Event.*: Added member and access function for the
weight of an event (taken from the GenEvent object.weights()[0].
* Analysis/RivetHandler.*: Now depends explicitly on the AIDA
interface. An AIDA analysis factory must be specified in the
constructor, where a tree and histogram factory is automatically
created. Added access functions to the relevant AIDA objects.
* Analysis/AnalysisBase.*: Added access to the RivetHandler and
its AIDA factories.
2005-12-27 Leif Lonnblad <Leif.Lonnblad@thep.lu.se>
* configure.ac: Added -I$THEPEGPATH/include to AM_CPPFLAGS.
* Config/Rivet.h: Added some std incudes and using std::
declaration.
* Analysis/RivetInfo.*: Fixed some bugs. The RivetInfo facility
now works, although it has not been thoroughly tested.
* Analysis/Examples/TestMultiplicity.*: Re-introduced
FinalStateHCM for testing purposes but commented it away again.
* .: Made a number of changes to implement handling of RivetInfo
objects.
diff --git a/Makefile.am b/Makefile.am
--- a/Makefile.am
+++ b/Makefile.am
@@ -1,39 +1,39 @@
ACLOCAL_AMFLAGS = -I m4
-SUBDIRS = src pyext data include bin analyses doc test
+SUBDIRS = src pyext data include bin analyses test doc
EXTRA_DIST = GUIDELINES
DISTCHECK_CONFIGURE_FLAGS = --enable-debug --with-yoda=$(YODAPATH) --with-hepmc=$(HEPMCPATH) --with-fastjet=$(FASTJETPATH)
pkgconfigdir = $(libdir)/pkgconfig
dist_pkgconfig_DATA = rivet.pc
doc:
cd doc && $(MAKE) doc
.PHONY : doc dox pyclean
clean-local:
@rm -rf a.out
## Doxygen
if WITH_DOXYGEN
dox:
@echo "Running Doxygen..."
@$(DOXYGEN) $(top_builddir)/Doxyfile || true
install-dox:
$(install_sh_DATA) doxy/html/* $(DESTDIR)$(pkgdatadir)/doc/html
mostlyclean-local:
@rm -rf $(top_builddir)/doxy
uninstall-local:
@rm -rf $(DESTDIR)$(pkgdatadir)/doc; \
test ! -d $(DESTDIR)$(pkgdatadir) || rmdir $(DESTDIR)$(pkgdatadir) || true
endif
## Upload to HepForge
RSH = rsync
DEST = login.hepforge.org:rivet/downloads/
upload: dist
$(RSH) $(DIST_ARCHIVES) $(DEST)
diff --git a/README b/README
--- a/README
+++ b/README
@@ -1,102 +1,91 @@
Rivet quickstart guide
----------------------
Assuming you've got a copy of Rivet installed on your machine, you'll now want
to know how to use it. Here's an example session with the 'rivet' command, which
should be illustrative.
GENERATING AND ANALYSING
The main interface to Rivet is the rivet command. We will demonstrate how to use
this to analyse HepMC events from a text file in the "IO_GenEvent" HepMC format.
-(This is the only supported HepMC text format from HepMC 2.5 onwards.)
Firstly, we recommend using a filesystem pipe (or 'FIFO') so that your events
don't create a huge file that takes all your disk space. The idea is that the
generator will push events into what looks like a file, and Rivet will read from
the same 'file'. In fact, though, the 'file' is a disguised pipe between the two
processes, so no slow filesystem access needs to take place, and the system will
automatically balance the data flow between the writing and reading processes:
the generator will only write more event data when Rivet has read that currently
available in the FIFO buffer. All this is completely transparent to the user:
good old Unix! Here's how you do it:
> mkfifo hepmc.fifo
> my-generator --num-events=500000 --hepmc-output=hepmc.fifo &
> rivet --analysis=ANALYSIS_NAME hepmc.fifo
The backgrounding of the generator process is important: the generator will wait
until the hepmc.fifo pipe is being read by Rivet, so unless it is backgrounded
you will never get the terminal focus back to run rivet!
The generator used above can be anything which writes HepMC text output to the
-specified FIFO. As a concrete example, the AGILe package
-(http://projects.hepforge.org/agile/) provides an interface to several
-generators with a command line tool called agile-rungen:
+specified FIFO. As a concrete example, you could use a Pythia 8 main program to
+write events to the FIFO, and pick them up on the other end with rivet:
-> agile-rungen Pythia6:418 --beams=TVT:1800 &
+> ./main42 py8config.cfg hepmc.fifo &
> rivet --analysis=CDF_2001_S4751469 hepmc.fifo
-The agile-rungen and rivet commands both provide extensive command line
-documentation when called with the -h/--help flag.
+The rivet command provides extensive command line documentation when called
+with the -h/--help flag.
CHECKING THE DATA
-By default, Rivet outputs its histograms in the AIDA XML format, which is not
-particularly easy to read or plot. An easier format is available if you convert
-the AIDA file to a flat text format (the long-term Rivet data format) with the
-aida2flat command:
+Rivet outputs its histograms in the YODA format. You can read it directly, but
+more conveniently there are a variety of command-line utilities whose names
+start with "yoda", for viewing and manipulating these files' contents.
-> aida2flat Rivet.aida | less
-
-Again, check the aida2flat --help documentation for details on more options.
-
-There is also an aida2root command which provides the data as ROOT TGraph
+There is also an yoda2root command which provides the data as ROOT TGraph
objects for those of a ROOTy disposition. Due to a ROOT bug, for TGraphs to
display properly you will have to specify the "AP" option in the top right-hand
box of the ROOT TBrowser or alternatively draw the TGraph programmatically using
'myTGraph->Draw("AP")'. This isn't a Rivet bug: it's ROOT forgetting to draw the
graph axes!
PLOTTING
-Because we don't get on well with ROOT, Rivet comes with two commands ---
-compare-histos and make-plots --- for comparing and plotting AIDA data. These
-commands produce nice comparison plots of publication quality from the YODA
-"dat" format text files, e.g.:
+Rivet comes with two commands --- rivet-cmphistos and make-plots --- for comparing
+and plotting our output data. These
+commands respectively combine many YODA files in (usually) convenient ways, to make
+.dat files describing plots to be made, and then render those plots to publication
+quality PDFs. This way you can tweak the .dat file for optimal aesthetics without
+re-running the data processing steps. rivet-cmphistos also accepts various
+command-line modifiers to change major rendering features. The most convenient way
+to make plots from Rivet YODA files, however, is with the rivet-mkhtml script:
-> compare-plots path/to/CDF_2001_S4751469.aida py.aida:'Pythia 6.418' hw.aida:'Herwig++ 2.3.0'
+> rivet-mkhtml path/to/CDF_2001_S4751469.aida py.aida:'Pythia 6.418' hw.aida:'Herwig++ 2.3.0'
-This command will have compared the three named data files (ending in .aida),
+will create a rivet-plots directory containing a set of web pages with thumbnail
+plot images, linked to full PDF versions of the plots.
+
+[In detail, this command compared the three named data files (ending in .yoda),
identified which plots are available in them, and combined the MC and reference
plots appropriately into a set of plot data files ending with .dat. The strings
after the ":" for the MC files are specifying ID strings to appear in the plot
-legends. You can also run compare-plots to just compare MC-MC data files. More
-options are described by running 'compare-histos --help'.
+legends. You can also run rivet-mkhtml to just compare MC-MC data files. More
+options are described by running 'rivet-mkhtml --help'.]
Incidentally, the reference files for each Rivet analysis are to be found in the
installed Rivet shared data directory. You can find the location of this by
using the rivet-config command:
> rivet-config --datadir
-You can now plot the created data files using the make-plots command:
-
-> make-plots --pdf *.dat
-
-The --pdf flag makes the output plots in PDF format: by default the output is in
-PostScript (.ps), and flags for conversion to EPS and PNG are also available.
-
THAT'S ALL!
We hope this was useful as a quick guide to getting started with running Rivet's
-built-in analyses for Monte Carlo generator validation. Be aware that we will be
-overhauling Rivet's histogramming system in version 1.3.0, from which point all
-the conversions away from AIDA XML will no longer be necessary, and a fully
-programmatic interface to the Rivet data files will be possible. Please bear
-with us while we get this sorted out: we're as keen to have better histogramming
-as you are! ;)
+built-in analyses for Monte Carlo generator validation. Get in touch via the developer
+mailing list if you need any assistance: rivet@projects.hepforge.org
diff --git a/analyses/pluginATLAS/ATLAS_2015_I1404878.cc b/analyses/pluginATLAS/ATLAS_2015_I1404878.cc
--- a/analyses/pluginATLAS/ATLAS_2015_I1404878.cc
+++ b/analyses/pluginATLAS/ATLAS_2015_I1404878.cc
@@ -1,262 +1,263 @@
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/FinalState.hh"
#include "Rivet/Projections/VetoedFinalState.hh"
#include "Rivet/Projections/IdentifiedFinalState.hh"
#include "Rivet/Projections/PromptFinalState.hh"
#include "Rivet/Projections/DressedLeptons.hh"
#include "Rivet/Projections/FastJets.hh"
#include "Rivet/Projections/VisibleFinalState.hh"
namespace Rivet {
class ATLAS_2015_I1404878 : public Analysis {
public:
/// Constructor
DEFAULT_RIVET_ANALYSIS_CTOR(ATLAS_2015_I1404878);
void init() {
// Eta ranges
Cut eta_full = (Cuts::abseta < 4.2) & (Cuts::pT >= 1.0*MeV);
Cut lep_cuts = (Cuts::abseta < 2.5) && (Cuts::pT > 25*GeV);
// All final state particles
FinalState fs(eta_full);
// Get photons to dress leptons
IdentifiedFinalState photons(fs);
photons.acceptIdPair(PID::PHOTON);
// Projection to find the electrons
IdentifiedFinalState el_id(fs);
el_id.acceptIdPair(PID::ELECTRON);
PromptFinalState electrons(el_id);
electrons.acceptTauDecays(true);
declare(electrons, "electrons");
DressedLeptons dressedelectrons(photons, electrons, 0.1, lep_cuts, true);
declare(dressedelectrons, "dressedelectrons");
DressedLeptons ewdressedelectrons(photons, electrons, 0.1, eta_full, true);
declare(ewdressedelectrons, "ewdressedelectrons");
// Projection to find the muons
IdentifiedFinalState mu_id(fs);
mu_id.acceptIdPair(PID::MUON);
PromptFinalState muons(mu_id);
muons.acceptTauDecays(true);
declare(muons, "muons");
DressedLeptons dressedmuons(photons, muons, 0.1, lep_cuts, true);
declare(dressedmuons, "dressedmuons");
DressedLeptons ewdressedmuons(photons, muons, 0.1, eta_full, true);
declare(ewdressedmuons, "ewdressedmuons");
// Projection to find neutrinos
IdentifiedFinalState nu_id;
nu_id.acceptNeutrinos();
PromptFinalState neutrinos(nu_id);
neutrinos.acceptTauDecays(true);
// get MET from generic invisibles
VetoedFinalState inv_fs(fs);
inv_fs.addVetoOnThisFinalState(VisibleFinalState(fs));
declare(inv_fs, "InvisibleFS");
// Jet clustering.
VetoedFinalState vfs;
vfs.addVetoOnThisFinalState(ewdressedelectrons);
vfs.addVetoOnThisFinalState(ewdressedmuons);
vfs.addVetoOnThisFinalState(neutrinos);
FastJets jets(vfs, FastJets::ANTIKT, 0.4);
jets.useInvisibles(true);
declare(jets, "jets");
// Histogram booking
_h["massttbar"] = bookHisto1D( 1, 1, 1);
_h["massttbar_norm"] = bookHisto1D( 2, 1, 1);
_h["ptttbar"] = bookHisto1D( 3, 1, 1);
_h["ptttbar_norm"] = bookHisto1D( 4, 1, 1);
_h["absrapttbar"] = bookHisto1D( 5, 1, 1);
_h["absrapttbar_norm"] = bookHisto1D( 6, 1, 1);
_h["ptpseudotophadron"] = bookHisto1D( 7, 1, 1);
_h["ptpseudotophadron_norm"] = bookHisto1D( 8, 1, 1);
_h["absrappseudotophadron"] = bookHisto1D( 9, 1, 1);
_h["absrappseudotophadron_norm"] = bookHisto1D(10, 1, 1);
_h["absPout"] = bookHisto1D(11, 1, 1);
_h["absPout_norm"] = bookHisto1D(12, 1, 1);
_h["dPhittbar"] = bookHisto1D(13, 1, 1);
_h["dPhittbar_norm"] = bookHisto1D(14, 1, 1);
_h["HTttbar"] = bookHisto1D(15, 1, 1);
_h["HTttbar_norm"] = bookHisto1D(16, 1, 1);
_h["Yboost"] = bookHisto1D(17, 1, 1);
_h["Yboost_norm"] = bookHisto1D(18, 1, 1);
_h["chittbar"] = bookHisto1D(19, 1, 1);
_h["chittbar_norm"] = bookHisto1D(20, 1, 1);
_h["RWt"] = bookHisto1D(21, 1, 1);
_h["RWt_norm"] = bookHisto1D(22, 1, 1);
}
+
void analyze(const Event& event) {
const double weight = event.weight();
// Get the selected objects, using the projections.
vector<DressedLepton> electrons = applyProjection<DressedLeptons>(event, "dressedelectrons").dressedLeptons();
vector<DressedLepton> muons = applyProjection<DressedLeptons>(event, "dressedmuons").dressedLeptons();
const Jets& jets = applyProjection<FastJets>(event, "jets").jetsByPt(Cuts::pT > 25*GeV && Cuts::abseta < 2.5);
const FinalState& ifs = applyProjection<FinalState>(event, "InvisibleFS");
// Calculate MET
FourMomentum met;
for (const Particle& p : ifs.particles()) met += p.momentum();
// Count the number of b-tags
Jets bjets, lightjets;
for (const Jet& jet : jets){
bool b_tagged = jet.bTags(Cuts::pT > 5*GeV).size();
if ( b_tagged && bjets.size() < 2 ) bjets += jet;
else lightjets += jet;
}
bool single_electron = (electrons.size() == 1) && (muons.empty());
bool single_muon = (muons.size() == 1) && (electrons.empty());
DressedLepton* lepton = nullptr;
if (single_electron) lepton = &electrons[0];
else if (single_muon) lepton = &muons[0];
if(!single_electron && !single_muon) vetoEvent;
if (jets.size() < 4 || bjets.size() < 2) vetoEvent;
FourMomentum pbjet1; // Momentum of bjet1
FourMomentum pbjet2; // Momentum of bjet2
if ( deltaR(bjets[0], *lepton) <= deltaR(bjets[1], *lepton) ) {
pbjet1 = bjets[0].momentum();
pbjet2 = bjets[1].momentum();
} else {
pbjet1 = bjets[1].momentum();
pbjet2 = bjets[0].momentum();
}
-
double bestWmass = 1000.0*TeV;
double mWPDG = 80.399*GeV;
int Wj1index = -1, Wj2index = -1;
for (unsigned int i = 0; i < (lightjets.size() - 1); ++i) {
for (unsigned int j = i + 1; j < lightjets.size(); ++j) {
double wmass = (lightjets[i].momentum() + lightjets[j].momentum()).mass();
if (fabs(wmass - mWPDG) < fabs(bestWmass - mWPDG)) {
bestWmass = wmass;
Wj1index = i;
Wj2index = j;
}
}
}
// Compute hadronic W boson
FourMomentum pWhadron = lightjets[Wj1index].momentum() + lightjets[Wj2index].momentum();
double pz = _computeneutrinoz(lepton->momentum(), met);
FourMomentum ppseudoneutrino( sqrt(sqr(met.px()) + sqr(met.py()) + sqr(pz)), met.px(), met.py(), pz);
// Compute leptonic, hadronic, combined pseudo-top
FourMomentum ppseudotoplepton = lepton->momentum() + ppseudoneutrino + pbjet1;
FourMomentum ppseudotophadron = pbjet2 + pWhadron;
FourMomentum pttbar = ppseudotoplepton + ppseudotophadron;
Vector3 z_versor(0,0,1);
Vector3 vpseudotophadron = ppseudotophadron.vector3();
Vector3 vpseudotoplepton = ppseudotoplepton.vector3();
// Observables
double ystar = 0.5 * deltaRap(ppseudotophadron, ppseudotoplepton);
double chi_ttbar = exp(2 * fabs(ystar));
double deltaPhi_ttbar = deltaPhi(ppseudotoplepton,ppseudotophadron);
double HT_ttbar = ppseudotophadron.pt() + ppseudotoplepton.pt();
double Yboost = 0.5 * fabs(ppseudotophadron.rapidity() + ppseudotoplepton.rapidity());
double R_Wt = pWhadron.pt() / ppseudotophadron.pt();
double absPout = fabs(vpseudotophadron.dot((vpseudotoplepton.cross(z_versor))/(vpseudotoplepton.cross(z_versor).mod())));
// absolute cross sections
_h["ptpseudotophadron"]->fill( ppseudotophadron.pt(), weight); //pT of pseudo top hadron
_h["ptttbar"]->fill( pttbar.pt(), weight); //fill pT of ttbar in combined channel
_h["absrappseudotophadron"]->fill(ppseudotophadron.absrap(), weight);
_h["absrapttbar"]->fill( pttbar.absrap(), weight);
_h["massttbar"]->fill( pttbar.mass(), weight);
_h["absPout"]->fill( absPout, weight);
_h["chittbar"]->fill( chi_ttbar, weight);
_h["dPhittbar"]->fill( deltaPhi_ttbar, weight);
_h["HTttbar"]->fill( HT_ttbar, weight);
_h["Yboost"]->fill( Yboost, weight);
_h["RWt"]->fill( R_Wt, weight);
// normalised cross sections
_h["ptpseudotophadron_norm"]->fill( ppseudotophadron.pt(), weight); //pT of pseudo top hadron
_h["ptttbar_norm"]->fill( pttbar.pt(), weight); //fill pT of ttbar in combined channel
_h["absrappseudotophadron_norm"]->fill(ppseudotophadron.absrap(), weight);
_h["absrapttbar_norm"]->fill( pttbar.absrap(), weight);
_h["massttbar_norm"]->fill( pttbar.mass(), weight);
_h["absPout_norm"]->fill( absPout, weight);
_h["chittbar_norm"]->fill( chi_ttbar, weight);
_h["dPhittbar_norm"]->fill( deltaPhi_ttbar, weight);
_h["HTttbar_norm"]->fill( HT_ttbar, weight);
_h["Yboost_norm"]->fill( Yboost, weight);
_h["RWt_norm"]->fill( R_Wt, weight);
}
+
void finalize() {
// Normalize to cross-section
const double sf = crossSection() / sumOfWeights();
for (auto& k_h : _h) {
scale(k_h.second, sf);
if (k_h.first.find("_norm") != string::npos) normalize(k_h.second);
}
}
private:
// Compute z component of neutrino momentum given lepton and met
double _computeneutrinoz(const FourMomentum& lepton, FourMomentum& met) const {
double m_W = 80.399; // in GeV, given in the paper
double k = (( sqr( m_W ) - sqr( lepton.mass() ) ) / 2 ) + (lepton.px() * met.px() + lepton.py() * met.py());
double a = sqr ( lepton.E() )- sqr ( lepton.pz() );
double b = -2*k*lepton.pz();
double c = sqr( lepton.E() ) * sqr( met.pT() ) - sqr( k );
double discriminant = sqr(b) - 4 * a * c;
double quad[2] = { (- b - sqrt(discriminant)) / (2 * a), (- b + sqrt(discriminant)) / (2 * a) }; //two possible quadratic solns
double pzneutrino;
if (discriminant < 0) { // if the discriminant is negative:
pzneutrino = - b / (2 * a);
} else { // if the discriminant is positive, take the soln with smallest absolute value
pzneutrino = (fabs(quad[0]) < fabs(quad[1])) ? quad[0] : quad[1];
}
return pzneutrino;
}
/// @todo Replace with central version
double _mT(const FourMomentum &l, FourMomentum &nu) const {
return sqrt( 2 * l.pT() * nu.pT() * (1 - cos(deltaPhi(l, nu))) );
}
/// @name Objects that are used by the event selection decisions
map<string, Histo1DPtr> _h;
};
// The hook for the plugin system
DECLARE_RIVET_PLUGIN(ATLAS_2015_I1404878);
}
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1517194.cc b/analyses/pluginATLAS/ATLAS_2017_I1517194.cc
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2017_I1517194.cc
@@ -0,0 +1,242 @@
+// -*- C++ -*-
+#include "Rivet/Analysis.hh"
+#include "Rivet/Projections/MissingMomentum.hh"
+#include "Rivet/Projections/FastJets.hh"
+#include "Rivet/Projections/WFinder.hh"
+
+namespace Rivet {
+
+
+ class ATLAS_2017_I1517194 : public Analysis {
+ public:
+
+ /// @name Constructors etc.
+ //@{
+
+ /// Constructor
+ ///@brief: Electroweak Wjj production at 8 TeV
+ ATLAS_2017_I1517194(string name="ATLAS_2017_I1517194", size_t mode = 0,
+ string ref_data="ATLAS_2017_I1517194") : Analysis(name) {
+ _mode = mode; // default is electron channel
+ //setRefDataName(ref_data);
+ }
+ //@}
+
+
+
+ /// @name Analysis methods
+ //@{
+ /// Book histograms and initialise projections before the run
+ void init() {
+
+ const FinalState fs;
+ // W Selection
+ WFinder wfinder(fs, Cuts::rap < 2.5 && Cuts::pT >= 25*GeV, _mode? PID::MUON : PID::ELECTRON, 0*GeV, 13*TeV, 0*GeV, 0.1);
+ declare(wfinder, "WFinder");
+
+ FastJets jets( wfinder.remainingFinalState(), FastJets::ANTIKT, 0.4);
+ jets.useMuons(JetAlg::DECAY_MUONS);
+ jets.useInvisibles(JetAlg::ALL_INVISIBLES);
+ declare(jets, "Jets_w");
+
+ MissingMomentum missmom(FinalState(Cuts::eta < 5.0));
+ addProjection(missmom, "mm");
+
+ const vector<string> phase_spaces = { "highmass15", "antiLC", "signal10",
+ "highmass10", "inclusive", "highmass20",
+ "antiLCantiJC", "antiJC", "signal", };
+ const vector<string> variables = { "dijetmass", "dijetpt", "dphi12", "dy12", "j1pt", "JC", "LC", "ngapjets" };
+ size_t hepdataid = 10;
+ for (size_t group = 0; group < 4; ++group) {
+ for ( size_t ps=0; ps < phase_spaces.size(); ++ps ) {
+ for ( size_t var=0; var < variables.size(); ++var ) {
+ if (group < 2) {
+ if ((ps == 0 || ps == 2 || ps == 3 || ps == 5) && var == 0) continue;
+ if ((ps == 1 || ps == 2 || ps > 5) && var > 4) continue;
+ if (group == 1 && ps == 7 && var == 3) continue;
+ }
+ else {
+ if (ps == 1 || ps == 4 || ps > 5) continue;
+ if ((ps == 0 || ps == 5) && var < 2) continue;
+ if (ps == 2 && var > 4) continue;
+ if ((ps == 0 || ps == 3 || ps == 5) && var == 5) continue;
+ if (group == 2) {
+ if ((ps == 0 || ps == 5) && var == 3) continue;
+ if (ps == 3 && var == 1) continue;
+ }
+ else {
+ if ((ps == 0 || ps == 3 || ps == 5) && var == 6) continue;
+ if ((ps == 2 || ps == 3) && var < 2) continue;
+ }
+ }
+
+ ++hepdataid;
+
+ string label = variables[var]+"_"+phase_spaces[ps];
+ //string pre = group > 1? "ew_" : "";
+ //std::cout << "rivet -- " << pre << label << suff << " " << hepdataid << std::endl;
+ string suff = group % 2? "" : "_norm";
+ if (group > 1) _hists["ew_" + label + suff] = bookHisto1D(hepdataid, 1, 1);
+ else _hists[label + suff] = bookHisto1D(hepdataid, 1, 1);
+ }
+ }
+ }
+ }
+
+
+ /// Perform the per-event analysis
+ void analyze(const Event& event) {
+ const double weight = event.weight();
+
+ FourMomentum boson, lepton, neutrino;
+ const WFinder& wfinder = apply<WFinder>(event, "WFinder");
+ const FastJets& jetpro = apply<FastJets>(event, "Jets_w");
+ const MissingMomentum& missmom = apply<MissingMomentum>(event, "mm");
+
+ if ( wfinder.bosons().size() != 1 ) { vetoEvent; }
+
+ boson = wfinder.bosons().front().momentum();
+ lepton = wfinder.constituentLeptons().front().momentum();
+ neutrino = wfinder.constituentNeutrinos().front().momentum();
+
+ vector<FourMomentum> jets;
+ for (const Jet& jet : jetpro.jetsByPt(30*GeV)) {
+ if ( fabs(jet.momentum().rapidity()) > 4.4 ) continue;
+ if ( fabs(deltaR(jet, lepton)) < 0.3 ) continue;
+ jets.push_back(jet.momentum());
+ }
+
+ if (jets.size() < 2) vetoEvent;
+
+ double mT = sqrt( 2.0*lepton.pT()*neutrino.Et()*( 1.0-cos( lepton.phi()-neutrino.phi() ) ) );
+ double DeltaRap = fabs( jets[0].rapidity()-jets[1].rapidity() );
+ double dijet_mass = FourMomentum(jets[0]+jets[1]).mass();
+ size_t nojets = jets.size();
+
+ if (missmom.vectorEt().mod() < 25*GeV) vetoEvent;
+ if (jets[0].pT() < 80*GeV) vetoEvent;
+ if (jets[1].pT() < 60*GeV) vetoEvent;
+ if (dijet_mass < 500*GeV) vetoEvent;
+ if (DeltaRap < 2.0) vetoEvent;
+ if (mT < 40*GeV) vetoEvent;
+
+ // By now, the event has passed all VBF cuts
+ double DijetPt = FourMomentum(jets[0]+jets[1]).pT();
+ double dphi = fabs(jets[0].phi() - jets[1].phi());
+ double DeltaPhi = ( dphi<=pi ) ? dphi/pi : (2.*pi-dphi)/pi;
+ double jet_1_rap = jets[0].rapidity();
+ double jet_2_rap = jets[1].rapidity();
+
+ // Njets in Gap Control Regions info
+ int njetsingap = 0;
+ bool firstIsForward = jet_1_rap > jet_2_rap;
+ int jF = (firstIsForward) ? 0 : 1; // sets most positive jet to be forward index
+ int jB = (firstIsForward) ? 1 : 0; // sets most negative jet to be backward index
+ for (size_t j = 2; j < nojets; ++j) {
+ if ( (jets[j].rapidity()<jets[jF].rapidity()) && (jets[j].rapidity()>jets[jB].rapidity()) ) njetsingap++;
+ }
+
+ // Third+ Jet Centrality Cut (Vetos any event that has a jet between raps of the two leading jets)
+ bool passJC = false;
+ std::vector<double> JCvals;
+ JCvals.clear();
+ if ( nojets < 3) passJC = true;
+ else if ( nojets > 2 ) {
+ passJC = true;
+ for (size_t j = 2; j < nojets; ++j) {
+ double jet_3_rap = jets[j].rapidity();
+ double jet3gap = fabs(( jet_3_rap - ((jet_1_rap + jet_2_rap)/2.0))/(jet_1_rap - jet_2_rap));
+ JCvals.push_back(jet3gap);
+ if ( jet3gap < 0.4 ) { passJC = false; }
+ }
+ }
+
+ double lepton_rap = lepton.rapidity();
+ double lep_cent = fabs((lepton_rap - ((jet_1_rap + jet_2_rap)/2.0) )/(jet_1_rap - jet_2_rap));
+ bool passLC = (lep_cent < 0.4);
+
+ map<string, bool> phaseSpaces;
+ phaseSpaces["inclusive"] = true;
+ phaseSpaces["highmass10"] = (dijet_mass>1000.0*GeV);
+ phaseSpaces["highmass15"] = (dijet_mass>1500.0*GeV);
+ phaseSpaces["highmass20"] = (dijet_mass>2000.0*GeV);
+ phaseSpaces["antiLC"] = ( !passLC && passJC );
+ phaseSpaces["antiJC"] = ( passLC && !passJC );
+ phaseSpaces["antiLCantiJC"] = ( !passLC && !passJC );
+ phaseSpaces["signal"] = ( passLC && passJC );
+ phaseSpaces["signal10"] = ( (dijet_mass>1000.0*GeV) && passLC && passJC );
+
+ for (const auto& ps : phaseSpaces) {
+ if (!ps.second) continue;
+ fillHisto("dijetmass_"+ps.first, dijet_mass, weight);
+ fillHisto("dijetpt_"+ps.first, DijetPt, weight);
+ fillHisto("dy12_"+ps.first, fabs(jet_1_rap-jet_2_rap), weight);
+ fillHisto("dphi12_"+ps.first, DeltaPhi, weight);
+ fillHisto("j1pt_"+ps.first, jets[0].pT(), weight);
+ if (ps.first == "inclusive" || ps.first.find("highmass") != string::npos) {
+ fillHisto("LC_"+ps.first, lep_cent, weight);
+ fillHisto("ngapjets_"+ps.first, njetsingap, weight);
+ for (auto& jc : JCvals) {
+ fillHisto("JC_"+ps.first, jc, weight);
+ }
+ }
+ }
+
+ }
+
+
+ /// Normalise histograms etc., after the run
+ void finalize() {
+ double factor = crossSection()/sumOfWeights()/femtobarn; // refData is in fb
+ for (const auto& key_hist : _hists) {
+ scale(key_hist.second, factor);
+ if (key_hist.first.find("_norm") != string::npos) normalize(key_hist.second);
+ }
+ }
+
+ //@}
+
+
+ void fillHisto(const string& label, const double value, const double weight) {
+ if (_hists.find(label) != _hists.end()) { // QCD+EW, absolute
+ _hists[label]->fill(value, weight);
+ }
+ if (_hists.find(label + "_norm") != _hists.end()) { // QCD+EW, normalised
+ _hists[label + "_norm"]->fill(value, weight);
+ }
+ if (_hists.find("ew_" + label) != _hists.end()) { // EW-only, absolute
+ _hists["ew_" + label]->fill(value, weight);
+ }
+ if (_hists.find("ew_" + label + "_norm") != _hists.end()) { // EW-only, normalised
+ _hists["ew_" + label + "_norm"]->fill(value, weight);
+ }
+ }
+
+
+ protected:
+
+ size_t _mode;
+
+ private:
+
+ map<string, Histo1DPtr> _hists;
+
+ };
+
+
+ struct ATLAS_2017_I1517194_EL : public ATLAS_2017_I1517194 {
+ ATLAS_2017_I1517194_EL() : ATLAS_2017_I1517194("ATLAS_2017_I1517194_EL", 0) { }
+ };
+
+ struct ATLAS_2017_I1517194_MU : public ATLAS_2017_I1517194 {
+ ATLAS_2017_I1517194_MU() : ATLAS_2017_I1517194("ATLAS_2017_I1517194_MU", 1) { }
+ };
+
+
+ // The hook for the plugin system
+ DECLARE_RIVET_PLUGIN(ATLAS_2017_I1517194);
+ DECLARE_RIVET_PLUGIN(ATLAS_2017_I1517194_EL);
+ DECLARE_RIVET_PLUGIN(ATLAS_2017_I1517194_MU);
+
+
+}
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1517194.info b/analyses/pluginATLAS/ATLAS_2017_I1517194.info
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2017_I1517194.info
@@ -0,0 +1,50 @@
+Name: ATLAS_2017_I1517194
+Year: 2017
+Summary: Electroweak $Wjj$ production at 8~TeV
+Experiment: ATLAS
+Collider: LHC
+InspireID: 1517194
+Status: VALIDATED
+Authors:
+ - Christian Johnson <christian.johnson@cern.ch>
+ - Christian Gutschow <chris.g@cern.ch>
+References:
+ - Eur.Phys.J. C77 (2017) no.7, 474
+ - arXiv:1703.04362 [hep-ex]
+Keywords:
+ - VJETS
+ - ELECTROWEAK
+ - VBF
+ - VJJ
+RunInfo:
+ $pp$ to electroweak lepton + neutrino + 2~jets at 8~TeV
+Luminosity_fb: 20.2
+NeedCrossSection: yes
+Beams: [p+, p+]
+Energies: [8000]
+PtCuts: [30.,30.,25.]
+Description:
+ 'Measurements of the electroweak production of a $W$ boson in association with two jets at high dijet invariant mass
+ are performed using $\sqrt{s} = 7$ and 8 TeV proton-proton collision data produced by the Large Hadron Collider,
+ corresponding respectively to 4.7 and 20.2 fb$^{-1}$ of integrated luminosity collected by the ATLAS detector.
+ The measurements are sensitive to the production of a $W$ boson via a triple-gauge-boson vertex and include both
+ the fiducial and differential cross sections of the electroweak process.'
+BibKey: Aaboud:2017fye
+BibTex: '@article{Aaboud:2017fye,
+ author = "Aaboud, Morad and others",
+ title = "{Measurements of electroweak $Wjj$ production and
+ constraints on anomalous gauge couplings with the ATLAS
+ detector}",
+ collaboration = "ATLAS",
+ journal = "Eur. Phys. J.",
+ volume = "C77",
+ year = "2017",
+ number = "7",
+ pages = "474",
+ doi = "10.1140/epjc/s10052-017-5007-2",
+ eprint = "1703.04362",
+ archivePrefix = "arXiv",
+ primaryClass = "hep-ex",
+ reportNumber = "CERN-EP-2017-008",
+ SLACcitation = "%%CITATION = ARXIV:1703.04362;%%"
+}'
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1517194.plot b/analyses/pluginATLAS/ATLAS_2017_I1517194.plot
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2017_I1517194.plot
@@ -0,0 +1,898 @@
+# BEGIN PLOT /ATLAS_2017_I1517194/d..
+RatioPlotYMax=2.0
+RatioPlotYMin=0.0
+LegendAlign=r
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d11-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d12-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d13-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d14-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d15-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d16-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d17-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d18-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d19-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d20-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d21-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d22-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d23-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d24-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d25-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d26-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d27-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d28-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d29-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d30-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d31-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d32-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d33-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d34-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d35-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d36-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d37-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d38-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d39-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d40-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d41-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d42-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d43-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d44-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d45-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d46-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d47-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d48-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d49-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d50-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d51-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d52-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d53-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d54-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d55-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d56-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d57-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d58-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d59-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d60-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d61-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d62-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d63-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d64-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d65-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d66-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d67-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d68-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d69-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d70-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d71-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d72-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d73-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d74-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d75-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d76-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d77-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d78-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d79-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d80-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d81-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d82-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d83-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d84-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d85-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d86-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d87-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d88-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d89-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d90-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d91-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d92-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d93-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d94-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d95-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d96-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d97-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d98-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d99-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d100-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d101-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d102-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d103-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d104-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d105-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d106-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d107-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d108-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d109-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d110-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d111-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d112-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d113-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d114-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d115-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d116-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d117-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d118-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d119-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d120-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d121-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d122-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d123-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d124-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d125-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d126-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d127-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d128-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d129-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d130-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d131-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d132-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d133-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d134-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d135-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d136-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d137-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d138-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d139-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d140-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d141-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d142-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d143-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d144-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d145-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d146-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d147-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d148-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194/d149-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\ell\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1517194.yoda b/analyses/pluginATLAS/ATLAS_2017_I1517194.yoda
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2017_I1517194.yoda
@@ -0,0 +1,8081 @@
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d01-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d01-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.600000e+01 5.000000e+00 5.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d01-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d01-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.300000e+01 5.000000e+00 5.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d01-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d01-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.000000e+01 8.000000e+00 8.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d01-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d01-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.900000e+01 5.000000e-01 5.000000e-01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d02-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d02-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t2
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.450000e+02 3.900000e+01 3.900000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d02-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d02-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t2
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.550000e+02 5.100000e+01 5.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d03-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d03-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+9.600000e+01 8.000000e+00 8.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d03-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d03-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+8.900000e+01 7.000000e+00 7.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d03-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d03-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.300000e+01 1.100000e+01 1.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d03-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d03-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.100000e+01 1.000000e+00 1.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d04-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d04-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.630000e+02 2.100000e+01 2.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d04-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d04-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.340000e+02 2.600000e+01 2.600000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d04-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d04-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+6.400000e+01 3.600000e+01 3.600000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d04-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d04-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.200000e+01 1.000000e+00 1.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d05-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d05-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t5
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.700000e+03 1.100000e+02 1.100000e+02
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d05-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d05-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t5
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.420000e+03 1.500000e+02 1.500000e+02
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d06-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d06-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.300000e+01 2.000000e+00 2.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d06-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d06-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.400000e+01 1.000000e+00 1.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d06-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d06-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.600000e+00 2.100000e+00 2.100000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d06-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d06-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+6.900000e+00 2.000000e-01 2.000000e-01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d07-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d07-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t7
+Type: Scatter1D
+---
+# xval xerr- xerr+
+3.130000e+02 3.000000e+01 3.000000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d07-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d07-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t7
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.650000e+02 3.200000e+01 3.200000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d08-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d08-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t8
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.920000e+02 3.600000e+01 3.600000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d08-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d08-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t8
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.350000e+02 2.800000e+01 2.800000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d09-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d09-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t9
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.440000e+02 3.502856e+01 3.502856e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d09-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d09-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t9
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.440000e+02 1.100000e+01 1.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d10-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d10-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.460000e+02 3.500000e+01 3.500000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d10-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d10-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.650000e+02 3.900000e+01 3.900000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d10-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d10-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.590000e+02 2.700000e+01 2.700000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194/d10-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d10-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.980000e+02 1.200000e+01 1.200000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d11-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d11-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t11
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.749800e-03 4.232811e-04 4.287836e-04
+7.500000e+01 2.500000e+01 2.500000e+01 6.616100e-03 3.022254e-04 3.100313e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.693800e-03 2.513928e-04 2.465816e-04
+1.925000e+02 3.250000e+01 3.250000e+01 1.981800e-03 1.724307e-04 1.687993e-04
+2.625000e+02 3.750000e+01 3.750000e+01 8.348400e-04 3.433320e-04 3.434536e-04
+3.975000e+02 9.750000e+01 9.750000e+01 7.549200e-05 6.703945e-04 6.703707e-04
+6.975000e+02 2.025000e+02 2.025000e+02 9.695400e-06 7.108535e-06 7.150889e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d11-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d11-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t11
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.239800e-03 1.671900e-04 1.537800e-04
+7.500000e+01 2.500000e+01 2.500000e+01 5.782700e-03 3.074600e-04 1.785100e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.876600e-03 1.339900e-04 1.442600e-04
+1.925000e+02 3.250000e+01 3.250000e+01 2.098800e-03 8.731500e-05 1.083800e-04
+2.625000e+02 3.750000e+01 3.750000e+01 9.471300e-04 6.157900e-05 6.167300e-05
+3.975000e+02 9.750000e+01 9.750000e+01 2.586000e-04 1.886600e-05 1.904300e-05
+6.975000e+02 2.025000e+02 2.025000e+02 2.074400e-05 3.918100e-06 3.685900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d11-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d11-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t11
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.484800e-03 3.184600e-04 8.493000e-05
+7.500000e+01 2.500000e+01 2.500000e+01 5.866100e-03 3.147500e-05 2.220000e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.747800e-03 1.022400e-04 4.123400e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.962700e-03 5.974100e-05 2.347300e-04
+2.625000e+02 3.750000e+01 3.750000e+01 9.212000e-04 3.596300e-05 2.579900e-05
+3.975000e+02 9.750000e+01 9.750000e+01 2.621700e-04 1.833200e-05 1.460400e-05
+6.975000e+02 2.025000e+02 2.025000e+02 2.420000e-05 1.322200e-06 1.930400e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d12-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d12-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t12
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 9.751100e-02 3.977561e-02 4.084700e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.765900e-01 5.286942e-02 5.808940e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.206100e+00 1.194382e-01 1.181789e-01
+8.500000e-01 5.000000e-02 5.000000e-02 2.246600e+00 1.386490e-01 1.371997e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.370700e+00 2.434256e-01 2.357765e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.842400e+00 3.555396e-01 3.616982e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d12-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d12-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t12
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 1.590100e-01 8.723300e-03 1.304800e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.869100e-01 2.390800e-02 4.090400e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.207900e+00 1.359500e-01 5.919100e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.344600e+00 9.678800e-02 7.534300e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.009600e+00 1.747300e-01 1.377000e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.347600e+00 2.075000e-01 1.826800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d12-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d12-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t12
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 1.335100e-01 4.507200e-03 1.568300e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.138700e-01 1.995400e-02 0.000000e+00
+7.500000e-01 5.000000e-02 5.000000e-02 1.068000e+00 4.893100e-02 9.925600e-03
+8.500000e-01 5.000000e-02 5.000000e-02 2.306300e+00 4.182800e-02 5.384700e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.241400e+00 1.185300e-01 1.532600e-01
+9.750000e-01 2.500000e-02 2.500000e-02 6.019500e+00 5.855200e-02 1.348000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d13-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d13-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t13
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.338100e-02 1.322149e-02 1.110759e-02
+3.200000e+00 4.000000e-01 4.000000e-01 1.236800e-01 1.453089e-02 1.377971e-02
+4.000000e+00 4.000000e-01 4.000000e-01 2.349200e-01 2.236358e-02 2.037699e-02
+4.800000e+00 4.000000e-01 4.000000e-01 2.834600e-01 3.255250e-02 3.248636e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.637300e-01 1.988253e-02 2.680273e-02
+7.400000e+00 1.400000e+00 1.400000e+00 4.309500e-02 9.407138e-03 8.677072e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d13-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d13-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t13
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 8.621500e-02 5.062100e-03 5.536000e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.400100e-01 7.046500e-03 6.643900e-03
+4.000000e+00 4.000000e-01 4.000000e-01 2.166400e-01 8.359100e-03 9.630700e-03
+4.800000e+00 4.000000e-01 4.000000e-01 3.167200e-01 1.178000e-02 1.072300e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.420800e-01 1.576300e-02 1.181000e-02
+7.400000e+00 1.400000e+00 1.400000e+00 4.237900e-02 4.155600e-03 2.035000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d13-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d13-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t13
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.090400e-01 4.823400e-03 1.074600e-02
+3.200000e+00 4.000000e-01 4.000000e-01 1.739800e-01 6.866900e-03 7.563000e-03
+4.000000e+00 4.000000e-01 4.000000e-01 2.314000e-01 1.125200e-03 7.648700e-03
+4.800000e+00 4.000000e-01 4.000000e-01 2.958200e-01 5.396400e-03 1.608000e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.899700e-01 5.055600e-03 1.239900e-02
+7.400000e+00 1.400000e+00 1.400000e+00 4.279600e-02 5.418600e-03 2.819200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d14-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d14-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t14
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.211900e-03 9.080313e-04 1.006137e-03
+1.400000e+02 2.500000e+01 2.500000e+01 4.935800e-03 2.966745e-04 2.758397e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.289800e-03 2.412451e-04 2.491068e-04
+2.500000e+02 3.000000e+01 3.000000e+01 2.146000e-03 2.152008e-04 2.015250e-04
+3.150000e+02 3.500000e+01 3.500000e+01 1.223400e-03 3.176380e-04 3.070309e-04
+3.925000e+02 4.250000e+01 4.250000e+01 9.110500e-04 1.164833e-04 1.114131e-04
+5.075000e+02 7.250000e+01 7.250000e+01 4.933900e-04 6.944737e-05 6.261648e-05
+7.300000e+02 1.500000e+02 1.500000e+02 8.824000e-05 2.004914e-05 1.974540e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d14-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d14-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t14
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.313200e-03 3.447100e-04 3.244800e-04
+1.400000e+02 2.500000e+01 2.500000e+01 4.565400e-03 1.476900e-04 1.601200e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.443000e-03 1.423500e-04 1.276700e-04
+2.500000e+02 3.000000e+01 3.000000e+01 2.332100e-03 1.155800e-04 1.053900e-04
+3.150000e+02 3.500000e+01 3.500000e+01 1.532800e-03 8.221700e-05 8.194200e-05
+3.925000e+02 4.250000e+01 4.250000e+01 9.368800e-04 5.091600e-05 5.667400e-05
+5.075000e+02 7.250000e+01 7.250000e+01 5.123200e-04 2.957000e-05 3.837100e-05
+7.300000e+02 1.500000e+02 1.500000e+02 1.008700e-04 9.784700e-06 8.927000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d14-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d14-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t14
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.274200e-03 3.095900e-04 1.827800e-04
+1.400000e+02 2.500000e+01 2.500000e+01 3.896800e-03 7.233700e-05 1.225600e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.224100e-03 8.615000e-05 7.443500e-05
+2.500000e+02 3.000000e+01 3.000000e+01 2.296100e-03 1.045900e-04 0.000000e+00
+3.150000e+02 3.500000e+01 3.500000e+01 1.655500e-03 7.178700e-05 7.007500e-05
+3.925000e+02 4.250000e+01 4.250000e+01 1.085700e-03 3.625200e-05 5.417900e-05
+5.075000e+02 7.250000e+01 7.250000e+01 6.390900e-04 4.034300e-05 3.477800e-05
+7.300000e+02 1.500000e+02 1.500000e+02 1.320800e-04 0.000000e+00 5.523000e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d15-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d15-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t15
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.935900e+00 1.770283e-01 1.752405e-01
+2.500000e-01 1.000000e-01 1.000000e-01 1.570100e+00 1.140556e-01 1.134172e-01
+5.000000e-01 1.500000e-01 1.500000e-01 1.058600e+00 6.660687e-02 6.792790e-02
+8.250000e-01 1.750000e-01 1.750000e-01 1.895200e-01 2.497173e-02 2.547942e-02
+1.500000e+00 5.000000e-01 5.000000e-01 1.168600e-02 3.338337e-03 3.320034e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d15-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d15-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t15
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.810300e+00 1.208200e-01 5.936800e-02
+2.500000e-01 1.000000e-01 1.000000e-01 1.670500e+00 6.907000e-02 6.500500e-02
+5.000000e-01 1.500000e-01 1.500000e-01 1.022200e+00 3.154400e-02 8.198000e-02
+8.250000e-01 1.750000e-01 1.750000e-01 2.131000e-01 1.859700e-02 1.637900e-02
+1.500000e+00 5.000000e-01 5.000000e-01 1.310600e-02 2.038200e-03 2.017800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d15-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d15-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t15
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.783400e+00 4.256400e-02 5.687700e-04
+2.500000e-01 1.000000e-01 1.000000e-01 1.615900e+00 0.000000e+00 6.360500e-02
+5.000000e-01 1.500000e-01 1.500000e-01 1.042200e+00 1.258100e-02 0.000000e+00
+8.250000e-01 1.750000e-01 1.750000e-01 2.307200e-01 2.185600e-02 1.116500e-03
+1.500000e+00 5.000000e-01 5.000000e-01 1.588700e-02 6.493200e-04 1.492400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d16-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d16-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t16
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.632100e+00 8.139210e-02 8.650309e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.839900e+00 9.080709e-02 9.079465e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.151400e+00 1.621326e-01 1.621340e-01
+6.750000e-01 1.250000e-01 1.250000e-01 4.450200e-01 4.802816e-02 4.379319e-02
+9.000000e-01 1.000000e-01 1.000000e-01 8.375700e-02 1.696566e-02 1.654870e-02
+1.100000e+00 1.000000e-01 1.000000e-01 2.444000e-02 8.960275e-03 9.146675e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d16-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d16-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t16
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.641100e+00 5.361500e-02 9.437600e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.834200e+00 6.979500e-02 4.664700e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.258900e+00 6.173500e-02 4.656100e-02
+6.750000e-01 1.250000e-01 1.250000e-01 3.905900e-01 1.993100e-02 2.938600e-02
+9.000000e-01 1.000000e-01 1.000000e-01 7.355400e-02 9.763500e-03 1.101500e-02
+1.100000e+00 1.000000e-01 1.000000e-01 1.878200e-02 4.898400e-03 5.685500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d16-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d16-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t16
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.469100e+00 1.254200e-01 7.854200e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.710900e+00 5.139400e-02 0.000000e+00
+4.750000e-01 7.500000e-02 7.500000e-02 1.444500e+00 4.751000e-02 1.492600e-01
+6.750000e-01 1.250000e-01 1.250000e-01 4.911600e-01 1.906200e-02 2.794500e-02
+9.000000e-01 1.000000e-01 1.000000e-01 9.905700e-02 1.735600e-02 4.798700e-03
+1.100000e+00 1.000000e-01 1.000000e-01 2.372400e-02 6.956100e-04 5.791000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d17-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d17-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t17
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.453100e-01 2.915590e-02 3.067239e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.652800e-01 1.821431e-02 1.778858e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.127600e-01 1.177660e-02 1.213810e-02
+3.000000e+00 5.000000e-01 5.000000e-01 5.119200e-02 1.000771e-02 8.594720e-03
+6.000000e+00 2.500000e+00 2.500000e+00 2.545900e-02 8.098885e-03 7.657466e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d17-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d17-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t17
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.713800e-01 1.753300e-02 2.481000e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.659600e-01 1.415800e-02 1.203300e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.088600e-01 6.584100e-03 7.909100e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.887500e-02 1.007500e-02 3.023800e-03
+6.000000e+00 2.500000e+00 2.500000e+00 1.492000e-02 2.059200e-03 2.499600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d17-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d17-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t17
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.319500e-01 2.661200e-02 1.470700e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.883800e-01 2.408000e-03 1.495100e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.247000e-01 1.134800e-02 1.348000e-02
+3.000000e+00 5.000000e-01 5.000000e-01 4.325500e-02 5.562300e-03 0.000000e+00
+6.000000e+00 2.500000e+00 2.500000e+00 1.171900e-02 0.000000e+00 4.214800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d18-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d18-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.440400e-03 1.444966e-04 1.591914e-04
+5.800000e+02 3.500000e+01 3.500000e+01 3.204600e-03 1.031389e-04 1.037089e-04
+6.550000e+02 4.000000e+01 4.000000e+01 2.167800e-03 5.068799e-05 4.855705e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.470600e-03 5.533391e-05 3.547807e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.771800e-04 3.221458e-05 4.100677e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.087400e-04 2.092369e-05 2.283223e-05
+1.042500e+03 5.750000e+01 5.750000e+01 3.716000e-04 2.189913e-05 1.686269e-05
+1.150000e+03 5.000000e+01 5.000000e+01 2.132600e-04 1.484543e-05 1.327452e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.349800e-04 1.005004e-05 9.475520e-06
+1.425000e+03 7.500000e+01 7.500000e+01 8.606100e-05 7.638507e-06 7.559277e-06
+1.750000e+03 2.500000e+02 2.500000e+02 2.592100e-05 4.816414e-06 4.932878e-06
+2.350000e+03 3.500000e+02 3.500000e+02 4.134000e-06 9.226464e-07 6.248307e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.995900e-07 9.477605e-08 9.183850e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d18-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d18-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.327300e-03 8.959800e-05 6.073900e-05
+5.800000e+02 3.500000e+01 3.500000e+01 3.231200e-03 6.876500e-05 5.383300e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.199600e-03 2.816700e-05 2.209800e-04
+7.400000e+02 4.500000e+01 4.500000e+01 1.458300e-03 4.772800e-05 2.290900e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.367200e-04 2.534400e-05 2.149900e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.019500e-04 1.968300e-05 2.233300e-05
+1.042500e+03 5.750000e+01 5.750000e+01 3.734400e-04 1.441100e-05 9.575900e-06
+1.150000e+03 5.000000e+01 5.000000e+01 2.386900e-04 9.187000e-06 1.263300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.464900e-04 6.239300e-06 5.689100e-06
+1.425000e+03 7.500000e+01 7.500000e+01 8.480900e-05 5.210700e-06 4.098200e-06
+1.750000e+03 2.500000e+02 2.500000e+02 2.961900e-05 1.367000e-06 1.856200e-06
+2.350000e+03 3.500000e+02 3.500000e+02 4.342600e-06 4.945700e-07 4.660800e-07
+3.350000e+03 6.500000e+02 6.500000e+02 2.395100e-07 7.790500e-08 7.294600e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d18-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d18-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.216800e-03 6.697900e-05 5.900400e-05
+5.800000e+02 3.500000e+01 3.500000e+01 3.184000e-03 3.231100e-05 2.809700e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.170600e-03 1.266500e-05 9.978400e-06
+7.400000e+02 4.500000e+01 4.500000e+01 1.446000e-03 6.956800e-06 5.955400e-06
+8.325000e+02 4.750000e+01 4.750000e+01 9.513000e-04 7.448400e-06 8.316700e-06
+9.325000e+02 5.250000e+01 5.250000e+01 6.213000e-04 8.686500e-06 9.835200e-06
+1.042500e+03 5.750000e+01 5.750000e+01 3.894000e-04 7.584600e-06 8.678800e-06
+1.150000e+03 5.000000e+01 5.000000e+01 2.527200e-04 6.468300e-06 7.434000e-06
+1.275000e+03 7.500000e+01 7.500000e+01 1.538600e-04 4.744300e-06 5.490300e-06
+1.425000e+03 7.500000e+01 7.500000e+01 9.608800e-05 4.001700e-06 5.471800e-06
+1.750000e+03 2.500000e+02 2.500000e+02 3.347500e-05 1.720700e-06 2.048000e-06
+2.350000e+03 3.500000e+02 3.500000e+02 4.742900e-06 3.186000e-07 3.818100e-07
+3.350000e+03 6.500000e+02 6.500000e+02 2.798700e-07 2.478700e-08 3.030100e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d18-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d18-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.056200e-03 0.000000e+00 8.612300e-05
+5.800000e+02 3.500000e+01 3.500000e+01 3.039100e-03 0.000000e+00 9.947800e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.138100e-03 0.000000e+00 6.928600e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.438800e-03 1.350100e-05 7.192600e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.003600e-03 1.038500e-04 0.000000e+00
+9.325000e+02 5.250000e+01 5.250000e+01 6.275600e-04 3.510700e-06 1.274000e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.088800e-04 1.119200e-05 0.000000e+00
+1.150000e+03 5.000000e+01 5.000000e+01 2.760400e-04 1.666400e-05 0.000000e+00
+1.275000e+03 7.500000e+01 7.500000e+01 1.768400e-04 7.752600e-06 1.623600e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.029100e-04 5.546300e-06 6.072800e-06
+1.750000e+03 2.500000e+02 2.500000e+02 4.181800e-05 2.889700e-06 2.327600e-06
+2.350000e+03 3.500000e+02 3.500000e+02 6.797600e-06 2.692200e-07 5.952000e-08
+3.350000e+03 6.500000e+02 6.500000e+02 5.375300e-07 1.629000e-07 1.112500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d19-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d19-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.771700e-03 1.665906e-04 1.679781e-04
+3.750000e+01 1.250000e+01 1.250000e+01 9.135000e-03 2.472353e-04 2.857557e-04
+6.250000e+01 1.250000e+01 1.250000e+01 8.020600e-03 3.544786e-04 3.577800e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.862500e-03 1.536794e-04 1.511097e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.882600e-03 1.629814e-04 1.499845e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.400100e-03 1.735127e-04 1.533771e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.470600e-03 1.385143e-04 1.326091e-04
+2.075000e+02 1.750000e+01 1.750000e+01 8.778400e-04 8.351002e-05 7.955276e-05
+2.425000e+02 1.750000e+01 1.750000e+01 5.066500e-04 3.164659e-05 3.288326e-05
+2.800000e+02 2.000000e+01 2.000000e+01 2.900700e-04 2.658457e-05 2.569169e-05
+3.975000e+02 9.750000e+01 9.750000e+01 5.744000e-05 1.314632e-05 1.329779e-05
+6.975000e+02 2.025000e+02 2.025000e+02 3.443700e-06 1.236977e-06 1.347234e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d19-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d19-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.122500e-03 2.377800e-04 8.118200e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.598800e-03 1.612200e-04 1.580800e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.809600e-03 2.112400e-04 9.228700e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.815200e-03 8.969100e-05 1.013400e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.965400e-03 1.058700e-04 6.823300e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.620900e-03 9.381800e-05 6.233500e-05
+1.750000e+02 1.500000e+01 1.500000e+01 1.710900e-03 6.542500e-05 4.296700e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.046900e-03 4.482200e-05 4.096700e-05
+2.425000e+02 1.750000e+01 1.750000e+01 6.156500e-04 3.230400e-05 3.392600e-05
+2.800000e+02 2.000000e+01 2.000000e+01 3.581000e-04 3.086100e-05 1.729900e-05
+3.975000e+02 9.750000e+01 9.750000e+01 9.328500e-05 8.335000e-06 4.098800e-06
+6.975000e+02 2.025000e+02 2.025000e+02 4.269500e-06 8.239300e-07 6.547400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d19-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d19-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.310300e-03 2.135100e-04 1.843000e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.337100e-03 2.183100e-04 1.891500e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.348600e-03 3.977300e-05 2.923400e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.676900e-03 4.768000e-05 4.924400e-05
+1.150000e+02 1.500000e+01 1.500000e+01 3.922900e-03 5.625400e-05 6.831000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.776300e-03 9.436500e-05 1.168300e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.785000e-03 4.319200e-05 5.379400e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.106300e-03 2.750900e-05 3.121600e-05
+2.425000e+02 1.750000e+01 1.750000e+01 6.841300e-04 1.913100e-05 2.118700e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.047100e-04 1.270500e-05 1.404500e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.148100e-04 4.107200e-06 4.443700e-06
+6.975000e+02 2.025000e+02 2.025000e+02 5.954800e-06 2.747900e-07 2.902200e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d19-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d19-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.071800e-03 7.261800e-05 3.997500e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.574000e-03 1.162800e-04 1.328500e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.877600e-03 2.836300e-04 0.000000e+00
+8.750000e+01 1.250000e+01 1.250000e+01 5.778600e-03 0.000000e+00 3.900900e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.934900e-03 4.599900e-05 1.268900e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.758000e-03 2.008100e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 1.716100e-03 2.574700e-05 1.737100e-04
+2.075000e+02 1.750000e+01 1.750000e+01 1.021400e-03 5.501200e-05 7.856900e-06
+2.425000e+02 1.750000e+01 1.750000e+01 5.876200e-04 3.429700e-05 1.182700e-04
+2.800000e+02 2.000000e+01 2.000000e+01 3.370800e-04 2.142500e-05 4.763200e-05
+3.975000e+02 9.750000e+01 9.750000e+01 9.380200e-05 5.579300e-06 0.000000e+00
+6.975000e+02 2.025000e+02 2.025000e+02 5.149500e-06 6.574600e-07 3.153900e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d20-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d20-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 5.940800e-02 1.317334e-02 1.263845e-02
+4.000000e-01 1.000000e-01 1.000000e-01 1.244000e-01 1.711124e-02 1.808593e-02
+5.500000e-01 5.000000e-02 5.000000e-02 2.259900e-01 4.134359e-02 4.101133e-02
+6.250000e-01 2.500000e-02 2.500000e-02 4.310900e-01 3.877452e-02 3.251981e-02
+6.750000e-01 2.500000e-02 2.500000e-02 5.768200e-01 5.031359e-02 4.845475e-02
+7.250000e-01 2.500000e-02 2.500000e-02 8.748100e-01 2.352047e-01 2.342052e-01
+7.750000e-01 2.500000e-02 2.500000e-02 1.431400e+00 6.251322e-02 6.227322e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.119800e+00 6.563713e-02 6.561217e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.058100e+00 7.745330e-02 7.826197e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.346500e+00 1.068673e-01 1.103522e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.855400e+00 1.268200e-01 1.257618e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d20-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d20-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 9.500500e-02 6.065600e-03 4.343500e-03
+4.000000e-01 1.000000e-01 1.000000e-01 1.654000e-01 4.748400e-03 6.766200e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.277500e-01 1.899100e-02 9.461300e-03
+6.250000e-01 2.500000e-02 2.500000e-02 4.855500e-01 2.436800e-02 1.983900e-02
+6.750000e-01 2.500000e-02 2.500000e-02 6.551700e-01 1.910700e-02 3.326800e-02
+7.250000e-01 2.500000e-02 2.500000e-02 9.611200e-01 4.323300e-02 2.289300e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.352500e+00 3.829100e-02 3.698400e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.003300e+00 4.650100e-02 3.551800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.956900e+00 5.402100e-02 5.587800e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.210100e+00 1.088500e-01 6.004500e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.488200e+00 8.542400e-02 2.846700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d20-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d20-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 8.984800e-02 2.468200e-03 2.902100e-03
+4.000000e-01 1.000000e-01 1.000000e-01 1.597600e-01 5.564900e-03 8.136400e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.333800e-01 1.970000e-02 2.483600e-02
+6.250000e-01 2.500000e-02 2.500000e-02 4.330800e-01 8.620600e-03 1.002600e-02
+6.750000e-01 2.500000e-02 2.500000e-02 6.027200e-01 1.105800e-02 1.310500e-02
+7.250000e-01 2.500000e-02 2.500000e-02 8.619600e-01 1.440900e-02 1.685700e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.271200e+00 1.866400e-02 2.118800e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.892200e+00 1.823100e-02 2.035100e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.849000e+00 6.445700e-03 7.303600e-03
+9.250000e-01 2.500000e-02 2.500000e-02 4.276200e+00 4.736100e-02 3.932600e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.968700e+00 1.375600e-01 1.118400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d20-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d20-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 8.741000e-02 6.002900e-03 1.561500e-02
+4.000000e-01 1.000000e-01 1.000000e-01 1.486300e-01 4.625000e-03 1.209200e-03
+5.500000e-01 5.000000e-02 5.000000e-02 2.762100e-01 3.935100e-03 5.499000e-03
+6.250000e-01 2.500000e-02 2.500000e-02 4.486600e-01 3.522900e-02 7.930400e-03
+6.750000e-01 2.500000e-02 2.500000e-02 5.925600e-01 0.000000e+00 1.334800e-01
+7.250000e-01 2.500000e-02 2.500000e-02 8.671400e-01 0.000000e+00 1.883000e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.264500e+00 6.197300e-03 4.311500e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.012700e+00 6.342200e-02 2.327800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.917200e+00 0.000000e+00 1.106500e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.405900e+00 1.372300e-01 0.000000e+00
+9.750000e-01 2.500000e-02 2.500000e-02 5.819800e+00 9.804100e-02 1.199400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d21-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d21-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.834100e-01 1.560863e-02 1.265172e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.103900e-01 1.438733e-02 1.483056e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.598600e-01 1.295458e-02 1.378529e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.673400e-01 1.262829e-02 1.272665e-02
+3.800000e+00 2.000000e-01 2.000000e-01 3.823200e-01 1.468431e-02 1.540477e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.273400e-01 2.903756e-02 2.956039e-02
+4.800000e+00 4.000000e-01 4.000000e-01 7.306600e-02 6.444668e-03 6.944151e-03
+5.800000e+00 6.000000e-01 6.000000e-01 7.564100e-03 2.980279e-03 1.409301e-03
+7.600000e+00 1.200000e+00 1.200000e+00 8.444000e-05 6.368777e-05 5.526415e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d21-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d21-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.697300e-01 1.330300e-02 1.034100e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.125800e-01 1.158500e-02 7.799200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.543400e-01 5.982800e-03 3.940900e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.674200e-01 1.099300e-02 5.939900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.947200e-01 5.186900e-03 7.095400e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.183000e-01 1.605500e-02 4.775000e-03
+4.800000e+00 4.000000e-01 4.000000e-01 7.827300e-02 3.313300e-03 2.017700e-03
+5.800000e+00 6.000000e-01 6.000000e-01 8.711800e-03 4.518600e-04 1.131500e-03
+7.600000e+00 1.200000e+00 1.200000e+00 3.968100e-05 2.123100e-05 4.692500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d21-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d21-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.697300e-01 6.193400e-03 6.375700e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.745000e-01 3.701800e-03 3.341900e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.631500e-01 1.789100e-03 1.517200e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.399400e-01 1.249100e-03 1.873000e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.343600e-01 5.382700e-03 4.828000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 1.775400e-01 2.925800e-03 2.870600e-03
+4.800000e+00 4.000000e-01 4.000000e-01 5.926700e-02 1.611700e-03 1.896800e-03
+5.800000e+00 6.000000e-01 6.000000e-01 7.319000e-03 4.508800e-04 5.522900e-04
+7.600000e+00 1.200000e+00 1.200000e+00 4.830200e-05 4.906100e-06 6.252100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d21-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d21-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.098700e-01 2.573700e-03 1.575600e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.439500e-01 3.798600e-03 2.151100e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.848900e-01 2.224400e-02 0.000000e+00
+3.400000e+00 2.000000e-01 2.000000e-01 4.566900e-01 1.668100e-03 4.104700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.514800e-01 7.027200e-04 2.169200e-02
+4.200000e+00 2.000000e-01 2.000000e-01 1.866400e-01 3.426200e-03 1.624400e-03
+4.800000e+00 4.000000e-01 4.000000e-01 6.674700e-02 2.036000e-03 0.000000e+00
+5.800000e+00 6.000000e-01 6.000000e-01 1.068200e-02 7.713500e-04 1.641900e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.578200e-04 3.405200e-05 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d22-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d22-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.388000e-03 4.975407e-04 5.599362e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.018200e-03 2.580735e-04 2.767615e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.820600e-03 1.941004e-04 2.077425e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.299200e-03 1.483642e-04 1.483644e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.304900e-03 1.654952e-04 1.606496e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.745100e-03 1.369758e-04 1.374536e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.431500e-03 9.879302e-05 9.193812e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.526100e-03 7.596880e-05 6.456659e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.702500e-04 4.695736e-05 5.217334e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.443200e-04 6.360786e-05 6.124815e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.943800e-04 2.632154e-05 2.572892e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.496300e-04 1.730628e-05 1.676646e-05
+4.575000e+02 2.250000e+01 2.250000e+01 8.145300e-05 1.175250e-05 1.107143e-05
+5.300000e+02 5.000000e+01 5.000000e+01 2.625100e-05 5.547672e-06 5.448345e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.068100e-05 2.657746e-06 2.575246e-06
+8.425000e+02 1.575000e+02 1.575000e+02 5.869200e-07 4.266142e-07 4.151498e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d22-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d22-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.915000e-03 4.964300e-04 1.112100e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.875800e-03 1.244800e-04 1.396700e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.883500e-03 1.008100e-04 6.921800e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.328100e-03 1.103000e-04 1.083300e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.349300e-03 1.493200e-04 1.086200e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.825900e-03 1.552300e-04 6.192000e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.425600e-03 6.284200e-05 7.292800e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.498300e-03 8.801600e-05 4.130800e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.873700e-04 3.762500e-05 4.230300e-05
+3.325000e+02 1.750000e+01 1.750000e+01 5.112700e-04 3.399200e-05 2.095900e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.952300e-04 2.400800e-05 1.614900e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.623100e-04 1.468600e-05 1.149700e-05
+4.575000e+02 2.250000e+01 2.250000e+01 8.975500e-05 9.267100e-06 7.890200e-06
+5.300000e+02 5.000000e+01 5.000000e+01 3.505200e-05 4.447700e-06 3.988900e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.086900e-05 2.004100e-06 1.758700e-06
+8.425000e+02 1.575000e+02 1.575000e+02 1.546300e-06 4.088400e-07 4.524600e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d22-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d22-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.317500e-03 1.055300e-04 1.081200e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.462000e-03 1.142300e-04 1.047500e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.247500e-03 1.100500e-05 1.534300e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.107400e-03 5.019600e-05 4.071500e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.824200e-03 3.300700e-05 3.122200e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.258700e-03 2.723000e-05 2.975100e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.841300e-03 2.738300e-05 2.780400e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.844500e-03 2.273200e-05 2.267200e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.127000e-03 2.055900e-05 2.169400e-05
+3.325000e+02 1.750000e+01 1.750000e+01 6.913400e-04 1.457200e-05 1.522500e-05
+3.700000e+02 2.000000e+01 2.000000e+01 3.961000e-04 1.201800e-05 1.289300e-05
+4.125000e+02 2.250000e+01 2.250000e+01 2.268900e-04 7.501500e-06 8.057600e-06
+4.575000e+02 2.250000e+01 2.250000e+01 1.283600e-04 3.885000e-06 4.208300e-06
+5.300000e+02 5.000000e+01 5.000000e+01 5.249100e-05 2.199100e-06 2.379700e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.628200e-05 8.408800e-07 9.309900e-07
+8.425000e+02 1.575000e+02 1.575000e+02 2.382200e-06 1.390900e-07 1.542100e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d22-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d22-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.495700e-03 8.486400e-05 1.967500e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.826500e-03 8.422000e-05 2.457500e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.566200e-03 0.000000e+00 1.552100e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.448600e-03 4.563300e-05 1.646200e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.743300e-03 3.242700e-04 8.462000e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.096500e-03 4.776300e-05 1.350700e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.736100e-03 1.944500e-04 0.000000e+00
+2.650000e+02 1.500000e+01 1.500000e+01 1.678700e-03 6.022500e-07 5.423100e-05
+2.975000e+02 1.750000e+01 1.750000e+01 9.884900e-04 0.000000e+00 1.110200e-04
+3.325000e+02 1.750000e+01 1.750000e+01 6.009400e-04 2.521500e-05 3.396300e-07
+3.700000e+02 2.000000e+01 2.000000e+01 3.612900e-04 1.601000e-05 2.103800e-05
+4.125000e+02 2.250000e+01 2.250000e+01 2.155900e-04 3.543600e-05 0.000000e+00
+4.575000e+02 2.250000e+01 2.250000e+01 1.092100e-04 2.428700e-06 4.792000e-06
+5.300000e+02 5.000000e+01 5.000000e+01 4.622000e-05 4.877400e-06 4.323600e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.567800e-05 0.000000e+00 1.910600e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.466200e-06 5.122400e-07 4.625500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d23-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d23-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t23
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.258400e-03 2.478400e-04 2.465506e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.317000e-03 4.732787e-04 4.975421e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.335500e-03 2.929429e-04 2.899776e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.543400e-03 2.794172e-04 2.773066e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.532000e-03 2.552473e-04 2.486133e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.887200e-03 2.285658e-04 2.546337e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.656500e-03 1.536124e-04 1.446930e-04
+2.250000e+02 3.500000e+01 3.500000e+01 9.632900e-04 1.614283e-04 1.612225e-04
+3.775000e+02 1.175000e+02 1.175000e+02 2.131500e-04 2.621424e-05 2.707416e-05
+6.975000e+02 2.025000e+02 2.025000e+02 9.516400e-06 5.034262e-06 5.433003e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d23-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d23-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t23
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.528200e-03 1.405600e-04 1.683900e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.247400e-03 2.281100e-04 3.308900e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.673100e-03 2.222800e-04 2.188800e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.450300e-03 2.732900e-04 1.859700e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.162500e-03 1.765200e-04 1.659600e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.991400e-03 2.047300e-04 1.181500e-04
+1.750000e+02 1.500000e+01 1.500000e+01 2.111500e-03 1.062500e-04 1.279900e-04
+2.250000e+02 3.500000e+01 3.500000e+01 1.188400e-03 5.249100e-05 6.289000e-05
+3.775000e+02 1.175000e+02 1.175000e+02 2.516800e-04 1.395700e-05 1.453300e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.784200e-05 2.873500e-06 2.562100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d23-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d23-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t23
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.482800e-03 0.000000e+00 7.189300e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.102400e-03 2.311000e-04 4.403700e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.712400e-03 9.401500e-05 4.128700e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.438900e-03 2.221700e-04 6.095100e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.079300e-03 3.305300e-05 9.262400e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.988700e-03 1.729900e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 2.095100e-03 2.791900e-05 6.174700e-05
+2.250000e+02 3.500000e+01 3.500000e+01 1.214200e-03 1.386900e-04 0.000000e+00
+3.775000e+02 1.175000e+02 1.175000e+02 2.696700e-04 9.227000e-06 5.146700e-05
+6.975000e+02 2.025000e+02 2.025000e+02 2.057000e-05 1.321200e-06 2.035000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d24-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d24-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t24
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 7.792800e-02 1.833950e-02 2.044247e-02
+5.000000e-01 1.000000e-01 1.000000e-01 2.777000e-01 3.353918e-02 3.287087e-02
+6.500000e-01 5.000000e-02 5.000000e-02 5.535500e-01 1.147128e-01 1.149884e-01
+7.500000e-01 5.000000e-02 5.000000e-02 1.213500e+00 9.393261e-02 8.723704e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.941600e+00 1.238391e-01 1.213781e-01
+8.750000e-01 2.500000e-02 2.500000e-02 3.154000e+00 1.771312e-01 1.804688e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.147900e+00 1.903174e-01 1.964199e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.488100e+00 2.557388e-01 2.468413e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d24-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d24-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t24
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.481400e-01 7.422900e-03 1.018000e-02
+5.000000e-01 1.000000e-01 1.000000e-01 2.978800e-01 1.936400e-02 1.543200e-02
+6.500000e-01 5.000000e-02 5.000000e-02 6.244600e-01 3.123400e-02 4.417800e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.183200e+00 8.480900e-02 4.072400e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.941900e+00 1.156800e-01 8.972900e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.802800e+00 9.223500e-02 1.075400e-01
+9.250000e-01 2.500000e-02 2.500000e-02 3.972600e+00 1.421300e-01 1.463800e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.290700e+00 1.398500e-01 1.998700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d24-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d24-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t24
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.402500e-01 4.252400e-03 5.770500e-03
+5.000000e-01 1.000000e-01 1.000000e-01 2.961400e-01 2.774800e-02 0.000000e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.922800e-01 3.841900e-02 5.191000e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.102700e+00 1.762800e-02 2.989200e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.913100e+00 1.261300e-01 0.000000e+00
+8.750000e-01 2.500000e-02 2.500000e-02 2.759400e+00 0.000000e+00 7.099200e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.061100e+00 9.978600e-02 2.478700e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.569800e+00 3.652600e-03 2.650900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d25-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d25-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t25
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.027700e-01 9.284787e-03 9.227062e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.838100e-01 1.233425e-02 1.257055e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.438500e-01 1.876639e-02 1.754049e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.291500e-01 3.401404e-02 3.406569e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.785700e-01 2.200760e-02 2.200187e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.159900e-01 2.129066e-02 2.405541e-02
+5.400000e+00 2.000000e-01 2.000000e-01 2.788200e-01 1.544991e-02 1.579130e-02
+6.000000e+00 4.000000e-01 4.000000e-01 1.215900e-01 1.367189e-02 1.521664e-02
+7.600000e+00 1.200000e+00 1.200000e+00 6.214200e-03 2.677408e-03 2.737504e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d25-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d25-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t25
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.066400e-02 4.421900e-03 4.128500e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.714600e-01 7.679800e-03 5.540700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.656100e-01 1.087200e-02 1.152200e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.485400e-01 1.454300e-02 1.433000e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.994800e-01 1.183400e-02 2.470300e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.057100e-01 1.219700e-02 1.611700e-02
+5.400000e+00 2.000000e-01 2.000000e-01 2.951700e-01 1.185300e-02 1.213600e-02
+6.000000e+00 4.000000e-01 4.000000e-01 1.098900e-01 1.019300e-02 4.662600e-03
+7.600000e+00 1.200000e+00 1.200000e+00 6.909200e-03 6.352300e-04 1.011000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d25-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d25-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t25
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.076300e-01 3.993700e-03 8.913900e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.962200e-01 9.356800e-03 2.597900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.810500e-01 6.926700e-03 8.369800e-04
+4.200000e+00 2.000000e-01 2.000000e-01 3.349500e-01 4.193800e-04 2.094800e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.700100e-01 1.136200e-02 3.674700e-03
+5.000000e+00 2.000000e-01 2.000000e-01 3.729400e-01 6.101600e-03 3.562200e-02
+5.400000e+00 2.000000e-01 2.000000e-01 2.694300e-01 1.992400e-02 5.923400e-03
+6.000000e+00 4.000000e-01 4.000000e-01 1.083900e-01 3.305500e-03 1.056900e-03
+7.600000e+00 1.200000e+00 1.200000e+00 7.858400e-03 5.538000e-04 1.633700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d26-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d26-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t26
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 7.061400e-03 1.064172e-03 1.166735e-03
+1.050000e+02 1.000000e+01 1.000000e+01 6.470000e-03 3.293624e-04 3.673980e-04
+1.250000e+02 1.000000e+01 1.000000e+01 6.337500e-03 3.588134e-04 3.547634e-04
+1.475000e+02 1.250000e+01 1.250000e+01 5.433300e-03 3.102824e-04 2.928755e-04
+1.725000e+02 1.250000e+01 1.250000e+01 3.797800e-03 2.339298e-04 2.325058e-04
+1.975000e+02 1.250000e+01 1.250000e+01 2.992900e-03 2.077934e-04 2.042392e-04
+2.250000e+02 1.500000e+01 1.500000e+01 2.608500e-03 1.839223e-04 1.741546e-04
+2.575000e+02 1.750000e+01 1.750000e+01 1.702400e-03 3.165812e-04 3.128749e-04
+2.975000e+02 2.250000e+01 2.250000e+01 1.628000e-03 1.310364e-04 1.308917e-04
+3.525000e+02 3.250000e+01 3.250000e+01 9.601900e-04 8.899306e-05 8.566333e-05
+5.350000e+02 1.500000e+02 1.500000e+02 1.960700e-04 1.723922e-05 1.863530e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d26-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d26-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t26
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.578400e-03 5.966600e-04 3.197200e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.212200e-03 2.801000e-04 3.227200e-04
+1.250000e+02 1.000000e+01 1.000000e+01 5.955100e-03 2.508000e-04 4.340100e-04
+1.475000e+02 1.250000e+01 1.250000e+01 5.489000e-03 2.305000e-04 2.332200e-04
+1.725000e+02 1.250000e+01 1.250000e+01 4.288800e-03 1.579800e-04 1.869900e-04
+1.975000e+02 1.250000e+01 1.250000e+01 3.477000e-03 1.483100e-04 1.883500e-04
+2.250000e+02 1.500000e+01 1.500000e+01 2.772200e-03 1.528500e-04 1.139600e-04
+2.575000e+02 1.750000e+01 1.750000e+01 2.035600e-03 1.042500e-04 9.601300e-05
+2.975000e+02 2.250000e+01 2.250000e+01 1.496700e-03 7.260700e-05 7.050600e-05
+3.525000e+02 3.250000e+01 3.250000e+01 9.374200e-04 5.267400e-05 4.572600e-05
+5.350000e+02 1.500000e+02 1.500000e+02 1.963800e-04 1.181100e-05 1.111400e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d26-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d26-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t26
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.831200e-03 4.644500e-04 4.732400e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.519100e-03 1.282800e-04 7.878400e-04
+1.250000e+02 1.000000e+01 1.000000e+01 5.305900e-03 8.813600e-05 0.000000e+00
+1.475000e+02 1.250000e+01 1.250000e+01 5.052000e-03 2.434500e-04 0.000000e+00
+1.725000e+02 1.250000e+01 1.250000e+01 4.294600e-03 4.349200e-06 1.952300e-04
+1.975000e+02 1.250000e+01 1.250000e+01 3.480000e-03 5.434700e-05 1.523500e-04
+2.250000e+02 1.500000e+01 1.500000e+01 2.806800e-03 1.424300e-04 2.433900e-04
+2.575000e+02 1.750000e+01 1.750000e+01 2.143500e-03 5.080400e-05 8.905100e-05
+2.975000e+02 2.250000e+01 2.250000e+01 1.584100e-03 6.944500e-05 2.519100e-06
+3.525000e+02 3.250000e+01 3.250000e+01 1.094700e-03 4.639700e-05 0.000000e+00
+5.350000e+02 1.500000e+02 1.500000e+02 2.456800e-04 1.835600e-05 2.551400e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d27-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d27-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t27
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.257700e-03 1.623662e-04 1.653812e-04
+3.750000e+01 1.250000e+01 1.250000e+01 6.563800e-03 2.487683e-04 2.756686e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.973900e-03 2.053310e-04 2.372230e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.919800e-03 1.744184e-04 1.741189e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.670500e-03 1.955170e-04 1.381912e-04
+1.925000e+02 3.250000e+01 3.250000e+01 1.886200e-03 1.007903e-04 9.622518e-05
+2.425000e+02 1.750000e+01 1.750000e+01 8.675200e-04 1.233013e-04 1.234435e-04
+2.800000e+02 2.000000e+01 2.000000e+01 6.001300e-04 5.349723e-05 5.411056e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.514500e-04 2.874679e-05 2.858273e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.329700e-05 2.901476e-06 3.023483e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d27-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d27-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t27
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.755900e-03 1.017500e-04 7.707800e-05
+3.750000e+01 1.250000e+01 1.250000e+01 6.177100e-03 1.755200e-04 1.251900e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.487600e-03 1.485600e-04 1.361700e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.600100e-03 1.306300e-04 1.369300e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.926100e-03 8.067300e-05 6.140100e-05
+1.925000e+02 3.250000e+01 3.250000e+01 2.004200e-03 4.039700e-05 4.930600e-05
+2.425000e+02 1.750000e+01 1.750000e+01 1.050700e-03 4.280800e-05 4.607100e-05
+2.800000e+02 2.000000e+01 2.000000e+01 6.548500e-04 3.254000e-05 4.616100e-05
+3.975000e+02 9.750000e+01 9.750000e+01 2.038700e-04 9.460900e-06 7.438700e-06
+6.975000e+02 2.025000e+02 2.025000e+02 1.462000e-05 1.617800e-06 1.771000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d27-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d27-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t27
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.744500e-03 0.000000e+00 2.339700e-04
+3.750000e+01 1.250000e+01 1.250000e+01 6.356200e-03 1.458600e-04 2.980300e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.649100e-03 1.653000e-04 3.590900e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.556100e-03 4.738600e-05 1.476900e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.854600e-03 9.694100e-05 1.502500e-06
+1.925000e+02 3.250000e+01 3.250000e+01 1.953600e-03 6.338800e-05 4.010600e-05
+2.425000e+02 1.750000e+01 1.750000e+01 1.029700e-03 4.858100e-05 1.291200e-05
+2.800000e+02 2.000000e+01 2.000000e+01 6.563300e-04 2.005900e-05 7.254200e-06
+3.975000e+02 9.750000e+01 9.750000e+01 2.035700e-04 8.780400e-06 2.288400e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.754000e-05 1.256100e-06 9.459300e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d28-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d28-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t28
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 8.706500e-02 2.170353e-02 2.178045e-02
+3.750000e-01 1.250000e-01 1.250000e-01 1.265700e-01 4.358021e-02 2.914534e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.748600e-01 3.738424e-02 4.124443e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.011700e+00 7.569924e-02 7.551336e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.398700e+00 8.535977e-02 8.444028e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.036100e+00 9.061304e-02 8.999392e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.042100e+00 1.075387e-01 1.036678e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.212000e+00 1.340380e-01 1.617700e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.331700e+00 2.198388e-01 2.293161e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d28-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d28-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t28
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 1.243900e-01 5.131200e-03 1.539400e-02
+3.750000e-01 1.250000e-01 1.250000e-01 2.045100e-01 1.311900e-02 6.579400e-03
+6.000000e-01 1.000000e-01 1.000000e-01 5.148300e-01 1.374800e-02 1.912400e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.030800e+00 3.500500e-02 5.802000e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.446300e+00 8.176300e-02 3.934900e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.991200e+00 5.634400e-02 6.071800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.812400e+00 5.698900e-02 6.058900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.918900e+00 9.251200e-02 6.713300e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.096700e+00 1.557500e-01 8.200400e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d28-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d28-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t28
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 1.046400e-01 3.977000e-03 1.583100e-03
+3.750000e-01 1.250000e-01 1.250000e-01 1.648700e-01 3.159600e-05 7.198300e-03
+6.000000e-01 1.000000e-01 1.000000e-01 4.451500e-01 2.469100e-02 5.824100e-03
+7.250000e-01 2.500000e-02 2.500000e-02 9.015000e-01 1.333400e-02 1.073400e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.353000e+00 0.000000e+00 6.110200e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.031900e+00 1.544200e-01 0.000000e+00
+8.750000e-01 2.500000e-02 2.500000e-02 2.827800e+00 3.145600e-02 9.867400e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.134200e+00 1.714900e-02 8.474300e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.623500e+00 0.000000e+00 1.282500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d29-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d29-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t29
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.430700e-01 1.253435e-02 1.231821e-02
+2.600000e+00 2.000000e-01 2.000000e-01 1.790300e-01 1.345455e-02 1.506671e-02
+3.000000e+00 2.000000e-01 2.000000e-01 1.997600e-01 1.358385e-02 1.421876e-02
+3.400000e+00 2.000000e-01 2.000000e-01 2.630500e-01 1.357823e-02 1.792132e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.858900e-01 1.594253e-02 1.480967e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.386800e-01 1.754336e-02 1.759609e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.687900e-01 1.381005e-02 1.354887e-02
+5.000000e+00 2.000000e-01 2.000000e-01 3.283800e-01 1.920619e-02 2.248360e-02
+5.600000e+00 4.000000e-01 4.000000e-01 1.646500e-01 2.112049e-02 1.518484e-02
+7.400000e+00 1.400000e+00 1.400000e+00 9.151600e-03 2.320183e-03 2.192566e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d29-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d29-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t29
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.280800e-01 4.758900e-03 4.389700e-03
+2.600000e+00 2.000000e-01 2.000000e-01 1.568500e-01 4.937800e-03 4.781300e-03
+3.000000e+00 2.000000e-01 2.000000e-01 1.955100e-01 6.700000e-03 5.085700e-03
+3.400000e+00 2.000000e-01 2.000000e-01 2.413800e-01 5.695000e-03 9.029900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.949700e-01 8.067700e-03 6.334000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 3.452600e-01 6.758400e-03 1.114200e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.761700e-01 7.417700e-03 1.191400e-02
+5.000000e+00 2.000000e-01 2.000000e-01 3.576400e-01 1.030500e-02 8.193400e-03
+5.600000e+00 4.000000e-01 4.000000e-01 1.684000e-01 5.452200e-03 3.752600e-03
+7.400000e+00 1.400000e+00 1.400000e+00 9.619900e-03 9.155800e-04 4.311900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d29-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d29-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t29
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.568600e-01 1.511500e-02 6.459200e-04
+2.600000e+00 2.000000e-01 2.000000e-01 1.910300e-01 8.064500e-04 4.665200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 2.302600e-01 8.200800e-03 1.013200e-02
+3.400000e+00 2.000000e-01 2.000000e-01 2.696500e-01 0.000000e+00 4.731600e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.036400e-01 1.827400e-03 7.172600e-03
+4.200000e+00 2.000000e-01 2.000000e-01 3.307800e-01 6.617800e-03 2.997700e-03
+4.600000e+00 2.000000e-01 2.000000e-01 3.329300e-01 4.209300e-03 2.642500e-03
+5.000000e+00 2.000000e-01 2.000000e-01 3.061800e-01 4.385700e-03 1.351500e-02
+5.600000e+00 4.000000e-01 4.000000e-01 1.529600e-01 3.437700e-03 7.283700e-03
+7.400000e+00 1.400000e+00 1.400000e+00 1.039600e-02 1.316000e-03 8.042500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d30-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d30-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t30
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.704800e-03 5.786448e-04 5.807020e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.227000e-03 6.148538e-04 4.409379e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.355700e-03 2.211034e-04 2.218206e-04
+1.525000e+02 1.250000e+01 1.250000e+01 4.681600e-03 1.876372e-04 1.781726e-04
+1.775000e+02 1.250000e+01 1.250000e+01 3.751700e-03 1.616567e-04 1.639011e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.110000e-03 1.444692e-04 1.560933e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.619900e-03 1.296107e-04 1.426961e-04
+2.650000e+02 1.500000e+01 1.500000e+01 2.080900e-03 1.782366e-04 1.793572e-04
+2.975000e+02 1.750000e+01 1.750000e+01 1.918000e-03 1.083583e-04 1.236735e-04
+3.325000e+02 1.750000e+01 1.750000e+01 1.464200e-03 1.512991e-04 1.650513e-04
+3.700000e+02 2.000000e+01 2.000000e+01 1.158300e-03 7.593764e-05 8.961609e-05
+4.125000e+02 2.250000e+01 2.250000e+01 7.211700e-04 6.090580e-05 5.800696e-05
+4.575000e+02 2.250000e+01 2.250000e+01 4.317400e-04 4.128534e-05 3.979584e-05
+5.300000e+02 5.000000e+01 5.000000e+01 2.047400e-04 2.085416e-05 2.066163e-05
+7.300000e+02 1.500000e+02 1.500000e+02 2.924600e-05 5.181227e-06 5.514166e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d30-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d30-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t30
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.437700e-03 2.230800e-04 2.381700e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.225800e-03 2.767100e-04 1.200700e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.251900e-03 1.201000e-04 2.268100e-04
+1.525000e+02 1.250000e+01 1.250000e+01 4.670800e-03 1.036400e-04 1.991500e-04
+1.775000e+02 1.250000e+01 1.250000e+01 3.984900e-03 9.313200e-05 1.327500e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.343600e-03 9.703100e-05 7.760900e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.721100e-03 7.529100e-05 7.913600e-05
+2.650000e+02 1.500000e+01 1.500000e+01 2.209900e-03 8.930000e-05 6.330600e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.781400e-03 5.228200e-05 6.618200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 1.418800e-03 6.033800e-05 5.262400e-05
+3.700000e+02 2.000000e+01 2.000000e+01 1.045200e-03 4.326200e-05 4.865100e-05
+4.125000e+02 2.250000e+01 2.250000e+01 6.916200e-04 3.261800e-05 2.888700e-05
+4.575000e+02 2.250000e+01 2.250000e+01 4.236500e-04 2.255500e-05 2.370100e-05
+5.300000e+02 5.000000e+01 5.000000e+01 1.947200e-04 1.421700e-05 1.172900e-05
+7.300000e+02 1.500000e+02 1.500000e+02 3.171700e-05 2.949400e-06 2.716600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d30-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d30-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t30
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.211800e-03 3.042300e-04 3.552600e-04
+1.050000e+02 1.000000e+01 1.000000e+01 4.461900e-03 0.000000e+00 4.569800e-04
+1.275000e+02 1.250000e+01 1.250000e+01 4.473100e-03 1.056900e-04 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 4.290300e-03 1.220900e-04 0.000000e+00
+1.775000e+02 1.250000e+01 1.250000e+01 3.976900e-03 5.031500e-05 0.000000e+00
+2.050000e+02 1.500000e+01 1.500000e+01 3.256600e-03 0.000000e+00 1.321200e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.786900e-03 6.025400e-05 0.000000e+00
+2.650000e+02 1.500000e+01 1.500000e+01 2.357500e-03 0.000000e+00 8.507400e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.966600e-03 6.833900e-05 7.402300e-05
+3.325000e+02 1.750000e+01 1.750000e+01 1.672100e-03 4.136400e-05 1.510000e-05
+3.700000e+02 2.000000e+01 2.000000e+01 1.257900e-03 6.745200e-05 0.000000e+00
+4.125000e+02 2.250000e+01 2.250000e+01 8.565200e-04 1.101700e-04 2.713300e-06
+4.575000e+02 2.250000e+01 2.250000e+01 5.077800e-04 2.648200e-06 2.871000e-05
+5.300000e+02 5.000000e+01 5.000000e+01 2.504900e-04 1.100700e-05 2.467000e-05
+7.300000e+02 1.500000e+02 1.500000e+02 4.310800e-05 7.085000e-07 1.368100e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d31-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d31-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t31
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.789000e+00 7.290329e-02 7.287356e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.582600e+00 7.671012e-02 7.482703e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.500900e+00 7.179555e-02 7.216504e-02
+4.500000e-01 1.000000e-01 1.000000e-01 1.106300e+00 6.265183e-02 5.067478e-02
+6.000000e-01 5.000000e-02 5.000000e-02 7.775100e-01 4.661478e-02 4.753280e-02
+7.500000e-01 1.000000e-01 1.000000e-01 3.650300e-01 2.890584e-02 2.938186e-02
+1.025000e+00 1.750000e-01 1.750000e-01 1.114400e-01 9.694101e-03 9.780663e-03
+1.850000e+00 6.500000e-01 6.500000e-01 9.433400e-03 1.232201e-03 1.246403e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d31-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d31-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t31
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.613000e+00 4.421500e-02 2.545300e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.565600e+00 3.100800e-02 4.651200e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.584800e+00 3.716700e-02 5.156000e-02
+4.500000e-01 1.000000e-01 1.000000e-01 1.183700e+00 1.901300e-02 3.285300e-02
+6.000000e-01 5.000000e-02 5.000000e-02 7.755200e-01 2.356900e-02 3.262800e-02
+7.500000e-01 1.000000e-01 1.000000e-01 3.992400e-01 1.308700e-02 1.307100e-02
+1.025000e+00 1.750000e-01 1.750000e-01 1.105900e-01 6.835800e-03 4.705500e-03
+1.850000e+00 6.500000e-01 6.500000e-01 7.813600e-03 6.471200e-04 6.451700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d31-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d31-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t31
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.622400e+00 4.205100e-03 2.895500e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.558300e+00 0.000000e+00 2.982000e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.556800e+00 0.000000e+00 2.726000e-02
+4.500000e-01 1.000000e-01 1.000000e-01 1.158300e+00 1.185900e-02 0.000000e+00
+6.000000e-01 5.000000e-02 5.000000e-02 7.657600e-01 2.603800e-02 1.830100e-03
+7.500000e-01 1.000000e-01 1.000000e-01 4.100700e-01 1.227900e-02 2.983300e-03
+1.025000e+00 1.750000e-01 1.750000e-01 1.244700e-01 8.628700e-03 0.000000e+00
+1.850000e+00 6.500000e-01 6.500000e-01 8.707600e-03 7.867400e-04 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d32-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d32-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t32
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.237200e+00 7.213350e-02 7.015125e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.466400e+00 1.038116e-01 8.555071e-02
+3.250000e-01 7.500000e-02 7.500000e-02 1.649600e+00 4.762733e-02 4.750989e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.427300e+00 5.380471e-02 5.434899e-02
+6.750000e-01 1.250000e-01 1.250000e-01 6.488400e-01 2.961493e-02 3.110388e-02
+9.000000e-01 1.000000e-01 1.000000e-01 1.522100e-01 1.512202e-02 1.526235e-02
+1.750000e+00 7.500000e-01 7.500000e-01 9.076000e-03 1.246709e-03 1.355970e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d32-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d32-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t32
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.287400e+00 3.781000e-02 6.025500e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.477600e+00 5.827900e-02 4.128500e-02
+3.250000e-01 7.500000e-02 7.500000e-02 1.694100e+00 3.660300e-02 2.931100e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.396600e+00 2.933300e-02 3.526100e-02
+6.750000e-01 1.250000e-01 1.250000e-01 6.244600e-01 1.603100e-02 1.809900e-02
+9.000000e-01 1.000000e-01 1.000000e-01 1.460900e-01 1.024100e-02 8.134300e-03
+1.750000e+00 7.500000e-01 7.500000e-01 6.797500e-03 4.949300e-04 6.945100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d32-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d32-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t32
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.192800e+00 6.288400e-02 4.246400e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.397100e+00 7.380800e-02 2.195100e-02
+3.250000e-01 7.500000e-02 7.500000e-02 1.613800e+00 0.000000e+00 2.917300e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.441400e+00 1.179200e-02 5.354800e-02
+6.750000e-01 1.250000e-01 1.250000e-01 7.026000e-01 2.780900e-02 9.095100e-03
+9.000000e-01 1.000000e-01 1.000000e-01 1.771200e-01 1.216100e-02 7.301300e-03
+1.750000e+00 7.500000e-01 7.500000e-01 8.006300e-03 5.803800e-04 5.083400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d33-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d33-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t33
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.393500e-01 2.046922e-02 1.981563e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.923000e-01 1.044840e-02 9.031703e-03
+2.000000e+00 5.000000e-01 5.000000e-01 1.174800e-01 8.355426e-03 9.773928e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.733500e-02 5.198399e-03 5.468499e-03
+6.000000e+00 2.500000e+00 2.500000e+00 1.353500e-02 3.708086e-03 3.370465e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d33-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d33-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t33
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.474800e-01 1.055500e-02 1.394400e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.919700e-01 8.680100e-03 6.940400e-03
+2.000000e+00 5.000000e-01 5.000000e-01 1.117600e-01 4.303400e-03 3.381900e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.529200e-02 2.780700e-03 2.294700e-03
+6.000000e+00 2.500000e+00 2.500000e+00 1.349000e-02 1.089000e-03 1.037400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d33-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d33-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t33
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.228100e-01 2.099700e-02 1.563000e-02
+1.000000e+00 5.000000e-01 5.000000e-01 3.077200e-01 8.596300e-03 1.270600e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.213500e-01 7.037800e-03 6.302600e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.816700e-02 1.169500e-03 1.169800e-03
+6.000000e+00 2.500000e+00 2.500000e+00 9.951600e-03 0.000000e+00 1.158600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d34-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d34-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.737500e-03 1.666680e-04 1.850338e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.921900e-03 6.047142e-05 6.091175e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.124600e-03 2.855445e-05 2.857154e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.472600e-03 2.917853e-05 2.275483e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.000300e-03 2.430507e-05 2.304261e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.689200e-04 2.167312e-05 2.336882e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.484100e-04 1.673976e-05 1.533606e-05
+1.150000e+03 5.000000e+01 5.000000e+01 2.937000e-04 1.499780e-05 1.309657e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.893900e-04 1.337960e-05 1.066005e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.209200e-04 8.375443e-06 1.088039e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.968000e-05 3.780448e-06 4.312506e-06
+2.350000e+03 3.500000e+02 3.500000e+02 8.636700e-06 1.116252e-06 9.972329e-07
+3.350000e+03 6.500000e+02 6.500000e+02 8.821400e-07 2.022031e-07 1.899388e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d34-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d34-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.643700e-03 8.146100e-05 2.662300e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.853800e-03 1.940300e-05 2.587500e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.064700e-03 1.499400e-05 8.612500e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.456700e-03 2.873500e-05 1.187400e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.002000e-03 1.017100e-05 1.075200e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.842000e-04 8.243100e-06 1.212200e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.599900e-04 6.143000e-06 1.678700e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.178400e-04 6.939300e-06 1.238900e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.102500e-04 5.147200e-06 5.221800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.307600e-04 3.959200e-06 3.100100e-06
+1.750000e+03 2.500000e+02 2.500000e+02 5.488200e-05 1.225500e-06 1.150300e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.158000e-05 5.154300e-07 5.177500e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.213000e-06 9.985200e-08 1.359400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d34-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d34-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.618200e-03 6.847200e-05 6.017500e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.849700e-03 3.701800e-05 3.216100e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.052900e-03 1.594100e-05 1.315600e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.458200e-03 1.114000e-06 9.146000e-07
+8.325000e+02 4.750000e+01 4.750000e+01 1.010400e-03 6.761400e-06 7.484600e-06
+9.325000e+02 5.250000e+01 5.250000e+01 6.917300e-04 8.662100e-06 1.000900e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.584500e-04 8.445500e-06 9.649900e-06
+1.150000e+03 5.000000e+01 5.000000e+01 3.190100e-04 7.767700e-06 8.926800e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.119300e-04 6.337300e-06 7.338900e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.337400e-04 5.026900e-06 6.102400e-06
+1.750000e+03 2.500000e+02 2.500000e+02 5.519400e-05 2.702400e-06 3.198300e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.139900e-05 7.966200e-07 9.631000e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.200700e-06 1.172900e-07 1.468400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d34-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d34-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.419400e-03 2.626300e-05 5.177600e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.715500e-03 8.987800e-06 4.218100e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.999800e-03 0.000000e+00 2.834800e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.433200e-03 9.737800e-06 2.960100e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.041500e-03 5.033900e-05 0.000000e+00
+9.325000e+02 5.250000e+01 5.250000e+01 7.136400e-04 2.509100e-07 5.515000e-06
+1.042500e+03 5.750000e+01 5.750000e+01 4.869900e-04 2.471000e-06 7.331000e-06
+1.150000e+03 5.000000e+01 5.000000e+01 3.432200e-04 4.655800e-06 4.298100e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.380700e-04 6.638500e-06 8.833200e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.504600e-04 7.648400e-06 2.034700e-06
+1.750000e+03 2.500000e+02 2.500000e+02 6.552800e-05 2.774300e-06 1.296900e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.399400e-05 5.862100e-07 9.503400e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.561600e-06 1.630900e-07 4.800100e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d35-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d35-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.933500e-03 1.324270e-04 1.319493e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.076500e-03 2.131621e-04 2.487014e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.869700e-03 1.732412e-04 1.825174e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.002900e-03 8.404852e-05 8.337837e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.080100e-03 1.263419e-04 1.181810e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.865600e-03 1.729448e-04 1.439489e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.838500e-03 1.101198e-04 1.039252e-04
+2.075000e+02 1.750000e+01 1.750000e+01 1.080300e-03 5.540438e-05 5.189075e-05
+2.425000e+02 1.750000e+01 1.750000e+01 6.179600e-04 2.886477e-05 3.012354e-05
+2.800000e+02 2.000000e+01 2.000000e+01 3.684100e-04 2.177920e-05 2.205978e-05
+3.975000e+02 9.750000e+01 9.750000e+01 7.096900e-05 9.637562e-06 9.983116e-06
+6.975000e+02 2.025000e+02 2.025000e+02 3.443500e-06 7.049974e-07 7.278381e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d35-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d35-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.378700e-03 1.517600e-04 2.223800e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.469400e-03 5.101500e-05 9.025600e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.440900e-03 8.244400e-05 5.268400e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.978500e-03 5.811300e-05 5.480200e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.359900e-03 4.094500e-05 5.730000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.055200e-03 4.307600e-05 3.026300e-05
+1.750000e+02 1.500000e+01 1.500000e+01 2.039900e-03 2.614000e-05 3.703500e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.260800e-03 2.183900e-05 1.994800e-05
+2.425000e+02 1.750000e+01 1.750000e+01 7.283000e-04 1.380700e-05 2.572100e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.181900e-04 1.488400e-05 1.552900e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.091700e-04 3.234800e-06 3.558500e-06
+6.975000e+02 2.025000e+02 2.025000e+02 5.000600e-06 5.161700e-07 3.977300e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d35-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d35-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.571100e-03 1.697800e-04 1.550400e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.492700e-03 1.936100e-04 1.751200e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.208200e-03 3.438500e-05 2.906200e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.853800e-03 4.013100e-05 4.118000e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.251100e-03 5.415300e-05 6.164000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.028000e-03 6.964700e-05 8.156600e-05
+1.750000e+02 1.500000e+01 1.500000e+01 2.051300e-03 4.503300e-05 5.197900e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.272000e-03 2.845900e-05 3.138100e-05
+2.425000e+02 1.750000e+01 1.750000e+01 7.714900e-04 1.860300e-05 1.992900e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.548600e-04 1.108800e-05 1.158100e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.260500e-04 3.504100e-06 3.557000e-06
+6.975000e+02 2.025000e+02 2.025000e+02 6.537500e-06 2.475100e-07 2.579500e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d35-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d35-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.356900e-03 5.197500e-05 2.060400e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.602500e-03 1.209700e-04 6.166400e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.512700e-03 1.501000e-04 5.842200e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.991900e-03 0.000000e+00 1.600700e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.327700e-03 1.226200e-05 8.728600e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.046000e-03 1.050400e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 1.995200e-03 2.327300e-05 1.004600e-04
+2.075000e+02 1.750000e+01 1.750000e+01 1.202900e-03 4.973400e-05 0.000000e+00
+2.425000e+02 1.750000e+01 1.750000e+01 7.151500e-04 8.055100e-06 1.557800e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.119800e-04 1.447900e-05 2.620800e-06
+3.975000e+02 9.750000e+01 9.750000e+01 1.087000e-04 5.432200e-06 3.744600e-06
+6.975000e+02 2.025000e+02 2.025000e+02 6.240200e-06 5.432900e-07 6.584400e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d36-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d36-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 8.122500e-02 1.352140e-02 1.326180e-02
+2.250000e-01 7.500000e-02 7.500000e-02 1.143700e-01 1.663477e-02 1.142533e-02
+3.500000e-01 5.000000e-02 5.000000e-02 1.271500e-01 1.512681e-02 1.596400e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.161500e-01 1.867401e-02 1.905356e-02
+5.500000e-01 5.000000e-02 5.000000e-02 3.501200e-01 2.792869e-02 2.667234e-02
+6.250000e-01 2.500000e-02 2.500000e-02 5.917600e-01 4.321160e-02 3.926561e-02
+6.750000e-01 2.500000e-02 2.500000e-02 7.344900e-01 4.441159e-02 4.303239e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.009500e+00 6.632819e-02 6.590522e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.519000e+00 3.722584e-02 3.723416e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.206900e+00 3.835284e-02 3.784168e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.029600e+00 5.015113e-02 5.043382e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.928900e+00 7.383253e-02 7.527868e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.006300e+00 9.790021e-02 1.114479e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d36-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d36-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.202300e-01 6.211600e-03 3.741400e-03
+2.250000e-01 7.500000e-02 7.500000e-02 1.409700e-01 3.038600e-03 4.526800e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.901900e-01 4.926700e-03 5.335500e-03
+4.500000e-01 5.000000e-02 5.000000e-02 2.664800e-01 5.314100e-03 8.613400e-03
+5.500000e-01 5.000000e-02 5.000000e-02 4.124900e-01 6.902700e-03 8.398800e-03
+6.250000e-01 2.500000e-02 2.500000e-02 6.083600e-01 1.381700e-02 1.152200e-02
+6.750000e-01 2.500000e-02 2.500000e-02 8.041500e-01 1.701300e-02 1.363700e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.107700e+00 2.066300e-02 1.472900e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.518200e+00 2.071200e-02 1.947000e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.090800e+00 2.068100e-02 2.676800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.869400e+00 2.542300e-02 3.118400e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.800300e+00 3.654600e-02 4.110300e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.679200e+00 7.771600e-02 6.736700e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d36-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d36-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.176200e-01 3.778900e-03 4.656300e-03
+2.250000e-01 7.500000e-02 7.500000e-02 1.375700e-01 4.262000e-03 5.147900e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.808400e-01 6.312800e-03 8.116400e-03
+4.500000e-01 5.000000e-02 5.000000e-02 2.441600e-01 6.809900e-03 8.501300e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.905200e-01 1.402100e-02 1.647000e-02
+6.250000e-01 2.500000e-02 2.500000e-02 5.466100e-01 1.315500e-02 1.498300e-02
+6.750000e-01 2.500000e-02 2.500000e-02 7.337600e-01 1.618400e-02 1.883900e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.016900e+00 2.104600e-02 2.477700e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.422900e+00 2.068500e-02 2.250500e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.009400e+00 1.773700e-02 1.814300e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.840200e+00 4.614300e-03 4.046000e-03
+9.250000e-01 2.500000e-02 2.500000e-02 3.950600e+00 5.492300e-02 4.720000e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.083000e+00 1.370900e-01 1.194200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d36-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d36-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.046500e-01 3.535600e-03 8.375800e-04
+2.250000e-01 7.500000e-02 7.500000e-02 1.217600e-01 2.058000e-03 9.735300e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.587500e-01 4.002300e-03 1.130700e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.222200e-01 5.742900e-04 4.499800e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.518000e-01 1.010000e-02 0.000000e+00
+6.250000e-01 2.500000e-02 2.500000e-02 5.401200e-01 3.005400e-02 2.790100e-03
+6.750000e-01 2.500000e-02 2.500000e-02 7.204000e-01 7.377300e-03 3.319600e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.026600e+00 1.074000e-02 5.218800e-03
+7.750000e-01 2.500000e-02 2.500000e-02 1.454700e+00 3.734400e-03 3.749400e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.097200e+00 2.579900e-02 5.751100e-03
+8.750000e-01 2.500000e-02 2.500000e-02 2.942800e+00 2.987300e-02 2.919000e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.039700e+00 5.567300e-02 0.000000e+00
+9.750000e-01 2.500000e-02 2.500000e-02 5.033700e+00 1.585000e-02 8.495600e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d37-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d37-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.985700e-01 1.264129e-02 1.152023e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.687100e-01 1.111696e-02 1.148468e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.271100e-01 8.868828e-03 1.018768e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.621200e-01 6.921333e-03 7.511135e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.161900e-01 8.640365e-03 8.613727e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.586500e-01 9.151680e-03 8.764364e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.411400e-01 6.786680e-03 7.270510e-03
+5.000000e+00 2.000000e-01 2.000000e-01 6.789800e-02 5.659691e-03 5.623306e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.495100e-02 4.305751e-03 3.045384e-03
+6.200000e+00 2.000000e-01 2.000000e-01 7.071900e-03 1.694080e-03 1.603269e-03
+7.600000e+00 1.200000e+00 1.200000e+00 4.397200e-04 1.957244e-04 1.706019e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d37-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d37-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.926100e-01 3.939500e-03 6.037100e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.558500e-01 3.746400e-03 5.975100e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.221100e-01 6.806300e-03 9.456900e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.601500e-01 3.170700e-03 3.596300e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.175800e-01 3.367500e-03 3.143000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.593300e-01 6.356700e-03 4.381600e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.482900e-01 4.272500e-03 2.168500e-03
+5.000000e+00 2.000000e-01 2.000000e-01 7.739500e-02 1.447900e-03 3.490300e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.780200e-02 8.388300e-04 6.688100e-04
+6.200000e+00 2.000000e-01 2.000000e-01 7.506600e-03 1.106900e-03 4.043100e-04
+7.600000e+00 1.200000e+00 1.200000e+00 5.968300e-04 4.654200e-05 8.824600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d37-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d37-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.591600e-01 3.434700e-03 2.984200e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.005800e-01 2.739500e-03 2.366900e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.335600e-01 2.705100e-03 2.007400e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.421000e-01 1.271900e-03 1.053900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.767300e-01 1.434400e-03 1.638400e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.322300e-01 2.152600e-03 2.474100e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.283400e-01 2.583100e-03 3.185700e-03
+5.000000e+00 2.000000e-01 2.000000e-01 6.750400e-02 2.119900e-03 2.513800e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.488900e-02 1.221100e-03 1.629100e-03
+6.200000e+00 2.000000e-01 2.000000e-01 6.623800e-03 5.518200e-04 8.267500e-04
+7.600000e+00 1.200000e+00 1.200000e+00 5.661000e-04 6.045300e-05 9.118600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d37-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d37-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.276100e-01 5.166600e-03 7.224900e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.853200e-01 0.000000e+00 8.155000e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.378500e-01 1.011300e-02 0.000000e+00
+3.400000e+00 2.000000e-01 2.000000e-01 4.483700e-01 3.856600e-03 2.567700e-04
+3.800000e+00 2.000000e-01 2.000000e-01 3.869000e-01 9.072800e-04 6.262900e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.362700e-01 9.595100e-04 2.763900e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.349000e-01 2.209400e-03 0.000000e+00
+5.000000e+00 2.000000e-01 2.000000e-01 7.258000e-02 3.110800e-03 4.607600e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.837600e-02 1.051000e-03 1.942900e-03
+6.200000e+00 2.000000e-01 2.000000e-01 8.507000e-03 1.396200e-03 6.039000e-05
+7.600000e+00 1.200000e+00 1.200000e+00 8.237200e-04 9.201200e-05 2.161600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d38-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d38-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.869000e-03 3.948115e-04 4.033031e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.557400e-03 2.631596e-04 2.844878e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.069300e-03 1.052295e-04 1.168430e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.146000e-03 1.066799e-04 9.007251e-05
+1.775000e+02 1.250000e+01 1.250000e+01 4.959700e-03 1.182551e-04 1.165410e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.550100e-03 1.126133e-04 1.104288e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.255600e-03 8.168077e-05 7.972379e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.423200e-03 7.170626e-05 6.679290e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.590200e-04 4.767594e-05 4.877268e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.796400e-04 3.442721e-05 3.512253e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.896300e-04 2.504993e-05 2.569215e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.568600e-04 1.225020e-05 1.136216e-05
+4.575000e+02 2.250000e+01 2.250000e+01 9.204500e-05 7.699796e-06 7.206928e-06
+5.300000e+02 5.000000e+01 5.000000e+01 3.546500e-05 3.495101e-06 3.369250e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.072900e-05 2.004789e-06 1.968167e-06
+8.425000e+02 1.575000e+02 1.575000e+02 8.339400e-07 4.776545e-07 4.762887e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d38-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d38-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.436400e-03 2.621100e-04 1.198200e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.304600e-03 1.894900e-04 6.331200e-05
+1.275000e+02 1.250000e+01 1.250000e+01 7.010200e-03 5.837400e-05 2.559000e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.155500e-03 4.948800e-05 6.622200e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.032400e-03 4.417300e-05 6.964200e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.612600e-03 5.412500e-05 4.575400e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.326400e-03 3.693700e-05 4.843900e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.466300e-03 3.766600e-05 3.160500e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.918200e-04 1.844800e-05 2.695900e-05
+3.325000e+02 1.750000e+01 1.750000e+01 5.312500e-04 2.358500e-05 1.471100e-05
+3.700000e+02 2.000000e+01 2.000000e+01 3.085300e-04 1.075600e-05 1.423400e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.734100e-04 6.608300e-06 7.148200e-06
+4.575000e+02 2.250000e+01 2.250000e+01 9.624800e-05 4.621200e-06 5.063100e-06
+5.300000e+02 5.000000e+01 5.000000e+01 4.070400e-05 3.289000e-06 2.511600e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.222500e-05 1.220900e-06 1.126500e-06
+8.425000e+02 1.575000e+02 1.575000e+02 1.957400e-06 3.419400e-07 2.825700e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d38-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d38-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.347700e-03 5.593500e-06 2.125700e-05
+1.050000e+02 1.000000e+01 1.000000e+01 6.296100e-03 3.499600e-05 4.331400e-05
+1.275000e+02 1.250000e+01 1.250000e+01 6.534200e-03 1.621500e-05 1.453300e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.079400e-03 3.335400e-05 2.739200e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.346200e-03 2.403300e-05 2.013900e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.902300e-03 9.939600e-06 9.665200e-06
+2.350000e+02 1.500000e+01 1.500000e+01 2.621200e-03 1.150100e-05 8.529200e-06
+2.650000e+02 1.500000e+01 1.500000e+01 1.716000e-03 1.480300e-05 1.257200e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.045300e-03 1.269800e-05 1.169700e-05
+3.325000e+02 1.750000e+01 1.750000e+01 6.395200e-04 1.039300e-05 9.935800e-06
+3.700000e+02 2.000000e+01 2.000000e+01 3.847600e-04 7.477900e-06 7.646200e-06
+4.125000e+02 2.250000e+01 2.250000e+01 2.229400e-04 5.319300e-06 5.796600e-06
+4.575000e+02 2.250000e+01 2.250000e+01 1.229800e-04 3.147500e-06 3.560300e-06
+5.300000e+02 5.000000e+01 5.000000e+01 5.323500e-05 1.671100e-06 1.865300e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.583700e-05 6.502500e-07 7.454400e-07
+8.425000e+02 1.575000e+02 1.575000e+02 2.440700e-06 1.241700e-07 1.433200e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d38-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d38-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.467600e-03 9.445400e-05 2.360600e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.452300e-03 9.176200e-05 1.273600e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.593500e-03 7.974300e-05 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 6.153400e-03 0.000000e+00 2.644500e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.249700e-03 1.252900e-04 1.048800e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.835600e-03 0.000000e+00 1.197900e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.573000e-03 3.335500e-05 0.000000e+00
+2.650000e+02 1.500000e+01 1.500000e+01 1.645000e-03 2.502300e-05 2.169700e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.016200e-03 6.174200e-06 3.150200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 6.441000e-04 2.990300e-05 0.000000e+00
+3.700000e+02 2.000000e+01 2.000000e+01 3.818400e-04 1.317600e-05 2.005300e-06
+4.125000e+02 2.250000e+01 2.250000e+01 2.231300e-04 1.822100e-05 5.658900e-06
+4.575000e+02 2.250000e+01 2.250000e+01 1.248600e-04 3.624900e-06 7.957200e-07
+5.300000e+02 5.000000e+01 5.000000e+01 5.546100e-05 1.851500e-06 4.965600e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.801100e-05 0.000000e+00 2.178800e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.965100e-06 3.640400e-07 2.030200e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d39-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d39-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.364800e+00 4.846605e-02 4.635862e-02
+1.000000e-01 5.000000e-02 5.000000e-02 1.438400e+00 4.449730e-02 3.998126e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.374900e+00 4.223074e-02 3.748985e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.382400e+00 3.299463e-02 3.453453e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.179700e+00 3.464802e-02 3.301143e-02
+5.000000e-01 5.000000e-02 5.000000e-02 9.105100e-01 2.360182e-02 2.415564e-02
+6.000000e-01 5.000000e-02 5.000000e-02 8.281800e-01 2.391483e-02 2.558667e-02
+7.000000e-01 5.000000e-02 5.000000e-02 6.688400e-01 1.935545e-02 1.916168e-02
+8.000000e-01 5.000000e-02 5.000000e-02 4.460100e-01 1.780996e-02 1.922288e-02
+9.250000e-01 7.500000e-02 7.500000e-02 2.734100e-01 1.195067e-02 1.259264e-02
+1.100000e+00 1.000000e-01 1.000000e-01 1.806200e-01 1.542226e-02 1.597271e-02
+1.350000e+00 1.500000e-01 1.500000e-01 7.597300e-02 4.640969e-03 5.404275e-03
+1.650000e+00 1.500000e-01 1.500000e-01 2.107300e-02 2.790816e-03 2.953377e-03
+2.050000e+00 2.500000e-01 2.500000e-01 4.614500e-03 8.474705e-04 8.540180e-04
+2.650000e+00 3.500000e-01 3.500000e-01 4.433600e-04 1.912842e-04 1.796024e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d39-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d39-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.340000e+00 1.768700e-02 2.039800e-02
+1.000000e-01 5.000000e-02 5.000000e-02 1.348800e+00 1.951700e-02 1.607900e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.373300e+00 1.300200e-02 1.758900e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.418700e+00 2.053200e-02 1.947300e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.240500e+00 1.258900e-02 1.170700e-02
+5.000000e-01 5.000000e-02 5.000000e-02 9.534900e-01 1.867300e-02 1.011800e-02
+6.000000e-01 5.000000e-02 5.000000e-02 8.350400e-01 2.020900e-02 9.484200e-03
+7.000000e-01 5.000000e-02 5.000000e-02 6.629900e-01 8.855300e-03 1.124500e-02
+8.000000e-01 5.000000e-02 5.000000e-02 4.486800e-01 7.802100e-03 6.648800e-02
+9.250000e-01 7.500000e-02 7.500000e-02 2.894800e-01 4.710700e-03 5.610800e-03
+1.100000e+00 1.000000e-01 1.000000e-01 1.616600e-01 5.108400e-03 2.928100e-03
+1.350000e+00 1.500000e-01 1.500000e-01 6.796800e-02 1.961300e-03 1.556300e-03
+1.650000e+00 1.500000e-01 1.500000e-01 2.154800e-02 9.118300e-04 9.585000e-04
+2.050000e+00 2.500000e-01 2.500000e-01 4.198600e-03 3.015200e-04 3.839000e-04
+2.650000e+00 3.500000e-01 3.500000e-01 2.037400e-04 5.669200e-05 5.861100e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d39-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d39-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.246500e+00 1.943300e-02 1.690500e-02
+1.000000e-01 5.000000e-02 5.000000e-02 1.252000e+00 2.007000e-02 1.785800e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.230100e+00 1.813900e-02 1.648500e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.257100e+00 1.764700e-02 1.598900e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.131600e+00 8.899400e-03 8.380200e-03
+5.000000e-01 5.000000e-02 5.000000e-02 9.962500e-01 7.983600e-03 9.595800e-03
+6.000000e-01 5.000000e-02 5.000000e-02 9.622300e-01 1.188700e-02 1.390700e-02
+7.000000e-01 5.000000e-02 5.000000e-02 7.572900e-01 1.006100e-02 1.134000e-02
+8.000000e-01 5.000000e-02 5.000000e-02 5.062100e-01 7.437400e-03 8.474900e-03
+9.250000e-01 7.500000e-02 7.500000e-02 3.514300e-01 8.886100e-03 9.969800e-03
+1.100000e+00 1.000000e-01 1.000000e-01 1.900700e-01 4.264200e-03 4.795900e-03
+1.350000e+00 1.500000e-01 1.500000e-01 8.502200e-02 1.929800e-03 2.018600e-03
+1.650000e+00 1.500000e-01 1.500000e-01 3.127600e-02 1.071000e-03 1.210700e-03
+2.050000e+00 2.500000e-01 2.500000e-01 5.223100e-03 2.560700e-04 2.875000e-04
+2.650000e+00 3.500000e-01 3.500000e-01 2.384800e-04 1.462000e-05 1.728000e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d39-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d39-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.403400e+00 3.298400e-02 0.000000e+00
+1.000000e-01 5.000000e-02 5.000000e-02 1.405200e+00 9.437700e-03 6.334600e-03
+2.000000e-01 5.000000e-02 5.000000e-02 1.413300e+00 1.851100e-02 2.031100e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.442900e+00 9.529100e-03 2.912800e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.225900e+00 1.891800e-02 2.859000e-03
+5.000000e-01 5.000000e-02 5.000000e-02 9.026700e-01 2.250600e-03 1.659600e-02
+6.000000e-01 5.000000e-02 5.000000e-02 7.963500e-01 1.087700e-02 1.878700e-02
+7.000000e-01 5.000000e-02 5.000000e-02 6.531900e-01 8.783100e-03 3.790500e-04
+8.000000e-01 5.000000e-02 5.000000e-02 4.262500e-01 0.000000e+00 1.540600e-02
+9.250000e-01 7.500000e-02 7.500000e-02 2.827300e-01 4.356200e-03 1.214400e-02
+1.100000e+00 1.000000e-01 1.000000e-01 1.580600e-01 3.746200e-03 1.291600e-03
+1.350000e+00 1.500000e-01 1.500000e-01 6.800000e-02 5.665800e-04 5.926800e-04
+1.650000e+00 1.500000e-01 1.500000e-01 2.147300e-02 7.799200e-04 4.937200e-04
+2.050000e+00 2.500000e-01 2.500000e-01 4.536500e-03 2.556900e-04 1.983600e-04
+2.650000e+00 3.500000e-01 3.500000e-01 1.892200e-04 6.747600e-05 6.935500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d40-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d40-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.092100e+00 3.106798e-02 3.155427e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.018500e+00 3.261042e-02 3.275854e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.162800e+00 2.888218e-02 2.932710e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.222600e+00 3.679887e-02 3.686037e-02
+2.250000e-01 2.500000e-02 2.500000e-02 1.265700e+00 4.198133e-02 3.813616e-02
+2.750000e-01 2.500000e-02 2.500000e-02 1.328900e+00 3.557280e-02 3.561967e-02
+3.250000e-01 2.500000e-02 2.500000e-02 1.357500e+00 3.641542e-02 3.624554e-02
+3.750000e-01 2.500000e-02 2.500000e-02 1.438400e+00 3.448402e-02 3.442345e-02
+4.250000e-01 2.500000e-02 2.500000e-02 1.314600e+00 3.158142e-02 3.158311e-02
+4.750000e-01 2.500000e-02 2.500000e-02 1.183600e+00 7.406805e-02 7.448768e-02
+5.250000e-01 2.500000e-02 2.500000e-02 1.161100e+00 3.762767e-02 3.800440e-02
+5.750000e-01 2.500000e-02 2.500000e-02 1.146800e+00 2.485644e-02 2.489803e-02
+6.250000e-01 2.500000e-02 2.500000e-02 1.010200e+00 3.103958e-02 3.050361e-02
+6.750000e-01 2.500000e-02 2.500000e-02 8.781000e-01 2.837291e-02 2.830434e-02
+7.250000e-01 2.500000e-02 2.500000e-02 7.318400e-01 2.162921e-02 2.185104e-02
+7.750000e-01 2.500000e-02 2.500000e-02 5.806800e-01 1.976100e-02 1.904239e-02
+8.250000e-01 2.500000e-02 2.500000e-02 4.710600e-01 1.722081e-02 1.747534e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.768200e-01 1.571927e-02 1.620136e-02
+9.250000e-01 2.500000e-02 2.500000e-02 2.961800e-01 1.371480e-02 1.385615e-02
+9.750000e-01 2.500000e-02 2.500000e-02 2.365800e-01 1.112368e-02 1.115901e-02
+1.025000e+00 2.500000e-02 2.500000e-02 1.879500e-01 1.031368e-02 1.003133e-02
+1.075000e+00 2.500000e-02 2.500000e-02 1.347400e-01 9.133185e-03 9.721705e-03
+1.125000e+00 2.500000e-02 2.500000e-02 1.007700e-01 7.617282e-03 7.873269e-03
+1.175000e+00 2.500000e-02 2.500000e-02 8.877400e-02 6.686759e-03 6.552150e-03
+1.250000e+00 5.000000e-02 5.000000e-02 5.083300e-02 3.534430e-03 3.516280e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.948700e-02 3.063042e-03 3.052132e-03
+1.500000e+00 1.000000e-01 1.000000e-01 1.072400e-02 1.203017e-03 1.201783e-03
+1.800000e+00 2.000000e-01 2.000000e-01 1.276900e-03 2.783425e-04 2.824434e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d40-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d40-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.058900e+00 2.440100e-02 2.870700e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.075000e+00 1.942100e-02 2.793500e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.117900e+00 1.888400e-02 3.722800e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.179800e+00 2.483900e-02 2.786300e-02
+2.250000e-01 2.500000e-02 2.500000e-02 1.265200e+00 3.155300e-02 1.714800e-02
+2.750000e-01 2.500000e-02 2.500000e-02 1.320200e+00 1.923900e-02 2.519200e-02
+3.250000e-01 2.500000e-02 2.500000e-02 1.412000e+00 5.713100e-02 1.568400e-02
+3.750000e-01 2.500000e-02 2.500000e-02 1.425600e+00 1.796800e-02 2.732000e-02
+4.250000e-01 2.500000e-02 2.500000e-02 1.363600e+00 2.205900e-02 1.904700e-02
+4.750000e-01 2.500000e-02 2.500000e-02 1.259300e+00 1.483900e-02 2.001100e-02
+5.250000e-01 2.500000e-02 2.500000e-02 1.189600e+00 1.625400e-02 1.656800e-02
+5.750000e-01 2.500000e-02 2.500000e-02 1.094900e+00 3.942300e-02 1.719900e-02
+6.250000e-01 2.500000e-02 2.500000e-02 1.008100e+00 1.360500e-02 1.420700e-01
+6.750000e-01 2.500000e-02 2.500000e-02 8.684100e-01 1.375800e-02 1.759400e-02
+7.250000e-01 2.500000e-02 2.500000e-02 7.206400e-01 1.408000e-02 1.219100e-02
+7.750000e-01 2.500000e-02 2.500000e-02 5.902600e-01 1.658200e-02 2.223300e-02
+8.250000e-01 2.500000e-02 2.500000e-02 4.710300e-01 9.983400e-03 1.482600e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.751400e-01 1.622500e-02 8.091700e-03
+9.250000e-01 2.500000e-02 2.500000e-02 2.900400e-01 1.133200e-02 9.283800e-03
+9.750000e-01 2.500000e-02 2.500000e-02 2.269700e-01 7.585900e-03 6.801000e-03
+1.025000e+00 2.500000e-02 2.500000e-02 1.741400e-01 7.122100e-03 5.601200e-03
+1.075000e+00 2.500000e-02 2.500000e-02 1.318600e-01 5.705100e-03 6.368000e-03
+1.125000e+00 2.500000e-02 2.500000e-02 9.990000e-02 4.566900e-03 5.090200e-03
+1.175000e+00 2.500000e-02 2.500000e-02 7.347300e-02 4.096900e-03 3.696500e-03
+1.250000e+00 5.000000e-02 5.000000e-02 4.924000e-02 2.277600e-03 2.281000e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.680000e-02 1.847100e-03 1.842600e-03
+1.500000e+00 1.000000e-01 1.000000e-01 1.073400e-02 7.668700e-04 9.794000e-04
+1.800000e+00 2.000000e-01 2.000000e-01 1.628600e-03 1.924300e-04 2.586500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d40-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d40-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.195900e+00 1.283400e-02 1.502300e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.201500e+00 1.065700e-02 1.185500e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.228500e+00 8.872800e-03 1.021600e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.275600e+00 6.065100e-03 6.637200e-03
+2.250000e-01 2.500000e-02 2.500000e-02 1.316900e+00 3.881300e-03 3.238400e-03
+2.750000e-01 2.500000e-02 2.500000e-02 1.352300e+00 2.811600e-03 3.149800e-03
+3.250000e-01 2.500000e-02 2.500000e-02 1.389300e+00 7.209400e-03 6.543600e-03
+3.750000e-01 2.500000e-02 2.500000e-02 1.372700e+00 7.557100e-03 7.226700e-03
+4.250000e-01 2.500000e-02 2.500000e-02 1.330400e+00 4.454500e-03 4.945200e-03
+4.750000e-01 2.500000e-02 2.500000e-02 1.222800e+00 7.781300e-03 6.579500e-03
+5.250000e-01 2.500000e-02 2.500000e-02 1.147500e+00 1.642500e-03 2.115600e-03
+5.750000e-01 2.500000e-02 2.500000e-02 1.035900e+00 5.270800e-03 5.003000e-03
+6.250000e-01 2.500000e-02 2.500000e-02 9.380800e-01 4.431300e-03 3.492500e-03
+6.750000e-01 2.500000e-02 2.500000e-02 8.012500e-01 4.041800e-03 3.306700e-03
+7.250000e-01 2.500000e-02 2.500000e-02 6.717300e-01 4.005300e-03 3.314500e-03
+7.750000e-01 2.500000e-02 2.500000e-02 5.560900e-01 1.436500e-03 1.014300e-03
+8.250000e-01 2.500000e-02 2.500000e-02 4.421000e-01 1.241600e-03 1.476800e-03
+8.750000e-01 2.500000e-02 2.500000e-02 3.563200e-01 1.775000e-03 1.817900e-03
+9.250000e-01 2.500000e-02 2.500000e-02 2.712100e-01 1.717300e-03 1.676500e-03
+9.750000e-01 2.500000e-02 2.500000e-02 2.147400e-01 1.241200e-03 1.471300e-03
+1.025000e+00 2.500000e-02 2.500000e-02 1.687000e-01 9.556200e-04 1.066900e-03
+1.075000e+00 2.500000e-02 2.500000e-02 1.313200e-01 9.833600e-04 1.150200e-03
+1.125000e+00 2.500000e-02 2.500000e-02 9.624500e-02 1.248900e-03 1.222400e-03
+1.175000e+00 2.500000e-02 2.500000e-02 7.322800e-02 1.067000e-03 1.110700e-03
+1.250000e+00 5.000000e-02 5.000000e-02 5.152800e-02 1.965200e-03 2.046800e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.555200e-02 5.289700e-04 5.892700e-04
+1.500000e+00 1.000000e-01 1.000000e-01 1.074700e-02 2.766600e-04 3.018000e-04
+1.800000e+00 2.000000e-01 2.000000e-01 1.577400e-03 9.334100e-05 1.177700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d40-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d40-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.006400e+00 2.651100e-02 4.459400e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.041000e+00 3.138200e-02 1.939700e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.085800e+00 2.771400e-02 4.315800e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.160700e+00 5.162200e-02 2.274600e-02
+2.250000e-01 2.500000e-02 2.500000e-02 1.241700e+00 2.946500e-02 4.578600e-02
+2.750000e-01 2.500000e-02 2.500000e-02 1.324100e+00 1.843700e-02 4.872300e-02
+3.250000e-01 2.500000e-02 2.500000e-02 1.374500e+00 1.193200e-02 1.566200e-02
+3.750000e-01 2.500000e-02 2.500000e-02 1.417800e+00 2.793200e-02 1.814500e-02
+4.250000e-01 2.500000e-02 2.500000e-02 1.368400e+00 1.022300e-02 9.238300e-03
+4.750000e-01 2.500000e-02 2.500000e-02 1.301800e+00 3.150100e-02 9.823400e-03
+5.250000e-01 2.500000e-02 2.500000e-02 1.204000e+00 2.169500e-02 2.649500e-02
+5.750000e-01 2.500000e-02 2.500000e-02 1.133300e+00 1.727300e-02 6.940400e-03
+6.250000e-01 2.500000e-02 2.500000e-02 1.024100e+00 2.797200e-02 3.219000e-02
+6.750000e-01 2.500000e-02 2.500000e-02 8.917100e-01 2.951600e-02 0.000000e+00
+7.250000e-01 2.500000e-02 2.500000e-02 7.427700e-01 4.053500e-02 0.000000e+00
+7.750000e-01 2.500000e-02 2.500000e-02 5.917100e-01 1.901600e-04 3.304800e-02
+8.250000e-01 2.500000e-02 2.500000e-02 4.877000e-01 1.963300e-02 5.870300e-03
+8.750000e-01 2.500000e-02 2.500000e-02 3.724000e-01 5.587000e-03 4.653900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 2.982400e-01 7.696900e-03 1.102500e-02
+9.750000e-01 2.500000e-02 2.500000e-02 2.318500e-01 0.000000e+00 1.112200e-02
+1.025000e+00 2.500000e-02 2.500000e-02 1.790100e-01 1.048900e-02 7.040500e-03
+1.075000e+00 2.500000e-02 2.500000e-02 1.332300e-01 7.665800e-03 4.872400e-03
+1.125000e+00 2.500000e-02 2.500000e-02 1.046500e-01 6.651300e-03 2.049700e-03
+1.175000e+00 2.500000e-02 2.500000e-02 7.552400e-02 0.000000e+00 8.733400e-03
+1.250000e+00 5.000000e-02 5.000000e-02 4.978900e-02 2.021200e-03 2.212300e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.532400e-02 1.114800e-03 2.417500e-03
+1.500000e+00 1.000000e-01 1.000000e-01 1.082000e-02 0.000000e+00 1.249500e-03
+1.800000e+00 2.000000e-01 2.000000e-01 1.752000e-03 1.180000e-04 5.657900e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d41-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d41-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.964000e-01 1.607332e-02 1.717396e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.848500e-01 7.374995e-03 6.654775e-03
+2.000000e+00 5.000000e-01 5.000000e-01 8.968700e-02 6.468044e-03 6.752842e-03
+3.000000e+00 5.000000e-01 5.000000e-01 2.270900e-02 3.138601e-03 2.722886e-03
+4.000000e+00 5.000000e-01 5.000000e-01 4.667900e-03 9.714106e-04 8.115541e-04
+6.500000e+00 2.000000e+00 2.000000e+00 1.683300e-03 4.780830e-04 4.506593e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d41-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d41-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.974500e-01 4.962600e-03 5.161900e-03
+1.000000e+00 5.000000e-01 5.000000e-01 2.853700e-01 3.791500e-03 2.628200e-03
+2.000000e+00 5.000000e-01 5.000000e-01 8.776600e-02 1.671000e-03 1.759900e-03
+3.000000e+00 5.000000e-01 5.000000e-01 2.271300e-02 7.866500e-04 5.123500e-04
+4.000000e+00 5.000000e-01 5.000000e-01 5.262600e-03 2.141000e-04 4.450100e-04
+6.500000e+00 2.000000e+00 2.000000e+00 1.437100e-03 1.139900e-04 1.704700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d41-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d41-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.285200e-01 2.975800e-02 2.687500e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.982700e-01 1.574400e-02 1.691700e-02
+2.000000e+00 5.000000e-01 5.000000e-01 6.750600e-02 7.575200e-03 8.807000e-03
+3.000000e+00 5.000000e-01 5.000000e-01 1.000000e-99 0.000000e+00 0.000000e+00
+4.000000e+00 5.000000e-01 5.000000e-01 1.000000e-99 0.000000e+00 0.000000e+00
+6.500000e+00 2.000000e+00 2.000000e+00 1.000000e-99 0.000000e+00 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d41-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d41-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.807900e-01 1.766100e-02 1.722700e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.978700e-01 1.318500e-02 9.317100e-03
+2.000000e+00 5.000000e-01 5.000000e-01 9.355500e-02 4.131100e-03 6.521300e-03
+3.000000e+00 5.000000e-01 5.000000e-01 2.286700e-02 2.761800e-04 1.435100e-03
+4.000000e+00 5.000000e-01 5.000000e-01 4.111000e-03 0.000000e+00 5.716300e-04
+6.500000e+00 2.000000e+00 2.000000e+00 8.071900e-04 8.568600e-05 7.494700e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d42-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d42-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t42
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.462800e-03 7.499147e-04 7.406124e-04
+7.500000e+01 2.500000e+01 2.500000e+01 7.215300e-03 5.754537e-04 5.787028e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.483700e-03 4.720876e-04 4.692823e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.239800e-03 1.940097e-04 1.965313e-04
+5.150000e+02 2.150000e+02 2.150000e+02 7.642600e-05 4.291271e-05 4.259800e-05
+8.150000e+02 8.500000e+01 8.500000e+01 3.737200e-06 3.442953e-04 3.442747e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d42-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d42-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t42
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.366300e-03 2.815300e-04 3.703300e-04
+7.500000e+01 2.500000e+01 2.500000e+01 5.617000e-03 3.670800e-04 3.587300e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.775800e-03 2.768900e-04 2.412400e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.481900e-03 9.808200e-05 1.029800e-04
+5.150000e+02 2.150000e+02 2.150000e+02 1.524100e-04 1.802100e-05 1.859600e-05
+8.150000e+02 8.500000e+01 8.500000e+01 7.551100e-06 6.318500e-06 6.374200e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d42-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d42-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t42
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.550900e-03 4.657300e-04 2.392800e-04
+7.500000e+01 2.500000e+01 2.500000e+01 5.704000e-03 2.641700e-04 2.175700e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.576100e-03 1.452600e-04 1.765400e-05
+2.300000e+02 7.000000e+01 7.000000e+01 1.457600e-03 7.701300e-05 2.489200e-04
+5.150000e+02 2.150000e+02 2.150000e+02 1.547500e-04 1.172200e-05 3.773100e-06
+8.150000e+02 8.500000e+01 8.500000e+01 1.225900e-05 6.416000e-08 7.997900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d43-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d43-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t43
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.825400e-01 4.804469e-02 5.256234e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.627400e+00 2.142801e-01 2.114021e-01
+9.500000e-01 5.000000e-02 5.000000e-02 5.467400e+00 4.834528e-01 4.842489e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d43-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d43-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t43
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.458000e-01 1.775100e-02 2.787700e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.731500e+00 1.090200e-01 8.821700e-02
+9.500000e-01 5.000000e-02 5.000000e-02 4.816400e+00 2.585600e-01 2.326400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d43-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d43-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t43
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.275600e-01 1.348500e-02 0.000000e+00
+8.000000e-01 1.000000e-01 1.000000e-01 1.633100e+00 1.205100e-01 1.407900e-02
+9.500000e-01 5.000000e-02 5.000000e-02 5.140800e+00 0.000000e+00 3.413200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d44-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d44-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t44
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 8.040500e-02 1.809084e-02 1.855774e-02
+4.400000e+00 8.000000e-01 8.000000e-01 2.001600e-01 2.488998e-02 2.451298e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.495500e-01 4.113629e-02 4.162140e-02
+7.400000e+00 1.400000e+00 1.400000e+00 1.026900e-01 1.709198e-02 1.605860e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d44-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d44-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t44
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 8.200600e-02 7.824900e-03 7.288100e-03
+4.400000e+00 8.000000e-01 8.000000e-01 2.052200e-01 1.095700e-02 1.105700e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.500600e-01 2.387300e-02 1.992000e-02
+7.400000e+00 1.400000e+00 1.400000e+00 9.885600e-02 5.658200e-03 8.310200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d44-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d44-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t44
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.045100e-01 3.400700e-03 3.302800e-02
+4.400000e+00 8.000000e-01 8.000000e-01 2.127100e-01 7.506800e-03 0.000000e+00
+5.600000e+00 4.000000e-01 4.000000e-01 2.870300e-01 4.455300e-03 1.426800e-02
+7.400000e+00 1.400000e+00 1.400000e+00 1.013300e-01 1.218200e-02 7.319700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d45-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d45-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t45
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 5.044100e-03 8.141980e-04 7.683542e-04
+1.800000e+02 4.000000e+01 4.000000e+01 3.701600e-03 3.954643e-04 3.997386e-04
+2.675000e+02 4.750000e+01 4.750000e+01 1.582200e-03 2.584380e-04 2.475394e-04
+3.750000e+02 6.000000e+01 6.000000e+01 1.056700e-03 1.982897e-04 1.946652e-04
+5.600000e+02 1.250000e+02 1.250000e+02 4.964500e-04 9.283398e-05 1.016880e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d45-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d45-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t45
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 4.474700e-03 2.669800e-04 3.519000e-04
+1.800000e+02 4.000000e+01 4.000000e+01 3.799800e-03 2.287400e-04 2.140200e-04
+2.675000e+02 4.750000e+01 4.750000e+01 2.111300e-03 1.472800e-04 1.444400e-04
+3.750000e+02 6.000000e+01 6.000000e+01 1.014500e-03 9.289300e-05 8.840900e-05
+5.600000e+02 1.250000e+02 1.250000e+02 4.208800e-04 4.172900e-05 4.030600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d45-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d45-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t45
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 4.513200e-03 5.134400e-04 4.478600e-04
+1.800000e+02 4.000000e+01 4.000000e+01 3.297000e-03 1.464500e-04 5.099500e-05
+2.675000e+02 4.750000e+01 4.750000e+01 2.072700e-03 1.924800e-04 0.000000e+00
+3.750000e+02 6.000000e+01 6.000000e+01 1.129300e-03 0.000000e+00 1.010000e-04
+5.600000e+02 1.250000e+02 1.250000e+02 5.321100e-04 2.994500e-05 4.663600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d46-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d46-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t46
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.764900e+00 3.425195e-01 3.447472e-01
+7.000000e-01 3.000000e-01 3.000000e-01 4.900900e-01 7.924038e-02 7.482411e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d46-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d46-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t46
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.798700e+00 8.229200e-02 8.746100e-02
+7.000000e-01 3.000000e-01 3.000000e-01 4.675100e-01 4.090200e-02 3.642200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d46-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d46-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t46
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.780100e+00 7.337200e-02 3.594900e-02
+7.000000e-01 3.000000e-01 3.000000e-01 4.799400e-01 2.286300e-02 4.606900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d47-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d47-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t47
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.859400e+00 1.383831e-01 1.371311e-01
+5.250000e-01 1.250000e-01 1.250000e-01 8.648800e-01 1.483110e-01 1.494041e-01
+8.250000e-01 1.750000e-01 1.750000e-01 1.143000e-01 3.684675e-02 3.779701e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d47-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d47-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t47
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.962100e+00 6.646300e-02 7.265300e-02
+5.250000e-01 1.250000e-01 1.250000e-01 7.367100e-01 7.076100e-02 5.149600e-02
+8.250000e-01 1.750000e-01 1.750000e-01 8.849300e-02 1.510200e-02 1.640000e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d47-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d47-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t47
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.787900e+00 7.472700e-02 4.901200e-02
+5.250000e-01 1.250000e-01 1.250000e-01 9.465600e-01 3.179200e-02 1.206000e-01
+8.250000e-01 1.750000e-01 1.750000e-01 1.377400e-01 3.181000e-02 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d48-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d48-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t48
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.259500e-01 4.071903e-02 4.353340e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.331100e-01 2.999246e-02 2.778104e-02
+3.000000e+00 1.500000e+00 1.500000e+00 1.409400e-01 3.220689e-02 3.230973e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d48-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d48-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t48
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.340400e-01 2.770900e-02 2.923400e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.317200e-01 2.357400e-02 1.444500e-02
+3.000000e+00 1.500000e+00 1.500000e+00 1.342300e-01 1.156500e-02 2.024000e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d48-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d48-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t48
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.690500e-01 4.568600e-02 8.327700e-03
+1.000000e+00 5.000000e-01 5.000000e-01 2.610700e-01 1.182600e-03 2.935000e-02
+3.000000e+00 1.500000e+00 1.500000e+00 1.698800e-01 8.419100e-03 2.333900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d49-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d49-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.464200e-03 1.996778e-04 2.113957e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.836000e-03 9.182172e-05 8.486924e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.184800e-03 5.965306e-05 5.928028e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.544600e-03 5.350731e-05 5.426567e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.723800e-04 6.713703e-05 6.666637e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.727900e-04 3.266261e-05 3.194779e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.167100e-04 2.703154e-05 2.736909e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.463200e-04 2.138141e-05 1.994644e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.157300e-04 1.707022e-05 1.933633e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.148800e-04 1.051342e-05 1.244345e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.075600e-05 4.292400e-06 4.616306e-06
+2.350000e+03 3.500000e+02 3.500000e+02 6.020500e-06 1.381048e-06 1.010973e-06
+3.350000e+03 6.500000e+02 6.500000e+02 4.115900e-07 1.815897e-07 1.841067e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d49-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d49-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.362400e-03 1.517800e-04 7.976300e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.763800e-03 4.917600e-05 4.543100e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.078900e-03 3.484700e-05 6.022000e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.516000e-03 4.289100e-05 2.805600e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.084100e-03 3.456400e-05 2.558000e-05
+9.325000e+02 5.250000e+01 5.250000e+01 7.263800e-04 1.870300e-05 2.226500e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.991600e-04 1.424200e-05 4.147700e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.393900e-04 1.345400e-05 3.205200e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.167400e-04 9.725900e-06 8.230800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.307500e-04 1.042800e-05 7.351200e-06
+1.750000e+03 2.500000e+02 2.500000e+02 4.830800e-05 2.449800e-06 2.340000e-06
+2.350000e+03 3.500000e+02 3.500000e+02 7.398900e-06 9.804100e-07 7.028100e-07
+3.350000e+03 6.500000e+02 6.500000e+02 3.216200e-07 1.115200e-07 1.137400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d49-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d49-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.340800e-03 6.275200e-05 5.554000e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.727800e-03 3.754100e-05 3.297400e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.047600e-03 1.641100e-05 1.416700e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.513300e-03 1.884800e-06 1.406900e-06
+8.325000e+02 4.750000e+01 4.750000e+01 1.093600e-03 7.142800e-06 6.258100e-06
+9.325000e+02 5.250000e+01 5.250000e+01 7.536900e-04 7.335400e-06 8.193300e-06
+1.042500e+03 5.750000e+01 5.750000e+01 4.879300e-04 7.938800e-06 8.993600e-06
+1.150000e+03 5.000000e+01 5.000000e+01 3.398100e-04 7.353300e-06 8.376900e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.316000e-04 6.621200e-06 7.595800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.364600e-04 4.720900e-06 5.463900e-06
+1.750000e+03 2.500000e+02 2.500000e+02 4.906600e-05 2.178600e-06 2.539400e-06
+2.350000e+03 3.500000e+02 3.500000e+02 7.462200e-06 4.830600e-07 5.763600e-07
+3.350000e+03 6.500000e+02 6.500000e+02 4.745900e-07 3.978200e-08 4.824000e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d49-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d49-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.076200e-03 2.259800e-05 0.000000e+00
+5.800000e+02 3.500000e+01 3.500000e+01 2.594500e-03 5.505600e-05 2.109200e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.979900e-03 0.000000e+00 5.741600e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.483800e-03 2.652200e-05 1.098100e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.120500e-03 5.984700e-05 0.000000e+00
+9.325000e+02 5.250000e+01 5.250000e+01 7.786500e-04 8.528000e-06 1.625300e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.361400e-04 3.902500e-06 2.148600e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.686100e-04 4.868100e-06 2.126300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.547800e-04 7.683900e-06 9.004900e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.563300e-04 6.102600e-06 4.274000e-06
+1.750000e+03 2.500000e+02 2.500000e+02 6.236300e-05 1.035100e-06 2.966500e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.072300e-05 6.190200e-07 1.829600e-06
+3.350000e+03 6.500000e+02 6.500000e+02 7.258400e-07 6.961000e-08 1.417800e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d50-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d50-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.229500e-03 1.760392e-04 1.805021e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.636300e-03 2.391740e-04 2.509045e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.791700e-03 2.040372e-04 1.978798e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.903100e-03 1.655871e-04 1.657681e-04
+1.450000e+02 1.500000e+01 1.500000e+01 3.430400e-03 2.001677e-04 1.964339e-04
+1.925000e+02 3.250000e+01 3.250000e+01 1.805500e-03 1.314386e-04 1.261339e-04
+2.625000e+02 3.750000e+01 3.750000e+01 6.032300e-04 4.792068e-05 4.885793e-05
+5.150000e+02 2.150000e+02 2.150000e+02 3.539900e-05 1.118806e-05 1.125360e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d50-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d50-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.036300e-03 6.760400e-05 1.112300e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.179700e-03 2.209500e-04 1.171000e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.496100e-03 1.463100e-04 1.102000e-04
+1.150000e+02 1.500000e+01 1.500000e+01 5.046700e-03 1.101200e-04 9.157500e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.600100e-03 7.650000e-05 8.250700e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.899000e-03 3.695100e-05 6.108000e-05
+2.625000e+02 3.750000e+01 3.750000e+01 6.468500e-04 2.218100e-05 2.566600e-05
+5.150000e+02 2.150000e+02 2.150000e+02 5.800200e-05 2.510800e-06 3.390100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d50-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d50-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.334000e-03 5.676300e-05 5.180300e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.387100e-03 7.000000e-05 6.461300e-05
+8.750000e+01 1.250000e+01 1.250000e+01 6.563100e-03 1.731800e-05 1.512600e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.897500e-03 9.733100e-06 1.240000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.383800e-03 4.071700e-05 4.674900e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.772500e-03 2.564800e-05 2.992200e-05
+2.625000e+02 3.750000e+01 3.750000e+01 6.140200e-04 9.495300e-06 9.943300e-06
+5.150000e+02 2.150000e+02 2.150000e+02 5.777400e-05 1.226300e-06 1.374600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d50-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d50-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.381400e-03 1.635300e-04 0.000000e+00
+6.250000e+01 1.250000e+01 1.250000e+01 7.233900e-03 2.045000e-04 8.229600e-05
+8.750000e+01 1.250000e+01 1.250000e+01 6.471800e-03 0.000000e+00 2.897600e-04
+1.150000e+02 1.500000e+01 1.500000e+01 5.026500e-03 0.000000e+00 8.197700e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.461800e-03 8.954200e-06 9.398300e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.777400e-03 1.895000e-05 7.372300e-06
+2.625000e+02 3.750000e+01 3.750000e+01 6.069100e-04 2.572100e-06 2.378200e-05
+5.150000e+02 2.150000e+02 2.150000e+02 5.253100e-05 2.034200e-06 1.387600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d51-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d51-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.021200e-01 1.267664e-02 1.298212e-02
+4.500000e-01 1.500000e-01 1.500000e-01 2.207600e-01 2.769733e-02 2.627560e-02
+6.500000e-01 5.000000e-02 5.000000e-02 7.932300e-01 5.151811e-02 5.025837e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.471100e+00 6.159276e-02 6.083139e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.509000e+00 9.585503e-02 9.570895e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.183200e+00 1.134895e-01 1.150631e-01
+9.250000e-01 2.500000e-02 2.500000e-02 3.752800e+00 1.518879e-01 1.516537e-01
+9.750000e-01 2.500000e-02 2.500000e-02 4.089000e+00 1.543104e-01 1.577002e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d51-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d51-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.220100e-01 4.518900e-03 9.244800e-03
+4.500000e-01 1.500000e-01 1.500000e-01 3.111600e-01 7.224300e-03 1.256900e-02
+6.500000e-01 5.000000e-02 5.000000e-02 8.244500e-01 4.298100e-02 1.962800e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.495500e+00 3.266400e-02 2.800800e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.274100e+00 4.610200e-02 5.724300e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.935100e+00 5.674800e-02 5.324900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.575100e+00 6.514400e-02 6.784100e-02
+9.750000e-01 2.500000e-02 2.500000e-02 3.976700e+00 9.147900e-02 7.812900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d51-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d51-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.156100e-01 4.403700e-03 5.437600e-03
+4.500000e-01 1.500000e-01 1.500000e-01 2.631000e-01 7.411500e-03 8.683900e-03
+6.500000e-01 5.000000e-02 5.000000e-02 7.011700e-01 1.146200e-02 1.265600e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.348100e+00 1.296400e-02 1.444500e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.216700e+00 4.095600e-03 2.309800e-03
+8.750000e-01 2.500000e-02 2.500000e-02 2.999700e+00 2.146300e-02 1.822100e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.891400e+00 4.270000e-02 3.788700e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.521500e+00 7.078200e-02 6.142300e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d51-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d51-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 9.199300e-02 0.000000e+00 6.011700e-03
+4.500000e-01 1.500000e-01 1.500000e-01 2.361700e-01 4.630400e-03 0.000000e+00
+6.500000e-01 5.000000e-02 5.000000e-02 6.701500e-01 7.539200e-03 3.591600e-03
+7.500000e-01 5.000000e-02 5.000000e-02 1.411500e+00 0.000000e+00 4.634900e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.238700e+00 2.544500e-02 3.225400e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.063800e+00 1.115200e-01 0.000000e+00
+9.250000e-01 2.500000e-02 2.500000e-02 3.933400e+00 0.000000e+00 5.605500e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.631700e+00 8.503900e-02 2.714100e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d52-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d52-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.585100e-01 2.518342e-02 2.672197e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.202800e-01 2.460143e-02 2.534064e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.931000e-01 1.687880e-02 1.797093e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.616300e-01 1.809483e-02 1.809607e-02
+4.000000e+00 4.000000e-01 4.000000e-01 2.988300e-01 1.424917e-02 1.217896e-02
+4.800000e+00 4.000000e-01 4.000000e-01 6.914100e-02 8.368347e-03 7.255041e-03
+7.000000e+00 1.800000e+00 1.800000e+00 3.395000e-03 6.473179e-04 8.672093e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d52-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d52-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.378200e-01 6.433500e-03 9.734800e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.044000e-01 8.529400e-03 1.097200e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.542900e-01 1.031700e-02 7.285100e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.611600e-01 7.634000e-03 7.996200e-03
+4.000000e+00 4.000000e-01 4.000000e-01 3.109100e-01 4.790400e-03 9.374000e-03
+4.800000e+00 4.000000e-01 4.000000e-01 9.313200e-02 4.360800e-03 2.659600e-03
+7.000000e+00 1.800000e+00 1.800000e+00 3.804900e-03 4.094000e-04 4.730600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d52-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d52-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.923400e-01 4.908300e-03 3.857800e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.344800e-01 4.387700e-03 3.463600e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.633100e-01 3.133200e-03 2.570600e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.337800e-01 1.285400e-03 1.214900e-03
+4.000000e+00 4.000000e-01 4.000000e-01 2.888900e-01 2.503900e-03 3.145100e-03
+4.800000e+00 4.000000e-01 4.000000e-01 8.277700e-02 2.155300e-03 2.719400e-03
+7.000000e+00 1.800000e+00 1.800000e+00 3.639800e-03 1.792500e-04 2.194100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d52-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d52-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.778100e-01 1.067500e-02 0.000000e+00
+2.600000e+00 2.000000e-01 2.000000e-01 4.312200e-01 0.000000e+00 1.555600e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.550200e-01 6.082600e-03 2.484300e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.389700e-01 1.130300e-02 0.000000e+00
+4.000000e+00 4.000000e-01 4.000000e-01 2.945800e-01 0.000000e+00 7.117200e-03
+4.800000e+00 4.000000e-01 4.000000e-01 8.617900e-02 1.615400e-03 0.000000e+00
+7.000000e+00 1.800000e+00 1.800000e+00 3.939400e-03 1.614400e-04 6.160800e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d53-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d53-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.340500e-03 3.722522e-04 2.395128e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.653100e-03 3.321929e-04 3.467350e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.519100e-03 2.240276e-04 2.436738e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.379400e-03 2.045837e-04 1.978199e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.527800e-03 2.223416e-04 2.251322e-04
+2.050000e+02 1.500000e+01 1.500000e+01 4.385000e-03 1.520537e-04 1.592443e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.670000e-03 1.328195e-04 1.378058e-04
+2.650000e+02 1.500000e+01 1.500000e+01 1.797800e-03 9.739703e-05 1.082551e-04
+3.150000e+02 3.500000e+01 3.500000e+01 8.616300e-04 8.359779e-05 8.738209e-05
+4.150000e+02 6.500000e+01 6.500000e+01 2.206100e-04 4.065504e-05 4.063993e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.216700e-05 5.730018e-06 5.618282e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d53-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d53-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.933000e-03 1.368500e-04 2.093900e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.061200e-03 2.334000e-04 1.518500e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.474500e-03 1.310900e-04 1.112400e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.137900e-03 1.142800e-04 1.156800e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.367000e-03 1.069000e-04 1.124600e-04
+2.050000e+02 1.500000e+01 1.500000e+01 4.026100e-03 9.907300e-05 8.043900e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.707900e-03 6.825300e-05 7.547100e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.767900e-03 6.554700e-05 5.563200e-05
+3.150000e+02 3.500000e+01 3.500000e+01 8.826800e-04 2.512700e-05 3.951400e-05
+4.150000e+02 6.500000e+01 6.500000e+01 2.406000e-04 9.303600e-06 1.188700e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.497400e-05 3.529500e-06 2.836700e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d53-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d53-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.368500e-03 7.678900e-05 1.016000e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.435400e-03 2.930000e-05 3.891400e-05
+1.275000e+02 1.250000e+01 1.250000e+01 6.012000e-03 2.458900e-05 2.809900e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.045600e-03 2.644600e-05 2.375300e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.498800e-03 4.430600e-05 3.706400e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.150100e-03 1.428900e-05 1.241200e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.914500e-03 1.523900e-05 1.148200e-05
+2.650000e+02 1.500000e+01 1.500000e+01 2.062300e-03 1.778200e-05 1.193900e-05
+3.150000e+02 3.500000e+01 3.500000e+01 9.659200e-04 1.178500e-05 9.862800e-06
+4.150000e+02 6.500000e+01 6.500000e+01 2.904800e-04 7.166700e-06 6.459100e-06
+5.825000e+02 1.025000e+02 1.025000e+02 3.739800e-05 1.258600e-06 1.421500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d53-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d53-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.181300e-03 1.496200e-04 6.003400e-05
+1.050000e+02 1.000000e+01 1.000000e+01 5.517600e-03 2.552600e-04 2.778900e-05
+1.275000e+02 1.250000e+01 1.250000e+01 5.899600e-03 8.435000e-05 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 5.839100e-03 6.783400e-05 6.978800e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.382100e-03 0.000000e+00 6.059300e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.166900e-03 0.000000e+00 1.995900e-04
+2.350000e+02 1.500000e+01 1.500000e+01 3.038600e-03 2.376700e-05 1.260300e-04
+2.650000e+02 1.500000e+01 1.500000e+01 1.940100e-03 2.828900e-05 5.446300e-05
+3.150000e+02 3.500000e+01 3.500000e+01 1.071000e-03 6.070700e-05 4.676800e-07
+4.150000e+02 6.500000e+01 6.500000e+01 3.052400e-04 2.268800e-06 8.337000e-06
+5.825000e+02 1.025000e+02 1.025000e+02 4.826200e-05 1.483400e-06 4.029900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d54-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d54-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.128800e-03 2.620050e-04 2.899555e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.649900e-03 1.365857e-04 1.343382e-04
+6.550000e+02 4.000000e+01 4.000000e+01 2.033600e-03 8.972807e-05 9.790188e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.463000e-03 7.369309e-05 6.555212e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.101500e-03 5.937838e-05 4.810172e-05
+9.325000e+02 5.250000e+01 5.250000e+01 7.242700e-04 6.319372e-05 7.426883e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.979900e-04 4.593612e-05 4.442757e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.372000e-04 3.600630e-05 3.230795e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.281200e-04 5.344951e-05 4.520928e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.710500e-04 2.235096e-05 2.038130e-05
+1.750000e+03 2.500000e+02 2.500000e+02 7.781400e-05 9.211709e-06 9.863134e-06
+3.000000e+03 1.000000e+03 1.000000e+03 4.450100e-06 1.035972e-06 1.055269e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d54-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d54-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.866500e-03 6.705400e-05 1.330400e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.419600e-03 4.278100e-05 5.760900e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.936500e-03 5.110200e-05 3.922100e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.480000e-03 3.637000e-05 2.943700e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.099600e-03 3.895100e-05 2.495200e-05
+9.325000e+02 5.250000e+01 5.250000e+01 7.932000e-04 2.155700e-05 2.120500e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.644900e-04 1.652600e-05 3.016000e-05
+1.150000e+03 5.000000e+01 5.000000e+01 4.028700e-04 2.143800e-05 1.508400e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.775000e-04 1.403900e-05 1.108400e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.772200e-04 8.951800e-06 9.651300e-06
+1.750000e+03 2.500000e+02 2.500000e+02 7.868200e-05 5.007200e-06 4.138300e-06
+3.000000e+03 1.000000e+03 1.000000e+03 6.509700e-06 4.254800e-07 4.360400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d54-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d54-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.857900e-03 6.863800e-05 6.031800e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.441400e-03 4.315400e-05 3.749800e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.924000e-03 2.031900e-05 1.742100e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.478200e-03 5.211700e-06 7.140200e-06
+8.325000e+02 4.750000e+01 4.750000e+01 1.116600e-03 4.712300e-06 3.505100e-06
+9.325000e+02 5.250000e+01 5.250000e+01 7.835000e-04 6.910300e-06 7.682700e-06
+1.042500e+03 5.750000e+01 5.750000e+01 5.489300e-04 8.016600e-06 9.075900e-06
+1.150000e+03 5.000000e+01 5.000000e+01 4.138100e-04 8.564600e-06 9.779600e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.804300e-04 7.022500e-06 8.104500e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.783300e-04 5.887600e-06 6.839400e-06
+1.750000e+03 2.500000e+02 2.500000e+02 7.794300e-05 3.586900e-06 4.234800e-06
+3.000000e+03 1.000000e+03 1.000000e+03 6.451900e-06 4.741000e-07 5.792000e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d54-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d54-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.694100e-03 4.588300e-05 1.186700e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.354400e-03 4.103500e-05 1.611100e-04
+6.550000e+02 4.000000e+01 4.000000e+01 1.864400e-03 3.899500e-05 9.574800e-06
+7.400000e+02 4.500000e+01 4.500000e+01 1.430600e-03 3.323100e-05 3.800600e-06
+8.325000e+02 4.750000e+01 4.750000e+01 1.103500e-03 1.491100e-06 4.704400e-05
+9.325000e+02 5.250000e+01 5.250000e+01 8.073400e-04 2.663000e-05 1.539800e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.665400e-04 0.000000e+00 3.498800e-05
+1.150000e+03 5.000000e+01 5.000000e+01 4.249600e-04 1.117400e-05 2.483100e-05
+1.275000e+03 7.500000e+01 7.500000e+01 3.121300e-04 2.072200e-05 5.586200e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.972000e-04 2.960700e-06 1.049200e-05
+1.750000e+03 2.500000e+02 2.500000e+02 9.100700e-05 4.209700e-06 5.599100e-07
+3.000000e+03 1.000000e+03 1.000000e+03 8.448800e-06 1.072300e-08 7.075800e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d55-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d55-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.549200e-03 2.524824e-04 2.841926e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.822300e-03 3.242681e-04 3.557233e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.470500e-03 2.433973e-04 2.439199e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.873900e-03 2.234423e-04 2.149565e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.179600e-03 1.084264e-04 9.723728e-05
+6.000000e+02 3.000000e+02 3.000000e+02 2.939500e-05 9.383853e-06 9.503880e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d55-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d55-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.059300e-03 1.180600e-04 6.540700e-05
+6.250000e+01 1.250000e+01 1.250000e+01 6.935900e-03 1.272000e-04 1.378500e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.167900e-03 1.183700e-04 1.659900e-04
+1.300000e+02 3.000000e+01 3.000000e+01 4.269300e-03 6.474800e-05 7.044300e-05
+2.300000e+02 7.000000e+01 7.000000e+01 1.320200e-03 2.689800e-05 2.864400e-05
+6.000000e+02 3.000000e+02 3.000000e+02 4.741800e-05 2.040700e-06 2.860900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d55-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d55-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.207900e-03 5.427800e-05 4.990900e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.049600e-03 2.618500e-05 2.292100e-05
+8.750000e+01 1.250000e+01 1.250000e+01 6.109500e-03 1.780300e-05 1.398800e-05
+1.300000e+02 3.000000e+01 3.000000e+01 4.136600e-03 2.373800e-05 2.731300e-05
+2.300000e+02 7.000000e+01 7.000000e+01 1.298100e-03 1.135600e-05 1.165400e-05
+6.000000e+02 3.000000e+02 3.000000e+02 5.116500e-05 8.963600e-07 1.009400e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d55-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d55-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.188400e-03 1.320500e-05 2.339400e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.118500e-03 2.043000e-04 0.000000e+00
+8.750000e+01 1.250000e+01 1.250000e+01 6.287900e-03 2.211800e-04 0.000000e+00
+1.300000e+02 3.000000e+01 3.000000e+01 4.151200e-03 0.000000e+00 1.346200e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.267700e-03 4.865800e-05 1.848200e-05
+6.000000e+02 3.000000e+02 3.000000e+02 4.812100e-05 7.884400e-07 1.691700e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d56-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d56-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.514700e-01 3.751747e-02 2.130119e-02
+4.500000e-01 1.500000e-01 1.500000e-01 3.266500e-01 4.156937e-02 4.061237e-02
+6.500000e-01 5.000000e-02 5.000000e-02 8.897000e-01 8.108349e-02 7.509931e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.500600e+00 7.684479e-02 7.875645e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.598000e+00 1.087935e-01 1.104730e-01
+9.500000e-01 5.000000e-02 5.000000e-02 3.577300e+00 1.397788e-01 1.588906e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d56-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d56-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.957800e-01 9.968400e-03 5.864100e-03
+4.500000e-01 1.500000e-01 1.500000e-01 4.135400e-01 1.110700e-02 1.130700e-02
+6.500000e-01 5.000000e-02 5.000000e-02 8.999300e-01 2.371600e-02 2.675100e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.519300e+00 3.362200e-02 3.832600e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.421200e+00 3.580800e-02 3.858400e-02
+9.500000e-01 5.000000e-02 5.000000e-02 3.331600e+00 4.430300e-02 4.442800e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d56-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d56-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.912000e-01 4.280800e-03 5.141900e-03
+4.500000e-01 1.500000e-01 1.500000e-01 3.777800e-01 6.925600e-03 8.243600e-03
+6.500000e-01 5.000000e-02 5.000000e-02 8.328200e-01 1.257400e-02 1.376900e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.467100e+00 1.240800e-02 1.466400e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.454800e+00 1.489600e-02 1.157000e-02
+9.500000e-01 5.000000e-02 5.000000e-02 3.538400e+00 5.431100e-02 4.755200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d56-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d56-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.592800e-01 2.592000e-03 1.464100e-02
+4.500000e-01 1.500000e-01 1.500000e-01 3.326200e-01 4.178100e-04 9.219100e-03
+6.500000e-01 5.000000e-02 5.000000e-02 7.922100e-01 4.346700e-02 1.424800e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.469400e+00 1.632700e-02 4.712500e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.559300e+00 4.775900e-03 2.721300e-02
+9.500000e-01 5.000000e-02 5.000000e-02 3.703400e+00 7.325300e-02 1.936400e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d57-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d57-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.020900e-01 2.337438e-02 2.330605e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.414000e-01 2.128435e-02 2.437171e-02
+3.000000e+00 2.000000e-01 2.000000e-01 3.860900e-01 2.054651e-02 2.264921e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.789700e-01 2.085667e-02 2.428364e-02
+3.800000e+00 2.000000e-01 2.000000e-01 4.331800e-01 1.931064e-02 1.911455e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.794300e-01 1.788684e-02 1.655674e-02
+4.800000e+00 4.000000e-01 4.000000e-01 1.441300e-01 1.360667e-02 1.320912e-02
+5.800000e+00 6.000000e-01 6.000000e-01 2.921000e-02 1.074458e-02 5.853417e-03
+7.600000e+00 1.200000e+00 1.200000e+00 4.910500e-04 3.696222e-04 2.965312e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d57-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d57-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.131800e-01 5.568900e-03 8.317900e-03
+2.600000e+00 2.000000e-01 2.000000e-01 2.933900e-01 6.218800e-03 1.134900e-02
+3.000000e+00 2.000000e-01 2.000000e-01 3.813900e-01 7.088100e-03 1.214800e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.505100e-01 7.703700e-03 9.715100e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.414000e-01 1.342000e-02 7.637000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 3.084400e-01 9.782500e-03 7.649800e-03
+4.800000e+00 4.000000e-01 4.000000e-01 1.544100e-01 9.954000e-03 3.189100e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.264500e-02 3.213400e-03 1.571300e-03
+7.600000e+00 1.200000e+00 1.200000e+00 8.210600e-04 1.343000e-04 1.573100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d57-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d57-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.410400e-01 4.783500e-03 3.724600e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.167900e-01 5.495500e-03 4.349800e-03
+3.000000e+00 2.000000e-01 2.000000e-01 3.915800e-01 4.882400e-03 3.733400e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.489200e-01 4.388700e-03 3.257900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.201900e-01 1.333200e-03 1.091000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.953200e-01 3.791500e-03 5.089900e-03
+4.800000e+00 4.000000e-01 4.000000e-01 1.432200e-01 3.242400e-03 3.960400e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.144700e-02 1.697800e-03 2.257300e-03
+7.600000e+00 1.200000e+00 1.200000e+00 8.951300e-04 1.019200e-04 1.461700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d57-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d57-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.522200e-01 5.291200e-03 3.194300e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.301700e-01 2.314200e-03 0.000000e+00
+3.000000e+00 2.000000e-01 2.000000e-01 3.968800e-01 0.000000e+00 1.996900e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.303700e-01 2.412700e-03 2.741700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.115800e-01 1.410000e-02 9.046400e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.828900e-01 1.086800e-02 2.722400e-03
+4.800000e+00 4.000000e-01 4.000000e-01 1.429200e-01 1.452700e-03 1.802300e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.382500e-02 9.918600e-04 1.378600e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.427900e-03 1.394800e-04 5.183800e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d58-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d58-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.960100e-03 5.601968e-04 4.767125e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.229700e-03 2.698135e-04 2.745017e-04
+1.650000e+02 2.500000e+01 2.500000e+01 5.404000e-03 1.892948e-04 2.011164e-04
+2.200000e+02 3.000000e+01 3.000000e+01 2.541500e-03 1.721515e-04 1.769221e-04
+2.825000e+02 3.250000e+01 3.250000e+01 1.104500e-03 9.399695e-05 9.223029e-05
+3.525000e+02 3.750000e+01 3.750000e+01 3.782300e-04 4.733330e-05 4.776250e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.281800e-04 2.227873e-05 2.203128e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.056800e-05 8.897889e-06 8.752365e-06
+8.425000e+02 1.575000e+02 1.575000e+02 4.757400e-10 2.158605e-05 2.158603e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d58-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d58-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.596100e-03 3.457600e-04 1.069400e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.140900e-03 1.603300e-04 1.319400e-04
+1.650000e+02 2.500000e+01 2.500000e+01 5.310000e-03 7.480800e-05 1.583100e-04
+2.200000e+02 3.000000e+01 3.000000e+01 2.755200e-03 5.001100e-05 8.580900e-05
+2.825000e+02 3.250000e+01 3.250000e+01 1.128300e-03 3.521600e-05 3.907100e-05
+3.525000e+02 3.750000e+01 3.750000e+01 4.258100e-04 2.307300e-05 1.763000e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.404700e-04 9.069100e-06 1.346600e-05
+5.825000e+02 1.025000e+02 1.025000e+02 2.965200e-05 2.811900e-06 2.971000e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.545900e-06 6.840100e-07 6.527900e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d58-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d58-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 6.945400e-03 8.267100e-05 1.108000e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.906400e-03 1.917200e-05 2.013900e-05
+1.650000e+02 2.500000e+01 2.500000e+01 5.440600e-03 3.022500e-05 2.197100e-05
+2.200000e+02 3.000000e+01 3.000000e+01 2.931100e-03 2.904300e-05 2.260200e-05
+2.825000e+02 3.250000e+01 3.250000e+01 1.201200e-03 1.480000e-05 1.198000e-05
+3.525000e+02 3.750000e+01 3.750000e+01 4.618700e-04 6.745900e-06 6.317300e-06
+4.350000e+02 4.500000e+01 4.500000e+01 1.697900e-04 6.088700e-06 5.403400e-06
+5.825000e+02 1.025000e+02 1.025000e+02 3.728700e-05 1.398200e-06 1.137000e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.267000e-06 1.110400e-07 1.279900e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d58-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d58-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 6.721900e-03 2.133300e-05 2.546300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.530400e-03 2.421000e-04 1.258800e-05
+1.650000e+02 2.500000e+01 2.500000e+01 5.359900e-03 6.805600e-05 0.000000e+00
+2.200000e+02 3.000000e+01 3.000000e+01 3.011000e-03 0.000000e+00 1.196600e-04
+2.825000e+02 3.250000e+01 3.250000e+01 1.315600e-03 1.542800e-05 1.985900e-05
+3.525000e+02 3.750000e+01 3.750000e+01 5.297400e-04 4.476400e-05 1.635500e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.952400e-04 2.498500e-05 0.000000e+00
+5.825000e+02 1.025000e+02 1.025000e+02 4.351800e-05 1.402500e-07 2.010700e-06
+8.425000e+02 1.575000e+02 1.575000e+02 3.440100e-06 1.239600e-07 8.070700e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d59-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d59-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.537000e-03 1.772834e-04 1.928197e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.842500e-03 5.819066e-05 6.263716e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.100200e-03 4.681870e-05 4.496857e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.439500e-03 3.619757e-05 3.539646e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.804900e-04 3.805045e-05 3.593377e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.920500e-04 2.436671e-05 2.348867e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.580400e-04 2.311139e-05 2.131238e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.181200e-04 1.862461e-05 1.782577e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.072200e-04 1.402972e-05 1.300234e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.314800e-04 1.340325e-05 1.854704e-05
+1.750000e+03 2.500000e+02 2.500000e+02 6.295500e-05 4.854287e-06 5.491534e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.318200e-05 1.855430e-06 1.959019e-06
+3.350000e+03 6.500000e+02 6.500000e+02 1.905100e-06 4.335459e-07 4.003406e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d59-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d59-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.533800e-03 1.215600e-04 4.578800e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.756100e-03 3.323400e-05 5.062300e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.989200e-03 2.576500e-05 3.384400e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.406900e-03 3.537000e-05 2.042900e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.691000e-04 1.650300e-05 2.582800e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.846800e-04 1.385600e-05 1.406400e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.702000e-04 1.044800e-05 1.888800e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.399900e-04 1.008700e-05 1.781500e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.346200e-04 7.144400e-06 1.023400e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.522100e-04 9.169600e-06 6.431700e-06
+1.750000e+03 2.500000e+02 2.500000e+02 7.137600e-05 2.767100e-06 3.571900e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.879700e-05 9.967600e-07 1.349200e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.609100e-06 2.379600e-07 3.590000e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d59-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d59-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.539200e-03 6.898200e-05 6.014000e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.783400e-03 3.631500e-05 3.130500e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.006100e-03 1.177600e-05 9.872800e-06
+7.400000e+02 4.500000e+01 4.500000e+01 1.435800e-03 3.024900e-06 3.135100e-06
+8.325000e+02 4.750000e+01 4.750000e+01 9.792100e-04 7.903700e-06 8.899900e-06
+9.325000e+02 5.250000e+01 5.250000e+01 6.869200e-04 9.667500e-06 1.106500e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.674200e-04 9.532000e-06 1.099600e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.273300e-04 8.618600e-06 1.000300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.252300e-04 7.246900e-06 8.468800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.467300e-04 5.775100e-06 6.802900e-06
+1.750000e+03 2.500000e+02 2.500000e+02 6.747300e-05 3.424100e-06 4.077800e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.723200e-05 1.260300e-06 1.537800e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.278500e-06 2.334000e-07 2.946500e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d59-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d59-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.384800e-03 9.748300e-05 1.598600e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.659700e-03 3.182600e-05 1.973900e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.945600e-03 3.306300e-05 1.792100e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.396700e-03 6.561700e-06 7.235800e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.959700e-04 2.656700e-05 1.527800e-07
+9.325000e+02 5.250000e+01 5.250000e+01 7.087700e-04 1.702200e-05 2.733000e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.918100e-04 1.358900e-05 1.068100e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.509700e-04 5.620100e-06 1.291000e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.494600e-04 6.587100e-06 1.179700e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.696500e-04 1.542400e-05 0.000000e+00
+1.750000e+03 2.500000e+02 2.500000e+02 7.781200e-05 3.638800e-06 3.344700e-06
+2.350000e+03 3.500000e+02 3.500000e+02 2.016300e-05 2.480400e-06 1.220400e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.753200e-06 1.980800e-07 3.293400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d60-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d60-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.710100e-03 1.829325e-04 1.857785e-04
+3.750000e+01 1.250000e+01 1.250000e+01 9.054400e-03 2.892417e-04 3.263673e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.914000e-03 1.567079e-04 1.543139e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.474500e-03 1.418444e-04 1.354520e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.614600e-03 1.939892e-04 1.822575e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.724300e-03 2.153469e-04 1.885156e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.628400e-03 1.053646e-04 1.011315e-04
+2.250000e+02 3.500000e+01 3.500000e+01 7.742300e-04 4.996039e-05 4.853135e-05
+3.250000e+02 6.500000e+01 6.500000e+01 1.788300e-04 1.661312e-05 1.753925e-05
+6.450000e+02 2.550000e+02 2.550000e+02 9.241300e-06 1.971697e-06 2.104979e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d60-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d60-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.882600e-03 2.072200e-04 6.438900e-05
+3.750000e+01 1.250000e+01 1.250000e+01 8.113600e-03 9.308000e-05 1.482900e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.476800e-03 8.935300e-05 1.161800e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.746600e-03 8.291700e-05 8.773200e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.093600e-03 6.117200e-05 6.436300e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.861200e-03 6.286400e-05 5.337000e-05
+1.750000e+02 1.500000e+01 1.500000e+01 1.895500e-03 4.107000e-05 5.535600e-05
+2.250000e+02 3.500000e+01 3.500000e+01 9.315100e-04 2.289500e-05 2.045200e-05
+3.250000e+02 6.500000e+01 6.500000e+01 2.422800e-04 7.179100e-06 9.367200e-06
+6.450000e+02 2.550000e+02 2.550000e+02 1.430800e-05 1.253200e-06 1.034600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d60-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d60-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.989000e-03 1.416000e-04 1.227700e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.896200e-03 1.508700e-04 1.308100e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.072600e-03 2.375100e-05 2.090600e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.584200e-03 2.727300e-05 3.133300e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.037200e-03 3.591300e-05 4.522400e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.875300e-03 3.753400e-05 4.502100e-05
+1.750000e+02 1.500000e+01 1.500000e+01 2.012700e-03 3.629500e-05 4.133300e-05
+2.250000e+02 3.500000e+01 3.500000e+01 1.016400e-03 2.015800e-05 2.279700e-05
+3.250000e+02 6.500000e+01 6.500000e+01 2.888100e-04 7.442300e-06 8.013600e-06
+6.450000e+02 2.550000e+02 2.550000e+02 1.960600e-05 7.823300e-07 8.430800e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d60-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d60-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.858600e-03 1.083200e-04 2.436400e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.188400e-03 2.454600e-04 9.662900e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.534300e-03 0.000000e+00 3.665000e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.742500e-03 0.000000e+00 1.257700e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.056400e-03 8.830300e-05 0.000000e+00
+1.450000e+02 1.500000e+01 1.500000e+01 2.795200e-03 1.041800e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 1.864000e-03 1.437800e-05 6.655600e-05
+2.250000e+02 3.500000e+01 3.500000e+01 9.169000e-04 5.235800e-05 0.000000e+00
+3.250000e+02 6.500000e+01 6.500000e+01 2.462900e-04 9.787600e-06 1.423500e-05
+6.450000e+02 2.550000e+02 2.550000e+02 1.811500e-05 2.899300e-06 2.472100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d61-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d61-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.017800e-01 1.362437e-02 1.440183e-02
+3.500000e-01 5.000000e-02 5.000000e-02 1.427300e-01 1.755702e-02 1.844077e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.347600e-01 1.911047e-02 1.769351e-02
+5.500000e-01 5.000000e-02 5.000000e-02 3.735000e-01 2.875614e-02 3.109851e-02
+6.500000e-01 5.000000e-02 5.000000e-02 6.200100e-01 5.213860e-02 4.875594e-02
+7.250000e-01 2.500000e-02 2.500000e-02 8.685600e-01 7.355007e-02 7.419387e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.398000e+00 5.384091e-02 5.125492e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.083100e+00 6.703512e-02 6.473012e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.013100e+00 7.244860e-02 6.892062e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.060300e+00 9.637095e-02 8.811582e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.224200e+00 1.368201e-01 1.611396e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d61-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d61-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.371300e-01 3.655300e-03 5.286600e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.934500e-01 9.496500e-03 1.204600e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.638600e-01 1.280300e-02 1.126500e-02
+5.500000e-01 5.000000e-02 5.000000e-02 3.928200e-01 1.118000e-02 1.290200e-02
+6.500000e-01 5.000000e-02 5.000000e-02 6.729900e-01 1.496600e-02 1.636600e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.047300e+00 2.364600e-02 4.420900e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.465400e+00 3.685200e-02 2.797100e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.030300e+00 3.630900e-02 3.610200e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.848100e+00 4.791700e-02 5.670700e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.857800e+00 4.582700e-02 5.787900e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.882100e+00 1.135100e-01 5.105400e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d61-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d61-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.385600e-01 2.832700e-03 3.549500e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.891400e-01 3.405400e-03 4.012300e-03
+4.500000e-01 5.000000e-02 5.000000e-02 2.536300e-01 3.773200e-03 4.445900e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.886500e-01 7.634400e-03 8.697300e-03
+6.500000e-01 5.000000e-02 5.000000e-02 6.374100e-01 9.694900e-03 1.192600e-02
+7.250000e-01 2.500000e-02 2.500000e-02 9.975600e-01 1.289300e-02 1.470800e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.383900e+00 1.481100e-02 1.762000e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.968000e+00 1.820200e-02 2.027300e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.790700e+00 7.981000e-03 8.883600e-03
+9.250000e-01 2.500000e-02 2.500000e-02 3.963400e+00 3.363300e-02 2.808100e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.127400e+00 1.046700e-01 8.970500e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d61-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d61-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.280000e-01 5.879600e-03 0.000000e+00
+3.500000e-01 5.000000e-02 5.000000e-02 1.700600e-01 3.540400e-03 3.672300e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.384500e-01 1.108900e-02 0.000000e+00
+5.500000e-01 5.000000e-02 5.000000e-02 3.580800e-01 1.351400e-02 0.000000e+00
+6.500000e-01 5.000000e-02 5.000000e-02 6.284800e-01 2.671300e-02 2.228500e-03
+7.250000e-01 2.500000e-02 2.500000e-02 9.671500e-01 1.578700e-02 2.034000e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.403500e+00 4.781600e-02 2.510000e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.032200e+00 4.323700e-02 2.043100e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.909300e+00 2.071200e-02 2.903900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.029500e+00 3.946400e-02 1.379900e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.100200e+00 0.000000e+00 1.294000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d62-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d62-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.324300e-01 1.120437e-02 1.026632e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.150300e-01 1.282128e-02 1.150696e-02
+3.000000e+00 2.000000e-01 2.000000e-01 3.809700e-01 1.159701e-02 1.186194e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.491000e-01 1.234324e-02 1.235734e-02
+3.800000e+00 2.000000e-01 2.000000e-01 4.631300e-01 1.109745e-02 1.165524e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.971800e-01 1.001354e-02 9.212471e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.697900e-01 7.399613e-03 7.898935e-03
+5.000000e+00 2.000000e-01 2.000000e-01 9.728100e-02 6.190592e-03 6.496378e-03
+5.800000e+00 6.000000e-01 6.000000e-01 2.961300e-02 2.490982e-03 2.677298e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.042000e-03 4.840271e-04 4.915910e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d62-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d62-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.316900e-01 4.071400e-03 5.071400e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.044200e-01 4.826500e-03 6.135200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 3.928600e-01 1.515000e-02 5.120400e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.571300e-01 5.670200e-03 8.701500e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.437400e-01 6.822200e-03 5.903000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.899600e-01 5.191900e-03 5.502000e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.742700e-01 3.686200e-03 7.415700e-03
+5.000000e+00 2.000000e-01 2.000000e-01 9.967300e-02 2.579100e-03 6.947600e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.278900e-02 1.044200e-03 8.575500e-04
+7.600000e+00 1.200000e+00 1.200000e+00 1.315800e-03 1.209800e-04 2.074000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d62-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d62-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.968300e-01 4.204600e-03 4.415700e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.559000e-01 3.120500e-03 3.212200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.123100e-01 2.298300e-03 2.030600e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.446600e-01 1.859900e-03 1.555500e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.036900e-01 2.640600e-03 2.612600e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.596200e-01 3.111700e-03 2.801400e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.533400e-01 3.039000e-03 3.531600e-03
+5.000000e+00 2.000000e-01 2.000000e-01 8.557900e-02 2.688400e-03 3.167800e-03
+5.800000e+00 6.000000e-01 6.000000e-01 2.714300e-02 1.375300e-03 1.659500e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.107700e-03 1.066400e-04 1.356900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d62-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d62-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.529600e-01 4.795900e-03 1.912800e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.264300e-01 9.110500e-03 1.435600e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.013700e-01 5.643400e-03 0.000000e+00
+3.400000e+00 2.000000e-01 2.000000e-01 4.556500e-01 7.727700e-03 2.058700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.190200e-01 3.059300e-03 7.213500e-04
+4.200000e+00 2.000000e-01 2.000000e-01 2.734900e-01 3.752200e-03 1.902400e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.653700e-01 4.197100e-03 0.000000e+00
+5.000000e+00 2.000000e-01 2.000000e-01 9.715800e-02 4.634600e-03 1.335200e-02
+5.800000e+00 6.000000e-01 6.000000e-01 3.299600e-02 2.767600e-03 1.251500e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.593800e-03 1.666000e-04 3.756000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d63-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d63-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 8.597000e-03 6.410279e-04 7.175628e-04
+1.050000e+02 1.000000e+01 1.000000e+01 8.682700e-03 3.006712e-04 3.650035e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.505700e-03 1.505876e-04 1.412089e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.857900e-03 1.808055e-04 1.727831e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.520500e-03 2.010371e-04 1.924766e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.195100e-03 1.721878e-04 1.558201e-04
+2.350000e+02 1.500000e+01 1.500000e+01 1.920200e-03 1.300336e-04 1.208145e-04
+2.650000e+02 1.500000e+01 1.500000e+01 1.142300e-03 1.115987e-04 1.085334e-04
+2.975000e+02 1.750000e+01 1.750000e+01 7.322200e-04 5.104252e-05 4.414265e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.056900e-04 2.982988e-05 3.087551e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.586600e-04 2.005086e-05 2.087936e-05
+4.350000e+02 4.500000e+01 4.500000e+01 9.667700e-05 1.040879e-05 1.008464e-05
+5.825000e+02 1.025000e+02 1.025000e+02 1.798100e-05 2.827337e-06 2.992954e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d63-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d63-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 7.389600e-03 1.191700e-04 3.547100e-04
+1.050000e+02 1.000000e+01 1.000000e+01 8.170500e-03 3.343000e-04 1.044600e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.376900e-03 8.894200e-05 1.317500e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.113700e-03 1.156400e-04 9.133100e-05
+1.775000e+02 1.250000e+01 1.250000e+01 4.718100e-03 7.099900e-05 1.090500e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.309400e-03 7.084500e-05 7.433000e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.091000e-03 6.414900e-05 4.732200e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.293500e-03 3.488000e-05 4.962200e-05
+2.975000e+02 1.750000e+01 1.750000e+01 7.833800e-04 2.595500e-05 3.265200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.624000e-04 2.169000e-05 2.394600e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.679800e-04 1.427900e-05 1.892700e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.192800e-04 7.325000e-06 6.514400e-06
+5.825000e+02 1.025000e+02 1.025000e+02 2.271200e-05 2.598000e-06 2.056800e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d63-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d63-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.165900e-03 7.892800e-05 7.739500e-05
+1.050000e+02 1.000000e+01 1.000000e+01 7.036200e-03 6.513100e-05 6.530800e-05
+1.275000e+02 1.250000e+01 1.250000e+01 6.867400e-03 4.194900e-05 3.719800e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.090300e-03 2.789300e-05 2.275700e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.079500e-03 1.978800e-05 1.763600e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.649000e-03 2.084000e-05 2.343300e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.413600e-03 2.156800e-05 2.305400e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.540300e-03 2.114100e-05 2.317100e-05
+2.975000e+02 1.750000e+01 1.750000e+01 9.495100e-04 1.876800e-05 2.042200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 5.796700e-04 1.327900e-05 1.454900e-05
+3.700000e+02 2.000000e+01 2.000000e+01 3.477200e-04 9.107700e-06 9.782700e-06
+4.350000e+02 4.500000e+01 4.500000e+01 1.546500e-04 5.233400e-06 5.679300e-06
+5.825000e+02 1.025000e+02 1.025000e+02 3.130300e-05 1.315300e-06 1.441600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d63-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d63-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.757100e-03 1.194100e-04 4.071500e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.433100e-03 1.479200e-04 2.407800e-05
+1.275000e+02 1.250000e+01 1.250000e+01 7.108400e-03 2.144300e-04 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 6.223700e-03 4.743400e-05 1.252000e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.883600e-03 3.559500e-05 6.937000e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.498200e-03 1.475300e-05 2.303600e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.191500e-03 2.483800e-05 5.854400e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.422400e-03 3.732900e-05 0.000000e+00
+2.975000e+02 1.750000e+01 1.750000e+01 8.711000e-04 4.319900e-05 8.767100e-07
+3.325000e+02 1.750000e+01 1.750000e+01 5.452100e-04 3.923000e-05 0.000000e+00
+3.700000e+02 2.000000e+01 2.000000e+01 3.155800e-04 1.819000e-05 1.109400e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.418900e-04 6.965100e-06 1.774200e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.056500e-05 9.495800e-07 4.727500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d64-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d64-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t64
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 2.674200e-01 4.491341e-02 4.525471e-02
+7.500000e+01 2.500000e+01 2.500000e+01 3.724900e-01 3.939895e-02 4.703968e-02
+1.300000e+02 3.000000e+01 3.000000e+01 2.079700e-01 2.739788e-02 2.350885e-02
+1.925000e+02 3.250000e+01 3.250000e+01 1.115800e-01 1.430191e-02 1.462209e-02
+2.625000e+02 3.750000e+01 3.750000e+01 4.700200e-02 1.992072e-02 1.996867e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.250300e-03 3.774957e-02 3.774449e-02
+6.975000e+02 2.025000e+02 2.025000e+02 5.458600e-04 4.095326e-04 4.107797e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d64-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d64-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t64
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 2.239700e-01 2.728900e-02 2.080900e-02
+7.500000e+01 2.500000e+01 2.500000e+01 3.054800e-01 3.943000e-02 3.231700e-02
+1.300000e+02 3.000000e+01 3.000000e+01 2.047900e-01 2.164900e-02 2.386800e-02
+1.925000e+02 3.250000e+01 3.250000e+01 1.108700e-01 1.228700e-02 1.570400e-02
+2.625000e+02 3.750000e+01 3.750000e+01 5.003400e-02 5.052900e-03 4.460700e-03
+3.975000e+02 9.750000e+01 9.750000e+01 1.366100e-02 1.616400e-03 1.518500e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.095800e-03 2.037400e-04 2.103500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d64-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d64-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t64
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 3.071800e-01 5.188900e-02 8.759200e-02
+7.500000e+01 2.500000e+01 2.500000e+01 4.018000e-01 6.570600e-02 1.603900e-01
+1.300000e+02 3.000000e+01 3.000000e+01 2.567100e-01 5.092800e-02 1.023200e-01
+1.925000e+02 3.250000e+01 3.250000e+01 1.344300e-01 2.596600e-02 7.378000e-02
+2.625000e+02 3.750000e+01 3.750000e+01 6.309800e-02 1.273100e-02 2.078300e-02
+3.975000e+02 9.750000e+01 9.750000e+01 1.795700e-02 4.193500e-03 5.390200e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.657600e-03 3.662100e-04 7.480000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d65-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d65-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t65
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 5.520100e+00 2.510942e+00 2.559797e+00
+6.000000e-01 1.000000e-01 1.000000e-01 2.698000e+01 4.953234e+00 5.259319e+00
+7.500000e-01 5.000000e-02 5.000000e-02 6.827800e+01 8.337523e+00 8.039806e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.271800e+02 1.647799e+01 1.591515e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.474300e+02 2.868073e+01 2.765007e+01
+9.750000e-01 2.500000e-02 2.500000e-02 3.307400e+02 2.781169e+01 2.893715e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d65-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d65-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t65
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 8.402700e+00 8.305200e-01 1.209400e+00
+6.000000e-01 1.000000e-01 1.000000e-01 2.572900e+01 2.931400e+00 4.718800e+00
+7.500000e-01 5.000000e-02 5.000000e-02 6.382600e+01 7.372200e+00 7.963400e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.239000e+02 1.470500e+01 1.391600e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.118700e+02 2.422000e+01 1.813300e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.825800e+02 3.478400e+01 2.253000e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d65-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d65-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t65
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 9.150600e+00 1.864200e+00 4.995100e+00
+6.000000e-01 1.000000e-01 1.000000e-01 2.836600e+01 6.116800e+00 1.033800e+01
+7.500000e-01 5.000000e-02 5.000000e-02 7.319900e+01 1.231600e+01 2.342400e+01
+8.500000e-01 5.000000e-02 5.000000e-02 1.580600e+02 2.766900e+01 6.570400e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.906900e+02 5.783000e+01 1.037100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 4.125600e+02 6.495900e+01 1.526100e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d66-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d66-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t66
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 5.239400e+00 5.621497e-01 5.416009e-01
+3.200000e+00 4.000000e-01 4.000000e-01 6.939200e+00 6.535603e-01 6.334484e-01
+4.000000e+00 4.000000e-01 4.000000e-01 1.318100e+01 1.157089e+00 1.069418e+00
+4.800000e+00 4.000000e-01 4.000000e-01 1.590400e+01 2.170391e+00 2.123716e+00
+5.600000e+00 4.000000e-01 4.000000e-01 2.040800e+01 2.625320e+00 3.189703e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.417900e+00 7.354390e-01 6.604592e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d66-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d66-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t66
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 4.555800e+00 5.744500e-01 5.165200e-01
+3.200000e+00 4.000000e-01 4.000000e-01 7.398600e+00 8.278200e-01 7.556400e-01
+4.000000e+00 4.000000e-01 4.000000e-01 1.144800e+01 1.197700e+00 1.233200e+00
+4.800000e+00 4.000000e-01 4.000000e-01 1.673600e+01 1.722100e+00 1.402400e+00
+5.600000e+00 4.000000e-01 4.000000e-01 1.807600e+01 2.023900e+00 2.263500e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.239400e+00 3.862600e-01 2.853700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d66-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d66-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t66
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 7.473100e+00 1.529300e+00 3.883900e+00
+3.200000e+00 4.000000e-01 4.000000e-01 1.192400e+01 2.392800e+00 3.974200e+00
+4.000000e+00 4.000000e-01 4.000000e-01 1.586000e+01 2.853400e+00 6.805400e+00
+4.800000e+00 4.000000e-01 4.000000e-01 2.027500e+01 3.681400e+00 7.261200e+00
+5.600000e+00 4.000000e-01 4.000000e-01 1.987400e+01 3.369800e+00 8.794800e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.933100e+00 5.047500e-01 6.107300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d67-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d67-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t67
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.903900e-01 7.502811e-02 8.013669e-02
+1.400000e+02 2.500000e+01 2.500000e+01 2.750100e-01 3.924753e-02 3.612656e-02
+1.925000e+02 2.750000e+01 2.750000e+01 1.833000e-01 1.943026e-02 2.300746e-02
+2.500000e+02 3.000000e+01 3.000000e+01 1.195700e-01 1.460465e-02 1.214861e-02
+3.150000e+02 3.500000e+01 3.500000e+01 6.816600e-02 1.704474e-02 1.669931e-02
+3.925000e+02 4.250000e+01 4.250000e+01 5.076100e-02 5.870752e-03 5.757623e-03
+5.075000e+02 7.250000e+01 7.250000e+01 2.749000e-02 3.412071e-03 3.229625e-03
+7.300000e+02 1.500000e+02 1.500000e+02 4.916500e-03 1.154162e-03 1.147772e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d67-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d67-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t67
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.275100e-01 3.310400e-02 4.021500e-02
+1.400000e+02 2.500000e+01 2.500000e+01 2.408100e-01 2.843500e-02 2.583700e-02
+1.925000e+02 2.750000e+01 2.750000e+01 1.816100e-01 2.001200e-02 1.553200e-02
+2.500000e+02 3.000000e+01 3.000000e+01 1.230200e-01 1.478200e-02 1.009200e-02
+3.150000e+02 3.500000e+01 3.500000e+01 8.085000e-02 7.994600e-03 8.493600e-03
+3.925000e+02 4.250000e+01 4.250000e+01 4.941800e-02 5.306900e-03 5.850600e-03
+5.075000e+02 7.250000e+01 7.250000e+01 2.702300e-02 2.931100e-03 3.213800e-03
+7.300000e+02 1.500000e+02 1.500000e+02 5.320900e-03 8.264500e-04 5.590800e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d67-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d67-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t67
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.923200e-01 4.814700e-02 9.105100e-02
+1.400000e+02 2.500000e+01 2.500000e+01 2.665100e-01 4.240900e-02 1.054600e-01
+1.925000e+02 2.750000e+01 2.750000e+01 2.205000e-01 4.364300e-02 8.326400e-02
+2.500000e+02 3.000000e+01 3.000000e+01 1.570400e-01 3.138500e-02 5.388200e-02
+3.150000e+02 3.500000e+01 3.500000e+01 1.132200e-01 2.396300e-02 5.003700e-02
+3.925000e+02 4.250000e+01 4.250000e+01 7.425500e-02 1.452500e-02 2.641600e-02
+5.075000e+02 7.250000e+01 7.250000e+01 4.370800e-02 9.631300e-03 1.718500e-02
+7.300000e+02 1.500000e+02 1.500000e+02 9.033100e-03 1.487100e-03 6.215500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d68-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d68-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t68
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 9.950900e+01 1.942476e+01 1.854141e+01
+2.500000e-01 1.000000e-01 1.000000e-01 8.070900e+01 1.408074e+01 1.343267e+01
+5.000000e-01 1.500000e-01 1.500000e-01 5.441500e+01 1.029418e+01 1.044141e+01
+8.250000e-01 1.750000e-01 1.750000e-01 9.741800e+00 1.900542e+00 1.972275e+00
+1.500000e+00 5.000000e-01 5.000000e-01 6.006700e-01 2.042429e-01 2.014581e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d68-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d68-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t68
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 7.690900e+01 1.619700e+01 8.542800e+00
+2.500000e-01 1.000000e-01 1.000000e-01 7.096900e+01 1.318800e+01 1.102600e+01
+5.000000e-01 1.500000e-01 1.500000e-01 4.342600e+01 4.416600e+00 6.735800e+00
+8.250000e-01 1.750000e-01 1.750000e-01 9.053000e+00 1.338500e+00 9.468000e-01
+1.500000e+00 5.000000e-01 5.000000e-01 5.568000e-01 1.107200e-01 9.573200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d68-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d68-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t68
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.108800e+02 2.293100e+01 5.061700e+01
+2.500000e-01 1.000000e-01 1.000000e-01 1.004700e+02 1.689300e+01 4.855200e+01
+5.000000e-01 1.500000e-01 1.500000e-01 6.479800e+01 1.333100e+01 2.844800e+01
+8.250000e-01 1.750000e-01 1.750000e-01 1.434400e+01 3.951300e+00 5.709500e+00
+1.500000e+00 5.000000e-01 5.000000e-01 9.877500e-01 2.295100e-01 5.180400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d69-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d69-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t69
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 9.167600e+01 8.744966e+00 9.993516e+00
+3.000000e-01 1.000000e-01 1.000000e-01 1.033500e+02 1.315957e+01 1.305025e+01
+4.750000e-01 7.500000e-02 7.500000e-02 6.467700e+01 1.181920e+01 1.180156e+01
+6.750000e-01 1.250000e-01 1.250000e-01 2.499700e+01 3.321205e+00 2.895415e+00
+9.000000e-01 1.000000e-01 1.000000e-01 4.704700e+00 9.374202e-01 9.543161e-01
+1.100000e+00 1.000000e-01 1.000000e-01 1.372800e+00 5.085533e-01 5.090083e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d69-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d69-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t69
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 8.662100e+01 6.075200e+00 7.395600e+00
+3.000000e-01 1.000000e-01 1.000000e-01 9.681400e+01 1.297600e+01 1.040300e+01
+4.750000e-01 7.500000e-02 7.500000e-02 6.644700e+01 9.621600e+00 6.649700e+00
+6.750000e-01 1.250000e-01 1.250000e-01 2.061600e+01 2.597700e+00 3.408100e+00
+9.000000e-01 1.000000e-01 1.000000e-01 3.882400e+00 7.499600e-01 8.866100e-01
+1.100000e+00 1.000000e-01 1.000000e-01 9.913800e-01 2.754400e-01 3.793300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d69-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d69-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t69
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.005500e+02 1.355700e+01 2.667400e+01
+3.000000e-01 1.000000e-01 1.000000e-01 1.171000e+02 2.349900e+01 4.233100e+01
+4.750000e-01 7.500000e-02 7.500000e-02 9.886900e+01 1.943700e+01 5.203700e+01
+6.750000e-01 1.250000e-01 1.250000e-01 3.361800e+01 6.727700e+00 1.553500e+01
+9.000000e-01 1.000000e-01 1.000000e-01 6.780200e+00 2.126500e+00 2.802800e+00
+1.100000e+00 1.000000e-01 1.000000e-01 1.623900e+00 3.248900e-01 1.118000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d70-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d70-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t70
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 3.074200e+01 2.901229e+00 3.069764e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.495500e+01 2.066467e+00 2.003503e+00
+2.000000e+00 5.000000e-01 5.000000e-01 6.357000e+00 1.046056e+00 1.122947e+00
+3.000000e+00 5.000000e-01 5.000000e-01 2.886000e+00 7.992817e-01 6.571748e-01
+6.000000e+00 2.500000e+00 2.500000e+00 1.435200e+00 5.450652e-01 4.914309e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d70-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d70-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t70
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 3.019200e+01 2.376700e+00 2.457800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.405400e+01 2.142600e+00 1.756100e+00
+2.000000e+00 5.000000e-01 5.000000e-01 5.752600e+00 7.362300e-01 9.443400e-01
+3.000000e+00 5.000000e-01 5.000000e-01 2.054200e+00 6.968700e-01 2.687600e-01
+6.000000e+00 2.500000e+00 2.500000e+00 7.883900e-01 1.387900e-01 2.023900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d70-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d70-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t70
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 3.645800e+01 6.348600e+00 1.145400e+01
+1.000000e+00 5.000000e-01 5.000000e-01 1.976500e+01 3.454400e+00 8.995000e+00
+2.000000e+00 5.000000e-01 5.000000e-01 8.546400e+00 2.081500e+00 4.554500e+00
+3.000000e+00 5.000000e-01 5.000000e-01 2.964600e+00 8.147700e-01 9.282500e-01
+6.000000e+00 2.500000e+00 2.500000e+00 8.032000e-01 1.145500e-01 3.909200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d71-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d71-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.415600e+00 1.986454e-01 2.133789e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.743300e+00 1.299251e-01 1.343406e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.179300e+00 7.270734e-02 7.321741e-02
+7.400000e+02 4.500000e+01 4.500000e+01 8.000100e-01 4.943582e-02 4.272418e-02
+8.325000e+02 4.750000e+01 4.750000e+01 5.315900e-01 3.537647e-02 4.513574e-02
+9.325000e+02 5.250000e+01 5.250000e+01 3.311600e-01 2.183101e-02 2.696344e-02
+1.042500e+03 5.750000e+01 5.750000e+01 2.021500e-01 2.018193e-02 1.723141e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.160100e-01 1.162131e-02 9.688182e-03
+1.275000e+03 7.500000e+01 7.500000e+01 7.343200e-02 7.372960e-03 6.168185e-03
+1.425000e+03 7.500000e+01 7.500000e+01 4.681700e-02 4.873837e-03 4.807159e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.410100e-02 2.775143e-03 2.904789e-03
+2.350000e+03 3.500000e+02 3.500000e+02 2.248900e-03 5.788196e-04 3.754865e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.085800e-04 5.300238e-05 5.091667e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d71-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d71-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.969200e+00 2.690900e-01 1.946600e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.470400e+00 1.817200e-01 1.657400e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.000900e+00 1.328000e-01 2.237600e-01
+7.400000e+02 4.500000e+01 4.500000e+01 6.636100e-01 1.062100e-01 7.794700e-02
+8.325000e+02 4.750000e+01 4.750000e+01 4.262500e-01 5.759400e-02 4.364300e-02
+9.325000e+02 5.250000e+01 5.250000e+01 2.739200e-01 3.568500e-02 3.587300e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.699400e-01 2.336700e-02 1.684900e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.086100e-01 1.400600e-02 1.659000e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.666000e-02 9.762500e-03 8.835900e-03
+1.425000e+03 7.500000e+01 7.500000e+01 3.859200e-02 5.034200e-03 4.425600e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.347800e-02 1.539800e-03 1.919000e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.976100e-03 2.840300e-04 2.513800e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.089900e-04 3.707200e-05 3.430300e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d71-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d71-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.056200e+00 4.627500e-01 6.714700e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.552700e+00 3.593300e-01 5.301400e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.057800e+00 2.419800e-01 3.546300e-01
+7.400000e+02 4.500000e+01 4.500000e+01 7.049000e-01 1.626500e-01 2.394000e-01
+8.325000e+02 4.750000e+01 4.750000e+01 4.634900e-01 1.088200e-01 1.622100e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.024700e-01 7.286500e-02 1.094500e-01
+1.042500e+03 5.750000e+01 5.750000e+01 1.893800e-01 4.552500e-02 6.812800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.230700e-01 2.992800e-02 4.511000e-02
+1.275000e+03 7.500000e+01 7.500000e+01 7.513800e-02 1.846900e-02 2.797300e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.677100e-02 1.236000e-02 1.962400e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.630500e-02 4.027900e-03 6.092800e-03
+2.350000e+03 3.500000e+02 3.500000e+02 2.306300e-03 6.167600e-04 9.615900e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.366400e-04 3.831500e-05 6.055100e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d71-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d71-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.975000e+00 3.615700e-01 8.545600e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.479800e+00 2.551400e-01 6.320200e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.041100e+00 1.671700e-01 4.564400e-01
+7.400000e+02 4.500000e+01 4.500000e+01 7.005600e-01 1.353200e-01 2.863100e-01
+8.325000e+02 4.750000e+01 4.750000e+01 4.886400e-01 1.314300e-01 1.449800e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.055600e-01 5.207500e-02 1.218400e-01
+1.042500e+03 5.750000e+01 5.750000e+01 1.990800e-01 4.164500e-02 7.744400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.344000e-01 3.122300e-02 4.936500e-02
+1.275000e+03 7.500000e+01 7.500000e+01 8.610500e-02 1.420100e-02 2.970300e-02
+1.425000e+03 7.500000e+01 7.500000e+01 5.010900e-02 8.459200e-03 1.657700e-02
+1.750000e+03 2.500000e+02 2.500000e+02 2.036100e-02 4.202000e-03 9.873600e-03
+2.350000e+03 3.500000e+02 3.500000e+02 3.309800e-03 7.252700e-04 1.386600e-03
+3.350000e+03 6.500000e+02 6.500000e+02 2.617200e-04 1.134100e-04 6.592500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d72-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d72-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.608800e+00 2.444261e-01 2.441014e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.994200e+00 4.615159e-01 4.827298e-01
+6.250000e+01 1.250000e+01 1.250000e+01 4.384900e+00 4.262507e-01 4.407255e-01
+8.750000e+01 1.250000e+01 1.250000e+01 3.205100e+00 2.156284e-01 2.213289e-01
+1.150000e+02 1.500000e+01 1.500000e+01 2.122700e+00 1.368441e-01 1.320994e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.312200e+00 1.052806e-01 9.578950e-02
+1.750000e+02 1.500000e+01 1.500000e+01 8.039800e-01 7.431028e-02 7.563143e-02
+2.075000e+02 1.750000e+01 1.750000e+01 4.799200e-01 5.407814e-02 5.051290e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.769900e-01 2.559383e-02 2.834501e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.585800e-01 2.203793e-02 2.026432e-02
+3.975000e+02 9.750000e+01 9.750000e+01 3.140300e-02 8.332853e-03 8.254493e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.882700e-03 7.983694e-04 8.074512e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d72-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d72-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.875900e+00 3.425300e-01 6.209600e-01
+3.750000e+01 1.250000e+01 1.250000e+01 3.912800e+00 4.769000e-01 4.861200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 3.553600e+00 4.906100e-01 3.903400e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.646200e+00 3.397200e-01 3.238300e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.804400e+00 2.422700e-01 2.159600e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.192600e+00 1.508800e-01 1.236300e-01
+1.750000e+02 1.500000e+01 1.500000e+01 7.785300e-01 1.011300e-01 6.947300e-02
+2.075000e+02 1.750000e+01 1.750000e+01 4.763700e-01 6.753400e-02 4.427900e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.801400e-01 2.907400e-02 2.482100e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.629500e-01 2.337900e-02 1.633500e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.244800e-02 5.189000e-03 2.135900e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.942800e-03 2.696000e-04 2.439500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d72-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d72-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.100100e+00 4.189000e-01 5.808200e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.063700e+00 8.731800e-01 1.251300e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.580000e+00 8.206600e-01 1.202300e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.766700e+00 6.605300e-01 9.814900e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.912000e+00 4.652000e-01 7.007300e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.354100e+00 3.498800e-01 5.411300e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.696100e-01 2.181600e-01 3.335600e-01
+2.075000e+02 1.750000e+01 1.750000e+01 5.394700e-01 1.356100e-01 2.055300e-01
+2.425000e+02 1.750000e+01 1.750000e+01 3.334100e-01 8.460600e-02 1.282600e-01
+2.800000e+02 2.000000e+01 2.000000e+01 1.971800e-01 5.055500e-02 7.684200e-02
+3.975000e+02 9.750000e+01 9.750000e+01 5.599800e-02 1.454600e-02 2.212400e-02
+6.975000e+02 2.025000e+02 2.025000e+02 2.896300e-03 7.754000e-04 1.183300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d72-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d72-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.982400e+00 2.688200e-01 7.563800e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.174400e+00 7.277300e-01 1.787700e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.835400e+00 8.292200e-01 1.533600e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.813400e+00 4.737500e-01 1.213200e+00
+1.150000e+02 1.500000e+01 1.500000e+01 1.915800e+00 3.763300e-01 8.659100e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.342800e+00 3.293400e-01 4.489400e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.355200e-01 1.582400e-01 3.490300e-01
+2.075000e+02 1.750000e+01 1.750000e+01 4.972900e-01 1.147400e-01 2.066200e-01
+2.425000e+02 1.750000e+01 1.750000e+01 2.861000e-01 6.359200e-02 9.284700e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.641100e-01 2.400200e-02 5.206000e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.566900e-02 1.055200e-02 1.474900e-02
+6.975000e+02 2.025000e+02 2.025000e+02 2.507100e-03 6.248900e-04 1.155500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d73-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d73-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 3.259200e+01 9.394090e+00 8.680227e+00
+4.000000e-01 1.000000e-01 1.000000e-01 6.824900e+01 1.221602e+01 1.280593e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.239800e+02 2.442462e+01 2.432244e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.365000e+02 2.418363e+01 1.910719e+01
+6.750000e-01 2.500000e-02 2.500000e-02 3.164500e+02 2.460514e+01 2.709276e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.799300e+02 1.373115e+02 1.368762e+02
+7.750000e-01 2.500000e-02 2.500000e-02 7.852600e+02 5.284852e+01 6.030013e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.163000e+03 8.378977e+01 8.799065e+01
+8.750000e-01 2.500000e-02 2.500000e-02 1.677700e+03 1.275951e+02 1.307555e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.384500e+03 1.899326e+02 1.936158e+02
+9.750000e-01 2.500000e-02 2.500000e-02 3.212400e+03 2.530477e+02 2.558266e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d73-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d73-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.323200e+01 6.333200e+00 3.119600e+00
+4.000000e-01 1.000000e-01 1.000000e-01 7.526600e+01 8.462900e+00 9.371900e+00
+5.500000e-01 5.000000e-02 5.000000e-02 1.491400e+02 2.541700e+01 1.710200e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.209500e+02 3.509200e+01 3.085700e+01
+6.750000e-01 2.500000e-02 2.500000e-02 2.981400e+02 4.193200e+01 4.393500e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.373600e+02 6.749200e+01 4.075700e+01
+7.750000e-01 2.500000e-02 2.500000e-02 6.154700e+02 7.359400e+01 6.547700e+01
+8.250000e-01 2.500000e-02 2.500000e-02 9.116200e+02 1.179500e+02 1.052600e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.345500e+03 1.659300e+02 1.638400e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.915800e+03 2.433400e+02 2.181100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.497400e+03 3.612500e+02 4.226200e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d73-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d73-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.375000e+01 1.108600e+01 1.690900e+01
+4.000000e-01 1.000000e-01 1.000000e-01 7.793300e+01 2.018700e+01 3.206900e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.627100e+02 4.517800e+01 7.210600e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.114800e+02 5.235700e+01 7.913400e+01
+6.750000e-01 2.500000e-02 2.500000e-02 2.941100e+02 7.246200e+01 1.095000e+02
+7.250000e-01 2.500000e-02 2.500000e-02 4.201600e+02 1.029900e+02 1.551900e+02
+7.750000e-01 2.500000e-02 2.500000e-02 6.193300e+02 1.508500e+02 2.263500e+02
+8.250000e-01 2.500000e-02 2.500000e-02 9.222500e+02 2.210500e+02 3.297400e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.388700e+03 3.238100e+02 4.785500e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.082800e+03 4.691000e+02 6.836100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.909500e+03 6.339900e+02 9.081600e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d73-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d73-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.256000e+01 9.324700e+00 1.319500e+01
+4.000000e-01 1.000000e-01 1.000000e-01 7.237000e+01 1.535900e+01 3.025600e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.344900e+02 2.669700e+01 5.513000e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.184500e+02 4.520700e+01 7.154500e+01
+6.750000e-01 2.500000e-02 2.500000e-02 2.885200e+02 5.168800e+01 1.176500e+02
+7.250000e-01 2.500000e-02 2.500000e-02 4.222100e+02 7.557700e+01 1.845800e+02
+7.750000e-01 2.500000e-02 2.500000e-02 6.157100e+02 1.049400e+02 2.798900e+02
+8.250000e-01 2.500000e-02 2.500000e-02 9.800100e+02 2.083000e+02 4.000400e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.420400e+03 2.332200e+02 6.533500e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.145300e+03 4.553400e+02 8.358500e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.833700e+03 4.822200e+02 1.107600e+03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d74-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d74-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.091100e+02 1.402670e+01 1.367168e+01
+2.600000e+00 2.000000e-01 2.000000e-01 2.238300e+02 1.418280e+01 1.464034e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.508100e+02 1.570909e+01 1.630807e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.548900e+02 1.680456e+01 1.726047e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.085200e+02 1.648540e+01 1.729891e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.239900e+02 1.942287e+01 2.008674e+01
+4.800000e+00 4.000000e-01 4.000000e-01 3.985000e+01 4.397196e+00 4.895263e+00
+5.800000e+00 6.000000e-01 6.000000e-01 4.125500e+00 1.785458e+00 8.646571e-01
+7.600000e+00 1.200000e+00 1.200000e+00 4.605400e-02 3.548376e-02 3.060149e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d74-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d74-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.682500e+02 1.911100e+01 1.705200e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.877400e+02 2.302200e+01 1.780900e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.067500e+02 2.724000e+01 4.304200e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.127000e+02 2.959100e+01 2.353200e+01
+3.800000e+00 2.000000e-01 2.000000e-01 1.796200e+02 2.303400e+01 2.226300e+01
+4.200000e+00 2.000000e-01 2.000000e-01 9.933600e+01 1.952700e+01 1.126700e+01
+4.800000e+00 4.000000e-01 4.000000e-01 3.561800e+01 5.320800e+00 4.564200e+00
+5.800000e+00 6.000000e-01 6.000000e-01 3.964300e+00 3.798400e-01 9.810600e-01
+7.600000e+00 1.200000e+00 1.200000e+00 1.805700e-02 9.709000e-03 2.504800e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d74-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d74-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.290900e+02 5.415400e+01 7.983400e+01
+2.600000e+00 2.000000e-01 2.000000e-01 2.313500e+02 5.433300e+01 7.991700e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.257000e+02 5.194100e+01 7.631300e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.144600e+02 5.025900e+01 7.480700e+01
+3.800000e+00 2.000000e-01 2.000000e-01 1.629000e+02 3.641200e+01 5.317800e+01
+4.200000e+00 2.000000e-01 2.000000e-01 8.647600e+01 1.982200e+01 2.937800e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.884000e+01 6.717800e+00 1.018600e+01
+5.800000e+00 6.000000e-01 6.000000e-01 3.563700e+00 8.811000e-01 1.425800e+00
+7.600000e+00 1.200000e+00 1.200000e+00 2.293000e-02 5.544400e-03 8.364100e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d74-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d74-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.995700e+02 3.832400e+01 8.540200e+01
+2.600000e+00 2.000000e-01 2.000000e-01 2.161600e+02 3.189100e+01 9.208600e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.361000e+02 5.285900e+01 8.408300e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.223600e+02 3.994100e+01 9.154700e+01
+3.800000e+00 2.000000e-01 2.000000e-01 1.711300e+02 3.226800e+01 7.569300e+01
+4.200000e+00 2.000000e-01 2.000000e-01 9.087400e+01 1.709200e+01 3.585100e+01
+4.800000e+00 4.000000e-01 4.000000e-01 3.249900e+01 6.881100e+00 1.188200e+01
+5.800000e+00 6.000000e-01 6.000000e-01 5.201100e+00 8.860400e-01 2.234300e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.684500e-02 2.217500e-02 2.512900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d75-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d75-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.474600e+00 4.513922e-01 4.906002e-01
+1.050000e+02 1.000000e+01 1.000000e+01 3.817400e+00 3.467802e-01 3.619172e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.709900e+00 2.775314e-01 2.966466e-01
+1.525000e+02 1.250000e+01 1.250000e+01 3.426300e+00 2.473760e-01 2.188008e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.885500e+00 1.772587e-01 1.786117e-01
+2.050000e+02 1.500000e+01 1.500000e+01 2.037100e+00 1.139894e-01 1.159287e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.322600e+00 6.547812e-02 6.509956e-02
+2.650000e+02 1.500000e+01 1.500000e+01 8.300900e-01 4.913497e-02 4.526458e-02
+2.975000e+02 1.750000e+01 1.750000e+01 4.733500e-01 2.818240e-02 3.180290e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.416800e-01 3.326100e-02 3.264959e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.601200e-01 1.262026e-02 1.280743e-02
+4.125000e+02 2.250000e+01 2.250000e+01 8.138600e-02 9.159946e-03 8.966827e-03
+4.575000e+02 2.250000e+01 2.250000e+01 4.430500e-02 6.159585e-03 6.015320e-03
+5.300000e+02 5.000000e+01 5.000000e+01 1.427900e-02 3.023692e-03 2.966646e-03
+6.325000e+02 5.250000e+01 5.250000e+01 5.809600e-03 1.447559e-03 1.407017e-03
+8.425000e+02 1.575000e+02 1.575000e+02 3.192400e-04 2.349571e-04 2.265932e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d75-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d75-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 2.691600e+00 5.538800e-01 3.010300e-01
+1.050000e+02 1.000000e+01 1.000000e+01 3.128800e+00 4.155600e-01 3.963100e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.132300e+00 4.416500e-01 7.005100e-01
+1.525000e+02 1.250000e+01 1.250000e+01 2.879600e+00 3.603200e-01 3.115000e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.434100e+00 2.976700e-01 2.874300e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.741000e+00 2.273500e-01 1.783500e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.103800e+00 1.276600e-01 1.050200e-01
+2.650000e+02 1.500000e+01 1.500000e+01 6.818000e-01 8.567600e-02 5.664200e-02
+2.975000e+02 1.750000e+01 1.750000e+01 4.037900e-01 4.674100e-02 3.902800e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.326500e-01 3.004600e-02 1.663400e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.343400e-01 1.635600e-02 9.528000e-03
+4.125000e+02 2.250000e+01 2.250000e+01 7.385600e-02 8.839400e-03 8.698400e-03
+4.575000e+02 2.250000e+01 2.250000e+01 4.084200e-02 5.505900e-03 4.583800e-03
+5.300000e+02 5.000000e+01 5.000000e+01 1.595000e-02 1.828200e-03 1.577400e-03
+6.325000e+02 5.250000e+01 5.250000e+01 4.946100e-03 1.038100e-03 7.978700e-04
+8.425000e+02 1.575000e+02 1.575000e+02 7.036200e-04 1.671500e-04 1.736300e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d75-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d75-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 2.101300e+00 4.511200e-01 6.576400e-01
+1.050000e+02 1.000000e+01 1.000000e+01 2.663100e+00 5.794100e-01 8.389100e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.045100e+00 7.054600e-01 1.051600e+00
+1.525000e+02 1.250000e+01 1.250000e+01 2.977300e+00 6.763600e-01 9.886300e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.838300e+00 6.630100e-01 9.766500e-01
+2.050000e+02 1.500000e+01 1.500000e+01 2.074600e+00 4.874400e-01 7.207400e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.386000e+00 3.322000e-01 4.937400e-01
+2.650000e+02 1.500000e+01 1.500000e+01 8.986100e-01 2.172400e-01 3.231500e-01
+2.975000e+02 1.750000e+01 1.750000e+01 5.496300e-01 1.353700e-01 2.027900e-01
+3.325000e+02 1.750000e+01 1.750000e+01 3.368700e-01 8.370200e-02 1.255400e-01
+3.700000e+02 2.000000e+01 2.000000e+01 1.930200e-01 4.933400e-02 7.466400e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.106700e-01 2.851700e-02 4.324900e-02
+4.575000e+02 2.250000e+01 2.250000e+01 6.263200e-02 1.600400e-02 2.424700e-02
+5.300000e+02 5.000000e+01 5.000000e+01 2.554700e-02 6.756100e-03 1.032100e-02
+6.325000e+02 5.250000e+01 5.250000e+01 7.936300e-03 2.158200e-03 3.332400e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.160000e-03 3.214500e-04 4.988500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d75-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d75-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 2.188800e+00 3.477800e-01 8.848000e-01
+1.050000e+02 1.000000e+01 1.000000e+01 2.836800e+00 5.356900e-01 1.211800e+00
+1.275000e+02 1.250000e+01 1.250000e+01 3.196900e+00 5.550400e-01 1.406300e+00
+1.525000e+02 1.250000e+01 1.250000e+01 3.139700e+00 6.049600e-01 1.335500e+00
+1.775000e+02 1.250000e+01 1.250000e+01 2.796300e+00 5.255700e-01 9.938500e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.994500e+00 3.917300e-01 7.904300e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.332100e+00 3.259900e-01 4.493100e-01
+2.650000e+02 1.500000e+01 1.500000e+01 8.173100e-01 1.530200e-01 3.694800e-01
+2.975000e+02 1.750000e+01 1.750000e+01 4.812700e-01 5.977900e-02 2.580000e-01
+3.325000e+02 1.750000e+01 1.750000e+01 2.925800e-01 5.854100e-02 1.017000e-01
+3.700000e+02 2.000000e+01 2.000000e+01 1.759000e-01 3.122300e-02 6.793000e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.049600e-01 2.999000e-02 2.634900e-02
+4.575000e+02 2.250000e+01 2.250000e+01 5.317300e-02 8.767800e-03 2.365200e-02
+5.300000e+02 5.000000e+01 5.000000e+01 2.250300e-02 6.137300e-03 8.894600e-03
+6.325000e+02 5.250000e+01 5.250000e+01 7.633200e-03 7.187800e-04 4.316800e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.200700e-03 3.819800e-04 2.757200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d76-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d76-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t76
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.087800e-01 4.281009e-02 4.256285e-02
+3.750000e+01 1.250000e+01 1.250000e+01 7.984000e-01 8.448911e-02 8.972912e-02
+6.250000e+01 1.250000e+01 1.250000e+01 7.041700e-01 6.612812e-02 5.708515e-02
+8.750000e+01 1.250000e+01 1.250000e+01 5.321400e-01 4.150655e-02 4.281049e-02
+1.150000e+02 1.500000e+01 1.500000e+01 3.390600e-01 2.796040e-02 2.700158e-02
+1.450000e+02 1.500000e+01 1.500000e+01 2.771500e-01 2.555827e-02 3.259398e-02
+1.750000e+02 1.500000e+01 1.500000e+01 1.590200e-01 1.852536e-02 1.688511e-02
+2.250000e+02 3.500000e+01 3.500000e+01 9.247100e-02 1.755659e-02 1.700525e-02
+3.775000e+02 1.175000e+02 1.175000e+02 2.046100e-02 3.483494e-03 3.448098e-03
+6.975000e+02 2.025000e+02 2.025000e+02 9.135300e-04 5.418348e-04 5.435699e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d76-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d76-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t76
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.126900e-01 2.520400e-02 3.117500e-02
+3.750000e+01 1.250000e+01 1.250000e+01 6.423100e-01 5.055000e-02 7.936300e-02
+6.250000e+01 1.250000e+01 1.250000e+01 5.914100e-01 6.345500e-02 4.912000e-02
+8.750000e+01 1.250000e+01 1.250000e+01 4.830300e-01 4.930400e-02 4.401200e-02
+1.150000e+02 1.500000e+01 1.500000e+01 3.689000e-01 3.256400e-02 3.069500e-02
+1.450000e+02 1.500000e+01 1.500000e+01 2.651200e-01 3.069900e-02 1.247100e-02
+1.750000e+02 1.500000e+01 1.500000e+01 1.871300e-01 2.147500e-02 1.730200e-02
+2.250000e+02 3.500000e+01 3.500000e+01 1.053200e-01 1.055100e-02 1.023300e-02
+3.775000e+02 1.175000e+02 1.175000e+02 2.230600e-02 1.722400e-03 1.640200e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.581200e-03 2.373000e-04 2.266600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d76-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d76-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t76
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.397000e-01 2.514400e-02 1.266800e-01
+3.750000e+01 1.250000e+01 1.250000e+01 6.927500e-01 8.516200e-02 1.792200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 6.547100e-01 9.976400e-02 2.494900e-01
+8.750000e+01 1.250000e+01 1.250000e+01 5.305000e-01 9.168900e-02 1.674400e-01
+1.150000e+02 1.500000e+01 1.500000e+01 3.978900e-01 5.852800e-02 1.240000e-01
+1.450000e+02 1.500000e+01 1.500000e+01 2.915100e-01 5.425500e-02 7.554500e-02
+1.750000e+02 1.500000e+01 1.500000e+01 2.043500e-01 2.879900e-02 5.797500e-02
+2.250000e+02 3.500000e+01 3.500000e+01 1.184300e-01 2.824900e-02 2.431300e-02
+3.775000e+02 1.175000e+02 1.175000e+02 2.630300e-02 3.446000e-03 1.045700e-02
+6.975000e+02 2.025000e+02 2.025000e+02 2.006400e-03 3.923500e-04 8.622500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d77-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d77-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t77
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 7.519900e+00 2.321114e+00 2.384740e+00
+5.000000e-01 1.000000e-01 1.000000e-01 2.679800e+01 4.691930e+00 4.498031e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.341600e+01 1.157207e+01 1.169160e+01
+7.500000e-01 5.000000e-02 5.000000e-02 1.171000e+02 1.120355e+01 1.013444e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.873600e+02 1.601033e+01 1.496033e+01
+8.750000e-01 2.500000e-02 2.500000e-02 3.043500e+02 2.868889e+01 2.886343e+01
+9.250000e-01 2.500000e-02 2.500000e-02 4.002600e+02 3.493286e+01 3.610713e+01
+9.750000e-01 2.500000e-02 2.500000e-02 5.295900e+02 4.400955e+01 4.310709e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d77-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d77-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t77
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.311200e+01 1.449400e+00 1.670800e+00
+5.000000e-01 1.000000e-01 1.000000e-01 2.636600e+01 3.089700e+00 2.952400e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.527100e+01 5.121500e+00 6.217600e+00
+7.500000e-01 5.000000e-02 5.000000e-02 1.047300e+02 1.156600e+01 7.577400e+00
+8.250000e-01 2.500000e-02 2.500000e-02 1.718800e+02 1.799500e+01 1.449400e+01
+8.750000e-01 2.500000e-02 2.500000e-02 2.480800e+02 2.195600e+01 1.937600e+01
+9.250000e-01 2.500000e-02 2.500000e-02 3.516200e+02 3.175100e+01 3.940000e+01
+9.750000e-01 2.500000e-02 2.500000e-02 4.682900e+02 3.856600e+01 3.326400e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d77-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d77-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t77
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.368400e+01 2.258100e+00 3.579800e+00
+5.000000e-01 1.000000e-01 1.000000e-01 2.889500e+01 5.533300e+00 5.176200e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.779100e+01 1.133300e+01 1.597600e+01
+7.500000e-01 5.000000e-02 5.000000e-02 1.076000e+02 1.657800e+01 3.618500e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.866700e+02 3.604000e+01 4.896000e+01
+8.750000e-01 2.500000e-02 2.500000e-02 2.692400e+02 3.183000e+01 8.255500e+01
+9.250000e-01 2.500000e-02 2.500000e-02 3.962600e+02 6.234700e+01 1.126200e+02
+9.750000e-01 2.500000e-02 2.500000e-02 5.434600e+02 7.657400e+01 1.930300e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d78-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d78-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t78
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.820400e+00 8.249588e-01 8.326482e-01
+3.200000e+00 4.000000e-01 4.000000e-01 1.756400e+01 1.168185e+00 1.177140e+00
+3.800000e+00 2.000000e-01 2.000000e-01 2.330100e+01 1.977673e+00 1.786061e+00
+4.200000e+00 2.000000e-01 2.000000e-01 3.145200e+01 3.527567e+00 3.524170e+00
+4.600000e+00 2.000000e-01 2.000000e-01 3.617400e+01 3.111277e+00 2.496711e+00
+5.000000e+00 2.000000e-01 2.000000e-01 3.975000e+01 3.459769e+00 3.847957e+00
+5.400000e+00 2.000000e-01 2.000000e-01 2.664300e+01 2.343107e+00 2.366723e+00
+6.000000e+00 4.000000e-01 4.000000e-01 1.161900e+01 1.765713e+00 1.903634e+00
+7.600000e+00 1.200000e+00 1.200000e+00 5.938000e-01 2.750364e-01 2.776955e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d78-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d78-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t78
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 8.024800e+00 7.481900e-01 5.866500e-01
+3.200000e+00 4.000000e-01 4.000000e-01 1.517600e+01 1.363500e+00 8.667600e-01
+3.800000e+00 2.000000e-01 2.000000e-01 2.350900e+01 2.088000e+00 1.665800e+00
+4.200000e+00 2.000000e-01 2.000000e-01 3.085000e+01 2.968500e+00 1.876900e+00
+4.600000e+00 2.000000e-01 2.000000e-01 3.535800e+01 3.058900e+00 5.057900e+00
+5.000000e+00 2.000000e-01 2.000000e-01 3.591000e+01 3.538300e+00 3.357600e+00
+5.400000e+00 2.000000e-01 2.000000e-01 2.612600e+01 2.867700e+00 2.040000e+00
+6.000000e+00 4.000000e-01 4.000000e-01 9.726500e+00 1.245000e+00 1.018200e+00
+7.600000e+00 1.200000e+00 1.200000e+00 6.115400e-01 5.622500e-02 1.297900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d78-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d78-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t78
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.050100e+01 1.808700e+00 4.292900e+00
+3.200000e+00 4.000000e-01 4.000000e-01 1.914600e+01 3.471700e+00 6.093500e+00
+3.800000e+00 2.000000e-01 2.000000e-01 2.742300e+01 4.321400e+00 8.361700e+00
+4.200000e+00 2.000000e-01 2.000000e-01 3.268200e+01 4.483800e+00 1.086000e+01
+4.600000e+00 2.000000e-01 2.000000e-01 3.610300e+01 6.019700e+00 1.085800e+01
+5.000000e+00 2.000000e-01 2.000000e-01 3.638900e+01 3.030000e+00 1.018000e+01
+5.400000e+00 2.000000e-01 2.000000e-01 2.628900e+01 3.828900e+00 5.384700e+00
+6.000000e+00 4.000000e-01 4.000000e-01 1.057600e+01 1.557600e+00 2.983400e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.667600e-01 5.681500e-02 1.605200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d79-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d79-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t79
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.672900e-01 1.283284e-01 1.395802e-01
+1.050000e+02 1.000000e+01 1.000000e+01 6.114000e-01 6.343564e-02 6.633891e-02
+1.250000e+02 1.000000e+01 1.000000e+01 5.988800e-01 5.511955e-02 5.249953e-02
+1.475000e+02 1.250000e+01 1.250000e+01 5.134400e-01 5.272883e-02 4.578762e-02
+1.725000e+02 1.250000e+01 1.250000e+01 3.588800e-01 3.374518e-02 2.980955e-02
+1.975000e+02 1.250000e+01 1.250000e+01 2.828200e-01 2.074717e-02 2.012721e-02
+2.250000e+02 1.500000e+01 1.500000e+01 2.465000e-01 1.908910e-02 1.803991e-02
+2.575000e+02 1.750000e+01 1.750000e+01 1.608700e-01 2.961223e-02 2.911250e-02
+2.975000e+02 2.250000e+01 2.250000e+01 1.538400e-01 1.000783e-02 1.008376e-02
+3.525000e+02 3.250000e+01 3.250000e+01 9.073600e-02 7.289540e-03 7.041303e-03
+5.350000e+02 1.500000e+02 1.500000e+02 1.852800e-02 1.661871e-03 1.817394e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d79-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d79-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t79
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.924000e-01 7.545600e-02 6.181500e-02
+1.050000e+02 1.000000e+01 1.000000e+01 5.483500e-01 5.016800e-02 6.953800e-02
+1.250000e+02 1.000000e+01 1.000000e+01 5.256600e-01 6.097800e-02 8.149600e-02
+1.475000e+02 1.250000e+01 1.250000e+01 4.845100e-01 4.727000e-02 2.968700e-02
+1.725000e+02 1.250000e+01 1.250000e+01 3.785700e-01 3.402800e-02 3.129500e-02
+1.975000e+02 1.250000e+01 1.250000e+01 3.069100e-01 2.527900e-02 2.378800e-02
+2.250000e+02 1.500000e+01 1.500000e+01 2.447000e-01 2.550100e-02 1.436600e-02
+2.575000e+02 1.750000e+01 1.750000e+01 1.796800e-01 1.607700e-02 1.257400e-02
+2.975000e+02 2.250000e+01 2.250000e+01 1.321200e-01 1.231400e-02 1.061600e-02
+3.525000e+02 3.250000e+01 3.250000e+01 8.274600e-02 7.921900e-03 5.743200e-03
+5.350000e+02 1.500000e+02 1.500000e+02 1.733400e-02 1.607500e-03 1.136100e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d79-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d79-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t79
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.666200e-01 5.114400e-02 1.285700e-01
+1.050000e+02 1.000000e+01 1.000000e+01 5.362900e-01 3.190200e-02 1.679900e-01
+1.250000e+02 1.000000e+01 1.000000e+01 5.155800e-01 7.619700e-02 1.457700e-01
+1.475000e+02 1.250000e+01 1.250000e+01 4.909100e-01 8.641500e-02 1.170000e-01
+1.725000e+02 1.250000e+01 1.250000e+01 4.173200e-01 5.892800e-02 1.503100e-01
+1.975000e+02 1.250000e+01 1.250000e+01 3.381500e-01 4.784000e-02 9.492700e-02
+2.250000e+02 1.500000e+01 1.500000e+01 2.727400e-01 4.908000e-02 1.128800e-01
+2.575000e+02 1.750000e+01 1.750000e+01 2.082900e-01 3.261500e-02 7.396100e-02
+2.975000e+02 2.250000e+01 2.250000e+01 1.539200e-01 2.740200e-02 4.535800e-02
+3.525000e+02 3.250000e+01 3.250000e+01 1.063700e-01 1.880300e-02 3.072000e-02
+5.350000e+02 1.500000e+02 1.500000e+02 2.387300e-02 4.790300e-03 7.053500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d80-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d80-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t80
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 8.546800e-01 8.612225e-02 7.912468e-02
+3.750000e+01 1.250000e+01 1.250000e+01 1.722100e+00 1.695759e-01 1.694289e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.829700e+00 1.588628e-01 1.642612e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.553100e+00 1.322698e-01 1.478433e-01
+1.300000e+02 3.000000e+01 3.000000e+01 9.629900e-01 1.177879e-01 8.760995e-02
+1.925000e+02 3.250000e+01 3.250000e+01 4.948700e-01 4.828867e-02 4.378868e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.276000e-01 3.738451e-02 3.755716e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.574500e-01 2.042846e-02 2.016106e-02
+3.975000e+02 9.750000e+01 9.750000e+01 3.973300e-02 8.807956e-03 8.492160e-03
+6.975000e+02 2.025000e+02 2.025000e+02 3.488700e-03 7.847399e-04 8.642819e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d80-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d80-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t80
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 6.460100e-01 9.349400e-02 6.639100e-02
+3.750000e+01 1.250000e+01 1.250000e+01 1.448000e+00 1.662900e-01 1.544200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.520800e+00 2.040700e-01 1.740800e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.312700e+00 1.501500e-01 1.647700e-01
+1.300000e+02 3.000000e+01 3.000000e+01 9.203100e-01 1.126200e-01 1.069400e-01
+1.925000e+02 3.250000e+01 3.250000e+01 4.698100e-01 5.616300e-02 5.496900e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.462900e-01 3.263300e-02 2.491600e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.535000e-01 1.313900e-02 1.577600e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.778900e-02 6.300400e-03 4.425600e-03
+6.975000e+02 2.025000e+02 2.025000e+02 3.427000e-03 3.940400e-04 4.199200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d80-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d80-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t80
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 7.780000e-01 8.816100e-02 3.056400e-01
+3.750000e+01 1.250000e+01 1.250000e+01 1.801800e+00 2.478100e-01 6.374600e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.884900e+00 3.691500e-01 7.408700e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.575000e+00 2.500000e-01 6.653100e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.092700e+00 2.151300e-01 4.219100e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.538200e-01 1.123600e-01 2.242100e-01
+2.425000e+02 1.750000e+01 1.750000e+01 2.919000e-01 6.249100e-02 9.346700e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.860600e-01 3.746100e-02 7.458800e-02
+3.975000e+02 9.750000e+01 9.750000e+01 5.770700e-02 1.065300e-02 1.880200e-02
+6.975000e+02 2.025000e+02 2.025000e+02 4.972300e-03 1.072000e-03 1.877000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d81-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d81-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t81
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 2.302100e+01 7.646984e+00 7.235272e+00
+3.750000e-01 1.250000e-01 1.250000e-01 3.346800e+01 1.401554e+01 8.684749e+00
+6.000000e-01 1.000000e-01 1.000000e-01 1.255600e+02 1.642000e+01 1.715345e+01
+7.250000e-01 2.500000e-02 2.500000e-02 2.675100e+02 2.695763e+01 2.902101e+01
+7.750000e-01 2.500000e-02 2.500000e-02 3.698200e+02 3.379826e+01 3.701121e+01
+8.250000e-01 2.500000e-02 2.500000e-02 5.383800e+02 4.780003e+01 4.492155e+01
+8.750000e-01 2.500000e-02 2.500000e-02 8.043800e+02 6.960621e+01 6.579602e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.113700e+03 9.127146e+01 9.587340e+01
+9.750000e-01 2.500000e-02 2.500000e-02 1.409800e+03 1.074742e+02 1.066351e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d81-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d81-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t81
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 2.916200e+01 2.912700e+00 5.335800e+00
+3.750000e-01 1.250000e-01 1.250000e-01 4.794600e+01 6.722000e+00 5.485200e+00
+6.000000e-01 1.000000e-01 1.000000e-01 1.207000e+02 1.627700e+01 1.727300e+01
+7.250000e-01 2.500000e-02 2.500000e-02 2.416600e+02 3.077700e+01 3.978400e+01
+7.750000e-01 2.500000e-02 2.500000e-02 3.390800e+02 4.503100e+01 3.079300e+01
+8.250000e-01 2.500000e-02 2.500000e-02 4.668300e+02 5.311000e+01 5.642600e+01
+8.750000e-01 2.500000e-02 2.500000e-02 6.593600e+02 7.662600e+01 7.962000e+01
+9.250000e-01 2.500000e-02 2.500000e-02 9.187700e+02 1.141800e+02 1.043400e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.194900e+03 1.412200e+02 9.735700e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d81-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d81-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t81
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 2.967200e+01 5.932200e+00 9.878100e+00
+3.750000e-01 1.250000e-01 1.250000e-01 4.675100e+01 8.243100e+00 2.085400e+01
+6.000000e-01 1.000000e-01 1.000000e-01 1.262300e+02 2.556200e+01 4.486100e+01
+7.250000e-01 2.500000e-02 2.500000e-02 2.556300e+02 4.740000e+01 9.881500e+01
+7.750000e-01 2.500000e-02 2.500000e-02 3.836500e+02 5.978400e+01 1.719300e+02
+8.250000e-01 2.500000e-02 2.500000e-02 5.761800e+02 1.360000e+02 1.727100e+02
+8.750000e-01 2.500000e-02 2.500000e-02 8.018600e+02 1.223500e+02 3.151600e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.172300e+03 1.867200e+02 4.640100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.594600e+03 2.723700e+02 6.336200e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d82-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d82-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t82
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.761100e+01 3.456050e+00 3.420067e+00
+2.600000e+00 2.000000e-01 2.000000e-01 4.706400e+01 3.788729e+00 3.818097e+00
+3.000000e+00 2.000000e-01 2.000000e-01 5.251400e+01 4.227319e+00 4.144895e+00
+3.400000e+00 2.000000e-01 2.000000e-01 6.915200e+01 4.739150e+00 5.247235e+00
+3.800000e+00 2.000000e-01 2.000000e-01 7.515600e+01 5.817993e+00 5.141712e+00
+4.200000e+00 2.000000e-01 2.000000e-01 8.903400e+01 7.203957e+00 6.757537e+00
+4.600000e+00 2.000000e-01 2.000000e-01 9.695100e+01 9.096673e+00 7.540531e+00
+5.000000e+00 2.000000e-01 2.000000e-01 8.632700e+01 9.180567e+00 1.022418e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.328400e+01 8.771251e+00 6.448629e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.405800e+00 7.574342e-01 6.852392e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d82-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d82-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t82
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.002800e+01 3.442700e+00 3.056500e+00
+2.600000e+00 2.000000e-01 2.000000e-01 3.677300e+01 4.418500e+00 3.821700e+00
+3.000000e+00 2.000000e-01 2.000000e-01 4.583700e+01 5.917900e+00 4.089500e+00
+3.400000e+00 2.000000e-01 2.000000e-01 5.659000e+01 5.753100e+00 6.190500e+00
+3.800000e+00 2.000000e-01 2.000000e-01 6.915600e+01 8.471800e+00 6.454300e+00
+4.200000e+00 2.000000e-01 2.000000e-01 8.094400e+01 9.034900e+00 9.059200e+00
+4.600000e+00 2.000000e-01 2.000000e-01 8.819200e+01 1.024200e+01 1.232100e+01
+5.000000e+00 2.000000e-01 2.000000e-01 8.384700e+01 1.179800e+01 9.276300e+00
+5.600000e+00 4.000000e-01 4.000000e-01 3.948100e+01 5.011100e+00 4.857200e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.255400e+00 3.980800e-01 2.832600e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d82-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d82-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t82
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.447900e+01 1.136600e+01 1.740400e+01
+2.600000e+00 2.000000e-01 2.000000e-01 5.416800e+01 9.518500e+00 2.271900e+01
+3.000000e+00 2.000000e-01 2.000000e-01 6.529200e+01 1.341800e+01 2.728000e+01
+3.400000e+00 2.000000e-01 2.000000e-01 7.646300e+01 1.244100e+01 3.134100e+01
+3.800000e+00 2.000000e-01 2.000000e-01 8.610200e+01 1.509900e+01 3.601700e+01
+4.200000e+00 2.000000e-01 2.000000e-01 9.379700e+01 1.766300e+01 3.356600e+01
+4.600000e+00 2.000000e-01 2.000000e-01 9.440600e+01 1.761400e+01 3.743900e+01
+5.000000e+00 2.000000e-01 2.000000e-01 8.682100e+01 1.334600e+01 3.175300e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.337200e+01 6.362300e+00 1.574200e+01
+7.400000e+00 1.400000e+00 1.400000e+00 2.947900e+00 5.055900e-01 6.195800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d83-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d83-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t83
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.230900e+00 2.363524e-01 2.208020e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.367500e+00 2.699029e-01 1.971903e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.401200e+00 1.569007e-01 1.398365e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.224800e+00 1.113375e-01 9.117330e-02
+1.775000e+02 1.250000e+01 1.250000e+01 9.815500e-01 8.478990e-02 8.393441e-02
+2.050000e+02 1.500000e+01 1.500000e+01 8.136600e-01 5.240337e-02 5.084697e-02
+2.350000e+02 1.500000e+01 1.500000e+01 6.854200e-01 4.803824e-02 4.945945e-02
+2.650000e+02 1.500000e+01 1.500000e+01 5.444200e-01 5.055078e-02 4.844646e-02
+2.975000e+02 1.750000e+01 1.750000e+01 5.018000e-01 3.177053e-02 3.279758e-02
+3.325000e+02 1.750000e+01 1.750000e+01 3.830600e-01 3.868264e-02 4.028094e-02
+3.700000e+02 2.000000e+01 2.000000e+01 3.030500e-01 2.151354e-02 2.319422e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.886800e-01 1.553877e-02 1.418631e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.129500e-01 1.066773e-02 1.014564e-02
+5.300000e+02 5.000000e+01 5.000000e+01 5.356500e-02 6.216788e-03 6.002569e-03
+7.300000e+02 1.500000e+02 1.500000e+02 7.651500e-03 1.465704e-03 1.534366e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d83-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d83-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t83
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.039900e+00 1.611800e-01 1.698200e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.224500e+00 1.710600e-01 1.401200e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.230700e+00 1.620600e-01 1.894200e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.094500e+00 1.256300e-01 1.221100e-01
+1.775000e+02 1.250000e+01 1.250000e+01 9.337600e-01 1.004600e-01 1.012000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 7.834900e-01 1.081600e-01 7.402400e-02
+2.350000e+02 1.500000e+01 1.500000e+01 6.376300e-01 7.086200e-02 6.465700e-02
+2.650000e+02 1.500000e+01 1.500000e+01 5.178300e-01 6.202500e-02 4.300600e-02
+2.975000e+02 1.750000e+01 1.750000e+01 4.174200e-01 4.358100e-02 4.600200e-02
+3.325000e+02 1.750000e+01 1.750000e+01 3.324600e-01 3.657400e-02 2.870000e-02
+3.700000e+02 2.000000e+01 2.000000e+01 2.449200e-01 2.993200e-02 2.903200e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.620600e-01 1.975900e-02 1.527800e-02
+4.575000e+02 2.250000e+01 2.250000e+01 9.927100e-02 1.168200e-02 1.401800e-02
+5.300000e+02 5.000000e+01 5.000000e+01 4.562900e-02 5.759600e-03 3.406500e-03
+7.300000e+02 1.500000e+02 1.500000e+02 7.432100e-03 8.321700e-04 6.613600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d83-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d83-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t83
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.193500e+00 1.333100e-01 3.407400e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.264400e+00 1.563100e-01 5.121700e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.267500e+00 2.238800e-01 4.767600e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.215700e+00 2.394700e-01 4.412900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.126900e+00 2.102700e-01 4.224000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 9.228200e-01 1.453900e-01 4.038200e-01
+2.350000e+02 1.500000e+01 1.500000e+01 7.897200e-01 1.531800e-01 2.964800e-01
+2.650000e+02 1.500000e+01 1.500000e+01 6.680500e-01 1.176200e-01 2.909900e-01
+2.975000e+02 1.750000e+01 1.750000e+01 5.572800e-01 1.033900e-01 2.439400e-01
+3.325000e+02 1.750000e+01 1.750000e+01 4.738300e-01 8.338800e-02 1.748400e-01
+3.700000e+02 2.000000e+01 2.000000e+01 3.564400e-01 7.142800e-02 1.213200e-01
+4.125000e+02 2.250000e+01 2.250000e+01 2.427100e-01 6.847700e-02 7.604900e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.438900e-01 2.485000e-02 6.675300e-02
+5.300000e+02 5.000000e+01 5.000000e+01 7.098200e-02 1.507400e-02 2.817900e-02
+7.300000e+02 1.500000e+02 1.500000e+02 1.221600e-02 2.064100e-03 6.538900e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d84-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d84-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t84
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 4.347400e+02 5.795541e+01 6.211122e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.845800e+02 5.274486e+01 5.032847e+01
+3.000000e-01 5.000000e-02 5.000000e-02 3.647200e+02 5.068410e+01 5.084223e+01
+4.500000e-01 1.000000e-01 1.000000e-01 2.688400e+02 4.779646e+01 4.023696e+01
+6.000000e-01 5.000000e-02 5.000000e-02 1.889400e+02 2.910514e+01 2.964744e+01
+7.500000e-01 1.000000e-01 1.000000e-01 8.870300e+01 1.384812e+01 1.426679e+01
+1.025000e+00 1.750000e-01 1.750000e-01 2.708000e+01 4.515114e+00 4.539786e+00
+1.850000e+00 6.500000e-01 6.500000e-01 2.292300e+00 4.370611e-01 4.426839e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d84-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d84-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t84
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.321700e+02 5.383300e+01 4.128500e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.224100e+02 4.767800e+01 4.784700e+01
+3.000000e-01 5.000000e-02 5.000000e-02 3.263500e+02 5.051200e+01 4.407900e+01
+4.500000e-01 1.000000e-01 1.000000e-01 2.437600e+02 3.066900e+01 3.452800e+01
+6.000000e-01 5.000000e-02 5.000000e-02 1.597000e+02 2.220900e+01 2.097700e+01
+7.500000e-01 1.000000e-01 1.000000e-01 8.221600e+01 1.097900e+01 9.676500e+00
+1.025000e+00 1.750000e-01 1.750000e-01 2.277500e+01 3.576700e+00 1.967800e+00
+1.850000e+00 6.500000e-01 6.500000e-01 1.609100e+00 2.676200e-01 2.410200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d84-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d84-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t84
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 4.378000e+02 8.450300e+01 1.977600e+02
+2.000000e-01 5.000000e-02 5.000000e-02 4.204900e+02 8.073100e+01 1.929300e+02
+3.000000e-01 5.000000e-02 5.000000e-02 4.200800e+02 8.238600e+01 1.944700e+02
+4.500000e-01 1.000000e-01 1.000000e-01 3.125500e+02 6.555000e+01 1.322200e+02
+6.000000e-01 5.000000e-02 5.000000e-02 2.066400e+02 4.837800e+01 8.167300e+01
+7.500000e-01 1.000000e-01 1.000000e-01 1.106500e+02 2.555100e+01 4.710600e+01
+1.025000e+00 1.750000e-01 1.750000e-01 3.358800e+01 8.781200e+00 1.261500e+01
+1.850000e+00 6.500000e-01 6.500000e-01 2.349700e+00 5.707100e-01 1.011300e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d85-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d85-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t85
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.247200e+02 2.503460e+01 2.851347e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.848800e+02 5.262616e+01 3.346398e+01
+3.250000e-01 7.500000e-02 7.500000e-02 4.329600e+02 3.719179e+01 3.749501e+01
+4.750000e-01 7.500000e-02 7.500000e-02 3.746100e+02 3.679920e+01 3.706925e+01
+6.750000e-01 1.250000e-01 1.250000e-01 1.703000e+02 1.989806e+01 1.730539e+01
+9.000000e-01 1.000000e-01 1.000000e-01 3.995000e+01 5.329199e+00 5.208289e+00
+1.750000e+00 7.500000e-01 7.500000e-01 2.382200e+00 3.930711e-01 3.966423e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d85-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d85-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t85
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.018300e+02 2.525500e+01 2.559800e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.464100e+02 3.608800e+01 3.342900e+01
+3.250000e-01 7.500000e-02 7.500000e-02 3.971700e+02 5.379100e+01 4.828200e+01
+4.750000e-01 7.500000e-02 7.500000e-02 3.274300e+02 4.371800e+01 3.635600e+01
+6.750000e-01 1.250000e-01 1.250000e-01 1.464000e+02 2.012900e+01 1.994100e+01
+9.000000e-01 1.000000e-01 1.000000e-01 3.425100e+01 5.986100e+00 4.486000e+00
+1.750000e+00 7.500000e-01 7.500000e-01 1.593600e+00 2.331500e-01 2.907300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d85-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d85-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t85
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.382400e+02 4.966400e+01 1.057100e+02
+2.000000e-01 5.000000e-02 5.000000e-02 3.961600e+02 6.686700e+01 1.237500e+02
+3.250000e-01 7.500000e-02 7.500000e-02 4.576100e+02 7.642000e+01 1.879100e+02
+4.750000e-01 7.500000e-02 7.500000e-02 4.087400e+02 7.475900e+01 1.786400e+02
+6.750000e-01 1.250000e-01 1.250000e-01 1.992300e+02 4.159300e+01 8.039300e+01
+9.000000e-01 1.000000e-01 1.000000e-01 5.022400e+01 1.168900e+01 2.223400e+01
+1.750000e+00 7.500000e-01 7.500000e-01 2.270300e+00 4.911400e-01 1.075100e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d86-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d86-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t86
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.414400e+02 8.672454e+00 7.780229e+00
+1.000000e+00 5.000000e-01 5.000000e-01 7.665500e+01 8.583108e+00 7.459364e+00
+2.000000e+00 5.000000e-01 5.000000e-01 3.080900e+01 4.180022e+00 4.464411e+00
+3.000000e+00 5.000000e-01 5.000000e-01 9.790800e+00 2.027761e+00 1.998234e+00
+6.000000e+00 2.500000e+00 2.500000e+00 3.549500e+00 1.178194e+00 1.009966e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d86-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d86-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t86
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.283600e+02 1.287900e+01 1.183900e+01
+1.000000e+00 5.000000e-01 5.000000e-01 6.845200e+01 9.888400e+00 8.883300e+00
+2.000000e+00 5.000000e-01 5.000000e-01 2.620200e+01 3.683300e+00 3.543100e+00
+3.000000e+00 5.000000e-01 5.000000e-01 8.274100e+00 1.530400e+00 1.346200e+00
+6.000000e+00 2.500000e+00 2.500000e+00 3.162600e+00 4.991000e-01 4.510400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d86-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d86-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t86
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.482500e+02 2.285400e+01 4.891200e+01
+1.000000e+00 5.000000e-01 5.000000e-01 8.725800e+01 1.738000e+01 3.863700e+01
+2.000000e+00 5.000000e-01 5.000000e-01 3.441100e+01 7.705900e+00 1.574400e+01
+3.000000e+00 5.000000e-01 5.000000e-01 1.082300e+01 2.179800e+00 4.632600e+00
+6.000000e+00 2.500000e+00 2.500000e+00 2.821900e+00 3.718700e-01 1.463200e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d87-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d87-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.345400e+00 6.283506e-01 6.385587e-01
+5.800000e+02 3.500000e+01 3.500000e+01 4.960800e+00 3.555689e-01 3.514885e-01
+6.550000e+02 4.000000e+01 4.000000e+01 3.607100e+00 2.477671e-01 2.512099e-01
+7.400000e+02 4.500000e+01 4.500000e+01 2.500100e+00 1.661609e-01 1.490339e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.698200e+00 1.253064e-01 1.200099e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.135700e+00 7.611003e-02 9.353712e-02
+1.042500e+03 5.750000e+01 5.750000e+01 7.612900e-01 5.902181e-02 5.512267e-02
+1.150000e+03 5.000000e+01 5.000000e+01 4.986300e-01 4.476704e-02 3.211264e-02
+1.275000e+03 7.500000e+01 7.500000e+01 3.215300e-01 3.539612e-02 2.299664e-02
+1.425000e+03 7.500000e+01 7.500000e+01 2.053000e-01 1.960732e-02 2.564483e-02
+1.750000e+03 2.500000e+02 2.500000e+02 8.434500e-02 9.472271e-03 1.062872e-02
+2.350000e+03 3.500000e+02 3.500000e+02 1.466300e-02 2.688886e-03 2.399257e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.497700e-03 4.270761e-04 3.916612e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d87-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d87-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 5.189500e+00 6.646800e-01 4.813300e-01
+5.800000e+02 3.500000e+01 3.500000e+01 4.064400e+00 4.873900e-01 4.491200e-01
+6.550000e+02 4.000000e+01 4.000000e+01 2.940600e+00 3.623100e-01 3.876200e-01
+7.400000e+02 4.500000e+01 4.500000e+01 2.074700e+00 2.906300e-01 2.113500e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.427100e+00 1.793300e-01 1.504700e-01
+9.325000e+02 5.250000e+01 5.250000e+01 9.744700e-01 1.204500e-01 1.030300e-01
+1.042500e+03 5.750000e+01 5.750000e+01 6.551300e-01 8.060800e-02 7.529300e-02
+1.150000e+03 5.000000e+01 5.000000e+01 4.526800e-01 5.282000e-02 6.030800e-02
+1.275000e+03 7.500000e+01 7.500000e+01 2.994500e-01 3.891800e-02 3.251400e-02
+1.425000e+03 7.500000e+01 7.500000e+01 1.862400e-01 2.447800e-02 1.554400e-02
+1.750000e+03 2.500000e+02 2.500000e+02 7.816500e-02 9.135900e-03 8.739000e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.649200e-02 1.713100e-03 1.375700e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.727600e-03 1.849300e-04 1.868400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d87-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d87-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 5.421500e+00 1.325300e+00 1.985600e+00
+5.800000e+02 3.500000e+01 3.500000e+01 4.268400e+00 1.064600e+00 1.610500e+00
+6.550000e+02 4.000000e+01 4.000000e+01 3.073400e+00 7.723900e-01 1.171600e+00
+7.400000e+02 4.500000e+01 4.500000e+01 2.184200e+00 5.600800e-01 8.571600e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.512900e+00 3.939700e-01 6.068100e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.035900e+00 2.749000e-01 4.269400e-01
+1.042500e+03 5.750000e+01 5.750000e+01 6.863500e-01 1.839600e-01 2.869700e-01
+1.150000e+03 5.000000e+01 5.000000e+01 4.767700e-01 1.302100e-01 2.047800e-01
+1.275000e+03 7.500000e+01 7.500000e+01 3.177100e-01 8.769500e-02 1.388000e-01
+1.425000e+03 7.500000e+01 7.500000e+01 2.005600e-01 5.687800e-02 9.136200e-02
+1.750000e+03 2.500000e+02 2.500000e+02 8.242300e-02 2.368700e-02 3.828700e-02
+2.350000e+03 3.500000e+02 3.500000e+02 1.697600e-02 5.169700e-03 8.610000e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.768800e-03 5.715800e-04 9.824900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d87-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d87-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 5.245900e+00 1.046600e+00 2.291600e+00
+5.800000e+02 3.500000e+01 3.500000e+01 4.166000e+00 7.955300e-01 1.822200e+00
+6.550000e+02 4.000000e+01 4.000000e+01 3.068100e+00 5.780100e-01 1.336000e+00
+7.400000e+02 4.500000e+01 4.500000e+01 2.198800e+00 4.371200e-01 9.161400e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.597800e+00 3.599300e-01 5.767300e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.094800e+00 2.048300e-01 4.545500e-01
+1.042500e+03 5.750000e+01 5.750000e+01 7.471200e-01 1.389900e-01 3.049900e-01
+1.150000e+03 5.000000e+01 5.000000e+01 5.265600e-01 9.647500e-02 2.111000e-01
+1.275000e+03 7.500000e+01 7.500000e+01 3.652300e-01 5.967500e-02 1.373000e-01
+1.425000e+03 7.500000e+01 7.500000e+01 2.308300e-01 4.210600e-02 7.928000e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.005300e-01 1.783600e-02 4.013200e-02
+2.350000e+03 3.500000e+02 3.500000e+02 2.146900e-02 3.521900e-03 7.645500e-03
+3.350000e+03 6.500000e+02 6.500000e+02 2.395800e-03 5.135400e-04 1.198300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d88-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d88-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 6.686800e+00 6.362590e-01 6.131993e-01
+3.750000e+01 1.250000e+01 1.250000e+01 1.373000e+01 1.237871e+00 1.291998e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.337800e+01 1.099245e+00 1.113073e+00
+8.750000e+01 1.250000e+01 1.250000e+01 1.020500e+01 7.321694e-01 7.441399e-01
+1.150000e+02 1.500000e+01 1.500000e+01 6.936000e+00 4.835363e-01 4.427047e-01
+1.450000e+02 1.500000e+01 1.500000e+01 4.871300e+00 4.563773e-01 3.811436e-01
+1.750000e+02 1.500000e+01 1.500000e+01 3.125300e+00 2.446411e-01 2.454333e-01
+2.075000e+02 1.750000e+01 1.750000e+01 1.836400e+00 1.628755e-01 1.472490e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.050500e+00 9.161548e-02 1.008043e-01
+2.800000e+02 2.000000e+01 2.000000e+01 6.262700e-01 7.411697e-02 7.248302e-02
+3.975000e+02 9.750000e+01 9.750000e+01 1.206400e-01 2.266544e-02 2.255991e-02
+6.975000e+02 2.025000e+02 2.025000e+02 5.853700e-03 1.238371e-03 1.310000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d88-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d88-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.812200e+00 7.881100e-01 7.603200e-01
+3.750000e+01 1.250000e+01 1.250000e+01 1.063800e+01 1.265400e+00 1.234200e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.059800e+01 1.325600e+00 1.134200e+00
+8.750000e+01 1.250000e+01 1.250000e+01 8.514900e+00 1.058100e+00 9.114000e-01
+1.150000e+02 1.500000e+01 1.500000e+01 6.209700e+00 7.671000e-01 7.232000e-01
+1.450000e+02 1.500000e+01 1.500000e+01 4.351500e+00 5.547000e-01 4.442300e-01
+1.750000e+02 1.500000e+01 1.500000e+01 2.905400e+00 3.307500e-01 3.042800e-01
+2.075000e+02 1.750000e+01 1.750000e+01 1.795700e+00 2.291700e-01 1.699700e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.037300e+00 1.075200e-01 1.064500e-01
+2.800000e+02 2.000000e+01 2.000000e+01 5.956100e-01 7.400100e-02 5.484300e-02
+3.975000e+02 9.750000e+01 9.750000e+01 1.554900e-01 1.658700e-02 1.475700e-02
+6.975000e+02 2.025000e+02 2.025000e+02 7.122200e-03 7.693000e-04 5.454900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d88-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d88-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 5.348700e+00 1.197000e+00 1.742800e+00
+3.750000e+01 1.250000e+01 1.250000e+01 1.122200e+01 2.678700e+00 3.995600e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.078700e+01 2.730100e+00 4.157200e+00
+8.750000e+01 1.250000e+01 1.250000e+01 8.765100e+00 2.285400e+00 3.510600e+00
+1.150000e+02 1.500000e+01 1.500000e+01 6.365800e+00 1.690500e+00 2.623900e+00
+1.450000e+02 1.500000e+01 1.500000e+01 4.535400e+00 1.239000e+00 1.948000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 3.070000e+00 8.363200e-01 1.311800e+00
+2.075000e+02 1.750000e+01 1.750000e+01 1.905700e+00 5.197300e-01 8.125000e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.155900e+00 3.167400e-01 4.947000e-01
+2.800000e+02 2.000000e+01 2.000000e+01 6.816100e-01 1.869100e-01 2.913600e-01
+3.975000e+02 9.750000e+01 9.750000e+01 1.888400e-01 5.226500e-02 8.144700e-02
+6.975000e+02 2.025000e+02 2.025000e+02 9.781400e-03 2.780300e-03 4.349400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d88-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d88-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 5.150100e+00 7.406100e-01 2.057300e+00
+3.750000e+01 1.250000e+01 1.250000e+01 1.166400e+01 2.178500e+00 4.761500e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.152600e+01 2.413900e+00 4.801200e+00
+8.750000e+01 1.250000e+01 1.250000e+01 9.192700e+00 1.649700e+00 3.884100e+00
+1.150000e+02 1.500000e+01 1.500000e+01 6.639500e+00 1.298700e+00 2.947600e+00
+1.450000e+02 1.500000e+01 1.500000e+01 4.673100e+00 9.886800e-01 1.890700e+00
+1.750000e+02 1.500000e+01 1.500000e+01 3.060900e+00 6.205400e-01 1.322500e+00
+2.075000e+02 1.750000e+01 1.750000e+01 1.845400e+00 4.101900e-01 7.583000e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.097200e+00 2.220700e-01 4.785800e-01
+2.800000e+02 2.000000e+01 2.000000e+01 6.320400e-01 1.189400e-01 2.311100e-01
+3.975000e+02 9.750000e+01 9.750000e+01 1.667700e-01 3.584900e-02 5.748000e-02
+6.975000e+02 2.025000e+02 2.025000e+02 9.573600e-03 2.066400e-03 3.171200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d89-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d89-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.385800e+02 3.239514e+01 3.056628e+01
+2.250000e-01 7.500000e-02 7.500000e-02 1.951300e+02 4.141045e+01 3.119311e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.169200e+02 3.649278e+01 3.761133e+01
+4.500000e-01 5.000000e-02 5.000000e-02 3.687800e+02 4.708633e+01 4.735659e+01
+5.500000e-01 5.000000e-02 5.000000e-02 5.973400e+02 6.784832e+01 6.418598e+01
+6.250000e-01 2.500000e-02 2.500000e-02 1.009600e+03 9.293142e+01 8.422428e+01
+6.750000e-01 2.500000e-02 2.500000e-02 1.253100e+03 9.759674e+01 1.006047e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.722200e+03 1.415085e+02 1.488028e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.591500e+03 1.797726e+02 1.835356e+02
+8.250000e-01 2.500000e-02 2.500000e-02 3.765200e+03 2.764705e+02 2.684448e+02
+8.750000e-01 2.500000e-02 2.500000e-02 5.168800e+03 3.773654e+02 3.749603e+02
+9.250000e-01 2.500000e-02 2.500000e-02 6.703100e+03 4.744396e+02 4.736964e+02
+9.750000e-01 2.500000e-02 2.500000e-02 8.541300e+03 6.196934e+02 6.302609e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d89-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d89-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.712500e+02 2.328800e+01 2.031300e+01
+2.250000e-01 7.500000e-02 7.500000e-02 2.007800e+02 2.529700e+01 2.049800e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.708900e+02 3.701700e+01 3.215900e+01
+4.500000e-01 5.000000e-02 5.000000e-02 3.795500e+02 4.916400e+01 5.146200e+01
+5.500000e-01 5.000000e-02 5.000000e-02 5.875100e+02 7.516400e+01 7.132500e+01
+6.250000e-01 2.500000e-02 2.500000e-02 8.664900e+02 1.208400e+02 1.000100e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.145400e+03 1.594900e+02 1.317400e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.577700e+03 2.174400e+02 1.737000e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.162400e+03 2.583800e+02 2.217400e+02
+8.250000e-01 2.500000e-02 2.500000e-02 2.978000e+03 3.504300e+02 3.354300e+02
+8.750000e-01 2.500000e-02 2.500000e-02 4.086900e+03 4.855200e+02 4.219000e+02
+9.250000e-01 2.500000e-02 2.500000e-02 5.412700e+03 6.471000e+02 5.975100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 6.664600e+03 8.707200e+02 6.753600e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d89-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d89-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.762300e+02 4.934000e+01 7.879400e+01
+2.250000e-01 7.500000e-02 7.500000e-02 2.058900e+02 5.747000e+01 9.143700e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.711900e+02 7.649000e+01 1.232500e+02
+4.500000e-01 5.000000e-02 5.000000e-02 3.657500e+02 1.012500e+02 1.611000e+02
+5.500000e-01 5.000000e-02 5.000000e-02 5.852100e+02 1.654900e+02 2.637600e+02
+6.250000e-01 2.500000e-02 2.500000e-02 8.188900e+02 2.243600e+02 3.522600e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.100100e+03 2.997600e+02 4.705600e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.521600e+03 4.130900e+02 6.481000e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.130800e+03 5.686900e+02 8.822000e+02
+8.250000e-01 2.500000e-02 2.500000e-02 3.007200e+03 7.898300e+02 1.216600e+03
+8.750000e-01 2.500000e-02 2.500000e-02 4.251700e+03 1.086500e+03 1.657100e+03
+9.250000e-01 2.500000e-02 2.500000e-02 5.916400e+03 1.462500e+03 2.204800e+03
+9.750000e-01 2.500000e-02 2.500000e-02 7.612900e+03 1.816500e+03 2.698500e+03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d89-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d89-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.605600e+02 3.541500e+01 6.150200e+01
+2.250000e-01 7.500000e-02 7.500000e-02 1.868100e+02 3.720000e+01 8.916700e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.435700e+02 5.204100e+01 1.019900e+02
+4.500000e-01 5.000000e-02 5.000000e-02 3.409500e+02 6.501800e+01 1.514000e+02
+5.500000e-01 5.000000e-02 5.000000e-02 5.397700e+02 1.168500e+02 2.200200e+02
+6.250000e-01 2.500000e-02 2.500000e-02 8.286900e+02 1.730700e+02 3.025800e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.105300e+03 2.099200e+02 4.431300e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.575100e+03 3.042800e+02 6.656500e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.232000e+03 3.918100e+02 1.008600e+03
+8.250000e-01 2.500000e-02 2.500000e-02 3.217700e+03 6.539700e+02 1.331300e+03
+8.750000e-01 2.500000e-02 2.500000e-02 4.515100e+03 8.594000e+02 1.925600e+03
+9.250000e-01 2.500000e-02 2.500000e-02 6.198000e+03 1.264400e+03 2.500100e+03
+9.750000e-01 2.500000e-02 2.500000e-02 7.723100e+03 1.387900e+03 3.173800e+03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d90-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d90-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 5.077600e+02 3.462433e+01 3.362834e+01
+2.600000e+00 2.000000e-01 2.000000e-01 6.270400e+02 3.931143e+01 3.957405e+01
+3.000000e+00 2.000000e-01 2.000000e-01 7.263600e+02 4.470956e+01 4.586098e+01
+3.400000e+00 2.000000e-01 2.000000e-01 7.859100e+02 5.164003e+01 5.295506e+01
+3.800000e+00 2.000000e-01 2.000000e-01 7.077900e+02 5.530817e+01 5.384023e+01
+4.200000e+00 2.000000e-01 2.000000e-01 4.398700e+02 3.673335e+01 3.512347e+01
+4.600000e+00 2.000000e-01 2.000000e-01 2.400300e+02 2.221590e+01 2.274785e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.154700e+02 1.446053e+01 1.405010e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.243200e+01 9.426323e+00 6.896334e+00
+6.200000e+00 2.000000e-01 2.000000e-01 1.202700e+01 3.301047e+00 3.078377e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.478100e-01 3.664103e-01 3.132278e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d90-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d90-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.167600e+02 4.547600e+01 4.181200e+01
+2.600000e+00 2.000000e-01 2.000000e-01 5.068400e+02 5.699200e+01 4.931700e+01
+3.000000e+00 2.000000e-01 2.000000e-01 6.012200e+02 7.730800e+01 6.630100e+01
+3.400000e+00 2.000000e-01 2.000000e-01 6.554000e+02 8.032000e+01 7.149600e+01
+3.800000e+00 2.000000e-01 2.000000e-01 5.947600e+02 7.543400e+01 6.385300e+01
+4.200000e+00 2.000000e-01 2.000000e-01 3.693700e+02 5.368700e+01 4.448200e+01
+4.600000e+00 2.000000e-01 2.000000e-01 2.112100e+02 2.990600e+01 2.417500e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.102300e+02 1.471400e+01 1.419000e+01
+5.600000e+00 4.000000e-01 4.000000e-01 3.959900e+01 5.101100e+00 4.811500e+00
+6.200000e+00 2.000000e-01 2.000000e-01 1.069200e+01 2.646100e+00 1.101200e+00
+7.600000e+00 1.200000e+00 1.200000e+00 8.500700e-01 6.860900e-02 1.690100e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d90-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d90-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 5.380500e+02 1.362000e+02 2.055300e+02
+2.600000e+00 2.000000e-01 2.000000e-01 6.000900e+02 1.519000e+02 2.296500e+02
+3.000000e+00 2.000000e-01 2.000000e-01 6.491400e+02 1.640400e+02 2.488300e+02
+3.400000e+00 2.000000e-01 2.000000e-01 6.621100e+02 1.685000e+02 2.572100e+02
+3.800000e+00 2.000000e-01 2.000000e-01 5.639300e+02 1.428500e+02 2.187200e+02
+4.200000e+00 2.000000e-01 2.000000e-01 3.478300e+02 9.099600e+01 1.415100e+02
+4.600000e+00 2.000000e-01 2.000000e-01 1.921300e+02 5.169100e+01 8.195400e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.011100e+02 2.798900e+01 4.487600e+01
+5.600000e+00 4.000000e-01 4.000000e-01 3.720400e+01 1.085000e+01 1.797400e+01
+6.200000e+00 2.000000e-01 2.000000e-01 9.907200e+00 3.151000e+00 5.605000e+00
+7.600000e+00 1.200000e+00 1.200000e+00 8.464300e-01 2.840000e-01 5.216000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d90-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d90-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 5.026400e+02 1.035700e+02 2.239800e+02
+2.600000e+00 2.000000e-01 2.000000e-01 5.912000e+02 1.082000e+02 2.596600e+02
+3.000000e+00 2.000000e-01 2.000000e-01 6.717900e+02 1.423900e+02 2.722900e+02
+3.400000e+00 2.000000e-01 2.000000e-01 6.879300e+02 1.342800e+02 2.848200e+02
+3.800000e+00 2.000000e-01 2.000000e-01 5.936200e+02 1.139300e+02 2.469100e+02
+4.200000e+00 2.000000e-01 2.000000e-01 3.625100e+02 6.665900e+01 1.489800e+02
+4.600000e+00 2.000000e-01 2.000000e-01 2.069800e+02 4.201700e+01 8.118200e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.113600e+02 1.582500e+01 3.950300e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.353700e+01 6.415000e+00 1.580300e+01
+6.200000e+00 2.000000e-01 2.000000e-01 1.305200e+01 2.727600e+00 2.389800e+00
+7.600000e+00 1.200000e+00 1.200000e+00 1.263800e+00 1.343500e-01 3.251800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d91-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d91-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.163300e+01 1.457982e+00 1.409526e+00
+1.050000e+02 1.000000e+01 1.000000e+01 1.279900e+01 1.308648e+00 1.298884e+00
+1.275000e+02 1.250000e+01 1.250000e+01 1.197200e+01 9.187943e-01 9.310671e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.040900e+01 6.983664e-01 6.436609e-01
+1.775000e+02 1.250000e+01 1.250000e+01 8.399800e+00 4.930730e-01 4.808062e-01
+2.050000e+02 1.500000e+01 1.500000e+01 6.012400e+00 3.049790e-01 2.986977e-01
+2.350000e+02 1.500000e+01 1.500000e+01 3.820000e+00 1.819593e-01 1.815982e-01
+2.650000e+02 1.500000e+01 1.500000e+01 2.410300e+00 1.304611e-01 1.238769e-01
+2.975000e+02 1.750000e+01 1.750000e+01 1.454800e+00 8.170435e-02 8.658265e-02
+3.325000e+02 1.750000e+01 1.750000e+01 8.123100e-01 5.041611e-02 5.304323e-02
+3.700000e+02 2.000000e+01 2.000000e+01 4.905100e-01 4.323071e-02 4.585957e-02
+4.125000e+02 2.250000e+01 2.250000e+01 2.656600e-01 2.211866e-02 2.000179e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.558900e-01 1.491181e-02 1.383376e-02
+5.300000e+02 5.000000e+01 5.000000e+01 6.006300e-02 7.026720e-03 6.682852e-03
+6.325000e+02 5.250000e+01 5.250000e+01 1.817100e-02 3.713347e-03 3.630039e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.412400e-03 8.271355e-04 8.225211e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d91-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d91-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 9.167100e+00 1.467600e+00 1.126000e+00
+1.050000e+02 1.000000e+01 1.000000e+01 1.040400e+01 1.455700e+00 1.138200e+00
+1.275000e+02 1.250000e+01 1.250000e+01 9.984400e+00 1.281800e+00 1.259100e+00
+1.525000e+02 1.250000e+01 1.250000e+01 8.767000e+00 1.040500e+00 9.026900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 7.167400e+00 8.299700e-01 7.835400e-01
+2.050000e+02 1.500000e+01 1.500000e+01 5.145300e+00 6.172900e-01 4.774200e-01
+2.350000e+02 1.500000e+01 1.500000e+01 3.313300e+00 3.656800e-01 3.232700e-01
+2.650000e+02 1.500000e+01 1.500000e+01 2.088400e+00 2.361100e-01 1.918000e-01
+2.975000e+02 1.750000e+01 1.750000e+01 1.270200e+00 1.327000e-01 1.306500e-01
+3.325000e+02 1.750000e+01 1.750000e+01 7.566400e-01 8.487200e-02 4.965600e-02
+3.700000e+02 2.000000e+01 2.000000e+01 4.394200e-01 4.849800e-02 4.406300e-02
+4.125000e+02 2.250000e+01 2.250000e+01 2.469700e-01 2.745000e-02 2.244800e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.370800e-01 1.516300e-02 1.641200e-02
+5.300000e+02 5.000000e+01 5.000000e+01 5.797400e-02 6.763700e-03 3.551500e-03
+6.325000e+02 5.250000e+01 5.250000e+01 1.741100e-02 2.438800e-03 1.845500e-03
+8.425000e+02 1.575000e+02 1.575000e+02 2.787800e-03 4.042100e-04 3.313600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d91-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d91-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 8.009900e+00 2.028500e+00 3.149900e+00
+1.050000e+02 1.000000e+01 1.000000e+01 9.429800e+00 2.366500e+00 3.623600e+00
+1.275000e+02 1.250000e+01 1.250000e+01 9.781600e+00 2.490900e+00 3.820600e+00
+1.525000e+02 1.250000e+01 1.250000e+01 9.104700e+00 2.301000e+00 3.499600e+00
+1.775000e+02 1.250000e+01 1.250000e+01 8.004500e+00 2.031700e+00 3.087800e+00
+2.050000e+02 1.500000e+01 1.500000e+01 5.844000e+00 1.498000e+00 2.286500e+00
+2.350000e+02 1.500000e+01 1.500000e+01 3.926600e+00 1.018300e+00 1.557100e+00
+2.650000e+02 1.500000e+01 1.500000e+01 2.567600e+00 6.739900e-01 1.032700e+00
+2.975000e+02 1.750000e+01 1.750000e+01 1.564700e+00 4.148300e-01 6.377500e-01
+3.325000e+02 1.750000e+01 1.750000e+01 9.581800e-01 2.569600e-01 3.963400e-01
+3.700000e+02 2.000000e+01 2.000000e+01 5.759000e-01 1.558000e-01 2.403300e-01
+4.125000e+02 2.250000e+01 2.250000e+01 3.337600e-01 9.139300e-02 1.414900e-01
+4.575000e+02 2.250000e+01 2.250000e+01 1.840600e-01 5.042800e-02 7.824000e-02
+5.300000e+02 5.000000e+01 5.000000e+01 7.972500e-02 2.227800e-02 3.464600e-02
+6.325000e+02 5.250000e+01 5.250000e+01 2.374100e-02 6.799300e-03 1.069900e-02
+8.425000e+02 1.575000e+02 1.575000e+02 3.652400e-03 1.064200e-03 1.681200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d91-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d91-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 8.388400e+00 1.329500e+00 3.479200e+00
+1.050000e+02 1.000000e+01 1.000000e+01 9.899200e+00 1.960200e+00 4.097100e+00
+1.275000e+02 1.250000e+01 1.250000e+01 1.011600e+01 2.010500e+00 4.103000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 9.440600e+00 1.792300e+00 3.947200e+00
+1.775000e+02 1.250000e+01 1.250000e+01 8.054100e+00 1.544000e+00 3.254500e+00
+2.050000e+02 1.500000e+01 1.500000e+01 5.884600e+00 1.114000e+00 2.684300e+00
+2.350000e+02 1.500000e+01 1.500000e+01 3.947500e+00 8.044100e-01 1.603300e+00
+2.650000e+02 1.500000e+01 1.500000e+01 2.523800e+00 5.188700e-01 1.095500e+00
+2.975000e+02 1.750000e+01 1.750000e+01 1.559100e+00 2.811500e-01 7.008000e-01
+3.325000e+02 1.750000e+01 1.750000e+01 9.881800e-01 2.219100e-01 3.556300e-01
+3.700000e+02 2.000000e+01 2.000000e+01 5.858200e-01 1.187100e-01 2.147400e-01
+4.125000e+02 2.250000e+01 2.250000e+01 3.423300e-01 8.872900e-02 1.057400e-01
+4.575000e+02 2.250000e+01 2.250000e+01 1.915600e-01 3.840500e-02 7.859200e-02
+5.300000e+02 5.000000e+01 5.000000e+01 8.508900e-02 1.874100e-02 3.255600e-02
+6.325000e+02 5.250000e+01 5.250000e+01 2.763300e-02 3.482600e-03 1.520300e-02
+8.425000e+02 1.575000e+02 1.575000e+02 4.549000e-03 1.121400e-03 4.244900e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d92-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d92-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 2.004000e+03 2.669950e+02 2.532186e+02
+1.000000e-01 5.000000e-02 5.000000e-02 2.112200e+03 2.638339e+02 2.532517e+02
+2.000000e-01 5.000000e-02 5.000000e-02 2.018900e+03 2.589280e+02 2.464791e+02
+3.000000e-01 5.000000e-02 5.000000e-02 2.029900e+03 2.615069e+02 2.640057e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.732300e+03 2.633165e+02 2.499944e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.337000e+03 2.024652e+02 1.992508e+02
+6.000000e-01 5.000000e-02 5.000000e-02 1.216100e+03 1.879114e+02 1.863348e+02
+7.000000e-01 5.000000e-02 5.000000e-02 9.821400e+02 1.492019e+02 1.446003e+02
+8.000000e-01 5.000000e-02 5.000000e-02 6.549300e+02 9.720235e+01 9.906715e+01
+9.250000e-01 7.500000e-02 7.500000e-02 4.014700e+02 6.243126e+01 6.498550e+01
+1.100000e+00 1.000000e-01 1.000000e-01 2.652300e+02 5.174281e+01 5.190148e+01
+1.350000e+00 1.500000e-01 1.500000e-01 1.115600e+02 2.057846e+01 2.120185e+01
+1.650000e+00 1.500000e-01 1.500000e-01 3.094300e+01 7.743732e+00 7.619970e+00
+2.050000e+00 2.500000e-01 2.500000e-01 6.776000e+00 2.000931e+00 1.900796e+00
+2.650000e+00 3.500000e-01 3.500000e-01 6.510400e-01 3.417055e-01 3.102679e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d92-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d92-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.567400e+03 2.039300e+02 1.984600e+02
+1.000000e-01 5.000000e-02 5.000000e-02 1.577700e+03 2.285200e+02 1.834500e+02
+2.000000e-01 5.000000e-02 5.000000e-02 1.606300e+03 2.160100e+02 2.042200e+02
+3.000000e-01 5.000000e-02 5.000000e-02 1.659400e+03 2.168000e+02 2.131000e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.451000e+03 1.935200e+02 1.638500e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.115300e+03 1.495400e+02 1.217100e+02
+6.000000e-01 5.000000e-02 5.000000e-02 9.767500e+02 1.380700e+02 1.037600e+02
+7.000000e-01 5.000000e-02 5.000000e-02 7.754900e+02 1.041100e+02 9.247600e+01
+8.000000e-01 5.000000e-02 5.000000e-02 5.248100e+02 6.686700e+01 1.333900e+02
+9.250000e-01 7.500000e-02 7.500000e-02 3.386100e+02 4.272100e+01 3.808000e+01
+1.100000e+00 1.000000e-01 1.000000e-01 1.891000e+02 2.639800e+01 1.704100e+01
+1.350000e+00 1.500000e-01 1.500000e-01 7.950200e+01 1.129200e+01 8.854900e+00
+1.650000e+00 1.500000e-01 1.500000e-01 2.520400e+01 3.801300e+00 2.876400e+00
+2.050000e+00 2.500000e-01 2.500000e-01 4.911000e+00 7.866200e-01 7.678600e-01
+2.650000e+00 3.500000e-01 3.500000e-01 2.383100e-01 7.195200e-02 7.958000e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d92-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d92-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.415600e+03 4.393400e+02 7.146200e+02
+1.000000e-01 5.000000e-02 5.000000e-02 1.422500e+03 4.407900e+02 7.171400e+02
+2.000000e-01 5.000000e-02 5.000000e-02 1.396600e+03 4.335900e+02 7.068400e+02
+3.000000e-01 5.000000e-02 5.000000e-02 1.427500e+03 4.438600e+02 7.240300e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.282900e+03 4.035400e+02 6.628100e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.128500e+03 3.659100e+02 6.104800e+02
+6.000000e-01 5.000000e-02 5.000000e-02 1.089800e+03 3.574300e+02 5.994600e+02
+7.000000e-01 5.000000e-02 5.000000e-02 8.591800e+02 2.823500e+02 4.738800e+02
+8.000000e-01 5.000000e-02 5.000000e-02 5.732900e+02 1.889500e+02 3.177500e+02
+9.250000e-01 7.500000e-02 7.500000e-02 3.983700e+02 1.341700e+02 2.278800e+02
+1.100000e+00 1.000000e-01 1.000000e-01 2.157300e+02 7.223900e+01 1.223700e+02
+1.350000e+00 1.500000e-01 1.500000e-01 9.648200e+01 3.232400e+01 5.436700e+01
+1.650000e+00 1.500000e-01 1.500000e-01 3.548600e+01 1.216800e+01 2.033000e+01
+2.050000e+00 2.500000e-01 2.500000e-01 5.952500e+00 2.100900e+00 3.647700e+00
+2.650000e+00 3.500000e-01 3.500000e-01 2.716300e-01 9.814000e-02 1.736900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d92-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d92-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.855800e+03 4.407700e+02 8.686100e+02
+1.000000e-01 5.000000e-02 5.000000e-02 1.858100e+03 4.098600e+02 8.931200e+02
+2.000000e-01 5.000000e-02 5.000000e-02 1.868800e+03 3.979300e+02 8.663800e+02
+3.000000e-01 5.000000e-02 5.000000e-02 1.908000e+03 4.346400e+02 9.787100e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.621100e+03 3.630100e+02 7.886400e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.193600e+03 2.611300e+02 5.891200e+02
+6.000000e-01 5.000000e-02 5.000000e-02 1.053000e+03 2.471300e+02 5.153900e+02
+7.000000e-01 5.000000e-02 5.000000e-02 8.637500e+02 1.992600e+02 3.999800e+02
+8.000000e-01 5.000000e-02 5.000000e-02 5.636500e+02 1.177500e+02 2.916200e+02
+9.250000e-01 7.500000e-02 7.500000e-02 3.738600e+02 8.372500e+01 1.720400e+02
+1.100000e+00 1.000000e-01 1.000000e-01 2.090100e+02 5.066300e+01 9.360700e+01
+1.350000e+00 1.500000e-01 1.500000e-01 8.991900e+01 1.970700e+01 4.232200e+01
+1.650000e+00 1.500000e-01 1.500000e-01 2.839400e+01 6.484700e+00 1.468300e+01
+2.050000e+00 2.500000e-01 2.500000e-01 5.998800e+00 1.140700e+00 2.396100e+00
+2.650000e+00 3.500000e-01 3.500000e-01 2.502100e-01 1.134800e-01 2.568700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d93-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d93-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.854500e+03 1.392862e+02 1.424013e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.729500e+03 1.256021e+02 1.309524e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.974600e+03 1.342602e+02 1.416856e+02
+1.750000e-01 2.500000e-02 2.500000e-02 2.076100e+03 1.712336e+02 1.392548e+02
+2.250000e-01 2.500000e-02 2.500000e-02 2.149300e+03 1.787284e+02 1.643144e+02
+2.750000e-01 2.500000e-02 2.500000e-02 2.256600e+03 1.661413e+02 1.631526e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.305200e+03 1.714270e+02 1.676101e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.442700e+03 1.706935e+02 1.573677e+02
+4.250000e-01 2.500000e-02 2.500000e-02 2.232300e+03 1.646229e+02 1.437125e+02
+4.750000e-01 2.500000e-02 2.500000e-02 2.009800e+03 1.755803e+02 1.795133e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.971700e+03 1.359661e+02 1.429800e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.947500e+03 1.238870e+02 1.337143e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.715400e+03 1.167966e+02 1.102475e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.491100e+03 9.812216e+01 9.746407e+01
+7.250000e-01 2.500000e-02 2.500000e-02 1.242800e+03 7.367909e+01 8.344958e+01
+7.750000e-01 2.500000e-02 2.500000e-02 9.860700e+02 7.374213e+01 6.988655e+01
+8.250000e-01 2.500000e-02 2.500000e-02 7.999100e+02 5.148815e+01 5.561172e+01
+8.750000e-01 2.500000e-02 2.500000e-02 6.398900e+02 3.807850e+01 4.632887e+01
+9.250000e-01 2.500000e-02 2.500000e-02 5.029500e+02 3.365246e+01 3.713072e+01
+9.750000e-01 2.500000e-02 2.500000e-02 4.017500e+02 2.904657e+01 2.896229e+01
+1.025000e+00 2.500000e-02 2.500000e-02 3.191600e+02 2.211350e+01 2.131723e+01
+1.075000e+00 2.500000e-02 2.500000e-02 2.288100e+02 1.785009e+01 1.773006e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.711300e+02 1.426725e+01 1.471588e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.507500e+02 1.353921e+01 1.257293e+01
+1.250000e+00 5.000000e-02 5.000000e-02 8.632100e+01 7.585372e+00 7.867592e+00
+1.350000e+00 5.000000e-02 5.000000e-02 5.007300e+01 5.882454e+00 5.621114e+00
+1.500000e+00 1.000000e-01 1.000000e-01 1.821000e+01 2.317406e+00 2.084775e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.168300e+00 5.117025e-01 5.212289e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d93-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d93-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.508200e+03 1.584600e+02 1.483800e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.531200e+03 1.624900e+02 1.401100e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.592200e+03 1.575500e+02 1.578200e+02
+1.750000e-01 2.500000e-02 2.500000e-02 1.680400e+03 1.817200e+02 1.455900e+02
+2.250000e-01 2.500000e-02 2.500000e-02 1.802000e+03 2.159100e+02 1.758000e+02
+2.750000e-01 2.500000e-02 2.500000e-02 1.880300e+03 2.296900e+02 1.994500e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.011100e+03 2.735800e+02 1.490700e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.030500e+03 2.511100e+02 2.315600e+02
+4.250000e-01 2.500000e-02 2.500000e-02 1.942200e+03 2.450300e+02 1.887100e+02
+4.750000e-01 2.500000e-02 2.500000e-02 1.793500e+03 2.210800e+02 2.065000e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.694300e+03 2.224300e+02 1.795100e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.559500e+03 2.420200e+02 1.761500e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.435800e+03 1.818300e+02 3.443900e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.236900e+03 1.634400e+02 1.504100e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.026400e+03 1.334100e+02 1.162000e+02
+7.750000e-01 2.500000e-02 2.500000e-02 8.407000e+02 1.224400e+02 1.200900e+02
+8.250000e-01 2.500000e-02 2.500000e-02 6.708800e+02 9.013300e+01 8.450900e+01
+8.750000e-01 2.500000e-02 2.500000e-02 5.343000e+02 8.322600e+01 5.769500e+01
+9.250000e-01 2.500000e-02 2.500000e-02 4.131000e+02 6.351800e+01 5.190300e+01
+9.750000e-01 2.500000e-02 2.500000e-02 3.232700e+02 4.456300e+01 3.899100e+01
+1.025000e+00 2.500000e-02 2.500000e-02 2.480300e+02 3.750200e+01 2.868300e+01
+1.075000e+00 2.500000e-02 2.500000e-02 1.878100e+02 2.796400e+01 2.714800e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.422900e+02 1.981100e+01 2.038300e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.046500e+02 1.639800e+01 1.343100e+01
+1.250000e+00 5.000000e-02 5.000000e-02 7.013100e+01 1.038700e+01 9.331100e+00
+1.350000e+00 5.000000e-02 5.000000e-02 3.817100e+01 6.390100e+00 6.026600e+00
+1.500000e+00 1.000000e-01 1.000000e-01 1.528800e+01 2.495700e+00 2.875200e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.319600e+00 4.327500e-01 5.803400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d93-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d93-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.788800e+03 4.681900e+02 7.238800e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.798500e+03 4.677900e+02 7.199600e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.840000e+03 4.768300e+02 7.337500e+02
+1.750000e-01 2.500000e-02 2.500000e-02 1.909400e+03 4.917200e+02 7.537700e+02
+2.250000e-01 2.500000e-02 2.500000e-02 1.971700e+03 5.035000e+02 7.702000e+02
+2.750000e-01 2.500000e-02 2.500000e-02 2.027600e+03 5.157100e+02 7.892800e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.079500e+03 5.252400e+02 8.001700e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.055100e+03 5.182200e+02 7.898700e+02
+4.250000e-01 2.500000e-02 2.500000e-02 1.991800e+03 5.054600e+02 7.726500e+02
+4.750000e-01 2.500000e-02 2.500000e-02 1.830700e+03 4.626700e+02 7.038300e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.718500e+03 4.411100e+02 6.780600e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.550600e+03 3.924800e+02 5.988700e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.404800e+03 3.572300e+02 5.442400e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.200800e+03 3.045100e+02 4.634400e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.006200e+03 2.554100e+02 3.888200e+02
+7.750000e-01 2.500000e-02 2.500000e-02 8.333700e+02 2.132100e+02 3.256600e+02
+8.250000e-01 2.500000e-02 2.500000e-02 6.624400e+02 1.707800e+02 2.614200e+02
+8.750000e-01 2.500000e-02 2.500000e-02 5.341500e+02 1.387700e+02 2.131900e+02
+9.250000e-01 2.500000e-02 2.500000e-02 4.061800e+02 1.059300e+02 1.627200e+02
+9.750000e-01 2.500000e-02 2.500000e-02 3.218500e+02 8.378900e+01 1.285100e+02
+1.025000e+00 2.500000e-02 2.500000e-02 2.528100e+02 6.580500e+01 1.010100e+02
+1.075000e+00 2.500000e-02 2.500000e-02 1.970200e+02 5.147500e+01 7.893100e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.443200e+02 3.835200e+01 5.912800e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.095400e+02 2.923700e+01 4.525200e+01
+1.250000e+00 5.000000e-02 5.000000e-02 7.723600e+01 2.197000e+01 3.454800e+01
+1.350000e+00 5.000000e-02 5.000000e-02 3.828300e+01 1.039300e+01 1.623600e+01
+1.500000e+00 1.000000e-01 1.000000e-01 1.613800e+01 4.441800e+00 6.957200e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.361900e+00 7.088000e-01 1.171300e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d93-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d93-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.544100e+03 2.433100e+02 5.838400e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.597200e+03 2.847700e+02 5.953500e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.665800e+03 2.686200e+02 6.318100e+02
+1.750000e-01 2.500000e-02 2.500000e-02 1.780800e+03 3.161100e+02 6.276500e+02
+2.250000e-01 2.500000e-02 2.500000e-02 1.905000e+03 3.644000e+02 7.595300e+02
+2.750000e-01 2.500000e-02 2.500000e-02 2.031500e+03 3.760100e+02 8.038700e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.108900e+03 3.883000e+02 8.859400e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.175300e+03 4.343800e+02 8.931900e+02
+4.250000e-01 2.500000e-02 2.500000e-02 2.099400e+03 4.185100e+02 8.907700e+02
+4.750000e-01 2.500000e-02 2.500000e-02 1.997300e+03 4.251100e+02 8.510400e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.847200e+03 3.461700e+02 8.248800e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.738800e+03 3.575200e+02 7.373800e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.571300e+03 3.383700e+02 7.226100e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.368100e+03 2.936400e+02 5.562500e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.139600e+03 2.698000e+02 4.358800e+02
+7.750000e-01 2.500000e-02 2.500000e-02 9.078300e+02 1.346000e+02 4.310700e+02
+8.250000e-01 2.500000e-02 2.500000e-02 7.482600e+02 1.676100e+02 3.235800e+02
+8.750000e-01 2.500000e-02 2.500000e-02 5.713600e+02 1.011600e+02 3.026700e+02
+9.250000e-01 2.500000e-02 2.500000e-02 4.575800e+02 9.798500e+01 2.140200e+02
+9.750000e-01 2.500000e-02 2.500000e-02 3.557200e+02 6.552400e+01 1.719200e+02
+1.025000e+00 2.500000e-02 2.500000e-02 2.746400e+02 6.075400e+01 1.240900e+02
+1.075000e+00 2.500000e-02 2.500000e-02 2.044100e+02 4.900500e+01 9.549500e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.605700e+02 3.927200e+01 6.517000e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.158700e+02 2.070900e+01 6.710000e+01
+1.250000e+00 5.000000e-02 5.000000e-02 7.638900e+01 1.726900e+01 3.369100e+01
+1.350000e+00 5.000000e-02 5.000000e-02 3.885300e+01 8.890800e+00 2.040400e+01
+1.500000e+00 1.000000e-01 1.000000e-01 1.660100e+01 3.015200e+00 9.609400e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.688100e+00 5.346700e-01 1.147400e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d94-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d94-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.012600e+03 5.337420e+01 5.472897e+01
+1.000000e+00 5.000000e-01 5.000000e-01 4.836400e+02 4.265705e+01 4.042195e+01
+2.000000e+00 5.000000e-01 5.000000e-01 1.522800e+02 1.960786e+01 1.954737e+01
+3.000000e+00 5.000000e-01 5.000000e-01 3.855700e+01 7.497954e+00 6.466930e+00
+4.000000e+00 5.000000e-01 5.000000e-01 7.925500e+00 2.062354e+00 1.694143e+00
+6.500000e+00 2.000000e+00 2.000000e+00 2.858000e+00 9.319546e-01 8.598858e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d94-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d94-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.509500e+02 1.008000e+02 8.228700e+01
+1.000000e+00 5.000000e-01 5.000000e-01 4.064600e+02 5.521900e+01 4.595000e+01
+2.000000e+00 5.000000e-01 5.000000e-01 1.250100e+02 1.633900e+01 1.555100e+01
+3.000000e+00 5.000000e-01 5.000000e-01 3.235100e+01 4.899000e+00 3.842200e+00
+4.000000e+00 5.000000e-01 5.000000e-01 7.495600e+00 9.653900e-01 1.432100e+00
+6.500000e+00 2.000000e+00 2.000000e+00 2.046900e+00 3.251200e-01 4.462700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d94-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d94-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.408100e+02 2.110000e+02 3.068000e+02
+1.000000e+00 5.000000e-01 5.000000e-01 4.470200e+02 1.320300e+02 2.105300e+02
+2.000000e+00 5.000000e-01 5.000000e-01 1.011600e+02 3.435000e+01 5.802700e+01
+3.000000e+00 5.000000e-01 5.000000e-01 6.145900e-01 0.000000e+00 0.000000e+00
+4.000000e+00 5.000000e-01 5.000000e-01 2.000000e-99 0.000000e+00 0.000000e+00
+6.500000e+00 2.000000e+00 2.000000e+00 2.000000e-99 0.000000e+00 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d94-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d94-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.911000e+02 1.509400e+02 3.318100e+02
+1.000000e+00 5.000000e-01 5.000000e-01 4.570200e+02 1.046700e+02 2.100800e+02
+2.000000e+00 5.000000e-01 5.000000e-01 1.435400e+02 3.286200e+01 7.379000e+01
+3.000000e+00 5.000000e-01 5.000000e-01 3.508500e+01 7.124300e+00 1.769100e+01
+4.000000e+00 5.000000e-01 5.000000e-01 6.307400e+00 9.342100e-01 3.861500e+00
+6.500000e+00 2.000000e+00 2.000000e+00 1.238500e+00 2.545000e-01 3.283900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d95-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d95-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t95
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 5.874900e-02 1.324906e-02 1.240497e-02
+7.500000e+01 2.500000e+01 2.500000e+01 9.498400e-02 1.592544e-02 1.470177e-02
+1.300000e+02 3.000000e+01 3.000000e+01 4.586100e-02 8.749442e-03 7.678501e-03
+2.300000e+02 7.000000e+01 7.000000e+01 1.632200e-02 3.132506e-03 3.457378e-03
+5.150000e+02 2.150000e+02 2.150000e+02 1.006100e-03 5.756198e-04 5.664343e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d95-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d95-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t95
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 6.033900e-02 5.201800e-03 5.724300e-03
+7.500000e+01 2.500000e+01 2.500000e+01 7.762200e-02 1.063500e-02 7.972400e-03
+1.300000e+02 3.000000e+01 3.000000e+01 5.217900e-02 6.130000e-03 5.684300e-03
+2.300000e+02 7.000000e+01 7.000000e+01 2.047900e-02 2.249500e-03 2.401700e-03
+5.150000e+02 2.150000e+02 2.150000e+02 2.106100e-03 3.194200e-04 3.445200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d95-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d95-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t95
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 8.308500e-02 1.079000e-02 2.195600e-02
+7.500000e+01 2.500000e+01 2.500000e+01 1.041400e-01 1.671300e-02 4.075200e-02
+1.300000e+02 3.000000e+01 3.000000e+01 6.528800e-02 1.279000e-02 1.865800e-02
+2.300000e+02 7.000000e+01 7.000000e+01 2.661100e-02 5.735800e-03 1.306200e-02
+5.150000e+02 2.150000e+02 2.150000e+02 2.825200e-03 6.625600e-04 8.601000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d96-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d96-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.427500e+00 8.575259e-01 8.622934e-01
+8.000000e-01 1.000000e-01 1.000000e-01 2.164200e+01 3.867042e+00 3.248226e+00
+9.500000e-01 5.000000e-02 5.000000e-02 7.270800e+01 1.019935e+01 9.433521e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d96-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d96-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 3.398700e+00 3.200700e-01 6.315900e-01
+8.000000e-01 1.000000e-01 1.000000e-01 2.394200e+01 3.318200e+00 2.258000e+00
+9.500000e-01 5.000000e-02 5.000000e-02 6.659700e+01 6.209700e+00 4.462200e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d96-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d96-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.158000e+00 9.062200e-01 1.287400e+00
+8.000000e-01 1.000000e-01 1.000000e-01 2.984100e+01 4.913000e+00 8.748200e+00
+9.500000e-01 5.000000e-02 5.000000e-02 9.393500e+01 1.526800e+01 3.573200e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d97-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d97-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.042000e+00 2.180337e-01 2.166378e-01
+4.400000e+00 8.000000e-01 8.000000e-01 2.593900e+00 3.371296e-01 3.088335e-01
+5.600000e+00 4.000000e-01 4.000000e-01 4.529700e+00 7.709864e-01 7.392904e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.330800e+00 3.734668e-01 3.154054e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d97-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d97-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.122000e+00 1.535800e-01 1.096500e-01
+4.400000e+00 8.000000e-01 8.000000e-01 2.807700e+00 2.830900e-01 2.426100e-01
+5.600000e+00 4.000000e-01 4.000000e-01 4.789300e+00 6.183900e-01 3.969900e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.352500e+00 1.326300e-01 1.845300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d97-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d97-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.887200e+00 3.199800e-01 1.275400e+00
+4.400000e+00 8.000000e-01 8.000000e-01 3.841200e+00 7.167900e-01 1.204300e+00
+5.600000e+00 4.000000e-01 4.000000e-01 5.183100e+00 9.569800e-01 2.108700e+00
+7.400000e+00 1.400000e+00 1.400000e+00 1.829800e+00 3.144700e-01 3.756300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d98-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d98-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 6.456000e-02 1.790904e-02 1.516966e-02
+1.800000e+02 4.000000e+01 4.000000e+01 4.737800e-02 7.729065e-03 7.460089e-03
+2.675000e+02 4.750000e+01 4.750000e+01 2.025100e-02 3.525959e-03 3.127624e-03
+3.750000e+02 6.000000e+01 6.000000e+01 1.352600e-02 2.489235e-03 2.377726e-03
+5.600000e+02 1.250000e+02 1.250000e+02 6.354100e-03 1.136201e-03 1.153537e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d98-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d98-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 6.004900e-02 6.597700e-03 7.504900e-03
+1.800000e+02 4.000000e+01 4.000000e+01 5.099200e-02 5.523500e-03 4.591400e-03
+2.675000e+02 4.750000e+01 4.750000e+01 2.833200e-02 3.254000e-03 2.663400e-03
+3.750000e+02 6.000000e+01 6.000000e+01 1.361500e-02 1.800900e-03 1.393600e-03
+5.600000e+02 1.250000e+02 1.250000e+02 5.648100e-03 7.691400e-04 7.387400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d98-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d98-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 7.937500e-02 1.064600e-02 2.201400e-02
+1.800000e+02 4.000000e+01 4.000000e+01 5.798500e-02 1.209400e-02 2.093000e-02
+2.675000e+02 4.750000e+01 4.750000e+01 3.645300e-02 7.944700e-03 8.914500e-03
+3.750000e+02 6.000000e+01 6.000000e+01 1.986100e-02 2.817600e-03 8.124700e-03
+5.600000e+02 1.250000e+02 1.250000e+02 9.358400e-03 1.777400e-03 4.263000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d99-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d99-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.587300e+01 5.107230e+00 4.670509e+00
+7.000000e-01 3.000000e-01 3.000000e-01 4.407800e+00 8.937790e-01 8.322673e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d99-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d99-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.650400e+01 2.185400e+00 2.651000e+00
+7.000000e-01 3.000000e-01 3.000000e-01 4.289500e+00 5.409600e-01 6.522500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d99-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d99-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.630900e+01 4.804900e+00 1.328900e+01
+7.000000e-01 3.000000e-01 3.000000e-01 7.093300e+00 1.625500e+00 3.412100e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d100-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d100-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.443200e+01 3.358132e+00 3.450598e+00
+5.250000e-01 1.250000e-01 1.250000e-01 1.136400e+01 3.206306e+00 2.324743e+00
+8.250000e-01 1.750000e-01 1.750000e-01 1.501800e+00 5.158532e-01 5.032079e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d100-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d100-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.707000e+01 2.413500e+00 2.268100e+00
+5.250000e-01 1.250000e-01 1.250000e-01 1.016400e+01 1.639400e+00 1.010900e+00
+8.250000e-01 1.750000e-01 1.750000e-01 1.220900e+00 2.434400e-01 2.627700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d100-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d100-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 3.254600e+01 5.455900e+00 9.249700e+00
+5.250000e-01 1.250000e-01 1.250000e-01 1.723100e+01 2.937000e+00 8.779800e+00
+8.250000e-01 1.750000e-01 1.750000e-01 2.507400e+00 8.521500e-01 7.612800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d101-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d101-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.252300e+00 1.003388e+00 9.687704e-01
+1.000000e+00 5.000000e-01 5.000000e-01 3.073300e+00 6.788961e-01 5.561707e-01
+3.000000e+00 1.500000e+00 1.500000e+00 1.858100e+00 5.350092e-01 5.029681e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d101-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d101-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.735300e+00 7.026900e-01 5.658500e-01
+1.000000e+00 5.000000e-01 5.000000e-01 3.192500e+00 5.716400e-01 2.904800e-01
+3.000000e+00 1.500000e+00 1.500000e+00 1.849300e+00 2.181300e-01 4.216700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d101-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d101-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.037200e+01 1.659300e+00 2.412800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 4.758700e+00 8.353000e-01 2.176900e+00
+3.000000e+00 1.500000e+00 1.500000e+00 3.096500e+00 6.270700e-01 1.623600e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d102-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d102-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.078600e+00 1.375043e-01 1.335721e-01
+5.800000e+02 3.500000e+01 3.500000e+01 8.830000e-01 8.820350e-02 8.160317e-02
+6.550000e+02 4.000000e+01 4.000000e+01 6.802500e-01 6.941339e-02 6.417338e-02
+7.400000e+02 4.500000e+01 4.500000e+01 4.809000e-01 4.593229e-02 4.950006e-02
+8.325000e+02 4.750000e+01 4.750000e+01 3.027500e-01 3.592337e-02 3.305425e-02
+9.325000e+02 5.250000e+01 5.250000e+01 2.094700e-01 1.978769e-02 1.908621e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.608800e-01 1.379026e-02 1.439896e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.078200e-01 1.139356e-02 8.991321e-03
+1.275000e+03 7.500000e+01 7.500000e+01 6.716700e-02 8.280411e-03 9.436231e-03
+1.425000e+03 7.500000e+01 7.500000e+01 3.576800e-02 4.113652e-03 5.353288e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.268900e-02 1.810116e-03 1.969695e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.874500e-03 5.472270e-04 3.790943e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.281500e-04 5.981958e-05 5.863538e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d102-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d102-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 8.926900e-01 1.097600e-01 1.143400e-01
+5.800000e+02 3.500000e+01 3.500000e+01 7.337500e-01 1.014800e-01 8.296000e-02
+6.550000e+02 4.000000e+01 4.000000e+01 5.519100e-01 7.098800e-02 8.231900e-02
+7.400000e+02 4.500000e+01 4.500000e+01 4.024800e-01 5.963000e-02 4.281100e-02
+8.325000e+02 4.750000e+01 4.750000e+01 2.878200e-01 3.697700e-02 3.155200e-02
+9.325000e+02 5.250000e+01 5.250000e+01 1.928500e-01 2.772000e-02 2.245800e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.325200e-01 1.797200e-02 2.089800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.010400e-02 1.147200e-02 1.275000e-02
+1.275000e+03 7.500000e+01 7.500000e+01 5.754100e-02 9.250100e-03 6.763600e-03
+1.425000e+03 7.500000e+01 7.500000e+01 3.471200e-02 6.809400e-03 3.559500e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.282500e-02 2.094600e-03 1.681900e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.964300e-03 3.959000e-04 2.603600e-04
+3.350000e+03 6.500000e+02 6.500000e+02 8.538600e-05 2.888600e-05 3.188200e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d102-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d102-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 7.912600e-01 2.356300e-01 3.752800e-01
+5.800000e+02 3.500000e+01 3.500000e+01 6.453100e-01 1.925600e-01 3.074500e-01
+6.550000e+02 4.000000e+01 4.000000e+01 4.842500e-01 1.452600e-01 2.328600e-01
+7.400000e+02 4.500000e+01 4.500000e+01 3.578500e-01 1.081600e-01 1.736300e-01
+8.325000e+02 4.750000e+01 4.750000e+01 2.587800e-01 7.820000e-02 1.255000e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.784000e-01 5.458300e-02 8.843000e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.154500e-01 3.554900e-02 5.776300e-02
+1.150000e+03 5.000000e+01 5.000000e+01 8.036800e-02 2.520400e-02 4.130300e-02
+1.275000e+03 7.500000e+01 7.500000e+01 5.470900e-02 1.709300e-02 2.804100e-02
+1.425000e+03 7.500000e+01 7.500000e+01 3.236000e-02 1.008500e-02 1.650700e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.160000e-02 3.701900e-03 6.109700e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.766300e-03 5.795500e-04 9.795000e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.101300e-04 3.561700e-05 5.885600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d102-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d102-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 9.442500e-01 2.217800e-01 4.539400e-01
+5.800000e+02 3.500000e+01 3.500000e+01 7.963900e-01 1.906200e-01 3.995700e-01
+6.550000e+02 4.000000e+01 4.000000e+01 6.077400e-01 1.409900e-01 3.183300e-01
+7.400000e+02 4.500000e+01 4.500000e+01 4.554500e-01 1.075800e-01 2.280200e-01
+8.325000e+02 4.750000e+01 4.750000e+01 3.439300e-01 8.882000e-02 1.511600e-01
+9.325000e+02 5.250000e+01 5.250000e+01 2.390100e-01 5.789500e-02 1.165400e-01
+1.042500e+03 5.750000e+01 5.750000e+01 1.645700e-01 3.763800e-02 7.879200e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.131400e-01 2.145700e-02 5.317100e-02
+1.275000e+03 7.500000e+01 7.500000e+01 7.820500e-02 1.773700e-02 3.477700e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.798500e-02 1.021600e-02 2.147800e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.914200e-02 3.778700e-03 1.006900e-02
+2.350000e+03 3.500000e+02 3.500000e+02 3.291400e-03 6.802200e-04 1.928200e-03
+3.350000e+03 6.500000e+02 6.500000e+02 2.228000e-04 4.651700e-05 7.725700e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d103-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d103-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.317100e+00 1.662208e-01 1.560145e-01
+6.250000e+01 1.250000e+01 1.250000e+01 2.377900e+00 2.383366e-01 2.360401e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.114900e+00 2.095572e-01 1.959945e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.526800e+00 1.335790e-01 1.361221e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.068200e+00 1.148175e-01 1.100250e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.622300e-01 5.386598e-02 5.118310e-02
+2.625000e+02 3.750000e+01 3.750000e+01 1.878500e-01 2.124380e-02 2.260063e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.102300e-02 3.707778e-03 3.772826e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d103-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d103-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.071500e+00 1.451000e-01 1.393100e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.905900e+00 2.717500e-01 2.225300e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.724400e+00 2.553500e-01 1.837400e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.339700e+00 1.915300e-01 1.716300e-01
+1.450000e+02 1.500000e+01 1.500000e+01 9.556800e-01 1.242400e-01 1.154100e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.041100e-01 6.082900e-02 7.070500e-02
+2.625000e+02 3.750000e+01 3.750000e+01 1.717100e-01 2.189300e-02 1.888900e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.539700e-02 1.907400e-03 2.367400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d103-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d103-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.025200e+00 3.016300e-01 4.789400e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.746600e+00 5.177800e-01 8.253500e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.552500e+00 4.687500e-01 7.514300e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.158900e+00 3.520200e-01 5.674900e-01
+1.450000e+02 1.500000e+01 1.500000e+01 8.005200e-01 2.489200e-01 4.060000e-01
+1.925000e+02 3.250000e+01 3.250000e+01 4.193600e-01 1.311100e-01 2.146000e-01
+2.625000e+02 3.750000e+01 3.750000e+01 1.452400e-01 4.550900e-02 7.417600e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.365700e-02 4.326000e-03 7.050100e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d103-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d103-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.344700e+00 3.459100e-01 6.262800e-01
+6.250000e+01 1.250000e+01 1.250000e+01 2.220100e+00 5.672400e-01 1.092600e+00
+8.750000e+01 1.250000e+01 1.250000e+01 1.986200e+00 3.963300e-01 1.002100e+00
+1.150000e+02 1.500000e+01 1.500000e+01 1.542700e+00 3.501400e-01 7.927800e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.062400e+00 2.263400e-01 5.405800e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.455000e-01 1.314700e-01 2.584200e-01
+2.625000e+02 3.750000e+01 3.750000e+01 1.862600e-01 3.796400e-02 9.110500e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.612200e-02 3.845700e-03 6.963700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d104-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d104-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 3.194600e+01 6.164026e+00 6.091542e+00
+4.500000e-01 1.500000e-01 1.500000e-01 6.906200e+01 1.111902e+01 1.017829e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.481600e+02 2.683081e+01 2.604132e+01
+7.500000e-01 5.000000e-02 5.000000e-02 4.602300e+02 3.992553e+01 4.030188e+01
+8.250000e-01 2.500000e-02 2.500000e-02 7.849300e+02 7.846769e+01 7.762066e+01
+8.750000e-01 2.500000e-02 2.500000e-02 9.958400e+02 9.472413e+01 9.582386e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.174000e+03 1.219903e+02 1.195064e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.279200e+03 1.442066e+02 1.373947e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d104-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d104-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 3.239300e+01 4.407000e+00 5.976200e+00
+4.500000e-01 1.500000e-01 1.500000e-01 8.260900e+01 9.607700e+00 1.179100e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.188800e+02 3.878000e+01 2.081300e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.970500e+02 5.861400e+01 5.088700e+01
+8.250000e-01 2.500000e-02 2.500000e-02 6.037600e+02 7.500900e+01 8.361700e+01
+8.750000e-01 2.500000e-02 2.500000e-02 7.792400e+02 1.042900e+02 9.046200e+01
+9.250000e-01 2.500000e-02 2.500000e-02 9.491400e+02 1.353100e+02 1.078500e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.055800e+03 1.328000e+02 1.232000e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d104-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d104-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 2.731600e+01 8.990000e+00 1.520300e+01
+4.500000e-01 1.500000e-01 1.500000e-01 6.230900e+01 2.007600e+01 3.337900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 1.658300e+02 5.206100e+01 8.514600e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.190700e+02 9.867400e+01 1.603500e+02
+8.250000e-01 2.500000e-02 2.500000e-02 5.245600e+02 1.583200e+02 2.538200e+02
+8.750000e-01 2.500000e-02 2.500000e-02 7.095700e+02 2.116700e+02 3.377500e+02
+9.250000e-01 2.500000e-02 2.500000e-02 9.207600e+02 2.723200e+02 4.330500e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.069500e+03 3.134300e+02 4.955400e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d104-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d104-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 2.823700e+01 5.189300e+00 1.595500e+01
+4.500000e-01 1.500000e-01 1.500000e-01 7.249300e+01 1.804100e+01 3.539900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.057000e+02 4.742000e+01 9.726900e+01
+7.500000e-01 5.000000e-02 5.000000e-02 4.332700e+02 9.266500e+01 2.147100e+02
+8.250000e-01 2.500000e-02 2.500000e-02 6.871700e+02 1.624200e+02 3.248100e+02
+8.750000e-01 2.500000e-02 2.500000e-02 9.404500e+02 2.333300e+02 4.317700e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.207400e+03 2.729700e+02 6.167700e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.421700e+03 3.464800e+02 7.012800e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d105-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d105-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.122000e+02 1.378747e+01 1.380599e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.315300e+02 1.435557e+01 1.417091e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.543200e+02 1.478781e+01 1.471536e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.444700e+02 1.466204e+01 1.458784e+01
+4.000000e+00 4.000000e-01 4.000000e-01 9.352000e+01 1.023297e+01 8.861253e+00
+4.800000e+00 4.000000e-01 4.000000e-01 2.163800e+01 3.713625e+00 3.160063e+00
+7.000000e+00 1.800000e+00 1.800000e+00 1.062500e+00 2.460275e-01 3.311533e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d105-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d105-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 8.968700e+01 1.057600e+01 1.083800e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.073600e+02 1.271300e+01 1.246500e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.206100e+02 1.716200e+01 1.310400e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.224300e+02 1.619400e+01 1.452800e+01
+4.000000e+00 4.000000e-01 4.000000e-01 8.254300e+01 1.173900e+01 1.258300e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.472600e+01 4.240800e+00 2.577700e+00
+7.000000e+00 1.800000e+00 1.800000e+00 1.010200e+00 2.236900e-01 1.725500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d105-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d105-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 9.278400e+01 2.746300e+01 4.342600e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.028200e+02 3.053500e+01 4.849000e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.096100e+02 3.273900e+01 5.223800e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.026800e+02 3.086600e+01 4.951700e+01
+4.000000e+00 4.000000e-01 4.000000e-01 6.834600e+01 2.109100e+01 3.436500e+01
+4.800000e+00 4.000000e-01 4.000000e-01 1.958400e+01 6.280600e+00 1.048600e+01
+7.000000e+00 1.800000e+00 1.800000e+00 8.589900e-01 2.893700e-01 4.949900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d105-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d105-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.159700e+02 2.875900e+01 5.190000e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.323700e+02 2.846600e+01 7.192100e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.396700e+02 3.409100e+01 6.664400e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.347400e+02 3.416600e+01 6.224300e+01
+4.000000e+00 4.000000e-01 4.000000e-01 9.042200e+01 1.947100e+01 4.696200e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.645300e+01 6.194500e+00 1.221300e+01
+7.000000e+00 1.800000e+00 1.800000e+00 1.209200e+00 2.682700e-01 5.639100e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d106-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d106-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.355200e+00 2.128349e-01 1.447406e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.765000e+00 2.276836e-01 2.227523e-01
+1.275000e+02 1.250000e+01 1.250000e+01 2.035400e+00 2.008478e-01 2.097645e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.991800e+00 1.870991e-01 1.673110e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.725900e+00 1.426544e-01 1.396621e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.369100e+00 1.107719e-01 1.099527e-01
+2.350000e+02 1.500000e+01 1.500000e+01 8.336300e-01 7.129823e-02 7.290835e-02
+2.650000e+02 1.500000e+01 1.500000e+01 5.613100e-01 5.021629e-02 5.395497e-02
+3.150000e+02 3.500000e+01 3.500000e+01 2.690200e-01 3.322067e-02 3.541971e-02
+4.150000e+02 6.500000e+01 6.500000e+01 6.887900e-02 1.398064e-02 1.388875e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.004300e-02 1.987628e-03 1.952282e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d106-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d106-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.308600e+00 1.926600e-01 1.876600e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.607900e+00 2.357600e-01 2.261800e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.717500e+00 2.507500e-01 2.160800e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.628200e+00 2.297500e-01 1.972400e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.423700e+00 1.929100e-01 1.677000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.068000e+00 1.444800e-01 1.143800e-01
+2.350000e+02 1.500000e+01 1.500000e+01 7.183400e-01 9.018700e-02 9.093100e-02
+2.650000e+02 1.500000e+01 1.500000e+01 4.689700e-01 6.093400e-02 4.755000e-02
+3.150000e+02 3.500000e+01 3.500000e+01 2.341500e-01 2.540800e-02 2.904400e-02
+4.150000e+02 6.500000e+01 6.500000e+01 6.382500e-02 7.698700e-03 9.501600e-03
+5.825000e+02 1.025000e+02 1.025000e+02 9.277700e-03 1.681800e-03 1.138000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d106-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d106-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.031500e+00 3.247300e-01 5.376400e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.285700e+00 3.935000e-01 6.393700e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.421100e+00 4.315900e-01 6.965200e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.428300e+00 4.300000e-01 6.900500e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.300400e+00 3.873100e-01 6.172100e-01
+2.050000e+02 1.500000e+01 1.500000e+01 9.809800e-01 2.952700e-01 4.743500e-01
+2.350000e+02 1.500000e+01 1.500000e+01 6.892200e-01 2.066300e-01 3.300400e-01
+2.650000e+02 1.500000e+01 1.500000e+01 4.874100e-01 1.468200e-01 2.336700e-01
+3.150000e+02 3.500000e+01 3.500000e+01 2.282500e-01 6.894600e-02 1.101900e-01
+4.150000e+02 6.500000e+01 6.500000e+01 6.858200e-02 2.065800e-02 3.296500e-02
+5.825000e+02 1.025000e+02 1.025000e+02 8.857500e-03 2.785100e-03 4.508500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d106-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d106-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.282000e+00 2.856700e-01 6.114500e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.691700e+00 4.555400e-01 8.108800e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.808800e+00 4.382900e-01 8.470800e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.790200e+00 4.345600e-01 9.083900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.650100e+00 3.842600e-01 8.355900e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.277600e+00 2.625100e-01 7.166600e-01
+2.350000e+02 1.500000e+01 1.500000e+01 9.316100e-01 1.882400e-01 4.509400e-01
+2.650000e+02 1.500000e+01 1.500000e+01 5.948100e-01 1.383300e-01 2.783100e-01
+3.150000e+02 3.500000e+01 3.500000e+01 3.283500e-01 8.045000e-02 1.330400e-01
+4.150000e+02 6.500000e+01 6.500000e+01 9.358300e-02 2.241700e-02 4.588500e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.479700e-02 3.010100e-03 6.567300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d107-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d107-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 9.110900e-01 1.588982e-01 1.548867e-01
+5.800000e+02 3.500000e+01 3.500000e+01 7.716400e-01 1.018759e-01 9.759468e-02
+6.550000e+02 4.000000e+01 4.000000e+01 5.921600e-01 7.745728e-02 8.440039e-02
+7.400000e+02 4.500000e+01 4.500000e+01 4.260100e-01 4.972377e-02 4.414964e-02
+8.325000e+02 4.750000e+01 4.750000e+01 3.207500e-01 3.728159e-02 3.134651e-02
+9.325000e+02 5.250000e+01 5.250000e+01 2.109000e-01 2.949601e-02 3.550327e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.450100e-01 1.674060e-02 2.071307e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.819000e-02 1.536497e-02 1.352539e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.642700e-02 1.940322e-02 1.038693e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.980900e-02 7.758158e-03 6.992196e-03
+1.750000e+03 2.500000e+02 2.500000e+02 2.265900e-02 3.901552e-03 4.085785e-03
+3.000000e+03 1.000000e+03 1.000000e+03 1.295800e-03 3.913357e-04 3.826879e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d107-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d107-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.749000e-01 6.962400e-02 7.161800e-02
+5.800000e+02 3.500000e+01 3.500000e+01 5.696800e-01 6.748400e-02 7.435200e-02
+6.550000e+02 4.000000e+01 4.000000e+01 4.559200e-01 6.081700e-02 4.467700e-02
+7.400000e+02 4.500000e+01 4.500000e+01 3.484500e-01 4.783200e-02 4.020400e-02
+8.325000e+02 4.750000e+01 4.750000e+01 2.588900e-01 4.026200e-02 3.184800e-02
+9.325000e+02 5.250000e+01 5.250000e+01 1.867500e-01 2.524300e-02 2.079800e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.329000e-01 1.810700e-02 1.948800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.485300e-02 1.387400e-02 1.198400e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.533400e-02 1.085500e-02 8.814600e-03
+1.425000e+03 7.500000e+01 7.500000e+01 4.172400e-02 5.692800e-03 5.957800e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.852500e-02 3.335100e-03 2.679400e-03
+3.000000e+03 1.000000e+03 1.000000e+03 1.532600e-03 2.376600e-04 2.115200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d107-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d107-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.933500e-01 2.056700e-01 3.275100e-01
+5.800000e+02 3.500000e+01 3.500000e+01 5.915400e-01 1.772200e-01 2.835800e-01
+6.550000e+02 4.000000e+01 4.000000e+01 4.668500e-01 1.406400e-01 2.255000e-01
+7.400000e+02 4.500000e+01 4.500000e+01 3.584700e-01 1.101100e-01 1.794000e-01
+8.325000e+02 4.750000e+01 4.750000e+01 2.709900e-01 8.322000e-02 1.345300e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.900500e-01 5.910400e-02 9.647700e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.331600e-01 4.170800e-02 6.846400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.995300e-02 3.139500e-02 5.163300e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.808800e-02 2.163600e-02 3.588400e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.331100e-02 1.395100e-02 2.331900e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.884200e-02 6.274900e-03 1.076900e-02
+3.000000e+03 1.000000e+03 1.000000e+03 1.560900e-03 5.455800e-04 9.647100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d107-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d107-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.985600e-01 1.620900e-01 3.070800e-01
+5.800000e+02 3.500000e+01 3.500000e+01 6.104800e-01 1.425200e-01 3.447700e-01
+6.550000e+02 4.000000e+01 4.000000e+01 4.834200e-01 1.095100e-01 2.226400e-01
+7.400000e+02 4.500000e+01 4.500000e+01 3.709300e-01 8.393800e-02 1.596900e-01
+8.325000e+02 4.750000e+01 4.750000e+01 2.861100e-01 6.263000e-02 1.323400e-01
+9.325000e+02 5.250000e+01 5.250000e+01 2.093300e-01 5.141200e-02 9.288200e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.469000e-01 2.522100e-02 7.490800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.101900e-01 1.950300e-02 4.855200e-02
+1.275000e+03 7.500000e+01 7.500000e+01 8.093100e-02 1.666400e-02 2.972600e-02
+1.425000e+03 7.500000e+01 7.500000e+01 5.113300e-02 9.438600e-03 2.281700e-02
+1.750000e+03 2.500000e+02 2.500000e+02 2.359700e-02 5.260200e-03 9.532100e-03
+3.000000e+03 1.000000e+03 1.000000e+03 2.190700e-03 3.414200e-04 1.014400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d108-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d108-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.322900e+00 2.052019e-01 2.008205e-01
+6.250000e+01 1.250000e+01 1.250000e+01 2.274700e+00 3.189118e-01 3.174077e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.881600e+00 2.311125e-01 2.476128e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.126500e+00 1.507024e-01 1.157130e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.430300e-01 3.666611e-02 3.595725e-02
+6.000000e+02 3.000000e+02 3.000000e+02 8.547800e-03 3.085704e-03 3.089450e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d108-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d108-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 9.556900e-01 1.426000e-01 1.002700e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.632900e+00 2.089400e-01 1.928300e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.452100e+00 1.867900e-01 1.838100e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.005100e+00 1.299600e-01 1.279200e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.108300e-01 3.934900e-02 3.405800e-02
+6.000000e+02 3.000000e+02 3.000000e+02 1.116400e-02 1.334800e-03 1.773700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d108-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d108-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.020800e+00 3.047500e-01 4.887200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.708300e+00 5.206200e-01 8.451500e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.481700e+00 4.521800e-01 7.315400e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.002800e+00 3.116200e-01 5.094200e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.148700e-01 9.850100e-02 1.610700e-01
+6.000000e+02 3.000000e+02 3.000000e+02 1.240100e-02 3.905500e-03 6.361600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d108-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d108-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.086100e+00 2.350100e-01 4.995300e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.846000e+00 4.406100e-01 7.994400e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.630600e+00 3.675200e-01 6.734600e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.076500e+00 2.144000e-01 5.511900e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.287400e-01 7.637500e-02 1.597300e-01
+6.000000e+02 3.000000e+02 3.000000e+02 1.247900e-02 2.462800e-03 5.497400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d109-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d109-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.427500e+01 1.496705e+01 9.122976e+00
+4.500000e-01 1.500000e-01 1.500000e-01 9.548000e+01 1.571207e+01 1.537634e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.600600e+02 2.651159e+01 2.948628e+01
+7.500000e-01 5.000000e-02 5.000000e-02 4.386300e+02 4.524406e+01 4.650106e+01
+8.500000e-01 5.000000e-02 5.000000e-02 7.594100e+02 9.625282e+01 9.274535e+01
+9.500000e-01 5.000000e-02 5.000000e-02 1.045600e+03 1.349422e+02 1.341298e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d109-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d109-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.609600e+01 6.268100e+00 4.698600e+00
+4.500000e-01 1.500000e-01 1.500000e-01 9.736800e+01 1.435600e+01 1.352900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.118900e+02 3.012500e+01 2.940000e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.577100e+02 4.684900e+01 3.778700e+01
+8.500000e-01 5.000000e-02 5.000000e-02 5.700600e+02 7.219900e+01 6.879200e+01
+9.500000e-01 5.000000e-02 5.000000e-02 7.844200e+02 1.002500e+02 8.880500e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d109-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d109-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.637100e+01 1.494500e+01 2.496500e+01
+4.500000e-01 1.500000e-01 1.500000e-01 9.160200e+01 2.926500e+01 4.862100e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.019100e+02 6.405400e+01 1.055700e+02
+7.500000e-01 5.000000e-02 5.000000e-02 3.559100e+02 1.112700e+02 1.826100e+02
+8.500000e-01 5.000000e-02 5.000000e-02 5.954700e+02 1.807200e+02 2.911900e+02
+9.500000e-01 5.000000e-02 5.000000e-02 8.576700e+02 2.551200e+02 4.074800e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d109-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d109-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.130600e+01 9.606300e+00 2.474900e+01
+4.500000e-01 1.500000e-01 1.500000e-01 8.626100e+01 1.905000e+01 4.357300e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.054500e+02 4.413400e+01 9.224000e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.810800e+02 7.425200e+01 1.830400e+02
+8.500000e-01 5.000000e-02 5.000000e-02 6.637100e+02 1.435700e+02 3.065000e+02
+9.500000e-01 5.000000e-02 5.000000e-02 9.604300e+02 2.219200e+02 4.183300e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d110-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d110-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.309600e+00 4.165370e-01 3.534697e-01
+1.275000e+02 1.250000e+01 1.250000e+01 2.097600e+00 2.465289e-01 2.532859e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.567900e+00 1.617279e-01 1.576783e-01
+2.200000e+02 3.000000e+01 3.000000e+01 7.374100e-01 6.806971e-02 6.868258e-02
+2.825000e+02 3.250000e+01 3.250000e+01 3.204600e-01 2.768212e-02 2.745194e-02
+3.525000e+02 3.750000e+01 3.750000e+01 1.097400e-01 1.318318e-02 1.399842e-02
+4.350000e+02 4.500000e+01 4.500000e+01 3.719100e-02 6.349371e-03 6.233725e-03
+5.825000e+02 1.025000e+02 1.025000e+02 8.869200e-03 2.721005e-03 2.612747e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.380300e-07 6.263013e-03 6.263008e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d110-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d110-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.788400e+00 3.026300e-01 1.971400e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.681200e+00 2.229900e-01 1.975800e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.250200e+00 1.363900e-01 1.673400e-01
+2.200000e+02 3.000000e+01 3.000000e+01 6.486800e-01 7.338500e-02 7.466100e-02
+2.825000e+02 3.250000e+01 3.250000e+01 2.656500e-01 3.279500e-02 3.134000e-02
+3.525000e+02 3.750000e+01 3.750000e+01 1.002500e-01 1.424200e-02 8.753200e-03
+4.350000e+02 4.500000e+01 4.500000e+01 3.307200e-02 4.235100e-03 5.561900e-03
+5.825000e+02 1.025000e+02 1.025000e+02 6.981200e-03 9.980600e-04 9.399700e-04
+8.425000e+02 1.575000e+02 1.575000e+02 5.993900e-04 1.825100e-04 1.561300e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d110-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d110-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.685600e+00 5.301900e-01 8.797400e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.672500e+00 5.137900e-01 8.347300e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.318500e+00 4.007900e-01 6.457800e-01
+2.200000e+02 3.000000e+01 3.000000e+01 7.110200e-01 2.143200e-01 3.436000e-01
+2.825000e+02 3.250000e+01 3.250000e+01 2.913200e-01 8.854600e-02 1.424500e-01
+3.525000e+02 3.750000e+01 3.750000e+01 1.122400e-01 3.456200e-02 5.565800e-02
+4.350000e+02 4.500000e+01 4.500000e+01 4.111900e-02 1.235000e-02 1.966000e-02
+5.825000e+02 1.025000e+02 1.025000e+02 9.051300e-03 2.747000e-03 4.374100e-03
+8.425000e+02 1.575000e+02 1.575000e+02 5.472200e-04 1.747300e-04 2.841000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d110-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d110-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.743200e+00 3.746100e-01 8.016600e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.693500e+00 4.213300e-01 7.914800e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.390000e+00 3.060800e-01 6.211300e-01
+2.200000e+02 3.000000e+01 3.000000e+01 7.808500e-01 1.474700e-01 4.022100e-01
+2.825000e+02 3.250000e+01 3.250000e+01 3.411600e-01 7.759400e-02 1.660200e-01
+3.525000e+02 3.750000e+01 3.750000e+01 1.373800e-01 3.107400e-02 5.632200e-02
+4.350000e+02 4.500000e+01 4.500000e+01 5.063200e-02 1.427800e-02 1.403200e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.128600e-02 2.130900e-03 5.189300e-03
+8.425000e+02 1.575000e+02 1.575000e+02 8.921200e-04 2.212200e-04 5.403600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d111-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d111-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.934400e+00 2.047777e-01 2.060855e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.554500e+00 1.147123e-01 1.160608e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.148600e+00 7.958526e-02 7.788120e-02
+7.400000e+02 4.500000e+01 4.500000e+01 7.872700e-01 5.305027e-02 5.174950e-02
+8.325000e+02 4.750000e+01 4.750000e+01 5.362300e-01 4.052583e-02 3.776656e-02
+9.325000e+02 5.250000e+01 5.250000e+01 3.784800e-01 2.161550e-02 2.500310e-02
+1.042500e+03 5.750000e+01 5.750000e+01 2.505000e-01 1.974661e-02 1.394663e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.739800e-01 1.214582e-02 8.120632e-03
+1.275000e+03 7.500000e+01 7.500000e+01 1.133300e-01 7.347170e-03 7.403166e-03
+1.425000e+03 7.500000e+01 7.500000e+01 7.190800e-02 7.881528e-03 1.177839e-02
+1.750000e+03 2.500000e+02 2.500000e+02 3.443000e-02 3.375883e-03 3.932118e-03
+2.350000e+03 3.500000e+02 3.500000e+02 7.209200e-03 1.282826e-03 1.334459e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.041900e-03 2.878364e-04 2.626336e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d111-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d111-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.642100e+00 2.224900e-01 1.048000e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.280700e+00 1.377300e-01 1.273100e-01
+6.550000e+02 4.000000e+01 4.000000e+01 9.243800e-01 9.858100e-02 8.465500e-02
+7.400000e+02 4.500000e+01 4.500000e+01 6.538000e-01 7.784700e-02 5.199500e-02
+8.325000e+02 4.750000e+01 4.750000e+01 4.503400e-01 4.545300e-02 4.479600e-02
+9.325000e+02 5.250000e+01 5.250000e+01 3.181700e-01 3.284500e-02 2.535500e-02
+1.042500e+03 5.750000e+01 5.750000e+01 2.185000e-01 2.233400e-02 1.953400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.579900e-01 1.483300e-02 2.066600e-02
+1.275000e+03 7.500000e+01 7.500000e+01 1.090300e-01 9.760300e-03 9.055100e-03
+1.425000e+03 7.500000e+01 7.500000e+01 7.073300e-02 7.780500e-03 3.461500e-03
+1.750000e+03 2.500000e+02 2.500000e+02 3.316800e-02 2.504200e-03 2.777300e-03
+2.350000e+03 3.500000e+02 3.500000e+02 8.734700e-03 6.407600e-04 6.425400e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.212400e-03 1.337400e-04 1.543400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d111-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d111-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.880700e+00 4.180500e-01 6.047600e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.478800e+00 3.320800e-01 4.824600e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.064500e+00 2.412500e-01 3.519000e-01
+7.400000e+02 4.500000e+01 4.500000e+01 7.629200e-01 1.761300e-01 2.584000e-01
+8.325000e+02 4.750000e+01 4.750000e+01 5.197000e-01 1.209900e-01 1.789600e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.649800e-01 8.578500e-02 1.272200e-01
+1.042500e+03 5.750000e+01 5.750000e+01 2.483800e-01 5.903100e-02 8.813500e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.733800e-01 4.181800e-02 6.280800e-02
+1.275000e+03 7.500000e+01 7.500000e+01 1.198100e-01 2.886900e-02 4.345000e-02
+1.425000e+03 7.500000e+01 7.500000e+01 7.811100e-02 1.921100e-02 2.916800e-02
+1.750000e+03 2.500000e+02 2.500000e+02 3.568000e-02 8.919700e-03 1.364200e-02
+2.350000e+03 3.500000e+02 3.500000e+02 9.058400e-03 2.335400e-03 3.635200e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.192200e-03 3.207500e-04 5.047000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d111-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d111-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.628100e+00 2.993500e-01 6.745500e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.279400e+00 2.076000e-01 4.473400e-01
+6.550000e+02 4.000000e+01 4.000000e+01 9.358600e-01 1.605300e-01 3.396800e-01
+7.400000e+02 4.500000e+01 4.500000e+01 6.718400e-01 1.099100e-01 2.416500e-01
+8.325000e+02 4.750000e+01 4.750000e+01 4.790800e-01 7.642600e-02 1.506700e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.409300e-01 4.338300e-02 1.233500e-01
+1.042500e+03 5.750000e+01 5.750000e+01 2.365700e-01 3.459200e-02 7.409400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.688300e-01 2.454700e-02 6.020900e-02
+1.275000e+03 7.500000e+01 7.500000e+01 1.199900e-01 1.771900e-02 4.314600e-02
+1.425000e+03 7.500000e+01 7.500000e+01 8.160500e-02 1.549200e-02 1.858400e-02
+1.750000e+03 2.500000e+02 2.500000e+02 3.742900e-02 5.936600e-03 1.075600e-02
+2.350000e+03 3.500000e+02 3.500000e+02 9.699000e-03 1.718800e-03 2.130700e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.324400e-03 2.172600e-04 3.806100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d112-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d112-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.579600e+00 2.711065e-01 2.643542e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.958800e+00 5.026961e-01 5.257734e-01
+6.250000e+01 1.250000e+01 1.250000e+01 4.334200e+00 3.792103e-01 3.718256e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.998200e+00 2.164359e-01 2.116842e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.979600e+00 1.334556e-01 1.287057e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.492000e+00 1.237087e-01 1.085712e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.918100e-01 5.857638e-02 6.881132e-02
+2.250000e+02 3.500000e+01 3.500000e+01 4.240200e-01 4.365110e-02 4.182401e-02
+3.250000e+02 6.500000e+01 6.500000e+01 9.793900e-02 1.567364e-02 1.537346e-02
+6.450000e+02 2.550000e+02 2.550000e+02 5.061200e-03 1.404259e-03 1.386970e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d112-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d112-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.804400e+00 2.658700e-01 6.646200e-02
+3.750000e+01 1.250000e+01 1.250000e+01 3.770700e+00 3.970400e-01 3.774700e-01
+6.250000e+01 1.250000e+01 1.250000e+01 3.474700e+00 3.558700e-01 3.319800e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.670600e+00 2.791500e-01 2.253000e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.902400e+00 1.977700e-01 1.693700e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.329700e+00 1.605800e-01 1.222500e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.809000e-01 8.616900e-02 8.474500e-02
+2.250000e+02 3.500000e+01 3.500000e+01 4.329000e-01 4.424100e-02 3.108600e-02
+3.250000e+02 6.500000e+01 6.500000e+01 1.126000e-01 1.057300e-02 1.004400e-02
+6.450000e+02 2.550000e+02 2.550000e+02 6.649600e-03 7.184800e-04 4.637200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d112-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d112-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.121400e+00 4.360100e-01 6.128600e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.193800e+00 9.078900e-01 1.303500e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.752500e+00 8.527900e-01 1.247000e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.964300e+00 6.888600e-01 1.015400e+00
+1.150000e+02 1.500000e+01 1.500000e+01 2.143700e+00 5.061400e-01 7.530900e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.526300e+00 3.652700e-01 5.453000e-01
+1.750000e+02 1.500000e+01 1.500000e+01 1.068700e+00 2.598600e-01 3.887800e-01
+2.250000e+02 3.500000e+01 3.500000e+01 5.398000e-01 1.320000e-01 1.977300e-01
+3.250000e+02 6.500000e+01 6.500000e+01 1.535300e-01 3.824600e-02 5.733000e-02
+6.450000e+02 2.550000e+02 2.550000e+02 1.039400e-02 2.702600e-03 4.093300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d112-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d112-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.856200e+00 1.978500e-01 6.439900e-01
+3.750000e+01 1.250000e+01 1.250000e+01 3.939000e+00 6.173000e-01 1.379000e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.624400e+00 5.748400e-01 1.373800e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.762400e+00 4.109300e-01 9.952400e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.951300e+00 3.472300e-01 6.723300e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.344600e+00 2.294300e-01 4.235100e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.966700e-01 1.489700e-01 3.301800e-01
+2.250000e+02 3.500000e+01 3.500000e+01 4.410700e-01 8.725500e-02 1.531300e-01
+3.250000e+02 6.500000e+01 6.500000e+01 1.184800e-01 2.013000e-02 3.517000e-02
+6.450000e+02 2.550000e+02 2.550000e+02 8.714200e-03 2.430900e-03 2.757300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d113-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d113-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 5.586400e+01 1.118706e+01 1.104381e+01
+3.500000e-01 5.000000e-02 5.000000e-02 7.833700e+01 1.351436e+01 1.384003e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.288400e+02 1.549411e+01 1.432772e+01
+5.500000e-01 5.000000e-02 5.000000e-02 2.049900e+02 1.895132e+01 2.163838e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.402900e+02 3.049171e+01 2.859075e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.767000e+02 4.588403e+01 4.887892e+01
+7.750000e-01 2.500000e-02 2.500000e-02 7.672700e+02 5.741062e+01 5.452588e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.143300e+03 8.074666e+01 7.674454e+01
+8.750000e-01 2.500000e-02 2.500000e-02 1.653700e+03 1.302137e+02 1.240733e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.228500e+03 1.588063e+02 1.556113e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.867300e+03 2.246193e+02 2.329989e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d113-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d113-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 6.373000e+01 7.492800e+00 7.065600e+00
+3.500000e-01 5.000000e-02 5.000000e-02 8.990700e+01 1.271000e+01 1.286600e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.226300e+02 1.766100e+01 1.461900e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.825600e+02 1.828600e+01 1.752200e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.127800e+02 3.363300e+01 2.949200e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.867400e+02 5.180100e+01 6.072000e+01
+7.750000e-01 2.500000e-02 2.500000e-02 6.810400e+02 7.480700e+01 5.491100e+01
+8.250000e-01 2.500000e-02 2.500000e-02 9.436000e+02 9.818500e+01 8.198000e+01
+8.750000e-01 2.500000e-02 2.500000e-02 1.323700e+03 1.334200e+02 9.886700e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.792900e+03 1.825600e+02 1.661600e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.268900e+03 2.638000e+02 1.420800e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d113-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d113-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 7.362100e+01 1.803800e+01 2.728200e+01
+3.500000e-01 5.000000e-02 5.000000e-02 1.007000e+02 2.448200e+01 3.672200e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.347300e+02 3.243200e+01 4.847100e+01
+5.500000e-01 5.000000e-02 5.000000e-02 2.064100e+02 5.044600e+01 7.559700e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.389400e+02 8.167600e+01 1.224700e+02
+7.250000e-01 2.500000e-02 2.500000e-02 5.284200e+02 1.264000e+02 1.881400e+02
+7.750000e-01 2.500000e-02 2.500000e-02 7.345100e+02 1.744500e+02 2.595400e+02
+8.250000e-01 2.500000e-02 2.500000e-02 1.043000e+03 2.465300e+02 3.651400e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.480000e+03 3.411800e+02 5.011000e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.107200e+03 4.715700e+02 6.848300e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.724500e+03 5.878600e+02 8.420200e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d113-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d113-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 6.158000e+01 1.220800e+01 2.139600e+01
+3.500000e-01 5.000000e-02 5.000000e-02 8.181400e+01 1.449300e+01 3.341900e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.147200e+02 2.020900e+01 3.300600e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.722700e+02 3.036500e+01 5.917900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.023600e+02 5.512700e+01 8.862700e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.652900e+02 7.566200e+01 1.763100e+02
+7.750000e-01 2.500000e-02 2.500000e-02 6.752300e+02 1.073700e+02 2.398400e+02
+8.250000e-01 2.500000e-02 2.500000e-02 9.776800e+02 1.698200e+02 3.293100e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.399600e+03 2.173500e+02 5.034200e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.938600e+03 3.075400e+02 6.884800e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.453700e+03 3.440500e+02 8.884500e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d114-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d114-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.269800e+02 8.348051e+00 8.261689e+00
+2.600000e+00 2.000000e-01 2.000000e-01 1.721100e+02 1.090471e+01 1.051043e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.081400e+02 1.294466e+01 1.299410e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.453600e+02 1.571388e+01 1.569201e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.530200e+02 1.746229e+01 1.794819e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.623600e+02 1.267874e+01 1.194071e+01
+4.600000e+00 2.000000e-01 2.000000e-01 9.276200e+01 7.698652e+00 7.934809e+00
+5.000000e+00 2.000000e-01 2.000000e-01 5.314900e+01 5.404704e+00 5.484141e+00
+5.800000e+00 6.000000e-01 6.000000e-01 1.617900e+01 1.942031e+00 2.003112e+00
+7.600000e+00 1.200000e+00 1.200000e+00 5.693000e-01 2.767259e-01 2.785675e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d114-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d114-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.076800e+02 1.043800e+01 8.709800e+00
+2.600000e+00 2.000000e-01 2.000000e-01 1.414800e+02 1.430800e+01 1.121600e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.825800e+02 2.318800e+01 8.498100e+00
+3.400000e+00 2.000000e-01 2.000000e-01 2.124500e+02 2.186700e+01 2.008200e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.062300e+02 2.360800e+01 1.781600e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.347600e+02 1.579900e+01 1.281300e+01
+4.600000e+00 2.000000e-01 2.000000e-01 8.099200e+01 8.587900e+00 1.024600e+01
+5.000000e+00 2.000000e-01 2.000000e-01 4.632300e+01 3.728200e+00 5.458600e+00
+5.800000e+00 6.000000e-01 6.000000e-01 1.523900e+01 1.658400e+00 1.293000e+00
+7.600000e+00 1.200000e+00 1.200000e+00 6.115400e-01 5.622500e-02 1.297900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d114-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d114-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.576800e+02 3.702000e+01 5.438600e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.890800e+02 4.376200e+01 6.410100e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.189000e+02 5.019500e+01 7.340100e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.361200e+02 5.356900e+01 7.828900e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.142900e+02 4.805700e+01 7.020000e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.379900e+02 3.135400e+01 4.597100e+01
+4.600000e+00 2.000000e-01 2.000000e-01 8.136100e+01 1.880900e+01 2.809400e+01
+5.000000e+00 2.000000e-01 2.000000e-01 4.554800e+01 1.057700e+01 1.586100e+01
+5.800000e+00 6.000000e-01 6.000000e-01 1.437000e+01 3.448400e+00 5.234100e+00
+7.600000e+00 1.200000e+00 1.200000e+00 5.877800e-01 1.400700e-01 2.165900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d114-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d114-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.217000e+02 2.136800e+01 5.508500e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.570500e+02 2.875600e+01 5.705200e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.931000e+02 3.311000e+01 6.632700e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.192100e+02 3.491800e+01 7.817500e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.015900e+02 3.189300e+01 6.867400e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.315700e+02 2.023700e+01 4.475300e+01
+4.600000e+00 2.000000e-01 2.000000e-01 7.956000e+01 1.362300e+01 2.580300e+01
+5.000000e+00 2.000000e-01 2.000000e-01 4.674200e+01 2.718300e+00 1.337300e+01
+5.800000e+00 6.000000e-01 6.000000e-01 1.587400e+01 2.351900e+00 3.766100e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.667600e-01 5.681500e-02 1.605200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d115-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d115-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.665800e+00 6.678500e-01 6.858559e-01
+1.050000e+02 1.000000e+01 1.000000e+01 4.712300e+00 4.874926e-01 5.099653e-01
+1.275000e+02 1.250000e+01 1.250000e+01 4.073500e+00 3.278462e-01 3.091421e-01
+1.525000e+02 1.250000e+01 1.250000e+01 3.179200e+00 1.990791e-01 1.957019e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.453400e+00 1.378531e-01 1.350295e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.734100e+00 8.475521e-02 7.626382e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.042200e+00 5.064959e-02 5.032267e-02
+2.650000e+02 1.500000e+01 1.500000e+01 6.199300e-01 5.535075e-02 5.525754e-02
+2.975000e+02 1.750000e+01 1.750000e+01 3.973900e-01 2.747221e-02 2.414900e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.201800e-01 1.781863e-02 1.807301e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.403800e-01 1.432198e-02 1.458703e-02
+4.350000e+02 4.500000e+01 4.500000e+01 5.246900e-02 7.396627e-03 7.142820e-03
+5.825000e+02 1.025000e+02 1.025000e+02 9.758700e-03 1.920456e-03 1.968488e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d115-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d115-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.432300e+00 3.867900e-01 4.608600e-01
+1.050000e+02 1.000000e+01 1.000000e+01 3.795000e+00 5.281400e-01 3.132500e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.426400e+00 3.683200e-01 3.154800e-01
+1.525000e+02 1.250000e+01 1.250000e+01 2.839700e+00 3.036700e-01 2.007900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.191500e+00 2.194300e-01 1.954000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.537100e+00 1.514900e-01 1.093400e-01
+2.350000e+02 1.500000e+01 1.500000e+01 9.712100e-01 1.018300e-01 6.519200e-02
+2.650000e+02 1.500000e+01 1.500000e+01 6.008100e-01 5.279200e-02 5.211700e-02
+2.975000e+02 1.750000e+01 1.750000e+01 3.638600e-01 3.233400e-02 2.857900e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.147700e-01 1.950300e-02 1.533300e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.244700e-01 1.198400e-02 1.009600e-02
+4.350000e+02 4.500000e+01 4.500000e+01 5.540200e-02 5.604400e-03 3.732800e-03
+5.825000e+02 1.025000e+02 1.025000e+02 1.054900e-02 1.160700e-03 1.025300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d115-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d115-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.274700e+00 7.190500e-01 1.045400e+00
+1.050000e+02 1.000000e+01 1.000000e+01 3.733000e+00 8.290900e-01 1.209400e+00
+1.275000e+02 1.250000e+01 1.250000e+01 3.642900e+00 8.199300e-01 1.195500e+00
+1.525000e+02 1.250000e+01 1.250000e+01 3.233700e+00 7.320600e-01 1.067800e+00
+1.775000e+02 1.250000e+01 1.250000e+01 2.694400e+00 6.155400e-01 9.005700e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.937000e+00 4.512200e-01 6.646500e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.280800e+00 3.024400e-01 4.471100e-01
+2.650000e+02 1.500000e+01 1.500000e+01 8.154200e-01 1.955600e-01 2.906500e-01
+2.975000e+02 1.750000e+01 1.750000e+01 5.032500e-01 1.230400e-01 1.837300e-01
+3.325000e+02 1.750000e+01 1.750000e+01 3.077000e-01 7.597300e-02 1.138100e-01
+3.700000e+02 2.000000e+01 2.000000e+01 1.843100e-01 4.597500e-02 6.892100e-02
+4.350000e+02 4.500000e+01 4.500000e+01 8.196700e-02 2.092900e-02 3.159100e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.661400e-02 4.346800e-03 6.610300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d115-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d115-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.247700e+00 3.663900e-01 1.274300e+00
+1.050000e+02 1.000000e+01 1.000000e+01 3.572600e+00 5.606600e-01 1.204500e+00
+1.275000e+02 1.250000e+01 1.250000e+01 3.416600e+00 5.932200e-01 1.058400e+00
+1.525000e+02 1.250000e+01 1.250000e+01 2.991300e+00 4.270100e-01 1.017700e+00
+1.775000e+02 1.250000e+01 1.250000e+01 2.347200e+00 3.826900e-01 8.677800e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.681400e+00 2.743900e-01 6.893000e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.053300e+00 1.782000e-01 3.952300e-01
+2.650000e+02 1.500000e+01 1.500000e+01 6.836400e-01 1.242200e-01 2.270900e-01
+2.975000e+02 1.750000e+01 1.750000e+01 4.186800e-01 7.698900e-02 1.473300e-01
+3.325000e+02 1.750000e+01 1.750000e+01 2.620500e-01 5.768200e-02 7.882800e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.516800e-01 3.156300e-02 4.312400e-02
+4.350000e+02 4.500000e+01 4.500000e+01 6.819800e-02 1.272900e-02 2.067600e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.469100e-02 2.229200e-03 5.345600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d116-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d116-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t116
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.023600e-01 1.130462e-01 1.130462e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.684200e+00 3.060627e-01 3.060627e-01
+9.250000e-01 2.500000e-02 2.500000e-02 5.084000e+00 7.082546e-01 7.082546e-01
+9.750000e-01 2.500000e-02 2.500000e-02 6.746000e+00 1.974846e+00 1.974846e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d116-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d116-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t116
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.365400e-01 0.000000e+00 5.099400e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.739800e+00 3.354900e-02 3.581100e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.069900e+00 3.253400e-01 0.000000e+00
+9.750000e-01 2.500000e-02 2.500000e-02 5.659300e+00 5.351000e-01 4.739900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d116-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d116-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t116
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.306000e-01 1.453200e-02 1.676400e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.810800e+00 7.618100e-02 8.004900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.103200e+00 2.293600e-01 2.443100e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.425300e+00 2.637300e-01 2.731000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d117-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d117-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t117
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.257200e-03 2.465346e-03 2.465346e-03
+1.400000e+02 2.500000e+01 2.500000e+01 6.199800e-03 1.093463e-03 1.093463e-03
+1.925000e+02 2.750000e+01 2.750000e+01 3.385000e-03 6.762096e-04 6.762096e-04
+2.500000e+02 3.000000e+01 3.000000e+01 1.877600e-03 5.037593e-04 5.037593e-04
+3.575000e+02 7.750000e+01 7.750000e+01 5.946800e-04 2.631693e-04 2.631693e-04
+5.600000e+02 1.250000e+02 1.250000e+02 1.800100e-04 1.291442e-04 1.291442e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d117-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d117-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t117
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.239800e-03 5.017000e-04 9.408800e-05
+1.400000e+02 2.500000e+01 2.500000e+01 4.804500e-03 2.900700e-05 4.066500e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.669900e-03 1.729000e-04 7.828200e-05
+2.500000e+02 3.000000e+01 3.000000e+01 2.402700e-03 2.034300e-04 0.000000e+00
+3.575000e+02 7.750000e+01 7.750000e+01 1.185100e-03 2.747100e-05 1.869300e-04
+5.600000e+02 1.250000e+02 1.250000e+02 3.267100e-04 3.025200e-05 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d117-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d117-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t117
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.768300e-03 2.965100e-04 3.865600e-04
+1.400000e+02 2.500000e+01 2.500000e+01 5.255000e-03 2.604300e-04 3.155800e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.835400e-03 2.121300e-04 2.214200e-04
+2.500000e+02 3.000000e+01 3.000000e+01 2.379100e-03 1.599600e-04 1.621900e-04
+3.575000e+02 7.750000e+01 7.750000e+01 1.025100e-03 6.532900e-05 7.927300e-05
+5.600000e+02 1.250000e+02 1.250000e+02 2.311300e-04 2.442600e-05 3.342300e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d118-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d118-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t118
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.892900e+00 7.182502e-01 7.182502e-01
+3.000000e-01 1.000000e-01 1.000000e-01 1.680700e+00 4.740168e-01 4.740168e-01
+7.000000e-01 3.000000e-01 3.000000e-01 1.421300e-01 2.328305e-01 2.328305e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d118-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d118-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t118
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.780400e+00 2.156200e-01 2.168200e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.659500e+00 1.473200e-01 3.328400e-02
+7.000000e-01 3.000000e-01 3.000000e-01 1.867100e-01 8.866000e-03 1.235300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d118-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d118-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t118
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.804200e+00 9.483400e-02 9.917100e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.670100e+00 7.318600e-02 7.585200e-02
+7.000000e-01 3.000000e-01 3.000000e-01 1.752300e-01 1.368700e-02 1.493600e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d119-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d119-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t119
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.358900e-01 2.310755e-01 2.310755e-01
+1.000000e+00 5.000000e-01 5.000000e-01 8.261700e-02 1.109725e-01 1.109725e-01
+5.000000e+00 3.500000e+00 3.500000e+00 8.149600e-02 1.171497e-01 1.171497e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d119-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d119-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t119
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.871300e-01 5.594200e-03 3.429900e-03
+1.000000e+00 5.000000e-01 5.000000e-01 9.468100e-02 2.927000e-03 4.937900e-03
+5.000000e+00 3.500000e+00 3.500000e+00 1.819300e-02 5.601600e-04 3.261200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d119-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d119-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t119
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.835900e-01 2.379900e-02 2.432100e-02
+1.000000e+00 5.000000e-01 5.000000e-01 8.941800e-02 7.570800e-03 8.527600e-03
+5.000000e+00 3.500000e+00 3.500000e+00 2.699100e-02 4.159500e-03 5.133800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d120-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d120-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t120
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 2.066400e-03 3.387979e-04 3.387979e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.585900e-03 1.985014e-04 1.985014e-04
+1.275000e+03 7.500000e+01 7.500000e+01 1.109000e-03 1.666473e-04 1.666473e-04
+1.425000e+03 7.500000e+01 7.500000e+01 7.989400e-04 1.911995e-04 1.911995e-04
+1.750000e+03 2.500000e+02 2.500000e+02 4.819700e-04 8.001193e-05 8.001193e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.159600e-04 2.753683e-05 2.753683e-05
+3.350000e+03 6.500000e+02 6.500000e+02 2.032200e-05 7.512427e-06 7.512427e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d120-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d120-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t120
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.776800e-03 1.456400e-04 1.308500e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.454200e-03 9.904800e-05 1.735200e-04
+1.275000e+03 7.500000e+01 7.500000e+01 1.146000e-03 0.000000e+00 9.799000e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.653700e-04 3.626500e-05 0.000000e+00
+1.750000e+03 2.500000e+02 2.500000e+02 4.798000e-04 1.186900e-05 8.028800e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.508700e-04 5.670100e-06 1.065200e-05
+3.350000e+03 6.500000e+02 6.500000e+02 2.284100e-05 2.336100e-06 2.329000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d120-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d120-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t120
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.704200e-03 7.203900e-05 7.770800e-05
+1.150000e+03 5.000000e+01 5.000000e+01 1.407700e-03 6.547200e-05 6.820500e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.136800e-03 4.804000e-05 5.452800e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.539800e-04 4.163800e-05 4.429600e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.888400e-04 1.725500e-05 1.779300e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.612200e-04 8.374800e-06 9.443100e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.532300e-05 2.435500e-06 3.029600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d121-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d121-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t121
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 5.257200e-03 6.442300e-04 6.442300e-04
+3.750000e+01 1.250000e+01 1.250000e+01 9.913900e-03 1.177899e-03 1.177899e-03
+6.250000e+01 1.250000e+01 1.250000e+01 8.067000e-03 7.212043e-04 7.212043e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.753700e-03 6.128160e-04 6.128160e-04
+1.300000e+02 3.000000e+01 3.000000e+01 2.662800e-03 4.035903e-04 4.035903e-04
+2.100000e+02 5.000000e+01 5.000000e+01 7.339100e-04 3.123464e-04 3.123464e-04
+3.775000e+02 1.175000e+02 1.175000e+02 1.642100e-04 5.264875e-05 5.264875e-05
+6.975000e+02 2.025000e+02 2.025000e+02 8.526300e-06 1.036673e-05 1.036673e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d121-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d121-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t121
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.495700e-03 0.000000e+00 1.008900e-03
+3.750000e+01 1.250000e+01 1.250000e+01 7.123200e-03 2.261500e-04 6.968700e-05
+6.250000e+01 1.250000e+01 1.250000e+01 6.530500e-03 1.064200e-04 6.587700e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.283000e-03 1.991700e-04 3.218000e-05
+1.300000e+02 3.000000e+01 3.000000e+01 3.408700e-03 5.727800e-05 0.000000e+00
+2.100000e+02 5.000000e+01 5.000000e+01 1.473500e-03 8.284200e-05 0.000000e+00
+3.775000e+02 1.175000e+02 1.175000e+02 3.184400e-04 8.217900e-06 8.099800e-05
+6.975000e+02 2.025000e+02 2.025000e+02 3.082200e-05 3.614800e-06 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d121-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d121-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t121
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.766100e-03 2.140500e-04 2.350700e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.678500e-03 3.056400e-04 3.240100e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.720100e-03 2.859300e-04 3.185400e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.420200e-03 2.567900e-04 2.766100e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.466100e-03 1.325500e-04 1.401200e-04
+2.100000e+02 5.000000e+01 5.000000e+01 1.389800e-03 6.501600e-05 6.730900e-05
+3.775000e+02 1.175000e+02 1.175000e+02 2.443900e-04 1.778500e-05 2.066400e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.481800e-05 3.335900e-06 3.868100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d122-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d122-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t122
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.128100e-01 6.931408e-02 6.931408e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.292600e+00 1.754933e-01 1.754933e-01
+8.500000e-01 5.000000e-02 5.000000e-02 2.849300e+00 2.906862e-01 2.906862e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.428100e+00 4.306034e-01 4.306034e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.708900e+00 8.452775e-01 8.452775e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d122-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d122-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t122
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.587700e-01 5.176900e-03 2.325000e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.197200e+00 6.864700e-02 0.000000e+00
+8.500000e-01 5.000000e-02 5.000000e-02 2.376700e+00 5.536800e-02 0.000000e+00
+9.250000e-01 2.500000e-02 2.500000e-02 3.964500e+00 1.953300e-02 3.789900e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.264900e+00 1.530600e-01 2.724500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d122-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d122-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t122
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.381100e-01 1.017100e-02 1.108400e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.219100e+00 6.088900e-02 6.469100e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.467100e+00 8.661800e-02 9.201500e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.032300e+00 1.566000e-01 1.788000e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.261800e+00 1.788900e-01 1.903600e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d123-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d123-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t123
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 7.847200e-02 2.251447e-02 2.251447e-02
+3.200000e+00 4.000000e-01 4.000000e-01 1.706800e-01 2.670302e-02 2.670302e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.068800e-01 3.931611e-02 3.931611e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.929200e-01 7.162762e-02 7.162762e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.695400e-01 5.304497e-02 5.304497e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.352300e-01 7.909049e-02 7.909049e-02
+7.000000e+00 1.800000e+00 1.800000e+00 7.745700e-02 1.941613e-02 1.941613e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d123-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d123-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t123
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 6.834100e-02 2.985400e-03 4.022800e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.694500e-01 9.073300e-03 2.084000e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.806500e-01 1.497700e-02 1.495200e-04
+4.200000e+00 2.000000e-01 2.000000e-01 3.504300e-01 1.630900e-02 2.860300e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.899700e-01 1.044300e-03 7.664500e-03
+5.000000e+00 2.000000e-01 2.000000e-01 3.913300e-01 1.002500e-02 4.957900e-02
+7.000000e+00 1.800000e+00 1.800000e+00 6.800400e-02 3.137100e-03 9.999400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d123-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d123-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t123
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 5.412600e-02 4.536000e-03 5.975800e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.451400e-01 7.427700e-03 9.474700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.525900e-01 1.385800e-02 1.670600e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.316000e-01 1.587800e-02 1.669200e-02
+4.600000e+00 2.000000e-01 2.000000e-01 4.138100e-01 1.773700e-02 2.019600e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.121500e-01 1.770100e-02 2.105400e-02
+7.000000e+00 1.800000e+00 1.800000e+00 7.681400e-02 2.547300e-03 3.641800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d124-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d124-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t124
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.391500e-03 1.374241e-03 1.374241e-03
+1.275000e+02 1.250000e+01 1.250000e+01 7.056900e-03 7.344399e-04 7.344399e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.575600e-03 6.293049e-04 6.293049e-04
+1.775000e+02 1.250000e+01 1.250000e+01 2.875100e-03 4.954216e-04 4.954216e-04
+2.200000e+02 3.000000e+01 3.000000e+01 2.567000e-03 3.226880e-04 3.226880e-04
+4.675000e+02 2.175000e+02 2.175000e+02 4.588300e-04 1.004593e-04 1.004593e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d124-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d124-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t124
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.130900e-03 2.415800e-04 6.232700e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.748200e-03 1.496600e-04 1.098200e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.150200e-03 1.595500e-04 1.408800e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.320400e-03 1.017000e-04 6.212500e-05
+2.200000e+02 3.000000e+01 3.000000e+01 3.072500e-03 4.842900e-05 3.440300e-04
+4.675000e+02 2.175000e+02 2.175000e+02 5.875800e-04 3.647300e-05 3.251500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d124-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d124-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t124
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.687900e-03 2.226200e-04 2.669300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.238100e-03 2.758500e-04 3.253600e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.468500e-03 2.582700e-04 3.195000e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.457300e-03 2.331800e-04 2.694300e-04
+2.200000e+02 3.000000e+01 3.000000e+01 3.068900e-03 1.248900e-04 1.447400e-04
+4.675000e+02 2.175000e+02 2.175000e+02 4.889500e-04 1.851400e-05 2.496300e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d125-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d125-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t125
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 2.594400e-03 4.190878e-04 4.190878e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.553700e-03 2.612375e-04 2.612375e-04
+1.275000e+03 7.500000e+01 7.500000e+01 1.072900e-03 1.985562e-04 1.985562e-04
+1.425000e+03 7.500000e+01 7.500000e+01 8.580400e-04 1.864359e-04 1.864359e-04
+1.750000e+03 2.500000e+02 2.500000e+02 4.344900e-04 1.704024e-04 1.704024e-04
+2.350000e+03 3.500000e+02 3.500000e+02 8.611900e-05 4.402697e-05 4.402697e-05
+3.350000e+03 6.500000e+02 6.500000e+02 1.387300e-05 1.362833e-05 1.362833e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d125-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d125-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t125
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.869000e-03 8.297400e-05 1.403700e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.514600e-03 8.065100e-05 8.493300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.174600e-03 3.970400e-05 5.986900e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.704500e-04 5.492200e-05 0.000000e+00
+1.750000e+03 2.500000e+02 2.500000e+02 4.639200e-04 8.550100e-06 3.618800e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.386100e-04 6.042900e-06 1.018900e-05
+3.350000e+03 6.500000e+02 6.500000e+02 1.991800e-05 2.218200e-06 1.967000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d125-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d125-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t125
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.811700e-03 6.565500e-05 7.262200e-05
+1.150000e+03 5.000000e+01 5.000000e+01 1.467600e-03 5.909100e-05 6.342100e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.161500e-03 4.292300e-05 4.829600e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.521900e-04 3.676600e-05 3.954900e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.755500e-04 1.504300e-05 1.586300e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.484300e-04 7.102900e-06 7.838100e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.179700e-05 1.997300e-06 2.419000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d126-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d126-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t126
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.316600e-02 1.167391e-01 1.167391e-01
+7.500000e-01 5.000000e-02 5.000000e-02 1.077800e+00 2.641903e-01 2.641903e-01
+8.500000e-01 5.000000e-02 5.000000e-02 2.940700e+00 4.358110e-01 4.358110e-01
+9.250000e-01 2.500000e-02 2.500000e-02 5.160700e+00 8.712068e-01 8.712068e-01
+9.750000e-01 2.500000e-02 2.500000e-02 6.198000e+00 2.041773e+00 2.041773e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d126-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d126-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t126
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.466500e-01 2.039700e-03 1.887900e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.174000e+00 7.784000e-02 0.000000e+00
+8.500000e-01 5.000000e-02 5.000000e-02 2.377200e+00 8.026200e-02 2.695900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.012100e+00 6.297600e-02 2.827100e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.432300e+00 1.540300e-01 1.159600e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d126-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d126-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t126
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.307800e-01 8.851600e-03 1.017500e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.213800e+00 5.371000e-02 5.589200e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.450700e+00 7.631600e-02 7.704000e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.073100e+00 1.391400e-01 1.458700e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.367000e+00 1.597200e-01 1.715200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d127-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d127-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t127
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.580200e-01 5.158983e-02 5.158983e-02
+3.200000e+00 4.000000e-01 4.000000e-01 2.251000e-01 4.386656e-02 4.386656e-02
+4.000000e+00 4.000000e-01 4.000000e-01 2.738800e-01 4.135038e-02 4.135038e-02
+4.800000e+00 4.000000e-01 4.000000e-01 3.212500e-01 7.000266e-02 7.000266e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.090600e-01 6.827894e-02 6.827894e-02
+7.400000e+00 1.400000e+00 1.400000e+00 1.791200e-02 1.692342e-02 1.692342e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d127-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d127-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t127
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.733600e-02 5.356100e-03 3.796600e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.961000e-01 6.955800e-03 1.301800e-02
+4.000000e+00 4.000000e-01 4.000000e-01 3.223100e-01 7.804600e-03 8.098900e-03
+4.800000e+00 4.000000e-01 4.000000e-01 3.665900e-01 1.322700e-02 1.837700e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.061100e-01 1.516000e-03 4.688500e-03
+7.400000e+00 1.400000e+00 1.400000e+00 1.758400e-02 1.554300e-03 9.895200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d127-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d127-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t127
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 7.695900e-02 4.781400e-03 7.292300e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.697600e-01 7.101500e-03 9.693300e-03
+4.000000e+00 4.000000e-01 4.000000e-01 3.024600e-01 9.479000e-03 1.106800e-02
+4.800000e+00 4.000000e-01 4.000000e-01 3.953700e-01 1.083800e-02 1.239700e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.304800e-01 8.274600e-03 1.024900e-02
+7.400000e+00 1.400000e+00 1.400000e+00 2.142100e-02 1.348400e-03 2.010000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d128-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d128-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t128
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.642600e-03 1.960698e-03 1.960698e-03
+1.275000e+02 1.250000e+01 1.250000e+01 6.181900e-03 1.086276e-03 1.086276e-03
+1.525000e+02 1.250000e+01 1.250000e+01 5.108300e-03 9.268621e-04 9.268621e-04
+1.775000e+02 1.250000e+01 1.250000e+01 3.381100e-03 6.160713e-04 6.160713e-04
+2.050000e+02 1.500000e+01 1.500000e+01 2.577200e-03 4.961571e-04 4.961571e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.464700e-03 5.046414e-04 5.046414e-04
+3.000000e+02 5.000000e+01 5.000000e+01 1.591500e-03 3.863047e-04 3.863047e-04
+4.150000e+02 6.500000e+01 6.500000e+01 7.435300e-04 1.969364e-04 1.969364e-04
+5.825000e+02 1.025000e+02 1.025000e+02 1.397800e-04 8.768520e-05 8.768520e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d128-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d128-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t128
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.591600e-03 3.631500e-04 4.697300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.321200e-03 2.273500e-04 7.368200e-05
+1.525000e+02 1.250000e+01 1.250000e+01 4.875200e-03 1.269000e-04 3.029000e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.188200e-03 2.541400e-05 8.894900e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.505400e-03 6.468700e-05 4.064000e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.725200e-03 7.818100e-05 6.547600e-05
+3.000000e+02 5.000000e+01 5.000000e+01 1.741000e-03 9.813200e-05 6.747100e-05
+4.150000e+02 6.500000e+01 6.500000e+01 6.680600e-04 2.667300e-05 1.152700e-04
+5.825000e+02 1.025000e+02 1.025000e+02 1.551800e-04 9.030200e-06 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d128-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d128-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t128
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.155200e-03 1.874000e-04 2.542300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.851400e-03 2.362300e-04 2.796300e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.218100e-03 2.230800e-04 2.756400e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.373900e-03 2.042400e-04 2.336300e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.536600e-03 1.676500e-04 1.888100e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.755400e-03 1.479800e-04 1.593700e-04
+3.000000e+02 5.000000e+01 5.000000e+01 1.546600e-03 6.072400e-05 7.170500e-05
+4.150000e+02 6.500000e+01 6.500000e+01 5.305400e-04 3.119300e-05 4.312000e-05
+5.825000e+02 1.025000e+02 1.025000e+02 1.028900e-04 1.093900e-05 1.551400e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d129-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d129-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t129
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.327800e+00 1.389135e+00 1.389135e+00
+3.000000e-01 1.000000e-01 1.000000e-01 1.539000e+00 2.244209e-01 2.244209e-01
+5.000000e-01 1.000000e-01 1.000000e-01 8.173400e-01 4.726766e-01 4.726766e-01
+8.000000e-01 2.000000e-01 2.000000e-01 1.579400e-01 1.700791e-01 1.700791e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d129-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d129-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t129
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.579100e+00 1.214900e-01 2.907000e-03
+3.000000e-01 1.000000e-01 1.000000e-01 1.669400e+00 0.000000e+00 4.594200e-02
+5.000000e-01 1.000000e-01 1.000000e-01 5.755300e-01 1.829200e-02 1.262200e-01
+8.000000e-01 2.000000e-01 2.000000e-01 8.800700e-02 1.777400e-03 3.412700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d129-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d129-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t129
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.616300e+00 5.581000e-02 6.133300e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.674600e+00 4.465000e-02 4.573200e-02
+5.000000e-01 1.000000e-01 1.000000e-01 5.580900e-01 2.577600e-02 2.870700e-02
+8.000000e-01 2.000000e-01 2.000000e-01 7.551800e-02 6.704700e-03 7.677700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d130-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d130-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t130
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 7.954800e-01 3.269501e-01 3.269501e-01
+1.000000e+00 5.000000e-01 5.000000e-01 1.242000e-01 1.342327e-01 1.342327e-01
+5.000000e+00 3.500000e+00 3.500000e+00 8.032600e-02 1.275911e-01 1.275911e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d130-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d130-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t130
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.785900e-01 7.975500e-03 4.351500e-03
+1.000000e+00 5.000000e-01 5.000000e-01 1.021400e-01 3.845900e-03 5.014800e-03
+5.000000e+00 3.500000e+00 3.500000e+00 1.927000e-02 8.246800e-04 2.957400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d130-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d130-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t130
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.725200e-01 1.440000e-02 1.481500e-02
+1.000000e+00 5.000000e-01 5.000000e-01 9.830500e-02 4.833500e-03 5.449800e-03
+5.000000e+00 3.500000e+00 3.500000e+00 2.917600e-02 2.633200e-03 3.563400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d131-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d131-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t131
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 8.262700e-02 1.237262e-01 1.237262e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.538700e+00 5.351295e-01 5.351295e-01
+9.500000e-01 5.000000e-02 5.000000e-02 6.344200e+00 1.601282e+00 1.601282e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d131-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d131-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t131
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.340000e-01 5.373100e-03 1.138000e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.696700e+00 2.749400e-02 7.501500e-03
+9.500000e-01 5.000000e-02 5.000000e-02 4.968600e+00 4.877900e-02 5.255200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d131-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d131-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t131
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.375100e-01 2.459900e-02 2.536700e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.746800e+00 1.248000e-01 1.334300e-01
+9.500000e-01 5.000000e-02 5.000000e-02 4.843900e+00 2.939100e-01 3.181300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d132-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d132-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t132
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 5.114000e-03 9.542262e-04 9.542262e-04
+4.525000e+02 2.325000e+02 2.325000e+02 6.108400e-04 2.507862e-04 2.507862e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d132-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d132-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t132
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 4.123000e-03 4.194100e-05 1.085200e-04
+4.525000e+02 2.325000e+02 2.325000e+02 9.092000e-04 3.134500e-05 1.458200e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d132-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d132-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t132
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 4.524800e-03 2.417200e-04 2.695300e-04
+4.525000e+02 2.325000e+02 2.325000e+02 7.882300e-04 5.535900e-05 6.577500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d133-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d133-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t133
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.243600e+00 3.735556e-01 3.735556e-01
+7.000000e-01 3.000000e-01 3.000000e-01 1.709500e-01 1.938156e-01 1.938156e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d133-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d133-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t133
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.287500e+00 0.000000e+00 1.302300e-02
+7.000000e-01 3.000000e-01 3.000000e-01 1.416900e-01 7.956400e-03 1.157900e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d133-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d133-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t133
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.317500e+00 1.016600e-01 1.022900e-01
+7.000000e-01 3.000000e-01 3.000000e-01 1.216800e-01 1.901900e-02 2.048700e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d134-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d134-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t134
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.675400e-01 7.910694e-02 7.910694e-02
+1.000000e+00 5.000000e-01 5.000000e-01 3.246400e-02 9.812075e-02 9.812075e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d134-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d134-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t134
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.112700e-01 1.310100e-02 0.000000e+00
+1.000000e+00 5.000000e-01 5.000000e-01 8.873400e-02 0.000000e+00 1.020200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d134-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d134-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t134
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.203000e-01 4.101300e-02 4.142100e-02
+1.000000e+00 5.000000e-01 5.000000e-01 7.970200e-02 1.207000e-02 1.335500e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d135-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d135-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t135
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.060600e+00 2.919681e+00 2.919681e+00
+8.000000e-01 1.000000e-01 1.000000e-01 3.390500e+01 1.401911e+01 1.401911e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.023500e+02 3.653857e+01 3.653857e+01
+9.750000e-01 2.500000e-02 2.500000e-02 1.358100e+02 4.366729e+01 4.366729e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d135-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d135-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t135
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.355200e+00 6.702500e-01 2.109900e+00
+8.000000e-01 1.000000e-01 1.000000e-01 3.203400e+01 5.241700e+00 7.890400e+00
+9.250000e-01 2.500000e-02 2.500000e-02 7.493700e+01 1.208700e+01 1.774600e+01
+9.750000e-01 2.500000e-02 2.500000e-02 1.042000e+02 1.573000e+01 2.590800e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d135-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d135-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t135
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.463200e+00 2.812500e-01 4.039600e-01
+8.000000e-01 1.000000e-01 1.000000e-01 3.504600e+01 1.474400e+00 2.058600e+00
+9.250000e-01 2.500000e-02 2.500000e-02 7.941600e+01 4.439100e+00 4.752700e+00
+9.750000e-01 2.500000e-02 2.500000e-02 1.050000e+02 5.104400e+00 6.932000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d136-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d136-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t136
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.800000e+00 8.000000e-01 8.000000e-01 9.893700e-01 8.486929e-01 8.486929e-01
+4.400000e+00 8.000000e-01 8.000000e-01 4.799600e+00 1.899958e+00 1.899958e+00
+5.600000e+00 4.000000e-01 4.000000e-01 8.789000e+00 3.581552e+00 3.581552e+00
+7.400000e+00 1.400000e+00 1.400000e+00 1.197200e+00 7.472867e-01 7.472867e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d136-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d136-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t136
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.800000e+00 8.000000e-01 8.000000e-01 1.569300e+00 2.406500e-01 4.016700e-01
+4.400000e+00 8.000000e-01 8.000000e-01 5.065000e+00 8.139200e-01 1.313100e+00
+5.600000e+00 4.000000e-01 4.000000e-01 6.571300e+00 1.022000e+00 1.836800e+00
+7.400000e+00 1.400000e+00 1.400000e+00 9.072200e-01 1.443100e-01 2.461900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d136-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d136-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t136
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.800000e+00 8.000000e-01 8.000000e-01 1.288000e+00 9.993400e-02 1.400400e-01
+4.400000e+00 8.000000e-01 8.000000e-01 5.131300e+00 1.994700e-01 2.381100e-01
+5.600000e+00 4.000000e-01 4.000000e-01 7.452000e+00 3.399500e-01 5.729900e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.115000e+00 7.028900e-02 1.142000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d137-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d137-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t137
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.422700e-01 8.477553e-02 8.477553e-02
+1.400000e+02 2.500000e+01 2.500000e+01 1.215400e-01 4.175641e-02 4.175641e-02
+1.925000e+02 2.750000e+01 2.750000e+01 6.635900e-02 2.673253e-02 2.673253e-02
+2.500000e+02 3.000000e+01 3.000000e+01 3.680800e-02 1.739959e-02 1.739959e-02
+3.575000e+02 7.750000e+01 7.750000e+01 1.165800e-02 8.279260e-03 8.279260e-03
+5.600000e+02 1.250000e+02 1.250000e+02 3.528800e-03 3.175272e-03 3.175272e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d137-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d137-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t137
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.701200e-02 1.165900e-02 1.630800e-02
+1.400000e+02 2.500000e+01 2.500000e+01 8.726900e-02 1.246800e-02 2.832200e-02
+1.925000e+02 2.750000e+01 2.750000e+01 6.666100e-02 1.029800e-02 1.754400e-02
+2.500000e+02 3.000000e+01 3.000000e+01 4.364300e-02 7.126000e-03 1.014400e-02
+3.575000e+02 7.750000e+01 7.750000e+01 2.152600e-02 3.619900e-03 8.907700e-03
+5.600000e+02 1.250000e+02 1.250000e+02 5.934300e-03 1.058900e-03 1.059400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d137-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d137-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t137
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 9.167000e-02 5.700400e-03 9.657400e-03
+1.400000e+02 2.500000e+01 2.500000e+01 1.010300e-01 5.006800e-03 7.355700e-03
+1.925000e+02 2.750000e+01 2.750000e+01 7.373500e-02 4.078300e-03 5.263900e-03
+2.500000e+02 3.000000e+01 3.000000e+01 4.573800e-02 3.075300e-03 3.371400e-03
+3.575000e+02 7.750000e+01 7.750000e+01 1.970800e-02 1.256000e-03 1.478400e-03
+5.600000e+02 1.250000e+02 1.250000e+02 4.443400e-03 4.695800e-04 6.250000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d138-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d138-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t138
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.657200e+01 3.750452e+00 3.750452e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.638000e+00 3.045752e+00 3.045752e+00
+5.000000e+00 3.500000e+00 3.500000e+00 1.615800e+00 2.799342e+00 2.799342e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d138-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d138-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t138
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.633400e+01 2.647400e+00 3.836800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.743300e+00 2.592200e-01 5.361400e-01
+5.000000e+00 3.500000e+00 3.500000e+00 3.349700e-01 3.766400e-02 9.854700e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d138-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d138-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t138
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.710200e+01 4.606200e-01 8.725200e-01
+1.000000e+00 5.000000e-01 5.000000e-01 1.730600e+00 1.465300e-01 1.663700e-01
+5.000000e+00 3.500000e+00 3.500000e+00 5.223900e-01 8.050500e-02 9.046300e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d139-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d139-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t139
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.967000e+00 4.111985e+00 4.111985e+00
+7.500000e-01 5.000000e-02 5.000000e-02 5.691300e+01 1.449033e+01 1.449033e+01
+8.500000e-01 5.000000e-02 5.000000e-02 1.254600e+02 2.475365e+01 2.475365e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.949700e+02 4.410050e+01 4.410050e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.513700e+02 5.102258e+01 5.102258e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d139-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d139-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t139
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.044000e+01 1.596100e+00 3.236600e+00
+7.500000e-01 5.000000e-02 5.000000e-02 4.830100e+01 7.897300e+00 6.428600e+00
+8.500000e-01 5.000000e-02 5.000000e-02 9.588600e+01 1.390000e+01 1.668600e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.599500e+02 2.010600e+01 3.136500e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.124100e+02 2.646000e+01 4.343600e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d139-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d139-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t139
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 9.713800e+00 4.149200e-01 4.991100e-01
+7.500000e-01 5.000000e-02 5.000000e-02 4.973500e+01 2.484000e+00 3.085300e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.006500e+02 3.533700e+00 5.445000e+00
+9.250000e-01 2.500000e-02 2.500000e-02 1.645000e+02 6.388800e+00 7.474400e+00
+9.750000e-01 2.500000e-02 2.500000e-02 2.146600e+02 7.298200e+00 1.126600e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d140-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d140-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t140
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 3.411300e+00 1.353607e+00 1.353607e+00
+3.200000e+00 4.000000e-01 4.000000e-01 7.419800e+00 1.935078e+00 1.935078e+00
+3.800000e+00 2.000000e-01 2.000000e-01 8.993400e+00 2.629859e+00 2.629859e+00
+4.200000e+00 2.000000e-01 2.000000e-01 1.273300e+01 4.117456e+00 4.117456e+00
+4.600000e+00 2.000000e-01 2.000000e-01 1.606500e+01 4.215204e+00 4.215204e+00
+5.000000e+00 2.000000e-01 2.000000e-01 1.892000e+01 5.206451e+00 5.206451e+00
+7.000000e+00 1.800000e+00 1.800000e+00 3.367200e+00 9.963553e-01 9.963553e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d140-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d140-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t140
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 2.757200e+00 2.856800e-01 4.122200e-01
+3.200000e+00 4.000000e-01 4.000000e-01 6.836500e+00 1.081500e+00 1.955700e+00
+3.800000e+00 2.000000e-01 2.000000e-01 1.132300e+01 1.574400e+00 1.561100e+00
+4.200000e+00 2.000000e-01 2.000000e-01 1.413800e+01 1.863600e+00 4.243300e+00
+4.600000e+00 2.000000e-01 2.000000e-01 1.573300e+01 1.928800e+00 3.127700e+00
+5.000000e+00 2.000000e-01 2.000000e-01 1.578800e+01 2.475500e+00 2.837200e+00
+7.000000e+00 1.800000e+00 1.800000e+00 2.743600e+00 3.962800e-01 6.027500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d140-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d140-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t140
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 2.208100e+00 1.850500e-01 2.195600e-01
+3.200000e+00 4.000000e-01 4.000000e-01 5.921000e+00 3.030200e-01 3.544900e-01
+3.800000e+00 2.000000e-01 2.000000e-01 1.030500e+01 5.653400e-01 6.553600e-01
+4.200000e+00 2.000000e-01 2.000000e-01 1.352800e+01 6.477500e-01 6.885100e-01
+4.600000e+00 2.000000e-01 2.000000e-01 1.688200e+01 7.236100e-01 9.713500e-01
+5.000000e+00 2.000000e-01 2.000000e-01 1.681400e+01 7.221500e-01 1.004100e+00
+7.000000e+00 1.800000e+00 1.800000e+00 3.133700e+00 1.039200e-01 2.169200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d141-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d141-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t141
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 3.192300e-01 1.120025e-01 1.120025e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.047800e-01 7.255875e-02 7.255875e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.408100e-01 5.214738e-02 5.214738e-02
+1.775000e+02 1.250000e+01 1.250000e+01 1.241700e-01 4.096810e-02 4.096810e-02
+2.200000e+02 3.000000e+01 3.000000e+01 1.108600e-01 2.379134e-02 2.379134e-02
+4.675000e+02 2.175000e+02 2.175000e+02 1.981600e-02 5.650998e-03 5.650998e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d141-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d141-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t141
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.058900e-01 2.813800e-02 3.543100e-02
+1.275000e+02 1.250000e+01 1.250000e+01 2.306600e-01 3.016000e-02 3.937900e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.066700e-01 2.396600e-02 3.607400e-02
+1.775000e+02 1.250000e+01 1.250000e+01 1.733700e-01 2.204000e-02 3.342500e-02
+2.200000e+02 3.000000e+01 3.000000e+01 1.232900e-01 1.758800e-02 3.371500e-02
+4.675000e+02 2.175000e+02 2.175000e+02 2.357800e-02 3.758700e-03 6.331500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d141-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d141-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t141
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.314000e-01 9.056700e-03 1.507300e-02
+1.275000e+02 1.250000e+01 1.250000e+01 2.537800e-01 1.122200e-02 1.632900e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.224700e-01 1.050700e-02 1.406000e-02
+1.775000e+02 1.250000e+01 1.250000e+01 1.813300e-01 9.486200e-03 1.208100e-02
+2.200000e+02 3.000000e+01 3.000000e+01 1.248500e-01 5.080900e-03 6.374900e-03
+4.675000e+02 2.175000e+02 2.175000e+02 1.989200e-02 7.532100e-04 9.231200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d142-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d142-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t142
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.829000e+00 1.063194e+01 1.063194e+01
+7.500000e-01 5.000000e-02 5.000000e-02 7.063200e+01 4.429856e+01 4.429856e+01
+8.500000e-01 5.000000e-02 5.000000e-02 1.927300e+02 8.025927e+01 8.025927e+01
+9.250000e-01 2.500000e-02 2.500000e-02 3.382100e+02 1.371993e+02 1.371993e+02
+9.750000e-01 2.500000e-02 2.500000e-02 4.062000e+02 1.660804e+02 1.660804e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d142-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d142-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t142
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.277500e+01 1.784700e+00 3.744300e+00
+7.500000e-01 5.000000e-02 5.000000e-02 6.080600e+01 8.843000e+00 9.730000e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.231300e+02 1.735900e+01 2.371100e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.078000e+02 2.311600e+01 4.653400e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.813600e+02 3.676700e+01 5.111300e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d142-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d142-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t142
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.204700e+01 4.620800e-01 5.575400e-01
+7.500000e-01 5.000000e-02 5.000000e-02 6.336500e+01 2.803800e+00 3.373100e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.279300e+02 3.983900e+00 5.374100e+00
+9.250000e-01 2.500000e-02 2.500000e-02 2.126300e+02 7.263500e+00 9.085400e+00
+9.750000e-01 2.500000e-02 2.500000e-02 2.801700e+02 8.337800e+00 1.225100e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d143-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d143-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t143
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.011900e+01 6.015301e+00 6.015301e+00
+3.200000e+00 4.000000e-01 4.000000e-01 1.441500e+01 7.616625e+00 7.616625e+00
+4.000000e+00 4.000000e-01 4.000000e-01 1.753800e+01 1.010305e+01 1.010305e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.057100e+01 1.376363e+01 1.376363e+01
+5.600000e+00 4.000000e-01 4.000000e-01 1.338700e+01 9.289119e+00 9.289119e+00
+7.400000e+00 1.400000e+00 1.400000e+00 1.147000e+00 7.083976e-01 7.083976e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d143-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d143-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t143
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 5.041500e+00 6.305600e-01 6.808800e-01
+3.200000e+00 4.000000e-01 4.000000e-01 1.015700e+01 1.416100e+00 2.615100e+00
+4.000000e+00 4.000000e-01 4.000000e-01 1.669400e+01 2.062600e+00 3.861900e+00
+4.800000e+00 4.000000e-01 4.000000e-01 1.898800e+01 2.606200e+00 3.640800e+00
+5.600000e+00 4.000000e-01 4.000000e-01 1.067500e+01 1.482900e+00 2.199400e+00
+7.400000e+00 1.400000e+00 1.400000e+00 9.107600e-01 1.466000e-01 2.447600e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d143-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d143-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t143
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 4.017500e+00 2.496100e-01 3.626100e-01
+3.200000e+00 4.000000e-01 4.000000e-01 8.862000e+00 3.707200e-01 4.803700e-01
+4.000000e+00 4.000000e-01 4.000000e-01 1.578900e+01 4.948300e-01 5.839000e-01
+4.800000e+00 4.000000e-01 4.000000e-01 2.063900e+01 5.657500e-01 9.146400e-01
+5.600000e+00 4.000000e-01 4.000000e-01 1.203200e+01 4.319600e-01 7.398200e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.118200e+00 7.038900e-02 1.151500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d144-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d144-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t144
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 3.586100e-01 2.847792e-01 2.847792e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.928800e-01 2.004844e-01 2.004844e-01
+1.525000e+02 1.250000e+01 1.250000e+01 3.246600e-01 1.533856e-01 1.533856e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.148800e-01 1.301488e-01 1.301488e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.637900e-01 9.830358e-02 9.830358e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.566400e-01 8.339904e-02 8.339904e-02
+3.000000e+02 5.000000e+01 5.000000e+01 1.011500e-01 5.663508e-02 5.663508e-02
+4.150000e+02 6.500000e+01 6.500000e+01 4.725400e-02 2.339085e-02 2.339085e-02
+5.825000e+02 1.025000e+02 1.025000e+02 8.883300e-03 5.141496e-03 5.141496e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d144-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d144-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t144
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.360800e-01 3.254100e-02 3.997100e-02
+1.275000e+02 1.250000e+01 1.250000e+01 2.736000e-01 3.329400e-02 4.618700e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.506700e-01 2.991800e-02 6.328300e-02
+1.775000e+02 1.250000e+01 1.250000e+01 2.153400e-01 2.457100e-02 4.439500e-02
+2.050000e+02 1.500000e+01 1.500000e+01 1.802300e-01 2.677100e-02 5.693700e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.401200e-01 1.564900e-02 2.655800e-02
+3.000000e+02 5.000000e+01 5.000000e+01 8.951600e-02 1.349100e-02 2.013200e-02
+4.150000e+02 6.500000e+01 6.500000e+01 3.434900e-02 4.557400e-03 1.402800e-02
+5.825000e+02 1.025000e+02 1.025000e+02 7.978700e-03 1.068200e-03 1.368800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d144-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d144-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t144
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.682500e-01 9.751300e-03 1.674800e-02
+1.275000e+02 1.250000e+01 1.250000e+01 3.044800e-01 1.229200e-02 1.774700e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.715300e-01 1.160800e-02 1.485000e-02
+1.775000e+02 1.250000e+01 1.250000e+01 2.276000e-01 1.062800e-02 1.307900e-02
+2.050000e+02 1.500000e+01 1.500000e+01 1.840300e-01 8.723800e-03 1.193600e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.433800e-01 7.700300e-03 8.618100e-03
+3.000000e+02 5.000000e+01 5.000000e+01 8.047900e-02 3.159800e-03 3.674600e-03
+4.150000e+02 6.500000e+01 6.500000e+01 2.760700e-02 1.623200e-03 2.186300e-03
+5.825000e+02 1.025000e+02 1.025000e+02 5.354000e-03 5.692300e-04 7.890300e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d145-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d145-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t145
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.081500e+01 1.340513e+01 1.340513e+01
+1.000000e+00 5.000000e-01 5.000000e-01 7.933800e+00 1.453248e+01 1.453248e+01
+5.000000e+00 3.500000e+00 3.500000e+00 5.131300e+00 1.108318e+01 1.108318e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d145-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d145-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t145
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 4.550600e+01 6.389100e+00 8.944800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 5.290500e+00 4.758300e-01 1.213800e+00
+5.000000e+00 3.500000e+00 3.500000e+00 9.981000e-01 1.181700e-01 2.592400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d145-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d145-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t145
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 4.554800e+01 7.517200e-01 1.603100e+00
+1.000000e+00 5.000000e-01 5.000000e-01 5.131800e+00 2.523200e-01 2.853600e-01
+5.000000e+00 3.500000e+00 3.500000e+00 1.523100e+00 1.374600e-01 1.651300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d146-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d146-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t146
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.779900e-01 8.090187e-01 8.090187e-01
+8.000000e-01 1.000000e-01 1.000000e-01 8.901100e+00 3.877624e+00 3.877624e+00
+9.500000e-01 5.000000e-02 5.000000e-02 3.670100e+01 1.155229e+01 1.155229e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d146-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d146-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t146
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.499800e+00 2.920200e-01 4.895300e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.087500e+01 1.950100e+00 3.323400e+00
+9.500000e-01 5.000000e-02 5.000000e-02 3.184500e+01 5.320200e+00 9.142800e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d146-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d146-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t146
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.652300e+00 1.711300e-01 2.110200e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.215200e+01 8.682100e-01 1.171900e+00
+9.500000e-01 5.000000e-02 5.000000e-02 3.369700e+01 2.044600e+00 2.568500e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d147-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d147-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t147
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.700000e+00 1.500000e+00 1.500000e+00 5.926800e-01 2.795387e-01 2.795387e-01
+5.600000e+00 4.000000e-01 4.000000e-01 2.243100e+00 8.148347e-01 8.148347e-01
+7.400000e+00 1.400000e+00 1.400000e+00 7.249500e-01 3.906053e-01 3.906053e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d147-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d147-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t147
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.700000e+00 1.500000e+00 1.500000e+00 9.124100e-01 1.824300e-01 2.578300e-01
+5.600000e+00 4.000000e-01 4.000000e-01 2.269900e+00 2.817400e-01 7.024200e-01
+7.400000e+00 1.400000e+00 1.400000e+00 6.537700e-01 1.258600e-01 2.023800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d147-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d147-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t147
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.700000e+00 1.500000e+00 1.500000e+00 8.459900e-01 5.914900e-02 6.840600e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.672200e+00 2.035700e-01 2.902100e-01
+7.400000e+00 1.400000e+00 1.400000e+00 8.064800e-01 5.977800e-02 9.021300e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d148-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d148-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t148
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 2.891900e-02 1.133468e-02 1.133468e-02
+4.525000e+02 2.325000e+02 2.325000e+02 3.454200e-03 1.637921e-03 1.637921e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d148-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d148-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t148
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 2.582200e-02 3.978900e-03 7.630100e-03
+4.525000e+02 2.325000e+02 2.325000e+02 5.694300e-03 1.162800e-03 1.730700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d148-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d148-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t148
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 3.105100e-02 1.658800e-03 2.820300e-03
+4.525000e+02 2.325000e+02 2.325000e+02 5.409100e-03 3.798900e-04 4.199000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d149-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d149-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t149
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.570500e+00 1.202954e+00 1.202954e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.869100e-01 6.709501e-01 6.709501e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d149-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d149-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t149
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.753000e+00 1.067200e+00 1.685900e+00
+1.000000e+00 5.000000e-01 5.000000e-01 5.601900e-01 6.930800e-02 1.839700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194/d149-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194/d149-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t149
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.246700e+00 2.783900e-01 4.721300e-01
+1.000000e+00 5.000000e-01 5.000000e-01 5.409900e-01 8.192500e-02 8.663100e-02
+END YODA_SCATTER2D_V2
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1517194_EL.info b/analyses/pluginATLAS/ATLAS_2017_I1517194_EL.info
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2017_I1517194_EL.info
@@ -0,0 +1,50 @@
+Name: ATLAS_2017_I1517194_EL
+Year: 2017
+Summary: Electroweak Wjj production at 8 TeV
+Experiment: ATLAS
+Collider: LHC
+InspireID: 1517194
+Status: VALIDATED
+Authors:
+ - Christian Johnson <christian.johnson@cern.ch>
+ - Christian Gutschow <chris.g@cern.ch>
+References:
+ - Eur.Phys.J. C77 (2017) no.7, 474
+ - arXiv:1703.04362 [hep-ex]
+Keywords:
+ - VJETS
+ - ELECTROWEAK
+ - VBF
+ - VJJ
+RunInfo:
+ pp -> electroweak electron + neutrino + 2 jets at 8 TeV
+Luminosity_fb: 20.2
+NeedCrossSection: yes
+Beams: [p+, p+]
+Energies: [8000]
+PtCuts: [30.,30.,25.]
+Description:
+ 'Measurements of the electroweak production of a $W$ boson in association with two jets at high dijet invariant mass
+ are performed using $\sqrt{s} = 7$ and 8 TeV proton-proton collision data produced by the Large Hadron Collider,
+ corresponding respectively to 4.7 and 20.2 fb$^{-1}$ of integrated luminosity collected by the ATLAS detector.
+ The measurements are sensitive to the production of a $W$ boson via a triple-gauge-boson vertex and include both
+ the fiducial and differential cross sections of the electroweak process.'
+BibKey: Aaboud:2017fye
+BibTex: '@article{Aaboud:2017fye,
+ author = "Aaboud, Morad and others",
+ title = "{Measurements of electroweak $Wjj$ production and
+ constraints on anomalous gauge couplings with the ATLAS
+ detector}",
+ collaboration = "ATLAS",
+ journal = "Eur. Phys. J.",
+ volume = "C77",
+ year = "2017",
+ number = "7",
+ pages = "474",
+ doi = "10.1140/epjc/s10052-017-5007-2",
+ eprint = "1703.04362",
+ archivePrefix = "arXiv",
+ primaryClass = "hep-ex",
+ reportNumber = "CERN-EP-2017-008",
+ SLACcitation = "%%CITATION = ARXIV:1703.04362;%%"
+}'
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1517194_EL.plot b/analyses/pluginATLAS/ATLAS_2017_I1517194_EL.plot
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2017_I1517194_EL.plot
@@ -0,0 +1,898 @@
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d..
+RatioPlotYMax=2.0
+RatioPlotYMin=0.0
+LegendAlign=r
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d11-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d12-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d13-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d14-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d15-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d16-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d17-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d18-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d19-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d20-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d21-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d22-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d23-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d24-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d25-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d26-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d27-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d28-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d29-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d30-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d31-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d32-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d33-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d34-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d35-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d36-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d37-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d38-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d39-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d40-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d41-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d42-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d43-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d44-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d45-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d46-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d47-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d48-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d49-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d50-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d51-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d52-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d53-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d54-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d55-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d56-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d57-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d58-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d59-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d60-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d61-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d62-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d63-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d64-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d65-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d66-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d67-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d68-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d69-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d70-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d71-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d72-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d73-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d74-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d75-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d76-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d77-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d78-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d79-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d80-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d81-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d82-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d83-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d84-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d85-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d86-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d87-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d88-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d89-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d90-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d91-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d92-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d93-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d94-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d95-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d96-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d97-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d98-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d99-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d100-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d101-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d102-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d103-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d104-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d105-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d106-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d107-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d108-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d109-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d110-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d111-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d112-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d113-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d114-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d115-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d116-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d117-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d118-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d119-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d120-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d121-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d122-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d123-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d124-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d125-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d126-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d127-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d128-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d129-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d130-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d131-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d132-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d133-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d134-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d135-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d136-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d137-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d138-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d139-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d140-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d141-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d142-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d143-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d144-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d145-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d146-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d147-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d148-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_EL/d149-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to e\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1517194_EL.yoda b/analyses/pluginATLAS/ATLAS_2017_I1517194_EL.yoda
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2017_I1517194_EL.yoda
@@ -0,0 +1,8081 @@
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d01-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d01-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.600000e+01 5.000000e+00 5.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d01-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d01-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.300000e+01 5.000000e+00 5.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d01-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d01-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.000000e+01 8.000000e+00 8.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d01-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d01-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.900000e+01 5.000000e-01 5.000000e-01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d02-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d02-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t2
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.450000e+02 3.900000e+01 3.900000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d02-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d02-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t2
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.550000e+02 5.100000e+01 5.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d03-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d03-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+9.600000e+01 8.000000e+00 8.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d03-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d03-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+8.900000e+01 7.000000e+00 7.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d03-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d03-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.300000e+01 1.100000e+01 1.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d03-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d03-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.100000e+01 1.000000e+00 1.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d04-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d04-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.630000e+02 2.100000e+01 2.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d04-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d04-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.340000e+02 2.600000e+01 2.600000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d04-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d04-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+6.400000e+01 3.600000e+01 3.600000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d04-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d04-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.200000e+01 1.000000e+00 1.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d05-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d05-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t5
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.700000e+03 1.100000e+02 1.100000e+02
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d05-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d05-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t5
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.420000e+03 1.500000e+02 1.500000e+02
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d06-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d06-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.300000e+01 2.000000e+00 2.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d06-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d06-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.400000e+01 1.000000e+00 1.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d06-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d06-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.600000e+00 2.100000e+00 2.100000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d06-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d06-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+6.900000e+00 2.000000e-01 2.000000e-01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d07-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d07-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t7
+Type: Scatter1D
+---
+# xval xerr- xerr+
+3.130000e+02 3.000000e+01 3.000000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d07-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d07-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t7
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.650000e+02 3.200000e+01 3.200000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d08-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d08-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t8
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.920000e+02 3.600000e+01 3.600000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d08-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d08-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t8
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.350000e+02 2.800000e+01 2.800000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d09-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d09-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t9
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.440000e+02 3.502856e+01 3.502856e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d09-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d09-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t9
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.440000e+02 1.100000e+01 1.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d10-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d10-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.460000e+02 3.500000e+01 3.500000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d10-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d10-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.650000e+02 3.900000e+01 3.900000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d10-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d10-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.590000e+02 2.700000e+01 2.700000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_EL/d10-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d10-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.980000e+02 1.200000e+01 1.200000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d11-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d11-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t11
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.749800e-03 4.232811e-04 4.287836e-04
+7.500000e+01 2.500000e+01 2.500000e+01 6.616100e-03 3.022254e-04 3.100313e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.693800e-03 2.513928e-04 2.465816e-04
+1.925000e+02 3.250000e+01 3.250000e+01 1.981800e-03 1.724307e-04 1.687993e-04
+2.625000e+02 3.750000e+01 3.750000e+01 8.348400e-04 3.433320e-04 3.434536e-04
+3.975000e+02 9.750000e+01 9.750000e+01 7.549200e-05 6.703945e-04 6.703707e-04
+6.975000e+02 2.025000e+02 2.025000e+02 9.695400e-06 7.108535e-06 7.150889e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d11-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d11-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t11
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.239800e-03 1.671900e-04 1.537800e-04
+7.500000e+01 2.500000e+01 2.500000e+01 5.782700e-03 3.074600e-04 1.785100e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.876600e-03 1.339900e-04 1.442600e-04
+1.925000e+02 3.250000e+01 3.250000e+01 2.098800e-03 8.731500e-05 1.083800e-04
+2.625000e+02 3.750000e+01 3.750000e+01 9.471300e-04 6.157900e-05 6.167300e-05
+3.975000e+02 9.750000e+01 9.750000e+01 2.586000e-04 1.886600e-05 1.904300e-05
+6.975000e+02 2.025000e+02 2.025000e+02 2.074400e-05 3.918100e-06 3.685900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d11-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d11-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t11
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.484800e-03 3.184600e-04 8.493000e-05
+7.500000e+01 2.500000e+01 2.500000e+01 5.866100e-03 3.147500e-05 2.220000e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.747800e-03 1.022400e-04 4.123400e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.962700e-03 5.974100e-05 2.347300e-04
+2.625000e+02 3.750000e+01 3.750000e+01 9.212000e-04 3.596300e-05 2.579900e-05
+3.975000e+02 9.750000e+01 9.750000e+01 2.621700e-04 1.833200e-05 1.460400e-05
+6.975000e+02 2.025000e+02 2.025000e+02 2.420000e-05 1.322200e-06 1.930400e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d12-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d12-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t12
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 9.751100e-02 3.977561e-02 4.084700e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.765900e-01 5.286942e-02 5.808940e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.206100e+00 1.194382e-01 1.181789e-01
+8.500000e-01 5.000000e-02 5.000000e-02 2.246600e+00 1.386490e-01 1.371997e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.370700e+00 2.434256e-01 2.357765e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.842400e+00 3.555396e-01 3.616982e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d12-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d12-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t12
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 1.590100e-01 8.723300e-03 1.304800e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.869100e-01 2.390800e-02 4.090400e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.207900e+00 1.359500e-01 5.919100e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.344600e+00 9.678800e-02 7.534300e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.009600e+00 1.747300e-01 1.377000e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.347600e+00 2.075000e-01 1.826800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d12-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d12-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t12
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 1.335100e-01 4.507200e-03 1.568300e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.138700e-01 1.995400e-02 0.000000e+00
+7.500000e-01 5.000000e-02 5.000000e-02 1.068000e+00 4.893100e-02 9.925600e-03
+8.500000e-01 5.000000e-02 5.000000e-02 2.306300e+00 4.182800e-02 5.384700e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.241400e+00 1.185300e-01 1.532600e-01
+9.750000e-01 2.500000e-02 2.500000e-02 6.019500e+00 5.855200e-02 1.348000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d13-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d13-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t13
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.338100e-02 1.322149e-02 1.110759e-02
+3.200000e+00 4.000000e-01 4.000000e-01 1.236800e-01 1.453089e-02 1.377971e-02
+4.000000e+00 4.000000e-01 4.000000e-01 2.349200e-01 2.236358e-02 2.037699e-02
+4.800000e+00 4.000000e-01 4.000000e-01 2.834600e-01 3.255250e-02 3.248636e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.637300e-01 1.988253e-02 2.680273e-02
+7.400000e+00 1.400000e+00 1.400000e+00 4.309500e-02 9.407138e-03 8.677072e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d13-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d13-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t13
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 8.621500e-02 5.062100e-03 5.536000e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.400100e-01 7.046500e-03 6.643900e-03
+4.000000e+00 4.000000e-01 4.000000e-01 2.166400e-01 8.359100e-03 9.630700e-03
+4.800000e+00 4.000000e-01 4.000000e-01 3.167200e-01 1.178000e-02 1.072300e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.420800e-01 1.576300e-02 1.181000e-02
+7.400000e+00 1.400000e+00 1.400000e+00 4.237900e-02 4.155600e-03 2.035000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d13-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d13-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t13
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.090400e-01 4.823400e-03 1.074600e-02
+3.200000e+00 4.000000e-01 4.000000e-01 1.739800e-01 6.866900e-03 7.563000e-03
+4.000000e+00 4.000000e-01 4.000000e-01 2.314000e-01 1.125200e-03 7.648700e-03
+4.800000e+00 4.000000e-01 4.000000e-01 2.958200e-01 5.396400e-03 1.608000e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.899700e-01 5.055600e-03 1.239900e-02
+7.400000e+00 1.400000e+00 1.400000e+00 4.279600e-02 5.418600e-03 2.819200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d14-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d14-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t14
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.211900e-03 9.080313e-04 1.006137e-03
+1.400000e+02 2.500000e+01 2.500000e+01 4.935800e-03 2.966745e-04 2.758397e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.289800e-03 2.412451e-04 2.491068e-04
+2.500000e+02 3.000000e+01 3.000000e+01 2.146000e-03 2.152008e-04 2.015250e-04
+3.150000e+02 3.500000e+01 3.500000e+01 1.223400e-03 3.176380e-04 3.070309e-04
+3.925000e+02 4.250000e+01 4.250000e+01 9.110500e-04 1.164833e-04 1.114131e-04
+5.075000e+02 7.250000e+01 7.250000e+01 4.933900e-04 6.944737e-05 6.261648e-05
+7.300000e+02 1.500000e+02 1.500000e+02 8.824000e-05 2.004914e-05 1.974540e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d14-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d14-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t14
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.313200e-03 3.447100e-04 3.244800e-04
+1.400000e+02 2.500000e+01 2.500000e+01 4.565400e-03 1.476900e-04 1.601200e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.443000e-03 1.423500e-04 1.276700e-04
+2.500000e+02 3.000000e+01 3.000000e+01 2.332100e-03 1.155800e-04 1.053900e-04
+3.150000e+02 3.500000e+01 3.500000e+01 1.532800e-03 8.221700e-05 8.194200e-05
+3.925000e+02 4.250000e+01 4.250000e+01 9.368800e-04 5.091600e-05 5.667400e-05
+5.075000e+02 7.250000e+01 7.250000e+01 5.123200e-04 2.957000e-05 3.837100e-05
+7.300000e+02 1.500000e+02 1.500000e+02 1.008700e-04 9.784700e-06 8.927000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d14-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d14-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t14
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.274200e-03 3.095900e-04 1.827800e-04
+1.400000e+02 2.500000e+01 2.500000e+01 3.896800e-03 7.233700e-05 1.225600e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.224100e-03 8.615000e-05 7.443500e-05
+2.500000e+02 3.000000e+01 3.000000e+01 2.296100e-03 1.045900e-04 0.000000e+00
+3.150000e+02 3.500000e+01 3.500000e+01 1.655500e-03 7.178700e-05 7.007500e-05
+3.925000e+02 4.250000e+01 4.250000e+01 1.085700e-03 3.625200e-05 5.417900e-05
+5.075000e+02 7.250000e+01 7.250000e+01 6.390900e-04 4.034300e-05 3.477800e-05
+7.300000e+02 1.500000e+02 1.500000e+02 1.320800e-04 0.000000e+00 5.523000e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d15-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d15-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t15
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.935900e+00 1.770283e-01 1.752405e-01
+2.500000e-01 1.000000e-01 1.000000e-01 1.570100e+00 1.140556e-01 1.134172e-01
+5.000000e-01 1.500000e-01 1.500000e-01 1.058600e+00 6.660687e-02 6.792790e-02
+8.250000e-01 1.750000e-01 1.750000e-01 1.895200e-01 2.497173e-02 2.547942e-02
+1.500000e+00 5.000000e-01 5.000000e-01 1.168600e-02 3.338337e-03 3.320034e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d15-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d15-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t15
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.810300e+00 1.208200e-01 5.936800e-02
+2.500000e-01 1.000000e-01 1.000000e-01 1.670500e+00 6.907000e-02 6.500500e-02
+5.000000e-01 1.500000e-01 1.500000e-01 1.022200e+00 3.154400e-02 8.198000e-02
+8.250000e-01 1.750000e-01 1.750000e-01 2.131000e-01 1.859700e-02 1.637900e-02
+1.500000e+00 5.000000e-01 5.000000e-01 1.310600e-02 2.038200e-03 2.017800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d15-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d15-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t15
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.783400e+00 4.256400e-02 5.687700e-04
+2.500000e-01 1.000000e-01 1.000000e-01 1.615900e+00 0.000000e+00 6.360500e-02
+5.000000e-01 1.500000e-01 1.500000e-01 1.042200e+00 1.258100e-02 0.000000e+00
+8.250000e-01 1.750000e-01 1.750000e-01 2.307200e-01 2.185600e-02 1.116500e-03
+1.500000e+00 5.000000e-01 5.000000e-01 1.588700e-02 6.493200e-04 1.492400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d16-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d16-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t16
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.632100e+00 8.139210e-02 8.650309e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.839900e+00 9.080709e-02 9.079465e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.151400e+00 1.621326e-01 1.621340e-01
+6.750000e-01 1.250000e-01 1.250000e-01 4.450200e-01 4.802816e-02 4.379319e-02
+9.000000e-01 1.000000e-01 1.000000e-01 8.375700e-02 1.696566e-02 1.654870e-02
+1.100000e+00 1.000000e-01 1.000000e-01 2.444000e-02 8.960275e-03 9.146675e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d16-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d16-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t16
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.641100e+00 5.361500e-02 9.437600e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.834200e+00 6.979500e-02 4.664700e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.258900e+00 6.173500e-02 4.656100e-02
+6.750000e-01 1.250000e-01 1.250000e-01 3.905900e-01 1.993100e-02 2.938600e-02
+9.000000e-01 1.000000e-01 1.000000e-01 7.355400e-02 9.763500e-03 1.101500e-02
+1.100000e+00 1.000000e-01 1.000000e-01 1.878200e-02 4.898400e-03 5.685500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d16-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d16-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t16
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.469100e+00 1.254200e-01 7.854200e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.710900e+00 5.139400e-02 0.000000e+00
+4.750000e-01 7.500000e-02 7.500000e-02 1.444500e+00 4.751000e-02 1.492600e-01
+6.750000e-01 1.250000e-01 1.250000e-01 4.911600e-01 1.906200e-02 2.794500e-02
+9.000000e-01 1.000000e-01 1.000000e-01 9.905700e-02 1.735600e-02 4.798700e-03
+1.100000e+00 1.000000e-01 1.000000e-01 2.372400e-02 6.956100e-04 5.791000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d17-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d17-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t17
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.453100e-01 2.915590e-02 3.067239e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.652800e-01 1.821431e-02 1.778858e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.127600e-01 1.177660e-02 1.213810e-02
+3.000000e+00 5.000000e-01 5.000000e-01 5.119200e-02 1.000771e-02 8.594720e-03
+6.000000e+00 2.500000e+00 2.500000e+00 2.545900e-02 8.098885e-03 7.657466e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d17-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d17-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t17
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.713800e-01 1.753300e-02 2.481000e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.659600e-01 1.415800e-02 1.203300e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.088600e-01 6.584100e-03 7.909100e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.887500e-02 1.007500e-02 3.023800e-03
+6.000000e+00 2.500000e+00 2.500000e+00 1.492000e-02 2.059200e-03 2.499600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d17-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d17-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t17
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.319500e-01 2.661200e-02 1.470700e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.883800e-01 2.408000e-03 1.495100e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.247000e-01 1.134800e-02 1.348000e-02
+3.000000e+00 5.000000e-01 5.000000e-01 4.325500e-02 5.562300e-03 0.000000e+00
+6.000000e+00 2.500000e+00 2.500000e+00 1.171900e-02 0.000000e+00 4.214800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d18-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d18-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.440400e-03 1.444966e-04 1.591914e-04
+5.800000e+02 3.500000e+01 3.500000e+01 3.204600e-03 1.031389e-04 1.037089e-04
+6.550000e+02 4.000000e+01 4.000000e+01 2.167800e-03 5.068799e-05 4.855705e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.470600e-03 5.533391e-05 3.547807e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.771800e-04 3.221458e-05 4.100677e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.087400e-04 2.092369e-05 2.283223e-05
+1.042500e+03 5.750000e+01 5.750000e+01 3.716000e-04 2.189913e-05 1.686269e-05
+1.150000e+03 5.000000e+01 5.000000e+01 2.132600e-04 1.484543e-05 1.327452e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.349800e-04 1.005004e-05 9.475520e-06
+1.425000e+03 7.500000e+01 7.500000e+01 8.606100e-05 7.638507e-06 7.559277e-06
+1.750000e+03 2.500000e+02 2.500000e+02 2.592100e-05 4.816414e-06 4.932878e-06
+2.350000e+03 3.500000e+02 3.500000e+02 4.134000e-06 9.226464e-07 6.248307e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.995900e-07 9.477605e-08 9.183850e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d18-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d18-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.327300e-03 8.959800e-05 6.073900e-05
+5.800000e+02 3.500000e+01 3.500000e+01 3.231200e-03 6.876500e-05 5.383300e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.199600e-03 2.816700e-05 2.209800e-04
+7.400000e+02 4.500000e+01 4.500000e+01 1.458300e-03 4.772800e-05 2.290900e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.367200e-04 2.534400e-05 2.149900e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.019500e-04 1.968300e-05 2.233300e-05
+1.042500e+03 5.750000e+01 5.750000e+01 3.734400e-04 1.441100e-05 9.575900e-06
+1.150000e+03 5.000000e+01 5.000000e+01 2.386900e-04 9.187000e-06 1.263300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.464900e-04 6.239300e-06 5.689100e-06
+1.425000e+03 7.500000e+01 7.500000e+01 8.480900e-05 5.210700e-06 4.098200e-06
+1.750000e+03 2.500000e+02 2.500000e+02 2.961900e-05 1.367000e-06 1.856200e-06
+2.350000e+03 3.500000e+02 3.500000e+02 4.342600e-06 4.945700e-07 4.660800e-07
+3.350000e+03 6.500000e+02 6.500000e+02 2.395100e-07 7.790500e-08 7.294600e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d18-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d18-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.216800e-03 6.697900e-05 5.900400e-05
+5.800000e+02 3.500000e+01 3.500000e+01 3.184000e-03 3.231100e-05 2.809700e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.170600e-03 1.266500e-05 9.978400e-06
+7.400000e+02 4.500000e+01 4.500000e+01 1.446000e-03 6.956800e-06 5.955400e-06
+8.325000e+02 4.750000e+01 4.750000e+01 9.513000e-04 7.448400e-06 8.316700e-06
+9.325000e+02 5.250000e+01 5.250000e+01 6.213000e-04 8.686500e-06 9.835200e-06
+1.042500e+03 5.750000e+01 5.750000e+01 3.894000e-04 7.584600e-06 8.678800e-06
+1.150000e+03 5.000000e+01 5.000000e+01 2.527200e-04 6.468300e-06 7.434000e-06
+1.275000e+03 7.500000e+01 7.500000e+01 1.538600e-04 4.744300e-06 5.490300e-06
+1.425000e+03 7.500000e+01 7.500000e+01 9.608800e-05 4.001700e-06 5.471800e-06
+1.750000e+03 2.500000e+02 2.500000e+02 3.347500e-05 1.720700e-06 2.048000e-06
+2.350000e+03 3.500000e+02 3.500000e+02 4.742900e-06 3.186000e-07 3.818100e-07
+3.350000e+03 6.500000e+02 6.500000e+02 2.798700e-07 2.478700e-08 3.030100e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d18-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d18-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.056200e-03 0.000000e+00 8.612300e-05
+5.800000e+02 3.500000e+01 3.500000e+01 3.039100e-03 0.000000e+00 9.947800e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.138100e-03 0.000000e+00 6.928600e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.438800e-03 1.350100e-05 7.192600e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.003600e-03 1.038500e-04 0.000000e+00
+9.325000e+02 5.250000e+01 5.250000e+01 6.275600e-04 3.510700e-06 1.274000e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.088800e-04 1.119200e-05 0.000000e+00
+1.150000e+03 5.000000e+01 5.000000e+01 2.760400e-04 1.666400e-05 0.000000e+00
+1.275000e+03 7.500000e+01 7.500000e+01 1.768400e-04 7.752600e-06 1.623600e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.029100e-04 5.546300e-06 6.072800e-06
+1.750000e+03 2.500000e+02 2.500000e+02 4.181800e-05 2.889700e-06 2.327600e-06
+2.350000e+03 3.500000e+02 3.500000e+02 6.797600e-06 2.692200e-07 5.952000e-08
+3.350000e+03 6.500000e+02 6.500000e+02 5.375300e-07 1.629000e-07 1.112500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d19-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d19-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.771700e-03 1.665906e-04 1.679781e-04
+3.750000e+01 1.250000e+01 1.250000e+01 9.135000e-03 2.472353e-04 2.857557e-04
+6.250000e+01 1.250000e+01 1.250000e+01 8.020600e-03 3.544786e-04 3.577800e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.862500e-03 1.536794e-04 1.511097e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.882600e-03 1.629814e-04 1.499845e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.400100e-03 1.735127e-04 1.533771e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.470600e-03 1.385143e-04 1.326091e-04
+2.075000e+02 1.750000e+01 1.750000e+01 8.778400e-04 8.351002e-05 7.955276e-05
+2.425000e+02 1.750000e+01 1.750000e+01 5.066500e-04 3.164659e-05 3.288326e-05
+2.800000e+02 2.000000e+01 2.000000e+01 2.900700e-04 2.658457e-05 2.569169e-05
+3.975000e+02 9.750000e+01 9.750000e+01 5.744000e-05 1.314632e-05 1.329779e-05
+6.975000e+02 2.025000e+02 2.025000e+02 3.443700e-06 1.236977e-06 1.347234e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d19-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d19-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.122500e-03 2.377800e-04 8.118200e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.598800e-03 1.612200e-04 1.580800e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.809600e-03 2.112400e-04 9.228700e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.815200e-03 8.969100e-05 1.013400e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.965400e-03 1.058700e-04 6.823300e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.620900e-03 9.381800e-05 6.233500e-05
+1.750000e+02 1.500000e+01 1.500000e+01 1.710900e-03 6.542500e-05 4.296700e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.046900e-03 4.482200e-05 4.096700e-05
+2.425000e+02 1.750000e+01 1.750000e+01 6.156500e-04 3.230400e-05 3.392600e-05
+2.800000e+02 2.000000e+01 2.000000e+01 3.581000e-04 3.086100e-05 1.729900e-05
+3.975000e+02 9.750000e+01 9.750000e+01 9.328500e-05 8.335000e-06 4.098800e-06
+6.975000e+02 2.025000e+02 2.025000e+02 4.269500e-06 8.239300e-07 6.547400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d19-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d19-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.310300e-03 2.135100e-04 1.843000e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.337100e-03 2.183100e-04 1.891500e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.348600e-03 3.977300e-05 2.923400e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.676900e-03 4.768000e-05 4.924400e-05
+1.150000e+02 1.500000e+01 1.500000e+01 3.922900e-03 5.625400e-05 6.831000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.776300e-03 9.436500e-05 1.168300e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.785000e-03 4.319200e-05 5.379400e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.106300e-03 2.750900e-05 3.121600e-05
+2.425000e+02 1.750000e+01 1.750000e+01 6.841300e-04 1.913100e-05 2.118700e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.047100e-04 1.270500e-05 1.404500e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.148100e-04 4.107200e-06 4.443700e-06
+6.975000e+02 2.025000e+02 2.025000e+02 5.954800e-06 2.747900e-07 2.902200e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d19-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d19-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.071800e-03 7.261800e-05 3.997500e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.574000e-03 1.162800e-04 1.328500e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.877600e-03 2.836300e-04 0.000000e+00
+8.750000e+01 1.250000e+01 1.250000e+01 5.778600e-03 0.000000e+00 3.900900e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.934900e-03 4.599900e-05 1.268900e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.758000e-03 2.008100e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 1.716100e-03 2.574700e-05 1.737100e-04
+2.075000e+02 1.750000e+01 1.750000e+01 1.021400e-03 5.501200e-05 7.856900e-06
+2.425000e+02 1.750000e+01 1.750000e+01 5.876200e-04 3.429700e-05 1.182700e-04
+2.800000e+02 2.000000e+01 2.000000e+01 3.370800e-04 2.142500e-05 4.763200e-05
+3.975000e+02 9.750000e+01 9.750000e+01 9.380200e-05 5.579300e-06 0.000000e+00
+6.975000e+02 2.025000e+02 2.025000e+02 5.149500e-06 6.574600e-07 3.153900e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d20-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d20-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 5.940800e-02 1.317334e-02 1.263845e-02
+4.000000e-01 1.000000e-01 1.000000e-01 1.244000e-01 1.711124e-02 1.808593e-02
+5.500000e-01 5.000000e-02 5.000000e-02 2.259900e-01 4.134359e-02 4.101133e-02
+6.250000e-01 2.500000e-02 2.500000e-02 4.310900e-01 3.877452e-02 3.251981e-02
+6.750000e-01 2.500000e-02 2.500000e-02 5.768200e-01 5.031359e-02 4.845475e-02
+7.250000e-01 2.500000e-02 2.500000e-02 8.748100e-01 2.352047e-01 2.342052e-01
+7.750000e-01 2.500000e-02 2.500000e-02 1.431400e+00 6.251322e-02 6.227322e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.119800e+00 6.563713e-02 6.561217e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.058100e+00 7.745330e-02 7.826197e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.346500e+00 1.068673e-01 1.103522e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.855400e+00 1.268200e-01 1.257618e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d20-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d20-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 9.500500e-02 6.065600e-03 4.343500e-03
+4.000000e-01 1.000000e-01 1.000000e-01 1.654000e-01 4.748400e-03 6.766200e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.277500e-01 1.899100e-02 9.461300e-03
+6.250000e-01 2.500000e-02 2.500000e-02 4.855500e-01 2.436800e-02 1.983900e-02
+6.750000e-01 2.500000e-02 2.500000e-02 6.551700e-01 1.910700e-02 3.326800e-02
+7.250000e-01 2.500000e-02 2.500000e-02 9.611200e-01 4.323300e-02 2.289300e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.352500e+00 3.829100e-02 3.698400e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.003300e+00 4.650100e-02 3.551800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.956900e+00 5.402100e-02 5.587800e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.210100e+00 1.088500e-01 6.004500e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.488200e+00 8.542400e-02 2.846700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d20-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d20-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 8.984800e-02 2.468200e-03 2.902100e-03
+4.000000e-01 1.000000e-01 1.000000e-01 1.597600e-01 5.564900e-03 8.136400e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.333800e-01 1.970000e-02 2.483600e-02
+6.250000e-01 2.500000e-02 2.500000e-02 4.330800e-01 8.620600e-03 1.002600e-02
+6.750000e-01 2.500000e-02 2.500000e-02 6.027200e-01 1.105800e-02 1.310500e-02
+7.250000e-01 2.500000e-02 2.500000e-02 8.619600e-01 1.440900e-02 1.685700e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.271200e+00 1.866400e-02 2.118800e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.892200e+00 1.823100e-02 2.035100e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.849000e+00 6.445700e-03 7.303600e-03
+9.250000e-01 2.500000e-02 2.500000e-02 4.276200e+00 4.736100e-02 3.932600e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.968700e+00 1.375600e-01 1.118400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d20-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d20-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 8.741000e-02 6.002900e-03 1.561500e-02
+4.000000e-01 1.000000e-01 1.000000e-01 1.486300e-01 4.625000e-03 1.209200e-03
+5.500000e-01 5.000000e-02 5.000000e-02 2.762100e-01 3.935100e-03 5.499000e-03
+6.250000e-01 2.500000e-02 2.500000e-02 4.486600e-01 3.522900e-02 7.930400e-03
+6.750000e-01 2.500000e-02 2.500000e-02 5.925600e-01 0.000000e+00 1.334800e-01
+7.250000e-01 2.500000e-02 2.500000e-02 8.671400e-01 0.000000e+00 1.883000e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.264500e+00 6.197300e-03 4.311500e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.012700e+00 6.342200e-02 2.327800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.917200e+00 0.000000e+00 1.106500e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.405900e+00 1.372300e-01 0.000000e+00
+9.750000e-01 2.500000e-02 2.500000e-02 5.819800e+00 9.804100e-02 1.199400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d21-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d21-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.834100e-01 1.560863e-02 1.265172e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.103900e-01 1.438733e-02 1.483056e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.598600e-01 1.295458e-02 1.378529e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.673400e-01 1.262829e-02 1.272665e-02
+3.800000e+00 2.000000e-01 2.000000e-01 3.823200e-01 1.468431e-02 1.540477e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.273400e-01 2.903756e-02 2.956039e-02
+4.800000e+00 4.000000e-01 4.000000e-01 7.306600e-02 6.444668e-03 6.944151e-03
+5.800000e+00 6.000000e-01 6.000000e-01 7.564100e-03 2.980279e-03 1.409301e-03
+7.600000e+00 1.200000e+00 1.200000e+00 8.444000e-05 6.368777e-05 5.526415e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d21-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d21-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.697300e-01 1.330300e-02 1.034100e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.125800e-01 1.158500e-02 7.799200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.543400e-01 5.982800e-03 3.940900e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.674200e-01 1.099300e-02 5.939900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.947200e-01 5.186900e-03 7.095400e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.183000e-01 1.605500e-02 4.775000e-03
+4.800000e+00 4.000000e-01 4.000000e-01 7.827300e-02 3.313300e-03 2.017700e-03
+5.800000e+00 6.000000e-01 6.000000e-01 8.711800e-03 4.518600e-04 1.131500e-03
+7.600000e+00 1.200000e+00 1.200000e+00 3.968100e-05 2.123100e-05 4.692500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d21-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d21-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.697300e-01 6.193400e-03 6.375700e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.745000e-01 3.701800e-03 3.341900e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.631500e-01 1.789100e-03 1.517200e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.399400e-01 1.249100e-03 1.873000e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.343600e-01 5.382700e-03 4.828000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 1.775400e-01 2.925800e-03 2.870600e-03
+4.800000e+00 4.000000e-01 4.000000e-01 5.926700e-02 1.611700e-03 1.896800e-03
+5.800000e+00 6.000000e-01 6.000000e-01 7.319000e-03 4.508800e-04 5.522900e-04
+7.600000e+00 1.200000e+00 1.200000e+00 4.830200e-05 4.906100e-06 6.252100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d21-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d21-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.098700e-01 2.573700e-03 1.575600e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.439500e-01 3.798600e-03 2.151100e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.848900e-01 2.224400e-02 0.000000e+00
+3.400000e+00 2.000000e-01 2.000000e-01 4.566900e-01 1.668100e-03 4.104700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.514800e-01 7.027200e-04 2.169200e-02
+4.200000e+00 2.000000e-01 2.000000e-01 1.866400e-01 3.426200e-03 1.624400e-03
+4.800000e+00 4.000000e-01 4.000000e-01 6.674700e-02 2.036000e-03 0.000000e+00
+5.800000e+00 6.000000e-01 6.000000e-01 1.068200e-02 7.713500e-04 1.641900e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.578200e-04 3.405200e-05 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d22-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d22-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.388000e-03 4.975407e-04 5.599362e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.018200e-03 2.580735e-04 2.767615e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.820600e-03 1.941004e-04 2.077425e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.299200e-03 1.483642e-04 1.483644e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.304900e-03 1.654952e-04 1.606496e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.745100e-03 1.369758e-04 1.374536e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.431500e-03 9.879302e-05 9.193812e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.526100e-03 7.596880e-05 6.456659e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.702500e-04 4.695736e-05 5.217334e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.443200e-04 6.360786e-05 6.124815e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.943800e-04 2.632154e-05 2.572892e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.496300e-04 1.730628e-05 1.676646e-05
+4.575000e+02 2.250000e+01 2.250000e+01 8.145300e-05 1.175250e-05 1.107143e-05
+5.300000e+02 5.000000e+01 5.000000e+01 2.625100e-05 5.547672e-06 5.448345e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.068100e-05 2.657746e-06 2.575246e-06
+8.425000e+02 1.575000e+02 1.575000e+02 5.869200e-07 4.266142e-07 4.151498e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d22-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d22-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.915000e-03 4.964300e-04 1.112100e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.875800e-03 1.244800e-04 1.396700e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.883500e-03 1.008100e-04 6.921800e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.328100e-03 1.103000e-04 1.083300e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.349300e-03 1.493200e-04 1.086200e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.825900e-03 1.552300e-04 6.192000e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.425600e-03 6.284200e-05 7.292800e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.498300e-03 8.801600e-05 4.130800e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.873700e-04 3.762500e-05 4.230300e-05
+3.325000e+02 1.750000e+01 1.750000e+01 5.112700e-04 3.399200e-05 2.095900e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.952300e-04 2.400800e-05 1.614900e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.623100e-04 1.468600e-05 1.149700e-05
+4.575000e+02 2.250000e+01 2.250000e+01 8.975500e-05 9.267100e-06 7.890200e-06
+5.300000e+02 5.000000e+01 5.000000e+01 3.505200e-05 4.447700e-06 3.988900e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.086900e-05 2.004100e-06 1.758700e-06
+8.425000e+02 1.575000e+02 1.575000e+02 1.546300e-06 4.088400e-07 4.524600e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d22-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d22-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.317500e-03 1.055300e-04 1.081200e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.462000e-03 1.142300e-04 1.047500e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.247500e-03 1.100500e-05 1.534300e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.107400e-03 5.019600e-05 4.071500e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.824200e-03 3.300700e-05 3.122200e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.258700e-03 2.723000e-05 2.975100e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.841300e-03 2.738300e-05 2.780400e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.844500e-03 2.273200e-05 2.267200e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.127000e-03 2.055900e-05 2.169400e-05
+3.325000e+02 1.750000e+01 1.750000e+01 6.913400e-04 1.457200e-05 1.522500e-05
+3.700000e+02 2.000000e+01 2.000000e+01 3.961000e-04 1.201800e-05 1.289300e-05
+4.125000e+02 2.250000e+01 2.250000e+01 2.268900e-04 7.501500e-06 8.057600e-06
+4.575000e+02 2.250000e+01 2.250000e+01 1.283600e-04 3.885000e-06 4.208300e-06
+5.300000e+02 5.000000e+01 5.000000e+01 5.249100e-05 2.199100e-06 2.379700e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.628200e-05 8.408800e-07 9.309900e-07
+8.425000e+02 1.575000e+02 1.575000e+02 2.382200e-06 1.390900e-07 1.542100e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d22-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d22-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.495700e-03 8.486400e-05 1.967500e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.826500e-03 8.422000e-05 2.457500e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.566200e-03 0.000000e+00 1.552100e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.448600e-03 4.563300e-05 1.646200e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.743300e-03 3.242700e-04 8.462000e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.096500e-03 4.776300e-05 1.350700e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.736100e-03 1.944500e-04 0.000000e+00
+2.650000e+02 1.500000e+01 1.500000e+01 1.678700e-03 6.022500e-07 5.423100e-05
+2.975000e+02 1.750000e+01 1.750000e+01 9.884900e-04 0.000000e+00 1.110200e-04
+3.325000e+02 1.750000e+01 1.750000e+01 6.009400e-04 2.521500e-05 3.396300e-07
+3.700000e+02 2.000000e+01 2.000000e+01 3.612900e-04 1.601000e-05 2.103800e-05
+4.125000e+02 2.250000e+01 2.250000e+01 2.155900e-04 3.543600e-05 0.000000e+00
+4.575000e+02 2.250000e+01 2.250000e+01 1.092100e-04 2.428700e-06 4.792000e-06
+5.300000e+02 5.000000e+01 5.000000e+01 4.622000e-05 4.877400e-06 4.323600e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.567800e-05 0.000000e+00 1.910600e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.466200e-06 5.122400e-07 4.625500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d23-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d23-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t23
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.258400e-03 2.478400e-04 2.465506e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.317000e-03 4.732787e-04 4.975421e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.335500e-03 2.929429e-04 2.899776e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.543400e-03 2.794172e-04 2.773066e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.532000e-03 2.552473e-04 2.486133e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.887200e-03 2.285658e-04 2.546337e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.656500e-03 1.536124e-04 1.446930e-04
+2.250000e+02 3.500000e+01 3.500000e+01 9.632900e-04 1.614283e-04 1.612225e-04
+3.775000e+02 1.175000e+02 1.175000e+02 2.131500e-04 2.621424e-05 2.707416e-05
+6.975000e+02 2.025000e+02 2.025000e+02 9.516400e-06 5.034262e-06 5.433003e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d23-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d23-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t23
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.528200e-03 1.405600e-04 1.683900e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.247400e-03 2.281100e-04 3.308900e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.673100e-03 2.222800e-04 2.188800e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.450300e-03 2.732900e-04 1.859700e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.162500e-03 1.765200e-04 1.659600e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.991400e-03 2.047300e-04 1.181500e-04
+1.750000e+02 1.500000e+01 1.500000e+01 2.111500e-03 1.062500e-04 1.279900e-04
+2.250000e+02 3.500000e+01 3.500000e+01 1.188400e-03 5.249100e-05 6.289000e-05
+3.775000e+02 1.175000e+02 1.175000e+02 2.516800e-04 1.395700e-05 1.453300e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.784200e-05 2.873500e-06 2.562100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d23-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d23-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t23
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.482800e-03 0.000000e+00 7.189300e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.102400e-03 2.311000e-04 4.403700e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.712400e-03 9.401500e-05 4.128700e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.438900e-03 2.221700e-04 6.095100e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.079300e-03 3.305300e-05 9.262400e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.988700e-03 1.729900e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 2.095100e-03 2.791900e-05 6.174700e-05
+2.250000e+02 3.500000e+01 3.500000e+01 1.214200e-03 1.386900e-04 0.000000e+00
+3.775000e+02 1.175000e+02 1.175000e+02 2.696700e-04 9.227000e-06 5.146700e-05
+6.975000e+02 2.025000e+02 2.025000e+02 2.057000e-05 1.321200e-06 2.035000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d24-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d24-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t24
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 7.792800e-02 1.833950e-02 2.044247e-02
+5.000000e-01 1.000000e-01 1.000000e-01 2.777000e-01 3.353918e-02 3.287087e-02
+6.500000e-01 5.000000e-02 5.000000e-02 5.535500e-01 1.147128e-01 1.149884e-01
+7.500000e-01 5.000000e-02 5.000000e-02 1.213500e+00 9.393261e-02 8.723704e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.941600e+00 1.238391e-01 1.213781e-01
+8.750000e-01 2.500000e-02 2.500000e-02 3.154000e+00 1.771312e-01 1.804688e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.147900e+00 1.903174e-01 1.964199e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.488100e+00 2.557388e-01 2.468413e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d24-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d24-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t24
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.481400e-01 7.422900e-03 1.018000e-02
+5.000000e-01 1.000000e-01 1.000000e-01 2.978800e-01 1.936400e-02 1.543200e-02
+6.500000e-01 5.000000e-02 5.000000e-02 6.244600e-01 3.123400e-02 4.417800e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.183200e+00 8.480900e-02 4.072400e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.941900e+00 1.156800e-01 8.972900e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.802800e+00 9.223500e-02 1.075400e-01
+9.250000e-01 2.500000e-02 2.500000e-02 3.972600e+00 1.421300e-01 1.463800e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.290700e+00 1.398500e-01 1.998700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d24-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d24-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t24
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.402500e-01 4.252400e-03 5.770500e-03
+5.000000e-01 1.000000e-01 1.000000e-01 2.961400e-01 2.774800e-02 0.000000e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.922800e-01 3.841900e-02 5.191000e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.102700e+00 1.762800e-02 2.989200e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.913100e+00 1.261300e-01 0.000000e+00
+8.750000e-01 2.500000e-02 2.500000e-02 2.759400e+00 0.000000e+00 7.099200e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.061100e+00 9.978600e-02 2.478700e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.569800e+00 3.652600e-03 2.650900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d25-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d25-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t25
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.027700e-01 9.284787e-03 9.227062e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.838100e-01 1.233425e-02 1.257055e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.438500e-01 1.876639e-02 1.754049e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.291500e-01 3.401404e-02 3.406569e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.785700e-01 2.200760e-02 2.200187e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.159900e-01 2.129066e-02 2.405541e-02
+5.400000e+00 2.000000e-01 2.000000e-01 2.788200e-01 1.544991e-02 1.579130e-02
+6.000000e+00 4.000000e-01 4.000000e-01 1.215900e-01 1.367189e-02 1.521664e-02
+7.600000e+00 1.200000e+00 1.200000e+00 6.214200e-03 2.677408e-03 2.737504e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d25-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d25-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t25
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.066400e-02 4.421900e-03 4.128500e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.714600e-01 7.679800e-03 5.540700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.656100e-01 1.087200e-02 1.152200e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.485400e-01 1.454300e-02 1.433000e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.994800e-01 1.183400e-02 2.470300e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.057100e-01 1.219700e-02 1.611700e-02
+5.400000e+00 2.000000e-01 2.000000e-01 2.951700e-01 1.185300e-02 1.213600e-02
+6.000000e+00 4.000000e-01 4.000000e-01 1.098900e-01 1.019300e-02 4.662600e-03
+7.600000e+00 1.200000e+00 1.200000e+00 6.909200e-03 6.352300e-04 1.011000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d25-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d25-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t25
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.076300e-01 3.993700e-03 8.913900e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.962200e-01 9.356800e-03 2.597900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.810500e-01 6.926700e-03 8.369800e-04
+4.200000e+00 2.000000e-01 2.000000e-01 3.349500e-01 4.193800e-04 2.094800e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.700100e-01 1.136200e-02 3.674700e-03
+5.000000e+00 2.000000e-01 2.000000e-01 3.729400e-01 6.101600e-03 3.562200e-02
+5.400000e+00 2.000000e-01 2.000000e-01 2.694300e-01 1.992400e-02 5.923400e-03
+6.000000e+00 4.000000e-01 4.000000e-01 1.083900e-01 3.305500e-03 1.056900e-03
+7.600000e+00 1.200000e+00 1.200000e+00 7.858400e-03 5.538000e-04 1.633700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d26-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d26-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t26
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 7.061400e-03 1.064172e-03 1.166735e-03
+1.050000e+02 1.000000e+01 1.000000e+01 6.470000e-03 3.293624e-04 3.673980e-04
+1.250000e+02 1.000000e+01 1.000000e+01 6.337500e-03 3.588134e-04 3.547634e-04
+1.475000e+02 1.250000e+01 1.250000e+01 5.433300e-03 3.102824e-04 2.928755e-04
+1.725000e+02 1.250000e+01 1.250000e+01 3.797800e-03 2.339298e-04 2.325058e-04
+1.975000e+02 1.250000e+01 1.250000e+01 2.992900e-03 2.077934e-04 2.042392e-04
+2.250000e+02 1.500000e+01 1.500000e+01 2.608500e-03 1.839223e-04 1.741546e-04
+2.575000e+02 1.750000e+01 1.750000e+01 1.702400e-03 3.165812e-04 3.128749e-04
+2.975000e+02 2.250000e+01 2.250000e+01 1.628000e-03 1.310364e-04 1.308917e-04
+3.525000e+02 3.250000e+01 3.250000e+01 9.601900e-04 8.899306e-05 8.566333e-05
+5.350000e+02 1.500000e+02 1.500000e+02 1.960700e-04 1.723922e-05 1.863530e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d26-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d26-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t26
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.578400e-03 5.966600e-04 3.197200e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.212200e-03 2.801000e-04 3.227200e-04
+1.250000e+02 1.000000e+01 1.000000e+01 5.955100e-03 2.508000e-04 4.340100e-04
+1.475000e+02 1.250000e+01 1.250000e+01 5.489000e-03 2.305000e-04 2.332200e-04
+1.725000e+02 1.250000e+01 1.250000e+01 4.288800e-03 1.579800e-04 1.869900e-04
+1.975000e+02 1.250000e+01 1.250000e+01 3.477000e-03 1.483100e-04 1.883500e-04
+2.250000e+02 1.500000e+01 1.500000e+01 2.772200e-03 1.528500e-04 1.139600e-04
+2.575000e+02 1.750000e+01 1.750000e+01 2.035600e-03 1.042500e-04 9.601300e-05
+2.975000e+02 2.250000e+01 2.250000e+01 1.496700e-03 7.260700e-05 7.050600e-05
+3.525000e+02 3.250000e+01 3.250000e+01 9.374200e-04 5.267400e-05 4.572600e-05
+5.350000e+02 1.500000e+02 1.500000e+02 1.963800e-04 1.181100e-05 1.111400e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d26-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d26-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t26
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.831200e-03 4.644500e-04 4.732400e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.519100e-03 1.282800e-04 7.878400e-04
+1.250000e+02 1.000000e+01 1.000000e+01 5.305900e-03 8.813600e-05 0.000000e+00
+1.475000e+02 1.250000e+01 1.250000e+01 5.052000e-03 2.434500e-04 0.000000e+00
+1.725000e+02 1.250000e+01 1.250000e+01 4.294600e-03 4.349200e-06 1.952300e-04
+1.975000e+02 1.250000e+01 1.250000e+01 3.480000e-03 5.434700e-05 1.523500e-04
+2.250000e+02 1.500000e+01 1.500000e+01 2.806800e-03 1.424300e-04 2.433900e-04
+2.575000e+02 1.750000e+01 1.750000e+01 2.143500e-03 5.080400e-05 8.905100e-05
+2.975000e+02 2.250000e+01 2.250000e+01 1.584100e-03 6.944500e-05 2.519100e-06
+3.525000e+02 3.250000e+01 3.250000e+01 1.094700e-03 4.639700e-05 0.000000e+00
+5.350000e+02 1.500000e+02 1.500000e+02 2.456800e-04 1.835600e-05 2.551400e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d27-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d27-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t27
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.257700e-03 1.623662e-04 1.653812e-04
+3.750000e+01 1.250000e+01 1.250000e+01 6.563800e-03 2.487683e-04 2.756686e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.973900e-03 2.053310e-04 2.372230e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.919800e-03 1.744184e-04 1.741189e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.670500e-03 1.955170e-04 1.381912e-04
+1.925000e+02 3.250000e+01 3.250000e+01 1.886200e-03 1.007903e-04 9.622518e-05
+2.425000e+02 1.750000e+01 1.750000e+01 8.675200e-04 1.233013e-04 1.234435e-04
+2.800000e+02 2.000000e+01 2.000000e+01 6.001300e-04 5.349723e-05 5.411056e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.514500e-04 2.874679e-05 2.858273e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.329700e-05 2.901476e-06 3.023483e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d27-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d27-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t27
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.755900e-03 1.017500e-04 7.707800e-05
+3.750000e+01 1.250000e+01 1.250000e+01 6.177100e-03 1.755200e-04 1.251900e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.487600e-03 1.485600e-04 1.361700e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.600100e-03 1.306300e-04 1.369300e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.926100e-03 8.067300e-05 6.140100e-05
+1.925000e+02 3.250000e+01 3.250000e+01 2.004200e-03 4.039700e-05 4.930600e-05
+2.425000e+02 1.750000e+01 1.750000e+01 1.050700e-03 4.280800e-05 4.607100e-05
+2.800000e+02 2.000000e+01 2.000000e+01 6.548500e-04 3.254000e-05 4.616100e-05
+3.975000e+02 9.750000e+01 9.750000e+01 2.038700e-04 9.460900e-06 7.438700e-06
+6.975000e+02 2.025000e+02 2.025000e+02 1.462000e-05 1.617800e-06 1.771000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d27-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d27-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t27
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.744500e-03 0.000000e+00 2.339700e-04
+3.750000e+01 1.250000e+01 1.250000e+01 6.356200e-03 1.458600e-04 2.980300e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.649100e-03 1.653000e-04 3.590900e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.556100e-03 4.738600e-05 1.476900e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.854600e-03 9.694100e-05 1.502500e-06
+1.925000e+02 3.250000e+01 3.250000e+01 1.953600e-03 6.338800e-05 4.010600e-05
+2.425000e+02 1.750000e+01 1.750000e+01 1.029700e-03 4.858100e-05 1.291200e-05
+2.800000e+02 2.000000e+01 2.000000e+01 6.563300e-04 2.005900e-05 7.254200e-06
+3.975000e+02 9.750000e+01 9.750000e+01 2.035700e-04 8.780400e-06 2.288400e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.754000e-05 1.256100e-06 9.459300e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d28-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d28-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t28
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 8.706500e-02 2.170353e-02 2.178045e-02
+3.750000e-01 1.250000e-01 1.250000e-01 1.265700e-01 4.358021e-02 2.914534e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.748600e-01 3.738424e-02 4.124443e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.011700e+00 7.569924e-02 7.551336e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.398700e+00 8.535977e-02 8.444028e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.036100e+00 9.061304e-02 8.999392e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.042100e+00 1.075387e-01 1.036678e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.212000e+00 1.340380e-01 1.617700e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.331700e+00 2.198388e-01 2.293161e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d28-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d28-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t28
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 1.243900e-01 5.131200e-03 1.539400e-02
+3.750000e-01 1.250000e-01 1.250000e-01 2.045100e-01 1.311900e-02 6.579400e-03
+6.000000e-01 1.000000e-01 1.000000e-01 5.148300e-01 1.374800e-02 1.912400e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.030800e+00 3.500500e-02 5.802000e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.446300e+00 8.176300e-02 3.934900e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.991200e+00 5.634400e-02 6.071800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.812400e+00 5.698900e-02 6.058900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.918900e+00 9.251200e-02 6.713300e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.096700e+00 1.557500e-01 8.200400e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d28-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d28-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t28
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 1.046400e-01 3.977000e-03 1.583100e-03
+3.750000e-01 1.250000e-01 1.250000e-01 1.648700e-01 3.159600e-05 7.198300e-03
+6.000000e-01 1.000000e-01 1.000000e-01 4.451500e-01 2.469100e-02 5.824100e-03
+7.250000e-01 2.500000e-02 2.500000e-02 9.015000e-01 1.333400e-02 1.073400e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.353000e+00 0.000000e+00 6.110200e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.031900e+00 1.544200e-01 0.000000e+00
+8.750000e-01 2.500000e-02 2.500000e-02 2.827800e+00 3.145600e-02 9.867400e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.134200e+00 1.714900e-02 8.474300e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.623500e+00 0.000000e+00 1.282500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d29-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d29-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t29
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.430700e-01 1.253435e-02 1.231821e-02
+2.600000e+00 2.000000e-01 2.000000e-01 1.790300e-01 1.345455e-02 1.506671e-02
+3.000000e+00 2.000000e-01 2.000000e-01 1.997600e-01 1.358385e-02 1.421876e-02
+3.400000e+00 2.000000e-01 2.000000e-01 2.630500e-01 1.357823e-02 1.792132e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.858900e-01 1.594253e-02 1.480967e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.386800e-01 1.754336e-02 1.759609e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.687900e-01 1.381005e-02 1.354887e-02
+5.000000e+00 2.000000e-01 2.000000e-01 3.283800e-01 1.920619e-02 2.248360e-02
+5.600000e+00 4.000000e-01 4.000000e-01 1.646500e-01 2.112049e-02 1.518484e-02
+7.400000e+00 1.400000e+00 1.400000e+00 9.151600e-03 2.320183e-03 2.192566e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d29-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d29-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t29
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.280800e-01 4.758900e-03 4.389700e-03
+2.600000e+00 2.000000e-01 2.000000e-01 1.568500e-01 4.937800e-03 4.781300e-03
+3.000000e+00 2.000000e-01 2.000000e-01 1.955100e-01 6.700000e-03 5.085700e-03
+3.400000e+00 2.000000e-01 2.000000e-01 2.413800e-01 5.695000e-03 9.029900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.949700e-01 8.067700e-03 6.334000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 3.452600e-01 6.758400e-03 1.114200e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.761700e-01 7.417700e-03 1.191400e-02
+5.000000e+00 2.000000e-01 2.000000e-01 3.576400e-01 1.030500e-02 8.193400e-03
+5.600000e+00 4.000000e-01 4.000000e-01 1.684000e-01 5.452200e-03 3.752600e-03
+7.400000e+00 1.400000e+00 1.400000e+00 9.619900e-03 9.155800e-04 4.311900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d29-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d29-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t29
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.568600e-01 1.511500e-02 6.459200e-04
+2.600000e+00 2.000000e-01 2.000000e-01 1.910300e-01 8.064500e-04 4.665200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 2.302600e-01 8.200800e-03 1.013200e-02
+3.400000e+00 2.000000e-01 2.000000e-01 2.696500e-01 0.000000e+00 4.731600e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.036400e-01 1.827400e-03 7.172600e-03
+4.200000e+00 2.000000e-01 2.000000e-01 3.307800e-01 6.617800e-03 2.997700e-03
+4.600000e+00 2.000000e-01 2.000000e-01 3.329300e-01 4.209300e-03 2.642500e-03
+5.000000e+00 2.000000e-01 2.000000e-01 3.061800e-01 4.385700e-03 1.351500e-02
+5.600000e+00 4.000000e-01 4.000000e-01 1.529600e-01 3.437700e-03 7.283700e-03
+7.400000e+00 1.400000e+00 1.400000e+00 1.039600e-02 1.316000e-03 8.042500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d30-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d30-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t30
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.704800e-03 5.786448e-04 5.807020e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.227000e-03 6.148538e-04 4.409379e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.355700e-03 2.211034e-04 2.218206e-04
+1.525000e+02 1.250000e+01 1.250000e+01 4.681600e-03 1.876372e-04 1.781726e-04
+1.775000e+02 1.250000e+01 1.250000e+01 3.751700e-03 1.616567e-04 1.639011e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.110000e-03 1.444692e-04 1.560933e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.619900e-03 1.296107e-04 1.426961e-04
+2.650000e+02 1.500000e+01 1.500000e+01 2.080900e-03 1.782366e-04 1.793572e-04
+2.975000e+02 1.750000e+01 1.750000e+01 1.918000e-03 1.083583e-04 1.236735e-04
+3.325000e+02 1.750000e+01 1.750000e+01 1.464200e-03 1.512991e-04 1.650513e-04
+3.700000e+02 2.000000e+01 2.000000e+01 1.158300e-03 7.593764e-05 8.961609e-05
+4.125000e+02 2.250000e+01 2.250000e+01 7.211700e-04 6.090580e-05 5.800696e-05
+4.575000e+02 2.250000e+01 2.250000e+01 4.317400e-04 4.128534e-05 3.979584e-05
+5.300000e+02 5.000000e+01 5.000000e+01 2.047400e-04 2.085416e-05 2.066163e-05
+7.300000e+02 1.500000e+02 1.500000e+02 2.924600e-05 5.181227e-06 5.514166e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d30-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d30-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t30
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.437700e-03 2.230800e-04 2.381700e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.225800e-03 2.767100e-04 1.200700e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.251900e-03 1.201000e-04 2.268100e-04
+1.525000e+02 1.250000e+01 1.250000e+01 4.670800e-03 1.036400e-04 1.991500e-04
+1.775000e+02 1.250000e+01 1.250000e+01 3.984900e-03 9.313200e-05 1.327500e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.343600e-03 9.703100e-05 7.760900e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.721100e-03 7.529100e-05 7.913600e-05
+2.650000e+02 1.500000e+01 1.500000e+01 2.209900e-03 8.930000e-05 6.330600e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.781400e-03 5.228200e-05 6.618200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 1.418800e-03 6.033800e-05 5.262400e-05
+3.700000e+02 2.000000e+01 2.000000e+01 1.045200e-03 4.326200e-05 4.865100e-05
+4.125000e+02 2.250000e+01 2.250000e+01 6.916200e-04 3.261800e-05 2.888700e-05
+4.575000e+02 2.250000e+01 2.250000e+01 4.236500e-04 2.255500e-05 2.370100e-05
+5.300000e+02 5.000000e+01 5.000000e+01 1.947200e-04 1.421700e-05 1.172900e-05
+7.300000e+02 1.500000e+02 1.500000e+02 3.171700e-05 2.949400e-06 2.716600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d30-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d30-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t30
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.211800e-03 3.042300e-04 3.552600e-04
+1.050000e+02 1.000000e+01 1.000000e+01 4.461900e-03 0.000000e+00 4.569800e-04
+1.275000e+02 1.250000e+01 1.250000e+01 4.473100e-03 1.056900e-04 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 4.290300e-03 1.220900e-04 0.000000e+00
+1.775000e+02 1.250000e+01 1.250000e+01 3.976900e-03 5.031500e-05 0.000000e+00
+2.050000e+02 1.500000e+01 1.500000e+01 3.256600e-03 0.000000e+00 1.321200e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.786900e-03 6.025400e-05 0.000000e+00
+2.650000e+02 1.500000e+01 1.500000e+01 2.357500e-03 0.000000e+00 8.507400e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.966600e-03 6.833900e-05 7.402300e-05
+3.325000e+02 1.750000e+01 1.750000e+01 1.672100e-03 4.136400e-05 1.510000e-05
+3.700000e+02 2.000000e+01 2.000000e+01 1.257900e-03 6.745200e-05 0.000000e+00
+4.125000e+02 2.250000e+01 2.250000e+01 8.565200e-04 1.101700e-04 2.713300e-06
+4.575000e+02 2.250000e+01 2.250000e+01 5.077800e-04 2.648200e-06 2.871000e-05
+5.300000e+02 5.000000e+01 5.000000e+01 2.504900e-04 1.100700e-05 2.467000e-05
+7.300000e+02 1.500000e+02 1.500000e+02 4.310800e-05 7.085000e-07 1.368100e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d31-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d31-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t31
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.789000e+00 7.290329e-02 7.287356e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.582600e+00 7.671012e-02 7.482703e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.500900e+00 7.179555e-02 7.216504e-02
+4.500000e-01 1.000000e-01 1.000000e-01 1.106300e+00 6.265183e-02 5.067478e-02
+6.000000e-01 5.000000e-02 5.000000e-02 7.775100e-01 4.661478e-02 4.753280e-02
+7.500000e-01 1.000000e-01 1.000000e-01 3.650300e-01 2.890584e-02 2.938186e-02
+1.025000e+00 1.750000e-01 1.750000e-01 1.114400e-01 9.694101e-03 9.780663e-03
+1.850000e+00 6.500000e-01 6.500000e-01 9.433400e-03 1.232201e-03 1.246403e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d31-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d31-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t31
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.613000e+00 4.421500e-02 2.545300e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.565600e+00 3.100800e-02 4.651200e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.584800e+00 3.716700e-02 5.156000e-02
+4.500000e-01 1.000000e-01 1.000000e-01 1.183700e+00 1.901300e-02 3.285300e-02
+6.000000e-01 5.000000e-02 5.000000e-02 7.755200e-01 2.356900e-02 3.262800e-02
+7.500000e-01 1.000000e-01 1.000000e-01 3.992400e-01 1.308700e-02 1.307100e-02
+1.025000e+00 1.750000e-01 1.750000e-01 1.105900e-01 6.835800e-03 4.705500e-03
+1.850000e+00 6.500000e-01 6.500000e-01 7.813600e-03 6.471200e-04 6.451700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d31-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d31-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t31
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.622400e+00 4.205100e-03 2.895500e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.558300e+00 0.000000e+00 2.982000e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.556800e+00 0.000000e+00 2.726000e-02
+4.500000e-01 1.000000e-01 1.000000e-01 1.158300e+00 1.185900e-02 0.000000e+00
+6.000000e-01 5.000000e-02 5.000000e-02 7.657600e-01 2.603800e-02 1.830100e-03
+7.500000e-01 1.000000e-01 1.000000e-01 4.100700e-01 1.227900e-02 2.983300e-03
+1.025000e+00 1.750000e-01 1.750000e-01 1.244700e-01 8.628700e-03 0.000000e+00
+1.850000e+00 6.500000e-01 6.500000e-01 8.707600e-03 7.867400e-04 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d32-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d32-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t32
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.237200e+00 7.213350e-02 7.015125e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.466400e+00 1.038116e-01 8.555071e-02
+3.250000e-01 7.500000e-02 7.500000e-02 1.649600e+00 4.762733e-02 4.750989e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.427300e+00 5.380471e-02 5.434899e-02
+6.750000e-01 1.250000e-01 1.250000e-01 6.488400e-01 2.961493e-02 3.110388e-02
+9.000000e-01 1.000000e-01 1.000000e-01 1.522100e-01 1.512202e-02 1.526235e-02
+1.750000e+00 7.500000e-01 7.500000e-01 9.076000e-03 1.246709e-03 1.355970e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d32-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d32-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t32
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.287400e+00 3.781000e-02 6.025500e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.477600e+00 5.827900e-02 4.128500e-02
+3.250000e-01 7.500000e-02 7.500000e-02 1.694100e+00 3.660300e-02 2.931100e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.396600e+00 2.933300e-02 3.526100e-02
+6.750000e-01 1.250000e-01 1.250000e-01 6.244600e-01 1.603100e-02 1.809900e-02
+9.000000e-01 1.000000e-01 1.000000e-01 1.460900e-01 1.024100e-02 8.134300e-03
+1.750000e+00 7.500000e-01 7.500000e-01 6.797500e-03 4.949300e-04 6.945100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d32-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d32-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t32
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.192800e+00 6.288400e-02 4.246400e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.397100e+00 7.380800e-02 2.195100e-02
+3.250000e-01 7.500000e-02 7.500000e-02 1.613800e+00 0.000000e+00 2.917300e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.441400e+00 1.179200e-02 5.354800e-02
+6.750000e-01 1.250000e-01 1.250000e-01 7.026000e-01 2.780900e-02 9.095100e-03
+9.000000e-01 1.000000e-01 1.000000e-01 1.771200e-01 1.216100e-02 7.301300e-03
+1.750000e+00 7.500000e-01 7.500000e-01 8.006300e-03 5.803800e-04 5.083400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d33-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d33-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t33
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.393500e-01 2.046922e-02 1.981563e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.923000e-01 1.044840e-02 9.031703e-03
+2.000000e+00 5.000000e-01 5.000000e-01 1.174800e-01 8.355426e-03 9.773928e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.733500e-02 5.198399e-03 5.468499e-03
+6.000000e+00 2.500000e+00 2.500000e+00 1.353500e-02 3.708086e-03 3.370465e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d33-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d33-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t33
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.474800e-01 1.055500e-02 1.394400e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.919700e-01 8.680100e-03 6.940400e-03
+2.000000e+00 5.000000e-01 5.000000e-01 1.117600e-01 4.303400e-03 3.381900e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.529200e-02 2.780700e-03 2.294700e-03
+6.000000e+00 2.500000e+00 2.500000e+00 1.349000e-02 1.089000e-03 1.037400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d33-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d33-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t33
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.228100e-01 2.099700e-02 1.563000e-02
+1.000000e+00 5.000000e-01 5.000000e-01 3.077200e-01 8.596300e-03 1.270600e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.213500e-01 7.037800e-03 6.302600e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.816700e-02 1.169500e-03 1.169800e-03
+6.000000e+00 2.500000e+00 2.500000e+00 9.951600e-03 0.000000e+00 1.158600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d34-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d34-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.737500e-03 1.666680e-04 1.850338e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.921900e-03 6.047142e-05 6.091175e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.124600e-03 2.855445e-05 2.857154e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.472600e-03 2.917853e-05 2.275483e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.000300e-03 2.430507e-05 2.304261e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.689200e-04 2.167312e-05 2.336882e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.484100e-04 1.673976e-05 1.533606e-05
+1.150000e+03 5.000000e+01 5.000000e+01 2.937000e-04 1.499780e-05 1.309657e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.893900e-04 1.337960e-05 1.066005e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.209200e-04 8.375443e-06 1.088039e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.968000e-05 3.780448e-06 4.312506e-06
+2.350000e+03 3.500000e+02 3.500000e+02 8.636700e-06 1.116252e-06 9.972329e-07
+3.350000e+03 6.500000e+02 6.500000e+02 8.821400e-07 2.022031e-07 1.899388e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d34-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d34-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.643700e-03 8.146100e-05 2.662300e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.853800e-03 1.940300e-05 2.587500e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.064700e-03 1.499400e-05 8.612500e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.456700e-03 2.873500e-05 1.187400e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.002000e-03 1.017100e-05 1.075200e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.842000e-04 8.243100e-06 1.212200e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.599900e-04 6.143000e-06 1.678700e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.178400e-04 6.939300e-06 1.238900e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.102500e-04 5.147200e-06 5.221800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.307600e-04 3.959200e-06 3.100100e-06
+1.750000e+03 2.500000e+02 2.500000e+02 5.488200e-05 1.225500e-06 1.150300e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.158000e-05 5.154300e-07 5.177500e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.213000e-06 9.985200e-08 1.359400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d34-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d34-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.618200e-03 6.847200e-05 6.017500e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.849700e-03 3.701800e-05 3.216100e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.052900e-03 1.594100e-05 1.315600e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.458200e-03 1.114000e-06 9.146000e-07
+8.325000e+02 4.750000e+01 4.750000e+01 1.010400e-03 6.761400e-06 7.484600e-06
+9.325000e+02 5.250000e+01 5.250000e+01 6.917300e-04 8.662100e-06 1.000900e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.584500e-04 8.445500e-06 9.649900e-06
+1.150000e+03 5.000000e+01 5.000000e+01 3.190100e-04 7.767700e-06 8.926800e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.119300e-04 6.337300e-06 7.338900e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.337400e-04 5.026900e-06 6.102400e-06
+1.750000e+03 2.500000e+02 2.500000e+02 5.519400e-05 2.702400e-06 3.198300e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.139900e-05 7.966200e-07 9.631000e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.200700e-06 1.172900e-07 1.468400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d34-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d34-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.419400e-03 2.626300e-05 5.177600e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.715500e-03 8.987800e-06 4.218100e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.999800e-03 0.000000e+00 2.834800e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.433200e-03 9.737800e-06 2.960100e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.041500e-03 5.033900e-05 0.000000e+00
+9.325000e+02 5.250000e+01 5.250000e+01 7.136400e-04 2.509100e-07 5.515000e-06
+1.042500e+03 5.750000e+01 5.750000e+01 4.869900e-04 2.471000e-06 7.331000e-06
+1.150000e+03 5.000000e+01 5.000000e+01 3.432200e-04 4.655800e-06 4.298100e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.380700e-04 6.638500e-06 8.833200e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.504600e-04 7.648400e-06 2.034700e-06
+1.750000e+03 2.500000e+02 2.500000e+02 6.552800e-05 2.774300e-06 1.296900e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.399400e-05 5.862100e-07 9.503400e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.561600e-06 1.630900e-07 4.800100e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d35-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d35-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.933500e-03 1.324270e-04 1.319493e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.076500e-03 2.131621e-04 2.487014e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.869700e-03 1.732412e-04 1.825174e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.002900e-03 8.404852e-05 8.337837e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.080100e-03 1.263419e-04 1.181810e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.865600e-03 1.729448e-04 1.439489e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.838500e-03 1.101198e-04 1.039252e-04
+2.075000e+02 1.750000e+01 1.750000e+01 1.080300e-03 5.540438e-05 5.189075e-05
+2.425000e+02 1.750000e+01 1.750000e+01 6.179600e-04 2.886477e-05 3.012354e-05
+2.800000e+02 2.000000e+01 2.000000e+01 3.684100e-04 2.177920e-05 2.205978e-05
+3.975000e+02 9.750000e+01 9.750000e+01 7.096900e-05 9.637562e-06 9.983116e-06
+6.975000e+02 2.025000e+02 2.025000e+02 3.443500e-06 7.049974e-07 7.278381e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d35-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d35-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.378700e-03 1.517600e-04 2.223800e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.469400e-03 5.101500e-05 9.025600e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.440900e-03 8.244400e-05 5.268400e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.978500e-03 5.811300e-05 5.480200e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.359900e-03 4.094500e-05 5.730000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.055200e-03 4.307600e-05 3.026300e-05
+1.750000e+02 1.500000e+01 1.500000e+01 2.039900e-03 2.614000e-05 3.703500e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.260800e-03 2.183900e-05 1.994800e-05
+2.425000e+02 1.750000e+01 1.750000e+01 7.283000e-04 1.380700e-05 2.572100e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.181900e-04 1.488400e-05 1.552900e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.091700e-04 3.234800e-06 3.558500e-06
+6.975000e+02 2.025000e+02 2.025000e+02 5.000600e-06 5.161700e-07 3.977300e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d35-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d35-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.571100e-03 1.697800e-04 1.550400e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.492700e-03 1.936100e-04 1.751200e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.208200e-03 3.438500e-05 2.906200e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.853800e-03 4.013100e-05 4.118000e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.251100e-03 5.415300e-05 6.164000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.028000e-03 6.964700e-05 8.156600e-05
+1.750000e+02 1.500000e+01 1.500000e+01 2.051300e-03 4.503300e-05 5.197900e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.272000e-03 2.845900e-05 3.138100e-05
+2.425000e+02 1.750000e+01 1.750000e+01 7.714900e-04 1.860300e-05 1.992900e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.548600e-04 1.108800e-05 1.158100e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.260500e-04 3.504100e-06 3.557000e-06
+6.975000e+02 2.025000e+02 2.025000e+02 6.537500e-06 2.475100e-07 2.579500e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d35-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d35-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.356900e-03 5.197500e-05 2.060400e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.602500e-03 1.209700e-04 6.166400e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.512700e-03 1.501000e-04 5.842200e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.991900e-03 0.000000e+00 1.600700e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.327700e-03 1.226200e-05 8.728600e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.046000e-03 1.050400e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 1.995200e-03 2.327300e-05 1.004600e-04
+2.075000e+02 1.750000e+01 1.750000e+01 1.202900e-03 4.973400e-05 0.000000e+00
+2.425000e+02 1.750000e+01 1.750000e+01 7.151500e-04 8.055100e-06 1.557800e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.119800e-04 1.447900e-05 2.620800e-06
+3.975000e+02 9.750000e+01 9.750000e+01 1.087000e-04 5.432200e-06 3.744600e-06
+6.975000e+02 2.025000e+02 2.025000e+02 6.240200e-06 5.432900e-07 6.584400e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d36-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d36-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 8.122500e-02 1.352140e-02 1.326180e-02
+2.250000e-01 7.500000e-02 7.500000e-02 1.143700e-01 1.663477e-02 1.142533e-02
+3.500000e-01 5.000000e-02 5.000000e-02 1.271500e-01 1.512681e-02 1.596400e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.161500e-01 1.867401e-02 1.905356e-02
+5.500000e-01 5.000000e-02 5.000000e-02 3.501200e-01 2.792869e-02 2.667234e-02
+6.250000e-01 2.500000e-02 2.500000e-02 5.917600e-01 4.321160e-02 3.926561e-02
+6.750000e-01 2.500000e-02 2.500000e-02 7.344900e-01 4.441159e-02 4.303239e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.009500e+00 6.632819e-02 6.590522e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.519000e+00 3.722584e-02 3.723416e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.206900e+00 3.835284e-02 3.784168e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.029600e+00 5.015113e-02 5.043382e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.928900e+00 7.383253e-02 7.527868e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.006300e+00 9.790021e-02 1.114479e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d36-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d36-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.202300e-01 6.211600e-03 3.741400e-03
+2.250000e-01 7.500000e-02 7.500000e-02 1.409700e-01 3.038600e-03 4.526800e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.901900e-01 4.926700e-03 5.335500e-03
+4.500000e-01 5.000000e-02 5.000000e-02 2.664800e-01 5.314100e-03 8.613400e-03
+5.500000e-01 5.000000e-02 5.000000e-02 4.124900e-01 6.902700e-03 8.398800e-03
+6.250000e-01 2.500000e-02 2.500000e-02 6.083600e-01 1.381700e-02 1.152200e-02
+6.750000e-01 2.500000e-02 2.500000e-02 8.041500e-01 1.701300e-02 1.363700e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.107700e+00 2.066300e-02 1.472900e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.518200e+00 2.071200e-02 1.947000e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.090800e+00 2.068100e-02 2.676800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.869400e+00 2.542300e-02 3.118400e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.800300e+00 3.654600e-02 4.110300e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.679200e+00 7.771600e-02 6.736700e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d36-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d36-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.176200e-01 3.778900e-03 4.656300e-03
+2.250000e-01 7.500000e-02 7.500000e-02 1.375700e-01 4.262000e-03 5.147900e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.808400e-01 6.312800e-03 8.116400e-03
+4.500000e-01 5.000000e-02 5.000000e-02 2.441600e-01 6.809900e-03 8.501300e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.905200e-01 1.402100e-02 1.647000e-02
+6.250000e-01 2.500000e-02 2.500000e-02 5.466100e-01 1.315500e-02 1.498300e-02
+6.750000e-01 2.500000e-02 2.500000e-02 7.337600e-01 1.618400e-02 1.883900e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.016900e+00 2.104600e-02 2.477700e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.422900e+00 2.068500e-02 2.250500e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.009400e+00 1.773700e-02 1.814300e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.840200e+00 4.614300e-03 4.046000e-03
+9.250000e-01 2.500000e-02 2.500000e-02 3.950600e+00 5.492300e-02 4.720000e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.083000e+00 1.370900e-01 1.194200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d36-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d36-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.046500e-01 3.535600e-03 8.375800e-04
+2.250000e-01 7.500000e-02 7.500000e-02 1.217600e-01 2.058000e-03 9.735300e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.587500e-01 4.002300e-03 1.130700e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.222200e-01 5.742900e-04 4.499800e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.518000e-01 1.010000e-02 0.000000e+00
+6.250000e-01 2.500000e-02 2.500000e-02 5.401200e-01 3.005400e-02 2.790100e-03
+6.750000e-01 2.500000e-02 2.500000e-02 7.204000e-01 7.377300e-03 3.319600e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.026600e+00 1.074000e-02 5.218800e-03
+7.750000e-01 2.500000e-02 2.500000e-02 1.454700e+00 3.734400e-03 3.749400e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.097200e+00 2.579900e-02 5.751100e-03
+8.750000e-01 2.500000e-02 2.500000e-02 2.942800e+00 2.987300e-02 2.919000e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.039700e+00 5.567300e-02 0.000000e+00
+9.750000e-01 2.500000e-02 2.500000e-02 5.033700e+00 1.585000e-02 8.495600e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d37-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d37-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.985700e-01 1.264129e-02 1.152023e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.687100e-01 1.111696e-02 1.148468e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.271100e-01 8.868828e-03 1.018768e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.621200e-01 6.921333e-03 7.511135e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.161900e-01 8.640365e-03 8.613727e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.586500e-01 9.151680e-03 8.764364e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.411400e-01 6.786680e-03 7.270510e-03
+5.000000e+00 2.000000e-01 2.000000e-01 6.789800e-02 5.659691e-03 5.623306e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.495100e-02 4.305751e-03 3.045384e-03
+6.200000e+00 2.000000e-01 2.000000e-01 7.071900e-03 1.694080e-03 1.603269e-03
+7.600000e+00 1.200000e+00 1.200000e+00 4.397200e-04 1.957244e-04 1.706019e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d37-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d37-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.926100e-01 3.939500e-03 6.037100e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.558500e-01 3.746400e-03 5.975100e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.221100e-01 6.806300e-03 9.456900e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.601500e-01 3.170700e-03 3.596300e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.175800e-01 3.367500e-03 3.143000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.593300e-01 6.356700e-03 4.381600e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.482900e-01 4.272500e-03 2.168500e-03
+5.000000e+00 2.000000e-01 2.000000e-01 7.739500e-02 1.447900e-03 3.490300e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.780200e-02 8.388300e-04 6.688100e-04
+6.200000e+00 2.000000e-01 2.000000e-01 7.506600e-03 1.106900e-03 4.043100e-04
+7.600000e+00 1.200000e+00 1.200000e+00 5.968300e-04 4.654200e-05 8.824600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d37-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d37-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.591600e-01 3.434700e-03 2.984200e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.005800e-01 2.739500e-03 2.366900e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.335600e-01 2.705100e-03 2.007400e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.421000e-01 1.271900e-03 1.053900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.767300e-01 1.434400e-03 1.638400e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.322300e-01 2.152600e-03 2.474100e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.283400e-01 2.583100e-03 3.185700e-03
+5.000000e+00 2.000000e-01 2.000000e-01 6.750400e-02 2.119900e-03 2.513800e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.488900e-02 1.221100e-03 1.629100e-03
+6.200000e+00 2.000000e-01 2.000000e-01 6.623800e-03 5.518200e-04 8.267500e-04
+7.600000e+00 1.200000e+00 1.200000e+00 5.661000e-04 6.045300e-05 9.118600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d37-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d37-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.276100e-01 5.166600e-03 7.224900e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.853200e-01 0.000000e+00 8.155000e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.378500e-01 1.011300e-02 0.000000e+00
+3.400000e+00 2.000000e-01 2.000000e-01 4.483700e-01 3.856600e-03 2.567700e-04
+3.800000e+00 2.000000e-01 2.000000e-01 3.869000e-01 9.072800e-04 6.262900e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.362700e-01 9.595100e-04 2.763900e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.349000e-01 2.209400e-03 0.000000e+00
+5.000000e+00 2.000000e-01 2.000000e-01 7.258000e-02 3.110800e-03 4.607600e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.837600e-02 1.051000e-03 1.942900e-03
+6.200000e+00 2.000000e-01 2.000000e-01 8.507000e-03 1.396200e-03 6.039000e-05
+7.600000e+00 1.200000e+00 1.200000e+00 8.237200e-04 9.201200e-05 2.161600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d38-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d38-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.869000e-03 3.948115e-04 4.033031e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.557400e-03 2.631596e-04 2.844878e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.069300e-03 1.052295e-04 1.168430e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.146000e-03 1.066799e-04 9.007251e-05
+1.775000e+02 1.250000e+01 1.250000e+01 4.959700e-03 1.182551e-04 1.165410e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.550100e-03 1.126133e-04 1.104288e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.255600e-03 8.168077e-05 7.972379e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.423200e-03 7.170626e-05 6.679290e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.590200e-04 4.767594e-05 4.877268e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.796400e-04 3.442721e-05 3.512253e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.896300e-04 2.504993e-05 2.569215e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.568600e-04 1.225020e-05 1.136216e-05
+4.575000e+02 2.250000e+01 2.250000e+01 9.204500e-05 7.699796e-06 7.206928e-06
+5.300000e+02 5.000000e+01 5.000000e+01 3.546500e-05 3.495101e-06 3.369250e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.072900e-05 2.004789e-06 1.968167e-06
+8.425000e+02 1.575000e+02 1.575000e+02 8.339400e-07 4.776545e-07 4.762887e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d38-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d38-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.436400e-03 2.621100e-04 1.198200e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.304600e-03 1.894900e-04 6.331200e-05
+1.275000e+02 1.250000e+01 1.250000e+01 7.010200e-03 5.837400e-05 2.559000e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.155500e-03 4.948800e-05 6.622200e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.032400e-03 4.417300e-05 6.964200e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.612600e-03 5.412500e-05 4.575400e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.326400e-03 3.693700e-05 4.843900e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.466300e-03 3.766600e-05 3.160500e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.918200e-04 1.844800e-05 2.695900e-05
+3.325000e+02 1.750000e+01 1.750000e+01 5.312500e-04 2.358500e-05 1.471100e-05
+3.700000e+02 2.000000e+01 2.000000e+01 3.085300e-04 1.075600e-05 1.423400e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.734100e-04 6.608300e-06 7.148200e-06
+4.575000e+02 2.250000e+01 2.250000e+01 9.624800e-05 4.621200e-06 5.063100e-06
+5.300000e+02 5.000000e+01 5.000000e+01 4.070400e-05 3.289000e-06 2.511600e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.222500e-05 1.220900e-06 1.126500e-06
+8.425000e+02 1.575000e+02 1.575000e+02 1.957400e-06 3.419400e-07 2.825700e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d38-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d38-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.347700e-03 5.593500e-06 2.125700e-05
+1.050000e+02 1.000000e+01 1.000000e+01 6.296100e-03 3.499600e-05 4.331400e-05
+1.275000e+02 1.250000e+01 1.250000e+01 6.534200e-03 1.621500e-05 1.453300e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.079400e-03 3.335400e-05 2.739200e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.346200e-03 2.403300e-05 2.013900e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.902300e-03 9.939600e-06 9.665200e-06
+2.350000e+02 1.500000e+01 1.500000e+01 2.621200e-03 1.150100e-05 8.529200e-06
+2.650000e+02 1.500000e+01 1.500000e+01 1.716000e-03 1.480300e-05 1.257200e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.045300e-03 1.269800e-05 1.169700e-05
+3.325000e+02 1.750000e+01 1.750000e+01 6.395200e-04 1.039300e-05 9.935800e-06
+3.700000e+02 2.000000e+01 2.000000e+01 3.847600e-04 7.477900e-06 7.646200e-06
+4.125000e+02 2.250000e+01 2.250000e+01 2.229400e-04 5.319300e-06 5.796600e-06
+4.575000e+02 2.250000e+01 2.250000e+01 1.229800e-04 3.147500e-06 3.560300e-06
+5.300000e+02 5.000000e+01 5.000000e+01 5.323500e-05 1.671100e-06 1.865300e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.583700e-05 6.502500e-07 7.454400e-07
+8.425000e+02 1.575000e+02 1.575000e+02 2.440700e-06 1.241700e-07 1.433200e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d38-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d38-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.467600e-03 9.445400e-05 2.360600e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.452300e-03 9.176200e-05 1.273600e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.593500e-03 7.974300e-05 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 6.153400e-03 0.000000e+00 2.644500e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.249700e-03 1.252900e-04 1.048800e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.835600e-03 0.000000e+00 1.197900e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.573000e-03 3.335500e-05 0.000000e+00
+2.650000e+02 1.500000e+01 1.500000e+01 1.645000e-03 2.502300e-05 2.169700e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.016200e-03 6.174200e-06 3.150200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 6.441000e-04 2.990300e-05 0.000000e+00
+3.700000e+02 2.000000e+01 2.000000e+01 3.818400e-04 1.317600e-05 2.005300e-06
+4.125000e+02 2.250000e+01 2.250000e+01 2.231300e-04 1.822100e-05 5.658900e-06
+4.575000e+02 2.250000e+01 2.250000e+01 1.248600e-04 3.624900e-06 7.957200e-07
+5.300000e+02 5.000000e+01 5.000000e+01 5.546100e-05 1.851500e-06 4.965600e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.801100e-05 0.000000e+00 2.178800e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.965100e-06 3.640400e-07 2.030200e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d39-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d39-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.364800e+00 4.846605e-02 4.635862e-02
+1.000000e-01 5.000000e-02 5.000000e-02 1.438400e+00 4.449730e-02 3.998126e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.374900e+00 4.223074e-02 3.748985e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.382400e+00 3.299463e-02 3.453453e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.179700e+00 3.464802e-02 3.301143e-02
+5.000000e-01 5.000000e-02 5.000000e-02 9.105100e-01 2.360182e-02 2.415564e-02
+6.000000e-01 5.000000e-02 5.000000e-02 8.281800e-01 2.391483e-02 2.558667e-02
+7.000000e-01 5.000000e-02 5.000000e-02 6.688400e-01 1.935545e-02 1.916168e-02
+8.000000e-01 5.000000e-02 5.000000e-02 4.460100e-01 1.780996e-02 1.922288e-02
+9.250000e-01 7.500000e-02 7.500000e-02 2.734100e-01 1.195067e-02 1.259264e-02
+1.100000e+00 1.000000e-01 1.000000e-01 1.806200e-01 1.542226e-02 1.597271e-02
+1.350000e+00 1.500000e-01 1.500000e-01 7.597300e-02 4.640969e-03 5.404275e-03
+1.650000e+00 1.500000e-01 1.500000e-01 2.107300e-02 2.790816e-03 2.953377e-03
+2.050000e+00 2.500000e-01 2.500000e-01 4.614500e-03 8.474705e-04 8.540180e-04
+2.650000e+00 3.500000e-01 3.500000e-01 4.433600e-04 1.912842e-04 1.796024e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d39-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d39-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.340000e+00 1.768700e-02 2.039800e-02
+1.000000e-01 5.000000e-02 5.000000e-02 1.348800e+00 1.951700e-02 1.607900e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.373300e+00 1.300200e-02 1.758900e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.418700e+00 2.053200e-02 1.947300e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.240500e+00 1.258900e-02 1.170700e-02
+5.000000e-01 5.000000e-02 5.000000e-02 9.534900e-01 1.867300e-02 1.011800e-02
+6.000000e-01 5.000000e-02 5.000000e-02 8.350400e-01 2.020900e-02 9.484200e-03
+7.000000e-01 5.000000e-02 5.000000e-02 6.629900e-01 8.855300e-03 1.124500e-02
+8.000000e-01 5.000000e-02 5.000000e-02 4.486800e-01 7.802100e-03 6.648800e-02
+9.250000e-01 7.500000e-02 7.500000e-02 2.894800e-01 4.710700e-03 5.610800e-03
+1.100000e+00 1.000000e-01 1.000000e-01 1.616600e-01 5.108400e-03 2.928100e-03
+1.350000e+00 1.500000e-01 1.500000e-01 6.796800e-02 1.961300e-03 1.556300e-03
+1.650000e+00 1.500000e-01 1.500000e-01 2.154800e-02 9.118300e-04 9.585000e-04
+2.050000e+00 2.500000e-01 2.500000e-01 4.198600e-03 3.015200e-04 3.839000e-04
+2.650000e+00 3.500000e-01 3.500000e-01 2.037400e-04 5.669200e-05 5.861100e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d39-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d39-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.246500e+00 1.943300e-02 1.690500e-02
+1.000000e-01 5.000000e-02 5.000000e-02 1.252000e+00 2.007000e-02 1.785800e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.230100e+00 1.813900e-02 1.648500e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.257100e+00 1.764700e-02 1.598900e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.131600e+00 8.899400e-03 8.380200e-03
+5.000000e-01 5.000000e-02 5.000000e-02 9.962500e-01 7.983600e-03 9.595800e-03
+6.000000e-01 5.000000e-02 5.000000e-02 9.622300e-01 1.188700e-02 1.390700e-02
+7.000000e-01 5.000000e-02 5.000000e-02 7.572900e-01 1.006100e-02 1.134000e-02
+8.000000e-01 5.000000e-02 5.000000e-02 5.062100e-01 7.437400e-03 8.474900e-03
+9.250000e-01 7.500000e-02 7.500000e-02 3.514300e-01 8.886100e-03 9.969800e-03
+1.100000e+00 1.000000e-01 1.000000e-01 1.900700e-01 4.264200e-03 4.795900e-03
+1.350000e+00 1.500000e-01 1.500000e-01 8.502200e-02 1.929800e-03 2.018600e-03
+1.650000e+00 1.500000e-01 1.500000e-01 3.127600e-02 1.071000e-03 1.210700e-03
+2.050000e+00 2.500000e-01 2.500000e-01 5.223100e-03 2.560700e-04 2.875000e-04
+2.650000e+00 3.500000e-01 3.500000e-01 2.384800e-04 1.462000e-05 1.728000e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d39-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d39-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.403400e+00 3.298400e-02 0.000000e+00
+1.000000e-01 5.000000e-02 5.000000e-02 1.405200e+00 9.437700e-03 6.334600e-03
+2.000000e-01 5.000000e-02 5.000000e-02 1.413300e+00 1.851100e-02 2.031100e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.442900e+00 9.529100e-03 2.912800e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.225900e+00 1.891800e-02 2.859000e-03
+5.000000e-01 5.000000e-02 5.000000e-02 9.026700e-01 2.250600e-03 1.659600e-02
+6.000000e-01 5.000000e-02 5.000000e-02 7.963500e-01 1.087700e-02 1.878700e-02
+7.000000e-01 5.000000e-02 5.000000e-02 6.531900e-01 8.783100e-03 3.790500e-04
+8.000000e-01 5.000000e-02 5.000000e-02 4.262500e-01 0.000000e+00 1.540600e-02
+9.250000e-01 7.500000e-02 7.500000e-02 2.827300e-01 4.356200e-03 1.214400e-02
+1.100000e+00 1.000000e-01 1.000000e-01 1.580600e-01 3.746200e-03 1.291600e-03
+1.350000e+00 1.500000e-01 1.500000e-01 6.800000e-02 5.665800e-04 5.926800e-04
+1.650000e+00 1.500000e-01 1.500000e-01 2.147300e-02 7.799200e-04 4.937200e-04
+2.050000e+00 2.500000e-01 2.500000e-01 4.536500e-03 2.556900e-04 1.983600e-04
+2.650000e+00 3.500000e-01 3.500000e-01 1.892200e-04 6.747600e-05 6.935500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d40-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d40-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.092100e+00 3.106798e-02 3.155427e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.018500e+00 3.261042e-02 3.275854e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.162800e+00 2.888218e-02 2.932710e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.222600e+00 3.679887e-02 3.686037e-02
+2.250000e-01 2.500000e-02 2.500000e-02 1.265700e+00 4.198133e-02 3.813616e-02
+2.750000e-01 2.500000e-02 2.500000e-02 1.328900e+00 3.557280e-02 3.561967e-02
+3.250000e-01 2.500000e-02 2.500000e-02 1.357500e+00 3.641542e-02 3.624554e-02
+3.750000e-01 2.500000e-02 2.500000e-02 1.438400e+00 3.448402e-02 3.442345e-02
+4.250000e-01 2.500000e-02 2.500000e-02 1.314600e+00 3.158142e-02 3.158311e-02
+4.750000e-01 2.500000e-02 2.500000e-02 1.183600e+00 7.406805e-02 7.448768e-02
+5.250000e-01 2.500000e-02 2.500000e-02 1.161100e+00 3.762767e-02 3.800440e-02
+5.750000e-01 2.500000e-02 2.500000e-02 1.146800e+00 2.485644e-02 2.489803e-02
+6.250000e-01 2.500000e-02 2.500000e-02 1.010200e+00 3.103958e-02 3.050361e-02
+6.750000e-01 2.500000e-02 2.500000e-02 8.781000e-01 2.837291e-02 2.830434e-02
+7.250000e-01 2.500000e-02 2.500000e-02 7.318400e-01 2.162921e-02 2.185104e-02
+7.750000e-01 2.500000e-02 2.500000e-02 5.806800e-01 1.976100e-02 1.904239e-02
+8.250000e-01 2.500000e-02 2.500000e-02 4.710600e-01 1.722081e-02 1.747534e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.768200e-01 1.571927e-02 1.620136e-02
+9.250000e-01 2.500000e-02 2.500000e-02 2.961800e-01 1.371480e-02 1.385615e-02
+9.750000e-01 2.500000e-02 2.500000e-02 2.365800e-01 1.112368e-02 1.115901e-02
+1.025000e+00 2.500000e-02 2.500000e-02 1.879500e-01 1.031368e-02 1.003133e-02
+1.075000e+00 2.500000e-02 2.500000e-02 1.347400e-01 9.133185e-03 9.721705e-03
+1.125000e+00 2.500000e-02 2.500000e-02 1.007700e-01 7.617282e-03 7.873269e-03
+1.175000e+00 2.500000e-02 2.500000e-02 8.877400e-02 6.686759e-03 6.552150e-03
+1.250000e+00 5.000000e-02 5.000000e-02 5.083300e-02 3.534430e-03 3.516280e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.948700e-02 3.063042e-03 3.052132e-03
+1.500000e+00 1.000000e-01 1.000000e-01 1.072400e-02 1.203017e-03 1.201783e-03
+1.800000e+00 2.000000e-01 2.000000e-01 1.276900e-03 2.783425e-04 2.824434e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d40-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d40-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.058900e+00 2.440100e-02 2.870700e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.075000e+00 1.942100e-02 2.793500e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.117900e+00 1.888400e-02 3.722800e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.179800e+00 2.483900e-02 2.786300e-02
+2.250000e-01 2.500000e-02 2.500000e-02 1.265200e+00 3.155300e-02 1.714800e-02
+2.750000e-01 2.500000e-02 2.500000e-02 1.320200e+00 1.923900e-02 2.519200e-02
+3.250000e-01 2.500000e-02 2.500000e-02 1.412000e+00 5.713100e-02 1.568400e-02
+3.750000e-01 2.500000e-02 2.500000e-02 1.425600e+00 1.796800e-02 2.732000e-02
+4.250000e-01 2.500000e-02 2.500000e-02 1.363600e+00 2.205900e-02 1.904700e-02
+4.750000e-01 2.500000e-02 2.500000e-02 1.259300e+00 1.483900e-02 2.001100e-02
+5.250000e-01 2.500000e-02 2.500000e-02 1.189600e+00 1.625400e-02 1.656800e-02
+5.750000e-01 2.500000e-02 2.500000e-02 1.094900e+00 3.942300e-02 1.719900e-02
+6.250000e-01 2.500000e-02 2.500000e-02 1.008100e+00 1.360500e-02 1.420700e-01
+6.750000e-01 2.500000e-02 2.500000e-02 8.684100e-01 1.375800e-02 1.759400e-02
+7.250000e-01 2.500000e-02 2.500000e-02 7.206400e-01 1.408000e-02 1.219100e-02
+7.750000e-01 2.500000e-02 2.500000e-02 5.902600e-01 1.658200e-02 2.223300e-02
+8.250000e-01 2.500000e-02 2.500000e-02 4.710300e-01 9.983400e-03 1.482600e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.751400e-01 1.622500e-02 8.091700e-03
+9.250000e-01 2.500000e-02 2.500000e-02 2.900400e-01 1.133200e-02 9.283800e-03
+9.750000e-01 2.500000e-02 2.500000e-02 2.269700e-01 7.585900e-03 6.801000e-03
+1.025000e+00 2.500000e-02 2.500000e-02 1.741400e-01 7.122100e-03 5.601200e-03
+1.075000e+00 2.500000e-02 2.500000e-02 1.318600e-01 5.705100e-03 6.368000e-03
+1.125000e+00 2.500000e-02 2.500000e-02 9.990000e-02 4.566900e-03 5.090200e-03
+1.175000e+00 2.500000e-02 2.500000e-02 7.347300e-02 4.096900e-03 3.696500e-03
+1.250000e+00 5.000000e-02 5.000000e-02 4.924000e-02 2.277600e-03 2.281000e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.680000e-02 1.847100e-03 1.842600e-03
+1.500000e+00 1.000000e-01 1.000000e-01 1.073400e-02 7.668700e-04 9.794000e-04
+1.800000e+00 2.000000e-01 2.000000e-01 1.628600e-03 1.924300e-04 2.586500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d40-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d40-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.195900e+00 1.283400e-02 1.502300e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.201500e+00 1.065700e-02 1.185500e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.228500e+00 8.872800e-03 1.021600e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.275600e+00 6.065100e-03 6.637200e-03
+2.250000e-01 2.500000e-02 2.500000e-02 1.316900e+00 3.881300e-03 3.238400e-03
+2.750000e-01 2.500000e-02 2.500000e-02 1.352300e+00 2.811600e-03 3.149800e-03
+3.250000e-01 2.500000e-02 2.500000e-02 1.389300e+00 7.209400e-03 6.543600e-03
+3.750000e-01 2.500000e-02 2.500000e-02 1.372700e+00 7.557100e-03 7.226700e-03
+4.250000e-01 2.500000e-02 2.500000e-02 1.330400e+00 4.454500e-03 4.945200e-03
+4.750000e-01 2.500000e-02 2.500000e-02 1.222800e+00 7.781300e-03 6.579500e-03
+5.250000e-01 2.500000e-02 2.500000e-02 1.147500e+00 1.642500e-03 2.115600e-03
+5.750000e-01 2.500000e-02 2.500000e-02 1.035900e+00 5.270800e-03 5.003000e-03
+6.250000e-01 2.500000e-02 2.500000e-02 9.380800e-01 4.431300e-03 3.492500e-03
+6.750000e-01 2.500000e-02 2.500000e-02 8.012500e-01 4.041800e-03 3.306700e-03
+7.250000e-01 2.500000e-02 2.500000e-02 6.717300e-01 4.005300e-03 3.314500e-03
+7.750000e-01 2.500000e-02 2.500000e-02 5.560900e-01 1.436500e-03 1.014300e-03
+8.250000e-01 2.500000e-02 2.500000e-02 4.421000e-01 1.241600e-03 1.476800e-03
+8.750000e-01 2.500000e-02 2.500000e-02 3.563200e-01 1.775000e-03 1.817900e-03
+9.250000e-01 2.500000e-02 2.500000e-02 2.712100e-01 1.717300e-03 1.676500e-03
+9.750000e-01 2.500000e-02 2.500000e-02 2.147400e-01 1.241200e-03 1.471300e-03
+1.025000e+00 2.500000e-02 2.500000e-02 1.687000e-01 9.556200e-04 1.066900e-03
+1.075000e+00 2.500000e-02 2.500000e-02 1.313200e-01 9.833600e-04 1.150200e-03
+1.125000e+00 2.500000e-02 2.500000e-02 9.624500e-02 1.248900e-03 1.222400e-03
+1.175000e+00 2.500000e-02 2.500000e-02 7.322800e-02 1.067000e-03 1.110700e-03
+1.250000e+00 5.000000e-02 5.000000e-02 5.152800e-02 1.965200e-03 2.046800e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.555200e-02 5.289700e-04 5.892700e-04
+1.500000e+00 1.000000e-01 1.000000e-01 1.074700e-02 2.766600e-04 3.018000e-04
+1.800000e+00 2.000000e-01 2.000000e-01 1.577400e-03 9.334100e-05 1.177700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d40-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d40-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.006400e+00 2.651100e-02 4.459400e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.041000e+00 3.138200e-02 1.939700e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.085800e+00 2.771400e-02 4.315800e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.160700e+00 5.162200e-02 2.274600e-02
+2.250000e-01 2.500000e-02 2.500000e-02 1.241700e+00 2.946500e-02 4.578600e-02
+2.750000e-01 2.500000e-02 2.500000e-02 1.324100e+00 1.843700e-02 4.872300e-02
+3.250000e-01 2.500000e-02 2.500000e-02 1.374500e+00 1.193200e-02 1.566200e-02
+3.750000e-01 2.500000e-02 2.500000e-02 1.417800e+00 2.793200e-02 1.814500e-02
+4.250000e-01 2.500000e-02 2.500000e-02 1.368400e+00 1.022300e-02 9.238300e-03
+4.750000e-01 2.500000e-02 2.500000e-02 1.301800e+00 3.150100e-02 9.823400e-03
+5.250000e-01 2.500000e-02 2.500000e-02 1.204000e+00 2.169500e-02 2.649500e-02
+5.750000e-01 2.500000e-02 2.500000e-02 1.133300e+00 1.727300e-02 6.940400e-03
+6.250000e-01 2.500000e-02 2.500000e-02 1.024100e+00 2.797200e-02 3.219000e-02
+6.750000e-01 2.500000e-02 2.500000e-02 8.917100e-01 2.951600e-02 0.000000e+00
+7.250000e-01 2.500000e-02 2.500000e-02 7.427700e-01 4.053500e-02 0.000000e+00
+7.750000e-01 2.500000e-02 2.500000e-02 5.917100e-01 1.901600e-04 3.304800e-02
+8.250000e-01 2.500000e-02 2.500000e-02 4.877000e-01 1.963300e-02 5.870300e-03
+8.750000e-01 2.500000e-02 2.500000e-02 3.724000e-01 5.587000e-03 4.653900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 2.982400e-01 7.696900e-03 1.102500e-02
+9.750000e-01 2.500000e-02 2.500000e-02 2.318500e-01 0.000000e+00 1.112200e-02
+1.025000e+00 2.500000e-02 2.500000e-02 1.790100e-01 1.048900e-02 7.040500e-03
+1.075000e+00 2.500000e-02 2.500000e-02 1.332300e-01 7.665800e-03 4.872400e-03
+1.125000e+00 2.500000e-02 2.500000e-02 1.046500e-01 6.651300e-03 2.049700e-03
+1.175000e+00 2.500000e-02 2.500000e-02 7.552400e-02 0.000000e+00 8.733400e-03
+1.250000e+00 5.000000e-02 5.000000e-02 4.978900e-02 2.021200e-03 2.212300e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.532400e-02 1.114800e-03 2.417500e-03
+1.500000e+00 1.000000e-01 1.000000e-01 1.082000e-02 0.000000e+00 1.249500e-03
+1.800000e+00 2.000000e-01 2.000000e-01 1.752000e-03 1.180000e-04 5.657900e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d41-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d41-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.964000e-01 1.607332e-02 1.717396e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.848500e-01 7.374995e-03 6.654775e-03
+2.000000e+00 5.000000e-01 5.000000e-01 8.968700e-02 6.468044e-03 6.752842e-03
+3.000000e+00 5.000000e-01 5.000000e-01 2.270900e-02 3.138601e-03 2.722886e-03
+4.000000e+00 5.000000e-01 5.000000e-01 4.667900e-03 9.714106e-04 8.115541e-04
+6.500000e+00 2.000000e+00 2.000000e+00 1.683300e-03 4.780830e-04 4.506593e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d41-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d41-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.974500e-01 4.962600e-03 5.161900e-03
+1.000000e+00 5.000000e-01 5.000000e-01 2.853700e-01 3.791500e-03 2.628200e-03
+2.000000e+00 5.000000e-01 5.000000e-01 8.776600e-02 1.671000e-03 1.759900e-03
+3.000000e+00 5.000000e-01 5.000000e-01 2.271300e-02 7.866500e-04 5.123500e-04
+4.000000e+00 5.000000e-01 5.000000e-01 5.262600e-03 2.141000e-04 4.450100e-04
+6.500000e+00 2.000000e+00 2.000000e+00 1.437100e-03 1.139900e-04 1.704700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d41-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d41-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.285200e-01 2.975800e-02 2.687500e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.982700e-01 1.574400e-02 1.691700e-02
+2.000000e+00 5.000000e-01 5.000000e-01 6.750600e-02 7.575200e-03 8.807000e-03
+3.000000e+00 5.000000e-01 5.000000e-01 1.000000e-99 0.000000e+00 0.000000e+00
+4.000000e+00 5.000000e-01 5.000000e-01 1.000000e-99 0.000000e+00 0.000000e+00
+6.500000e+00 2.000000e+00 2.000000e+00 1.000000e-99 0.000000e+00 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d41-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d41-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.807900e-01 1.766100e-02 1.722700e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.978700e-01 1.318500e-02 9.317100e-03
+2.000000e+00 5.000000e-01 5.000000e-01 9.355500e-02 4.131100e-03 6.521300e-03
+3.000000e+00 5.000000e-01 5.000000e-01 2.286700e-02 2.761800e-04 1.435100e-03
+4.000000e+00 5.000000e-01 5.000000e-01 4.111000e-03 0.000000e+00 5.716300e-04
+6.500000e+00 2.000000e+00 2.000000e+00 8.071900e-04 8.568600e-05 7.494700e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d42-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d42-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t42
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.462800e-03 7.499147e-04 7.406124e-04
+7.500000e+01 2.500000e+01 2.500000e+01 7.215300e-03 5.754537e-04 5.787028e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.483700e-03 4.720876e-04 4.692823e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.239800e-03 1.940097e-04 1.965313e-04
+5.150000e+02 2.150000e+02 2.150000e+02 7.642600e-05 4.291271e-05 4.259800e-05
+8.150000e+02 8.500000e+01 8.500000e+01 3.737200e-06 3.442953e-04 3.442747e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d42-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d42-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t42
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.366300e-03 2.815300e-04 3.703300e-04
+7.500000e+01 2.500000e+01 2.500000e+01 5.617000e-03 3.670800e-04 3.587300e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.775800e-03 2.768900e-04 2.412400e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.481900e-03 9.808200e-05 1.029800e-04
+5.150000e+02 2.150000e+02 2.150000e+02 1.524100e-04 1.802100e-05 1.859600e-05
+8.150000e+02 8.500000e+01 8.500000e+01 7.551100e-06 6.318500e-06 6.374200e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d42-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d42-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t42
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.550900e-03 4.657300e-04 2.392800e-04
+7.500000e+01 2.500000e+01 2.500000e+01 5.704000e-03 2.641700e-04 2.175700e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.576100e-03 1.452600e-04 1.765400e-05
+2.300000e+02 7.000000e+01 7.000000e+01 1.457600e-03 7.701300e-05 2.489200e-04
+5.150000e+02 2.150000e+02 2.150000e+02 1.547500e-04 1.172200e-05 3.773100e-06
+8.150000e+02 8.500000e+01 8.500000e+01 1.225900e-05 6.416000e-08 7.997900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d43-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d43-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t43
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.825400e-01 4.804469e-02 5.256234e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.627400e+00 2.142801e-01 2.114021e-01
+9.500000e-01 5.000000e-02 5.000000e-02 5.467400e+00 4.834528e-01 4.842489e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d43-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d43-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t43
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.458000e-01 1.775100e-02 2.787700e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.731500e+00 1.090200e-01 8.821700e-02
+9.500000e-01 5.000000e-02 5.000000e-02 4.816400e+00 2.585600e-01 2.326400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d43-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d43-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t43
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.275600e-01 1.348500e-02 0.000000e+00
+8.000000e-01 1.000000e-01 1.000000e-01 1.633100e+00 1.205100e-01 1.407900e-02
+9.500000e-01 5.000000e-02 5.000000e-02 5.140800e+00 0.000000e+00 3.413200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d44-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d44-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t44
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 8.040500e-02 1.809084e-02 1.855774e-02
+4.400000e+00 8.000000e-01 8.000000e-01 2.001600e-01 2.488998e-02 2.451298e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.495500e-01 4.113629e-02 4.162140e-02
+7.400000e+00 1.400000e+00 1.400000e+00 1.026900e-01 1.709198e-02 1.605860e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d44-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d44-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t44
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 8.200600e-02 7.824900e-03 7.288100e-03
+4.400000e+00 8.000000e-01 8.000000e-01 2.052200e-01 1.095700e-02 1.105700e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.500600e-01 2.387300e-02 1.992000e-02
+7.400000e+00 1.400000e+00 1.400000e+00 9.885600e-02 5.658200e-03 8.310200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d44-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d44-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t44
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.045100e-01 3.400700e-03 3.302800e-02
+4.400000e+00 8.000000e-01 8.000000e-01 2.127100e-01 7.506800e-03 0.000000e+00
+5.600000e+00 4.000000e-01 4.000000e-01 2.870300e-01 4.455300e-03 1.426800e-02
+7.400000e+00 1.400000e+00 1.400000e+00 1.013300e-01 1.218200e-02 7.319700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d45-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d45-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t45
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 5.044100e-03 8.141980e-04 7.683542e-04
+1.800000e+02 4.000000e+01 4.000000e+01 3.701600e-03 3.954643e-04 3.997386e-04
+2.675000e+02 4.750000e+01 4.750000e+01 1.582200e-03 2.584380e-04 2.475394e-04
+3.750000e+02 6.000000e+01 6.000000e+01 1.056700e-03 1.982897e-04 1.946652e-04
+5.600000e+02 1.250000e+02 1.250000e+02 4.964500e-04 9.283398e-05 1.016880e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d45-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d45-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t45
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 4.474700e-03 2.669800e-04 3.519000e-04
+1.800000e+02 4.000000e+01 4.000000e+01 3.799800e-03 2.287400e-04 2.140200e-04
+2.675000e+02 4.750000e+01 4.750000e+01 2.111300e-03 1.472800e-04 1.444400e-04
+3.750000e+02 6.000000e+01 6.000000e+01 1.014500e-03 9.289300e-05 8.840900e-05
+5.600000e+02 1.250000e+02 1.250000e+02 4.208800e-04 4.172900e-05 4.030600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d45-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d45-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t45
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 4.513200e-03 5.134400e-04 4.478600e-04
+1.800000e+02 4.000000e+01 4.000000e+01 3.297000e-03 1.464500e-04 5.099500e-05
+2.675000e+02 4.750000e+01 4.750000e+01 2.072700e-03 1.924800e-04 0.000000e+00
+3.750000e+02 6.000000e+01 6.000000e+01 1.129300e-03 0.000000e+00 1.010000e-04
+5.600000e+02 1.250000e+02 1.250000e+02 5.321100e-04 2.994500e-05 4.663600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d46-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d46-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t46
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.764900e+00 3.425195e-01 3.447472e-01
+7.000000e-01 3.000000e-01 3.000000e-01 4.900900e-01 7.924038e-02 7.482411e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d46-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d46-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t46
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.798700e+00 8.229200e-02 8.746100e-02
+7.000000e-01 3.000000e-01 3.000000e-01 4.675100e-01 4.090200e-02 3.642200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d46-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d46-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t46
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.780100e+00 7.337200e-02 3.594900e-02
+7.000000e-01 3.000000e-01 3.000000e-01 4.799400e-01 2.286300e-02 4.606900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d47-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d47-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t47
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.859400e+00 1.383831e-01 1.371311e-01
+5.250000e-01 1.250000e-01 1.250000e-01 8.648800e-01 1.483110e-01 1.494041e-01
+8.250000e-01 1.750000e-01 1.750000e-01 1.143000e-01 3.684675e-02 3.779701e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d47-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d47-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t47
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.962100e+00 6.646300e-02 7.265300e-02
+5.250000e-01 1.250000e-01 1.250000e-01 7.367100e-01 7.076100e-02 5.149600e-02
+8.250000e-01 1.750000e-01 1.750000e-01 8.849300e-02 1.510200e-02 1.640000e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d47-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d47-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t47
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.787900e+00 7.472700e-02 4.901200e-02
+5.250000e-01 1.250000e-01 1.250000e-01 9.465600e-01 3.179200e-02 1.206000e-01
+8.250000e-01 1.750000e-01 1.750000e-01 1.377400e-01 3.181000e-02 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d48-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d48-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t48
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.259500e-01 4.071903e-02 4.353340e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.331100e-01 2.999246e-02 2.778104e-02
+3.000000e+00 1.500000e+00 1.500000e+00 1.409400e-01 3.220689e-02 3.230973e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d48-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d48-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t48
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.340400e-01 2.770900e-02 2.923400e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.317200e-01 2.357400e-02 1.444500e-02
+3.000000e+00 1.500000e+00 1.500000e+00 1.342300e-01 1.156500e-02 2.024000e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d48-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d48-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t48
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.690500e-01 4.568600e-02 8.327700e-03
+1.000000e+00 5.000000e-01 5.000000e-01 2.610700e-01 1.182600e-03 2.935000e-02
+3.000000e+00 1.500000e+00 1.500000e+00 1.698800e-01 8.419100e-03 2.333900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d49-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d49-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.464200e-03 1.996778e-04 2.113957e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.836000e-03 9.182172e-05 8.486924e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.184800e-03 5.965306e-05 5.928028e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.544600e-03 5.350731e-05 5.426567e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.723800e-04 6.713703e-05 6.666637e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.727900e-04 3.266261e-05 3.194779e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.167100e-04 2.703154e-05 2.736909e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.463200e-04 2.138141e-05 1.994644e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.157300e-04 1.707022e-05 1.933633e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.148800e-04 1.051342e-05 1.244345e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.075600e-05 4.292400e-06 4.616306e-06
+2.350000e+03 3.500000e+02 3.500000e+02 6.020500e-06 1.381048e-06 1.010973e-06
+3.350000e+03 6.500000e+02 6.500000e+02 4.115900e-07 1.815897e-07 1.841067e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d49-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d49-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.362400e-03 1.517800e-04 7.976300e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.763800e-03 4.917600e-05 4.543100e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.078900e-03 3.484700e-05 6.022000e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.516000e-03 4.289100e-05 2.805600e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.084100e-03 3.456400e-05 2.558000e-05
+9.325000e+02 5.250000e+01 5.250000e+01 7.263800e-04 1.870300e-05 2.226500e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.991600e-04 1.424200e-05 4.147700e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.393900e-04 1.345400e-05 3.205200e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.167400e-04 9.725900e-06 8.230800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.307500e-04 1.042800e-05 7.351200e-06
+1.750000e+03 2.500000e+02 2.500000e+02 4.830800e-05 2.449800e-06 2.340000e-06
+2.350000e+03 3.500000e+02 3.500000e+02 7.398900e-06 9.804100e-07 7.028100e-07
+3.350000e+03 6.500000e+02 6.500000e+02 3.216200e-07 1.115200e-07 1.137400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d49-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d49-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.340800e-03 6.275200e-05 5.554000e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.727800e-03 3.754100e-05 3.297400e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.047600e-03 1.641100e-05 1.416700e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.513300e-03 1.884800e-06 1.406900e-06
+8.325000e+02 4.750000e+01 4.750000e+01 1.093600e-03 7.142800e-06 6.258100e-06
+9.325000e+02 5.250000e+01 5.250000e+01 7.536900e-04 7.335400e-06 8.193300e-06
+1.042500e+03 5.750000e+01 5.750000e+01 4.879300e-04 7.938800e-06 8.993600e-06
+1.150000e+03 5.000000e+01 5.000000e+01 3.398100e-04 7.353300e-06 8.376900e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.316000e-04 6.621200e-06 7.595800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.364600e-04 4.720900e-06 5.463900e-06
+1.750000e+03 2.500000e+02 2.500000e+02 4.906600e-05 2.178600e-06 2.539400e-06
+2.350000e+03 3.500000e+02 3.500000e+02 7.462200e-06 4.830600e-07 5.763600e-07
+3.350000e+03 6.500000e+02 6.500000e+02 4.745900e-07 3.978200e-08 4.824000e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d49-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d49-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.076200e-03 2.259800e-05 0.000000e+00
+5.800000e+02 3.500000e+01 3.500000e+01 2.594500e-03 5.505600e-05 2.109200e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.979900e-03 0.000000e+00 5.741600e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.483800e-03 2.652200e-05 1.098100e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.120500e-03 5.984700e-05 0.000000e+00
+9.325000e+02 5.250000e+01 5.250000e+01 7.786500e-04 8.528000e-06 1.625300e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.361400e-04 3.902500e-06 2.148600e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.686100e-04 4.868100e-06 2.126300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.547800e-04 7.683900e-06 9.004900e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.563300e-04 6.102600e-06 4.274000e-06
+1.750000e+03 2.500000e+02 2.500000e+02 6.236300e-05 1.035100e-06 2.966500e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.072300e-05 6.190200e-07 1.829600e-06
+3.350000e+03 6.500000e+02 6.500000e+02 7.258400e-07 6.961000e-08 1.417800e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d50-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d50-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.229500e-03 1.760392e-04 1.805021e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.636300e-03 2.391740e-04 2.509045e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.791700e-03 2.040372e-04 1.978798e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.903100e-03 1.655871e-04 1.657681e-04
+1.450000e+02 1.500000e+01 1.500000e+01 3.430400e-03 2.001677e-04 1.964339e-04
+1.925000e+02 3.250000e+01 3.250000e+01 1.805500e-03 1.314386e-04 1.261339e-04
+2.625000e+02 3.750000e+01 3.750000e+01 6.032300e-04 4.792068e-05 4.885793e-05
+5.150000e+02 2.150000e+02 2.150000e+02 3.539900e-05 1.118806e-05 1.125360e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d50-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d50-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.036300e-03 6.760400e-05 1.112300e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.179700e-03 2.209500e-04 1.171000e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.496100e-03 1.463100e-04 1.102000e-04
+1.150000e+02 1.500000e+01 1.500000e+01 5.046700e-03 1.101200e-04 9.157500e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.600100e-03 7.650000e-05 8.250700e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.899000e-03 3.695100e-05 6.108000e-05
+2.625000e+02 3.750000e+01 3.750000e+01 6.468500e-04 2.218100e-05 2.566600e-05
+5.150000e+02 2.150000e+02 2.150000e+02 5.800200e-05 2.510800e-06 3.390100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d50-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d50-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.334000e-03 5.676300e-05 5.180300e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.387100e-03 7.000000e-05 6.461300e-05
+8.750000e+01 1.250000e+01 1.250000e+01 6.563100e-03 1.731800e-05 1.512600e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.897500e-03 9.733100e-06 1.240000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.383800e-03 4.071700e-05 4.674900e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.772500e-03 2.564800e-05 2.992200e-05
+2.625000e+02 3.750000e+01 3.750000e+01 6.140200e-04 9.495300e-06 9.943300e-06
+5.150000e+02 2.150000e+02 2.150000e+02 5.777400e-05 1.226300e-06 1.374600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d50-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d50-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.381400e-03 1.635300e-04 0.000000e+00
+6.250000e+01 1.250000e+01 1.250000e+01 7.233900e-03 2.045000e-04 8.229600e-05
+8.750000e+01 1.250000e+01 1.250000e+01 6.471800e-03 0.000000e+00 2.897600e-04
+1.150000e+02 1.500000e+01 1.500000e+01 5.026500e-03 0.000000e+00 8.197700e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.461800e-03 8.954200e-06 9.398300e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.777400e-03 1.895000e-05 7.372300e-06
+2.625000e+02 3.750000e+01 3.750000e+01 6.069100e-04 2.572100e-06 2.378200e-05
+5.150000e+02 2.150000e+02 2.150000e+02 5.253100e-05 2.034200e-06 1.387600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d51-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d51-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.021200e-01 1.267664e-02 1.298212e-02
+4.500000e-01 1.500000e-01 1.500000e-01 2.207600e-01 2.769733e-02 2.627560e-02
+6.500000e-01 5.000000e-02 5.000000e-02 7.932300e-01 5.151811e-02 5.025837e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.471100e+00 6.159276e-02 6.083139e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.509000e+00 9.585503e-02 9.570895e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.183200e+00 1.134895e-01 1.150631e-01
+9.250000e-01 2.500000e-02 2.500000e-02 3.752800e+00 1.518879e-01 1.516537e-01
+9.750000e-01 2.500000e-02 2.500000e-02 4.089000e+00 1.543104e-01 1.577002e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d51-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d51-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.220100e-01 4.518900e-03 9.244800e-03
+4.500000e-01 1.500000e-01 1.500000e-01 3.111600e-01 7.224300e-03 1.256900e-02
+6.500000e-01 5.000000e-02 5.000000e-02 8.244500e-01 4.298100e-02 1.962800e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.495500e+00 3.266400e-02 2.800800e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.274100e+00 4.610200e-02 5.724300e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.935100e+00 5.674800e-02 5.324900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.575100e+00 6.514400e-02 6.784100e-02
+9.750000e-01 2.500000e-02 2.500000e-02 3.976700e+00 9.147900e-02 7.812900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d51-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d51-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.156100e-01 4.403700e-03 5.437600e-03
+4.500000e-01 1.500000e-01 1.500000e-01 2.631000e-01 7.411500e-03 8.683900e-03
+6.500000e-01 5.000000e-02 5.000000e-02 7.011700e-01 1.146200e-02 1.265600e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.348100e+00 1.296400e-02 1.444500e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.216700e+00 4.095600e-03 2.309800e-03
+8.750000e-01 2.500000e-02 2.500000e-02 2.999700e+00 2.146300e-02 1.822100e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.891400e+00 4.270000e-02 3.788700e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.521500e+00 7.078200e-02 6.142300e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d51-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d51-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 9.199300e-02 0.000000e+00 6.011700e-03
+4.500000e-01 1.500000e-01 1.500000e-01 2.361700e-01 4.630400e-03 0.000000e+00
+6.500000e-01 5.000000e-02 5.000000e-02 6.701500e-01 7.539200e-03 3.591600e-03
+7.500000e-01 5.000000e-02 5.000000e-02 1.411500e+00 0.000000e+00 4.634900e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.238700e+00 2.544500e-02 3.225400e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.063800e+00 1.115200e-01 0.000000e+00
+9.250000e-01 2.500000e-02 2.500000e-02 3.933400e+00 0.000000e+00 5.605500e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.631700e+00 8.503900e-02 2.714100e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d52-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d52-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.585100e-01 2.518342e-02 2.672197e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.202800e-01 2.460143e-02 2.534064e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.931000e-01 1.687880e-02 1.797093e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.616300e-01 1.809483e-02 1.809607e-02
+4.000000e+00 4.000000e-01 4.000000e-01 2.988300e-01 1.424917e-02 1.217896e-02
+4.800000e+00 4.000000e-01 4.000000e-01 6.914100e-02 8.368347e-03 7.255041e-03
+7.000000e+00 1.800000e+00 1.800000e+00 3.395000e-03 6.473179e-04 8.672093e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d52-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d52-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.378200e-01 6.433500e-03 9.734800e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.044000e-01 8.529400e-03 1.097200e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.542900e-01 1.031700e-02 7.285100e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.611600e-01 7.634000e-03 7.996200e-03
+4.000000e+00 4.000000e-01 4.000000e-01 3.109100e-01 4.790400e-03 9.374000e-03
+4.800000e+00 4.000000e-01 4.000000e-01 9.313200e-02 4.360800e-03 2.659600e-03
+7.000000e+00 1.800000e+00 1.800000e+00 3.804900e-03 4.094000e-04 4.730600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d52-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d52-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.923400e-01 4.908300e-03 3.857800e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.344800e-01 4.387700e-03 3.463600e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.633100e-01 3.133200e-03 2.570600e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.337800e-01 1.285400e-03 1.214900e-03
+4.000000e+00 4.000000e-01 4.000000e-01 2.888900e-01 2.503900e-03 3.145100e-03
+4.800000e+00 4.000000e-01 4.000000e-01 8.277700e-02 2.155300e-03 2.719400e-03
+7.000000e+00 1.800000e+00 1.800000e+00 3.639800e-03 1.792500e-04 2.194100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d52-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d52-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.778100e-01 1.067500e-02 0.000000e+00
+2.600000e+00 2.000000e-01 2.000000e-01 4.312200e-01 0.000000e+00 1.555600e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.550200e-01 6.082600e-03 2.484300e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.389700e-01 1.130300e-02 0.000000e+00
+4.000000e+00 4.000000e-01 4.000000e-01 2.945800e-01 0.000000e+00 7.117200e-03
+4.800000e+00 4.000000e-01 4.000000e-01 8.617900e-02 1.615400e-03 0.000000e+00
+7.000000e+00 1.800000e+00 1.800000e+00 3.939400e-03 1.614400e-04 6.160800e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d53-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d53-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.340500e-03 3.722522e-04 2.395128e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.653100e-03 3.321929e-04 3.467350e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.519100e-03 2.240276e-04 2.436738e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.379400e-03 2.045837e-04 1.978199e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.527800e-03 2.223416e-04 2.251322e-04
+2.050000e+02 1.500000e+01 1.500000e+01 4.385000e-03 1.520537e-04 1.592443e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.670000e-03 1.328195e-04 1.378058e-04
+2.650000e+02 1.500000e+01 1.500000e+01 1.797800e-03 9.739703e-05 1.082551e-04
+3.150000e+02 3.500000e+01 3.500000e+01 8.616300e-04 8.359779e-05 8.738209e-05
+4.150000e+02 6.500000e+01 6.500000e+01 2.206100e-04 4.065504e-05 4.063993e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.216700e-05 5.730018e-06 5.618282e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d53-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d53-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.933000e-03 1.368500e-04 2.093900e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.061200e-03 2.334000e-04 1.518500e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.474500e-03 1.310900e-04 1.112400e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.137900e-03 1.142800e-04 1.156800e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.367000e-03 1.069000e-04 1.124600e-04
+2.050000e+02 1.500000e+01 1.500000e+01 4.026100e-03 9.907300e-05 8.043900e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.707900e-03 6.825300e-05 7.547100e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.767900e-03 6.554700e-05 5.563200e-05
+3.150000e+02 3.500000e+01 3.500000e+01 8.826800e-04 2.512700e-05 3.951400e-05
+4.150000e+02 6.500000e+01 6.500000e+01 2.406000e-04 9.303600e-06 1.188700e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.497400e-05 3.529500e-06 2.836700e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d53-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d53-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.368500e-03 7.678900e-05 1.016000e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.435400e-03 2.930000e-05 3.891400e-05
+1.275000e+02 1.250000e+01 1.250000e+01 6.012000e-03 2.458900e-05 2.809900e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.045600e-03 2.644600e-05 2.375300e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.498800e-03 4.430600e-05 3.706400e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.150100e-03 1.428900e-05 1.241200e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.914500e-03 1.523900e-05 1.148200e-05
+2.650000e+02 1.500000e+01 1.500000e+01 2.062300e-03 1.778200e-05 1.193900e-05
+3.150000e+02 3.500000e+01 3.500000e+01 9.659200e-04 1.178500e-05 9.862800e-06
+4.150000e+02 6.500000e+01 6.500000e+01 2.904800e-04 7.166700e-06 6.459100e-06
+5.825000e+02 1.025000e+02 1.025000e+02 3.739800e-05 1.258600e-06 1.421500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d53-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d53-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.181300e-03 1.496200e-04 6.003400e-05
+1.050000e+02 1.000000e+01 1.000000e+01 5.517600e-03 2.552600e-04 2.778900e-05
+1.275000e+02 1.250000e+01 1.250000e+01 5.899600e-03 8.435000e-05 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 5.839100e-03 6.783400e-05 6.978800e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.382100e-03 0.000000e+00 6.059300e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.166900e-03 0.000000e+00 1.995900e-04
+2.350000e+02 1.500000e+01 1.500000e+01 3.038600e-03 2.376700e-05 1.260300e-04
+2.650000e+02 1.500000e+01 1.500000e+01 1.940100e-03 2.828900e-05 5.446300e-05
+3.150000e+02 3.500000e+01 3.500000e+01 1.071000e-03 6.070700e-05 4.676800e-07
+4.150000e+02 6.500000e+01 6.500000e+01 3.052400e-04 2.268800e-06 8.337000e-06
+5.825000e+02 1.025000e+02 1.025000e+02 4.826200e-05 1.483400e-06 4.029900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d54-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d54-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.128800e-03 2.620050e-04 2.899555e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.649900e-03 1.365857e-04 1.343382e-04
+6.550000e+02 4.000000e+01 4.000000e+01 2.033600e-03 8.972807e-05 9.790188e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.463000e-03 7.369309e-05 6.555212e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.101500e-03 5.937838e-05 4.810172e-05
+9.325000e+02 5.250000e+01 5.250000e+01 7.242700e-04 6.319372e-05 7.426883e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.979900e-04 4.593612e-05 4.442757e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.372000e-04 3.600630e-05 3.230795e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.281200e-04 5.344951e-05 4.520928e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.710500e-04 2.235096e-05 2.038130e-05
+1.750000e+03 2.500000e+02 2.500000e+02 7.781400e-05 9.211709e-06 9.863134e-06
+3.000000e+03 1.000000e+03 1.000000e+03 4.450100e-06 1.035972e-06 1.055269e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d54-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d54-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.866500e-03 6.705400e-05 1.330400e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.419600e-03 4.278100e-05 5.760900e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.936500e-03 5.110200e-05 3.922100e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.480000e-03 3.637000e-05 2.943700e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.099600e-03 3.895100e-05 2.495200e-05
+9.325000e+02 5.250000e+01 5.250000e+01 7.932000e-04 2.155700e-05 2.120500e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.644900e-04 1.652600e-05 3.016000e-05
+1.150000e+03 5.000000e+01 5.000000e+01 4.028700e-04 2.143800e-05 1.508400e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.775000e-04 1.403900e-05 1.108400e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.772200e-04 8.951800e-06 9.651300e-06
+1.750000e+03 2.500000e+02 2.500000e+02 7.868200e-05 5.007200e-06 4.138300e-06
+3.000000e+03 1.000000e+03 1.000000e+03 6.509700e-06 4.254800e-07 4.360400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d54-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d54-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.857900e-03 6.863800e-05 6.031800e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.441400e-03 4.315400e-05 3.749800e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.924000e-03 2.031900e-05 1.742100e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.478200e-03 5.211700e-06 7.140200e-06
+8.325000e+02 4.750000e+01 4.750000e+01 1.116600e-03 4.712300e-06 3.505100e-06
+9.325000e+02 5.250000e+01 5.250000e+01 7.835000e-04 6.910300e-06 7.682700e-06
+1.042500e+03 5.750000e+01 5.750000e+01 5.489300e-04 8.016600e-06 9.075900e-06
+1.150000e+03 5.000000e+01 5.000000e+01 4.138100e-04 8.564600e-06 9.779600e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.804300e-04 7.022500e-06 8.104500e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.783300e-04 5.887600e-06 6.839400e-06
+1.750000e+03 2.500000e+02 2.500000e+02 7.794300e-05 3.586900e-06 4.234800e-06
+3.000000e+03 1.000000e+03 1.000000e+03 6.451900e-06 4.741000e-07 5.792000e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d54-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d54-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.694100e-03 4.588300e-05 1.186700e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.354400e-03 4.103500e-05 1.611100e-04
+6.550000e+02 4.000000e+01 4.000000e+01 1.864400e-03 3.899500e-05 9.574800e-06
+7.400000e+02 4.500000e+01 4.500000e+01 1.430600e-03 3.323100e-05 3.800600e-06
+8.325000e+02 4.750000e+01 4.750000e+01 1.103500e-03 1.491100e-06 4.704400e-05
+9.325000e+02 5.250000e+01 5.250000e+01 8.073400e-04 2.663000e-05 1.539800e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.665400e-04 0.000000e+00 3.498800e-05
+1.150000e+03 5.000000e+01 5.000000e+01 4.249600e-04 1.117400e-05 2.483100e-05
+1.275000e+03 7.500000e+01 7.500000e+01 3.121300e-04 2.072200e-05 5.586200e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.972000e-04 2.960700e-06 1.049200e-05
+1.750000e+03 2.500000e+02 2.500000e+02 9.100700e-05 4.209700e-06 5.599100e-07
+3.000000e+03 1.000000e+03 1.000000e+03 8.448800e-06 1.072300e-08 7.075800e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d55-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d55-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.549200e-03 2.524824e-04 2.841926e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.822300e-03 3.242681e-04 3.557233e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.470500e-03 2.433973e-04 2.439199e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.873900e-03 2.234423e-04 2.149565e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.179600e-03 1.084264e-04 9.723728e-05
+6.000000e+02 3.000000e+02 3.000000e+02 2.939500e-05 9.383853e-06 9.503880e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d55-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d55-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.059300e-03 1.180600e-04 6.540700e-05
+6.250000e+01 1.250000e+01 1.250000e+01 6.935900e-03 1.272000e-04 1.378500e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.167900e-03 1.183700e-04 1.659900e-04
+1.300000e+02 3.000000e+01 3.000000e+01 4.269300e-03 6.474800e-05 7.044300e-05
+2.300000e+02 7.000000e+01 7.000000e+01 1.320200e-03 2.689800e-05 2.864400e-05
+6.000000e+02 3.000000e+02 3.000000e+02 4.741800e-05 2.040700e-06 2.860900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d55-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d55-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.207900e-03 5.427800e-05 4.990900e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.049600e-03 2.618500e-05 2.292100e-05
+8.750000e+01 1.250000e+01 1.250000e+01 6.109500e-03 1.780300e-05 1.398800e-05
+1.300000e+02 3.000000e+01 3.000000e+01 4.136600e-03 2.373800e-05 2.731300e-05
+2.300000e+02 7.000000e+01 7.000000e+01 1.298100e-03 1.135600e-05 1.165400e-05
+6.000000e+02 3.000000e+02 3.000000e+02 5.116500e-05 8.963600e-07 1.009400e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d55-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d55-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.188400e-03 1.320500e-05 2.339400e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.118500e-03 2.043000e-04 0.000000e+00
+8.750000e+01 1.250000e+01 1.250000e+01 6.287900e-03 2.211800e-04 0.000000e+00
+1.300000e+02 3.000000e+01 3.000000e+01 4.151200e-03 0.000000e+00 1.346200e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.267700e-03 4.865800e-05 1.848200e-05
+6.000000e+02 3.000000e+02 3.000000e+02 4.812100e-05 7.884400e-07 1.691700e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d56-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d56-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.514700e-01 3.751747e-02 2.130119e-02
+4.500000e-01 1.500000e-01 1.500000e-01 3.266500e-01 4.156937e-02 4.061237e-02
+6.500000e-01 5.000000e-02 5.000000e-02 8.897000e-01 8.108349e-02 7.509931e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.500600e+00 7.684479e-02 7.875645e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.598000e+00 1.087935e-01 1.104730e-01
+9.500000e-01 5.000000e-02 5.000000e-02 3.577300e+00 1.397788e-01 1.588906e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d56-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d56-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.957800e-01 9.968400e-03 5.864100e-03
+4.500000e-01 1.500000e-01 1.500000e-01 4.135400e-01 1.110700e-02 1.130700e-02
+6.500000e-01 5.000000e-02 5.000000e-02 8.999300e-01 2.371600e-02 2.675100e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.519300e+00 3.362200e-02 3.832600e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.421200e+00 3.580800e-02 3.858400e-02
+9.500000e-01 5.000000e-02 5.000000e-02 3.331600e+00 4.430300e-02 4.442800e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d56-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d56-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.912000e-01 4.280800e-03 5.141900e-03
+4.500000e-01 1.500000e-01 1.500000e-01 3.777800e-01 6.925600e-03 8.243600e-03
+6.500000e-01 5.000000e-02 5.000000e-02 8.328200e-01 1.257400e-02 1.376900e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.467100e+00 1.240800e-02 1.466400e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.454800e+00 1.489600e-02 1.157000e-02
+9.500000e-01 5.000000e-02 5.000000e-02 3.538400e+00 5.431100e-02 4.755200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d56-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d56-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.592800e-01 2.592000e-03 1.464100e-02
+4.500000e-01 1.500000e-01 1.500000e-01 3.326200e-01 4.178100e-04 9.219100e-03
+6.500000e-01 5.000000e-02 5.000000e-02 7.922100e-01 4.346700e-02 1.424800e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.469400e+00 1.632700e-02 4.712500e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.559300e+00 4.775900e-03 2.721300e-02
+9.500000e-01 5.000000e-02 5.000000e-02 3.703400e+00 7.325300e-02 1.936400e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d57-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d57-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.020900e-01 2.337438e-02 2.330605e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.414000e-01 2.128435e-02 2.437171e-02
+3.000000e+00 2.000000e-01 2.000000e-01 3.860900e-01 2.054651e-02 2.264921e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.789700e-01 2.085667e-02 2.428364e-02
+3.800000e+00 2.000000e-01 2.000000e-01 4.331800e-01 1.931064e-02 1.911455e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.794300e-01 1.788684e-02 1.655674e-02
+4.800000e+00 4.000000e-01 4.000000e-01 1.441300e-01 1.360667e-02 1.320912e-02
+5.800000e+00 6.000000e-01 6.000000e-01 2.921000e-02 1.074458e-02 5.853417e-03
+7.600000e+00 1.200000e+00 1.200000e+00 4.910500e-04 3.696222e-04 2.965312e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d57-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d57-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.131800e-01 5.568900e-03 8.317900e-03
+2.600000e+00 2.000000e-01 2.000000e-01 2.933900e-01 6.218800e-03 1.134900e-02
+3.000000e+00 2.000000e-01 2.000000e-01 3.813900e-01 7.088100e-03 1.214800e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.505100e-01 7.703700e-03 9.715100e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.414000e-01 1.342000e-02 7.637000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 3.084400e-01 9.782500e-03 7.649800e-03
+4.800000e+00 4.000000e-01 4.000000e-01 1.544100e-01 9.954000e-03 3.189100e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.264500e-02 3.213400e-03 1.571300e-03
+7.600000e+00 1.200000e+00 1.200000e+00 8.210600e-04 1.343000e-04 1.573100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d57-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d57-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.410400e-01 4.783500e-03 3.724600e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.167900e-01 5.495500e-03 4.349800e-03
+3.000000e+00 2.000000e-01 2.000000e-01 3.915800e-01 4.882400e-03 3.733400e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.489200e-01 4.388700e-03 3.257900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.201900e-01 1.333200e-03 1.091000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.953200e-01 3.791500e-03 5.089900e-03
+4.800000e+00 4.000000e-01 4.000000e-01 1.432200e-01 3.242400e-03 3.960400e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.144700e-02 1.697800e-03 2.257300e-03
+7.600000e+00 1.200000e+00 1.200000e+00 8.951300e-04 1.019200e-04 1.461700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d57-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d57-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.522200e-01 5.291200e-03 3.194300e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.301700e-01 2.314200e-03 0.000000e+00
+3.000000e+00 2.000000e-01 2.000000e-01 3.968800e-01 0.000000e+00 1.996900e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.303700e-01 2.412700e-03 2.741700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.115800e-01 1.410000e-02 9.046400e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.828900e-01 1.086800e-02 2.722400e-03
+4.800000e+00 4.000000e-01 4.000000e-01 1.429200e-01 1.452700e-03 1.802300e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.382500e-02 9.918600e-04 1.378600e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.427900e-03 1.394800e-04 5.183800e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d58-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d58-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.960100e-03 5.601968e-04 4.767125e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.229700e-03 2.698135e-04 2.745017e-04
+1.650000e+02 2.500000e+01 2.500000e+01 5.404000e-03 1.892948e-04 2.011164e-04
+2.200000e+02 3.000000e+01 3.000000e+01 2.541500e-03 1.721515e-04 1.769221e-04
+2.825000e+02 3.250000e+01 3.250000e+01 1.104500e-03 9.399695e-05 9.223029e-05
+3.525000e+02 3.750000e+01 3.750000e+01 3.782300e-04 4.733330e-05 4.776250e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.281800e-04 2.227873e-05 2.203128e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.056800e-05 8.897889e-06 8.752365e-06
+8.425000e+02 1.575000e+02 1.575000e+02 4.757400e-10 2.158605e-05 2.158603e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d58-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d58-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.596100e-03 3.457600e-04 1.069400e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.140900e-03 1.603300e-04 1.319400e-04
+1.650000e+02 2.500000e+01 2.500000e+01 5.310000e-03 7.480800e-05 1.583100e-04
+2.200000e+02 3.000000e+01 3.000000e+01 2.755200e-03 5.001100e-05 8.580900e-05
+2.825000e+02 3.250000e+01 3.250000e+01 1.128300e-03 3.521600e-05 3.907100e-05
+3.525000e+02 3.750000e+01 3.750000e+01 4.258100e-04 2.307300e-05 1.763000e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.404700e-04 9.069100e-06 1.346600e-05
+5.825000e+02 1.025000e+02 1.025000e+02 2.965200e-05 2.811900e-06 2.971000e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.545900e-06 6.840100e-07 6.527900e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d58-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d58-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 6.945400e-03 8.267100e-05 1.108000e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.906400e-03 1.917200e-05 2.013900e-05
+1.650000e+02 2.500000e+01 2.500000e+01 5.440600e-03 3.022500e-05 2.197100e-05
+2.200000e+02 3.000000e+01 3.000000e+01 2.931100e-03 2.904300e-05 2.260200e-05
+2.825000e+02 3.250000e+01 3.250000e+01 1.201200e-03 1.480000e-05 1.198000e-05
+3.525000e+02 3.750000e+01 3.750000e+01 4.618700e-04 6.745900e-06 6.317300e-06
+4.350000e+02 4.500000e+01 4.500000e+01 1.697900e-04 6.088700e-06 5.403400e-06
+5.825000e+02 1.025000e+02 1.025000e+02 3.728700e-05 1.398200e-06 1.137000e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.267000e-06 1.110400e-07 1.279900e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d58-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d58-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 6.721900e-03 2.133300e-05 2.546300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.530400e-03 2.421000e-04 1.258800e-05
+1.650000e+02 2.500000e+01 2.500000e+01 5.359900e-03 6.805600e-05 0.000000e+00
+2.200000e+02 3.000000e+01 3.000000e+01 3.011000e-03 0.000000e+00 1.196600e-04
+2.825000e+02 3.250000e+01 3.250000e+01 1.315600e-03 1.542800e-05 1.985900e-05
+3.525000e+02 3.750000e+01 3.750000e+01 5.297400e-04 4.476400e-05 1.635500e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.952400e-04 2.498500e-05 0.000000e+00
+5.825000e+02 1.025000e+02 1.025000e+02 4.351800e-05 1.402500e-07 2.010700e-06
+8.425000e+02 1.575000e+02 1.575000e+02 3.440100e-06 1.239600e-07 8.070700e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d59-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d59-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.537000e-03 1.772834e-04 1.928197e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.842500e-03 5.819066e-05 6.263716e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.100200e-03 4.681870e-05 4.496857e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.439500e-03 3.619757e-05 3.539646e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.804900e-04 3.805045e-05 3.593377e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.920500e-04 2.436671e-05 2.348867e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.580400e-04 2.311139e-05 2.131238e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.181200e-04 1.862461e-05 1.782577e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.072200e-04 1.402972e-05 1.300234e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.314800e-04 1.340325e-05 1.854704e-05
+1.750000e+03 2.500000e+02 2.500000e+02 6.295500e-05 4.854287e-06 5.491534e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.318200e-05 1.855430e-06 1.959019e-06
+3.350000e+03 6.500000e+02 6.500000e+02 1.905100e-06 4.335459e-07 4.003406e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d59-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d59-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.533800e-03 1.215600e-04 4.578800e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.756100e-03 3.323400e-05 5.062300e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.989200e-03 2.576500e-05 3.384400e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.406900e-03 3.537000e-05 2.042900e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.691000e-04 1.650300e-05 2.582800e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.846800e-04 1.385600e-05 1.406400e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.702000e-04 1.044800e-05 1.888800e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.399900e-04 1.008700e-05 1.781500e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.346200e-04 7.144400e-06 1.023400e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.522100e-04 9.169600e-06 6.431700e-06
+1.750000e+03 2.500000e+02 2.500000e+02 7.137600e-05 2.767100e-06 3.571900e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.879700e-05 9.967600e-07 1.349200e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.609100e-06 2.379600e-07 3.590000e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d59-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d59-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.539200e-03 6.898200e-05 6.014000e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.783400e-03 3.631500e-05 3.130500e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.006100e-03 1.177600e-05 9.872800e-06
+7.400000e+02 4.500000e+01 4.500000e+01 1.435800e-03 3.024900e-06 3.135100e-06
+8.325000e+02 4.750000e+01 4.750000e+01 9.792100e-04 7.903700e-06 8.899900e-06
+9.325000e+02 5.250000e+01 5.250000e+01 6.869200e-04 9.667500e-06 1.106500e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.674200e-04 9.532000e-06 1.099600e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.273300e-04 8.618600e-06 1.000300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.252300e-04 7.246900e-06 8.468800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.467300e-04 5.775100e-06 6.802900e-06
+1.750000e+03 2.500000e+02 2.500000e+02 6.747300e-05 3.424100e-06 4.077800e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.723200e-05 1.260300e-06 1.537800e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.278500e-06 2.334000e-07 2.946500e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d59-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d59-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.384800e-03 9.748300e-05 1.598600e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.659700e-03 3.182600e-05 1.973900e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.945600e-03 3.306300e-05 1.792100e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.396700e-03 6.561700e-06 7.235800e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.959700e-04 2.656700e-05 1.527800e-07
+9.325000e+02 5.250000e+01 5.250000e+01 7.087700e-04 1.702200e-05 2.733000e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.918100e-04 1.358900e-05 1.068100e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.509700e-04 5.620100e-06 1.291000e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.494600e-04 6.587100e-06 1.179700e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.696500e-04 1.542400e-05 0.000000e+00
+1.750000e+03 2.500000e+02 2.500000e+02 7.781200e-05 3.638800e-06 3.344700e-06
+2.350000e+03 3.500000e+02 3.500000e+02 2.016300e-05 2.480400e-06 1.220400e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.753200e-06 1.980800e-07 3.293400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d60-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d60-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.710100e-03 1.829325e-04 1.857785e-04
+3.750000e+01 1.250000e+01 1.250000e+01 9.054400e-03 2.892417e-04 3.263673e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.914000e-03 1.567079e-04 1.543139e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.474500e-03 1.418444e-04 1.354520e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.614600e-03 1.939892e-04 1.822575e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.724300e-03 2.153469e-04 1.885156e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.628400e-03 1.053646e-04 1.011315e-04
+2.250000e+02 3.500000e+01 3.500000e+01 7.742300e-04 4.996039e-05 4.853135e-05
+3.250000e+02 6.500000e+01 6.500000e+01 1.788300e-04 1.661312e-05 1.753925e-05
+6.450000e+02 2.550000e+02 2.550000e+02 9.241300e-06 1.971697e-06 2.104979e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d60-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d60-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.882600e-03 2.072200e-04 6.438900e-05
+3.750000e+01 1.250000e+01 1.250000e+01 8.113600e-03 9.308000e-05 1.482900e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.476800e-03 8.935300e-05 1.161800e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.746600e-03 8.291700e-05 8.773200e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.093600e-03 6.117200e-05 6.436300e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.861200e-03 6.286400e-05 5.337000e-05
+1.750000e+02 1.500000e+01 1.500000e+01 1.895500e-03 4.107000e-05 5.535600e-05
+2.250000e+02 3.500000e+01 3.500000e+01 9.315100e-04 2.289500e-05 2.045200e-05
+3.250000e+02 6.500000e+01 6.500000e+01 2.422800e-04 7.179100e-06 9.367200e-06
+6.450000e+02 2.550000e+02 2.550000e+02 1.430800e-05 1.253200e-06 1.034600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d60-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d60-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.989000e-03 1.416000e-04 1.227700e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.896200e-03 1.508700e-04 1.308100e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.072600e-03 2.375100e-05 2.090600e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.584200e-03 2.727300e-05 3.133300e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.037200e-03 3.591300e-05 4.522400e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.875300e-03 3.753400e-05 4.502100e-05
+1.750000e+02 1.500000e+01 1.500000e+01 2.012700e-03 3.629500e-05 4.133300e-05
+2.250000e+02 3.500000e+01 3.500000e+01 1.016400e-03 2.015800e-05 2.279700e-05
+3.250000e+02 6.500000e+01 6.500000e+01 2.888100e-04 7.442300e-06 8.013600e-06
+6.450000e+02 2.550000e+02 2.550000e+02 1.960600e-05 7.823300e-07 8.430800e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d60-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d60-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.858600e-03 1.083200e-04 2.436400e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.188400e-03 2.454600e-04 9.662900e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.534300e-03 0.000000e+00 3.665000e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.742500e-03 0.000000e+00 1.257700e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.056400e-03 8.830300e-05 0.000000e+00
+1.450000e+02 1.500000e+01 1.500000e+01 2.795200e-03 1.041800e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 1.864000e-03 1.437800e-05 6.655600e-05
+2.250000e+02 3.500000e+01 3.500000e+01 9.169000e-04 5.235800e-05 0.000000e+00
+3.250000e+02 6.500000e+01 6.500000e+01 2.462900e-04 9.787600e-06 1.423500e-05
+6.450000e+02 2.550000e+02 2.550000e+02 1.811500e-05 2.899300e-06 2.472100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d61-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d61-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.017800e-01 1.362437e-02 1.440183e-02
+3.500000e-01 5.000000e-02 5.000000e-02 1.427300e-01 1.755702e-02 1.844077e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.347600e-01 1.911047e-02 1.769351e-02
+5.500000e-01 5.000000e-02 5.000000e-02 3.735000e-01 2.875614e-02 3.109851e-02
+6.500000e-01 5.000000e-02 5.000000e-02 6.200100e-01 5.213860e-02 4.875594e-02
+7.250000e-01 2.500000e-02 2.500000e-02 8.685600e-01 7.355007e-02 7.419387e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.398000e+00 5.384091e-02 5.125492e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.083100e+00 6.703512e-02 6.473012e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.013100e+00 7.244860e-02 6.892062e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.060300e+00 9.637095e-02 8.811582e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.224200e+00 1.368201e-01 1.611396e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d61-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d61-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.371300e-01 3.655300e-03 5.286600e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.934500e-01 9.496500e-03 1.204600e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.638600e-01 1.280300e-02 1.126500e-02
+5.500000e-01 5.000000e-02 5.000000e-02 3.928200e-01 1.118000e-02 1.290200e-02
+6.500000e-01 5.000000e-02 5.000000e-02 6.729900e-01 1.496600e-02 1.636600e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.047300e+00 2.364600e-02 4.420900e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.465400e+00 3.685200e-02 2.797100e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.030300e+00 3.630900e-02 3.610200e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.848100e+00 4.791700e-02 5.670700e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.857800e+00 4.582700e-02 5.787900e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.882100e+00 1.135100e-01 5.105400e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d61-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d61-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.385600e-01 2.832700e-03 3.549500e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.891400e-01 3.405400e-03 4.012300e-03
+4.500000e-01 5.000000e-02 5.000000e-02 2.536300e-01 3.773200e-03 4.445900e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.886500e-01 7.634400e-03 8.697300e-03
+6.500000e-01 5.000000e-02 5.000000e-02 6.374100e-01 9.694900e-03 1.192600e-02
+7.250000e-01 2.500000e-02 2.500000e-02 9.975600e-01 1.289300e-02 1.470800e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.383900e+00 1.481100e-02 1.762000e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.968000e+00 1.820200e-02 2.027300e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.790700e+00 7.981000e-03 8.883600e-03
+9.250000e-01 2.500000e-02 2.500000e-02 3.963400e+00 3.363300e-02 2.808100e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.127400e+00 1.046700e-01 8.970500e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d61-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d61-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.280000e-01 5.879600e-03 0.000000e+00
+3.500000e-01 5.000000e-02 5.000000e-02 1.700600e-01 3.540400e-03 3.672300e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.384500e-01 1.108900e-02 0.000000e+00
+5.500000e-01 5.000000e-02 5.000000e-02 3.580800e-01 1.351400e-02 0.000000e+00
+6.500000e-01 5.000000e-02 5.000000e-02 6.284800e-01 2.671300e-02 2.228500e-03
+7.250000e-01 2.500000e-02 2.500000e-02 9.671500e-01 1.578700e-02 2.034000e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.403500e+00 4.781600e-02 2.510000e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.032200e+00 4.323700e-02 2.043100e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.909300e+00 2.071200e-02 2.903900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.029500e+00 3.946400e-02 1.379900e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.100200e+00 0.000000e+00 1.294000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d62-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d62-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.324300e-01 1.120437e-02 1.026632e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.150300e-01 1.282128e-02 1.150696e-02
+3.000000e+00 2.000000e-01 2.000000e-01 3.809700e-01 1.159701e-02 1.186194e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.491000e-01 1.234324e-02 1.235734e-02
+3.800000e+00 2.000000e-01 2.000000e-01 4.631300e-01 1.109745e-02 1.165524e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.971800e-01 1.001354e-02 9.212471e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.697900e-01 7.399613e-03 7.898935e-03
+5.000000e+00 2.000000e-01 2.000000e-01 9.728100e-02 6.190592e-03 6.496378e-03
+5.800000e+00 6.000000e-01 6.000000e-01 2.961300e-02 2.490982e-03 2.677298e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.042000e-03 4.840271e-04 4.915910e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d62-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d62-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.316900e-01 4.071400e-03 5.071400e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.044200e-01 4.826500e-03 6.135200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 3.928600e-01 1.515000e-02 5.120400e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.571300e-01 5.670200e-03 8.701500e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.437400e-01 6.822200e-03 5.903000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.899600e-01 5.191900e-03 5.502000e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.742700e-01 3.686200e-03 7.415700e-03
+5.000000e+00 2.000000e-01 2.000000e-01 9.967300e-02 2.579100e-03 6.947600e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.278900e-02 1.044200e-03 8.575500e-04
+7.600000e+00 1.200000e+00 1.200000e+00 1.315800e-03 1.209800e-04 2.074000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d62-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d62-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.968300e-01 4.204600e-03 4.415700e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.559000e-01 3.120500e-03 3.212200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.123100e-01 2.298300e-03 2.030600e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.446600e-01 1.859900e-03 1.555500e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.036900e-01 2.640600e-03 2.612600e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.596200e-01 3.111700e-03 2.801400e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.533400e-01 3.039000e-03 3.531600e-03
+5.000000e+00 2.000000e-01 2.000000e-01 8.557900e-02 2.688400e-03 3.167800e-03
+5.800000e+00 6.000000e-01 6.000000e-01 2.714300e-02 1.375300e-03 1.659500e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.107700e-03 1.066400e-04 1.356900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d62-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d62-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.529600e-01 4.795900e-03 1.912800e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.264300e-01 9.110500e-03 1.435600e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.013700e-01 5.643400e-03 0.000000e+00
+3.400000e+00 2.000000e-01 2.000000e-01 4.556500e-01 7.727700e-03 2.058700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.190200e-01 3.059300e-03 7.213500e-04
+4.200000e+00 2.000000e-01 2.000000e-01 2.734900e-01 3.752200e-03 1.902400e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.653700e-01 4.197100e-03 0.000000e+00
+5.000000e+00 2.000000e-01 2.000000e-01 9.715800e-02 4.634600e-03 1.335200e-02
+5.800000e+00 6.000000e-01 6.000000e-01 3.299600e-02 2.767600e-03 1.251500e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.593800e-03 1.666000e-04 3.756000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d63-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d63-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 8.597000e-03 6.410279e-04 7.175628e-04
+1.050000e+02 1.000000e+01 1.000000e+01 8.682700e-03 3.006712e-04 3.650035e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.505700e-03 1.505876e-04 1.412089e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.857900e-03 1.808055e-04 1.727831e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.520500e-03 2.010371e-04 1.924766e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.195100e-03 1.721878e-04 1.558201e-04
+2.350000e+02 1.500000e+01 1.500000e+01 1.920200e-03 1.300336e-04 1.208145e-04
+2.650000e+02 1.500000e+01 1.500000e+01 1.142300e-03 1.115987e-04 1.085334e-04
+2.975000e+02 1.750000e+01 1.750000e+01 7.322200e-04 5.104252e-05 4.414265e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.056900e-04 2.982988e-05 3.087551e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.586600e-04 2.005086e-05 2.087936e-05
+4.350000e+02 4.500000e+01 4.500000e+01 9.667700e-05 1.040879e-05 1.008464e-05
+5.825000e+02 1.025000e+02 1.025000e+02 1.798100e-05 2.827337e-06 2.992954e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d63-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d63-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 7.389600e-03 1.191700e-04 3.547100e-04
+1.050000e+02 1.000000e+01 1.000000e+01 8.170500e-03 3.343000e-04 1.044600e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.376900e-03 8.894200e-05 1.317500e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.113700e-03 1.156400e-04 9.133100e-05
+1.775000e+02 1.250000e+01 1.250000e+01 4.718100e-03 7.099900e-05 1.090500e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.309400e-03 7.084500e-05 7.433000e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.091000e-03 6.414900e-05 4.732200e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.293500e-03 3.488000e-05 4.962200e-05
+2.975000e+02 1.750000e+01 1.750000e+01 7.833800e-04 2.595500e-05 3.265200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.624000e-04 2.169000e-05 2.394600e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.679800e-04 1.427900e-05 1.892700e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.192800e-04 7.325000e-06 6.514400e-06
+5.825000e+02 1.025000e+02 1.025000e+02 2.271200e-05 2.598000e-06 2.056800e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d63-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d63-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.165900e-03 7.892800e-05 7.739500e-05
+1.050000e+02 1.000000e+01 1.000000e+01 7.036200e-03 6.513100e-05 6.530800e-05
+1.275000e+02 1.250000e+01 1.250000e+01 6.867400e-03 4.194900e-05 3.719800e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.090300e-03 2.789300e-05 2.275700e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.079500e-03 1.978800e-05 1.763600e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.649000e-03 2.084000e-05 2.343300e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.413600e-03 2.156800e-05 2.305400e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.540300e-03 2.114100e-05 2.317100e-05
+2.975000e+02 1.750000e+01 1.750000e+01 9.495100e-04 1.876800e-05 2.042200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 5.796700e-04 1.327900e-05 1.454900e-05
+3.700000e+02 2.000000e+01 2.000000e+01 3.477200e-04 9.107700e-06 9.782700e-06
+4.350000e+02 4.500000e+01 4.500000e+01 1.546500e-04 5.233400e-06 5.679300e-06
+5.825000e+02 1.025000e+02 1.025000e+02 3.130300e-05 1.315300e-06 1.441600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d63-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d63-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.757100e-03 1.194100e-04 4.071500e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.433100e-03 1.479200e-04 2.407800e-05
+1.275000e+02 1.250000e+01 1.250000e+01 7.108400e-03 2.144300e-04 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 6.223700e-03 4.743400e-05 1.252000e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.883600e-03 3.559500e-05 6.937000e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.498200e-03 1.475300e-05 2.303600e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.191500e-03 2.483800e-05 5.854400e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.422400e-03 3.732900e-05 0.000000e+00
+2.975000e+02 1.750000e+01 1.750000e+01 8.711000e-04 4.319900e-05 8.767100e-07
+3.325000e+02 1.750000e+01 1.750000e+01 5.452100e-04 3.923000e-05 0.000000e+00
+3.700000e+02 2.000000e+01 2.000000e+01 3.155800e-04 1.819000e-05 1.109400e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.418900e-04 6.965100e-06 1.774200e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.056500e-05 9.495800e-07 4.727500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d64-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d64-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t64
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 2.674200e-01 4.491341e-02 4.525471e-02
+7.500000e+01 2.500000e+01 2.500000e+01 3.724900e-01 3.939895e-02 4.703968e-02
+1.300000e+02 3.000000e+01 3.000000e+01 2.079700e-01 2.739788e-02 2.350885e-02
+1.925000e+02 3.250000e+01 3.250000e+01 1.115800e-01 1.430191e-02 1.462209e-02
+2.625000e+02 3.750000e+01 3.750000e+01 4.700200e-02 1.992072e-02 1.996867e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.250300e-03 3.774957e-02 3.774449e-02
+6.975000e+02 2.025000e+02 2.025000e+02 5.458600e-04 4.095326e-04 4.107797e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d64-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d64-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t64
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 2.239700e-01 2.728900e-02 2.080900e-02
+7.500000e+01 2.500000e+01 2.500000e+01 3.054800e-01 3.943000e-02 3.231700e-02
+1.300000e+02 3.000000e+01 3.000000e+01 2.047900e-01 2.164900e-02 2.386800e-02
+1.925000e+02 3.250000e+01 3.250000e+01 1.108700e-01 1.228700e-02 1.570400e-02
+2.625000e+02 3.750000e+01 3.750000e+01 5.003400e-02 5.052900e-03 4.460700e-03
+3.975000e+02 9.750000e+01 9.750000e+01 1.366100e-02 1.616400e-03 1.518500e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.095800e-03 2.037400e-04 2.103500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d64-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d64-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t64
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 3.071800e-01 5.188900e-02 8.759200e-02
+7.500000e+01 2.500000e+01 2.500000e+01 4.018000e-01 6.570600e-02 1.603900e-01
+1.300000e+02 3.000000e+01 3.000000e+01 2.567100e-01 5.092800e-02 1.023200e-01
+1.925000e+02 3.250000e+01 3.250000e+01 1.344300e-01 2.596600e-02 7.378000e-02
+2.625000e+02 3.750000e+01 3.750000e+01 6.309800e-02 1.273100e-02 2.078300e-02
+3.975000e+02 9.750000e+01 9.750000e+01 1.795700e-02 4.193500e-03 5.390200e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.657600e-03 3.662100e-04 7.480000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d65-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d65-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t65
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 5.520100e+00 2.510942e+00 2.559797e+00
+6.000000e-01 1.000000e-01 1.000000e-01 2.698000e+01 4.953234e+00 5.259319e+00
+7.500000e-01 5.000000e-02 5.000000e-02 6.827800e+01 8.337523e+00 8.039806e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.271800e+02 1.647799e+01 1.591515e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.474300e+02 2.868073e+01 2.765007e+01
+9.750000e-01 2.500000e-02 2.500000e-02 3.307400e+02 2.781169e+01 2.893715e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d65-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d65-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t65
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 8.402700e+00 8.305200e-01 1.209400e+00
+6.000000e-01 1.000000e-01 1.000000e-01 2.572900e+01 2.931400e+00 4.718800e+00
+7.500000e-01 5.000000e-02 5.000000e-02 6.382600e+01 7.372200e+00 7.963400e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.239000e+02 1.470500e+01 1.391600e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.118700e+02 2.422000e+01 1.813300e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.825800e+02 3.478400e+01 2.253000e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d65-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d65-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t65
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 9.150600e+00 1.864200e+00 4.995100e+00
+6.000000e-01 1.000000e-01 1.000000e-01 2.836600e+01 6.116800e+00 1.033800e+01
+7.500000e-01 5.000000e-02 5.000000e-02 7.319900e+01 1.231600e+01 2.342400e+01
+8.500000e-01 5.000000e-02 5.000000e-02 1.580600e+02 2.766900e+01 6.570400e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.906900e+02 5.783000e+01 1.037100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 4.125600e+02 6.495900e+01 1.526100e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d66-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d66-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t66
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 5.239400e+00 5.621497e-01 5.416009e-01
+3.200000e+00 4.000000e-01 4.000000e-01 6.939200e+00 6.535603e-01 6.334484e-01
+4.000000e+00 4.000000e-01 4.000000e-01 1.318100e+01 1.157089e+00 1.069418e+00
+4.800000e+00 4.000000e-01 4.000000e-01 1.590400e+01 2.170391e+00 2.123716e+00
+5.600000e+00 4.000000e-01 4.000000e-01 2.040800e+01 2.625320e+00 3.189703e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.417900e+00 7.354390e-01 6.604592e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d66-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d66-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t66
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 4.555800e+00 5.744500e-01 5.165200e-01
+3.200000e+00 4.000000e-01 4.000000e-01 7.398600e+00 8.278200e-01 7.556400e-01
+4.000000e+00 4.000000e-01 4.000000e-01 1.144800e+01 1.197700e+00 1.233200e+00
+4.800000e+00 4.000000e-01 4.000000e-01 1.673600e+01 1.722100e+00 1.402400e+00
+5.600000e+00 4.000000e-01 4.000000e-01 1.807600e+01 2.023900e+00 2.263500e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.239400e+00 3.862600e-01 2.853700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d66-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d66-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t66
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 7.473100e+00 1.529300e+00 3.883900e+00
+3.200000e+00 4.000000e-01 4.000000e-01 1.192400e+01 2.392800e+00 3.974200e+00
+4.000000e+00 4.000000e-01 4.000000e-01 1.586000e+01 2.853400e+00 6.805400e+00
+4.800000e+00 4.000000e-01 4.000000e-01 2.027500e+01 3.681400e+00 7.261200e+00
+5.600000e+00 4.000000e-01 4.000000e-01 1.987400e+01 3.369800e+00 8.794800e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.933100e+00 5.047500e-01 6.107300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d67-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d67-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t67
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.903900e-01 7.502811e-02 8.013669e-02
+1.400000e+02 2.500000e+01 2.500000e+01 2.750100e-01 3.924753e-02 3.612656e-02
+1.925000e+02 2.750000e+01 2.750000e+01 1.833000e-01 1.943026e-02 2.300746e-02
+2.500000e+02 3.000000e+01 3.000000e+01 1.195700e-01 1.460465e-02 1.214861e-02
+3.150000e+02 3.500000e+01 3.500000e+01 6.816600e-02 1.704474e-02 1.669931e-02
+3.925000e+02 4.250000e+01 4.250000e+01 5.076100e-02 5.870752e-03 5.757623e-03
+5.075000e+02 7.250000e+01 7.250000e+01 2.749000e-02 3.412071e-03 3.229625e-03
+7.300000e+02 1.500000e+02 1.500000e+02 4.916500e-03 1.154162e-03 1.147772e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d67-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d67-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t67
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.275100e-01 3.310400e-02 4.021500e-02
+1.400000e+02 2.500000e+01 2.500000e+01 2.408100e-01 2.843500e-02 2.583700e-02
+1.925000e+02 2.750000e+01 2.750000e+01 1.816100e-01 2.001200e-02 1.553200e-02
+2.500000e+02 3.000000e+01 3.000000e+01 1.230200e-01 1.478200e-02 1.009200e-02
+3.150000e+02 3.500000e+01 3.500000e+01 8.085000e-02 7.994600e-03 8.493600e-03
+3.925000e+02 4.250000e+01 4.250000e+01 4.941800e-02 5.306900e-03 5.850600e-03
+5.075000e+02 7.250000e+01 7.250000e+01 2.702300e-02 2.931100e-03 3.213800e-03
+7.300000e+02 1.500000e+02 1.500000e+02 5.320900e-03 8.264500e-04 5.590800e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d67-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d67-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t67
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.923200e-01 4.814700e-02 9.105100e-02
+1.400000e+02 2.500000e+01 2.500000e+01 2.665100e-01 4.240900e-02 1.054600e-01
+1.925000e+02 2.750000e+01 2.750000e+01 2.205000e-01 4.364300e-02 8.326400e-02
+2.500000e+02 3.000000e+01 3.000000e+01 1.570400e-01 3.138500e-02 5.388200e-02
+3.150000e+02 3.500000e+01 3.500000e+01 1.132200e-01 2.396300e-02 5.003700e-02
+3.925000e+02 4.250000e+01 4.250000e+01 7.425500e-02 1.452500e-02 2.641600e-02
+5.075000e+02 7.250000e+01 7.250000e+01 4.370800e-02 9.631300e-03 1.718500e-02
+7.300000e+02 1.500000e+02 1.500000e+02 9.033100e-03 1.487100e-03 6.215500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d68-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d68-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t68
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 9.950900e+01 1.942476e+01 1.854141e+01
+2.500000e-01 1.000000e-01 1.000000e-01 8.070900e+01 1.408074e+01 1.343267e+01
+5.000000e-01 1.500000e-01 1.500000e-01 5.441500e+01 1.029418e+01 1.044141e+01
+8.250000e-01 1.750000e-01 1.750000e-01 9.741800e+00 1.900542e+00 1.972275e+00
+1.500000e+00 5.000000e-01 5.000000e-01 6.006700e-01 2.042429e-01 2.014581e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d68-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d68-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t68
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 7.690900e+01 1.619700e+01 8.542800e+00
+2.500000e-01 1.000000e-01 1.000000e-01 7.096900e+01 1.318800e+01 1.102600e+01
+5.000000e-01 1.500000e-01 1.500000e-01 4.342600e+01 4.416600e+00 6.735800e+00
+8.250000e-01 1.750000e-01 1.750000e-01 9.053000e+00 1.338500e+00 9.468000e-01
+1.500000e+00 5.000000e-01 5.000000e-01 5.568000e-01 1.107200e-01 9.573200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d68-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d68-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t68
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.108800e+02 2.293100e+01 5.061700e+01
+2.500000e-01 1.000000e-01 1.000000e-01 1.004700e+02 1.689300e+01 4.855200e+01
+5.000000e-01 1.500000e-01 1.500000e-01 6.479800e+01 1.333100e+01 2.844800e+01
+8.250000e-01 1.750000e-01 1.750000e-01 1.434400e+01 3.951300e+00 5.709500e+00
+1.500000e+00 5.000000e-01 5.000000e-01 9.877500e-01 2.295100e-01 5.180400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d69-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d69-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t69
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 9.167600e+01 8.744966e+00 9.993516e+00
+3.000000e-01 1.000000e-01 1.000000e-01 1.033500e+02 1.315957e+01 1.305025e+01
+4.750000e-01 7.500000e-02 7.500000e-02 6.467700e+01 1.181920e+01 1.180156e+01
+6.750000e-01 1.250000e-01 1.250000e-01 2.499700e+01 3.321205e+00 2.895415e+00
+9.000000e-01 1.000000e-01 1.000000e-01 4.704700e+00 9.374202e-01 9.543161e-01
+1.100000e+00 1.000000e-01 1.000000e-01 1.372800e+00 5.085533e-01 5.090083e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d69-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d69-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t69
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 8.662100e+01 6.075200e+00 7.395600e+00
+3.000000e-01 1.000000e-01 1.000000e-01 9.681400e+01 1.297600e+01 1.040300e+01
+4.750000e-01 7.500000e-02 7.500000e-02 6.644700e+01 9.621600e+00 6.649700e+00
+6.750000e-01 1.250000e-01 1.250000e-01 2.061600e+01 2.597700e+00 3.408100e+00
+9.000000e-01 1.000000e-01 1.000000e-01 3.882400e+00 7.499600e-01 8.866100e-01
+1.100000e+00 1.000000e-01 1.000000e-01 9.913800e-01 2.754400e-01 3.793300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d69-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d69-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t69
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.005500e+02 1.355700e+01 2.667400e+01
+3.000000e-01 1.000000e-01 1.000000e-01 1.171000e+02 2.349900e+01 4.233100e+01
+4.750000e-01 7.500000e-02 7.500000e-02 9.886900e+01 1.943700e+01 5.203700e+01
+6.750000e-01 1.250000e-01 1.250000e-01 3.361800e+01 6.727700e+00 1.553500e+01
+9.000000e-01 1.000000e-01 1.000000e-01 6.780200e+00 2.126500e+00 2.802800e+00
+1.100000e+00 1.000000e-01 1.000000e-01 1.623900e+00 3.248900e-01 1.118000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d70-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d70-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t70
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 3.074200e+01 2.901229e+00 3.069764e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.495500e+01 2.066467e+00 2.003503e+00
+2.000000e+00 5.000000e-01 5.000000e-01 6.357000e+00 1.046056e+00 1.122947e+00
+3.000000e+00 5.000000e-01 5.000000e-01 2.886000e+00 7.992817e-01 6.571748e-01
+6.000000e+00 2.500000e+00 2.500000e+00 1.435200e+00 5.450652e-01 4.914309e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d70-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d70-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t70
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 3.019200e+01 2.376700e+00 2.457800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.405400e+01 2.142600e+00 1.756100e+00
+2.000000e+00 5.000000e-01 5.000000e-01 5.752600e+00 7.362300e-01 9.443400e-01
+3.000000e+00 5.000000e-01 5.000000e-01 2.054200e+00 6.968700e-01 2.687600e-01
+6.000000e+00 2.500000e+00 2.500000e+00 7.883900e-01 1.387900e-01 2.023900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d70-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d70-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t70
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 3.645800e+01 6.348600e+00 1.145400e+01
+1.000000e+00 5.000000e-01 5.000000e-01 1.976500e+01 3.454400e+00 8.995000e+00
+2.000000e+00 5.000000e-01 5.000000e-01 8.546400e+00 2.081500e+00 4.554500e+00
+3.000000e+00 5.000000e-01 5.000000e-01 2.964600e+00 8.147700e-01 9.282500e-01
+6.000000e+00 2.500000e+00 2.500000e+00 8.032000e-01 1.145500e-01 3.909200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d71-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d71-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.415600e+00 1.986454e-01 2.133789e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.743300e+00 1.299251e-01 1.343406e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.179300e+00 7.270734e-02 7.321741e-02
+7.400000e+02 4.500000e+01 4.500000e+01 8.000100e-01 4.943582e-02 4.272418e-02
+8.325000e+02 4.750000e+01 4.750000e+01 5.315900e-01 3.537647e-02 4.513574e-02
+9.325000e+02 5.250000e+01 5.250000e+01 3.311600e-01 2.183101e-02 2.696344e-02
+1.042500e+03 5.750000e+01 5.750000e+01 2.021500e-01 2.018193e-02 1.723141e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.160100e-01 1.162131e-02 9.688182e-03
+1.275000e+03 7.500000e+01 7.500000e+01 7.343200e-02 7.372960e-03 6.168185e-03
+1.425000e+03 7.500000e+01 7.500000e+01 4.681700e-02 4.873837e-03 4.807159e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.410100e-02 2.775143e-03 2.904789e-03
+2.350000e+03 3.500000e+02 3.500000e+02 2.248900e-03 5.788196e-04 3.754865e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.085800e-04 5.300238e-05 5.091667e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d71-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d71-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.969200e+00 2.690900e-01 1.946600e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.470400e+00 1.817200e-01 1.657400e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.000900e+00 1.328000e-01 2.237600e-01
+7.400000e+02 4.500000e+01 4.500000e+01 6.636100e-01 1.062100e-01 7.794700e-02
+8.325000e+02 4.750000e+01 4.750000e+01 4.262500e-01 5.759400e-02 4.364300e-02
+9.325000e+02 5.250000e+01 5.250000e+01 2.739200e-01 3.568500e-02 3.587300e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.699400e-01 2.336700e-02 1.684900e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.086100e-01 1.400600e-02 1.659000e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.666000e-02 9.762500e-03 8.835900e-03
+1.425000e+03 7.500000e+01 7.500000e+01 3.859200e-02 5.034200e-03 4.425600e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.347800e-02 1.539800e-03 1.919000e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.976100e-03 2.840300e-04 2.513800e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.089900e-04 3.707200e-05 3.430300e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d71-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d71-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.056200e+00 4.627500e-01 6.714700e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.552700e+00 3.593300e-01 5.301400e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.057800e+00 2.419800e-01 3.546300e-01
+7.400000e+02 4.500000e+01 4.500000e+01 7.049000e-01 1.626500e-01 2.394000e-01
+8.325000e+02 4.750000e+01 4.750000e+01 4.634900e-01 1.088200e-01 1.622100e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.024700e-01 7.286500e-02 1.094500e-01
+1.042500e+03 5.750000e+01 5.750000e+01 1.893800e-01 4.552500e-02 6.812800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.230700e-01 2.992800e-02 4.511000e-02
+1.275000e+03 7.500000e+01 7.500000e+01 7.513800e-02 1.846900e-02 2.797300e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.677100e-02 1.236000e-02 1.962400e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.630500e-02 4.027900e-03 6.092800e-03
+2.350000e+03 3.500000e+02 3.500000e+02 2.306300e-03 6.167600e-04 9.615900e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.366400e-04 3.831500e-05 6.055100e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d71-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d71-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.975000e+00 3.615700e-01 8.545600e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.479800e+00 2.551400e-01 6.320200e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.041100e+00 1.671700e-01 4.564400e-01
+7.400000e+02 4.500000e+01 4.500000e+01 7.005600e-01 1.353200e-01 2.863100e-01
+8.325000e+02 4.750000e+01 4.750000e+01 4.886400e-01 1.314300e-01 1.449800e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.055600e-01 5.207500e-02 1.218400e-01
+1.042500e+03 5.750000e+01 5.750000e+01 1.990800e-01 4.164500e-02 7.744400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.344000e-01 3.122300e-02 4.936500e-02
+1.275000e+03 7.500000e+01 7.500000e+01 8.610500e-02 1.420100e-02 2.970300e-02
+1.425000e+03 7.500000e+01 7.500000e+01 5.010900e-02 8.459200e-03 1.657700e-02
+1.750000e+03 2.500000e+02 2.500000e+02 2.036100e-02 4.202000e-03 9.873600e-03
+2.350000e+03 3.500000e+02 3.500000e+02 3.309800e-03 7.252700e-04 1.386600e-03
+3.350000e+03 6.500000e+02 6.500000e+02 2.617200e-04 1.134100e-04 6.592500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d72-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d72-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.608800e+00 2.444261e-01 2.441014e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.994200e+00 4.615159e-01 4.827298e-01
+6.250000e+01 1.250000e+01 1.250000e+01 4.384900e+00 4.262507e-01 4.407255e-01
+8.750000e+01 1.250000e+01 1.250000e+01 3.205100e+00 2.156284e-01 2.213289e-01
+1.150000e+02 1.500000e+01 1.500000e+01 2.122700e+00 1.368441e-01 1.320994e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.312200e+00 1.052806e-01 9.578950e-02
+1.750000e+02 1.500000e+01 1.500000e+01 8.039800e-01 7.431028e-02 7.563143e-02
+2.075000e+02 1.750000e+01 1.750000e+01 4.799200e-01 5.407814e-02 5.051290e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.769900e-01 2.559383e-02 2.834501e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.585800e-01 2.203793e-02 2.026432e-02
+3.975000e+02 9.750000e+01 9.750000e+01 3.140300e-02 8.332853e-03 8.254493e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.882700e-03 7.983694e-04 8.074512e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d72-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d72-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.875900e+00 3.425300e-01 6.209600e-01
+3.750000e+01 1.250000e+01 1.250000e+01 3.912800e+00 4.769000e-01 4.861200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 3.553600e+00 4.906100e-01 3.903400e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.646200e+00 3.397200e-01 3.238300e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.804400e+00 2.422700e-01 2.159600e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.192600e+00 1.508800e-01 1.236300e-01
+1.750000e+02 1.500000e+01 1.500000e+01 7.785300e-01 1.011300e-01 6.947300e-02
+2.075000e+02 1.750000e+01 1.750000e+01 4.763700e-01 6.753400e-02 4.427900e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.801400e-01 2.907400e-02 2.482100e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.629500e-01 2.337900e-02 1.633500e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.244800e-02 5.189000e-03 2.135900e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.942800e-03 2.696000e-04 2.439500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d72-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d72-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.100100e+00 4.189000e-01 5.808200e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.063700e+00 8.731800e-01 1.251300e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.580000e+00 8.206600e-01 1.202300e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.766700e+00 6.605300e-01 9.814900e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.912000e+00 4.652000e-01 7.007300e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.354100e+00 3.498800e-01 5.411300e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.696100e-01 2.181600e-01 3.335600e-01
+2.075000e+02 1.750000e+01 1.750000e+01 5.394700e-01 1.356100e-01 2.055300e-01
+2.425000e+02 1.750000e+01 1.750000e+01 3.334100e-01 8.460600e-02 1.282600e-01
+2.800000e+02 2.000000e+01 2.000000e+01 1.971800e-01 5.055500e-02 7.684200e-02
+3.975000e+02 9.750000e+01 9.750000e+01 5.599800e-02 1.454600e-02 2.212400e-02
+6.975000e+02 2.025000e+02 2.025000e+02 2.896300e-03 7.754000e-04 1.183300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d72-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d72-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.982400e+00 2.688200e-01 7.563800e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.174400e+00 7.277300e-01 1.787700e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.835400e+00 8.292200e-01 1.533600e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.813400e+00 4.737500e-01 1.213200e+00
+1.150000e+02 1.500000e+01 1.500000e+01 1.915800e+00 3.763300e-01 8.659100e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.342800e+00 3.293400e-01 4.489400e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.355200e-01 1.582400e-01 3.490300e-01
+2.075000e+02 1.750000e+01 1.750000e+01 4.972900e-01 1.147400e-01 2.066200e-01
+2.425000e+02 1.750000e+01 1.750000e+01 2.861000e-01 6.359200e-02 9.284700e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.641100e-01 2.400200e-02 5.206000e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.566900e-02 1.055200e-02 1.474900e-02
+6.975000e+02 2.025000e+02 2.025000e+02 2.507100e-03 6.248900e-04 1.155500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d73-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d73-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 3.259200e+01 9.394090e+00 8.680227e+00
+4.000000e-01 1.000000e-01 1.000000e-01 6.824900e+01 1.221602e+01 1.280593e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.239800e+02 2.442462e+01 2.432244e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.365000e+02 2.418363e+01 1.910719e+01
+6.750000e-01 2.500000e-02 2.500000e-02 3.164500e+02 2.460514e+01 2.709276e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.799300e+02 1.373115e+02 1.368762e+02
+7.750000e-01 2.500000e-02 2.500000e-02 7.852600e+02 5.284852e+01 6.030013e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.163000e+03 8.378977e+01 8.799065e+01
+8.750000e-01 2.500000e-02 2.500000e-02 1.677700e+03 1.275951e+02 1.307555e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.384500e+03 1.899326e+02 1.936158e+02
+9.750000e-01 2.500000e-02 2.500000e-02 3.212400e+03 2.530477e+02 2.558266e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d73-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d73-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.323200e+01 6.333200e+00 3.119600e+00
+4.000000e-01 1.000000e-01 1.000000e-01 7.526600e+01 8.462900e+00 9.371900e+00
+5.500000e-01 5.000000e-02 5.000000e-02 1.491400e+02 2.541700e+01 1.710200e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.209500e+02 3.509200e+01 3.085700e+01
+6.750000e-01 2.500000e-02 2.500000e-02 2.981400e+02 4.193200e+01 4.393500e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.373600e+02 6.749200e+01 4.075700e+01
+7.750000e-01 2.500000e-02 2.500000e-02 6.154700e+02 7.359400e+01 6.547700e+01
+8.250000e-01 2.500000e-02 2.500000e-02 9.116200e+02 1.179500e+02 1.052600e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.345500e+03 1.659300e+02 1.638400e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.915800e+03 2.433400e+02 2.181100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.497400e+03 3.612500e+02 4.226200e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d73-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d73-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.375000e+01 1.108600e+01 1.690900e+01
+4.000000e-01 1.000000e-01 1.000000e-01 7.793300e+01 2.018700e+01 3.206900e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.627100e+02 4.517800e+01 7.210600e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.114800e+02 5.235700e+01 7.913400e+01
+6.750000e-01 2.500000e-02 2.500000e-02 2.941100e+02 7.246200e+01 1.095000e+02
+7.250000e-01 2.500000e-02 2.500000e-02 4.201600e+02 1.029900e+02 1.551900e+02
+7.750000e-01 2.500000e-02 2.500000e-02 6.193300e+02 1.508500e+02 2.263500e+02
+8.250000e-01 2.500000e-02 2.500000e-02 9.222500e+02 2.210500e+02 3.297400e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.388700e+03 3.238100e+02 4.785500e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.082800e+03 4.691000e+02 6.836100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.909500e+03 6.339900e+02 9.081600e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d73-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d73-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.256000e+01 9.324700e+00 1.319500e+01
+4.000000e-01 1.000000e-01 1.000000e-01 7.237000e+01 1.535900e+01 3.025600e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.344900e+02 2.669700e+01 5.513000e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.184500e+02 4.520700e+01 7.154500e+01
+6.750000e-01 2.500000e-02 2.500000e-02 2.885200e+02 5.168800e+01 1.176500e+02
+7.250000e-01 2.500000e-02 2.500000e-02 4.222100e+02 7.557700e+01 1.845800e+02
+7.750000e-01 2.500000e-02 2.500000e-02 6.157100e+02 1.049400e+02 2.798900e+02
+8.250000e-01 2.500000e-02 2.500000e-02 9.800100e+02 2.083000e+02 4.000400e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.420400e+03 2.332200e+02 6.533500e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.145300e+03 4.553400e+02 8.358500e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.833700e+03 4.822200e+02 1.107600e+03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d74-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d74-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.091100e+02 1.402670e+01 1.367168e+01
+2.600000e+00 2.000000e-01 2.000000e-01 2.238300e+02 1.418280e+01 1.464034e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.508100e+02 1.570909e+01 1.630807e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.548900e+02 1.680456e+01 1.726047e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.085200e+02 1.648540e+01 1.729891e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.239900e+02 1.942287e+01 2.008674e+01
+4.800000e+00 4.000000e-01 4.000000e-01 3.985000e+01 4.397196e+00 4.895263e+00
+5.800000e+00 6.000000e-01 6.000000e-01 4.125500e+00 1.785458e+00 8.646571e-01
+7.600000e+00 1.200000e+00 1.200000e+00 4.605400e-02 3.548376e-02 3.060149e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d74-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d74-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.682500e+02 1.911100e+01 1.705200e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.877400e+02 2.302200e+01 1.780900e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.067500e+02 2.724000e+01 4.304200e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.127000e+02 2.959100e+01 2.353200e+01
+3.800000e+00 2.000000e-01 2.000000e-01 1.796200e+02 2.303400e+01 2.226300e+01
+4.200000e+00 2.000000e-01 2.000000e-01 9.933600e+01 1.952700e+01 1.126700e+01
+4.800000e+00 4.000000e-01 4.000000e-01 3.561800e+01 5.320800e+00 4.564200e+00
+5.800000e+00 6.000000e-01 6.000000e-01 3.964300e+00 3.798400e-01 9.810600e-01
+7.600000e+00 1.200000e+00 1.200000e+00 1.805700e-02 9.709000e-03 2.504800e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d74-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d74-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.290900e+02 5.415400e+01 7.983400e+01
+2.600000e+00 2.000000e-01 2.000000e-01 2.313500e+02 5.433300e+01 7.991700e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.257000e+02 5.194100e+01 7.631300e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.144600e+02 5.025900e+01 7.480700e+01
+3.800000e+00 2.000000e-01 2.000000e-01 1.629000e+02 3.641200e+01 5.317800e+01
+4.200000e+00 2.000000e-01 2.000000e-01 8.647600e+01 1.982200e+01 2.937800e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.884000e+01 6.717800e+00 1.018600e+01
+5.800000e+00 6.000000e-01 6.000000e-01 3.563700e+00 8.811000e-01 1.425800e+00
+7.600000e+00 1.200000e+00 1.200000e+00 2.293000e-02 5.544400e-03 8.364100e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d74-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d74-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.995700e+02 3.832400e+01 8.540200e+01
+2.600000e+00 2.000000e-01 2.000000e-01 2.161600e+02 3.189100e+01 9.208600e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.361000e+02 5.285900e+01 8.408300e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.223600e+02 3.994100e+01 9.154700e+01
+3.800000e+00 2.000000e-01 2.000000e-01 1.711300e+02 3.226800e+01 7.569300e+01
+4.200000e+00 2.000000e-01 2.000000e-01 9.087400e+01 1.709200e+01 3.585100e+01
+4.800000e+00 4.000000e-01 4.000000e-01 3.249900e+01 6.881100e+00 1.188200e+01
+5.800000e+00 6.000000e-01 6.000000e-01 5.201100e+00 8.860400e-01 2.234300e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.684500e-02 2.217500e-02 2.512900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d75-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d75-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.474600e+00 4.513922e-01 4.906002e-01
+1.050000e+02 1.000000e+01 1.000000e+01 3.817400e+00 3.467802e-01 3.619172e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.709900e+00 2.775314e-01 2.966466e-01
+1.525000e+02 1.250000e+01 1.250000e+01 3.426300e+00 2.473760e-01 2.188008e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.885500e+00 1.772587e-01 1.786117e-01
+2.050000e+02 1.500000e+01 1.500000e+01 2.037100e+00 1.139894e-01 1.159287e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.322600e+00 6.547812e-02 6.509956e-02
+2.650000e+02 1.500000e+01 1.500000e+01 8.300900e-01 4.913497e-02 4.526458e-02
+2.975000e+02 1.750000e+01 1.750000e+01 4.733500e-01 2.818240e-02 3.180290e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.416800e-01 3.326100e-02 3.264959e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.601200e-01 1.262026e-02 1.280743e-02
+4.125000e+02 2.250000e+01 2.250000e+01 8.138600e-02 9.159946e-03 8.966827e-03
+4.575000e+02 2.250000e+01 2.250000e+01 4.430500e-02 6.159585e-03 6.015320e-03
+5.300000e+02 5.000000e+01 5.000000e+01 1.427900e-02 3.023692e-03 2.966646e-03
+6.325000e+02 5.250000e+01 5.250000e+01 5.809600e-03 1.447559e-03 1.407017e-03
+8.425000e+02 1.575000e+02 1.575000e+02 3.192400e-04 2.349571e-04 2.265932e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d75-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d75-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 2.691600e+00 5.538800e-01 3.010300e-01
+1.050000e+02 1.000000e+01 1.000000e+01 3.128800e+00 4.155600e-01 3.963100e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.132300e+00 4.416500e-01 7.005100e-01
+1.525000e+02 1.250000e+01 1.250000e+01 2.879600e+00 3.603200e-01 3.115000e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.434100e+00 2.976700e-01 2.874300e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.741000e+00 2.273500e-01 1.783500e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.103800e+00 1.276600e-01 1.050200e-01
+2.650000e+02 1.500000e+01 1.500000e+01 6.818000e-01 8.567600e-02 5.664200e-02
+2.975000e+02 1.750000e+01 1.750000e+01 4.037900e-01 4.674100e-02 3.902800e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.326500e-01 3.004600e-02 1.663400e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.343400e-01 1.635600e-02 9.528000e-03
+4.125000e+02 2.250000e+01 2.250000e+01 7.385600e-02 8.839400e-03 8.698400e-03
+4.575000e+02 2.250000e+01 2.250000e+01 4.084200e-02 5.505900e-03 4.583800e-03
+5.300000e+02 5.000000e+01 5.000000e+01 1.595000e-02 1.828200e-03 1.577400e-03
+6.325000e+02 5.250000e+01 5.250000e+01 4.946100e-03 1.038100e-03 7.978700e-04
+8.425000e+02 1.575000e+02 1.575000e+02 7.036200e-04 1.671500e-04 1.736300e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d75-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d75-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 2.101300e+00 4.511200e-01 6.576400e-01
+1.050000e+02 1.000000e+01 1.000000e+01 2.663100e+00 5.794100e-01 8.389100e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.045100e+00 7.054600e-01 1.051600e+00
+1.525000e+02 1.250000e+01 1.250000e+01 2.977300e+00 6.763600e-01 9.886300e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.838300e+00 6.630100e-01 9.766500e-01
+2.050000e+02 1.500000e+01 1.500000e+01 2.074600e+00 4.874400e-01 7.207400e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.386000e+00 3.322000e-01 4.937400e-01
+2.650000e+02 1.500000e+01 1.500000e+01 8.986100e-01 2.172400e-01 3.231500e-01
+2.975000e+02 1.750000e+01 1.750000e+01 5.496300e-01 1.353700e-01 2.027900e-01
+3.325000e+02 1.750000e+01 1.750000e+01 3.368700e-01 8.370200e-02 1.255400e-01
+3.700000e+02 2.000000e+01 2.000000e+01 1.930200e-01 4.933400e-02 7.466400e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.106700e-01 2.851700e-02 4.324900e-02
+4.575000e+02 2.250000e+01 2.250000e+01 6.263200e-02 1.600400e-02 2.424700e-02
+5.300000e+02 5.000000e+01 5.000000e+01 2.554700e-02 6.756100e-03 1.032100e-02
+6.325000e+02 5.250000e+01 5.250000e+01 7.936300e-03 2.158200e-03 3.332400e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.160000e-03 3.214500e-04 4.988500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d75-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d75-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 2.188800e+00 3.477800e-01 8.848000e-01
+1.050000e+02 1.000000e+01 1.000000e+01 2.836800e+00 5.356900e-01 1.211800e+00
+1.275000e+02 1.250000e+01 1.250000e+01 3.196900e+00 5.550400e-01 1.406300e+00
+1.525000e+02 1.250000e+01 1.250000e+01 3.139700e+00 6.049600e-01 1.335500e+00
+1.775000e+02 1.250000e+01 1.250000e+01 2.796300e+00 5.255700e-01 9.938500e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.994500e+00 3.917300e-01 7.904300e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.332100e+00 3.259900e-01 4.493100e-01
+2.650000e+02 1.500000e+01 1.500000e+01 8.173100e-01 1.530200e-01 3.694800e-01
+2.975000e+02 1.750000e+01 1.750000e+01 4.812700e-01 5.977900e-02 2.580000e-01
+3.325000e+02 1.750000e+01 1.750000e+01 2.925800e-01 5.854100e-02 1.017000e-01
+3.700000e+02 2.000000e+01 2.000000e+01 1.759000e-01 3.122300e-02 6.793000e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.049600e-01 2.999000e-02 2.634900e-02
+4.575000e+02 2.250000e+01 2.250000e+01 5.317300e-02 8.767800e-03 2.365200e-02
+5.300000e+02 5.000000e+01 5.000000e+01 2.250300e-02 6.137300e-03 8.894600e-03
+6.325000e+02 5.250000e+01 5.250000e+01 7.633200e-03 7.187800e-04 4.316800e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.200700e-03 3.819800e-04 2.757200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d76-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d76-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t76
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.087800e-01 4.281009e-02 4.256285e-02
+3.750000e+01 1.250000e+01 1.250000e+01 7.984000e-01 8.448911e-02 8.972912e-02
+6.250000e+01 1.250000e+01 1.250000e+01 7.041700e-01 6.612812e-02 5.708515e-02
+8.750000e+01 1.250000e+01 1.250000e+01 5.321400e-01 4.150655e-02 4.281049e-02
+1.150000e+02 1.500000e+01 1.500000e+01 3.390600e-01 2.796040e-02 2.700158e-02
+1.450000e+02 1.500000e+01 1.500000e+01 2.771500e-01 2.555827e-02 3.259398e-02
+1.750000e+02 1.500000e+01 1.500000e+01 1.590200e-01 1.852536e-02 1.688511e-02
+2.250000e+02 3.500000e+01 3.500000e+01 9.247100e-02 1.755659e-02 1.700525e-02
+3.775000e+02 1.175000e+02 1.175000e+02 2.046100e-02 3.483494e-03 3.448098e-03
+6.975000e+02 2.025000e+02 2.025000e+02 9.135300e-04 5.418348e-04 5.435699e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d76-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d76-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t76
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.126900e-01 2.520400e-02 3.117500e-02
+3.750000e+01 1.250000e+01 1.250000e+01 6.423100e-01 5.055000e-02 7.936300e-02
+6.250000e+01 1.250000e+01 1.250000e+01 5.914100e-01 6.345500e-02 4.912000e-02
+8.750000e+01 1.250000e+01 1.250000e+01 4.830300e-01 4.930400e-02 4.401200e-02
+1.150000e+02 1.500000e+01 1.500000e+01 3.689000e-01 3.256400e-02 3.069500e-02
+1.450000e+02 1.500000e+01 1.500000e+01 2.651200e-01 3.069900e-02 1.247100e-02
+1.750000e+02 1.500000e+01 1.500000e+01 1.871300e-01 2.147500e-02 1.730200e-02
+2.250000e+02 3.500000e+01 3.500000e+01 1.053200e-01 1.055100e-02 1.023300e-02
+3.775000e+02 1.175000e+02 1.175000e+02 2.230600e-02 1.722400e-03 1.640200e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.581200e-03 2.373000e-04 2.266600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d76-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d76-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t76
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.397000e-01 2.514400e-02 1.266800e-01
+3.750000e+01 1.250000e+01 1.250000e+01 6.927500e-01 8.516200e-02 1.792200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 6.547100e-01 9.976400e-02 2.494900e-01
+8.750000e+01 1.250000e+01 1.250000e+01 5.305000e-01 9.168900e-02 1.674400e-01
+1.150000e+02 1.500000e+01 1.500000e+01 3.978900e-01 5.852800e-02 1.240000e-01
+1.450000e+02 1.500000e+01 1.500000e+01 2.915100e-01 5.425500e-02 7.554500e-02
+1.750000e+02 1.500000e+01 1.500000e+01 2.043500e-01 2.879900e-02 5.797500e-02
+2.250000e+02 3.500000e+01 3.500000e+01 1.184300e-01 2.824900e-02 2.431300e-02
+3.775000e+02 1.175000e+02 1.175000e+02 2.630300e-02 3.446000e-03 1.045700e-02
+6.975000e+02 2.025000e+02 2.025000e+02 2.006400e-03 3.923500e-04 8.622500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d77-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d77-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t77
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 7.519900e+00 2.321114e+00 2.384740e+00
+5.000000e-01 1.000000e-01 1.000000e-01 2.679800e+01 4.691930e+00 4.498031e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.341600e+01 1.157207e+01 1.169160e+01
+7.500000e-01 5.000000e-02 5.000000e-02 1.171000e+02 1.120355e+01 1.013444e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.873600e+02 1.601033e+01 1.496033e+01
+8.750000e-01 2.500000e-02 2.500000e-02 3.043500e+02 2.868889e+01 2.886343e+01
+9.250000e-01 2.500000e-02 2.500000e-02 4.002600e+02 3.493286e+01 3.610713e+01
+9.750000e-01 2.500000e-02 2.500000e-02 5.295900e+02 4.400955e+01 4.310709e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d77-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d77-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t77
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.311200e+01 1.449400e+00 1.670800e+00
+5.000000e-01 1.000000e-01 1.000000e-01 2.636600e+01 3.089700e+00 2.952400e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.527100e+01 5.121500e+00 6.217600e+00
+7.500000e-01 5.000000e-02 5.000000e-02 1.047300e+02 1.156600e+01 7.577400e+00
+8.250000e-01 2.500000e-02 2.500000e-02 1.718800e+02 1.799500e+01 1.449400e+01
+8.750000e-01 2.500000e-02 2.500000e-02 2.480800e+02 2.195600e+01 1.937600e+01
+9.250000e-01 2.500000e-02 2.500000e-02 3.516200e+02 3.175100e+01 3.940000e+01
+9.750000e-01 2.500000e-02 2.500000e-02 4.682900e+02 3.856600e+01 3.326400e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d77-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d77-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t77
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.368400e+01 2.258100e+00 3.579800e+00
+5.000000e-01 1.000000e-01 1.000000e-01 2.889500e+01 5.533300e+00 5.176200e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.779100e+01 1.133300e+01 1.597600e+01
+7.500000e-01 5.000000e-02 5.000000e-02 1.076000e+02 1.657800e+01 3.618500e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.866700e+02 3.604000e+01 4.896000e+01
+8.750000e-01 2.500000e-02 2.500000e-02 2.692400e+02 3.183000e+01 8.255500e+01
+9.250000e-01 2.500000e-02 2.500000e-02 3.962600e+02 6.234700e+01 1.126200e+02
+9.750000e-01 2.500000e-02 2.500000e-02 5.434600e+02 7.657400e+01 1.930300e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d78-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d78-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t78
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.820400e+00 8.249588e-01 8.326482e-01
+3.200000e+00 4.000000e-01 4.000000e-01 1.756400e+01 1.168185e+00 1.177140e+00
+3.800000e+00 2.000000e-01 2.000000e-01 2.330100e+01 1.977673e+00 1.786061e+00
+4.200000e+00 2.000000e-01 2.000000e-01 3.145200e+01 3.527567e+00 3.524170e+00
+4.600000e+00 2.000000e-01 2.000000e-01 3.617400e+01 3.111277e+00 2.496711e+00
+5.000000e+00 2.000000e-01 2.000000e-01 3.975000e+01 3.459769e+00 3.847957e+00
+5.400000e+00 2.000000e-01 2.000000e-01 2.664300e+01 2.343107e+00 2.366723e+00
+6.000000e+00 4.000000e-01 4.000000e-01 1.161900e+01 1.765713e+00 1.903634e+00
+7.600000e+00 1.200000e+00 1.200000e+00 5.938000e-01 2.750364e-01 2.776955e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d78-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d78-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t78
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 8.024800e+00 7.481900e-01 5.866500e-01
+3.200000e+00 4.000000e-01 4.000000e-01 1.517600e+01 1.363500e+00 8.667600e-01
+3.800000e+00 2.000000e-01 2.000000e-01 2.350900e+01 2.088000e+00 1.665800e+00
+4.200000e+00 2.000000e-01 2.000000e-01 3.085000e+01 2.968500e+00 1.876900e+00
+4.600000e+00 2.000000e-01 2.000000e-01 3.535800e+01 3.058900e+00 5.057900e+00
+5.000000e+00 2.000000e-01 2.000000e-01 3.591000e+01 3.538300e+00 3.357600e+00
+5.400000e+00 2.000000e-01 2.000000e-01 2.612600e+01 2.867700e+00 2.040000e+00
+6.000000e+00 4.000000e-01 4.000000e-01 9.726500e+00 1.245000e+00 1.018200e+00
+7.600000e+00 1.200000e+00 1.200000e+00 6.115400e-01 5.622500e-02 1.297900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d78-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d78-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t78
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.050100e+01 1.808700e+00 4.292900e+00
+3.200000e+00 4.000000e-01 4.000000e-01 1.914600e+01 3.471700e+00 6.093500e+00
+3.800000e+00 2.000000e-01 2.000000e-01 2.742300e+01 4.321400e+00 8.361700e+00
+4.200000e+00 2.000000e-01 2.000000e-01 3.268200e+01 4.483800e+00 1.086000e+01
+4.600000e+00 2.000000e-01 2.000000e-01 3.610300e+01 6.019700e+00 1.085800e+01
+5.000000e+00 2.000000e-01 2.000000e-01 3.638900e+01 3.030000e+00 1.018000e+01
+5.400000e+00 2.000000e-01 2.000000e-01 2.628900e+01 3.828900e+00 5.384700e+00
+6.000000e+00 4.000000e-01 4.000000e-01 1.057600e+01 1.557600e+00 2.983400e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.667600e-01 5.681500e-02 1.605200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d79-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d79-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t79
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.672900e-01 1.283284e-01 1.395802e-01
+1.050000e+02 1.000000e+01 1.000000e+01 6.114000e-01 6.343564e-02 6.633891e-02
+1.250000e+02 1.000000e+01 1.000000e+01 5.988800e-01 5.511955e-02 5.249953e-02
+1.475000e+02 1.250000e+01 1.250000e+01 5.134400e-01 5.272883e-02 4.578762e-02
+1.725000e+02 1.250000e+01 1.250000e+01 3.588800e-01 3.374518e-02 2.980955e-02
+1.975000e+02 1.250000e+01 1.250000e+01 2.828200e-01 2.074717e-02 2.012721e-02
+2.250000e+02 1.500000e+01 1.500000e+01 2.465000e-01 1.908910e-02 1.803991e-02
+2.575000e+02 1.750000e+01 1.750000e+01 1.608700e-01 2.961223e-02 2.911250e-02
+2.975000e+02 2.250000e+01 2.250000e+01 1.538400e-01 1.000783e-02 1.008376e-02
+3.525000e+02 3.250000e+01 3.250000e+01 9.073600e-02 7.289540e-03 7.041303e-03
+5.350000e+02 1.500000e+02 1.500000e+02 1.852800e-02 1.661871e-03 1.817394e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d79-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d79-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t79
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.924000e-01 7.545600e-02 6.181500e-02
+1.050000e+02 1.000000e+01 1.000000e+01 5.483500e-01 5.016800e-02 6.953800e-02
+1.250000e+02 1.000000e+01 1.000000e+01 5.256600e-01 6.097800e-02 8.149600e-02
+1.475000e+02 1.250000e+01 1.250000e+01 4.845100e-01 4.727000e-02 2.968700e-02
+1.725000e+02 1.250000e+01 1.250000e+01 3.785700e-01 3.402800e-02 3.129500e-02
+1.975000e+02 1.250000e+01 1.250000e+01 3.069100e-01 2.527900e-02 2.378800e-02
+2.250000e+02 1.500000e+01 1.500000e+01 2.447000e-01 2.550100e-02 1.436600e-02
+2.575000e+02 1.750000e+01 1.750000e+01 1.796800e-01 1.607700e-02 1.257400e-02
+2.975000e+02 2.250000e+01 2.250000e+01 1.321200e-01 1.231400e-02 1.061600e-02
+3.525000e+02 3.250000e+01 3.250000e+01 8.274600e-02 7.921900e-03 5.743200e-03
+5.350000e+02 1.500000e+02 1.500000e+02 1.733400e-02 1.607500e-03 1.136100e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d79-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d79-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t79
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.666200e-01 5.114400e-02 1.285700e-01
+1.050000e+02 1.000000e+01 1.000000e+01 5.362900e-01 3.190200e-02 1.679900e-01
+1.250000e+02 1.000000e+01 1.000000e+01 5.155800e-01 7.619700e-02 1.457700e-01
+1.475000e+02 1.250000e+01 1.250000e+01 4.909100e-01 8.641500e-02 1.170000e-01
+1.725000e+02 1.250000e+01 1.250000e+01 4.173200e-01 5.892800e-02 1.503100e-01
+1.975000e+02 1.250000e+01 1.250000e+01 3.381500e-01 4.784000e-02 9.492700e-02
+2.250000e+02 1.500000e+01 1.500000e+01 2.727400e-01 4.908000e-02 1.128800e-01
+2.575000e+02 1.750000e+01 1.750000e+01 2.082900e-01 3.261500e-02 7.396100e-02
+2.975000e+02 2.250000e+01 2.250000e+01 1.539200e-01 2.740200e-02 4.535800e-02
+3.525000e+02 3.250000e+01 3.250000e+01 1.063700e-01 1.880300e-02 3.072000e-02
+5.350000e+02 1.500000e+02 1.500000e+02 2.387300e-02 4.790300e-03 7.053500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d80-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d80-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t80
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 8.546800e-01 8.612225e-02 7.912468e-02
+3.750000e+01 1.250000e+01 1.250000e+01 1.722100e+00 1.695759e-01 1.694289e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.829700e+00 1.588628e-01 1.642612e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.553100e+00 1.322698e-01 1.478433e-01
+1.300000e+02 3.000000e+01 3.000000e+01 9.629900e-01 1.177879e-01 8.760995e-02
+1.925000e+02 3.250000e+01 3.250000e+01 4.948700e-01 4.828867e-02 4.378868e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.276000e-01 3.738451e-02 3.755716e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.574500e-01 2.042846e-02 2.016106e-02
+3.975000e+02 9.750000e+01 9.750000e+01 3.973300e-02 8.807956e-03 8.492160e-03
+6.975000e+02 2.025000e+02 2.025000e+02 3.488700e-03 7.847399e-04 8.642819e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d80-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d80-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t80
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 6.460100e-01 9.349400e-02 6.639100e-02
+3.750000e+01 1.250000e+01 1.250000e+01 1.448000e+00 1.662900e-01 1.544200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.520800e+00 2.040700e-01 1.740800e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.312700e+00 1.501500e-01 1.647700e-01
+1.300000e+02 3.000000e+01 3.000000e+01 9.203100e-01 1.126200e-01 1.069400e-01
+1.925000e+02 3.250000e+01 3.250000e+01 4.698100e-01 5.616300e-02 5.496900e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.462900e-01 3.263300e-02 2.491600e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.535000e-01 1.313900e-02 1.577600e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.778900e-02 6.300400e-03 4.425600e-03
+6.975000e+02 2.025000e+02 2.025000e+02 3.427000e-03 3.940400e-04 4.199200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d80-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d80-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t80
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 7.780000e-01 8.816100e-02 3.056400e-01
+3.750000e+01 1.250000e+01 1.250000e+01 1.801800e+00 2.478100e-01 6.374600e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.884900e+00 3.691500e-01 7.408700e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.575000e+00 2.500000e-01 6.653100e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.092700e+00 2.151300e-01 4.219100e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.538200e-01 1.123600e-01 2.242100e-01
+2.425000e+02 1.750000e+01 1.750000e+01 2.919000e-01 6.249100e-02 9.346700e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.860600e-01 3.746100e-02 7.458800e-02
+3.975000e+02 9.750000e+01 9.750000e+01 5.770700e-02 1.065300e-02 1.880200e-02
+6.975000e+02 2.025000e+02 2.025000e+02 4.972300e-03 1.072000e-03 1.877000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d81-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d81-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t81
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 2.302100e+01 7.646984e+00 7.235272e+00
+3.750000e-01 1.250000e-01 1.250000e-01 3.346800e+01 1.401554e+01 8.684749e+00
+6.000000e-01 1.000000e-01 1.000000e-01 1.255600e+02 1.642000e+01 1.715345e+01
+7.250000e-01 2.500000e-02 2.500000e-02 2.675100e+02 2.695763e+01 2.902101e+01
+7.750000e-01 2.500000e-02 2.500000e-02 3.698200e+02 3.379826e+01 3.701121e+01
+8.250000e-01 2.500000e-02 2.500000e-02 5.383800e+02 4.780003e+01 4.492155e+01
+8.750000e-01 2.500000e-02 2.500000e-02 8.043800e+02 6.960621e+01 6.579602e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.113700e+03 9.127146e+01 9.587340e+01
+9.750000e-01 2.500000e-02 2.500000e-02 1.409800e+03 1.074742e+02 1.066351e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d81-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d81-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t81
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 2.916200e+01 2.912700e+00 5.335800e+00
+3.750000e-01 1.250000e-01 1.250000e-01 4.794600e+01 6.722000e+00 5.485200e+00
+6.000000e-01 1.000000e-01 1.000000e-01 1.207000e+02 1.627700e+01 1.727300e+01
+7.250000e-01 2.500000e-02 2.500000e-02 2.416600e+02 3.077700e+01 3.978400e+01
+7.750000e-01 2.500000e-02 2.500000e-02 3.390800e+02 4.503100e+01 3.079300e+01
+8.250000e-01 2.500000e-02 2.500000e-02 4.668300e+02 5.311000e+01 5.642600e+01
+8.750000e-01 2.500000e-02 2.500000e-02 6.593600e+02 7.662600e+01 7.962000e+01
+9.250000e-01 2.500000e-02 2.500000e-02 9.187700e+02 1.141800e+02 1.043400e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.194900e+03 1.412200e+02 9.735700e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d81-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d81-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t81
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 2.967200e+01 5.932200e+00 9.878100e+00
+3.750000e-01 1.250000e-01 1.250000e-01 4.675100e+01 8.243100e+00 2.085400e+01
+6.000000e-01 1.000000e-01 1.000000e-01 1.262300e+02 2.556200e+01 4.486100e+01
+7.250000e-01 2.500000e-02 2.500000e-02 2.556300e+02 4.740000e+01 9.881500e+01
+7.750000e-01 2.500000e-02 2.500000e-02 3.836500e+02 5.978400e+01 1.719300e+02
+8.250000e-01 2.500000e-02 2.500000e-02 5.761800e+02 1.360000e+02 1.727100e+02
+8.750000e-01 2.500000e-02 2.500000e-02 8.018600e+02 1.223500e+02 3.151600e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.172300e+03 1.867200e+02 4.640100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.594600e+03 2.723700e+02 6.336200e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d82-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d82-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t82
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.761100e+01 3.456050e+00 3.420067e+00
+2.600000e+00 2.000000e-01 2.000000e-01 4.706400e+01 3.788729e+00 3.818097e+00
+3.000000e+00 2.000000e-01 2.000000e-01 5.251400e+01 4.227319e+00 4.144895e+00
+3.400000e+00 2.000000e-01 2.000000e-01 6.915200e+01 4.739150e+00 5.247235e+00
+3.800000e+00 2.000000e-01 2.000000e-01 7.515600e+01 5.817993e+00 5.141712e+00
+4.200000e+00 2.000000e-01 2.000000e-01 8.903400e+01 7.203957e+00 6.757537e+00
+4.600000e+00 2.000000e-01 2.000000e-01 9.695100e+01 9.096673e+00 7.540531e+00
+5.000000e+00 2.000000e-01 2.000000e-01 8.632700e+01 9.180567e+00 1.022418e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.328400e+01 8.771251e+00 6.448629e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.405800e+00 7.574342e-01 6.852392e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d82-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d82-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t82
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.002800e+01 3.442700e+00 3.056500e+00
+2.600000e+00 2.000000e-01 2.000000e-01 3.677300e+01 4.418500e+00 3.821700e+00
+3.000000e+00 2.000000e-01 2.000000e-01 4.583700e+01 5.917900e+00 4.089500e+00
+3.400000e+00 2.000000e-01 2.000000e-01 5.659000e+01 5.753100e+00 6.190500e+00
+3.800000e+00 2.000000e-01 2.000000e-01 6.915600e+01 8.471800e+00 6.454300e+00
+4.200000e+00 2.000000e-01 2.000000e-01 8.094400e+01 9.034900e+00 9.059200e+00
+4.600000e+00 2.000000e-01 2.000000e-01 8.819200e+01 1.024200e+01 1.232100e+01
+5.000000e+00 2.000000e-01 2.000000e-01 8.384700e+01 1.179800e+01 9.276300e+00
+5.600000e+00 4.000000e-01 4.000000e-01 3.948100e+01 5.011100e+00 4.857200e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.255400e+00 3.980800e-01 2.832600e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d82-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d82-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t82
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.447900e+01 1.136600e+01 1.740400e+01
+2.600000e+00 2.000000e-01 2.000000e-01 5.416800e+01 9.518500e+00 2.271900e+01
+3.000000e+00 2.000000e-01 2.000000e-01 6.529200e+01 1.341800e+01 2.728000e+01
+3.400000e+00 2.000000e-01 2.000000e-01 7.646300e+01 1.244100e+01 3.134100e+01
+3.800000e+00 2.000000e-01 2.000000e-01 8.610200e+01 1.509900e+01 3.601700e+01
+4.200000e+00 2.000000e-01 2.000000e-01 9.379700e+01 1.766300e+01 3.356600e+01
+4.600000e+00 2.000000e-01 2.000000e-01 9.440600e+01 1.761400e+01 3.743900e+01
+5.000000e+00 2.000000e-01 2.000000e-01 8.682100e+01 1.334600e+01 3.175300e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.337200e+01 6.362300e+00 1.574200e+01
+7.400000e+00 1.400000e+00 1.400000e+00 2.947900e+00 5.055900e-01 6.195800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d83-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d83-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t83
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.230900e+00 2.363524e-01 2.208020e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.367500e+00 2.699029e-01 1.971903e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.401200e+00 1.569007e-01 1.398365e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.224800e+00 1.113375e-01 9.117330e-02
+1.775000e+02 1.250000e+01 1.250000e+01 9.815500e-01 8.478990e-02 8.393441e-02
+2.050000e+02 1.500000e+01 1.500000e+01 8.136600e-01 5.240337e-02 5.084697e-02
+2.350000e+02 1.500000e+01 1.500000e+01 6.854200e-01 4.803824e-02 4.945945e-02
+2.650000e+02 1.500000e+01 1.500000e+01 5.444200e-01 5.055078e-02 4.844646e-02
+2.975000e+02 1.750000e+01 1.750000e+01 5.018000e-01 3.177053e-02 3.279758e-02
+3.325000e+02 1.750000e+01 1.750000e+01 3.830600e-01 3.868264e-02 4.028094e-02
+3.700000e+02 2.000000e+01 2.000000e+01 3.030500e-01 2.151354e-02 2.319422e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.886800e-01 1.553877e-02 1.418631e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.129500e-01 1.066773e-02 1.014564e-02
+5.300000e+02 5.000000e+01 5.000000e+01 5.356500e-02 6.216788e-03 6.002569e-03
+7.300000e+02 1.500000e+02 1.500000e+02 7.651500e-03 1.465704e-03 1.534366e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d83-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d83-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t83
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.039900e+00 1.611800e-01 1.698200e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.224500e+00 1.710600e-01 1.401200e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.230700e+00 1.620600e-01 1.894200e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.094500e+00 1.256300e-01 1.221100e-01
+1.775000e+02 1.250000e+01 1.250000e+01 9.337600e-01 1.004600e-01 1.012000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 7.834900e-01 1.081600e-01 7.402400e-02
+2.350000e+02 1.500000e+01 1.500000e+01 6.376300e-01 7.086200e-02 6.465700e-02
+2.650000e+02 1.500000e+01 1.500000e+01 5.178300e-01 6.202500e-02 4.300600e-02
+2.975000e+02 1.750000e+01 1.750000e+01 4.174200e-01 4.358100e-02 4.600200e-02
+3.325000e+02 1.750000e+01 1.750000e+01 3.324600e-01 3.657400e-02 2.870000e-02
+3.700000e+02 2.000000e+01 2.000000e+01 2.449200e-01 2.993200e-02 2.903200e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.620600e-01 1.975900e-02 1.527800e-02
+4.575000e+02 2.250000e+01 2.250000e+01 9.927100e-02 1.168200e-02 1.401800e-02
+5.300000e+02 5.000000e+01 5.000000e+01 4.562900e-02 5.759600e-03 3.406500e-03
+7.300000e+02 1.500000e+02 1.500000e+02 7.432100e-03 8.321700e-04 6.613600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d83-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d83-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t83
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.193500e+00 1.333100e-01 3.407400e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.264400e+00 1.563100e-01 5.121700e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.267500e+00 2.238800e-01 4.767600e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.215700e+00 2.394700e-01 4.412900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.126900e+00 2.102700e-01 4.224000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 9.228200e-01 1.453900e-01 4.038200e-01
+2.350000e+02 1.500000e+01 1.500000e+01 7.897200e-01 1.531800e-01 2.964800e-01
+2.650000e+02 1.500000e+01 1.500000e+01 6.680500e-01 1.176200e-01 2.909900e-01
+2.975000e+02 1.750000e+01 1.750000e+01 5.572800e-01 1.033900e-01 2.439400e-01
+3.325000e+02 1.750000e+01 1.750000e+01 4.738300e-01 8.338800e-02 1.748400e-01
+3.700000e+02 2.000000e+01 2.000000e+01 3.564400e-01 7.142800e-02 1.213200e-01
+4.125000e+02 2.250000e+01 2.250000e+01 2.427100e-01 6.847700e-02 7.604900e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.438900e-01 2.485000e-02 6.675300e-02
+5.300000e+02 5.000000e+01 5.000000e+01 7.098200e-02 1.507400e-02 2.817900e-02
+7.300000e+02 1.500000e+02 1.500000e+02 1.221600e-02 2.064100e-03 6.538900e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d84-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d84-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t84
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 4.347400e+02 5.795541e+01 6.211122e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.845800e+02 5.274486e+01 5.032847e+01
+3.000000e-01 5.000000e-02 5.000000e-02 3.647200e+02 5.068410e+01 5.084223e+01
+4.500000e-01 1.000000e-01 1.000000e-01 2.688400e+02 4.779646e+01 4.023696e+01
+6.000000e-01 5.000000e-02 5.000000e-02 1.889400e+02 2.910514e+01 2.964744e+01
+7.500000e-01 1.000000e-01 1.000000e-01 8.870300e+01 1.384812e+01 1.426679e+01
+1.025000e+00 1.750000e-01 1.750000e-01 2.708000e+01 4.515114e+00 4.539786e+00
+1.850000e+00 6.500000e-01 6.500000e-01 2.292300e+00 4.370611e-01 4.426839e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d84-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d84-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t84
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.321700e+02 5.383300e+01 4.128500e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.224100e+02 4.767800e+01 4.784700e+01
+3.000000e-01 5.000000e-02 5.000000e-02 3.263500e+02 5.051200e+01 4.407900e+01
+4.500000e-01 1.000000e-01 1.000000e-01 2.437600e+02 3.066900e+01 3.452800e+01
+6.000000e-01 5.000000e-02 5.000000e-02 1.597000e+02 2.220900e+01 2.097700e+01
+7.500000e-01 1.000000e-01 1.000000e-01 8.221600e+01 1.097900e+01 9.676500e+00
+1.025000e+00 1.750000e-01 1.750000e-01 2.277500e+01 3.576700e+00 1.967800e+00
+1.850000e+00 6.500000e-01 6.500000e-01 1.609100e+00 2.676200e-01 2.410200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d84-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d84-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t84
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 4.378000e+02 8.450300e+01 1.977600e+02
+2.000000e-01 5.000000e-02 5.000000e-02 4.204900e+02 8.073100e+01 1.929300e+02
+3.000000e-01 5.000000e-02 5.000000e-02 4.200800e+02 8.238600e+01 1.944700e+02
+4.500000e-01 1.000000e-01 1.000000e-01 3.125500e+02 6.555000e+01 1.322200e+02
+6.000000e-01 5.000000e-02 5.000000e-02 2.066400e+02 4.837800e+01 8.167300e+01
+7.500000e-01 1.000000e-01 1.000000e-01 1.106500e+02 2.555100e+01 4.710600e+01
+1.025000e+00 1.750000e-01 1.750000e-01 3.358800e+01 8.781200e+00 1.261500e+01
+1.850000e+00 6.500000e-01 6.500000e-01 2.349700e+00 5.707100e-01 1.011300e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d85-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d85-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t85
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.247200e+02 2.503460e+01 2.851347e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.848800e+02 5.262616e+01 3.346398e+01
+3.250000e-01 7.500000e-02 7.500000e-02 4.329600e+02 3.719179e+01 3.749501e+01
+4.750000e-01 7.500000e-02 7.500000e-02 3.746100e+02 3.679920e+01 3.706925e+01
+6.750000e-01 1.250000e-01 1.250000e-01 1.703000e+02 1.989806e+01 1.730539e+01
+9.000000e-01 1.000000e-01 1.000000e-01 3.995000e+01 5.329199e+00 5.208289e+00
+1.750000e+00 7.500000e-01 7.500000e-01 2.382200e+00 3.930711e-01 3.966423e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d85-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d85-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t85
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.018300e+02 2.525500e+01 2.559800e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.464100e+02 3.608800e+01 3.342900e+01
+3.250000e-01 7.500000e-02 7.500000e-02 3.971700e+02 5.379100e+01 4.828200e+01
+4.750000e-01 7.500000e-02 7.500000e-02 3.274300e+02 4.371800e+01 3.635600e+01
+6.750000e-01 1.250000e-01 1.250000e-01 1.464000e+02 2.012900e+01 1.994100e+01
+9.000000e-01 1.000000e-01 1.000000e-01 3.425100e+01 5.986100e+00 4.486000e+00
+1.750000e+00 7.500000e-01 7.500000e-01 1.593600e+00 2.331500e-01 2.907300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d85-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d85-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t85
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.382400e+02 4.966400e+01 1.057100e+02
+2.000000e-01 5.000000e-02 5.000000e-02 3.961600e+02 6.686700e+01 1.237500e+02
+3.250000e-01 7.500000e-02 7.500000e-02 4.576100e+02 7.642000e+01 1.879100e+02
+4.750000e-01 7.500000e-02 7.500000e-02 4.087400e+02 7.475900e+01 1.786400e+02
+6.750000e-01 1.250000e-01 1.250000e-01 1.992300e+02 4.159300e+01 8.039300e+01
+9.000000e-01 1.000000e-01 1.000000e-01 5.022400e+01 1.168900e+01 2.223400e+01
+1.750000e+00 7.500000e-01 7.500000e-01 2.270300e+00 4.911400e-01 1.075100e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d86-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d86-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t86
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.414400e+02 8.672454e+00 7.780229e+00
+1.000000e+00 5.000000e-01 5.000000e-01 7.665500e+01 8.583108e+00 7.459364e+00
+2.000000e+00 5.000000e-01 5.000000e-01 3.080900e+01 4.180022e+00 4.464411e+00
+3.000000e+00 5.000000e-01 5.000000e-01 9.790800e+00 2.027761e+00 1.998234e+00
+6.000000e+00 2.500000e+00 2.500000e+00 3.549500e+00 1.178194e+00 1.009966e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d86-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d86-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t86
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.283600e+02 1.287900e+01 1.183900e+01
+1.000000e+00 5.000000e-01 5.000000e-01 6.845200e+01 9.888400e+00 8.883300e+00
+2.000000e+00 5.000000e-01 5.000000e-01 2.620200e+01 3.683300e+00 3.543100e+00
+3.000000e+00 5.000000e-01 5.000000e-01 8.274100e+00 1.530400e+00 1.346200e+00
+6.000000e+00 2.500000e+00 2.500000e+00 3.162600e+00 4.991000e-01 4.510400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d86-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d86-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t86
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.482500e+02 2.285400e+01 4.891200e+01
+1.000000e+00 5.000000e-01 5.000000e-01 8.725800e+01 1.738000e+01 3.863700e+01
+2.000000e+00 5.000000e-01 5.000000e-01 3.441100e+01 7.705900e+00 1.574400e+01
+3.000000e+00 5.000000e-01 5.000000e-01 1.082300e+01 2.179800e+00 4.632600e+00
+6.000000e+00 2.500000e+00 2.500000e+00 2.821900e+00 3.718700e-01 1.463200e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d87-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d87-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.345400e+00 6.283506e-01 6.385587e-01
+5.800000e+02 3.500000e+01 3.500000e+01 4.960800e+00 3.555689e-01 3.514885e-01
+6.550000e+02 4.000000e+01 4.000000e+01 3.607100e+00 2.477671e-01 2.512099e-01
+7.400000e+02 4.500000e+01 4.500000e+01 2.500100e+00 1.661609e-01 1.490339e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.698200e+00 1.253064e-01 1.200099e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.135700e+00 7.611003e-02 9.353712e-02
+1.042500e+03 5.750000e+01 5.750000e+01 7.612900e-01 5.902181e-02 5.512267e-02
+1.150000e+03 5.000000e+01 5.000000e+01 4.986300e-01 4.476704e-02 3.211264e-02
+1.275000e+03 7.500000e+01 7.500000e+01 3.215300e-01 3.539612e-02 2.299664e-02
+1.425000e+03 7.500000e+01 7.500000e+01 2.053000e-01 1.960732e-02 2.564483e-02
+1.750000e+03 2.500000e+02 2.500000e+02 8.434500e-02 9.472271e-03 1.062872e-02
+2.350000e+03 3.500000e+02 3.500000e+02 1.466300e-02 2.688886e-03 2.399257e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.497700e-03 4.270761e-04 3.916612e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d87-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d87-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 5.189500e+00 6.646800e-01 4.813300e-01
+5.800000e+02 3.500000e+01 3.500000e+01 4.064400e+00 4.873900e-01 4.491200e-01
+6.550000e+02 4.000000e+01 4.000000e+01 2.940600e+00 3.623100e-01 3.876200e-01
+7.400000e+02 4.500000e+01 4.500000e+01 2.074700e+00 2.906300e-01 2.113500e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.427100e+00 1.793300e-01 1.504700e-01
+9.325000e+02 5.250000e+01 5.250000e+01 9.744700e-01 1.204500e-01 1.030300e-01
+1.042500e+03 5.750000e+01 5.750000e+01 6.551300e-01 8.060800e-02 7.529300e-02
+1.150000e+03 5.000000e+01 5.000000e+01 4.526800e-01 5.282000e-02 6.030800e-02
+1.275000e+03 7.500000e+01 7.500000e+01 2.994500e-01 3.891800e-02 3.251400e-02
+1.425000e+03 7.500000e+01 7.500000e+01 1.862400e-01 2.447800e-02 1.554400e-02
+1.750000e+03 2.500000e+02 2.500000e+02 7.816500e-02 9.135900e-03 8.739000e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.649200e-02 1.713100e-03 1.375700e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.727600e-03 1.849300e-04 1.868400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d87-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d87-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 5.421500e+00 1.325300e+00 1.985600e+00
+5.800000e+02 3.500000e+01 3.500000e+01 4.268400e+00 1.064600e+00 1.610500e+00
+6.550000e+02 4.000000e+01 4.000000e+01 3.073400e+00 7.723900e-01 1.171600e+00
+7.400000e+02 4.500000e+01 4.500000e+01 2.184200e+00 5.600800e-01 8.571600e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.512900e+00 3.939700e-01 6.068100e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.035900e+00 2.749000e-01 4.269400e-01
+1.042500e+03 5.750000e+01 5.750000e+01 6.863500e-01 1.839600e-01 2.869700e-01
+1.150000e+03 5.000000e+01 5.000000e+01 4.767700e-01 1.302100e-01 2.047800e-01
+1.275000e+03 7.500000e+01 7.500000e+01 3.177100e-01 8.769500e-02 1.388000e-01
+1.425000e+03 7.500000e+01 7.500000e+01 2.005600e-01 5.687800e-02 9.136200e-02
+1.750000e+03 2.500000e+02 2.500000e+02 8.242300e-02 2.368700e-02 3.828700e-02
+2.350000e+03 3.500000e+02 3.500000e+02 1.697600e-02 5.169700e-03 8.610000e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.768800e-03 5.715800e-04 9.824900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d87-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d87-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 5.245900e+00 1.046600e+00 2.291600e+00
+5.800000e+02 3.500000e+01 3.500000e+01 4.166000e+00 7.955300e-01 1.822200e+00
+6.550000e+02 4.000000e+01 4.000000e+01 3.068100e+00 5.780100e-01 1.336000e+00
+7.400000e+02 4.500000e+01 4.500000e+01 2.198800e+00 4.371200e-01 9.161400e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.597800e+00 3.599300e-01 5.767300e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.094800e+00 2.048300e-01 4.545500e-01
+1.042500e+03 5.750000e+01 5.750000e+01 7.471200e-01 1.389900e-01 3.049900e-01
+1.150000e+03 5.000000e+01 5.000000e+01 5.265600e-01 9.647500e-02 2.111000e-01
+1.275000e+03 7.500000e+01 7.500000e+01 3.652300e-01 5.967500e-02 1.373000e-01
+1.425000e+03 7.500000e+01 7.500000e+01 2.308300e-01 4.210600e-02 7.928000e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.005300e-01 1.783600e-02 4.013200e-02
+2.350000e+03 3.500000e+02 3.500000e+02 2.146900e-02 3.521900e-03 7.645500e-03
+3.350000e+03 6.500000e+02 6.500000e+02 2.395800e-03 5.135400e-04 1.198300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d88-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d88-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 6.686800e+00 6.362590e-01 6.131993e-01
+3.750000e+01 1.250000e+01 1.250000e+01 1.373000e+01 1.237871e+00 1.291998e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.337800e+01 1.099245e+00 1.113073e+00
+8.750000e+01 1.250000e+01 1.250000e+01 1.020500e+01 7.321694e-01 7.441399e-01
+1.150000e+02 1.500000e+01 1.500000e+01 6.936000e+00 4.835363e-01 4.427047e-01
+1.450000e+02 1.500000e+01 1.500000e+01 4.871300e+00 4.563773e-01 3.811436e-01
+1.750000e+02 1.500000e+01 1.500000e+01 3.125300e+00 2.446411e-01 2.454333e-01
+2.075000e+02 1.750000e+01 1.750000e+01 1.836400e+00 1.628755e-01 1.472490e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.050500e+00 9.161548e-02 1.008043e-01
+2.800000e+02 2.000000e+01 2.000000e+01 6.262700e-01 7.411697e-02 7.248302e-02
+3.975000e+02 9.750000e+01 9.750000e+01 1.206400e-01 2.266544e-02 2.255991e-02
+6.975000e+02 2.025000e+02 2.025000e+02 5.853700e-03 1.238371e-03 1.310000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d88-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d88-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.812200e+00 7.881100e-01 7.603200e-01
+3.750000e+01 1.250000e+01 1.250000e+01 1.063800e+01 1.265400e+00 1.234200e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.059800e+01 1.325600e+00 1.134200e+00
+8.750000e+01 1.250000e+01 1.250000e+01 8.514900e+00 1.058100e+00 9.114000e-01
+1.150000e+02 1.500000e+01 1.500000e+01 6.209700e+00 7.671000e-01 7.232000e-01
+1.450000e+02 1.500000e+01 1.500000e+01 4.351500e+00 5.547000e-01 4.442300e-01
+1.750000e+02 1.500000e+01 1.500000e+01 2.905400e+00 3.307500e-01 3.042800e-01
+2.075000e+02 1.750000e+01 1.750000e+01 1.795700e+00 2.291700e-01 1.699700e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.037300e+00 1.075200e-01 1.064500e-01
+2.800000e+02 2.000000e+01 2.000000e+01 5.956100e-01 7.400100e-02 5.484300e-02
+3.975000e+02 9.750000e+01 9.750000e+01 1.554900e-01 1.658700e-02 1.475700e-02
+6.975000e+02 2.025000e+02 2.025000e+02 7.122200e-03 7.693000e-04 5.454900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d88-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d88-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 5.348700e+00 1.197000e+00 1.742800e+00
+3.750000e+01 1.250000e+01 1.250000e+01 1.122200e+01 2.678700e+00 3.995600e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.078700e+01 2.730100e+00 4.157200e+00
+8.750000e+01 1.250000e+01 1.250000e+01 8.765100e+00 2.285400e+00 3.510600e+00
+1.150000e+02 1.500000e+01 1.500000e+01 6.365800e+00 1.690500e+00 2.623900e+00
+1.450000e+02 1.500000e+01 1.500000e+01 4.535400e+00 1.239000e+00 1.948000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 3.070000e+00 8.363200e-01 1.311800e+00
+2.075000e+02 1.750000e+01 1.750000e+01 1.905700e+00 5.197300e-01 8.125000e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.155900e+00 3.167400e-01 4.947000e-01
+2.800000e+02 2.000000e+01 2.000000e+01 6.816100e-01 1.869100e-01 2.913600e-01
+3.975000e+02 9.750000e+01 9.750000e+01 1.888400e-01 5.226500e-02 8.144700e-02
+6.975000e+02 2.025000e+02 2.025000e+02 9.781400e-03 2.780300e-03 4.349400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d88-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d88-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 5.150100e+00 7.406100e-01 2.057300e+00
+3.750000e+01 1.250000e+01 1.250000e+01 1.166400e+01 2.178500e+00 4.761500e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.152600e+01 2.413900e+00 4.801200e+00
+8.750000e+01 1.250000e+01 1.250000e+01 9.192700e+00 1.649700e+00 3.884100e+00
+1.150000e+02 1.500000e+01 1.500000e+01 6.639500e+00 1.298700e+00 2.947600e+00
+1.450000e+02 1.500000e+01 1.500000e+01 4.673100e+00 9.886800e-01 1.890700e+00
+1.750000e+02 1.500000e+01 1.500000e+01 3.060900e+00 6.205400e-01 1.322500e+00
+2.075000e+02 1.750000e+01 1.750000e+01 1.845400e+00 4.101900e-01 7.583000e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.097200e+00 2.220700e-01 4.785800e-01
+2.800000e+02 2.000000e+01 2.000000e+01 6.320400e-01 1.189400e-01 2.311100e-01
+3.975000e+02 9.750000e+01 9.750000e+01 1.667700e-01 3.584900e-02 5.748000e-02
+6.975000e+02 2.025000e+02 2.025000e+02 9.573600e-03 2.066400e-03 3.171200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d89-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d89-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.385800e+02 3.239514e+01 3.056628e+01
+2.250000e-01 7.500000e-02 7.500000e-02 1.951300e+02 4.141045e+01 3.119311e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.169200e+02 3.649278e+01 3.761133e+01
+4.500000e-01 5.000000e-02 5.000000e-02 3.687800e+02 4.708633e+01 4.735659e+01
+5.500000e-01 5.000000e-02 5.000000e-02 5.973400e+02 6.784832e+01 6.418598e+01
+6.250000e-01 2.500000e-02 2.500000e-02 1.009600e+03 9.293142e+01 8.422428e+01
+6.750000e-01 2.500000e-02 2.500000e-02 1.253100e+03 9.759674e+01 1.006047e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.722200e+03 1.415085e+02 1.488028e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.591500e+03 1.797726e+02 1.835356e+02
+8.250000e-01 2.500000e-02 2.500000e-02 3.765200e+03 2.764705e+02 2.684448e+02
+8.750000e-01 2.500000e-02 2.500000e-02 5.168800e+03 3.773654e+02 3.749603e+02
+9.250000e-01 2.500000e-02 2.500000e-02 6.703100e+03 4.744396e+02 4.736964e+02
+9.750000e-01 2.500000e-02 2.500000e-02 8.541300e+03 6.196934e+02 6.302609e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d89-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d89-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.712500e+02 2.328800e+01 2.031300e+01
+2.250000e-01 7.500000e-02 7.500000e-02 2.007800e+02 2.529700e+01 2.049800e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.708900e+02 3.701700e+01 3.215900e+01
+4.500000e-01 5.000000e-02 5.000000e-02 3.795500e+02 4.916400e+01 5.146200e+01
+5.500000e-01 5.000000e-02 5.000000e-02 5.875100e+02 7.516400e+01 7.132500e+01
+6.250000e-01 2.500000e-02 2.500000e-02 8.664900e+02 1.208400e+02 1.000100e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.145400e+03 1.594900e+02 1.317400e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.577700e+03 2.174400e+02 1.737000e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.162400e+03 2.583800e+02 2.217400e+02
+8.250000e-01 2.500000e-02 2.500000e-02 2.978000e+03 3.504300e+02 3.354300e+02
+8.750000e-01 2.500000e-02 2.500000e-02 4.086900e+03 4.855200e+02 4.219000e+02
+9.250000e-01 2.500000e-02 2.500000e-02 5.412700e+03 6.471000e+02 5.975100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 6.664600e+03 8.707200e+02 6.753600e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d89-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d89-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.762300e+02 4.934000e+01 7.879400e+01
+2.250000e-01 7.500000e-02 7.500000e-02 2.058900e+02 5.747000e+01 9.143700e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.711900e+02 7.649000e+01 1.232500e+02
+4.500000e-01 5.000000e-02 5.000000e-02 3.657500e+02 1.012500e+02 1.611000e+02
+5.500000e-01 5.000000e-02 5.000000e-02 5.852100e+02 1.654900e+02 2.637600e+02
+6.250000e-01 2.500000e-02 2.500000e-02 8.188900e+02 2.243600e+02 3.522600e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.100100e+03 2.997600e+02 4.705600e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.521600e+03 4.130900e+02 6.481000e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.130800e+03 5.686900e+02 8.822000e+02
+8.250000e-01 2.500000e-02 2.500000e-02 3.007200e+03 7.898300e+02 1.216600e+03
+8.750000e-01 2.500000e-02 2.500000e-02 4.251700e+03 1.086500e+03 1.657100e+03
+9.250000e-01 2.500000e-02 2.500000e-02 5.916400e+03 1.462500e+03 2.204800e+03
+9.750000e-01 2.500000e-02 2.500000e-02 7.612900e+03 1.816500e+03 2.698500e+03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d89-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d89-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.605600e+02 3.541500e+01 6.150200e+01
+2.250000e-01 7.500000e-02 7.500000e-02 1.868100e+02 3.720000e+01 8.916700e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.435700e+02 5.204100e+01 1.019900e+02
+4.500000e-01 5.000000e-02 5.000000e-02 3.409500e+02 6.501800e+01 1.514000e+02
+5.500000e-01 5.000000e-02 5.000000e-02 5.397700e+02 1.168500e+02 2.200200e+02
+6.250000e-01 2.500000e-02 2.500000e-02 8.286900e+02 1.730700e+02 3.025800e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.105300e+03 2.099200e+02 4.431300e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.575100e+03 3.042800e+02 6.656500e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.232000e+03 3.918100e+02 1.008600e+03
+8.250000e-01 2.500000e-02 2.500000e-02 3.217700e+03 6.539700e+02 1.331300e+03
+8.750000e-01 2.500000e-02 2.500000e-02 4.515100e+03 8.594000e+02 1.925600e+03
+9.250000e-01 2.500000e-02 2.500000e-02 6.198000e+03 1.264400e+03 2.500100e+03
+9.750000e-01 2.500000e-02 2.500000e-02 7.723100e+03 1.387900e+03 3.173800e+03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d90-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d90-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 5.077600e+02 3.462433e+01 3.362834e+01
+2.600000e+00 2.000000e-01 2.000000e-01 6.270400e+02 3.931143e+01 3.957405e+01
+3.000000e+00 2.000000e-01 2.000000e-01 7.263600e+02 4.470956e+01 4.586098e+01
+3.400000e+00 2.000000e-01 2.000000e-01 7.859100e+02 5.164003e+01 5.295506e+01
+3.800000e+00 2.000000e-01 2.000000e-01 7.077900e+02 5.530817e+01 5.384023e+01
+4.200000e+00 2.000000e-01 2.000000e-01 4.398700e+02 3.673335e+01 3.512347e+01
+4.600000e+00 2.000000e-01 2.000000e-01 2.400300e+02 2.221590e+01 2.274785e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.154700e+02 1.446053e+01 1.405010e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.243200e+01 9.426323e+00 6.896334e+00
+6.200000e+00 2.000000e-01 2.000000e-01 1.202700e+01 3.301047e+00 3.078377e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.478100e-01 3.664103e-01 3.132278e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d90-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d90-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.167600e+02 4.547600e+01 4.181200e+01
+2.600000e+00 2.000000e-01 2.000000e-01 5.068400e+02 5.699200e+01 4.931700e+01
+3.000000e+00 2.000000e-01 2.000000e-01 6.012200e+02 7.730800e+01 6.630100e+01
+3.400000e+00 2.000000e-01 2.000000e-01 6.554000e+02 8.032000e+01 7.149600e+01
+3.800000e+00 2.000000e-01 2.000000e-01 5.947600e+02 7.543400e+01 6.385300e+01
+4.200000e+00 2.000000e-01 2.000000e-01 3.693700e+02 5.368700e+01 4.448200e+01
+4.600000e+00 2.000000e-01 2.000000e-01 2.112100e+02 2.990600e+01 2.417500e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.102300e+02 1.471400e+01 1.419000e+01
+5.600000e+00 4.000000e-01 4.000000e-01 3.959900e+01 5.101100e+00 4.811500e+00
+6.200000e+00 2.000000e-01 2.000000e-01 1.069200e+01 2.646100e+00 1.101200e+00
+7.600000e+00 1.200000e+00 1.200000e+00 8.500700e-01 6.860900e-02 1.690100e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d90-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d90-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 5.380500e+02 1.362000e+02 2.055300e+02
+2.600000e+00 2.000000e-01 2.000000e-01 6.000900e+02 1.519000e+02 2.296500e+02
+3.000000e+00 2.000000e-01 2.000000e-01 6.491400e+02 1.640400e+02 2.488300e+02
+3.400000e+00 2.000000e-01 2.000000e-01 6.621100e+02 1.685000e+02 2.572100e+02
+3.800000e+00 2.000000e-01 2.000000e-01 5.639300e+02 1.428500e+02 2.187200e+02
+4.200000e+00 2.000000e-01 2.000000e-01 3.478300e+02 9.099600e+01 1.415100e+02
+4.600000e+00 2.000000e-01 2.000000e-01 1.921300e+02 5.169100e+01 8.195400e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.011100e+02 2.798900e+01 4.487600e+01
+5.600000e+00 4.000000e-01 4.000000e-01 3.720400e+01 1.085000e+01 1.797400e+01
+6.200000e+00 2.000000e-01 2.000000e-01 9.907200e+00 3.151000e+00 5.605000e+00
+7.600000e+00 1.200000e+00 1.200000e+00 8.464300e-01 2.840000e-01 5.216000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d90-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d90-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 5.026400e+02 1.035700e+02 2.239800e+02
+2.600000e+00 2.000000e-01 2.000000e-01 5.912000e+02 1.082000e+02 2.596600e+02
+3.000000e+00 2.000000e-01 2.000000e-01 6.717900e+02 1.423900e+02 2.722900e+02
+3.400000e+00 2.000000e-01 2.000000e-01 6.879300e+02 1.342800e+02 2.848200e+02
+3.800000e+00 2.000000e-01 2.000000e-01 5.936200e+02 1.139300e+02 2.469100e+02
+4.200000e+00 2.000000e-01 2.000000e-01 3.625100e+02 6.665900e+01 1.489800e+02
+4.600000e+00 2.000000e-01 2.000000e-01 2.069800e+02 4.201700e+01 8.118200e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.113600e+02 1.582500e+01 3.950300e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.353700e+01 6.415000e+00 1.580300e+01
+6.200000e+00 2.000000e-01 2.000000e-01 1.305200e+01 2.727600e+00 2.389800e+00
+7.600000e+00 1.200000e+00 1.200000e+00 1.263800e+00 1.343500e-01 3.251800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d91-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d91-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.163300e+01 1.457982e+00 1.409526e+00
+1.050000e+02 1.000000e+01 1.000000e+01 1.279900e+01 1.308648e+00 1.298884e+00
+1.275000e+02 1.250000e+01 1.250000e+01 1.197200e+01 9.187943e-01 9.310671e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.040900e+01 6.983664e-01 6.436609e-01
+1.775000e+02 1.250000e+01 1.250000e+01 8.399800e+00 4.930730e-01 4.808062e-01
+2.050000e+02 1.500000e+01 1.500000e+01 6.012400e+00 3.049790e-01 2.986977e-01
+2.350000e+02 1.500000e+01 1.500000e+01 3.820000e+00 1.819593e-01 1.815982e-01
+2.650000e+02 1.500000e+01 1.500000e+01 2.410300e+00 1.304611e-01 1.238769e-01
+2.975000e+02 1.750000e+01 1.750000e+01 1.454800e+00 8.170435e-02 8.658265e-02
+3.325000e+02 1.750000e+01 1.750000e+01 8.123100e-01 5.041611e-02 5.304323e-02
+3.700000e+02 2.000000e+01 2.000000e+01 4.905100e-01 4.323071e-02 4.585957e-02
+4.125000e+02 2.250000e+01 2.250000e+01 2.656600e-01 2.211866e-02 2.000179e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.558900e-01 1.491181e-02 1.383376e-02
+5.300000e+02 5.000000e+01 5.000000e+01 6.006300e-02 7.026720e-03 6.682852e-03
+6.325000e+02 5.250000e+01 5.250000e+01 1.817100e-02 3.713347e-03 3.630039e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.412400e-03 8.271355e-04 8.225211e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d91-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d91-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 9.167100e+00 1.467600e+00 1.126000e+00
+1.050000e+02 1.000000e+01 1.000000e+01 1.040400e+01 1.455700e+00 1.138200e+00
+1.275000e+02 1.250000e+01 1.250000e+01 9.984400e+00 1.281800e+00 1.259100e+00
+1.525000e+02 1.250000e+01 1.250000e+01 8.767000e+00 1.040500e+00 9.026900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 7.167400e+00 8.299700e-01 7.835400e-01
+2.050000e+02 1.500000e+01 1.500000e+01 5.145300e+00 6.172900e-01 4.774200e-01
+2.350000e+02 1.500000e+01 1.500000e+01 3.313300e+00 3.656800e-01 3.232700e-01
+2.650000e+02 1.500000e+01 1.500000e+01 2.088400e+00 2.361100e-01 1.918000e-01
+2.975000e+02 1.750000e+01 1.750000e+01 1.270200e+00 1.327000e-01 1.306500e-01
+3.325000e+02 1.750000e+01 1.750000e+01 7.566400e-01 8.487200e-02 4.965600e-02
+3.700000e+02 2.000000e+01 2.000000e+01 4.394200e-01 4.849800e-02 4.406300e-02
+4.125000e+02 2.250000e+01 2.250000e+01 2.469700e-01 2.745000e-02 2.244800e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.370800e-01 1.516300e-02 1.641200e-02
+5.300000e+02 5.000000e+01 5.000000e+01 5.797400e-02 6.763700e-03 3.551500e-03
+6.325000e+02 5.250000e+01 5.250000e+01 1.741100e-02 2.438800e-03 1.845500e-03
+8.425000e+02 1.575000e+02 1.575000e+02 2.787800e-03 4.042100e-04 3.313600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d91-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d91-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 8.009900e+00 2.028500e+00 3.149900e+00
+1.050000e+02 1.000000e+01 1.000000e+01 9.429800e+00 2.366500e+00 3.623600e+00
+1.275000e+02 1.250000e+01 1.250000e+01 9.781600e+00 2.490900e+00 3.820600e+00
+1.525000e+02 1.250000e+01 1.250000e+01 9.104700e+00 2.301000e+00 3.499600e+00
+1.775000e+02 1.250000e+01 1.250000e+01 8.004500e+00 2.031700e+00 3.087800e+00
+2.050000e+02 1.500000e+01 1.500000e+01 5.844000e+00 1.498000e+00 2.286500e+00
+2.350000e+02 1.500000e+01 1.500000e+01 3.926600e+00 1.018300e+00 1.557100e+00
+2.650000e+02 1.500000e+01 1.500000e+01 2.567600e+00 6.739900e-01 1.032700e+00
+2.975000e+02 1.750000e+01 1.750000e+01 1.564700e+00 4.148300e-01 6.377500e-01
+3.325000e+02 1.750000e+01 1.750000e+01 9.581800e-01 2.569600e-01 3.963400e-01
+3.700000e+02 2.000000e+01 2.000000e+01 5.759000e-01 1.558000e-01 2.403300e-01
+4.125000e+02 2.250000e+01 2.250000e+01 3.337600e-01 9.139300e-02 1.414900e-01
+4.575000e+02 2.250000e+01 2.250000e+01 1.840600e-01 5.042800e-02 7.824000e-02
+5.300000e+02 5.000000e+01 5.000000e+01 7.972500e-02 2.227800e-02 3.464600e-02
+6.325000e+02 5.250000e+01 5.250000e+01 2.374100e-02 6.799300e-03 1.069900e-02
+8.425000e+02 1.575000e+02 1.575000e+02 3.652400e-03 1.064200e-03 1.681200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d91-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d91-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 8.388400e+00 1.329500e+00 3.479200e+00
+1.050000e+02 1.000000e+01 1.000000e+01 9.899200e+00 1.960200e+00 4.097100e+00
+1.275000e+02 1.250000e+01 1.250000e+01 1.011600e+01 2.010500e+00 4.103000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 9.440600e+00 1.792300e+00 3.947200e+00
+1.775000e+02 1.250000e+01 1.250000e+01 8.054100e+00 1.544000e+00 3.254500e+00
+2.050000e+02 1.500000e+01 1.500000e+01 5.884600e+00 1.114000e+00 2.684300e+00
+2.350000e+02 1.500000e+01 1.500000e+01 3.947500e+00 8.044100e-01 1.603300e+00
+2.650000e+02 1.500000e+01 1.500000e+01 2.523800e+00 5.188700e-01 1.095500e+00
+2.975000e+02 1.750000e+01 1.750000e+01 1.559100e+00 2.811500e-01 7.008000e-01
+3.325000e+02 1.750000e+01 1.750000e+01 9.881800e-01 2.219100e-01 3.556300e-01
+3.700000e+02 2.000000e+01 2.000000e+01 5.858200e-01 1.187100e-01 2.147400e-01
+4.125000e+02 2.250000e+01 2.250000e+01 3.423300e-01 8.872900e-02 1.057400e-01
+4.575000e+02 2.250000e+01 2.250000e+01 1.915600e-01 3.840500e-02 7.859200e-02
+5.300000e+02 5.000000e+01 5.000000e+01 8.508900e-02 1.874100e-02 3.255600e-02
+6.325000e+02 5.250000e+01 5.250000e+01 2.763300e-02 3.482600e-03 1.520300e-02
+8.425000e+02 1.575000e+02 1.575000e+02 4.549000e-03 1.121400e-03 4.244900e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d92-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d92-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 2.004000e+03 2.669950e+02 2.532186e+02
+1.000000e-01 5.000000e-02 5.000000e-02 2.112200e+03 2.638339e+02 2.532517e+02
+2.000000e-01 5.000000e-02 5.000000e-02 2.018900e+03 2.589280e+02 2.464791e+02
+3.000000e-01 5.000000e-02 5.000000e-02 2.029900e+03 2.615069e+02 2.640057e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.732300e+03 2.633165e+02 2.499944e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.337000e+03 2.024652e+02 1.992508e+02
+6.000000e-01 5.000000e-02 5.000000e-02 1.216100e+03 1.879114e+02 1.863348e+02
+7.000000e-01 5.000000e-02 5.000000e-02 9.821400e+02 1.492019e+02 1.446003e+02
+8.000000e-01 5.000000e-02 5.000000e-02 6.549300e+02 9.720235e+01 9.906715e+01
+9.250000e-01 7.500000e-02 7.500000e-02 4.014700e+02 6.243126e+01 6.498550e+01
+1.100000e+00 1.000000e-01 1.000000e-01 2.652300e+02 5.174281e+01 5.190148e+01
+1.350000e+00 1.500000e-01 1.500000e-01 1.115600e+02 2.057846e+01 2.120185e+01
+1.650000e+00 1.500000e-01 1.500000e-01 3.094300e+01 7.743732e+00 7.619970e+00
+2.050000e+00 2.500000e-01 2.500000e-01 6.776000e+00 2.000931e+00 1.900796e+00
+2.650000e+00 3.500000e-01 3.500000e-01 6.510400e-01 3.417055e-01 3.102679e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d92-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d92-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.567400e+03 2.039300e+02 1.984600e+02
+1.000000e-01 5.000000e-02 5.000000e-02 1.577700e+03 2.285200e+02 1.834500e+02
+2.000000e-01 5.000000e-02 5.000000e-02 1.606300e+03 2.160100e+02 2.042200e+02
+3.000000e-01 5.000000e-02 5.000000e-02 1.659400e+03 2.168000e+02 2.131000e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.451000e+03 1.935200e+02 1.638500e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.115300e+03 1.495400e+02 1.217100e+02
+6.000000e-01 5.000000e-02 5.000000e-02 9.767500e+02 1.380700e+02 1.037600e+02
+7.000000e-01 5.000000e-02 5.000000e-02 7.754900e+02 1.041100e+02 9.247600e+01
+8.000000e-01 5.000000e-02 5.000000e-02 5.248100e+02 6.686700e+01 1.333900e+02
+9.250000e-01 7.500000e-02 7.500000e-02 3.386100e+02 4.272100e+01 3.808000e+01
+1.100000e+00 1.000000e-01 1.000000e-01 1.891000e+02 2.639800e+01 1.704100e+01
+1.350000e+00 1.500000e-01 1.500000e-01 7.950200e+01 1.129200e+01 8.854900e+00
+1.650000e+00 1.500000e-01 1.500000e-01 2.520400e+01 3.801300e+00 2.876400e+00
+2.050000e+00 2.500000e-01 2.500000e-01 4.911000e+00 7.866200e-01 7.678600e-01
+2.650000e+00 3.500000e-01 3.500000e-01 2.383100e-01 7.195200e-02 7.958000e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d92-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d92-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.415600e+03 4.393400e+02 7.146200e+02
+1.000000e-01 5.000000e-02 5.000000e-02 1.422500e+03 4.407900e+02 7.171400e+02
+2.000000e-01 5.000000e-02 5.000000e-02 1.396600e+03 4.335900e+02 7.068400e+02
+3.000000e-01 5.000000e-02 5.000000e-02 1.427500e+03 4.438600e+02 7.240300e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.282900e+03 4.035400e+02 6.628100e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.128500e+03 3.659100e+02 6.104800e+02
+6.000000e-01 5.000000e-02 5.000000e-02 1.089800e+03 3.574300e+02 5.994600e+02
+7.000000e-01 5.000000e-02 5.000000e-02 8.591800e+02 2.823500e+02 4.738800e+02
+8.000000e-01 5.000000e-02 5.000000e-02 5.732900e+02 1.889500e+02 3.177500e+02
+9.250000e-01 7.500000e-02 7.500000e-02 3.983700e+02 1.341700e+02 2.278800e+02
+1.100000e+00 1.000000e-01 1.000000e-01 2.157300e+02 7.223900e+01 1.223700e+02
+1.350000e+00 1.500000e-01 1.500000e-01 9.648200e+01 3.232400e+01 5.436700e+01
+1.650000e+00 1.500000e-01 1.500000e-01 3.548600e+01 1.216800e+01 2.033000e+01
+2.050000e+00 2.500000e-01 2.500000e-01 5.952500e+00 2.100900e+00 3.647700e+00
+2.650000e+00 3.500000e-01 3.500000e-01 2.716300e-01 9.814000e-02 1.736900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d92-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d92-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.855800e+03 4.407700e+02 8.686100e+02
+1.000000e-01 5.000000e-02 5.000000e-02 1.858100e+03 4.098600e+02 8.931200e+02
+2.000000e-01 5.000000e-02 5.000000e-02 1.868800e+03 3.979300e+02 8.663800e+02
+3.000000e-01 5.000000e-02 5.000000e-02 1.908000e+03 4.346400e+02 9.787100e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.621100e+03 3.630100e+02 7.886400e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.193600e+03 2.611300e+02 5.891200e+02
+6.000000e-01 5.000000e-02 5.000000e-02 1.053000e+03 2.471300e+02 5.153900e+02
+7.000000e-01 5.000000e-02 5.000000e-02 8.637500e+02 1.992600e+02 3.999800e+02
+8.000000e-01 5.000000e-02 5.000000e-02 5.636500e+02 1.177500e+02 2.916200e+02
+9.250000e-01 7.500000e-02 7.500000e-02 3.738600e+02 8.372500e+01 1.720400e+02
+1.100000e+00 1.000000e-01 1.000000e-01 2.090100e+02 5.066300e+01 9.360700e+01
+1.350000e+00 1.500000e-01 1.500000e-01 8.991900e+01 1.970700e+01 4.232200e+01
+1.650000e+00 1.500000e-01 1.500000e-01 2.839400e+01 6.484700e+00 1.468300e+01
+2.050000e+00 2.500000e-01 2.500000e-01 5.998800e+00 1.140700e+00 2.396100e+00
+2.650000e+00 3.500000e-01 3.500000e-01 2.502100e-01 1.134800e-01 2.568700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d93-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d93-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.854500e+03 1.392862e+02 1.424013e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.729500e+03 1.256021e+02 1.309524e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.974600e+03 1.342602e+02 1.416856e+02
+1.750000e-01 2.500000e-02 2.500000e-02 2.076100e+03 1.712336e+02 1.392548e+02
+2.250000e-01 2.500000e-02 2.500000e-02 2.149300e+03 1.787284e+02 1.643144e+02
+2.750000e-01 2.500000e-02 2.500000e-02 2.256600e+03 1.661413e+02 1.631526e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.305200e+03 1.714270e+02 1.676101e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.442700e+03 1.706935e+02 1.573677e+02
+4.250000e-01 2.500000e-02 2.500000e-02 2.232300e+03 1.646229e+02 1.437125e+02
+4.750000e-01 2.500000e-02 2.500000e-02 2.009800e+03 1.755803e+02 1.795133e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.971700e+03 1.359661e+02 1.429800e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.947500e+03 1.238870e+02 1.337143e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.715400e+03 1.167966e+02 1.102475e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.491100e+03 9.812216e+01 9.746407e+01
+7.250000e-01 2.500000e-02 2.500000e-02 1.242800e+03 7.367909e+01 8.344958e+01
+7.750000e-01 2.500000e-02 2.500000e-02 9.860700e+02 7.374213e+01 6.988655e+01
+8.250000e-01 2.500000e-02 2.500000e-02 7.999100e+02 5.148815e+01 5.561172e+01
+8.750000e-01 2.500000e-02 2.500000e-02 6.398900e+02 3.807850e+01 4.632887e+01
+9.250000e-01 2.500000e-02 2.500000e-02 5.029500e+02 3.365246e+01 3.713072e+01
+9.750000e-01 2.500000e-02 2.500000e-02 4.017500e+02 2.904657e+01 2.896229e+01
+1.025000e+00 2.500000e-02 2.500000e-02 3.191600e+02 2.211350e+01 2.131723e+01
+1.075000e+00 2.500000e-02 2.500000e-02 2.288100e+02 1.785009e+01 1.773006e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.711300e+02 1.426725e+01 1.471588e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.507500e+02 1.353921e+01 1.257293e+01
+1.250000e+00 5.000000e-02 5.000000e-02 8.632100e+01 7.585372e+00 7.867592e+00
+1.350000e+00 5.000000e-02 5.000000e-02 5.007300e+01 5.882454e+00 5.621114e+00
+1.500000e+00 1.000000e-01 1.000000e-01 1.821000e+01 2.317406e+00 2.084775e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.168300e+00 5.117025e-01 5.212289e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d93-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d93-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.508200e+03 1.584600e+02 1.483800e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.531200e+03 1.624900e+02 1.401100e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.592200e+03 1.575500e+02 1.578200e+02
+1.750000e-01 2.500000e-02 2.500000e-02 1.680400e+03 1.817200e+02 1.455900e+02
+2.250000e-01 2.500000e-02 2.500000e-02 1.802000e+03 2.159100e+02 1.758000e+02
+2.750000e-01 2.500000e-02 2.500000e-02 1.880300e+03 2.296900e+02 1.994500e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.011100e+03 2.735800e+02 1.490700e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.030500e+03 2.511100e+02 2.315600e+02
+4.250000e-01 2.500000e-02 2.500000e-02 1.942200e+03 2.450300e+02 1.887100e+02
+4.750000e-01 2.500000e-02 2.500000e-02 1.793500e+03 2.210800e+02 2.065000e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.694300e+03 2.224300e+02 1.795100e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.559500e+03 2.420200e+02 1.761500e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.435800e+03 1.818300e+02 3.443900e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.236900e+03 1.634400e+02 1.504100e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.026400e+03 1.334100e+02 1.162000e+02
+7.750000e-01 2.500000e-02 2.500000e-02 8.407000e+02 1.224400e+02 1.200900e+02
+8.250000e-01 2.500000e-02 2.500000e-02 6.708800e+02 9.013300e+01 8.450900e+01
+8.750000e-01 2.500000e-02 2.500000e-02 5.343000e+02 8.322600e+01 5.769500e+01
+9.250000e-01 2.500000e-02 2.500000e-02 4.131000e+02 6.351800e+01 5.190300e+01
+9.750000e-01 2.500000e-02 2.500000e-02 3.232700e+02 4.456300e+01 3.899100e+01
+1.025000e+00 2.500000e-02 2.500000e-02 2.480300e+02 3.750200e+01 2.868300e+01
+1.075000e+00 2.500000e-02 2.500000e-02 1.878100e+02 2.796400e+01 2.714800e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.422900e+02 1.981100e+01 2.038300e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.046500e+02 1.639800e+01 1.343100e+01
+1.250000e+00 5.000000e-02 5.000000e-02 7.013100e+01 1.038700e+01 9.331100e+00
+1.350000e+00 5.000000e-02 5.000000e-02 3.817100e+01 6.390100e+00 6.026600e+00
+1.500000e+00 1.000000e-01 1.000000e-01 1.528800e+01 2.495700e+00 2.875200e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.319600e+00 4.327500e-01 5.803400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d93-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d93-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.788800e+03 4.681900e+02 7.238800e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.798500e+03 4.677900e+02 7.199600e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.840000e+03 4.768300e+02 7.337500e+02
+1.750000e-01 2.500000e-02 2.500000e-02 1.909400e+03 4.917200e+02 7.537700e+02
+2.250000e-01 2.500000e-02 2.500000e-02 1.971700e+03 5.035000e+02 7.702000e+02
+2.750000e-01 2.500000e-02 2.500000e-02 2.027600e+03 5.157100e+02 7.892800e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.079500e+03 5.252400e+02 8.001700e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.055100e+03 5.182200e+02 7.898700e+02
+4.250000e-01 2.500000e-02 2.500000e-02 1.991800e+03 5.054600e+02 7.726500e+02
+4.750000e-01 2.500000e-02 2.500000e-02 1.830700e+03 4.626700e+02 7.038300e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.718500e+03 4.411100e+02 6.780600e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.550600e+03 3.924800e+02 5.988700e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.404800e+03 3.572300e+02 5.442400e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.200800e+03 3.045100e+02 4.634400e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.006200e+03 2.554100e+02 3.888200e+02
+7.750000e-01 2.500000e-02 2.500000e-02 8.333700e+02 2.132100e+02 3.256600e+02
+8.250000e-01 2.500000e-02 2.500000e-02 6.624400e+02 1.707800e+02 2.614200e+02
+8.750000e-01 2.500000e-02 2.500000e-02 5.341500e+02 1.387700e+02 2.131900e+02
+9.250000e-01 2.500000e-02 2.500000e-02 4.061800e+02 1.059300e+02 1.627200e+02
+9.750000e-01 2.500000e-02 2.500000e-02 3.218500e+02 8.378900e+01 1.285100e+02
+1.025000e+00 2.500000e-02 2.500000e-02 2.528100e+02 6.580500e+01 1.010100e+02
+1.075000e+00 2.500000e-02 2.500000e-02 1.970200e+02 5.147500e+01 7.893100e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.443200e+02 3.835200e+01 5.912800e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.095400e+02 2.923700e+01 4.525200e+01
+1.250000e+00 5.000000e-02 5.000000e-02 7.723600e+01 2.197000e+01 3.454800e+01
+1.350000e+00 5.000000e-02 5.000000e-02 3.828300e+01 1.039300e+01 1.623600e+01
+1.500000e+00 1.000000e-01 1.000000e-01 1.613800e+01 4.441800e+00 6.957200e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.361900e+00 7.088000e-01 1.171300e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d93-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d93-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.544100e+03 2.433100e+02 5.838400e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.597200e+03 2.847700e+02 5.953500e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.665800e+03 2.686200e+02 6.318100e+02
+1.750000e-01 2.500000e-02 2.500000e-02 1.780800e+03 3.161100e+02 6.276500e+02
+2.250000e-01 2.500000e-02 2.500000e-02 1.905000e+03 3.644000e+02 7.595300e+02
+2.750000e-01 2.500000e-02 2.500000e-02 2.031500e+03 3.760100e+02 8.038700e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.108900e+03 3.883000e+02 8.859400e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.175300e+03 4.343800e+02 8.931900e+02
+4.250000e-01 2.500000e-02 2.500000e-02 2.099400e+03 4.185100e+02 8.907700e+02
+4.750000e-01 2.500000e-02 2.500000e-02 1.997300e+03 4.251100e+02 8.510400e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.847200e+03 3.461700e+02 8.248800e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.738800e+03 3.575200e+02 7.373800e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.571300e+03 3.383700e+02 7.226100e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.368100e+03 2.936400e+02 5.562500e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.139600e+03 2.698000e+02 4.358800e+02
+7.750000e-01 2.500000e-02 2.500000e-02 9.078300e+02 1.346000e+02 4.310700e+02
+8.250000e-01 2.500000e-02 2.500000e-02 7.482600e+02 1.676100e+02 3.235800e+02
+8.750000e-01 2.500000e-02 2.500000e-02 5.713600e+02 1.011600e+02 3.026700e+02
+9.250000e-01 2.500000e-02 2.500000e-02 4.575800e+02 9.798500e+01 2.140200e+02
+9.750000e-01 2.500000e-02 2.500000e-02 3.557200e+02 6.552400e+01 1.719200e+02
+1.025000e+00 2.500000e-02 2.500000e-02 2.746400e+02 6.075400e+01 1.240900e+02
+1.075000e+00 2.500000e-02 2.500000e-02 2.044100e+02 4.900500e+01 9.549500e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.605700e+02 3.927200e+01 6.517000e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.158700e+02 2.070900e+01 6.710000e+01
+1.250000e+00 5.000000e-02 5.000000e-02 7.638900e+01 1.726900e+01 3.369100e+01
+1.350000e+00 5.000000e-02 5.000000e-02 3.885300e+01 8.890800e+00 2.040400e+01
+1.500000e+00 1.000000e-01 1.000000e-01 1.660100e+01 3.015200e+00 9.609400e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.688100e+00 5.346700e-01 1.147400e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d94-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d94-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.012600e+03 5.337420e+01 5.472897e+01
+1.000000e+00 5.000000e-01 5.000000e-01 4.836400e+02 4.265705e+01 4.042195e+01
+2.000000e+00 5.000000e-01 5.000000e-01 1.522800e+02 1.960786e+01 1.954737e+01
+3.000000e+00 5.000000e-01 5.000000e-01 3.855700e+01 7.497954e+00 6.466930e+00
+4.000000e+00 5.000000e-01 5.000000e-01 7.925500e+00 2.062354e+00 1.694143e+00
+6.500000e+00 2.000000e+00 2.000000e+00 2.858000e+00 9.319546e-01 8.598858e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d94-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d94-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.509500e+02 1.008000e+02 8.228700e+01
+1.000000e+00 5.000000e-01 5.000000e-01 4.064600e+02 5.521900e+01 4.595000e+01
+2.000000e+00 5.000000e-01 5.000000e-01 1.250100e+02 1.633900e+01 1.555100e+01
+3.000000e+00 5.000000e-01 5.000000e-01 3.235100e+01 4.899000e+00 3.842200e+00
+4.000000e+00 5.000000e-01 5.000000e-01 7.495600e+00 9.653900e-01 1.432100e+00
+6.500000e+00 2.000000e+00 2.000000e+00 2.046900e+00 3.251200e-01 4.462700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d94-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d94-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.408100e+02 2.110000e+02 3.068000e+02
+1.000000e+00 5.000000e-01 5.000000e-01 4.470200e+02 1.320300e+02 2.105300e+02
+2.000000e+00 5.000000e-01 5.000000e-01 1.011600e+02 3.435000e+01 5.802700e+01
+3.000000e+00 5.000000e-01 5.000000e-01 6.145900e-01 0.000000e+00 0.000000e+00
+4.000000e+00 5.000000e-01 5.000000e-01 2.000000e-99 0.000000e+00 0.000000e+00
+6.500000e+00 2.000000e+00 2.000000e+00 2.000000e-99 0.000000e+00 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d94-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d94-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.911000e+02 1.509400e+02 3.318100e+02
+1.000000e+00 5.000000e-01 5.000000e-01 4.570200e+02 1.046700e+02 2.100800e+02
+2.000000e+00 5.000000e-01 5.000000e-01 1.435400e+02 3.286200e+01 7.379000e+01
+3.000000e+00 5.000000e-01 5.000000e-01 3.508500e+01 7.124300e+00 1.769100e+01
+4.000000e+00 5.000000e-01 5.000000e-01 6.307400e+00 9.342100e-01 3.861500e+00
+6.500000e+00 2.000000e+00 2.000000e+00 1.238500e+00 2.545000e-01 3.283900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d95-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d95-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t95
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 5.874900e-02 1.324906e-02 1.240497e-02
+7.500000e+01 2.500000e+01 2.500000e+01 9.498400e-02 1.592544e-02 1.470177e-02
+1.300000e+02 3.000000e+01 3.000000e+01 4.586100e-02 8.749442e-03 7.678501e-03
+2.300000e+02 7.000000e+01 7.000000e+01 1.632200e-02 3.132506e-03 3.457378e-03
+5.150000e+02 2.150000e+02 2.150000e+02 1.006100e-03 5.756198e-04 5.664343e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d95-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d95-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t95
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 6.033900e-02 5.201800e-03 5.724300e-03
+7.500000e+01 2.500000e+01 2.500000e+01 7.762200e-02 1.063500e-02 7.972400e-03
+1.300000e+02 3.000000e+01 3.000000e+01 5.217900e-02 6.130000e-03 5.684300e-03
+2.300000e+02 7.000000e+01 7.000000e+01 2.047900e-02 2.249500e-03 2.401700e-03
+5.150000e+02 2.150000e+02 2.150000e+02 2.106100e-03 3.194200e-04 3.445200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d95-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d95-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t95
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 8.308500e-02 1.079000e-02 2.195600e-02
+7.500000e+01 2.500000e+01 2.500000e+01 1.041400e-01 1.671300e-02 4.075200e-02
+1.300000e+02 3.000000e+01 3.000000e+01 6.528800e-02 1.279000e-02 1.865800e-02
+2.300000e+02 7.000000e+01 7.000000e+01 2.661100e-02 5.735800e-03 1.306200e-02
+5.150000e+02 2.150000e+02 2.150000e+02 2.825200e-03 6.625600e-04 8.601000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d96-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d96-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.427500e+00 8.575259e-01 8.622934e-01
+8.000000e-01 1.000000e-01 1.000000e-01 2.164200e+01 3.867042e+00 3.248226e+00
+9.500000e-01 5.000000e-02 5.000000e-02 7.270800e+01 1.019935e+01 9.433521e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d96-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d96-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 3.398700e+00 3.200700e-01 6.315900e-01
+8.000000e-01 1.000000e-01 1.000000e-01 2.394200e+01 3.318200e+00 2.258000e+00
+9.500000e-01 5.000000e-02 5.000000e-02 6.659700e+01 6.209700e+00 4.462200e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d96-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d96-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.158000e+00 9.062200e-01 1.287400e+00
+8.000000e-01 1.000000e-01 1.000000e-01 2.984100e+01 4.913000e+00 8.748200e+00
+9.500000e-01 5.000000e-02 5.000000e-02 9.393500e+01 1.526800e+01 3.573200e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d97-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d97-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.042000e+00 2.180337e-01 2.166378e-01
+4.400000e+00 8.000000e-01 8.000000e-01 2.593900e+00 3.371296e-01 3.088335e-01
+5.600000e+00 4.000000e-01 4.000000e-01 4.529700e+00 7.709864e-01 7.392904e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.330800e+00 3.734668e-01 3.154054e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d97-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d97-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.122000e+00 1.535800e-01 1.096500e-01
+4.400000e+00 8.000000e-01 8.000000e-01 2.807700e+00 2.830900e-01 2.426100e-01
+5.600000e+00 4.000000e-01 4.000000e-01 4.789300e+00 6.183900e-01 3.969900e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.352500e+00 1.326300e-01 1.845300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d97-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d97-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.887200e+00 3.199800e-01 1.275400e+00
+4.400000e+00 8.000000e-01 8.000000e-01 3.841200e+00 7.167900e-01 1.204300e+00
+5.600000e+00 4.000000e-01 4.000000e-01 5.183100e+00 9.569800e-01 2.108700e+00
+7.400000e+00 1.400000e+00 1.400000e+00 1.829800e+00 3.144700e-01 3.756300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d98-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d98-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 6.456000e-02 1.790904e-02 1.516966e-02
+1.800000e+02 4.000000e+01 4.000000e+01 4.737800e-02 7.729065e-03 7.460089e-03
+2.675000e+02 4.750000e+01 4.750000e+01 2.025100e-02 3.525959e-03 3.127624e-03
+3.750000e+02 6.000000e+01 6.000000e+01 1.352600e-02 2.489235e-03 2.377726e-03
+5.600000e+02 1.250000e+02 1.250000e+02 6.354100e-03 1.136201e-03 1.153537e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d98-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d98-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 6.004900e-02 6.597700e-03 7.504900e-03
+1.800000e+02 4.000000e+01 4.000000e+01 5.099200e-02 5.523500e-03 4.591400e-03
+2.675000e+02 4.750000e+01 4.750000e+01 2.833200e-02 3.254000e-03 2.663400e-03
+3.750000e+02 6.000000e+01 6.000000e+01 1.361500e-02 1.800900e-03 1.393600e-03
+5.600000e+02 1.250000e+02 1.250000e+02 5.648100e-03 7.691400e-04 7.387400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d98-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d98-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 7.937500e-02 1.064600e-02 2.201400e-02
+1.800000e+02 4.000000e+01 4.000000e+01 5.798500e-02 1.209400e-02 2.093000e-02
+2.675000e+02 4.750000e+01 4.750000e+01 3.645300e-02 7.944700e-03 8.914500e-03
+3.750000e+02 6.000000e+01 6.000000e+01 1.986100e-02 2.817600e-03 8.124700e-03
+5.600000e+02 1.250000e+02 1.250000e+02 9.358400e-03 1.777400e-03 4.263000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d99-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d99-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.587300e+01 5.107230e+00 4.670509e+00
+7.000000e-01 3.000000e-01 3.000000e-01 4.407800e+00 8.937790e-01 8.322673e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d99-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d99-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.650400e+01 2.185400e+00 2.651000e+00
+7.000000e-01 3.000000e-01 3.000000e-01 4.289500e+00 5.409600e-01 6.522500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d99-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d99-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.630900e+01 4.804900e+00 1.328900e+01
+7.000000e-01 3.000000e-01 3.000000e-01 7.093300e+00 1.625500e+00 3.412100e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d100-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d100-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.443200e+01 3.358132e+00 3.450598e+00
+5.250000e-01 1.250000e-01 1.250000e-01 1.136400e+01 3.206306e+00 2.324743e+00
+8.250000e-01 1.750000e-01 1.750000e-01 1.501800e+00 5.158532e-01 5.032079e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d100-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d100-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.707000e+01 2.413500e+00 2.268100e+00
+5.250000e-01 1.250000e-01 1.250000e-01 1.016400e+01 1.639400e+00 1.010900e+00
+8.250000e-01 1.750000e-01 1.750000e-01 1.220900e+00 2.434400e-01 2.627700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d100-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d100-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 3.254600e+01 5.455900e+00 9.249700e+00
+5.250000e-01 1.250000e-01 1.250000e-01 1.723100e+01 2.937000e+00 8.779800e+00
+8.250000e-01 1.750000e-01 1.750000e-01 2.507400e+00 8.521500e-01 7.612800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d101-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d101-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.252300e+00 1.003388e+00 9.687704e-01
+1.000000e+00 5.000000e-01 5.000000e-01 3.073300e+00 6.788961e-01 5.561707e-01
+3.000000e+00 1.500000e+00 1.500000e+00 1.858100e+00 5.350092e-01 5.029681e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d101-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d101-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.735300e+00 7.026900e-01 5.658500e-01
+1.000000e+00 5.000000e-01 5.000000e-01 3.192500e+00 5.716400e-01 2.904800e-01
+3.000000e+00 1.500000e+00 1.500000e+00 1.849300e+00 2.181300e-01 4.216700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d101-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d101-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.037200e+01 1.659300e+00 2.412800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 4.758700e+00 8.353000e-01 2.176900e+00
+3.000000e+00 1.500000e+00 1.500000e+00 3.096500e+00 6.270700e-01 1.623600e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d102-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d102-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.078600e+00 1.375043e-01 1.335721e-01
+5.800000e+02 3.500000e+01 3.500000e+01 8.830000e-01 8.820350e-02 8.160317e-02
+6.550000e+02 4.000000e+01 4.000000e+01 6.802500e-01 6.941339e-02 6.417338e-02
+7.400000e+02 4.500000e+01 4.500000e+01 4.809000e-01 4.593229e-02 4.950006e-02
+8.325000e+02 4.750000e+01 4.750000e+01 3.027500e-01 3.592337e-02 3.305425e-02
+9.325000e+02 5.250000e+01 5.250000e+01 2.094700e-01 1.978769e-02 1.908621e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.608800e-01 1.379026e-02 1.439896e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.078200e-01 1.139356e-02 8.991321e-03
+1.275000e+03 7.500000e+01 7.500000e+01 6.716700e-02 8.280411e-03 9.436231e-03
+1.425000e+03 7.500000e+01 7.500000e+01 3.576800e-02 4.113652e-03 5.353288e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.268900e-02 1.810116e-03 1.969695e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.874500e-03 5.472270e-04 3.790943e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.281500e-04 5.981958e-05 5.863538e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d102-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d102-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 8.926900e-01 1.097600e-01 1.143400e-01
+5.800000e+02 3.500000e+01 3.500000e+01 7.337500e-01 1.014800e-01 8.296000e-02
+6.550000e+02 4.000000e+01 4.000000e+01 5.519100e-01 7.098800e-02 8.231900e-02
+7.400000e+02 4.500000e+01 4.500000e+01 4.024800e-01 5.963000e-02 4.281100e-02
+8.325000e+02 4.750000e+01 4.750000e+01 2.878200e-01 3.697700e-02 3.155200e-02
+9.325000e+02 5.250000e+01 5.250000e+01 1.928500e-01 2.772000e-02 2.245800e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.325200e-01 1.797200e-02 2.089800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.010400e-02 1.147200e-02 1.275000e-02
+1.275000e+03 7.500000e+01 7.500000e+01 5.754100e-02 9.250100e-03 6.763600e-03
+1.425000e+03 7.500000e+01 7.500000e+01 3.471200e-02 6.809400e-03 3.559500e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.282500e-02 2.094600e-03 1.681900e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.964300e-03 3.959000e-04 2.603600e-04
+3.350000e+03 6.500000e+02 6.500000e+02 8.538600e-05 2.888600e-05 3.188200e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d102-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d102-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 7.912600e-01 2.356300e-01 3.752800e-01
+5.800000e+02 3.500000e+01 3.500000e+01 6.453100e-01 1.925600e-01 3.074500e-01
+6.550000e+02 4.000000e+01 4.000000e+01 4.842500e-01 1.452600e-01 2.328600e-01
+7.400000e+02 4.500000e+01 4.500000e+01 3.578500e-01 1.081600e-01 1.736300e-01
+8.325000e+02 4.750000e+01 4.750000e+01 2.587800e-01 7.820000e-02 1.255000e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.784000e-01 5.458300e-02 8.843000e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.154500e-01 3.554900e-02 5.776300e-02
+1.150000e+03 5.000000e+01 5.000000e+01 8.036800e-02 2.520400e-02 4.130300e-02
+1.275000e+03 7.500000e+01 7.500000e+01 5.470900e-02 1.709300e-02 2.804100e-02
+1.425000e+03 7.500000e+01 7.500000e+01 3.236000e-02 1.008500e-02 1.650700e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.160000e-02 3.701900e-03 6.109700e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.766300e-03 5.795500e-04 9.795000e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.101300e-04 3.561700e-05 5.885600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d102-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d102-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 9.442500e-01 2.217800e-01 4.539400e-01
+5.800000e+02 3.500000e+01 3.500000e+01 7.963900e-01 1.906200e-01 3.995700e-01
+6.550000e+02 4.000000e+01 4.000000e+01 6.077400e-01 1.409900e-01 3.183300e-01
+7.400000e+02 4.500000e+01 4.500000e+01 4.554500e-01 1.075800e-01 2.280200e-01
+8.325000e+02 4.750000e+01 4.750000e+01 3.439300e-01 8.882000e-02 1.511600e-01
+9.325000e+02 5.250000e+01 5.250000e+01 2.390100e-01 5.789500e-02 1.165400e-01
+1.042500e+03 5.750000e+01 5.750000e+01 1.645700e-01 3.763800e-02 7.879200e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.131400e-01 2.145700e-02 5.317100e-02
+1.275000e+03 7.500000e+01 7.500000e+01 7.820500e-02 1.773700e-02 3.477700e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.798500e-02 1.021600e-02 2.147800e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.914200e-02 3.778700e-03 1.006900e-02
+2.350000e+03 3.500000e+02 3.500000e+02 3.291400e-03 6.802200e-04 1.928200e-03
+3.350000e+03 6.500000e+02 6.500000e+02 2.228000e-04 4.651700e-05 7.725700e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d103-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d103-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.317100e+00 1.662208e-01 1.560145e-01
+6.250000e+01 1.250000e+01 1.250000e+01 2.377900e+00 2.383366e-01 2.360401e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.114900e+00 2.095572e-01 1.959945e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.526800e+00 1.335790e-01 1.361221e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.068200e+00 1.148175e-01 1.100250e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.622300e-01 5.386598e-02 5.118310e-02
+2.625000e+02 3.750000e+01 3.750000e+01 1.878500e-01 2.124380e-02 2.260063e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.102300e-02 3.707778e-03 3.772826e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d103-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d103-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.071500e+00 1.451000e-01 1.393100e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.905900e+00 2.717500e-01 2.225300e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.724400e+00 2.553500e-01 1.837400e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.339700e+00 1.915300e-01 1.716300e-01
+1.450000e+02 1.500000e+01 1.500000e+01 9.556800e-01 1.242400e-01 1.154100e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.041100e-01 6.082900e-02 7.070500e-02
+2.625000e+02 3.750000e+01 3.750000e+01 1.717100e-01 2.189300e-02 1.888900e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.539700e-02 1.907400e-03 2.367400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d103-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d103-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.025200e+00 3.016300e-01 4.789400e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.746600e+00 5.177800e-01 8.253500e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.552500e+00 4.687500e-01 7.514300e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.158900e+00 3.520200e-01 5.674900e-01
+1.450000e+02 1.500000e+01 1.500000e+01 8.005200e-01 2.489200e-01 4.060000e-01
+1.925000e+02 3.250000e+01 3.250000e+01 4.193600e-01 1.311100e-01 2.146000e-01
+2.625000e+02 3.750000e+01 3.750000e+01 1.452400e-01 4.550900e-02 7.417600e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.365700e-02 4.326000e-03 7.050100e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d103-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d103-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.344700e+00 3.459100e-01 6.262800e-01
+6.250000e+01 1.250000e+01 1.250000e+01 2.220100e+00 5.672400e-01 1.092600e+00
+8.750000e+01 1.250000e+01 1.250000e+01 1.986200e+00 3.963300e-01 1.002100e+00
+1.150000e+02 1.500000e+01 1.500000e+01 1.542700e+00 3.501400e-01 7.927800e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.062400e+00 2.263400e-01 5.405800e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.455000e-01 1.314700e-01 2.584200e-01
+2.625000e+02 3.750000e+01 3.750000e+01 1.862600e-01 3.796400e-02 9.110500e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.612200e-02 3.845700e-03 6.963700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d104-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d104-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 3.194600e+01 6.164026e+00 6.091542e+00
+4.500000e-01 1.500000e-01 1.500000e-01 6.906200e+01 1.111902e+01 1.017829e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.481600e+02 2.683081e+01 2.604132e+01
+7.500000e-01 5.000000e-02 5.000000e-02 4.602300e+02 3.992553e+01 4.030188e+01
+8.250000e-01 2.500000e-02 2.500000e-02 7.849300e+02 7.846769e+01 7.762066e+01
+8.750000e-01 2.500000e-02 2.500000e-02 9.958400e+02 9.472413e+01 9.582386e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.174000e+03 1.219903e+02 1.195064e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.279200e+03 1.442066e+02 1.373947e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d104-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d104-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 3.239300e+01 4.407000e+00 5.976200e+00
+4.500000e-01 1.500000e-01 1.500000e-01 8.260900e+01 9.607700e+00 1.179100e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.188800e+02 3.878000e+01 2.081300e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.970500e+02 5.861400e+01 5.088700e+01
+8.250000e-01 2.500000e-02 2.500000e-02 6.037600e+02 7.500900e+01 8.361700e+01
+8.750000e-01 2.500000e-02 2.500000e-02 7.792400e+02 1.042900e+02 9.046200e+01
+9.250000e-01 2.500000e-02 2.500000e-02 9.491400e+02 1.353100e+02 1.078500e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.055800e+03 1.328000e+02 1.232000e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d104-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d104-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 2.731600e+01 8.990000e+00 1.520300e+01
+4.500000e-01 1.500000e-01 1.500000e-01 6.230900e+01 2.007600e+01 3.337900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 1.658300e+02 5.206100e+01 8.514600e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.190700e+02 9.867400e+01 1.603500e+02
+8.250000e-01 2.500000e-02 2.500000e-02 5.245600e+02 1.583200e+02 2.538200e+02
+8.750000e-01 2.500000e-02 2.500000e-02 7.095700e+02 2.116700e+02 3.377500e+02
+9.250000e-01 2.500000e-02 2.500000e-02 9.207600e+02 2.723200e+02 4.330500e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.069500e+03 3.134300e+02 4.955400e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d104-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d104-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 2.823700e+01 5.189300e+00 1.595500e+01
+4.500000e-01 1.500000e-01 1.500000e-01 7.249300e+01 1.804100e+01 3.539900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.057000e+02 4.742000e+01 9.726900e+01
+7.500000e-01 5.000000e-02 5.000000e-02 4.332700e+02 9.266500e+01 2.147100e+02
+8.250000e-01 2.500000e-02 2.500000e-02 6.871700e+02 1.624200e+02 3.248100e+02
+8.750000e-01 2.500000e-02 2.500000e-02 9.404500e+02 2.333300e+02 4.317700e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.207400e+03 2.729700e+02 6.167700e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.421700e+03 3.464800e+02 7.012800e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d105-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d105-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.122000e+02 1.378747e+01 1.380599e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.315300e+02 1.435557e+01 1.417091e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.543200e+02 1.478781e+01 1.471536e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.444700e+02 1.466204e+01 1.458784e+01
+4.000000e+00 4.000000e-01 4.000000e-01 9.352000e+01 1.023297e+01 8.861253e+00
+4.800000e+00 4.000000e-01 4.000000e-01 2.163800e+01 3.713625e+00 3.160063e+00
+7.000000e+00 1.800000e+00 1.800000e+00 1.062500e+00 2.460275e-01 3.311533e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d105-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d105-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 8.968700e+01 1.057600e+01 1.083800e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.073600e+02 1.271300e+01 1.246500e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.206100e+02 1.716200e+01 1.310400e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.224300e+02 1.619400e+01 1.452800e+01
+4.000000e+00 4.000000e-01 4.000000e-01 8.254300e+01 1.173900e+01 1.258300e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.472600e+01 4.240800e+00 2.577700e+00
+7.000000e+00 1.800000e+00 1.800000e+00 1.010200e+00 2.236900e-01 1.725500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d105-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d105-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 9.278400e+01 2.746300e+01 4.342600e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.028200e+02 3.053500e+01 4.849000e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.096100e+02 3.273900e+01 5.223800e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.026800e+02 3.086600e+01 4.951700e+01
+4.000000e+00 4.000000e-01 4.000000e-01 6.834600e+01 2.109100e+01 3.436500e+01
+4.800000e+00 4.000000e-01 4.000000e-01 1.958400e+01 6.280600e+00 1.048600e+01
+7.000000e+00 1.800000e+00 1.800000e+00 8.589900e-01 2.893700e-01 4.949900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d105-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d105-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.159700e+02 2.875900e+01 5.190000e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.323700e+02 2.846600e+01 7.192100e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.396700e+02 3.409100e+01 6.664400e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.347400e+02 3.416600e+01 6.224300e+01
+4.000000e+00 4.000000e-01 4.000000e-01 9.042200e+01 1.947100e+01 4.696200e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.645300e+01 6.194500e+00 1.221300e+01
+7.000000e+00 1.800000e+00 1.800000e+00 1.209200e+00 2.682700e-01 5.639100e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d106-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d106-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.355200e+00 2.128349e-01 1.447406e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.765000e+00 2.276836e-01 2.227523e-01
+1.275000e+02 1.250000e+01 1.250000e+01 2.035400e+00 2.008478e-01 2.097645e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.991800e+00 1.870991e-01 1.673110e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.725900e+00 1.426544e-01 1.396621e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.369100e+00 1.107719e-01 1.099527e-01
+2.350000e+02 1.500000e+01 1.500000e+01 8.336300e-01 7.129823e-02 7.290835e-02
+2.650000e+02 1.500000e+01 1.500000e+01 5.613100e-01 5.021629e-02 5.395497e-02
+3.150000e+02 3.500000e+01 3.500000e+01 2.690200e-01 3.322067e-02 3.541971e-02
+4.150000e+02 6.500000e+01 6.500000e+01 6.887900e-02 1.398064e-02 1.388875e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.004300e-02 1.987628e-03 1.952282e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d106-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d106-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.308600e+00 1.926600e-01 1.876600e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.607900e+00 2.357600e-01 2.261800e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.717500e+00 2.507500e-01 2.160800e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.628200e+00 2.297500e-01 1.972400e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.423700e+00 1.929100e-01 1.677000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.068000e+00 1.444800e-01 1.143800e-01
+2.350000e+02 1.500000e+01 1.500000e+01 7.183400e-01 9.018700e-02 9.093100e-02
+2.650000e+02 1.500000e+01 1.500000e+01 4.689700e-01 6.093400e-02 4.755000e-02
+3.150000e+02 3.500000e+01 3.500000e+01 2.341500e-01 2.540800e-02 2.904400e-02
+4.150000e+02 6.500000e+01 6.500000e+01 6.382500e-02 7.698700e-03 9.501600e-03
+5.825000e+02 1.025000e+02 1.025000e+02 9.277700e-03 1.681800e-03 1.138000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d106-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d106-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.031500e+00 3.247300e-01 5.376400e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.285700e+00 3.935000e-01 6.393700e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.421100e+00 4.315900e-01 6.965200e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.428300e+00 4.300000e-01 6.900500e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.300400e+00 3.873100e-01 6.172100e-01
+2.050000e+02 1.500000e+01 1.500000e+01 9.809800e-01 2.952700e-01 4.743500e-01
+2.350000e+02 1.500000e+01 1.500000e+01 6.892200e-01 2.066300e-01 3.300400e-01
+2.650000e+02 1.500000e+01 1.500000e+01 4.874100e-01 1.468200e-01 2.336700e-01
+3.150000e+02 3.500000e+01 3.500000e+01 2.282500e-01 6.894600e-02 1.101900e-01
+4.150000e+02 6.500000e+01 6.500000e+01 6.858200e-02 2.065800e-02 3.296500e-02
+5.825000e+02 1.025000e+02 1.025000e+02 8.857500e-03 2.785100e-03 4.508500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d106-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d106-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.282000e+00 2.856700e-01 6.114500e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.691700e+00 4.555400e-01 8.108800e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.808800e+00 4.382900e-01 8.470800e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.790200e+00 4.345600e-01 9.083900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.650100e+00 3.842600e-01 8.355900e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.277600e+00 2.625100e-01 7.166600e-01
+2.350000e+02 1.500000e+01 1.500000e+01 9.316100e-01 1.882400e-01 4.509400e-01
+2.650000e+02 1.500000e+01 1.500000e+01 5.948100e-01 1.383300e-01 2.783100e-01
+3.150000e+02 3.500000e+01 3.500000e+01 3.283500e-01 8.045000e-02 1.330400e-01
+4.150000e+02 6.500000e+01 6.500000e+01 9.358300e-02 2.241700e-02 4.588500e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.479700e-02 3.010100e-03 6.567300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d107-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d107-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 9.110900e-01 1.588982e-01 1.548867e-01
+5.800000e+02 3.500000e+01 3.500000e+01 7.716400e-01 1.018759e-01 9.759468e-02
+6.550000e+02 4.000000e+01 4.000000e+01 5.921600e-01 7.745728e-02 8.440039e-02
+7.400000e+02 4.500000e+01 4.500000e+01 4.260100e-01 4.972377e-02 4.414964e-02
+8.325000e+02 4.750000e+01 4.750000e+01 3.207500e-01 3.728159e-02 3.134651e-02
+9.325000e+02 5.250000e+01 5.250000e+01 2.109000e-01 2.949601e-02 3.550327e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.450100e-01 1.674060e-02 2.071307e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.819000e-02 1.536497e-02 1.352539e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.642700e-02 1.940322e-02 1.038693e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.980900e-02 7.758158e-03 6.992196e-03
+1.750000e+03 2.500000e+02 2.500000e+02 2.265900e-02 3.901552e-03 4.085785e-03
+3.000000e+03 1.000000e+03 1.000000e+03 1.295800e-03 3.913357e-04 3.826879e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d107-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d107-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.749000e-01 6.962400e-02 7.161800e-02
+5.800000e+02 3.500000e+01 3.500000e+01 5.696800e-01 6.748400e-02 7.435200e-02
+6.550000e+02 4.000000e+01 4.000000e+01 4.559200e-01 6.081700e-02 4.467700e-02
+7.400000e+02 4.500000e+01 4.500000e+01 3.484500e-01 4.783200e-02 4.020400e-02
+8.325000e+02 4.750000e+01 4.750000e+01 2.588900e-01 4.026200e-02 3.184800e-02
+9.325000e+02 5.250000e+01 5.250000e+01 1.867500e-01 2.524300e-02 2.079800e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.329000e-01 1.810700e-02 1.948800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.485300e-02 1.387400e-02 1.198400e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.533400e-02 1.085500e-02 8.814600e-03
+1.425000e+03 7.500000e+01 7.500000e+01 4.172400e-02 5.692800e-03 5.957800e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.852500e-02 3.335100e-03 2.679400e-03
+3.000000e+03 1.000000e+03 1.000000e+03 1.532600e-03 2.376600e-04 2.115200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d107-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d107-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.933500e-01 2.056700e-01 3.275100e-01
+5.800000e+02 3.500000e+01 3.500000e+01 5.915400e-01 1.772200e-01 2.835800e-01
+6.550000e+02 4.000000e+01 4.000000e+01 4.668500e-01 1.406400e-01 2.255000e-01
+7.400000e+02 4.500000e+01 4.500000e+01 3.584700e-01 1.101100e-01 1.794000e-01
+8.325000e+02 4.750000e+01 4.750000e+01 2.709900e-01 8.322000e-02 1.345300e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.900500e-01 5.910400e-02 9.647700e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.331600e-01 4.170800e-02 6.846400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.995300e-02 3.139500e-02 5.163300e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.808800e-02 2.163600e-02 3.588400e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.331100e-02 1.395100e-02 2.331900e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.884200e-02 6.274900e-03 1.076900e-02
+3.000000e+03 1.000000e+03 1.000000e+03 1.560900e-03 5.455800e-04 9.647100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d107-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d107-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.985600e-01 1.620900e-01 3.070800e-01
+5.800000e+02 3.500000e+01 3.500000e+01 6.104800e-01 1.425200e-01 3.447700e-01
+6.550000e+02 4.000000e+01 4.000000e+01 4.834200e-01 1.095100e-01 2.226400e-01
+7.400000e+02 4.500000e+01 4.500000e+01 3.709300e-01 8.393800e-02 1.596900e-01
+8.325000e+02 4.750000e+01 4.750000e+01 2.861100e-01 6.263000e-02 1.323400e-01
+9.325000e+02 5.250000e+01 5.250000e+01 2.093300e-01 5.141200e-02 9.288200e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.469000e-01 2.522100e-02 7.490800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.101900e-01 1.950300e-02 4.855200e-02
+1.275000e+03 7.500000e+01 7.500000e+01 8.093100e-02 1.666400e-02 2.972600e-02
+1.425000e+03 7.500000e+01 7.500000e+01 5.113300e-02 9.438600e-03 2.281700e-02
+1.750000e+03 2.500000e+02 2.500000e+02 2.359700e-02 5.260200e-03 9.532100e-03
+3.000000e+03 1.000000e+03 1.000000e+03 2.190700e-03 3.414200e-04 1.014400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d108-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d108-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.322900e+00 2.052019e-01 2.008205e-01
+6.250000e+01 1.250000e+01 1.250000e+01 2.274700e+00 3.189118e-01 3.174077e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.881600e+00 2.311125e-01 2.476128e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.126500e+00 1.507024e-01 1.157130e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.430300e-01 3.666611e-02 3.595725e-02
+6.000000e+02 3.000000e+02 3.000000e+02 8.547800e-03 3.085704e-03 3.089450e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d108-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d108-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 9.556900e-01 1.426000e-01 1.002700e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.632900e+00 2.089400e-01 1.928300e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.452100e+00 1.867900e-01 1.838100e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.005100e+00 1.299600e-01 1.279200e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.108300e-01 3.934900e-02 3.405800e-02
+6.000000e+02 3.000000e+02 3.000000e+02 1.116400e-02 1.334800e-03 1.773700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d108-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d108-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.020800e+00 3.047500e-01 4.887200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.708300e+00 5.206200e-01 8.451500e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.481700e+00 4.521800e-01 7.315400e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.002800e+00 3.116200e-01 5.094200e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.148700e-01 9.850100e-02 1.610700e-01
+6.000000e+02 3.000000e+02 3.000000e+02 1.240100e-02 3.905500e-03 6.361600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d108-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d108-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.086100e+00 2.350100e-01 4.995300e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.846000e+00 4.406100e-01 7.994400e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.630600e+00 3.675200e-01 6.734600e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.076500e+00 2.144000e-01 5.511900e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.287400e-01 7.637500e-02 1.597300e-01
+6.000000e+02 3.000000e+02 3.000000e+02 1.247900e-02 2.462800e-03 5.497400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d109-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d109-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.427500e+01 1.496705e+01 9.122976e+00
+4.500000e-01 1.500000e-01 1.500000e-01 9.548000e+01 1.571207e+01 1.537634e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.600600e+02 2.651159e+01 2.948628e+01
+7.500000e-01 5.000000e-02 5.000000e-02 4.386300e+02 4.524406e+01 4.650106e+01
+8.500000e-01 5.000000e-02 5.000000e-02 7.594100e+02 9.625282e+01 9.274535e+01
+9.500000e-01 5.000000e-02 5.000000e-02 1.045600e+03 1.349422e+02 1.341298e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d109-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d109-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.609600e+01 6.268100e+00 4.698600e+00
+4.500000e-01 1.500000e-01 1.500000e-01 9.736800e+01 1.435600e+01 1.352900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.118900e+02 3.012500e+01 2.940000e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.577100e+02 4.684900e+01 3.778700e+01
+8.500000e-01 5.000000e-02 5.000000e-02 5.700600e+02 7.219900e+01 6.879200e+01
+9.500000e-01 5.000000e-02 5.000000e-02 7.844200e+02 1.002500e+02 8.880500e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d109-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d109-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.637100e+01 1.494500e+01 2.496500e+01
+4.500000e-01 1.500000e-01 1.500000e-01 9.160200e+01 2.926500e+01 4.862100e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.019100e+02 6.405400e+01 1.055700e+02
+7.500000e-01 5.000000e-02 5.000000e-02 3.559100e+02 1.112700e+02 1.826100e+02
+8.500000e-01 5.000000e-02 5.000000e-02 5.954700e+02 1.807200e+02 2.911900e+02
+9.500000e-01 5.000000e-02 5.000000e-02 8.576700e+02 2.551200e+02 4.074800e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d109-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d109-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.130600e+01 9.606300e+00 2.474900e+01
+4.500000e-01 1.500000e-01 1.500000e-01 8.626100e+01 1.905000e+01 4.357300e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.054500e+02 4.413400e+01 9.224000e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.810800e+02 7.425200e+01 1.830400e+02
+8.500000e-01 5.000000e-02 5.000000e-02 6.637100e+02 1.435700e+02 3.065000e+02
+9.500000e-01 5.000000e-02 5.000000e-02 9.604300e+02 2.219200e+02 4.183300e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d110-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d110-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.309600e+00 4.165370e-01 3.534697e-01
+1.275000e+02 1.250000e+01 1.250000e+01 2.097600e+00 2.465289e-01 2.532859e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.567900e+00 1.617279e-01 1.576783e-01
+2.200000e+02 3.000000e+01 3.000000e+01 7.374100e-01 6.806971e-02 6.868258e-02
+2.825000e+02 3.250000e+01 3.250000e+01 3.204600e-01 2.768212e-02 2.745194e-02
+3.525000e+02 3.750000e+01 3.750000e+01 1.097400e-01 1.318318e-02 1.399842e-02
+4.350000e+02 4.500000e+01 4.500000e+01 3.719100e-02 6.349371e-03 6.233725e-03
+5.825000e+02 1.025000e+02 1.025000e+02 8.869200e-03 2.721005e-03 2.612747e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.380300e-07 6.263013e-03 6.263008e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d110-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d110-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.788400e+00 3.026300e-01 1.971400e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.681200e+00 2.229900e-01 1.975800e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.250200e+00 1.363900e-01 1.673400e-01
+2.200000e+02 3.000000e+01 3.000000e+01 6.486800e-01 7.338500e-02 7.466100e-02
+2.825000e+02 3.250000e+01 3.250000e+01 2.656500e-01 3.279500e-02 3.134000e-02
+3.525000e+02 3.750000e+01 3.750000e+01 1.002500e-01 1.424200e-02 8.753200e-03
+4.350000e+02 4.500000e+01 4.500000e+01 3.307200e-02 4.235100e-03 5.561900e-03
+5.825000e+02 1.025000e+02 1.025000e+02 6.981200e-03 9.980600e-04 9.399700e-04
+8.425000e+02 1.575000e+02 1.575000e+02 5.993900e-04 1.825100e-04 1.561300e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d110-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d110-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.685600e+00 5.301900e-01 8.797400e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.672500e+00 5.137900e-01 8.347300e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.318500e+00 4.007900e-01 6.457800e-01
+2.200000e+02 3.000000e+01 3.000000e+01 7.110200e-01 2.143200e-01 3.436000e-01
+2.825000e+02 3.250000e+01 3.250000e+01 2.913200e-01 8.854600e-02 1.424500e-01
+3.525000e+02 3.750000e+01 3.750000e+01 1.122400e-01 3.456200e-02 5.565800e-02
+4.350000e+02 4.500000e+01 4.500000e+01 4.111900e-02 1.235000e-02 1.966000e-02
+5.825000e+02 1.025000e+02 1.025000e+02 9.051300e-03 2.747000e-03 4.374100e-03
+8.425000e+02 1.575000e+02 1.575000e+02 5.472200e-04 1.747300e-04 2.841000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d110-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d110-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.743200e+00 3.746100e-01 8.016600e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.693500e+00 4.213300e-01 7.914800e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.390000e+00 3.060800e-01 6.211300e-01
+2.200000e+02 3.000000e+01 3.000000e+01 7.808500e-01 1.474700e-01 4.022100e-01
+2.825000e+02 3.250000e+01 3.250000e+01 3.411600e-01 7.759400e-02 1.660200e-01
+3.525000e+02 3.750000e+01 3.750000e+01 1.373800e-01 3.107400e-02 5.632200e-02
+4.350000e+02 4.500000e+01 4.500000e+01 5.063200e-02 1.427800e-02 1.403200e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.128600e-02 2.130900e-03 5.189300e-03
+8.425000e+02 1.575000e+02 1.575000e+02 8.921200e-04 2.212200e-04 5.403600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d111-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d111-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.934400e+00 2.047777e-01 2.060855e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.554500e+00 1.147123e-01 1.160608e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.148600e+00 7.958526e-02 7.788120e-02
+7.400000e+02 4.500000e+01 4.500000e+01 7.872700e-01 5.305027e-02 5.174950e-02
+8.325000e+02 4.750000e+01 4.750000e+01 5.362300e-01 4.052583e-02 3.776656e-02
+9.325000e+02 5.250000e+01 5.250000e+01 3.784800e-01 2.161550e-02 2.500310e-02
+1.042500e+03 5.750000e+01 5.750000e+01 2.505000e-01 1.974661e-02 1.394663e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.739800e-01 1.214582e-02 8.120632e-03
+1.275000e+03 7.500000e+01 7.500000e+01 1.133300e-01 7.347170e-03 7.403166e-03
+1.425000e+03 7.500000e+01 7.500000e+01 7.190800e-02 7.881528e-03 1.177839e-02
+1.750000e+03 2.500000e+02 2.500000e+02 3.443000e-02 3.375883e-03 3.932118e-03
+2.350000e+03 3.500000e+02 3.500000e+02 7.209200e-03 1.282826e-03 1.334459e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.041900e-03 2.878364e-04 2.626336e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d111-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d111-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.642100e+00 2.224900e-01 1.048000e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.280700e+00 1.377300e-01 1.273100e-01
+6.550000e+02 4.000000e+01 4.000000e+01 9.243800e-01 9.858100e-02 8.465500e-02
+7.400000e+02 4.500000e+01 4.500000e+01 6.538000e-01 7.784700e-02 5.199500e-02
+8.325000e+02 4.750000e+01 4.750000e+01 4.503400e-01 4.545300e-02 4.479600e-02
+9.325000e+02 5.250000e+01 5.250000e+01 3.181700e-01 3.284500e-02 2.535500e-02
+1.042500e+03 5.750000e+01 5.750000e+01 2.185000e-01 2.233400e-02 1.953400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.579900e-01 1.483300e-02 2.066600e-02
+1.275000e+03 7.500000e+01 7.500000e+01 1.090300e-01 9.760300e-03 9.055100e-03
+1.425000e+03 7.500000e+01 7.500000e+01 7.073300e-02 7.780500e-03 3.461500e-03
+1.750000e+03 2.500000e+02 2.500000e+02 3.316800e-02 2.504200e-03 2.777300e-03
+2.350000e+03 3.500000e+02 3.500000e+02 8.734700e-03 6.407600e-04 6.425400e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.212400e-03 1.337400e-04 1.543400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d111-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d111-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.880700e+00 4.180500e-01 6.047600e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.478800e+00 3.320800e-01 4.824600e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.064500e+00 2.412500e-01 3.519000e-01
+7.400000e+02 4.500000e+01 4.500000e+01 7.629200e-01 1.761300e-01 2.584000e-01
+8.325000e+02 4.750000e+01 4.750000e+01 5.197000e-01 1.209900e-01 1.789600e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.649800e-01 8.578500e-02 1.272200e-01
+1.042500e+03 5.750000e+01 5.750000e+01 2.483800e-01 5.903100e-02 8.813500e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.733800e-01 4.181800e-02 6.280800e-02
+1.275000e+03 7.500000e+01 7.500000e+01 1.198100e-01 2.886900e-02 4.345000e-02
+1.425000e+03 7.500000e+01 7.500000e+01 7.811100e-02 1.921100e-02 2.916800e-02
+1.750000e+03 2.500000e+02 2.500000e+02 3.568000e-02 8.919700e-03 1.364200e-02
+2.350000e+03 3.500000e+02 3.500000e+02 9.058400e-03 2.335400e-03 3.635200e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.192200e-03 3.207500e-04 5.047000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d111-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d111-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.628100e+00 2.993500e-01 6.745500e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.279400e+00 2.076000e-01 4.473400e-01
+6.550000e+02 4.000000e+01 4.000000e+01 9.358600e-01 1.605300e-01 3.396800e-01
+7.400000e+02 4.500000e+01 4.500000e+01 6.718400e-01 1.099100e-01 2.416500e-01
+8.325000e+02 4.750000e+01 4.750000e+01 4.790800e-01 7.642600e-02 1.506700e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.409300e-01 4.338300e-02 1.233500e-01
+1.042500e+03 5.750000e+01 5.750000e+01 2.365700e-01 3.459200e-02 7.409400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.688300e-01 2.454700e-02 6.020900e-02
+1.275000e+03 7.500000e+01 7.500000e+01 1.199900e-01 1.771900e-02 4.314600e-02
+1.425000e+03 7.500000e+01 7.500000e+01 8.160500e-02 1.549200e-02 1.858400e-02
+1.750000e+03 2.500000e+02 2.500000e+02 3.742900e-02 5.936600e-03 1.075600e-02
+2.350000e+03 3.500000e+02 3.500000e+02 9.699000e-03 1.718800e-03 2.130700e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.324400e-03 2.172600e-04 3.806100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d112-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d112-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.579600e+00 2.711065e-01 2.643542e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.958800e+00 5.026961e-01 5.257734e-01
+6.250000e+01 1.250000e+01 1.250000e+01 4.334200e+00 3.792103e-01 3.718256e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.998200e+00 2.164359e-01 2.116842e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.979600e+00 1.334556e-01 1.287057e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.492000e+00 1.237087e-01 1.085712e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.918100e-01 5.857638e-02 6.881132e-02
+2.250000e+02 3.500000e+01 3.500000e+01 4.240200e-01 4.365110e-02 4.182401e-02
+3.250000e+02 6.500000e+01 6.500000e+01 9.793900e-02 1.567364e-02 1.537346e-02
+6.450000e+02 2.550000e+02 2.550000e+02 5.061200e-03 1.404259e-03 1.386970e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d112-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d112-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.804400e+00 2.658700e-01 6.646200e-02
+3.750000e+01 1.250000e+01 1.250000e+01 3.770700e+00 3.970400e-01 3.774700e-01
+6.250000e+01 1.250000e+01 1.250000e+01 3.474700e+00 3.558700e-01 3.319800e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.670600e+00 2.791500e-01 2.253000e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.902400e+00 1.977700e-01 1.693700e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.329700e+00 1.605800e-01 1.222500e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.809000e-01 8.616900e-02 8.474500e-02
+2.250000e+02 3.500000e+01 3.500000e+01 4.329000e-01 4.424100e-02 3.108600e-02
+3.250000e+02 6.500000e+01 6.500000e+01 1.126000e-01 1.057300e-02 1.004400e-02
+6.450000e+02 2.550000e+02 2.550000e+02 6.649600e-03 7.184800e-04 4.637200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d112-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d112-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.121400e+00 4.360100e-01 6.128600e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.193800e+00 9.078900e-01 1.303500e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.752500e+00 8.527900e-01 1.247000e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.964300e+00 6.888600e-01 1.015400e+00
+1.150000e+02 1.500000e+01 1.500000e+01 2.143700e+00 5.061400e-01 7.530900e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.526300e+00 3.652700e-01 5.453000e-01
+1.750000e+02 1.500000e+01 1.500000e+01 1.068700e+00 2.598600e-01 3.887800e-01
+2.250000e+02 3.500000e+01 3.500000e+01 5.398000e-01 1.320000e-01 1.977300e-01
+3.250000e+02 6.500000e+01 6.500000e+01 1.535300e-01 3.824600e-02 5.733000e-02
+6.450000e+02 2.550000e+02 2.550000e+02 1.039400e-02 2.702600e-03 4.093300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d112-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d112-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.856200e+00 1.978500e-01 6.439900e-01
+3.750000e+01 1.250000e+01 1.250000e+01 3.939000e+00 6.173000e-01 1.379000e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.624400e+00 5.748400e-01 1.373800e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.762400e+00 4.109300e-01 9.952400e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.951300e+00 3.472300e-01 6.723300e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.344600e+00 2.294300e-01 4.235100e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.966700e-01 1.489700e-01 3.301800e-01
+2.250000e+02 3.500000e+01 3.500000e+01 4.410700e-01 8.725500e-02 1.531300e-01
+3.250000e+02 6.500000e+01 6.500000e+01 1.184800e-01 2.013000e-02 3.517000e-02
+6.450000e+02 2.550000e+02 2.550000e+02 8.714200e-03 2.430900e-03 2.757300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d113-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d113-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 5.586400e+01 1.118706e+01 1.104381e+01
+3.500000e-01 5.000000e-02 5.000000e-02 7.833700e+01 1.351436e+01 1.384003e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.288400e+02 1.549411e+01 1.432772e+01
+5.500000e-01 5.000000e-02 5.000000e-02 2.049900e+02 1.895132e+01 2.163838e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.402900e+02 3.049171e+01 2.859075e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.767000e+02 4.588403e+01 4.887892e+01
+7.750000e-01 2.500000e-02 2.500000e-02 7.672700e+02 5.741062e+01 5.452588e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.143300e+03 8.074666e+01 7.674454e+01
+8.750000e-01 2.500000e-02 2.500000e-02 1.653700e+03 1.302137e+02 1.240733e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.228500e+03 1.588063e+02 1.556113e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.867300e+03 2.246193e+02 2.329989e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d113-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d113-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 6.373000e+01 7.492800e+00 7.065600e+00
+3.500000e-01 5.000000e-02 5.000000e-02 8.990700e+01 1.271000e+01 1.286600e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.226300e+02 1.766100e+01 1.461900e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.825600e+02 1.828600e+01 1.752200e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.127800e+02 3.363300e+01 2.949200e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.867400e+02 5.180100e+01 6.072000e+01
+7.750000e-01 2.500000e-02 2.500000e-02 6.810400e+02 7.480700e+01 5.491100e+01
+8.250000e-01 2.500000e-02 2.500000e-02 9.436000e+02 9.818500e+01 8.198000e+01
+8.750000e-01 2.500000e-02 2.500000e-02 1.323700e+03 1.334200e+02 9.886700e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.792900e+03 1.825600e+02 1.661600e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.268900e+03 2.638000e+02 1.420800e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d113-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d113-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 7.362100e+01 1.803800e+01 2.728200e+01
+3.500000e-01 5.000000e-02 5.000000e-02 1.007000e+02 2.448200e+01 3.672200e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.347300e+02 3.243200e+01 4.847100e+01
+5.500000e-01 5.000000e-02 5.000000e-02 2.064100e+02 5.044600e+01 7.559700e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.389400e+02 8.167600e+01 1.224700e+02
+7.250000e-01 2.500000e-02 2.500000e-02 5.284200e+02 1.264000e+02 1.881400e+02
+7.750000e-01 2.500000e-02 2.500000e-02 7.345100e+02 1.744500e+02 2.595400e+02
+8.250000e-01 2.500000e-02 2.500000e-02 1.043000e+03 2.465300e+02 3.651400e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.480000e+03 3.411800e+02 5.011000e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.107200e+03 4.715700e+02 6.848300e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.724500e+03 5.878600e+02 8.420200e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d113-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d113-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 6.158000e+01 1.220800e+01 2.139600e+01
+3.500000e-01 5.000000e-02 5.000000e-02 8.181400e+01 1.449300e+01 3.341900e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.147200e+02 2.020900e+01 3.300600e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.722700e+02 3.036500e+01 5.917900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.023600e+02 5.512700e+01 8.862700e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.652900e+02 7.566200e+01 1.763100e+02
+7.750000e-01 2.500000e-02 2.500000e-02 6.752300e+02 1.073700e+02 2.398400e+02
+8.250000e-01 2.500000e-02 2.500000e-02 9.776800e+02 1.698200e+02 3.293100e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.399600e+03 2.173500e+02 5.034200e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.938600e+03 3.075400e+02 6.884800e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.453700e+03 3.440500e+02 8.884500e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d114-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d114-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.269800e+02 8.348051e+00 8.261689e+00
+2.600000e+00 2.000000e-01 2.000000e-01 1.721100e+02 1.090471e+01 1.051043e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.081400e+02 1.294466e+01 1.299410e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.453600e+02 1.571388e+01 1.569201e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.530200e+02 1.746229e+01 1.794819e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.623600e+02 1.267874e+01 1.194071e+01
+4.600000e+00 2.000000e-01 2.000000e-01 9.276200e+01 7.698652e+00 7.934809e+00
+5.000000e+00 2.000000e-01 2.000000e-01 5.314900e+01 5.404704e+00 5.484141e+00
+5.800000e+00 6.000000e-01 6.000000e-01 1.617900e+01 1.942031e+00 2.003112e+00
+7.600000e+00 1.200000e+00 1.200000e+00 5.693000e-01 2.767259e-01 2.785675e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d114-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d114-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.076800e+02 1.043800e+01 8.709800e+00
+2.600000e+00 2.000000e-01 2.000000e-01 1.414800e+02 1.430800e+01 1.121600e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.825800e+02 2.318800e+01 8.498100e+00
+3.400000e+00 2.000000e-01 2.000000e-01 2.124500e+02 2.186700e+01 2.008200e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.062300e+02 2.360800e+01 1.781600e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.347600e+02 1.579900e+01 1.281300e+01
+4.600000e+00 2.000000e-01 2.000000e-01 8.099200e+01 8.587900e+00 1.024600e+01
+5.000000e+00 2.000000e-01 2.000000e-01 4.632300e+01 3.728200e+00 5.458600e+00
+5.800000e+00 6.000000e-01 6.000000e-01 1.523900e+01 1.658400e+00 1.293000e+00
+7.600000e+00 1.200000e+00 1.200000e+00 6.115400e-01 5.622500e-02 1.297900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d114-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d114-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.576800e+02 3.702000e+01 5.438600e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.890800e+02 4.376200e+01 6.410100e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.189000e+02 5.019500e+01 7.340100e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.361200e+02 5.356900e+01 7.828900e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.142900e+02 4.805700e+01 7.020000e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.379900e+02 3.135400e+01 4.597100e+01
+4.600000e+00 2.000000e-01 2.000000e-01 8.136100e+01 1.880900e+01 2.809400e+01
+5.000000e+00 2.000000e-01 2.000000e-01 4.554800e+01 1.057700e+01 1.586100e+01
+5.800000e+00 6.000000e-01 6.000000e-01 1.437000e+01 3.448400e+00 5.234100e+00
+7.600000e+00 1.200000e+00 1.200000e+00 5.877800e-01 1.400700e-01 2.165900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d114-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d114-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.217000e+02 2.136800e+01 5.508500e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.570500e+02 2.875600e+01 5.705200e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.931000e+02 3.311000e+01 6.632700e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.192100e+02 3.491800e+01 7.817500e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.015900e+02 3.189300e+01 6.867400e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.315700e+02 2.023700e+01 4.475300e+01
+4.600000e+00 2.000000e-01 2.000000e-01 7.956000e+01 1.362300e+01 2.580300e+01
+5.000000e+00 2.000000e-01 2.000000e-01 4.674200e+01 2.718300e+00 1.337300e+01
+5.800000e+00 6.000000e-01 6.000000e-01 1.587400e+01 2.351900e+00 3.766100e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.667600e-01 5.681500e-02 1.605200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d115-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d115-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.665800e+00 6.678500e-01 6.858559e-01
+1.050000e+02 1.000000e+01 1.000000e+01 4.712300e+00 4.874926e-01 5.099653e-01
+1.275000e+02 1.250000e+01 1.250000e+01 4.073500e+00 3.278462e-01 3.091421e-01
+1.525000e+02 1.250000e+01 1.250000e+01 3.179200e+00 1.990791e-01 1.957019e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.453400e+00 1.378531e-01 1.350295e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.734100e+00 8.475521e-02 7.626382e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.042200e+00 5.064959e-02 5.032267e-02
+2.650000e+02 1.500000e+01 1.500000e+01 6.199300e-01 5.535075e-02 5.525754e-02
+2.975000e+02 1.750000e+01 1.750000e+01 3.973900e-01 2.747221e-02 2.414900e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.201800e-01 1.781863e-02 1.807301e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.403800e-01 1.432198e-02 1.458703e-02
+4.350000e+02 4.500000e+01 4.500000e+01 5.246900e-02 7.396627e-03 7.142820e-03
+5.825000e+02 1.025000e+02 1.025000e+02 9.758700e-03 1.920456e-03 1.968488e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d115-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d115-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.432300e+00 3.867900e-01 4.608600e-01
+1.050000e+02 1.000000e+01 1.000000e+01 3.795000e+00 5.281400e-01 3.132500e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.426400e+00 3.683200e-01 3.154800e-01
+1.525000e+02 1.250000e+01 1.250000e+01 2.839700e+00 3.036700e-01 2.007900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.191500e+00 2.194300e-01 1.954000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.537100e+00 1.514900e-01 1.093400e-01
+2.350000e+02 1.500000e+01 1.500000e+01 9.712100e-01 1.018300e-01 6.519200e-02
+2.650000e+02 1.500000e+01 1.500000e+01 6.008100e-01 5.279200e-02 5.211700e-02
+2.975000e+02 1.750000e+01 1.750000e+01 3.638600e-01 3.233400e-02 2.857900e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.147700e-01 1.950300e-02 1.533300e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.244700e-01 1.198400e-02 1.009600e-02
+4.350000e+02 4.500000e+01 4.500000e+01 5.540200e-02 5.604400e-03 3.732800e-03
+5.825000e+02 1.025000e+02 1.025000e+02 1.054900e-02 1.160700e-03 1.025300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d115-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d115-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.274700e+00 7.190500e-01 1.045400e+00
+1.050000e+02 1.000000e+01 1.000000e+01 3.733000e+00 8.290900e-01 1.209400e+00
+1.275000e+02 1.250000e+01 1.250000e+01 3.642900e+00 8.199300e-01 1.195500e+00
+1.525000e+02 1.250000e+01 1.250000e+01 3.233700e+00 7.320600e-01 1.067800e+00
+1.775000e+02 1.250000e+01 1.250000e+01 2.694400e+00 6.155400e-01 9.005700e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.937000e+00 4.512200e-01 6.646500e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.280800e+00 3.024400e-01 4.471100e-01
+2.650000e+02 1.500000e+01 1.500000e+01 8.154200e-01 1.955600e-01 2.906500e-01
+2.975000e+02 1.750000e+01 1.750000e+01 5.032500e-01 1.230400e-01 1.837300e-01
+3.325000e+02 1.750000e+01 1.750000e+01 3.077000e-01 7.597300e-02 1.138100e-01
+3.700000e+02 2.000000e+01 2.000000e+01 1.843100e-01 4.597500e-02 6.892100e-02
+4.350000e+02 4.500000e+01 4.500000e+01 8.196700e-02 2.092900e-02 3.159100e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.661400e-02 4.346800e-03 6.610300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d115-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d115-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.247700e+00 3.663900e-01 1.274300e+00
+1.050000e+02 1.000000e+01 1.000000e+01 3.572600e+00 5.606600e-01 1.204500e+00
+1.275000e+02 1.250000e+01 1.250000e+01 3.416600e+00 5.932200e-01 1.058400e+00
+1.525000e+02 1.250000e+01 1.250000e+01 2.991300e+00 4.270100e-01 1.017700e+00
+1.775000e+02 1.250000e+01 1.250000e+01 2.347200e+00 3.826900e-01 8.677800e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.681400e+00 2.743900e-01 6.893000e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.053300e+00 1.782000e-01 3.952300e-01
+2.650000e+02 1.500000e+01 1.500000e+01 6.836400e-01 1.242200e-01 2.270900e-01
+2.975000e+02 1.750000e+01 1.750000e+01 4.186800e-01 7.698900e-02 1.473300e-01
+3.325000e+02 1.750000e+01 1.750000e+01 2.620500e-01 5.768200e-02 7.882800e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.516800e-01 3.156300e-02 4.312400e-02
+4.350000e+02 4.500000e+01 4.500000e+01 6.819800e-02 1.272900e-02 2.067600e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.469100e-02 2.229200e-03 5.345600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d116-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d116-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t116
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.023600e-01 1.130462e-01 1.130462e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.684200e+00 3.060627e-01 3.060627e-01
+9.250000e-01 2.500000e-02 2.500000e-02 5.084000e+00 7.082546e-01 7.082546e-01
+9.750000e-01 2.500000e-02 2.500000e-02 6.746000e+00 1.974846e+00 1.974846e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d116-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d116-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t116
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.365400e-01 0.000000e+00 5.099400e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.739800e+00 3.354900e-02 3.581100e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.069900e+00 3.253400e-01 0.000000e+00
+9.750000e-01 2.500000e-02 2.500000e-02 5.659300e+00 5.351000e-01 4.739900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d116-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d116-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t116
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.306000e-01 1.453200e-02 1.676400e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.810800e+00 7.618100e-02 8.004900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.103200e+00 2.293600e-01 2.443100e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.425300e+00 2.637300e-01 2.731000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d117-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d117-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t117
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.257200e-03 2.465346e-03 2.465346e-03
+1.400000e+02 2.500000e+01 2.500000e+01 6.199800e-03 1.093463e-03 1.093463e-03
+1.925000e+02 2.750000e+01 2.750000e+01 3.385000e-03 6.762096e-04 6.762096e-04
+2.500000e+02 3.000000e+01 3.000000e+01 1.877600e-03 5.037593e-04 5.037593e-04
+3.575000e+02 7.750000e+01 7.750000e+01 5.946800e-04 2.631693e-04 2.631693e-04
+5.600000e+02 1.250000e+02 1.250000e+02 1.800100e-04 1.291442e-04 1.291442e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d117-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d117-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t117
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.239800e-03 5.017000e-04 9.408800e-05
+1.400000e+02 2.500000e+01 2.500000e+01 4.804500e-03 2.900700e-05 4.066500e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.669900e-03 1.729000e-04 7.828200e-05
+2.500000e+02 3.000000e+01 3.000000e+01 2.402700e-03 2.034300e-04 0.000000e+00
+3.575000e+02 7.750000e+01 7.750000e+01 1.185100e-03 2.747100e-05 1.869300e-04
+5.600000e+02 1.250000e+02 1.250000e+02 3.267100e-04 3.025200e-05 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d117-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d117-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t117
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.768300e-03 2.965100e-04 3.865600e-04
+1.400000e+02 2.500000e+01 2.500000e+01 5.255000e-03 2.604300e-04 3.155800e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.835400e-03 2.121300e-04 2.214200e-04
+2.500000e+02 3.000000e+01 3.000000e+01 2.379100e-03 1.599600e-04 1.621900e-04
+3.575000e+02 7.750000e+01 7.750000e+01 1.025100e-03 6.532900e-05 7.927300e-05
+5.600000e+02 1.250000e+02 1.250000e+02 2.311300e-04 2.442600e-05 3.342300e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d118-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d118-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t118
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.892900e+00 7.182502e-01 7.182502e-01
+3.000000e-01 1.000000e-01 1.000000e-01 1.680700e+00 4.740168e-01 4.740168e-01
+7.000000e-01 3.000000e-01 3.000000e-01 1.421300e-01 2.328305e-01 2.328305e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d118-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d118-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t118
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.780400e+00 2.156200e-01 2.168200e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.659500e+00 1.473200e-01 3.328400e-02
+7.000000e-01 3.000000e-01 3.000000e-01 1.867100e-01 8.866000e-03 1.235300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d118-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d118-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t118
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.804200e+00 9.483400e-02 9.917100e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.670100e+00 7.318600e-02 7.585200e-02
+7.000000e-01 3.000000e-01 3.000000e-01 1.752300e-01 1.368700e-02 1.493600e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d119-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d119-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t119
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.358900e-01 2.310755e-01 2.310755e-01
+1.000000e+00 5.000000e-01 5.000000e-01 8.261700e-02 1.109725e-01 1.109725e-01
+5.000000e+00 3.500000e+00 3.500000e+00 8.149600e-02 1.171497e-01 1.171497e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d119-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d119-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t119
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.871300e-01 5.594200e-03 3.429900e-03
+1.000000e+00 5.000000e-01 5.000000e-01 9.468100e-02 2.927000e-03 4.937900e-03
+5.000000e+00 3.500000e+00 3.500000e+00 1.819300e-02 5.601600e-04 3.261200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d119-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d119-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t119
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.835900e-01 2.379900e-02 2.432100e-02
+1.000000e+00 5.000000e-01 5.000000e-01 8.941800e-02 7.570800e-03 8.527600e-03
+5.000000e+00 3.500000e+00 3.500000e+00 2.699100e-02 4.159500e-03 5.133800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d120-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d120-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t120
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 2.066400e-03 3.387979e-04 3.387979e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.585900e-03 1.985014e-04 1.985014e-04
+1.275000e+03 7.500000e+01 7.500000e+01 1.109000e-03 1.666473e-04 1.666473e-04
+1.425000e+03 7.500000e+01 7.500000e+01 7.989400e-04 1.911995e-04 1.911995e-04
+1.750000e+03 2.500000e+02 2.500000e+02 4.819700e-04 8.001193e-05 8.001193e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.159600e-04 2.753683e-05 2.753683e-05
+3.350000e+03 6.500000e+02 6.500000e+02 2.032200e-05 7.512427e-06 7.512427e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d120-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d120-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t120
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.776800e-03 1.456400e-04 1.308500e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.454200e-03 9.904800e-05 1.735200e-04
+1.275000e+03 7.500000e+01 7.500000e+01 1.146000e-03 0.000000e+00 9.799000e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.653700e-04 3.626500e-05 0.000000e+00
+1.750000e+03 2.500000e+02 2.500000e+02 4.798000e-04 1.186900e-05 8.028800e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.508700e-04 5.670100e-06 1.065200e-05
+3.350000e+03 6.500000e+02 6.500000e+02 2.284100e-05 2.336100e-06 2.329000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d120-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d120-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t120
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.704200e-03 7.203900e-05 7.770800e-05
+1.150000e+03 5.000000e+01 5.000000e+01 1.407700e-03 6.547200e-05 6.820500e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.136800e-03 4.804000e-05 5.452800e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.539800e-04 4.163800e-05 4.429600e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.888400e-04 1.725500e-05 1.779300e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.612200e-04 8.374800e-06 9.443100e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.532300e-05 2.435500e-06 3.029600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d121-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d121-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t121
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 5.257200e-03 6.442300e-04 6.442300e-04
+3.750000e+01 1.250000e+01 1.250000e+01 9.913900e-03 1.177899e-03 1.177899e-03
+6.250000e+01 1.250000e+01 1.250000e+01 8.067000e-03 7.212043e-04 7.212043e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.753700e-03 6.128160e-04 6.128160e-04
+1.300000e+02 3.000000e+01 3.000000e+01 2.662800e-03 4.035903e-04 4.035903e-04
+2.100000e+02 5.000000e+01 5.000000e+01 7.339100e-04 3.123464e-04 3.123464e-04
+3.775000e+02 1.175000e+02 1.175000e+02 1.642100e-04 5.264875e-05 5.264875e-05
+6.975000e+02 2.025000e+02 2.025000e+02 8.526300e-06 1.036673e-05 1.036673e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d121-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d121-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t121
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.495700e-03 0.000000e+00 1.008900e-03
+3.750000e+01 1.250000e+01 1.250000e+01 7.123200e-03 2.261500e-04 6.968700e-05
+6.250000e+01 1.250000e+01 1.250000e+01 6.530500e-03 1.064200e-04 6.587700e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.283000e-03 1.991700e-04 3.218000e-05
+1.300000e+02 3.000000e+01 3.000000e+01 3.408700e-03 5.727800e-05 0.000000e+00
+2.100000e+02 5.000000e+01 5.000000e+01 1.473500e-03 8.284200e-05 0.000000e+00
+3.775000e+02 1.175000e+02 1.175000e+02 3.184400e-04 8.217900e-06 8.099800e-05
+6.975000e+02 2.025000e+02 2.025000e+02 3.082200e-05 3.614800e-06 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d121-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d121-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t121
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.766100e-03 2.140500e-04 2.350700e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.678500e-03 3.056400e-04 3.240100e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.720100e-03 2.859300e-04 3.185400e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.420200e-03 2.567900e-04 2.766100e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.466100e-03 1.325500e-04 1.401200e-04
+2.100000e+02 5.000000e+01 5.000000e+01 1.389800e-03 6.501600e-05 6.730900e-05
+3.775000e+02 1.175000e+02 1.175000e+02 2.443900e-04 1.778500e-05 2.066400e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.481800e-05 3.335900e-06 3.868100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d122-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d122-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t122
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.128100e-01 6.931408e-02 6.931408e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.292600e+00 1.754933e-01 1.754933e-01
+8.500000e-01 5.000000e-02 5.000000e-02 2.849300e+00 2.906862e-01 2.906862e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.428100e+00 4.306034e-01 4.306034e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.708900e+00 8.452775e-01 8.452775e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d122-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d122-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t122
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.587700e-01 5.176900e-03 2.325000e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.197200e+00 6.864700e-02 0.000000e+00
+8.500000e-01 5.000000e-02 5.000000e-02 2.376700e+00 5.536800e-02 0.000000e+00
+9.250000e-01 2.500000e-02 2.500000e-02 3.964500e+00 1.953300e-02 3.789900e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.264900e+00 1.530600e-01 2.724500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d122-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d122-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t122
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.381100e-01 1.017100e-02 1.108400e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.219100e+00 6.088900e-02 6.469100e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.467100e+00 8.661800e-02 9.201500e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.032300e+00 1.566000e-01 1.788000e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.261800e+00 1.788900e-01 1.903600e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d123-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d123-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t123
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 7.847200e-02 2.251447e-02 2.251447e-02
+3.200000e+00 4.000000e-01 4.000000e-01 1.706800e-01 2.670302e-02 2.670302e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.068800e-01 3.931611e-02 3.931611e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.929200e-01 7.162762e-02 7.162762e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.695400e-01 5.304497e-02 5.304497e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.352300e-01 7.909049e-02 7.909049e-02
+7.000000e+00 1.800000e+00 1.800000e+00 7.745700e-02 1.941613e-02 1.941613e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d123-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d123-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t123
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 6.834100e-02 2.985400e-03 4.022800e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.694500e-01 9.073300e-03 2.084000e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.806500e-01 1.497700e-02 1.495200e-04
+4.200000e+00 2.000000e-01 2.000000e-01 3.504300e-01 1.630900e-02 2.860300e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.899700e-01 1.044300e-03 7.664500e-03
+5.000000e+00 2.000000e-01 2.000000e-01 3.913300e-01 1.002500e-02 4.957900e-02
+7.000000e+00 1.800000e+00 1.800000e+00 6.800400e-02 3.137100e-03 9.999400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d123-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d123-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t123
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 5.412600e-02 4.536000e-03 5.975800e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.451400e-01 7.427700e-03 9.474700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.525900e-01 1.385800e-02 1.670600e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.316000e-01 1.587800e-02 1.669200e-02
+4.600000e+00 2.000000e-01 2.000000e-01 4.138100e-01 1.773700e-02 2.019600e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.121500e-01 1.770100e-02 2.105400e-02
+7.000000e+00 1.800000e+00 1.800000e+00 7.681400e-02 2.547300e-03 3.641800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d124-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d124-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t124
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.391500e-03 1.374241e-03 1.374241e-03
+1.275000e+02 1.250000e+01 1.250000e+01 7.056900e-03 7.344399e-04 7.344399e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.575600e-03 6.293049e-04 6.293049e-04
+1.775000e+02 1.250000e+01 1.250000e+01 2.875100e-03 4.954216e-04 4.954216e-04
+2.200000e+02 3.000000e+01 3.000000e+01 2.567000e-03 3.226880e-04 3.226880e-04
+4.675000e+02 2.175000e+02 2.175000e+02 4.588300e-04 1.004593e-04 1.004593e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d124-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d124-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t124
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.130900e-03 2.415800e-04 6.232700e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.748200e-03 1.496600e-04 1.098200e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.150200e-03 1.595500e-04 1.408800e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.320400e-03 1.017000e-04 6.212500e-05
+2.200000e+02 3.000000e+01 3.000000e+01 3.072500e-03 4.842900e-05 3.440300e-04
+4.675000e+02 2.175000e+02 2.175000e+02 5.875800e-04 3.647300e-05 3.251500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d124-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d124-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t124
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.687900e-03 2.226200e-04 2.669300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.238100e-03 2.758500e-04 3.253600e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.468500e-03 2.582700e-04 3.195000e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.457300e-03 2.331800e-04 2.694300e-04
+2.200000e+02 3.000000e+01 3.000000e+01 3.068900e-03 1.248900e-04 1.447400e-04
+4.675000e+02 2.175000e+02 2.175000e+02 4.889500e-04 1.851400e-05 2.496300e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d125-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d125-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t125
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 2.594400e-03 4.190878e-04 4.190878e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.553700e-03 2.612375e-04 2.612375e-04
+1.275000e+03 7.500000e+01 7.500000e+01 1.072900e-03 1.985562e-04 1.985562e-04
+1.425000e+03 7.500000e+01 7.500000e+01 8.580400e-04 1.864359e-04 1.864359e-04
+1.750000e+03 2.500000e+02 2.500000e+02 4.344900e-04 1.704024e-04 1.704024e-04
+2.350000e+03 3.500000e+02 3.500000e+02 8.611900e-05 4.402697e-05 4.402697e-05
+3.350000e+03 6.500000e+02 6.500000e+02 1.387300e-05 1.362833e-05 1.362833e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d125-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d125-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t125
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.869000e-03 8.297400e-05 1.403700e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.514600e-03 8.065100e-05 8.493300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.174600e-03 3.970400e-05 5.986900e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.704500e-04 5.492200e-05 0.000000e+00
+1.750000e+03 2.500000e+02 2.500000e+02 4.639200e-04 8.550100e-06 3.618800e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.386100e-04 6.042900e-06 1.018900e-05
+3.350000e+03 6.500000e+02 6.500000e+02 1.991800e-05 2.218200e-06 1.967000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d125-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d125-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t125
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.811700e-03 6.565500e-05 7.262200e-05
+1.150000e+03 5.000000e+01 5.000000e+01 1.467600e-03 5.909100e-05 6.342100e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.161500e-03 4.292300e-05 4.829600e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.521900e-04 3.676600e-05 3.954900e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.755500e-04 1.504300e-05 1.586300e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.484300e-04 7.102900e-06 7.838100e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.179700e-05 1.997300e-06 2.419000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d126-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d126-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t126
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.316600e-02 1.167391e-01 1.167391e-01
+7.500000e-01 5.000000e-02 5.000000e-02 1.077800e+00 2.641903e-01 2.641903e-01
+8.500000e-01 5.000000e-02 5.000000e-02 2.940700e+00 4.358110e-01 4.358110e-01
+9.250000e-01 2.500000e-02 2.500000e-02 5.160700e+00 8.712068e-01 8.712068e-01
+9.750000e-01 2.500000e-02 2.500000e-02 6.198000e+00 2.041773e+00 2.041773e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d126-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d126-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t126
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.466500e-01 2.039700e-03 1.887900e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.174000e+00 7.784000e-02 0.000000e+00
+8.500000e-01 5.000000e-02 5.000000e-02 2.377200e+00 8.026200e-02 2.695900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.012100e+00 6.297600e-02 2.827100e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.432300e+00 1.540300e-01 1.159600e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d126-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d126-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t126
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.307800e-01 8.851600e-03 1.017500e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.213800e+00 5.371000e-02 5.589200e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.450700e+00 7.631600e-02 7.704000e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.073100e+00 1.391400e-01 1.458700e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.367000e+00 1.597200e-01 1.715200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d127-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d127-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t127
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.580200e-01 5.158983e-02 5.158983e-02
+3.200000e+00 4.000000e-01 4.000000e-01 2.251000e-01 4.386656e-02 4.386656e-02
+4.000000e+00 4.000000e-01 4.000000e-01 2.738800e-01 4.135038e-02 4.135038e-02
+4.800000e+00 4.000000e-01 4.000000e-01 3.212500e-01 7.000266e-02 7.000266e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.090600e-01 6.827894e-02 6.827894e-02
+7.400000e+00 1.400000e+00 1.400000e+00 1.791200e-02 1.692342e-02 1.692342e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d127-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d127-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t127
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.733600e-02 5.356100e-03 3.796600e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.961000e-01 6.955800e-03 1.301800e-02
+4.000000e+00 4.000000e-01 4.000000e-01 3.223100e-01 7.804600e-03 8.098900e-03
+4.800000e+00 4.000000e-01 4.000000e-01 3.665900e-01 1.322700e-02 1.837700e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.061100e-01 1.516000e-03 4.688500e-03
+7.400000e+00 1.400000e+00 1.400000e+00 1.758400e-02 1.554300e-03 9.895200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d127-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d127-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t127
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 7.695900e-02 4.781400e-03 7.292300e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.697600e-01 7.101500e-03 9.693300e-03
+4.000000e+00 4.000000e-01 4.000000e-01 3.024600e-01 9.479000e-03 1.106800e-02
+4.800000e+00 4.000000e-01 4.000000e-01 3.953700e-01 1.083800e-02 1.239700e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.304800e-01 8.274600e-03 1.024900e-02
+7.400000e+00 1.400000e+00 1.400000e+00 2.142100e-02 1.348400e-03 2.010000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d128-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d128-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t128
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.642600e-03 1.960698e-03 1.960698e-03
+1.275000e+02 1.250000e+01 1.250000e+01 6.181900e-03 1.086276e-03 1.086276e-03
+1.525000e+02 1.250000e+01 1.250000e+01 5.108300e-03 9.268621e-04 9.268621e-04
+1.775000e+02 1.250000e+01 1.250000e+01 3.381100e-03 6.160713e-04 6.160713e-04
+2.050000e+02 1.500000e+01 1.500000e+01 2.577200e-03 4.961571e-04 4.961571e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.464700e-03 5.046414e-04 5.046414e-04
+3.000000e+02 5.000000e+01 5.000000e+01 1.591500e-03 3.863047e-04 3.863047e-04
+4.150000e+02 6.500000e+01 6.500000e+01 7.435300e-04 1.969364e-04 1.969364e-04
+5.825000e+02 1.025000e+02 1.025000e+02 1.397800e-04 8.768520e-05 8.768520e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d128-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d128-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t128
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.591600e-03 3.631500e-04 4.697300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.321200e-03 2.273500e-04 7.368200e-05
+1.525000e+02 1.250000e+01 1.250000e+01 4.875200e-03 1.269000e-04 3.029000e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.188200e-03 2.541400e-05 8.894900e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.505400e-03 6.468700e-05 4.064000e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.725200e-03 7.818100e-05 6.547600e-05
+3.000000e+02 5.000000e+01 5.000000e+01 1.741000e-03 9.813200e-05 6.747100e-05
+4.150000e+02 6.500000e+01 6.500000e+01 6.680600e-04 2.667300e-05 1.152700e-04
+5.825000e+02 1.025000e+02 1.025000e+02 1.551800e-04 9.030200e-06 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d128-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d128-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t128
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.155200e-03 1.874000e-04 2.542300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.851400e-03 2.362300e-04 2.796300e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.218100e-03 2.230800e-04 2.756400e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.373900e-03 2.042400e-04 2.336300e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.536600e-03 1.676500e-04 1.888100e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.755400e-03 1.479800e-04 1.593700e-04
+3.000000e+02 5.000000e+01 5.000000e+01 1.546600e-03 6.072400e-05 7.170500e-05
+4.150000e+02 6.500000e+01 6.500000e+01 5.305400e-04 3.119300e-05 4.312000e-05
+5.825000e+02 1.025000e+02 1.025000e+02 1.028900e-04 1.093900e-05 1.551400e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d129-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d129-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t129
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.327800e+00 1.389135e+00 1.389135e+00
+3.000000e-01 1.000000e-01 1.000000e-01 1.539000e+00 2.244209e-01 2.244209e-01
+5.000000e-01 1.000000e-01 1.000000e-01 8.173400e-01 4.726766e-01 4.726766e-01
+8.000000e-01 2.000000e-01 2.000000e-01 1.579400e-01 1.700791e-01 1.700791e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d129-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d129-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t129
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.579100e+00 1.214900e-01 2.907000e-03
+3.000000e-01 1.000000e-01 1.000000e-01 1.669400e+00 0.000000e+00 4.594200e-02
+5.000000e-01 1.000000e-01 1.000000e-01 5.755300e-01 1.829200e-02 1.262200e-01
+8.000000e-01 2.000000e-01 2.000000e-01 8.800700e-02 1.777400e-03 3.412700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d129-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d129-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t129
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.616300e+00 5.581000e-02 6.133300e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.674600e+00 4.465000e-02 4.573200e-02
+5.000000e-01 1.000000e-01 1.000000e-01 5.580900e-01 2.577600e-02 2.870700e-02
+8.000000e-01 2.000000e-01 2.000000e-01 7.551800e-02 6.704700e-03 7.677700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d130-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d130-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t130
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 7.954800e-01 3.269501e-01 3.269501e-01
+1.000000e+00 5.000000e-01 5.000000e-01 1.242000e-01 1.342327e-01 1.342327e-01
+5.000000e+00 3.500000e+00 3.500000e+00 8.032600e-02 1.275911e-01 1.275911e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d130-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d130-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t130
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.785900e-01 7.975500e-03 4.351500e-03
+1.000000e+00 5.000000e-01 5.000000e-01 1.021400e-01 3.845900e-03 5.014800e-03
+5.000000e+00 3.500000e+00 3.500000e+00 1.927000e-02 8.246800e-04 2.957400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d130-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d130-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t130
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.725200e-01 1.440000e-02 1.481500e-02
+1.000000e+00 5.000000e-01 5.000000e-01 9.830500e-02 4.833500e-03 5.449800e-03
+5.000000e+00 3.500000e+00 3.500000e+00 2.917600e-02 2.633200e-03 3.563400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d131-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d131-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t131
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 8.262700e-02 1.237262e-01 1.237262e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.538700e+00 5.351295e-01 5.351295e-01
+9.500000e-01 5.000000e-02 5.000000e-02 6.344200e+00 1.601282e+00 1.601282e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d131-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d131-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t131
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.340000e-01 5.373100e-03 1.138000e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.696700e+00 2.749400e-02 7.501500e-03
+9.500000e-01 5.000000e-02 5.000000e-02 4.968600e+00 4.877900e-02 5.255200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d131-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d131-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t131
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.375100e-01 2.459900e-02 2.536700e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.746800e+00 1.248000e-01 1.334300e-01
+9.500000e-01 5.000000e-02 5.000000e-02 4.843900e+00 2.939100e-01 3.181300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d132-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d132-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t132
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 5.114000e-03 9.542262e-04 9.542262e-04
+4.525000e+02 2.325000e+02 2.325000e+02 6.108400e-04 2.507862e-04 2.507862e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d132-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d132-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t132
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 4.123000e-03 4.194100e-05 1.085200e-04
+4.525000e+02 2.325000e+02 2.325000e+02 9.092000e-04 3.134500e-05 1.458200e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d132-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d132-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t132
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 4.524800e-03 2.417200e-04 2.695300e-04
+4.525000e+02 2.325000e+02 2.325000e+02 7.882300e-04 5.535900e-05 6.577500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d133-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d133-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t133
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.243600e+00 3.735556e-01 3.735556e-01
+7.000000e-01 3.000000e-01 3.000000e-01 1.709500e-01 1.938156e-01 1.938156e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d133-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d133-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t133
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.287500e+00 0.000000e+00 1.302300e-02
+7.000000e-01 3.000000e-01 3.000000e-01 1.416900e-01 7.956400e-03 1.157900e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d133-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d133-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t133
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.317500e+00 1.016600e-01 1.022900e-01
+7.000000e-01 3.000000e-01 3.000000e-01 1.216800e-01 1.901900e-02 2.048700e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d134-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d134-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t134
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.675400e-01 7.910694e-02 7.910694e-02
+1.000000e+00 5.000000e-01 5.000000e-01 3.246400e-02 9.812075e-02 9.812075e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d134-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d134-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t134
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.112700e-01 1.310100e-02 0.000000e+00
+1.000000e+00 5.000000e-01 5.000000e-01 8.873400e-02 0.000000e+00 1.020200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d134-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d134-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t134
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.203000e-01 4.101300e-02 4.142100e-02
+1.000000e+00 5.000000e-01 5.000000e-01 7.970200e-02 1.207000e-02 1.335500e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d135-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d135-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t135
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.060600e+00 2.919681e+00 2.919681e+00
+8.000000e-01 1.000000e-01 1.000000e-01 3.390500e+01 1.401911e+01 1.401911e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.023500e+02 3.653857e+01 3.653857e+01
+9.750000e-01 2.500000e-02 2.500000e-02 1.358100e+02 4.366729e+01 4.366729e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d135-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d135-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t135
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.355200e+00 6.702500e-01 2.109900e+00
+8.000000e-01 1.000000e-01 1.000000e-01 3.203400e+01 5.241700e+00 7.890400e+00
+9.250000e-01 2.500000e-02 2.500000e-02 7.493700e+01 1.208700e+01 1.774600e+01
+9.750000e-01 2.500000e-02 2.500000e-02 1.042000e+02 1.573000e+01 2.590800e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d135-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d135-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t135
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.463200e+00 2.812500e-01 4.039600e-01
+8.000000e-01 1.000000e-01 1.000000e-01 3.504600e+01 1.474400e+00 2.058600e+00
+9.250000e-01 2.500000e-02 2.500000e-02 7.941600e+01 4.439100e+00 4.752700e+00
+9.750000e-01 2.500000e-02 2.500000e-02 1.050000e+02 5.104400e+00 6.932000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d136-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d136-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t136
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.800000e+00 8.000000e-01 8.000000e-01 9.893700e-01 8.486929e-01 8.486929e-01
+4.400000e+00 8.000000e-01 8.000000e-01 4.799600e+00 1.899958e+00 1.899958e+00
+5.600000e+00 4.000000e-01 4.000000e-01 8.789000e+00 3.581552e+00 3.581552e+00
+7.400000e+00 1.400000e+00 1.400000e+00 1.197200e+00 7.472867e-01 7.472867e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d136-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d136-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t136
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.800000e+00 8.000000e-01 8.000000e-01 1.569300e+00 2.406500e-01 4.016700e-01
+4.400000e+00 8.000000e-01 8.000000e-01 5.065000e+00 8.139200e-01 1.313100e+00
+5.600000e+00 4.000000e-01 4.000000e-01 6.571300e+00 1.022000e+00 1.836800e+00
+7.400000e+00 1.400000e+00 1.400000e+00 9.072200e-01 1.443100e-01 2.461900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d136-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d136-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t136
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.800000e+00 8.000000e-01 8.000000e-01 1.288000e+00 9.993400e-02 1.400400e-01
+4.400000e+00 8.000000e-01 8.000000e-01 5.131300e+00 1.994700e-01 2.381100e-01
+5.600000e+00 4.000000e-01 4.000000e-01 7.452000e+00 3.399500e-01 5.729900e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.115000e+00 7.028900e-02 1.142000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d137-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d137-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t137
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.422700e-01 8.477553e-02 8.477553e-02
+1.400000e+02 2.500000e+01 2.500000e+01 1.215400e-01 4.175641e-02 4.175641e-02
+1.925000e+02 2.750000e+01 2.750000e+01 6.635900e-02 2.673253e-02 2.673253e-02
+2.500000e+02 3.000000e+01 3.000000e+01 3.680800e-02 1.739959e-02 1.739959e-02
+3.575000e+02 7.750000e+01 7.750000e+01 1.165800e-02 8.279260e-03 8.279260e-03
+5.600000e+02 1.250000e+02 1.250000e+02 3.528800e-03 3.175272e-03 3.175272e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d137-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d137-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t137
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.701200e-02 1.165900e-02 1.630800e-02
+1.400000e+02 2.500000e+01 2.500000e+01 8.726900e-02 1.246800e-02 2.832200e-02
+1.925000e+02 2.750000e+01 2.750000e+01 6.666100e-02 1.029800e-02 1.754400e-02
+2.500000e+02 3.000000e+01 3.000000e+01 4.364300e-02 7.126000e-03 1.014400e-02
+3.575000e+02 7.750000e+01 7.750000e+01 2.152600e-02 3.619900e-03 8.907700e-03
+5.600000e+02 1.250000e+02 1.250000e+02 5.934300e-03 1.058900e-03 1.059400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d137-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d137-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t137
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 9.167000e-02 5.700400e-03 9.657400e-03
+1.400000e+02 2.500000e+01 2.500000e+01 1.010300e-01 5.006800e-03 7.355700e-03
+1.925000e+02 2.750000e+01 2.750000e+01 7.373500e-02 4.078300e-03 5.263900e-03
+2.500000e+02 3.000000e+01 3.000000e+01 4.573800e-02 3.075300e-03 3.371400e-03
+3.575000e+02 7.750000e+01 7.750000e+01 1.970800e-02 1.256000e-03 1.478400e-03
+5.600000e+02 1.250000e+02 1.250000e+02 4.443400e-03 4.695800e-04 6.250000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d138-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d138-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t138
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.657200e+01 3.750452e+00 3.750452e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.638000e+00 3.045752e+00 3.045752e+00
+5.000000e+00 3.500000e+00 3.500000e+00 1.615800e+00 2.799342e+00 2.799342e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d138-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d138-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t138
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.633400e+01 2.647400e+00 3.836800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.743300e+00 2.592200e-01 5.361400e-01
+5.000000e+00 3.500000e+00 3.500000e+00 3.349700e-01 3.766400e-02 9.854700e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d138-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d138-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t138
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.710200e+01 4.606200e-01 8.725200e-01
+1.000000e+00 5.000000e-01 5.000000e-01 1.730600e+00 1.465300e-01 1.663700e-01
+5.000000e+00 3.500000e+00 3.500000e+00 5.223900e-01 8.050500e-02 9.046300e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d139-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d139-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t139
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.967000e+00 4.111985e+00 4.111985e+00
+7.500000e-01 5.000000e-02 5.000000e-02 5.691300e+01 1.449033e+01 1.449033e+01
+8.500000e-01 5.000000e-02 5.000000e-02 1.254600e+02 2.475365e+01 2.475365e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.949700e+02 4.410050e+01 4.410050e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.513700e+02 5.102258e+01 5.102258e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d139-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d139-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t139
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.044000e+01 1.596100e+00 3.236600e+00
+7.500000e-01 5.000000e-02 5.000000e-02 4.830100e+01 7.897300e+00 6.428600e+00
+8.500000e-01 5.000000e-02 5.000000e-02 9.588600e+01 1.390000e+01 1.668600e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.599500e+02 2.010600e+01 3.136500e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.124100e+02 2.646000e+01 4.343600e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d139-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d139-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t139
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 9.713800e+00 4.149200e-01 4.991100e-01
+7.500000e-01 5.000000e-02 5.000000e-02 4.973500e+01 2.484000e+00 3.085300e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.006500e+02 3.533700e+00 5.445000e+00
+9.250000e-01 2.500000e-02 2.500000e-02 1.645000e+02 6.388800e+00 7.474400e+00
+9.750000e-01 2.500000e-02 2.500000e-02 2.146600e+02 7.298200e+00 1.126600e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d140-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d140-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t140
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 3.411300e+00 1.353607e+00 1.353607e+00
+3.200000e+00 4.000000e-01 4.000000e-01 7.419800e+00 1.935078e+00 1.935078e+00
+3.800000e+00 2.000000e-01 2.000000e-01 8.993400e+00 2.629859e+00 2.629859e+00
+4.200000e+00 2.000000e-01 2.000000e-01 1.273300e+01 4.117456e+00 4.117456e+00
+4.600000e+00 2.000000e-01 2.000000e-01 1.606500e+01 4.215204e+00 4.215204e+00
+5.000000e+00 2.000000e-01 2.000000e-01 1.892000e+01 5.206451e+00 5.206451e+00
+7.000000e+00 1.800000e+00 1.800000e+00 3.367200e+00 9.963553e-01 9.963553e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d140-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d140-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t140
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 2.757200e+00 2.856800e-01 4.122200e-01
+3.200000e+00 4.000000e-01 4.000000e-01 6.836500e+00 1.081500e+00 1.955700e+00
+3.800000e+00 2.000000e-01 2.000000e-01 1.132300e+01 1.574400e+00 1.561100e+00
+4.200000e+00 2.000000e-01 2.000000e-01 1.413800e+01 1.863600e+00 4.243300e+00
+4.600000e+00 2.000000e-01 2.000000e-01 1.573300e+01 1.928800e+00 3.127700e+00
+5.000000e+00 2.000000e-01 2.000000e-01 1.578800e+01 2.475500e+00 2.837200e+00
+7.000000e+00 1.800000e+00 1.800000e+00 2.743600e+00 3.962800e-01 6.027500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d140-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d140-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t140
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 2.208100e+00 1.850500e-01 2.195600e-01
+3.200000e+00 4.000000e-01 4.000000e-01 5.921000e+00 3.030200e-01 3.544900e-01
+3.800000e+00 2.000000e-01 2.000000e-01 1.030500e+01 5.653400e-01 6.553600e-01
+4.200000e+00 2.000000e-01 2.000000e-01 1.352800e+01 6.477500e-01 6.885100e-01
+4.600000e+00 2.000000e-01 2.000000e-01 1.688200e+01 7.236100e-01 9.713500e-01
+5.000000e+00 2.000000e-01 2.000000e-01 1.681400e+01 7.221500e-01 1.004100e+00
+7.000000e+00 1.800000e+00 1.800000e+00 3.133700e+00 1.039200e-01 2.169200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d141-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d141-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t141
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 3.192300e-01 1.120025e-01 1.120025e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.047800e-01 7.255875e-02 7.255875e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.408100e-01 5.214738e-02 5.214738e-02
+1.775000e+02 1.250000e+01 1.250000e+01 1.241700e-01 4.096810e-02 4.096810e-02
+2.200000e+02 3.000000e+01 3.000000e+01 1.108600e-01 2.379134e-02 2.379134e-02
+4.675000e+02 2.175000e+02 2.175000e+02 1.981600e-02 5.650998e-03 5.650998e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d141-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d141-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t141
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.058900e-01 2.813800e-02 3.543100e-02
+1.275000e+02 1.250000e+01 1.250000e+01 2.306600e-01 3.016000e-02 3.937900e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.066700e-01 2.396600e-02 3.607400e-02
+1.775000e+02 1.250000e+01 1.250000e+01 1.733700e-01 2.204000e-02 3.342500e-02
+2.200000e+02 3.000000e+01 3.000000e+01 1.232900e-01 1.758800e-02 3.371500e-02
+4.675000e+02 2.175000e+02 2.175000e+02 2.357800e-02 3.758700e-03 6.331500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d141-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d141-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t141
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.314000e-01 9.056700e-03 1.507300e-02
+1.275000e+02 1.250000e+01 1.250000e+01 2.537800e-01 1.122200e-02 1.632900e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.224700e-01 1.050700e-02 1.406000e-02
+1.775000e+02 1.250000e+01 1.250000e+01 1.813300e-01 9.486200e-03 1.208100e-02
+2.200000e+02 3.000000e+01 3.000000e+01 1.248500e-01 5.080900e-03 6.374900e-03
+4.675000e+02 2.175000e+02 2.175000e+02 1.989200e-02 7.532100e-04 9.231200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d142-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d142-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t142
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.829000e+00 1.063194e+01 1.063194e+01
+7.500000e-01 5.000000e-02 5.000000e-02 7.063200e+01 4.429856e+01 4.429856e+01
+8.500000e-01 5.000000e-02 5.000000e-02 1.927300e+02 8.025927e+01 8.025927e+01
+9.250000e-01 2.500000e-02 2.500000e-02 3.382100e+02 1.371993e+02 1.371993e+02
+9.750000e-01 2.500000e-02 2.500000e-02 4.062000e+02 1.660804e+02 1.660804e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d142-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d142-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t142
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.277500e+01 1.784700e+00 3.744300e+00
+7.500000e-01 5.000000e-02 5.000000e-02 6.080600e+01 8.843000e+00 9.730000e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.231300e+02 1.735900e+01 2.371100e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.078000e+02 2.311600e+01 4.653400e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.813600e+02 3.676700e+01 5.111300e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d142-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d142-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t142
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.204700e+01 4.620800e-01 5.575400e-01
+7.500000e-01 5.000000e-02 5.000000e-02 6.336500e+01 2.803800e+00 3.373100e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.279300e+02 3.983900e+00 5.374100e+00
+9.250000e-01 2.500000e-02 2.500000e-02 2.126300e+02 7.263500e+00 9.085400e+00
+9.750000e-01 2.500000e-02 2.500000e-02 2.801700e+02 8.337800e+00 1.225100e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d143-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d143-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t143
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.011900e+01 6.015301e+00 6.015301e+00
+3.200000e+00 4.000000e-01 4.000000e-01 1.441500e+01 7.616625e+00 7.616625e+00
+4.000000e+00 4.000000e-01 4.000000e-01 1.753800e+01 1.010305e+01 1.010305e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.057100e+01 1.376363e+01 1.376363e+01
+5.600000e+00 4.000000e-01 4.000000e-01 1.338700e+01 9.289119e+00 9.289119e+00
+7.400000e+00 1.400000e+00 1.400000e+00 1.147000e+00 7.083976e-01 7.083976e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d143-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d143-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t143
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 5.041500e+00 6.305600e-01 6.808800e-01
+3.200000e+00 4.000000e-01 4.000000e-01 1.015700e+01 1.416100e+00 2.615100e+00
+4.000000e+00 4.000000e-01 4.000000e-01 1.669400e+01 2.062600e+00 3.861900e+00
+4.800000e+00 4.000000e-01 4.000000e-01 1.898800e+01 2.606200e+00 3.640800e+00
+5.600000e+00 4.000000e-01 4.000000e-01 1.067500e+01 1.482900e+00 2.199400e+00
+7.400000e+00 1.400000e+00 1.400000e+00 9.107600e-01 1.466000e-01 2.447600e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d143-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d143-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t143
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 4.017500e+00 2.496100e-01 3.626100e-01
+3.200000e+00 4.000000e-01 4.000000e-01 8.862000e+00 3.707200e-01 4.803700e-01
+4.000000e+00 4.000000e-01 4.000000e-01 1.578900e+01 4.948300e-01 5.839000e-01
+4.800000e+00 4.000000e-01 4.000000e-01 2.063900e+01 5.657500e-01 9.146400e-01
+5.600000e+00 4.000000e-01 4.000000e-01 1.203200e+01 4.319600e-01 7.398200e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.118200e+00 7.038900e-02 1.151500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d144-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d144-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t144
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 3.586100e-01 2.847792e-01 2.847792e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.928800e-01 2.004844e-01 2.004844e-01
+1.525000e+02 1.250000e+01 1.250000e+01 3.246600e-01 1.533856e-01 1.533856e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.148800e-01 1.301488e-01 1.301488e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.637900e-01 9.830358e-02 9.830358e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.566400e-01 8.339904e-02 8.339904e-02
+3.000000e+02 5.000000e+01 5.000000e+01 1.011500e-01 5.663508e-02 5.663508e-02
+4.150000e+02 6.500000e+01 6.500000e+01 4.725400e-02 2.339085e-02 2.339085e-02
+5.825000e+02 1.025000e+02 1.025000e+02 8.883300e-03 5.141496e-03 5.141496e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d144-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d144-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t144
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.360800e-01 3.254100e-02 3.997100e-02
+1.275000e+02 1.250000e+01 1.250000e+01 2.736000e-01 3.329400e-02 4.618700e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.506700e-01 2.991800e-02 6.328300e-02
+1.775000e+02 1.250000e+01 1.250000e+01 2.153400e-01 2.457100e-02 4.439500e-02
+2.050000e+02 1.500000e+01 1.500000e+01 1.802300e-01 2.677100e-02 5.693700e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.401200e-01 1.564900e-02 2.655800e-02
+3.000000e+02 5.000000e+01 5.000000e+01 8.951600e-02 1.349100e-02 2.013200e-02
+4.150000e+02 6.500000e+01 6.500000e+01 3.434900e-02 4.557400e-03 1.402800e-02
+5.825000e+02 1.025000e+02 1.025000e+02 7.978700e-03 1.068200e-03 1.368800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d144-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d144-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t144
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.682500e-01 9.751300e-03 1.674800e-02
+1.275000e+02 1.250000e+01 1.250000e+01 3.044800e-01 1.229200e-02 1.774700e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.715300e-01 1.160800e-02 1.485000e-02
+1.775000e+02 1.250000e+01 1.250000e+01 2.276000e-01 1.062800e-02 1.307900e-02
+2.050000e+02 1.500000e+01 1.500000e+01 1.840300e-01 8.723800e-03 1.193600e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.433800e-01 7.700300e-03 8.618100e-03
+3.000000e+02 5.000000e+01 5.000000e+01 8.047900e-02 3.159800e-03 3.674600e-03
+4.150000e+02 6.500000e+01 6.500000e+01 2.760700e-02 1.623200e-03 2.186300e-03
+5.825000e+02 1.025000e+02 1.025000e+02 5.354000e-03 5.692300e-04 7.890300e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d145-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d145-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t145
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.081500e+01 1.340513e+01 1.340513e+01
+1.000000e+00 5.000000e-01 5.000000e-01 7.933800e+00 1.453248e+01 1.453248e+01
+5.000000e+00 3.500000e+00 3.500000e+00 5.131300e+00 1.108318e+01 1.108318e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d145-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d145-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t145
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 4.550600e+01 6.389100e+00 8.944800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 5.290500e+00 4.758300e-01 1.213800e+00
+5.000000e+00 3.500000e+00 3.500000e+00 9.981000e-01 1.181700e-01 2.592400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d145-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d145-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t145
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 4.554800e+01 7.517200e-01 1.603100e+00
+1.000000e+00 5.000000e-01 5.000000e-01 5.131800e+00 2.523200e-01 2.853600e-01
+5.000000e+00 3.500000e+00 3.500000e+00 1.523100e+00 1.374600e-01 1.651300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d146-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d146-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t146
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.779900e-01 8.090187e-01 8.090187e-01
+8.000000e-01 1.000000e-01 1.000000e-01 8.901100e+00 3.877624e+00 3.877624e+00
+9.500000e-01 5.000000e-02 5.000000e-02 3.670100e+01 1.155229e+01 1.155229e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d146-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d146-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t146
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.499800e+00 2.920200e-01 4.895300e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.087500e+01 1.950100e+00 3.323400e+00
+9.500000e-01 5.000000e-02 5.000000e-02 3.184500e+01 5.320200e+00 9.142800e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d146-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d146-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t146
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.652300e+00 1.711300e-01 2.110200e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.215200e+01 8.682100e-01 1.171900e+00
+9.500000e-01 5.000000e-02 5.000000e-02 3.369700e+01 2.044600e+00 2.568500e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d147-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d147-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t147
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.700000e+00 1.500000e+00 1.500000e+00 5.926800e-01 2.795387e-01 2.795387e-01
+5.600000e+00 4.000000e-01 4.000000e-01 2.243100e+00 8.148347e-01 8.148347e-01
+7.400000e+00 1.400000e+00 1.400000e+00 7.249500e-01 3.906053e-01 3.906053e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d147-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d147-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t147
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.700000e+00 1.500000e+00 1.500000e+00 9.124100e-01 1.824300e-01 2.578300e-01
+5.600000e+00 4.000000e-01 4.000000e-01 2.269900e+00 2.817400e-01 7.024200e-01
+7.400000e+00 1.400000e+00 1.400000e+00 6.537700e-01 1.258600e-01 2.023800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d147-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d147-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t147
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.700000e+00 1.500000e+00 1.500000e+00 8.459900e-01 5.914900e-02 6.840600e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.672200e+00 2.035700e-01 2.902100e-01
+7.400000e+00 1.400000e+00 1.400000e+00 8.064800e-01 5.977800e-02 9.021300e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d148-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d148-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t148
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 2.891900e-02 1.133468e-02 1.133468e-02
+4.525000e+02 2.325000e+02 2.325000e+02 3.454200e-03 1.637921e-03 1.637921e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d148-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d148-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t148
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 2.582200e-02 3.978900e-03 7.630100e-03
+4.525000e+02 2.325000e+02 2.325000e+02 5.694300e-03 1.162800e-03 1.730700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d148-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d148-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t148
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 3.105100e-02 1.658800e-03 2.820300e-03
+4.525000e+02 2.325000e+02 2.325000e+02 5.409100e-03 3.798900e-04 4.199000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d149-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d149-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t149
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.570500e+00 1.202954e+00 1.202954e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.869100e-01 6.709501e-01 6.709501e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d149-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d149-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t149
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.753000e+00 1.067200e+00 1.685900e+00
+1.000000e+00 5.000000e-01 5.000000e-01 5.601900e-01 6.930800e-02 1.839700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_EL/d149-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_EL/d149-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t149
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.246700e+00 2.783900e-01 4.721300e-01
+1.000000e+00 5.000000e-01 5.000000e-01 5.409900e-01 8.192500e-02 8.663100e-02
+END YODA_SCATTER2D_V2
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1517194_MU.info b/analyses/pluginATLAS/ATLAS_2017_I1517194_MU.info
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2017_I1517194_MU.info
@@ -0,0 +1,50 @@
+Name: ATLAS_2017_I1517194_MU
+Year: 2017
+Summary: Electroweak Wjj production at 8 TeV
+Experiment: ATLAS
+Collider: LHC
+InspireID: 1517194
+Status: VALIDATED
+Authors:
+ - Christian Johnson <christian.johnson@cern.ch>
+ - Christian Gutschow <chris.g@cern.ch>
+References:
+ - Eur.Phys.J. C77 (2017) no.7, 474
+ - arXiv:1703.04362 [hep-ex]
+Keywords:
+ - VJETS
+ - ELECTROWEAK
+ - VBF
+ - VJJ
+RunInfo:
+ pp -> electroweak muon + neutrino + 2 jets at 8 TeV
+Luminosity_fb: 20.2
+NeedCrossSection: yes
+Beams: [p+, p+]
+Energies: [8000]
+PtCuts: [30.,30.,25.]
+Description:
+ 'Measurements of the electroweak production of a $W$ boson in association with two jets at high dijet invariant mass
+ are performed using $\sqrt{s} = 7$ and 8 TeV proton-proton collision data produced by the Large Hadron Collider,
+ corresponding respectively to 4.7 and 20.2 fb$^{-1}$ of integrated luminosity collected by the ATLAS detector.
+ The measurements are sensitive to the production of a $W$ boson via a triple-gauge-boson vertex and include both
+ the fiducial and differential cross sections of the electroweak process.'
+BibKey: Aaboud:2017fye
+BibTex: '@article{Aaboud:2017fye,
+ author = "Aaboud, Morad and others",
+ title = "{Measurements of electroweak $Wjj$ production and
+ constraints on anomalous gauge couplings with the ATLAS
+ detector}",
+ collaboration = "ATLAS",
+ journal = "Eur. Phys. J.",
+ volume = "C77",
+ year = "2017",
+ number = "7",
+ pages = "474",
+ doi = "10.1140/epjc/s10052-017-5007-2",
+ eprint = "1703.04362",
+ archivePrefix = "arXiv",
+ primaryClass = "hep-ex",
+ reportNumber = "CERN-EP-2017-008",
+ SLACcitation = "%%CITATION = ARXIV:1703.04362;%%"
+}'
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1517194_MU.plot b/analyses/pluginATLAS/ATLAS_2017_I1517194_MU.plot
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2017_I1517194_MU.plot
@@ -0,0 +1,898 @@
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d..
+RatioPlotYMax=2.0
+RatioPlotYMin=0.0
+LegendAlign=r
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d11-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d12-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d13-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d14-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d15-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d16-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d17-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d18-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d19-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d20-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d21-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d22-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d23-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d24-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d25-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d26-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d27-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d28-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d29-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d30-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d31-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d32-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d33-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d34-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d35-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d36-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d37-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d38-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d39-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d40-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d41-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d42-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d43-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d44-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d45-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d46-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Jet centrality
+YLabel=1/\sigma $\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d47-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d48-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d49-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d50-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d51-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d52-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d53-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d54-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d55-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d56-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d57-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d58-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d59-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d60-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d61-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d62-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d63-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d64-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d65-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d66-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d67-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d68-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d69-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d70-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d71-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d72-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d73-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d74-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d75-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton control region: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d76-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d77-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d78-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d79-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d80-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d81-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d82-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d83-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d84-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d85-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d86-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d87-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d88-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d89-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d90-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d91-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d92-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d93-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d94-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 0.5$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d95-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d96-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d97-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d98-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d99-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Jet centrality
+YLabel=$\langle N_\text{jet}^\text{gap} \rangle \text{d}\sigma / \text{d}C_j$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d100-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=$\text{d}\sigma / \text{d}C_\ell$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d101-x01-y01
+Title=QCD+EW $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d102-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d103-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d104-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d105-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d106-x01-y01
+Title=QCD+EW $Wjj$ forward-lepton/central-jet region: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d107-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d108-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d109-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d110-x01-y01
+Title=QCD+EW $Wjj$ central-jet validation region: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d111-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=$\text{d}\sigma / \text{d}M_{jj}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d112-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d113-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d114-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d115-x01-y01
+Title=QCD+EW $Wjj$ signal region ($M_{jj}>0.5$ TeV): $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d116-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d117-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d118-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d119-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d120-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d121-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=Dijet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d122-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d123-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d124-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d125-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Dijet mass [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}M_{jj}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d126-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d127-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta y$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d128-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d129-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d130-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d131-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=1/\sigma $\text{d}\sigma / \text{d}\Delta \phi$
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d132-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=1/\sigma $\text{d}\sigma / \text{d}p_\text{T}$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d133-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Lepton centrality
+YLabel=1/\sigma $\text{d}\sigma / \text{d}C_\ell$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d134-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=1/\sigma $\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d135-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d136-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d137-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d138-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.5$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d139-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d140-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d141-x01-y01
+Title=EW-only $Wjj$ signal region ($M_{jj}>1.0$ TeV): $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d142-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d143-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d144-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d145-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 1.0$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d146-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta\phi(j_1,j_2) / \pi$
+YLabel=$\text{d}\sigma / \text{d}\Delta \phi$ [fb]
+LegendAlign=l
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d147-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=$\Delta y(j_1, j_2)$
+YLabel=$\text{d}\sigma / \text{d}\Delta y$ [fb]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d148-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Leading-jet $p_\text{T}$ [GeV]
+YLabel=$\text{d}\sigma / \text{d}p_\text{T}$ [fb/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2017_I1517194_MU/d149-x01-y01
+Title=EW-only $Wjj$ inclusive region with $M_{jj} > 2.0$ TeV: $W\to\mu\nu$
+XLabel=Number of jets in the rapidity gap
+YLabel=$\text{d}\sigma / \text{d}N_\text{jets}^\text{gap}$ [fb]
+# END PLOT
+
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1517194_MU.yoda b/analyses/pluginATLAS/ATLAS_2017_I1517194_MU.yoda
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2017_I1517194_MU.yoda
@@ -0,0 +1,8081 @@
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d01-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d01-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.600000e+01 5.000000e+00 5.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d01-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d01-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.300000e+01 5.000000e+00 5.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d01-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d01-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.000000e+01 8.000000e+00 8.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d01-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d01-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t1
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.900000e+01 5.000000e-01 5.000000e-01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d02-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d02-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t2
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.450000e+02 3.900000e+01 3.900000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d02-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d02-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t2
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.550000e+02 5.100000e+01 5.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d03-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d03-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+9.600000e+01 8.000000e+00 8.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d03-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d03-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+8.900000e+01 7.000000e+00 7.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d03-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d03-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.300000e+01 1.100000e+01 1.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d03-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d03-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t3
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.100000e+01 1.000000e+00 1.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d04-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d04-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.630000e+02 2.100000e+01 2.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d04-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d04-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.340000e+02 2.600000e+01 2.600000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d04-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d04-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+6.400000e+01 3.600000e+01 3.600000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d04-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d04-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t4
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.200000e+01 1.000000e+00 1.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d05-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d05-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t5
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.700000e+03 1.100000e+02 1.100000e+02
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d05-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d05-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t5
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.420000e+03 1.500000e+02 1.500000e+02
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d06-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d06-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.300000e+01 2.000000e+00 2.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d06-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d06-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.400000e+01 1.000000e+00 1.000000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d06-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d06-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.600000e+00 2.100000e+00 2.100000e+00
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d06-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d06-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t6
+Type: Scatter1D
+---
+# xval xerr- xerr+
+6.900000e+00 2.000000e-01 2.000000e-01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d07-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d07-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t7
+Type: Scatter1D
+---
+# xval xerr- xerr+
+3.130000e+02 3.000000e+01 3.000000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d07-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d07-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t7
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.650000e+02 3.200000e+01 3.200000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d08-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d08-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t8
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.920000e+02 3.600000e+01 3.600000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d08-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d08-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t8
+Type: Scatter1D
+---
+# xval xerr- xerr+
+2.350000e+02 2.800000e+01 2.800000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d09-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d09-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t9
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.440000e+02 3.502856e+01 3.502856e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d09-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d09-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t9
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.440000e+02 1.100000e+01 1.100000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d10-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d10-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+5.460000e+02 3.500000e+01 3.500000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d10-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d10-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+4.650000e+02 3.900000e+01 3.900000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d10-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d10-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.590000e+02 2.700000e+01 2.700000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER1D_V2 /REF/ATLAS_2017_I1517194_MU/d10-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d10-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t10
+Type: Scatter1D
+---
+# xval xerr- xerr+
+1.980000e+02 1.200000e+01 1.200000e+01
+END YODA_SCATTER1D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d11-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d11-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t11
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.749800e-03 4.232811e-04 4.287836e-04
+7.500000e+01 2.500000e+01 2.500000e+01 6.616100e-03 3.022254e-04 3.100313e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.693800e-03 2.513928e-04 2.465816e-04
+1.925000e+02 3.250000e+01 3.250000e+01 1.981800e-03 1.724307e-04 1.687993e-04
+2.625000e+02 3.750000e+01 3.750000e+01 8.348400e-04 3.433320e-04 3.434536e-04
+3.975000e+02 9.750000e+01 9.750000e+01 7.549200e-05 6.703945e-04 6.703707e-04
+6.975000e+02 2.025000e+02 2.025000e+02 9.695400e-06 7.108535e-06 7.150889e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d11-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d11-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t11
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.239800e-03 1.671900e-04 1.537800e-04
+7.500000e+01 2.500000e+01 2.500000e+01 5.782700e-03 3.074600e-04 1.785100e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.876600e-03 1.339900e-04 1.442600e-04
+1.925000e+02 3.250000e+01 3.250000e+01 2.098800e-03 8.731500e-05 1.083800e-04
+2.625000e+02 3.750000e+01 3.750000e+01 9.471300e-04 6.157900e-05 6.167300e-05
+3.975000e+02 9.750000e+01 9.750000e+01 2.586000e-04 1.886600e-05 1.904300e-05
+6.975000e+02 2.025000e+02 2.025000e+02 2.074400e-05 3.918100e-06 3.685900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d11-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d11-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t11
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.484800e-03 3.184600e-04 8.493000e-05
+7.500000e+01 2.500000e+01 2.500000e+01 5.866100e-03 3.147500e-05 2.220000e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.747800e-03 1.022400e-04 4.123400e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.962700e-03 5.974100e-05 2.347300e-04
+2.625000e+02 3.750000e+01 3.750000e+01 9.212000e-04 3.596300e-05 2.579900e-05
+3.975000e+02 9.750000e+01 9.750000e+01 2.621700e-04 1.833200e-05 1.460400e-05
+6.975000e+02 2.025000e+02 2.025000e+02 2.420000e-05 1.322200e-06 1.930400e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d12-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d12-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t12
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 9.751100e-02 3.977561e-02 4.084700e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.765900e-01 5.286942e-02 5.808940e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.206100e+00 1.194382e-01 1.181789e-01
+8.500000e-01 5.000000e-02 5.000000e-02 2.246600e+00 1.386490e-01 1.371997e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.370700e+00 2.434256e-01 2.357765e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.842400e+00 3.555396e-01 3.616982e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d12-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d12-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t12
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 1.590100e-01 8.723300e-03 1.304800e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.869100e-01 2.390800e-02 4.090400e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.207900e+00 1.359500e-01 5.919100e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.344600e+00 9.678800e-02 7.534300e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.009600e+00 1.747300e-01 1.377000e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.347600e+00 2.075000e-01 1.826800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d12-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d12-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t12
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 1.335100e-01 4.507200e-03 1.568300e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.138700e-01 1.995400e-02 0.000000e+00
+7.500000e-01 5.000000e-02 5.000000e-02 1.068000e+00 4.893100e-02 9.925600e-03
+8.500000e-01 5.000000e-02 5.000000e-02 2.306300e+00 4.182800e-02 5.384700e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.241400e+00 1.185300e-01 1.532600e-01
+9.750000e-01 2.500000e-02 2.500000e-02 6.019500e+00 5.855200e-02 1.348000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d13-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d13-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t13
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.338100e-02 1.322149e-02 1.110759e-02
+3.200000e+00 4.000000e-01 4.000000e-01 1.236800e-01 1.453089e-02 1.377971e-02
+4.000000e+00 4.000000e-01 4.000000e-01 2.349200e-01 2.236358e-02 2.037699e-02
+4.800000e+00 4.000000e-01 4.000000e-01 2.834600e-01 3.255250e-02 3.248636e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.637300e-01 1.988253e-02 2.680273e-02
+7.400000e+00 1.400000e+00 1.400000e+00 4.309500e-02 9.407138e-03 8.677072e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d13-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d13-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t13
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 8.621500e-02 5.062100e-03 5.536000e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.400100e-01 7.046500e-03 6.643900e-03
+4.000000e+00 4.000000e-01 4.000000e-01 2.166400e-01 8.359100e-03 9.630700e-03
+4.800000e+00 4.000000e-01 4.000000e-01 3.167200e-01 1.178000e-02 1.072300e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.420800e-01 1.576300e-02 1.181000e-02
+7.400000e+00 1.400000e+00 1.400000e+00 4.237900e-02 4.155600e-03 2.035000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d13-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d13-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t13
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.090400e-01 4.823400e-03 1.074600e-02
+3.200000e+00 4.000000e-01 4.000000e-01 1.739800e-01 6.866900e-03 7.563000e-03
+4.000000e+00 4.000000e-01 4.000000e-01 2.314000e-01 1.125200e-03 7.648700e-03
+4.800000e+00 4.000000e-01 4.000000e-01 2.958200e-01 5.396400e-03 1.608000e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.899700e-01 5.055600e-03 1.239900e-02
+7.400000e+00 1.400000e+00 1.400000e+00 4.279600e-02 5.418600e-03 2.819200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d14-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d14-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t14
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.211900e-03 9.080313e-04 1.006137e-03
+1.400000e+02 2.500000e+01 2.500000e+01 4.935800e-03 2.966745e-04 2.758397e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.289800e-03 2.412451e-04 2.491068e-04
+2.500000e+02 3.000000e+01 3.000000e+01 2.146000e-03 2.152008e-04 2.015250e-04
+3.150000e+02 3.500000e+01 3.500000e+01 1.223400e-03 3.176380e-04 3.070309e-04
+3.925000e+02 4.250000e+01 4.250000e+01 9.110500e-04 1.164833e-04 1.114131e-04
+5.075000e+02 7.250000e+01 7.250000e+01 4.933900e-04 6.944737e-05 6.261648e-05
+7.300000e+02 1.500000e+02 1.500000e+02 8.824000e-05 2.004914e-05 1.974540e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d14-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d14-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t14
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.313200e-03 3.447100e-04 3.244800e-04
+1.400000e+02 2.500000e+01 2.500000e+01 4.565400e-03 1.476900e-04 1.601200e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.443000e-03 1.423500e-04 1.276700e-04
+2.500000e+02 3.000000e+01 3.000000e+01 2.332100e-03 1.155800e-04 1.053900e-04
+3.150000e+02 3.500000e+01 3.500000e+01 1.532800e-03 8.221700e-05 8.194200e-05
+3.925000e+02 4.250000e+01 4.250000e+01 9.368800e-04 5.091600e-05 5.667400e-05
+5.075000e+02 7.250000e+01 7.250000e+01 5.123200e-04 2.957000e-05 3.837100e-05
+7.300000e+02 1.500000e+02 1.500000e+02 1.008700e-04 9.784700e-06 8.927000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d14-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d14-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t14
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.274200e-03 3.095900e-04 1.827800e-04
+1.400000e+02 2.500000e+01 2.500000e+01 3.896800e-03 7.233700e-05 1.225600e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.224100e-03 8.615000e-05 7.443500e-05
+2.500000e+02 3.000000e+01 3.000000e+01 2.296100e-03 1.045900e-04 0.000000e+00
+3.150000e+02 3.500000e+01 3.500000e+01 1.655500e-03 7.178700e-05 7.007500e-05
+3.925000e+02 4.250000e+01 4.250000e+01 1.085700e-03 3.625200e-05 5.417900e-05
+5.075000e+02 7.250000e+01 7.250000e+01 6.390900e-04 4.034300e-05 3.477800e-05
+7.300000e+02 1.500000e+02 1.500000e+02 1.320800e-04 0.000000e+00 5.523000e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d15-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d15-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t15
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.935900e+00 1.770283e-01 1.752405e-01
+2.500000e-01 1.000000e-01 1.000000e-01 1.570100e+00 1.140556e-01 1.134172e-01
+5.000000e-01 1.500000e-01 1.500000e-01 1.058600e+00 6.660687e-02 6.792790e-02
+8.250000e-01 1.750000e-01 1.750000e-01 1.895200e-01 2.497173e-02 2.547942e-02
+1.500000e+00 5.000000e-01 5.000000e-01 1.168600e-02 3.338337e-03 3.320034e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d15-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d15-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t15
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.810300e+00 1.208200e-01 5.936800e-02
+2.500000e-01 1.000000e-01 1.000000e-01 1.670500e+00 6.907000e-02 6.500500e-02
+5.000000e-01 1.500000e-01 1.500000e-01 1.022200e+00 3.154400e-02 8.198000e-02
+8.250000e-01 1.750000e-01 1.750000e-01 2.131000e-01 1.859700e-02 1.637900e-02
+1.500000e+00 5.000000e-01 5.000000e-01 1.310600e-02 2.038200e-03 2.017800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d15-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d15-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t15
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.783400e+00 4.256400e-02 5.687700e-04
+2.500000e-01 1.000000e-01 1.000000e-01 1.615900e+00 0.000000e+00 6.360500e-02
+5.000000e-01 1.500000e-01 1.500000e-01 1.042200e+00 1.258100e-02 0.000000e+00
+8.250000e-01 1.750000e-01 1.750000e-01 2.307200e-01 2.185600e-02 1.116500e-03
+1.500000e+00 5.000000e-01 5.000000e-01 1.588700e-02 6.493200e-04 1.492400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d16-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d16-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t16
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.632100e+00 8.139210e-02 8.650309e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.839900e+00 9.080709e-02 9.079465e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.151400e+00 1.621326e-01 1.621340e-01
+6.750000e-01 1.250000e-01 1.250000e-01 4.450200e-01 4.802816e-02 4.379319e-02
+9.000000e-01 1.000000e-01 1.000000e-01 8.375700e-02 1.696566e-02 1.654870e-02
+1.100000e+00 1.000000e-01 1.000000e-01 2.444000e-02 8.960275e-03 9.146675e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d16-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d16-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t16
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.641100e+00 5.361500e-02 9.437600e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.834200e+00 6.979500e-02 4.664700e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.258900e+00 6.173500e-02 4.656100e-02
+6.750000e-01 1.250000e-01 1.250000e-01 3.905900e-01 1.993100e-02 2.938600e-02
+9.000000e-01 1.000000e-01 1.000000e-01 7.355400e-02 9.763500e-03 1.101500e-02
+1.100000e+00 1.000000e-01 1.000000e-01 1.878200e-02 4.898400e-03 5.685500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d16-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d16-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t16
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.469100e+00 1.254200e-01 7.854200e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.710900e+00 5.139400e-02 0.000000e+00
+4.750000e-01 7.500000e-02 7.500000e-02 1.444500e+00 4.751000e-02 1.492600e-01
+6.750000e-01 1.250000e-01 1.250000e-01 4.911600e-01 1.906200e-02 2.794500e-02
+9.000000e-01 1.000000e-01 1.000000e-01 9.905700e-02 1.735600e-02 4.798700e-03
+1.100000e+00 1.000000e-01 1.000000e-01 2.372400e-02 6.956100e-04 5.791000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d17-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d17-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t17
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.453100e-01 2.915590e-02 3.067239e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.652800e-01 1.821431e-02 1.778858e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.127600e-01 1.177660e-02 1.213810e-02
+3.000000e+00 5.000000e-01 5.000000e-01 5.119200e-02 1.000771e-02 8.594720e-03
+6.000000e+00 2.500000e+00 2.500000e+00 2.545900e-02 8.098885e-03 7.657466e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d17-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d17-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t17
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.713800e-01 1.753300e-02 2.481000e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.659600e-01 1.415800e-02 1.203300e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.088600e-01 6.584100e-03 7.909100e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.887500e-02 1.007500e-02 3.023800e-03
+6.000000e+00 2.500000e+00 2.500000e+00 1.492000e-02 2.059200e-03 2.499600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d17-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d17-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t17
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.319500e-01 2.661200e-02 1.470700e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.883800e-01 2.408000e-03 1.495100e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.247000e-01 1.134800e-02 1.348000e-02
+3.000000e+00 5.000000e-01 5.000000e-01 4.325500e-02 5.562300e-03 0.000000e+00
+6.000000e+00 2.500000e+00 2.500000e+00 1.171900e-02 0.000000e+00 4.214800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d18-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d18-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.440400e-03 1.444966e-04 1.591914e-04
+5.800000e+02 3.500000e+01 3.500000e+01 3.204600e-03 1.031389e-04 1.037089e-04
+6.550000e+02 4.000000e+01 4.000000e+01 2.167800e-03 5.068799e-05 4.855705e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.470600e-03 5.533391e-05 3.547807e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.771800e-04 3.221458e-05 4.100677e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.087400e-04 2.092369e-05 2.283223e-05
+1.042500e+03 5.750000e+01 5.750000e+01 3.716000e-04 2.189913e-05 1.686269e-05
+1.150000e+03 5.000000e+01 5.000000e+01 2.132600e-04 1.484543e-05 1.327452e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.349800e-04 1.005004e-05 9.475520e-06
+1.425000e+03 7.500000e+01 7.500000e+01 8.606100e-05 7.638507e-06 7.559277e-06
+1.750000e+03 2.500000e+02 2.500000e+02 2.592100e-05 4.816414e-06 4.932878e-06
+2.350000e+03 3.500000e+02 3.500000e+02 4.134000e-06 9.226464e-07 6.248307e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.995900e-07 9.477605e-08 9.183850e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d18-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d18-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.327300e-03 8.959800e-05 6.073900e-05
+5.800000e+02 3.500000e+01 3.500000e+01 3.231200e-03 6.876500e-05 5.383300e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.199600e-03 2.816700e-05 2.209800e-04
+7.400000e+02 4.500000e+01 4.500000e+01 1.458300e-03 4.772800e-05 2.290900e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.367200e-04 2.534400e-05 2.149900e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.019500e-04 1.968300e-05 2.233300e-05
+1.042500e+03 5.750000e+01 5.750000e+01 3.734400e-04 1.441100e-05 9.575900e-06
+1.150000e+03 5.000000e+01 5.000000e+01 2.386900e-04 9.187000e-06 1.263300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.464900e-04 6.239300e-06 5.689100e-06
+1.425000e+03 7.500000e+01 7.500000e+01 8.480900e-05 5.210700e-06 4.098200e-06
+1.750000e+03 2.500000e+02 2.500000e+02 2.961900e-05 1.367000e-06 1.856200e-06
+2.350000e+03 3.500000e+02 3.500000e+02 4.342600e-06 4.945700e-07 4.660800e-07
+3.350000e+03 6.500000e+02 6.500000e+02 2.395100e-07 7.790500e-08 7.294600e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d18-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d18-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.216800e-03 6.697900e-05 5.900400e-05
+5.800000e+02 3.500000e+01 3.500000e+01 3.184000e-03 3.231100e-05 2.809700e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.170600e-03 1.266500e-05 9.978400e-06
+7.400000e+02 4.500000e+01 4.500000e+01 1.446000e-03 6.956800e-06 5.955400e-06
+8.325000e+02 4.750000e+01 4.750000e+01 9.513000e-04 7.448400e-06 8.316700e-06
+9.325000e+02 5.250000e+01 5.250000e+01 6.213000e-04 8.686500e-06 9.835200e-06
+1.042500e+03 5.750000e+01 5.750000e+01 3.894000e-04 7.584600e-06 8.678800e-06
+1.150000e+03 5.000000e+01 5.000000e+01 2.527200e-04 6.468300e-06 7.434000e-06
+1.275000e+03 7.500000e+01 7.500000e+01 1.538600e-04 4.744300e-06 5.490300e-06
+1.425000e+03 7.500000e+01 7.500000e+01 9.608800e-05 4.001700e-06 5.471800e-06
+1.750000e+03 2.500000e+02 2.500000e+02 3.347500e-05 1.720700e-06 2.048000e-06
+2.350000e+03 3.500000e+02 3.500000e+02 4.742900e-06 3.186000e-07 3.818100e-07
+3.350000e+03 6.500000e+02 6.500000e+02 2.798700e-07 2.478700e-08 3.030100e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d18-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d18-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t18
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 4.056200e-03 0.000000e+00 8.612300e-05
+5.800000e+02 3.500000e+01 3.500000e+01 3.039100e-03 0.000000e+00 9.947800e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.138100e-03 0.000000e+00 6.928600e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.438800e-03 1.350100e-05 7.192600e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.003600e-03 1.038500e-04 0.000000e+00
+9.325000e+02 5.250000e+01 5.250000e+01 6.275600e-04 3.510700e-06 1.274000e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.088800e-04 1.119200e-05 0.000000e+00
+1.150000e+03 5.000000e+01 5.000000e+01 2.760400e-04 1.666400e-05 0.000000e+00
+1.275000e+03 7.500000e+01 7.500000e+01 1.768400e-04 7.752600e-06 1.623600e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.029100e-04 5.546300e-06 6.072800e-06
+1.750000e+03 2.500000e+02 2.500000e+02 4.181800e-05 2.889700e-06 2.327600e-06
+2.350000e+03 3.500000e+02 3.500000e+02 6.797600e-06 2.692200e-07 5.952000e-08
+3.350000e+03 6.500000e+02 6.500000e+02 5.375300e-07 1.629000e-07 1.112500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d19-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d19-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.771700e-03 1.665906e-04 1.679781e-04
+3.750000e+01 1.250000e+01 1.250000e+01 9.135000e-03 2.472353e-04 2.857557e-04
+6.250000e+01 1.250000e+01 1.250000e+01 8.020600e-03 3.544786e-04 3.577800e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.862500e-03 1.536794e-04 1.511097e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.882600e-03 1.629814e-04 1.499845e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.400100e-03 1.735127e-04 1.533771e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.470600e-03 1.385143e-04 1.326091e-04
+2.075000e+02 1.750000e+01 1.750000e+01 8.778400e-04 8.351002e-05 7.955276e-05
+2.425000e+02 1.750000e+01 1.750000e+01 5.066500e-04 3.164659e-05 3.288326e-05
+2.800000e+02 2.000000e+01 2.000000e+01 2.900700e-04 2.658457e-05 2.569169e-05
+3.975000e+02 9.750000e+01 9.750000e+01 5.744000e-05 1.314632e-05 1.329779e-05
+6.975000e+02 2.025000e+02 2.025000e+02 3.443700e-06 1.236977e-06 1.347234e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d19-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d19-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.122500e-03 2.377800e-04 8.118200e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.598800e-03 1.612200e-04 1.580800e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.809600e-03 2.112400e-04 9.228700e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.815200e-03 8.969100e-05 1.013400e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.965400e-03 1.058700e-04 6.823300e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.620900e-03 9.381800e-05 6.233500e-05
+1.750000e+02 1.500000e+01 1.500000e+01 1.710900e-03 6.542500e-05 4.296700e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.046900e-03 4.482200e-05 4.096700e-05
+2.425000e+02 1.750000e+01 1.750000e+01 6.156500e-04 3.230400e-05 3.392600e-05
+2.800000e+02 2.000000e+01 2.000000e+01 3.581000e-04 3.086100e-05 1.729900e-05
+3.975000e+02 9.750000e+01 9.750000e+01 9.328500e-05 8.335000e-06 4.098800e-06
+6.975000e+02 2.025000e+02 2.025000e+02 4.269500e-06 8.239300e-07 6.547400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d19-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d19-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.310300e-03 2.135100e-04 1.843000e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.337100e-03 2.183100e-04 1.891500e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.348600e-03 3.977300e-05 2.923400e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.676900e-03 4.768000e-05 4.924400e-05
+1.150000e+02 1.500000e+01 1.500000e+01 3.922900e-03 5.625400e-05 6.831000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.776300e-03 9.436500e-05 1.168300e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.785000e-03 4.319200e-05 5.379400e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.106300e-03 2.750900e-05 3.121600e-05
+2.425000e+02 1.750000e+01 1.750000e+01 6.841300e-04 1.913100e-05 2.118700e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.047100e-04 1.270500e-05 1.404500e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.148100e-04 4.107200e-06 4.443700e-06
+6.975000e+02 2.025000e+02 2.025000e+02 5.954800e-06 2.747900e-07 2.902200e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d19-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d19-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t19
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.071800e-03 7.261800e-05 3.997500e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.574000e-03 1.162800e-04 1.328500e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.877600e-03 2.836300e-04 0.000000e+00
+8.750000e+01 1.250000e+01 1.250000e+01 5.778600e-03 0.000000e+00 3.900900e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.934900e-03 4.599900e-05 1.268900e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.758000e-03 2.008100e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 1.716100e-03 2.574700e-05 1.737100e-04
+2.075000e+02 1.750000e+01 1.750000e+01 1.021400e-03 5.501200e-05 7.856900e-06
+2.425000e+02 1.750000e+01 1.750000e+01 5.876200e-04 3.429700e-05 1.182700e-04
+2.800000e+02 2.000000e+01 2.000000e+01 3.370800e-04 2.142500e-05 4.763200e-05
+3.975000e+02 9.750000e+01 9.750000e+01 9.380200e-05 5.579300e-06 0.000000e+00
+6.975000e+02 2.025000e+02 2.025000e+02 5.149500e-06 6.574600e-07 3.153900e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d20-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d20-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 5.940800e-02 1.317334e-02 1.263845e-02
+4.000000e-01 1.000000e-01 1.000000e-01 1.244000e-01 1.711124e-02 1.808593e-02
+5.500000e-01 5.000000e-02 5.000000e-02 2.259900e-01 4.134359e-02 4.101133e-02
+6.250000e-01 2.500000e-02 2.500000e-02 4.310900e-01 3.877452e-02 3.251981e-02
+6.750000e-01 2.500000e-02 2.500000e-02 5.768200e-01 5.031359e-02 4.845475e-02
+7.250000e-01 2.500000e-02 2.500000e-02 8.748100e-01 2.352047e-01 2.342052e-01
+7.750000e-01 2.500000e-02 2.500000e-02 1.431400e+00 6.251322e-02 6.227322e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.119800e+00 6.563713e-02 6.561217e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.058100e+00 7.745330e-02 7.826197e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.346500e+00 1.068673e-01 1.103522e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.855400e+00 1.268200e-01 1.257618e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d20-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d20-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 9.500500e-02 6.065600e-03 4.343500e-03
+4.000000e-01 1.000000e-01 1.000000e-01 1.654000e-01 4.748400e-03 6.766200e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.277500e-01 1.899100e-02 9.461300e-03
+6.250000e-01 2.500000e-02 2.500000e-02 4.855500e-01 2.436800e-02 1.983900e-02
+6.750000e-01 2.500000e-02 2.500000e-02 6.551700e-01 1.910700e-02 3.326800e-02
+7.250000e-01 2.500000e-02 2.500000e-02 9.611200e-01 4.323300e-02 2.289300e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.352500e+00 3.829100e-02 3.698400e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.003300e+00 4.650100e-02 3.551800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.956900e+00 5.402100e-02 5.587800e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.210100e+00 1.088500e-01 6.004500e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.488200e+00 8.542400e-02 2.846700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d20-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d20-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 8.984800e-02 2.468200e-03 2.902100e-03
+4.000000e-01 1.000000e-01 1.000000e-01 1.597600e-01 5.564900e-03 8.136400e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.333800e-01 1.970000e-02 2.483600e-02
+6.250000e-01 2.500000e-02 2.500000e-02 4.330800e-01 8.620600e-03 1.002600e-02
+6.750000e-01 2.500000e-02 2.500000e-02 6.027200e-01 1.105800e-02 1.310500e-02
+7.250000e-01 2.500000e-02 2.500000e-02 8.619600e-01 1.440900e-02 1.685700e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.271200e+00 1.866400e-02 2.118800e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.892200e+00 1.823100e-02 2.035100e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.849000e+00 6.445700e-03 7.303600e-03
+9.250000e-01 2.500000e-02 2.500000e-02 4.276200e+00 4.736100e-02 3.932600e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.968700e+00 1.375600e-01 1.118400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d20-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d20-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t20
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 8.741000e-02 6.002900e-03 1.561500e-02
+4.000000e-01 1.000000e-01 1.000000e-01 1.486300e-01 4.625000e-03 1.209200e-03
+5.500000e-01 5.000000e-02 5.000000e-02 2.762100e-01 3.935100e-03 5.499000e-03
+6.250000e-01 2.500000e-02 2.500000e-02 4.486600e-01 3.522900e-02 7.930400e-03
+6.750000e-01 2.500000e-02 2.500000e-02 5.925600e-01 0.000000e+00 1.334800e-01
+7.250000e-01 2.500000e-02 2.500000e-02 8.671400e-01 0.000000e+00 1.883000e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.264500e+00 6.197300e-03 4.311500e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.012700e+00 6.342200e-02 2.327800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.917200e+00 0.000000e+00 1.106500e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.405900e+00 1.372300e-01 0.000000e+00
+9.750000e-01 2.500000e-02 2.500000e-02 5.819800e+00 9.804100e-02 1.199400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d21-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d21-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.834100e-01 1.560863e-02 1.265172e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.103900e-01 1.438733e-02 1.483056e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.598600e-01 1.295458e-02 1.378529e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.673400e-01 1.262829e-02 1.272665e-02
+3.800000e+00 2.000000e-01 2.000000e-01 3.823200e-01 1.468431e-02 1.540477e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.273400e-01 2.903756e-02 2.956039e-02
+4.800000e+00 4.000000e-01 4.000000e-01 7.306600e-02 6.444668e-03 6.944151e-03
+5.800000e+00 6.000000e-01 6.000000e-01 7.564100e-03 2.980279e-03 1.409301e-03
+7.600000e+00 1.200000e+00 1.200000e+00 8.444000e-05 6.368777e-05 5.526415e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d21-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d21-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.697300e-01 1.330300e-02 1.034100e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.125800e-01 1.158500e-02 7.799200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.543400e-01 5.982800e-03 3.940900e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.674200e-01 1.099300e-02 5.939900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.947200e-01 5.186900e-03 7.095400e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.183000e-01 1.605500e-02 4.775000e-03
+4.800000e+00 4.000000e-01 4.000000e-01 7.827300e-02 3.313300e-03 2.017700e-03
+5.800000e+00 6.000000e-01 6.000000e-01 8.711800e-03 4.518600e-04 1.131500e-03
+7.600000e+00 1.200000e+00 1.200000e+00 3.968100e-05 2.123100e-05 4.692500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d21-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d21-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.697300e-01 6.193400e-03 6.375700e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.745000e-01 3.701800e-03 3.341900e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.631500e-01 1.789100e-03 1.517200e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.399400e-01 1.249100e-03 1.873000e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.343600e-01 5.382700e-03 4.828000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 1.775400e-01 2.925800e-03 2.870600e-03
+4.800000e+00 4.000000e-01 4.000000e-01 5.926700e-02 1.611700e-03 1.896800e-03
+5.800000e+00 6.000000e-01 6.000000e-01 7.319000e-03 4.508800e-04 5.522900e-04
+7.600000e+00 1.200000e+00 1.200000e+00 4.830200e-05 4.906100e-06 6.252100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d21-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d21-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t21
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.098700e-01 2.573700e-03 1.575600e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.439500e-01 3.798600e-03 2.151100e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.848900e-01 2.224400e-02 0.000000e+00
+3.400000e+00 2.000000e-01 2.000000e-01 4.566900e-01 1.668100e-03 4.104700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.514800e-01 7.027200e-04 2.169200e-02
+4.200000e+00 2.000000e-01 2.000000e-01 1.866400e-01 3.426200e-03 1.624400e-03
+4.800000e+00 4.000000e-01 4.000000e-01 6.674700e-02 2.036000e-03 0.000000e+00
+5.800000e+00 6.000000e-01 6.000000e-01 1.068200e-02 7.713500e-04 1.641900e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.578200e-04 3.405200e-05 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d22-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d22-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.388000e-03 4.975407e-04 5.599362e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.018200e-03 2.580735e-04 2.767615e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.820600e-03 1.941004e-04 2.077425e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.299200e-03 1.483642e-04 1.483644e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.304900e-03 1.654952e-04 1.606496e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.745100e-03 1.369758e-04 1.374536e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.431500e-03 9.879302e-05 9.193812e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.526100e-03 7.596880e-05 6.456659e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.702500e-04 4.695736e-05 5.217334e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.443200e-04 6.360786e-05 6.124815e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.943800e-04 2.632154e-05 2.572892e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.496300e-04 1.730628e-05 1.676646e-05
+4.575000e+02 2.250000e+01 2.250000e+01 8.145300e-05 1.175250e-05 1.107143e-05
+5.300000e+02 5.000000e+01 5.000000e+01 2.625100e-05 5.547672e-06 5.448345e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.068100e-05 2.657746e-06 2.575246e-06
+8.425000e+02 1.575000e+02 1.575000e+02 5.869200e-07 4.266142e-07 4.151498e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d22-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d22-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.915000e-03 4.964300e-04 1.112100e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.875800e-03 1.244800e-04 1.396700e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.883500e-03 1.008100e-04 6.921800e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.328100e-03 1.103000e-04 1.083300e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.349300e-03 1.493200e-04 1.086200e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.825900e-03 1.552300e-04 6.192000e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.425600e-03 6.284200e-05 7.292800e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.498300e-03 8.801600e-05 4.130800e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.873700e-04 3.762500e-05 4.230300e-05
+3.325000e+02 1.750000e+01 1.750000e+01 5.112700e-04 3.399200e-05 2.095900e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.952300e-04 2.400800e-05 1.614900e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.623100e-04 1.468600e-05 1.149700e-05
+4.575000e+02 2.250000e+01 2.250000e+01 8.975500e-05 9.267100e-06 7.890200e-06
+5.300000e+02 5.000000e+01 5.000000e+01 3.505200e-05 4.447700e-06 3.988900e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.086900e-05 2.004100e-06 1.758700e-06
+8.425000e+02 1.575000e+02 1.575000e+02 1.546300e-06 4.088400e-07 4.524600e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d22-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d22-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.317500e-03 1.055300e-04 1.081200e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.462000e-03 1.142300e-04 1.047500e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.247500e-03 1.100500e-05 1.534300e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.107400e-03 5.019600e-05 4.071500e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.824200e-03 3.300700e-05 3.122200e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.258700e-03 2.723000e-05 2.975100e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.841300e-03 2.738300e-05 2.780400e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.844500e-03 2.273200e-05 2.267200e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.127000e-03 2.055900e-05 2.169400e-05
+3.325000e+02 1.750000e+01 1.750000e+01 6.913400e-04 1.457200e-05 1.522500e-05
+3.700000e+02 2.000000e+01 2.000000e+01 3.961000e-04 1.201800e-05 1.289300e-05
+4.125000e+02 2.250000e+01 2.250000e+01 2.268900e-04 7.501500e-06 8.057600e-06
+4.575000e+02 2.250000e+01 2.250000e+01 1.283600e-04 3.885000e-06 4.208300e-06
+5.300000e+02 5.000000e+01 5.000000e+01 5.249100e-05 2.199100e-06 2.379700e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.628200e-05 8.408800e-07 9.309900e-07
+8.425000e+02 1.575000e+02 1.575000e+02 2.382200e-06 1.390900e-07 1.542100e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d22-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d22-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t22
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.495700e-03 8.486400e-05 1.967500e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.826500e-03 8.422000e-05 2.457500e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.566200e-03 0.000000e+00 1.552100e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.448600e-03 4.563300e-05 1.646200e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.743300e-03 3.242700e-04 8.462000e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.096500e-03 4.776300e-05 1.350700e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.736100e-03 1.944500e-04 0.000000e+00
+2.650000e+02 1.500000e+01 1.500000e+01 1.678700e-03 6.022500e-07 5.423100e-05
+2.975000e+02 1.750000e+01 1.750000e+01 9.884900e-04 0.000000e+00 1.110200e-04
+3.325000e+02 1.750000e+01 1.750000e+01 6.009400e-04 2.521500e-05 3.396300e-07
+3.700000e+02 2.000000e+01 2.000000e+01 3.612900e-04 1.601000e-05 2.103800e-05
+4.125000e+02 2.250000e+01 2.250000e+01 2.155900e-04 3.543600e-05 0.000000e+00
+4.575000e+02 2.250000e+01 2.250000e+01 1.092100e-04 2.428700e-06 4.792000e-06
+5.300000e+02 5.000000e+01 5.000000e+01 4.622000e-05 4.877400e-06 4.323600e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.567800e-05 0.000000e+00 1.910600e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.466200e-06 5.122400e-07 4.625500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d23-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d23-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t23
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.258400e-03 2.478400e-04 2.465506e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.317000e-03 4.732787e-04 4.975421e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.335500e-03 2.929429e-04 2.899776e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.543400e-03 2.794172e-04 2.773066e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.532000e-03 2.552473e-04 2.486133e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.887200e-03 2.285658e-04 2.546337e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.656500e-03 1.536124e-04 1.446930e-04
+2.250000e+02 3.500000e+01 3.500000e+01 9.632900e-04 1.614283e-04 1.612225e-04
+3.775000e+02 1.175000e+02 1.175000e+02 2.131500e-04 2.621424e-05 2.707416e-05
+6.975000e+02 2.025000e+02 2.025000e+02 9.516400e-06 5.034262e-06 5.433003e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d23-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d23-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t23
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.528200e-03 1.405600e-04 1.683900e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.247400e-03 2.281100e-04 3.308900e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.673100e-03 2.222800e-04 2.188800e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.450300e-03 2.732900e-04 1.859700e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.162500e-03 1.765200e-04 1.659600e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.991400e-03 2.047300e-04 1.181500e-04
+1.750000e+02 1.500000e+01 1.500000e+01 2.111500e-03 1.062500e-04 1.279900e-04
+2.250000e+02 3.500000e+01 3.500000e+01 1.188400e-03 5.249100e-05 6.289000e-05
+3.775000e+02 1.175000e+02 1.175000e+02 2.516800e-04 1.395700e-05 1.453300e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.784200e-05 2.873500e-06 2.562100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d23-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d23-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t23
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.482800e-03 0.000000e+00 7.189300e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.102400e-03 2.311000e-04 4.403700e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.712400e-03 9.401500e-05 4.128700e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.438900e-03 2.221700e-04 6.095100e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.079300e-03 3.305300e-05 9.262400e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.988700e-03 1.729900e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 2.095100e-03 2.791900e-05 6.174700e-05
+2.250000e+02 3.500000e+01 3.500000e+01 1.214200e-03 1.386900e-04 0.000000e+00
+3.775000e+02 1.175000e+02 1.175000e+02 2.696700e-04 9.227000e-06 5.146700e-05
+6.975000e+02 2.025000e+02 2.025000e+02 2.057000e-05 1.321200e-06 2.035000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d24-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d24-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t24
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 7.792800e-02 1.833950e-02 2.044247e-02
+5.000000e-01 1.000000e-01 1.000000e-01 2.777000e-01 3.353918e-02 3.287087e-02
+6.500000e-01 5.000000e-02 5.000000e-02 5.535500e-01 1.147128e-01 1.149884e-01
+7.500000e-01 5.000000e-02 5.000000e-02 1.213500e+00 9.393261e-02 8.723704e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.941600e+00 1.238391e-01 1.213781e-01
+8.750000e-01 2.500000e-02 2.500000e-02 3.154000e+00 1.771312e-01 1.804688e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.147900e+00 1.903174e-01 1.964199e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.488100e+00 2.557388e-01 2.468413e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d24-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d24-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t24
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.481400e-01 7.422900e-03 1.018000e-02
+5.000000e-01 1.000000e-01 1.000000e-01 2.978800e-01 1.936400e-02 1.543200e-02
+6.500000e-01 5.000000e-02 5.000000e-02 6.244600e-01 3.123400e-02 4.417800e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.183200e+00 8.480900e-02 4.072400e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.941900e+00 1.156800e-01 8.972900e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.802800e+00 9.223500e-02 1.075400e-01
+9.250000e-01 2.500000e-02 2.500000e-02 3.972600e+00 1.421300e-01 1.463800e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.290700e+00 1.398500e-01 1.998700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d24-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d24-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t24
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.402500e-01 4.252400e-03 5.770500e-03
+5.000000e-01 1.000000e-01 1.000000e-01 2.961400e-01 2.774800e-02 0.000000e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.922800e-01 3.841900e-02 5.191000e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.102700e+00 1.762800e-02 2.989200e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.913100e+00 1.261300e-01 0.000000e+00
+8.750000e-01 2.500000e-02 2.500000e-02 2.759400e+00 0.000000e+00 7.099200e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.061100e+00 9.978600e-02 2.478700e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.569800e+00 3.652600e-03 2.650900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d25-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d25-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t25
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.027700e-01 9.284787e-03 9.227062e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.838100e-01 1.233425e-02 1.257055e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.438500e-01 1.876639e-02 1.754049e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.291500e-01 3.401404e-02 3.406569e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.785700e-01 2.200760e-02 2.200187e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.159900e-01 2.129066e-02 2.405541e-02
+5.400000e+00 2.000000e-01 2.000000e-01 2.788200e-01 1.544991e-02 1.579130e-02
+6.000000e+00 4.000000e-01 4.000000e-01 1.215900e-01 1.367189e-02 1.521664e-02
+7.600000e+00 1.200000e+00 1.200000e+00 6.214200e-03 2.677408e-03 2.737504e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d25-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d25-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t25
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.066400e-02 4.421900e-03 4.128500e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.714600e-01 7.679800e-03 5.540700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.656100e-01 1.087200e-02 1.152200e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.485400e-01 1.454300e-02 1.433000e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.994800e-01 1.183400e-02 2.470300e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.057100e-01 1.219700e-02 1.611700e-02
+5.400000e+00 2.000000e-01 2.000000e-01 2.951700e-01 1.185300e-02 1.213600e-02
+6.000000e+00 4.000000e-01 4.000000e-01 1.098900e-01 1.019300e-02 4.662600e-03
+7.600000e+00 1.200000e+00 1.200000e+00 6.909200e-03 6.352300e-04 1.011000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d25-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d25-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t25
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.076300e-01 3.993700e-03 8.913900e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.962200e-01 9.356800e-03 2.597900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.810500e-01 6.926700e-03 8.369800e-04
+4.200000e+00 2.000000e-01 2.000000e-01 3.349500e-01 4.193800e-04 2.094800e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.700100e-01 1.136200e-02 3.674700e-03
+5.000000e+00 2.000000e-01 2.000000e-01 3.729400e-01 6.101600e-03 3.562200e-02
+5.400000e+00 2.000000e-01 2.000000e-01 2.694300e-01 1.992400e-02 5.923400e-03
+6.000000e+00 4.000000e-01 4.000000e-01 1.083900e-01 3.305500e-03 1.056900e-03
+7.600000e+00 1.200000e+00 1.200000e+00 7.858400e-03 5.538000e-04 1.633700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d26-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d26-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t26
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 7.061400e-03 1.064172e-03 1.166735e-03
+1.050000e+02 1.000000e+01 1.000000e+01 6.470000e-03 3.293624e-04 3.673980e-04
+1.250000e+02 1.000000e+01 1.000000e+01 6.337500e-03 3.588134e-04 3.547634e-04
+1.475000e+02 1.250000e+01 1.250000e+01 5.433300e-03 3.102824e-04 2.928755e-04
+1.725000e+02 1.250000e+01 1.250000e+01 3.797800e-03 2.339298e-04 2.325058e-04
+1.975000e+02 1.250000e+01 1.250000e+01 2.992900e-03 2.077934e-04 2.042392e-04
+2.250000e+02 1.500000e+01 1.500000e+01 2.608500e-03 1.839223e-04 1.741546e-04
+2.575000e+02 1.750000e+01 1.750000e+01 1.702400e-03 3.165812e-04 3.128749e-04
+2.975000e+02 2.250000e+01 2.250000e+01 1.628000e-03 1.310364e-04 1.308917e-04
+3.525000e+02 3.250000e+01 3.250000e+01 9.601900e-04 8.899306e-05 8.566333e-05
+5.350000e+02 1.500000e+02 1.500000e+02 1.960700e-04 1.723922e-05 1.863530e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d26-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d26-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t26
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.578400e-03 5.966600e-04 3.197200e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.212200e-03 2.801000e-04 3.227200e-04
+1.250000e+02 1.000000e+01 1.000000e+01 5.955100e-03 2.508000e-04 4.340100e-04
+1.475000e+02 1.250000e+01 1.250000e+01 5.489000e-03 2.305000e-04 2.332200e-04
+1.725000e+02 1.250000e+01 1.250000e+01 4.288800e-03 1.579800e-04 1.869900e-04
+1.975000e+02 1.250000e+01 1.250000e+01 3.477000e-03 1.483100e-04 1.883500e-04
+2.250000e+02 1.500000e+01 1.500000e+01 2.772200e-03 1.528500e-04 1.139600e-04
+2.575000e+02 1.750000e+01 1.750000e+01 2.035600e-03 1.042500e-04 9.601300e-05
+2.975000e+02 2.250000e+01 2.250000e+01 1.496700e-03 7.260700e-05 7.050600e-05
+3.525000e+02 3.250000e+01 3.250000e+01 9.374200e-04 5.267400e-05 4.572600e-05
+5.350000e+02 1.500000e+02 1.500000e+02 1.963800e-04 1.181100e-05 1.111400e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d26-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d26-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t26
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.831200e-03 4.644500e-04 4.732400e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.519100e-03 1.282800e-04 7.878400e-04
+1.250000e+02 1.000000e+01 1.000000e+01 5.305900e-03 8.813600e-05 0.000000e+00
+1.475000e+02 1.250000e+01 1.250000e+01 5.052000e-03 2.434500e-04 0.000000e+00
+1.725000e+02 1.250000e+01 1.250000e+01 4.294600e-03 4.349200e-06 1.952300e-04
+1.975000e+02 1.250000e+01 1.250000e+01 3.480000e-03 5.434700e-05 1.523500e-04
+2.250000e+02 1.500000e+01 1.500000e+01 2.806800e-03 1.424300e-04 2.433900e-04
+2.575000e+02 1.750000e+01 1.750000e+01 2.143500e-03 5.080400e-05 8.905100e-05
+2.975000e+02 2.250000e+01 2.250000e+01 1.584100e-03 6.944500e-05 2.519100e-06
+3.525000e+02 3.250000e+01 3.250000e+01 1.094700e-03 4.639700e-05 0.000000e+00
+5.350000e+02 1.500000e+02 1.500000e+02 2.456800e-04 1.835600e-05 2.551400e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d27-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d27-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t27
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.257700e-03 1.623662e-04 1.653812e-04
+3.750000e+01 1.250000e+01 1.250000e+01 6.563800e-03 2.487683e-04 2.756686e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.973900e-03 2.053310e-04 2.372230e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.919800e-03 1.744184e-04 1.741189e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.670500e-03 1.955170e-04 1.381912e-04
+1.925000e+02 3.250000e+01 3.250000e+01 1.886200e-03 1.007903e-04 9.622518e-05
+2.425000e+02 1.750000e+01 1.750000e+01 8.675200e-04 1.233013e-04 1.234435e-04
+2.800000e+02 2.000000e+01 2.000000e+01 6.001300e-04 5.349723e-05 5.411056e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.514500e-04 2.874679e-05 2.858273e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.329700e-05 2.901476e-06 3.023483e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d27-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d27-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t27
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.755900e-03 1.017500e-04 7.707800e-05
+3.750000e+01 1.250000e+01 1.250000e+01 6.177100e-03 1.755200e-04 1.251900e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.487600e-03 1.485600e-04 1.361700e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.600100e-03 1.306300e-04 1.369300e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.926100e-03 8.067300e-05 6.140100e-05
+1.925000e+02 3.250000e+01 3.250000e+01 2.004200e-03 4.039700e-05 4.930600e-05
+2.425000e+02 1.750000e+01 1.750000e+01 1.050700e-03 4.280800e-05 4.607100e-05
+2.800000e+02 2.000000e+01 2.000000e+01 6.548500e-04 3.254000e-05 4.616100e-05
+3.975000e+02 9.750000e+01 9.750000e+01 2.038700e-04 9.460900e-06 7.438700e-06
+6.975000e+02 2.025000e+02 2.025000e+02 1.462000e-05 1.617800e-06 1.771000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d27-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d27-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t27
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.744500e-03 0.000000e+00 2.339700e-04
+3.750000e+01 1.250000e+01 1.250000e+01 6.356200e-03 1.458600e-04 2.980300e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.649100e-03 1.653000e-04 3.590900e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.556100e-03 4.738600e-05 1.476900e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.854600e-03 9.694100e-05 1.502500e-06
+1.925000e+02 3.250000e+01 3.250000e+01 1.953600e-03 6.338800e-05 4.010600e-05
+2.425000e+02 1.750000e+01 1.750000e+01 1.029700e-03 4.858100e-05 1.291200e-05
+2.800000e+02 2.000000e+01 2.000000e+01 6.563300e-04 2.005900e-05 7.254200e-06
+3.975000e+02 9.750000e+01 9.750000e+01 2.035700e-04 8.780400e-06 2.288400e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.754000e-05 1.256100e-06 9.459300e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d28-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d28-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t28
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 8.706500e-02 2.170353e-02 2.178045e-02
+3.750000e-01 1.250000e-01 1.250000e-01 1.265700e-01 4.358021e-02 2.914534e-02
+6.000000e-01 1.000000e-01 1.000000e-01 4.748600e-01 3.738424e-02 4.124443e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.011700e+00 7.569924e-02 7.551336e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.398700e+00 8.535977e-02 8.444028e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.036100e+00 9.061304e-02 8.999392e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.042100e+00 1.075387e-01 1.036678e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.212000e+00 1.340380e-01 1.617700e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.331700e+00 2.198388e-01 2.293161e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d28-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d28-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t28
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 1.243900e-01 5.131200e-03 1.539400e-02
+3.750000e-01 1.250000e-01 1.250000e-01 2.045100e-01 1.311900e-02 6.579400e-03
+6.000000e-01 1.000000e-01 1.000000e-01 5.148300e-01 1.374800e-02 1.912400e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.030800e+00 3.500500e-02 5.802000e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.446300e+00 8.176300e-02 3.934900e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.991200e+00 5.634400e-02 6.071800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.812400e+00 5.698900e-02 6.058900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.918900e+00 9.251200e-02 6.713300e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.096700e+00 1.557500e-01 8.200400e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d28-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d28-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t28
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 1.046400e-01 3.977000e-03 1.583100e-03
+3.750000e-01 1.250000e-01 1.250000e-01 1.648700e-01 3.159600e-05 7.198300e-03
+6.000000e-01 1.000000e-01 1.000000e-01 4.451500e-01 2.469100e-02 5.824100e-03
+7.250000e-01 2.500000e-02 2.500000e-02 9.015000e-01 1.333400e-02 1.073400e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.353000e+00 0.000000e+00 6.110200e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.031900e+00 1.544200e-01 0.000000e+00
+8.750000e-01 2.500000e-02 2.500000e-02 2.827800e+00 3.145600e-02 9.867400e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.134200e+00 1.714900e-02 8.474300e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.623500e+00 0.000000e+00 1.282500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d29-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d29-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t29
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.430700e-01 1.253435e-02 1.231821e-02
+2.600000e+00 2.000000e-01 2.000000e-01 1.790300e-01 1.345455e-02 1.506671e-02
+3.000000e+00 2.000000e-01 2.000000e-01 1.997600e-01 1.358385e-02 1.421876e-02
+3.400000e+00 2.000000e-01 2.000000e-01 2.630500e-01 1.357823e-02 1.792132e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.858900e-01 1.594253e-02 1.480967e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.386800e-01 1.754336e-02 1.759609e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.687900e-01 1.381005e-02 1.354887e-02
+5.000000e+00 2.000000e-01 2.000000e-01 3.283800e-01 1.920619e-02 2.248360e-02
+5.600000e+00 4.000000e-01 4.000000e-01 1.646500e-01 2.112049e-02 1.518484e-02
+7.400000e+00 1.400000e+00 1.400000e+00 9.151600e-03 2.320183e-03 2.192566e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d29-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d29-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t29
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.280800e-01 4.758900e-03 4.389700e-03
+2.600000e+00 2.000000e-01 2.000000e-01 1.568500e-01 4.937800e-03 4.781300e-03
+3.000000e+00 2.000000e-01 2.000000e-01 1.955100e-01 6.700000e-03 5.085700e-03
+3.400000e+00 2.000000e-01 2.000000e-01 2.413800e-01 5.695000e-03 9.029900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.949700e-01 8.067700e-03 6.334000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 3.452600e-01 6.758400e-03 1.114200e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.761700e-01 7.417700e-03 1.191400e-02
+5.000000e+00 2.000000e-01 2.000000e-01 3.576400e-01 1.030500e-02 8.193400e-03
+5.600000e+00 4.000000e-01 4.000000e-01 1.684000e-01 5.452200e-03 3.752600e-03
+7.400000e+00 1.400000e+00 1.400000e+00 9.619900e-03 9.155800e-04 4.311900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d29-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d29-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t29
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.568600e-01 1.511500e-02 6.459200e-04
+2.600000e+00 2.000000e-01 2.000000e-01 1.910300e-01 8.064500e-04 4.665200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 2.302600e-01 8.200800e-03 1.013200e-02
+3.400000e+00 2.000000e-01 2.000000e-01 2.696500e-01 0.000000e+00 4.731600e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.036400e-01 1.827400e-03 7.172600e-03
+4.200000e+00 2.000000e-01 2.000000e-01 3.307800e-01 6.617800e-03 2.997700e-03
+4.600000e+00 2.000000e-01 2.000000e-01 3.329300e-01 4.209300e-03 2.642500e-03
+5.000000e+00 2.000000e-01 2.000000e-01 3.061800e-01 4.385700e-03 1.351500e-02
+5.600000e+00 4.000000e-01 4.000000e-01 1.529600e-01 3.437700e-03 7.283700e-03
+7.400000e+00 1.400000e+00 1.400000e+00 1.039600e-02 1.316000e-03 8.042500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d30-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d30-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t30
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.704800e-03 5.786448e-04 5.807020e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.227000e-03 6.148538e-04 4.409379e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.355700e-03 2.211034e-04 2.218206e-04
+1.525000e+02 1.250000e+01 1.250000e+01 4.681600e-03 1.876372e-04 1.781726e-04
+1.775000e+02 1.250000e+01 1.250000e+01 3.751700e-03 1.616567e-04 1.639011e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.110000e-03 1.444692e-04 1.560933e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.619900e-03 1.296107e-04 1.426961e-04
+2.650000e+02 1.500000e+01 1.500000e+01 2.080900e-03 1.782366e-04 1.793572e-04
+2.975000e+02 1.750000e+01 1.750000e+01 1.918000e-03 1.083583e-04 1.236735e-04
+3.325000e+02 1.750000e+01 1.750000e+01 1.464200e-03 1.512991e-04 1.650513e-04
+3.700000e+02 2.000000e+01 2.000000e+01 1.158300e-03 7.593764e-05 8.961609e-05
+4.125000e+02 2.250000e+01 2.250000e+01 7.211700e-04 6.090580e-05 5.800696e-05
+4.575000e+02 2.250000e+01 2.250000e+01 4.317400e-04 4.128534e-05 3.979584e-05
+5.300000e+02 5.000000e+01 5.000000e+01 2.047400e-04 2.085416e-05 2.066163e-05
+7.300000e+02 1.500000e+02 1.500000e+02 2.924600e-05 5.181227e-06 5.514166e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d30-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d30-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t30
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.437700e-03 2.230800e-04 2.381700e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.225800e-03 2.767100e-04 1.200700e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.251900e-03 1.201000e-04 2.268100e-04
+1.525000e+02 1.250000e+01 1.250000e+01 4.670800e-03 1.036400e-04 1.991500e-04
+1.775000e+02 1.250000e+01 1.250000e+01 3.984900e-03 9.313200e-05 1.327500e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.343600e-03 9.703100e-05 7.760900e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.721100e-03 7.529100e-05 7.913600e-05
+2.650000e+02 1.500000e+01 1.500000e+01 2.209900e-03 8.930000e-05 6.330600e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.781400e-03 5.228200e-05 6.618200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 1.418800e-03 6.033800e-05 5.262400e-05
+3.700000e+02 2.000000e+01 2.000000e+01 1.045200e-03 4.326200e-05 4.865100e-05
+4.125000e+02 2.250000e+01 2.250000e+01 6.916200e-04 3.261800e-05 2.888700e-05
+4.575000e+02 2.250000e+01 2.250000e+01 4.236500e-04 2.255500e-05 2.370100e-05
+5.300000e+02 5.000000e+01 5.000000e+01 1.947200e-04 1.421700e-05 1.172900e-05
+7.300000e+02 1.500000e+02 1.500000e+02 3.171700e-05 2.949400e-06 2.716600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d30-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d30-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t30
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.211800e-03 3.042300e-04 3.552600e-04
+1.050000e+02 1.000000e+01 1.000000e+01 4.461900e-03 0.000000e+00 4.569800e-04
+1.275000e+02 1.250000e+01 1.250000e+01 4.473100e-03 1.056900e-04 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 4.290300e-03 1.220900e-04 0.000000e+00
+1.775000e+02 1.250000e+01 1.250000e+01 3.976900e-03 5.031500e-05 0.000000e+00
+2.050000e+02 1.500000e+01 1.500000e+01 3.256600e-03 0.000000e+00 1.321200e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.786900e-03 6.025400e-05 0.000000e+00
+2.650000e+02 1.500000e+01 1.500000e+01 2.357500e-03 0.000000e+00 8.507400e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.966600e-03 6.833900e-05 7.402300e-05
+3.325000e+02 1.750000e+01 1.750000e+01 1.672100e-03 4.136400e-05 1.510000e-05
+3.700000e+02 2.000000e+01 2.000000e+01 1.257900e-03 6.745200e-05 0.000000e+00
+4.125000e+02 2.250000e+01 2.250000e+01 8.565200e-04 1.101700e-04 2.713300e-06
+4.575000e+02 2.250000e+01 2.250000e+01 5.077800e-04 2.648200e-06 2.871000e-05
+5.300000e+02 5.000000e+01 5.000000e+01 2.504900e-04 1.100700e-05 2.467000e-05
+7.300000e+02 1.500000e+02 1.500000e+02 4.310800e-05 7.085000e-07 1.368100e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d31-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d31-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t31
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.789000e+00 7.290329e-02 7.287356e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.582600e+00 7.671012e-02 7.482703e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.500900e+00 7.179555e-02 7.216504e-02
+4.500000e-01 1.000000e-01 1.000000e-01 1.106300e+00 6.265183e-02 5.067478e-02
+6.000000e-01 5.000000e-02 5.000000e-02 7.775100e-01 4.661478e-02 4.753280e-02
+7.500000e-01 1.000000e-01 1.000000e-01 3.650300e-01 2.890584e-02 2.938186e-02
+1.025000e+00 1.750000e-01 1.750000e-01 1.114400e-01 9.694101e-03 9.780663e-03
+1.850000e+00 6.500000e-01 6.500000e-01 9.433400e-03 1.232201e-03 1.246403e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d31-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d31-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t31
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.613000e+00 4.421500e-02 2.545300e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.565600e+00 3.100800e-02 4.651200e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.584800e+00 3.716700e-02 5.156000e-02
+4.500000e-01 1.000000e-01 1.000000e-01 1.183700e+00 1.901300e-02 3.285300e-02
+6.000000e-01 5.000000e-02 5.000000e-02 7.755200e-01 2.356900e-02 3.262800e-02
+7.500000e-01 1.000000e-01 1.000000e-01 3.992400e-01 1.308700e-02 1.307100e-02
+1.025000e+00 1.750000e-01 1.750000e-01 1.105900e-01 6.835800e-03 4.705500e-03
+1.850000e+00 6.500000e-01 6.500000e-01 7.813600e-03 6.471200e-04 6.451700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d31-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d31-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t31
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.622400e+00 4.205100e-03 2.895500e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.558300e+00 0.000000e+00 2.982000e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.556800e+00 0.000000e+00 2.726000e-02
+4.500000e-01 1.000000e-01 1.000000e-01 1.158300e+00 1.185900e-02 0.000000e+00
+6.000000e-01 5.000000e-02 5.000000e-02 7.657600e-01 2.603800e-02 1.830100e-03
+7.500000e-01 1.000000e-01 1.000000e-01 4.100700e-01 1.227900e-02 2.983300e-03
+1.025000e+00 1.750000e-01 1.750000e-01 1.244700e-01 8.628700e-03 0.000000e+00
+1.850000e+00 6.500000e-01 6.500000e-01 8.707600e-03 7.867400e-04 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d32-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d32-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t32
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.237200e+00 7.213350e-02 7.015125e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.466400e+00 1.038116e-01 8.555071e-02
+3.250000e-01 7.500000e-02 7.500000e-02 1.649600e+00 4.762733e-02 4.750989e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.427300e+00 5.380471e-02 5.434899e-02
+6.750000e-01 1.250000e-01 1.250000e-01 6.488400e-01 2.961493e-02 3.110388e-02
+9.000000e-01 1.000000e-01 1.000000e-01 1.522100e-01 1.512202e-02 1.526235e-02
+1.750000e+00 7.500000e-01 7.500000e-01 9.076000e-03 1.246709e-03 1.355970e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d32-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d32-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t32
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.287400e+00 3.781000e-02 6.025500e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.477600e+00 5.827900e-02 4.128500e-02
+3.250000e-01 7.500000e-02 7.500000e-02 1.694100e+00 3.660300e-02 2.931100e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.396600e+00 2.933300e-02 3.526100e-02
+6.750000e-01 1.250000e-01 1.250000e-01 6.244600e-01 1.603100e-02 1.809900e-02
+9.000000e-01 1.000000e-01 1.000000e-01 1.460900e-01 1.024100e-02 8.134300e-03
+1.750000e+00 7.500000e-01 7.500000e-01 6.797500e-03 4.949300e-04 6.945100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d32-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d32-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t32
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.192800e+00 6.288400e-02 4.246400e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.397100e+00 7.380800e-02 2.195100e-02
+3.250000e-01 7.500000e-02 7.500000e-02 1.613800e+00 0.000000e+00 2.917300e-02
+4.750000e-01 7.500000e-02 7.500000e-02 1.441400e+00 1.179200e-02 5.354800e-02
+6.750000e-01 1.250000e-01 1.250000e-01 7.026000e-01 2.780900e-02 9.095100e-03
+9.000000e-01 1.000000e-01 1.000000e-01 1.771200e-01 1.216100e-02 7.301300e-03
+1.750000e+00 7.500000e-01 7.500000e-01 8.006300e-03 5.803800e-04 5.083400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d33-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d33-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t33
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.393500e-01 2.046922e-02 1.981563e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.923000e-01 1.044840e-02 9.031703e-03
+2.000000e+00 5.000000e-01 5.000000e-01 1.174800e-01 8.355426e-03 9.773928e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.733500e-02 5.198399e-03 5.468499e-03
+6.000000e+00 2.500000e+00 2.500000e+00 1.353500e-02 3.708086e-03 3.370465e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d33-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d33-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t33
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.474800e-01 1.055500e-02 1.394400e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.919700e-01 8.680100e-03 6.940400e-03
+2.000000e+00 5.000000e-01 5.000000e-01 1.117600e-01 4.303400e-03 3.381900e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.529200e-02 2.780700e-03 2.294700e-03
+6.000000e+00 2.500000e+00 2.500000e+00 1.349000e-02 1.089000e-03 1.037400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d33-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d33-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t33
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.228100e-01 2.099700e-02 1.563000e-02
+1.000000e+00 5.000000e-01 5.000000e-01 3.077200e-01 8.596300e-03 1.270600e-02
+2.000000e+00 5.000000e-01 5.000000e-01 1.213500e-01 7.037800e-03 6.302600e-03
+3.000000e+00 5.000000e-01 5.000000e-01 3.816700e-02 1.169500e-03 1.169800e-03
+6.000000e+00 2.500000e+00 2.500000e+00 9.951600e-03 0.000000e+00 1.158600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d34-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d34-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.737500e-03 1.666680e-04 1.850338e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.921900e-03 6.047142e-05 6.091175e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.124600e-03 2.855445e-05 2.857154e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.472600e-03 2.917853e-05 2.275483e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.000300e-03 2.430507e-05 2.304261e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.689200e-04 2.167312e-05 2.336882e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.484100e-04 1.673976e-05 1.533606e-05
+1.150000e+03 5.000000e+01 5.000000e+01 2.937000e-04 1.499780e-05 1.309657e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.893900e-04 1.337960e-05 1.066005e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.209200e-04 8.375443e-06 1.088039e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.968000e-05 3.780448e-06 4.312506e-06
+2.350000e+03 3.500000e+02 3.500000e+02 8.636700e-06 1.116252e-06 9.972329e-07
+3.350000e+03 6.500000e+02 6.500000e+02 8.821400e-07 2.022031e-07 1.899388e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d34-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d34-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.643700e-03 8.146100e-05 2.662300e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.853800e-03 1.940300e-05 2.587500e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.064700e-03 1.499400e-05 8.612500e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.456700e-03 2.873500e-05 1.187400e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.002000e-03 1.017100e-05 1.075200e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.842000e-04 8.243100e-06 1.212200e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.599900e-04 6.143000e-06 1.678700e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.178400e-04 6.939300e-06 1.238900e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.102500e-04 5.147200e-06 5.221800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.307600e-04 3.959200e-06 3.100100e-06
+1.750000e+03 2.500000e+02 2.500000e+02 5.488200e-05 1.225500e-06 1.150300e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.158000e-05 5.154300e-07 5.177500e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.213000e-06 9.985200e-08 1.359400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d34-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d34-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.618200e-03 6.847200e-05 6.017500e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.849700e-03 3.701800e-05 3.216100e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.052900e-03 1.594100e-05 1.315600e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.458200e-03 1.114000e-06 9.146000e-07
+8.325000e+02 4.750000e+01 4.750000e+01 1.010400e-03 6.761400e-06 7.484600e-06
+9.325000e+02 5.250000e+01 5.250000e+01 6.917300e-04 8.662100e-06 1.000900e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.584500e-04 8.445500e-06 9.649900e-06
+1.150000e+03 5.000000e+01 5.000000e+01 3.190100e-04 7.767700e-06 8.926800e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.119300e-04 6.337300e-06 7.338900e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.337400e-04 5.026900e-06 6.102400e-06
+1.750000e+03 2.500000e+02 2.500000e+02 5.519400e-05 2.702400e-06 3.198300e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.139900e-05 7.966200e-07 9.631000e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.200700e-06 1.172900e-07 1.468400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d34-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d34-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t34
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.419400e-03 2.626300e-05 5.177600e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.715500e-03 8.987800e-06 4.218100e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.999800e-03 0.000000e+00 2.834800e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.433200e-03 9.737800e-06 2.960100e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.041500e-03 5.033900e-05 0.000000e+00
+9.325000e+02 5.250000e+01 5.250000e+01 7.136400e-04 2.509100e-07 5.515000e-06
+1.042500e+03 5.750000e+01 5.750000e+01 4.869900e-04 2.471000e-06 7.331000e-06
+1.150000e+03 5.000000e+01 5.000000e+01 3.432200e-04 4.655800e-06 4.298100e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.380700e-04 6.638500e-06 8.833200e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.504600e-04 7.648400e-06 2.034700e-06
+1.750000e+03 2.500000e+02 2.500000e+02 6.552800e-05 2.774300e-06 1.296900e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.399400e-05 5.862100e-07 9.503400e-07
+3.350000e+03 6.500000e+02 6.500000e+02 1.561600e-06 1.630900e-07 4.800100e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d35-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d35-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.933500e-03 1.324270e-04 1.319493e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.076500e-03 2.131621e-04 2.487014e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.869700e-03 1.732412e-04 1.825174e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.002900e-03 8.404852e-05 8.337837e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.080100e-03 1.263419e-04 1.181810e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.865600e-03 1.729448e-04 1.439489e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.838500e-03 1.101198e-04 1.039252e-04
+2.075000e+02 1.750000e+01 1.750000e+01 1.080300e-03 5.540438e-05 5.189075e-05
+2.425000e+02 1.750000e+01 1.750000e+01 6.179600e-04 2.886477e-05 3.012354e-05
+2.800000e+02 2.000000e+01 2.000000e+01 3.684100e-04 2.177920e-05 2.205978e-05
+3.975000e+02 9.750000e+01 9.750000e+01 7.096900e-05 9.637562e-06 9.983116e-06
+6.975000e+02 2.025000e+02 2.025000e+02 3.443500e-06 7.049974e-07 7.278381e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d35-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d35-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.378700e-03 1.517600e-04 2.223800e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.469400e-03 5.101500e-05 9.025600e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.440900e-03 8.244400e-05 5.268400e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.978500e-03 5.811300e-05 5.480200e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.359900e-03 4.094500e-05 5.730000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.055200e-03 4.307600e-05 3.026300e-05
+1.750000e+02 1.500000e+01 1.500000e+01 2.039900e-03 2.614000e-05 3.703500e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.260800e-03 2.183900e-05 1.994800e-05
+2.425000e+02 1.750000e+01 1.750000e+01 7.283000e-04 1.380700e-05 2.572100e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.181900e-04 1.488400e-05 1.552900e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.091700e-04 3.234800e-06 3.558500e-06
+6.975000e+02 2.025000e+02 2.025000e+02 5.000600e-06 5.161700e-07 3.977300e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d35-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d35-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.571100e-03 1.697800e-04 1.550400e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.492700e-03 1.936100e-04 1.751200e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.208200e-03 3.438500e-05 2.906200e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.853800e-03 4.013100e-05 4.118000e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.251100e-03 5.415300e-05 6.164000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.028000e-03 6.964700e-05 8.156600e-05
+1.750000e+02 1.500000e+01 1.500000e+01 2.051300e-03 4.503300e-05 5.197900e-05
+2.075000e+02 1.750000e+01 1.750000e+01 1.272000e-03 2.845900e-05 3.138100e-05
+2.425000e+02 1.750000e+01 1.750000e+01 7.714900e-04 1.860300e-05 1.992900e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.548600e-04 1.108800e-05 1.158100e-05
+3.975000e+02 9.750000e+01 9.750000e+01 1.260500e-04 3.504100e-06 3.557000e-06
+6.975000e+02 2.025000e+02 2.025000e+02 6.537500e-06 2.475100e-07 2.579500e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d35-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d35-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t35
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.356900e-03 5.197500e-05 2.060400e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.602500e-03 1.209700e-04 6.166400e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.512700e-03 1.501000e-04 5.842200e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.991900e-03 0.000000e+00 1.600700e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.327700e-03 1.226200e-05 8.728600e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.046000e-03 1.050400e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 1.995200e-03 2.327300e-05 1.004600e-04
+2.075000e+02 1.750000e+01 1.750000e+01 1.202900e-03 4.973400e-05 0.000000e+00
+2.425000e+02 1.750000e+01 1.750000e+01 7.151500e-04 8.055100e-06 1.557800e-05
+2.800000e+02 2.000000e+01 2.000000e+01 4.119800e-04 1.447900e-05 2.620800e-06
+3.975000e+02 9.750000e+01 9.750000e+01 1.087000e-04 5.432200e-06 3.744600e-06
+6.975000e+02 2.025000e+02 2.025000e+02 6.240200e-06 5.432900e-07 6.584400e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d36-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d36-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 8.122500e-02 1.352140e-02 1.326180e-02
+2.250000e-01 7.500000e-02 7.500000e-02 1.143700e-01 1.663477e-02 1.142533e-02
+3.500000e-01 5.000000e-02 5.000000e-02 1.271500e-01 1.512681e-02 1.596400e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.161500e-01 1.867401e-02 1.905356e-02
+5.500000e-01 5.000000e-02 5.000000e-02 3.501200e-01 2.792869e-02 2.667234e-02
+6.250000e-01 2.500000e-02 2.500000e-02 5.917600e-01 4.321160e-02 3.926561e-02
+6.750000e-01 2.500000e-02 2.500000e-02 7.344900e-01 4.441159e-02 4.303239e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.009500e+00 6.632819e-02 6.590522e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.519000e+00 3.722584e-02 3.723416e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.206900e+00 3.835284e-02 3.784168e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.029600e+00 5.015113e-02 5.043382e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.928900e+00 7.383253e-02 7.527868e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.006300e+00 9.790021e-02 1.114479e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d36-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d36-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.202300e-01 6.211600e-03 3.741400e-03
+2.250000e-01 7.500000e-02 7.500000e-02 1.409700e-01 3.038600e-03 4.526800e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.901900e-01 4.926700e-03 5.335500e-03
+4.500000e-01 5.000000e-02 5.000000e-02 2.664800e-01 5.314100e-03 8.613400e-03
+5.500000e-01 5.000000e-02 5.000000e-02 4.124900e-01 6.902700e-03 8.398800e-03
+6.250000e-01 2.500000e-02 2.500000e-02 6.083600e-01 1.381700e-02 1.152200e-02
+6.750000e-01 2.500000e-02 2.500000e-02 8.041500e-01 1.701300e-02 1.363700e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.107700e+00 2.066300e-02 1.472900e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.518200e+00 2.071200e-02 1.947000e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.090800e+00 2.068100e-02 2.676800e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.869400e+00 2.542300e-02 3.118400e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.800300e+00 3.654600e-02 4.110300e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.679200e+00 7.771600e-02 6.736700e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d36-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d36-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.176200e-01 3.778900e-03 4.656300e-03
+2.250000e-01 7.500000e-02 7.500000e-02 1.375700e-01 4.262000e-03 5.147900e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.808400e-01 6.312800e-03 8.116400e-03
+4.500000e-01 5.000000e-02 5.000000e-02 2.441600e-01 6.809900e-03 8.501300e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.905200e-01 1.402100e-02 1.647000e-02
+6.250000e-01 2.500000e-02 2.500000e-02 5.466100e-01 1.315500e-02 1.498300e-02
+6.750000e-01 2.500000e-02 2.500000e-02 7.337600e-01 1.618400e-02 1.883900e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.016900e+00 2.104600e-02 2.477700e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.422900e+00 2.068500e-02 2.250500e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.009400e+00 1.773700e-02 1.814300e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.840200e+00 4.614300e-03 4.046000e-03
+9.250000e-01 2.500000e-02 2.500000e-02 3.950600e+00 5.492300e-02 4.720000e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.083000e+00 1.370900e-01 1.194200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d36-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d36-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t36
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.046500e-01 3.535600e-03 8.375800e-04
+2.250000e-01 7.500000e-02 7.500000e-02 1.217600e-01 2.058000e-03 9.735300e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.587500e-01 4.002300e-03 1.130700e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.222200e-01 5.742900e-04 4.499800e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.518000e-01 1.010000e-02 0.000000e+00
+6.250000e-01 2.500000e-02 2.500000e-02 5.401200e-01 3.005400e-02 2.790100e-03
+6.750000e-01 2.500000e-02 2.500000e-02 7.204000e-01 7.377300e-03 3.319600e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.026600e+00 1.074000e-02 5.218800e-03
+7.750000e-01 2.500000e-02 2.500000e-02 1.454700e+00 3.734400e-03 3.749400e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.097200e+00 2.579900e-02 5.751100e-03
+8.750000e-01 2.500000e-02 2.500000e-02 2.942800e+00 2.987300e-02 2.919000e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.039700e+00 5.567300e-02 0.000000e+00
+9.750000e-01 2.500000e-02 2.500000e-02 5.033700e+00 1.585000e-02 8.495600e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d37-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d37-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.985700e-01 1.264129e-02 1.152023e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.687100e-01 1.111696e-02 1.148468e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.271100e-01 8.868828e-03 1.018768e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.621200e-01 6.921333e-03 7.511135e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.161900e-01 8.640365e-03 8.613727e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.586500e-01 9.151680e-03 8.764364e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.411400e-01 6.786680e-03 7.270510e-03
+5.000000e+00 2.000000e-01 2.000000e-01 6.789800e-02 5.659691e-03 5.623306e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.495100e-02 4.305751e-03 3.045384e-03
+6.200000e+00 2.000000e-01 2.000000e-01 7.071900e-03 1.694080e-03 1.603269e-03
+7.600000e+00 1.200000e+00 1.200000e+00 4.397200e-04 1.957244e-04 1.706019e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d37-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d37-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.926100e-01 3.939500e-03 6.037100e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.558500e-01 3.746400e-03 5.975100e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.221100e-01 6.806300e-03 9.456900e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.601500e-01 3.170700e-03 3.596300e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.175800e-01 3.367500e-03 3.143000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.593300e-01 6.356700e-03 4.381600e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.482900e-01 4.272500e-03 2.168500e-03
+5.000000e+00 2.000000e-01 2.000000e-01 7.739500e-02 1.447900e-03 3.490300e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.780200e-02 8.388300e-04 6.688100e-04
+6.200000e+00 2.000000e-01 2.000000e-01 7.506600e-03 1.106900e-03 4.043100e-04
+7.600000e+00 1.200000e+00 1.200000e+00 5.968300e-04 4.654200e-05 8.824600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d37-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d37-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.591600e-01 3.434700e-03 2.984200e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.005800e-01 2.739500e-03 2.366900e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.335600e-01 2.705100e-03 2.007400e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.421000e-01 1.271900e-03 1.053900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 3.767300e-01 1.434400e-03 1.638400e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.322300e-01 2.152600e-03 2.474100e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.283400e-01 2.583100e-03 3.185700e-03
+5.000000e+00 2.000000e-01 2.000000e-01 6.750400e-02 2.119900e-03 2.513800e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.488900e-02 1.221100e-03 1.629100e-03
+6.200000e+00 2.000000e-01 2.000000e-01 6.623800e-03 5.518200e-04 8.267500e-04
+7.600000e+00 1.200000e+00 1.200000e+00 5.661000e-04 6.045300e-05 9.118600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d37-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d37-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t37
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.276100e-01 5.166600e-03 7.224900e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.853200e-01 0.000000e+00 8.155000e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.378500e-01 1.011300e-02 0.000000e+00
+3.400000e+00 2.000000e-01 2.000000e-01 4.483700e-01 3.856600e-03 2.567700e-04
+3.800000e+00 2.000000e-01 2.000000e-01 3.869000e-01 9.072800e-04 6.262900e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.362700e-01 9.595100e-04 2.763900e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.349000e-01 2.209400e-03 0.000000e+00
+5.000000e+00 2.000000e-01 2.000000e-01 7.258000e-02 3.110800e-03 4.607600e-03
+5.600000e+00 4.000000e-01 4.000000e-01 2.837600e-02 1.051000e-03 1.942900e-03
+6.200000e+00 2.000000e-01 2.000000e-01 8.507000e-03 1.396200e-03 6.039000e-05
+7.600000e+00 1.200000e+00 1.200000e+00 8.237200e-04 9.201200e-05 2.161600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d38-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d38-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.869000e-03 3.948115e-04 4.033031e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.557400e-03 2.631596e-04 2.844878e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.069300e-03 1.052295e-04 1.168430e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.146000e-03 1.066799e-04 9.007251e-05
+1.775000e+02 1.250000e+01 1.250000e+01 4.959700e-03 1.182551e-04 1.165410e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.550100e-03 1.126133e-04 1.104288e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.255600e-03 8.168077e-05 7.972379e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.423200e-03 7.170626e-05 6.679290e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.590200e-04 4.767594e-05 4.877268e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.796400e-04 3.442721e-05 3.512253e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.896300e-04 2.504993e-05 2.569215e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.568600e-04 1.225020e-05 1.136216e-05
+4.575000e+02 2.250000e+01 2.250000e+01 9.204500e-05 7.699796e-06 7.206928e-06
+5.300000e+02 5.000000e+01 5.000000e+01 3.546500e-05 3.495101e-06 3.369250e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.072900e-05 2.004789e-06 1.968167e-06
+8.425000e+02 1.575000e+02 1.575000e+02 8.339400e-07 4.776545e-07 4.762887e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d38-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d38-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.436400e-03 2.621100e-04 1.198200e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.304600e-03 1.894900e-04 6.331200e-05
+1.275000e+02 1.250000e+01 1.250000e+01 7.010200e-03 5.837400e-05 2.559000e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.155500e-03 4.948800e-05 6.622200e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.032400e-03 4.417300e-05 6.964200e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.612600e-03 5.412500e-05 4.575400e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.326400e-03 3.693700e-05 4.843900e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.466300e-03 3.766600e-05 3.160500e-05
+2.975000e+02 1.750000e+01 1.750000e+01 8.918200e-04 1.844800e-05 2.695900e-05
+3.325000e+02 1.750000e+01 1.750000e+01 5.312500e-04 2.358500e-05 1.471100e-05
+3.700000e+02 2.000000e+01 2.000000e+01 3.085300e-04 1.075600e-05 1.423400e-05
+4.125000e+02 2.250000e+01 2.250000e+01 1.734100e-04 6.608300e-06 7.148200e-06
+4.575000e+02 2.250000e+01 2.250000e+01 9.624800e-05 4.621200e-06 5.063100e-06
+5.300000e+02 5.000000e+01 5.000000e+01 4.070400e-05 3.289000e-06 2.511600e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.222500e-05 1.220900e-06 1.126500e-06
+8.425000e+02 1.575000e+02 1.575000e+02 1.957400e-06 3.419400e-07 2.825700e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d38-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d38-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.347700e-03 5.593500e-06 2.125700e-05
+1.050000e+02 1.000000e+01 1.000000e+01 6.296100e-03 3.499600e-05 4.331400e-05
+1.275000e+02 1.250000e+01 1.250000e+01 6.534200e-03 1.621500e-05 1.453300e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.079400e-03 3.335400e-05 2.739200e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.346200e-03 2.403300e-05 2.013900e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.902300e-03 9.939600e-06 9.665200e-06
+2.350000e+02 1.500000e+01 1.500000e+01 2.621200e-03 1.150100e-05 8.529200e-06
+2.650000e+02 1.500000e+01 1.500000e+01 1.716000e-03 1.480300e-05 1.257200e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.045300e-03 1.269800e-05 1.169700e-05
+3.325000e+02 1.750000e+01 1.750000e+01 6.395200e-04 1.039300e-05 9.935800e-06
+3.700000e+02 2.000000e+01 2.000000e+01 3.847600e-04 7.477900e-06 7.646200e-06
+4.125000e+02 2.250000e+01 2.250000e+01 2.229400e-04 5.319300e-06 5.796600e-06
+4.575000e+02 2.250000e+01 2.250000e+01 1.229800e-04 3.147500e-06 3.560300e-06
+5.300000e+02 5.000000e+01 5.000000e+01 5.323500e-05 1.671100e-06 1.865300e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.583700e-05 6.502500e-07 7.454400e-07
+8.425000e+02 1.575000e+02 1.575000e+02 2.440700e-06 1.241700e-07 1.433200e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d38-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d38-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t38
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.467600e-03 9.445400e-05 2.360600e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.452300e-03 9.176200e-05 1.273600e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.593500e-03 7.974300e-05 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 6.153400e-03 0.000000e+00 2.644500e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.249700e-03 1.252900e-04 1.048800e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.835600e-03 0.000000e+00 1.197900e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.573000e-03 3.335500e-05 0.000000e+00
+2.650000e+02 1.500000e+01 1.500000e+01 1.645000e-03 2.502300e-05 2.169700e-05
+2.975000e+02 1.750000e+01 1.750000e+01 1.016200e-03 6.174200e-06 3.150200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 6.441000e-04 2.990300e-05 0.000000e+00
+3.700000e+02 2.000000e+01 2.000000e+01 3.818400e-04 1.317600e-05 2.005300e-06
+4.125000e+02 2.250000e+01 2.250000e+01 2.231300e-04 1.822100e-05 5.658900e-06
+4.575000e+02 2.250000e+01 2.250000e+01 1.248600e-04 3.624900e-06 7.957200e-07
+5.300000e+02 5.000000e+01 5.000000e+01 5.546100e-05 1.851500e-06 4.965600e-06
+6.325000e+02 5.250000e+01 5.250000e+01 1.801100e-05 0.000000e+00 2.178800e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.965100e-06 3.640400e-07 2.030200e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d39-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d39-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.364800e+00 4.846605e-02 4.635862e-02
+1.000000e-01 5.000000e-02 5.000000e-02 1.438400e+00 4.449730e-02 3.998126e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.374900e+00 4.223074e-02 3.748985e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.382400e+00 3.299463e-02 3.453453e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.179700e+00 3.464802e-02 3.301143e-02
+5.000000e-01 5.000000e-02 5.000000e-02 9.105100e-01 2.360182e-02 2.415564e-02
+6.000000e-01 5.000000e-02 5.000000e-02 8.281800e-01 2.391483e-02 2.558667e-02
+7.000000e-01 5.000000e-02 5.000000e-02 6.688400e-01 1.935545e-02 1.916168e-02
+8.000000e-01 5.000000e-02 5.000000e-02 4.460100e-01 1.780996e-02 1.922288e-02
+9.250000e-01 7.500000e-02 7.500000e-02 2.734100e-01 1.195067e-02 1.259264e-02
+1.100000e+00 1.000000e-01 1.000000e-01 1.806200e-01 1.542226e-02 1.597271e-02
+1.350000e+00 1.500000e-01 1.500000e-01 7.597300e-02 4.640969e-03 5.404275e-03
+1.650000e+00 1.500000e-01 1.500000e-01 2.107300e-02 2.790816e-03 2.953377e-03
+2.050000e+00 2.500000e-01 2.500000e-01 4.614500e-03 8.474705e-04 8.540180e-04
+2.650000e+00 3.500000e-01 3.500000e-01 4.433600e-04 1.912842e-04 1.796024e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d39-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d39-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.340000e+00 1.768700e-02 2.039800e-02
+1.000000e-01 5.000000e-02 5.000000e-02 1.348800e+00 1.951700e-02 1.607900e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.373300e+00 1.300200e-02 1.758900e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.418700e+00 2.053200e-02 1.947300e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.240500e+00 1.258900e-02 1.170700e-02
+5.000000e-01 5.000000e-02 5.000000e-02 9.534900e-01 1.867300e-02 1.011800e-02
+6.000000e-01 5.000000e-02 5.000000e-02 8.350400e-01 2.020900e-02 9.484200e-03
+7.000000e-01 5.000000e-02 5.000000e-02 6.629900e-01 8.855300e-03 1.124500e-02
+8.000000e-01 5.000000e-02 5.000000e-02 4.486800e-01 7.802100e-03 6.648800e-02
+9.250000e-01 7.500000e-02 7.500000e-02 2.894800e-01 4.710700e-03 5.610800e-03
+1.100000e+00 1.000000e-01 1.000000e-01 1.616600e-01 5.108400e-03 2.928100e-03
+1.350000e+00 1.500000e-01 1.500000e-01 6.796800e-02 1.961300e-03 1.556300e-03
+1.650000e+00 1.500000e-01 1.500000e-01 2.154800e-02 9.118300e-04 9.585000e-04
+2.050000e+00 2.500000e-01 2.500000e-01 4.198600e-03 3.015200e-04 3.839000e-04
+2.650000e+00 3.500000e-01 3.500000e-01 2.037400e-04 5.669200e-05 5.861100e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d39-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d39-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.246500e+00 1.943300e-02 1.690500e-02
+1.000000e-01 5.000000e-02 5.000000e-02 1.252000e+00 2.007000e-02 1.785800e-02
+2.000000e-01 5.000000e-02 5.000000e-02 1.230100e+00 1.813900e-02 1.648500e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.257100e+00 1.764700e-02 1.598900e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.131600e+00 8.899400e-03 8.380200e-03
+5.000000e-01 5.000000e-02 5.000000e-02 9.962500e-01 7.983600e-03 9.595800e-03
+6.000000e-01 5.000000e-02 5.000000e-02 9.622300e-01 1.188700e-02 1.390700e-02
+7.000000e-01 5.000000e-02 5.000000e-02 7.572900e-01 1.006100e-02 1.134000e-02
+8.000000e-01 5.000000e-02 5.000000e-02 5.062100e-01 7.437400e-03 8.474900e-03
+9.250000e-01 7.500000e-02 7.500000e-02 3.514300e-01 8.886100e-03 9.969800e-03
+1.100000e+00 1.000000e-01 1.000000e-01 1.900700e-01 4.264200e-03 4.795900e-03
+1.350000e+00 1.500000e-01 1.500000e-01 8.502200e-02 1.929800e-03 2.018600e-03
+1.650000e+00 1.500000e-01 1.500000e-01 3.127600e-02 1.071000e-03 1.210700e-03
+2.050000e+00 2.500000e-01 2.500000e-01 5.223100e-03 2.560700e-04 2.875000e-04
+2.650000e+00 3.500000e-01 3.500000e-01 2.384800e-04 1.462000e-05 1.728000e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d39-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d39-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t39
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.403400e+00 3.298400e-02 0.000000e+00
+1.000000e-01 5.000000e-02 5.000000e-02 1.405200e+00 9.437700e-03 6.334600e-03
+2.000000e-01 5.000000e-02 5.000000e-02 1.413300e+00 1.851100e-02 2.031100e-02
+3.000000e-01 5.000000e-02 5.000000e-02 1.442900e+00 9.529100e-03 2.912800e-02
+4.000000e-01 5.000000e-02 5.000000e-02 1.225900e+00 1.891800e-02 2.859000e-03
+5.000000e-01 5.000000e-02 5.000000e-02 9.026700e-01 2.250600e-03 1.659600e-02
+6.000000e-01 5.000000e-02 5.000000e-02 7.963500e-01 1.087700e-02 1.878700e-02
+7.000000e-01 5.000000e-02 5.000000e-02 6.531900e-01 8.783100e-03 3.790500e-04
+8.000000e-01 5.000000e-02 5.000000e-02 4.262500e-01 0.000000e+00 1.540600e-02
+9.250000e-01 7.500000e-02 7.500000e-02 2.827300e-01 4.356200e-03 1.214400e-02
+1.100000e+00 1.000000e-01 1.000000e-01 1.580600e-01 3.746200e-03 1.291600e-03
+1.350000e+00 1.500000e-01 1.500000e-01 6.800000e-02 5.665800e-04 5.926800e-04
+1.650000e+00 1.500000e-01 1.500000e-01 2.147300e-02 7.799200e-04 4.937200e-04
+2.050000e+00 2.500000e-01 2.500000e-01 4.536500e-03 2.556900e-04 1.983600e-04
+2.650000e+00 3.500000e-01 3.500000e-01 1.892200e-04 6.747600e-05 6.935500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d40-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d40-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.092100e+00 3.106798e-02 3.155427e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.018500e+00 3.261042e-02 3.275854e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.162800e+00 2.888218e-02 2.932710e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.222600e+00 3.679887e-02 3.686037e-02
+2.250000e-01 2.500000e-02 2.500000e-02 1.265700e+00 4.198133e-02 3.813616e-02
+2.750000e-01 2.500000e-02 2.500000e-02 1.328900e+00 3.557280e-02 3.561967e-02
+3.250000e-01 2.500000e-02 2.500000e-02 1.357500e+00 3.641542e-02 3.624554e-02
+3.750000e-01 2.500000e-02 2.500000e-02 1.438400e+00 3.448402e-02 3.442345e-02
+4.250000e-01 2.500000e-02 2.500000e-02 1.314600e+00 3.158142e-02 3.158311e-02
+4.750000e-01 2.500000e-02 2.500000e-02 1.183600e+00 7.406805e-02 7.448768e-02
+5.250000e-01 2.500000e-02 2.500000e-02 1.161100e+00 3.762767e-02 3.800440e-02
+5.750000e-01 2.500000e-02 2.500000e-02 1.146800e+00 2.485644e-02 2.489803e-02
+6.250000e-01 2.500000e-02 2.500000e-02 1.010200e+00 3.103958e-02 3.050361e-02
+6.750000e-01 2.500000e-02 2.500000e-02 8.781000e-01 2.837291e-02 2.830434e-02
+7.250000e-01 2.500000e-02 2.500000e-02 7.318400e-01 2.162921e-02 2.185104e-02
+7.750000e-01 2.500000e-02 2.500000e-02 5.806800e-01 1.976100e-02 1.904239e-02
+8.250000e-01 2.500000e-02 2.500000e-02 4.710600e-01 1.722081e-02 1.747534e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.768200e-01 1.571927e-02 1.620136e-02
+9.250000e-01 2.500000e-02 2.500000e-02 2.961800e-01 1.371480e-02 1.385615e-02
+9.750000e-01 2.500000e-02 2.500000e-02 2.365800e-01 1.112368e-02 1.115901e-02
+1.025000e+00 2.500000e-02 2.500000e-02 1.879500e-01 1.031368e-02 1.003133e-02
+1.075000e+00 2.500000e-02 2.500000e-02 1.347400e-01 9.133185e-03 9.721705e-03
+1.125000e+00 2.500000e-02 2.500000e-02 1.007700e-01 7.617282e-03 7.873269e-03
+1.175000e+00 2.500000e-02 2.500000e-02 8.877400e-02 6.686759e-03 6.552150e-03
+1.250000e+00 5.000000e-02 5.000000e-02 5.083300e-02 3.534430e-03 3.516280e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.948700e-02 3.063042e-03 3.052132e-03
+1.500000e+00 1.000000e-01 1.000000e-01 1.072400e-02 1.203017e-03 1.201783e-03
+1.800000e+00 2.000000e-01 2.000000e-01 1.276900e-03 2.783425e-04 2.824434e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d40-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d40-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.058900e+00 2.440100e-02 2.870700e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.075000e+00 1.942100e-02 2.793500e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.117900e+00 1.888400e-02 3.722800e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.179800e+00 2.483900e-02 2.786300e-02
+2.250000e-01 2.500000e-02 2.500000e-02 1.265200e+00 3.155300e-02 1.714800e-02
+2.750000e-01 2.500000e-02 2.500000e-02 1.320200e+00 1.923900e-02 2.519200e-02
+3.250000e-01 2.500000e-02 2.500000e-02 1.412000e+00 5.713100e-02 1.568400e-02
+3.750000e-01 2.500000e-02 2.500000e-02 1.425600e+00 1.796800e-02 2.732000e-02
+4.250000e-01 2.500000e-02 2.500000e-02 1.363600e+00 2.205900e-02 1.904700e-02
+4.750000e-01 2.500000e-02 2.500000e-02 1.259300e+00 1.483900e-02 2.001100e-02
+5.250000e-01 2.500000e-02 2.500000e-02 1.189600e+00 1.625400e-02 1.656800e-02
+5.750000e-01 2.500000e-02 2.500000e-02 1.094900e+00 3.942300e-02 1.719900e-02
+6.250000e-01 2.500000e-02 2.500000e-02 1.008100e+00 1.360500e-02 1.420700e-01
+6.750000e-01 2.500000e-02 2.500000e-02 8.684100e-01 1.375800e-02 1.759400e-02
+7.250000e-01 2.500000e-02 2.500000e-02 7.206400e-01 1.408000e-02 1.219100e-02
+7.750000e-01 2.500000e-02 2.500000e-02 5.902600e-01 1.658200e-02 2.223300e-02
+8.250000e-01 2.500000e-02 2.500000e-02 4.710300e-01 9.983400e-03 1.482600e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.751400e-01 1.622500e-02 8.091700e-03
+9.250000e-01 2.500000e-02 2.500000e-02 2.900400e-01 1.133200e-02 9.283800e-03
+9.750000e-01 2.500000e-02 2.500000e-02 2.269700e-01 7.585900e-03 6.801000e-03
+1.025000e+00 2.500000e-02 2.500000e-02 1.741400e-01 7.122100e-03 5.601200e-03
+1.075000e+00 2.500000e-02 2.500000e-02 1.318600e-01 5.705100e-03 6.368000e-03
+1.125000e+00 2.500000e-02 2.500000e-02 9.990000e-02 4.566900e-03 5.090200e-03
+1.175000e+00 2.500000e-02 2.500000e-02 7.347300e-02 4.096900e-03 3.696500e-03
+1.250000e+00 5.000000e-02 5.000000e-02 4.924000e-02 2.277600e-03 2.281000e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.680000e-02 1.847100e-03 1.842600e-03
+1.500000e+00 1.000000e-01 1.000000e-01 1.073400e-02 7.668700e-04 9.794000e-04
+1.800000e+00 2.000000e-01 2.000000e-01 1.628600e-03 1.924300e-04 2.586500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d40-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d40-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.195900e+00 1.283400e-02 1.502300e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.201500e+00 1.065700e-02 1.185500e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.228500e+00 8.872800e-03 1.021600e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.275600e+00 6.065100e-03 6.637200e-03
+2.250000e-01 2.500000e-02 2.500000e-02 1.316900e+00 3.881300e-03 3.238400e-03
+2.750000e-01 2.500000e-02 2.500000e-02 1.352300e+00 2.811600e-03 3.149800e-03
+3.250000e-01 2.500000e-02 2.500000e-02 1.389300e+00 7.209400e-03 6.543600e-03
+3.750000e-01 2.500000e-02 2.500000e-02 1.372700e+00 7.557100e-03 7.226700e-03
+4.250000e-01 2.500000e-02 2.500000e-02 1.330400e+00 4.454500e-03 4.945200e-03
+4.750000e-01 2.500000e-02 2.500000e-02 1.222800e+00 7.781300e-03 6.579500e-03
+5.250000e-01 2.500000e-02 2.500000e-02 1.147500e+00 1.642500e-03 2.115600e-03
+5.750000e-01 2.500000e-02 2.500000e-02 1.035900e+00 5.270800e-03 5.003000e-03
+6.250000e-01 2.500000e-02 2.500000e-02 9.380800e-01 4.431300e-03 3.492500e-03
+6.750000e-01 2.500000e-02 2.500000e-02 8.012500e-01 4.041800e-03 3.306700e-03
+7.250000e-01 2.500000e-02 2.500000e-02 6.717300e-01 4.005300e-03 3.314500e-03
+7.750000e-01 2.500000e-02 2.500000e-02 5.560900e-01 1.436500e-03 1.014300e-03
+8.250000e-01 2.500000e-02 2.500000e-02 4.421000e-01 1.241600e-03 1.476800e-03
+8.750000e-01 2.500000e-02 2.500000e-02 3.563200e-01 1.775000e-03 1.817900e-03
+9.250000e-01 2.500000e-02 2.500000e-02 2.712100e-01 1.717300e-03 1.676500e-03
+9.750000e-01 2.500000e-02 2.500000e-02 2.147400e-01 1.241200e-03 1.471300e-03
+1.025000e+00 2.500000e-02 2.500000e-02 1.687000e-01 9.556200e-04 1.066900e-03
+1.075000e+00 2.500000e-02 2.500000e-02 1.313200e-01 9.833600e-04 1.150200e-03
+1.125000e+00 2.500000e-02 2.500000e-02 9.624500e-02 1.248900e-03 1.222400e-03
+1.175000e+00 2.500000e-02 2.500000e-02 7.322800e-02 1.067000e-03 1.110700e-03
+1.250000e+00 5.000000e-02 5.000000e-02 5.152800e-02 1.965200e-03 2.046800e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.555200e-02 5.289700e-04 5.892700e-04
+1.500000e+00 1.000000e-01 1.000000e-01 1.074700e-02 2.766600e-04 3.018000e-04
+1.800000e+00 2.000000e-01 2.000000e-01 1.577400e-03 9.334100e-05 1.177700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d40-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d40-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t40
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.006400e+00 2.651100e-02 4.459400e-02
+7.500000e-02 2.500000e-02 2.500000e-02 1.041000e+00 3.138200e-02 1.939700e-02
+1.250000e-01 2.500000e-02 2.500000e-02 1.085800e+00 2.771400e-02 4.315800e-02
+1.750000e-01 2.500000e-02 2.500000e-02 1.160700e+00 5.162200e-02 2.274600e-02
+2.250000e-01 2.500000e-02 2.500000e-02 1.241700e+00 2.946500e-02 4.578600e-02
+2.750000e-01 2.500000e-02 2.500000e-02 1.324100e+00 1.843700e-02 4.872300e-02
+3.250000e-01 2.500000e-02 2.500000e-02 1.374500e+00 1.193200e-02 1.566200e-02
+3.750000e-01 2.500000e-02 2.500000e-02 1.417800e+00 2.793200e-02 1.814500e-02
+4.250000e-01 2.500000e-02 2.500000e-02 1.368400e+00 1.022300e-02 9.238300e-03
+4.750000e-01 2.500000e-02 2.500000e-02 1.301800e+00 3.150100e-02 9.823400e-03
+5.250000e-01 2.500000e-02 2.500000e-02 1.204000e+00 2.169500e-02 2.649500e-02
+5.750000e-01 2.500000e-02 2.500000e-02 1.133300e+00 1.727300e-02 6.940400e-03
+6.250000e-01 2.500000e-02 2.500000e-02 1.024100e+00 2.797200e-02 3.219000e-02
+6.750000e-01 2.500000e-02 2.500000e-02 8.917100e-01 2.951600e-02 0.000000e+00
+7.250000e-01 2.500000e-02 2.500000e-02 7.427700e-01 4.053500e-02 0.000000e+00
+7.750000e-01 2.500000e-02 2.500000e-02 5.917100e-01 1.901600e-04 3.304800e-02
+8.250000e-01 2.500000e-02 2.500000e-02 4.877000e-01 1.963300e-02 5.870300e-03
+8.750000e-01 2.500000e-02 2.500000e-02 3.724000e-01 5.587000e-03 4.653900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 2.982400e-01 7.696900e-03 1.102500e-02
+9.750000e-01 2.500000e-02 2.500000e-02 2.318500e-01 0.000000e+00 1.112200e-02
+1.025000e+00 2.500000e-02 2.500000e-02 1.790100e-01 1.048900e-02 7.040500e-03
+1.075000e+00 2.500000e-02 2.500000e-02 1.332300e-01 7.665800e-03 4.872400e-03
+1.125000e+00 2.500000e-02 2.500000e-02 1.046500e-01 6.651300e-03 2.049700e-03
+1.175000e+00 2.500000e-02 2.500000e-02 7.552400e-02 0.000000e+00 8.733400e-03
+1.250000e+00 5.000000e-02 5.000000e-02 4.978900e-02 2.021200e-03 2.212300e-03
+1.350000e+00 5.000000e-02 5.000000e-02 2.532400e-02 1.114800e-03 2.417500e-03
+1.500000e+00 1.000000e-01 1.000000e-01 1.082000e-02 0.000000e+00 1.249500e-03
+1.800000e+00 2.000000e-01 2.000000e-01 1.752000e-03 1.180000e-04 5.657900e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d41-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d41-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.964000e-01 1.607332e-02 1.717396e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.848500e-01 7.374995e-03 6.654775e-03
+2.000000e+00 5.000000e-01 5.000000e-01 8.968700e-02 6.468044e-03 6.752842e-03
+3.000000e+00 5.000000e-01 5.000000e-01 2.270900e-02 3.138601e-03 2.722886e-03
+4.000000e+00 5.000000e-01 5.000000e-01 4.667900e-03 9.714106e-04 8.115541e-04
+6.500000e+00 2.000000e+00 2.000000e+00 1.683300e-03 4.780830e-04 4.506593e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d41-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d41-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.974500e-01 4.962600e-03 5.161900e-03
+1.000000e+00 5.000000e-01 5.000000e-01 2.853700e-01 3.791500e-03 2.628200e-03
+2.000000e+00 5.000000e-01 5.000000e-01 8.776600e-02 1.671000e-03 1.759900e-03
+3.000000e+00 5.000000e-01 5.000000e-01 2.271300e-02 7.866500e-04 5.123500e-04
+4.000000e+00 5.000000e-01 5.000000e-01 5.262600e-03 2.141000e-04 4.450100e-04
+6.500000e+00 2.000000e+00 2.000000e+00 1.437100e-03 1.139900e-04 1.704700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d41-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d41-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.285200e-01 2.975800e-02 2.687500e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.982700e-01 1.574400e-02 1.691700e-02
+2.000000e+00 5.000000e-01 5.000000e-01 6.750600e-02 7.575200e-03 8.807000e-03
+3.000000e+00 5.000000e-01 5.000000e-01 1.000000e-99 0.000000e+00 0.000000e+00
+4.000000e+00 5.000000e-01 5.000000e-01 1.000000e-99 0.000000e+00 0.000000e+00
+6.500000e+00 2.000000e+00 2.000000e+00 1.000000e-99 0.000000e+00 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d41-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d41-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t41
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.807900e-01 1.766100e-02 1.722700e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.978700e-01 1.318500e-02 9.317100e-03
+2.000000e+00 5.000000e-01 5.000000e-01 9.355500e-02 4.131100e-03 6.521300e-03
+3.000000e+00 5.000000e-01 5.000000e-01 2.286700e-02 2.761800e-04 1.435100e-03
+4.000000e+00 5.000000e-01 5.000000e-01 4.111000e-03 0.000000e+00 5.716300e-04
+6.500000e+00 2.000000e+00 2.000000e+00 8.071900e-04 8.568600e-05 7.494700e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d42-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d42-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t42
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.462800e-03 7.499147e-04 7.406124e-04
+7.500000e+01 2.500000e+01 2.500000e+01 7.215300e-03 5.754537e-04 5.787028e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.483700e-03 4.720876e-04 4.692823e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.239800e-03 1.940097e-04 1.965313e-04
+5.150000e+02 2.150000e+02 2.150000e+02 7.642600e-05 4.291271e-05 4.259800e-05
+8.150000e+02 8.500000e+01 8.500000e+01 3.737200e-06 3.442953e-04 3.442747e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d42-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d42-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t42
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.366300e-03 2.815300e-04 3.703300e-04
+7.500000e+01 2.500000e+01 2.500000e+01 5.617000e-03 3.670800e-04 3.587300e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.775800e-03 2.768900e-04 2.412400e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.481900e-03 9.808200e-05 1.029800e-04
+5.150000e+02 2.150000e+02 2.150000e+02 1.524100e-04 1.802100e-05 1.859600e-05
+8.150000e+02 8.500000e+01 8.500000e+01 7.551100e-06 6.318500e-06 6.374200e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d42-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d42-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t42
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.550900e-03 4.657300e-04 2.392800e-04
+7.500000e+01 2.500000e+01 2.500000e+01 5.704000e-03 2.641700e-04 2.175700e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.576100e-03 1.452600e-04 1.765400e-05
+2.300000e+02 7.000000e+01 7.000000e+01 1.457600e-03 7.701300e-05 2.489200e-04
+5.150000e+02 2.150000e+02 2.150000e+02 1.547500e-04 1.172200e-05 3.773100e-06
+8.150000e+02 8.500000e+01 8.500000e+01 1.225900e-05 6.416000e-08 7.997900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d43-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d43-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t43
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.825400e-01 4.804469e-02 5.256234e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.627400e+00 2.142801e-01 2.114021e-01
+9.500000e-01 5.000000e-02 5.000000e-02 5.467400e+00 4.834528e-01 4.842489e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d43-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d43-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t43
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.458000e-01 1.775100e-02 2.787700e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.731500e+00 1.090200e-01 8.821700e-02
+9.500000e-01 5.000000e-02 5.000000e-02 4.816400e+00 2.585600e-01 2.326400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d43-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d43-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t43
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.275600e-01 1.348500e-02 0.000000e+00
+8.000000e-01 1.000000e-01 1.000000e-01 1.633100e+00 1.205100e-01 1.407900e-02
+9.500000e-01 5.000000e-02 5.000000e-02 5.140800e+00 0.000000e+00 3.413200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d44-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d44-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t44
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 8.040500e-02 1.809084e-02 1.855774e-02
+4.400000e+00 8.000000e-01 8.000000e-01 2.001600e-01 2.488998e-02 2.451298e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.495500e-01 4.113629e-02 4.162140e-02
+7.400000e+00 1.400000e+00 1.400000e+00 1.026900e-01 1.709198e-02 1.605860e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d44-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d44-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t44
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 8.200600e-02 7.824900e-03 7.288100e-03
+4.400000e+00 8.000000e-01 8.000000e-01 2.052200e-01 1.095700e-02 1.105700e-02
+5.600000e+00 4.000000e-01 4.000000e-01 3.500600e-01 2.387300e-02 1.992000e-02
+7.400000e+00 1.400000e+00 1.400000e+00 9.885600e-02 5.658200e-03 8.310200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d44-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d44-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t44
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.045100e-01 3.400700e-03 3.302800e-02
+4.400000e+00 8.000000e-01 8.000000e-01 2.127100e-01 7.506800e-03 0.000000e+00
+5.600000e+00 4.000000e-01 4.000000e-01 2.870300e-01 4.455300e-03 1.426800e-02
+7.400000e+00 1.400000e+00 1.400000e+00 1.013300e-01 1.218200e-02 7.319700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d45-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d45-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t45
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 5.044100e-03 8.141980e-04 7.683542e-04
+1.800000e+02 4.000000e+01 4.000000e+01 3.701600e-03 3.954643e-04 3.997386e-04
+2.675000e+02 4.750000e+01 4.750000e+01 1.582200e-03 2.584380e-04 2.475394e-04
+3.750000e+02 6.000000e+01 6.000000e+01 1.056700e-03 1.982897e-04 1.946652e-04
+5.600000e+02 1.250000e+02 1.250000e+02 4.964500e-04 9.283398e-05 1.016880e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d45-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d45-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t45
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 4.474700e-03 2.669800e-04 3.519000e-04
+1.800000e+02 4.000000e+01 4.000000e+01 3.799800e-03 2.287400e-04 2.140200e-04
+2.675000e+02 4.750000e+01 4.750000e+01 2.111300e-03 1.472800e-04 1.444400e-04
+3.750000e+02 6.000000e+01 6.000000e+01 1.014500e-03 9.289300e-05 8.840900e-05
+5.600000e+02 1.250000e+02 1.250000e+02 4.208800e-04 4.172900e-05 4.030600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d45-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d45-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t45
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 4.513200e-03 5.134400e-04 4.478600e-04
+1.800000e+02 4.000000e+01 4.000000e+01 3.297000e-03 1.464500e-04 5.099500e-05
+2.675000e+02 4.750000e+01 4.750000e+01 2.072700e-03 1.924800e-04 0.000000e+00
+3.750000e+02 6.000000e+01 6.000000e+01 1.129300e-03 0.000000e+00 1.010000e-04
+5.600000e+02 1.250000e+02 1.250000e+02 5.321100e-04 2.994500e-05 4.663600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d46-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d46-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t46
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.764900e+00 3.425195e-01 3.447472e-01
+7.000000e-01 3.000000e-01 3.000000e-01 4.900900e-01 7.924038e-02 7.482411e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d46-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d46-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t46
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.798700e+00 8.229200e-02 8.746100e-02
+7.000000e-01 3.000000e-01 3.000000e-01 4.675100e-01 4.090200e-02 3.642200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d46-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d46-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t46
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.780100e+00 7.337200e-02 3.594900e-02
+7.000000e-01 3.000000e-01 3.000000e-01 4.799400e-01 2.286300e-02 4.606900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d47-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d47-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t47
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.859400e+00 1.383831e-01 1.371311e-01
+5.250000e-01 1.250000e-01 1.250000e-01 8.648800e-01 1.483110e-01 1.494041e-01
+8.250000e-01 1.750000e-01 1.750000e-01 1.143000e-01 3.684675e-02 3.779701e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d47-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d47-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t47
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.962100e+00 6.646300e-02 7.265300e-02
+5.250000e-01 1.250000e-01 1.250000e-01 7.367100e-01 7.076100e-02 5.149600e-02
+8.250000e-01 1.750000e-01 1.750000e-01 8.849300e-02 1.510200e-02 1.640000e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d47-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d47-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t47
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.787900e+00 7.472700e-02 4.901200e-02
+5.250000e-01 1.250000e-01 1.250000e-01 9.465600e-01 3.179200e-02 1.206000e-01
+8.250000e-01 1.750000e-01 1.750000e-01 1.377400e-01 3.181000e-02 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d48-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d48-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t48
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.259500e-01 4.071903e-02 4.353340e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.331100e-01 2.999246e-02 2.778104e-02
+3.000000e+00 1.500000e+00 1.500000e+00 1.409400e-01 3.220689e-02 3.230973e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d48-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d48-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t48
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.340400e-01 2.770900e-02 2.923400e-02
+1.000000e+00 5.000000e-01 5.000000e-01 2.317200e-01 2.357400e-02 1.444500e-02
+3.000000e+00 1.500000e+00 1.500000e+00 1.342300e-01 1.156500e-02 2.024000e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d48-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d48-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t48
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.690500e-01 4.568600e-02 8.327700e-03
+1.000000e+00 5.000000e-01 5.000000e-01 2.610700e-01 1.182600e-03 2.935000e-02
+3.000000e+00 1.500000e+00 1.500000e+00 1.698800e-01 8.419100e-03 2.333900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d49-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d49-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.464200e-03 1.996778e-04 2.113957e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.836000e-03 9.182172e-05 8.486924e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.184800e-03 5.965306e-05 5.928028e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.544600e-03 5.350731e-05 5.426567e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.723800e-04 6.713703e-05 6.666637e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.727900e-04 3.266261e-05 3.194779e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.167100e-04 2.703154e-05 2.736909e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.463200e-04 2.138141e-05 1.994644e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.157300e-04 1.707022e-05 1.933633e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.148800e-04 1.051342e-05 1.244345e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.075600e-05 4.292400e-06 4.616306e-06
+2.350000e+03 3.500000e+02 3.500000e+02 6.020500e-06 1.381048e-06 1.010973e-06
+3.350000e+03 6.500000e+02 6.500000e+02 4.115900e-07 1.815897e-07 1.841067e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d49-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d49-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.362400e-03 1.517800e-04 7.976300e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.763800e-03 4.917600e-05 4.543100e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.078900e-03 3.484700e-05 6.022000e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.516000e-03 4.289100e-05 2.805600e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.084100e-03 3.456400e-05 2.558000e-05
+9.325000e+02 5.250000e+01 5.250000e+01 7.263800e-04 1.870300e-05 2.226500e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.991600e-04 1.424200e-05 4.147700e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.393900e-04 1.345400e-05 3.205200e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.167400e-04 9.725900e-06 8.230800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.307500e-04 1.042800e-05 7.351200e-06
+1.750000e+03 2.500000e+02 2.500000e+02 4.830800e-05 2.449800e-06 2.340000e-06
+2.350000e+03 3.500000e+02 3.500000e+02 7.398900e-06 9.804100e-07 7.028100e-07
+3.350000e+03 6.500000e+02 6.500000e+02 3.216200e-07 1.115200e-07 1.137400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d49-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d49-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.340800e-03 6.275200e-05 5.554000e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.727800e-03 3.754100e-05 3.297400e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.047600e-03 1.641100e-05 1.416700e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.513300e-03 1.884800e-06 1.406900e-06
+8.325000e+02 4.750000e+01 4.750000e+01 1.093600e-03 7.142800e-06 6.258100e-06
+9.325000e+02 5.250000e+01 5.250000e+01 7.536900e-04 7.335400e-06 8.193300e-06
+1.042500e+03 5.750000e+01 5.750000e+01 4.879300e-04 7.938800e-06 8.993600e-06
+1.150000e+03 5.000000e+01 5.000000e+01 3.398100e-04 7.353300e-06 8.376900e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.316000e-04 6.621200e-06 7.595800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.364600e-04 4.720900e-06 5.463900e-06
+1.750000e+03 2.500000e+02 2.500000e+02 4.906600e-05 2.178600e-06 2.539400e-06
+2.350000e+03 3.500000e+02 3.500000e+02 7.462200e-06 4.830600e-07 5.763600e-07
+3.350000e+03 6.500000e+02 6.500000e+02 4.745900e-07 3.978200e-08 4.824000e-08
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d49-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d49-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t49
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.076200e-03 2.259800e-05 0.000000e+00
+5.800000e+02 3.500000e+01 3.500000e+01 2.594500e-03 5.505600e-05 2.109200e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.979900e-03 0.000000e+00 5.741600e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.483800e-03 2.652200e-05 1.098100e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.120500e-03 5.984700e-05 0.000000e+00
+9.325000e+02 5.250000e+01 5.250000e+01 7.786500e-04 8.528000e-06 1.625300e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.361400e-04 3.902500e-06 2.148600e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.686100e-04 4.868100e-06 2.126300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.547800e-04 7.683900e-06 9.004900e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.563300e-04 6.102600e-06 4.274000e-06
+1.750000e+03 2.500000e+02 2.500000e+02 6.236300e-05 1.035100e-06 2.966500e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.072300e-05 6.190200e-07 1.829600e-06
+3.350000e+03 6.500000e+02 6.500000e+02 7.258400e-07 6.961000e-08 1.417800e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d50-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d50-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.229500e-03 1.760392e-04 1.805021e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.636300e-03 2.391740e-04 2.509045e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.791700e-03 2.040372e-04 1.978798e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.903100e-03 1.655871e-04 1.657681e-04
+1.450000e+02 1.500000e+01 1.500000e+01 3.430400e-03 2.001677e-04 1.964339e-04
+1.925000e+02 3.250000e+01 3.250000e+01 1.805500e-03 1.314386e-04 1.261339e-04
+2.625000e+02 3.750000e+01 3.750000e+01 6.032300e-04 4.792068e-05 4.885793e-05
+5.150000e+02 2.150000e+02 2.150000e+02 3.539900e-05 1.118806e-05 1.125360e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d50-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d50-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.036300e-03 6.760400e-05 1.112300e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.179700e-03 2.209500e-04 1.171000e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.496100e-03 1.463100e-04 1.102000e-04
+1.150000e+02 1.500000e+01 1.500000e+01 5.046700e-03 1.101200e-04 9.157500e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.600100e-03 7.650000e-05 8.250700e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.899000e-03 3.695100e-05 6.108000e-05
+2.625000e+02 3.750000e+01 3.750000e+01 6.468500e-04 2.218100e-05 2.566600e-05
+5.150000e+02 2.150000e+02 2.150000e+02 5.800200e-05 2.510800e-06 3.390100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d50-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d50-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.334000e-03 5.676300e-05 5.180300e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.387100e-03 7.000000e-05 6.461300e-05
+8.750000e+01 1.250000e+01 1.250000e+01 6.563100e-03 1.731800e-05 1.512600e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.897500e-03 9.733100e-06 1.240000e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.383800e-03 4.071700e-05 4.674900e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.772500e-03 2.564800e-05 2.992200e-05
+2.625000e+02 3.750000e+01 3.750000e+01 6.140200e-04 9.495300e-06 9.943300e-06
+5.150000e+02 2.150000e+02 2.150000e+02 5.777400e-05 1.226300e-06 1.374600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d50-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d50-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t50
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.381400e-03 1.635300e-04 0.000000e+00
+6.250000e+01 1.250000e+01 1.250000e+01 7.233900e-03 2.045000e-04 8.229600e-05
+8.750000e+01 1.250000e+01 1.250000e+01 6.471800e-03 0.000000e+00 2.897600e-04
+1.150000e+02 1.500000e+01 1.500000e+01 5.026500e-03 0.000000e+00 8.197700e-05
+1.450000e+02 1.500000e+01 1.500000e+01 3.461800e-03 8.954200e-06 9.398300e-05
+1.925000e+02 3.250000e+01 3.250000e+01 1.777400e-03 1.895000e-05 7.372300e-06
+2.625000e+02 3.750000e+01 3.750000e+01 6.069100e-04 2.572100e-06 2.378200e-05
+5.150000e+02 2.150000e+02 2.150000e+02 5.253100e-05 2.034200e-06 1.387600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d51-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d51-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.021200e-01 1.267664e-02 1.298212e-02
+4.500000e-01 1.500000e-01 1.500000e-01 2.207600e-01 2.769733e-02 2.627560e-02
+6.500000e-01 5.000000e-02 5.000000e-02 7.932300e-01 5.151811e-02 5.025837e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.471100e+00 6.159276e-02 6.083139e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.509000e+00 9.585503e-02 9.570895e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.183200e+00 1.134895e-01 1.150631e-01
+9.250000e-01 2.500000e-02 2.500000e-02 3.752800e+00 1.518879e-01 1.516537e-01
+9.750000e-01 2.500000e-02 2.500000e-02 4.089000e+00 1.543104e-01 1.577002e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d51-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d51-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.220100e-01 4.518900e-03 9.244800e-03
+4.500000e-01 1.500000e-01 1.500000e-01 3.111600e-01 7.224300e-03 1.256900e-02
+6.500000e-01 5.000000e-02 5.000000e-02 8.244500e-01 4.298100e-02 1.962800e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.495500e+00 3.266400e-02 2.800800e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.274100e+00 4.610200e-02 5.724300e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.935100e+00 5.674800e-02 5.324900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.575100e+00 6.514400e-02 6.784100e-02
+9.750000e-01 2.500000e-02 2.500000e-02 3.976700e+00 9.147900e-02 7.812900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d51-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d51-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.156100e-01 4.403700e-03 5.437600e-03
+4.500000e-01 1.500000e-01 1.500000e-01 2.631000e-01 7.411500e-03 8.683900e-03
+6.500000e-01 5.000000e-02 5.000000e-02 7.011700e-01 1.146200e-02 1.265600e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.348100e+00 1.296400e-02 1.444500e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.216700e+00 4.095600e-03 2.309800e-03
+8.750000e-01 2.500000e-02 2.500000e-02 2.999700e+00 2.146300e-02 1.822100e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.891400e+00 4.270000e-02 3.788700e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.521500e+00 7.078200e-02 6.142300e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d51-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d51-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t51
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 9.199300e-02 0.000000e+00 6.011700e-03
+4.500000e-01 1.500000e-01 1.500000e-01 2.361700e-01 4.630400e-03 0.000000e+00
+6.500000e-01 5.000000e-02 5.000000e-02 6.701500e-01 7.539200e-03 3.591600e-03
+7.500000e-01 5.000000e-02 5.000000e-02 1.411500e+00 0.000000e+00 4.634900e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.238700e+00 2.544500e-02 3.225400e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.063800e+00 1.115200e-01 0.000000e+00
+9.250000e-01 2.500000e-02 2.500000e-02 3.933400e+00 0.000000e+00 5.605500e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.631700e+00 8.503900e-02 2.714100e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d52-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d52-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.585100e-01 2.518342e-02 2.672197e-02
+2.600000e+00 2.000000e-01 2.000000e-01 4.202800e-01 2.460143e-02 2.534064e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.931000e-01 1.687880e-02 1.797093e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.616300e-01 1.809483e-02 1.809607e-02
+4.000000e+00 4.000000e-01 4.000000e-01 2.988300e-01 1.424917e-02 1.217896e-02
+4.800000e+00 4.000000e-01 4.000000e-01 6.914100e-02 8.368347e-03 7.255041e-03
+7.000000e+00 1.800000e+00 1.800000e+00 3.395000e-03 6.473179e-04 8.672093e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d52-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d52-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.378200e-01 6.433500e-03 9.734800e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.044000e-01 8.529400e-03 1.097200e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.542900e-01 1.031700e-02 7.285100e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.611600e-01 7.634000e-03 7.996200e-03
+4.000000e+00 4.000000e-01 4.000000e-01 3.109100e-01 4.790400e-03 9.374000e-03
+4.800000e+00 4.000000e-01 4.000000e-01 9.313200e-02 4.360800e-03 2.659600e-03
+7.000000e+00 1.800000e+00 1.800000e+00 3.804900e-03 4.094000e-04 4.730600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d52-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d52-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.923400e-01 4.908300e-03 3.857800e-03
+2.600000e+00 2.000000e-01 2.000000e-01 4.344800e-01 4.387700e-03 3.463600e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.633100e-01 3.133200e-03 2.570600e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.337800e-01 1.285400e-03 1.214900e-03
+4.000000e+00 4.000000e-01 4.000000e-01 2.888900e-01 2.503900e-03 3.145100e-03
+4.800000e+00 4.000000e-01 4.000000e-01 8.277700e-02 2.155300e-03 2.719400e-03
+7.000000e+00 1.800000e+00 1.800000e+00 3.639800e-03 1.792500e-04 2.194100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d52-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d52-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t52
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.778100e-01 1.067500e-02 0.000000e+00
+2.600000e+00 2.000000e-01 2.000000e-01 4.312200e-01 0.000000e+00 1.555600e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.550200e-01 6.082600e-03 2.484300e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.389700e-01 1.130300e-02 0.000000e+00
+4.000000e+00 4.000000e-01 4.000000e-01 2.945800e-01 0.000000e+00 7.117200e-03
+4.800000e+00 4.000000e-01 4.000000e-01 8.617900e-02 1.615400e-03 0.000000e+00
+7.000000e+00 1.800000e+00 1.800000e+00 3.939400e-03 1.614400e-04 6.160800e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d53-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d53-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.340500e-03 3.722522e-04 2.395128e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.653100e-03 3.321929e-04 3.467350e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.519100e-03 2.240276e-04 2.436738e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.379400e-03 2.045837e-04 1.978199e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.527800e-03 2.223416e-04 2.251322e-04
+2.050000e+02 1.500000e+01 1.500000e+01 4.385000e-03 1.520537e-04 1.592443e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.670000e-03 1.328195e-04 1.378058e-04
+2.650000e+02 1.500000e+01 1.500000e+01 1.797800e-03 9.739703e-05 1.082551e-04
+3.150000e+02 3.500000e+01 3.500000e+01 8.616300e-04 8.359779e-05 8.738209e-05
+4.150000e+02 6.500000e+01 6.500000e+01 2.206100e-04 4.065504e-05 4.063993e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.216700e-05 5.730018e-06 5.618282e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d53-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d53-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.933000e-03 1.368500e-04 2.093900e-04
+1.050000e+02 1.000000e+01 1.000000e+01 6.061200e-03 2.334000e-04 1.518500e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.474500e-03 1.310900e-04 1.112400e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.137900e-03 1.142800e-04 1.156800e-04
+1.775000e+02 1.250000e+01 1.250000e+01 5.367000e-03 1.069000e-04 1.124600e-04
+2.050000e+02 1.500000e+01 1.500000e+01 4.026100e-03 9.907300e-05 8.043900e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.707900e-03 6.825300e-05 7.547100e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.767900e-03 6.554700e-05 5.563200e-05
+3.150000e+02 3.500000e+01 3.500000e+01 8.826800e-04 2.512700e-05 3.951400e-05
+4.150000e+02 6.500000e+01 6.500000e+01 2.406000e-04 9.303600e-06 1.188700e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.497400e-05 3.529500e-06 2.836700e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d53-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d53-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.368500e-03 7.678900e-05 1.016000e-04
+1.050000e+02 1.000000e+01 1.000000e+01 5.435400e-03 2.930000e-05 3.891400e-05
+1.275000e+02 1.250000e+01 1.250000e+01 6.012000e-03 2.458900e-05 2.809900e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.045600e-03 2.644600e-05 2.375300e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.498800e-03 4.430600e-05 3.706400e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.150100e-03 1.428900e-05 1.241200e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.914500e-03 1.523900e-05 1.148200e-05
+2.650000e+02 1.500000e+01 1.500000e+01 2.062300e-03 1.778200e-05 1.193900e-05
+3.150000e+02 3.500000e+01 3.500000e+01 9.659200e-04 1.178500e-05 9.862800e-06
+4.150000e+02 6.500000e+01 6.500000e+01 2.904800e-04 7.166700e-06 6.459100e-06
+5.825000e+02 1.025000e+02 1.025000e+02 3.739800e-05 1.258600e-06 1.421500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d53-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d53-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t53
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.181300e-03 1.496200e-04 6.003400e-05
+1.050000e+02 1.000000e+01 1.000000e+01 5.517600e-03 2.552600e-04 2.778900e-05
+1.275000e+02 1.250000e+01 1.250000e+01 5.899600e-03 8.435000e-05 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 5.839100e-03 6.783400e-05 6.978800e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.382100e-03 0.000000e+00 6.059300e-05
+2.050000e+02 1.500000e+01 1.500000e+01 4.166900e-03 0.000000e+00 1.995900e-04
+2.350000e+02 1.500000e+01 1.500000e+01 3.038600e-03 2.376700e-05 1.260300e-04
+2.650000e+02 1.500000e+01 1.500000e+01 1.940100e-03 2.828900e-05 5.446300e-05
+3.150000e+02 3.500000e+01 3.500000e+01 1.071000e-03 6.070700e-05 4.676800e-07
+4.150000e+02 6.500000e+01 6.500000e+01 3.052400e-04 2.268800e-06 8.337000e-06
+5.825000e+02 1.025000e+02 1.025000e+02 4.826200e-05 1.483400e-06 4.029900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d54-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d54-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.128800e-03 2.620050e-04 2.899555e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.649900e-03 1.365857e-04 1.343382e-04
+6.550000e+02 4.000000e+01 4.000000e+01 2.033600e-03 8.972807e-05 9.790188e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.463000e-03 7.369309e-05 6.555212e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.101500e-03 5.937838e-05 4.810172e-05
+9.325000e+02 5.250000e+01 5.250000e+01 7.242700e-04 6.319372e-05 7.426883e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.979900e-04 4.593612e-05 4.442757e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.372000e-04 3.600630e-05 3.230795e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.281200e-04 5.344951e-05 4.520928e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.710500e-04 2.235096e-05 2.038130e-05
+1.750000e+03 2.500000e+02 2.500000e+02 7.781400e-05 9.211709e-06 9.863134e-06
+3.000000e+03 1.000000e+03 1.000000e+03 4.450100e-06 1.035972e-06 1.055269e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d54-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d54-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.866500e-03 6.705400e-05 1.330400e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.419600e-03 4.278100e-05 5.760900e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.936500e-03 5.110200e-05 3.922100e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.480000e-03 3.637000e-05 2.943700e-05
+8.325000e+02 4.750000e+01 4.750000e+01 1.099600e-03 3.895100e-05 2.495200e-05
+9.325000e+02 5.250000e+01 5.250000e+01 7.932000e-04 2.155700e-05 2.120500e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.644900e-04 1.652600e-05 3.016000e-05
+1.150000e+03 5.000000e+01 5.000000e+01 4.028700e-04 2.143800e-05 1.508400e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.775000e-04 1.403900e-05 1.108400e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.772200e-04 8.951800e-06 9.651300e-06
+1.750000e+03 2.500000e+02 2.500000e+02 7.868200e-05 5.007200e-06 4.138300e-06
+3.000000e+03 1.000000e+03 1.000000e+03 6.509700e-06 4.254800e-07 4.360400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d54-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d54-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.857900e-03 6.863800e-05 6.031800e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.441400e-03 4.315400e-05 3.749800e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.924000e-03 2.031900e-05 1.742100e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.478200e-03 5.211700e-06 7.140200e-06
+8.325000e+02 4.750000e+01 4.750000e+01 1.116600e-03 4.712300e-06 3.505100e-06
+9.325000e+02 5.250000e+01 5.250000e+01 7.835000e-04 6.910300e-06 7.682700e-06
+1.042500e+03 5.750000e+01 5.750000e+01 5.489300e-04 8.016600e-06 9.075900e-06
+1.150000e+03 5.000000e+01 5.000000e+01 4.138100e-04 8.564600e-06 9.779600e-06
+1.275000e+03 7.500000e+01 7.500000e+01 2.804300e-04 7.022500e-06 8.104500e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.783300e-04 5.887600e-06 6.839400e-06
+1.750000e+03 2.500000e+02 2.500000e+02 7.794300e-05 3.586900e-06 4.234800e-06
+3.000000e+03 1.000000e+03 1.000000e+03 6.451900e-06 4.741000e-07 5.792000e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d54-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d54-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t54
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.694100e-03 4.588300e-05 1.186700e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.354400e-03 4.103500e-05 1.611100e-04
+6.550000e+02 4.000000e+01 4.000000e+01 1.864400e-03 3.899500e-05 9.574800e-06
+7.400000e+02 4.500000e+01 4.500000e+01 1.430600e-03 3.323100e-05 3.800600e-06
+8.325000e+02 4.750000e+01 4.750000e+01 1.103500e-03 1.491100e-06 4.704400e-05
+9.325000e+02 5.250000e+01 5.250000e+01 8.073400e-04 2.663000e-05 1.539800e-05
+1.042500e+03 5.750000e+01 5.750000e+01 5.665400e-04 0.000000e+00 3.498800e-05
+1.150000e+03 5.000000e+01 5.000000e+01 4.249600e-04 1.117400e-05 2.483100e-05
+1.275000e+03 7.500000e+01 7.500000e+01 3.121300e-04 2.072200e-05 5.586200e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.972000e-04 2.960700e-06 1.049200e-05
+1.750000e+03 2.500000e+02 2.500000e+02 9.100700e-05 4.209700e-06 5.599100e-07
+3.000000e+03 1.000000e+03 1.000000e+03 8.448800e-06 1.072300e-08 7.075800e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d55-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d55-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.549200e-03 2.524824e-04 2.841926e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.822300e-03 3.242681e-04 3.557233e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.470500e-03 2.433973e-04 2.439199e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.873900e-03 2.234423e-04 2.149565e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.179600e-03 1.084264e-04 9.723728e-05
+6.000000e+02 3.000000e+02 3.000000e+02 2.939500e-05 9.383853e-06 9.503880e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d55-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d55-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.059300e-03 1.180600e-04 6.540700e-05
+6.250000e+01 1.250000e+01 1.250000e+01 6.935900e-03 1.272000e-04 1.378500e-04
+8.750000e+01 1.250000e+01 1.250000e+01 6.167900e-03 1.183700e-04 1.659900e-04
+1.300000e+02 3.000000e+01 3.000000e+01 4.269300e-03 6.474800e-05 7.044300e-05
+2.300000e+02 7.000000e+01 7.000000e+01 1.320200e-03 2.689800e-05 2.864400e-05
+6.000000e+02 3.000000e+02 3.000000e+02 4.741800e-05 2.040700e-06 2.860900e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d55-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d55-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.207900e-03 5.427800e-05 4.990900e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.049600e-03 2.618500e-05 2.292100e-05
+8.750000e+01 1.250000e+01 1.250000e+01 6.109500e-03 1.780300e-05 1.398800e-05
+1.300000e+02 3.000000e+01 3.000000e+01 4.136600e-03 2.373800e-05 2.731300e-05
+2.300000e+02 7.000000e+01 7.000000e+01 1.298100e-03 1.135600e-05 1.165400e-05
+6.000000e+02 3.000000e+02 3.000000e+02 5.116500e-05 8.963600e-07 1.009400e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d55-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d55-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t55
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 4.188400e-03 1.320500e-05 2.339400e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.118500e-03 2.043000e-04 0.000000e+00
+8.750000e+01 1.250000e+01 1.250000e+01 6.287900e-03 2.211800e-04 0.000000e+00
+1.300000e+02 3.000000e+01 3.000000e+01 4.151200e-03 0.000000e+00 1.346200e-04
+2.300000e+02 7.000000e+01 7.000000e+01 1.267700e-03 4.865800e-05 1.848200e-05
+6.000000e+02 3.000000e+02 3.000000e+02 4.812100e-05 7.884400e-07 1.691700e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d56-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d56-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.514700e-01 3.751747e-02 2.130119e-02
+4.500000e-01 1.500000e-01 1.500000e-01 3.266500e-01 4.156937e-02 4.061237e-02
+6.500000e-01 5.000000e-02 5.000000e-02 8.897000e-01 8.108349e-02 7.509931e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.500600e+00 7.684479e-02 7.875645e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.598000e+00 1.087935e-01 1.104730e-01
+9.500000e-01 5.000000e-02 5.000000e-02 3.577300e+00 1.397788e-01 1.588906e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d56-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d56-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.957800e-01 9.968400e-03 5.864100e-03
+4.500000e-01 1.500000e-01 1.500000e-01 4.135400e-01 1.110700e-02 1.130700e-02
+6.500000e-01 5.000000e-02 5.000000e-02 8.999300e-01 2.371600e-02 2.675100e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.519300e+00 3.362200e-02 3.832600e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.421200e+00 3.580800e-02 3.858400e-02
+9.500000e-01 5.000000e-02 5.000000e-02 3.331600e+00 4.430300e-02 4.442800e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d56-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d56-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.912000e-01 4.280800e-03 5.141900e-03
+4.500000e-01 1.500000e-01 1.500000e-01 3.777800e-01 6.925600e-03 8.243600e-03
+6.500000e-01 5.000000e-02 5.000000e-02 8.328200e-01 1.257400e-02 1.376900e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.467100e+00 1.240800e-02 1.466400e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.454800e+00 1.489600e-02 1.157000e-02
+9.500000e-01 5.000000e-02 5.000000e-02 3.538400e+00 5.431100e-02 4.755200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d56-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d56-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t56
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.592800e-01 2.592000e-03 1.464100e-02
+4.500000e-01 1.500000e-01 1.500000e-01 3.326200e-01 4.178100e-04 9.219100e-03
+6.500000e-01 5.000000e-02 5.000000e-02 7.922100e-01 4.346700e-02 1.424800e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.469400e+00 1.632700e-02 4.712500e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.559300e+00 4.775900e-03 2.721300e-02
+9.500000e-01 5.000000e-02 5.000000e-02 3.703400e+00 7.325300e-02 1.936400e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d57-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d57-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.020900e-01 2.337438e-02 2.330605e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.414000e-01 2.128435e-02 2.437171e-02
+3.000000e+00 2.000000e-01 2.000000e-01 3.860900e-01 2.054651e-02 2.264921e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.789700e-01 2.085667e-02 2.428364e-02
+3.800000e+00 2.000000e-01 2.000000e-01 4.331800e-01 1.931064e-02 1.911455e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.794300e-01 1.788684e-02 1.655674e-02
+4.800000e+00 4.000000e-01 4.000000e-01 1.441300e-01 1.360667e-02 1.320912e-02
+5.800000e+00 6.000000e-01 6.000000e-01 2.921000e-02 1.074458e-02 5.853417e-03
+7.600000e+00 1.200000e+00 1.200000e+00 4.910500e-04 3.696222e-04 2.965312e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d57-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d57-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.131800e-01 5.568900e-03 8.317900e-03
+2.600000e+00 2.000000e-01 2.000000e-01 2.933900e-01 6.218800e-03 1.134900e-02
+3.000000e+00 2.000000e-01 2.000000e-01 3.813900e-01 7.088100e-03 1.214800e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.505100e-01 7.703700e-03 9.715100e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.414000e-01 1.342000e-02 7.637000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 3.084400e-01 9.782500e-03 7.649800e-03
+4.800000e+00 4.000000e-01 4.000000e-01 1.544100e-01 9.954000e-03 3.189100e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.264500e-02 3.213400e-03 1.571300e-03
+7.600000e+00 1.200000e+00 1.200000e+00 8.210600e-04 1.343000e-04 1.573100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d57-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d57-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.410400e-01 4.783500e-03 3.724600e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.167900e-01 5.495500e-03 4.349800e-03
+3.000000e+00 2.000000e-01 2.000000e-01 3.915800e-01 4.882400e-03 3.733400e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.489200e-01 4.388700e-03 3.257900e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.201900e-01 1.333200e-03 1.091000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.953200e-01 3.791500e-03 5.089900e-03
+4.800000e+00 4.000000e-01 4.000000e-01 1.432200e-01 3.242400e-03 3.960400e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.144700e-02 1.697800e-03 2.257300e-03
+7.600000e+00 1.200000e+00 1.200000e+00 8.951300e-04 1.019200e-04 1.461700e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d57-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d57-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t57
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.522200e-01 5.291200e-03 3.194300e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.301700e-01 2.314200e-03 0.000000e+00
+3.000000e+00 2.000000e-01 2.000000e-01 3.968800e-01 0.000000e+00 1.996900e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.303700e-01 2.412700e-03 2.741700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.115800e-01 1.410000e-02 9.046400e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.828900e-01 1.086800e-02 2.722400e-03
+4.800000e+00 4.000000e-01 4.000000e-01 1.429200e-01 1.452700e-03 1.802300e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.382500e-02 9.918600e-04 1.378600e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.427900e-03 1.394800e-04 5.183800e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d58-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d58-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.960100e-03 5.601968e-04 4.767125e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.229700e-03 2.698135e-04 2.745017e-04
+1.650000e+02 2.500000e+01 2.500000e+01 5.404000e-03 1.892948e-04 2.011164e-04
+2.200000e+02 3.000000e+01 3.000000e+01 2.541500e-03 1.721515e-04 1.769221e-04
+2.825000e+02 3.250000e+01 3.250000e+01 1.104500e-03 9.399695e-05 9.223029e-05
+3.525000e+02 3.750000e+01 3.750000e+01 3.782300e-04 4.733330e-05 4.776250e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.281800e-04 2.227873e-05 2.203128e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.056800e-05 8.897889e-06 8.752365e-06
+8.425000e+02 1.575000e+02 1.575000e+02 4.757400e-10 2.158605e-05 2.158603e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d58-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d58-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.596100e-03 3.457600e-04 1.069400e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.140900e-03 1.603300e-04 1.319400e-04
+1.650000e+02 2.500000e+01 2.500000e+01 5.310000e-03 7.480800e-05 1.583100e-04
+2.200000e+02 3.000000e+01 3.000000e+01 2.755200e-03 5.001100e-05 8.580900e-05
+2.825000e+02 3.250000e+01 3.250000e+01 1.128300e-03 3.521600e-05 3.907100e-05
+3.525000e+02 3.750000e+01 3.750000e+01 4.258100e-04 2.307300e-05 1.763000e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.404700e-04 9.069100e-06 1.346600e-05
+5.825000e+02 1.025000e+02 1.025000e+02 2.965200e-05 2.811900e-06 2.971000e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.545900e-06 6.840100e-07 6.527900e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d58-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d58-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 6.945400e-03 8.267100e-05 1.108000e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.906400e-03 1.917200e-05 2.013900e-05
+1.650000e+02 2.500000e+01 2.500000e+01 5.440600e-03 3.022500e-05 2.197100e-05
+2.200000e+02 3.000000e+01 3.000000e+01 2.931100e-03 2.904300e-05 2.260200e-05
+2.825000e+02 3.250000e+01 3.250000e+01 1.201200e-03 1.480000e-05 1.198000e-05
+3.525000e+02 3.750000e+01 3.750000e+01 4.618700e-04 6.745900e-06 6.317300e-06
+4.350000e+02 4.500000e+01 4.500000e+01 1.697900e-04 6.088700e-06 5.403400e-06
+5.825000e+02 1.025000e+02 1.025000e+02 3.728700e-05 1.398200e-06 1.137000e-06
+8.425000e+02 1.575000e+02 1.575000e+02 2.267000e-06 1.110400e-07 1.279900e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d58-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d58-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t58
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 6.721900e-03 2.133300e-05 2.546300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.530400e-03 2.421000e-04 1.258800e-05
+1.650000e+02 2.500000e+01 2.500000e+01 5.359900e-03 6.805600e-05 0.000000e+00
+2.200000e+02 3.000000e+01 3.000000e+01 3.011000e-03 0.000000e+00 1.196600e-04
+2.825000e+02 3.250000e+01 3.250000e+01 1.315600e-03 1.542800e-05 1.985900e-05
+3.525000e+02 3.750000e+01 3.750000e+01 5.297400e-04 4.476400e-05 1.635500e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.952400e-04 2.498500e-05 0.000000e+00
+5.825000e+02 1.025000e+02 1.025000e+02 4.351800e-05 1.402500e-07 2.010700e-06
+8.425000e+02 1.575000e+02 1.575000e+02 3.440100e-06 1.239600e-07 8.070700e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d59-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d59-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.537000e-03 1.772834e-04 1.928197e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.842500e-03 5.819066e-05 6.263716e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.100200e-03 4.681870e-05 4.496857e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.439500e-03 3.619757e-05 3.539646e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.804900e-04 3.805045e-05 3.593377e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.920500e-04 2.436671e-05 2.348867e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.580400e-04 2.311139e-05 2.131238e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.181200e-04 1.862461e-05 1.782577e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.072200e-04 1.402972e-05 1.300234e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.314800e-04 1.340325e-05 1.854704e-05
+1.750000e+03 2.500000e+02 2.500000e+02 6.295500e-05 4.854287e-06 5.491534e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.318200e-05 1.855430e-06 1.959019e-06
+3.350000e+03 6.500000e+02 6.500000e+02 1.905100e-06 4.335459e-07 4.003406e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d59-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d59-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.533800e-03 1.215600e-04 4.578800e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.756100e-03 3.323400e-05 5.062300e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.989200e-03 2.576500e-05 3.384400e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.406900e-03 3.537000e-05 2.042900e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.691000e-04 1.650300e-05 2.582800e-05
+9.325000e+02 5.250000e+01 5.250000e+01 6.846800e-04 1.385600e-05 1.406400e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.702000e-04 1.044800e-05 1.888800e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.399900e-04 1.008700e-05 1.781500e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.346200e-04 7.144400e-06 1.023400e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.522100e-04 9.169600e-06 6.431700e-06
+1.750000e+03 2.500000e+02 2.500000e+02 7.137600e-05 2.767100e-06 3.571900e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.879700e-05 9.967600e-07 1.349200e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.609100e-06 2.379600e-07 3.590000e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d59-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d59-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.539200e-03 6.898200e-05 6.014000e-05
+5.800000e+02 3.500000e+01 3.500000e+01 2.783400e-03 3.631500e-05 3.130500e-05
+6.550000e+02 4.000000e+01 4.000000e+01 2.006100e-03 1.177600e-05 9.872800e-06
+7.400000e+02 4.500000e+01 4.500000e+01 1.435800e-03 3.024900e-06 3.135100e-06
+8.325000e+02 4.750000e+01 4.750000e+01 9.792100e-04 7.903700e-06 8.899900e-06
+9.325000e+02 5.250000e+01 5.250000e+01 6.869200e-04 9.667500e-06 1.106500e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.674200e-04 9.532000e-06 1.099600e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.273300e-04 8.618600e-06 1.000300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.252300e-04 7.246900e-06 8.468800e-06
+1.425000e+03 7.500000e+01 7.500000e+01 1.467300e-04 5.775100e-06 6.802900e-06
+1.750000e+03 2.500000e+02 2.500000e+02 6.747300e-05 3.424100e-06 4.077800e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.723200e-05 1.260300e-06 1.537800e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.278500e-06 2.334000e-07 2.946500e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d59-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d59-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t59
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 3.384800e-03 9.748300e-05 1.598600e-04
+5.800000e+02 3.500000e+01 3.500000e+01 2.659700e-03 3.182600e-05 1.973900e-05
+6.550000e+02 4.000000e+01 4.000000e+01 1.945600e-03 3.306300e-05 1.792100e-05
+7.400000e+02 4.500000e+01 4.500000e+01 1.396700e-03 6.561700e-06 7.235800e-05
+8.325000e+02 4.750000e+01 4.750000e+01 9.959700e-04 2.656700e-05 1.527800e-07
+9.325000e+02 5.250000e+01 5.250000e+01 7.087700e-04 1.702200e-05 2.733000e-05
+1.042500e+03 5.750000e+01 5.750000e+01 4.918100e-04 1.358900e-05 1.068100e-05
+1.150000e+03 5.000000e+01 5.000000e+01 3.509700e-04 5.620100e-06 1.291000e-05
+1.275000e+03 7.500000e+01 7.500000e+01 2.494600e-04 6.587100e-06 1.179700e-05
+1.425000e+03 7.500000e+01 7.500000e+01 1.696500e-04 1.542400e-05 0.000000e+00
+1.750000e+03 2.500000e+02 2.500000e+02 7.781200e-05 3.638800e-06 3.344700e-06
+2.350000e+03 3.500000e+02 3.500000e+02 2.016300e-05 2.480400e-06 1.220400e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.753200e-06 1.980800e-07 3.293400e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d60-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d60-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.710100e-03 1.829325e-04 1.857785e-04
+3.750000e+01 1.250000e+01 1.250000e+01 9.054400e-03 2.892417e-04 3.263673e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.914000e-03 1.567079e-04 1.543139e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.474500e-03 1.418444e-04 1.354520e-04
+1.150000e+02 1.500000e+01 1.500000e+01 3.614600e-03 1.939892e-04 1.822575e-04
+1.450000e+02 1.500000e+01 1.500000e+01 2.724300e-03 2.153469e-04 1.885156e-04
+1.750000e+02 1.500000e+01 1.500000e+01 1.628400e-03 1.053646e-04 1.011315e-04
+2.250000e+02 3.500000e+01 3.500000e+01 7.742300e-04 4.996039e-05 4.853135e-05
+3.250000e+02 6.500000e+01 6.500000e+01 1.788300e-04 1.661312e-05 1.753925e-05
+6.450000e+02 2.550000e+02 2.550000e+02 9.241300e-06 1.971697e-06 2.104979e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d60-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d60-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.882600e-03 2.072200e-04 6.438900e-05
+3.750000e+01 1.250000e+01 1.250000e+01 8.113600e-03 9.308000e-05 1.482900e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.476800e-03 8.935300e-05 1.161800e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.746600e-03 8.291700e-05 8.773200e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.093600e-03 6.117200e-05 6.436300e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.861200e-03 6.286400e-05 5.337000e-05
+1.750000e+02 1.500000e+01 1.500000e+01 1.895500e-03 4.107000e-05 5.535600e-05
+2.250000e+02 3.500000e+01 3.500000e+01 9.315100e-04 2.289500e-05 2.045200e-05
+3.250000e+02 6.500000e+01 6.500000e+01 2.422800e-04 7.179100e-06 9.367200e-06
+6.450000e+02 2.550000e+02 2.550000e+02 1.430800e-05 1.253200e-06 1.034600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d60-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d60-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.989000e-03 1.416000e-04 1.227700e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.896200e-03 1.508700e-04 1.308100e-04
+6.250000e+01 1.250000e+01 1.250000e+01 7.072600e-03 2.375100e-05 2.090600e-05
+8.750000e+01 1.250000e+01 1.250000e+01 5.584200e-03 2.727300e-05 3.133300e-05
+1.150000e+02 1.500000e+01 1.500000e+01 4.037200e-03 3.591300e-05 4.522400e-05
+1.450000e+02 1.500000e+01 1.500000e+01 2.875300e-03 3.753400e-05 4.502100e-05
+1.750000e+02 1.500000e+01 1.500000e+01 2.012700e-03 3.629500e-05 4.133300e-05
+2.250000e+02 3.500000e+01 3.500000e+01 1.016400e-03 2.015800e-05 2.279700e-05
+3.250000e+02 6.500000e+01 6.500000e+01 2.888100e-04 7.442300e-06 8.013600e-06
+6.450000e+02 2.550000e+02 2.550000e+02 1.960600e-05 7.823300e-07 8.430800e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d60-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d60-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t60
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.858600e-03 1.083200e-04 2.436400e-04
+3.750000e+01 1.250000e+01 1.250000e+01 8.188400e-03 2.454600e-04 9.662900e-05
+6.250000e+01 1.250000e+01 1.250000e+01 7.534300e-03 0.000000e+00 3.665000e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.742500e-03 0.000000e+00 1.257700e-04
+1.150000e+02 1.500000e+01 1.500000e+01 4.056400e-03 8.830300e-05 0.000000e+00
+1.450000e+02 1.500000e+01 1.500000e+01 2.795200e-03 1.041800e-04 0.000000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 1.864000e-03 1.437800e-05 6.655600e-05
+2.250000e+02 3.500000e+01 3.500000e+01 9.169000e-04 5.235800e-05 0.000000e+00
+3.250000e+02 6.500000e+01 6.500000e+01 2.462900e-04 9.787600e-06 1.423500e-05
+6.450000e+02 2.550000e+02 2.550000e+02 1.811500e-05 2.899300e-06 2.472100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d61-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d61-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.017800e-01 1.362437e-02 1.440183e-02
+3.500000e-01 5.000000e-02 5.000000e-02 1.427300e-01 1.755702e-02 1.844077e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.347600e-01 1.911047e-02 1.769351e-02
+5.500000e-01 5.000000e-02 5.000000e-02 3.735000e-01 2.875614e-02 3.109851e-02
+6.500000e-01 5.000000e-02 5.000000e-02 6.200100e-01 5.213860e-02 4.875594e-02
+7.250000e-01 2.500000e-02 2.500000e-02 8.685600e-01 7.355007e-02 7.419387e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.398000e+00 5.384091e-02 5.125492e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.083100e+00 6.703512e-02 6.473012e-02
+8.750000e-01 2.500000e-02 2.500000e-02 3.013100e+00 7.244860e-02 6.892062e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.060300e+00 9.637095e-02 8.811582e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.224200e+00 1.368201e-01 1.611396e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d61-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d61-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.371300e-01 3.655300e-03 5.286600e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.934500e-01 9.496500e-03 1.204600e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.638600e-01 1.280300e-02 1.126500e-02
+5.500000e-01 5.000000e-02 5.000000e-02 3.928200e-01 1.118000e-02 1.290200e-02
+6.500000e-01 5.000000e-02 5.000000e-02 6.729900e-01 1.496600e-02 1.636600e-02
+7.250000e-01 2.500000e-02 2.500000e-02 1.047300e+00 2.364600e-02 4.420900e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.465400e+00 3.685200e-02 2.797100e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.030300e+00 3.630900e-02 3.610200e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.848100e+00 4.791700e-02 5.670700e-02
+9.250000e-01 2.500000e-02 2.500000e-02 3.857800e+00 4.582700e-02 5.787900e-02
+9.750000e-01 2.500000e-02 2.500000e-02 4.882100e+00 1.135100e-01 5.105400e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d61-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d61-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.385600e-01 2.832700e-03 3.549500e-03
+3.500000e-01 5.000000e-02 5.000000e-02 1.891400e-01 3.405400e-03 4.012300e-03
+4.500000e-01 5.000000e-02 5.000000e-02 2.536300e-01 3.773200e-03 4.445900e-03
+5.500000e-01 5.000000e-02 5.000000e-02 3.886500e-01 7.634400e-03 8.697300e-03
+6.500000e-01 5.000000e-02 5.000000e-02 6.374100e-01 9.694900e-03 1.192600e-02
+7.250000e-01 2.500000e-02 2.500000e-02 9.975600e-01 1.289300e-02 1.470800e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.383900e+00 1.481100e-02 1.762000e-02
+8.250000e-01 2.500000e-02 2.500000e-02 1.968000e+00 1.820200e-02 2.027300e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.790700e+00 7.981000e-03 8.883600e-03
+9.250000e-01 2.500000e-02 2.500000e-02 3.963400e+00 3.363300e-02 2.808100e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.127400e+00 1.046700e-01 8.970500e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d61-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d61-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t61
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 1.280000e-01 5.879600e-03 0.000000e+00
+3.500000e-01 5.000000e-02 5.000000e-02 1.700600e-01 3.540400e-03 3.672300e-02
+4.500000e-01 5.000000e-02 5.000000e-02 2.384500e-01 1.108900e-02 0.000000e+00
+5.500000e-01 5.000000e-02 5.000000e-02 3.580800e-01 1.351400e-02 0.000000e+00
+6.500000e-01 5.000000e-02 5.000000e-02 6.284800e-01 2.671300e-02 2.228500e-03
+7.250000e-01 2.500000e-02 2.500000e-02 9.671500e-01 1.578700e-02 2.034000e-02
+7.750000e-01 2.500000e-02 2.500000e-02 1.403500e+00 4.781600e-02 2.510000e-02
+8.250000e-01 2.500000e-02 2.500000e-02 2.032200e+00 4.323700e-02 2.043100e-02
+8.750000e-01 2.500000e-02 2.500000e-02 2.909300e+00 2.071200e-02 2.903900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.029500e+00 3.946400e-02 1.379900e-02
+9.750000e-01 2.500000e-02 2.500000e-02 5.100200e+00 0.000000e+00 1.294000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d62-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d62-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.324300e-01 1.120437e-02 1.026632e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.150300e-01 1.282128e-02 1.150696e-02
+3.000000e+00 2.000000e-01 2.000000e-01 3.809700e-01 1.159701e-02 1.186194e-02
+3.400000e+00 2.000000e-01 2.000000e-01 4.491000e-01 1.234324e-02 1.235734e-02
+3.800000e+00 2.000000e-01 2.000000e-01 4.631300e-01 1.109745e-02 1.165524e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.971800e-01 1.001354e-02 9.212471e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.697900e-01 7.399613e-03 7.898935e-03
+5.000000e+00 2.000000e-01 2.000000e-01 9.728100e-02 6.190592e-03 6.496378e-03
+5.800000e+00 6.000000e-01 6.000000e-01 2.961300e-02 2.490982e-03 2.677298e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.042000e-03 4.840271e-04 4.915910e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d62-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d62-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.316900e-01 4.071400e-03 5.071400e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.044200e-01 4.826500e-03 6.135200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 3.928600e-01 1.515000e-02 5.120400e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.571300e-01 5.670200e-03 8.701500e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.437400e-01 6.822200e-03 5.903000e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.899600e-01 5.191900e-03 5.502000e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.742700e-01 3.686200e-03 7.415700e-03
+5.000000e+00 2.000000e-01 2.000000e-01 9.967300e-02 2.579100e-03 6.947600e-03
+5.800000e+00 6.000000e-01 6.000000e-01 3.278900e-02 1.044200e-03 8.575500e-04
+7.600000e+00 1.200000e+00 1.200000e+00 1.315800e-03 1.209800e-04 2.074000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d62-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d62-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.968300e-01 4.204600e-03 4.415700e-03
+2.600000e+00 2.000000e-01 2.000000e-01 3.559000e-01 3.120500e-03 3.212200e-03
+3.000000e+00 2.000000e-01 2.000000e-01 4.123100e-01 2.298300e-03 2.030600e-03
+3.400000e+00 2.000000e-01 2.000000e-01 4.446600e-01 1.859900e-03 1.555500e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.036900e-01 2.640600e-03 2.612600e-03
+4.200000e+00 2.000000e-01 2.000000e-01 2.596200e-01 3.111700e-03 2.801400e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.533400e-01 3.039000e-03 3.531600e-03
+5.000000e+00 2.000000e-01 2.000000e-01 8.557900e-02 2.688400e-03 3.167800e-03
+5.800000e+00 6.000000e-01 6.000000e-01 2.714300e-02 1.375300e-03 1.659500e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.107700e-03 1.066400e-04 1.356900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d62-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d62-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t62
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.529600e-01 4.795900e-03 1.912800e-02
+2.600000e+00 2.000000e-01 2.000000e-01 3.264300e-01 9.110500e-03 1.435600e-02
+3.000000e+00 2.000000e-01 2.000000e-01 4.013700e-01 5.643400e-03 0.000000e+00
+3.400000e+00 2.000000e-01 2.000000e-01 4.556500e-01 7.727700e-03 2.058700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 4.190200e-01 3.059300e-03 7.213500e-04
+4.200000e+00 2.000000e-01 2.000000e-01 2.734900e-01 3.752200e-03 1.902400e-03
+4.600000e+00 2.000000e-01 2.000000e-01 1.653700e-01 4.197100e-03 0.000000e+00
+5.000000e+00 2.000000e-01 2.000000e-01 9.715800e-02 4.634600e-03 1.335200e-02
+5.800000e+00 6.000000e-01 6.000000e-01 3.299600e-02 2.767600e-03 1.251500e-03
+7.600000e+00 1.200000e+00 1.200000e+00 1.593800e-03 1.666000e-04 3.756000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d63-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d63-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 8.597000e-03 6.410279e-04 7.175628e-04
+1.050000e+02 1.000000e+01 1.000000e+01 8.682700e-03 3.006712e-04 3.650035e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.505700e-03 1.505876e-04 1.412089e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.857900e-03 1.808055e-04 1.727831e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.520500e-03 2.010371e-04 1.924766e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.195100e-03 1.721878e-04 1.558201e-04
+2.350000e+02 1.500000e+01 1.500000e+01 1.920200e-03 1.300336e-04 1.208145e-04
+2.650000e+02 1.500000e+01 1.500000e+01 1.142300e-03 1.115987e-04 1.085334e-04
+2.975000e+02 1.750000e+01 1.750000e+01 7.322200e-04 5.104252e-05 4.414265e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.056900e-04 2.982988e-05 3.087551e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.586600e-04 2.005086e-05 2.087936e-05
+4.350000e+02 4.500000e+01 4.500000e+01 9.667700e-05 1.040879e-05 1.008464e-05
+5.825000e+02 1.025000e+02 1.025000e+02 1.798100e-05 2.827337e-06 2.992954e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d63-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d63-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 7.389600e-03 1.191700e-04 3.547100e-04
+1.050000e+02 1.000000e+01 1.000000e+01 8.170500e-03 3.343000e-04 1.044600e-04
+1.275000e+02 1.250000e+01 1.250000e+01 7.376900e-03 8.894200e-05 1.317500e-04
+1.525000e+02 1.250000e+01 1.250000e+01 6.113700e-03 1.156400e-04 9.133100e-05
+1.775000e+02 1.250000e+01 1.250000e+01 4.718100e-03 7.099900e-05 1.090500e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.309400e-03 7.084500e-05 7.433000e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.091000e-03 6.414900e-05 4.732200e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.293500e-03 3.488000e-05 4.962200e-05
+2.975000e+02 1.750000e+01 1.750000e+01 7.833800e-04 2.595500e-05 3.265200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 4.624000e-04 2.169000e-05 2.394600e-05
+3.700000e+02 2.000000e+01 2.000000e+01 2.679800e-04 1.427900e-05 1.892700e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.192800e-04 7.325000e-06 6.514400e-06
+5.825000e+02 1.025000e+02 1.025000e+02 2.271200e-05 2.598000e-06 2.056800e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d63-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d63-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.165900e-03 7.892800e-05 7.739500e-05
+1.050000e+02 1.000000e+01 1.000000e+01 7.036200e-03 6.513100e-05 6.530800e-05
+1.275000e+02 1.250000e+01 1.250000e+01 6.867400e-03 4.194900e-05 3.719800e-05
+1.525000e+02 1.250000e+01 1.250000e+01 6.090300e-03 2.789300e-05 2.275700e-05
+1.775000e+02 1.250000e+01 1.250000e+01 5.079500e-03 1.978800e-05 1.763600e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.649000e-03 2.084000e-05 2.343300e-05
+2.350000e+02 1.500000e+01 1.500000e+01 2.413600e-03 2.156800e-05 2.305400e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.540300e-03 2.114100e-05 2.317100e-05
+2.975000e+02 1.750000e+01 1.750000e+01 9.495100e-04 1.876800e-05 2.042200e-05
+3.325000e+02 1.750000e+01 1.750000e+01 5.796700e-04 1.327900e-05 1.454900e-05
+3.700000e+02 2.000000e+01 2.000000e+01 3.477200e-04 9.107700e-06 9.782700e-06
+4.350000e+02 4.500000e+01 4.500000e+01 1.546500e-04 5.233400e-06 5.679300e-06
+5.825000e+02 1.025000e+02 1.025000e+02 3.130300e-05 1.315300e-06 1.441600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d63-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d63-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t63
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.757100e-03 1.194100e-04 4.071500e-04
+1.050000e+02 1.000000e+01 1.000000e+01 7.433100e-03 1.479200e-04 2.407800e-05
+1.275000e+02 1.250000e+01 1.250000e+01 7.108400e-03 2.144300e-04 0.000000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 6.223700e-03 4.743400e-05 1.252000e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.883600e-03 3.559500e-05 6.937000e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.498200e-03 1.475300e-05 2.303600e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.191500e-03 2.483800e-05 5.854400e-05
+2.650000e+02 1.500000e+01 1.500000e+01 1.422400e-03 3.732900e-05 0.000000e+00
+2.975000e+02 1.750000e+01 1.750000e+01 8.711000e-04 4.319900e-05 8.767100e-07
+3.325000e+02 1.750000e+01 1.750000e+01 5.452100e-04 3.923000e-05 0.000000e+00
+3.700000e+02 2.000000e+01 2.000000e+01 3.155800e-04 1.819000e-05 1.109400e-05
+4.350000e+02 4.500000e+01 4.500000e+01 1.418900e-04 6.965100e-06 1.774200e-05
+5.825000e+02 1.025000e+02 1.025000e+02 3.056500e-05 9.495800e-07 4.727500e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d64-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d64-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t64
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 2.674200e-01 4.491341e-02 4.525471e-02
+7.500000e+01 2.500000e+01 2.500000e+01 3.724900e-01 3.939895e-02 4.703968e-02
+1.300000e+02 3.000000e+01 3.000000e+01 2.079700e-01 2.739788e-02 2.350885e-02
+1.925000e+02 3.250000e+01 3.250000e+01 1.115800e-01 1.430191e-02 1.462209e-02
+2.625000e+02 3.750000e+01 3.750000e+01 4.700200e-02 1.992072e-02 1.996867e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.250300e-03 3.774957e-02 3.774449e-02
+6.975000e+02 2.025000e+02 2.025000e+02 5.458600e-04 4.095326e-04 4.107797e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d64-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d64-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t64
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 2.239700e-01 2.728900e-02 2.080900e-02
+7.500000e+01 2.500000e+01 2.500000e+01 3.054800e-01 3.943000e-02 3.231700e-02
+1.300000e+02 3.000000e+01 3.000000e+01 2.047900e-01 2.164900e-02 2.386800e-02
+1.925000e+02 3.250000e+01 3.250000e+01 1.108700e-01 1.228700e-02 1.570400e-02
+2.625000e+02 3.750000e+01 3.750000e+01 5.003400e-02 5.052900e-03 4.460700e-03
+3.975000e+02 9.750000e+01 9.750000e+01 1.366100e-02 1.616400e-03 1.518500e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.095800e-03 2.037400e-04 2.103500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d64-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d64-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t64
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 3.071800e-01 5.188900e-02 8.759200e-02
+7.500000e+01 2.500000e+01 2.500000e+01 4.018000e-01 6.570600e-02 1.603900e-01
+1.300000e+02 3.000000e+01 3.000000e+01 2.567100e-01 5.092800e-02 1.023200e-01
+1.925000e+02 3.250000e+01 3.250000e+01 1.344300e-01 2.596600e-02 7.378000e-02
+2.625000e+02 3.750000e+01 3.750000e+01 6.309800e-02 1.273100e-02 2.078300e-02
+3.975000e+02 9.750000e+01 9.750000e+01 1.795700e-02 4.193500e-03 5.390200e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.657600e-03 3.662100e-04 7.480000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d65-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d65-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t65
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 5.520100e+00 2.510942e+00 2.559797e+00
+6.000000e-01 1.000000e-01 1.000000e-01 2.698000e+01 4.953234e+00 5.259319e+00
+7.500000e-01 5.000000e-02 5.000000e-02 6.827800e+01 8.337523e+00 8.039806e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.271800e+02 1.647799e+01 1.591515e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.474300e+02 2.868073e+01 2.765007e+01
+9.750000e-01 2.500000e-02 2.500000e-02 3.307400e+02 2.781169e+01 2.893715e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d65-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d65-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t65
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 8.402700e+00 8.305200e-01 1.209400e+00
+6.000000e-01 1.000000e-01 1.000000e-01 2.572900e+01 2.931400e+00 4.718800e+00
+7.500000e-01 5.000000e-02 5.000000e-02 6.382600e+01 7.372200e+00 7.963400e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.239000e+02 1.470500e+01 1.391600e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.118700e+02 2.422000e+01 1.813300e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.825800e+02 3.478400e+01 2.253000e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d65-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d65-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t65
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 2.500000e-01 2.500000e-01 9.150600e+00 1.864200e+00 4.995100e+00
+6.000000e-01 1.000000e-01 1.000000e-01 2.836600e+01 6.116800e+00 1.033800e+01
+7.500000e-01 5.000000e-02 5.000000e-02 7.319900e+01 1.231600e+01 2.342400e+01
+8.500000e-01 5.000000e-02 5.000000e-02 1.580600e+02 2.766900e+01 6.570400e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.906900e+02 5.783000e+01 1.037100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 4.125600e+02 6.495900e+01 1.526100e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d66-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d66-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t66
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 5.239400e+00 5.621497e-01 5.416009e-01
+3.200000e+00 4.000000e-01 4.000000e-01 6.939200e+00 6.535603e-01 6.334484e-01
+4.000000e+00 4.000000e-01 4.000000e-01 1.318100e+01 1.157089e+00 1.069418e+00
+4.800000e+00 4.000000e-01 4.000000e-01 1.590400e+01 2.170391e+00 2.123716e+00
+5.600000e+00 4.000000e-01 4.000000e-01 2.040800e+01 2.625320e+00 3.189703e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.417900e+00 7.354390e-01 6.604592e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d66-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d66-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t66
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 4.555800e+00 5.744500e-01 5.165200e-01
+3.200000e+00 4.000000e-01 4.000000e-01 7.398600e+00 8.278200e-01 7.556400e-01
+4.000000e+00 4.000000e-01 4.000000e-01 1.144800e+01 1.197700e+00 1.233200e+00
+4.800000e+00 4.000000e-01 4.000000e-01 1.673600e+01 1.722100e+00 1.402400e+00
+5.600000e+00 4.000000e-01 4.000000e-01 1.807600e+01 2.023900e+00 2.263500e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.239400e+00 3.862600e-01 2.853700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d66-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d66-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t66
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 7.473100e+00 1.529300e+00 3.883900e+00
+3.200000e+00 4.000000e-01 4.000000e-01 1.192400e+01 2.392800e+00 3.974200e+00
+4.000000e+00 4.000000e-01 4.000000e-01 1.586000e+01 2.853400e+00 6.805400e+00
+4.800000e+00 4.000000e-01 4.000000e-01 2.027500e+01 3.681400e+00 7.261200e+00
+5.600000e+00 4.000000e-01 4.000000e-01 1.987400e+01 3.369800e+00 8.794800e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.933100e+00 5.047500e-01 6.107300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d67-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d67-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t67
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.903900e-01 7.502811e-02 8.013669e-02
+1.400000e+02 2.500000e+01 2.500000e+01 2.750100e-01 3.924753e-02 3.612656e-02
+1.925000e+02 2.750000e+01 2.750000e+01 1.833000e-01 1.943026e-02 2.300746e-02
+2.500000e+02 3.000000e+01 3.000000e+01 1.195700e-01 1.460465e-02 1.214861e-02
+3.150000e+02 3.500000e+01 3.500000e+01 6.816600e-02 1.704474e-02 1.669931e-02
+3.925000e+02 4.250000e+01 4.250000e+01 5.076100e-02 5.870752e-03 5.757623e-03
+5.075000e+02 7.250000e+01 7.250000e+01 2.749000e-02 3.412071e-03 3.229625e-03
+7.300000e+02 1.500000e+02 1.500000e+02 4.916500e-03 1.154162e-03 1.147772e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d67-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d67-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t67
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.275100e-01 3.310400e-02 4.021500e-02
+1.400000e+02 2.500000e+01 2.500000e+01 2.408100e-01 2.843500e-02 2.583700e-02
+1.925000e+02 2.750000e+01 2.750000e+01 1.816100e-01 2.001200e-02 1.553200e-02
+2.500000e+02 3.000000e+01 3.000000e+01 1.230200e-01 1.478200e-02 1.009200e-02
+3.150000e+02 3.500000e+01 3.500000e+01 8.085000e-02 7.994600e-03 8.493600e-03
+3.925000e+02 4.250000e+01 4.250000e+01 4.941800e-02 5.306900e-03 5.850600e-03
+5.075000e+02 7.250000e+01 7.250000e+01 2.702300e-02 2.931100e-03 3.213800e-03
+7.300000e+02 1.500000e+02 1.500000e+02 5.320900e-03 8.264500e-04 5.590800e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d67-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d67-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t67
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.923200e-01 4.814700e-02 9.105100e-02
+1.400000e+02 2.500000e+01 2.500000e+01 2.665100e-01 4.240900e-02 1.054600e-01
+1.925000e+02 2.750000e+01 2.750000e+01 2.205000e-01 4.364300e-02 8.326400e-02
+2.500000e+02 3.000000e+01 3.000000e+01 1.570400e-01 3.138500e-02 5.388200e-02
+3.150000e+02 3.500000e+01 3.500000e+01 1.132200e-01 2.396300e-02 5.003700e-02
+3.925000e+02 4.250000e+01 4.250000e+01 7.425500e-02 1.452500e-02 2.641600e-02
+5.075000e+02 7.250000e+01 7.250000e+01 4.370800e-02 9.631300e-03 1.718500e-02
+7.300000e+02 1.500000e+02 1.500000e+02 9.033100e-03 1.487100e-03 6.215500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d68-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d68-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t68
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 9.950900e+01 1.942476e+01 1.854141e+01
+2.500000e-01 1.000000e-01 1.000000e-01 8.070900e+01 1.408074e+01 1.343267e+01
+5.000000e-01 1.500000e-01 1.500000e-01 5.441500e+01 1.029418e+01 1.044141e+01
+8.250000e-01 1.750000e-01 1.750000e-01 9.741800e+00 1.900542e+00 1.972275e+00
+1.500000e+00 5.000000e-01 5.000000e-01 6.006700e-01 2.042429e-01 2.014581e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d68-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d68-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t68
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 7.690900e+01 1.619700e+01 8.542800e+00
+2.500000e-01 1.000000e-01 1.000000e-01 7.096900e+01 1.318800e+01 1.102600e+01
+5.000000e-01 1.500000e-01 1.500000e-01 4.342600e+01 4.416600e+00 6.735800e+00
+8.250000e-01 1.750000e-01 1.750000e-01 9.053000e+00 1.338500e+00 9.468000e-01
+1.500000e+00 5.000000e-01 5.000000e-01 5.568000e-01 1.107200e-01 9.573200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d68-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d68-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t68
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.108800e+02 2.293100e+01 5.061700e+01
+2.500000e-01 1.000000e-01 1.000000e-01 1.004700e+02 1.689300e+01 4.855200e+01
+5.000000e-01 1.500000e-01 1.500000e-01 6.479800e+01 1.333100e+01 2.844800e+01
+8.250000e-01 1.750000e-01 1.750000e-01 1.434400e+01 3.951300e+00 5.709500e+00
+1.500000e+00 5.000000e-01 5.000000e-01 9.877500e-01 2.295100e-01 5.180400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d69-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d69-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t69
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 9.167600e+01 8.744966e+00 9.993516e+00
+3.000000e-01 1.000000e-01 1.000000e-01 1.033500e+02 1.315957e+01 1.305025e+01
+4.750000e-01 7.500000e-02 7.500000e-02 6.467700e+01 1.181920e+01 1.180156e+01
+6.750000e-01 1.250000e-01 1.250000e-01 2.499700e+01 3.321205e+00 2.895415e+00
+9.000000e-01 1.000000e-01 1.000000e-01 4.704700e+00 9.374202e-01 9.543161e-01
+1.100000e+00 1.000000e-01 1.000000e-01 1.372800e+00 5.085533e-01 5.090083e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d69-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d69-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t69
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 8.662100e+01 6.075200e+00 7.395600e+00
+3.000000e-01 1.000000e-01 1.000000e-01 9.681400e+01 1.297600e+01 1.040300e+01
+4.750000e-01 7.500000e-02 7.500000e-02 6.644700e+01 9.621600e+00 6.649700e+00
+6.750000e-01 1.250000e-01 1.250000e-01 2.061600e+01 2.597700e+00 3.408100e+00
+9.000000e-01 1.000000e-01 1.000000e-01 3.882400e+00 7.499600e-01 8.866100e-01
+1.100000e+00 1.000000e-01 1.000000e-01 9.913800e-01 2.754400e-01 3.793300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d69-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d69-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t69
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.005500e+02 1.355700e+01 2.667400e+01
+3.000000e-01 1.000000e-01 1.000000e-01 1.171000e+02 2.349900e+01 4.233100e+01
+4.750000e-01 7.500000e-02 7.500000e-02 9.886900e+01 1.943700e+01 5.203700e+01
+6.750000e-01 1.250000e-01 1.250000e-01 3.361800e+01 6.727700e+00 1.553500e+01
+9.000000e-01 1.000000e-01 1.000000e-01 6.780200e+00 2.126500e+00 2.802800e+00
+1.100000e+00 1.000000e-01 1.000000e-01 1.623900e+00 3.248900e-01 1.118000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d70-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d70-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t70
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 3.074200e+01 2.901229e+00 3.069764e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.495500e+01 2.066467e+00 2.003503e+00
+2.000000e+00 5.000000e-01 5.000000e-01 6.357000e+00 1.046056e+00 1.122947e+00
+3.000000e+00 5.000000e-01 5.000000e-01 2.886000e+00 7.992817e-01 6.571748e-01
+6.000000e+00 2.500000e+00 2.500000e+00 1.435200e+00 5.450652e-01 4.914309e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d70-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d70-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t70
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 3.019200e+01 2.376700e+00 2.457800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.405400e+01 2.142600e+00 1.756100e+00
+2.000000e+00 5.000000e-01 5.000000e-01 5.752600e+00 7.362300e-01 9.443400e-01
+3.000000e+00 5.000000e-01 5.000000e-01 2.054200e+00 6.968700e-01 2.687600e-01
+6.000000e+00 2.500000e+00 2.500000e+00 7.883900e-01 1.387900e-01 2.023900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d70-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d70-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t70
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 3.645800e+01 6.348600e+00 1.145400e+01
+1.000000e+00 5.000000e-01 5.000000e-01 1.976500e+01 3.454400e+00 8.995000e+00
+2.000000e+00 5.000000e-01 5.000000e-01 8.546400e+00 2.081500e+00 4.554500e+00
+3.000000e+00 5.000000e-01 5.000000e-01 2.964600e+00 8.147700e-01 9.282500e-01
+6.000000e+00 2.500000e+00 2.500000e+00 8.032000e-01 1.145500e-01 3.909200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d71-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d71-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.415600e+00 1.986454e-01 2.133789e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.743300e+00 1.299251e-01 1.343406e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.179300e+00 7.270734e-02 7.321741e-02
+7.400000e+02 4.500000e+01 4.500000e+01 8.000100e-01 4.943582e-02 4.272418e-02
+8.325000e+02 4.750000e+01 4.750000e+01 5.315900e-01 3.537647e-02 4.513574e-02
+9.325000e+02 5.250000e+01 5.250000e+01 3.311600e-01 2.183101e-02 2.696344e-02
+1.042500e+03 5.750000e+01 5.750000e+01 2.021500e-01 2.018193e-02 1.723141e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.160100e-01 1.162131e-02 9.688182e-03
+1.275000e+03 7.500000e+01 7.500000e+01 7.343200e-02 7.372960e-03 6.168185e-03
+1.425000e+03 7.500000e+01 7.500000e+01 4.681700e-02 4.873837e-03 4.807159e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.410100e-02 2.775143e-03 2.904789e-03
+2.350000e+03 3.500000e+02 3.500000e+02 2.248900e-03 5.788196e-04 3.754865e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.085800e-04 5.300238e-05 5.091667e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d71-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d71-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.969200e+00 2.690900e-01 1.946600e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.470400e+00 1.817200e-01 1.657400e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.000900e+00 1.328000e-01 2.237600e-01
+7.400000e+02 4.500000e+01 4.500000e+01 6.636100e-01 1.062100e-01 7.794700e-02
+8.325000e+02 4.750000e+01 4.750000e+01 4.262500e-01 5.759400e-02 4.364300e-02
+9.325000e+02 5.250000e+01 5.250000e+01 2.739200e-01 3.568500e-02 3.587300e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.699400e-01 2.336700e-02 1.684900e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.086100e-01 1.400600e-02 1.659000e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.666000e-02 9.762500e-03 8.835900e-03
+1.425000e+03 7.500000e+01 7.500000e+01 3.859200e-02 5.034200e-03 4.425600e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.347800e-02 1.539800e-03 1.919000e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.976100e-03 2.840300e-04 2.513800e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.089900e-04 3.707200e-05 3.430300e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d71-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d71-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 2.056200e+00 4.627500e-01 6.714700e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.552700e+00 3.593300e-01 5.301400e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.057800e+00 2.419800e-01 3.546300e-01
+7.400000e+02 4.500000e+01 4.500000e+01 7.049000e-01 1.626500e-01 2.394000e-01
+8.325000e+02 4.750000e+01 4.750000e+01 4.634900e-01 1.088200e-01 1.622100e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.024700e-01 7.286500e-02 1.094500e-01
+1.042500e+03 5.750000e+01 5.750000e+01 1.893800e-01 4.552500e-02 6.812800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.230700e-01 2.992800e-02 4.511000e-02
+1.275000e+03 7.500000e+01 7.500000e+01 7.513800e-02 1.846900e-02 2.797300e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.677100e-02 1.236000e-02 1.962400e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.630500e-02 4.027900e-03 6.092800e-03
+2.350000e+03 3.500000e+02 3.500000e+02 2.306300e-03 6.167600e-04 9.615900e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.366400e-04 3.831500e-05 6.055100e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d71-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d71-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t71
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.975000e+00 3.615700e-01 8.545600e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.479800e+00 2.551400e-01 6.320200e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.041100e+00 1.671700e-01 4.564400e-01
+7.400000e+02 4.500000e+01 4.500000e+01 7.005600e-01 1.353200e-01 2.863100e-01
+8.325000e+02 4.750000e+01 4.750000e+01 4.886400e-01 1.314300e-01 1.449800e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.055600e-01 5.207500e-02 1.218400e-01
+1.042500e+03 5.750000e+01 5.750000e+01 1.990800e-01 4.164500e-02 7.744400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.344000e-01 3.122300e-02 4.936500e-02
+1.275000e+03 7.500000e+01 7.500000e+01 8.610500e-02 1.420100e-02 2.970300e-02
+1.425000e+03 7.500000e+01 7.500000e+01 5.010900e-02 8.459200e-03 1.657700e-02
+1.750000e+03 2.500000e+02 2.500000e+02 2.036100e-02 4.202000e-03 9.873600e-03
+2.350000e+03 3.500000e+02 3.500000e+02 3.309800e-03 7.252700e-04 1.386600e-03
+3.350000e+03 6.500000e+02 6.500000e+02 2.617200e-04 1.134100e-04 6.592500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d72-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d72-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.608800e+00 2.444261e-01 2.441014e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.994200e+00 4.615159e-01 4.827298e-01
+6.250000e+01 1.250000e+01 1.250000e+01 4.384900e+00 4.262507e-01 4.407255e-01
+8.750000e+01 1.250000e+01 1.250000e+01 3.205100e+00 2.156284e-01 2.213289e-01
+1.150000e+02 1.500000e+01 1.500000e+01 2.122700e+00 1.368441e-01 1.320994e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.312200e+00 1.052806e-01 9.578950e-02
+1.750000e+02 1.500000e+01 1.500000e+01 8.039800e-01 7.431028e-02 7.563143e-02
+2.075000e+02 1.750000e+01 1.750000e+01 4.799200e-01 5.407814e-02 5.051290e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.769900e-01 2.559383e-02 2.834501e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.585800e-01 2.203793e-02 2.026432e-02
+3.975000e+02 9.750000e+01 9.750000e+01 3.140300e-02 8.332853e-03 8.254493e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.882700e-03 7.983694e-04 8.074512e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d72-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d72-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.875900e+00 3.425300e-01 6.209600e-01
+3.750000e+01 1.250000e+01 1.250000e+01 3.912800e+00 4.769000e-01 4.861200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 3.553600e+00 4.906100e-01 3.903400e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.646200e+00 3.397200e-01 3.238300e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.804400e+00 2.422700e-01 2.159600e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.192600e+00 1.508800e-01 1.236300e-01
+1.750000e+02 1.500000e+01 1.500000e+01 7.785300e-01 1.011300e-01 6.947300e-02
+2.075000e+02 1.750000e+01 1.750000e+01 4.763700e-01 6.753400e-02 4.427900e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.801400e-01 2.907400e-02 2.482100e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.629500e-01 2.337900e-02 1.633500e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.244800e-02 5.189000e-03 2.135900e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.942800e-03 2.696000e-04 2.439500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d72-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d72-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.100100e+00 4.189000e-01 5.808200e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.063700e+00 8.731800e-01 1.251300e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.580000e+00 8.206600e-01 1.202300e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.766700e+00 6.605300e-01 9.814900e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.912000e+00 4.652000e-01 7.007300e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.354100e+00 3.498800e-01 5.411300e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.696100e-01 2.181600e-01 3.335600e-01
+2.075000e+02 1.750000e+01 1.750000e+01 5.394700e-01 1.356100e-01 2.055300e-01
+2.425000e+02 1.750000e+01 1.750000e+01 3.334100e-01 8.460600e-02 1.282600e-01
+2.800000e+02 2.000000e+01 2.000000e+01 1.971800e-01 5.055500e-02 7.684200e-02
+3.975000e+02 9.750000e+01 9.750000e+01 5.599800e-02 1.454600e-02 2.212400e-02
+6.975000e+02 2.025000e+02 2.025000e+02 2.896300e-03 7.754000e-04 1.183300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d72-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d72-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t72
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.982400e+00 2.688200e-01 7.563800e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.174400e+00 7.277300e-01 1.787700e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.835400e+00 8.292200e-01 1.533600e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.813400e+00 4.737500e-01 1.213200e+00
+1.150000e+02 1.500000e+01 1.500000e+01 1.915800e+00 3.763300e-01 8.659100e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.342800e+00 3.293400e-01 4.489400e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.355200e-01 1.582400e-01 3.490300e-01
+2.075000e+02 1.750000e+01 1.750000e+01 4.972900e-01 1.147400e-01 2.066200e-01
+2.425000e+02 1.750000e+01 1.750000e+01 2.861000e-01 6.359200e-02 9.284700e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.641100e-01 2.400200e-02 5.206000e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.566900e-02 1.055200e-02 1.474900e-02
+6.975000e+02 2.025000e+02 2.025000e+02 2.507100e-03 6.248900e-04 1.155500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d73-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d73-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 3.259200e+01 9.394090e+00 8.680227e+00
+4.000000e-01 1.000000e-01 1.000000e-01 6.824900e+01 1.221602e+01 1.280593e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.239800e+02 2.442462e+01 2.432244e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.365000e+02 2.418363e+01 1.910719e+01
+6.750000e-01 2.500000e-02 2.500000e-02 3.164500e+02 2.460514e+01 2.709276e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.799300e+02 1.373115e+02 1.368762e+02
+7.750000e-01 2.500000e-02 2.500000e-02 7.852600e+02 5.284852e+01 6.030013e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.163000e+03 8.378977e+01 8.799065e+01
+8.750000e-01 2.500000e-02 2.500000e-02 1.677700e+03 1.275951e+02 1.307555e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.384500e+03 1.899326e+02 1.936158e+02
+9.750000e-01 2.500000e-02 2.500000e-02 3.212400e+03 2.530477e+02 2.558266e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d73-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d73-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.323200e+01 6.333200e+00 3.119600e+00
+4.000000e-01 1.000000e-01 1.000000e-01 7.526600e+01 8.462900e+00 9.371900e+00
+5.500000e-01 5.000000e-02 5.000000e-02 1.491400e+02 2.541700e+01 1.710200e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.209500e+02 3.509200e+01 3.085700e+01
+6.750000e-01 2.500000e-02 2.500000e-02 2.981400e+02 4.193200e+01 4.393500e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.373600e+02 6.749200e+01 4.075700e+01
+7.750000e-01 2.500000e-02 2.500000e-02 6.154700e+02 7.359400e+01 6.547700e+01
+8.250000e-01 2.500000e-02 2.500000e-02 9.116200e+02 1.179500e+02 1.052600e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.345500e+03 1.659300e+02 1.638400e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.915800e+03 2.433400e+02 2.181100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.497400e+03 3.612500e+02 4.226200e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d73-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d73-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.375000e+01 1.108600e+01 1.690900e+01
+4.000000e-01 1.000000e-01 1.000000e-01 7.793300e+01 2.018700e+01 3.206900e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.627100e+02 4.517800e+01 7.210600e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.114800e+02 5.235700e+01 7.913400e+01
+6.750000e-01 2.500000e-02 2.500000e-02 2.941100e+02 7.246200e+01 1.095000e+02
+7.250000e-01 2.500000e-02 2.500000e-02 4.201600e+02 1.029900e+02 1.551900e+02
+7.750000e-01 2.500000e-02 2.500000e-02 6.193300e+02 1.508500e+02 2.263500e+02
+8.250000e-01 2.500000e-02 2.500000e-02 9.222500e+02 2.210500e+02 3.297400e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.388700e+03 3.238100e+02 4.785500e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.082800e+03 4.691000e+02 6.836100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.909500e+03 6.339900e+02 9.081600e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d73-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d73-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t73
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.256000e+01 9.324700e+00 1.319500e+01
+4.000000e-01 1.000000e-01 1.000000e-01 7.237000e+01 1.535900e+01 3.025600e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.344900e+02 2.669700e+01 5.513000e+01
+6.250000e-01 2.500000e-02 2.500000e-02 2.184500e+02 4.520700e+01 7.154500e+01
+6.750000e-01 2.500000e-02 2.500000e-02 2.885200e+02 5.168800e+01 1.176500e+02
+7.250000e-01 2.500000e-02 2.500000e-02 4.222100e+02 7.557700e+01 1.845800e+02
+7.750000e-01 2.500000e-02 2.500000e-02 6.157100e+02 1.049400e+02 2.798900e+02
+8.250000e-01 2.500000e-02 2.500000e-02 9.800100e+02 2.083000e+02 4.000400e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.420400e+03 2.332200e+02 6.533500e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.145300e+03 4.553400e+02 8.358500e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.833700e+03 4.822200e+02 1.107600e+03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d74-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d74-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.091100e+02 1.402670e+01 1.367168e+01
+2.600000e+00 2.000000e-01 2.000000e-01 2.238300e+02 1.418280e+01 1.464034e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.508100e+02 1.570909e+01 1.630807e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.548900e+02 1.680456e+01 1.726047e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.085200e+02 1.648540e+01 1.729891e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.239900e+02 1.942287e+01 2.008674e+01
+4.800000e+00 4.000000e-01 4.000000e-01 3.985000e+01 4.397196e+00 4.895263e+00
+5.800000e+00 6.000000e-01 6.000000e-01 4.125500e+00 1.785458e+00 8.646571e-01
+7.600000e+00 1.200000e+00 1.200000e+00 4.605400e-02 3.548376e-02 3.060149e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d74-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d74-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.682500e+02 1.911100e+01 1.705200e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.877400e+02 2.302200e+01 1.780900e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.067500e+02 2.724000e+01 4.304200e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.127000e+02 2.959100e+01 2.353200e+01
+3.800000e+00 2.000000e-01 2.000000e-01 1.796200e+02 2.303400e+01 2.226300e+01
+4.200000e+00 2.000000e-01 2.000000e-01 9.933600e+01 1.952700e+01 1.126700e+01
+4.800000e+00 4.000000e-01 4.000000e-01 3.561800e+01 5.320800e+00 4.564200e+00
+5.800000e+00 6.000000e-01 6.000000e-01 3.964300e+00 3.798400e-01 9.810600e-01
+7.600000e+00 1.200000e+00 1.200000e+00 1.805700e-02 9.709000e-03 2.504800e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d74-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d74-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 2.290900e+02 5.415400e+01 7.983400e+01
+2.600000e+00 2.000000e-01 2.000000e-01 2.313500e+02 5.433300e+01 7.991700e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.257000e+02 5.194100e+01 7.631300e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.144600e+02 5.025900e+01 7.480700e+01
+3.800000e+00 2.000000e-01 2.000000e-01 1.629000e+02 3.641200e+01 5.317800e+01
+4.200000e+00 2.000000e-01 2.000000e-01 8.647600e+01 1.982200e+01 2.937800e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.884000e+01 6.717800e+00 1.018600e+01
+5.800000e+00 6.000000e-01 6.000000e-01 3.563700e+00 8.811000e-01 1.425800e+00
+7.600000e+00 1.200000e+00 1.200000e+00 2.293000e-02 5.544400e-03 8.364100e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d74-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d74-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t74
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.995700e+02 3.832400e+01 8.540200e+01
+2.600000e+00 2.000000e-01 2.000000e-01 2.161600e+02 3.189100e+01 9.208600e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.361000e+02 5.285900e+01 8.408300e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.223600e+02 3.994100e+01 9.154700e+01
+3.800000e+00 2.000000e-01 2.000000e-01 1.711300e+02 3.226800e+01 7.569300e+01
+4.200000e+00 2.000000e-01 2.000000e-01 9.087400e+01 1.709200e+01 3.585100e+01
+4.800000e+00 4.000000e-01 4.000000e-01 3.249900e+01 6.881100e+00 1.188200e+01
+5.800000e+00 6.000000e-01 6.000000e-01 5.201100e+00 8.860400e-01 2.234300e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.684500e-02 2.217500e-02 2.512900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d75-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d75-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.474600e+00 4.513922e-01 4.906002e-01
+1.050000e+02 1.000000e+01 1.000000e+01 3.817400e+00 3.467802e-01 3.619172e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.709900e+00 2.775314e-01 2.966466e-01
+1.525000e+02 1.250000e+01 1.250000e+01 3.426300e+00 2.473760e-01 2.188008e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.885500e+00 1.772587e-01 1.786117e-01
+2.050000e+02 1.500000e+01 1.500000e+01 2.037100e+00 1.139894e-01 1.159287e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.322600e+00 6.547812e-02 6.509956e-02
+2.650000e+02 1.500000e+01 1.500000e+01 8.300900e-01 4.913497e-02 4.526458e-02
+2.975000e+02 1.750000e+01 1.750000e+01 4.733500e-01 2.818240e-02 3.180290e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.416800e-01 3.326100e-02 3.264959e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.601200e-01 1.262026e-02 1.280743e-02
+4.125000e+02 2.250000e+01 2.250000e+01 8.138600e-02 9.159946e-03 8.966827e-03
+4.575000e+02 2.250000e+01 2.250000e+01 4.430500e-02 6.159585e-03 6.015320e-03
+5.300000e+02 5.000000e+01 5.000000e+01 1.427900e-02 3.023692e-03 2.966646e-03
+6.325000e+02 5.250000e+01 5.250000e+01 5.809600e-03 1.447559e-03 1.407017e-03
+8.425000e+02 1.575000e+02 1.575000e+02 3.192400e-04 2.349571e-04 2.265932e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d75-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d75-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 2.691600e+00 5.538800e-01 3.010300e-01
+1.050000e+02 1.000000e+01 1.000000e+01 3.128800e+00 4.155600e-01 3.963100e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.132300e+00 4.416500e-01 7.005100e-01
+1.525000e+02 1.250000e+01 1.250000e+01 2.879600e+00 3.603200e-01 3.115000e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.434100e+00 2.976700e-01 2.874300e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.741000e+00 2.273500e-01 1.783500e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.103800e+00 1.276600e-01 1.050200e-01
+2.650000e+02 1.500000e+01 1.500000e+01 6.818000e-01 8.567600e-02 5.664200e-02
+2.975000e+02 1.750000e+01 1.750000e+01 4.037900e-01 4.674100e-02 3.902800e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.326500e-01 3.004600e-02 1.663400e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.343400e-01 1.635600e-02 9.528000e-03
+4.125000e+02 2.250000e+01 2.250000e+01 7.385600e-02 8.839400e-03 8.698400e-03
+4.575000e+02 2.250000e+01 2.250000e+01 4.084200e-02 5.505900e-03 4.583800e-03
+5.300000e+02 5.000000e+01 5.000000e+01 1.595000e-02 1.828200e-03 1.577400e-03
+6.325000e+02 5.250000e+01 5.250000e+01 4.946100e-03 1.038100e-03 7.978700e-04
+8.425000e+02 1.575000e+02 1.575000e+02 7.036200e-04 1.671500e-04 1.736300e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d75-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d75-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 2.101300e+00 4.511200e-01 6.576400e-01
+1.050000e+02 1.000000e+01 1.000000e+01 2.663100e+00 5.794100e-01 8.389100e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.045100e+00 7.054600e-01 1.051600e+00
+1.525000e+02 1.250000e+01 1.250000e+01 2.977300e+00 6.763600e-01 9.886300e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.838300e+00 6.630100e-01 9.766500e-01
+2.050000e+02 1.500000e+01 1.500000e+01 2.074600e+00 4.874400e-01 7.207400e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.386000e+00 3.322000e-01 4.937400e-01
+2.650000e+02 1.500000e+01 1.500000e+01 8.986100e-01 2.172400e-01 3.231500e-01
+2.975000e+02 1.750000e+01 1.750000e+01 5.496300e-01 1.353700e-01 2.027900e-01
+3.325000e+02 1.750000e+01 1.750000e+01 3.368700e-01 8.370200e-02 1.255400e-01
+3.700000e+02 2.000000e+01 2.000000e+01 1.930200e-01 4.933400e-02 7.466400e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.106700e-01 2.851700e-02 4.324900e-02
+4.575000e+02 2.250000e+01 2.250000e+01 6.263200e-02 1.600400e-02 2.424700e-02
+5.300000e+02 5.000000e+01 5.000000e+01 2.554700e-02 6.756100e-03 1.032100e-02
+6.325000e+02 5.250000e+01 5.250000e+01 7.936300e-03 2.158200e-03 3.332400e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.160000e-03 3.214500e-04 4.988500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d75-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d75-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t75
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 2.188800e+00 3.477800e-01 8.848000e-01
+1.050000e+02 1.000000e+01 1.000000e+01 2.836800e+00 5.356900e-01 1.211800e+00
+1.275000e+02 1.250000e+01 1.250000e+01 3.196900e+00 5.550400e-01 1.406300e+00
+1.525000e+02 1.250000e+01 1.250000e+01 3.139700e+00 6.049600e-01 1.335500e+00
+1.775000e+02 1.250000e+01 1.250000e+01 2.796300e+00 5.255700e-01 9.938500e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.994500e+00 3.917300e-01 7.904300e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.332100e+00 3.259900e-01 4.493100e-01
+2.650000e+02 1.500000e+01 1.500000e+01 8.173100e-01 1.530200e-01 3.694800e-01
+2.975000e+02 1.750000e+01 1.750000e+01 4.812700e-01 5.977900e-02 2.580000e-01
+3.325000e+02 1.750000e+01 1.750000e+01 2.925800e-01 5.854100e-02 1.017000e-01
+3.700000e+02 2.000000e+01 2.000000e+01 1.759000e-01 3.122300e-02 6.793000e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.049600e-01 2.999000e-02 2.634900e-02
+4.575000e+02 2.250000e+01 2.250000e+01 5.317300e-02 8.767800e-03 2.365200e-02
+5.300000e+02 5.000000e+01 5.000000e+01 2.250300e-02 6.137300e-03 8.894600e-03
+6.325000e+02 5.250000e+01 5.250000e+01 7.633200e-03 7.187800e-04 4.316800e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.200700e-03 3.819800e-04 2.757200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d76-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d76-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t76
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.087800e-01 4.281009e-02 4.256285e-02
+3.750000e+01 1.250000e+01 1.250000e+01 7.984000e-01 8.448911e-02 8.972912e-02
+6.250000e+01 1.250000e+01 1.250000e+01 7.041700e-01 6.612812e-02 5.708515e-02
+8.750000e+01 1.250000e+01 1.250000e+01 5.321400e-01 4.150655e-02 4.281049e-02
+1.150000e+02 1.500000e+01 1.500000e+01 3.390600e-01 2.796040e-02 2.700158e-02
+1.450000e+02 1.500000e+01 1.500000e+01 2.771500e-01 2.555827e-02 3.259398e-02
+1.750000e+02 1.500000e+01 1.500000e+01 1.590200e-01 1.852536e-02 1.688511e-02
+2.250000e+02 3.500000e+01 3.500000e+01 9.247100e-02 1.755659e-02 1.700525e-02
+3.775000e+02 1.175000e+02 1.175000e+02 2.046100e-02 3.483494e-03 3.448098e-03
+6.975000e+02 2.025000e+02 2.025000e+02 9.135300e-04 5.418348e-04 5.435699e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d76-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d76-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t76
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.126900e-01 2.520400e-02 3.117500e-02
+3.750000e+01 1.250000e+01 1.250000e+01 6.423100e-01 5.055000e-02 7.936300e-02
+6.250000e+01 1.250000e+01 1.250000e+01 5.914100e-01 6.345500e-02 4.912000e-02
+8.750000e+01 1.250000e+01 1.250000e+01 4.830300e-01 4.930400e-02 4.401200e-02
+1.150000e+02 1.500000e+01 1.500000e+01 3.689000e-01 3.256400e-02 3.069500e-02
+1.450000e+02 1.500000e+01 1.500000e+01 2.651200e-01 3.069900e-02 1.247100e-02
+1.750000e+02 1.500000e+01 1.500000e+01 1.871300e-01 2.147500e-02 1.730200e-02
+2.250000e+02 3.500000e+01 3.500000e+01 1.053200e-01 1.055100e-02 1.023300e-02
+3.775000e+02 1.175000e+02 1.175000e+02 2.230600e-02 1.722400e-03 1.640200e-03
+6.975000e+02 2.025000e+02 2.025000e+02 1.581200e-03 2.373000e-04 2.266600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d76-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d76-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t76
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.397000e-01 2.514400e-02 1.266800e-01
+3.750000e+01 1.250000e+01 1.250000e+01 6.927500e-01 8.516200e-02 1.792200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 6.547100e-01 9.976400e-02 2.494900e-01
+8.750000e+01 1.250000e+01 1.250000e+01 5.305000e-01 9.168900e-02 1.674400e-01
+1.150000e+02 1.500000e+01 1.500000e+01 3.978900e-01 5.852800e-02 1.240000e-01
+1.450000e+02 1.500000e+01 1.500000e+01 2.915100e-01 5.425500e-02 7.554500e-02
+1.750000e+02 1.500000e+01 1.500000e+01 2.043500e-01 2.879900e-02 5.797500e-02
+2.250000e+02 3.500000e+01 3.500000e+01 1.184300e-01 2.824900e-02 2.431300e-02
+3.775000e+02 1.175000e+02 1.175000e+02 2.630300e-02 3.446000e-03 1.045700e-02
+6.975000e+02 2.025000e+02 2.025000e+02 2.006400e-03 3.923500e-04 8.622500e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d77-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d77-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t77
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 7.519900e+00 2.321114e+00 2.384740e+00
+5.000000e-01 1.000000e-01 1.000000e-01 2.679800e+01 4.691930e+00 4.498031e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.341600e+01 1.157207e+01 1.169160e+01
+7.500000e-01 5.000000e-02 5.000000e-02 1.171000e+02 1.120355e+01 1.013444e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.873600e+02 1.601033e+01 1.496033e+01
+8.750000e-01 2.500000e-02 2.500000e-02 3.043500e+02 2.868889e+01 2.886343e+01
+9.250000e-01 2.500000e-02 2.500000e-02 4.002600e+02 3.493286e+01 3.610713e+01
+9.750000e-01 2.500000e-02 2.500000e-02 5.295900e+02 4.400955e+01 4.310709e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d77-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d77-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t77
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.311200e+01 1.449400e+00 1.670800e+00
+5.000000e-01 1.000000e-01 1.000000e-01 2.636600e+01 3.089700e+00 2.952400e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.527100e+01 5.121500e+00 6.217600e+00
+7.500000e-01 5.000000e-02 5.000000e-02 1.047300e+02 1.156600e+01 7.577400e+00
+8.250000e-01 2.500000e-02 2.500000e-02 1.718800e+02 1.799500e+01 1.449400e+01
+8.750000e-01 2.500000e-02 2.500000e-02 2.480800e+02 2.195600e+01 1.937600e+01
+9.250000e-01 2.500000e-02 2.500000e-02 3.516200e+02 3.175100e+01 3.940000e+01
+9.750000e-01 2.500000e-02 2.500000e-02 4.682900e+02 3.856600e+01 3.326400e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d77-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d77-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t77
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.368400e+01 2.258100e+00 3.579800e+00
+5.000000e-01 1.000000e-01 1.000000e-01 2.889500e+01 5.533300e+00 5.176200e+00
+6.500000e-01 5.000000e-02 5.000000e-02 5.779100e+01 1.133300e+01 1.597600e+01
+7.500000e-01 5.000000e-02 5.000000e-02 1.076000e+02 1.657800e+01 3.618500e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.866700e+02 3.604000e+01 4.896000e+01
+8.750000e-01 2.500000e-02 2.500000e-02 2.692400e+02 3.183000e+01 8.255500e+01
+9.250000e-01 2.500000e-02 2.500000e-02 3.962600e+02 6.234700e+01 1.126200e+02
+9.750000e-01 2.500000e-02 2.500000e-02 5.434600e+02 7.657400e+01 1.930300e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d78-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d78-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t78
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.820400e+00 8.249588e-01 8.326482e-01
+3.200000e+00 4.000000e-01 4.000000e-01 1.756400e+01 1.168185e+00 1.177140e+00
+3.800000e+00 2.000000e-01 2.000000e-01 2.330100e+01 1.977673e+00 1.786061e+00
+4.200000e+00 2.000000e-01 2.000000e-01 3.145200e+01 3.527567e+00 3.524170e+00
+4.600000e+00 2.000000e-01 2.000000e-01 3.617400e+01 3.111277e+00 2.496711e+00
+5.000000e+00 2.000000e-01 2.000000e-01 3.975000e+01 3.459769e+00 3.847957e+00
+5.400000e+00 2.000000e-01 2.000000e-01 2.664300e+01 2.343107e+00 2.366723e+00
+6.000000e+00 4.000000e-01 4.000000e-01 1.161900e+01 1.765713e+00 1.903634e+00
+7.600000e+00 1.200000e+00 1.200000e+00 5.938000e-01 2.750364e-01 2.776955e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d78-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d78-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t78
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 8.024800e+00 7.481900e-01 5.866500e-01
+3.200000e+00 4.000000e-01 4.000000e-01 1.517600e+01 1.363500e+00 8.667600e-01
+3.800000e+00 2.000000e-01 2.000000e-01 2.350900e+01 2.088000e+00 1.665800e+00
+4.200000e+00 2.000000e-01 2.000000e-01 3.085000e+01 2.968500e+00 1.876900e+00
+4.600000e+00 2.000000e-01 2.000000e-01 3.535800e+01 3.058900e+00 5.057900e+00
+5.000000e+00 2.000000e-01 2.000000e-01 3.591000e+01 3.538300e+00 3.357600e+00
+5.400000e+00 2.000000e-01 2.000000e-01 2.612600e+01 2.867700e+00 2.040000e+00
+6.000000e+00 4.000000e-01 4.000000e-01 9.726500e+00 1.245000e+00 1.018200e+00
+7.600000e+00 1.200000e+00 1.200000e+00 6.115400e-01 5.622500e-02 1.297900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d78-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d78-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t78
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.050100e+01 1.808700e+00 4.292900e+00
+3.200000e+00 4.000000e-01 4.000000e-01 1.914600e+01 3.471700e+00 6.093500e+00
+3.800000e+00 2.000000e-01 2.000000e-01 2.742300e+01 4.321400e+00 8.361700e+00
+4.200000e+00 2.000000e-01 2.000000e-01 3.268200e+01 4.483800e+00 1.086000e+01
+4.600000e+00 2.000000e-01 2.000000e-01 3.610300e+01 6.019700e+00 1.085800e+01
+5.000000e+00 2.000000e-01 2.000000e-01 3.638900e+01 3.030000e+00 1.018000e+01
+5.400000e+00 2.000000e-01 2.000000e-01 2.628900e+01 3.828900e+00 5.384700e+00
+6.000000e+00 4.000000e-01 4.000000e-01 1.057600e+01 1.557600e+00 2.983400e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.667600e-01 5.681500e-02 1.605200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d79-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d79-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t79
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 6.672900e-01 1.283284e-01 1.395802e-01
+1.050000e+02 1.000000e+01 1.000000e+01 6.114000e-01 6.343564e-02 6.633891e-02
+1.250000e+02 1.000000e+01 1.000000e+01 5.988800e-01 5.511955e-02 5.249953e-02
+1.475000e+02 1.250000e+01 1.250000e+01 5.134400e-01 5.272883e-02 4.578762e-02
+1.725000e+02 1.250000e+01 1.250000e+01 3.588800e-01 3.374518e-02 2.980955e-02
+1.975000e+02 1.250000e+01 1.250000e+01 2.828200e-01 2.074717e-02 2.012721e-02
+2.250000e+02 1.500000e+01 1.500000e+01 2.465000e-01 1.908910e-02 1.803991e-02
+2.575000e+02 1.750000e+01 1.750000e+01 1.608700e-01 2.961223e-02 2.911250e-02
+2.975000e+02 2.250000e+01 2.250000e+01 1.538400e-01 1.000783e-02 1.008376e-02
+3.525000e+02 3.250000e+01 3.250000e+01 9.073600e-02 7.289540e-03 7.041303e-03
+5.350000e+02 1.500000e+02 1.500000e+02 1.852800e-02 1.661871e-03 1.817394e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d79-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d79-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t79
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.924000e-01 7.545600e-02 6.181500e-02
+1.050000e+02 1.000000e+01 1.000000e+01 5.483500e-01 5.016800e-02 6.953800e-02
+1.250000e+02 1.000000e+01 1.000000e+01 5.256600e-01 6.097800e-02 8.149600e-02
+1.475000e+02 1.250000e+01 1.250000e+01 4.845100e-01 4.727000e-02 2.968700e-02
+1.725000e+02 1.250000e+01 1.250000e+01 3.785700e-01 3.402800e-02 3.129500e-02
+1.975000e+02 1.250000e+01 1.250000e+01 3.069100e-01 2.527900e-02 2.378800e-02
+2.250000e+02 1.500000e+01 1.500000e+01 2.447000e-01 2.550100e-02 1.436600e-02
+2.575000e+02 1.750000e+01 1.750000e+01 1.796800e-01 1.607700e-02 1.257400e-02
+2.975000e+02 2.250000e+01 2.250000e+01 1.321200e-01 1.231400e-02 1.061600e-02
+3.525000e+02 3.250000e+01 3.250000e+01 8.274600e-02 7.921900e-03 5.743200e-03
+5.350000e+02 1.500000e+02 1.500000e+02 1.733400e-02 1.607500e-03 1.136100e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d79-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d79-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t79
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 5.666200e-01 5.114400e-02 1.285700e-01
+1.050000e+02 1.000000e+01 1.000000e+01 5.362900e-01 3.190200e-02 1.679900e-01
+1.250000e+02 1.000000e+01 1.000000e+01 5.155800e-01 7.619700e-02 1.457700e-01
+1.475000e+02 1.250000e+01 1.250000e+01 4.909100e-01 8.641500e-02 1.170000e-01
+1.725000e+02 1.250000e+01 1.250000e+01 4.173200e-01 5.892800e-02 1.503100e-01
+1.975000e+02 1.250000e+01 1.250000e+01 3.381500e-01 4.784000e-02 9.492700e-02
+2.250000e+02 1.500000e+01 1.500000e+01 2.727400e-01 4.908000e-02 1.128800e-01
+2.575000e+02 1.750000e+01 1.750000e+01 2.082900e-01 3.261500e-02 7.396100e-02
+2.975000e+02 2.250000e+01 2.250000e+01 1.539200e-01 2.740200e-02 4.535800e-02
+3.525000e+02 3.250000e+01 3.250000e+01 1.063700e-01 1.880300e-02 3.072000e-02
+5.350000e+02 1.500000e+02 1.500000e+02 2.387300e-02 4.790300e-03 7.053500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d80-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d80-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t80
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 8.546800e-01 8.612225e-02 7.912468e-02
+3.750000e+01 1.250000e+01 1.250000e+01 1.722100e+00 1.695759e-01 1.694289e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.829700e+00 1.588628e-01 1.642612e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.553100e+00 1.322698e-01 1.478433e-01
+1.300000e+02 3.000000e+01 3.000000e+01 9.629900e-01 1.177879e-01 8.760995e-02
+1.925000e+02 3.250000e+01 3.250000e+01 4.948700e-01 4.828867e-02 4.378868e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.276000e-01 3.738451e-02 3.755716e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.574500e-01 2.042846e-02 2.016106e-02
+3.975000e+02 9.750000e+01 9.750000e+01 3.973300e-02 8.807956e-03 8.492160e-03
+6.975000e+02 2.025000e+02 2.025000e+02 3.488700e-03 7.847399e-04 8.642819e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d80-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d80-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t80
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 6.460100e-01 9.349400e-02 6.639100e-02
+3.750000e+01 1.250000e+01 1.250000e+01 1.448000e+00 1.662900e-01 1.544200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.520800e+00 2.040700e-01 1.740800e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.312700e+00 1.501500e-01 1.647700e-01
+1.300000e+02 3.000000e+01 3.000000e+01 9.203100e-01 1.126200e-01 1.069400e-01
+1.925000e+02 3.250000e+01 3.250000e+01 4.698100e-01 5.616300e-02 5.496900e-02
+2.425000e+02 1.750000e+01 1.750000e+01 2.462900e-01 3.263300e-02 2.491600e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.535000e-01 1.313900e-02 1.577600e-02
+3.975000e+02 9.750000e+01 9.750000e+01 4.778900e-02 6.300400e-03 4.425600e-03
+6.975000e+02 2.025000e+02 2.025000e+02 3.427000e-03 3.940400e-04 4.199200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d80-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d80-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t80
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 7.780000e-01 8.816100e-02 3.056400e-01
+3.750000e+01 1.250000e+01 1.250000e+01 1.801800e+00 2.478100e-01 6.374600e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.884900e+00 3.691500e-01 7.408700e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.575000e+00 2.500000e-01 6.653100e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.092700e+00 2.151300e-01 4.219100e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.538200e-01 1.123600e-01 2.242100e-01
+2.425000e+02 1.750000e+01 1.750000e+01 2.919000e-01 6.249100e-02 9.346700e-02
+2.800000e+02 2.000000e+01 2.000000e+01 1.860600e-01 3.746100e-02 7.458800e-02
+3.975000e+02 9.750000e+01 9.750000e+01 5.770700e-02 1.065300e-02 1.880200e-02
+6.975000e+02 2.025000e+02 2.025000e+02 4.972300e-03 1.072000e-03 1.877000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d81-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d81-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t81
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 2.302100e+01 7.646984e+00 7.235272e+00
+3.750000e-01 1.250000e-01 1.250000e-01 3.346800e+01 1.401554e+01 8.684749e+00
+6.000000e-01 1.000000e-01 1.000000e-01 1.255600e+02 1.642000e+01 1.715345e+01
+7.250000e-01 2.500000e-02 2.500000e-02 2.675100e+02 2.695763e+01 2.902101e+01
+7.750000e-01 2.500000e-02 2.500000e-02 3.698200e+02 3.379826e+01 3.701121e+01
+8.250000e-01 2.500000e-02 2.500000e-02 5.383800e+02 4.780003e+01 4.492155e+01
+8.750000e-01 2.500000e-02 2.500000e-02 8.043800e+02 6.960621e+01 6.579602e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.113700e+03 9.127146e+01 9.587340e+01
+9.750000e-01 2.500000e-02 2.500000e-02 1.409800e+03 1.074742e+02 1.066351e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d81-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d81-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t81
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 2.916200e+01 2.912700e+00 5.335800e+00
+3.750000e-01 1.250000e-01 1.250000e-01 4.794600e+01 6.722000e+00 5.485200e+00
+6.000000e-01 1.000000e-01 1.000000e-01 1.207000e+02 1.627700e+01 1.727300e+01
+7.250000e-01 2.500000e-02 2.500000e-02 2.416600e+02 3.077700e+01 3.978400e+01
+7.750000e-01 2.500000e-02 2.500000e-02 3.390800e+02 4.503100e+01 3.079300e+01
+8.250000e-01 2.500000e-02 2.500000e-02 4.668300e+02 5.311000e+01 5.642600e+01
+8.750000e-01 2.500000e-02 2.500000e-02 6.593600e+02 7.662600e+01 7.962000e+01
+9.250000e-01 2.500000e-02 2.500000e-02 9.187700e+02 1.141800e+02 1.043400e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.194900e+03 1.412200e+02 9.735700e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d81-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d81-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t81
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-01 1.250000e-01 1.250000e-01 2.967200e+01 5.932200e+00 9.878100e+00
+3.750000e-01 1.250000e-01 1.250000e-01 4.675100e+01 8.243100e+00 2.085400e+01
+6.000000e-01 1.000000e-01 1.000000e-01 1.262300e+02 2.556200e+01 4.486100e+01
+7.250000e-01 2.500000e-02 2.500000e-02 2.556300e+02 4.740000e+01 9.881500e+01
+7.750000e-01 2.500000e-02 2.500000e-02 3.836500e+02 5.978400e+01 1.719300e+02
+8.250000e-01 2.500000e-02 2.500000e-02 5.761800e+02 1.360000e+02 1.727100e+02
+8.750000e-01 2.500000e-02 2.500000e-02 8.018600e+02 1.223500e+02 3.151600e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.172300e+03 1.867200e+02 4.640100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.594600e+03 2.723700e+02 6.336200e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d82-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d82-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t82
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.761100e+01 3.456050e+00 3.420067e+00
+2.600000e+00 2.000000e-01 2.000000e-01 4.706400e+01 3.788729e+00 3.818097e+00
+3.000000e+00 2.000000e-01 2.000000e-01 5.251400e+01 4.227319e+00 4.144895e+00
+3.400000e+00 2.000000e-01 2.000000e-01 6.915200e+01 4.739150e+00 5.247235e+00
+3.800000e+00 2.000000e-01 2.000000e-01 7.515600e+01 5.817993e+00 5.141712e+00
+4.200000e+00 2.000000e-01 2.000000e-01 8.903400e+01 7.203957e+00 6.757537e+00
+4.600000e+00 2.000000e-01 2.000000e-01 9.695100e+01 9.096673e+00 7.540531e+00
+5.000000e+00 2.000000e-01 2.000000e-01 8.632700e+01 9.180567e+00 1.022418e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.328400e+01 8.771251e+00 6.448629e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.405800e+00 7.574342e-01 6.852392e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d82-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d82-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t82
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 3.002800e+01 3.442700e+00 3.056500e+00
+2.600000e+00 2.000000e-01 2.000000e-01 3.677300e+01 4.418500e+00 3.821700e+00
+3.000000e+00 2.000000e-01 2.000000e-01 4.583700e+01 5.917900e+00 4.089500e+00
+3.400000e+00 2.000000e-01 2.000000e-01 5.659000e+01 5.753100e+00 6.190500e+00
+3.800000e+00 2.000000e-01 2.000000e-01 6.915600e+01 8.471800e+00 6.454300e+00
+4.200000e+00 2.000000e-01 2.000000e-01 8.094400e+01 9.034900e+00 9.059200e+00
+4.600000e+00 2.000000e-01 2.000000e-01 8.819200e+01 1.024200e+01 1.232100e+01
+5.000000e+00 2.000000e-01 2.000000e-01 8.384700e+01 1.179800e+01 9.276300e+00
+5.600000e+00 4.000000e-01 4.000000e-01 3.948100e+01 5.011100e+00 4.857200e+00
+7.400000e+00 1.400000e+00 1.400000e+00 2.255400e+00 3.980800e-01 2.832600e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d82-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d82-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t82
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.447900e+01 1.136600e+01 1.740400e+01
+2.600000e+00 2.000000e-01 2.000000e-01 5.416800e+01 9.518500e+00 2.271900e+01
+3.000000e+00 2.000000e-01 2.000000e-01 6.529200e+01 1.341800e+01 2.728000e+01
+3.400000e+00 2.000000e-01 2.000000e-01 7.646300e+01 1.244100e+01 3.134100e+01
+3.800000e+00 2.000000e-01 2.000000e-01 8.610200e+01 1.509900e+01 3.601700e+01
+4.200000e+00 2.000000e-01 2.000000e-01 9.379700e+01 1.766300e+01 3.356600e+01
+4.600000e+00 2.000000e-01 2.000000e-01 9.440600e+01 1.761400e+01 3.743900e+01
+5.000000e+00 2.000000e-01 2.000000e-01 8.682100e+01 1.334600e+01 3.175300e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.337200e+01 6.362300e+00 1.574200e+01
+7.400000e+00 1.400000e+00 1.400000e+00 2.947900e+00 5.055900e-01 6.195800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d83-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d83-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t83
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.230900e+00 2.363524e-01 2.208020e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.367500e+00 2.699029e-01 1.971903e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.401200e+00 1.569007e-01 1.398365e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.224800e+00 1.113375e-01 9.117330e-02
+1.775000e+02 1.250000e+01 1.250000e+01 9.815500e-01 8.478990e-02 8.393441e-02
+2.050000e+02 1.500000e+01 1.500000e+01 8.136600e-01 5.240337e-02 5.084697e-02
+2.350000e+02 1.500000e+01 1.500000e+01 6.854200e-01 4.803824e-02 4.945945e-02
+2.650000e+02 1.500000e+01 1.500000e+01 5.444200e-01 5.055078e-02 4.844646e-02
+2.975000e+02 1.750000e+01 1.750000e+01 5.018000e-01 3.177053e-02 3.279758e-02
+3.325000e+02 1.750000e+01 1.750000e+01 3.830600e-01 3.868264e-02 4.028094e-02
+3.700000e+02 2.000000e+01 2.000000e+01 3.030500e-01 2.151354e-02 2.319422e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.886800e-01 1.553877e-02 1.418631e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.129500e-01 1.066773e-02 1.014564e-02
+5.300000e+02 5.000000e+01 5.000000e+01 5.356500e-02 6.216788e-03 6.002569e-03
+7.300000e+02 1.500000e+02 1.500000e+02 7.651500e-03 1.465704e-03 1.534366e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d83-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d83-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t83
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.039900e+00 1.611800e-01 1.698200e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.224500e+00 1.710600e-01 1.401200e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.230700e+00 1.620600e-01 1.894200e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.094500e+00 1.256300e-01 1.221100e-01
+1.775000e+02 1.250000e+01 1.250000e+01 9.337600e-01 1.004600e-01 1.012000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 7.834900e-01 1.081600e-01 7.402400e-02
+2.350000e+02 1.500000e+01 1.500000e+01 6.376300e-01 7.086200e-02 6.465700e-02
+2.650000e+02 1.500000e+01 1.500000e+01 5.178300e-01 6.202500e-02 4.300600e-02
+2.975000e+02 1.750000e+01 1.750000e+01 4.174200e-01 4.358100e-02 4.600200e-02
+3.325000e+02 1.750000e+01 1.750000e+01 3.324600e-01 3.657400e-02 2.870000e-02
+3.700000e+02 2.000000e+01 2.000000e+01 2.449200e-01 2.993200e-02 2.903200e-02
+4.125000e+02 2.250000e+01 2.250000e+01 1.620600e-01 1.975900e-02 1.527800e-02
+4.575000e+02 2.250000e+01 2.250000e+01 9.927100e-02 1.168200e-02 1.401800e-02
+5.300000e+02 5.000000e+01 5.000000e+01 4.562900e-02 5.759600e-03 3.406500e-03
+7.300000e+02 1.500000e+02 1.500000e+02 7.432100e-03 8.321700e-04 6.613600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d83-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d83-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t83
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.193500e+00 1.333100e-01 3.407400e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.264400e+00 1.563100e-01 5.121700e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.267500e+00 2.238800e-01 4.767600e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.215700e+00 2.394700e-01 4.412900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.126900e+00 2.102700e-01 4.224000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 9.228200e-01 1.453900e-01 4.038200e-01
+2.350000e+02 1.500000e+01 1.500000e+01 7.897200e-01 1.531800e-01 2.964800e-01
+2.650000e+02 1.500000e+01 1.500000e+01 6.680500e-01 1.176200e-01 2.909900e-01
+2.975000e+02 1.750000e+01 1.750000e+01 5.572800e-01 1.033900e-01 2.439400e-01
+3.325000e+02 1.750000e+01 1.750000e+01 4.738300e-01 8.338800e-02 1.748400e-01
+3.700000e+02 2.000000e+01 2.000000e+01 3.564400e-01 7.142800e-02 1.213200e-01
+4.125000e+02 2.250000e+01 2.250000e+01 2.427100e-01 6.847700e-02 7.604900e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.438900e-01 2.485000e-02 6.675300e-02
+5.300000e+02 5.000000e+01 5.000000e+01 7.098200e-02 1.507400e-02 2.817900e-02
+7.300000e+02 1.500000e+02 1.500000e+02 1.221600e-02 2.064100e-03 6.538900e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d84-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d84-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t84
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 4.347400e+02 5.795541e+01 6.211122e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.845800e+02 5.274486e+01 5.032847e+01
+3.000000e-01 5.000000e-02 5.000000e-02 3.647200e+02 5.068410e+01 5.084223e+01
+4.500000e-01 1.000000e-01 1.000000e-01 2.688400e+02 4.779646e+01 4.023696e+01
+6.000000e-01 5.000000e-02 5.000000e-02 1.889400e+02 2.910514e+01 2.964744e+01
+7.500000e-01 1.000000e-01 1.000000e-01 8.870300e+01 1.384812e+01 1.426679e+01
+1.025000e+00 1.750000e-01 1.750000e-01 2.708000e+01 4.515114e+00 4.539786e+00
+1.850000e+00 6.500000e-01 6.500000e-01 2.292300e+00 4.370611e-01 4.426839e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d84-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d84-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t84
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.321700e+02 5.383300e+01 4.128500e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.224100e+02 4.767800e+01 4.784700e+01
+3.000000e-01 5.000000e-02 5.000000e-02 3.263500e+02 5.051200e+01 4.407900e+01
+4.500000e-01 1.000000e-01 1.000000e-01 2.437600e+02 3.066900e+01 3.452800e+01
+6.000000e-01 5.000000e-02 5.000000e-02 1.597000e+02 2.220900e+01 2.097700e+01
+7.500000e-01 1.000000e-01 1.000000e-01 8.221600e+01 1.097900e+01 9.676500e+00
+1.025000e+00 1.750000e-01 1.750000e-01 2.277500e+01 3.576700e+00 1.967800e+00
+1.850000e+00 6.500000e-01 6.500000e-01 1.609100e+00 2.676200e-01 2.410200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d84-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d84-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t84
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 4.378000e+02 8.450300e+01 1.977600e+02
+2.000000e-01 5.000000e-02 5.000000e-02 4.204900e+02 8.073100e+01 1.929300e+02
+3.000000e-01 5.000000e-02 5.000000e-02 4.200800e+02 8.238600e+01 1.944700e+02
+4.500000e-01 1.000000e-01 1.000000e-01 3.125500e+02 6.555000e+01 1.322200e+02
+6.000000e-01 5.000000e-02 5.000000e-02 2.066400e+02 4.837800e+01 8.167300e+01
+7.500000e-01 1.000000e-01 1.000000e-01 1.106500e+02 2.555100e+01 4.710600e+01
+1.025000e+00 1.750000e-01 1.750000e-01 3.358800e+01 8.781200e+00 1.261500e+01
+1.850000e+00 6.500000e-01 6.500000e-01 2.349700e+00 5.707100e-01 1.011300e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d85-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d85-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t85
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.247200e+02 2.503460e+01 2.851347e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.848800e+02 5.262616e+01 3.346398e+01
+3.250000e-01 7.500000e-02 7.500000e-02 4.329600e+02 3.719179e+01 3.749501e+01
+4.750000e-01 7.500000e-02 7.500000e-02 3.746100e+02 3.679920e+01 3.706925e+01
+6.750000e-01 1.250000e-01 1.250000e-01 1.703000e+02 1.989806e+01 1.730539e+01
+9.000000e-01 1.000000e-01 1.000000e-01 3.995000e+01 5.329199e+00 5.208289e+00
+1.750000e+00 7.500000e-01 7.500000e-01 2.382200e+00 3.930711e-01 3.966423e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d85-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d85-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t85
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.018300e+02 2.525500e+01 2.559800e+01
+2.000000e-01 5.000000e-02 5.000000e-02 3.464100e+02 3.608800e+01 3.342900e+01
+3.250000e-01 7.500000e-02 7.500000e-02 3.971700e+02 5.379100e+01 4.828200e+01
+4.750000e-01 7.500000e-02 7.500000e-02 3.274300e+02 4.371800e+01 3.635600e+01
+6.750000e-01 1.250000e-01 1.250000e-01 1.464000e+02 2.012900e+01 1.994100e+01
+9.000000e-01 1.000000e-01 1.000000e-01 3.425100e+01 5.986100e+00 4.486000e+00
+1.750000e+00 7.500000e-01 7.500000e-01 1.593600e+00 2.331500e-01 2.907300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d85-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d85-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t85
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 3.382400e+02 4.966400e+01 1.057100e+02
+2.000000e-01 5.000000e-02 5.000000e-02 3.961600e+02 6.686700e+01 1.237500e+02
+3.250000e-01 7.500000e-02 7.500000e-02 4.576100e+02 7.642000e+01 1.879100e+02
+4.750000e-01 7.500000e-02 7.500000e-02 4.087400e+02 7.475900e+01 1.786400e+02
+6.750000e-01 1.250000e-01 1.250000e-01 1.992300e+02 4.159300e+01 8.039300e+01
+9.000000e-01 1.000000e-01 1.000000e-01 5.022400e+01 1.168900e+01 2.223400e+01
+1.750000e+00 7.500000e-01 7.500000e-01 2.270300e+00 4.911400e-01 1.075100e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d86-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d86-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t86
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.414400e+02 8.672454e+00 7.780229e+00
+1.000000e+00 5.000000e-01 5.000000e-01 7.665500e+01 8.583108e+00 7.459364e+00
+2.000000e+00 5.000000e-01 5.000000e-01 3.080900e+01 4.180022e+00 4.464411e+00
+3.000000e+00 5.000000e-01 5.000000e-01 9.790800e+00 2.027761e+00 1.998234e+00
+6.000000e+00 2.500000e+00 2.500000e+00 3.549500e+00 1.178194e+00 1.009966e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d86-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d86-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t86
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.283600e+02 1.287900e+01 1.183900e+01
+1.000000e+00 5.000000e-01 5.000000e-01 6.845200e+01 9.888400e+00 8.883300e+00
+2.000000e+00 5.000000e-01 5.000000e-01 2.620200e+01 3.683300e+00 3.543100e+00
+3.000000e+00 5.000000e-01 5.000000e-01 8.274100e+00 1.530400e+00 1.346200e+00
+6.000000e+00 2.500000e+00 2.500000e+00 3.162600e+00 4.991000e-01 4.510400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d86-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d86-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t86
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.482500e+02 2.285400e+01 4.891200e+01
+1.000000e+00 5.000000e-01 5.000000e-01 8.725800e+01 1.738000e+01 3.863700e+01
+2.000000e+00 5.000000e-01 5.000000e-01 3.441100e+01 7.705900e+00 1.574400e+01
+3.000000e+00 5.000000e-01 5.000000e-01 1.082300e+01 2.179800e+00 4.632600e+00
+6.000000e+00 2.500000e+00 2.500000e+00 2.821900e+00 3.718700e-01 1.463200e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d87-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d87-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.345400e+00 6.283506e-01 6.385587e-01
+5.800000e+02 3.500000e+01 3.500000e+01 4.960800e+00 3.555689e-01 3.514885e-01
+6.550000e+02 4.000000e+01 4.000000e+01 3.607100e+00 2.477671e-01 2.512099e-01
+7.400000e+02 4.500000e+01 4.500000e+01 2.500100e+00 1.661609e-01 1.490339e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.698200e+00 1.253064e-01 1.200099e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.135700e+00 7.611003e-02 9.353712e-02
+1.042500e+03 5.750000e+01 5.750000e+01 7.612900e-01 5.902181e-02 5.512267e-02
+1.150000e+03 5.000000e+01 5.000000e+01 4.986300e-01 4.476704e-02 3.211264e-02
+1.275000e+03 7.500000e+01 7.500000e+01 3.215300e-01 3.539612e-02 2.299664e-02
+1.425000e+03 7.500000e+01 7.500000e+01 2.053000e-01 1.960732e-02 2.564483e-02
+1.750000e+03 2.500000e+02 2.500000e+02 8.434500e-02 9.472271e-03 1.062872e-02
+2.350000e+03 3.500000e+02 3.500000e+02 1.466300e-02 2.688886e-03 2.399257e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.497700e-03 4.270761e-04 3.916612e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d87-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d87-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 5.189500e+00 6.646800e-01 4.813300e-01
+5.800000e+02 3.500000e+01 3.500000e+01 4.064400e+00 4.873900e-01 4.491200e-01
+6.550000e+02 4.000000e+01 4.000000e+01 2.940600e+00 3.623100e-01 3.876200e-01
+7.400000e+02 4.500000e+01 4.500000e+01 2.074700e+00 2.906300e-01 2.113500e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.427100e+00 1.793300e-01 1.504700e-01
+9.325000e+02 5.250000e+01 5.250000e+01 9.744700e-01 1.204500e-01 1.030300e-01
+1.042500e+03 5.750000e+01 5.750000e+01 6.551300e-01 8.060800e-02 7.529300e-02
+1.150000e+03 5.000000e+01 5.000000e+01 4.526800e-01 5.282000e-02 6.030800e-02
+1.275000e+03 7.500000e+01 7.500000e+01 2.994500e-01 3.891800e-02 3.251400e-02
+1.425000e+03 7.500000e+01 7.500000e+01 1.862400e-01 2.447800e-02 1.554400e-02
+1.750000e+03 2.500000e+02 2.500000e+02 7.816500e-02 9.135900e-03 8.739000e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.649200e-02 1.713100e-03 1.375700e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.727600e-03 1.849300e-04 1.868400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d87-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d87-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 5.421500e+00 1.325300e+00 1.985600e+00
+5.800000e+02 3.500000e+01 3.500000e+01 4.268400e+00 1.064600e+00 1.610500e+00
+6.550000e+02 4.000000e+01 4.000000e+01 3.073400e+00 7.723900e-01 1.171600e+00
+7.400000e+02 4.500000e+01 4.500000e+01 2.184200e+00 5.600800e-01 8.571600e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.512900e+00 3.939700e-01 6.068100e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.035900e+00 2.749000e-01 4.269400e-01
+1.042500e+03 5.750000e+01 5.750000e+01 6.863500e-01 1.839600e-01 2.869700e-01
+1.150000e+03 5.000000e+01 5.000000e+01 4.767700e-01 1.302100e-01 2.047800e-01
+1.275000e+03 7.500000e+01 7.500000e+01 3.177100e-01 8.769500e-02 1.388000e-01
+1.425000e+03 7.500000e+01 7.500000e+01 2.005600e-01 5.687800e-02 9.136200e-02
+1.750000e+03 2.500000e+02 2.500000e+02 8.242300e-02 2.368700e-02 3.828700e-02
+2.350000e+03 3.500000e+02 3.500000e+02 1.697600e-02 5.169700e-03 8.610000e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.768800e-03 5.715800e-04 9.824900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d87-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d87-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t87
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 5.245900e+00 1.046600e+00 2.291600e+00
+5.800000e+02 3.500000e+01 3.500000e+01 4.166000e+00 7.955300e-01 1.822200e+00
+6.550000e+02 4.000000e+01 4.000000e+01 3.068100e+00 5.780100e-01 1.336000e+00
+7.400000e+02 4.500000e+01 4.500000e+01 2.198800e+00 4.371200e-01 9.161400e-01
+8.325000e+02 4.750000e+01 4.750000e+01 1.597800e+00 3.599300e-01 5.767300e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.094800e+00 2.048300e-01 4.545500e-01
+1.042500e+03 5.750000e+01 5.750000e+01 7.471200e-01 1.389900e-01 3.049900e-01
+1.150000e+03 5.000000e+01 5.000000e+01 5.265600e-01 9.647500e-02 2.111000e-01
+1.275000e+03 7.500000e+01 7.500000e+01 3.652300e-01 5.967500e-02 1.373000e-01
+1.425000e+03 7.500000e+01 7.500000e+01 2.308300e-01 4.210600e-02 7.928000e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.005300e-01 1.783600e-02 4.013200e-02
+2.350000e+03 3.500000e+02 3.500000e+02 2.146900e-02 3.521900e-03 7.645500e-03
+3.350000e+03 6.500000e+02 6.500000e+02 2.395800e-03 5.135400e-04 1.198300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d88-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d88-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 6.686800e+00 6.362590e-01 6.131993e-01
+3.750000e+01 1.250000e+01 1.250000e+01 1.373000e+01 1.237871e+00 1.291998e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.337800e+01 1.099245e+00 1.113073e+00
+8.750000e+01 1.250000e+01 1.250000e+01 1.020500e+01 7.321694e-01 7.441399e-01
+1.150000e+02 1.500000e+01 1.500000e+01 6.936000e+00 4.835363e-01 4.427047e-01
+1.450000e+02 1.500000e+01 1.500000e+01 4.871300e+00 4.563773e-01 3.811436e-01
+1.750000e+02 1.500000e+01 1.500000e+01 3.125300e+00 2.446411e-01 2.454333e-01
+2.075000e+02 1.750000e+01 1.750000e+01 1.836400e+00 1.628755e-01 1.472490e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.050500e+00 9.161548e-02 1.008043e-01
+2.800000e+02 2.000000e+01 2.000000e+01 6.262700e-01 7.411697e-02 7.248302e-02
+3.975000e+02 9.750000e+01 9.750000e+01 1.206400e-01 2.266544e-02 2.255991e-02
+6.975000e+02 2.025000e+02 2.025000e+02 5.853700e-03 1.238371e-03 1.310000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d88-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d88-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 4.812200e+00 7.881100e-01 7.603200e-01
+3.750000e+01 1.250000e+01 1.250000e+01 1.063800e+01 1.265400e+00 1.234200e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.059800e+01 1.325600e+00 1.134200e+00
+8.750000e+01 1.250000e+01 1.250000e+01 8.514900e+00 1.058100e+00 9.114000e-01
+1.150000e+02 1.500000e+01 1.500000e+01 6.209700e+00 7.671000e-01 7.232000e-01
+1.450000e+02 1.500000e+01 1.500000e+01 4.351500e+00 5.547000e-01 4.442300e-01
+1.750000e+02 1.500000e+01 1.500000e+01 2.905400e+00 3.307500e-01 3.042800e-01
+2.075000e+02 1.750000e+01 1.750000e+01 1.795700e+00 2.291700e-01 1.699700e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.037300e+00 1.075200e-01 1.064500e-01
+2.800000e+02 2.000000e+01 2.000000e+01 5.956100e-01 7.400100e-02 5.484300e-02
+3.975000e+02 9.750000e+01 9.750000e+01 1.554900e-01 1.658700e-02 1.475700e-02
+6.975000e+02 2.025000e+02 2.025000e+02 7.122200e-03 7.693000e-04 5.454900e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d88-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d88-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 5.348700e+00 1.197000e+00 1.742800e+00
+3.750000e+01 1.250000e+01 1.250000e+01 1.122200e+01 2.678700e+00 3.995600e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.078700e+01 2.730100e+00 4.157200e+00
+8.750000e+01 1.250000e+01 1.250000e+01 8.765100e+00 2.285400e+00 3.510600e+00
+1.150000e+02 1.500000e+01 1.500000e+01 6.365800e+00 1.690500e+00 2.623900e+00
+1.450000e+02 1.500000e+01 1.500000e+01 4.535400e+00 1.239000e+00 1.948000e+00
+1.750000e+02 1.500000e+01 1.500000e+01 3.070000e+00 8.363200e-01 1.311800e+00
+2.075000e+02 1.750000e+01 1.750000e+01 1.905700e+00 5.197300e-01 8.125000e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.155900e+00 3.167400e-01 4.947000e-01
+2.800000e+02 2.000000e+01 2.000000e+01 6.816100e-01 1.869100e-01 2.913600e-01
+3.975000e+02 9.750000e+01 9.750000e+01 1.888400e-01 5.226500e-02 8.144700e-02
+6.975000e+02 2.025000e+02 2.025000e+02 9.781400e-03 2.780300e-03 4.349400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d88-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d88-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t88
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 5.150100e+00 7.406100e-01 2.057300e+00
+3.750000e+01 1.250000e+01 1.250000e+01 1.166400e+01 2.178500e+00 4.761500e+00
+6.250000e+01 1.250000e+01 1.250000e+01 1.152600e+01 2.413900e+00 4.801200e+00
+8.750000e+01 1.250000e+01 1.250000e+01 9.192700e+00 1.649700e+00 3.884100e+00
+1.150000e+02 1.500000e+01 1.500000e+01 6.639500e+00 1.298700e+00 2.947600e+00
+1.450000e+02 1.500000e+01 1.500000e+01 4.673100e+00 9.886800e-01 1.890700e+00
+1.750000e+02 1.500000e+01 1.500000e+01 3.060900e+00 6.205400e-01 1.322500e+00
+2.075000e+02 1.750000e+01 1.750000e+01 1.845400e+00 4.101900e-01 7.583000e-01
+2.425000e+02 1.750000e+01 1.750000e+01 1.097200e+00 2.220700e-01 4.785800e-01
+2.800000e+02 2.000000e+01 2.000000e+01 6.320400e-01 1.189400e-01 2.311100e-01
+3.975000e+02 9.750000e+01 9.750000e+01 1.667700e-01 3.584900e-02 5.748000e-02
+6.975000e+02 2.025000e+02 2.025000e+02 9.573600e-03 2.066400e-03 3.171200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d89-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d89-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.385800e+02 3.239514e+01 3.056628e+01
+2.250000e-01 7.500000e-02 7.500000e-02 1.951300e+02 4.141045e+01 3.119311e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.169200e+02 3.649278e+01 3.761133e+01
+4.500000e-01 5.000000e-02 5.000000e-02 3.687800e+02 4.708633e+01 4.735659e+01
+5.500000e-01 5.000000e-02 5.000000e-02 5.973400e+02 6.784832e+01 6.418598e+01
+6.250000e-01 2.500000e-02 2.500000e-02 1.009600e+03 9.293142e+01 8.422428e+01
+6.750000e-01 2.500000e-02 2.500000e-02 1.253100e+03 9.759674e+01 1.006047e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.722200e+03 1.415085e+02 1.488028e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.591500e+03 1.797726e+02 1.835356e+02
+8.250000e-01 2.500000e-02 2.500000e-02 3.765200e+03 2.764705e+02 2.684448e+02
+8.750000e-01 2.500000e-02 2.500000e-02 5.168800e+03 3.773654e+02 3.749603e+02
+9.250000e-01 2.500000e-02 2.500000e-02 6.703100e+03 4.744396e+02 4.736964e+02
+9.750000e-01 2.500000e-02 2.500000e-02 8.541300e+03 6.196934e+02 6.302609e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d89-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d89-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.712500e+02 2.328800e+01 2.031300e+01
+2.250000e-01 7.500000e-02 7.500000e-02 2.007800e+02 2.529700e+01 2.049800e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.708900e+02 3.701700e+01 3.215900e+01
+4.500000e-01 5.000000e-02 5.000000e-02 3.795500e+02 4.916400e+01 5.146200e+01
+5.500000e-01 5.000000e-02 5.000000e-02 5.875100e+02 7.516400e+01 7.132500e+01
+6.250000e-01 2.500000e-02 2.500000e-02 8.664900e+02 1.208400e+02 1.000100e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.145400e+03 1.594900e+02 1.317400e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.577700e+03 2.174400e+02 1.737000e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.162400e+03 2.583800e+02 2.217400e+02
+8.250000e-01 2.500000e-02 2.500000e-02 2.978000e+03 3.504300e+02 3.354300e+02
+8.750000e-01 2.500000e-02 2.500000e-02 4.086900e+03 4.855200e+02 4.219000e+02
+9.250000e-01 2.500000e-02 2.500000e-02 5.412700e+03 6.471000e+02 5.975100e+02
+9.750000e-01 2.500000e-02 2.500000e-02 6.664600e+03 8.707200e+02 6.753600e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d89-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d89-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.762300e+02 4.934000e+01 7.879400e+01
+2.250000e-01 7.500000e-02 7.500000e-02 2.058900e+02 5.747000e+01 9.143700e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.711900e+02 7.649000e+01 1.232500e+02
+4.500000e-01 5.000000e-02 5.000000e-02 3.657500e+02 1.012500e+02 1.611000e+02
+5.500000e-01 5.000000e-02 5.000000e-02 5.852100e+02 1.654900e+02 2.637600e+02
+6.250000e-01 2.500000e-02 2.500000e-02 8.188900e+02 2.243600e+02 3.522600e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.100100e+03 2.997600e+02 4.705600e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.521600e+03 4.130900e+02 6.481000e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.130800e+03 5.686900e+02 8.822000e+02
+8.250000e-01 2.500000e-02 2.500000e-02 3.007200e+03 7.898300e+02 1.216600e+03
+8.750000e-01 2.500000e-02 2.500000e-02 4.251700e+03 1.086500e+03 1.657100e+03
+9.250000e-01 2.500000e-02 2.500000e-02 5.916400e+03 1.462500e+03 2.204800e+03
+9.750000e-01 2.500000e-02 2.500000e-02 7.612900e+03 1.816500e+03 2.698500e+03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d89-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d89-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t89
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.605600e+02 3.541500e+01 6.150200e+01
+2.250000e-01 7.500000e-02 7.500000e-02 1.868100e+02 3.720000e+01 8.916700e+01
+3.500000e-01 5.000000e-02 5.000000e-02 2.435700e+02 5.204100e+01 1.019900e+02
+4.500000e-01 5.000000e-02 5.000000e-02 3.409500e+02 6.501800e+01 1.514000e+02
+5.500000e-01 5.000000e-02 5.000000e-02 5.397700e+02 1.168500e+02 2.200200e+02
+6.250000e-01 2.500000e-02 2.500000e-02 8.286900e+02 1.730700e+02 3.025800e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.105300e+03 2.099200e+02 4.431300e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.575100e+03 3.042800e+02 6.656500e+02
+7.750000e-01 2.500000e-02 2.500000e-02 2.232000e+03 3.918100e+02 1.008600e+03
+8.250000e-01 2.500000e-02 2.500000e-02 3.217700e+03 6.539700e+02 1.331300e+03
+8.750000e-01 2.500000e-02 2.500000e-02 4.515100e+03 8.594000e+02 1.925600e+03
+9.250000e-01 2.500000e-02 2.500000e-02 6.198000e+03 1.264400e+03 2.500100e+03
+9.750000e-01 2.500000e-02 2.500000e-02 7.723100e+03 1.387900e+03 3.173800e+03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d90-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d90-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 5.077600e+02 3.462433e+01 3.362834e+01
+2.600000e+00 2.000000e-01 2.000000e-01 6.270400e+02 3.931143e+01 3.957405e+01
+3.000000e+00 2.000000e-01 2.000000e-01 7.263600e+02 4.470956e+01 4.586098e+01
+3.400000e+00 2.000000e-01 2.000000e-01 7.859100e+02 5.164003e+01 5.295506e+01
+3.800000e+00 2.000000e-01 2.000000e-01 7.077900e+02 5.530817e+01 5.384023e+01
+4.200000e+00 2.000000e-01 2.000000e-01 4.398700e+02 3.673335e+01 3.512347e+01
+4.600000e+00 2.000000e-01 2.000000e-01 2.400300e+02 2.221590e+01 2.274785e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.154700e+02 1.446053e+01 1.405010e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.243200e+01 9.426323e+00 6.896334e+00
+6.200000e+00 2.000000e-01 2.000000e-01 1.202700e+01 3.301047e+00 3.078377e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.478100e-01 3.664103e-01 3.132278e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d90-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d90-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 4.167600e+02 4.547600e+01 4.181200e+01
+2.600000e+00 2.000000e-01 2.000000e-01 5.068400e+02 5.699200e+01 4.931700e+01
+3.000000e+00 2.000000e-01 2.000000e-01 6.012200e+02 7.730800e+01 6.630100e+01
+3.400000e+00 2.000000e-01 2.000000e-01 6.554000e+02 8.032000e+01 7.149600e+01
+3.800000e+00 2.000000e-01 2.000000e-01 5.947600e+02 7.543400e+01 6.385300e+01
+4.200000e+00 2.000000e-01 2.000000e-01 3.693700e+02 5.368700e+01 4.448200e+01
+4.600000e+00 2.000000e-01 2.000000e-01 2.112100e+02 2.990600e+01 2.417500e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.102300e+02 1.471400e+01 1.419000e+01
+5.600000e+00 4.000000e-01 4.000000e-01 3.959900e+01 5.101100e+00 4.811500e+00
+6.200000e+00 2.000000e-01 2.000000e-01 1.069200e+01 2.646100e+00 1.101200e+00
+7.600000e+00 1.200000e+00 1.200000e+00 8.500700e-01 6.860900e-02 1.690100e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d90-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d90-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 5.380500e+02 1.362000e+02 2.055300e+02
+2.600000e+00 2.000000e-01 2.000000e-01 6.000900e+02 1.519000e+02 2.296500e+02
+3.000000e+00 2.000000e-01 2.000000e-01 6.491400e+02 1.640400e+02 2.488300e+02
+3.400000e+00 2.000000e-01 2.000000e-01 6.621100e+02 1.685000e+02 2.572100e+02
+3.800000e+00 2.000000e-01 2.000000e-01 5.639300e+02 1.428500e+02 2.187200e+02
+4.200000e+00 2.000000e-01 2.000000e-01 3.478300e+02 9.099600e+01 1.415100e+02
+4.600000e+00 2.000000e-01 2.000000e-01 1.921300e+02 5.169100e+01 8.195400e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.011100e+02 2.798900e+01 4.487600e+01
+5.600000e+00 4.000000e-01 4.000000e-01 3.720400e+01 1.085000e+01 1.797400e+01
+6.200000e+00 2.000000e-01 2.000000e-01 9.907200e+00 3.151000e+00 5.605000e+00
+7.600000e+00 1.200000e+00 1.200000e+00 8.464300e-01 2.840000e-01 5.216000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d90-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d90-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t90
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 5.026400e+02 1.035700e+02 2.239800e+02
+2.600000e+00 2.000000e-01 2.000000e-01 5.912000e+02 1.082000e+02 2.596600e+02
+3.000000e+00 2.000000e-01 2.000000e-01 6.717900e+02 1.423900e+02 2.722900e+02
+3.400000e+00 2.000000e-01 2.000000e-01 6.879300e+02 1.342800e+02 2.848200e+02
+3.800000e+00 2.000000e-01 2.000000e-01 5.936200e+02 1.139300e+02 2.469100e+02
+4.200000e+00 2.000000e-01 2.000000e-01 3.625100e+02 6.665900e+01 1.489800e+02
+4.600000e+00 2.000000e-01 2.000000e-01 2.069800e+02 4.201700e+01 8.118200e+01
+5.000000e+00 2.000000e-01 2.000000e-01 1.113600e+02 1.582500e+01 3.950300e+01
+5.600000e+00 4.000000e-01 4.000000e-01 4.353700e+01 6.415000e+00 1.580300e+01
+6.200000e+00 2.000000e-01 2.000000e-01 1.305200e+01 2.727600e+00 2.389800e+00
+7.600000e+00 1.200000e+00 1.200000e+00 1.263800e+00 1.343500e-01 3.251800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d91-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d91-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.163300e+01 1.457982e+00 1.409526e+00
+1.050000e+02 1.000000e+01 1.000000e+01 1.279900e+01 1.308648e+00 1.298884e+00
+1.275000e+02 1.250000e+01 1.250000e+01 1.197200e+01 9.187943e-01 9.310671e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.040900e+01 6.983664e-01 6.436609e-01
+1.775000e+02 1.250000e+01 1.250000e+01 8.399800e+00 4.930730e-01 4.808062e-01
+2.050000e+02 1.500000e+01 1.500000e+01 6.012400e+00 3.049790e-01 2.986977e-01
+2.350000e+02 1.500000e+01 1.500000e+01 3.820000e+00 1.819593e-01 1.815982e-01
+2.650000e+02 1.500000e+01 1.500000e+01 2.410300e+00 1.304611e-01 1.238769e-01
+2.975000e+02 1.750000e+01 1.750000e+01 1.454800e+00 8.170435e-02 8.658265e-02
+3.325000e+02 1.750000e+01 1.750000e+01 8.123100e-01 5.041611e-02 5.304323e-02
+3.700000e+02 2.000000e+01 2.000000e+01 4.905100e-01 4.323071e-02 4.585957e-02
+4.125000e+02 2.250000e+01 2.250000e+01 2.656600e-01 2.211866e-02 2.000179e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.558900e-01 1.491181e-02 1.383376e-02
+5.300000e+02 5.000000e+01 5.000000e+01 6.006300e-02 7.026720e-03 6.682852e-03
+6.325000e+02 5.250000e+01 5.250000e+01 1.817100e-02 3.713347e-03 3.630039e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.412400e-03 8.271355e-04 8.225211e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d91-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d91-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 9.167100e+00 1.467600e+00 1.126000e+00
+1.050000e+02 1.000000e+01 1.000000e+01 1.040400e+01 1.455700e+00 1.138200e+00
+1.275000e+02 1.250000e+01 1.250000e+01 9.984400e+00 1.281800e+00 1.259100e+00
+1.525000e+02 1.250000e+01 1.250000e+01 8.767000e+00 1.040500e+00 9.026900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 7.167400e+00 8.299700e-01 7.835400e-01
+2.050000e+02 1.500000e+01 1.500000e+01 5.145300e+00 6.172900e-01 4.774200e-01
+2.350000e+02 1.500000e+01 1.500000e+01 3.313300e+00 3.656800e-01 3.232700e-01
+2.650000e+02 1.500000e+01 1.500000e+01 2.088400e+00 2.361100e-01 1.918000e-01
+2.975000e+02 1.750000e+01 1.750000e+01 1.270200e+00 1.327000e-01 1.306500e-01
+3.325000e+02 1.750000e+01 1.750000e+01 7.566400e-01 8.487200e-02 4.965600e-02
+3.700000e+02 2.000000e+01 2.000000e+01 4.394200e-01 4.849800e-02 4.406300e-02
+4.125000e+02 2.250000e+01 2.250000e+01 2.469700e-01 2.745000e-02 2.244800e-02
+4.575000e+02 2.250000e+01 2.250000e+01 1.370800e-01 1.516300e-02 1.641200e-02
+5.300000e+02 5.000000e+01 5.000000e+01 5.797400e-02 6.763700e-03 3.551500e-03
+6.325000e+02 5.250000e+01 5.250000e+01 1.741100e-02 2.438800e-03 1.845500e-03
+8.425000e+02 1.575000e+02 1.575000e+02 2.787800e-03 4.042100e-04 3.313600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d91-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d91-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 8.009900e+00 2.028500e+00 3.149900e+00
+1.050000e+02 1.000000e+01 1.000000e+01 9.429800e+00 2.366500e+00 3.623600e+00
+1.275000e+02 1.250000e+01 1.250000e+01 9.781600e+00 2.490900e+00 3.820600e+00
+1.525000e+02 1.250000e+01 1.250000e+01 9.104700e+00 2.301000e+00 3.499600e+00
+1.775000e+02 1.250000e+01 1.250000e+01 8.004500e+00 2.031700e+00 3.087800e+00
+2.050000e+02 1.500000e+01 1.500000e+01 5.844000e+00 1.498000e+00 2.286500e+00
+2.350000e+02 1.500000e+01 1.500000e+01 3.926600e+00 1.018300e+00 1.557100e+00
+2.650000e+02 1.500000e+01 1.500000e+01 2.567600e+00 6.739900e-01 1.032700e+00
+2.975000e+02 1.750000e+01 1.750000e+01 1.564700e+00 4.148300e-01 6.377500e-01
+3.325000e+02 1.750000e+01 1.750000e+01 9.581800e-01 2.569600e-01 3.963400e-01
+3.700000e+02 2.000000e+01 2.000000e+01 5.759000e-01 1.558000e-01 2.403300e-01
+4.125000e+02 2.250000e+01 2.250000e+01 3.337600e-01 9.139300e-02 1.414900e-01
+4.575000e+02 2.250000e+01 2.250000e+01 1.840600e-01 5.042800e-02 7.824000e-02
+5.300000e+02 5.000000e+01 5.000000e+01 7.972500e-02 2.227800e-02 3.464600e-02
+6.325000e+02 5.250000e+01 5.250000e+01 2.374100e-02 6.799300e-03 1.069900e-02
+8.425000e+02 1.575000e+02 1.575000e+02 3.652400e-03 1.064200e-03 1.681200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d91-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d91-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t91
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 8.388400e+00 1.329500e+00 3.479200e+00
+1.050000e+02 1.000000e+01 1.000000e+01 9.899200e+00 1.960200e+00 4.097100e+00
+1.275000e+02 1.250000e+01 1.250000e+01 1.011600e+01 2.010500e+00 4.103000e+00
+1.525000e+02 1.250000e+01 1.250000e+01 9.440600e+00 1.792300e+00 3.947200e+00
+1.775000e+02 1.250000e+01 1.250000e+01 8.054100e+00 1.544000e+00 3.254500e+00
+2.050000e+02 1.500000e+01 1.500000e+01 5.884600e+00 1.114000e+00 2.684300e+00
+2.350000e+02 1.500000e+01 1.500000e+01 3.947500e+00 8.044100e-01 1.603300e+00
+2.650000e+02 1.500000e+01 1.500000e+01 2.523800e+00 5.188700e-01 1.095500e+00
+2.975000e+02 1.750000e+01 1.750000e+01 1.559100e+00 2.811500e-01 7.008000e-01
+3.325000e+02 1.750000e+01 1.750000e+01 9.881800e-01 2.219100e-01 3.556300e-01
+3.700000e+02 2.000000e+01 2.000000e+01 5.858200e-01 1.187100e-01 2.147400e-01
+4.125000e+02 2.250000e+01 2.250000e+01 3.423300e-01 8.872900e-02 1.057400e-01
+4.575000e+02 2.250000e+01 2.250000e+01 1.915600e-01 3.840500e-02 7.859200e-02
+5.300000e+02 5.000000e+01 5.000000e+01 8.508900e-02 1.874100e-02 3.255600e-02
+6.325000e+02 5.250000e+01 5.250000e+01 2.763300e-02 3.482600e-03 1.520300e-02
+8.425000e+02 1.575000e+02 1.575000e+02 4.549000e-03 1.121400e-03 4.244900e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d92-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d92-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 2.004000e+03 2.669950e+02 2.532186e+02
+1.000000e-01 5.000000e-02 5.000000e-02 2.112200e+03 2.638339e+02 2.532517e+02
+2.000000e-01 5.000000e-02 5.000000e-02 2.018900e+03 2.589280e+02 2.464791e+02
+3.000000e-01 5.000000e-02 5.000000e-02 2.029900e+03 2.615069e+02 2.640057e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.732300e+03 2.633165e+02 2.499944e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.337000e+03 2.024652e+02 1.992508e+02
+6.000000e-01 5.000000e-02 5.000000e-02 1.216100e+03 1.879114e+02 1.863348e+02
+7.000000e-01 5.000000e-02 5.000000e-02 9.821400e+02 1.492019e+02 1.446003e+02
+8.000000e-01 5.000000e-02 5.000000e-02 6.549300e+02 9.720235e+01 9.906715e+01
+9.250000e-01 7.500000e-02 7.500000e-02 4.014700e+02 6.243126e+01 6.498550e+01
+1.100000e+00 1.000000e-01 1.000000e-01 2.652300e+02 5.174281e+01 5.190148e+01
+1.350000e+00 1.500000e-01 1.500000e-01 1.115600e+02 2.057846e+01 2.120185e+01
+1.650000e+00 1.500000e-01 1.500000e-01 3.094300e+01 7.743732e+00 7.619970e+00
+2.050000e+00 2.500000e-01 2.500000e-01 6.776000e+00 2.000931e+00 1.900796e+00
+2.650000e+00 3.500000e-01 3.500000e-01 6.510400e-01 3.417055e-01 3.102679e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d92-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d92-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.567400e+03 2.039300e+02 1.984600e+02
+1.000000e-01 5.000000e-02 5.000000e-02 1.577700e+03 2.285200e+02 1.834500e+02
+2.000000e-01 5.000000e-02 5.000000e-02 1.606300e+03 2.160100e+02 2.042200e+02
+3.000000e-01 5.000000e-02 5.000000e-02 1.659400e+03 2.168000e+02 2.131000e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.451000e+03 1.935200e+02 1.638500e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.115300e+03 1.495400e+02 1.217100e+02
+6.000000e-01 5.000000e-02 5.000000e-02 9.767500e+02 1.380700e+02 1.037600e+02
+7.000000e-01 5.000000e-02 5.000000e-02 7.754900e+02 1.041100e+02 9.247600e+01
+8.000000e-01 5.000000e-02 5.000000e-02 5.248100e+02 6.686700e+01 1.333900e+02
+9.250000e-01 7.500000e-02 7.500000e-02 3.386100e+02 4.272100e+01 3.808000e+01
+1.100000e+00 1.000000e-01 1.000000e-01 1.891000e+02 2.639800e+01 1.704100e+01
+1.350000e+00 1.500000e-01 1.500000e-01 7.950200e+01 1.129200e+01 8.854900e+00
+1.650000e+00 1.500000e-01 1.500000e-01 2.520400e+01 3.801300e+00 2.876400e+00
+2.050000e+00 2.500000e-01 2.500000e-01 4.911000e+00 7.866200e-01 7.678600e-01
+2.650000e+00 3.500000e-01 3.500000e-01 2.383100e-01 7.195200e-02 7.958000e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d92-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d92-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.415600e+03 4.393400e+02 7.146200e+02
+1.000000e-01 5.000000e-02 5.000000e-02 1.422500e+03 4.407900e+02 7.171400e+02
+2.000000e-01 5.000000e-02 5.000000e-02 1.396600e+03 4.335900e+02 7.068400e+02
+3.000000e-01 5.000000e-02 5.000000e-02 1.427500e+03 4.438600e+02 7.240300e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.282900e+03 4.035400e+02 6.628100e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.128500e+03 3.659100e+02 6.104800e+02
+6.000000e-01 5.000000e-02 5.000000e-02 1.089800e+03 3.574300e+02 5.994600e+02
+7.000000e-01 5.000000e-02 5.000000e-02 8.591800e+02 2.823500e+02 4.738800e+02
+8.000000e-01 5.000000e-02 5.000000e-02 5.732900e+02 1.889500e+02 3.177500e+02
+9.250000e-01 7.500000e-02 7.500000e-02 3.983700e+02 1.341700e+02 2.278800e+02
+1.100000e+00 1.000000e-01 1.000000e-01 2.157300e+02 7.223900e+01 1.223700e+02
+1.350000e+00 1.500000e-01 1.500000e-01 9.648200e+01 3.232400e+01 5.436700e+01
+1.650000e+00 1.500000e-01 1.500000e-01 3.548600e+01 1.216800e+01 2.033000e+01
+2.050000e+00 2.500000e-01 2.500000e-01 5.952500e+00 2.100900e+00 3.647700e+00
+2.650000e+00 3.500000e-01 3.500000e-01 2.716300e-01 9.814000e-02 1.736900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d92-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d92-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t92
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.855800e+03 4.407700e+02 8.686100e+02
+1.000000e-01 5.000000e-02 5.000000e-02 1.858100e+03 4.098600e+02 8.931200e+02
+2.000000e-01 5.000000e-02 5.000000e-02 1.868800e+03 3.979300e+02 8.663800e+02
+3.000000e-01 5.000000e-02 5.000000e-02 1.908000e+03 4.346400e+02 9.787100e+02
+4.000000e-01 5.000000e-02 5.000000e-02 1.621100e+03 3.630100e+02 7.886400e+02
+5.000000e-01 5.000000e-02 5.000000e-02 1.193600e+03 2.611300e+02 5.891200e+02
+6.000000e-01 5.000000e-02 5.000000e-02 1.053000e+03 2.471300e+02 5.153900e+02
+7.000000e-01 5.000000e-02 5.000000e-02 8.637500e+02 1.992600e+02 3.999800e+02
+8.000000e-01 5.000000e-02 5.000000e-02 5.636500e+02 1.177500e+02 2.916200e+02
+9.250000e-01 7.500000e-02 7.500000e-02 3.738600e+02 8.372500e+01 1.720400e+02
+1.100000e+00 1.000000e-01 1.000000e-01 2.090100e+02 5.066300e+01 9.360700e+01
+1.350000e+00 1.500000e-01 1.500000e-01 8.991900e+01 1.970700e+01 4.232200e+01
+1.650000e+00 1.500000e-01 1.500000e-01 2.839400e+01 6.484700e+00 1.468300e+01
+2.050000e+00 2.500000e-01 2.500000e-01 5.998800e+00 1.140700e+00 2.396100e+00
+2.650000e+00 3.500000e-01 3.500000e-01 2.502100e-01 1.134800e-01 2.568700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d93-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d93-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.854500e+03 1.392862e+02 1.424013e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.729500e+03 1.256021e+02 1.309524e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.974600e+03 1.342602e+02 1.416856e+02
+1.750000e-01 2.500000e-02 2.500000e-02 2.076100e+03 1.712336e+02 1.392548e+02
+2.250000e-01 2.500000e-02 2.500000e-02 2.149300e+03 1.787284e+02 1.643144e+02
+2.750000e-01 2.500000e-02 2.500000e-02 2.256600e+03 1.661413e+02 1.631526e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.305200e+03 1.714270e+02 1.676101e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.442700e+03 1.706935e+02 1.573677e+02
+4.250000e-01 2.500000e-02 2.500000e-02 2.232300e+03 1.646229e+02 1.437125e+02
+4.750000e-01 2.500000e-02 2.500000e-02 2.009800e+03 1.755803e+02 1.795133e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.971700e+03 1.359661e+02 1.429800e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.947500e+03 1.238870e+02 1.337143e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.715400e+03 1.167966e+02 1.102475e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.491100e+03 9.812216e+01 9.746407e+01
+7.250000e-01 2.500000e-02 2.500000e-02 1.242800e+03 7.367909e+01 8.344958e+01
+7.750000e-01 2.500000e-02 2.500000e-02 9.860700e+02 7.374213e+01 6.988655e+01
+8.250000e-01 2.500000e-02 2.500000e-02 7.999100e+02 5.148815e+01 5.561172e+01
+8.750000e-01 2.500000e-02 2.500000e-02 6.398900e+02 3.807850e+01 4.632887e+01
+9.250000e-01 2.500000e-02 2.500000e-02 5.029500e+02 3.365246e+01 3.713072e+01
+9.750000e-01 2.500000e-02 2.500000e-02 4.017500e+02 2.904657e+01 2.896229e+01
+1.025000e+00 2.500000e-02 2.500000e-02 3.191600e+02 2.211350e+01 2.131723e+01
+1.075000e+00 2.500000e-02 2.500000e-02 2.288100e+02 1.785009e+01 1.773006e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.711300e+02 1.426725e+01 1.471588e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.507500e+02 1.353921e+01 1.257293e+01
+1.250000e+00 5.000000e-02 5.000000e-02 8.632100e+01 7.585372e+00 7.867592e+00
+1.350000e+00 5.000000e-02 5.000000e-02 5.007300e+01 5.882454e+00 5.621114e+00
+1.500000e+00 1.000000e-01 1.000000e-01 1.821000e+01 2.317406e+00 2.084775e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.168300e+00 5.117025e-01 5.212289e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d93-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d93-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.508200e+03 1.584600e+02 1.483800e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.531200e+03 1.624900e+02 1.401100e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.592200e+03 1.575500e+02 1.578200e+02
+1.750000e-01 2.500000e-02 2.500000e-02 1.680400e+03 1.817200e+02 1.455900e+02
+2.250000e-01 2.500000e-02 2.500000e-02 1.802000e+03 2.159100e+02 1.758000e+02
+2.750000e-01 2.500000e-02 2.500000e-02 1.880300e+03 2.296900e+02 1.994500e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.011100e+03 2.735800e+02 1.490700e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.030500e+03 2.511100e+02 2.315600e+02
+4.250000e-01 2.500000e-02 2.500000e-02 1.942200e+03 2.450300e+02 1.887100e+02
+4.750000e-01 2.500000e-02 2.500000e-02 1.793500e+03 2.210800e+02 2.065000e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.694300e+03 2.224300e+02 1.795100e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.559500e+03 2.420200e+02 1.761500e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.435800e+03 1.818300e+02 3.443900e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.236900e+03 1.634400e+02 1.504100e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.026400e+03 1.334100e+02 1.162000e+02
+7.750000e-01 2.500000e-02 2.500000e-02 8.407000e+02 1.224400e+02 1.200900e+02
+8.250000e-01 2.500000e-02 2.500000e-02 6.708800e+02 9.013300e+01 8.450900e+01
+8.750000e-01 2.500000e-02 2.500000e-02 5.343000e+02 8.322600e+01 5.769500e+01
+9.250000e-01 2.500000e-02 2.500000e-02 4.131000e+02 6.351800e+01 5.190300e+01
+9.750000e-01 2.500000e-02 2.500000e-02 3.232700e+02 4.456300e+01 3.899100e+01
+1.025000e+00 2.500000e-02 2.500000e-02 2.480300e+02 3.750200e+01 2.868300e+01
+1.075000e+00 2.500000e-02 2.500000e-02 1.878100e+02 2.796400e+01 2.714800e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.422900e+02 1.981100e+01 2.038300e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.046500e+02 1.639800e+01 1.343100e+01
+1.250000e+00 5.000000e-02 5.000000e-02 7.013100e+01 1.038700e+01 9.331100e+00
+1.350000e+00 5.000000e-02 5.000000e-02 3.817100e+01 6.390100e+00 6.026600e+00
+1.500000e+00 1.000000e-01 1.000000e-01 1.528800e+01 2.495700e+00 2.875200e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.319600e+00 4.327500e-01 5.803400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d93-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d93-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.788800e+03 4.681900e+02 7.238800e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.798500e+03 4.677900e+02 7.199600e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.840000e+03 4.768300e+02 7.337500e+02
+1.750000e-01 2.500000e-02 2.500000e-02 1.909400e+03 4.917200e+02 7.537700e+02
+2.250000e-01 2.500000e-02 2.500000e-02 1.971700e+03 5.035000e+02 7.702000e+02
+2.750000e-01 2.500000e-02 2.500000e-02 2.027600e+03 5.157100e+02 7.892800e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.079500e+03 5.252400e+02 8.001700e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.055100e+03 5.182200e+02 7.898700e+02
+4.250000e-01 2.500000e-02 2.500000e-02 1.991800e+03 5.054600e+02 7.726500e+02
+4.750000e-01 2.500000e-02 2.500000e-02 1.830700e+03 4.626700e+02 7.038300e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.718500e+03 4.411100e+02 6.780600e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.550600e+03 3.924800e+02 5.988700e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.404800e+03 3.572300e+02 5.442400e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.200800e+03 3.045100e+02 4.634400e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.006200e+03 2.554100e+02 3.888200e+02
+7.750000e-01 2.500000e-02 2.500000e-02 8.333700e+02 2.132100e+02 3.256600e+02
+8.250000e-01 2.500000e-02 2.500000e-02 6.624400e+02 1.707800e+02 2.614200e+02
+8.750000e-01 2.500000e-02 2.500000e-02 5.341500e+02 1.387700e+02 2.131900e+02
+9.250000e-01 2.500000e-02 2.500000e-02 4.061800e+02 1.059300e+02 1.627200e+02
+9.750000e-01 2.500000e-02 2.500000e-02 3.218500e+02 8.378900e+01 1.285100e+02
+1.025000e+00 2.500000e-02 2.500000e-02 2.528100e+02 6.580500e+01 1.010100e+02
+1.075000e+00 2.500000e-02 2.500000e-02 1.970200e+02 5.147500e+01 7.893100e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.443200e+02 3.835200e+01 5.912800e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.095400e+02 2.923700e+01 4.525200e+01
+1.250000e+00 5.000000e-02 5.000000e-02 7.723600e+01 2.197000e+01 3.454800e+01
+1.350000e+00 5.000000e-02 5.000000e-02 3.828300e+01 1.039300e+01 1.623600e+01
+1.500000e+00 1.000000e-01 1.000000e-01 1.613800e+01 4.441800e+00 6.957200e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.361900e+00 7.088000e-01 1.171300e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d93-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d93-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t93
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 1.544100e+03 2.433100e+02 5.838400e+02
+7.500000e-02 2.500000e-02 2.500000e-02 1.597200e+03 2.847700e+02 5.953500e+02
+1.250000e-01 2.500000e-02 2.500000e-02 1.665800e+03 2.686200e+02 6.318100e+02
+1.750000e-01 2.500000e-02 2.500000e-02 1.780800e+03 3.161100e+02 6.276500e+02
+2.250000e-01 2.500000e-02 2.500000e-02 1.905000e+03 3.644000e+02 7.595300e+02
+2.750000e-01 2.500000e-02 2.500000e-02 2.031500e+03 3.760100e+02 8.038700e+02
+3.250000e-01 2.500000e-02 2.500000e-02 2.108900e+03 3.883000e+02 8.859400e+02
+3.750000e-01 2.500000e-02 2.500000e-02 2.175300e+03 4.343800e+02 8.931900e+02
+4.250000e-01 2.500000e-02 2.500000e-02 2.099400e+03 4.185100e+02 8.907700e+02
+4.750000e-01 2.500000e-02 2.500000e-02 1.997300e+03 4.251100e+02 8.510400e+02
+5.250000e-01 2.500000e-02 2.500000e-02 1.847200e+03 3.461700e+02 8.248800e+02
+5.750000e-01 2.500000e-02 2.500000e-02 1.738800e+03 3.575200e+02 7.373800e+02
+6.250000e-01 2.500000e-02 2.500000e-02 1.571300e+03 3.383700e+02 7.226100e+02
+6.750000e-01 2.500000e-02 2.500000e-02 1.368100e+03 2.936400e+02 5.562500e+02
+7.250000e-01 2.500000e-02 2.500000e-02 1.139600e+03 2.698000e+02 4.358800e+02
+7.750000e-01 2.500000e-02 2.500000e-02 9.078300e+02 1.346000e+02 4.310700e+02
+8.250000e-01 2.500000e-02 2.500000e-02 7.482600e+02 1.676100e+02 3.235800e+02
+8.750000e-01 2.500000e-02 2.500000e-02 5.713600e+02 1.011600e+02 3.026700e+02
+9.250000e-01 2.500000e-02 2.500000e-02 4.575800e+02 9.798500e+01 2.140200e+02
+9.750000e-01 2.500000e-02 2.500000e-02 3.557200e+02 6.552400e+01 1.719200e+02
+1.025000e+00 2.500000e-02 2.500000e-02 2.746400e+02 6.075400e+01 1.240900e+02
+1.075000e+00 2.500000e-02 2.500000e-02 2.044100e+02 4.900500e+01 9.549500e+01
+1.125000e+00 2.500000e-02 2.500000e-02 1.605700e+02 3.927200e+01 6.517000e+01
+1.175000e+00 2.500000e-02 2.500000e-02 1.158700e+02 2.070900e+01 6.710000e+01
+1.250000e+00 5.000000e-02 5.000000e-02 7.638900e+01 1.726900e+01 3.369100e+01
+1.350000e+00 5.000000e-02 5.000000e-02 3.885300e+01 8.890800e+00 2.040400e+01
+1.500000e+00 1.000000e-01 1.000000e-01 1.660100e+01 3.015200e+00 9.609400e+00
+1.800000e+00 2.000000e-01 2.000000e-01 2.688100e+00 5.346700e-01 1.147400e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d94-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d94-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.012600e+03 5.337420e+01 5.472897e+01
+1.000000e+00 5.000000e-01 5.000000e-01 4.836400e+02 4.265705e+01 4.042195e+01
+2.000000e+00 5.000000e-01 5.000000e-01 1.522800e+02 1.960786e+01 1.954737e+01
+3.000000e+00 5.000000e-01 5.000000e-01 3.855700e+01 7.497954e+00 6.466930e+00
+4.000000e+00 5.000000e-01 5.000000e-01 7.925500e+00 2.062354e+00 1.694143e+00
+6.500000e+00 2.000000e+00 2.000000e+00 2.858000e+00 9.319546e-01 8.598858e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d94-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d94-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.509500e+02 1.008000e+02 8.228700e+01
+1.000000e+00 5.000000e-01 5.000000e-01 4.064600e+02 5.521900e+01 4.595000e+01
+2.000000e+00 5.000000e-01 5.000000e-01 1.250100e+02 1.633900e+01 1.555100e+01
+3.000000e+00 5.000000e-01 5.000000e-01 3.235100e+01 4.899000e+00 3.842200e+00
+4.000000e+00 5.000000e-01 5.000000e-01 7.495600e+00 9.653900e-01 1.432100e+00
+6.500000e+00 2.000000e+00 2.000000e+00 2.046900e+00 3.251200e-01 4.462700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d94-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d94-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.408100e+02 2.110000e+02 3.068000e+02
+1.000000e+00 5.000000e-01 5.000000e-01 4.470200e+02 1.320300e+02 2.105300e+02
+2.000000e+00 5.000000e-01 5.000000e-01 1.011600e+02 3.435000e+01 5.802700e+01
+3.000000e+00 5.000000e-01 5.000000e-01 6.145900e-01 0.000000e+00 0.000000e+00
+4.000000e+00 5.000000e-01 5.000000e-01 2.000000e-99 0.000000e+00 0.000000e+00
+6.500000e+00 2.000000e+00 2.000000e+00 2.000000e-99 0.000000e+00 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d94-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d94-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t94
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.911000e+02 1.509400e+02 3.318100e+02
+1.000000e+00 5.000000e-01 5.000000e-01 4.570200e+02 1.046700e+02 2.100800e+02
+2.000000e+00 5.000000e-01 5.000000e-01 1.435400e+02 3.286200e+01 7.379000e+01
+3.000000e+00 5.000000e-01 5.000000e-01 3.508500e+01 7.124300e+00 1.769100e+01
+4.000000e+00 5.000000e-01 5.000000e-01 6.307400e+00 9.342100e-01 3.861500e+00
+6.500000e+00 2.000000e+00 2.000000e+00 1.238500e+00 2.545000e-01 3.283900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d95-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d95-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t95
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 5.874900e-02 1.324906e-02 1.240497e-02
+7.500000e+01 2.500000e+01 2.500000e+01 9.498400e-02 1.592544e-02 1.470177e-02
+1.300000e+02 3.000000e+01 3.000000e+01 4.586100e-02 8.749442e-03 7.678501e-03
+2.300000e+02 7.000000e+01 7.000000e+01 1.632200e-02 3.132506e-03 3.457378e-03
+5.150000e+02 2.150000e+02 2.150000e+02 1.006100e-03 5.756198e-04 5.664343e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d95-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d95-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t95
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 6.033900e-02 5.201800e-03 5.724300e-03
+7.500000e+01 2.500000e+01 2.500000e+01 7.762200e-02 1.063500e-02 7.972400e-03
+1.300000e+02 3.000000e+01 3.000000e+01 5.217900e-02 6.130000e-03 5.684300e-03
+2.300000e+02 7.000000e+01 7.000000e+01 2.047900e-02 2.249500e-03 2.401700e-03
+5.150000e+02 2.150000e+02 2.150000e+02 2.106100e-03 3.194200e-04 3.445200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d95-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d95-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t95
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 8.308500e-02 1.079000e-02 2.195600e-02
+7.500000e+01 2.500000e+01 2.500000e+01 1.041400e-01 1.671300e-02 4.075200e-02
+1.300000e+02 3.000000e+01 3.000000e+01 6.528800e-02 1.279000e-02 1.865800e-02
+2.300000e+02 7.000000e+01 7.000000e+01 2.661100e-02 5.735800e-03 1.306200e-02
+5.150000e+02 2.150000e+02 2.150000e+02 2.825200e-03 6.625600e-04 8.601000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d96-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d96-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.427500e+00 8.575259e-01 8.622934e-01
+8.000000e-01 1.000000e-01 1.000000e-01 2.164200e+01 3.867042e+00 3.248226e+00
+9.500000e-01 5.000000e-02 5.000000e-02 7.270800e+01 1.019935e+01 9.433521e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d96-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d96-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 3.398700e+00 3.200700e-01 6.315900e-01
+8.000000e-01 1.000000e-01 1.000000e-01 2.394200e+01 3.318200e+00 2.258000e+00
+9.500000e-01 5.000000e-02 5.000000e-02 6.659700e+01 6.209700e+00 4.462200e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d96-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d96-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.158000e+00 9.062200e-01 1.287400e+00
+8.000000e-01 1.000000e-01 1.000000e-01 2.984100e+01 4.913000e+00 8.748200e+00
+9.500000e-01 5.000000e-02 5.000000e-02 9.393500e+01 1.526800e+01 3.573200e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d97-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d97-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.042000e+00 2.180337e-01 2.166378e-01
+4.400000e+00 8.000000e-01 8.000000e-01 2.593900e+00 3.371296e-01 3.088335e-01
+5.600000e+00 4.000000e-01 4.000000e-01 4.529700e+00 7.709864e-01 7.392904e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.330800e+00 3.734668e-01 3.154054e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d97-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d97-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.122000e+00 1.535800e-01 1.096500e-01
+4.400000e+00 8.000000e-01 8.000000e-01 2.807700e+00 2.830900e-01 2.426100e-01
+5.600000e+00 4.000000e-01 4.000000e-01 4.789300e+00 6.183900e-01 3.969900e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.352500e+00 1.326300e-01 1.845300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d97-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d97-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.900000e+00 7.000000e-01 7.000000e-01 1.887200e+00 3.199800e-01 1.275400e+00
+4.400000e+00 8.000000e-01 8.000000e-01 3.841200e+00 7.167900e-01 1.204300e+00
+5.600000e+00 4.000000e-01 4.000000e-01 5.183100e+00 9.569800e-01 2.108700e+00
+7.400000e+00 1.400000e+00 1.400000e+00 1.829800e+00 3.144700e-01 3.756300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d98-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d98-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 6.456000e-02 1.790904e-02 1.516966e-02
+1.800000e+02 4.000000e+01 4.000000e+01 4.737800e-02 7.729065e-03 7.460089e-03
+2.675000e+02 4.750000e+01 4.750000e+01 2.025100e-02 3.525959e-03 3.127624e-03
+3.750000e+02 6.000000e+01 6.000000e+01 1.352600e-02 2.489235e-03 2.377726e-03
+5.600000e+02 1.250000e+02 1.250000e+02 6.354100e-03 1.136201e-03 1.153537e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d98-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d98-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 6.004900e-02 6.597700e-03 7.504900e-03
+1.800000e+02 4.000000e+01 4.000000e+01 5.099200e-02 5.523500e-03 4.591400e-03
+2.675000e+02 4.750000e+01 4.750000e+01 2.833200e-02 3.254000e-03 2.663400e-03
+3.750000e+02 6.000000e+01 6.000000e+01 1.361500e-02 1.800900e-03 1.393600e-03
+5.600000e+02 1.250000e+02 1.250000e+02 5.648100e-03 7.691400e-04 7.387400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d98-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d98-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e+02 3.000000e+01 3.000000e+01 7.937500e-02 1.064600e-02 2.201400e-02
+1.800000e+02 4.000000e+01 4.000000e+01 5.798500e-02 1.209400e-02 2.093000e-02
+2.675000e+02 4.750000e+01 4.750000e+01 3.645300e-02 7.944700e-03 8.914500e-03
+3.750000e+02 6.000000e+01 6.000000e+01 1.986100e-02 2.817600e-03 8.124700e-03
+5.600000e+02 1.250000e+02 1.250000e+02 9.358400e-03 1.777400e-03 4.263000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d99-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d99-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.587300e+01 5.107230e+00 4.670509e+00
+7.000000e-01 3.000000e-01 3.000000e-01 4.407800e+00 8.937790e-01 8.322673e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d99-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d99-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.650400e+01 2.185400e+00 2.651000e+00
+7.000000e-01 3.000000e-01 3.000000e-01 4.289500e+00 5.409600e-01 6.522500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d99-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d99-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.630900e+01 4.804900e+00 1.328900e+01
+7.000000e-01 3.000000e-01 3.000000e-01 7.093300e+00 1.625500e+00 3.412100e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d100-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d100-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.443200e+01 3.358132e+00 3.450598e+00
+5.250000e-01 1.250000e-01 1.250000e-01 1.136400e+01 3.206306e+00 2.324743e+00
+8.250000e-01 1.750000e-01 1.750000e-01 1.501800e+00 5.158532e-01 5.032079e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d100-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d100-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.707000e+01 2.413500e+00 2.268100e+00
+5.250000e-01 1.250000e-01 1.250000e-01 1.016400e+01 1.639400e+00 1.010900e+00
+8.250000e-01 1.750000e-01 1.750000e-01 1.220900e+00 2.434400e-01 2.627700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d100-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d100-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 3.254600e+01 5.455900e+00 9.249700e+00
+5.250000e-01 1.250000e-01 1.250000e-01 1.723100e+01 2.937000e+00 8.779800e+00
+8.250000e-01 1.750000e-01 1.750000e-01 2.507400e+00 8.521500e-01 7.612800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d101-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d101-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.252300e+00 1.003388e+00 9.687704e-01
+1.000000e+00 5.000000e-01 5.000000e-01 3.073300e+00 6.788961e-01 5.561707e-01
+3.000000e+00 1.500000e+00 1.500000e+00 1.858100e+00 5.350092e-01 5.029681e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d101-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d101-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.735300e+00 7.026900e-01 5.658500e-01
+1.000000e+00 5.000000e-01 5.000000e-01 3.192500e+00 5.716400e-01 2.904800e-01
+3.000000e+00 1.500000e+00 1.500000e+00 1.849300e+00 2.181300e-01 4.216700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d101-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d101-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.037200e+01 1.659300e+00 2.412800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 4.758700e+00 8.353000e-01 2.176900e+00
+3.000000e+00 1.500000e+00 1.500000e+00 3.096500e+00 6.270700e-01 1.623600e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d102-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d102-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.078600e+00 1.375043e-01 1.335721e-01
+5.800000e+02 3.500000e+01 3.500000e+01 8.830000e-01 8.820350e-02 8.160317e-02
+6.550000e+02 4.000000e+01 4.000000e+01 6.802500e-01 6.941339e-02 6.417338e-02
+7.400000e+02 4.500000e+01 4.500000e+01 4.809000e-01 4.593229e-02 4.950006e-02
+8.325000e+02 4.750000e+01 4.750000e+01 3.027500e-01 3.592337e-02 3.305425e-02
+9.325000e+02 5.250000e+01 5.250000e+01 2.094700e-01 1.978769e-02 1.908621e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.608800e-01 1.379026e-02 1.439896e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.078200e-01 1.139356e-02 8.991321e-03
+1.275000e+03 7.500000e+01 7.500000e+01 6.716700e-02 8.280411e-03 9.436231e-03
+1.425000e+03 7.500000e+01 7.500000e+01 3.576800e-02 4.113652e-03 5.353288e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.268900e-02 1.810116e-03 1.969695e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.874500e-03 5.472270e-04 3.790943e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.281500e-04 5.981958e-05 5.863538e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d102-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d102-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 8.926900e-01 1.097600e-01 1.143400e-01
+5.800000e+02 3.500000e+01 3.500000e+01 7.337500e-01 1.014800e-01 8.296000e-02
+6.550000e+02 4.000000e+01 4.000000e+01 5.519100e-01 7.098800e-02 8.231900e-02
+7.400000e+02 4.500000e+01 4.500000e+01 4.024800e-01 5.963000e-02 4.281100e-02
+8.325000e+02 4.750000e+01 4.750000e+01 2.878200e-01 3.697700e-02 3.155200e-02
+9.325000e+02 5.250000e+01 5.250000e+01 1.928500e-01 2.772000e-02 2.245800e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.325200e-01 1.797200e-02 2.089800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.010400e-02 1.147200e-02 1.275000e-02
+1.275000e+03 7.500000e+01 7.500000e+01 5.754100e-02 9.250100e-03 6.763600e-03
+1.425000e+03 7.500000e+01 7.500000e+01 3.471200e-02 6.809400e-03 3.559500e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.282500e-02 2.094600e-03 1.681900e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.964300e-03 3.959000e-04 2.603600e-04
+3.350000e+03 6.500000e+02 6.500000e+02 8.538600e-05 2.888600e-05 3.188200e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d102-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d102-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 7.912600e-01 2.356300e-01 3.752800e-01
+5.800000e+02 3.500000e+01 3.500000e+01 6.453100e-01 1.925600e-01 3.074500e-01
+6.550000e+02 4.000000e+01 4.000000e+01 4.842500e-01 1.452600e-01 2.328600e-01
+7.400000e+02 4.500000e+01 4.500000e+01 3.578500e-01 1.081600e-01 1.736300e-01
+8.325000e+02 4.750000e+01 4.750000e+01 2.587800e-01 7.820000e-02 1.255000e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.784000e-01 5.458300e-02 8.843000e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.154500e-01 3.554900e-02 5.776300e-02
+1.150000e+03 5.000000e+01 5.000000e+01 8.036800e-02 2.520400e-02 4.130300e-02
+1.275000e+03 7.500000e+01 7.500000e+01 5.470900e-02 1.709300e-02 2.804100e-02
+1.425000e+03 7.500000e+01 7.500000e+01 3.236000e-02 1.008500e-02 1.650700e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.160000e-02 3.701900e-03 6.109700e-03
+2.350000e+03 3.500000e+02 3.500000e+02 1.766300e-03 5.795500e-04 9.795000e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.101300e-04 3.561700e-05 5.885600e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d102-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d102-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 9.442500e-01 2.217800e-01 4.539400e-01
+5.800000e+02 3.500000e+01 3.500000e+01 7.963900e-01 1.906200e-01 3.995700e-01
+6.550000e+02 4.000000e+01 4.000000e+01 6.077400e-01 1.409900e-01 3.183300e-01
+7.400000e+02 4.500000e+01 4.500000e+01 4.554500e-01 1.075800e-01 2.280200e-01
+8.325000e+02 4.750000e+01 4.750000e+01 3.439300e-01 8.882000e-02 1.511600e-01
+9.325000e+02 5.250000e+01 5.250000e+01 2.390100e-01 5.789500e-02 1.165400e-01
+1.042500e+03 5.750000e+01 5.750000e+01 1.645700e-01 3.763800e-02 7.879200e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.131400e-01 2.145700e-02 5.317100e-02
+1.275000e+03 7.500000e+01 7.500000e+01 7.820500e-02 1.773700e-02 3.477700e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.798500e-02 1.021600e-02 2.147800e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.914200e-02 3.778700e-03 1.006900e-02
+2.350000e+03 3.500000e+02 3.500000e+02 3.291400e-03 6.802200e-04 1.928200e-03
+3.350000e+03 6.500000e+02 6.500000e+02 2.228000e-04 4.651700e-05 7.725700e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d103-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d103-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.317100e+00 1.662208e-01 1.560145e-01
+6.250000e+01 1.250000e+01 1.250000e+01 2.377900e+00 2.383366e-01 2.360401e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.114900e+00 2.095572e-01 1.959945e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.526800e+00 1.335790e-01 1.361221e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.068200e+00 1.148175e-01 1.100250e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.622300e-01 5.386598e-02 5.118310e-02
+2.625000e+02 3.750000e+01 3.750000e+01 1.878500e-01 2.124380e-02 2.260063e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.102300e-02 3.707778e-03 3.772826e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d103-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d103-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.071500e+00 1.451000e-01 1.393100e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.905900e+00 2.717500e-01 2.225300e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.724400e+00 2.553500e-01 1.837400e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.339700e+00 1.915300e-01 1.716300e-01
+1.450000e+02 1.500000e+01 1.500000e+01 9.556800e-01 1.242400e-01 1.154100e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.041100e-01 6.082900e-02 7.070500e-02
+2.625000e+02 3.750000e+01 3.750000e+01 1.717100e-01 2.189300e-02 1.888900e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.539700e-02 1.907400e-03 2.367400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d103-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d103-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.025200e+00 3.016300e-01 4.789400e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.746600e+00 5.177800e-01 8.253500e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.552500e+00 4.687500e-01 7.514300e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.158900e+00 3.520200e-01 5.674900e-01
+1.450000e+02 1.500000e+01 1.500000e+01 8.005200e-01 2.489200e-01 4.060000e-01
+1.925000e+02 3.250000e+01 3.250000e+01 4.193600e-01 1.311100e-01 2.146000e-01
+2.625000e+02 3.750000e+01 3.750000e+01 1.452400e-01 4.550900e-02 7.417600e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.365700e-02 4.326000e-03 7.050100e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d103-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d103-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.344700e+00 3.459100e-01 6.262800e-01
+6.250000e+01 1.250000e+01 1.250000e+01 2.220100e+00 5.672400e-01 1.092600e+00
+8.750000e+01 1.250000e+01 1.250000e+01 1.986200e+00 3.963300e-01 1.002100e+00
+1.150000e+02 1.500000e+01 1.500000e+01 1.542700e+00 3.501400e-01 7.927800e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.062400e+00 2.263400e-01 5.405800e-01
+1.925000e+02 3.250000e+01 3.250000e+01 5.455000e-01 1.314700e-01 2.584200e-01
+2.625000e+02 3.750000e+01 3.750000e+01 1.862600e-01 3.796400e-02 9.110500e-02
+5.150000e+02 2.150000e+02 2.150000e+02 1.612200e-02 3.845700e-03 6.963700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d104-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d104-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 3.194600e+01 6.164026e+00 6.091542e+00
+4.500000e-01 1.500000e-01 1.500000e-01 6.906200e+01 1.111902e+01 1.017829e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.481600e+02 2.683081e+01 2.604132e+01
+7.500000e-01 5.000000e-02 5.000000e-02 4.602300e+02 3.992553e+01 4.030188e+01
+8.250000e-01 2.500000e-02 2.500000e-02 7.849300e+02 7.846769e+01 7.762066e+01
+8.750000e-01 2.500000e-02 2.500000e-02 9.958400e+02 9.472413e+01 9.582386e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.174000e+03 1.219903e+02 1.195064e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.279200e+03 1.442066e+02 1.373947e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d104-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d104-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 3.239300e+01 4.407000e+00 5.976200e+00
+4.500000e-01 1.500000e-01 1.500000e-01 8.260900e+01 9.607700e+00 1.179100e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.188800e+02 3.878000e+01 2.081300e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.970500e+02 5.861400e+01 5.088700e+01
+8.250000e-01 2.500000e-02 2.500000e-02 6.037600e+02 7.500900e+01 8.361700e+01
+8.750000e-01 2.500000e-02 2.500000e-02 7.792400e+02 1.042900e+02 9.046200e+01
+9.250000e-01 2.500000e-02 2.500000e-02 9.491400e+02 1.353100e+02 1.078500e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.055800e+03 1.328000e+02 1.232000e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d104-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d104-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 2.731600e+01 8.990000e+00 1.520300e+01
+4.500000e-01 1.500000e-01 1.500000e-01 6.230900e+01 2.007600e+01 3.337900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 1.658300e+02 5.206100e+01 8.514600e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.190700e+02 9.867400e+01 1.603500e+02
+8.250000e-01 2.500000e-02 2.500000e-02 5.245600e+02 1.583200e+02 2.538200e+02
+8.750000e-01 2.500000e-02 2.500000e-02 7.095700e+02 2.116700e+02 3.377500e+02
+9.250000e-01 2.500000e-02 2.500000e-02 9.207600e+02 2.723200e+02 4.330500e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.069500e+03 3.134300e+02 4.955400e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d104-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d104-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 2.823700e+01 5.189300e+00 1.595500e+01
+4.500000e-01 1.500000e-01 1.500000e-01 7.249300e+01 1.804100e+01 3.539900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.057000e+02 4.742000e+01 9.726900e+01
+7.500000e-01 5.000000e-02 5.000000e-02 4.332700e+02 9.266500e+01 2.147100e+02
+8.250000e-01 2.500000e-02 2.500000e-02 6.871700e+02 1.624200e+02 3.248100e+02
+8.750000e-01 2.500000e-02 2.500000e-02 9.404500e+02 2.333300e+02 4.317700e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.207400e+03 2.729700e+02 6.167700e+02
+9.750000e-01 2.500000e-02 2.500000e-02 1.421700e+03 3.464800e+02 7.012800e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d105-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d105-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.122000e+02 1.378747e+01 1.380599e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.315300e+02 1.435557e+01 1.417091e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.543200e+02 1.478781e+01 1.471536e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.444700e+02 1.466204e+01 1.458784e+01
+4.000000e+00 4.000000e-01 4.000000e-01 9.352000e+01 1.023297e+01 8.861253e+00
+4.800000e+00 4.000000e-01 4.000000e-01 2.163800e+01 3.713625e+00 3.160063e+00
+7.000000e+00 1.800000e+00 1.800000e+00 1.062500e+00 2.460275e-01 3.311533e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d105-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d105-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 8.968700e+01 1.057600e+01 1.083800e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.073600e+02 1.271300e+01 1.246500e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.206100e+02 1.716200e+01 1.310400e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.224300e+02 1.619400e+01 1.452800e+01
+4.000000e+00 4.000000e-01 4.000000e-01 8.254300e+01 1.173900e+01 1.258300e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.472600e+01 4.240800e+00 2.577700e+00
+7.000000e+00 1.800000e+00 1.800000e+00 1.010200e+00 2.236900e-01 1.725500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d105-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d105-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 9.278400e+01 2.746300e+01 4.342600e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.028200e+02 3.053500e+01 4.849000e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.096100e+02 3.273900e+01 5.223800e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.026800e+02 3.086600e+01 4.951700e+01
+4.000000e+00 4.000000e-01 4.000000e-01 6.834600e+01 2.109100e+01 3.436500e+01
+4.800000e+00 4.000000e-01 4.000000e-01 1.958400e+01 6.280600e+00 1.048600e+01
+7.000000e+00 1.800000e+00 1.800000e+00 8.589900e-01 2.893700e-01 4.949900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d105-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d105-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.159700e+02 2.875900e+01 5.190000e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.323700e+02 2.846600e+01 7.192100e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.396700e+02 3.409100e+01 6.664400e+01
+3.400000e+00 2.000000e-01 2.000000e-01 1.347400e+02 3.416600e+01 6.224300e+01
+4.000000e+00 4.000000e-01 4.000000e-01 9.042200e+01 1.947100e+01 4.696200e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.645300e+01 6.194500e+00 1.221300e+01
+7.000000e+00 1.800000e+00 1.800000e+00 1.209200e+00 2.682700e-01 5.639100e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d106-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d106-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.355200e+00 2.128349e-01 1.447406e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.765000e+00 2.276836e-01 2.227523e-01
+1.275000e+02 1.250000e+01 1.250000e+01 2.035400e+00 2.008478e-01 2.097645e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.991800e+00 1.870991e-01 1.673110e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.725900e+00 1.426544e-01 1.396621e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.369100e+00 1.107719e-01 1.099527e-01
+2.350000e+02 1.500000e+01 1.500000e+01 8.336300e-01 7.129823e-02 7.290835e-02
+2.650000e+02 1.500000e+01 1.500000e+01 5.613100e-01 5.021629e-02 5.395497e-02
+3.150000e+02 3.500000e+01 3.500000e+01 2.690200e-01 3.322067e-02 3.541971e-02
+4.150000e+02 6.500000e+01 6.500000e+01 6.887900e-02 1.398064e-02 1.388875e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.004300e-02 1.987628e-03 1.952282e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d106-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d106-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.308600e+00 1.926600e-01 1.876600e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.607900e+00 2.357600e-01 2.261800e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.717500e+00 2.507500e-01 2.160800e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.628200e+00 2.297500e-01 1.972400e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.423700e+00 1.929100e-01 1.677000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.068000e+00 1.444800e-01 1.143800e-01
+2.350000e+02 1.500000e+01 1.500000e+01 7.183400e-01 9.018700e-02 9.093100e-02
+2.650000e+02 1.500000e+01 1.500000e+01 4.689700e-01 6.093400e-02 4.755000e-02
+3.150000e+02 3.500000e+01 3.500000e+01 2.341500e-01 2.540800e-02 2.904400e-02
+4.150000e+02 6.500000e+01 6.500000e+01 6.382500e-02 7.698700e-03 9.501600e-03
+5.825000e+02 1.025000e+02 1.025000e+02 9.277700e-03 1.681800e-03 1.138000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d106-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d106-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.031500e+00 3.247300e-01 5.376400e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.285700e+00 3.935000e-01 6.393700e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.421100e+00 4.315900e-01 6.965200e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.428300e+00 4.300000e-01 6.900500e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.300400e+00 3.873100e-01 6.172100e-01
+2.050000e+02 1.500000e+01 1.500000e+01 9.809800e-01 2.952700e-01 4.743500e-01
+2.350000e+02 1.500000e+01 1.500000e+01 6.892200e-01 2.066300e-01 3.300400e-01
+2.650000e+02 1.500000e+01 1.500000e+01 4.874100e-01 1.468200e-01 2.336700e-01
+3.150000e+02 3.500000e+01 3.500000e+01 2.282500e-01 6.894600e-02 1.101900e-01
+4.150000e+02 6.500000e+01 6.500000e+01 6.858200e-02 2.065800e-02 3.296500e-02
+5.825000e+02 1.025000e+02 1.025000e+02 8.857500e-03 2.785100e-03 4.508500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d106-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d106-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 1.282000e+00 2.856700e-01 6.114500e-01
+1.050000e+02 1.000000e+01 1.000000e+01 1.691700e+00 4.555400e-01 8.108800e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.808800e+00 4.382900e-01 8.470800e-01
+1.525000e+02 1.250000e+01 1.250000e+01 1.790200e+00 4.345600e-01 9.083900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 1.650100e+00 3.842600e-01 8.355900e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.277600e+00 2.625100e-01 7.166600e-01
+2.350000e+02 1.500000e+01 1.500000e+01 9.316100e-01 1.882400e-01 4.509400e-01
+2.650000e+02 1.500000e+01 1.500000e+01 5.948100e-01 1.383300e-01 2.783100e-01
+3.150000e+02 3.500000e+01 3.500000e+01 3.283500e-01 8.045000e-02 1.330400e-01
+4.150000e+02 6.500000e+01 6.500000e+01 9.358300e-02 2.241700e-02 4.588500e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.479700e-02 3.010100e-03 6.567300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d107-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d107-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 9.110900e-01 1.588982e-01 1.548867e-01
+5.800000e+02 3.500000e+01 3.500000e+01 7.716400e-01 1.018759e-01 9.759468e-02
+6.550000e+02 4.000000e+01 4.000000e+01 5.921600e-01 7.745728e-02 8.440039e-02
+7.400000e+02 4.500000e+01 4.500000e+01 4.260100e-01 4.972377e-02 4.414964e-02
+8.325000e+02 4.750000e+01 4.750000e+01 3.207500e-01 3.728159e-02 3.134651e-02
+9.325000e+02 5.250000e+01 5.250000e+01 2.109000e-01 2.949601e-02 3.550327e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.450100e-01 1.674060e-02 2.071307e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.819000e-02 1.536497e-02 1.352539e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.642700e-02 1.940322e-02 1.038693e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.980900e-02 7.758158e-03 6.992196e-03
+1.750000e+03 2.500000e+02 2.500000e+02 2.265900e-02 3.901552e-03 4.085785e-03
+3.000000e+03 1.000000e+03 1.000000e+03 1.295800e-03 3.913357e-04 3.826879e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d107-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d107-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.749000e-01 6.962400e-02 7.161800e-02
+5.800000e+02 3.500000e+01 3.500000e+01 5.696800e-01 6.748400e-02 7.435200e-02
+6.550000e+02 4.000000e+01 4.000000e+01 4.559200e-01 6.081700e-02 4.467700e-02
+7.400000e+02 4.500000e+01 4.500000e+01 3.484500e-01 4.783200e-02 4.020400e-02
+8.325000e+02 4.750000e+01 4.750000e+01 2.588900e-01 4.026200e-02 3.184800e-02
+9.325000e+02 5.250000e+01 5.250000e+01 1.867500e-01 2.524300e-02 2.079800e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.329000e-01 1.810700e-02 1.948800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.485300e-02 1.387400e-02 1.198400e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.533400e-02 1.085500e-02 8.814600e-03
+1.425000e+03 7.500000e+01 7.500000e+01 4.172400e-02 5.692800e-03 5.957800e-03
+1.750000e+03 2.500000e+02 2.500000e+02 1.852500e-02 3.335100e-03 2.679400e-03
+3.000000e+03 1.000000e+03 1.000000e+03 1.532600e-03 2.376600e-04 2.115200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d107-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d107-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.933500e-01 2.056700e-01 3.275100e-01
+5.800000e+02 3.500000e+01 3.500000e+01 5.915400e-01 1.772200e-01 2.835800e-01
+6.550000e+02 4.000000e+01 4.000000e+01 4.668500e-01 1.406400e-01 2.255000e-01
+7.400000e+02 4.500000e+01 4.500000e+01 3.584700e-01 1.101100e-01 1.794000e-01
+8.325000e+02 4.750000e+01 4.750000e+01 2.709900e-01 8.322000e-02 1.345300e-01
+9.325000e+02 5.250000e+01 5.250000e+01 1.900500e-01 5.910400e-02 9.647700e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.331600e-01 4.170800e-02 6.846400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 9.995300e-02 3.139500e-02 5.163300e-02
+1.275000e+03 7.500000e+01 7.500000e+01 6.808800e-02 2.163600e-02 3.588400e-02
+1.425000e+03 7.500000e+01 7.500000e+01 4.331100e-02 1.395100e-02 2.331900e-02
+1.750000e+03 2.500000e+02 2.500000e+02 1.884200e-02 6.274900e-03 1.076900e-02
+3.000000e+03 1.000000e+03 1.000000e+03 1.560900e-03 5.455800e-04 9.647100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d107-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d107-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 6.985600e-01 1.620900e-01 3.070800e-01
+5.800000e+02 3.500000e+01 3.500000e+01 6.104800e-01 1.425200e-01 3.447700e-01
+6.550000e+02 4.000000e+01 4.000000e+01 4.834200e-01 1.095100e-01 2.226400e-01
+7.400000e+02 4.500000e+01 4.500000e+01 3.709300e-01 8.393800e-02 1.596900e-01
+8.325000e+02 4.750000e+01 4.750000e+01 2.861100e-01 6.263000e-02 1.323400e-01
+9.325000e+02 5.250000e+01 5.250000e+01 2.093300e-01 5.141200e-02 9.288200e-02
+1.042500e+03 5.750000e+01 5.750000e+01 1.469000e-01 2.522100e-02 7.490800e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.101900e-01 1.950300e-02 4.855200e-02
+1.275000e+03 7.500000e+01 7.500000e+01 8.093100e-02 1.666400e-02 2.972600e-02
+1.425000e+03 7.500000e+01 7.500000e+01 5.113300e-02 9.438600e-03 2.281700e-02
+1.750000e+03 2.500000e+02 2.500000e+02 2.359700e-02 5.260200e-03 9.532100e-03
+3.000000e+03 1.000000e+03 1.000000e+03 2.190700e-03 3.414200e-04 1.014400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d108-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d108-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.322900e+00 2.052019e-01 2.008205e-01
+6.250000e+01 1.250000e+01 1.250000e+01 2.274700e+00 3.189118e-01 3.174077e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.881600e+00 2.311125e-01 2.476128e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.126500e+00 1.507024e-01 1.157130e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.430300e-01 3.666611e-02 3.595725e-02
+6.000000e+02 3.000000e+02 3.000000e+02 8.547800e-03 3.085704e-03 3.089450e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d108-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d108-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 9.556900e-01 1.426000e-01 1.002700e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.632900e+00 2.089400e-01 1.928300e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.452100e+00 1.867900e-01 1.838100e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.005100e+00 1.299600e-01 1.279200e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.108300e-01 3.934900e-02 3.405800e-02
+6.000000e+02 3.000000e+02 3.000000e+02 1.116400e-02 1.334800e-03 1.773700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d108-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d108-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.020800e+00 3.047500e-01 4.887200e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.708300e+00 5.206200e-01 8.451500e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.481700e+00 4.521800e-01 7.315400e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.002800e+00 3.116200e-01 5.094200e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.148700e-01 9.850100e-02 1.610700e-01
+6.000000e+02 3.000000e+02 3.000000e+02 1.240100e-02 3.905500e-03 6.361600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d108-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d108-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+01 2.500000e+01 2.500000e+01 1.086100e+00 2.350100e-01 4.995300e-01
+6.250000e+01 1.250000e+01 1.250000e+01 1.846000e+00 4.406100e-01 7.994400e-01
+8.750000e+01 1.250000e+01 1.250000e+01 1.630600e+00 3.675200e-01 6.734600e-01
+1.300000e+02 3.000000e+01 3.000000e+01 1.076500e+00 2.144000e-01 5.511900e-01
+2.300000e+02 7.000000e+01 7.000000e+01 3.287400e-01 7.637500e-02 1.597300e-01
+6.000000e+02 3.000000e+02 3.000000e+02 1.247900e-02 2.462800e-03 5.497400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d109-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d109-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.427500e+01 1.496705e+01 9.122976e+00
+4.500000e-01 1.500000e-01 1.500000e-01 9.548000e+01 1.571207e+01 1.537634e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.600600e+02 2.651159e+01 2.948628e+01
+7.500000e-01 5.000000e-02 5.000000e-02 4.386300e+02 4.524406e+01 4.650106e+01
+8.500000e-01 5.000000e-02 5.000000e-02 7.594100e+02 9.625282e+01 9.274535e+01
+9.500000e-01 5.000000e-02 5.000000e-02 1.045600e+03 1.349422e+02 1.341298e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d109-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d109-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.609600e+01 6.268100e+00 4.698600e+00
+4.500000e-01 1.500000e-01 1.500000e-01 9.736800e+01 1.435600e+01 1.352900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.118900e+02 3.012500e+01 2.940000e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.577100e+02 4.684900e+01 3.778700e+01
+8.500000e-01 5.000000e-02 5.000000e-02 5.700600e+02 7.219900e+01 6.879200e+01
+9.500000e-01 5.000000e-02 5.000000e-02 7.844200e+02 1.002500e+02 8.880500e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d109-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d109-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.637100e+01 1.494500e+01 2.496500e+01
+4.500000e-01 1.500000e-01 1.500000e-01 9.160200e+01 2.926500e+01 4.862100e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.019100e+02 6.405400e+01 1.055700e+02
+7.500000e-01 5.000000e-02 5.000000e-02 3.559100e+02 1.112700e+02 1.826100e+02
+8.500000e-01 5.000000e-02 5.000000e-02 5.954700e+02 1.807200e+02 2.911900e+02
+9.500000e-01 5.000000e-02 5.000000e-02 8.576700e+02 2.551200e+02 4.074800e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d109-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d109-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 4.130600e+01 9.606300e+00 2.474900e+01
+4.500000e-01 1.500000e-01 1.500000e-01 8.626100e+01 1.905000e+01 4.357300e+01
+6.500000e-01 5.000000e-02 5.000000e-02 2.054500e+02 4.413400e+01 9.224000e+01
+7.500000e-01 5.000000e-02 5.000000e-02 3.810800e+02 7.425200e+01 1.830400e+02
+8.500000e-01 5.000000e-02 5.000000e-02 6.637100e+02 1.435700e+02 3.065000e+02
+9.500000e-01 5.000000e-02 5.000000e-02 9.604300e+02 2.219200e+02 4.183300e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d110-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d110-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.309600e+00 4.165370e-01 3.534697e-01
+1.275000e+02 1.250000e+01 1.250000e+01 2.097600e+00 2.465289e-01 2.532859e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.567900e+00 1.617279e-01 1.576783e-01
+2.200000e+02 3.000000e+01 3.000000e+01 7.374100e-01 6.806971e-02 6.868258e-02
+2.825000e+02 3.250000e+01 3.250000e+01 3.204600e-01 2.768212e-02 2.745194e-02
+3.525000e+02 3.750000e+01 3.750000e+01 1.097400e-01 1.318318e-02 1.399842e-02
+4.350000e+02 4.500000e+01 4.500000e+01 3.719100e-02 6.349371e-03 6.233725e-03
+5.825000e+02 1.025000e+02 1.025000e+02 8.869200e-03 2.721005e-03 2.612747e-03
+8.425000e+02 1.575000e+02 1.575000e+02 1.380300e-07 6.263013e-03 6.263008e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d110-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d110-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.788400e+00 3.026300e-01 1.971400e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.681200e+00 2.229900e-01 1.975800e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.250200e+00 1.363900e-01 1.673400e-01
+2.200000e+02 3.000000e+01 3.000000e+01 6.486800e-01 7.338500e-02 7.466100e-02
+2.825000e+02 3.250000e+01 3.250000e+01 2.656500e-01 3.279500e-02 3.134000e-02
+3.525000e+02 3.750000e+01 3.750000e+01 1.002500e-01 1.424200e-02 8.753200e-03
+4.350000e+02 4.500000e+01 4.500000e+01 3.307200e-02 4.235100e-03 5.561900e-03
+5.825000e+02 1.025000e+02 1.025000e+02 6.981200e-03 9.980600e-04 9.399700e-04
+8.425000e+02 1.575000e+02 1.575000e+02 5.993900e-04 1.825100e-04 1.561300e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d110-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d110-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.685600e+00 5.301900e-01 8.797400e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.672500e+00 5.137900e-01 8.347300e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.318500e+00 4.007900e-01 6.457800e-01
+2.200000e+02 3.000000e+01 3.000000e+01 7.110200e-01 2.143200e-01 3.436000e-01
+2.825000e+02 3.250000e+01 3.250000e+01 2.913200e-01 8.854600e-02 1.424500e-01
+3.525000e+02 3.750000e+01 3.750000e+01 1.122400e-01 3.456200e-02 5.565800e-02
+4.350000e+02 4.500000e+01 4.500000e+01 4.111900e-02 1.235000e-02 1.966000e-02
+5.825000e+02 1.025000e+02 1.025000e+02 9.051300e-03 2.747000e-03 4.374100e-03
+8.425000e+02 1.575000e+02 1.575000e+02 5.472200e-04 1.747300e-04 2.841000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d110-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d110-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.743200e+00 3.746100e-01 8.016600e-01
+1.275000e+02 1.250000e+01 1.250000e+01 1.693500e+00 4.213300e-01 7.914800e-01
+1.650000e+02 2.500000e+01 2.500000e+01 1.390000e+00 3.060800e-01 6.211300e-01
+2.200000e+02 3.000000e+01 3.000000e+01 7.808500e-01 1.474700e-01 4.022100e-01
+2.825000e+02 3.250000e+01 3.250000e+01 3.411600e-01 7.759400e-02 1.660200e-01
+3.525000e+02 3.750000e+01 3.750000e+01 1.373800e-01 3.107400e-02 5.632200e-02
+4.350000e+02 4.500000e+01 4.500000e+01 5.063200e-02 1.427800e-02 1.403200e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.128600e-02 2.130900e-03 5.189300e-03
+8.425000e+02 1.575000e+02 1.575000e+02 8.921200e-04 2.212200e-04 5.403600e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d111-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d111-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.934400e+00 2.047777e-01 2.060855e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.554500e+00 1.147123e-01 1.160608e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.148600e+00 7.958526e-02 7.788120e-02
+7.400000e+02 4.500000e+01 4.500000e+01 7.872700e-01 5.305027e-02 5.174950e-02
+8.325000e+02 4.750000e+01 4.750000e+01 5.362300e-01 4.052583e-02 3.776656e-02
+9.325000e+02 5.250000e+01 5.250000e+01 3.784800e-01 2.161550e-02 2.500310e-02
+1.042500e+03 5.750000e+01 5.750000e+01 2.505000e-01 1.974661e-02 1.394663e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.739800e-01 1.214582e-02 8.120632e-03
+1.275000e+03 7.500000e+01 7.500000e+01 1.133300e-01 7.347170e-03 7.403166e-03
+1.425000e+03 7.500000e+01 7.500000e+01 7.190800e-02 7.881528e-03 1.177839e-02
+1.750000e+03 2.500000e+02 2.500000e+02 3.443000e-02 3.375883e-03 3.932118e-03
+2.350000e+03 3.500000e+02 3.500000e+02 7.209200e-03 1.282826e-03 1.334459e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.041900e-03 2.878364e-04 2.626336e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d111-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d111-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.642100e+00 2.224900e-01 1.048000e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.280700e+00 1.377300e-01 1.273100e-01
+6.550000e+02 4.000000e+01 4.000000e+01 9.243800e-01 9.858100e-02 8.465500e-02
+7.400000e+02 4.500000e+01 4.500000e+01 6.538000e-01 7.784700e-02 5.199500e-02
+8.325000e+02 4.750000e+01 4.750000e+01 4.503400e-01 4.545300e-02 4.479600e-02
+9.325000e+02 5.250000e+01 5.250000e+01 3.181700e-01 3.284500e-02 2.535500e-02
+1.042500e+03 5.750000e+01 5.750000e+01 2.185000e-01 2.233400e-02 1.953400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.579900e-01 1.483300e-02 2.066600e-02
+1.275000e+03 7.500000e+01 7.500000e+01 1.090300e-01 9.760300e-03 9.055100e-03
+1.425000e+03 7.500000e+01 7.500000e+01 7.073300e-02 7.780500e-03 3.461500e-03
+1.750000e+03 2.500000e+02 2.500000e+02 3.316800e-02 2.504200e-03 2.777300e-03
+2.350000e+03 3.500000e+02 3.500000e+02 8.734700e-03 6.407600e-04 6.425400e-04
+3.350000e+03 6.500000e+02 6.500000e+02 1.212400e-03 1.337400e-04 1.543400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d111-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d111-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.880700e+00 4.180500e-01 6.047600e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.478800e+00 3.320800e-01 4.824600e-01
+6.550000e+02 4.000000e+01 4.000000e+01 1.064500e+00 2.412500e-01 3.519000e-01
+7.400000e+02 4.500000e+01 4.500000e+01 7.629200e-01 1.761300e-01 2.584000e-01
+8.325000e+02 4.750000e+01 4.750000e+01 5.197000e-01 1.209900e-01 1.789600e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.649800e-01 8.578500e-02 1.272200e-01
+1.042500e+03 5.750000e+01 5.750000e+01 2.483800e-01 5.903100e-02 8.813500e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.733800e-01 4.181800e-02 6.280800e-02
+1.275000e+03 7.500000e+01 7.500000e+01 1.198100e-01 2.886900e-02 4.345000e-02
+1.425000e+03 7.500000e+01 7.500000e+01 7.811100e-02 1.921100e-02 2.916800e-02
+1.750000e+03 2.500000e+02 2.500000e+02 3.568000e-02 8.919700e-03 1.364200e-02
+2.350000e+03 3.500000e+02 3.500000e+02 9.058400e-03 2.335400e-03 3.635200e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.192200e-03 3.207500e-04 5.047000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d111-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d111-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+5.225000e+02 2.250000e+01 2.250000e+01 1.628100e+00 2.993500e-01 6.745500e-01
+5.800000e+02 3.500000e+01 3.500000e+01 1.279400e+00 2.076000e-01 4.473400e-01
+6.550000e+02 4.000000e+01 4.000000e+01 9.358600e-01 1.605300e-01 3.396800e-01
+7.400000e+02 4.500000e+01 4.500000e+01 6.718400e-01 1.099100e-01 2.416500e-01
+8.325000e+02 4.750000e+01 4.750000e+01 4.790800e-01 7.642600e-02 1.506700e-01
+9.325000e+02 5.250000e+01 5.250000e+01 3.409300e-01 4.338300e-02 1.233500e-01
+1.042500e+03 5.750000e+01 5.750000e+01 2.365700e-01 3.459200e-02 7.409400e-02
+1.150000e+03 5.000000e+01 5.000000e+01 1.688300e-01 2.454700e-02 6.020900e-02
+1.275000e+03 7.500000e+01 7.500000e+01 1.199900e-01 1.771900e-02 4.314600e-02
+1.425000e+03 7.500000e+01 7.500000e+01 8.160500e-02 1.549200e-02 1.858400e-02
+1.750000e+03 2.500000e+02 2.500000e+02 3.742900e-02 5.936600e-03 1.075600e-02
+2.350000e+03 3.500000e+02 3.500000e+02 9.699000e-03 1.718800e-03 2.130700e-03
+3.350000e+03 6.500000e+02 6.500000e+02 1.324400e-03 2.172600e-04 3.806100e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d112-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d112-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.579600e+00 2.711065e-01 2.643542e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.958800e+00 5.026961e-01 5.257734e-01
+6.250000e+01 1.250000e+01 1.250000e+01 4.334200e+00 3.792103e-01 3.718256e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.998200e+00 2.164359e-01 2.116842e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.979600e+00 1.334556e-01 1.287057e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.492000e+00 1.237087e-01 1.085712e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.918100e-01 5.857638e-02 6.881132e-02
+2.250000e+02 3.500000e+01 3.500000e+01 4.240200e-01 4.365110e-02 4.182401e-02
+3.250000e+02 6.500000e+01 6.500000e+01 9.793900e-02 1.567364e-02 1.537346e-02
+6.450000e+02 2.550000e+02 2.550000e+02 5.061200e-03 1.404259e-03 1.386970e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d112-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d112-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.804400e+00 2.658700e-01 6.646200e-02
+3.750000e+01 1.250000e+01 1.250000e+01 3.770700e+00 3.970400e-01 3.774700e-01
+6.250000e+01 1.250000e+01 1.250000e+01 3.474700e+00 3.558700e-01 3.319800e-01
+8.750000e+01 1.250000e+01 1.250000e+01 2.670600e+00 2.791500e-01 2.253000e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.902400e+00 1.977700e-01 1.693700e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.329700e+00 1.605800e-01 1.222500e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.809000e-01 8.616900e-02 8.474500e-02
+2.250000e+02 3.500000e+01 3.500000e+01 4.329000e-01 4.424100e-02 3.108600e-02
+3.250000e+02 6.500000e+01 6.500000e+01 1.126000e-01 1.057300e-02 1.004400e-02
+6.450000e+02 2.550000e+02 2.550000e+02 6.649600e-03 7.184800e-04 4.637200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d112-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d112-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 2.121400e+00 4.360100e-01 6.128600e-01
+3.750000e+01 1.250000e+01 1.250000e+01 4.193800e+00 9.078900e-01 1.303500e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.752500e+00 8.527900e-01 1.247000e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.964300e+00 6.888600e-01 1.015400e+00
+1.150000e+02 1.500000e+01 1.500000e+01 2.143700e+00 5.061400e-01 7.530900e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.526300e+00 3.652700e-01 5.453000e-01
+1.750000e+02 1.500000e+01 1.500000e+01 1.068700e+00 2.598600e-01 3.887800e-01
+2.250000e+02 3.500000e+01 3.500000e+01 5.398000e-01 1.320000e-01 1.977300e-01
+3.250000e+02 6.500000e+01 6.500000e+01 1.535300e-01 3.824600e-02 5.733000e-02
+6.450000e+02 2.550000e+02 2.550000e+02 1.039400e-02 2.702600e-03 4.093300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d112-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d112-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 1.856200e+00 1.978500e-01 6.439900e-01
+3.750000e+01 1.250000e+01 1.250000e+01 3.939000e+00 6.173000e-01 1.379000e+00
+6.250000e+01 1.250000e+01 1.250000e+01 3.624400e+00 5.748400e-01 1.373800e+00
+8.750000e+01 1.250000e+01 1.250000e+01 2.762400e+00 4.109300e-01 9.952400e-01
+1.150000e+02 1.500000e+01 1.500000e+01 1.951300e+00 3.472300e-01 6.723300e-01
+1.450000e+02 1.500000e+01 1.500000e+01 1.344600e+00 2.294300e-01 4.235100e-01
+1.750000e+02 1.500000e+01 1.500000e+01 8.966700e-01 1.489700e-01 3.301800e-01
+2.250000e+02 3.500000e+01 3.500000e+01 4.410700e-01 8.725500e-02 1.531300e-01
+3.250000e+02 6.500000e+01 6.500000e+01 1.184800e-01 2.013000e-02 3.517000e-02
+6.450000e+02 2.550000e+02 2.550000e+02 8.714200e-03 2.430900e-03 2.757300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d113-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d113-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 5.586400e+01 1.118706e+01 1.104381e+01
+3.500000e-01 5.000000e-02 5.000000e-02 7.833700e+01 1.351436e+01 1.384003e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.288400e+02 1.549411e+01 1.432772e+01
+5.500000e-01 5.000000e-02 5.000000e-02 2.049900e+02 1.895132e+01 2.163838e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.402900e+02 3.049171e+01 2.859075e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.767000e+02 4.588403e+01 4.887892e+01
+7.750000e-01 2.500000e-02 2.500000e-02 7.672700e+02 5.741062e+01 5.452588e+01
+8.250000e-01 2.500000e-02 2.500000e-02 1.143300e+03 8.074666e+01 7.674454e+01
+8.750000e-01 2.500000e-02 2.500000e-02 1.653700e+03 1.302137e+02 1.240733e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.228500e+03 1.588063e+02 1.556113e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.867300e+03 2.246193e+02 2.329989e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d113-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d113-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 6.373000e+01 7.492800e+00 7.065600e+00
+3.500000e-01 5.000000e-02 5.000000e-02 8.990700e+01 1.271000e+01 1.286600e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.226300e+02 1.766100e+01 1.461900e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.825600e+02 1.828600e+01 1.752200e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.127800e+02 3.363300e+01 2.949200e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.867400e+02 5.180100e+01 6.072000e+01
+7.750000e-01 2.500000e-02 2.500000e-02 6.810400e+02 7.480700e+01 5.491100e+01
+8.250000e-01 2.500000e-02 2.500000e-02 9.436000e+02 9.818500e+01 8.198000e+01
+8.750000e-01 2.500000e-02 2.500000e-02 1.323700e+03 1.334200e+02 9.886700e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.792900e+03 1.825600e+02 1.661600e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.268900e+03 2.638000e+02 1.420800e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d113-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d113-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 7.362100e+01 1.803800e+01 2.728200e+01
+3.500000e-01 5.000000e-02 5.000000e-02 1.007000e+02 2.448200e+01 3.672200e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.347300e+02 3.243200e+01 4.847100e+01
+5.500000e-01 5.000000e-02 5.000000e-02 2.064100e+02 5.044600e+01 7.559700e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.389400e+02 8.167600e+01 1.224700e+02
+7.250000e-01 2.500000e-02 2.500000e-02 5.284200e+02 1.264000e+02 1.881400e+02
+7.750000e-01 2.500000e-02 2.500000e-02 7.345100e+02 1.744500e+02 2.595400e+02
+8.250000e-01 2.500000e-02 2.500000e-02 1.043000e+03 2.465300e+02 3.651400e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.480000e+03 3.411800e+02 5.011000e+02
+9.250000e-01 2.500000e-02 2.500000e-02 2.107200e+03 4.715700e+02 6.848300e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.724500e+03 5.878600e+02 8.420200e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d113-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d113-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-01 1.500000e-01 1.500000e-01 6.158000e+01 1.220800e+01 2.139600e+01
+3.500000e-01 5.000000e-02 5.000000e-02 8.181400e+01 1.449300e+01 3.341900e+01
+4.500000e-01 5.000000e-02 5.000000e-02 1.147200e+02 2.020900e+01 3.300600e+01
+5.500000e-01 5.000000e-02 5.000000e-02 1.722700e+02 3.036500e+01 5.917900e+01
+6.500000e-01 5.000000e-02 5.000000e-02 3.023600e+02 5.512700e+01 8.862700e+01
+7.250000e-01 2.500000e-02 2.500000e-02 4.652900e+02 7.566200e+01 1.763100e+02
+7.750000e-01 2.500000e-02 2.500000e-02 6.752300e+02 1.073700e+02 2.398400e+02
+8.250000e-01 2.500000e-02 2.500000e-02 9.776800e+02 1.698200e+02 3.293100e+02
+8.750000e-01 2.500000e-02 2.500000e-02 1.399600e+03 2.173500e+02 5.034200e+02
+9.250000e-01 2.500000e-02 2.500000e-02 1.938600e+03 3.075400e+02 6.884800e+02
+9.750000e-01 2.500000e-02 2.500000e-02 2.453700e+03 3.440500e+02 8.884500e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d114-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d114-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.269800e+02 8.348051e+00 8.261689e+00
+2.600000e+00 2.000000e-01 2.000000e-01 1.721100e+02 1.090471e+01 1.051043e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.081400e+02 1.294466e+01 1.299410e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.453600e+02 1.571388e+01 1.569201e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.530200e+02 1.746229e+01 1.794819e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.623600e+02 1.267874e+01 1.194071e+01
+4.600000e+00 2.000000e-01 2.000000e-01 9.276200e+01 7.698652e+00 7.934809e+00
+5.000000e+00 2.000000e-01 2.000000e-01 5.314900e+01 5.404704e+00 5.484141e+00
+5.800000e+00 6.000000e-01 6.000000e-01 1.617900e+01 1.942031e+00 2.003112e+00
+7.600000e+00 1.200000e+00 1.200000e+00 5.693000e-01 2.767259e-01 2.785675e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d114-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d114-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.076800e+02 1.043800e+01 8.709800e+00
+2.600000e+00 2.000000e-01 2.000000e-01 1.414800e+02 1.430800e+01 1.121600e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.825800e+02 2.318800e+01 8.498100e+00
+3.400000e+00 2.000000e-01 2.000000e-01 2.124500e+02 2.186700e+01 2.008200e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.062300e+02 2.360800e+01 1.781600e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.347600e+02 1.579900e+01 1.281300e+01
+4.600000e+00 2.000000e-01 2.000000e-01 8.099200e+01 8.587900e+00 1.024600e+01
+5.000000e+00 2.000000e-01 2.000000e-01 4.632300e+01 3.728200e+00 5.458600e+00
+5.800000e+00 6.000000e-01 6.000000e-01 1.523900e+01 1.658400e+00 1.293000e+00
+7.600000e+00 1.200000e+00 1.200000e+00 6.115400e-01 5.622500e-02 1.297900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d114-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d114-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.576800e+02 3.702000e+01 5.438600e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.890800e+02 4.376200e+01 6.410100e+01
+3.000000e+00 2.000000e-01 2.000000e-01 2.189000e+02 5.019500e+01 7.340100e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.361200e+02 5.356900e+01 7.828900e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.142900e+02 4.805700e+01 7.020000e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.379900e+02 3.135400e+01 4.597100e+01
+4.600000e+00 2.000000e-01 2.000000e-01 8.136100e+01 1.880900e+01 2.809400e+01
+5.000000e+00 2.000000e-01 2.000000e-01 4.554800e+01 1.057700e+01 1.586100e+01
+5.800000e+00 6.000000e-01 6.000000e-01 1.437000e+01 3.448400e+00 5.234100e+00
+7.600000e+00 1.200000e+00 1.200000e+00 5.877800e-01 1.400700e-01 2.165900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d114-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d114-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e+00 2.000000e-01 2.000000e-01 1.217000e+02 2.136800e+01 5.508500e+01
+2.600000e+00 2.000000e-01 2.000000e-01 1.570500e+02 2.875600e+01 5.705200e+01
+3.000000e+00 2.000000e-01 2.000000e-01 1.931000e+02 3.311000e+01 6.632700e+01
+3.400000e+00 2.000000e-01 2.000000e-01 2.192100e+02 3.491800e+01 7.817500e+01
+3.800000e+00 2.000000e-01 2.000000e-01 2.015900e+02 3.189300e+01 6.867400e+01
+4.200000e+00 2.000000e-01 2.000000e-01 1.315700e+02 2.023700e+01 4.475300e+01
+4.600000e+00 2.000000e-01 2.000000e-01 7.956000e+01 1.362300e+01 2.580300e+01
+5.000000e+00 2.000000e-01 2.000000e-01 4.674200e+01 2.718300e+00 1.337300e+01
+5.800000e+00 6.000000e-01 6.000000e-01 1.587400e+01 2.351900e+00 3.766100e+00
+7.600000e+00 1.200000e+00 1.200000e+00 7.667600e-01 5.681500e-02 1.605200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d115-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d115-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 4.665800e+00 6.678500e-01 6.858559e-01
+1.050000e+02 1.000000e+01 1.000000e+01 4.712300e+00 4.874926e-01 5.099653e-01
+1.275000e+02 1.250000e+01 1.250000e+01 4.073500e+00 3.278462e-01 3.091421e-01
+1.525000e+02 1.250000e+01 1.250000e+01 3.179200e+00 1.990791e-01 1.957019e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.453400e+00 1.378531e-01 1.350295e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.734100e+00 8.475521e-02 7.626382e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.042200e+00 5.064959e-02 5.032267e-02
+2.650000e+02 1.500000e+01 1.500000e+01 6.199300e-01 5.535075e-02 5.525754e-02
+2.975000e+02 1.750000e+01 1.750000e+01 3.973900e-01 2.747221e-02 2.414900e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.201800e-01 1.781863e-02 1.807301e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.403800e-01 1.432198e-02 1.458703e-02
+4.350000e+02 4.500000e+01 4.500000e+01 5.246900e-02 7.396627e-03 7.142820e-03
+5.825000e+02 1.025000e+02 1.025000e+02 9.758700e-03 1.920456e-03 1.968488e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d115-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d115-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.432300e+00 3.867900e-01 4.608600e-01
+1.050000e+02 1.000000e+01 1.000000e+01 3.795000e+00 5.281400e-01 3.132500e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.426400e+00 3.683200e-01 3.154800e-01
+1.525000e+02 1.250000e+01 1.250000e+01 2.839700e+00 3.036700e-01 2.007900e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.191500e+00 2.194300e-01 1.954000e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.537100e+00 1.514900e-01 1.093400e-01
+2.350000e+02 1.500000e+01 1.500000e+01 9.712100e-01 1.018300e-01 6.519200e-02
+2.650000e+02 1.500000e+01 1.500000e+01 6.008100e-01 5.279200e-02 5.211700e-02
+2.975000e+02 1.750000e+01 1.750000e+01 3.638600e-01 3.233400e-02 2.857900e-02
+3.325000e+02 1.750000e+01 1.750000e+01 2.147700e-01 1.950300e-02 1.533300e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.244700e-01 1.198400e-02 1.009600e-02
+4.350000e+02 4.500000e+01 4.500000e+01 5.540200e-02 5.604400e-03 3.732800e-03
+5.825000e+02 1.025000e+02 1.025000e+02 1.054900e-02 1.160700e-03 1.025300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d115-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d115-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.274700e+00 7.190500e-01 1.045400e+00
+1.050000e+02 1.000000e+01 1.000000e+01 3.733000e+00 8.290900e-01 1.209400e+00
+1.275000e+02 1.250000e+01 1.250000e+01 3.642900e+00 8.199300e-01 1.195500e+00
+1.525000e+02 1.250000e+01 1.250000e+01 3.233700e+00 7.320600e-01 1.067800e+00
+1.775000e+02 1.250000e+01 1.250000e+01 2.694400e+00 6.155400e-01 9.005700e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.937000e+00 4.512200e-01 6.646500e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.280800e+00 3.024400e-01 4.471100e-01
+2.650000e+02 1.500000e+01 1.500000e+01 8.154200e-01 1.955600e-01 2.906500e-01
+2.975000e+02 1.750000e+01 1.750000e+01 5.032500e-01 1.230400e-01 1.837300e-01
+3.325000e+02 1.750000e+01 1.750000e+01 3.077000e-01 7.597300e-02 1.138100e-01
+3.700000e+02 2.000000e+01 2.000000e+01 1.843100e-01 4.597500e-02 6.892100e-02
+4.350000e+02 4.500000e+01 4.500000e+01 8.196700e-02 2.092900e-02 3.159100e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.661400e-02 4.346800e-03 6.610300e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d115-x01-y04
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d115-x01-y04
+Title: doi:10.17182/hepdata.76505.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+8.750000e+01 7.500000e+00 7.500000e+00 3.247700e+00 3.663900e-01 1.274300e+00
+1.050000e+02 1.000000e+01 1.000000e+01 3.572600e+00 5.606600e-01 1.204500e+00
+1.275000e+02 1.250000e+01 1.250000e+01 3.416600e+00 5.932200e-01 1.058400e+00
+1.525000e+02 1.250000e+01 1.250000e+01 2.991300e+00 4.270100e-01 1.017700e+00
+1.775000e+02 1.250000e+01 1.250000e+01 2.347200e+00 3.826900e-01 8.677800e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.681400e+00 2.743900e-01 6.893000e-01
+2.350000e+02 1.500000e+01 1.500000e+01 1.053300e+00 1.782000e-01 3.952300e-01
+2.650000e+02 1.500000e+01 1.500000e+01 6.836400e-01 1.242200e-01 2.270900e-01
+2.975000e+02 1.750000e+01 1.750000e+01 4.186800e-01 7.698900e-02 1.473300e-01
+3.325000e+02 1.750000e+01 1.750000e+01 2.620500e-01 5.768200e-02 7.882800e-02
+3.700000e+02 2.000000e+01 2.000000e+01 1.516800e-01 3.156300e-02 4.312400e-02
+4.350000e+02 4.500000e+01 4.500000e+01 6.819800e-02 1.272900e-02 2.067600e-02
+5.825000e+02 1.025000e+02 1.025000e+02 1.469100e-02 2.229200e-03 5.345600e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d116-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d116-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t116
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.023600e-01 1.130462e-01 1.130462e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.684200e+00 3.060627e-01 3.060627e-01
+9.250000e-01 2.500000e-02 2.500000e-02 5.084000e+00 7.082546e-01 7.082546e-01
+9.750000e-01 2.500000e-02 2.500000e-02 6.746000e+00 1.974846e+00 1.974846e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d116-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d116-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t116
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.365400e-01 0.000000e+00 5.099400e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.739800e+00 3.354900e-02 3.581100e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.069900e+00 3.253400e-01 0.000000e+00
+9.750000e-01 2.500000e-02 2.500000e-02 5.659300e+00 5.351000e-01 4.739900e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d116-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d116-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t116
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.306000e-01 1.453200e-02 1.676400e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.810800e+00 7.618100e-02 8.004900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.103200e+00 2.293600e-01 2.443100e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.425300e+00 2.637300e-01 2.731000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d117-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d117-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t117
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.257200e-03 2.465346e-03 2.465346e-03
+1.400000e+02 2.500000e+01 2.500000e+01 6.199800e-03 1.093463e-03 1.093463e-03
+1.925000e+02 2.750000e+01 2.750000e+01 3.385000e-03 6.762096e-04 6.762096e-04
+2.500000e+02 3.000000e+01 3.000000e+01 1.877600e-03 5.037593e-04 5.037593e-04
+3.575000e+02 7.750000e+01 7.750000e+01 5.946800e-04 2.631693e-04 2.631693e-04
+5.600000e+02 1.250000e+02 1.250000e+02 1.800100e-04 1.291442e-04 1.291442e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d117-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d117-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t117
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.239800e-03 5.017000e-04 9.408800e-05
+1.400000e+02 2.500000e+01 2.500000e+01 4.804500e-03 2.900700e-05 4.066500e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.669900e-03 1.729000e-04 7.828200e-05
+2.500000e+02 3.000000e+01 3.000000e+01 2.402700e-03 2.034300e-04 0.000000e+00
+3.575000e+02 7.750000e+01 7.750000e+01 1.185100e-03 2.747100e-05 1.869300e-04
+5.600000e+02 1.250000e+02 1.250000e+02 3.267100e-04 3.025200e-05 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d117-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d117-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t117
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.768300e-03 2.965100e-04 3.865600e-04
+1.400000e+02 2.500000e+01 2.500000e+01 5.255000e-03 2.604300e-04 3.155800e-04
+1.925000e+02 2.750000e+01 2.750000e+01 3.835400e-03 2.121300e-04 2.214200e-04
+2.500000e+02 3.000000e+01 3.000000e+01 2.379100e-03 1.599600e-04 1.621900e-04
+3.575000e+02 7.750000e+01 7.750000e+01 1.025100e-03 6.532900e-05 7.927300e-05
+5.600000e+02 1.250000e+02 1.250000e+02 2.311300e-04 2.442600e-05 3.342300e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d118-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d118-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t118
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.892900e+00 7.182502e-01 7.182502e-01
+3.000000e-01 1.000000e-01 1.000000e-01 1.680700e+00 4.740168e-01 4.740168e-01
+7.000000e-01 3.000000e-01 3.000000e-01 1.421300e-01 2.328305e-01 2.328305e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d118-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d118-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t118
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.780400e+00 2.156200e-01 2.168200e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.659500e+00 1.473200e-01 3.328400e-02
+7.000000e-01 3.000000e-01 3.000000e-01 1.867100e-01 8.866000e-03 1.235300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d118-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d118-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t118
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.804200e+00 9.483400e-02 9.917100e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.670100e+00 7.318600e-02 7.585200e-02
+7.000000e-01 3.000000e-01 3.000000e-01 1.752300e-01 1.368700e-02 1.493600e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d119-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d119-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t119
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.358900e-01 2.310755e-01 2.310755e-01
+1.000000e+00 5.000000e-01 5.000000e-01 8.261700e-02 1.109725e-01 1.109725e-01
+5.000000e+00 3.500000e+00 3.500000e+00 8.149600e-02 1.171497e-01 1.171497e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d119-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d119-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t119
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.871300e-01 5.594200e-03 3.429900e-03
+1.000000e+00 5.000000e-01 5.000000e-01 9.468100e-02 2.927000e-03 4.937900e-03
+5.000000e+00 3.500000e+00 3.500000e+00 1.819300e-02 5.601600e-04 3.261200e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d119-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d119-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t119
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.835900e-01 2.379900e-02 2.432100e-02
+1.000000e+00 5.000000e-01 5.000000e-01 8.941800e-02 7.570800e-03 8.527600e-03
+5.000000e+00 3.500000e+00 3.500000e+00 2.699100e-02 4.159500e-03 5.133800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d120-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d120-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t120
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 2.066400e-03 3.387979e-04 3.387979e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.585900e-03 1.985014e-04 1.985014e-04
+1.275000e+03 7.500000e+01 7.500000e+01 1.109000e-03 1.666473e-04 1.666473e-04
+1.425000e+03 7.500000e+01 7.500000e+01 7.989400e-04 1.911995e-04 1.911995e-04
+1.750000e+03 2.500000e+02 2.500000e+02 4.819700e-04 8.001193e-05 8.001193e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.159600e-04 2.753683e-05 2.753683e-05
+3.350000e+03 6.500000e+02 6.500000e+02 2.032200e-05 7.512427e-06 7.512427e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d120-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d120-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t120
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.776800e-03 1.456400e-04 1.308500e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.454200e-03 9.904800e-05 1.735200e-04
+1.275000e+03 7.500000e+01 7.500000e+01 1.146000e-03 0.000000e+00 9.799000e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.653700e-04 3.626500e-05 0.000000e+00
+1.750000e+03 2.500000e+02 2.500000e+02 4.798000e-04 1.186900e-05 8.028800e-06
+2.350000e+03 3.500000e+02 3.500000e+02 1.508700e-04 5.670100e-06 1.065200e-05
+3.350000e+03 6.500000e+02 6.500000e+02 2.284100e-05 2.336100e-06 2.329000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d120-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d120-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t120
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.704200e-03 7.203900e-05 7.770800e-05
+1.150000e+03 5.000000e+01 5.000000e+01 1.407700e-03 6.547200e-05 6.820500e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.136800e-03 4.804000e-05 5.452800e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.539800e-04 4.163800e-05 4.429600e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.888400e-04 1.725500e-05 1.779300e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.612200e-04 8.374800e-06 9.443100e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.532300e-05 2.435500e-06 3.029600e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d121-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d121-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t121
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 5.257200e-03 6.442300e-04 6.442300e-04
+3.750000e+01 1.250000e+01 1.250000e+01 9.913900e-03 1.177899e-03 1.177899e-03
+6.250000e+01 1.250000e+01 1.250000e+01 8.067000e-03 7.212043e-04 7.212043e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.753700e-03 6.128160e-04 6.128160e-04
+1.300000e+02 3.000000e+01 3.000000e+01 2.662800e-03 4.035903e-04 4.035903e-04
+2.100000e+02 5.000000e+01 5.000000e+01 7.339100e-04 3.123464e-04 3.123464e-04
+3.775000e+02 1.175000e+02 1.175000e+02 1.642100e-04 5.264875e-05 5.264875e-05
+6.975000e+02 2.025000e+02 2.025000e+02 8.526300e-06 1.036673e-05 1.036673e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d121-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d121-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t121
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.495700e-03 0.000000e+00 1.008900e-03
+3.750000e+01 1.250000e+01 1.250000e+01 7.123200e-03 2.261500e-04 6.968700e-05
+6.250000e+01 1.250000e+01 1.250000e+01 6.530500e-03 1.064200e-04 6.587700e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.283000e-03 1.991700e-04 3.218000e-05
+1.300000e+02 3.000000e+01 3.000000e+01 3.408700e-03 5.727800e-05 0.000000e+00
+2.100000e+02 5.000000e+01 5.000000e+01 1.473500e-03 8.284200e-05 0.000000e+00
+3.775000e+02 1.175000e+02 1.175000e+02 3.184400e-04 8.217900e-06 8.099800e-05
+6.975000e+02 2.025000e+02 2.025000e+02 3.082200e-05 3.614800e-06 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d121-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d121-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t121
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e+01 1.250000e+01 1.250000e+01 3.766100e-03 2.140500e-04 2.350700e-04
+3.750000e+01 1.250000e+01 1.250000e+01 7.678500e-03 3.056400e-04 3.240100e-04
+6.250000e+01 1.250000e+01 1.250000e+01 6.720100e-03 2.859300e-04 3.185400e-04
+8.750000e+01 1.250000e+01 1.250000e+01 5.420200e-03 2.567900e-04 2.766100e-04
+1.300000e+02 3.000000e+01 3.000000e+01 3.466100e-03 1.325500e-04 1.401200e-04
+2.100000e+02 5.000000e+01 5.000000e+01 1.389800e-03 6.501600e-05 6.730900e-05
+3.775000e+02 1.175000e+02 1.175000e+02 2.443900e-04 1.778500e-05 2.066400e-05
+6.975000e+02 2.025000e+02 2.025000e+02 1.481800e-05 3.335900e-06 3.868100e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d122-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d122-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t122
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.128100e-01 6.931408e-02 6.931408e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.292600e+00 1.754933e-01 1.754933e-01
+8.500000e-01 5.000000e-02 5.000000e-02 2.849300e+00 2.906862e-01 2.906862e-01
+9.250000e-01 2.500000e-02 2.500000e-02 4.428100e+00 4.306034e-01 4.306034e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.708900e+00 8.452775e-01 8.452775e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d122-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d122-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t122
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.587700e-01 5.176900e-03 2.325000e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.197200e+00 6.864700e-02 0.000000e+00
+8.500000e-01 5.000000e-02 5.000000e-02 2.376700e+00 5.536800e-02 0.000000e+00
+9.250000e-01 2.500000e-02 2.500000e-02 3.964500e+00 1.953300e-02 3.789900e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.264900e+00 1.530600e-01 2.724500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d122-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d122-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t122
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.381100e-01 1.017100e-02 1.108400e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.219100e+00 6.088900e-02 6.469100e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.467100e+00 8.661800e-02 9.201500e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.032300e+00 1.566000e-01 1.788000e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.261800e+00 1.788900e-01 1.903600e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d123-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d123-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t123
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 7.847200e-02 2.251447e-02 2.251447e-02
+3.200000e+00 4.000000e-01 4.000000e-01 1.706800e-01 2.670302e-02 2.670302e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.068800e-01 3.931611e-02 3.931611e-02
+4.200000e+00 2.000000e-01 2.000000e-01 2.929200e-01 7.162762e-02 7.162762e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.695400e-01 5.304497e-02 5.304497e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.352300e-01 7.909049e-02 7.909049e-02
+7.000000e+00 1.800000e+00 1.800000e+00 7.745700e-02 1.941613e-02 1.941613e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d123-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d123-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t123
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 6.834100e-02 2.985400e-03 4.022800e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.694500e-01 9.073300e-03 2.084000e-02
+3.800000e+00 2.000000e-01 2.000000e-01 2.806500e-01 1.497700e-02 1.495200e-04
+4.200000e+00 2.000000e-01 2.000000e-01 3.504300e-01 1.630900e-02 2.860300e-02
+4.600000e+00 2.000000e-01 2.000000e-01 3.899700e-01 1.044300e-03 7.664500e-03
+5.000000e+00 2.000000e-01 2.000000e-01 3.913300e-01 1.002500e-02 4.957900e-02
+7.000000e+00 1.800000e+00 1.800000e+00 6.800400e-02 3.137100e-03 9.999400e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d123-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d123-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t123
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 5.412600e-02 4.536000e-03 5.975800e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.451400e-01 7.427700e-03 9.474700e-03
+3.800000e+00 2.000000e-01 2.000000e-01 2.525900e-01 1.385800e-02 1.670600e-02
+4.200000e+00 2.000000e-01 2.000000e-01 3.316000e-01 1.587800e-02 1.669200e-02
+4.600000e+00 2.000000e-01 2.000000e-01 4.138100e-01 1.773700e-02 2.019600e-02
+5.000000e+00 2.000000e-01 2.000000e-01 4.121500e-01 1.770100e-02 2.105400e-02
+7.000000e+00 1.800000e+00 1.800000e+00 7.681400e-02 2.547300e-03 3.641800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d124-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d124-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t124
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.391500e-03 1.374241e-03 1.374241e-03
+1.275000e+02 1.250000e+01 1.250000e+01 7.056900e-03 7.344399e-04 7.344399e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.575600e-03 6.293049e-04 6.293049e-04
+1.775000e+02 1.250000e+01 1.250000e+01 2.875100e-03 4.954216e-04 4.954216e-04
+2.200000e+02 3.000000e+01 3.000000e+01 2.567000e-03 3.226880e-04 3.226880e-04
+4.675000e+02 2.175000e+02 2.175000e+02 4.588300e-04 1.004593e-04 1.004593e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d124-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d124-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t124
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.130900e-03 2.415800e-04 6.232700e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.748200e-03 1.496600e-04 1.098200e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.150200e-03 1.595500e-04 1.408800e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.320400e-03 1.017000e-04 6.212500e-05
+2.200000e+02 3.000000e+01 3.000000e+01 3.072500e-03 4.842900e-05 3.440300e-04
+4.675000e+02 2.175000e+02 2.175000e+02 5.875800e-04 3.647300e-05 3.251500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d124-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d124-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t124
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.687900e-03 2.226200e-04 2.669300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 6.238100e-03 2.758500e-04 3.253600e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.468500e-03 2.582700e-04 3.195000e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.457300e-03 2.331800e-04 2.694300e-04
+2.200000e+02 3.000000e+01 3.000000e+01 3.068900e-03 1.248900e-04 1.447400e-04
+4.675000e+02 2.175000e+02 2.175000e+02 4.889500e-04 1.851400e-05 2.496300e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d125-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d125-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t125
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 2.594400e-03 4.190878e-04 4.190878e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.553700e-03 2.612375e-04 2.612375e-04
+1.275000e+03 7.500000e+01 7.500000e+01 1.072900e-03 1.985562e-04 1.985562e-04
+1.425000e+03 7.500000e+01 7.500000e+01 8.580400e-04 1.864359e-04 1.864359e-04
+1.750000e+03 2.500000e+02 2.500000e+02 4.344900e-04 1.704024e-04 1.704024e-04
+2.350000e+03 3.500000e+02 3.500000e+02 8.611900e-05 4.402697e-05 4.402697e-05
+3.350000e+03 6.500000e+02 6.500000e+02 1.387300e-05 1.362833e-05 1.362833e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d125-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d125-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t125
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.869000e-03 8.297400e-05 1.403700e-04
+1.150000e+03 5.000000e+01 5.000000e+01 1.514600e-03 8.065100e-05 8.493300e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.174600e-03 3.970400e-05 5.986900e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.704500e-04 5.492200e-05 0.000000e+00
+1.750000e+03 2.500000e+02 2.500000e+02 4.639200e-04 8.550100e-06 3.618800e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.386100e-04 6.042900e-06 1.018900e-05
+3.350000e+03 6.500000e+02 6.500000e+02 1.991800e-05 2.218200e-06 1.967000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d125-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d125-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t125
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e+03 5.000000e+01 5.000000e+01 1.811700e-03 6.565500e-05 7.262200e-05
+1.150000e+03 5.000000e+01 5.000000e+01 1.467600e-03 5.909100e-05 6.342100e-05
+1.275000e+03 7.500000e+01 7.500000e+01 1.161500e-03 4.292300e-05 4.829600e-05
+1.425000e+03 7.500000e+01 7.500000e+01 8.521900e-04 3.676600e-05 3.954900e-05
+1.750000e+03 2.500000e+02 2.500000e+02 4.755500e-04 1.504300e-05 1.586300e-05
+2.350000e+03 3.500000e+02 3.500000e+02 1.484300e-04 7.102900e-06 7.838100e-06
+3.350000e+03 6.500000e+02 6.500000e+02 2.179700e-05 1.997300e-06 2.419000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d126-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d126-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t126
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.316600e-02 1.167391e-01 1.167391e-01
+7.500000e-01 5.000000e-02 5.000000e-02 1.077800e+00 2.641903e-01 2.641903e-01
+8.500000e-01 5.000000e-02 5.000000e-02 2.940700e+00 4.358110e-01 4.358110e-01
+9.250000e-01 2.500000e-02 2.500000e-02 5.160700e+00 8.712068e-01 8.712068e-01
+9.750000e-01 2.500000e-02 2.500000e-02 6.198000e+00 2.041773e+00 2.041773e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d126-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d126-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t126
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.466500e-01 2.039700e-03 1.887900e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.174000e+00 7.784000e-02 0.000000e+00
+8.500000e-01 5.000000e-02 5.000000e-02 2.377200e+00 8.026200e-02 2.695900e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.012100e+00 6.297600e-02 2.827100e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.432300e+00 1.540300e-01 1.159600e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d126-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d126-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t126
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.307800e-01 8.851600e-03 1.017500e-02
+7.500000e-01 5.000000e-02 5.000000e-02 1.213800e+00 5.371000e-02 5.589200e-02
+8.500000e-01 5.000000e-02 5.000000e-02 2.450700e+00 7.631600e-02 7.704000e-02
+9.250000e-01 2.500000e-02 2.500000e-02 4.073100e+00 1.391400e-01 1.458700e-01
+9.750000e-01 2.500000e-02 2.500000e-02 5.367000e+00 1.597200e-01 1.715200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d127-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d127-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t127
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.580200e-01 5.158983e-02 5.158983e-02
+3.200000e+00 4.000000e-01 4.000000e-01 2.251000e-01 4.386656e-02 4.386656e-02
+4.000000e+00 4.000000e-01 4.000000e-01 2.738800e-01 4.135038e-02 4.135038e-02
+4.800000e+00 4.000000e-01 4.000000e-01 3.212500e-01 7.000266e-02 7.000266e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.090600e-01 6.827894e-02 6.827894e-02
+7.400000e+00 1.400000e+00 1.400000e+00 1.791200e-02 1.692342e-02 1.692342e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d127-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d127-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t127
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 9.733600e-02 5.356100e-03 3.796600e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.961000e-01 6.955800e-03 1.301800e-02
+4.000000e+00 4.000000e-01 4.000000e-01 3.223100e-01 7.804600e-03 8.098900e-03
+4.800000e+00 4.000000e-01 4.000000e-01 3.665900e-01 1.322700e-02 1.837700e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.061100e-01 1.516000e-03 4.688500e-03
+7.400000e+00 1.400000e+00 1.400000e+00 1.758400e-02 1.554300e-03 9.895200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d127-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d127-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t127
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 7.695900e-02 4.781400e-03 7.292300e-03
+3.200000e+00 4.000000e-01 4.000000e-01 1.697600e-01 7.101500e-03 9.693300e-03
+4.000000e+00 4.000000e-01 4.000000e-01 3.024600e-01 9.479000e-03 1.106800e-02
+4.800000e+00 4.000000e-01 4.000000e-01 3.953700e-01 1.083800e-02 1.239700e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.304800e-01 8.274600e-03 1.024900e-02
+7.400000e+00 1.400000e+00 1.400000e+00 2.142100e-02 1.348400e-03 2.010000e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d128-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d128-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t128
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.642600e-03 1.960698e-03 1.960698e-03
+1.275000e+02 1.250000e+01 1.250000e+01 6.181900e-03 1.086276e-03 1.086276e-03
+1.525000e+02 1.250000e+01 1.250000e+01 5.108300e-03 9.268621e-04 9.268621e-04
+1.775000e+02 1.250000e+01 1.250000e+01 3.381100e-03 6.160713e-04 6.160713e-04
+2.050000e+02 1.500000e+01 1.500000e+01 2.577200e-03 4.961571e-04 4.961571e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.464700e-03 5.046414e-04 5.046414e-04
+3.000000e+02 5.000000e+01 5.000000e+01 1.591500e-03 3.863047e-04 3.863047e-04
+4.150000e+02 6.500000e+01 6.500000e+01 7.435300e-04 1.969364e-04 1.969364e-04
+5.825000e+02 1.025000e+02 1.025000e+02 1.397800e-04 8.768520e-05 8.768520e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d128-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d128-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t128
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 4.591600e-03 3.631500e-04 4.697300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.321200e-03 2.273500e-04 7.368200e-05
+1.525000e+02 1.250000e+01 1.250000e+01 4.875200e-03 1.269000e-04 3.029000e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.188200e-03 2.541400e-05 8.894900e-05
+2.050000e+02 1.500000e+01 1.500000e+01 3.505400e-03 6.468700e-05 4.064000e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.725200e-03 7.818100e-05 6.547600e-05
+3.000000e+02 5.000000e+01 5.000000e+01 1.741000e-03 9.813200e-05 6.747100e-05
+4.150000e+02 6.500000e+01 6.500000e+01 6.680600e-04 2.667300e-05 1.152700e-04
+5.825000e+02 1.025000e+02 1.025000e+02 1.551800e-04 9.030200e-06 0.000000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d128-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d128-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t128
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 5.155200e-03 1.874000e-04 2.542300e-04
+1.275000e+02 1.250000e+01 1.250000e+01 5.851400e-03 2.362300e-04 2.796300e-04
+1.525000e+02 1.250000e+01 1.250000e+01 5.218100e-03 2.230800e-04 2.756400e-04
+1.775000e+02 1.250000e+01 1.250000e+01 4.373900e-03 2.042400e-04 2.336300e-04
+2.050000e+02 1.500000e+01 1.500000e+01 3.536600e-03 1.676500e-04 1.888100e-04
+2.350000e+02 1.500000e+01 1.500000e+01 2.755400e-03 1.479800e-04 1.593700e-04
+3.000000e+02 5.000000e+01 5.000000e+01 1.546600e-03 6.072400e-05 7.170500e-05
+4.150000e+02 6.500000e+01 6.500000e+01 5.305400e-04 3.119300e-05 4.312000e-05
+5.825000e+02 1.025000e+02 1.025000e+02 1.028900e-04 1.093900e-05 1.551400e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d129-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d129-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t129
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.327800e+00 1.389135e+00 1.389135e+00
+3.000000e-01 1.000000e-01 1.000000e-01 1.539000e+00 2.244209e-01 2.244209e-01
+5.000000e-01 1.000000e-01 1.000000e-01 8.173400e-01 4.726766e-01 4.726766e-01
+8.000000e-01 2.000000e-01 2.000000e-01 1.579400e-01 1.700791e-01 1.700791e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d129-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d129-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t129
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.579100e+00 1.214900e-01 2.907000e-03
+3.000000e-01 1.000000e-01 1.000000e-01 1.669400e+00 0.000000e+00 4.594200e-02
+5.000000e-01 1.000000e-01 1.000000e-01 5.755300e-01 1.829200e-02 1.262200e-01
+8.000000e-01 2.000000e-01 2.000000e-01 8.800700e-02 1.777400e-03 3.412700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d129-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d129-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t129
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 2.616300e+00 5.581000e-02 6.133300e-02
+3.000000e-01 1.000000e-01 1.000000e-01 1.674600e+00 4.465000e-02 4.573200e-02
+5.000000e-01 1.000000e-01 1.000000e-01 5.580900e-01 2.577600e-02 2.870700e-02
+8.000000e-01 2.000000e-01 2.000000e-01 7.551800e-02 6.704700e-03 7.677700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d130-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d130-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t130
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 7.954800e-01 3.269501e-01 3.269501e-01
+1.000000e+00 5.000000e-01 5.000000e-01 1.242000e-01 1.342327e-01 1.342327e-01
+5.000000e+00 3.500000e+00 3.500000e+00 8.032600e-02 1.275911e-01 1.275911e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d130-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d130-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t130
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.785900e-01 7.975500e-03 4.351500e-03
+1.000000e+00 5.000000e-01 5.000000e-01 1.021400e-01 3.845900e-03 5.014800e-03
+5.000000e+00 3.500000e+00 3.500000e+00 1.927000e-02 8.246800e-04 2.957400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d130-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d130-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t130
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 8.725200e-01 1.440000e-02 1.481500e-02
+1.000000e+00 5.000000e-01 5.000000e-01 9.830500e-02 4.833500e-03 5.449800e-03
+5.000000e+00 3.500000e+00 3.500000e+00 2.917600e-02 2.633200e-03 3.563400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d131-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d131-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t131
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 8.262700e-02 1.237262e-01 1.237262e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.538700e+00 5.351295e-01 5.351295e-01
+9.500000e-01 5.000000e-02 5.000000e-02 6.344200e+00 1.601282e+00 1.601282e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d131-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d131-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t131
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.340000e-01 5.373100e-03 1.138000e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.696700e+00 2.749400e-02 7.501500e-03
+9.500000e-01 5.000000e-02 5.000000e-02 4.968600e+00 4.877900e-02 5.255200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d131-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d131-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t131
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.375100e-01 2.459900e-02 2.536700e-02
+8.000000e-01 1.000000e-01 1.000000e-01 1.746800e+00 1.248000e-01 1.334300e-01
+9.500000e-01 5.000000e-02 5.000000e-02 4.843900e+00 2.939100e-01 3.181300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d132-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d132-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t132
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 5.114000e-03 9.542262e-04 9.542262e-04
+4.525000e+02 2.325000e+02 2.325000e+02 6.108400e-04 2.507862e-04 2.507862e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d132-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d132-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t132
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 4.123000e-03 4.194100e-05 1.085200e-04
+4.525000e+02 2.325000e+02 2.325000e+02 9.092000e-04 3.134500e-05 1.458200e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d132-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d132-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t132
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 4.524800e-03 2.417200e-04 2.695300e-04
+4.525000e+02 2.325000e+02 2.325000e+02 7.882300e-04 5.535900e-05 6.577500e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d133-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d133-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t133
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.243600e+00 3.735556e-01 3.735556e-01
+7.000000e-01 3.000000e-01 3.000000e-01 1.709500e-01 1.938156e-01 1.938156e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d133-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d133-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t133
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.287500e+00 0.000000e+00 1.302300e-02
+7.000000e-01 3.000000e-01 3.000000e-01 1.416900e-01 7.956400e-03 1.157900e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d133-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d133-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t133
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.317500e+00 1.016600e-01 1.022900e-01
+7.000000e-01 3.000000e-01 3.000000e-01 1.216800e-01 1.901900e-02 2.048700e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d134-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d134-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t134
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.675400e-01 7.910694e-02 7.910694e-02
+1.000000e+00 5.000000e-01 5.000000e-01 3.246400e-02 9.812075e-02 9.812075e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d134-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d134-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t134
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.112700e-01 1.310100e-02 0.000000e+00
+1.000000e+00 5.000000e-01 5.000000e-01 8.873400e-02 0.000000e+00 1.020200e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d134-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d134-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t134
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 9.203000e-01 4.101300e-02 4.142100e-02
+1.000000e+00 5.000000e-01 5.000000e-01 7.970200e-02 1.207000e-02 1.335500e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d135-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d135-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t135
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.060600e+00 2.919681e+00 2.919681e+00
+8.000000e-01 1.000000e-01 1.000000e-01 3.390500e+01 1.401911e+01 1.401911e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.023500e+02 3.653857e+01 3.653857e+01
+9.750000e-01 2.500000e-02 2.500000e-02 1.358100e+02 4.366729e+01 4.366729e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d135-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d135-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t135
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.355200e+00 6.702500e-01 2.109900e+00
+8.000000e-01 1.000000e-01 1.000000e-01 3.203400e+01 5.241700e+00 7.890400e+00
+9.250000e-01 2.500000e-02 2.500000e-02 7.493700e+01 1.208700e+01 1.774600e+01
+9.750000e-01 2.500000e-02 2.500000e-02 1.042000e+02 1.573000e+01 2.590800e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d135-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d135-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t135
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.463200e+00 2.812500e-01 4.039600e-01
+8.000000e-01 1.000000e-01 1.000000e-01 3.504600e+01 1.474400e+00 2.058600e+00
+9.250000e-01 2.500000e-02 2.500000e-02 7.941600e+01 4.439100e+00 4.752700e+00
+9.750000e-01 2.500000e-02 2.500000e-02 1.050000e+02 5.104400e+00 6.932000e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d136-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d136-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t136
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.800000e+00 8.000000e-01 8.000000e-01 9.893700e-01 8.486929e-01 8.486929e-01
+4.400000e+00 8.000000e-01 8.000000e-01 4.799600e+00 1.899958e+00 1.899958e+00
+5.600000e+00 4.000000e-01 4.000000e-01 8.789000e+00 3.581552e+00 3.581552e+00
+7.400000e+00 1.400000e+00 1.400000e+00 1.197200e+00 7.472867e-01 7.472867e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d136-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d136-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t136
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.800000e+00 8.000000e-01 8.000000e-01 1.569300e+00 2.406500e-01 4.016700e-01
+4.400000e+00 8.000000e-01 8.000000e-01 5.065000e+00 8.139200e-01 1.313100e+00
+5.600000e+00 4.000000e-01 4.000000e-01 6.571300e+00 1.022000e+00 1.836800e+00
+7.400000e+00 1.400000e+00 1.400000e+00 9.072200e-01 1.443100e-01 2.461900e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d136-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d136-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t136
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.800000e+00 8.000000e-01 8.000000e-01 1.288000e+00 9.993400e-02 1.400400e-01
+4.400000e+00 8.000000e-01 8.000000e-01 5.131300e+00 1.994700e-01 2.381100e-01
+5.600000e+00 4.000000e-01 4.000000e-01 7.452000e+00 3.399500e-01 5.729900e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.115000e+00 7.028900e-02 1.142000e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d137-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d137-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t137
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 1.422700e-01 8.477553e-02 8.477553e-02
+1.400000e+02 2.500000e+01 2.500000e+01 1.215400e-01 4.175641e-02 4.175641e-02
+1.925000e+02 2.750000e+01 2.750000e+01 6.635900e-02 2.673253e-02 2.673253e-02
+2.500000e+02 3.000000e+01 3.000000e+01 3.680800e-02 1.739959e-02 1.739959e-02
+3.575000e+02 7.750000e+01 7.750000e+01 1.165800e-02 8.279260e-03 8.279260e-03
+5.600000e+02 1.250000e+02 1.250000e+02 3.528800e-03 3.175272e-03 3.175272e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d137-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d137-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t137
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 7.701200e-02 1.165900e-02 1.630800e-02
+1.400000e+02 2.500000e+01 2.500000e+01 8.726900e-02 1.246800e-02 2.832200e-02
+1.925000e+02 2.750000e+01 2.750000e+01 6.666100e-02 1.029800e-02 1.754400e-02
+2.500000e+02 3.000000e+01 3.000000e+01 4.364300e-02 7.126000e-03 1.014400e-02
+3.575000e+02 7.750000e+01 7.750000e+01 2.152600e-02 3.619900e-03 8.907700e-03
+5.600000e+02 1.250000e+02 1.250000e+02 5.934300e-03 1.058900e-03 1.059400e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d137-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d137-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t137
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 9.167000e-02 5.700400e-03 9.657400e-03
+1.400000e+02 2.500000e+01 2.500000e+01 1.010300e-01 5.006800e-03 7.355700e-03
+1.925000e+02 2.750000e+01 2.750000e+01 7.373500e-02 4.078300e-03 5.263900e-03
+2.500000e+02 3.000000e+01 3.000000e+01 4.573800e-02 3.075300e-03 3.371400e-03
+3.575000e+02 7.750000e+01 7.750000e+01 1.970800e-02 1.256000e-03 1.478400e-03
+5.600000e+02 1.250000e+02 1.250000e+02 4.443400e-03 4.695800e-04 6.250000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d138-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d138-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t138
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.657200e+01 3.750452e+00 3.750452e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.638000e+00 3.045752e+00 3.045752e+00
+5.000000e+00 3.500000e+00 3.500000e+00 1.615800e+00 2.799342e+00 2.799342e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d138-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d138-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t138
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.633400e+01 2.647400e+00 3.836800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.743300e+00 2.592200e-01 5.361400e-01
+5.000000e+00 3.500000e+00 3.500000e+00 3.349700e-01 3.766400e-02 9.854700e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d138-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d138-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t138
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 1.710200e+01 4.606200e-01 8.725200e-01
+1.000000e+00 5.000000e-01 5.000000e-01 1.730600e+00 1.465300e-01 1.663700e-01
+5.000000e+00 3.500000e+00 3.500000e+00 5.223900e-01 8.050500e-02 9.046300e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d139-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d139-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t139
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.967000e+00 4.111985e+00 4.111985e+00
+7.500000e-01 5.000000e-02 5.000000e-02 5.691300e+01 1.449033e+01 1.449033e+01
+8.500000e-01 5.000000e-02 5.000000e-02 1.254600e+02 2.475365e+01 2.475365e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.949700e+02 4.410050e+01 4.410050e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.513700e+02 5.102258e+01 5.102258e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d139-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d139-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t139
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.044000e+01 1.596100e+00 3.236600e+00
+7.500000e-01 5.000000e-02 5.000000e-02 4.830100e+01 7.897300e+00 6.428600e+00
+8.500000e-01 5.000000e-02 5.000000e-02 9.588600e+01 1.390000e+01 1.668600e+01
+9.250000e-01 2.500000e-02 2.500000e-02 1.599500e+02 2.010600e+01 3.136500e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.124100e+02 2.646000e+01 4.343600e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d139-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d139-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t139
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 9.713800e+00 4.149200e-01 4.991100e-01
+7.500000e-01 5.000000e-02 5.000000e-02 4.973500e+01 2.484000e+00 3.085300e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.006500e+02 3.533700e+00 5.445000e+00
+9.250000e-01 2.500000e-02 2.500000e-02 1.645000e+02 6.388800e+00 7.474400e+00
+9.750000e-01 2.500000e-02 2.500000e-02 2.146600e+02 7.298200e+00 1.126600e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d140-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d140-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t140
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 3.411300e+00 1.353607e+00 1.353607e+00
+3.200000e+00 4.000000e-01 4.000000e-01 7.419800e+00 1.935078e+00 1.935078e+00
+3.800000e+00 2.000000e-01 2.000000e-01 8.993400e+00 2.629859e+00 2.629859e+00
+4.200000e+00 2.000000e-01 2.000000e-01 1.273300e+01 4.117456e+00 4.117456e+00
+4.600000e+00 2.000000e-01 2.000000e-01 1.606500e+01 4.215204e+00 4.215204e+00
+5.000000e+00 2.000000e-01 2.000000e-01 1.892000e+01 5.206451e+00 5.206451e+00
+7.000000e+00 1.800000e+00 1.800000e+00 3.367200e+00 9.963553e-01 9.963553e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d140-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d140-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t140
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 2.757200e+00 2.856800e-01 4.122200e-01
+3.200000e+00 4.000000e-01 4.000000e-01 6.836500e+00 1.081500e+00 1.955700e+00
+3.800000e+00 2.000000e-01 2.000000e-01 1.132300e+01 1.574400e+00 1.561100e+00
+4.200000e+00 2.000000e-01 2.000000e-01 1.413800e+01 1.863600e+00 4.243300e+00
+4.600000e+00 2.000000e-01 2.000000e-01 1.573300e+01 1.928800e+00 3.127700e+00
+5.000000e+00 2.000000e-01 2.000000e-01 1.578800e+01 2.475500e+00 2.837200e+00
+7.000000e+00 1.800000e+00 1.800000e+00 2.743600e+00 3.962800e-01 6.027500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d140-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d140-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t140
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 2.208100e+00 1.850500e-01 2.195600e-01
+3.200000e+00 4.000000e-01 4.000000e-01 5.921000e+00 3.030200e-01 3.544900e-01
+3.800000e+00 2.000000e-01 2.000000e-01 1.030500e+01 5.653400e-01 6.553600e-01
+4.200000e+00 2.000000e-01 2.000000e-01 1.352800e+01 6.477500e-01 6.885100e-01
+4.600000e+00 2.000000e-01 2.000000e-01 1.688200e+01 7.236100e-01 9.713500e-01
+5.000000e+00 2.000000e-01 2.000000e-01 1.681400e+01 7.221500e-01 1.004100e+00
+7.000000e+00 1.800000e+00 1.800000e+00 3.133700e+00 1.039200e-01 2.169200e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d141-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d141-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t141
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 3.192300e-01 1.120025e-01 1.120025e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.047800e-01 7.255875e-02 7.255875e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.408100e-01 5.214738e-02 5.214738e-02
+1.775000e+02 1.250000e+01 1.250000e+01 1.241700e-01 4.096810e-02 4.096810e-02
+2.200000e+02 3.000000e+01 3.000000e+01 1.108600e-01 2.379134e-02 2.379134e-02
+4.675000e+02 2.175000e+02 2.175000e+02 1.981600e-02 5.650998e-03 5.650998e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d141-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d141-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t141
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.058900e-01 2.813800e-02 3.543100e-02
+1.275000e+02 1.250000e+01 1.250000e+01 2.306600e-01 3.016000e-02 3.937900e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.066700e-01 2.396600e-02 3.607400e-02
+1.775000e+02 1.250000e+01 1.250000e+01 1.733700e-01 2.204000e-02 3.342500e-02
+2.200000e+02 3.000000e+01 3.000000e+01 1.232900e-01 1.758800e-02 3.371500e-02
+4.675000e+02 2.175000e+02 2.175000e+02 2.357800e-02 3.758700e-03 6.331500e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d141-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d141-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t141
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.314000e-01 9.056700e-03 1.507300e-02
+1.275000e+02 1.250000e+01 1.250000e+01 2.537800e-01 1.122200e-02 1.632900e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.224700e-01 1.050700e-02 1.406000e-02
+1.775000e+02 1.250000e+01 1.250000e+01 1.813300e-01 9.486200e-03 1.208100e-02
+2.200000e+02 3.000000e+01 3.000000e+01 1.248500e-01 5.080900e-03 6.374900e-03
+4.675000e+02 2.175000e+02 2.175000e+02 1.989200e-02 7.532100e-04 9.231200e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d142-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d142-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t142
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 2.829000e+00 1.063194e+01 1.063194e+01
+7.500000e-01 5.000000e-02 5.000000e-02 7.063200e+01 4.429856e+01 4.429856e+01
+8.500000e-01 5.000000e-02 5.000000e-02 1.927300e+02 8.025927e+01 8.025927e+01
+9.250000e-01 2.500000e-02 2.500000e-02 3.382100e+02 1.371993e+02 1.371993e+02
+9.750000e-01 2.500000e-02 2.500000e-02 4.062000e+02 1.660804e+02 1.660804e+02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d142-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d142-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t142
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.277500e+01 1.784700e+00 3.744300e+00
+7.500000e-01 5.000000e-02 5.000000e-02 6.080600e+01 8.843000e+00 9.730000e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.231300e+02 1.735900e+01 2.371100e+01
+9.250000e-01 2.500000e-02 2.500000e-02 2.078000e+02 2.311600e+01 4.653400e+01
+9.750000e-01 2.500000e-02 2.500000e-02 2.813600e+02 3.676700e+01 5.111300e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d142-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d142-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t142
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.204700e+01 4.620800e-01 5.575400e-01
+7.500000e-01 5.000000e-02 5.000000e-02 6.336500e+01 2.803800e+00 3.373100e+00
+8.500000e-01 5.000000e-02 5.000000e-02 1.279300e+02 3.983900e+00 5.374100e+00
+9.250000e-01 2.500000e-02 2.500000e-02 2.126300e+02 7.263500e+00 9.085400e+00
+9.750000e-01 2.500000e-02 2.500000e-02 2.801700e+02 8.337800e+00 1.225100e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d143-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d143-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t143
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 1.011900e+01 6.015301e+00 6.015301e+00
+3.200000e+00 4.000000e-01 4.000000e-01 1.441500e+01 7.616625e+00 7.616625e+00
+4.000000e+00 4.000000e-01 4.000000e-01 1.753800e+01 1.010305e+01 1.010305e+01
+4.800000e+00 4.000000e-01 4.000000e-01 2.057100e+01 1.376363e+01 1.376363e+01
+5.600000e+00 4.000000e-01 4.000000e-01 1.338700e+01 9.289119e+00 9.289119e+00
+7.400000e+00 1.400000e+00 1.400000e+00 1.147000e+00 7.083976e-01 7.083976e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d143-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d143-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t143
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 5.041500e+00 6.305600e-01 6.808800e-01
+3.200000e+00 4.000000e-01 4.000000e-01 1.015700e+01 1.416100e+00 2.615100e+00
+4.000000e+00 4.000000e-01 4.000000e-01 1.669400e+01 2.062600e+00 3.861900e+00
+4.800000e+00 4.000000e-01 4.000000e-01 1.898800e+01 2.606200e+00 3.640800e+00
+5.600000e+00 4.000000e-01 4.000000e-01 1.067500e+01 1.482900e+00 2.199400e+00
+7.400000e+00 1.400000e+00 1.400000e+00 9.107600e-01 1.466000e-01 2.447600e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d143-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d143-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t143
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e+00 4.000000e-01 4.000000e-01 4.017500e+00 2.496100e-01 3.626100e-01
+3.200000e+00 4.000000e-01 4.000000e-01 8.862000e+00 3.707200e-01 4.803700e-01
+4.000000e+00 4.000000e-01 4.000000e-01 1.578900e+01 4.948300e-01 5.839000e-01
+4.800000e+00 4.000000e-01 4.000000e-01 2.063900e+01 5.657500e-01 9.146400e-01
+5.600000e+00 4.000000e-01 4.000000e-01 1.203200e+01 4.319600e-01 7.398200e-01
+7.400000e+00 1.400000e+00 1.400000e+00 1.118200e+00 7.038900e-02 1.151500e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d144-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d144-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t144
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 3.586100e-01 2.847792e-01 2.847792e-01
+1.275000e+02 1.250000e+01 1.250000e+01 3.928800e-01 2.004844e-01 2.004844e-01
+1.525000e+02 1.250000e+01 1.250000e+01 3.246600e-01 1.533856e-01 1.533856e-01
+1.775000e+02 1.250000e+01 1.250000e+01 2.148800e-01 1.301488e-01 1.301488e-01
+2.050000e+02 1.500000e+01 1.500000e+01 1.637900e-01 9.830358e-02 9.830358e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.566400e-01 8.339904e-02 8.339904e-02
+3.000000e+02 5.000000e+01 5.000000e+01 1.011500e-01 5.663508e-02 5.663508e-02
+4.150000e+02 6.500000e+01 6.500000e+01 4.725400e-02 2.339085e-02 2.339085e-02
+5.825000e+02 1.025000e+02 1.025000e+02 8.883300e-03 5.141496e-03 5.141496e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d144-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d144-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t144
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.360800e-01 3.254100e-02 3.997100e-02
+1.275000e+02 1.250000e+01 1.250000e+01 2.736000e-01 3.329400e-02 4.618700e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.506700e-01 2.991800e-02 6.328300e-02
+1.775000e+02 1.250000e+01 1.250000e+01 2.153400e-01 2.457100e-02 4.439500e-02
+2.050000e+02 1.500000e+01 1.500000e+01 1.802300e-01 2.677100e-02 5.693700e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.401200e-01 1.564900e-02 2.655800e-02
+3.000000e+02 5.000000e+01 5.000000e+01 8.951600e-02 1.349100e-02 2.013200e-02
+4.150000e+02 6.500000e+01 6.500000e+01 3.434900e-02 4.557400e-03 1.402800e-02
+5.825000e+02 1.025000e+02 1.025000e+02 7.978700e-03 1.068200e-03 1.368800e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d144-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d144-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t144
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+9.750000e+01 1.750000e+01 1.750000e+01 2.682500e-01 9.751300e-03 1.674800e-02
+1.275000e+02 1.250000e+01 1.250000e+01 3.044800e-01 1.229200e-02 1.774700e-02
+1.525000e+02 1.250000e+01 1.250000e+01 2.715300e-01 1.160800e-02 1.485000e-02
+1.775000e+02 1.250000e+01 1.250000e+01 2.276000e-01 1.062800e-02 1.307900e-02
+2.050000e+02 1.500000e+01 1.500000e+01 1.840300e-01 8.723800e-03 1.193600e-02
+2.350000e+02 1.500000e+01 1.500000e+01 1.433800e-01 7.700300e-03 8.618100e-03
+3.000000e+02 5.000000e+01 5.000000e+01 8.047900e-02 3.159800e-03 3.674600e-03
+4.150000e+02 6.500000e+01 6.500000e+01 2.760700e-02 1.623200e-03 2.186300e-03
+5.825000e+02 1.025000e+02 1.025000e+02 5.354000e-03 5.692300e-04 7.890300e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d145-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d145-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t145
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.081500e+01 1.340513e+01 1.340513e+01
+1.000000e+00 5.000000e-01 5.000000e-01 7.933800e+00 1.453248e+01 1.453248e+01
+5.000000e+00 3.500000e+00 3.500000e+00 5.131300e+00 1.108318e+01 1.108318e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d145-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d145-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t145
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 4.550600e+01 6.389100e+00 8.944800e+00
+1.000000e+00 5.000000e-01 5.000000e-01 5.290500e+00 4.758300e-01 1.213800e+00
+5.000000e+00 3.500000e+00 3.500000e+00 9.981000e-01 1.181700e-01 2.592400e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d145-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d145-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t145
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 4.554800e+01 7.517200e-01 1.603100e+00
+1.000000e+00 5.000000e-01 5.000000e-01 5.131800e+00 2.523200e-01 2.853600e-01
+5.000000e+00 3.500000e+00 3.500000e+00 1.523100e+00 1.374600e-01 1.651300e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d146-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d146-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t146
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 4.779900e-01 8.090187e-01 8.090187e-01
+8.000000e-01 1.000000e-01 1.000000e-01 8.901100e+00 3.877624e+00 3.877624e+00
+9.500000e-01 5.000000e-02 5.000000e-02 3.670100e+01 1.155229e+01 1.155229e+01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d146-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d146-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t146
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.499800e+00 2.920200e-01 4.895300e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.087500e+01 1.950100e+00 3.323400e+00
+9.500000e-01 5.000000e-02 5.000000e-02 3.184500e+01 5.320200e+00 9.142800e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d146-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d146-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t146
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-01 3.500000e-01 3.500000e-01 1.652300e+00 1.711300e-01 2.110200e-01
+8.000000e-01 1.000000e-01 1.000000e-01 1.215200e+01 8.682100e-01 1.171900e+00
+9.500000e-01 5.000000e-02 5.000000e-02 3.369700e+01 2.044600e+00 2.568500e+00
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d147-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d147-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t147
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.700000e+00 1.500000e+00 1.500000e+00 5.926800e-01 2.795387e-01 2.795387e-01
+5.600000e+00 4.000000e-01 4.000000e-01 2.243100e+00 8.148347e-01 8.148347e-01
+7.400000e+00 1.400000e+00 1.400000e+00 7.249500e-01 3.906053e-01 3.906053e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d147-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d147-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t147
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.700000e+00 1.500000e+00 1.500000e+00 9.124100e-01 1.824300e-01 2.578300e-01
+5.600000e+00 4.000000e-01 4.000000e-01 2.269900e+00 2.817400e-01 7.024200e-01
+7.400000e+00 1.400000e+00 1.400000e+00 6.537700e-01 1.258600e-01 2.023800e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d147-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d147-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t147
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+3.700000e+00 1.500000e+00 1.500000e+00 8.459900e-01 5.914900e-02 6.840600e-02
+5.600000e+00 4.000000e-01 4.000000e-01 2.672200e+00 2.035700e-01 2.902100e-01
+7.400000e+00 1.400000e+00 1.400000e+00 8.064800e-01 5.977800e-02 9.021300e-02
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d148-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d148-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t148
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 2.891900e-02 1.133468e-02 1.133468e-02
+4.525000e+02 2.325000e+02 2.325000e+02 3.454200e-03 1.637921e-03 1.637921e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d148-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d148-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t148
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 2.582200e-02 3.978900e-03 7.630100e-03
+4.525000e+02 2.325000e+02 2.325000e+02 5.694300e-03 1.162800e-03 1.730700e-03
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d148-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d148-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t148
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+02 7.000000e+01 7.000000e+01 3.105100e-02 1.658800e-03 2.820300e-03
+4.525000e+02 2.325000e+02 2.325000e+02 5.409100e-03 3.798900e-04 4.199000e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d149-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d149-x01-y01
+Title: doi:10.17182/hepdata.76505.v1/t149
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.570500e+00 1.202954e+00 1.202954e+00
+1.000000e+00 5.000000e-01 5.000000e-01 1.869100e-01 6.709501e-01 6.709501e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d149-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d149-x01-y02
+Title: doi:10.17182/hepdata.76505.v1/t149
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 5.753000e+00 1.067200e+00 1.685900e+00
+1.000000e+00 5.000000e-01 5.000000e-01 5.601900e-01 6.930800e-02 1.839700e-01
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2017_I1517194_MU/d149-x01-y03
+IsRef: 1
+Path: /REF/ATLAS_2017_I1517194_MU/d149-x01-y03
+Title: doi:10.17182/hepdata.76505.v1/t149
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+0.000000e+00 5.000000e-01 5.000000e-01 6.246700e+00 2.783900e-01 4.721300e-01
+1.000000e+00 5.000000e-01 5.000000e-01 5.409900e-01 8.192500e-02 8.663100e-02
+END YODA_SCATTER2D_V2
diff --git a/analyses/pluginATLAS/ATLAS_2017_I1614149.cc b/analyses/pluginATLAS/ATLAS_2017_I1614149.cc
--- a/analyses/pluginATLAS/ATLAS_2017_I1614149.cc
+++ b/analyses/pluginATLAS/ATLAS_2017_I1614149.cc
@@ -1,353 +1,363 @@
// -*- C++ -*
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/FinalState.hh"
#include "Rivet/Projections/VetoedFinalState.hh"
#include "Rivet/Projections/IdentifiedFinalState.hh"
#include "Rivet/Projections/PromptFinalState.hh"
#include "Rivet/Projections/DressedLeptons.hh"
#include "Rivet/Projections/FastJets.hh"
#include "Rivet/Projections/MissingMomentum.hh"
-#include "fastjet/tools/Filter.hh"
-
-// substructure includes included in fjcontrib-1.021 (http://fastjet.hepforge.org/contrib/)
-#include "Rivet/Tools/Nsubjettiness/Njettiness.hh"
-#include "Rivet/Tools/Nsubjettiness/Nsubjettiness.hh"
-#include "Rivet/Tools/Nsubjettiness/NjettinessPlugin.hh"
+#include "Rivet/Tools/fjcontrib/Njettiness.hh"
+#include "Rivet/Tools/fjcontrib/Nsubjettiness.hh"
+#include "Rivet/Tools/fjcontrib/NjettinessPlugin.hh"
namespace Rivet {
+
+
class ATLAS_2017_I1614149 : public Analysis {
- public:
+ public:
- /// Constructor
- ///@brief: Resolved and boosted ttbar l+jets cross sections at 13 TeV
- DEFAULT_RIVET_ANALYSIS_CTOR(ATLAS_2017_I1614149);
+ /// Constructor
+ ///@brief: Resolved and boosted ttbar l+jets cross sections at 13 TeV
+ DEFAULT_RIVET_ANALYSIS_CTOR(ATLAS_2017_I1614149);
- void init() {
- // Eta ranges
- Cut eta_full = (Cuts::abseta < 5.0);
- Cut lep_cuts = (Cuts::abseta < 2.5) && (Cuts::pT > 25*GeV);
+ void init() {
+ // Eta ranges
+ Cut eta_full = (Cuts::abseta < 5.0);
+ Cut lep_cuts = (Cuts::abseta < 2.5) && (Cuts::pT > 25*GeV);
- // All final state particles
- FinalState fs(eta_full);
+ // All final state particles
+ FinalState fs(eta_full);
- IdentifiedFinalState all_photons(fs);
- all_photons.acceptIdPair(PID::PHOTON);
+ IdentifiedFinalState all_photons(fs);
+ all_photons.acceptIdPair(PID::PHOTON);
- // Get photons to dress leptons
- IdentifiedFinalState ph_id(fs);
- ph_id.acceptIdPair(PID::PHOTON);
+ // Get photons to dress leptons
+ IdentifiedFinalState ph_id(fs);
+ ph_id.acceptIdPair(PID::PHOTON);
- // Projection to find the electrons
- IdentifiedFinalState el_id(fs);
- el_id.acceptIdPair(PID::ELECTRON);
+ // Projection to find the electrons
+ IdentifiedFinalState el_id(fs);
+ el_id.acceptIdPair(PID::ELECTRON);
- PromptFinalState photons(ph_id);
- photons.acceptTauDecays(true);
- addProjection(photons, "photons");
+ PromptFinalState photons(ph_id);
+ photons.acceptTauDecays(true);
+ addProjection(photons, "photons");
- PromptFinalState electrons(el_id);
- electrons.acceptTauDecays(true);
- DressedLeptons dressedelectrons(photons, electrons, 0.1, lep_cuts);
- addProjection(dressedelectrons, "elecs");
- DressedLeptons ewdressedelectrons(all_photons, electrons, 0.1, eta_full);
+ PromptFinalState electrons(el_id);
+ electrons.acceptTauDecays(true);
+ DressedLeptons dressedelectrons(photons, electrons, 0.1, lep_cuts);
+ addProjection(dressedelectrons, "elecs");
+ DressedLeptons ewdressedelectrons(all_photons, electrons, 0.1, eta_full);
- // Projection to find the muons
- IdentifiedFinalState mu_id(fs);
- mu_id.acceptIdPair(PID::MUON);
+ // Projection to find the muons
+ IdentifiedFinalState mu_id(fs);
+ mu_id.acceptIdPair(PID::MUON);
- PromptFinalState muons(mu_id);
- muons.acceptTauDecays(true);
- DressedLeptons dressedmuons(photons, muons, 0.1, lep_cuts);
- addProjection(dressedmuons, "muons");
- DressedLeptons ewdressedmuons(all_photons, muons, 0.1, eta_full);
+ PromptFinalState muons(mu_id);
+ muons.acceptTauDecays(true);
+ DressedLeptons dressedmuons(photons, muons, 0.1, lep_cuts);
+ addProjection(dressedmuons, "muons");
+ DressedLeptons ewdressedmuons(all_photons, muons, 0.1, eta_full);
- // Projection to find MET
- declare(MissingMomentum(fs), "MET");
+ // Projection to find MET
+ declare(MissingMomentum(fs), "MET");
- // remove prompt neutrinos from jet clustering
- IdentifiedFinalState nu_id(fs);
- nu_id.acceptNeutrinos();
- PromptFinalState neutrinos(nu_id);
- neutrinos.acceptTauDecays(true);
+ // remove prompt neutrinos from jet clustering
+ IdentifiedFinalState nu_id(fs);
+ nu_id.acceptNeutrinos();
+ PromptFinalState neutrinos(nu_id);
+ neutrinos.acceptTauDecays(true);
- // Jet clustering.
- VetoedFinalState vfs(fs);
- vfs.addVetoOnThisFinalState(ewdressedelectrons);
- vfs.addVetoOnThisFinalState(ewdressedmuons);
- vfs.addVetoOnThisFinalState(neutrinos);
- FastJets jets(vfs, FastJets::ANTIKT, 0.4);
- jets.useInvisibles(true);
- addProjection(jets, "jets");
+ // Jet clustering.
+ VetoedFinalState vfs(fs);
+ vfs.addVetoOnThisFinalState(ewdressedelectrons);
+ vfs.addVetoOnThisFinalState(ewdressedmuons);
+ vfs.addVetoOnThisFinalState(neutrinos);
+ FastJets jets(vfs, FastJets::ANTIKT, 0.4);
+ jets.useInvisibles(true);
+ addProjection(jets, "jets");
- // Addition of the large-R jets
- VetoedFinalState vfs1(fs);
- vfs1.addVetoOnThisFinalState(neutrinos);
- FastJets fjets(vfs1, FastJets::ANTIKT, 1.);
- fjets.useInvisibles(JetAlg::NO_INVISIBLES);
- fjets.useMuons(JetAlg::NO_MUONS);
- addProjection(fjets, "fjets");
+ // Addition of the large-R jets
+ VetoedFinalState vfs1(fs);
+ vfs1.addVetoOnThisFinalState(neutrinos);
+ FastJets fjets(vfs1, FastJets::ANTIKT, 1.);
+ fjets.useInvisibles(JetAlg::NO_INVISIBLES);
+ fjets.useMuons(JetAlg::NO_MUONS);
+ addProjection(fjets, "fjets");
- bookHists("top_pt_res", 15);
- bookHists("top_absrap_res", 17);
- bookHists("ttbar_pt_res", 19);
- bookHists("ttbar_absrap_res", 21);
- bookHists("ttbar_m_res", 23);
- bookHists("top_pt_boost", 25);
- bookHists("top_absrap_boost", 27);
+ bookHists("top_pt_res", 15);
+ bookHists("top_absrap_res", 17);
+ bookHists("ttbar_pt_res", 19);
+ bookHists("ttbar_absrap_res", 21);
+ bookHists("ttbar_m_res", 23);
+ bookHists("top_pt_boost", 25);
+ bookHists("top_absrap_boost", 27);
+ }
+
+
+ void analyze(const Event& event) {
+
+ const double weight = event.weight();
+
+ // Get the selected objects, using the projections.
+ vector<DressedLepton> electrons = apply<DressedLeptons>(event, "elecs").dressedLeptons();
+ vector<DressedLepton> muons = apply<DressedLeptons>(event, "muons").dressedLeptons();
+ const Jets& jets = apply<FastJets>(event, "jets").jetsByPt(Cuts::pT > 25*GeV && Cuts::abseta < 2.5);
+ const PseudoJets& all_fjets = apply<FastJets>(event, "fjets").pseudoJetsByPt();
+
+
+ // get MET
+ const Vector3 met = apply<MissingMomentum>(event, "MET").vectorMPT();
+
+ Jets bjets, lightjets;
+ for (const Jet& jet : jets) {
+ bool b_tagged = jet.bTags(Cuts::pT > 5*GeV).size();
+ if ( b_tagged && bjets.size() < 2) bjets +=jet;
+ else lightjets += jet;
}
- void analyze(const Event& event) {
+ // Implementing large-R jets definition
+ // trim the jets
+ PseudoJets trimmed_fatJets;
+ float Rfilt = 0.2;
+ float pt_fraction_min = 0.05;
+ fastjet::Filter trimmer(fastjet::JetDefinition(fastjet::kt_algorithm, Rfilt), fastjet::SelectorPtFractionMin(pt_fraction_min));
+ for (PseudoJet pjet : all_fjets) trimmed_fatJets += trimmer(pjet);
+ trimmed_fatJets = fastjet::sorted_by_pt(trimmed_fatJets);
+ PseudoJets trimmed_jets;
+ for (unsigned int i = 0; i < trimmed_fatJets.size(); ++i) {
+ FourMomentum tj_mom = momentum(trimmed_fatJets[i]);
+ if (tj_mom.pt() <= 300*GeV) continue;
+ if (tj_mom.abseta() >= 2.0) continue;
+ trimmed_jets.push_back(trimmed_fatJets[i]);
+ }
- const double weight = event.weight();
+ bool single_electron = (electrons.size() == 1) && (muons.empty());
+ bool single_muon = (muons.size() == 1) && (electrons.empty());
- // Get the selected objects, using the projections.
- vector<DressedLepton> electrons = apply<DressedLeptons>(event, "elecs").dressedLeptons();
- vector<DressedLepton> muons = apply<DressedLeptons>(event, "muons").dressedLeptons();
- const Jets& jets = apply<FastJets>(event, "jets").jetsByPt(Cuts::pT > 25*GeV && Cuts::abseta < 2.5);
- const PseudoJets& all_fjets = apply<FastJets>(event, "fjets").pseudoJetsByPt();
+ DressedLepton *lepton = NULL;
+ if (single_electron) lepton = &electrons[0];
+ else if (single_muon) lepton = &muons[0];
+ if (!single_electron && !single_muon) vetoEvent;
- // get MET
- const Vector3 met = apply<MissingMomentum>(event, "MET").vectorMPT();
+ bool pass_resolved = true;
+ bool num_b_tagged_jets = (bjets.size() == 2);
+ if (!num_b_tagged_jets) pass_resolved = false;
- Jets bjets, lightjets;
- for (const Jet& jet : jets) {
- bool b_tagged = jet.bTags(Cuts::pT > 5*GeV).size();
- if ( b_tagged && bjets.size() < 2) bjets +=jet;
- else lightjets += jet;
- }
+ if (jets.size() < 4) pass_resolved = false;
- // Implementing large-R jets definition
- // trim the jets
- PseudoJets trimmed_fatJets;
- float Rfilt = 0.2;
- float pt_fraction_min = 0.05;
- fastjet::Filter trimmer(fastjet::JetDefinition(fastjet::kt_algorithm, Rfilt), fastjet::SelectorPtFractionMin(pt_fraction_min));
- for (PseudoJet pjet : all_fjets) trimmed_fatJets += trimmer(pjet);
- trimmed_fatJets = fastjet::sorted_by_pt(trimmed_fatJets);
- PseudoJets trimmed_jets;
- for (unsigned int i = 0; i < trimmed_fatJets.size(); ++i) {
- FourMomentum tj_mom = momentum(trimmed_fatJets[i]);
- if (tj_mom.pt() <= 300*GeV) continue;
- if (tj_mom.abseta() >= 2.0) continue;
- trimmed_jets.push_back(trimmed_fatJets[i]);
- }
-
- bool single_electron = (electrons.size() == 1) && (muons.empty());
- bool single_muon = (muons.size() == 1) && (electrons.empty());
-
- DressedLepton *lepton = NULL;
- if (single_electron) lepton = &electrons[0];
- else if (single_muon) lepton = &muons[0];
-
- if (!single_electron && !single_muon) vetoEvent;
-
- bool pass_resolved = true;
- bool num_b_tagged_jets = (bjets.size() == 2);
- if (!num_b_tagged_jets) pass_resolved = false;
-
- if (jets.size() < 4) pass_resolved = false;
-
- bool pass_boosted = true;
- int fatJetIndex = -1;
- bool passTopTag = false;
- bool passDphi = false;
- bool passAddJet = false;
- bool goodLepJet = false;
- bool lepbtag = false;
- bool hadbtag=false;
- vector<int> lepJetIndex;
- vector<int> jet_farFromHadTopJetCandidate;
- if (met.mod() < 20*GeV) pass_boosted = false;
- if (pass_boosted) {
- double transmass = _mT(lepton->momentum(), met);
- if (transmass + met.mod() < 60*GeV) pass_boosted = false;
- }
- if (pass_boosted) {
- if (trimmed_jets.size() >= 1) {
- for (unsigned int j = 0; j<trimmed_jets.size(); ++j) {
- if (tau32( trimmed_jets.at(j), 1. ) < 0.75 &&
- momentum(trimmed_jets.at(j)).mass() > 100*GeV &&
- momentum(trimmed_jets.at(j)).pt() > 300*GeV &&
- momentum(trimmed_jets.at(j)).pt() < 1500*GeV &&
- fabs(momentum(trimmed_jets.at(j)).eta()) < 2.) {
- passTopTag = true;
- fatJetIndex = j;
- break;
- }
+ bool pass_boosted = true;
+ int fatJetIndex = -1;
+ bool passTopTag = false;
+ bool passDphi = false;
+ bool passAddJet = false;
+ bool goodLepJet = false;
+ bool lepbtag = false;
+ bool hadbtag=false;
+ vector<int> lepJetIndex;
+ vector<int> jet_farFromHadTopJetCandidate;
+ if (met.mod() < 20*GeV) pass_boosted = false;
+ if (pass_boosted) {
+ double transmass = _mT(lepton->momentum(), met);
+ if (transmass + met.mod() < 60*GeV) pass_boosted = false;
+ }
+ if (pass_boosted) {
+ if (trimmed_jets.size() >= 1) {
+ for (unsigned int j = 0; j<trimmed_jets.size(); ++j) {
+ if (tau32( trimmed_jets.at(j), 1. ) < 0.75 &&
+ momentum(trimmed_jets.at(j)).mass() > 100*GeV &&
+ momentum(trimmed_jets.at(j)).pt() > 300*GeV &&
+ momentum(trimmed_jets.at(j)).pt() < 1500*GeV &&
+ fabs(momentum(trimmed_jets.at(j)).eta()) < 2.) {
+ passTopTag = true;
+ fatJetIndex = j;
+ break;
}
}
}
- if(!passTopTag && fatJetIndex == -1) pass_boosted = false;
- if (pass_boosted) {
- double dPhi_fatjet = deltaPhi(lepton->phi(), momentum(trimmed_jets.at(fatJetIndex)).phi());
- double dPhi_fatjet_lep_cut = 1.0; //2.3
- if (dPhi_fatjet > dPhi_fatjet_lep_cut ) {
- passDphi = true;
+ }
+ if(!passTopTag && fatJetIndex == -1) pass_boosted = false;
+ if (pass_boosted) {
+ double dPhi_fatjet = deltaPhi(lepton->phi(), momentum(trimmed_jets.at(fatJetIndex)).phi());
+ double dPhi_fatjet_lep_cut = 1.0; //2.3
+ if (dPhi_fatjet > dPhi_fatjet_lep_cut ) {
+ passDphi = true;
+ }
+ }
+ if (!passDphi) pass_boosted = false;
+ if (bjets.empty()) pass_boosted = false;
+ if (pass_boosted) {
+ for (unsigned int sj = 0; sj < jets.size(); ++sj) {
+ double dR = deltaR(jets.at(sj).momentum(), momentum(trimmed_jets.at(fatJetIndex)));
+ if(dR > 1.5) {
+ passAddJet = true;
+ jet_farFromHadTopJetCandidate.push_back(sj);
}
}
- if (!passDphi) pass_boosted = false;
- if (bjets.empty()) pass_boosted = false;
- if (pass_boosted) {
- for (unsigned int sj = 0; sj < jets.size(); ++sj) {
- double dR = deltaR(jets.at(sj).momentum(), momentum(trimmed_jets.at(fatJetIndex)));
- if(dR > 1.5) {
- passAddJet = true;
- jet_farFromHadTopJetCandidate.push_back(sj);
+ }
+ if (!passAddJet) pass_boosted = false;
+ if (pass_boosted) {
+ for (int ltj : jet_farFromHadTopJetCandidate) {
+ double dR_jet_lep = deltaR(jets.at(ltj).momentum(), lepton->momentum());
+ double dR_jet_lep_cut = 2.0;//1.5
+ if (dR_jet_lep < dR_jet_lep_cut) {
+ lepJetIndex.push_back(ltj);
+ goodLepJet = true;
+ }
+ }
+ }
+ if(!goodLepJet) pass_boosted = false;
+ if (pass_boosted) {
+ for (int lepj : lepJetIndex) {
+ lepbtag = jets.at(lepj).bTags(Cuts::pT > 5*GeV).size();
+ if (lepbtag) break;
+ }
+ }
+ double dR_fatBjet_cut = 1.0;
+ if (pass_boosted) {
+ for (const Jet& bjet : bjets) {
+ hadbtag |= deltaR(momentum(trimmed_jets.at(fatJetIndex)), bjet) < dR_fatBjet_cut;
+ }
+ }
+
+ if (!(lepbtag || hadbtag)) pass_boosted = false;
+
+ FourMomentum pbjet1; //Momentum of bjet1
+ FourMomentum pbjet2; //Momentum of bjet
+ int Wj1index = -1, Wj2index = -1;
+
+ if (pass_resolved) {
+
+ if ( deltaR(bjets[0], *lepton) <= deltaR(bjets[1], *lepton) ) {
+ pbjet1 = bjets[0].momentum();
+ pbjet2 = bjets[1].momentum();
+ } else {
+ pbjet1 = bjets[1].momentum();
+ pbjet2 = bjets[0].momentum();
+ }
+
+ double bestWmass = 1000.0*TeV;
+ double mWPDG = 80.399*GeV;
+ for (unsigned int i = 0; i < (lightjets.size() - 1); ++i) {
+ for (unsigned int j = i + 1; j < lightjets.size(); ++j) {
+ double wmass = (lightjets[i].momentum() + lightjets[j].momentum()).mass();
+ if (fabs(wmass - mWPDG) < fabs(bestWmass - mWPDG)) {
+ bestWmass = wmass;
+ Wj1index = i;
+ Wj2index = j;
}
}
}
- if (!passAddJet) pass_boosted = false;
- if (pass_boosted) {
- for (int ltj : jet_farFromHadTopJetCandidate) {
- double dR_jet_lep = deltaR(jets.at(ltj).momentum(), lepton->momentum());
- double dR_jet_lep_cut = 2.0;//1.5
- if (dR_jet_lep < dR_jet_lep_cut) {
- lepJetIndex.push_back(ltj);
- goodLepJet = true;
- }
- }
- }
- if(!goodLepJet) pass_boosted = false;
- if (pass_boosted) {
- for (int lepj : lepJetIndex) {
- lepbtag = jets.at(lepj).bTags(Cuts::pT > 5*GeV).size();
- if (lepbtag) break;
- }
- }
- double dR_fatBjet_cut = 1.0;
- if (pass_boosted) {
- for (const Jet& bjet : bjets) {
- hadbtag |= deltaR(momentum(trimmed_jets.at(fatJetIndex)), bjet) < dR_fatBjet_cut;
- }
- }
- if (!(lepbtag || hadbtag)) pass_boosted = false;
+ FourMomentum pjet1 = lightjets[Wj1index].momentum();
+ FourMomentum pjet2 = lightjets[Wj2index].momentum();
- FourMomentum pbjet1; //Momentum of bjet1
- FourMomentum pbjet2; //Momentum of bjet
- int Wj1index = -1, Wj2index = -1;
+ // compute hadronic W boson
+ FourMomentum pWhadron = pjet1 + pjet2;
+ double pz = computeneutrinoz(lepton->momentum(), met);
+ FourMomentum ppseudoneutrino( sqrt(sqr(met.x()) + sqr(met.y()) + sqr(pz)), met.x(), met.y(), pz);
- if (pass_resolved) {
+ //compute leptonic, hadronic, combined pseudo-top
+ FourMomentum ppseudotoplepton = lepton->momentum() + ppseudoneutrino + pbjet1;
+ FourMomentum ppseudotophadron = pbjet2 + pWhadron;
+ FourMomentum pttbar = ppseudotoplepton + ppseudotophadron;
- if ( deltaR(bjets[0], *lepton) <= deltaR(bjets[1], *lepton) ) {
- pbjet1 = bjets[0].momentum();
- pbjet2 = bjets[1].momentum();
- } else {
- pbjet1 = bjets[1].momentum();
- pbjet2 = bjets[0].momentum();
- }
-
- double bestWmass = 1000.0*TeV;
- double mWPDG = 80.399*GeV;
- for (unsigned int i = 0; i < (lightjets.size() - 1); ++i) {
- for (unsigned int j = i + 1; j < lightjets.size(); ++j) {
- double wmass = (lightjets[i].momentum() + lightjets[j].momentum()).mass();
- if (fabs(wmass - mWPDG) < fabs(bestWmass - mWPDG)) {
- bestWmass = wmass;
- Wj1index = i;
- Wj2index = j;
- }
- }
- }
-
- FourMomentum pjet1 = lightjets[Wj1index].momentum();
- FourMomentum pjet2 = lightjets[Wj2index].momentum();
-
- // compute hadronic W boson
- FourMomentum pWhadron = pjet1 + pjet2;
- double pz = computeneutrinoz(lepton->momentum(), met);
- FourMomentum ppseudoneutrino( sqrt(sqr(met.x()) + sqr(met.y()) + sqr(pz)), met.x(), met.y(), pz);
-
- //compute leptonic, hadronic, combined pseudo-top
- FourMomentum ppseudotoplepton = lepton->momentum() + ppseudoneutrino + pbjet1;
- FourMomentum ppseudotophadron = pbjet2 + pWhadron;
- FourMomentum pttbar = ppseudotoplepton + ppseudotophadron;
-
- fillHists("top_pt_res", ppseudotophadron.pt()/GeV, weight);
- fillHists("top_absrap_res", ppseudotophadron.absrap(), weight);
- fillHists("ttbar_pt_res", pttbar.pt()/GeV, weight);
- fillHists("ttbar_absrap_res", pttbar.absrap(), weight);
- fillHists("ttbar_m_res", pttbar.mass()/GeV, weight);
- }
-
- if (pass_boosted) {// Boosted selection
- double hadtop_pt= momentum(trimmed_jets.at(fatJetIndex)).pt() / GeV;
- double hadtop_absrap= momentum(trimmed_jets.at(fatJetIndex)).absrap();
- fillHists("top_pt_boost", hadtop_pt, weight);
- fillHists("top_absrap_boost", hadtop_absrap, weight);
- }
+ fillHists("top_pt_res", ppseudotophadron.pt()/GeV, weight);
+ fillHists("top_absrap_res", ppseudotophadron.absrap(), weight);
+ fillHists("ttbar_pt_res", pttbar.pt()/GeV, weight);
+ fillHists("ttbar_absrap_res", pttbar.absrap(), weight);
+ fillHists("ttbar_m_res", pttbar.mass()/GeV, weight);
}
- void finalize() {
- // Normalize to cross-section
- const double sf = (crossSection() / sumOfWeights());
- for (HistoMap::value_type& hist : _h) {
- scale(hist.second, sf);
- if (hist.first.find("_norm") != string::npos) normalize(hist.second);
- }
+ if (pass_boosted) {// Boosted selection
+ double hadtop_pt= momentum(trimmed_jets.at(fatJetIndex)).pt() / GeV;
+ double hadtop_absrap= momentum(trimmed_jets.at(fatJetIndex)).absrap();
+ fillHists("top_pt_boost", hadtop_pt, weight);
+ fillHists("top_absrap_boost", hadtop_absrap, weight);
+ }
+ }
+
+
+ void finalize() {
+ // Normalize to cross-section
+ const double sf = (crossSection() / sumOfWeights());
+ for (HistoMap::value_type& hist : _h) {
+ scale(hist.second, sf);
+ if (hist.first.find("_norm") != string::npos) normalize(hist.second);
+ }
+ }
+
+
+ void bookHists(std::string name, unsigned int index) {
+ _h[name] = bookHisto1D(index, 1 ,1);
+ _h[name + "_norm"] = bookHisto1D(index + 1, 1 ,1);
+ }
+
+
+ void fillHists(std::string name, double value, double weight) {
+ _h[name]->fill(value, weight);
+ _h[name + "_norm"]->fill(value, weight);
+ }
+
+
+ double _mT(const FourMomentum &l, const Vector3 &met) const {
+ return sqrt(2.0 * l.pT() * met.mod() * (1 - cos(deltaPhi(l, met))) );
+ }
+
+
+ double tau32(const fastjet::PseudoJet &jet, double jet_rad) const {
+ double alpha = 1.0;
+ fjcontrib::Nsubjettiness::NormalizedCutoffMeasure normalized_measure(alpha, jet_rad, 1000000);
+ // WTA definition
+ // Nsubjettiness::OnePass_WTA_KT_Axes wta_kt_axes;
+ // as in JetSubStructure recommendations
+ fjcontrib::Nsubjettiness::KT_Axes kt_axes;
+
+ /// NsubjettinessRatio uses the results from Nsubjettiness to calculate the ratio
+ /// tau_N/tau_M, where N and M are specified by the user. The ratio of different tau values
+ /// is often used in analyses, so this class is helpful to streamline code.
+ fjcontrib::Nsubjettiness::NsubjettinessRatio tau32_kt(3, 2, kt_axes, normalized_measure);
+
+ double tau32 = tau32_kt.result(jet);
+ return tau32;
+ }
+
+
+ double computeneutrinoz(const FourMomentum& lepton, const Vector3 &met) const {
+ //computing z component of neutrino momentum given lepton and met
+ double pzneutrino;
+ double m_W = 80.399; // in GeV, given in the paper
+ double k = (( sqr( m_W ) - sqr( lepton.mass() ) ) / 2 ) + (lepton.px() * met.x() + lepton.py() * met.y());
+ double a = sqr ( lepton.E() )- sqr ( lepton.pz() );
+ double b = -2*k*lepton.pz();
+ double c = sqr( lepton.E() ) * sqr( met.mod() ) - sqr( k );
+ double discriminant = sqr(b) - 4 * a * c;
+ double quad[2] = { (- b - sqrt(discriminant)) / (2 * a), (- b + sqrt(discriminant)) / (2 * a) }; //two possible quadratic solns
+ if (discriminant < 0) pzneutrino = - b / (2 * a); //if the discriminant is negative
+ else { //if the discriminant is greater than or equal to zero, take the soln with smallest absolute value
+ double absquad[2];
+ for (int n=0; n<2; ++n) absquad[n] = fabs(quad[n]);
+ if (absquad[0] < absquad[1]) pzneutrino = quad[0];
+ else pzneutrino = quad[1];
}
- void bookHists(std::string name, unsigned int index) {
- _h[name] = bookHisto1D(index, 1 ,1);
- _h[name + "_norm"] = bookHisto1D(index + 1, 1 ,1);
- }
+ return pzneutrino;
+ }
- void fillHists(std::string name, double value, double weight) {
- _h[name]->fill(value, weight);
- _h[name + "_norm"]->fill(value, weight);
- }
- double _mT(const FourMomentum &l, const Vector3 &met) const {
- return sqrt(2.0 * l.pT() * met.mod() * (1 - cos(deltaPhi(l, met))) );
- }
+ private:
- double tau32(const fastjet::PseudoJet &jet, double jet_rad) const {
- double alpha = 1.0;
- Nsubjettiness::NormalizedCutoffMeasure normalized_measure(alpha, jet_rad, 1000000);
- // WTA definition
- // Nsubjettiness::OnePass_WTA_KT_Axes wta_kt_axes;
- // as in JetSubStructure recommendations
- Nsubjettiness::KT_Axes kt_axes;
+ /// @name Objects that are used by the event selection decisions
+ typedef map<string, Histo1DPtr> HistoMap;
+ HistoMap _h;
- /// NsubjettinessRatio uses the results from Nsubjettiness to calculate the ratio
- /// tau_N/tau_M, where N and M are specified by the user. The ratio of different tau values
- /// is often used in analyses, so this class is helpful to streamline code.
- Nsubjettiness::NsubjettinessRatio tau32_kt(3, 2, kt_axes, normalized_measure);
-
- double tau32 = tau32_kt.result(jet);
- return tau32;
- }
-
- double computeneutrinoz(const FourMomentum& lepton, const Vector3 &met) const {
- //computing z component of neutrino momentum given lepton and met
- double pzneutrino;
- double m_W = 80.399; // in GeV, given in the paper
- double k = (( sqr( m_W ) - sqr( lepton.mass() ) ) / 2 ) + (lepton.px() * met.x() + lepton.py() * met.y());
- double a = sqr ( lepton.E() )- sqr ( lepton.pz() );
- double b = -2*k*lepton.pz();
- double c = sqr( lepton.E() ) * sqr( met.mod() ) - sqr( k );
- double discriminant = sqr(b) - 4 * a * c;
- double quad[2] = { (- b - sqrt(discriminant)) / (2 * a), (- b + sqrt(discriminant)) / (2 * a) }; //two possible quadratic solns
- if (discriminant < 0) pzneutrino = - b / (2 * a); //if the discriminant is negative
- else { //if the discriminant is greater than or equal to zero, take the soln with smallest absolute value
- double absquad[2];
- for (int n=0; n<2; ++n) absquad[n] = fabs(quad[n]);
- if (absquad[0] < absquad[1]) pzneutrino = quad[0];
- else pzneutrino = quad[1];
- }
-
- return pzneutrino;
- }
-
- private:
-
- /// @name Objects that are used by the event selection decisions
- typedef map<string, Histo1DPtr> HistoMap;
- HistoMap _h;
};
- // The hook for the plugin system
+
DECLARE_RIVET_PLUGIN(ATLAS_2017_I1614149);
+
+
}
diff --git a/analyses/pluginATLAS/ATLAS_2018_I1656578.cc b/analyses/pluginATLAS/ATLAS_2018_I1656578.cc
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2018_I1656578.cc
@@ -0,0 +1,244 @@
+#include "Rivet/Analysis.hh"
+#include "Rivet/Projections/FinalState.hh"
+#include "Rivet/Projections/VetoedFinalState.hh"
+#include "Rivet/Projections/IdentifiedFinalState.hh"
+#include "Rivet/Projections/PromptFinalState.hh"
+#include "Rivet/Projections/DressedLeptons.hh"
+#include "Rivet/Projections/FastJets.hh"
+#include "Rivet/Projections/MissingMomentum.hh"
+
+namespace Rivet {
+
+
+ /// ttbar l+jets cross sections at 13 TeV
+ class ATLAS_2018_I1656578 : public Analysis {
+ public:
+
+ /// Constructor
+ DEFAULT_RIVET_ANALYSIS_CTOR(ATLAS_2018_I1656578);
+
+
+ /// Book cuts and projections
+ void init() {
+ // Eta ranges
+ Cut eta_full = (Cuts::abseta < 5.0);
+ Cut lep_cuts = (Cuts::abseta < 2.5) && (Cuts::pT > 25*GeV);
+
+ // All final state particles
+ FinalState fs(eta_full);
+
+ // Get photons to dress leptons
+ IdentifiedFinalState all_photons(fs);
+ all_photons.acceptIdPair(PID::PHOTON);
+
+ PromptFinalState photons(Cuts::abspid == PID::PHOTON, true);
+ declare(photons, "photons");
+
+ // Projection to find the electrons
+ PromptFinalState electrons(Cuts::abspid == PID::ELECTRON, true);
+
+ DressedLeptons dressedelectrons(photons, electrons, 0.1, lep_cuts);
+ declare(dressedelectrons, "elecs");
+
+ DressedLeptons ewdressedelectrons(all_photons, electrons, 0.1, eta_full);
+
+ // Projection to find the muons
+ PromptFinalState muons(Cuts::abspid == PID::MUON, true);
+
+ DressedLeptons dressedmuons(photons, muons, 0.1, lep_cuts);
+ declare(dressedmuons, "muons");
+
+ DressedLeptons ewdressedmuons(all_photons, muons, 0.1, eta_full);
+
+ // Projection to find MET
+ declare(MissingMomentum(fs), "MET");
+
+ // Jet clustering.
+ VetoedFinalState vfs(fs);
+ vfs.addVetoOnThisFinalState(ewdressedelectrons);
+ vfs.addVetoOnThisFinalState(ewdressedmuons);
+ FastJets jets(vfs, FastJets::ANTIKT, 0.4, JetAlg::ALL_MUONS, JetAlg::DECAY_INVISIBLES);
+ declare(jets, "jets");
+
+
+ _h["absPout_inc"] = bookHisto1D(114, 1, 1);
+ _h["absPout_inc_norm"] = bookHisto1D(115, 1, 1);
+ _h["ptpseudotophadron_r1"] = bookHisto1D(98, 1, 1);
+ _h["ptpseudotophadron_r1_norm"] = bookHisto1D(99, 1, 1);
+ _h["ptttbar_r1"] = bookHisto1D(100, 1, 1);
+ _h["ptttbar_r1_norm"] = bookHisto1D(101, 1, 1);
+ _h["absPout_r1"] = bookHisto1D(96, 1, 1);
+ _h["absPout_r1_norm"] = bookHisto1D(97, 1, 1);
+ _h["ptpseudotophadron_r2"] = bookHisto1D(110, 1, 1);
+ _h["ptpseudotophadron_r2_norm"] = bookHisto1D(111, 1, 1);
+ _h["ptttbar_r2"] = bookHisto1D(112, 1, 1);
+ _h["ptttbar_r2_norm"] = bookHisto1D(113, 1, 1);
+ _h["absPout_r2"] = bookHisto1D(108, 1, 1);
+ _h["absPout_r2_norm"] = bookHisto1D(109, 1, 1);
+ _h["ptpseudotophadron_r3"] = bookHisto1D(104, 1, 1);
+ _h["ptpseudotophadron_r3_norm"] = bookHisto1D(105, 1, 1);
+ _h["ptttbar_r3"] = bookHisto1D(106, 1, 1);
+ _h["ptttbar_r3_norm"] = bookHisto1D(107, 1, 1);
+ _h["absPout_r3"] = bookHisto1D(102, 1, 1);
+ _h["absPout_r3_norm"] = bookHisto1D(103, 1, 1);
+
+ }
+
+
+ void analyze(const Event& event) {
+
+ const double weight = event.weight();
+
+ // Get the selected objects, using the projections.
+ vector<DressedLepton> electrons = apply<DressedLeptons>(event, "elecs").dressedLeptons();
+ vector<DressedLepton> muons = apply<DressedLeptons>(event, "muons").dressedLeptons();
+ const Jets& jets = apply<FastJets>(event, "jets").jetsByPt(Cuts::pT > 25*GeV && Cuts::abseta < 2.5);
+
+ const Vector3 met = apply<MissingMomentum>(event, "MET").vectorMPT();
+
+ Jets bjets, lightjets;
+ for (Jet jet : jets) {
+ bool b_tagged = jet.bTagged(Cuts::pT > 5*GeV);
+ if ( b_tagged && bjets.size() < 2) bjets += jet;
+ else lightjets += jet;
+ }
+
+ bool single_electron = (electrons.size() == 1) && (muons.empty());
+ bool single_muon = (muons.size() == 1) && (electrons.empty());
+
+
+ DressedLepton *lepton = NULL;
+ if (single_electron) lepton = &electrons[0];
+ else if (single_muon) lepton = &muons[0];
+
+ if (!single_electron && !single_muon) vetoEvent;
+
+ bool num_b_tagged_jets = (bjets.size() == 2);
+ if (!num_b_tagged_jets) vetoEvent;
+
+ if (jets.size() < 4) vetoEvent;
+
+ bool reg_4jex2bin = (jets.size() == 4);
+ bool reg_5jex2bin = (jets.size() == 5);
+ bool reg_6jin2bin = (jets.size() >= 6);
+
+
+ FourMomentum pbjet1; //Momentum of bjet1
+ FourMomentum pbjet2; //Momentum of bjet
+
+ if ( deltaR(bjets[0], *lepton) <= deltaR(bjets[1], *lepton) ) {
+ pbjet1 = bjets[0].momentum();
+ pbjet2 = bjets[1].momentum();
+ } else {
+ pbjet1 = bjets[1].momentum();
+ pbjet2 = bjets[0].momentum();
+ }
+
+ double bestWmass = 1000.0*TeV;
+ double mWPDG = 80.399*GeV;
+ int Wj1index = -1, Wj2index = -1;
+ for (unsigned int i = 0; i < (lightjets.size() - 1); ++i) {
+ for (unsigned int j = i + 1; j < lightjets.size(); ++j) {
+ double wmass = (lightjets[i].momentum() + lightjets[j].momentum()).mass();
+ if (fabs(wmass - mWPDG) < fabs(bestWmass - mWPDG)) {
+ bestWmass = wmass;
+ Wj1index = i;
+ Wj2index = j;
+ }
+ }
+ }
+
+ FourMomentum pjet1 = lightjets[Wj1index].momentum();
+ FourMomentum pjet2 = lightjets[Wj2index].momentum();
+
+ // compute hadronic W boson
+ FourMomentum pWhadron = pjet1 + pjet2;
+ double pz = computeneutrinoz(lepton->momentum(), met);
+ FourMomentum ppseudoneutrino( sqrt(sqr(met.x()) + sqr(met.y()) + sqr(pz)), met.x(), met.y(), pz);
+
+ //compute leptonic, hadronic, combined pseudo-top
+ FourMomentum ppseudotoplepton = lepton->momentum() + ppseudoneutrino + pbjet1;
+ FourMomentum ppseudotophadron = pbjet2 + pWhadron;
+ FourMomentum pttbar = ppseudotoplepton + ppseudotophadron;
+
+ Vector3 z_versor(0,0,1);
+ Vector3 vpseudotophadron = ppseudotophadron.vector3();
+ Vector3 vpseudotoplepton = ppseudotoplepton.vector3();
+ // Variables
+ double absPout = fabs(vpseudotophadron.dot((vpseudotoplepton.cross(z_versor))/(vpseudotoplepton.cross(z_versor).mod())));
+
+ //pseudotop hadrons and leptons fill histogram
+ if (reg_4jex2bin) {
+ _h["ptpseudotophadron_r1"]->fill(ppseudotophadron.pt(), weight); //pT of pseudo top hadron
+ _h["ptpseudotophadron_r1_norm"]->fill(ppseudotophadron.pt(), weight); //pT of pseudo top hadron
+ _h["ptttbar_r1"]->fill(pttbar.pt(), weight); //fill pT of ttbar in combined channel
+ _h["ptttbar_r1_norm"]->fill(pttbar.pt(), weight); //fill pT of ttbar in combined channel
+ _h["absPout_r1"]->fill(absPout, weight);
+ _h["absPout_r1_norm"]->fill(absPout, weight);
+ }
+ if (reg_5jex2bin) {
+ _h["ptpseudotophadron_r2"]->fill(ppseudotophadron.pt(), weight); //pT of pseudo top hadron
+ _h["ptpseudotophadron_r2_norm"]->fill(ppseudotophadron.pt(), weight); //pT of pseudo top hadron
+ _h["ptttbar_r2"]->fill(pttbar.pt(), weight); //fill pT of ttbar in combined channel
+ _h["ptttbar_r2_norm"]->fill(pttbar.pt(), weight); //fill pT of ttbar in combined channel
+ _h["absPout_r2"]->fill(absPout, weight);
+ _h["absPout_r2_norm"]->fill(absPout, weight);
+ }
+ if (reg_6jin2bin) {
+ _h["ptpseudotophadron_r3"]->fill(ppseudotophadron.pt(), weight); //pT of pseudo top hadron
+ _h["ptpseudotophadron_r3_norm"]->fill(ppseudotophadron.pt(), weight); //pT of pseudo top hadron
+ _h["ptttbar_r3"]->fill(pttbar.pt(), weight); //fill pT of ttbar in combined channel
+ _h["ptttbar_r3_norm"]->fill(pttbar.pt(), weight); //fill pT of ttbar in combined channel
+ _h["absPout_r3"]->fill(absPout, weight);
+ _h["absPout_r3_norm"]->fill(absPout, weight);
+ }
+ _h["absPout_inc"]->fill(absPout, weight);
+ _h["absPout_inc_norm"]->fill(absPout, weight);
+ }
+
+
+ void finalize() {
+ // Normalize to cross-section
+ const double sf = (crossSection() / sumOfWeights());
+ for (auto hist : _h) {
+ scale(hist.second, sf);
+ // Normalized distributions
+ if (hist.first.find("_norm") != string::npos) normalize(hist.second);
+ }
+ }
+
+
+ double computeneutrinoz(const FourMomentum& lepton, const Vector3 &met) const {
+ // computing z component of neutrino momentum given lepton and met
+ double pzneutrino;
+ double m_W = 80.399; // in GeV, given in the paper
+ double k = (( sqr( m_W ) - sqr( lepton.mass() ) ) / 2 ) + (lepton.px() * met.x() + lepton.py() * met.y());
+ double a = sqr ( lepton.E() )- sqr ( lepton.pz() );
+ double b = -2*k*lepton.pz();
+ double c = sqr( lepton.E() ) * sqr( met.mod() ) - sqr( k );
+ double discriminant = sqr(b) - 4 * a * c;
+ double quad[2] = { (- b - sqrt(discriminant)) / (2 * a), (- b + sqrt(discriminant)) / (2 * a) }; //two possible quadratic solns
+ if (discriminant < 0) pzneutrino = - b / (2 * a); //if the discriminant is negative
+ else { //if the discriminant is greater than or equal to zero, take the soln with smallest absolute value
+ double absquad[2];
+ for (int n=0; n<2; ++n) absquad[n] = fabs(quad[n]);
+ if (absquad[0] < absquad[1]) pzneutrino = quad[0];
+ else pzneutrino = quad[1];
+ }
+ return pzneutrino;
+ }
+
+
+ private:
+
+ /// @name Objects that are used by the event selection decisions
+ map<string, Histo1DPtr> _h;
+
+ };
+
+
+ // The hook for the plugin system
+ DECLARE_RIVET_PLUGIN(ATLAS_2018_I1656578);
+
+
+}
diff --git a/analyses/pluginATLAS/ATLAS_2018_I1656578.info b/analyses/pluginATLAS/ATLAS_2018_I1656578.info
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2018_I1656578.info
@@ -0,0 +1,45 @@
+Name: ATLAS_2018_I1656578
+Year: 2018
+Summary: Differential $t\bar{t}$ $l$+jets cross-sections at 13~TeV
+Experiment: ATLAS
+Collider: LHC
+InspireID: 1656578
+Status: VALIDATED
+Authors:
+ - Francesco La Ruffa <francesco.la.ruffa@cern.ch>
+ - Christian Gutschow <chris.g@cern.ch>
+References:
+ - Submitted to JHEP
+ - arXiv:1802.06572 [hep-ex]
+Keywords:
+ - TTBAR
+ - NONALLHADRONIC
+ - JETS
+RunInfo:
+ non-all-hadronic ttbar production at 13 TeV
+Luminosity_fb: 3.2
+NeedCrossSection: yes
+Beams: [p+, p+]
+Energies: [13000]
+PtCuts: [25.]
+Description:
+ 'Measurements of differential cross sections of top quark pair production in association with jets by the ATLAS experiment at the
+ LHC are presented. The measurements are performed as functions of the top quark transverse momentum, the transverse momentum of
+ the top quark-antitop quark system and the out-of-plane transverse momentum using data from pp collisions at $\sqrt{s}=13$ TeV
+ collected by the ATLAS detector at the LHC in 2015 and corresponding to an integrated luminosity of 3.2 $\text{fb}^{-1}$. The top quark
+ pair events are selected in the lepton (electron or muon) + jets channel. The measured cross sections, which are compared to several
+ predictions, allow a detailed study of top quark production.'
+BibKey: Aaboud:2018uzf
+BibTex: '@article{Aaboud:2018uzf,
+ author = "Aaboud, Morad and others",
+ title = "{Measurements of differential cross sections of top quark
+ pair production in association with jets in ${pp}$
+ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector}",
+ collaboration = "ATLAS",
+ year = "2018",
+ eprint = "1802.06572",
+ archivePrefix = "arXiv",
+ primaryClass = "hep-ex",
+ reportNumber = "CERN-EP-2017-227",
+ SLACcitation = "%%CITATION = ARXIV:1802.06572;%%"
+}'
diff --git a/analyses/pluginATLAS/ATLAS_2018_I1656578.plot b/analyses/pluginATLAS/ATLAS_2018_I1656578.plot
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2018_I1656578.plot
@@ -0,0 +1,141 @@
+# BEGIN PLOT /ATLAS_2018_I1656578/d.
+LegendAlign=r
+XTwosidedTicks=1
+YTwosidedTicks=1
+LeftMargin=1.9
+YLabelSep=8.0
+RatioPlotYMin=0.4
+RatioPlotYMax=1.6
+Title=combined lepton channels
+# END PLOT
+
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d114-x01-y01
+Title=combined lepton channels, 4ji2bi
+XLabel=$|p_{\text{out}}^{t\bar{t}}|$ [GeV]
+YLabel=$\dfrac{\text{d}\sigma^\text{fid}}{\text{d}|p_{\text{out}}^{t\bar{t}}|}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d115-x01-y01
+Title=combined lepton channels, 4ji2bi
+XLabel=$|p_\text{out}^{t\bar{t}}|$ [GeV]
+YLabel=$1/\sigma$ $\text{d}\sigma / \text{d}|p_\text{out}^{t\bar{t}}|$ [1/GeV]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d100-x01-y01
+Title=combined lepton channels, 4je2bi
+XLabel=$p_{\text{T}}^{t\bar{t}}$ [GeV]
+YLabel=$\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}^{t\bar{t}}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d96-x01-y01
+Title=combined lepton channels, 4je2bi
+RatioPlotYMin=0.0
+RatioPlotYMax=2.0
+XLabel=$|p_{\text{out}}^{t\bar{t}}|$ [GeV]
+YLabel=$\dfrac{\text{d}\sigma^\text{fid}}{\text{d}|p_{\text{out}}^{t\bar{t}}|}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d98-x01-y01
+Title=combined lepton channels, 4je2bi
+XLabel=$p_{\text{T}}^{t,\text{had}}$ [GeV]
+YLabel=$\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}}^{t,\text{had}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d101-x01-y01
+Title=combined lepton channels, 4je2bi
+XLabel=$p_{\text{T}}^{t\bar{t}}$ [GeV]
+YLabel=$1/\sigma$ $\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}^{t\bar{t}}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d97-x01-y01
+Title=combined lepton channels, 4je2bi
+RatioPlotYMin=0.0
+RatioPlotYMax=2.0
+XLabel=$|p_{\text{out}}^{t\bar{t}}|$ [GeV]
+YLabel=$1/\sigma$ $\dfrac{\text{d}\sigma^\text{fid}}{\text{d}|p_{\text{out}}^{t\bar{t}}|}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d99-x01-y01
+Title=combined lepton channels, 4je2bi
+XLabel=$p_{\text{T}}^{t,\text{had}}$ [GeV]
+YLabel=$1/\sigma$ $\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}}^{t,\text{had}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d112-x01-y01
+Title=combined lepton channels, 5je2bi
+XLabel=$p_{\text{T}}^{t\bar{t}}$ [GeV]
+YLabel=$\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}^{t\bar{t}}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d108-x01-y01
+Title=combined lepton channels, 5je2bi
+XLabel=$|p_{\text{out}}^{t\bar{t}}|$ [GeV]
+YLabel=$\dfrac{\text{d}\sigma^\text{fid}}{\text{d}|p_{\text{out}}^{t\bar{t}}|}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d110-x01-y01
+Title=combined lepton channels, 5je2bi
+XLabel=$p_{\text{T}}^{t,\text{had}}$ [GeV]
+YLabel=$\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}}^{t,\text{had}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d113-x01-y01
+Title=combined lepton channels, 5je2bi
+XLabel=$p_{\text{T}}^{t\bar{t}}$ [GeV]
+YLabel=$1/\sigma$ $\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}^{t\bar{t}}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d109-x01-y01
+Title=combined lepton channels, 5je2bi
+XLabel=$|p_{\text{out}}^{t\bar{t}}|$ [GeV]
+YLabel=$1/\sigma$ $\dfrac{\text{d}\sigma^\text{fid}}{\text{d}|p_{\text{out}}^{t\bar{t}}|}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d11-x01-y01
+Title=combined lepton channels, 5je2bi
+XLabel=$p_{\text{T}}^{t,\text{had}}$ [GeV]
+YLabel=$1/\sigma$ $\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}}^{t,\text{had}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d106-x01-y01
+Title=combined lepton channels, 6ji2bi
+XLabel=$p_{\text{T}}^{t\bar{t}}$ [GeV]
+YLabel=$\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}^{t\bar{t}}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d102-x01-y01
+Title=combined lepton channels, 6ji2bi
+XLabel=$|p_{\text{out}}^{t\bar{t}}|$ [GeV]
+YLabel=$\dfrac{\text{d}\sigma^\text{fid}}{\text{d}|p_{\text{out}}^{t\bar{t}}|}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d104-x01-y01
+Title=combined lepton channels, 6ji2bi
+XLabel=$p_{\text{T}}^{t,\text{had}}$ [GeV]
+YLabel=$\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}}^{t,\text{had}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d107-x01-y01
+Title=combined lepton channels, 6ji2bi
+XLabel=$p_{\text{T}}^{t\bar{t}}$ [GeV]
+YLabel=$1/\sigma$ $\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}^{t\bar{t}}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d103-x01-y01
+Title=combined lepton channels, 6ji2bi
+XLabel=$|p_{\text{out}}^{t\bar{t}}|$ [GeV]
+YLabel=$1/\sigma$ $\dfrac{\text{d}\sigma^\text{fid}}{\text{d}|p_{\text{out}}^{t\bar{t}}|}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
+
+# BEGIN PLOT /ATLAS_2018_I1656578/d105-x01-y01
+Title=combined lepton channels, 6ji2bi
+XLabel=$p_{\text{T}}^{t,\text{had}}$ [GeV]
+YLabel=$1/\sigma$ $\dfrac{\text{d}\sigma^\text{fid}}{\text{d}p_{\text{T}}^{t,\text{had}}}$ [$\dfrac{\text{pb}}{\text{GeV}}$]
+# END PLOT
diff --git a/analyses/pluginATLAS/ATLAS_2018_I1656578.yoda b/analyses/pluginATLAS/ATLAS_2018_I1656578.yoda
new file mode 100644
--- /dev/null
+++ b/analyses/pluginATLAS/ATLAS_2018_I1656578.yoda
@@ -0,0 +1,11580 @@
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d01-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d01-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t1
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.104670e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.293530e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.010640e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.902540e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.631050e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.104670e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.077140e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.216200e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.672000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.091890e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.293530e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.077140e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.098410e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.232440e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.685830e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.010640e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.216200e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.098410e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.270760e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -5.875750e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.902540e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.672000e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.232440e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.270760e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -7.569440e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.631050e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.091890e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.685830e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.875750e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.569440e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d02-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d02-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t2
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.016680e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.071640e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.291660e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.523080e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.250410e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.063090e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.927470e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -8.595670e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.062400e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.391420e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.598030e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -5.164470e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.359370e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.033620e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.764530e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -8.565450e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.072140e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.079580e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.374990e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.701610e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.700420e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.113410e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.866040e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.809690e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.457060e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.182000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.923800e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -9.423250e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.247240e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -7.906620e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.598450e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.142670e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.245230e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.628900e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.826500e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -9.047800e-05 0.000000e+00 0.000000e+00
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+8.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.818290e-02 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.713840e-02 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.666570e-04 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -8.167810e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.048980e-04 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.461430e-01 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.993060e-02 0.000000e+00 0.000000e+00
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+1.600000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.108820e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.754650e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.519410e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.856630e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.720250e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.776100e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.873390e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.358060e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.296390e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.530860e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.061560e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.822310e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.134130e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.365200e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d03-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d03-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t3
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.884660e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -9.359730e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.466840e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.938200e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.372160e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.721010e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.540110e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.385250e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -9.909240e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.422430e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.381770e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.519890e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.175670e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.867350e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.678400e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.541180e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.023130e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.548220e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.350870e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.181340e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.156540e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.166340e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.755120e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -9.231160e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.451580e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000280e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.733940e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.601890e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.058870e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.288510e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.621110e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.553460e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.704760e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.085510e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.605620e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.627690e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d04-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d04-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t4
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.498160e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.756130e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.316220e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.311990e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.873220e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.935360e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.569600e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.255610e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.473240e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.540420e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.024180e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.967680e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.772760e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.286500e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.947940e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -6.342660e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.285290e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.964580e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.255590e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -6.703260e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.438800e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.041760e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.950980e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.824160e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.065540e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -9.948960e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -9.913130e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.312990e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.769370e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.203480e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.141910e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.424700e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.847190e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.610700e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.083500e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.321600e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d05-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d05-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t5
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.191830e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.270530e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.710050e-05 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.211860e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.250040e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.988530e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.609070e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.108280e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.953200e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.871130e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.820850e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.842070e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.958830e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -8.974350e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.326750e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.398950e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.089810e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.092530e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.425400e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.306610e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.727700e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.640770e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.349510e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.559400e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.509380e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.995990e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.338190e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.615760e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.093790e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.906680e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.177810e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.994420e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.385170e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.396230e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.446340e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.184350e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.807550e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.960600e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.104670e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.939920e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.229940e-04 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.554320e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.746680e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.533240e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.740570e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.197060e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.994630e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.684550e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.398090e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.674060e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.713790e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.183450e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.251120e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.816830e-04 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.444910e-04 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.316010e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.380590e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.884610e-05 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.917450e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.631040e-04 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.891390e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.211510e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.307690e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.764370e-04 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.954050e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.457590e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.789370e-04 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.192570e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.229040e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.541930e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.571450e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.850890e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.724460e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.210060e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.073090e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.191460e-04 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.220940e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.341510e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.572660e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.614160e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.561040e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.415710e-04 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.764290e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.162220e-05 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.787130e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.943870e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.939060e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.730680e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.226610e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.496680e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.960270e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.746240e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.884190e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.186760e-04 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.944070e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.643690e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -8.678510e-04 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.497130e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.574350e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.862890e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.739880e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.726040e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.134270e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.531240e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.204850e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.058010e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.445100e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.487510e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d06-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d06-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t6
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.531070e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.032740e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.122130e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.366790e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -8.565100e-05 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.518820e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.729770e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.733390e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.192110e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.990790e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.873530e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.454330e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.692810e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.592340e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.668390e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.703170e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.269310e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.524470e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.612380e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.743640e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.013310e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.276860e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -8.877810e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.832230e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.857530e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.826660e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -9.454070e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.552140e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.410290e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.531110e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.036070e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.973650e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.105220e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.455500e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.007260e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.167180e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d07-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d07-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t7
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.233570e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.644100e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -4.189310e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.605360e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.403440e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.577080e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.190510e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.833900e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.573780e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.695490e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.231740e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.721610e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.429040e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.001350e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.321360e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.373740e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.316680e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.516910e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.612300e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.227020e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.028940e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.445800e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.476660e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.207400e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.521160e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.012300e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.999800e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.448520e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.482210e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.050600e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.799940e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.961180e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.352660e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.479750e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.164580e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -5.037470e-04 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d08-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d08-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t8
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.894410e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.222930e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.737600e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.789060e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.635880e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.905600e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.189170e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.059670e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.380180e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.170450e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.450630e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.683030e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.445710e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.169040e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.579110e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.086010e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.678840e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.494540e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.027480e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -9.619230e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.705050e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.332780e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.515550e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.875950e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.124740e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.821500e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.733940e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.177720e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.334550e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.358550e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.064040e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.183230e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.093840e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.259220e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.983620e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.078310e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.069370e-04 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.524790e-05 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.231590e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.135290e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.397770e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.119780e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.529560e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.069750e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.030190e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.261020e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.499100e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -5.250490e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.017220e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.682180e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.454340e-04 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.450370e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.660490e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.343350e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -9.117420e-05 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.933340e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.334400e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.423840e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.974220e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.350230e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -8.954310e-04 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.332030e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.311900e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.252220e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.556330e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.211500e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.261270e-04 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.218790e-04 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.491670e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.588460e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.417120e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.758100e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.017590e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.209700e-04 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.268120e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -8.245510e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.732870e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.597290e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.610890e-04 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.108750e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.420100e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.858260e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.815730e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.238130e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.981400e-05 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.115820e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.704460e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.615940e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.754440e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.079700e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.733950e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.046240e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.023350e-04 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.111940e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.176220e-04 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.385190e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.838920e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.267130e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.207200e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.137010e-04 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.382400e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.382860e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.193600e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -6.977760e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.164290e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.255860e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.391210e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.805860e-04 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d09-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d09-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t9
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -8.225480e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -6.084020e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.835680e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.422170e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.294240e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.587220e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.237610e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.242460e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.028790e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.107180e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.151560e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.235290e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.273630e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.094590e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.851540e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.187790e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.124360e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.883480e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.296410e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.553470e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.845860e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -8.819930e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.940270e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.185310e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.507790e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.888340e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.162320e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.478320e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.366980e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.407700e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.470950e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.563310e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.418490e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.917950e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.776350e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.359140e-04 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d10-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d10-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t10
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.768830e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.374060e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -7.175560e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.815870e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.283730e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -5.448760e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -9.049960e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.728330e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.205130e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.512140e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.889800e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.618240e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -7.086440e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.952940e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.380410e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.679100e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.446790e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.307690e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.204340e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.161440e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -4.810050e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.782400e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.486020e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.179760e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.507250e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.700270e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.933470e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.110930e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.869880e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.261340e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.915660e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.003660e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.042160e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.640630e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.321120e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.354180e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d11-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d11-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t11
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.832350e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.477540e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -6.329050e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.795810e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.548950e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -3.840460e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -7.569760e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -1.131560e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 2.506590e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 5.738570e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 6.883630e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 3.346810e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 -1.033780e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 2.332940e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 -1.629280e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -1.502730e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 8.175980e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.832350e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.468160e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.396310e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.484940e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.090460e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.941630e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -2.028360e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -4.761250e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 -1.405100e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 3.994020e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 5.089410e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 2.339450e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 -9.366060e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 -3.496120e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 -1.951180e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -1.853460e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 -6.507120e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.477540e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.468160e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.727650e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.369450e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.461560e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 1.793800e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 1.437460e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 4.672060e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 -9.895930e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 -3.639470e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 -8.279500e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 -1.403650e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 6.427920e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 3.498600e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 5.317270e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 1.396480e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 -4.084720e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.329050e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.396310e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.727650e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.734610e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.470540e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -6.933530e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 2.551370e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 1.252220e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 3.330970e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 -2.960190e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 -4.962590e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 -3.384450e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 1.600220e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 2.065170e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 -2.195510e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -7.885070e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 5.975410e-03 0.000000e+00 0.000000e+00
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d12-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d12-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t12
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d13-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d13-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t13
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d14-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d14-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t14
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d15-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d15-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t15
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d16-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d16-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t16
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d17-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d17-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t17
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+1.800000e+01 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -5.875540e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 5.069510e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d18-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d18-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t18
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.514810e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.640370e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.954110e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.324050e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.264060e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.587590e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -1.974060e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -2.231500e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -6.143370e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 -3.061900e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 5.350440e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 -9.834320e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 -7.325290e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 2.449430e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 -7.002510e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 2.487700e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -5.030520e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 -7.084350e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.534150e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.944430e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.501950e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.447870e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.829100e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.345800e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -1.480100e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 6.211390e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 1.663540e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 -8.291330e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 -2.263140e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 -3.805660e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 6.390290e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 3.946180e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 7.197190e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 -7.689980e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -2.698200e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 -6.959750e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.946050e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.011660e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -4.104800e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.878320e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.655220e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.548380e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 4.149630e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 4.146460e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -2.690120e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 -1.741090e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 -3.789260e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 -6.783520e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 7.977690e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 -6.240720e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 -5.322680e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 -3.422690e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -1.145380e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 -2.526800e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.460590e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.182310e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.078070e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.581040e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.197760e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.040030e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 4.016310e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 6.503630e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 9.250310e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 -2.531590e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 -5.112870e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 -3.779950e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 2.773220e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 4.107240e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 -4.646160e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 6.402750e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -2.391400e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 -4.902970e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.681040e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.503130e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.695760e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.650700e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.968070e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.581350e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -3.528100e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -2.665020e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -4.468630e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 2.699750e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 4.789600e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 2.245880e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 -1.397230e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 -3.695560e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 2.185630e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 5.188880e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -1.341990e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 3.110190e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.587650e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.185100e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.353730e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.489640e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.200070e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.074280e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -3.233480e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -2.705310e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 3.491270e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 6.852500e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 3.911870e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 1.232330e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 -1.623900e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 -4.343710e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 -3.211520e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 -1.264560e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -4.977980e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 -7.147080e-04 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d19-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d19-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t19
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.955520e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.539630e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.844230e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.870410e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.959150e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.071980e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 2.134270e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 2.104890e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 1.940520e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 1.833620e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 1.667780e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 1.464240e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 1.355430e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 1.267540e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 1.011860e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 9.479920e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 7.287920e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 3.228270e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.430140e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -8.604910e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.096550e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.581230e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.572380e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.429790e-02 0.000000e+00 0.000000e+00
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+2.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 2.466840e-02 0.000000e+00 0.000000e+00
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+2.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 2.636820e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 2.292440e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 1.494150e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 1.043450e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.290220e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.996740e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.275680e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.183110e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.005480e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.004010e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.914300e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 1.309160e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 1.878320e-02 0.000000e+00 0.000000e+00
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+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 5.017210e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 -3.118230e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 -6.223500e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 2.091840e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 -1.750560e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 5.126710e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 6.931990e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -1.473890e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 -1.868610e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.483340e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.555420e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.555050e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.496550e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.466620e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.278160e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -5.452430e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -3.017060e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 4.380240e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 1.427390e-02 0.000000e+00 0.000000e+00
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+4.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 8.067220e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 8.484630e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 2.919310e-03 0.000000e+00 0.000000e+00
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+4.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 1.933280e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 7.089400e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.070950e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.136250e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.237500e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.442660e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.540400e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.190720e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 1.392100e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -4.747750e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -3.833070e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 -2.952740e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 -1.388650e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 5.831370e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 1.467600e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 3.044700e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 2.153120e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 6.158170e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -8.466330e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 4.890030e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.088270e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.754610e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -7.940320e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.594300e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.957450e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.650250e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -1.073010e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 2.468700e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 2.428750e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 3.866120e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 -2.033220e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 -2.911540e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 -9.776740e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 -4.526560e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 5.398950e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 -5.644900e-05 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 4.006600e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.512170e-04 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d20-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d20-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t20
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.605170e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.251220e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.666920e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.197270e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.417110e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.605170e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.150700e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.346340e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.518070e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.810900e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.251220e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.150700e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.800550e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.399330e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.535630e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.666920e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.346340e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.800550e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.183400e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.172570e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.197270e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -7.518070e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.399330e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.183400e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.226170e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.417110e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.810900e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.535630e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.172570e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.226170e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d21-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d21-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t21
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.501580e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.790710e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.193680e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.679740e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.632380e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -9.293630e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.874310e-03 0.000000e+00 0.000000e+00
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d22-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d22-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t22
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.747110e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.300600e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.530510e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.437240e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.014240e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.237660e-04 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d23-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d23-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t23
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.773990e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -9.410590e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.520210e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.308670e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.458420e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.916820e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -8.750710e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.981240e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.585640e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.506080e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -8.443730e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.866280e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.858930e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.202180e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.945870e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.246280e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.380440e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.899850e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.874160e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.116850e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.807140e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.967750e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.185140e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.065420e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.611870e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.153730e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.084080e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.256310e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.540200e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.627260e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.209030e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.976980e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.190210e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.679230e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.913640e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.676360e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d24-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d24-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t24
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.752210e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.209410e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.137730e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.146450e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.226150e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.618230e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.599280e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.637930e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.385460e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.281820e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.631370e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.378990e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -9.693130e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.618540e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.142930e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.332220e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.859760e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.163740e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.253880e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.180580e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.856670e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.624190e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.815230e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.370320e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.408170e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.191640e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.542650e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.640310e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.068690e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.656590e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.197150e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.059190e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -7.665230e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.874740e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.851250e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.377720e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d25-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d25-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t25
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.887180e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.198420e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.204130e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.483320e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.621230e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.556740e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.839700e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.180040e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.851460e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.597570e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.444320e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.044170e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.043340e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.382120e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.136660e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.157430e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.410710e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.072260e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.169830e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.034460e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -4.628090e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.185460e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.001770e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.532480e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.569190e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.333470e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.838270e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.727270e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.985230e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.508580e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.184300e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.973170e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.481820e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.481790e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.929290e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.354160e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.396550e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -9.456930e-04 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.707310e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.164550e-04 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.311070e-04 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.032160e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.257310e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.128140e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.563420e-05 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.082490e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.453950e-04 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.615950e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.370730e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.322670e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.635720e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.126740e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.141870e-04 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.732880e-04 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.451540e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.191540e-04 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.009350e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.958080e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.786750e-04 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.603560e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.222590e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.971110e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.457610e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.394620e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.048400e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.183730e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.597930e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.982410e-04 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.806300e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.621200e-04 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.457410e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.715790e-05 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.579160e-04 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.582390e-04 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.041010e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.919560e-04 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.274630e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.239250e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.196990e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.306570e-04 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.443410e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.810250e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.215290e-04 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.661010e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.216740e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.161260e-04 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.022550e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.233540e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.037340e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.935210e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.999700e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.259950e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -9.444220e-04 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -6.061900e-04 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.553290e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.205460e-06 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.060510e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.814780e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.765520e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.919410e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.218240e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.170760e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -7.508060e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.839480e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.299870e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.182990e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.989840e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.969900e-04 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d26-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d26-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t26
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.226410e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.632110e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -4.822260e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.321680e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.690260e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -9.753840e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.186940e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.174100e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.367050e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.719300e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.400490e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.237610e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.265610e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -7.640450e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.175630e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.669860e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.103280e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.290450e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.005450e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.596400e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -4.752990e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.006130e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.616840e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.568950e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.533070e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.158840e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.441580e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.242350e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.751670e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.489690e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.693730e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.909040e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.926650e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.740000e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.482950e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.824820e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d27-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d27-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t27
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.563110e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.638400e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.390700e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.324990e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.694450e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.286560e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.575040e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.065520e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.635620e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.844050e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.466930e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.087200e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.531480e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.836570e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.876410e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.275710e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.935810e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.984390e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.210570e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.374310e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.474200e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.364710e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.371810e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.731510e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.973590e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.323570e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.171930e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.857030e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.476140e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.697030e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -5.422400e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.714870e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.294840e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.066080e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.405310e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.184210e-02 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d28-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d28-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t28
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.196320e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.307900e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.638760e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.940810e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.804990e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.196320e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -4.768140e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.275030e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.900390e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.856160e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.307900e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.768140e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.953870e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.100220e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.635640e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.638760e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.275030e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -4.953870e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.832960e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -5.630720e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.940810e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.900390e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.100220e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -9.832960e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.656000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.804990e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.856160e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.635640e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.630720e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.656000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d29-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d29-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t29
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.317690e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.557230e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.263330e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.220720e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.972310e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.860250e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.824710e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.123440e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.571570e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.220490e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.588670e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.950910e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.209570e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.384260e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.186540e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.419920e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.024610e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.192220e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.172630e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.557020e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.758830e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -6.345580e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.934890e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.855250e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.429290e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.721950e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.535320e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.540930e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.124900e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.234340e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.222700e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.435090e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.638740e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.497440e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.981340e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.543100e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.165880e-01 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.683350e-01 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.742430e-01 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.791290e-02 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.156120e-02 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -9.866380e-04 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.106940e-01 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.308020e-01 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.405000e-01 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.461270e-02 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.328140e-02 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.466230e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.038610e-01 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.122210e-01 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.802260e-01 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.486990e-02 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -8.911180e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.212590e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000690e-01 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.485390e-02 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.235360e-01 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.734810e-01 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.240130e-02 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.439430e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.946790e-02 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.771270e-02 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.918170e-02 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.989960e-01 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.650030e-02 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.068160e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.454140e-02 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.486810e-02 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.549290e-02 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.670030e-01 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.195360e-02 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.760240e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.193230e-02 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.884170e-02 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.445530e-02 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.111790e-01 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.296580e-01 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.801000e-02 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.545080e-02 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.620990e-02 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.169310e-02 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.957560e-02 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.360030e-01 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.663810e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.303040e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.921180e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.772890e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.031720e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.269640e-01 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.162060e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.931710e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.620400e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.475060e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.888050e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.715390e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.846130e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.819400e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.650370e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.537560e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.425340e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.852420e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.109190e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.694450e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.730680e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.959680e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.094600e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.882940e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.656110e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d30-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d30-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t30
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.208160e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -7.590370e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.664850e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.202680e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.026950e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.130870e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.047870e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.651500e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.164980e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.686560e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.776930e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.264810e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.395950e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.363950e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.934370e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.026610e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.520790e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.036860e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.143000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.285120e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.060450e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.665670e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.705870e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.258660e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.033520e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.614880e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.037950e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.976590e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.272590e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.185060e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.987280e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.406710e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.368900e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.177540e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.137130e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.350380e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d31-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d31-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t31
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.189470e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.919920e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.707420e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.609460e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -8.723600e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.550240e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -8.345590e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.016120e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.237290e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.803490e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.270370e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.059470e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.097120e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.095320e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.142180e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.812310e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.696170e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.129740e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.260000e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.341060e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.919570e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.320240e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.741560e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.673330e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.826900e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.010030e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.519070e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.106810e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.200060e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.071470e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.291690e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.207360e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.899980e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.319750e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.394710e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.892860e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d32-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d32-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t32
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.168410e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.453140e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -7.842610e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.235880e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.928190e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.492910e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.744360e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.870020e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.863650e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.596350e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.441630e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.882310e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.877140e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.374760e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.453020e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -6.343620e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.200600e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.143880e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -7.811370e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.448470e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.191410e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.107240e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.233970e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.716330e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -5.381250e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.443160e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.489050e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.763100e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.284090e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.002890e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.047600e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.657620e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.217180e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.412630e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.987400e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.681880e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.004590e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.056330e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.940650e-04 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.534530e-06 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.021710e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.860730e-04 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.329460e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.572510e-04 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.982680e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.035990e-04 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.617360e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.447070e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.121870e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.412790e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.477250e-04 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.692270e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.792590e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.899880e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.841690e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.065970e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.092120e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.295270e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.962130e-05 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.914750e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.366030e-04 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.447680e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.439850e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.848110e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.078860e-04 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.288410e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.262100e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.850410e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.746460e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.255520e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.702110e-04 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.691430e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.732960e-04 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.522780e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.817210e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.758880e-04 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.804930e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.786480e-04 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.312350e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.308710e-04 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.898130e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.507120e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.242870e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.830860e-04 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.349220e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -6.983620e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.658360e-04 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.752540e-04 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.106880e-04 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.595910e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.161950e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.518080e-04 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.621010e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.090240e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.523010e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -8.557630e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.317440e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.366540e-04 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.627750e-05 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.238650e-04 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.034860e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.734080e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -9.778980e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.559520e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.725550e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.402810e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.265230e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -5.897790e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d33-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d33-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t33
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.283100e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.270040e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.437380e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.316760e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.458080e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.507360e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.024130e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -6.735300e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.441920e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.129820e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.046900e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.373950e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.809230e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -8.130180e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.119430e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.154130e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.797310e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.992280e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.857010e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.840340e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -4.391560e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.628960e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.326010e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.253920e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.336130e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.478900e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.672540e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.134040e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.109890e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.724920e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.844670e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.400260e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.925170e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.626330e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.105400e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.114780e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d34-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d34-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t34
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.728920e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.107290e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.317300e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.101520e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.197090e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.352850e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -9.774850e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.885270e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.882070e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.689670e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.564830e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.353950e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -7.840390e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.845800e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.832410e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.196230e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -8.326860e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.090150e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.396460e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -9.254750e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.872270e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.399210e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.619880e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.507530e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.408480e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.248100e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.401910e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.072510e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.747750e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.296490e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.214160e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.136630e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.382980e-02 0.000000e+00 0.000000e+00
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+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.825440e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d35-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d35-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t35
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.356920e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.671230e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.132370e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.319750e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -2.641770e-03 0.000000e+00 0.000000e+00
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d36-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d36-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t36
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d37-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d37-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t37
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d38-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d38-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t38
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d39-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d39-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t39
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d40-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d40-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t40
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+5.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 9.424650e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 7.042210e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 3.976190e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.088070e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.218590e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.610040e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.428570e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -9.283850e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.327640e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.092860e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -9.725890e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 3.317750e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -2.546340e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 -4.793890e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 -2.343050e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 1.115880e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 -1.315030e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 -3.235550e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 5.091760e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 1.443440e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 1.654560e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.292700e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d41-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d41-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t41
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.213810e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.667320e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.158030e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.878340e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.179450e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.213810e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.367610e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.941360e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.234180e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.509140e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.667320e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.367610e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.161120e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.839710e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.544030e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.158030e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.941360e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.161120e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.654070e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -7.218150e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.878340e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.234180e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.839710e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -9.654070e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.562910e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.179450e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.509140e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.544030e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.218150e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.562910e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d42-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d42-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t42
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.253980e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.585370e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.967690e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.480010e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.071270e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.697180e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -7.168260e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.730320e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.857080e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.020060e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.609980e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.347450e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -9.714380e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.182430e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.820350e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.423890e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.578170e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.843740e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -9.217640e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.448400e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -9.202130e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.225330e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.068930e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.461690e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.284890e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.536540e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.431490e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.694280e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.593000e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.890530e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.082340e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.260360e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.333890e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.144330e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.247610e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.044500e-05 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d43-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d43-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t43
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.990130e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.075020e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.015650e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.595250e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.662120e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.216120e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.636140e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.100360e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -9.466890e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.148290e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.432620e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.846110e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.906230e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.727860e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.610340e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.635050e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.136850e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.811390e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.854920e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.600050e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.911000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.893200e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.739380e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.436090e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.448320e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.644370e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.746630e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.923330e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.418150e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.321210e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.377050e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.408340e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.246940e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.844510e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.263570e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.223710e-04 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.955110e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.270620e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.423120e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.980280e-04 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.342870e-03 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.501410e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.875730e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.175860e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.862280e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.281990e-04 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.517940e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.771490e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.089900e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.599480e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.195750e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.723560e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.439820e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -8.442680e-04 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.604940e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.670200e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.159040e-04 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.443100e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.538990e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.160440e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.140970e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.833750e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.511380e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.380540e-03 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.169560e-04 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.039080e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.710040e-04 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.238250e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.340200e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.820310e-04 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.272000e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.074400e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -7.789590e-04 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.264840e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.250810e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.190960e-04 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.705420e-04 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.963100e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.764550e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.029470e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.967330e-04 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.033040e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.679900e-03 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.729920e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.614800e-05 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -6.042930e-04 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.161980e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.289530e-04 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.962920e-03 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.187000e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.024550e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.695000e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.826210e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.162360e-03 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.916180e-04 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.082790e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.030450e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.380670e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.237970e-04 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.063660e-04 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.835080e-03 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.070550e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.695010e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.187440e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.353780e-04 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.974510e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.940680e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.504830e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d44-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d44-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t44
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.242830e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.982270e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.643230e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.098500e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.251520e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.873280e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -5.804830e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.588060e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.886360e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.755260e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.353300e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.527910e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -9.111030e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.952040e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.189020e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.287930e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.438260e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.809520e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.475270e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.029490e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.908770e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.282040e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.093580e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.959570e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.445880e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.463320e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.368700e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.656690e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.358490e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.265620e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -5.183320e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.414610e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -4.413440e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.917980e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.382310e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.334190e-03 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d45-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d45-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t45
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.577160e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.373870e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.746280e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.994410e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.064000e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.102860e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.267760e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.706100e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.065020e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.981860e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.888360e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.866600e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.095700e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.068090e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.201550e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.544370e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.814090e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.720420e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.606200e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.585500e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.299820e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.059240e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.500630e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.027760e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.092430e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.041070e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.757480e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.674740e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.774080e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.656750e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.051680e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.666800e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.149860e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.050350e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.072120e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.647230e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d46-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d46-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t46
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.289500e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.339950e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.872340e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.903990e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -7.308110e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.289500e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.468360e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.261120e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.564420e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.439280e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.339950e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.468360e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.295980e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.228670e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.246930e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.872340e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.261120e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.295980e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.297720e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.499120e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.903990e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.564420e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.228670e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.297720e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.577940e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -7.308110e-05 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.439280e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.246930e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -6.499120e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.577940e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d47-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d47-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t47
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.158630e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.571970e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.950690e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -8.343610e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.360450e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.800020e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.501510e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.333760e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.634510e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.759600e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.100500e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.770040e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.810260e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.211790e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.692970e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.760680e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.620880e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.213620e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.124690e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.277600e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.691000e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -9.648370e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.755420e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.381680e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.759490e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.177920e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.376950e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.681450e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.282090e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.864590e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.701580e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.039020e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.223770e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -9.797990e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.426440e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.050950e-04 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.685670e-01 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.430270e-01 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.397020e-01 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.657940e-02 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.308080e-02 0.000000e+00 0.000000e+00
+7.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.071920e-03 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.560530e-01 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.186410e-01 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.792380e-01 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.362370e-02 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.180340e-02 0.000000e+00 0.000000e+00
+8.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.835020e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.395980e-01 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.196320e-01 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.265990e-01 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.931940e-02 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.813960e-03 0.000000e+00 0.000000e+00
+9.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.966520e-03 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.367160e-01 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.178360e-01 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.992050e-02 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.286870e-01 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.067350e-02 0.000000e+00 0.000000e+00
+1.000000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.576640e-04 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.316620e-01 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.481150e-02 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.422780e-02 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.528970e-01 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.031130e-02 0.000000e+00 0.000000e+00
+1.100000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.796100e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.266730e-01 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.872320e-02 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.891530e-02 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.234780e-01 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.692160e-03 0.000000e+00 0.000000e+00
+1.200000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.376080e-03 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.004020e-01 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.868190e-02 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.059090e-02 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.470900e-02 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.928430e-02 0.000000e+00 0.000000e+00
+1.300000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.618090e-02 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.418790e-02 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.957280e-02 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.703670e-02 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.291190e-02 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.712150e-01 0.000000e+00 0.000000e+00
+1.400000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.114320e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.266110e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.975540e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.063740e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.456820e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.669900e-02 0.000000e+00 0.000000e+00
+1.500000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.583360e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.741430e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.120590e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.845140e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.289920e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.478240e-02 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.868870e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.866020e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.887120e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.193610e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.337980e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.678480e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.586910e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.054970e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.706820e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.713050e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.232110e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.120000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.574150e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d48-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d48-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t48
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.353230e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -8.708600e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.254500e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.445740e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.337740e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.500830e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.664570e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.224140e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.674220e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.313560e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.593270e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.867170e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.418330e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.212230e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.438030e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.018500e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.608080e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.380240e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.048750e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.009270e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.236870e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.074810e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.350620e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.014530e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.560260e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.486960e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.011730e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.039220e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.371150e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.564160e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.262930e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.885100e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.762640e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.249980e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.054980e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.655290e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d49-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d49-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t49
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.021880e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.268310e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.493540e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.006730e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.358800e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.504980e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.276010e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.531040e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.757650e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.638430e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.533350e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.892820e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -8.460680e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.385080e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.414530e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.008140e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.995270e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.326920e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.544500e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -8.184490e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -7.746320e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.162620e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.839790e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.628900e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.689340e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.026500e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.406530e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.552280e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.052190e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -9.298030e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.459960e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.830660e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.703420e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.035720e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.007940e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.043900e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d50-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d50-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t50
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.728580e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.458080e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.419370e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.151360e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.259240e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -9.681960e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -7.679180e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -4.059100e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 -2.559640e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 5.810930e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 2.547690e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 -2.559790e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 -3.498990e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 -6.962320e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 -4.671770e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 -1.474170e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.146180e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.728580e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.051550e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.526390e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.451980e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.269730e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.657470e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 5.020270e-03 0.000000e+00 0.000000e+00
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+1.800000e+01 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d51-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d51-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t51
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+6.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 9.801440e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.067580e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d52-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d52-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t52
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.993230e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.259270e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.402840e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.019480e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.523200e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.253510e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 8.354210e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 7.585610e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 7.121720e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 6.578500e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 6.439670e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 6.323900e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 4.896830e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 4.643650e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 4.179600e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 3.484660e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 2.665890e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.124470e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -5.103100e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.074040e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.654880e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.742100e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.498080e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.417590e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 1.018910e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 8.455650e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 8.648120e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 8.959700e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 7.002020e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 5.427490e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 6.026760e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 5.336400e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 3.904340e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 4.492650e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 3.603000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.388000e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.489840e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -9.358660e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.511700e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.236760e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.116490e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.435550e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.457440e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 1.164650e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 8.625520e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 5.945520e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 5.902240e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 5.257680e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 5.059570e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 4.063880e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 2.840720e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 3.552650e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 3.402510e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.114940e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.507490e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.211270e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.450070e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -8.236900e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.135460e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -8.088320e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -1.116380e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -8.278030e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 3.880640e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 8.017190e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 9.806700e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 7.716620e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 4.855310e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 3.244120e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 2.909230e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 3.450000e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 2.038710e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.130090e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.731870e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.687360e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.256590e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.567950e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.725930e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.266620e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -6.230550e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -8.306860e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -4.634790e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 -6.554360e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 -1.339590e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 -3.984940e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 4.405020e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 1.046820e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 5.157240e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 4.064670e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 2.203850e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.901170e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.207060e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.988100e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.882970e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.848530e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.562040e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.943110e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 1.559220e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -1.436330e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 3.516110e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 4.448480e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 2.391110e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 3.388780e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 -8.461120e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 -1.326160e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 4.351310e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 5.343450e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 9.776820e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 9.086890e-02 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d53-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d53-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t53
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.120230e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.556190e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.147230e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.449470e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.432940e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.120230e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.027600e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.674220e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.192170e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.198610e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.556190e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -6.027600e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.905300e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.554050e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.527170e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.147230e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.674220e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.905300e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.439000e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -7.206350e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.449470e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.192170e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.554050e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.439000e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.632500e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.432940e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.198610e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.527170e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.206350e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.632500e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d54-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d54-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t54
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.669220e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.308110e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.342990e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.739330e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.670230e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.872710e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.459280e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.226410e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.194940e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.848070e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.794080e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.026690e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -5.335630e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.083700e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.321230e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.480440e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.220750e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.653850e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.752030e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.991550e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.847260e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.929010e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.250660e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.553290e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.327960e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.196240e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.352060e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.449070e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.370140e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.243040e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.535010e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.020290e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.971650e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.522340e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.766420e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.198070e-01 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d55-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d55-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t55
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.844390e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.205960e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.866620e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.653140e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.239310e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.844390e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.054850e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.267690e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.668720e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.161640e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.205960e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.054850e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.776490e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.181270e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.464190e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.866620e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.267690e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.776490e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -7.980940e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.083750e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.653140e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.668720e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.181270e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.980940e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.596770e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.239310e-04 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.161640e-03 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.464190e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -6.083750e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.596770e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d56-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d56-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t56
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.071000e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.634000e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.795000e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.367000e-05 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.167000e-06 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.142000e-07 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.634000e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.487000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.164000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.756000e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.982000e-06 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.938000e-07 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.795000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.164000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.409000e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.619000e-06 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.763000e-07 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.835000e-08 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.367000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.756000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.619000e-06 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.073000e-06 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.668000e-07 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.924000e-08 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.167000e-06 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.982000e-06 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.763000e-07 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.668000e-07 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.272000e-08 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.553000e-09 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.142000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.938000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.835000e-08 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.924000e-08 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.553000e-09 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.452000e-10 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d57-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d57-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t57
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.862000e-07 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.330000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.536000e-09 0.000000e+00 0.000000e+00
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+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.014000e-14 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d58-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d58-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t58
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d59-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d59-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t59
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+1.800000e+01 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 3.987000e-11 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 3.480000e-11 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 3.008000e-11 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 1.157000e-11 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.963000e-12 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d60-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d60-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t60
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.257000e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.296000e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.536000e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.627000e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.261000e-05 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.871000e-06 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.296000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.504000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.166000e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.538000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.063000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.869000e-06 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.536000e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.166000e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.931000e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.268000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.409000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.372000e-06 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.627000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.538000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.268000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.224000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.736000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.056000e-06 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.261000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.063000e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.409000e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.736000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.628000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.519000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.871000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.869000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.372000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.056000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.519000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.075000e-08 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d61-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d61-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t61
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.239000e-06 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.468000e-06 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.579000e-07 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.632000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.123000e-09 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.384000e-10 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.468000e-06 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.953000e-06 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.978000e-07 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.553000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.116000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.431000e-11 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.579000e-07 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.978000e-07 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.205000e-07 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.208000e-07 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.535000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.461000e-10 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.632000e-08 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.553000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.208000e-07 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.412000e-08 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.253000e-08 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.295000e-10 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.123000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.116000e-08 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.535000e-08 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.253000e-08 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.397000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.407000e-11 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.384000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.431000e-11 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.461000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.295000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.407000e-11 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.751000e-12 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d62-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d62-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t62
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.128000e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.409000e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.321000e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.403000e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.449000e-05 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.553000e-06 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.409000e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.495000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.273000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.620000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.690000e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.900000e-06 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.321000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.273000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.104000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.653000e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.691000e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.132000e-06 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.403000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.620000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.653000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.052000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.031000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.660000e-07 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.449000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.690000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.691000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.031000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.356000e-06 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.813000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.553000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.900000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.132000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.660000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.813000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.744000e-08 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d63-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d63-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t63
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.246000e-07 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.514000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.653000e-09 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.003000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.293000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.369000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.514000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.102000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.617000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.064000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.388000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.649000e-11 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.653000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.617000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.968000e-08 0.000000e+00 0.000000e+00
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+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.189000e-11 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d64-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d64-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t64
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.282000e-05 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.126000e-05 0.000000e+00 0.000000e+00
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d65-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d65-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t65
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d66-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d66-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t66
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.506000e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.025000e-05 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.546000e-06 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.398000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.867000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.740000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.644000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.950000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.855000e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.353000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.740000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.711000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.638000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.944000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.854000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.506000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.644000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.638000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.446000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.300000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.224000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.025000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.950000e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.944000e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.300000e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.171000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.617000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.546000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.855000e-05 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.854000e-05 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.224000e-05 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.617000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.803000e-07 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d67-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d67-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t67
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.367000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.700000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.683000e-09 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.576000e-09 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.911000e-10 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.088000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.700000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.077000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.062000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.016000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.020000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.031000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.683000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.062000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.994000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.060000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -8.020000e-10 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.545000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.576000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.016000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.060000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.650000e-08 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.285000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.378000e-10 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.911000e-10 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.020000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.020000e-10 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.285000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.320000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.093000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.088000e-09 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.031000e-09 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.545000e-09 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.378000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.093000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.016000e-10 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d68-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d68-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t68
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.718000e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.273000e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.398000e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.777000e-05 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.865000e-05 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.899000e-07 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.273000e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.290000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.745000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.651000e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.012000e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.507000e-07 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.398000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.745000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.864000e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.525000e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.271000e-06 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.602000e-07 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.777000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.651000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.525000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.414000e-06 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.910000e-06 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.827000e-07 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.865000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.012000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.271000e-06 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.910000e-06 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.050000e-06 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.449000e-08 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.899000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.507000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.602000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.827000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.449000e-08 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.368000e-08 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d69-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d69-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t69
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.112000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.411000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -3.162000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.471000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.786000e-09 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -7.380000e-10 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.411000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.142000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.451000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.790000e-10 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.729000e-10 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.345000e-11 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.162000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.451000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.779000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.406000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.934000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.133000e-10 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.471000e-08 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.790000e-10 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.406000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.891000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.747000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.887000e-10 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.786000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.729000e-10 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.934000e-09 0.000000e+00 0.000000e+00
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+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.738000e-11 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d70-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d70-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t70
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d71-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d71-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t71
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d72-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d72-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t72
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.681000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.431000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.554000e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.576000e-06 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.365000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.397000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.431000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.256000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.363000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.603000e-06 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.029000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.072000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.554000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.363000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.193000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.163000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.641000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.162000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.576000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.603000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.163000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.787000e-08 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d73-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d73-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t73
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.673000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.843000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.653000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.896000e-09 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.303000e-09 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.186000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.843000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.255000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.604000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.301000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.581000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.605000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.653000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.604000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.989000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.078000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.401000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.922000e-10 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.896000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.301000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.078000e-08 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.938000e-08 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.980000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.274000e-10 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.303000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -6.581000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.401000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.980000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.002000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.402000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.186000e-09 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.605000e-09 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.922000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.274000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.402000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.010000e-10 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d74-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d74-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t74
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.953000e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.182000e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.735000e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.204000e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.664000e-04 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.758000e-05 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.182000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.650000e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.238000e-03 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.519000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.919000e-04 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.504000e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.735000e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.238000e-03 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.865000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.275000e-04 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.765000e-05 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.055000e-06 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.204000e-03 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.519000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.275000e-04 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.370000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.198000e-05 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.851000e-06 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.664000e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.919000e-04 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.765000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.198000e-05 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.194000e-06 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.945000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.758000e-05 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.504000e-05 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.055000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.851000e-06 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.945000e-07 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.505000e-08 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d75-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d75-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t75
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.188000e-07 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.063000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.283000e-08 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.119000e-09 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.568000e-09 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.476000e-10 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.063000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.611000e-07 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.480000e-08 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.155000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.059000e-09 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.361000e-10 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.283000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.480000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.152000e-08 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.925000e-09 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.375000e-10 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.834000e-11 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -3.119000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.155000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.925000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.464000e-09 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.538000e-10 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.184000e-11 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.568000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.059000e-09 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.375000e-10 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.538000e-10 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.873000e-10 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.007000e-11 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.476000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.361000e-10 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.834000e-11 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.184000e-11 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.007000e-11 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.568000e-12 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d76-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d76-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t76
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.199000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.502000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.602000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.400000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.195000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.199000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.309000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.514000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.436000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.209000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.502000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.309000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.535000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.790000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.302000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.602000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.514000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.535000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.443000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.193000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.400000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.436000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.790000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.443000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.778000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.195000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.209000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.302000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.193000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.778000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d77-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d77-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t77
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.436000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.428000e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.016000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.404000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -9.886000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.436000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.337000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.513000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.284000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.089000e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.428000e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.337000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.060000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.234000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.437000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.016000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.513000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.060000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.113000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.691000e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.404000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.284000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.234000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.113000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.110000e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -9.886000e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.089000e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.437000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.691000e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.110000e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d78-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d78-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t78
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.507000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.923000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.280000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.121000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.852000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 8.033000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 7.943000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 7.727000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 7.870000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 7.683000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 7.264000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 7.238000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 7.093000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 6.772000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 6.134000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 5.780000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 5.566000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.507000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.319000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.170000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.172000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.132000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.199000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 8.944000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 8.587000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 8.412000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 8.376000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 7.982000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 7.456000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 6.931000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 6.499000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 5.521000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 4.969000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 5.202000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.923000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.319000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.619000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.328000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.410000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.275000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 8.957000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 8.703000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 8.436000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 8.267000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 8.039000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 7.579000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 7.184000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 6.553000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 5.482000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 5.135000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 5.336000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.280000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.170000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.619000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.623000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.453000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.320000e-01 0.000000e+00 0.000000e+00
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d79-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d79-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t79
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+1.600000e+01 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 5.844000e-01 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 6.598000e-01 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 6.679000e-01 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 6.758000e-01 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 6.926000e-01 0.000000e+00 0.000000e+00
+1.600000e+01 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 5.153000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.568000e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.437000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.054000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.468000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -3.742000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.531000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -3.047000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -1.646000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 6.605000e-02 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 3.525000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 4.176000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 4.060000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 5.298000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 6.588000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 6.438000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 6.926000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 5.789000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.705000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.336000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.121000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -4.475000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.451000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -9.365000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -1.239000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -8.802000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -1.873000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 2.432000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 3.279000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 2.426000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 3.848000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 3.697000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 3.935000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 5.153000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 5.789000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d80-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d80-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t80
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.426000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.178000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.169000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.384000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.470000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.426000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.275000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.575000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 2.148000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.043000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.178000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.275000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.001000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.450000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.007000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.169000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.575000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.001000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.869000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.831000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.384000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.148000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.450000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.869000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.411000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.470000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.043000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.007000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.831000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.411000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d81-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d81-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t81
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.814000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.809000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.373000e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -9.408000e-03 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.989000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.814000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.143000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.985000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.205000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.912000e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.809000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.143000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.952000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.221000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.969000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.373000e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.985000e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.952000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.944000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.082000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -9.408000e-03 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.205000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.221000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.944000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.645000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.989000e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.912000e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.969000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.082000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.645000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d82-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d82-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t82
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.914000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.445000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.430000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.775000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.221000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.914000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.560000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.518000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.847000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.541000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.445000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.560000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.550000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.889000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.597000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.430000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.518000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.550000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.940000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.167000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.775000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.847000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.889000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.940000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.966000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.221000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.541000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.597000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.167000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.966000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d83-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d83-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t83
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.959000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -6.008000e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -5.601000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.866000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.286000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.959000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.048000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.405000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.272000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.257000e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.008000e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.048000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.308000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.247000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.730000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -5.601000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.405000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.308000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.402000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.680000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.866000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.272000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.247000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.402000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.881000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.286000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.257000e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.730000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.680000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.881000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d84-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d84-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t84
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.194000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.097000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.257000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.298000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.268000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.296000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 9.278000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 9.308000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 9.249000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 8.974000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 9.044000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 8.827000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 8.975000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 8.796000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 7.598000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 8.008000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 5.979000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.194000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.672000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.668000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.536000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.646000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.630000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 9.568000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 9.552000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 9.577000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 9.184000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 9.378000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 9.247000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 9.181000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 8.704000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 7.891000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 8.308000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 6.066000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.097000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.672000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.818000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.578000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.716000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.716000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 9.663000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 9.652000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 9.667000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 9.269000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 9.419000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 9.388000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 9.326000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 8.863000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 8.019000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 8.292000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 5.954000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.257000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.668000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.818000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.722000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.767000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.771000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 9.753000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 9.742000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 9.746000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 9.334000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 9.522000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 9.462000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 9.375000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 8.918000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 7.999000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 8.409000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 6.009000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.298000e-01 0.000000e+00 0.000000e+00
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d85-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d85-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t85
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+1.700000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -5.451000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -3.810000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -4.864000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -3.304000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 2.683000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 3.076000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 2.474000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 3.272000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 4.872000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 4.073000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 4.888000e-01 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.700000e+01 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 4.129000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.227000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.358000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -1.320000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -9.150000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.691000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -2.362000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -2.257000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -1.280000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 2.464000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 2.436000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 4.842000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 3.717000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 4.906000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 4.645000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 5.582000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 6.390000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 4.129000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d86-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d86-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t86
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.871000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.816000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.599000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.449000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.121000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.871000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.917000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.620000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.506000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.286000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.816000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.917000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.732000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.604000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.406000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.599000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.620000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.732000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.819000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.485000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.449000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.506000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.604000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.819000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.474000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.121000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.286000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.406000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.485000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.474000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d87-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d87-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t87
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.452000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.654000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.381000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -4.351000e-02 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.644000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.452000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.483000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -3.512000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.848000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.711000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.654000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.483000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.687000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -5.884000e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -5.462000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.381000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.512000e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.687000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.068000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.312000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.351000e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.848000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.884000e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.068000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.183000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.644000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -6.711000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -5.462000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.312000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.183000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d88-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d88-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t88
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.735000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.511000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.183000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.491000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.623000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.735000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.088000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.812000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.938000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.218000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.511000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.088000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.316000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.169000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 2.905000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 6.183000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.812000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.316000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.846000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.735000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.491000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.938000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.169000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.846000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.382000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.623000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.218000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.905000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.735000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.382000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d89-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d89-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t89
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -4.636000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -8.324000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -7.383000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.416000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -6.215000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.636000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.422000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -2.395000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -6.877000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -3.018000e-02 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -8.324000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.422000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.723000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.903000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.836000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -7.383000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.395000e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.723000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.726000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.470000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.416000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -6.877000e-02 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.903000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.726000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.094000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -6.215000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -3.018000e-02 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.836000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.470000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.094000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d90-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d90-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t90
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.421000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.271000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.563000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.465000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 8.294000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 8.286000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 8.228000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 8.188000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 8.097000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 7.968000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 7.826000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 7.352000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 7.319000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 6.552000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 6.328000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 5.211000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 2.852000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.421000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.077000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.155000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.122000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.325000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.307000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 9.001000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 9.051000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 8.650000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 8.827000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 8.619000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 8.123000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 8.551000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 7.635000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 6.907000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 6.190000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 4.052000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.271000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.077000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.610000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.532000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.395000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.401000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 9.381000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 9.273000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 9.339000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 9.129000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 9.003000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 8.759000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 8.062000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 7.428000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 7.251000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 5.844000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 3.133000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.563000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.155000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.610000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 9.701000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.408000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.510000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 9.423000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 9.360000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 9.268000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 9.213000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 9.099000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 8.708000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 8.422000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 7.759000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 7.268000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 6.327000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 3.825000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.465000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.122000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.532000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.701000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 9.623000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 9.512000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 9.465000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 9.402000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 9.398000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 9.248000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 9.147000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 8.843000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 8.333000e-01 0.000000e+00 0.000000e+00
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+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d91-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d91-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t91
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
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+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.027000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.237000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -9.191000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.082000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.905000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -1.792000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 -3.697000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 -3.384000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 -4.256000e-02 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 5.020000e-03 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 2.031000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 2.289000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 2.975000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.400000e+01 0.000000e+00 0.000000e+00 4.459000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.500000e+01 0.000000e+00 0.000000e+00 5.550000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 5.927000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 6.690000e-01 0.000000e+00 0.000000e+00
+1.800000e+01 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d92-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d92-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t92
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.620000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.001000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.424000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.106000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.121000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.620000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.249000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.304000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.195000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.520000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 9.001000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.249000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.430000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.380000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.957000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.424000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.304000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.430000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.650000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.478000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.106000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 7.195000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.380000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.650000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.554000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.121000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 4.520000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 5.957000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.478000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.554000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d93-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d93-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t93
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.088000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.510000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 2.170000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -1.009000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -4.008000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.088000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 2.796000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -8.253000e-02 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 -2.957000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 -5.560000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 4.510000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 2.796000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.476000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 4.137000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.456000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 2.170000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -8.253000e-02 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.476000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.472000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 4.485000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.009000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -2.957000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 4.137000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.472000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.940000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -4.008000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -5.560000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.456000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 4.485000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 6.940000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d94-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d94-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t94
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.434000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 7.751000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.160000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.449000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.499000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.434000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.788000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.312000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.223000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.326000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.751000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.788000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 9.451000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.427000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 6.180000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 8.160000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.312000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.451000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 8.944000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.393000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.449000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 8.223000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 8.427000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 8.944000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 7.122000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 7.499000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 6.326000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.180000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 7.393000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 7.122000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER3D_V2 /REF/ATLAS_2018_I1656578/d95-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d95-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t95
+Type: Scatter3D
+---
+# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+
+1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 -1.793000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 -2.756000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 -1.444000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.729000e-01 0.000000e+00 0.000000e+00
+1.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.367000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.793000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 9.306000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.310000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.026000e-01 0.000000e+00 0.000000e+00
+2.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.586000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -2.756000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 9.306000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 6.993000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 3.771000e-01 0.000000e+00 0.000000e+00
+3.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.861000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 -1.444000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 5.310000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 6.993000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.455000e-01 0.000000e+00 0.000000e+00
+4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 3.894000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 3.729000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 3.026000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 3.771000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 5.455000e-01 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+5.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 5.539000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 5.367000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 1.586000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 1.861000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 3.894000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 5.539000e-01 0.000000e+00 0.000000e+00
+6.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00
+END YODA_SCATTER3D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d96-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d96-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 1.091328e+00 1.110602e-01 1.050563e-01
+6.000000e+01 2.000000e+01 2.000000e+01 1.563556e-01 2.549203e-02 2.599126e-02
+1.000000e+02 2.000000e+01 2.000000e+01 2.281198e-02 5.003797e-03 4.945086e-03
+1.450000e+02 2.500000e+01 2.500000e+01 5.145449e-03 1.503565e-03 1.403014e-03
+2.000000e+02 3.000000e+01 3.000000e+01 9.830373e-04 2.714148e-04 2.852302e-04
+4.150000e+02 1.850000e+02 1.850000e+02 2.351663e-05 1.808958e-05 1.680552e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d96-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d96-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t96
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 1.091328e+00 1.110878e-01 1.050758e-01
+6.000000e+01 2.000000e+01 2.000000e+01 1.563556e-01 2.550510e-02 2.600335e-02
+1.000000e+02 2.000000e+01 2.000000e+01 2.281198e-02 5.013441e-03 4.954889e-03
+1.450000e+02 2.500000e+01 2.500000e+01 5.145449e-03 1.509704e-03 1.409591e-03
+2.000000e+02 3.000000e+01 3.000000e+01 9.830373e-04 2.767245e-04 2.902905e-04
+4.150000e+02 1.850000e+02 1.850000e+02 2.351663e-05 1.821357e-05 1.693896e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d97-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d97-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 2.133801e-02 7.162603e-04 6.806397e-04
+6.000000e+01 2.000000e+01 2.000000e+01 3.057117e-03 3.919334e-04 4.326992e-04
+1.000000e+02 2.000000e+01 2.000000e+01 4.460274e-04 8.830170e-05 9.099357e-05
+1.450000e+02 2.500000e+01 2.500000e+01 1.006055e-04 2.613795e-05 2.520694e-05
+2.000000e+02 3.000000e+01 3.000000e+01 1.922068e-05 5.212339e-06 5.504734e-06
+4.150000e+02 1.850000e+02 1.850000e+02 4.598051e-07 3.458052e-07 3.183623e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d97-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d97-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t97
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 2.133801e-02 7.166439e-04 6.808812e-04
+6.000000e+01 2.000000e+01 2.000000e+01 3.057117e-03 3.922313e-04 4.329860e-04
+1.000000e+02 2.000000e+01 2.000000e+01 4.460274e-04 8.850642e-05 9.119214e-05
+1.450000e+02 2.500000e+01 2.500000e+01 1.006055e-04 2.627241e-05 2.534640e-05
+2.000000e+02 3.000000e+01 3.000000e+01 1.922068e-05 5.318106e-06 5.604968e-06
+4.150000e+02 1.850000e+02 1.850000e+02 4.598051e-07 3.482830e-07 3.210529e-07
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d98-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d98-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 4.063329e-02 6.583950e-03 5.965852e-03
+2.250000e+01 7.500000e+00 7.500000e+00 1.190516e-01 1.545399e-02 1.517502e-02
+3.750000e+01 7.500000e+00 7.500000e+00 1.995954e-01 2.546613e-02 2.507118e-02
+5.250000e+01 7.500000e+00 7.500000e+00 2.623467e-01 3.256684e-02 3.076766e-02
+6.750000e+01 7.500000e+00 7.500000e+00 3.101524e-01 3.711885e-02 3.487645e-02
+8.250000e+01 7.500000e+00 7.500000e+00 3.289564e-01 3.709059e-02 3.493560e-02
+9.750000e+01 7.500000e+00 7.500000e+00 3.477461e-01 3.583188e-02 3.515008e-02
+1.125000e+02 7.500000e+00 7.500000e+00 3.306449e-01 3.225773e-02 2.986823e-02
+1.275000e+02 7.500000e+00 7.500000e+00 2.821092e-01 2.737116e-02 2.475994e-02
+1.425000e+02 7.500000e+00 7.500000e+00 2.311646e-01 2.231715e-02 2.148982e-02
+1.575000e+02 7.500000e+00 7.500000e+00 1.892674e-01 1.630916e-02 1.711005e-02
+1.725000e+02 7.500000e+00 7.500000e+00 1.518968e-01 1.304693e-02 1.193984e-02
+1.900000e+02 1.000000e+01 1.000000e+01 1.147653e-01 1.170434e-02 9.479514e-03
+2.150000e+02 1.500000e+01 1.500000e+01 7.987874e-02 7.884744e-03 7.185652e-03
+2.475000e+02 1.750000e+01 1.750000e+01 4.873722e-02 4.927492e-03 4.794517e-03
+2.950000e+02 3.000000e+01 3.000000e+01 2.810237e-02 3.097677e-03 2.849676e-03
+3.875000e+02 6.250000e+01 6.250000e+01 7.241062e-03 9.640391e-04 8.997010e-04
+7.250000e+02 2.750000e+02 2.750000e+02 4.127725e-04 8.843982e-05 8.170131e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d98-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d98-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t98
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 4.063329e-02 6.724485e-03 6.120823e-03
+2.250000e+01 7.500000e+00 7.500000e+00 1.190516e-01 1.554748e-02 1.527047e-02
+3.750000e+01 7.500000e+00 7.500000e+00 1.995954e-01 2.554966e-02 2.515653e-02
+5.250000e+01 7.500000e+00 7.500000e+00 2.623467e-01 3.264622e-02 3.085243e-02
+6.750000e+01 7.500000e+00 7.500000e+00 3.101524e-01 3.718246e-02 3.494480e-02
+8.250000e+01 7.500000e+00 7.500000e+00 3.289564e-01 3.716012e-02 3.500959e-02
+9.750000e+01 7.500000e+00 7.500000e+00 3.477461e-01 3.587600e-02 3.519294e-02
+1.125000e+02 7.500000e+00 7.500000e+00 3.306449e-01 3.231539e-02 2.993036e-02
+1.275000e+02 7.500000e+00 7.500000e+00 2.821092e-01 2.741353e-02 2.480672e-02
+1.425000e+02 7.500000e+00 7.500000e+00 2.311646e-01 2.235209e-02 2.152669e-02
+1.575000e+02 7.500000e+00 7.500000e+00 1.892674e-01 1.634982e-02 1.714914e-02
+1.725000e+02 7.500000e+00 7.500000e+00 1.518968e-01 1.308892e-02 1.198671e-02
+1.900000e+02 1.000000e+01 1.000000e+01 1.147653e-01 1.173709e-02 9.520633e-03
+2.150000e+02 1.500000e+01 1.500000e+01 7.987874e-02 7.908575e-03 7.211899e-03
+2.475000e+02 1.750000e+01 1.750000e+01 4.873722e-02 4.944770e-03 4.812085e-03
+2.950000e+02 3.000000e+01 3.000000e+01 2.810237e-02 3.111264e-03 2.864541e-03
+3.875000e+02 6.250000e+01 6.250000e+01 7.241062e-03 9.682080e-04 9.042097e-04
+7.250000e+02 2.750000e+02 2.750000e+02 4.127725e-04 8.886071e-05 8.215921e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d99-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d99-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 7.948727e-04 7.388738e-05 6.900388e-05
+2.250000e+01 7.500000e+00 7.500000e+00 2.328900e-03 1.478751e-04 1.487628e-04
+3.750000e+01 7.500000e+00 7.500000e+00 3.904507e-03 2.177550e-04 2.142829e-04
+5.250000e+01 7.500000e+00 7.500000e+00 5.132053e-03 2.394171e-04 2.279987e-04
+6.750000e+01 7.500000e+00 7.500000e+00 6.067234e-03 2.625875e-04 2.358358e-04
+8.250000e+01 7.500000e+00 7.500000e+00 6.435080e-03 2.234849e-04 2.241185e-04
+9.750000e+01 7.500000e+00 7.500000e+00 6.802645e-03 1.993196e-04 2.441485e-04
+1.125000e+02 7.500000e+00 7.500000e+00 6.468110e-03 1.904835e-04 1.954177e-04
+1.275000e+02 7.500000e+00 7.500000e+00 5.518650e-03 1.655340e-04 1.612993e-04
+1.425000e+02 7.500000e+00 7.500000e+00 4.522066e-03 1.660249e-04 1.765453e-04
+1.575000e+02 7.500000e+00 7.500000e+00 3.702469e-03 1.475899e-04 1.701554e-04
+1.725000e+02 7.500000e+00 7.500000e+00 2.971422e-03 1.206260e-04 1.201439e-04
+1.900000e+02 1.000000e+01 1.000000e+01 2.245051e-03 1.139575e-04 1.011800e-04
+2.150000e+02 1.500000e+01 1.500000e+01 1.562596e-03 7.954267e-05 8.067212e-05
+2.475000e+02 1.750000e+01 1.750000e+01 9.534025e-04 5.813520e-05 6.759920e-05
+2.950000e+02 3.000000e+01 3.000000e+01 5.497414e-04 4.318697e-05 3.970431e-05
+3.875000e+02 6.250000e+01 6.250000e+01 1.416504e-04 1.394851e-05 1.376161e-05
+7.250000e+02 2.750000e+02 2.750000e+02 8.074700e-06 1.368652e-06 1.282695e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d99-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d99-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t99
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 7.948727e-04 7.852681e-05 7.394405e-05
+2.250000e+01 7.500000e+00 7.500000e+00 2.328900e-03 1.514216e-04 1.522748e-04
+3.750000e+01 7.500000e+00 7.500000e+00 3.904507e-03 2.212458e-04 2.178366e-04
+5.250000e+01 7.500000e+00 7.500000e+00 5.132053e-03 2.433528e-04 2.320970e-04
+6.750000e+01 7.500000e+00 7.500000e+00 6.067234e-03 2.656286e-04 2.391723e-04
+8.250000e+01 7.500000e+00 7.500000e+00 6.435080e-03 2.274358e-04 2.280711e-04
+9.750000e+01 7.500000e+00 7.500000e+00 6.802645e-03 2.021124e-04 2.464296e-04
+1.125000e+02 7.500000e+00 7.500000e+00 6.468110e-03 1.938556e-04 1.987392e-04
+1.275000e+02 7.500000e+00 7.500000e+00 5.518650e-03 1.680612e-04 1.639006e-04
+1.425000e+02 7.500000e+00 7.500000e+00 4.522066e-03 1.677666e-04 1.781999e-04
+1.575000e+02 7.500000e+00 7.500000e+00 3.702469e-03 1.492835e-04 1.716269e-04
+1.725000e+02 7.500000e+00 7.500000e+00 2.971422e-03 1.223542e-04 1.218797e-04
+1.900000e+02 1.000000e+01 1.000000e+01 2.245051e-03 1.152118e-04 1.025783e-04
+2.150000e+02 1.500000e+01 1.500000e+01 1.562596e-03 8.044308e-05 8.156350e-05
+2.475000e+02 1.750000e+01 1.750000e+01 9.534025e-04 5.867831e-05 6.806646e-05
+2.950000e+02 3.000000e+01 3.000000e+01 5.497414e-04 4.355496e-05 4.010563e-05
+3.875000e+02 6.250000e+01 6.250000e+01 1.416504e-04 1.405802e-05 1.387299e-05
+7.250000e+02 2.750000e+02 2.750000e+02 8.074700e-06 1.379131e-06 1.293776e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d100-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d100-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 6.578824e-01 1.164647e-01 1.112831e-01
+2.500000e+01 1.000000e+01 1.000000e+01 1.028300e+00 1.307006e-01 1.239529e-01
+5.500000e+01 2.000000e+01 2.000000e+01 4.000902e-01 5.652409e-02 5.339248e-02
+1.000000e+02 2.500000e+01 2.500000e+01 6.732053e-02 1.436307e-02 1.511037e-02
+1.475000e+02 2.250000e+01 2.250000e+01 1.945086e-02 4.135056e-03 4.092889e-03
+4.850000e+02 3.150000e+02 3.150000e+02 6.091283e-04 1.053785e-04 9.116650e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d100-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d100-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t100
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 6.578824e-01 1.164879e-01 1.113051e-01
+2.500000e+01 1.000000e+01 1.000000e+01 1.028300e+00 1.307175e-01 1.239745e-01
+5.500000e+01 2.000000e+01 2.000000e+01 4.000902e-01 5.653952e-02 5.340877e-02
+1.000000e+02 2.500000e+01 2.500000e+01 6.732053e-02 1.437186e-02 1.511923e-02
+1.475000e+02 2.250000e+01 2.250000e+01 1.945086e-02 4.144702e-03 4.102594e-03
+4.850000e+02 3.150000e+02 3.150000e+02 6.091283e-04 1.060054e-04 9.188990e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d101-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d101-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 1.288376e-02 1.863383e-03 1.837781e-03
+2.500000e+01 1.000000e+01 1.000000e+01 2.013790e-02 1.529066e-03 1.472597e-03
+5.500000e+01 2.000000e+01 2.000000e+01 7.835241e-03 8.900209e-04 8.913287e-04
+1.000000e+02 2.500000e+01 2.500000e+01 1.318384e-03 2.501265e-04 2.786242e-04
+1.475000e+02 2.250000e+01 2.250000e+01 3.809195e-04 6.488024e-05 6.784829e-05
+4.850000e+02 3.150000e+02 3.150000e+02 1.192898e-05 1.631941e-06 1.521704e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d101-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d101-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t101
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 1.288376e-02 1.863779e-03 1.838123e-03
+2.500000e+01 1.000000e+01 1.000000e+01 2.013790e-02 1.529395e-03 1.473033e-03
+5.500000e+01 2.000000e+01 2.000000e+01 7.835241e-03 8.901919e-04 8.915205e-04
+1.000000e+02 2.500000e+01 2.500000e+01 1.318384e-03 2.503183e-04 2.787977e-04
+1.475000e+02 2.250000e+01 2.250000e+01 3.809195e-04 6.511651e-05 6.807058e-05
+4.850000e+02 3.150000e+02 3.150000e+02 1.192898e-05 1.647421e-06 1.538343e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d102-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d102-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 2.128782e-01 4.694704e-02 4.647496e-02
+6.000000e+01 2.000000e+01 2.000000e+01 1.522911e-01 3.042657e-02 3.208673e-02
+1.000000e+02 2.000000e+01 2.000000e+01 7.551200e-02 1.490604e-02 1.436841e-02
+1.450000e+02 2.500000e+01 2.500000e+01 3.335587e-02 5.582527e-03 5.561654e-03
+2.000000e+02 3.000000e+01 3.000000e+01 1.482179e-02 2.264330e-03 2.016745e-03
+4.150000e+02 1.850000e+02 1.850000e+02 1.084321e-03 1.881616e-04 1.850757e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d102-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d102-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t102
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 2.128782e-01 4.695498e-02 4.648218e-02
+6.000000e+01 2.000000e+01 2.000000e+01 1.522911e-01 3.043520e-02 3.209480e-02
+1.000000e+02 2.000000e+01 2.000000e+01 7.551200e-02 1.491518e-02 1.437786e-02
+1.450000e+02 2.500000e+01 2.500000e+01 3.335587e-02 5.593023e-03 5.572158e-03
+2.000000e+02 3.000000e+01 3.000000e+01 1.482179e-02 2.275002e-03 2.028638e-03
+4.150000e+02 1.850000e+02 1.850000e+02 1.084321e-03 1.892430e-04 1.861709e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d103-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d103-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 1.034115e-02 4.095172e-04 3.593405e-04
+6.000000e+01 2.000000e+01 2.000000e+01 7.397961e-03 1.938573e-04 2.193973e-04
+1.000000e+02 2.000000e+01 2.000000e+01 3.668204e-03 1.904346e-04 1.833405e-04
+1.450000e+02 2.500000e+01 2.500000e+01 1.620353e-03 9.284145e-05 1.015713e-04
+2.000000e+02 3.000000e+01 3.000000e+01 7.200092e-04 7.198744e-05 6.893148e-05
+4.150000e+02 1.850000e+02 1.850000e+02 5.267391e-05 7.814426e-06 8.318704e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d103-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d103-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t103
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 1.034115e-02 4.108572e-04 3.609603e-04
+6.000000e+01 2.000000e+01 2.000000e+01 7.397961e-03 1.964679e-04 2.217161e-04
+1.000000e+02 2.000000e+01 2.000000e+01 3.668204e-03 1.918907e-04 1.848656e-04
+1.450000e+02 2.500000e+01 2.500000e+01 1.620353e-03 9.423063e-05 1.028364e-04
+2.000000e+02 3.000000e+01 3.000000e+01 7.200092e-04 7.275637e-05 6.973580e-05
+4.150000e+02 1.850000e+02 1.850000e+02 5.267391e-05 7.874691e-06 8.375266e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d104-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d104-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 1.561840e-02 3.909731e-03 3.890711e-03
+2.250000e+01 7.500000e+00 7.500000e+00 4.750517e-02 1.058611e-02 1.102137e-02
+3.750000e+01 7.500000e+00 7.500000e+00 7.980193e-02 1.759369e-02 1.696316e-02
+5.250000e+01 7.500000e+00 7.500000e+00 1.013044e-01 2.320027e-02 2.263330e-02
+6.750000e+01 7.500000e+00 7.500000e+00 1.117994e-01 2.486833e-02 2.647098e-02
+8.250000e+01 7.500000e+00 7.500000e+00 1.178205e-01 2.613727e-02 2.466073e-02
+9.750000e+01 7.500000e+00 7.500000e+00 1.147695e-01 2.375186e-02 2.538747e-02
+1.125000e+02 7.500000e+00 7.500000e+00 1.099132e-01 2.360905e-02 2.488880e-02
+1.275000e+02 7.500000e+00 7.500000e+00 9.969275e-02 2.205072e-02 2.098092e-02
+1.425000e+02 7.500000e+00 7.500000e+00 8.941819e-02 1.694318e-02 1.728111e-02
+1.575000e+02 7.500000e+00 7.500000e+00 7.280748e-02 1.442074e-02 1.472675e-02
+1.725000e+02 7.500000e+00 7.500000e+00 5.754136e-02 1.170490e-02 1.150597e-02
+1.900000e+02 1.000000e+01 1.000000e+01 5.059591e-02 9.630425e-03 9.121423e-03
+2.150000e+02 1.500000e+01 1.500000e+01 4.342562e-02 8.043208e-03 7.519167e-03
+2.475000e+02 1.750000e+01 1.750000e+01 2.864620e-02 5.190524e-03 5.599864e-03
+2.950000e+02 3.000000e+01 3.000000e+01 1.676982e-02 3.168911e-03 2.924246e-03
+3.875000e+02 6.250000e+01 6.250000e+01 6.188119e-03 9.177031e-04 9.741818e-04
+7.250000e+02 2.750000e+02 2.750000e+02 3.406650e-04 8.597109e-05 8.703856e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d104-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d104-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t104
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 1.561840e-02 3.928084e-03 3.909107e-03
+2.250000e+01 7.500000e+00 7.500000e+00 4.750517e-02 1.060404e-02 1.103898e-02
+3.750000e+01 7.500000e+00 7.500000e+00 7.980193e-02 1.761395e-02 1.698468e-02
+5.250000e+01 7.500000e+00 7.500000e+00 1.013044e-01 2.321690e-02 2.265073e-02
+6.750000e+01 7.500000e+00 7.500000e+00 1.117994e-01 2.488361e-02 2.648487e-02
+8.250000e+01 7.500000e+00 7.500000e+00 1.178205e-01 2.615326e-02 2.467844e-02
+9.750000e+01 7.500000e+00 7.500000e+00 1.147695e-01 2.376718e-02 2.540144e-02
+1.125000e+02 7.500000e+00 7.500000e+00 1.099132e-01 2.362306e-02 2.490191e-02
+1.275000e+02 7.500000e+00 7.500000e+00 9.969275e-02 2.207288e-02 2.100517e-02
+1.425000e+02 7.500000e+00 7.500000e+00 8.941819e-02 1.696231e-02 1.730077e-02
+1.575000e+02 7.500000e+00 7.500000e+00 7.280748e-02 1.443362e-02 1.473918e-02
+1.725000e+02 7.500000e+00 7.500000e+00 5.754136e-02 1.171676e-02 1.151802e-02
+1.900000e+02 1.000000e+01 1.000000e+01 5.059591e-02 9.643320e-03 9.135100e-03
+2.150000e+02 1.500000e+01 1.500000e+01 4.342562e-02 8.055019e-03 7.531373e-03
+2.475000e+02 1.750000e+01 1.750000e+01 2.864620e-02 5.201524e-03 5.610142e-03
+2.950000e+02 3.000000e+01 3.000000e+01 1.676982e-02 3.175256e-03 2.931110e-03
+3.875000e+02 6.250000e+01 6.250000e+01 6.188119e-03 9.209939e-04 9.773039e-04
+7.250000e+02 2.750000e+02 2.750000e+02 3.406650e-04 8.642054e-05 8.748382e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d105-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d105-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 7.598619e-04 7.621058e-05 7.512122e-05
+2.250000e+01 7.500000e+00 7.500000e+00 2.311208e-03 1.448184e-04 1.432405e-04
+3.750000e+01 7.500000e+00 7.500000e+00 3.882501e-03 2.051773e-04 1.861752e-04
+5.250000e+01 7.500000e+00 7.500000e+00 4.928635e-03 2.657054e-04 2.350091e-04
+6.750000e+01 7.500000e+00 7.500000e+00 5.439234e-03 2.587557e-04 2.927052e-04
+8.250000e+01 7.500000e+00 7.500000e+00 5.732170e-03 2.485406e-04 2.086647e-04
+9.750000e+01 7.500000e+00 7.500000e+00 5.583732e-03 1.942831e-04 2.153875e-04
+1.125000e+02 7.500000e+00 7.500000e+00 5.347468e-03 2.038176e-04 2.402661e-04
+1.275000e+02 7.500000e+00 7.500000e+00 4.850224e-03 2.619351e-04 2.328520e-04
+1.425000e+02 7.500000e+00 7.500000e+00 4.350348e-03 1.561024e-04 1.891803e-04
+1.575000e+02 7.500000e+00 7.500000e+00 3.542209e-03 1.878625e-04 1.935420e-04
+1.725000e+02 7.500000e+00 7.500000e+00 2.799486e-03 1.335845e-04 1.251102e-04
+1.900000e+02 1.000000e+01 1.000000e+01 2.461578e-03 1.670466e-04 1.513155e-04
+2.150000e+02 1.500000e+01 1.500000e+01 2.112731e-03 1.187506e-04 1.036099e-04
+2.475000e+02 1.750000e+01 1.750000e+01 1.393687e-03 1.174067e-04 1.315403e-04
+2.950000e+02 3.000000e+01 3.000000e+01 8.158806e-04 8.545341e-05 8.263904e-05
+3.875000e+02 6.250000e+01 6.250000e+01 3.010626e-04 2.604645e-05 3.173561e-05
+7.250000e+02 2.750000e+02 2.750000e+02 1.657394e-05 3.121188e-06 3.227049e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d105-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d105-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t105
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 7.598619e-04 7.838705e-05 7.733213e-05
+2.250000e+01 7.500000e+00 7.500000e+00 2.311208e-03 1.478768e-04 1.463226e-04
+3.750000e+01 7.500000e+00 7.500000e+00 3.882501e-03 2.090755e-04 1.904365e-04
+5.250000e+01 7.500000e+00 7.500000e+00 4.928635e-03 2.688452e-04 2.385788e-04
+6.750000e+01 7.500000e+00 7.500000e+00 5.439234e-03 2.619212e-04 2.955135e-04
+8.250000e+01 7.500000e+00 7.500000e+00 5.732170e-03 2.522866e-04 2.131196e-04
+9.750000e+01 7.500000e+00 7.500000e+00 5.583732e-03 1.985217e-04 2.192188e-04
+1.125000e+02 7.500000e+00 7.500000e+00 5.347468e-03 2.072766e-04 2.431965e-04
+1.275000e+02 7.500000e+00 7.500000e+00 4.850224e-03 2.659412e-04 2.373487e-04
+1.425000e+02 7.500000e+00 7.500000e+00 4.350348e-03 1.607219e-04 1.930009e-04
+1.575000e+02 7.500000e+00 7.500000e+00 3.542209e-03 1.901264e-04 1.957277e-04
+1.725000e+02 7.500000e+00 7.500000e+00 2.799486e-03 1.358736e-04 1.275608e-04
+1.900000e+02 1.000000e+01 1.000000e+01 2.461578e-03 1.687363e-04 1.531913e-04
+2.150000e+02 1.500000e+01 1.500000e+01 2.112731e-03 1.205344e-04 1.056484e-04
+2.475000e+02 1.750000e+01 1.750000e+01 1.393687e-03 1.185183e-04 1.325421e-04
+2.950000e+02 3.000000e+01 3.000000e+01 8.158806e-04 8.599214e-05 8.319407e-05
+3.875000e+02 6.250000e+01 6.250000e+01 3.010626e-04 2.630922e-05 3.195103e-05
+7.250000e+02 2.750000e+02 2.750000e+02 1.657394e-05 3.150005e-06 3.255008e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d106-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d106-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e+01 1.750000e+01 1.750000e+01 4.339131e-02 9.401971e-03 1.075752e-02
+5.500000e+01 2.000000e+01 2.000000e+01 1.067533e-01 2.414350e-02 2.423053e-02
+1.000000e+02 2.500000e+01 2.500000e+01 1.118213e-01 2.374527e-02 2.390634e-02
+1.475000e+02 2.250000e+01 2.250000e+01 7.759650e-02 1.539752e-02 1.589126e-02
+1.975000e+02 2.750000e+01 2.750000e+01 4.580285e-02 8.886301e-03 8.094882e-03
+5.125000e+02 2.875000e+02 2.875000e+02 5.392794e-03 8.367453e-04 8.017010e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d106-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d106-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t106
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e+01 1.750000e+01 1.750000e+01 4.339131e-02 9.409114e-03 1.076386e-02
+5.500000e+01 2.000000e+01 2.000000e+01 1.067533e-01 2.414950e-02 2.423749e-02
+1.000000e+02 2.500000e+01 2.500000e+01 1.118213e-01 2.375093e-02 2.391201e-02
+1.475000e+02 2.250000e+01 2.250000e+01 7.759650e-02 1.540532e-02 1.589830e-02
+1.975000e+02 2.750000e+01 2.750000e+01 4.580285e-02 8.892920e-03 8.102194e-03
+5.125000e+02 2.875000e+02 2.875000e+02 5.392794e-03 8.373560e-04 8.023161e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d107-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d107-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e+01 1.750000e+01 1.750000e+01 2.117501e-03 1.147056e-04 1.419093e-04
+5.500000e+01 2.000000e+01 2.000000e+01 5.209573e-03 2.419647e-04 2.307058e-04
+1.000000e+02 2.500000e+01 2.500000e+01 5.456896e-03 1.767100e-04 1.728649e-04
+1.475000e+02 2.250000e+01 2.250000e+01 3.786719e-03 1.431993e-04 1.503310e-04
+1.975000e+02 2.750000e+01 2.750000e+01 2.235185e-03 1.108726e-04 9.896469e-05
+5.125000e+02 2.875000e+02 2.875000e+02 2.631691e-04 1.828969e-05 1.895417e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d107-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d107-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t107
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e+01 1.750000e+01 1.750000e+01 2.117501e-03 1.160358e-04 1.429897e-04
+5.500000e+01 2.000000e+01 2.000000e+01 5.209573e-03 2.431989e-04 2.320061e-04
+1.000000e+02 2.500000e+01 2.500000e+01 5.456896e-03 1.782025e-04 1.744114e-04
+1.475000e+02 2.250000e+01 2.250000e+01 3.786719e-03 1.448780e-04 1.519108e-04
+1.975000e+02 2.750000e+01 2.750000e+01 2.235185e-03 1.119939e-04 1.002210e-04
+5.125000e+02 2.875000e+02 2.875000e+02 2.631691e-04 1.834619e-05 1.900697e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d108-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d108-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 4.100937e-01 5.728535e-02 5.383764e-02
+6.000000e+01 2.000000e+01 2.000000e+01 2.197165e-01 2.769745e-02 2.652037e-02
+1.000000e+02 2.000000e+01 2.000000e+01 7.841046e-02 9.189586e-03 9.295863e-03
+1.450000e+02 2.500000e+01 2.500000e+01 2.435284e-02 3.437684e-03 3.166404e-03
+2.000000e+02 3.000000e+01 3.000000e+01 9.005711e-03 1.426268e-03 1.343364e-03
+4.150000e+02 1.850000e+02 1.850000e+02 6.885695e-04 1.362526e-04 1.311870e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d108-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d108-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t108
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 4.100937e-01 5.729817e-02 5.384754e-02
+6.000000e+01 2.000000e+01 2.000000e+01 2.197165e-01 2.771439e-02 2.653895e-02
+1.000000e+02 2.000000e+01 2.000000e+01 7.841046e-02 9.210274e-03 9.316108e-03
+1.450000e+02 2.500000e+01 2.500000e+01 2.435284e-02 3.452119e-03 3.182027e-03
+2.000000e+02 3.000000e+01 3.000000e+01 9.005711e-03 1.439750e-03 1.357665e-03
+4.150000e+02 1.850000e+02 1.850000e+02 6.885695e-04 1.374935e-04 1.324740e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d109-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d109-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 1.351590e-02 5.419175e-04 5.286187e-04
+6.000000e+01 2.000000e+01 2.000000e+01 7.241433e-03 2.190482e-04 2.422758e-04
+1.000000e+02 2.000000e+01 2.000000e+01 2.584257e-03 1.799348e-04 1.946957e-04
+1.450000e+02 2.500000e+01 2.500000e+01 8.026224e-04 9.397111e-05 7.940326e-05
+2.000000e+02 3.000000e+01 3.000000e+01 2.968108e-04 4.796484e-05 4.701431e-05
+4.150000e+02 1.850000e+02 1.850000e+02 2.269392e-05 4.563486e-06 4.305850e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d109-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d109-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t109
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 1.351590e-02 5.427419e-04 5.294638e-04
+6.000000e+01 2.000000e+01 2.000000e+01 7.241433e-03 2.208571e-04 2.439290e-04
+1.000000e+02 2.000000e+01 2.000000e+01 2.584257e-03 1.809861e-04 1.956710e-04
+1.450000e+02 2.500000e+01 2.500000e+01 8.026224e-04 9.452831e-05 8.006582e-05
+2.000000e+02 3.000000e+01 3.000000e+01 2.968108e-04 4.839471e-05 4.745272e-05
+4.150000e+02 1.850000e+02 1.850000e+02 2.269392e-05 4.603356e-06 4.348049e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d110-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d110-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 2.174049e-02 3.497601e-03 3.577509e-03
+2.250000e+01 7.500000e+00 7.500000e+00 7.535165e-02 1.116062e-02 1.035610e-02
+3.750000e+01 7.500000e+00 7.500000e+00 1.166285e-01 1.719628e-02 1.733647e-02
+5.250000e+01 7.500000e+00 7.500000e+00 1.496832e-01 2.268939e-02 1.996178e-02
+6.750000e+01 7.500000e+00 7.500000e+00 1.833478e-01 2.510865e-02 2.347292e-02
+8.250000e+01 7.500000e+00 7.500000e+00 1.887459e-01 2.503184e-02 2.514458e-02
+9.750000e+01 7.500000e+00 7.500000e+00 1.821275e-01 2.591629e-02 2.336110e-02
+1.125000e+02 7.500000e+00 7.500000e+00 1.702186e-01 2.393265e-02 2.151100e-02
+1.275000e+02 7.500000e+00 7.500000e+00 1.520217e-01 2.107446e-02 1.917897e-02
+1.425000e+02 7.500000e+00 7.500000e+00 1.287073e-01 1.663060e-02 1.643501e-02
+1.575000e+02 7.500000e+00 7.500000e+00 1.106275e-01 1.393410e-02 1.350459e-02
+1.725000e+02 7.500000e+00 7.500000e+00 9.576870e-02 1.170149e-02 1.082682e-02
+1.900000e+02 1.000000e+01 1.000000e+01 7.599576e-02 8.486872e-03 8.525461e-03
+2.150000e+02 1.500000e+01 1.500000e+01 5.610183e-02 7.386233e-03 6.302448e-03
+2.475000e+02 1.750000e+01 1.750000e+01 3.550773e-02 4.483631e-03 3.678892e-03
+2.950000e+02 3.000000e+01 3.000000e+01 1.967260e-02 1.796745e-03 1.996371e-03
+3.875000e+02 6.250000e+01 6.250000e+01 6.680246e-03 9.040614e-04 8.142951e-04
+7.250000e+02 2.750000e+02 2.750000e+02 3.667169e-04 7.762088e-05 7.844866e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d110-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d110-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t110
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 2.174049e-02 3.531131e-03 3.610127e-03
+2.250000e+01 7.500000e+00 7.500000e+00 7.535165e-02 1.119341e-02 1.039153e-02
+3.750000e+01 7.500000e+00 7.500000e+00 1.166285e-01 1.722639e-02 1.736565e-02
+5.250000e+01 7.500000e+00 7.500000e+00 1.496832e-01 2.272246e-02 1.999995e-02
+6.750000e+01 7.500000e+00 7.500000e+00 1.833478e-01 2.514087e-02 2.350640e-02
+8.250000e+01 7.500000e+00 7.500000e+00 1.887459e-01 2.506245e-02 2.517588e-02
+9.750000e+01 7.500000e+00 7.500000e+00 1.821275e-01 2.594562e-02 2.339195e-02
+1.125000e+02 7.500000e+00 7.500000e+00 1.702186e-01 2.395393e-02 2.153514e-02
+1.275000e+02 7.500000e+00 7.500000e+00 1.520217e-01 2.110000e-02 1.920592e-02
+1.425000e+02 7.500000e+00 7.500000e+00 1.287073e-01 1.666366e-02 1.646879e-02
+1.575000e+02 7.500000e+00 7.500000e+00 1.106275e-01 1.395598e-02 1.352771e-02
+1.725000e+02 7.500000e+00 7.500000e+00 9.576870e-02 1.173055e-02 1.085821e-02
+1.900000e+02 1.000000e+01 1.000000e+01 7.599576e-02 8.510425e-03 8.548586e-03
+2.150000e+02 1.500000e+01 1.500000e+01 5.610183e-02 7.402870e-03 6.322040e-03
+2.475000e+02 1.750000e+01 1.750000e+01 3.550773e-02 4.499752e-03 3.698780e-03
+2.950000e+02 3.000000e+01 3.000000e+01 1.967260e-02 1.808310e-03 2.006841e-03
+3.875000e+02 6.250000e+01 6.250000e+01 6.680246e-03 9.081937e-04 8.187985e-04
+7.250000e+02 2.750000e+02 2.750000e+02 3.667169e-04 7.834794e-05 7.916930e-05
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d111-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d111-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 7.178073e-04 6.277439e-05 6.613597e-05
+2.250000e+01 7.500000e+00 7.500000e+00 2.487891e-03 1.533133e-04 1.502746e-04
+3.750000e+01 7.500000e+00 7.500000e+00 3.850732e-03 1.807092e-04 1.939954e-04
+5.250000e+01 7.500000e+00 7.500000e+00 4.942103e-03 2.239253e-04 2.082219e-04
+6.750000e+01 7.500000e+00 7.500000e+00 6.053610e-03 2.160100e-04 2.309847e-04
+8.250000e+01 7.500000e+00 7.500000e+00 6.231837e-03 2.456291e-04 2.829159e-04
+9.750000e+01 7.500000e+00 7.500000e+00 6.013319e-03 2.447523e-04 2.191790e-04
+1.125000e+02 7.500000e+00 7.500000e+00 5.620120e-03 2.342040e-04 2.037469e-04
+1.275000e+02 7.500000e+00 7.500000e+00 5.019313e-03 1.899147e-04 1.870976e-04
+1.425000e+02 7.500000e+00 7.500000e+00 4.249539e-03 1.422281e-04 1.569535e-04
+1.575000e+02 7.500000e+00 7.500000e+00 3.652598e-03 1.277718e-04 1.285696e-04
+1.725000e+02 7.500000e+00 7.500000e+00 3.162002e-03 1.151248e-04 1.190050e-04
+1.900000e+02 1.000000e+01 1.000000e+01 2.509158e-03 1.092811e-04 1.196867e-04
+2.150000e+02 1.500000e+01 1.500000e+01 1.852319e-03 1.215622e-04 1.115610e-04
+2.475000e+02 1.750000e+01 1.750000e+01 1.172362e-03 9.216659e-05 8.128108e-05
+2.950000e+02 3.000000e+01 3.000000e+01 6.495318e-04 4.718252e-05 5.672684e-05
+3.875000e+02 6.250000e+01 6.250000e+01 2.205622e-04 2.163455e-05 2.129070e-05
+7.250000e+02 2.750000e+02 2.750000e+02 1.210792e-05 2.419514e-06 2.399666e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d111-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d111-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t111
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e+00 7.500000e+00 7.500000e+00 7.178073e-04 6.477973e-05 6.804092e-05
+2.250000e+01 7.500000e+00 7.500000e+00 2.487891e-03 1.558509e-04 1.528735e-04
+3.750000e+01 7.500000e+00 7.500000e+00 3.850732e-03 1.836941e-04 1.967772e-04
+5.250000e+01 7.500000e+00 7.500000e+00 4.942103e-03 2.273857e-04 2.119455e-04
+6.750000e+01 7.500000e+00 7.500000e+00 6.053610e-03 2.196832e-04 2.344217e-04
+8.250000e+01 7.500000e+00 7.500000e+00 6.231837e-03 2.486749e-04 2.855726e-04
+9.750000e+01 7.500000e+00 7.500000e+00 6.013319e-03 2.477703e-04 2.225195e-04
+1.125000e+02 7.500000e+00 7.500000e+00 5.620120e-03 2.365602e-04 2.064598e-04
+1.275000e+02 7.500000e+00 7.500000e+00 5.019313e-03 1.926779e-04 1.899200e-04
+1.425000e+02 7.500000e+00 7.500000e+00 4.249539e-03 1.460999e-04 1.604906e-04
+1.575000e+02 7.500000e+00 7.500000e+00 3.652598e-03 1.302540e-04 1.310205e-04
+1.725000e+02 7.500000e+00 7.500000e+00 3.162002e-03 1.181636e-04 1.219404e-04
+1.900000e+02 1.000000e+01 1.000000e+01 2.509158e-03 1.111615e-04 1.214128e-04
+2.150000e+02 1.500000e+01 1.500000e+01 1.852319e-03 1.226328e-04 1.127269e-04
+2.475000e+02 1.750000e+01 1.750000e+01 1.172362e-03 9.300031e-05 8.222573e-05
+2.950000e+02 3.000000e+01 3.000000e+01 6.495318e-04 4.765210e-05 5.712175e-05
+3.875000e+02 6.250000e+01 6.250000e+01 2.205622e-04 2.181703e-05 2.147627e-05
+7.250000e+02 2.750000e+02 2.750000e+02 1.210792e-05 2.444768e-06 2.425163e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d112-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d112-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e+01 1.750000e+01 1.750000e+01 1.334121e-01 2.145085e-02 2.035247e-02
+5.500000e+01 2.000000e+01 2.000000e+01 2.832749e-01 3.879574e-02 3.628020e-02
+1.000000e+02 2.500000e+01 2.500000e+01 1.558130e-01 2.030096e-02 1.916733e-02
+1.475000e+02 2.250000e+01 2.250000e+01 6.776909e-02 8.220697e-03 8.093007e-03
+1.975000e+02 2.750000e+01 2.750000e+01 3.203683e-02 3.497337e-03 3.691986e-03
+5.125000e+02 2.875000e+02 2.875000e+02 2.996525e-03 3.298308e-04 3.273211e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d112-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d112-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t112
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e+01 1.750000e+01 1.750000e+01 1.334121e-01 2.146171e-02 2.036381e-02
+5.500000e+01 2.000000e+01 2.000000e+01 2.832749e-01 3.880526e-02 3.628964e-02
+1.000000e+02 2.500000e+01 2.500000e+01 1.558130e-01 2.031460e-02 1.918062e-02
+1.475000e+02 2.250000e+01 2.250000e+01 6.776909e-02 8.235812e-03 8.108319e-03
+1.975000e+02 2.750000e+01 2.750000e+01 3.203683e-02 3.512424e-03 3.706422e-03
+5.125000e+02 2.875000e+02 2.875000e+02 2.996525e-03 3.309996e-04 3.285118e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d113-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d113-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e+01 1.750000e+01 1.750000e+01 4.399306e-03 3.096074e-04 3.032296e-04
+5.500000e+01 2.000000e+01 2.000000e+01 9.341081e-03 3.429123e-04 3.361030e-04
+1.000000e+02 2.500000e+01 2.500000e+01 5.137985e-03 2.297163e-04 2.206420e-04
+1.475000e+02 2.250000e+01 2.250000e+01 2.234708e-03 1.391592e-04 1.482603e-04
+1.975000e+02 2.750000e+01 2.750000e+01 1.056425e-03 7.231675e-05 8.516204e-05
+5.125000e+02 2.875000e+02 2.875000e+02 9.881139e-05 1.087714e-05 9.579000e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d113-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d113-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t113
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e+01 1.750000e+01 1.750000e+01 4.399306e-03 3.103300e-04 3.039590e-04
+5.500000e+01 2.000000e+01 2.000000e+01 9.341081e-03 3.437747e-04 3.370376e-04
+1.000000e+02 2.500000e+01 2.500000e+01 5.137985e-03 2.307384e-04 2.216793e-04
+1.475000e+02 2.250000e+01 2.250000e+01 2.234708e-03 1.400758e-04 1.491201e-04
+1.975000e+02 2.750000e+01 2.750000e+01 1.056425e-03 7.308430e-05 8.580969e-05
+5.125000e+02 2.875000e+02 2.875000e+02 9.881139e-05 1.091425e-05 9.620007e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d114-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d114-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 1.712543e+00 1.871097e-01 1.709333e-01
+6.000000e+01 2.000000e+01 2.000000e+01 5.358253e-01 8.168736e-02 8.249875e-02
+1.000000e+02 2.000000e+01 2.000000e+01 1.791376e-01 2.848395e-02 2.795310e-02
+1.450000e+02 2.500000e+01 2.500000e+01 6.317582e-02 9.130445e-03 8.207692e-03
+2.000000e+02 3.000000e+01 3.000000e+01 2.480229e-02 3.094746e-03 2.818306e-03
+4.150000e+02 1.850000e+02 1.850000e+02 1.792559e-03 2.919523e-04 2.752374e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d114-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d114-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t114
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 1.712543e+00 1.871326e-01 1.709569e-01
+6.000000e+01 2.000000e+01 2.000000e+01 5.358253e-01 8.170192e-02 8.251637e-02
+1.000000e+02 2.000000e+01 2.000000e+01 1.791376e-01 2.849834e-02 2.796558e-02
+1.450000e+02 2.500000e+01 2.500000e+01 6.317582e-02 9.143305e-03 8.221557e-03
+2.000000e+02 3.000000e+01 3.000000e+01 2.480229e-02 3.109256e-03 2.834073e-03
+4.150000e+02 1.850000e+02 1.850000e+02 1.792559e-03 2.932145e-04 2.765645e-04
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d115-x01-y01
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d115-x01-y01
+Title: doi:10.17182/hepdata.81950.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 1.672235e-02 6.557407e-04 6.292375e-04
+6.000000e+01 2.000000e+01 2.000000e+01 5.232138e-03 3.855559e-04 4.221048e-04
+1.000000e+02 2.000000e+01 2.000000e+01 1.749212e-03 1.451464e-04 1.508088e-04
+1.450000e+02 2.500000e+01 2.500000e+01 6.168887e-04 4.101550e-05 3.793790e-05
+2.000000e+02 3.000000e+01 3.000000e+01 2.421853e-04 1.726437e-05 1.693520e-05
+4.150000e+02 1.850000e+02 1.850000e+02 1.750368e-05 2.041546e-06 1.992443e-06
+END YODA_SCATTER2D_V2
+BEGIN YODA_SCATTER2D_V2 /REF/ATLAS_2018_I1656578/d115-x01-y02
+IsRef: 1
+Path: /REF/ATLAS_2018_I1656578/d115-x01-y02
+Title: doi:10.17182/hepdata.81950.v1/t115
+Type: Scatter2D
+---
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e+01 2.000000e+01 2.000000e+01 1.672235e-02 6.560428e-04 6.294862e-04
+6.000000e+01 2.000000e+01 2.000000e+01 5.232138e-03 3.857917e-04 4.223353e-04
+1.000000e+02 2.000000e+01 2.000000e+01 1.749212e-03 1.453800e-04 1.510303e-04
+1.450000e+02 2.500000e+01 2.500000e+01 6.168887e-04 4.128176e-05 3.822995e-05
+2.000000e+02 3.000000e+01 3.000000e+01 2.421853e-04 1.750775e-05 1.718440e-05
+4.150000e+02 1.850000e+02 1.850000e+02 1.750368e-05 2.058579e-06 2.009817e-06
+END YODA_SCATTER2D_V2
diff --git a/analyses/pluginCMS/CMS_2012_I1102908.cc b/analyses/pluginCMS/CMS_2012_I1102908.cc
--- a/analyses/pluginCMS/CMS_2012_I1102908.cc
+++ b/analyses/pluginCMS/CMS_2012_I1102908.cc
@@ -1,89 +1,87 @@
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Tools/BinnedHistogram.hh"
#include "Rivet/Projections/FinalState.hh"
#include "Rivet/Projections/FastJets.hh"
#include <sstream>
namespace Rivet {
- /// @cond
- inline double _invert(double x) { return (x > 0) ? 1/x : 0; }
- /// @endcond
-
/// @brief CMS inclusive and exclusive dijet production ratio at large rapidity intervals
class CMS_2012_I1102908 : public Analysis {
public:
CMS_2012_I1102908()
: Analysis("CMS_2012_I1102908")
{ }
void init() {
// Projections
declare(FastJets(FinalState(), FastJets::ANTIKT, 0.5), "antikT");
// Histograms
/// @todo Can we manage to only register these as they are "really" created in the finalize()?
_h_dijet_ratio = bookScatter2D(1, 1, 1);
_h_MN_dijet_ratio = bookScatter2D(2, 1, 1);
// Temporary histograms (directly instantiated)
_h_DeltaY_exclusive = bookHisto1D("TMP/excl",refData(1, 1, 1));
_h_DeltaY_inclusive = bookHisto1D("TMP/incl",refData(1, 1, 1));
_h_DeltaY_MN = bookHisto1D("TMP/YMN",refData(1, 1, 1));
}
void analyze(const Event & event) {
const double weight = event.weight();
// Jets with pT > 35.0, -4.7 < y < 4.7
const JetAlg& jet_alg = apply<JetAlg>(event, "antikT");
const Jets& jets = jet_alg.jets(Cuts::pT > 35*GeV && Cuts::absrap < 4.7);
// Veto event if number of jets less than 2
if (jets.size() < 2) return;
// Loop over jet pairs
double deltaY_MN = 0.0;
for (size_t ij1 = 0; ij1 < jets.size(); ++ij1) {
for (size_t ij2 = ij1 + 1; ij2 < jets.size(); ++ij2) {
const double deltaY = fabs(jets[ij1].rapidity() - jets[ij2].rapidity());
// Exclusive dijet case:
if (jets.size() == 2) _h_DeltaY_exclusive->fill(deltaY, weight);
// Inclusive jets case:
_h_DeltaY_inclusive->fill(deltaY, weight);
// Mueller-Navelet:
if (deltaY > deltaY_MN) deltaY_MN = deltaY;
}
}
_h_DeltaY_MN->fill(deltaY_MN, weight);
}
-
void finalize() {
- *_h_dijet_ratio = YODA::efficiency(*_h_DeltaY_exclusive, *_h_DeltaY_inclusive);
- *_h_MN_dijet_ratio = YODA::efficiency(*_h_DeltaY_exclusive, *_h_DeltaY_MN);
+ efficiency(_h_DeltaY_exclusive, _h_DeltaY_inclusive, _h_dijet_ratio);
+ efficiency(_h_DeltaY_exclusive, _h_DeltaY_MN, _h_MN_dijet_ratio);
transformY(*_h_dijet_ratio, _invert);
transformY(*_h_MN_dijet_ratio, _invert);
}
private:
+ /// Reciprocal function with div-by-zero protection, for inverting the efficiency measure
+ static double _invert(double x) { return (x > 0) ? 1/x : 0; }
+
/// @name Histograms
//@{
Scatter2DPtr _h_dijet_ratio, _h_MN_dijet_ratio;
Histo1DPtr _h_DeltaY_inclusive, _h_DeltaY_exclusive, _h_DeltaY_MN;
//@}
};
DECLARE_RIVET_PLUGIN(CMS_2012_I1102908);
}
diff --git a/analyses/pluginCMS/CMS_2018_I1653948.cc b/analyses/pluginCMS/CMS_2018_I1653948.cc
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1653948.cc
@@ -0,0 +1,88 @@
+// -*- C++ -*-
+#include "Rivet/Analysis.hh"
+#include "Rivet/Projections/FinalState.hh"
+
+namespace Rivet {
+
+
+ class CMS_2018_I1653948 : public Analysis {
+ public:
+
+ CMS_2018_I1653948()
+ : Analysis("CMS_2018_I1653948"), _xi_hf_cut(1E-6), _xi_castor_cut(1E-7)
+ { }
+
+
+ /// Book projections and histograms
+ void init() {
+ addProjection(FinalState(),"FS");
+ _h_xsec = bookHisto1D(1, 1, 1);
+ }
+
+
+ /// Analyze each event
+ void analyze(const Event& event) {
+
+ const double weight = event.weight();
+
+ const FinalState& fs = applyProjection<FinalState>(event, "FS");
+ if (fs.size() < 3) vetoEvent; // veto on elastic events
+ const ParticleVector particlesByRapidity = fs.particles(cmpMomByRap);
+ const size_t num_particles = particlesByRapidity.size();
+
+ vector<double> gaps;
+ vector<double> midpoints;
+
+ for (size_t ip = 1; ip < num_particles; ++ip) {
+ const Particle& p1 = particlesByRapidity[ip-1];
+ const Particle& p2 = particlesByRapidity[ip];
+ const double gap = p2.momentum().rapidity() - p1.momentum().rapidity();
+ const double mid = (p2.momentum().rapidity() + p1.momentum().rapidity()) / 2.;
+ gaps.push_back(gap);
+ midpoints.push_back(mid);
+ }
+
+ int imid = std::distance(gaps.begin(), max_element(gaps.begin(), gaps.end()));
+ double gapcenter = midpoints[imid];
+
+ FourMomentum MxFourVector(0.,0.,0.,0.);
+ FourMomentum MyFourVector(0.,0.,0.,0.);
+
+ for (const Particle& p : fs.particles(cmpMomByEta)) {
+ if (p.momentum().rapidity() < gapcenter) {
+ MxFourVector += p.momentum();
+ } else {
+ MyFourVector += p.momentum();
+ }
+ }
+
+ double Mx = MxFourVector.mass();
+ double My = MyFourVector.mass();
+
+ double xix = (Mx * Mx) / (sqrtS()/GeV * sqrtS()/GeV);
+ double xiy = (My * My) / (sqrtS()/GeV * sqrtS()/GeV);
+ double xi = max(xix, xiy);
+
+ if (xi > _xi_hf_cut) _h_xsec->fill(0.5, weight);
+ if (xix > _xi_castor_cut || xiy > _xi_hf_cut) _h_xsec->fill(1.5, weight);
+ }
+
+
+ /// Normalizations, etc.
+ void finalize() {
+ scale(_h_xsec, crossSection()/millibarn/sumOfWeights());
+ }
+
+
+ private:
+
+ Histo1DPtr _h_xsec;
+ double _xi_hf_cut;
+ double _xi_castor_cut;
+
+ };
+
+
+ DECLARE_RIVET_PLUGIN(CMS_2018_I1653948);
+
+}
diff --git a/analyses/pluginCMS/CMS_2018_I1653948.info b/analyses/pluginCMS/CMS_2018_I1653948.info
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1653948.info
@@ -0,0 +1,48 @@
+Name: CMS_2018_I1653948
+Year: 2018
+Summary: Measurement of the inelastic proton-proton cross section at 13 TeV
+Experiment: CMS
+Collider: LHC
+InspireID: 1653948
+Status: VALIDATED
+Authors:
+ - cms-pag-conveners-smp@cern.ch
+ - Sercan Sen <Sercan.Sen@cern.ch>
+ - Pierre Van Mechelen <pierre.vanmechelen@uantwerpen.be>
+ - Hans Van Haevermaet <hans.vanhaevermaet@uantwerpen.be>
+References:
+ - JHEP 07 (2018) 161
+ - DOI 10.1007/JHEP07(2018)161
+ - CMS-FSQ-15-005
+ - arXiv:1802.02613 [hep-ex]
+ - CERN-EP-2018-004
+ - http://cms-results.web.cern.ch/cms-results/public-results/publications/FSQ-15-005/
+RunInfo:
+ Inelastic events (non-diffractive and inelastic diffractive).
+NumEvents: 1M
+Beams: [p+, p+]
+Energies: [13000]
+PtCuts:
+Description:
+ 'A measurement of the inelastic proton-proton cross section at $\sqrt{s} = 13$ TeV with the CMS
+ detector at the LHC has been presented. An inelastic cross section of $67.5 \pm 0.8 \text{(syst)}
+ \pm 1.6 \text{(lumi)}$ mb is obtained for $\xi = M^2/s > 10^{-6}$ (corresponding to $M > 13$ GeV),
+ with $M$ the larger of $M_{\mathrm{X}}$ and $M_{\mathrm{Y}}$, where $M_{\mathrm{X}}$ and
+ $M_{\mathrm{Y}}$ are the masses of the diffractive dissociation systems with negative and positive
+ pseudorapidities, respectively. In addition, an inelastic cross section of $68.6 \pm 0.5 \text{(syst)}
+ \pm 1.6 \text{(lumi)}$ mb is obtained in the enlarged phase space $\xi_{\mathrm{X}} > 10^{-7}$
+ and/or $\xi_{\mathrm{Y}} > 10^{-6}$ (corresponding to $M_{\mathrm{X}} > 4.1$ GeV and/or
+ $M_{\mathrm{Y}} > 13$ GeV).'
+BibKey: Sirunyan:2018nqx
+BibTeX: '@article{Sirunyan:2018nqx,
+ author = "Sirunyan, Albert M and others",
+ title = "{Measurement of the inelastic proton-proton cross section
+ at $\sqrt{s}=$ 13 TeV}",
+ collaboration = "CMS",
+ year = "2018",
+ eprint = "1802.02613",
+ archivePrefix = "arXiv",
+ primaryClass = "hep-ex",
+ reportNumber = "CMS-FSQ-15-005, CERN-EP-2018-004",
+ SLACcitation = "%%CITATION = ARXIV:1802.02613;%%"
+}'
diff --git a/analyses/pluginCMS/CMS_2018_I1653948.plot b/analyses/pluginCMS/CMS_2018_I1653948.plot
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1653948.plot
@@ -0,0 +1,8 @@
+# BEGIN PLOT /CMS_2018_I1653948/d01-x01-y01
+Title=CMS, $13$ TeV, proton-proton inelastic cross section
+XCustomMajorTicks=0.5 $\xi>10^{-6}$ 1.5 $\xi_{X}>10^{-7}\;\text{or}\;\xi_{Y}>10^{-6}$
+LegendXPos=0.1
+LegendYPos=0.6
+YLabel=$\sigma$ [mb]
+LogY=0
+# END PLOT
diff --git a/analyses/pluginCMS/CMS_2018_I1653948.yoda b/analyses/pluginCMS/CMS_2018_I1653948.yoda
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1653948.yoda
@@ -0,0 +1,9 @@
+BEGIN YODA_SCATTER2D /REF/CMS_2018_I1653948/d01-x01-y01
+IsRef=1
+Path=/REF/CMS_2018_I1653948/d01-x01-y01
+Title=
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e-01 5.000000e-01 5.000000e-01 6.750000e+01 1.788854e+00 1.788854e+00
+1.500000e+00 5.000000e-01 5.000000e-01 6.860000e+01 1.676305e+00 1.676305e+00
+END YODA_SCATTER2D
diff --git a/analyses/pluginCMS/CMS_2018_I1680318.cc b/analyses/pluginCMS/CMS_2018_I1680318.cc
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1680318.cc
@@ -0,0 +1,222 @@
+// -*- C++ -*-
+#include "Rivet/Analysis.hh"
+#include "Rivet/Projections/FinalState.hh"
+#include "Rivet/Projections/ChargedFinalState.hh"
+
+namespace Rivet {
+
+
+ class CMS_2018_I1680318 : public Analysis {
+ public:
+
+ /// Constructor
+ DEFAULT_RIVET_ANALYSIS_CTOR(CMS_2018_I1680318);
+
+
+ /// Book histograms and initialise projections before the run
+ void init() {
+
+ // Cuts
+ MinEnergy = 5.0; // Particle's energy cut in the forward region [GeV]
+ EtaForwardMin = 3.0;
+ EtaForwardMax = 5.0;
+ EtaCentralCut = 2.4;
+ MinParticlePt = 0.5; // [GeV]
+
+
+ // Initialise and register projections
+ const FinalState fsa(-1.0*EtaForwardMax, EtaForwardMax, 0.0000*GeV);
+ addProjection(fsa, "FSA");
+
+ const ChargedFinalState cfs(-1.0*EtaCentralCut, EtaCentralCut, MinParticlePt*GeV);
+ addProjection(cfs, "CFS");
+
+
+ // Event counters
+ _num_evts_noCuts = 0;
+ _num_evts_after_cuts_or = 0;
+ _num_evts_after_cuts_and = 0;
+ _num_evts_after_cuts_xor = 0;
+ _num_evts_after_cuts_xorm = 0;
+ _num_evts_after_cuts_xorp = 0;
+
+
+ // Histograms
+ _hist_dNch_all_dEta_OR = bookHisto1D(1,1,1);
+ _hist_dNch_all_dEta_AND = bookHisto1D(1,2,1);
+ _hist_dNch_all_dEta_XOR = bookHisto1D(1,3,1);
+ _hist_dNch_all_dEta_XORpm = bookHisto1D(1,4,1);
+
+ _hist_dNch_all_dpt_OR = bookHisto1D(2,1,1);
+ _hist_dNch_all_dpt_AND = bookHisto1D(2,2,1);
+ _hist_dNch_all_dpt_XOR = bookHisto1D(2,3,1);
+
+ _hist_dNch_leading_dpt_OR = bookHisto1D(3,1,1);
+ _hist_dNch_leading_dpt_AND = bookHisto1D(3,2,1);
+ _hist_dNch_leading_dpt_XOR = bookHisto1D(3,3,1);
+
+ _hist_integrated_leading_pt_OR = bookHisto1D(4,1,1);
+ _hist_integrated_leading_pt_AND = bookHisto1D(4,2,1);
+ _hist_integrated_leading_pt_XOR = bookHisto1D(4,3,1);
+
+ _hist_dNev_all_dM_OR = bookHisto1D(5,1,1);
+ _hist_dNev_all_dM_AND = bookHisto1D(5,2,1);
+ }
+
+
+ /// Perform the per-event analysis
+ void analyze(const Event& event) {
+ const double weight = event.weight();
+
+ const ChargedFinalState& charged = applyProjection<ChargedFinalState>(event, "CFS");
+ const FinalState& fsa = applyProjection<FinalState>(event, "FSA");
+
+ bool activity_plus_side = false,
+ activity_minus_side = false;
+
+ for (const Particle& p : fsa.particles()) {
+ if ( p.energy() >= MinEnergy ) {
+ if ( inRange(p.eta(), EtaForwardMin, EtaForwardMax) ) activity_plus_side = true;
+ if ( inRange(p.eta(), -1.0*EtaForwardMax, -1.0*EtaForwardMin) ) activity_minus_side = true;
+ }
+
+ // If activity already found in both sides,
+ // then there is no point in keep going the loop
+ if (activity_plus_side && activity_minus_side) break;
+ }
+
+ // Event selections
+ const bool cutsor = ( activity_plus_side || activity_minus_side);
+ const bool cutsand = ( activity_plus_side && activity_minus_side);
+ const bool cutsxor = ((activity_plus_side && !activity_minus_side) || (!activity_plus_side && activity_minus_side));
+ const bool cutsxorm = (!activity_plus_side && activity_minus_side);
+ const bool cutsxorp = ( activity_plus_side && !activity_minus_side);
+
+ _num_evts_noCuts += weight;
+ if ( charged.size() >= 1 ) {
+ if (cutsor) _num_evts_after_cuts_or += weight;
+ if (cutsand) _num_evts_after_cuts_and += weight;
+ if (cutsxor) _num_evts_after_cuts_xor += weight;
+ if (cutsxorm) _num_evts_after_cuts_xorm += weight;
+ if (cutsxorp) _num_evts_after_cuts_xorp += weight;
+ }
+
+ // Loop over charged particles
+ double leading_pt = 0;
+ for (const Particle& p : charged.particles()) {
+ // Find the leading-pt particle of the event
+ if (p.pT() > leading_pt) leading_pt = p.pT();
+
+ // Filling histograms
+ if (cutsor) _hist_dNch_all_dEta_OR -> fill(p.eta(), weight);
+ if (cutsand) _hist_dNch_all_dEta_AND -> fill(p.eta(), weight);
+ if (cutsxor) _hist_dNch_all_dEta_XOR -> fill(p.eta(), weight);
+
+ //Average xorm & xorp
+ if (cutsxorm) _hist_dNch_all_dEta_XORpm -> fill(p.eta(), weight);
+ if (cutsxorp) _hist_dNch_all_dEta_XORpm -> fill(-1.0*p.eta(), weight);
+
+ if (cutsor) _hist_dNch_all_dpt_OR -> fill(p.pT(), weight);
+ if (cutsand) _hist_dNch_all_dpt_AND -> fill(p.pT(), weight);
+ if (cutsxor) _hist_dNch_all_dpt_XOR -> fill(p.pT(), weight);
+ }
+
+ // Filling multiplicity histograms
+ if ( charged.size() >= 1 ) {
+ if (cutsor) _hist_dNev_all_dM_OR -> fill(charged.size(), weight);
+ if (cutsand) _hist_dNev_all_dM_AND -> fill(charged.size(), weight);
+ }
+
+ // Filling leading-pt histograms
+ if (cutsor) _hist_dNch_leading_dpt_OR -> fill(leading_pt, weight);
+ if (cutsand) _hist_dNch_leading_dpt_AND -> fill(leading_pt, weight);
+ if (cutsxor) _hist_dNch_leading_dpt_XOR -> fill(leading_pt, weight);
+
+ // Integrating leading-pt histograms
+ for (size_t i = 0 ; i < _hist_integrated_leading_pt_OR->numBins() ; ++i) {
+ double binlimitlow_t = _hist_integrated_leading_pt_OR->bin(i).xMin(),
+ weightbw_t = _hist_integrated_leading_pt_OR->bin(i).xWidth()*weight,
+ xbin_t = _hist_integrated_leading_pt_OR->bin(i).xMid();
+ if (leading_pt > binlimitlow_t) {
+ if (cutsor) _hist_integrated_leading_pt_OR -> fill(xbin_t, weightbw_t);
+ if (cutsand) _hist_integrated_leading_pt_AND -> fill(xbin_t, weightbw_t);
+ if (cutsxor) _hist_integrated_leading_pt_XOR -> fill(xbin_t, weightbw_t);
+ }
+ }
+
+ }
+
+
+ /// Normalise histograms etc., after the run
+ void finalize() {
+ MSG_INFO("Number of selected events: " << endl
+ << "\t All = " << _num_evts_noCuts << endl
+ << "\t Inelastic = " << _num_evts_after_cuts_or << endl
+ << "\t NSD = " << _num_evts_after_cuts_and << endl
+ << "\t Xor = " << _num_evts_after_cuts_xor << endl
+ << "\t Xorm = " << _num_evts_after_cuts_xorm << endl
+ << "\t Xorp = " << _num_evts_after_cuts_xorp);
+
+ scale(_hist_dNch_all_dEta_OR, 1./_num_evts_after_cuts_or);
+ scale(_hist_dNch_all_dEta_AND, 1./_num_evts_after_cuts_and);
+ scale(_hist_dNch_all_dEta_XOR, 1./_num_evts_after_cuts_xor);
+ scale(_hist_dNch_all_dEta_XORpm, 1./(_num_evts_after_cuts_xorm + _num_evts_after_cuts_xorp));
+
+ scale(_hist_dNch_all_dpt_OR, 1./_num_evts_after_cuts_or);
+ scale(_hist_dNch_all_dpt_AND, 1./_num_evts_after_cuts_and);
+ scale(_hist_dNch_all_dpt_XOR, 1./_num_evts_after_cuts_xor);
+
+ scale(_hist_dNch_leading_dpt_OR, 1./_num_evts_after_cuts_or);
+ scale(_hist_dNch_leading_dpt_AND, 1./_num_evts_after_cuts_and);
+ scale(_hist_dNch_leading_dpt_XOR, 1./_num_evts_after_cuts_xor);
+
+ scale(_hist_integrated_leading_pt_OR, 1./_num_evts_after_cuts_or);
+ scale(_hist_integrated_leading_pt_AND, 1./_num_evts_after_cuts_and);
+ scale(_hist_integrated_leading_pt_XOR, 1./_num_evts_after_cuts_xor);
+
+ scale(_hist_dNev_all_dM_OR, 1./_num_evts_after_cuts_or);
+ scale(_hist_dNev_all_dM_AND, 1./_num_evts_after_cuts_and);
+ }
+
+
+ private:
+
+ // Cuts
+ double MinEnergy, EtaForwardMin, EtaForwardMax, EtaCentralCut, MinParticlePt;
+
+ // Counters
+ double _num_evts_noCuts,
+ _num_evts_after_cuts_and,
+ _num_evts_after_cuts_or,
+ _num_evts_after_cuts_xor,
+ _num_evts_after_cuts_xorp,
+ _num_evts_after_cuts_xorm;
+
+ // Histograms
+ Histo1DPtr
+ _hist_dNch_all_dEta_AND,
+ _hist_dNch_all_dEta_OR,
+ _hist_dNch_all_dEta_XOR,
+ _hist_dNch_all_dEta_XORpm;
+ Histo1DPtr
+ _hist_dNch_all_dpt_AND,
+ _hist_dNch_all_dpt_OR,
+ _hist_dNch_all_dpt_XOR;
+ Histo1DPtr
+ _hist_dNch_leading_dpt_AND,
+ _hist_dNch_leading_dpt_OR,
+ _hist_dNch_leading_dpt_XOR;
+ Histo1DPtr
+ _hist_integrated_leading_pt_AND,
+ _hist_integrated_leading_pt_OR,
+ _hist_integrated_leading_pt_XOR;
+ Histo1DPtr
+ _hist_dNev_all_dM_AND,
+ _hist_dNev_all_dM_OR;
+
+ };
+
+
+ DECLARE_RIVET_PLUGIN(CMS_2018_I1680318);
+
+}
diff --git a/analyses/pluginCMS/CMS_2018_I1680318.info b/analyses/pluginCMS/CMS_2018_I1680318.info
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1680318.info
@@ -0,0 +1,50 @@
+Name: CMS_2018_I1680318
+Year: 2018
+Summary: Charged particle distributions in different final states at 13~TeV
+Experiment: CMS collaboration
+Collider: LHC
+InspireID: 1680318
+Status: VALIDATED
+Authors:
+ - cms-pag-conveners-smp@cern.ch
+ - Juan Manuel Grados Luyando <juan.grados.luyando@desy.de>
+ - Pieters Maxim <Maxim.Pieters@uantwerpen.be>
+References:
+ - 'Eur.Phys.J. C78 (2018) no.9, 697'
+ - 'DOI: 10.1140/epjc/s10052-018-6144-y'
+ - 'arXiv:1806.11245 [hep-ex]'
+ - 'http://cms-results.web.cern.ch/cms-results/public-results/publications/FSQ-16-011/'
+RunInfo:
+ 'Inelastic events at 13~TeV centre of mass energy.
+ Tracks in $|\eta|<2.4$ and with $\pT > 0.5~GeV$'
+#NumEvents: 10000000
+NeedCrossSection: no
+Beams: [p+, p+]
+Energies: [13000]
+Description:
+ 'Charged particle distributions in different final states at $\sqrt{s} = 13$~TeV by the CMS experiment.
+ Pseudorapidity, multiplicity and transverse momentum distributions of all charged particles.
+ Also the $\pT$ leading charged particle spectrum and its integration as function of $\pT$.
+ The distributions are presented for inelastic, non-single-diffractive
+ and single-diffractive event selections.
+ Please note, that the MC predictions are not scaled to the datapoints,
+ in contrast to Figure 6 in the publication.'
+BibKey: Sirunyan:2018zdc
+BibTeX: '@article{Sirunyan:2018zdc,
+ author = "Sirunyan, Albert M. and others",
+ title = "{Measurement of charged particle spectra in minimum-bias
+ events from proton-proton collisions at
+ $\sqrt{s}=13\,\text {TeV} $}",
+ collaboration = "CMS",
+ journal = "Eur. Phys. J.",
+ volume = "C78",
+ year = "2018",
+ number = "9",
+ pages = "697",
+ doi = "10.1140/epjc/s10052-018-6144-y",
+ eprint = "1806.11245",
+ archivePrefix = "arXiv",
+ primaryClass = "hep-ex",
+ reportNumber = "CMS-FSQ-16-011, CERN-EP-2018-187",
+ SLACcitation = "%%CITATION = ARXIV:1806.11245;%%"
+}'
diff --git a/analyses/pluginCMS/CMS_2018_I1680318.plot b/analyses/pluginCMS/CMS_2018_I1680318.plot
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1680318.plot
@@ -0,0 +1,148 @@
+## General Settings ##
+#
+# BEGIN PLOT /CMS_2018_I1680318/*
+##LegendYPos=0.4
+##LegendXPos=0.5
+RatioPlotYMin=0.6
+RatioPlotYMax=1.4
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d01-*
+LogY=0
+LogX=0
+XLabel=$\eta$
+YLabel=$(1/N^{tot}_{events})dN_{ch}/d\eta$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d02-*
+LogY=1
+LogX=1
+XLabel=$p_{T} [GeV]$
+YLabel=$(1/N^{tot}_{events})dN_{ch}/dp_{T}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d03-*
+LogY=1
+LogX=1
+XLabel=leading $p_{T} [GeV]$
+YLabel=$(1/N^{tot}_{events})dN_{ch}/dp_{T,leading}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d04-*
+LogY=1
+LogX=1
+XLabel=$p_{T, min} [GeV]$
+YLabel=$D(p_{T, min})$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d05-*
+LogY=1
+LogX=0
+XLabel=$n_{ch}$
+YLabel=$(1/N^{tot}_{events})dN_{events}/dn_{ch}$
+# END PLOT
+
+
+
+## Titles ##
+#
+# BEGIN PLOT /CMS_2018_I1680318/d0[1-5]-x01-y01
+Title= CMS, 13 TeV, $pp$ Inelastic
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d0[1-5]-x02-y01
+Title= CMS, 13 TeV, $pp$ Non-Single Diffractive enhanced
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d0[1-4]-x03-y01
+Title= CMS, 13 TeV, $pp$ Single Diffractive enhanced
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d01-x04-y01
+Title= CMS, 13 TeV, $pp$ Single Diffractive enhanced (One-Side)
+# END PLOT
+
+
+
+
+## Individual Settings ##
+#
+## Eta ##
+# BEGIN PLOT /CMS_2018_I1680318/d01-x0[1-2]-y01
+YMax=5.
+YMin=0.
+RatioPlotYMin=0.6
+RatioPlotYMax=1.4
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d01-x0[3-4]-y01
+YMax=1.8
+YMin=0.15
+# END PLOT
+
+
+
+## Pt ##
+# BEGIN PLOT /CMS_2018_I1680318/d02-x01-y01
+YMax=100.
+YMin=0.000001
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d02-x02-y01
+YMax=100.
+YMin=0.000001
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d02-x03-y01
+YMax=100.
+YMin=0.0003
+# END PLOT
+
+
+
+## Pt leading ##
+# BEGIN PLOT /CMS_2018_I1680318/d03-x01-y01
+YMax=100.
+YMin=0.000001
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d03-x02-y01
+YMax=100.
+YMin=0.000001
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d03-x03-y01
+YMax=100.
+YMin=0.0003
+# END PLOT
+
+
+
+## Pt leading integrated ##
+# BEGIN PLOT /CMS_2018_I1680318/d04-x01-y01
+YMax=100.
+YMin=0.0005
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d04-x02-y01
+YMax=100.
+YMin=0.0005
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d04-x03-y01
+YMax=100.
+YMin=0.0003
+# END PLOT
+
+
+
+## M ##
+# BEGIN PLOT /CMS_2018_I1680318/d05-x01-y01
+YMax=10.
+YMin=0.0003
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1680318/d05-x02-y01
+YMax=10.
+YMin=0.0003
+# END PLOT
diff --git a/analyses/pluginCMS/CMS_2018_I1680318.yoda b/analyses/pluginCMS/CMS_2018_I1680318.yoda
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1680318.yoda
@@ -0,0 +1,422 @@
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d01-x01-y01
+Path=/REF/CMS_2018_I1680318/d01-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+-2.3 0.10000000000000009 0.09999999999999964 2.8373 0.12040365442958947 0.11391527553405645
+-2.1 0.10000000000000009 0.10000000000000009 2.9235 0.1241974234837422 0.1174088582688717
+-1.9 0.10000000000000009 0.09999999999999987 2.9391 0.1250017999870402 0.1180137703829515
+-1.7000000000000002 0.09999999999999987 0.10000000000000009 2.9845 0.12690441284683524 0.11981652640600127
+-1.5 0.10000000000000009 0.10000000000000009 3.0112 0.12790848290867968 0.12092055243009767
+-1.2999999999999998 0.10000000000000009 0.09999999999999987 3.0491 0.12920638529113027 0.12241785000562622
+-1.1 0.09999999999999987 0.10000000000000009 3.0137 0.12750345093369042 0.12101437931089015
+-0.9 0.09999999999999998 0.09999999999999998 2.9481 0.12450261041440054 0.11841304826749458
+-0.7 0.10000000000000009 0.09999999999999998 2.9514 0.12460244780902179 0.11851286849958531
+-0.5 0.09999999999999998 0.09999999999999998 2.955 0.12480212337937205 0.1186126890345211
+-0.30000000000000004 0.09999999999999998 0.10000000000000003 2.9439 0.12440277328098438 0.11821340871491694
+-0.1 0.1 0.1 2.9086 0.12289951179724028 0.11680993108464707
+0.1 0.1 0.1 2.9086 0.12289951179724028 0.11680993108464707
+0.30000000000000004 0.10000000000000003 0.09999999999999998 2.9439 0.12440277328098438 0.11821340871491694
+0.5 0.09999999999999998 0.09999999999999998 2.955 0.12480212337937205 0.1186126890345211
+0.7 0.09999999999999998 0.10000000000000009 2.9514 0.12460244780902179 0.11851286849958531
+0.9 0.09999999999999998 0.09999999999999998 2.9481 0.12450261041440054 0.11841304826749458
+1.1 0.10000000000000009 0.09999999999999987 3.0137 0.12750345093369042 0.12101437931089015
+1.2999999999999998 0.09999999999999987 0.10000000000000009 3.0491 0.12920638529113027 0.12241785000562622
+1.5 0.10000000000000009 0.10000000000000009 3.0112 0.12790848290867968 0.12092055243009767
+1.7000000000000002 0.10000000000000009 0.09999999999999987 2.9845 0.12690441284683524 0.11981652640600127
+1.9 0.09999999999999987 0.10000000000000009 2.9391 0.1250017999870402 0.1180137703829515
+2.1 0.10000000000000009 0.10000000000000009 2.9235 0.1241974234837422 0.1174088582688717
+2.3 0.09999999999999964 0.10000000000000009 2.8373 0.12040365442958947 0.11391527553405645
+# END YODA_SCATTER2D
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d01-x02-y01
+Path=/REF/CMS_2018_I1680318/d01-x02-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+-2.3 0.10000000000000009 0.09999999999999964 2.9798 0.13260109350981988 0.12231802810706197
+-2.1 0.10000000000000009 0.10000000000000009 3.0712 0.1367004389166326 0.12601745910785536
+-1.9 0.10000000000000009 0.09999999999999987 3.0881 0.13749927272534937 0.12671625783615928
+-1.7000000000000002 0.09999999999999987 0.10000000000000009 3.1375 0.13960701988080684 0.12882437657524293
+-1.5 0.10000000000000009 0.10000000000000009 3.165 0.14051113834853093 0.12992836487849757
+-1.2999999999999998 0.10000000000000009 0.09999999999999987 3.2058 0.14180920280433143 0.1316254154789264
+-1.1 0.09999999999999987 0.10000000000000009 3.1695 0.1398067237295832 0.13012213493483726
+-0.9 0.09999999999999998 0.09999999999999998 3.1005 0.13640634149481468 0.1273210901618424
+-0.7 0.10000000000000009 0.09999999999999998 3.1055 0.13660603939797097 0.12752074341063105
+-0.5 0.09999999999999998 0.09999999999999998 3.1095 0.13680573818374725 0.12772039774444802
+-0.30000000000000004 0.09999999999999998 0.10000000000000003 3.0977 0.13640634149481468 0.12722126394593006
+-0.1 0.1 0.1 3.0602 0.13480326405543747 0.12571797803019263
+0.1 0.1 0.1 3.0602 0.13480326405543747 0.12571797803019263
+0.30000000000000004 0.10000000000000003 0.09999999999999998 3.0977 0.13640634149481468 0.12722126394593006
+0.5 0.09999999999999998 0.09999999999999998 3.1095 0.13680573818374725 0.12772039774444802
+0.7 0.09999999999999998 0.10000000000000009 3.1055 0.13660603939797097 0.12752074341063105
+0.9 0.09999999999999998 0.09999999999999998 3.1005 0.13640634149481468 0.1273210901618424
+1.1 0.10000000000000009 0.09999999999999987 3.1695 0.1398067237295832 0.13012213493483726
+1.2999999999999998 0.09999999999999987 0.10000000000000009 3.2058 0.14180920280433143 0.1316254154789264
+1.5 0.10000000000000009 0.10000000000000009 3.165 0.14051113834853093 0.12992836487849757
+1.7000000000000002 0.10000000000000009 0.09999999999999987 3.1375 0.13960701988080684 0.12882437657524293
+1.9 0.09999999999999987 0.10000000000000009 3.0881 0.13749927272534937 0.12671625783615928
+2.1 0.10000000000000009 0.10000000000000009 3.0712 0.1367004389166326 0.12601745910785536
+2.3 0.09999999999999964 0.10000000000000009 2.9798 0.13260109350981988 0.12231802810706197
+# END YODA_SCATTER2D
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d01-x03-y01
+Path=/REF/CMS_2018_I1680318/d01-x03-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+-2.3 0.10000000000000009 0.09999999999999964 0.7119 0.05032941485850993 0.05301773288249885
+-2.1 0.10000000000000009 0.10000000000000009 0.7274 0.052402290026295616 0.05608894721778971
+-1.9 0.10000000000000009 0.09999999999999987 0.728 0.053389980333392144 0.058274007928063434
+-1.7000000000000002 0.09999999999999987 0.10000000000000009 0.7184 0.053489625162268614 0.06006879389500009
+-1.5 0.10000000000000009 0.10000000000000009 0.7289 0.05499272679182221 0.06356665792693525
+-1.2999999999999998 0.10000000000000009 0.09999999999999987 0.7302 0.05608083451590213 0.06625299993207856
+-1.1 0.09999999999999987 0.10000000000000009 0.7153 0.05616484665696151 0.06703804889762231
+-0.9 0.09999999999999998 0.09999999999999998 0.6938 0.05577382898815536 0.06684496989302935
+-0.7 0.10000000000000009 0.09999999999999998 0.6808 0.05577382898815536 0.06704453743594627
+-0.5 0.09999999999999998 0.09999999999999998 0.6813 0.056471674315536284 0.06804241324350571
+-0.30000000000000004 0.09999999999999998 0.10000000000000003 0.6775 0.05627228447468611 0.06824199586764737
+-0.1 0.1 0.1 0.6708 0.055766029085815315 0.06783642089615283
+0.1 0.1 0.1 0.6708 0.055766029085815315 0.06783642089615283
+0.30000000000000004 0.10000000000000003 0.09999999999999998 0.6775 0.05627228447468611 0.06824199586764737
+0.5 0.09999999999999998 0.09999999999999998 0.6813 0.056471674315536284 0.06814220424964253
+0.7 0.09999999999999998 0.10000000000000009 0.6808 0.05577382898815536 0.06704453743594627
+0.9 0.09999999999999998 0.09999999999999998 0.6938 0.05577382898815536 0.06684496989302935
+1.1 0.10000000000000009 0.09999999999999987 0.7153 0.05616484665696151 0.06703804889762231
+1.2999999999999998 0.09999999999999987 0.10000000000000009 0.7302 0.05608083451590213 0.06625299993207856
+1.5 0.10000000000000009 0.10000000000000009 0.7289 0.05499272679182221 0.06356665792693525
+1.7000000000000002 0.10000000000000009 0.09999999999999987 0.7184 0.053489625162268614 0.06006879389500009
+1.9 0.09999999999999987 0.10000000000000009 0.728 0.053389980333392144 0.058274007928063434
+2.1 0.10000000000000009 0.10000000000000009 0.7274 0.052402290026295616 0.05608894721778971
+2.3 0.09999999999999964 0.10000000000000009 0.7119 0.05032941485850993 0.05301773288249885
+# END YODA_SCATTER2D
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d01-x04-y01
+Path=/REF/CMS_2018_I1680318/d01-x04-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+-2.3 0.10000000000000009 0.09999999999999964 1.1853 0.07975587752636167 0.08422618357731756
+-2.1 0.10000000000000009 0.10000000000000009 1.1668 0.08018435009401771 0.08615062390952255
+-1.9 0.10000000000000009 0.09999999999999987 1.1297 0.07904758060813753 0.08710596994465994
+-1.7000000000000002 0.09999999999999987 0.10000000000000009 1.0687 0.07584457792090347 0.08639004572287248
+-1.5 0.10000000000000009 0.10000000000000009 1.0501 0.07544693499407382 0.08887907515270396
+-1.2999999999999998 0.10000000000000009 0.09999999999999987 1.0038 0.07301780604756623 0.08854422623751364
+-1.1 0.09999999999999987 0.10000000000000009 0.9534 0.07066774370248424 0.08709810560511635
+-0.9 0.09999999999999998 0.09999999999999998 0.8768 0.06656906188313007 0.08239787618622219
+-0.7 0.10000000000000009 0.09999999999999998 0.8153 0.06336592144047146 0.07849509538818333
+-0.5 0.09999999999999998 0.09999999999999998 0.7748 0.06155485358604957 0.07598716996967317
+-0.30000000000000004 0.09999999999999998 0.10000000000000003 0.737 0.059644362684163205 0.07328001091702975
+-0.1 0.1 0.1 0.6851 0.056419943282495416 0.06866265360441584
+0.1 0.1 0.1 0.6566 0.05511669438563964 0.06606398413659291
+0.30000000000000004 0.10000000000000003 0.09999999999999998 0.6186 0.05290793891279455 0.06226146480769626
+0.5 0.09999999999999998 0.09999999999999998 0.5885 0.051285085551259435 0.05914702021234882
+0.7 0.09999999999999998 0.10000000000000009 0.5484 0.04866795660390931 0.05483766953472768
+0.9 0.09999999999999998 0.09999999999999998 0.5156 0.04644868135910857 0.051125825176714754
+1.1 0.10000000000000009 0.09999999999999987 0.4852 0.044219452732931916 0.04740464112299554
+1.2999999999999998 0.09999999999999987 0.10000000000000009 0.4648 0.042837016702847085 0.04452796873876014
+1.5 0.10000000000000009 0.10000000000000009 0.4188 0.039324928480545265 0.0391260782599023
+1.7000000000000002 0.10000000000000009 0.09999999999999987 0.3789 0.03709514793069304 0.034708644456388674
+1.9 0.09999999999999987 0.10000000000000009 0.3408 0.035871158330893084 0.03129632566292727
+2.1 0.10000000000000009 0.10000000000000009 0.302 0.035245567097154214 0.028679086456859116
+2.3 0.09999999999999964 0.10000000000000009 0.2535 0.03313608305156178 0.025675864152935532
+# END YODA_SCATTER2D
+
+
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d02-x01-y01
+Path=/REF/CMS_2018_I1680318/d02-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+0.55 0.050000000000000044 0.04999999999999993 28.26676865 1.2672741914950716 1.2034327606316253
+0.7 0.09999999999999998 0.10000000000000009 19.51651113 0.8356492860193333 0.8065007988071112
+1.05 0.25 0.25 9.06552682 0.3813388670509556 0.36740955288472615
+1.4500000000000002 0.15000000000000013 0.1499999999999999 3.83949608 0.16852617818383497 0.15725296925301635
+1.95 0.34999999999999987 0.34999999999999987 1.62286931 0.0741674989348542 0.0655631159670321
+2.75 0.4500000000000002 0.4500000000000002 0.46519693 0.02167942965798916 0.01877452302819435
+3.85 0.6499999999999999 0.6499999999999999 0.11437308 0.005139841760959184 0.004614443015630381
+5.4 0.9000000000000004 0.8999999999999995 0.02352298 9.946388543587066E-4 9.547841452914894E-4
+7.65 1.3500000000000005 1.3499999999999996 0.00438519 1.8441405694794526E-4 1.8483639387306818E-4
+10.5 1.5 1.5 8.8352E-4 4.077248091544099E-5 4.4832025383647346E-5
+15.0 3.0 3.0 1.7185E-4 9.21588302877158E-6 1.0864492625060774E-5
+34.0 16.0 16.0 8.01E-6 6.762396025078685E-7 7.655063683601856E-7
+# END YODA_SCATTER2D
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d02-x02-y01
+Path=/REF/CMS_2018_I1680318/d02-x02-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+0.55 0.050000000000000044 0.04999999999999993 29.56954245 1.3822884453251219 1.2815764383777046
+0.7 0.09999999999999998 0.10000000000000009 20.45781851 0.9119724430199055 0.8618805147736702
+1.05 0.25 0.25 9.54482798 0.4151940403995859 0.3955391473324729
+1.4500000000000002 0.15000000000000013 0.1499999999999999 4.05561075 0.18191162315863382 0.17016126099885043
+1.95 0.34999999999999987 0.34999999999999987 1.71735614 0.07972952588079589 0.07133560406617162
+2.75 0.4500000000000002 0.4500000000000002 0.49357387 0.023544078369500898 0.020554122376331224
+3.85 0.6499999999999999 0.6499999999999999 0.12155757 0.005712713576094989 0.005079604584788072
+5.4 0.9000000000000004 0.8999999999999995 0.02505338 0.0011349696465104255 0.0010564878351405661
+7.65 1.3500000000000005 1.3499999999999996 0.00467869 2.1039579511007342E-4 2.069910611596549E-4
+10.5 1.5 1.5 9.4578E-4 4.5426420726268984E-5 5.01974152721034E-5
+15.0 3.0 3.0 1.8334E-4 1.009475606441285E-5 1.1942466244457214E-5
+34.0 16.0 16.0 8.57E-6 7.262231062146123E-7 8.237718130647588E-7
+# END YODA_SCATTER2D
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d02-x03-y01
+Path=/REF/CMS_2018_I1680318/d02-x03-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+0.55 0.050000000000000044 0.04999999999999993 9.16606139 0.6113024593397445 0.6944868982915421
+0.7 0.09999999999999998 0.10000000000000009 5.53586894 0.4266275297834177 0.5599304003378122
+1.05 0.25 0.25 1.91979084 0.17136807633807558 0.23480974502715088
+1.4500000000000002 0.15000000000000013 0.1499999999999999 0.55607454 0.05664920843443887 0.07441293891885538
+1.95 0.34999999999999987 0.34999999999999987 0.17418338 0.018983788239129194 0.023442140458245275
+2.75 0.4500000000000002 0.4500000000000002 0.03333793 0.003694030814882302 0.004335883432531368
+3.85 0.6499999999999999 0.6499999999999999 0.00645551 7.354895159687867E-4 8.391637280650303E-4
+5.4 0.9000000000000004 0.8999999999999995 0.00101259 1.387906282859185E-4 1.5407770020350121E-4
+# END YODA_SCATTER2D
+
+
+
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d03-x01-y01
+Path=/REF/CMS_2018_I1680318/d03-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+0.55 0.050000000000000044 0.04999999999999993 0.37041339 0.015989881281100873 0.02127889544359857
+0.7 0.09999999999999998 0.10000000000000009 0.48464371 0.020105707887863585 0.02753105974626658
+1.05 0.25 0.25 0.492215 0.01996790681581823 0.027241500117535743
+1.4500000000000002 0.15000000000000013 0.1499999999999999 0.40529761 0.016610413172037593 0.020794232763756876
+1.95 0.34999999999999987 0.34999999999999987 0.3035739 0.01227328786722205 0.013360114710574158
+2.75 0.4500000000000002 0.4500000000000002 0.17253044 0.006972972174933728 0.006968801590668226
+3.85 0.6499999999999999 0.6499999999999999 0.068625 0.002924279415514188 0.0027710415263037832
+5.4 0.9000000000000004 0.8999999999999995 0.01798014 8.149128214109776E-4 7.311030800783157E-4
+7.65 1.3500000000000005 1.3499999999999996 0.00365457 1.6612952807974865E-4 1.5381546931307009E-4
+10.5 1.5 1.5 7.5384E-4 3.5753268382065434E-5 3.6845766378242155E-5
+15.0 3.0 3.0 1.5006E-4 8.240400475705048E-6 9.04734767763459E-6
+34.0 16.0 16.0 7.19E-6 6.184658438426491E-7 6.989277502002621E-7
+# END YODA_SCATTER2D
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d03-x02-y01
+Path=/REF/CMS_2018_I1680318/d03-x02-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+0.55 0.050000000000000044 0.04999999999999993 0.29664025 0.015775449314859465 0.019538621830561643
+0.7 0.09999999999999998 0.10000000000000009 0.4233072 0.01956911802859291 0.025805969039619497
+1.05 0.25 0.25 0.47174089 0.019763561976690838 0.02646653794647309
+1.4500000000000002 0.15000000000000013 0.1499999999999999 0.41074324 0.016855930245139247 0.020565732020147012
+1.95 0.34999999999999987 0.34999999999999987 0.31605791 0.012830420894580972 0.013562992892426066
+2.75 0.4500000000000002 0.4500000000000002 0.18235953 0.007578342796746529 0.0075108335604312255
+3.85 0.6499999999999999 0.6499999999999999 0.07294307 0.0033557570660880686 0.0030331452211359747
+5.4 0.9000000000000004 0.8999999999999995 0.0191776 9.501342962971077E-4 8.058229200637073E-4
+7.65 1.3500000000000005 1.3499999999999996 0.0039065 1.927815618776858E-4 1.6966011493571494E-4
+10.5 1.5 1.5 8.0835E-4 4.0302362213646976E-5 4.051816012604718E-5
+15.0 3.0 3.0 1.6038E-4 9.00724708221108E-6 9.763042558547003E-6
+34.0 16.0 16.0 7.7E-6 6.684309986827361E-7 7.40607858451421E-7
+# END YODA_SCATTER2D
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d03-x03-y01
+Path=/REF/CMS_2018_I1680318/d03-x03-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+0.55 0.050000000000000044 0.04999999999999993 1.37053979 0.21830512682245096 0.0987324496130472
+0.7 0.09999999999999998 0.10000000000000009 1.3100567 0.08609415339439723 0.06443796273548148
+1.05 0.25 0.25 0.75655756 0.031269058426593214 0.04288746115464985
+1.4500000000000002 0.15000000000000013 0.1499999999999999 0.31477856 0.017912198278036674 0.03341319759102681
+1.95 0.34999999999999987 0.34999999999999987 0.11783005 0.009054469011361184 0.015301541921420862
+2.75 0.4500000000000002 0.4500000000000002 0.02657141 0.002492976345655931 0.003631278430195074
+3.85 0.6499999999999999 0.6499999999999999 0.0055175 6.034820246701637E-4 7.665638606795915E-4
+5.4 0.9000000000000004 0.8999999999999995 8.8334E-4 1.2329088287460675E-4 1.356387381982006E-4
+# END YODA_SCATTER2D
+
+
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d04-x01-y01
+Path=/REF/CMS_2018_I1680318/d04-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+0.55 0.050000000000000044 0.04999999999999993 1.00428195 0.040269813789985426 0.04648952454547261
+0.7 0.09999999999999998 0.10000000000000009 0.96724062 0.03878715392090531 0.04397006348089573
+1.05 0.25 0.25 0.87031187 0.03490622005055832 0.038168501307760304
+1.4500000000000002 0.15000000000000013 0.1499999999999999 0.62420437 0.02504608112578293 0.02598730877565047
+1.95 0.34999999999999987 0.34999999999999987 0.50261509 0.020233191052451416 0.020199214864219352
+2.75 0.4500000000000002 0.4500000000000002 0.29011336 0.011979766210147841 0.011650481718186593
+3.85 0.6499999999999999 0.6499999999999999 0.13483596 0.005841347649515478 0.005422844261833452
+5.4 0.9000000000000004 0.8999999999999995 0.04562347 0.0020022008805561944 0.0018452328186166645
+7.65 1.3500000000000005 1.3499999999999996 0.01325922 5.704682946492294E-4 5.556576594450939E-4
+10.5 1.5 1.5 0.00339189 1.5143606241579317E-4 1.6169069299127887E-4
+15.0 3.0 3.0 0.00113037 5.916921496859663E-5 6.696554711192913E-5
+34.0 16.0 16.0 2.3001E-4 1.9859103705857423E-5 2.200400190874378E-5
+# END YODA_SCATTER2D
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d04-x02-y01
+Path=/REF/CMS_2018_I1680318/d04-x02-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+0.55 0.050000000000000044 0.04999999999999993 1.0023098 0.04024792386510514 0.04492369997688637
+0.7 0.09999999999999998 0.10000000000000009 0.97264577 0.03900130998980547 0.04254128564069732
+1.05 0.25 0.25 0.88798433 0.03565365720071084 0.037580061605742475
+1.4500000000000002 0.15000000000000013 0.1499999999999999 0.65211389 0.02634937954166663 0.026695867053843747
+1.95 0.34999999999999987 0.34999999999999987 0.52889092 0.02174565368696237 0.02157480409285331
+2.75 0.4500000000000002 0.4500000000000002 0.30765038 0.013483335099050977 0.012660082292189099
+3.85 0.6499999999999999 0.6499999999999999 0.14352681 0.006761869847645694 0.005947498803740948
+5.4 0.9000000000000004 0.8999999999999995 0.04870082 0.002338958420857455 0.0020341414383960622
+7.65 1.3500000000000005 1.3499999999999996 0.01418114 6.580030943696238E-4 6.135490898860498E-4
+10.5 1.5 1.5 0.0036336 1.6901852975339716E-4 1.77591540620605E-4
+15.0 3.0 3.0 0.00120856 6.481913914886558E-5 7.243944022423145E-5
+34.0 16.0 16.0 2.4628E-4 2.1450561764205618E-5 2.3789043696626394E-5
+# END YODA_SCATTER2D
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d04-x03-y01
+Path=/REF/CMS_2018_I1680318/d04-x03-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+0.55 0.050000000000000044 0.04999999999999993 0.98739462 0.04014186023319049 0.04350373704674691
+0.7 0.09999999999999998 0.10000000000000009 0.85034064 0.03494181414541895 0.05400829305447544
+1.05 0.25 0.25 0.5883293 0.029335417718029857 0.054337628898369315
+1.4500000000000002 0.15000000000000013 0.1499999999999999 0.21005052 0.013876954351276076 0.024150685539657046
+1.95 0.34999999999999987 0.34999999999999987 0.11561695 0.009627548199889731 0.014752531893058222
+2.75 0.4500000000000002 0.4500000000000002 0.03313592 0.0032464547480135927 0.004459824987799409
+3.85 0.6499999999999999 0.6499999999999999 0.00922166 0.001039293364936003 0.0013100923488059918
+5.4 0.9000000000000004 0.8999999999999995 0.0020489 2.8788582406919584E-4 3.2604311156655345E-4
+# END YODA_SCATTER2D
+
+
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d05-x01-y01
+Path=/REF/CMS_2018_I1680318/d05-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.5 0.5 0.5 0.07824546 0.0031958960626716254 0.004507591581609851
+2.5 0.5 0.5 0.08827195 0.0037426584579012814 0.004825458879536742
+3.5 0.5 0.5 0.08278952 0.0033826238754109212 0.00409406795901094
+4.5 0.5 0.5 0.06965208 0.002833948712891608 0.0032529979404389417
+5.5 0.5 0.5 0.0558193 0.002275028006333109 0.002656646034476554
+6.5 0.5 0.5 0.05005993 0.002038137112193387 0.0024971299210293403
+7.5 0.5 0.5 0.04081031 0.0016746875320488893 0.0021320054916674114
+8.5 0.5 0.5 0.03515179 0.0014366723991571634 0.0018901660001439027
+9.5 0.5 0.5 0.03175887 0.0012917144471592782 0.001742549133711873
+10.5 0.5 0.5 0.02980017 0.0012199671439018346 0.001661234707107939
+11.5 0.5 0.5 0.02602138 0.001061426760638717 0.001446985606873821
+12.5 0.5 0.5 0.02427961 9.877601295861258E-4 0.0013271832735911042
+13.5 0.5 0.5 0.02346917 9.505400306141767E-4 0.001252663134685459
+14.5 0.5 0.5 0.02213922 8.957369415738082E-4 0.0011599881835605052
+15.5 0.5 0.5 0.02105518 8.527935180921581E-4 0.0010905119603654056
+16.5 0.5 0.5 0.01916391 7.731403511006265E-4 9.744966073311903E-4
+17.5 0.5 0.5 0.01824895 7.371561072798624E-4 9.043233953072318E-4
+18.5 0.5 0.5 0.01716126 6.942971834164387E-4 8.202227954037854E-4
+19.5 0.5 0.5 0.0163875 6.636500838544361E-4 7.507564384006307E-4
+20.5 0.5 0.5 0.01543813 6.252821914144045E-4 6.783646388926829E-4
+21.5 0.5 0.5 0.01442144 5.817886332681312E-4 6.089485404367105E-4
+22.5 0.5 0.5 0.01366029 5.515372543174215E-4 5.626764002515123E-4
+23.5 0.5 0.5 0.01294189 5.231059258888203E-4 5.288962606220619E-4
+24.5 0.5 0.5 0.01215537 4.935612198096605E-4 4.960669899318035E-4
+25.5 0.5 0.5 0.01139513 4.671033298960734E-4 4.638934063984958E-4
+26.5 0.5 0.5 0.01089734 4.4841004538257167E-4 4.4075546564960484E-4
+27.5 0.5 0.5 0.01035253 4.2844812766541524E-4 4.1848855587697976E-4
+28.5 0.5 0.5 0.00970073 4.0334243082026466E-4 3.9248260050606066E-4
+29.5 0.5 0.5 0.00914782 3.8208064201160466E-4 3.705709791659352E-4
+30.5 0.5 0.5 0.00857261 3.6165181058581743E-4 3.4768450138020245E-4
+31.5 0.5 0.5 0.00833451 3.5650688913399693E-4 3.369552767059747E-4
+32.5 0.5 0.5 0.0077616 3.3987486285396275E-4 3.1414446692564873E-4
+33.5 0.5 0.5 0.00728249 3.278873869181308E-4 2.9508721151551114E-4
+34.5 0.5 0.5 0.00683814 3.171266348006739E-4 2.7742106625128525E-4
+35.5 0.5 0.5 0.00642644 3.064020575975299E-4 2.6119750764507687E-4
+36.5 0.5 0.5 0.00618038 3.0034728865098816E-4 2.505227514618183E-4
+37.5 0.5 0.5 0.00575625 2.845572125250035E-4 2.3402901978173562E-4
+38.5 0.5 0.5 0.00537446 2.69028258924597E-4 2.1914038970486475E-4
+39.5 0.5 0.5 0.00507211 2.562123800677867E-4 2.0724427374477683E-4
+40.5 0.5 0.5 0.00471086 2.395706726625778E-4 1.9279575513999264E-4
+41.5 0.5 0.5 0.00454379 2.3185432409165887E-4 1.8513235157583882E-4
+42.5 0.5 0.5 0.00424957 2.1932541143241928E-4 1.7336597042095662E-4
+43.5 0.5 0.5 0.00394573 2.0719526828574052E-4 1.6129099323892825E-4
+44.5 0.5 0.5 0.00374147 2.0105043397118048E-4 1.535822532065473E-4
+45.5 0.5 0.5 0.00343771 1.9021946298946381E-4 1.4159845550005127E-4
+46.5 0.5 0.5 0.00328749 1.876784529454567E-4 1.3456195599053993E-4
+47.5 0.5 0.5 0.00305235 1.8126706319682018E-4 1.2504482796181536E-4
+48.5 0.5 0.5 0.00282641 1.7512763830989102E-4 1.1594512538265677E-4
+49.5 0.5 0.5 0.00264204 1.7055444467969753E-4 1.0847430386962619E-4
+50.5 0.5 0.5 0.00246332 1.6516995761941698E-4 1.0140328051892602E-4
+52.0 1.0 1.0 0.00224234 1.555625745479934E-4 9.199198334637643E-5
+54.0 1.0 1.0 0.00192206 1.3926740034911255E-4 7.932316496459278E-5
+56.0 1.0 1.0 0.00166475 1.277508387448004E-4 6.89656907454714E-5
+58.0 1.0 1.0 0.00144092 1.1865955545172078E-4 5.989631457777682E-5
+60.0 1.0 1.0 0.00122473 1.0857506896152541E-4 5.1464581995776476E-5
+62.0 1.0 1.0 0.00108437 1.018113834499856E-4 4.539868830704253E-5
+64.0 1.0 1.0 9.1698E-4 8.973160535730986E-5 3.886788134179686E-5
+66.0 1.0 1.0 8.0714E-4 8.119718344868866E-5 3.44670871992398E-5
+69.0 2.0 2.0 6.4392E-4 6.69727601342516E-5 2.7689077268843757E-5
+# END YODA_SCATTER2D
+
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1680318/d05-x02-y01
+Path=/REF/CMS_2018_I1680318/d05-x02-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.5 0.5 0.5 0.05895015 0.003059226043887571 0.003773159493064135
+2.5 0.5 0.5 0.07833396 0.003996802095788582 0.004627262006889172
+3.5 0.5 0.5 0.07879023 0.0037152749991487843 0.004149537931203907
+4.5 0.5 0.5 0.06647921 0.002917855503019298 0.0032896735998119934
+5.5 0.5 0.5 0.05556334 0.0023077390813088035 0.0027458207678215272
+6.5 0.5 0.5 0.05094401 0.002053704162848193 0.0026021826427251415
+7.5 0.5 0.5 0.04217759 0.0017043370818297652 0.00226684664082068
+8.5 0.5 0.5 0.03647094 0.0014815821003238397 0.002050953288619709
+9.5 0.5 0.5 0.03302295 0.0013488564984089303 0.001918267785477304
+10.5 0.5 0.5 0.031037 0.0012823163326184377 0.00182826718290845
+11.5 0.5 0.5 0.02733772 0.0011340730990549064 0.0015876914143812708
+12.5 0.5 0.5 0.02580791 0.001078384014440125 0.0014575579366186444
+13.5 0.5 0.5 0.02477004 0.0010356866053493209 0.0013596342768553609
+14.5 0.5 0.5 0.02366559 9.834796645076095E-4 0.0012763575405034438
+15.5 0.5 0.5 0.02217186 9.140452267256802E-4 0.0011856121482592863
+16.5 0.5 0.5 0.02040342 8.317746241019859E-4 0.0010772247984984376
+17.5 0.5 0.5 0.01937488 7.867216230026985E-4 9.982770754655243E-4
+18.5 0.5 0.5 0.01833743 7.436839802631223E-4 9.031183063696583E-4
+19.5 0.5 0.5 0.01737397 7.050384537030587E-4 8.04793033021534E-4
+20.5 0.5 0.5 0.01638479 6.662103890663969E-4 7.152731137824209E-4
+21.5 0.5 0.5 0.01529399 6.212827102857442E-4 6.418991058569875E-4
+22.5 0.5 0.5 0.01444041 5.905057541633274E-4 6.003513467961908E-4
+23.5 0.5 0.5 0.01372236 5.706650648147301E-4 5.692221338809656E-4
+24.5 0.5 0.5 0.01283181 5.456756674985609E-4 5.31451704390907E-4
+25.5 0.5 0.5 0.01224409 5.314063849823409E-4 5.061601889718313E-4
+26.5 0.5 0.5 0.01161479 5.102251507912953E-4 4.770651344418286E-4
+27.5 0.5 0.5 0.01095783 4.867856242741768E-4 4.49197614419311E-4
+28.5 0.5 0.5 0.01029935 4.616245999727484E-4 4.2206290822577623E-4
+29.5 0.5 0.5 0.00979014 4.4248608486595375E-4 4.014429436420573E-4
+30.5 0.5 0.5 0.00914331 4.172716435369171E-4 3.756824942687641E-4
+31.5 0.5 0.5 0.0088391 4.0775671300421286E-4 3.635802153583168E-4
+32.5 0.5 0.5 0.00836502 3.9431460155566134E-4 3.475524387772297E-4
+33.5 0.5 0.5 0.00774093 3.7618459949870356E-4 3.2637007368936264E-4
+34.5 0.5 0.5 0.00734641 3.700233242648361E-4 3.1414907862350956E-4
+35.5 0.5 0.5 0.0068472 3.5708538278680636E-4 2.953080779457277E-4
+36.5 0.5 0.5 0.0065852 3.523819463309663E-4 2.83293860152316E-4
+37.5 0.5 0.5 0.00612913 3.350975768339723E-4 2.6277446603503924E-4
+38.5 0.5 0.5 0.00572784 3.184484085373956E-4 2.443591655739559E-4
+39.5 0.5 0.5 0.00539994 3.0447557964473934E-4 2.2969684934713404E-4
+40.5 0.5 0.5 0.00500842 2.8608745306287023E-4 2.131381870993558E-4
+41.5 0.5 0.5 0.00484396 2.794476654044546E-4 2.0575069501705212E-4
+42.5 0.5 0.5 0.00451528 2.635101383248849E-4 1.9252610758024484E-4
+43.5 0.5 0.5 0.00418842 2.470128632278085E-4 1.790789328759807E-4
+44.5 0.5 0.5 0.00395923 2.3633141348538498E-4 1.695981948606765E-4
+45.5 0.5 0.5 0.00366031 2.226217249057243E-4 1.5725208424691866E-4
+46.5 0.5 0.5 0.00350778 2.1885646666251377E-4 1.503349689859282E-4
+47.5 0.5 0.5 0.0032475 2.1032998478581223E-4 1.3954447212268924E-4
+48.5 0.5 0.5 0.00303581 2.0531696909900068E-4 1.3051647137430586E-4
+49.5 0.5 0.5 0.00280553 1.983541239803196E-4 1.2044526101096713E-4
+50.5 0.5 0.5 0.00262443 1.9314962127842757E-4 1.122114864886835E-4
+52.0 1.0 1.0 0.00238542 1.814436907142268E-4 1.0089224846339781E-4
+54.0 1.0 1.0 0.00203063 1.6027453103971322E-4 8.585812599864965E-5
+56.0 1.0 1.0 0.00177859 1.4730806664945407E-4 7.529645941211312E-5
+58.0 1.0 1.0 0.0015359 1.3543968473087937E-4 6.529792186586032E-5
+60.0 1.0 1.0 0.00131202 1.2385817130896128E-4 5.661406274063009E-5
+62.0 1.0 1.0 0.00115186 1.1490422664114666E-4 4.991781746030168E-5
+64.0 1.0 1.0 9.7897E-4 1.0174249112342395E-4 4.330796924354685E-5
+66.0 1.0 1.0 8.6201E-4 9.202607728247467E-5 3.863490779075317E-5
+69.0 2.0 2.0 6.8621E-4 7.547362519450089E-5 3.10446452709642E-5
+# END YODA_SCATTER2D
diff --git a/analyses/pluginCMS/CMS_2018_I1682495.cc b/analyses/pluginCMS/CMS_2018_I1682495.cc
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1682495.cc
@@ -0,0 +1,157 @@
+// -*- C++ -*-
+#include "Rivet/Analysis.hh"
+#include "Rivet/Projections/FinalState.hh"
+#include "Rivet/Projections/VetoedFinalState.hh"
+#include "Rivet/Projections/FastJets.hh"
+#include "Rivet/Tools/fjcontrib/SoftDrop.hh"
+
+namespace Rivet {
+
+
+
+ // Soft-drop and ungroomed jet mass measurement
+ class CMS_2018_I1682495 : public Analysis {
+ public:
+
+ /// @name Constructors etc.
+ //@{
+
+ /// Constructor
+ CMS_2018_I1682495()
+ : Analysis("CMS_2018_I1682495"),
+ _softdrop(fjcontrib::SoftDrop(0, 0.1, 0.8) ) // parameters are beta, zcut, R0
+ { }
+
+ //@}
+
+
+ /// @name Analysis methods
+ //@{
+
+ /// Book histograms and initialise projections before the run
+ void init() {
+ // define a projection that keeps all the particles up to |eta|=5
+ const FinalState fs(Cuts::abseta < 5.);
+
+ // use FastJet, anti-kt(R=0.8) to do the clustering
+ addProjection(FastJets(fs, FastJets::ANTIKT, 0.8), "JetsAK8");
+
+ // Histograms
+ for (size_t i = 0; i < N_PT_BINS_dj; ++i ) {
+ _h_ungroomedJetMass_dj[i][0] = bookHisto1D(i+1+0*N_PT_BINS_dj, 1, 1); // Ungroomed mass, absolute
+ _h_sdJetMass_dj[i][0] = bookHisto1D(i+1+1*N_PT_BINS_dj, 1, 1); // Groomed mass, absolute
+ _h_ungroomedJetMass_dj[i][1] = bookHisto1D(i+1+2*N_PT_BINS_dj, 1, 1); // Ungroomed mass, normalized
+ _h_sdJetMass_dj[i][1] = bookHisto1D(i+1+3*N_PT_BINS_dj, 1, 1); // Groomed mass, normalized
+ }
+ }
+
+
+ // Find the pT histogram bin index for value pt (in GeV), to hack a 2D histogram equivalent
+ /// @todo Use a YODA axis/finder alg when available
+ size_t findPtBin(double ptJ) {
+ const double ptBins_dj[N_PT_BINS_dj+1] = { 200., 260., 350., 460., 550., 650., 760., 900, 1000, 1100, 1200, 1300, 13000};
+ for (size_t ibin = 0; ibin < N_PT_BINS_dj; ++ibin) {
+ if (inRange(ptJ, ptBins_dj[ibin], ptBins_dj[ibin+1])) return ibin;
+ }
+ return N_PT_BINS_dj;
+ }
+
+
+ /// Perform the per-event analysis
+ void analyze(const Event& event) {
+ const double weight = event.weight();
+
+ // Look at events with >= 2 jets
+ auto jetsAK8 = applyProjection<FastJets>(event, "JetsAK8").jetsByPt(Cuts::pT > 200*GeV and Cuts::abseta < 2.4);
+ if (jetsAK8.size() < 2) vetoEvent;
+
+ // Get the leading two jets
+ const fastjet::PseudoJet& j0 = jetsAK8[0].pseudojet();
+ const fastjet::PseudoJet& j1 = jetsAK8[1].pseudojet();
+
+ // Calculate delta phi and the pt asymmetry
+ double deltaPhi = Rivet::deltaPhi( j0.phi(), j1.phi() );
+ double ptasym = (j0.pt() - j1.pt()) / (j0.pt() + j1.pt());
+ if (deltaPhi < 2.0 ) vetoEvent;
+ if (ptasym > 0.3) vetoEvent;
+
+ // Find the appropriate pT bins and fill the histogram
+ const size_t njetBin0 = findPtBin(j0.pt()/GeV);
+ const size_t njetBin1 = findPtBin(j1.pt()/GeV);
+ if (njetBin0 < N_PT_BINS_dj && njetBin1 < N_PT_BINS_dj) {
+ for ( size_t jbin = 0; jbin < N_CATEGORIES; jbin++ ){
+ _h_ungroomedJetMass_dj[njetBin0][jbin]->fill(j0.m()/GeV, weight);
+ _h_ungroomedJetMass_dj[njetBin1][jbin]->fill(j1.m()/GeV, weight);
+ }
+ }
+
+ // Now run the substructure algs...
+ fastjet::PseudoJet sd0 = _softdrop(j0);
+ fastjet::PseudoJet sd1 = _softdrop(j1);
+ // ... and repeat
+ if (njetBin0 < N_PT_BINS_dj && njetBin1 < N_PT_BINS_dj) {
+ for ( size_t jbin = 0; jbin < N_CATEGORIES; jbin++ ){
+ _h_sdJetMass_dj[njetBin0][jbin]->fill(sd0.m()/GeV, weight);
+ _h_sdJetMass_dj[njetBin1][jbin]->fill(sd1.m()/GeV, weight);
+ }
+ }
+ }
+
+
+ /// Normalise histograms etc., after the run
+ void finalize() {
+ // Normalize the normalized cross section histograms to unity,
+ for (size_t i = 0; i < N_PT_BINS_dj; ++i) {
+ normalize(_h_ungroomedJetMass_dj[i][1]);
+ normalize(_h_sdJetMass_dj[i][1]);
+ }
+ // Normalize the absolute cross section histograms to xs * lumi.
+ for (size_t i = 0; i < N_PT_BINS_dj; ++i) {
+ scale(_h_ungroomedJetMass_dj[i][0], crossSection()/picobarn / sumOfWeights());
+ scale(_h_sdJetMass_dj[i][0], crossSection()/picobarn / sumOfWeights());
+ }
+ }
+ //@}
+
+
+ private:
+
+ /// @name FastJet grooming tools (configured in constructor init list)
+ //@{
+ const fjcontrib::SoftDrop _softdrop;
+ //@}
+
+
+ /// @name Histograms
+ //@{
+ enum { PT_200_260_dj=0,
+ PT_260_350_dj,
+ PT_350_460_dj,
+ PT_460_550_dj,
+ PT_550_650_dj,
+ PT_650_760_dj,
+ PT_760_900_dj,
+ PT_900_1000_dj,
+ PT_1000_1100_dj,
+ PT_1100_1200_dj,
+ PT_1200_1300_dj,
+ PT_1300_Inf_dj,
+ N_PT_BINS_dj } BINS_dj;
+ static const int N_CATEGORIES=2;
+
+ Histo1DPtr _h_ungroomedJet0pt, _h_ungroomedJet1pt;
+ Histo1DPtr _h_sdJet0pt, _h_sdJet1pt;
+ // Here, store both the absolute (index 0) and normalized (index 1) cross sections.
+ Histo1DPtr _h_ungroomedJetMass_dj[N_PT_BINS_dj][2];
+ Histo1DPtr _h_sdJetMass_dj[N_PT_BINS_dj][2];
+ //@}
+
+
+ };
+
+
+ // The hook for the plugin system
+ DECLARE_RIVET_PLUGIN(CMS_2018_I1682495);
+
+
+}
diff --git a/analyses/pluginCMS/CMS_2018_I1682495.info b/analyses/pluginCMS/CMS_2018_I1682495.info
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1682495.info
@@ -0,0 +1,42 @@
+Name: CMS_2018_I1682495
+Year: 2018
+Summary: Jet mass in dijet events in $pp$ collisions at 13~TeV
+Experiment: CMS
+Collider: LHC
+InspireID: 1682495
+Status: VALIDATED
+Authors:
+ - cms-pag-conveners-smp@cern.ch
+ - Salvatore Rappoccio <salvatore.rappoccio@cern.ch>
+References:
+ - JHEP 11 (2018) 113
+ - DOI 10.1007/JHEP11(2018)113
+ - hep-ex arXiv:1807.05974
+ - inspirehep 1682495
+ - http://cms-results.web.cern.ch/cms-results/public-results/publications/SMP-16-010/index.html
+RunInfo:
+ $pp$ QCD interactions at $\sqrt{s} = 13$ TeV. Data collected by CMS during the year 2015.
+Beams: [p+, p+]
+Energies: [13000]
+PtCuts: [200]
+NeedCrossSection: yes
+Description:
+ 'Measurements of the differential jet cross section are presented as a function
+ of jet mass in dijet events, in bins of jet transverse momentum, with and without
+ a jet grooming algorithm. The data have been recorded by the CMS Collaboration
+ in proton-proton collisions at the LHC at a center-of-mass energy of 13\TeV and
+ correspond to an integrated luminosity of 2.3\fbinv.
+ The absolute cross sections show slightly different jet
+ transverse momentum spectra in data and Monte Carlo event generators
+ for the settings used. Removing this transverse momentum dependence,
+ the normalized cross section for ungroomed jets is consistent with the
+ prediction from Monte Carlo event generators for masses below 30\% of
+ the transverse momentum. The normalized cross section for groomed jets
+ is measured with higher precision than the ungroomed cross
+ section. Semi-analytical calculations of the jet mass beyond leading
+ logarithmic accuracy are compared to data, as well as predictions at
+ leading order and next-to-leading order, which include parton
+ showering and hadronization. Overall, in the normalized cross section,
+ the theoretical predictions agree with the measured cross sections
+ within the uncertainties for masses from 10 to 30\% of the jet
+ transverse momentum.'
diff --git a/analyses/pluginCMS/CMS_2018_I1682495.plot b/analyses/pluginCMS/CMS_2018_I1682495.plot
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1682495.plot
@@ -0,0 +1,355 @@
+# BEGIN PLOT /CMS_2018_I1682495/d01-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($200 < p_T < 260$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d02-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($260 < p_T < 350$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d03-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($350 < p_T < 460$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d04-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($460 < p_T < 550$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d05-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($550 < p_T < 650$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d06-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($650 < p_T < 760$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d07-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($760 < p_T < 900$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d08-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($900 < p_T < 1000$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d09-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($1000 < p_T < 1100$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d10-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($1100 < p_T < 1200$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d11-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($1200 < p_T < 1300$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d12-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($p_T > 1300$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d13-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($200 < p_T < 260$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d14-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($260 < p_T < 350$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d15-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($350 < p_T < 460$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d16-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($460 < p_T < 550$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d17-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($550 < p_T < 650$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d18-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($650 < p_T < 760$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d19-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($760 < p_T < 900$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d20-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($900 < p_T < 1000$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d21-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($1000 < p_T < 1100$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d22-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($1100 < p_T < 1200$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d23-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($1200 < p_T < 1300$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d24-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($p_T > 1300$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+
+
+
+
+
+
+
+
+
+
+
+# BEGIN PLOT /CMS_2018_I1682495/d25-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($200 < p_T < 260$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d26-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($260 < p_T < 350$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d27-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($350 < p_T < 460$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d28-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($460 < p_T < 550$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d29-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($550 < p_T < 650$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d30-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($650 < p_T < 760$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d31-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($760 < p_T < 900$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d32-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($900 < p_T < 1000$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d33-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($1000 < p_T < 1100$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d34-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($1100 < p_T < 1200$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d35-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($1200 < p_T < 1300$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d36-x01-y01
+Title=CMS, 13 TeV, Ungroomed jet mass $m_u$ ($p_T > 1300$ GeV)
+XLabel=$m_u$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_u}$
+LogY=0
+# END PLOT
+
+
+
+
+
+
+
+
+
+
+# BEGIN PLOT /CMS_2018_I1682495/d37-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($200 < p_T < 260$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d38-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($260 < p_T < 350$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d39-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($350 < p_T < 460$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d40-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($460 < p_T < 550$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d41-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($550 < p_T < 650$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d42-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($650 < p_T < 760$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d43-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($760 < p_T < 900$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d44-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($900 < p_T < 1000$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d45-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($1000 < p_T < 1100$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d46-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($1100 < p_T < 1200$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d47-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($1200 < p_T < 1300$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1682495/d48-x01-y01
+Title=CMS, 13 TeV, Groomed jet mass $m_g$ ($p_T > 1300$ GeV)
+XLabel=$m_g$
+YLabel=$\frac{1}{d\sigma/dp_{T}}\frac{d^2\sigma}{dp_{T} dm_g}$
+LogY=0
+# END PLOT
diff --git a/analyses/pluginCMS/CMS_2018_I1682495.yoda b/analyses/pluginCMS/CMS_2018_I1682495.yoda
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1682495.yoda
@@ -0,0 +1,788 @@
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d01-x01-y01
+Path=/REF/CMS_2018_I1682495/d01-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 2.086000e+01 5.387430e+00 5.387430e+00
+5.000000e+01 1.000000e+01 1.000000e+01 2.558600e+01 6.608156e+00 6.608156e+00
+7.000000e+01 1.000000e+01 1.000000e+01 1.079000e+01 2.786643e+00 2.786643e+00
+9.000000e+01 1.000000e+01 1.000000e+01 3.916200e+00 4.255372e-01 4.255372e-01
+1.250000e+02 2.500000e+01 2.500000e+01 4.133500e-01 6.630631e-02 6.630631e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d02-x01-y01
+Path=/REF/CMS_2018_I1682495/d02-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 3.271300e+00 9.972403e-01 9.972403e-01
+5.000000e+01 1.000000e+01 1.000000e+01 5.649900e+00 1.722396e+00 1.722396e+00
+7.000000e+01 1.000000e+01 1.000000e+01 3.204200e+00 9.767949e-01 9.767949e-01
+9.000000e+01 1.000000e+01 1.000000e+01 1.568700e+00 1.867796e-01 1.867796e-01
+1.250000e+02 2.500000e+01 2.500000e+01 4.270800e-01 4.365237e-02 4.365237e-02
+1.750000e+02 2.500000e+01 2.500000e+01 8.339600e-03 2.469832e-03 2.469832e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d03-x01-y01
+Path=/REF/CMS_2018_I1682495/d03-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 3.495000e-01 1.178110e-01 1.178110e-01
+5.000000e+01 1.000000e+01 1.000000e+01 7.962600e-01 2.684033e-01 2.684033e-01
+7.000000e+01 1.000000e+01 1.000000e+01 6.065100e-01 2.044411e-01 2.044411e-01
+9.000000e+01 1.000000e+01 1.000000e+01 3.514300e-01 4.872207e-02 4.872207e-02
+1.250000e+02 2.500000e+01 2.500000e+01 1.551700e-01 1.206645e-02 1.206645e-02
+1.750000e+02 2.500000e+01 2.500000e+01 2.873100e-02 3.299335e-03 3.299335e-03
+2.250000e+02 2.500000e+01 2.500000e+01 7.464700e-04 2.591853e-04 2.591853e-04
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d04-x01-y01
+Path=/REF/CMS_2018_I1682495/d04-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 5.299400e-02 2.258068e-02 2.258068e-02
+5.000000e+01 1.000000e+01 1.000000e+01 1.499600e-01 6.389659e-02 6.389659e-02
+7.000000e+01 1.000000e+01 1.000000e+01 1.465000e-01 6.242441e-02 6.242441e-02
+9.000000e+01 1.000000e+01 1.000000e+01 9.410000e-02 1.324552e-02 1.324552e-02
+1.250000e+02 2.500000e+01 2.500000e+01 4.755800e-02 4.600930e-03 4.600930e-03
+1.750000e+02 2.500000e+01 2.500000e+01 1.810700e-02 1.155904e-03 1.155904e-03
+2.250000e+02 2.500000e+01 2.500000e+01 3.446100e-03 4.798954e-04 4.798954e-04
+2.750000e+02 2.500000e+01 2.500000e+01 1.051300e-04 3.651474e-05 3.651474e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d05-x01-y01
+Path=/REF/CMS_2018_I1682495/d05-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 1.175200e-02 4.132444e-03 4.132444e-03
+5.000000e+01 1.000000e+01 1.000000e+01 3.953400e-02 6.969234e-03 6.969234e-03
+7.000000e+01 1.000000e+01 1.000000e+01 4.689400e-02 8.266836e-03 8.266836e-03
+9.000000e+01 1.000000e+01 1.000000e+01 3.372900e-02 5.945959e-03 5.945959e-03
+1.250000e+02 2.500000e+01 2.500000e+01 1.778600e-02 2.256327e-03 2.256327e-03
+1.750000e+02 2.500000e+01 2.500000e+01 7.899800e-03 4.906774e-04 4.906774e-04
+2.250000e+02 2.500000e+01 2.500000e+01 3.073400e-03 2.518752e-04 2.518752e-04
+2.750000e+02 2.500000e+01 2.500000e+01 5.675100e-04 9.395261e-05 9.395261e-05
+3.250000e+02 2.500000e+01 2.500000e+01 2.404500e-05 9.162751e-06 9.162751e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d06-x01-y01
+Path=/REF/CMS_2018_I1682495/d06-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 2.670100e-03 1.151328e-03 1.151328e-03
+5.000000e+01 1.000000e+01 1.000000e+01 1.049200e-02 2.139017e-03 2.139017e-03
+7.000000e+01 1.000000e+01 1.000000e+01 1.484900e-02 3.027398e-03 3.027398e-03
+9.000000e+01 1.000000e+01 1.000000e+01 1.194200e-02 2.434644e-03 2.434644e-03
+1.250000e+02 2.500000e+01 2.500000e+01 6.585500e-03 9.276038e-04 9.276038e-04
+1.750000e+02 2.500000e+01 2.500000e+01 3.277100e-03 2.032801e-04 2.032801e-04
+2.250000e+02 2.500000e+01 2.500000e+01 1.600400e-03 1.047327e-04 1.047327e-04
+2.750000e+02 2.500000e+01 2.500000e+01 6.544500e-04 6.257664e-05 6.257664e-05
+3.250000e+02 2.500000e+01 2.500000e+01 1.212300e-04 2.444579e-05 2.444579e-05
+3.750000e+02 2.500000e+01 2.500000e+01 4.537700e-06 2.309659e-06 2.309659e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d07-x01-y01
+Path=/REF/CMS_2018_I1682495/d07-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 2.691900e-03 6.056330e-04 6.056330e-04
+7.000000e+01 1.000000e+01 1.000000e+01 4.365100e-03 9.820651e-04 9.820651e-04
+9.000000e+01 1.000000e+01 1.000000e+01 4.046500e-03 9.103748e-04 9.103748e-04
+1.250000e+02 2.500000e+01 2.500000e+01 2.416300e-03 3.397990e-04 3.397990e-04
+1.750000e+02 2.500000e+01 2.500000e+01 1.222000e-03 9.010093e-05 9.010093e-05
+2.250000e+02 2.500000e+01 2.500000e+01 6.787800e-04 4.320779e-05 4.320779e-05
+2.750000e+02 2.500000e+01 2.500000e+01 3.643400e-04 2.547397e-05 2.547397e-05
+3.250000e+02 2.500000e+01 2.500000e+01 1.659900e-04 1.724977e-05 1.724977e-05
+3.750000e+02 2.500000e+01 2.500000e+01 3.946000e-05 7.919477e-06 7.919477e-06
+4.250000e+02 2.500000e+01 2.500000e+01 2.140800e-06 1.179636e-06 1.179636e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d08-x01-y01
+Path=/REF/CMS_2018_I1682495/d08-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 7.535400e-04 1.944198e-04 1.944198e-04
+7.000000e+01 1.000000e+01 1.000000e+01 1.400300e-03 2.075915e-04 2.075915e-04
+9.000000e+01 1.000000e+01 1.000000e+01 1.488600e-03 2.206819e-04 2.206819e-04
+1.250000e+02 2.500000e+01 2.500000e+01 9.681100e-04 1.435229e-04 1.435229e-04
+1.750000e+02 2.500000e+01 2.500000e+01 4.919400e-04 4.789730e-05 4.789730e-05
+2.250000e+02 2.500000e+01 2.500000e+01 2.990600e-04 2.211283e-05 2.211283e-05
+2.750000e+02 2.500000e+01 2.500000e+01 1.682300e-04 1.321640e-05 1.321640e-05
+3.250000e+02 2.500000e+01 2.500000e+01 1.068100e-04 8.567957e-06 8.567957e-06
+3.750000e+02 2.500000e+01 2.500000e+01 5.462100e-05 6.482260e-06 6.482260e-06
+4.250000e+02 2.500000e+01 2.500000e+01 1.673300e-05 4.191255e-06 4.191255e-06
+4.750000e+02 2.500000e+01 2.500000e+01 1.065800e-06 5.427459e-07 5.427459e-07
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d09-x01-y01
+Path=/REF/CMS_2018_I1682495/d09-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 2.937600e-04 8.412267e-05 8.412267e-05
+7.000000e+01 1.000000e+01 1.000000e+01 5.833000e-04 9.265646e-05 9.265646e-05
+9.000000e+01 1.000000e+01 1.000000e+01 6.808800e-04 1.081624e-04 1.081624e-04
+1.250000e+02 2.500000e+01 2.500000e+01 4.746900e-04 7.540449e-05 7.540449e-05
+1.750000e+02 2.500000e+01 2.500000e+01 2.433000e-04 2.845034e-05 2.845034e-05
+2.250000e+02 2.500000e+01 2.500000e+01 1.602100e-04 1.276913e-05 1.276913e-05
+2.750000e+02 2.500000e+01 2.500000e+01 9.057000e-05 8.357574e-06 8.357574e-06
+3.250000e+02 2.500000e+01 2.500000e+01 6.038700e-05 5.801216e-06 5.801216e-06
+3.750000e+02 2.500000e+01 2.500000e+01 3.804000e-05 4.392958e-06 4.392958e-06
+4.250000e+02 2.500000e+01 2.500000e+01 1.921000e-05 4.313171e-06 4.313171e-06
+4.750000e+02 2.500000e+01 2.500000e+01 4.379200e-06 1.386512e-06 1.386512e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d10-x01-y01
+Path=/REF/CMS_2018_I1682495/d10-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 1.222100e-04 3.560744e-05 3.560744e-05
+7.000000e+01 1.000000e+01 1.000000e+01 2.636800e-04 4.483958e-05 4.483958e-05
+9.000000e+01 1.000000e+01 1.000000e+01 3.297900e-04 5.479976e-05 5.479976e-05
+1.250000e+02 2.500000e+01 2.500000e+01 2.440900e-04 4.055943e-05 4.055943e-05
+1.750000e+02 2.500000e+01 2.500000e+01 1.303500e-04 1.764780e-05 1.764780e-05
+2.250000e+02 2.500000e+01 2.500000e+01 8.632600e-05 7.715155e-06 7.715155e-06
+2.750000e+02 2.500000e+01 2.500000e+01 5.030900e-05 5.147269e-06 5.147269e-06
+3.250000e+02 2.500000e+01 2.500000e+01 3.310300e-05 3.743140e-06 3.743140e-06
+3.750000e+02 2.500000e+01 2.500000e+01 2.332900e-05 2.871196e-06 2.871196e-06
+4.250000e+02 2.500000e+01 2.500000e+01 1.340300e-05 2.213058e-06 2.213058e-06
+4.750000e+02 2.500000e+01 2.500000e+01 6.512900e-06 1.393905e-06 1.393905e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d11-x01-y01
+Path=/REF/CMS_2018_I1682495/d11-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 5.202200e-05 1.745849e-05 1.745849e-05
+7.000000e+01 1.000000e+01 1.000000e+01 1.197500e-04 2.464028e-05 2.464028e-05
+9.000000e+01 1.000000e+01 1.000000e+01 1.645600e-04 3.094150e-05 3.094150e-05
+1.250000e+02 2.500000e+01 2.500000e+01 1.323900e-04 2.489322e-05 2.489322e-05
+1.750000e+02 2.500000e+01 2.500000e+01 7.286900e-05 1.085102e-05 1.085102e-05
+2.250000e+02 2.500000e+01 2.500000e+01 4.780700e-05 5.055438e-06 5.055438e-06
+2.750000e+02 2.500000e+01 2.500000e+01 2.920600e-05 3.273494e-06 3.273494e-06
+3.250000e+02 2.500000e+01 2.500000e+01 1.947200e-05 2.479702e-06 2.479702e-06
+3.750000e+02 2.500000e+01 2.500000e+01 1.305800e-05 2.124325e-06 2.124325e-06
+4.250000e+02 2.500000e+01 2.500000e+01 9.388800e-06 1.693595e-06 1.693595e-06
+4.750000e+02 2.500000e+01 2.500000e+01 6.086500e-06 1.476854e-06 1.476854e-06
+5.250000e+02 2.500000e+01 2.500000e+01 3.037100e-06 9.191100e-07 9.191100e-07
+5.750000e+02 2.500000e+01 2.500000e+01 8.503600e-07 5.019803e-07 5.019803e-07
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d12-x01-y01
+Path=/REF/CMS_2018_I1682495/d12-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 4.276600e-07 1.444594e-07 1.444594e-07
+7.000000e+01 1.000000e+01 1.000000e+01 1.069000e-06 2.308217e-07 2.308217e-07
+9.000000e+01 1.000000e+01 1.000000e+01 1.590700e-06 3.111016e-07 3.111016e-07
+1.250000e+02 2.500000e+01 2.500000e+01 1.458700e-06 2.852895e-07 2.852895e-07
+1.750000e+02 2.500000e+01 2.500000e+01 8.449300e-07 1.417248e-07 1.417248e-07
+2.250000e+02 2.500000e+01 2.500000e+01 5.230500e-07 5.898276e-08 5.898276e-08
+2.750000e+02 2.500000e+01 2.500000e+01 3.798500e-07 3.693493e-08 3.693493e-08
+3.250000e+02 2.500000e+01 2.500000e+01 2.818800e-07 3.296581e-08 3.296581e-08
+3.750000e+02 2.500000e+01 2.500000e+01 1.758800e-07 2.219854e-08 2.219854e-08
+4.250000e+02 2.500000e+01 2.500000e+01 1.183700e-07 1.692053e-08 1.692053e-08
+4.750000e+02 2.500000e+01 2.500000e+01 8.876300e-08 1.259098e-08 1.259098e-08
+5.250000e+02 2.500000e+01 2.500000e+01 7.378200e-08 1.272547e-08 1.272547e-08
+5.750000e+02 2.500000e+01 2.500000e+01 3.436900e-08 7.185395e-09 7.185395e-09
+6.250000e+02 2.500000e+01 2.500000e+01 1.762300e-08 5.516278e-09 5.516278e-09
+6.750000e+02 2.500000e+01 2.500000e+01 4.677600e-09 2.315304e-09 2.315304e-09
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d13-x01-y01
+Path=/REF/CMS_2018_I1682495/d13-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.981300e+01 2.280200e+00 2.280200e+00
+3.000000e+01 1.000000e+01 1.000000e+01 1.159000e+01 1.164389e+00 1.164389e+00
+5.000000e+01 1.000000e+01 1.000000e+01 8.547000e+00 9.118576e-01 9.118576e-01
+7.000000e+01 1.000000e+01 1.000000e+01 6.353700e+00 6.598104e-01 6.598104e-01
+9.000000e+01 1.000000e+01 1.000000e+01 3.331700e+00 3.695806e-01 3.695806e-01
+1.250000e+02 2.500000e+01 2.500000e+01 4.293500e-01 6.960729e-02 6.960729e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d14-x01-y01
+Path=/REF/CMS_2018_I1682495/d14-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 4.467800e+00 4.436926e-01 4.436926e-01
+3.000000e+01 1.000000e+01 1.000000e+01 2.450500e+00 1.802410e-01 1.802410e-01
+5.000000e+01 1.000000e+01 1.000000e+01 1.636100e+00 1.323063e-01 1.323063e-01
+7.000000e+01 1.000000e+01 1.000000e+01 1.339600e+00 1.215305e-01 1.215305e-01
+9.000000e+01 1.000000e+01 1.000000e+01 1.051000e+00 9.555276e-02 9.555276e-02
+1.250000e+02 2.500000e+01 2.500000e+01 3.979200e-01 3.990050e-02 3.990050e-02
+1.750000e+02 2.500000e+01 2.500000e+01 1.171900e-02 3.206833e-03 3.206833e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d15-x01-y01
+Path=/REF/CMS_2018_I1682495/d15-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 7.277200e-01 6.351976e-02 6.351976e-02
+3.000000e+01 1.000000e+01 1.000000e+01 3.784400e-01 2.270016e-02 2.270016e-02
+5.000000e+01 1.000000e+01 1.000000e+01 2.488800e-01 1.594560e-02 1.594560e-02
+7.000000e+01 1.000000e+01 1.000000e+01 1.982300e-01 1.283625e-02 1.283625e-02
+9.000000e+01 1.000000e+01 1.000000e+01 1.680400e-01 1.201418e-02 1.201418e-02
+1.250000e+02 2.500000e+01 2.500000e+01 1.129600e-01 7.660373e-03 7.660373e-03
+1.750000e+02 2.500000e+01 2.500000e+01 3.059200e-02 3.386705e-03 3.386705e-03
+2.250000e+02 2.500000e+01 2.500000e+01 9.820800e-04 3.324113e-04 3.324113e-04
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d16-x01-y01
+Path=/REF/CMS_2018_I1682495/d16-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.706500e-01 1.178079e-02 1.178079e-02
+3.000000e+01 1.000000e+01 1.000000e+01 8.193000e-02 4.570001e-03 4.570001e-03
+5.000000e+01 1.000000e+01 1.000000e+01 5.369500e-02 2.961712e-03 2.961712e-03
+7.000000e+01 1.000000e+01 1.000000e+01 4.185900e-02 2.398887e-03 2.398887e-03
+9.000000e+01 1.000000e+01 1.000000e+01 3.545200e-02 1.892967e-03 1.892967e-03
+1.250000e+02 2.500000e+01 2.500000e+01 2.749200e-02 1.703744e-03 1.703744e-03
+1.750000e+02 2.500000e+01 2.500000e+01 1.574800e-02 1.031341e-03 1.031341e-03
+2.250000e+02 2.500000e+01 2.500000e+01 3.655000e-03 5.034778e-04 5.034778e-04
+2.750000e+02 2.500000e+01 2.500000e+01 1.283600e-04 4.127190e-05 4.127190e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d17-x01-y01
+Path=/REF/CMS_2018_I1682495/d17-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 5.575900e-02 3.678882e-03 3.678882e-03
+3.000000e+01 1.000000e+01 1.000000e+01 2.599500e-02 1.445305e-03 1.445305e-03
+5.000000e+01 1.000000e+01 1.000000e+01 1.656800e-02 9.651798e-04 9.651798e-04
+7.000000e+01 1.000000e+01 1.000000e+01 1.315100e-02 7.266766e-04 7.266766e-04
+9.000000e+01 1.000000e+01 1.000000e+01 1.121600e-02 6.272762e-04 6.272762e-04
+1.250000e+02 2.500000e+01 2.500000e+01 8.420800e-03 5.093614e-04 5.093614e-04
+1.750000e+02 2.500000e+01 2.500000e+01 6.051800e-03 4.042247e-04 4.042247e-04
+2.250000e+02 2.500000e+01 2.500000e+01 2.919100e-03 2.278523e-04 2.278523e-04
+2.750000e+02 2.500000e+01 2.500000e+01 6.007000e-04 9.508619e-05 9.508619e-05
+3.250000e+02 2.500000e+01 2.500000e+01 3.063200e-05 1.104201e-05 1.104201e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d18-x01-y01
+Path=/REF/CMS_2018_I1682495/d18-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.911200e-02 1.319387e-03 1.319387e-03
+3.000000e+01 1.000000e+01 1.000000e+01 8.933500e-03 5.454529e-04 5.454529e-04
+5.000000e+01 1.000000e+01 1.000000e+01 5.435600e-03 3.695256e-04 3.695256e-04
+7.000000e+01 1.000000e+01 1.000000e+01 4.174600e-03 2.282106e-04 2.282106e-04
+9.000000e+01 1.000000e+01 1.000000e+01 3.519100e-03 2.052986e-04 2.052986e-04
+1.250000e+02 2.500000e+01 2.500000e+01 2.601100e-03 1.477562e-04 1.477562e-04
+1.750000e+02 2.500000e+01 2.500000e+01 2.104600e-03 1.265042e-04 1.265042e-04
+2.250000e+02 2.500000e+01 2.500000e+01 1.385900e-03 9.186474e-05 9.186474e-05
+2.750000e+02 2.500000e+01 2.500000e+01 6.418400e-04 5.517145e-05 5.517145e-05
+3.250000e+02 2.500000e+01 2.500000e+01 1.260300e-04 2.506718e-05 2.506718e-05
+3.750000e+02 2.500000e+01 2.500000e+01 4.627600e-06 2.614630e-06 2.614630e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d19-x01-y01
+Path=/REF/CMS_2018_I1682495/d19-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 6.447600e-03 5.307046e-04 5.307046e-04
+3.000000e+01 1.000000e+01 1.000000e+01 2.955000e-03 1.911001e-04 1.911001e-04
+5.000000e+01 1.000000e+01 1.000000e+01 1.733900e-03 1.133157e-04 1.133157e-04
+7.000000e+01 1.000000e+01 1.000000e+01 1.363200e-03 8.489869e-05 8.489869e-05
+9.000000e+01 1.000000e+01 1.000000e+01 1.127900e-03 6.850011e-05 6.850011e-05
+1.250000e+02 2.500000e+01 2.500000e+01 8.248000e-04 5.591012e-05 5.591012e-05
+1.750000e+02 2.500000e+01 2.500000e+01 6.574500e-04 3.899583e-05 3.899583e-05
+2.250000e+02 2.500000e+01 2.500000e+01 5.122700e-04 3.485670e-05 3.485670e-05
+2.750000e+02 2.500000e+01 2.500000e+01 3.332500e-04 2.532030e-05 2.532030e-05
+3.250000e+02 2.500000e+01 2.500000e+01 1.600600e-04 1.815150e-05 1.815150e-05
+3.750000e+02 2.500000e+01 2.500000e+01 4.000600e-05 7.501004e-06 7.501004e-06
+4.250000e+02 2.500000e+01 2.500000e+01 2.243000e-06 1.145130e-06 1.145130e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d20-x01-y01
+Path=/REF/CMS_2018_I1682495/d20-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 2.365300e-03 2.855890e-04 2.855890e-04
+3.000000e+01 1.000000e+01 1.000000e+01 1.105700e-03 9.007958e-05 9.007958e-05
+5.000000e+01 1.000000e+01 1.000000e+01 6.443400e-04 4.286794e-05 4.286794e-05
+7.000000e+01 1.000000e+01 1.000000e+01 4.710600e-04 3.266194e-05 3.266194e-05
+9.000000e+01 1.000000e+01 1.000000e+01 3.900900e-04 2.814234e-05 2.814234e-05
+1.250000e+02 2.500000e+01 2.500000e+01 2.950400e-04 1.970259e-05 1.970259e-05
+1.750000e+02 2.500000e+01 2.500000e+01 2.261000e-04 1.674464e-05 1.674464e-05
+2.250000e+02 2.500000e+01 2.500000e+01 1.919200e-04 1.650371e-05 1.650371e-05
+2.750000e+02 2.500000e+01 2.500000e+01 1.363000e-04 1.111324e-05 1.111324e-05
+3.250000e+02 2.500000e+01 2.500000e+01 1.003000e-04 7.960126e-06 7.960126e-06
+3.750000e+02 2.500000e+01 2.500000e+01 5.275500e-05 6.396633e-06 6.396633e-06
+4.250000e+02 2.500000e+01 2.500000e+01 1.669300e-05 3.840080e-06 3.840080e-06
+4.750000e+02 2.500000e+01 2.500000e+01 1.088000e-06 5.352590e-07 5.352590e-07
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d21-x01-y01
+Path=/REF/CMS_2018_I1682495/d21-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.089800e-03 1.233556e-04 1.233556e-04
+3.000000e+01 1.000000e+01 1.000000e+01 5.234200e-04 4.908558e-05 4.908558e-05
+5.000000e+01 1.000000e+01 1.000000e+01 2.972700e-04 2.721409e-05 2.721409e-05
+7.000000e+01 1.000000e+01 1.000000e+01 2.270100e-04 2.208271e-05 2.208271e-05
+9.000000e+01 1.000000e+01 1.000000e+01 1.874800e-04 1.462695e-05 1.462695e-05
+1.250000e+02 2.500000e+01 2.500000e+01 1.362300e-04 1.007142e-05 1.007142e-05
+1.750000e+02 2.500000e+01 2.500000e+01 1.033500e-04 8.263328e-06 8.263328e-06
+2.250000e+02 2.500000e+01 2.500000e+01 9.001100e-05 8.176565e-06 8.176565e-06
+2.750000e+02 2.500000e+01 2.500000e+01 6.752500e-05 6.495363e-06 6.495363e-06
+3.250000e+02 2.500000e+01 2.500000e+01 5.550700e-05 5.309619e-06 5.309619e-06
+3.750000e+02 2.500000e+01 2.500000e+01 3.767500e-05 4.489609e-06 4.489609e-06
+4.250000e+02 2.500000e+01 2.500000e+01 1.804600e-05 4.021493e-06 4.021493e-06
+4.750000e+02 2.500000e+01 2.500000e+01 4.509800e-06 1.389365e-06 1.389365e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d22-x01-y01
+Path=/REF/CMS_2018_I1682495/d22-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 5.293000e-04 5.626387e-05 5.626387e-05
+3.000000e+01 1.000000e+01 1.000000e+01 2.743200e-04 3.407331e-05 3.407331e-05
+5.000000e+01 1.000000e+01 1.000000e+01 1.359800e-04 1.492723e-05 1.492723e-05
+7.000000e+01 1.000000e+01 1.000000e+01 1.038100e-04 1.063401e-05 1.063401e-05
+9.000000e+01 1.000000e+01 1.000000e+01 9.568300e-05 9.051511e-06 9.051511e-06
+1.250000e+02 2.500000e+01 2.500000e+01 7.710500e-05 6.369358e-06 6.369358e-06
+1.750000e+02 2.500000e+01 2.500000e+01 5.118200e-05 4.760742e-06 4.760742e-06
+2.250000e+02 2.500000e+01 2.500000e+01 4.322300e-05 4.410448e-06 4.410448e-06
+2.750000e+02 2.500000e+01 2.500000e+01 3.532800e-05 3.998347e-06 3.998347e-06
+3.250000e+02 2.500000e+01 2.500000e+01 2.638600e-05 3.275007e-06 3.275007e-06
+3.750000e+02 2.500000e+01 2.500000e+01 2.271000e-05 2.935752e-06 2.935752e-06
+4.250000e+02 2.500000e+01 2.500000e+01 1.204700e-05 1.961648e-06 1.961648e-06
+4.750000e+02 2.500000e+01 2.500000e+01 6.314400e-06 1.342186e-06 1.342186e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d23-x01-y01
+Path=/REF/CMS_2018_I1682495/d23-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 2.607200e-04 3.490080e-05 3.490080e-05
+3.000000e+01 1.000000e+01 1.000000e+01 1.542300e-04 1.910506e-05 1.910506e-05
+5.000000e+01 1.000000e+01 1.000000e+01 7.440100e-05 8.724695e-06 8.724695e-06
+7.000000e+01 1.000000e+01 1.000000e+01 5.682000e-05 6.060397e-06 6.060397e-06
+9.000000e+01 1.000000e+01 1.000000e+01 5.106500e-05 6.178196e-06 6.178196e-06
+1.250000e+02 2.500000e+01 2.500000e+01 3.686200e-05 4.329497e-06 4.329497e-06
+1.750000e+02 2.500000e+01 2.500000e+01 2.701500e-05 3.326312e-06 3.326312e-06
+2.250000e+02 2.500000e+01 2.500000e+01 2.035300e-05 2.696309e-06 2.696309e-06
+2.750000e+02 2.500000e+01 2.500000e+01 2.018900e-05 2.707034e-06 2.707034e-06
+3.250000e+02 2.500000e+01 2.500000e+01 1.434400e-05 1.999368e-06 1.999368e-06
+3.750000e+02 2.500000e+01 2.500000e+01 1.102900e-05 1.929411e-06 1.929411e-06
+4.250000e+02 2.500000e+01 2.500000e+01 9.210900e-06 1.658619e-06 1.658619e-06
+4.750000e+02 2.500000e+01 2.500000e+01 5.715800e-06 1.427013e-06 1.427013e-06
+5.250000e+02 2.500000e+01 2.500000e+01 3.106300e-06 8.996972e-07 8.996972e-07
+5.750000e+02 2.500000e+01 2.500000e+01 9.943200e-07 5.846897e-07 5.846897e-07
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d24-x01-y01
+Path=/REF/CMS_2018_I1682495/d24-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 2.781900e-06 3.324993e-07 3.324993e-07
+3.000000e+01 1.000000e+01 1.000000e+01 1.760700e-06 2.885316e-07 2.885316e-07
+5.000000e+01 1.000000e+01 1.000000e+01 8.093200e-07 1.210751e-07 1.210751e-07
+7.000000e+01 1.000000e+01 1.000000e+01 5.575900e-07 7.694582e-08 7.694582e-08
+9.000000e+01 1.000000e+01 1.000000e+01 4.813200e-07 5.577909e-08 5.577909e-08
+1.250000e+02 2.500000e+01 2.500000e+01 3.606600e-07 3.657467e-08 3.657467e-08
+1.750000e+02 2.500000e+01 2.500000e+01 2.570300e-07 2.893861e-08 2.893861e-08
+2.250000e+02 2.500000e+01 2.500000e+01 2.191700e-07 2.389313e-08 2.389313e-08
+2.750000e+02 2.500000e+01 2.500000e+01 1.845000e-07 2.106926e-08 2.106926e-08
+3.250000e+02 2.500000e+01 2.500000e+01 1.868400e-07 2.215946e-08 2.215946e-08
+3.750000e+02 2.500000e+01 2.500000e+01 1.353900e-07 1.885486e-08 1.885486e-08
+4.250000e+02 2.500000e+01 2.500000e+01 9.020500e-08 1.382030e-08 1.382030e-08
+4.750000e+02 2.500000e+01 2.500000e+01 9.087400e-08 1.144201e-08 1.144201e-08
+5.250000e+02 2.500000e+01 2.500000e+01 6.476800e-08 1.268326e-08 1.268326e-08
+5.750000e+02 2.500000e+01 2.500000e+01 2.724000e-08 6.375330e-09 6.375330e-09
+6.250000e+02 2.500000e+01 2.500000e+01 1.631700e-08 4.643502e-09 4.643502e-09
+6.750000e+02 2.500000e+01 2.500000e+01 6.055800e-09 2.879351e-09 2.879351e-09
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d25-x01-y01
+Path=/REF/CMS_2018_I1682495/d25-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 1.640600e-02 3.726120e-03 3.726120e-03
+5.000000e+01 1.000000e+01 1.000000e+01 2.012300e-02 4.570356e-03 4.570356e-03
+7.000000e+01 1.000000e+01 1.000000e+01 8.485600e-03 1.927294e-03 1.927294e-03
+9.000000e+01 1.000000e+01 1.000000e+01 3.079900e-03 3.470363e-04 3.470363e-04
+1.250000e+02 2.500000e+01 2.500000e+01 3.250800e-04 6.075231e-05 6.075231e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d26-x01-y01
+Path=/REF/CMS_2018_I1682495/d26-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 1.093800e-02 3.161346e-03 3.161346e-03
+5.000000e+01 1.000000e+01 1.000000e+01 1.889100e-02 5.459970e-03 5.459970e-03
+7.000000e+01 1.000000e+01 1.000000e+01 1.071400e-02 3.096492e-03 3.096492e-03
+9.000000e+01 1.000000e+01 1.000000e+01 5.245100e-03 5.083709e-04 5.083709e-04
+1.250000e+02 2.500000e+01 2.500000e+01 1.428000e-03 1.051018e-04 1.051018e-04
+1.750000e+02 2.500000e+01 2.500000e+01 2.788400e-05 7.960878e-06 7.960878e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d27-x01-y01
+Path=/REF/CMS_2018_I1682495/d27-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 6.773300e-03 2.220316e-03 2.220316e-03
+5.000000e+01 1.000000e+01 1.000000e+01 1.543200e-02 5.058560e-03 5.058560e-03
+7.000000e+01 1.000000e+01 1.000000e+01 1.175400e-02 3.853117e-03 3.853117e-03
+9.000000e+01 1.000000e+01 1.000000e+01 6.810900e-03 8.405442e-04 8.405442e-04
+1.250000e+02 2.500000e+01 2.500000e+01 3.007300e-03 1.531694e-04 1.531694e-04
+1.750000e+02 2.500000e+01 2.500000e+01 5.568100e-04 5.450803e-05 5.450803e-05
+2.250000e+02 2.500000e+01 2.500000e+01 1.446700e-05 5.007693e-06 5.007693e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d28-x01-y01
+Path=/REF/CMS_2018_I1682495/d28-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 4.285600e-03 1.796920e-03 1.796920e-03
+5.000000e+01 1.000000e+01 1.000000e+01 1.212700e-02 5.084924e-03 5.084924e-03
+7.000000e+01 1.000000e+01 1.000000e+01 1.184700e-02 4.967709e-03 4.967709e-03
+9.000000e+01 1.000000e+01 1.000000e+01 7.609800e-03 9.699616e-04 9.699616e-04
+1.250000e+02 2.500000e+01 2.500000e+01 3.846000e-03 3.022397e-04 3.022397e-04
+1.750000e+02 2.500000e+01 2.500000e+01 1.464300e-03 5.119488e-05 5.119488e-05
+2.250000e+02 2.500000e+01 2.500000e+01 2.786900e-04 3.483326e-05 3.483326e-05
+2.750000e+02 2.500000e+01 2.500000e+01 8.501900e-06 2.905587e-06 2.905587e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d29-x01-y01
+Path=/REF/CMS_2018_I1682495/d29-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 2.858300e-03 1.006629e-03 1.006629e-03
+5.000000e+01 1.000000e+01 1.000000e+01 9.615100e-03 1.599933e-03 1.599933e-03
+7.000000e+01 1.000000e+01 1.000000e+01 1.140500e-02 1.897888e-03 1.897888e-03
+9.000000e+01 1.000000e+01 1.000000e+01 8.203400e-03 1.365111e-03 1.365111e-03
+1.250000e+02 2.500000e+01 2.500000e+01 4.325700e-03 4.789883e-04 4.789883e-04
+1.750000e+02 2.500000e+01 2.500000e+01 1.921300e-03 4.896861e-05 4.896861e-05
+2.250000e+02 2.500000e+01 2.500000e+01 7.474900e-04 4.321946e-05 4.321946e-05
+2.750000e+02 2.500000e+01 2.500000e+01 1.380200e-04 2.124023e-05 2.124023e-05
+3.250000e+02 2.500000e+01 2.500000e+01 5.848100e-06 2.169685e-06 2.169685e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d30-x01-y01
+Path=/REF/CMS_2018_I1682495/d30-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e+01 1.000000e+01 1.000000e+01 1.890500e-03 8.174213e-04 8.174213e-04
+5.000000e+01 1.000000e+01 1.000000e+01 7.428300e-03 1.457375e-03 1.457375e-03
+7.000000e+01 1.000000e+01 1.000000e+01 1.051400e-02 2.062755e-03 2.062755e-03
+9.000000e+01 1.000000e+01 1.000000e+01 8.455000e-03 1.658768e-03 1.658768e-03
+1.250000e+02 2.500000e+01 2.500000e+01 4.662700e-03 5.842101e-04 5.842101e-04
+1.750000e+02 2.500000e+01 2.500000e+01 2.320200e-03 6.599047e-05 6.599047e-05
+2.250000e+02 2.500000e+01 2.500000e+01 1.133100e-03 4.021126e-05 4.021126e-05
+2.750000e+02 2.500000e+01 2.500000e+01 4.633700e-04 3.393016e-05 3.393016e-05
+3.250000e+02 2.500000e+01 2.500000e+01 8.583700e-05 1.635977e-05 1.635977e-05
+3.750000e+02 2.500000e+01 2.500000e+01 3.212800e-06 1.616409e-06 1.616409e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d31-x01-y01
+Path=/REF/CMS_2018_I1682495/d31-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 5.625400e-03 1.250756e-03 1.250756e-03
+7.000000e+01 1.000000e+01 1.000000e+01 9.121800e-03 1.981498e-03 1.981498e-03
+9.000000e+01 1.000000e+01 1.000000e+01 8.456000e-03 1.836833e-03 1.836833e-03
+1.250000e+02 2.500000e+01 2.500000e+01 5.049400e-03 6.220141e-04 6.220141e-04
+1.750000e+02 2.500000e+01 2.500000e+01 2.553700e-03 1.087081e-04 1.087081e-04
+2.250000e+02 2.500000e+01 2.500000e+01 1.418500e-03 4.314815e-05 4.314815e-05
+2.750000e+02 2.500000e+01 2.500000e+01 7.613700e-04 2.838383e-05 2.838383e-05
+3.250000e+02 2.500000e+01 2.500000e+01 3.468800e-04 2.971742e-05 2.971742e-05
+3.750000e+02 2.500000e+01 2.500000e+01 8.246000e-05 1.528838e-05 1.528838e-05
+4.250000e+02 2.500000e+01 2.500000e+01 4.473600e-06 2.441762e-06 2.441762e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d32-x01-y01
+Path=/REF/CMS_2018_I1682495/d32-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 4.160100e-03 1.074622e-03 1.074622e-03
+7.000000e+01 1.000000e+01 1.000000e+01 7.730900e-03 1.039133e-03 1.039133e-03
+9.000000e+01 1.000000e+01 1.000000e+01 8.218200e-03 1.104717e-03 1.104717e-03
+1.250000e+02 2.500000e+01 2.500000e+01 5.344700e-03 7.184374e-04 7.184374e-04
+1.750000e+02 2.500000e+01 2.500000e+01 2.715900e-03 1.918941e-04 1.918941e-04
+2.250000e+02 2.500000e+01 2.500000e+01 1.651000e-03 6.276093e-05 6.276093e-05
+2.750000e+02 2.500000e+01 2.500000e+01 9.287900e-04 4.351027e-05 4.351027e-05
+3.250000e+02 2.500000e+01 2.500000e+01 5.896800e-04 3.448223e-05 3.448223e-05
+3.750000e+02 2.500000e+01 2.500000e+01 3.015500e-04 3.111079e-05 3.111079e-05
+4.250000e+02 2.500000e+01 2.500000e+01 9.237900e-05 2.234801e-05 2.234801e-05
+4.750000e+02 2.500000e+01 2.500000e+01 5.884200e-06 2.929690e-06 2.929690e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d33-x01-y01
+Path=/REF/CMS_2018_I1682495/d33-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 3.385200e-03 9.747277e-04 9.747277e-04
+7.000000e+01 1.000000e+01 1.000000e+01 6.721700e-03 1.030026e-03 1.030026e-03
+9.000000e+01 1.000000e+01 1.000000e+01 7.846200e-03 1.134875e-03 1.134875e-03
+1.250000e+02 2.500000e+01 2.500000e+01 5.470200e-03 7.912072e-04 7.912072e-04
+1.750000e+02 2.500000e+01 2.500000e+01 2.803700e-03 2.583993e-04 2.583993e-04
+2.250000e+02 2.500000e+01 2.500000e+01 1.846200e-03 7.940261e-05 7.940261e-05
+2.750000e+02 2.500000e+01 2.500000e+01 1.043700e-03 6.551007e-05 6.551007e-05
+3.250000e+02 2.500000e+01 2.500000e+01 6.958800e-04 4.842119e-05 4.842119e-05
+3.750000e+02 2.500000e+01 2.500000e+01 4.383600e-04 3.965802e-05 3.965802e-05
+4.250000e+02 2.500000e+01 2.500000e+01 2.213700e-04 4.644706e-05 4.644706e-05
+4.750000e+02 2.500000e+01 2.500000e+01 5.046500e-05 1.530094e-05 1.530094e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d34-x01-y01
+Path=/REF/CMS_2018_I1682495/d34-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 2.766400e-03 8.083755e-04 8.083755e-04
+7.000000e+01 1.000000e+01 1.000000e+01 5.968700e-03 9.996400e-04 9.996400e-04
+9.000000e+01 1.000000e+01 1.000000e+01 7.465200e-03 1.150516e-03 1.150516e-03
+1.250000e+02 2.500000e+01 2.500000e+01 5.525200e-03 8.515365e-04 8.515365e-04
+1.750000e+02 2.500000e+01 2.500000e+01 2.950600e-03 3.353552e-04 3.353552e-04
+2.250000e+02 2.500000e+01 2.500000e+01 1.954100e-03 1.159665e-04 1.159665e-04
+2.750000e+02 2.500000e+01 2.500000e+01 1.138800e-03 8.098884e-05 8.098884e-05
+3.250000e+02 2.500000e+01 2.500000e+01 7.493400e-04 6.527717e-05 6.527717e-05
+3.750000e+02 2.500000e+01 2.500000e+01 5.280800e-04 5.525160e-05 5.525160e-05
+4.250000e+02 2.500000e+01 2.500000e+01 3.033900e-04 4.450798e-05 4.450798e-05
+4.750000e+02 2.500000e+01 2.500000e+01 1.474300e-04 3.042597e-05 3.042597e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d35-x01-y01
+Path=/REF/CMS_2018_I1682495/d35-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 2.204300e-03 7.374464e-04 7.374464e-04
+7.000000e+01 1.000000e+01 1.000000e+01 5.074100e-03 1.023901e-03 1.023901e-03
+9.000000e+01 1.000000e+01 1.000000e+01 6.972800e-03 1.227795e-03 1.227795e-03
+1.250000e+02 2.500000e+01 2.500000e+01 5.609800e-03 9.878297e-04 9.878297e-04
+1.750000e+02 2.500000e+01 2.500000e+01 3.087700e-03 3.965683e-04 3.965683e-04
+2.250000e+02 2.500000e+01 2.500000e+01 2.025700e-03 1.526592e-04 1.526592e-04
+2.750000e+02 2.500000e+01 2.500000e+01 1.237600e-03 1.134935e-04 1.134935e-04
+3.250000e+02 2.500000e+01 2.500000e+01 8.251000e-04 9.066844e-05 9.066844e-05
+3.750000e+02 2.500000e+01 2.500000e+01 5.533200e-04 7.926805e-05 7.926805e-05
+4.250000e+02 2.500000e+01 2.500000e+01 3.978300e-04 6.504437e-05 6.504437e-05
+4.750000e+02 2.500000e+01 2.500000e+01 2.579000e-04 6.053704e-05 6.053704e-05
+5.250000e+02 2.500000e+01 2.500000e+01 1.286900e-04 3.828680e-05 3.828680e-05
+5.750000e+02 2.500000e+01 2.500000e+01 3.603200e-05 2.124770e-05 2.124770e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d36-x01-y01
+Path=/REF/CMS_2018_I1682495/d36-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+01 1.000000e+01 1.000000e+01 1.622800e-03 5.542381e-04 5.542381e-04
+7.000000e+01 1.000000e+01 1.000000e+01 4.056500e-03 8.779840e-04 8.779840e-04
+9.000000e+01 1.000000e+01 1.000000e+01 6.035800e-03 1.101904e-03 1.101904e-03
+1.250000e+02 2.500000e+01 2.500000e+01 5.535100e-03 1.010465e-03 1.010465e-03
+1.750000e+02 2.500000e+01 2.500000e+01 3.206100e-03 4.384043e-04 4.384043e-04
+2.250000e+02 2.500000e+01 2.500000e+01 1.984700e-03 1.336983e-04 1.336983e-04
+2.750000e+02 2.500000e+01 2.500000e+01 1.441400e-03 7.936981e-05 7.936981e-05
+3.250000e+02 2.500000e+01 2.500000e+01 1.069600e-03 8.396442e-05 8.396442e-05
+3.750000e+02 2.500000e+01 2.500000e+01 6.673700e-04 5.891488e-05 5.891488e-05
+4.250000e+02 2.500000e+01 2.500000e+01 4.491700e-04 4.794922e-05 4.794922e-05
+4.750000e+02 2.500000e+01 2.500000e+01 3.368100e-04 4.265912e-05 4.265912e-05
+5.250000e+02 2.500000e+01 2.500000e+01 2.799700e-04 4.003265e-05 4.003265e-05
+5.750000e+02 2.500000e+01 2.500000e+01 1.304100e-04 2.397119e-05 2.397119e-05
+6.250000e+02 2.500000e+01 2.500000e+01 6.687000e-05 1.908508e-05 1.908508e-05
+6.750000e+02 2.500000e+01 2.500000e+01 1.774900e-05 8.376557e-06 8.376557e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d37-x01-y01
+Path=/REF/CMS_2018_I1682495/d37-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.586300e-02 1.093486e-03 1.093486e-03
+3.000000e+01 1.000000e+01 1.000000e+01 9.278800e-03 3.985755e-04 3.985755e-04
+5.000000e+01 1.000000e+01 1.000000e+01 6.842800e-03 3.539937e-04 3.539937e-04
+7.000000e+01 1.000000e+01 1.000000e+01 5.086800e-03 2.826270e-04 2.826270e-04
+9.000000e+01 1.000000e+01 1.000000e+01 2.667400e-03 2.518178e-04 2.518178e-04
+1.250000e+02 2.500000e+01 2.500000e+01 3.437400e-04 6.143681e-05 6.143681e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d38-x01-y01
+Path=/REF/CMS_2018_I1682495/d38-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.503700e-02 1.084955e-03 1.084955e-03
+3.000000e+01 1.000000e+01 1.000000e+01 8.247200e-03 2.254222e-04 2.254222e-04
+5.000000e+01 1.000000e+01 1.000000e+01 5.506200e-03 2.053754e-04 2.053754e-04
+7.000000e+01 1.000000e+01 1.000000e+01 4.508300e-03 2.520057e-04 2.520057e-04
+9.000000e+01 1.000000e+01 1.000000e+01 3.537100e-03 2.136130e-04 2.136130e-04
+1.250000e+02 2.500000e+01 2.500000e+01 1.339200e-03 9.305939e-05 9.305939e-05
+1.750000e+02 2.500000e+01 2.500000e+01 3.943900e-05 1.040427e-05 1.040427e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d39-x01-y01
+Path=/REF/CMS_2018_I1682495/d39-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.419000e-02 8.793591e-04 8.793591e-04
+3.000000e+01 1.000000e+01 1.000000e+01 7.379100e-03 1.170495e-04 1.170495e-04
+5.000000e+01 1.000000e+01 1.000000e+01 4.852900e-03 1.657890e-04 1.657890e-04
+7.000000e+01 1.000000e+01 1.000000e+01 3.865200e-03 1.292146e-04 1.292146e-04
+9.000000e+01 1.000000e+01 1.000000e+01 3.276700e-03 1.272354e-04 1.272354e-04
+1.250000e+02 2.500000e+01 2.500000e+01 2.202600e-03 8.744496e-05 8.744496e-05
+1.750000e+02 2.500000e+01 2.500000e+01 5.965100e-04 5.495277e-05 5.495277e-05
+2.250000e+02 2.500000e+01 2.500000e+01 1.914900e-05 6.264371e-06 6.264371e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d40-x01-y01
+Path=/REF/CMS_2018_I1682495/d40-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.383700e-02 5.988903e-04 5.988903e-04
+3.000000e+01 1.000000e+01 1.000000e+01 6.643300e-03 9.798867e-05 9.798867e-05
+5.000000e+01 1.000000e+01 1.000000e+01 4.353900e-03 9.511029e-05 9.511029e-05
+7.000000e+01 1.000000e+01 1.000000e+01 3.394100e-03 8.937354e-05 8.937354e-05
+9.000000e+01 1.000000e+01 1.000000e+01 2.874600e-03 6.926149e-05 6.926149e-05
+1.250000e+02 2.500000e+01 2.500000e+01 2.229200e-03 8.356183e-05 8.356183e-05
+1.750000e+02 2.500000e+01 2.500000e+01 1.277000e-03 5.003141e-05 5.003141e-05
+2.250000e+02 2.500000e+01 2.500000e+01 2.963700e-04 3.638264e-05 3.638264e-05
+2.750000e+02 2.500000e+01 2.500000e+01 1.040800e-05 3.275523e-06 3.275523e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d41-x01-y01
+Path=/REF/CMS_2018_I1682495/d41-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.358900e-02 5.721610e-04 5.721610e-04
+3.000000e+01 1.000000e+01 1.000000e+01 6.335300e-03 1.156513e-04 1.156513e-04
+5.000000e+01 1.000000e+01 1.000000e+01 4.037900e-03 9.421659e-05 9.421659e-05
+7.000000e+01 1.000000e+01 1.000000e+01 3.205100e-03 6.649502e-05 6.649502e-05
+9.000000e+01 1.000000e+01 1.000000e+01 2.733500e-03 6.434884e-05 6.434884e-05
+1.250000e+02 2.500000e+01 2.500000e+01 2.052200e-03 5.519060e-05 5.519060e-05
+1.750000e+02 2.500000e+01 2.500000e+01 1.474900e-03 6.018396e-05 6.018396e-05
+2.250000e+02 2.500000e+01 2.500000e+01 7.114200e-04 3.801648e-05 3.801648e-05
+2.750000e+02 2.500000e+01 2.500000e+01 1.464000e-04 2.186873e-05 2.186873e-05
+3.250000e+02 2.500000e+01 2.500000e+01 7.465300e-06 2.633197e-06 2.633197e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d42-x01-y01
+Path=/REF/CMS_2018_I1682495/d42-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.353400e-02 6.297974e-04 6.297974e-04
+3.000000e+01 1.000000e+01 1.000000e+01 6.326400e-03 2.033463e-04 2.033463e-04
+5.000000e+01 1.000000e+01 1.000000e+01 3.849400e-03 1.682225e-04 1.682225e-04
+7.000000e+01 1.000000e+01 1.000000e+01 2.956400e-03 6.898713e-05 6.898713e-05
+9.000000e+01 1.000000e+01 1.000000e+01 2.492100e-03 6.208664e-05 6.208664e-05
+1.250000e+02 2.500000e+01 2.500000e+01 1.842000e-03 3.221599e-05 3.221599e-05
+1.750000e+02 2.500000e+01 2.500000e+01 1.490400e-03 4.485444e-05 4.485444e-05
+2.250000e+02 2.500000e+01 2.500000e+01 9.814700e-04 3.898958e-05 3.898958e-05
+2.750000e+02 2.500000e+01 2.500000e+01 4.545300e-04 2.916593e-05 2.916593e-05
+3.250000e+02 2.500000e+01 2.500000e+01 8.925000e-05 1.701443e-05 1.701443e-05
+3.750000e+02 2.500000e+01 2.500000e+01 3.277100e-06 1.841338e-06 1.841338e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d43-x01-y01
+Path=/REF/CMS_2018_I1682495/d43-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.343700e-02 8.648348e-04 8.648348e-04
+3.000000e+01 1.000000e+01 1.000000e+01 6.158100e-03 2.208162e-04 2.208162e-04
+5.000000e+01 1.000000e+01 1.000000e+01 3.613400e-03 1.271408e-04 1.271408e-04
+7.000000e+01 1.000000e+01 1.000000e+01 2.840800e-03 7.914576e-05 7.914576e-05
+9.000000e+01 1.000000e+01 1.000000e+01 2.350500e-03 6.492530e-05 6.492530e-05
+1.250000e+02 2.500000e+01 2.500000e+01 1.718900e-03 7.016723e-05 7.016723e-05
+1.750000e+02 2.500000e+01 2.500000e+01 1.370100e-03 3.396972e-05 3.396972e-05
+2.250000e+02 2.500000e+01 2.500000e+01 1.067600e-03 4.488199e-05 4.488199e-05
+2.750000e+02 2.500000e+01 2.500000e+01 6.944900e-04 3.502861e-05 3.502861e-05
+3.250000e+02 2.500000e+01 2.500000e+01 3.335500e-04 3.253084e-05 3.253084e-05
+3.750000e+02 2.500000e+01 2.500000e+01 8.337200e-05 1.456441e-05 1.456441e-05
+4.250000e+02 2.500000e+01 2.500000e+01 4.674300e-06 2.381409e-06 2.381409e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d44-x01-y01
+Path=/REF/CMS_2018_I1682495/d44-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.305000e-02 1.404545e-03 1.404545e-03
+3.000000e+01 1.000000e+01 1.000000e+01 6.100200e-03 3.587100e-04 3.587100e-04
+5.000000e+01 1.000000e+01 1.000000e+01 3.555000e-03 1.393527e-04 1.393527e-04
+7.000000e+01 1.000000e+01 1.000000e+01 2.598900e-03 9.384839e-05 9.384839e-05
+9.000000e+01 1.000000e+01 1.000000e+01 2.152200e-03 8.649345e-05 8.649345e-05
+1.250000e+02 2.500000e+01 2.500000e+01 1.627800e-03 5.104028e-05 5.104028e-05
+1.750000e+02 2.500000e+01 2.500000e+01 1.247400e-03 4.831640e-05 4.831640e-05
+2.250000e+02 2.500000e+01 2.500000e+01 1.058900e-03 6.461868e-05 6.461868e-05
+2.750000e+02 2.500000e+01 2.500000e+01 7.519800e-04 3.999753e-05 3.999753e-05
+3.250000e+02 2.500000e+01 2.500000e+01 5.533700e-04 3.464598e-05 3.464598e-05
+3.750000e+02 2.500000e+01 2.500000e+01 2.910600e-04 3.170688e-05 3.170688e-05
+4.250000e+02 2.500000e+01 2.500000e+01 9.210100e-05 2.030625e-05 2.030625e-05
+4.750000e+02 2.500000e+01 2.500000e+01 6.002500e-06 2.919514e-06 2.919514e-06
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d45-x01-y01
+Path=/REF/CMS_2018_I1682495/d45-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.253000e-02 1.221055e-03 1.221055e-03
+3.000000e+01 1.000000e+01 1.000000e+01 6.017900e-03 4.334288e-04 4.334288e-04
+5.000000e+01 1.000000e+01 1.000000e+01 3.417700e-03 2.174126e-04 2.174126e-04
+7.000000e+01 1.000000e+01 1.000000e+01 2.609900e-03 1.878778e-04 1.878778e-04
+9.000000e+01 1.000000e+01 1.000000e+01 2.155400e-03 1.164588e-04 1.164588e-04
+1.250000e+02 2.500000e+01 2.500000e+01 1.566300e-03 6.970922e-05 6.970922e-05
+1.750000e+02 2.500000e+01 2.500000e+01 1.188300e-03 6.090188e-05 6.090188e-05
+2.250000e+02 2.500000e+01 2.500000e+01 1.034900e-03 6.766909e-05 6.766909e-05
+2.750000e+02 2.500000e+01 2.500000e+01 7.763500e-04 5.411898e-05 5.411898e-05
+3.250000e+02 2.500000e+01 2.500000e+01 6.381800e-04 4.804365e-05 4.804365e-05
+3.750000e+02 2.500000e+01 2.500000e+01 4.331500e-04 4.229846e-05 4.229846e-05
+4.250000e+02 2.500000e+01 2.500000e+01 2.074800e-04 4.259217e-05 4.259217e-05
+4.750000e+02 2.500000e+01 2.500000e+01 5.185000e-05 1.551707e-05 1.551707e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d46-x01-y01
+Path=/REF/CMS_2018_I1682495/d46-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.195900e-02 1.030495e-03 1.030495e-03
+3.000000e+01 1.000000e+01 1.000000e+01 6.197900e-03 6.922886e-04 6.922886e-04
+5.000000e+01 1.000000e+01 1.000000e+01 3.072300e-03 2.693268e-04 2.693268e-04
+7.000000e+01 1.000000e+01 1.000000e+01 2.345500e-03 1.883963e-04 1.883963e-04
+9.000000e+01 1.000000e+01 1.000000e+01 2.161900e-03 1.588528e-04 1.588528e-04
+1.250000e+02 2.500000e+01 2.500000e+01 1.742100e-03 9.867642e-05 9.867642e-05
+1.750000e+02 2.500000e+01 2.500000e+01 1.156400e-03 8.016350e-05 8.016350e-05
+2.250000e+02 2.500000e+01 2.500000e+01 9.765900e-04 7.579684e-05 7.579684e-05
+2.750000e+02 2.500000e+01 2.500000e+01 7.982100e-04 7.498612e-05 7.498612e-05
+3.250000e+02 2.500000e+01 2.500000e+01 5.961700e-04 5.916806e-05 5.916806e-05
+3.750000e+02 2.500000e+01 2.500000e+01 5.131200e-04 5.696563e-05 5.696563e-05
+4.250000e+02 2.500000e+01 2.500000e+01 2.722000e-04 4.001450e-05 4.001450e-05
+4.750000e+02 2.500000e+01 2.500000e+01 1.426700e-04 2.943247e-05 2.943247e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d47-x01-y01
+Path=/REF/CMS_2018_I1682495/d47-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.104900e-02 1.275600e-03 1.275600e-03
+3.000000e+01 1.000000e+01 1.000000e+01 6.536300e-03 7.599381e-04 7.599381e-04
+5.000000e+01 1.000000e+01 1.000000e+01 3.153100e-03 3.051030e-04 3.051030e-04
+7.000000e+01 1.000000e+01 1.000000e+01 2.408000e-03 2.232916e-04 2.232916e-04
+9.000000e+01 1.000000e+01 1.000000e+01 2.164200e-03 2.240377e-04 2.240377e-04
+1.250000e+02 2.500000e+01 2.500000e+01 1.562200e-03 1.376464e-04 1.376464e-04
+1.750000e+02 2.500000e+01 2.500000e+01 1.144900e-03 1.106290e-04 1.106290e-04
+2.250000e+02 2.500000e+01 2.500000e+01 8.625800e-04 9.687764e-05 9.687764e-05
+2.750000e+02 2.500000e+01 2.500000e+01 8.556000e-04 9.886224e-05 9.886224e-05
+3.250000e+02 2.500000e+01 2.500000e+01 6.078800e-04 7.796261e-05 7.796261e-05
+3.750000e+02 2.500000e+01 2.500000e+01 4.674000e-04 7.371973e-05 7.371973e-05
+4.250000e+02 2.500000e+01 2.500000e+01 3.903600e-04 6.442705e-05 6.442705e-05
+4.750000e+02 2.500000e+01 2.500000e+01 2.422400e-04 5.919134e-05 5.919134e-05
+5.250000e+02 2.500000e+01 2.500000e+01 1.316500e-04 3.741943e-05 3.741943e-05
+5.750000e+02 2.500000e+01 2.500000e+01 4.213900e-05 2.467944e-05 2.467944e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1682495/d48-x01-y01
+Path=/REF/CMS_2018_I1682495/d48-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+01 5.000000e+00 5.000000e+00 1.053000e-02 1.002888e-03 1.002888e-03
+3.000000e+01 1.000000e+01 1.000000e+01 6.664200e-03 9.899610e-04 9.899610e-04
+5.000000e+01 1.000000e+01 1.000000e+01 3.063300e-03 3.717042e-04 3.717042e-04
+7.000000e+01 1.000000e+01 1.000000e+01 2.110500e-03 2.389640e-04 2.389640e-04
+9.000000e+01 1.000000e+01 1.000000e+01 1.821800e-03 1.479741e-04 1.479741e-04
+1.250000e+02 2.500000e+01 2.500000e+01 1.365100e-03 8.342230e-05 8.342230e-05
+1.750000e+02 2.500000e+01 2.500000e+01 9.728700e-04 7.679215e-05 7.679215e-05
+2.250000e+02 2.500000e+01 2.500000e+01 8.295800e-04 6.334366e-05 6.334366e-05
+2.750000e+02 2.500000e+01 2.500000e+01 6.983500e-04 5.833489e-05 5.833489e-05
+3.250000e+02 2.500000e+01 2.500000e+01 7.072000e-04 6.586152e-05 6.586152e-05
+3.750000e+02 2.500000e+01 2.500000e+01 5.124600e-04 5.323459e-05 5.323459e-05
+4.250000e+02 2.500000e+01 2.500000e+01 3.414300e-04 4.179184e-05 4.179184e-05
+4.750000e+02 2.500000e+01 2.500000e+01 3.439600e-04 3.899417e-05 3.899417e-05
+5.250000e+02 2.500000e+01 2.500000e+01 2.451500e-04 3.990460e-05 3.990460e-05
+5.750000e+02 2.500000e+01 2.500000e+01 1.031000e-04 2.124488e-05 2.124488e-05
+6.250000e+02 2.500000e+01 2.500000e+01 6.176200e-05 1.666378e-05 1.666378e-05
+6.750000e+02 2.500000e+01 2.500000e+01 2.292100e-05 1.033043e-05 1.033043e-05
+# END YODA_SCATTER2D
+
diff --git a/analyses/pluginCMS/CMS_2018_I1690148.cc b/analyses/pluginCMS/CMS_2018_I1690148.cc
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1690148.cc
@@ -0,0 +1,439 @@
+#include "Rivet/Analysis.hh"
+#include "Rivet/Projections/FinalState.hh"
+#include "Rivet/Projections/FastJets.hh"
+#include "Rivet/Projections/ChargedLeptons.hh"
+#include "Rivet/Projections/DressedLeptons.hh"
+#include "Rivet/Projections/IdentifiedFinalState.hh"
+#include "Rivet/Projections/PromptFinalState.hh"
+#include "Rivet/Projections/VetoedFinalState.hh"
+#include "Rivet/Projections/InvMassFinalState.hh"
+#include "Rivet/Projections/MissingMomentum.hh"
+#include "Rivet/Math/MatrixN.hh"
+#include "Rivet/Math/MatrixDiag.hh"
+#include "Rivet/Tools/fjcontrib/Nsubjettiness.hh"
+#include "Rivet/Tools/fjcontrib/EnergyCorrelator.hh"
+
+namespace Rivet {
+
+
+ /// Measurement of jet substructure observables in $t\bar{t}$ events from $pp$ collisions at 13~TeV
+ class CMS_2018_I1690148 : public Analysis {
+ public:
+
+ enum Reconstruction { CHARGED=0, ALL=1 };
+ enum Observable { MULT=0, PTDS=1, GA_LHA=2, GA_WIDTH=3, GA_THRUST=4, ECC=5, ZG=6, ZGDR=7, NSD=8, TAU21=9, TAU32=10, TAU43=11, C1_00=12, C1_02=13, C1_05=14, C1_10=15, C1_20=16, C2_00=17, C2_02=18, C2_05=19, C2_10=20, C2_20=21, C3_00=22, C3_02=23, C3_05=24, C3_10=25, C3_20=26, M2_B1=27, N2_B1=28, N3_B1=29, M2_B2=30, N2_B2=31, N3_B2=32 };
+ enum Flavor { INCL=0, BOTTOM=1, QUARK=2, GLUON=3 };
+
+
+ /// Minimal constructor
+ DEFAULT_RIVET_ANALYSIS_CTOR(CMS_2018_I1690148);
+
+
+ /// @name Analysis methods
+ //@{
+
+
+ /// Set up projections and book histograms
+ void init() {
+
+ // Cuts
+ particle_cut = (Cuts::abseta < 5.0 && Cuts::pT > 0.*GeV);
+ lepton_cut = (Cuts::abseta < 2.4 && Cuts::pT > 15.*GeV);
+ jet_cut = (Cuts::abseta < 2.4 && Cuts::pT > 30.*GeV);
+
+ // Generic final state
+ FinalState fs(particle_cut);
+
+ // Dressed leptons
+ ChargedLeptons charged_leptons(fs);
+ IdentifiedFinalState photons(fs);
+ photons.acceptIdPair(PID::PHOTON);
+
+ PromptFinalState prompt_leptons(charged_leptons);
+ prompt_leptons.acceptMuonDecays(true);
+ prompt_leptons.acceptTauDecays(true);
+
+ PromptFinalState prompt_photons(photons);
+ prompt_photons.acceptMuonDecays(true);
+ prompt_photons.acceptTauDecays(true);
+
+ // NB. useDecayPhotons=true allows for photons with tau ancestor; photons from hadrons are vetoed by the PromptFinalState;
+ DressedLeptons dressed_leptons(prompt_photons, prompt_leptons, 0.1, lepton_cut, true);
+ addProjection(dressed_leptons, "DressedLeptons");
+
+ // Projection for jets
+ VetoedFinalState fsForJets(fs);
+ fsForJets.addVetoOnThisFinalState(dressed_leptons);
+ addProjection(FastJets(fsForJets, FastJets::ANTIKT, 0.4,
+ JetAlg::ALL_MUONS, JetAlg::NO_INVISIBLES), "Jets");
+
+ // Booking of histograms
+ int d = 0;
+ for (int r = 0; r < 2; ++r) { // reconstruction (charged, all)
+ for (int o = 0; o < 33; ++o) { // observable
+ d += 1;
+ for (int f = 0; f < 4; ++f) { // flavor
+ char buffer [11];
+ sprintf(buffer, "d%02d-x01-y%02d", d, f+1);
+ _h[r][o][f] = bookHisto1D(buffer);
+ }
+ }
+ }
+ }
+
+
+ void analyze(const Event& event) {
+ const double weight = event.weight();
+
+ // select ttbar -> lepton+jets
+ const vector<DressedLepton>& leptons = applyProjection<DressedLeptons>(event, "DressedLeptons").dressedLeptons();
+ int nsel_leptons = 0;
+ for (const DressedLepton& lepton : leptons) {
+ if (lepton.pt() > 26.) nsel_leptons += 1; else vetoEvent; // found veto lepton
+ }
+ if (nsel_leptons != 1) vetoEvent;
+
+ const Jets all_jets = applyProjection<FastJets>(event, "Jets").jetsByPt(jet_cut);
+ if (all_jets.size() < 4) vetoEvent;
+
+ // categorize jets
+ int nsel_bjets = 0;
+ int nsel_wjets = 0;
+ Jets jets[4];
+ for (const Jet& jet : all_jets) {
+ // check for jet-lepton overlap -> do not consider for selection
+ if (deltaR(jet, leptons[0]) < 0.4) continue;
+
+ bool overlap = false;
+ bool w_jet = false;
+ for (const Jet& jet2 : all_jets) {
+ if (jet.momentum() == jet2.momentum()) continue;
+ // check for jet-jet overlap -> do not consider for analysis
+ if (deltaR(jet, jet2) < 0.8)
+ overlap = true;
+ // check for W candidate
+ if (jet.bTagged() or jet2.bTagged()) continue;
+ FourMomentum w_cand = jet.momentum() + jet2.momentum();
+ if (abs(w_cand.mass() - 80.4) < 15.) w_jet = true;
+ }
+
+ // count jets for event selection
+ if (jet.bTagged()) nsel_bjets += 1;
+ if (w_jet) nsel_wjets += 1;
+
+ // jets for analysis
+ if (jet.abseta() > 2. or overlap) continue;
+
+ if (jet.bTagged()) {
+ jets[BOTTOM].push_back(jet);
+ } else if (w_jet) {
+ jets[QUARK].push_back(jet);
+ } else {
+ jets[GLUON].push_back(jet);
+ }
+ }
+
+ if (nsel_bjets != 2) vetoEvent;
+ if (nsel_wjets < 2) vetoEvent;
+
+ // substructure analysis
+ // no loop over incl jets -> more loc but faster
+ for (int f = 1; f < 4; ++f) {
+ for (const Jet& jet : jets[f]) {
+ // apply cuts on constituents
+ vector<PseudoJet> particles[2];
+ for (const Particle& p : jet.particles(Cuts::pT > 1.*GeV)) {
+ particles[ALL].push_back( PseudoJet(p.px(), p.py(), p.pz(), p.energy()) );
+ if (p.charge3() != 0)
+ particles[CHARGED].push_back( PseudoJet(p.px(), p.py(), p.pz(), p.energy()) );
+ }
+
+ if (particles[CHARGED].size() == 0) continue;
+
+ // recluster with C/A and anti-kt+WTA
+ PseudoJet ca_jet[2];
+ JetDefinition ca_def(fastjet::cambridge_algorithm, fastjet::JetDefinition::max_allowable_R);
+ ClusterSequence ca_charged(particles[CHARGED], ca_def);
+ ClusterSequence ca_all(particles[ALL], ca_def);
+ ca_jet[CHARGED] = ca_charged.exclusive_jets(1)[0];
+ ca_jet[ALL] = ca_all.exclusive_jets(1)[0];
+
+ PseudoJet akwta_jet[2];
+ JetDefinition akwta_def(fastjet::antikt_algorithm, fastjet::JetDefinition::max_allowable_R, fastjet::RecombinationScheme::WTA_pt_scheme);
+ ClusterSequence akwta_charged(particles[CHARGED], akwta_def);
+ ClusterSequence akwta_all(particles[ALL], akwta_def);
+ akwta_jet[CHARGED] = akwta_charged.exclusive_jets(1)[0];
+ akwta_jet[ALL] = akwta_all.exclusive_jets(1)[0];
+
+ // calculate observables
+ for (int r = 0; r < 2; ++r) {
+ int mult = akwta_jet[r].constituents().size();
+ // generalized angularities
+ _h[r][MULT][INCL]->fill(mult, weight);
+ _h[r][MULT][f]->fill(mult, weight);
+ if (mult > 1) {
+ double ptds = getPtDs(akwta_jet[r]);
+ double ga_lha = calcGA(0.5, 1., akwta_jet[r]);
+ double ga_width = calcGA(1., 1., akwta_jet[r]);
+ double ga_thrust = calcGA(2., 1., akwta_jet[r]);
+ _h[r][PTDS][INCL]->fill(ptds, weight);
+ _h[r][PTDS][f]->fill(ptds, weight);
+ _h[r][GA_LHA][INCL]->fill(ga_lha, weight);
+ _h[r][GA_LHA][f]->fill(ga_lha, weight);
+ _h[r][GA_WIDTH][INCL]->fill(ga_width, weight);
+ _h[r][GA_WIDTH][f]->fill(ga_width, weight);
+ _h[r][GA_THRUST][INCL]->fill(ga_thrust, weight);
+ _h[r][GA_THRUST][f]->fill(ga_thrust, weight);
+ }
+ // eccentricity
+ if (mult > 3) {
+ double ecc = getEcc(akwta_jet[r]);
+ _h[r][ECC][INCL]->fill(ecc, weight);
+ _h[r][ECC][f]->fill(ecc, weight);
+ }
+ // N-subjettiness
+ if (mult > 2) {
+ double tau21 = getTau(2, 1, ca_jet[r]);
+ _h[r][TAU21][INCL]->fill(tau21, weight);
+ _h[r][TAU21][f]->fill(tau21, weight);
+ }
+ if (mult > 3) {
+ double tau32 = getTau(3, 2, ca_jet[r]);
+ _h[r][TAU32][INCL]->fill(tau32, weight);
+ _h[r][TAU32][f]->fill(tau32, weight);
+ }
+ if (mult > 4) {
+ double tau43 = getTau(4, 3, ca_jet[r]);
+ _h[r][TAU43][INCL]->fill(tau43, weight);
+ _h[r][TAU43][f]->fill(tau43, weight);
+ }
+ // soft drop
+ if (mult > 1) {
+ vector<double> sd_results = getZg(ca_jet[r]);
+ if (sd_results[0] > 0.) {
+ _h[r][ZG][INCL]->fill(sd_results[0], weight);
+ _h[r][ZG][f]->fill(sd_results[0], weight);
+ _h[r][ZGDR][INCL]->fill(sd_results[1], weight);
+ _h[r][ZGDR][f]->fill(sd_results[1], weight);
+ }
+ }
+ int nsd = getNSD(0.007, -1., ca_jet[r]);
+ _h[r][NSD][INCL]->fill(nsd, weight);
+ _h[r][NSD][f]->fill(nsd, weight);
+ // C-series energy correlation ratios
+ if (mult > 1) {
+ double cn_00 = getC(1, 0.0, ca_jet[r]);
+ double cn_02 = getC(1, 0.2, ca_jet[r]);
+ double cn_05 = getC(1, 0.5, ca_jet[r]);
+ double cn_10 = getC(1, 1.0, ca_jet[r]);
+ double cn_20 = getC(1, 2.0, ca_jet[r]);
+ _h[r][C1_00][INCL]->fill(cn_00, weight);
+ _h[r][C1_02][INCL]->fill(cn_02, weight);
+ _h[r][C1_05][INCL]->fill(cn_05, weight);
+ _h[r][C1_10][INCL]->fill(cn_10, weight);
+ _h[r][C1_20][INCL]->fill(cn_20, weight);
+ _h[r][C1_00][f]->fill(cn_00, weight);
+ _h[r][C1_02][f]->fill(cn_02, weight);
+ _h[r][C1_05][f]->fill(cn_05, weight);
+ _h[r][C1_10][f]->fill(cn_10, weight);
+ _h[r][C1_20][f]->fill(cn_20, weight);
+ }
+ if (mult > 2) {
+ double cn_00 = getC(2, 0.0, ca_jet[r]);
+ double cn_02 = getC(2, 0.2, ca_jet[r]);
+ double cn_05 = getC(2, 0.5, ca_jet[r]);
+ double cn_10 = getC(2, 1.0, ca_jet[r]);
+ double cn_20 = getC(2, 2.0, ca_jet[r]);
+ _h[r][C2_00][INCL]->fill(cn_00, weight);
+ _h[r][C2_02][INCL]->fill(cn_02, weight);
+ _h[r][C2_05][INCL]->fill(cn_05, weight);
+ _h[r][C2_10][INCL]->fill(cn_10, weight);
+ _h[r][C2_20][INCL]->fill(cn_20, weight);
+ _h[r][C2_00][f]->fill(cn_00, weight);
+ _h[r][C2_02][f]->fill(cn_02, weight);
+ _h[r][C2_05][f]->fill(cn_05, weight);
+ _h[r][C2_10][f]->fill(cn_10, weight);
+ _h[r][C2_20][f]->fill(cn_20, weight);
+ }
+ if (mult > 3) {
+ double cn_00 = getC(3, 0.0, ca_jet[r]);
+ double cn_02 = getC(3, 0.2, ca_jet[r]);
+ double cn_05 = getC(3, 0.5, ca_jet[r]);
+ double cn_10 = getC(3, 1.0, ca_jet[r]);
+ double cn_20 = getC(3, 2.0, ca_jet[r]);
+ _h[r][C3_00][INCL]->fill(cn_00, weight);
+ _h[r][C3_02][INCL]->fill(cn_02, weight);
+ _h[r][C3_05][INCL]->fill(cn_05, weight);
+ _h[r][C3_10][INCL]->fill(cn_10, weight);
+ _h[r][C3_20][INCL]->fill(cn_20, weight);
+ _h[r][C3_00][f]->fill(cn_00, weight);
+ _h[r][C3_02][f]->fill(cn_02, weight);
+ _h[r][C3_05][f]->fill(cn_05, weight);
+ _h[r][C3_10][f]->fill(cn_10, weight);
+ _h[r][C3_20][f]->fill(cn_20, weight);
+ }
+ // M/N-series energy correlation ratios
+ if (mult > 2) {
+ double m2_b1 = getM(2, 1., ca_jet[r]);
+ double m2_b2 = getM(2, 2., ca_jet[r]);
+ double n2_b1 = getN(2, 1., ca_jet[r]);
+ double n2_b2 = getN(2, 2., ca_jet[r]);
+ _h[r][M2_B1][INCL]->fill(m2_b1, weight);
+ _h[r][M2_B2][INCL]->fill(m2_b2, weight);
+ _h[r][N2_B1][INCL]->fill(n2_b1, weight);
+ _h[r][N2_B2][INCL]->fill(n2_b2, weight);
+ _h[r][M2_B1][f]->fill(m2_b1, weight);
+ _h[r][M2_B2][f]->fill(m2_b2, weight);
+ _h[r][N2_B1][f]->fill(n2_b1, weight);
+ _h[r][N2_B2][f]->fill(n2_b2, weight);
+ }
+ if (mult > 3) {
+ double n3_b1 = getN(3, 1., ca_jet[r]);
+ double n3_b2 = getN(3, 2., ca_jet[r]);
+ _h[r][N3_B1][INCL]->fill(n3_b1, weight);
+ _h[r][N3_B2][INCL]->fill(n3_b2, weight);
+ _h[r][N3_B1][f]->fill(n3_b1, weight);
+ _h[r][N3_B2][f]->fill(n3_b2, weight);
+ }
+ }
+ }
+ }
+ }
+
+
+ void finalize() {
+ for (int r = 0; r < 2; ++r) { // reconstruction (charged, all)
+ for (int o = 0; o < 33; ++o) { // observable
+ for (int f = 0; f < 4; ++f) { // flavor
+ normalize(_h[r][o][f], 1.0, false);
+ }
+ }
+ }
+ }
+
+ //@}
+
+
+ private:
+
+ double deltaR(PseudoJet j1, PseudoJet j2) {
+ double deta = j1.eta() - j2.eta();
+ double dphi = j1.delta_phi_to(j2);
+ return sqrt(deta*deta + dphi*dphi);
+ }
+
+
+ double getPtDs(PseudoJet jet) {
+ double mult = jet.constituents().size();
+ double sumpt = 0.; // would be jet.pt() in WTA scheme but better keep it generic
+ double sumpt2 = 0.;
+ for (auto p : jet.constituents()) {
+ sumpt += p.pt();
+ sumpt2 += pow(p.pt(), 2);
+ }
+ double ptd = sumpt2/pow(sumpt,2);
+ return max(0., sqrt((ptd-1./mult) * mult/(mult-1.)));
+ }
+
+
+ double calcGA(double beta, double kappa, PseudoJet jet) {
+ double sumpt = 0.;
+ for (const auto& p : jet.constituents()) {
+ sumpt += p.pt();
+ }
+ double ga = 0.;
+ for (auto p : jet.constituents()) {
+ ga += pow(p.pt()/sumpt, kappa) * pow(deltaR(jet, p)/0.4, beta);
+ }
+ return ga;
+ }
+
+
+ double getEcc(PseudoJet jet) {
+ // Covariance matrix
+ Matrix<2> M;
+ for (const auto& p : jet.constituents()) {
+ Matrix<2> MPart;
+ MPart.set(0, 0, (p.eta() - jet.eta()) * (p.eta() - jet.eta()));
+ MPart.set(0, 1, (p.eta() - jet.eta()) * mapAngleMPiToPi(p.phi() - jet.phi()));
+ MPart.set(1, 0, mapAngleMPiToPi(p.phi() - jet.phi()) * (p.eta() - jet.eta()));
+ MPart.set(1, 1, mapAngleMPiToPi(p.phi() - jet.phi()) * mapAngleMPiToPi(p.phi() - jet.phi()));
+ M += MPart * p.e();
+ }
+ // Calculate eccentricity from eigenvalues
+ const EigenSystem<2> eigen = diagonalize(M);
+ return 1. - eigen.getEigenValues()[1]/eigen.getEigenValues()[0];
+ }
+
+
+ double getTau(int N, int M, PseudoJet jet) {
+ fjcontrib::Nsubjettiness::NsubjettinessRatio tau_ratio(N, M, fjcontrib::Nsubjettiness::OnePass_WTA_KT_Axes(),
+ fjcontrib::Nsubjettiness::NormalizedMeasure(1.0, 0.4));
+ return tau_ratio(jet);
+ }
+
+
+ vector<double> getZg(PseudoJet jet) {
+ PseudoJet jet0 = jet;
+ PseudoJet jet1, jet2;
+ double zg = 0.;
+ while (zg < 0.1 && jet0.has_parents(jet1, jet2)) {
+ zg = jet2.pt()/jet0.pt();
+ jet0 = jet1;
+ }
+ if (zg < 0.1) return {-1., -1.};
+ return {zg, jet1.delta_R(jet2)};
+ }
+
+
+ int getNSD(double zcut, double beta, PseudoJet jet) {
+ PseudoJet jet0 = jet;
+ PseudoJet jet1, jet2;
+ int nsd = 0.;
+ double zg = 0.;
+ while (jet0.has_parents(jet1, jet2)) {
+ zg = jet2.pt()/jet0.pt();
+ if (zg > zcut * pow(jet1.delta_R(jet2)/0.4, beta))
+ nsd += 1;
+ jet0 = jet1;
+ }
+ return nsd;
+ }
+
+
+ double getC(int N, double beta, PseudoJet jet) {
+ fjcontrib::EnergyCorrelatorDoubleRatio C(N, beta);
+ return C(jet);
+ }
+
+
+ double getM(int N, double beta, PseudoJet jet) {
+ fjcontrib::EnergyCorrelatorMseries CM(N, beta);
+ return CM(jet);
+ }
+
+
+ double getN(int N, double beta, PseudoJet jet) {
+ fjcontrib::EnergyCorrelatorNseries CN(N, beta);
+ return CN(jet);
+ }
+
+
+ private:
+
+ // @name Histogram data members
+ //@{
+
+ Cut particle_cut, lepton_cut, jet_cut;
+ Histo1DPtr _h[2][33][4];
+
+ //@}
+
+ };
+
+
+
+ // The hook for the plugin system
+ DECLARE_RIVET_PLUGIN(CMS_2018_I1690148);
+
+}
diff --git a/analyses/pluginCMS/CMS_2018_I1690148.info b/analyses/pluginCMS/CMS_2018_I1690148.info
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1690148.info
@@ -0,0 +1,46 @@
+Name: CMS_2018_I1690148
+Year: 2018
+Summary: Measurement of jet substructure observables in $t\bar{t}$ events from $pp$ collisions at 13~TeV
+Experiment: CMS
+Collider: LHC
+InspireID: 1690148
+Status: VALIDATED
+Authors:
+ - Markus Seidel <markus.seidel@cern.ch>
+References:
+ - arXiv:1808.07340
+ - CMS-TOP-17-013
+ - Phys. Rev. D 98, 092014 (2018)
+RunInfo:
+ $t\bar{t}$ events at $\sqrt{s} = 13~\TeV$, lepton+jets selection at particle level.
+Luminosity: 35.9 / fb
+Beams: [p+, p+]
+Energies: [13000]
+Description:
+ 'A measurement of jet substructure observables is presented using $t\bar{t}$ events in the lepton+jets channel
+ from proton-proton collisions at $\sqrt{s}=13$ TeV recorded by the CMS experiment at the LHC, corresponding to
+ an integrated luminosity of 35.9/fb. Multiple jet substructure observables are measured for jets identified as
+ bottom, light-quark, and gluon jets, as well as for inclusive jets (no flavor information). The results are
+ unfolded to the particle level and compared to next-to-leading-order predictions from POWHEG interfaced with
+ the parton shower generators PYTHIA 8 and HERWIG 7, as well as from SHERPA 2 and DIRE 2. A value of the strong
+ coupling at the Z boson mass, $\alpha_{S}(m_{Z}) = 0.115^{+0.015}_{-0.013}$, is extracted from the substructure
+ data at leading-order plus leading-log accuracy.'
+BibKey: Sirunyan:2018asm
+BibTeX: '@article{Sirunyan:2018asm,
+ author = "Sirunyan, A. M. and others",
+ title = "{Measurement of jet substructure observables in
+ $\mathrm{t\overline{t}}$ events from proton-proton
+ collisions at $\sqrt{s}=$ 13TeV}",
+ collaboration = "CMS",
+ journal = "Phys. Rev.",
+ volume = "D98",
+ year = "2018",
+ number = "9",
+ pages = "092014",
+ doi = "10.1103/PhysRevD.98.092014",
+ eprint = "1808.07340",
+ archivePrefix = "arXiv",
+ primaryClass = "hep-ex",
+ reportNumber = "CMS-TOP-17-013, CERN-EP-2018-214",
+ SLACcitation = "%%CITATION = ARXIV:1808.07340;%%"
+}'
diff --git a/analyses/pluginCMS/CMS_2018_I1690148.plot b/analyses/pluginCMS/CMS_2018_I1690148.plot
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1690148.plot
@@ -0,0 +1,1721 @@
+# BEGIN PLOT /CMS_2018_I1690148/*
+LogY=0
+LogX=0
+XTwosidedTicks=1
+YTwosidedTicks=1
+LegendXPos=0.55
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d01-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$\lambda_{0}^{0}$ (N)
+YLabel=1/N dN/d$\lambda_{0}^{0}$ (N)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d01-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$\lambda_{0}^{0}$ (N)
+YLabel=1/N dN/d$\lambda_{0}^{0}$ (N)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d01-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$\lambda_{0}^{0}$ (N)
+YLabel=1/N dN/d$\lambda_{0}^{0}$ (N)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d01-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$\lambda_{0}^{0}$ (N)
+YLabel=1/N dN/d$\lambda_{0}^{0}$ (N)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d02-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+YLabel=1/N dN/d$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d02-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+YLabel=1/N dN/d$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d02-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+YLabel=1/N dN/d$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d02-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+YLabel=1/N dN/d$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d03-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$\lambda_{0.5}^{1}$ (LHA)
+YLabel=1/N dN/d$\lambda_{0.5}^{1}$ (LHA)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d03-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$\lambda_{0.5}^{1}$ (LHA)
+YLabel=1/N dN/d$\lambda_{0.5}^{1}$ (LHA)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d03-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$\lambda_{0.5}^{1}$ (LHA)
+YLabel=1/N dN/d$\lambda_{0.5}^{1}$ (LHA)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d03-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$\lambda_{0.5}^{1}$ (LHA)
+YLabel=1/N dN/d$\lambda_{0.5}^{1}$ (LHA)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d04-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$\lambda_{1}^{1}$ (width)
+YLabel=1/N dN/d$\lambda_{1}^{1}$ (width)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d04-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$\lambda_{1}^{1}$ (width)
+YLabel=1/N dN/d$\lambda_{1}^{1}$ (width)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d04-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$\lambda_{1}^{1}$ (width)
+YLabel=1/N dN/d$\lambda_{1}^{1}$ (width)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d04-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$\lambda_{1}^{1}$ (width)
+YLabel=1/N dN/d$\lambda_{1}^{1}$ (width)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d05-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$\lambda_{2}^{1}$ (thrust)
+YLabel=1/N dN/d$\lambda_{2}^{1}$ (thrust)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d05-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$\lambda_{2}^{1}$ (thrust)
+YLabel=1/N dN/d$\lambda_{2}^{1}$ (thrust)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d05-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$\lambda_{2}^{1}$ (thrust)
+YLabel=1/N dN/d$\lambda_{2}^{1}$ (thrust)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d05-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$\lambda_{2}^{1}$ (thrust)
+YLabel=1/N dN/d$\lambda_{2}^{1}$ (thrust)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d06-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$\varepsilon$
+YLabel=1/N dN/d$\varepsilon$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d06-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$\varepsilon$
+YLabel=1/N dN/d$\varepsilon$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d06-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$\varepsilon$
+YLabel=1/N dN/d$\varepsilon$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d06-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$\varepsilon$
+YLabel=1/N dN/d$\varepsilon$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d07-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$z_{g}$
+YLabel=1/N dN/d$z_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d07-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$z_{g}$
+YLabel=1/N dN/d$z_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d07-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$z_{g}$
+YLabel=1/N dN/d$z_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d07-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$z_{g}$
+YLabel=1/N dN/d$z_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d08-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$\Delta R_{g}$
+YLabel=1/N dN/d$\Delta R_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d08-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$\Delta R_{g}$
+YLabel=1/N dN/d$\Delta R_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d08-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$\Delta R_{g}$
+YLabel=1/N dN/d$\Delta R_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d08-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$\Delta R_{g}$
+YLabel=1/N dN/d$\Delta R_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d09-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$n_{SD}$
+YLabel=1/N dN/d$n_{SD}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d09-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$n_{SD}$
+YLabel=1/N dN/d$n_{SD}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d09-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$n_{SD}$
+YLabel=1/N dN/d$n_{SD}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d09-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$n_{SD}$
+YLabel=1/N dN/d$n_{SD}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d10-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$\tau_{21}$
+YLabel=1/N dN/d$\tau_{21}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d10-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$\tau_{21}$
+YLabel=1/N dN/d$\tau_{21}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d10-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$\tau_{21}$
+YLabel=1/N dN/d$\tau_{21}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d10-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$\tau_{21}$
+YLabel=1/N dN/d$\tau_{21}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d11-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$\tau_{32}$
+YLabel=1/N dN/d$\tau_{32}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d11-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$\tau_{32}$
+YLabel=1/N dN/d$\tau_{32}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d11-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$\tau_{32}$
+YLabel=1/N dN/d$\tau_{32}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d11-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$\tau_{32}$
+YLabel=1/N dN/d$\tau_{32}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d12-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$\tau_{43}$
+YLabel=1/N dN/d$\tau_{43}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d12-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$\tau_{43}$
+YLabel=1/N dN/d$\tau_{43}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d12-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$\tau_{43}$
+YLabel=1/N dN/d$\tau_{43}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d12-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$\tau_{43}$
+YLabel=1/N dN/d$\tau_{43}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d13-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{1}^{(0)}$
+YLabel=1/N dN/d$C_{1}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d13-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{1}^{(0)}$
+YLabel=1/N dN/d$C_{1}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d13-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{1}^{(0)}$
+YLabel=1/N dN/d$C_{1}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d13-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{1}^{(0)}$
+YLabel=1/N dN/d$C_{1}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d14-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{1}^{(0.2)}$
+YLabel=1/N dN/d$C_{1}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d14-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{1}^{(0.2)}$
+YLabel=1/N dN/d$C_{1}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d14-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{1}^{(0.2)}$
+YLabel=1/N dN/d$C_{1}^{(0.2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d14-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{1}^{(0.2)}$
+YLabel=1/N dN/d$C_{1}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d15-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{1}^{(0.5)}$
+YLabel=1/N dN/d$C_{1}^{(0.5)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d15-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{1}^{(0.5)}$
+YLabel=1/N dN/d$C_{1}^{(0.5)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d15-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{1}^{(0.5)}$
+YLabel=1/N dN/d$C_{1}^{(0.5)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d15-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{1}^{(0.5)}$
+YLabel=1/N dN/d$C_{1}^{(0.5)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d16-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{1}^{(1)}$
+YLabel=1/N dN/d$C_{1}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d16-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{1}^{(1)}$
+YLabel=1/N dN/d$C_{1}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d16-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{1}^{(1)}$
+YLabel=1/N dN/d$C_{1}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d16-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{1}^{(1)}$
+YLabel=1/N dN/d$C_{1}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d17-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{1}^{(2)}$
+YLabel=1/N dN/d$C_{1}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d17-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{1}^{(2)}$
+YLabel=1/N dN/d$C_{1}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d17-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{1}^{(2)}$
+YLabel=1/N dN/d$C_{1}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d17-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{1}^{(2)}$
+YLabel=1/N dN/d$C_{1}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d18-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{2}^{(0)}$
+YLabel=1/N dN/d$C_{2}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d18-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{2}^{(0)}$
+YLabel=1/N dN/d$C_{2}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d18-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{2}^{(0)}$
+YLabel=1/N dN/d$C_{2}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d18-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{2}^{(0)}$
+YLabel=1/N dN/d$C_{2}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d19-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{2}^{(0.2)}$
+YLabel=1/N dN/d$C_{2}^{(0.2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d19-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{2}^{(0.2)}$
+YLabel=1/N dN/d$C_{2}^{(0.2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d19-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{2}^{(0.2)}$
+YLabel=1/N dN/d$C_{2}^{(0.2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d19-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{2}^{(0.2)}$
+YLabel=1/N dN/d$C_{2}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d20-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{2}^{(0.5)}$
+YLabel=1/N dN/d$C_{2}^{(0.5)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d20-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{2}^{(0.5)}$
+YLabel=1/N dN/d$C_{2}^{(0.5)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d20-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{2}^{(0.5)}$
+YLabel=1/N dN/d$C_{2}^{(0.5)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d20-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{2}^{(0.5)}$
+YLabel=1/N dN/d$C_{2}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d21-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{2}^{(1)}$
+YLabel=1/N dN/d$C_{2}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d21-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{2}^{(1)}$
+YLabel=1/N dN/d$C_{2}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d21-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{2}^{(1)}$
+YLabel=1/N dN/d$C_{2}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d21-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{2}^{(1)}$
+YLabel=1/N dN/d$C_{2}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d22-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{2}^{(2)}$
+YLabel=1/N dN/d$C_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d22-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{2}^{(2)}$
+YLabel=1/N dN/d$C_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d22-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{2}^{(2)}$
+YLabel=1/N dN/d$C_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d22-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{2}^{(2)}$
+YLabel=1/N dN/d$C_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d23-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{3}^{(0)}$
+YLabel=1/N dN/d$C_{3}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d23-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{3}^{(0)}$
+YLabel=1/N dN/d$C_{3}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d23-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{3}^{(0)}$
+YLabel=1/N dN/d$C_{3}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d23-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{3}^{(0)}$
+YLabel=1/N dN/d$C_{3}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d24-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{3}^{(0.2)}$
+YLabel=1/N dN/d$C_{3}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d24-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{3}^{(0.2)}$
+YLabel=1/N dN/d$C_{3}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d24-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{3}^{(0.2)}$
+YLabel=1/N dN/d$C_{3}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d24-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{3}^{(0.2)}$
+YLabel=1/N dN/d$C_{3}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d25-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{3}^{(0.5)}$
+YLabel=1/N dN/d$C_{3}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d25-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{3}^{(0.5)}$
+YLabel=1/N dN/d$C_{3}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d25-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{3}^{(0.5)}$
+YLabel=1/N dN/d$C_{3}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d25-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{3}^{(0.5)}$
+YLabel=1/N dN/d$C_{3}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d26-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{3}^{(1)}$
+YLabel=1/N dN/d$C_{3}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d26-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{3}^{(1)}$
+YLabel=1/N dN/d$C_{3}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d26-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{3}^{(1)}$
+YLabel=1/N dN/d$C_{3}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d26-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{3}^{(1)}$
+YLabel=1/N dN/d$C_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d27-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$C_{3}^{(2)}$
+YLabel=1/N dN/d$C_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d27-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$C_{3}^{(2)}$
+YLabel=1/N dN/d$C_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d27-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$C_{3}^{(2)}$
+YLabel=1/N dN/d$C_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d27-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$C_{3}^{(2)}$
+YLabel=1/N dN/d$C_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d28-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$M_{2}^{(1)}$
+YLabel=1/N dN/d$M_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d28-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$M_{2}^{(1)}$
+YLabel=1/N dN/d$M_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d28-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$M_{2}^{(1)}$
+YLabel=1/N dN/d$M_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d28-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$M_{2}^{(1)}$
+YLabel=1/N dN/d$M_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d29-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$N_{2}^{(1)}$
+YLabel=1/N dN/d$N_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d29-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$N_{2}^{(1)}$
+YLabel=1/N dN/d$N_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d29-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$N_{2}^{(1)}$
+YLabel=1/N dN/d$N_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d29-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$N_{2}^{(1)}$
+YLabel=1/N dN/d$N_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d30-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$N_{3}^{(1)}$
+YLabel=1/N dN/d$N_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d30-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$N_{3}^{(1)}$
+YLabel=1/N dN/d$N_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d30-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$N_{3}^{(1)}$
+YLabel=1/N dN/d$N_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d30-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$N_{3}^{(1)}$
+YLabel=1/N dN/d$N_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d31-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$M_{2}^{(2)}$
+YLabel=1/N dN/d$M_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d31-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$M_{2}^{(2)}$
+YLabel=1/N dN/d$M_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d31-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$M_{2}^{(2)}$
+YLabel=1/N dN/d$M_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d31-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$M_{2}^{(2)}$
+YLabel=1/N dN/d$M_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d32-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$N_{2}^{(2)}$
+YLabel=1/N dN/d$N_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d32-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$N_{2}^{(2)}$
+YLabel=1/N dN/d$N_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d32-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$N_{2}^{(2)}$
+YLabel=1/N dN/d$N_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d32-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$N_{2}^{(2)}$
+YLabel=1/N dN/d$N_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d33-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, charged particles
+XLabel=$N_{3}^{(2)}$
+YLabel=1/N dN/d$N_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d33-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, charged particles
+XLabel=$N_{3}^{(2)}$
+YLabel=1/N dN/d$N_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d33-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, charged particles
+XLabel=$N_{3}^{(2)}$
+YLabel=1/N dN/d$N_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d33-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, charged particles
+XLabel=$N_{3}^{(2)}$
+YLabel=1/N dN/d$N_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d34-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$\lambda_{0}^{0}$ (N)
+YLabel=1/N dN/d$\lambda_{0}^{0}$ (N)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d34-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$\lambda_{0}^{0}$ (N)
+YLabel=1/N dN/d$\lambda_{0}^{0}$ (N)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d34-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$\lambda_{0}^{0}$ (N)
+YLabel=1/N dN/d$\lambda_{0}^{0}$ (N)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d34-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$\lambda_{0}^{0}$ (N)
+YLabel=1/N dN/d$\lambda_{0}^{0}$ (N)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d35-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+YLabel=1/N dN/d$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d35-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+YLabel=1/N dN/d$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d35-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+YLabel=1/N dN/d$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d35-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+YLabel=1/N dN/d$\lambda_{0}^{2}$ ($p_{T}^{d,*})$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d36-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$\lambda_{0.5}^{1}$ (LHA)
+YLabel=1/N dN/d$\lambda_{0.5}^{1}$ (LHA)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d36-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$\lambda_{0.5}^{1}$ (LHA)
+YLabel=1/N dN/d$\lambda_{0.5}^{1}$ (LHA)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d36-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$\lambda_{0.5}^{1}$ (LHA)
+YLabel=1/N dN/d$\lambda_{0.5}^{1}$ (LHA)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d36-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$\lambda_{0.5}^{1}$ (LHA)
+YLabel=1/N dN/d$\lambda_{0.5}^{1}$ (LHA)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d37-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$\lambda_{1}^{1}$ (width)
+YLabel=1/N dN/d$\lambda_{1}^{1}$ (width)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d37-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$\lambda_{1}^{1}$ (width)
+YLabel=1/N dN/d$\lambda_{1}^{1}$ (width)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d37-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$\lambda_{1}^{1}$ (width)
+YLabel=1/N dN/d$\lambda_{1}^{1}$ (width)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d37-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$\lambda_{1}^{1}$ (width)
+YLabel=1/N dN/d$\lambda_{1}^{1}$ (width)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d38-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$\lambda_{2}^{1}$ (thrust)
+YLabel=1/N dN/d$\lambda_{2}^{1}$ (thrust)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d38-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$\lambda_{2}^{1}$ (thrust)
+YLabel=1/N dN/d$\lambda_{2}^{1}$ (thrust)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d38-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$\lambda_{2}^{1}$ (thrust)
+YLabel=1/N dN/d$\lambda_{2}^{1}$ (thrust)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d38-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$\lambda_{2}^{1}$ (thrust)
+YLabel=1/N dN/d$\lambda_{2}^{1}$ (thrust)
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d39-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$\varepsilon$
+YLabel=1/N dN/d$\varepsilon$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d39-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$\varepsilon$
+YLabel=1/N dN/d$\varepsilon$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d39-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$\varepsilon$
+YLabel=1/N dN/d$\varepsilon$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d39-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$\varepsilon$
+YLabel=1/N dN/d$\varepsilon$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d40-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$z_{g}$
+YLabel=1/N dN/d$z_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d40-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$z_{g}$
+YLabel=1/N dN/d$z_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d40-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$z_{g}$
+YLabel=1/N dN/d$z_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d40-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$z_{g}$
+YLabel=1/N dN/d$z_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d41-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$\Delta R_{g}$
+YLabel=1/N dN/d$\Delta R_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d41-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$\Delta R_{g}$
+YLabel=1/N dN/d$\Delta R_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d41-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$\Delta R_{g}$
+YLabel=1/N dN/d$\Delta R_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d41-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$\Delta R_{g}$
+YLabel=1/N dN/d$\Delta R_{g}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d42-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$n_{SD}$
+YLabel=1/N dN/d$n_{SD}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d42-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$n_{SD}$
+YLabel=1/N dN/d$n_{SD}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d42-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$n_{SD}$
+YLabel=1/N dN/d$n_{SD}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d42-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$n_{SD}$
+YLabel=1/N dN/d$n_{SD}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d43-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$\tau_{21}$
+YLabel=1/N dN/d$\tau_{21}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d43-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$\tau_{21}$
+YLabel=1/N dN/d$\tau_{21}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d43-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$\tau_{21}$
+YLabel=1/N dN/d$\tau_{21}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d43-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$\tau_{21}$
+YLabel=1/N dN/d$\tau_{21}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d44-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$\tau_{32}$
+YLabel=1/N dN/d$\tau_{32}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d44-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$\tau_{32}$
+YLabel=1/N dN/d$\tau_{32}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d44-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$\tau_{32}$
+YLabel=1/N dN/d$\tau_{32}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d44-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$\tau_{32}$
+YLabel=1/N dN/d$\tau_{32}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d45-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$\tau_{43}$
+YLabel=1/N dN/d$\tau_{43}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d45-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$\tau_{43}$
+YLabel=1/N dN/d$\tau_{43}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d45-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$\tau_{43}$
+YLabel=1/N dN/d$\tau_{43}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d45-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$\tau_{43}$
+YLabel=1/N dN/d$\tau_{43}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d46-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{1}^{(0)}$
+YLabel=1/N dN/d$C_{1}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d46-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{1}^{(0)}$
+YLabel=1/N dN/d$C_{1}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d46-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{1}^{(0)}$
+YLabel=1/N dN/d$C_{1}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d46-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{1}^{(0)}$
+YLabel=1/N dN/d$C_{1}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d47-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{1}^{(0.2)}$
+YLabel=1/N dN/d$C_{1}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d47-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{1}^{(0.2)}$
+YLabel=1/N dN/d$C_{1}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d47-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{1}^{(0.2)}$
+YLabel=1/N dN/d$C_{1}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d47-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{1}^{(0.2)}$
+YLabel=1/N dN/d$C_{1}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d48-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{1}^{(0.5)}$
+YLabel=1/N dN/d$C_{1}^{(0.5)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d48-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{1}^{(0.5)}$
+YLabel=1/N dN/d$C_{1}^{(0.5)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d48-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{1}^{(0.5)}$
+YLabel=1/N dN/d$C_{1}^{(0.5)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d48-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{1}^{(0.5)}$
+YLabel=1/N dN/d$C_{1}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d49-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{1}^{(1)}$
+YLabel=1/N dN/d$C_{1}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d49-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{1}^{(1)}$
+YLabel=1/N dN/d$C_{1}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d49-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{1}^{(1)}$
+YLabel=1/N dN/d$C_{1}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d49-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{1}^{(1)}$
+YLabel=1/N dN/d$C_{1}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d50-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{1}^{(2)}$
+YLabel=1/N dN/d$C_{1}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d50-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{1}^{(2)}$
+YLabel=1/N dN/d$C_{1}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d50-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{1}^{(2)}$
+YLabel=1/N dN/d$C_{1}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d50-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{1}^{(2)}$
+YLabel=1/N dN/d$C_{1}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d51-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{2}^{(0)}$
+YLabel=1/N dN/d$C_{2}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d51-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{2}^{(0)}$
+YLabel=1/N dN/d$C_{2}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d51-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{2}^{(0)}$
+YLabel=1/N dN/d$C_{2}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d51-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{2}^{(0)}$
+YLabel=1/N dN/d$C_{2}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d52-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{2}^{(0.2)}$
+YLabel=1/N dN/d$C_{2}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d52-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{2}^{(0.2)}$
+YLabel=1/N dN/d$C_{2}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d52-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{2}^{(0.2)}$
+YLabel=1/N dN/d$C_{2}^{(0.2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d52-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{2}^{(0.2)}$
+YLabel=1/N dN/d$C_{2}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d53-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{2}^{(0.5)}$
+YLabel=1/N dN/d$C_{2}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d53-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{2}^{(0.5)}$
+YLabel=1/N dN/d$C_{2}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d53-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{2}^{(0.5)}$
+YLabel=1/N dN/d$C_{2}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d53-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{2}^{(0.5)}$
+YLabel=1/N dN/d$C_{2}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d54-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{2}^{(1)}$
+YLabel=1/N dN/d$C_{2}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d54-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{2}^{(1)}$
+YLabel=1/N dN/d$C_{2}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d54-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{2}^{(1)}$
+YLabel=1/N dN/d$C_{2}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d54-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{2}^{(1)}$
+YLabel=1/N dN/d$C_{2}^{(1)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d55-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{2}^{(2)}$
+YLabel=1/N dN/d$C_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d55-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{2}^{(2)}$
+YLabel=1/N dN/d$C_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d55-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{2}^{(2)}$
+YLabel=1/N dN/d$C_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d55-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{2}^{(2)}$
+YLabel=1/N dN/d$C_{2}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d56-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{3}^{(0)}$
+YLabel=1/N dN/d$C_{3}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d56-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{3}^{(0)}$
+YLabel=1/N dN/d$C_{3}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d56-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{3}^{(0)}$
+YLabel=1/N dN/d$C_{3}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d56-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{3}^{(0)}$
+YLabel=1/N dN/d$C_{3}^{(0)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d57-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{3}^{(0.2)}$
+YLabel=1/N dN/d$C_{3}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d57-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{3}^{(0.2)}$
+YLabel=1/N dN/d$C_{3}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d57-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{3}^{(0.2)}$
+YLabel=1/N dN/d$C_{3}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d57-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{3}^{(0.2)}$
+YLabel=1/N dN/d$C_{3}^{(0.2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d58-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{3}^{(0.5)}$
+YLabel=1/N dN/d$C_{3}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d58-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{3}^{(0.5)}$
+YLabel=1/N dN/d$C_{3}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d58-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{3}^{(0.5)}$
+YLabel=1/N dN/d$C_{3}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d58-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{3}^{(0.5)}$
+YLabel=1/N dN/d$C_{3}^{(0.5)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d59-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{3}^{(1)}$
+YLabel=1/N dN/d$C_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d59-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{3}^{(1)}$
+YLabel=1/N dN/d$C_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d59-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{3}^{(1)}$
+YLabel=1/N dN/d$C_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d59-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{3}^{(1)}$
+YLabel=1/N dN/d$C_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d60-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$C_{3}^{(2)}$
+YLabel=1/N dN/d$C_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d60-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$C_{3}^{(2)}$
+YLabel=1/N dN/d$C_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d60-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$C_{3}^{(2)}$
+YLabel=1/N dN/d$C_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d60-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$C_{3}^{(2)}$
+YLabel=1/N dN/d$C_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d61-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$M_{2}^{(1)}$
+YLabel=1/N dN/d$M_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d61-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$M_{2}^{(1)}$
+YLabel=1/N dN/d$M_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d61-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$M_{2}^{(1)}$
+YLabel=1/N dN/d$M_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d61-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$M_{2}^{(1)}$
+YLabel=1/N dN/d$M_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d62-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$N_{2}^{(1)}$
+YLabel=1/N dN/d$N_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d62-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$N_{2}^{(1)}$
+YLabel=1/N dN/d$N_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d62-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$N_{2}^{(1)}$
+YLabel=1/N dN/d$N_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d62-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$N_{2}^{(1)}$
+YLabel=1/N dN/d$N_{2}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d63-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$N_{3}^{(1)}$
+YLabel=1/N dN/d$N_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d63-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$N_{3}^{(1)}$
+YLabel=1/N dN/d$N_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d63-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$N_{3}^{(1)}$
+YLabel=1/N dN/d$N_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d63-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$N_{3}^{(1)}$
+YLabel=1/N dN/d$N_{3}^{(1)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d64-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$M_{2}^{(2)}$
+YLabel=1/N dN/d$M_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d64-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$M_{2}^{(2)}$
+YLabel=1/N dN/d$M_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d64-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$M_{2}^{(2)}$
+YLabel=1/N dN/d$M_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d64-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$M_{2}^{(2)}$
+YLabel=1/N dN/d$M_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d65-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$N_{2}^{(2)}$
+YLabel=1/N dN/d$N_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d65-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$N_{2}^{(2)}$
+YLabel=1/N dN/d$N_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d65-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$N_{2}^{(2)}$
+YLabel=1/N dN/d$N_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d65-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$N_{2}^{(2)}$
+YLabel=1/N dN/d$N_{2}^{(2)}$
+LegendXPos=0.05
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d66-x01-y01
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, incl jets, all particles
+XLabel=$N_{3}^{(2)}$
+YLabel=1/N dN/d$N_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d66-x01-y02
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, bottom jets, all particles
+XLabel=$N_{3}^{(2)}$
+YLabel=1/N dN/d$N_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d66-x01-y03
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, light jets, all particles
+XLabel=$N_{3}^{(2)}$
+YLabel=1/N dN/d$N_{3}^{(2)}$
+# END PLOT
+
+# BEGIN PLOT /CMS_2018_I1690148/d66-x01-y04
+Title=CMS, 13 TeV, $t\bar{t}$ lepton+jets, gluon jets, all particles
+XLabel=$N_{3}^{(2)}$
+YLabel=1/N dN/d$N_{3}^{(2)}$
+# END PLOT
diff --git a/analyses/pluginCMS/CMS_2018_I1690148.yoda b/analyses/pluginCMS/CMS_2018_I1690148.yoda
new file mode 100644
--- /dev/null
+++ b/analyses/pluginCMS/CMS_2018_I1690148.yoda
@@ -0,0 +1,3132 @@
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d01-x01-y01
+Path=/REF/CMS_2018_I1690148/d01-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+00 1.500000e+00 1.500000e+00 3.068700e-02 3.428569e-03 3.188483e-03
+4.000000e+00 1.000000e+00 1.000000e+00 1.307100e-01 9.342085e-03 8.428131e-03
+6.000000e+00 1.000000e+00 1.000000e+00 1.473200e-01 2.462668e-03 2.780886e-03
+8.000000e+00 1.000000e+00 1.000000e+00 9.890700e-02 4.680102e-03 5.527589e-03
+1.000000e+01 1.000000e+00 1.000000e+00 4.571200e-02 4.594459e-03 5.051157e-03
+1.150000e+01 5.000000e-01 5.000000e-01 2.357600e-02 4.616802e-03 4.460861e-03
+1.300000e+01 1.000000e+00 1.000000e+00 1.097700e-02 1.363611e-03 2.388624e-03
+1.500000e+01 1.000000e+00 1.000000e+00 5.477200e-03 1.333892e-03 1.157311e-03
+2.300000e+01 7.000000e+00 7.000000e+00 4.388600e-04 1.286309e-04 1.527141e-04
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d01-x01-y02
+Path=/REF/CMS_2018_I1690148/d01-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+00 1.500000e+00 1.500000e+00 2.351300e-02 5.840971e-03 4.782906e-03
+4.000000e+00 1.000000e+00 1.000000e+00 1.054000e-01 1.046906e-02 1.157122e-02
+6.000000e+00 1.000000e+00 1.000000e+00 1.484000e-01 5.501301e-03 4.306286e-03
+8.000000e+00 1.000000e+00 1.000000e+00 1.157000e-01 6.991174e-03 7.328836e-03
+1.000000e+01 1.000000e+00 1.000000e+00 5.832400e-02 7.034833e-03 8.570393e-03
+1.150000e+01 5.000000e-01 5.000000e-01 2.745900e-02 7.374771e-03 6.389653e-03
+1.300000e+01 1.000000e+00 1.000000e+00 1.454100e-02 2.215298e-03 2.879889e-03
+1.500000e+01 1.000000e+00 1.000000e+00 5.955700e-03 1.734195e-03 2.175353e-03
+2.300000e+01 7.000000e+00 7.000000e+00 3.838300e-04 1.921280e-04 1.959904e-04
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d01-x01-y03
+Path=/REF/CMS_2018_I1690148/d01-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+00 1.500000e+00 1.500000e+00 4.438600e-02 3.983963e-03 3.375279e-03
+4.000000e+00 1.000000e+00 1.000000e+00 1.605700e-01 9.078751e-03 6.896409e-03
+6.000000e+00 1.000000e+00 1.000000e+00 1.486300e-01 2.190487e-03 4.203461e-03
+8.000000e+00 1.000000e+00 1.000000e+00 7.936200e-02 5.114759e-03 5.579236e-03
+1.000000e+01 1.000000e+00 1.000000e+00 2.954300e-02 3.158420e-03 3.629785e-03
+1.150000e+01 5.000000e-01 5.000000e-01 1.520800e-02 3.192406e-03 3.718798e-03
+1.300000e+01 1.000000e+00 1.000000e+00 4.468200e-03 8.788269e-04 1.883180e-03
+1.500000e+01 1.000000e+00 1.000000e+00 2.594000e-03 1.068166e-03 4.311480e-04
+2.300000e+01 7.000000e+00 7.000000e+00 9.250900e-05 3.076011e-05 5.623822e-05
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d01-x01-y04
+Path=/REF/CMS_2018_I1690148/d01-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+00 1.500000e+00 1.500000e+00 2.037800e-02 2.414540e-03 5.647009e-03
+4.000000e+00 1.000000e+00 1.000000e+00 9.634600e-02 1.124718e-02 9.219264e-03
+6.000000e+00 1.000000e+00 1.000000e+00 1.258700e-01 1.034944e-02 4.598092e-03
+8.000000e+00 1.000000e+00 1.000000e+00 1.058500e-01 4.315962e-03 1.102058e-02
+1.000000e+01 1.000000e+00 1.000000e+00 6.102100e-02 1.012643e-02 6.264368e-03
+1.150000e+01 5.000000e-01 5.000000e-01 4.085300e-02 1.603477e-02 1.614464e-02
+1.300000e+01 1.000000e+00 1.000000e+00 2.728100e-02 5.584087e-03 9.071668e-03
+1.500000e+01 1.000000e+00 1.000000e+00 1.607400e-02 5.380431e-03 2.624344e-03
+2.300000e+01 7.000000e+00 7.000000e+00 2.367600e-03 6.505432e-04 6.689120e-04
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d02-x01-y01
+Path=/REF/CMS_2018_I1690148/d02-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+9.000000e-02 9.000000e-02 9.000000e-02 6.049800e-01 3.177035e-02 1.217042e-02
+2.100000e-01 3.000000e-02 3.000000e-02 2.679300e+00 8.905530e-02 1.244722e-01
+2.700000e-01 3.000000e-02 3.000000e-02 3.051200e+00 6.990035e-02 1.085288e-01
+3.400000e-01 4.000000e-02 4.000000e-02 2.561200e+00 6.061295e-02 4.665073e-02
+4.200000e-01 4.000000e-02 4.000000e-02 1.713500e+00 4.020347e-02 5.128512e-02
+5.100000e-01 5.000000e-02 5.000000e-02 9.882300e-01 4.127747e-02 2.459756e-02
+7.800000e-01 2.200000e-01 2.200000e-01 2.419800e-01 1.824527e-02 1.606969e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d02-x01-y02
+Path=/REF/CMS_2018_I1690148/d02-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+9.000000e-02 9.000000e-02 9.000000e-02 5.831400e-01 3.344284e-02 3.145020e-02
+2.100000e-01 3.000000e-02 3.000000e-02 2.977000e+00 1.316175e-01 1.796261e-01
+2.700000e-01 3.000000e-02 3.000000e-02 3.325500e+00 1.257653e-01 1.112177e-01
+3.400000e-01 4.000000e-02 4.000000e-02 2.589300e+00 9.224229e-02 7.253618e-02
+4.200000e-01 4.000000e-02 4.000000e-02 1.624300e+00 5.742312e-02 8.260558e-02
+5.100000e-01 5.000000e-02 5.000000e-02 9.066300e-01 8.365841e-02 3.615729e-02
+7.800000e-01 2.200000e-01 2.200000e-01 2.025900e-01 2.309872e-02 2.520804e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d02-x01-y03
+Path=/REF/CMS_2018_I1690148/d02-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+9.000000e-02 9.000000e-02 9.000000e-02 6.268000e-01 3.752936e-02 1.348304e-02
+2.100000e-01 3.000000e-02 3.000000e-02 2.360100e+00 7.384644e-02 1.042525e-01
+2.700000e-01 3.000000e-02 3.000000e-02 2.754600e+00 5.179944e-02 1.560684e-01
+3.400000e-01 4.000000e-02 4.000000e-02 2.481000e+00 7.466134e-02 4.957803e-02
+4.200000e-01 4.000000e-02 4.000000e-02 1.816500e+00 5.018274e-02 4.780347e-02
+5.100000e-01 5.000000e-02 5.000000e-02 1.090100e+00 3.210724e-02 2.972302e-02
+7.800000e-01 2.200000e-01 2.200000e-01 2.897300e-01 1.727965e-02 1.357566e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d02-x01-y04
+Path=/REF/CMS_2018_I1690148/d02-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+9.000000e-02 9.000000e-02 9.000000e-02 5.720600e-01 4.980457e-02 3.774789e-02
+2.100000e-01 3.000000e-02 3.000000e-02 2.864900e+00 1.731385e-01 1.621447e-01
+2.700000e-01 3.000000e-02 3.000000e-02 3.171200e+00 1.571492e-01 1.704014e-01
+3.400000e-01 4.000000e-02 4.000000e-02 2.754000e+00 9.241209e-02 1.461711e-01
+4.200000e-01 4.000000e-02 4.000000e-02 1.686200e+00 1.428777e-01 1.220582e-01
+5.100000e-01 5.000000e-02 5.000000e-02 8.553900e-01 7.531086e-02 1.118733e-01
+7.800000e-01 2.200000e-01 2.200000e-01 2.138900e-01 2.038834e-02 1.193777e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d03-x01-y01
+Path=/REF/CMS_2018_I1690148/d03-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 9.360100e-01 5.446309e-02 5.019807e-02
+2.200000e-01 2.000000e-02 2.000000e-02 2.515100e+00 1.035162e-01 8.450579e-02
+2.800000e-01 4.000000e-02 4.000000e-02 2.979100e+00 3.207006e-02 6.003380e-02
+3.500000e-01 3.000000e-02 3.000000e-02 2.683300e+00 6.728625e-02 6.583729e-02
+4.000000e-01 2.000000e-02 2.000000e-02 2.197700e+00 7.437011e-02 8.087154e-02
+4.500000e-01 3.000000e-02 3.000000e-02 1.660700e+00 4.979066e-02 8.105083e-02
+5.200000e-01 4.000000e-02 4.000000e-02 9.878700e-01 6.310374e-02 3.021993e-02
+6.100000e-01 5.000000e-02 5.000000e-02 3.865100e-01 1.829602e-02 2.040727e-02
+8.300000e-01 1.700000e-01 1.700000e-01 2.247700e-02 4.073294e-03 2.735591e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d03-x01-y02
+Path=/REF/CMS_2018_I1690148/d03-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 7.571200e-01 8.249823e-02 7.030175e-02
+2.200000e-01 2.000000e-02 2.000000e-02 2.308000e+00 8.454346e-02 1.860576e-01
+2.800000e-01 4.000000e-02 4.000000e-02 3.156100e+00 6.330679e-02 5.992201e-02
+3.500000e-01 3.000000e-02 3.000000e-02 3.018300e+00 1.383749e-01 8.638275e-02
+4.000000e-01 2.000000e-02 2.000000e-02 2.422000e+00 1.158275e-01 1.684225e-01
+4.500000e-01 3.000000e-02 3.000000e-02 1.751400e+00 7.647870e-02 1.242162e-01
+5.200000e-01 4.000000e-02 4.000000e-02 9.997500e-01 6.944472e-02 4.301467e-02
+6.100000e-01 5.000000e-02 5.000000e-02 3.548300e-01 1.893594e-02 2.945223e-02
+8.300000e-01 1.700000e-01 1.700000e-01 1.542000e-02 9.636098e-03 6.615589e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d03-x01-y03
+Path=/REF/CMS_2018_I1690148/d03-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 1.124200e+00 4.248127e-02 4.008688e-02
+2.200000e-01 2.000000e-02 2.000000e-02 2.742800e+00 2.256667e-01 8.205412e-02
+2.800000e-01 4.000000e-02 4.000000e-02 2.872700e+00 4.156897e-02 8.829330e-02
+3.500000e-01 3.000000e-02 3.000000e-02 2.397800e+00 6.037704e-02 8.634659e-02
+4.000000e-01 2.000000e-02 2.000000e-02 1.959300e+00 1.007774e-01 8.703909e-02
+4.500000e-01 3.000000e-02 3.000000e-02 1.540200e+00 6.866949e-02 7.113284e-02
+5.200000e-01 4.000000e-02 4.000000e-02 9.016400e-01 4.143462e-02 3.696788e-02
+6.100000e-01 5.000000e-02 5.000000e-02 4.029700e-01 2.114563e-02 2.779404e-02
+8.300000e-01 1.700000e-01 1.700000e-01 2.514700e-02 4.919703e-03 3.034812e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d03-x01-y04
+Path=/REF/CMS_2018_I1690148/d03-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-01 1.000000e-01 1.000000e-01 9.470000e-01 5.632758e-02 5.127970e-02
+2.200000e-01 2.000000e-02 2.000000e-02 2.261100e+00 2.015157e-01 2.682643e-01
+2.800000e-01 4.000000e-02 4.000000e-02 2.613400e+00 1.288155e-01 1.213156e-01
+3.500000e-01 3.000000e-02 3.000000e-02 2.529900e+00 1.627060e-01 1.901354e-01
+4.000000e-01 2.000000e-02 2.000000e-02 2.180700e+00 2.669366e-01 1.842487e-01
+4.500000e-01 3.000000e-02 3.000000e-02 1.898100e+00 2.799568e-01 1.009524e-01
+5.200000e-01 4.000000e-02 4.000000e-02 1.248400e+00 8.246392e-02 2.686987e-01
+6.100000e-01 5.000000e-02 5.000000e-02 4.589700e-01 1.198522e-01 8.209787e-02
+8.300000e-01 1.700000e-01 1.700000e-01 3.648700e-02 7.467236e-03 6.033548e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d04-x01-y01
+Path=/REF/CMS_2018_I1690148/d04-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-02 3.500000e-02 3.500000e-02 1.502200e+00 1.150490e-01 9.327989e-02
+9.500000e-02 2.500000e-02 2.500000e-02 3.671000e+00 7.108730e-02 7.821159e-02
+1.450000e-01 2.500000e-02 2.500000e-02 3.847800e+00 6.344829e-02 9.892484e-02
+1.900000e-01 2.000000e-02 2.000000e-02 3.192700e+00 1.258798e-01 5.483110e-02
+2.400000e-01 3.000000e-02 3.000000e-02 2.430400e+00 5.529029e-02 6.250213e-02
+3.000000e-01 3.000000e-02 3.000000e-02 1.666200e+00 8.672601e-02 3.051678e-02
+3.600000e-01 3.000000e-02 3.000000e-02 1.021800e+00 2.508222e-02 7.814928e-02
+4.350000e-01 4.500000e-02 4.500000e-02 5.913700e-01 5.184192e-02 2.750412e-02
+7.400000e-01 2.600000e-01 2.600000e-01 5.937500e-02 1.203434e-02 1.627630e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d04-x01-y02
+Path=/REF/CMS_2018_I1690148/d04-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-02 3.500000e-02 3.500000e-02 1.146000e+00 1.489477e-01 1.302745e-01
+9.500000e-02 2.500000e-02 2.500000e-02 3.502300e+00 6.351878e-02 1.270757e-01
+1.450000e-01 2.500000e-02 2.500000e-02 4.116900e+00 1.327464e-01 8.340752e-02
+1.900000e-01 2.000000e-02 2.000000e-02 3.507200e+00 1.832340e-01 1.026828e-01
+2.400000e-01 3.000000e-02 3.000000e-02 2.612100e+00 7.662353e-02 1.128808e-01
+3.000000e-01 3.000000e-02 3.000000e-02 1.737400e+00 9.873238e-02 8.678746e-02
+3.600000e-01 3.000000e-02 3.000000e-02 1.037700e+00 5.126065e-02 9.919475e-02
+4.350000e-01 4.500000e-02 4.500000e-02 5.326700e-01 2.762401e-02 3.870836e-02
+7.400000e-01 2.600000e-01 2.600000e-01 5.262100e-02 5.319904e-03 6.316940e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d04-x01-y03
+Path=/REF/CMS_2018_I1690148/d04-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-02 3.500000e-02 3.500000e-02 1.811700e+00 8.880241e-02 7.983399e-02
+9.500000e-02 2.500000e-02 2.500000e-02 3.885600e+00 1.047387e-01 9.247025e-02
+1.450000e-01 2.500000e-02 2.500000e-02 3.696600e+00 6.657120e-02 1.444118e-01
+1.900000e-01 2.000000e-02 2.000000e-02 2.970400e+00 1.050547e-01 1.021348e-01
+2.400000e-01 3.000000e-02 3.000000e-02 2.231800e+00 6.047705e-02 6.359759e-02
+3.000000e-01 3.000000e-02 3.000000e-02 1.542400e+00 7.379189e-02 4.854433e-02
+3.600000e-01 3.000000e-02 3.000000e-02 1.012400e+00 5.403433e-02 5.216278e-02
+4.350000e-01 4.500000e-02 4.500000e-02 5.790400e-01 4.057313e-02 2.452339e-02
+7.400000e-01 2.600000e-01 2.600000e-01 6.910200e-02 4.131045e-03 8.110299e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d04-x01-y04
+Path=/REF/CMS_2018_I1690148/d04-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-02 3.500000e-02 3.500000e-02 1.771100e+00 1.158117e-01 1.278447e-01
+9.500000e-02 2.500000e-02 2.500000e-02 3.230900e+00 1.367918e-01 1.659228e-01
+1.450000e-01 2.500000e-02 2.500000e-02 3.309400e+00 1.363272e-01 2.318168e-01
+1.900000e-01 2.000000e-02 2.000000e-02 2.758900e+00 1.990118e-01 1.752016e-01
+2.400000e-01 3.000000e-02 3.000000e-02 2.520100e+00 1.796757e-01 1.453932e-01
+3.000000e-01 3.000000e-02 3.000000e-02 1.822300e+00 2.181225e-01 1.359469e-01
+3.600000e-01 3.000000e-02 3.000000e-02 1.094300e+00 1.336757e-01 1.787148e-01
+4.350000e-01 4.500000e-02 4.500000e-02 8.653900e-01 1.097537e-01 7.768058e-02
+7.400000e-01 2.600000e-01 2.600000e-01 6.648100e-02 2.687523e-02 2.082659e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d05-x01-y01
+Path=/REF/CMS_2018_I1690148/d05-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-02 3.500000e-02 3.500000e-02 6.828800e+00 1.234611e-01 1.351000e-01
+9.000000e-02 2.000000e-02 2.000000e-02 4.180300e+00 2.428331e-01 2.191961e-01
+1.350000e-01 2.500000e-02 2.500000e-02 2.680300e+00 5.893610e-02 6.034848e-02
+2.000000e-01 4.000000e-02 4.000000e-02 1.443700e+00 3.964272e-02 2.919765e-02
+2.750000e-01 3.500000e-02 3.500000e-02 7.462800e-01 3.366064e-02 2.176060e-02
+4.050000e-01 9.500000e-02 9.500000e-02 2.790600e-01 1.307684e-02 2.151847e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d05-x01-y02
+Path=/REF/CMS_2018_I1690148/d05-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-02 3.500000e-02 3.500000e-02 6.772900e+00 1.430556e-01 1.427438e-01
+9.000000e-02 2.000000e-02 2.000000e-02 4.427300e+00 2.878255e-01 2.092673e-01
+1.350000e-01 2.500000e-02 2.500000e-02 2.775000e+00 7.453146e-02 1.024084e-01
+2.000000e-01 4.000000e-02 4.000000e-02 1.428100e+00 6.013236e-02 3.763686e-02
+2.750000e-01 3.500000e-02 3.500000e-02 6.980500e-01 6.522547e-02 2.900437e-02
+4.050000e-01 9.500000e-02 9.500000e-02 2.470400e-01 1.831314e-02 5.599834e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d05-x01-y03
+Path=/REF/CMS_2018_I1690148/d05-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-02 3.500000e-02 3.500000e-02 6.969400e+00 1.322195e-01 1.550465e-01
+9.000000e-02 2.000000e-02 2.000000e-02 4.034100e+00 2.174722e-01 2.016379e-01
+1.350000e-01 2.500000e-02 2.500000e-02 2.557200e+00 8.852923e-02 7.861058e-02
+2.000000e-01 4.000000e-02 4.000000e-02 1.428100e+00 4.328848e-02 4.733805e-02
+2.750000e-01 3.500000e-02 3.500000e-02 7.641400e-01 4.003894e-02 4.550534e-02
+4.050000e-01 9.500000e-02 9.500000e-02 2.903800e-01 2.573995e-02 2.035197e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d05-x01-y04
+Path=/REF/CMS_2018_I1690148/d05-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.500000e-02 3.500000e-02 3.500000e-02 6.310500e+00 1.703254e-01 2.568879e-01
+9.000000e-02 2.000000e-02 2.000000e-02 3.825600e+00 3.150697e-01 3.430326e-01
+1.350000e-01 2.500000e-02 2.500000e-02 2.907800e+00 2.040171e-01 1.805178e-01
+2.000000e-01 4.000000e-02 4.000000e-02 1.601300e+00 1.356180e-01 9.241834e-02
+2.750000e-01 3.500000e-02 3.500000e-02 8.778700e-01 7.197645e-02 1.479208e-01
+4.050000e-01 9.500000e-02 9.500000e-02 3.699800e-01 8.699607e-02 6.918461e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d06-x01-y01
+Path=/REF/CMS_2018_I1690148/d06-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.072400e-01 5.756498e-03 1.216757e-02
+4.500000e-01 5.000000e-02 5.000000e-02 6.005700e-01 3.734793e-02 3.812108e-02
+5.400000e-01 4.000000e-02 4.000000e-02 8.972100e-01 5.853474e-02 3.811952e-02
+6.200000e-01 4.000000e-02 4.000000e-02 1.174200e+00 5.288092e-02 5.011638e-02
+7.000000e-01 4.000000e-02 4.000000e-02 1.595600e+00 4.528813e-02 6.143627e-02
+7.800000e-01 4.000000e-02 4.000000e-02 1.901000e+00 7.971629e-02 1.006958e-01
+9.100000e-01 9.000000e-02 9.000000e-02 2.286700e+00 9.776790e-02 7.764499e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d06-x01-y02
+Path=/REF/CMS_2018_I1690148/d06-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.145200e-01 8.054350e-03 1.875044e-02
+4.500000e-01 5.000000e-02 5.000000e-02 6.655900e-01 4.474240e-02 5.559943e-02
+5.400000e-01 4.000000e-02 4.000000e-02 8.938600e-01 7.651342e-02 6.748756e-02
+6.200000e-01 4.000000e-02 4.000000e-02 1.197000e+00 8.859498e-02 7.600160e-02
+7.000000e-01 4.000000e-02 4.000000e-02 1.651200e+00 9.354027e-02 7.464224e-02
+7.800000e-01 4.000000e-02 4.000000e-02 1.858900e+00 1.224812e-01 1.095607e-01
+9.100000e-01 9.000000e-02 9.000000e-02 2.219700e+00 1.203478e-01 1.077262e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d06-x01-y03
+Path=/REF/CMS_2018_I1690148/d06-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 1.972800e-01 8.111048e-03 1.071901e-02
+4.500000e-01 5.000000e-02 5.000000e-02 5.405500e-01 6.437207e-02 4.520429e-02
+5.400000e-01 4.000000e-02 4.000000e-02 8.758100e-01 7.950952e-02 5.833244e-02
+6.200000e-01 4.000000e-02 4.000000e-02 1.116500e+00 4.373920e-02 4.903231e-02
+7.000000e-01 4.000000e-02 4.000000e-02 1.540100e+00 6.089689e-02 7.566649e-02
+7.800000e-01 4.000000e-02 4.000000e-02 1.908500e+00 6.788948e-02 1.365249e-01
+9.100000e-01 9.000000e-02 9.000000e-02 2.398700e+00 8.573452e-02 6.585913e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d06-x01-y04
+Path=/REF/CMS_2018_I1690148/d06-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-01 2.000000e-01 2.000000e-01 2.119300e-01 1.792069e-02 1.625077e-02
+4.500000e-01 5.000000e-02 5.000000e-02 5.642700e-01 8.162126e-02 1.036061e-01
+5.400000e-01 4.000000e-02 4.000000e-02 9.504000e-01 1.785657e-01 1.099423e-01
+6.200000e-01 4.000000e-02 4.000000e-02 1.345000e+00 1.943261e-01 1.135200e-01
+7.000000e-01 4.000000e-02 4.000000e-02 1.478300e+00 1.364304e-01 2.160361e-01
+7.800000e-01 4.000000e-02 4.000000e-02 2.109200e+00 2.136732e-01 2.219583e-01
+9.100000e-01 9.000000e-02 9.000000e-02 2.156500e+00 1.180761e-01 1.055629e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d07-x01-y01
+Path=/REF/CMS_2018_I1690148/d07-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.450000e-01 4.500000e-02 4.500000e-02 4.125300e+00 4.268334e-02 1.378764e-01
+2.100000e-01 2.000000e-02 2.000000e-02 2.841800e+00 1.105067e-01 5.397425e-02
+2.500000e-01 2.000000e-02 2.000000e-02 2.429400e+00 6.851680e-02 7.639518e-02
+2.950000e-01 2.500000e-02 2.500000e-02 2.094200e+00 7.403946e-02 6.879051e-02
+4.100000e-01 9.000000e-02 9.000000e-02 1.739800e+00 4.652625e-02 3.286101e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d07-x01-y02
+Path=/REF/CMS_2018_I1690148/d07-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.450000e-01 4.500000e-02 4.500000e-02 3.996100e+00 8.850389e-02 1.868615e-01
+2.100000e-01 2.000000e-02 2.000000e-02 2.842100e+00 2.116179e-01 9.530884e-02
+2.500000e-01 2.000000e-02 2.000000e-02 2.449800e+00 7.660146e-02 1.627800e-01
+2.950000e-01 2.500000e-02 2.500000e-02 2.154900e+00 1.048469e-01 1.114769e-01
+4.100000e-01 9.000000e-02 9.000000e-02 1.783000e+00 7.123118e-02 4.962022e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d07-x01-y03
+Path=/REF/CMS_2018_I1690148/d07-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.450000e-01 4.500000e-02 4.500000e-02 4.269200e+00 7.025258e-02 1.219314e-01
+2.100000e-01 2.000000e-02 2.000000e-02 2.853900e+00 1.137432e-01 9.333106e-02
+2.500000e-01 2.000000e-02 2.000000e-02 2.449600e+00 1.417856e-01 7.526648e-02
+2.950000e-01 2.500000e-02 2.500000e-02 2.036700e+00 8.834096e-02 9.018811e-02
+4.100000e-01 9.000000e-02 9.000000e-02 1.676700e+00 4.863537e-02 4.190603e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d07-x01-y04
+Path=/REF/CMS_2018_I1690148/d07-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.450000e-01 4.500000e-02 4.500000e-02 4.035500e+00 1.028366e-01 2.351772e-01
+2.100000e-01 2.000000e-02 2.000000e-02 2.920300e+00 1.595591e-01 4.575517e-01
+2.500000e-01 2.000000e-02 2.000000e-02 2.191400e+00 2.534422e-01 2.258771e-01
+2.950000e-01 2.500000e-02 2.500000e-02 2.085100e+00 1.691782e-01 2.303985e-01
+4.100000e-01 9.000000e-02 9.000000e-02 1.822700e+00 2.056350e-01 8.767386e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d08-x01-y01
+Path=/REF/CMS_2018_I1690148/d08-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e-02 3.000000e-02 3.000000e-02 1.890200e+00 4.013066e-02 7.630683e-02
+8.000000e-02 2.000000e-02 2.000000e-02 3.858400e+00 6.971616e-02 8.272906e-02
+1.100000e-01 1.000000e-02 1.000000e-02 3.813000e+00 9.863351e-02 1.120442e-01
+1.350000e-01 1.500000e-02 1.500000e-02 3.428300e+00 7.362464e-02 4.949422e-02
+1.650000e-01 1.500000e-02 1.500000e-02 3.081600e+00 6.418134e-02 1.138264e-01
+1.950000e-01 1.500000e-02 1.500000e-02 2.755500e+00 1.207106e-01 4.992337e-02
+2.300000e-01 2.000000e-02 2.000000e-02 2.346000e+00 3.825838e-02 7.798360e-02
+2.700000e-01 2.000000e-02 2.000000e-02 2.058300e+00 6.662729e-02 4.930047e-02
+3.100000e-01 2.000000e-02 2.000000e-02 1.952200e+00 7.401108e-02 5.195062e-02
+3.500000e-01 2.000000e-02 2.000000e-02 1.569000e+00 7.930568e-02 4.419915e-02
+4.350000e-01 6.500000e-02 6.500000e-02 4.693500e-01 2.278173e-02 3.285754e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d08-x01-y02
+Path=/REF/CMS_2018_I1690148/d08-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e-02 3.000000e-02 3.000000e-02 1.523300e+00 4.517456e-02 9.603340e-02
+8.000000e-02 2.000000e-02 2.000000e-02 4.050100e+00 1.046288e-01 1.041213e-01
+1.100000e-01 1.000000e-02 1.000000e-02 4.269500e+00 2.345152e-01 9.419942e-02
+1.350000e-01 1.500000e-02 1.500000e-02 3.861500e+00 1.024357e-01 1.093262e-01
+1.650000e-01 1.500000e-02 1.500000e-02 3.409800e+00 1.051106e-01 1.610694e-01
+1.950000e-01 1.500000e-02 1.500000e-02 2.973800e+00 1.384199e-01 8.491435e-02
+2.300000e-01 2.000000e-02 2.000000e-02 2.446200e+00 6.613834e-02 1.075482e-01
+2.700000e-01 2.000000e-02 2.000000e-02 2.030300e+00 1.140868e-01 7.203072e-02
+3.100000e-01 2.000000e-02 2.000000e-02 1.747900e+00 6.644397e-02 8.049708e-02
+3.500000e-01 2.000000e-02 2.000000e-02 1.370900e+00 1.117482e-01 8.354960e-02
+4.350000e-01 6.500000e-02 6.500000e-02 3.849800e-01 3.727618e-02 3.395653e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d08-x01-y03
+Path=/REF/CMS_2018_I1690148/d08-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e-02 3.000000e-02 3.000000e-02 2.114300e+00 7.049328e-02 9.670316e-02
+8.000000e-02 2.000000e-02 2.000000e-02 3.809300e+00 9.912364e-02 1.124257e-01
+1.100000e-01 1.000000e-02 1.000000e-02 3.522100e+00 8.232908e-02 1.702618e-01
+1.350000e-01 1.500000e-02 1.500000e-02 3.098500e+00 1.187219e-01 7.721389e-02
+1.650000e-01 1.500000e-02 1.500000e-02 2.863300e+00 5.809228e-02 1.052943e-01
+1.950000e-01 1.500000e-02 1.500000e-02 2.581000e+00 1.606289e-01 4.833266e-02
+2.300000e-01 2.000000e-02 2.000000e-02 2.274200e+00 6.108390e-02 1.018641e-01
+2.700000e-01 2.000000e-02 2.000000e-02 2.066400e+00 9.712385e-02 1.025625e-01
+3.100000e-01 2.000000e-02 2.000000e-02 2.050500e+00 1.264807e-01 5.620602e-02
+3.500000e-01 2.000000e-02 2.000000e-02 1.739100e+00 9.984660e-02 5.758406e-02
+4.350000e-01 6.500000e-02 6.500000e-02 5.295200e-01 3.180413e-02 6.155727e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d08-x01-y04
+Path=/REF/CMS_2018_I1690148/d08-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.000000e-02 3.000000e-02 3.000000e-02 2.559400e+00 1.365048e-01 1.347897e-01
+8.000000e-02 2.000000e-02 2.000000e-02 3.217000e+00 1.566455e-01 1.836067e-01
+1.100000e-01 1.000000e-02 1.000000e-02 2.903900e+00 2.271457e-01 2.873524e-01
+1.350000e-01 1.500000e-02 1.500000e-02 2.851000e+00 1.659479e-01 1.558273e-01
+1.650000e-01 1.500000e-02 1.500000e-02 2.671400e+00 2.285379e-01 2.691266e-01
+1.950000e-01 1.500000e-02 1.500000e-02 2.561200e+00 1.968545e-01 2.062974e-01
+2.300000e-01 2.000000e-02 2.000000e-02 2.272300e+00 1.388951e-01 1.937550e-01
+2.700000e-01 2.000000e-02 2.000000e-02 2.181500e+00 1.996062e-01 1.174251e-01
+3.100000e-01 2.000000e-02 2.000000e-02 2.407100e+00 1.471366e-01 1.844499e-01
+3.500000e-01 2.000000e-02 2.000000e-02 1.718500e+00 2.964639e-01 1.526488e-01
+4.350000e-01 6.500000e-02 6.500000e-02 5.691300e-01 7.942342e-02 7.975176e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d09-x01-y01
+Path=/REF/CMS_2018_I1690148/d09-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+00 1.500000e+00 1.500000e+00 1.028100e-01 8.031247e-03 7.073915e-03
+3.500000e+00 5.000000e-01 5.000000e-01 2.393900e-01 4.490353e-03 5.309194e-03
+4.500000e+00 5.000000e-01 5.000000e-01 2.213200e-01 6.430759e-03 6.220112e-03
+5.500000e+00 5.000000e-01 5.000000e-01 1.380300e-01 9.265578e-03 9.535062e-03
+6.500000e+00 5.000000e-01 5.000000e-01 6.333400e-02 6.434467e-03 8.780042e-03
+7.500000e+00 5.000000e-01 5.000000e-01 2.215000e-02 3.299051e-03 4.543965e-03
+1.150000e+01 3.500000e+00 3.500000e+00 1.047200e-03 9.423135e-04 2.399360e-04
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d09-x01-y02
+Path=/REF/CMS_2018_I1690148/d09-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+00 1.500000e+00 1.500000e+00 8.407800e-02 8.967752e-03 8.704557e-03
+3.500000e+00 5.000000e-01 5.000000e-01 2.262400e-01 8.350692e-03 7.596000e-03
+4.500000e+00 5.000000e-01 5.000000e-01 2.417300e-01 1.092979e-02 7.516348e-03
+5.500000e+00 5.000000e-01 5.000000e-01 1.628700e-01 1.256192e-02 1.196025e-02
+6.500000e+00 5.000000e-01 5.000000e-01 8.067300e-02 9.292561e-03 1.183205e-02
+7.500000e+00 5.000000e-01 5.000000e-01 2.699200e-02 5.176448e-03 5.521940e-03
+1.150000e+01 3.500000e+00 3.500000e+00 1.323700e-03 3.168009e-04 3.636601e-04
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d09-x01-y03
+Path=/REF/CMS_2018_I1690148/d09-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+00 1.500000e+00 1.500000e+00 1.273400e-01 8.345683e-03 6.539469e-03
+3.500000e+00 5.000000e-01 5.000000e-01 2.530800e-01 8.430621e-03 5.618476e-03
+4.500000e+00 5.000000e-01 5.000000e-01 1.999800e-01 5.618925e-03 9.208484e-03
+5.500000e+00 5.000000e-01 5.000000e-01 1.057400e-01 9.002643e-03 8.409560e-03
+6.500000e+00 5.000000e-01 5.000000e-01 4.268700e-02 5.400286e-03 7.143729e-03
+7.500000e+00 5.000000e-01 5.000000e-01 1.333900e-02 2.552542e-03 4.585324e-03
+1.150000e+01 3.500000e+00 3.500000e+00 4.502400e-04 4.073474e-04 1.858026e-04
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d09-x01-y04
+Path=/REF/CMS_2018_I1690148/d09-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e+00 1.500000e+00 1.500000e+00 8.251500e-02 6.773946e-03 6.650514e-03
+3.500000e+00 5.000000e-01 5.000000e-01 2.078000e-01 1.340041e-02 2.394901e-02
+4.500000e+00 5.000000e-01 5.000000e-01 2.311700e-01 2.355290e-02 8.288150e-03
+5.500000e+00 5.000000e-01 5.000000e-01 1.742600e-01 1.747778e-02 2.234161e-02
+6.500000e+00 5.000000e-01 5.000000e-01 7.662200e-02 2.311185e-02 2.292340e-02
+7.500000e+00 5.000000e-01 5.000000e-01 4.721800e-02 9.350507e-03 1.256938e-02
+1.150000e+01 3.500000e+00 3.500000e+00 2.197200e-03 2.025040e-03 6.085806e-04
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d10-x01-y01
+Path=/REF/CMS_2018_I1690148/d10-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e-01 2.200000e-01 2.200000e-01 7.753000e-01 4.854009e-02 3.777012e-02
+4.900000e-01 5.000000e-02 5.000000e-02 2.270900e+00 3.696174e-02 5.446451e-02
+5.900000e-01 5.000000e-02 5.000000e-02 2.484600e+00 7.638054e-02 5.814748e-02
+6.800000e-01 4.000000e-02 4.000000e-02 1.717000e+00 8.433632e-02 1.246067e-01
+8.600000e-01 1.400000e-01 1.400000e-01 1.641600e-01 1.601892e-02 2.176071e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d10-x01-y02
+Path=/REF/CMS_2018_I1690148/d10-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e-01 2.200000e-01 2.200000e-01 7.221400e-01 5.101136e-02 4.996902e-02
+4.900000e-01 5.000000e-02 5.000000e-02 2.233300e+00 8.964979e-02 8.599149e-02
+5.900000e-01 5.000000e-02 5.000000e-02 2.571400e+00 1.107962e-01 7.104788e-02
+6.800000e-01 4.000000e-02 4.000000e-02 1.891300e+00 1.018338e-01 1.697169e-01
+8.600000e-01 1.400000e-01 1.400000e-01 1.802700e-01 2.181735e-02 2.529746e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d10-x01-y03
+Path=/REF/CMS_2018_I1690148/d10-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e-01 2.200000e-01 2.200000e-01 8.533100e-01 5.039802e-02 3.292587e-02
+4.900000e-01 5.000000e-02 5.000000e-02 2.342100e+00 5.070600e-02 6.233054e-02
+5.900000e-01 5.000000e-02 5.000000e-02 2.348100e+00 8.852051e-02 1.020969e-01
+6.800000e-01 4.000000e-02 4.000000e-02 1.486300e+00 8.827152e-02 1.079398e-01
+8.600000e-01 1.400000e-01 1.400000e-01 1.307800e-01 1.446202e-02 1.881307e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d10-x01-y04
+Path=/REF/CMS_2018_I1690148/d10-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.200000e-01 2.200000e-01 2.200000e-01 6.625600e-01 6.284352e-02 3.640791e-02
+4.900000e-01 5.000000e-02 5.000000e-02 2.129700e+00 1.033460e-01 1.907623e-01
+5.900000e-01 5.000000e-02 5.000000e-02 2.674600e+00 1.410846e-01 1.511572e-01
+6.800000e-01 4.000000e-02 4.000000e-02 1.972900e+00 2.224202e-01 2.179277e-01
+8.600000e-01 1.400000e-01 1.400000e-01 2.507200e-01 2.680069e-02 4.360111e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d11-x01-y01
+Path=/REF/CMS_2018_I1690148/d11-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.100000e-01 2.100000e-01 2.100000e-01 5.713600e-01 4.060471e-02 3.711071e-02
+4.800000e-01 6.000000e-02 6.000000e-02 1.972400e+00 7.688854e-02 5.867111e-02
+5.800000e-01 4.000000e-02 4.000000e-02 2.579300e+00 5.603664e-02 1.139188e-01
+6.600000e-01 4.000000e-02 4.000000e-02 2.374600e+00 1.068126e-01 1.048490e-01
+7.400000e-01 4.000000e-02 4.000000e-02 1.403000e+00 1.232151e-01 1.390672e-01
+8.900000e-01 1.100000e-01 1.100000e-01 6.721600e-02 1.888487e-02 2.200740e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d11-x01-y02
+Path=/REF/CMS_2018_I1690148/d11-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.100000e-01 2.100000e-01 2.100000e-01 5.260100e-01 4.834652e-02 5.159037e-02
+4.800000e-01 6.000000e-02 6.000000e-02 1.904000e+00 1.272904e-01 8.407042e-02
+5.800000e-01 4.000000e-02 4.000000e-02 2.636300e+00 1.065811e-01 1.670416e-01
+6.600000e-01 4.000000e-02 4.000000e-02 2.479300e+00 1.362063e-01 1.345191e-01
+7.400000e-01 4.000000e-02 4.000000e-02 1.566900e+00 1.676651e-01 1.733917e-01
+8.900000e-01 1.100000e-01 1.100000e-01 7.271900e-02 2.276649e-02 2.619567e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d11-x01-y03
+Path=/REF/CMS_2018_I1690148/d11-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.100000e-01 2.100000e-01 2.100000e-01 6.656200e-01 4.148329e-02 3.317934e-02
+4.800000e-01 6.000000e-02 6.000000e-02 2.146300e+00 9.630194e-02 6.173544e-02
+5.800000e-01 4.000000e-02 4.000000e-02 2.486600e+00 7.722578e-02 1.424667e-01
+6.600000e-01 4.000000e-02 4.000000e-02 2.129200e+00 1.100732e-01 1.193802e-01
+7.400000e-01 4.000000e-02 4.000000e-02 1.043800e+00 1.060350e-01 1.127530e-01
+8.900000e-01 1.100000e-01 1.100000e-01 4.594700e-02 1.388719e-02 1.412596e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d11-x01-y04
+Path=/REF/CMS_2018_I1690148/d11-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.100000e-01 2.100000e-01 2.100000e-01 4.163000e-01 5.090024e-02 3.281107e-02
+4.800000e-01 6.000000e-02 6.000000e-02 1.586500e+00 1.010468e-01 2.327615e-01
+5.800000e-01 4.000000e-02 4.000000e-02 2.741800e+00 3.156946e-01 2.879622e-01
+6.600000e-01 4.000000e-02 4.000000e-02 2.645700e+00 4.082293e-01 2.495895e-01
+7.400000e-01 4.000000e-02 4.000000e-02 2.190400e+00 2.234148e-01 2.944344e-01
+8.900000e-01 1.100000e-01 1.100000e-01 1.297300e-01 6.515145e-02 6.393757e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d12-x01-y01
+Path=/REF/CMS_2018_I1690148/d12-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 1.500000e-01 1.500000e-01 6.936100e-01 4.197636e-02 4.573376e-02
+4.600000e-01 6.000000e-02 6.000000e-02 1.881300e+00 1.099247e-01 9.091936e-02
+5.700000e-01 5.000000e-02 5.000000e-02 2.377600e+00 7.390351e-02 7.259619e-02
+6.700000e-01 5.000000e-02 5.000000e-02 2.256100e+00 1.237470e-01 1.217602e-01
+7.500000e-01 3.000000e-02 3.000000e-02 1.234900e+00 1.248778e-01 1.522222e-01
+8.400000e-01 6.000000e-02 6.000000e-02 2.390700e-01 3.866973e-02 4.546382e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d12-x01-y02
+Path=/REF/CMS_2018_I1690148/d12-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 1.500000e-01 1.500000e-01 6.501900e-01 5.456279e-02 6.384610e-02
+4.600000e-01 6.000000e-02 6.000000e-02 1.785100e+00 1.657397e-01 1.211962e-01
+5.700000e-01 5.000000e-02 5.000000e-02 2.441000e+00 1.152704e-01 1.333826e-01
+6.700000e-01 5.000000e-02 5.000000e-02 2.374000e+00 1.590382e-01 1.456191e-01
+7.500000e-01 3.000000e-02 3.000000e-02 1.404100e+00 1.902230e-01 2.135818e-01
+8.400000e-01 6.000000e-02 6.000000e-02 2.082500e-01 5.311140e-02 6.047174e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d12-x01-y03
+Path=/REF/CMS_2018_I1690148/d12-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 1.500000e-01 1.500000e-01 8.107200e-01 4.192220e-02 3.881228e-02
+4.600000e-01 6.000000e-02 6.000000e-02 2.143000e+00 1.142120e-01 1.110634e-01
+5.700000e-01 5.000000e-02 5.000000e-02 2.338200e+00 9.426576e-02 9.204745e-02
+6.700000e-01 5.000000e-02 5.000000e-02 1.964500e+00 1.448079e-01 1.477654e-01
+7.500000e-01 3.000000e-02 3.000000e-02 8.237600e-01 9.822516e-02 1.455513e-01
+8.400000e-01 6.000000e-02 6.000000e-02 1.660200e-01 6.997448e-02 6.020554e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d12-x01-y04
+Path=/REF/CMS_2018_I1690148/d12-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-01 1.500000e-01 1.500000e-01 5.039700e-01 6.671568e-02 4.991708e-02
+4.600000e-01 6.000000e-02 6.000000e-02 1.407300e+00 2.063728e-01 2.008122e-01
+5.700000e-01 5.000000e-02 5.000000e-02 2.160600e+00 1.878669e-01 2.074687e-01
+6.700000e-01 5.000000e-02 5.000000e-02 2.748300e+00 2.545598e-01 2.403018e-01
+7.500000e-01 3.000000e-02 3.000000e-02 1.890000e+00 3.394225e-01 3.394563e-01
+8.400000e-01 6.000000e-02 6.000000e-02 6.303300e-01 1.460581e-01 2.231074e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d13-x01-y01
+Path=/REF/CMS_2018_I1690148/d13-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.450000e-01 4.500000e-02 4.500000e-02 1.769000e+00 1.396814e-01 1.279181e-01
+3.100000e-01 2.000000e-02 2.000000e-02 3.691800e+00 1.992675e-01 1.567280e-01
+3.500000e-01 2.000000e-02 2.000000e-02 5.528300e+00 1.434774e-01 1.871226e-01
+3.850000e-01 1.500000e-02 1.500000e-02 7.417200e+00 1.793623e-01 1.451081e-01
+4.150000e-01 1.500000e-02 1.500000e-02 6.368900e+00 3.775250e-01 4.516753e-01
+4.350000e-01 5.000000e-03 5.000000e-03 3.602300e+00 5.960225e-01 5.908269e-01
+4.700000e-01 3.000000e-02 3.000000e-02 3.730800e-01 6.319613e-02 7.628643e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d13-x01-y02
+Path=/REF/CMS_2018_I1690148/d13-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.450000e-01 4.500000e-02 4.500000e-02 1.426600e+00 1.896262e-01 1.677716e-01
+3.100000e-01 2.000000e-02 2.000000e-02 3.178800e+00 2.094021e-01 3.361226e-01
+3.500000e-01 2.000000e-02 2.000000e-02 5.152100e+00 3.644836e-01 2.291293e-01
+3.850000e-01 1.500000e-02 1.500000e-02 8.140200e+00 3.093012e-01 2.312254e-01
+4.150000e-01 1.500000e-02 1.500000e-02 7.509400e+00 5.254606e-01 6.404596e-01
+4.350000e-01 5.000000e-03 5.000000e-03 4.331200e+00 8.965113e-01 8.723735e-01
+4.700000e-01 3.000000e-02 3.000000e-02 4.260800e-01 8.373064e-02 9.893660e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d13-x01-y03
+Path=/REF/CMS_2018_I1690148/d13-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.450000e-01 4.500000e-02 4.500000e-02 2.248300e+00 1.358370e-01 1.306788e-01
+3.100000e-01 2.000000e-02 2.000000e-02 4.391900e+00 3.014821e-01 1.053360e-01
+3.500000e-01 2.000000e-02 2.000000e-02 5.971500e+00 7.471053e-02 2.336008e-01
+3.850000e-01 1.500000e-02 1.500000e-02 6.674100e+00 1.695738e-01 2.250195e-01
+4.150000e-01 1.500000e-02 1.500000e-02 4.902000e+00 3.071898e-01 3.433443e-01
+4.350000e-01 5.000000e-03 5.000000e-03 2.280000e+00 4.214809e-01 3.828889e-01
+4.700000e-01 3.000000e-02 3.000000e-02 2.171500e-01 3.587142e-02 4.465442e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d13-x01-y04
+Path=/REF/CMS_2018_I1690148/d13-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.450000e-01 4.500000e-02 4.500000e-02 1.372300e+00 1.273200e-01 9.663104e-02
+3.100000e-01 2.000000e-02 2.000000e-02 2.866600e+00 2.652819e-01 2.766690e-01
+3.500000e-01 2.000000e-02 2.000000e-02 5.087200e+00 2.864637e-01 4.448677e-01
+3.850000e-01 1.500000e-02 1.500000e-02 7.345700e+00 5.389440e-01 3.442515e-01
+4.150000e-01 1.500000e-02 1.500000e-02 7.672600e+00 3.916193e-01 5.515686e-01
+4.350000e-01 5.000000e-03 5.000000e-03 6.071600e+00 1.010238e+00 8.086279e-01
+4.700000e-01 3.000000e-02 3.000000e-02 7.844800e-01 2.042423e-01 2.039472e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d14-x01-y01
+Path=/REF/CMS_2018_I1690148/d14-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.000000e-02 8.000000e-02 8.000000e-02 8.293800e-01 7.266918e-02 5.669854e-02
+1.800000e-01 2.000000e-02 2.000000e-02 3.992200e+00 1.542316e-01 1.788359e-01
+2.150000e-01 1.500000e-02 1.500000e-02 6.319700e+00 1.237935e-01 1.308412e-01
+2.400000e-01 1.000000e-02 1.000000e-02 7.623500e+00 1.851571e-01 2.187517e-01
+2.650000e-01 1.500000e-02 1.500000e-02 6.782400e+00 2.297204e-01 2.378343e-01
+2.900000e-01 1.000000e-02 1.000000e-02 4.462300e+00 2.852916e-01 2.682885e-01
+3.050000e-01 5.000000e-03 5.000000e-03 3.169100e+00 1.737052e-01 2.725793e-01
+3.200000e-01 1.000000e-02 1.000000e-02 1.717600e+00 1.525005e-01 1.254611e-01
+4.150000e-01 8.500000e-02 8.500000e-02 3.992300e-02 9.773724e-03 1.023041e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d14-x01-y02
+Path=/REF/CMS_2018_I1690148/d14-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.000000e-02 8.000000e-02 8.000000e-02 6.413200e-01 1.065966e-01 9.552486e-02
+1.800000e-01 2.000000e-02 2.000000e-02 3.353700e+00 2.489347e-01 2.707514e-01
+2.150000e-01 1.500000e-02 1.500000e-02 6.540400e+00 2.361736e-01 1.529073e-01
+2.400000e-01 1.000000e-02 1.000000e-02 8.441900e+00 2.934037e-01 3.862990e-01
+2.650000e-01 1.500000e-02 1.500000e-02 7.683400e+00 3.973586e-01 4.149243e-01
+2.900000e-01 1.000000e-02 1.000000e-02 4.736200e+00 4.125343e-01 3.944817e-01
+3.050000e-01 5.000000e-03 5.000000e-03 3.280000e+00 3.473384e-01 3.244442e-01
+3.200000e-01 1.000000e-02 1.000000e-02 1.663700e+00 1.521582e-01 1.556162e-01
+4.150000e-01 8.500000e-02 8.500000e-02 4.053600e-02 1.138509e-02 1.133449e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d14-x01-y03
+Path=/REF/CMS_2018_I1690148/d14-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.000000e-02 8.000000e-02 8.000000e-02 1.077200e+00 6.376996e-02 4.680781e-02
+1.800000e-01 2.000000e-02 2.000000e-02 4.671300e+00 1.364662e-01 1.280524e-01
+2.150000e-01 1.500000e-02 1.500000e-02 6.208800e+00 1.215086e-01 1.847917e-01
+2.400000e-01 1.000000e-02 1.000000e-02 6.921300e+00 2.649100e-01 2.498924e-01
+2.650000e-01 1.500000e-02 1.500000e-02 5.793800e+00 1.724395e-01 2.109078e-01
+2.900000e-01 1.000000e-02 1.000000e-02 3.922000e+00 2.774036e-01 2.384773e-01
+3.050000e-01 5.000000e-03 5.000000e-03 2.624500e+00 1.598336e-01 4.510271e-01
+3.200000e-01 1.000000e-02 1.000000e-02 1.557400e+00 1.674727e-01 1.043852e-01
+4.150000e-01 8.500000e-02 8.500000e-02 3.799100e-02 4.918996e-03 6.914569e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d14-x01-y04
+Path=/REF/CMS_2018_I1690148/d14-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.000000e-02 8.000000e-02 8.000000e-02 7.331300e-01 7.608859e-02 5.392876e-02
+1.800000e-01 2.000000e-02 2.000000e-02 3.542300e+00 1.640178e-01 2.693703e-01
+2.150000e-01 1.500000e-02 1.500000e-02 5.490900e+00 2.381886e-01 3.312450e-01
+2.400000e-01 1.000000e-02 1.000000e-02 6.955200e+00 3.584672e-01 5.700992e-01
+2.650000e-01 1.500000e-02 1.500000e-02 7.079900e+00 4.061900e-01 3.208730e-01
+2.900000e-01 1.000000e-02 1.000000e-02 5.661300e+00 4.165022e-01 4.362040e-01
+3.050000e-01 5.000000e-03 5.000000e-03 4.964800e+00 7.773703e-01 5.361872e-01
+3.200000e-01 1.000000e-02 1.000000e-02 2.664900e+00 4.168974e-01 3.235581e-01
+4.150000e-01 8.500000e-02 8.500000e-02 5.065000e-02 5.143563e-02 4.519051e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d15-x01-y01
+Path=/REF/CMS_2018_I1690148/d15-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.000000e-02 4.000000e-02 4.000000e-02 1.867600e+00 1.390225e-01 1.057262e-01
+9.000000e-02 1.000000e-02 1.000000e-02 6.700800e+00 1.050576e-01 3.513715e-01
+1.100000e-01 1.000000e-02 1.000000e-02 8.430700e+00 1.852489e-01 1.256968e-01
+1.300000e-01 1.000000e-02 1.000000e-02 8.588100e+00 2.306353e-01 1.633221e-01
+1.475000e-01 7.500000e-03 7.500000e-03 7.214700e+00 1.515338e-01 2.924357e-01
+1.650000e-01 1.000000e-02 1.000000e-02 6.002500e+00 2.588524e-01 1.628417e-01
+1.850000e-01 1.000000e-02 1.000000e-02 3.962300e+00 1.284064e-01 1.934384e-01
+2.050000e-01 1.000000e-02 1.000000e-02 2.348300e+00 1.305387e-01 9.291370e-02
+2.575000e-01 4.250000e-02 4.250000e-02 2.554900e-01 1.857816e-02 1.677272e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d15-x01-y02
+Path=/REF/CMS_2018_I1690148/d15-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.000000e-02 4.000000e-02 4.000000e-02 1.418800e+00 1.937695e-01 1.680842e-01
+9.000000e-02 1.000000e-02 1.000000e-02 6.290900e+00 1.810018e-01 4.214759e-01
+1.100000e-01 1.000000e-02 1.000000e-02 9.032300e+00 3.183939e-01 1.621891e-01
+1.300000e-01 1.000000e-02 1.000000e-02 9.580500e+00 4.074784e-01 2.871970e-01
+1.475000e-01 7.500000e-03 7.500000e-03 7.858100e+00 2.061844e-01 5.667927e-01
+1.650000e-01 1.000000e-02 1.000000e-02 6.470800e+00 4.535578e-01 2.476135e-01
+1.850000e-01 1.000000e-02 1.000000e-02 3.852000e+00 2.080113e-01 2.926936e-01
+2.050000e-01 1.000000e-02 1.000000e-02 2.183700e+00 1.545507e-01 1.476058e-01
+2.575000e-01 4.250000e-02 4.250000e-02 2.402300e-01 2.375616e-02 1.909218e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d15-x01-y03
+Path=/REF/CMS_2018_I1690148/d15-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.000000e-02 4.000000e-02 4.000000e-02 2.329700e+00 1.205360e-01 7.903094e-02
+9.000000e-02 1.000000e-02 1.000000e-02 7.177000e+00 1.007850e-01 3.590073e-01
+1.100000e-01 1.000000e-02 1.000000e-02 8.140900e+00 2.118414e-01 2.033675e-01
+1.300000e-01 1.000000e-02 1.000000e-02 7.818700e+00 1.977121e-01 1.718401e-01
+1.475000e-01 7.500000e-03 7.500000e-03 6.569300e+00 2.576917e-01 1.952011e-01
+1.650000e-01 1.000000e-02 1.000000e-02 5.443200e+00 1.754967e-01 1.579906e-01
+1.850000e-01 1.000000e-02 1.000000e-02 3.833700e+00 1.609482e-01 2.228610e-01
+2.050000e-01 1.000000e-02 1.000000e-02 2.266400e+00 1.415676e-01 1.252405e-01
+2.575000e-01 4.250000e-02 4.250000e-02 2.527500e-01 2.319976e-02 2.313727e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d15-x01-y04
+Path=/REF/CMS_2018_I1690148/d15-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.000000e-02 4.000000e-02 4.000000e-02 1.931600e+00 1.313944e-01 8.738119e-02
+9.000000e-02 1.000000e-02 1.000000e-02 5.744400e+00 2.982795e-01 5.870928e-01
+1.100000e-01 1.000000e-02 1.000000e-02 6.937700e+00 2.373068e-01 5.939065e-01
+1.300000e-01 1.000000e-02 1.000000e-02 7.538700e+00 4.655556e-01 4.899684e-01
+1.475000e-01 7.500000e-03 7.500000e-03 7.591700e+00 9.886876e-01 4.574199e-01
+1.650000e-01 1.000000e-02 1.000000e-02 6.611200e+00 5.492918e-01 6.621396e-01
+1.850000e-01 1.000000e-02 1.000000e-02 4.997400e+00 3.332560e-01 4.500691e-01
+2.050000e-01 1.000000e-02 1.000000e-02 3.449500e+00 4.288764e-01 3.255278e-01
+2.575000e-01 4.250000e-02 4.250000e-02 3.060600e-01 1.393717e-01 8.942996e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d16-x01-y01
+Path=/REF/CMS_2018_I1690148/d16-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e-02 1.750000e-02 1.750000e-02 8.339100e+00 2.771191e-01 5.002999e-01
+4.000000e-02 5.000000e-03 5.000000e-03 1.436500e+01 5.867893e-01 7.600167e-01
+5.250000e-02 7.500000e-03 7.500000e-03 1.286900e+01 5.214588e-01 1.308612e-01
+6.750000e-02 7.500000e-03 7.500000e-03 9.627700e+00 3.218724e-01 2.577559e-01
+8.250000e-02 7.500000e-03 7.500000e-03 6.759200e+00 3.485596e-01 1.117038e-01
+1.000000e-01 1.000000e-02 1.000000e-02 3.979400e+00 9.948169e-02 1.608850e-01
+1.200000e-01 1.000000e-02 1.000000e-02 1.798900e+00 3.375024e-01 6.310776e-02
+1.650000e-01 3.500000e-02 3.500000e-02 1.439000e-01 2.780042e-02 1.823253e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d16-x01-y02
+Path=/REF/CMS_2018_I1690148/d16-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e-02 1.750000e-02 1.750000e-02 7.496400e+00 2.793475e-01 9.235520e-01
+4.000000e-02 5.000000e-03 5.000000e-03 1.546700e+01 1.236431e+00 4.902029e-01
+5.250000e-02 7.500000e-03 7.500000e-03 1.420300e+01 5.515038e-01 2.543683e-01
+6.750000e-02 7.500000e-03 7.500000e-03 1.015100e+01 5.284116e-01 4.140020e-01
+8.250000e-02 7.500000e-03 7.500000e-03 6.914200e+00 4.277986e-01 1.897388e-01
+1.000000e-01 1.000000e-02 1.000000e-02 3.692000e+00 1.541924e-01 1.876769e-01
+1.200000e-01 1.000000e-02 1.000000e-02 1.604300e+00 1.636497e-01 8.794712e-02
+1.650000e-01 3.500000e-02 3.500000e-02 1.145200e-01 2.853432e-02 4.268231e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d16-x01-y03
+Path=/REF/CMS_2018_I1690148/d16-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e-02 1.750000e-02 1.750000e-02 9.141300e+00 2.799375e-01 2.730839e-01
+4.000000e-02 5.000000e-03 5.000000e-03 1.380900e+01 5.383454e-01 9.556736e-01
+5.250000e-02 7.500000e-03 7.500000e-03 1.193800e+01 3.193916e-01 2.054597e-01
+6.750000e-02 7.500000e-03 7.500000e-03 8.923700e+00 2.061781e-01 2.787750e-01
+8.250000e-02 7.500000e-03 7.500000e-03 6.488200e+00 2.197814e-01 1.784752e-01
+1.000000e-01 1.000000e-02 1.000000e-02 3.992600e+00 1.171329e-01 2.532327e-01
+1.200000e-01 1.000000e-02 1.000000e-02 1.769000e+00 1.117038e-01 1.805839e-01
+1.650000e-01 3.500000e-02 3.500000e-02 2.355500e-01 1.603289e-01 6.846489e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d16-x01-y04
+Path=/REF/CMS_2018_I1690148/d16-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.750000e-02 1.750000e-02 1.750000e-02 8.021900e+00 2.038511e-01 3.246609e-01
+4.000000e-02 5.000000e-03 5.000000e-03 1.205600e+01 7.717210e-01 1.226567e+00
+5.250000e-02 7.500000e-03 7.500000e-03 1.082300e+01 1.194176e+00 6.694572e-01
+6.750000e-02 7.500000e-03 7.500000e-03 1.082100e+01 7.134114e-01 7.048458e-01
+8.250000e-02 7.500000e-03 7.500000e-03 7.202100e+00 6.428678e-01 5.973672e-01
+1.000000e-01 1.000000e-02 1.000000e-02 5.103900e+00 4.371288e-01 3.238742e-01
+1.200000e-01 1.000000e-02 1.000000e-02 2.615400e+00 4.635001e-01 2.189569e-01
+1.650000e-01 3.500000e-02 3.500000e-02 1.657800e-01 1.404480e-01 1.731640e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d17-x01-y01
+Path=/REF/CMS_2018_I1690148/d17-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.000000e-03 6.000000e-03 6.000000e-03 4.906200e+01 9.919724e-01 1.041173e+00
+1.500000e-02 3.000000e-03 3.000000e-03 2.507900e+01 1.890301e+00 2.190775e+00
+2.100000e-02 3.000000e-03 3.000000e-03 1.688600e+01 7.079661e-01 3.510611e-01
+2.800000e-02 4.000000e-03 4.000000e-03 9.691000e+00 3.332890e-01 3.042866e-01
+3.700000e-02 5.000000e-03 5.000000e-03 5.091400e+00 1.722654e-01 2.576414e-01
+7.100000e-02 2.900000e-02 2.900000e-02 5.348300e-01 5.436879e-02 3.327122e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d17-x01-y02
+Path=/REF/CMS_2018_I1690148/d17-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.000000e-03 6.000000e-03 6.000000e-03 4.995900e+01 1.104368e+00 1.488784e+00
+1.500000e-02 3.000000e-03 3.000000e-03 2.605500e+01 2.361667e+00 2.137543e+00
+2.100000e-02 3.000000e-03 3.000000e-03 1.670000e+01 1.603294e+00 9.818305e-01
+2.800000e-02 4.000000e-03 4.000000e-03 9.166600e+00 5.370810e-01 9.296244e-01
+3.700000e-02 5.000000e-03 5.000000e-03 4.523000e+00 3.647390e-01 2.943729e-01
+7.100000e-02 2.900000e-02 2.900000e-02 4.380200e-01 5.467376e-02 1.209999e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d17-x01-y03
+Path=/REF/CMS_2018_I1690148/d17-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.000000e-03 6.000000e-03 6.000000e-03 4.903600e+01 1.125117e+00 1.046822e+00
+1.500000e-02 3.000000e-03 3.000000e-03 2.405400e+01 1.723852e+00 2.122014e+00
+2.100000e-02 3.000000e-03 3.000000e-03 1.670000e+01 6.289264e-01 6.163679e-01
+2.800000e-02 4.000000e-03 4.000000e-03 9.904800e+00 5.970737e-01 5.164493e-01
+3.700000e-02 5.000000e-03 5.000000e-03 5.301100e+00 2.392552e-01 2.885154e-01
+7.100000e-02 2.900000e-02 2.900000e-02 5.998700e-01 4.850092e-02 3.412697e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d17-x01-y04
+Path=/REF/CMS_2018_I1690148/d17-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.000000e-03 6.000000e-03 6.000000e-03 4.453400e+01 1.489276e+00 1.758383e+00
+1.500000e-02 3.000000e-03 3.000000e-03 2.594800e+01 2.509658e+00 3.072683e+00
+2.100000e-02 3.000000e-03 3.000000e-03 1.913700e+01 1.021072e+00 1.576854e+00
+2.800000e-02 4.000000e-03 4.000000e-03 1.123800e+01 8.473882e-01 8.816562e-01
+3.700000e-02 5.000000e-03 5.000000e-03 6.663900e+00 5.307559e-01 7.219838e-01
+7.100000e-02 2.900000e-02 2.900000e-02 6.644000e-01 2.981155e-01 1.383080e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d18-x01-y01
+Path=/REF/CMS_2018_I1690148/d18-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.700000e-01 7.000000e-02 7.000000e-02 1.052300e+00 1.040650e-01 8.381764e-02
+3.700000e-01 3.000000e-02 3.000000e-02 1.766500e+00 9.528014e-02 1.095963e-01
+4.300000e-01 3.000000e-02 3.000000e-02 3.376100e+00 1.151476e-01 1.145775e-01
+4.800000e-01 2.000000e-02 2.000000e-02 4.472900e+00 1.427536e-01 1.202817e-01
+5.150000e-01 1.500000e-02 1.500000e-02 5.177300e+00 2.077803e-01 2.156051e-01
+5.500000e-01 2.000000e-02 2.000000e-02 3.975300e+00 2.822341e-01 3.383468e-01
+5.750000e-01 5.000000e-03 5.000000e-03 2.312700e+00 4.373796e-01 3.464652e-01
+5.900000e-01 1.000000e-02 1.000000e-02 1.208400e+00 1.689324e-01 2.318145e-01
+6.500000e-01 5.000000e-02 5.000000e-02 3.577500e-02 1.552260e-02 1.752115e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d18-x01-y02
+Path=/REF/CMS_2018_I1690148/d18-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.700000e-01 7.000000e-02 7.000000e-02 8.524500e-01 1.321508e-01 1.112161e-01
+3.700000e-01 3.000000e-02 3.000000e-02 1.454400e+00 1.217150e-01 2.100502e-01
+4.300000e-01 3.000000e-02 3.000000e-02 3.065000e+00 1.942418e-01 1.890691e-01
+4.800000e-01 2.000000e-02 2.000000e-02 4.692300e+00 2.813501e-01 1.158433e-01
+5.150000e-01 1.500000e-02 1.500000e-02 5.771100e+00 2.578029e-01 3.041691e-01
+5.500000e-01 2.000000e-02 2.000000e-02 4.783800e+00 4.115965e-01 4.724805e-01
+5.750000e-01 5.000000e-03 5.000000e-03 2.549900e+00 6.006838e-01 5.310978e-01
+5.900000e-01 1.000000e-02 1.000000e-02 1.435000e+00 2.315989e-01 3.208497e-01
+6.500000e-01 5.000000e-02 5.000000e-02 3.114000e-02 2.128700e-02 2.447555e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d18-x01-y03
+Path=/REF/CMS_2018_I1690148/d18-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.700000e-01 7.000000e-02 7.000000e-02 1.388000e+00 1.148765e-01 8.412516e-02
+3.700000e-01 3.000000e-02 3.000000e-02 2.124400e+00 1.196019e-01 7.734939e-02
+4.300000e-01 3.000000e-02 3.000000e-02 3.771400e+00 8.835937e-02 1.104463e-01
+4.800000e-01 2.000000e-02 2.000000e-02 4.383200e+00 1.489225e-01 2.451421e-01
+5.150000e-01 1.500000e-02 1.500000e-02 4.317900e+00 2.385623e-01 2.782461e-01
+5.500000e-01 2.000000e-02 2.000000e-02 2.920800e+00 2.185255e-01 2.597993e-01
+5.750000e-01 5.000000e-03 5.000000e-03 1.499700e+00 3.136136e-01 2.684699e-01
+5.900000e-01 1.000000e-02 1.000000e-02 6.682400e-01 1.117127e-01 1.472709e-01
+6.500000e-01 5.000000e-02 5.000000e-02 1.874700e-02 4.963336e-03 5.982597e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d18-x01-y04
+Path=/REF/CMS_2018_I1690148/d18-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.700000e-01 7.000000e-02 7.000000e-02 7.324400e-01 8.935519e-02 9.124216e-02
+3.700000e-01 3.000000e-02 3.000000e-02 1.484200e+00 2.052259e-01 1.268319e-01
+4.300000e-01 3.000000e-02 3.000000e-02 2.890800e+00 3.198182e-01 1.738871e-01
+4.800000e-01 2.000000e-02 2.000000e-02 3.980600e+00 2.298770e-01 6.217777e-01
+5.150000e-01 1.500000e-02 1.500000e-02 5.767200e+00 7.354361e-01 3.446900e-01
+5.500000e-01 2.000000e-02 2.000000e-02 4.963000e+00 3.043994e-01 5.689807e-01
+5.750000e-01 5.000000e-03 5.000000e-03 4.082500e+00 1.109879e+00 6.367181e-01
+5.900000e-01 1.000000e-02 1.000000e-02 2.592500e+00 3.971779e-01 4.830554e-01
+6.500000e-01 5.000000e-02 5.000000e-02 1.151900e-01 1.012761e-01 7.429242e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d19-x01-y01
+Path=/REF/CMS_2018_I1690148/d19-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.400000e-01 1.400000e-01 1.400000e-01 1.094900e+00 8.297819e-02 7.182826e-02
+3.000000e-01 2.000000e-02 2.000000e-02 5.333200e+00 8.889403e-02 1.331067e-01
+3.400000e-01 2.000000e-02 2.000000e-02 5.911600e+00 2.007678e-01 2.042013e-01
+3.700000e-01 1.000000e-02 1.000000e-02 4.955300e+00 2.775496e-01 3.124873e-01
+4.000000e-01 2.000000e-02 2.000000e-02 2.941000e+00 1.734334e-01 1.895007e-01
+4.300000e-01 1.000000e-02 1.000000e-02 1.059100e+00 1.391085e-01 1.056643e-01
+5.700000e-01 1.300000e-01 1.300000e-01 2.193400e-02 5.195324e-03 6.730085e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d19-x01-y02
+Path=/REF/CMS_2018_I1690148/d19-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.400000e-01 1.400000e-01 1.400000e-01 9.397000e-01 1.081365e-01 1.000004e-01
+3.000000e-01 2.000000e-02 2.000000e-02 5.561800e+00 1.600878e-01 2.021142e-01
+3.400000e-01 2.000000e-02 2.000000e-02 6.446900e+00 2.906388e-01 3.038563e-01
+3.700000e-01 1.000000e-02 1.000000e-02 5.487700e+00 4.516240e-01 4.517682e-01
+4.000000e-01 2.000000e-02 2.000000e-02 3.011900e+00 2.299463e-01 2.470172e-01
+4.300000e-01 1.000000e-02 1.000000e-02 9.984200e-01 1.671935e-01 1.063400e-01
+5.700000e-01 1.300000e-01 1.300000e-01 2.436100e-02 6.068169e-03 7.980876e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d19-x01-y03
+Path=/REF/CMS_2018_I1690148/d19-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.400000e-01 1.400000e-01 1.400000e-01 1.305000e+00 7.271302e-02 5.705566e-02
+3.000000e-01 2.000000e-02 2.000000e-02 5.240900e+00 1.264416e-01 1.865965e-01
+3.400000e-01 2.000000e-02 2.000000e-02 5.342400e+00 1.672104e-01 1.735370e-01
+3.700000e-01 1.000000e-02 1.000000e-02 4.298600e+00 2.345508e-01 2.683502e-01
+4.000000e-01 2.000000e-02 2.000000e-02 2.557200e+00 1.241074e-01 1.812785e-01
+4.300000e-01 1.000000e-02 1.000000e-02 9.163000e-01 1.264093e-01 9.616671e-02
+5.700000e-01 1.300000e-01 1.300000e-01 1.805200e-02 3.325532e-03 4.219605e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d19-x01-y04
+Path=/REF/CMS_2018_I1690148/d19-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.400000e-01 1.400000e-01 1.400000e-01 8.916500e-01 7.173476e-02 6.556777e-02
+3.000000e-01 2.000000e-02 2.000000e-02 4.424500e+00 2.535780e-01 3.096569e-01
+3.400000e-01 2.000000e-02 2.000000e-02 5.924500e+00 3.909038e-01 2.711975e-01
+3.700000e-01 1.000000e-02 1.000000e-02 5.881300e+00 3.396251e-01 7.227580e-01
+4.000000e-01 2.000000e-02 2.000000e-02 4.305600e+00 3.641504e-01 1.976350e-01
+4.300000e-01 1.000000e-02 1.000000e-02 1.889700e+00 3.091360e-01 3.070799e-01
+5.700000e-01 1.300000e-01 1.300000e-01 3.357800e-02 2.393404e-02 2.592777e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d20-x01-y01
+Path=/REF/CMS_2018_I1690148/d20-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.712400e+00 1.206641e-01 9.550543e-02
+1.650000e-01 1.500000e-02 1.500000e-02 6.220300e+00 7.934263e-02 2.557688e-01
+1.950000e-01 1.500000e-02 1.500000e-02 7.086900e+00 2.450756e-01 1.522782e-01
+2.250000e-01 1.500000e-02 1.500000e-02 5.923700e+00 1.776185e-01 2.196992e-01
+2.550000e-01 1.500000e-02 1.500000e-02 3.764200e+00 1.905334e-01 2.033012e-01
+2.800000e-01 1.000000e-02 1.000000e-02 1.812900e+00 1.642778e-01 1.552258e-01
+3.450000e-01 5.500000e-02 5.500000e-02 1.547400e-01 5.947421e-02 1.624225e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d20-x01-y02
+Path=/REF/CMS_2018_I1690148/d20-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.620800e+00 1.421286e-01 1.239815e-01
+1.650000e-01 1.500000e-02 1.500000e-02 6.391900e+00 1.201979e-01 2.775122e-01
+1.950000e-01 1.500000e-02 1.500000e-02 7.452000e+00 2.997615e-01 2.113205e-01
+2.250000e-01 1.500000e-02 1.500000e-02 6.031600e+00 2.478269e-01 2.619198e-01
+2.550000e-01 1.500000e-02 1.500000e-02 3.704800e+00 2.025059e-01 2.535008e-01
+2.800000e-01 1.000000e-02 1.000000e-02 1.647500e+00 2.452077e-01 1.060362e-01
+3.450000e-01 5.500000e-02 5.500000e-02 1.501900e-01 1.633677e-02 2.169898e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d20-x01-y03
+Path=/REF/CMS_2018_I1690148/d20-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.882300e+00 1.053791e-01 7.462163e-02
+1.650000e-01 1.500000e-02 1.500000e-02 6.186000e+00 1.155204e-01 2.315332e-01
+1.950000e-01 1.500000e-02 1.500000e-02 6.780000e+00 2.368806e-01 1.722154e-01
+2.250000e-01 1.500000e-02 1.500000e-02 5.665400e+00 1.367723e-01 2.016457e-01
+2.550000e-01 1.500000e-02 1.500000e-02 3.586900e+00 2.208333e-01 2.080807e-01
+2.800000e-01 1.000000e-02 1.000000e-02 1.783300e+00 9.774905e-02 2.084128e-01
+3.450000e-01 5.500000e-02 5.500000e-02 1.404000e-01 6.860276e-02 1.339385e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d20-x01-y04
+Path=/REF/CMS_2018_I1690148/d20-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+7.500000e-02 7.500000e-02 7.500000e-02 1.353400e+00 1.168826e-01 7.820708e-02
+1.650000e-01 1.500000e-02 1.500000e-02 5.364000e+00 2.019246e-01 5.786618e-01
+1.950000e-01 1.500000e-02 1.500000e-02 6.724400e+00 3.180389e-01 4.157893e-01
+2.250000e-01 1.500000e-02 1.500000e-02 6.849500e+00 4.783362e-01 3.689432e-01
+2.550000e-01 1.500000e-02 1.500000e-02 4.900900e+00 3.039279e-01 3.378124e-01
+2.800000e-01 1.000000e-02 1.000000e-02 2.912100e+00 5.162293e-01 3.084753e-01
+3.450000e-01 5.500000e-02 5.500000e-02 2.143900e-01 7.385343e-02 4.787857e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d21-x01-y01
+Path=/REF/CMS_2018_I1690148/d21-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-02 2.000000e-02 2.000000e-02 3.128600e+00 2.732277e-01 1.851578e-01
+5.250000e-02 1.250000e-02 1.250000e-02 7.237400e+00 3.287321e-01 1.719558e-01
+7.750000e-02 1.250000e-02 1.250000e-02 8.888300e+00 2.175701e-01 4.502911e-01
+1.000000e-01 1.000000e-02 1.000000e-02 9.058200e+00 3.318487e-01 3.581762e-01
+1.200000e-01 1.000000e-02 1.000000e-02 7.224500e+00 2.458536e-01 4.450264e-01
+1.425000e-01 1.250000e-02 1.250000e-02 4.181900e+00 2.532119e-01 4.884842e-01
+2.025000e-01 4.750000e-02 4.750000e-02 4.369900e-01 2.736609e-01 2.295084e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d21-x01-y02
+Path=/REF/CMS_2018_I1690148/d21-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-02 2.000000e-02 2.000000e-02 2.954700e+00 3.625760e-01 2.415019e-01
+5.250000e-02 1.250000e-02 1.250000e-02 7.569000e+00 3.098872e-01 1.748570e-01
+7.750000e-02 1.250000e-02 1.250000e-02 9.140700e+00 2.660578e-01 3.851776e-01
+1.000000e-01 1.000000e-02 1.000000e-02 9.306000e+00 4.634374e-01 4.543611e-01
+1.200000e-01 1.000000e-02 1.000000e-02 7.067300e+00 2.694162e-01 6.043687e-01
+1.425000e-01 1.250000e-02 1.250000e-02 3.987500e+00 2.581804e-01 3.006164e-01
+2.025000e-01 4.750000e-02 4.750000e-02 3.885700e-01 6.075736e-02 2.513260e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d21-x01-y03
+Path=/REF/CMS_2018_I1690148/d21-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-02 2.000000e-02 2.000000e-02 3.473100e+00 2.055459e-01 1.804902e-01
+5.250000e-02 1.250000e-02 1.250000e-02 7.210200e+00 3.522269e-01 1.760977e-01
+7.750000e-02 1.250000e-02 1.250000e-02 8.689300e+00 1.452801e-01 4.389990e-01
+1.000000e-01 1.000000e-02 1.000000e-02 8.811900e+00 3.889358e-01 2.595959e-01
+1.200000e-01 1.000000e-02 1.000000e-02 7.044800e+00 2.745349e-01 2.970085e-01
+1.425000e-01 1.250000e-02 1.250000e-02 4.179600e+00 1.871993e-01 3.859952e-01
+2.025000e-01 4.750000e-02 4.750000e-02 4.417000e-01 1.601820e-01 3.568597e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d21-x01-y04
+Path=/REF/CMS_2018_I1690148/d21-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-02 2.000000e-02 2.000000e-02 2.365500e+00 2.551525e-01 1.569424e-01
+5.250000e-02 1.250000e-02 1.250000e-02 5.684800e+00 3.955579e-01 4.191331e-01
+7.750000e-02 1.250000e-02 1.250000e-02 8.509700e+00 3.249055e-01 5.206476e-01
+1.000000e-01 1.000000e-02 1.000000e-02 9.386900e+00 5.374408e-01 7.040576e-01
+1.200000e-01 1.000000e-02 1.000000e-02 8.744100e+00 4.586702e-01 6.158451e-01
+1.425000e-01 1.250000e-02 1.250000e-02 5.187500e+00 5.959254e-01 2.706052e-01
+2.025000e-01 4.750000e-02 4.750000e-02 6.127200e-01 9.689679e-02 6.621767e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d22-x01-y01
+Path=/REF/CMS_2018_I1690148/d22-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-02 1.000000e-02 1.000000e-02 2.654500e+01 1.058161e+00 9.217548e-01
+2.500000e-02 5.000000e-03 5.000000e-03 1.705000e+01 5.588863e-01 8.148511e-01
+3.700000e-02 7.000000e-03 7.000000e-03 1.174700e+01 3.833269e-01 4.310831e-01
+5.000000e-02 6.000000e-03 6.000000e-03 6.198500e+00 4.629567e-01 4.485644e-01
+7.800000e-02 2.200000e-02 2.200000e-02 1.358300e+00 1.079364e-01 9.363010e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d22-x01-y02
+Path=/REF/CMS_2018_I1690148/d22-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-02 1.000000e-02 1.000000e-02 2.644900e+01 1.094462e+00 1.003830e+00
+2.500000e-02 5.000000e-03 5.000000e-03 1.751500e+01 7.804989e-01 9.695307e-01
+3.700000e-02 7.000000e-03 7.000000e-03 1.200800e+01 5.527544e-01 5.037095e-01
+5.000000e-02 6.000000e-03 6.000000e-03 6.080300e+00 5.250197e-01 4.112838e-01
+7.800000e-02 2.200000e-02 2.200000e-02 1.245600e+00 8.209872e-02 1.179021e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d22-x01-y03
+Path=/REF/CMS_2018_I1690148/d22-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-02 1.000000e-02 1.000000e-02 2.745000e+01 9.910941e-01 7.581264e-01
+2.500000e-02 5.000000e-03 5.000000e-03 1.651600e+01 5.150619e-01 5.400423e-01
+3.700000e-02 7.000000e-03 7.000000e-03 1.100800e+01 2.848154e-01 5.115387e-01
+5.000000e-02 6.000000e-03 6.000000e-03 6.027600e+00 4.035222e-01 5.008135e-01
+7.800000e-02 2.200000e-02 2.200000e-02 1.349900e+00 1.376654e-01 1.364737e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d22-x01-y04
+Path=/REF/CMS_2018_I1690148/d22-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.000000e-02 1.000000e-02 1.000000e-02 2.243700e+01 1.533668e+00 1.151397e+00
+2.500000e-02 5.000000e-03 5.000000e-03 1.765600e+01 9.063725e-01 2.080842e+00
+3.700000e-02 7.000000e-03 7.000000e-03 1.421300e+01 8.766165e-01 7.327084e-01
+5.000000e-02 6.000000e-03 6.000000e-03 7.561000e+00 1.103572e+00 8.330688e-01
+7.800000e-02 2.200000e-02 2.200000e-02 1.931800e+00 2.711596e-01 1.822728e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d23-x01-y01
+Path=/REF/CMS_2018_I1690148/d23-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-01 5.000000e-02 5.000000e-02 3.115700e+00 2.227997e-01 2.280071e-01
+5.250000e-01 2.500000e-02 2.500000e-02 4.604900e+00 1.149819e-01 1.483159e-01
+5.700000e-01 2.000000e-02 2.000000e-02 5.139100e+00 2.091534e-01 1.209040e-01
+6.050000e-01 1.500000e-02 1.500000e-02 4.547200e+00 2.978975e-01 3.820394e-01
+6.300000e-01 1.000000e-02 1.000000e-02 2.972500e+00 3.435570e-01 3.747594e-01
+6.500000e-01 1.000000e-02 1.000000e-02 2.071600e+00 2.811926e-01 2.858517e-01
+7.050000e-01 4.500000e-02 4.500000e-02 1.702300e-01 3.770152e-02 4.596320e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d23-x01-y02
+Path=/REF/CMS_2018_I1690148/d23-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-01 5.000000e-02 5.000000e-02 2.759400e+00 2.871150e-01 3.037197e-01
+5.250000e-01 2.500000e-02 2.500000e-02 4.613200e+00 2.002594e-01 1.589429e-01
+5.700000e-01 2.000000e-02 2.000000e-02 5.375600e+00 2.310059e-01 1.883721e-01
+6.050000e-01 1.500000e-02 1.500000e-02 5.103600e+00 3.563355e-01 5.381379e-01
+6.300000e-01 1.000000e-02 1.000000e-02 3.304700e+00 4.861391e-01 4.396835e-01
+6.500000e-01 1.000000e-02 1.000000e-02 2.196900e+00 3.177345e-01 3.445343e-01
+7.050000e-01 4.500000e-02 4.500000e-02 1.692300e-01 4.633213e-02 5.491796e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d23-x01-y03
+Path=/REF/CMS_2018_I1690148/d23-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-01 5.000000e-02 5.000000e-02 3.805100e+00 2.079340e-01 2.100171e-01
+5.250000e-01 2.500000e-02 2.500000e-02 4.767600e+00 1.888494e-01 2.627076e-01
+5.700000e-01 2.000000e-02 2.000000e-02 4.746700e+00 2.775545e-01 2.557518e-01
+6.050000e-01 1.500000e-02 1.500000e-02 3.755800e+00 3.522881e-01 3.121261e-01
+6.300000e-01 1.000000e-02 1.000000e-02 2.159600e+00 2.848957e-01 3.712561e-01
+6.500000e-01 1.000000e-02 1.000000e-02 1.363100e+00 2.244124e-01 2.011954e-01
+7.050000e-01 4.500000e-02 4.500000e-02 9.018800e-02 1.702688e-02 2.320216e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d23-x01-y04
+Path=/REF/CMS_2018_I1690148/d23-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-01 5.000000e-02 5.000000e-02 2.365100e+00 2.772682e-01 1.967313e-01
+5.250000e-01 2.500000e-02 2.500000e-02 4.048900e+00 3.432252e-01 3.606322e-01
+5.700000e-01 2.000000e-02 2.000000e-02 5.301800e+00 5.569917e-01 5.303882e-01
+6.050000e-01 1.500000e-02 1.500000e-02 4.761500e+00 5.810352e-01 8.994795e-01
+6.300000e-01 1.000000e-02 1.000000e-02 4.548400e+00 9.204870e-01 7.511399e-01
+6.500000e-01 1.000000e-02 1.000000e-02 3.797200e+00 6.133035e-01 5.319886e-01
+7.050000e-01 4.500000e-02 4.500000e-02 4.357200e-01 1.528549e-01 1.365041e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d24-x01-y01
+Path=/REF/CMS_2018_I1690148/d24-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.050000e-01 1.050000e-01 1.050000e-01 1.424500e+00 1.144555e-01 9.848213e-02
+3.350000e-01 2.500000e-02 2.500000e-02 4.320800e+00 1.317020e-01 9.732311e-02
+3.800000e-01 2.000000e-02 2.000000e-02 5.287200e+00 1.339958e-01 2.656117e-01
+4.200000e-01 2.000000e-02 2.000000e-02 4.261000e+00 2.769413e-01 2.571882e-01
+4.550000e-01 1.500000e-02 1.500000e-02 2.400600e+00 1.942099e-01 1.915023e-01
+4.800000e-01 1.000000e-02 1.000000e-02 1.136500e+00 1.176165e-01 1.301826e-01
+5.450000e-01 5.500000e-02 5.500000e-02 7.394200e-02 1.469458e-02 1.613690e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d24-x01-y02
+Path=/REF/CMS_2018_I1690148/d24-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.050000e-01 1.050000e-01 1.050000e-01 1.289900e+00 1.393448e-01 1.364577e-01
+3.350000e-01 2.500000e-02 2.500000e-02 4.388700e+00 1.883783e-01 1.557168e-01
+3.800000e-01 2.000000e-02 2.000000e-02 5.719000e+00 2.309260e-01 2.977396e-01
+4.200000e-01 2.000000e-02 2.000000e-02 4.519000e+00 3.736966e-01 3.599655e-01
+4.550000e-01 1.500000e-02 1.500000e-02 2.333000e+00 2.660835e-01 2.439994e-01
+4.800000e-01 1.000000e-02 1.000000e-02 1.069400e+00 1.393310e-01 1.489536e-01
+5.450000e-01 5.500000e-02 5.500000e-02 7.986000e-02 1.516626e-02 1.695136e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d24-x01-y03
+Path=/REF/CMS_2018_I1690148/d24-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.050000e-01 1.050000e-01 1.050000e-01 1.675100e+00 1.061224e-01 7.560343e-02
+3.350000e-01 2.500000e-02 2.500000e-02 4.349400e+00 1.139617e-01 1.217623e-01
+3.800000e-01 2.000000e-02 2.000000e-02 4.783700e+00 1.298806e-01 3.319563e-01
+4.200000e-01 2.000000e-02 2.000000e-02 3.782300e+00 2.433596e-01 2.002581e-01
+4.550000e-01 1.500000e-02 1.500000e-02 2.071200e+00 1.514696e-01 1.944400e-01
+4.800000e-01 1.000000e-02 1.000000e-02 1.009600e+00 1.272752e-01 1.352358e-01
+5.450000e-01 5.500000e-02 5.500000e-02 5.261300e-02 1.196095e-02 1.123281e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d24-x01-y04
+Path=/REF/CMS_2018_I1690148/d24-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.050000e-01 1.050000e-01 1.050000e-01 1.047700e+00 1.248311e-01 9.511129e-02
+3.350000e-01 2.500000e-02 2.500000e-02 3.759500e+00 2.849470e-01 4.026403e-01
+3.800000e-01 2.000000e-02 2.000000e-02 5.231500e+00 3.656740e-01 5.783268e-01
+4.200000e-01 2.000000e-02 2.000000e-02 5.239200e+00 4.354391e-01 3.964242e-01
+4.550000e-01 1.500000e-02 1.500000e-02 4.013900e+00 3.795037e-01 3.196780e-01
+4.800000e-01 1.000000e-02 1.000000e-02 1.936600e+00 3.759546e-01 3.469075e-01
+5.450000e-01 5.500000e-02 5.500000e-02 1.276000e-01 7.653396e-02 7.536610e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d25-x01-y01
+Path=/REF/CMS_2018_I1690148/d25-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.500000e-02 8.500000e-02 8.500000e-02 1.640800e+00 1.144629e-01 1.088632e-01
+1.900000e-01 2.000000e-02 2.000000e-02 5.202900e+00 1.427371e-01 9.308327e-02
+2.250000e-01 1.500000e-02 1.500000e-02 5.863900e+00 1.467728e-01 1.736111e-01
+2.600000e-01 2.000000e-02 2.000000e-02 5.024100e+00 2.126188e-01 2.501782e-01
+2.950000e-01 1.500000e-02 1.500000e-02 3.141000e+00 2.126072e-01 1.920538e-01
+3.250000e-01 1.500000e-02 1.500000e-02 1.120200e+00 2.004634e-01 1.101597e-01
+3.700000e-01 3.000000e-02 3.000000e-02 1.373400e-01 3.856280e-02 2.540125e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d25-x01-y02
+Path=/REF/CMS_2018_I1690148/d25-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.500000e-02 8.500000e-02 8.500000e-02 1.579700e+00 1.341179e-01 1.484682e-01
+1.900000e-01 2.000000e-02 2.000000e-02 5.311700e+00 1.984897e-01 1.011725e-01
+2.250000e-01 1.500000e-02 1.500000e-02 6.053600e+00 2.021247e-01 3.155056e-01
+2.600000e-01 2.000000e-02 2.000000e-02 5.194400e+00 2.690693e-01 2.363868e-01
+2.950000e-01 1.500000e-02 1.500000e-02 3.021900e+00 2.576644e-01 2.361011e-01
+3.250000e-01 1.500000e-02 1.500000e-02 9.778900e-01 1.513437e-01 2.106150e-01
+3.700000e-01 3.000000e-02 3.000000e-02 1.602300e-01 1.791641e-01 1.163542e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d25-x01-y03
+Path=/REF/CMS_2018_I1690148/d25-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.500000e-02 8.500000e-02 8.500000e-02 1.813900e+00 1.070913e-01 8.070044e-02
+1.900000e-01 2.000000e-02 2.000000e-02 5.266500e+00 1.411583e-01 2.151647e-01
+2.250000e-01 1.500000e-02 1.500000e-02 5.537600e+00 1.958821e-01 1.744470e-01
+2.600000e-01 2.000000e-02 2.000000e-02 4.669600e+00 1.741000e-01 2.719702e-01
+2.950000e-01 1.500000e-02 1.500000e-02 2.986700e+00 1.937705e-01 2.040273e-01
+3.250000e-01 1.500000e-02 1.500000e-02 1.059000e+00 1.529045e-01 1.292684e-01
+3.700000e-01 3.000000e-02 3.000000e-02 1.114900e-01 6.142496e-02 2.923828e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d25-x01-y04
+Path=/REF/CMS_2018_I1690148/d25-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.500000e-02 8.500000e-02 8.500000e-02 1.195700e+00 1.162320e-01 1.051817e-01
+1.900000e-01 2.000000e-02 2.000000e-02 4.334000e+00 2.852931e-01 3.340274e-01
+2.250000e-01 1.500000e-02 1.500000e-02 6.109200e+00 3.849774e-01 3.944545e-01
+2.600000e-01 2.000000e-02 2.000000e-02 6.001500e+00 3.228289e-01 4.037270e-01
+2.950000e-01 1.500000e-02 1.500000e-02 4.305400e+00 4.241266e-01 2.366496e-01
+3.250000e-01 1.500000e-02 1.500000e-02 1.987100e+00 3.475578e-01 4.240467e-01
+3.700000e-01 3.000000e-02 3.000000e-02 1.877400e-01 2.803454e-01 2.275236e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d26-x01-y01
+Path=/REF/CMS_2018_I1690148/d26-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-02 2.000000e-02 2.000000e-02 3.586800e+00 2.661864e-01 2.608416e-01
+5.750000e-02 1.750000e-02 1.750000e-02 7.354800e+00 2.482220e-01 2.275119e-01
+9.000000e-02 1.500000e-02 1.500000e-02 7.513400e+00 1.260819e-01 1.488361e-01
+1.175000e-01 1.250000e-02 1.250000e-02 6.596400e+00 2.227214e-01 2.065267e-01
+1.425000e-01 1.250000e-02 1.250000e-02 4.689700e+00 2.369306e-01 2.416056e-01
+1.700000e-01 1.500000e-02 1.500000e-02 2.392300e+00 1.836688e-01 1.897685e-01
+2.175000e-01 3.250000e-02 3.250000e-02 3.044200e-01 5.270306e-02 5.467113e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d26-x01-y02
+Path=/REF/CMS_2018_I1690148/d26-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-02 2.000000e-02 2.000000e-02 3.440400e+00 3.260227e-01 3.849298e-01
+5.750000e-02 1.750000e-02 1.750000e-02 7.453800e+00 2.290780e-01 3.660600e-01
+9.000000e-02 1.500000e-02 1.500000e-02 7.715100e+00 2.227125e-01 3.765390e-01
+1.175000e-01 1.250000e-02 1.250000e-02 6.834800e+00 2.893582e-01 4.453367e-01
+1.425000e-01 1.250000e-02 1.250000e-02 4.443100e+00 3.138278e-01 3.684840e-01
+1.700000e-01 1.500000e-02 1.500000e-02 2.297200e+00 2.146584e-01 7.404841e-01
+2.175000e-01 3.250000e-02 3.250000e-02 2.951300e-01 7.813713e-01 5.905368e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d26-x01-y03
+Path=/REF/CMS_2018_I1690148/d26-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-02 2.000000e-02 2.000000e-02 3.996200e+00 2.200922e-01 2.165674e-01
+5.750000e-02 1.750000e-02 1.750000e-02 7.592200e+00 2.797880e-01 1.632267e-01
+9.000000e-02 1.500000e-02 1.500000e-02 7.353400e+00 1.488457e-01 2.217845e-01
+1.175000e-01 1.250000e-02 1.250000e-02 6.109900e+00 2.063781e-01 1.957922e-01
+1.425000e-01 1.250000e-02 1.250000e-02 4.557200e+00 1.937631e-01 3.137590e-01
+1.700000e-01 1.500000e-02 1.500000e-02 2.287500e+00 1.921716e-01 2.058485e-01
+2.175000e-01 3.250000e-02 3.250000e-02 2.849500e-01 1.262167e-01 4.945997e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d26-x01-y04
+Path=/REF/CMS_2018_I1690148/d26-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.000000e-02 2.000000e-02 2.000000e-02 2.619600e+00 3.159030e-01 1.838674e-01
+5.750000e-02 1.750000e-02 1.750000e-02 5.677600e+00 2.853949e-01 5.809931e-01
+9.000000e-02 1.500000e-02 1.500000e-02 7.089300e+00 4.132940e-01 3.926596e-01
+1.175000e-01 1.250000e-02 1.250000e-02 7.425900e+00 3.215830e-01 4.548305e-01
+1.425000e-01 1.250000e-02 1.250000e-02 6.521400e+00 6.996668e-01 3.538256e-01
+1.700000e-01 1.500000e-02 1.500000e-02 3.570500e+00 4.696657e-01 6.880968e-01
+2.175000e-01 3.250000e-02 3.250000e-02 4.311500e-01 2.130912e-01 1.540474e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d27-x01-y01
+Path=/REF/CMS_2018_I1690148/d27-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-02 1.500000e-02 1.500000e-02 2.664600e+01 2.775459e-01 1.844995e+00
+3.750000e-02 7.500000e-03 7.500000e-03 6.838900e+00 8.682784e-01 2.277863e+00
+5.250000e-02 7.500000e-03 7.500000e-03 4.337000e+00 4.124411e+00 4.759583e-01
+1.050000e-01 4.500000e-02 4.500000e-02 3.665100e-01 3.533283e-01 5.390430e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d27-x01-y02
+Path=/REF/CMS_2018_I1690148/d27-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-02 1.500000e-02 1.500000e-02 2.743300e+01 6.657330e-01 8.349162e-01
+3.750000e-02 7.500000e-03 7.500000e-03 6.796300e+00 1.194513e+00 1.023518e+00
+5.250000e-02 7.500000e-03 7.500000e-03 3.298400e+00 4.156939e-01 4.488552e-01
+1.050000e-01 4.500000e-02 4.500000e-02 2.843700e-01 1.884229e-01 3.336006e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d27-x01-y03
+Path=/REF/CMS_2018_I1690148/d27-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-02 1.500000e-02 1.500000e-02 2.734400e+01 1.051325e+00 5.120375e-01
+3.750000e-02 7.500000e-03 7.500000e-03 7.047800e+00 6.859253e-01 1.317381e+00
+5.250000e-02 7.500000e-03 7.500000e-03 3.317800e+00 2.041679e-01 5.353803e-01
+1.050000e-01 4.500000e-02 4.500000e-02 2.689400e-01 3.507549e-02 5.545610e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d27-x01-y04
+Path=/REF/CMS_2018_I1690148/d27-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-02 1.500000e-02 1.500000e-02 2.427100e+01 1.837217e+00 4.238762e-01
+3.750000e-02 7.500000e-03 7.500000e-03 1.033600e+01 2.595186e+00 7.726363e-01
+5.250000e-02 7.500000e-03 7.500000e-03 4.939600e+00 8.124541e-01 4.048765e+00
+1.050000e-01 4.500000e-02 4.500000e-02 4.749400e-01 6.596762e-02 2.635386e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d28-x01-y01
+Path=/REF/CMS_2018_I1690148/d28-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.250000e-02 3.250000e-02 3.250000e-02 3.858600e+00 2.481281e-01 1.987425e-01
+7.750000e-02 1.250000e-02 1.250000e-02 9.086300e+00 1.822435e-01 2.139473e-01
+1.000000e-01 1.000000e-02 1.000000e-02 1.054400e+01 1.791362e-01 2.818248e-01
+1.175000e-01 7.500000e-03 7.500000e-03 9.539300e+00 3.743959e-01 3.363815e-01
+1.325000e-01 7.500000e-03 7.500000e-03 7.067800e+00 3.843378e-01 4.127415e-01
+1.450000e-01 5.000000e-03 5.000000e-03 4.006800e+00 3.166409e-01 3.810036e-01
+1.650000e-01 1.500000e-02 1.500000e-02 7.328200e-01 7.155433e-02 8.564102e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d28-x01-y02
+Path=/REF/CMS_2018_I1690148/d28-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.250000e-02 3.250000e-02 3.250000e-02 3.178500e+00 3.504371e-01 3.156112e-01
+7.750000e-02 1.250000e-02 1.250000e-02 8.468600e+00 3.531022e-01 2.796330e-01
+1.000000e-01 1.000000e-02 1.000000e-02 1.095900e+01 2.950463e-01 4.512216e-01
+1.175000e-01 7.500000e-03 7.500000e-03 1.100300e+01 5.961085e-01 5.774171e-01
+1.325000e-01 7.500000e-03 7.500000e-03 8.400000e+00 7.044700e-01 6.427642e-01
+1.450000e-01 5.000000e-03 5.000000e-03 4.586200e+00 4.086679e-01 6.748566e-01
+1.650000e-01 1.500000e-02 1.500000e-02 8.527900e-01 1.160108e-01 1.134878e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d28-x01-y03
+Path=/REF/CMS_2018_I1690148/d28-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.250000e-02 3.250000e-02 3.250000e-02 4.775800e+00 2.332405e-01 1.513602e-01
+7.750000e-02 1.250000e-02 1.250000e-02 9.664400e+00 1.316564e-01 3.236721e-01
+1.000000e-01 1.000000e-02 1.000000e-02 1.001100e+01 2.026917e-01 2.612139e-01
+1.175000e-01 7.500000e-03 7.500000e-03 7.793400e+00 3.659992e-01 2.778968e-01
+1.325000e-01 7.500000e-03 7.500000e-03 5.479300e+00 2.898573e-01 3.534071e-01
+1.450000e-01 5.000000e-03 5.000000e-03 3.119700e+00 2.890588e-01 4.154613e-01
+1.650000e-01 1.500000e-02 1.500000e-02 5.816200e-01 7.894500e-02 6.625488e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d28-x01-y04
+Path=/REF/CMS_2018_I1690148/d28-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.250000e-02 3.250000e-02 3.250000e-02 3.360200e+00 2.418353e-01 2.013036e-01
+7.750000e-02 1.250000e-02 1.250000e-02 8.890200e+00 3.830374e-01 4.130432e-01
+1.000000e-01 1.000000e-02 1.000000e-02 1.048400e+01 5.821684e-01 6.644016e-01
+1.175000e-01 7.500000e-03 7.500000e-03 1.057400e+01 7.375298e-01 6.816988e-01
+1.325000e-01 7.500000e-03 7.500000e-03 7.865100e+00 7.321974e-01 7.837431e-01
+1.450000e-01 5.000000e-03 5.000000e-03 4.868300e+00 8.374029e-01 5.183925e-01
+1.650000e-01 1.500000e-02 1.500000e-02 8.130700e-01 1.676413e-01 1.896605e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d29-x01-y01
+Path=/REF/CMS_2018_I1690148/d29-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.300000e-01 8.000000e-02 8.000000e-02 2.428400e+00 1.382449e-01 1.215559e-01
+3.300000e-01 2.000000e-02 2.000000e-02 5.944300e+00 1.484035e-01 7.355117e-02
+3.650000e-01 1.500000e-02 1.500000e-02 7.132700e+00 2.130590e-01 3.829079e-01
+3.900000e-01 1.000000e-02 1.000000e-02 5.361500e+00 4.632502e-01 3.879089e-01
+4.100000e-01 1.000000e-02 1.000000e-02 2.364100e+00 2.211953e-01 3.483099e-01
+4.350000e-01 1.500000e-02 1.500000e-02 1.732800e-01 4.390871e-02 3.683802e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d29-x01-y02
+Path=/REF/CMS_2018_I1690148/d29-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.300000e-01 8.000000e-02 8.000000e-02 2.152400e+00 1.640070e-01 1.522043e-01
+3.300000e-01 2.000000e-02 2.000000e-02 5.908400e+00 1.851365e-01 2.032026e-01
+3.650000e-01 1.500000e-02 1.500000e-02 7.642300e+00 2.878698e-01 4.034639e-01
+3.900000e-01 1.000000e-02 1.000000e-02 6.281900e+00 5.575654e-01 5.017819e-01
+4.100000e-01 1.000000e-02 1.000000e-02 2.864900e+00 2.981505e-01 4.522340e-01
+4.350000e-01 1.500000e-02 1.500000e-02 2.357900e-01 6.534234e-02 5.780588e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d29-x01-y03
+Path=/REF/CMS_2018_I1690148/d29-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.300000e-01 8.000000e-02 8.000000e-02 2.829800e+00 1.376319e-01 1.121169e-01
+3.300000e-01 2.000000e-02 2.000000e-02 6.010600e+00 2.006583e-01 1.411930e-01
+3.650000e-01 1.500000e-02 1.500000e-02 6.378900e+00 2.092634e-01 3.842195e-01
+3.900000e-01 1.000000e-02 1.000000e-02 4.158500e+00 3.630814e-01 3.590074e-01
+4.100000e-01 1.000000e-02 1.000000e-02 1.533500e+00 1.471352e-01 2.588398e-01
+4.350000e-01 1.500000e-02 1.500000e-02 5.356200e-02 3.290778e-02 2.338415e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d29-x01-y04
+Path=/REF/CMS_2018_I1690148/d29-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.300000e-01 8.000000e-02 8.000000e-02 1.985000e+00 1.587023e-01 1.189665e-01
+3.300000e-01 2.000000e-02 2.000000e-02 5.781000e+00 4.070955e-01 2.729020e-01
+3.650000e-01 1.500000e-02 1.500000e-02 7.916400e+00 3.453901e-01 8.745672e-01
+3.900000e-01 1.000000e-02 1.000000e-02 6.347200e+00 8.930903e-01 5.920981e-01
+4.100000e-01 1.000000e-02 1.000000e-02 3.788400e+00 4.103921e-01 4.965136e-01
+4.350000e-01 1.500000e-02 1.500000e-02 3.652100e-01 9.671120e-02 1.339917e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d30-x01-y01
+Path=/REF/CMS_2018_I1690148/d30-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.250000e-01 4.250000e-01 4.250000e-01 2.082700e-01 1.720261e-02 1.790110e-02
+1.150000e+00 1.000000e-01 1.000000e-01 1.042700e+00 4.489370e-02 3.658014e-02
+1.300000e+00 5.000000e-02 5.000000e-02 1.785900e+00 9.702097e-02 7.341153e-02
+1.425000e+00 7.500000e-02 7.500000e-02 1.361800e+00 6.657555e-02 7.802198e-02
+1.575000e+00 7.500000e-02 7.500000e-02 7.063100e-01 3.863100e-02 2.824523e-02
+1.725000e+00 7.500000e-02 7.500000e-02 3.438000e-01 1.328036e-02 2.003816e-02
+1.925000e+00 1.250000e-01 1.250000e-01 1.769000e-01 9.334157e-03 9.022795e-03
+2.275000e+00 2.250000e-01 2.250000e-01 6.627700e-02 5.907562e-03 9.221268e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d30-x01-y02
+Path=/REF/CMS_2018_I1690148/d30-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.250000e-01 4.250000e-01 4.250000e-01 1.950800e-01 2.067206e-02 2.274436e-02
+1.150000e+00 1.000000e-01 1.000000e-01 1.065900e+00 5.093660e-02 4.980775e-02
+1.300000e+00 5.000000e-02 5.000000e-02 1.920700e+00 1.142978e-01 1.063690e-01
+1.425000e+00 7.500000e-02 7.500000e-02 1.447000e+00 9.045246e-02 9.417470e-02
+1.575000e+00 7.500000e-02 7.500000e-02 7.112600e-01 4.384158e-02 3.354986e-02
+1.725000e+00 7.500000e-02 7.500000e-02 3.184800e-01 2.465114e-02 2.607644e-02
+1.925000e+00 1.250000e-01 1.250000e-01 1.507100e-01 1.217050e-02 1.299491e-02
+2.275000e+00 2.250000e-01 2.250000e-01 4.387000e-02 1.119325e-02 1.557937e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d30-x01-y03
+Path=/REF/CMS_2018_I1690148/d30-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.250000e-01 4.250000e-01 4.250000e-01 2.395300e-01 1.683375e-02 1.689298e-02
+1.150000e+00 1.000000e-01 1.000000e-01 1.073100e+00 5.415427e-02 3.518666e-02
+1.300000e+00 5.000000e-02 5.000000e-02 1.625800e+00 9.713190e-02 9.492636e-02
+1.425000e+00 7.500000e-02 7.500000e-02 1.222600e+00 5.526087e-02 7.168626e-02
+1.575000e+00 7.500000e-02 7.500000e-02 6.553100e-01 4.903058e-02 3.090604e-02
+1.725000e+00 7.500000e-02 7.500000e-02 3.502700e-01 1.726834e-02 4.085733e-02
+1.925000e+00 1.250000e-01 1.250000e-01 1.943600e-01 1.589007e-02 1.199499e-02
+2.275000e+00 2.250000e-01 2.250000e-01 8.086600e-02 9.851638e-03 8.251773e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d30-x01-y04
+Path=/REF/CMS_2018_I1690148/d30-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.250000e-01 4.250000e-01 4.250000e-01 1.428600e-01 2.252369e-02 1.979677e-02
+1.150000e+00 1.000000e-01 1.000000e-01 8.231800e-01 7.131306e-02 7.991916e-02
+1.300000e+00 5.000000e-02 5.000000e-02 1.685500e+00 1.926886e-01 9.089708e-02
+1.425000e+00 7.500000e-02 7.500000e-02 1.527400e+00 1.337389e-01 1.446767e-01
+1.575000e+00 7.500000e-02 7.500000e-02 9.069200e-01 5.887928e-02 6.508979e-02
+1.725000e+00 7.500000e-02 7.500000e-02 4.421600e-01 7.321108e-02 3.100902e-02
+1.925000e+00 1.250000e-01 1.250000e-01 2.419800e-01 2.278934e-02 3.355897e-02
+2.275000e+00 2.250000e-01 2.250000e-01 1.187100e-01 2.497134e-02 4.498097e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d31-x01-y01
+Path=/REF/CMS_2018_I1690148/d31-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.375000e-02 1.375000e-02 1.375000e-02 7.916600e+00 5.040832e-01 4.120900e-01
+3.375000e-02 6.250000e-03 6.250000e-03 1.246800e+01 2.489091e-01 3.154597e-01
+4.625000e-02 6.250000e-03 6.250000e-03 1.397700e+01 1.658771e-01 4.455309e-01
+5.875000e-02 6.250000e-03 6.250000e-03 1.368900e+01 4.292950e-01 2.697409e-01
+7.250000e-02 7.500000e-03 7.500000e-03 1.076800e+01 3.637031e-01 3.993997e-01
+8.625000e-02 6.250000e-03 6.250000e-03 6.542700e+00 4.084514e-01 2.553127e-01
+9.875000e-02 6.250000e-03 6.250000e-03 2.592500e+00 1.836715e-01 3.075691e-01
+1.125000e-01 7.500000e-03 7.500000e-03 3.264100e-01 5.902599e-02 4.382344e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d31-x01-y02
+Path=/REF/CMS_2018_I1690148/d31-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.375000e-02 1.375000e-02 1.375000e-02 6.613600e+00 7.119545e-01 6.459117e-01
+3.375000e-02 6.250000e-03 6.250000e-03 1.157000e+01 3.812948e-01 5.321546e-01
+4.625000e-02 6.250000e-03 6.250000e-03 1.411100e+01 3.161144e-01 6.366302e-01
+5.875000e-02 6.250000e-03 6.250000e-03 1.466200e+01 6.390597e-01 4.789543e-01
+7.250000e-02 7.500000e-03 7.500000e-03 1.194800e+01 5.524767e-01 5.936876e-01
+8.625000e-02 6.250000e-03 6.250000e-03 7.360700e+00 6.347253e-01 4.042692e-01
+9.875000e-02 6.250000e-03 6.250000e-03 2.928700e+00 2.286597e-01 4.248185e-01
+1.125000e-01 7.500000e-03 7.500000e-03 3.997800e-01 2.461443e-01 4.631064e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d31-x01-y03
+Path=/REF/CMS_2018_I1690148/d31-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.375000e-02 1.375000e-02 1.375000e-02 9.460100e+00 4.744193e-01 3.042040e-01
+3.375000e-02 6.250000e-03 6.250000e-03 1.333100e+01 3.660672e-01 4.658326e-01
+4.625000e-02 6.250000e-03 6.250000e-03 1.376700e+01 2.400246e-01 5.475922e-01
+5.875000e-02 6.250000e-03 6.250000e-03 1.259100e+01 3.950784e-01 3.470209e-01
+7.250000e-02 7.500000e-03 7.500000e-03 9.453300e+00 3.652134e-01 3.775787e-01
+8.625000e-02 6.250000e-03 6.250000e-03 5.434700e+00 3.029091e-01 2.106521e-01
+9.875000e-02 6.250000e-03 6.250000e-03 2.422300e+00 2.260779e-01 3.585331e-01
+1.125000e-01 7.500000e-03 7.500000e-03 2.487700e-01 6.288875e-02 2.034447e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d31-x01-y04
+Path=/REF/CMS_2018_I1690148/d31-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.375000e-02 1.375000e-02 1.375000e-02 7.913200e+00 4.460076e-01 5.021159e-01
+3.375000e-02 6.250000e-03 6.250000e-03 1.196600e+01 7.243340e-01 7.546810e-01
+4.625000e-02 6.250000e-03 6.250000e-03 1.369500e+01 8.912710e-01 8.253811e-01
+5.875000e-02 6.250000e-03 6.250000e-03 1.376500e+01 8.147409e-01 7.214252e-01
+7.250000e-02 7.500000e-03 7.500000e-03 1.119500e+01 5.663194e-01 9.769750e-01
+8.625000e-02 6.250000e-03 6.250000e-03 7.288100e+00 7.696537e-01 5.009770e-01
+9.875000e-02 6.250000e-03 6.250000e-03 1.948700e+00 9.664308e-01 5.438933e-01
+1.125000e-01 7.500000e-03 7.500000e-03 4.108000e-01 8.245707e-02 1.600748e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d32-x01-y01
+Path=/REF/CMS_2018_I1690148/d32-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.500000e-02 6.500000e-02 6.500000e-02 1.566900e+00 1.217591e-01 8.681513e-02
+1.600000e-01 3.000000e-02 3.000000e-02 3.399300e+00 7.134494e-02 1.061069e-01
+2.100000e-01 2.000000e-02 2.000000e-02 4.599200e+00 8.580883e-02 1.130698e-01
+2.500000e-01 2.000000e-02 2.000000e-02 5.407000e+00 1.337605e-01 1.430328e-01
+2.950000e-01 2.500000e-02 2.500000e-02 3.619700e+00 2.063534e-01 2.533332e-01
+3.400000e-01 2.000000e-02 2.000000e-02 2.777600e-01 5.023078e-02 6.017412e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d32-x01-y02
+Path=/REF/CMS_2018_I1690148/d32-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.500000e-02 6.500000e-02 6.500000e-02 1.383100e+00 1.347186e-01 1.216908e-01
+1.600000e-01 3.000000e-02 3.000000e-02 3.085600e+00 1.326097e-01 1.512970e-01
+2.100000e-01 2.000000e-02 2.000000e-02 4.796700e+00 9.972520e-02 1.654629e-01
+2.500000e-01 2.000000e-02 2.000000e-02 5.665200e+00 1.846786e-01 1.850421e-01
+2.950000e-01 2.500000e-02 2.500000e-02 4.084900e+00 2.939855e-01 3.010467e-01
+3.400000e-01 2.000000e-02 2.000000e-02 3.084600e-01 5.972014e-02 6.687591e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d32-x01-y03
+Path=/REF/CMS_2018_I1690148/d32-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.500000e-02 6.500000e-02 6.500000e-02 1.840600e+00 1.295761e-01 6.972366e-02
+1.600000e-01 3.000000e-02 3.000000e-02 3.702600e+00 5.681819e-02 1.080929e-01
+2.100000e-01 2.000000e-02 2.000000e-02 4.454400e+00 1.401310e-01 1.199062e-01
+2.500000e-01 2.000000e-02 2.000000e-02 5.006900e+00 1.626826e-01 1.821669e-01
+2.950000e-01 2.500000e-02 2.500000e-02 3.056200e+00 1.453276e-01 2.557619e-01
+3.400000e-01 2.000000e-02 2.000000e-02 1.825100e-01 9.540857e-02 6.380761e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d32-x01-y04
+Path=/REF/CMS_2018_I1690148/d32-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.500000e-02 6.500000e-02 6.500000e-02 1.318700e+00 1.608639e-01 1.112887e-01
+1.600000e-01 3.000000e-02 3.000000e-02 3.367200e+00 1.706950e-01 2.758027e-01
+2.100000e-01 2.000000e-02 2.000000e-02 4.306900e+00 2.019296e-01 4.255714e-01
+2.500000e-01 2.000000e-02 2.000000e-02 5.817700e+00 3.394961e-01 3.262279e-01
+2.950000e-01 2.500000e-02 2.500000e-02 3.935700e+00 2.590262e-01 4.302648e-01
+3.400000e-01 2.000000e-02 2.000000e-02 6.191300e-01 9.402320e-01 1.530309e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d33-x01-y01
+Path=/REF/CMS_2018_I1690148/d33-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-01 4.500000e-01 4.500000e-01 2.708500e-01 2.091286e-02 2.046557e-02
+1.050000e+00 1.500000e-01 1.500000e-01 9.582000e-01 2.796689e-02 1.901842e-02
+1.350000e+00 1.500000e-01 1.500000e-01 8.140700e-01 3.687978e-02 3.889295e-02
+1.650000e+00 1.500000e-01 1.500000e-01 3.742900e-01 1.234429e-02 1.639559e-02
+2.000000e+00 2.000000e-01 2.000000e-01 1.596300e-01 5.203062e-03 8.782674e-03
+2.850000e+00 6.500000e-01 6.500000e-01 3.724300e-02 2.309899e-03 2.422482e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d33-x01-y02
+Path=/REF/CMS_2018_I1690148/d33-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-01 4.500000e-01 4.500000e-01 2.605100e-01 2.604978e-02 2.575535e-02
+1.050000e+00 1.500000e-01 1.500000e-01 9.831300e-01 2.717803e-02 2.613982e-02
+1.350000e+00 1.500000e-01 1.500000e-01 8.399100e-01 4.833679e-02 4.716867e-02
+1.650000e+00 1.500000e-01 1.500000e-01 3.812800e-01 1.859317e-02 2.557757e-02
+2.000000e+00 2.000000e-01 2.000000e-01 1.507400e-01 9.185184e-03 1.032175e-02
+2.850000e+00 6.500000e-01 6.500000e-01 3.380700e-02 2.344506e-03 3.564079e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d33-x01-y03
+Path=/REF/CMS_2018_I1690148/d33-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-01 4.500000e-01 4.500000e-01 2.993200e-01 1.909650e-02 1.828652e-02
+1.050000e+00 1.500000e-01 1.500000e-01 9.618400e-01 4.062735e-02 2.431150e-02
+1.350000e+00 1.500000e-01 1.500000e-01 7.485200e-01 3.083828e-02 4.056991e-02
+1.650000e+00 1.500000e-01 1.500000e-01 3.533800e-01 1.721163e-02 1.880551e-02
+2.000000e+00 2.000000e-01 2.000000e-01 1.578300e-01 6.614466e-03 1.386554e-02
+2.850000e+00 6.500000e-01 6.500000e-01 3.719800e-02 3.613995e-03 3.128230e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d33-x01-y04
+Path=/REF/CMS_2018_I1690148/d33-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-01 4.500000e-01 4.500000e-01 2.087900e-01 3.076772e-02 2.479948e-02
+1.050000e+00 1.500000e-01 1.500000e-01 8.074100e-01 4.181469e-02 6.549745e-02
+1.350000e+00 1.500000e-01 1.500000e-01 9.436100e-01 6.366802e-02 5.197642e-02
+1.650000e+00 1.500000e-01 1.500000e-01 4.392800e-01 2.467188e-02 3.928200e-02
+2.000000e+00 2.000000e-01 2.000000e-01 2.077400e-01 2.561754e-02 1.760905e-02
+2.850000e+00 6.500000e-01 6.500000e-01 5.531000e-02 1.056342e-02 9.305764e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d34-x01-y01
+Path=/REF/CMS_2018_I1690148/d34-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+00 5.000000e+00 5.000000e+00 4.293400e-02 4.031556e-03 2.997977e-03
+1.150000e+01 1.500000e+00 1.500000e+00 8.191400e-02 9.813596e-03 1.604128e-02
+1.500000e+01 2.000000e+00 2.000000e+00 5.357900e-02 8.453835e-03 5.564721e-03
+1.900000e+01 2.000000e+00 2.000000e+00 1.857900e-02 4.833584e-03 6.131436e-03
+2.250000e+01 1.500000e+00 1.500000e+00 7.874900e-03 5.785483e-03 4.594963e-03
+2.700000e+01 3.000000e+00 3.000000e+00 2.109900e-03 1.636001e-03 1.761429e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d34-x01-y02
+Path=/REF/CMS_2018_I1690148/d34-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+00 5.000000e+00 5.000000e+00 3.091600e-02 3.525579e-03 3.378292e-03
+1.150000e+01 1.500000e+00 1.500000e+00 8.605200e-02 8.217073e-03 6.223847e-03
+1.500000e+01 2.000000e+00 2.000000e+00 6.994800e-02 5.006680e-03 9.459490e-03
+1.900000e+01 2.000000e+00 2.000000e+00 2.750500e-02 1.116810e-02 5.835368e-03
+2.250000e+01 1.500000e+00 1.500000e+00 9.250600e-03 6.575262e-03 1.257669e-02
+2.700000e+01 3.000000e+00 3.000000e+00 2.518900e-03 4.040248e-03 2.388440e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d34-x01-y03
+Path=/REF/CMS_2018_I1690148/d34-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+00 5.000000e+00 5.000000e+00 5.732600e-02 5.317093e-03 3.420687e-03
+1.150000e+01 1.500000e+00 1.500000e+00 7.678700e-02 1.249519e-02 2.230705e-02
+1.500000e+01 2.000000e+00 2.000000e+00 3.687200e-02 8.823354e-03 4.017223e-03
+1.900000e+01 2.000000e+00 2.000000e+00 8.814400e-03 1.953251e-03 4.916026e-03
+2.250000e+01 1.500000e+00 1.500000e+00 3.161700e-03 3.530249e-03 1.495838e-03
+2.700000e+01 3.000000e+00 3.000000e+00 6.908100e-04 6.928010e-04 1.024440e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d34-x01-y04
+Path=/REF/CMS_2018_I1690148/d34-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e+00 5.000000e+00 5.000000e+00 3.181500e-02 3.464754e-03 4.273081e-03
+1.150000e+01 1.500000e+00 1.500000e+00 7.231500e-02 2.069296e-02 2.076189e-02
+1.500000e+01 2.000000e+00 2.000000e+00 6.389800e-02 1.747337e-02 1.718817e-02
+1.900000e+01 2.000000e+00 2.000000e+00 2.181600e-02 2.120981e-02 1.937504e-02
+2.250000e+01 1.500000e+00 1.500000e+00 3.021800e-02 2.623301e-02 2.664924e-02
+2.700000e+01 3.000000e+00 3.000000e+00 5.232300e-03 8.928036e-03 8.739666e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d35-x01-y01
+Path=/REF/CMS_2018_I1690148/d35-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 1.764400e+00 1.040156e-01 8.755400e-02
+2.900000e-01 3.000000e-02 3.000000e-02 3.687500e+00 3.303111e-01 3.941501e-01
+3.700000e-01 5.000000e-02 5.000000e-02 1.865200e+00 8.064449e-02 8.765281e-02
+4.900000e-01 7.000000e-02 7.000000e-02 6.855400e-01 4.797779e-02 5.148289e-02
+7.800000e-01 2.200000e-01 2.200000e-01 8.526700e-02 8.883941e-03 7.296774e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d35-x01-y02
+Path=/REF/CMS_2018_I1690148/d35-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 2.020100e+00 1.202223e-01 1.004992e-01
+2.900000e-01 3.000000e-02 3.000000e-02 3.697900e+00 3.926983e-01 4.862441e-01
+3.700000e-01 5.000000e-02 5.000000e-02 1.604300e+00 1.306424e-01 1.051713e-01
+4.900000e-01 7.000000e-02 7.000000e-02 5.155800e-01 5.324681e-02 5.110976e-02
+7.800000e-01 2.200000e-01 2.200000e-01 4.612000e-02 7.114887e-03 9.620271e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d35-x01-y03
+Path=/REF/CMS_2018_I1690148/d35-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 1.510500e+00 9.171952e-02 9.326595e-02
+2.900000e-01 3.000000e-02 3.000000e-02 3.593600e+00 3.175034e-01 2.927743e-01
+3.700000e-01 5.000000e-02 5.000000e-02 2.153800e+00 7.785621e-02 1.032485e-01
+4.900000e-01 7.000000e-02 7.000000e-02 8.717800e-01 6.299726e-02 6.413732e-02
+7.800000e-01 2.200000e-01 2.200000e-01 1.232200e-01 1.159328e-02 7.984715e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d35-x01-y04
+Path=/REF/CMS_2018_I1690148/d35-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 1.817300e+00 1.318415e-01 1.337688e-01
+2.900000e-01 3.000000e-02 3.000000e-02 4.011600e+00 7.664021e-01 6.514645e-01
+3.700000e-01 5.000000e-02 5.000000e-02 1.709700e+00 2.813517e-01 3.646541e-01
+4.900000e-01 7.000000e-02 7.000000e-02 5.543400e-01 1.374193e-01 1.497714e-01
+7.800000e-01 2.200000e-01 2.200000e-01 8.686000e-02 1.499610e-02 1.664660e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d36-x01-y01
+Path=/REF/CMS_2018_I1690148/d36-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 7.999800e-01 3.680220e-02 2.038176e-02
+2.900000e-01 3.000000e-02 3.000000e-02 3.118500e+00 7.609483e-02 2.485476e-01
+3.600000e-01 4.000000e-02 4.000000e-02 3.286000e+00 1.573725e-01 7.280270e-02
+4.300000e-01 3.000000e-02 3.000000e-02 2.372400e+00 1.085529e-01 1.682397e-01
+5.000000e-01 4.000000e-02 4.000000e-02 1.517200e+00 7.817794e-02 4.630654e-02
+5.900000e-01 5.000000e-02 5.000000e-02 6.416900e-01 4.183022e-02 3.819341e-02
+8.200000e-01 1.800000e-01 1.800000e-01 3.922100e-02 3.958760e-03 4.022178e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d36-x01-y02
+Path=/REF/CMS_2018_I1690148/d36-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 5.279000e-01 3.734203e-02 2.500561e-02
+2.900000e-01 3.000000e-02 3.000000e-02 3.089200e+00 1.212928e-01 1.906864e-01
+3.600000e-01 4.000000e-02 4.000000e-02 3.717400e+00 1.296434e-01 1.203347e-01
+4.300000e-01 3.000000e-02 3.000000e-02 2.764300e+00 1.424339e-01 2.061595e-01
+5.000000e-01 4.000000e-02 4.000000e-02 1.691500e+00 1.217330e-01 6.164901e-02
+5.900000e-01 5.000000e-02 5.000000e-02 6.644500e-01 4.184382e-02 5.334849e-02
+8.200000e-01 1.800000e-01 1.800000e-01 3.435900e-02 7.388923e-03 6.416795e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d36-x01-y03
+Path=/REF/CMS_2018_I1690148/d36-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 1.037400e+00 5.177381e-02 2.839486e-02
+2.900000e-01 3.000000e-02 3.000000e-02 3.240200e+00 1.410792e-01 3.838180e-01
+3.600000e-01 4.000000e-02 4.000000e-02 2.974700e+00 2.398269e-01 7.178725e-02
+4.300000e-01 3.000000e-02 3.000000e-02 2.021400e+00 9.547977e-02 2.183222e-01
+5.000000e-01 4.000000e-02 4.000000e-02 1.298400e+00 1.045380e-01 6.004348e-02
+5.900000e-01 5.000000e-02 5.000000e-02 5.755100e-01 5.791329e-02 5.689242e-02
+8.200000e-01 1.800000e-01 1.800000e-01 4.216200e-02 5.586638e-03 6.733882e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d36-x01-y04
+Path=/REF/CMS_2018_I1690148/d36-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 9.030000e-01 2.565328e-02 5.345570e-02
+2.900000e-01 3.000000e-02 3.000000e-02 2.556900e+00 2.189661e-01 2.700289e-01
+3.600000e-01 4.000000e-02 4.000000e-02 2.808000e+00 2.528019e-01 2.438454e-01
+4.300000e-01 3.000000e-02 3.000000e-02 2.360800e+00 3.272044e-01 2.454664e-01
+5.000000e-01 4.000000e-02 4.000000e-02 1.774000e+00 1.746200e-01 2.133026e-01
+5.900000e-01 5.000000e-02 5.000000e-02 8.722400e-01 1.138723e-01 8.656088e-02
+8.200000e-01 1.800000e-01 1.800000e-01 4.548200e-02 1.991144e-02 1.562883e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d37-x01-y01
+Path=/REF/CMS_2018_I1690148/d37-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.000000e-02 6.000000e-02 6.000000e-02 1.693300e+00 7.051217e-02 4.565908e-02
+1.400000e-01 2.000000e-02 2.000000e-02 4.292800e+00 2.528900e-01 6.388756e-01
+1.850000e-01 2.500000e-02 2.500000e-02 3.854000e+00 4.109098e-01 1.406530e-01
+2.400000e-01 3.000000e-02 3.000000e-02 2.866000e+00 8.986156e-02 2.301834e-01
+3.050000e-01 3.500000e-02 3.500000e-02 1.739000e+00 1.606941e-01 7.183118e-02
+3.900000e-01 5.000000e-02 5.000000e-02 9.220400e-01 4.293859e-02 6.825372e-02
+4.850000e-01 4.500000e-02 4.500000e-02 3.435000e-01 5.928139e-02 5.847059e-02
+7.650000e-01 2.350000e-01 2.350000e-01 3.314700e-02 1.591258e-02 4.312940e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d37-x01-y02
+Path=/REF/CMS_2018_I1690148/d37-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.000000e-02 6.000000e-02 6.000000e-02 1.240200e+00 6.323468e-02 4.655452e-02
+1.400000e-01 2.000000e-02 2.000000e-02 4.341500e+00 2.411109e-01 4.126811e-01
+1.850000e-01 2.500000e-02 2.500000e-02 4.157700e+00 2.632446e-01 2.173787e-01
+2.400000e-01 3.000000e-02 3.000000e-02 3.263700e+00 2.039704e-01 1.981416e-01
+3.050000e-01 3.500000e-02 3.500000e-02 1.899400e+00 1.564465e-01 1.500968e-01
+3.900000e-01 5.000000e-02 5.000000e-02 9.701800e-01 9.496841e-02 6.876782e-02
+4.850000e-01 4.500000e-02 4.500000e-02 3.371400e-01 5.584969e-02 7.517135e-02
+7.650000e-01 2.350000e-01 2.350000e-01 2.869600e-02 6.548560e-03 5.592554e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d37-x01-y03
+Path=/REF/CMS_2018_I1690148/d37-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.000000e-02 6.000000e-02 6.000000e-02 2.092100e+00 1.289837e-01 8.687320e-02
+1.400000e-01 2.000000e-02 2.000000e-02 4.301100e+00 4.631779e-01 1.112963e+00
+1.850000e-01 2.500000e-02 2.500000e-02 3.821800e+00 8.662639e-01 2.228966e-01
+2.400000e-01 3.000000e-02 3.000000e-02 2.418900e+00 1.306116e-01 4.848071e-01
+3.050000e-01 3.500000e-02 3.500000e-02 1.605700e+00 2.767282e-01 8.036573e-02
+3.900000e-01 5.000000e-02 5.000000e-02 8.228800e-01 4.205870e-02 9.737204e-02
+4.850000e-01 4.500000e-02 4.500000e-02 3.235300e-01 8.171523e-02 4.262633e-02
+7.650000e-01 2.350000e-01 2.350000e-01 3.590400e-02 4.447840e-03 6.858691e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d37-x01-y04
+Path=/REF/CMS_2018_I1690148/d37-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+6.000000e-02 6.000000e-02 6.000000e-02 1.943000e+00 7.017258e-02 1.050065e-01
+1.400000e-01 2.000000e-02 2.000000e-02 3.540200e+00 3.695325e-01 5.957558e-01
+1.850000e-01 2.500000e-02 2.500000e-02 2.892200e+00 3.913462e-01 4.210123e-01
+2.400000e-01 3.000000e-02 3.000000e-02 2.952600e+00 4.595295e-01 2.295837e-01
+3.050000e-01 3.500000e-02 3.500000e-02 1.797000e+00 2.701930e-01 2.034766e-01
+3.900000e-01 5.000000e-02 5.000000e-02 1.166500e+00 1.014373e-01 2.048784e-01
+4.850000e-01 4.500000e-02 4.500000e-02 4.816000e-01 1.507818e-01 8.609028e-02
+7.650000e-01 2.350000e-01 2.350000e-01 3.762000e-02 1.397442e-02 1.265082e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d38-x01-y01
+Path=/REF/CMS_2018_I1690148/d38-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 6.147500e+00 2.377917e-01 3.225194e-01
+7.000000e-02 2.000000e-02 2.000000e-02 6.179600e+00 6.247371e-01 9.066721e-01
+1.150000e-01 2.500000e-02 2.500000e-02 3.698800e+00 5.954325e-01 2.361959e-01
+1.700000e-01 3.000000e-02 3.000000e-02 2.032300e+00 1.402570e-01 1.776138e-01
+2.450000e-01 4.500000e-02 4.500000e-02 8.895400e-01 8.862108e-02 7.006659e-02
+3.950000e-01 1.050000e-01 1.050000e-01 2.785800e-01 2.934645e-02 2.393642e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d38-x01-y02
+Path=/REF/CMS_2018_I1690148/d38-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 5.510600e+00 1.479980e-01 2.629606e-01
+7.000000e-02 2.000000e-02 2.000000e-02 6.628800e+00 5.201886e-01 6.629265e-01
+1.150000e-01 2.500000e-02 2.500000e-02 3.729800e+00 4.759077e-01 2.106776e-01
+1.700000e-01 3.000000e-02 3.000000e-02 2.240300e+00 1.185275e-01 1.878666e-01
+2.450000e-01 4.500000e-02 4.500000e-02 8.259400e-01 1.172571e-01 7.419607e-02
+3.950000e-01 1.050000e-01 1.050000e-01 3.051100e-01 3.777769e-02 3.359136e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d38-x01-y03
+Path=/REF/CMS_2018_I1690148/d38-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 6.881000e+00 4.874143e-01 5.242344e-01
+7.000000e-02 2.000000e-02 2.000000e-02 5.805300e+00 9.583116e-01 1.356626e+00
+1.150000e-01 2.500000e-02 2.500000e-02 3.737100e+00 8.081179e-01 4.179392e-01
+1.700000e-01 3.000000e-02 3.000000e-02 1.745600e+00 2.358848e-01 2.606004e-01
+2.450000e-01 4.500000e-02 4.500000e-02 9.539000e-01 1.189572e-01 1.004808e-01
+3.950000e-01 1.050000e-01 1.050000e-01 2.204700e-01 3.892751e-02 4.387716e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d38-x01-y04
+Path=/REF/CMS_2018_I1690148/d38-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e-02 2.500000e-02 2.500000e-02 5.953200e+00 1.939387e-01 3.594985e-01
+7.000000e-02 2.000000e-02 2.000000e-02 5.234600e+00 5.787831e-01 7.641711e-01
+1.150000e-01 2.500000e-02 2.500000e-02 3.462800e+00 7.241719e-01 3.590700e-01
+1.700000e-01 3.000000e-02 3.000000e-02 2.442600e+00 4.042081e-01 4.092166e-01
+2.450000e-01 4.500000e-02 4.500000e-02 9.323600e-01 2.044136e-01 2.495148e-01
+3.950000e-01 1.050000e-01 1.050000e-01 4.254300e-01 9.615493e-02 8.186349e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d39-x01-y01
+Path=/REF/CMS_2018_I1690148/d39-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.300000e-01 3.300000e-01 3.300000e-01 5.990500e-01 1.331741e-02 2.505963e-02
+7.100000e-01 5.000000e-02 5.000000e-02 1.705900e+00 3.941601e-01 5.320744e-01
+8.800000e-01 1.200000e-01 1.200000e-01 1.808500e+00 2.658531e-01 1.587636e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d39-x01-y02
+Path=/REF/CMS_2018_I1690148/d39-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.300000e-01 3.300000e-01 3.300000e-01 6.474100e-01 2.812118e-02 2.323621e-02
+7.100000e-01 5.000000e-02 5.000000e-02 1.774900e+00 3.775345e-01 5.151322e-01
+8.800000e-01 1.200000e-01 1.200000e-01 1.646700e+00 2.177457e-01 1.622099e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d39-x01-y03
+Path=/REF/CMS_2018_I1690148/d39-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.300000e-01 3.300000e-01 3.300000e-01 5.556500e-01 1.555042e-02 3.642199e-02
+7.100000e-01 5.000000e-02 5.000000e-02 1.644600e+00 4.856325e-01 6.294818e-01
+8.800000e-01 1.200000e-01 1.200000e-01 1.953400e+00 3.097006e-01 1.750879e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d39-x01-y04
+Path=/REF/CMS_2018_I1690148/d39-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.300000e-01 3.300000e-01 3.300000e-01 5.724300e-01 2.951154e-02 8.496436e-02
+7.100000e-01 5.000000e-02 5.000000e-02 1.874700e+00 8.411561e-01 4.670530e-01
+8.800000e-01 1.200000e-01 1.200000e-01 1.811400e+00 2.883438e-01 2.005085e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d40-x01-y01
+Path=/REF/CMS_2018_I1690148/d40-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.450000e-01 4.500000e-02 4.500000e-02 4.483700e+00 1.548905e-01 2.890904e-01
+3.450000e-01 1.550000e-01 1.550000e-01 1.924100e+00 8.551594e-02 4.786284e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d40-x01-y02
+Path=/REF/CMS_2018_I1690148/d40-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.450000e-01 4.500000e-02 4.500000e-02 4.298400e+00 1.680870e-01 4.185938e-01
+3.450000e-01 1.550000e-01 1.550000e-01 1.977900e+00 1.240952e-01 5.487498e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d40-x01-y03
+Path=/REF/CMS_2018_I1690148/d40-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.450000e-01 4.500000e-02 4.500000e-02 4.761800e+00 2.751476e-01 3.683518e-01
+3.450000e-01 1.550000e-01 1.550000e-01 1.843300e+00 1.095204e-01 8.330404e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d40-x01-y04
+Path=/REF/CMS_2018_I1690148/d40-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.450000e-01 4.500000e-02 4.500000e-02 4.139400e+00 3.726130e-01 4.427281e-01
+3.450000e-01 1.550000e-01 1.550000e-01 2.024000e+00 1.360179e-01 1.169731e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d41-x01-y01
+Path=/REF/CMS_2018_I1690148/d41-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.000000e-02 4.000000e-02 4.000000e-02 2.445700e+00 9.002189e-02 1.283143e-01
+1.000000e-01 2.000000e-02 2.000000e-02 4.604200e+00 1.432906e-01 1.577894e-01
+1.350000e-01 1.500000e-02 1.500000e-02 3.979200e+00 1.643543e-01 1.292602e-01
+1.700000e-01 2.000000e-02 2.000000e-02 3.149300e+00 1.040260e-01 1.618703e-01
+2.050000e-01 1.500000e-02 1.500000e-02 2.529300e+00 1.750205e-01 1.627624e-01
+2.450000e-01 2.500000e-02 2.500000e-02 2.042700e+00 1.519442e-01 1.084277e-01
+3.050000e-01 3.500000e-02 3.500000e-02 1.662600e+00 6.343673e-02 1.532655e-01
+4.200000e-01 8.000000e-02 8.000000e-02 5.026800e-01 7.161756e-02 2.443699e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d41-x01-y02
+Path=/REF/CMS_2018_I1690148/d41-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.000000e-02 4.000000e-02 4.000000e-02 1.973200e+00 7.330609e-02 1.012632e-01
+1.000000e-01 2.000000e-02 2.000000e-02 4.808400e+00 1.527638e-01 1.831076e-01
+1.350000e-01 1.500000e-02 1.500000e-02 4.567100e+00 1.847160e-01 1.262103e-01
+1.700000e-01 2.000000e-02 2.000000e-02 3.556900e+00 1.470150e-01 2.630357e-01
+2.050000e-01 1.500000e-02 1.500000e-02 2.857200e+00 2.966138e-01 3.814354e-01
+2.450000e-01 2.500000e-02 2.500000e-02 2.155400e+00 2.889936e-01 1.685989e-01
+3.050000e-01 3.500000e-02 3.500000e-02 1.523000e+00 1.170939e-01 1.530745e-01
+4.200000e-01 8.000000e-02 8.000000e-02 4.401300e-01 6.245515e-02 3.635691e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d41-x01-y03
+Path=/REF/CMS_2018_I1690148/d41-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.000000e-02 4.000000e-02 4.000000e-02 2.800300e+00 1.706274e-01 2.112755e-01
+1.000000e-01 2.000000e-02 2.000000e-02 4.709800e+00 2.612715e-01 1.789551e-01
+1.350000e-01 1.500000e-02 1.500000e-02 3.476400e+00 3.202652e-01 2.686429e-01
+1.700000e-01 2.000000e-02 2.000000e-02 2.897600e+00 1.639602e-01 1.897608e-01
+2.050000e-01 1.500000e-02 1.500000e-02 2.197400e+00 2.900933e-01 1.777358e-01
+2.450000e-01 2.500000e-02 2.500000e-02 1.935000e+00 1.982966e-01 1.298531e-01
+3.050000e-01 3.500000e-02 3.500000e-02 1.680600e+00 1.368730e-01 1.782366e-01
+4.200000e-01 8.000000e-02 8.000000e-02 5.442100e-01 6.348329e-02 6.772503e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d41-x01-y04
+Path=/REF/CMS_2018_I1690148/d41-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.000000e-02 4.000000e-02 4.000000e-02 3.032100e+00 1.395242e-01 1.800165e-01
+1.000000e-01 2.000000e-02 2.000000e-02 3.178000e+00 3.282869e-01 2.805660e-01
+1.350000e-01 1.500000e-02 1.500000e-02 3.535600e+00 4.864895e-01 4.159916e-01
+1.700000e-01 2.000000e-02 2.000000e-02 2.205900e+00 3.906720e-01 5.098147e-01
+2.050000e-01 1.500000e-02 1.500000e-02 2.784800e+00 4.706246e-01 5.566927e-01
+2.450000e-01 2.500000e-02 2.500000e-02 2.058000e+00 2.682651e-01 3.380814e-01
+3.050000e-01 3.500000e-02 3.500000e-02 2.222900e+00 2.422234e-01 2.396916e-01
+4.200000e-01 8.000000e-02 8.000000e-02 5.872800e-01 1.019216e-01 4.101165e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d42-x01-y01
+Path=/REF/CMS_2018_I1690148/d42-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+00 2.500000e+00 2.500000e+00 7.224000e-02 9.843741e-03 7.087022e-03
+5.500000e+00 5.000000e-01 5.000000e-01 1.730600e-01 8.006090e-02 1.258579e-01
+6.500000e+00 5.000000e-01 5.000000e-01 2.766500e-01 2.114360e-01 1.552144e-01
+7.500000e+00 5.000000e-01 5.000000e-01 1.039700e-01 2.712048e-01 1.830764e-01
+1.150000e+01 3.500000e+00 3.500000e+00 1.215900e-02 9.969518e-03 2.568480e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d42-x01-y02
+Path=/REF/CMS_2018_I1690148/d42-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+00 2.500000e+00 2.500000e+00 5.906100e-02 7.452722e-03 9.214896e-03
+5.500000e+00 5.000000e-01 5.000000e-01 1.769500e-01 1.126550e-01 1.073844e-01
+6.500000e+00 5.000000e-01 5.000000e-01 2.713100e-01 2.405423e-01 1.864478e-01
+7.500000e+00 5.000000e-01 5.000000e-01 1.699200e-01 1.415418e-01 2.591895e-01
+1.150000e+01 3.500000e+00 3.500000e+00 1.235900e-02 1.767556e-02 5.661811e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d42-x01-y03
+Path=/REF/CMS_2018_I1690148/d42-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+00 2.500000e+00 2.500000e+00 8.898100e-02 1.174196e-02 7.769250e-03
+5.500000e+00 5.000000e-01 5.000000e-01 1.322100e-01 7.905835e-02 1.275312e-01
+6.500000e+00 5.000000e-01 5.000000e-01 3.509200e-01 1.515189e-01 9.578856e-02
+7.500000e+00 5.000000e-01 5.000000e-01 -2.257700e-02 7.285176e-02 1.011970e-01
+1.150000e+01 3.500000e+00 3.500000e+00 1.350600e-02 5.259028e-03 5.271884e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d42-x01-y04
+Path=/REF/CMS_2018_I1690148/d42-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.500000e+00 2.500000e+00 2.500000e+00 5.931600e-02 4.642392e-03 1.282866e-02
+5.500000e+00 5.000000e-01 5.000000e-01 2.703700e-01 2.857612e-01 1.206557e-01
+6.500000e+00 5.000000e-01 5.000000e-01 1.113400e-01 2.308020e-01 4.837353e-01
+7.500000e+00 5.000000e-01 5.000000e-01 2.133400e-01 3.125362e-01 1.880499e-01
+1.150000e+01 3.500000e+00 3.500000e+00 1.548300e-02 1.259168e-02 1.137469e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d43-x01-y01
+Path=/REF/CMS_2018_I1690148/d43-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.200000e-01 3.200000e-01 3.200000e-01 9.265800e-01 5.942267e-02 3.376114e-02
+6.900000e-01 5.000000e-02 5.000000e-02 2.976900e+00 3.092155e-01 3.841692e-01
+8.700000e-01 1.300000e-01 1.300000e-01 4.203800e-01 4.001081e-02 5.872995e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d43-x01-y02
+Path=/REF/CMS_2018_I1690148/d43-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.200000e-01 3.200000e-01 3.200000e-01 8.634500e-01 4.973764e-02 3.313122e-02
+6.900000e-01 5.000000e-02 5.000000e-02 3.387400e+00 3.114469e-01 2.854297e-01
+8.700000e-01 1.300000e-01 1.300000e-01 4.178900e-01 4.796469e-02 7.468433e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d43-x01-y03
+Path=/REF/CMS_2018_I1690148/d43-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.200000e-01 3.200000e-01 3.200000e-01 9.998500e-01 7.639741e-02 3.709116e-02
+6.900000e-01 5.000000e-02 5.000000e-02 2.486300e+00 3.520602e-01 5.565161e-01
+8.700000e-01 1.300000e-01 1.300000e-01 4.287100e-01 4.525230e-02 6.497633e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d43-x01-y04
+Path=/REF/CMS_2018_I1690148/d43-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.200000e-01 3.200000e-01 3.200000e-01 8.786600e-01 6.573162e-02 4.016103e-02
+6.900000e-01 5.000000e-02 5.000000e-02 3.157200e+00 3.439699e-01 4.141152e-01
+8.700000e-01 1.300000e-01 1.300000e-01 4.689700e-01 7.459319e-02 8.569682e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d44-x01-y01
+Path=/REF/CMS_2018_I1690148/d44-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.400000e-01 3.400000e-01 3.400000e-01 7.902100e-01 7.375328e-02 6.106530e-02
+7.300000e-01 5.000000e-02 5.000000e-02 3.555200e+00 4.150926e-01 4.159903e-01
+8.900000e-01 1.100000e-01 1.100000e-01 4.869500e-01 5.923836e-02 8.382494e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d44-x01-y02
+Path=/REF/CMS_2018_I1690148/d44-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.400000e-01 3.400000e-01 3.400000e-01 7.161400e-01 6.371609e-02 6.134453e-02
+7.300000e-01 5.000000e-02 5.000000e-02 3.856800e+00 7.368387e-01 3.809320e-01
+8.900000e-01 1.100000e-01 1.100000e-01 5.788500e-01 9.117552e-02 2.780754e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d44-x01-y03
+Path=/REF/CMS_2018_I1690148/d44-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.400000e-01 3.400000e-01 3.400000e-01 9.056400e-01 1.023679e-01 6.864294e-02
+7.300000e-01 5.000000e-02 5.000000e-02 2.964300e+00 5.043865e-01 7.724842e-01
+8.900000e-01 1.100000e-01 1.100000e-01 3.987800e-01 6.308983e-02 5.895918e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d44-x01-y04
+Path=/REF/CMS_2018_I1690148/d44-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.400000e-01 3.400000e-01 3.400000e-01 6.397500e-01 8.809720e-02 7.915250e-02
+7.300000e-01 5.000000e-02 5.000000e-02 4.297600e+00 6.552919e-01 5.462054e-01
+8.900000e-01 1.100000e-01 1.100000e-01 6.145700e-01 9.685194e-02 2.200970e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d45-x01-y01
+Path=/REF/CMS_2018_I1690148/d45-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.100000e-01 3.100000e-01 3.100000e-01 1.026800e+00 9.649820e-02 7.557754e-02
+8.100000e-01 9.000000e-02 9.000000e-02 2.018700e+00 2.612598e-01 3.331241e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d45-x01-y02
+Path=/REF/CMS_2018_I1690148/d45-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.100000e-01 3.100000e-01 3.100000e-01 9.192300e-01 9.674435e-02 7.686715e-02
+8.100000e-01 9.000000e-02 9.000000e-02 2.389300e+00 2.673881e-01 3.353204e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d45-x01-y03
+Path=/REF/CMS_2018_I1690148/d45-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.100000e-01 3.100000e-01 3.100000e-01 1.201500e+00 1.358042e-01 1.000650e-01
+8.100000e-01 9.000000e-02 9.000000e-02 1.416900e+00 3.462086e-01 4.689247e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d45-x01-y04
+Path=/REF/CMS_2018_I1690148/d45-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.100000e-01 3.100000e-01 3.100000e-01 8.356300e-01 1.123321e-01 9.081867e-02
+8.100000e-01 9.000000e-02 9.000000e-02 2.677300e+00 3.264278e-01 3.980045e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d46-x01-y01
+Path=/REF/CMS_2018_I1690148/d46-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.950000e-01 9.500000e-02 9.500000e-02 1.465300e+00 1.047899e-01 9.414749e-02
+4.100000e-01 2.000000e-02 2.000000e-02 9.143900e+00 3.734161e-01 3.540641e-01
+4.450000e-01 1.500000e-02 1.500000e-02 1.094100e+01 6.036212e-01 6.147676e-01
+4.800000e-01 2.000000e-02 2.000000e-02 6.901900e-01 2.095679e-01 1.957559e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d46-x01-y02
+Path=/REF/CMS_2018_I1690148/d46-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.950000e-01 9.500000e-02 9.500000e-02 1.027400e+00 1.042585e-01 9.971282e-02
+4.100000e-01 2.000000e-02 2.000000e-02 8.943300e+00 6.001376e-01 6.430520e-01
+4.450000e-01 1.500000e-02 1.500000e-02 1.380500e+01 8.599012e-01 8.925125e-01
+4.800000e-01 2.000000e-02 2.000000e-02 8.227200e-01 3.345608e-01 2.773970e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d46-x01-y03
+Path=/REF/CMS_2018_I1690148/d46-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.950000e-01 9.500000e-02 9.500000e-02 1.959900e+00 1.220791e-01 1.071258e-01
+4.100000e-01 2.000000e-02 2.000000e-02 9.447000e+00 2.223820e-01 3.455755e-01
+4.450000e-01 1.500000e-02 1.500000e-02 7.859200e+00 5.188755e-01 5.081949e-01
+4.800000e-01 2.000000e-02 2.000000e-02 3.492600e-01 9.461441e-02 9.354334e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d46-x01-y04
+Path=/REF/CMS_2018_I1690148/d46-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.950000e-01 9.500000e-02 9.500000e-02 1.165300e+00 9.454158e-02 1.207850e-01
+4.100000e-01 2.000000e-02 2.000000e-02 8.387500e+00 1.014569e+00 5.341810e-01
+4.450000e-01 1.500000e-02 1.500000e-02 1.267400e+01 7.033280e-01 8.089541e-01
+4.800000e-01 2.000000e-02 2.000000e-02 1.571900e+00 4.193381e-01 5.019893e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d47-x01-y01
+Path=/REF/CMS_2018_I1690148/d47-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e-01 1.050000e-01 1.050000e-01 5.908500e-01 4.517967e-02 5.080462e-02
+2.250000e-01 1.500000e-02 1.500000e-02 5.394900e+00 2.142611e-01 2.601987e-01
+2.550000e-01 1.500000e-02 1.500000e-02 8.965300e+00 1.573592e-01 2.738069e-01
+2.800000e-01 1.000000e-02 1.000000e-02 9.539800e+00 4.472986e-01 2.444844e-01
+3.050000e-01 1.500000e-02 1.500000e-02 6.219100e+00 1.516094e-01 2.499103e-01
+3.300000e-01 1.000000e-02 1.000000e-02 2.857100e+00 2.326990e-01 1.313958e-01
+4.200000e-01 8.000000e-02 8.000000e-02 6.626900e-02 9.451694e-03 1.099451e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d47-x01-y02
+Path=/REF/CMS_2018_I1690148/d47-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e-01 1.050000e-01 1.050000e-01 2.883600e-01 3.967280e-02 3.000882e-02
+2.250000e-01 1.500000e-02 1.500000e-02 4.483600e+00 2.942929e-01 3.509093e-01
+2.550000e-01 1.500000e-02 1.500000e-02 9.839000e+00 3.744839e-01 3.251720e-01
+2.800000e-01 1.000000e-02 1.000000e-02 1.158500e+01 4.775778e-01 7.115500e-01
+3.050000e-01 1.500000e-02 1.500000e-02 6.939700e+00 4.019220e-01 2.490110e-01
+3.300000e-01 1.000000e-02 1.000000e-02 2.974600e+00 2.416858e-01 3.010642e-01
+4.200000e-01 8.000000e-02 8.000000e-02 6.487600e-02 2.154886e-02 1.603755e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d47-x01-y03
+Path=/REF/CMS_2018_I1690148/d47-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e-01 1.050000e-01 1.050000e-01 8.702200e-01 5.883190e-02 7.689490e-02
+2.250000e-01 1.500000e-02 1.500000e-02 6.322700e+00 4.163799e-01 4.441776e-01
+2.550000e-01 1.500000e-02 1.500000e-02 8.471900e+00 2.952742e-01 5.571764e-01
+2.800000e-01 1.000000e-02 1.000000e-02 7.851100e+00 9.978297e-01 3.175253e-01
+3.050000e-01 1.500000e-02 1.500000e-02 5.225600e+00 1.784699e-01 4.714124e-01
+3.300000e-01 1.000000e-02 1.000000e-02 2.481800e+00 3.817003e-01 1.410608e-01
+4.200000e-01 8.000000e-02 8.000000e-02 6.242600e-02 7.280881e-03 1.451396e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d47-x01-y04
+Path=/REF/CMS_2018_I1690148/d47-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.050000e-01 1.050000e-01 1.050000e-01 6.411200e-01 4.235611e-02 6.837943e-02
+2.250000e-01 1.500000e-02 1.500000e-02 4.793800e+00 5.369650e-01 4.176000e-01
+2.550000e-01 1.500000e-02 1.500000e-02 7.429900e+00 5.225990e-01 1.035025e+00
+2.800000e-01 1.000000e-02 1.000000e-02 8.381300e+00 1.683255e+00 8.445109e-01
+3.050000e-01 1.500000e-02 1.500000e-02 7.762800e+00 3.773690e-01 5.901070e-01
+3.300000e-01 1.000000e-02 1.000000e-02 4.174100e+00 5.615428e-01 4.839159e-01
+4.200000e-01 8.000000e-02 8.000000e-02 9.162200e-02 5.086750e-02 3.752339e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d48-x01-y01
+Path=/REF/CMS_2018_I1690148/d48-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-02 4.500000e-02 4.500000e-02 9.620900e-01 7.215783e-02 7.003142e-02
+1.000000e-01 1.000000e-02 1.000000e-02 6.371100e+00 2.644409e-01 5.393984e-01
+1.225000e-01 1.250000e-02 1.250000e-02 9.311800e+00 3.974951e-01 3.646547e-01
+1.450000e-01 1.000000e-02 1.000000e-02 9.760700e+00 6.026418e-01 5.873241e-01
+1.650000e-01 1.000000e-02 1.000000e-02 7.329200e+00 6.778538e-01 5.084261e-01
+1.875000e-01 1.250000e-02 1.250000e-02 5.220900e+00 2.274635e-01 2.948283e-01
+2.125000e-01 1.250000e-02 1.250000e-02 2.501000e+00 2.399287e-01 2.019523e-01
+2.625000e-01 3.750000e-02 3.750000e-02 2.446600e-01 2.373594e-02 2.078649e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d48-x01-y02
+Path=/REF/CMS_2018_I1690148/d48-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-02 4.500000e-02 4.500000e-02 4.512500e-01 4.663655e-02 5.313171e-02
+1.000000e-01 1.000000e-02 1.000000e-02 5.288900e+00 4.543544e-01 2.745640e-01
+1.225000e-01 1.250000e-02 1.250000e-02 9.905400e+00 3.568157e-01 4.774449e-01
+1.450000e-01 1.000000e-02 1.000000e-02 1.073000e+01 5.801952e-01 6.229299e-01
+1.650000e-01 1.000000e-02 1.000000e-02 8.843200e+00 6.939455e-01 5.355806e-01
+1.875000e-01 1.250000e-02 1.250000e-02 5.362400e+00 2.751974e-01 3.220950e-01
+2.125000e-01 1.250000e-02 1.250000e-02 2.477100e+00 3.126945e-01 2.501624e-01
+2.625000e-01 3.750000e-02 3.750000e-02 2.469500e-01 3.650056e-02 3.497273e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d48-x01-y03
+Path=/REF/CMS_2018_I1690148/d48-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-02 4.500000e-02 4.500000e-02 1.362500e+00 1.424989e-01 1.093089e-01
+1.000000e-01 1.000000e-02 1.000000e-02 7.616000e+00 3.842998e-01 1.219691e+00
+1.225000e-01 1.250000e-02 1.250000e-02 8.989500e+00 8.974837e-01 4.833965e-01
+1.450000e-01 1.000000e-02 1.000000e-02 9.368900e+00 8.280245e-01 8.960888e-01
+1.650000e-01 1.000000e-02 1.000000e-02 5.774600e+00 8.717231e-01 7.076342e-01
+1.875000e-01 1.250000e-02 1.250000e-02 4.873100e+00 3.223820e-01 4.548697e-01
+2.125000e-01 1.250000e-02 1.250000e-02 2.320500e+00 2.768799e-01 2.250603e-01
+2.625000e-01 3.750000e-02 3.750000e-02 2.348300e-01 3.224148e-02 3.084878e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d48-x01-y04
+Path=/REF/CMS_2018_I1690148/d48-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+4.500000e-02 4.500000e-02 4.500000e-02 1.325900e+00 5.647322e-02 1.390794e-01
+1.000000e-01 1.000000e-02 1.000000e-02 6.092600e+00 8.953465e-01 6.451604e-01
+1.225000e-01 1.250000e-02 1.250000e-02 6.892100e+00 5.648277e-01 1.316994e+00
+1.450000e-01 1.000000e-02 1.000000e-02 8.353300e+00 1.814577e+00 8.268551e-01
+1.650000e-01 1.000000e-02 1.000000e-02 7.445700e+00 1.097010e+00 1.243726e+00
+1.875000e-01 1.250000e-02 1.250000e-02 6.435100e+00 8.431303e-01 6.147827e-01
+2.125000e-01 1.250000e-02 1.250000e-02 3.530100e+00 4.582065e-01 5.989622e-01
+2.625000e-01 3.750000e-02 3.750000e-02 2.853600e-01 9.475985e-02 6.183748e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d49-x01-y01
+Path=/REF/CMS_2018_I1690148/d49-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-02 1.500000e-02 1.500000e-02 4.327700e+00 2.424589e-01 1.509945e-01
+3.500000e-02 5.000000e-03 5.000000e-03 1.468000e+01 9.314969e-01 2.136612e+00
+4.750000e-02 7.500000e-03 7.500000e-03 1.584900e+01 7.589274e-01 6.963551e-01
+6.250000e-02 7.500000e-03 7.500000e-03 1.249500e+01 6.846484e-01 4.866054e-01
+8.000000e-02 1.000000e-02 1.000000e-02 8.003900e+00 3.859201e-01 3.546546e-01
+9.750000e-02 7.500000e-03 7.500000e-03 4.983800e+00 4.613607e-01 3.993947e-01
+1.525000e-01 4.750000e-02 4.750000e-02 6.670900e-01 4.925135e-02 4.919836e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d49-x01-y02
+Path=/REF/CMS_2018_I1690148/d49-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-02 1.500000e-02 1.500000e-02 2.948600e+00 1.735445e-01 2.055470e-01
+3.500000e-02 5.000000e-03 5.000000e-03 1.461300e+01 1.367538e+00 8.972798e-01
+4.750000e-02 7.500000e-03 7.500000e-03 1.660600e+01 4.608805e-01 1.233282e+00
+6.250000e-02 7.500000e-03 7.500000e-03 1.404100e+01 9.172068e-01 6.704369e-01
+8.000000e-02 1.000000e-02 1.000000e-02 8.620900e+00 5.779115e-01 4.272304e-01
+9.750000e-02 7.500000e-03 7.500000e-03 4.809100e+00 4.415903e-01 6.385562e-01
+1.525000e-01 4.750000e-02 4.750000e-02 6.437500e-01 6.427199e-02 5.805239e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d49-x01-y03
+Path=/REF/CMS_2018_I1690148/d49-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-02 1.500000e-02 1.500000e-02 5.498200e+00 4.393753e-01 1.638116e-01
+3.500000e-02 5.000000e-03 5.000000e-03 1.491500e+01 8.966939e-01 3.792404e+00
+4.750000e-02 7.500000e-03 7.500000e-03 1.589800e+01 1.900769e+00 8.068410e-01
+6.250000e-02 7.500000e-03 7.500000e-03 1.119400e+01 8.204608e-01 9.535726e-01
+8.000000e-02 1.000000e-02 1.000000e-02 7.332500e+00 5.940720e-01 5.203903e-01
+9.750000e-02 7.500000e-03 7.500000e-03 4.675600e+00 6.266525e-01 5.220841e-01
+1.525000e-01 4.750000e-02 4.750000e-02 6.603600e-01 5.239179e-02 5.605454e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d49-x01-y04
+Path=/REF/CMS_2018_I1690148/d49-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.500000e-02 1.500000e-02 1.500000e-02 5.265100e+00 3.033817e-01 4.268912e-01
+3.500000e-02 5.000000e-03 5.000000e-03 1.350300e+01 1.850010e+00 2.788570e+00
+4.750000e-02 7.500000e-03 7.500000e-03 1.119600e+01 1.544181e+00 2.227081e+00
+6.250000e-02 7.500000e-03 7.500000e-03 1.235000e+01 3.128683e+00 1.312960e+00
+8.000000e-02 1.000000e-02 1.000000e-02 8.569300e+00 6.397952e-01 1.705104e+00
+9.750000e-02 7.500000e-03 7.500000e-03 6.974300e+00 1.739086e+00 6.994385e-01
+1.525000e-01 4.750000e-02 4.750000e-02 8.192500e-01 1.112935e-01 1.222218e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d50-x01-y01
+Path=/REF/CMS_2018_I1690148/d50-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e-03 5.000000e-03 5.000000e-03 4.810300e+01 2.103069e+00 2.477732e+00
+1.300000e-02 3.000000e-03 3.000000e-03 3.448200e+01 7.390852e+00 7.283087e+00
+1.900000e-02 3.000000e-03 3.000000e-03 2.181700e+01 4.554859e+00 3.903735e+00
+2.700000e-02 5.000000e-03 5.000000e-03 1.110100e+01 1.002217e+00 7.605593e-01
+3.800000e-02 6.000000e-03 6.000000e-03 4.377300e+00 6.334613e-01 5.260976e-01
+7.200000e-02 2.800000e-02 2.800000e-02 3.149300e-01 7.930938e-02 1.627130e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d50-x01-y02
+Path=/REF/CMS_2018_I1690148/d50-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e-03 5.000000e-03 5.000000e-03 4.678900e+01 1.353048e+00 1.898294e+00
+1.300000e-02 3.000000e-03 3.000000e-03 3.725500e+01 6.624020e+00 5.302014e+00
+1.900000e-02 3.000000e-03 3.000000e-03 2.289100e+01 4.013406e+00 3.708804e+00
+2.700000e-02 5.000000e-03 5.000000e-03 1.055500e+01 7.622884e-01 1.232655e+00
+3.800000e-02 6.000000e-03 6.000000e-03 4.042000e+00 7.120526e-01 5.021338e-01
+7.200000e-02 2.800000e-02 2.800000e-02 3.067300e-01 4.066063e-02 5.763267e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d50-x01-y03
+Path=/REF/CMS_2018_I1690148/d50-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e-03 5.000000e-03 5.000000e-03 5.012800e+01 2.525980e+00 4.312947e+00
+1.300000e-02 3.000000e-03 3.000000e-03 3.190200e+01 9.542452e+00 9.350681e+00
+1.900000e-02 3.000000e-03 3.000000e-03 2.023600e+01 4.732169e+00 6.375575e+00
+2.700000e-02 5.000000e-03 5.000000e-03 1.108000e+01 2.345396e+00 6.738418e-01
+3.800000e-02 6.000000e-03 6.000000e-03 3.815300e+00 3.644794e-01 2.497425e+00
+7.200000e-02 2.800000e-02 2.800000e-02 5.233300e-01 8.310780e-01 1.116673e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d50-x01-y04
+Path=/REF/CMS_2018_I1690148/d50-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.000000e-03 5.000000e-03 5.000000e-03 4.341300e+01 1.358511e+00 2.297491e+00
+1.300000e-02 3.000000e-03 3.000000e-03 3.162600e+01 6.592337e+00 5.416745e+00
+1.900000e-02 3.000000e-03 3.000000e-03 2.307900e+01 2.773159e+00 5.412571e+00
+2.700000e-02 5.000000e-03 5.000000e-03 1.455200e+01 2.549153e+00 1.293615e+00
+3.800000e-02 6.000000e-03 6.000000e-03 5.669700e+00 7.506073e-01 1.201108e+00
+7.200000e-02 2.800000e-02 2.800000e-02 4.301400e-01 1.772880e-01 7.762776e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d51-x01-y01
+Path=/REF/CMS_2018_I1690148/d51-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.600000e-01 1.600000e-01 1.600000e-01 9.353800e-01 8.363913e-02 6.630952e-02
+5.400000e-01 2.000000e-02 2.000000e-02 6.132500e+00 3.648805e-01 6.242643e-01
+5.750000e-01 1.500000e-02 1.500000e-02 9.492100e+00 6.521476e-01 5.004281e-01
+6.050000e-01 1.500000e-02 1.500000e-02 5.368000e+00 5.746140e-01 5.490581e-01
+6.600000e-01 4.000000e-02 4.000000e-02 1.196800e-01 3.671916e-02 4.356637e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d51-x01-y02
+Path=/REF/CMS_2018_I1690148/d51-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.600000e-01 1.600000e-01 1.600000e-01 6.371700e-01 6.801865e-02 7.280877e-02
+5.400000e-01 2.000000e-02 2.000000e-02 5.619000e+00 4.202176e-01 3.753401e-01
+5.750000e-01 1.500000e-02 1.500000e-02 1.169100e+01 7.166749e-01 7.900396e-01
+6.050000e-01 1.500000e-02 1.500000e-02 7.003700e+00 8.828785e-01 7.552336e-01
+6.600000e-01 4.000000e-02 4.000000e-02 1.314700e-01 5.963142e-02 7.236819e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d51-x01-y03
+Path=/REF/CMS_2018_I1690148/d51-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.600000e-01 1.600000e-01 1.600000e-01 1.280400e+00 1.138399e-01 8.132491e-02
+5.400000e-01 2.000000e-02 2.000000e-02 6.569700e+00 5.683056e-01 9.924126e-01
+5.750000e-01 1.500000e-02 1.500000e-02 7.499200e+00 6.647203e-01 3.554195e-01
+6.050000e-01 1.500000e-02 1.500000e-02 3.280400e+00 3.658266e-01 4.404177e-01
+6.600000e-01 4.000000e-02 4.000000e-02 5.126900e-02 1.368974e-02 1.797789e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d51-x01-y04
+Path=/REF/CMS_2018_I1690148/d51-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+3.600000e-01 1.600000e-01 1.600000e-01 7.007500e-01 6.456417e-02 7.763484e-02
+5.400000e-01 2.000000e-02 2.000000e-02 5.739900e+00 7.216976e-01 6.821918e-01
+5.750000e-01 1.500000e-02 1.500000e-02 9.539400e+00 1.237821e+00 1.003085e+00
+6.050000e-01 1.500000e-02 1.500000e-02 7.672700e+00 7.813959e-01 9.566951e-01
+6.600000e-01 4.000000e-02 4.000000e-02 3.725000e-01 1.794464e-01 1.378361e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d52-x01-y01
+Path=/REF/CMS_2018_I1690148/d52-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.700000e-01 1.700000e-01 1.700000e-01 9.167000e-01 6.844354e-02 5.084949e-02
+3.500000e-01 1.000000e-02 1.000000e-02 7.778700e+00 7.107739e-01 1.672433e+00
+3.800000e-01 2.000000e-02 2.000000e-02 7.882000e+00 5.682421e-01 2.491734e-01
+4.200000e-01 2.000000e-02 2.000000e-02 4.562900e+00 1.806258e-01 2.465938e-01
+5.700000e-01 1.300000e-01 1.300000e-01 1.344300e-01 1.443204e-02 9.177112e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d52-x01-y02
+Path=/REF/CMS_2018_I1690148/d52-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.700000e-01 1.700000e-01 1.700000e-01 6.996000e-01 6.193193e-02 5.778582e-02
+3.500000e-01 1.000000e-02 1.000000e-02 8.269600e+00 1.073265e+00 1.010691e+00
+3.800000e-01 2.000000e-02 2.000000e-02 9.230700e+00 3.978958e-01 4.756905e-01
+4.200000e-01 2.000000e-02 2.000000e-02 4.737200e+00 3.540425e-01 2.889778e-01
+5.700000e-01 1.300000e-01 1.300000e-01 1.462600e-01 1.595931e-02 1.306393e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d52-x01-y03
+Path=/REF/CMS_2018_I1690148/d52-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.700000e-01 1.700000e-01 1.700000e-01 1.152100e+00 9.987409e-02 6.432893e-02
+3.500000e-01 1.000000e-02 1.000000e-02 7.263400e+00 1.037357e+00 2.971717e+00
+3.800000e-01 2.000000e-02 2.000000e-02 6.826500e+00 1.013747e+00 2.515668e-01
+4.200000e-01 2.000000e-02 2.000000e-02 4.022900e+00 1.374778e-01 3.493774e-01
+5.700000e-01 1.300000e-01 1.300000e-01 1.117400e-01 1.841653e-02 8.197245e-03
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d52-x01-y04
+Path=/REF/CMS_2018_I1690148/d52-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.700000e-01 1.700000e-01 1.700000e-01 7.900700e-01 3.845780e-02 5.879011e-02
+3.500000e-01 1.000000e-02 1.000000e-02 6.911400e+00 1.343543e+00 1.451616e+00
+3.800000e-01 2.000000e-02 2.000000e-02 7.195100e+00 8.615900e-01 5.649114e-01
+4.200000e-01 2.000000e-02 2.000000e-02 6.334500e+00 3.490378e-01 4.915189e-01
+5.700000e-01 1.300000e-01 1.300000e-01 1.998500e-01 4.311589e-02 3.171104e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d53-x01-y01
+Path=/REF/CMS_2018_I1690148/d53-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e-01 1.100000e-01 1.100000e-01 2.565300e+00 1.489068e-01 1.666056e-01
+2.350000e-01 1.500000e-02 1.500000e-02 6.749000e+00 1.709985e+00 1.880904e+00
+2.650000e-01 1.500000e-02 1.500000e-02 5.497600e+00 1.130398e+00 7.825129e-01
+3.400000e-01 6.000000e-02 6.000000e-02 5.685800e-01 7.002119e-02 6.626666e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d53-x01-y02
+Path=/REF/CMS_2018_I1690148/d53-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e-01 1.100000e-01 1.100000e-01 2.526000e+00 1.160343e-01 1.565849e-01
+2.350000e-01 1.500000e-02 1.500000e-02 7.232300e+00 1.698213e+00 1.575438e+00
+2.650000e-01 1.500000e-02 1.500000e-02 5.334000e+00 1.012404e+00 8.382751e-01
+3.400000e-01 6.000000e-02 6.000000e-02 5.607400e-01 6.804568e-02 6.172944e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d53-x01-y03
+Path=/REF/CMS_2018_I1690148/d53-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e-01 1.100000e-01 1.100000e-01 2.665800e+00 1.833913e-01 2.021722e-01
+2.350000e-01 1.500000e-02 1.500000e-02 6.339200e+00 2.051204e+00 2.227569e+00
+2.650000e-01 1.500000e-02 1.500000e-02 5.326500e+00 1.221969e+00 9.695015e-01
+3.400000e-01 6.000000e-02 6.000000e-02 5.295500e-01 9.326552e-02 6.680731e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d53-x01-y04
+Path=/REF/CMS_2018_I1690148/d53-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e-01 1.100000e-01 1.100000e-01 2.240900e+00 1.359162e-01 1.527923e-01
+2.350000e-01 1.500000e-02 1.500000e-02 6.538700e+00 1.852896e+00 1.927600e+00
+2.650000e-01 1.500000e-02 1.500000e-02 7.299600e+00 1.159959e+00 1.717817e+00
+3.400000e-01 6.000000e-02 6.000000e-02 7.653600e-01 2.057369e-01 8.444204e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d54-x01-y01
+Path=/REF/CMS_2018_I1690148/d54-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.250000e-02 5.250000e-02 5.250000e-02 5.569200e+00 1.978102e+00 6.927943e-01
+1.200000e-01 1.500000e-02 1.500000e-02 6.488800e+00 4.287774e+00 1.332830e+01
+1.500000e-01 1.500000e-02 1.500000e-02 6.706200e+00 9.570444e+00 4.009669e+00
+2.075000e-01 4.250000e-02 4.250000e-02 2.280500e-01 4.858370e-01 1.048837e+00
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d54-x01-y02
+Path=/REF/CMS_2018_I1690148/d54-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.250000e-02 5.250000e-02 5.250000e-02 5.536000e+00 9.157972e-01 3.925796e-01
+1.200000e-01 1.500000e-02 1.500000e-02 7.593500e+00 1.996385e+00 7.356487e+00
+1.500000e-01 1.500000e-02 1.500000e-02 5.497900e+00 4.904912e+00 8.600260e-01
+2.075000e-01 4.250000e-02 4.250000e-02 3.055700e-01 8.758001e-02 2.620399e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d54-x01-y03
+Path=/REF/CMS_2018_I1690148/d54-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.250000e-02 5.250000e-02 5.250000e-02 5.262200e+00 4.870424e-01 4.138349e-01
+1.200000e-01 1.500000e-02 1.500000e-02 8.533200e+00 1.595663e+00 2.673930e+00
+1.500000e-01 1.500000e-02 1.500000e-02 5.328500e+00 1.442166e+00 5.290137e-01
+2.075000e-01 4.250000e-02 4.250000e-02 3.719900e-01 1.018731e-01 1.136758e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d54-x01-y04
+Path=/REF/CMS_2018_I1690148/d54-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.250000e-02 5.250000e-02 5.250000e-02 4.672000e+00 5.311911e-01 3.722090e-01
+1.200000e-01 1.500000e-02 1.500000e-02 8.323800e+00 1.632024e+00 3.096524e+00
+1.500000e-01 1.500000e-02 1.500000e-02 7.412700e+00 1.538432e+00 1.406657e+00
+2.075000e-01 4.250000e-02 4.250000e-02 4.394100e-01 2.093904e-01 9.952559e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d55-x01-y01
+Path=/REF/CMS_2018_I1690148/d55-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e-02 1.100000e-02 1.100000e-02 1.844100e+01 2.232980e+00 2.259235e+00
+3.000000e-02 8.000000e-03 8.000000e-03 1.954600e+01 2.770360e+00 2.519343e+00
+6.900000e-02 3.100000e-02 3.100000e-02 4.541600e+00 2.035407e-01 3.174712e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d55-x01-y02
+Path=/REF/CMS_2018_I1690148/d55-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e-02 1.100000e-02 1.100000e-02 1.878400e+01 2.320407e+00 2.716519e+00
+3.000000e-02 8.000000e-03 8.000000e-03 1.928000e+01 3.547890e+00 3.242939e+00
+6.900000e-02 3.100000e-02 3.100000e-02 4.488200e+00 2.998190e-01 3.155999e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d55-x01-y03
+Path=/REF/CMS_2018_I1690148/d55-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e-02 1.100000e-02 1.100000e-02 1.885900e+01 2.183043e+00 2.130539e+00
+3.000000e-02 8.000000e-03 8.000000e-03 1.937100e+01 2.403449e+00 2.141809e+00
+6.900000e-02 3.100000e-02 3.100000e-02 4.438200e+00 2.572573e-01 4.357065e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d55-x01-y04
+Path=/REF/CMS_2018_I1690148/d55-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.100000e-02 1.100000e-02 1.100000e-02 1.526000e+01 2.635935e+00 2.369069e+00
+3.000000e-02 8.000000e-03 8.000000e-03 1.952000e+01 3.690847e+00 2.478120e+00
+6.900000e-02 3.100000e-02 3.100000e-02 5.676600e+00 5.897441e-01 7.568218e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d56-x01-y01
+Path=/REF/CMS_2018_I1690148/d56-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.100000e-01 1.100000e-01 1.100000e-01 2.295500e+00 1.692999e-01 1.607990e-01
+6.400000e-01 2.000000e-02 2.000000e-02 7.682700e+00 7.027704e-01 7.942806e-01
+6.750000e-01 1.500000e-02 1.500000e-02 5.393900e+00 4.181140e-01 3.637349e-01
+6.950000e-01 5.000000e-03 5.000000e-03 1.852600e+00 7.494174e-01 6.961937e-01
+7.250000e-01 2.500000e-02 2.500000e-02 1.466900e-01 3.854043e-02 4.194053e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d56-x01-y02
+Path=/REF/CMS_2018_I1690148/d56-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.100000e-01 1.100000e-01 1.100000e-01 1.801000e+00 1.828547e-01 1.660884e-01
+6.400000e-01 2.000000e-02 2.000000e-02 9.103800e+00 4.639304e-01 6.395185e-01
+6.750000e-01 1.500000e-02 1.500000e-02 6.897700e+00 5.161988e-01 5.328843e-01
+6.950000e-01 5.000000e-03 5.000000e-03 2.459300e+00 1.014416e+00 8.838172e-01
+7.250000e-01 2.500000e-02 2.500000e-02 1.623000e-01 6.466699e-02 7.858949e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d56-x01-y03
+Path=/REF/CMS_2018_I1690148/d56-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.100000e-01 1.100000e-01 1.100000e-01 2.899400e+00 2.103450e-01 1.962294e-01
+6.400000e-01 2.000000e-02 2.000000e-02 6.187000e+00 1.165134e+00 1.165332e+00
+6.750000e-01 1.500000e-02 1.500000e-02 3.495700e+00 3.660269e-01 4.277556e-01
+6.950000e-01 5.000000e-03 5.000000e-03 6.796400e-01 5.549617e-01 4.903098e-01
+7.250000e-01 2.500000e-02 2.500000e-02 5.958000e-02 1.701950e-02 2.461177e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d56-x01-y04
+Path=/REF/CMS_2018_I1690148/d56-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.100000e-01 1.100000e-01 1.100000e-01 1.843800e+00 1.721118e-01 1.604887e-01
+6.400000e-01 2.000000e-02 2.000000e-02 7.693400e+00 8.917274e-01 8.654116e-01
+6.750000e-01 1.500000e-02 1.500000e-02 7.225000e+00 8.946919e-01 8.217710e-01
+6.950000e-01 5.000000e-03 5.000000e-03 4.818500e+00 1.468613e+00 1.740537e+00
+7.250000e-01 2.500000e-02 2.500000e-02 4.337100e-01 2.369892e-01 1.899787e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d57-x01-y01
+Path=/REF/CMS_2018_I1690148/d57-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e-01 1.400000e-01 1.400000e-01 9.074400e-01 9.157447e-02 6.483660e-02
+4.050000e-01 2.500000e-02 2.500000e-02 7.110300e+00 2.190032e-01 5.605864e-01
+4.450000e-01 1.500000e-02 1.500000e-02 6.683300e+00 6.575897e-01 3.010718e-01
+4.750000e-01 1.500000e-02 1.500000e-02 4.510500e+00 2.219610e-01 3.785522e-01
+5.050000e-01 1.500000e-02 1.500000e-02 1.710500e+00 1.968930e-01 1.278387e-01
+5.600000e-01 4.000000e-02 4.000000e-02 4.087500e-02 2.105826e-02 2.472897e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d57-x01-y02
+Path=/REF/CMS_2018_I1690148/d57-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e-01 1.400000e-01 1.400000e-01 6.825200e-01 8.540801e-02 8.304593e-02
+4.050000e-01 2.500000e-02 2.500000e-02 7.620300e+00 4.176552e-01 3.888247e-01
+4.450000e-01 1.500000e-02 1.500000e-02 7.819900e+00 4.900777e-01 6.346893e-01
+4.750000e-01 1.500000e-02 1.500000e-02 4.482800e+00 4.209864e-01 3.978324e-01
+5.050000e-01 1.500000e-02 1.500000e-02 1.886700e+00 2.707542e-01 2.154484e-01
+5.600000e-01 4.000000e-02 4.000000e-02 2.743000e-02 3.736050e-02 4.281182e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d57-x01-y03
+Path=/REF/CMS_2018_I1690148/d57-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e-01 1.400000e-01 1.400000e-01 1.176400e+00 1.308406e-01 6.652234e-02
+4.050000e-01 2.500000e-02 2.500000e-02 6.544700e+00 2.479909e-01 1.076358e+00
+4.450000e-01 1.500000e-02 1.500000e-02 6.108300e+00 1.440319e+00 4.180543e-01
+4.750000e-01 1.500000e-02 1.500000e-02 3.689200e+00 3.953533e-01 9.464461e-01
+5.050000e-01 1.500000e-02 1.500000e-02 1.637100e+00 4.978274e-01 2.236476e-01
+5.600000e-01 4.000000e-02 4.000000e-02 3.992000e-03 4.408877e-02 5.283605e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d57-x01-y04
+Path=/REF/CMS_2018_I1690148/d57-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.400000e-01 1.400000e-01 1.400000e-01 7.245400e-01 7.112751e-02 8.343761e-02
+4.050000e-01 2.500000e-02 2.500000e-02 6.200800e+00 5.644365e-01 6.297208e-01
+4.450000e-01 1.500000e-02 1.500000e-02 6.592400e+00 1.174510e+00 9.507458e-01
+4.750000e-01 1.500000e-02 1.500000e-02 6.764700e+00 6.812614e-01 8.104754e-01
+5.050000e-01 1.500000e-02 1.500000e-02 2.620800e+00 3.731784e-01 3.864933e-01
+5.600000e-01 4.000000e-02 4.000000e-02 9.689400e-02 7.253597e-02 6.198341e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d58-x01-y01
+Path=/REF/CMS_2018_I1690148/d58-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 2.238100e+00 1.951886e-01 1.812900e-01
+2.800000e-01 2.000000e-02 2.000000e-02 6.008000e+00 1.326485e+00 1.783407e+00
+3.200000e-01 2.000000e-02 2.000000e-02 3.834800e+00 7.619363e-01 3.793421e-01
+3.700000e-01 3.000000e-02 3.000000e-02 4.062100e-01 1.322879e-01 1.142076e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d58-x01-y02
+Path=/REF/CMS_2018_I1690148/d58-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 2.230900e+00 1.933115e-01 2.098508e-01
+2.800000e-01 2.000000e-02 2.000000e-02 6.184300e+00 1.681894e+00 1.623885e+00
+3.200000e-01 2.000000e-02 2.000000e-02 3.657000e+00 7.672771e-01 5.997520e-01
+3.700000e-01 3.000000e-02 3.000000e-02 4.385200e-01 1.666849e-01 3.971144e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d58-x01-y03
+Path=/REF/CMS_2018_I1690148/d58-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 2.317200e+00 2.037698e-01 1.847109e-01
+2.800000e-01 2.000000e-02 2.000000e-02 5.763200e+00 1.359472e+00 1.847545e+00
+3.200000e-01 2.000000e-02 2.000000e-02 3.662800e+00 7.997301e-01 4.434052e-01
+3.700000e-01 3.000000e-02 3.000000e-02 3.414800e-01 1.616006e-01 1.092391e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d58-x01-y04
+Path=/REF/CMS_2018_I1690148/d58-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.300000e-01 1.300000e-01 1.300000e-01 1.872900e+00 2.324713e-01 1.555935e-01
+2.800000e-01 2.000000e-02 2.000000e-02 6.350000e+00 9.052951e-01 2.279429e+00
+3.200000e-01 2.000000e-02 2.000000e-02 5.553400e+00 1.052481e+00 7.114298e-01
+3.700000e-01 3.000000e-02 3.000000e-02 6.152800e-01 4.969936e-01 2.899114e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d59-x01-y01
+Path=/REF/CMS_2018_I1690148/d59-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.500000e-02 5.500000e-02 5.500000e-02 4.117900e+00 5.061028e-01 4.542654e-01
+1.275000e-01 1.750000e-02 1.750000e-02 8.435000e+00 1.479120e+00 1.786873e+00
+1.650000e-01 2.000000e-02 2.000000e-02 4.917100e+00 4.092931e-01 4.856329e-01
+2.175000e-01 3.250000e-02 3.250000e-02 8.479400e-01 1.794334e-01 1.927793e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d59-x01-y02
+Path=/REF/CMS_2018_I1690148/d59-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.500000e-02 5.500000e-02 5.500000e-02 4.117900e+00 5.653142e-01 6.179148e-01
+1.275000e-01 1.750000e-02 1.750000e-02 8.493100e+00 2.193016e+00 2.046394e+00
+1.650000e-01 2.000000e-02 2.000000e-02 4.940000e+00 5.543239e-01 9.534142e-01
+2.175000e-01 3.250000e-02 3.250000e-02 8.025300e-01 3.351986e-01 2.633293e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d59-x01-y03
+Path=/REF/CMS_2018_I1690148/d59-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.500000e-02 5.500000e-02 5.500000e-02 4.409500e+00 5.177978e-01 4.417813e-01
+1.275000e-01 1.750000e-02 1.750000e-02 7.745100e+00 1.485671e+00 1.874719e+00
+1.650000e-01 2.000000e-02 2.000000e-02 4.819000e+00 4.768874e-01 5.996537e-01
+2.175000e-01 3.250000e-02 3.250000e-02 7.864200e-01 2.749545e-01 1.593024e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d59-x01-y04
+Path=/REF/CMS_2018_I1690148/d59-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.500000e-02 5.500000e-02 5.500000e-02 3.050100e+00 4.797262e-01 3.597655e-01
+1.275000e-01 1.750000e-02 1.750000e-02 9.651300e+00 1.150925e+00 1.468762e+00
+1.650000e-01 2.000000e-02 2.000000e-02 5.957000e+00 6.715083e-01 1.273343e+00
+2.175000e-01 3.250000e-02 3.250000e-02 1.360200e+00 6.327973e-01 2.448777e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d60-x01-y01
+Path=/REF/CMS_2018_I1690148/d60-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-02 1.250000e-02 1.250000e-02 2.279900e+01 2.222718e+00 3.919657e+00
+8.750000e-02 6.250000e-02 6.250000e-02 3.440100e+00 7.840279e-01 4.447136e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d60-x01-y02
+Path=/REF/CMS_2018_I1690148/d60-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-02 1.250000e-02 1.250000e-02 2.277300e+01 2.354320e+00 6.283966e+00
+8.750000e-02 6.250000e-02 6.250000e-02 3.445400e+00 1.257116e+00 4.716608e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d60-x01-y03
+Path=/REF/CMS_2018_I1690148/d60-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-02 1.250000e-02 1.250000e-02 2.421100e+01 2.172034e+00 4.524323e+00
+8.750000e-02 6.250000e-02 6.250000e-02 3.157800e+00 9.049476e-01 4.345690e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d60-x01-y04
+Path=/REF/CMS_2018_I1690148/d60-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.250000e-02 1.250000e-02 1.250000e-02 1.737500e+01 2.137763e+00 4.083631e+00
+8.750000e-02 6.250000e-02 6.250000e-02 4.525000e+00 8.183988e-01 4.307579e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d61-x01-y01
+Path=/REF/CMS_2018_I1690148/d61-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.250000e-02 5.250000e-02 5.250000e-02 3.082900e+00 2.526675e-01 2.026824e-01
+1.150000e-01 1.000000e-02 1.000000e-02 1.206000e+01 8.575487e-01 1.868759e+00
+1.325000e-01 7.500000e-03 7.500000e-03 1.422300e+01 2.377128e+00 1.068613e+00
+1.475000e-01 7.500000e-03 7.500000e-03 1.037300e+01 1.126948e+00 1.573984e+00
+1.675000e-01 1.250000e-02 1.250000e-02 2.645600e+00 2.673601e-01 2.318051e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d61-x01-y02
+Path=/REF/CMS_2018_I1690148/d61-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.250000e-02 5.250000e-02 5.250000e-02 2.101800e+00 2.340277e-01 1.925700e-01
+1.150000e-01 1.000000e-02 1.000000e-02 1.166100e+01 7.808193e-01 1.122231e+00
+1.325000e-01 7.500000e-03 7.500000e-03 1.726000e+01 1.654012e+00 1.415543e+00
+1.475000e-01 7.500000e-03 7.500000e-03 1.306900e+01 1.512756e+00 1.416175e+00
+1.675000e-01 1.250000e-02 1.250000e-02 3.645800e+00 4.508115e-01 4.909387e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d61-x01-y03
+Path=/REF/CMS_2018_I1690148/d61-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.250000e-02 5.250000e-02 5.250000e-02 4.078400e+00 3.504603e-01 2.875738e-01
+1.150000e-01 1.000000e-02 1.000000e-02 1.180300e+01 1.903608e+00 2.918975e+00
+1.325000e-01 7.500000e-03 7.500000e-03 1.211800e+01 3.492509e+00 1.666185e+00
+1.475000e-01 7.500000e-03 7.500000e-03 7.115200e+00 1.239546e+00 2.150953e+00
+1.675000e-01 1.250000e-02 1.250000e-02 1.888700e+00 3.438147e-01 2.207876e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d61-x01-y04
+Path=/REF/CMS_2018_I1690148/d61-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+5.250000e-02 5.250000e-02 5.250000e-02 3.104900e+00 2.086227e-01 2.211193e-01
+1.150000e-01 1.000000e-02 1.000000e-02 1.250500e+01 1.498077e+00 2.349950e+00
+1.325000e-01 7.500000e-03 7.500000e-03 1.278300e+01 3.740386e+00 2.679269e+00
+1.475000e-01 7.500000e-03 7.500000e-03 1.182600e+01 2.679786e+00 3.067828e+00
+1.675000e-01 1.250000e-02 1.250000e-02 2.189400e+00 1.010543e+00 5.917051e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d62-x01-y01
+Path=/REF/CMS_2018_I1690148/d62-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.700000e-01 1.200000e-01 1.200000e-01 2.599400e+00 1.479847e-01 1.106853e-01
+4.050000e-01 1.500000e-02 1.500000e-02 9.795200e+00 9.740314e-01 1.246325e+00
+4.350000e-01 1.500000e-02 1.500000e-02 2.743100e+00 2.958198e-01 3.224583e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d62-x01-y02
+Path=/REF/CMS_2018_I1690148/d62-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.700000e-01 1.200000e-01 1.200000e-01 2.271900e+00 1.213263e-01 1.117586e-01
+4.050000e-01 1.500000e-02 1.500000e-02 1.172700e+01 9.161129e-01 7.333328e-01
+4.350000e-01 1.500000e-02 1.500000e-02 3.431900e+00 2.958950e-01 4.919596e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d62-x01-y03
+Path=/REF/CMS_2018_I1690148/d62-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.700000e-01 1.200000e-01 1.200000e-01 2.985300e+00 2.103432e-01 1.389361e-01
+4.050000e-01 1.500000e-02 1.500000e-02 7.762000e+00 1.366437e+00 1.915780e+00
+4.350000e-01 1.500000e-02 1.500000e-02 1.689000e+00 7.729733e-01 8.399297e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d62-x01-y04
+Path=/REF/CMS_2018_I1690148/d62-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.700000e-01 1.200000e-01 1.200000e-01 2.366700e+00 1.655108e-01 1.577117e-01
+4.050000e-01 1.500000e-02 1.500000e-02 1.049900e+01 1.767121e+00 1.483060e+00
+4.350000e-01 1.500000e-02 1.500000e-02 3.901300e+00 6.230481e-01 9.821765e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d63-x01-y01
+Path=/REF/CMS_2018_I1690148/d63-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.250000e-01 6.250000e-01 6.250000e-01 4.501100e-01 2.203183e-02 1.518570e-02
+1.500000e+00 5.000000e-02 5.000000e-02 1.628000e+00 1.493233e-01 3.328577e-01
+1.625000e+00 7.500000e-02 7.500000e-02 9.603200e-01 2.145536e-01 9.020479e-02
+2.100000e+00 4.000000e-01 4.000000e-01 1.631400e-01 1.060688e-02 2.154875e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d63-x01-y02
+Path=/REF/CMS_2018_I1690148/d63-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.250000e-01 6.250000e-01 6.250000e-01 4.901000e-01 2.325775e-02 1.375800e-02
+1.500000e+00 5.000000e-02 5.000000e-02 1.667500e+00 1.665394e-01 3.819890e-01
+1.625000e+00 7.500000e-02 7.500000e-02 9.208200e-01 2.222393e-01 1.294670e-01
+2.100000e+00 4.000000e-01 4.000000e-01 1.031300e-01 1.374526e-02 2.022783e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d63-x01-y03
+Path=/REF/CMS_2018_I1690148/d63-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.250000e-01 6.250000e-01 6.250000e-01 4.254600e-01 2.496807e-02 1.922196e-02
+1.500000e+00 5.000000e-02 5.000000e-02 1.566400e+00 1.992179e-01 3.080104e-01
+1.625000e+00 7.500000e-02 7.500000e-02 9.315600e-01 2.255986e-01 1.131969e-01
+2.100000e+00 4.000000e-01 4.000000e-01 2.147500e-01 1.749579e-02 2.838496e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d63-x01-y04
+Path=/REF/CMS_2018_I1690148/d63-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+8.250000e-01 6.250000e-01 6.250000e-01 3.708300e-01 1.812031e-02 2.389050e-02
+1.500000e+00 5.000000e-02 5.000000e-02 1.880800e+00 3.204288e-01 3.669347e-01
+1.625000e+00 7.500000e-02 7.500000e-02 1.230100e+00 3.622952e-01 2.155137e-01
+2.100000e+00 4.000000e-01 4.000000e-01 2.048300e-01 3.780793e-02 4.779933e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d64-x01-y01
+Path=/REF/CMS_2018_I1690148/d64-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.625000e-02 2.625000e-02 2.625000e-02 7.052700e+00 7.741769e-01 6.492117e-01
+6.125000e-02 8.750000e-03 8.750000e-03 1.574400e+01 1.643401e+00 2.930691e+00
+7.750000e-02 7.500000e-03 7.500000e-03 1.405900e+01 2.442619e+00 6.846882e-01
+9.125000e-02 6.250000e-03 6.250000e-03 8.630400e+00 1.151408e+00 2.503003e+00
+1.087500e-01 1.125000e-02 1.125000e-02 1.575300e+00 4.264402e-01 1.466135e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d64-x01-y02
+Path=/REF/CMS_2018_I1690148/d64-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.625000e-02 2.625000e-02 2.625000e-02 5.278000e+00 6.117439e-01 5.820089e-01
+6.125000e-02 8.750000e-03 8.750000e-03 1.679200e+01 9.936998e-01 2.234263e+00
+7.750000e-02 7.500000e-03 7.500000e-03 1.660200e+01 2.588026e+00 8.873565e-01
+9.125000e-02 6.250000e-03 6.250000e-03 1.073500e+01 1.191829e+00 2.802802e+00
+1.087500e-01 1.125000e-02 1.125000e-02 2.037500e+00 7.275838e-01 3.598573e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d64-x01-y03
+Path=/REF/CMS_2018_I1690148/d64-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.625000e-02 2.625000e-02 2.625000e-02 8.652300e+00 9.909604e-01 9.065599e-01
+6.125000e-02 8.750000e-03 8.750000e-03 1.472500e+01 3.020663e+00 4.261458e+00
+7.750000e-02 7.500000e-03 7.500000e-03 1.169900e+01 3.737787e+00 1.448815e+00
+9.125000e-02 6.250000e-03 6.250000e-03 6.644100e+00 9.574371e-01 3.359287e+00
+1.087500e-01 1.125000e-02 1.125000e-02 1.312700e+00 6.536395e-01 1.619326e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d64-x01-y04
+Path=/REF/CMS_2018_I1690148/d64-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+2.625000e-02 2.625000e-02 2.625000e-02 7.698100e+00 6.516370e-01 5.680128e-01
+6.125000e-02 8.750000e-03 8.750000e-03 1.455500e+01 2.066708e+00 2.204668e+00
+7.750000e-02 7.500000e-03 7.500000e-03 1.442900e+01 1.902513e+00 2.595696e+00
+9.125000e-02 6.250000e-03 6.250000e-03 7.909600e+00 2.510182e+00 2.075349e+00
+1.087500e-01 1.125000e-02 1.125000e-02 1.148200e+00 2.960798e-01 3.606143e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d65-x01-y01
+Path=/REF/CMS_2018_I1690148/d65-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.400000e-01 1.400000e-01 1.400000e-01 2.499600e+00 2.014832e-01 1.095455e-01
+3.200000e-01 4.000000e-02 4.000000e-02 3.751600e+00 3.843045e-01 7.056655e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d65-x01-y02
+Path=/REF/CMS_2018_I1690148/d65-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.400000e-01 1.400000e-01 1.400000e-01 2.290200e+00 1.424775e-01 1.195976e-01
+3.200000e-01 4.000000e-02 4.000000e-02 4.484400e+00 4.203525e-01 5.001535e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d65-x01-y03
+Path=/REF/CMS_2018_I1690148/d65-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.400000e-01 1.400000e-01 1.400000e-01 2.729500e+00 2.725923e-01 1.133377e-01
+3.200000e-01 4.000000e-02 4.000000e-02 2.946900e+00 3.984809e-01 9.548282e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d65-x01-y04
+Path=/REF/CMS_2018_I1690148/d65-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+1.400000e-01 1.400000e-01 1.400000e-01 2.437700e+00 2.634415e-01 1.703672e-01
+3.200000e-01 4.000000e-02 4.000000e-02 3.968200e+00 6.087943e-01 9.301985e-01
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d66-x01-y01
+Path=/REF/CMS_2018_I1690148/d66-x01-y01
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+9.000000e-01 9.000000e-01 9.000000e-01 4.557400e-01 1.615482e-02 1.234874e-02
+2.650000e+00 8.500000e-01 8.500000e-01 1.056900e-01 1.306609e-02 1.709726e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d66-x01-y02
+Path=/REF/CMS_2018_I1690148/d66-x01-y02
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+9.000000e-01 9.000000e-01 9.000000e-01 4.783800e-01 1.674015e-02 1.045538e-02
+2.650000e+00 8.500000e-01 8.500000e-01 8.171200e-02 1.100530e-02 1.768441e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d66-x01-y03
+Path=/REF/CMS_2018_I1690148/d66-x01-y03
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+9.000000e-01 9.000000e-01 9.000000e-01 4.409700e-01 1.805623e-02 1.616937e-02
+2.650000e+00 8.500000e-01 8.500000e-01 1.213200e-01 1.712427e-02 1.912099e-02
+# END YODA_SCATTER2D
+
+# BEGIN YODA_SCATTER2D /REF/CMS_2018_I1690148/d66-x01-y04
+Path=/REF/CMS_2018_I1690148/d66-x01-y04
+Type=Scatter2D
+# xval xerr- xerr+ yval yerr- yerr+
+9.000000e-01 9.000000e-01 9.000000e-01 4.150200e-01 1.058208e-02 1.217018e-02
+2.650000e+00 8.500000e-01 8.500000e-01 1.488000e-01 1.290962e-02 1.123193e-02
+# END YODA_SCATTER2D
+
diff --git a/analyses/pluginMC/MC_PARTONICTOPS.cc b/analyses/pluginMC/MC_PARTONICTOPS.cc
--- a/analyses/pluginMC/MC_PARTONICTOPS.cc
+++ b/analyses/pluginMC/MC_PARTONICTOPS.cc
@@ -1,96 +1,108 @@
// -*- C++ -*-
#include "Rivet/Analysis.hh"
#include "Rivet/Projections/PartonicTops.hh"
namespace Rivet {
/// Find and plot partonic top properties (requires tops in event record)
class MC_PARTONICTOPS : public Analysis {
public:
/// Constructor
DEFAULT_RIVET_ANALYSIS_CTOR(MC_PARTONICTOPS);
/// @name Analysis methods
//@{
/// Book histograms and initialise projections before the run
void init() {
// Initialise and register projections
declare(PartonicTops(PartonicTops::ALL), "AllTops");
+ declare(PartonicTops(PartonicTops::ALL, true, false, Cuts::OPEN, PartonicTops::FIRST), "AllTopsFirst"); ///< @todo API ick!
declare(PartonicTops(PartonicTops::E_MU), "LeptonicTops");
declare(PartonicTops(PartonicTops::HADRONIC), "HadronicTops");
// Book histograms
_h_tall_n = bookHisto1D("t_all_n", linspace(5, -0.5, 4.5));
_h_tall_pt = bookHisto1D("t_all_pT", logspace(50, 1, 500));
_h_tall_y = bookHisto1D("t_all_y", linspace(50, -5, 5));
+ _h_tall_n_first = bookHisto1D("t_all_n_firsttop", linspace(5, -0.5, 4.5));
+ _h_tall_pt_first = bookHisto1D("t_all_pT_firsttop", logspace(50, 1, 500));
+ _h_tall_y_first = bookHisto1D("t_all_y_firsttop", linspace(50, -5, 5));
+
_h_tlep_n = bookHisto1D("t_lep_n", linspace(5, -0.5, 4.5));
_h_tlep_pt = bookHisto1D("t_lep_pT", logspace(50, 1, 500));
_h_tlep_y = bookHisto1D("t_lep_y", linspace(50, -5, 5));
_h_thad_n = bookHisto1D("t_had_n", linspace(5, -0.5, 4.5));
_h_thad_pt = bookHisto1D("t_had_pT", logspace(50, 1, 500));
_h_thad_y = bookHisto1D("t_had_y", linspace(50, -5, 5));
}
/// Perform the per-event analysis
void analyze(const Event& event) {
const Particles& alltops = apply<PartonicTops>(event, "AllTops").particlesByPt();
_h_tall_n->fill(alltops.size(), event.weight());
for (const Particle& t : alltops) {
_h_tall_pt->fill(t.pT()/GeV, event.weight());
_h_tall_y->fill(t.rap(), event.weight());
}
+ const Particles& alltops_first = apply<PartonicTops>(event, "AllTopsFirst").particlesByPt();
+ _h_tall_n_first->fill(alltops_first.size(), event.weight());
+ for (const Particle& t : alltops_first) {
+ _h_tall_pt_first->fill(t.pT()/GeV, event.weight());
+ _h_tall_y_first->fill(t.rap(), event.weight());
+ }
+
const Particles& leptops = apply<PartonicTops>(event, "LeptonicTops").particlesByPt();
_h_tlep_n->fill(leptops.size(), event.weight());
for (const Particle& t : leptops) {
_h_tlep_pt->fill(t.pT()/GeV, event.weight());
_h_tlep_y->fill(t.rap(), event.weight());
}
const Particles& hadtops = apply<PartonicTops>(event, "HadronicTops").particlesByPt();
_h_thad_n->fill(hadtops.size(), event.weight());
for (const Particle& t : hadtops) {
_h_thad_pt->fill(t.pT()/GeV, event.weight());
_h_thad_y->fill(t.rap(), event.weight());
}
}
/// Normalise histograms etc., after the run
void finalize() {
- normalize({_h_tall_n, _h_tlep_n, _h_thad_n});
- normalize({_h_tall_pt, _h_tlep_pt, _h_thad_pt});
- normalize({_h_tall_y, _h_tlep_y, _h_thad_y});
+ normalize({_h_tall_n, _h_tall_n_first, _h_tlep_n, _h_thad_n});
+ normalize({_h_tall_pt, _h_tall_pt_first, _h_tlep_pt, _h_thad_pt});
+ normalize({_h_tall_y, _h_tall_y_first, _h_tlep_y, _h_thad_y});
}
//@}
/// @name Histograms
//@{
- Histo1DPtr _h_tall_n, _h_tlep_n, _h_thad_n;
- Histo1DPtr _h_tall_pt, _h_tlep_pt, _h_thad_pt;
- Histo1DPtr _h_tall_y, _h_tlep_y, _h_thad_y;
+ Histo1DPtr _h_tall_n, _h_tall_n_first, _h_tlep_n, _h_thad_n;
+ Histo1DPtr _h_tall_pt, _h_tall_pt_first, _h_tlep_pt, _h_thad_pt;
+ Histo1DPtr _h_tall_y, _h_tall_y_first, _h_tlep_y, _h_thad_y;
//@}
};
// The hook for the plugin system
DECLARE_RIVET_PLUGIN(MC_PARTONICTOPS);
}
diff --git a/configure.ac b/configure.ac
--- a/configure.ac
+++ b/configure.ac
@@ -1,331 +1,334 @@
## Process this file with autoconf to produce a configure script.
AC_PREREQ(2.59)
-AC_INIT([Rivet],[2.6.1-options],[rivet@projects.hepforge.org],[Rivet])
+AC_INIT([Rivet],[2.7.0-beta1],[rivet@projects.hepforge.org],[Rivet])
## Check and block installation into the src/build dir
if test "$prefix" = "$PWD"; then
AC_MSG_ERROR([Installation into the build directory is not supported: use a different --prefix argument])
fi
## Force default prefix to have a path value rather than NONE
if test "$prefix" = "NONE"; then
prefix=/usr/local
fi
AC_CONFIG_SRCDIR([src/Core/Analysis.cc])
AC_CONFIG_HEADERS([include/Rivet/Config/DummyConfig.hh include/Rivet/Config/RivetConfig.hh include/Rivet/Config/BuildOptions.hh])
AM_INIT_AUTOMAKE([dist-bzip2 -Wall 1.10])
m4_ifdef([AM_SILENT_RULES], [AM_SILENT_RULES([yes])])
m4_ifdef([AM_PROG_AR], [AM_PROG_AR])
AC_CONFIG_MACRO_DIR([m4])
AC_SUBST(LT_OBJDIR)
## Package-specific #defines
AC_DEFINE_UNQUOTED(RIVET_VERSION, "$PACKAGE_VERSION", "Rivet version string")
AC_DEFINE_UNQUOTED(RIVET_NAME, "$PACKAGE_NAME", "Rivet name string")
AC_DEFINE_UNQUOTED(RIVET_STRING, "$PACKAGE_STRING", "Rivet name and version string")
AC_DEFINE_UNQUOTED(RIVET_TARNAME, "$PACKAGE_TARNAME", "Rivet short name string")
AC_DEFINE_UNQUOTED(RIVET_BUGREPORT, "$PACKAGE_BUGREPORT", "Rivet contact email address")
## OS X
AC_CEDAR_OSX
## Work out the LCG platform tag
AC_LCG_TAG
## Set default compiler flags
if test "x$CXXFLAGS" == "x"; then CXXFLAGS="-O2"; fi
## Compiler setup
AC_LANG(C++)
AC_PROG_CXX
AX_CXX_COMPILE_STDCXX([11], [noext], [mandatory])
## Store and propagate the compiler identity and flags
RIVETCXX="$CXX"
AC_SUBST(RIVETCXX)
RIVETCXXFLAGS="$CXXFLAGS"
AC_SUBST(RIVETCXXFLAGS)
## Checks for programs.
AC_PROG_INSTALL
AC_PROG_LN_S
AC_DISABLE_STATIC
AC_LIBTOOL_DLOPEN
AC_PROG_LIBTOOL
AC_FUNC_STRERROR_R
## YODA histogramming library
AC_CEDAR_LIBRARYANDHEADERS([YODA], , , [AC_MSG_ERROR([YODA is required])])
YODABINPATH=$YODALIBPATH/../bin
AC_SUBST(YODABINPATH)
AC_PATH_PROG(YODACONFIG, yoda-config, [], [$YODALIBPATH/../bin:$PATH])
YODA_PYTHONPATH=""
if test -f "$YODACONFIG"; then
AC_MSG_CHECKING([YODA version using yoda-config])
YODA_VERSION=`$YODACONFIG --version`
AC_MSG_RESULT([$YODA_VERSION])
YODA_VERSION1=[`echo $YODA_VERSION | cut -d. -f1 | sed -e 's/\([0-9]*\).*/\1/g'`]
YODA_VERSION2=[`echo $YODA_VERSION | cut -d. -f2 | sed -e 's/\([0-9]*\).*/\1/g'`]
YODA_VERSION3=[`echo $YODA_VERSION | cut -d. -f3 | sed -e 's/\([0-9]*\).*/\1/g'`]
let YODA_VERSION_INT=YODA_VERSION1*10000+YODA_VERSION2*100+YODA_VERSION3
if test $YODA_VERSION_INT -lt 10500; then
AC_MSG_ERROR([YODA version isn't sufficient: at least version 1.5.0 required])
fi
AC_MSG_CHECKING([YODA Python path using yoda-config])
YODA_PYTHONPATH=`$YODACONFIG --pythonpath`
AC_MSG_RESULT([$YODA_PYTHONPATH])
fi
AC_SUBST(YODA_PYTHONPATH)
## HepMC event record library
AC_CEDAR_LIBRARYANDHEADERS([HepMC], , , [AC_MSG_ERROR([HepMC is required])])
oldCPPFLAGS=$CPPFLAGS
CPPFLAGS="$CPPFLAGS -I$HEPMCINCPATH"
if test -e "$HEPMCINCPATH/HepMC/HepMCDefs.h"; then
AC_LANG_CONFTEST([AC_LANG_SOURCE([#include <iostream>
#include "HepMC/HepMCDefs.h"
int main() { std::cout << HEPMC_VERSION << std::endl; return 0; }])])
else
AC_LANG_CONFTEST([AC_LANG_SOURCE([#include <iostream>
#include "HepMC/defs.h"
int main() { std::cout << VERSION << std::endl; return 0; }])])
fi
if test -f conftest.cc; then
$CXX $CPPFLAGS conftest.cc -o conftest 2>&1 1>&5
elif test -f conftest.C; then
$CXX $CPPFLAGS conftest.C -o conftest 2>&1 1>&5
else
$CXX $CPPFLAGS conftest.cpp -o conftest 2>&1 1>&5
fi
hepmc_version=`./conftest`
if test x$hepmc_version != x; then
let hepmc_major=`echo "$hepmc_version" | cut -d. -f1`
let hepmc_minor=`echo "$hepmc_version" | cut -d. -f2`
fi
rm -f conftest conftest.cpp conftest.cc conftest.C
HEPMC_VERSION=$hepmc_major$hepmc_minor
AC_MSG_NOTICE([HepMC version is $hepmc_version -> $HEPMC_VERSION])
AC_SUBST(HEPMC_VERSION)
CPPFLAGS=$oldCPPFLAGS
## FastJet clustering library
AC_CEDAR_LIBRARYANDHEADERS([fastjet], , , [AC_MSG_ERROR([FastJet is required])])
AC_PATH_PROG(FJCONFIG, fastjet-config, [], $FASTJETPATH/bin:$PATH)
if test -f "$FJCONFIG"; then
AC_MSG_CHECKING([FastJet version using fastjet-config])
fjversion=`$FJCONFIG --version`
AC_MSG_RESULT([$fjversion])
fjmajor=$(echo $fjversion | cut -f1 -d.)
fjminor=$(echo $fjversion | cut -f2 -d.)
fjmicro=$(echo $fjversion | cut -f3 -d.)
if test "$fjmajor" -lt 3; then
AC_MSG_ERROR([FastJet version 3.0.0 or later is required])
fi
FASTJETCONFIGLIBADD="$($FJCONFIG --plugins --shared --libs)"
else
FASTJETCONFIGLIBADD="-L$FASTJETLIBPATH -l$FASTJETLIBNAME"
FASTJETCONFIGLIBADD="$FASTJETCONFIGLIBADD -lSISConePlugin -lsiscone -lsiscone_spherical"
FASTJETCONFIGLIBADD="$FASTJETCONFIGLIBADD -lCDFConesPlugin -lD0RunIIConePlugin -lNestedDefsPlugin"
FASTJETCONFIGLIBADD="$FASTJETCONFIGLIBADD -lTrackJetPlugin -lATLASConePlugin -lCMSIterativeConePlugin"
FASTJETCONFIGLIBADD="$FASTJETCONFIGLIBADD -lEECambridgePlugin -lJadePlugin"
fi;
AC_MSG_NOTICE([FastJet LIBADD = $FASTJETCONFIGLIBADD])
AC_SUBST(FASTJETCONFIGLIBADD)
# Check for FastJet headers that require the --enable-all(cxx)plugins option
FASTJET_ERRMSG="Required FastJet plugin headers were not found: did you build FastJet with the --enable-allcxxplugins option?"
oldCPPFLAGS=$CPPFLAGS
CPPFLAGS="$CPPFLAGS -I$FASTJETINCPATH"
AC_CHECK_HEADER([fastjet/D0RunIIConePlugin.hh], [], [AC_MSG_ERROR([$FASTJET_ERRMSG])])
AC_CHECK_HEADER([fastjet/TrackJetPlugin.hh], [], [AC_MSG_ERROR([$FASTJET_ERRMSG])])
CPPFLAGS=$oldCPPFLAGS
# ## GNU Scientific Library
# AC_SEARCH_GSL
# AC_CEDAR_HEADERS([gsl], , , [AC_MSG_ERROR([GSL (GNU Scientific Library) is required])])
# oldCPPFLAGS=$CPPFLAGS
# CPPFLAGS="$CPPFLAGS -I$GSLINCPATH"
# AC_CHECK_HEADER([gsl/gsl_vector.h], [], [AC_MSG_ERROR([GSL vectors not found.])])
# CPPFLAGS=$oldCPPFLAGS
## Disable build/install of standard analyses
AC_ARG_ENABLE([analyses],
[AC_HELP_STRING(--disable-analyses, [don't try to build or install standard analyses])],
[], [enable_analyses=yes])
if test x$enable_analyses != xyes; then
AC_MSG_WARN([Not building standard Rivet analyses, by request])
fi
AM_CONDITIONAL(ENABLE_ANALYSES, [test x$enable_analyses = xyes])
## Build LaTeX docs if possible...
AC_PATH_PROG(PDFLATEX, pdflatex)
AM_CONDITIONAL(WITH_PDFLATEX, [test x$PDFLATEX != x])
## ... unless told otherwise!
AC_ARG_ENABLE([pdfmanual],
[AC_HELP_STRING(--enable-pdfmanual, [build and install the manual])],
[], [enable_pdfmanual=no])
if test x$enable_pdfmanual = xyes; then
AC_MSG_WARN([Building Rivet manual, by request])
fi
AM_CONDITIONAL(ENABLE_PDFMANUAL, [test x$enable_pdfmanual = xyes])
## Build Doxygen documentation if possible
AC_ARG_ENABLE([doxygen],
[AC_HELP_STRING(--disable-doxygen, [don't try to make Doxygen documentation])],
[], [enable_doxygen=yes])
if test x$enable_doxygen = xyes; then
AC_PATH_PROG(DOXYGEN, doxygen)
fi
AM_CONDITIONAL(WITH_DOXYGEN, [test x$DOXYGEN != x])
## Build asciidoc docs if possible
AC_PATH_PROG(ASCIIDOC, asciidoc)
AM_CONDITIONAL(WITH_ASCIIDOC, [test x$ASCIIDOC != x])
## Python extension
AC_ARG_ENABLE(pyext, [AC_HELP_STRING(--disable-pyext,
[don't build Python module (default=build)])],
[], [enable_pyext=yes])
## Basic Python checks
if test x$enable_pyext == xyes; then
AX_PYTHON_DEVEL([>= '2.7.3'])
AC_SUBST(PYTHON_VERSION)
RIVET_PYTHONPATH=`$PYTHON -c "from __future__ import print_function;
import distutils.sysconfig; print(distutils.sysconfig.get_python_lib(prefix='$prefix', plat_specific=True));"`
AC_SUBST(RIVET_PYTHONPATH)
if test -z "$PYTHON"; then
AC_MSG_ERROR([Can't build Python extension since python can't be found])
enable_pyext=no
fi
if test -z "$PYTHON_CPPFLAGS"; then
AC_MSG_ERROR([Can't build Python extension since Python.h header file cannot be found])
enable_pyext=no
fi
fi
AM_CONDITIONAL(ENABLE_PYEXT, [test x$enable_pyext == xyes])
dnl
dnl setup.py puts its build artifacts into a labelled path
dnl this helps the test scripts to find them locally instead of
dnl having to install first
dnl
RIVET_SETUP_PY_PATH=$(${PYTHON} -c 'from __future__ import print_function;
import distutils.util as u, sys; vi=sys.version_info; print("lib.%s-%s.%s" % (u.get_platform(),vi.major, vi.minor))')
AC_SUBST(RIVET_SETUP_PY_PATH)
## Cython checks
if test x$enable_pyext == xyes; then
AM_CHECK_CYTHON([0.24.0], [:], [:])
if test x$CYTHON_FOUND = xyes; then
AC_MSG_NOTICE([Cython >= 0.24 found: Python extension source can be rebuilt (for developers)])
fi
AC_CHECK_FILE([pyext/rivet/core.cpp],
[],
[if test "x$CYTHON_FOUND" != "xyes"; then
AC_MSG_ERROR([Cython is required for --enable-pyext, no pre-built core.cpp was found.])
fi])
cython_compiler=$CXX
## Set extra Python extension build flags (to cope with Cython output code oddities)
PYEXT_CXXFLAGS="$CXXFLAGS"
AC_CEDAR_CHECKCXXFLAG([-Wno-unused-but-set-variable], [PYEXT_CXXFLAGS="$PYEXT_CXXFLAGS -Wno-unused-but-set-variable"])
AC_CEDAR_CHECKCXXFLAG([-Wno-sign-compare], [PYEXT_CXXFLAGS="$PYEXT_CXXFLAGS -Wno-sign-compare"])
AC_SUBST(PYEXT_CXXFLAGS)
AC_MSG_NOTICE([All Python build checks successful: 'rivet' Python extension will be built])
fi
AM_CONDITIONAL(WITH_CYTHON, [test x$CYTHON_FOUND = xyes])
## Set default build flags
AM_CPPFLAGS="-I\$(top_srcdir)/include -I\$(top_builddir)/include"
#AM_CPPFLAGS="$AM_CPPFLAGS -I\$(top_srcdir)/include/eigen3"
#AM_CPPFLAGS="$AM_CPPFLAGS \$(GSL_CPPFLAGS)"
dnl AM_CPPFLAGS="$AM_CPPFLAGS \$(BOOST_CPPFLAGS)"
AM_CPPFLAGS="$AM_CPPFLAGS -I\$(YODAINCPATH)"
AM_CPPFLAGS="$AM_CPPFLAGS -I\$(HEPMCINCPATH)"
AM_CPPFLAGS="$AM_CPPFLAGS -I\$(FASTJETINCPATH)"
AC_CEDAR_CHECKCXXFLAG([-pedantic], [AM_CXXFLAGS="$AM_CXXFLAGS -pedantic"])
AC_CEDAR_CHECKCXXFLAG([-Wall], [AM_CXXFLAGS="$AM_CXXFLAGS -Wall"])
AC_CEDAR_CHECKCXXFLAG([-Wno-long-long], [AM_CXXFLAGS="$AM_CXXFLAGS -Wno-long-long"])
AC_CEDAR_CHECKCXXFLAG([-Wno-format], [AM_CXXFLAGS="$AM_CXXFLAGS -Wno-format"])
dnl AC_CEDAR_CHECKCXXFLAG([-Wno-unused-variable], [AM_CXXFLAGS="$AM_CXXFLAGS -Wno-unused-variable"])
AC_CEDAR_CHECKCXXFLAG([-Werror=uninitialized], [AM_CXXFLAGS="$AM_CXXFLAGS -Werror=uninitialized"])
AC_CEDAR_CHECKCXXFLAG([-Werror=delete-non-virtual-dtor], [AM_CXXFLAGS="$AM_CXXFLAGS -Werror=delete-non-virtual-dtor"])
## Add OpenMP-enabling flags if possible
AX_OPENMP([AM_CXXFLAGS="$AM_CXXFLAGS $OPENMP_CXXFLAGS"])
## Optional zlib support for gzip-compressed data streams/files
AX_CHECK_ZLIB
## Debug flag (default=-DNDEBUG, enabled=-g)
AC_ARG_ENABLE([debug], [AC_HELP_STRING(--enable-debug,
[build with debugging symbols @<:@default=no@:>@])], [], [enable_debug=no])
if test x$enable_debug == xyes; then
AM_CXXFLAGS="$AM_CXXFLAGS -g"
fi
## Extra warnings flag (default=none)
AC_ARG_ENABLE([extra-warnings], [AC_HELP_STRING(--enable-extra-warnings,
[build with extra compiler warnings (recommended for developers) @<:@default=no@:>@])], [], [enable_extra_warnings=no])
if test x$enable_extra_warnings == xyes; then
AC_CEDAR_CHECKCXXFLAG([-Wextra], [AM_CXXFLAGS="$AM_CXXFLAGS -Wextra "])
fi
AC_SUBST(AM_CPPFLAGS)
AC_SUBST(AM_CXXFLAGS)
AC_EMPTY_SUBST
AC_CONFIG_FILES(Makefile Doxyfile)
AC_CONFIG_FILES(include/Makefile include/Rivet/Makefile)
AC_CONFIG_FILES(src/Makefile)
AC_CONFIG_FILES(src/Core/Makefile src/Core/yamlcpp/Makefile)
AC_CONFIG_FILES(src/Tools/Makefile)
-AC_CONFIG_FILES(src/Tools/Nsubjettiness/Makefile)
+AC_CONFIG_FILES(src/Tools/fjcontrib/Makefile)
+AC_CONFIG_FILES(src/Tools/fjcontrib/EnergyCorrelator/Makefile)
+AC_CONFIG_FILES(src/Tools/fjcontrib/Nsubjettiness/Makefile)
+AC_CONFIG_FILES(src/Tools/fjcontrib/RecursiveTools/Makefile)
AC_CONFIG_FILES(src/Projections/Makefile)
AC_CONFIG_FILES(src/AnalysisTools/Makefile)
AC_CONFIG_FILES(analyses/Makefile)
AC_CONFIG_FILES(test/Makefile)
AC_CONFIG_FILES(pyext/Makefile pyext/rivet/Makefile pyext/setup.py)
AC_CONFIG_FILES(data/Makefile data/texmf/Makefile)
AC_CONFIG_FILES(doc/Makefile)
AC_CONFIG_FILES(doc/rivetversion.sty)
AC_CONFIG_FILES(bin/Makefile bin/rivet-config bin/rivet-buildplugin)
AC_CONFIG_FILES(rivetenv.sh rivetenv.csh rivet.pc)
AC_OUTPUT
if test x$enable_pyrivet == xyes; then
cat <<EOF
************************************************************
RIVET CONFIGURED!
Now build and install (to the $prefix tree) with e.g.
make -j2 && make -j2 install
To use Rivet, we recommend reading HepMC files from a file
or pipe (the latter may be made with mkfifo) using the
'rivet' executable.
For a more pleasant command line experience, you can include
the data/rivet-completion file into your .bashrc file,
or your bash_completion.d directory if you have one.
The rivetenv.*sh files will not be installed, but can help you
to set up a Rivet runtime environment in future.
************************************************************
EOF
fi
diff --git a/doc/Makefile.am b/doc/Makefile.am
--- a/doc/Makefile.am
+++ b/doc/Makefile.am
@@ -1,137 +1,142 @@
-dist_noinst_SCRIPTS = mk-analysis-html mk-analysis-latex mk-analysis-json
+dist_noinst_SCRIPTS = \
+ mk-analysis-html mk-analysis-latex mk-analysis-json \
+ mk-coverage-html mk-coverage-htmls
-LATEXSUBSOURCES = preamble.tex intro.tex gettingstarted.tex writinganalyses.tex agilerunmc.tex acknowledgements.tex
+LATEXSUBSOURCES = \
+ preamble.tex intro.tex gettingstarted.tex writinganalyses.tex \
+ agilerunmc.tex acknowledgements.tex
DOCSOURCES = $(LATEXSUBSOURCES) \
compare-histos.txt slip.eps thinker.eps cone.eps bend.eps \
h-physrev3.bst hepnames.sty JHEP3.cls JHEP.bst make-plots.txt rivet-manual.tex \
heppennames.sty hepnicenames.sty hepparticles.sty maybemath.sty \
hepunits.sty underscore.sty microtype.sty
EXTRA_DIST = $(DOCSOURCES) refs.bib
DOCS =
DOCDIRS =
if ENABLE_PYEXT
DOCS += analyses.html
DOCDIRS += analyses
analyses.html: $(top_srcdir)/analyses $(srcdir)/mk-analysis-html
LD_LIBRARY_PATH=$(top_builddir)/src/.libs:$(LD_LIBRARY_PATH) \
DYLD_LIBRARY_PATH=$(top_builddir)/src/.libs:$(DYLD_LIBRARY_PATH) \
PYTHONPATH=$(YODA_PYTHONPATH):$(RIVET_PYTHONPATH):$(PYTHONPATH) \
- $(PYTHON) $(srcdir)/mk-analysis-html
+ RIVET_ANALYSIS_PATH=$(top_builddir)/analyses:: \
+ $(PYTHON) $(srcdir)/mk-analysis-html || true
endif
if ENABLE_PYEXT
DOCS += analyses.json
analyses.json: $(top_srcdir)/analyses $(srcdir)/mk-analysis-json
LD_LIBRARY_PATH=$(top_builddir)/src/.libs:$(LD_LIBRARY_PATH) \
DYLD_LIBRARY_PATH=$(top_builddir)/src/.libs:$(DYLD_LIBRARY_PATH) \
PYTHONPATH=$(YODA_PYTHONPATH):$(RIVET_PYTHONPATH):$(PYTHONPATH) \
- $(PYTHON) $(srcdir)/mk-analysis-json
+ RIVET_ANALYSIS_PATH=$(top_builddir)/analyses:: \
+ $(PYTHON) $(srcdir)/mk-analysis-json || true
endif
if ENABLE_PYEXT
DOCS += rivet-coverage.html
-rivet-coverage.html: $(wildcard $(srcdir)/inspire*.json) $(top_srcdir)/analyses $(srcdir)/mk-coverage-html
+rivet-coverage.html: $(wildcard $(srcdir)/inspire*.json) $(wildcard $(srcdir)/*.rank) $(top_srcdir)/analyses $(srcdir)/mk-coverage-html
LD_LIBRARY_PATH=$(top_builddir)/src/.libs:$(LD_LIBRARY_PATH) \
DYLD_LIBRARY_PATH=$(top_builddir)/src/.libs:$(DYLD_LIBRARY_PATH) \
PYTHONPATH=$(YODA_PYTHONPATH):$(RIVET_PYTHONPATH):$(PYTHONPATH) \
- $(srcdir)/mk-coverage-htmls
+ RIVET_ANALYSIS_PATH=$(top_builddir)/analyses:: \
+ $(srcdir)/mk-coverage-htmls || true
endif
if WITH_ASCIIDOC
DOCS += compare-histos.html make-plots.html
EXTRA_DIST += compare-histos.html make-plots.html
compare-histos.html: compare-histos.txt
- asciidoc -a toc compare-histos.txt
+ asciidoc -a toc compare-histos.txt || true
make-plots.html: make-plots.txt
- asciidoc -a toc make-plots.txt
+ asciidoc -a toc make-plots.txt || true
endif
-if ENABLE_PDFMANUAL
if WITH_PDFLATEX
DOCS += rivet-manual.pdf
if ENABLE_PYEXT
analyses.bib analyses.tex: $(top_srcdir)/analyses $(srcdir)/mk-analysis-latex
LD_LIBRARY_PATH=$(top_builddir)/src/.libs:$(YAML_CPPLIBPATH):$(FASTJETLIBPATH):$(HEPMCLIBPATH):$(YODALIBPATH):$(LD_LIBRARY_PATH) \
DYLD_LIBRARY_PATH=$(top_builddir)/src/.libs:$(YAML_CPPLIBPATH):$(FASTJETLIBPATH):$(HEPMCLIBPATH):$(YODALIBPATH):$(DYLD_LIBRARY_PATH) \
PYTHONPATH=$(YODA_PYTHONPATH):$(RIVET_PYTHONPATH):$(PYTHONPATH) \
- $(PYTHON) $(srcdir)/mk-analysis-latex
+ RIVET_ANALYSIS_PATH=$(top_builddir)/analyses:: \
+ $(PYTHON) $(srcdir)/mk-analysis-latex || true
else
analyses.bib analyses.tex:
> analyses.tex
> analyses.bib
endif
LATEX = pdflatex --interaction=batchmode
RERUN = "(There were undefined references|Rerun to get (cross-references|the bars) right)"
RERUNBIB = "No file.*\.bbl|Citation.*undefined"
MAKEIDX = "^[^%]*\\makeindex"
rivet-manual.pdf : rivet-manual.tex $(LATEXSUBSOURCES) analyses.tex refs.bib analyses.bib
$(LATEX) $<; true
egrep -c $(RERUNBIB) rivet-manual.log && (bibtex rivet-manual && cp rivet-manual.toc rivet-manual.toc.bak && $(LATEX) $<); true
for i in `seq 5`; do if egrep $(RERUN) rivet-manual.log; then echo "LaTeX re-run $i"; cp rivet-manual.toc rivet-manual.toc.bak; $(LATEX) $<; else break; fi; done; true
if cmp -s rivet-manual.toc rivet-manual.toc.bak; then true; else $(LATEX) $<; true; fi
rm -f rivet-manual.toc.bak; true
paper.pdf : paper.tex $(LATEXSUBSOURCES) analyses.tex refs.bib analyses.bib
$(LATEX) $<; true
egrep -c $(RERUNBIB) paper.log && (bibtex paper && cp paper.toc paper.toc.bak && $(LATEX) $<); true
for i in `seq 5`; do if egrep $(RERUN) paper.log; then echo "LaTeX re-run $i"; cp paper.toc paper.toc.bak; $(LATEX) $<; else break; fi; done; true
if cmp -s paper.toc paper.toc.bak; then true; else $(LATEX) $<; true; fi
rm -f paper.toc.bak; true
endif
-endif
################
-.PHONY = all doc upload arxivtar
+RSH = rsync
+DEST = login.hepforge.org:rivet/public_html/
+
+
+.PHONY = doc upload arxivtar
doc: $(DOCS)
@true
-RSH = rsync
-DEST = login.hepforge.org:rivet/public_html/
upload: $(DOCS) $(DOCDIRS)
$(RSH) -r $? $(DEST)
arxivtar: $(DOCSOURCES) rivet-manual.bbl
for i in *.png; do convert $$i $${i/.png/.eps}; done
tar czf rivet-manual.tar.gz \
rivet-manual.tex $(LATEXSUBSOURCES) analyses.tex refs.bib analyses.bib rivetversion.sty rivet-manual.bbl \
hepnames.sty hepnicenames.sty hepparticles.sty heppennames.sty hepunits.sty maybemath.sty microtype.sty underscore.sty \
bend.eps cone.eps thinker.eps slip.eps \
h-physrev3.bst JHEP3.cls JHEP.bst
-## Install!
-pkgdata_DATA = $(DOCS)
+all-local:
+ @echo "No default target in doc: run 'make doc' to build documentation"
+ @true
-install-data-local: doc
- @$(NORMAL_INSTALL)
- test "$(DOCDIRS)" && cp -r $(DOCDIRS) $(DESTDIR)$(pkgdatadir)/
-
-uninstall-local:
- @$(NORMAL_UNINSTALL)
- rm -rf $(DESTDIR)$(pkgdatadir)/analyses
+install-data-local:
+ @echo "No local docs installation: copy the documentation to wherever you require"
+ @true
mostlyclean-local:
rm -rf *.aux *.log *.toc
clean-local:
- rm -rf $(DOCS) $(DOCDIRS)
+ rm -rf rivet-coverage-*.html $(DOCS) $(DOCDIRS)
diff --git a/doc/get-rivethd-marcxml b/doc/get-rivethd-marcxml
--- a/doc/get-rivethd-marcxml
+++ b/doc/get-rivethd-marcxml
@@ -1,94 +1,96 @@
#! /usr/bin/env python
"""\
%prog <file.marc.xml> [<file.marc.xml> ...]
"""
from __future__ import print_function
import argparse
ap = argparse.ArgumentParser(usage=__doc__)
ap.add_argument("XMLFILES", metavar='file', nargs="+", help="Inspire-exported MARC XML file to read")
args = ap.parse_args()
+if not args.XMLFILES:
+ exit(1)
import rivet
anas = {}
for aname in rivet.AnalysisLoader.analysisNames():
ana = rivet.AnalysisLoader.getAnalysis(aname)
# TODO: all anas *should* have an Inspire ID...
anas.setdefault(ana.inspireId(), []).append(ana.name())
del anas[""]
# print(anas.keys())
from lxml import etree #as ET
#nsm = {None : "http://www.loc.gov/MARC21/slim"}
nsm = {"mx" : "http://www.loc.gov/MARC21/slim"}
for ifile, xmlfile in enumerate(args.XMLFILES):
import urllib2, re, os
if ifile > 0: print()
print("Processing {}...".format(xmlfile))
jsonfile = xmlfile.replace(".marc.xml", ".json")
if os.path.exists(jsonfile):
print("{} exists, skipping {} testing".format(jsonfile, xmlfile))
continue
OUT = {}
tree = etree.parse(xmlfile)
recnodes = tree.findall("/mx:record", namespaces=nsm)
for rn in recnodes:
print()
# ctl = rn.find("./mx:controlfield", namespaces=nsm)
ctls = rn.xpath("./mx:controlfield[@tag=001]", namespaces=nsm)
ins = ctls[0].text if ctls else None
print("Inspire", ins)
summs = rn.xpath("./mx:datafield[@tag='245']/mx:subfield[@code='a']", namespaces=nsm)
summ = summs[0].text if summs else None
print("Title:", summ)
expts = rn.xpath("./mx:datafield[@tag='710']/mx:subfield[@code='g']", namespaces=nsm)
expt = expts[0].text if expts else None
print("Expt:", expt)
dois = rn.xpath("./mx:datafield[@tag='024']/mx:subfield[(@code='2') and (text()='DOI')]/../mx:subfield[@code='a']", namespaces=nsm)
doi = dois[0].text.replace("oai:arXiv.org:", "") if dois else None
print("DOI:", doi)
arxs = rn.xpath("./mx:datafield[@tag='035']/mx:subfield[(@code='9') and (text()='arXiv')]/../mx:subfield[@code='a']", namespaces=nsm)
arx = arxs[0].text.replace("oai:arXiv.org:", "") if arxs else None
print("arXiv:", arx)
cdss = rn.xpath("./mx:datafield[@tag='035']/mx:subfield[(@code='9') and (text()='CDS')]/../mx:subfield[@code='a']", namespaces=nsm)
cds = cdss[0].text if cdss else None
print("CDS:", cds)
hds = rn.xpath("./mx:datafield[@tag='035']/mx:subfield[(@code='9') and (text()='HEPDATA')]/../mx:subfield[@code='a']", namespaces=nsm)
hd = hds[0].text if hds else None
if not hd:
try:
hdurl = "https://hepdata.net/record/ins{}".format(ins)
u = urllib2.urlopen(hdurl)
hd = "ins{}".format(ins)
except urllib2.URLError:
pass
print("HepData:", hd)
rivetanas = anas.get(ins)
- nums = rn.xpath("./mx:datafield[@tag='037']/mx:subfield[(@code='9') and (text()='arXiv:reportnumber')]/../mx:subfield[@code='a']", namespaces=nsm)
- reportnums = [num.text for num in nums]
+ nums = rn.xpath("./mx:datafield[@tag='037']/mx:subfield[@code='a']", namespaces=nsm)
+ reportnums = [num.text for num in nums if not 'arXiv' in num.text]
print("Nums:", reportnums)
OUT[ins] = [summ, expt, doi, cds, arx, hd, rivetanas, reportnums]
print(OUT[ins])
## Write out as JSON
import json
with open(jsonfile, "wb") as jf:
json.dump(OUT, jf)
diff --git a/doc/inspire-alice-2018.json b/doc/inspire-alice-2018.json
--- a/doc/inspire-alice-2018.json
+++ b/doc/inspire-alice-2018.json
@@ -1,1 +1,1 @@
-{"1693305": ["Energy dependence of exclusive $J/\\psi$ photoproduction off protons in ultra-peripheral p-Pb collisions at $\\sqrt{s_{\\rm{NN}}}$ = 5.02 TeV", "ALICE", null, "2636152", "1809.03235", null, null, ["CERN-EP-2018-236"]], "1672944": ["Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV", "ALICE", null, "2316322", "1805.05212", null, null, ["CERN-EP-2018-115"]], "1672756": ["Centrality and pseudorapidity dependence of the charged-particle multiplicity density in Xe-Xe collisions at $\\sqrt{s_{\\rm NN}}$ = 5.44 TeV", "ALICE", null, "2316786", "1805.04432", null, null, ["CERN-EP-2018-120"]], "1693308": ["Charged jet cross section and fragmentation in proton-proton collisions at $\\sqrt{s}$ = 7 TeV", "ALICE", null, "2636150", "1809.03232", null, null, ["CERN-EP-2018-235"]], "1675759": ["p-p, p-$\\Lambda$ and $\\Lambda$-$\\Lambda$ correlations studied via femtoscopy in pp reactions at $\\sqrt{s}$ = 7 TeV", "ALICE", null, "2320574", "1805.12455", null, null, ["CERN-EP-2018-150"]], "1672792": ["Dielectron production in proton-proton collisions at $ \\sqrt{s}=7 $ TeV", "ALICE", "10.1007/JHEP09(2018)064", "2316031", "1805.04391", "ins1672792", null, ["CERN-EP-2018-102"]], "1666817": ["Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at $ \\sqrt{s_{\\mathrm{NN}}}=5.02 $ and 2.76 TeV", "ALICE", "10.1007/JHEP07(2018)103", "2310570", "1804.02944", "ins1666817", null, ["CERN-EP-2018-057"]], "1680638": ["Measurement of dielectron production in central Pb-Pb collisions at $\\sqrt{{\\textit{s}}_{\\mathrm{NN}}}$ = 2.76 TeV", "ALICE", null, "2625083", "1807.00923", null, null, ["CERN-EP-2018-181"]], "1672798": ["$\\Upsilon$ suppression at forward rapidity in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV", "ALICE", null, "2316306", "1805.04387", null, null, ["CERN-EP-2018-114"]], "1672812": ["Azimuthal anisotropy of heavy-flavour decay electrons in p-Pb collisions at $ \\sqrt{s_{\\rm NN}}$ = 5.02 TeV", "ALICE", null, "2316782", "1805.04367", null, null, ["CERN-EP-2018-119"]], "1672811": ["Measurements of low-$p_{\\rm T}$ electrons from semileptonic heavy-flavour hadron decays at mid-rapidity in pp and Pb-Pb collisions at $\\mathbf{\\sqrt{{\\it s}_\\mathrm{NN}}}$ = 2.76 TeV", "ALICE", null, "2315859", "1805.04379", "ins1672811", null, ["CERN-EP-2018-095"]], "1682990": ["Medium modification of the shape of small-radius jets in central Pb-Pb collisions at $\\sqrt{s_{\\mathrm {NN}}} = 2.76\\,\\rm{TeV}$", "ALICE", null, "2630402", "1807.06854", null, null, ["CERN-EP-2018-201"]], "1649235": ["Neutral pion and $\\eta$ meson production in p-Pb collisions at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV", "ALICE", "10.1140/epjc/s10052-018-6013-8", "2299472", "1801.07051", "ins1649235", null, []], "1684320": ["Multiplicity dependence of light-flavor hadron production in pp collisions at $\\sqrt{s}$ = 7 TeV", "ALICE", null, "2632051", "1807.11321", null, null, ["CERN-EP-2018-209"]], "1672765": ["Two particle differential transverse momentum and number density correlations in p-Pb and Pb-Pb at the LHC", "ALICE", null, "2316778", "1805.04422", null, null, ["CERN-EP-2018-118"]], "1696315": ["$\\Lambda_\\mathrm{c}^+$ production in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV", "ALICE", null, "2639229", "1809.10922", null, null, ["CERN-EP-2018-261"]], "1672790": ["Transverse momentum spectra and nuclear modification factors of charged particles in Xe-Xe collisions at $\\sqrt{s_{\\rm NN}}$ = 5.44 TeV", "ALICE", null, "2316249", "1805.04399", null, null, ["CERN-EP-2018-112"]], "1672788": ["Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\\sqrt{s_{\\rm NN}}$ = 13 TeV", "ALICE", null, "2316934", "1805.04407", null, null, ["CERN-EP-2018-122"]], "1662651": ["Neutral pion and $\\eta$ meson production at mid-rapidity in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 2.76 TeV", "ALICE", null, "2307650", "1803.05490", "ins1662651", null, []], "1657384": ["Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC", "ALICE", null, "2304800", "1802.09145", null, null, []], "1695028": ["Measuring K$^0_{\\rm S}$K$^{\\rm{\\pm}}$ interactions using pp collisions at $\\sqrt{s}=7$ TeV", "ALICE", null, "2636148", "1809.07899", null, null, ["CERN-EP-2018-234"]], "1664312": ["Direct photon production at low transverse momentum in proton-proton collisions at $\\mathbf{\\sqrt{s}=2.76}$ and 8 TeV", "ALICE", null, "2308256", "1803.09857", null, null, []], "1669819": ["Measurement of D$^0$, D$^+$, D$^{*+}$ and D$^+_{\\rm s}$ production in Pb-Pb collisions at $\\mathbf{\\sqrt{s_{\\rm NN}}}= 5.02$ TeV", "ALICE", null, "2311747", "1804.09083", null, null, ["CERN-EP-2018-066"]], "1669805": ["$\\phi$ meson production at forward rapidity in Pb-Pb collisions at $\\sqrt{s_\\mathrm{NN}}=2.76$ TeV", "ALICE", "10.1140/epjc/s10052-018-6034-3", "2314216", "1804.08906", "ins1669805", null, ["CERN-EP-2018-082"]], "1672884": ["Particle identification studies with a full-size 4-GEM prototype for the ALICE TPC upgrade", "ALICE TPC", "10.1016/j.nima.2018.06.084", "2622276", "1805.03234", null, null, []], "1695334": ["Event-shape engineering for the D-meson elliptic flow in mid-central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} =5.02$ TeV", "ALICE", null, "2638995", "1809.09371", null, null, ["CERN-EP-2018-260"]], "1672800": ["Inclusive J/$\\psi$ production in Xe\u2013Xe collisions at $\\sqrt{s_{\\rm NN}}$ = 5.44 TeV", "ALICE", "10.1016/j.physletb.2018.08.047", "2316136", "1805.04383", "ins1672800", null, ["CERN-EP-2018-107"]], "1672822": ["Anisotropic flow of identified particles in Pb-Pb collisions at $ {\\sqrt{s}}_{\\mathrm{NN}}=5.02 $ TeV", "ALICE", "10.1007/JHEP09(2018)006", "2316069", "1805.04390", "ins1672822", null, ["CERN-EP-2018-103"]], "1672807": ["Inclusive J/$\\psi$ production at forward and backward rapidity in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV", "ALICE", "10.1007/JHEP07(2018)160", "2316010", "1805.04381", "ins1672807", null, ["CERN-EP-2018-101"]], "1672806": ["Suppression of $\\Lambda(1520)$ resonance production in central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 2.76 TeV", "ALICE", null, "2316371", "1805.04361", "ins1672806", null, ["CERN-EP-2018-116"]], "1672860": ["Production of the $\\rho$(770)${^{0}}$ meson in pp and Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 2.76 TeV", "ALICE", null, "2316135", "1805.04365", null, null, ["CERN-EP-2018-106"]], "1672801": ["Measurement of the inclusive J/ $\\psi $ polarization at forward rapidity in pp collisions at $\\mathbf {\\sqrt{s} = 8}$ \u00a0TeV", "ALICE", "10.1140/epjc/s10052-018-6027-2", "2315951", "1805.04374", "ins1672801", null, ["CERN-EP-2018-098"]], "1671792": ["Anisotropic flow in Xe-Xe collisions at $\\mathbf{\\sqrt{s_{\\rm{NN}}} = 5.44}$ TeV", "ALICE", "10.1016/j.physletb.2018.06.059", "2315558", "1805.01832", "ins1671792", null, ["CERN-EP-2018-090"]], "1664538": ["Azimuthally-differential pion femtoscopy relative to the third harmonic event plane in Pb-Pb collisions at $\\mathbf{\\sqrt{\\textit{s}_{_{\\rm NN}}}}$ = 2.76 TeV", "ALICE", "10.1016/j.physletb.2018.06.042", "2306302", "1803.10594", null, null, []], "1652829": ["Prompt and non-prompt $\\hbox {J}/\\psi $ production and nuclear modification at mid-rapidity in p\u2013Pb collisions at $\\mathbf{\\sqrt{{ s}_{\\text {NN}}}= 5.02}$ \u00a0TeV", "ALICE", "10.1140/epjc/s10052-018-5881-2", "2302066", "1802.00765", "ins1652829", null, []], "1672789": ["Direct photon elliptic flow in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 2.76 TeV", "ALICE", null, "2316393", "1805.04403", null, null, ["CERN-EP-2018-117"]]}
\ No newline at end of file
+{"1693305": ["Energy dependence of exclusive $J/\\psi$ photoproduction off protons in ultra-peripheral p-Pb collisions at $\\sqrt{s_{\\rm{NN}}}$ = 5.02 TeV", "ALICE", null, "2636152", "1809.03235", null, null, ["CERN-EP-2018-236"]], "1672944": ["Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV", "ALICE", null, "2316322", "1805.05212", null, null, ["CERN-EP-2018-115"]], "1672756": ["Centrality and pseudorapidity dependence of the charged-particle multiplicity density in Xe-Xe collisions at $\\sqrt{s_{\\rm NN}}$ = 5.44 TeV", "ALICE", null, "2316786", "1805.04432", null, null, ["CERN-EP-2018-120"]], "1693308": ["Charged jet cross section and fragmentation in proton-proton collisions at $\\sqrt{s}$ = 7 TeV", "ALICE", null, "2636150", "1809.03232", null, null, ["CERN-EP-2018-235"]], "1672807": ["Inclusive J/$\\psi$ production at forward and backward rapidity in p-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 8.16 TeV", "ALICE", "10.1007/JHEP07(2018)160", "2316010", "1805.04381", "ins1672807", null, ["CERN-EP-2018-101"]], "1675759": ["p-p, p-$\\Lambda$ and $\\Lambda$-$\\Lambda$ correlations studied via femtoscopy in pp reactions at $\\sqrt{s}$ = 7 TeV", "ALICE", null, "2320574", "1805.12455", null, null, ["CERN-EP-2018-150"]], "1672792": ["Dielectron production in proton-proton collisions at $ \\sqrt{s}=7 $ TeV", "ALICE", "10.1007/JHEP09(2018)064", "2316031", "1805.04391", "ins1672792", null, ["CERN-EP-2018-102"]], "1666817": ["Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at $ \\sqrt{s_{\\mathrm{NN}}}=5.02 $ and 2.76 TeV", "ALICE", "10.1007/JHEP07(2018)103", "2310570", "1804.02944", "ins1666817", null, ["CERN-EP-2018-057"]], "1680638": ["Measurement of dielectron production in central Pb-Pb collisions at $\\sqrt{{\\textit{s}}_{\\mathrm{NN}}}$ = 2.76 TeV", "ALICE", null, "2625083", "1807.00923", null, null, ["CERN-EP-2018-181"]], "1672798": ["$\\Upsilon$ suppression at forward rapidity in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 5.02 TeV", "ALICE", null, "2316306", "1805.04387", null, null, ["CERN-EP-2018-114"]], "1672812": ["Azimuthal anisotropy of heavy-flavour decay electrons in p-Pb collisions at $ \\sqrt{s_{\\rm NN}}$ = 5.02 TeV", "ALICE", null, "2316782", "1805.04367", null, null, ["CERN-EP-2018-119"]], "1672811": ["Measurements of low-p$_{T}$ electrons from semileptonic heavy-flavour hadron decays at mid-rapidity in pp and Pb-Pb collisions at $ \\sqrt{s_{\\mathrm{NN}}}=2.76 $ TeV", "ALICE", "10.1007/JHEP10(2018)061", "2315859", "1805.04379", "ins1672811", null, ["CERN-EP-2018-095"]], "1682990": ["Medium modification of the shape of small-radius jets in central Pb-Pb collisions at $\\sqrt{s_{\\mathrm {NN}}} = 2.76\\,\\rm{TeV}$", "ALICE", "10.1007/JHEP10(2018)139", "2630402", "1807.06854", null, null, ["CERN-EP-2018-201"]], "1672806": ["Suppression of $\\Lambda(1520)$ resonance production in central Pb-Pb collisions at $\\sqrt{s_{\\rm NN}}$ = 2.76 TeV", "ALICE", null, "2316371", "1805.04361", "ins1672806", null, ["CERN-EP-2018-116"]], "1649235": ["Neutral pion and $\\eta$ meson production in p-Pb collisions at $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV", "ALICE", "10.1140/epjc/s10052-018-6013-8", "2299472", "1801.07051", "ins1649235", null, []], "1684320": ["Multiplicity dependence of light-flavor hadron production in pp collisions at $\\sqrt{s}$ = 7 TeV", "ALICE", null, "2632051", "1807.11321", null, null, ["CERN-EP-2018-209"]], "1672765": ["Two particle differential transverse momentum and number density correlations in p-Pb and Pb-Pb at the LHC", "ALICE", null, "2316778", "1805.04422", null, null, ["CERN-EP-2018-118"]], "1696315": ["$\\Lambda_\\mathrm{c}^+$ production in Pb-Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV", "ALICE", null, "2639229", "1809.10922", null, null, ["CERN-EP-2018-261"]], "1672790": ["Transverse momentum spectra and nuclear modification factors of charged particles in Xe-Xe collisions at $\\sqrt{s_{\\rm NN}}$ = 5.44 TeV", "ALICE", "10.1016/j.physletb.2018.10.052", "2316249", "1805.04399", "ins1672790", null, ["CERN-EP-2018-112"]], "1672788": ["Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\\sqrt{s_{\\rm NN}}$ = 13 TeV", "ALICE", "10.1016/j.physletb.2018.11.009", "2316934", "1805.04407", "ins1672788", null, ["CERN-EP-2018-122"]], "1662651": ["Neutral pion and $\\eta$ meson production at mid-rapidity in Pb-Pb collisions at $\\sqrt{s_{NN}}$ = 2.76 TeV", "ALICE", "10.1103/PhysRevC.98.044901", "2307650", "1803.05490", "ins1662651", null, []], "1657384": ["Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC", "ALICE", "10.1007/JHEP11(2018)013", "2304800", "1802.09145", null, null, []], "1695028": ["Measuring K$^0_{\\rm S}$K$^{\\rm{\\pm}}$ interactions using pp collisions at $\\sqrt{s}=7$ TeV", "ALICE", null, "2636148", "1809.07899", null, null, ["CERN-EP-2018-234"]], "1664312": ["Direct photon production at low transverse momentum in proton-proton collisions at $\\mathbf{\\sqrt{s}=2.76}$ and 8 TeV", "ALICE", null, "2308256", "1803.09857", null, null, []], "1669819": ["Measurement of D$^{0}$, D$^{+}$, D$^{*+}$ and D$_{s}^{+}$ production in Pb-Pb collisions at $ \\sqrt{{\\mathrm{s}}_{\\mathrm{NN}}}=5.02 $ TeV", "ALICE", "10.1007/JHEP10(2018)174", "2311747", "1804.09083", null, null, ["CERN-EP-2018-066"]], "1669805": ["$\\phi$ meson production at forward rapidity in Pb-Pb collisions at $\\sqrt{s_\\mathrm{NN}}=2.76$ TeV", "ALICE", "10.1140/epjc/s10052-018-6034-3", "2314216", "1804.08906", "ins1669805", null, ["CERN-EP-2018-082"]], "1672884": ["Particle identification studies with a full-size 4-GEM prototype for the ALICE TPC upgrade", "ALICE TPC", "10.1016/j.nima.2018.06.084", "2622276", "1805.03234", null, null, []], "1704923": ["Jet fragmentation transverse momentum measurements from di-hadron correlations in $\\sqrt{s}$ = 7 TeV pp and $\\sqrt{s_{\\rm{NN}}}$ = 5.02 TeV 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diff --git a/doc/inspire-atlas-2018.json b/doc/inspire-atlas-2018.json
--- a/doc/inspire-atlas-2018.json
+++ b/doc/inspire-atlas-2018.json
@@ -1,1 +1,1 @@
-{"1676481": ["Search for pair production of heavy vector-like quarks decaying into high-$p_T$ $W$ bosons and top quarks in the lepton-plus-jets final state in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1007/JHEP08(2018)048", "2621963", "1806.01762", "ins1676481", null, ["CERN-EP-2018-088"]], "1653453": ["Search for a Structure in the $B^0_s \\pi^\\pm$ Invariant Mass Spectrum with the ATLAS Experiment", "ATLAS", "10.1103/PhysRevLett.120.202007", "2302747", "1802.01840", null, null, []], "1686834": ["Measurement of the azimuthal anisotropy of charged particles produced in $\\sqrt{s_\\mathrm{NN}} = 5.02$ TeV Pb+Pb collisions with the ATLAS detector", "ATLAS", null, "2634051", "1808.03951", null, null, ["CERN-EP-2018-194"]], "1683827": ["In situ calibration of large-$R$ jet energy and mass in 13 TeV proton-proton collisions with the ATLAS detector", "ATLAS", null, "2632341", "1807.09477", null, null, ["CERN-EP-2018-191"]], "1686832": ["Search for heavy charged long-lived particles in proton-proton collisions at $\\sqrt{s} = 13$ TeV using an ionisation measurement with the ATLAS detector", "ATLAS", null, "2634050", "1808.04095", "ins1686832", null, ["CERN-EP-2018-198"]], "1691822": ["Measurements of gluon-gluon fusion and vector-boson fusion Higgs boson production cross-sections in the $H \\to WW^{\\ast} \\to e\\nu\\mu\\nu$ decay channel in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", null, "2636382", "1808.09054", null, null, ["CERN-EP-2018-212"]], "1684216": ["Search for vector-boson resonances decaying to a top quark and bottom quark in the lepton plus jets final state in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", null, "2632527", "1807.10473", "ins1684216", null, ["CERN-EP-2018-142"]], "1674946": ["Combined measurement of differential and total cross sections in the $H \\rightarrow \\gamma \\gamma$ and the $H \\rightarrow ZZ^* \\rightarrow 4\\ell$ decay channels at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.09.019", "2320499", "1805.10197", "ins1674946", null, ["CERN-EP-2018-080"]], "1691634": ["Observation of $H \\rightarrow b\\bar{b}$ decays and $VH$ production with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.09.013", "2636066", "1808.08238", null, null, ["CERN-EP-2018-215"]], "1672147": ["Measurement of colour flow using jet-pull observables in $t\\bar{t}$ events with the ATLAS experiment at $\\sqrt{s} = 13$ TeV", "ATLAS", null, "2316982", "1805.02935", null, null, ["CERN-EP-2018-041"]], "1654582": ["Measurements of Higgs boson properties in the diphoton decay channel with 36 fb$^{-1}$ of $pp$ collision data at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.052005", "2302492", "1802.04146", null, null, ["CERN-EP-2017-288"]], "1668124": ["Search for pair production of Higgs bosons in the $b\\bar{b}b\\bar{b}$ final state using proton-proton collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", null, "2313703", "1804.06174", "ins1668124", null, ["CERN-EP-2018-029"]], "1680462": ["Searches for exclusive Higgs and $Z$ boson decays into $J/\\psi\\gamma$, $\\psi(2S)\\gamma$, and $\\Upsilon(nS)\\gamma$ at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.09.024", "2628217", "1807.00802", null, null, ["CERN-EP-2018-154"]], "1690929": ["Performance of top-quark and $W$-boson tagging with ATLAS in Run 2 of the LHC", "ATLAS", null, "2635896", "1808.07858", null, null, ["CERN-EP-2018-192"]], "1673177": ["Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevC.98.024908", "2318279", "1805.05424", null, null, ["CERN-EP-2018-096"]], "1658902": ["Search for electroweak production of supersymmetric particles in final states with two or three leptons at $\\sqrt{s}=13\\,$TeV with the ATLAS detector", "ATLAS", null, "2307399", "1803.02762", "ins1658902", null, ["CERN-EP-2017-303"]], "1677498": ["Probing the quantum interference between singly and doubly resonant top-quark production in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", null, "2623971", "1806.04667", null, null, []], "1682785": ["Search for lepton-flavor violation in different-flavor, high-mass final states in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", null, "2631602", "1807.06573", null, null, ["CERN-EP-2018-137"]], "1676078": ["Measurement of the Higgs boson mass in the $H\\rightarrow ZZ^* \\rightarrow 4\\ell$ and $H \\rightarrow \\gamma\\gamma$ channels with $\\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.07.050", "2621113", "1806.00242", null, null, ["CERN-EP-2018-085"]], "1667045": ["Search for supersymmetry in events with four or more leptons in $\\sqrt{s}=13$ TeV $pp$ collisions with ATLAS", "ATLAS", "10.1103/PhysRevD.98.032009", "2312374", "1804.03602", "ins1667045", null, ["CERN-EP-2017-300"]], "1675352": ["Search for new phenomena using the invariant mass distribution of same-flavour opposite-sign dilepton pairs in events with missing transverse momentum in $\\sqrt{s}=13$ \u00a0 $\\text {Te}\\text {V}$ pp collisions with the ATLAS detector", "ATLAS", "10.1140/epjc/s10052-018-6081-9", "2320693", "1805.11381", "ins1675352", null, ["CERN-EP-2018-053"]], "1672957": ["Measurement of the suppression and azimuthal anisotropy of muons from heavy-flavor decays in Pb+Pb collisions at $\\sqrt{s_{\\mathrm{NN}}} = 2.76$ TeV with the ATLAS detector", "ATLAS", null, "2318293", "1805.05220", null, null, ["CERN-EP-2018-072"]], "1664317": ["Search for pair production of up-type vector-like quarks and for four-top-quark events in final states with multiple $b$-jets with the ATLAS detector", "ATLAS", "10.1007/JHEP07(2018)089", "2310460", "1803.09678", null, null, ["CERN-EP-2018-031"]], "1676472": ["Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", null, "2621727", "1806.01532", "ins1676472", null, ["CERN-EP-2018-077"]], "1684645": ["A search for resonant and non-resonant Higgs boson pair production in the ${b\\bar{b}\\tau^+\\tau^-}$ decay channel in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", null, "2632994", "1808.00336", "ins1684645", null, ["CERN-EP-2018-164"]], "1682295": ["Prompt and non-prompt $J/\\psi$ elliptic flow in Pb+Pb collisions at $\\sqrt{s_{_\\text{NN}}} = 5.02$ TeV with the ATLAS detector", "ATLAS", "10.1140/epjc/s10052-018-6243-9", "2630897", "1807.05198", null, null, ["CERN-EP-2018-170"]], "1696805": ["Measurement of the top quark mass in the $t\\bar{t}\\to$ lepton+jets channel from $\\sqrt{s}=8$ TeV ATLAS data and combination with previous results", "ATLAS", null, null, "1810.01772", null, null, ["CERN Preprint ID: CERN-EP-2018-238"]], "1685418": ["Search for doubly charged scalar bosons decaying into same-sign $W$ boson pairs with the ATLAS detector", "ATLAS", null, "2633369", "1808.01899", null, null, ["CERN-EP-2018-188"]], "1667040": ["Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in $pp$ collisions at $\\sqrt{s}=13$ TeV", "ATLAS", "10.1103/PhysRevLett.121.081801", "2312376", "1804.03496", "ins1667040", null, ["CERN-EP-2018-033"]], "1683114": ["A strategy for a general search for new phenomena using data-derived signal regions and its application within the ATLAS experiment", "ATLAS", null, "2631806", "1807.07447", null, null, ["CERN-EP-2018-070"]], "1694476": ["Search for invisible Higgs boson decays in vector boson fusion at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", null, "2638994", "1809.06682", null, null, ["CERN-EP-2018-184"]], "1671810": ["Measurements of b-jet tagging efficiency with the ATLAS detector using $ t\\overline{t} $ events at $ \\sqrt{s}=13 $ TeV", "ATLAS", "10.1007/JHEP08(2018)089", "2316380", "1805.01845", null, null, ["CERN-EP-2018-047"]], "1665234": ["Search for Higgs boson decays into pairs of light (pseudo)scalar particles in the $\\gamma\\gamma jj$ final state in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.06.011", "2310780", "1803.11145", null, null, []], "1670803": ["Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton\u2013proton collisions at $\\sqrt{s} = 13$ \u00a0 $\\text {TeV}$ with the ATLAS detector", "ATLAS", "10.1140/epjc/s10052-018-5995-6", "2315706", "1804.10823", null, null, ["CERN-EP-2018-48", "CERN-EP-2018-048"]], "1683331": ["Search for charged Higgs bosons decaying via $H^{\\pm} \\to \\tau^{\\pm}\\nu_{\\tau}$ in the $\\tau$+jets and $\\tau$+lepton final states with 36 fb$^{-1}$ of $pp$ collision data recorded at $\\sqrt{s} = 13$ TeV with the ATLAS experiment", "ATLAS", "10.1007/JHEP09(2018)139", "2631950", "1807.07915", "ins1683331", null, ["CERN-EP-2018-148"]], "1650152": ["Search for $W' \\rightarrow tb$ decays in the hadronic final state using pp collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.03.036", "2302089", "1801.07893", "ins1650152", null, []], "1658490": ["Production and Integration of the ATLAS Insertable B-Layer", "ATLAS IBL", "10.1088/1748-0221/13/05/T05008", "2307576", "1803.00844", null, null, []], "1679959": ["Search for pair- and single-production of vector-like quarks in final states with at least one $Z$ boson decaying into a pair of electrons or muons in $pp$ collision data collected with the ATLAS detector at $\\sqrt{s} = 13$ TeV", "ATLAS", null, "2626965", "1806.10555", null, null, ["CERN-EP-2018-145"]], "1676179": ["Observation of Higgs boson production in association with a top quark pair at the LHC with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.07.035", "2621167", "1806.00425", null, null, ["CERN-EP-2018-138"]], "1676551": ["Search for chargino-neutralino production using recursive jigsaw reconstruction in final states with two or three charged leptons in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", null, "2622094", "1806.02293", "ins1676551", null, ["CERN-EP-2018-113"]], "1685058": ["Constraints on off-shell Higgs boson production and the Higgs boson total width in $ZZ\\to4\\ell$ and $ZZ\\to2\\ell2\\nu$ final states with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.09.048", "2633244", "1808.01191", null, null, ["CERN-EP-2018-178"]], "1654357": ["Search for photonic signatures of gauge-mediated supersymmetry in 13\u00a0TeV $pp$ collisions with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.97.092006", "2303558", "1802.03158", "ins1654357", null, []], "1692387": ["A search for pairs of highly collimated photon-jets in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", null, "2636769", "1808.10515", null, null, ["CERN-EP-2018-143"]], "1672010": ["Search for heavy resonances decaying to a photon and a hadronically decaying $Z/W/H$ boson in $pp$ collisions at $\\sqrt{s}=13$ $\\mathrm{TeV}$ with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.032015", "2316379", "1805.01908", "ins1672010", null, ["CERN-EP-2018-055"]], "1679217": ["Observation of centrality-dependent acoplanarity for muon pairs produced via two-photon scattering in Pb+Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}=5.02$ TeV with the ATLAS detector", "ATLAS", null, "2625324", "1806.08708", null, null, ["CERN-EP-2018-100"]], "1649273": ["Search for High-Mass Resonances Decaying to $\\tau\\nu$ in pp Collisions at $\\sqrt{s}$=13\u2009\u2009TeV with the ATLAS Detector", "ATLAS", "10.1103/PhysRevLett.120.161802", "2301691", "1801.06992", "ins1649273", null, []], "1677389": ["Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\\sqrt{s} = 13$ TeV $pp$ collisions using the ATLAS detector", "ATLAS", null, "2622693", "1806.04030", null, null, []], "1650592": ["Search for light resonances decaying to boosted quark pairs and produced in association with a photon or a jet in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", null, "2302092", "1801.08769", null, null, []], "1684341": ["Search for dark matter in events with a hadronically decaying vector boson and missing transverse momentum in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", null, "2632806", "1807.11471", "ins1684341", null, ["CERN-EP-2018-083"]], "1696330": ["Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with two charged leptons and two jets at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", null, "2641297", "1809.11105", "ins1696330", null, []], "1678484": ["Search for the Higgs boson produced in association with a vector boson and decaying into two spin-zero particles in the $H \\rightarrow aa \\rightarrow 4b$ channel in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", null, "2624918", "1806.07355", null, null, ["CERN-EP-2018-128"]], "1682345": ["Search for Higgs boson pair production in the $\\gamma\\gamma b\\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment", "ATLAS", null, "2630823", "1807.04873", "ins1682345", null, ["CERN-EP-2018-130"]], "1680457": ["Search for Higgs boson decays into a pair of light bosons in the $bb\\mu\\mu$ final state in $pp$ collision at $\\sqrt{s} = $13 TeV with the ATLAS detector", "ATLAS", null, "2628120", "1807.00539", null, null, ["CERN-EP-2018-153"]], "1667046": ["Search for R-parity-violating supersymmetric particles in multi-jet final states produced in $p$-$p$ collisions at $\\sqrt{s} =13$ TeV using the ATLAS detector at the LHC", "ATLAS", "10.1016/j.physletb.2018.08.021", "2312375", "1804.03568", null, null, ["CERN-EP-2017-298"]], "1665828": ["Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\\ell\\ell bb$ final state in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.07.006", "2311387", "1804.01126", "ins1665828", null, ["CERN-EP-2018-030"]], "1654372": ["Search for Higgs boson decays to beyond-the-Standard-Model light bosons in four-lepton events with the ATLAS detector at $\\sqrt{s}=13$ TeV", "ATLAS", "10.1007/JHEP06(2018)166", "2304159", "1802.03388", null, null, []], "1672469": ["Prompt and non-prompt $J/\\psi $ and $\\psi (2\\mathrm {S})$ suppression at high transverse momentum in $5.02~\\mathrm {TeV}$ Pb+Pb collisions with the ATLAS experiment", "ATLAS", "10.1140/epjc/s10052-018-6219-9", "2317228", "1805.04077", null, null, ["CERN-EP-2018-049"]], "1672099": ["Search for supersymmetry in final states with charm jets and missing transverse momentum in 13 TeV $pp$ collisions with the ATLAS detector", "ATLAS", "10.1007/JHEP09(2018)050", "2316225", "1805.01649", "ins1672099", null, ["CERN-EP-2018-034"]], "1664486": ["Search for top squarks decaying to tau sleptons in $pp$ collisions at $\\sqrt{s}= 13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.032008", "2310589", "1803.10178", "ins1664486", null, ["CERN-EP-2018-024"]], "1684489": ["Search for new phenomena in events with same-charge leptons and $b$-jets in $pp$ collisions at $\\sqrt{s}= 13$ TeV with the ATLAS detector", "ATLAS", null, "2632923", "1807.11883", "ins1684489", null, ["CERN-EP-2018-171"]], "1672883": ["Search for flavor-changing neutral currents in top quark decays $t\\to Hc$ and $t \\to Hu$ in multilepton final states in proton-proton collisions at $\\sqrt{s}= 13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.032002", "2317118", "1805.03483", null, null, ["CERN-EP-2018-067"]], "1673184": ["Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\\sqrt{s_\\mathrm{NN}}=5.02$ TeV with the ATLAS 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using the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.012003", "2299430", "1801.02052", "ins1646686", ["ATLAS_2018_I1646686"], ["CERN-EP-2017-226"]], "1676554": ["Operation and performance of the ATLAS Tile Calorimeter in Run 1", "ATLAS", null, "2622093", "1806.02129", null, null, ["CERN-EP-2018-062"]], "1672475": ["Angular analysis of $B^0_d \\rightarrow K^{*}\\mu^+\\mu^-$ decays in $pp$ collisions at $\\sqrt{s}= 8$ TeV with the ATLAS detector", "ATLAS", null, "2317227", "1805.04000", null, null, ["CERN-EP-2017-161"]], "1683431": ["Search for Higgs boson pair production in the $\\gamma\\gamma WW^{*}$ channel using $pp$ collision data recorded at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", null, "2632142", "1807.08567", null, null, ["CERN-EP-2018-104"]], "1674532": ["Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.032016", "2319920", "1805.09299", "ins1674532", null, ["CERN-EP-2018-075"]], "1686365": ["Search for charged Higgs bosons decaying into top and bottom quarks at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", null, "2634037", "1808.03599", null, null, ["CERN-EP-2018-168"]], "1654814": ["Search for the Decay of the Higgs Boson to Charm Quarks with the ATLAS Experiment", "ATLAS", "10.1103/PhysRevLett.120.211802", "2304413", "1802.04329", null, null, []], "1685421": ["Combination of the searches for pair-produced vector-like partners of the third-generation quarks at $\\sqrt{s} =$ 13 TeV with the ATLAS detector", "ATLAS", null, "2633568", "1808.02343", "ins1685421", null, ["CERN-EP-2018-205"]], "1685420": ["Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.052008", "2633569", "1808.02380", null, null, ["CERN-EP-2018-179"]], "1688943": ["Search for squarks and gluinos in final states with hadronically decaying $\\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", null, "2634894", "1808.06358", "ins1688943", null, ["CERN-EP-2018-185"]], "1672961": ["Measurement of dijet azimuthal decorrelations in $pp$ collisions at $\\sqrt{s}=8$ TeV with the ATLAS detector and determination of the strong coupling", "ATLAS", null, "2318117", "1805.04691", null, null, ["CERN-EP-2017-282"]], "1685207": ["Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", null, "2633505", "1808.01771", "ins1685207", null, ["CERN-EP-2018-176"]], "1664332": ["Search for flavour-changing neutral current top-quark decays $t\\to qZ$ in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1007/JHEP07(2018)176", "2310281", "1803.09923", null, null, ["CERN-EP-2018-018"]], "1685997": ["Search for long-lived particles in final states with displaced dimuon vertices in $pp$ collisions at $\\sqrt{s}=$ 13 TeV with the ATLAS detector", "ATLAS", null, "2633725", "1808.03057", null, null, ["CERN-EP-2018-173"]], "1656834": ["Performance of missing transverse momentum reconstruction with the ATLAS detector using proton-proton collisions at $\\sqrt{s}$ = 13 TeV", "ATLAS", null, "2305380", "1802.08168", null, null, ["CERN-EP-2017-274"]], "1670020": ["A search for lepton-flavor-violating decays of the $Z$ boson into a $\\tau$-lepton and a light lepton with the ATLAS detector", "ATLAS", null, "2315063", "1804.09568", null, null, ["CERN-EP-2018-052"]], "1656578": ["Measurements of differential cross sections of top quark pair production in association with jets in ${pp}$ collisions at $\\sqrt{s}=13$ TeV using the ATLAS detector", "ATLAS", null, "2304924", "1802.06572", "ins1656578", null, []]}
\ No newline at end of file
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["CERN-EP-2018-198"]], "1658490": ["Production and Integration of the ATLAS Insertable B-Layer", "ATLAS IBL", "10.1088/1748-0221/13/05/T05008", "2307576", "1803.00844", null, null, []], "1684216": ["Search for vector-boson resonances decaying to a top quark and bottom quark in the lepton plus jets final state in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.11.032", "2632527", "1807.10473", "ins1684216", null, ["CERN-EP-2018-142"]], "1674946": ["Combined measurement of differential and total cross sections in the $H \\rightarrow \\gamma \\gamma$ and the $H \\rightarrow ZZ^* \\rightarrow 4\\ell$ decay channels at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.09.019", "2320499", "1805.10197", "ins1674946", null, ["CERN-EP-2018-080"]], "1654582": ["Measurements of Higgs boson properties in the diphoton decay channel with 36 fb$^{-1}$ of $pp$ collision data at $\\sqrt{s} = 13$ TeV with the ATLAS 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decays $t\\to qZ$ in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1007/JHEP07(2018)176", "2310281", "1803.09923", null, null, ["CERN-EP-2018-018"]], "1692387": ["A search for pairs of highly collimated photon-jets in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", null, "2636769", "1808.10515", null, null, ["CERN-EP-2018-143"]], "1670020": ["A search for lepton-flavor-violating decays of the $Z$ boson into a $\\tau$-lepton and a light lepton with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.092010", "2315063", "1804.09568", null, null, ["CERN-EP-2018-052"]], "1707015": ["Measurements of inclusive and differential fiducial cross-sections of $t\\bar{t}\\gamma$ production in leptonic final states at $\\sqrt{s}$ = 13 TeV in ATLAS", "ATLAS", null, null, "1812.01697", null, null, ["CERN-EP-2018-302"]], "1694678": ["Measurement of photon-jet transverse momentum correlations in 5.02 TeV Pb+Pb and $pp$ collisions with 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searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.052008", "2633569", "1808.02380", null, null, ["CERN-EP-2018-179"]], "1702261": ["Search for the production of a long-lived neutral particle decaying within the ATLAS hadronic calorimeter in association with a $Z$ boson from $pp$ collisions at $\\sqrt{s} = 13$ TeV", "ATLAS", null, "2646156", "1811.02542", "ins1702261", null, ["CERN-EP-2018-275"]], "1702263": ["Search for four-top-quark production in the single-lepton and opposite-sign dilepton final states in pp collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", null, "2646128", "1811.02305", null, null, ["CERN-EP-2018-174"]], "1682785": ["Search for lepton-flavor violation in different-flavor, high-mass final states in $pp$ collisions at $\\sqrt s=13\u2009$\u2009TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.092008", "2631602", "1807.06573", null, null, ["CERN-EP-2018-137"]], "1664317": ["Search for pair production of up-type vector-like quarks and for four-top-quark events in final states with multiple $b$-jets with the ATLAS detector", "ATLAS", "10.1007/JHEP07(2018)089", "2310460", "1803.09678", null, null, ["CERN-EP-2018-031"]], "1670803": ["Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton\u2013proton collisions at $\\sqrt{s} = 13$ \u00a0 $\\text {TeV}$ with the ATLAS detector", "ATLAS", "10.1140/epjc/s10052-018-5995-6", "2315706", "1804.10823", null, null, ["CERN-EP-2018-48", "CERN-EP-2018-048"]], "1679217": ["Observation of centrality-dependent acoplanarity for muon pairs produced via two-photon scattering in Pb+Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}=5.02$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevLett.121.212301", "2625324", "1806.08708", null, null, ["CERN-EP-2018-100"]], "1650152": ["Search for $W' \\rightarrow tb$ decays in the hadronic final state using pp collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.03.036", "2302089", "1801.07893", "ins1650152", null, []], "1696330": ["Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with two charged leptons and two jets at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", null, "2640802", "1809.11105", "ins1696330", null, ["CERN-EP-2018-199"]], "1682345": ["Search for Higgs boson pair production in the $\\gamma\\gamma b\\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment", "ATLAS", "10.1007/JHEP11(2018)040", "2630823", "1807.04873", "ins1682345", null, ["CERN-EP-2018-130"]], "1697671": ["Comparison between simulated and observed LHC beam backgrounds in the ATLAS experiment at ${E_{\\textrm {beam}}}$ = 4 TeV", "ATLAS", "10.1088/1748-0221/13/12/P12006", "2643265", "1810.04450", null, null, ["CERN-EP-2018-240"]], "1664486": ["Search for top squarks decaying to tau sleptons in $pp$ collisions at $\\sqrt{s}= 13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.032008", "2310589", "1803.10178", "ins1664486", null, ["CERN-EP-2018-024"]], "1656578": ["Measurements of differential cross sections of top quark pair production in association with jets in ${pp}$ collisions at $\\sqrt{s}=13$ TeV using the ATLAS detector", "ATLAS", "10.1007/JHEP10(2018)159", "2304924", "1802.06572", "ins1656578", ["ATLAS_2018_I1656578"], ["CERN-EP-2017-227"]], "1674532": ["Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.032016", "2319920", "1805.09299", "ins1674532", null, ["CERN-EP-2018-075"]], "1686365": ["Search for charged Higgs bosons decaying into top and bottom quarks at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", "10.1007/JHEP11(2018)085", "2634037", "1808.03599", "ins1686365", null, ["CERN-EP-2018-168"]], "1656834": ["Performance of missing transverse momentum reconstruction with the ATLAS detector using proton-proton collisions at $\\sqrt{s}$ = 13 TeV", "ATLAS", "10.1140/epjc/s10052-018-6288-9", "2305380", "1802.08168", null, null, ["CERN-EP-2017-274"]], "1676481": ["Search for pair production of heavy vector-like quarks decaying into high-$p_T$ $W$ bosons and top quarks in the lepton-plus-jets final state in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1007/JHEP08(2018)048", "2621963", "1806.01762", "ins1676481", null, ["CERN-EP-2018-088"]], "1683827": ["In situ calibration of large-$R$ jet energy and mass in 13 TeV proton-proton collisions with the ATLAS detector", "ATLAS", null, "2632341", "1807.09477", null, null, ["CERN-EP-2018-191"]], "1654357": ["Search for photonic signatures of gauge-mediated supersymmetry in 13\u00a0TeV $pp$ collisions with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.97.092006", "2303558", "1802.03158", "ins1654357", null, []], "1682295": ["Prompt and non-prompt $J/\\psi $ elliptic flow in Pb+Pb collisions at $\\sqrt{s_{_\\text {NN}}} = 5.02$ Tev with the ATLAS detector", "ATLAS", "10.1140/epjc/s10052-018-6243-9", "2630897", "1807.05198", null, null, ["CERN-EP-2018-170"]], "1698025": ["Measurement of the photon identification efficiencies with the ATLAS detector using LHC Run 2 data collected in 2015 and 2016", "ATLAS", null, "2643391", "1810.05087", null, null, ["CERN-EP-2018-216"]], "1680462": ["Searches for exclusive Higgs and $Z$ boson decays into $J/\\psi\\gamma$, $\\psi(2S)\\gamma$, and $\\Upsilon(nS)\\gamma$ at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.09.024", "2628217", "1807.00802", null, null, ["CERN-EP-2018-154"]], "1658902": ["Search for electroweak production of supersymmetric particles in final states with two or three leptons at $\\sqrt{s}=13\\,$TeV 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"ATLAS", null, "2633369", "1808.01899", null, null, ["CERN-EP-2018-188"]], "1654814": ["Search for the Decay of the Higgs Boson to Charm Quarks with the ATLAS Experiment", "ATLAS", "10.1103/PhysRevLett.120.211802", "2304413", "1802.04329", null, null, []], "1671810": ["Measurements of b-jet tagging efficiency with the ATLAS detector using $ t\\overline{t} $ events at $ \\sqrt{s}=13 $ TeV", "ATLAS", "10.1007/JHEP08(2018)089", "2316380", "1805.01845", null, null, ["CERN-EP-2018-047"]], "1679959": ["Search for pair- and single-production of vector-like quarks in final states with at least one $Z$ boson decaying into a pair of electrons or muons in $pp$ collision data collected with the ATLAS detector at $\\sqrt{s} = 13$ TeV", "ATLAS", null, "2626965", "1806.10555", null, null, ["CERN-EP-2018-145"]], "1677389": ["Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\\sqrt{s} = 13$ TeV $pp$ collisions using the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.092002", "2622693", "1806.04030", "ins1677389", null, ["CERN-EP-2018-050"]], "1678484": ["Search for the Higgs boson produced in association with a vector boson and decaying into two spin-zero particles in the $H \\rightarrow aa \\rightarrow 4b$ channel in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", "10.1007/JHEP10(2018)031", "2624918", "1806.07355", null, null, ["CERN-EP-2018-128"]], "1654372": ["Search for Higgs boson decays to beyond-the-Standard-Model light bosons in four-lepton events with the ATLAS detector at $\\sqrt{s}=13$ TeV", "ATLAS", "10.1007/JHEP06(2018)166", "2304159", "1802.03388", null, null, []], "1672099": ["Search for supersymmetry in final states with charm jets and missing transverse momentum in 13 TeV $pp$ collisions with the ATLAS detector", "ATLAS", "10.1007/JHEP09(2018)050", "2316225", "1805.01649", "ins1672099", null, ["CERN-EP-2018-034"]], "1684489": ["Search for new phenomena in events with same-charge leptons and $b$-jets in $pp$ collisions at $\\sqrt{s}= 13$ TeV with the ATLAS detector", "ATLAS", null, "2632923", "1807.11883", "ins1684489", null, ["CERN-EP-2018-171"]], "1672883": ["Search for flavor-changing neutral currents in top quark decays $t\\to Hc$ and $t \\to Hu$ in multilepton final states in proton-proton collisions at $\\sqrt{s}= 13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.032002", "2317118", "1805.03483", null, null, ["CERN-EP-2018-067"]], "1649273": ["Search for High-Mass Resonances Decaying to $\\tau\\nu$ in pp Collisions at $\\sqrt{s}$=13\u2009\u2009TeV with the ATLAS Detector", "ATLAS", "10.1103/PhysRevLett.120.161802", "2301691", "1801.06992", "ins1649273", null, []], "1683434": ["Search for Higgs bosons produced via vector-boson fusion and decaying into bottom quark pairs in $\\sqrt{s} = 13$ $\\mathrm{TeV}$ $pp$ collisions with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.052003", "2632158", "1807.08639", null, null, ["CERN-EP-2018-140"]], "1646686": ["Measurements of $t\\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\\sqrt{s}=13\\,$ TeV using the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.012003", "2299430", "1801.02052", "ins1646686", ["ATLAS_2018_I1646686"], ["CERN-EP-2017-226"]], "1683431": ["Search for Higgs boson pair production in the $\\gamma\\gamma WW^{*}$ channel using $pp$ collision data recorded at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", null, "2632142", "1807.08567", "ins1683431", null, ["CERN-EP-2018-104"]], "1685421": ["Combination of the searches for pair-produced vector-like partners of the third-generation quarks at $\\sqrt{s} =$ 13 TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevLett.121.211801", "2633568", "1808.02343", "ins1685421", null, ["CERN-EP-2018-205"]], "1668124": ["Search for pair production of Higgs bosons in the $b\\bar{b}b\\bar{b}$ final state using proton-proton collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", null, "2313703", "1804.06174", "ins1668124", null, ["CERN-EP-2018-029"]], "1688943": ["Search for squarks and gluinos in final states with hadronically decaying $\\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", null, "2634894", "1808.06358", "ins1688943", null, ["CERN-EP-2018-185"]], "1704495": ["Cross-section measurements of the Higgs boson decaying into a pair of $\\tau$-leptons in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", null, "2648520", "1811.08856", null, null, ["CERN-EP-2018-232"]], "1691822": ["Measurements of gluon-gluon fusion and vector-boson fusion Higgs boson production cross-sections in the $H \\to WW^{\\ast} \\to e\\nu\\mu\\nu$ decay channel in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", null, "2636382", "1808.09054", null, null, ["CERN-EP-2018-212"]], "1672147": ["Measurement of colour flow using jet-pull observables in $t\\bar{t}$ events with the ATLAS experiment at $\\sqrt{s} = 13\\,\\hbox {TeV}$", "ATLAS", "10.1140/epjc/s10052-018-6290-2", "2316982", "1805.02935", null, null, ["CERN-EP-2018-041"]], "1698006": ["Measurement of the $Z\\gamma\\rightarrow\\nu\\bar{\\nu}\\gamma$ production cross section in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector and limits on anomalous triple gauge-boson couplings", "ATLAS", null, "2643440", "1810.04995", null, null, ["CERN-EP-2018-220"]], "1673177": ["Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevC.98.024908", "2318279", "1805.05424", null, null, ["CERN-EP-2018-096"]], "1705857": ["Measurements of fiducial and differential cross-sections of $t\\bar{t}$ production with additional heavy-flavour jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector", "ATLAS", null, "2649375", "1811.12113", null, null, ["CERN-EP-2018-276"]], "1675352": ["Search for new phenomena using the invariant mass distribution of same-flavour opposite-sign dilepton pairs in events with missing transverse momentum in $\\sqrt{s}=13$ \u00a0 $\\text {Te}\\text {V}$ pp collisions with the ATLAS detector", "ATLAS", "10.1140/epjc/s10052-018-6081-9", "2320693", "1805.11381", "ins1675352", null, ["CERN-EP-2018-053"]], "1672957": ["Measurement of the suppression and azimuthal anisotropy of muons from heavy-flavor decays in Pb+Pb collisions at $\\sqrt{s_{\\mathrm{NN}}} = 2.76$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevC.98.044905", "2318293", "1805.05220", null, null, ["CERN-EP-2018-072"]], "1684645": ["Search for Resonant and Nonresonant Higgs Boson Pair Production in the ${b\\bar{b}\\tau^+\\tau^-}$ Decay Channel in $pp$ Collisions at $\\sqrt{s}=13$\u2009\u2009TeV with the ATLAS Detector", "ATLAS", "10.1103/PhysRevLett.121.191801", "2632994", "1808.00336", "ins1684645", null, ["CERN-EP-2018-164"]], "1705395": ["Study of the hard double-parton scattering contribution to inclusive four-lepton production in $pp$ collisions at $\\sqrt{s}$ = 8 TeV with the ATLAS detector", "ATLAS", null, "2649192", "1811.11094", null, null, ["CERN-EP-2018-274"]], "1705396": ["Search for Higgs boson pair production in the $WW^{(*)}WW^{(*)}$ decay channel using ATLAS data recorded at $\\sqrt{s}=13$ TeV", "ATLAS", null, "2649134", "1811.11028", null, null, ["CERN-EP-2018-227"]], "1683114": ["A strategy for a general search for new phenomena using data-derived signal regions and its application within the ATLAS experiment", "ATLAS", null, "2631806", "1807.07447", null, null, ["CERN-EP-2018-070"]], "1694476": ["Search for invisible Higgs boson decays in vector boson fusion at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", null, "2638994", "1809.06682", null, null, ["CERN-EP-2018-184"]], "1672010": ["Search for heavy resonances decaying to a photon and a hadronically decaying $Z/W/H$ boson in $pp$ collisions at $\\sqrt{s}=13$ $\\mathrm{TeV}$ with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.032015", "2316379", "1805.01908", "ins1672010", null, ["CERN-EP-2018-055"]], "1676554": ["Operation and performance of the ATLAS Tile Calorimeter in Run\u00a01", "ATLAS", "10.1140/epjc/s10052-018-6374-z", "2622093", "1806.02129", null, null, ["CERN-EP-2018-062"]], "1676551": ["Search for chargino-neutralino production using recursive jigsaw reconstruction in final states with two or three charged leptons in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.092012", "2622094", "1806.02293", "ins1676551", null, ["CERN-EP-2018-113"]], "1685058": ["Constraints on off-shell Higgs boson production and the Higgs boson total width in $ZZ\\to4\\ell$ and $ZZ\\to2\\ell2\\nu$ final states with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.09.048", "2633244", "1808.01191", null, null, ["CERN-EP-2018-178"]], "1650592": ["Search for light resonances decaying to boosted quark pairs and produced in association with a photon or a jet in proton-proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.09.062", "2302092", "1801.08769", null, null, ["CERN-EP-2017-280"]], "1684341": ["Search for dark matter in events with a hadronically decaying vector boson and missing transverse momentum in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", "10.1007/JHEP10(2018)180", "2632806", "1807.11471", "ins1684341", null, ["CERN-EP-2018-083"]], "1672469": ["Prompt and non-prompt $J/\\psi $ and $\\psi (2\\mathrm {S})$ suppression at high transverse momentum in $5.02~\\mathrm {TeV}$ Pb+Pb collisions with the ATLAS experiment", "ATLAS", "10.1140/epjc/s10052-018-6219-9", "2317228", "1805.04077", null, null, ["CERN-EP-2018-049"]], "1667046": ["Search for R-parity-violating supersymmetric particles in multi-jet final states produced in $p$-$p$ collisions at $\\sqrt{s} =13$ TeV using the ATLAS detector at the LHC", "ATLAS", "10.1016/j.physletb.2018.08.021", "2312375", "1804.03568", null, null, ["CERN-EP-2017-298"]], "1667045": ["Search for supersymmetry in events with four or more leptons in $\\sqrt{s}=13$ TeV $pp$ collisions with ATLAS", "ATLAS", "10.1103/PhysRevD.98.032009", "2312374", "1804.03602", "ins1667045", null, ["CERN-EP-2017-300"]], "1673184": ["Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\\sqrt{s_\\mathrm{NN}}=5.02$ TeV with the ATLAS detector", "ATLAS", null, "2318295", "1805.05635", "ins1673184", null, ["CERN-EP-2018-105"]], "1667040": ["Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in $pp$ collisions at $\\sqrt{s}=13$ TeV", "ATLAS", "10.1103/PhysRevLett.121.081801", "2312376", "1804.03496", "ins1667040", null, ["CERN-EP-2018-033"]], "1665828": ["Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\\ell\\ell bb$ final state in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector", "ATLAS", "10.1016/j.physletb.2018.07.006", "2311387", "1804.01126", "ins1665828", null, ["CERN-EP-2018-030"]], "1685207": ["Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector", "ATLAS", "10.1103/PhysRevD.98.092005", "2633505", "1808.01771", "ins1685207", null, ["CERN-EP-2018-176"]], "1685997": ["Search for long-lived particles in final states with displaced dimuon vertices in $pp$ collisions at $\\sqrt{s}=$ 13 TeV with the ATLAS detector", "ATLAS", null, "2633725", "1808.03057", null, null, ["CERN-EP-2018-173"]], "1704138": ["Search for long-lived particles produced in $pp$ collisions at $\\sqrt{s}=13$ TeV that decay into displaced hadronic jets in the ATLAS muon spectrometer", "ATLAS", null, "2647833", "1811.07370", "ins1704138", null, ["CERN-EP-2018-241"]]}
\ No newline at end of file
diff --git a/doc/inspire-atlas-2018.marc.xml b/doc/inspire-atlas-2018.marc.xml
--- a/doc/inspire-atlas-2018.marc.xml
+++ b/doc/inspire-atlas-2018.marc.xml
@@ -1,3580 +1,4311 @@
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["Search for Low Mass Vector Resonances Decaying to Quark-Antiquark Pairs in Proton-Proton Collisions at $\\sqrt{s}=13\\text{ }\\text{ }\\mathrm{TeV}$", "CMS", "10.1103/PhysRevLett.119.111802", "2266573", "1705.10532", null, null, ["CMS-EXO-16-030", "CERN-EP-2017-098"]], "1613900": ["Observation of the Higgs boson decay to a pair of $\\tau$ leptons with the CMS detector", "CMS", "10.1016/j.physletb.2018.02.004", "2276465", "1708.00373", null, null, ["CMS-HIG-16-043", "CERN-EP-2017-181"]], "1620050": ["Measurement of normalized differential $ \\mathrm{t}\\overline{\\mathrm{t}} $ cross sections in the dilepton channel from pp collisions at $ \\sqrt{s}=13 $ TeV", "CMS", "10.1007/JHEP04(2018)060", "2280888", "1708.07638", null, null, ["CMS-TOP-16-007", "CERN-EP-2017-120"]], "1620205": ["Search for Evidence of the Type-III Seesaw Mechanism in Multilepton Final States in Proton-Proton Collisions at $\\sqrt{s}=13\\text{ }\\text{ }\\mathrm{TeV}$", "CMS", "10.1103/PhysRevLett.119.221802", 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\ No newline at end of file
diff --git a/doc/inspire-cms-2018.json b/doc/inspire-cms-2018.json
--- a/doc/inspire-cms-2018.json
+++ b/doc/inspire-cms-2018.json
@@ -1,1 +1,1 @@
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["Charged-particle nuclear modification factors in XeXe collisions at $ \\sqrt{s_{\\mathrm{NN}}} = 5.44 $ TeV", "CMS", "10.1007/JHEP10(2018)138", "2636844", "1809.00201", null, null, ["CMS-HIN-18-004", "CERN-EP-2018-228"]], "1677677": ["Search for dark matter produced in association with a Higgs boson decaying to $\\gamma\\gamma$ or $\\tau^+\\tau^-$ at $\\sqrt{s} =$ 13 TeV", "CMS", "10.1007/JHEP09(2018)046", "2623974", "1806.04771", null, null, ["CMS-EXO-16-055", "CERN-EP-2018-129"]], "1693412": ["Performance of reconstruction and identification of $\\tau$ leptons decaying to hadrons and $\\nu_\\tau$ in pp collisions at $\\sqrt{s}=$ 13 TeV", "CMS", "10.1088/1748-0221/13/10/P10005", "2637646", "1809.02816", null, null, ["CMS-TAU-16-003", "CERN-EP-2018-229"]], "1677275": ["Search for a singly produced third-generation scalar leptoquark decaying to a $\\tau$ lepton and a bottom quark in proton-proton collisions at $\\sqrt{s} =$ 13 TeV", "CMS", "10.1007/JHEP07(2018)115", "2622479", 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["Search for pair production of second-generation leptoquarks at $\\sqrt{s}=$ 13 TeV", "CMS", null, "2634349", "1808.05082", null, null, ["CMS-EXO-17-003", "CERN-EP-2018-218"]], "1682495": ["Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at $ \\sqrt{s}=13 $ TeV", "CMS", "10.1007/JHEP11(2018)113", "2631525", "1807.05974", "ins1682495", ["CMS_2018_I1682495"], ["CMS-SMP-16-010", "CERN-EP-2018-180"]], "1697571": ["Measurement of B$^0_\\mathrm{s}$ meson production in pp and PbPb collisions at $\\sqrt{s_\\mathrm{NN}} =$ 5.02 TeV", "CMS", null, "2642213", "1810.03022", null, null, ["CMS-HIN-17-008", "CERN-EP-2018-257"]], "1655968": ["Search for narrow resonances in the b-tagged dijet mass spectrum in proton-proton collisions at $\\sqrt{s} =$ 8 TeV", "CMS", "10.1103/PhysRevLett.120.201801", "2304884", "1802.06149", null, null, ["CMS-EXO-16-057", "CERN-EP-2018-007"]], "1654926": ["Measurement of the $\\Lambda_b$ 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null, ["CMS-SMP-16-015", "CERN-EP-2018-071"]], "1653451": ["Search for natural and split supersymmetry in proton-proton collisions at $ \\sqrt{s}=13 $ TeV in final states with jets and missing transverse momentum", "CMS", "10.1007/JHEP05(2018)025", "2303202", "1802.02110", null, null, ["CMS-SUS-16-038", "CERN-EP-2018-003"]], "1700575": ["Studies of beauty suppression via nonprompt D$^0$ mesons in PbPb collisions at $\\sqrt{s_\\mathrm{NN}}=$ 5.02 TeV", "CMS", null, "2645047", "1810.11102", null, null, ["CMS-HIN-16-016", "CERN-EP-2018-264"]], "1702163": ["Search for pair production of first-generation scalar leptoquarks at $\\sqrt{s}=$ 13 TeV", "CMS", null, "2645910", "1811.01197", null, null, ["CMS-EXO-17-009", "CERN-EP-2018-265"]], "1662081": ["Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at $ \\sqrt{s}=13 $ TeV", "CMS", "10.1007/JHEP06(2018)002", "2308090", "1803.03991", null, 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resonant production of second-generation sleptons with same-sign dimuon events in proton-proton collisions at $\\sqrt{s} =$ 13 TeV", "CMS", null, "2648887", "1811.09760", null, null, ["CMS-SUS-17-008", "CERN-EP-2018-297"]], "1665226": ["Search for a heavy right-handed W boson and a heavy neutrino in events with two same-flavor leptons and two jets at $\\sqrt{s}=$ 13 TeV", "CMS", "10.1007/JHEP05(2018)148", "2310971", "1803.11116", null, null, ["CMS-EXO-17-011", "CERN-EP-2018-028"]], "1647947": ["Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at $\\sqrt{s} =$ 13 TeV", "CMS", "10.1007/JHEP03(2018)160", "2299904", "1801.03957", null, null, ["CMS-SUS-17-004", "CERN-EP-2017-283"]], "1680318": ["Measurement of charged particle spectra in minimum-bias events from proton\u2013proton collisions at $\\sqrt{s}=13\\,\\text {TeV} $", "CMS", "10.1140/epjc/s10052-018-6144-y", "2627556", "1806.11245", "ins1680318", ["CMS_2018_I1680318"], 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resonances in final states with a lepton and missing transverse momentum at $ \\sqrt{s}=13 $ TeV", "CMS", "10.1007/JHEP06(2018)128", "2310972", "1803.11133", null, null, ["CMS-EXO-16-033", "CERN-EP-2018-020"]], "1697570": ["Search for top quark partners with charge 5/3 in the same-sign dilepton and single-lepton final states in proton-proton collisions at $\\sqrt{s} =$ 13 TeV", "CMS", null, "2642373", "1810.03188", null, null, ["CMS-B2G-17-014", "CERN-EP-2018-258"]], "1696402": ["Fast timing measurement for CMS RPC Phase-II upgrade", "CMS", "10.1088/1748-0221/13/09/C09001", null, null, null, null, []], "1662083": ["Search for a heavy resonance decaying into a Z boson and a vector boson in the $ \\nu \\overline{\\nu}\\mathrm{q}\\overline{\\mathrm{q}} $ final state", "CMS", "10.1007/JHEP07(2018)075", "2308045", "1803.03838", null, null, ["CMS-B2G-17-005", "CERN-EP-2018-023"]], "1656983": ["Quality control for the first large areas of triple-GEM chambers for the CMS endcaps", "CMS", 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diff --git a/doc/inspire-lhcb-2018.marc.xml b/doc/inspire-lhcb-2018.marc.xml
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diff --git a/doc/inspire-star-2018.json b/doc/inspire-star-2018.json
--- a/doc/inspire-star-2018.json
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+{"1672453": ["$J/\\psi$ production cross section and its dependence on charged-particle multiplicity in $p+p$ collisions at $\\sqrt{s}$ = 200 GeV", "STAR", "10.1016/j.physletb.2018.09.029", null, "1805.03745", null, null, []], "1685527": ["The Proton-$\\Omega$ correlation function in Au+Au collisions at $\\sqrt{s_{NN}}$=200 GeV", "STAR", null, null, "1808.02511", null, null, []], "1672785": ["Global polarization of $\\Lambda$ hyperons in Au+Au collisions at $\\sqrt{s_{_{NN}}}$ = 200 GeV", "STAR", "10.1103/PhysRevC.98.014910", null, "1805.04400", null, null, []], "1700232": ["Measurements of Dielectron Production in Au$+$Au Collisions at $\\sqrt{s_{NN}}$= 27, 39, and 62.4 GeV from the STAR Experiment", "STAR", null, null, "1810.10159", null, null, []], "1691152": ["Improved measurement of the longitudinal spin transfer to $\\Lambda$ and $\\bar \\Lambda$ hyperons in polarized proton-proton collisions at $\\sqrt s$ = 200 GeV", "STAR", null, null, "1808.07634", null, null, []], "1674826": ["Longitudinal Double-Spin Asymmetries for $\\pi^{0}$s in the Forward Direction for 510 GeV Polarized $pp$ Collisions", "STAR", "10.1103/PhysRevD.98.032013", null, "1805.09745", null, null, []], "1691271": ["Transverse spin transfer to $\\Lambda$ and $\\bar{\\Lambda}$ hyperons in polarized proton-proton collisions at $\\sqrt{s}=200\\,\\mathrm{GeV}$", "STAR", "10.1103/PhysRevD.98.091103", null, "1808.08000", null, null, []], "1674714": ["Longitudinal double-spin asymmetries for dijet production at intermediate pseudorapidity in polarized $pp$ collisions at $\\sqrt{s}=$ 200\u2009\u2009GeV", "STAR", "10.1103/PhysRevD.98.032011", null, "1805.09742", null, null, []], "1662057": ["Correlation Measurements Between Flow Harmonics in Au+Au Collisions at RHIC", "STAR", "10.1016/j.physletb.2018.05.076", null, "1803.03876", null, null, []], "1676541": ["Low-$p_T$ $e^{+}e^{-}$ pair production in Au$+$Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV and U$+$U collisions at $\\sqrt{s_{NN}}$ = 193 GeV at STAR", "STAR", "10.1103/PhysRevLett.121.132301", null, "1806.02295", null, null, []], "1669807": ["Beam energy dependence of rapidity-even dipolar flow in Au+Au collisions", "STAR", "10.1016/j.physletb.2018.07.013", null, "1804.08647", null, null, []]}
\ No newline at end of file
diff --git a/doc/inspire-star-2018.marc.xml b/doc/inspire-star-2018.marc.xml
--- a/doc/inspire-star-2018.marc.xml
+++ b/doc/inspire-star-2018.marc.xml
@@ -1,320 +1,351 @@
<?xml version="1.0" encoding="UTF-8"?>
-<!-- Search-Engine-Total-Number-Of-Results: 10 -->
+<!-- Search-Engine-Total-Number-Of-Results: 11 -->
<collection xmlns="http://www.loc.gov/MARC21/slim">
<record>
+ <controlfield tag="001">1700232</controlfield>
+ <datafield tag="035" ind1=" " ind2=" ">
+ <subfield code="9">INSPIRETeX</subfield>
+ <subfield code="a">Adam:2018qev</subfield>
+ </datafield>
+ <datafield tag="035" ind1=" " ind2=" ">
+ <subfield code="9">arXiv</subfield>
+ <subfield code="a">oai:arXiv.org:1810.10159</subfield>
+ </datafield>
+ <datafield tag="035" ind1=" " ind2=" ">
+ <subfield code="9">DESY</subfield>
+ <subfield code="z">D18-kj45a</subfield>
+ </datafield>
+ <datafield tag="037" ind1=" " ind2=" ">
+ <subfield code="9">arXiv</subfield>
+ <subfield code="a">arXiv:1810.10159</subfield>
+ <subfield code="c">nucl-ex</subfield>
+ </datafield>
+ <datafield tag="245" ind1=" " ind2=" ">
+ <subfield code="9">arXiv</subfield>
+ <subfield code="a">Measurements of Dielectron Production in Au$+$Au Collisions at $\sqrt{s_{NN}}$= 27, 39, and 62.4 GeV from the STAR Experiment</subfield>
+ </datafield>
+ <datafield tag="710" ind1=" " ind2=" ">
+ <subfield code="g">STAR</subfield>
+ </datafield>
+</record>
+<record>
<controlfield tag="001">1691271</controlfield>
+ <datafield tag="024" ind1="7" ind2=" ">
+ <subfield code="2">DOI</subfield>
+ <subfield code="a">10.1103/PhysRevD.98.091103</subfield>
+ </datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">INSPIRETeX</subfield>
<subfield code="a">Adam:2018wce</subfield>
</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
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</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">DESY</subfield>
<subfield code="z">D18-kj36o</subfield>
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<datafield tag="037" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">arXiv:1808.08000</subfield>
<subfield code="c">hep-ex</subfield>
</datafield>
<datafield tag="245" ind1=" " ind2=" ">
- <subfield code="9">arXiv</subfield>
+ <subfield code="9">APS</subfield>
<subfield code="a">Transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ hyperons in polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$</subfield>
</datafield>
<datafield tag="710" ind1=" " ind2=" ">
<subfield code="g">STAR</subfield>
</datafield>
</record>
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<subfield code="9">INSPIRETeX</subfield>
<subfield code="a">Adam:2018kzl</subfield>
</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">oai:arXiv.org:1808.07634</subfield>
</datafield>
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<subfield code="9">DESY</subfield>
<subfield code="z">D18-kj35n</subfield>
</datafield>
<datafield tag="037" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">arXiv:1808.07634</subfield>
<subfield code="c">hep-ex</subfield>
</datafield>
<datafield tag="245" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">Improved measurement of the longitudinal spin transfer to $\Lambda$ and $\bar \Lambda$ hyperons in polarized proton-proton collisions at $\sqrt s$ = 200 GeV</subfield>
</datafield>
<datafield tag="710" ind1=" " ind2=" ">
<subfield code="g">STAR</subfield>
</datafield>
</record>
<record>
<controlfield tag="001">1685527</controlfield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">INSPIRETeX</subfield>
<subfield code="a">STAR:2018uho</subfield>
</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">oai:arXiv.org:1808.02511</subfield>
</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">DESY</subfield>
<subfield code="z">D18-kj33h</subfield>
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<subfield code="9">arXiv</subfield>
<subfield code="a">arXiv:1808.02511</subfield>
<subfield code="c">hep-ex</subfield>
</datafield>
<datafield tag="245" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">The Proton-$\Omega$ correlation function in Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV</subfield>
</datafield>
<datafield tag="710" ind1=" " ind2=" ">
<subfield code="g">STAR</subfield>
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<controlfield tag="001">1676541</controlfield>
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<subfield code="2">DOI</subfield>
<subfield code="9">arXiv</subfield>
<subfield code="a">10.1103/PhysRevLett.121.132301</subfield>
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<subfield code="a">Adam:2018tdm</subfield>
</datafield>
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<subfield code="9">arXiv</subfield>
<subfield code="a">oai:arXiv.org:1806.02295</subfield>
</datafield>
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<subfield code="9">DESY</subfield>
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<subfield code="9">arXiv</subfield>
<subfield code="a">arXiv:1806.02295</subfield>
<subfield code="c">hep-ex</subfield>
</datafield>
<datafield tag="245" ind1=" " ind2=" ">
- <subfield code="9">arXiv</subfield>
+ <subfield code="9">APS</subfield>
<subfield code="a">Low-$p_T$ $e^{+}e^{-}$ pair production in Au$+$Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U$+$U collisions at $\sqrt{s_{NN}}$ = 193 GeV at STAR</subfield>
</datafield>
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<subfield code="a">10.1103/PhysRevD.98.032013</subfield>
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<datafield tag="024" ind1="7" ind2=" ">
<subfield code="2">DOI</subfield>
<subfield code="9">arXiv</subfield>
<subfield code="a">10.1103/PhysRevD.98.032013</subfield>
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<subfield code="a">Adam:2018cto</subfield>
</datafield>
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<subfield code="a">oai:arXiv.org:1805.09745</subfield>
</datafield>
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<subfield code="9">arXiv</subfield>
<subfield code="a">arXiv:1805.09745</subfield>
<subfield code="c">hep-ex</subfield>
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<subfield code="9">APS</subfield>
<subfield code="a">Longitudinal Double-Spin Asymmetries for $\pi^{0}$s in the Forward Direction for 510 GeV Polarized $pp$ Collisions</subfield>
</datafield>
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<subfield code="g">STAR</subfield>
</datafield>
</record>
<record>
<controlfield tag="001">1674714</controlfield>
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<subfield code="2">DOI</subfield>
<subfield code="a">10.1103/PhysRevD.98.032011</subfield>
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<subfield code="2">DOI</subfield>
<subfield code="9">arXiv</subfield>
<subfield code="a">10.1103/PhysRevD.98.032011</subfield>
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<subfield code="a">Adam:2018pns</subfield>
</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">oai:arXiv.org:1805.09742</subfield>
</datafield>
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<subfield code="9">DESY</subfield>
<subfield code="z">D18-kj22k</subfield>
</datafield>
<datafield tag="037" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">arXiv:1805.09742</subfield>
<subfield code="c">hep-ex</subfield>
</datafield>
<datafield tag="245" ind1=" " ind2=" ">
<subfield code="9">APS</subfield>
<subfield code="a">Longitudinal double-spin asymmetries for dijet production at intermediate pseudorapidity in polarized $pp$ collisions at $\sqrt{s}=$ 200  GeV</subfield>
</datafield>
<datafield tag="710" ind1=" " ind2=" ">
<subfield code="g">STAR</subfield>
</datafield>
</record>
<record>
<controlfield tag="001">1672785</controlfield>
<datafield tag="024" ind1="7" ind2=" ">
<subfield code="2">DOI</subfield>
<subfield code="a">10.1103/PhysRevC.98.014910</subfield>
</datafield>
<datafield tag="024" ind1="7" ind2=" ">
<subfield code="2">DOI</subfield>
<subfield code="9">arXiv</subfield>
<subfield code="a">10.1103/PhysRevC.98.014910</subfield>
<subfield code="q">publication</subfield>
</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">INSPIRETeX</subfield>
<subfield code="a">Adam:2018ivw</subfield>
</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">oai:arXiv.org:1805.04400</subfield>
</datafield>
<datafield tag="037" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">arXiv:1805.04400</subfield>
<subfield code="c">nucl-ex</subfield>
</datafield>
<datafield tag="245" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">Global polarization of $\Lambda$ hyperons in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV</subfield>
</datafield>
<datafield tag="710" ind1=" " ind2=" ">
<subfield code="g">STAR</subfield>
</datafield>
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<controlfield tag="001">1672453</controlfield>
<datafield tag="024" ind1="7" ind2=" ">
<subfield code="2">DOI</subfield>
<subfield code="9">bibmatch</subfield>
<subfield code="a">10.1016/j.physletb.2018.09.029</subfield>
</datafield>
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<subfield code="9">INSPIRETeX</subfield>
<subfield code="a">Adam:2018jmp</subfield>
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<subfield code="9">arXiv</subfield>
<subfield code="a">oai:arXiv.org:1805.03745</subfield>
</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">DESY</subfield>
<subfield code="z">D18-kj20j</subfield>
</datafield>
<datafield tag="037" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">arXiv:1805.03745</subfield>
<subfield code="c">hep-ex</subfield>
</datafield>
<datafield tag="245" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">$J/\psi$ production cross section and its dependence on charged-particle multiplicity in $p+p$ collisions at $\sqrt{s}$ = 200 GeV</subfield>
</datafield>
<datafield tag="245" ind1=" " ind2=" ">
<subfield code="9">Elsevier</subfield>
<subfield code="a">$J/\psi$ production cross section and its dependence on charged-particle multiplicity in $p  +  p$ collisions at $\sqrt{s}$ = 200 GeV</subfield>
</datafield>
<datafield tag="710" ind1=" " ind2=" ">
<subfield code="g">STAR</subfield>
</datafield>
</record>
<record>
<controlfield tag="001">1669807</controlfield>
<datafield tag="024" ind1="7" ind2=" ">
<subfield code="2">DOI</subfield>
<subfield code="9">arXiv</subfield>
<subfield code="a">10.1016/j.physletb.2018.07.013</subfield>
<subfield code="q">publication</subfield>
</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">INSPIRETeX</subfield>
<subfield code="a">Star:2018zpt</subfield>
</datafield>
<datafield tag="035" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">oai:arXiv.org:1804.08647</subfield>
</datafield>
<datafield tag="037" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">arXiv:1804.08647</subfield>
<subfield code="c">nucl-ex</subfield>
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<datafield tag="245" ind1=" " ind2=" ">
<subfield code="9">arXiv</subfield>
<subfield code="a">Beam energy dependence of rapidity-even dipolar flow in Au+Au collisions</subfield>
</datafield>
<datafield tag="710" ind1=" " ind2=" ">
<subfield code="g">STAR</subfield>
</datafield>
</record>
<record>
<controlfield tag="001">1662057</controlfield>
<datafield tag="024" ind1="7" ind2=" ">
<subfield code="2">DOI</subfield>
<subfield code="9">bibmatch</subfield>
<subfield code="a">10.1016/j.physletb.2018.05.076</subfield>
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<subfield code="9">INSPIRETeX</subfield>
<subfield code="a">STAR:2018fpo</subfield>
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<subfield code="9">arXiv</subfield>
<subfield code="a">oai:arXiv.org:1803.03876</subfield>
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<subfield code="9">arXiv</subfield>
<subfield code="a">arXiv:1803.03876</subfield>
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<subfield code="9">arXiv</subfield>
<subfield code="a">Correlation Measurements Between Flow Harmonics in Au+Au Collisions at RHIC</subfield>
</datafield>
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</record>
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\ No newline at end of file
diff --git a/doc/mk-coverage-html b/doc/mk-coverage-html
--- a/doc/mk-coverage-html
+++ b/doc/mk-coverage-html
@@ -1,392 +1,395 @@
#! /usr/bin/env python
from __future__ import division, print_function
"""\
%prog <file.json> [<file.json> ...]
TODO:
- do Rivet lookup in this script, not the JSON-maker
- get and write year of publication in table
"""
import argparse
ap = argparse.ArgumentParser(usage=__doc__)
ap.add_argument("JSONFILES", metavar="file", nargs="+",
help="JSON Inspire xref file to read")
ap.add_argument("-r", "--ranking", dest="RANKFILES", metavar="file", action="append", default=[],
help="lists of Inspire IDs to exclude, suppress, and highlight")
ap.add_argument("-R", "--reverse", dest="REVERSE", action="store_true", default=False,
help="show list *reverse* ordered in Inspire ID")
ap.add_argument("-s", "--only-searches", dest="ONLYSEARCHES", action="store_true", default=False,
help="only show search analyses")
ap.add_argument("-S", "--no-searches", dest="NOSEARCHES", action="store_true", default=False,
help="exclude search analyses")
ap.add_argument("-i", "--only-heavyion", dest="ONLYHEAVYION", action="store_true", default=False,
help="only show heavy ion analyses")
ap.add_argument("-I", "--no-heavyion", dest="NOHEAVYION", action="store_true", default=False,
help="exclude heavy ion analyses")
ap.add_argument("-o", "--outfile", dest="OUTFILE", default=None,
help="output HTML filename")
ap.add_argument("--basename", dest="BASENAME", default="rivet-coverage",
help="the base name for output files [default=%(default)s]")
ap.add_argument("--update-ranking", dest="UPDATERANK", action="store_true", default=False,
help="update the per-experiment ranking files")
ap.add_argument("-v", "--verbose", dest="VERBOSE", action="store_true", default=False,
help="print debug info to the terminal")
args = ap.parse_args()
import datetime
now = datetime.datetime.now()
EXPTS = ["ALICE", "ATLAS", "CMS", "LHCb", "Other"]
## Add the rivet Python module build dir(s) to the Python module path, then import
import os, sys, re
pybuild = os.path.abspath(os.path.join(os.getcwd(), "..", "pyext", "build"))
pydirs = [os.path.join(pybuild, d) for d in os.listdir(pybuild)
if re.match(r"lib\..*-.*-%d\.%d" % (sys.version_info[0], sys.version_info[1]), d)]
sys.path = pydirs + sys.path
import rivet
## Add info file locations
from glob import glob
dirpatt = os.path.join(os.getcwd(), "..", "analyses", "plugin*")
for d in glob(dirpatt):
#print(d)
rivet.addAnalysisDataPath(os.path.abspath(d))
## Rivet analyses to cross-reference
ranas = {}
for aname in rivet.AnalysisLoader.analysisNames():
ana = rivet.AnalysisLoader.getAnalysis(aname)
# TODO: all anas *should* have an Inspire ID...
try:
# print(aname, ":", ana.inspireId(), ":")
ranas.setdefault(int(ana.inspireId()), []).append(ana.name())
except:
pass
## Read data from JSON files
records = {}
import json
for jsonfile in args.JSONFILES:
with open(jsonfile) as jf:
recs = json.load(jf)
if args.VERBOSE:
print("Reading {} records from {}".format(len(recs), jsonfile))
records.update(recs)
records = {int(k) : v for k, v in records.items()}
if args.VERBOSE:
print("Read total of {} records".format(len(records)))
## Read Inspire IDs from ranking files
blacklist, greylist, hotlist = [], [], []
assigned = {}
for rankfilestr in args.RANKFILES:
for rankfile in rankfilestr.split(" "):
with open(rankfile) as rf:
if args.VERBOSE:
print("Reading rankings from {}".format(rankfile))
for line in rf:
line = line.strip()
if not line or line.startswith("#"):
continue
tokens = line.split()
ins = int(tokens[0])
code = tokens[1]
if code == "X":
blacklist.append(ins)
elif code == "?":
greylist.append(ins)
elif code == "!":
hotlist.append(ins)
# Detect an optional assigned email address
last = tokens[-1]
if "@" in last:
if last.startswith("<") and last.endswith(">"):
last = last[1:-1]
assigned[ins] = last
## Add rankings/tags to the record
for ins, rec in records.items():
## Sanitise title and experiment
rec[0] = (rec[0] or "[NO TITLE]").replace("\n", " ")
rec[1] = (rec[1] or "UNKNOWN").upper().split()[0].strip()
## Ranking
code = "default"
if ins in ranas:
code = "rivet"
elif ins in greylist:
code = "grey"
elif ins in blacklist:
code = "black"
elif ins in hotlist:
code = "hot"
## Tags
+ import re
title = rec[0] or ""
if "search" in title.lower():
code += " search"
- if "Pb" in title or "Xe" in title:
+ if any(re.search(x, title) is not None for x in ["Pb", "Xe", "lead[ ,$]", "heavy[- ]ion"]):
code += " heavyion"
rm = False
rm |= args.ONLYSEARCHES and not "search" in code
rm |= args.NOSEARCHES and "search" in code
rm |= args.ONLYHEAVYION and not "heavyion" in code
rm |= args.NOHEAVYION and "heavyion" in code
if rm:
del records[ins]
else:
rec.append(code)
## Group and count records by experiment (and update rank file if requested)
ex_records = {}
ex_ntots, ex_ndefaults, ex_nurgents, ex_nwanteds, ex_ntargets, ex_nrivets = {}, {}, {}, {}, {}, {}
for ex in EXPTS:
if ex != "Other":
ex_records[ex] = {ins : rec for ins, rec in records.items() if rec[1].upper() == ex.upper()}
else:
namedexpts = [e.upper() for e in EXPTS[:-1]]
ex_records[ex] = {ins : rec for ins, rec in records.items() if rec[1].upper() not in namedexpts}
ex_ntots[ex] = len(ex_records[ex])
ex_nrivets[ex] = len([ins for ins, rec in ex_records[ex].items() if "rivet" in rec[-1]])
ex_ndefaults[ex] = len([ins for ins, rec in ex_records[ex].items() if "default" in rec[-1]])
ex_nurgents[ex] = len([ins for ins, rec in ex_records[ex].items() if "hot" in rec[-1]])
ex_nwanteds[ex] = ex_ndefaults[ex] + ex_nurgents[ex]
ex_ntargets[ex] = ex_nwanteds[ex] + ex_nrivets[ex]
if args.VERBOSE:
print(ex, "#urgent/#wanted =", ex_nurgents[ex], "/", ex_nwanteds[ex])
if args.UPDATERANK:
if args.ONLYSEARCHES or args.NOSEARCHES or args.ONLYHEAVYION or args.NOHEAVYION:
print("Won't update rank lists while search/HI/experiment filtering is enabled")
sys.exit(1)
rfname = "{}-{}.rank".format(args.BASENAME, ex.lower())
print("Writing updated rank file to {}".format(rfname))
syms = { "default" : ".", "rivet" : ".", "grey" : "?", "black" : "X", "hot" : "!" }
with open(rfname, "w") as rf:
for ins, rec in sorted(ex_records[ex].items()):
rankcode = rec[-1].split()[0]
# line = u"{} {} {}\n".format(ins.encode("UTF-8"), syms[code], rec[3].encode("UTF-8"))
line = u"{} {} {}".format(ins, syms[rankcode], rec[0])
# print(assigned.get(ins))
if ins in assigned:
#print(ins, rec[0], assigned[ins])
line += " <{}>".format(assigned[ins])
line += "\n"
rf.write(line.encode("UTF-8"))
ntot = len(records)
nrivet = len([ins for ins, rec in records.items() if "rivet" in rec[-1]])
ndefault = len([ins for ins, rec in records.items() if "default" in rec[-1]])
nurgent = len([ins for ins, rec in records.items() if "hot" in rec[-1]])
nwanted = ndefault + nurgent
ntarget = nwanted + nrivet
## Register filter strings
excls = []
if args.ONLYSEARCHES:
excls.append("searches only")
if args.NOSEARCHES:
excls.append("no searches")
if args.ONLYHEAVYION:
excls.append("heavy ion only")
if args.NOHEAVYION:
excls.append("no heavy ion")
## Web page rendering
import html
OUT = html.HTML("html")
title = "Rivet LHC analysis coverage"
exclstr = " ({})".format(", ".join(excls)) if excls else ""
title += exclstr
head = OUT.head(newlines=True)
head.meta(charset="utf-8")
head.title(title)
head.link("", rel="stylesheet", href="https://code.jquery.com/ui/1.12.1/themes/base/jquery-ui.css")
head.script("MathJax.Hub.Config({ tex2jax: {inlineMath: [['$','$']]} });", type="text/x-mathjax-config")
head.script("", type="text/javascript", src="https://cdnjs.cloudflare.com/ajax/libs/mathjax/2.7.4/MathJax.js?config=TeX-MML-AM_CHTML", async="async")
head.script("", type="text/javascript", src="https://code.jquery.com/jquery-3.3.1.js", integrity="sha256-2Kok7MbOyxpgUVvAk/HJ2jigOSYS2auK4Pfzbm7uH60=", crossorigin="anonymous")
head.script("", type="text/javascript", src="https://code.jquery.com/ui/1.12.1/jquery-ui.js", integrity="sha256-T0Vest3yCU7pafRw9r+settMBX6JkKN06dqBnpQ8d30=", crossorigin="anonymous")
head.script("""
$(document).ready( function(){
$("#blacktoggle").click( function(){
var b = $("#blacktoggle"); var t = b.text();
b.text(t.indexOf("Show") != -1 ? t.replace("Show", "Hide") : t.replace("Hide", "Show") );
$(".black").toggle(100);
});
$("#greytoggle").click( function(){
var b = $("#greytoggle"); var t = b.text();
b.text(t.indexOf("Show") != -1 ? t.replace("Show", "Hide") : t.replace("Hide", "Show") );
$(".grey").toggle(100);
});
$("#tabs").tabs();
});
""")
style = head.style(newlines="True")
style += "html { font-family: sans; font-size: large; color: #333; }"
style += "body { padding: 2em; }"
style += "table { margin: 2em 0 2em 0; border: 0; border-collapse: collapse; text-align: left; }"
style += "table.list { border-top: 3px solid black; border-bottom: 3px solid black; }"
style += "table.list thead { border-bottom: 1px solid #333; }"
style += "table.key { border: 1px solid #333; margin: 0; }"
style += "td { padding: 15px; }"
style += "tr.ana { border-top: 1px solid #ccc; }"
style += "tr.ana td { padding-bottom: 1em; padding-top: 1em; }"
style += "a { color: #339; }"
style += "button { margin: 1em; }"
# style += ".row { margin: 1em 0 3em 0; }"
# style += ".row:after { content: ''; display: table; clear: both; }"
# style += ".col { float: left; width: 50%; }"
style += "button { border: none; margin: 0 1em 1em 0; border-radius: 1ex; color: #333; background: #ddf; padding: 1ex; }"
style += "button:hover { background: #cce; }"
style += "button:active { color: white; }"
style += "#tabs { border: 0; }"
style += ".rivet { background: #cfc; }"
style += ".hot { background: #fbb; }"
style += ".default { background: #fee; }"
style += ".grey { color: #666; background: #ddd; font-size: normal; display: none; }"
style += ".grey a { color: #669; }"
style += ".black { color: #eee; background: #333; display: none; }"
style += ".black a { color: #99c; }"
style += ".hot.assigned { background: repeating-linear-gradient(135deg, #fbb, #fbb 10px, #bd7 10px, #bd7 20px); }"
style += ".default.assigned { background: repeating-linear-gradient(135deg, #fee, #fee 10px, #de9 10px, #de9 20px); }"
style += ".grey.assigned { background: repeating-linear-gradient(135deg, #ddd, #ddd 10px, #dfd 10px, #dfd 20px); }"
body = OUT.html.body(newlines=True)
body.h1(title)
body.p().b("Rivet analyses exist for {}/{} papers = {:.0f}%. {} priority analyses required.".format(nrivet, ntarget, 100*nrivet/ntarget, nurgent))
body.p("Total number of Inspire papers scanned = {}, at {}".format(ntot, now.strftime("%Y-%m-%d")))
body.p("Breakdown by identified experiment (in development):")
t = body.table(klass="list")
th = t.thead(newlines=True)
r = th.tr(klass="thead")
r.td().b("Key")
for ex in EXPTS:
r.td().b(ex)
#
tb = t.tbody(newlines=True)
r = tb.tr(klass="default")
r.td().b("Rivet wanted (total):")
for ex in EXPTS:
r.td("{}".format(ex_nwanteds[ex]))
#
r = tb.tr(klass="hot")
r.td().b("Rivet REALLY wanted:")
for ex in EXPTS:
r.td("{}".format(ex_nurgents[ex]))
r = tb.tr(klass="rivet")
#
r.td().b("Rivet provided:")
for ex in EXPTS:
# txt = "{}".format(ex_nrivets[ex])
# if ex_ntargets[ex]:
# txt += "<span style=\"color: #666\"> / {:d} = </span> {:.0f}%".format(ex_ntargets[ex], 100*ex_nrivets[ex]/ex_ntargets[ex])
# r.td(txt)
b = r.td().b("{}".format(ex_nrivets[ex]))
if ex_ntargets[ex]:
b.span("/{:d} = ".format(ex_ntargets[ex]), style="color: #777")
b += "{:.0f}%".format(100*ex_nrivets[ex]/ex_ntargets[ex])
body.button("Show greylist", id="greytoggle")
body.button("Show blacklist", id="blacktoggle")
#body.input(klass="search", placeholder="Search")
#body.button("Sort by name", klass="sort", data-sort="name")
tabs = body.div(id="tabs")
u = tabs.ul()
for ex in EXPTS:
u.li().a(ex, href="#{}expt".format(ex.lower()))
for ex in EXPTS:
d = tabs.div(id="{}expt".format(ex.lower()))
t = d.table(klass="list").tbody(newlines=True)
for i, (ins, rec) in enumerate(sorted(ex_records[ex].items(), reverse=args.REVERSE)):
expt = rec[1]
code = rec[-1]
if ins in assigned:
code += " assigned"
if expt:
code += " {}expt".format(expt.lower())
cell = t.tr(klass=code+" ana", newlines=True).td(newlines=False)
# Title
summ = u""
summ += u"{}: {}".format(expt, rec[0])
cell.span().b(summ)
## Inspire ID and report numbers
p = cell.p()
p.span("Inspire ID: {} ".format(ins))
+ if rec[4]:
+ p.span("arXiv ID: {} ".format(rec[4]))
if rec[7]:
p.span(u" Report IDs: " + u", ".join(rec[7]))
## Links
p = cell.span("Links: ")
## Inspire
p.a("Inspire", href="http://inspirehep.net/record/{}".format(ins)) # Inspire
p += " "
## DOI
if rec[2]:
p.a("DOI/journal", href="http://dx.doi.org/{}".format(rec[2]))
p += " "
## CDS
if rec[3]:
p.a("CDS", href="https://cds.cern.ch/record/{}".format(rec[3]))
p += " "
## arXiv
if rec[4]:
p.a("arXiv", href="https://arxiv.org/abs/{}".format(rec[4]))
p += " "
## HepData
if rec[5]:
p.a("HepData", href="https://hepdata.net/record/{}".format(rec[5]))
p += " "
## Rivet
if ins in ranas:
anas = u", ".join(ranas[ins])
p += " "
p.a(anas, href="https://rivet.hepforge.org/analyses/{}.html".format(ranas[ins][0]))
## In-progress/assignment
if ins in assigned:
p += " "
p.a("IN PROGRESS: assigned to {}".format(assigned[ins]), href="mailto:{}".format(assigned[ins]))
## Time-created footer
body.p("Generated at {}".format(now.strftime("%c")))
body.p("Generated from JSON files extracted from Inspire ({} papers in total):".format(ntot))
body.p(", ".join(args.JSONFILES), style="font-family: monospace; font-size: smaller")
## Write out
outfile = args.OUTFILE
if not outfile:
outfile = args.BASENAME
exclparts = [e.replace(" ", "") for e in excls]
if exclparts:
outfile += "-" + "-".join(exclparts)
if not outfile.endswith(".html"):
outfile += ".html"
print("Writing output to {} {}".format(outfile, exclstr))
with open(outfile, "wb") as hf:
a = unicode(OUT)
hf.write(a.encode("UTF-8"))
diff --git a/doc/rivet-coverage-alice.rank b/doc/rivet-coverage-alice.rank
--- a/doc/rivet-coverage-alice.rank
+++ b/doc/rivet-coverage-alice.rank
@@ -1,234 +1,237 @@
841752 X Alignment of the ALICE Inner Tracking System with cosmic-ray tracks
852264 . Charged-particle multiplicity measurement in proton-proton collisions at $\sqrt{s}=7$ TeV with ALICE at LHC
852450 . Charged-particle multiplicity measurement in proton-proton collisions at $\sqrt{s}=0.9$ and 2.36 TeV with ALICE at LHC
-859610 . Midrapidity antiproton-to-proton ratio in pp collisions at $\sqrt{s} = 0.9$ and $7$~TeV measured by the ALICE experiment
+859610 ! Midrapidity antiproton-to-proton ratio in pp collisions at $\sqrt{s} = 0.9$ and $7$~TeV measured by the ALICE experiment
860416 . Transverse momentum spectra of charged particles in proton-proton collisions at $\sqrt{s} = 900$~GeV with ALICE at the LHC
860477 . Two-pion Bose-Einstein correlations in $pp$ collisions at $\sqrt{s}=900$ GeV
864292 . ALICE EMCal Physics Performance Report
877821 . Charged-particle multiplicity density at mid-rapidity in central Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV
877822 ! Elliptic flow of charged particles in Pb-Pb collisions at 2.76 TeV
879583 ? Suppression of Charged Particle Production at Large Transverse Momentum in Central Pb-Pb Collisions at $\sqrt{s_{NN}} =$ 2.76 TeV
880049 . Centrality dependence of the charged-particle multiplicity density at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV
881474 . Strange particle production in proton-proton collisions at sqrt(s) = 0.9 TeV with ALICE at the LHC
881884 . Two-pion Bose-Einstein correlations in central Pb-Pb collisions at $\sqrt{{s}_{NN}} =$ 2.76 TeV
884741 . Femtoscopy of $pp$ collisions at $\sqrt{s}=0.9$ and 7 TeV at the LHC with two-pion Bose-Einstein correlations
-885104 . Production of pions, kaons and protons in $pp$ collisions at $\sqrt{s}= 900$ GeV with ALICE at the LHC
+885104 ! Production of pions, kaons and protons in $pp$ collisions at $\sqrt{s}= 900$ GeV with ALICE at the LHC
897764 . Rapidity and transverse momentum dependence of inclusive J$/\psi$ production in $pp$ collisions at $\sqrt{s} = 7$ TeV
900651 ! Higher harmonic anisotropic flow measurements of charged particles in Pb-Pb collisions at $\sqrt{s_{NN}}$=2.76 TeV
927105 . Harmonic decomposition of two-particle angular correlations in Pb-Pb collisions at $\sqrt{s_{NN}}=$ 2.76 TeV
930312 . Particle-yield modification in jet-like azimuthal di-hadron correlations in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV
944730 . $J/\psi$ polarization in $pp$ collisions at $\sqrt{s}=7$ TeV
944757 . Measurement of charm production at central rapidity in proton-proton collisions at $\sqrt{s} = 7$ TeV
1080735 ! Underlying Event measurements in $pp$ collisions at $\sqrt{s}=0.9$ and 7 TeV with the ALICE experiment at the LHC
-1080945 . Light vector meson production in $pp$ collisions at $\sqrt{s}=7$ TeV
+1080945 ! Light vector meson production in $pp$ collisions at $\sqrt{s}=7$ TeV
1084331 ? Measurement of Event Background Fluctuations for Charged Particle Jet Reconstruction in Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV
1084981 . Heavy flavour decay muon production at forward rapidity in proton–proton collisions at $\sqrt{s} =$ 7 TeV
1088222 . $J/\psi$ suppression at forward rapidity in Pb-Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV
1088833 ! $J/\psi$ Production as a Function of Charged Particle Multiplicity in $pp$ Collisions at $\sqrt{s} = 7$ TeV
1093488 . Suppression of high transverse momentum D mesons in central Pb-Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV
1093519 ? Measurement of the Cross Section for Electromagnetic Dissociation with Neutron Emission in Pb-Pb Collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
1094079 . Inclusive $J/\psi$ production in $pp$ collisions at $\sqrt{s} = 2.76$ TeV
1097057 X Multi-strange baryon production in $pp$ collisions at $\sqrt{s} = 7$ TeV with ALICE
1115186 . Transverse sphericity of primary charged particles in minimum bias proton-proton collisions at $\sqrt{s}=0.9$, 2.76 and 7 TeV
1115187 ? Measurement of charm production at central rapidity in proton-proton collisions at $\sqrt{s}=2.76$ TeV
1115824 ? Measurement of electrons from semileptonic heavy-flavour hadron decays in pp collisions at \sqrt{s} = 7 TeV
1116147 . Neutral pion and $\eta$ meson production in proton-proton collisions at $\sqrt{s}=0.9$ TeV and $\sqrt{s}=7$ TeV
1116150 . Anisotropic flow of charged hadrons, pions and (anti-)protons measured at high transverse momentum in Pb-Pb collisions at $\sqrt{s_{NN}}$=2.76 TeV
-1116251 . Measurement of prompt $J/\psi$ and beauty hadron production cross sections at mid-rapidity in $pp$ collisions at $\sqrt{s} = 7$ TeV
-1116417 . Production of muons from heavy flavour decays at forward rapidity in pp and Pb-Pb collisions at $\sqrt {s_{NN}}$ = 2.76 TeV
+1116251 ! Measurement of prompt $J/\psi$ and beauty hadron production cross sections at mid-rapidity in $pp$ collisions at $\sqrt{s} = 7$ TeV
+1116417 ! Production of muons from heavy flavour decays at forward rapidity in pp and Pb-Pb collisions at $\sqrt {s_{NN}}$ = 2.76 TeV
1117885 ? $K^0_s-K^0_s$ correlations in $pp$ collisions at $\sqrt{s}=7$ TeV from the LHC ALICE experiment
1121161 . Charge separation relative to the reaction plane in Pb-Pb collisions at $\sqrt{s_{NN}}= 2.76$ TeV
1123802 ? Net-Charge Fluctuations in Pb-Pb collisions at $\sqrt{s}_{NN} = 2.76$ TeV
-1126962 ? Measurement of electrons from beauty hadron decays in $pp$ collisions at $\sqrt{s}=7$ TeV
+1126962 . Measurement of electrons from beauty hadron decays in $pp$ collisions at $\sqrt{s}=7$ TeV
1126963 . $D_{s}^+$ meson production at central rapidity in proton--proton collisions at $\sqrt{s}=7$ TeV
1126966 . Pion, Kaon, and Proton Production in Central Pb--Pb Collisions at $\sqrt{s_{NN}} = 2.76$ TeV
1127497 . Centrality Dependence of Charged Particle Production at Large Transverse Momentum in Pb--Pb Collisions at $\sqrt{s_{\rm{NN}}} = 2.76$ TeV
1181770 . Measurement of inelastic, single- and double-diffraction cross sections in proton--proton collisions at the LHC with ALICE
1182213 ? Production of $K^*(892)^0$ and $\phi(1020)$ in $pp$ collisions at $\sqrt{s}=7$ TeV
1185785 ? Coherent $J/\psi$ photoproduction in ultra-peripheral Pb-Pb collisions at $\sqrt{s_{NN}} = 2.76$ TeV
1190545 ! Pseudorapidity density of charged particles in $p$ + Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV
1190895 . Transverse momentum distribution and nuclear modification factor of charged particles in $p$-Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV
1206610 . Long-range angular correlations on the near and away side in $p$-Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV
1208696 . Charged kaon femtoscopic correlations in $pp$ collisions at $\sqrt{s}=7$ TeV
-1210881 . Measurement of the inclusive differential jet cross section in $pp$ collisions at $\sqrt{s} = 2.76$ TeV
+1210881 ! Measurement of the inclusive differential jet cross section in $pp$ collisions at $\sqrt{s} = 2.76$ TeV
1211186 . Charge correlations using the balance function in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
1215085 ! Centrality determination of Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV with ALICE
1222333 ! Centrality dependence of $\pi$, K, p production in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
1225273 . J/Psi Elliptic Flow in Pb-Pb Collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1225979 . Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1232206 . Charmonium and $e^+e^-$ pair photoproduction at mid-rapidity in ultra-peripheral Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=2.76 TeV
-1232209 . Mid-rapidity anti-baryon to baryon ratios in pp collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV measured by ALICE
+1232209 ! Mid-rapidity anti-baryon to baryon ratios in pp collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV measured by ALICE
1233087 . D meson elliptic flow in non-central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76TeV
1238451 X Performance of the ALICE VZERO system
1238980 . Directed Flow of Charged Particles at Midrapidity Relative to the Spectator Plane in Pb-Pb Collisions at $\sqrt{s_{NN}}$=2.76 TeV
-1241422 . Energy Dependence of the Transverse Momentum Distributions of Charged Particles in pp Collisions Measured by ALICE
-1241423 . Multiplicity dependence of the average transverse momentum in pp, p-Pb, and Pb-Pb collisions at the LHC
+1241422 ! Energy Dependence of the Transverse Momentum Distributions of Charged Particles in pp Collisions Measured by ALICE
+1241423 ! Multiplicity dependence of the average transverse momentum in pp, p-Pb, and Pb-Pb collisions at the LHC
1241570 . Multiplicity dependence of two-particle azimuthal correlations in pp collisions at the LHC
1242302 . Long-range angular correlations of $\rm \pi$, K and p in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
1243863 . $K^0_S$ and $\Lambda$ production in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
1243865 . Multi-strange baryon production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
1244523 . Multiplicity Dependence of Pion, Kaon, Proton and Lambda Production in p-Pb Collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
1251898 . $J/\psi$ production and nuclear effects in p-Pb collisions at $\sqrt{S_{NN}}$ = 5.02 TeV
1262523 . Two- and three-pion quantum statistics correlations in Pb-Pb collisions at $\sqrt{{s}_{NN}} =$ 2.76 TeV at the CERN Large Hadron Collider
1263062 . Centrality, rapidity and transverse momentum dependence of $J/\psi$ suppression in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=2.76 TeV
1263194 . Measurement of charged jet suppression in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
1276299 . Production of charged pions, kaons and protons at large transverse momenta in pp and Pb–Pb collisions at $\sqrt{s_{\rm NN}}$ =2.76 TeV
1281831 X Performance of the ALICE Experiment at the CERN LHC
1285950 . Measurement of quarkonium production at forward rapidity in $pp$ collisions at $\sqrt{s} = 7$ TeV
1288320 . $K^*(892)^0$ and $ϕ(1020)$ production in Pb-Pb collisions at $\sqrt{s{NN}}$ = 2.76 TeV
-1288705 . Freeze-out radii extracted from three-pion cumulants in pp, p–Pb and Pb–Pb collisions at the LHC
+1288705 ? Freeze-out radii extracted from three-pion cumulants in pp, p–Pb and Pb–Pb collisions at the LHC
1294934 . Measurement of visible cross sections in proton-lead collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV in van der Meer scans with the ALICE detector
1294938 . Azimuthal anisotropy of D meson production in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV
1295687 . Transverse momentum dependence of inclusive primary charged-particle production in p-Pb collisions at $\sqrt{s_\mathrm{{NN}}}=5.02~\text {TeV}$
1296081 . Measurement of prompt $D$-meson production in $p-Pb$ collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
1296306 . Neutral pion production at midrapidity in pp and Pb-Pb collisions at $\sqrt{s_{{\mathrm {NN}}}}= 2.76\,{\mathrm {TeV}}$
1296307 . Suppression of $\psi$(2S) production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
-1296860 . Measurement of electrons from semileptonic heavy-flavor hadron decays in $pp$ collisions at $\sqrt{s} = 2.76$ TeV
-1296861 . Beauty production in pp collisions at $\sqrt{s}$ = 2.76 TeV measured via semi-electronic decays
+1296860 ! Measurement of electrons from semileptonic heavy-flavor hadron decays in $pp$ collisions at $\sqrt{s} = 2.76$ TeV
+1296861 ! Beauty production in pp collisions at $\sqrt{s}$ = 2.76 TeV measured via semi-electronic decays
1297101 ! Suppression of $\Upsilon (1S)$ at forward rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV
1297103 . Elliptic flow of identified hadrons in Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV
1300038 . Multiparticle azimuthal correlations in p -Pb and Pb-Pb collisions at the CERN Large Hadron Collider
1300380 . Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in proton-proton collisions at $\sqrt{s}=$ 7 TeV
1301858 . Multiplicity dependence of jet-like two-particle correlation structures in p–Pb collisions at $\sqrt{s_{NN}}$=5.02 TeV
1303903 . Exclusive $\mathrm{J/}\psi$ photoproduction off protons in ultra-peripheral p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
1305020 . Upgrade of the ALICE Experiment: Letter Of Intent
1305021 . Technical Design Report for the Upgrade of the ALICE Inner Tracking System
1307102 . Event-by-event mean ${p}_{\mathbf {T}}$ fluctuations in pp and Pb-Pb collisions at the LHC
1321022 ! Production of inclusive $\Upsilon$(1S) and $\Upsilon$(2S) in p-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV
1328629 . Charged jet cross sections and properties in proton-proton collisions at $\sqrt{s}=7$ TeV
1328669 . Inclusive photon production at forward rapidities in proton-proton collisions at $\sqrt{s}$ = 0.9, 2.76 and 7 TeV
1335350 ! Centrality dependence of particle production in p-Pb collisions at $\sqrt{s_{\rm NN} }$= 5.02 TeV
-1342496 . Forward-backward multiplicity correlations in pp collisions at $ \sqrt{s} $ = 0.9, 2.76 and 7 TeV
+1342496 ! Forward-backward multiplicity correlations in pp collisions at $ \sqrt{s} $ = 0.9, 2.76 and 7 TeV
1342499 . Two-pion femtoscopy in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
1343112 . Measurement of jet suppression in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1346963 . Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at $\sqrt{s_\rm{NN}} = 5.02$ TeV
1351451 . Measurement of dijet $k_T$ in p–Pb collisions at $\sqrt{s}_{NN}$=5.02 TeV
1355544 . Rapidity and transverse-momentum dependence of the inclusive J/$\psi$ nuclear modification factor in p-Pb collisions at $ \sqrt{s_{N\ N}} =$ 5.02 TeV
1357206 . Coherent ρ$^{0}$ photoproduction in ultra-peripheral Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV
1357424 . Measurement of pion, kaon and proton production in proton–proton collisions at $\sqrt{s} = 7$ TeV
1364887 . Inclusive, prompt and non-prompt J/$\psi$ production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1366028 . Measurement of charm and beauty production at central rapidity versus charged-particle multiplicity in proton-proton collisions at $ \sqrt{s}=7 $ TeV
1376027 . Measurement of jet quenching with semi-inclusive hadron-jet distributions in central Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV
1377363 . Centrality dependence of high-p$_{T}$ D meson suppression in Pb-Pb collisions at $ \sqrt{s_{\mathrm{N}\mathrm{N}}}=2.76 $ TeV
1377750 . Centrality dependence of the nuclear modification factor of charged pions, kaons, and protons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV
1377753 X Search for weakly decaying $\overline{\Lambda\mathrm{n}}$ and $\Lambda\Lambda $ exotic bound states in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1379971 . One-dimensional pion, kaon, and proton femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm {NN}}}$ =2.76 TeV
1379977 . Forward-central two-particle correlations in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
1380192 . Differential studies of inclusive J/ψ and ψ(2S) production at forward rapidity in Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV
1380193 . Centrality dependence of inclusive J/ψ production in p-Pb collisions at $ \sqrt{s_{\mathrm{NN}}}=5.02 $ TeV
1380234 . $^{3}_{\Lambda}\mathrm H$ and $^{3}_{\bar{\Lambda}} \overline{\mathrm H}$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV
1380453 . $\phi$-meson production at forward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV and in pp collisions at $\sqrt{s}$ = 2.76 TeV
1380491 . Production of light nuclei and anti-nuclei in pp and Pb-Pb collisions at energies available at the CERN Large Hadron Collider
1382591 . Elliptic flow of muons from heavy-flavour hadron decays at forward rapidity in Pb–Pb collisions at $\sqrt{s_{\rm NN}}= 2.76$ TeV
1384270 . Event shape engineering for inclusive spectra and elliptic flow in Pb-Pb collisions at $\sqrt{s_\rm{NN}}=2.76$ TeV
1384807 . Centrality dependence of pion freeze-out radii in Pb-Pb collisions at $\sqrt{s}_{NN}=$ 2.76 TeV
1385276 . Study of cosmic ray events with high muon multiplicity using the ALICE detector at the CERN Large Hadron Collider
1388181 . Precision measurement of the mass difference between light nuclei and anti-nuclei
1388730 . Coherent $\psi$(2S) photo-production in ultra-peripheral Pb Pb collisions at $\sqrt{s}_{\rm NN}$ = 2.76 TeV
1394580 . Transverse momentum dependence of D-meson production in Pb-Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}}=$ 2.76 TeV
1394672 . Multiplicity and transverse momentum evolution of charge-dependent correlations in pp, p–Pb, and Pb–Pb collisions at the LHC
1394675 . Measurement of D$_{s}^{+}$ production and nuclear modification factor in Pb-Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}}=$ 2.76 TeV
1394676 ! Centrality evolution of the charged-particle pseudorapidity density over a broad pseudorapidity range in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV
1394677 ! Direct photon production in Pb-Pb collisions at $\sqrt{s_\rm{NN}} =$ 2.76 TeV
1394678 . Azimuthal anisotropy of charged jet production in $\sqrt{s_{\rm NN}}$ = 2.76 TeV Pb-Pb collisions
1394682 . Measurement of electrons from heavy-flavour hadron decays in p-Pb collisions at $\sqrt{s_{\rm NN}} =$ 5.02 TeV
1394854 . Charged-particle multiplicities in proton–proton collisions at $\sqrt{s} = 0.9$ to 8 TeV
1395099 . Inclusive quarkonium production at forward rapidity in pp collisions at $\sqrt{s}=8$ TeV
1395253 . Pseudorapidity and transverse-momentum distributions of charged particles in proton–proton collisions at $\sqrt s=$ 13 TeV
1395296 . Measurement of an excess in the yield of $J/\psi$ at very low $p_{\rm T}$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1410144 . Charge-dependent flow and the search for the chiral magnetic wave in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV
1410589 . Centrality dependence of the charged-particle multiplicity density at midrapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
1411084 ! Multi-strange baryon production in p-Pb collisions at $\sqrt{s_\mathbf{NN}}=5.02$ TeV
1411653 . Multipion Bose-Einstein correlations in pp,p -Pb, and Pb-Pb collisions at energies available at the CERN Large Hadron Collider
1415274 . Multiplicity dependence of charged pion, kaon, and (anti)proton production at large transverse momentum in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}}$ = 5.02 TeV
1418181 . Production of K$^{*}$ (892)$^{0}$ and $\phi $ (1020) in p–Pb collisions at $\sqrt{s_{{\text {NN}}}}$ = 5.02 TeV
1419244 . Anisotropic flow of charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
1419249 X Particle identification in ALICE: a Bayesian approach
1423072 . Measurement of D-meson production versus multiplicity in p-Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}}=5.02 $ TeV
1426826 . Centrality dependence of $\mathbf{\psi}$(2S) suppression in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}}$ = 5.02 TeV
1427026 . Centrality dependence of charged jet production in p–Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV
1427723 . Measurement of transverse energy at midrapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV
1452590 . Correlated event-by-event fluctuations of flow harmonics in Pb-Pb collisions at $\sqrt{s_{_{\rm NN}}}=2.76$ TeV
1456145 . Pseudorapidity dependence of the anisotropic flow of charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV
1464839 . Measurement of azimuthal correlations of D mesons and charged particles in pp collisions at $\sqrt{s}=7$ TeV and p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
1465513 ! $D$-meson production in $p$-Pb collisions at $\sqrt{s_{\rm NN}}=$5.02 TeV and in pp collisions at $\sqrt{s}=$7 TeV
1466626 . Elliptic flow of electrons from heavy-flavour hadron decays at mid-rapidity in Pb-Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}}=2.76 $ TeV
1471285 . Higher harmonic flow coefficients of identified hadrons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1471838 ! Enhanced production of multi-strange hadrons in high-multiplicity proton-proton collisions
1472319 . J/$\psi$ suppression at forward rapidity in Pb-Pb collisions at $\mathbf{\sqrt{s_{{\rm NN}}} = 5.02}$ TeV
1483164 . Jet-like correlations with neutral pion triggers in pp and central Pb–Pb collisions at 2.76 TeV
1486391 . Measurement of electrons from beauty-hadron decays in p-Pb collisions at $ \sqrt{s_{\mathrm{NN}}}=5.02 $ TeV and Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV
1487545 . Anomalous evolution of the near-side jet peak shape in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1487546 . Evolution of the longitudinal and azimuthal structure of the near-side jet peak in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV
1487727 . Measurement of the production of high-$p_{\rm T}$ electrons from heavy-flavour hadron decays in Pb-Pb collisions at $\mathbf{\sqrt{\it s_{\rm{NN}}}}$ = 2.76 TeV
1491202 . Determination of the event collision time with the ALICE detector at the LHC
1496634 . W and Z boson production in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
1507090 ! Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
1507157 ! Insight into particle production mechanisms via angular correlations of identified particles in pp collisions at $\sqrt{\mathrm{s}}=7$  TeV
1510878 . Production of $\Sigma(1385)^{\pm}$ and $\Xi(1530)^{0}$ in p-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
1511864 . K$^{*}(892)^{0}$ and $\phi(1020)$ meson production at high transverse momentum in pp and Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 2.76 TeV
1511865 . Energy dependence of forward-rapidity $\mathrm {J}/\psi $ and $\psi \mathrm {(2S)}$ production in pp collisions at the LHC
1511870 . Measurement of D-meson production at mid-rapidity in pp collisions at ${\sqrt{s}=7}$  TeV
1512107 . First measurement of jet mass in Pb–Pb and p–Pb collisions at the LHC
1512110 . Production of ${\pi ^0}$ and $\eta $ mesons up to high transverse momentum in pp collisions at 2.76 TeV
1512297 . Production of muons from heavy-flavour hadron decays in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{NN}} = 5.02}$ TeV
1512303 . Azimuthally differential pion femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76$ TeV
1512772 . Flow dominance and factorization of transverse momentum correlations in Pb-Pb collisions at the LHC
1589286 . J/$\psi$ production as a function of charged-particle pseudorapidity density in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
1599396 . Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV
1599554 . Measuring K$^0_{\rm S}$K$^{\rm \pm}$ interactions using Pb-Pb collisions at ${\sqrt{s_{\rm NN}}=2.76}$ TeV
1608612 . $D$-meson azimuthal anisotropy in midcentral Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}=5.02}$ TeV
1610453 . Searches for transverse momentum dependent flow vector fluctuations in Pb-Pb and p-Pb collisions at the LHC
1611301 . Measurement of deuteron spectra and elliptic flow in Pb–Pb collisions at $\sqrt{s_{\mathrm {NN}}}$ = 2.76 TeV at the LHC
1614477 ! Charged-particle multiplicity distributions over a wide pseudorapidity range in proton-proton collisions at $\sqrt{s}=$ 0.9, 7, and 8 TeV
1620477 . $\pi ^{0}$ and $\eta $ meson production in proton-proton collisions at $\sqrt{s}=8$ TeV
1621591 . Systematic studies of correlations between different order flow harmonics in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1621809 . Kaon femtoscopy in Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV
1622554 X The ALICE Transition Radiation Detector: construction, operation, and performance
1623558 . Constraining the magnitude of the Chiral Magnetic Effect with Event Shape Engineering in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 2.76 TeV
1623907 . J/$\psi$ elliptic flow in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV
1624550 . Search for collectivity with azimuthal J/$\psi$-hadron correlations in high multiplicity p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 and 8.16 TeV
1625294 . Production of deuterons, tritons, $^{3}$He nuclei and their antinuclei in pp collisions at $\mathbf{\sqrt{{\textit s}}}$ = 0.9, 2.76 and 7 TeV
1631788 . Production of $^{4}$He and $^{4}\overline{\textrm{He}}$ in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 2.76 TeV at the LHC
1632046 . Longitudinal asymmetry and its effect on pseudorapidity distributions in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
1639439 . Measurement of Z$^0$-boson production at large rapidities in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV
1642729 . First measurement of $\Xi_{\rm c}^0$ production in pp collisions at $\mathbf{\sqrt{s}}$ = 7 TeV
1643642 . Constraints on jet quenching in p-Pb collisions at $\mathbf{\sqrt{s_{NN}}}$ = 5.02 TeV measured by the event-activity dependence of semi-inclusive hadron-jet distributions
1644609 . Relative particle yield fluctuations in Pb-Pb collisions at ${\mathbf{\sqrt{s_{\rm NN}}=2.76}}$ TeV
1645239 . $\Lambda_{\rm c}^+$ production in pp collisions at $\sqrt{s} = 7$ TeV and in p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
1649235 . Neutral pion and $\eta$ meson production in p-Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
1652829 . Prompt and non-prompt $\hbox {J}/\psi $ production and nuclear modification at mid-rapidity in p–Pb collisions at $\mathbf{\sqrt{{ s}_{\text {NN}}}= 5.02}$  TeV
1657384 ! Transverse momentum spectra and nuclear modification factors of charged particles in pp, p-Pb and Pb-Pb collisions at the LHC
1662651 . Neutral pion and $\eta$ meson production at mid-rapidity in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
1664312 . Direct photon production at low transverse momentum in proton-proton collisions at $\mathbf{\sqrt{s}=2.76}$ and 8 TeV
1664538 . Azimuthally-differential pion femtoscopy relative to the third harmonic event plane in Pb-Pb collisions at $\mathbf{\sqrt{\textit{s}_{_{\rm NN}}}}$ = 2.76 TeV
1666817 . Energy dependence and fluctuations of anisotropic flow in Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}}=5.02 $ and 2.76 TeV
1669805 . $\phi$ meson production at forward rapidity in Pb-Pb collisions at $\sqrt{s_\mathrm{NN}}=2.76$ TeV
-1669819 ! Measurement of D$^0$, D$^+$, D$^{*+}$ and D$^+_{\rm s}$ production in Pb-Pb collisions at $\mathbf{\sqrt{s_{\rm NN}}}= 5.02$ TeV
+1669819 ! Measurement of D$^{0}$, D$^{+}$, D$^{*+}$ and D$_{s}^{+}$ production in Pb-Pb collisions at $ \sqrt{{\mathrm{s}}_{\mathrm{NN}}}=5.02 $ TeV
1671792 . Anisotropic flow in Xe-Xe collisions at $\mathbf{\sqrt{s_{\rm{NN}}} = 5.44}$ TeV
1672756 ! Centrality and pseudorapidity dependence of the charged-particle multiplicity density in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV
1672765 . Two particle differential transverse momentum and number density correlations in p-Pb and Pb-Pb at the LHC
-1672788 . Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV
+1672788 ! Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at $\sqrt{s_{\rm NN}}$ = 13 TeV
1672789 ! Direct photon elliptic flow in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1672790 . Transverse momentum spectra and nuclear modification factors of charged particles in Xe-Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV
-1672792 . Dielectron production in proton-proton collisions at $ \sqrt{s}=7 $ TeV
+1672792 ! Dielectron production in proton-proton collisions at $ \sqrt{s}=7 $ TeV
1672798 . $\Upsilon$ suppression at forward rapidity in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV
1672800 . Inclusive J/$\psi$ production in Xe–Xe collisions at $\sqrt{s_{\rm NN}}$ = 5.44 TeV
1672801 . Measurement of the inclusive J/ $\psi $ polarization at forward rapidity in pp collisions at $\mathbf {\sqrt{s} = 8}$  TeV
1672806 . Suppression of $\Lambda(1520)$ resonance production in central Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1672807 . Inclusive J/$\psi$ production at forward and backward rapidity in p-Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV
-1672811 . Measurements of low-$p_{\rm T}$ electrons from semileptonic heavy-flavour hadron decays at mid-rapidity in pp and Pb-Pb collisions at $\mathbf{\sqrt{{\it s}_\mathrm{NN}}}$ = 2.76 TeV
+1672811 . Measurements of low-p$_{T}$ electrons from semileptonic heavy-flavour hadron decays at mid-rapidity in pp and Pb-Pb collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV
1672812 . Azimuthal anisotropy of heavy-flavour decay electrons in p-Pb collisions at $ \sqrt{s_{\rm NN}}$ = 5.02 TeV
1672822 ! Anisotropic flow of identified particles in Pb-Pb collisions at $ {\sqrt{s}}_{\mathrm{NN}}=5.02 $ TeV
1672860 . Production of the $\rho$(770)${^{0}}$ meson in pp and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
-1672884 . Particle identification studies with a full-size 4-GEM prototype for the ALICE TPC upgrade
+1672884 X Particle identification studies with a full-size 4-GEM prototype for the ALICE TPC upgrade
1672944 ? Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV
1675759 . p-p, p-$\Lambda$ and $\Lambda$-$\Lambda$ correlations studied via femtoscopy in pp reactions at $\sqrt{s}$ = 7 TeV
1680638 . Measurement of dielectron production in central Pb-Pb collisions at $\sqrt{{\textit{s}}_{\mathrm{NN}}}$ = 2.76 TeV
1682990 . Medium modification of the shape of small-radius jets in central Pb-Pb collisions at $\sqrt{s_{\mathrm {NN}}} = 2.76\,\rm{TeV}$
-1684320 . Multiplicity dependence of light-flavor hadron production in pp collisions at $\sqrt{s}$ = 7 TeV
+1684320 ! Multiplicity dependence of light-flavor hadron production in pp collisions at $\sqrt{s}$ = 7 TeV
1693305 . Energy dependence of exclusive $J/\psi$ photoproduction off protons in ultra-peripheral p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV
-1693308 . Charged jet cross section and fragmentation in proton-proton collisions at $\sqrt{s}$ = 7 TeV
+1693308 ! Charged jet cross section and fragmentation in proton-proton collisions at $\sqrt{s}$ = 7 TeV
1695028 . Measuring K$^0_{\rm S}$K$^{\rm{\pm}}$ interactions using pp collisions at $\sqrt{s}=7$ TeV
1695334 . Event-shape engineering for the D-meson elliptic flow in mid-central Pb-Pb collisions at $\sqrt{s_{\rm NN}} =5.02$ TeV
1696315 . $\Lambda_\mathrm{c}^+$ production in Pb-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV
+1704923 ! Jet fragmentation transverse momentum measurements from di-hadron correlations in $\sqrt{s}$ = 7 TeV pp and $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV p-Pb collisions
+1706006 . Study of J/$\psi$ azimuthal anisotropy at forward rapidity in Pb-Pb collisions at $\sqrt{{\textit s}_{\rm NN}}$ = 5.02 TeV
+1706753 . Charged-particle pseudorapidity density at mid-rapidity in p-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 8.16 TeV
diff --git a/doc/rivet-coverage-atlas.rank b/doc/rivet-coverage-atlas.rank
--- a/doc/rivet-coverage-atlas.rank
+++ b/doc/rivet-coverage-atlas.rank
@@ -1,807 +1,820 @@
846365 X Drift Time Measurement in the ATLAS Liquid Argon Electromagnetic Calorimeter using Cosmic Muons
-849050 . Charged-particle multiplicities in $pp$ interactions at $\sqrt{s}=900$ GeV measured with the ATLAS detector at the LHC
+849050 ! Charged-particle multiplicities in $pp$ interactions at $\sqrt{s}=900$ GeV measured with the ATLAS detector at the LHC
853395 X The ATLAS Inner Detector commissioning and calibration
856179 X The ATLAS Simulation Infrastructure
856566 X Performance of the ATLAS Detector using First Collision Data
859286 X Commissioning of the ATLAS Muon Spectrometer with Cosmic Rays
863749 X Readiness of the ATLAS Tile Calorimeter for LHC collisions
865423 ? Search for New Particles in Two-Jet Final States in 7 TeV Proton-Proton Collisions with the ATLAS Detector at the LHC
871366 . Measurement of inclusive jet and dijet cross sections in proton-proton collisions at 7 TeV centre-of-mass energy with the ATLAS detector
871487 ? Search for quark contact interactions in dijet angular distributions in $pp$ collisions at $\sqrt{s}=7$ TeV measured with the ATLAS detector
872570 . Measurement of the $W \to \ell\nu$ and $Z/\gamma^* \to \ell\ell$ production cross sections in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector
-874862 . Study of energy response and resolution of the ATLAS barrel calorimeter to hadrons of energies from 20-GeV to 350-GeV
+874862 X Study of energy response and resolution of the ATLAS barrel calorimeter to hadrons of energies from 20-GeV to 350-GeV
878496 X Studies of the performance of the ATLAS detector using cosmic-ray muons
878733 ? Observation of a Centrality-Dependent Dijet Asymmetry in Lead-Lead Collisions at $\sqrt{s_{NN}}=2.77$ TeV with the ATLAS Detector at the LHC
879407 . Measurement of underlying event characteristics using charged particles in pp collisions at $\sqrt{s} = 900 GeV$ and 7 TeV with the ATLAS detector
880002 . Measurement of the top quark-pair production cross section with ATLAS in pp collisions at $\sqrt{s}=7$ TeV
881812 ? Search for Diphoton Events with Large Missing Transverse Energy in 7 TeV Proton-Proton Collisions with the ATLAS Detector
882098 . Charged-particle multiplicities in pp interactions measured with the ATLAS detector at the LHC
882463 . Measurement of the inclusive isolated prompt photon cross section in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
882519 . Measurement of the centrality dependence of J/ψ yields and observation of Z production in lead–lead collisions with the ATLAS detector at the LHC
882534 . Measurement of the production cross section for W-bosons in association with jets in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
-882984 . Study of Jet Shapes in Inclusive Jet Production in $pp$ Collisions at $\sqrt{s}=7$ TeV using the ATLAS Detector
+882984 ! Study of Jet Shapes in Inclusive Jet Production in $pp$ Collisions at $\sqrt{s}=7$ TeV using the ATLAS Detector
884120 X Luminosity Determination in $pp$ Collisions at $\sqrt{s}=7$ TeV Using the ATLAS Detector at the LHC
886505 ? Search for Massive Long-lived Highly Ionising Particles with the ATLAS Detector at the LHC
889431 ? Search for supersymmetry using final states with one lepton, jets, and missing transverse momentum with the ATLAS detector in $\sqrt{s}=7$ TeV $pp$
889546 . Measurement of Dijet Azimuthal Decorrelations in $pp$ Collisions at $\sqrt{s}=7$ TeV
890749 . Search for squarks and gluinos using final states with jets and missing transverse momentum with the ATLAS detector in $\sqrt{s}=7$ TeV proton-proton collisions
891737 ? Search for high-mass states with one lepton plus missing transverse momentum in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector
891834 . Measurements of underlying-event properties using neutral and charged particles in $pp$ collisions at 900 GeV and 7 TeV with the ATLAS detector at the LHC
892044 ? Search for stable hadronising squarks and gluinos with the ATLAS experiment at the LHC
892704 . Measurement of the $W$ charge asymmetry in the $W \to \mu \nu$ decay mode in $pp$ collisions at $\sqrt s=7$ TeV with the ATLAS detector
893264 ? Search for New Physics in Dijet Mass and Angular Distributions in pp Collisions at $\sqrt{s} = 7$ TeV Measured with the ATLAS Detector
893493 ? Search for supersymmetry in $pp$ collisions at $\sqrt{s}=7$TeV in final states with missing transverse momentum and $b$-jets
894358 ? Search for a heavy particle decaying into an electron and a muon with the ATLAS detector in $\sqrt{s}=7$ TeV $pp$ collisions at the LHC
894576 ? Search for high mass dilepton resonances in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS experiment
894578 . Search for supersymmetric particles in events with lepton pairs and large missing transverse momentum in $\sqrt{s}=7$ TeV proton-proton collisions with the ATLAS experiment
894579 ? Search for an excess of events with an identical flavour lepton pair and significant missing transverse momentum in $\sqrt{s}=7$ TeV proton-proton collisions with the ATLAS detector
894867 . Measurement of the Inelastic Proton-Proton Cross-Section at $\sqrt{s}=7$ TeV with the ATLAS Detector
896268 . Measurement of the differential cross-sections of inclusive, prompt and non-prompt $J/\psi$ production in proton-proton collisions at $\sqrt{s}=7$ TeV
897002 . Search for pair production of first or second generation leptoquarks in proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector at the LHC
897028 ? Search for Contact Interactions in Dimuon Events from $pp$ Collisions at $\sqrt{s}=7$ TeV with the ATLAS Detector
897330 . Measurement of the $W W$ cross section in $\sqrt{s}=7$ TeV $pp$ collisions with ATLAS
913039 ? Measurement of Wgamma and Zgamma production in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS Detector
913576 X Limits on the production of the Standard Model Higgs Boson in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
914491 . Search for heavy long-lived charged particles with the ATLAS detector in $pp$ collisions at $\sqrt{s}=$ 7 TeV
915920 . Search for new phenomena with the monojet and missing transverse momentum signature using the ATLAS detector in $\sqrt{s}=7$ TeV proton-proton collisions
915921 . Measurement of the $\Upsilon$(1S) production cross-section in $pp$ collisions at $\sqrt{s}=$ 7 TeV in ATLAS
916832 . Measurement of the isolated di-photon cross-section in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
916840 ? Search for Diphoton Events with Large Missing Transverse Energy with 36 pb$^{-1}$ of 7 TeV Proton-Proton Collision Data with the {ATLAS} Detector
917526 . Measurement of dijet production with a veto on additional central jet activity in $pp$ collisions at $\sqrt{s}=7$ TeV using the ATLAS detector
917599 . Measurement of multi-jet cross sections in proton-proton collisions at a 7 TeV center-of-mass energy
917931 . Measurement of the transverse momentum distribution of Z/γ⁎ bosons in proton–proton collisions at $\sqrt{s}$=7 TeV with the ATLAS detector
919017 . Properties of jets measured from tracks in proton-proton collisions at center-of-mass energy $\sqrt{s}=7$ TeV with the ATLAS detector
920199 . Search for neutral MSSM Higgs bosons decaying to $\tau^{+}\tau^-$ pairs in proton-proton collisions at $\sqrt{s}=$ 7 TeV with the ATLAS detector
921594 . Measurement of the inclusive isolated prompt photon cross-section in $pp$ collisions at $\sqrt{s}=$ 7 TeV using 35 pb$^{-1}$ of ATLAS data
921596 . Inclusive search for same-sign dilepton signatures in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
922291 ? Search for a heavy gauge boson decaying to a charged lepton and a neutrino in 1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=$ 7 TeV using the ATLAS detector
922410 . Search for dilepton resonances in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
922601 . Measurement of the Z to tau tau Cross Section with the ATLAS Detector
924315 . Measurement of the top quark pair production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV in dilepton final states with ATLAS
924669 . Measurement of the $W \to \tau \nu_\tau$ cross section in $pp$ collisions at $\sqrt{s}=$7 TeV with the ATLAS experiment
924848 . A measurement of the ratio of the $W$ and $Z$ cross sections with exactly one associated jet in $pp$ collisions at $\sqrt{s}=$7 TeV with ATLAS
925052 ? Search for a heavy Standard Model Higgs boson in the channel $H \to ZZ \to \ell^+ \ell^− q \bar q$ using the ATLAS detector
925553 X Performance of Missing Transverse Momentum Reconstruction in Proton-Proton Collisions at 7 TeV with ATLAS
925716 . Search for the Standard Model Higgs boson in the two photon decay channel with the ATLAS detector at the LHC
925720 . Measurement of the pseudorapidity and transverse momentum dependence of the elliptic flow of charged particles in lead-lead collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector
925723 . Measurement of the centrality dependence of the charged particle pseudorapidity distribution in lead-lead collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector
925932 . Measurement of the Transverse Momentum Distribution of $W$ Bosons in $pp$ Collisions at $\sqrt{s}=7$ TeV with the ATLAS Detector
925933 . Search for New Physics in the Dijet Mass Distribution using 1 fb$^{-1}$ of $pp$ Collision Data at $\sqrt{s}=$7 TeV collected by the ATLAS Detector
926145 . Measurements of the electron and muon inclusive cross-sections in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
926641 . Measurement of the cross section for the production of a $W$ boson in association with $b^-$ jets in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
926666 . Measurement of the cross-section for $b$-jets produced in association with a $Z$ boson at $\sqrt{s}=$ 7 TeV with the ATLAS detector
927046 ? Search for displaced vertices arising from decays of new heavy particles in 7 TeV pp collisions at ATLAS
927405 . Search for a heavy neutral particle decaying into an electron and a muon using 1 fb$^{-1}$ of ATLAS data
927504 . Search for a Standard Model Higgs boson in the $H -> ZZ -> l^+l^-v\nu^-$ decay channel with the ATLAS detector
927667 ? Search for the Higgs boson in the $H -> WW -> lvjj$ decay channel in pp collisions at sqrt{s} = 7 TeV with the ATLAS detector
928224 . Search for New Phenomena in $t\bar{t}$ Events With Large Missing Transverse Momentum in Proton-Proton Collisions at $\sqrt{s}=7$ TeV with the ATLAS Detector
928289 . Measurement of the inclusive $W^\pm$ and Z/gamma cross sections in the electron and muon decay channels in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
929691 . Measurement of the jet fragmentation function and transverse profile in proton-proton collisions at a center-of-mass energy of 7 TeV with the ATLAS detector
929699 . Search for the Standard Model Higgs boson in the decay channel H→ZZ$^{(⁎)}$→4ℓ with the ATLAS detector
930002 . Search for squarks and gluinos using final states with jets and missing transverse momentum with the ATLAS detector in $\sqrt{s}=7$ TeV proton-proton collisions
930005 . Search for supersymmetry in final states with jets, missing transverse momentum and one isolated lepton in $\sqrt{s} = 7$ TeV pp collisions using 1 $fb^{-1}$ of ATLAS data
930220 . Measurement of the inclusive and dijet cross-sections of $b^-$ jets in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
-930968 . Performance of the ATLAS Trigger System in 2010
+930968 X Performance of the ATLAS Trigger System in 2010
939504 . Search for new phenomena in final states with large jet multiplicities and missing transverse momentum using $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector
939560 . Search for Massive Colored Scalars in Four-Jet Final States in $\sqrt{s}=7$ TeV proton-proton collisions with the ATLAS Detector
-940010 . Electron performance measurements with the ATLAS detector using the 2010 LHC proton-proton collision data
+940010 X Electron performance measurements with the ATLAS detector using the 2010 LHC proton-proton collision data
941539 ? Measurement of the $Z Z$ production cross section and limits on anomalous neutral triple gauge couplings in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
943401 . Searches for supersymmetry with the ATLAS detector using final states with two leptons and missing transverse momentum in $\sqrt{s}=7$ TeV proton-proton collisions
-943402 . A study of the material in the ATLAS inner detector using secondary hadronic interactions
+943402 X A study of the material in the ATLAS inner detector using secondary hadronic interactions
943969 . Search for strong gravity signatures in same-sign dimuon final states using the ATLAS detector at the LHC
944826 . Kshort and $\Lambda$ production in $pp$ interactions at $\sqrt{s}=0.9$ and 7 TeV measured with the ATLAS detector at the LHC
945498 . Measurement of the production cross section for Z/gamma* in association with jets in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
946427 . Search for diphoton events with large missing transverse momentum in fb$^{-1}$ of 7 TeV proton–proton collision data with the ATLAS detector
954993 . Measurement of the $W^\pm Z$ production cross section and limits on anomalous triple gauge couplings in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1080740 . Search for extra dimensions using diphoton events in 7 TeV proton–proton collisions with the ATLAS detector
1080891 . Search for the Higgs boson in the $H \to$ WW(*) $\to \ell_\nu\ell_\nu$ decay channel in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1081556 . Search for production of resonant states in the photon-jet mass distribution using $pp$ collisions at $\sqrt{s}=7$ TeV collected by the ATLAS detector
1081778 ? Search for scalar bottom quark pair production with the ATLAS detector in $pp$ Collisions at $\sqrt{s}=7$ TeV
1081998 ? Search for contact interactions in dilepton events from $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1082009 . Measurement of $D^{*+/-}$ meson production in jets from pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
1082275 . Search for first generation scalar leptoquarks in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
-1082461 . Observation of a new $\chi_b$ state in radiative transitions to $\Upsilon(1S)$ and $\Upsilon(2S)$ at ATLAS
+1082461 X Observation of a new $\chi_b$ state in radiative transitions to $\Upsilon(1S)$ and $\Upsilon(2S)$ at ATLAS
1082928 . Search for heavy vector-like quarks coupling to light quarks in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1082936 . Measurement of inclusive jet and dijet production in $pp$ collisions at $\sqrt{s}=7$ TeV using the ATLAS detector
-1082939 . Jet energy measurement with the ATLAS detector in proton-proton collisions at $\sqrt{s}=7$ TeV
+1082939 X Jet energy measurement with the ATLAS detector in proton-proton collisions at $\sqrt{s}=7$ TeV
1083313 . Search for anomalous production of prompt like-sign muon pairs and constraints on physics beyond the Standard Model with the ATLAS detector
1083318 . Study of jets produced in association with a $W$ boson in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1083794 . Measurement of the top quark pair production cross-section with ATLAS in the single lepton channel
1084540 . Rapidity gap cross sections measured with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV
1084697 ? Search for excited leptons in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1085980 . Search for decays of stopped, long-lived particles from 7 TeV pp collisions with the ATLAS detector
1088223 X Combined search for the Standard Model Higgs boson using up to 4.9 fb$^{-1}$ of $pp$ collision data at $\sqrt{s}=7$ TeV with the ATLAS detector at the LHC
1088224 X Search for the Standard Model Higgs boson in the diphoton decay channel with 4.9 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=7$ TeV with ATLAS
1088225 ? Search for the Standard Model Higgs boson in the decay channel $H \to ZZ^{(*)} \to 4 \ell$ with 4.8 fb$^{-1}$ of $pp$ collision data at $\sqrt{s}=7$ TeV with ATLAS
1089079 . Search for pair production of a heavy up-type quark decaying to a W boson and a b quark in the lepton+jets channel with the ATLAS detector
1089152 . Search for pair-produced heavy quarks decaying to Wq in the two-lepton channel at $\sqrt{s}=7$ TeV with the ATLAS detector
1090055 . Search for anomaly-mediated supersymmetry breaking with the ATLAS detector based on a disappearing-track signature in $pp$ collisions at $\sqrt{s}=7$ TeV
1090057 . Measurement of the cross section for top-quark pair production in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector using final states with two high-pt leptons
1090422 . Search for same-sign top-quark production and fourth-generation down-type quarks in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1091070 . Search for down-type fourth generation quarks with the ATLAS detector in events with one lepton and hadronically decaying $W$ bosons
1091481 . Measurement of the azimuthal ordering of charged hadrons with the ATLAS detector
1091527 ? Search for FCNC single top-quark production at $\sqrt{s}=7$ TeV with the ATLAS detector
1092728 . Search for new particles decaying to $Z Z$ using final states with leptons and jets with the ATLAS detector in $\sqrt{s}=7$ TeV proton-proton collisions
-1092978 . Single hadron response measurement and calorimeter jet energy scale uncertainty with the ATLAS detector at the LHC
+1092978 X Single hadron response measurement and calorimeter jet energy scale uncertainty with the ATLAS detector at the LHC
1092979 . Search for a light Higgs boson decaying to long-lived weakly-interacting particles in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1093486 . Measurement of the polarisation of $W$ bosons produced with large transverse momentum in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS experiment
1093733 . Measurement of the azimuthal anisotropy for charged particle production in $\sqrt{s_{NN}}=2.76$ TeV lead-lead collisions with the ATLAS detector
1093734 . Forward-backward correlations and charged-particle azimuthal distributions in pp interactions using the ATLAS detector
1093738 . Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1093739 . Search for second generation scalar leptoquarks in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1094061 . Measurement of inclusive two-particle angular correlations in pp collisions with the ATLAS detector at the LHC
-1094167 . Determination of the strange quark density of the proton from ATLAS measurements of the $W \to \ell \nu$ and $Z \to \ell\ell$ cross sections
-1094169 . Observation of spin correlation in $t \bar{t}$ events from pp collisions at sqrt(s) = 7 TeV using the ATLAS detector
+1094167 X Determination of the strange quark density of the proton from ATLAS measurements of the $W \to \ell \nu$ and $Z \to \ell\ell$ cross sections
+1094169 ? Observation of spin correlation in $t \bar{t}$ events from pp collisions at sqrt(s) = 7 TeV using the ATLAS detector
1094175 . Measurement of the charge asymmetry in top quark pair production in $pp$ collisions at $\sqrt{s}=7$ TeV using the ATLAS detector
-1094564 . Jet mass and substructure of inclusive jets in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS experiment
+1094564 ! Jet mass and substructure of inclusive jets in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS experiment
1094568 . Measurement of $t \bar{t}$ production with a veto on additional central jet activity in pp collisions at sqrt(s) = 7 TeV using the ATLAS detector
1094857 . Search for heavy neutrinos and right-handed $W$ bosons in events with two leptons and jets in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
-1094859 . Measurement of the top quark mass with the template method in the $t \bar{t}$ -> lepton + jets channel using ATLAS data
+1094859 ? Measurement of the top quark mass with the template method in the $t \bar{t}$ -> lepton + jets channel using ATLAS data
1094860 . Search for gluinos in events with two same-sign leptons, jets and missing transverse momentum with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV
1095236 . Search for supersymmetry in $pp$ collisions at $\sqrt{s}=7$ TeV in final states with missing transverse momentum and $b^-$ jets with the ATLAS detector
1095238 . Measurement of the $W W$ cross section in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector and limits on anomalous gauge couplings
1095404 . Search for events with large missing transverse momentum, jets, and at least two tau leptons in 7 TeV proton–proton collision data with the ATLAS detector
1102909 . Search for the decay $B_s^0 \to \mu \mu$ with the ATLAS detector
1104755 . Search for pair production of a new quark that decays to a Z boson and a bottom quark with the ATLAS detector
1107731 . Search for resonant $WZ$ production in the $WZ \to \ell \nu \ell^\prime\ell^\prime$ channel in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector
1110689 . Search for charged Higgs bosons decaying via $H^{+} \to \tau \nu$ in top quark pair events using $pp$ collision data at $\sqrt{s}=7$ TeV with the ATLAS detector
1111144 . Search for supersymmetry with jets, missing transverse momentum and at least one hadronically decaying $\tau$ lepton in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1111820 . Search for TeV-scale gravity signatures in final states with leptons and jets with the ATLAS detector at $\sqrt{s}=7$ TeV
1112263 . Search for supersymmetry in events with three leptons and missing transverse momentum in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector
1112906 . Measurement of $\tau$ polarization in $W -> \tau \nu$ decays with the ATLAS detector in pp collisions at sqrt(s) = 7 TeV
1112907 ? Search for scalar top quark pair production in natural gauge mediated supersymmetry models with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV
1113444 ? Search for a fermiophobic Higgs boson in the diphoton decay channel with the ATLAS detector
1113445 . Search for lepton flavour violation in the emu continuum with the ATLAS detector in $\sqrt{s}=7$ TeV $pp$ collisions at the LHC
1113597 . Search for tb resonances in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1114034 . Measurement of the top quark pair cross section with ATLAS in $pp$ collisions at $\sqrt{s} =$ 7 TeV using final states with an electron or a muon and a hadronically decaying $\tau$ lepton
1114314 . Measurement of the W boson polarization in top quark decays with the ATLAS detector
1114319 . Measurement of $W \gamma$ and $Z \gamma$ production cross sections in $pp$ collisions at $\sqrt{s}=7$ TeV and limits on anomalous triple gauge couplings with the ATLAS detector
1114487 . Measurement of the $t$-channel single top-quark production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1115822 . A search for $t\bar{t}$ resonances with the ATLAS detector in 2.05 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=7$ TeV
1116151 . Evidence for the associated production of a $W$ boson and a top quark in ATLAS at $\sqrt{s}=7$ TeV
1116532 . Search for a standard sodel Higgs boson in the H $\to$ ZZ $\to \ell^{+}\ell^{-}\nu \bar{\nu}$ decay channel using 4.7 fb$^{-1}$ of $\sqrt{s} =$ 7 TeV data with the ATLAS detector
1116876 . A search for flavour changing neutral currents in top-quark decays in $pp$ collision data collected with the ATLAS detector at $\sqrt{s}=7$ TeV
1117206 . Search for the Standard Model Higgs boson in the $H \to$ WW(*) $\to \ell \nu \ell \nu$ decay mode with 4.7 /fb of ATLAS data at $\sqrt{s}=7$ TeV
1117704 . Hunt for new phenomena using large jet multiplicities and missing transverse momentum with ATLAS in 4.7 fb$^{-1}$ of $\sqrt{s}=7$ TeV proton-proton collisions
-1117887 . Measurement of event shapes at large momentum transfer with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV
+1117887 ! Measurement of event shapes at large momentum transfer with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV
1118040 . Search for a standard model Higgs boson in the mass range 200-600 GeV in the $H \to ZZ \to \ell^+ \ell^- q \bar{q}$ decay channel with the ATLAS detector
-1118269 . Measurement of the b-hadron production cross section using decays to $D^{*}\mu^-X$ final states in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
-1119557 . ATLAS Measurements of the Properties of Jets for Boosted Particle Searches
+1118269 ? Measurement of the b-hadron production cross section using decays to $D^{*}\mu^-X$ final states in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
+1119557 ! ATLAS Measurements of the Properties of Jets for Boosted Particle Searches
1120011 . Search for the Standard Model Higgs boson in the $H$ to $\tau^{+} \tau^{-}$ decay mode in $\sqrt{s}=7$ TeV $pp$ collisions with ATLAS
1120014 . Search for the Higgs boson in the $H \to W W \to$ lnujj decay channel at $\sqrt{s}=7$ TeV with the ATLAS detector
1120736 ? Search for the Standard Model Higgs boson produced in association with a vector boson and decaying to a $b$-quark pair with the ATLAS detector
1120741 X Combined search for the Standard Model Higgs boson in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector
-1121875 . Measurement of the $Λ_b^0$ lifetime and mass in the ATLAS experiment
+1121875 ? Measurement of the $Λ_b^0$ lifetime and mass in the ATLAS experiment
1121877 . A search for $t\bar{t}$ resonances in lepton+jets events with highly boosted top quarks collected in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector
1123116 . Search for top and bottom squarks from gluino pair production in final states with missing transverse energy and at least three b-jets with the ATLAS detector
-1123657 . Measurements of top quark pair relative differential cross-sections with ATLAS in $pp$ collisions at $\sqrt{s}=7$ TeV
+1123657 ! Measurements of top quark pair relative differential cross-sections with ATLAS in $pp$ collisions at $\sqrt{s}=7$ TeV
1124035 ? Search for magnetic monopoles in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector
1124167 . Measurement of charged-particle event shape variables in $\sqrt{s}=7$ TeV proton-proton interactions with the ATLAS detector
1124337 X Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC
1125575 . Underlying event characteristics and their dependence on jet size of charged-particle jet events in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
-1125576 . Time-dependent angular analysis of the decay $B_{s}^{0} \to J/{\psi\phi}$ and extraction of $\Delta\Gamma_{s}$ and the CP-violating weak phase $\phi_s$ by ATLAS
+1125576 ? Time-dependent angular analysis of the decay $B_{s}^{0} \to J/{\psi\phi}$ and extraction of $\Delta\Gamma_{s}$ and the CP-violating weak phase $\phi_s$ by ATLAS
1125961 . Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using 4.7 fb$^{-1}$ of $\sqrt{s}=7$ TeV proton-proton collision data
1126131 . Measurement of $WZ$ production in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1126136 . Search for a supersymmetric partner to the top quark in final states with jets and missing transverse momentum at $\sqrt{s}=7$ TeV with the ATLAS detector
1126965 . Measurement of the jet radius and transverse momentum dependence of inclusive jet suppression in lead-lead collisions at $\sqrt{s_{NN}}$= 2.76 TeV with the ATLAS detector
1127331 . Search for direct top squark pair production in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}=7$ TeV $pp$ collisions using 4.7 $fb^{-1}$ of ATLAS data
1127504 . Search for new phenomena in the $W W$ to $\ell \nu \ell$' $\nu$' final state in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1127505 . Search for direct slepton and gaugino production in final states with two leptons and missing transverse momentum with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV
1127601 . Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector
1128464 . Search for light scalar top quark pair production in final states with two leptons with the ATLAS detector in $\sqrt{s}=7$ TeV proton-proton collisions
1180197 . Further search for supersymmetry at $\sqrt{s}=7$ TeV in final states with jets, missing transverse momentum and isolated leptons with the ATLAS detector
1183818 . Measurements of the pseudorapidity dependence of the total transverse energy in proton-proton collisions at $\sqrt{s}=7$ TeV with ATLAS
1184351 ? Search for diphoton events with large missing transverse momentum in 7 TeV proton-proton collision data with the ATLAS detector
-1184943 . Prototype ATLAS IBL Modules using the FE-I4A Front-End Readout Chip
+1184943 X Prototype ATLAS IBL Modules using the FE-I4A Front-End Readout Chip
1184952 . Search for light top squark pair production in final states with leptons and $b^-$ jets with the ATLAS detector in $\sqrt{s}=7$ TeV proton-proton collisions
1185259 . Search for high-mass resonances decaying to dilepton final states in pp collisions at s**(1/2) = 7-TeV with the ATLAS detector
1186556 . Search for a heavy top-quark partner in final states with two leptons with the ATLAS detector at the LHC
1186731 . ATLAS search for a heavy gauge boson decaying to a charged lepton and a neutrino in $pp$ collisions at $\sqrt{s}=7$ TeV
1186740 . Search for dark matter candidates and large extra dimensions in events with a photon and missing transverse momentum in $pp$ collision data at $\sqrt{s}=7$ TeV with the ATLAS detector
1188681 . Search for resonant top plus jet production in $t\bar{t}$ + jets events with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV
1188890 . Search for displaced muonic lepton jets from light Higgs boson decay in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1188891 . Measurement of the flavour composition of dijet events in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1189432 ? Search for Supersymmetry in Events with Large Missing Transverse Momentum, Jets, and at Least One Tau Lepton in 7 TeV Proton-Proton Collision Data with the ATLAS Detector
1189659 . ATLAS search for new phenomena in dijet mass and angular distributions using $pp$ collisions at $\sqrt{s}=7$ TeV
1190185 ? Search for direct chargino production in anomaly-mediated supersymmetry breaking models based on a disappearing-track signature in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1190187 . Measurement of $W^+W^-$ production in pp collisions at $\sqrt{s}$=7  TeV with the ATLAS detector and limits on anomalous WWZ and WWγ couplings
1190891 . Search for R-parity-violating supersymmetry in events with four or more leptons in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector
1190892 . Search for dark matter candidates and large extra dimensions in events with a jet and missing transverse momentum with the ATLAS detector
1190896 . Search for anomalous production of prompt like-sign lepton pairs at $\sqrt{s}=7$ TeV with the ATLAS detector
1191022 . Search for pair production of massive particles decaying into three quarks with the ATLAS detector in $\sqrt{s}=7$ TeV $pp$ collisions at the LHC
1191023 ? Search for pair-produced massive coloured scalars in four-jet final states with the ATLAS detector in proton-proton collisions at $\sqrt{s}=7$ TeV
1191430 . Search for doubly-charged Higgs bosons in like-sign dilepton final states at $\sqrt{s}=7$ TeV with the ATLAS detector
1191898 . Search for pair production of heavy top-like quarks decaying to a high-pT $W$ boson and a $b$ quark in the lepton plus jets final state at $\sqrt{s}$=7 TeV with the ATLAS detector
-1192920 . Jet energy resolution in proton-proton collisions at $\sqrt{s}=7$ TeV recorded in 2010 with the ATLAS detector
+1192920 X Jet energy resolution in proton-proton collisions at $\sqrt{s}=7$ TeV recorded in 2010 with the ATLAS detector
1193044 . Measurement of $Z$ boson Production in Pb+Pb Collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS Detector
1193050 . A search for high-mass resonances decaying to $\tau^+\tau^-$ in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1193933 . Search for long-lived, heavy particles in final states with a muon and multi-track displaced vertex in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
-1194807 . The ATLAS Trigger/DAQ Authorlist, version 4.0
-1196722 . Muon Detection Based on a Hadronic Calorimeter
+1194807 X The ATLAS Trigger/DAQ Authorlist, version 4.0
+1196722 X Muon Detection Based on a Hadronic Calorimeter
1197323 ? Search for Extra Dimensions in diphoton events using proton-proton collisions recorded at $\sqrt{s}=7$ TeV with the ATLAS detector at the LHC
1198341 ? Search for contact interactions and large extra dimensions in dilepton events from $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1198427 ? Search for supersymmetry in events with photons, bottom quarks, and missing transverse momentum in proton–proton collisions at a centre-of-mass energy of 7 TeV with the ATLAS detector
1199005 ? Searches for heavy long-lived sleptons and R-Hadrons with the ATLAS detector in $pp$ collisions at $\sqrt{s}=7$ TeV
1199269 . Measurement of isolated-photon pair production in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1201945 ? Search for resonances decaying into top-quark pairs using fully hadronic decays in $pp$ collisions with ATLAS at $\sqrt{s}=7$ TeV
1203852 . Measurement of $ZZ$ production in $pp$ collisions at $\sqrt{s}=7$ TeV and limits on anomalous $ZZZ$ and $ZZ\gamma$ couplings with the ATLAS detector
1204447 . Search for new phenomena in events with three charged leptons at $/sqrt{s}$ = 7 TeV with the ATLAS detector
1204784 . Measurement of angular correlations in Drell-Yan lepton pairs to probe Z/gamma* boson transverse momentum at sqrt(s)=7 TeV with the ATLAS detector
1204786 ? Search for the neutral Higgs bosons of the Minimal Supersymmetric Standard Model in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1204991 . Measurement of the ttbar production cross section in the tau+jets channel using the ATLAS detector
1204994 . Measurement of Upsilon production in 7 TeV pp collisions at ATLAS
1205881 ? Search for a heavy narrow resonance decaying to $e \mu$, $e \tau$, or $\mu \tau$ with the ATLAS detector in $\sqrt{s}=7$ TeV $pp$ collisions at the LHC
1207451 ? Search for charged Higgs bosons through the violation of lepton universality in $t\bar{t}$ events using $pp$ collision data at $\sqrt{s}=7$ TeV with the ATLAS experiment
1208304 ? Observation of Associated Near-Side and Away-Side Long-Range Correlations in $\sqrt{s_{NN}}$=5.02  TeV Proton-Lead Collisions with the ATLAS Detector
1208548 ? A search for prompt lepton-jets in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1208701 ? Multi-channel search for squarks and gluinos in $\sqrt{s}=7$ TeV $pp$ collisions with the ATLAS detector
1209719 ? Search for single $b^*$-quark production with the ATLAS detector at $\sqrt{s}=7$ TeV
-1210114 . Evaluation of the local hadronic calibration with combined beam-test data for the endcap and forward calorimeters of ATLAS in the pseudorapidity region 2.5 < |eta| < 4.0
+1210114 X Evaluation of the local hadronic calibration with combined beam-test data for the endcap and forward calorimeters of ATLAS in the pseudorapidity region 2.5 < |eta| < 4.0
1215605 ? Search for long-lived, multi-charged particles in pp collisions at $\sqrt{s}$=7 TeV using the ATLAS detector
1216670 . Measurement of hard double-parton interactions in $W(\to l\nu)$+ 2 jet events at $\sqrt{s}$=7 TeV with the ATLAS detector
1217863 . Measurements of $W \gamma$ and $Z \gamma$ production in $pp$ collisions at $\sqrt{s}$=7  TeV with the ATLAS detector at the LHC
1217867 . Measurement of kT splitting scales in W->lv events at sqrt(s)=7 TeV with the ATLAS detector
1219109 . Measurement of the cross-section for W boson production in association with b-jets in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector
1219797 ? Search for a light charged Higgs boson in the decay channel $H^+ \to c\bar{s}$ in $t\bar{t}$ events using pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector
1219960 X Improved luminosity determination in pp collisions at sqrt(s) = 7 TeV using the ATLAS detector at the LHC
1219961 ? Search for WH production with a light Higgs boson decaying to prompt electron-jets in proton-proton collisions at $\sqrt{s}$=7 TeV with the ATLAS detector
1222129 X Characterisation and mitigation of beam-induced backgrounds observed in the ATLAS detector during the 2011 proton-proton run
1222326 ? Search for third generation scalar leptoquarks in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector
1223123 . Measurement with the ATLAS detector of multi-particle azimuthal correlations in p+Pb collisions at $\sqrt{s_{NN}}$ =5.02 TeV
1223730 X A particle consistent with the Higgs Boson observed with the ATLAS Detector at the Large Hadron Collider
-1228693 . Measurement of the inclusive jet cross section in pp collisions at sqrt(s)=2.76 TeV and comparison to the inclusive jet cross section at sqrt(s)=7 TeV using the ATLAS detector
+1228693 ! Measurement of the inclusive jet cross section in pp collisions at sqrt(s)=2.76 TeV and comparison to the inclusive jet cross section at sqrt(s)=7 TeV using the ATLAS detector
1229502 ? Search for nonpointing photons in the diphoton and $E^{miss}_T$ final state in $\sqrt{s}$=7  TeV proton-proton collisions using the ATLAS detector
1229507 ? Study of heavy-flavor quarks produced in association with top-quark pairs at $\sqrt{s}=7$  TeV using the ATLAS detector
-1230812 . Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector
+1230812 ! Measurement of the production cross section of jets in association with a Z boson in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector
1231616 ? Search for resonant diboson production in the WW/WZ→ℓνjj decay channels with the ATLAS detector at $\sqrt{s}$ = 7  TeV
1232965 X Triggers for displaced decays of long-lived neutral particles in the ATLAS detector
1233089 ? Search for $t\bar t$ resonances in the lepton plus jets final state with ATLAS using 4.7 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 7$ TeV
1233359 . Measurement of the distributions of event-by-event flow harmonics in lead-lead collisions at = 2.76 TeV with the ATLAS detector at the LHC
1234228 . Measurement of the high-mass Drell--Yan differential cross-section in pp collisions at sqrt(s)=7 TeV with the ATLAS detector
-1239348 . Performance of jet substructure techniques for large-$R$ jets in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector
+1239348 ? Performance of jet substructure techniques for large-$R$ jets in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector
1240088 . Measurement of the Azimuthal Angle Dependence of Inclusive Jet Yields in Pb+Pb Collisions at $\sqrt{s_{NN}}=$ 2.76 TeV with the ATLAS detector
1240670 . Measurement of the differential cross-section of $B^{+}$ meson production in pp collisions at $\sqrt{s}$ = 7 TeV at ATLAS
-1241574 . Measurements of Higgs boson production and couplings in diboson final states with the ATLAS detector at the LHC
+1241574 ? Measurements of Higgs boson production and couplings in diboson final states with the ATLAS detector at the LHC
1241575 X Evidence for the spin-0 nature of the Higgs boson using ATLAS data
-1243158 . Measurement of the top quark charge in $pp$ collisions at $\sqrt{s} =$ 7 TeV with the ATLAS detector
-1243871 . Measurement of jet shapes in top-quark pair events at $\sqrt{s}$ = 7 TeV using the ATLAS detector
+1243158 ? Measurement of the top quark charge in $pp$ collisions at $\sqrt{s} =$ 7 TeV with the ATLAS detector
+1243871 ! Measurement of jet shapes in top-quark pair events at $\sqrt{s}$ = 7 TeV using the ATLAS detector
1244318 . Measurement of Top Quark Polarization in Top-Antitop Events from Proton-Proton Collisions at $\sqrt{s}$ = 7  TeV Using the ATLAS Detector
1244522 . Dynamics of isolated-photon plus jet production in pp collisions at $\sqrt(s)=7$ TeV with the ATLAS detector
1246787 ? Search for excited electrons and muons in $\sqrt{s}$=8 TeV proton-proton collisions with the ATLAS detector
1247060 ? Search for new phenomena in final states with large jet multiplicities and missing transverse momentum at $\sqrt{s}$=8 TeV proton-proton collisions using the ATLAS experiment
1247462 ? Search for direct third-generation squark pair production in final states with missing transverse momentum and two $b$-jets in $\sqrt{s} =$ 8 TeV $pp$ collisions with the ATLAS detector
1249597 ? Search for microscopic black holes in a like-sign dimuon final state using large track multiplicity with the ATLAS detector
1253852 . Search for new phenomena in photon+jet events collected in proton--proton collisions at sqrt(s) = 8 TeV with the ATLAS detector
1254228 ? Search for dark matter in events with a hadronically decaying W or Z boson and missing transverse momentum in $pp$ collisions at $\sqrt{s} =$ 8 TeV with the ATLAS detector
1258398 ? Search for charginos nearly mass degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at $\sqrt(s)$=8  TeV with the ATLAS detector
1261966 X Measurement of the mass difference between top and anti-top quarks in pp collisions at $\sqrt(s) = 7$ TeV using the ATLAS detector
1261968 ? Search for long-lived stopped R-hadrons decaying out-of-time with pp collisions using the ATLAS detector
1263495 . Measurement of the inclusive isolated prompt photons cross section in pp collisions at $\sqrt{s}=7$  TeV with the ATLAS detector using 4.6  fb$^{−1}$
-1263563 . Mechanical construction and installation of the ATLAS tile calorimeter
+1263563 X Mechanical construction and installation of the ATLAS tile calorimeter
1263762 ? Search for Quantum Black Hole Production in High-Invariant-Mass Lepton$+$Jet Final States Using $pp$ Collisions at $\sqrt{s} =$ 8  TeV and the ATLAS Detector
-1266254 . Measurement of the top quark pair production charge asymmetry in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector <james.ferrando@cern.ch>
+1266254 . Measurement of the top quark pair production charge asymmetry in proton-proton collisions at $\sqrt{s}$ = 7 TeV using the ATLAS detector <james.ferrando@cern.ch>
1266438 X Standalone vertex finding in the ATLAS muon spectrometer
1268153 ? Search for a multi-Higgs-boson cascade in $W^+W^−b\bar{b}$ events with the ATLAS detector in pp collisions at $\sqrt{s} = 8$  TeV
1268975 . Measurement of dijet cross sections in $pp$ collisions at 7 TeV centre-of-mass energy using the ATLAS detector
1276825 . Measurement of the production cross section of prompt $J/\psi$ mesons in association with a $W^\pm$ boson in $pp$ collisions at $\sqrt{s} =$ 7 TeV with the ATLAS detector
1279489 . Measurement of the electroweak production of dijets in association with a Z-boson and distributions sensitive to vector boson fusion in proton-proton collisions at $\sqrt{s} =$ 8 TeV using the ATLAS detector
1281233 ? Search for Higgs boson decays to a photon and a Z boson in pp collisions at $\sqrt{s}$=7 and 8 TeV with the ATLAS detector
1281236 ? Search for Invisible Decays of a Higgs Boson Produced in Association with a Z Boson in ATLAS
1282441 . The differential production cross section of the $\phi $ (1020) meson in $\sqrt{s}$ = 7 TeV $pp$ collisions measured with the ATLAS detector
1282447 . Measurement of the production of a $W$ boson in association with a charm quark in $pp$ collisions at $\sqrt{s} =$ 7 TeV with the ATLAS detector
1282905 ? Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in $\sqrt{s} =$ 8TeV $pp$ collisions with the ATLAS detector
1283339 . Measurement of event-plane correlations in $\sqrt{s_{NN}}=2.76$ TeV lead-lead collisions with the ATLAS detector
1286444 ? Search for direct top-squark pair production in final states with two leptons in pp collisions at $\sqrt{s} =$ 8TeV with the ATLAS detector
1286622 ? Search for direct top squark pair production in events with a Z boson, b-jets and missing transverse momentum in sqrt(s)=8 TeV pp collisions with the ATLAS detector
1286761 ? Search for direct production of charginos, neutralinos and sleptons in final states with two leptons and missing transverse momentum in $pp$ collisions at $\sqrt{s} =$ 8 TeV with the ATLAS detector
-1286892 . Measurements of Four-Lepton Production at the Z Resonance in pp Collisions at $\sqrt s=$7 and 8 TeV with ATLAS
+1286892 X Measurements of Four-Lepton Production at the Z Resonance in pp Collisions at $\sqrt s=$7 and 8 TeV with ATLAS
1287055 ? Search for top quark decays $t \to qH$ with $H \to \gamma\gamma$ using the ATLAS detector
1288061 ? Search for dark matter in events with a Z boson and missing transverse momentum in pp collisions at $\sqrt{s}$=8 TeV with the ATLAS detector
1288490 X Measurement of the parity-violating asymmetry parameter $\alpha_b$ and the helicity amplitudes for the decay $\Lambda_b^0\to J/\psi+\Lambda^0$ with the ATLAS detector
-1288706 . Measurement of the low-mass Drell-Yan differential cross section at $\sqrt{s}$ = 7 TeV using the ATLAS detector
+1288706 ! Measurement of the low-mass Drell-Yan differential cross section at $\sqrt{s}$ = 7 TeV using the ATLAS detector
1289059 X Electron reconstruction and identification efficiency measurements with the ATLAS detector using the 2011 LHC proton-proton collision data
1289225 ? Search for supersymmetry at $\sqrt{s}$=8 TeV in final states with jets and two same-sign leptons or three leptons with the ATLAS detector
1291133 X Muon reconstruction efficiency and momentum resolution of the ATLAS experiment in proton-proton collisions at $\sqrt{s}$ = 7 TeV in 2010
-1292798 . Measurement of $\chi_{c1}$ and $\chi_{c2}$ production with $\sqrt{s}$ = 7 TeV $pp$ collisions at ATLAS
+1292798 ? Measurement of $\chi_{c1}$ and $\chi_{c2}$ production with $\sqrt{s}$ = 7 TeV $pp$ collisions at ATLAS
1292799 . Measurement of the cross section of high transverse momentum $Z\rightarrow b\bar{b}$ production in proton--proton collisions at $\sqrt{s}=8 TeV$ with the ATLAS Detector
1293018 X Operation and performance of the ATLAS semiconductor tracker
1296250 X Monitoring and data quality assessment of the ATLAS liquid argon calorimeter
1296260 . Measurement of the centrality and pseudorapidity dependence of the integrated elliptic flow in lead-lead collisions at $\sqrt{s_{\mathrm {NN}}}=2.76$ TeV with the ATLAS detector
1296830 ? Search for high-mass dilepton resonances in pp collisions at $\sqrt{s}=8$  TeV with the ATLAS detector
1296834 ? Search for microscopic black holes and string balls in final states with leptons and jets with the ATLAS detector at sqrt(s) = 8 TeV
1297226 ? Search for supersymmetry in events with four or more leptons in $\sqrt{s}$ = 8 TeV pp collisions with the ATLAS detector
-1298023 . Evidence for Electroweak Production of $W^{\pm}W^{\pm}jj$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector
+1298023 ? Evidence for Electroweak Production of $W^{\pm}W^{\pm}jj$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector
1298030 X Light-quark and gluon jet discrimination in $pp$ collisions at $\sqrt{s}=7\mathrm {\ TeV}$ with the ATLAS detector
1298722 ? Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using $\sqrt{s}=8$ TeV proton--proton collision data
1298805 X Jet energy measurement and its systematic uncertainty in proton-proton collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
-1298811 . Measurement of the underlying event in jet events from 7 TeV proton-proton collisions with the ATLAS detector
+1298811 ! Measurement of the underlying event in jet events from 7 TeV proton-proton collisions with the ATLAS detector
1299143 ? Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1300152 . Measurement of inclusive jet charged-particle fragmentation functions in Pb+Pb collisions at $\sqrt{s_{NN}}=2.76$ TeV with the ATLAS detector
1300647 . Measurement of the $Z/\gamma^*$ boson transverse momentum distribution in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector
1300650 X Measurement of the Higgs boson mass from the $H\rightarrow \gamma\gamma$ and $H \rightarrow ZZ^{*} \rightarrow 4\ell$ channels with the ATLAS detector using 25 fb$^{-1}$ of $pp$ collision data
1300821 ? Search for WZ resonances in the fully leptonic channel using pp collisions at sqrt(s) = 8 TeV with the ATLAS detector
1301558 ? Search For Higgs Boson Pair Production in the $\gamma\gamma b\bar{b}$ Final State using $pp$ Collision Data at $\sqrt{s}=8$ TeV from the ATLAS Detector
1301856 . Measurement of the $t\bar{t}$ production cross-section using $e\mu $ events with b-tagged jets in pp collisions at $\sqrt{s}$ = 7 and 8  $\,\mathrm{TeV}$ with the ATLAS detector <neil.warrack@cern.ch>
1303897 ? Search for the Standard Model Higgs boson decay to $\mu^{+}\mu^{-}$ with the ATLAS detector
1303898 X A neural network clustering algorithm for the ATLAS silicon pixel detector
1303905 . Comprehensive measurements of $t$-channel single top-quark production cross sections at $\sqrt{s} = 7$ TeV with the ATLAS detector
1304288 ? Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1304289 ! Measurements of normalized differential cross sections for $t\bar{t}$ production in pp collisions at $\sqrt{s}=7$  TeV using the ATLAS detector <neil.warrack@cern.ch>
1304455 ! Simultaneous measurements of the $t\bar{t}$, $W^+W^-$, and $Z/\gamma^{*}\rightarrow\tau\tau$ production cross-sections in $pp$ collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector
1304456 ? Search for top squark pair production in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt s =$8 TeV $pp$ collisions with the ATLAS detector
1304457 ? Search for strong production of supersymmetric particles in final states with missing transverse momentum and at least three $b$-jets at $\sqrt{s}$= 8 TeV proton-proton collisions with the ATLAS detector
1304458 ? Search for supersymmetry in events with large missing transverse momentum, jets, and at least one tau lepton in 20 fb$^{-1}$ of $\sqrt{s}=$ 8 TeV proton-proton collision data with the ATLAS detector
1304459 ? Search for pair-produced third-generation squarks decaying via charm quarks or in compressed supersymmetric scenarios in $pp$ collisions at $\sqrt{s}=8~$TeV with the ATLAS detector
1304687 ! Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in $pp$ collisions at ${\sqrt{s}}$ = 7 TeV with the ATLAS detector
1304688 . Measurement of the $ t\overline{t} $ production cross-section as a function of jet multiplicity and jet transverse momentum in 7 TeV proton-proton collisions with the ATLAS detector
1304691 ? Observation of an Excited $B_c^\pm$ Meson State with the ATLAS Detector
1305096 ? Search for new phenomena in the dijet mass distribution using $p-p$ collision data at $\sqrt{s}=8$ TeV with the ATLAS detector
-1305098 . Flavor tagged time-dependent angular analysis of the $B_s \rightarrow J/\psi \phi$ decay and extraction of $\Delta\Gamma$s and the weak phase $\phi_s$ in ATLAS
+1305098 ? Flavor tagged time-dependent angular analysis of the $B_s \rightarrow J/\psi \phi$ decay and extraction of $\Delta\Gamma$s and the weak phase $\phi_s$ in ATLAS
1305430 ? Search for contact interactions and large extra dimensions in the dilepton channel using proton-proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
-1306294 . Measurement of differential production cross-sections for a $Z$ boson in association with $b$-jets in 7 TeV proton-proton collisions with the ATLAS detector
+1306294 ! Measurement of differential production cross-sections for a $Z$ boson in association with $b$-jets in 7 TeV proton-proton collisions with the ATLAS detector
1306491 X Measurement of the muon reconstruction performance of the ATLAS detector using 2011 and 2012 LHC proton–proton collision data
-1306615 . Measurements of fiducial and differential cross sections for Higgs boson production in the diphoton decay channel at $\sqrt{s}=8$ TeV with ATLAS
-1306619 . Measurements of spin correlation in top-antitop quark events from proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector
+1306615 ! Measurements of fiducial and differential cross sections for Higgs boson production in the diphoton decay channel at $\sqrt{s}=8$ TeV with ATLAS
+1306619 ! Measurements of spin correlation in top-antitop quark events from proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector
1306905 X Electron and photon energy calibration with the ATLAS detector using LHC Run 1 data
1307103 . Measurement of the production cross-section of $\psi(2S) \to J/\psi ( \to \mu^{+} \mu^{-}) \pi^{+} \pi^{-}$ in pp collisions at $ \sqrt{s} $ = 7 TeV at ATLAS
-1307243 . Measurements of jet vetoes and azimuthal decorrelations in dijet events produced in $pp$ collisions at $\sqrt{s}=7\,\mathrm{TeV}$ using the ATLAS detector
+1307243 ! Measurements of jet vetoes and azimuthal decorrelations in dijet events produced in $pp$ collisions at $\sqrt{s}=7\,\mathrm{TeV}$ using the ATLAS detector
1307756 . Search for Scalar Diphoton Resonances in the Mass Range $65-600$ GeV with the ATLAS Detector in $pp$ Collision Data at $\sqrt{s}$ = 8 $TeV$
1308524 ? Search for new particles in events with one lepton and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1308923 ? Search for new resonances in $W\gamma$ and $Z\gamma$ final states in $pp$ collisions at $\sqrt s=8$ TeV with the ATLAS detector
1309877 ? Search for $W' \rightarrow tb \rightarrow qqbb$ decays in $pp$ collisions at $\sqrt{s}$  = 8 TeV with the ATLAS detector
1310834 X Performance of the ATLAS muon trigger in pp collisions at $\sqrt{s}=8$ TeV
-1310835 . Fiducial and differential cross sections of Higgs boson production measured in the four-lepton decay channel in $pp$ collisions at $\sqrt{s}$=8 TeV with the ATLAS detector
+1310835 ! Fiducial and differential cross sections of Higgs boson production measured in the four-lepton decay channel in $pp$ collisions at $\sqrt{s}$=8 TeV with the ATLAS detector
1311487 . Measurement of flow harmonics with multi-particle cumulants in Pb+Pb collisions at $\sqrt{s_{\mathrm {NN}}}=2.76$  TeV with the ATLAS detector
1311623 . Measurement of the production and lepton charge asymmetry of $W$ bosons in Pb+Pb collisions at $\mathbf {\sqrt{\mathbf {s}_{\mathrm {\mathbf {NN}}}}=2.76\;TeV}$ with the ATLAS detector
1311990 . Measurements of Higgs boson production and couplings in the four-lepton channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
1312169 ? Search for the lepton flavor violating decay Z→eμ in pp collisions at $\sqrt{s}$  TeV with the ATLAS detector
1312171 . Measurement of the total cross section from elastic scattering in pp collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1312627 . A measurement of the ratio of the production cross sections for $W$ and $Z$ bosons in association with jets with the ATLAS detector
-1312978 . Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
+1312978 ? Measurement of Higgs boson production in the diphoton decay channel in pp collisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector
1313596 ? Search for long-lived neutral particles decaying into lepton jets in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
-1313597 . Measurement of the top-quark mass in the fully hadronic decay channel from ATLAS data at $\sqrt{s}=7\mathrm{\,TeV}$
+1313597 ? Measurement of the top-quark mass in the fully hadronic decay channel from ATLAS data at $\sqrt{s}=7\mathrm{\,TeV}$
1315325 . Measurement of long-range pseudorapidity correlations and azimuthal harmonics in $\sqrt{s_{NN}}=5.02$ TeV proton-lead collisions with the ATLAS detector
1315819 ? Search for $H \to \gamma\gamma$ produced in association with top quarks and constraints on the Yukawa coupling between the top quark and the Higgs boson using data taken at 7 TeV and 8 TeV with the ATLAS detector
-1315949 . Measurement of distributions sensitive to the underlying event in inclusive Z-boson production in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
+1315949 ! Measurement of distributions sensitive to the underlying event in inclusive Z-boson production in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1318334 ? Search for pair and single production of new heavy quarks that decay to a $Z$ boson and a third-generation quark in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1318336 ? Search for nonpointing and delayed photons in the diphoton and missing transverse momentum final state in 8 TeV $pp$ collisions at the LHC using the ATLAS detector
1318481 ? Search for neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1318483 ? Search for resonant diboson production in the $\mathrm {\ell \ell }q\bar{q}$ final state in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
1318484 ? Search for the $b\bar{b}$ decay of the Standard Model Higgs boson in associated $(W/Z)H$ production with the ATLAS detector
-1319490 . Measurements of the W production cross sections in association with jets with the ATLAS detector
+1319490 ! Measurements of the W production cross sections in association with jets with the ATLAS detector
1319760 ? Search for $s$-channel single top-quark production in proton–proton collisions at $\sqrt s=8$ TeV with the ATLAS detector
1322381 ? Search for dark matter in events with heavy quarks and missing transverse momentum in $pp$ collisions with the ATLAS detector
1322383 ? Search for $W' \to t\bar{b}$ in the lepton plus jets final state in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}$ = 8 TeV with the ATLAS detector
1322568 ? Search for the $X_b$ and other hidden-beauty states in the $\pi^+ \pi^- \Upsilon(1 \rm S)$ channel at ATLAS
1322928 ? Search for invisible particles produced in association with single-top-quarks in proton-proton collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1324374 . Measurement of the $WW+WZ$ cross section and limits on anomalous triple gauge couplings using final states with one lepton, missing transverse momentum, and two jets with the ATLAS detector at $\sqrt{\rm{s}} = 7$ TeV
1325553 . Measurement of the inclusive jet cross-section in proton-proton collisions at $ \sqrt{s}=7 $ TeV using 4.5 fb$^{−1}$ of data with the ATLAS detector
1326409 ? Search for new phenomena in events with a photon and missing transverse momentum in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1326641 . Measurement of three-jet production cross-sections in $pp$ collisions at 7 TeV centre-of-mass energy using the ATLAS detector
-1326911 . Measurements of the Nuclear Modification Factor for Jets in Pb+Pb Collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV with the ATLAS Detector
+1326911 ? Measurements of the Nuclear Modification Factor for Jets in Pb+Pb Collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$ TeV with the ATLAS Detector
1327229 . Search for new phenomena in events with three or more charged leptons in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1329957 ? Searches for heavy long-lived charged particles with the ATLAS detector in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1331782 ? Search for anomalous production of prompt same-sign lepton pairs and pair-produced doubly charged Higgs bosons with $ \sqrt{s}=8 $ TeV $pp$ collisions using the ATLAS detector
1332748 . Measurement of the transverse polarization of $\Lambda$ and $\bar{\Lambda}$ hyperons produced in proton-proton collisions at $\sqrt{s}=7$ TeV using the ATLAS detector
-1333228 . Observation and measurement of Higgs boson decays to WW$^*$ with the ATLAS detector
+1333228 ? Observation and measurement of Higgs boson decays to WW$^*$ with the ATLAS detector
1334140 . Centrality and rapidity dependence of inclusive jet production in $\sqrt{s_\mathrm{NN}} = 5.02$ TeV proton-lead collisions with the ATLAS detector
1334362 . Measurement of Spin Correlation in Top-Antitop Quark Events and Search for Top Squark Pair Production in pp Collisions at $\sqrt{s}=8$ TeV Using the ATLAS Detector
1335136 . Observation and measurements of the production of prompt and non-prompt $J/\psi$ mesons in association with a $Z$ boson in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1335266 ? Search for charged Higgs bosons decaying via $H^{\pm} \rightarrow \tau^{\pm}\nu$ in fully hadronic final states using $pp$ collision data at $\sqrt{s} = 8$ TeV with the ATLAS detector
1335273 X Identification and energy calibration of hadronically decaying tau leptons with the ATLAS experiment in $pp$ collisions at $\sqrt{s}$=8 TeV
1337472 ? Search for Scalar Charm Quark Pair Production in $pp$ Collisions at $\sqrt{s}=$ 8  TeV with the ATLAS Detector
1339252 ? Search for Higgs and Z Boson Decays to J/ψγ and ϒ(nS)γ with the ATLAS Detector
1339376 ? Search for squarks and gluinos in events with isolated leptons, jets and missing transverse momentum at $\sqrt{s}=8$ TeV with the ATLAS detector
1339624 ? Search for pair-produced long-lived neutral particles decaying in the ATLAS hadronic calorimeter in $pp$ collisions at $\sqrt{s}$ = 8 TeV
-1340321 . Evidence for the Higgs-boson Yukawa coupling to tau leptons with the ATLAS detector
+1340321 X Evidence for the Higgs-boson Yukawa coupling to tau leptons with the ATLAS detector
1341609 ? Search for direct pair production of a chargino and a neutralino decaying to the 125 GeV Higgs boson in $\sqrt{s} = 8$  TeV ${pp}$ collisions with the ATLAS detector
1341999 . Measurement of the charge asymmetry in dileptonic decays of top quark pairs in $pp$ collisions at $\sqrt{s}=7$ TeV using the ATLAS detector
1342452 ? Observation of top-quark pair production in association with a photon and measurement of the $t\bar{t}\gamma$ production cross section in pp collisions at $\sqrt{s}=7$ TeV using the ATLAS detector
1343107 ? Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at $\sqrt{s}=$8 TeV with the ATLAS detector
1345028 ? Search for a CP-odd Higgs boson decaying to Zh in pp collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
1345355 ? Search for massive supersymmetric particles decaying to many jets using the ATLAS detector in $pp$ collisions at $\sqrt{s} = 8$ TeV
1345452 . Differential top-antitop cross-section measurements as a function of observables constructed from final-state particles using pp collisions at $\sqrt{s}=7$ TeV in the ATLAS detector
1346398 ? A search for high-mass resonances decaying to $\tau^{+}\tau^{-}$ in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1346844 . Two-particle Bose–Einstein correlations in pp collisions at $\mathbf {\sqrt{s} =}$ 0.9 and 7 TeV measured with the ATLAS detector
1347135 ? Constraints on the off-shell Higgs boson signal strength in the high-mass $ZZ$ and $WW$ final states with the ATLAS detector
1351760 ? Evidence of Wγγ Production in pp Collisions at s=8  TeV and Limits on Anomalous Quartic Gauge Couplings with the ATLAS Detector
1351762 ? Search for supersymmetry in events containing a same-flavour opposite-sign dilepton pair, jets, and large missing transverse momentum in $\sqrt{s}=8$  TeV pp collisions with the ATLAS detector
1351913 X Determination of spin and parity of the Higgs boson in the $WW^*\rightarrow e \nu \mu \nu $ decay channel with the ATLAS detector
1351916 . Measurement of the forward-backward asymmetry of electron and muon pair-production in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector
1352819 ? Search for a Charged Higgs Boson Produced in the Vector-Boson Fusion Mode with Decay $H^\pm \to W^\pm Z$ using $pp$ Collisions at $\sqrt{s}=8$  TeV with the ATLAS Experiment
1352821 ? Search for a Heavy Neutral Particle Decaying to $e\mu$, $e\tau$, or $\mu\tau$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector
1352826 ? Search for production of $WW/WZ$ resonances decaying to a lepton, neutrino and jets in $pp$ collisions at $\sqrt{s}=8$  TeV with the ATLAS detector
1353124 ? Search for the Standard Model Higgs boson produced in association with top quarks and decaying into $b\bar{b}$ in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1353390 ? Search for vector-like $B$ quarks in events with one isolated lepton, missing transverse momentum and jets at $\sqrt{s}=$ 8 TeV with the ATLAS detector
1353391 X Measurement of the top quark mass in the $t\bar{t}\rightarrow \text{ lepton+jets } $ and $t\bar{t}\rightarrow \text{ dilepton } $ channels using $\sqrt{s}=7$   ${\mathrm { TeV}}$ ATLAS data
1356276 X Combined Measurement of the Higgs Boson Mass in $pp$ Collisions at $\sqrt{s}=7$ and 8 TeV with the ATLAS and CMS Experiments
1356730 ? Search for a new resonance decaying to a W or Z boson and a Higgs boson in the $\ell \ell / \ell \nu / \nu \nu + b \bar{b}$ final states with the ATLAS detector
1357199 ? Search for low-scale gravity signatures in multi-jet final states with the ATLAS detector at $ \sqrt{s}=8 $ TeV
1357594 ? Search for New Phenomena in Dijet Angular Distributions in Proton-Proton Collisions at $\sqrt{s} = 8$ TeV Measured with the ATLAS Detector
1357991 . Measurement of the correlation between flow harmonics of different order in lead-lead collisions at $\sqrt{s_{NN}}$=2.76 TeV with the ATLAS detector
1359456 ? Search for long-lived, weakly interacting particles that decay to displaced hadronic jets in proton-proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1360282 ? Search for heavy long-lived multi-charged particles in pp collisions at $\sqrt{s}=\;8$  TeV using the ATLAS detector
1360283 . Measurement of the top pair production cross section in 8 TeV proton-proton collisions using kinematic information in the lepton+jets final state with ATLAS
1360288 ? Search for invisible decays of the Higgs boson produced in association with a hadronically decaying vector boson in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1360290 ! Measurement of charged-particle spectra in Pb+Pb collisions at $\sqrt{{s}_\mathsf{{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC
1361912 ? Analysis of events with $b$-jets and a pair of leptons of the same charge in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1362183 ? Search for massive, long-lived particles using multitrack displaced vertices or displaced lepton pairs in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1362490 ? Search for high-mass diphoton resonances in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1364361 . Measurements of the Total and Differential Higgs Boson Production Cross Sections Combining the H→γγ and H→ZZ*→4ℓ Decay Channels at $\sqrt{s}$=8  TeV with the ATLAS Detector
1367302 ? Search for Higgs bosons decaying to $aa$ in the $\mu\mu\tau\tau$ final state in $pp$ collisions at $\sqrt{s} = $ 8 TeV with the ATLAS experiment
1370678 ? Search for production of vector-like quark pairs and of four top quarks in the lepton-plus-jets final state in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1373299 ? A search for $ t\overline{t} $ resonances using lepton-plus-jets events in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
1373520 ? Search for new light gauge bosons in Higgs boson decays to four-lepton final states in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector at the LHC
1373747 . Measurement of differential $J/\psi$ production cross sections and forward-backward ratios in p + Pb collisions with the ATLAS detector
1373912 ? Search for Higgs boson pair production in the $b\bar{b}b\bar{b}$ final state from pp collisions at $\sqrt{s} = 8$ TeVwith the ATLAS detector
1374218 ? Search for high-mass diboson resonances with boson-tagged jets in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
1374488 ? Search for Dark Matter in Events with Missing Transverse Momentum and a Higgs Boson Decaying to Two Photons in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector
1374493 ? Search for heavy lepton resonances decaying to a $Z$ boson and a lepton in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1374908 ? Search for type-III Seesaw heavy leptons in $pp$ collisions at $\sqrt{s}= 8$ TeV with the ATLAS Detector
1376287 X Measurements of the top quark branching ratios into channels with leptons and quarks with the ATLAS detector
1376482 ? Search for metastable heavy charged particles with large ionisation energy loss in pp collisions at $\sqrt{s} = 8$  TeV using the ATLAS experiment
1376944 ? Modelling $Z\rightarrow\tau\tau$ processes in ATLAS with $\tau$-embedded $Z\rightarrow\mu\mu$ data
1376945 . Measurement of colour flow with the jet pull angle in $t\bar{t}$ events using the ATLAS detector at $\sqrt{s}=8$ TeV
1376946 ? Study of the spin and parity of the Higgs boson in diboson decays with the ATLAS detector
1377202 ? Search for the associated production of the Higgs boson with a top quark pair in multilepton final states with the ATLAS detector
1377205 ? Search for heavy Majorana neutrinos with the ATLAS detector in pp collisions at $ \sqrt{s}=8 $ TeV
1377364 ? Study of (W/Z)H production and Higgs boson couplings using $H \rightarrow WW^{\ast}$ decays with the ATLAS detector
1377585 . Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the ATLAS detector
1380180 . Centrality, rapidity and transverse momentum dependence of isolated prompt photon production in lead-lead collisions at $\sqrt{s_{\mathrm{NN}}} = 2.76$ TeV measured with the ATLAS detector
1380183 ? ATLAS Run 1 searches for direct pair production of third-generation squarks at the Large Hadron Collider
1380185 . Measurement of the production of neighbouring jets in lead–lead collisions at $\sqrt{s_{\mathrm{NN}}} = 2.76$TeV with the ATLAS detector
1381766 X Determination of the top-quark pole mass using $ t\overline{t} $ + 1-jet events collected with the ATLAS experiment in 7 TeV pp collisions
1383128 X Measurements of the Higgs boson production and decay rates and coupling strengths using pp collision data at $\sqrt{s}=7$ and 8 TeV in the ATLAS experiment
1383883 ? Search for photonic signatures of gauge-mediated supersymmetry in 8 TeV pp collisions with the ATLAS detector
1383884 X Summary of the searches for squarks and gluinos using $ \sqrt{s}=8 $ TeV pp collisions with the ATLAS experiment at the LHC
1384120 ? Search for an additional, heavy Higgs boson in the $H\rightarrow ZZ$ decay channel at $\sqrt{s} = 8\;\text{ TeV }$ in $pp$ collision data with the ATLAS detector
1384272 . $Z$ boson production in $p+$Pb collisions at $\sqrt{s_{NN}}=5.02$ TeV measured with the ATLAS detector
1385102 X Study of the $B_c^+ \rightarrow J/\psi D_s^+$ and $B_c^+ \rightarrow J/\psi D_s^{*+}$ decays with the ATLAS detector
1385604 X Measurement of the branching ratio $\Gamma(\Lambda_b^0 \rightarrow \psi(2S)\Lambda^0)/\Gamma(\Lambda_b^0 \rightarrow J/\psi\Lambda^0)$ with the ATLAS detector
1385880 X Determination of the ratio of $b$-quark fragmentation fractions $f_s/f_d$ in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1386475 . Measurement of the centrality dependence of the charged-particle pseudorapidity distribution in proton–lead collisions at $\sqrt{s_{_\text {NN}}} = 5.02$  TeV with the ATLAS detector
1387176 . Measurement of transverse energy-energy correlations in multi-jet events in $pp$ collisions at $\sqrt{s} = 7$ TeV using the ATLAS detector and determination of the strong coupling constant $\alpha_{\mathrm{s}}(m_Z)$
1387509 X Constraints on non-Standard Model Higgs boson interactions in an effective Lagrangian using differential cross sections measured in the $H \rightarrow \gamma\gamma$ decay channel at $\sqrt{s} = 8$TeV with the ATLAS detector
1388016 ? Search for lepton-flavour-violating H → μτ decays of the Higgs boson with the ATLAS detector
1388506 ? Searches for scalar leptoquarks in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1389174 ? Search for flavour-changing neutral current top-quark decays to $qZ$ in $pp$ collision data collected with the ATLAS detector at $\sqrt s =8$  TeV
1389857 X Summary of the ATLAS experiment’s sensitivity to supersymmetry after LHC Run 1 — interpreted in the phenomenological MSSM
1390114 . Measurements of fiducial cross-sections for $t\bar{t}$ production with one or two additional b-jets in pp collisions at $\sqrt{s}$ =8 TeV using the ATLAS detector
1391149 ? Search for invisible decays of a Higgs boson using vector-boson fusion in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1391318 ? Search for single top-quark production via flavour-changing neutral currents at 8 TeV with the ATLAS detector
1391323 ? Search for a high-mass Higgs boson decaying to a $W$ boson pair in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
1391509 ? Constraints on new phenomena via Higgs boson couplings and invisible decays with the ATLAS detector
1392455 . Measurement of the charge asymmetry in top-quark pair production in the lepton-plus-jets final state in pp collision data at $\sqrt{s}=8\,\mathrm TeV{}$ with the ATLAS detector
1393281 ? Search for pair production of a new heavy quark that decays into a $W$ boson and a light quark in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
1393493 ? Searches for Higgs boson pair production in the $hh\to bb\tau\tau, \gamma\gamma WW^*, \gamma\gamma bb, bbbb$ channels with the ATLAS detector
1393658 . Observation of Long-Range Elliptic Azimuthal Anisotropies in $\sqrt{s}=$13 and 2.76 TeV $pp$ Collisions with the ATLAS Detector
1393661 X A new method to distinguish hadronically decaying boosted $Z$ bosons from $W$ bosons using the ATLAS detector
1393662 ? Search for direct top squark pair production in final states with two tau leptons in pp collisions at $\sqrt{s}=8$  TeV with the ATLAS detector
1393757 ? Search for new phenomena in events with at least three photons collected in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1393758 . Measurement of jet charge in dijet events from $\sqrt{s}$=8  TeV pp collisions with the ATLAS detector
1393760 . Measurement of the $ t\overline{t}W $ and $ t\overline{t}Z $ production cross sections in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
1394161 ? Search for flavour-changing neutral current top quark decays $t\to Hq$ in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1394670 ? Search for the electroweak production of supersymmetric particles in $\sqrt{s}$=8 TeV $pp$ collisions with the ATLAS detector
1394679 . Measurement of four-jet differential cross sections in $\sqrt{s}=8$ TeV proton-proton collisions using the ATLAS detector
1394865 . Measurements of four-lepton production in $pp$ collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector
1395092 ? Search for magnetic monopoles and stable particles with high electric charges in 8 TeV $pp$ collisions with the ATLAS detector
1397001 ? Search for the production of single vector-like and excited quarks in the $Wt$ final state in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1397635 . Measurement of the production cross-section of a single top quark in association with a $W$ boson at 8 TeV with the ATLAS experiment
1397636 ? Search for anomalous couplings in the $Wtb$ vertex from the measurement of double differential angular decay rates of single top quarks produced in the $t$-channel with the ATLAS detector
1397637 . Measurement of the differential cross-section of highly boosted top quarks as a function of their transverse momentum in $\sqrt{s}$ = 8 TeV proton-proton collisions using the ATLAS detector
1397638 X Performance of pile-up mitigation techniques for jets in $pp$ collisions at $\sqrt{s}=8$  TeV using the ATLAS detector
1399051 X Identification of boosted, hadronically decaying W bosons and comparisons with ATLAS data taken at $\sqrt{s} = 8$ TeV
1399193 ? Search for dark matter produced in association with a Higgs boson decaying to two bottom quarks in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
-1400803 . Measurement of the correlations between the polar angles of leptons from top quark decays in the helicity basis at $\sqrt{s}=7$TeV using the ATLAS detector
-1402356 . Dijet production in $\sqrt{s}=$ 7 TeV $pp$ collisions with large rapidity gaps at the ATLAS experiment
+1400803 ! Measurement of the correlations between the polar angles of leptons from top quark decays in the helicity basis at $\sqrt{s}=7$TeV using the ATLAS detector
+1402356 ! Dijet production in $\sqrt{s}=$ 7 TeV $pp$ collisions with large rapidity gaps at the ATLAS experiment
1404878 . Measurements of top-quark pair differential cross-sections in the lepton+jets channel in $pp$ collisions at $\sqrt{s}=8$ TeV using the ATLAS detector
1405096 ? A search for prompt lepton-jets in $pp$ collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector
1405430 ? Evidence for single top-quark production in the $s$-channel in proton-proton collisions at $\sqrt{s}=$8 TeV with the ATLAS detector using the Matrix Element Method
1406935 ? Search for the Standard Model Higgs boson produced in association with a vector boson and decaying into a tau pair in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
-1407478 . Measurement of the dependence of transverse energy production at large pseudorapidity on the hard-scattering kinematics of proton-proton collisions at $\sqrt{s} = 2.76$ TeV with ATLAS
+1407478 ! Measurement of the dependence of transverse energy production at large pseudorapidity on the hard-scattering kinematics of proton-proton collisions at $\sqrt{s} = 2.76$ TeV with ATLAS
1407952 X Performance of $b$-Jet Identification in the ATLAS Experiment
1408292 ? Search for new phenomena in dijet mass and angular distributions from $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector
1408516 . Measurement of the transverse momentum and $\phi ^*_{\eta }$ distributions of Drell–Yan lepton pairs in proton–proton collisions at $\sqrt{s}=8$  TeV with the ATLAS detector
1408744 ? Search for strong gravity in multijet final states produced in pp collisions at $\sqrt{s} =$ 13 TeV using the ATLAS detector at the LHC
1408878 . Measurement of $D^{*\pm}$, $D^\pm$ and $D_s^\pm$ meson production cross sections in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1409298 . Measurement of the differential cross-sections of prompt and non-prompt production of $J/\psi $ and $\psi (2\mathrm {S})$ in $pp$ collisions at $\sqrt{s} = 7$ and 8 TeV with the ATLAS detector
1409300 ? Search for charged Higgs bosons in the $H^{\pm} \rightarrow tb$ decay channel in $pp$ collisions at $\sqrt{s}=8 $ TeV using the ATLAS detector
1409918 ? Combination of searches for $WW$, $WZ$, and $ZZ$ resonances in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
1409923 . Measurement of the $ZZ$ Production Cross Section in $pp$ Collisions at $\sqrt{s}$ = 13 TeV with the ATLAS Detector
1410580 ? Search for new phenomena with photon+jet events in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector
1410581 X Reconstruction of hadronic decay products of tau leptons with the ATLAS experiment
-1410588 . Measurement of the charge asymmetry in highly boosted top-quark pair production in $\sqrt{s} =$ 8 TeV $pp$ collision data collected by the ATLAS experiment
+1410588 ! Measurement of the charge asymmetry in highly boosted top-quark pair production in $\sqrt{s} =$ 8 TeV $pp$ collision data collected by the ATLAS experiment
1415119 X Measurement of the CP-violating phase $\phi_s$ and the $B^0_s$ meson decay width difference with $B^0_s \to J/\psi\phi$ decays in ATLAS
1415270 ? Probing lepton flavour violation via neutrinoless $\tau\longrightarrow 3\mu$ decays with the ATLAS detector
1416473 ? A search for an excited muon decaying to a muon and two jets in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1417099 ? A search for top squarks with R-parity-violating decays to all-hadronic final states with the ATLAS detector in $\sqrt{s}$ = 8 TeV proton-proton collisions
1419070 . Measurement of the charged-particle multiplicity inside jets from $\sqrt{s}=8$ TeV $pp$ collisions with the ATLAS detector
1419652 . Charged-particle distributions in $\sqrt{s}$ = 13 TeV pp interactions measured with the ATLAS detector at the LHC
1421648 X Test of CP Invariance in vector-boson fusion production of the Higgs boson using the Optimal Observable method in the ditau decay channel with the ATLAS detector
1422202 ? Search for single production of vector-like quarks decaying into Wb in pp collisions at $\sqrt{s} = 8$  TeV with the ATLAS detector
1422612 ? Search for single production of a vector-like quark via a heavy gluon in the $4b$ final state with the ATLAS detector in $pp$ collisions at $\sqrt{s} = 8$ TeV
1422615 ? Search for new phenomena in final states with large jet multiplicities and missing transverse momentum with ATLAS using $\sqrt{s} =$ 13 TeV proton-proton collisions
1424838 . Measurement of event-shape observables in $Z \rightarrow \ell ^{+} \ell ^{-}$ events in $pp$ collisions at $\sqrt{s}=$ 7 TeV with the ATLAS detector at the LHC
1424844 ? Search for supersymmetry at $\sqrt{s}=13$  TeV in final states with jets and two same-sign leptons or three leptons with the ATLAS detector
1426515 . Measurement of total and differential $W^+W^-$ production cross sections in proton-proton collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplings
1426523 . Measurements of $W^\pm Z$ production cross sections in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector and limits on anomalous gauge boson self-couplings
1426695 . Charged-particle distributions in $pp$ interactions at $\sqrt{s}=$ 8 TeV measured with the ATLAS detector
1426830 X Topological cell clustering in the ATLAS calorimeters and its performance in LHC Run 1
1427022 X Identification of high transverse momentum top quarks in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1429662 X Muon reconstruction performance of the ATLAS detector in proton–proton collision data at $\sqrt{s}$ =13 TeV
1436362 ? Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton--proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1436495 X Beam-induced and cosmic-ray backgrounds observed in the ATLAS detector during the LHC 2012 proton-proton running period
1436496 ? Search for charged Higgs bosons produced in association with a top quark and decaying via $H^{\pm} \rightarrow \tau\nu$ using $pp$ collision data recorded at $\sqrt{s} = 13$ TeV by the ATLAS detector
1436497 . Measurement of $W^{\pm}$ and $Z$-boson production cross sections in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1442359 ? Search for new phenomena in events with a photon and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
-1444991 . Measurement of fiducial differential cross sections of gluon-fusion production of Higgs bosons decaying to WW$^{∗}$→eνμν with the ATLAS detector at $ \sqrt{s}=8 $ TeV
+1444991 ! Measurement of fiducial differential cross sections of gluon-fusion production of Higgs bosons decaying to WW$^{∗}$→eνμν with the ATLAS detector at $ \sqrt{s}=8 $ TeV
1446750 ? Search for the Standard Model Higgs boson decaying into $ b\overline{b} $ produced in association with top quarks decaying hadronically in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
-1446983 . Study of the rare decays of $B^0_s$ and $B^0$ into muon pairs from data collected during the LHC Run 1 with the ATLAS detector
+1446983 X Study of the rare decays of $B^0_s$ and $B^0$ into muon pairs from data collected during the LHC Run 1 with the ATLAS detector
1448101 ? Search for metastable heavy charged particles with large ionization energy loss in pp collisions at $\sqrt{s} = 13$ TeV using the ATLAS experiment
1448301 . Measurements of $Z\gamma$ and $Z\gamma\gamma$ production in $pp$ collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector
1449082 . Measurements of the charge asymmetry in top-quark pair production in the dilepton final state at $\sqrt{s}=8$  TeV with the ATLAS detector
1452557 ? Search for lepton-flavour-violating decays of the Higgs and $Z$ bosons with the ATLAS detector
1452559 . Search for new phenomena in final states with an energetic jet and large missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$  TeV using the ATLAS detector
-1455739 . Gas gain stabilisation in the ATLAS TRT detector
+1455739 X Gas gain stabilisation in the ATLAS TRT detector
1457605 . Measurement of the inclusive isolated prompt photon cross section in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
1458270 . Search for squarks and gluinos in final states with jets and missing transverse momentum at $\sqrt{s} =$ 13 TeV with the ATLAS detector
1458952 ? Search for gluinos in events with an isolated lepton, jets and missing transverse momentum at $\sqrt{s}$ = 13 Te V with the ATLAS detector
1462258 ? Search for scalar leptoquarks in pp collisions at $\sqrt{s}$ = 13 TeV with the ATLAS experiment
1463284 . Transverse momentum, rapidity, and centrality dependence of inclusive charged-particle production in $\sqrt{s_{NN}}=5.02$ TeV $p$ + Pb collisions measured by the ATLAS experiment
1465511 X Measurement of the relative width difference of the $B^0$-$\bar B^0$ system with the ATLAS detector
1466302 ? Search for pair production of gluinos decaying via stop and sbottom in events with $b$-jets and large missing transverse momentum in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
-1466778 . Measurement of the angular coefficients in $Z$-boson events using electron and muon pairs from data taken at $\sqrt{s}=8$ TeV with the ATLAS detector
+1466778 ? Measurement of the angular coefficients in $Z$-boson events using electron and muon pairs from data taken at $\sqrt{s}=8$ TeV with the ATLAS detector
1467230 ! Charged-particle distributions at low transverse momentum in $\sqrt{s} = 13$  TeV $pp$ interactions measured with the ATLAS detector at the LHC
-1467454 . Measurement of the double-differential high-mass Drell-Yan cross section in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
+1467454 ! Measurement of the double-differential high-mass Drell-Yan cross section in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
1467455 X Measurement of the photon identification efficiencies with the ATLAS detector using LHC Run-1 data
1468064 X Measurement of the top quark mass in the $t\bar{t}\to$ dilepton channel from $\sqrt{s}=8$ TeV ATLAS data
1468065 ? Search for the Standard Model Higgs boson produced by vector-boson fusion and decaying to bottom quarks in $ \sqrt{s}=8 $ TeV pp collisions with the ATLAS detector
1468067 ? Search for TeV-scale gravity signatures in high-mass final states with leptons and jets with the ATLAS detector at $\sqrt{s}=13$ TeV
1468068 ? Measurements of the Higgs boson production and decay rates and constraints on its couplings from a combined ATLAS and CMS analysis of the LHC pp collision data at $ \sqrt{s}=7 $ and 8 TeV
1468167 . Measurement of the Inelastic Proton-Proton Cross Section at $\sqrt{s} = 13$  TeV with the ATLAS Detector at the LHC
1468168 . Measurement of the $t\bar{t}$ production cross-section using $e\mu$ events with b-tagged jets in pp collisions at $\sqrt{s}$=13 TeV with the ATLAS detector
1469066 ? Search for resonances in diphoton events at $\sqrt{s}$=13 TeV with the ATLAS detector
1469069 ? Search for top squarks in final states with one isolated lepton, jets, and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector
1469070 ? Search for new resonances in events with one lepton and missing transverse momentum in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
1469071 . Measurement of the $W^{\pm}Z$ boson pair-production cross section in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS Detector
1469452 ? Search for pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state using proton--proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
1469453 ? Searches for heavy diboson resonances in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1470936 ? Search for heavy long-lived charged $R$-hadrons with the ATLAS detector in 3.2 fb$^{-1}$ of proton--proton collision data at $\sqrt{s} = 13$ TeV
-1471458 . The ATLAS Data Acquisition and High Level Trigger system
+1471458 X The ATLAS Data Acquisition and High Level Trigger system
1472089 X The performance of the jet trigger for the ATLAS detector during 2011 data taking
1472317 . Measurement of forward-backward multiplicity correlations in lead-lead, proton-lead, and proton-proton collisions with the ATLAS detector
1472323 ? Search for the Higgs boson produced in association with a $W$ boson and decaying to four $b$-quarks via two spin-zero particles in $pp$ collisions at 13 TeV with the ATLAS detector
1472822 ? Search for bottom squark pair production in proton–proton collisions at $\sqrt{s}=13$  TeV with the ATLAS detector
1473191 ! Measurement of jet activity in top quark events using the $e\mu$ final state with two $b$-tagged jets in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1473744 ? Search for supersymmetry in a final state containing two photons and missing transverse momentum in $\sqrt{s}$ = 13 TeV $pp$ collisions at the LHC using the ATLAS detector
1475286 ? Search for Higgs and $Z$ Boson Decays to $\phi\,\gamma$ with the ATLAS Detector
1475476 ? Search for high-mass new phenomena in the dilepton final state using proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1475477 . Measurement of exclusive $\gamma\gamma\rightarrow W^+W^-$ production and search for exclusive Higgs boson production in $pp$ collisions at $\sqrt{s} = 8$ TeV using the ATLAS detector
1477027 ? Search for new resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $\ell^+ \ell^- b\bar b$, $\ell \nu b\bar b$, and $\nu\bar{\nu} b\bar b$ channels with $pp$ collisions at $\sqrt s = 13$ TeV with the ATLAS detector
1477209 ? Search for squarks and gluinos in events with hadronically decaying tau leptons, jets and missing transverse momentum in proton–proton collisions at $\sqrt{s}=13$  TeV recorded with the ATLAS detector
1477403 ? Search for heavy resonances decaying to a $Z$ boson and a photon in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1477585 . Measurement of the total cross section from elastic scattering in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
-1477814 . Measurement of top quark pair differential cross-sections in the dilepton channel in $pp$ collisions at $\sqrt{s}$ = 7 and 8 TeV with ATLAS <james.ferrando@desy.de>
+1477814 ! Measurement of top quark pair differential cross-sections in the dilepton channel in $pp$ collisions at $\sqrt{s}$ = 7 and 8 TeV with ATLAS <james.ferrando@desy.de>
1478190 ? Search for new phenomena in different-flavour high-mass dilepton final states in pp collisions at $\sqrt{s}=13$  Tev with the ATLAS detector
-1478355 . Measurement of the $b\overline{b}$ dijet cross section in pp collisions at $\sqrt{s} = 7$  TeV with the ATLAS detector
+1478355 ! Measurement of the $b\overline{b}$ dijet cross section in pp collisions at $\sqrt{s} = 7$  TeV with the ATLAS detector
1478601 X A measurement of the calorimeter response to single hadrons and determination of the jet energy scale uncertainty using LHC Run-1 $pp$-collision data with the ATLAS detector
1478981 ? Dark matter interpretations of ATLAS searches for the electroweak production of supersymmetric particles in $ \sqrt{s}=8 $ TeV proton-proton collisions
1478983 ? Search for Minimal Supersymmetric Standard Model Higgs bosons $H/A$ and for a $Z^{\prime}$ boson in the $\tau \tau$ final state produced in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS Detector
1479760 . Study of hard double-parton scattering in four-jet events in pp collisions at $ \sqrt{s}=7 $ TeV with the ATLAS experiment
1479947 ? Search for dark matter produced in association with a hadronically decaying vector boson in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector
-1480190 . The Laser calibration of the Atlas Tile Calorimeter during the LHC run 1
+1480190 X The Laser calibration of the Atlas Tile Calorimeter during the LHC run 1
1480365 . Measurement of $W^+W^-$ production in association with one jet in proton--proton collisions at $\sqrt{s} =8$ TeV with the ATLAS detector
1481187 X Luminosity determination in pp collisions at $\sqrt{s}$ = 8 TeV using the ATLAS detector at the LHC
-1485353 . Measurement of the $t\bar{t}Z$ and $t\bar{t}W$ production cross sections in multilepton final states using 3.2 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
-1486394 . Measurement of the inclusive cross-sections of single top-quark and top-antiquark $t$-channel production in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
+1485353 ? Measurement of the $t\bar{t}Z$ and $t\bar{t}W$ production cross sections in multilepton final states using 3.2 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
+1486394 ? Measurement of the inclusive cross-sections of single top-quark and top-antiquark $t$-channel production in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
1486521 X A measurement of material in the ATLAS tracker using secondary hadronic interactions in 7 TeV pp collisions
1486673 ? Search for dark matter in association with a Higgs boson decaying to $b$-quarks in $pp$ collisions at $\sqrt s=13$ TeV with the ATLAS detector
1486878 ? Search for anomalous electroweak production of $WW/WZ$ in association with a high-mass dijet system in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1487472 . Measurements of long-range azimuthal anisotropies and associated Fourier coefficients for $pp$ collisions at $\sqrt{s}=5.02$ and $13$ TeV and $p$+Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ATLAS detector
1487726 ! Measurement of $W$ boson angular distributions in events with high transverse momentum jets at $\sqrt{s}=$ 8 TeV using the ATLAS detector
1488580 X Performance of algorithms that reconstruct missing transverse momentum in $\sqrt{s}=$ 8 TeV proton-proton collisions in the ATLAS detector
1492320 . Search for triboson $W^{\pm }W^{\pm }W^{\mp }$ production in $pp$ collisions at $\sqrt{s}=8$   $\text {TeV}$ with the ATLAS detector
-1494075 . Measurement of the $ZZ$ production cross section in proton-proton collisions at $\sqrt s =$ 8 TeV using the $ZZ\to\ell^{-}\ell^{+}\ell^{\prime -}\ell^{\prime +}$ and $ZZ\to\ell^{-}\ell^{+}\nu\bar{\nu}$ channels with the ATLAS detector
-1494410 . Measurements of charge and CP asymmetries in $b$-hadron decays using top-quark events collected by the ATLAS detector in $pp$ collisions at $\sqrt{s}=8$ TeV
-1495026 . Measurements of $\psi(2S)$ and $X(3872) \to J/\psi\pi^+\pi^-$ production in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
+1494075 ? Measurement of the $ZZ$ production cross section in proton-proton collisions at $\sqrt s =$ 8 TeV using the $ZZ\to\ell^{-}\ell^{+}\ell^{\prime -}\ell^{\prime +}$ and $ZZ\to\ell^{-}\ell^{+}\nu\bar{\nu}$ channels with the ATLAS detector
+1494410 ? Measurements of charge and CP asymmetries in $b$-hadron decays using top-quark events collected by the ATLAS detector in $pp$ collisions at $\sqrt{s}=8$ TeV
+1495026 ? Measurements of $\psi(2S)$ and $X(3872) \to J/\psi\pi^+\pi^-$ production in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
1495243 . Measurement of jet activity produced in top-quark events with an electron, a muon and two $b$-tagged jets in the final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
-1496384 . Measurement of $W^{\pm}W^{\pm}$ vector-boson scattering and limits on anomalous quartic gauge couplings with the ATLAS detector
+1496384 ? Measurement of $W^{\pm}W^{\pm}$ vector-boson scattering and limits on anomalous quartic gauge couplings with the ATLAS detector
1498566 ? Search for new phenomena in events containing a same-flavour opposite-sign dilepton pair, jets, and large missing transverse momentum in $\sqrt{s}=$ 13 $pp$ collisions with the ATLAS detector
1499475 . High-$E_{\rm T}$ isolated-photon plus jets production in $pp$ collisions at $\sqrt s=$ 8 TeV with the ATLAS detector
1500696 X Performance of the ATLAS Trigger System in 2015
1500997 X Reconstruction of primary vertices at the ATLAS experiment in Run 1 proton–proton collisions at the LHC
1501691 X Electron efficiency measurements with the ATLAS detector using 2012 LHC proton–proton collision data
1502345 . Measurement of the W boson polarisation in $t\bar{t}$ events from pp collisions at $\sqrt{s}$ = 8 TeV in the lepton + jets channel with ATLAS
1502618 . Measurement of the prompt J/ $\psi $ pair production cross-section in pp collisions at $\sqrt{s} = 8$  TeV with the ATLAS detector
1502620 . Precision measurement and interpretation of inclusive $W^+$ , $W^-$ and $Z/\gamma ^*$ production cross sections with the ATLAS detector
1502921 . Measurements of top-quark pair to $Z$-boson cross-section ratios at $\sqrt s = 13, 8, 7$ TeV with the ATLAS detector
-1504059 ! Measurements of top-quark pair differential cross-sections in the $e\mu$ channel in $pp$ collisions at $\sqrt{s} = 13$ TeV using the ATLAS detector <neil.warrack@cern.ch>
+1504059 ! Measurements of top-quark pair differential cross-sections in the $e\mu$ channel in $pp$ collisions at $\sqrt{s} = 13$ TeV using the ATLAS detector <neil.warrack@cern.ch>
1505422 . Measurements of top quark spin observables in $ t\overline{t} $ events using dilepton final states in $ \sqrt{s}=8 $ TeV pp collisions with the ATLAS detector <james.ferrando@desy.de>
1505427 . Measurement of the cross-section for producing a W boson in association with a single top quark in pp collisions at $ \sqrt{s}=13 $ TeV with ATLAS
1509919 . Measurement of charged-particle distributions sensitive to the underlying event in $ \sqrt{s}=13 $ TeV proton-proton collisions with the ATLAS detector at the LHC
1510441 . Measurement of the cross section for inclusive isolated-photon production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector
-1510564 . Measurement of the $W$-boson mass in pp collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
+1510564 ? Measurement of the $W$-boson mass in pp collisions at $\sqrt{s}=7$ TeV with the ATLAS detector
1511869 . Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{{s_\mathrm{NN}}} = 2.76$ TeV with the ATLAS detector at the LHC
1512305 . Evidence for light-by-light scattering in heavy-ion collisions with the ATLAS detector at the LHC
1512776 ! Fiducial, total and differential cross-section measurements of $t$-channel single top-quark production in $pp$ collisions at 8 TeV using data collected by the ATLAS detector <neil.warrack@cern.ch>
1513473 ! Measurement of the $W^+W^-$ production cross section in $pp$ collisions at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV with the ATLAS experiment
1514251 . Measurements of the production cross section of a $Z$ boson in association with jets in pp collisions at $\sqrt{s} = 13$  TeV with the ATLAS detector
1514548 X Performance of the ATLAS Transition Radiation Tracker in Run 1 of the LHC: tracker properties
1515025 ! Top-quark mass measurement in the all-hadronic $ t\overline{t} $ decay channel at $ \sqrt{s}=8 $ TeV with the ATLAS detector
1515204 ? Probing the W tb vertex structure in t-channel single-top-quark production and decay in pp collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
1515374 . Measurement of the $t\bar{t}$ production cross section in the $\tau$ + jets final state in $pp$ collisions at $\sqrt{s}=8$ TeV using the ATLAS detector
-1517194 ! Measurements of electroweak $Wjj$ production and constraints on anomalous gauge couplings with the ATLAS detector
+1517194 . Measurements of electroweak $Wjj$ production and constraints on anomalous gauge couplings with the ATLAS detector
1519428 ? Search for new phenomena in dijet events using 37 fb$^{-1}$ of $pp$ collision data collected at $\sqrt{s}=$13 TeV with the ATLAS detector
1519834 X Jet energy scale measurements and their systematic uncertainties in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
1520722 X Jet reconstruction and performance using particle flow with the ATLAS Detector
1589844 . Measurement of the $k_\mathrm{t}$ splitting scales in $Z \to \ell\ell$ events in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector
1590025 . Femtoscopy with identified charged pions in proton-lead collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with ATLAS
1591327 . Measurements of integrated and differential cross sections for isolated photon pair production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1591328 ? Search for dark matter at $\sqrt{s}=13$ TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector
1596896 X Performance of the ATLAS Track Reconstruction Algorithms in Dense Environments in LHC Run 2
1597123 ? Search for new phenomena in a lepton plus high jet multiplicity final state with the ATLAS experiment using $ \sqrt{s}=13 $ TeV proton-proton collision data
1598259 ? Studies of $Z\gamma$ production in association with a high-mass dijet system in $pp$ collisions at $\sqrt{s}=$ 8 TeV with the ATLAS detector
1598265 X Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector
1598613 . Measurement of $b$-hadron pair production with the ATLAS detector in proton-proton collisions at $\sqrt{s}=8$ TeV
1599077 . Measurement of multi-particle azimuthal correlations in $pp$, $p+$Pb and low-multiplicity Pb$+$Pb collisions with the ATLAS detector
1599399 ? Search for the dimuon decay of the Higgs boson in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
1601647 ? Search for pair production of vector-like top quarks in events with one lepton, jets, and missing transverse momentum in $ \sqrt{s}=13 $ TeV $pp$ collisions with the ATLAS detector
-1602949 . Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings
+1602949 ? Measurement of $WW/WZ \to \ell \nu q q^{\prime}$ production with the hadronically decaying boson reconstructed as one or two jets in $pp$ collisions at $\sqrt{s}=8$ TeV with ATLAS, and constraints on anomalous gauge couplings
1604026 . Measurement of jet fragmentation in 5.02 TeV proton-lead and proton-proton collisions with the ATLAS detector
1604029 . Measurement of the $ t\overline{t}\gamma $ production cross section in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
1604271 ! Measurement of the inclusive jet cross-sections in proton-proton collisions at $ \sqrt{s}=8 $ TeV with the ATLAS detector
1604276 ? Search for supersymmetry in final states with two same-sign or three leptons and jets using 36 fb$^{-1}$ of $\sqrt{s}=13$ TeV $pp$ collision data with the ATLAS detector
1604888 ? Search for dark matter in association with a Higgs boson decaying to two photons at $\sqrt{s}$ = 13 TeV with the ATLAS detector
1604889 ? Search for direct top squark pair production in events with a Higgs or $Z$ boson, and missing transverse momentum in $\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector
1605396 ? Search for a new heavy gauge boson resonance decaying into a lepton and missing transverse momentum in 36 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS experiment
1607896 . Measurement of jet $p_{\mathrm{T}}$ correlations in Pb+Pb and $pp$ collisions at $\sqrt{s_{\mathrm{NN}}}=$ 2.76 TeV with the ATLAS detector
1608773 ? Search for Dark Matter Produced in Association with a Higgs Boson Decaying to $b\bar b$ using 36 fb$^{-1}$ of $pp$ collisions at $\sqrt s=13$ TeV with the ATLAS Detector
1608777 ? Search for top quark decays $t\rightarrow qH$, with $H\to\gamma\gamma$, in $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector
1609250 ? Search for new high-mass phenomena in the dilepton final state using 36 fb$^{−1}$ of proton-proton collision data at $ \sqrt{s}=13 $ TeV with the ATLAS detector
1609253 . Determination of the strong coupling constant $\alpha _\mathrm {s}$ from transverse energy–energy correlations in multijet events at $\sqrt{s} = 8~\hbox {TeV}$ using the ATLAS detector
1609258 X Study of the material of the ATLAS inner detector for Run 2 of the LHC
1609448 . Measurement of detector-corrected observables sensitive to the anomalous production of events with jets and large missing transverse momentum in $pp$ collisions at $\mathbf {\sqrt{s}=13}$  TeV using the ATLAS detector
1609451 ? Search for pair production of heavy vector-like quarks decaying to high-p$_{T}$ W bosons and b quarks in the lepton-plus-jets final state in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector
1609773 ? Search for new phenomena in high-mass diphoton final states using 37 fb$^{-1}$ of proton--proton collisions collected at $\sqrt{s}=13$ TeV with the ATLAS detector
1610449 X Analysis of the $Wtb$ vertex from the measurement of triple-differential angular decay rates of single top quarks produced in the $t$-channel at $\sqrt{s}$ = 8 TeV with the ATLAS detector
1610451 ? Study of $WW\gamma$ and $WZ\gamma$ production in $pp$ collisions at $\sqrt{s} = 8$ TeV and search for anomalous quartic gauge couplings with the ATLAS experiment
1610625 ? Search for Heavy Higgs Bosons $A/H$ Decaying to a Top Quark Pair in $pp$ Collisions at $\sqrt{s}=8\text{ }\text{ }\mathrm{TeV}$ with the ATLAS Detector
1611039 ? Search for heavy resonances decaying to a $W$ or $Z$ boson and a Higgs boson in the $q\bar{q}^{(\prime)}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
1613896 ? Searches for the $Z\gamma$ decay mode of the Higgs boson and for new high-mass resonances in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
1614149 . Measurements of top-quark pair differential cross-sections in the lepton+jets channel in $pp$ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector
1615205 . Search for new phenomena with large jet multiplicities and missing transverse momentum using large-radius jets and flavour-tagging at ATLAS in 13 TeV $pp$ collisions
1615206 ! Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1615470 ? Search for direct top squark pair production in final states with two leptons in $\sqrt{s} = 13$ TeV $pp$ collisions with the ATLAS detector
1615472 X Evidence for the $ H\to b\overline{b} $ decay with the ATLAS detector
1615757 . Measurement of long-range multiparticle azimuthal correlations with the subevent cumulant method in $pp$ and $p + Pb$ collisions with the ATLAS detector at the CERN Large Hadron Collider
1615866 ? Measurement of the exclusive $\gamma \gamma \rightarrow \mu^+ \mu^-$ process in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1616092 ? Search for diboson resonances with boson-tagged jets in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1620202 ? Search for the direct production of charginos and neutralinos in final states with tau leptons in $\sqrt{s} = $ 13 TeV $pp$ collisions with the ATLAS detector
1620206 ? Search for squarks and gluinos in events with an isolated lepton, jets, and missing transverse momentum at $\sqrt{s}=13$ TeV with the ATLAS detector
1620694 ? Search for supersymmetry in events with $b$-tagged jets and missing transverse momentum in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1620909 ? Search for an invisibly decaying Higgs boson or dark matter candidates produced in association with a $Z$ boson in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector
1620910 ? Searches for heavy $ZZ$ and $ZW$ resonances in the $\ell\ell qq$ and $\nu\nu qq$ final states in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1622266 . Measurement of longitudinal flow decorrelations in Pb+Pb collisions at $\sqrt{s_{\text {NN}}}=2.76$ and 5.02 TeV with the ATLAS detector
1622737 . Measurement of quarkonium production in proton–lead and proton–proton collisions at $5.02~\mathrm {TeV}$ with the ATLAS detector
-1622745 . Measurement of $\tau $ polarisation in $Z/\gamma ^{*}\rightarrow \tau \tau $ decays in proton–proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
+1622745 ? Measurement of $\tau $ polarisation in $Z/\gamma ^{*}\rightarrow \tau \tau $ decays in proton–proton collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1623207 ? Search for a scalar partner of the top quark in the jets plus missing transverse momentum final state at $\sqrt{s}$=13 TeV with the ATLAS detector
1623208 X Direct top-quark decay width measurement in the $t\bar{t}$ lepton+jets channel at $\sqrt{s}$=8 TeV with the ATLAS experiment
1623908 X Combination of inclusive and differential $ \mathrm{t}\overline{\mathrm{t}} $ charge asymmetry measurements using ATLAS and CMS data at $ \sqrt{s}=7 $ and 8 TeV <stephen.brown.7@research.gla.ac.uk>
1624549 ? A search for resonances decaying into a Higgs boson and a new particle $X$ in the $XH \to qqbb$ final state with the ATLAS detector
1624690 ? Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36 fb$^{−1}$ of pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector
-1624693 . Study of ordered hadron chains with the ATLAS detector
-1625109 . $ZZ \to \ell^{+}\ell^{-}\ell^{\prime +}\ell^{\prime -}$ cross-section measurements and search for anomalous triple gauge couplings in 13 TeV $pp$ collisions with the ATLAS detector
-1626105 . Measurement of lepton differential distributions and the top quark mass in $t\bar{t}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
+1624693 ! Study of ordered hadron chains with the ATLAS detector
+1625109 ? $ZZ \to \ell^{+}\ell^{-}\ell^{\prime +}\ell^{\prime -}$ cross-section measurements and search for anomalous triple gauge couplings in 13 TeV $pp$ collisions with the ATLAS detector
+1626105 ! Measurement of lepton differential distributions and the top quark mass in $t\bar{t}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector
1627873 . Measurement of the cross-section for electroweak production of dijets in association with a Z boson in pp collisions at $\sqrt {s}$ = 13 TeV with the ATLAS detector
1627878 ? Search for new phenomena in high-mass final states with a photon and a jet from $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
1628411 ? Search for heavy resonances decaying into $WW$ in the $e\nu\mu\nu$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1629567 . Measurement of the production cross-section of a single top quark in association with a Z boson in proton–proton collisions at 13 TeV with the ATLAS detector <stephen.brown.7@research.gla.ac.uk>
1630632 ? Search for long-lived, massive particles in events with displaced vertices and missing transverse momentum in $\sqrt{s}$ = 13 TeV $pp$ collisions with the ATLAS detector
1630886 ! Measurement of the Drell-Yan triple-differential cross section in $pp$ collisions at $\sqrt{s} = 8$ TeV
1630899 ? Search for B-L R -parity-violating top squarks in $\sqrt s$ =13  TeV pp collisions with the ATLAS experiment
1631641 ? A search for pair-produced resonances in four-jet final states at $\sqrt{s} =$ 13 TeV with the ATLAS detector
1631642 ? Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector
1632756 . Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at $\sqrt{s}=8$ TeV using the ATLAS detector
1632760 ? Search for doubly charged Higgs boson production in multi-lepton final states with the ATLAS detector using proton–proton collisions at $\sqrt{s}=13\,\text {TeV}$
1633591 ? Search for dark matter produced in association with bottom or top quarks in $\sqrt{s}=13$ TeV pp collisions with the ATLAS detector
1634607 ? Search for supersymmetry in final states with missing transverse momentum and multiple $b$-jets in proton-proton collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector
1634970 ! Measurement of inclusive jet and dijet cross-sections in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1635273 ! Measurement of differential cross sections and $W^+/W^-$ cross-section ratios for $W$ boson production in association with jets at $\sqrt{s}=8$ TeV with the ATLAS detector
1635274 ? Search for dark matter and other new phenomena in events with an energetic jet and large missing transverse momentum using the ATLAS detector
1637587 ! Measurement of the Soft-Drop Jet Mass in pp Collisions at $\sqrt{s} = 13$  TeV with the ATLAS Detector
1639856 . Search for top-squark pair production in final states with one lepton, jets, and missing transverse momentum using 36 fb$^{−1}$ of $ \sqrt{s}=13 $ TeV pp collision data with the ATLAS detector
1641076 ! Measurement of differential cross-sections of a single top quark produced in association with a $W$ boson at $\sqrt{s}=13$ TeV with ATLAS <stephen.brown.7@research.gla.ac.uk>
1641262 . Search for long-lived charginos based on a disappearing-track signature in pp collisions at $ \sqrt{s}=13 $ TeV with the ATLAS detector
-1641268 . Measurement of the Higgs boson coupling properties in the $H\rightarrow ZZ^{*} \rightarrow 4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector
+1641268 ? Measurement of the Higgs boson coupling properties in the $H\rightarrow ZZ^{*} \rightarrow 4\ell$ decay channel at $\sqrt{s}$ = 13 TeV with the ATLAS detector
1641270 . Search for squarks and gluinos in final states with jets and missing transverse momentum using 36  fb$^{-1}$ of $\sqrt{s}=13$  TeV pp collision data with the ATLAS detector
1641767 ? Search for exclusive Higgs and $Z$ boson decays to $\phi\gamma$ and $\rho\gamma$ with the ATLAS detector
1643838 ? Search for heavy ZZ resonances in the $\ell ^+\ell ^-\ell ^+\ell ^-$ and $\ell ^+\ell ^-\nu \bar{\nu }$ final states using proton–proton collisions at $\sqrt{s}= 13$   $\text {TeV}$ with the ATLAS detector
1643843 ? Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector
1644099 ! Measurement of the inclusive and fiducial $t\bar{t}$ production cross-sections in the lepton+jets channel in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector <neil.warrack@cern.ch>
1644367 . Measurement of the production cross section of three isolated photons in $pp$ collisions at $\sqrt{s}$ = 8 TeV using the ATLAS detector
1644618 ? Search for electroweak production of supersymmetric states in scenarios with compressed mass spectra at $\sqrt{s}=13$ TeV with the ATLAS detector
1644899 ? Evidence for the associated production of the Higgs boson and a top quark pair with the ATLAS detector
1644900 ? Search for the standard model Higgs boson produced in association with top quarks and decaying into a $b\bar{b}$ pair in $pp$ collisions at $\sqrt{s}$ = 13  TeV with the ATLAS detector
1645627 . Measurement of the cross section for isolated-photon plus jet production in $pp$ collisions at $\sqrt s=13$ TeV using the ATLAS detector
1646686 . Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ collisions at $\sqrt{s}=13\,$ TeV using the ATLAS detector
1649273 . Search for High-Mass Resonances Decaying to $\tau\nu$ in pp Collisions at $\sqrt{s}$=13  TeV with the ATLAS Detector
1650152 . Search for $W' \rightarrow tb$ decays in the hadronic final state using pp collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1650592 . Search for light resonances decaying to boosted quark pairs and produced in association with a photon or a jet in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1653453 ? Search for a Structure in the $B^0_s \pi^\pm$ Invariant Mass Spectrum with the ATLAS Experiment
1654357 ? Search for photonic signatures of gauge-mediated supersymmetry in 13 TeV $pp$ collisions with the ATLAS detector
1654372 ? Search for Higgs boson decays to beyond-the-Standard-Model light bosons in four-lepton events with the ATLAS detector at $\sqrt{s}=13$ TeV
-1654582 . Measurements of Higgs boson properties in the diphoton decay channel with 36 fb$^{-1}$ of $pp$ collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector
+1654582 ? Measurements of Higgs boson properties in the diphoton decay channel with 36 fb$^{-1}$ of $pp$ collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector
1654814 ? Search for the Decay of the Higgs Boson to Charm Quarks with the ATLAS Experiment
-1656578 ! Measurements of differential cross sections of top quark pair production in association with jets in ${pp}$ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector
+1656578 . Measurements of differential cross sections of top quark pair production in association with jets in ${pp}$ collisions at $\sqrt{s}=13$ TeV using the ATLAS detector
1656834 X Performance of missing transverse momentum reconstruction with the ATLAS detector using proton-proton collisions at $\sqrt{s}$ = 13 TeV
-1658490 . Production and Integration of the ATLAS Insertable B-Layer
+1658490 X Production and Integration of the ATLAS Insertable B-Layer
1658902 ? Search for electroweak production of supersymmetric particles in final states with two or three leptons at $\sqrt{s}=13\,$TeV with the ATLAS detector
1664317 ? Search for pair production of up-type vector-like quarks and for four-top-quark events in final states with multiple $b$-jets with the ATLAS detector
1664332 ? Search for flavour-changing neutral current top-quark decays $t\to qZ$ in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1664486 ? Search for top squarks decaying to tau sleptons in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector
1665234 ? Search for Higgs boson decays into pairs of light (pseudo)scalar particles in the $\gamma\gamma jj$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1665828 ? Search for a heavy Higgs boson decaying into a $Z$ boson and another heavy Higgs boson in the $\ell\ell bb$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1667040 ? Search for low-mass dijet resonances using trigger-level jets with the ATLAS detector in $pp$ collisions at $\sqrt{s}=13$ TeV
1667045 ? Search for supersymmetry in events with four or more leptons in $\sqrt{s}=13$ TeV $pp$ collisions with ATLAS
1667046 ? Search for R-parity-violating supersymmetric particles in multi-jet final states produced in $p$-$p$ collisions at $\sqrt{s} =13$ TeV using the ATLAS detector at the LHC
1668124 ? Search for pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state using proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
1670020 ? A search for lepton-flavor-violating decays of the $Z$ boson into a $\tau$-lepton and a light lepton with the ATLAS detector
1670803 ? Search for heavy particles decaying into top-quark pairs using lepton-plus-jets events in proton–proton collisions at $\sqrt{s} = 13$   $\text {TeV}$ with the ATLAS detector
1671810 ? Measurements of b-jet tagging efficiency with the ATLAS detector using $ t\overline{t} $ events at $ \sqrt{s}=13 $ TeV
1672010 ? Search for heavy resonances decaying to a photon and a hadronically decaying $Z/W/H$ boson in $pp$ collisions at $\sqrt{s}=13$ $\mathrm{TeV}$ with the ATLAS detector
1672099 ? Search for supersymmetry in final states with charm jets and missing transverse momentum in 13 TeV $pp$ collisions with the ATLAS detector
-1672147 . Measurement of colour flow using jet-pull observables in $t\bar{t}$ events with the ATLAS experiment at $\sqrt{s} = 13$ TeV
+1672147 ! Measurement of colour flow using jet-pull observables in $t\bar{t}$ events with the ATLAS experiment at $\sqrt{s} = 13\,\hbox {TeV}$
1672469 ? Prompt and non-prompt $J/\psi $ and $\psi (2\mathrm {S})$ suppression at high transverse momentum in $5.02~\mathrm {TeV}$ Pb+Pb collisions with the ATLAS experiment
1672475 ? Angular analysis of $B^0_d \rightarrow K^{*}\mu^+\mu^-$ decays in $pp$ collisions at $\sqrt{s}= 8$ TeV with the ATLAS detector
1672883 ? Search for flavor-changing neutral currents in top quark decays $t\to Hc$ and $t \to Hu$ in multilepton final states in proton-proton collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector
1672957 ? Measurement of the suppression and azimuthal anisotropy of muons from heavy-flavor decays in Pb+Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 2.76$ TeV with the ATLAS detector
1672961 ! Measurement of dijet azimuthal decorrelations in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector and determination of the strong coupling
1673177 ? Measurement of jet fragmentation in Pb+Pb and $pp$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV with the ATLAS detector
-1673184 . Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector
+1673184 ? Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector
1674532 . Search for resonances in the mass distribution of jet pairs with one or two jets identified as $b$-jets in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1674946 ! Combined measurement of differential and total cross sections in the $H \rightarrow \gamma \gamma$ and the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channels at $\sqrt{s} = 13$ TeV with the ATLAS detector
1675352 . Search for new phenomena using the invariant mass distribution of same-flavour opposite-sign dilepton pairs in events with missing transverse momentum in $\sqrt{s}=13$   $\text {Te}\text {V}$ pp collisions with the ATLAS detector
1676078 ? Measurement of the Higgs boson mass in the $H\rightarrow ZZ^* \rightarrow 4\ell$ and $H \rightarrow \gamma\gamma$ channels with $\sqrt{s}=13$ TeV $pp$ collisions using the ATLAS detector
1676179 X Observation of Higgs boson production in association with a top quark pair at the LHC with the ATLAS detector
1676472 . Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
1676481 . Search for pair production of heavy vector-like quarks decaying into high-$p_T$ $W$ bosons and top quarks in the lepton-plus-jets final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1676551 ! Search for chargino-neutralino production using recursive jigsaw reconstruction in final states with two or three charged leptons in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
-1676554 X Operation and performance of the ATLAS Tile Calorimeter in Run 1
+1676554 X Operation and performance of the ATLAS Tile Calorimeter in Run 1
1677389 . Search for pair production of higgsinos in final states with at least three $b$-tagged jets in $\sqrt{s} = 13$ TeV $pp$ collisions using the ATLAS detector
-1677498 . Probing the quantum interference between singly and doubly resonant top-quark production in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
+1677498 ! Probing the quantum interference between singly and doubly resonant top-quark production in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1678484 . Search for the Higgs boson produced in association with a vector boson and decaying into two spin-zero particles in the $H \rightarrow aa \rightarrow 4b$ channel in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
-1679217 . Observation of centrality-dependent acoplanarity for muon pairs produced via two-photon scattering in Pb+Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ATLAS detector
+1679217 X Observation of centrality-dependent acoplanarity for muon pairs produced via two-photon scattering in Pb+Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$ TeV with the ATLAS detector
1679959 . Search for pair- and single-production of vector-like quarks in final states with at least one $Z$ boson decaying into a pair of electrons or muons in $pp$ collision data collected with the ATLAS detector at $\sqrt{s} = 13$ TeV
1680457 . Search for Higgs boson decays into a pair of light bosons in the $bb\mu\mu$ final state in $pp$ collision at $\sqrt{s} = $13 TeV with the ATLAS detector
1680462 . Searches for exclusive Higgs and $Z$ boson decays into $J/\psi\gamma$, $\psi(2S)\gamma$, and $\Upsilon(nS)\gamma$ at $\sqrt{s}=13$ TeV with the ATLAS detector
1681154 ? Correlated long-range mixed-harmonic fluctuations measured in $pp$, $p$+Pb and low-multiplicity Pb+Pb collisions with the ATLAS detector
-1682295 . Prompt and non-prompt $J/\psi$ elliptic flow in Pb+Pb collisions at $\sqrt{s_{_\text{NN}}} = 5.02$ TeV with the ATLAS detector
+1682295 . Prompt and non-prompt $J/\psi $ elliptic flow in Pb+Pb collisions at $\sqrt{s_{_\text {NN}}} = 5.02$ Tev with the ATLAS detector
1682345 . Search for Higgs boson pair production in the $\gamma\gamma b\bar{b}$ final state with 13 TeV $pp$ collision data collected by the ATLAS experiment
-1682785 . Search for lepton-flavor violation in different-flavor, high-mass final states in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
-1683114 ! A strategy for a general search for new phenomena using data-derived signal regions and its application within the ATLAS experiment
+1682785 . Search for lepton-flavor violation in different-flavor, high-mass final states in $pp$ collisions at $\sqrt s=13 $ TeV with the ATLAS detector
+1683114 X A strategy for a general search for new phenomena using data-derived signal regions and its application within the ATLAS experiment
1683331 . Search for charged Higgs bosons decaying via $H^{\pm} \to \tau^{\pm}\nu_{\tau}$ in the $\tau$+jets and $\tau$+lepton final states with 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV with the ATLAS experiment
1683431 . Search for Higgs boson pair production in the $\gamma\gamma WW^{*}$ channel using $pp$ collision data recorded at $\sqrt{s} = 13$ TeV with the ATLAS detector
1683434 . Search for Higgs bosons produced via vector-boson fusion and decaying into bottom quark pairs in $\sqrt{s} = 13$ $\mathrm{TeV}$ $pp$ collisions with the ATLAS detector
1683827 X In situ calibration of large-$R$ jet energy and mass in 13 TeV proton-proton collisions with the ATLAS detector
1684216 . Search for vector-boson resonances decaying to a top quark and bottom quark in the lepton plus jets final state in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
1684341 . Search for dark matter in events with a hadronically decaying vector boson and missing transverse momentum in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
1684489 . Search for new phenomena in events with same-charge leptons and $b$-jets in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector
-1684645 ? A search for resonant and non-resonant Higgs boson pair production in the ${b\bar{b}\tau^+\tau^-}$ decay channel in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
-1685058 . Constraints on off-shell Higgs boson production and the Higgs boson total width in $ZZ\to4\ell$ and $ZZ\to2\ell2\nu$ final states with the ATLAS detector
+1684645 ? Search for Resonant and Nonresonant Higgs Boson Pair Production in the ${b\bar{b}\tau^+\tau^-}$ Decay Channel in $pp$ Collisions at $\sqrt{s}=13$  TeV with the ATLAS Detector
+1685058 X Constraints on off-shell Higgs boson production and the Higgs boson total width in $ZZ\to4\ell$ and $ZZ\to2\ell2\nu$ final states with the ATLAS detector
1685207 . Search for pair production of heavy vector-like quarks decaying into hadronic final states in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector
1685418 . Search for doubly charged scalar bosons decaying into same-sign $W$ boson pairs with the ATLAS detector
-1685420 . Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb$^{-1}$ of proton-proton collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector
-1685421 . Combination of the searches for pair-produced vector-like partners of the third-generation quarks at $\sqrt{s} =$ 13 TeV with the ATLAS detector
+1685420 ? Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb$^{-1}$ of proton-proton collision data at $\sqrt{s} = 13$ TeV with the ATLAS detector
+1685421 ? Combination of the searches for pair-produced vector-like partners of the third-generation quarks at $\sqrt{s} =$ 13 TeV with the ATLAS detector
1685997 . Search for long-lived particles in final states with displaced dimuon vertices in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector
1686365 . Search for charged Higgs bosons decaying into top and bottom quarks at $\sqrt{s}$ = 13 TeV with the ATLAS detector
-1686832 . Search for heavy charged long-lived particles in proton-proton collisions at $\sqrt{s} = 13$ TeV using an ionisation measurement with the ATLAS detector
+1686832 . Search for heavy charged long-lived particles in proton-proton collisions at $\sqrt{s} = 13$ TeV using an ionisation measurement with the \mbox{ATLAS} detector
1686834 . Measurement of the azimuthal anisotropy of charged particles produced in $\sqrt{s_\mathrm{NN}} = 5.02$ TeV Pb+Pb collisions with the ATLAS detector
1688943 . Search for squarks and gluinos in final states with hadronically decaying $\tau$-leptons, jets, and missing transverse momentum using $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
-1690929 . Performance of top-quark and $W$-boson tagging with ATLAS in Run 2 of the LHC
-1691634 . Observation of $H \rightarrow b\bar{b}$ decays and $VH$ production with the ATLAS detector
-1691822 . Measurements of gluon-gluon fusion and vector-boson fusion Higgs boson production cross-sections in the $H \to WW^{\ast} \to e\nu\mu\nu$ decay channel in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
+1690929 X Performance of top-quark and $W$-boson tagging with ATLAS in Run 2 of the LHC
+1691634 X Observation of $H \rightarrow b\bar{b}$ decays and $VH$ production with the ATLAS detector
+1691822 X Measurements of gluon-gluon fusion and vector-boson fusion Higgs boson production cross-sections in the $H \to WW^{\ast} \to e\nu\mu\nu$ decay channel in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
1692387 . A search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
1694476 . Search for invisible Higgs boson decays in vector boson fusion at $\sqrt{s} = 13$ TeV with the ATLAS detector
1694678 . Measurement of photon-jet transverse momentum correlations in 5.02 TeV Pb+Pb and $pp$ collisions with ATLAS
-1696330 . Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with two charged leptons and two jets at $\sqrt{s}$ = 13 TeV with the ATLAS detector
-1696805 . Measurement of the top quark mass in the $t\bar{t}\to$ lepton+jets channel from $\sqrt{s}=8$ TeV ATLAS data and combination with previous results
+1696330 X Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with two charged leptons and two jets at $\sqrt{s}$ = 13 TeV with the ATLAS detector
+1696805 X Measurement of the top quark mass in the $t\bar{t}\to$ lepton+jets channel from $\sqrt{s}=8$ TeV ATLAS data and combination with previous results
+1697671 X Comparison between simulated and observed LHC beam backgrounds in the ATLAS experiment at ${E_{\textrm {beam}}}$ = 4 TeV
+1698006 ? Measurement of the $Z\gamma\rightarrow\nu\bar{\nu}\gamma$ production cross section in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector and limits on anomalous triple gauge-boson couplings
+1698025 X Measurement of the photon identification efficiencies with the ATLAS detector using LHC Run 2 data collected in 2015 and 2016
+1699375 ! Measurements of $W$ and $Z$ boson production in $pp$ collisions at $\sqrt{s}=5.02$ TeV with the ATLAS detector
+1702261 ! Search for the production of a long-lived neutral particle decaying within the ATLAS hadronic calorimeter in association with a $Z$ boson from $pp$ collisions at $\sqrt{s} = 13$ TeV
+1702263 . Search for four-top-quark production in the single-lepton and opposite-sign dilepton final states in pp collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
+1703139 . Search for Higgs boson pair production in the $b\bar{b}WW^{*}$ decay mode at $\sqrt{s}=13$ TeV with the ATLAS detector
+1704138 ! Search for long-lived particles produced in $pp$ collisions at $\sqrt{s}=13$ TeV that decay into displaced hadronic jets in the ATLAS muon spectrometer
+1704495 ? Cross-section measurements of the Higgs boson decaying into a pair of $\tau$-leptons in proton-proton collisions at $\sqrt{s}=13$ TeV with the ATLAS detector
+1705395 . Study of the hard double-parton scattering contribution to inclusive four-lepton production in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector
+1705396 . Search for Higgs boson pair production in the $WW^{(*)}WW^{(*)}$ decay channel using ATLAS data recorded at $\sqrt{s}=13$ TeV
+1705857 ! Measurements of fiducial and differential cross-sections of $t\bar{t}$ production with additional heavy-flavour jets in proton-proton collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector
+1707015 ! Measurements of inclusive and differential fiducial cross-sections of $t\bar{t}\gamma$ production in leptonic final states at $\sqrt{s}$ = 13 TeV in ATLAS
diff --git a/doc/rivet-coverage-cms.rank b/doc/rivet-coverage-cms.rank
--- a/doc/rivet-coverage-cms.rank
+++ b/doc/rivet-coverage-cms.rank
@@ -1,820 +1,848 @@
-845323 . Transverse momentum and pseudorapidity distributions of charged hadrons in pp collisions at $\sqrt{s} = 0.9$ and 2.36 TeV
-855299 . Transverse-momentum and pseudorapidity distributions of charged hadrons in $pp$ collisions at $\sqrt{s}=7$ TeV
-855303 . First Measurement of Bose-Einstein Correlations in proton-proton Collisions at $\sqrt{s}$ =0.9 and 2.36 TeV at the LHC
-856534 . Measurement of the charge ratio of atmospheric muons with the CMS detector
-857644 . First Measurement of the Underlying Event Activity at the LHC with $\sqrt{s} = 0.9$ TeV
+845323 ! Transverse momentum and pseudorapidity distributions of charged hadrons in pp collisions at $\sqrt{s} = 0.9$ and 2.36 TeV
+855299 ! Transverse-momentum and pseudorapidity distributions of charged hadrons in $pp$ collisions at $\sqrt{s}=7$ TeV
+855303 ? First Measurement of Bose-Einstein Correlations in proton-proton Collisions at $\sqrt{s}$ =0.9 and 2.36 TeV at the LHC
+856534 X Measurement of the charge ratio of atmospheric muons with the CMS detector
+857644 ! First Measurement of the Underlying Event Activity at the LHC with $\sqrt{s} = 0.9$ TeV
861153 X CMS Tracking Performance Results from early LHC Operation
870473 ! Observation of Long-Range Near-Side Angular Correlations in Proton-Proton Collisions at the LHC
871540 ? Search for Dijet Resonances in 7 TeV pp Collisions at CMS
873627 ? Search for Quark Compositeness with the Dijet Centrality Ratio in $pp$ Collisions at $\sqrt{s}=7$ TeV
874738 ? First Measurement of the Cross Section for Top-Quark Pair Production in Proton-Proton Collisions at $\sqrt{s}=7$ TeV
878118 . Prompt and non-prompt $J/\psi$ production in $pp$ collisions at $\sqrt{s}=7$ TeV
879277 ? Search for Stopped Gluinos in $pp$ collisions at $\sqrt{s}=7$ TeV
879315 . Charged particle multiplicities in $pp$ interactions at $\sqrt{s}=0.9$, 2.36, and 7 TeV
879403 . Measurement of the Isolated Prompt Photon Production Cross Section in $pp$ Collisions at $\sqrt{s} = 7$~TeV
881087 . Measurements of Inclusive $W$ and $Z$ Cross Sections in $pp$ Collisions at $\sqrt{s}=7$ TeV
881434 ? Search for Microscopic Black Hole Signatures at the Large Hadron Collider
881885 ? Search for Pair Production of Second-Generation Scalar Leptoquarks in $pp$ Collisions at $\sqrt{s}=7$ TeV
881886 ? Search for Pair Production of First-Generation Scalar Leptoquarks in $pp$ Collisions at $\sqrt{s}=7$ TeV
-882871 . Upsilon Production Cross-Section in pp Collisions at $sqrt{s}=7$ TeV
+882871 ? Upsilon Production Cross-Section in pp Collisions at $sqrt{s}=7$ TeV
882963 ? Search for a heavy gauge boson $W$ ' in the final state with an electron and large missing transverse energy in $pp$ collisions at $\sqrt{s}=7$ TeV
-883318 . Measurement of the $B^+$ Production Cross Section in pp Collisions at $\sqrt{s} = 7$~TeV
+883318 ? Measurement of the $B^+$ Production Cross Section in pp Collisions at $\sqrt{s} = 7$~TeV
883765 ? Search for Heavy Stable Charged Particles in $pp$ collisions at $\sqrt{s}=7$ TeV
883771 ? Search for Supersymmetry in pp Collisions at 7 TeV in Events with Jets and Missing Transverse Energy
884808 . Measurement of Bose-Einstein Correlations in $pp$ Collisions at $\sqrt{s}=0.9$ and 7 TeV
-884811 . Inclusive b-hadron production cross section with muons in $pp$ collisions at $\sqrt{s} = 7$ TeV
+884811 ? Inclusive b-hadron production cross section with muons in $pp$ collisions at $\sqrt{s} = 7$ TeV
885663 . Dijet Azimuthal Decorrelations in $pp$ Collisions at $\sqrt{s} = 7$~TeV
886332 . First Measurement of Hadronic Event Shapes in $pp$ Collisions at $\sqrt {s}=7$ TeV
889010 ! Observation and studies of jet quenching in PbPb collisions at nucleon-nucleon center-of-mass energy = 2.76 TeV
889175 . Measurement of Dijet Angular Distributions and Search for Quark Compositeness in pp Collisions at $sqrt{s} = 7$ TeV
889807 . Measurement of $B\bar{B}$ Angular Correlations based on Secondary Vertex Reconstruction at $\sqrt{s}=7$ TeV
890166 . Strange Particle Production in $pp$ Collisions at $\sqrt{s}=0.9$ and 7 TeV
890505 ? Search for a Heavy Bottom-like Quark in $pp$ Collisions at $\sqrt{s} = 7$ TeV
890909 ? Study of Z boson production in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
890910 ? Measurement of $W^+ W^-$ production and search for the Higgs boson in pp collisions at $\sqrt s=7$ TeV
891040 ? Search for a $W^\prime$ boson decaying to a muon and a neutrino in $pp$ collisions at $\sqrt{s} = 7$ TeV
891470 ? Search for Resonances in the Dilepton Mass Distribution in $pp$ Collisions at $\sqrt(s) = 7$ TeV
891482 ? Search for Supersymmetry in $pp$ Collisions at $\sqrt{s} = 7$ TeV in Events with Two Photons and Missing Transverse Energy
891814 ? Search for Physics Beyond the Standard Model in Opposite-Sign Dilepton Events at $\sqrt{s} = 7$ TeV
892975 . Measurement of the lepton charge asymmetry in inclusive $W$ production in pp collisions at $\sqrt{s} = 7$ TeV
893512 ? Search for Large Extra Dimensions in the Diphoton Final State at the Large Hadron Collider
895579 ? Search for Neutral MSSM Higgs Bosons Decaying to Tau Pairs in $pp$ Collisions at $\sqrt{s}=7$ TeV
-895581 . Measurement of the Inclusive Z Cross Section via Decays to Tau Pairs in $pp$ Collisions at $\sqrt{s}=7$ TeV
+895581 ? Measurement of the Inclusive Z Cross Section via Decays to Tau Pairs in $pp$ Collisions at $\sqrt{s}=7$ TeV
895742 ! Measurement of the differential dijet production cross section in proton-proton collisions at $\sqrt{s}=7$ TeV
-896211 . Measurement of the $B^0$ production cross section in $pp$ Collisions at $\sqrt{s}=7$ TeV
+896211 ? Measurement of the $B^0$ production cross section in $pp$ Collisions at $\sqrt{s}=7$ TeV
896527 ? Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy at the LHC
896585 . Measurement of the Polarization of W Bosons with Large Transverse Momenta in W+Jets Events at the LHC
896764 X Charged particle transverse momentum spectra in $pp$ collisions at $\sqrt{s} = 0.9$ and 7 TeV
899324 . Long-range and short-range dihadron angular correlations in central PbPb collisions at a nucleon-nucleon center of mass energy of 2.76 TeV
899577 . Measurement of $W\gamma$ and $Z\gamma$ production in $pp$ collisions at $\sqrt{s} = 7$ TeV
900114 . Search for supersymmetry in events with a lepton, a photon, and large missing transverse energy in $pp$ collisions at $\sqrt{s}=7$ TeV
901277 . Indications of suppression of excited $\Upsilon$ states in PbPb collisions at $\sqrt{S_{NN}}$ = 2.76 TeV
901401 . Search for First Generation Scalar Leptoquarks in the e$\nu$jj channel in $pp$ collisions at $\sqrt{s}=$ 7 TeV
901829 . Measurement of the $t\bar{t}$ production cross section and the top quark mass in the dilepton channel in $pp$ collisions at $\sqrt{s}=7$ TeV
902309 . Measurement of the Inclusive Jet Cross Section in $pp$ Collisions at $\sqrt{s}=7$ TeV
912560 . Measurement of the ratio of the 3-jet to 2-jet cross sections in $pp$ collisions at $\sqrt{s} = 7$ TeV
912697 . Search for physics beyond the standard model using multilepton signatures in $pp$ collisions at $\sqrt{s}=$ 7 TeV
912706 . Measurement of the Top-antitop Production Cross Section in $pp$ Collisions at $\sqrt{s}=7$ TeV using the Kinematic Properties of Events with Leptons and Jets
913321 . Search for Same-Sign Top-Quark Pair Production at $\sqrt{s}=7$ TeV and Limits on Flavour Changing Neutral Currents in the Top Sector
913455 ? Search for Light Resonances Decaying into Pairs of Muons as a Signal of New Physics
913689 . Measurement of the $t$-channel single top quark production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV
913831 . Search for Supersymmetry in Events with b Jets and Missing Transverse Momentum at the LHC
-914325 . Measurement of the Strange $B$ Meson Production Cross Section with J/Psi $\phi$ Decays in $pp$ Collisions at $\sqrt{s}=7$ TeV
+914325 ? Measurement of the Strange $B$ Meson Production Cross Section with J/Psi $\phi$ Decays in $pp$ Collisions at $\sqrt{s}=7$ TeV
914487 . Search for New Physics with Jets and Missing Transverse Momentum in $pp$ collisions at $\sqrt{s}=7$ TeV
914953 . Search for New Physics with a Mono-Jet and Missing Transverse Energy in $pp$ Collisions at $\sqrt{s} = 7$ TeV
-915810 . Missing transverse energy performance of the CMS detector
+915810 X Missing transverse energy performance of the CMS detector
916908 . Measurement of the Underlying Event Activity at the LHC with $\sqrt{s}= 7$ TeV and Comparison with $\sqrt{s} = 0.9$ TeV
917436 ? Inclusive search for squarks and gluinos in $pp$ collisions at $\sqrt{s}=7$ TeV
917583 . A search for excited leptons in $pp$ Collisions at $\sqrt{s}=$ 7 TeV
917588 . Search for supersymmetry in $pp$ collisions at $\sqrt{s}=7$ TeV in events with a single lepton, jets, and missing transverse momentum
918745 . Search for Three-Jet Resonances in $pp$ Collisions at $\sqrt{s}=7$ TeV
-919443 . Determination of Jet Energy Calibration and Transverse Momentum Resolution in CMS
+919443 X Determination of Jet Energy Calibration and Transverse Momentum Resolution in CMS
919733 . Dependence on pseudorapidity and centrality of charged hadron production in PbPb collisions at a nucleon-nucleon centre-of-mass energy of 2.76 TeV
919737 ? Measurement of the Inclusive $W$ and $Z$ Production Cross Sections in $pp$ Collisions at $\sqrt{s}=7$ TeV
919742 ? Search for Resonances in the Dijet Mass Spectrum from 7 TeV pp Collisions at CMS
921468 ? Search for B(s) and B to dimuon decays in pp collisions at 7 TeV
921788 . Measurement of the Drell-Yan Cross Section in $pp$ Collisions at $\sqrt{s}=7$ TeV
922830 ! Measurement of the Differential Cross Section for Isolated Prompt Photon Production in pp Collisions at 7 TeV
924377 . Measurement of the $t \bar{t}$ Production Cross Section in $pp$ Collisions at 7 TeV in Lepton + Jets Events Using $b$-quark Jet Identification
927049 ? Search for Supersymmetry at the LHC in Events with Jets and Missing Transverse Energy
928282 . Search for a Vector-like Quark with Charge 2/3 in $t$ + $Z$ Events from $pp$ Collisions at $\sqrt{s}=7$ TeV
929904 X Performance of tau-lepton reconstruction and identification in CMS
930318 . Forward Energy Flow, Central Charged-Particle Multiplicities, and Pseudorapidity Gaps in W and Z Boson Events from pp Collisions at $\sqrt{s}$ = 7 TeV
930319 . Measurement of energy flow at large pseudorapidities in $pp$ collisions at $\sqrt{s} = 0.9$ and 7 TeV
-939559 . Measurement of the weak mixing angle with the Drell-Yan process in proton-proton collisions at the LHC
+939559 X Measurement of the weak mixing angle with the Drell-Yan process in proton-proton collisions at the LHC
940012 X Jet Production Rates in Association with $W$ and $Z$ Bosons in $pp$ Collisions at $\sqrt{s}=7$ TeV
941555 . Measurement of the Rapidity and Transverse Momentum Distributions of $Z$ Bosons in $pp$ Collisions at $\sqrt{s}=7$ TeV
943720 . Measurement of the Production Cross Section for Pairs of Isolated Photons in $pp$ collisions at $\sqrt{s}=7$ TeV
944755 . $J/\psi$ and $\psi_{2S}$ production in $pp$ collisions at $\sqrt{s}=7$ TeV
954992 . Exclusive photon-photon production of muon pairs in proton-proton collisions at $\sqrt{s}=7$ TeV
1079910 ? Search for signatures of extra dimensions in the diphoton mass spectrum at the Large Hadron Collider
1082456 . Measurement of the charge asymmetry in top-quark pair production in proton-proton collisions at $\sqrt{s}=7$ TeV
1084729 . Measurement of isolated photon production in $pp$ and PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV
1084730 . Centrality dependence of dihadron correlations and azimuthal anisotropy harmonics in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV
1085651 ? Suppression of non-prompt $J/\psi$, prompt $J/\psi$, and Y(1S) in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV
1087342 . Measurement of the inclusive production cross sections for forward jets and for dijet events with one forward and one central jet in $pp$ collisions at $\sqrt{s}=7$ TeV
1088226 . Search for a Higgs boson in the decay channel $H$ to ZZ(*) to $q$ qbar $\ell^-$ l+ in $pp$ collisions at $\sqrt{s}=7$ TeV
1088230 . Search for the standard model Higgs boson decaying into two photons in $pp$ collisions at $\sqrt{s}=7$ TeV
1088231 . Combined results of searches for the standard model Higgs boson in $pp$ collisions at $\sqrt{s}=7$ TeV
1088232 . Search for the standard model Higgs boson decaying to $W^+W^−$ in the fully leptonic final state in pp collisions at $\sqrt{s}=7$ TeV
1088604 . Search for the standard model Higgs boson in the decay channel $H$ to $Z Z$ to 4 leptons in $pp$ collisions at $\sqrt{s}=7$ TeV
1088823 . Study of high-pT charged particle suppression in PbPb compared to $pp$ collisions at $\sqrt{s_{NN}}=2.76$ TeV
1089288 . Search for the standard model Higgs boson in the $H$ to $Z Z$ to $\ell \ell \tau \tau$ decay channel in $pp$ collisions at $\sqrt{s}=7$ TeV
1089334 . Search for the standard model Higgs boson in the $H$ to $Z Z$ to 2 $\ell 2 \nu$ channel in $pp$ collisions at $\sqrt{s}=7$ TeV
1089399 . Search for large extra dimensions in dimuon and dielectron events in pp collisions at $\sqrt{s} = 7$ TeV
1089661 . Search for neutral Higgs bosons decaying to tau pairs in $pp$ collisions at $\sqrt{s}=7$ TeV
1089700 . Search for the standard model Higgs boson decaying to bottom quarks in $pp$ collisions at $\sqrt{s}=7$ TeV
1089835 . Inclusive $b$-jet production in $pp$ collisions at $\sqrt{s}=7$ TeV
1090064 . Jet momentum dependence of jet quenching in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV
1090423 . Search for quark compositeness in dijet angular distributions from $pp$ collisions at $\sqrt{s}=7$ TeV
1091050 . Search for microscopic black holes in $pp$ collisions at $\sqrt{s}=7$ TeV
1093951 . Measurement of the cross section for production of $b b^-$ bar $X$, decaying to muons in $pp$ collisions at $\sqrt{s}=7$ TeV
1094164 . Search for $B^0_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$ decays
1094855 ? Search for heavy, top-like quark pair production in the dilepton final state in $pp$ collisions at $\sqrt{s} = 7$ TeV
1095503 . Measurement of the top quark pair production cross section in $pp$ collisions at $\sqrt{s} = 7$ TeV in dilepton final states containing a $\tau$
1102908 . Ratios of dijet production cross sections as a function of the absolute difference in rapidity between jets in proton-proton collisions at $\sqrt{s}=7$ TeV
1103032 . Search for Dark Matter and Large Extra Dimensions in pp Collisions Yielding a Photon and Missing Transverse Energy
1104744 . Search for heavy bottom-like quarks in 4.9 inverse femtobarns of $pp$ collisions at $\sqrt{s}=7$ TeV
1107658 . Measurement of the underlying event in the Drell-Yan process in proton-proton collisions at $\sqrt{s}=7$ TeV
1107659 . Measurement of the elliptic anisotropy of charged particles produced in PbPb collisions at $\sqrt{s}_{NN}$=2.76 TeV
1107730 . Measurement of the Z/$\gamma$*+b-jet cross section in pp collisions at $\sqrt{s}$ = 7 TeV
1107735 . Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV
1108144 . Search for Anomalous $t\bar{t}$ Production in the Highly-Boosted All-Hadronic Final State
-1110691 . Measurement of the mass difference between top and antitop quarks
+1110691 X Measurement of the mass difference between top and antitop quarks
1111014 . Shape, Transverse Size, and Charged Hadron Multiplicity of Jets in pp Collisions at 7 TeV
1111141 . Search for physics beyond the standard model in events with a $Z$ boson, jets, and missing transverse energy in $pp$ collisions at $\sqrt{s}=7$ TeV
1111995 . Search for leptonic decays of $W$ ' bosons in $pp$ collisions at $\sqrt{s}=7$ TeV
1112169 . Search for anomalous production of multilepton events in $pp$ collisions at $\sqrt{s}=7$ TeV
-1112562 . Observation of a new Xi(b) baryon
+1112562 X Observation of a new Xi(b) baryon
1112986 . Studies of jet quenching using isolated-photon+jet correlations in PbPb and $pp$ collisions at $\sqrt{s_{NN}}=2.76$ TeV
1113310 . Search for heavy long-lived charged particles in $pp$ collisions at $\sqrt{s}=7$ TeV
1113442 . Measurement of the $\Lambda_b$ cross section and the $_{\bar{\Lambda}_b}$ to $\Lambda_b$ ratio with $J/\Psi \Lambda$ decays in $pp$ collisions at $\sqrt{s}=7$ TeV
1114315 . Measurement of the pseudorapidity and centrality dependence of the transverse energy density in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV
1115185 . Search for new physics in events with same-sign dileptons and $b$-tagged jets in $pp$ collisions at $\sqrt{s}=7$ TeV
1116149 . Search for a light charged Higgs boson in top quark decays in $pp$ collisions at $\sqrt{s}=7$ TeV
1116250 . Measurement of jet fragmentation into charged particles in $pp$ and PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV
1116412 . Study of $W$ boson production in PbPb and $pp$ collisions at $\sqrt{s_{NN}}=2.76$ TeV
1116526 . Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
1117012 . Search for a $W^\prime$ or Techni-$\rho$ Decaying into $WZ$ in $pp$ Collisions at $\sqrt{s}=7$ TeV
1117702 . Search for high-mass resonances decaying into τ -lepton pairs in pp collisions at $\sqrt{s}=7$ TeV
1117706 . Search for narrow resonances in dilepton mass spectra in $pp$ collisions at $\sqrt{s}=7$ TeV
1118047 . Measurement of the electron charge asymmetry in inclusive $W$ production in $pp$ collisions at $\sqrt{s}=7$ TeV
1118577 . Search for charge-asymmetric production of W$′$ bosons in $t\bar{t} +$ jet events from pp collisions at $\sqrt{s} =$ 7 TeV
1118578 . Search for new physics in events with opposite-sign leptons, jets, and missing transverse energy in $pp$ collisions at $\sqrt{s}=7$ TeV
-1118729 . Performance of CMS muon reconstruction in $pp$ collision events at $\sqrt{s}=7$ TeV
+1118729 X Performance of CMS muon reconstruction in $pp$ collision events at $\sqrt{s}=7$ TeV
1119567 . Search for dark matter and large extra dimensions in monojet events in $pp$ collisions at $\sqrt{s}=7$ TeV
1120142 . Search for a light pseudoscalar Higgs boson in the dimuon decay channel in $pp$ collisions at $\sqrt{s}=7$ TeV
1120732 ! Inclusive and differential measurements of the $t \bar{t}$ charge asymmetry in proton-proton collisions at $\sqrt{s} =$ 7 TeV
1120733 ? Search for stopped long-lived particles produced in $pp$ collisions at $\sqrt{s}=7$ TeV
1120997 . Search for new physics with long-lived particles decaying to photons and missing energy in $pp$ collisions at $\sqrt{s}=7$ TeV
1121375 . Search for a fermiophobic Higgs boson in $pp$ collisions at $\sqrt{s}=7$ TeV
1121700 . Search for supersymmetry in hadronic final states using MT2 in $pp$ collisions at $\sqrt{s} = 7$ TeV
1121703 . Search for new physics in the multijet and missing transverse momentum final state in proton-proton collisions at $\sqrt{s} = 7$ TeV
-1121876 . Measurement of the underlying event activity in $pp$ collisions at $\sqrt{s} = 0.9$ and 7 TeV with the novel jet-area/median approach
+1121876 ! Measurement of the underlying event activity in $pp$ collisions at $\sqrt{s} = 0.9$ and 7 TeV with the novel jet-area/median approach
1122035 . A search for a doubly-charged Higgs boson in $pp$ collisions at $\sqrt{s}=7$ TeV
1122847 . Forward-backward asymmetry of Drell-Yan lepton pairs in $pp$ collisions at $\sqrt{s} = 7$ TeV
1123117 . Study of the inclusive production of charged pions, kaons, and protons in $pp$ collisions at $\sqrt{s}=0.9$, 2.76, and 7 TeV
1123507 . Search for pair production of first- and second-generation scalar leptoquarks in $pp$ collisions at $\sqrt{s}= 7$ TeV
1123803 . Search for heavy Majorana neutrinos in $\mu^{\pm}\mu^{\pm} +$ jets and $e^{\pm}e^{\pm} +$ jets events in pp collisions at $\sqrt{s} =$ 7 TeV
1124338 X Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC
1125962 . Search for a $W$ ' boson decaying to a bottom quark and a top quark in $pp$ collisions at $\sqrt{s}=7$ TeV
1125963 . Search for flavor changing neutral currents in top quark decays in pp collisions at 7 TeV
1127329 . Measurement of the azimuthal anisotropy of neutral pions in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV
1127335 . Measurement of the $t\bar{t}$ production cross section in the dilepton channel in $pp$ collisions at $\sqrt{s}=7$ TeV
1127501 . Observation of sequential Upsilon suppression in PbPb collisions
1127510 . Search for three-jet resonances in $pp$ collisions at $\sqrt{s}=7$ TeV
1128019 . Study of the dijet mass spectrum in $pp \to W +$ jets events at $\sqrt{s}=7$ TeV
1181767 . Search for supersymmetry in events with b-quark jets and missing transverse energy in pp collisions at 7 TeV
1184341 X Search for pair produced fourth-generation up-type quarks in $pp$ collisions at $\sqrt{s}=7$ TeV with a lepton in the final state
1184487 . Combined search for the quarks of a sequential fourth generation
1184938 . Search for exclusive or semi-exclusive photon pair production and observation of exclusive and semi-exclusive electron pair production in $pp$ collisions at $\sqrt{s}=7$ TeV
-1184941 . Observation of a diffractive contribution to dijet production in proton-proton collisions at $\sqrt{s}=7$ TeV
-1185101 . Measurement of the top-quark mass in $t\bar{t}$ events with lepton+jets final states in $pp$ collisions at $\sqrt{s}=7$ TeV
-1185104 . Measurement of the top-quark mass in $t\bar{t}$ events with dilepton final states in $pp$ collisions at $\sqrt{s}=7$ TeV
+1184941 ? Observation of a diffractive contribution to dijet production in proton-proton collisions at $\sqrt{s}=7$ TeV
+1185101 X Measurement of the top-quark mass in $t\bar{t}$ events with lepton+jets final states in $pp$ collisions at $\sqrt{s}=7$ TeV
+1185104 X Measurement of the top-quark mass in $t\bar{t}$ events with dilepton final states in $pp$ collisions at $\sqrt{s}=7$ TeV
1185414 . Measurement of the $Y(1S), Y(2S)$ and $Y(3S)$ polarizations in $pp$ collisions at $\sqrt{s}=7$ TeV
1185781 . Evidence for associated production of a single top quark and W boson in $pp$ collisions at $\sqrt{s}$ = 7 TeV
1186381 . Search for a narrow spin-2 resonance decaying to a pair of Z vector bosons in the semileptonic final state
1186385 . Search for the standard model Higgs boson produced in association with $W$ and $Z$ bosons in $pp$ collisions at $\sqrt{s}=7$ TeV
1186730 . Search for resonant $t\bar{t}$ production in lepton+jets events in $pp$ collisions at $\sqrt{s}=7$ TeV
1186734 . Measurement of the single-top-quark $t$-channel cross section in $pp$ collisions at $\sqrt{s}=7$ TeV
1188683 . Search for electroweak production of charginos and neutralinos using leptonic final states in $pp$ collisions at $\sqrt{s}=7$ TeV
1189049 . Search for anomalous production of highly boosted $Z$ bosons decaying to $\mu^+ \mu^-$ in proton-proton collisions at $\sqrt{s}=7$ TeV
1189050 . Measurement of the relative prompt production rate of chi(c2) and chi(c1) in $pp$ collisions at $\sqrt{s}=7$ TeV
1189663 . Search for heavy lepton partners of neutrinos in proton-proton collisions in the context of the type III seesaw mechanism
1189815 X Search for supersymmetry in events with photons and low missing transverse energy in $pp$ collisions at $\sqrt{s}=7$ TeV
1189819 X Search for fractionally charged particles in $pp$ collisions at $\sqrt{s}=7$ TeV
1189823 X Search for narrow resonances and quantum black holes in inclusive and $b$-tagged dijet mass spectra from $pp$ collisions at $\sqrt{s}=7$ TeV
1189986 . Search for heavy neutrinos and W[R] bosons with right-handed couplings in a left-right symmetric model in pp collisions at sqrt(s) = 7 TeV
1189987 . Search for excited leptons in $pp$ collisions at $\sqrt{s}=7$ TeV
1190671 . Observation of Z decays to four leptons with the CMS detector at the LHC
1191899 . Observation of long-range near-side angular correlations in proton-lead collisions at the LHC
1192033 . Search for third-generation leptoquarks and scalar bottom quarks in $pp$ collisions at $\sqrt{s}=7$ TeV
1192034 . Search for pair production of third-generation leptoquarks and top squarks in $pp$ collisions at $\sqrt{s}=7$ TeV
1193338 . Measurement of the inelastic proton-proton cross section at $\sqrt{s}=7$ TeV
1193934 . Search for heavy quarks decaying into a top quark and a $W$ or $Z$ boson using lepton + jets events in $pp$ collisions at $\sqrt{s}$ = 7 TeV
1193935 . Measurement of the sum of $W W$ and $WZ$ production with $W+$dijet events in $pp$ collisions at $\sqrt{s}=7$ TeV
1193937 . Search for a non-standard-model Higgs boson decaying to a pair of new light bosons in four-muon final states
1194120 . Search for supersymmetry in final states with missing transverse energy and 0, 1, 2, or at least 3 b-quark jets in 7 TeV pp collisions using the variable alphaT
1201946 ! Measurement of differential top-quark pair production cross sections in $pp$ colisions at $\sqrt{s}=7$ TeV
1202275 X Search in leptonic channels for heavy resonances decaying to long-lived neutral particles
1202674 X Search for supersymmetry in final states with a single lepton, $b$-quark jets, and missing transverse energy in proton-proton collisions at $\sqrt{s}=7$ TeV
1202680 X Search for $Z$ ' resonances decaying to $t\bar{t}$ in dilepton+jets final states in $pp$ collisions at $\sqrt{s}=7$ TeV
1203133 X Identification of b-quark jets with the CMS experiment
1203307 X Search for new physics in events with photons, jets, and missing transverse energy in $pp$ collisions at $\sqrt{s}=7$ TeV
1203454 ? Measurement of the $ZZ$ production cross section and search for anomalous couplings in 2 l2l ' final states in $pp$ collisions at $\sqrt{s}=7$ TeV
1203843 X Search for exotic resonances decaying into $WZ/ZZ$ in $pp$ collisions at $\sqrt{s}=7$ TeV
1206603 . Search for long-lived particles decaying to photons and missing energy in proton-proton collisions at $\sqrt{s}=7$ TeV
1206606 . Search for heavy resonances in the W/Z-tagged dijet mass spectrum in pp collisions at 7 TeV
1208097 X Search for contact interactions in $\mu^+\mu^-$ events in $pp$ collisions at $\sqrt{s}=7$ TeV
1208702 X Search for heavy narrow dilepton resonances in $pp$ collisions at $\sqrt{s}=7$ TeV and $\sqrt{s}=8$ TeV
1208703 X Search for new physics in events with same-sign dileptons and $b$ jets in $pp$ collisions at $\sqrt{s}=8$ TeV
1208812 X Inclusive search for supersymmetry using the razor variables in $pp$ collisions at $\sqrt{s}=7$ TeV
1208913 . Measurement of the $t\bar{t}$ production cross section in $pp$ collisions at $\sqrt{s}=7$ TeV with lepton + jets final states
1208923 . Measurements of differential jet cross sections in proton-proton collisions at $\sqrt{s}=7$ TeV with the CMS detector
1208931 X Study of the Mass and Spin-Parity of the Higgs Boson Candidate Via Its Decays to Z Boson Pairs
1208988 X Search for supersymmetry in $pp$ collisions at $\sqrt{s}=7$ TeV in events with a single lepton, jets, and missing transverse momentum
1209556 X Search for supersymmetry in events with opposite-sign dileptons and missing transverse energy using an artificial neural network
1209721 . Event shapes and azimuthal correlations in $Z$ + jets events in $pp$ collisions at $\sqrt{s}=7$ TeV
1210032 X Interpretation of Searches for Supersymmetry with simplified Models
1211187 X Search for physics beyond the standard model in events with $\tau$ leptons, jets, and large transverse momentum imbalance in pp collisions at $\sqrt{s}$ = 7 TeV
1215317 . Measurement of W+W- and ZZ production cross sections in pp collisions at sqrt(s) = 8 TeV
1215599 X Search for contact interactions using the inclusive jet $p_T$ spectrum in $pp$ collisions at $\sqrt{s} = 7$ TeV
1216035 . Measurement of the top-antitop production cross section in the tau+jets channel in pp collisions at sqrt(s) = 7 TeV
1217551 . Measurement of the $t\bar{t}$ production cross section in the all-jet final state in pp collisions at $\sqrt{s}$ = 7 TeV
1217552 X Search for pair-produced dijet resonances in four-jet final states in pp collisions at $\sqrt{s}$=7  TeV
1218021 X Searches for Higgs bosons in pp collisions at sqrt(s) = 7 and 8 TeV in the context of four-generation and fermiophobic models
1218372 . Study of the underlying event at forward rapidity in pp collisions at $\sqrt{s}$ = 0.9, 2.76, and 7 TeV
1218995 X Search for new physics in final states with a lepton and missing transverse energy in pp collisions at the LHC
1219000 X Search for a Higgs boson decaying into a b-quark pair and produced in association with b quarks in proton–proton collisions at 7 TeV
1219950 X Measurement of the X(3872) production cross section via decays to J/psi pi pi in pp collisions at sqrt(s) = 7 TeV
1220378 X Search for narrow resonances using the dijet mass spectrum in pp collisions at $\sqrt{s}$=8  TeV
1222336 . Search for the standard model Higgs boson produced in association with a top-quark pair in pp collisions at the LHC
1223519 . Search for supersymmetry in hadronic final states with missing transverse energy using the variables $\alpha_T$ and b-quark multiplicity in pp collisions at $\sqrt s=8$ TeV
1223628 ? Measurement of associated production of vector bosons and top quark-antiquark pairs at sqrt(s) = 7 TeV
1223729 X A New Boson with a Mass of 125 GeV Observed with the CMS Experiment at the Large Hadron Collider
1224273 X Observation of a new boson with mass near 125 GeV in pp collisions at $\sqrt{s}$ = 7 and 8 TeV
1224539 . Studies of jet mass in dijet and W/Z + jet events
1224805 X Search for microscopic black holes in pp collisions at sqrt(s) = 8 TeV
1225274 ? Measurement of the $\Upsilon(1S), \Upsilon(2S)$, and $\Upsilon(3S)$ cross sections in pp collisions at $\sqrt{s}$ = 7 TeV
1225976 X Search for a standard-model-like Higgs boson with a mass in the range 145 to 1000 GeV at the LHC
1229333 . Measurement of masses in the $t \bar{t}$ system by kinematic endpoints in pp collisions at $\sqrt{s}$ = 7 TeV
1230936 X Measurement of the $\Lambda_{b}^0$ lifetime in pp collisions at $\sqrt{s} = 7$ TeV
1230937 ! Measurement of the ratio of the inclusive 3-jet cross section to the inclusive 2-jet cross section in pp collisions at $\sqrt{s}$ = 7 TeV and first determination of the strong coupling constant in the TeV range
1231738 X Searches for long-lived charged particles in pp collisions at $\sqrt{s}$=7 and 8 TeV
1231945 . Multiplicity and transverse momentum dependence of two- and four-particle correlations in pPb and PbPb collisions
1232968 X Search for gluino mediated bottom- and top-squark production in multijet final states in pp collisions at 8 TeV
1235421 X Study of exclusive two-photon production of $W^+W^-$ in $pp$ collisions at $\sqrt{s} = 7$ TeV and constraints on anomalous quartic gauge couplings
-1235536 . Measurement of neutral strange particle production in the underlying event in proton-proton collisions at sqrt(s) = 7 TeV
-1236361 . Measurement of the hadronic activity in events with a Z and two jets and extraction of the cross section for the electroweak production of a Z with two jets in pp collisions at $\sqrt{s}$ = 7 TeV
+1235536 ! Measurement of neutral strange particle production in the underlying event in proton-proton collisions at sqrt(s) = 7 TeV
+1236361 ! Measurement of the hadronic activity in events with a Z and two jets and extraction of the cross section for the electroweak production of a Z with two jets in pp collisions at $\sqrt{s}$ = 7 TeV
1237104 ? Measurement of the $W^+W^-$ Cross section in $pp$ Collisions at $\sqrt{s} = 7$ TeV and Limits on Anomalous $WW\gamma$ and $WWZ$ couplings
1237915 X Energy Calibration and Resolution of the CMS Electromagnetic Calorimeter in $pp$ Collisions at $\sqrt{s} = 7$ TeV
1240497 X Search for top squarks in $R$-parity-violating supersymmetry using three or more leptons and b-tagged jets
1240504 X The performance of the CMS muon detector in proton-proton collisions at sqrt(s) = 7 TeV at the LHC
1241819 X Determination of the top-quark pole mass and strong coupling constant from the t t-bar production cross section in pp collisions at $\sqrt{s}$ = 7 TeV
1242440 . Study of the production of charged pions, kaons, and protons in pPb collisions at $\sqrt{s_{NN}} =\ $ 5.02 $\,\text {TeV}$
1243161 X Measurement of the top-quark mass in all-jets $t\bar{t}$ events in pp collisions at $\sqrt{s}$=7 TeV
1243425 X Measurement of the B(s) to mu+ mu- branching fraction and search for B0 to mu+ mu- with the CMS Experiment
1243861 X Search for a Higgs boson decaying into a Z and a photon in pp collisions at sqrt(s) = 7 and 8 TeV
1244128 ? Measurement of the prompt $J/\psi$ and $\psi$(2S) polarizations in $pp$ collisions at $\sqrt{s}$ = 7 TeV
1246905 . Search for top-squark pair production in the single-lepton final state in pp collisions at $\sqrt{s}$ = 8 TeV
1247976 X Angular analysis and branching fraction measurement of the decay $B^0 \to K^{*0} \mu^+\mu^-$
1249595 . Measurement of the W-boson helicity in top-quark decays from $t\bar{t}$ production in lepton+jets events in pp collisions at $\sqrt{s} =$ 7 TeV
1251905 ? Measurement of the $W\gamma$ and $Z\gamma$ inclusive cross sections in $pp$ collisions at $\sqrt s=7$  TeV and limits on anomalous triple gauge boson couplings
1252068 X Search for a new bottomonium state decaying to $\Upsilon(1S)\pi^+\pi^-$ in pp collisions at $\sqrt{s}$ = 8 TeV
1252719 . Measurement of the production cross section for $Z\gamma \to \nu\bar{\nu}\gamma$ in pp collisions at $\sqrt{s} =$ 7 TeV and limits on $ZZ\gamma$ and $Z\gamma\gamma$ triple gauge boson couplings
1253367 X Searches for new physics using the $t\bar{t}$ invariant mass distribution in pp collisions at $\sqrt{s}$=8  TeV
-1255647 . Observation of a peaking structure in the $J/\psi \phi$ mass spectrum from $B^{\pm} \to J/\psi \phi K^{\pm}$ decays
+1255647 X Observation of a peaking structure in the $J/\psi \phi$ mass spectrum from $B^{\pm} \to J/\psi \phi K^{\pm}$ decays
1256590 ! Modification of jet shapes in PbPb collisions at $\sqrt {s_{NN}} = 2.76$ TeV
1256938 . Measurement of associated W + charm production in pp collisions at $\sqrt{s}$ = 7 TeV
1256943 . Measurement of the cross section and angular correlations for associated production of a Z boson with b hadrons in pp collisions at $\sqrt{s} =$ 7 TeV
1257387 X Search for baryon number violation in top-quark decays
1258128 . Rapidity distributions in exclusive Z + jet and $\gamma$ + jet events in $pp$ collisions at $\sqrt{s}$ = 7 TeV
1258399 X Search for the standard model Higgs boson produced in association with a W or a Z boson and decaying to bottom quarks
1261026 . Jet and underlying event properties as a function of charged-particle multiplicity in proton–proton collisions at $\sqrt{s}$ = 7 TeV
1262319 ! Measurement of the differential and double-differential Drell-Yan cross sections in proton-proton collisions at $\sqrt{s} =$ 7 TeV
1262804 . Measurement of higher-order harmonic azimuthal anisotropy in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
1263658 . Searches for light- and heavy-flavour three-jet resonances in pp collisions at $\sqrt{s} = 8$ TeV
1264662 . Measurements of $t\bar{t}$ spin correlations and top-quark polarization using dilepton final states in $pp$ collisions at $\sqrt{s}$ = 7 TeV
1265220 X Search for supersymmetry in pp collisions at $\sqrt{s}$=8 TeV in events with a single lepton, large jet multiplicity, and multiple b jets
1265512 X Search for pair production of excited top quarks in the lepton + jets final state
1265659 . Probing color coherence effects in pp collisions at $\sqrt{s}=7\,\text {TeV} $
1266056 . Measurement of the triple-differential cross section for photon+jets production in proton-proton collisions at $\sqrt{s}$=7 TeV
1266257 . Search for new physics in events with same-sign dileptons and jets in pp collisions at $\sqrt{s}$ = 8 TeV
1266766 X Inclusive search for a vector-like T quark with charge $\frac{2}{3}$ in pp collisions at $\sqrt{s}$ = 8 TeV
1267508 X Measurement of Higgs boson production and properties in the WW decay channel with leptonic final states
1268151 X Studies of azimuthal dihadron correlations in ultra-central PbPb collisions at $\sqrt{s_{NN}} =$ 2.76 TeV
1268328 X Search for top-quark partners with charge 5/3 in the same-sign dilepton final state
1268812 X Search for top squark and higgsino production using diphoton Higgs boson decays
1269437 X Search for Flavor-Changing Neutral Currents in Top-Quark Decays $t \to Zq$ in $pp$ Collisions at $\sqrt{s}=8$  TeV
1269454 X Evidence of b-Jet Quenching in PbPb Collisions at $\sqrt{s_{NN}}=2.76$  TeV
1272842 X Measurement of the properties of a Higgs boson in the four-lepton final state
1272853 . Study of double parton scattering using W + 2-jet events in proton-proton collisions at $\sqrt{s}$ = 7 TeV
1273570 ? Measurement of the muon charge asymmetry in inclusive $pp \to W+X$ production at $\sqrt s =$ 7 TeV and an improved determination of light parton distribution functions
1273571 X Event activity dependence of Y(nS) production in $\sqrt{s_{NN}}$=5.02 TeV pPb and $\sqrt{s}$=2.76 TeV pp collisions
1273574 . Measurement of four-jet production in proton-proton collisions at $\sqrt{s}=7$  TeV
1273578 ! Measurement of the production cross section for a W boson and two b jets in pp collisions at $\sqrt{s}$=7 TeV
1275617 . Measurement of the $t \bar{t}$ production cross section in the dilepton channel in pp collisions at $\sqrt{s}$ = 8 TeV
1276827 X Observation of the associated production of a single top quark and a $W$ boson in $pp$ collisions at $\sqrt s = $8 TeV
1278063 . Studies of dijet transverse momentum balance and pseudorapidity distributions in pPb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ $\,\text {TeV}$
1278199 X Evidence for the 125 GeV Higgs boson decaying to a pair of $\tau$ leptons
1278857 X Evidence for the direct decay of the 125 GeV Higgs boson to fermions
1280200 ? Measurement of inclusive W and Z boson production cross sections in pp collisions at $\sqrt{s}$ = 8 TeV
1280529 ! Measurement of the production cross sections for a Z boson and one or more b jets in pp collisions at sqrt(s) = 7 TeV
1280718 X Search for W' $\to $ tb decays in the lepton + jets final state in pp collisions at $\sqrt{s}$ = 8 TeV
1281538 . Measurements of the $t\bar{t}$ charge asymmetry using the dilepton decay channel in pp collisions at $\sqrt{s} =$ 7 TeV
1281837 X Search for new physics in the multijet and missing transverse momentum final state in proton-proton collisions at $\sqrt{s}$= 8 TeV
1285228 X Alignment of the CMS tracker with LHC and cosmic ray data
1285492 . Measurement of WZ and ZZ production in pp collisions at $\sqrt{s} = 8\,\text {TeV} $ in final states with b-tagged jets
1287736 ? Measurement of the t-channel single-top-quark production cross section and of the $\mid V_{tb} \mid$ CKM matrix element in pp collisions at $\sqrt{s}$= 8 TeV
1288709 X Search for invisible decays of Higgs bosons in the vector boson fusion and associated ZH production modes
1289223 ? Measurement of the ratio $\mathcal B(t \to Wb)/\mathcal B(t \to Wq)$ in pp collisions at $\sqrt{s}$ = 8 TeV
1290126 ! Measurement of jet multiplicity distributions in $\mathrm {t}\overline{\mathrm {t}}$ production in pp collisions at $\sqrt{s} = 7\,\text {TeV} $
1291135 X Search for $WW \gamma$ and $WZ \gamma$ production and constraints on anomalous quartic gauge couplings in $pp$ collisions at $\sqrt s =$ 8 TeV
1291940 X Search for anomalous production of events with three or more leptons in $pp$ collisions at $\sqrt(s) =$ 8 TeV
1294140 . Measurement of pseudorapidity distributions of charged particles in proton-proton collisions at $\sqrt{s}$ = 8 TeV by the CMS and TOTEM experiments
1294937 X Search for massive resonances in dijet systems containing jets tagged as W or Z boson decays in pp collisions at $ \sqrt{s} $ = 8 TeV
1296080 X Search for massive resonances decaying into pairs of boosted bosons in semi-leptonic final states at $\sqrt{s} =$ 8 TeV
1296082 X Constraints on the Higgs boson width from off-shell production and decay to Z-boson pairs
1296259 X Search for top-squark pairs decaying into Higgs or Z bosons in pp collisions at $\sqrt{s}$=8 TeV
1296262 X Search for supersymmetry with razor variables in pp collisions at $\sqrt{s}$=7  TeV
1298029 X Description and performance of track and primary-vertex reconstruction with the CMS tracker
1298393 ! Measurement of differential cross sections for the production of a pair of isolated photons in pp collisions at $\sqrt{s}=7\,\text {TeV} $
1298508 X Searches for electroweak production of charginos, neutralinos, and sleptons decaying to leptons and W, Z, and Higgs bosons in pp collisions at 8 TeV
1298512 X Search for jet extinction in the inclusive jet-$p_t$ spectrum from proton-proton collisions at $\sqrt s =$ 8 TeV
1298807 . Measurement of the $pp \to ZZ$ production cross section and constraints on anomalous triple gauge couplings in four-lepton final states at $\sqrt s=$8 TeV
1298810 ! Measurement of the ratio of inclusive jet cross sections using the anti-$k_T$ algorithm with radius parameters R=0.5 and 0.7 in pp collisions at $\sqrt{s}=7$  TeV
1298812 . Measurement of prompt $J/\psi$ pair production in pp collisions at $ \sqrt{s} $ = 7 Tev
1299142 . Measurement of jet fragmentation in PbPb and pp collisions at $\sqrt{s_{NN}}=2.76$ TeV
-1300149 . Radiation background with the CMS RPCs at the LHC
+1300149 X Radiation background with the CMS RPCs at the LHC
1301560 X Search for excited quarks in the $\gamma +$jet final state in proton–proton collisions at $\sqrt s=8$ TeV
1303894 . Differential cross section measurements for the production of a W boson in association with jets in proton–proton collisions at $\sqrt s=7$ TeV
-1303895 . CMS RPC muon detector performance with 2010-2012 LHC data
+1303895 X CMS RPC muon detector performance with 2010-2012 LHC data
1303904 . Measurement of top quark-antiquark pair production in association with a W or Z boson in pp collisions at $\sqrt{s} = 8$ $\,\text {TeV}$
1304454 X Observation of the diphoton decay of the Higgs boson and measurement of its properties
1305624 . Study of hadronic event-shape variables in multijet final states in pp collisions at sqrt(s) = 7 TeV
1306289 X Search for new resonances decaying via WZ to leptons in proton-proton collisions at $\sqrt s =$ 8 TeV
1306295 X Search for heavy neutrinos and $\mathrm {W}$ bosons with right-handed couplings in proton-proton collisions at $\sqrt{s} = 8\,\text {TeV} $
1307759 . Measurement of the $t \bar t$ production cross section in $pp$ collisions at $\sqrt s = 8$ TeV in dilepton final states containing one $\tau$ lepton
1309874 X Search for pair production of third-generation scalar leptoquarks and top squarks in proton–proton collisions at $\sqrt{s}$=8 TeV
1310104 X Search for the associated production of the Higgs boson with a top-quark pair
1310653 X Search for physics beyond the standard model in final states with a lepton and missing transverse energy in proton-proton collisions at sqrt(s) = 8 TeV
1310737 . Measurements of jet multiplicity and differential production cross sections of $Z +$ jets events in proton-proton collisions at $\sqrt{s} =$ 7 TeV
1310838 X Search for neutral MSSM Higgs bosons decaying to a pair of tau leptons in pp collisions
1311223 X Search for dark matter, extra dimensions, and unparticles in monojet events in proton–proton collisions at $\sqrt{s} = 8$ TeV
1315820 X Searches for electroweak neutralino and chargino production in channels with Higgs, Z, and W bosons in pp collisions at 8 TeV
1315947 . Long-range two-particle correlations of strange hadrons with charged particles in pPb and PbPb collisions at LHC energies
1317640 ? Search for Displaced Supersymmetry in events with an electron and a muon with large impact parameters
1318344 ? Measurement of the production cross section ratio $\sigma$(Xb2(1P)) / $\sigma$(Xb1(1P) in pp collisions at $\sqrt s $ = 8 TeV
1318946 X Search for Standard Model Production of Four Top Quarks in the Lepton + Jets Channel in pp Collisions at $\sqrt{s}$ = 8 TeV
1320560 X Search for Monotop Signatures in Proton-Proton Collisions at $\sqrt s =$ 8 TeV
1320561 ? Measurement of the W boson helicity in events with a single reconstructed top quark in pp collisions at $ \sqrt{s}=8 $ TeV
1320775 ? Measurement of Prompt $\psi(2S) \to J/\psi$ Yield Ratios in Pb-Pb and $p-p$ Collisions at $\sqrt {s_{NN}}=$ 2.76  TeV
1321537 X Searches for heavy Higgs bosons in two-Higgs-doublet models and for $t→ch$ decay using multilepton and diphoton final states in $pp$ collisions at 8 TeV
1321687 . Measurement of electroweak production of two jets in association with a Z boson in proton-proton collisions at $\sqrt{s}=8\,\text {TeV}$
1322563 X Identification techniques for highly boosted W bosons that decay into hadrons
1322726 ? Study of Z production in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV in the dimuon and dielectron decay channels
1323075 X Measurement of the ratio of the production cross sections times branching fractions of $B_{c}^{\pm} \to J/\psi \pi^{\pm}$ and $B^{\pm} \to J/\psi K^{\pm}$ and $\mathcal{B}(B_{c}^{\pm} \to J/\psi \pi^{\pm}\pi^{\pm}\pi^{\mp})/\mathcal{B}(B_{c}^{\pm} \to J/\psi \pi^{\pm})$ in pp collisions at $\sqrt{s} =$ 7 TeV
-1323393 . CMS RPC tracker muon reconstruction
+1323393 X CMS RPC tracker muon reconstruction
1323444 X Study of vector boson scattering and search for new physics in events with two same-sign leptons and two jets
1323624 X Search for a standard model-like Higgs boson in the $μ^+μ^−$ and $e^+e^−$ decay channels at the LHC
1323630 X Constraints on parton distribution functions and extraction of the strong coupling constant from the inclusive jet cross section in pp collisions at $\sqrt{s} = 7$ $\,\text {TeV}$
1325549 X Search for new phenomena in monophoton final states in proton-proton collisions at $\sqrt s =$ 8 TeV
1325798 X Performance of the CMS missing transverse momentum reconstruction in pp data at $\sqrt{s}$ = 8 TeV
-1326189 . CMS RPC commissioning of the existing detector during the long shutdown
+1326189 X CMS RPC commissioning of the existing detector during the long shutdown
1327224 . Search for quark contact interactions and extra spatial dimensions using dijet angular distributions in proton–proton collisions at $\sqrt s =$ 8 TeV
1327726 X Constraints on the spin-parity and anomalous HVV couplings of the Higgs boson in proton collisions at 7 and 8 TeV
1328493 X Observation of the rare $B^0_s\to\mu^+\mu^-$ decay from the combined analysis of CMS and LHCb data
1328962 . Measurement of the cross section ratio $\sigma_\mathrm{t \bar{t} b \bar{b}} / \sigma_\mathrm{t \bar{t} jj }$ in pp collisions at $\sqrt{s}$ = 8 TeV
1329620 ? Search for disappearing tracks in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1329792 ? Search for Long-Lived Neutral Particles Decaying to Quark-Antiquark Pairs in Proton-Proton Collisions at $\sqrt{s} =$ 8 TeV
1329959 ? Search for long-lived particles that decay into final states containing two electrons or two muons in proton-proton collisions at $\sqrt{s} =$ 8 TeV
1330294 ? Search for stealth supersymmetry in events with jets, either photons or leptons, and low missing transverse momentum in pp collisions at 8 TeV
1332509 ! Measurements of differential and double-differential Drell-Yan cross sections in proton-proton collisions at 8 TeV
1332746 ! Measurement of the inclusive 3-jet production differential cross section in proton–proton collisions at 7 TeV and determination of the strong coupling constant in the TeV range
1334141 ? Searches for supersymmetry based on events with b jets and four W bosons in pp collisions at 8 TeV
1335131 ? Search for physics beyond the standard model in dilepton mass spectra in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1335501 ? Search for pair-produced resonances decaying to jet pairs in proton–proton collisions at $\sqrt{s} =$ 8 TeV
1335811 X Precise determination of the mass of the Higgs boson and tests of compatibility of its couplings with the standard model predictions using proton collisions at 7 and 8 $\,\text {TeV}$
1340084 ? Search for resonances and quantum black holes using dijet mass spectra in proton-proton collisions at $\sqrt{s} =$ 8 TeV
1340696 ? Search for heavy Majorana neutrinos in $\mu^\pm \mu^\pm+$ jets events in proton-proton collisions at $\sqrt{s}$ = 8 TeV
1340699 ? Search for Decays of Stopped Long-Lived Particles Produced in Proton–Proton Collisions at $\sqrt{s}= 8\,\text {TeV} $
1341039 X Measurement of the ratio $B(B^0_s \to J/\psi f_0(980))$ / $B(B^0_s \to J/\psi \phi(1020))$ in pp collisions at $\sqrt s$ = 7 TeV
1342266 ? Measurements of the $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) differential cross sections in pp collisions at $\sqrt{s} =$ 7 TeV
1342447 ? Search for Supersymmetry Using Razor Variables in Events with $b$-Tagged Jets in $pp$ Collisions at $\sqrt{s} =$ 8 TeV
1343506 X Search for a Standard Model Higgs Boson Produced in Association with a Top-Quark Pair and Decaying to Bottom Quarks Using a Matrix Element Method
1343509 X Constraints on the pMSSM, AMSB model and on other models from the search for long-lived charged particles in proton-proton collisions at sqrt(s) = 8 TeV
1343791 X Performance of Electron Reconstruction and Selection with the CMS Detector in Proton-Proton Collisions at √s = 8  TeV
1343792 X Performance of Photon Reconstruction and Identification with the CMS Detector in Proton-Proton Collisions at sqrt(s) = 8 TeV
1345023 ? Measurement of J/ψ and ψ(2S) Prompt Double-Differential Cross Sections in pp Collisions at $\sqrt{s}$=7  TeV
1345027 X Searches for Supersymmetry using the M$_{T2}$ Variable in Hadronic Events Produced in pp Collisions at 8 TeV
1345159 . Distributions of Topological Observables in Inclusive Three- and Four-Jet Events in pp Collisions at sqrt(s) = 7 TeV
1345160 X Search for Narrow High-Mass Resonances in Proton–Proton Collisions at $\sqrt{s}$ = 8 TeV Decaying to a Z and a Higgs Boson
1345262 X Evidence for Collective Multiparticle Correlations in p-Pb Collisions
1345263 ? Nuclear Effects on the Transverse Momentum Spectra of Charged Particles in pPb Collisions at $\sqrt{s_{_\mathrm {NN}}} =5.02$ TeV
1345354 ? Measurement of the Zγ Production Cross Section in pp Collisions at 8 TeV and Search for Anomalous Triple Gauge Boson Couplings
1345823 ? Search for Physics Beyond the Standard Model in Events with Two Leptons, Jets, and Missing Transverse Momentum in pp Collisions at sqrt(s) = 8 TeV
1346512 ? Search for Lepton-Flavour-Violating Decays of the Higgs Boson
1346843 . Study of Final-State Radiation in Decays of Z Bosons Produced in $pp$ Collisions at 7 TeV
1347386 . Evidence for transverse momentum and pseudorapidity dependent event plane fluctuations in PbPb and pPb collisions
1348542 X Search for vector-like T quarks decaying to top quarks and Higgs bosons in the all-hadronic channel using jet substructure
1352128 X Search for resonant pair production of Higgs bosons decaying to two bottom quark–antiquark pairs in proton–proton collisions at 8 TeV
1353393 X Measurements of the $\mathrm{Z}$ $\mathrm{Z}$ production cross sections in the $2\mathrm{l} 2\nu $ channel in proton–proton collisions at $\sqrt{s} = 7$ and $8~\mathrm{TeV} $ and combined constraints on triple gauge couplings
1353541 ? Study of W boson production in pPb collisions at $\sqrt{s_{\mathrm{NN}}} =$ 5.02 TeV
1356728 ? Searches for third-generation squark production in fully hadronic final states in proton-proton collisions at $ \sqrt{s} = 8$ TeV
1356998 . Measurement of diffraction dissociation cross sections in pp collisions at $\sqrt{s}$ = 7 TeV
1357201 ? Search for Third-Generation Scalar Leptoquarks in the t$\tau$ Channel in Proton-Proton Collisions at $\sqrt{s}$ = 8 TeV
1357982 X Search for a Higgs boson in the mass range from 145 to 1000 GeV decaying to a pair of W or Z bosons
1359293 ? Search for the production of dark matter in association with top-quark pairs in the single-lepton final state in proton-proton collisions at sqrt(s) = 8 TeV
1359450 ! Measurement of the Z boson differential cross section in transverse momentum and rapidity in proton–proton collisions at 8 TeV
-1359451 . Angular coefficients of Z bosons produced in pp collisions at $\sqrt{s}$ = 8 TeV and decaying to $\mu^+ \mu^-$ as a function of transverse momentum and rapidity
+1359451 ? Angular coefficients of Z bosons produced in pp collisions at $\sqrt{s}$ = 8 TeV and decaying to $\mu^+ \mu^-$ as a function of transverse momentum and rapidity
1362177 X Search for a pseudoscalar boson decaying into a Z boson and the 125 GeV Higgs boson in $ℓ^+ℓ^−b\overline{b}$ final states
-1367339 . Trapping in proton irradiated p$^+$-n-n$^+$ silicon sensors at fluences anticipated at the HL-LHC outer tracker
-1369161 . Impact of low-dose electron irradiation on $n^{+}p$ silicon strip sensors
+1367339 X Trapping in proton irradiated p$^+$-n-n$^+$ silicon sensors at fluences anticipated at the HL-LHC outer tracker
+1369161 X Impact of low-dose electron irradiation on $n^{+}p$ silicon strip sensors
1370682 . Measurement of the differential cross section for top quark pair production in pp collisions at $\sqrt{s} = 8\,\text {TeV} $
1372730 ? Comparison of the Z/$\gamma$$^{∗}$ + jets to $\gamma$ + jets cross sections in pp collisions at $ \sqrt{s}=8 $ TeV
1373745 X Search for neutral color-octet weak-triplet scalar particles in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1373914 X A search for pair production of new light bosons decaying into muons
1374219 X Search for the standard model Higgs boson produced through vector boson fusion and decaying to $b \overline{b}$
1374621 X Search for a massive resonance decaying into a Higgs boson and a W or Z boson in hadronic final states in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1375026 X Search for diphoton resonances in the mass range from 150 to 850 GeV in pp collisions at $\sqrt{s} =$ 8 TeV
1375314 X Search for resonant $t \bar t$ production in proton-proton collisions at $\sqrt s=$ 8  TeV
1380177 X Search for neutral MSSM Higgs bosons decaying into a pair of bottom quarks
1380605 . Production of leading charged particles and leading charged-particle jets at small transverse momenta in pp collisions at sqrt(s) = 8 TeV
1380907 X Search for exotic decays of a Higgs boson into undetectable particles and one or more photons
1382346 ? Search for supersymmetry with photons in pp collisions at $\sqrt{s}$=8  TeV
1382587 ? Search for a Higgs boson decaying into $\gamma^* \gamma \to \ell \ell \gamma$ with low dilepton mass in pp collisions at $\sqrt s = $ 8 TeV
1382590 ! Inclusive and differential measurements of the $t\overline{t}$ charge asymmetry in pp collisions at $\sqrt{s} =$ 8 TeV
1382594 ? Measurement of the ${{\mathrm{W} }^{+} }\mathrm{W}^{-} $ cross section in pp collisions at $\sqrt{s} =$ 8 TeV and limits on anomalous gauge couplings
1384119 . Pseudorapidity distribution of charged hadrons in proton-proton collisions at $\sqrt{s}$ = 13 TeV
1384772 X Limits on the Higgs boson lifetime and width from its decay to four charged leptons
1385104 ? Search for pair-produced vectorlike B quarks in proton-proton collisions at $\sqrt{s}$=8  TeV
1385107 . Measurement of the underlying event activity using charged-particle jets in proton-proton collisions at sqrt(s) = 2.76 TeV
1385111 X Measurement of the CP-violating weak phase $\phi_s$ and the decay width difference $\Delta \Gamma_s$ using the B$_s^0 \to J/\psi\phi$(1020) decay channel in pp collisions at $\sqrt{s}=$ 8 TeV
1385600 X Angular analysis of the decay $B^0 \to K^{*0} \mu^+ \mu^-$ from pp collisions at $\sqrt s = 8$ TeV
1386851 ? Search for supersymmetry in events with a photon, a lepton, and missing transverse momentum in pp collisions at $\sqrt s=$ 8 TeV
1386854 ? Search for neutral MSSM Higgs bosons decaying to $\mu^{+} \mu^{-}$ in pp collisions at $ \sqrt{s} =$ 7 and 8 TeV
1388178 . Measurement of the charge asymmetry in top quark pair production in pp collisions at $\sqrt(s) =$ 8 TeV using a template method
1388363 ? Search for W' decaying to tau lepton and neutrino in proton-proton collisions at $\sqrt(s) =$ 8 TeV
1390110 ? Study of B Meson Production in p$+$Pb Collisions at $\sqrt{s_{NN}}=5.02$  TeV Using Exclusive Hadronic Decays
1391140 ? Search for supersymmetry in the vector-boson fusion topology in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1391146 ? Search for a charged Higgs boson in pp collisions at $ \sqrt{s}=8 $ TeV
1391147 ! Measurement of differential cross sections for Higgs boson production in the diphoton decay channel in pp collisions at $\sqrt{s}=8\,\text {TeV} $
1393257 ? Search for pair production of first and second generation leptoquarks in proton-proton collisions at $\sqrt{s}$ = 8  TeV
1393258 ? Search for single production of scalar leptoquarks in proton-proton collisions at $\sqrt{s} = 8$ $TeV$
1393261 . Measurement of the inelastic cross section in proton–lead collisions at $\sqrt {s_{NN}}=$ 5.02 TeV
1393269 X Measurement of the top quark mass using proton-proton data at ${\sqrt{(s)}}$ = 7 and 8 TeV
1393276 ? Search for vector-like charge 2/3 T quarks in proton-proton collisions at sqrt(s) = 8 TeV
1394163 ? Search for $W' \to tb$ in proton-proton collisions at $\sqrt{s} = $ 8 TeV
1394164 ? Measurement of the $\mathrm{t}\overline{{\mathrm{t}}}$ production cross section in the all-jets final state in pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$
1395094 X Search for the production of an excited bottom quark decaying to $tW$ in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1395096 X Search for the associated production of a Higgs boson with a single top quark in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1395457 . Measurement of transverse momentum relative to dijet systems in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV
1396140 X Observation of top quark pairs produced in association with a vector boson in pp collisions at $ \sqrt{s}=8 $ TeV
1396141 X Searches for a heavy scalar boson H decaying to a pair of 125 GeV Higgs bosons hh or for a heavy pseudoscalar boson A decaying to Zh, in the final states with $h \to \tau \tau$
1397173 ! Measurement of long-range near-side two-particle angular correlations in pp collisions at $\sqrt s =$13 TeV
1397174 . Measurement of $\mathrm {t}\overline{\mathrm {t}}$ production with additional jet activity, including $\mathrm {b}$ quark jets, in the dilepton decay channel using pp collisions at $\sqrt{s} =$ 8 TeV
1397180 . Transverse momentum spectra of inclusive b jets in pPb collisions at $\sqrt{s_{NN}} = $ 5.02 TeV
1397832 X Search for a light charged Higgs boson decaying to $ \mathrm{c}\overline{\mathrm{s}} $ in pp collisions at $ \sqrt{s}=8 $ TeV
1398582 ? Measurement of the top quark pair production cross section in proton-proton collisions at $\sqrt(s) =$ 13 TeV
1399359 X Search for a very light NMSSM Higgs boson produced in decays of the 125 GeV scalar boson and decaying into $\tau$ leptons in pp collisions at $\sqrt{s}=8$ TeV
1400805 X Reconstruction and identification of τ lepton decays to hadrons and ν$_τ$ at CMS
1402803 ? Search for Excited Leptons in Proton-Proton Collisions at $\sqrt{s}$ = 8 TeV
1403169 . Measurement of Top Quark Polarisation in T-Channel Single Top Quark Production
1403990 X Search for a Low-Mass Pseudoscalar Higgs Boson Produced in Association with a $b\bar{b}$ Pair in $pp$ Collisions at $\sqrt{s} =$ 8 TeV
1404159 X Search for Anomalous Single Top Quark Production in Association with a Photon in $pp$ Collisions at $ \sqrt{s}=8 $ TeV
1405439 ? Measurement of Spin Correlations in $t\bar{t}$ Production using the Matrix Element Method in the Muon+Jets Final State in $pp$ Collisions at $\sqrt{s} =$ 8 TeV
1407148 ? Search for dark matter and unparticles produced in association with a Z boson in proton-proton collisions at $\sqrt s=$ 8  TeV
1407839 X Event generator tunes obtained from underlying event and multiparton scattering measurements
1407955 ? Search for narrow resonances decaying to dijets in proton-proton collisions at $\sqrt(s) =$ 13 TeV
1410826 ! Measurement of the inclusive jet cross section in pp collisions at $\sqrt{s} = 2.76\,\text {TeV}$
1410832 . Study of Z boson production in pPb collisions at $\sqrt {s_{NN}} = 5.02$ TeV
1411443 ? Search for supersymmetry in events with soft leptons, low jet multiplicity, and missing transverse energy in proton–proton collisions at $\sqrt{s}$=8 TeV
1411454 ! Measurement of differential and integrated fiducial cross sections for Higgs boson production in the four-lepton decay channel in pp collisions at $ \sqrt{s}=7 $ and 8 TeV
1412059 . Correlations between jets and charged particles in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=2.76 $ TeV
1413748 . Measurements of t t-bar spin correlations and top quark polarization using dilepton final states in pp collisions at sqrt(s) = 8 TeV
1414605 . Measurement of inclusive jet production and nuclear modifications in pPb collisions at $\sqrt{s_{_\mathrm {NN}}} =$ 5.02 TeV
1415949 ? Forward–backward asymmetry of Drell–Yan lepton pairs in pp collisions at $\sqrt{s} = 8$ $\,\mathrm{TeV}$
1416821 ? Search for massive WH resonances decaying into the $\ell \nu \mathrm{b} \overline{\mathrm{b}} $ final state at $\sqrt{s}=8$ $~\text {TeV}$
1416827 ! Azimuthal decorrelation of jets widely separated in rapidity in pp collisions at $ \sqrt{s}=7 $ TeV
1420551 ? Search for supersymmetry in pp collisions at sqrt(s) = 8 TeV in final states with boosted W bosons and b jets using razor variables
1420556 ? Search for direct pair production of scalar top quarks in the single- and dilepton channels in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1421644 X Combined search for anomalous pseudoscalar HVV couplings in VH(H $\to b \bar b$) production and H $\to$ VV decay
1421645 ? Search for R-parity violating decays of a top squark in proton-proton collisions at $\sqrt{s}$ = 8 TeV
-1421646 ! Measurement of dijet azimuthal decorrelation in pp collisions at $\sqrt{s}=8\,\mathrm{TeV} $
+1421646 . Measurement of dijet azimuthal decorrelation in pp collisions at $\sqrt{s}=8\,\mathrm{TeV} $
1422778 ? Search for supersymmetry in the multijet and missing transverse momentum final state in pp collisions at 13 TeV
1423069 ? Measurement of the $ \mathrm{ Z } \gamma \rightarrow \nu \bar{\nu} \gamma$ production cross section in pp collisions at $\sqrt{s}=$ 8 TeV and limits on anomalous $ \mathrm{ ZZ } \gamma$ and $ \mathrm{Z} \gamma \gamma$ trilinear gauge boson couplings
1424833 ? Search for heavy resonances decaying to two Higgs bosons in final states containing four b quarks
1424834 ! Search for supersymmetry in electroweak production with photons and large missing transverse energy in pp collisions at $\sqrt s = 8$ TeV
1424842 ? Measurements of the $\mathrm{t}\overline{\mathrm{t}}$ production cross section in lepton+jets final states in pp collisions at 8 $\,\text {TeV}$ and ratio of 8 to 7  $\,\text {TeV}$ cross sections
1425690 ? Search for direct pair production of supersymmetric top quarks decaying to all-hadronic final states in pp collisions at $\sqrt{s} = 8\;\text {TeV} $
1426517 ! Measurement of the differential cross section and charge asymmetry for inclusive $\mathrm {p}\mathrm {p}\rightarrow \mathrm {W}^{\pm }+X$ production at ${\sqrt{s}} = 8$ TeV
1426525 X Search for heavy Majorana neutrinos in e$^{±}$e$^{±}$+ jets and e$^{±}$ $\mu^{±}$+ jets events in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1426692 ? Measurement of the t-tbar production cross section in the e-mu channel in proton-proton collisions at sqrt(s) = 7 and 8 TeV
1426696 X Search for s channel single top quark production in pp collisions at $ \sqrt{s}=7 $ and 8 TeV
1426828 . $\Upsilon(\mathrm{nS})$ polarizations versus particle multiplicity in pp collisions at $\sqrt{s} =$ 7 TeV
1426832 ? Search for neutral resonances decaying into a Z boson and a pair of b jets or $\tau$ leptons
1427411 ? Search for new physics with the M$_{T2}$ variable in all-jets final states produced in pp collisions at $ \sqrt{s}=13 $ TeV
-1430578 . Physics motivations and expected performance of the CMS muon system upgrade with triple-GEM detectors
+1430578 X Physics motivations and expected performance of the CMS muon system upgrade with triple-GEM detectors
1430892 . Measurements of $t \bar t$ charge asymmetry using dilepton final states in pp collisions at $\sqrt s=8$ TeV
1430902 X Measurement of the top quark mass using charged particles in pp collisions at $\sqrt s =$ 8 TeV
1431986 ? Search for two Higgs bosons in final states containing two photons and two bottom quarks in proton-proton collisions at 8 TeV
1436367 . Search for dark matter particles in proton-proton collisions at $ \sqrt{s}=8 $ TeV using the razor variables
1448100 X Evidence for exclusive $\gamma\gamma \to W^+ W^-$ production and constraints on anomalous quartic gauge couplings in $pp$ collisions at $ \sqrt{s}=7 $ and 8 TeV
1448302 ? Search for lepton flavour violating decays of heavy resonances and quantum black holes to an e$\mu$ pair in proton-proton collisions at $\sqrt{s}$ = 8 TeV
1449080 . Pseudorapidity dependence of long-range two-particle correlations in $p$Pb collisions at $\sqrt {s_{NN}}=$ 5.02 TeV
1454081 ? Search for narrow resonances in dijet final states at $\sqrt(s)=$ 8 TeV with the novel CMS technique of data scouting
1454211 . Measurement of the integrated and differential $t \bar t$ production cross sections for high-$p_t$ top quarks in $pp$ collisions at $\sqrt s =$ 8 TeV
1456795 X Search for Higgs boson off-shell production in proton-proton collisions at 7 and 8 TeV and derivation of constraints on its total decay width
1456935 . Search for new physics in same-sign dilepton events in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $
-1459051 ! Measurement of the double-differential inclusive jet cross section in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $
+1459051 . Measurement of the double-differential inclusive jet cross section in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $
1459054 ? Search for supersymmetry in pp collisions at $ \sqrt{s}=13 $ TeV in the single-lepton final state using the sum of masses of large-radius jets
1464834 . Multiplicity and rapidity dependence of strange hadron production in pp, pPb, and PbPb collisions at the LHC
1464840 ? Coherent $J/\psi$ photoproduction in ultra-peripheral PbPb collisions at $\sqrt {s_{NN}} =$ 2.76 TeV with the CMS experiment
1466293 ? Search for top squark pair production in compressed-mass-spectrum scenarios in proton-proton collisions at $\sqrt{s}$ = 8 TeV using the $\alpha_T$ variable
1466294 . Measurement of the W boson helicity fractions in the decays of top quark pairs to lepton $+$ jets final states produced in pp collisions at $\sqrt s=$ 8TeV
1466301 ? Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at $\sqrt{s} =$ 8  TeV
-1467450 . High rate, fast timing Glass RPC for the high $\eta$ CMS muon detectors
+1467450 X High rate, fast timing Glass RPC for the high $\eta$ CMS muon detectors
1467451 . Measurement of the transverse momentum spectrum of the Higgs boson produced in pp collisions at $ \sqrt{s}=8 $ TeV using $H \to WW$ decays
1469062 X Phenomenological MSSM interpretation of CMS searches in pp collisions at sqrt(s) = 7 and 8 TeV
1469073 ? Search for Resonant Production of High-Mass Photon Pairs in Proton-Proton Collisions at $\sqrt s$ =8 and 13 TeV
1471281 ! Measurement of the transverse momentum spectra of weak vector bosons produced in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1471287 ? Evidence for collectivity in pp collisions at the LHC
1472314 ? Searches for $R$-parity-violating supersymmetry in $pp $collisions at $\sqrt(s) =$ 8 TeV in final states with 0-4 leptons
1473674 . Measurement of the differential cross sections for top quark pair production as a function of kinematic event variables in pp collisions at $\sqrt s$=7 and 8 TeV
1473675 ? Search for new physics in final states with two opposite-sign, same-flavor leptons, jets, and missing transverse momentum in pp collisions at sqrt(s) = 13 TeV
1475003 X Observation of the decay $B^+ \to \psi(2S) \phi(1020) K^+$ in pp collisions at $\sqrt s =$ 8 TeV
1475472 X Search for lepton flavour violating decays of the Higgs boson to $e \tau$ and $e \mu$ in proton–proton collisions at $\sqrt s=$ 8 TeV
1475475 X Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV
1477207 ? Search for dark matter in proton-proton collisions at 8 TeV with missing transverse momentum and vector boson tagged jets
1477805 X Measurement of the WZ production cross section in pp collisions at $\sqrt(s) =$ 13 TeV
1477806 . Measurement of electroweak production of a W boson and two forward jets in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1478600 X Measurement of the ZZ production cross section and Z $\to \ell^+\ell^-\ell'^+\ell'^-$ branching fraction in pp collisions at $\sqrt s$=13 TeV
1479163 ? Search for new phenomena in events with high jet multiplicity and low missing transverse momentum in proton–proton collisions at $\sqrt{s}=8$ TeV
1480862 X Measurement of the mass of the top quark in decays with a $J/\psi$ meson in pp collisions at 8 TeV
-1483165 . Dose rate effects in the radiation damage of the plastic scintillators of the CMS Hadron Endcap Calorimeter
+1483165 X Dose rate effects in the radiation damage of the plastic scintillators of the CMS Hadron Endcap Calorimeter
1484162 ! Measurement of the production cross section of a W boson in association with two b jets in pp collisions at $\sqrt{s} = 8{\,\mathrm{{TeV}}} $
1485195 ! Measurement of the total and differential inclusive $B^+$ hadron cross sections in pp collisions at $\sqrt{s}$ = 13 TeV
1485699 X The CMS trigger system
1485701 . Decomposing transverse momentum balance contributions for quenched jets in PbPb collisions at $ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=2.76 $ TeV
1485702 ? Search for high-mass diphoton resonances in proton–proton collisions at 13 TeV and combination with 8 TeV search
1486238 . Studies of inclusive four-jet production with two $b$-tagged jets in proton-proton collisions at 7 TeV
1487277 . Measurement and QCD analysis of double-differential inclusive jet cross sections in pp collisions at $ \sqrt{s}=8 $ TeV and cross section ratios to 2.76 and 7 TeV
1487278 . Measurement of inclusive jet cross sections in $pp$ and PbPb collisions at $\sqrt{s_{NN}}=$ 2.76 TeV
1487279 ? Search for narrow resonances in dilepton mass spectra in proton-proton collisions at $\sqrt{s}$ = 13 TeV and combination with 8 TeV data
1487288 X Measurement of the WZ production cross section in pp collisions at $\sqrt{s} = 7$ and 8 $\,\text{TeV}$ and search for anomalous triple gauge couplings at $\sqrt{s} = 8\,\text{TeV} $
1488103 ? Inclusive search for supersymmetry using razor variables in pp collisions at $\sqrt s=$ 13  TeV
1488280 ? Search for long-lived charged particles in proton-proton collisions at $\sqrt s=$ 13  TeV
1488581 ? Search for supersymmetry in events with one lepton and multiple jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1489183 ? Observation of charge-dependent azimuthal correlations in $p$-Pb collisions and its implication for the search for the chiral magnetic effect
1489189 . Suppression and azimuthal anisotropy of prompt and nonprompt ${\mathrm{J}}/\psi $ production in PbPb collisions at $\sqrt{{s_{_{\text {NN}}}}} =2.76$ $\,\mathrm{TeV}$
1489193 ? Cross section measurement of $t$-channel single top quark production in pp collisions at $\sqrt s =$ 13 TeV
1490903 ? Search for high-mass Z$\gamma$ resonances in $\mathrm{ e }^{+}\mathrm{ e }^{-}\gamma $ and $ \mu^{+}\mu^{-}\gamma$ final states in proton-proton collisions at $\sqrt{s} =$ 8 and 13 TeV
1491379 X Search for anomalous Wtb couplings and flavour-changing neutral currents in t-channel single top quark production in pp collisions at $\sqrt{s} =$ 7 and 8 TeV
-1491950 ! Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV
+1491950 . Measurement of differential cross sections for top quark pair production using the lepton+jets final state in proton-proton collisions at 13 TeV
1491953 . Measurements of differential cross sections for associated production of a W boson and jets in proton-proton collisions at $\sqrt{s} =$ 8 TeV
1492316 X Search for top quark decays via Higgs-boson-mediated flavor-changing neutral currents in pp collisions at $ \sqrt{s}=8 $ TeV
1492317 ? Search for electroweak production of charginos in final states with two τ leptons in pp collisions at $ \sqrt{s}=8 $ TeV
1492321 ? Search for R-parity violating supersymmetry with displaced vertices in proton-proton collisions at $\sqrt{s}$ = 8 TeV
1494067 X Observation of $\Upsilon$(1S) pair production in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1494580 ? Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos, and b quarks
1495025 ? Searches for invisible decays of the Higgs boson in pp collisions at $\sqrt{s}$ = 7, 8, and 13 TeV
1495237 X Measurement of the mass difference between top quark and antiquark in pp collisions at $\sqrt{s} = 8$ TeV
1495423 ? A search for new phenomena in pp collisions at $\sqrt{s} = 13\,\text {TeV} $ in final states with missing transverse momentum and at least one jet using the $\alpha _{\mathrm {T}}$ variable
1495840 . Relative Modification of Prompt ψ(2S) and J/ψ Yields from pp to PbPb Collisions at $\sqrt{s_{NN}}=5.02$ TeV
1495866 ! Suppression of $\Upsilon(1S), \Upsilon(2S)$ and $\Upsilon(3S)$ production in PbPb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV
1496050 . Charged-particle nuclear modification factors in PbPb and pPb collisions at $ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $ TeV
1497514 ? Search for dijet resonances in proton–proton collisions at $\sqrt{s}$ = 13 TeV and constraints on dark matter and other models
1497519 ! Measurements of differential production cross sections for a Z boson in association with jets in pp collisions at $ \sqrt{s}=8 $ TeV
1497736 . Measurement of the $t\bar{t}$ production cross section using events in the e$\mu$ final state in pp collisions at $\sqrt{s} =$ 13 TeV
1499471 ! Measurements of the associated production of a Z boson and b jets in pp collisions at ${\sqrt{s}} = 8\,\text {TeV} $
1499476 ? Search for heavy resonances decaying to tau lepton pairs in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1499477 ? Search for supersymmetry in events with photons and missing transverse energy in pp collisions at 13 TeV
1500513 X Search for CP violation in $ t\overline{t} $ production and decay in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1501681 ? Search for single production of a heavy vector-like T quark decaying to a Higgs boson and a top quark with a lepton and jets in the final state
1501683 ? Search for heavy neutrinos or third-generation leptoquarks in final states with two hadronically decaying $\tau$ leptons and two jets in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1502925 ? Searches for pair production of third-generation squarks in $\sqrt{s}=13$ $\,\text {TeV}$ pp collisions
1504209 ? Search for electroweak production of a vector-like quark decaying to a top quark and a Higgs boson using boosted topologies in fully hadronic final states
1507091 . Measurements of the charm jet cross section and nuclear modification factor in pPb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV
1507094 X Search for massive resonances decaying into WW, WZ or ZZ bosons in proton-proton collisions at $\sqrt{s} = $ 13 TeV
1507095 ? Measurement of electroweak-induced production of W$\gamma$ with two jets in pp collisions at $ \sqrt{s}=8 $ TeV and constraints on anomalous quartic gauge couplings
1507096 ? Search for heavy gauge W' boson in events with an energetic lepton and large missing transverse momentum at $ \sqrt{s} = $ 13 TeV
1507303 ? Search for high-mass $\mathrm{ Z }\gamma$ resonances in proton-proton collisions at $\sqrt{s}=$ 8 and 13 TeV using jet substructure techniques
1507892 ? Search for leptophobic Z′ bosons decaying into four-lepton final states in proton–proton collisions at $\sqrt s$ =8TeV
1508171 ? Search for supersymmetry in the all-hadronic final state using top quark tagging in pp collisions at $\sqrt s = 13$ TeV
1508172 X Mechanical stability of the CMS strip tracker measured with a laser alignment system
1508173 ? Search for light bosons in decays of the 125 GeV Higgs boson in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1508174 ? Search for dark matter and unparticles in events with a Z boson and missing transverse momentum in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1510260 ! Measurement of the $t \bar t$ production cross section using events with one lepton and at least one jet in pp collisions at $\sqrt{s}$ = 13 TeV
1510442 ? Search for new phenomena with multiple charged leptons in proton–proton collisions at $\sqrt{s}= 13$ $\,\text {TeV}$
1510567 ? Search for single production of vector-like quarks decaying to a Z boson and a top or a bottom quark in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1511277 ? Search for single production of vector-like quarks decaying into a b quark and a W boson in proton-proton collisions at $\sqrt s =$ 13 TeV
1511284 . Measurement of the inclusive energy spectrum in the very forward direction in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1511868 . Azimuthal anisotropy of charged particles with transverse momentum up to 100 GeV/ c in PbPb collisions at $\sqrt {s}_{{NN}}$=5.02 TeV
1512112 ! Study of Jet Quenching with $Z+\text{jet}$ Correlations in Pb-Pb and $pp$ Collisions at ${\sqrt{s}}_{NN}=5.02\text{ }\text{ }\mathrm{TeV}$
1512295 . Search for associated production of a Z boson with a single top quark and for tZ flavour-changing interactions in pp collisions at $ \sqrt{s}=8 $ TeV
1512296 ? Measurement of prompt and nonprompt $\mathrm{J}/{\psi }$ production in $\mathrm {p}\mathrm {p}$ and $\mathrm {p}\mathrm {Pb}$ collisions at $\sqrt{s_{\mathrm {NN}}} =5.02\,\text {TeV} $
1512924 ? Measurement of the cross section for electroweak production of Z$\gamma$ in association with two jets and constraints on anomalous quartic gauge couplings in proton–proton collisions at $\sqrt{s} = 8$ TeV
-1513926 . The Triple GEM Detector Control System for CMS forward muon spectrometer upgrade
+1513926 X The Triple GEM Detector Control System for CMS forward muon spectrometer upgrade
1514542 X Search for standard model production of four top quarks in proton-proton collisions at $\sqrt{s}$ = 13 TeV
1516191 ! Measurement of double-differential cross sections for top quark pair production in pp collisions at $\sqrt{s} = 8$ $\,\text {TeV}$ and impact on parton distribution functions <neil.warrack@cern.ch>
1516193 ? Search for dark matter produced with an energetic jet or a hadronically decaying W or Z boson at $ \sqrt{s}=13 $ TeV
1516412 X Measurement of the top quark mass using single top quark events in proton-proton collisions at $\sqrt{s}= 8$  TeV
1517191 ? Search for third-generation scalar leptoquarks and heavy right-handed neutrinos in final states with two tau leptons and two jets in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1517496 ? Search for associated production of dark matter with a Higgs boson decaying to $ \mathrm{b}\overline{\mathrm{b}} $ or $\gamma \gamma$ at $ \sqrt{s}=13$ TeV
1518145 X Search for anomalous couplings in boosted $\mathrm{ WW/WZ }\to\ell\nu\mathrm{ q \bar{q} }$ production in proton-proton collisions at $\sqrt{s} =$ 8 TeV
-1518399 . Measurement of the jet mass in highly boosted ${\mathrm{t}}\overline{\mathrm{t}}$ events from pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$
+1518399 ! Measurement of the jet mass in highly boosted ${\mathrm{t}}\overline{\mathrm{t}}$ events from pp collisions at $\sqrt{s}=8$ $\,\text {TeV}$
1518400 ? Search for a heavy resonance decaying to a top quark and a vector-like top quark at $ \sqrt{s}=13 $ TeV
1519995 . Search for new physics with dijet angular distributions in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1589287 ? Measurements of the pp $\to W\gamma\gamma$ and pp $\to Z\gamma\gamma$ cross sections and limits on anomalous quartic gauge couplings at $ \sqrt{s}=8 $ TeV
1591147 ? Search for $ \mathrm{t}\overline{\mathrm{t}} $ resonances in highly boosted lepton+jets and fully hadronic final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1593762 X Measurement of the top quark mass in the dileptonic $t\bar{t}$ decay channel using the mass observables $M_{b\ell}$, $M_{T2}$, and $M_{b\ell\nu}$ in pp collisions at $\sqrt{s}=8$ TeV
1594731 ? Search for physics beyond the standard model in events with two leptons of same sign, missing transverse momentum, and jets in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $
1594909 . Search for supersymmetry in multijet events with missing transverse momentum in proton-proton collisions at 13 TeV
1598036 ? Search for black holes in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=$13 TeV
1598460 ! Measurement of the triple-differential dijet cross section in proton-proton collisions at $\sqrt{s}=8\,\text {TeV} $ and constraints on parton distribution functions
1598467 X Search for Charged Higgs Bosons Produced via Vector Boson Fusion and Decaying into a Pair of $W$ and $Z$ Bosons Using $pp$ Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$
1599400 ? Search for new phenomena with the $M_{\mathrm {T2}}$ variable in the all-hadronic final state produced in proton–proton collisions at $\sqrt{s} = 13$ $\,\text {TeV}$
1599402 ? Search for Supersymmetry in $pp$ Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$ in the Single-Lepton Final State Using the Sum of Masses of Large-Radius Jets
1599548 ? Measurement of the ${B}^{\pm}$ Meson Nuclear Modification Factor in Pb-Pb Collisions at $\sqrt{{s}_{NN}}=5.02\text{ }\text{ }\mathrm{TeV}$
1601294 X Combination of searches for heavy resonances decaying to WW, WZ, ZZ, WH, and ZH boson pairs in proton–proton collisions at $\sqrt{s}=8$ and 13 TeV
1601505 ! Measurements of $t\bar{t}$ cross sections in association with $b$ jets and inclusive jets and their ratio using dilepton final states in pp collisions at $\sqrt{s}$ = 13 TeV
1601645 ? Search for Low Mass Vector Resonances Decaying to Quark-Antiquark Pairs in Proton-Proton Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$
1601901 X Search for top quark partners with charge 5/3 in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1603635 ? Search for dark matter produced in association with heavy-flavor quark pairs in proton-proton collisions at $\sqrt{s}=13$ TeV
1604273 ? Search for pair production of vector-like T and B quarks in single-lepton final states using boosted jet substructure in proton-proton collisions at $\sqrt{s}=13$ TeV
1604886 ? Search for new physics in the monophoton final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1605124 ? Searches for W′ bosons decaying to a top quark and a bottom quark in proton-proton collisions at 13 TeV
1605128 ? Search for top squark pair production in pp collisions at $ \sqrt{s}=13 $ TeV using single lepton events
1605397 X Particle-flow reconstruction and global event description with the CMS detector
1605749 ! Measurements of jet charge with dijet events in pp collisions at $\sqrt{s}=8$ TeV
1605750 ? Suppression of Excited $\Upsilon$ States Relative to the Ground State in Pb-Pb Collisions at $\sqrt{s_\mathrm{NN}}$=5.02 TeV
1607560 ? Measurement of the semileptonic $ \mathrm{t}\overline{\mathrm{t}} $ + γ production cross section in pp collisions at $ \sqrt{s}=8 $ TeV <neil.warrack@cern.ch>
1607561 . Exclusive and semi-exclusive pi+pi- production in proton-proton collisions at sqrt(s) = 7 TeV
1607793 ? Search for a heavy composite Majorana neutrino in the final state with two leptons and two quarks at $\sqrt{s}=13$ TeV
1608161 ? Search for electroweak production of charginos and neutralinos in WH events in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1608162 X Measurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at $ \sqrt{s}=13 $ TeV
-1608166 . Measurement of charged pion, kaon, and proton production in proton-proton collisions at $\sqrt{s}=13$ TeV
+1608166 ! Measurement of charged pion, kaon, and proton production in proton-proton collisions at $\sqrt{s}=13$ TeV
1608383 X Search for Higgs boson pair production in the $bb\tau\tau$ final state in proton-proton collisions at $\sqrt{(}s)=8\text{ }\text{ }\mathrm{TeV}$
1608386 X Constraints on anomalous Higgs boson couplings using production and decay information in the four-lepton final state
-1608556 . P-Type Silicon Strip Sensors for the new CMS Tracker at HL-LHC
+1608556 X P-Type Silicon Strip Sensors for the new CMS Tracker at HL-LHC
1608774 ? Search for heavy resonances that decay into a vector boson and a Higgs boson in hadronic final states at $\sqrt{s} = 13$ $\,\text {TeV}$
1609262 ? Search for Higgs boson pair production in events with two bottom quarks and two tau leptons in proton–proton collisions at $\sqrt s$ =13TeV
1609449 ? Search for direct production of supersymmetric partners of the top quark in the all-jets final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1609450 ? Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at $\sqrt{s} =$ 8 TeV
1610623 ! Measurement of the differential cross sections for the associated production of a $W$ boson and jets in proton-proton collisions at $\sqrt{s}=13$ TeV
1610629 ? Search for supersymmetry in events with at least one photon, missing transverse momentum, and large transverse event activity in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1611299 ? Search for the pair production of third-generation squarks with two-body decays to a bottom or charm quark and a neutralino in proton–proton collisions at $\sqrt{s}$ = 13 TeV
1611300 X Search for a light pseudoscalar Higgs boson produced in association with bottom quarks in pp collisions at $ \sqrt{s}=8 $ TeV
1613900 X Observation of the Higgs boson decay to a pair of $\tau$ leptons with the CMS detector
1614320 ? Search for single production of a vector-like T quark decaying to a Z boson and a top quark in proton-proton collisions at $\sqrt s$ = 13 TeV
-1614482 . Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in $p\mathrm{Pb}$ and PbPb collisions at the CERN Large Hadron Collider
+1614482 X Constraints on the chiral magnetic effect using charge-dependent azimuthal correlations in $p\mathrm{Pb}$ and PbPb collisions at the CERN Large Hadron Collider
1614779 ? Search for vectorlike light-flavor quark partners in proton-proton collisions at $\sqrt s$ =8  TeV
1615207 ? Measurement of vector boson scattering and constraints on anomalous quartic couplings from events with four leptons and two jets in proton–proton collisions at $\sqrt{s}=$ 13 TeV
1615780 . Measurement of prompt $D^0$ meson azimuthal anisotropy in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV
1615868 ? Search for resonant and nonresonant Higgs boson pair production in the $ \mathrm{b}\overline{\mathrm{b}}\mathit{\ell \nu \ell \nu } $ final state in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1616207 . Nuclear modification factor of D$^0$ mesons in PbPb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV
1616497 ? Search for massive resonances decaying into $WW$, $WZ$, $ZZ$, $qW$, and $qZ$ with dijet final states at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$
1618346 . Principal-component analysis of two-particle azimuthal correlations in PbPb and $p\text{Pb}$ collisions at CMS
1620050 ! Measurement of normalized differential $ \mathrm{t}\overline{\mathrm{t}} $ cross sections in the dilepton channel from pp collisions at $ \sqrt{s}=13 $ TeV <neil.warrack@cern.ch>
1620205 X Search for Evidence of the Type-III Seesaw Mechanism in Multilepton Final States in Proton-Proton Collisions at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$
1620470 ? Search for heavy resonances decaying to a top quark and a bottom quark in the lepton+jets final state in proton–proton collisions at 13 TeV
1620518 . Challenges to the chiral magnetic wave using charge-dependent azimuthal anisotropies in pPb and PbPb collisions at $\sqrt{\smash[b]{s_{_{\mathrm{NN}}}}} = $ 5.02 TeV
1620905 ! Measurement of the Splitting Function in $pp$ and Pb-Pb Collisions at $\sqrt{s_{_{\mathrm{NN}}}} =$ 5.02 TeV
1621281 ? Search for supersymmetry with Higgs boson to diphoton decays using the razor variables at $\sqrt{s} = $ 13 TeV
1623562 ? Search for Higgsino pair production in $pp$ collisions at $\sqrt{s}$ = 13  TeV in final states with large missing transverse momentum and two Higgs bosons decaying via $H \to b \bar b$
1624165 ! Search for electroweak production of charginos and neutralinos in multilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV <andy.buckley@cern.ch>
1624166 ? Inclusive search for a highly boosted Higgs boson decaying to a bottom quark-antiquark pair
1624170 X Observation of electroweak production of same-sign W boson pairs in the two jet and two same-sign lepton final state in proton-proton collisions at $\sqrt{s} = $ 13 TeV
1624694 X Observation of top quark production in proton-nucleus collisions
1625108 X Evidence for the Higgs boson decay to a bottom quark–antiquark pair
1625296 ? Measurements of the $\mathrm {p}\mathrm {p}\rightarrow \mathrm{Z}\mathrm{Z}$ production cross section and the $\mathrm{Z}\rightarrow 4\ell $ branching fraction, and constraints on anomalous triple gauge couplings at $\sqrt{s} = 13\,\text {TeV} $
1625745 ! Search for new phenomena in final states with two opposite-charge, same-flavor leptons, jets, and missing transverse momentum in pp collisions at $ \sqrt{s}=13 $ TeV
-1625783 . Brightness and uniformity measurements of plastic scintillator tiles at the CERN H2 test beam
+1625783 X Brightness and uniformity measurements of plastic scintillator tiles at the CERN H2 test beam
1626103 ? Observation of Correlated Azimuthal Anisotropy Fourier Harmonics in $pp$ and $p+Pb$ Collisions at the LHC
1627612 ? Search for supersymmetry in events with one lepton and multiple jets exploiting the angular correlation between the lepton and the missing transverse momentum in proton-proton collisions at $\sqrt{s} = $ 13 TeV
1628094 ? Search for low mass vector resonances decaying into quark-antiquark pairs in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1628648 ? Search for pair production of vector-like quarks in the bW$\overline{\mathrm{b}}$W channel from proton-proton collisions at $\sqrt{s} =$ 13 TeV
1629153 ! Study of dijet events with a large rapidity gap between the two leading jets in pp collisions at $\sqrt{s}=7$ $\,\text {TeV}$
1629160 ? Measurement of angular parameters from the decay $\mathrm{B}^0 \to \mathrm{K}^{*0} \mu^+ \mu^-$ in proton-proton collisions at $\sqrt{s} = $ 8 TeV
1630635 ? Search for a massive resonance decaying to a pair of Higgs bosons in the four b quark final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1631982 ! Pseudorapidity and transverse momentum dependence of flow harmonics in pPb and PbPb collisions
1631985 ! Measurement of differential cross sections in the kinematic angular variable $\phi^*$ for inclusive Z boson production in pp collisions at $\sqrt{s}=$ 8 TeV
1632444 X Measurement of b hadron lifetimes in pp collisions at $\sqrt{s} =$ 8 TeV
1632447 ? Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1632453 ! Pseudorapidity distributions of charged hadrons in proton-lead collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 and 8.16 TeV
1633423 X Search for standard model production of four top quarks with same-sign and multilepton final states in proton–proton collisions at $\sqrt{s} = 13\,\text {TeV} $
1633431 ? Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV
1633588 ? Search for supersymmetry in proton-proton collisions at 13 TeV using identified top quarks
1633763 ! Search for new physics in events with a leptonically decaying Z boson and a large transverse momentum imbalance in proton–proton collisions at $\sqrt{s} $ = 13 $\,\text {TeV}$
1634253 ? Search for top squarks and dark matter particles in opposite-charge dilepton final states at $\sqrt{s}=$ 13 TeV
1634835 . Measurement of associated Z + charm production in proton-proton collisions at $\sqrt{s} = $ 8 TeV
1634843 . Measurement of the cross section for top quark pair production in association with a W or Z boson in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1635271 ? Measurement of the inclusive $ \mathrm{t}\overline{\mathrm{t}} $ cross section in pp collisions at $ \sqrt{s}=5.02 $ TeV using final states with at least one charged lepton
1635889 . Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1635891 X Search for ZZ resonances in the 2$\ell$2$\nu$ final state in proton-proton collisions at 13 TeV
1635896 ? Search for excited quarks of light and heavy flavor in $\gamma +$ jet final states in proton–proton collisions at $\sqrt{s} =$ 13TeV
1636197 . Non-Gaussian elliptic-flow fluctuations in PbPb collisions at $\sqrt{\smash[b]{s_{_\text{NN}}}} = 5.02$ TeV
1637580 ? Search for gauge-mediated supersymmetry in events with at least one photon and missing transverse momentum in pp collisions at $\sqrt{s} = $ 13 TeV
1638988 ? Search for new long-lived particles at $\sqrt{s} =$ 13 TeV
1638996 . Study of jet quenching with isolated-photon+jet correlations in PbPb and pp collisions at $\sqrt{s_{_{\mathrm{NN}}}} =$ 5.02 TeV
1639443 ? Search for pair production of excited top quarks in the lepton + jets final state
1641267 ? Constraints on the double-parton scattering cross section from same-sign W boson pair production in proton-proton collisions at $ \sqrt{s}=8 $ TeV
1641762 ? Search for new physics in final states with an energetic jet or a hadronically decaying $W$ or $Z$ boson and transverse momentum imbalance at $\sqrt{s}=13\text{ }\text{ }\mathrm{TeV}$
1641763 ? Search for the flavor-changing neutral current interactions of the top quark and the Higgs boson which decays into a pair of b quarks at $\sqrt{s}=$ 13 TeV
1642230 ? Measurement of the associated production of a single top quark and a Z boson in pp collisions at $\sqrt{s} =$ TeV
1642233 ? Search for Z$\gamma$ resonances using leptonic and hadronic final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV
-1643640 . Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV
+1643640 ! Azimuthal correlations for inclusive 2-jet, 3-jet, and 4-jet events in pp collisions at $\sqrt{s}= $ 13 TeV
1643829 X Search for the X(5568) state decaying into $\mathrm{B}^{0}_{\mathrm{s}}\pi^{\pm}$ in proton-proton collisions at $\sqrt{s} = $ 8 TeV
1644362 X Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV
1644363 ? Search for lepton flavour violating decays of the Higgs boson to $\mu\tau$ and e$\tau$ in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1644364 . Bose-Einstein correlations in $pp, p\mathrm{Pb}$, and PbPb collisions at $\sqrt{{s}_{NN}}=0.9-7$ TeV
1644788 ? Search for Physics Beyond the Standard Model in Events with High-Momentum Higgs Bosons and Missing Transverse Momentum in Proton-Proton Collisions at 13 TeV
1644901 ! Search for $R$-parity violating supersymmetry in pp collisions at $\sqrt{s} = $ 13 TeV using b jets in a final state with a single lepton, many jets, and high sum of large-radius jet masses <andy.buckley@cern.ch>
1644903 . Measurement of prompt and nonprompt charmonium suppression in $\text {PbPb}$ collisions at 5.02 $\,\text {Te}\text {V}$
1645246 ? Electroweak production of two jets in association with a Z boson in proton–proton collisions at $\sqrt{s}= $ 13 $\,\text {TeV}$
1645630 ? Search for decays of stopped exotic long-lived particles produced in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1646260 . Search for new physics in events with two soft oppositely charged leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s}=$ 13 TeV
-1646584 . Radioactive source calibration test of the CMS Hadron Endcap Calorimeter test wedge with Phase I upgrade electronics
+1646584 X Radioactive source calibration test of the CMS Hadron Endcap Calorimeter test wedge with Phase I upgrade electronics
1647562 . Measurement of the $\mathrm{Z}\gamma^{*} \to \tau\tau$ cross section in pp collisions at $\sqrt{s} = $ 13 TeV and validation of $\tau$ lepton analysis techniques
1647947 ! Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1648162 ! Observation of medium induced modifications of jet fragmentation in PbPb collisions using isolated-photon-tagged jets
1650462 . Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at $ \sqrt{s}=13 $ TeV
1652833 . Comparing transverse momentum balance of b jet pairs in pp and PbPb collisions at $ \sqrt{s_{\mathrm{NN}}}=5.02 $ TeV
1653123 . Search for lepton-flavor violating decays of heavy resonances and quantum black holes to eμ final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1653127 . Search for single production of vector-like quarks decaying to a b quark and a Higgs boson
1653451 . Search for natural and split supersymmetry in proton-proton collisions at $ \sqrt{s}=13 $ TeV in final states with jets and missing transverse momentum
-1653948 ! Measurement of the inelastic proton-proton cross section at $ \sqrt{s}=13 $ TeV
+1653948 . Measurement of the inelastic proton-proton cross section at $ \sqrt{s}=13 $ TeV
1653954 . Search for heavy neutral leptons in events with three charged leptons in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1654926 ? Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV
1655968 . Search for narrow resonances in the b-tagged dijet mass spectrum in proton-proton collisions at $\sqrt{s} =$ 8 TeV
-1656983 . Quality control for the first large areas of triple-GEM chambers for the CMS endcaps
+1656983 X Quality control for the first large areas of triple-GEM chambers for the CMS endcaps
1657397 . Search for a heavy resonance decaying to a pair of vector bosons in the lepton plus merged jet final state at $ \sqrt{s}=13 $ TeV
1658057 . Jet properties in PbPb and pp collisions at $ \sqrt{s_{\mathrm{N}\;\mathrm{N}}}=5.02 $ TeV
1659106 . Search for third-generation scalar leptoquarks decaying to a top quark and a $\tau$ lepton at $\sqrt{s}=$ 13 TeV
-1662008 . Test beam demonstration of silicon microstrip modules with transverse momentum discrimination for the future CMS tracking detector
+1662008 X Test beam demonstration of silicon microstrip modules with transverse momentum discrimination for the future CMS tracking detector
1662081 . Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1662083 . Search for a heavy resonance decaying into a Z boson and a vector boson in the $ \nu \overline{\nu}\mathrm{q}\overline{\mathrm{q}} $ final state
-1662293 . Observation of proton-tagged, central (semi)exclusive production of high-mass lepton pairs in pp collisions at 13 TeV with the CMS-TOTEM precision proton spectrometer
+1662293 X Observation of proton-tagged, central (semi)exclusive production of high-mass lepton pairs in pp collisions at 13 TeV with the CMS-TOTEM precision proton spectrometer
1662661 X Evidence for associated production of a Higgs boson with a top quark pair in final states with electrons, muons, and hadronically decaying $\tau$ leptons at $\sqrt{s} =$ 13 TeV
1662926 ! Search for high-mass resonances in dilepton final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1663234 ? Search for additional neutral MSSM Higgs bosons in the $\tau\tau$ final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1663385 X Search for $\mathrm{t}\overline{\mathrm{t}}$H production in the all-jet final state in proton-proton collisions at $\sqrt{s}=$ 13 TeV
-1663452 . Search for new physics in dijet angular distributions using proton-proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models
-1663958 ! Measurement of differential cross sections for the production of top quark pairs and of additional jets in lepton+jets events from pp collisions at $\sqrt{s} =$ 13 TeV
+1663452 . Search for new physics in dijet angular distributions using proton–proton collisions at $\sqrt{s}=$ 13 TeV and constraints on dark matter and other models
+1663958 . Measurement of differential cross sections for the production of top quark pairs and of additional jets in lepton+jets events from pp collisions at $\sqrt{s} =$ 13 TeV
1664330 . Search for a heavy resonance decaying into a Z boson and a Z or W boson in 2ℓ2q final states at $ \sqrt{s}=13 $ TeV
1665226 . Search for a heavy right-handed W boson and a heavy neutrino in events with two same-flavor leptons and two jets at $\sqrt{s}=$ 13 TeV
1665228 ! Search for high-mass resonances in final states with a lepton and missing transverse momentum at $ \sqrt{s}=13 $ TeV
1666019 . Search for a new scalar resonance decaying to a pair of Z bosons in proton-proton collisions at $\sqrt{s}=13 $ TeV
1666824 X Observation of $\mathrm{t\overline{t}}$H production
1666825 X Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1667189 X Search for $\mathrm{t\overline{t}}$H production in the $H\to\mathrm{b\overline{b}}$ decay channel with leptonic $\mathrm{t\overline{t}}$ decays in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1667449 X Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at $\sqrt{s}=$ 13 TeV
1667854 ! Measurement of differential cross sections for Z boson production in association with jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1669245 . Search for disappearing tracks as a signature of new long-lived particles in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1670168 ! Elliptic flow of charm and strange hadrons in high-multiplicity pPb collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 8.16 TeV
-1671499 X Measurement of the top quark mass with lepton+jets final states using pp collisions at $\sqrt{s}=$ 13 TeV
+1671499 X Measurement of the top quark mass with lepton+jets final states using $\mathrm {p}$ $\mathrm {p}$ collisions at $\sqrt{s}=13\,\text {TeV} $
1672011 . Measurement of prompt $\psi$(2S) production cross sections in proton-lead and proton-proton collisions at $\sqrt{s_{_\mathrm{NN}}}=$ 5.02 TeV
1672941 X Constraining gluon distributions in nuclei using dijets in proton-proton and proton-lead collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 TeV
-1672962 ! Measurement of the groomed jet mass in PbPb and pp collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 TeV
+1672962 ! Measurement of the groomed jet mass in PbPb and pp collisions at $ \sqrt{s_{\mathrm{NN}}}=5.02 $ TeV
1672970 . Search for vector-like T and B quark pairs in final states with leptons at $\sqrt{s} =$ 13 TeV
-1673011 . Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two $\tau$ leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1673011 . Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state of two muons and two $\tau$ leptons in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1673197 . Search for top squarks decaying via four-body or chargino-mediated modes in single-lepton final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV
-1673362 . Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV
-1674077 ? Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1673362 . Search for black holes and sphalerons in high-multiplicity final states in proton-proton collisions at $ \sqrt{s}=13 $ TeV
+1674077 ? Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at $ \sqrt{s}=13 $ TeV
1674529 . Measurement of nuclear modification factors of $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) mesons in PbPb collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 TeV
1674926 . Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state with two b quarks and two $\tau$ leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV
-1674927 . Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=$ 13 TeV
+1674927 X Constraints on models of scalar and vector leptoquarks decaying to a quark and a neutrino at $\sqrt{s}=$ 13 TeV
1675256 X Observation of the $\chi_\mathrm{b1}$(3P) and $\chi_\mathrm{b2}$(3P) and measurement of their masses
1675818 ? Search for beyond the standard model Higgs bosons decaying into a $\mathrm{b\overline{b}}$ pair in pp collisions at $\sqrt{s} =$ 13 TeV
1676092 ? Search for Higgs boson pair production in the $\gamma\gamma\mathrm{b\overline{b}}$ final state in pp collisions at $\sqrt{s}=$ 13 TeV
1676212 ? Angular analysis of the decay B$^+$$\to$ K$^+\mu^+\mu^-$ in proton-proton collisions at $\sqrt{s} =$ 8 TeV
1676214 . Search for narrow and broad dijet resonances in proton-proton collisions at $ \sqrt{s}=13 $ TeV and constraints on dark matter mediators and other new particles
1676216 ? Measurement of the weak mixing angle using the forward-backward asymmetry of Drell-Yan events in pp collisions at 8 TeV
1676219 . Search for pair-produced resonances each decaying into at least four quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1677275 ? Search for a singly produced third-generation scalar leptoquark decaying to a $\tau$ lepton and a bottom quark in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1677276 . Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV
1677496 ? Observation of the Z$\to\psi\ell^+\ell^-$ decay in pp collisions at $\sqrt{s}=$ 13 TeV
1677677 . Search for dark matter produced in association with a Higgs boson decaying to $\gamma\gamma$ or $\tau^+\tau^-$ at $\sqrt{s} =$ 13 TeV
1677887 ? Measurements of properties of the Higgs boson decaying to a W boson pair in pp collisions at $\sqrt{s}=$ 13 TeV
1677905 . Search for supersymmetric partners of electrons and muons in proton-proton collisions at $\sqrt{s}=$ 13 TeV
-1678088 . Search for the decay of a Higgs boson in the $\ell\ell\gamma$ channel in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1678088 . Search for the decay of a Higgs boson in the $\ell\ell\gamma$ channel in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1680021 . Search for heavy Majorana neutrinos in same-sign dilepton channels in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1680022 ! Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV
-1680298 . RPC upgrade project for CMS Phase II
-1680318 ! Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $
-1680459 . Measurement of differential cross sections for inclusive isolated-photon and photon+jets production in proton-proton collisions at $\sqrt{s} =$ 13 TeV
-1681016 . Search for supersymmetry in events with a $\tau$ lepton pair and missing transverse momentum in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1680298 X RPC upgrade project for CMS Phase II
+1680318 . Measurement of charged particle spectra in minimum-bias events from proton–proton collisions at $\sqrt{s}=13\,\text {TeV} $
+1680459 ! Measurement of differential cross sections for inclusive isolated-photon and photon+jets production in proton-proton collisions at $\sqrt{s} =$ 13 TeV
+1681016 . Search for supersymmetry in events with a $\tau$ lepton pair and missing transverse momentum in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1681435 ! Study of the underlying event in top quark pair production in pp collisions at 13 TeV
1681436 . Search for heavy resonances decaying into a vector boson and a Higgs boson in final states with charged leptons, neutrinos and b quarks at $\sqrt{s}=$ 13 TeV
1681748 ! Measurement of inclusive and differential Higgs boson production cross sections in the diphoton decay channel in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1682069 X Precision measurement of the structure of the CMS inner tracking system using nuclear interactions
-1682495 ! Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at $\sqrt{s} =$ 13 TeV
+1682495 ! Measurements of the differential jet cross section as a function of the jet mass in dijet events from proton-proton collisions at $ \sqrt{s}=13 $ TeV
1682776 . Search for the Higgs boson decaying to two muons in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1682779 . Search for dark matter particles produced in association with a top quark pair at $\sqrt{s} =$ 13 TeV
1683312 . Searches for pair production of charginos and top squarks in final states with two oppositely charged leptons in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1684340 . Search for a W' boson decaying to a $\tau$ lepton and a neutrino in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1685054 . Search for narrow H$\gamma$ resonances in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1685201 . Search for resonances in the mass spectrum of muon pairs produced in association with b quark jets in proton-proton collisions at $\sqrt{s} =$ 8 and 13 TeV
1685232 . Search for production of Higgs boson pairs in the four b quark final state using large-area jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1685235 . Search for heavy resonances decaying into two Higgs bosons or into a Higgs boson and a W or Z boson in proton-proton collisions at 13 TeV
1685989 . Search for pair-produced resonances decaying to quark pairs in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1685992 . Search for long-lived particles with displaced vertices in multijet events in proton-proton collisions at $\sqrt{s}= $13 TeV
-1686000 . Evidence for the associated production of a single top quark and a photon in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1686000 ! Evidence for the associated production of a single top quark and a photon in proton-proton collisions at $\sqrt{s}=$ 13 TeV <andy.buckley@cern.ch>
1686833 . Search for an $L_{\mu}-L_{\tau}$ gauge boson using Z$\to4\mu$ events in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1687544 . Search for pair production of second-generation leptoquarks at $\sqrt{s}=$ 13 TeV
-1688938 . Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at $\sqrt{s} =$ 8 TeV
-1690148 . Measurement of jet substructure observables in $\mathrm{t\overline{t}}$ events from proton-proton collisions at $\sqrt{s}=$ 13TeV
-1691854 . Observation of Higgs boson decay to bottom quarks
-1692558 . Charged-particle nuclear modification factors in XeXe collisions at $\sqrt{s_\mathrm{NN}}=$ 5.44 TeV
+1688938 . Search for a charged Higgs boson decaying to charm and bottom quarks in proton-proton collisions at $ \sqrt{s}=8 $ TeV
+1690148 ! Measurement of jet substructure observables in $\mathrm{t\overline{t}}$ events from proton-proton collisions at $\sqrt{s}=$ 13TeV
+1691854 X Observation of Higgs boson decay to bottom quarks
+1692558 ? Charged-particle nuclear modification factors in XeXe collisions at $ \sqrt{s_{\mathrm{NN}}} = 5.44 $ TeV
1692559 . Search for physics beyond the standard model in high-mass diphoton events from proton-proton collisions at $\sqrt{s} =$ 13 TeV
-1693412 . Performance of reconstruction and identification of $\tau$ leptons decaying to hadrons and $\nu_\tau$ in pp collisions at $\sqrt{s}=$ 13 TeV
-1693614 . Studies of B$^*_\mathrm{s2}(5840)^0$ and B$_\mathrm{s1}(5830)^0$ mesons including the observation of the B$^*_\mathrm{s2}(5840)^0\to$ B$^0$K$_\mathrm{S}^0$ decay in proton-proton collisions at $\sqrt{s}=$8 TeV
+1693412 X Performance of reconstruction and identification of $\tau$ leptons decaying to hadrons and $\nu_\tau$ in pp collisions at $\sqrt{s}=$ 13 TeV
+1693614 X Studies of ${\mathrm {B}} ^{*{\mathrm {s}}2}(5840)^0 $ and ${\mathrm {B}} _{{\mathrm {s}}1}(5830)^0 $ mesons including the observation of the ${\mathrm {B}} ^{*{\mathrm {s}}2}(5840)^0 \rightarrow {\mathrm {B}} ^0 \mathrm {K} ^0_{\mathrm {S}} $ decay in proton-proton collisions at $\sqrt{s}=8\,\text {TeV} $
1693616 . Search for the associated production of the Higgs boson and a vector boson in proton-proton collisions at $\sqrt{s}=$ 13 TeV via Higgs boson decays to $\tau$ leptons
1694380 . Search for invisible decays of a Higgs boson produced through vector boson fusion in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1694381 . Search for leptoquarks coupled to third-generation quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV
1695278 . Jet shapes of isolated photon-tagged jets in PbPb and pp collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV
1695301 . Search for single production of vector-like quarks decaying to a top quark and a W boson in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1696325 . Measurement of exclusive $\Upsilon$ photoproduction from protons in pPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV
-1696607 . Combined measurements of Higgs boson couplings in proton-proton collisions at $\sqrt{s}=$ 13 TeV
-1696608 . Search for new physics in final states with a single photon and missing transverse momentum in proton--proton collisions at $\sqrt{s} =$ 13 TeV
+1696402 X Fast timing measurement for CMS RPC Phase-II upgrade
+1696607 X Combined measurements of Higgs boson couplings in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1696608 ! Search for new physics in final states with a single photon and missing transverse momentum in proton-proton collisions at $\sqrt{s} =$ 13 TeV
1696868 . Observation of prompt J/$\psi$ meson elliptic flow in high-multiplicity pPb collisions at $\sqrt{s_\mathrm{NN}} =$ 8.16 TeV
+1697570 . Search for top quark partners with charge 5/3 in the same-sign dilepton and single-lepton final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV
+1697571 . Measurement of B$^0_\mathrm{s}$ meson production in pp and PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV
+1697838 . Evidence for light-by-light scattering and searches for axion-like particles in ultraperipheral PbPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV
+1698385 . Centrality and pseudorapidity dependence of the transverse energy density in pPb collisions at $\sqrt{s_\mathrm{NN}}=$ 5.02 TeV
+1698822 . Search for resonant $\mathrm{t \bar{t}}$ production in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1700167 . Search for pair-produced three-jet resonances in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1700173 . Search for new particles decaying to a jet and an emerging jet
+1700175 . Search for rare decays of Z and Higgs bosons to J$/\psi$ and a photon in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1700575 . Studies of beauty suppression via nonprompt D$^0$ mesons in PbPb collisions at $\sqrt{s_\mathrm{NN}}=$ 5.02 TeV
+1700756 . Search for low-mass resonances decaying into bottom quark-antiquark pairs in proton-proton collisions at $\sqrt{s} =$ 13 TeV
+1700771 . Search for nonresonant Higgs boson pair production in the $\mathrm{b\overline{b}b\overline{b}}$ final state at $\sqrt{s} =$ 13 TeV
+1701612 ! Event shape variables measured using multijet final states in proton-proton collisions at $\sqrt{s} =$ 13 TeV
+1701635 . Search for heavy neutrinos and third-generation leptoquarks in hadronic states of two $\tau$ leptons and two jets in proton-proton collisions at $\sqrt{s} =$ 13 TeV
+1702163 . Search for pair production of first-generation scalar leptoquarks at $\sqrt{s}=$ 13 TeV
+1702433 . Search for excited leptons in $\ell\ell\gamma$ final states in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1703980 . Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1703993 ! Measurements of $\mathrm{t\overline{t}}$ differential cross sections in proton-proton collisions at $\sqrt{s}=$ 13 TeV using events containing two leptons
+1704130 . Search for a W' boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state
+1704319 . Search for long-lived particles decaying into displaced jets in proton-proton collisions at $\sqrt{s}=$ 13 TeV
+1704494 . Search for a standard model-like Higgs boson in the mass range between 70 and 110 GeV in the diphoton final state in proton-proton collisions at $\sqrt{s}=$ 8 and 13 TeV
+1704939 ? Combination of searches for Higgs boson pair production in proton-proton collisions at $\sqrt{s} = $ 13 TeV
+1704945 . Search for associated production of a Higgs boson and a single top quark in proton-proton collisions at $\sqrt{s} =$ 13 TeV
+1704953 . Search for resonant production of second-generation sleptons with same-sign dimuon events in proton-proton collisions at $\sqrt{s} =$ 13 TeV
+1704960 . Search for dark matter in events with a leptoquark and missing transverse momentum in proton-proton collisions at 13 TeV
+1705068 . Measurement of associated production of a W boson and a charm quark in proton-proton collisions at $\sqrt{s} =$ 13 TeV
+1706172 . A search for pair production of new light bosons decaying into muons in proton-proton collisions at 13 TeV
+1706995 . Measurement of inclusive very forward jet cross sections in proton-lead collisions at $\sqrt{s_\mathrm{NN}}=$ 5.02 TeV
diff --git a/doc/rivet-coverage-lhcb.rank b/doc/rivet-coverage-lhcb.rank
--- a/doc/rivet-coverage-lhcb.rank
+++ b/doc/rivet-coverage-lhcb.rank
@@ -1,453 +1,458 @@
865584 . Prompt $K^0_s$ production in $pp$ collisions at $\sqrt{s}=0.9~\rm{TeV}$
867355 . Measurement of $\sigma(pp \to b \bar{b} X)$ at $\sqrt{s}=7~\rm{TeV}$ in the forward region
886284 ? First observation of $B^0_s \to J/\psi f_0(980)$ decays
886536 ? First observation of $\bar{B}^0_s \to D_{s2}^{*+} X \mu^-\bar{\nu}$ decays
891233 ? Measurement of $J/\psi$ production in $pp$ collisions at $\sqrt{s}=7~\rm{TeV}$
892495 ? Search for the rare decays $B^0_s \to \mu^+\mu^-$ and $B^0 \to \mu^+\mu^-$
914506 . Determination of $f_s/f_d$ for $7~\rm{TeV}$ $pp$ collisions and a measurement of the branching fraction of the decay $B_d\to D^-K^+$
917009 . Measurement of $V^0$ production ratios in $pp$ collisions at $\sqrt{s} = 0.9$ and $7~\rm{TeV}$
919315 . Measurement of the inclusive $\phi$ cross-section in $pp$ collisions at $\sqrt{s}=$ 7 TeV
926280 X Observation of $J/\psi$ pair production in $pp$ collisions at $\sqrt{s}=7 TeV$
930219 . Measurements of the Branching fractions for $B_{(s)} \to D_{(s)}\pi\pi\pi$ and $\Lambda_b^0 \to \Lambda_c^+\pi\pi\pi$
930417 ? Search for the lepton number violating decays $B^{+}\to \pi^- \mu^+ \mu^+$ and $B^{+}\to K^- \mu^+ \mu^+$
939619 X Absolute luminosity measurements with the LHCb detector at the LHC
940142 X First observation of the decay $\bar{B}^0_s \to D^0 K^{*0}$ and a measurement of the ratio of branching fractions $\frac{{\cal B}(\bar{B}^0_s \to D^0 K^{*0})}{{\cal B}(\bar{B}^0 \to D^0 \rho^0)}$
940366 X Search for CP violation in $D^{+} \to K^{-}K^{+}\pi^{+}$ decays
944152 . Measurement of the effective $B^0_s\rightarrow K^+K^-$ lifetime
945381 . Measurement of $b$-hadron production fractions in $7~\rm{TeV}$ pp collisions
946440 X First observation of the decay $B^0_s \to K^{*0} \bar{K}^{*0}$
1079920 ? Evidence for CP violation in time-integrated $D^0 \to h^-h^+$ decay rates
1080385 . Search for the rare decays $B^0_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$
1081268 . Measurement of the CP violating phase $\phi_s$ in $\bar{B}^0_s \to J/\psi f_0(980)$
1081275 . Measurement of the CP-violating phase $\phi_s$ in the decay $B^0_s\to J/\psi \phi$
1081581 . Differential branching fraction and angular analysis of the decay $B^{0} \to K^{*0} \mu^+ \mu^-$
1082063 . Measurement of the $B^0_s - \bar{B}^0_s$ oscillation frequency $\Delta m_s$ in $B^0_s \to D_s^-(3) \pi$ decays
1082327 . Measurement of mixing and CP violation parameters in two-body charm decays
1082328 . Observation of $B_s \to J/\psi f^\prime_2(1525)$ in $J/\psi K^+K^-$ final states
1082369 . Measurement of charged particle multiplicities in $pp$ collisions at ${\sqrt{s} =7}$TeV in the forward region
1082449 . Measurement of $b$-hadron masses
1082706 . Observation of $X(3872) $ production in $pp$ collisions at $\sqrt{s}=7$ TeV
1085516 . First observation of the decays $\bar{B}^0 \to D^{+} K^{-} \pi^{+} \pi^{-}$ and $B^{-} \to D^0 K^{-} \pi^{+} \pi^{-}$
1085982 ? Searches for Majorana neutrinos in $B^-$ decays
1087907 . Measurement of the cross-section ratio $\sigma(\chi_{c2})/\sigma(\chi_{c1})$ for prompt $\chi_c$ production at $\sqrt{s}=7$ TeV
1089837 . Determination of the sign of the decay width difference in the $B_s$ system
1089993 . Measurement of the $B^\pm$ production cross-section in $pp$ collisions at $\sqrt{s}=7$ TeV
1090061 . Opposite-side flavour tagging of B mesons at the LHCb experiment
1090150 . Search for the $X(4140)$ state in $B^+ \to J/\psi \phi K^+$ decays
1090895 X First evidence of direct $C\!P$ violation in charmless two-body decays of $B^0_s$ mesons
1090962 . Measurement of the ratio of branching fractions $\mathcal{B}(B^0\to K^{*0}\gamma)/\mathcal{B}(B_s^0\to\phi\gamma)$
1091071 . Measurement of Upsilon production in pp collisions at $\sqrt{s}$ = 7 TeV
1094045 . Measurements of the branching fractions and $C\!P$ asymmetries of $B^{\pm} \to J\!/\!\psi\, \pi^{\pm}$ and $B^{\pm} \to \psi(2S) \pi^{\pm}$ decays
1094080 . Observation of CP violation in $B^\pm \to DK^\pm$ decays
1094383 . Strong constraints on the rare decays $B_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$
1097092 . First observation of the decay $B_c^+ \to J/\psi \pi^+\pi^-\pi^+$
1104751 . Measurements of the branching fractions of the decays $B^{0}_{s} \to D^{\mp}_{s} K^{\pm} $ and $B^{0}_{s} \to D^{-}_{s} \pi^{+}$
1104754 X Measurement of $\psi(2S)$ meson production in pp collisions at $\sqrt{s}$=7 TeV
1107645 . Measurement of the ratio of prompt $\chi_{c}$ to $J/\psi$ production in $pp$ collisions at $\sqrt{s}=7$ TeV
1107729 . Inclusive $W$ and $Z$ production in the forward region at $\sqrt{s} = 7$ TeV
1110692 X Measurement of the polarization amplitudes and triple product asymmetries in the $B_s^0 \to \phi\phi$ decay
1112264 X Analysis of the resonant components in $B_s \to J/\psi\pi^+\pi^-$
1112268 X Measurement of the CP-violating phase $\phi_s$ in $\overline{B}^0_s \to J/\psi\pi^+\pi^-$ decays
1113593 ? Measurement of the $D_s^+ - D_s^-$ production asymmetry in 7 TeV $pp$ collisions
1113594 X Measurement of relative branching fractions of B decays to $\psi(2S)$ and $J/\psi$ mesons
1113595 X Measurement of the $B_s^0\to J/\psi K_S^0$ branching fraction
1113596 X Observation of double charm production involving open charm in pp collisions at $\sqrt{s}$ = 7 TeV
1114752 . Measurement of the isospin asymmetry in $B \to K^{(*)}\mu^+\mu^-$ decays
1114753 . Observation of excited $\Lambda_b^0$ baryons
1118162 . Measurement of $b$-hadron branching fractions for two-body decays into charmless charged hadrons
1119400 . Measurement of prompt hadron production ratios in $pp$ collisions at $\sqrt{s} = $ 0.9 and 7 TeV
1121120 X Measurement of the $B_s$ effective lifetime in the $J/\psi f_0(980)$ final state
1123797 X Observation of $B^0 \to \bar{D}^0 K^+ K^-$ and evidence of $B^0_s \to \bar{D}^0 K^+ K^-$
1123798 . Measurement of the effective $B_s^0 \rightarrow K^+ K^-$ lifetime
1123799 . Study of $D_{sJ}$ decays to $D^+K^0_S$ and $D^0K^+$ final states in $pp$ collisions
1125853 X Measurement of the $B^0_s \rightarrow J/\psi \bar{K}^{*0}$ branching fraction and angular amplitudes
1127719 . Implications of LHCb measurements and future prospects
1184177 . Measurement of the fraction of $\Upsilon(1S)$ originating from $\chi_b(1P)$ decays in $pp$ collisions at $\sqrt{s} = 7$ TeV
1184178 . Measurement of the ratio of branching fractions $BR(B_0 \to K^{\star 0} \gamma)/BR(B_{s0} \to \phi \gamma)$ and the direct CP asymmetry in $B_0 \to K^{\star 0} \gamma$
1186389 . Search for the rare decay $K_S \to \mu^+ \mu^-$
1186557 . Differential branching fraction and angular analysis of the $B^{+} \rightarrow K^{+}\mu^{+}\mu^{-}$ decay
1188009 . Measurements of $B_c^+$ production and mass with the $B_c^+ \to J/\psi \pi^+$ decay
1188164 . A model-independent Dalitz plot analysis of $B^\pm \to D K^\pm$ with $D \to K^0_{\rm S} h^+h^-$ ($h=\pi, K$) decays and constraints on the CKM angle $\gamma$
1189187 . First evidence for the annihilation decay mode $B^{+} \to D_{s}^{+} \phi$
1189991 . Evidence for the decay $B^0\to J/\psi \omega$ and measurement of the relative branching fractions of $B^0_s$ meson decays to $J/\psi\eta$ and $J/\psi\eta^{'}$
1189993 . First observation of the decay $B^{+} \rightarrow \pi^{+} \mu^{+} \mu^{-}$
1190679 X Measurement of the D+/- production asymmetry in 7 TeV pp collisions
1190893 X Measurement of the $C\!P$ asymmetry in $B^0 \to K^{*0} \mu^+ \mu^-$ decays
1192922 . A study of the $Z$ production cross-section in $pp$ collisions at $\sqrt{s} = 7$ TeV using tau final states
1193340 . Measurement of the $B^0$--$\bar B^0$ oscillation frequency $\Delta m_d$ with the decays $B^0 \to D^- \pi^+$ and $B^0 \to J\ \psi K^{*0}$
1198431 X Observation of $D^0 - \overline{D}^0$ oscillations
1199002 X First observation of the decays $\bar{B}^0_{(s)}\to D_s^+K^-\pi^+\pi^-$ and $\bar{B}^0_s\to D_{s1}(2536)^+\pi^-$
1202279 X First Evidence for the Decay $B_s^0 \to \mu^+ \mu^-$
1203846 X First observation of the decay $B_{s2}^*(5840)^0 \to B^{*+} K^-$ and studies of excited $B^0_s$ mesons
1203851 X Measurement of the time-dependent $CP$ asymmetry in $B^0 \to J/\psi K^0_{\rm S}$ decays
1205646 . Measurement of $J/\psi$ production in $pp$ collisions at $\sqrt{s}=2.76$ TeV
1208102 . Measurement of the cross-section for $Z \to e^+e^-$ production in $pp$ collisions at $\sqrt{s}=7$ TeV
1208105 . Measurement of the forward energy flow in $pp$ collisions at $\sqrt{s}=7$ TeV
1208305 . Measurement of CP observables in $B^0 \to D K^{*0}$ with $D \to K^+ K^-$
1215607 . Measurement of the fragmentation fraction ratio $f_{s}/f_{d}$ and its dependence on $B$ meson kinematics
1215769 ? Analysis of the resonant components in $B^¯+0 \to J/\psi\pi^+\pi^-$
1216886 . Exclusive $J/\psi$ and $\psi$(2S) production in pp collisions at $ \sqrt{s} = 7$ TeV
1217726 X Measurement of the $\Lambda_b^0$, $\Xi_b^-$ and $\Omega_b^-$ baryon masses
1217862 X Amplitude analysis and the branching fraction measurement of $\bar{B}^0_s \to J/\psi K^+K^-$
1218996 . Prompt charm production in pp collisions at sqrt(s)=7 TeV
1220792 ? Measurements of the $\Lambda_b^0 \to J/\psi \Lambda$ decay amplitudes and the $\Lambda_b^0$ polarisation in $pp$ collisions at $\sqrt{s} = 7$ TeV
1221043 . First observations of $\bar{B}_s^0 \to D^+D^-$, $D_s^+D^-$ and $D^0\bar{D}^0$ decays
1221245 X Determination of the X(3872) meson quantum numbers
1221248 X Observations of $B^0_s \rightarrow\psi(2S)\eta$ and $B^0_{(s)}\rightarrow\psi(2S)\pi^+\pi^-$ decays
1221251 . Search for the decay $B_s^0 \to D^{*\mp} \pi^\pm$
1222505 X Search for rare $B^0_{(s)}\rightarrow \mu^+ \mu^- \mu^+ \mu^-$ decays
1222846 X Observation of the decay $B_c^+ \to \psi(2S)\pi^+$
1223327 X Search for direct CP violation in D0 -> h- h+ modes using semileptonic B decays
1224274 X Observation of the suppressed ADS modes $B^\pm \to [\pi^\pm K^\mp \pi^+\pi^-]_D K^\pm$ and $B^\pm \to [\pi^\pm K^\mp \pi^+\pi^-]_D \pi^\pm$
1224542 X Search for CP violation in D+ -> phi pi+ and Ds+ -> Ks pi+ decays
1225663 . Study of $B^0 \to D^{*-} \pi^+ \pi^- \pi^+$ and $B^0 \to D^{*-}K^+\pi^-\pi^+$ decays
1225786 X First measurement of the CP-violating phase in $B_s^0 \to \phi \phi$ decays
1225787 . Measurements of the branching fractions of $B^{+} \to p \bar p K^{+}$ decays
1227655 . Limits on neutral Higgs boson production in the forward region in $pp$ collisions at $\sqrt{s} = 7$ TeV
1227656 X Measurement of CP violation and the $B^0_s$ meson decay width difference with $B^0_s$ → $J/ψK^+K^-$ and $B^0_s$ → $J/ψπ^+π^-$ decays
1227805 X Measurement of the $B^0 \rightarrow K^{*0}e^+e^-$ branching fraction at low dilepton mass
1228504 . Measurement of the effective B_s^0 -> J/{\psi} K_S^0 lifetime
1228505 X Searches for violation of lepton flavour and baryon number in tau lepton decays at LHCb
1228506 . Observation of $B^+_c \rightarrow J/\psi D_s^+$ and $B^+_c \rightarrow J/\psi D_s^{*+}$ decays
1228694 . Precision measurement of the $B^{0}_{s}$-$\bar{B}^{0}_{s}$ oscillation frequency with the decay $B^{0}_{s}\rightarrow D^{-}_{s}\pi^{+}$
1229496 X First observation of $CP$ violation in the decays of $B^0_s$ mesons
1229503 X Measurement of the branching fractions of the decays $B^0_s \to \overline{D}^0K^-\pi^+$ and $B^0 \to \overline{D}^0K^+\pi^-$
1229504 X Differential branching fraction and angular analysis of the decay $B^{0} \to K^{*0} \mu^{+}\mu^{-}$
1229506 X Search for D+(s) to pi+ mu+ mu- and D+(s) to pi- mu+ mu+ decays
1230340 X Precision measurement of D meson mass differences
1230344 . Production of J/psi and Upsilon mesons in pp collisions at sqrt(s) = 8 TeV
1232503 X Measurement of the CKM angle $\gamma$ from a combination of $B^{\pm} \to Dh^{\pm}$ analyses
1232507 X Differential branching fraction and angular analysis of the decay $B_s^0\to\phi\mu^{+}\mu^{-}$
1235028 X Search for the rare decay $D^0 \to \mu^+ \mu^-$
1235731 X Observation of $B^0_s\rightarrow\chi_{c1}\phi$ decay and study of $B^0\rightarrow\chi_{c1,2}K^{*0}$ decays
1237228 X Measurement of CP violation in the phase space of $B^{\pm} \to K^{\pm} \pi^{+} \pi^{-}$ and $B^{\pm} \to K^{\pm} K^{+} K^{-}$ decays
1237918 X First observation of the decay $B_s^0 \rightarrow \phi \bar{K}^{*0}$
1238106 ? Measurement of the differential branching fraction of the decay $\Lambda_b^0\rightarrow\Lambda\mu^+\mu^-$
1238809 . Measurement of B meson production cross-sections in proton-proton collisions at $\sqrt{s}$ = 7 TeV
1239158 . Searches for $B^0_{(s)} \to J/\psi p\bar{p}$ and $B^+ \to J/\psi p\bar{p}\pi^+$ decays
1240498 X First observation of the decay $B_{c}^{+}\to J/\psi K^+$
1242008 X Precision measurement of the $\Lambda_b$ baryon lifetime
1242126 ? Measurement of the polarization amplitudes in $B^0 \to J/\psi K^{*}(892)^0$ decays
1242869 . Measurement of the relative rate of prompt $\chi_{c0}$, $\chi_{c1}$ and $\chi_{c2}$ production at $\sqrt{s}=7$TeV
1243156 . Study of $D_J$ meson decays to $D^+\pi^-$, $D^0 \pi^+$ and $D^{*+}\pi^-$ final states in pp collision
1243421 X Search for the lepton-flavor violating decays $B^0_s \rightarrow e^{\pm}\mu^{\mp}$ and $B^0 \rightarrow e^{\pm} \mu^{\mp}$
1243424 X Measurement of the $B^0_s \to \mu^+ \mu^-$ branching fraction and search for $B^0 \to \mu^+ \mu^-$ decays at the LHCb experiment
1244131 . Studies of the decays $B^+ \to p \bar p h^+$ and observation of $B^+ \to \kern 0.1em\bar{\kern -0.1em\Lambda}(1520)p$
1244315 . Measurement of $J/\psi$ polarization in $pp$ collisions at $\sqrt{s}=7$ TeV
1245025 X Observation of a resonance in $B^+ \to K^+ \mu^+\mu^-$ decays at low recoil
1245030 . Study of $B_{(s)}^0 \to K_{\rm S}^0 h^{+} h^{\prime -}$ decays with first observation of $B_{s}^0 \to K_{\rm S}^0 K^{\pm} \pi^{\mp}$ and $B_{s}^0 \to K_{\rm S}^0 \pi^{+} \pi^{-}$
1246367 X First evidence for the two-body charmless baryonic decay $B^0 \to p \bar{p}$
1246368 . Measurement of the flavour-specific CP-violating asymmetry $a_{sl}^s$ in $B_s^0$ decays
1246783 X Branching fraction and CP asymmetry of the decays $B^+ \to K_{\rm \scriptscriptstyle S}^0 \pi^+$ and $B^+ \to K_{\rm \scriptscriptstyle S}^0 K^+$
1246784 . Observation of $B^0_s$-$\bar{B}^0_s$ mixing and measurement of mixing frequencies using semileptonic B decays
1246785 . Measurement of the $CP$ asymmetry in $B^+ \rightarrow K^+ \mu^+ \mu^-$ decays
1246901 . First measurement of time-dependent $C\!P$ violation in $B^0_s \to K^+K^-$ decays
1247054 . Measurement of Form-Factor-Independent Observables in the Decay $B^{0} \to K^{*0} \mu^+ \mu^-$
1247810 . Model-independent search for $CP$ violation in $D^{0} \to K^{-}K^{+}\pi^{-}\pi^{+}$ and $D^{0} \to \pi^{-}\pi^{+}\pi^{+}\pi^{-}$ decays
1250004 . Observation of the Decay $B^+_c → B^0_sπ^+$
1250005 . Observation of the decay $B_s^0\to\bar{D}^0\phi$
1251062 X First observation of $\bar B^0 \to J/\psi K^+K^-$ and search for $\bar B^0 \to J/\psi\phi$ decays
1251899 . Study of $J/\psi$ production and cold nuclear matter effects in $pPb$ collisions at $\sqrt{s_{NN}} = 5$ TeV
1252556 X Observation of the decay $B_c \rightarrow J/\psi K^+ K^- \pi^+ $
1254225 ? Measurement of the charge asymmetry in $B^{\pm}\rightarrow \phi K^{\pm}$ and search for $B^{\pm}\rightarrow \phi \pi^{\pm}$ decays
1255432 X Measurement of $D^0–\bar D^0$ Mixing Parameters and Search for $CP$ Violation Using $D^0 \to K^+ \pi^-$ Decays
1257611 . Observation of $\bar{B}_{(s)} \to J/\psi f_1$(1285) Decays and Measurement of the $f_1$(1285) Mixing Angle
1257744 . Search for the decay $D_0 \to \pi^+ \pi^- \mu^+ \mu^-$
1257745 X Search for the doubly charmed baryon $\Xi_{cc}^+$
1261027 . Measurement of CP violation in the phase space of $B^{\pm} \rightarrow K^{+} K^{-} \pi^{\pm}$ and $B^{\pm} \rightarrow \pi^{+} \pi^{-} \pi^{\pm}$ decays
1262317 . Measurements of indirect CP asymmetries in $D^0\to K^-K^+$ and $D^0\to\pi^-\pi^+$ decays
1262699 . Search for CP violation in the decay $D^+ \to \pi^-\pi^+\pi^+$
1262703 . Study of forward Z + jet production in pp collisions at $\sqrt{s} = 7$ TeV
1265071 . Studies of beauty baryon decays to $D^0 p h^-$ and $\Lambda_c^+ h^-$ final states
1267510 X Measurement of the $\bar{B}_s^0\to D_s^-D_s^+$ and $\bar{B}_s^0\to D^-D_s^+$ effective lifetimes
1277075 . Observation of associated production of a Z boson with a D meson in the forward region
1277076 . Updated measurements of exclusive $J/\psi$ and $\psi$(2S) production cross-sections in pp collisions at $\sqrt{s}=7$ TeV
1278342 X Search for Majorana neutrinos in $B^- \to \pi^+\mu^-\mu^-$ decays
1278863 X Measurement of the $B_c^+$ meson lifetime using $B_c^+ \to J\!/\!\psi \mu^+ \nu_{\mu} X$ decays
1280069 X Searches for $\Lambda^0_{b}$ and $\Xi^{0}_{b}$ decays to $K^0_{\rm S} p \pi^{-}$ and $K^0_{\rm S}p K^{-}$ final states with first observation of the $\Lambda^0_{b} \rightarrow K^0_{\rm S}p \pi^{-}$ decay
1280929 . Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}=2.76$ TeV
1280930 X Measurements of the $B^+, B^0, B^0_s$ meson and $\Lambda^0_b$ baryon lifetimes
1281231 X A study of CP violation in $B^{\pm} \to DK^{\pm}$ and $B^{\pm} \to D\pi^{\pm}$ decays with $D \to K_S^0K^{\pm}\pi^{\mp}$ final states
1281685 . Measurement of charged particle multiplicities and densities in $pp$ collisions at $\sqrt{s}=7\;$TeV in the forward region
1282444 X Precision measurement of the ratio of the $\Lambda^0_b$ to $\overline{B}^0$ lifetimes
1282445 X Measurement of resonant and CP components in $\bar{B}_s^0\to J/\psi\pi^+\pi^-$ decays
1282900 X Observation of Photon Polarization in the b→sγ Transition
1283844 ? Measurement of $\psi(2S)$ polarisation in $pp$ collisions at $\sqrt{s}=7$ TeV
1285485 X Measurement of polarization amplitudes and CP asymmetries in $B^0 \to \phi K^*(892)^0$
1285949 . Study of beauty hadron decays into pairs of charm hadrons
1287928 X Differential branching fractions and isospin asymmetries of $B \to K^{(*)} \mu^+ \mu^-$ decays
1287929 X Angular analysis of charged and neutral $B \to K \mu^+\mu^-$ decays
1288066 X Evidence for the decay $X(3872)\rightarrow\psi(2S)\gamma$
1288067 X Evidence for the decay $B_c^+ \rightarrow J/\psi 3\pi^+ 2\pi^-$
1288881 X Observation of the resonant character of the $Z(4430)^-$ state
1291939 X Measurement of the resonant and CP components in $\overline{B}^0\to J/\psi \pi^+\pi^-$ decays
1294766 X Measurement of the $\Xi_b^-$ and $\Omega_b^-$ baryon lifetimes
1295690 ? Measurement of $CP$ asymmetry in $D^0 \rightarrow K^- K^+$ and $D^0 \rightarrow \pi^- \pi^+$ decays
1295905 X Observation of the $B_s^0 \to J/\psi K_s^0 K^\pm \pi^\mp$ decay
1296831 X Measurement of the CP-violating phase $\phi_s$ in $\overline{B}^0_s\rightarrow J/\psi \pi^+\pi^-$ decays
1297230 . Study of $\Upsilon$ production and cold nuclear matter effects in $p$Pb collisions at $\sqrt{s_{NN}}$=5 TeV
1298273 . Study of the kinematic dependences of $\Lambda_{b}^{0}$ production in pp collisions and a measurement of the $\Lambda_{b}^{0} \to \Lambda_{c}^{+}$ $\pi^{-}$ branching fraction
1298392 X Precision measurement of the mass and lifetime of the $\Xi_b^0$ baryon
1298985 X Observation of the $\Lambda_b^0 \rightarrow J/\psi p \pi^-$ decay
1299995 X Search for CP violation in $D^{\pm}\rightarrow K^0_{\mathrm{S}} K^{\pm}$ and $D^{\pm}_{s}\rightarrow K^0_{\mathrm{S}} \pi^{\pm}$ decays
1300150 X Observation of $Z$ production in proton-lead collisions at LHCb
1301220 . First measurement of the charge asymmetry in beauty-quark pair production
1303108 X Test of lepton universality using $B^{+}\rightarrow K^{+}\ell^{+}\ell^{-}$ decays
1303541 X Effective lifetime measurements in the $B_s^0 → K^+K^− , B^0 → K^+π^−$ and $B_s^0 → π^+K^−$ decays
1305287 X Measurement of the ratio of $B_c^+$ branching fractions to $J/\psi\pi^+$ and $J/\psi\mu^+\nu_\mu$
1305288 X Measurement of CP violation in $B_s^0 \to \phi \phi$ decays
1307246 X Measurement of the $\bar B_s^0$ meson lifetime in $D_s^+\pi^-$ decays
1307247 X Evidence for CP Violation in $B^+\to p \overline p K^+$ Decays
1307250 ? Observation of charmonium pairs produced exclusively in $pp$ collisions
1307415 X Measurement of CP asymmetry in $B^0_s \rightarrow D^{\mp}_s K^{\pm}$ decays
1307418 X Measurement of $CP$ violation and constraints on the CKM angle $\gamma$ in $B^{\pm}\rightarrow D K^{\pm}$ with $D \rightarrow K_S^0 \pi^+ \pi^-$ decays
1308733 X Observation of overlapping spin-1 and spin-3 $\bar{D}^0 K^-$ resonances at mass $2.86 {\rm GeV}/c^2$
1308736 X Observation of $B^0_s \to K^{*\pm}K^\mp$ and evidence for $B^0_s \to K^{*-}\pi^+$ decays
1308737 X Dalitz plot analysis of $B_s^0 \rightarrow \bar{D}^0 K^- \pi^+$ decays
1308738 . Study of $\chi _{{\mathrm {b}}}$ meson production in $\mathrm {p} $ $\mathrm {p} $ collisions at $\sqrt{s}=7$ and $8{\mathrm {\,TeV}} $ and observation of the decay $\chi _{{\mathrm {b}}}\mathrm {(3P)} \rightarrow \Upsilon \mathrm {(3S)} {\gamma } $
1308922 X Measurement of CP violation parameters in $B^0 \to DK^{*0}$ decays
1309439 ? Measurement of the $\bar{B}^0-B^0$ and $\bar{B}^0_s-B^0_s$ production asymmetries in $pp$ collisions at $\sqrt{s}=7$ TeV
1309880 X First observation of a baryonic $B_c^+$ decay
1309881 X Measurement of $C\!P$ asymmetries in the decays $B^0 \rightarrow K^{*0} \mu^+ \mu^-$ and $B^+ \rightarrow K^{+} \mu^+ \mu^-$
1309994 X First observations of the rare decays $B^+\!\rightarrow K^+\pi^+\pi^-\mu^+\mu^-$ and $B^+\rightarrow\phi K^+\mu^+\mu^-$
1309999 . Measurement of the track reconstruction efficiency at LHCb
1310000 X Search for $CP$ violation using $T$-odd correlations in $D^0 \to K^+K^-\pi^+\pi^-$ decays
1310654 X Measurement of the CKM angle $\gamma$ using $B^\pm \to D K^\pm$ with $D \to K^0_{\rm S} \pi^+\pi^-, K^0_{\rm S} K^+ K^-$ decays
1311488 ! Measurement of the forward $W$ boson cross-section in $pp$ collisions at $\sqrt{s} = 7 {\rm \, TeV}$
1311489 X Determination of $\gamma$ and −2$\beta_s$ from charmless two-body decays of beauty mesons
1311994 X Measurements of $CP$ violation in the three-body phase space of charmless $B^{\pm}$ decays
1315113 X Measurement of the $\chi_b(3P)$ mass and of the relative rate of $\chi_{b1}(1P)$ and $\chi_{b2}(1P)$ production
1316329 ? Measurement of the $\eta_c (1S)$ production cross-section in proton-proton collisions via the decay $\eta_c (1S) \rightarrow p \bar{p}$
1317237 X Measurement of the $CP$-violating phase $\phi_s$ in $\bar{B}^{0}_{s}\to D_{s}^{+}D_{s}^{-}$ decays
1319484 X Search for the lepton flavour violating decay τ$^{−}$ → μ$^{−}$ μ$^{+}$ μ$^{−}$
1319485 X Precision Measurement of the Mass and Lifetime of the $\Xi_b^-$ Baryon
1319487 X Measurement of the semileptonic $CP$ asymmetry in $B^0-\overline{B}{}^0$ mixing
1319638 X Precision luminosity measurements at LHCb
1322386 X Search for CP violation in $D^0 \to \pi^− \pi^+ \pi^0$ decays with the energy test
1325983 X Study of $\eta-\eta^{\prime}$ mixing from measurement of $B^0_{(s)} \rightarrow J/\psi \eta^{(\prime)}$~decay rates
1326136 ! Measurement of the Z+b-jet cross-section in pp collisions at $ \sqrt{s} $ = 7 TeV in the forward region
1326411 X Measurement of the CP-violating phase $\beta$ in $B^0\rightarrow J/\psi \pi^+\pi^-$ decays and limits on penguin effects
1327230 X Measurement of $B_c^+$ production in proton-proton collisions at $\sqrt{s}=8$ TeV
1327481 X Precision measurement of $CP$ violation in $B_s^0 \to J/\psi K^+K^-$ decays
1328624 X Observation of two new $\Xi_b^-$ baryon resonances
1329958 X Measurement of the lifetime of the $B_c^+$ meson using the $B_c^+\rightarrow J/\psi\pi^+$ decay mode
1333223 . Measurement of the inelastic pp cross-section at a centre-of-mass energy of $ \sqrt{s} $ = 7 TeV
1333397 . Search for long-lived particles decaying to jet pairs
1335135 . LHCb Detector Performance
1335137 X Study of the rare $B_s^0$ and $B^0$ decays into the $\pi^+\pi^-\mu^+\mu^-$ final state
1335499 X Determination of the branching fractions of B$_{S}^{0} \to$ D$_{S}^{∓}$ K$^{∓}$ and B$^{0}\to$  D$_{S}^{−}$ K$^{+}$
1338587 X Angular analysis of the $B^{0} \to K^{*0} e^{+} e^{−}$ decay in the low-q$^{2}$ region
1341286 X Measurement of indirect $CP$ asymmetries in $D^0\rightarrow K^-K^+$ and $D^0\rightarrow \pi^-\pi^+$ decays using semileptonic $B$ decays
1343514 X Precise measurements of the properties of the $B_1(5721)^{0,+}$ and $B^\ast_2(5747)^{0,+}$ states and observation of $B^{+,0}\pi^{-,+}$ mass structures
1347133 . Measurement of forward $\rm Z\rightarrow e^+e^-$ production at $\sqrt{s}=8$ TeV
1351449 X First observation and amplitude analysis of the $B^{-}\to D^{+}K^{-}\pi^{-}$ decay
1353388 X Measurement of $CP$ asymmetries and polarisation fractions in $B_s^0 \rightarrow K^{*0}\bar{K}{}^{*0}$ decays
1355373 X Measurement of the time-dependent CP asymmetries in $B_s^0\rightarrow J/\psi K_{\rm S}^0$
1355375 X Measurement of $CP$ violation in $B^0 \rightarrow J/\psi K^0_S$ decays
1355376 X Observation of the decay $\overline{B}_s^0 \rightarrow \psi(2S) K^+ \pi^-$
1355377 X Differential branching fraction and angular analysis of $\Lambda^{0}_{b} \rightarrow \Lambda \mu^+\mu^-$ decays
1355552 X Observation of the $B^0_s\to\eta'\eta'$ decay
1356281 X Observation of the $B^0 \to \rho^0 \rho^0$ decay from an amplitude analysis of $B^0 \to (\pi^+\pi^-)(\pi^+\pi^-)$ decays
1357203 X First observation and measurement of the branching fraction for the decay $B^0_s \to D_s^{*\mp} K^{\pm}$
1358215 X Determination of the quark coupling strength $|V_{ub}|$ using baryonic decays
1362487 X A study of $CP$ violation in $B^\mp \rightarrow Dh^\mp$ ($h=K,\pi$) with the modes $D \rightarrow K^\mp \pi^\pm \pi^0$, $D \rightarrow \pi^+\pi^-\pi^0$ and $D \rightarrow K^+K^-\pi^0$
1364718 X Quantum numbers of the $X(3872)$ state and orbital angular momentum in its $\rho^0 J\psi$ decay
1365284 X Identification of beauty and charm quark jets at LHCb
1367298 X Amplitude analysis of $B^0 \rightarrow \bar{D}^0 K^+ \pi^-$ decays
1367305 X Search for the decay $ {B}_s^0\to {\overline{D}}^0{f}_0(980) $
1367306 X Dalitz plot analysis of $B^0 \to \overline{D}^0 \pi^+\pi^-$ decays
1369996 X Search for the $\Lambda^0_b \rightarrow \Lambda \eta^\prime$ and $\Lambda^0_b \rightarrow \Lambda \eta$ decays with the LHCb detector
1370436 ! Study of $W$ boson production in association with beauty and charm
1373300 ! Measurement of the forward $Z$ boson production cross-section in $pp$ collisions at $\sqrt{s}=7$ TeV
1373302 X Study of $B^{-}\to DK^-\pi^+\pi^-$ and $B^-\to D\pi^-\pi^+\pi^-$ decays and determination of the CKM angle $\gamma$
1373746 . Measurement of the exclusive Υ production cross-section in pp collisions at $ \sqrt{s}=7 $ TeV and 8 TeV
1374216 . First observation of top quark production in the forward region
1380182 X Measurement of the ratio of branching fractions $\mathcal{B}(\bar{B}^0 \to D^{*+}\tau^{-}\bar{\nu}_{\tau})/\mathcal{B}(\bar{B}^0 \to D^{*+}\mu^{-}\bar{\nu}_{\mu})$
1380184 X First observation of the decay B$_{s}^{0}$  → K$_{S}^{0}$ K$^{∗}$(892)$^{0}$ at LHCb
1380188 X Angular analysis and differential branching fraction of the decay $B^0_s\to\phi\mu^+\mu^-$
1380452 . Search for long-lived heavy charged particles using a ring imaging Cherenkov technique at LHCb
1382595 X Observation of $J/\psi p$ Resonances Consistent with Pentaquark States in $\Lambda_b^0 \to J/\psi K^- p$ Decays
1382599 X Measurement of the branching fraction ratio $\mathcal{B}(B_c^+ \rightarrow \psi(2S)\pi^+)/\mathcal{B}(B_c^+ \rightarrow J/\psi \pi^+)$
1384027 . Till Moritz Karbach, Scientific Legacy
1385321 X $B$ flavour tagging using charm decays at the LHCb experiment
1386473 X Measurement of the $B_s^0 \to \phi \phi$ branching fraction and search for the decay $B^0 \to \phi \phi$
1388185 X Search for hidden-sector bosons in $B^0 \!\to K^{*0}\mu^+\mu^-$ decays
1389705 X Measurement of the time-integrated $CP$ asymmetry in $D^0 \to K^0_S K^0_S$ decays
1391317 . Study of the production of $\Lambda_b^0$ and $\overline{B}^0$ hadrons in $pp$ collisions and first measurement of the $\Lambda_b^0\rightarrow J/\psi pK^-$ branching fraction
1391324 X Measurement of CP violation parameters and polarisation fractions in $ {\mathrm{B}}_{\mathrm{s}}^0\to \mathrm{J}/\psi {\overline{\mathrm{K}}}^{\ast 0} $ decays
1391325 X First measurement of the differential branching fraction and $C\!P$ asymmetry of the $B^\pm\to\pi^\pm\mu^+\mu^-$ decay
1391511 . Measurement of forward $J/\psi$ production cross-sections in $pp$ collisions at $\sqrt{s}=13$ TeV
1392456 . Forward production of $\Upsilon$ mesons in $pp$ collisions at $\sqrt{s}=7$ and 8TeV
1394391 X Studies of the resonance structure in $D^0\to K^0_S K^{\pm}\pi^{\mp}$ decays
1394859 ! Measurement of the forward-backward asymmetry in $Z/\gamma^{\ast} \rightarrow \mu^{+}\mu^{-}$ decays and determination of the effective weak mixing angle
1396327 X Model-independent measurement of mixing parameters in D$^{0}$ → K$_{S}^{0}$ π$^{+}$π$^{−}$ decays
1396331 . Measurements of prompt charm production cross-sections in $pp$ collisions at $ \sqrt{s}=13 $ TeV
1396563 X Model-independent confirmation of the $Z(4430)^-$ state
1397639 X Evidence for the strangeness-changing weak decay $\Xi_b^-\to\Lambda_b^0\pi^-$
1398352 X Search for the rare decays $B^{0}\to J/\psi \gamma$ and $B^{0}_{s} \to J/\psi \gamma$
1399056 ! Production of associated Y and open charm hadrons in pp collisions at $ \sqrt{s}=7 $ and 8 TeV via double parton scattering
1401225 X First observation of the decay $D^{0}\rightarrow K^{-}\pi^{+}\mu^{+}\mu^{-}$ in the $\rho^{0}$-$\omega$ region of the dimuon mass spectrum
1406555 . Measurement of forward W and Z boson production in $pp$ collisions at $ \sqrt{s}=8 $ TeV
1407482 X Search for the lepton-flavour violating decay $D^0 \to e^\pm\mu^\mp$
1407486 . Measurements of long-range near-side angular correlations in $\sqrt{s_{\text{NN}}}=5$TeV proton-lead collisions in the forward region
1408740 X First observation of the rare $B^{+}\to D^{+} K^{+} \pi^{-}$ decay
1409497 X Angular analysis of the $B^{0} \to K^{*0} \mu^{+} \mu^{-}$ decay using 3 fb$^{-1}$ of integrated luminosity
1414195 X Study of D$_{sJ}^{(*) +}$ mesons decaying to D$^{∗ +}$ K$_S^0$ and D$^{*0}$ K$^{+}$ final states
1416176 X Observation of the $B_s^0 \rightarrow J/\psi \phi \phi$ decay
1418182 . Study of $\psi(2S)$ production and cold nuclear matter effects in pPb collisions at $\sqrt{s_{NN}}=5~\mathrm{TeV}$
1420555 X Measurement of the difference of time-integrated CP asymmetries in $D^0 \rightarrow K^{-} K^{+} $ and $D^0 \rightarrow \pi^{-} \pi^{+} $ decays
1420702 X Constraints on the unitarity triangle angle $\gamma$ from Dalitz plot analysis of $B^0 \to D K^+ \pi^-$ decays
1423070 X First observation of $D^0-\bar D^0$ oscillations in $D^0\to K^+\pi^-\pi^+\pi^-$ decays and measurement of the associated coherence parameters
1423074 X A new algorithm for identifying the flavour of $B_s^0$ mesons at LHCb
1423299 X Measurement of the $B_{s}^{0} \rightarrow D_{s}^{(*)+}D_{s}^{(*)-}$ branching fractions
1425547 X Observations of $\Lambda_b^0 \to \Lambda K^+\pi^-$ and $\Lambda_b^0 \to \Lambda K^+K^-$ decays and searches for other $\Lambda_b^0$ and $\Xi_b^0$ decays to $\Lambda h^+h^{\prime -}$ final states
1426694 X Observation of $B^0_s\to\bar{D}^0 K^0_S$ and evidence for $B^0_s\to\bar{D}^{*0} K^0_S$ decays
1426827 X Observation of the $\Lambda_b^0\to\Lambda\phi$ decay
1427724 X Search for violations of Lorentz invariance and $ CPT$ symmetry in $ B^0_{(s)}$ mixing
1432696 X Observation of $ \Lambda_b^0 \to \psi(2S)pK^-$ and $ \Lambda_b^0 \to J/\psi \pi^+ \pi^- pK^-$ decays and a measurement of the $\Lambda_b^0$ baryon mass
1432698 X Search for $B_c^+$ decays to the $p\bar p\pi^+$ final state
1436488 X Measurement of $C\!P$ observables in $B^\pm \rightarrow D K^\pm$ and $B^\pm \rightarrow D \pi^\pm$ with two- and four-body $D$ decays
1444339 X Measurement of the mass and lifetime of the $\Omega_b^-$ baryon
1444343 X Model-independent measurement of the CKM angle $\gamma$ using $B^0 \to D K^{\ast 0}$ decays with $D \to K_{S}^{0} \pi^{+} \pi^{-}$ and $K_{S}^{0} K^{+} K^{-}$
1445118 X A precise measurement of the $B^0$ meson oscillation frequency
1446752 X Measurement of the properties of the $\Xi_b^{*0}$ baryon
1449086 X Model-independent evidence for $J/\psi p$ contributions to $\Lambda_b^0\to J/\psi p K^-$ decays
1454404 . Measurement of forward $W$ and $Z$ boson production in association with jets in proton-proton collisions at $\sqrt{s}=8$ TeV
1455783 X Measurement of the CKM angle $\gamma$ using $B^0 \rightarrow D K^{*0}$ with $D \rightarrow K^0_S \pi^+ \pi^-$ decays
1466441 X Measurement of the $CP$ asymmetry in $B_s^0-\overline{B}{}_s^0$ mixing
1469448 X Measurements of the S-wave fraction in $B^{0}\rightarrow K^{+}\pi^{-}\mu^{+}\mu^{-}$ decays and the $B^{0}\rightarrow K^{\ast}(892)^{0}\mu^{+}\mu^{-}$ differential branching fraction
1471725 X Evidence for exotic hadron contributions to $\Lambda_b^0 \to J/\psi p \pi^-$ decays
1472310 X Observation of $J/\psi\phi$ structures consistent with exotic states from amplitude analysis of $B^+\to J/\psi \phi K^+$ decays
1472311 X Amplitude analysis of $B^+\to J/\psi \phi K^+$ decays
1477400 X Study of $B_c^+$ decays to the $K^+K^-\pi^+$ final state and evidence for the decay $B_c^+\to\chi_{c0}\pi^+$
1477402 X Measurement of the $B_{s}^{0} \rightarrow J/\psi \eta$ lifetime
1477405 X Observation of $\eta_{c}(2S) \to p \bar p$ and search for $X(3872) \to p \bar p$ decays
1477581 . Measurement of the forward Z boson production cross-section in pp collisions at $\sqrt{s} = 13$ TeV
1477804 X Measurement of the ratio of branching fractions $\mathcal{B}(B_{c}^{+} \to J/\psi K^{+})/\mathcal{B}(B_{c}^{+} \to J/\psi\pi^{+})$
1478792 X Search for Structure in the $B_s^0\pi^\pm$ Invariant Mass Spectrum
1479164 X Amplitude analysis of $B^{-} \to D^{+} \pi^{-} \pi^{-}$ decays
1479452 X Search for the suppressed decays $B^{+}\rightarrow K^{+}K^{+}\pi^{-}$ and $B^{+}\rightarrow \pi^{+}\pi^{+}K^{-}$
1479453 . Measurement of forward $W\to e\nu$ production in $pp$ collisions at $\sqrt{s}=8\,$TeV
1481810 X First study of the CP -violating phase and decay-width difference in $B_s^0\to\psi(2S)\phi$ decays
1482943 X Measurement of $CP$ violation in $B^0 \!\rightarrow D^+ D^-$ decays
1485571 ? First experimental study of photon polarization in radiative $B^{0}_{s}$ decays
1486230 X Search for Higgs-like bosons decaying into long-lived exotic particles
1486676 X Differential branching fraction and angular moments analysis of the decay $B^0 \to K^+ \pi^- \mu^+ \mu^-$ in the $K^*_{0,2}(1430)^0$ region
1487273 X Measurement of matter-antimatter differences in beauty baryon decays
1489630 X Observation of $B^+\rightarrow J/\psi 3\pi^+ 2\pi^-$ and $B^+\rightarrow \psi(2S) \pi^+\pi^+\pi^-$ decays
1490663 . Measurements of prompt charm production cross-sections in pp collisions at $ \sqrt{s}=5 $ TeV
1491381 X Search for the $C\!P$-violating strong decays $\eta \to \pi^+\pi^-$ and $\eta^\prime(958) \to \pi^+\pi^-$
1492324 X Observation of the decay $B^0_s \to \phi\pi^+\pi^-$ and evidence for $B^0 \to \phi\pi^+\pi^-$
1492731 X New algorithms for identifying the flavour of ${\mathrm {B}} ^0$ mesons using pions and protons
1494582 . Measurement of forward $t\overline{t}$, $W+b\overline{b}$ and $W+c\overline{c}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV
1494585 X Observation of the annihilation decay mode $B^{0}\to K^{+}K^{-}$
1495235 X Measurement of $CP$ asymmetry in $D^0\rightarrow K^-K^+$ decays
1496635 X Measurement of the CKM angle $\gamma$ from a combination of LHCb results
1499047 X Measurements of charm mixing and $C\!P$ violation using $D^0 \to K^\pm \pi^\mp$ decays
1499874 X Search for decays of neutral beauty mesons into four muons
1499877 X Evidence for the two-body charmless baryonic decay $ {B}^{+}\to p\overline{\varLambda} $
1501678 X Search for massive long-lived particles decaying semileptonically in the LHCb detector
1502093 X Observation of the decay $\Xi_b^- \to p K^-K^-$
1502914 X Search for $CP$ violation in the phase space of $D^0\rightarrow\pi^+\pi^-\pi^+\pi^-$ decays
1504058 ! Measurement of the $b$-quark production cross-section in 7 and 13 TeV $pp$ collisions
1504948 X Measurement of the ratio of branching fractions and difference in $CP$ asymmetries of the decays $B^+\to J/\psi\pi^+$ and $B^+\to J/\psi K^+$
1505172 X Measurement of the phase difference between short- and long-distance amplitudes in the $B^{+}\to K^{+}\mu^{+}\mu^{-}$ decay
1505591 X Observation of $B_{c}^{+} \to J/\psi D^{(*)} K^{(*)}$ decays
1505592 . Measurement of the J/$\psi$ pair production cross-section in pp collisions at $ \sqrt{s}=13 $ TeV
1505730 X Search for long-lived scalar particles in $B^+ \to K^+ \chi (\mu^+\mu^-)$ decays
1506403 X Search for the $B^{0}_{s} \to \eta^{\prime}\phi$ decay
1508166 X Observation of $B_{c}^{+} \rightarrow D^{0} K^{+}$ decays
1508167 X Measurement of $CP$ asymmetries in $D^{\pm}\rightarrow \eta^{\prime} \pi^{\pm}$ and $D_s^{\pm}\rightarrow \eta^{\prime} \pi^{\pm}$ decays
1509507 . Study of J/ψ Production in Jets
1509918 X Observation of the $\varXi^{-}_{b}\to J/\psi\varLambda K^{-}$ decay
1509922 X Measurement of the $B^{\pm}$ production asymmetry and the $CP$ asymmetry in $B^{\pm} \to J/\psi K^{\pm}$ decays
1511124 X Study of the $D^0 p$ amplitude in $\Lambda_b^0\to D^0 p \pi^-$ decays
1511285 X Observation of the suppressed decay $\Lambda^{0}_{b}\rightarrow p\pi^{-}\mu^{+}\mu^{-}$
1514549 X Measurement of the $C\!P$ violation parameter $A_\Gamma$ in $D^0 \to K^+K^-$ and $D^0 \to \pi^+\pi^-$ decays
1515201 X Observation of the decay $B_{s}^{0} \to \eta_{c} \phi$ and evidence for $B_{s}^{0} \to \eta_{c} \pi^{+} \pi^{-} $
1515507 X Observation of the decay $\Lambda^0_b \to p K^- \mu^+ \mu^-$ and a search for $C\!P$ violation
1516410 X Search for the decays $B_s^0\to\tau^+\tau^-$ and $B^0\to\tau^+\tau^-$
1517483 X Observation of five new narrow $\Omega_c^0$ states decaying to $\Xi_c^+ K^-$
1517782 X Measurement of the $B^0_s\to\mu^+\mu^-$ branching fraction and effective lifetime and search for $B^0\to\mu^+\mu^-$ decays
1519165 . Measurement of $B^0$, $B^0_s$, $B^+$ and $\Lambda^0_b$ production asymmetries in 7 and 8 TeV proton-proton collisions
1594907 X Observation of the $B^+ \to D^{*-}K^+\pi^+$ decay
1596892 X Observation of the decays $\Lambda_b^0 \to \chi_{c1} p K^-$ and $\Lambda_b^0 \to \chi_{c2} p K^-$
1596893 . First observation of a baryonic $B_s^0$ decay
1596902 X Resonances and $CP$ violation in $B_s^0$ and $\overline{B}_s^0 \to J/\psi K^+K^-$ decays in the mass region above the $\phi(1020)$
1597124 X Observation of charmless baryonic decays $B^0_{(s)} \to p \bar{p} h^+ h^{\prime-}$
1598757 X Measurement of $B^{0}_{s}$ and $D^{-}_{s}$ meson lifetimes
1599846 X Test of lepton universality with $B^{0} \rightarrow K^{*0}\ell^{+}\ell^{-}$ decays
1600787 . Updated search for long-lived particles decaying to jet pairs
1602477 X Improved limit on the branching fraction of the rare decay ${{K} ^0_{\mathrm { \scriptscriptstyle S}}} \rightarrow \mu ^+\mu ^-$
1606204 ? Study of charmonium production in ${b}$-hadron decays and first evidence for the decay ${{{B}} ^0_{{s}}} \!\rightarrow \phi \phi \phi $
1606329 ? Prompt and nonprompt J/$\psi$ production and nuclear modification in $p$Pb collisions at $\sqrt{s_{\text{NN}}}= 8.16$ TeV
1608879 X Observation of the doubly charmed baryon $\Xi_{cc}^{++}$
1608881 . Updated branching fraction measurements of $B^0_{(s)} \to K_{\mathrm{\scriptscriptstyle S}}^0 h^+ h^{\prime -}$ decays
1609255 X Study of prompt D$^{0}$ meson production in $p$Pb collisions at $ \sqrt{s_{\mathrm{NN}}}=5 $ TeV
1611681 X Observation of $D^0$ meson decays to $\pi^+\pi^-\mu^+\mu^-$ and $K^+K^-\mu^+\mu^-$ final states
1614076 . Framework TDR for the LHCb Upgrade
1617762 X Search for Baryon-Number Violating ${\mathrm{\Xi}}_{b}^{0}$ Oscillations
1617765 ! Study of $b\bar{b}$ correlations in high energy proton-proton collisions
1618003 X Measurement of $CP$ observables in $B^\pm \to D^{(*)} K^\pm$ and $B^\pm \to D^{(*)} \pi^\pm$ decays
1620479 X Measurement of the ratio of the $B^0 \to D^{*-} \tau^+ \nu_{\tau}$ and $B^0 \to D^{*-} \mu^+ \nu_{\mu}$ branching fractions using three-prong $\tau$-lepton decays
1621592 X First Observation of the Rare Purely Baryonic Decay $B^0\to p\bar p$
1621596 . Measurement of the $\Upsilon$ polarizations in $pp$ collisions at $\sqrt{s}=7$ and 8 TeV
1621810 X Bose-Einstein correlations of same-sign charged pions in the forward region in $pp$ collisions at $\sqrt{s}$ = 7 TeV
1621811 X Measurement of the shape of the $\Lambda_b^0\to\Lambda_c^+ \mu^- \overline{\nu}_{\mu}$ differential decay rate
1622743 X First observation of forward $Z \rightarrow b \bar{b}$ production in $pp$ collisions at $\sqrt{s}=8$ TeV
1623025 X Measurement of $CP$ violation in $B^0\rightarrow J/\psi K^0_\mathrm{S}$ and $B^0\rightarrow\psi(2S) K^0_\mathrm{S}$ decays
1623210 X $\chi_{c1}$ and $\chi_{c2}$ Resonance Parameters with the Decays $\chi_{c1,c2}\to J/\psi\mu^+\mu^-$
1624171 X Measurement of $CP$ observables in $B^{\pm} \rightarrow D K^{*\pm}$ decays using two- and four-body $D$ final states
1629161 . Search for Dark Photons Produced in 13 TeV $pp$ Collisions
1629971 X Search for the lepton-flavour violating decays B$_{(s)}^{0} \to e^{\pm}\mu^{\mp}$
1630633 . Measurement of the $B^{\pm}$ production cross-section in pp collisions at $\sqrt{s} =$ 7 and 13 TeV
1634432 X Measurements of the branching fractions of $\Lambda_{c}^{+} \rightarrow p \pi^{-} \pi^{+}$, $\Lambda_{c}^{+} \rightarrow p K^{-} K^{+}$, and $\Lambda_{c}^{+} \rightarrow p \pi^{-} K^{+}$
1634841 . Test of Lepton Flavor Universality by the measurement of the $B^0 \to D^{*-} \tau^+ \nu_{\tau}$ branching fraction using three-prong $\tau$ decays
1636196 X Measurement of branching fractions of charmless four-body $\Lambda_b^0$ and $\Xi_b^0$ decays
1636198 X Measurement of the ratio of branching fractions $\mathcal{B}(B_c^+\,\to\,J/\psi\tau^+\nu_\tau)$/$\mathcal{B}(B_c^+\,\to\,J/\psi\mu^+\nu_\mu)$
1636199 X First observation of $B^{+} \to D_s^{+}K^{+}K^{-}$ decays and a search for $B^{+} \to D_s^{+}\phi$ decays
1642234 X Updated determination of $D^0$-$\overline{D}{}^0$ mixing and CP violation parameters with $D^0\to K^+\pi^-$ decays
1642726 X Search for excited $B_{c}^{+}$ states
1643022 X Search for $B_c^+$ decays to two charm mesons
1644103 X A measurement of the $CP$ asymmetry difference in $\varLambda_{c}^{+} \to pK^{-}K^{+}$ and $p\pi^{-}\pi^{+}$ decays
1644370 X Measurement of $CP$ asymmetry in $B_s^0 \to D_s^{\mp} K^{\pm}$ decays
1644610 . Search for the rare decay $\Lambda_{c}^{+} \to p\mu^+\mu^-$
1644616 X Search for weakly decaying $b$-flavored pentaquarks
1644790 X Evidence for the rare decay $\Sigma^+ \to p \mu^+ \mu^-$
1644791 X Studies of the resonance structure in $D^{0} \rightarrow K^\mp \pi ^\pm \pi ^\pm \pi ^\mp $ decays
1644897 X First measurement of the $CP$-violating phase $\phi_s^{d\overline{d}}$ in $B_s^0\to(K^+\pi^-)(K^-\pi^+)$ decays
1644906 . Amplitude analysis of the decay $\overline{B}^0 \to K_{S}^0 \pi^+ \pi^-$ and first observation of the CP asymmetry in $\overline{B}^0 \to K^{*}(892)^- \pi^+$
1662483 ! Measurement of forward top pair production in the dilepton channel in $pp$ collisions at $\sqrt{s}=13$ TeV
1665223 ! Measurement of the inelastic $pp$ cross-section at a centre-of-mass energy of 13 TeV
1665225 X Measurement of the $CP$ asymmetry in $B^-\to D_s^-D^0$ and $B^-\to D^-D^0$ decays
1668916 X Evidence for the decay $ {B}_S^0\to {\overline{K}}^{\ast 0}{\mu}^{+}{\mu}^{-} $
1670013 . Measurement of $\Upsilon$ production in $pp$ collisions at $\sqrt{s}$= 13 TeV
1670022 X Observation of the decay $\Lambda_b^0 \to \Lambda_c^+ p \overline{p} \pi^-$
1672368 X Measurement of $CP$ violation in $B^{0}\rightarrow D^{\mp}\pi^{\pm}$ decays
1672471 . Search for CP violation using triple product asymmetries in $\Lambda^{0}_{b}\to pK^{-}\pi^{+}\pi^{-}$, $\Lambda^{0}_{b}\to pK^{-}K^{+}K^{-}$ and $\Xi^{0}_{b}\to pK^{-}K^{-}\pi^{+}$ decays
1673686 . Measurement of $C\!P$ asymmetries in two-body $B_{(s)}^{0}$-meson decays to charged pions and kaons
1674704 . Search for a dimuon resonance in the $\Upsilon$ mass region
1674835 X Observation of a new $\Xi_b^-$ resonance
1674916 X Measurement of $D_s^{\pm}$ production asymmetry in $pp$ collisions at $\sqrt{s} =7$ and 8 TeV
1676225 X Measurement of the CKM angle $\gamma$ using $B^\pm\to DK^\pm$ with $D\to K_\text{S}^0\pi^+\pi^-$, $K_\text{S}^0K^+K^-$ decays
1676395 X Measurement of the time-integrated $CP$ asymmetry in $D^0 \rightarrow K^0_S K^0_S$ decays
1676811 X Measurement of the Lifetime of the Doubly Charmed Baryon $\Xi_{cc}^{++}$
1677283 . Central exclusive production of $J/\psi$ and $\psi(2S)$ mesons in $pp$ collisions at $\sqrt{s}=13~$TeV
1677775 . Measurement of $Z\rightarrow\tau^+\tau^-$ production in proton-proton collisions at $\sqrt{s} = 8$ TeV
1679066 . Observation of the decay $\Lambda^0_b\rightarrow\psi(2S)p\pi^-$
1679857 . Search for beautiful tetraquarks in the $\Upsilon(1S)\mu^+\mu^-$ invariant-mass spectrum
1680225 . Observation of the decay $ {\overline{B}}_s^0\to {\chi}_{c2}{K}^{+}{K}^{-} $ in the ϕ mass region
1680229 . Measurement of Angular and CP Asymmetries in $D^0\to\pi^+\pi^-\mu^+\mu^-$ and $D^0\to K^+K^-\mu^+\mu^-$ decays
-1681011 . First observation of the doubly charmed baryon decay $\Xi_{cc}^{++}\rightarrow \Xi_{c}^{+}\pi^{+}$
+1681011 . First Observation of the Doubly Charmed Baryon Decay $\Xi_{cc}^{++}\rightarrow \Xi_{c}^{+}\pi^{+}$
1681144 . Measurement of the $\Omega_c^0$ baryon lifetime
1681145 . Observation of the decay $B_s^0 \to \overline{D}^0 K^+ K^-$
1681146 . Observation of $B_s^0 \to \overline{D}^{*0} \phi$ and search for $B^0 \to \overline{D}^0 \phi$ decays
1682900 . Search for $C\!P$ violation in $\Lambda^0_b \to p K^-$ and $\Lambda^0_b \to p \pi^-$ decays
1684260 . Measurement of the relative $B^{-} \!\rightarrow D^{0} / D^{*0} / D^{**0} \mu^{-} \overline{\nu}_\mu$ branching fractions using $B^{-}$ mesons from $\overline{B}{}_{s2}^{*0}$ decays
1684712 . Angular moments of the decay $\Lambda_b^0 \rightarrow \Lambda \mu^{+} \mu^{-}$ at low hadronic recoil
1688924 . Measurement of antiproton production in ${\rm p He}$ collisions at $\sqrt{s_{NN}}=110$ GeV
1690146 . Search for lepton-flavour-violating decays of Higgs-like bosons
1691586 . Physics case for an LHCb Upgrade II - Opportunities in flavour physics, and beyond, in the HL-LHC era
1692810 . Prompt $\Lambda^+_c$ production in $p\mathrm{Pb}$ collisions at $\sqrt{s_{NN}} = 5.02$ TeV
1694807 . Observation of two resonances in the $\Lambda_b^0 \pi^\pm$ systems and precise measurement of $\Sigma_b^\pm$ and $\Sigma_b^{*\pm}$ properties
1694990 . Evidence for an $\eta_c(1S) \pi^-$ resonance in $B^0 \to \eta_c(1S) K^+\pi^-$ decays
+1697372 . Measurement of the branching fractions of the decays $D^+\rightarrow K^-K ^+K^+$, $D^+\rightarrow \pi^-\pi^+K^+$ and $D^+_s\rightarrow \pi^-K^+K^+$
+1698962 . Measurement of the charm-mixing parameter $y_{CP}$
+1699106 . Study of $\Upsilon$ production in $p$Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV
+1699199 . First measurement of charm production in fixed-target configuration at the LHC
+1704426 . Search for $CP$ violation through an amplitude analysis of $D^0 \rightarrow K^+ K^- \pi^+ \pi^-$ decays
diff --git a/doc/rivet-coverage-other.rank b/doc/rivet-coverage-other.rank
--- a/doc/rivet-coverage-other.rank
+++ b/doc/rivet-coverage-other.rank
@@ -1,581 +1,588 @@
841618 . Measurement of the branching fractions and the invariant mass distributions for $\tau^- \to h^-h^+h^-\nu_{\tau}$ decays
841764 . Measurement of Leading Neutron Production in Deep-Inelastic Scattering at HERA
842635 . Search for Charged Lepton Flavor Violation in Narrow Upsilon Decays
842959 . $\Upsilon$ cross section in $p+p$ collisions at $\sqrt(s) = 200$ GeV
843256 . Search for CP violation in the decays $D^+_{(s)} \to K_S^0\pi^+$ and $D^+_{(s)} \to K_S^0K^+$
843520 . Search for $B^0 \to K^{*0} \overline{K}{}^{*0}$, $B^0 \to K^{*0} K^{*0}$ and $B^0 \to K^+\pi^- K^{\mp}\pi^{\pm}$ Decays
843985 . Charged and strange hadron elliptic flow in Cu+Cu collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV
844129 . Scaled momentum spectra in deep inelastic scattering at HERA
844288 . Observation of the $\chi_{c2}(2p)$ Meson in the Reaction $\gamma \gamma \to D \bar{D}$ at {BaBar}
844299 . Inelastic Production of J/psi Mesons in Photoproduction and Deep Inelastic Scattering at HERA
844983 . Longitudinal scaling property of the charge balance function in Au + Au collisions at 200 GeV
845914 . Measurement of the gamma gamma* --> eta_c transition form factor
846307 . Test of lepton universality in Upsilon(1S) decays at BaBar
846499 . Limits on tau Lepton-Flavor Violating Decays in three charged leptons
847330 . Observation of the Rare Decay B0 ---> K0(s)K+-pi-+
847922 . Search for Lepton Flavor Violating tau- Decays into \ell-K0s and \ell-K0sK0s
848409 . Observation of an Antimatter Hypernucleus
848650 . Search for leptonic decays of $D^0$ mesons
848883 . Inclusive-jet cross sections in NC DIS at HERA and a comparison of the kT, anti-kT and SIScone jet algorithms
849068 . Measurement of the Branching Fraction for $D^+_s\to\tau^{+}\nu_{\tau}$ and Extraction of the Decay Constant f_{D_s}
849155 . Search for CP violation using $T$-odd correlations in $D^0 \to K^+ K^- \pi^+ \pi^-$ decays
849165 . Evidence for direct CP violation in the decay B->D(*)K, D->KsPi+Pi- and measurement of the CKM phase phi3
850301 . Observation of $B_s^0 -> D_s^{*-} \pi^+, B_s^0 - >D_s^{(*)-} \ rho^+$ Decays and Measurement of $B_s^0 -> D_s^{*-} \rho^+$ Polarization
850435 . Measurement of Y(5S) decays to B^0 and B^+ mesons
850492 . Observation of the $\Upsilon{1^3D_J}$ Bottomonium State through Decays to $\pi^+\pi^-\Upsilon{1S}$
850804 . B-meson decays to $\eta^{\prime} \rho$, $\eta^{\prime} f_{0}$, and $\eta^{\prime} K^*$
850950 . Pion femtoscopy in $p^+ p$ collisions at $\sqrt{s}=200$ GeV
851937 . Azimuthal di-hadron correlations in d+Au and Au+Au collisions at $\sqrt{s_{NN}}=200$ GeV from STAR
853279 . Measurement of D0-antiD0 mixing parameters using D0 ---> K(S)0 pi+ pi- and D0 ---> K(S)0 K+ K- decays
853304 . Higher Moments of Net-proton Multiplicity Distributions at RHIC
853759 . Search for B+ ---> D+K0 and B+ ---> D+K*0 decays
854415 . Evidence for direct CP violation in the measurement of the Cabibbo-Kobayashi-Maskawa angle gamma with B-+ ---> D(*) K(*)-+ decays
854539 . Search for a Low Mass Particle Decaying into mu^+ mu^- in B^0 -> K^{*0} X and B^0 -> rho^0 X at Belle
855083 . Observation of the Rare Decay B^+ -> K^+ \pi^0 \pi^0
855232 . Measurement of beauty production in DIS and $F_2^{b\bar{b}}$ extraction at ZEUS
855306 . Study of $B \to \pi \ell \nu$ and $B \to \rho \ell \nu$ Decays and Determination of $|V_{ub}|$
855746 . Balance Functions from Au$+$Au, $d+$Au, and $p+p$ Collisions at $\sqrt{s_{NN}}$ = 200 GeV
855748 . Observation of B+ -> Dbar*0 tau+ nu_tau and Evidence for B+ -> Dbar^0 tau+ nu_tau at Belle
856113 . Study of $B \to X\gamma$ Decays and Determination of $|V_{td}/V_{ts}|$
856587 . Evidence for the decay X(3872) ---> J/ psi omega
857109 . Diffractive Dijet Photoproduction in ep Collisions at HERA
857694 . $K^{*0}$ production in Cu+Cu and Au+Au collisions at $\sqrt{s_NN} = 62.4$ GeV and 200 GeV
857959 . Correlated leading baryon-antibaryon production in $e^+e^- -> c\bar{c} -> \Lambda_c^+ \^-Lambda_c^- X$
859147 . Search for b ---> u transitions in $B^- -> DK^- and D^*K^-$ Decays
859160 . Evidence for $B^- -> \tau^- \bar{\nu}$ with a Semileptonic Tagging Method
859723 . Search for $B_{s}^{0} -> hh$ Decays at the $\Upsilon(5S)$ Resonance
860478 . Measurement of CP observables in $B^{+-} -> D_{CP} K^{+-}$ decays and constraints on the CKM angle $\gamma$
860571 . Measurement of the Bottom contribution to non-photonic electron production in $p+p$ collisions at $\sqrt{s} $=200 GeV
860780 . Observation of the decay $\bar{B}^0 -> \Lambda_c^+ \bar{p} pi^0$
860842 . Measurement of $D^+$ and $\Lambda_{c}^{+}$ production in deep inelastic scattering at HERA
861351 . An Experimental Exploration of the QCD Phase Diagram: The Search for the Critical Point and the Onset of De-confinement
861716 . Search for $B^+$ meson decay to $a_1^+(1260)K^{*0}(892)$
862141 . Search for f_J(2220) in radiative J/psi decays
862241 . Measurement of CP violating asymmetries in $B^0 -> K^+K^- K^0_S$ decays with a time-dependent Dalitz approach
862260 . Measurement of eta eta production in two-photon collisions
862603 . Dalitz-plot Analysis of $B^0 -> \bar{D}^0 \pi^+ \pi^-$
863104 . Search for Production of Invisible Final States in Single-Photon Decays of $\Upsilon(1S)$
863111 . Measurements of Branching Fractions for $B^0 -> D_s^+\pi^-$ and $\bar{B}^0 -> D_s^+K^-$
864027 . Exclusive Production of $D^+_s D^-_s$, $D^{*+}_s D^-_s$, and $D^{*+}_s D^{*-}_s$ via $e^+ e^-$ Annihilation with Initial-State-Radiation
864107 . Evidence for $B^+ -> \tau^+ \nu_{\tau}$ decays using hadronic B tags
865016 . Search for charmonium and charmonium-like states in $\Upsilon(1S)$ radiative decays
865032 . Measurement of Charm and Beauty Jets in Deep Inelastic Scattering at HERA
865394 . Search for $CP$ violating charge asymmetry in $B^{+-} -> J/\psi K^{+-} decays
865572 . Scaling properties at freeze-out in relativistic heavy ion collisions
865819 . Measurement of high-$Q^2$ charged current deep inelastic scattering cross sections with a longitudinally polarised positron beam at HERA
866025 . Measurement of the Absolute Branching Fractions for $D^-_s\!\rightarrow\!\ell^-\bar{\nu}_{\ell}$ and Extraction of the Decay Constant $f_{D_s}$
866608 . Search for CP violating charge asymmetry in $B^+ -> J/psi K^{+-} decays
866968 . Measurement of the parity-violating longitudinal single-spin asymmetry for $W^{\pm}$ boson production in polarized proton-proton collisions at $\sqrt{s} = 500-GeV$
867611 . Observation of new resonances decaying to $D\pi$ and $D^*\pi$ in inclusive $e^+e^-$ collisions near $\sqrt{s}=$10.58 GeV
868017 . Search for the Rare Decay $B \to K \nu \bar{\nu}$
871475 . Study of the $K^+ \pi^+ \pi^-$ Final State in $B^+ \to J/\psi K^+ \pi^+ \pi^-$ and $B^+ \to \psi-prime K^+ \pi^+ \pi^-$
871561 . Strange and Multi-strange Particle Production in Au+Au Collisions at $\sqrt{s_{NN}}$ = 62.4 GeV
871959 . Measurement of the $B^0 \to \pi^\ell \ell^+ \nu$ and $B^+ \to \eta^{(')} \ell^+ \nu$ Branching Fractions, the $B^0 \to \pi^- \ell^+ \nu$ and $B^+ \to \eta \ell^+ \nu$ Form-Factor Shapes, and Determination of $|V_{ub}|$
872067 . Measurements of Dihadron Correlations Relative to the Event Plane in Au+Au Collisions at $\sqrt{s_{NN}}=200$ GeV
872494 . Search for the Decay $B^{0} \to \gamma \gamma$
874639 . Measurement of the form factors of the decay B0 -> D*- ell+ nu and determination of the CKM matrix element |Vcb|
875006 . Inclusive dijet cross sections in neutral current deep inelastic scattering at HERA
875348 . Belle II Technical Design Report
875888 . Measurement of the energy dependence of the total photon-proton cross section at HERA
877816 . Measurement of the B ---> D-bar(*)D(*)K branching fractions
877820 . Studies of tau- ---> eta K-nu and tau- ---> eta pi- nu(tau) at BaBar and a search for a second-class current
878120 . Dalitz plot analysis of $D_s^+ \to K^+ K^- \pi^+$
878228 . Measurement of $e^+e^-\to D_s^{(*)+} D_s^{(*)-}$ cross sections near threshold using initial-state radiation
878656 . Search for Squarks in R-parity Violating Supersymmetry in ep Collisions at HERA
878990 . Measurement of the decay $B^0\to\pi^-\ell^+\nu$ and determination of $|V_{ub}|$
879997 . Analysis of the $D^+ \to K^- \pi^+ e^+ \nu_e$ decay channel
881851 . Observation of the Decay $B^{-} \rightarrow D_{s}^{(*)+} K^{-} \ell^{-} \bar{\nu}_{\ell}$
881876 . Measurements of branching fractions, polarizations, and direct CP-violation asymmetries in B+ -> rho0 K*+ and B+ -> f0(980)K*+ decays
882140 . Measurement of partial branching fractions of inclusive charmless B meson decays to K+, K0, and pi+
882470 . Measurement of the Inclusive e{\pm}p Scattering Cross Section at High Inelasticity y and of the Structure Function $F_L$
883084 . Search for Lepton-Flavor-Violating tau Decays into a Lepton and a Vector Meson
883260 . Search for CP violation in $\tau \to K^0_S \pi \nu_\tau$ decays at Belle
883525 . Measurement of the $\gamma \gamma^* --> \eta$ and $\gamma \gamma* --> \eta'$ transition form factors
883710 . Study of tau-pair production at HERA
884579 . Search for CP Violation in the Decays $D^0\rightarrow K^0_S P^0$
884735 . Measurement of beauty production in deep inelastic scattering at HERA using decays into electrons
884880 . Searches for the baryon- and lepton-number violating decays $B^0\rightarrow\Lambda_c^+\ell^-$, $B^-\rightarrow\Lambda\ell^-$, and $B^-\rightarrow\bar{\Lambda}\ell^-$
886797 . Study of the decays $B -> D_{s1}(2536)^+ \bar{D}^{(*)}$
886818 . Measurements of time-dependent CP asymmetries in $B \to D^{*\mp} \pi^{\pm}$ decays using a partial reconstruction technique
889524 . Observation of $B_s^0\to J/\psi f_0(980)$ and Evidence for $B_s^0\to J/\psi f_0(1370)$
889553 . Studies of di-jet survival and surface emission bias in Au+Au collisions via angular correlations with respect to back-to-back leading hadrons
889563 . High $p_{T}$ non-photonic electron production in $p+p$ collisions at $\sqrt{s} = 200$ GeV
890325 . Evidence for the $h_b(1P)$ meson in the decay $\Upsilon(3S) \to \pi^0 h_b(1P)$
892421 . Measurement of the mass and width of the D(s1)(2536)+ meson
892684 . Cross Sections for the Reactions e+e- --> K+ K- pi+pi-, K+ K- pi0pi0, and K+ K- K+ K- Measured Using Initial-State Radiation Events
892990 . First observation of the $P$-wave spin-singlet bottomonium states $h_b(1P)$ and $h_b(2P)$
893021 . Observation of the antimatter helium-4 nucleus
893232 . Observation of $\eta_c(1S)$ and $\eta_c(2S)$ decays to $K^+ K^- \pi^+ \pi^- \pi^0$ in two-photon interactions
894023 . Search for Lepton Flavour Violation at HERA
894464 . Evidence for the Suppressed Decay B- -> DK-, D -> K+pi-
895958 . Observation of transverse polarization asymmetries of charged pion pairs in $e^+e^-$ annihilation near $\sqrt{s}=10.58$ GeV
897008 . Search for $b \to u$ Transitions in $B^\pm \to [K^\mp pi^\pm \pi^0]_D K^\pm$ Decays
897416 . Study of radiative bottomonium transitions using converted photons
897420 . Measurement of heavy-quark jet photoproduction at HERA
897683 . First Observation of Radiative B^0 -> \phi K^0 \gamma Decays and Measurements of Their Time-Dependent CP Violation
897836 . Observation of $X(3872)\to J/\psi \gamma$ and search for $X(3872)\to\psi'\gamma$ in B decays
897848 . Amplitude Analysis of $B^0\to K^+ \pi^- \pi^0$ and Evidence of Direct CP Violation in $B\to K^* \pi$ decays
898660 . Study of $B^{\pm}\to K^{\pm}(K_{S}K\pi)^0$ decay and determination of $\eta_c$ and $\eta_{c}(2S)$ parameters
899013 . Search for CP violation in the decay $D^\pm \to K_S^0\pi^\pm$
900947 . Search for CP violation using $T$-odd correlations in $D^+\rightarrow K^+K^0_S\pi^+\pi^-$ and $D_s^+\rightarrow K^+ K^0_S\pi^+\pi^-$ decays
900997 . Study of di-pion bottomonium transitions and search for the $h_b(1P)$ state
901433 . Measurements of branching fractions and CP asymmetries and studies of angular distributions for B ---> phi phi K decays
912665 . Measurement of D^{*\pm} Meson Production and Determination of F_2^{ccbar} at low Q2 in Deep-Inelastic Scattering at HERA
914546 . Evolution of the differential transverse momentum correlation function with centrality in Au$+$Au collisions at $\sqrt{s_{NN}} =$ 200 GeV
916222 . Measurement of Photon Production in the Very Forward Direction in Deep-Inelastic Scattering at HERA
916807 . Search for Lepton-number-violating $B^+ \to D^- l^+ l^{\prime +}$ Decays
916845 . Observation of $D^+ \rightarrow K^{+} \eta^{(\prime)}$ and Search for CP Violation in $D^+ \rightarrow \pi^+ \eta^{(\prime)}$ Decays
918292 . Search for Contact Interactions in e^{\pm}p Collisions at HERA
918779 . Strangeness Enhancement in Cu+Cu and Au+Au Collisions at $\sqrt{s_{NN}} = 200$ GeV
918972 . Measurement of the Diffractive Longitudinal Structure Function $F_L^D$ at HERA
919140 . Search for first generation leptoquarks in $ep$ collisions at HERA
919582 . Searches for Rare or Forbidden Semileptonic Charm Decays
919778 . $\rho^{0}$ Photoproduction in AuAu Collisions at $\sqrt{s_{NN}}$=62.4 GeV with STAR
920989 . Branching Fraction Measurements of the Color-Suppressed Decays $\bar{B}^0 \to D^{(*)0} \pi^0$, $D^{(*)0} \eta$, $D^{(*)0} \omega$, and $D^{(*)0} \eta^\prime$ and Measurement of the Polarization in the Decay $\bar{B}^0 \to D^{*0} \omega$
924163 . Observation of the baryonic $B$ decay $\bar{B}^0\to \Lambda_c^+ \bar{\Lambda} K^-$
924239 . Search for hadronic decays of a light Higgs boson in the radiative decay $\Upsilon \to \gamma A^0$
924618 . Observation of $B^- \to \bar{p} \Lambda D^0$ at Belle
924711 . Search for charmonium and charmonium-like states in $\Upsilon(2S)$ radiative decays
925713 . Study of $\Upsilon(3S,2S) -> \eta \Upsilon(1S)$ and $\Upsilon(3S,2S) -> \pi^+\pi^- \Upsilon(1S)$ hadronic trasitions
926068 . Observation of the rare decay $B^+ -> K^+\pi^0\pi^0$ and measurement of the quasi-two body contributions $B^+ -> K^*(892)^+\pi^0$, $B^+ -> f_0(980)K^+$ and $B^+ -> \chi_{c0}K^+$
926621 . Search for CP Violation in the Decay $\tau^- -> \pi^- K^0_S (>= 0 \pi^0) \nu_tau$
927960 . Anomalous centrality evolution of two-particle angular correlations from Au-Au collisions at $\sqrt{s_{\rm NN}}$ = 62 and 200 GeV
929522 . Directed and elliptic flow of charged particles in Cu+Cu collisions at $\sqrt{s_{NN}} =$ 22.4 GeV
930416 . Search for CP Violation in $D^\pm$ Meson Decays to $\phi \pi^\pm$
930463 . Identified hadron compositions in p+p and Au+Au collisions at high transverse momenta at $\sqrt{s_{_{NN}}} = 200$ GeV
931212 . Evidence for Direct CP Violation in $B^\pm \to \eta h^\pm$ and Observation of $B^0 \to \eta K^0$
939487 . Observation of two charged bottomonium-like resonances in Y(5S) decays
942722 . A Measurement of the Semileptonic Branching Fraction of the B_s Meson
943192 . System size and energy dependence of near-side di-hadron correlations
943293 . Search for Bbar --> Lambda_c+ X l- nu_l Decays in Events With a Fully Reconstructed B Meson
943722 . Search for the Decay $D^0 -> \gamma \gamma$ and Measurement of the Branching Fraction for $D^0 -> \pi^0 \pi^0$
944155 . Measurement of Dijet Production in Diffractive Deep-Inelastic Scattering with a Leading Proton at HERA
945298 . Measurement of the t dependence in exclusive photoproduction of $\Upsilon$(1S) mesons at HERA
945935 . Scaled momentum distributions for $K^0_S$ and $\Lambda/\bar{\Lambda}$ in DIS at HERA
945938 . Amplitude analysis and measurement of the time-dependent CP asymmetry of $B^0 \to K_S^0 K_S^0 K_S^0$ decays
946107 . Search for single-top production in $ep$ collisions at HERA
946655 . Measurement of the Azimuthal Correlation between the most Forward Jet and the Scattered Positron in Deep-Inelastic Scattering at HERA
946659 . Observation and study of the baryonic B-meson decays B to D(*) p pbar (pi) (pi)
946807 . Exclusive electroproduction of two pions at HERA
955160 . Energy and system-size dependence of two- and four-particle $v_2$ measurements in heavy-ion collisions at RHIC and their implications on flow fluctuations and nonflow
955166 . Search for the $Z_1(4050)^+$ and $Z_2(4250)^+$ states in $\bar B^0 \to \chi_{c1} K^- \pi^+$ and $B^+ \to \chi_{c1} K^0_S \pi^+$
1079912 . Study of $\bar{B}\to X_u \ell \bar{\nu}$ decays in $B\bar{B}$ events tagged by a fully reconstructed B-meson decay and determination of $\|V_{ub}\|$
1081120 . Measurement of the $W \to e \nu$ and $Z/\gamma^* \to e^+e^-$ Production Cross Sections at Mid-rapidity in Proton-Proton Collisions at $\sqrt{s}$ = 500 GeV
1081744 . Directed Flow of Identified Particles in Au + Au Collisions at $\sqrt{s{_NN}} = 200$ GeV at RHIC
1081760 . $B^0$ meson decays to $\rho^0 K^{*0}$, $f_0 K^{*0}$, and $\rho^-K^{*+}$, including higher $K^*$ resonances
1084854 . Measurement of the CP-violation Parameter sin2$\phi_1$ with a New Tagging Method at the $\Upsilon(5S)$ Resonance
1086164 . Initial-State Radiation Measurement of the $e^+e^- -> \pi^+\pi^-\pi^+\pi^-$ Cross Section
1086537 . Study of CP violation in Dalitz-plot analyses of B0 ---> K+K-K0(S), B+ ---> K+K-K+, and B+ ---> K0(S)K0(S)K+
1086982 . First observation of $B_s^0\to J/\psi\eta$ and $B_s^0\to J/\psi\eta'$
1088220 . Search for Low-Mass Dark-Sector Higgs Bosons
1089359 . Search for lepton-number violating processes in $B^+ \to h^- l^+ l^+$ decays
1090664 . Observation of new resonant structures in $\gamma \gamma \to \omega \phi$, $\phi \phi$ and $\omega \omega$
1092976 . Measurement of Inclusive and Dijet D* Meson Cross Sections in Photoproduction at HERA
1094384 . Inclusive Measurement of Diffractive Deep-Inelastic Scattering at HERA
1095371 . Evidence for CP Violation in the Decay $D^+\rightarrow K^0_S\pi^+$
1095407 . Measurements of Branching Fractions and Time-dependent CP Violating Asymmetries in $B^{0} \to D^{(*)\pm}D^{\mp}$ Decays
1107765 . Di-electron spectrum at mid-rapidity in $p+p$ collisions at $\sqrt{s} = 200$ GeV
1107905 . Study of the reaction $e^{+}e^{-} \to J/\psi\pi^{+}\pi^{-}$ via initial-state radiation at BaBar
1111233 . Measurement of Branching Fractions and Rate Asymmetries in the Rare Decays $B \to K^{(*)} l^+ l^-$
1111571 . Measurements of $D^{0}$ and $D^{*}$ Production in $p+p$ Collisions at $\sqrt{s} = 200$ GeV
1112901 . First Measurement of phi_3 with a Model-independent Dalitz Plot Analysis of B->DK, D->KsPiPi Decay
1113314 . Search for the decay $B^0\to DK^{*0}$ followed by $D\to K^-\pi^+$
1113755 . First observation of exclusive $\Upsilon(1S)$ and $\Upsilon(2S)$ decays into light hadrons
1114155 . Precise Measurement of the $e^+ e^- \to \pi^+\pi^- (\gamma)$ Cross Section with the Initial-State Radiation Method at BABAR
1114313 . Determination of the Integrated Luminosity at HERA using Elastic QED Compton Events
1114316 . Measurement of Beauty and Charm Photoproduction using Semi-muonic Decays in Dijet Events at HERA
1114529 . Longitudinal and transverse spin asymmetries for inclusive jet production at mid-rapidity in polarized $p+p$ collisions at $\sqrt{s}=200$ GeV
1114749 . Measurement of $\gamma \gamma^* \to \pi^0$ transition form factor at Belle
1115725 . Search for first-generation leptoquarks at HERA
1115826 . Evidence for an excess of $\bar{B} \to D^{(*)} \tau^-\bar{\nu}_\tau$ decays
1116254 . Measurement of Branching Fraction and First Evidence of CP Violation in $B^0 \to a_1^{\pm}(1260) \pi^\mp$ Decays
1116258 . Inclusive-jet photoproduction at HERA and determination of alphas
1116411 . Branching fraction measurement of $B^+ \to \omega \ell^+ \nu$ decays
1116415 . Evidence for the $\eta_b(2S)$ and observation of $h_b(1P) \to \eta_b(1S) \gamma$ and $h_b(2P) \to \eta_b(1S) \gamma$
1116643 . Transverse Single-Spin Asymmetry and Cross-Section for $\pi^0$ and $\eta$ Mesons at Large Feynman-$x$ in Polarized $p+p$ Collisions at $\sqrt{s}=200$ GeV
1117881 . Single Spin Asymmetry $A_N$ in Polarized Proton-Proton Elastic Scattering at $\sqrt{s}=200$ GeV
1117883 . Search for resonances decaying to $\eta_c \pi^+ \pi^-$ in two-photon interactions
1117891 . Measurement of isolated photons accompanied by jets in deep inelastic $ep$ scattering
1118043 . Improved Limits on $B^0$ Decays to Invisible Final States and to $\nu \bar{\nu} \gamma$
1118428 . Measurement of CP Asymmetries and Branching Fractions in Charmless Two-Body $B$-Meson Decays to Pions and Kaons
1118830 . Measurement of Beauty Photoproduction near Threshold using Di-electron Events with the H1 Detector at HERA
1119057 . Search for $B \to \phi \pi$ decays
1119397 . First study of $\eta_c$, $\eta(1760)$ and $X(1835)$ production via $\eta^\prime\pi^+\pi^-$ final states in two-photon collisions
1119560 . Search for the decay modes $D^0 \to e^+e^-$, $D^0 \to \mu^+ \mu^-$, and $D^0 \to e \mu$
1119563 . Search for Lepton-Flavor-Violating and Lepton-Number-Violating $\tau \to \ell h h^\prime$ Decay Modes
1119620 . Inclusive charged hadron elliptic flow in Au + Au collisions at $\sqrt{s_{NN}}$ = 7.7 - 39 GeV
1120010 . Search for $B^{0}$ decays to invisible final states
1120512 . Inclusive Deep Inelastic Scattering at High $Q^2$ with Longitudinally Polarised Lepton Beams at HERA
1120999 . Evidence of $B^+ \to \tau^+\nu$ decays with hadronic B tags
1122031 . Exclusive Measurements of $b \to s\gamma$ Transition Rate and Photon Energy Spectrum
1122034 . Study of $X(3915) \to J/\psi \omega$ in two-photon collisions
1122036 . Precision Measurement of the $B \to X_s \gamma$ Photon Energy Spectrum, Branching Fraction, and Direct CP Asymmetry $A_{CP}(B \to X_{s+d}\gamma)$
1122970 . Evidence for a Zb0(10610) in Dalitz analysis of Y(5S) -> Y(nS) pi0 pi0
1123363 . Combined inclusive diffractive cross sections measured with forward proton spectrometers in deep inelastic $ep$ scattering at HERA
1123656 . First observation of CP violation and improved measurement of the branching fraction and polarization of B0 -> D*+ D*- decays
1123662 . Measurement of B($B\to X_s \gamma$), the $B\to X_s \gamma$ photon energy spectrum, and the direct CP asymmetry in $B\to X_{s+d} \gamma$ decays
1123792 . Observation of Time Reversal Violation in the $B^0$ Meson System
1123910 . Evidence for $B^-\to D_s^+ K^- \ell^-\bar{\nu}_\ell$ and search for $B^-\to D_s^{*+} K^- \ell^-\bar{\nu}_\ell$
1124584 . Precise measurement of the branching fractions for $B_s\to D_s^{(*)+} D_s^{(*)-}$ and first measurement of the $D_s^{*+} D_s^{*-}$ polarization using $e^+e^-$ collisions
1125496 . A search for the decay modes $B^{+-} \to h^{+-} \tau^{+-}l$
1125567 . The branching fraction of $\tau^- \to \pi^- K^0_S K^0_S (\pi^0) \nu_\tau$ decays
1125973 . Branching fraction and form-factor shape measurements of exclusive charmless semileptonic B decays, and determination of $|V_{ub}|$
1126127 . Measurement of the Time-Dependent CP Asymmetry of Partially Reconstructed $B^0\to D^{*+}D^{*-}$ Decays
1127499 . $J/\psi$ production at high transverse momenta in $p+p$ and Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV
1127599 . Study of the baryonic $B$ decay $B^- \to \Sigma_c^{++} \bar{p} \pi^- \pi^-$
1180018 . Production of the excited charm mesons $D_1$ and $D^*_2$ at HERA
1180196 . Evidence for $B^- \to \tau^- \bar{\nu}_\tau$ with a Hadronic Tagging Method Using the Full Data Sample of Belle
1183813 . Measurement of high-Q2 neutral current deep inelastic $e^+p$ scattering cross sections with a longitudinally polarized positron beam at HERA
1185407 . Study of high-multiplicity 3-prong and 5-prong tau decays at BABAR
1186384 . Measurement of $D^0-\bar{D}^0$ Mixing and CP Violation in Two-Body $D^0$ Decays
1188677 . Study of Three-Body Y(10860) Decays
1188886 . Search for di-muon decays of a low-mass Higgs boson in radiative decays of the Υ(1S)
1189434 . Measurements of branching fractions and direct CP asymmetries for B→Kπ, B→ππ and B→KK decays
1191900 . Production of $Z^0$ bosons in elastic and quasi-elastic $ep$ collisions at HERA
1192035 . Search for a low-mass scalar Higgs boson decaying to a tau pair in single-photon decays of $\Upsilon(1S)$
1193349 . Study of the hadronic transitions Υ(2S)→(η,π$^0$)Υ(1S) at Belle
1198429 . Combination and QCD Analysis of Charm Production Cross Section Measurements in Deep-Inelastic ep Scattering at HERA
1204444 . Study of the reaction $e^{+}e^{-}\to \psi(2S)\pi^{-}\pi^{-}$ via initial-state radiation at BaBar
1204785 . Measurement of inelastic $J/\psi$ and $\psi^\prime$ photoproduction at HERA
1206352 . Experimental studies of di-jets in Au + Au collisions using angular correlations with respect to back-to-back leading hadrons
1206605 . Search for direct CP violation in singly Cabibbo-suppressed D±→K+K-π± decays
1207260 . Search for CP violation in the Decays $D^{\pm} \to K^0_{\scriptscriptstyle S} K^\pm$, $D_s^{\pm} \to K^0_{\scriptscriptstyle S} K^\pm$, and $D_s^{\pm}\to K^0_{\scriptscriptstyle S} \pi^\pm$
1207322 . Measurement of $J/\psi$ Azimuthal Anisotropy in Au+Au Collisions at $\sqrt{s_{NN}}$ = 200 GeV
1207589 . Study of $B^0 \to \rho^0 \rho^0$ decays, implications for the CKM angle $\phi_2$ and search for other B0 decay modes with a four-pion final state
1208699 . Search for CP Violation in the Decay $D^+\rightarrow K^0_S K^+$
1208997 . Measurement of the inclusive semileptonic branching fraction $\mathcal{B}(B_s^0 \to X^- \ell^+ \nu_{\ell})$ at Belle
1209559 . Observation of direct CP violation in the measurement of the Cabibbo-Kobayashi-Maskawa angle gamma with $B^\pm\to D^{(*)}K^{(*)\pm}$ decays
1209562 . Search for heavy neutrinos at Belle
1210062 . Third Harmonic Flow of Charged Particles in Au+Au Collisions at sqrtsNN = 200 GeV
1210463 . Observation of an Energy-Dependent Difference in Elliptic Flow between Particles and Antiparticles in Relativistic Heavy Ion Collisions
1210464 . Elliptic flow of identified hadrons in Au+Au collisions at $\sqrt{s_{NN}}=$ 7.7-62.4 GeV
1210649 . Time-Integrated Luminosity Recorded by the BABAR Detector at the PEP-II $e^+ e^-$ Collider
1216515 . Precision Measurement of Charged Pion and Kaon Differential Cross Sections in e+e- Annihilation at s=10.52  GeV
1216565 . System-size dependence of transverse momentum correlations at $\sqrt{s_{NN}}=62.4$ and 200 GeV at the BNL Relativistic Heavy Ion Collider
1217421 . Study of $e^+e^- \to p \bar{p}$ via initial-state radiation at BABAR
1217425 . Study of the decay $\bar{B}^{0}\rightarrow\Lambda_{c}^{+}\bar{p}\pi^{+}\pi^{-}$ and its intermediate states
1217553 . Measurement of the CP violation parameters in $B^0 \to \pi^+ \pi^-$ decays
1217865 . Measurement of Charged Particle Spectra in Deep-Inelastic ep Scattering at HERA
1219133 . Freeze-out dynamics via charged kaon femtoscopy in $\sqrt{{s}_{NN}}$ = 200 GeV central Au + Au collisions
1219828 . Fluctuations of charge separation perpendicular to the event plane and local parity violation in $\sqrt{s_{NN}}=200$ GeV Au+Au collisions at the BNL Relativistic Heavy Ion Collider
1219953 . Search for an $H$-dibaryon with mass near $2m_\Lambda$ in $\Upsilon(1S)$ and $\Upsilon(2S)$ decays
1220382 . Measurement of $D^\pm$ production in deep inelastic $ep$ scattering with the ZEUS detector at HERA
1221099 . Jet-Hadron Correlations in $\sqrt{s_{NN}} = 200$ GeV $p+p$ and Central $Au+Au$ Collisions
1222328 . Measurement of an Excess of $\bar{B} \to D^{(*)}\tau^- \bar{\nu}_\tau$ Decays and Implications for Charged Higgs Bosons
1222542 . Measurement of charge multiplicity asymmetry correlations in high-energy nucleus-nucleus collisions at $\sqrt{{s}_{NN}} =$ 200 GeV
1223991 . Search for $B \to h^{(*)} \nu \bar{\nu}$ with the full Belle $\Upsilon(4S)$ data sample
1225276 . Search for the rare decays $B → πℓ^+ℓ^-$ and $B^0 → ηℓ^+ℓ^-$
1225526 . Measurement of $ D^{*\pm}$ production in deep inelastic scattering at HERA
1225884 . Search for $B \to K^{(*)} \nu \overline \nu$ and invisible quarkonium decays
1225975 . Study of $e^+e^- → π^+ π^- J/ψ$ and Observation of a Charged Charmoniumlike State at Belle
1228201 . Measurement of CP-violating asymmetries in $B^0 \to (\rho \pi)^0$ decays using a time-dependent Dalitz plot analysis
1228343 . Evidence of a new narrow resonance decaying to $\chi_{c1}\gamma$ in $B \to \chi_{c1} \gamma K$
1228910 . Measurement of the $D^*(2010)^+$ natural line width and the $D^*(2010)^+ - D^0$ mass difference
1228913 . Elastic and Proton-Dissociative Photoproduction of J/psi Mesons at HERA
1229032 . Evidence for the decay $B^0 \to K^+K^-\pi^0$
1229331 . Measurement of the $D*(2010)^+$ meson width and the $D*(2010)^+ - D^0$ mass difference
1230342 . Evidence for $\bar{B}_s^0 \to \Lambda_c^+ \bar{\Lambda} \pi^-$
1232210 . Search for $CP$ Violation in $B^0$-$\bar{B}^0$ Mixing using Partial Reconstruction of $B^0 \to D^{*-}X\ell^+ \nu_\ell$ and a Kaon Tag
1233527 . The BABAR Detector: Upgrades, Operation and Performance
1234230 . Study of the $K^+ K^-$ invariant-mass dependence of CP asymmetry in $B^+ \rightarrow K^+ K^- K^+$ decays
1235533 . Measurement of exclusive $\Upsilon(1S)$ and $\Upsilon(2S)$ decays into Vector-Pseudoscalar final states
1238273 . Study of Exclusive $B \to X_u \ell \nu$ Decays and Extraction of $\|V_{ub}\|$ using Full Reconstruction Tagging at the Belle Experiment
1238276 . Production of charged pions, kaons, and protons in $e^+e^-$ annihilations into hadrons at $\sqrt{s}$=10.54  GeV
1238601 . Evidence for semileptonic $B^- \to p\bar{p}l^-\bar{\nu}_l$ decays
1238807 . Precision measurement of the $e^+e^- → K^+K^-(γ)$ cross section with the initial-state radiation method at BABAR
1239346 . Measurement of charm fragmentation fractions in photoproduction at HERA
1239347 . Experimental constraints on the spin and parity of the $Z$(4430)$^+$
1239834 . First observation of Cabibbo-suppressed $\Xi_c^0$ decays
1239960 . Search for Bottomonium States in Exclusive Radiative $\Upsilon(2S)$ Decays
1243605 . Search for a light Higgs boson decaying to two gluons or $s\bar{s}$ in the radiative decays of $\Upsilon(1S)$
1244125 . Measurement of the wrong-sign decay $D^0 \to K^+ \pi^-\pi^+ \pi^-$
1244311 . Measurements of branching fractions of leptonic and hadronic $D_{s}^{+}$ meson decays and extraction of the $D_{s}^{+}$ meson decay constant
1245023 . High-statistics study of $K^0_S$ pair production in two-photon collisions
1246781 . Measurement of the Mass of the D0 Meson
1247058 . Measurement of the $e^+e^- \to p\bar{p}$ cross section in the energy range from 3.0 to 6.5 GeV
1247059 . Angular analysis of $B^0 \to \phi K^{*}$ decays and search for $CP$ violation at Belle
1247460 . Measurement of the $B^+ \to \omega \ell^+ \nu$ branching fraction with semileptonically tagged B mesons
1247463 . First observation of the $Z \frac{0}{b}$(10610) in a Dalitz analysis of $\Upsilon$(10860) $\to \Upsilon$(nS)$\pi^0 \pi^0$
1252555 . Measurement of $e^+ e^- \to \omega \pi^0$, $K^{\ast}(892)\bar{K}$ and $K_2^{\ast}(1430)\bar{K}$ at $\sqrt{s}$ near 10.6 GeV
1252560 . Measurement of the decays $B^0_s → J/ψϕ(1020), B^0_s → J/ψf_2′(1525)$ and $B^0_s → J/ψK^+K^-$ at Belle
1253360 . Neutral pion cross section and spin asymmetries at intermediate pseudorapidity in polarized proton collisions at < math display="inline" > < mrow > < msqrt > < mrow > < mi > s < /mi > < /mrow > < /msqrt > < mo $\ge$ < /mo > < mn > 200 < /mn > < mtext >   < /mtext > < mtext >   < /mtext > < mi > GeV < /mi > < /mrow > < /math >
1254862 . Measurement of Collins asymmetries in inclusive production of charged pion pairs in e^+e^- annihilation at BABAR
1255072 . Energy Dependence of Moments of Net-proton Multiplicity Distributions at RHIC
1257389 . Evidence for the suppressed decay $B^-$→$DK^-$, D→$K^+π^-π^0$
1257984 . Measurement of branching fractions for B \to J/\psi \eta K decays and search for a narrow resonance in the J/\psi \eta final state
1258446 . $J/\psi$ production at low $p_T$ in Au + Au and Cu + Cu collisions at $\sqrt{s_{NN}}=200$ GeV with the STAR detector
1262705 . Search for lepton-number violating <math display="inline"><mrow><msup><mrow><mi>B</mi></mrow><mrow><mo>+</mo></mrow></msup><mo stretchy="false">→</mo><msup><mrow><mi>X</mi></mrow><mrow><mo>−</mo></mrow></msup><msup><mrow><mo>ℓ</mo></mrow><mrow><mo>+</mo></mrow></msup><msup><mrow><mo>ℓ</mo></mrow><mrow><mo>′</mo><mo>+</mo></mrow></msup></mrow></math> decays
1262797 . Measurement of the $\tau$-lepton lifetime at Belle
1263695 . J/ψ polarization in p+p collisions at $\sqrt{s}$ = 200 GeV in STAR
1264205 . Search for CP violation in $\tau \to K^0_S \pi \nu_\tau$ decays at Belle
1266057 . Search for the process $e^+e^-\to J/\psi X(1835)$ at $\sqrt{s}\approx10.6$ GeV
1266253 . Measurement of branching fractions and CP violation parameters in $B\to\omega K$ decays with first evidence of CP violation in $B^0 \to \omega K^0_S$
1266952 . Evidence for the decay $B^0 \to \omega \omega$ and search for $B^0 \to \omega \phi$
1267506 . Search for doubly charmed baryons and study of charmed strange baryons at Belle
1267651 . Photoproduction of Isolated Photons, Inclusively and with a Jet, at HERA
1269346 . Suppression of $\Upsilon$ production in d+Au and Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV
1269455 . Search for $B^0 \to p \overline {\Lambda} \pi^- \gamma$ at Belle
1269458 . Measurement of neutral current e$\pm$p cross sections at high Bjorken x with the ZEUS detector
1269731 . Measurement of inclusive $e p$ cross sections at high $Q^2$ at $\sqrt s =$ 225 and 252 GeV and of the longitudinal proton structure function $F_L$ at HERA
1272843 . Measurement of the $B \to X_s l^+l^-$ branching fraction and search for direct CP violation from a sum of exclusive final states
1273667 . Search for the decay $\bar{B}^0 \to \Lambda_c^+ \bar{p}p \bar{p}$
1275614 . Dielectron Mass Spectra from Au+Au Collisions at $\sqrt{s_{\rm NN}}$ = 200 GeV
1275621 . Measurement of the Branching Fraction $\mathcal B(\Lambda_c^+ \to p K^- \pi^+)$
1277069 . Beam-Energy Dependence of the Directed Flow of Protons, Antiprotons, and Pions in Au+Au Collisions
1277238 . Observation of $D^0-\bar{D}^0$ Mixing in $e^+e^-$ Collisions
1278588 . Evidence for the baryonic decay $\bar{B}^0 \to D^0\Lambda\bar{\Lambda}$
1280557 . Beam energy dependence of moments of the net-charge multiplicity distributions in Au+Au collisions at RHIC
1280745 . Dielectron azimuthal anisotropy at mid-rapidity in Au + Au collisions at $\sqrt{s_{_{NN}}} = 200$ GeV
1282136 . Measurements of Branching Fractions of $\tau$ Lepton Decays with one or more $K^{0}_{S}$
1282602 . Updated cross section measurement of $e^+ e^- \to K^+ K^- J/\psi$ and $K_S^0K_S^0J/\psi$ via initial state radiation at Belle
1283183 . Measurement of the lepton forward-backward asymmetry in $B \rightarrow X_s \ell^+ \ell^-$ decays with a sum of exclusive modes
1283743 . Amplitude analysis of $e^+e^- \to \Upsilon(nS) \pi^+\pi^-$ at $\sqrt{s}=10.865$~GeV
1286317 . Antideuteron production in $\Upsilon(nS)$ decays and in $e^+e^- \to q\bar{q}$ at $\sqrt{s} \approx 10.58$ GeV
1286656 . Beam-energy-dependent two-pion interferometry and the freeze-out eccentricity of pions measured in heavy ion collisions at the STAR detector
1287632 . Dalitz plot analysis of $\eta_c \to K^+ K^- \eta$ and $\eta_c \to K^+ K^- \pi^0$ in two-photon interactions
1287920 . Cross sections for the reactions $e^+ e^-\to K_S^0 K_L^0$, $K_S^0 K_L^0 \pi^+\pi^-$, $K_S^0 K_S^0 \pi^+\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation
1288065 . Measurement of Feynman-$x$ Spectra of Photons and Neutrons in the Very Forward Direction in Deep-Inelastic Scattering at HERA
1288534 . Event-plane-dependent dihadron correlations with harmonic $v_n$ subtraction in Au + Au collisions at $\sqrt{s_{NN}}=200$ GeV
1288708 . Search for {CP} violation in $D^0 \to \pi^0 \pi^0$ decays
1288917 . Beam-energy dependence of charge separation along the magnetic field in Au+Au collisions at RHIC
1289224 . Measurement of $D^0-\bar{D}^0$ mixing and search for indirect CP violation using $D^0\to K_S^0\pi^+\pi^-$ decays
1291549 . Measurements of the masses and widths of the $\Sigma_{c}(2455)^{0/++}$ and $\Sigma_{c}(2520)^{0/++}$ baryons
1292132 . Observation of $D^0$ Meson Nuclear Modifications in Au+Au Collisions at $\sqrt{s_{NN}}=200$  GeV
1292476 . Deep inelastic cross-section measurements at large y with the ZEUS detector at HERA
1292792 . Measurement of longitudinal spin asymmetries for weak boson production in polarized proton-proton collisions at RHIC
1297225 . Measurement of $D^{\ast}$ photoproduction at three different centre-of-mass energies at HERA
1297229 . Precision Measurement of the Longitudinal Double-spin Asymmetry for Inclusive Jet Production in Polarized Proton Collisions at $\sqrt{s}=200$ GeV
1298024 . Elliptic flow of electrons from heavy-flavor hadron decays in Au + Au collisions at $\sqrt{s_{\rm NN}} = $ 200, 62.4, and 39 GeV
1298276 . Measurement of beauty and charm production in deep inelastic scattering at HERA and measurement of the beauty-quark mass
1298390 . Further studies of the photoproduction of isolated photons with a jet at HERA
1298980 . Measurements of direct CP asymmetries in $B→X_sγ$ decays using sum of exclusive decays
1300153 . Search for a Dark Photon in $e^+e^-$ Collisions at BaBar
1301218 . Measurement of multijet production in $ep$ collisions at high $Q^2$ and determination of the strong coupling $\alpha _s$
1302816 . The Physics of the B Factories
1302818 . Search for $B^+ \to e^+ \nu$ and $B^+ \to \mu^+ \nu$ decays using hadronic tagging
1308513 . Study of $B^{\pm,0} \to J/\psi K^+ K^- K^{\pm,0}$ and search for $B^0 \to J/\psi\phi$ at BABAR
1309588 . Observation of $e^+e^- \to \pi^+ \pi^- \pi^0 \chi_{bJ}$ and Search for $X_b \to \omega \Upsilon(1S)$ at $\sqrt{s}=10.867$  GeV
1311513 . $\Lambda\Lambda$ Correlation Function in Au+Au collisions at $\sqrt{s_{NN}}=$ 200 GeV
1311834 . Charged-to-neutral correlation at forward rapidity in Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV
1312368 . Measurement of Time-Dependent $CP$ Violation in $B^0\to \eta'K^0$ Decays
1312621 . Observation of the decay $B^0 \to \eta' K^*(892)^0$
1312626 . Observation of a new charged charmoniumlike state in $\bar{B}^0 → J/ψK^-π^+$ decays
1315466 . Isolation of Flow and Nonflow Correlations by Two- and Four-Particle Cumulant Measurements of Azimuthal Harmonics in $\sqrt{s_{_{\rm NN}}} =$ 200 GeV Au+Au Collisions
1317648 . Study of Michel parameters in leptonic $\tau$ decays at Belle
1317877 . Measurement of the branching fraction of $B^+ \to \tau^+ \nu_\tau$ decays with the semileptonic tagging method and the full Belle data sample
1319178 . Evidence of $ϒ(1S) → J/ψ + χ_{c1}$ and search for double-charmonium production in ϒ(1S) and ϒ(2S) decays
1322094 . Observation of the baryonic decay $\bar{B}^0 \to \Lambda^+_c \bar{p} K^- K^+$
1322126 . Di-hadron correlations with identified leading hadrons in 200 GeV Au + Au and d + Au collisions at STAR
1322376 . Bottomonium spectroscopy and radiative transitions involving the $\chi_bJ(1P,2P)$ states at BABAR
1322965 . Energy Dependence of $K/\pi$, $p/\pi$, and $K/p$ Fluctuations in Au+Au Collisions from $\rm \sqrt{s_{NN}}$ = 7.7 to 200 GeV
1324785 . Measurement of $e^+e^- \to \pi^+\pi^-\psi(2S)$ via Initial State Radiation at Belle
1326639 . Search for new $\pi^0$-like particles produced in association with a $\tau$-lepton pair
1326640 . Study of $CP$ Asymmetry in $B^0-\bar B^0$ Mixing with Inclusive Dilepton Events
1326905 . Measurement of $B^0 \to D_s^- K^0_S\pi^+$ and $B^+ \to D_s^- K^+K^+$ branching fractions
1330289 . Measurement of the $\bar{B} \rightarrow X_s \gamma$ Branching Fraction with a Sum of Exclusive Decays
1331399 . Search for $B_{s}^{0}\rightarrow\gamma\gamma$ and a measurement of the branching fraction for $B_{s}^{0}\rightarrow\phi\gamma$
1332186 . Measurement of Dijet Production in Diffractive Deep-Inelastic ep Scattering at HERA
1334693 . Measurement of the $D^0 \to \pi^- e^+ \nu_e$ differential decay branching fraction as a function of $q^2$ and study of form factor parameterizations
1335269 . Dalitz plot analyses of $B^0 → D^−D^0K^+$ and $B^+ → \overline{D}^0D^0K^+$ decays
1335765 . Effect of event selection on jetlike correlation measurement in $d$+Au collisions at $\sqrt{s_{\rm{NN}}}=200$ GeV
1336340 . Evidence for $CP$ violation in $B^{+} \to K^{*}(892)^{+} \pi^{0}$ from a Dalitz plot analysis of $B^{+} \to K^{0}_{\rm S} \pi^{+} \pi^{0}$ decays
1336624 . Measurements of the $\Upsilon$(10860) and $\Upsilon$(11020) resonances via $\sigma(e^+e^-\to \Upsilon(nS)\pi^+ \pi^-)$
1337783 . Measurement of the direct $CP$ asymmetry in $\bar{B}\rightarrow X_{s+d}\gamma$ decays with a lepton tag
1340691 . Energy dependence of acceptance-corrected dielectron excess mass spectrum at mid-rapidity in Au$+$Au collisions at $\sqrt{s_{NN}} =$ 19.6 and 200 GeV
1341041 . Search for B decays to final states with the η$_{c}$ meson
1341290 . Observation of X(3872) in B→X(3872)Kπ decays
1342448 . Search for the decay $B^+\rightarrow\overline{K}{}^{*0}K^{*+}$ at Belle
1343110 . Diffractive Dijet Production with a Leading Proton in $ep$ Collisions at HERA
1343322 . Measurement of the branching fractions of the radiative leptonic $\tau$ decays $\tau \to e\gamma\nu\bar{\nu}$ and $\tau \to \mu\gamma\nu\bar{\nu}$ at $B{\small A}B{\small AR}$
1343511 . Search for Long-Lived Particles in $e^+e^-$ Collisions
1345821 . Search for a light Higgs resonance in radiative decays of the Y(1S) with a charm tag
1346514 . Measurement of the amplitude ratio of $B^0 \to D^0K^{*0}$ and $B^0 \to \bar{D^0}K^{*0}$ decays with a model-independent Dalitz plot analysis using $D\to K_S^0\pi^+\pi^-$ decays
1346551 . Long-range pseudorapidity dihadron correlations in $d$+Au collisions at $\sqrt{s_{\rm NN}}=200$ GeV
1347265 . Search for $B^+ \to e^+ \nu$ and $B^+ \to \mu^+ \nu$ decays using hadronic tagging
1352818 . The $\phi (1020)\rightarrow e^{+}e^{-}$ meson decay measured with the STAR experiment in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV
1353536 . Measurement of the branching fraction of B^+ -> tau^+ nu_tau decays with the semileptonic tagging method
1353667 . Combination of differential D$^{∗\pm}$ cross-section measurements in deep-inelastic ep scattering at HERA
1357596 . Observation of Transverse Spin-Dependent Azimuthal Correlations of Charged Pion Pairs in $p^\uparrow+p$ at $\sqrt{s}=200$ GeV
1357984 . Evidence for the decay $B^{0} \to \eta \pi^0$
1357992 . Measurements of Dielectron Production in Au$+$Au Collisions at $\sqrt{s_{\rm NN}}$ = 200 GeV from the STAR Experiment
1358399 . Semi-inclusive studies of semileptonic $B_s$ decays at Belle
1358666 . Observation of charge asymmetry dependence of pion elliptic flow and the possible chiral magnetic wave in heavy-ion collisions
1358936 . Measurements of $B\rightarrow \bar{D} D_{s0} ^{*+}(2317)$ decay rates and a search for isospin partners of the $D_{s0}^{*+} (2317)$
1364360 . Search for $B^+ → ℓ^+ν_ℓγ$ decays with hadronic tagging using the full Belle data sample
1369998 . Study of $D^{**}$ production and light hadronic states in the $\bar{B}^0 \to D^{*+} \omega \pi^-$ decay
1370440 . First Observation of CP Violation in $\overline{B}^0 \to D^{(*)}_{\rm CP} h^0$ Decays by a Combined Time-Dependent Analysis of BABAR and Belle Data
1372086 . Production of exclusive dijets in diffractive deep inelastic scattering at HERA
1373553 . Azimuthal anisotropy in U$+$U and Au$+$Au collisions at RHIC
1373743 . Measurement of Azimuthal Modulations in the Cross-Section of Di-Pion Pairs in Di-Jet Production from Electron-Positron Annihilation
1373909 . Search for mixing-induced CP violation using partial reconstruction of $\bar B^0 \to D^{*+} X\ell^- \bar \nu_{\ell}$ and kaon tagging
1376480 . Measurement of $e^+e^- \to \gamma\chi_{cJ}$ via initial state radiation at Belle
1377201 . Collins asymmetries in inclusive charged $KK$ and $K\pi$ pairs produced in $e^+e^-$ annihilation
1377206 . Combination of measurements of inclusive deep inelastic ${e^{\pm }p}$ scattering cross sections and QCD analysis of HERA data
1378002 . Probing parton dynamics of QCD matter with $\Omega$ and $\phi$ production
1380446 . First observation of the hadronic transition $ \Upsilon(4S) \to \eta h_{b}(1P)$ and new measurement of the $h_b(1P)$ and $\eta_b(1S)$ parameters
1382593 . Measurement of the branching ratio of $\bar{B} \to D^{(\ast)} \tau^- \bar{\nu}_\tau$ relative to $\bar{B} \to D^{(\ast)} \ell^- \bar{\nu}_\ell$ decays with hadronic tagging at Belle
1382600 . Beam-energy dependence of charge balance functions from Au + Au collisions at energies available at the BNL Relativistic Heavy Ion Collider
1383130 . Study of the $e^+e^-\to K^+K^-$ reaction in the energy range from 2.6 to 8.0 GeV
1383879 . Centrality and transverse momentum dependence of elliptic flow of multistrange hadrons and $\phi$ meson in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV
1385105 . Measurement of Interaction between Antiprotons
1385752 . Observation of $\overline{B} \to D^{(*)} \pi^+\pi^- \ell^-\overline{\nu}$ decays in $e^+e^-$ collisions at the $\Upsilon(4S)$ resonance
1387751 . Exclusive $\rho ^0$ meson photoproduction with a leading neutron at HERA
1388182 . Measurement of initial-state–final-state radiation interference in the processes $e^+e^- → μ^+μ^-γ$ and $e^+e^- → π^+π^-γ$
1389855 . Energy scan of the $e^+e^- \to h_b(nP)\pi^+\pi^-$ $(n=1,2)$ cross sections and evidence for $\Upsilon(11020)$ decays into charged bottomonium-like states
1390112 . Study of $\pi^0$ pair production in single-tag two-photon collisions
1391152 . Measurement of angular asymmetries in the decays $B \to K^*ℓ^+ℓ^-$
1391505 . Inclusive cross sections for pairs of identified light charged hadrons and for single protons in $e^+e^-$ at $\sqrt{s}=$ 10.58 GeV
1391645 . First model-independent Dalitz analysis of $B^0 \to DK^{*0}$, $D\to K_S^0\pi^+\pi^-$ decay
1392799 . Observation of $B^{0} \rightarrow p\bar{\Lambda} D^{(*)-}$
1394389 . Search for $B^0 \to \pi^- \tau^+ \nu_\tau$ with hadronic tagging at Belle
1395100 . Measurement of $D^0 – \bar {D^0}$ mixing and search for CP violation in $D^0 \to K^+ K^−, \pi^+ \pi^−$ decays with the full Belle data set
1395151 . Centrality dependence of identified particle elliptic flow in relativistic heavy ion collisions at $\sqrt{s_{NN}}$=7.7–62.4 GeV
1396144 . Study of $\mathbf{B^{0}\rightarrow\rho^{+}\rho^{-}}$ decays and implications for the CKM angle $\mathbf{\phi_2}$
1397632 . Measurement of the decay $B\to D\ell\nu_\ell$ in fully reconstructed events and determination of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cb}|$
1403544 . Measurement of the I=1/2 $K \pi$ $\mathcal{S}$-wave amplitude from Dalitz plot analyses of $\eta_c \to K \bar K \pi$ in two-photon interactions
1405433 . Measurement of the transverse single-spin asymmetry in $p^\uparrow+p \to W^{\pm}/Z^0$ at RHIC
1408515 . Observation of the decay $B_s^0\rightarrow K^0\overline{K}^0$
1408873 . Inclusive and exclusive measurements of $B$ decays to $\chi_{c1}$ and $\chi_{c2}$ at Belle
1408879 . Search for the rare decay $D^0\to\gamma\gamma$ at Belle
1409292 . Time-dependent analysis of $B^0 \to {{K^0_{S}}} \pi^- \pi^+ \gamma$ decays and studies of the $K^+\pi^-\pi^+$ system in $B^+ \to K^+ \pi^- \pi^+ \gamma$ decays
1411075 . First observation of the decay B$^0\to \psi$(2S)$\pi^0$
1411218 . First Observation of Doubly Cabibbo-Suppressed Decay of a Charmed Baryon: $\Lambda^{+}_{c} \rightarrow p K^{+} \pi^{-}$
1411223 . Observation of Zb(10610) and Zb(10650) Decaying to B Mesons
1414638 . Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC
1416992 . Measurement of elliptic flow of light nuclei at $\sqrt{s_{NN}}=$ 200, 62.4, 39, 27, 19.6, 11.5, and 7.7 GeV at the BNL Relativistic Heavy Ion Collider
1420183 . $\rm{J}/\psi$ production at low transverse momentum in p+p and d+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV
1427025 . Observation of $D^0\to \rho^0\gamma$ and search for $CP$ violation in radiative charm decays
1429661 . Search for QCD instanton-induced processes at HERA in the high- $\pmb {Q^2}$ domain
1429700 . Near-side azimuthal and pseudorapidity correlations using neutral strange baryons and mesons in d+Au, Cu+Cu and Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV
1430903 . Search for the decay B0→ϕγ
1431982 . Measurement of the branching ratio of $\bar{B}^0 \rightarrow D^{*+} \tau^- \bar{\nu}_{\tau}$ relative to $\bar{B}^0 \rightarrow D^{*+} \ell^- \bar{\nu}_{\ell}$ decays with a semileptonic tagging method
1437948 . Combined QCD and electroweak analysis of HERA data
1441203 . Measurement of the neutral $D$ meson mixing parameters in a time-dependent amplitude analysis of the $D^0\to\pi^+\pi^-\pi^0$ decay
1442357 . Jet-like Correlations with Direct-Photon and Neutral-Pion Triggers at $\sqrt{s_{_{NN}}} = 200$ GeV
1442358 . Limits on the effective quark radius from inclusive $ep$ scattering at HERA
1444882 . Search for a narrow baryonic state decaying to ${pK^0_S}$ and ${\bar{p}K^0_S}$ in deep inelastic scattering at HERA
1444981 . First observation of $\gamma \gamma \to p \bar{p} K^+ K^-$ and search for exotic baryons in $pK$ systems
1446979 . Angular analysis of $B^0 \to K^\ast(892)^0 \ell^+ \ell^-$
1454405 . Search for $XYZ$ states in $\Upsilon(1S)$ inclusive decays
1459050 . Search for a massive invisible particle $X^0$ in $B^{+}\to e^{+}X^{0}$ and $B^{+}\to \mu^{+}X^{0}$ decays
1459053 . Tests of CPT symmetry in $B^0-\overline{B}^0$ mixing and in $B^0 \to c\overline{c}K^0$ decays
1466295 . Studies of charmed strange baryons in the $\Lambda$D final state at Belle
1466440 . Search for $B^{+}\rightarrow K^{+} \tau^{+}\tau^{-}$ at the BaBar experiment
1467448 . Study of \chi_{bJ}(1P) Properties in the Radiative \Upsilon(2S) Decays
1469061 . Search for a muonic dark force at BABAR
1474129 . Direct virtual photon production in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV
1477208 . Measurement of the CKM angle $\varphi_1$ in $B^0\to\bar{D}{}^{(*)0}h^0$, $\bar{D}{}^0\to K_S^0\pi^+\pi^-$ decays with time-dependent binned Dalitz plot analysis
1477810 . Study of Excited $\Xi_c$ States Decaying into $\Xi_c^0$ and $\Xi_c^+$ Baryons
1478040 . Energy dependence of $J/\psi$ production in Au+Au collisions at $\sqrt{s_{NN}} =$ 39, 62.4 and 200 GeV
1478188 . Measurement of the branching ratio of $\bar{B}^0 \rightarrow D^{*+} \tau^- \bar{\nu}_{\tau}$ relative to $\bar{B}^0 \rightarrow D^{*+} \ell^- \bar{\nu}_{\ell}$ decays with a semileptonic tagging method
1479946 . Measurement of the inclusive $B\to X_{s+d} \gamma$ branching fraction, photon energy spectrum and HQE parameters
1481225 . Charge-dependent directed flow in Cu+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV
1482939 . $\Upsilon$ production in U + U collisions at $\sqrt{{s}_{NN}}=$ 193 GeV measured with the STAR experiment
1486427 . Dijet imbalance measurements in $Au+Au$ and $pp$ collisions at $\sqrt{s_{NN}} = 200$  GeV at STAR
1487285 . Search for a dark vector gauge boson decaying to $\pi^+ \pi^-$ using $\eta \rightarrow \pi^+\pi^- \gamma$ decays
1487722 . Measurement of the B^0 -> D^*- pi^+ pi^- pi^+ branching fraction
1488276 . Measurement of Michel Parameters ($\bar\eta$, $\xi\kappa$) in the radiative leptonic decay of tau at Belle
1493842 . Measurement of the cross section and longitudinal double-spin asymmetry for di-jet production in polarized $pp$ collisions at $\sqrt{s}$ = 200 GeV
1496981 . Measurement of Jet Production Cross Sections in Deep-inelastic ep Scattering at HERA
1498564 . Measurement of the inclusive electron spectrum from B meson decays and determination of |Vub|
1499479 . Observation of Transverse $\Lambda/\bar{\Lambda}$ Hyperon Polarization in $e^+e^-$ Annihilation at Belle
1499706 . Search for the $0^{--}$ Glueball in $\Upsilon(1S)$ and $\Upsilon(2S)$ decays
1500691 . Search for $D^{0}$ decays to invisible final states at Belle
1501479 . Measurement of the $\tau$ lepton polarization and $R(D^*)$ in the decay $\bar{B} \to D^* \tau^- \bar{\nu}_\tau$
1504055 . Lepton-Flavor-Dependent Angular Analysis of $B\to K^\ast \ell^+\ell^-$
1510298 . Measurement of $D^0$ Azimuthal Anisotropy at Midrapidity in Au+Au Collisions at $\sqrt{s_{NN}}$=200  GeV
1510300 . Harmonic decomposition of three-particle azimuthal correlations at RHIC
1510301 . Constraining the initial conditions and temperature dependent transport with three-particle correlations in Au+Au collisions
1510474 . Global $\Lambda$ hyperon polarization in nuclear collisions: evidence for the most vortical fluid
1510593 . Bulk Properties of the Medium Produced in Relativistic Heavy-Ion Collisions from the Beam Energy Scan Program
1511276 . Cross sections for the reactions $e^+ e^-\to K^0_S K^0_L\pi^0$, $K^0_S K^0_L\eta$, and $K^0_S K^0_L\pi^0\pi^0$ from events with initial-state radiation
1512115 . Measurements of jet quenching with semi-inclusive hadron+jet distributions in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV
1512299 . Precise determination of the CKM matrix element $\left| V_{cb}\right|$ with $\bar B^0 \to D^{*\,+} \, \ell^- \, \bar \nu_\ell$ decays with hadronic tagging at Belle
1512302 . Dalitz plot analyses of $J/\psi \to \pi^+ \pi^- \pi^0$, $J/\psi \to K^+ K^- \pi^0$, and $J/\psi \to K^0_S K^{\pm} \pi^{\mp}$ produced via $e^+ e^-$ annihilation with initial-state radiation
1512929 . Search for $\boldsymbol{B\to h\nu\bar{\nu}}$ decays with semileptonic tagging at Belle
1513134 . Search for Invisible Decays of a Dark Photon Produced in ${e}^{+}{e}^{-}$ Collisions at BaBar
1515028 . Coherent diffractive photoproduction of ρ0 mesons on gold nuclei at 200 GeV/nucleon-pair at the Relativistic Heavy Ion Collider
1517778 . First measurement of $\boldsymbol{T}$-odd moments in $\boldsymbol{D^{0} \rightarrow K_{S}^{0} \pi^{+} \pi^{-} \pi^{0}}$ decays
1519830 . Measurement of $D^{*}$ production in diffractive deep inelastic scattering at HERA
1520716 . Measurement of the decays $\boldsymbol{B\to\eta\ell\nu_\ell}$ and $\boldsymbol{B\to\eta^\prime\ell\nu_\ell}$ in fully reconstructed events at Belle
1590028 . Observation of an alternative $\chi_{c0}(2P)$ candidate in $e^+ e^- \rightarrow J/\psi D \bar{D}$
1591716 . Measurement of the $e^+e^-\to K^0_{\scriptscriptstyle S}K^\pm\pi^{\mp}\pi^0$ and $K^0_{\scriptscriptstyle S}K^\pm\pi^\mp\eta$ cross sections using initial-state radiation
1596830 . The Silicon Vertex Detector of the Belle II Experiment
1598261 . Measurement of the branching fraction and $CP$ asymmetry in $B^{0} \to \pi^{0}\pi^{0}$ decays, and an improved constraint on $\phi_{2}$
1598461 . Measurement of branching fraction and direct $CP$ asymmetry in charmless $B^+ \to K^+K^- \pi^+$ decays at Belle
1601508 . Studies of the diffractive photoproduction of isolated photons at HERA
1606201 . Production cross sections of hyperons and charmed baryons from $e^+e^-$ annihilation near $\sqrt{s} = 10.52$~GeV
1607562 . Invariant-mass and fractional-energy dependence of inclusive production of di-hadrons in $e^+e^-$ annihilation at $\sqrt{s}=$ 10.58 GeV
1608380 . Search for $\Lambda_c^+\to\phi p \pi^0$ and branching fraction measurement of $\Lambda_c^+\to K^-\pi^+ p \pi^0$
1608384 . Evidence for Isospin Violation and Measurement of $CP$ Asymmetries in $B \to K^{\ast}(892) \gamma$
1609067 . Beam Energy Dependence of Jet-Quenching Effects in Au+Au Collisions at $\sqrt{s_{_{ \mathrm{NN}}}}$ = 7.7, 11.5, 14.5, 19.6, 27, 39, and 62.4 GeV
1610301 . Study of $\eta$ and dipion transitions in $\Upsilon(4S)$ decays to lower bottomonia
1613517 . Angular analysis of the $e^+ e^- \to D^{(*) \pm} D^{* \mp}$ process near the open charm threshold using initial-state radiation
1613519 . Measurement of the ${D}^{*}(2010{)}^{+}\text{-}{D}^{+}$ Mass Difference
1615382 . The Belle II SVD detector
1615383 . The Monitoring System of the Belle II Vertex Detector
1615384 . Performance studies of the Belle II Silicon Vertex Detector with data taken at the DESY test beam in April 2016
1615385 . The Software Framework of the Belle II Silicon Vertex Detector and its Development for the 2016 Test-Beam at DESY
1618345 . Azimuthal transverse single-spin asymmetries of inclusive jets and charged pions within jets from polarized-proton collisions at $\sqrt{s} = 500$ GeV
1618747 . Beam-Energy Dependence of Directed Flow of $\Lambda$, $\bar{\Lambda}$, $K^\pm$, $K^0_s$ and $\phi$ in Au+Au Collisions
1621272 . Measurement of the $\tau$ lepton polarization and $R(D^*)$ in the decay $\bar{B} \rightarrow D^* \tau^- \bar{\nu}_\tau$ with one-prong hadronic $\tau$ decays at Belle
1621460 . Collision Energy Dependence of Moments of Net-Kaon Multiplicity Distributions at RHIC
1621593 . Measurement of the ${e}^{+}{e}^{{-}}{\rightarrow}{{\pi}}^{+}{{\pi}}^{{-}}{{\pi}}^{0}{{\pi}}^{0}$ cross section using initial-state radiation at BABAR
1624416 . Measurements of the absolute branching fractions of $B^{+} \to X_{c\bar{c}} K^{+}$ and $B^{+} \to \bar{D}^{(\ast) 0} \pi^{+} $ at Belle
1624691 . Determination of the strong coupling constant $\alpha_s(m_Z)$ in next-to-next-to-leading order QCD using H1 jet cross section measurements
1625743 . Measurement of the tau Michel parameters $\bar{\eta}$ and $\xi\kappa$ in the radiative leptonic decay $\tau^- \rightarrow \ell^- \nu_{\tau} \bar{\nu}_{\ell}\gamma$
1628155 . Measurement of the $^3_{\Lambda}$H lifetime in Au+Au collisions at the BNL Relativistic Heavy Ion Collider
1630825 . Multi-messenger Observations of a Binary Neutron Star Merger
1632938 . Transverse spin-dependent azimuthal correlations of charged pion pairs measured in p$^\uparrow$+p collisions at $\sqrt{s}$ = 500 GeV
1634603 . Search for light tetraquark states in $\Upsilon(1S)$ and $\Upsilon(2S)$ decays
1637368 . Observation of Excited $\Omega_c$ Charmed Baryons in $e^+e^-$ Collisions
1640639 . Search for $CP$ violation in the $D^{+}\to\pi^{+}\pi^{0}$ decay at Belle
1641071 . Measurement of branching fractions of hadronic decays of the $\Omega_c^0$ baryon
1641113 . Azimuthal anisotropy in Cu$+$Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV
1641263 . Study of $K^0_S$ pair production in single-tag two-photon collisions
1642436 . Observation of $\Xi_{c}(2930)^0$ and updated measurement of $B^{-} \to K^{-} \Lambda_{c}^{+} \bar{\Lambda}_{c}^{-}$ at Belle
1642727 . Search for $B^{-}\to\mu^{-}\bar\nu_\mu$ Decays at the Belle Experiment
1642730 . Further studies of isolated photon production with a jet in deep inelastic scattering at HERA
1647139 . Study of the process $e^+e^- \to \pi^+\pi^-\eta $ using initial state radiation
1649636 . Measurement of the cross-section ratio sigma_{psi(2S)}/sigma_{J/psi(1S)} in deep inelastic exclusive ep scattering at HERA
1654571 . Measurement of the Decays $\Lambda_c\to \Sigma\pi\pi$ at Belle
1659108 . Inclusive study of bottomonium production in association with an $\eta $ meson in $e^+e^-$ annihilations near $\varUpsilon (5S)$
1662057 . Correlation Measurements Between Flow Harmonics in Au+Au Collisions at RHIC
1663226 . Measurement of the branching fraction of $B \rightarrow D^{(*)}\pi \ell\nu$ at Belle using hadronic tagging in fully reconstructed events
1663447 . Measurement of time-dependent $CP$ asymmetries in $B^{0}\to K_S^0 \eta \gamma$ decays
1664541 . Observation of $\Upsilon(4S)\to \eta' \Upsilon(1S)$
1664542 . Search for the decay mode $B^0\rightarrow p p \bar{p} \bar{p}$
1665080 . Electronics and Firmware of the Belle II Silicon Vertex Detector Readout System
1665693 . Combination and QCD analysis of charm and beauty production cross-section measurements in deep inelastic $ep$ scattering at HERA
1667191 . Study of $\Upsilon(1S)$ radiative decays to $\gamma \pi^+ \pi^-$ and $\gamma K^+ K^-$
1668122 . First evidence for $\cos 2\beta>0$ and resolution of the CKM Unitarity Triangle ambiguity by a time-dependent Dalitz plot analysis of $B^{0} \to D^{(*)} h^{0}$ with $D \to K_{S}^{0} \pi^{+} \pi^{-}$ decays
1668123 . Measurement of $\cos{2\beta}$ in $B^{0} \to D^{(*)} h^{0}$ with $D \to K_{S}^{0} \pi^{+} \pi^{-}$ decays by a combined time-dependent Dalitz plot analysis of BaBar and Belle data
1669807 . Beam energy dependence of rapidity-even dipolar flow in Au+Au collisions
1672018 . Search for $\Upsilon(1S,2S) \to Z^{+}_{c}Z^{(\prime) -}_{c}$ and $e^{+}e^{-} \to Z^{+}_{c}Z^{(\prime) -}_{c}$ at $\sqrt{s}$ = 10.52, 10.58, and 10.867 GeV
1672149 . Measurement of eta_c(1S), eta_c(2S) and non-resonant eta' pi+ pi- production via two-photon collisions
1672453 . $J/\psi$ production cross section and its dependence on charged-particle multiplicity in $p+p$ collisions at $\sqrt{s}$ = 200 GeV
1672785 . Global polarization of $\Lambda$ hyperons in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV
1674698 . Observation of an Excited $\Omega^-$ Baryon
1674714 . Longitudinal double-spin asymmetries for dijet production at intermediate pseudorapidity in polarized $pp$ collisions at $\sqrt{s}=$ 200  GeV
1674826 . Longitudinal Double-Spin Asymmetries for $\pi^{0}$s in the Forward Direction for 510 GeV Polarized $pp$ Collisions
1676227 . Determination of electroweak parameters in polarised deep-inelastic scattering at HERA
1676541 . Low-$p_T$ $e^{+}e^{-}$ pair production in Au$+$Au collisions at $\sqrt{s_{NN}}$ = 200 GeV and U$+$U collisions at $\sqrt{s_{NN}}$ = 193 GeV at STAR
-1678261 . Observation of $e^+e^-\to\pi^+\pi^-\pi^0\chi_{b1,2}(1P)$ and search for $e^+e^-\to\phi\chi_{b1,2}(1P)$ at $\sqrt{s}=$10.96---11.05 GeV
-1679584 . Evidence of charged $\Xi_{c}(2930)$ and updated measurement of $B^{0} \to K^{0} \Lambda_{c}^{+} \bar{\Lambda}_{c}^{-}$ at Belle
+1678261 . Observation of $e^+e^-\to\pi^+\pi^-\pi^0\chi_{b1,2}(1P)$ and search for $e^+e^-\to\phi\chi_{b1,2}(1P)$ at $\sqrt{s}=$ 10.96—11.05  GeV
+1679584 . Evidence of a structure in $\bar{K}^{0} \Lambda _{c}^{+}$ consistent with a charged $\Xi _c(2930)^{+}$ , and updated measurement of $\bar{B}^{0} \rightarrow \bar{K}^{0} \Lambda _{c}^{+} \bar{\Lambda }_{c}^{-}$ at Belle
1679886 . Measurement of the spectral function for the $\tau^-\to K^-K_S\nu_{\tau}$ decay
1680647 . Observation of $\Upsilon(2S)\to\gamma \eta_{b}(1S)$ decay
-1681440 . Search for the Lepton-Flavor-Violating Decay $B^{0}\to K^{\ast 0} \mu^{\pm} e^{\mp}$
+1681440 . Search for the lepton-flavor-violating decay $B^{0}\to K^{\ast 0} \mu^{\pm} e^{\mp}$
1683069 . Measurements of branching fraction and $CP$ asymmetry of the $\bar{B}^{0}(B^{0})\to K^{0}_{S}K^{\mp}\pi^{\pm}$ decay at Belle
1684192 . Observation of $B^{+} \rightarrow p\bar{\Lambda} K^+ K^-$ and $B^{+} \rightarrow \bar{p}\Lambda K^+ K^+$
1684644 . Study of charmless decays $B^{\pm} \to K^{0}_{S} K^{0}_{S} h^{\pm}$ ($h=K,\pi$) at Belle
1685527 . The Proton-$\Omega$ correlation function in Au+Au collisions at $\sqrt{s_{NN}}$=200 GeV
1687566 . Observation of Transverse $\Lambda/\bar{\Lambda}$ Hyperon Polarization in $e^+e^-$ Annihilation at Belle
1691152 . Improved measurement of the longitudinal spin transfer to $\Lambda$ and $\bar \Lambda$ hyperons in polarized proton-proton collisions at $\sqrt s$ = 200 GeV
1691222 . Measurement of the $\gamma^{\star}\gamma^{\star} \to \eta'$ transition form factor
1691271 . Transverse spin transfer to $\Lambda$ and $\bar{\Lambda}$ hyperons in polarized proton-proton collisions at $\sqrt{s}=200\,\mathrm{GeV}$
1691954 . Observation of the decay $D^0\rightarrow K^-\pi^+e^+e^-$
1692393 . The Belle II Physics Book
1693396 . Measurement of CKM Matrix Element $|V_{cb}|$ from $\bar{B} \to D^{*+} \ell^{-} \bar{\nu}_\ell$
1694309 . Search for a light CP-odd Higgs boson and low-mass dark matter at the Belle experiment
1696692 . Measurement of the branching fraction and time-dependent $CP$ asymmetry for $B^0\to J/\psi\pi^0$ decays
1697367 . Measurement of time-dependent $CP$ violation in $B^0 \to K^0_S \pi^0 \pi^0$ decays
+1698003 . Search for a Stable Six-Quark State at BABAR
+1698390 . Observation of $\Xi(1620)^0$ and evidence for $\Xi(1690)^0$ in $\Xi_c^+ \rightarrow \Xi^-\pi^+\pi^+$ decays
+1698419 . Search for $CP$ violation with Kinematic Asymmetries in the $D^{0}\rightarrow K^{+}K^{-}\pi^{+}\pi^{-}$ Decay
+1700174 . Observation of $e^+e^- \to \gamma \chi_{c1}$ and search for $e^+e^- \to \gamma \chi_{c0}, \gamma \chi_{c2},$ and $\gamma\eta_c$ at $\sqrt{s}$ near 10.6 GeV at Belle
+1700232 . Measurements of Dielectron Production in Au$+$Au Collisions at $\sqrt{s_{NN}}$= 27, 39, and 62.4 GeV from the STAR Experiment
+1701180 . Search for the rare decay of $B^+ \to \ell^{\,+} \nu_{\ell} \gamma$ with improved hadronic tagging
+1705069 . First measurements of absolute branching fractions of $\Xi_c^0$ at Belle
diff --git a/docker/rivet-herwig/Dockerfile b/docker/rivet-herwig/Dockerfile
--- a/docker/rivet-herwig/Dockerfile
+++ b/docker/rivet-herwig/Dockerfile
@@ -1,30 +1,30 @@
-FROM hepstore/rivet:2.6.1
+FROM hepstore/rivet:2.6.2
MAINTAINER Andy Buckley <andy.buckley@cern.ch>
RUN dnf install -y boost-devel
RUN mkdir /code
RUN cd /code && \
wget https://www.hepforge.org/archive/lhapdf/LHAPDF-6.2.1.tar.gz -O- | tar xz && \
cd LHAPDF-*/ && ./configure --prefix=/usr/local && \
make -j5 && make install
#RUN lhapdf install MMHT2014{,n}lo68cl
RUN cd /usr/local/share/LHAPDF/ && \
for pdf in MMHT2014{,n}lo68cl; do \
wget https://lhapdf.hepforge.org/downloads?f=pdfsets/current/$pdf.tar.gz -O- | tar xz; \
done
RUN cd /code && \
- wget https://www.hepforge.org/archive/thepeg/ThePEG-2.1.3.tar.bz2 -O- | tar xj && \
+ wget https://www.hepforge.org/archive/thepeg/ThePEG-2.1.4.tar.bz2 -O- | tar xj && \
cd ThePEG-*/ && ./configure --enable-shared --{prefix,with-{fastjet,hepmc,lhapdf,rivet}}=/usr/local && \
make -j5 && make install
RUN cd code/ && \
- wget https://www.hepforge.org/archive/herwig/Herwig-7.1.3.tar.bz2 -O- | tar xj && \
+ wget https://www.hepforge.org/archive/herwig/Herwig-7.1.4.tar.bz2 -O- | tar xj && \
cd Herwig-*/ && \
./configure --{prefix,with-{thepeg,fastjet}}=/usr/local && \
make -j5 && make install
RUN rm -rf /code
diff --git a/docker/rivet-pythia/Dockerfile b/docker/rivet-pythia/Dockerfile
--- a/docker/rivet-pythia/Dockerfile
+++ b/docker/rivet-pythia/Dockerfile
@@ -1,23 +1,23 @@
-FROM hepstore/rivet:2.6.1
+FROM hepstore/rivet:2.6.2
MAINTAINER Andy Buckley <andy.buckley@cern.ch>
RUN dnf install -y rsync
RUN mkdir /code
RUN cd /code && \
wget https://www.hepforge.org/archive/lhapdf/LHAPDF-6.2.1.tar.gz -O- | tar xz && \
cd LHAPDF-*/ && ./configure --prefix=/usr/local && \
make -j5 && make install
RUN cd /code && \
- wget http://home.thep.lu.se/~torbjorn/pythia8/pythia8235.tgz -O- | tar xz && \
+ wget http://home.thep.lu.se/~torbjorn/pythia8/pythia8240.tgz -O- | tar xz && \
cd pythia*/ && ./configure --enable-shared --{prefix,with-{hepmc2,lhapdf6}}=/usr/local && \
make -j5 && make install
RUN cd code/ && \
wget https://www.hepforge.org/archive/agile/Sacrifice-1.1.1b.tar.gz -O- | tar xz && \
cd Sacrifice-*/ && \
./configure --{prefix,with-{pythia,hepmc,LHAPDF}}=/usr/local && \
make -j5 && make install
RUN rm -rf /code
diff --git a/include/Rivet/Analysis.hh b/include/Rivet/Analysis.hh
--- a/include/Rivet/Analysis.hh
+++ b/include/Rivet/Analysis.hh
@@ -1,1237 +1,1239 @@
// -*- C++ -*-
#ifndef RIVET_Analysis_HH
#define RIVET_Analysis_HH
#include "Rivet/Config/RivetCommon.hh"
#include "Rivet/AnalysisInfo.hh"
#include "Rivet/Event.hh"
#include "Rivet/Projection.hh"
#include "Rivet/ProjectionApplier.hh"
#include "Rivet/ProjectionHandler.hh"
#include "Rivet/AnalysisLoader.hh"
#include "Rivet/Tools/Cuts.hh"
#include "Rivet/Tools/Logging.hh"
#include "Rivet/Tools/ParticleUtils.hh"
#include "Rivet/Tools/BinnedHistogram.hh"
#include "Rivet/Tools/RivetMT2.hh"
#include "Rivet/Tools/RivetYODA.hh"
#include "Rivet/Tools/Percentile.hh"
#include "Rivet/Projections/CentralityProjection.hh"
/// @def vetoEvent
/// Preprocessor define for vetoing events, including the log message and return.
#define vetoEvent \
do { MSG_DEBUG("Vetoing event on line " << __LINE__ << " of " << __FILE__); return; } while(0)
namespace Rivet {
// Forward declaration
class AnalysisHandler;
/// @brief This is the base class of all analysis classes in Rivet.
///
/// There are
/// three virtual functions which should be implemented in base classes:
///
/// void init() is called by Rivet before a run is started. Here the
/// analysis class should book necessary histograms. The needed
/// projections should probably rather be constructed in the
/// constructor.
///
/// void analyze(const Event&) is called once for each event. Here the
/// analysis class should apply the necessary Projections and fill the
/// histograms.
///
/// void finalize() is called after a run is finished. Here the analysis
/// class should do whatever manipulations are necessary on the
/// histograms. Writing the histograms to a file is, however, done by
/// the Rivet class.
class Analysis : public ProjectionApplier {
/// The AnalysisHandler is a friend.
friend class AnalysisHandler;
public:
/// @name Standard constructors and destructors.
//@{
// /// The default constructor.
// Analysis();
/// Constructor
Analysis(const std::string& name);
/// The destructor.
virtual ~Analysis() {}
//@}
public:
/// @name Main analysis methods
//@{
/// Initialize this analysis object. A concrete class should here
/// book all necessary histograms. An overridden function must make
/// sure it first calls the base class function.
virtual void init() { }
/// Analyze one event. A concrete class should here apply the
/// necessary projections on the \a event and fill the relevant
/// histograms. An overridden function must make sure it first calls
/// the base class function.
virtual void analyze(const Event& event) = 0;
/// Finalize this analysis object. A concrete class should here make
/// all necessary operations on the histograms. Writing the
/// histograms to a file is, however, done by the Rivet class. An
/// overridden function must make sure it first calls the base class
/// function.
virtual void finalize() { }
//@}
public:
/// @name Metadata
/// Metadata is used for querying from the command line and also for
/// building web pages and the analysis pages in the Rivet manual.
//@{
/// Get the actual AnalysisInfo object in which all this metadata is stored.
const AnalysisInfo& info() const {
assert(_info && "No AnalysisInfo object :O");
return *_info;
}
/// @brief Get the name of the analysis.
///
/// By default this is computed by combining the results of the
/// experiment, year and Spires ID metadata methods and you should
/// only override it if there's a good reason why those won't
/// work. If options has been set for this instance, a
/// corresponding string is appended at the end.
virtual std::string name() const {
return ( (info().name().empty()) ? _defaultname : info().name() ) + _optstring;
}
// get name of reference data file, which could be different from plugin name
virtual std::string getRefDataName() const {
return (info().getRefDataName().empty()) ? _defaultname : info().getRefDataName();
}
// set name of reference data file, which could be different from plugin name
virtual void setRefDataName(const std::string& ref_data="") {
info().setRefDataName(!ref_data.empty() ? ref_data : name());
}
/// Get the Inspire ID code for this analysis.
virtual std::string inspireId() const {
return info().inspireId();
}
/// Get the SPIRES ID code for this analysis (~deprecated).
virtual std::string spiresId() const {
return info().spiresId();
}
/// @brief Names & emails of paper/analysis authors.
///
/// Names and email of authors in 'NAME \<EMAIL\>' format. The first
/// name in the list should be the primary contact person.
virtual std::vector<std::string> authors() const {
return info().authors();
}
/// @brief Get a short description of the analysis.
///
/// Short (one sentence) description used as an index entry.
/// Use @a description() to provide full descriptive paragraphs
/// of analysis details.
virtual std::string summary() const {
return info().summary();
}
/// @brief Get a full description of the analysis.
///
/// Full textual description of this analysis, what it is useful for,
/// what experimental techniques are applied, etc. Should be treated
/// as a chunk of restructuredText (http://docutils.sourceforge.net/rst.html),
/// with equations to be rendered as LaTeX with amsmath operators.
virtual std::string description() const {
return info().description();
}
/// @brief Information about the events needed as input for this analysis.
///
/// Event types, energies, kinematic cuts, particles to be considered
/// stable, etc. etc. Should be treated as a restructuredText bullet list
/// (http://docutils.sourceforge.net/rst.html)
virtual std::string runInfo() const {
return info().runInfo();
}
/// Experiment which performed and published this analysis.
virtual std::string experiment() const {
return info().experiment();
}
/// Collider on which the experiment ran.
virtual std::string collider() const {
return info().collider();
}
/// When the original experimental analysis was published.
virtual std::string year() const {
return info().year();
}
/// The luminosity in inverse femtobarn
virtual std::string luminosityfb() const {
return info().luminosityfb();
}
/// Journal, and preprint references.
virtual std::vector<std::string> references() const {
return info().references();
}
/// BibTeX citation key for this article.
virtual std::string bibKey() const {
return info().bibKey();
}
/// BibTeX citation entry for this article.
virtual std::string bibTeX() const {
return info().bibTeX();
}
/// Whether this analysis is trusted (in any way!)
virtual std::string status() const {
return (info().status().empty()) ? "UNVALIDATED" : info().status();
}
/// Any work to be done on this analysis.
virtual std::vector<std::string> todos() const {
return info().todos();
}
/// Return the allowed pairs of incoming beams required by this analysis.
virtual const std::vector<PdgIdPair>& requiredBeams() const {
return info().beams();
}
/// Declare the allowed pairs of incoming beams required by this analysis.
virtual Analysis& setRequiredBeams(const std::vector<PdgIdPair>& requiredBeams) {
info().setBeams(requiredBeams);
return *this;
}
/// Sets of valid beam energy pairs, in GeV
virtual const std::vector<std::pair<double, double> >& requiredEnergies() const {
return info().energies();
}
/// Get vector of analysis keywords
virtual const std::vector<std::string> & keywords() const {
return info().keywords();
}
/// Declare the list of valid beam energy pairs, in GeV
virtual Analysis& setRequiredEnergies(const std::vector<std::pair<double, double> >& requiredEnergies) {
info().setEnergies(requiredEnergies);
return *this;
}
/// Return true if this analysis needs to know the process cross-section.
/// @todo Remove this and require HepMC >= 2.06
bool needsCrossSection() const {
return info().needsCrossSection();
}
/// Declare whether this analysis needs to know the process cross-section from the generator.
/// @todo Remove this and require HepMC >= 2.06
Analysis& setNeedsCrossSection(bool needed=true) {
info().setNeedsCrossSection(needed);
return *this;
}
//@}
/// @name Internal metadata modifying methods
//@{
/// Get the actual AnalysisInfo object in which all this metadata is stored (non-const).
AnalysisInfo& info() {
assert(_info && "No AnalysisInfo object :O");
return *_info;
}
//@}
/// @name Run conditions
//@{
/// Incoming beams for this run
const ParticlePair& beams() const;
/// Incoming beam IDs for this run
const PdgIdPair beamIds() const;
/// Centre of mass energy for this run
double sqrtS() const;
/// Check if we are running rivet-merge.
bool merging() const {
return sqrtS() <= 0.0;
}
//@}
/// @name Analysis / beam compatibility testing
+ /// @todo Replace with beamsCompatible() with no args (calling beams() function internally)
+ /// @todo Add beamsMatch() methods with same (shared-code?) tolerance as in beamsCompatible()
//@{
/// Check if analysis is compatible with the provided beam particle IDs and energies
bool isCompatible(const ParticlePair& beams) const;
/// Check if analysis is compatible with the provided beam particle IDs and energies
bool isCompatible(PdgId beam1, PdgId beam2, double e1, double e2) const;
/// Check if analysis is compatible with the provided beam particle IDs and energies
bool isCompatible(const PdgIdPair& beams, const std::pair<double,double>& energies) const;
//@}
/// Set the cross section from the generator
Analysis& setCrossSection(double xs); //, double xserr=0.0);
/// Access the controlling AnalysisHandler object.
AnalysisHandler& handler() const { return *_analysishandler; }
protected:
/// Get a Log object based on the name() property of the calling analysis object.
Log& getLog() const;
/// Get the process cross-section in pb. Throws if this hasn't been set.
double crossSection() const;
/// Get the process cross-section per generated event in pb. Throws if this
/// hasn't been set.
double crossSectionPerEvent() const;
/// @brief Get the number of events seen (via the analysis handler).
///
/// @note Use in the finalize phase only.
size_t numEvents() const;
/// @brief Get the sum of event weights seen (via the analysis handler).
///
/// @note Use in the finalize phase only.
double sumW() const;
/// Alias
double sumOfWeights() const { return sumW(); }
/// @brief Get the sum of squared event weights seen (via the analysis handler).
///
/// @note Use in the finalize phase only.
double sumW2() const;
protected:
/// @name Histogram paths
//@{
/// Get the canonical histogram "directory" path for this analysis.
const std::string histoDir() const;
/// Get the canonical histogram path for the named histogram in this analysis.
const std::string histoPath(const std::string& hname) const;
/// Get the canonical histogram path for the numbered histogram in this analysis.
const std::string histoPath(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const;
/// Get the internal histogram name for given d, x and y (cf. HepData)
const std::string mkAxisCode(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const;
/// Alias
/// @deprecated Prefer the "mk" form, consistent with other "making function" names
const std::string makeAxisCode(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const {
return mkAxisCode(datasetId, xAxisId, yAxisId);
}
//@}
/// @name Histogram reference data
//@{
/// Get reference data for a named histo
/// @todo SFINAE to ensure that the type inherits from YODA::AnalysisObject?
template <typename T=YODA::Scatter2D>
const T& refData(const string& hname) const {
_cacheRefData();
MSG_TRACE("Using histo bin edges for " << name() << ":" << hname);
if (!_refdata[hname]) {
MSG_ERROR("Can't find reference histogram " << hname);
throw Exception("Reference data " + hname + " not found.");
}
return dynamic_cast<T&>(*_refdata[hname]);
}
/// Get reference data for a numbered histo
/// @todo SFINAE to ensure that the type inherits from YODA::AnalysisObject?
template <typename T=YODA::Scatter2D>
const T& refData(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const {
const string hname = makeAxisCode(datasetId, xAxisId, yAxisId);
return refData(hname);
}
//@}
/// @name Counter booking
//@{
/// Book a counter.
CounterPtr bookCounter(const std::string& name,
const std::string& title="");
// const std::string& valtitle=""
/// Book a counter, using a path generated from the dataset and axis ID codes
///
/// The paper, dataset and x/y-axis IDs will be used to build the histo name in the HepData standard way.
CounterPtr bookCounter(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
const std::string& title="");
// const std::string& valtitle=""
//@}
/// @name 1D histogram booking
//@{
/// Book a 1D histogram with @a nbins uniformly distributed across the range @a lower - @a upper .
Histo1DPtr bookHisto1D(const std::string& name,
size_t nbins, double lower, double upper,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// Book a 1D histogram with non-uniform bins defined by the vector of bin edges @a binedges .
Histo1DPtr bookHisto1D(const std::string& name,
const std::vector<double>& binedges,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// Book a 1D histogram with non-uniform bins defined by the vector of bin edges @a binedges .
Histo1DPtr bookHisto1D(const std::string& name,
const std::initializer_list<double>& binedges,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// Book a 1D histogram with binning from a reference scatter.
Histo1DPtr bookHisto1D(const std::string& name,
const Scatter2D& refscatter,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// Book a 1D histogram, using the binnings in the reference data histogram.
Histo1DPtr bookHisto1D(const std::string& name,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// Book a 1D histogram, using the binnings in the reference data histogram.
///
/// The paper, dataset and x/y-axis IDs will be used to build the histo name in the HepData standard way.
Histo1DPtr bookHisto1D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
//@}
/// @name 2D histogram booking
//@{
/// Book a 2D histogram with @a nxbins and @a nybins uniformly
/// distributed across the ranges @a xlower - @a xupper and @a
/// ylower - @a yupper respectively along the x- and y-axis.
Histo2DPtr bookHisto2D(const std::string& name,
size_t nxbins, double xlower, double xupper,
size_t nybins, double ylower, double yupper,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
/// Book a 2D histogram with non-uniform bins defined by the
/// vectors of bin edges @a xbinedges and @a ybinedges.
Histo2DPtr bookHisto2D(const std::string& name,
const std::vector<double>& xbinedges,
const std::vector<double>& ybinedges,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
/// Book a 2D histogram with non-uniform bins defined by the
/// vectors of bin edges @a xbinedges and @a ybinedges.
Histo2DPtr bookHisto2D(const std::string& name,
const std::initializer_list<double>& xbinedges,
const std::initializer_list<double>& ybinedges,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
/// Book a 2D histogram with binning from a reference scatter.
Histo2DPtr bookHisto2D(const std::string& name,
const Scatter3D& refscatter,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
/// Book a 2D histogram, using the binnings in the reference data histogram.
Histo2DPtr bookHisto2D(const std::string& name,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
/// Book a 2D histogram, using the binnings in the reference data histogram.
///
/// The paper, dataset and x/y-axis IDs will be used to build the histo name in the HepData standard way.
Histo2DPtr bookHisto2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
//@}
/// @name 1D profile histogram booking
//@{
/// Book a 1D profile histogram with @a nbins uniformly distributed across the range @a lower - @a upper .
Profile1DPtr bookProfile1D(const std::string& name,
size_t nbins, double lower, double upper,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// Book a 1D profile histogram with non-uniform bins defined by the vector of bin edges @a binedges .
Profile1DPtr bookProfile1D(const std::string& name,
const std::vector<double>& binedges,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// Book a 1D profile histogram with non-uniform bins defined by the vector of bin edges @a binedges .
Profile1DPtr bookProfile1D(const std::string& name,
const std::initializer_list<double>& binedges,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// Book a 1D profile histogram with binning from a reference scatter.
Profile1DPtr bookProfile1D(const std::string& name,
const Scatter2D& refscatter,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// Book a 1D profile histogram, using the binnings in the reference data histogram.
Profile1DPtr bookProfile1D(const std::string& name,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// Book a 1D profile histogram, using the binnings in the reference data histogram.
///
/// The paper, dataset and x/y-axis IDs will be used to build the histo name in the HepData standard way.
Profile1DPtr bookProfile1D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
//@}
/// @name 2D profile histogram booking
//@{
/// Book a 2D profile histogram with @a nxbins and @a nybins uniformly
/// distributed across the ranges @a xlower - @a xupper and @a ylower - @a
/// yupper respectively along the x- and y-axis.
Profile2DPtr bookProfile2D(const std::string& name,
size_t nxbins, double xlower, double xupper,
size_t nybins, double ylower, double yupper,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
/// Book a 2D profile histogram with non-uniform bins defined by the vectorx
/// of bin edges @a xbinedges and @a ybinedges.
Profile2DPtr bookProfile2D(const std::string& name,
const std::vector<double>& xbinedges,
const std::vector<double>& ybinedges,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
/// Book a 2D profile histogram with non-uniform bins defined by the vectorx
/// of bin edges @a xbinedges and @a ybinedges.
Profile2DPtr bookProfile2D(const std::string& name,
const std::initializer_list<double>& xbinedges,
const std::initializer_list<double>& ybinedges,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
/// Book a 2D profile histogram with binning from a reference scatter.
Profile2DPtr bookProfile2D(const std::string& name,
const Scatter3D& refscatter,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
/// Book a 2D profile histogram, using the binnings in the reference data histogram.
Profile2DPtr bookProfile2D(const std::string& name,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
/// Book a 2D profile histogram, using the binnings in the reference data histogram.
///
/// The paper, dataset and x/y-axis IDs will be used to build the histo name in the HepData standard way.
Profile2DPtr bookProfile2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="",
const std::string& ztitle="");
//@}
/// @name 2D scatter booking
//@{
/// @brief Book a 2-dimensional data point set with the given name.
///
/// @note Unlike histogram booking, scatter booking by default makes no
/// attempt to use reference data to pre-fill the data object. If you want
/// this, which is sometimes useful e.g. when the x-position is not really
/// meaningful and can't be extracted from the data, then set the @a
/// copy_pts parameter to true. This creates points to match the reference
/// data's x values and errors, but with the y values and errors zeroed...
/// assuming that there is a reference histo with the same name: if there
/// isn't, an exception will be thrown.
Scatter2DPtr bookScatter2D(const std::string& name,
bool copy_pts=false,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// @brief Book a 2-dimensional data point set, using the binnings in the reference data histogram.
///
/// The paper, dataset and x/y-axis IDs will be used to build the histo name in the HepData standard way.
///
/// @note Unlike histogram booking, scatter booking by default makes no
/// attempt to use reference data to pre-fill the data object. If you want
/// this, which is sometimes useful e.g. when the x-position is not really
/// meaningful and can't be extracted from the data, then set the @a
/// copy_pts parameter to true. This creates points to match the reference
/// data's x values and errors, but with the y values and errors zeroed.
Scatter2DPtr bookScatter2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
bool copy_pts=false,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// @brief Book a 2-dimensional data point set with equally spaced x-points in a range.
///
/// The y values and errors will be set to 0.
Scatter2DPtr bookScatter2D(const std::string& name,
size_t npts, double lower, double upper,
const std::string& title="",
const std::string& xtitle="",
const std::string& ytitle="");
/// @brief Book a 2-dimensional data point set based on provided contiguous "bin edges".
///
/// The y values and errors will be set to 0.
Scatter2DPtr bookScatter2D(const std::string& hname,
const std::vector<double>& binedges,
const std::string& title,
const std::string& xtitle,
const std::string& ytitle);
/// Book a 2-dimensional data point set with x-points from an existing scatter and a new path.
Scatter2DPtr bookScatter2D(const Scatter2DPtr scPtr,
const std::string& path, const std::string& title = "",
const std::string& xtitle = "", const std::string& ytitle = "" );
//@}
public:
/// @name accessing options for this Analysis instance.
//@{
/// Get an option for this analysis instance as a string.
std::string getOption(std::string optname) {
if ( _options.find(optname) != _options.end() )
return _options.find(optname)->second;
return "";
}
/// Get an option for this analysis instance converted to a
/// specific type (given by the specified @a def value).
template<typename T>
T getOption(std::string optname, T def) {
if (_options.find(optname) == _options.end()) return def;
std::stringstream ss;
ss << _options.find(optname)->second;
T ret;
ss >> ret;
return ret;
}
//@}
/// @brief Book a CentralityProjection
///
/// Using a SingleValueProjection, @a proj, giving the value of an
/// experimental observable to be used as a centrality estimator,
/// book a CentralityProjection based on the experimentally
/// measured pecentiles of this observable (as given by the
/// reference data for the @a calHistName histogram in the @a
/// calAnaName analysis. If a preloaded file with the output of a
/// run using the @a calAnaName analysis contains a valid
/// generated @a calHistName histogram, it will be used as an
/// optional percentile binning. Also if this preloaded file
/// contains a histogram with the name @a calHistName with an
/// appended "_IMP" This histogram will be used to add an optional
/// centrality percentile based on the generated impact
/// parameter. If @increasing is true, a low (high) value of @proj
/// is assumed to correspond to a more peripheral (central) event.
const CentralityProjection&
declareCentrality(const SingleValueProjection &proj,
string calAnaName, string calHistName,
const string projName, bool increasing = false);
/// @brief Book a Pecentile wrapper around AnalysisObjects.
///
/// Based on a previously registered CentralityProjection named @a
/// projName book one AnalysisObject for each @a centralityBin and
/// name them according to the corresponding code in the @a ref
/// vector.
template <class T>
Percentile<T> bookPercentile(string projName,
vector<pair<float, float> > centralityBins,
vector<tuple<int, int, int> > ref) {
typedef typename ReferenceTraits<T>::RefT RefT;
Percentile<T> pctl(this, projName);
const int nCent = centralityBins.size();
for (int iCent = 0; iCent < nCent; ++iCent) {
const string axisCode = makeAxisCode(std::get<0>(ref[iCent]),
std::get<1>(ref[iCent]),
std::get<2>(ref[iCent]));
const RefT & refscatter = refData<RefT>(axisCode);
shared_ptr<T> ao = addOrGetCompatAO(make_shared<T>(refscatter, histoPath(axisCode)));
CounterPtr cnt =
addOrGetCompatAO(make_shared<Counter>(histoPath("TMP/COUNTER/" + axisCode)));
pctl.add(ao, cnt, centralityBins[iCent]);
}
return pctl;
}
/// @brief Book Pecentile wrappers around AnalysisObjects.
///
/// Based on a previously registered CentralityProjection named @a
/// projName book one (or several) AnalysisObject(s) named
/// according to @a ref where the x-axis will be filled according
/// to the percentile output(s) of the @projName.
template <class T>
PercentileXaxis<T> bookPercentileXaxis(string projName,
tuple<int, int, int> ref) {
typedef typename ReferenceTraits<T>::RefT RefT;
PercentileXaxis<T> pctl(this, projName);
const string axisCode = makeAxisCode(std::get<0>(ref),
std::get<1>(ref),
std::get<2>(ref));
const RefT & refscatter = refData<RefT>(axisCode);
shared_ptr<T> ao = addOrGetCompatAO(make_shared<T>(refscatter, histoPath(axisCode)));
pctl.add(proj, ao, make_shared<Counter>());
return pctl;
}
/// @name Analysis object manipulation
/// @todo Should really be protected: only public to keep BinnedHistogram happy for now...
//@{
/// Multiplicatively scale the given counter, @a cnt, by factor @s factor.
void scale(CounterPtr cnt, double factor);
/// Multiplicatively scale the given counters, @a cnts, by factor @s factor.
/// @note Constness intentional, if weird, to allow passing rvalue refs of smart ptrs (argh)
/// @todo Use SFINAE for a generic iterable of CounterPtrs
void scale(const std::vector<CounterPtr>& cnts, double factor) {
for (auto& c : cnts) scale(c, factor);
}
/// @todo YUCK!
template <std::size_t array_size>
void scale(const CounterPtr (&cnts)[array_size], double factor) {
// for (size_t i = 0; i < std::extent<decltype(cnts)>::value; ++i) scale(cnts[i], factor);
for (auto& c : cnts) scale(c, factor);
}
/// Normalize the given histogram, @a histo, to area = @a norm.
void normalize(Histo1DPtr histo, double norm=1.0, bool includeoverflows=true);
/// Normalize the given histograms, @a histos, to area = @a norm.
/// @note Constness intentional, if weird, to allow passing rvalue refs of smart ptrs (argh)
/// @todo Use SFINAE for a generic iterable of Histo1DPtrs
void normalize(const std::vector<Histo1DPtr>& histos, double norm=1.0, bool includeoverflows=true) {
for (auto& h : histos) normalize(h, norm, includeoverflows);
}
/// @todo YUCK!
template <std::size_t array_size>
void normalize(const Histo1DPtr (&histos)[array_size], double norm=1.0, bool includeoverflows=true) {
for (auto& h : histos) normalize(h, norm, includeoverflows);
}
/// Multiplicatively scale the given histogram, @a histo, by factor @s factor.
void scale(Histo1DPtr histo, double factor);
/// Multiplicatively scale the given histograms, @a histos, by factor @s factor.
/// @note Constness intentional, if weird, to allow passing rvalue refs of smart ptrs (argh)
/// @todo Use SFINAE for a generic iterable of Histo1DPtrs
void scale(const std::vector<Histo1DPtr>& histos, double factor) {
for (auto& h : histos) scale(h, factor);
}
/// @todo YUCK!
template <std::size_t array_size>
void scale(const Histo1DPtr (&histos)[array_size], double factor) {
for (auto& h : histos) scale(h, factor);
}
/// Normalize the given histogram, @a histo, to area = @a norm.
void normalize(Histo2DPtr histo, double norm=1.0, bool includeoverflows=true);
/// Normalize the given histograms, @a histos, to area = @a norm.
/// @note Constness intentional, if weird, to allow passing rvalue refs of smart ptrs (argh)
/// @todo Use SFINAE for a generic iterable of Histo2DPtrs
void normalize(const std::vector<Histo2DPtr>& histos, double norm=1.0, bool includeoverflows=true) {
for (auto& h : histos) normalize(h, norm, includeoverflows);
}
/// @todo YUCK!
template <std::size_t array_size>
void normalize(const Histo2DPtr (&histos)[array_size], double norm=1.0, bool includeoverflows=true) {
for (auto& h : histos) normalize(h, norm, includeoverflows);
}
/// Multiplicatively scale the given histogram, @a histo, by factor @s factor.
void scale(Histo2DPtr histo, double factor);
/// Multiplicatively scale the given histograms, @a histos, by factor @s factor.
/// @note Constness intentional, if weird, to allow passing rvalue refs of smart ptrs (argh)
/// @todo Use SFINAE for a generic iterable of Histo2DPtrs
void scale(const std::vector<Histo2DPtr>& histos, double factor) {
for (auto& h : histos) scale(h, factor);
}
/// @todo YUCK!
template <std::size_t array_size>
void scale(const Histo2DPtr (&histos)[array_size], double factor) {
for (auto& h : histos) scale(h, factor);
}
/// Helper for counter division.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void divide(CounterPtr c1, CounterPtr c2, Scatter1DPtr s) const;
/// Helper for histogram division with raw YODA objects.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void divide(const YODA::Counter& c1, const YODA::Counter& c2, Scatter1DPtr s) const;
/// Helper for histogram division.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void divide(Histo1DPtr h1, Histo1DPtr h2, Scatter2DPtr s) const;
/// Helper for histogram division with raw YODA objects.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void divide(const YODA::Histo1D& h1, const YODA::Histo1D& h2, Scatter2DPtr s) const;
/// Helper for profile histogram division.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void divide(Profile1DPtr p1, Profile1DPtr p2, Scatter2DPtr s) const;
/// Helper for profile histogram division with raw YODA objects.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void divide(const YODA::Profile1D& p1, const YODA::Profile1D& p2, Scatter2DPtr s) const;
/// Helper for 2D histogram division.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void divide(Histo2DPtr h1, Histo2DPtr h2, Scatter3DPtr s) const;
/// Helper for 2D histogram division with raw YODA objects.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void divide(const YODA::Histo2D& h1, const YODA::Histo2D& h2, Scatter3DPtr s) const;
/// Helper for 2D profile histogram division.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void divide(Profile2DPtr p1, Profile2DPtr p2, Scatter3DPtr s) const;
/// Helper for 2D profile histogram division with raw YODA objects
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void divide(const YODA::Profile2D& p1, const YODA::Profile2D& p2, Scatter3DPtr s) const;
/// Helper for histogram efficiency calculation.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void efficiency(Histo1DPtr h1, Histo1DPtr h2, Scatter2DPtr s) const;
/// Helper for histogram efficiency calculation.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void efficiency(const YODA::Histo1D& h1, const YODA::Histo1D& h2, Scatter2DPtr s) const;
/// Helper for histogram asymmetry calculation.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void asymm(Histo1DPtr h1, Histo1DPtr h2, Scatter2DPtr s) const;
/// Helper for histogram asymmetry calculation.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void asymm(const YODA::Histo1D& h1, const YODA::Histo1D& h2, Scatter2DPtr s) const;
/// Helper for converting a differential histo to an integral one.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void integrate(Histo1DPtr h, Scatter2DPtr s) const;
/// Helper for converting a differential histo to an integral one.
///
/// @note Assigns to the (already registered) output scatter, @a s. Preserves the path information of the target.
void integrate(const Histo1D& h, Scatter2DPtr s) const;
//@}
public:
/// List of registered analysis data objects
const vector<AnalysisObjectPtr>& analysisObjects() const {
return _analysisobjects;
}
protected:
/// @name Data object registration, retrieval, and removal
//@{
/// Register a data object in the histogram system
void addAnalysisObject(AnalysisObjectPtr ao);
/// Register a data object in the system and return its pointer,
/// or, if an object of the same path is already there, check if it
/// is compatible (eg. same type and same binning) and return that
/// object instead. Emits a warning if an incompatible object with
/// the same name is found and replcaces that with the given data
/// object.
template <typename AO=YODA::AnalysisObject>
std::shared_ptr<AO> addOrGetCompatAO(std::shared_ptr<AO> aonew) {
foreach (const AnalysisObjectPtr& ao, analysisObjects()) {
if ( ao->path() == aonew->path() ) {
std::shared_ptr<AO> aoold = dynamic_pointer_cast<AO>(ao);
if ( aoold && bookingCompatible(aonew, aoold) ) {
MSG_TRACE("Bound pre-existing data object " << aonew->path()
<< " for " << name());
return aoold;
} else {
MSG_WARNING("Found incompatible pre-existing data object with same path "
<< aonew->path() << " for " << name());
}
}
}
MSG_TRACE("Registered " << aonew->annotation("Type") << " " << aonew->path()
<< " for " << name());
addAnalysisObject(aonew);
return aonew;
}
/// Get a data object from the histogram system
template <typename AO=YODA::AnalysisObject>
const std::shared_ptr<AO> getAnalysisObject(const std::string& name) const {
foreach (const AnalysisObjectPtr& ao, analysisObjects()) {
if (ao->path() == histoPath(name)) return dynamic_pointer_cast<AO>(ao);
}
throw LookupError("Data object " + histoPath(name) + " not found");
}
/// Get a data object from the histogram system (non-const)
template <typename AO=YODA::AnalysisObject>
std::shared_ptr<AO> getAnalysisObject(const std::string& name) {
foreach (const AnalysisObjectPtr& ao, analysisObjects()) {
if (ao->path() == histoPath(name)) return dynamic_pointer_cast<AO>(ao);
}
throw LookupError("Data object " + histoPath(name) + " not found");
}
/// Unregister a data object from the histogram system (by name)
void removeAnalysisObject(const std::string& path);
/// Unregister a data object from the histogram system (by pointer)
void removeAnalysisObject(AnalysisObjectPtr ao);
/// Get all data object from the AnalysisHandler.
vector<AnalysisObjectPtr> getAllData(bool includeorphans) const;
/// Get a data object from another analysis (e.g. preloaded
/// calibration histogram).
/// Get a data object from the histogram system (non-const)
template <typename AO=YODA::AnalysisObject>
std::shared_ptr<AO> getAnalysisObject(const std::string & ananame,
const std::string& name) {
std::string path = "/" + ananame + "/" + name;
for ( AnalysisObjectPtr ao : getAllData(true) ) {
if ( ao->path() == path )
return dynamic_pointer_cast<AO>(ao);
}
return std::shared_ptr<AO>();
}
/// Get a named Histo1D object from the histogram system
const Histo1DPtr getHisto1D(const std::string& name) const {
return getAnalysisObject<Histo1D>(name);
}
/// Get a named Histo1D object from the histogram system (non-const)
Histo1DPtr getHisto1D(const std::string& name) {
return getAnalysisObject<Histo1D>(name);
}
/// Get a Histo1D object from the histogram system by axis ID codes (non-const)
const Histo1DPtr getHisto1D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const {
return getAnalysisObject<Histo1D>(makeAxisCode(datasetId, xAxisId, yAxisId));
}
/// Get a Histo1D object from the histogram system by axis ID codes (non-const)
Histo1DPtr getHisto1D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) {
return getAnalysisObject<Histo1D>(makeAxisCode(datasetId, xAxisId, yAxisId));
}
/// Get a named Histo2D object from the histogram system
const Histo2DPtr getHisto2D(const std::string& name) const {
return getAnalysisObject<Histo2D>(name);
}
/// Get a named Histo2D object from the histogram system (non-const)
Histo2DPtr getHisto2D(const std::string& name) {
return getAnalysisObject<Histo2D>(name);
}
/// Get a Histo2D object from the histogram system by axis ID codes (non-const)
const Histo2DPtr getHisto2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const {
return getAnalysisObject<Histo2D>(makeAxisCode(datasetId, xAxisId, yAxisId));
}
/// Get a Histo2D object from the histogram system by axis ID codes (non-const)
Histo2DPtr getHisto2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) {
return getAnalysisObject<Histo2D>(makeAxisCode(datasetId, xAxisId, yAxisId));
}
/// Get a named Profile1D object from the histogram system
const Profile1DPtr getProfile1D(const std::string& name) const {
return getAnalysisObject<Profile1D>(name);
}
/// Get a named Profile1D object from the histogram system (non-const)
Profile1DPtr getProfile1D(const std::string& name) {
return getAnalysisObject<Profile1D>(name);
}
/// Get a Profile1D object from the histogram system by axis ID codes (non-const)
const Profile1DPtr getProfile1D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const {
return getAnalysisObject<Profile1D>(makeAxisCode(datasetId, xAxisId, yAxisId));
}
/// Get a Profile1D object from the histogram system by axis ID codes (non-const)
Profile1DPtr getProfile1D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) {
return getAnalysisObject<Profile1D>(makeAxisCode(datasetId, xAxisId, yAxisId));
}
/// Get a named Profile2D object from the histogram system
const Profile2DPtr getProfile2D(const std::string& name) const {
return getAnalysisObject<Profile2D>(name);
}
/// Get a named Profile2D object from the histogram system (non-const)
Profile2DPtr getProfile2D(const std::string& name) {
return getAnalysisObject<Profile2D>(name);
}
/// Get a Profile2D object from the histogram system by axis ID codes (non-const)
const Profile2DPtr getProfile2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const {
return getAnalysisObject<Profile2D>(makeAxisCode(datasetId, xAxisId, yAxisId));
}
/// Get a Profile2D object from the histogram system by axis ID codes (non-const)
Profile2DPtr getProfile2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) {
return getAnalysisObject<Profile2D>(makeAxisCode(datasetId, xAxisId, yAxisId));
}
/// Get a named Scatter2D object from the histogram system
const Scatter2DPtr getScatter2D(const std::string& name) const {
return getAnalysisObject<Scatter2D>(name);
}
/// Get a named Scatter2D object from the histogram system (non-const)
Scatter2DPtr getScatter2D(const std::string& name) {
return getAnalysisObject<Scatter2D>(name);
}
/// Get a Scatter2D object from the histogram system by axis ID codes (non-const)
const Scatter2DPtr getScatter2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const {
return getAnalysisObject<Scatter2D>(makeAxisCode(datasetId, xAxisId, yAxisId));
}
/// Get a Scatter2D object from the histogram system by axis ID codes (non-const)
Scatter2DPtr getScatter2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) {
return getAnalysisObject<Scatter2D>(makeAxisCode(datasetId, xAxisId, yAxisId));
}
//@}
private:
/// Name passed to constructor (used to find .info analysis data file, and as a fallback)
string _defaultname;
/// Pointer to analysis metadata object
unique_ptr<AnalysisInfo> _info;
/// Storage of all plot objects
/// @todo Make this a map for fast lookup by path?
vector<AnalysisObjectPtr> _analysisobjects;
/// @name Cross-section variables
//@{
double _crossSection;
bool _gotCrossSection;
//@}
/// The controlling AnalysisHandler object.
AnalysisHandler* _analysishandler;
/// Collection of cached refdata to speed up many autobookings: the
/// reference data file should only be read once.
mutable std::map<std::string, AnalysisObjectPtr> _refdata;
/// Options the (this instance of) the analysis
map<string, string> _options;
/// The string of options.
string _optstring;
private:
/// @name Utility functions
//@{
/// Get the reference data for this paper and cache it.
void _cacheRefData() const;
//@}
/// The assignment operator is private and must never be called.
/// In fact, it should not even be implemented.
Analysis& operator=(const Analysis&);
};
}
// Include definition of analysis plugin system so that analyses automatically see it when including Analysis.hh
#include "Rivet/AnalysisBuilder.hh"
/// @def DECLARE_RIVET_PLUGIN
/// Preprocessor define to prettify the global-object plugin hook mechanism.
#define DECLARE_RIVET_PLUGIN(clsname) Rivet::AnalysisBuilder<clsname> plugin_ ## clsname
/// @def DECLARE_ALIASED_RIVET_PLUGIN
/// Preprocessor define to prettify the global-object plugin hook mechanism, with an extra alias name for this analysis.
// #define DECLARE_ALIASED_RIVET_PLUGIN(clsname, alias) Rivet::AnalysisBuilder<clsname> plugin_ ## clsname ## ( ## #alias ## )
#define DECLARE_ALIASED_RIVET_PLUGIN(clsname, alias) DECLARE_RIVET_PLUGIN(clsname)( #alias )
/// @def DEFAULT_RIVET_ANALYSIS_CONSTRUCTOR
/// Preprocessor define to prettify the manky constructor with name string argument
#define DEFAULT_RIVET_ANALYSIS_CONSTRUCTOR(clsname) clsname() : Analysis(# clsname) {}
/// @def DEFAULT_RIVET_ANALYSIS_CTOR
/// Slight abbreviation for DEFAULT_RIVET_ANALYSIS_CONSTRUCTOR
#define DEFAULT_RIVET_ANALYSIS_CTOR(clsname) DEFAULT_RIVET_ANALYSIS_CONSTRUCTOR(clsname)
#endif
diff --git a/include/Rivet/AnalysisHandler.hh b/include/Rivet/AnalysisHandler.hh
--- a/include/Rivet/AnalysisHandler.hh
+++ b/include/Rivet/AnalysisHandler.hh
@@ -1,316 +1,315 @@
// -*- C++ -*-
#ifndef RIVET_RivetHandler_HH
#define RIVET_RivetHandler_HH
#include "Rivet/Config/RivetCommon.hh"
#include "Rivet/Particle.hh"
#include "Rivet/AnalysisLoader.hh"
#include "Rivet/Tools/RivetYODA.hh"
namespace Rivet {
// Forward declaration and smart pointer for Analysis
class Analysis;
typedef std::shared_ptr<Analysis> AnaHandle;
// Needed to make smart pointers compare equivalent in the STL set
struct CmpAnaHandle {
bool operator() (const AnaHandle& a, const AnaHandle& b) const {
return a.get() < b.get();
}
};
/// A class which handles a number of analysis objects to be applied to
/// generated events. An {@link Analysis}' AnalysisHandler is also responsible
/// for handling the final writing-out of histograms.
class AnalysisHandler {
public:
/// @name Constructors and destructors. */
//@{
/// Preferred constructor, with optional run name.
AnalysisHandler(const string& runname="");
/// @brief Destructor
/// The destructor is not virtual, as this class should not be inherited from.
~AnalysisHandler();
//@}
private:
/// Get a logger object.
Log& getLog() const;
public:
/// @name Run properties
//@{
/// Get the name of this run.
string runName() const { return _runname; }
/// Get the number of events seen. Should only really be used by external
/// steering code or analyses in the finalize phase.
size_t numEvents() const { return _eventcounter.numEntries(); }
/// @brief Access the sum of the event weights seen
///
/// This is the weighted equivalent of the number of events. It should only
/// be used by external steering code or analyses in the finalize phase.
double sumW() const { return _eventcounter.sumW(); }
/// Access to the sum of squared-weights
double sumW2() const { return _eventcounter.sumW2(); }
/// @brief Compatibility alias for sumOfWeights
///
/// @deprecated Prefer sumW
double sumOfWeights() const { return sumW(); }
/// @brief Set the sum of weights
///
/// This is useful if Rivet is steered externally and
/// the analyses are run for a sub-contribution of the events
/// (but of course have to be normalised to the total sum of weights)
///
/// @todo What about the sumW2 term? That needs to be set coherently. Need a
/// new version, with all three N,sumW,sumW2 numbers (or a counter)
/// supplied.
///
/// @deprecated Weight sums are no longer tracked this way...
void setSumOfWeights(const double& sum) {
//_sumOfWeights = sum;
throw Error("Can't set sum of weights independently, since it's now tracked by a Counter. "
"Please contact the Rivet authors if you need this.");
}
/// Is cross-section information required by at least one child analysis?
/// @deprecated Should no-longer be an issue: does any generator not write the cross-section?
bool needCrossSection() const;
/// Whether the handler knows about a cross-section.
/// @deprecated Should no-longer be an issue: does any generator not write the cross-section?
bool hasCrossSection() const;
/// Get the cross-section known to the handler.
double crossSection() const { return _xs; }
/// Set the cross-section for the process being generated.
- /// @todo What about the xsec uncertainty? Add a second, optional argument?
- AnalysisHandler& setCrossSection(double xs);
+ AnalysisHandler& setCrossSection(double xs, double xserr=0);
/// Set the beam particles for this run
AnalysisHandler& setRunBeams(const ParticlePair& beams) {
_beams = beams;
MSG_DEBUG("Setting run beams = " << beams << " @ " << sqrtS()/GeV << " GeV");
return *this;
}
/// Get the beam particles for this run, usually determined from the first event.
const ParticlePair& beams() const { return _beams; }
/// Get beam IDs for this run, usually determined from the first event.
/// @deprecated Use standalone beamIds(ah.beams()), to clean AH interface
PdgIdPair beamIds() const;
/// Get energy for this run, usually determined from the first event.
/// @deprecated Use standalone sqrtS(ah.beams()), to clean AH interface
double sqrtS() const;
/// Setter for _ignoreBeams
void setIgnoreBeams(bool ignore=true);
//@}
/// @name Handle analyses
//@{
/// Get a list of the currently registered analyses' names.
std::vector<std::string> analysisNames() const;
/// Get the collection of currently registered analyses.
const std::set<AnaHandle, CmpAnaHandle>& analyses() const {
return _analyses;
}
/// Get a registered analysis by name.
const AnaHandle analysis(const std::string& analysisname) const;
/// Add an analysis to the run list by object
AnalysisHandler& addAnalysis(Analysis* analysis);
/// @brief Add an analysis to the run list using its name.
///
/// The actual Analysis to be used will be obtained via
/// AnalysisLoader::getAnalysis(string). If no matching analysis is found,
/// no analysis is added (i.e. the null pointer is checked and discarded.
AnalysisHandler& addAnalysis(const std::string& analysisname);
/// @brief Add an analysis with a map of analysis options.
AnalysisHandler& addAnalysis(const std::string& analysisname, std::map<string, string> pars);
/// @brief Add analyses to the run list using their names.
///
/// The actual {@link Analysis}' to be used will be obtained via
/// AnalysisHandler::addAnalysis(string), which in turn uses
/// AnalysisLoader::getAnalysis(string). If no matching analysis is found
/// for a given name, no analysis is added, but also no error is thrown.
AnalysisHandler& addAnalyses(const std::vector<std::string>& analysisnames);
/// Remove an analysis from the run list using its name.
AnalysisHandler& removeAnalysis(const std::string& analysisname);
/// Remove analyses from the run list using their names.
AnalysisHandler& removeAnalyses(const std::vector<std::string>& analysisnames);
//@}
/// @name Main init/execute/finalise
//@{
/// Initialize a run, with the run beams taken from the example event.
void init(const GenEvent& event);
/// @brief Analyze the given \a event by reference.
///
/// This function will call the AnalysisBase::analyze() function of all
/// included analysis objects.
void analyze(const GenEvent& event);
/// @brief Analyze the given \a event by pointer.
///
/// This function will call the AnalysisBase::analyze() function of all
/// included analysis objects, after checking the event pointer validity.
void analyze(const GenEvent* event);
/// Finalize a run. This function calls the AnalysisBase::finalize()
/// functions of all included analysis objects.
void finalize();
//@}
/// @name Histogram / data object access
//@{
/// Add a vector of analysis objects to the current state.
void addData(const std::vector<AnalysisObjectPtr>& aos);
/// Read analysis plots into the histo collection (via addData) from the named file.
void readData(const std::string& filename);
/// Get all analyses' plots as a vector of analysis objects.
std::vector<AnalysisObjectPtr> getData(bool includeorphans = false,
bool includetmps = false) const;
/// Write all analyses' plots (via getData) to the named file.
void writeData(const std::string& filename) const;
/// Tell Rivet to dump intermediate result to a file named @a
/// dumpfile every @a period'th event. If @period is not positive,
/// no dumping will be done.
void dump(string dumpfile, int period) {
_dumpPeriod = period;
_dumpFile = dumpfile;
}
/// Take the vector of yoda files and merge them together using
/// the cross section and weight information provided in each
/// file. Each file in @a aofiles is assumed to have been produced
/// by Rivet. By default the files are assumed to contain
/// different processes (or the same processs but mutually
/// exclusive cuts), but if @a equiv if ture, the files are
/// assumed to contain output of completely equivalent (but
/// statistically independent) Rivet runs. The corresponding
/// analyses will be loaded and their analysis objects will be
/// filled with the merged result. finalize() will be run on each
/// relevant anslysis. The resulting YODA file can then be rwitten
/// out by writeData(). If delopts is non-empty, it is assumed to
/// contain names different options to be merged into the same
/// analysis objects.
void mergeYodas(const vector<string> & aofiles,
const vector<string> & delopts = vector<string>(),
bool equiv = false);
/// Helper function to strip specific options from data object paths.
void stripOptions(AnalysisObjectPtr ao,
const vector<string> & delopts) const;
//@}
private:
/// The collection of Analysis objects to be used.
set<AnaHandle, CmpAnaHandle> _analyses;
/// A vector of pre-loaded object which do not have a valid
/// Analysis plugged in.
vector<AnalysisObjectPtr> _orphanedPreloads;
/// A vector containing copies of analysis objects after
/// finalize() has been run.
vector<AnalysisObjectPtr> _finalizedAOs;
/// @name Run properties
//@{
/// Run name
std::string _runname;
/// Event counter
Counter _eventcounter;
/// Cross-section known to AH
double _xs, _xserr;
/// Beams used by this run.
ParticlePair _beams;
/// Flag to check if init has been called
bool _initialised;
/// Flag whether input event beams should be ignored in compatibility check
bool _ignoreBeams;
/// Determines how often Rivet runs finalize() and writes the
/// result to a YODA file.
int _dumpPeriod;
/// The name of a YODA file to which Rivet periodically dumps
/// results.
string _dumpFile;
/// Flag to indicate periodic dumping is in progress
bool _dumping;
//@}
private:
/// The assignment operator is private and must never be called.
/// In fact, it should not even be implemented.
AnalysisHandler& operator=(const AnalysisHandler&);
/// The copy constructor is private and must never be called. In
/// fact, it should not even be implemented.
AnalysisHandler(const AnalysisHandler&);
};
}
#endif
diff --git a/include/Rivet/Makefile.am b/include/Rivet/Makefile.am
--- a/include/Rivet/Makefile.am
+++ b/include/Rivet/Makefile.am
@@ -1,187 +1,196 @@
## Internal headers - not to be installed
nobase_dist_noinst_HEADERS =
## Public headers - to be installed
nobase_pkginclude_HEADERS =
## Rivet interface
nobase_pkginclude_HEADERS += \
Rivet.hh \
Run.hh \
Event.hh \
ParticleBase.hh \
Particle.fhh Particle.hh \
Jet.fhh Jet.hh \
Projection.fhh Projection.hh \
ProjectionApplier.hh \
ProjectionHandler.hh \
Analysis.hh \
AnalysisHandler.hh \
AnalysisInfo.hh \
AnalysisBuilder.hh \
AnalysisLoader.hh
## Build config stuff
nobase_pkginclude_HEADERS += \
Config/RivetCommon.hh \
Config/RivetConfig.hh \
Config/BuildOptions.hh
## Projections
nobase_pkginclude_HEADERS += \
Projections/AliceCommon.hh \
Projections/AxesDefinition.hh \
Projections/Beam.hh \
Projections/BeamThrust.hh \
Projections/CentralEtHCM.hh \
Projections/CentralityProjection.hh \
Projections/ChargedFinalState.hh \
Projections/ChargedLeptons.hh \
Projections/ConstLossyFinalState.hh \
Projections/DirectFinalState.hh \
Projections/DISFinalState.hh \
Projections/DISKinematics.hh \
Projections/DISLepton.hh \
Projections/DressedLeptons.hh \
Projections/FastJets.hh \
Projections/PxConePlugin.hh \
Projections/FinalPartons.hh \
Projections/FinalState.hh \
Projections/FoxWolframMoments.hh \
Projections/FParameter.hh \
Projections/GeneratedPercentileProjection.hh \
Projections/HadronicFinalState.hh \
Projections/HeavyHadrons.hh \
Projections/Hemispheres.hh \
Projections/IdentifiedFinalState.hh \
Projections/ImpactParameterProjection.hh \
Projections/IndirectFinalState.hh \
Projections/InitialQuarks.hh \
Projections/InvMassFinalState.hh \
Projections/JetAlg.hh \
Projections/JetShape.hh \
Projections/LeadingParticlesFinalState.hh \
Projections/LossyFinalState.hh \
Projections/MergedFinalState.hh \
Projections/MissingMomentum.hh \
Projections/MixedFinalState.hh \
Projections/NeutralFinalState.hh \
Projections/NonHadronicFinalState.hh \
Projections/NonPromptFinalState.hh \
Projections/ParisiTensor.hh \
Projections/ParticleFinder.hh \
Projections/PartonicTops.hh \
Projections/PercentileProjection.hh \
Projections/PrimaryHadrons.hh \
Projections/PrimaryParticles.hh \
Projections/PromptFinalState.hh \
Projections/SingleValueProjection.hh \
Projections/SmearedParticles.hh \
Projections/SmearedJets.hh \
Projections/SmearedMET.hh \
Projections/Sphericity.hh \
Projections/Spherocity.hh \
Projections/TauFinder.hh \
Projections/Thrust.hh \
Projections/TriggerCDFRun0Run1.hh \
Projections/TriggerCDFRun2.hh \
Projections/TriggerProjection.hh \
Projections/TriggerUA5.hh \
Projections/UnstableFinalState.hh \
Projections/UserCentEstimate.hh \
Projections/VetoedFinalState.hh \
Projections/VisibleFinalState.hh \
Projections/WFinder.hh \
Projections/ZFinder.hh
## Meta-projection convenience headers
nobase_pkginclude_HEADERS += \
Projections/FinalStates.hh \
Projections/Smearing.hh
## Analysis base class headers
# TODO: Move to Rivet/AnalysisTools header dir?
nobase_pkginclude_HEADERS += \
Analyses/MC_Cent_pPb.hh \
Analyses/MC_ParticleAnalysis.hh \
Analyses/MC_JetAnalysis.hh \
Analyses/MC_JetSplittings.hh
## Tools
nobase_pkginclude_HEADERS += \
Tools/AliceCommon.hh \
Tools/AtlasCommon.hh \
Tools/BeamConstraint.hh \
Tools/BinnedHistogram.hh \
Tools/CentralityBinner.hh \
Tools/Cmp.fhh \
Tools/Cmp.hh \
Tools/Correlators.hh \
Tools/Cutflow.hh \
Tools/Cuts.fhh \
Tools/Cuts.hh \
Tools/Exceptions.hh \
Tools/JetUtils.hh \
Tools/Logging.hh \
Tools/Random.hh \
Tools/ParticleBaseUtils.hh \
Tools/ParticleIdUtils.hh \
Tools/ParticleUtils.hh \
Tools/ParticleName.hh \
Tools/Percentile.hh \
Tools/PrettyPrint.hh \
Tools/RivetPaths.hh \
Tools/RivetSTL.hh \
Tools/RivetFastJet.hh \
Tools/RivetHepMC.hh \
Tools/RivetYODA.hh \
Tools/RivetMT2.hh \
Tools/SmearingFunctions.hh \
Tools/MomentumSmearingFunctions.hh \
Tools/ParticleSmearingFunctions.hh \
Tools/JetSmearingFunctions.hh \
Tools/TypeTraits.hh \
Tools/Utils.hh \
- Tools/Nsubjettiness/AxesDefinition.hh \
- Tools/Nsubjettiness/ExtraRecombiners.hh \
- Tools/Nsubjettiness/MeasureDefinition.hh \
- Tools/Nsubjettiness/Njettiness.hh \
- Tools/Nsubjettiness/NjettinessPlugin.hh \
- Tools/Nsubjettiness/Nsubjettiness.hh \
- Tools/Nsubjettiness/TauComponents.hh \
- Tools/Nsubjettiness/XConePlugin.hh
+ Tools/fjcontrib/AxesDefinition.hh \
+ Tools/fjcontrib/BottomUpSoftDrop.hh \
+ Tools/fjcontrib/EnergyCorrelator.hh \
+ Tools/fjcontrib/ExtraRecombiners.hh \
+ Tools/fjcontrib/IteratedSoftDrop.hh \
+ Tools/fjcontrib/MeasureDefinition.hh \
+ Tools/fjcontrib/ModifiedMassDropTagger.hh \
+ Tools/fjcontrib/Njettiness.hh \
+ Tools/fjcontrib/NjettinessPlugin.hh \
+ Tools/fjcontrib/Nsubjettiness.hh \
+ Tools/fjcontrib/Recluster.hh \
+ Tools/fjcontrib/RecursiveSoftDrop.hh \
+ Tools/fjcontrib/RecursiveSymmetryCutBase.hh \
+ Tools/fjcontrib/SoftDrop.hh \
+ Tools/fjcontrib/TauComponents.hh \
+ Tools/fjcontrib/XConePlugin.hh
+
nobase_dist_noinst_HEADERS += \
Tools/osdir.hh
## Maths
nobase_pkginclude_HEADERS += \
Math/Matrices.hh \
Math/Vector3.hh \
Math/VectorN.hh \
Math/MatrixN.hh \
Math/MatrixDiag.hh \
Math/MathHeader.hh \
Math/Vectors.hh \
Math/LorentzTrans.hh \
Math/Matrix3.hh \
Math/MathUtils.hh \
Math/Vector4.hh \
Math/Math.hh \
Math/Units.hh \
Math/Constants.hh \
Math/eigen/util.h \
Math/eigen/regressioninternal.h \
Math/eigen/regression.h \
Math/eigen/vector.h \
Math/eigen/ludecompositionbase.h \
Math/eigen/ludecomposition.h \
Math/eigen/linearsolver.h \
Math/eigen/linearsolverbase.h \
Math/eigen/matrix.h \
Math/eigen/vectorbase.h \
Math/eigen/projective.h \
Math/eigen/matrixbase.h
diff --git a/include/Rivet/Math/MathUtils.hh b/include/Rivet/Math/MathUtils.hh
--- a/include/Rivet/Math/MathUtils.hh
+++ b/include/Rivet/Math/MathUtils.hh
@@ -1,626 +1,627 @@
// -*- C++ -*-
#ifndef RIVET_MathUtils_HH
#define RIVET_MathUtils_HH
#include "Rivet/Math/MathHeader.hh"
#include <type_traits>
#include <cassert>
namespace Rivet {
/// @name Comparison functions for safe (floating point) equality tests
//@{
/// @brief Compare a number to zero
///
/// This version for floating point types has a degree of fuzziness expressed
/// by the absolute @a tolerance parameter, for floating point safety.
template <typename NUM>
inline typename std::enable_if<std::is_floating_point<NUM>::value, bool>::type
isZero(NUM val, double tolerance=1e-8) {
return fabs(val) < tolerance;
}
/// @brief Compare a number to zero
///
/// SFINAE template specialisation for integers, since there is no FP
/// precision issue.
template <typename NUM>
inline typename std::enable_if<std::is_integral<NUM>::value, bool>::type
isZero(NUM val, double=1e-5) { //< NB. unused tolerance parameter for ints, still needs a default value!
return val == 0;
}
/// @brief Compare two numbers for equality with a degree of fuzziness
///
/// This version for floating point types (if any argument is FP) has a degree
/// of fuzziness expressed by the fractional @a tolerance parameter, for
/// floating point safety.
template <typename N1, typename N2>
inline typename std::enable_if<
std::is_arithmetic<N1>::value && std::is_arithmetic<N2>::value &&
(std::is_floating_point<N1>::value || std::is_floating_point<N2>::value), bool>::type
fuzzyEquals(N1 a, N2 b, double tolerance=1e-5) {
const double absavg = (std::abs(a) + std::abs(b))/2.0;
const double absdiff = std::abs(a - b);
const bool rtn = (isZero(a) && isZero(b)) || absdiff < tolerance*absavg;
return rtn;
}
/// @brief Compare two numbers for equality with a degree of fuzziness
///
/// Simpler SFINAE template specialisation for integers, since there is no FP
/// precision issue.
template <typename N1, typename N2>
inline typename std::enable_if<
std::is_integral<N1>::value && std::is_integral<N2>::value, bool>::type
fuzzyEquals(N1 a, N2 b, double) { //< NB. unused tolerance parameter for ints, still needs a default value!
return a == b;
}
/// @brief Compare two numbers for >= with a degree of fuzziness
///
/// The @a tolerance parameter on the equality test is as for @c fuzzyEquals.
template <typename N1, typename N2>
inline typename std::enable_if<
std::is_arithmetic<N1>::value && std::is_arithmetic<N2>::value, bool>::type
fuzzyGtrEquals(N1 a, N2 b, double tolerance=1e-5) {
return a > b || fuzzyEquals(a, b, tolerance);
}
/// @brief Compare two floating point numbers for <= with a degree of fuzziness
///
/// The @a tolerance parameter on the equality test is as for @c fuzzyEquals.
template <typename N1, typename N2>
inline typename std::enable_if<
std::is_arithmetic<N1>::value && std::is_arithmetic<N2>::value, bool>::type
fuzzyLessEquals(N1 a, N2 b, double tolerance=1e-5) {
return a < b || fuzzyEquals(a, b, tolerance);
}
//@}
/// @name Ranges and intervals
//@{
/// Represents whether an interval is open (non-inclusive) or closed (inclusive).
///
/// For example, the interval \f$ [0, \pi) \f$ is closed (an inclusive
/// boundary) at 0, and open (a non-inclusive boundary) at \f$ \pi \f$.
enum RangeBoundary { OPEN=0, SOFT=0, CLOSED=1, HARD=1 };
/// @brief Determine if @a value is in the range @a low to @a high, for floating point numbers
///
/// Interval boundary types are defined by @a lowbound and @a highbound.
template <typename N1, typename N2, typename N3>
inline typename std::enable_if<
std::is_arithmetic<N1>::value && std::is_arithmetic<N2>::value && std::is_arithmetic<N3>::value, bool>::type
inRange(N1 value, N2 low, N3 high,
RangeBoundary lowbound=CLOSED, RangeBoundary highbound=OPEN) {
if (lowbound == OPEN && highbound == OPEN) {
return (value > low && value < high);
} else if (lowbound == OPEN && highbound == CLOSED) {
return (value > low && value <= high);
} else if (lowbound == CLOSED && highbound == OPEN) {
return (value >= low && value < high);
} else { // if (lowbound == CLOSED && highbound == CLOSED) {
return (value >= low && value <= high);
}
}
/// @brief Determine if @a value is in the range @a low to @a high, for floating point numbers
///
/// Interval boundary types are defined by @a lowbound and @a highbound.
/// Closed intervals are compared fuzzily.
template <typename N1, typename N2, typename N3>
inline typename std::enable_if<
std::is_arithmetic<N1>::value && std::is_arithmetic<N2>::value && std::is_arithmetic<N3>::value, bool>::type
fuzzyInRange(N1 value, N2 low, N3 high,
RangeBoundary lowbound=CLOSED, RangeBoundary highbound=OPEN) {
if (lowbound == OPEN && highbound == OPEN) {
return (value > low && value < high);
} else if (lowbound == OPEN && highbound == CLOSED) {
return (value > low && fuzzyLessEquals(value, high));
} else if (lowbound == CLOSED && highbound == OPEN) {
return (fuzzyGtrEquals(value, low) && value < high);
} else { // if (lowbound == CLOSED && highbound == CLOSED) {
return (fuzzyGtrEquals(value, low) && fuzzyLessEquals(value, high));
}
}
/// Alternative version of inRange which accepts a pair for the range arguments.
template <typename N1, typename N2, typename N3>
inline typename std::enable_if<
std::is_arithmetic<N1>::value && std::is_arithmetic<N2>::value && std::is_arithmetic<N3>::value, bool>::type
inRange(N1 value, pair<N2, N3> lowhigh,
RangeBoundary lowbound=CLOSED, RangeBoundary highbound=OPEN) {
return inRange(value, lowhigh.first, lowhigh.second, lowbound, highbound);
}
// Alternative forms, with snake_case names and boundary types in names rather than as args -- from MCUtils
/// @brief Boolean function to determine if @a value is within the given range
///
/// @note The interval is closed (inclusive) at the low end, and open (exclusive) at the high end.
template <typename N1, typename N2, typename N3>
inline typename std::enable_if<
std::is_arithmetic<N1>::value && std::is_arithmetic<N2>::value && std::is_arithmetic<N3>::value, bool>::type
in_range(N1 val, N2 low, N3 high) {
return inRange(val, low, high, CLOSED, OPEN);
}
/// @brief Boolean function to determine if @a value is within the given range
///
/// @note The interval is closed at both ends.
template <typename N1, typename N2, typename N3>
inline typename std::enable_if<
std::is_arithmetic<N1>::value && std::is_arithmetic<N2>::value && std::is_arithmetic<N3>::value, bool>::type
in_closed_range(N1 val, N2 low, N3 high) {
return inRange(val, low, high, CLOSED, CLOSED);
}
/// @brief Boolean function to determine if @a value is within the given range
///
/// @note The interval is open at both ends.
template <typename N1, typename N2, typename N3>
inline typename std::enable_if<
std::is_arithmetic<N1>::value && std::is_arithmetic<N2>::value && std::is_arithmetic<N3>::value, bool>::type
in_open_range(N1 val, N2 low, N3 high) {
return inRange(val, low, high, OPEN, OPEN);
}
/// @todo Add pair-based versions of the named range-boundary functions
//@}
/// @name Miscellaneous numerical helpers
//@{
/// Named number-type squaring operation.
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, NUM>::type
sqr(NUM a) {
return a*a;
}
/// @brief Named number-type addition in quadrature operation.
///
/// @note Result has the sqrt operation applied.
/// @todo When std::common_type can be used, generalise to multiple numeric types with appropriate return type.
// template <typename N1, typename N2>
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, NUM>::type
//std::common_type<N1, N2>::type
add_quad(NUM a, NUM b) {
return sqrt(a*a + b*b);
}
/// Named number-type addition in quadrature operation.
///
/// @note Result has the sqrt operation applied.
/// @todo When std::common_type can be used, generalise to multiple numeric types with appropriate return type.
// template <typename N1, typename N2>
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, NUM>::type
//std::common_type<N1, N2, N3>::type
add_quad(NUM a, NUM b, NUM c) {
return sqrt(a*a + b*b + c*c);
}
/// Return a/b, or @a fail if b = 0
/// @todo When std::common_type can be used, generalise to multiple numeric types with appropriate return type.
inline double safediv(double num, double den, double fail=0.0) {
return (!isZero(den)) ? num/den : fail;
}
/// A more efficient version of pow for raising numbers to integer powers.
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, NUM>::type
intpow(NUM val, unsigned int exp) {
assert(exp >= 0);
if (exp == 0) return (NUM) 1;
else if (exp == 1) return val;
return val * intpow(val, exp-1);
}
/// Find the sign of a number
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, int>::type
sign(NUM val) {
if (isZero(val)) return ZERO;
const int valsign = (val > 0) ? PLUS : MINUS;
return valsign;
}
//@}
/// @name Physics statistical distributions
//@{
/// @brief CDF for the Breit-Wigner distribution
inline double cdfBW(double x, double mu, double gamma) {
// normalize to (0;1) distribution
const double xn = (x - mu)/gamma;
return std::atan(xn)/M_PI + 0.5;
}
/// @brief Inverse CDF for the Breit-Wigner distribution
inline double invcdfBW(double p, double mu, double gamma) {
const double xn = std::tan(M_PI*(p-0.5));
return gamma*xn + mu;
}
//@}
/// @name Binning helper functions
//@{
/// @brief Make a list of @a nbins + 1 values equally spaced between @a start and @a end inclusive.
///
/// NB. The arg ordering and the meaning of the nbins variable is "histogram-like",
/// as opposed to the Numpy/Matlab version.
inline vector<double> linspace(size_t nbins, double start, double end, bool include_end=true) {
assert(end >= start);
assert(nbins > 0);
vector<double> rtn;
const double interval = (end-start)/static_cast<double>(nbins);
for (size_t i = 0; i < nbins; ++i) {
rtn.push_back(start + i*interval);
}
assert(rtn.size() == nbins);
if (include_end) rtn.push_back(end); //< exact end, not result of n * interval
return rtn;
}
/// @brief Make a list of @a nbins + 1 values exponentially spaced between @a start and @a end inclusive.
///
/// NB. The arg ordering and the meaning of the nbins variable is "histogram-like",
/// as opposed to the Numpy/Matlab version, and the start and end arguments are expressed
/// in "normal" space, rather than as the logarithms of the start/end values as in Numpy/Matlab.
inline vector<double> logspace(size_t nbins, double start, double end, bool include_end=true) {
assert(end >= start);
assert(start > 0);
assert(nbins > 0);
const double logstart = std::log(start);
const double logend = std::log(end);
const vector<double> logvals = linspace(nbins, logstart, logend, false);
assert(logvals.size() == nbins);
vector<double> rtn; rtn.reserve(nbins+1);
rtn.push_back(start); //< exact start, not exp(log(start))
for (size_t i = 1; i < logvals.size(); ++i) {
rtn.push_back(std::exp(logvals[i]));
}
assert(rtn.size() == nbins);
if (include_end) rtn.push_back(end); //< exact end, not exp(n * loginterval)
return rtn;
}
/// @todo geomspace
/// @brief Make a list of @a nbins + 1 values spaced for equal area
/// Breit-Wigner binning between @a start and @a end inclusive. @a
/// mu and @a gamma are the Breit-Wigner parameters.
///
/// @note The arg ordering and the meaning of the nbins variable is "histogram-like",
/// as opposed to the Numpy/Matlab version, and the start and end arguments are expressed
/// in "normal" space.
inline vector<double> bwspace(size_t nbins, double start, double end, double mu, double gamma) {
assert(end >= start);
assert(nbins > 0);
const double pmin = cdfBW(start, mu, gamma);
const double pmax = cdfBW(end, mu, gamma);
const vector<double> edges = linspace(nbins, pmin, pmax);
assert(edges.size() == nbins+1);
vector<double> rtn;
for (double edge : edges) {
rtn.push_back(invcdfBW(edge, mu, gamma));
}
assert(rtn.size() == nbins+1);
return rtn;
}
/// Actual helper implementation of binIndex (so generic and specific overloading can work)
template <typename NUM, typename CONTAINER>
inline typename std::enable_if<std::is_arithmetic<NUM>::value && std::is_arithmetic<typename CONTAINER::value_type>::value, int>::type
_binIndex(NUM val, const CONTAINER& binedges, bool allow_overflow=false) {
if (val < *begin(binedges)) return -1; ///< Below/out of histo range
// CONTAINER::iterator_type itend =
if (val >= *(end(binedges)-1)) return allow_overflow ? int(binedges.size())-1 : -1; ///< Above/out of histo range
auto it = std::upper_bound(begin(binedges), end(binedges), val);
return std::distance(begin(binedges), --it);
}
/// @brief Return the bin index of the given value, @a val, given a vector of bin edges
///
/// An underflow always returns -1. If allow_overflow is false (default) an overflow
/// also returns -1, otherwise it returns the Nedge-1, the index of an inclusive bin
/// starting at the last edge.
///
/// @note The @a binedges vector must be sorted
/// @todo Use std::common_type<NUM1, NUM2>::type x = val; ?
template <typename NUM1, typename NUM2>
inline typename std::enable_if<std::is_arithmetic<NUM1>::value && std::is_arithmetic<NUM2>::value, int>::type
binIndex(NUM1 val, std::initializer_list<NUM2> binedges, bool allow_overflow=false) {
return _binIndex(val, binedges, allow_overflow);
}
/// @brief Return the bin index of the given value, @a val, given a vector of bin edges
///
/// An underflow always returns -1. If allow_overflow is false (default) an overflow
/// also returns -1, otherwise it returns the Nedge-1, the index of an inclusive bin
/// starting at the last edge.
///
/// @note The @a binedges vector must be sorted
/// @todo Use std::common_type<NUM1, NUM2>::type x = val; ?
template <typename NUM, typename CONTAINER>
inline typename std::enable_if<std::is_arithmetic<NUM>::value && std::is_arithmetic<typename CONTAINER::value_type>::value, int>::type
binIndex(NUM val, const CONTAINER& binedges, bool allow_overflow=false) {
return _binIndex(val, binedges, allow_overflow);
}
//@}
/// @name Discrete statistics functions
//@{
/// Calculate the median of a sample
/// @todo Support multiple container types via SFINAE
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, NUM>::type
median(const vector<NUM>& sample) {
if (sample.empty()) throw RangeError("Can't compute median of an empty set");
vector<NUM> tmp = sample;
std::sort(tmp.begin(), tmp.end());
const size_t imid = tmp.size()/2; // len1->idx0, len2->idx1, len3->idx1, len4->idx2, ...
if (sample.size() % 2 == 0) return (tmp.at(imid-1) + tmp.at(imid)) / 2.0;
else return tmp.at(imid);
}
/// Calculate the mean of a sample
/// @todo Support multiple container types via SFINAE
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, double>::type
mean(const vector<NUM>& sample) {
if (sample.empty()) throw RangeError("Can't compute mean of an empty set");
double mean = 0.0;
for (size_t i = 0; i < sample.size(); ++i) {
mean += sample[i];
}
return mean/sample.size();
}
// Calculate the error on the mean, assuming Poissonian errors
/// @todo Support multiple container types via SFINAE
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, double>::type
mean_err(const vector<NUM>& sample) {
if (sample.empty()) throw RangeError("Can't compute mean_err of an empty set");
double mean_e = 0.0;
for (size_t i = 0; i < sample.size(); ++i) {
mean_e += sqrt(sample[i]);
}
return mean_e/sample.size();
}
/// Calculate the covariance (variance) between two samples
/// @todo Support multiple container types via SFINAE
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, double>::type
covariance(const vector<NUM>& sample1, const vector<NUM>& sample2) {
if (sample1.empty() || sample2.empty()) throw RangeError("Can't compute covariance of an empty set");
if (sample1.size() != sample2.size()) throw RangeError("Sizes of samples must be equal for covariance calculation");
const double mean1 = mean(sample1);
const double mean2 = mean(sample2);
const size_t N = sample1.size();
double cov = 0.0;
for (size_t i = 0; i < N; i++) {
const double cov_i = (sample1[i] - mean1)*(sample2[i] - mean2);
cov += cov_i;
}
if (N > 1) return cov/(N-1);
else return 0.0;
}
/// Calculate the error on the covariance (variance) of two samples, assuming poissonian errors
/// @todo Support multiple container types via SFINAE
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, double>::type
covariance_err(const vector<NUM>& sample1, const vector<NUM>& sample2) {
if (sample1.empty() || sample2.empty()) throw RangeError("Can't compute covariance_err of an empty set");
if (sample1.size() != sample2.size()) throw RangeError("Sizes of samples must be equal for covariance_err calculation");
const double mean1 = mean(sample1);
const double mean2 = mean(sample2);
const double mean1_e = mean_err(sample1);
const double mean2_e = mean_err(sample2);
const size_t N = sample1.size();
double cov_e = 0.0;
for (size_t i = 0; i < N; i++) {
const double cov_i = (sqrt(sample1[i]) - mean1_e)*(sample2[i] - mean2) +
(sample1[i] - mean1)*(sqrt(sample2[i]) - mean2_e);
cov_e += cov_i;
}
if (N > 1) return cov_e/(N-1);
else return 0.0;
}
/// Calculate the correlation strength between two samples
/// @todo Support multiple container types via SFINAE
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, double>::type
correlation(const vector<NUM>& sample1, const vector<NUM>& sample2) {
const double cov = covariance(sample1, sample2);
const double var1 = covariance(sample1, sample1);
const double var2 = covariance(sample2, sample2);
const double correlation = cov/sqrt(var1*var2);
const double corr_strength = correlation*sqrt(var2/var1);
return corr_strength;
}
/// Calculate the error of the correlation strength between two samples assuming Poissonian errors
/// @todo Support multiple container types via SFINAE
template <typename NUM>
inline typename std::enable_if<std::is_arithmetic<NUM>::value, double>::type
correlation_err(const vector<NUM>& sample1, const vector<NUM>& sample2) {
const double cov = covariance(sample1, sample2);
const double var1 = covariance(sample1, sample1);
const double var2 = covariance(sample2, sample2);
const double cov_e = covariance_err(sample1, sample2);
const double var1_e = covariance_err(sample1, sample1);
const double var2_e = covariance_err(sample2, sample2);
// Calculate the correlation
const double correlation = cov/sqrt(var1*var2);
// Calculate the error on the correlation
const double correlation_err = cov_e/sqrt(var1*var2) -
cov/(2*pow(3./2., var1*var2)) * (var1_e * var2 + var1 * var2_e);
// Calculate the error on the correlation strength
const double corr_strength_err = correlation_err*sqrt(var2/var1) +
correlation/(2*sqrt(var2/var1)) * (var2_e/var1 - var2*var1_e/pow(2, var2));
return corr_strength_err;
}
//@}
/// @name Angle range mappings
//@{
/// @brief Reduce any number to the range [-2PI, 2PI]
///
/// Achieved by repeated addition or subtraction of 2PI as required. Used to
/// normalise angular measures.
inline double _mapAngleM2PITo2Pi(double angle) {
double rtn = fmod(angle, TWOPI);
if (isZero(rtn)) return 0;
assert(rtn >= -TWOPI && rtn <= TWOPI);
return rtn;
}
/// Map an angle into the range (-PI, PI].
inline double mapAngleMPiToPi(double angle) {
double rtn = _mapAngleM2PITo2Pi(angle);
if (isZero(rtn)) return 0;
if (rtn > PI) rtn -= TWOPI;
if (rtn <= -PI) rtn += TWOPI;
assert(rtn > -PI && rtn <= PI);
return rtn;
}
/// Map an angle into the range [0, 2PI).
inline double mapAngle0To2Pi(double angle) {
double rtn = _mapAngleM2PITo2Pi(angle);
if (isZero(rtn)) return 0;
if (rtn < 0) rtn += TWOPI;
if (rtn == TWOPI) rtn = 0;
assert(rtn >= 0 && rtn < TWOPI);
return rtn;
}
/// Map an angle into the range [0, PI].
inline double mapAngle0ToPi(double angle) {
double rtn = fabs(mapAngleMPiToPi(angle));
if (isZero(rtn)) return 0;
assert(rtn > 0 && rtn <= PI);
return rtn;
}
/// Map an angle into the enum-specified range.
inline double mapAngle(double angle, PhiMapping mapping) {
switch (mapping) {
case MINUSPI_PLUSPI:
return mapAngleMPiToPi(angle);
case ZERO_2PI:
return mapAngle0To2Pi(angle);
case ZERO_PI:
return mapAngle0To2Pi(angle);
default:
throw Rivet::UserError("The specified phi mapping scheme is not implemented");
}
}
//@}
/// @name Phase-space measure helpers
//@{
/// @brief Calculate the difference between two angles in radians
///
/// Returns in the range [0, PI].
- inline double deltaPhi(double phi1, double phi2) {
- return mapAngle0ToPi(phi1 - phi2);
+ inline double deltaPhi(double phi1, double phi2, bool sign=false) {
+ const double x = mapAngleMPiToPi(phi1 - phi2);
+ return sign ? x : fabs(x);
}
/// Calculate the abs difference between two pseudorapidities
///
/// @note Just a cosmetic name for analysis code clarity.
inline double deltaEta(double eta1, double eta2) {
return fabs(eta1 - eta2);
}
/// Calculate the abs difference between two rapidities
///
/// @note Just a cosmetic name for analysis code clarity.
inline double deltaRap(double y1, double y2) {
return fabs(y1 - y2);
}
/// Calculate the squared distance between two points in 2D rapidity-azimuthal
/// ("\f$ \eta-\phi \f$") space. The phi values are given in radians.
inline double deltaR2(double rap1, double phi1, double rap2, double phi2) {
const double dphi = deltaPhi(phi1, phi2);
return sqr(rap1-rap2) + sqr(dphi);
}
/// Calculate the distance between two points in 2D rapidity-azimuthal
/// ("\f$ \eta-\phi \f$") space. The phi values are given in radians.
inline double deltaR(double rap1, double phi1, double rap2, double phi2) {
return sqrt(deltaR2(rap1, phi1, rap2, phi2));
}
/// Calculate a rapidity value from the supplied energy @a E and longitudinal momentum @a pz.
inline double rapidity(double E, double pz) {
if (isZero(E - pz)) {
throw std::runtime_error("Divergent positive rapidity");
return MAXDOUBLE;
}
if (isZero(E + pz)) {
throw std::runtime_error("Divergent negative rapidity");
return -MAXDOUBLE;
}
return 0.5*log((E+pz)/(E-pz));
}
//@}
/// Calculate transverse mass of two vectors from provided pT and deltaPhi
/// @note Several versions taking two vectors are found in Vector4.hh
inline double mT(double pT1, double pT2, double dphi) {
return sqrt(2*pT1*pT2 * (1 - cos(dphi)) );
}
}
#endif
diff --git a/include/Rivet/Math/Vector3.hh b/include/Rivet/Math/Vector3.hh
--- a/include/Rivet/Math/Vector3.hh
+++ b/include/Rivet/Math/Vector3.hh
@@ -1,381 +1,381 @@
#ifndef RIVET_MATH_VECTOR3
#define RIVET_MATH_VECTOR3
#include "Rivet/Math/MathHeader.hh"
#include "Rivet/Math/MathUtils.hh"
#include "Rivet/Math/VectorN.hh"
namespace Rivet {
class Vector3;
typedef Vector3 ThreeVector;
class Matrix3;
Vector3 multiply(const double, const Vector3&);
Vector3 multiply(const Vector3&, const double);
Vector3 add(const Vector3&, const Vector3&);
Vector3 operator*(const double, const Vector3&);
Vector3 operator*(const Vector3&, const double);
Vector3 operator/(const Vector3&, const double);
Vector3 operator+(const Vector3&, const Vector3&);
Vector3 operator-(const Vector3&, const Vector3&);
/// @brief Three-dimensional specialisation of Vector.
class Vector3 : public Vector<3> {
friend class Matrix3;
friend Vector3 multiply(const double, const Vector3&);
friend Vector3 multiply(const Vector3&, const double);
friend Vector3 add(const Vector3&, const Vector3&);
friend Vector3 subtract(const Vector3&, const Vector3&);
public:
Vector3() : Vector<3>() { }
template<typename V3>
Vector3(const V3& other) {
this->setX(other.x());
this->setY(other.y());
this->setZ(other.z());
}
Vector3(const Vector<3>& other) {
this->setX(other.get(0));
this->setY(other.get(1));
this->setZ(other.get(2));
}
Vector3(double x, double y, double z) {
this->setX(x);
this->setY(y);
this->setZ(z);
}
~Vector3() { }
public:
static Vector3 mkX() { return Vector3(1,0,0); }
static Vector3 mkY() { return Vector3(0,1,0); }
static Vector3 mkZ() { return Vector3(0,0,1); }
public:
double x() const { return get(0); }
double y() const { return get(1); }
double z() const { return get(2); }
Vector3& setX(double x) { set(0, x); return *this; }
Vector3& setY(double y) { set(1, y); return *this; }
Vector3& setZ(double z) { set(2, z); return *this; }
/// Dot-product with another vector
double dot(const Vector3& v) const {
return _vec.dot(v._vec);
}
/// Cross-product with another vector
Vector3 cross(const Vector3& v) const {
Vector3 result;
result._vec = _vec.cross(v._vec);
return result;
}
/// Angle in radians to another vector
double angle(const Vector3& v) const {
const double localDotOther = unit().dot(v.unit());
if (localDotOther > 1.0) return 0.0;
if (localDotOther < -1.0) return M_PI;
return acos(localDotOther);
}
/// Unit-normalized version of this vector
Vector3 unitVec() const {
/// @todo What to do in this situation?
if (isZero()) return *this;
else return *this * 1.0/this->mod();
}
/// Synonym for unitVec
Vector3 unit() const {
return unitVec();
}
/// Polar projection of this vector into the x-y plane
Vector3 polarVec() const {
Vector3 rtn = *this;
rtn.setZ(0.);
return rtn;
}
/// Synonym for polarVec
Vector3 perpVec() const {
return polarVec();
}
/// Synonym for polarVec
Vector3 rhoVec() const {
return polarVec();
}
/// Square of the polar radius (
double polarRadius2() const {
return x()*x() + y()*y();
}
/// Synonym for polarRadius2
double perp2() const {
return polarRadius2();
}
/// Synonym for polarRadius2
double rho2() const {
return polarRadius2();
}
/// Polar radius
double polarRadius() const {
return sqrt(polarRadius2());
}
/// Synonym for polarRadius
double perp() const {
return polarRadius();
}
/// Synonym for polarRadius
double rho() const {
return polarRadius();
}
/// Angle subtended by the vector's projection in x-y and the x-axis.
double azimuthalAngle(const PhiMapping mapping = ZERO_2PI) const {
// If this is a null vector, return zero rather than let atan2 set an error state
if (Rivet::isZero(mod2())) return 0.0;
// Calculate the arctan and return in the requested range
const double value = atan2( y(), x() );
return mapAngle(value, mapping);
}
/// Synonym for azimuthalAngle.
double phi(const PhiMapping mapping = ZERO_2PI) const {
return azimuthalAngle(mapping);
}
/// Angle subtended by the vector and the z-axis.
double polarAngle() const {
// Get number beween [0,PI]
const double polarangle = atan2(polarRadius(), z());
return mapAngle0ToPi(polarangle);
}
/// Synonym for polarAngle
double theta() const {
return polarAngle();
}
/// Purely geometric approximation to rapidity
///
/// Also invariant under z-boosts, equal to y for massless particles.
///
/// @note A cut-off is applied such that |eta| < log(2/DBL_EPSILON)
double pseudorapidity() const {
const double epsilon = DBL_EPSILON;
double m = mod();
if ( m == 0.0 ) return 0.0;
double pt = max(epsilon*m, perp());
double rap = std::log((m + fabs(z()))/pt);
return z() > 0.0 ? rap: -rap;
}
/// Synonym for pseudorapidity
double eta() const {
return pseudorapidity();
}
/// Convenience shortcut for fabs(eta())
double abseta() const {
return fabs(eta());
}
public:
Vector3& operator*=(const double a) {
_vec = multiply(a, *this)._vec;
return *this;
}
Vector3& operator/=(const double a) {
_vec = multiply(1.0/a, *this)._vec;
return *this;
}
Vector3& operator+=(const Vector3& v) {
_vec = add(*this, v)._vec;
return *this;
}
Vector3& operator-=(const Vector3& v) {
_vec = subtract(*this, v)._vec;
return *this;
}
Vector3 operator-() const {
Vector3 rtn;
rtn._vec = -_vec;
return rtn;
}
};
inline double dot(const Vector3& a, const Vector3& b) {
return a.dot(b);
}
inline Vector3 cross(const Vector3& a, const Vector3& b) {
return a.cross(b);
}
inline Vector3 multiply(const double a, const Vector3& v) {
Vector3 result;
result._vec = a * v._vec;
return result;
}
inline Vector3 multiply(const Vector3& v, const double a) {
return multiply(a, v);
}
inline Vector3 operator*(const double a, const Vector3& v) {
return multiply(a, v);
}
inline Vector3 operator*(const Vector3& v, const double a) {
return multiply(a, v);
}
inline Vector3 operator/(const Vector3& v, const double a) {
return multiply(1.0/a, v);
}
inline Vector3 add(const Vector3& a, const Vector3& b) {
Vector3 result;
result._vec = a._vec + b._vec;
return result;
}
inline Vector3 subtract(const Vector3& a, const Vector3& b) {
Vector3 result;
result._vec = a._vec - b._vec;
return result;
}
inline Vector3 operator+(const Vector3& a, const Vector3& b) {
return add(a, b);
}
inline Vector3 operator-(const Vector3& a, const Vector3& b) {
return subtract(a, b);
}
// More physicsy coordinates etc.
/// Angle (in radians) between two 3-vectors.
inline double angle(const Vector3& a, const Vector3& b) {
return a.angle(b);
}
/////////////////////////////////////////////////////
/// @name \f$ |\Delta eta| \f$ calculations from 3-vectors
//@{
/// Calculate the difference in pseudorapidity between two spatial vectors.
inline double deltaEta(const Vector3& a, const Vector3& b) {
return deltaEta(a.pseudorapidity(), b.pseudorapidity());
}
/// Calculate the difference in pseudorapidity between two spatial vectors.
inline double deltaEta(const Vector3& v, double eta2) {
return deltaEta(v.pseudorapidity(), eta2);
}
/// Calculate the difference in pseudorapidity between two spatial vectors.
inline double deltaEta(double eta1, const Vector3& v) {
return deltaEta(eta1, v.pseudorapidity());
}
//@}
/// @name \f$ \Delta phi \f$ calculations from 3-vectors
//@{
/// Calculate the difference in azimuthal angle between two spatial vectors.
- inline double deltaPhi(const Vector3& a, const Vector3& b) {
- return deltaPhi(a.azimuthalAngle(), b.azimuthalAngle());
+ inline double deltaPhi(const Vector3& a, const Vector3& b, bool sign=false) {
+ return deltaPhi(a.azimuthalAngle(), b.azimuthalAngle(), sign);
}
/// Calculate the difference in azimuthal angle between two spatial vectors.
- inline double deltaPhi(const Vector3& v, double phi2) {
- return deltaPhi(v.azimuthalAngle(), phi2);
+ inline double deltaPhi(const Vector3& v, double phi2, bool sign=false) {
+ return deltaPhi(v.azimuthalAngle(), phi2, sign);
}
/// Calculate the difference in azimuthal angle between two spatial vectors.
- inline double deltaPhi(double phi1, const Vector3& v) {
- return deltaPhi(phi1, v.azimuthalAngle());
+ inline double deltaPhi(double phi1, const Vector3& v, bool sign=false) {
+ return deltaPhi(phi1, v.azimuthalAngle(), sign);
}
//@}
/// @name \f$ \Delta R \f$ calculations from 3-vectors
//@{
/// Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two spatial vectors.
inline double deltaR2(const Vector3& a, const Vector3& b) {
return deltaR2(a.pseudorapidity(), a.azimuthalAngle(),
b.pseudorapidity(), b.azimuthalAngle());
}
/// Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two spatial vectors.
inline double deltaR(const Vector3& a, const Vector3& b) {
return sqrt(deltaR2(a,b));
}
/// Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two spatial vectors.
inline double deltaR2(const Vector3& v, double eta2, double phi2) {
return deltaR2(v.pseudorapidity(), v.azimuthalAngle(), eta2, phi2);
}
/// Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two spatial vectors.
inline double deltaR(const Vector3& v, double eta2, double phi2) {
return sqrt(deltaR2(v, eta2, phi2));
}
/// Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two spatial vectors.
inline double deltaR2(double eta1, double phi1, const Vector3& v) {
return deltaR2(eta1, phi1, v.pseudorapidity(), v.azimuthalAngle());
}
/// Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two spatial vectors.
inline double deltaR(double eta1, double phi1, const Vector3& v) {
return sqrt(deltaR2(eta1, phi1, v));
}
//@}
/// @name Typedefs of vector types to short names
/// @todo Switch canonical and alias names
//@{
//typedef Vector3 V3; //< generic
typedef Vector3 X3; //< spatial
//@}
}
#endif
diff --git a/include/Rivet/Math/Vector4.hh b/include/Rivet/Math/Vector4.hh
--- a/include/Rivet/Math/Vector4.hh
+++ b/include/Rivet/Math/Vector4.hh
@@ -1,1551 +1,1551 @@
#ifndef RIVET_MATH_VECTOR4
#define RIVET_MATH_VECTOR4
#include "Rivet/Math/MathHeader.hh"
#include "Rivet/Math/MathUtils.hh"
#include "Rivet/Math/VectorN.hh"
#include "Rivet/Math/Vector3.hh"
namespace Rivet {
class FourVector;
class FourMomentum;
class LorentzTransform;
typedef FourVector Vector4;
FourVector transform(const LorentzTransform& lt, const FourVector& v4);
/// @brief Specialisation of VectorN to a general (non-momentum) Lorentz 4-vector.
///
/// @todo Add composite set/mk methods from different coord systems
class FourVector : public Vector<4> {
friend FourVector multiply(const double a, const FourVector& v);
friend FourVector multiply(const FourVector& v, const double a);
friend FourVector add(const FourVector& a, const FourVector& b);
friend FourVector transform(const LorentzTransform& lt, const FourVector& v4);
public:
FourVector() : Vector<4>() { }
template<typename V4>
FourVector(const V4& other) {
this->setT(other.t());
this->setX(other.x());
this->setY(other.y());
this->setZ(other.z());
}
FourVector(const Vector<4>& other)
: Vector<4>(other) { }
FourVector(const double t, const double x, const double y, const double z) {
this->setT(t);
this->setX(x);
this->setY(y);
this->setZ(z);
}
virtual ~FourVector() { }
public:
double t() const { return get(0); }
double t2() const { return sqr(t()); }
FourVector& setT(const double t) { set(0, t); return *this; }
double x() const { return get(1); }
double x2() const { return sqr(x()); }
FourVector& setX(const double x) { set(1, x); return *this; }
double y() const { return get(2); }
double y2() const { return sqr(y()); }
FourVector& setY(const double y) { set(2, y); return *this; }
double z() const { return get(3); }
double z2() const { return sqr(z()); }
FourVector& setZ(const double z) { set(3, z); return *this; }
double invariant() const {
// Done this way for numerical precision
return (t() + z())*(t() - z()) - x()*x() - y()*y();
}
bool isNull() const {
return Rivet::isZero(invariant());
}
/// Angle between this vector and another
double angle(const FourVector& v) const {
return vector3().angle( v.vector3() );
}
/// Angle between this vector and another (3-vector)
double angle(const Vector3& v3) const {
return vector3().angle(v3);
}
/// @brief Mod-square of the projection of the 3-vector on to the \f$ x-y \f$ plane
/// This is a more efficient function than @c polarRadius, as it avoids the square root.
/// Use it if you only need the squared value, or e.g. an ordering by magnitude.
double polarRadius2() const {
return vector3().polarRadius2();
}
/// Synonym for polarRadius2
double perp2() const {
return vector3().perp2();
}
/// Synonym for polarRadius2
double rho2() const {
return vector3().rho2();
}
/// Magnitude of projection of 3-vector on to the \f$ x-y \f$ plane
double polarRadius() const {
return vector3().polarRadius();
}
/// Synonym for polarRadius
double perp() const {
return vector3().perp();
}
/// Synonym for polarRadius
double rho() const {
return vector3().rho();
}
/// Projection of 3-vector on to the \f$ x-y \f$ plane
Vector3 polarVec() const {
return vector3().polarVec();
}
/// Synonym for polarVec
Vector3 perpVec() const {
return vector3().perpVec();
}
/// Synonym for polarVec
Vector3 rhoVec() const {
return vector3().rhoVec();
}
/// Angle subtended by the 3-vector's projection in x-y and the x-axis.
double azimuthalAngle(const PhiMapping mapping=ZERO_2PI) const {
return vector3().azimuthalAngle(mapping);
}
/// Synonym for azimuthalAngle.
double phi(const PhiMapping mapping=ZERO_2PI) const {
return vector3().phi(mapping);
}
/// Angle subtended by the 3-vector and the z-axis.
double polarAngle() const {
return vector3().polarAngle();
}
/// Synonym for polarAngle.
double theta() const {
return vector3().theta();
}
/// Pseudorapidity (defined purely by the 3-vector components)
double pseudorapidity() const {
return vector3().pseudorapidity();
}
/// Synonym for pseudorapidity.
double eta() const {
return vector3().eta();
}
/// Get the \f$ |\eta| \f$ directly.
double abspseudorapidity() const { return fabs(eta()); }
/// Get the \f$ |\eta| \f$ directly (alias).
double abseta() const { return fabs(eta()); }
/// Get the spatial part of the 4-vector as a 3-vector.
Vector3 vector3() const {
return Vector3(get(1), get(2), get(3));
}
/// Implicit cast to a 3-vector
operator Vector3 () const { return vector3(); }
public:
/// Contract two 4-vectors, with metric signature (+ - - -).
double contract(const FourVector& v) const {
const double result = t()*v.t() - x()*v.x() - y()*v.y() - z()*v.z();
return result;
}
/// Contract two 4-vectors, with metric signature (+ - - -).
double dot(const FourVector& v) const {
return contract(v);
}
/// Contract two 4-vectors, with metric signature (+ - - -).
double operator*(const FourVector& v) const {
return contract(v);
}
/// Multiply by a scalar.
FourVector& operator*=(double a) {
_vec = multiply(a, *this)._vec;
return *this;
}
/// Divide by a scalar.
FourVector& operator/=(double a) {
_vec = multiply(1.0/a, *this)._vec;
return *this;
}
/// Add to this 4-vector.
FourVector& operator+=(const FourVector& v) {
_vec = add(*this, v)._vec;
return *this;
}
/// Subtract from this 4-vector. NB time as well as space components are subtracted.
FourVector& operator-=(const FourVector& v) {
_vec = add(*this, -v)._vec;
return *this;
}
/// Multiply all components (space and time) by -1.
FourVector operator-() const {
FourVector result;
result._vec = -_vec;
return result;
}
/// Multiply space components only by -1.
FourVector reverse() const {
FourVector result = -*this;
result.setT(-result.t());
return result;
}
};
/// Contract two 4-vectors, with metric signature (+ - - -).
inline double contract(const FourVector& a, const FourVector& b) {
return a.contract(b);
}
/// Contract two 4-vectors, with metric signature (+ - - -).
inline double dot(const FourVector& a, const FourVector& b) {
return contract(a, b);
}
inline FourVector multiply(const double a, const FourVector& v) {
FourVector result;
result._vec = a * v._vec;
return result;
}
inline FourVector multiply(const FourVector& v, const double a) {
return multiply(a, v);
}
inline FourVector operator*(const double a, const FourVector& v) {
return multiply(a, v);
}
inline FourVector operator*(const FourVector& v, const double a) {
return multiply(a, v);
}
inline FourVector operator/(const FourVector& v, const double a) {
return multiply(1.0/a, v);
}
inline FourVector add(const FourVector& a, const FourVector& b) {
FourVector result;
result._vec = a._vec + b._vec;
return result;
}
inline FourVector operator+(const FourVector& a, const FourVector& b) {
return add(a, b);
}
inline FourVector operator-(const FourVector& a, const FourVector& b) {
return add(a, -b);
}
/// Calculate the Lorentz self-invariant of a 4-vector.
/// \f$ v_\mu v^\mu = g_{\mu\nu} x^\mu x^\nu \f$.
inline double invariant(const FourVector& lv) {
return lv.invariant();
}
/// Angle (in radians) between spatial parts of two Lorentz vectors.
inline double angle(const FourVector& a, const FourVector& b) {
return a.angle(b);
}
/// Angle (in radians) between spatial parts of two Lorentz vectors.
inline double angle(const Vector3& a, const FourVector& b) {
return angle( a, b.vector3() );
}
/// Angle (in radians) between spatial parts of two Lorentz vectors.
inline double angle(const FourVector& a, const Vector3& b) {
return a.angle(b);
}
////////////////////////////////////////////////
/// Specialized version of the FourVector with momentum/energy functionality.
class FourMomentum : public FourVector {
friend FourMomentum multiply(const double a, const FourMomentum& v);
friend FourMomentum multiply(const FourMomentum& v, const double a);
friend FourMomentum add(const FourMomentum& a, const FourMomentum& b);
friend FourMomentum transform(const LorentzTransform& lt, const FourMomentum& v4);
public:
FourMomentum() { }
template<typename V4>
FourMomentum(const V4& other) {
this->setE(other.t());
this->setPx(other.x());
this->setPy(other.y());
this->setPz(other.z());
}
FourMomentum(const Vector<4>& other)
: FourVector(other) { }
FourMomentum(const double E, const double px, const double py, const double pz) {
this->setE(E);
this->setPx(px);
this->setPy(py);
this->setPz(pz);
}
~FourMomentum() {}
public:
/// @name Coordinate setters
//@{
/// Set energy \f$ E \f$ (time component of momentum).
FourMomentum& setE(double E) {
setT(E);
return *this;
}
/// Set x-component of momentum \f$ p_x \f$.
FourMomentum& setPx(double px) {
setX(px);
return *this;
}
/// Set y-component of momentum \f$ p_y \f$.
FourMomentum& setPy(double py) {
setY(py);
return *this;
}
/// Set z-component of momentum \f$ p_z \f$.
FourMomentum& setPz(double pz) {
setZ(pz);
return *this;
}
/// Set the p coordinates and energy simultaneously
FourMomentum& setPE(double px, double py, double pz, double E) {
if (E < 0)
throw std::invalid_argument("Negative energy given as argument: " + to_str(E));
setPx(px); setPy(py); setPz(pz); setE(E);
return *this;
}
/// Alias for setPE
FourMomentum& setXYZE(double px, double py, double pz, double E) {
return setPE(px, py, pz, E);
}
// /// Near-alias with switched arg order
// FourMomentum& setEP(double E, double px, double py, double pz) {
// return setPE(px, py, pz, E);
// }
// /// Alias for setEP
// FourMomentum& setEXYZ(double E, double px, double py, double pz) {
// return setEP(E, px, py, pz);
// }
/// Set the p coordinates and mass simultaneously
FourMomentum& setPM(double px, double py, double pz, double mass) {
if (mass < 0)
throw std::invalid_argument("Negative mass given as argument: " + to_str(mass));
const double E = sqrt( sqr(mass) + sqr(px) + sqr(py) + sqr(pz) );
// setPx(px); setPy(py); setPz(pz); setE(E);
return setPE(px, py, pz, E);
}
/// Alias for setPM
FourMomentum& setXYZM(double px, double py, double pz, double mass) {
return setPM(px, py, pz, mass);
}
/// Set the vector state from (eta,phi,energy) coordinates and the mass
///
/// eta = -ln(tan(theta/2))
/// -> theta = 2 atan(exp(-eta))
FourMomentum& setEtaPhiME(double eta, double phi, double mass, double E) {
if (mass < 0)
throw std::invalid_argument("Negative mass given as argument");
if (E < 0)
throw std::invalid_argument("Negative energy given as argument");
const double theta = 2 * atan(exp(-eta));
if (theta < 0 || theta > M_PI)
throw std::domain_error("Polar angle outside 0..pi in calculation");
setThetaPhiME(theta, phi, mass, E);
return *this;
}
/// Set the vector state from (eta,phi,pT) coordinates and the mass
///
/// eta = -ln(tan(theta/2))
/// -> theta = 2 atan(exp(-eta))
FourMomentum& setEtaPhiMPt(double eta, double phi, double mass, double pt) {
if (mass < 0)
throw std::invalid_argument("Negative mass given as argument");
if (pt < 0)
throw std::invalid_argument("Negative transverse momentum given as argument");
const double theta = 2 * atan(exp(-eta));
if (theta < 0 || theta > M_PI)
throw std::domain_error("Polar angle outside 0..pi in calculation");
const double p = pt / sin(theta);
const double E = sqrt( sqr(p) + sqr(mass) );
setThetaPhiME(theta, phi, mass, E);
return *this;
}
/// Set the vector state from (y,phi,energy) coordinates and the mass
///
/// y = 0.5 * ln((E+pz)/(E-pz))
/// -> (E^2 - pz^2) exp(2y) = (E+pz)^2
/// & (E^2 - pz^2) exp(-2y) = (E-pz)^2
/// -> E = sqrt(pt^2 + m^2) cosh(y)
/// -> pz = sqrt(pt^2 + m^2) sinh(y)
/// -> sqrt(pt^2 + m^2) = E / cosh(y)
FourMomentum& setRapPhiME(double y, double phi, double mass, double E) {
if (mass < 0)
throw std::invalid_argument("Negative mass given as argument");
if (E < 0)
throw std::invalid_argument("Negative energy given as argument");
const double sqrt_pt2_m2 = E / cosh(y);
const double pt = sqrt( sqr(sqrt_pt2_m2) - sqr(mass) );
if (pt < 0)
throw std::domain_error("Negative transverse momentum in calculation");
const double pz = sqrt_pt2_m2 * sinh(y);
const double px = pt * cos(phi);
const double py = pt * sin(phi);
setPE(px, py, pz, E);
return *this;
}
/// Set the vector state from (y,phi,pT) coordinates and the mass
///
/// y = 0.5 * ln((E+pz)/(E-pz))
/// -> E = sqrt(pt^2 + m^2) cosh(y) [see above]
FourMomentum& setRapPhiMPt(double y, double phi, double mass, double pt) {
if (mass < 0)
throw std::invalid_argument("Negative mass given as argument");
if (pt < 0)
throw std::invalid_argument("Negative transverse mass given as argument");
const double E = sqrt( sqr(pt) + sqr(mass) ) * cosh(y);
if (E < 0)
throw std::domain_error("Negative energy in calculation");
setRapPhiME(y, phi, mass, E);
return *this;
}
/// Set the vector state from (theta,phi,energy) coordinates and the mass
///
/// p = sqrt(E^2 - mass^2)
/// pz = p cos(theta)
/// pt = p sin(theta)
FourMomentum& setThetaPhiME(double theta, double phi, double mass, double E) {
if (theta < 0 || theta > M_PI)
throw std::invalid_argument("Polar angle outside 0..pi given as argument");
if (mass < 0)
throw std::invalid_argument("Negative mass given as argument");
if (E < 0)
throw std::invalid_argument("Negative energy given as argument");
const double p = sqrt( sqr(E) - sqr(mass) );
const double pz = p * cos(theta);
const double pt = p * sin(theta);
if (pt < 0)
throw std::invalid_argument("Negative transverse momentum in calculation");
const double px = pt * cos(phi);
const double py = pt * sin(phi);
setPE(px, py, pz, E);
return *this;
}
/// Set the vector state from (theta,phi,pT) coordinates and the mass
///
/// p = pt / sin(theta)
/// pz = p cos(theta)
/// E = sqrt(p^2 + mass^2)
FourMomentum& setThetaPhiMPt(double theta, double phi, double mass, double pt) {
if (theta < 0 || theta > M_PI)
throw std::invalid_argument("Polar angle outside 0..pi given as argument");
if (mass < 0)
throw std::invalid_argument("Negative mass given as argument");
if (pt < 0)
throw std::invalid_argument("Negative transverse momentum given as argument");
const double p = pt / sin(theta);
const double px = pt * cos(phi);
const double py = pt * sin(phi);
const double pz = p * cos(theta);
const double E = sqrt( sqr(p) + sqr(mass) );
setPE(px, py, pz, E);
return *this;
}
/// Set the vector state from (pT,phi,energy) coordinates and the mass
///
/// pz = sqrt(E^2 - mass^2 - pt^2)
FourMomentum& setPtPhiME(double pt, double phi, double mass, double E) {
if (pt < 0)
throw std::invalid_argument("Negative transverse momentum given as argument");
if (mass < 0)
throw std::invalid_argument("Negative mass given as argument");
if (E < 0)
throw std::invalid_argument("Negative energy given as argument");
const double px = pt * cos(phi);
const double py = pt * sin(phi);
const double pz = sqrt(sqr(E) - sqr(mass) - sqr(pt));
setPE(px, py, pz, E);
return *this;
}
//@}
/// @name Accessors
//@{
/// Get energy \f$ E \f$ (time component of momentum).
double E() const { return t(); }
/// Get energy-squared \f$ E^2 \f$.
double E2() const { return t2(); }
/// Get x-component of momentum \f$ p_x \f$.
double px() const { return x(); }
/// Get x-squared \f$ p_x^2 \f$.
double px2() const { return x2(); }
/// Get y-component of momentum \f$ p_y \f$.
double py() const { return y(); }
/// Get y-squared \f$ p_y^2 \f$.
double py2() const { return y2(); }
/// Get z-component of momentum \f$ p_z \f$.
double pz() const { return z(); }
/// Get z-squared \f$ p_z^2 \f$.
double pz2() const { return z2(); }
/// @brief Get the mass \f$ m = \sqrt{E^2 - p^2} \f$ (the Lorentz self-invariant).
///
/// For spacelike momenta, the mass will be -sqrt(|mass2|).
double mass() const {
// assert(Rivet::isZero(mass2()) || mass2() > 0);
// if (Rivet::isZero(mass2())) {
// return 0.0;
// } else {
// return sqrt(mass2());
// }
return sign(mass2()) * sqrt(fabs(mass2()));
}
/// Get the squared mass \f$ m^2 = E^2 - p^2 \f$ (the Lorentz self-invariant).
double mass2() const {
return invariant();
}
/// Get 3-momentum part, \f$ p \f$.
Vector3 p3() const { return vector3(); }
/// Get the modulus of the 3-momentum
double p() const {
return p3().mod();
}
/// Get the modulus-squared of the 3-momentum
double p2() const {
return p3().mod2();
}
/// Calculate the rapidity.
double rapidity() const {
return 0.5 * std::log( (E() + pz()) / (E() - pz()) );
}
/// Alias for rapidity.
double rap() const {
return rapidity();
}
/// Absolute rapidity.
double absrapidity() const {
return fabs(rapidity());
}
/// Absolute rapidity.
double absrap() const {
return fabs(rap());
}
/// Calculate the transverse momentum vector \f$ \vec{p}_T \f$.
Vector3 pTvec() const {
return p3().polarVec();
}
/// Synonym for pTvec
Vector3 ptvec() const {
return pTvec();
}
/// Calculate the squared transverse momentum \f$ p_T^2 \f$.
double pT2() const {
return vector3().polarRadius2();
}
/// Calculate the squared transverse momentum \f$ p_T^2 \f$.
double pt2() const {
return vector3().polarRadius2();
}
/// Calculate the transverse momentum \f$ p_T \f$.
double pT() const {
return sqrt(pT2());
}
/// Calculate the transverse momentum \f$ p_T \f$.
double pt() const {
return sqrt(pT2());
}
/// Calculate the transverse energy \f$ E_T^2 = E^2 \sin^2{\theta} \f$.
double Et2() const {
return Et() * Et();
}
/// Calculate the transverse energy \f$ E_T = E \sin{\theta} \f$.
double Et() const {
return E() * sin(polarAngle());
}
//@}
/// @name Lorentz boost factors and vectors
//@{
/// Calculate the boost factor \f$ \gamma \f$.
/// @note \f$ \gamma = E/mc^2 \f$ so we rely on the c=1 convention
double gamma() const {
return sqrt(E2()/mass2());
}
/// Calculate the boost vector \f$ \vec{\gamma} \f$.
/// @note \f$ \gamma = E/mc^2 \f$ so we rely on the c=1 convention
Vector3 gammaVec() const {
return gamma() * p3().unit();
}
/// Calculate the boost factor \f$ \beta \f$.
/// @note \f$ \beta = pc/E \f$ so we rely on the c=1 convention
double beta() const {
return p()/E();
}
/// Calculate the boost vector \f$ \vec{\beta} \f$.
/// @note \f$ \beta = pc/E \f$ so we rely on the c=1 convention
Vector3 betaVec() const {
// return Vector3(px()/E(), py()/E(), pz()/E());
return p3()/E();
}
/// @brief Deprecated alias for betaVec
/// @deprecated This will be removed; use betaVec() instead
Vector3 boostVector() const { return betaVec(); }
//@}
////////////////////////////////////////
/// @name Sorting helpers
//@{
/// Struct for sorting by increasing energy
struct byEAscending {
bool operator()(const FourMomentum& left, const FourMomentum& right) const{
const double pt2left = left.E();
const double pt2right = right.E();
return pt2left < pt2right;
}
bool operator()(const FourMomentum* left, const FourMomentum* right) const{
return (*this)(*left, *right);
}
};
/// Struct for sorting by decreasing energy
struct byEDescending {
bool operator()(const FourMomentum& left, const FourMomentum& right) const{
return byEAscending()(right, left);
}
bool operator()(const FourMomentum* left, const FourVector* right) const{
return (*this)(*left, *right);
}
};
//@}
////////////////////////////////////////
/// @name Arithmetic operators
//@{
/// Multiply by a scalar
FourMomentum& operator*=(double a) {
_vec = multiply(a, *this)._vec;
return *this;
}
/// Divide by a scalar
FourMomentum& operator/=(double a) {
_vec = multiply(1.0/a, *this)._vec;
return *this;
}
/// Add to this 4-vector. NB time as well as space components are added.
FourMomentum& operator+=(const FourMomentum& v) {
_vec = add(*this, v)._vec;
return *this;
}
/// Subtract from this 4-vector. NB time as well as space components are subtracted.
FourMomentum& operator-=(const FourMomentum& v) {
_vec = add(*this, -v)._vec;
return *this;
}
/// Multiply all components (time and space) by -1.
FourMomentum operator-() const {
FourMomentum result;
result._vec = -_vec;
return result;
}
/// Multiply space components only by -1.
FourMomentum reverse() const {
FourMomentum result = -*this;
result.setE(-result.E());
return result;
}
//@}
////////////////////////////////////////
/// @name Factory functions
//@{
/// Make a vector from (px,py,pz,E) coordinates
static FourMomentum mkXYZE(double px, double py, double pz, double E) {
return FourMomentum().setPE(px, py, pz, E);
}
/// Make a vector from (px,py,pz) coordinates and the mass
static FourMomentum mkXYZM(double px, double py, double pz, double mass) {
return FourMomentum().setPM(px, py, pz, mass);
}
/// Make a vector from (eta,phi,energy) coordinates and the mass
static FourMomentum mkEtaPhiME(double eta, double phi, double mass, double E) {
return FourMomentum().setEtaPhiME(eta, phi, mass, E);
}
/// Make a vector from (eta,phi,pT) coordinates and the mass
static FourMomentum mkEtaPhiMPt(double eta, double phi, double mass, double pt) {
return FourMomentum().setEtaPhiMPt(eta, phi, mass, pt);
}
/// Make a vector from (y,phi,energy) coordinates and the mass
static FourMomentum mkRapPhiME(double y, double phi, double mass, double E) {
return FourMomentum().setRapPhiME(y, phi, mass, E);
}
/// Make a vector from (y,phi,pT) coordinates and the mass
static FourMomentum mkRapPhiMPt(double y, double phi, double mass, double pt) {
return FourMomentum().setRapPhiMPt(y, phi, mass, pt);
}
/// Make a vector from (theta,phi,energy) coordinates and the mass
static FourMomentum mkThetaPhiME(double theta, double phi, double mass, double E) {
return FourMomentum().setThetaPhiME(theta, phi, mass, E);
}
/// Make a vector from (theta,phi,pT) coordinates and the mass
static FourMomentum mkThetaPhiMPt(double theta, double phi, double mass, double pt) {
return FourMomentum().setThetaPhiMPt(theta, phi, mass, pt);
}
/// Make a vector from (pT,phi,energy) coordinates and the mass
static FourMomentum mkPtPhiME(double pt, double phi, double mass, double E) {
return FourMomentum().setPtPhiME(pt, phi, mass, E);
}
//@}
};
inline FourMomentum multiply(const double a, const FourMomentum& v) {
FourMomentum result;
result._vec = a * v._vec;
return result;
}
inline FourMomentum multiply(const FourMomentum& v, const double a) {
return multiply(a, v);
}
inline FourMomentum operator*(const double a, const FourMomentum& v) {
return multiply(a, v);
}
inline FourMomentum operator*(const FourMomentum& v, const double a) {
return multiply(a, v);
}
inline FourMomentum operator/(const FourMomentum& v, const double a) {
return multiply(1.0/a, v);
}
inline FourMomentum add(const FourMomentum& a, const FourMomentum& b) {
FourMomentum result;
result._vec = a._vec + b._vec;
return result;
}
inline FourMomentum operator+(const FourMomentum& a, const FourMomentum& b) {
return add(a, b);
}
inline FourMomentum operator-(const FourMomentum& a, const FourMomentum& b) {
return add(a, -b);
}
//////////////////////////////////////////////////////
/// @name \f$ \Delta R \f$ calculations from 4-vectors
//@{
/// @brief Calculate the squared 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
///
/// There is a scheme ambiguity for momentum-type four vectors as to whether
/// the pseudorapidity (a purely geometric concept) or the rapidity (a
/// relativistic energy-momentum quantity) is to be used: this can be chosen
/// via the optional scheme parameter. Use of this scheme option is
/// discouraged in this case since @c RAPIDITY is only a valid option for
/// vectors whose type is really the FourMomentum derived class.
inline double deltaR2(const FourVector& a, const FourVector& b,
RapScheme scheme=PSEUDORAPIDITY) {
switch (scheme) {
case PSEUDORAPIDITY :
return deltaR2(a.vector3(), b.vector3());
case RAPIDITY:
{
const FourMomentum* ma = dynamic_cast<const FourMomentum*>(&a);
const FourMomentum* mb = dynamic_cast<const FourMomentum*>(&b);
if (!ma || !mb) {
string err = "deltaR with scheme RAPIDITY can only be called with FourMomentum objects, not FourVectors";
throw std::runtime_error(err);
}
return deltaR2(*ma, *mb, scheme);
}
default:
throw std::runtime_error("The specified deltaR scheme is not yet implemented");
}
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
///
/// There is a scheme ambiguity for momentum-type four vectors as to whether
/// the pseudorapidity (a purely geometric concept) or the rapidity (a
/// relativistic energy-momentum quantity) is to be used: this can be chosen
/// via the optional scheme parameter. Use of this scheme option is
/// discouraged in this case since @c RAPIDITY is only a valid option for
/// vectors whose type is really the FourMomentum derived class.
inline double deltaR(const FourVector& a, const FourVector& b,
RapScheme scheme=PSEUDORAPIDITY) {
return sqrt(deltaR2(a, b, scheme));
}
/// @brief Calculate the squared 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
///
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR2(const FourVector& v,
double eta2, double phi2,
RapScheme scheme=PSEUDORAPIDITY) {
switch (scheme) {
case PSEUDORAPIDITY :
return deltaR2(v.vector3(), eta2, phi2);
case RAPIDITY:
{
const FourMomentum* mv = dynamic_cast<const FourMomentum*>(&v);
if (!mv) {
string err = "deltaR with scheme RAPIDITY can only be called with FourMomentum objects, not FourVectors";
throw std::runtime_error(err);
}
return deltaR2(*mv, eta2, phi2, scheme);
}
default:
throw std::runtime_error("The specified deltaR scheme is not yet implemented");
}
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
///
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR(const FourVector& v,
double eta2, double phi2,
RapScheme scheme=PSEUDORAPIDITY) {
return sqrt(deltaR2(v, eta2, phi2, scheme));
}
/// @brief Calculate the squared 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
///
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR2(double eta1, double phi1,
const FourVector& v,
RapScheme scheme=PSEUDORAPIDITY) {
switch (scheme) {
case PSEUDORAPIDITY :
return deltaR2(eta1, phi1, v.vector3());
case RAPIDITY:
{
const FourMomentum* mv = dynamic_cast<const FourMomentum*>(&v);
if (!mv) {
string err = "deltaR with scheme RAPIDITY can only be called with FourMomentum objects, not FourVectors";
throw std::runtime_error(err);
}
return deltaR2(eta1, phi1, *mv, scheme);
}
default:
throw std::runtime_error("The specified deltaR scheme is not yet implemented");
}
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
///
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR(double eta1, double phi1,
const FourVector& v,
RapScheme scheme=PSEUDORAPIDITY) {
return sqrt(deltaR2(eta1, phi1, v, scheme));
}
/// @brief Calculate the squared 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
///
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR2(const FourMomentum& a, const FourMomentum& b,
RapScheme scheme=PSEUDORAPIDITY) {
switch (scheme) {
case PSEUDORAPIDITY:
return deltaR2(a.vector3(), b.vector3());
case RAPIDITY:
return deltaR2(a.rapidity(), a.azimuthalAngle(), b.rapidity(), b.azimuthalAngle());
default:
throw std::runtime_error("The specified deltaR scheme is not yet implemented");
}
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
///
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR(const FourMomentum& a, const FourMomentum& b,
RapScheme scheme=PSEUDORAPIDITY) {
return sqrt(deltaR2(a, b, scheme));
}
/// @brief Calculate the squared 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR2(const FourMomentum& v,
double eta2, double phi2,
RapScheme scheme=PSEUDORAPIDITY) {
switch (scheme) {
case PSEUDORAPIDITY:
return deltaR2(v.vector3(), eta2, phi2);
case RAPIDITY:
return deltaR2(v.rapidity(), v.azimuthalAngle(), eta2, phi2);
default:
throw std::runtime_error("The specified deltaR scheme is not yet implemented");
}
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR(const FourMomentum& v,
double eta2, double phi2,
RapScheme scheme=PSEUDORAPIDITY) {
return sqrt(deltaR2(v, eta2, phi2, scheme));
}
/// @brief Calculate the squared 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR2(double eta1, double phi1,
const FourMomentum& v,
RapScheme scheme=PSEUDORAPIDITY) {
switch (scheme) {
case PSEUDORAPIDITY:
return deltaR2(eta1, phi1, v.vector3());
case RAPIDITY:
return deltaR2(eta1, phi1, v.rapidity(), v.azimuthalAngle());
default:
throw std::runtime_error("The specified deltaR scheme is not yet implemented");
}
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR(double eta1, double phi1,
const FourMomentum& v,
RapScheme scheme=PSEUDORAPIDITY) {
return sqrt(deltaR2(eta1, phi1, v, scheme));
}
/// @brief Calculate the squared 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR2(const FourMomentum& a, const FourVector& b,
RapScheme scheme=PSEUDORAPIDITY) {
switch (scheme) {
case PSEUDORAPIDITY:
return deltaR2(a.vector3(), b.vector3());
case RAPIDITY:
return deltaR2(a.rapidity(), a.azimuthalAngle(), FourMomentum(b).rapidity(), b.azimuthalAngle());
default:
throw std::runtime_error("The specified deltaR scheme is not yet implemented");
}
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR(const FourMomentum& a, const FourVector& b,
RapScheme scheme=PSEUDORAPIDITY) {
return sqrt(deltaR2(a, b, scheme));
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR2(const FourVector& a, const FourMomentum& b,
RapScheme scheme=PSEUDORAPIDITY) {
return deltaR2(b, a, scheme); //< note reversed args
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between two four-vectors.
/// There is a scheme ambiguity for momentum-type four vectors
/// as to whether the pseudorapidity (a purely geometric concept) or the
/// rapidity (a relativistic energy-momentum quantity) is to be used: this can
/// be chosen via the optional scheme parameter.
inline double deltaR(const FourVector& a, const FourMomentum& b,
RapScheme scheme=PSEUDORAPIDITY) {
return deltaR(b, a, scheme); //< note reversed args
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between a
/// three-vector and a four-vector.
inline double deltaR2(const FourMomentum& a, const Vector3& b) {
return deltaR2(a.vector3(), b);
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between a
/// three-vector and a four-vector.
inline double deltaR(const FourMomentum& a, const Vector3& b) {
return deltaR(a.vector3(), b);
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between a
/// three-vector and a four-vector.
inline double deltaR2(const Vector3& a, const FourMomentum& b) {
return deltaR2(a, b.vector3());
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between a
/// three-vector and a four-vector.
inline double deltaR(const Vector3& a, const FourMomentum& b) {
return deltaR(a, b.vector3());
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between a
/// three-vector and a four-vector.
inline double deltaR2(const FourVector& a, const Vector3& b) {
return deltaR2(a.vector3(), b);
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between a
/// three-vector and a four-vector.
inline double deltaR(const FourVector& a, const Vector3& b) {
return deltaR(a.vector3(), b);
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between a
/// three-vector and a four-vector.
inline double deltaR2(const Vector3& a, const FourVector& b) {
return deltaR2(a, b.vector3());
}
/// @brief Calculate the 2D rapidity-azimuthal ("eta-phi") distance between a
/// three-vector and a four-vector.
inline double deltaR(const Vector3& a, const FourVector& b) {
return deltaR(a, b.vector3());
}
//@}
//////////////////////////////////////////////////////
/// @name \f$ \Delta phi \f$ calculations from 4-vectors
//@{
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(const FourMomentum& a, const FourMomentum& b) {
- return deltaPhi(a.vector3(), b.vector3());
+ inline double deltaPhi(const FourMomentum& a, const FourMomentum& b, bool sign=false) {
+ return deltaPhi(a.vector3(), b.vector3(), sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(const FourMomentum& v, double phi2) {
- return deltaPhi(v.vector3(), phi2);
+ inline double deltaPhi(const FourMomentum& v, double phi2, bool sign=false) {
+ return deltaPhi(v.vector3(), phi2, sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(double phi1, const FourMomentum& v) {
- return deltaPhi(phi1, v.vector3());
+ inline double deltaPhi(double phi1, const FourMomentum& v, bool sign=false) {
+ return deltaPhi(phi1, v.vector3(), sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(const FourVector& a, const FourVector& b) {
- return deltaPhi(a.vector3(), b.vector3());
+ inline double deltaPhi(const FourVector& a, const FourVector& b, bool sign=false) {
+ return deltaPhi(a.vector3(), b.vector3(), sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(const FourVector& v, double phi2) {
- return deltaPhi(v.vector3(), phi2);
+ inline double deltaPhi(const FourVector& v, double phi2, bool sign=false) {
+ return deltaPhi(v.vector3(), phi2, sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(double phi1, const FourVector& v) {
- return deltaPhi(phi1, v.vector3());
+ inline double deltaPhi(double phi1, const FourVector& v, bool sign=false) {
+ return deltaPhi(phi1, v.vector3(), sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(const FourVector& a, const FourMomentum& b) {
- return deltaPhi(a.vector3(), b.vector3());
+ inline double deltaPhi(const FourVector& a, const FourMomentum& b, bool sign=false) {
+ return deltaPhi(a.vector3(), b.vector3(), sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(const FourMomentum& a, const FourVector& b) {
- return deltaPhi(a.vector3(), b.vector3());
+ inline double deltaPhi(const FourMomentum& a, const FourVector& b, bool sign=false) {
+ return deltaPhi(a.vector3(), b.vector3(), sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(const FourVector& a, const Vector3& b) {
- return deltaPhi(a.vector3(), b);
+ inline double deltaPhi(const FourVector& a, const Vector3& b, bool sign=false) {
+ return deltaPhi(a.vector3(), b, sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(const Vector3& a, const FourVector& b) {
- return deltaPhi(a, b.vector3());
+ inline double deltaPhi(const Vector3& a, const FourVector& b, bool sign=false) {
+ return deltaPhi(a, b.vector3(), sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(const FourMomentum& a, const Vector3& b) {
- return deltaPhi(a.vector3(), b);
+ inline double deltaPhi(const FourMomentum& a, const Vector3& b, bool sign=false) {
+ return deltaPhi(a.vector3(), b, sign);
}
/// Calculate the difference in azimuthal angle between two vectors.
- inline double deltaPhi(const Vector3& a, const FourMomentum& b) {
- return deltaPhi(a, b.vector3());
+ inline double deltaPhi(const Vector3& a, const FourMomentum& b, bool sign=false) {
+ return deltaPhi(a, b.vector3(), sign);
}
//@}
//////////////////////////////////////////////////////
/// @name \f$ |\Delta eta| \f$ calculations from 4-vectors
//@{
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(const FourMomentum& a, const FourMomentum& b) {
return deltaEta(a.vector3(), b.vector3());
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(const FourMomentum& v, double eta2) {
return deltaEta(v.vector3(), eta2);
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(double eta1, const FourMomentum& v) {
return deltaEta(eta1, v.vector3());
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(const FourVector& a, const FourVector& b) {
return deltaEta(a.vector3(), b.vector3());
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(const FourVector& v, double eta2) {
return deltaEta(v.vector3(), eta2);
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(double eta1, const FourVector& v) {
return deltaEta(eta1, v.vector3());
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(const FourVector& a, const FourMomentum& b) {
return deltaEta(a.vector3(), b.vector3());
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(const FourMomentum& a, const FourVector& b) {
return deltaEta(a.vector3(), b.vector3());
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(const FourVector& a, const Vector3& b) {
return deltaEta(a.vector3(), b);
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(const Vector3& a, const FourVector& b) {
return deltaEta(a, b.vector3());
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(const FourMomentum& a, const Vector3& b) {
return deltaEta(a.vector3(), b);
}
/// Calculate the difference in pseudorapidity between two vectors.
inline double deltaEta(const Vector3& a, const FourMomentum& b) {
return deltaEta(a, b.vector3());
}
//@}
/// @name \f$ |\Delta y| \f$ calculations from 4-momentum vectors
//@{
/// Calculate the difference in rapidity between two 4-momentum vectors.
inline double deltaRap(const FourMomentum& a, const FourMomentum& b) {
return deltaRap(a.rapidity(), b.rapidity());
}
/// Calculate the difference in rapidity between two 4-momentum vectors.
inline double deltaRap(const FourMomentum& v, double y2) {
return deltaRap(v.rapidity(), y2);
}
/// Calculate the difference in rapidity between two 4-momentum vectors.
inline double deltaRap(double y1, const FourMomentum& v) {
return deltaRap(y1, v.rapidity());
}
//@}
//////////////////////////////////////////////////////
/// @name 4-vector comparison functions (for sorting)
//@{
/// Comparison to give a sorting by decreasing pT
inline bool cmpMomByPt(const FourMomentum& a, const FourMomentum& b) {
return a.pt() > b.pt();
}
/// Comparison to give a sorting by increasing pT
inline bool cmpMomByAscPt(const FourMomentum& a, const FourMomentum& b) {
return a.pt() < b.pt();
}
/// Comparison to give a sorting by decreasing 3-momentum magnitude |p|
inline bool cmpMomByP(const FourMomentum& a, const FourMomentum& b) {
return a.vector3().mod() > b.vector3().mod();
}
/// Comparison to give a sorting by increasing 3-momentum magnitude |p|
inline bool cmpMomByAscP(const FourMomentum& a, const FourMomentum& b) {
return a.vector3().mod() < b.vector3().mod();
}
/// Comparison to give a sorting by decreasing transverse energy
inline bool cmpMomByEt(const FourMomentum& a, const FourMomentum& b) {
return a.Et() > b.Et();
}
/// Comparison to give a sorting by increasing transverse energy
inline bool cmpMomByAscEt(const FourMomentum& a, const FourMomentum& b) {
return a.Et() < b.Et();
}
/// Comparison to give a sorting by decreasing energy
inline bool cmpMomByE(const FourMomentum& a, const FourMomentum& b) {
return a.E() > b.E();
}
/// Comparison to give a sorting by increasing energy
inline bool cmpMomByAscE(const FourMomentum& a, const FourMomentum& b) {
return a.E() < b.E();
}
/// Comparison to give a sorting by decreasing mass
inline bool cmpMomByMass(const FourMomentum& a, const FourMomentum& b) {
return a.mass() > b.mass();
}
/// Comparison to give a sorting by increasing mass
inline bool cmpMomByAscMass(const FourMomentum& a, const FourMomentum& b) {
return a.mass() < b.mass();
}
/// Comparison to give a sorting by increasing eta (pseudorapidity)
inline bool cmpMomByEta(const FourMomentum& a, const FourMomentum& b) {
return a.eta() < b.eta();
}
/// Comparison to give a sorting by decreasing eta (pseudorapidity)
inline bool cmpMomByDescEta(const FourMomentum& a, const FourMomentum& b) {
return a.pseudorapidity() > b.pseudorapidity();
}
/// Comparison to give a sorting by increasing absolute eta (pseudorapidity)
inline bool cmpMomByAbsEta(const FourMomentum& a, const FourMomentum& b) {
return fabs(a.eta()) < fabs(b.eta());
}
/// Comparison to give a sorting by increasing absolute eta (pseudorapidity)
inline bool cmpMomByDescAbsEta(const FourMomentum& a, const FourMomentum& b) {
return fabs(a.eta()) > fabs(b.eta());
}
/// Comparison to give a sorting by increasing rapidity
inline bool cmpMomByRap(const FourMomentum& a, const FourMomentum& b) {
return a.rapidity() < b.rapidity();
}
/// Comparison to give a sorting by decreasing rapidity
inline bool cmpMomByDescRap(const FourMomentum& a, const FourMomentum& b) {
return a.rapidity() > b.rapidity();
}
/// Comparison to give a sorting by increasing absolute rapidity
inline bool cmpMomByAbsRap(const FourMomentum& a, const FourMomentum& b) {
return fabs(a.rapidity()) < fabs(b.rapidity());
}
/// Comparison to give a sorting by decreasing absolute rapidity
inline bool cmpMomByDescAbsRap(const FourMomentum& a, const FourMomentum& b) {
return fabs(a.rapidity()) > fabs(b.rapidity());
}
/// @todo Add sorting by phi [0..2PI]
/// Sort a container of momenta by cmp and return by reference for non-const inputs
template<typename MOMS, typename CMP>
inline MOMS& sortBy(MOMS& pbs, const CMP& cmp) {
std::sort(pbs.begin(), pbs.end(), cmp);
return pbs;
}
/// Sort a container of momenta by cmp and return by value for const inputs
template<typename MOMS, typename CMP>
inline MOMS sortBy(const MOMS& pbs, const CMP& cmp) {
MOMS rtn = pbs;
std::sort(rtn.begin(), rtn.end(), cmp);
return rtn;
}
/// Sort a container of momenta by pT (decreasing) and return by reference for non-const inputs
template<typename MOMS>
inline MOMS& sortByPt(MOMS& pbs) {
return sortBy(pbs, cmpMomByPt);
}
/// Sort a container of momenta by pT (decreasing) and return by value for const inputs
template<typename MOMS>
inline MOMS sortByPt(const MOMS& pbs) {
return sortBy(pbs, cmpMomByPt);
}
/// Sort a container of momenta by E (decreasing) and return by reference for non-const inputs
template<typename MOMS>
inline MOMS& sortByE(MOMS& pbs) {
return sortBy(pbs, cmpMomByE);
}
/// Sort a container of momenta by E (decreasing) and return by value for const inputs
template<typename MOMS>
inline MOMS sortByE(const MOMS& pbs) {
return sortBy(pbs, cmpMomByE);
}
/// Sort a container of momenta by Et (decreasing) and return by reference for non-const inputs
template<typename MOMS>
inline MOMS& sortByEt(MOMS& pbs) {
return sortBy(pbs, cmpMomByEt);
}
/// Sort a container of momenta by Et (decreasing) and return by value for const inputs
template<typename MOMS>
inline MOMS sortByEt(const MOMS& pbs) {
return sortBy(pbs, cmpMomByEt);
}
//@}
/// @name MT calculation
//@{
/// Calculate transverse mass of a visible and an invisible 3-vector
inline double mT(const Vector3& vis, const Vector3& invis) {
// return sqrt(2*vis.perp()*invis.perp() * (1 - cos(deltaPhi(vis, invis))) );
return mT(vis.perp(), invis.perp(), deltaPhi(vis, invis));
}
/// Calculate transverse mass of a visible and an invisible 4-vector
inline double mT(const FourMomentum& vis, const FourMomentum& invis) {
return mT(vis.p3(), invis.p3());
}
/// Calculate transverse mass of a visible 4-vector and an invisible 3-vector
inline double mT(const FourMomentum& vis, const Vector3& invis) {
return mT(vis.p3(), invis);
}
/// Calculate transverse mass of a visible 4-vector and an invisible 3-vector
inline double mT(const Vector3& vis, const FourMomentum& invis) {
return mT(vis, invis.p3());
}
//@}
//////////////////////////////////////////////////////
/// @name 4-vector string representations
//@{
/// Render a 4-vector as a string.
inline std::string toString(const FourVector& lv) {
ostringstream out;
out << "(" << (fabs(lv.t()) < 1E-30 ? 0.0 : lv.t())
<< "; " << (fabs(lv.x()) < 1E-30 ? 0.0 : lv.x())
<< ", " << (fabs(lv.y()) < 1E-30 ? 0.0 : lv.y())
<< ", " << (fabs(lv.z()) < 1E-30 ? 0.0 : lv.z())
<< ")";
return out.str();
}
/// Write a 4-vector to an ostream.
inline std::ostream& operator<<(std::ostream& out, const FourVector& lv) {
out << toString(lv);
return out;
}
//@}
/// @name Typedefs of vector types to short names
/// @todo Switch canonical and alias names
//@{
//typedef FourVector V4; //< generic
typedef FourVector X4; //< spatial
typedef FourMomentum P4; //< momentum
//@}
/// @name Typedefs for lists of vector types
//@{
typedef std::vector<FourVector> FourVectors;
typedef std::vector<FourMomentum> FourMomenta;
typedef std::vector<X4> X4s;
typedef std::vector<P4> P4a;
//@}
}
#endif
diff --git a/include/Rivet/Particle.hh b/include/Rivet/Particle.hh
--- a/include/Rivet/Particle.hh
+++ b/include/Rivet/Particle.hh
@@ -1,709 +1,713 @@
// -*- C++ -*-
#ifndef RIVET_Particle_HH
#define RIVET_Particle_HH
#include "Rivet/Particle.fhh"
#include "Rivet/ParticleBase.hh"
#include "Rivet/Config/RivetCommon.hh"
#include "Rivet/Tools/Cuts.hh"
#include "Rivet/Tools/Utils.hh"
#include "Rivet/Math/LorentzTrans.hh"
// NOTE: Rivet/Tools/ParticleUtils.hh included at the end
#include "fastjet/PseudoJet.hh"
namespace Rivet {
/// Particle representation, either from a HepMC::GenEvent or reconstructed.
class Particle : public ParticleBase {
public:
/// @name Constructors
//@{
/// Default constructor.
/// @note A particle without info is useless. This only exists to keep STL containers happy.
Particle()
: ParticleBase(),
- _original(nullptr), _id(PID::ANY)
- { }
+ _original(nullptr), _id(PID::ANY), _isDirect{false,false}
+ { }
/// Constructor without GenParticle.
Particle(PdgId pid, const FourMomentum& mom, const FourVector& pos=FourVector())
: ParticleBase(),
- _original(nullptr), _id(pid), _momentum(mom), _origin(pos)
- { }
+ _original(nullptr), _id(pid),
+ _momentum(mom), _origin(pos),
+ _isDirect{false,false}
+ { }
/// Constructor from a HepMC GenParticle pointer.
Particle(const GenParticle* gp)
: ParticleBase(),
_original(gp), _id(gp->pdg_id()),
- _momentum(gp->momentum())
+ _momentum(gp->momentum()),
+ _isDirect{false,false}
{
const GenVertex* vprod = gp->production_vertex();
if (vprod != nullptr) {
setOrigin(vprod->position().t(), vprod->position().x(), vprod->position().y(), vprod->position().z());
}
}
- /// Constructor from a HepMC GenParticle.
+ /// Constructor from a HepMC GenParticle reference.
Particle(const GenParticle& gp)
- : ParticleBase(),
- _original(&gp), _id(gp.pdg_id()),
- _momentum(gp.momentum())
- {
- const GenVertex* vprod = gp.production_vertex();
- if (vprod != nullptr) {
- setOrigin(vprod->position().t(), vprod->position().x(), vprod->position().y(), vprod->position().z());
- }
- }
+ : Particle(&gp)
+ { }
//@}
/// @name Kinematic properties
//@{
/// The momentum.
const FourMomentum& momentum() const {
return _momentum;
}
/// Set the momentum.
Particle& setMomentum(const FourMomentum& momentum) {
_momentum = momentum;
return *this;
}
/// Set the momentum via components.
Particle& setMomentum(double E, double px, double py, double pz) {
_momentum = FourMomentum(E, px, py, pz);
return *this;
}
/// Apply an active Lorentz transform to this particle
Particle& transformBy(const LorentzTransform& lt);
//@
/// @name Positional properties
//@{
/// The origin position.
const FourVector& origin() const {
return _origin;
}
/// Set the origin position.
Particle& setOrigin(const FourVector& position) {
_origin = position;
return *this;
}
/// Set the origin position via components.
Particle& setOrigin(double t, double x, double y, double z) {
_origin = FourMomentum(t, x, y, z);
return *this;
}
//@}
/// @name Other representations and implicit casts to momentum-like objects
//@{
/// Converter to FastJet3 PseudoJet
virtual fastjet::PseudoJet pseudojet() const {
return fastjet::PseudoJet(mom().px(), mom().py(), mom().pz(), mom().E());
}
/// Cast operator to FastJet3 PseudoJet
operator PseudoJet () const { return pseudojet(); }
/// Get a const pointer to the original GenParticle
const GenParticle* genParticle() const {
return _original;
}
/// Cast operator for conversion to GenParticle*
+ /// @todo This one's a bad idea since it enables accidental Particle comparisons
operator const GenParticle* () const { return genParticle(); }
//@}
/// @name Particle ID code accessors
//@{
/// This Particle's PDG ID code.
PdgId pid() const { return _id; }
/// Absolute value of the PDG ID code.
PdgId abspid() const { return std::abs(_id); }
/// This Particle's PDG ID code (alias).
/// @deprecated Prefer the pid/abspid form
PdgId pdgId() const { return _id; }
//@}
/// @name Charge
//@{
/// The charge of this Particle.
double charge() const { return PID::charge(pid()); }
/// The absolute charge of this Particle.
double abscharge() const { return PID::abscharge(pid()); }
/// Three times the charge of this Particle (i.e. integer multiple of smallest quark charge).
int charge3() const { return PID::charge3(pid()); }
/// Alias for charge3
/// @deprecated Use charge3
int threeCharge() const { return PID::threeCharge(pid()); }
/// Three times the absolute charge of this Particle (i.e. integer multiple of smallest quark charge).
int abscharge3() const { return PID::abscharge3(pid()); }
/// Is this Particle charged?
bool isCharged() const { return charge3() != 0; }
//@}
/// @name Particle species
//@{
/// Is this a hadron?
bool isHadron() const { return PID::isHadron(pid()); }
/// Is this a meson?
bool isMeson() const { return PID::isMeson(pid()); }
/// Is this a baryon?
bool isBaryon() const { return PID::isBaryon(pid()); }
/// Is this a lepton?
bool isLepton() const { return PID::isLepton(pid()); }
/// Is this a charged lepton?
bool isChargedLepton() const { return PID::isChargedLepton(pid()); }
/// Is this a neutrino?
bool isNeutrino() const { return PID::isNeutrino(pid()); }
/// Does this (hadron) contain a b quark?
bool hasBottom() const { return PID::hasBottom(pid()); }
/// Does this (hadron) contain a c quark?
bool hasCharm() const { return PID::hasCharm(pid()); }
// /// Does this (hadron) contain an s quark?
// bool hasStrange() const { return PID::hasStrange(pid()); }
/// Is this particle potentially visible in a detector?
bool isVisible() const;
+ /// Is this a parton? (Hopefully not very often... fiducial FTW)
+ bool isParton() const { return PID::isParton(pid()); }
+
//@}
/// @name Constituents (for composite particles)
//@{
/// Set direct constituents of this particle
virtual void setConstituents(const Particles& cs, bool setmom=false);
/// Add a single direct constituent to this particle
virtual void addConstituent(const Particle& c, bool addmom=false);
/// Add direct constituents to this particle
virtual void addConstituents(const Particles& cs, bool addmom=false);
/// Determine if this Particle is a composite of other Rivet Particles
bool isComposite() const { return !constituents().empty(); }
/// @brief Direct constituents of this particle, returned by reference
///
/// The returned vector will be empty if this particle is non-composite,
/// and its entries may themselves be composites.
const Particles& constituents() const { return _constituents; }
/// @brief Direct constituents of this particle, sorted by a functor
/// @note Returns a copy, thanks to the sorting
const Particles constituents(const ParticleSorter& sorter) const {
return sortBy(constituents(), sorter);
}
/// @brief Direct constituents of this particle, filtered by a Cut
/// @note Returns a copy, thanks to the filtering
const Particles constituents(const Cut& c) const {
return filter_select(constituents(), c);
}
/// @brief Direct constituents of this particle, sorted by a functor
/// @note Returns a copy, thanks to the filtering and sorting
const Particles constituents(const Cut& c, const ParticleSorter& sorter) const {
return sortBy(constituents(c), sorter);
}
/// @brief Direct constituents of this particle, filtered by a selection functor
/// @note Returns a copy, thanks to the filtering
const Particles constituents(const ParticleSelector& selector) const {
return filter_select(constituents(), selector);
}
/// @brief Direct constituents of this particle, filtered and sorted by functors
/// @note Returns a copy, thanks to the filtering and sorting
const Particles constituents(const ParticleSelector& selector, const ParticleSorter& sorter) const {
return sortBy(constituents(selector), sorter);
}
/// @brief Fundamental constituents of this particle
/// @note Returns {{*this}} if this particle is non-composite.
Particles rawConstituents() const;
/// @brief Fundamental constituents of this particle, sorted by a functor
/// @note Returns a copy, thanks to the sorting
const Particles rawConstituents(const ParticleSorter& sorter) const {
return sortBy(rawConstituents(), sorter);
}
/// @brief Fundamental constituents of this particle, filtered by a Cut
/// @note Returns a copy, thanks to the filtering
const Particles rawConstituents(const Cut& c) const {
return filter_select(rawConstituents(), c);
}
/// @brief Fundamental constituents of this particle, sorted by a functor
/// @note Returns a copy, thanks to the filtering and sorting
const Particles rawConstituents(const Cut& c, const ParticleSorter& sorter) const {
return sortBy(rawConstituents(c), sorter);
}
/// @brief Fundamental constituents of this particle, filtered by a selection functor
/// @note Returns a copy, thanks to the filtering
const Particles rawConstituents(const ParticleSelector& selector) const {
return filter_select(rawConstituents(), selector);
}
/// @brief Fundamental constituents of this particle, filtered and sorted by functors
/// @note Returns a copy, thanks to the filtering and sorting
const Particles rawConstituents(const ParticleSelector& selector, const ParticleSorter& sorter) const {
return sortBy(rawConstituents(selector), sorter);
}
//@}
/// @name Ancestry (for fundamental particles with a HepMC link)
//@{
/// Get a list of the direct parents of the current particle (with optional selection Cut)
///
/// @note This is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
Particles parents(const Cut& c=Cuts::OPEN) const;
/// Get a list of the direct parents of the current particle (with selector function)
///
/// @note This is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
Particles parents(const ParticleSelector& f) const {
return filter_select(parents(), f);
}
/// Check whether any particle in the particle's parent list has the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasParentWith(const ParticleSelector& f) const {
return !parents(f).empty();
}
/// Check whether any particle in the particle's parent list has the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasParentWith(const Cut& c) const;
/// Check whether any particle in the particle's parent list does not have the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasParentWithout(const ParticleSelector& f) const {
return hasParentWith([&](const Particle& p){ return !f(p); });
}
/// Check whether any particle in the particle's parent list does not have the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasParentWithout(const Cut& c) const;
/// Check whether a given PID is found in the particle's parent list
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
///
/// @deprecated Prefer e.g. hasParentWith(Cut::pid == 123)
//DEPRECATED("Prefer e.g. hasParentWith(Cut::pid == 123)");
bool hasParent(PdgId pid) const;
/// Get a list of the ancestors of the current particle (with optional selection Cut)
///
/// @note By default only physical ancestors, with status=2, are returned.
///
/// @note This is valid in MC, but may not be answerable experimentally --
/// use this function with care when replicating experimental analyses!
Particles ancestors(const Cut& c=Cuts::OPEN, bool only_physical=true) const;
/// Get a list of the direct parents of the current particle (with selector function)
///
/// @note By default only physical ancestors, with status=2, are returned.
///
/// @note This is valid in MC, but may not be answerable experimentally --
/// use this function with care when replicating experimental analyses!
Particles ancestors(const ParticleSelector& f, bool only_physical=true) const {
return filter_select(ancestors(Cuts::OPEN, only_physical), f);
}
/// Check whether any particle in the particle's ancestor list has the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasAncestorWith(const ParticleSelector& f, bool only_physical=true) const {
return !ancestors(f, only_physical).empty();
}
/// Check whether any particle in the particle's ancestor list has the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasAncestorWith(const Cut& c, bool only_physical=true) const;
/// Check whether any particle in the particle's ancestor list does not have the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasAncestorWithout(const ParticleSelector& f, bool only_physical=true) const {
return hasAncestorWith([&](const Particle& p){ return !f(p); }, only_physical);
}
/// Check whether any particle in the particle's ancestor list does not have the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasAncestorWithout(const Cut& c, bool only_physical=true) const;
/// Check whether a given PID is found in the particle's ancestor list
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
///
/// @deprecated Prefer hasAncestorWith(Cuts::pid == pid) etc.
//DEPRECATED("Prefer e.g. hasAncestorWith(Cut::pid == 123)");
bool hasAncestor(PdgId pid, bool only_physical=true) const;
/// @brief Determine whether the particle is from a b-hadron decay
///
/// @note This question is valid in MC, but may not be perfectly answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool fromBottom() const;
/// @brief Determine whether the particle is from a c-hadron decay
///
/// @note If a hadron contains b and c quarks it is considered a bottom
/// hadron and NOT a charm hadron.
///
/// @note This question is valid in MC, but may not be perfectly answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool fromCharm() const;
// /// @brief Determine whether the particle is from a s-hadron decay
// ///
// /// @note If a hadron contains b or c quarks as well as strange it is
// /// considered a b or c hadron, but NOT a strange hadron.
// ///
// /// @note This question is valid in MC, but may not be perfectly answerable
// /// experimentally -- use this function with care when replicating
// /// experimental analyses!
// bool fromStrange() const;
/// @brief Determine whether the particle is from a hadron decay
///
/// @note This question is valid in MC, but may not be perfectly answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool fromHadron() const;
/// @brief Determine whether the particle is from a tau decay
///
/// @note This question is valid in MC, but may not be perfectly answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool fromTau(bool prompt_taus_only=false) const;
/// @brief Determine whether the particle is from a prompt tau decay
///
/// @note This question is valid in MC, but may not be perfectly answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool fromPromptTau() const { return fromTau(true); }
/// @brief Determine whether the particle is from a tau which decayed hadronically
///
/// @note This question is valid in MC, but may not be perfectly answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool fromHadronicTau(bool prompt_taus_only=false) const;
/// @brief Determine whether the particle is from a hadron or tau decay
///
/// Specifically, walk up the ancestor chain until a status 2 hadron or
/// tau is found, if at all.
///
/// @note This question is valid in MC, but may not be perfectly answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
///
/// @deprecated Too vague: use fromHadron or fromHadronicTau
bool fromDecay() const { return fromHadron() || fromPromptTau(); }
/// @brief Shorthand definition of 'promptness' based on set definition flags
///
/// A "direct" particle is one directly connected to the hard process. It is a
/// preferred alias for "prompt", since it has no confusing implications about
/// distinguishability by timing information.
///
/// The boolean arguments allow a decay lepton to be considered direct if
/// its parent was a "real" direct lepton.
///
/// @note This one doesn't make any judgements about final-stateness
bool isDirect(bool allow_from_direct_tau=false, bool allow_from_direct_mu=false) const;
/// Alias for isDirect
bool isPrompt(bool allow_from_prompt_tau=false, bool allow_from_prompt_mu=false) const {
return isDirect(allow_from_prompt_tau, allow_from_prompt_mu);
}
//@}
/// @name Decay info
//@{
/// Whether this particle is stable according to the generator
bool isStable() const;
/// @todo isDecayed? How to restrict to physical particles?
/// Get a list of the direct descendants from the current particle (with optional selection Cut)
Particles children(const Cut& c=Cuts::OPEN) const;
/// Get a list of the direct descendants from the current particle (with selector function)
Particles children(const ParticleSelector& f) const {
return filter_select(children(), f);
}
/// Check whether any direct child of this particle has the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasChildWith(const ParticleSelector& f) const {
return !children(f).empty();
}
/// Check whether any direct child of this particle has the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasChildWith(const Cut& c) const;
/// Check whether any direct child of this particle does not have the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasChildWithout(const ParticleSelector& f) const {
return hasChildWith([&](const Particle& p){ return !f(p); });
}
/// Check whether any direct child of this particle does not have the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasChildWithout(const Cut& c) const;
/// Get a list of all the descendants from the current particle (with optional selection Cut)
Particles allDescendants(const Cut& c=Cuts::OPEN, bool remove_duplicates=true) const;
/// Get a list of all the descendants from the current particle (with selector function)
Particles allDescendants(const ParticleSelector& f, bool remove_duplicates=true) const {
return filter_select(allDescendants(Cuts::OPEN, remove_duplicates), f);
}
/// Check whether any descendant of this particle has the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasDescendantWith(const ParticleSelector& f, bool remove_duplicates=true) const {
return !allDescendants(f, remove_duplicates).empty();
}
/// Check whether any descendant of this particle has the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasDescendantWith(const Cut& c, bool remove_duplicates=true) const;
/// Check whether any descendant of this particle does not have the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasDescendantWithout(const ParticleSelector& f, bool remove_duplicates=true) const {
return hasDescendantWith([&](const Particle& p){ return !f(p); }, remove_duplicates);
}
/// Check whether any descendant of this particle does not have the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasDescendantWithout(const Cut& c, bool remove_duplicates=true) const;
/// Get a list of all the stable descendants from the current particle (with optional selection Cut)
///
/// @todo Use recursion through replica-avoiding MCUtils functions to avoid bookkeeping duplicates
/// @todo Insist that the current particle is post-hadronization, otherwise throw an exception?
Particles stableDescendants(const Cut& c=Cuts::OPEN) const;
/// Get a list of all the stable descendants from the current particle (with selector function)
Particles stableDescendants(const ParticleSelector& f) const {
return filter_select(stableDescendants(), f);
}
/// Check whether any stable descendant of this particle has the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasStableDescendantWith(const ParticleSelector& f) const {
return !stableDescendants(f).empty();
}
/// Check whether any stable descendant of this particle has the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasStableDescendantWith(const Cut& c) const;
/// Check whether any stable descendant of this particle does not have the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasStableDescendantWithout(const ParticleSelector& f) const {
return hasStableDescendantWith([&](const Particle& p){ return !f(p); });
}
/// Check whether any stable descendant of this particle does not have the requested property
///
/// @note This question is valid in MC, but may not be answerable
/// experimentally -- use this function with care when replicating
/// experimental analyses!
bool hasStableDescendantWithout(const Cut& c) const;
/// Flight length (divide by mm or cm to get the appropriate units)
double flightLength() const;
//@}
/// @name Duplicate testing
//@{
/// @brief Determine whether a particle is the first in a decay chain to meet the function requirement
inline bool isFirstWith(const ParticleSelector& f) const {
if (!f(*this)) return false; //< This doesn't even meet f, let alone being the last to do so
if (any(parents(), f)) return false; //< If a direct parent has this property, this isn't the first
return true;
}
/// @brief Determine whether a particle is the first in a decay chain not to meet the function requirement
inline bool isFirstWithout(const ParticleSelector& f) const {
return isFirstWith([&](const Particle& p){ return !f(p); });
}
/// @brief Determine whether a particle is the last in a decay chain to meet the function requirement
inline bool isLastWith(const ParticleSelector& f) const {
if (!f(*this)) return false; //< This doesn't even meet f, let alone being the last to do so
if (any(children(), f)) return false; //< If a child has this property, this isn't the last
return true;
}
/// @brief Determine whether a particle is the last in a decay chain not to meet the function requirement
inline bool isLastWithout(const ParticleSelector& f) const {
return isLastWith([&](const Particle& p){ return !f(p); });
}
//@}
protected:
/// A pointer to the original GenParticle from which this Particle is projected (may be null)
const GenParticle* _original;
/// Constituent particles if this is a composite (may be empty)
Particles _constituents;
/// The PDG ID code for this Particle.
PdgId _id;
/// The momentum of this particle.
FourMomentum _momentum;
/// The creation position of this particle.
FourVector _origin;
+ /// Cached computation of directness, via ancestry. Second element is cache status
+ /// @todo Replace this awkward caching with C++17 std::optional
+ mutable std::pair<bool,bool> _isDirect;
+
};
/// @name String representation and streaming support
//@{
/// Allow a Particle to be passed to an ostream.
std::ostream& operator << (std::ostream& os, const Particle& p);
/// Allow ParticlePair to be passed to an ostream.
std::ostream& operator << (std::ostream& os, const ParticlePair& pp);
//@}
}
#include "Rivet/Tools/ParticleUtils.hh"
#endif
diff --git a/include/Rivet/Projections/DressedLeptons.hh b/include/Rivet/Projections/DressedLeptons.hh
--- a/include/Rivet/Projections/DressedLeptons.hh
+++ b/include/Rivet/Projections/DressedLeptons.hh
@@ -1,136 +1,171 @@
// -*- C++ -*-
#ifndef RIVET_DressedLeptons_HH
#define RIVET_DressedLeptons_HH
#include "Rivet/Projection.hh"
#include "Rivet/Projections/FinalState.hh"
#include "Rivet/Projections/IdentifiedFinalState.hh"
#include "Rivet/Config/RivetCommon.hh"
namespace Rivet {
/// A charged lepton meta-particle created by clustering photons close to the bare lepton
/// @todo Remove completely -- it's unnecessary and too confusing (esp. between copying & aggregating)
/// @deprecated Just use Particle.constituents() now.
class DressedLepton : public Particle {
public:
/// Copy constructor (from Particle)
DressedLepton(const Particle& dlepton);
/// Components constructor
/// @note This is not a copy constructor, hence the explicit second argument even if empty
DressedLepton(const Particle& lepton, const Particles& photons, bool momsum=true);
/// Add a photon to the dressed lepton
/// @todo Deprecate and override add/setConstituents instead?
void addPhoton(const Particle& p, bool momsum=true);
/// Retrieve the bare lepton
const Particle& bareLepton() const;
/// Retrieve the bare lepton (alias)
/// @deprecated Prefer the more physicsy bareLepton()
const Particle& constituentLepton() const { return bareLepton(); }
/// Retrieve the clustered photons
const Particles photons() const { return slice(constituents(), 1); }
/// Retrieve the clustered photons (alias)
/// @deprecated Prefer the shorter photons()
const Particles constituentPhotons() const { return photons(); }
};
- /// @brief Cluster photons from a given FS to all charged particles (typically leptons)
+ /// @brief Cluster photons from a given FS to charged leptons
///
- /// This stores the original (bare) charged particles and photons as particles()
- /// while the newly created clustered lepton objects are accessible as
- /// dressedLeptons(). The clustering is done by a delta(R) cone around each bare
- /// lepton, with double counting being avoided by only adding a photon to the _closest_
- /// bare lepton if it happens to be within the capture radius of more than one.
+ /// This stores the original (bare) charged particles and photons as
+ /// particles() while the newly created clustered lepton objects are
+ /// accessible as dressedLeptons(). The clustering is done by a delta(R) cone
+ /// around each bare lepton or by jet clustering. In both modes, double
+ /// counting is avoided: for the dR clustering, a photon is only added to the
+ /// _closest_ bare lepton if it happens to be within the capture radius of
+ /// more than one; for the jet clustering, only the bare lepton with the
+ /// highest pT is retained if more than one is clustered into a jet.
class DressedLeptons : public FinalState {
public:
/// @brief Constructor with a single input FinalState (used for both photons and bare leptons)
///
- /// Provide a single final state projection used to select the photons and bare
- /// leptons, a photon-clustering delta(R) cone size around each bare lepton, and an optional
- /// cut on the _dressed_ leptons (i.e. the momenta after clustering).
- /// The final argument controls whether non-prompt photons are to be included.
- /// Set the clustering radius to 0 or negative to disable clustering.
+ /// Provide a single final state projection used to select the photons and
+ /// bare leptons, a photon-clustering delta(R) cone size around each bare
+ /// lepton, and an optional cut on the _dressed_ leptons (i.e. the momenta
+ /// after clustering). The final arguments control whether non-prompt
+ /// photons are to be included, and whether the matching of photons to
+ /// leptons is to be done via dR matching to the bare lepton or by a jet
+ /// clustering algorithm. Set the clustering radius to 0 or negative to
+ /// disable clustering.
DressedLeptons(const FinalState& barefs,
double dRmax, const Cut& cut=Cuts::open(),
- bool useDecayPhotons=false);
+ bool useDecayPhotons=false,
+ bool useJetClustering=false);
+
+ /// @brief Constructor with default input FinalState
+ ///
+ /// DressedLepton construction from a default-constructed FinalState.
+ /// Provide a photon-clustering delta(R) cone size around each bare
+ /// lepton, and an optional cut on the _dressed_ leptons (i.e. the momenta
+ /// after clustering). The final arguments control whether non-prompt
+ /// photons are to be included, and whether the matching of photons to
+ /// leptons is to be done via dR matching to the bare lepton or by a jet
+ /// clustering algorithm. Set the clustering radius to 0 or negative to
+ /// disable clustering.
+ DressedLeptons(double dRmax, const Cut& cut=Cuts::open(),
+ bool useDecayPhotons=false,
+ bool useJetClustering=false)
+ : DressedLeptons(FinalState(), dRmax, cut, useDecayPhotons, useJetClustering)
+ { }
/// @brief Constructor with distinct photon and lepton finders
///
/// Provide final state projections used to select the photons and bare
- /// leptons (wish we had put the first two args the other way around...),
- /// a clustering delta(R) cone size around each bare lepton, and an optional
- /// cut on the _dressed_ leptons (i.e. the momenta after clustering.)
- /// The final argument controls whether non-prompt photons are to be included.
- /// Set the clustering radius to 0 or negative to disable clustering.
+ /// leptons, a
+ /// clustering delta(R) cone size around each bare lepton, and an optional
+ /// cut on the _dressed_ leptons (i.e. the momenta after clustering.) The
+ /// final arguments control whether non-prompt photons are to be included,
+ /// and whether the matching of photons to leptons is to be done via dR
+ /// matching to the bare lepton or by a jet clustering algorithm. Set the
+ /// clustering radius to 0 or negative to disable clustering.
+ ///
+ /// @note Wish we had put the first two args the other way around...
///
/// @todo Convert second arg to a general ParticleFinder rather than an FS, to
/// allow clustering on to unstables, e.g. taus via TauFinder.
DressedLeptons(const FinalState& photons, const FinalState& bareleptons,
double dRmax, const Cut& cut=Cuts::open(),
- bool useDecayPhotons=false);
+ bool useDecayPhotons=false,
+ bool useJetClustering=false);
// For compatibility only
/// @cond INTERNAL
DEPRECATED("Use the new form with no bool cluster argument")
DressedLeptons(const FinalState& photons, const FinalState& bareleptons,
- double dRmax, const Cut& cut, bool, bool useDecayPhotons)
- : DressedLeptons(photons, bareleptons, dRmax, cut, useDecayPhotons)
+ double dRmax, const Cut& cut, bool,
+ bool useDecayPhotons, bool useJetClustering)
+ : DressedLeptons(photons, bareleptons, dRmax, cut, useDecayPhotons, useJetClustering)
{ }
/// @endcond
+
/// Clone this projection
DEFAULT_RIVET_PROJ_CLONE(DressedLeptons);
+
/// @brief Retrieve the dressed leptons
/// @note Like particles() but with helper functions
vector<DressedLepton> dressedLeptons() const {
vector<DressedLepton> rtn;
for (const Particle& p : particles(cmpMomByPt))
rtn += DressedLepton(p); //static_cast<const DressedLepton>(p);
return rtn;
}
/// @brief Retrieve the dressed leptons ordered by supplied sorting functor
/// @note Like particles() but with helper functions
vector<DressedLepton> dressedLeptons(const ParticleSorter& sorter) const {
vector<DressedLepton> rtn;
for (const Particle& p : particles(sorter))
rtn += DressedLepton(p); //static_cast<const DressedLepton>(p);
return rtn;
}
protected:
/// Apply the projection on the supplied event.
void project(const Event& e);
/// Compare projections.
int compare(const Projection& p) const;
private:
/// Maximum cone radius to find photons in
double _dRmax;
/// Whether to include photons from hadron (particularly pi0) and hadronic tau decays
bool _fromDecay;
+ /// Whether to use a jet clustering algorithm rather than nearest-lepton association
+ bool _useJetClustering;
+
+
};
}
#endif
diff --git a/include/Rivet/Projections/IdentifiedFinalState.hh b/include/Rivet/Projections/IdentifiedFinalState.hh
--- a/include/Rivet/Projections/IdentifiedFinalState.hh
+++ b/include/Rivet/Projections/IdentifiedFinalState.hh
@@ -1,136 +1,134 @@
// -*- C++ -*-
#ifndef RIVET_IdentifiedFinalState_HH
#define RIVET_IdentifiedFinalState_HH
#include "Rivet/Projections/FinalState.hh"
namespace Rivet {
/// @brief Produce a final state which only contains specified particle IDs.
class IdentifiedFinalState : public FinalState {
public:
/// @name Constructors
//@{
/// Constructor with a FinalState and optional list of PDG ID codes.
IdentifiedFinalState(const FinalState& fsp, const vector<PdgId>& pids=vector<PdgId>());
/// Constructor with a list of PDG ID codes and a FinalState
/// @deprecated Use the version with FinalState as 1st arg
DEPRECATED("Use the version with FinalState as 1st arg")
IdentifiedFinalState(const vector<PdgId>& pids, const FinalState& fsp);
/// Constructor with a FinalState and a single PDG ID code.
IdentifiedFinalState(const FinalState& fsp, PdgId pid);
/// Constructor with a single PDG ID code and a FinalState.
/// @deprecated Use the version with FinalState as 1st arg
DEPRECATED("Use the version with FinalState as 1st arg")
IdentifiedFinalState(PdgId pid, const FinalState& fsp);
/// Construction using optional Cuts object and optional list of PDG ID codes
IdentifiedFinalState(const Cut& c=Cuts::open(), const vector<PdgId>& pids=vector<PdgId>());
/// Construction using list of PDG ID codes and an optional Cuts object
IdentifiedFinalState(const vector<PdgId>& pids, const Cut& c=Cuts::open());
/// Construction using Cuts object and a single PDG ID code
IdentifiedFinalState(const Cut& c, PdgId pid);
/// Construction using a single PDG ID code and an optional Cuts object
IdentifiedFinalState(PdgId pid, const Cut& c=Cuts::open());
/// Clone on the heap.
DEFAULT_RIVET_PROJ_CLONE(IdentifiedFinalState);
//@}
/// Get the list of particle IDs to accept.
const set<PdgId>& acceptedIds() const {
return _pids;
}
/// Add an accepted particle ID.
IdentifiedFinalState& acceptId(PdgId pid) {
_pids.insert(pid);
return *this;
}
/// Add a set of accepted particle IDs.
IdentifiedFinalState& acceptIds(const vector<PdgId>& pids) {
- foreach (const PdgId pid, pids) {
- _pids.insert(pid);
- }
+ for (const PdgId pid : pids) _pids.insert(pid);
return *this;
}
/// Add an accepted particle ID and its antiparticle.
IdentifiedFinalState& acceptIdPair(PdgId pid) {
_pids.insert(pid);
_pids.insert(-pid);
return *this;
}
/// Add a set of accepted particle IDs and their antiparticles.
IdentifiedFinalState& acceptIdPairs(const vector<PdgId>& pids) {
- foreach (const PdgId pid, pids) {
+ for (const PdgId pid : pids) {
_pids.insert(pid);
_pids.insert(-pid);
}
return *this;
}
/// Accept all neutrinos (convenience method).
IdentifiedFinalState& acceptNeutrinos() {
acceptIdPair(PID::NU_E);
acceptIdPair(PID::NU_MU);
acceptIdPair(PID::NU_TAU);
return *this;
}
/// Accept all charged leptons (convenience method).
IdentifiedFinalState& acceptChLeptons() {
acceptIdPair(PID::ELECTRON);
acceptIdPair(PID::MUON);
acceptIdPair(PID::TAU);
return *this;
}
/// Reset the list of particle IDs to accept.
void reset() {
_pids.clear();
}
// The remaining particles
virtual const Particles& remainingParticles() const {
return _remainingParticles;
}
/// Apply the projection on the supplied event.
void project(const Event& e);
/// Compare projections.
int compare(const Projection& p) const;
private:
/// The final-state particles.
set<PdgId> _pids;
// A vector of all other particles in the final state
Particles _remainingParticles;
};
}
#endif
diff --git a/include/Rivet/Projections/MergedFinalState.hh b/include/Rivet/Projections/MergedFinalState.hh
--- a/include/Rivet/Projections/MergedFinalState.hh
+++ b/include/Rivet/Projections/MergedFinalState.hh
@@ -1,46 +1,47 @@
// -*- C++ -*-
#ifndef RIVET_MergedFinalState_HH
#define RIVET_MergedFinalState_HH
#include "Rivet/Tools/Logging.hh"
#include "Rivet/Config/RivetCommon.hh"
#include "Rivet/Particle.hh"
#include "Rivet/Event.hh"
#include "Rivet/Projection.hh"
#include "Rivet/Projections/FinalState.hh"
namespace Rivet {
/// @brief Get final state particles merged from two FinalState projections.
+ ///
+ /// @todo Extend to merging many FS projections
class MergedFinalState : public FinalState {
-
public:
/// @name Constructors
//@{
MergedFinalState(const FinalState& fspa, const FinalState& fspb) {
setName("MergedFinalState");
addProjection(fspa, "FSA");
addProjection(fspb, "FSB");
}
/// Clone on the heap.
DEFAULT_RIVET_PROJ_CLONE(MergedFinalState);
//@}
protected:
/// Apply the projection on the supplied event.
void project(const Event& e);
/// Compare projections.
int compare(const Projection& p) const;
};
}
#endif
diff --git a/include/Rivet/Projections/PartonicTops.hh b/include/Rivet/Projections/PartonicTops.hh
--- a/include/Rivet/Projections/PartonicTops.hh
+++ b/include/Rivet/Projections/PartonicTops.hh
@@ -1,107 +1,115 @@
// -*- C++ -*-
#ifndef RIVET_PartonicTops_HH
#define RIVET_PartonicTops_HH
#include "Rivet/Projections/ParticleFinder.hh"
namespace Rivet {
/// @brief Convenience finder of partonic top quarks
///
/// @warning Requires there to be tops in the event record. A fiducial pseudo-top
/// analysis approach is strongly recommended instead of this.
class PartonicTops : public ParticleFinder {
public:
/// @brief Enum for categorising top quark decay modes
///
/// More specifically, the decay mode of the W from the top. We presume top decay to a W and b quark.
enum DecayMode { ALL = 0, ANY = 0, ELECTRON, MUON, TAU, E_MU, E_MU_TAU, HADRONIC };
+ /// @brief Enum for categorising which top quark to be selected: last (weakly decaying) or first?
+ enum TopMode { FIRST, LAST };
+
/// @name Constructors
//@{
/// Constructor optionally taking cuts object
- PartonicTops(const Cut& c=Cuts::OPEN)
- : ParticleFinder(c), _decaymode(ALL), _emu_from_prompt_tau(true), _include_hadronic_taus(false)
+ PartonicTops(const Cut& c=Cuts::OPEN, TopMode whichtop=LAST)
+ : ParticleFinder(c), _topmode(whichtop), _decaymode(ALL),
+ _emu_from_prompt_tau(true), _include_hadronic_taus(false)
{ }
/// Constructor taking decay mode details (and an optional cuts object)
- PartonicTops(DecayMode decaymode, bool emu_from_prompt_tau=true, bool include_hadronic_taus=false, const Cut& c=Cuts::OPEN)
- : ParticleFinder(c), _decaymode(decaymode),
+ PartonicTops(DecayMode decaymode, bool emu_from_prompt_tau=true, bool include_hadronic_taus=false, const Cut& c=Cuts::OPEN, TopMode whichtop=LAST)
+ : ParticleFinder(c), _topmode(whichtop), _decaymode(decaymode),
_emu_from_prompt_tau(emu_from_prompt_tau), _include_hadronic_taus(include_hadronic_taus)
{ }
/// Constructor taking decay mode details (and an optional cuts object)
- PartonicTops(DecayMode decaymode, const Cut& c, bool emu_from_prompt_tau=true, bool include_hadronic_taus=false)
- : ParticleFinder(c), _decaymode(decaymode),
+ PartonicTops(DecayMode decaymode, const Cut& c, bool emu_from_prompt_tau=true, bool include_hadronic_taus=false, TopMode whichtop=LAST)
+ : ParticleFinder(c), _topmode(whichtop), _decaymode(decaymode),
_emu_from_prompt_tau(emu_from_prompt_tau), _include_hadronic_taus(include_hadronic_taus)
{ }
/// Clone on the heap.
DEFAULT_RIVET_PROJ_CLONE(PartonicTops);
//@}
/// Access to the found partonic tops
const Particles& tops() const { return _theParticles; }
/// Clear the projection
void clear() {
_theParticles.clear();
}
protected:
/// Apply the projection on the supplied event.
void project(const Event& event) {
// Find partonic tops
- _theParticles = filter_select(event.allParticles(_cuts), lastParticleWith(isTop));
+ _theParticles = filter_select(event.allParticles(_cuts), (_topmode == LAST ? lastParticleWith(isTop) : firstParticleWith(isTop)));
// Filtering by decay mode
if (_decaymode != ALL) {
const auto fn = [&](const Particle& t) {
const Particles descendants = t.allDescendants();
const bool prompt_e = any(descendants, [&](const Particle& p){ return p.abspid() == PID::ELECTRON && p.isPrompt(_emu_from_prompt_tau) && !p.hasAncestor(PID::PHOTON, false); });
const bool prompt_mu = any(descendants, [&](const Particle& p){ return p.abspid() == PID::MUON && p.isPrompt(_emu_from_prompt_tau) && !p.hasAncestor(PID::PHOTON, false); });
if (prompt_e && (_decaymode == ELECTRON || _decaymode == E_MU || _decaymode == E_MU_TAU)) return true;
if (prompt_mu && (_decaymode == MUON || _decaymode == E_MU || _decaymode == E_MU_TAU)) return true;
const bool prompt_tau = any(descendants, [&](const Particle& p){ return p.abspid() == PID::TAU && p.isPrompt() && !p.hasAncestor(PID::PHOTON, false); });
const bool prompt_hadronic_tau = any(descendants, [&](const Particle& p){ return p.abspid() == PID::TAU && p.isPrompt() && !p.hasAncestor(PID::PHOTON, false) && none(p.children(), isChargedLepton); });
if (prompt_tau && (_decaymode == TAU || _decaymode == E_MU_TAU)) return (_include_hadronic_taus || !prompt_hadronic_tau);
if (_decaymode == HADRONIC && (!prompt_e && !prompt_mu && (!prompt_tau || (_include_hadronic_taus && prompt_hadronic_tau)))) return true; //< logical hairiness...
return false;
};
ifilter_select(_theParticles, fn);
}
}
/// Compare projections.
int compare(const Projection& p) const {
const PartonicTops& other = dynamic_cast<const PartonicTops&>(p);
- return cmp(_cuts, other._cuts) || cmp(_decaymode, other._decaymode) ||
+ return cmp(_cuts, other._cuts) ||
+ cmp(_topmode, other._topmode) ||
+ cmp(_decaymode, other._decaymode) ||
cmp(_emu_from_prompt_tau, other._emu_from_prompt_tau) ||
cmp(_include_hadronic_taus, other._include_hadronic_taus);
}
private:
+ TopMode _topmode;
+
DecayMode _decaymode;
bool _emu_from_prompt_tau, _include_hadronic_taus;
};
}
#endif
diff --git a/include/Rivet/Projections/VetoedFinalState.hh b/include/Rivet/Projections/VetoedFinalState.hh
--- a/include/Rivet/Projections/VetoedFinalState.hh
+++ b/include/Rivet/Projections/VetoedFinalState.hh
@@ -1,181 +1,236 @@
// -*- C++ -*-
#ifndef RIVET_VetoedFinalState_HH
#define RIVET_VetoedFinalState_HH
#include "Rivet/Projections/FinalState.hh"
namespace Rivet {
/// @brief FS modifier to exclude classes of particles from the final state.
class VetoedFinalState : public FinalState {
public:
- /// Typedef for a pair of back-to-back cuts.
- typedef pair<double, double> BinaryCut;
-
- /// Typedef for a vetoing entry.
- typedef map<long, BinaryCut> VetoDetails;
-
- /// Typedef for a veto on a composite particle mass.
- typedef multimap<int, BinaryCut> CompositeVeto;
-
-
/// @name Constructors
//@{
- /// Default constructor.
- VetoedFinalState() {
- setName("VetoedFinalState");
- addProjection(FinalState(), "FS");
- }
- /// Constructor with specific FinalState.
- VetoedFinalState(const FinalState& fsp)
+ /// Constructor with a specific FinalState and a cuts list to veto
+ VetoedFinalState(const FinalState& fsp, const vector<Cut>& cuts)
+ : FinalState(), _vetoCuts(cuts)
{
setName("VetoedFinalState");
addProjection(fsp, "FS");
}
- /// You can add a map of ID plus a pair containing \f$ p_{Tmin} \f$ and
- /// \f$ p_{Tmax} \f$ - these define the range of particles to be vetoed.
- VetoedFinalState(const VetoDetails& vetocodes)
- : _vetoCodes(vetocodes)
+ /// Constructor with a specific FinalState and a single cut to veto
+ VetoedFinalState(const FinalState& fsp, const Cut& cut)
+ : VetoedFinalState(fsp, vector<Cut>{cut})
+ { }
+
+ /// Constructor with a default FinalState and a cuts list to veto
+ VetoedFinalState(const vector<Cut>& cuts)
+ : VetoedFinalState(FinalState(), cuts)
+ { }
+
+ /// Constructor with a default FinalState and a single cut to veto
+ VetoedFinalState(const Cut& cut)
+ : VetoedFinalState(FinalState(), {cut})
+ { }
+
+ /// Constructor with a specific FinalState and a PID list to veto
+ VetoedFinalState(const FinalState& fsp, const vector<PdgId>& vetopids)
+ : VetoedFinalState(fsp, {})
{
- setName("VetoedFinalState");
- addProjection(FinalState(), "FS");
+ _vetoCuts.reserve(vetopids.size());
+ for (PdgId pid : vetopids) addVeto(pid);
}
+ /// Constructor with a specific FinalState and a PID to veto
+ VetoedFinalState(const FinalState& fsp, PdgId vetopid)
+ : VetoedFinalState(fsp, {Cuts::pid == vetopid})
+ { }
+
+ /// Constructor with a default FinalState and a PID list to veto
+ VetoedFinalState(const vector<PdgId>& vetopids)
+ : VetoedFinalState(FinalState(), {})
+ {
+ _vetoCuts.reserve(vetopids.size());
+ for (PdgId pid : vetopids) addVeto(pid);
+ }
+
+ /// Constructor with a default FinalState and a PID to veto
+ VetoedFinalState(PdgId vetopid)
+ : VetoedFinalState(FinalState(), {Cuts::pid == vetopid})
+ { }
+
+ /// Constructor with specific FinalState but no cuts
+ VetoedFinalState(const FinalState& fsp)
+ : VetoedFinalState(fsp, vector<Cut>())
+ { }
+
+ /// Default constructor with default FinalState and no cuts
+ VetoedFinalState()
+ : VetoedFinalState(FinalState(), vector<Cut>())
+ { }
+
/// You can add a map of ID plus a pair containing \f$ p_{Tmin} \f$ and
- /// \f$ p_{Tmax} \f$ - these define the range of particles to be vetoed.
- /// This version also supplies a specific FinalState to be used.
- VetoedFinalState(const FinalState& fsp, const VetoDetails& vetocodes)
- : _vetoCodes(vetocodes)
+ /// \f$ p_{Tmax} \f$ -- these define the range of particles to be vetoed.
+ //DEPRECATED("Prefer constructors using Cut arguments")
+ VetoedFinalState(const map<PdgId,pair<double,double>>& vetocodes)
+ : VetoedFinalState(FinalState(), {})
{
- setName("VetoedFinalState");
- addProjection(fsp, "FS");
+ for (const auto& it : vetocodes) {
+ addVeto(it.first, Cuts::pT > it.second.first && Cuts::pT < it.second.second);
+ }
}
/// Clone on the heap.
DEFAULT_RIVET_PROJ_CLONE(VetoedFinalState);
//@}
/// Get the list of particle IDs and \f$ p_T \f$ ranges to veto.
- const VetoDetails& vetoDetails() const {
- return _vetoCodes;
+ const vector<Cut>& vetoDetails() const {
+ return _vetoCuts;
}
+ //using vetos = vetoDetails;
- /// Add a particle ID and \f$ p_T \f$ range to veto. Particles with \f$ p_T \f$
- /// IN the given range will be rejected.
- VetoedFinalState& addVetoDetail(const long id, const double ptmin, const double ptmax) {
- BinaryCut ptrange(ptmin, ptmax);
- _vetoCodes.insert(make_pair(id, ptrange));
+
+ /// Add a particle selection to be vetoed from the final state
+ VetoedFinalState& addVeto(const Cut& cut) {
+ _vetoCuts.push_back(cut);
return *this;
}
- /// Add a particle/antiparticle pair to veto in a given \f$ p_T \f$ range. Given a single ID, both
- /// the particle and its conjugate antiparticle will be rejected if their \f$ p_T \f$ is IN the given range.
- VetoedFinalState& addVetoPairDetail(const long id, const double ptmin, const double ptmax) {
- addVetoDetail(id, ptmin, ptmax);
- addVetoDetail(-id, ptmin, ptmax);
+ /// Add a particle selection to be vetoed from the final state
+ VetoedFinalState& addVeto(PdgId pid, const Cut& cut=Cuts::OPEN) {
+ _vetoCuts.push_back(Cuts::pid == pid && cut);
return *this;
}
- /// Add a particle/antiparticle pair to veto. Given a single ID, both the particle and its corresponding
- /// antiparticle (for all \f$ p_T \f$ values) will be vetoed.
- VetoedFinalState& addVetoPairId(const long id) {
- addVetoId(id);
- addVetoId(-id);
+ /// Add a particle/antiparticle selection to be vetoed from the final state
+ VetoedFinalState& addVetoPair(PdgId pid, const Cut& cut=Cuts::OPEN) {
+ _vetoCuts.push_back(Cuts::abspid == pid && cut);
return *this;
}
- /// Add a particle ID to veto (all \f$ p_T \f$ range will be vetoed).
- VetoedFinalState& addVetoId(const long id) {
- BinaryCut ptrange(0.0, numeric_limits<double>::max());
- _vetoCodes.insert(make_pair(id, ptrange));
+
+ /// @brief Add a particle ID and \f$ p_T \f$ range to veto
+ ///
+ /// Particles with \f$ p_T \f$ IN the given range will be rejected.
+ VetoedFinalState& addVetoDetail(PdgId pid, double ptmin, double ptmax=numeric_limits<double>::max()) {
+ return addVeto(pid, Cuts::ptIn(ptmin, ptmax));
+ }
+ //const auto addVeto = addVetoDetail;
+
+ /// @brief Add a particle/antiparticle pair to veto in a given \f$ p_T \f$ range
+ ///
+ /// Given a single ID, both the particle and its conjugate antiparticle will
+ /// be rejected if their \f$ p_T \f$ is IN the given range.
+ VetoedFinalState& addVetoPairDetail(PdgId pid, double ptmin, double ptmax=numeric_limits<double>::max()) {
+ return addVetoPair(pid, Cuts::ptIn(ptmin, ptmax));
+ }
+ //using addVetoPair = addVetoPairDetail;
+
+ /// @brief Add a particle ID to veto (all \f$ p_T \f$ range will be vetoed)
+ VetoedFinalState& addVetoId(PdgId pid) {
+ return addVeto(pid);
+ }
+ //using addVeto = addVetoId;
+
+ /// @brief Add a particle/antiparticle pair to veto
+ ///
+ /// Given a single ID, both the particle and its corresponding antiparticle
+ /// (for all \f$ p_T \f$ values) will be vetoed.
+ VetoedFinalState& addVetoPairId(PdgId pid) {
+ return addVetoPair(pid);
+ }
+ //using addVetoPair = addVetoPairId;
+
+
+ /// Set the list of particle selections to veto
+ VetoedFinalState& setVetoDetails(const vector<Cut>& cuts) {
+ _vetoCuts = cuts;
return *this;
}
+ //const auto setVetos = setVetoDetails;
+
/// Veto all neutrinos (convenience method)
VetoedFinalState& vetoNeutrinos() {
addVetoPairId(PID::NU_E);
addVetoPairId(PID::NU_MU);
addVetoPairId(PID::NU_TAU);
return *this;
}
+
/// Add a veto on composite masses within a given width.
/// The composite mass is composed of nProducts decay products
/// @ todo might we want to specify a range of pdg ids for the decay products?
- VetoedFinalState& addCompositeMassVeto(const double &mass, const double &width, int nProducts=2){
- double halfWidth = 0.5*width;
- BinaryCut massRange(mass - halfWidth, mass + halfWidth);
+ VetoedFinalState& addCompositeMassVeto(double mass, double width, int nProducts=2) {
+ const double halfWidth = 0.5*width;
+ pair<double,double> massRange(mass-halfWidth, mass+halfWidth);
_compositeVetoes.insert(make_pair(nProducts, massRange));
_nCompositeDecays.insert(nProducts);
return *this;
}
- /// Veto the decay products of particle with pdg id
+
+ /// Veto the decay products of particle with PDG code @a pid
/// @todo Need HepMC to sort themselves out and keep vector bosons from
/// the hard vtx in the event record before this will work reliably for all pdg ids
- VetoedFinalState& addDecayProductsVeto(const long id) {
- _parentVetoes.insert(id);
+ VetoedFinalState& addDecayProductsVeto(PdgId pid) {
+ _parentVetoes.insert(pid);
return *this;
}
- /// Set the list of particle IDs and \f$ p_T \f$ ranges to veto.
- VetoedFinalState& setVetoDetails(const VetoDetails& ids) {
- _vetoCodes = ids;
- return *this;
- }
-
- /// Clear the list of particle IDs and ranges to veto.
- VetoedFinalState& reset() {
- _vetoCodes.clear();
- return *this;
- }
-
-
/// Veto particles from a supplied final state
VetoedFinalState& addVetoOnThisFinalState(const ParticleFinder& fs) {
const string name = "FS_" + to_str(_vetofsnames.size());
addProjection(fs, name);
_vetofsnames.insert(name);
return *this;
}
+ /// Clear the list of particle IDs and ranges to veto.
+ VetoedFinalState& reset() {
+ _vetoCuts.clear();
+ return *this;
+ }
+
+
/// Apply the projection on the supplied event.
void project(const Event& e);
/// Compare projections.
int compare(const Projection& p) const;
private:
- /// The final-state particles.
- VetoDetails _vetoCodes;
+ /// The veto cuts
+ vector<Cut> _vetoCuts;
/// Composite particle masses to veto
- CompositeVeto _compositeVetoes;
+ /// @todo Also generalise to use Cuts
+ multimap<PdgId, pair<double,double> > _compositeVetoes;
set<int> _nCompositeDecays;
- typedef set<long> ParentVetos;
-
/// Set of decaying particle IDs to veto
- ParentVetos _parentVetoes;
+ set<PdgId> _parentVetoes;
/// Set of finalstate to be vetoed
set<string> _vetofsnames;
};
}
#endif
diff --git a/include/Rivet/Tools/JetUtils.hh b/include/Rivet/Tools/JetUtils.hh
--- a/include/Rivet/Tools/JetUtils.hh
+++ b/include/Rivet/Tools/JetUtils.hh
@@ -1,200 +1,210 @@
#ifndef RIVET_JETUTILS_HH
#define RIVET_JETUTILS_HH
#include "Rivet/Jet.hh"
#include "Rivet/Tools/ParticleBaseUtils.hh"
namespace Rivet {
/// @name Unbound functions for converting between Jets, Particles and PseudoJets
//@{
inline PseudoJets mkPseudoJets(const Particles& ps) {
PseudoJets rtn; rtn.reserve(ps.size());
for (const Particle& p : ps)
rtn.push_back(p);
return rtn;
}
inline PseudoJets mkPseudoJets(const Jets& js) {
PseudoJets rtn; rtn.reserve(js.size());
for (const Jet& j : js)
rtn.push_back(j);
return rtn;
}
inline Jets mkJets(const PseudoJets& pjs) {
Jets rtn; rtn.reserve(pjs.size());
for (const PseudoJet& pj : pjs)
rtn.push_back(pj);
return rtn;
}
//@}
/// @name Jet classifier -> bool functors
//@{
/// std::function instantiation for functors taking a Jet and returning a bool
using JetSelector = function<bool(const Jet&)>;
/// std::function instantiation for functors taking two Jets and returning a bool
using JetSorter = function<bool(const Jet&, const Jet&)>;
/// Base type for Jet -> bool functors
struct BoolJetFunctor {
virtual bool operator()(const Jet& p) const = 0;
virtual ~BoolJetFunctor() {}
};
/// Functor for and-combination of selector logic
struct BoolJetAND : public BoolJetFunctor {
BoolJetAND(const std::vector<JetSelector>& sels) : selectors(sels) {}
BoolJetAND(const JetSelector& a, const JetSelector& b) : selectors({a,b}) {}
BoolJetAND(const JetSelector& a, const JetSelector& b, const JetSelector& c) : selectors({a,b,c}) {}
bool operator()(const Jet& j) const {
for (const JetSelector& sel : selectors) if (!sel(j)) return false;
return true;
}
std::vector<JetSelector> selectors;
};
/// Operator syntactic sugar for AND construction
inline BoolJetAND operator && (const JetSelector& a, const JetSelector& b) {
return BoolJetAND(a, b);
}
/// Functor for or-combination of selector logic
struct BoolJetOR : public BoolJetFunctor {
BoolJetOR(const std::vector<JetSelector>& sels) : selectors(sels) {}
BoolJetOR(const JetSelector& a, const JetSelector& b) : selectors({a,b}) {}
BoolJetOR(const JetSelector& a, const JetSelector& b, const JetSelector& c) : selectors({a,b,c}) {}
bool operator()(const Jet& j) const {
for (const JetSelector& sel : selectors) if (sel(j)) return true;
return false;
}
std::vector<JetSelector> selectors;
};
/// Operator syntactic sugar for OR construction
inline BoolJetOR operator || (const JetSelector& a, const JetSelector& b) {
return BoolJetOR(a, b);
}
/// Functor for inverting selector logic
struct BoolJetNOT : public BoolJetFunctor {
BoolJetNOT(const JetSelector& sel) : selector(sel) {}
bool operator()(const Jet& j) const { return !selector(j); }
JetSelector selector;
};
/// Operator syntactic sugar for NOT construction
inline BoolJetNOT operator ! (const JetSelector& a) {
return BoolJetNOT(a);
}
/// B-tagging functor, with a tag selection cut as the stored state
struct HasBTag : BoolJetFunctor {
HasBTag(const Cut& c=Cuts::open()) : cut(c) {}
// HasBTag(const std::function<bool(const Jet& j)>& f) : selector(f) {}
bool operator() (const Jet& j) const { return j.bTagged(cut); }
// const std::function<bool(const Jet& j)> selector;
const Cut cut;
};
using hasBTag = HasBTag;
/// C-tagging functor, with a tag selection cut as the stored state
struct HasCTag : BoolJetFunctor {
HasCTag(const Cut& c=Cuts::open()) : cut(c) {}
// HasCTag(const std::function<bool(const Jet& j)>& f) : selector(f) {}
bool operator() (const Jet& j) const { return j.cTagged(cut); }
// const std::function<bool(const Jet& j)> selector;
const Cut cut;
};
using hasCTag = HasCTag;
+ /// Anti-B/C-tagging functor, with a tag selection cut as the stored state
+ struct HasNoTag : BoolJetFunctor {
+ HasNoTag(const Cut& c=Cuts::open()) : cut(c) {}
+ // HasNoTag(const std::function<bool(const Jet& j)>& f) : selector(f) {}
+ bool operator() (const Jet& j) const { return !j.bTagged(cut) && j.cTagged(cut); }
+ // const std::function<bool(const Jet& j)> selector;
+ const Cut cut;
+ };
+ using hasNoTag = HasNoTag;
+
//@}
/// @name Unbound functions for filtering jets
//@{
/// Filter a jet collection in-place to the subset that passes the supplied Cut
Jets& ifilter_select(Jets& jets, const Cut& c);
/// Alias for ifilter_select
/// @deprecated Use ifilter_select
inline Jets& ifilterBy(Jets& jets, const Cut& c) { return ifilter_select(jets, c); }
/// Filter a jet collection in-place to the subset that passes the supplied Cut
inline Jets filter_select(const Jets& jets, const Cut& c) {
Jets rtn = jets;
return ifilter_select(rtn, c);
}
/// Alias for ifilter_select
/// @deprecated Use filter_select
inline Jets filterBy(const Jets& jets, const Cut& c) { return filter_select(jets, c); }
/// Filter a jet collection in-place to the subset that passes the supplied Cut
inline Jets filter_select(const Jets& jets, const Cut& c, Jets& out) {
out = filter_select(jets, c);
return out;
}
/// Alias for ifilter_select
/// @deprecated Use filter_select
inline Jets filterBy(const Jets& jets, const Cut& c, Jets& out) { return filter_select(jets, c, out); }
/// Filter a jet collection in-place to the subset that fails the supplied Cut
Jets& ifilter_discard(Jets& jets, const Cut& c);
/// Filter a jet collection in-place to the subset that fails the supplied Cut
inline Jets filter_discard(const Jets& jets, const Cut& c) {
Jets rtn = jets;
return ifilter_discard(rtn, c);
}
/// Filter a jet collection in-place to the subset that fails the supplied Cut
inline Jets filter_discard(const Jets& jets, const Cut& c, Jets& out) {
out = filter_discard(jets, c);
return out;
}
//@}
/// @name Operations on collections of Jet
/// @note This can't be done on generic collections of ParticleBase -- thanks, C++ :-/
//@{
namespace Kin {
inline double sumPt(const Jets& js) {
return sum(js, pT, 0.0);
}
inline FourMomentum sumP4(const Jets& js) {
return sum(js, p4, FourMomentum());
}
inline Vector3 sumP3(const Jets& js) {
return sum(js, p3, Vector3());
}
/// @todo Min dPhi, min dR?
/// @todo Isolation routines?
}
//@}
// Import Kin namespace into Rivet
using namespace Kin;
}
#endif
diff --git a/include/Rivet/Tools/Nsubjettiness/AxesDefinition.hh b/include/Rivet/Tools/Nsubjettiness/AxesDefinition.hh
deleted file mode 100644
--- a/include/Rivet/Tools/Nsubjettiness/AxesDefinition.hh
+++ /dev/null
@@ -1,1282 +0,0 @@
-// Nsubjettiness Package
-// Questions/Comments? jthaler@jthaler.net
-//
-// Copyright (c) 2011-14
-// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
-//
-// $Id: AxesDefinition.hh 833 2015-07-23 14:35:23Z jthaler $
-//----------------------------------------------------------------------
-// This file is part of FastJet contrib.
-//
-// It is free software; you can redistribute it and/or modify it under
-// the terms of the GNU General Public License as published by the
-// Free Software Foundation; either version 2 of the License, or (at
-// your option) any later version.
-//
-// It is distributed in the hope that it will be useful, but WITHOUT
-// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
-// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
-// License for more details.
-//
-// You should have received a copy of the GNU General Public License
-// along with this code. If not, see <http://www.gnu.org/licenses/>.
-//----------------------------------------------------------------------
-
-#ifndef __FASTJET_CONTRIB_AXES_DEFINITION_HH__
-#define __FASTJET_CONTRIB_AXES_DEFINITION_HH__
-
-
-#include "MeasureDefinition.hh"
-#include "ExtraRecombiners.hh"
-
-#include "fastjet/PseudoJet.hh"
-#include <fastjet/LimitedWarning.hh>
-
-#include <iomanip>
-#include <cmath>
-#include <vector>
-#include <list>
-
-namespace Rivet {
-
-namespace Nsubjettiness { using namespace fastjet;
-
-// The following AxesDefinitions are currently available (and the relevant arguments, if needed)
-class KT_Axes;
-class CA_Axes;
-class AntiKT_Axes; // (R0)
-class WTA_KT_Axes;
-class WTA_CA_Axes;
-class GenKT_Axes; // (p, R0 = infinity)
-class WTA_GenKT_Axes; // (p, R0 = infinity)
-class GenET_GenKT_Axes; // (delta, p, R0 = infinity)
-class Manual_Axes;
-
-class OnePass_KT_Axes;
-class OnePass_CA_Axes;
-class OnePass_AntiKT_Axes; // (R0)
-class OnePass_WTA_KT_Axes;
-class OnePass_WTA_CA_Axes;
-class OnePass_GenKT_Axes; // (p, R0 = infinity)
-class OnePass_WTA_GenKT_Axes; // (p, R0 = infinity)
-class OnePass_GenET_GenKT_Axes; // (delta, p, R0 = infinity)
-class OnePass_Manual_Axes;
-
-class MultiPass_Axes; // (NPass) (currently only defined for KT_Axes)
-class MultiPass_Manual_Axes; // (NPass)
-
-class Comb_GenKT_Axes; // (nExtra, p, R0 = infinity)
-class Comb_WTA_GenKT_Axes; // (nExtra, p, R0 = infinity)
-class Comb_GenET_GenKT_Axes; // (nExtra, delta, p, R0 = infinity)
-
-///////
-//
-// AxesDefinition
-//
-///////
-
-///------------------------------------------------------------------------
-/// \class AxesDefinition
-/// \brief Base class for axes definitions
-///
-/// A generic AxesDefinition first finds a set of seed axes.
-/// Then, if desired, uses measure information
-/// (from MeasureDefinition) to refine those axes starting from those seed axes.
-/// The AxesDefinitions are typically based on sequential jet algorithms.
-///------------------------------------------------------------------------
-class AxesDefinition {
-
-public:
-
- /// This function should be overloaded in all derived classes, and defines how to find the seed axes.
- /// If desired, the measure information (which might be NULL) can be used to test multiple axes choices, but should
- /// not be used for iterative refining (since that is the job of MeasureDefinition).
- virtual std::vector<fastjet::PseudoJet> get_starting_axes(int n_jets,
- const std::vector<fastjet::PseudoJet>& inputs,
- const MeasureDefinition * measure) const = 0;
-
- /// Short description of AxesDefinitions (and any parameters)
- virtual std::string short_description() const = 0;
-
- /// Long description of AxesDefinitions (and any parameters)
- virtual std::string description() const = 0;
-
- /// This has to be defined in all derived classes, and allows these to be copied around.
- virtual AxesDefinition* create() const = 0;
-
-public:
-
- /// Starting from seeds, refine axes using one or more passes.
- /// Note that in order to do >0 passes, we need information from the MeasureDefinition about how to do the appropriate minimization.
- std::vector<fastjet::PseudoJet> get_refined_axes(int n_jets,
- const std::vector<fastjet::PseudoJet>& inputs,
- const std::vector<fastjet::PseudoJet>& seedAxes,
- const MeasureDefinition * measure = NULL) const {
-
- assert(n_jets == (int)seedAxes.size()); //added int casting to get rid of compiler warning
-
- if (_Npass == 0) {
- // no refining, just use seeds
- return seedAxes;
- } else if (_Npass == 1) {
- if (measure == NULL) throw Error("AxesDefinition: One-pass minimization requires specifying a MeasureDefinition.");
-
- // do one pass minimum using measure definition
- return measure->get_one_pass_axes(n_jets, inputs, seedAxes,_nAttempts,_accuracy);
- } else {
- if (measure == NULL) throw Error("AxesDefinition: Multi-pass minimization requires specifying a MeasureDefinition.");
- return get_multi_pass_axes(n_jets, inputs, seedAxes, measure);
- }
- }
-
- /// Combines get_starting_axes with get_refined_axes.
- /// In the Njettiness class, these two steps are done separately in order to store seed axes information.
- std::vector<fastjet::PseudoJet> get_axes(int n_jets,
- const std::vector<fastjet::PseudoJet>& inputs,
- const MeasureDefinition * measure = NULL) const {
- std::vector<fastjet::PseudoJet> seedAxes = get_starting_axes(n_jets, inputs, measure);
- return get_refined_axes(n_jets,inputs,seedAxes,measure);
- }
-
-
- /// Short-hand for the get_axes function. Useful when trying to write terse code.
- inline std::vector<fastjet::PseudoJet> operator() (int n_jets,
- const std::vector<fastjet::PseudoJet>& inputs,
- const MeasureDefinition * measure = NULL) const {
- return get_axes(n_jets,inputs,measure);
- }
-
- /// \enum AxesRefiningEnum
- /// Defines the cases of zero pass and one pass for convenience
- enum AxesRefiningEnum {
- UNDEFINED_REFINE = -1, // added to create a default value
- NO_REFINING = 0,
- ONE_PASS = 1,
- MULTI_PASS = 100,
- };
-
- /// A integer that is used externally to decide how to do multi-pass minimization
- int nPass() const { return _Npass; }
-
- /// A flag that indicates whether results are deterministics.
- bool givesRandomizedResults() const {
- return (_Npass > 1);
- }
-
- /// A flag that indicates whether manual axes are being used.
- bool needsManualAxes() const {
- return _needsManualAxes; // if there is no starting axes finder
- }
-
- /// Allows user to change number of passes. Also used internally to set nPass.
- /// Can also specify details of one/multi pass minimziation
- void setNPass(int nPass,
- int nAttempts = 1000,
- double accuracy = 0.0001,
- double noise_range = 1.0 // only needed for MultiPass minimization
- )
- {
- _Npass = nPass;
- _nAttempts = nAttempts;
- _accuracy = accuracy;
- _noise_range = noise_range;
- if (nPass < 0) throw Error("AxesDefinition requires a nPass >= 0");
- }
-
- /// Destructor
- virtual ~AxesDefinition() {};
-
-protected:
-
- /// Default constructor contains no information. Number of passes has to be set
- /// manually by derived classes using setNPass function.
- AxesDefinition() : _Npass(UNDEFINED_REFINE),
- _nAttempts(0),
- _accuracy(0.0),
- _noise_range(0.0),
- _needsManualAxes(false) {}
-
- /// Does multi-pass minimization by randomly jiggling the axes within _noise_range
- std::vector<fastjet::PseudoJet> get_multi_pass_axes(int n_jets,
- const std::vector<fastjet::PseudoJet>& inputs,
- const std::vector<fastjet::PseudoJet>& seedAxes,
- const MeasureDefinition* measure) const;
-
- /// Function to jiggle axes within _noise_range
- PseudoJet jiggle(const PseudoJet& axis) const;
-
- int _Npass; ///< Number of passes (0 = no refining, 1 = one-pass, >1 multi-pass)
- int _nAttempts; ///< Number of attempts per pass
- double _accuracy; ///< Accuracy goal per pass
- double _noise_range; ///< Noise in rapidity/phi (for multi-pass minimization only)
- bool _needsManualAxes; ///< Flag to indicate special case of manual axes
-};
-
-///------------------------------------------------------------------------
-/// \class ExclusiveJetAxes
-/// \brief Base class for axes defined from exclusive jet algorithm
-///
-/// This class finds axes by clustering particles with an exclusive jet definition.
-/// This can be implemented with different jet algorithms. The user can call this directly
-/// using their favorite fastjet::JetDefinition
-///------------------------------------------------------------------------
-class ExclusiveJetAxes : public AxesDefinition {
-
-public:
- /// Constructor takes JetDefinition as an argument
- ExclusiveJetAxes(fastjet::JetDefinition def)
- : AxesDefinition(), _def(def) {
- setNPass(NO_REFINING); // default to no minimization
- }
-
- /// Starting axes obtained by creating a cluster sequenence and running exclusive_jets.
- virtual std::vector<fastjet::PseudoJet> get_starting_axes(int n_jets,
- const std::vector <fastjet::PseudoJet> & inputs,
- const MeasureDefinition * ) const {
- fastjet::ClusterSequence jet_clust_seq(inputs, _def);
-
- std::vector<fastjet::PseudoJet> axes = jet_clust_seq.exclusive_jets_up_to(n_jets);
-
- if ((int)axes.size() < n_jets) {
- _too_few_axes_warning.warn("ExclusiveJetAxes::get_starting_axes: Fewer than N axes found; results are unpredictable.");
- axes.resize(n_jets); // resize to make sure there are enough axes to not yield an error elsewhere
- }
-
- return axes;
- }
-
- /// Short description
- virtual std::string short_description() const { return "ExclAxes";}
- /// Long description
- virtual std::string description() const { return "ExclAxes: " + _def.description();}
-
- /// To make it possible to copy around.
- virtual ExclusiveJetAxes* create() const {return new ExclusiveJetAxes(*this);}
-
-private:
- fastjet::JetDefinition _def; ///< Jet definition to use.
- static LimitedWarning _too_few_axes_warning;
-};
-
-///------------------------------------------------------------------------
-/// \class ExclusiveCombinatorialJetAxes
-/// \brief Base class for axes defined from exclusive jet algorithm, checking combinatorial options
-///
-/// This class finds axes by clustering particles with an exclusive jet definition.
-/// It takes an extra number of jets (specificed by the user via nExtra), and then finds the set of N that minimizes N-jettiness.
-/// WARNING: If one wants to be guarenteed that results improve by increasing nExtra, then one should use
-/// winner-take-all-style recombination schemes
-///------------------------------------------------------------------------
-class ExclusiveCombinatorialJetAxes : public AxesDefinition {
-
-public:
- /// Constructor takes JetDefinition and nExtra as options (nExtra=0 acts the same as ExclusiveJetAxes)
- ExclusiveCombinatorialJetAxes(fastjet::JetDefinition def, int nExtra = 0)
- : AxesDefinition(), _def(def), _nExtra(nExtra) {
- if (nExtra < 0) throw Error("Need nExtra >= 0");
- setNPass(NO_REFINING); // default to no minimization
- }
-
- /// Find n_jets + _nExtra axes, and then choose the n_jets subset with the smallest N-(sub)jettiness value.
- virtual std::vector<fastjet::PseudoJet> get_starting_axes(int n_jets,
- const std::vector<fastjet::PseudoJet> & inputs,
- const MeasureDefinition *measure) const {
- int starting_number = n_jets + _nExtra;
- fastjet::ClusterSequence jet_clust_seq(inputs, _def);
- std::vector<fastjet::PseudoJet> starting_axes = jet_clust_seq.exclusive_jets_up_to(starting_number);
-
- if ((int)starting_axes.size() < n_jets) {
- _too_few_axes_warning.warn("ExclusiveCombinatorialJetAxes::get_starting_axes: Fewer than N + nExtra axes found; results are unpredictable.");
- starting_axes.resize(n_jets); // resize to make sure there are enough axes to not yield an error elsewhere
- }
-
- std::vector<fastjet::PseudoJet> final_axes;
-
- // check so that no computation time is wasted if there are no extra axes
- if (_nExtra == 0) final_axes = starting_axes;
-
- else {
-
- // define string of 1's based on number of desired jets
- std::string bitmask(n_jets, 1);
- // expand the array size to the total number of jets with extra 0's at the end, makes string easy to permute
- bitmask.resize(starting_number, 0);
-
- double min_tau = std::numeric_limits<double>::max();
- std::vector<fastjet::PseudoJet> temp_axes;
-
- do {
-
- temp_axes.clear();
-
- // only take an axis if it is listed as true (1) in the string
- for (int i = 0; i < (int)starting_axes.size(); ++i) {
- if (bitmask[i]) temp_axes.push_back(starting_axes[i]);
- }
-
- double temp_tau = measure->result(inputs, temp_axes);
- if (temp_tau < min_tau) {
- min_tau = temp_tau;
- final_axes = temp_axes;
- }
-
- // permutes string of 1's and 0's according to next lexicographic ordering and returns true
- // continues to loop through all possible lexicographic orderings
- // returns false and breaks the loop when there are no more possible orderings
- } while (std::prev_permutation(bitmask.begin(), bitmask.end()));
- }
-
- return final_axes;
- }
-
- /// Short description
- virtual std::string short_description() const { return "ExclCombAxes";}
- /// Long description
- virtual std::string description() const { return "ExclCombAxes: " + _def.description();}
- /// To make it possible to copy around.
- virtual ExclusiveCombinatorialJetAxes* create() const {return new ExclusiveCombinatorialJetAxes(*this);}
-
-private:
- fastjet::JetDefinition _def; ///< Jet definition to use
- int _nExtra; ///< Extra axes to find
- static LimitedWarning _too_few_axes_warning;
-};
-
-///------------------------------------------------------------------------
-/// \class HardestJetAxes
-/// \brief Base class for axes defined from an inclusive jet algorithm
-///
-/// This class finds axes by running an inclusive algorithm and then finding the n hardest jets.
-/// This can be implemented with different jet algorithms, and can be called by the user.
-///------------------------------------------------------------------------
-class HardestJetAxes : public AxesDefinition {
-public:
- /// Constructor takes JetDefinition
- HardestJetAxes(fastjet::JetDefinition def)
- : AxesDefinition(), _def(def) {
- setNPass(NO_REFINING); // default to no minimization
- }
-
- /// Finds seed axes by running a ClusterSequence, running inclusive_jets, and finding the N hardest
- virtual std::vector<fastjet::PseudoJet> get_starting_axes(int n_jets,
- const std::vector <fastjet::PseudoJet> & inputs,
- const MeasureDefinition * ) const {
- fastjet::ClusterSequence jet_clust_seq(inputs, _def);
- std::vector<fastjet::PseudoJet> axes = sorted_by_pt(jet_clust_seq.inclusive_jets());
-
- if ((int)axes.size() < n_jets) {
- _too_few_axes_warning.warn("HardestJetAxes::get_starting_axes: Fewer than N axes found; results are unpredictable.");
- }
-
- axes.resize(n_jets); // only keep n hardest
- return axes;
- }
-
- /// Short description
- virtual std::string short_description() const { return "HardAxes";}
- /// Long description
- virtual std::string description() const { return "HardAxes: " + _def.description();}
- /// To make it possible to copy around.
- virtual HardestJetAxes* create() const {return new HardestJetAxes(*this);}
-
-private:
- fastjet::JetDefinition _def; ///< Jet Definition to use.
-
- static LimitedWarning _too_few_axes_warning;
-
-};
-
-///------------------------------------------------------------------------
-/// \class KT_Axes
-/// \brief Axes from exclusive kT
-///
-/// Axes from kT algorithm with E_scheme recombination.
-///------------------------------------------------------------------------
-class KT_Axes : public ExclusiveJetAxes {
-public:
- /// Constructor
- KT_Axes()
- : ExclusiveJetAxes(fastjet::JetDefinition(fastjet::kt_algorithm,
- fastjet::JetDefinition::max_allowable_R, //maximum jet radius constant
- fastjet::E_scheme,
- fastjet::Best)
- ) {
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "KT";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "KT Axes";
- return stream.str();
- };
-
- /// For copying purposes
- virtual KT_Axes* create() const {return new KT_Axes(*this);}
-
-};
-
-///------------------------------------------------------------------------
-/// \class CA_Axes
-/// \brief Axes from exclusive CA
-///
-/// Axes from CA algorithm with E_scheme recombination.
-///------------------------------------------------------------------------
-class CA_Axes : public ExclusiveJetAxes {
-public:
- /// Constructor
- CA_Axes()
- : ExclusiveJetAxes(fastjet::JetDefinition(fastjet::cambridge_algorithm,
- fastjet::JetDefinition::max_allowable_R, //maximum jet radius constant
- fastjet::E_scheme,
- fastjet::Best)
- ) {
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "CA";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "CA Axes";
- return stream.str();
- };
-
- /// For copying purposes
- virtual CA_Axes* create() const {return new CA_Axes(*this);}
-
-};
-
-
-///------------------------------------------------------------------------
-/// \class AntiKT_Axes
-/// \brief Axes from inclusive anti-kT
-///
-/// Axes from anti-kT algorithm and E_scheme.
-/// The one parameter R0 is subjet radius
-///------------------------------------------------------------------------
-class AntiKT_Axes : public HardestJetAxes {
-
-public:
- /// Constructor. Takes jet radius as argument
- AntiKT_Axes(double R0)
- : HardestJetAxes(fastjet::JetDefinition(fastjet::antikt_algorithm,
- R0,
- fastjet::E_scheme,
- fastjet::Best)
- ), _R0(R0) {
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "AKT" << _R0;
- return stream.str();
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "Anti-KT Axes (R0 = " << _R0 << ")";
- return stream.str();
- };
-
- /// For copying purposes
- virtual AntiKT_Axes* create() const {return new AntiKT_Axes(*this);}
-
-protected:
- double _R0; ///< AKT jet radius
-
-};
-
-///------------------------------------------------------------------------
-/// \class JetDefinitionWrapper
-/// \brief Wrapper for jet definitions (for memory management)
-///
-/// This class was introduced to avoid issue of a FastJet bug when using genKT clustering
-/// Now using this for all AxesDefinition with a manual recombiner to use the delete_recombiner_when_unused function
-///------------------------------------------------------------------------
-class JetDefinitionWrapper {
-
-public:
-
- /// Default Constructor
- JetDefinitionWrapper(JetAlgorithm jet_algorithm_in, double R_in, double xtra_param_in, const JetDefinition::Recombiner *recombiner) {
- jet_def = fastjet::JetDefinition(jet_algorithm_in, R_in, xtra_param_in);
- jet_def.set_recombiner(recombiner);
- jet_def.delete_recombiner_when_unused(); // added to prevent memory leaks
- }
-
- /// Additional constructor so that build-in FastJet algorithms can also be called
- JetDefinitionWrapper(JetAlgorithm jet_algorithm_in, double R_in, const JetDefinition::Recombiner *recombiner, fastjet::Strategy strategy_in) {
- jet_def = fastjet::JetDefinition(jet_algorithm_in, R_in, recombiner, strategy_in);
- jet_def.delete_recombiner_when_unused();
- }
-
- /// Return jet definition
- JetDefinition getJetDef() {
- return jet_def;
- }
-
-private:
- JetDefinition jet_def; ///< my jet definition
-};
-
-///------------------------------------------------------------------------
-/// \class WTA_KT_Axes
-/// \brief Axes from exclusive kT, winner-take-all recombination
-///
-/// Axes from kT algorithm and winner-take-all recombination
-///------------------------------------------------------------------------
-class WTA_KT_Axes : public ExclusiveJetAxes {
-public:
- /// Constructor
- WTA_KT_Axes()
- : ExclusiveJetAxes(JetDefinitionWrapper(fastjet::kt_algorithm,
- fastjet::JetDefinition::max_allowable_R, //maximum jet radius constant
- _recomb = new WinnerTakeAllRecombiner(), // Needs to be explicitly declared (this will be deleted by JetDefinitionWrapper)
- fastjet::Best).getJetDef()
- ) {
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "WTA KT";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "Winner-Take-All KT Axes";
- return stream.str();
- };
-
- /// For copying purposes
- virtual WTA_KT_Axes* create() const {return new WTA_KT_Axes(*this);}
-
-private:
- const WinnerTakeAllRecombiner *_recomb; ///< Internal recombiner
-
-};
-
-///------------------------------------------------------------------------
-/// \class WTA_CA_Axes
-/// \brief Axes from exclusive CA, winner-take-all recombination
-///
-/// Axes from CA algorithm and winner-take-all recombination
-///------------------------------------------------------------------------
-class WTA_CA_Axes : public ExclusiveJetAxes {
-public:
- /// Constructor
- WTA_CA_Axes()
- : ExclusiveJetAxes(JetDefinitionWrapper(fastjet::cambridge_algorithm,
- fastjet::JetDefinition::max_allowable_R, //maximum jet radius constant
- _recomb = new WinnerTakeAllRecombiner(), // Needs to be explicitly declared (this will be deleted by JetDefinitionWrapper)
- fastjet::Best).getJetDef()) {
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "WTA CA";
- };
-
- /// Long descriptions
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "Winner-Take-All CA Axes";
- return stream.str();
- };
-
- /// For copying purposes
- virtual WTA_CA_Axes* create() const {return new WTA_CA_Axes(*this);}
-
-private:
- const WinnerTakeAllRecombiner *_recomb; ///< Internal recombiner
-
-};
-
-
-///------------------------------------------------------------------------
-/// \class GenKT_Axes
-/// \brief Axes from exclusive generalized kT
-///
-/// Axes from a general KT algorithm (standard E-scheme recombination)
-/// Requires the power of the KT algorithm to be used and the radius parameter
-///------------------------------------------------------------------------
-class GenKT_Axes : public ExclusiveJetAxes {
-
-public:
- /// Constructor
- GenKT_Axes(double p, double R0 = fastjet::JetDefinition::max_allowable_R)
- : ExclusiveJetAxes(fastjet::JetDefinition(fastjet::genkt_algorithm,
- R0,
- p)), _p(p), _R0(R0) {
- if (p < 0) throw Error("GenKT_Axes: Currently only p >=0 is supported.");
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "GenKT Axes";
- return stream.str();
- };
-
- /// Long descriptions
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "General KT (p = " << _p << "), R0 = " << _R0;
- return stream.str();
- };
-
- /// For copying purposes
- virtual GenKT_Axes* create() const {return new GenKT_Axes(*this);}
-
-protected:
- double _p; ///< genkT power
- double _R0; ///< jet radius
-};
-
-
-///------------------------------------------------------------------------
-/// \class WTA_GenKT_Axes
-/// \brief Axes from exclusive generalized kT, winner-take-all recombination
-///
-/// Axes from a general KT algorithm with a Winner Take All Recombiner
-/// Requires the power of the KT algorithm to be used and the radius parameter
-///------------------------------------------------------------------------
-class WTA_GenKT_Axes : public ExclusiveJetAxes {
-
-public:
- /// Constructor
- WTA_GenKT_Axes(double p, double R0 = fastjet::JetDefinition::max_allowable_R)
- : ExclusiveJetAxes(JetDefinitionWrapper(fastjet::genkt_algorithm,
- R0,
- p,
- _recomb = new WinnerTakeAllRecombiner()
- ).getJetDef()), _p(p), _R0(R0) {
- if (p < 0) throw Error("WTA_GenKT_Axes: Currently only p >=0 is supported.");
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "WTA, GenKT Axes";
- return stream.str();
- };
-
- /// Long descriptions
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
- return stream.str();
- };
-
- /// For copying purposes
- virtual WTA_GenKT_Axes* create() const {return new WTA_GenKT_Axes(*this);}
-
-protected:
- double _p; ///< genkT power
- double _R0; ///< jet radius
- const WinnerTakeAllRecombiner *_recomb; ///< Internal recombiner
-};
-
-///------------------------------------------------------------------------
-/// \class GenET_GenKT_Axes
-/// \brief Axes from exclusive kT, generalized Et-scheme recombination
-///
-/// Class using general KT algorithm with a more general recombination scheme
-/// Requires power of KT algorithm, power of recombination weights, and radius parameter
-///------------------------------------------------------------------------
-class GenET_GenKT_Axes : public ExclusiveJetAxes {
-
-public:
- /// Constructor
- GenET_GenKT_Axes(double delta, double p, double R0 = fastjet::JetDefinition::max_allowable_R)
- : ExclusiveJetAxes((JetDefinitionWrapper(fastjet::genkt_algorithm, R0, p, _recomb = new GeneralEtSchemeRecombiner(delta))).getJetDef() ),
- _delta(delta), _p(p), _R0(R0) {
- if (p < 0) throw Error("GenET_GenKT_Axes: Currently only p >=0 is supported.");
- if (delta <= 0) throw Error("GenET_GenKT_Axes: Currently only delta >0 is supported.");
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "GenET, GenKT Axes";
- return stream.str();
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2);
- // TODO: if _delta is huge, change to "WTA"
- if (_delta < std::numeric_limits<int>::max()) stream << "General Recombiner (delta = " << _delta << "), " << "General KT (p = " << _p << ") Axes, R0 = " << _R0;
- else stream << "Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
-
- return stream.str();
- };
-
- /// For copying purposes
- virtual GenET_GenKT_Axes* create() const {return new GenET_GenKT_Axes(*this);}
-
-protected:
- double _delta; ///< Recombination pT weighting
- double _p; ///< GenkT power
- double _R0; ///< jet radius
- const GeneralEtSchemeRecombiner *_recomb; ///< Internal recombiner
-};
-
-///------------------------------------------------------------------------
-/// \class OnePass_KT_Axes
-/// \brief Axes from exclusive kT, with one-pass minimization
-///
-/// Onepass minimization from kt axes
-///------------------------------------------------------------------------
-class OnePass_KT_Axes : public KT_Axes {
-public:
- /// Constructor
- OnePass_KT_Axes() : KT_Axes() {
- setNPass(ONE_PASS);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "OnePass KT";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "One-Pass Minimization from KT Axes";
- return stream.str();
- };
-
- /// For copying purposes
- virtual OnePass_KT_Axes* create() const {return new OnePass_KT_Axes(*this);}
-
-
-};
-
-///------------------------------------------------------------------------
-/// \class OnePass_CA_Axes
-/// \brief Axes from exclusive CA, with one-pass minimization
-///
-/// Onepass minimization from CA axes
-///------------------------------------------------------------------------
-class OnePass_CA_Axes : public CA_Axes {
-public:
- /// Constructor
- OnePass_CA_Axes() : CA_Axes() {
- setNPass(ONE_PASS);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "OnePass CA";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "One-Pass Minimization from CA Axes";
- return stream.str();
- };
-
- /// For copying purposes
- virtual OnePass_CA_Axes* create() const {return new OnePass_CA_Axes(*this);}
-
-
-};
-
-///------------------------------------------------------------------------
-/// \class OnePass_AntiKT_Axes
-/// \brief Axes from inclusive anti-kT, with one-pass minimization
-///
-/// Onepass minimization from AntiKT axes, one parameter R0
-///------------------------------------------------------------------------
-class OnePass_AntiKT_Axes : public AntiKT_Axes {
-
-public:
- /// Constructor
- OnePass_AntiKT_Axes(double R0) : AntiKT_Axes(R0) {
- setNPass(ONE_PASS);
- }
-
- /// Short Description
- virtual std::string short_description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "OnePassAKT" << _R0;
- return stream.str();
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "One-Pass Minimization from Anti-KT Axes (R0 = " << _R0 << ")";
- return stream.str();
- };
-
- /// For copying purposes
- virtual OnePass_AntiKT_Axes* create() const {return new OnePass_AntiKT_Axes(*this);}
-
-};
-
-///------------------------------------------------------------------------
-/// \class OnePass_WTA_KT_Axes
-/// \brief Axes from exclusive kT, winner-take-all recombination, with one-pass minimization
-///
-/// Onepass minimization from winner-take-all kt axes
-///------------------------------------------------------------------------
-class OnePass_WTA_KT_Axes : public WTA_KT_Axes {
-public:
- /// Constructor
- OnePass_WTA_KT_Axes() : WTA_KT_Axes() {
- setNPass(ONE_PASS);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "OnePass WTA KT";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "One-Pass Minimization from Winner-Take-All KT Axes";
- return stream.str();
- };
-
- /// For copying purposes
- virtual OnePass_WTA_KT_Axes* create() const {return new OnePass_WTA_KT_Axes(*this);}
-
-
-};
-
-///------------------------------------------------------------------------
-/// \class OnePass_WTA_CA_Axes
-/// \brief Axes from exclusive CA, winner-take-all recombination, with one-pass minimization
-///
-/// Onepass minimization from winner-take-all CA axes
-///------------------------------------------------------------------------
-class OnePass_WTA_CA_Axes : public WTA_CA_Axes {
-
-public:
- /// Constructor
- OnePass_WTA_CA_Axes() : WTA_CA_Axes() {
- setNPass(ONE_PASS);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "OnePass WTA CA";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "One-Pass Minimization from Winner-Take-All CA Axes";
- return stream.str();
- };
-
- /// For copying purposes
- virtual OnePass_WTA_CA_Axes* create() const {return new OnePass_WTA_CA_Axes(*this);}
-
-};
-
-///------------------------------------------------------------------------
-/// \class OnePass_GenKT_Axes
-/// \brief Axes from exclusive generalized kT with one-pass minimization
-///
-/// Onepass minimization, General KT Axes (standard E-scheme recombination)
-///------------------------------------------------------------------------
-class OnePass_GenKT_Axes : public GenKT_Axes {
-
-public:
- /// Constructor
- OnePass_GenKT_Axes(double p, double R0 = fastjet::JetDefinition::max_allowable_R) : GenKT_Axes(p, R0) {
- setNPass(ONE_PASS);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "OnePass GenKT";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "One-Pass Minimization from General KT (p = " << _p << "), R0 = " << _R0;
- return stream.str();
- };
-
- /// For copying purposes
- virtual OnePass_GenKT_Axes* create() const {return new OnePass_GenKT_Axes(*this);}
-};
-
-///------------------------------------------------------------------------
-/// \class OnePass_WTA_GenKT_Axes
-/// \brief Axes from exclusive generalized kT, winner-take-all recombination, with one-pass minimization
-///
-/// Onepass minimization from winner-take-all, General KT Axes
-///------------------------------------------------------------------------
-class OnePass_WTA_GenKT_Axes : public WTA_GenKT_Axes {
-
-public:
- /// Constructor
- OnePass_WTA_GenKT_Axes(double p, double R0 = fastjet::JetDefinition::max_allowable_R) : WTA_GenKT_Axes(p, R0) {
- setNPass(ONE_PASS);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "OnePass WTA GenKT";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "One-Pass Minimization from Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
- return stream.str();
- };
-
- /// For copying purposes
- virtual OnePass_WTA_GenKT_Axes* create() const {return new OnePass_WTA_GenKT_Axes(*this);}
-};
-
-///------------------------------------------------------------------------
-/// \class OnePass_GenET_GenKT_Axes
-/// \brief Axes from exclusive generalized kT, generalized Et-scheme recombination, with one-pass minimization
-///
-/// Onepass minimization from General Recomb, General KT axes
-///------------------------------------------------------------------------
-class OnePass_GenET_GenKT_Axes : public GenET_GenKT_Axes {
-
-public:
- /// Constructor
- OnePass_GenET_GenKT_Axes(double delta, double p, double R0 = fastjet::JetDefinition::max_allowable_R) : GenET_GenKT_Axes(delta, p, R0) {
- setNPass(ONE_PASS);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "OnePass GenET, GenKT";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2);
- if (_delta < std::numeric_limits<int>::max()) stream << "One-Pass Minimization from General Recombiner (delta = "
- << _delta << "), " << "General KT (p = " << _p << ") Axes, R0 = " << _R0;
- else stream << "One-Pass Minimization from Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
- return stream.str();
- };
-
- /// For copying purposes
- virtual OnePass_GenET_GenKT_Axes* create() const {return new OnePass_GenET_GenKT_Axes(*this);}
-};
-
-
-///------------------------------------------------------------------------
-/// \class Manual_Axes
-/// \brief Manual axes finding
-///
-/// Allows the user to set the axes manually
-///------------------------------------------------------------------------
-class Manual_Axes : public AxesDefinition {
-public:
- /// Constructor. Note that _needsManualAxes is set to true.
- Manual_Axes() : AxesDefinition() {
- setNPass(NO_REFINING);
- _needsManualAxes = true;
- }
-
- /// This is now a dummy function since this is manual mode
- virtual std::vector<fastjet::PseudoJet> get_starting_axes(int,
- const std::vector<fastjet::PseudoJet>&,
- const MeasureDefinition *) const;
-
-
- /// Short description
- virtual std::string short_description() const {
- return "Manual";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "Manual Axes";
- return stream.str();
- };
-
- /// For copying purposes
- virtual Manual_Axes* create() const {return new Manual_Axes(*this);}
-
-
-};
-
-///------------------------------------------------------------------------
-/// \class OnePass_Manual_Axes
-/// \brief Manual axes finding, with one-pass minimization
-///
-/// One pass minimization from manual starting point
-///------------------------------------------------------------------------
-class OnePass_Manual_Axes : public Manual_Axes {
-public:
- /// Constructor. Note that _needsManualAxes is set to true.
- OnePass_Manual_Axes() : Manual_Axes() {
- setNPass(ONE_PASS);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "OnePass Manual";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "One-Pass Minimization from Manual Axes";
- return stream.str();
- };
-
- // For copying purposes
- virtual OnePass_Manual_Axes* create() const {return new OnePass_Manual_Axes(*this);}
-
-};
-
-///------------------------------------------------------------------------
-/// \class MultiPass_Axes
-/// \brief Manual axes finding, with multi-pass (randomized) minimization
-///
-/// Multi-pass minimization from kT starting point
-///------------------------------------------------------------------------
-class MultiPass_Axes : public KT_Axes {
-
-public:
-
- /// Constructor
- MultiPass_Axes(unsigned int Npass) : KT_Axes() {
- setNPass(Npass);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "MultiPass";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "Multi-Pass Axes (Npass = " << _Npass << ")";
- return stream.str();
- };
-
- /// For copying purposs
- virtual MultiPass_Axes* create() const {return new MultiPass_Axes(*this);}
-
-};
-
-///------------------------------------------------------------------------
-/// \class MultiPass_Manual_Axes
-/// \brief Axes finding from exclusive kT, with multi-pass (randomized) minimization
-///
-/// multi-pass minimization from kT starting point
-///------------------------------------------------------------------------
-class MultiPass_Manual_Axes : public Manual_Axes {
-
-public:
- /// Constructor
- MultiPass_Manual_Axes(unsigned int Npass) : Manual_Axes() {
- setNPass(Npass);
- }
-
- /// Short Description
- virtual std::string short_description() const {
- return "MultiPass Manual";
- };
-
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "Multi-Pass Manual Axes (Npass = " << _Npass << ")";
- return stream.str();
- };
-
- /// For copying purposes
- virtual MultiPass_Manual_Axes* create() const {return new MultiPass_Manual_Axes(*this);}
-
-};
-
-///------------------------------------------------------------------------
-/// \class Comb_GenKT_Axes
-/// \brief Axes from exclusive generalized kT with combinatorial testing
-///
-/// Axes from kT algorithm (standard E-scheme recombination)
-/// Requires nExtra parameter and returns set of N that minimizes N-jettiness
-/// Note that this method is not guaranteed to find a deeper minimum than GenKT_Axes
-///------------------------------------------------------------------------
-class Comb_GenKT_Axes : public ExclusiveCombinatorialJetAxes {
-public:
- /// Constructor
- Comb_GenKT_Axes(int nExtra, double p, double R0 = fastjet::JetDefinition::max_allowable_R)
- : ExclusiveCombinatorialJetAxes(fastjet::JetDefinition(fastjet::genkt_algorithm, R0, p), nExtra),
- _p(p), _R0(R0) {
- if (p < 0) throw Error("Comb_GenKT_Axes: Currently only p >=0 is supported.");
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "N Choose M GenKT";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "N Choose M Minimization (nExtra = " << _nExtra << ") from General KT (p = " << _p << "), R0 = " << _R0;
- return stream.str();
- };
-
- /// For copying purposes
- virtual Comb_GenKT_Axes* create() const {return new Comb_GenKT_Axes(*this);}
-
-private:
- double _nExtra; ///< Number of extra axes
- double _p; ///< GenkT power
- double _R0; ///< jet radius
-};
-
-
-
-///------------------------------------------------------------------------
-/// \class Comb_WTA_GenKT_Axes
-/// \brief Axes from exclusive generalized kT, winner-take-all recombination, with combinatorial testing
-///
-/// Axes from kT algorithm and winner-take-all recombination
-/// Requires nExtra parameter and returns set of N that minimizes N-jettiness
-///------------------------------------------------------------------------
-class Comb_WTA_GenKT_Axes : public ExclusiveCombinatorialJetAxes {
-public:
- /// Constructor
- Comb_WTA_GenKT_Axes(int nExtra, double p, double R0 = fastjet::JetDefinition::max_allowable_R)
- : ExclusiveCombinatorialJetAxes((JetDefinitionWrapper(fastjet::genkt_algorithm, R0, p, _recomb = new WinnerTakeAllRecombiner())).getJetDef(), nExtra),
- _p(p), _R0(R0) {
- if (p < 0) throw Error("Comb_WTA_GenKT_Axes: Currently only p >=0 is supported.");
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "N Choose M WTA GenKT";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2)
- << "N Choose M Minimization (nExtra = " << _nExtra << ") from Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
- return stream.str();
- };
-
- /// For copying purposes
- virtual Comb_WTA_GenKT_Axes* create() const {return new Comb_WTA_GenKT_Axes(*this);}
-
-private:
- double _nExtra; ///< Number of extra axes
- double _p; ///< GenkT power
- double _R0; ///< jet radius
- const WinnerTakeAllRecombiner *_recomb; ///< Internal recombiner
-};
-
-///------------------------------------------------------------------------
-/// \class Comb_GenET_GenKT_Axes
-/// \brief Axes from exclusive generalized kT, generalized Et-scheme recombination, with combinatorial testing
-///
-/// Axes from kT algorithm and General Et scheme recombination
-/// Requires nExtra parameter and returns set of N that minimizes N-jettiness
-///------------------------------------------------------------------------
-class Comb_GenET_GenKT_Axes : public ExclusiveCombinatorialJetAxes {
-public:
- /// Constructor
- Comb_GenET_GenKT_Axes(int nExtra, double delta, double p, double R0 = fastjet::JetDefinition::max_allowable_R)
- : ExclusiveCombinatorialJetAxes((JetDefinitionWrapper(fastjet::genkt_algorithm, R0, p, _recomb = new GeneralEtSchemeRecombiner(delta))).getJetDef(), nExtra),
- _delta(delta), _p(p), _R0(R0) {
- if (p < 0) throw Error("Comb_GenET_GenKT_Axes: Currently only p >=0 is supported.");
- if (delta <= 0) throw Error("Comb_GenET_GenKT_Axes: Currently only delta >=0 is supported.");
- setNPass(NO_REFINING);
- }
-
- /// Short description
- virtual std::string short_description() const {
- return "N Choose M GenET GenKT";
- };
-
- /// Long description
- virtual std::string description() const {
- std::stringstream stream;
- stream << std::fixed << std::setprecision(2);
- if (_delta < std::numeric_limits<int>::max()) stream << "N choose M Minimization (nExtra = " << _nExtra
- << ") from General Recombiner (delta = " << _delta << "), " << "General KT (p = " << _p << ") Axes, R0 = " << _R0;
- else stream << "N choose M Minimization (nExtra = " << _nExtra << ") from Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
- return stream.str();
- };
-
- /// For copying purposes
- virtual Comb_GenET_GenKT_Axes* create() const {return new Comb_GenET_GenKT_Axes(*this);}
-
-private:
- double _nExtra; ///< Number of extra axes
- double _delta; ///< Recombination pT weighting exponent
- double _p; ///< GenkT power
- double _R0; ///< jet radius
- const GeneralEtSchemeRecombiner *_recomb; ///< Internal recombiner
-};
-
-
-} // namespace Nsubjettiness
-
-}
-
-#endif // __FASTJET_CONTRIB_NJETTINESS_HH__
-
diff --git a/include/Rivet/Tools/Nsubjettiness/ExtraRecombiners.hh b/include/Rivet/Tools/Nsubjettiness/ExtraRecombiners.hh
deleted file mode 100644
--- a/include/Rivet/Tools/Nsubjettiness/ExtraRecombiners.hh
+++ /dev/null
@@ -1,103 +0,0 @@
-// Nsubjettiness Package
-// Questions/Comments? jthaler@jthaler.net
-//
-// Copyright (c) 2011-14
-// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
-//
-// $Id: ExtraRecombiners.hh 828 2015-07-20 14:52:06Z jthaler $
-//----------------------------------------------------------------------
-// This file is part of FastJet contrib.
-//
-// It is free software; you can redistribute it and/or modify it under
-// the terms of the GNU General Public License as published by the
-// Free Software Foundation; either version 2 of the License, or (at
-// your option) any later version.
-//
-// It is distributed in the hope that it will be useful, but WITHOUT
-// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
-// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
-// License for more details.
-//
-// You should have received a copy of the GNU General Public License
-// along with this code. If not, see <http://www.gnu.org/licenses/>.
-//----------------------------------------------------------------------
-
-#ifndef __FASTJET_CONTRIB_WINNERTAKEALLRECOMBINER_HH__
-#define __FASTJET_CONTRIB_WINNERTAKEALLRECOMBINER_HH__
-
-#include "fastjet/PseudoJet.hh"
-#include "fastjet/JetDefinition.hh"
-
-#include <cmath>
-#include <vector>
-#include <list>
-#include <limits>
-#include <stdio.h>
-#include <string.h>
-#include <errno.h>
-
-namespace Rivet {
-
-namespace Nsubjettiness { using namespace fastjet;
-
-///------------------------------------------------------------------------
-/// \class GeneralEtSchemeRecombiner
-/// \brief Recombination scheme with generalized Et weighting
-///
-/// GeneralEtSchemeRecombiner defines a new recombination scheme by inheriting from JetDefinition::Recombiner.
-/// This scheme compares the pT of two input particles, and then combines them into a particle with
-/// a pT equal to the sum of the two particle pTs and a direction (in rapidity/phi) weighted by the respective momenta of the
-/// particle. The weighting is dependent on the power delta. For delta = infinity, this should return the same result as the
-/// WinnerTakeAllRecombiner.
-///------------------------------------------------------------------------
-class GeneralEtSchemeRecombiner : public fastjet::JetDefinition::Recombiner {
-public:
-
- /// Constructor takes delta weighting
- /// (delta = 1.0 for Et-scheme, delta = infinity for winner-take-all scheme)
- GeneralEtSchemeRecombiner(double delta) : _delta(delta) {}
-
- /// Description
- virtual std::string description() const;
-
- /// Recombine pa and pb and put result into pab
- virtual void recombine(const fastjet::PseudoJet & pa,
- const fastjet::PseudoJet & pb,
- fastjet::PseudoJet & pab) const;
-
-private:
- double _delta; ///< Weighting exponent
-};
-
-///------------------------------------------------------------------------
-/// \class WinnerTakeAllRecombiner
-/// \brief Recombination scheme with winner-take-all weighting
-///
-/// WinnerTakeAllRecombiner defines a new recombination scheme by inheriting from JetDefinition::Recombiner.
-/// This scheme compares the pT of two input particles, and then combines them into a particle with
-/// a pT equal to the sum of the two particle pTs and a direction (in rapidity/phi) identical to that of the harder
-/// particle. This creates a jet with an axis guaranteed to align with a particle in the event.
-///------------------------------------------------------------------------
-class WinnerTakeAllRecombiner : public fastjet::JetDefinition::Recombiner {
-public:
-
- /// Constructor to choose value of alpha (defaulted to 1 for normal pT sum)
- WinnerTakeAllRecombiner(double alpha = 1.0) : _alpha(alpha) {}
-
- /// Description
- virtual std::string description() const;
-
- /// recombine pa and pb and put result into pab
- virtual void recombine(const fastjet::PseudoJet & pa,
- const fastjet::PseudoJet & pb,
- fastjet::PseudoJet & pab) const;
-
-private:
- double _alpha; //power of (pt/E) term when recombining particles
-};
-
-} //namespace Nsubjettiness
-
-}
-
-#endif // __FASTJET_CONTRIB_WINNERTAKEALLRECOMBINER_HH__
diff --git a/include/Rivet/Tools/Nsubjettiness/MeasureDefinition.hh b/include/Rivet/Tools/Nsubjettiness/MeasureDefinition.hh
deleted file mode 100644
--- a/include/Rivet/Tools/Nsubjettiness/MeasureDefinition.hh
+++ /dev/null
@@ -1,853 +0,0 @@
-// Nsubjettiness Package
-// Questions/Comments? jthaler@jthaler.net
-//
-// Copyright (c) 2011-14
-// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
-//
-// $Id: MeasureDefinition.hh 828 2015-07-20 14:52:06Z jthaler $
-//----------------------------------------------------------------------
-// This file is part of FastJet contrib.
-//
-// It is free software; you can redistribute it and/or modify it under
-// the terms of the GNU General Public License as published by the
-// Free Software Foundation; either version 2 of the License, or (at
-// your option) any later version.
-//
-// It is distributed in the hope that it will be useful, but WITHOUT
-// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
-// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
-// License for more details.
-//
-// You should have received a copy of the GNU General Public License
-// along with this code. If not, see <http://www.gnu.org/licenses/>.
-//----------------------------------------------------------------------
-
-#ifndef __FASTJET_CONTRIB_MEASUREDEFINITION_HH__
-#define __FASTJET_CONTRIB_MEASUREDEFINITION_HH__
-
-#include "fastjet/PseudoJet.hh"
-#include <cmath>
-#include <vector>
-#include <list>
-#include <limits>
-
-#include "TauComponents.hh"
-
-namespace Rivet {
-
-namespace Nsubjettiness{
-
-
-
-// The following Measures are available (and their relevant arguments):
-// Recommended for usage as jet shapes
-class DefaultMeasure; // Default measure from which next classes derive (should not be called directly)
-class NormalizedMeasure; // (beta,R0)
-class UnnormalizedMeasure; // (beta)
-class NormalizedCutoffMeasure; // (beta,R0,Rcutoff)
-class UnnormalizedCutoffMeasure; // (beta,Rcutoff)
-
-// New measures as of v2.2
-// Recommended for usage as event shapes (or for jet finding)
-class ConicalMeasure; // (beta,R)
-class OriginalGeometricMeasure; // (R)
-class ModifiedGeometricMeasure; // (R)
-class ConicalGeometricMeasure; // (beta, gamma, R)
-class XConeMeasure; // (beta, R)
-
-// Formerly GeometricMeasure, now no longer recommended, kept commented out only for cross-check purposes
-//class DeprecatedGeometricMeasure; // (beta)
-//class DeprecatedGeometricCutoffMeasure; // (beta,Rcutoff)
-
-
-///////
-//
-// MeasureDefinition
-//
-///////
-
-//This is a helper class for the Minimum Axes Finders. It is defined later.
-class LightLikeAxis;
-
-///------------------------------------------------------------------------
-/// \class MeasureDefinition
-/// \brief Base class for measure definitions
-///
-/// This is the base class for measure definitions. Derived classes will calculate
-/// the tau_N of a jet given a specific measure and a set of axes. The measure is
-/// determined by various jet and beam distances (and possible normalization factors).
-///------------------------------------------------------------------------
-class MeasureDefinition {
-
-public:
-
- /// Description of measure and parameters
- virtual std::string description() const = 0;
-
- /// In derived classes, this should return a copy of the corresponding derived class
- virtual MeasureDefinition* create() const = 0;
-
- //The following five functions define the measure by which tau_N is calculated,
- //and are overloaded by the various measures below
-
- /// Distanes to jet axis. This is called many times, so needs to be as fast as possible
- /// Unless overloaded, it just calls jet_numerator
- virtual double jet_distance_squared(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
- return jet_numerator(particle,axis);
- }
-
- /// Distanes to beam. This is called many times, so needs to be as fast as possible
- /// Unless overloaded, it just calls beam_numerator
- virtual double beam_distance_squared(const fastjet::PseudoJet& particle) const {
- return beam_numerator(particle);
- }
-
- /// The jet measure used in N-(sub)jettiness
- virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const = 0;
- /// The beam measure used in N-(sub)jettiness
- virtual double beam_numerator(const fastjet::PseudoJet& particle) const = 0;
-
- /// A possible normalization factor
- virtual double denominator(const fastjet::PseudoJet& particle) const = 0;
-
- /// Run a one-pass minimization routine. There is a generic one-pass minimization that works for a wide variety of measures.
- /// This should be overloaded to create a measure-specific minimization scheme
- virtual std::vector<fastjet::PseudoJet> get_one_pass_axes(int n_jets,
- const std::vector<fastjet::PseudoJet>& inputs,
- const std::vector<fastjet::PseudoJet>& seedAxes,
- int nAttempts = 1000, // cap number of iterations
- double accuracy = 0.0001 // cap distance of closest approach
- ) const;
-
-public:
-
- /// Returns the tau value for a give set of particles and axes
- double result(const std::vector<fastjet::PseudoJet>& particles, const std::vector<fastjet::PseudoJet>& axes) const {
- return component_result(particles,axes).tau();
- }
-
- /// Short-hand for the result() function
- inline double operator() (const std::vector<fastjet::PseudoJet>& particles, const std::vector<fastjet::PseudoJet>& axes) const {
- return result(particles,axes);
- }
-
- /// Return all of the TauComponents for specific input particles and axes
- TauComponents component_result(const std::vector<fastjet::PseudoJet>& particles, const std::vector<fastjet::PseudoJet>& axes) const;
-
- /// Create the partitioning according the jet/beam distances and stores them a TauPartition
- TauPartition get_partition(const std::vector<fastjet::PseudoJet>& particles, const std::vector<fastjet::PseudoJet>& axes) const;
-
- /// Calculate the tau result using an existing partition
- TauComponents component_result_from_partition(const TauPartition& partition, const std::vector<fastjet::PseudoJet>& axes) const;
-
-
-
- /// virtual destructor
- virtual ~MeasureDefinition(){}
-
-protected:
-
- /// Flag set by derived classes to choose whether or not to use beam/denominator
- TauMode _tau_mode;
-
- /// Flag set by derived classes to say whether cheap get_one_pass_axes method can be used (true by default)
- bool _useAxisScaling;
-
- /// This is the only constructor, which requires _tau_mode and _useAxisScaling to be manually set by derived classes.
- MeasureDefinition() : _tau_mode(UNDEFINED_SHAPE), _useAxisScaling(true) {}
-
-
- /// Used by derived classes to set whether or not to use beam/denominator information
- void setTauMode(TauMode tau_mode) {
- _tau_mode = tau_mode;
- }
-
- /// Used by derived classes to say whether one can use cheap get_one_pass_axes
- void setAxisScaling(bool useAxisScaling) {
- _useAxisScaling = useAxisScaling;
- }
-
- /// Uses denominator information?
- bool has_denominator() const { return (_tau_mode == NORMALIZED_JET_SHAPE || _tau_mode == NORMALIZED_EVENT_SHAPE);}
- /// Uses beam information?
- bool has_beam() const {return (_tau_mode == UNNORMALIZED_EVENT_SHAPE || _tau_mode == NORMALIZED_EVENT_SHAPE);}
-
- /// Create light-like axis (used in default one-pass minimization routine)
- fastjet::PseudoJet lightFrom(const fastjet::PseudoJet& input) const {
- double length = sqrt(pow(input.px(),2) + pow(input.py(),2) + pow(input.pz(),2));
- return fastjet::PseudoJet(input.px()/length,input.py()/length,input.pz()/length,1.0);
- }
-
- /// Shorthand for squaring
- static inline double sq(double x) {return x*x;}
-
-};
-
-
-///////
-//
-// Default Measures
-//
-///////
-
-
-///------------------------------------------------------------------------
-/// \enum DefaultMeasureType
-/// \brief Options for default measure
-///
-/// Can be used to switch between pp and ee measure types in the DefaultMeasure
-///------------------------------------------------------------------------
-enum DefaultMeasureType {
- pt_R, /// use transverse momenta and boost-invariant angles,
- E_theta, /// use energies and angles,
- lorentz_dot, /// use dot product inspired measure
- perp_lorentz_dot /// use conical geometric inspired measures
-};
-
-///------------------------------------------------------------------------
-/// \class DefaultMeasure
-/// \brief Base class for default N-subjettiness measure definitions
-///
-/// This class is the default measure as defined in the original N-subjettiness papers.
-/// Based on the conical measure, but with a normalization factor
-/// This measure is defined as the pT of the particle multiplied by deltaR
-/// to the power of beta. This class includes the normalization factor determined by R0
-///------------------------------------------------------------------------
-class DefaultMeasure : public MeasureDefinition {
-
-public:
-
- /// Description
- virtual std::string description() const;
- /// To allow copying around of these objects
- virtual DefaultMeasure* create() const {return new DefaultMeasure(*this);}
-
- /// fast jet distance
- virtual double jet_distance_squared(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
- return angleSquared(particle, axis);
- }
-
- /// fast beam distance
- virtual double beam_distance_squared(const fastjet::PseudoJet& /*particle*/) const {
- return _RcutoffSq;
- }
-
- /// true jet distance (given by general definitions of energy and angle)
- virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const{
- double jet_dist = angleSquared(particle, axis);
- if (jet_dist > 0.0) {
- return energy(particle) * std::pow(jet_dist,_beta/2.0);
- } else {
- return 0.0;
- }
- }
-
- /// true beam distance
- virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
- return energy(particle) * std::pow(_Rcutoff,_beta);
- }
-
- /// possible denominator for normalization
- virtual double denominator(const fastjet::PseudoJet& particle) const {
- return energy(particle) * std::pow(_R0,_beta);
- }
-
- /// Special minimization routine (from v1.0 of N-subjettiness)
- virtual std::vector<fastjet::PseudoJet> get_one_pass_axes(int n_jets,
- const std::vector<fastjet::PseudoJet>& inputs,
- const std::vector<fastjet::PseudoJet>& seedAxes,
- int nAttempts, // cap number of iterations
- double accuracy // cap distance of closest approach
- ) const;
-
-protected:
- double _beta; ///< Angular exponent
- double _R0; ///< Normalization factor
- double _Rcutoff; ///< Cutoff radius
- double _RcutoffSq; ///< Cutoff radius squared
- DefaultMeasureType _measure_type; ///< Type of measure used (i.e. pp style or ee style)
-
-
- /// Constructor is protected so that no one tries to call this directly.
- DefaultMeasure(double beta, double R0, double Rcutoff, DefaultMeasureType measure_type = pt_R)
- : MeasureDefinition(), _beta(beta), _R0(R0), _Rcutoff(Rcutoff), _RcutoffSq(sq(Rcutoff)), _measure_type(measure_type)
- {
- if (beta <= 0) throw Error("DefaultMeasure: You must choose beta > 0.");
- if (R0 <= 0) throw Error("DefaultMeasure: You must choose R0 > 0.");
- if (Rcutoff <= 0) throw Error("DefaultMeasure: You must choose Rcutoff > 0.");
- }
-
- /// Added set measure method in case it becomes useful later
- void setDefaultMeasureType(DefaultMeasureType measure_type) {
- _measure_type = measure_type;
- }
-
- /// Generalized energy value (determined by _measure_type)
- double energy(const PseudoJet& jet) const;
- /// Generalized angle value (determined by _measure_type)
- double angleSquared(const PseudoJet& jet1, const PseudoJet& jet2) const;
-
- /// Name of _measure_type, so description will include the measure type
- std::string measure_type_name() const {
- if (_measure_type == pt_R) return "pt_R";
- else if (_measure_type == E_theta) return "E_theta";
- else if (_measure_type == lorentz_dot) return "lorentz_dot";
- else if (_measure_type == perp_lorentz_dot) return "perp_lorentz_dot";
- else return "Measure Type Undefined";
- }
-
- /// templated for speed (TODO: probably should remove, since not clear that there is a speed gain)
- template <int N> std::vector<LightLikeAxis> UpdateAxesFast(const std::vector <LightLikeAxis> & old_axes,
- const std::vector <fastjet::PseudoJet> & inputJets,
- double accuracy) const;
-
- /// called by get_one_pass_axes to update axes iteratively
- std::vector<LightLikeAxis> UpdateAxes(const std::vector <LightLikeAxis> & old_axes,
- const std::vector <fastjet::PseudoJet> & inputJets,
- double accuracy) const;
-};
-
-
-///------------------------------------------------------------------------
-/// \class NormalizedCutoffMeasure
-/// \brief Dimensionless default measure, with radius cutoff
-///
-/// This measure is just a wrapper for DefaultMeasure
-///------------------------------------------------------------------------
-class NormalizedCutoffMeasure : public DefaultMeasure {
-
-public:
-
- /// Constructor
- NormalizedCutoffMeasure(double beta, double R0, double Rcutoff, DefaultMeasureType measure_type = pt_R)
- : DefaultMeasure(beta, R0, Rcutoff, measure_type) {
- setTauMode(NORMALIZED_JET_SHAPE);
- }
-
- /// Description
- virtual std::string description() const;
-
- /// For copying purposes
- virtual NormalizedCutoffMeasure* create() const {return new NormalizedCutoffMeasure(*this);}
-
-};
-
-///------------------------------------------------------------------------
-/// \class NormalizedMeasure
-/// \brief Dimensionless default measure, with no cutoff
-///
-/// This measure is the same as NormalizedCutoffMeasure, with Rcutoff taken to infinity.
-///------------------------------------------------------------------------
-class NormalizedMeasure : public NormalizedCutoffMeasure {
-
-public:
-
- /// Constructor
- NormalizedMeasure(double beta, double R0, DefaultMeasureType measure_type = pt_R)
- : NormalizedCutoffMeasure(beta, R0, std::numeric_limits<double>::max(), measure_type) {
- _RcutoffSq = std::numeric_limits<double>::max();
- setTauMode(NORMALIZED_JET_SHAPE);
- }
-
- /// Description
- virtual std::string description() const;
- /// For copying purposes
- virtual NormalizedMeasure* create() const {return new NormalizedMeasure(*this);}
-
-};
-
-
-///------------------------------------------------------------------------
-/// \class UnnormalizedCutoffMeasure
-/// \brief Dimensionful default measure, with radius cutoff
-///
-/// This class is the unnormalized conical measure. The only difference from NormalizedCutoffMeasure
-/// is that the denominator is defined to be 1.0 by setting _has_denominator to false.
-/// class UnnormalizedCutoffMeasure : public NormalizedCutoffMeasure {
-///------------------------------------------------------------------------
-class UnnormalizedCutoffMeasure : public DefaultMeasure {
-
-public:
-
- /// Since all methods are identical, UnnormalizedMeasure inherits directly
- /// from NormalizedMeasure. R0 is a dummy value since the value of R0 is unecessary for this class,
- /// and the "false" flag sets _has_denominator in MeasureDefinition to false so no denominator is used.
- UnnormalizedCutoffMeasure(double beta, double Rcutoff, DefaultMeasureType measure_type = pt_R)
- : DefaultMeasure(beta, std::numeric_limits<double>::quiet_NaN(), Rcutoff, measure_type) {
- setTauMode(UNNORMALIZED_EVENT_SHAPE);
- }
-
- /// Description
- virtual std::string description() const;
- /// For copying purposes
- virtual UnnormalizedCutoffMeasure* create() const {return new UnnormalizedCutoffMeasure(*this);}
-
-};
-
-
-///------------------------------------------------------------------------
-/// \class UnnormalizedMeasure
-/// \brief Dimensionless default measure, with no cutoff
-///
-/// This measure is the same as UnnormalizedCutoffMeasure, with Rcutoff taken to infinity.
-///------------------------------------------------------------------------
-class UnnormalizedMeasure : public UnnormalizedCutoffMeasure {
-
-public:
- /// Since all methods are identical, UnnormalizedMeasure inherits directly
- /// from NormalizedMeasure. R0 is a dummy value since the value of R0 is unecessary for this class,
- /// and the "false" flag sets _has_denominator in MeasureDefinition to false so no denominator is used.
- UnnormalizedMeasure(double beta, DefaultMeasureType measure_type = pt_R)
- : UnnormalizedCutoffMeasure(beta, std::numeric_limits<double>::max(), measure_type) {
- _RcutoffSq = std::numeric_limits<double>::max();
- setTauMode(UNNORMALIZED_JET_SHAPE);
- }
-
- /// Description
- virtual std::string description() const;
-
- /// For copying purposes
- virtual UnnormalizedMeasure* create() const {return new UnnormalizedMeasure(*this);}
-
-};
-
-
-///------------------------------------------------------------------------
-/// \class ConicalMeasure
-/// \brief Dimensionful event-shape measure, with radius cutoff
-///
-/// Very similar to UnnormalizedCutoffMeasure, but with different normalization convention
-/// and using the new default one-pass minimization algorithm.
-/// Axes are also made to be light-like to ensure sensible behavior
-/// Intended to be used as an event shape.
-///------------------------------------------------------------------------
-class ConicalMeasure : public MeasureDefinition {
-
-public:
-
- /// Constructor
- ConicalMeasure(double beta, double Rcutoff)
- : MeasureDefinition(), _beta(beta), _Rcutoff(Rcutoff), _RcutoffSq(sq(Rcutoff)) {
- if (beta <= 0) throw Error("ConicalMeasure: You must choose beta > 0.");
- if (Rcutoff <= 0) throw Error("ConicalMeasure: You must choose Rcutoff > 0.");
- setTauMode(UNNORMALIZED_EVENT_SHAPE);
- }
-
- /// Description
- virtual std::string description() const;
- /// For copying purposes
- virtual ConicalMeasure* create() const {return new ConicalMeasure(*this);}
-
- /// fast jet distance
- virtual double jet_distance_squared(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
- PseudoJet lightAxis = lightFrom(axis);
- return particle.squared_distance(lightAxis);
- }
-
- /// fast beam distance
- virtual double beam_distance_squared(const fastjet::PseudoJet& /*particle*/) const {
- return _RcutoffSq;
- }
-
-
- /// true jet distance
- virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
- PseudoJet lightAxis = lightFrom(axis);
- double jet_dist = particle.squared_distance(lightAxis)/_RcutoffSq;
- double jet_perp = particle.perp();
-
- if (_beta == 2.0) {
- return jet_perp * jet_dist;
- } else {
- return jet_perp * pow(jet_dist,_beta/2.0);
- }
- }
-
- /// true beam distance
- virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
- return particle.perp();
- }
-
- /// no denominator used for this measure
- virtual double denominator(const fastjet::PseudoJet& /*particle*/) const {
- return std::numeric_limits<double>::quiet_NaN();
- }
-
-protected:
- double _beta; ///< angular exponent
- double _Rcutoff; ///< effective jet radius
- double _RcutoffSq;///< effective jet radius squared
-};
-
-
-
-///------------------------------------------------------------------------
-/// \class OriginalGeometricMeasure
-/// \brief Dimensionful event-shape measure, with dot-product distances
-///
-/// This class is the original (and hopefully now correctly coded) geometric measure.
-/// This measure is defined by the Lorentz dot product between
-/// the particle and the axis. This class does not include normalization of tau_N.
-/// New in Nsubjettiness v2.2
-/// NOTE: This is defined differently from the DeprecatedGeometricMeasure which are now commented out.
-///------------------------------------------------------------------------
-class OriginalGeometricMeasure : public MeasureDefinition {
-
-public:
- /// Constructor
- OriginalGeometricMeasure(double Rcutoff)
- : MeasureDefinition(), _Rcutoff(Rcutoff), _RcutoffSq(sq(Rcutoff)) {
- if (Rcutoff <= 0) throw Error("OriginalGeometricMeasure: You must choose Rcutoff > 0.");
- setTauMode(UNNORMALIZED_EVENT_SHAPE);
- setAxisScaling(false); // No need to rescale axes (for speed up in one-pass minimization)
- }
-
- /// Description
- virtual std::string description() const;
- /// For copying purposes
- virtual OriginalGeometricMeasure* create() const {return new OriginalGeometricMeasure(*this);}
-
- // This class uses the default jet_distance_squared and beam_distance_squared
-
- /// true jet measure
- virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
- return dot_product(lightFrom(axis), particle)/_RcutoffSq;
- }
-
- /// true beam measure
- virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
- fastjet::PseudoJet beam_a(0,0,1,1);
- fastjet::PseudoJet beam_b(0,0,-1,1);
- double min_perp = std::min(dot_product(beam_a, particle),dot_product(beam_b, particle));
- return min_perp;
- }
-
- /// no denominator needed for this measure.
- virtual double denominator(const fastjet::PseudoJet& /*particle*/) const {
- return std::numeric_limits<double>::quiet_NaN();
- }
-
-protected:
- double _Rcutoff; ///< Effective jet radius (rho = R^2)
- double _RcutoffSq; ///< Effective jet radius squared
-
-};
-
-
-///------------------------------------------------------------------------
-/// \class ModifiedGeometricMeasure
-/// \brief Dimensionful event-shape measure, with dot-product distances, modified beam measure
-///
-/// This class is the Modified geometric measure. This jet measure is defined by the Lorentz dot product between
-/// the particle and the axis, as in the Original Geometric Measure. The beam measure is defined differently from
-/// the above OriginalGeometric to allow for more conical jets. New in Nsubjettiness v2.2
-///------------------------------------------------------------------------
-class ModifiedGeometricMeasure : public MeasureDefinition {
-
-public:
- /// Constructor
- ModifiedGeometricMeasure(double Rcutoff)
- : MeasureDefinition(), _Rcutoff(Rcutoff), _RcutoffSq(sq(Rcutoff)) {
- if (Rcutoff <= 0) throw Error("ModifiedGeometricMeasure: You must choose Rcutoff > 0.");
- setTauMode(UNNORMALIZED_EVENT_SHAPE);
- setAxisScaling(false); // No need to rescale axes (for speed up in one-pass minimization)
- }
-
- /// Description
- virtual std::string description() const;
- /// For copying purposes
- virtual ModifiedGeometricMeasure* create() const {return new ModifiedGeometricMeasure(*this);}
-
- // This class uses the default jet_distance_squared and beam_distance_squared
-
- /// True jet measure
- virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
- return dot_product(lightFrom(axis), particle)/_RcutoffSq;
- }
-
- /// True beam measure
- virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
- fastjet::PseudoJet lightParticle = lightFrom(particle);
- return 0.5*particle.mperp()*lightParticle.pt();
- }
-
- /// This measure does not require a denominator
- virtual double denominator(const fastjet::PseudoJet& /*particle*/) const {
- return std::numeric_limits<double>::quiet_NaN();
- }
-
-protected:
- double _Rcutoff; ///< Effective jet radius (rho = R^2)
- double _RcutoffSq; ///< Effective jet radius squared
-
-
-};
-
-///------------------------------------------------------------------------
-/// \class ConicalGeometricMeasure
-/// \brief Dimensionful event-shape measure, basis for XCone jet algorithm
-///
-/// This class is the Conical Geometric measure. This measure is defined by the Lorentz dot product between
-/// the particle and the axis normalized by the axis and particle pT, as well as a factor of cosh(y) to vary
-/// the rapidity depepdence of the beam. New in Nsubjettiness v2.2, and the basis for the XCone jet algorithm
-///------------------------------------------------------------------------
-class ConicalGeometricMeasure : public MeasureDefinition {
-
-public:
-
- /// Constructor
- ConicalGeometricMeasure(double jet_beta, double beam_gamma, double Rcutoff)
- : MeasureDefinition(), _jet_beta(jet_beta), _beam_gamma(beam_gamma), _Rcutoff(Rcutoff), _RcutoffSq(sq(Rcutoff)){
- if (jet_beta <= 0) throw Error("ConicalGeometricMeasure: You must choose beta > 0.");
- if (beam_gamma <= 0) throw Error("ConicalGeometricMeasure: You must choose gamma > 0.");
- if (Rcutoff <= 0) throw Error("ConicalGeometricMeasure: You must choose Rcutoff > 0.");
- setTauMode(UNNORMALIZED_EVENT_SHAPE);
- }
-
- /// Description
- virtual std::string description() const;
- /// For copying purposes
- virtual ConicalGeometricMeasure* create() const {return new ConicalGeometricMeasure(*this);}
-
- /// fast jet measure
- virtual double jet_distance_squared(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
- fastjet::PseudoJet lightAxis = lightFrom(axis);
- double pseudoRsquared = 2.0*dot_product(lightFrom(axis),particle)/(lightAxis.pt()*particle.pt());
- return pseudoRsquared;
- }
-
- /// fast beam measure
- virtual double beam_distance_squared(const fastjet::PseudoJet& /*particle*/) const {
- return _RcutoffSq;
- }
-
- /// true jet measure
- virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
- double jet_dist = jet_distance_squared(particle,axis)/_RcutoffSq;
- if (jet_dist > 0.0) {
- fastjet::PseudoJet lightParticle = lightFrom(particle);
- double weight = (_beam_gamma == 1.0) ? 1.0 : std::pow(0.5*lightParticle.pt(),_beam_gamma - 1.0);
- return particle.pt() * weight * std::pow(jet_dist,_jet_beta/2.0);
- } else {
- return 0.0;
- }
- }
-
- /// true beam measure
- virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
- fastjet::PseudoJet lightParticle = lightFrom(particle);
- double weight = (_beam_gamma == 1.0) ? 1.0 : std::pow(0.5*lightParticle.pt(),_beam_gamma - 1.0);
- return particle.pt() * weight;
- }
-
- /// no denominator needed
- virtual double denominator(const fastjet::PseudoJet& /*particle*/) const {
- return std::numeric_limits<double>::quiet_NaN();
- }
-
-protected:
- double _jet_beta; ///< jet angular exponent
- double _beam_gamma; ///< beam angular exponent (gamma = 1.0 is recommended)
- double _Rcutoff; ///< effective jet radius
- double _RcutoffSq; ///< effective jet radius squared
-
-};
-
-///------------------------------------------------------------------------
-/// \class XConeMeasure
-/// \brief Dimensionful event-shape measure used in XCone jet algorithm
-///
-/// This class is the XCone Measure. This is the default measure for use with the
-/// XCone algorithm. It is identical to the conical geometric measure but with gamma = 1.0.
-///------------------------------------------------------------------------
-class XConeMeasure : public ConicalGeometricMeasure {
-
-public:
- /// Constructor
- XConeMeasure(double jet_beta, double R)
- : ConicalGeometricMeasure(jet_beta,
- 1.0, // beam_gamma, hard coded at gamma = 1.0 default
- R // Rcutoff scale
- ) { }
-
- /// Description
- virtual std::string description() const;
- /// For copying purposes
- virtual XConeMeasure* create() const {return new XConeMeasure(*this);}
-
-};
-
-///------------------------------------------------------------------------
-/// \class LightLikeAxis
-/// \brief Helper class to define light-like axes directions
-///
-/// This is a helper class for the minimization routines.
-/// It creates a convenient way of defining axes in order to better facilitate calculations.
-///------------------------------------------------------------------------
-class LightLikeAxis {
-
-public:
- /// Bare constructor
- LightLikeAxis() : _rap(0.0), _phi(0.0), _weight(0.0), _mom(0.0) {}
- /// Constructor
- LightLikeAxis(double my_rap, double my_phi, double my_weight, double my_mom) :
- _rap(my_rap), _phi(my_phi), _weight(my_weight), _mom(my_mom) {}
-
- /// Rapidity
- double rap() const {return _rap;}
- /// Azimuth
- double phi() const {return _phi;}
- /// weight factor
- double weight() const {return _weight;}
- /// pt momentum
- double mom() const {return _mom;}
-
- /// set rapidity
- void set_rap(double my_set_rap) {_rap = my_set_rap;}
- /// set azimuth
- void set_phi(double my_set_phi) {_phi = my_set_phi;}
- /// set weight factor
- void set_weight(double my_set_weight) {_weight = my_set_weight;}
- /// set pt momentum
- void set_mom(double my_set_mom) {_mom = my_set_mom;}
- /// set all kinematics
- void reset(double my_rap, double my_phi, double my_weight, double my_mom) {_rap=my_rap; _phi=my_phi; _weight=my_weight; _mom=my_mom;}
-
- /// Return PseudoJet version
- fastjet::PseudoJet ConvertToPseudoJet();
-
- /// Squared distance to PseudoJet
- double DistanceSq(const fastjet::PseudoJet& input) const {
- return DistanceSq(input.rap(),input.phi());
- }
-
- /// Distance to PseudoJet
- double Distance(const fastjet::PseudoJet& input) const {
- return std::sqrt(DistanceSq(input));
- }
-
- /// Squared distance to Lightlikeaxis
- double DistanceSq(const LightLikeAxis& input) const {
- return DistanceSq(input.rap(),input.phi());
- }
-
- /// Distance to Lightlikeaxis
- double Distance(const LightLikeAxis& input) const {
- return std::sqrt(DistanceSq(input));
- }
-
-private:
- double _rap; ///< rapidity
- double _phi; ///< azimuth
- double _weight; ///< weight factor
- double _mom; ///< pt momentum
-
- /// Internal squared distance calculation
- double DistanceSq(double rap2, double phi2) const {
- double rap1 = _rap;
- double phi1 = _phi;
-
- double distRap = rap1-rap2;
- double distPhi = std::fabs(phi1-phi2);
- if (distPhi > M_PI) {distPhi = 2.0*M_PI - distPhi;}
- return distRap*distRap + distPhi*distPhi;
- }
-
- /// Internal distance calculation
- double Distance(double rap2, double phi2) const {
- return std::sqrt(DistanceSq(rap2,phi2));
- }
-
-};
-
-
-////------------------------------------------------------------------------
-///// \class DeprecatedGeometricCutoffMeasure
-//// This class is the old, incorrectly coded geometric measure.
-//// It is kept in case anyone wants to check old code, but should not be used for production purposes.
-//class DeprecatedGeometricCutoffMeasure : public MeasureDefinition {
-//
-//public:
-//
-// // Please, please don't use this.
-// DeprecatedGeometricCutoffMeasure(double jet_beta, double Rcutoff)
-// : MeasureDefinition(),
-// _jet_beta(jet_beta),
-// _beam_beta(1.0), // This is hard coded, since alternative beta_beam values were never checked.
-// _Rcutoff(Rcutoff),
-// _RcutoffSq(sq(Rcutoff)) {
-// setTauMode(UNNORMALIZED_EVENT_SHAPE);
-// setAxisScaling(false);
-// if (jet_beta != 2.0) {
-// throw Error("Geometric minimization is currently only defined for beta = 2.0.");
-// }
-// }
-//
-// virtual std::string description() const;
-//
-// virtual DeprecatedGeometricCutoffMeasure* create() const {return new DeprecatedGeometricCutoffMeasure(*this);}
-//
-// virtual double jet_distance_squared(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
-// fastjet::PseudoJet lightAxis = lightFrom(axis);
-// double pseudoRsquared = 2.0*dot_product(lightFrom(axis),particle)/(lightAxis.pt()*particle.pt());
-// return pseudoRsquared;
-// }
-//
-// virtual double beam_distance_squared(const fastjet::PseudoJet& /*particle*/) const {
-// return _RcutoffSq;
-// }
-//
-// virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
-// fastjet::PseudoJet lightAxis = lightFrom(axis);
-// double weight = (_beam_beta == 1.0) ? 1.0 : std::pow(lightAxis.pt(),_beam_beta - 1.0);
-// return particle.pt() * weight * std::pow(jet_distance_squared(particle,axis),_jet_beta/2.0);
-// }
-//
-// virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
-// double weight = (_beam_beta == 1.0) ? 1.0 : std::pow(particle.pt()/particle.e(),_beam_beta - 1.0);
-// return particle.pt() * weight * std::pow(_Rcutoff,_jet_beta);
-// }
-//
-// virtual double denominator(const fastjet::PseudoJet& /*particle*/) const {
-// return std::numeric_limits<double>::quiet_NaN();
-// }
-//
-// virtual std::vector<fastjet::PseudoJet> get_one_pass_axes(int n_jets,
-// const std::vector<fastjet::PseudoJet>& inputs,
-// const std::vector<fastjet::PseudoJet>& seedAxes,
-// int nAttempts, // cap number of iterations
-// double accuracy // cap distance of closest approach
-// ) const;
-//
-//protected:
-// double _jet_beta;
-// double _beam_beta;
-// double _Rcutoff;
-// double _RcutoffSq;
-//
-//};
-//
-//// ------------------------------------------------------------------------
-//// / \class DeprecatedGeometricMeasure
-//// Same as DeprecatedGeometricMeasureCutoffMeasure, but with Rcutoff taken to infinity.
-//// NOTE: This class should not be used for production purposes.
-//class DeprecatedGeometricMeasure : public DeprecatedGeometricCutoffMeasure {
-//
-//public:
-// DeprecatedGeometricMeasure(double beta)
-// : DeprecatedGeometricCutoffMeasure(beta,std::numeric_limits<double>::max()) {
-// _RcutoffSq = std::numeric_limits<double>::max();
-// setTauMode(UNNORMALIZED_JET_SHAPE);
-// }
-//
-// virtual std::string description() const;
-//
-// virtual DeprecatedGeometricMeasure* create() const {return new DeprecatedGeometricMeasure(*this);}
-//};
-
-
-} //namespace Nsubjettiness
-
-}
-
-#endif // __FASTJET_CONTRIB_MEASUREDEFINITION_HH__
diff --git a/include/Rivet/Tools/Nsubjettiness/Njettiness.hh b/include/Rivet/Tools/Nsubjettiness/Njettiness.hh
deleted file mode 100644
--- a/include/Rivet/Tools/Nsubjettiness/Njettiness.hh
+++ /dev/null
@@ -1,265 +0,0 @@
-// Nsubjettiness Package
-// Questions/Comments? jthaler@jthaler.net
-//
-// Copyright (c) 2011-14
-// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
-//
-// $Id: Njettiness.hh 822 2015-06-15 23:52:57Z jthaler $
-//----------------------------------------------------------------------
-// This file is part of FastJet contrib.
-//
-// It is free software; you can redistribute it and/or modify it under
-// the terms of the GNU General Public License as published by the
-// Free Software Foundation; either version 2 of the License, or (at
-// your option) any later version.
-//
-// It is distributed in the hope that it will be useful, but WITHOUT
-// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
-// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
-// License for more details.
-//
-// You should have received a copy of the GNU General Public License
-// along with this code. If not, see <http://www.gnu.org/licenses/>.
-//----------------------------------------------------------------------
-
-#ifndef __FASTJET_CONTRIB_NJETTINESS_HH__
-#define __FASTJET_CONTRIB_NJETTINESS_HH__
-
-
-#include "MeasureDefinition.hh"
-#include "AxesDefinition.hh"
-#include "TauComponents.hh"
-
-#include "fastjet/PseudoJet.hh"
-#include "fastjet/SharedPtr.hh"
-#include <fastjet/LimitedWarning.hh>
-
-#include <cmath>
-#include <vector>
-#include <list>
-
-namespace Rivet {
-
-namespace Nsubjettiness { using namespace fastjet;
-
-/** \mainpage Nsubjettiness Documentation
- *
- * These Doxygen pages provide automatically generated documentation for the
- * Nsubjettiness FastJet contrib. This documentation is being slowly improved.
- *
- * \section core_classes Core Classes
- *
- * - Nsubjettiness: Calculating N-subjettiness jet shapes
- * - NsubjettinessRatio: Calculating N-subjettiness ratios
- * - XConePlugin: Running the XCone jet algorithm
- * - NjettinessPlugin: Running generic N-jettiness as a jet algorithm
- *
- * \subsection core_classes_helper Helper Classes for Core
- * - Njettiness: Core code for all N-(sub)jettiness calculations
- * - NjettinessExtras: Way to access additional N-jettiness information
- * - TauComponents: Output format for all N-(sub)jettiness information
- * - TauPartition: Access to N-(sub)jettiness partitioning information
- * - PseudoXConePlugin: Testing code to compare to XConePlugin (doesn't use one-pass minimization)
- *
- * \section axes_classes Axes Definitions
- *
- * \subsection axes_classes_base Base Classes
- * - AxesDefinition: Defines generic axes definition
- * - ExclusiveJetAxes: Axes finder from exclusive jet algorithm
- * - ExclusiveCombinatorialJetAxes: Axes finder from exclusive jet algorithm (with extra axes to test combinatoric options)
- * - HardestJetAxes: Axes finder from inclusive jet algorithm
- *
- * \subsection axes_classes_derived Derived Classes
- *
- * \b OnePass means iterative improvement to a (local) N-(sub)jettiness minimum.
- *
- * \b MultiPass means using multiple random seed inputs
- *
- * \b Comb means checking N + Nextra choose N combinatorial options
- *
- * - KT_Axes / OnePass_KT_Axes: Axes from exclusive kT
- * - CA_Axes / OnePass_CA_Axes: Axes from exclusive Cambridge/Aachen
- * - AntiKT_Axes / OnePass_AntiKT_Axes: Axes from inclusive anti-kT
- * - WTA_KT_Axes / OnePass_WTA_KT_Axes: Axes from exclusive kT, using winner-take-all recombination
- * - WTA_CA_Axes / OnePass_WTA_CA_Axes: Axes from exclusive CA, using winner-take-all recombination
- *
- * - GenET_GenKT_Axes / OnePass_GenET_GenKT_Axes / Comb_GenET_GenKT_Axes: Axes from exclusive generalized kt, with generalized Et recombination
- * - WTA_GenKT_Axes / OnePass_WTA_GenKT_Axes / Comb_WTA_GenKT_Axes: Axes from exclusive generalized kt, with winner-take-all recombination
- *
- * - Manual_Axes / OnePass_Manual_Axes / MultiPass_Manual_Axes: Use manual axes
- * - MultiPass_Axes: Multiple passes with random input seeds
- *
- * \subsection axes_classes_helper Helper Classes for Axes
- * - GeneralEtSchemeRecombiner: Generalized Et-scheme recombiner
- * - WinnerTakeAllRecombiner: Winner-take-all recombiner (similar functionality now in FastJet 3.1)
- * - JetDefinitionWrapper: Wrapper for Jet Definitions to handle memory management
- *
- * \section measure_classes Measure Definitions
- *
- * \subsection measure_classes_bases Base Classes
- * - MeasureDefinition: Defines generic measures
- * - DefaultMeasure: Base class for the original N-subjettiness measures
- *
- * \subsection measure_classes_derived Derived Classes
- * - NormalizedMeasure / UnnormalizedMeasure / NormalizedCutoffMeasure / UnnormalizedCutoffMeasure : Variants on the default N-subjettiness measure.
- * - ConicalMeasure: Similar to default measure, but intended as N-jettiness event shape
- * - ConicalGeometricMeasure / XConeMeasure: Measure used in XCone jet algorithm
- * - OriginalGeometricMeasure / ModifiedGeometricMeasure: Dot product measures useful for theoretical calcualtions
- *
- * \subsection measure_classes_helper Helper Classes for Measures
- * - LightLikeAxis : Defines light-like axis
- */
-
-///////
-//
-// Main Njettiness Class
-//
-///////
-
-///------------------------------------------------------------------------
-/// \class Njettiness
-/// \brief Core class for N-(sub)jettiness calculations
-///
-/**
- * The N-jettiness event shape.
- *
- * This is the core class used to perform N-jettiness jet finding (via NjettinessPlugin or XConePluggin)
- * as well as find the N-subjettiness jet shape (via Nsubjettiness).
- *
- * In general, the user should never need to call this object. In addition, its API should not be considered
- * fixed, since all code improvements effectively happen from reorganizing this class.
- *
- * Njettiness uses AxesDefinition and MeasureDefinition together in order to find tau_N for the event.
- * It also can return information about the axes and jets it used in the calculation, as well as
- * information about how the event was partitioned.
- */
-class Njettiness {
-public:
-
- /// Main constructor that uses AxesMode and MeasureDefinition to specify measure
- /// Unlike Nsubjettiness or NjettinessPlugin, the value N is not chosen
- Njettiness(const AxesDefinition & axes_def, const MeasureDefinition & measure_def);
-
- /// Destructor
- ~Njettiness() {};
-
- /// setAxes for Manual mode
- void setAxes(const std::vector<fastjet::PseudoJet> & myAxes);
-
- /// Calculates and returns all TauComponents that user would want.
- /// This information is stored in _current_tau_components for later access as well.
- TauComponents getTauComponents(unsigned n_jets, const std::vector<fastjet::PseudoJet> & inputJets) const;
-
- /// Calculates the value of N-subjettiness,
- /// but only returns the tau value from _current_tau_components
- double getTau(unsigned n_jets, const std::vector<fastjet::PseudoJet> & inputJets) const {
- return getTauComponents(n_jets, inputJets).tau();
- }
-
- /// Return all relevant information about tau components
- TauComponents currentTauComponents() const {return _current_tau_components;}
- /// Return axes found by getTauComponents.
- std::vector<fastjet::PseudoJet> currentAxes() const { return _currentAxes;}
- /// Return seedAxes used if onepass minimization (otherwise, same as currentAxes)
- std::vector<fastjet::PseudoJet> seedAxes() const { return _seedAxes;}
- /// Return jet partition found by getTauComponents.
- std::vector<fastjet::PseudoJet> currentJets() const {return _currentPartition.jets();}
- /// Return beam partition found by getTauComponents.
- fastjet::PseudoJet currentBeam() const {return _currentPartition.beam();}
- /// Return beam partition found by getTauComponents.
- TauPartition currentPartition() const {return _currentPartition;}
-
-
-private:
-
- /// AxesDefinition to use. Implemented as SharedPtrs to avoid memory management headaches
- SharedPtr<const AxesDefinition> _axes_def;
- /// MeasureDefinition to use. Implemented as SharedPtrs to avoid memory management headaches
- SharedPtr<const MeasureDefinition> _measure_def;
-
-
- // Information about the current information
- // Defined as mutables, so user should be aware that these change when getTau is called.
- // TODO: These are not thread safe and should be fixed somehow
- mutable TauComponents _current_tau_components; //automatically set to have components of 0; these values will be set by the getTau function call
- mutable std::vector<fastjet::PseudoJet> _currentAxes; //axes found after minimization
- mutable std::vector<fastjet::PseudoJet> _seedAxes; // axes used prior to minimization (if applicable)
- mutable TauPartition _currentPartition; //partitioning information
-
- /// Warning if the user tries to use v1.0.3 measure style.
- static LimitedWarning _old_measure_warning;
- /// Warning if the user tries to use v1.0.3 axes style.
- static LimitedWarning _old_axes_warning;
-
-
-public:
-
- // These interfaces are included for backwards compability, and will be deprecated in a future release (scheduled for deletion in v3.0)
-
- /// \deprecated
- /// Deprecated enum to determine axes mode
- /// The various axes choices available to the user
- /// It is recommended to use AxesDefinition instead of these.
- enum AxesMode {
- kt_axes, // exclusive kt axes
- ca_axes, // exclusive ca axes
- antikt_0p2_axes, // inclusive hardest axes with antikt-0.2
- wta_kt_axes, // Winner Take All axes with kt
- wta_ca_axes, // Winner Take All axes with CA
- onepass_kt_axes, // one-pass minimization from kt starting point
- onepass_ca_axes, // one-pass minimization from ca starting point
- onepass_antikt_0p2_axes, // one-pass minimization from antikt-0.2 starting point
- onepass_wta_kt_axes, //one-pass minimization of WTA axes with kt
- onepass_wta_ca_axes, //one-pass minimization of WTA axes with ca
- min_axes, // axes that minimize N-subjettiness (100 passes by default)
- manual_axes, // set your own axes with setAxes()
- onepass_manual_axes // one-pass minimization from manual starting point
- };
-
- /// \deprecated
- /// Deprecated enum to determine measure mode
- /// The measures available to the user.
- /// "normalized_cutoff_measure" was the default in v1.0 of Nsubjettiness
- /// "unnormalized_measure" is now the recommended default usage
- /// But it is recommended to use MeasureDefinition instead of these.
- enum MeasureMode {
- normalized_measure, //default normalized measure
- unnormalized_measure, //default unnormalized measure
- geometric_measure, //geometric measure
- normalized_cutoff_measure, //default normalized measure with explicit Rcutoff
- unnormalized_cutoff_measure, //default unnormalized measure with explicit Rcutoff
- geometric_cutoff_measure //geometric measure with explicit Rcutoff
- };
-
- /// \deprecated
- /// Intermediate constructor (needed to enable v1.0.3 backwards compatibility?)
- Njettiness(AxesMode axes_mode, const MeasureDefinition & measure_def);
-
- /// \deprecated
- /// Old-style constructor which takes axes/measure information as enums with measure parameters
- /// This version absolutely is not recommended
- Njettiness(AxesMode axes_mode,
- MeasureMode measure_mode,
- int num_para,
- double para1 = std::numeric_limits<double>::quiet_NaN(),
- double para2 = std::numeric_limits<double>::quiet_NaN(),
- double para3 = std::numeric_limits<double>::quiet_NaN())
- : _axes_def(createAxesDef(axes_mode)), _measure_def(createMeasureDef(measure_mode, num_para, para1, para2, para3)) {
- }
-
- /// \deprecated
- /// Convert old style enums into new style MeasureDefinition
- AxesDefinition* createAxesDef(AxesMode axes_mode) const;
-
- /// \deprecated
- /// Convert old style enums into new style MeasureDefinition
- MeasureDefinition* createMeasureDef(MeasureMode measure_mode, int num_para, double para1, double para2, double para3) const;
-
-};
-
-} // namespace Nsubjettiness
-
-}
-
-#endif // __FASTJET_CONTRIB_NJETTINESS_HH__
-
diff --git a/include/Rivet/Tools/Nsubjettiness/NjettinessPlugin.hh b/include/Rivet/Tools/Nsubjettiness/NjettinessPlugin.hh
deleted file mode 100644
--- a/include/Rivet/Tools/Nsubjettiness/NjettinessPlugin.hh
+++ /dev/null
@@ -1,181 +0,0 @@
-// Nsubjettiness Package
-// Questions/Comments? jthaler@jthaler.net
-//
-// Copyright (c) 2011-14
-// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
-//
-// $Id: NjettinessPlugin.hh 822 2015-06-15 23:52:57Z jthaler $
-//----------------------------------------------------------------------
-// This file is part of FastJet contrib.
-//
-// It is free software; you can redistribute it and/or modify it under
-// the terms of the GNU General Public License as published by the
-// Free Software Foundation; either version 2 of the License, or (at
-// your option) any later version.
-//
-// It is distributed in the hope that it will be useful, but WITHOUT
-// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
-// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
-// License for more details.
-//
-// You should have received a copy of the GNU General Public License
-// along with this code. If not, see <http://www.gnu.org/licenses/>.
-//----------------------------------------------------------------------
-
-#ifndef __FASTJET_CONTRIB_NJETTINESSPLUGIN_HH__
-#define __FASTJET_CONTRIB_NJETTINESSPLUGIN_HH__
-
-#include <fastjet/config.h>
-
-#include "Njettiness.hh"
-#include "MeasureDefinition.hh"
-#include "AxesDefinition.hh"
-#include "TauComponents.hh"
-
-#include "fastjet/ClusterSequence.hh"
-#include "fastjet/JetDefinition.hh"
-
-#include <string>
-#include <climits>
-
-namespace Rivet {
-
-
-namespace Nsubjettiness { using namespace fastjet;
-
-
-/// \class NjettinessPlugin
-/// \brief Implements the N-jettiness Jet Algorithm
-/**
- * An exclusive jet finder that identifies N jets; first N axes are found, then
- * particles are assigned to the nearest (DeltaR) axis and for each axis the
- * corresponding jet is simply the four-momentum sum of these particles.
- *
- * As of version 2.2, it is recommended to use the XConePlugin, which has
- * sensible default values for jet finding.
- *
- * Axes can be found in several ways, specified by the AxesDefinition argument.
- * The recommended AxesDefinitions for jet finding (different than for jet shapes)
- * OnePass_AntiKT(R0) : one-pass minimization from anti-kT starting point
- * OnePass_GenET_GenKT_Axes(delta, p, R0) : one-pass min. from GenET/KT
- * OnePass_WTA_GenKT_Axes(p, R0) : one-pass min from WTA/GenKT
- * For recommendations on which axes to use, please see the README file.
- *
- * Jet regions are determined by the MeasureDefinition. The recommended choices
- * for jet finding are
- * ConicalMeasure(beta,R0) : perfect cones in rapidity/azimuth plane
- * XConeMeasure(beta,R0) : approximate cones based on dot product distances.
- *
- * Other measures introduced in version 2.2 include OriginalGeometricMeasure,
- * ModifiedGeometricMeasure, and ConicalGeometricMeasure, which define N-jettiness
- * through dot products of particle momenta with light-like axes. OriginalGeometricMeasure
- * produces football-shaped jets due to its central weighting of the beam measure,
- * but ModifiedGeometric and ConicalGeometric both deform the original geometric measure
- * to allow for cone-shaped jets. The size of these cones can be controlled through Rcutoff
- * just as in the other measures. See the README file or MeasureDefinition.hh for information
- * on how to call these measures.
- *
- */
-class NjettinessPlugin : public JetDefinition::Plugin {
-public:
-
- /// Constructor with same arguments as Nsubjettiness (N, AxesDefinition, MeasureDefinition)
- NjettinessPlugin(int N,
- const AxesDefinition & axes_def,
- const MeasureDefinition & measure_def)
- : _njettinessFinder(axes_def, measure_def), _N(N) {}
-
-
- /// Description
- virtual std::string description () const;
- /// Jet radius (this does not make sense yet)
- virtual double R() const {return -1.0;} // TODO: make this not stupid
-
- /// The actually clustering, which first called Njettiness and then creates a dummy ClusterSequence
- virtual void run_clustering(ClusterSequence&) const;
-
- /// For using manual axes with Njettiness Plugin
- void setAxes(const std::vector<fastjet::PseudoJet> & myAxes) {
- // Cross check that manual axes are being used is in Njettiness
- _njettinessFinder.setAxes(myAxes);
- }
-
- /// Destructor
- virtual ~NjettinessPlugin() {}
-
-private:
-
- Njettiness _njettinessFinder; ///< The core Njettiness that does the heavy lifting
- int _N; ///< Number of exclusive jets to find.
-
- /// Warning if the user tries to use v1.0.3 constructor.
- static LimitedWarning _old_constructor_warning;
-
-public:
-
- // Alternative constructors that define the measure via enums and parameters
- // These constructors are deprecated and will be removed in a future version.
-
- /// \deprecated
- /// Old-style constructor with 0 arguments (DEPRECATED)
- NjettinessPlugin(int N,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode)
- : _njettinessFinder(axes_mode, measure_mode, 0), _N(N) {
- _old_constructor_warning.warn("NjettinessPlugin: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the NjettinessPlugin constructor based on AxesDefinition and MeasureDefinition instead.");
- }
-
- /// \deprecated
- /// Old-style constructor with 1 argument (DEPRECATED)
- NjettinessPlugin(int N,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode,
- double para1)
- : _njettinessFinder(axes_mode, measure_mode, 1, para1), _N(N) {
- _old_constructor_warning.warn("NjettinessPlugin: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the NjettinessPlugin constructor based on AxesDefinition and MeasureDefinition instead.");
-
- }
-
- /// \deprecated
- /// Old-style constructor with 2 arguments (DEPRECATED)
- NjettinessPlugin(int N,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode,
- double para1,
- double para2)
- : _njettinessFinder(axes_mode, measure_mode, 2, para1, para2), _N(N) {
- _old_constructor_warning.warn("NjettinessPlugin: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the NjettinessPlugin constructor based on AxesDefinition and MeasureDefinition instead.");
-
- }
-
- /// \deprecated
- /// Old-style constructor with 3 arguments (DEPRECATED)
- NjettinessPlugin(int N,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode,
- double para1,
- double para2,
- double para3)
- : _njettinessFinder(axes_mode, measure_mode, 3, para1, para2, para3), _N(N) {
- _old_constructor_warning.warn("NjettinessPlugin: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the NjettinessPlugin constructor based on AxesDefinition and MeasureDefinition instead.");
- }
-
- /// \deprecated
- /// Old-style constructor for backwards compatibility with v1.0, when NormalizedCutoffMeasure was the only option
- NjettinessPlugin(int N,
- Njettiness::AxesMode mode,
- double beta,
- double R0,
- double Rcutoff=std::numeric_limits<double>::max())
- : _njettinessFinder(mode, NormalizedCutoffMeasure(beta, R0, Rcutoff)), _N(N) {
- _old_constructor_warning.warn("NjettinessPlugin: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the NjettinessPlugin constructor based on AxesDefinition and MeasureDefinition instead.");
- }
-
-
-};
-
-} // namespace Nsubjettiness
-
-}
-
-#endif // __FASTJET_CONTRIB_NJETTINESSPLUGIN_HH__
diff --git a/include/Rivet/Tools/Nsubjettiness/Nsubjettiness.hh b/include/Rivet/Tools/Nsubjettiness/Nsubjettiness.hh
deleted file mode 100644
--- a/include/Rivet/Tools/Nsubjettiness/Nsubjettiness.hh
+++ /dev/null
@@ -1,301 +0,0 @@
-// Nsubjettiness Package
-// Questions/Comments? jthaler@jthaler.net
-//
-// Copyright (c) 2011-14
-// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
-//
-// $Id: Nsubjettiness.hh 822 2015-06-15 23:52:57Z jthaler $
-//----------------------------------------------------------------------
-// This file is part of FastJet contrib.
-//
-// It is free software; you can redistribute it and/or modify it under
-// the terms of the GNU General Public License as published by the
-// Free Software Foundation; either version 2 of the License, or (at
-// your option) any later version.
-//
-// It is distributed in the hope that it will be useful, but WITHOUT
-// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
-// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
-// License for more details.
-//
-// You should have received a copy of the GNU General Public License
-// along with this code. If not, see <http://www.gnu.org/licenses/>.
-//----------------------------------------------------------------------
-
-#ifndef __FASTJET_CONTRIB_NSUBJETTINESS_HH__
-#define __FASTJET_CONTRIB_NSUBJETTINESS_HH__
-
-#include <fastjet/internal/base.hh>
-
-#include "Njettiness.hh"
-
-#include "fastjet/FunctionOfPseudoJet.hh"
-#include <string>
-#include <climits>
-
-namespace Rivet {
-
-namespace Nsubjettiness { using namespace fastjet;
-
-// Classes defined in this file.
-class Nsubjettiness;
-class NsubjettinessRatio;
-
-///------------------------------------------------------------------------
-/// \class Nsubjettiness
-/// \brief Implements the N-subjettiness jet shape
-///
-/**
- * The N-jettiness jet shape.
- *
- * Nsubjettiness extends the concept of Njettiness to a jet shape, but other
- * than the set of particles considered, they are identical. This class
- * wraps the core Njettiness code to provide the fastjet::FunctionOfPseudoJet
- * interface for convenience in larger analyses.
- *
- * The recommended AxesDefinitions are:
- * KT_Axes : exclusive kt axes
- * WTA_KT_Axes : exclusive kt with winner-take-all recombination
- * OnePass_KT_Axes : one-pass minimization from kt starting point
- * OnePass_WTA_KT_Axes : one-pass min. from wta_kt starting point
- * More AxesDefinitions are listed in the README and defined in AxesDefinition.hh
- *
- * The recommended MeasureDefinitions are (with the corresponding parameters)
- * NormalizedMeasure(beta,R0)
- * : This was the original N-subjettiness measure (dimensionless)
- * UnnormalizedMeasure(beta)
- * : This is the new recommended default, same as above but without
- * : the normalization factor, and hence has units of GeV
- * NormalizedCutoffMeasure(beta,R0,Rcutoff)
- * : Same as normalized_measure, but cuts off at Rcutoff
- * UnnormalizedCutoffMeasure(beta,Rcutoff)
- * : Same as unnormalized_measure, but cuts off at Rcutoff
- * More MeasureDefinitions are listed in the README and defined in MeasureDefinition.hh
- *
- * For example, for the UnnormalizedMeasure(beta), N-subjettiness is defined as:
- *
- * tau_N = Sum_{i in jet} p_T^i min((DR_i1)^beta, (DR_i2)^beta, ...)
- *
- * DR_ij is the distance sqrt(Delta_phi^2 + Delta_rap^2) between particle i
- * and jet j.
- *
- * The NormalizedMeausure include an extra parameter R0, and the various cutoff
- * measures include an Rcutoff, which effectively defines an angular cutoff
- * similar in effect to a cone-jet radius.
- */
-class Nsubjettiness : public FunctionOfPseudoJet<double> {
-
-public:
-
- /// Main constructor, which takes N, the AxesDefinition, and the MeasureDefinition.
- /// The Definitions are given in AxesDefinition.hh and MeasureDefinition.hh
- Nsubjettiness(int N,
- const AxesDefinition& axes_def,
- const MeasureDefinition& measure_def)
- : _njettinessFinder(axes_def,measure_def), _N(N) {}
-
- /// Returns tau_N, measured on the constituents of this jet
- double result(const PseudoJet& jet) const;
-
- /// Returns components of tau_N, so that user can find individual tau values.
- TauComponents component_result(const PseudoJet& jet) const;
-
- /// To set axes in manual mode
- void setAxes(const std::vector<fastjet::PseudoJet> & myAxes) {
- // Note that cross check that manual mode has been set is in Njettiness
- _njettinessFinder.setAxes(myAxes);
- }
-
- /// returns seed axes used for onepass minimization (otherwise same as currentAxes)
- std::vector<fastjet::PseudoJet> seedAxes() const {
- return _njettinessFinder.seedAxes();
- }
-
- /// returns current axes found by result() calculation
- std::vector<fastjet::PseudoJet> currentAxes() const {
- return _njettinessFinder.currentAxes();
- }
-
- /// returns subjet regions found by result() calculation (these have valid constituents)
- /// Note that the axes and the subjets are not the same
- std::vector<fastjet::PseudoJet> currentSubjets() const {
- return _njettinessFinder.currentJets();
- }
-
- /// returns components of tau_N without recalculating anything
- TauComponents currentTauComponents() const {
- return _njettinessFinder.currentTauComponents();
- }
-
- /// returns components of tau_N without recalculating anything
- TauPartition currentPartition() const {
- return _njettinessFinder.currentPartition();
- }
-
-private:
-
- /// Core Njettiness code that is called
- Njettiness _njettinessFinder; // TODO: should muck with this so result can be const without this mutable
- /// Number of subjets to find
- int _N;
-
- /// Warning if the user tries to use v1.0.3 constructor.
- static LimitedWarning _old_constructor_warning;
-
-public:
-
- // The following interfaces are included for backwards compatibility, but no longer recommended.
- // They may be deleted in a future release
-
- /// \deprecated
- /// Alternative constructors that define the measure via enums and parameters
- /// These constructors will be removed in v3.0
- /// Zero parameter arguments
- /// (Currently, no measure uses this)
- Nsubjettiness(int N,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode)
- : _njettinessFinder(axes_mode, measure_mode, 0), _N(N) {
- _old_constructor_warning.warn("Nsubjettiness: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the Nsubjettiness constructor based on AxesDefinition and MeasureDefinition instead.");
- }
-
- /// \deprecated
- /// Construcotr for one parameter argument
- /// (for unnormalized_measure, para1=beta)
- Nsubjettiness(int N,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode,
- double para1)
- : _njettinessFinder(axes_mode, measure_mode, 1, para1), _N(N) {
- _old_constructor_warning.warn("Nsubjettiness: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the Nsubjettiness constructor based on AxesDefinition and MeasureDefinition instead.");
- }
-
- /// \deprecated
- /// Constructor for two parameter arguments
- /// (for normalized_measure, para1=beta, para2=R0)
- /// (for unnormalized_cutoff_measure, para1=beta, para2=Rcutoff)
- Nsubjettiness(int N,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode,
- double para1,
- double para2)
- : _njettinessFinder(axes_mode, measure_mode, 2, para1, para2), _N(N) {
- _old_constructor_warning.warn("Nsubjettiness: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the Nsubjettiness constructor based on AxesDefinition and MeasureDefinition instead.");
- }
-
- /// \deprecated
- /// Constructor for three parameter arguments
- /// (for unnormalized_cutoff_measure, para1=beta, para2=R0, para3=Rcutoff)
- Nsubjettiness(int N,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode,
- double para1,
- double para2,
- double para3)
- : _njettinessFinder(axes_mode, measure_mode, 3, para1, para2, para3), _N(N) {
- _old_constructor_warning.warn("Nsubjettiness: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the Nsubjettiness constructor based on AxesDefinition and MeasureDefinition instead.");
- }
-
- /// \deprecated
- /// Old constructor for backwards compatibility with v1.0,
- /// where normalized_cutoff_measure was the only option
- Nsubjettiness(int N,
- Njettiness::AxesMode axes_mode,
- double beta,
- double R0,
- double Rcutoff=std::numeric_limits<double>::max())
- : _njettinessFinder(axes_mode, NormalizedCutoffMeasure(beta,R0,Rcutoff)), _N(N) {
- _old_constructor_warning.warn("Nsubjettiness: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the Nsubjettiness constructor based on AxesDefinition and MeasureDefinition instead.");
- }
-
-};
-
-
-///------------------------------------------------------------------------
-/// \class NsubjettinessRatio
-/// \brief Implements ratios of N-subjettiness jet shapes
-///
-/// NsubjettinessRatio uses the results from Nsubjettiness to calculate the ratio
-/// tau_N/tau_M, where N and M are specified by the user. The ratio of different tau values
-/// is often used in analyses, so this class is helpful to streamline code. Note that
-/// manual axis mode is not supported
-class NsubjettinessRatio : public FunctionOfPseudoJet<double> {
-public:
-
- /// Main constructor. Apart from specifying both N and M, the same options as Nsubjettiness
- NsubjettinessRatio(int N,
- int M,
- const AxesDefinition & axes_def,
- const MeasureDefinition & measure_def)
- : _nsub_numerator(N,axes_def,measure_def),
- _nsub_denominator(M,axes_def,measure_def) {
- if (axes_def.needsManualAxes()) {
- throw Error("NsubjettinessRatio does not support ManualAxes mode.");
- }
- }
-
- /// Returns tau_N/tau_M based off the input jet using result function from Nsubjettiness
- double result(const PseudoJet& jet) const;
-
-private:
-
- Nsubjettiness _nsub_numerator; ///< Function for numerator
- Nsubjettiness _nsub_denominator; ///< Function for denominator
-
-public:
-
- // The following interfaces are included for backwards compatibility, but no longer recommended.
- // They may be deprecated at some point.
-
- /// \deprecated
- /// Old-style constructor for zero arguments
- /// Alternative constructor with enums and parameters
- /// Again, likely to be removed
- NsubjettinessRatio(int N,
- int M,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode)
- : _nsub_numerator(N, axes_mode, measure_mode),
- _nsub_denominator(M, axes_mode, measure_mode) {}
-
- /// \deprecated
- /// Old-style constructor for one argument
- NsubjettinessRatio(int N,
- int M,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode,
- double para1)
- : _nsub_numerator(N, axes_mode, measure_mode, para1),
- _nsub_denominator(M, axes_mode, measure_mode, para1) {}
-
- /// \deprecated
- /// Old-style constructor for 2 arguments
- NsubjettinessRatio(int N,
- int M,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode,
- double para1,
- double para2)
- : _nsub_numerator(N, axes_mode, measure_mode, para1, para2),
- _nsub_denominator(M, axes_mode, measure_mode, para1, para2) {}
-
- /// \deprecated
- /// Old-style constructor for 3 arguments
- NsubjettinessRatio(int N,
- int M,
- Njettiness::AxesMode axes_mode,
- Njettiness::MeasureMode measure_mode,
- double para1,
- double para2,
- double para3)
- : _nsub_numerator(N, axes_mode, measure_mode, para1, para2, para3),
- _nsub_denominator(M, axes_mode, measure_mode, para1, para2, para3) {}
-
-
-};
-
-} // namespace Nsubjettiness
-
-}
-
-#endif // __FASTJET_CONTRIB_NSUBJETTINESS_HH__
diff --git a/include/Rivet/Tools/Nsubjettiness/TauComponents.hh b/include/Rivet/Tools/Nsubjettiness/TauComponents.hh
deleted file mode 100644
--- a/include/Rivet/Tools/Nsubjettiness/TauComponents.hh
+++ /dev/null
@@ -1,352 +0,0 @@
-// Nsubjettiness Package
-// Questions/Comments? jthaler@jthaler.net
-//
-// Copyright (c) 2011-14
-// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
-//
-// $Id: MeasureFunction.hh 742 2014-08-23 15:43:29Z jthaler $
-//----------------------------------------------------------------------
-// This file is part of FastJet contrib.
-//
-// It is free software; you can redistribute it and/or modify it under
-// the terms of the GNU General Public License as published by the
-// Free Software Foundation; either version 2 of the License, or (at
-// your option) any later version.
-//
-// It is distributed in the hope that it will be useful, but WITHOUT
-// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
-// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
-// License for more details.
-//
-// You should have received a copy of the GNU General Public License
-// along with this code. If not, see <http://www.gnu.org/licenses/>.
-//----------------------------------------------------------------------
-
-#ifndef __FASTJET_CONTRIB_TAUCOMPONENTS_HH__
-#define __FASTJET_CONTRIB_TAUCOMPONENTS_HH__
-
-#include "fastjet/PseudoJet.hh"
-#include "fastjet/ClusterSequence.hh"
-#include "fastjet/WrappedStructure.hh"
-
-
-#include <cmath>
-#include <vector>
-#include <list>
-#include <limits>
-
-
-namespace Rivet {
-
-namespace Nsubjettiness { using namespace fastjet;
-
-// Classes defined in this file.
-class TauComponents;
-class TauPartition;
-class NjettinessExtras;
-
-///------------------------------------------------------------------------
-/// \enum TauMode
-/// Specified whether tau value has beam region or denominators
-///------------------------------------------------------------------------
-enum TauMode {
- UNDEFINED_SHAPE = -1, // Added so that constructor would default to some value
- UNNORMALIZED_JET_SHAPE = 0,
- NORMALIZED_JET_SHAPE = 1,
- UNNORMALIZED_EVENT_SHAPE = 2,
- NORMALIZED_EVENT_SHAPE = 3,
-};
-
-///////
-//
-// TauComponents
-//
-///////
-
-///------------------------------------------------------------------------
-/// \class TauComponents
-/// \brief Output wrapper for supplemental N-(sub)jettiness information
-///
-/// This class creates a wrapper for the various tau/subtau values calculated in Njettiness. This class allows Njettiness access to these variables
-/// without ever having to do the calculation itself. It takes in subtau numerators and tau denominator from MeasureFunction
-/// and outputs tau numerator, and normalized tau and subtau.
-///------------------------------------------------------------------------
-class TauComponents {
-
-public:
-
- /// empty constructor necessary to initialize tau_components in Njettiness
- /// later set correctly in Njettiness::getTau function
- TauComponents() {}
-
- /// This constructor takes input vector and double and calculates all necessary tau components
- TauComponents(TauMode tau_mode,
- const std::vector<double> & jet_pieces_numerator,
- double beam_piece_numerator,
- double denominator,
- const std::vector<PseudoJet> & jets,
- const std::vector<PseudoJet> & axes
- );
-
- /// Test for denominator
- bool has_denominator() const;
- /// Test for beam region
- bool has_beam() const;
-
- /// Return tau value
- double tau() const { return _tau; }
- /// Return jet regions
- const std::vector<double>& jet_pieces() const { return _jet_pieces; }
- /// Return beam region
- double beam_piece() const { return _beam_piece; }
-
- /// Return jet regions (no denominator)
- std::vector<double> jet_pieces_numerator() const { return _jet_pieces_numerator; }
- /// Return beam regions (no denominator)
- double beam_piece_numerator() const { return _beam_piece_numerator; }
- /// Return numerator
- double numerator() const { return _numerator; }
- /// Return denominator
- double denominator() const { return _denominator; }
-
- /// Four-vector of total jet (sum of clustered regions)
- PseudoJet total_jet() const { return _total_jet;}
- /// Four-vector of jet regions
- const std::vector<PseudoJet>& jets() const { return _jets;}
- /// Four-vector of axes
- const std::vector<PseudoJet>& axes() const { return _axes;}
-
- class StructureType;
-
-protected:
-
- /// Defines whether there is a beam or denominator
- TauMode _tau_mode;
-
- std::vector<double> _jet_pieces_numerator; ///< Constructor input (jet region numerator)
- double _beam_piece_numerator; ///< Constructor input (beam region numerator)
- double _denominator; ///< Constructor input (denominator)
-
- std::vector<double> _jet_pieces; ///< Derived value (jet regions)
- double _beam_piece; ///< Derived value (beam region)
- double _numerator; ///< Derived value (total numerator)
- double _tau; ///< Derived value (final value)
-
- PseudoJet _total_jet; ///< Total jet four-vector
- std::vector<PseudoJet> _jets; ///< Jet four-vectors
- std::vector<PseudoJet> _axes; ///< AXes four-vectors
-
-};
-
-///////
-//
-// TauPartition
-//
-///////
-
-///------------------------------------------------------------------------
-/// \class TauPartition
-/// \brief Output wrapper for N-(sub)jettiness partitioning information
-///
-/// Class for storing partitioning information.
-///------------------------------------------------------------------------
-class TauPartition {
-
-public:
- /// empty constructor
- TauPartition() {}
-
- /// Make partition of size to hold n_jet partitions
- TauPartition(int n_jet) {
- _jets_list.resize(n_jet);
- _jets_partition.resize(n_jet);
- }
-
- /// add a particle to the jet
- void push_back_jet(int jet_num, const PseudoJet& part_to_add, int part_index) {
- _jets_list[jet_num].push_back(part_index);
- _jets_partition[jet_num].push_back(part_to_add);
- }
-
- /// add a particle to the beam
- void push_back_beam(const PseudoJet& part_to_add, int part_index) {
- _beam_list.push_back(part_index);
- _beam_partition.push_back(part_to_add);
- }
-
- /// return jet regions
- PseudoJet jet(int jet_num) const { return join(_jets_partition.at(jet_num)); }
- /// return beam region
- PseudoJet beam() const { return join(_beam_partition);}
-
- /// return jets
- std::vector<PseudoJet> jets() const {
- std::vector<PseudoJet> jets;
- for (unsigned int i = 0; i < _jets_partition.size(); i++) {
- jets.push_back(jet(i));
- }
- return jets;
- }
-
- /// jets in list form
- const std::list<int> & jet_list(int jet_num) const { return _jets_list.at(jet_num);}
- /// beam in list form
- const std::list<int> & beam_list() const { return _beam_list;}
- /// all jets in list form
- const std::vector<std::list<int> > & jets_list() const { return _jets_list;}
-
-private:
-
- std::vector<std::list<int> > _jets_list; ///< jets in list form
- std::list<int> _beam_list; ///< beam in list form
-
- std::vector<std::vector<PseudoJet> > _jets_partition; ///< Partition in jet regions
- std::vector<PseudoJet> _beam_partition; ///< Partition in beam region
-
-};
-
-
-///////
-//
-// NjettinessExtras
-//
-///////
-
-///------------------------------------------------------------------------
-/// \class NjettinessExtras
-/// \brief ClusterSequence add on for N-jettiness information
-///
-/// This class contains the same information as TauComponents, but adds additional ways of linking up
-/// the jets found in the ClusterSequence::Extras class.
-/// This is done in order to help improve the interface for the main NjettinessPlugin class.
-///------------------------------------------------------------------------
-class NjettinessExtras : public ClusterSequence::Extras, public TauComponents {
-
-public:
- /// Constructor
- NjettinessExtras(TauComponents tau_components,
- std::vector<int> cluster_hist_indices)
- : TauComponents(tau_components), _cluster_hist_indices(cluster_hist_indices) {}
-
-
-
- /// Ask for tau of the whole event, but by querying a jet
- double tau(const fastjet::PseudoJet& /*jet*/) const {return _tau;}
-
- /// Ask for tau of an individual jet
- double tau_piece(const fastjet::PseudoJet& jet) const {
- if (labelOf(jet) == -1) return std::numeric_limits<double>::quiet_NaN(); // nonsense
- return _jet_pieces[labelOf(jet)];
- }
-
- /// Find axis associated with jet
- fastjet::PseudoJet axis(const fastjet::PseudoJet& jet) const {
- return _axes[labelOf(jet)];
- }
-
- /// Check if extra information is available.
- bool has_njettiness_extras(const fastjet::PseudoJet& jet) const {
- return (labelOf(jet) >= 0);
- }
-
-private:
-
- /// Store cluster history indices to link up with ClusterSequence
- std::vector<int> _cluster_hist_indices;
-
- /// Figure out which jet things belonged to
- int labelOf(const fastjet::PseudoJet& jet) const {
- int thisJet = -1;
- for (unsigned int i = 0; i < _jets.size(); i++) {
- if (_cluster_hist_indices[i] == jet.cluster_hist_index()) {
- thisJet = i;
- break;
- }
- }
- return thisJet;
- }
-
-public:
-
- // These are old methods for gaining this information
- // The recommended interface is given in TauComponents
-
- /// Tau value
- double totalTau() const {return _tau;}
- /// Jet regions
- std::vector<double> subTaus() const {return _jet_pieces;}
-
- /// Tau value
- double totalTau(const fastjet::PseudoJet& /*jet*/) const {
- return _tau;
- }
-
- /// Jet region
- double subTau(const fastjet::PseudoJet& jet) const {
- if (labelOf(jet) == -1) return std::numeric_limits<double>::quiet_NaN(); // nonsense
- return _jet_pieces[labelOf(jet)];
- }
-
- /// beam region
- double beamTau() const {
- return _beam_piece;
- }
-
-};
-
-
-/// Helper function to find out what njettiness_extras are (from jet)
-inline const NjettinessExtras * njettiness_extras(const fastjet::PseudoJet& jet) {
- const ClusterSequence * myCS = jet.associated_cluster_sequence();
- if (myCS == NULL) return NULL;
- const NjettinessExtras* extras = dynamic_cast<const NjettinessExtras*>(myCS->extras());
- return extras;
-}
-
-/// Helper function to find out what njettiness_extras are (from ClusterSequence)
-inline const NjettinessExtras * njettiness_extras(const fastjet::ClusterSequence& myCS) {
- const NjettinessExtras* extras = dynamic_cast<const NjettinessExtras*>(myCS.extras());
- return extras;
-}
-
-///////
-//
-// TauComponents::StructureType
-//
-///////
-
-
-///------------------------------------------------------------------------
-/// \class TauComponents::StructureType
-/// \brief Wrapped structure for jet-based N-(sub)jettiness information
-///
-/// Small wrapped structure to store tau information
-/// TODO: Can these be auto-joined?
-///------------------------------------------------------------------------
-class TauComponents::StructureType : public WrappedStructure {
-
-public:
- /// Constructor
- StructureType(const PseudoJet& j) :
- WrappedStructure(j.structure_shared_ptr())
- {}
-
- /// tau associated with jet
- double tau_piece() const { return _tau_piece; }
-
- /// alternative call, though might be confusing
- double tau() const { return _tau_piece; }
-
-private:
- friend class TauComponents;
- double _tau_piece; ///< tau value associated with jet
-};
-
-
-
-
-} //namespace Nsubjettiness
-
-}
-
-#endif // __FASTJET_CONTRIB_TAUCOMPONENTS_HH__
diff --git a/include/Rivet/Tools/Nsubjettiness/XConePlugin.hh b/include/Rivet/Tools/Nsubjettiness/XConePlugin.hh
deleted file mode 100644
--- a/include/Rivet/Tools/Nsubjettiness/XConePlugin.hh
+++ /dev/null
@@ -1,169 +0,0 @@
-// Nsubjettiness Package
-// Questions/Comments? jthaler@jthaler.net
-//
-// Copyright (c) 2011-14
-// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
-//
-// $Id: XConePlugin.hh 748 2014-10-02 06:13:28Z tjwilk $
-//----------------------------------------------------------------------
-// This file is part of FastJet contrib.
-//
-// It is free software; you can redistribute it and/or modify it under
-// the terms of the GNU General Public License as published by the
-// Free Software Foundation; either version 2 of the License, or (at
-// your option) any later version.
-//
-// It is distributed in the hope that it will be useful, but WITHOUT
-// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
-// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
-// License for more details.
-//
-// You should have received a copy of the GNU General Public License
-// along with this code. If not, see <http://www.gnu.org/licenses/>.
-//----------------------------------------------------------------------
-
-#ifndef __FASTJET_CONTRIB_XCONEPLUGIN_HH__
-#define __FASTJET_CONTRIB_XCONEPLUGIN_HH__
-
-#include <fastjet/config.h>
-
-#include "NjettinessPlugin.hh"
-
-#include "fastjet/ClusterSequence.hh"
-#include "fastjet/JetDefinition.hh"
-
-#include <string>
-#include <climits>
-
-namespace Rivet {
-
-
-namespace Nsubjettiness { using namespace fastjet;
-
-///------------------------------------------------------------------------
-/// \class XConePlugin
-/// \brief Implements the XCone Jet Algorithm
-/**
- * An exclusive jet finder that identifies N jets. First N axes are found, then
- * particles are assigned to the nearest (approximte DeltaR) axis and for each axis the
- * corresponding jet is simply the four-momentum sum of these particles.
- *
- * The XConePlugin is based on NjettinessPlugin, but with sensible default
- * values for the AxesDefinition and MeasureDefinition. There are three arguments
- *
- * int N: number of exclusive jets to be found
- * double R0: approximate jet radius
- * double beta: determines style of jet finding with the recommended values being:
- * beta = 2: standard "mean" jets where jet momentum/axis align approximately.
- * beta = 1: recoil-free "median" variant where jet axis points at hardest cluster.
- *
- * The AxesDefinition is OnePass_GenET_GenKT_Axes, which uses a generalized kT
- * clustering algorithm matched to the beta value.
- *
- * The MeasureDefinition is the XConeMeasure, which is based on the
- * ConicalGeometric measure.
- */
-class XConePlugin : public NjettinessPlugin {
-public:
-
- /// Constructor with N, R0, and beta as the options. beta = 2.0 is the default
- /// All this does is use the NjettinessPlugin with OnePass_GenET_GenKT_Axes and the XConeMeasure.
- /// For more advanced usage, call NjettinessPlugin directly
- /// Note that the order of the R0 and beta values is reversed from the XConeMeasure to
- /// standard usage for Plugins.
- XConePlugin(int N, double R0, double beta = 2.0)
- : NjettinessPlugin(N,
- OnePass_GenET_GenKT_Axes(calc_delta(beta), calc_power(beta), R0), // use recommended axes method only
- XConeMeasure(beta, R0) // use recommended XCone measure.
- ),
- _N(N), _R0(R0), _beta(beta)
- {}
-
- // The things that are required by base class.
- virtual std::string description () const;
- virtual double R() const {return _R0;}
-
- // run_clustering is done by NjettinessPlugin
-
- virtual ~XConePlugin() {}
-
-private:
-
- /// Static call used within the constructor to set the recommended delta value
- static double calc_delta(double beta) {
- double delta;
- if (beta > 1) delta = 1/(beta - 1);
- else delta = std::numeric_limits<int>::max(); // use winner take all
- return delta;
- }
-
- /// Static call used within the constructor to set the recommended p value
- static double calc_power(double beta) {
- return (double) 1.0/beta;
- }
-
- double _N; ///< Number of desired jets
- double _R0; ///< Jet radius
- double _beta; ///< Angular exponent (beta = 2.0 is dafault, beta = 1.0 is recoil-free)
-
-public:
-
-};
-
-
-/// \class PseudoXConePlugin
-/// \brief Implements a faster, non-optimal version of the XCone Jet Algorithm
-///
-/// A "poor man's" version of XCone with no minimization step
-/// Right now, used just for testing purposes by the developers
-class PseudoXConePlugin : public NjettinessPlugin {
-public:
-
- /// Constructor with N, R0, and beta as the options. beta = 2.0 is the default
- /// All this does is use the NjettinessPlugin with GenET_GenKT_Axes and the XConeMeasure.
- PseudoXConePlugin(int N, double R0, double beta = 2.0)
- : NjettinessPlugin(N,
- GenET_GenKT_Axes(calc_delta(beta), calc_power(beta), R0), // poor man's axes
- XConeMeasure(beta, R0) // use recommended XCone measure.
- ),
- _N(N), _R0(R0), _beta(beta)
- {}
-
- // The things that are required by base class.
- virtual std::string description () const;
- virtual double R() const {return _R0;}
-
- // run_clustering is done by NjettinessPlugin
-
- virtual ~PseudoXConePlugin() {}
-
-private:
-
- /// Static call used within the constructor to set the recommended delta value
- static double calc_delta(double beta) {
- double delta;
- if (beta > 1) delta = 1/(beta - 1);
- else delta = std::numeric_limits<int>::max(); // use winner take all
- return delta;
- }
-
- /// Static call used within the constructor to set the recommended p value
- static double calc_power(double beta) {
- return (double) 1.0/beta;
- }
-
- double _N; ///< Number of desired jets
- double _R0; ///< Jet radius
- double _beta; ///< Angular exponent (beta = 2.0 is dafault, beta = 1.0 is recoil-free)
-
-public:
-
-};
-
-
-
-} // namespace Nsubjettiness
-
-}
-
-#endif // __FASTJET_CONTRIB_XConePlugin_HH__
diff --git a/include/Rivet/Tools/RivetFastJet.hh b/include/Rivet/Tools/RivetFastJet.hh
--- a/include/Rivet/Tools/RivetFastJet.hh
+++ b/include/Rivet/Tools/RivetFastJet.hh
@@ -1,37 +1,40 @@
#ifndef RIVET_RIVETFASTJET_HH
#define RIVET_RIVETFASTJET_HH
#include "Rivet/Config/RivetCommon.hh"
#include "fastjet/JetDefinition.hh"
#include "fastjet/AreaDefinition.hh"
#include "fastjet/ClusterSequence.hh"
#include "fastjet/ClusterSequenceArea.hh"
#include "fastjet/PseudoJet.hh"
#include "fastjet/tools/Filter.hh"
+#include "fastjet/tools/Recluster.hh"
namespace Rivet {
/// Unscoped awareness of FastJet's PseudoJet
using fastjet::PseudoJet;
+ using fastjet::ClusterSequence;
+ using fastjet::JetDefinition;
/// Typedef for a collection of PseudoJet objects.
/// @todo Make into an explicit container with conversion to Jets and FourMomenta?
typedef std::vector<PseudoJet> PseudoJets;
/// Make a 3-momentum vector from a FastJet pseudojet
inline Vector3 momentum3(const fastjet::PseudoJet& pj) {
return Vector3(pj.px(), pj.py(), pj.pz());
}
/// Make a 4-momentum vector from a FastJet pseudojet
inline FourMomentum momentum(const fastjet::PseudoJet& pj) {
return FourMomentum(pj.E(), pj.px(), pj.py(), pj.pz());
}
}
#endif
diff --git a/include/Rivet/Tools/SmearingFunctions.hh b/include/Rivet/Tools/SmearingFunctions.hh
--- a/include/Rivet/Tools/SmearingFunctions.hh
+++ b/include/Rivet/Tools/SmearingFunctions.hh
@@ -1,741 +1,764 @@
// -*- C++ -*-
#ifndef RIVET_SmearingFunctions_HH
#define RIVET_SmearingFunctions_HH
#include "Rivet/Tools/MomentumSmearingFunctions.hh"
#include "Rivet/Tools/ParticleSmearingFunctions.hh"
#include "Rivet/Tools/JetSmearingFunctions.hh"
namespace Rivet {
/// @name Electron efficiency and smearing functions
//@{
/// ATLAS Run 1 electron reconstruction efficiency
/// @todo Include reco eff (but no e/y discrimination) in forward region
/// @todo How to use this in combination with tracking eff?
inline double ELECTRON_EFF_ATLAS_RUN1(const Particle& e) {
if (e.abseta() > 2.5) return 0;
if (e.pT() < 10*GeV) return 0;
return (e.abseta() < 1.5) ? 0.95 : 0.85;
}
/// ATLAS Run 2 electron reco efficiency
/// @todo Currently just a copy of Run 1: fix!
inline double ELECTRON_EFF_ATLAS_RUN2(const Particle& e) {
return ELECTRON_EFF_ATLAS_RUN1(e);
}
/// @brief ATLAS Run 2 'loose' electron identification/selection efficiency
///
/// Values read from Fig 3 of ATL-PHYS-PUB-2015-041
/// @todo What about faking by jets or non-electrons?
inline double ELECTRON_IDEFF_ATLAS_RUN2_LOOSE(const Particle& e) {
// Manually symmetrised eta eff histogram
const static vector<double> edges_eta = { 0.0, 0.1, 0.8, 1.37, 1.52, 2.01, 2.37, 2.47 };
const static vector<double> effs_eta = { 0.950, 0.965, 0.955, 0.885, 0.950, 0.935, 0.90 };
// Et eff histogram (10-20 is a guess)
const static vector<double> edges_et = { 0, 10, 20, 25, 30, 35, 40, 45, 50, 60, 80 };
const static vector<double> effs_et = { 0.0, 0.90, 0.91, 0.92, 0.94, 0.95, 0.955, 0.965, 0.97, 0.98 };
if (e.abseta() > 2.47) return 0.0; // no ID outside the tracker
const int i_eta = binIndex(e.abseta(), edges_eta);
const int i_et = binIndex(e.Et()/GeV, edges_et, true);
const double eff = effs_et[i_et] * effs_eta[i_eta] / 0.95; //< norm factor as approximate double differential
return min(eff, 1.0);
}
/// @brief ATLAS Run 1 'medium' electron identification/selection efficiency
inline double ELECTRON_IDEFF_ATLAS_RUN1_MEDIUM(const Particle& e) {
const static vector<double> eta_edges_10 = {0.000, 0.049, 0.454, 1.107, 1.46, 1.790, 2.277, 2.500};
const static vector<double> eta_vals_10 = {0.730, 0.757, 0.780, 0.771, 0.77, 0.777, 0.778};
const static vector<double> eta_edges_15 = {0.000, 0.053, 0.456, 1.102, 1.463, 1.783, 2.263, 2.500};
const static vector<double> eta_vals_15 = {0.780, 0.800, 0.819, 0.759, 0.749, 0.813, 0.829};
const static vector<double> eta_edges_20 = {0.000, 0.065, 0.362, 0.719, 0.980, 1.289, 1.455, 1.681, 1.942, 2.239, 2.452, 2.500};
const static vector<double> eta_vals_20 = {0.794, 0.806, 0.816, 0.806, 0.797, 0.774, 0.764, 0.788, 0.793, 0.806, 0.825};
const static vector<double> eta_edges_25 = {0.000, 0.077, 0.338, 0.742, 1.004, 1.265, 1.467, 1.692, 1.940, 2.227, 2.452, 2.500};
const static vector<double> eta_vals_25 = {0.833, 0.843, 0.853, 0.845, 0.839, 0.804, 0.790, 0.825, 0.830, 0.833, 0.839};
const static vector<double> eta_edges_30 = {0.000, 0.077, 0.350, 0.707, 0.980, 1.289, 1.479, 1.681, 1.942, 2.239, 2.441, 2.500};
const static vector<double> eta_vals_30 = {0.863, 0.872, 0.881, 0.874, 0.870, 0.824, 0.808, 0.847, 0.845, 0.840, 0.842};
const static vector<double> eta_edges_35 = {0.000, 0.058, 0.344, 0.700, 1.009, 1.270, 1.458, 1.685, 1.935, 2.231, 2.468, 2.500};
const static vector<double> eta_vals_35 = {0.878, 0.889, 0.901, 0.895, 0.893, 0.849, 0.835, 0.868, 0.863, 0.845, 0.832};
const static vector<double> eta_edges_40 = {0.000, 0.047, 0.355, 0.699, 0.983, 1.280, 1.446, 1.694, 1.943, 2.227, 2.441, 2.500};
const static vector<double> eta_vals_40 = {0.894, 0.901, 0.909, 0.905, 0.904, 0.875, 0.868, 0.889, 0.876, 0.848, 0.827};
const static vector<double> eta_edges_45 = {0.000, 0.058, 0.356, 0.712, 0.997, 1.282, 1.459, 1.686, 1.935, 2.220, 2.444, 2.500};
const static vector<double> eta_vals_45 = {0.900, 0.911, 0.923, 0.918, 0.917, 0.897, 0.891, 0.904, 0.894, 0.843, 0.796};
const static vector<double> eta_edges_50 = {0.000, 0.059, 0.355, 0.711, 0.983, 1.280, 1.469, 1.682, 1.919, 2.227, 2.441, 2.500};
const static vector<double> eta_vals_50 = {0.903, 0.913, 0.923, 0.922, 0.923, 0.903, 0.898, 0.908, 0.895, 0.831, 0.774};
const static vector<double> eta_edges_60 = {0.000, 0.053, 0.351, 0.720, 1.006, 1.291, 1.469, 1.696, 1.946, 2.243, 2.455, 2.500};
const static vector<double> eta_vals_60 = {0.903, 0.917, 0.928, 0.924, 0.927, 0.915, 0.911, 0.915, 0.899, 0.827, 0.760};
const static vector<double> eta_edges_80 = {0.000, 0.053, 0.351, 0.720, 0.994, 1.292, 1.482, 1.708, 1.934, 2.220, 2.458, 2.500};
const static vector<double> eta_vals_80 = {0.936, 0.942, 0.952, 0.956, 0.956, 0.934, 0.931, 0.944, 0.933, 0.940, 0.948};
const static vector<double> et_edges = { 10, 15, 20, 25, 30, 35, 40, 45, 50, 60, 80 };
const static vector< vector<double> > et_eta_edges = { eta_edges_10, eta_edges_15, eta_edges_20, eta_edges_25, eta_edges_30, eta_edges_35, eta_edges_40, eta_edges_45, eta_edges_50, eta_edges_60, eta_edges_80 };
const static vector< vector<double> > et_eta_vals = { eta_vals_10, eta_vals_15, eta_vals_20, eta_vals_25, eta_vals_30, eta_vals_35, eta_vals_40, eta_vals_45, eta_vals_50, eta_vals_60, eta_vals_80 };
if (e.abseta() > 2.5 || e.Et() < 10*GeV) return 0.0;
const int i_et = binIndex(e.Et()/GeV, et_edges, true);
const int i_eta = binIndex(e.abseta(), et_eta_edges[i_et]);
return et_eta_vals[i_et][i_eta];
}
/// @brief ATLAS Run 2 'medium' electron identification/selection efficiency
/// @todo Currently just a copy of Run 1: fix!
inline double ELECTRON_IDEFF_ATLAS_RUN2_MEDIUM(const Particle& e) {
return ELECTRON_IDEFF_ATLAS_RUN1_MEDIUM(e);
}
/// @brief ATLAS Run 1 'tight' electron identification/selection efficiency
inline double ELECTRON_IDEFF_ATLAS_RUN1_TIGHT(const Particle& e) {
const static vector<double> eta_edges_10 = {0.000, 0.049, 0.459, 1.100, 1.461, 1.789, 2.270, 2.500};
const static vector<double> eta_vals_10 = {0.581, 0.632, 0.668, 0.558, 0.548, 0.662, 0.690};
const static vector<double> eta_edges_15 = {0.000, 0.053, 0.450, 1.096, 1.463, 1.783, 2.269, 2.500};
const static vector<double> eta_vals_15 = {0.630, 0.678, 0.714, 0.633, 0.616, 0.700, 0.733};
const static vector<double> eta_edges_20 = {0.000, 0.065, 0.362, 0.719, 0.992, 1.277, 1.479, 1.692, 1.930, 2.227, 2.464, 2.500};
const static vector<double> eta_vals_20 = {0.653, 0.695, 0.735, 0.714, 0.688, 0.635, 0.625, 0.655, 0.680, 0.691, 0.674};
const static vector<double> eta_edges_25 = {0.000, 0.077, 0.362, 0.719, 0.992, 1.300, 1.479, 1.692, 1.942, 2.227, 2.464, 2.500};
const static vector<double> eta_vals_25 = {0.692, 0.732, 0.768, 0.750, 0.726, 0.677, 0.667, 0.692, 0.710, 0.706, 0.679};
const static vector<double> eta_edges_30 = {0.000, 0.053, 0.362, 0.719, 1.004, 1.277, 1.467, 1.681, 1.954, 2.239, 2.452, 2.500};
const static vector<double> eta_vals_30 = {0.724, 0.763, 0.804, 0.789, 0.762, 0.702, 0.690, 0.720, 0.731, 0.714, 0.681};
const static vector<double> eta_edges_35 = {0.000, 0.044, 0.342, 0.711, 0.971, 1.280, 1.456, 1.683, 1.944, 2.218, 2.442, 2.500};
const static vector<double> eta_vals_35 = {0.736, 0.778, 0.824, 0.811, 0.784, 0.730, 0.718, 0.739, 0.743, 0.718, 0.678};
const static vector<double> eta_edges_40 = {0.000, 0.047, 0.355, 0.699, 0.983, 1.268, 1.457, 1.671, 1.931, 2.204, 2.453, 2.500};
const static vector<double> eta_vals_40 = {0.741, 0.774, 0.823, 0.823, 0.802, 0.764, 0.756, 0.771, 0.771, 0.734, 0.684};
const static vector<double> eta_edges_45 = {0.000, 0.056, 0.354, 0.711, 0.984, 1.280, 1.458, 1.684, 1.945, 2.207, 2.442, 2.500};
const static vector<double> eta_vals_45 = {0.758, 0.792, 0.841, 0.841, 0.823, 0.792, 0.786, 0.796, 0.794, 0.734, 0.663};
const static vector<double> eta_edges_50 = {0.000, 0.059, 0.355, 0.699, 0.983, 1.268, 1.446, 1.682, 1.943, 2.216, 2.453, 2.500};
const static vector<double> eta_vals_50 = {0.771, 0.806, 0.855, 0.858, 0.843, 0.810, 0.800, 0.808, 0.802, 0.730, 0.653};
const static vector<double> eta_edges_60 = {0.000, 0.050, 0.350, 0.707, 0.981, 1.278, 1.468, 1.694, 1.944, 2.242, 2.453, 2.500};
const static vector<double> eta_vals_60 = {0.773, 0.816, 0.866, 0.865, 0.853, 0.820, 0.812, 0.817, 0.804, 0.726, 0.645};
const static vector<double> eta_edges_80 = {0.000, 0.051, 0.374, 0.720, 0.981, 1.279, 1.468, 1.707, 1.945, 2.207, 2.457, 2.500};
const static vector<double> eta_vals_80 = {0.819, 0.855, 0.899, 0.906, 0.900, 0.869, 0.865, 0.873, 0.869, 0.868, 0.859};
const static vector<double> et_edges = { 10, 15, 20, 25, 30, 35, 40, 45, 50, 60, 80 };
const static vector< vector<double> > et_eta_edges = { eta_edges_10, eta_edges_15, eta_edges_20, eta_edges_25, eta_edges_30, eta_edges_35, eta_edges_40, eta_edges_45, eta_edges_50, eta_edges_60, eta_edges_80 };
const static vector< vector<double> > et_eta_vals = { eta_vals_10, eta_vals_15, eta_vals_20, eta_vals_25, eta_vals_30, eta_vals_35, eta_vals_40, eta_vals_45, eta_vals_50, eta_vals_60, eta_vals_80 };
if (e.abseta() > 2.5 || e.Et() < 10*GeV) return 0.0;
const int i_et = binIndex(e.Et()/GeV, et_edges, true);
const int i_eta = binIndex(e.abseta(), et_eta_edges[i_et]);
return et_eta_vals[i_et][i_eta];
}
/// @brief ATLAS Run 2 'tight' electron identification/selection efficiency
/// @todo Currently just a copy of Run 1: fix!
inline double ELECTRON_IDEFF_ATLAS_RUN2_TIGHT(const Particle& e) {
return ELECTRON_IDEFF_ATLAS_RUN1_TIGHT(e);
}
/// ATLAS Run 1 electron reco smearing
inline Particle ELECTRON_SMEAR_ATLAS_RUN1(const Particle& e) {
static const vector<double> edges_eta = {0., 2.5, 3.};
static const vector<double> edges_pt = {0., 0.1, 25.};
static const vector<double> e2s = {0.000, 0.015, 0.005,
0.005, 0.005, 0.005,
0.107, 0.107, 0.107};
static const vector<double> es = {0.00, 0.00, 0.05,
0.05, 0.05, 0.05,
2.08, 2.08, 2.08};
static const vector<double> cs = {0.00, 0.00, 0.25,
0.25, 0.25, 0.25,
0.00, 0.00, 0.00};
const int i_eta = binIndex(e.abseta(), edges_eta, true);
const int i_pt = binIndex(e.pT()/GeV, edges_pt, true);
const int i = i_eta*edges_pt.size() + i_pt;
// Calculate absolute resolution in GeV
const double c1 = sqr(e2s[i]), c2 = sqr(es[i]), c3 = sqr(cs[i]);
const double resolution = sqrt(c1*e.E2() + c2*e.E() + c3) * GeV;
// normal_distribution<> d(e.E(), resolution);
// const double mass = e.mass2() > 0 ? e.mass() : 0; //< numerical carefulness...
// const double smeared_E = max(d(gen), mass); //< can't let the energy go below the mass!
// return Particle(e.pid(), FourMomentum::mkEtaPhiME(e.eta(), e.phi(), mass, smeared_E));
return Particle(e.pid(), P4_SMEAR_E_GAUSS(e, resolution));
}
/// ATLAS Run 2 electron reco smearing
/// @todo Currently just a copy of the Run 1 version: fix!
inline Particle ELECTRON_SMEAR_ATLAS_RUN2(const Particle& e) {
return ELECTRON_SMEAR_ATLAS_RUN1(e);
}
/// @todo Add charge flip efficiency?
/// CMS Run 1 electron reconstruction efficiency
inline double ELECTRON_EFF_CMS_RUN1(const Particle& e) {
if (e.abseta() > 2.5) return 0;
if (e.pT() < 10*GeV) return 0;
return (e.abseta() < 1.5) ? 0.95 : 0.85;
}
/// CMS Run 2 electron reco efficiency
/// @todo Currently just a copy of Run 1: fix!
inline double ELECTRON_EFF_CMS_RUN2(const Particle& e) {
return ELECTRON_EFF_CMS_RUN1(e);
}
/// @brief CMS electron energy smearing, preserving direction
///
/// Calculate resolution
/// for pT > 0.1 GeV, E resolution = |eta| < 0.5 -> sqrt(0.06^2 + pt^2 * 1.3e-3^2)
/// |eta| < 1.5 -> sqrt(0.10^2 + pt^2 * 1.7e-3^2)
/// |eta| < 2.5 -> sqrt(0.25^2 + pt^2 * 3.1e-3^2)
inline Particle ELECTRON_SMEAR_CMS_RUN1(const Particle& e) {
// Calculate absolute resolution in GeV from functional form
double resolution = 0;
const double abseta = e.abseta();
if (e.pT() > 0.1*GeV && abseta < 2.5) { //< should be a given from efficiencies
if (abseta < 0.5) {
resolution = add_quad(0.06, 1.3e-3 * e.pT()/GeV) * GeV;
} else if (abseta < 1.5) {
resolution = add_quad(0.10, 1.7e-3 * e.pT()/GeV) * GeV;
} else { // still |eta| < 2.5
resolution = add_quad(0.25, 3.1e-3 * e.pT()/GeV) * GeV;
}
}
// normal_distribution<> d(e.E(), resolution);
// const double mass = e.mass2() > 0 ? e.mass() : 0; //< numerical carefulness...
// const double smeared_E = max(d(gen), mass); //< can't let the energy go below the mass!
// return Particle(e.pid(), FourMomentum::mkEtaPhiME(e.eta(), e.phi(), mass, smeared_E));
return Particle(e.pid(), P4_SMEAR_E_GAUSS(e, resolution));
}
/// CMS Run 2 electron reco smearing
/// @todo Currently just a copy of the Run 1 version: fix!
inline Particle ELECTRON_SMEAR_CMS_RUN2(const Particle& e) {
return ELECTRON_SMEAR_CMS_RUN1(e);
}
//@}
/// @name Photon efficiency and smearing functions
//@{
/// @brief ATLAS Run 2 photon reco efficiency
///
/// Taken from converted photons, Fig 8, in arXiv:1606.01813
inline double PHOTON_EFF_ATLAS_RUN1(const Particle& y) {
if (y.pT() < 10*GeV) return 0;
if (inRange(y.abseta(), 1.37, 1.52) || y.abseta() > 2.37) return 0;
static const vector<double> edges_eta = {0., 0.6, 1.37, 1.52, 1.81, 2.37};
static const vector<double> edges_pt = {10., 15., 20., 25., 30., 35., 40., 45.,
50., 60., 80., 100., 125., 150., 175., 250.};
static const vector<double> effs = {0.53, 0.65, 0.73, 0.83, 0.86, 0.93, 0.94, 0.96,
0.97, 0.98, 0.98, 0.98, 0.98, 0.98, 0.98, 0.98,//
0.45, 0.57, 0.67, 0.74, 0.84, 0.87, 0.93, 0.94,
0.95, 0.96, 0.97, 0.98, 0.98, 0.99, 0.99, 0.99,//
0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00,
0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00,//
0.48, 0.56, 0.68, 0.76, 0.86, 0.90, 0.93, 0.95,
0.96, 0.97, 0.98, 0.99, 0.99, 1.00, 1.00, 1.00,//
0.50, 0.61, 0.74, 0.82, 0.88, 0.92, 0.94, 0.95,
0.96, 0.97, 0.98, 0.98, 0.98, 0.98, 0.99, 0.99};
const int i_eta = binIndex(y.abseta(), edges_eta);
const int i_pt = binIndex(y.pT()/GeV, edges_pt, true);
const int i = i_eta*edges_pt.size() + i_pt;
const double eff = effs[i];
return eff;
}
/// @brief ATLAS Run 2 photon reco efficiency
///
/// Taken from converted photons, Fig 6, in ATL-PHYS-PUB-2016-014
inline double PHOTON_EFF_ATLAS_RUN2(const Particle& y) {
if (y.pT() < 10*GeV) return 0;
if (inRange(y.abseta(), 1.37, 1.52) || y.abseta() > 2.37) return 0;
static const vector<double> edges_eta = {0., 0.6, 1.37, 1.52, 1.81, 2.37};
static const vector<double> edges_pt = {10., 15., 20., 25., 30., 35., 40., 45.,
50., 60., 80., 100., 125., 150., 175., 250.};
static const vector<double> effs = {0.55, 0.70, 0.85, 0.89, 0.93, 0.95, 0.96, 0.96,
0.97, 0.97, 0.98, 0.97, 0.97, 0.97, 0.97, 0.97,//
0.47, 0.66, 0.79, 0.86, 0.89, 0.94, 0.96, 0.97,
0.97, 0.98, 0.97, 0.98, 0.98, 0.98, 0.98, 0.98,//
0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00,
0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00, 0.00,//
0.54, 0.71, 0.84, 0.88, 0.92, 0.93, 0.94, 0.95,
0.96, 0.96, 0.96, 0.96, 0.96, 0.96, 0.96, 0.96,//
0.61, 0.74, 0.83, 0.88, 0.91, 0.94, 0.95, 0.96,
0.97, 0.98, 0.98, 0.98, 0.98, 0.98, 0.98, 0.98};
const int i_eta = binIndex(y.abseta(), edges_eta);
const int i_pt = binIndex(y.pT()/GeV, edges_pt, true);
const int i = i_eta*edges_pt.size() + i_pt;
const double eff = effs[i];
return eff;
}
/// CMS Run 1 photon reco efficiency
/// @todo Currently from Delphes
inline double PHOTON_EFF_CMS_RUN1(const Particle& y) {
if (y.pT() < 10*GeV || y.abseta() > 2.5) return 0;
return (y.abseta() < 1.5) ? 0.95 : 0.85;
}
/// CMS Run 2 photon reco efficiency
/// @todo Currently just a copy of Run 1: fix!
inline double PHOTON_EFF_CMS_RUN2(const Particle& y) {
return PHOTON_EFF_CMS_RUN1(y);
}
/// @todo Use real photon smearing
inline Particle PHOTON_SMEAR_ATLAS_RUN1(const Particle& y) { return y; }
inline Particle PHOTON_SMEAR_ATLAS_RUN2(const Particle& y) { return y; }
inline Particle PHOTON_SMEAR_CMS_RUN1(const Particle& y) { return y; }
inline Particle PHOTON_SMEAR_CMS_RUN2(const Particle& y) { return y; }
//@}
/// @name Muon efficiency and smearing functions
//@{
/// ATLAS Run 1 muon reco efficiency
inline double MUON_EFF_ATLAS_RUN1(const Particle& m) {
if (m.abseta() > 2.7) return 0;
if (m.pT() < 10*GeV) return 0;
return (m.abseta() < 1.5) ? 0.95 : 0.85;
}
/// @brief ATLAS Run 2 muon reco efficiency
///
/// For medium ID, from Fig 3 of
/// https://cds.cern.ch/record/2047831/files/ATL-PHYS-PUB-2015-037.pdf
inline double MUON_EFF_ATLAS_RUN2(const Particle& m) {
if (m.abseta() > 2.7) return 0;
static const vector<double> edges_pt = {0., 3.5, 4., 5., 6., 7., 8., 10.};
static const vector<double> effs = {0.00, 0.76, 0.94, 0.97, 0.98, 0.98, 0.98, 0.99};
const int i_pt = binIndex(m.pT()/GeV, edges_pt, true);
const double eff = effs[i_pt];
return eff;
}
/// ATLAS Run 1 muon reco smearing
inline Particle MUON_SMEAR_ATLAS_RUN1(const Particle& m) {
static const vector<double> edges_eta = {0, 1.5, 2.5};
static const vector<double> edges_pt = {0, 0.1, 1.0, 10., 200.};
static const vector<double> res = {0., 0.03, 0.02, 0.03, 0.05,
0., 0.04, 0.03, 0.04, 0.05};
const int i_eta = binIndex(m.abseta(), edges_eta);
const int i_pt = binIndex(m.pT()/GeV, edges_pt, true);
const int i = i_eta*edges_pt.size() + i_pt;
const double resolution = res[i];
// Smear by a Gaussian centered on the current pT, with width given by the resolution
// normal_distribution<> d(m.pT(), resolution*m.pT());
// const double smeared_pt = max(d(gen), 0.);
// const double mass = m.mass2() > 0 ? m.mass() : 0; //< numerical carefulness...
// return Particle(m.pid(), FourMomentum::mkEtaPhiMPt(m.eta(), m.phi(), mass, smeared_pt));
return Particle(m.pid(), P4_SMEAR_PT_GAUSS(m, resolution*m.pT()));
}
/// ATLAS Run 2 muon reco smearing
/// @todo Currently just a copy of the Run 1 version: fix!
inline Particle MUON_SMEAR_ATLAS_RUN2(const Particle& m) {
return MUON_SMEAR_ATLAS_RUN1(m);
}
/// CMS Run 1 muon reco efficiency
inline double MUON_EFF_CMS_RUN1(const Particle& m) {
if (m.abseta() > 2.4) return 0;
if (m.pT() < 10*GeV) return 0;
return 0.95 * (m.abseta() < 1.5 ? 1 : exp(0.5 - 5e-4*m.pT()/GeV));
}
/// CMS Run 2 muon reco efficiency
/// @todo Currently just a copy of Run 1: fix!
inline double MUON_EFF_CMS_RUN2(const Particle& m) {
return MUON_EFF_CMS_RUN1(m);
}
/// CMS Run 1 muon reco smearing
inline Particle MUON_SMEAR_CMS_RUN1(const Particle& m) {
// Calculate fractional resolution
// for pT > 0.1 GeV, mom resolution = |eta| < 0.5 -> sqrt(0.01^2 + pt^2 * 2.0e-4^2)
// |eta| < 1.5 -> sqrt(0.02^2 + pt^2 * 3.0e-4^2)
// |eta| < 2.5 -> sqrt(0.05^2 + pt^2 * 2.6e-4^2)
double resolution = 0;
const double abseta = m.abseta();
if (m.pT() > 0.1*GeV && abseta < 2.5) {
if (abseta < 0.5) {
resolution = add_quad(0.01, 2.0e-4 * m.pT()/GeV);
} else if (abseta < 1.5) {
resolution = add_quad(0.02, 3.0e-4 * m.pT()/GeV);
} else { // still |eta| < 2.5... but isn't CMS' mu acceptance < 2.4?
resolution = add_quad(0.05, 2.6e-4 * m.pT()/GeV);
}
}
// Smear by a Gaussian centered on the current pT, with width given by the resolution
// normal_distribution<> d(m.pT(), resolution*m.pT());
// const double smeared_pt = max(d(gen), 0.);
// const double mass = m.mass2() > 0 ? m.mass() : 0; //< numerical carefulness...
// return Particle(m.pid(), FourMomentum::mkEtaPhiMPt(m.eta(), m.phi(), mass, smeared_pt));
return Particle(m.pid(), P4_SMEAR_PT_GAUSS(m, resolution*m.pT()));
}
/// CMS Run 2 muon reco smearing
/// @todo Currently just a copy of the Run 1 version: fix!
inline Particle MUON_SMEAR_CMS_RUN2(const Particle& m) {
return MUON_SMEAR_CMS_RUN1(m);
}
//@}
/// @name Tau efficiency and smearing functions
//@{
/// @brief ATLAS Run 1 8 TeV tau efficiencies (medium working point)
///
/// Taken from http://arxiv.org/pdf/1412.7086.pdf
/// 20-40 GeV 1-prong LMT eff|mis = 0.66|1/10, 0.56|1/20, 0.36|1/80
/// 20-40 GeV 3-prong LMT eff|mis = 0.45|1/60, 0.38|1/100, 0.27|1/300
/// > 40 GeV 1-prong LMT eff|mis = 0.66|1/15, 0.56|1/25, 0.36|1/80
/// > 40 GeV 3-prong LMT eff|mis = 0.45|1/250, 0.38|1/400, 0.27|1/1300
inline double TAU_EFF_ATLAS_RUN1(const Particle& t) {
if (t.abseta() > 2.5) return 0; //< hmm... mostly
double pThadvis = 0;
Particles chargedhadrons;
for (const Particle& p : t.children()) {
if (p.isHadron()) {
pThadvis += p.pT(); //< right definition? Paper is unclear
if (p.charge3() != 0 && p.abseta() < 2.5 && p.pT() > 1*GeV) chargedhadrons += p;
}
}
if (chargedhadrons.empty()) return 0; //< leptonic tau
if (pThadvis < 20*GeV) return 0; //< below threshold
if (pThadvis < 40*GeV) {
if (chargedhadrons.size() == 1) return (t.abspid() == PID::TAU) ? 0.56 : 1/20.;
if (chargedhadrons.size() == 3) return (t.abspid() == PID::TAU) ? 0.38 : 1/100.;
} else {
if (chargedhadrons.size() == 1) return (t.abspid() == PID::TAU) ? 0.56 : 1/25.;
if (chargedhadrons.size() == 3) return (t.abspid() == PID::TAU) ? 0.38 : 1/400.;
}
return 0;
}
/// @brief ATLAS Run 2 13 TeV tau efficiencies (medium working point)
///
/// From https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PUBNOTES/ATL-PHYS-PUB-2015-045/ATL-PHYS-PUB-2015-045.pdf
/// LMT 1 prong efficiency/mistag = 0.6|1/30, 0.55|1/50, 0.45|1/120
/// LMT 3 prong efficiency/mistag = 0.5|1/30, 0.4|1/110, 0.3|1/300
inline double TAU_EFF_ATLAS_RUN2(const Particle& t) {
if (t.abseta() > 2.5) return 0; //< hmm... mostly
double pThadvis = 0;
Particles chargedhadrons;
for (const Particle& p : t.children()) {
if (p.isHadron()) {
pThadvis += p.pT(); //< right definition? Paper is unclear
if (p.charge3() != 0 && p.abseta() < 2.5 && p.pT() > 1*GeV) chargedhadrons += p;
}
}
if (chargedhadrons.empty()) return 0; //< leptonic tau
if (pThadvis < 20*GeV) return 0; //< below threshold
if (chargedhadrons.size() == 1) return (t.abspid() == PID::TAU) ? 0.55 : 1/50.;
if (chargedhadrons.size() == 3) return (t.abspid() == PID::TAU) ? 0.40 : 1/110.;
return 0;
}
/// ATLAS Run 1 tau smearing
/// @todo Currently a copy of the crappy jet smearing that is probably wrong...
inline Particle TAU_SMEAR_ATLAS_RUN1(const Particle& t) {
// Const fractional resolution for now
static const double resolution = 0.03;
// Smear by a Gaussian centered on 1 with width given by the (fractional) resolution
/// @todo Is this the best way to smear? Should we preserve the energy, or pT, or direction?
const double fsmear = max(randnorm(1., resolution), 0.);
const double mass = t.mass2() > 0 ? t.mass() : 0; //< numerical carefulness...
return Particle(t.pid(), FourMomentum::mkXYZM(t.px()*fsmear, t.py()*fsmear, t.pz()*fsmear, mass));
}
/// ATLAS Run 2 tau smearing
/// @todo Currently a copy of the Run 1 version
inline Particle TAU_SMEAR_ATLAS_RUN2(const Particle& t) {
return TAU_SMEAR_ATLAS_RUN1(t);
}
/// CMS Run 2 tau efficiency
///
/// @todo Needs work; this is the dumb version from Delphes 3.3.2
inline double TAU_EFF_CMS_RUN2(const Particle& t) {
return (t.abspid() == PID::TAU) ? 0.6 : 0;
}
/// CMS Run 1 tau efficiency
///
/// @todo Needs work; this is just a copy of the Run 2 version in Delphes 3.3.2
inline double TAU_EFF_CMS_RUN1(const Particle& t) {
return TAU_EFF_CMS_RUN2(t);
}
/// CMS Run 1 tau smearing
/// @todo Currently a copy of the crappy ATLAS one
inline Particle TAU_SMEAR_CMS_RUN1(const Particle& t) {
return TAU_SMEAR_ATLAS_RUN1(t);
}
/// CMS Run 2 tau smearing
/// @todo Currently a copy of the Run 1 version
inline Particle TAU_SMEAR_CMS_RUN2(const Particle& t) {
return TAU_SMEAR_CMS_RUN1(t);
}
//@}
/// @name Jet efficiency and smearing functions
//@{
/// Return the ATLAS Run 1 jet flavour tagging efficiency for the given Jet
inline double JET_BTAG_ATLAS_RUN1(const Jet& j) {
/// @todo This form drops past ~100 GeV, asymptotically to zero efficiency... really?!
if (j.abseta() > 2.5) return 0;
const auto ftagsel = [&](const Particle& p){ return p.pT() > 5*GeV && deltaR(p,j) < 0.3; };
if (j.bTagged(ftagsel)) return 0.80*tanh(0.003*j.pT()/GeV)*(30/(1+0.0860*j.pT()/GeV));
if (j.cTagged(ftagsel)) return 0.20*tanh(0.020*j.pT()/GeV)*( 1/(1+0.0034*j.pT()/GeV));
return 0.002 + 7.3e-6*j.pT()/GeV;
}
/// Return the ATLAS Run 2 MC2c20 jet flavour tagging efficiency for the given Jet
inline double JET_BTAG_ATLAS_RUN2_MV2C20(const Jet& j) {
if (j.abseta() > 2.5) return 0;
if (j.bTagged(Cuts::pT > 5*GeV)) return 0.77;
if (j.cTagged(Cuts::pT > 5*GeV)) return 1/4.5;
return 1/140.;
}
/// Return the ATLAS Run 2 MC2c10 jet flavour tagging efficiency for the given Jet
inline double JET_BTAG_ATLAS_RUN2_MV2C10(const Jet& j) {
if (j.abseta() > 2.5) return 0;
if (j.bTagged(Cuts::pT > 5*GeV)) return 0.77;
if (j.cTagged(Cuts::pT > 5*GeV)) return 1/6.0;
return 1/134.;
}
/// ATLAS Run 1 jet smearing
inline Jet JET_SMEAR_ATLAS_RUN1(const Jet& j) {
// Jet energy resolution lookup
// Implemented by Matthias Danninger for GAMBIT, based roughly on
// https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2015-017/
// Parameterisation can be still improved, but eta dependence is minimal
/// @todo Also need a JES uncertainty component?
static const vector<double> binedges_pt = {0., 50., 70., 100., 150., 200., 1000., 10000.};
static const vector<double> jer = {0.145, 0.115, 0.095, 0.075, 0.07, 0.05, 0.04, 0.04}; //< note overflow value
const int ipt = binIndex(j.pT()/GeV, binedges_pt, true);
if (ipt < 0) return j;
const double resolution = jer.at(ipt);
// Smear by a Gaussian centered on 1 with width given by the (fractional) resolution
/// @todo Is this the best way to smear? Should we preserve the energy, or pT, or direction?
const double fsmear = max(randnorm(1., resolution), 0.);
const double mass = j.mass2() > 0 ? j.mass() : 0; //< numerical carefulness...
Jet rtn(FourMomentum::mkXYZM(j.px()*fsmear, j.py()*fsmear, j.pz()*fsmear, mass));
//if (deltaPhi(j, rtn) > 0.01) cout << "jdphi: " << deltaPhi(j, rtn) << endl;
return rtn;
}
/// ATLAS Run 2 jet smearing
/// @todo Just a copy of the Run 1 one: improve!!
inline Jet JET_SMEAR_ATLAS_RUN2(const Jet& j) {
return JET_SMEAR_ATLAS_RUN1(j);
}
/// CMS Run 2 jet smearing
/// @todo Just a copy of the suboptimal ATLAS one: improve!!
inline Jet JET_SMEAR_CMS_RUN2(const Jet& j) {
return JET_SMEAR_ATLAS_RUN1(j);
}
//@}
/// @name ETmiss smearing functions
//@{
inline Vector3 MET_SMEAR_IDENTITY(const Vector3& met, double) { return met; }
/// @brief ATLAS Run 1 ETmiss smearing
///
/// Based on https://arxiv.org/pdf/1108.5602v2.pdf, Figs 14 and 15
inline Vector3 MET_SMEAR_ATLAS_RUN1(const Vector3& met, double set) {
+ Vector3 smeared_met = met;
+
// Linearity offset (Fig 14)
- Vector3 smeared_met = met;
- if (met.mod()/GeV < 25*GeV) smeared_met *= 1.05;
- else if (met.mod()/GeV < 40*GeV) smeared_met *= (1.05 - (0.04/15)*(met.mod()/GeV - 25)); //< linear decrease
+ if (met.mod() < 25*GeV) smeared_met *= 1.05;
+ else if (met.mod() < 40*GeV) smeared_met *= (1.05 - (0.04/15)*(met.mod()/GeV - 25)); //< linear decrease
else smeared_met *= 1.01;
// Smear by a Gaussian with width given by the resolution(sumEt) ~ 0.45 sqrt(sumEt) GeV
const double resolution = 0.45 * sqrt(set/GeV) * GeV;
const double metsmear = max(randnorm(smeared_met.mod(), resolution), 0.);
smeared_met = metsmear * smeared_met.unit();
return smeared_met;
}
/// ATLAS Run 2 ETmiss smearing
/// @todo Just a copy of the Run 1 one: improve!!
inline Vector3 MET_SMEAR_ATLAS_RUN2(const Vector3& met, double set) {
return MET_SMEAR_ATLAS_RUN1(met, set);
}
/// CMS Run 1 ETmiss smearing
- /// @todo Just a copy of the ATLAS one: improve!!
+ /// From https://arxiv.org/pdf/1411.0511.pdf Table 2, p16 (Z channels)
inline Vector3 MET_SMEAR_CMS_RUN1(const Vector3& met, double set) {
- return MET_SMEAR_ATLAS_RUN1(met, set);
+ Vector3 smeared_met = met;
+
+ // Calculate parallel and perpendicular resolutions and combine in quadrature (?)
+ const double resolution_x = (1.1 + 0.6*sqrt(set/GeV)) * GeV;
+ const double resolution_y = (1.4 + 0.6*sqrt(set/GeV)) * GeV;
+ const double resolution = sqrt(sqr(resolution_x) + sqr(resolution_y));
+
+ // Smear by a Gaussian with width given by the resolution
+ const double metsmear = max(randnorm(smeared_met.mod(), resolution), 0.);
+ smeared_met = metsmear * smeared_met.unit();
+
+ return smeared_met;
}
/// CMS Run 2 ETmiss smearing
- /// @todo Just a copy of the ATLAS one: improve!!
+ /// From http://inspirehep.net/record/1681214/files/JME-17-001-pas.pdf Table 3, p20
inline Vector3 MET_SMEAR_CMS_RUN2(const Vector3& met, double set) {
- return MET_SMEAR_ATLAS_RUN2(met, set);
+ Vector3 smeared_met = met;
+
+ // Calculate parallel and perpendicular resolutions and combine in quadrature (?)
+ const double resolution_para = ( 2.0 + 0.64*sqrt(set/GeV)) * GeV;
+ const double resolution_perp = (-1.5 + 0.68*sqrt(set/GeV)) * GeV;
+ const double resolution = sqrt(sqr(resolution_para) + sqr(resolution_perp));
+
+ // Smear by a Gaussian with width given by the resolution
+ const double metsmear = max(randnorm(smeared_met.mod(), resolution), 0.);
+ smeared_met = metsmear * smeared_met.unit();
+
+ return smeared_met;
}
//@}
/// @name Tracking efficiency and smearing functions
//@{
/// ATLAS Run 1 tracking efficiency
inline double TRK_EFF_ATLAS_RUN1(const Particle& p) {
if (p.charge3() == 0) return 0;
if (p.abseta() > 2.5) return 0;
if (p.pT() < 0.1*GeV) return 0;
if (p.abspid() == PID::ELECTRON) {
if (p.abseta() < 1.5) {
if (p.pT() < 1*GeV) return 0.73;
if (p.pT() < 100*GeV) return 0.95;
return 0.99;
} else {
if (p.pT() < 1*GeV) return 0.50;
if (p.pT() < 100*GeV) return 0.83;
else return 0.90;
}
} else if (p.abspid() == PID::MUON) {
if (p.abseta() < 1.5) {
return (p.pT() < 1*GeV) ? 0.75 : 0.99;
} else {
return (p.pT() < 1*GeV) ? 0.70 : 0.98;
}
} else { // charged hadrons
if (p.abseta() < 1.5) {
return (p.pT() < 1*GeV) ? 0.70 : 0.95;
} else {
return (p.pT() < 1*GeV) ? 0.60 : 0.85;
}
}
}
/// ATLAS Run 2 tracking efficiency
/// @todo Currently just a copy of Run 1: fix!
inline double TRK_EFF_ATLAS_RUN2(const Particle& p) {
return TRK_EFF_ATLAS_RUN1(p);
}
/// CMS Run 1 tracking efficiency
inline double TRK_EFF_CMS_RUN1(const Particle& p) {
if (p.charge3() == 0) return 0;
if (p.abseta() > 2.5) return 0;
if (p.pT() < 0.1*GeV) return 0;
if (p.abspid() == PID::ELECTRON) {
if (p.abseta() < 1.5) {
if (p.pT() < 1*GeV) return 0.73;
if (p.pT() < 100*GeV) return 0.95;
return 0.99;
} else {
if (p.pT() < 1*GeV) return 0.50;
if (p.pT() < 100*GeV) return 0.83;
else return 0.90;
}
} else if (p.abspid() == PID::MUON) {
if (p.abseta() < 1.5) {
return (p.pT() < 1*GeV) ? 0.75 : 0.99;
} else {
return (p.pT() < 1*GeV) ? 0.70 : 0.98;
}
} else { // charged hadrons
if (p.abseta() < 1.5) {
return (p.pT() < 1*GeV) ? 0.70 : 0.95;
} else {
return (p.pT() < 1*GeV) ? 0.60 : 0.85;
}
}
}
/// CMS Run 2 tracking efficiency
/// @todo Currently just a copy of Run 1: fix!
inline double TRK_EFF_CMS_RUN2(const Particle& p) {
return TRK_EFF_CMS_RUN1(p);
}
//@}
}
#endif
diff --git a/include/Rivet/Tools/fjcontrib/AxesDefinition.hh b/include/Rivet/Tools/fjcontrib/AxesDefinition.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/AxesDefinition.hh
@@ -0,0 +1,1283 @@
+// Nsubjettiness Package
+// Questions/Comments? jthaler@jthaler.net
+//
+// Copyright (c) 2011-14
+// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
+//
+// $Id: AxesDefinition.hh 833 2015-07-23 14:35:23Z jthaler $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_AXES_DEFINITION_HH__
+#define __FASTJET_CONTRIB_AXES_DEFINITION_HH__
+
+
+#include "MeasureDefinition.hh"
+#include "ExtraRecombiners.hh"
+
+#include "fastjet/PseudoJet.hh"
+#include <fastjet/LimitedWarning.hh>
+
+#include <iomanip>
+#include <cmath>
+#include <vector>
+#include <list>
+
+namespace Rivet {
+namespace fjcontrib {
+
+namespace Nsubjettiness { using namespace fastjet;
+
+// The following AxesDefinitions are currently available (and the relevant arguments, if needed)
+class KT_Axes;
+class CA_Axes;
+class AntiKT_Axes; // (R0)
+class WTA_KT_Axes;
+class WTA_CA_Axes;
+class GenKT_Axes; // (p, R0 = infinity)
+class WTA_GenKT_Axes; // (p, R0 = infinity)
+class GenET_GenKT_Axes; // (delta, p, R0 = infinity)
+class Manual_Axes;
+
+class OnePass_KT_Axes;
+class OnePass_CA_Axes;
+class OnePass_AntiKT_Axes; // (R0)
+class OnePass_WTA_KT_Axes;
+class OnePass_WTA_CA_Axes;
+class OnePass_GenKT_Axes; // (p, R0 = infinity)
+class OnePass_WTA_GenKT_Axes; // (p, R0 = infinity)
+class OnePass_GenET_GenKT_Axes; // (delta, p, R0 = infinity)
+class OnePass_Manual_Axes;
+
+class MultiPass_Axes; // (NPass) (currently only defined for KT_Axes)
+class MultiPass_Manual_Axes; // (NPass)
+
+class Comb_GenKT_Axes; // (nExtra, p, R0 = infinity)
+class Comb_WTA_GenKT_Axes; // (nExtra, p, R0 = infinity)
+class Comb_GenET_GenKT_Axes; // (nExtra, delta, p, R0 = infinity)
+
+///////
+//
+// AxesDefinition
+//
+///////
+
+///------------------------------------------------------------------------
+/// \class AxesDefinition
+/// \brief Base class for axes definitions
+///
+/// A generic AxesDefinition first finds a set of seed axes.
+/// Then, if desired, uses measure information
+/// (from MeasureDefinition) to refine those axes starting from those seed axes.
+/// The AxesDefinitions are typically based on sequential jet algorithms.
+///------------------------------------------------------------------------
+class AxesDefinition {
+
+public:
+
+ /// This function should be overloaded in all derived classes, and defines how to find the seed axes.
+ /// If desired, the measure information (which might be NULL) can be used to test multiple axes choices, but should
+ /// not be used for iterative refining (since that is the job of MeasureDefinition).
+ virtual std::vector<fastjet::PseudoJet> get_starting_axes(int n_jets,
+ const std::vector<fastjet::PseudoJet>& inputs,
+ const MeasureDefinition * measure) const = 0;
+
+ /// Short description of AxesDefinitions (and any parameters)
+ virtual std::string short_description() const = 0;
+
+ /// Long description of AxesDefinitions (and any parameters)
+ virtual std::string description() const = 0;
+
+ /// This has to be defined in all derived classes, and allows these to be copied around.
+ virtual AxesDefinition* create() const = 0;
+
+public:
+
+ /// Starting from seeds, refine axes using one or more passes.
+ /// Note that in order to do >0 passes, we need information from the MeasureDefinition about how to do the appropriate minimization.
+ std::vector<fastjet::PseudoJet> get_refined_axes(int n_jets,
+ const std::vector<fastjet::PseudoJet>& inputs,
+ const std::vector<fastjet::PseudoJet>& seedAxes,
+ const MeasureDefinition * measure = NULL) const {
+
+ assert(n_jets == (int)seedAxes.size()); //added int casting to get rid of compiler warning
+
+ if (_Npass == 0) {
+ // no refining, just use seeds
+ return seedAxes;
+ } else if (_Npass == 1) {
+ if (measure == NULL) throw Error("AxesDefinition: One-pass minimization requires specifying a MeasureDefinition.");
+
+ // do one pass minimum using measure definition
+ return measure->get_one_pass_axes(n_jets, inputs, seedAxes,_nAttempts,_accuracy);
+ } else {
+ if (measure == NULL) throw Error("AxesDefinition: Multi-pass minimization requires specifying a MeasureDefinition.");
+ return get_multi_pass_axes(n_jets, inputs, seedAxes, measure);
+ }
+ }
+
+ /// Combines get_starting_axes with get_refined_axes.
+ /// In the Njettiness class, these two steps are done separately in order to store seed axes information.
+ std::vector<fastjet::PseudoJet> get_axes(int n_jets,
+ const std::vector<fastjet::PseudoJet>& inputs,
+ const MeasureDefinition * measure = NULL) const {
+ std::vector<fastjet::PseudoJet> seedAxes = get_starting_axes(n_jets, inputs, measure);
+ return get_refined_axes(n_jets,inputs,seedAxes,measure);
+ }
+
+
+ /// Short-hand for the get_axes function. Useful when trying to write terse code.
+ inline std::vector<fastjet::PseudoJet> operator() (int n_jets,
+ const std::vector<fastjet::PseudoJet>& inputs,
+ const MeasureDefinition * measure = NULL) const {
+ return get_axes(n_jets,inputs,measure);
+ }
+
+ /// \enum AxesRefiningEnum
+ /// Defines the cases of zero pass and one pass for convenience
+ enum AxesRefiningEnum {
+ UNDEFINED_REFINE = -1, // added to create a default value
+ NO_REFINING = 0,
+ ONE_PASS = 1,
+ MULTI_PASS = 100,
+ };
+
+ /// A integer that is used externally to decide how to do multi-pass minimization
+ int nPass() const { return _Npass; }
+
+ /// A flag that indicates whether results are deterministics.
+ bool givesRandomizedResults() const {
+ return (_Npass > 1);
+ }
+
+ /// A flag that indicates whether manual axes are being used.
+ bool needsManualAxes() const {
+ return _needsManualAxes; // if there is no starting axes finder
+ }
+
+ /// Allows user to change number of passes. Also used internally to set nPass.
+ /// Can also specify details of one/multi pass minimziation
+ void setNPass(int nPass,
+ int nAttempts = 1000,
+ double accuracy = 0.0001,
+ double noise_range = 1.0 // only needed for MultiPass minimization
+ )
+ {
+ _Npass = nPass;
+ _nAttempts = nAttempts;
+ _accuracy = accuracy;
+ _noise_range = noise_range;
+ if (nPass < 0) throw Error("AxesDefinition requires a nPass >= 0");
+ }
+
+ /// Destructor
+ virtual ~AxesDefinition() {};
+
+protected:
+
+ /// Default constructor contains no information. Number of passes has to be set
+ /// manually by derived classes using setNPass function.
+ AxesDefinition() : _Npass(UNDEFINED_REFINE),
+ _nAttempts(0),
+ _accuracy(0.0),
+ _noise_range(0.0),
+ _needsManualAxes(false) {}
+
+ /// Does multi-pass minimization by randomly jiggling the axes within _noise_range
+ std::vector<fastjet::PseudoJet> get_multi_pass_axes(int n_jets,
+ const std::vector<fastjet::PseudoJet>& inputs,
+ const std::vector<fastjet::PseudoJet>& seedAxes,
+ const MeasureDefinition* measure) const;
+
+ /// Function to jiggle axes within _noise_range
+ PseudoJet jiggle(const PseudoJet& axis) const;
+
+ int _Npass; ///< Number of passes (0 = no refining, 1 = one-pass, >1 multi-pass)
+ int _nAttempts; ///< Number of attempts per pass
+ double _accuracy; ///< Accuracy goal per pass
+ double _noise_range; ///< Noise in rapidity/phi (for multi-pass minimization only)
+ bool _needsManualAxes; ///< Flag to indicate special case of manual axes
+};
+
+///------------------------------------------------------------------------
+/// \class ExclusiveJetAxes
+/// \brief Base class for axes defined from exclusive jet algorithm
+///
+/// This class finds axes by clustering particles with an exclusive jet definition.
+/// This can be implemented with different jet algorithms. The user can call this directly
+/// using their favorite fastjet::JetDefinition
+///------------------------------------------------------------------------
+class ExclusiveJetAxes : public AxesDefinition {
+
+public:
+ /// Constructor takes JetDefinition as an argument
+ ExclusiveJetAxes(fastjet::JetDefinition def)
+ : AxesDefinition(), _def(def) {
+ setNPass(NO_REFINING); // default to no minimization
+ }
+
+ /// Starting axes obtained by creating a cluster sequenence and running exclusive_jets.
+ virtual std::vector<fastjet::PseudoJet> get_starting_axes(int n_jets,
+ const std::vector <fastjet::PseudoJet> & inputs,
+ const MeasureDefinition * ) const {
+ fastjet::ClusterSequence jet_clust_seq(inputs, _def);
+
+ std::vector<fastjet::PseudoJet> axes = jet_clust_seq.exclusive_jets_up_to(n_jets);
+
+ if ((int)axes.size() < n_jets) {
+ _too_few_axes_warning.warn("ExclusiveJetAxes::get_starting_axes: Fewer than N axes found; results are unpredictable.");
+ axes.resize(n_jets); // resize to make sure there are enough axes to not yield an error elsewhere
+ }
+
+ return axes;
+ }
+
+ /// Short description
+ virtual std::string short_description() const { return "ExclAxes";}
+ /// Long description
+ virtual std::string description() const { return "ExclAxes: " + _def.description();}
+
+ /// To make it possible to copy around.
+ virtual ExclusiveJetAxes* create() const {return new ExclusiveJetAxes(*this);}
+
+private:
+ fastjet::JetDefinition _def; ///< Jet definition to use.
+ static LimitedWarning _too_few_axes_warning;
+};
+
+///------------------------------------------------------------------------
+/// \class ExclusiveCombinatorialJetAxes
+/// \brief Base class for axes defined from exclusive jet algorithm, checking combinatorial options
+///
+/// This class finds axes by clustering particles with an exclusive jet definition.
+/// It takes an extra number of jets (specificed by the user via nExtra), and then finds the set of N that minimizes N-jettiness.
+/// WARNING: If one wants to be guarenteed that results improve by increasing nExtra, then one should use
+/// winner-take-all-style recombination schemes
+///------------------------------------------------------------------------
+class ExclusiveCombinatorialJetAxes : public AxesDefinition {
+
+public:
+ /// Constructor takes JetDefinition and nExtra as options (nExtra=0 acts the same as ExclusiveJetAxes)
+ ExclusiveCombinatorialJetAxes(fastjet::JetDefinition def, int nExtra = 0)
+ : AxesDefinition(), _def(def), _nExtra(nExtra) {
+ if (nExtra < 0) throw Error("Need nExtra >= 0");
+ setNPass(NO_REFINING); // default to no minimization
+ }
+
+ /// Find n_jets + _nExtra axes, and then choose the n_jets subset with the smallest N-(sub)jettiness value.
+ virtual std::vector<fastjet::PseudoJet> get_starting_axes(int n_jets,
+ const std::vector<fastjet::PseudoJet> & inputs,
+ const MeasureDefinition *measure) const {
+ int starting_number = n_jets + _nExtra;
+ fastjet::ClusterSequence jet_clust_seq(inputs, _def);
+ std::vector<fastjet::PseudoJet> starting_axes = jet_clust_seq.exclusive_jets_up_to(starting_number);
+
+ if ((int)starting_axes.size() < n_jets) {
+ _too_few_axes_warning.warn("ExclusiveCombinatorialJetAxes::get_starting_axes: Fewer than N + nExtra axes found; results are unpredictable.");
+ starting_axes.resize(n_jets); // resize to make sure there are enough axes to not yield an error elsewhere
+ }
+
+ std::vector<fastjet::PseudoJet> final_axes;
+
+ // check so that no computation time is wasted if there are no extra axes
+ if (_nExtra == 0) final_axes = starting_axes;
+
+ else {
+
+ // define string of 1's based on number of desired jets
+ std::string bitmask(n_jets, 1);
+ // expand the array size to the total number of jets with extra 0's at the end, makes string easy to permute
+ bitmask.resize(starting_number, 0);
+
+ double min_tau = std::numeric_limits<double>::max();
+ std::vector<fastjet::PseudoJet> temp_axes;
+
+ do {
+
+ temp_axes.clear();
+
+ // only take an axis if it is listed as true (1) in the string
+ for (int i = 0; i < (int)starting_axes.size(); ++i) {
+ if (bitmask[i]) temp_axes.push_back(starting_axes[i]);
+ }
+
+ double temp_tau = measure->result(inputs, temp_axes);
+ if (temp_tau < min_tau) {
+ min_tau = temp_tau;
+ final_axes = temp_axes;
+ }
+
+ // permutes string of 1's and 0's according to next lexicographic ordering and returns true
+ // continues to loop through all possible lexicographic orderings
+ // returns false and breaks the loop when there are no more possible orderings
+ } while (std::prev_permutation(bitmask.begin(), bitmask.end()));
+ }
+
+ return final_axes;
+ }
+
+ /// Short description
+ virtual std::string short_description() const { return "ExclCombAxes";}
+ /// Long description
+ virtual std::string description() const { return "ExclCombAxes: " + _def.description();}
+ /// To make it possible to copy around.
+ virtual ExclusiveCombinatorialJetAxes* create() const {return new ExclusiveCombinatorialJetAxes(*this);}
+
+private:
+ fastjet::JetDefinition _def; ///< Jet definition to use
+ int _nExtra; ///< Extra axes to find
+ static LimitedWarning _too_few_axes_warning;
+};
+
+///------------------------------------------------------------------------
+/// \class HardestJetAxes
+/// \brief Base class for axes defined from an inclusive jet algorithm
+///
+/// This class finds axes by running an inclusive algorithm and then finding the n hardest jets.
+/// This can be implemented with different jet algorithms, and can be called by the user.
+///------------------------------------------------------------------------
+class HardestJetAxes : public AxesDefinition {
+public:
+ /// Constructor takes JetDefinition
+ HardestJetAxes(fastjet::JetDefinition def)
+ : AxesDefinition(), _def(def) {
+ setNPass(NO_REFINING); // default to no minimization
+ }
+
+ /// Finds seed axes by running a ClusterSequence, running inclusive_jets, and finding the N hardest
+ virtual std::vector<fastjet::PseudoJet> get_starting_axes(int n_jets,
+ const std::vector <fastjet::PseudoJet> & inputs,
+ const MeasureDefinition * ) const {
+ fastjet::ClusterSequence jet_clust_seq(inputs, _def);
+ std::vector<fastjet::PseudoJet> axes = sorted_by_pt(jet_clust_seq.inclusive_jets());
+
+ if ((int)axes.size() < n_jets) {
+ _too_few_axes_warning.warn("HardestJetAxes::get_starting_axes: Fewer than N axes found; results are unpredictable.");
+ }
+
+ axes.resize(n_jets); // only keep n hardest
+ return axes;
+ }
+
+ /// Short description
+ virtual std::string short_description() const { return "HardAxes";}
+ /// Long description
+ virtual std::string description() const { return "HardAxes: " + _def.description();}
+ /// To make it possible to copy around.
+ virtual HardestJetAxes* create() const {return new HardestJetAxes(*this);}
+
+private:
+ fastjet::JetDefinition _def; ///< Jet Definition to use.
+
+ static LimitedWarning _too_few_axes_warning;
+
+};
+
+///------------------------------------------------------------------------
+/// \class KT_Axes
+/// \brief Axes from exclusive kT
+///
+/// Axes from kT algorithm with E_scheme recombination.
+///------------------------------------------------------------------------
+class KT_Axes : public ExclusiveJetAxes {
+public:
+ /// Constructor
+ KT_Axes()
+ : ExclusiveJetAxes(fastjet::JetDefinition(fastjet::kt_algorithm,
+ fastjet::JetDefinition::max_allowable_R, //maximum jet radius constant
+ fastjet::E_scheme,
+ fastjet::Best)
+ ) {
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "KT";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "KT Axes";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual KT_Axes* create() const {return new KT_Axes(*this);}
+
+};
+
+///------------------------------------------------------------------------
+/// \class CA_Axes
+/// \brief Axes from exclusive CA
+///
+/// Axes from CA algorithm with E_scheme recombination.
+///------------------------------------------------------------------------
+class CA_Axes : public ExclusiveJetAxes {
+public:
+ /// Constructor
+ CA_Axes()
+ : ExclusiveJetAxes(fastjet::JetDefinition(fastjet::cambridge_algorithm,
+ fastjet::JetDefinition::max_allowable_R, //maximum jet radius constant
+ fastjet::E_scheme,
+ fastjet::Best)
+ ) {
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "CA";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "CA Axes";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual CA_Axes* create() const {return new CA_Axes(*this);}
+
+};
+
+
+///------------------------------------------------------------------------
+/// \class AntiKT_Axes
+/// \brief Axes from inclusive anti-kT
+///
+/// Axes from anti-kT algorithm and E_scheme.
+/// The one parameter R0 is subjet radius
+///------------------------------------------------------------------------
+class AntiKT_Axes : public HardestJetAxes {
+
+public:
+ /// Constructor. Takes jet radius as argument
+ AntiKT_Axes(double R0)
+ : HardestJetAxes(fastjet::JetDefinition(fastjet::antikt_algorithm,
+ R0,
+ fastjet::E_scheme,
+ fastjet::Best)
+ ), _R0(R0) {
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "AKT" << _R0;
+ return stream.str();
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "Anti-KT Axes (R0 = " << _R0 << ")";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual AntiKT_Axes* create() const {return new AntiKT_Axes(*this);}
+
+protected:
+ double _R0; ///< AKT jet radius
+
+};
+
+///------------------------------------------------------------------------
+/// \class JetDefinitionWrapper
+/// \brief Wrapper for jet definitions (for memory management)
+///
+/// This class was introduced to avoid issue of a FastJet bug when using genKT clustering
+/// Now using this for all AxesDefinition with a manual recombiner to use the delete_recombiner_when_unused function
+///------------------------------------------------------------------------
+class JetDefinitionWrapper {
+
+public:
+
+ /// Default Constructor
+ JetDefinitionWrapper(JetAlgorithm jet_algorithm_in, double R_in, double xtra_param_in, const JetDefinition::Recombiner *recombiner) {
+ jet_def = fastjet::JetDefinition(jet_algorithm_in, R_in, xtra_param_in);
+ jet_def.set_recombiner(recombiner);
+ jet_def.delete_recombiner_when_unused(); // added to prevent memory leaks
+ }
+
+ /// Additional constructor so that build-in FastJet algorithms can also be called
+ JetDefinitionWrapper(JetAlgorithm jet_algorithm_in, double R_in, const JetDefinition::Recombiner *recombiner, fastjet::Strategy strategy_in) {
+ jet_def = fastjet::JetDefinition(jet_algorithm_in, R_in, recombiner, strategy_in);
+ jet_def.delete_recombiner_when_unused();
+ }
+
+ /// Return jet definition
+ JetDefinition getJetDef() {
+ return jet_def;
+ }
+
+private:
+ JetDefinition jet_def; ///< my jet definition
+};
+
+///------------------------------------------------------------------------
+/// \class WTA_KT_Axes
+/// \brief Axes from exclusive kT, winner-take-all recombination
+///
+/// Axes from kT algorithm and winner-take-all recombination
+///------------------------------------------------------------------------
+class WTA_KT_Axes : public ExclusiveJetAxes {
+public:
+ /// Constructor
+ WTA_KT_Axes()
+ : ExclusiveJetAxes(JetDefinitionWrapper(fastjet::kt_algorithm,
+ fastjet::JetDefinition::max_allowable_R, //maximum jet radius constant
+ _recomb = new WinnerTakeAllRecombiner(), // Needs to be explicitly declared (this will be deleted by JetDefinitionWrapper)
+ fastjet::Best).getJetDef()
+ ) {
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "WTA KT";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "Winner-Take-All KT Axes";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual WTA_KT_Axes* create() const {return new WTA_KT_Axes(*this);}
+
+private:
+ const WinnerTakeAllRecombiner *_recomb; ///< Internal recombiner
+
+};
+
+///------------------------------------------------------------------------
+/// \class WTA_CA_Axes
+/// \brief Axes from exclusive CA, winner-take-all recombination
+///
+/// Axes from CA algorithm and winner-take-all recombination
+///------------------------------------------------------------------------
+class WTA_CA_Axes : public ExclusiveJetAxes {
+public:
+ /// Constructor
+ WTA_CA_Axes()
+ : ExclusiveJetAxes(JetDefinitionWrapper(fastjet::cambridge_algorithm,
+ fastjet::JetDefinition::max_allowable_R, //maximum jet radius constant
+ _recomb = new WinnerTakeAllRecombiner(), // Needs to be explicitly declared (this will be deleted by JetDefinitionWrapper)
+ fastjet::Best).getJetDef()) {
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "WTA CA";
+ };
+
+ /// Long descriptions
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "Winner-Take-All CA Axes";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual WTA_CA_Axes* create() const {return new WTA_CA_Axes(*this);}
+
+private:
+ const WinnerTakeAllRecombiner *_recomb; ///< Internal recombiner
+
+};
+
+
+///------------------------------------------------------------------------
+/// \class GenKT_Axes
+/// \brief Axes from exclusive generalized kT
+///
+/// Axes from a general KT algorithm (standard E-scheme recombination)
+/// Requires the power of the KT algorithm to be used and the radius parameter
+///------------------------------------------------------------------------
+class GenKT_Axes : public ExclusiveJetAxes {
+
+public:
+ /// Constructor
+ GenKT_Axes(double p, double R0 = fastjet::JetDefinition::max_allowable_R)
+ : ExclusiveJetAxes(fastjet::JetDefinition(fastjet::genkt_algorithm,
+ R0,
+ p)), _p(p), _R0(R0) {
+ if (p < 0) throw Error("GenKT_Axes: Currently only p >=0 is supported.");
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "GenKT Axes";
+ return stream.str();
+ };
+
+ /// Long descriptions
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "General KT (p = " << _p << "), R0 = " << _R0;
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual GenKT_Axes* create() const {return new GenKT_Axes(*this);}
+
+protected:
+ double _p; ///< genkT power
+ double _R0; ///< jet radius
+};
+
+
+///------------------------------------------------------------------------
+/// \class WTA_GenKT_Axes
+/// \brief Axes from exclusive generalized kT, winner-take-all recombination
+///
+/// Axes from a general KT algorithm with a Winner Take All Recombiner
+/// Requires the power of the KT algorithm to be used and the radius parameter
+///------------------------------------------------------------------------
+class WTA_GenKT_Axes : public ExclusiveJetAxes {
+
+public:
+ /// Constructor
+ WTA_GenKT_Axes(double p, double R0 = fastjet::JetDefinition::max_allowable_R)
+ : ExclusiveJetAxes(JetDefinitionWrapper(fastjet::genkt_algorithm,
+ R0,
+ p,
+ _recomb = new WinnerTakeAllRecombiner()
+ ).getJetDef()), _p(p), _R0(R0) {
+ if (p < 0) throw Error("WTA_GenKT_Axes: Currently only p >=0 is supported.");
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "WTA, GenKT Axes";
+ return stream.str();
+ };
+
+ /// Long descriptions
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual WTA_GenKT_Axes* create() const {return new WTA_GenKT_Axes(*this);}
+
+protected:
+ double _p; ///< genkT power
+ double _R0; ///< jet radius
+ const WinnerTakeAllRecombiner *_recomb; ///< Internal recombiner
+};
+
+///------------------------------------------------------------------------
+/// \class GenET_GenKT_Axes
+/// \brief Axes from exclusive kT, generalized Et-scheme recombination
+///
+/// Class using general KT algorithm with a more general recombination scheme
+/// Requires power of KT algorithm, power of recombination weights, and radius parameter
+///------------------------------------------------------------------------
+class GenET_GenKT_Axes : public ExclusiveJetAxes {
+
+public:
+ /// Constructor
+ GenET_GenKT_Axes(double delta, double p, double R0 = fastjet::JetDefinition::max_allowable_R)
+ : ExclusiveJetAxes((JetDefinitionWrapper(fastjet::genkt_algorithm, R0, p, _recomb = new GeneralEtSchemeRecombiner(delta))).getJetDef() ),
+ _delta(delta), _p(p), _R0(R0) {
+ if (p < 0) throw Error("GenET_GenKT_Axes: Currently only p >=0 is supported.");
+ if (delta <= 0) throw Error("GenET_GenKT_Axes: Currently only delta >0 is supported.");
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "GenET, GenKT Axes";
+ return stream.str();
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2);
+ // TODO: if _delta is huge, change to "WTA"
+ if (_delta < std::numeric_limits<int>::max()) stream << "General Recombiner (delta = " << _delta << "), " << "General KT (p = " << _p << ") Axes, R0 = " << _R0;
+ else stream << "Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
+
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual GenET_GenKT_Axes* create() const {return new GenET_GenKT_Axes(*this);}
+
+protected:
+ double _delta; ///< Recombination pT weighting
+ double _p; ///< GenkT power
+ double _R0; ///< jet radius
+ const GeneralEtSchemeRecombiner *_recomb; ///< Internal recombiner
+};
+
+///------------------------------------------------------------------------
+/// \class OnePass_KT_Axes
+/// \brief Axes from exclusive kT, with one-pass minimization
+///
+/// Onepass minimization from kt axes
+///------------------------------------------------------------------------
+class OnePass_KT_Axes : public KT_Axes {
+public:
+ /// Constructor
+ OnePass_KT_Axes() : KT_Axes() {
+ setNPass(ONE_PASS);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "OnePass KT";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "One-Pass Minimization from KT Axes";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual OnePass_KT_Axes* create() const {return new OnePass_KT_Axes(*this);}
+
+
+};
+
+///------------------------------------------------------------------------
+/// \class OnePass_CA_Axes
+/// \brief Axes from exclusive CA, with one-pass minimization
+///
+/// Onepass minimization from CA axes
+///------------------------------------------------------------------------
+class OnePass_CA_Axes : public CA_Axes {
+public:
+ /// Constructor
+ OnePass_CA_Axes() : CA_Axes() {
+ setNPass(ONE_PASS);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "OnePass CA";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "One-Pass Minimization from CA Axes";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual OnePass_CA_Axes* create() const {return new OnePass_CA_Axes(*this);}
+
+
+};
+
+///------------------------------------------------------------------------
+/// \class OnePass_AntiKT_Axes
+/// \brief Axes from inclusive anti-kT, with one-pass minimization
+///
+/// Onepass minimization from AntiKT axes, one parameter R0
+///------------------------------------------------------------------------
+class OnePass_AntiKT_Axes : public AntiKT_Axes {
+
+public:
+ /// Constructor
+ OnePass_AntiKT_Axes(double R0) : AntiKT_Axes(R0) {
+ setNPass(ONE_PASS);
+ }
+
+ /// Short Description
+ virtual std::string short_description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "OnePassAKT" << _R0;
+ return stream.str();
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "One-Pass Minimization from Anti-KT Axes (R0 = " << _R0 << ")";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual OnePass_AntiKT_Axes* create() const {return new OnePass_AntiKT_Axes(*this);}
+
+};
+
+///------------------------------------------------------------------------
+/// \class OnePass_WTA_KT_Axes
+/// \brief Axes from exclusive kT, winner-take-all recombination, with one-pass minimization
+///
+/// Onepass minimization from winner-take-all kt axes
+///------------------------------------------------------------------------
+class OnePass_WTA_KT_Axes : public WTA_KT_Axes {
+public:
+ /// Constructor
+ OnePass_WTA_KT_Axes() : WTA_KT_Axes() {
+ setNPass(ONE_PASS);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "OnePass WTA KT";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "One-Pass Minimization from Winner-Take-All KT Axes";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual OnePass_WTA_KT_Axes* create() const {return new OnePass_WTA_KT_Axes(*this);}
+
+
+};
+
+///------------------------------------------------------------------------
+/// \class OnePass_WTA_CA_Axes
+/// \brief Axes from exclusive CA, winner-take-all recombination, with one-pass minimization
+///
+/// Onepass minimization from winner-take-all CA axes
+///------------------------------------------------------------------------
+class OnePass_WTA_CA_Axes : public WTA_CA_Axes {
+
+public:
+ /// Constructor
+ OnePass_WTA_CA_Axes() : WTA_CA_Axes() {
+ setNPass(ONE_PASS);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "OnePass WTA CA";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "One-Pass Minimization from Winner-Take-All CA Axes";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual OnePass_WTA_CA_Axes* create() const {return new OnePass_WTA_CA_Axes(*this);}
+
+};
+
+///------------------------------------------------------------------------
+/// \class OnePass_GenKT_Axes
+/// \brief Axes from exclusive generalized kT with one-pass minimization
+///
+/// Onepass minimization, General KT Axes (standard E-scheme recombination)
+///------------------------------------------------------------------------
+class OnePass_GenKT_Axes : public GenKT_Axes {
+
+public:
+ /// Constructor
+ OnePass_GenKT_Axes(double p, double R0 = fastjet::JetDefinition::max_allowable_R) : GenKT_Axes(p, R0) {
+ setNPass(ONE_PASS);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "OnePass GenKT";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "One-Pass Minimization from General KT (p = " << _p << "), R0 = " << _R0;
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual OnePass_GenKT_Axes* create() const {return new OnePass_GenKT_Axes(*this);}
+};
+
+///------------------------------------------------------------------------
+/// \class OnePass_WTA_GenKT_Axes
+/// \brief Axes from exclusive generalized kT, winner-take-all recombination, with one-pass minimization
+///
+/// Onepass minimization from winner-take-all, General KT Axes
+///------------------------------------------------------------------------
+class OnePass_WTA_GenKT_Axes : public WTA_GenKT_Axes {
+
+public:
+ /// Constructor
+ OnePass_WTA_GenKT_Axes(double p, double R0 = fastjet::JetDefinition::max_allowable_R) : WTA_GenKT_Axes(p, R0) {
+ setNPass(ONE_PASS);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "OnePass WTA GenKT";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "One-Pass Minimization from Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual OnePass_WTA_GenKT_Axes* create() const {return new OnePass_WTA_GenKT_Axes(*this);}
+};
+
+///------------------------------------------------------------------------
+/// \class OnePass_GenET_GenKT_Axes
+/// \brief Axes from exclusive generalized kT, generalized Et-scheme recombination, with one-pass minimization
+///
+/// Onepass minimization from General Recomb, General KT axes
+///------------------------------------------------------------------------
+class OnePass_GenET_GenKT_Axes : public GenET_GenKT_Axes {
+
+public:
+ /// Constructor
+ OnePass_GenET_GenKT_Axes(double delta, double p, double R0 = fastjet::JetDefinition::max_allowable_R) : GenET_GenKT_Axes(delta, p, R0) {
+ setNPass(ONE_PASS);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "OnePass GenET, GenKT";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2);
+ if (_delta < std::numeric_limits<int>::max()) stream << "One-Pass Minimization from General Recombiner (delta = "
+ << _delta << "), " << "General KT (p = " << _p << ") Axes, R0 = " << _R0;
+ else stream << "One-Pass Minimization from Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual OnePass_GenET_GenKT_Axes* create() const {return new OnePass_GenET_GenKT_Axes(*this);}
+};
+
+
+///------------------------------------------------------------------------
+/// \class Manual_Axes
+/// \brief Manual axes finding
+///
+/// Allows the user to set the axes manually
+///------------------------------------------------------------------------
+class Manual_Axes : public AxesDefinition {
+public:
+ /// Constructor. Note that _needsManualAxes is set to true.
+ Manual_Axes() : AxesDefinition() {
+ setNPass(NO_REFINING);
+ _needsManualAxes = true;
+ }
+
+ /// This is now a dummy function since this is manual mode
+ virtual std::vector<fastjet::PseudoJet> get_starting_axes(int,
+ const std::vector<fastjet::PseudoJet>&,
+ const MeasureDefinition *) const;
+
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "Manual";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "Manual Axes";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual Manual_Axes* create() const {return new Manual_Axes(*this);}
+
+
+};
+
+///------------------------------------------------------------------------
+/// \class OnePass_Manual_Axes
+/// \brief Manual axes finding, with one-pass minimization
+///
+/// One pass minimization from manual starting point
+///------------------------------------------------------------------------
+class OnePass_Manual_Axes : public Manual_Axes {
+public:
+ /// Constructor. Note that _needsManualAxes is set to true.
+ OnePass_Manual_Axes() : Manual_Axes() {
+ setNPass(ONE_PASS);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "OnePass Manual";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "One-Pass Minimization from Manual Axes";
+ return stream.str();
+ };
+
+ // For copying purposes
+ virtual OnePass_Manual_Axes* create() const {return new OnePass_Manual_Axes(*this);}
+
+};
+
+///------------------------------------------------------------------------
+/// \class MultiPass_Axes
+/// \brief Manual axes finding, with multi-pass (randomized) minimization
+///
+/// Multi-pass minimization from kT starting point
+///------------------------------------------------------------------------
+class MultiPass_Axes : public KT_Axes {
+
+public:
+
+ /// Constructor
+ MultiPass_Axes(unsigned int Npass) : KT_Axes() {
+ setNPass(Npass);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "MultiPass";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "Multi-Pass Axes (Npass = " << _Npass << ")";
+ return stream.str();
+ };
+
+ /// For copying purposs
+ virtual MultiPass_Axes* create() const {return new MultiPass_Axes(*this);}
+
+};
+
+///------------------------------------------------------------------------
+/// \class MultiPass_Manual_Axes
+/// \brief Axes finding from exclusive kT, with multi-pass (randomized) minimization
+///
+/// multi-pass minimization from kT starting point
+///------------------------------------------------------------------------
+class MultiPass_Manual_Axes : public Manual_Axes {
+
+public:
+ /// Constructor
+ MultiPass_Manual_Axes(unsigned int Npass) : Manual_Axes() {
+ setNPass(Npass);
+ }
+
+ /// Short Description
+ virtual std::string short_description() const {
+ return "MultiPass Manual";
+ };
+
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "Multi-Pass Manual Axes (Npass = " << _Npass << ")";
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual MultiPass_Manual_Axes* create() const {return new MultiPass_Manual_Axes(*this);}
+
+};
+
+///------------------------------------------------------------------------
+/// \class Comb_GenKT_Axes
+/// \brief Axes from exclusive generalized kT with combinatorial testing
+///
+/// Axes from kT algorithm (standard E-scheme recombination)
+/// Requires nExtra parameter and returns set of N that minimizes N-jettiness
+/// Note that this method is not guaranteed to find a deeper minimum than GenKT_Axes
+///------------------------------------------------------------------------
+class Comb_GenKT_Axes : public ExclusiveCombinatorialJetAxes {
+public:
+ /// Constructor
+ Comb_GenKT_Axes(int nExtra, double p, double R0 = fastjet::JetDefinition::max_allowable_R)
+ : ExclusiveCombinatorialJetAxes(fastjet::JetDefinition(fastjet::genkt_algorithm, R0, p), nExtra),
+ _p(p), _R0(R0) {
+ if (p < 0) throw Error("Comb_GenKT_Axes: Currently only p >=0 is supported.");
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "N Choose M GenKT";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "N Choose M Minimization (nExtra = " << _nExtra << ") from General KT (p = " << _p << "), R0 = " << _R0;
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual Comb_GenKT_Axes* create() const {return new Comb_GenKT_Axes(*this);}
+
+private:
+ double _nExtra; ///< Number of extra axes
+ double _p; ///< GenkT power
+ double _R0; ///< jet radius
+};
+
+
+
+///------------------------------------------------------------------------
+/// \class Comb_WTA_GenKT_Axes
+/// \brief Axes from exclusive generalized kT, winner-take-all recombination, with combinatorial testing
+///
+/// Axes from kT algorithm and winner-take-all recombination
+/// Requires nExtra parameter and returns set of N that minimizes N-jettiness
+///------------------------------------------------------------------------
+class Comb_WTA_GenKT_Axes : public ExclusiveCombinatorialJetAxes {
+public:
+ /// Constructor
+ Comb_WTA_GenKT_Axes(int nExtra, double p, double R0 = fastjet::JetDefinition::max_allowable_R)
+ : ExclusiveCombinatorialJetAxes((JetDefinitionWrapper(fastjet::genkt_algorithm, R0, p, _recomb = new WinnerTakeAllRecombiner())).getJetDef(), nExtra),
+ _p(p), _R0(R0) {
+ if (p < 0) throw Error("Comb_WTA_GenKT_Axes: Currently only p >=0 is supported.");
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "N Choose M WTA GenKT";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2)
+ << "N Choose M Minimization (nExtra = " << _nExtra << ") from Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual Comb_WTA_GenKT_Axes* create() const {return new Comb_WTA_GenKT_Axes(*this);}
+
+private:
+ double _nExtra; ///< Number of extra axes
+ double _p; ///< GenkT power
+ double _R0; ///< jet radius
+ const WinnerTakeAllRecombiner *_recomb; ///< Internal recombiner
+};
+
+///------------------------------------------------------------------------
+/// \class Comb_GenET_GenKT_Axes
+/// \brief Axes from exclusive generalized kT, generalized Et-scheme recombination, with combinatorial testing
+///
+/// Axes from kT algorithm and General Et scheme recombination
+/// Requires nExtra parameter and returns set of N that minimizes N-jettiness
+///------------------------------------------------------------------------
+class Comb_GenET_GenKT_Axes : public ExclusiveCombinatorialJetAxes {
+public:
+ /// Constructor
+ Comb_GenET_GenKT_Axes(int nExtra, double delta, double p, double R0 = fastjet::JetDefinition::max_allowable_R)
+ : ExclusiveCombinatorialJetAxes((JetDefinitionWrapper(fastjet::genkt_algorithm, R0, p, _recomb = new GeneralEtSchemeRecombiner(delta))).getJetDef(), nExtra),
+ _delta(delta), _p(p), _R0(R0) {
+ if (p < 0) throw Error("Comb_GenET_GenKT_Axes: Currently only p >=0 is supported.");
+ if (delta <= 0) throw Error("Comb_GenET_GenKT_Axes: Currently only delta >=0 is supported.");
+ setNPass(NO_REFINING);
+ }
+
+ /// Short description
+ virtual std::string short_description() const {
+ return "N Choose M GenET GenKT";
+ };
+
+ /// Long description
+ virtual std::string description() const {
+ std::stringstream stream;
+ stream << std::fixed << std::setprecision(2);
+ if (_delta < std::numeric_limits<int>::max()) stream << "N choose M Minimization (nExtra = " << _nExtra
+ << ") from General Recombiner (delta = " << _delta << "), " << "General KT (p = " << _p << ") Axes, R0 = " << _R0;
+ else stream << "N choose M Minimization (nExtra = " << _nExtra << ") from Winner-Take-All General KT (p = " << _p << "), R0 = " << _R0;
+ return stream.str();
+ };
+
+ /// For copying purposes
+ virtual Comb_GenET_GenKT_Axes* create() const {return new Comb_GenET_GenKT_Axes(*this);}
+
+private:
+ double _nExtra; ///< Number of extra axes
+ double _delta; ///< Recombination pT weighting exponent
+ double _p; ///< GenkT power
+ double _R0; ///< jet radius
+ const GeneralEtSchemeRecombiner *_recomb; ///< Internal recombiner
+};
+
+
+} // namespace Nsubjettiness
+
+}
+}
+
+#endif // __FASTJET_CONTRIB_NJETTINESS_HH__
diff --git a/include/Rivet/Tools/fjcontrib/BottomUpSoftDrop.hh b/include/Rivet/Tools/fjcontrib/BottomUpSoftDrop.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/BottomUpSoftDrop.hh
@@ -0,0 +1,308 @@
+// $Id: BottomUpSoftDrop.hh 1085 2017-10-11 02:16:59Z jthaler $
+//
+// Copyright (c) 2017-, Gavin P. Salam, Gregory Soyez, Jesse Thaler,
+// Kevin Zhou, Frederic Dreyer
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __BOTTOMUPSOFTDROP_HH__
+#define __BOTTOMUPSOFTDROP_HH__
+
+#include "fastjet/ClusterSequence.hh"
+#include "fastjet/WrappedStructure.hh"
+#include "fastjet/tools/Transformer.hh"
+
+#include <iostream>
+#include <string>
+
+// TODO
+//
+// - missing class description
+//
+// - check what to do when pta=ptb=0
+// for the moment, we recombine both for multiple reasons
+// . this avois breakingteh symemtry between pa and pb
+// . it would be groomed in later steps anyway
+// Note that this is slightly inconsistent with our use of
+// > (instead of >=) in the cdt
+
+//FASTJET_BEGIN_NAMESPACE
+
+//namespace contrib{
+
+namespace Rivet {
+ namespace fjcontrib {
+ using namespace fastjet;
+
+
+// fwd declarations
+class BottomUpSoftDrop;
+class BottomUpSoftDropStructure;
+class BottomUpSoftDropRecombiner;
+class BottomUpSoftDropPlugin;
+
+//----------------------------------------------------------------------
+/// \class BottomUpSoftDrop
+/// Implementation of the BottomUpSoftDrop transformer
+///
+/// Bottom-Up Soft drop grooms a jet by applying a modified
+/// recombination scheme, where particles are recombined only if they
+/// pass the Soft Drop condition
+///
+/// \f[
+/// z < z_{\rm cut} (\theta/R0)^\beta
+/// \f]
+///
+/// the groomed jet contains the particles remaining after this
+/// pair-wise recombination
+///
+/// Note:
+/// - one can use BottomUpSoftDrop on a full event with the
+/// global_grooming(event) method.
+/// - if two recombined particles a and b have momentum pta=ptb=0,
+/// we recombine both.
+///
+
+
+class BottomUpSoftDrop : public Transformer {
+public:
+ /// minimal constructor, which the jet algorithm to CA, sets the radius
+ /// to JetDefinition::max_allowable_R (practically equivalent to
+ /// infinity) and also tries to use a recombiner based on the one in
+ /// the jet definition of the particular jet being Soft Dropped.
+ ///
+ /// \param beta the value for beta
+ /// \param symmetry_cut the value for symmetry_cut
+ /// \param R0 the value for R0
+ BottomUpSoftDrop(double beta, double symmetry_cut, double R0 = 1.0)
+ : _jet_def(cambridge_algorithm, JetDefinition::max_allowable_R),
+ _beta(beta),_symmetry_cut(symmetry_cut), _R0(R0),
+ _get_recombiner_from_jet(true) {}
+
+ /// alternative constructor which takes a specified jet algorithm
+ ///
+ /// \param jet_alg the jet algorithm for the internal clustering (uses R=infty)
+ /// \param symmetry_cut the value of symmetry_cut
+ /// \param beta the value for beta
+ /// \param R0 the value for R0
+ BottomUpSoftDrop(const JetAlgorithm jet_alg, double beta, double symmetry_cut,
+ double R0 = 1.0)
+ : _jet_def(jet_alg, JetDefinition::max_allowable_R),
+ _beta(beta), _symmetry_cut(symmetry_cut), _R0(R0),
+ _get_recombiner_from_jet(true) {}
+
+
+ /// alternative ctor in which the full reclustering jet definition can
+ /// be specified.
+ ///
+ /// \param jet_def the jet definition for the internal clustering
+ /// \param symmetry_cut the value of symmetry_cut
+ /// \param beta the value for beta
+ /// \param R0 the value for R0
+ BottomUpSoftDrop(const JetDefinition &jet_def, double beta, double symmetry_cut,
+ double R0 = 1.0)
+ : _jet_def(jet_def), _beta(beta), _symmetry_cut(symmetry_cut), _R0(R0),
+ _get_recombiner_from_jet(false) {}
+
+ /// action on a single jet
+ virtual PseudoJet result(const PseudoJet &jet) const;
+
+ /// global grooming on a full event
+ /// note: does not support jet areas
+ virtual std::vector<PseudoJet> global_grooming(const std::vector<PseudoJet> & event) const;
+
+ /// description
+ virtual std::string description() const;
+
+ // the type of the associated structure
+ typedef BottomUpSoftDropStructure StructureType;
+
+private:
+ /// check if the jet has explicit_ghosts (knowing that there is an
+ /// area support)
+ bool _check_explicit_ghosts(const PseudoJet &jet) const;
+
+ /// see if there is a common recombiner among the pieces; if there
+ /// is return true and set jet_def_for_recombiner so that the
+ /// recombiner can be taken from that JetDefinition. Otherwise,
+ /// return false. 'assigned' is initially false; when true, each
+ /// time we meet a new jet definition, we'll check it shares the
+ /// same recombiner as jet_def_for_recombiner.
+ bool _check_common_recombiner(const PseudoJet &jet,
+ JetDefinition &jet_def_for_recombiner,
+ bool assigned=false) const;
+
+
+ JetDefinition _jet_def; ///< the internal jet definition
+ double _beta; ///< the value of beta
+ double _symmetry_cut; ///< the value of symmetry_cut
+ double _R0; ///< the value of R0
+ bool _get_recombiner_from_jet; ///< true for minimal constructor,
+ ///< causes recombiner to be set equal
+ ///< to that already used in the jet
+ ///< (if it can be deduced)
+};
+
+//----------------------------------------------------------------------
+/// The structure associated with a PseudoJet thas has gone through a
+/// bottom/up SoftDrop transformer
+class BottomUpSoftDropStructure : public WrappedStructure{
+public:
+ /// default ctor
+ /// \param result_jet the jet for which we have to keep the structure
+ BottomUpSoftDropStructure(const PseudoJet & result_jet)
+ : WrappedStructure(result_jet.structure_shared_ptr()){}
+
+ /// description
+ virtual std::string description() const{
+ return "Bottom/Up Soft Dropped PseudoJet";
+ }
+
+ /// return the constituents that have been rejected
+ std::vector<PseudoJet> rejected() const{
+ return validated_cs()->childless_pseudojets();
+ }
+
+ /// return the other jets that may have been found along with the
+ /// result of the bottom/up Soft Drop
+ /// The resulting vector is sorted in pt
+ std::vector<PseudoJet> extra_jets() const {
+ return sorted_by_pt((!SelectorNHardest(1))(validated_cs()->inclusive_jets()));
+ }
+
+ /// return the value of beta that was used for this specific Soft Drop.
+ double beta() const {return _beta;}
+
+ /// return the value of symmetry_cut that was used for this specific Soft Drop.
+ double symmetry_cut() const {return _symmetry_cut;}
+
+ /// return the value of R0 that was used for this specific Soft Drop.
+ double R0() const {return _R0;}
+
+protected:
+ friend class BottomUpSoftDrop; ///< to allow setting the internal information
+
+private:
+ double _beta, _symmetry_cut, _R0;
+};
+
+//----------------------------------------------------------------------
+/// Class for Soft Drop recombination
+/// recombines the objects that are not vetoed by Bottom-Up SoftDrop
+///
+/// This recombiner only recombines, using the provided 'recombiner',
+/// objects (i and j) that pass the following SoftDrop criterion:
+///
+/// min(pti, ptj) > zcut (pti+ptj) (theta_ij/R0)^beta
+///
+/// If the criterion fail, the hardest of i and j is kept and the
+/// softest is rejected.
+///
+/// Note that this in not meant for standalone use [in particular
+/// because it could lead to memory issues due to the rejected indices
+/// stored internally].
+///
+/// This class is a direct adaptation of PruningRecombiner in Fastjet tools
+class BottomUpSoftDropRecombiner : public JetDefinition::Recombiner {
+public:
+ /// ctor
+ /// \param symmetry_cut value of cut on symmetry measure
+ /// \param beta avalue of beta parameter
+ /// \param recomb pointer to a recombiner to use to cluster pairs
+ BottomUpSoftDropRecombiner(double beta, double symmetry_cut, double R0,
+ const JetDefinition::Recombiner *recombiner)
+ : _beta(beta), _symmetry_cut(symmetry_cut), _R0sqr(R0*R0),
+ _recombiner(recombiner) {}
+
+ /// perform a recombination taking into account the Soft Drop
+ /// conditions
+ virtual void recombine(const PseudoJet &pa,
+ const PseudoJet &pb,
+ PseudoJet &pab) const;
+
+ /// returns the description of the recombiner
+ virtual std::string description() const {
+ std::ostringstream oss;
+ oss << "SoftDrop recombiner with symmetry_cut = " << _symmetry_cut
+ << ", beta = " << _beta
+ << ", and underlying recombiner = " << _recombiner->description();
+ return oss.str();
+ }
+
+ /// return the history indices that have been soft dropped away
+ const std::vector<unsigned int> & rejected() const{ return _rejected;}
+
+ /// clears the list of rejected indices
+ ///
+ /// If one decides to use this recombiner standalone, one has to
+ /// call this after each clustering in order for the rejected() vector
+ /// to remain sensible and not grow to infinite size.
+ void clear_rejected(){ _rejected.clear();}
+
+private:
+ double _beta; ///< beta parameter
+ double _symmetry_cut; ///< value of symmetry_cut
+ double _R0sqr; ///< normalisation of the angular distance
+ const JetDefinition::Recombiner *_recombiner; ///< the underlying recombiner to use
+ mutable std::vector<unsigned int> _rejected; ///< list of rejected history indices
+};
+
+//----------------------------------------------------------------------
+/// \class BottomUpSoftDropPlugin
+/// Class for a bottom/up Soft Drop algorithm, based on the Pruner plugin
+///
+/// This is an internal plugin that clusters the particles using the
+/// BottomUpRecombiner.
+///
+/// See BottomUpRecombiner for a description of what bottom-up
+/// SoftDrop does.
+///
+/// Note that this is an internal class used by the BottomUpSoftDrop
+/// transformer and it is not meant to be used as a standalone
+/// clustering tool.
+class BottomUpSoftDropPlugin : public JetDefinition::Plugin {
+public:
+ /// ctor
+ /// \param jet_def the jet definition to be used for the
+ /// internal clustering
+ /// \param symmetry_cut value of cut on symmetry measure
+ /// \param beta value of beta parameter
+ BottomUpSoftDropPlugin(const JetDefinition &jet_def, double beta, double symmetry_cut,
+ double R0 = 1.0)
+ : _jet_def(jet_def), _beta(beta), _symmetry_cut(symmetry_cut), _R0(R0) {}
+
+ /// the actual clustering work for the plugin
+ virtual void run_clustering(ClusterSequence &input_cs) const;
+
+ /// description of the plugin
+ virtual std::string description() const;
+
+ /// returns the radius
+ virtual double R() const {return _jet_def.R();}
+
+private:
+ JetDefinition _jet_def; ///< the internal jet definition
+ double _beta; ///< beta parameter
+ double _symmetry_cut; ///< value of symmetry_cut
+ double _R0; ///< normalisation of the angular distance
+};
+
+ } }
+
+ //FASTJET_END_NAMESPACE // defined in fastjet/internal/base.hh
+#endif // __BOTTOMUPSOFTDROP_HH__
diff --git a/include/Rivet/Tools/fjcontrib/EnergyCorrelator.hh b/include/Rivet/Tools/fjcontrib/EnergyCorrelator.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/EnergyCorrelator.hh
@@ -0,0 +1,1080 @@
+#ifndef __FASTJET_CONTRIB_ENERGYCORRELATOR_HH__
+#define __FASTJET_CONTRIB_ENERGYCORRELATOR_HH__
+
+// EnergyCorrelator Package
+// Questions/Comments? Email the authors.
+// larkoski@mit.edu, lnecib@mit.edu,
+// gavin.salam@cern.ch jthaler@jthaler.net
+//
+// Copyright (c) 2013-2016
+// Andrew Larkoski, Lina Necib Gavin Salam, and Jesse Thaler
+//
+// $Id: EnergyCorrelator.hh 1098 2018-01-07 20:17:52Z linoush $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <fastjet/internal/base.hh>
+#include "fastjet/FunctionOfPseudoJet.hh"
+
+#include <string>
+#include <climits>
+
+namespace Rivet {
+ // FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+ namespace fjcontrib {
+
+ using namespace fastjet;
+
+/// \mainpage EnergyCorrelator contrib
+///
+/// The EnergyCorrelator contrib provides an implementation of energy
+/// correlators and their ratios as described in arXiv:1305.0007 by
+/// Larkoski, Salam and Thaler. Additionally, the ratio observable
+/// D2 described in arXiv:1409.6298 by Larkoski, Moult and Neill
+/// is also included in this contrib. Finally, a generalized version of
+/// the energy correlation functions is added, defined in
+/// arXiv:1609.07483 by Moult, Necib and Thaler, which allow the
+/// definition of the M series, N series, and U series observables.
+/// There is also a generalized version of D2.
+///
+///
+/// <p>There are 4 main classes:
+///
+/// - EnergyCorrelator
+/// - EnergyCorrelatorRatio
+/// - EnergyCorrelatorDoubleRatio
+/// - EnergyCorrelatorGeneralized
+///
+/// <p>There are five classes that define useful combinations of the ECFs.
+///
+/// - EnergyCorrelatorNseries
+/// - EnergyCorrelatorMseries
+/// - EnergyCorrelatorUseries
+/// - EnergyCorrelatorD2
+/// - EnergyCorrelatorGeneralizedD2
+///
+/// <p> There are also aliases for easier access:
+/// - EnergyCorrelatorCseries (same as EnergyCorrelatorDoubleRatio)
+/// - EnergyCorrelatorC1 (EnergyCorrelatorCseries with i=1)
+/// - EnergyCorrelatorC2 (EnergyCorrelatorCseries with i=2)
+/// - EnergyCorrelatorN2 (EnergyCorrelatorNseries with i=2)
+/// - EnergyCorrelatorN3 (EnergyCorrelatorNseries with i=3)
+/// - EnergyCorrelatorM2 (EnergyCorrelatorMseries with i=2)
+/// - EnergyCorrelatorU1 (EnergyCorrelatorUseries with i=1)
+/// - EnergyCorrelatorU2 (EnergyCorrelatorUseries with i=2)
+/// - EnergyCorrelatorU3 (EnergyCorrelatorUseries with i=3)
+///
+/// Each of these classes is a FastJet FunctionOfPseudoJet.
+/// EnergyCorrelatorDoubleRatio (which is equivalent to EnergyCorrelatorCseries)
+/// is in particular is useful for quark/gluon discrimination and boosted
+/// object tagging.
+///
+/// Using the original 2- and 3-point correlators, EnergyCorrelationD2 has
+/// been shown to be the optimal combination for boosted 2-prong tagging.
+///
+/// The EnergyCorrelatorNseries and EnergyCorrelatorMseries use
+/// generalized correlation functions with different angular scaling,
+/// and are intended for use on 2-prong and 3-prong jets.
+/// The EnergyCorrelatorUseries is useful for quark/gluon discrimimation.
+///
+/// See the file example.cc for an illustration of usage and
+/// example_basic_usage.cc for the most commonly used functions.
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelator
+/// ECF(N,beta) is the N-point energy correlation function, with an angular exponent beta.
+///
+/// It is defined as follows
+///
+/// - \f$ \mathrm{ECF}(1,\beta) = \sum_i E_i \f$
+/// - \f$ \mathrm{ECF}(2,\beta) = \sum_{i<j} E_i E_j \theta_{ij}^\beta \f$
+/// - \f$ \mathrm{ECF}(3,\beta) = \sum_{i<j<k} E_i E_j E_k (\theta_{ij} \theta_{ik} \theta_{jk})^\beta \f$
+/// - \f$ \mathrm{ECF}(4,\beta) = \sum_{i<j<k<l} E_i E_j E_k E_l (\theta_{ij} \theta_{ik} \theta_{il} \theta_{jk} \theta_{jl} \theta_{kl})^\beta \f$
+/// - ...
+///
+/// The correlation can be determined with energies and angles (as
+/// given above) or with transverse momenta and boost invariant angles
+/// (the code's default). The choice is controlled by
+/// EnergyCorrelator::Measure provided in the constructor.
+///
+/// The current implementation handles values of N up to and including 5.
+/// Run times scale as n^N/N!, where n is the number of particles in a jet.
+
+ class EnergyCorrelator : public FunctionOfPseudoJet<double> {
+ friend class EnergyCorrelatorGeneralized; ///< This allow ECFG to access the energy and angle definitions
+ ///< of this class, which are otherwise private.
+ public:
+
+ enum Measure {
+ pt_R, ///< use transverse momenta and boost-invariant angles,
+ ///< eg \f$\mathrm{ECF}(2,\beta) = \sum_{i<j} p_{ti} p_{tj} \Delta R_{ij}^{\beta} \f$
+ E_theta, /// use energies and angles,
+ /// eg \f$\mathrm{ECF}(2,\beta) = \sum_{i<j} E_{i} E_{j} \theta_{ij}^{\beta} \f$
+ E_inv /// use energies and invariant mass,
+ /// eg \f$\mathrm{ECF}(2,\beta) = \sum_{i<j} E_{i} E_{j} (\frac{2 p_{i} \cdot p_{j}}{E_{i} E_{j}})^{\beta/2} \f$
+ };
+
+ enum Strategy {
+ slow, ///< interparticle angles are not cached.
+ ///< For N>=3 this leads to many expensive recomputations,
+ ///< but has only O(n) memory usage for n particles
+
+ storage_array /// the interparticle angles are cached. This gives a significant speed
+ /// improvement for N>=3, but has a memory requirement of (4n^2) bytes.
+ };
+
+ public:
+
+ /// constructs an N-point correlator with angular exponent beta,
+ /// using the specified choice of energy and angular measure as well
+ /// one of two possible underlying computational Strategy
+ EnergyCorrelator(unsigned int N,
+ double beta,
+ Measure measure = pt_R,
+ Strategy strategy = storage_array) :
+ _N(N), _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ /// destructor
+ virtual ~EnergyCorrelator(){}
+
+ /// returns the value of the energy correlator for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ /// returns the the part of the description related to the parameters
+ std::string description_parameters() const;
+ std::string description_no_N() const;
+
+ private:
+
+ unsigned int _N;
+ double _beta;
+ Measure _measure;
+ Strategy _strategy;
+
+ double energy(const PseudoJet& jet) const;
+ double angleSquared(const PseudoJet& jet1, const PseudoJet& jet2) const;
+ double multiply_angles(double angles[], int n_angles, unsigned int N_total) const;
+ void precompute_energies_and_angles(std::vector<fastjet::PseudoJet> const &particles, double* energyStore, double** angleStore) const;
+ double evaluate_n3(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ double evaluate_n4(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ double evaluate_n5(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ };
+
+// core EnergyCorrelator::result code in .cc file.
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorRatio
+/// A class to calculate the ratio of (N+1)-point to N-point energy correlators,
+/// ECF(N+1,beta)/ECF(N,beta),
+/// called \f$ r_N^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorRatio : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an (N+1)-point to N-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorRatio(unsigned int N,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _N(N), _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorRatio() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _N;
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+ inline double EnergyCorrelatorRatio::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelator(_N + 1, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelator(_N, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorDoubleRatio
+/// Calculates the double ratio of energy correlators, ECF(N-1,beta)*ECF(N+1)/ECF(N,beta)^2.
+///
+/// A class to calculate a double ratio of energy correlators,
+/// ECF(N-1,beta)*ECF(N+1,beta)/ECF(N,beta)^2,
+/// called \f$C_N^{(\beta)}\f$ in the publication, and equal to
+/// \f$ r_N^{(\beta)}/r_{N-1}^{(\beta)} \f$.
+///
+
+ class EnergyCorrelatorDoubleRatio : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ EnergyCorrelatorDoubleRatio(unsigned int N,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _N(N), _beta(beta), _measure(measure), _strategy(strategy) {
+
+ if (_N < 1) throw Error("EnergyCorrelatorDoubleRatio: N must be 1 or greater.");
+
+ };
+
+ virtual ~EnergyCorrelatorDoubleRatio() {}
+
+
+ /// returns the value of the energy correlator double-ratio for a
+ /// jet's constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _N;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorDoubleRatio::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelator(_N - 1, _beta, _measure, _strategy).result(jet) * EnergyCorrelator(_N + 1, _beta, _measure, _strategy).result(jet);
+ double denominator = pow(EnergyCorrelator(_N, _beta, _measure, _strategy).result(jet), 2.0);
+
+ return numerator/denominator;
+
+ }
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorC1
+/// A class to calculate the normalized 2-point energy correlators,
+/// ECF(2,beta)/ECF(1,beta)^2,
+/// called \f$ C_1^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorC1 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorC1(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorC1() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorC1::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelator(2, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelator(1, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorC2
+/// A class to calculate the double ratio of 3-point to 2-point
+/// energy correlators,
+/// ECF(3,beta)*ECF(1,beta)/ECF(2,beta)^2,
+/// called \f$ C_2^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorC2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a 3-point to 2-point correlator double ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorC2(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorC2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorC2::result(const PseudoJet& jet) const {
+
+ double numerator3 = EnergyCorrelator(3, _beta, _measure, _strategy).result(jet);
+ double numerator1 = EnergyCorrelator(1, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelator(2, _beta, _measure, _strategy).result(jet);
+
+ return numerator3*numerator1/denominator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorD2
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// ECF(3,beta)*ECF(1,beta)^3/ECF(2,beta)^3,
+/// called \f$ D_2^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorD2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorD2(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorD2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorD2::result(const PseudoJet& jet) const {
+
+ double numerator3 = EnergyCorrelator(3, _beta, _measure, _strategy).result(jet);
+ double numerator1 = EnergyCorrelator(1, _beta, _measure, _strategy).result(jet);
+ double denominator2 = EnergyCorrelator(2, _beta, _measure, _strategy).result(jet);
+
+ return numerator3*numerator1*numerator1*numerator1/denominator2/denominator2/denominator2;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorGeneralized
+/// A generalized and normalized version of the N-point energy correlators, with
+/// angular exponent beta and v number of pairwise angles. When \f$v = {N \choose 2}\f$
+/// (or, for convenience, \f$v = -1\f$), EnergyCorrelatorGeneralized just gives normalized
+/// versions of EnergyCorrelator:
+/// - \f$ \mathrm{ECFG}(-1,1,\beta) = \mathrm{ECFN}(N,\beta) = \mathrm{ECF}(N,\beta)/\mathrm{ECF}(1,\beta)\f$
+///
+/// Note that there is no separate class that implements ECFN, though it is a
+/// notation that we will use in this documentation. Examples of the low-point normalized
+/// correlators are:
+/// - \f$\mathrm{ECFN}(1,\beta) = 1\f$
+/// - \f$\mathrm{ECFN}(2,\beta) = \sum_{i<j} z_i z_j \theta_{ij}^\beta \f$
+/// - \f$\mathrm{ECFN}(3,\beta) = \sum_{i<j<k} z_i z_j z_k (\theta_{ij} \theta_{ik} \theta_{jk})^\beta \f$
+/// - \f$\mathrm{ECFN}(4,\beta) = \sum_{i<j<k<l} z_i z_j z_k z_l (\theta_{ij} \theta_{ik} \theta_{il} \theta_{jk} \theta_{jl} \theta_{kl})^\beta \f$
+/// - ...
+/// where the \f$z_i\f$'s are the energy fractions.
+///
+/// When a new value of v is given, the generalized energy correlators are defined as
+/// - \f$\mathrm{ECFG}(0,1,\beta) = 1\f$
+/// - \f$\mathrm{ECFG}(1,2,\beta) = \sum_{i<j} z_i z_j \theta_{ij}^\beta \f$
+/// - \f$\mathrm{ECFG}(v,3,\beta) = \sum_{i<j<k} z_i z_j z_k \prod_{m = 1}^{v} \min^{(m)} \{ \theta_{ij}, \theta_{jk}, \theta_{ki} \}^\beta \f$
+/// - \f$\mathrm{ECFG}(v,4,\beta) = \sum_{i<j<k<l} z_i z_j z_k z_l \prod_{m = 1}^{v} \min^{(m)} \{ \theta_{ij}, \theta_{ik}, \theta_{il}, \theta_{jk}, \theta_{jl}, \theta_{kl} \}^\beta \f$
+/// - \f$\mathrm{ECFG}(v,n,\beta) = \sum_{i_1 < i_2 < \dots < i_n} z_{i_1} z_{i_2} \dots z_{i_n} \prod_{m = 1}^{v} \min^{(m)}_{s < t \in \{i_1, i_2 , \dots, i_n \}} \{ \theta_{st}^{\beta} \}\f$,
+///
+/// where \f$\min^{(m)}\f$ means the m-th smallest element of the list.
+///
+/// The correlation can be determined with energies and angles (as
+/// given above) or with transverse momenta and boost invariant angles
+/// (the code's default). The choice is controlled by
+/// EnergyCorrelator::Measure provided in the constructor.
+///
+/// The current implementation handles values of N up to and including 5.
+///
+ class EnergyCorrelatorGeneralized : public FunctionOfPseudoJet<double> {
+ public:
+
+ /// constructs an N-point correlator with v_angles pairwise angles
+ /// and angular exponent beta,
+ /// using the specified choice of energy and angular measure as well
+ /// one of two possible underlying computational Strategy
+ EnergyCorrelatorGeneralized(int v_angles,
+ unsigned int N,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _angles(v_angles), _N(N), _beta(beta), _measure(measure), _strategy(strategy), _helper_correlator(1,_beta, _measure, _strategy) {};
+
+ /// destructor
+ virtual ~EnergyCorrelatorGeneralized(){}
+
+ /// returns the value of the normalized energy correlator for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+
+ double result(const PseudoJet& jet) const;
+ std::vector<double> result_all_angles(const PseudoJet& jet) const;
+
+ private:
+
+ int _angles;
+ unsigned int _N;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+ EnergyCorrelator _helper_correlator;
+
+ double energy(const PseudoJet& jet) const;
+ double angleSquared(const PseudoJet& jet1, const PseudoJet& jet2) const;
+ double multiply_angles(double angles[], int n_angles, unsigned int N_total) const;
+ void precompute_energies_and_angles(std::vector<fastjet::PseudoJet> const &particles, double* energyStore, double** angleStore) const;
+ double evaluate_n3(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ double evaluate_n4(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ double evaluate_n5(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ };
+
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorGeneralizedD2
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// ECFN(3,alpha)/ECFN(2,beta)^3 alpha/beta,
+/// called \f$ D_2^{(\alpha, \beta)} \f$ in the publication.
+ class EnergyCorrelatorGeneralizedD2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorGeneralizedD2(
+ double alpha,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _alpha(alpha), _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorGeneralizedD2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _alpha;
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorGeneralizedD2::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelatorGeneralized(-1, 3, _alpha, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(-1, 2, _beta, _measure, _strategy).result(jet);
+
+ return numerator/pow(denominator, 3.0*_alpha/_beta);
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorNseries
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// N_n = ECFG(2,n+1,beta)/ECFG(1,n,beta)^2,
+/// called \f$ N_i^{(\alpha, \beta)} \f$ in the publication.
+/// By definition, N_1^{beta} = ECFG(1, 2, 2*beta), where the angular exponent
+/// is twice as big since the N series should involve two pairwise angles.
+ class EnergyCorrelatorNseries : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a n 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorNseries(
+ unsigned int n,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _n(n), _beta(beta), _measure(measure), _strategy(strategy) {
+
+ if (_n < 1) throw Error("EnergyCorrelatorNseries: n must be 1 or greater.");
+
+ };
+
+ virtual ~EnergyCorrelatorNseries() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _n;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+ };
+
+
+ inline double EnergyCorrelatorNseries::result(const PseudoJet& jet) const {
+
+ if (_n == 1) return EnergyCorrelatorGeneralized(1, 2, 2*_beta, _measure, _strategy).result(jet);
+ // By definition, N1 = ECFN(2, 2 beta)
+ double numerator = EnergyCorrelatorGeneralized(2, _n + 1, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(1, _n, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator/denominator;
+
+ }
+
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorN2
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// ECFG(2,3,beta)/ECFG(1,2,beta)^2,
+/// called \f$ N_2^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorN2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorN2(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorN2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorN2::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelatorGeneralized(2, 3, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(1, 2, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorN3
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// ECFG(2,4,beta)/ECFG(1,3,beta)^2,
+/// called \f$ N_3^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorN3 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorN3(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorN3() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorN3::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelatorGeneralized(2, 4, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(1, 3, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorMseries
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// M_n = ECFG(1,n+1,beta)/ECFG(1,n,beta),
+/// called \f$ M_i^{(\alpha, \beta)} \f$ in the publication.
+/// By definition, M_1^{beta} = ECFG(1,2,beta)
+ class EnergyCorrelatorMseries : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a n 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorMseries(
+ unsigned int n,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _n(n), _beta(beta), _measure(measure), _strategy(strategy) {
+
+ if (_n < 1) throw Error("EnergyCorrelatorMseries: n must be 1 or greater.");
+
+ };
+
+ virtual ~EnergyCorrelatorMseries() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _n;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+ };
+
+
+ inline double EnergyCorrelatorMseries::result(const PseudoJet& jet) const {
+
+ if (_n == 1) return EnergyCorrelatorGeneralized(1, 2, _beta, _measure, _strategy).result(jet);
+
+ double numerator = EnergyCorrelatorGeneralized(1, _n + 1, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(1, _n, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator;
+
+ }
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorM2
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// ECFG(1,3,beta)/ECFG(1,2,beta),
+/// called \f$ M_2^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorM2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorM2(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorM2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorM2::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelatorGeneralized(1, 3, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(1, 2, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorCseries
+/// Calculates the C series energy correlators, ECFN(N-1,beta)*ECFN(N+1,beta)/ECFN(N,beta)^2.
+/// This is equivalent to EnergyCorrelatorDoubleRatio
+///
+/// A class to calculate a double ratio of energy correlators,
+/// ECFN(N-1,beta)*ECFN(N+1,beta)/ECFN(N,beta)^2,
+/// called \f$C_N^{(\beta)}\f$ in the publication, and equal to
+/// \f$ r_N^{(\beta)}/r_{N-1}^{(\beta)} \f$.
+///
+
+ class EnergyCorrelatorCseries : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ EnergyCorrelatorCseries(unsigned int N,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _N(N), _beta(beta), _measure(measure), _strategy(strategy) {
+
+ if (_N < 1) throw Error("EnergyCorrelatorCseries: N must be 1 or greater.");
+
+ };
+
+ virtual ~EnergyCorrelatorCseries() {}
+
+
+ /// returns the value of the energy correlator double-ratio for a
+ /// jet's constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _N;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorCseries::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelatorGeneralized(-1, _N - 1, _beta, _measure, _strategy).result(jet) * EnergyCorrelatorGeneralized(-1, _N + 1, _beta, _measure, _strategy).result(jet);
+ double denominator = pow(EnergyCorrelatorGeneralized(-1, _N, _beta, _measure, _strategy).result(jet), 2.0);
+
+ return numerator/denominator;
+
+ }
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorUseries
+/// A class to calculate the observable used for quark versus gluon discrimination
+/// U_n = ECFG(1,n+1,beta),
+/// called \f$ U_i^{(\beta)} \f$ in the publication.
+
+ class EnergyCorrelatorUseries : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a n 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorUseries(
+ unsigned int n,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _n(n), _beta(beta), _measure(measure), _strategy(strategy) {
+
+ if (_n < 1) throw Error("EnergyCorrelatorUseries: n must be 1 or greater.");
+
+ };
+
+ virtual ~EnergyCorrelatorUseries() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _n;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+ };
+
+
+ inline double EnergyCorrelatorUseries::result(const PseudoJet& jet) const {
+
+ double answer = EnergyCorrelatorGeneralized(1, _n + 1, _beta, _measure, _strategy).result(jet);
+ return answer;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorU1
+/// A class to calculate the observable formed from
+/// ECFG(1,2,beta),
+/// called \f$ U_1^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorU1 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a 2-point correlator with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorU1(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorU1() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorU1::result(const PseudoJet& jet) const {
+
+ double answer = EnergyCorrelatorGeneralized(1, 2, _beta, _measure, _strategy).result(jet);
+
+ return answer;
+
+ }
+
+
+ //------------------------------------------------------------------------
+ /// \class EnergyCorrelatorU2
+ /// A class to calculate the observable formed from
+ /// ECFG(1,3,beta),
+ /// called \f$ U_2^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorU2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a 3-point correlator with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorU2(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorU2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorU2::result(const PseudoJet& jet) const {
+
+ double answer = EnergyCorrelatorGeneralized(1, 3, _beta, _measure, _strategy).result(jet);
+
+ return answer;
+
+ }
+
+
+ //------------------------------------------------------------------------
+ /// \class EnergyCorrelatorU3
+ /// A class to calculate the observable formed from
+ /// ECFG(1,4,beta),
+ /// called \f$ U_3^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorU3 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a 4-point correlator with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorU3(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorU3() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorU3::result(const PseudoJet& jet) const {
+
+ double answer = EnergyCorrelatorGeneralized(1, 4, _beta, _measure, _strategy).result(jet);
+
+ return answer;
+
+ }
+
+
+
+} // namespace contrib
+ //FASTJET_END_NAMESPACE
+} // namespace Rivet
+
+#endif // __FASTJET_CONTRIB_ENERGYCORRELATOR_HH__
diff --git a/include/Rivet/Tools/fjcontrib/ExtraRecombiners.hh b/include/Rivet/Tools/fjcontrib/ExtraRecombiners.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/ExtraRecombiners.hh
@@ -0,0 +1,105 @@
+// Nsubjettiness Package
+// Questions/Comments? jthaler@jthaler.net
+//
+// Copyright (c) 2011-14
+// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
+//
+// $Id: ExtraRecombiners.hh 828 2015-07-20 14:52:06Z jthaler $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_WINNERTAKEALLRECOMBINER_HH__
+#define __FASTJET_CONTRIB_WINNERTAKEALLRECOMBINER_HH__
+
+#include "fastjet/PseudoJet.hh"
+#include "fastjet/JetDefinition.hh"
+
+#include <cmath>
+#include <vector>
+#include <list>
+#include <limits>
+#include <stdio.h>
+#include <string.h>
+#include <errno.h>
+
+namespace Rivet {
+namespace fjcontrib {
+
+namespace Nsubjettiness { using namespace fastjet;
+
+///------------------------------------------------------------------------
+/// \class GeneralEtSchemeRecombiner
+/// \brief Recombination scheme with generalized Et weighting
+///
+/// GeneralEtSchemeRecombiner defines a new recombination scheme by inheriting from JetDefinition::Recombiner.
+/// This scheme compares the pT of two input particles, and then combines them into a particle with
+/// a pT equal to the sum of the two particle pTs and a direction (in rapidity/phi) weighted by the respective momenta of the
+/// particle. The weighting is dependent on the power delta. For delta = infinity, this should return the same result as the
+/// WinnerTakeAllRecombiner.
+///------------------------------------------------------------------------
+class GeneralEtSchemeRecombiner : public fastjet::JetDefinition::Recombiner {
+public:
+
+ /// Constructor takes delta weighting
+ /// (delta = 1.0 for Et-scheme, delta = infinity for winner-take-all scheme)
+ GeneralEtSchemeRecombiner(double delta) : _delta(delta) {}
+
+ /// Description
+ virtual std::string description() const;
+
+ /// Recombine pa and pb and put result into pab
+ virtual void recombine(const fastjet::PseudoJet & pa,
+ const fastjet::PseudoJet & pb,
+ fastjet::PseudoJet & pab) const;
+
+private:
+ double _delta; ///< Weighting exponent
+};
+
+///------------------------------------------------------------------------
+/// \class WinnerTakeAllRecombiner
+/// \brief Recombination scheme with winner-take-all weighting
+///
+/// WinnerTakeAllRecombiner defines a new recombination scheme by inheriting from JetDefinition::Recombiner.
+/// This scheme compares the pT of two input particles, and then combines them into a particle with
+/// a pT equal to the sum of the two particle pTs and a direction (in rapidity/phi) identical to that of the harder
+/// particle. This creates a jet with an axis guaranteed to align with a particle in the event.
+///------------------------------------------------------------------------
+class WinnerTakeAllRecombiner : public fastjet::JetDefinition::Recombiner {
+public:
+
+ /// Constructor to choose value of alpha (defaulted to 1 for normal pT sum)
+ WinnerTakeAllRecombiner(double alpha = 1.0) : _alpha(alpha) {}
+
+ /// Description
+ virtual std::string description() const;
+
+ /// recombine pa and pb and put result into pab
+ virtual void recombine(const fastjet::PseudoJet & pa,
+ const fastjet::PseudoJet & pb,
+ fastjet::PseudoJet & pab) const;
+
+private:
+ double _alpha; //power of (pt/E) term when recombining particles
+};
+
+} //namespace Nsubjettiness
+
+}
+}
+
+#endif // __FASTJET_CONTRIB_WINNERTAKEALLRECOMBINER_HH__
diff --git a/include/Rivet/Tools/fjcontrib/IteratedSoftDrop.hh b/include/Rivet/Tools/fjcontrib/IteratedSoftDrop.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/IteratedSoftDrop.hh
@@ -0,0 +1,223 @@
+// $Id: IteratedSoftDrop.hh 1086 2017-10-11 08:07:26Z gsoyez $
+//
+// Copyright (c) 2017-, Jesse Thaler, Kevin Zhou, Gavin P. Salam,
+// Gregory Soyez
+//
+// based on arXiv:1704.06266 by Christopher Frye, Andrew J. Larkoski,
+// Jesse Thaler, Kevin Zhou
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_ITERATEDSOFTDROP_HH__
+#define __FASTJET_CONTRIB_ITERATEDSOFTDROP_HH__
+
+#include "RecursiveSoftDrop.hh"
+
+// FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+ //namespace contrib{
+
+namespace Rivet {
+ namespace fjcontrib {
+ using namespace fastjet;
+
+//------------------------------------------------------------------------
+/// \class IteratedSoftDropInfo
+/// helper class that carries all the relevant information one can get
+/// from running IteratedSoftDrop on a given jet (or vector of jets)
+///
+class IteratedSoftDropInfo{
+public:
+ /// ctor without initialisation
+ IteratedSoftDropInfo(){}
+
+ /// ctor with initialisation
+ IteratedSoftDropInfo(std::vector<std::pair<double,double> > zg_thetag_in)
+ : _all_zg_thetag(zg_thetag_in){}
+
+ /// get the raw list of (angular-ordered) zg and thetag
+ const std::vector<std::pair<double,double> > &all_zg_thetag() const{
+ return _all_zg_thetag;
+ }
+
+ /// overloadd the () operator so that it also returns the full (zg,thetag) list
+ const std::vector<std::pair<double,double> > & operator()() const{
+ return _all_zg_thetag;
+ }
+
+ /// overloadd the [] operator to access the ith (zg,thetag) pair
+ const std::pair<double,double> & operator[](unsigned int i) const{
+ return _all_zg_thetag[i];
+ }
+
+ /// returns the angularity with angular exponent alpha and z
+ /// exponent kappa calculated on the zg's and thetag's found by
+ /// iterated SoftDrop
+ ///
+ /// returns 0 if no substructure was found
+ double angularity(double alpha, double kappa=1.0) const;
+
+ /// returns the Iterated SoftDrop multiplicity
+ unsigned int multiplicity() const{ return _all_zg_thetag.size(); }
+
+ /// returns the Iterated SoftDrop multiplicity (i.e. size)
+ unsigned int size() const{ return _all_zg_thetag.size(); }
+
+protected:
+ /// the real information: angular-ordered list of all the zg and
+ /// thetag that passed the (recursive) SD conddition
+ std::vector<std::pair<double,double> > _all_zg_thetag;
+};
+
+
+
+//------------------------------------------------------------------------
+/// \class IteratedSoftDrop
+/// implementation of the IteratedSoftDrop procedure
+///
+/// This class provides an implementation of the IteratedSoftDrop
+/// procedure. It is based on the SoftDrop procedure can be used to
+/// define a 'groomed symmetry factor', equal to the symmetry factor
+/// of the two subjets of the resulting groomed jet. The Iterated
+/// Soft Drop procedure recursively performs Soft Drop on the harder
+/// branch of the groomed jet, halting at a specified angular cut
+/// \f$\theta_{\rm cut}\f$, returning a list of symmetry factors which
+/// can be used to define observables.
+///
+/// Like SoftDrop, the cut applied recursively is
+/// \f[
+/// z > z_{\rm cut} (\theta/R_0)^\beta
+/// \f]
+/// with z the asymmetry measure and \f$\theta\f$ the geometrical
+/// distance between the two subjets. The procedure halts when
+/// \f$\theta < \theta_{\rm cut}\f$.
+///
+/// By default, this implementation returs the IteratedSoftDropInfo
+/// obtained after running IteratedSoftDrop on a jet
+///
+/// Although all these quantities can be obtained from the returned
+/// IteratedSoftDropInfo, we also provide helpers to directly get the
+/// multiplicity, some (generalised) angularity, or the raw list of
+/// (angular-ordered) (zg, thetag) pairs that passed the (recursive)
+/// SoftDrop condition.
+///
+/// We stress the fact that IteratedSoftDrop is _not_ a Transformer
+/// since it returns an IteratedSoftDropInfo and not a modified
+/// PseudoJet
+///
+class IteratedSoftDrop : public FunctionOfPseudoJet<IteratedSoftDropInfo> {
+public:
+ /// Constructor. Takes in the standard Soft Drop parameters, an angular cut \f$\theta_{\rm cut}\f$,
+ /// and a choice of angular and symmetry measure.
+ ///
+ /// \param beta the Soft Drop beta parameter
+ /// \param symmetry_cut the Soft Drop symmetry cut
+ /// \param angular_cut the angular cutoff to halt Iterated Soft Drop
+ /// \param R0 the angular distance normalization
+ /// \param subtractor an optional pointer to a pileup subtractor (ignored if zero)
+ IteratedSoftDrop(double beta, double symmetry_cut, double angular_cut, double R0 = 1.0,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor = 0);
+
+ /// Full constructor, which takes the following parameters:
+ ///
+ /// \param beta the value of the beta parameter
+ /// \param symmetry_cut the value of the cut on the symmetry measure
+ /// \param symmetry_measure the choice of measure to use to estimate the symmetry
+ /// \param angular_cut the angular cutoff to halt Iterated Soft Drop
+ /// \param R0 the angular distance normalisation [1 by default]
+ /// \param mu_cut the maximal allowed value of mass drop variable mu = m_heavy/m_parent
+ /// \param recursion_choice the strategy used to decide which subjet to recurse into
+ /// \param subtractor an optional pointer to a pileup subtractor (ignored if zero)
+ ///
+ /// Notes:
+ ///
+ /// - by default, SoftDrop will recluster the jet with the
+ /// Cambridge/Aachen algorithm if it is not already the case. This
+ /// behaviour can be changed using the "set_reclustering" method
+ /// defined below
+ ///
+ IteratedSoftDrop(double beta,
+ double symmetry_cut,
+ RecursiveSoftDrop::SymmetryMeasure symmetry_measure,
+ double angular_cut,
+ double R0 = 1.0,
+ double mu_cut = std::numeric_limits<double>::infinity(),
+ RecursiveSoftDrop::RecursionChoice recursion_choice = RecursiveSoftDrop::larger_pt,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor = 0);
+
+ /// default destructor
+ virtual ~IteratedSoftDrop(){}
+
+ //----------------------------------------------------------------------
+ // behaviour tweaks (inherited from RecursiveSoftDrop and RecursiveSymmetryCutBase)
+
+ /// switch to using a dynamical R0 (see RecursiveSoftDrop)
+ void set_dynamical_R0(bool value=true) { _rsd.set_dynamical_R0(value); }
+ bool use_dynamical_R0() const { return _rsd.use_dynamical_R0(); }
+
+ /// an alternative way to set the subtractor (see RecursiveSymmetryCutBase)
+ void set_subtractor(const FunctionOfPseudoJet<PseudoJet> * subtractor_) {_rsd.set_subtractor(subtractor_);}
+ const FunctionOfPseudoJet<PseudoJet> * subtractor() const {return _rsd.subtractor();}
+
+ /// returns the IteratedSoftDropInfo associated with the jet "jet"
+ IteratedSoftDropInfo result(const PseudoJet& jet) const;
+
+ /// Tells the tagger whether to assume that the input jet has
+ /// already been subtracted (relevant only with a non-null
+ /// subtractor, see RecursiveSymmetryCutBase)
+ void set_input_jet_is_subtracted(bool is_subtracted) { _rsd.set_input_jet_is_subtracted(is_subtracted);}
+ bool input_jet_is_subtracted() const {return _rsd.input_jet_is_subtracted();}
+
+ /// configure the reclustering prior to the recursive de-clustering
+ void set_reclustering(bool do_reclustering=true, const Recluster *recluster=0){
+ _rsd.set_reclustering(do_reclustering, recluster);
+ }
+
+ //----------------------------------------------------------------------
+ // actions on jets
+ /// returns vector of ISD symmetry factors and splitting angles
+ std::vector<std::pair<double,double> > all_zg_thetag(const PseudoJet& jet) const{
+ return result(jet).all_zg_thetag();
+ }
+
+ /// returns the angularity with angular exponent alpha and z
+ /// exponent kappa calculated on the zg's and thetag's found by
+ /// iterated SoftDrop
+ ///
+ /// returns 0 if no substructure was found
+ double angularity(const PseudoJet& jet, double alpha, double kappa=1.0) const{
+ return result(jet).angularity(alpha, kappa);
+ }
+
+ /// returns the Iterated SoftDrop multiplicity
+ double multiplicity(const PseudoJet& jet) const{ return result(jet).multiplicity(); }
+
+ /// description of the class
+ std::string description() const;
+
+protected:
+ RecursiveSoftDrop _rsd;
+};
+
+
+
+} } // namespace contrib
+
+ //FASTJET_END_NAMESPACE
+
+#endif // __FASTJET_CONTRIB_ITERATEDSOFTDROP_HH__
diff --git a/include/Rivet/Tools/fjcontrib/MeasureDefinition.hh b/include/Rivet/Tools/fjcontrib/MeasureDefinition.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/MeasureDefinition.hh
@@ -0,0 +1,855 @@
+// Nsubjettiness Package
+// Questions/Comments? jthaler@jthaler.net
+//
+// Copyright (c) 2011-14
+// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
+//
+// $Id: MeasureDefinition.hh 828 2015-07-20 14:52:06Z jthaler $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_MEASUREDEFINITION_HH__
+#define __FASTJET_CONTRIB_MEASUREDEFINITION_HH__
+
+#include "fastjet/PseudoJet.hh"
+#include <cmath>
+#include <vector>
+#include <list>
+#include <limits>
+
+#include "TauComponents.hh"
+
+namespace Rivet {
+namespace fjcontrib {
+
+namespace Nsubjettiness{
+
+
+
+// The following Measures are available (and their relevant arguments):
+// Recommended for usage as jet shapes
+class DefaultMeasure; // Default measure from which next classes derive (should not be called directly)
+class NormalizedMeasure; // (beta,R0)
+class UnnormalizedMeasure; // (beta)
+class NormalizedCutoffMeasure; // (beta,R0,Rcutoff)
+class UnnormalizedCutoffMeasure; // (beta,Rcutoff)
+
+// New measures as of v2.2
+// Recommended for usage as event shapes (or for jet finding)
+class ConicalMeasure; // (beta,R)
+class OriginalGeometricMeasure; // (R)
+class ModifiedGeometricMeasure; // (R)
+class ConicalGeometricMeasure; // (beta, gamma, R)
+class XConeMeasure; // (beta, R)
+
+// Formerly GeometricMeasure, now no longer recommended, kept commented out only for cross-check purposes
+//class DeprecatedGeometricMeasure; // (beta)
+//class DeprecatedGeometricCutoffMeasure; // (beta,Rcutoff)
+
+
+///////
+//
+// MeasureDefinition
+//
+///////
+
+//This is a helper class for the Minimum Axes Finders. It is defined later.
+class LightLikeAxis;
+
+///------------------------------------------------------------------------
+/// \class MeasureDefinition
+/// \brief Base class for measure definitions
+///
+/// This is the base class for measure definitions. Derived classes will calculate
+/// the tau_N of a jet given a specific measure and a set of axes. The measure is
+/// determined by various jet and beam distances (and possible normalization factors).
+///------------------------------------------------------------------------
+class MeasureDefinition {
+
+public:
+
+ /// Description of measure and parameters
+ virtual std::string description() const = 0;
+
+ /// In derived classes, this should return a copy of the corresponding derived class
+ virtual MeasureDefinition* create() const = 0;
+
+ //The following five functions define the measure by which tau_N is calculated,
+ //and are overloaded by the various measures below
+
+ /// Distanes to jet axis. This is called many times, so needs to be as fast as possible
+ /// Unless overloaded, it just calls jet_numerator
+ virtual double jet_distance_squared(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
+ return jet_numerator(particle,axis);
+ }
+
+ /// Distanes to beam. This is called many times, so needs to be as fast as possible
+ /// Unless overloaded, it just calls beam_numerator
+ virtual double beam_distance_squared(const fastjet::PseudoJet& particle) const {
+ return beam_numerator(particle);
+ }
+
+ /// The jet measure used in N-(sub)jettiness
+ virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const = 0;
+ /// The beam measure used in N-(sub)jettiness
+ virtual double beam_numerator(const fastjet::PseudoJet& particle) const = 0;
+
+ /// A possible normalization factor
+ virtual double denominator(const fastjet::PseudoJet& particle) const = 0;
+
+ /// Run a one-pass minimization routine. There is a generic one-pass minimization that works for a wide variety of measures.
+ /// This should be overloaded to create a measure-specific minimization scheme
+ virtual std::vector<fastjet::PseudoJet> get_one_pass_axes(int n_jets,
+ const std::vector<fastjet::PseudoJet>& inputs,
+ const std::vector<fastjet::PseudoJet>& seedAxes,
+ int nAttempts = 1000, // cap number of iterations
+ double accuracy = 0.0001 // cap distance of closest approach
+ ) const;
+
+public:
+
+ /// Returns the tau value for a give set of particles and axes
+ double result(const std::vector<fastjet::PseudoJet>& particles, const std::vector<fastjet::PseudoJet>& axes) const {
+ return component_result(particles,axes).tau();
+ }
+
+ /// Short-hand for the result() function
+ inline double operator() (const std::vector<fastjet::PseudoJet>& particles, const std::vector<fastjet::PseudoJet>& axes) const {
+ return result(particles,axes);
+ }
+
+ /// Return all of the TauComponents for specific input particles and axes
+ TauComponents component_result(const std::vector<fastjet::PseudoJet>& particles, const std::vector<fastjet::PseudoJet>& axes) const;
+
+ /// Create the partitioning according the jet/beam distances and stores them a TauPartition
+ TauPartition get_partition(const std::vector<fastjet::PseudoJet>& particles, const std::vector<fastjet::PseudoJet>& axes) const;
+
+ /// Calculate the tau result using an existing partition
+ TauComponents component_result_from_partition(const TauPartition& partition, const std::vector<fastjet::PseudoJet>& axes) const;
+
+
+
+ /// virtual destructor
+ virtual ~MeasureDefinition(){}
+
+protected:
+
+ /// Flag set by derived classes to choose whether or not to use beam/denominator
+ TauMode _tau_mode;
+
+ /// Flag set by derived classes to say whether cheap get_one_pass_axes method can be used (true by default)
+ bool _useAxisScaling;
+
+ /// This is the only constructor, which requires _tau_mode and _useAxisScaling to be manually set by derived classes.
+ MeasureDefinition() : _tau_mode(UNDEFINED_SHAPE), _useAxisScaling(true) {}
+
+
+ /// Used by derived classes to set whether or not to use beam/denominator information
+ void setTauMode(TauMode tau_mode) {
+ _tau_mode = tau_mode;
+ }
+
+ /// Used by derived classes to say whether one can use cheap get_one_pass_axes
+ void setAxisScaling(bool useAxisScaling) {
+ _useAxisScaling = useAxisScaling;
+ }
+
+ /// Uses denominator information?
+ bool has_denominator() const { return (_tau_mode == NORMALIZED_JET_SHAPE || _tau_mode == NORMALIZED_EVENT_SHAPE);}
+ /// Uses beam information?
+ bool has_beam() const {return (_tau_mode == UNNORMALIZED_EVENT_SHAPE || _tau_mode == NORMALIZED_EVENT_SHAPE);}
+
+ /// Create light-like axis (used in default one-pass minimization routine)
+ fastjet::PseudoJet lightFrom(const fastjet::PseudoJet& input) const {
+ double length = sqrt(pow(input.px(),2) + pow(input.py(),2) + pow(input.pz(),2));
+ return fastjet::PseudoJet(input.px()/length,input.py()/length,input.pz()/length,1.0);
+ }
+
+ /// Shorthand for squaring
+ static inline double sq(double x) {return x*x;}
+
+};
+
+
+///////
+//
+// Default Measures
+//
+///////
+
+
+///------------------------------------------------------------------------
+/// \enum DefaultMeasureType
+/// \brief Options for default measure
+///
+/// Can be used to switch between pp and ee measure types in the DefaultMeasure
+///------------------------------------------------------------------------
+enum DefaultMeasureType {
+ pt_R, /// use transverse momenta and boost-invariant angles,
+ E_theta, /// use energies and angles,
+ lorentz_dot, /// use dot product inspired measure
+ perp_lorentz_dot /// use conical geometric inspired measures
+};
+
+///------------------------------------------------------------------------
+/// \class DefaultMeasure
+/// \brief Base class for default N-subjettiness measure definitions
+///
+/// This class is the default measure as defined in the original N-subjettiness papers.
+/// Based on the conical measure, but with a normalization factor
+/// This measure is defined as the pT of the particle multiplied by deltaR
+/// to the power of beta. This class includes the normalization factor determined by R0
+///------------------------------------------------------------------------
+class DefaultMeasure : public MeasureDefinition {
+
+public:
+
+ /// Description
+ virtual std::string description() const;
+ /// To allow copying around of these objects
+ virtual DefaultMeasure* create() const {return new DefaultMeasure(*this);}
+
+ /// fast jet distance
+ virtual double jet_distance_squared(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
+ return angleSquared(particle, axis);
+ }
+
+ /// fast beam distance
+ virtual double beam_distance_squared(const fastjet::PseudoJet& /*particle*/) const {
+ return _RcutoffSq;
+ }
+
+ /// true jet distance (given by general definitions of energy and angle)
+ virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const{
+ double jet_dist = angleSquared(particle, axis);
+ if (jet_dist > 0.0) {
+ return energy(particle) * std::pow(jet_dist,_beta/2.0);
+ } else {
+ return 0.0;
+ }
+ }
+
+ /// true beam distance
+ virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
+ return energy(particle) * std::pow(_Rcutoff,_beta);
+ }
+
+ /// possible denominator for normalization
+ virtual double denominator(const fastjet::PseudoJet& particle) const {
+ return energy(particle) * std::pow(_R0,_beta);
+ }
+
+ /// Special minimization routine (from v1.0 of N-subjettiness)
+ virtual std::vector<fastjet::PseudoJet> get_one_pass_axes(int n_jets,
+ const std::vector<fastjet::PseudoJet>& inputs,
+ const std::vector<fastjet::PseudoJet>& seedAxes,
+ int nAttempts, // cap number of iterations
+ double accuracy // cap distance of closest approach
+ ) const;
+
+protected:
+ double _beta; ///< Angular exponent
+ double _R0; ///< Normalization factor
+ double _Rcutoff; ///< Cutoff radius
+ double _RcutoffSq; ///< Cutoff radius squared
+ DefaultMeasureType _measure_type; ///< Type of measure used (i.e. pp style or ee style)
+
+
+ /// Constructor is protected so that no one tries to call this directly.
+ DefaultMeasure(double beta, double R0, double Rcutoff, DefaultMeasureType measure_type = pt_R)
+ : MeasureDefinition(), _beta(beta), _R0(R0), _Rcutoff(Rcutoff), _RcutoffSq(sq(Rcutoff)), _measure_type(measure_type)
+ {
+ if (beta <= 0) throw Error("DefaultMeasure: You must choose beta > 0.");
+ if (R0 <= 0) throw Error("DefaultMeasure: You must choose R0 > 0.");
+ if (Rcutoff <= 0) throw Error("DefaultMeasure: You must choose Rcutoff > 0.");
+ }
+
+ /// Added set measure method in case it becomes useful later
+ void setDefaultMeasureType(DefaultMeasureType measure_type) {
+ _measure_type = measure_type;
+ }
+
+ /// Generalized energy value (determined by _measure_type)
+ double energy(const PseudoJet& jet) const;
+ /// Generalized angle value (determined by _measure_type)
+ double angleSquared(const PseudoJet& jet1, const PseudoJet& jet2) const;
+
+ /// Name of _measure_type, so description will include the measure type
+ std::string measure_type_name() const {
+ if (_measure_type == pt_R) return "pt_R";
+ else if (_measure_type == E_theta) return "E_theta";
+ else if (_measure_type == lorentz_dot) return "lorentz_dot";
+ else if (_measure_type == perp_lorentz_dot) return "perp_lorentz_dot";
+ else return "Measure Type Undefined";
+ }
+
+ /// templated for speed (TODO: probably should remove, since not clear that there is a speed gain)
+ template <int N> std::vector<LightLikeAxis> UpdateAxesFast(const std::vector <LightLikeAxis> & old_axes,
+ const std::vector <fastjet::PseudoJet> & inputJets,
+ double accuracy) const;
+
+ /// called by get_one_pass_axes to update axes iteratively
+ std::vector<LightLikeAxis> UpdateAxes(const std::vector <LightLikeAxis> & old_axes,
+ const std::vector <fastjet::PseudoJet> & inputJets,
+ double accuracy) const;
+};
+
+
+///------------------------------------------------------------------------
+/// \class NormalizedCutoffMeasure
+/// \brief Dimensionless default measure, with radius cutoff
+///
+/// This measure is just a wrapper for DefaultMeasure
+///------------------------------------------------------------------------
+class NormalizedCutoffMeasure : public DefaultMeasure {
+
+public:
+
+ /// Constructor
+ NormalizedCutoffMeasure(double beta, double R0, double Rcutoff, DefaultMeasureType measure_type = pt_R)
+ : DefaultMeasure(beta, R0, Rcutoff, measure_type) {
+ setTauMode(NORMALIZED_JET_SHAPE);
+ }
+
+ /// Description
+ virtual std::string description() const;
+
+ /// For copying purposes
+ virtual NormalizedCutoffMeasure* create() const {return new NormalizedCutoffMeasure(*this);}
+
+};
+
+///------------------------------------------------------------------------
+/// \class NormalizedMeasure
+/// \brief Dimensionless default measure, with no cutoff
+///
+/// This measure is the same as NormalizedCutoffMeasure, with Rcutoff taken to infinity.
+///------------------------------------------------------------------------
+class NormalizedMeasure : public NormalizedCutoffMeasure {
+
+public:
+
+ /// Constructor
+ NormalizedMeasure(double beta, double R0, DefaultMeasureType measure_type = pt_R)
+ : NormalizedCutoffMeasure(beta, R0, std::numeric_limits<double>::max(), measure_type) {
+ _RcutoffSq = std::numeric_limits<double>::max();
+ setTauMode(NORMALIZED_JET_SHAPE);
+ }
+
+ /// Description
+ virtual std::string description() const;
+ /// For copying purposes
+ virtual NormalizedMeasure* create() const {return new NormalizedMeasure(*this);}
+
+};
+
+
+///------------------------------------------------------------------------
+/// \class UnnormalizedCutoffMeasure
+/// \brief Dimensionful default measure, with radius cutoff
+///
+/// This class is the unnormalized conical measure. The only difference from NormalizedCutoffMeasure
+/// is that the denominator is defined to be 1.0 by setting _has_denominator to false.
+/// class UnnormalizedCutoffMeasure : public NormalizedCutoffMeasure {
+///------------------------------------------------------------------------
+class UnnormalizedCutoffMeasure : public DefaultMeasure {
+
+public:
+
+ /// Since all methods are identical, UnnormalizedMeasure inherits directly
+ /// from NormalizedMeasure. R0 is a dummy value since the value of R0 is unecessary for this class,
+ /// and the "false" flag sets _has_denominator in MeasureDefinition to false so no denominator is used.
+ UnnormalizedCutoffMeasure(double beta, double Rcutoff, DefaultMeasureType measure_type = pt_R)
+ : DefaultMeasure(beta, std::numeric_limits<double>::quiet_NaN(), Rcutoff, measure_type) {
+ setTauMode(UNNORMALIZED_EVENT_SHAPE);
+ }
+
+ /// Description
+ virtual std::string description() const;
+ /// For copying purposes
+ virtual UnnormalizedCutoffMeasure* create() const {return new UnnormalizedCutoffMeasure(*this);}
+
+};
+
+
+///------------------------------------------------------------------------
+/// \class UnnormalizedMeasure
+/// \brief Dimensionless default measure, with no cutoff
+///
+/// This measure is the same as UnnormalizedCutoffMeasure, with Rcutoff taken to infinity.
+///------------------------------------------------------------------------
+class UnnormalizedMeasure : public UnnormalizedCutoffMeasure {
+
+public:
+ /// Since all methods are identical, UnnormalizedMeasure inherits directly
+ /// from NormalizedMeasure. R0 is a dummy value since the value of R0 is unecessary for this class,
+ /// and the "false" flag sets _has_denominator in MeasureDefinition to false so no denominator is used.
+ UnnormalizedMeasure(double beta, DefaultMeasureType measure_type = pt_R)
+ : UnnormalizedCutoffMeasure(beta, std::numeric_limits<double>::max(), measure_type) {
+ _RcutoffSq = std::numeric_limits<double>::max();
+ setTauMode(UNNORMALIZED_JET_SHAPE);
+ }
+
+ /// Description
+ virtual std::string description() const;
+
+ /// For copying purposes
+ virtual UnnormalizedMeasure* create() const {return new UnnormalizedMeasure(*this);}
+
+};
+
+
+///------------------------------------------------------------------------
+/// \class ConicalMeasure
+/// \brief Dimensionful event-shape measure, with radius cutoff
+///
+/// Very similar to UnnormalizedCutoffMeasure, but with different normalization convention
+/// and using the new default one-pass minimization algorithm.
+/// Axes are also made to be light-like to ensure sensible behavior
+/// Intended to be used as an event shape.
+///------------------------------------------------------------------------
+class ConicalMeasure : public MeasureDefinition {
+
+public:
+
+ /// Constructor
+ ConicalMeasure(double beta, double Rcutoff)
+ : MeasureDefinition(), _beta(beta), _Rcutoff(Rcutoff), _RcutoffSq(sq(Rcutoff)) {
+ if (beta <= 0) throw Error("ConicalMeasure: You must choose beta > 0.");
+ if (Rcutoff <= 0) throw Error("ConicalMeasure: You must choose Rcutoff > 0.");
+ setTauMode(UNNORMALIZED_EVENT_SHAPE);
+ }
+
+ /// Description
+ virtual std::string description() const;
+ /// For copying purposes
+ virtual ConicalMeasure* create() const {return new ConicalMeasure(*this);}
+
+ /// fast jet distance
+ virtual double jet_distance_squared(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
+ PseudoJet lightAxis = lightFrom(axis);
+ return particle.squared_distance(lightAxis);
+ }
+
+ /// fast beam distance
+ virtual double beam_distance_squared(const fastjet::PseudoJet& /*particle*/) const {
+ return _RcutoffSq;
+ }
+
+
+ /// true jet distance
+ virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
+ PseudoJet lightAxis = lightFrom(axis);
+ double jet_dist = particle.squared_distance(lightAxis)/_RcutoffSq;
+ double jet_perp = particle.perp();
+
+ if (_beta == 2.0) {
+ return jet_perp * jet_dist;
+ } else {
+ return jet_perp * pow(jet_dist,_beta/2.0);
+ }
+ }
+
+ /// true beam distance
+ virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
+ return particle.perp();
+ }
+
+ /// no denominator used for this measure
+ virtual double denominator(const fastjet::PseudoJet& /*particle*/) const {
+ return std::numeric_limits<double>::quiet_NaN();
+ }
+
+protected:
+ double _beta; ///< angular exponent
+ double _Rcutoff; ///< effective jet radius
+ double _RcutoffSq;///< effective jet radius squared
+};
+
+
+
+///------------------------------------------------------------------------
+/// \class OriginalGeometricMeasure
+/// \brief Dimensionful event-shape measure, with dot-product distances
+///
+/// This class is the original (and hopefully now correctly coded) geometric measure.
+/// This measure is defined by the Lorentz dot product between
+/// the particle and the axis. This class does not include normalization of tau_N.
+/// New in Nsubjettiness v2.2
+/// NOTE: This is defined differently from the DeprecatedGeometricMeasure which are now commented out.
+///------------------------------------------------------------------------
+class OriginalGeometricMeasure : public MeasureDefinition {
+
+public:
+ /// Constructor
+ OriginalGeometricMeasure(double Rcutoff)
+ : MeasureDefinition(), _Rcutoff(Rcutoff), _RcutoffSq(sq(Rcutoff)) {
+ if (Rcutoff <= 0) throw Error("OriginalGeometricMeasure: You must choose Rcutoff > 0.");
+ setTauMode(UNNORMALIZED_EVENT_SHAPE);
+ setAxisScaling(false); // No need to rescale axes (for speed up in one-pass minimization)
+ }
+
+ /// Description
+ virtual std::string description() const;
+ /// For copying purposes
+ virtual OriginalGeometricMeasure* create() const {return new OriginalGeometricMeasure(*this);}
+
+ // This class uses the default jet_distance_squared and beam_distance_squared
+
+ /// true jet measure
+ virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
+ return dot_product(lightFrom(axis), particle)/_RcutoffSq;
+ }
+
+ /// true beam measure
+ virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
+ fastjet::PseudoJet beam_a(0,0,1,1);
+ fastjet::PseudoJet beam_b(0,0,-1,1);
+ double min_perp = std::min(dot_product(beam_a, particle),dot_product(beam_b, particle));
+ return min_perp;
+ }
+
+ /// no denominator needed for this measure.
+ virtual double denominator(const fastjet::PseudoJet& /*particle*/) const {
+ return std::numeric_limits<double>::quiet_NaN();
+ }
+
+protected:
+ double _Rcutoff; ///< Effective jet radius (rho = R^2)
+ double _RcutoffSq; ///< Effective jet radius squared
+
+};
+
+
+///------------------------------------------------------------------------
+/// \class ModifiedGeometricMeasure
+/// \brief Dimensionful event-shape measure, with dot-product distances, modified beam measure
+///
+/// This class is the Modified geometric measure. This jet measure is defined by the Lorentz dot product between
+/// the particle and the axis, as in the Original Geometric Measure. The beam measure is defined differently from
+/// the above OriginalGeometric to allow for more conical jets. New in Nsubjettiness v2.2
+///------------------------------------------------------------------------
+class ModifiedGeometricMeasure : public MeasureDefinition {
+
+public:
+ /// Constructor
+ ModifiedGeometricMeasure(double Rcutoff)
+ : MeasureDefinition(), _Rcutoff(Rcutoff), _RcutoffSq(sq(Rcutoff)) {
+ if (Rcutoff <= 0) throw Error("ModifiedGeometricMeasure: You must choose Rcutoff > 0.");
+ setTauMode(UNNORMALIZED_EVENT_SHAPE);
+ setAxisScaling(false); // No need to rescale axes (for speed up in one-pass minimization)
+ }
+
+ /// Description
+ virtual std::string description() const;
+ /// For copying purposes
+ virtual ModifiedGeometricMeasure* create() const {return new ModifiedGeometricMeasure(*this);}
+
+ // This class uses the default jet_distance_squared and beam_distance_squared
+
+ /// True jet measure
+ virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
+ return dot_product(lightFrom(axis), particle)/_RcutoffSq;
+ }
+
+ /// True beam measure
+ virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
+ fastjet::PseudoJet lightParticle = lightFrom(particle);
+ return 0.5*particle.mperp()*lightParticle.pt();
+ }
+
+ /// This measure does not require a denominator
+ virtual double denominator(const fastjet::PseudoJet& /*particle*/) const {
+ return std::numeric_limits<double>::quiet_NaN();
+ }
+
+protected:
+ double _Rcutoff; ///< Effective jet radius (rho = R^2)
+ double _RcutoffSq; ///< Effective jet radius squared
+
+
+};
+
+///------------------------------------------------------------------------
+/// \class ConicalGeometricMeasure
+/// \brief Dimensionful event-shape measure, basis for XCone jet algorithm
+///
+/// This class is the Conical Geometric measure. This measure is defined by the Lorentz dot product between
+/// the particle and the axis normalized by the axis and particle pT, as well as a factor of cosh(y) to vary
+/// the rapidity depepdence of the beam. New in Nsubjettiness v2.2, and the basis for the XCone jet algorithm
+///------------------------------------------------------------------------
+class ConicalGeometricMeasure : public MeasureDefinition {
+
+public:
+
+ /// Constructor
+ ConicalGeometricMeasure(double jet_beta, double beam_gamma, double Rcutoff)
+ : MeasureDefinition(), _jet_beta(jet_beta), _beam_gamma(beam_gamma), _Rcutoff(Rcutoff), _RcutoffSq(sq(Rcutoff)){
+ if (jet_beta <= 0) throw Error("ConicalGeometricMeasure: You must choose beta > 0.");
+ if (beam_gamma <= 0) throw Error("ConicalGeometricMeasure: You must choose gamma > 0.");
+ if (Rcutoff <= 0) throw Error("ConicalGeometricMeasure: You must choose Rcutoff > 0.");
+ setTauMode(UNNORMALIZED_EVENT_SHAPE);
+ }
+
+ /// Description
+ virtual std::string description() const;
+ /// For copying purposes
+ virtual ConicalGeometricMeasure* create() const {return new ConicalGeometricMeasure(*this);}
+
+ /// fast jet measure
+ virtual double jet_distance_squared(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
+ fastjet::PseudoJet lightAxis = lightFrom(axis);
+ double pseudoRsquared = 2.0*dot_product(lightFrom(axis),particle)/(lightAxis.pt()*particle.pt());
+ return pseudoRsquared;
+ }
+
+ /// fast beam measure
+ virtual double beam_distance_squared(const fastjet::PseudoJet& /*particle*/) const {
+ return _RcutoffSq;
+ }
+
+ /// true jet measure
+ virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
+ double jet_dist = jet_distance_squared(particle,axis)/_RcutoffSq;
+ if (jet_dist > 0.0) {
+ fastjet::PseudoJet lightParticle = lightFrom(particle);
+ double weight = (_beam_gamma == 1.0) ? 1.0 : std::pow(0.5*lightParticle.pt(),_beam_gamma - 1.0);
+ return particle.pt() * weight * std::pow(jet_dist,_jet_beta/2.0);
+ } else {
+ return 0.0;
+ }
+ }
+
+ /// true beam measure
+ virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
+ fastjet::PseudoJet lightParticle = lightFrom(particle);
+ double weight = (_beam_gamma == 1.0) ? 1.0 : std::pow(0.5*lightParticle.pt(),_beam_gamma - 1.0);
+ return particle.pt() * weight;
+ }
+
+ /// no denominator needed
+ virtual double denominator(const fastjet::PseudoJet& /*particle*/) const {
+ return std::numeric_limits<double>::quiet_NaN();
+ }
+
+protected:
+ double _jet_beta; ///< jet angular exponent
+ double _beam_gamma; ///< beam angular exponent (gamma = 1.0 is recommended)
+ double _Rcutoff; ///< effective jet radius
+ double _RcutoffSq; ///< effective jet radius squared
+
+};
+
+///------------------------------------------------------------------------
+/// \class XConeMeasure
+/// \brief Dimensionful event-shape measure used in XCone jet algorithm
+///
+/// This class is the XCone Measure. This is the default measure for use with the
+/// XCone algorithm. It is identical to the conical geometric measure but with gamma = 1.0.
+///------------------------------------------------------------------------
+class XConeMeasure : public ConicalGeometricMeasure {
+
+public:
+ /// Constructor
+ XConeMeasure(double jet_beta, double R)
+ : ConicalGeometricMeasure(jet_beta,
+ 1.0, // beam_gamma, hard coded at gamma = 1.0 default
+ R // Rcutoff scale
+ ) { }
+
+ /// Description
+ virtual std::string description() const;
+ /// For copying purposes
+ virtual XConeMeasure* create() const {return new XConeMeasure(*this);}
+
+};
+
+///------------------------------------------------------------------------
+/// \class LightLikeAxis
+/// \brief Helper class to define light-like axes directions
+///
+/// This is a helper class for the minimization routines.
+/// It creates a convenient way of defining axes in order to better facilitate calculations.
+///------------------------------------------------------------------------
+class LightLikeAxis {
+
+public:
+ /// Bare constructor
+ LightLikeAxis() : _rap(0.0), _phi(0.0), _weight(0.0), _mom(0.0) {}
+ /// Constructor
+ LightLikeAxis(double my_rap, double my_phi, double my_weight, double my_mom) :
+ _rap(my_rap), _phi(my_phi), _weight(my_weight), _mom(my_mom) {}
+
+ /// Rapidity
+ double rap() const {return _rap;}
+ /// Azimuth
+ double phi() const {return _phi;}
+ /// weight factor
+ double weight() const {return _weight;}
+ /// pt momentum
+ double mom() const {return _mom;}
+
+ /// set rapidity
+ void set_rap(double my_set_rap) {_rap = my_set_rap;}
+ /// set azimuth
+ void set_phi(double my_set_phi) {_phi = my_set_phi;}
+ /// set weight factor
+ void set_weight(double my_set_weight) {_weight = my_set_weight;}
+ /// set pt momentum
+ void set_mom(double my_set_mom) {_mom = my_set_mom;}
+ /// set all kinematics
+ void reset(double my_rap, double my_phi, double my_weight, double my_mom) {_rap=my_rap; _phi=my_phi; _weight=my_weight; _mom=my_mom;}
+
+ /// Return PseudoJet version
+ fastjet::PseudoJet ConvertToPseudoJet();
+
+ /// Squared distance to PseudoJet
+ double DistanceSq(const fastjet::PseudoJet& input) const {
+ return DistanceSq(input.rap(),input.phi());
+ }
+
+ /// Distance to PseudoJet
+ double Distance(const fastjet::PseudoJet& input) const {
+ return std::sqrt(DistanceSq(input));
+ }
+
+ /// Squared distance to Lightlikeaxis
+ double DistanceSq(const LightLikeAxis& input) const {
+ return DistanceSq(input.rap(),input.phi());
+ }
+
+ /// Distance to Lightlikeaxis
+ double Distance(const LightLikeAxis& input) const {
+ return std::sqrt(DistanceSq(input));
+ }
+
+private:
+ double _rap; ///< rapidity
+ double _phi; ///< azimuth
+ double _weight; ///< weight factor
+ double _mom; ///< pt momentum
+
+ /// Internal squared distance calculation
+ double DistanceSq(double rap2, double phi2) const {
+ double rap1 = _rap;
+ double phi1 = _phi;
+
+ double distRap = rap1-rap2;
+ double distPhi = std::fabs(phi1-phi2);
+ if (distPhi > M_PI) {distPhi = 2.0*M_PI - distPhi;}
+ return distRap*distRap + distPhi*distPhi;
+ }
+
+ /// Internal distance calculation
+ double Distance(double rap2, double phi2) const {
+ return std::sqrt(DistanceSq(rap2,phi2));
+ }
+
+};
+
+
+////------------------------------------------------------------------------
+///// \class DeprecatedGeometricCutoffMeasure
+//// This class is the old, incorrectly coded geometric measure.
+//// It is kept in case anyone wants to check old code, but should not be used for production purposes.
+//class DeprecatedGeometricCutoffMeasure : public MeasureDefinition {
+//
+//public:
+//
+// // Please, please don't use this.
+// DeprecatedGeometricCutoffMeasure(double jet_beta, double Rcutoff)
+// : MeasureDefinition(),
+// _jet_beta(jet_beta),
+// _beam_beta(1.0), // This is hard coded, since alternative beta_beam values were never checked.
+// _Rcutoff(Rcutoff),
+// _RcutoffSq(sq(Rcutoff)) {
+// setTauMode(UNNORMALIZED_EVENT_SHAPE);
+// setAxisScaling(false);
+// if (jet_beta != 2.0) {
+// throw Error("Geometric minimization is currently only defined for beta = 2.0.");
+// }
+// }
+//
+// virtual std::string description() const;
+//
+// virtual DeprecatedGeometricCutoffMeasure* create() const {return new DeprecatedGeometricCutoffMeasure(*this);}
+//
+// virtual double jet_distance_squared(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
+// fastjet::PseudoJet lightAxis = lightFrom(axis);
+// double pseudoRsquared = 2.0*dot_product(lightFrom(axis),particle)/(lightAxis.pt()*particle.pt());
+// return pseudoRsquared;
+// }
+//
+// virtual double beam_distance_squared(const fastjet::PseudoJet& /*particle*/) const {
+// return _RcutoffSq;
+// }
+//
+// virtual double jet_numerator(const fastjet::PseudoJet& particle, const fastjet::PseudoJet& axis) const {
+// fastjet::PseudoJet lightAxis = lightFrom(axis);
+// double weight = (_beam_beta == 1.0) ? 1.0 : std::pow(lightAxis.pt(),_beam_beta - 1.0);
+// return particle.pt() * weight * std::pow(jet_distance_squared(particle,axis),_jet_beta/2.0);
+// }
+//
+// virtual double beam_numerator(const fastjet::PseudoJet& particle) const {
+// double weight = (_beam_beta == 1.0) ? 1.0 : std::pow(particle.pt()/particle.e(),_beam_beta - 1.0);
+// return particle.pt() * weight * std::pow(_Rcutoff,_jet_beta);
+// }
+//
+// virtual double denominator(const fastjet::PseudoJet& /*particle*/) const {
+// return std::numeric_limits<double>::quiet_NaN();
+// }
+//
+// virtual std::vector<fastjet::PseudoJet> get_one_pass_axes(int n_jets,
+// const std::vector<fastjet::PseudoJet>& inputs,
+// const std::vector<fastjet::PseudoJet>& seedAxes,
+// int nAttempts, // cap number of iterations
+// double accuracy // cap distance of closest approach
+// ) const;
+//
+//protected:
+// double _jet_beta;
+// double _beam_beta;
+// double _Rcutoff;
+// double _RcutoffSq;
+//
+//};
+//
+//// ------------------------------------------------------------------------
+//// / \class DeprecatedGeometricMeasure
+//// Same as DeprecatedGeometricMeasureCutoffMeasure, but with Rcutoff taken to infinity.
+//// NOTE: This class should not be used for production purposes.
+//class DeprecatedGeometricMeasure : public DeprecatedGeometricCutoffMeasure {
+//
+//public:
+// DeprecatedGeometricMeasure(double beta)
+// : DeprecatedGeometricCutoffMeasure(beta,std::numeric_limits<double>::max()) {
+// _RcutoffSq = std::numeric_limits<double>::max();
+// setTauMode(UNNORMALIZED_JET_SHAPE);
+// }
+//
+// virtual std::string description() const;
+//
+// virtual DeprecatedGeometricMeasure* create() const {return new DeprecatedGeometricMeasure(*this);}
+//};
+
+
+} //namespace Nsubjettiness
+
+}
+}
+
+#endif // __FASTJET_CONTRIB_MEASUREDEFINITION_HH__
diff --git a/include/Rivet/Tools/fjcontrib/ModifiedMassDropTagger.hh b/include/Rivet/Tools/fjcontrib/ModifiedMassDropTagger.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/ModifiedMassDropTagger.hh
@@ -0,0 +1,132 @@
+// $Id: ModifiedMassDropTagger.hh 1032 2017-07-31 14:20:03Z gsoyez $
+//
+// Copyright (c) 2014-, Gavin P. Salam
+// based on arXiv:1307.007 by Mrinal Dasgupta, Simone Marzani and Gavin P. Salam
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_MODIFIEDMASSDROPTAGGER_HH__
+#define __FASTJET_CONTRIB_MODIFIEDMASSDROPTAGGER_HH__
+
+#include "RecursiveSymmetryCutBase.hh"
+
+//FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+ //namespace contrib{
+
+namespace Rivet {
+ namespace fjcontrib {
+ using namespace fastjet;
+
+//------------------------------------------------------------------------
+/// \class ModifiedMassDropTagger
+/// An implementation of the modified Mass-Drop Tagger from arXiv:1307.0007.
+///
+class ModifiedMassDropTagger : public RecursiveSymmetryCutBase {
+public:
+
+ /// Simplified constructor, which takes just a symmetry cut (applied
+ /// on the scalar_z variable) and an optional subtractor.
+ ///
+ /// In this incarnation the ModifiedMassDropTagger is a bit of a
+ /// misnomer, because there is no mass-drop condition
+ /// applied. Recursion into the jet structure chooses the prong with
+ /// largest pt. (Results from arXiv:1307.0007 were based on the
+ /// largest mt, but this only makes a difference for values of the
+ /// symmetry_cut close to 1/2).
+ ///
+ /// If the (optional) pileup subtractor can be supplied, then see
+ /// also the documentation for the set_input_jet_is_subtracted() member
+ /// function.
+ ///
+ /// NB: The configuration of MMDT provided by this constructor is
+ /// probably the most robust for use with subtraction.
+ ModifiedMassDropTagger(double symmetry_cut,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor = 0
+ ) :
+ RecursiveSymmetryCutBase(scalar_z, // the default SymmetryMeasure
+ std::numeric_limits<double>::infinity(), // the default is no mass drop
+ larger_pt, // the default RecursionChoice
+ subtractor),
+ _symmetry_cut(symmetry_cut)
+ {}
+
+ /// Full constructor, which takes the following parameters:
+ ///
+ /// \param symmetry_cut the value of the cut on the symmetry measure
+ /// \param symmetry_measure the choice of measure to use to estimate the symmetry
+ /// \param mu_cut the maximal allowed value of mass drop variable mu = m_heavy/m_parent
+ /// \param recursion_choice the strategy used to decide which subjet to recurse into
+ /// \param subtractor an optional pointer to a pileup subtractor (ignored if zero)
+ ///
+ /// To obtain the mMDT as discussed in arXiv:1307.0007, use an
+ /// symmetry_measure that's one of the following
+ ///
+ /// - RecursiveSymmetryCutBase::y (for a cut on y)
+ /// - RecursiveSymmetryCutBase::scalar_z (for a cut on z)
+ ///
+ /// and use the default recursion choice of
+ /// RecursiveSymmetryCutBase::larger_pt (larger_mt will give something
+ /// very similar, while larger_m will give the behaviour of the
+ /// original, but now deprecated MassDropTagger)
+ ///
+ /// Notes:
+ ///
+ /// - By default the ModifiedMassDropTagger will relcuster the jets
+ /// with the C/A algorithm (if needed).
+ ///
+ /// - the mu_cut parameter is mostly irrelevant when it's taken
+ /// larger than about 1/2: the tagger is then one that cuts
+ /// essentially on the (a)symmetry of the jet's momentum
+ /// sharing. The default value of infinity turns off its use
+ /// entirely
+ ModifiedMassDropTagger(double symmetry_cut,
+ SymmetryMeasure symmetry_measure,
+ double mu_cut = std::numeric_limits<double>::infinity(),
+ RecursionChoice recursion_choice = larger_pt,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor = 0
+ ) :
+ RecursiveSymmetryCutBase(symmetry_measure, mu_cut, recursion_choice, subtractor),
+ _symmetry_cut(symmetry_cut)
+ {}
+
+ /// default destructor
+ virtual ~ModifiedMassDropTagger(){}
+
+ //----------------------------------------------------------------------
+ // access to class info
+ double symmetry_cut() const { return _symmetry_cut; }
+
+protected:
+
+ /// The symmetry cut function for MMDT returns just a constant, since the cut value
+ /// has no dependence on the subjet kinematics
+ virtual double symmetry_cut_fn(const PseudoJet & /* p1 */,
+ const PseudoJet & /* p2 */,
+ void *extra_parameters = 0
+ ) const {return _symmetry_cut;}
+ virtual std::string symmetry_cut_description() const;
+
+ double _symmetry_cut;
+};
+
+} } // namespace contrib
+
+ //FASTJET_END_NAMESPACE
+
+#endif // __FASTJET_CONTRIB_MODIFIEDMASSDROPTAGGER_HH__
diff --git a/include/Rivet/Tools/fjcontrib/Njettiness.hh b/include/Rivet/Tools/fjcontrib/Njettiness.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/Njettiness.hh
@@ -0,0 +1,266 @@
+// Nsubjettiness Package
+// Questions/Comments? jthaler@jthaler.net
+//
+// Copyright (c) 2011-14
+// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
+//
+// $Id: Njettiness.hh 822 2015-06-15 23:52:57Z jthaler $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_NJETTINESS_HH__
+#define __FASTJET_CONTRIB_NJETTINESS_HH__
+
+
+#include "MeasureDefinition.hh"
+#include "AxesDefinition.hh"
+#include "TauComponents.hh"
+
+#include "fastjet/PseudoJet.hh"
+#include "fastjet/SharedPtr.hh"
+#include <fastjet/LimitedWarning.hh>
+
+#include <cmath>
+#include <vector>
+#include <list>
+
+namespace Rivet {
+namespace fjcontrib {
+
+namespace Nsubjettiness { using namespace fastjet;
+
+/** \mainpage Nsubjettiness Documentation
+ *
+ * These Doxygen pages provide automatically generated documentation for the
+ * Nsubjettiness FastJet contrib. This documentation is being slowly improved.
+ *
+ * \section core_classes Core Classes
+ *
+ * - Nsubjettiness: Calculating N-subjettiness jet shapes
+ * - NsubjettinessRatio: Calculating N-subjettiness ratios
+ * - XConePlugin: Running the XCone jet algorithm
+ * - NjettinessPlugin: Running generic N-jettiness as a jet algorithm
+ *
+ * \subsection core_classes_helper Helper Classes for Core
+ * - Njettiness: Core code for all N-(sub)jettiness calculations
+ * - NjettinessExtras: Way to access additional N-jettiness information
+ * - TauComponents: Output format for all N-(sub)jettiness information
+ * - TauPartition: Access to N-(sub)jettiness partitioning information
+ * - PseudoXConePlugin: Testing code to compare to XConePlugin (doesn't use one-pass minimization)
+ *
+ * \section axes_classes Axes Definitions
+ *
+ * \subsection axes_classes_base Base Classes
+ * - AxesDefinition: Defines generic axes definition
+ * - ExclusiveJetAxes: Axes finder from exclusive jet algorithm
+ * - ExclusiveCombinatorialJetAxes: Axes finder from exclusive jet algorithm (with extra axes to test combinatoric options)
+ * - HardestJetAxes: Axes finder from inclusive jet algorithm
+ *
+ * \subsection axes_classes_derived Derived Classes
+ *
+ * \b OnePass means iterative improvement to a (local) N-(sub)jettiness minimum.
+ *
+ * \b MultiPass means using multiple random seed inputs
+ *
+ * \b Comb means checking N + Nextra choose N combinatorial options
+ *
+ * - KT_Axes / OnePass_KT_Axes: Axes from exclusive kT
+ * - CA_Axes / OnePass_CA_Axes: Axes from exclusive Cambridge/Aachen
+ * - AntiKT_Axes / OnePass_AntiKT_Axes: Axes from inclusive anti-kT
+ * - WTA_KT_Axes / OnePass_WTA_KT_Axes: Axes from exclusive kT, using winner-take-all recombination
+ * - WTA_CA_Axes / OnePass_WTA_CA_Axes: Axes from exclusive CA, using winner-take-all recombination
+ *
+ * - GenET_GenKT_Axes / OnePass_GenET_GenKT_Axes / Comb_GenET_GenKT_Axes: Axes from exclusive generalized kt, with generalized Et recombination
+ * - WTA_GenKT_Axes / OnePass_WTA_GenKT_Axes / Comb_WTA_GenKT_Axes: Axes from exclusive generalized kt, with winner-take-all recombination
+ *
+ * - Manual_Axes / OnePass_Manual_Axes / MultiPass_Manual_Axes: Use manual axes
+ * - MultiPass_Axes: Multiple passes with random input seeds
+ *
+ * \subsection axes_classes_helper Helper Classes for Axes
+ * - GeneralEtSchemeRecombiner: Generalized Et-scheme recombiner
+ * - WinnerTakeAllRecombiner: Winner-take-all recombiner (similar functionality now in FastJet 3.1)
+ * - JetDefinitionWrapper: Wrapper for Jet Definitions to handle memory management
+ *
+ * \section measure_classes Measure Definitions
+ *
+ * \subsection measure_classes_bases Base Classes
+ * - MeasureDefinition: Defines generic measures
+ * - DefaultMeasure: Base class for the original N-subjettiness measures
+ *
+ * \subsection measure_classes_derived Derived Classes
+ * - NormalizedMeasure / UnnormalizedMeasure / NormalizedCutoffMeasure / UnnormalizedCutoffMeasure : Variants on the default N-subjettiness measure.
+ * - ConicalMeasure: Similar to default measure, but intended as N-jettiness event shape
+ * - ConicalGeometricMeasure / XConeMeasure: Measure used in XCone jet algorithm
+ * - OriginalGeometricMeasure / ModifiedGeometricMeasure: Dot product measures useful for theoretical calcualtions
+ *
+ * \subsection measure_classes_helper Helper Classes for Measures
+ * - LightLikeAxis : Defines light-like axis
+ */
+
+///////
+//
+// Main Njettiness Class
+//
+///////
+
+///------------------------------------------------------------------------
+/// \class Njettiness
+/// \brief Core class for N-(sub)jettiness calculations
+///
+/**
+ * The N-jettiness event shape.
+ *
+ * This is the core class used to perform N-jettiness jet finding (via NjettinessPlugin or XConePluggin)
+ * as well as find the N-subjettiness jet shape (via Nsubjettiness).
+ *
+ * In general, the user should never need to call this object. In addition, its API should not be considered
+ * fixed, since all code improvements effectively happen from reorganizing this class.
+ *
+ * Njettiness uses AxesDefinition and MeasureDefinition together in order to find tau_N for the event.
+ * It also can return information about the axes and jets it used in the calculation, as well as
+ * information about how the event was partitioned.
+ */
+class Njettiness {
+public:
+
+ /// Main constructor that uses AxesMode and MeasureDefinition to specify measure
+ /// Unlike Nsubjettiness or NjettinessPlugin, the value N is not chosen
+ Njettiness(const AxesDefinition & axes_def, const MeasureDefinition & measure_def);
+
+ /// Destructor
+ ~Njettiness() {};
+
+ /// setAxes for Manual mode
+ void setAxes(const std::vector<fastjet::PseudoJet> & myAxes);
+
+ /// Calculates and returns all TauComponents that user would want.
+ /// This information is stored in _current_tau_components for later access as well.
+ TauComponents getTauComponents(unsigned n_jets, const std::vector<fastjet::PseudoJet> & inputJets) const;
+
+ /// Calculates the value of N-subjettiness,
+ /// but only returns the tau value from _current_tau_components
+ double getTau(unsigned n_jets, const std::vector<fastjet::PseudoJet> & inputJets) const {
+ return getTauComponents(n_jets, inputJets).tau();
+ }
+
+ /// Return all relevant information about tau components
+ TauComponents currentTauComponents() const {return _current_tau_components;}
+ /// Return axes found by getTauComponents.
+ std::vector<fastjet::PseudoJet> currentAxes() const { return _currentAxes;}
+ /// Return seedAxes used if onepass minimization (otherwise, same as currentAxes)
+ std::vector<fastjet::PseudoJet> seedAxes() const { return _seedAxes;}
+ /// Return jet partition found by getTauComponents.
+ std::vector<fastjet::PseudoJet> currentJets() const {return _currentPartition.jets();}
+ /// Return beam partition found by getTauComponents.
+ fastjet::PseudoJet currentBeam() const {return _currentPartition.beam();}
+ /// Return beam partition found by getTauComponents.
+ TauPartition currentPartition() const {return _currentPartition;}
+
+
+private:
+
+ /// AxesDefinition to use. Implemented as SharedPtrs to avoid memory management headaches
+ SharedPtr<const AxesDefinition> _axes_def;
+ /// MeasureDefinition to use. Implemented as SharedPtrs to avoid memory management headaches
+ SharedPtr<const MeasureDefinition> _measure_def;
+
+
+ // Information about the current information
+ // Defined as mutables, so user should be aware that these change when getTau is called.
+ // TODO: These are not thread safe and should be fixed somehow
+ mutable TauComponents _current_tau_components; //automatically set to have components of 0; these values will be set by the getTau function call
+ mutable std::vector<fastjet::PseudoJet> _currentAxes; //axes found after minimization
+ mutable std::vector<fastjet::PseudoJet> _seedAxes; // axes used prior to minimization (if applicable)
+ mutable TauPartition _currentPartition; //partitioning information
+
+ /// Warning if the user tries to use v1.0.3 measure style.
+ static LimitedWarning _old_measure_warning;
+ /// Warning if the user tries to use v1.0.3 axes style.
+ static LimitedWarning _old_axes_warning;
+
+
+public:
+
+ // These interfaces are included for backwards compability, and will be deprecated in a future release (scheduled for deletion in v3.0)
+
+ /// \deprecated
+ /// Deprecated enum to determine axes mode
+ /// The various axes choices available to the user
+ /// It is recommended to use AxesDefinition instead of these.
+ enum AxesMode {
+ kt_axes, // exclusive kt axes
+ ca_axes, // exclusive ca axes
+ antikt_0p2_axes, // inclusive hardest axes with antikt-0.2
+ wta_kt_axes, // Winner Take All axes with kt
+ wta_ca_axes, // Winner Take All axes with CA
+ onepass_kt_axes, // one-pass minimization from kt starting point
+ onepass_ca_axes, // one-pass minimization from ca starting point
+ onepass_antikt_0p2_axes, // one-pass minimization from antikt-0.2 starting point
+ onepass_wta_kt_axes, //one-pass minimization of WTA axes with kt
+ onepass_wta_ca_axes, //one-pass minimization of WTA axes with ca
+ min_axes, // axes that minimize N-subjettiness (100 passes by default)
+ manual_axes, // set your own axes with setAxes()
+ onepass_manual_axes // one-pass minimization from manual starting point
+ };
+
+ /// \deprecated
+ /// Deprecated enum to determine measure mode
+ /// The measures available to the user.
+ /// "normalized_cutoff_measure" was the default in v1.0 of Nsubjettiness
+ /// "unnormalized_measure" is now the recommended default usage
+ /// But it is recommended to use MeasureDefinition instead of these.
+ enum MeasureMode {
+ normalized_measure, //default normalized measure
+ unnormalized_measure, //default unnormalized measure
+ geometric_measure, //geometric measure
+ normalized_cutoff_measure, //default normalized measure with explicit Rcutoff
+ unnormalized_cutoff_measure, //default unnormalized measure with explicit Rcutoff
+ geometric_cutoff_measure //geometric measure with explicit Rcutoff
+ };
+
+ /// \deprecated
+ /// Intermediate constructor (needed to enable v1.0.3 backwards compatibility?)
+ Njettiness(AxesMode axes_mode, const MeasureDefinition & measure_def);
+
+ /// \deprecated
+ /// Old-style constructor which takes axes/measure information as enums with measure parameters
+ /// This version absolutely is not recommended
+ Njettiness(AxesMode axes_mode,
+ MeasureMode measure_mode,
+ int num_para,
+ double para1 = std::numeric_limits<double>::quiet_NaN(),
+ double para2 = std::numeric_limits<double>::quiet_NaN(),
+ double para3 = std::numeric_limits<double>::quiet_NaN())
+ : _axes_def(createAxesDef(axes_mode)), _measure_def(createMeasureDef(measure_mode, num_para, para1, para2, para3)) {
+ }
+
+ /// \deprecated
+ /// Convert old style enums into new style MeasureDefinition
+ AxesDefinition* createAxesDef(AxesMode axes_mode) const;
+
+ /// \deprecated
+ /// Convert old style enums into new style MeasureDefinition
+ MeasureDefinition* createMeasureDef(MeasureMode measure_mode, int num_para, double para1, double para2, double para3) const;
+
+};
+
+} // namespace Nsubjettiness
+
+}
+}
+
+#endif // __FASTJET_CONTRIB_NJETTINESS_HH__
diff --git a/include/Rivet/Tools/fjcontrib/NjettinessPlugin.hh b/include/Rivet/Tools/fjcontrib/NjettinessPlugin.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/NjettinessPlugin.hh
@@ -0,0 +1,182 @@
+// Nsubjettiness Package
+// Questions/Comments? jthaler@jthaler.net
+//
+// Copyright (c) 2011-14
+// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
+//
+// $Id: NjettinessPlugin.hh 822 2015-06-15 23:52:57Z jthaler $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_NJETTINESSPLUGIN_HH__
+#define __FASTJET_CONTRIB_NJETTINESSPLUGIN_HH__
+
+#include <fastjet/config.h>
+
+#include "Njettiness.hh"
+#include "MeasureDefinition.hh"
+#include "AxesDefinition.hh"
+#include "TauComponents.hh"
+
+#include "fastjet/ClusterSequence.hh"
+#include "fastjet/JetDefinition.hh"
+
+#include <string>
+#include <climits>
+
+namespace Rivet {
+namespace fjcontrib {
+
+namespace Nsubjettiness { using namespace fastjet;
+
+
+/// \class NjettinessPlugin
+/// \brief Implements the N-jettiness Jet Algorithm
+/**
+ * An exclusive jet finder that identifies N jets; first N axes are found, then
+ * particles are assigned to the nearest (DeltaR) axis and for each axis the
+ * corresponding jet is simply the four-momentum sum of these particles.
+ *
+ * As of version 2.2, it is recommended to use the XConePlugin, which has
+ * sensible default values for jet finding.
+ *
+ * Axes can be found in several ways, specified by the AxesDefinition argument.
+ * The recommended AxesDefinitions for jet finding (different than for jet shapes)
+ * OnePass_AntiKT(R0) : one-pass minimization from anti-kT starting point
+ * OnePass_GenET_GenKT_Axes(delta, p, R0) : one-pass min. from GenET/KT
+ * OnePass_WTA_GenKT_Axes(p, R0) : one-pass min from WTA/GenKT
+ * For recommendations on which axes to use, please see the README file.
+ *
+ * Jet regions are determined by the MeasureDefinition. The recommended choices
+ * for jet finding are
+ * ConicalMeasure(beta,R0) : perfect cones in rapidity/azimuth plane
+ * XConeMeasure(beta,R0) : approximate cones based on dot product distances.
+ *
+ * Other measures introduced in version 2.2 include OriginalGeometricMeasure,
+ * ModifiedGeometricMeasure, and ConicalGeometricMeasure, which define N-jettiness
+ * through dot products of particle momenta with light-like axes. OriginalGeometricMeasure
+ * produces football-shaped jets due to its central weighting of the beam measure,
+ * but ModifiedGeometric and ConicalGeometric both deform the original geometric measure
+ * to allow for cone-shaped jets. The size of these cones can be controlled through Rcutoff
+ * just as in the other measures. See the README file or MeasureDefinition.hh for information
+ * on how to call these measures.
+ *
+ */
+class NjettinessPlugin : public JetDefinition::Plugin {
+public:
+
+ /// Constructor with same arguments as Nsubjettiness (N, AxesDefinition, MeasureDefinition)
+ NjettinessPlugin(int N,
+ const AxesDefinition & axes_def,
+ const MeasureDefinition & measure_def)
+ : _njettinessFinder(axes_def, measure_def), _N(N) {}
+
+
+ /// Description
+ virtual std::string description () const;
+ /// Jet radius (this does not make sense yet)
+ virtual double R() const {return -1.0;} // TODO: make this not stupid
+
+ /// The actually clustering, which first called Njettiness and then creates a dummy ClusterSequence
+ virtual void run_clustering(ClusterSequence&) const;
+
+ /// For using manual axes with Njettiness Plugin
+ void setAxes(const std::vector<fastjet::PseudoJet> & myAxes) {
+ // Cross check that manual axes are being used is in Njettiness
+ _njettinessFinder.setAxes(myAxes);
+ }
+
+ /// Destructor
+ virtual ~NjettinessPlugin() {}
+
+private:
+
+ Njettiness _njettinessFinder; ///< The core Njettiness that does the heavy lifting
+ int _N; ///< Number of exclusive jets to find.
+
+ /// Warning if the user tries to use v1.0.3 constructor.
+ static LimitedWarning _old_constructor_warning;
+
+public:
+
+ // Alternative constructors that define the measure via enums and parameters
+ // These constructors are deprecated and will be removed in a future version.
+
+ /// \deprecated
+ /// Old-style constructor with 0 arguments (DEPRECATED)
+ NjettinessPlugin(int N,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode)
+ : _njettinessFinder(axes_mode, measure_mode, 0), _N(N) {
+ _old_constructor_warning.warn("NjettinessPlugin: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the NjettinessPlugin constructor based on AxesDefinition and MeasureDefinition instead.");
+ }
+
+ /// \deprecated
+ /// Old-style constructor with 1 argument (DEPRECATED)
+ NjettinessPlugin(int N,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode,
+ double para1)
+ : _njettinessFinder(axes_mode, measure_mode, 1, para1), _N(N) {
+ _old_constructor_warning.warn("NjettinessPlugin: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the NjettinessPlugin constructor based on AxesDefinition and MeasureDefinition instead.");
+
+ }
+
+ /// \deprecated
+ /// Old-style constructor with 2 arguments (DEPRECATED)
+ NjettinessPlugin(int N,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode,
+ double para1,
+ double para2)
+ : _njettinessFinder(axes_mode, measure_mode, 2, para1, para2), _N(N) {
+ _old_constructor_warning.warn("NjettinessPlugin: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the NjettinessPlugin constructor based on AxesDefinition and MeasureDefinition instead.");
+
+ }
+
+ /// \deprecated
+ /// Old-style constructor with 3 arguments (DEPRECATED)
+ NjettinessPlugin(int N,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode,
+ double para1,
+ double para2,
+ double para3)
+ : _njettinessFinder(axes_mode, measure_mode, 3, para1, para2, para3), _N(N) {
+ _old_constructor_warning.warn("NjettinessPlugin: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the NjettinessPlugin constructor based on AxesDefinition and MeasureDefinition instead.");
+ }
+
+ /// \deprecated
+ /// Old-style constructor for backwards compatibility with v1.0, when NormalizedCutoffMeasure was the only option
+ NjettinessPlugin(int N,
+ Njettiness::AxesMode mode,
+ double beta,
+ double R0,
+ double Rcutoff=std::numeric_limits<double>::max())
+ : _njettinessFinder(mode, NormalizedCutoffMeasure(beta, R0, Rcutoff)), _N(N) {
+ _old_constructor_warning.warn("NjettinessPlugin: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the NjettinessPlugin constructor based on AxesDefinition and MeasureDefinition instead.");
+ }
+
+
+};
+
+} // namespace Nsubjettiness
+
+}
+}
+
+#endif // __FASTJET_CONTRIB_NJETTINESSPLUGIN_HH__
diff --git a/include/Rivet/Tools/fjcontrib/Nsubjettiness.hh b/include/Rivet/Tools/fjcontrib/Nsubjettiness.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/Nsubjettiness.hh
@@ -0,0 +1,303 @@
+// Nsubjettiness Package
+// Questions/Comments? jthaler@jthaler.net
+//
+// Copyright (c) 2011-14
+// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
+//
+// $Id: Nsubjettiness.hh 822 2015-06-15 23:52:57Z jthaler $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_NSUBJETTINESS_HH__
+#define __FASTJET_CONTRIB_NSUBJETTINESS_HH__
+
+#include <fastjet/internal/base.hh>
+
+#include "Njettiness.hh"
+
+#include "fastjet/FunctionOfPseudoJet.hh"
+#include <string>
+#include <climits>
+
+namespace Rivet {
+namespace fjcontrib {
+
+namespace Nsubjettiness { using namespace fastjet;
+
+// Classes defined in this file.
+class Nsubjettiness;
+class NsubjettinessRatio;
+
+///------------------------------------------------------------------------
+/// \class Nsubjettiness
+/// \brief Implements the N-subjettiness jet shape
+///
+/**
+ * The N-jettiness jet shape.
+ *
+ * Nsubjettiness extends the concept of Njettiness to a jet shape, but other
+ * than the set of particles considered, they are identical. This class
+ * wraps the core Njettiness code to provide the fastjet::FunctionOfPseudoJet
+ * interface for convenience in larger analyses.
+ *
+ * The recommended AxesDefinitions are:
+ * KT_Axes : exclusive kt axes
+ * WTA_KT_Axes : exclusive kt with winner-take-all recombination
+ * OnePass_KT_Axes : one-pass minimization from kt starting point
+ * OnePass_WTA_KT_Axes : one-pass min. from wta_kt starting point
+ * More AxesDefinitions are listed in the README and defined in AxesDefinition.hh
+ *
+ * The recommended MeasureDefinitions are (with the corresponding parameters)
+ * NormalizedMeasure(beta,R0)
+ * : This was the original N-subjettiness measure (dimensionless)
+ * UnnormalizedMeasure(beta)
+ * : This is the new recommended default, same as above but without
+ * : the normalization factor, and hence has units of GeV
+ * NormalizedCutoffMeasure(beta,R0,Rcutoff)
+ * : Same as normalized_measure, but cuts off at Rcutoff
+ * UnnormalizedCutoffMeasure(beta,Rcutoff)
+ * : Same as unnormalized_measure, but cuts off at Rcutoff
+ * More MeasureDefinitions are listed in the README and defined in MeasureDefinition.hh
+ *
+ * For example, for the UnnormalizedMeasure(beta), N-subjettiness is defined as:
+ *
+ * tau_N = Sum_{i in jet} p_T^i min((DR_i1)^beta, (DR_i2)^beta, ...)
+ *
+ * DR_ij is the distance sqrt(Delta_phi^2 + Delta_rap^2) between particle i
+ * and jet j.
+ *
+ * The NormalizedMeausure include an extra parameter R0, and the various cutoff
+ * measures include an Rcutoff, which effectively defines an angular cutoff
+ * similar in effect to a cone-jet radius.
+ */
+class Nsubjettiness : public FunctionOfPseudoJet<double> {
+
+public:
+
+ /// Main constructor, which takes N, the AxesDefinition, and the MeasureDefinition.
+ /// The Definitions are given in AxesDefinition.hh and MeasureDefinition.hh
+ Nsubjettiness(int N,
+ const AxesDefinition& axes_def,
+ const MeasureDefinition& measure_def)
+ : _njettinessFinder(axes_def,measure_def), _N(N) {}
+
+ /// Returns tau_N, measured on the constituents of this jet
+ double result(const PseudoJet& jet) const;
+
+ /// Returns components of tau_N, so that user can find individual tau values.
+ TauComponents component_result(const PseudoJet& jet) const;
+
+ /// To set axes in manual mode
+ void setAxes(const std::vector<fastjet::PseudoJet> & myAxes) {
+ // Note that cross check that manual mode has been set is in Njettiness
+ _njettinessFinder.setAxes(myAxes);
+ }
+
+ /// returns seed axes used for onepass minimization (otherwise same as currentAxes)
+ std::vector<fastjet::PseudoJet> seedAxes() const {
+ return _njettinessFinder.seedAxes();
+ }
+
+ /// returns current axes found by result() calculation
+ std::vector<fastjet::PseudoJet> currentAxes() const {
+ return _njettinessFinder.currentAxes();
+ }
+
+ /// returns subjet regions found by result() calculation (these have valid constituents)
+ /// Note that the axes and the subjets are not the same
+ std::vector<fastjet::PseudoJet> currentSubjets() const {
+ return _njettinessFinder.currentJets();
+ }
+
+ /// returns components of tau_N without recalculating anything
+ TauComponents currentTauComponents() const {
+ return _njettinessFinder.currentTauComponents();
+ }
+
+ /// returns components of tau_N without recalculating anything
+ TauPartition currentPartition() const {
+ return _njettinessFinder.currentPartition();
+ }
+
+private:
+
+ /// Core Njettiness code that is called
+ Njettiness _njettinessFinder; // TODO: should muck with this so result can be const without this mutable
+ /// Number of subjets to find
+ int _N;
+
+ /// Warning if the user tries to use v1.0.3 constructor.
+ static LimitedWarning _old_constructor_warning;
+
+public:
+
+ // The following interfaces are included for backwards compatibility, but no longer recommended.
+ // They may be deleted in a future release
+
+ /// \deprecated
+ /// Alternative constructors that define the measure via enums and parameters
+ /// These constructors will be removed in v3.0
+ /// Zero parameter arguments
+ /// (Currently, no measure uses this)
+ Nsubjettiness(int N,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode)
+ : _njettinessFinder(axes_mode, measure_mode, 0), _N(N) {
+ _old_constructor_warning.warn("Nsubjettiness: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the Nsubjettiness constructor based on AxesDefinition and MeasureDefinition instead.");
+ }
+
+ /// \deprecated
+ /// Construcotr for one parameter argument
+ /// (for unnormalized_measure, para1=beta)
+ Nsubjettiness(int N,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode,
+ double para1)
+ : _njettinessFinder(axes_mode, measure_mode, 1, para1), _N(N) {
+ _old_constructor_warning.warn("Nsubjettiness: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the Nsubjettiness constructor based on AxesDefinition and MeasureDefinition instead.");
+ }
+
+ /// \deprecated
+ /// Constructor for two parameter arguments
+ /// (for normalized_measure, para1=beta, para2=R0)
+ /// (for unnormalized_cutoff_measure, para1=beta, para2=Rcutoff)
+ Nsubjettiness(int N,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode,
+ double para1,
+ double para2)
+ : _njettinessFinder(axes_mode, measure_mode, 2, para1, para2), _N(N) {
+ _old_constructor_warning.warn("Nsubjettiness: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the Nsubjettiness constructor based on AxesDefinition and MeasureDefinition instead.");
+ }
+
+ /// \deprecated
+ /// Constructor for three parameter arguments
+ /// (for unnormalized_cutoff_measure, para1=beta, para2=R0, para3=Rcutoff)
+ Nsubjettiness(int N,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode,
+ double para1,
+ double para2,
+ double para3)
+ : _njettinessFinder(axes_mode, measure_mode, 3, para1, para2, para3), _N(N) {
+ _old_constructor_warning.warn("Nsubjettiness: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the Nsubjettiness constructor based on AxesDefinition and MeasureDefinition instead.");
+ }
+
+ /// \deprecated
+ /// Old constructor for backwards compatibility with v1.0,
+ /// where normalized_cutoff_measure was the only option
+ Nsubjettiness(int N,
+ Njettiness::AxesMode axes_mode,
+ double beta,
+ double R0,
+ double Rcutoff=std::numeric_limits<double>::max())
+ : _njettinessFinder(axes_mode, NormalizedCutoffMeasure(beta,R0,Rcutoff)), _N(N) {
+ _old_constructor_warning.warn("Nsubjettiness: You are using the old style constructor. This is deprecated as of v2.1 and will be removed in v3.0. Please use the Nsubjettiness constructor based on AxesDefinition and MeasureDefinition instead.");
+ }
+
+};
+
+
+///------------------------------------------------------------------------
+/// \class NsubjettinessRatio
+/// \brief Implements ratios of N-subjettiness jet shapes
+///
+/// NsubjettinessRatio uses the results from Nsubjettiness to calculate the ratio
+/// tau_N/tau_M, where N and M are specified by the user. The ratio of different tau values
+/// is often used in analyses, so this class is helpful to streamline code. Note that
+/// manual axis mode is not supported
+class NsubjettinessRatio : public FunctionOfPseudoJet<double> {
+public:
+
+ /// Main constructor. Apart from specifying both N and M, the same options as Nsubjettiness
+ NsubjettinessRatio(int N,
+ int M,
+ const AxesDefinition & axes_def,
+ const MeasureDefinition & measure_def)
+ : _nsub_numerator(N,axes_def,measure_def),
+ _nsub_denominator(M,axes_def,measure_def) {
+ if (axes_def.needsManualAxes()) {
+ throw Error("NsubjettinessRatio does not support ManualAxes mode.");
+ }
+ }
+
+ /// Returns tau_N/tau_M based off the input jet using result function from Nsubjettiness
+ double result(const PseudoJet& jet) const;
+
+private:
+
+ Nsubjettiness _nsub_numerator; ///< Function for numerator
+ Nsubjettiness _nsub_denominator; ///< Function for denominator
+
+public:
+
+ // The following interfaces are included for backwards compatibility, but no longer recommended.
+ // They may be deprecated at some point.
+
+ /// \deprecated
+ /// Old-style constructor for zero arguments
+ /// Alternative constructor with enums and parameters
+ /// Again, likely to be removed
+ NsubjettinessRatio(int N,
+ int M,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode)
+ : _nsub_numerator(N, axes_mode, measure_mode),
+ _nsub_denominator(M, axes_mode, measure_mode) {}
+
+ /// \deprecated
+ /// Old-style constructor for one argument
+ NsubjettinessRatio(int N,
+ int M,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode,
+ double para1)
+ : _nsub_numerator(N, axes_mode, measure_mode, para1),
+ _nsub_denominator(M, axes_mode, measure_mode, para1) {}
+
+ /// \deprecated
+ /// Old-style constructor for 2 arguments
+ NsubjettinessRatio(int N,
+ int M,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode,
+ double para1,
+ double para2)
+ : _nsub_numerator(N, axes_mode, measure_mode, para1, para2),
+ _nsub_denominator(M, axes_mode, measure_mode, para1, para2) {}
+
+ /// \deprecated
+ /// Old-style constructor for 3 arguments
+ NsubjettinessRatio(int N,
+ int M,
+ Njettiness::AxesMode axes_mode,
+ Njettiness::MeasureMode measure_mode,
+ double para1,
+ double para2,
+ double para3)
+ : _nsub_numerator(N, axes_mode, measure_mode, para1, para2, para3),
+ _nsub_denominator(M, axes_mode, measure_mode, para1, para2, para3) {}
+
+
+};
+
+} // namespace Nsubjettiness
+
+}
+}
+
+#endif // __FASTJET_CONTRIB_NSUBJETTINESS_HH__
diff --git a/include/Rivet/Tools/fjcontrib/Recluster.hh b/include/Rivet/Tools/fjcontrib/Recluster.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/Recluster.hh
@@ -0,0 +1,187 @@
+#ifndef __FASTJET_CONTRIB_TOOLS_RECLUSTER_HH__
+#define __FASTJET_CONTRIB_TOOLS_RECLUSTER_HH__
+
+// $Id: Recluster.hh 723 2014-07-30 09:11:01Z gsoyez $
+//
+// Copyright (c) 2014-, Matteo Cacciari, Gavin P. Salam and Gregory Soyez
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <fastjet/JetDefinition.hh>
+#include <fastjet/CompositeJetStructure.hh> // to derive the ReclusterStructure from CompositeJetStructure
+#include <fastjet/tools/Transformer.hh> // to derive Recluster from Transformer
+#include <iostream>
+#include <string>
+
+//FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+ //namespace contrib{
+
+namespace Rivet {
+ namespace fjcontrib {
+ using namespace fastjet;
+
+//----------------------------------------------------------------------
+/// \class Recluster
+/// Class that helps reclustering a jet with a new jet definition
+///
+/// The result of the reclustering is returned as a single PseudoJet
+/// with a CompositeJet structure. The pieces of that PseudoJet will
+/// be the individual subjets
+///
+/// When constructed from a JetDefinition, that definition will be
+/// used to obtain the subjets. When constructed from a JetAlgorithm
+/// and parameters (0 parameters for e+e-, just R or R and an extra
+/// parameter for others) the recombination scheme will be taken as
+/// the same one used to initially cluster the original jet.
+///
+/// The result of this transformer depends on its usage. There are two
+/// typical use-cases: either we recluster one fat jet into subjets,
+/// OR, we recluster the jet with a different jet alg. When Recluster
+/// is created from a full jet definition. The last parameter of the
+/// constructors below dicatate that behaviour: if "single" is true
+/// (the default), a single jet, issued from a regular clustering is
+/// returned (if there are more than one, the hardest is taken);
+/// otherwise (single==false), the result will be a composite jet with
+/// each subjet as pieces
+///
+/// Open points for discussion:
+///
+/// - do we add an option to force area support? [could be useful
+/// e.g. for the filter with a subtractor where area support is
+/// mandatory]
+///
+class Recluster : public Transformer {
+public:
+ /// define a recluster that decomposes a jet into subjets using a
+ /// generic JetDefinition
+ ///
+ /// \param subjet_def the jet definition applied to obtain the subjets
+ /// \param single when true, cluster the jet in a single jet (the
+ /// hardest one) with an associated ClusterSequence,
+ /// otherwise return a composite jet with subjets
+ /// as pieces.
+ Recluster(const JetDefinition & subjet_def, bool single=true)
+ : _subjet_def(subjet_def), _use_full_def(true), _single(single) {}
+
+ /// define a recluster that decomposes a jet into subjets using a
+ /// JetAlgorithm and its parameters
+ ///
+ /// \param subjet_alg the jet algorithm applied to obtain the subjets
+ /// \param subjet_radius the jet radius if required
+ /// \param subjet_extra optional extra parameters for the jet algorithm (only when needed)
+ /// \param single when true, cluster the jet in a single jet (the
+ /// hardest one) with an associated ClusterSequence,
+ /// otherwise return a composite jet with subjets
+ /// as pieces.
+ ///
+ /// Typically, for e+e- algoriothm you should use the third version
+ /// below with no parameters, for "standard" pp algorithms, just the
+ /// clustering radius has to be specified and for genkt-type of
+ /// algorithms, both the radius and the extra parameter have to be
+ /// specified.
+ Recluster(JetAlgorithm subjet_alg, double subjet_radius, double subjet_extra,
+ bool single=true)
+ : _subjet_alg(subjet_alg), _use_full_def(false),
+ _subjet_radius(subjet_radius), _has_subjet_radius(true),
+ _subjet_extra(subjet_extra), _has_subjet_extra(true), _single(single) {}
+ Recluster(JetAlgorithm subjet_alg, double subjet_radius, bool single=true)
+ : _subjet_alg(subjet_alg), _use_full_def(false),
+ _subjet_radius(subjet_radius), _has_subjet_radius(true),
+ _has_subjet_extra(false), _single(single) {}
+ Recluster(JetAlgorithm subjet_alg, bool single=true)
+ : _subjet_alg(subjet_alg), _use_full_def(false),
+ _has_subjet_radius(false), _has_subjet_extra(false), _single(single) {}
+
+ /// default dtor
+ virtual ~Recluster(){};
+
+ //----------------------------------------------------------------------
+ // standard Transformer behaviour inherited from the base class
+ // (i.e. result(), description() and structural info)
+
+ /// runs the reclustering and sets kept and rejected to be the jets of interest
+ /// (with non-zero rho, they will have been subtracted).
+ ///
+ /// \param jet the jet that gets reclustered
+ /// \return the reclustered jet
+ virtual PseudoJet result(const PseudoJet & jet) const;
+
+ /// class description
+ virtual std::string description() const;
+
+ // the type of the associated structure
+ typedef CompositeJetStructure StructureType;
+
+private:
+ /// set the reclustered elements in the simple case of C/A+C/A
+ void _recluster_cafilt(const std::vector<PseudoJet> & all_pieces,
+ std::vector<PseudoJet> & subjets,
+ double Rfilt) const;
+
+ /// set the reclustered elements in the generic re-clustering case
+ void _recluster_generic(const PseudoJet & jet,
+ std::vector<PseudoJet> & subjets,
+ const JetDefinition & subjet_def,
+ bool do_areas) const;
+
+ // a series of checks
+ //--------------------------------------------------------------------
+ /// get the pieces down to the fundamental pieces
+ bool _get_all_pieces(const PseudoJet &jet, std::vector<PseudoJet> &all_pieces) const;
+
+ /// get the common recombiner to all pieces (NULL if none)
+ const JetDefinition::Recombiner* _get_common_recombiner(const std::vector<PseudoJet> &all_pieces) const;
+
+ /// construct the proper jet definition ensuring that the recombiner
+ /// is taken from the underlying pieces (an error is thrown if the
+ /// pieces do no share a common recombiner)
+ void _build_jet_def_with_recombiner(const std::vector<PseudoJet> &all_pieces,
+ JetDefinition &subjet_def) const;
+
+ /// check if one can apply the simplified trick for C/A subjets
+ bool _check_ca(const std::vector<PseudoJet> &all_pieces,
+ const JetDefinition &subjet_def) const;
+
+ /// check if the jet (or all its pieces) have explicit ghosts
+ /// (assuming the jet has area support
+ ///
+ /// Note that if the jet has an associated cluster sequence that is no
+ /// longer valid, an error will be thrown
+ bool _check_explicit_ghosts(const std::vector<PseudoJet> &all_pieces) const;
+
+ JetDefinition _subjet_def; ///< the jet definition to use to extract the subjets
+ JetAlgorithm _subjet_alg; ///< the jet algorithm to be used
+ bool _use_full_def; ///< true when the full JetDefinition is supplied to the ctor
+ double _subjet_radius; ///< the jet radius (only if needed for the jet alg)
+ bool _has_subjet_radius; ///< the subjet radius has been specified
+ double _subjet_extra; ///< the jet alg extra param (only if needed)
+ bool _has_subjet_extra; ///< the extra param has been specified
+
+ bool _single; ///< (true) return a single jet with a
+ ///< regular clustering or (false) a
+ ///< composite jet with subjets as pieces
+
+ static LimitedWarning _explicit_ghost_warning;
+};
+
+} } // namespace contrib
+
+ //FASTJET_END_NAMESPACE // defined in fastjet/internal/base.hh
+
+#endif // __FASTJET_CONTRIB_TOOLS_RECLUSTER_HH__
diff --git a/include/Rivet/Tools/fjcontrib/RecursiveSoftDrop.hh b/include/Rivet/Tools/fjcontrib/RecursiveSoftDrop.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/RecursiveSoftDrop.hh
@@ -0,0 +1,212 @@
+// $Id: RecursiveSoftDrop.hh 1082 2017-10-10 12:00:13Z gsoyez $
+//
+// Copyright (c) 2014-, Gavin P. Salam, Gregory Soyez, Jesse Thaler,
+// Kevin Zhou, Frederic Dreyer
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __RECURSIVESOFTDROP_HH__
+#define __RECURSIVESOFTDROP_HH__
+
+#include "Recluster.hh"
+#include "SoftDrop.hh"
+#include "fastjet/WrappedStructure.hh"
+
+#include <iostream>
+#include <queue>
+#include <vector>
+
+//FASTJET_BEGIN_NAMESPACE
+
+//namespace contrib{
+
+namespace Rivet {
+ namespace fjcontrib {
+ using namespace fastjet;
+
+
+//------------------------------------------------------------------------
+/// \class RecursiveSoftDrop
+/// An implementation of the RecursiveSoftDrop.
+///
+/// Recursive Soft Drop will recursively groom a jet, removing
+/// particles that fail the criterion
+/// \f[
+/// z > z_{\rm cut} (\theta/R0)^\beta
+/// \f]
+/// until n subjets have been found.
+///
+/// Several variants are supported:
+/// - set_fixed_depth_mode() switches to fixed depth on all branches
+/// of the clustering tree
+/// - set_dynamical_R0() switches to dynamical R0 implementation of
+/// RSD
+/// - set_hardest_branch_only() switches to following only the
+/// hardest branch (e.g. for Iterated Soft Drop)
+/// - set_min_deltaR_square(val) sets a minimum angle considered for
+/// substructure (e.g. for Iterated Soft Drop)
+///
+/// Notes:
+///
+/// - Even though the calls to "set_tagging_mode()" or
+/// "set_grooming_mode(false)" are allowed, they should not be used
+/// with n=-1, and the default grooming_mode has to remain
+/// untouched (except for beta<0 and finite n).
+///
+//----------------------------------------------------------------------
+class RecursiveSoftDrop : public SoftDrop {
+public:
+ /// Simplified constructor. This takes the value of the "beta"
+ /// parameter and the symmetry cut (applied by default on the
+ /// scalar_z variable, as for the mMDT). It also takes an optional
+ /// subtractor.
+ ///
+ /// n is the number of times we require the SoftDrop condition to be
+ /// satisfied. n=-1 means infinity, i.e. we recurse into the jet
+ /// until individual constituents
+ ///
+ /// If the (optional) pileup subtractor can be supplied, then see
+ /// also the documentation for the set_input_jet_is_subtracted() member
+ /// function.
+ ///
+ /// \param beta the value of the beta parameter
+ /// \param symmetry_cut the value of the cut on the symmetry measure
+ /// \param n the requested number of iterations
+ /// \param R0 the angular distance normalisation [1 by default]
+ RecursiveSoftDrop(double beta,
+ double symmetry_cut,
+ int n = -1,
+ double R0 = 1,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor = 0) :
+ SoftDrop(beta, symmetry_cut, R0, subtractor), _n(n) { set_defaults(); }
+
+ /// Full constructor, which takes the following parameters:
+ ///
+ /// \param beta the value of the beta parameter
+ /// \param symmetry_cut the value of the cut on the symmetry measure
+ /// \param symmetry_measure the choice of measure to use to estimate the symmetry
+ /// \param n the requested number of iterations
+ /// \param R0 the angular distance normalisation [1 by default]
+ /// \param mu_cut the maximal allowed value of mass drop variable mu = m_heavy/m_parent
+ /// \param recursion_choice the strategy used to decide which subjet to recurse into
+ /// \param subtractor an optional pointer to a pileup subtractor (ignored if zero)
+ RecursiveSoftDrop(double beta,
+ double symmetry_cut,
+ SymmetryMeasure symmetry_measure,
+ int n = -1,
+ double R0 = 1.0,
+ double mu_cut = std::numeric_limits<double>::infinity(),
+ RecursionChoice recursion_choice = larger_pt,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor = 0) :
+ SoftDrop(beta, symmetry_cut, symmetry_measure, R0, mu_cut, recursion_choice, subtractor),
+ _n(n) { set_defaults(); }
+
+ /// default destructor
+ virtual ~RecursiveSoftDrop(){}
+
+ //----------------------------------------------------------------------
+ // access to class info
+ int n() const { return _n; }
+
+ //----------------------------------------------------------------------
+ // on top of the tweaks that we inherit from SoftDrop (via
+ // RecursiveSymmetryBase):
+ // - set_verbose_structure()
+ // - set_subtractor()
+ // - set_input_jet_is_subtracted()
+ // we provide several other knobs, given below
+
+ /// initialise all the flags below to their default value
+ void set_defaults();
+
+ /// switch to using the "same depth" variant where instead of
+ /// recursing from large to small angles and requiring n SD
+ /// conditions to be met (our default), we recurse simultaneously in
+ /// all the branches found during the previous iteration, up to a
+ /// maximum depth of n.
+ /// default: false
+ void set_fixed_depth_mode(bool value=true) { _fixed_depth = value; }
+ bool fixed_depth_mode() const { return _fixed_depth; }
+
+ /// switch to using a dynamical R0 (used for the normalisation of
+ /// the symmetry measure) set by the last deltaR at which some
+ /// substructure was found.
+ /// default: false
+ void set_dynamical_R0(bool value=true) { _dynamical_R0 = value; }
+ bool use_dynamical_R0() const { return _dynamical_R0; }
+
+ /// when finding some substructure, only follow the hardest branch
+ /// for the recursion
+ /// default: false (i.e. recurse in both branches)
+ void set_hardest_branch_only(bool value=true) { _hardest_branch_only = value; }
+ bool use_hardest_branch_only() const { return _hardest_branch_only; }
+
+ /// set the minimum angle (squared) that we should consider for
+ /// substructure
+ /// default: -1.0 (i.e. no minimum)
+ void set_min_deltaR_squared(double value=-1.0) { _min_dR2 = value; }
+ double min_deltaR_squared() const { return _min_dR2; }
+
+ /// description of the tool
+ virtual std::string description() const;
+
+ //----------------------------------------------------------------------
+ /// action on a single jet with RecursiveSoftDrop.
+ ///
+ /// uses "result_fixed_tags" by default (i.e. recurse from R0 to
+ /// smaller angles until n SD conditions have been met), or
+ /// "result_fixed_depth" where each of the previous SD branches are
+ /// recirsed into down to a depth of n.
+ virtual PseudoJet result(const PseudoJet &jet) const;
+
+ /// this routine applies the Soft Drop criterion recursively on the
+ /// CA tree until we find n subjets (or until it converges), and
+ /// adds them together into a groomed PseudoJet
+ PseudoJet result_fixed_tags(const PseudoJet &jet) const;
+
+ /// this routine applies the Soft Drop criterion recursively on the
+ /// CA tree, recursing into all the branches found during the previous iteration
+ /// until n layers have been found (or until it converges)
+ PseudoJet result_fixed_depth(const PseudoJet &jet) const;
+
+protected:
+ /// return false if we reached desired layer of grooming _n
+ bool continue_grooming(int current_n) const {
+ return ((_n < 0) or (current_n < _n));
+ }
+
+private:
+ int _n; ///< the value of n
+
+ // behaviour tweaks
+ bool _fixed_depth; ///< look in parallel into each all branches until depth n
+ bool _dynamical_R0; ///< when true, use the last deltaR with substructure as D0
+ bool _hardest_branch_only; ///< recurse only in the hardest branch
+ /// when substructure is found
+ double _min_dR2; ///< the min allowed angle to search for substructure
+};
+
+// helper to get the (linear) list of prongs inside a jet resulting
+// from RecursiveSoftDrop. This would avoid having amnually to go
+// through the successive pairwise compositeness
+std::vector<PseudoJet> recursive_soft_drop_prongs(const PseudoJet & rsd_jet);
+
+} }
+
+ //FASTJET_END_NAMESPACE // defined in fastjet/internal/base.hh
+#endif // __RECURSIVESOFTDROP_HH__
diff --git a/include/Rivet/Tools/fjcontrib/RecursiveSymmetryCutBase.hh b/include/Rivet/Tools/fjcontrib/RecursiveSymmetryCutBase.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/RecursiveSymmetryCutBase.hh
@@ -0,0 +1,392 @@
+// $Id: RecursiveSymmetryCutBase.hh 1074 2017-09-18 15:15:20Z gsoyez $
+//
+// Copyright (c) 2014-, Gavin P. Salam, Gregory Soyez, Jesse Thaler
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_RECURSIVESYMMETRYCUTBASE_HH__
+#define __FASTJET_CONTRIB_RECURSIVESYMMETRYCUTBASE_HH__
+
+#include <limits>
+#include <cassert>
+#include <fastjet/internal/base.hh>
+#include "fastjet/tools/Transformer.hh"
+#include "fastjet/WrappedStructure.hh"
+#include "fastjet/CompositeJetStructure.hh"
+
+#include "fastjet/config.h"
+
+// we'll use the native FJ class for reculstering if available
+#if FASTJET_VERSION_NUMBER >= 30100
+#include "fastjet/tools/Recluster.hh"
+#else
+#include "Recluster.hh"
+#endif
+
+/** \mainpage RecursiveTools contrib
+
+ The RecursiveTools contrib provides a set of tools for
+ recursive investigation jet substructure. Currently it includes:
+ - fastjet::contrib::ModifiedMassDropTagger
+ - fastjet::contrib::SoftDrop
+ - fastjet::contrib::RecursiveSymmetryCutBase (from which the above two classes derive)
+ - fastjet::contrib::IteratedSoftDropSymmetryFactors (defines ISD procedure)
+ - fastjet::contrib::IteratedSoftDropMultiplicity (defines a useful observable using ISD)
+ - example*.cc provides usage examples
+ */
+
+
+//FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+ //namespace contrib{
+
+namespace Rivet {
+ namespace fjcontrib {
+ using namespace fastjet;
+
+
+//------------------------------------------------------------------------
+/// \class RecursiveSymmetryCutBase
+/// A base class for all the tools that de-cluster a jet until a
+/// sufficiently symmetric configuration if found.
+///
+/// Derived classes (so far, ModifiedMassDropTagger and SoftDrop) have to
+/// implement the symmetry cut and its description
+///
+/// Note that by default, the jet will be reculstered with
+/// Cambridge/Aachen before applying the de-clustering procedure. This
+/// behaviour can be changed using set_clustering (see below).
+///
+/// By default, this class behaves as a tagger, i.e. returns an empty
+/// PseudoJet if no substructure is found. While the derived
+/// ModifiedMassDropTagger is a tagger, the derived SoftDrop is a groomer
+/// (i.e. it returns a non-zero jet even if no substructure is found).
+///
+/// This class provides support for
+/// - an optional mass-drop cut (see ctor)
+/// - options to select which symmetry measure should be used (see ctor)
+/// - options to select how the recursion proceeds (see ctor)
+/// - options for reclustering the jet before running the de-clustering
+/// (see set_reclustering)
+/// - an optional subtractor (see ctor and other methods below)
+class RecursiveSymmetryCutBase : public Transformer {
+public:
+ // ctors and dtors
+ //----------------------------------------------------------------------
+
+ /// an enum of the different (a)symmetry measures that can be used
+ enum SymmetryMeasure{scalar_z, ///< \f$ \min(p_{ti}, p_{tj})/(p_{ti} + p_{tj}) \f$
+ vector_z, ///< \f$ \min(p_{ti}, p_{tj})/p_{t(i+j)} \f$
+ y, ///< \f$ \min(p_{ti}^2,p_{tj}^2) \Delta R_{ij}^2 / m_{ij}^2 \f$
+ theta_E, ///< \f$ \min(E_i,E_j)/(E_i+E_j) \f$ with 3d angle (ee collisions)
+ cos_theta_E ///< \f$ \min(E_i,E_j)/(E_i+E_j) \f$ with
+ /// \f$ \sqrt{2[1-cos(theta)]}\f$ for angles (ee collisions)
+ };
+
+ /// an enum for the options of how to choose which of two subjets to recurse into
+ enum RecursionChoice{larger_pt, ///< choose the subjet with larger \f$ p_t \f$
+ larger_mt, ///< choose the subjet with larger \f$ m_t \equiv (m^2+p_t^2)^{\frac12}] \f$
+ larger_m, ///< choose the subjet with larger mass (deprecated)
+ larger_E ///< choose the subjet with larger energy (meant for ee collisions)
+ };
+
+ /// Full constructor, which takes the following parameters:
+ ///
+ /// \param symmetry_measure the choice of measure to use to estimate the symmetry
+ /// \param mu_cut the maximal allowed value of mass drop variable mu = m_heavy/m_parent
+ /// \param recursion_choice the strategy used to decide which subjet to recurse into
+ /// \param subtractor an optional pointer to a pileup subtractor (ignored if zero)
+ ///
+ /// If the (optional) pileup subtractor is supplied, then, by
+ /// default, the input jet is assumed unsubtracted and the
+ /// RecursiveSymmetryCutBase returns a subtracted 4-vector. [see
+ /// also the set_input_jet_is_subtracted() member function].
+ ///
+ RecursiveSymmetryCutBase(SymmetryMeasure symmetry_measure = scalar_z,
+ double mu_cut = std::numeric_limits<double>::infinity(),
+ RecursionChoice recursion_choice = larger_pt,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor = 0
+ ) :
+ _symmetry_measure(symmetry_measure),
+ _mu_cut(mu_cut),
+ _recursion_choice(recursion_choice),
+ _subtractor(subtractor), _input_jet_is_subtracted(false),
+ _do_reclustering(true), _recluster(0),
+ _grooming_mode(false),
+ _verbose_structure(false) // by default, don't story verbose information
+ {}
+
+ /// default destructor
+ virtual ~RecursiveSymmetryCutBase(){}
+
+ // access to class info
+ //----------------------------------------------------------------------
+ SymmetryMeasure symmetry_measure() const { return _symmetry_measure; }
+ double mu_cut() const { return _mu_cut; }
+ RecursionChoice recursion_choice() const { return _recursion_choice; }
+
+ // internal subtraction configuration
+ //----------------------------------------------------------------------
+
+ /// This tells the tagger whether to assume that the input jet has
+ /// already been subtracted. This is relevant only if a non-null
+ /// subtractor pointer has been supplied, and the default assymption
+ /// is that the input jet is passed unsubtracted.
+ ///
+ /// Note: given that subtractors usually change the momentum of the
+ /// main jet, but not that of the subjets, subjets will continue to
+ /// have subtraction applied to them.
+ void set_input_jet_is_subtracted(bool is_subtracted) {_input_jet_is_subtracted = is_subtracted;}
+
+ /// returns a bool to indicate if the input jet is assumed already subtracted
+ bool input_jet_is_subtracted() const {return _input_jet_is_subtracted;}
+
+ /// an alternative way to set the subtractor
+ ///
+ /// Note that when a subtractor is provided, the result of the
+ /// RecursiveSymmetryCutBase will be a subtracted jet.
+ void set_subtractor(const FunctionOfPseudoJet<PseudoJet> * subtractor_) {_subtractor = subtractor_;}
+
+ /// returns a pointer to the subtractor
+ const FunctionOfPseudoJet<PseudoJet> * subtractor() const {return _subtractor;}
+
+ // reclustering behaviour
+ //----------------------------------------------------------------------
+
+ /// configure the reclustering prior to the recursive de-clustering
+ /// \param do_reclustering recluster the jet or not?
+ /// \param recluster how to recluster the jet
+ /// (only if do_recluster is true;
+ /// Cambridge/Aachen used if NULL)
+ ///
+ /// Note that the ModifiedMassDropTagger and SoftDrop are designed
+ /// to work with a Cambridge/Aachen clustering. Use any other option
+ /// at your own risk!
+ void set_reclustering(bool do_reclustering=true, const Recluster *recluster=0){
+ _do_reclustering = do_reclustering;
+ _recluster = recluster;
+ }
+
+ // what to do when no substructure is found
+ //----------------------------------------------------------------------
+ /// specify the behaviour adopted when no substructure is found
+ /// - in tagging mode, an empty PseudoJet will be returned
+ /// - in grooming mode, a single particle is returned
+ /// for clarity, we provide both function although they are redundant
+ void set_grooming_mode(bool enable=true){ _grooming_mode = enable;}
+ void set_tagging_mode(bool enable=true){ _grooming_mode = !enable;}
+
+
+ /// Allows access to verbose information about recursive declustering,
+ /// in particular values of symmetry, delta_R, and mu of dropped branches
+ void set_verbose_structure(bool enable=true) { _verbose_structure = enable; }
+ bool has_verbose_structure() const { return _verbose_structure; }
+
+
+ // inherited from the Transformer base
+ //----------------------------------------------------------------------
+
+ /// the function that carries out the tagging; if a subtractor is
+ /// being used, then this function assumes that input jet is
+ /// unsubtracted (unless set_input_jet_is_subtracted(true) has been
+ /// explicitly called before) and the result of the MMDT will be a
+ /// subtracted jet.
+ virtual PseudoJet result(const PseudoJet & j) const;
+
+ /// description of the tool
+ virtual std::string description() const;
+
+ /// returns the gepometrical distance between the two particles
+ /// depending on the symmetry measure used
+ double squared_geometric_distance(const PseudoJet &j1,
+ const PseudoJet &j2) const;
+
+
+ class StructureType;
+
+ /// for testing
+ static bool _verbose;
+
+protected:
+ // the methods below have to be defined by deerived classes
+ //----------------------------------------------------------------------
+ /// the cut on the symmetry measure (typically z) that one need to
+ /// apply for a given pair of subjets p1 and p2
+ virtual double symmetry_cut_fn(const PseudoJet & /* p1 */,
+ const PseudoJet & /* p2 */,
+ void *extra_parameters = 0) const = 0;
+ /// the associated dwescription
+ virtual std::string symmetry_cut_description() const = 0;
+
+ //----------------------------------------------------------------------
+ /// this defines status codes when checking for substructure
+ enum RecursionStatus{
+ recursion_success=0, //< found some substructure
+ recursion_dropped, //< dropped softest prong; recursion continues
+ recursion_no_parents, //< down to constituents; bottom of recursion
+ recursion_issue //< something went wrong; recursion stops
+ };
+
+ //----------------------------------------------------------------------
+ /// the method below is the one actually performing one step of the
+ /// recursion.
+ ///
+ /// It returns a status code (defined above)
+ ///
+ /// In case of success, all the information is filled
+ /// In case of "no parents", piee1 is the same subjet
+ /// In case of trouble, piece2 will be a 0 PJ and piece1 is the PJ we
+ /// should return (either 0 itself if the issue was critical, or
+ /// non-wero in case of a minor issue just causing the recursion to
+ /// stop)
+ ///
+ /// The extra_parameter argument allows one to pass extra agruments
+ /// to the symmetry condition
+ RecursionStatus recurse_one_step(const PseudoJet & subjet,
+ PseudoJet &piece1, PseudoJet &piece2,
+ double &sym, double &mu2,
+ void *extra_parameters = 0) const;
+
+ //----------------------------------------------------------------------
+ /// helper for handling the reclustering
+ PseudoJet _recluster_if_needed(const PseudoJet &jet) const;
+
+ //----------------------------------------------------------------------
+ // helpers for selecting between ee and pp cases
+ bool is_ee() const{
+ return ((_symmetry_measure==theta_E) || (_symmetry_measure==cos_theta_E));
+ }
+
+private:
+ SymmetryMeasure _symmetry_measure;
+ double _mu_cut;
+ RecursionChoice _recursion_choice;
+ const FunctionOfPseudoJet<PseudoJet> * _subtractor;
+ bool _input_jet_is_subtracted;
+
+ bool _do_reclustering; ///< start with a reclustering
+ const Recluster *_recluster; ///< how to recluster the jet
+
+ bool _grooming_mode; ///< grooming or tagging mode
+
+ static LimitedWarning _negative_mass_warning;
+ static LimitedWarning _mu2_gt1_warning;
+ //static LimitedWarning _nonca_warning;
+ static LimitedWarning _explicit_ghost_warning;
+
+ // additional verbose structure information
+ bool _verbose_structure;
+
+ /// decide what to return when no substructure has been found
+ PseudoJet _result_no_substructure(const PseudoJet &last_parent) const;
+};
+
+
+
+//----------------------------------------------------------------------
+/// class to hold the structure of a jet tagged by RecursiveSymmetryCutBase.
+class RecursiveSymmetryCutBase::StructureType : public WrappedStructure {
+public:
+ StructureType(const PseudoJet & j) :
+ WrappedStructure(j.structure_shared_ptr()), _delta_R(-1.0), _symmetry(-1.0), _mu(-1.0),
+ _is_composite(false), _has_verbose(false) // by default, do not store verbose structure
+ {}
+
+ /// construct a structure with
+ /// - basic info inherited from the reference jet "j"
+ /// - a given deltaR for substructure
+ /// - a given symmetry for substructure
+ /// - a given mu parameter for substructure
+ /// If j is a "copmposite jet", it means that it has further
+ /// substructure to potentially recurse into
+ StructureType(const PseudoJet & j, double delta_R_in, double symmetry_in, double mu_in=-1.0) :
+ WrappedStructure(j.structure_shared_ptr()), _delta_R(delta_R_in), _symmetry(symmetry_in), _mu(mu_in),
+ _is_composite(dynamic_cast<const CompositeJetStructure*>(j.structure_ptr()) != NULL),
+ _has_verbose(false) // by default, do not store verbose structure
+ {}
+
+ // information about kept branch
+ double delta_R() const {return _delta_R;}
+ double thetag() const {return _delta_R;} // alternative name
+ double symmetry() const {return _symmetry;}
+ double zg() const {return _symmetry;} // alternative name
+ double mu() const {return _mu;}
+
+ // additional verbose information about dropped branches
+ bool has_verbose() const { return _has_verbose;}
+ void set_verbose(bool value) { _has_verbose = value;}
+
+ /// returns true if the current jet has some substructure (i.e. has
+ /// been tagged by the resursion) or not
+ ///
+ /// Note that this should include deltaR==0 (e.g. a perfectly
+ /// collinear branching with SoftDrop)
+ bool has_substructure() const { return _delta_R>=0; }
+
+ /// number of dropped branches
+ int dropped_count(bool global=true) const;
+
+ /// delta_R of dropped branches
+ /// when "global" is set, recurse into possile further substructure
+ std::vector<double> dropped_delta_R(bool global=true) const;
+ void set_dropped_delta_R(const std::vector<double> &v) { _dropped_delta_R = v; }
+
+ /// symmetry values of dropped branches
+ std::vector<double> dropped_symmetry(bool global=true) const;
+ void set_dropped_symmetry(const std::vector<double> &v) { _dropped_symmetry = v; }
+
+ /// mass drop values of dropped branches
+ std::vector<double> dropped_mu(bool global=true) const;
+ void set_dropped_mu(const std::vector<double> &v) { _dropped_mu = v; }
+
+ /// maximum symmetry value dropped
+ double max_dropped_symmetry(bool global=true) const;
+
+ /// (global) list of groomed away elements as zg and thetag
+ /// sorted from largest to smallest anlge
+ std::vector<std::pair<double,double> > sorted_zg_and_thetag() const;
+
+private:
+ double _delta_R, _symmetry, _mu;
+ friend class RecursiveSymmetryCutBase;
+
+ bool _is_composite;
+
+ // additional verbose information
+ bool _has_verbose;
+ // information about dropped values
+ std::vector<double> _dropped_delta_R;
+ std::vector<double> _dropped_symmetry;
+ std::vector<double> _dropped_mu;
+
+ bool check_verbose(const std::string &what) const{
+ if (!_has_verbose){
+ throw Error("RecursiveSymmetryCutBase::StructureType: Verbose structure must be turned on to get "+what+".");
+ return false;
+ }
+ return true;
+ }
+
+
+};
+
+} } // namespace contrib
+
+ //FASTJET_END_NAMESPACE
+
+#endif // __FASTJET_CONTRIB_RECURSIVESYMMETRYCUTBASE_HH__
diff --git a/include/Rivet/Tools/fjcontrib/SoftDrop.hh b/include/Rivet/Tools/fjcontrib/SoftDrop.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/SoftDrop.hh
@@ -0,0 +1,152 @@
+// $Id: SoftDrop.hh 1034 2017-08-01 10:03:53Z gsoyez $
+//
+// Copyright (c) 2014-, Gregory Soyez, Jesse Thaler
+// based on arXiv:1402.2657 by Andrew J. Larkoski, Simone Marzani,
+// Gregory Soyez, Jesse Thaler
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_SOFTDROP_HH__
+#define __FASTJET_CONTRIB_SOFTDROP_HH__
+
+#include "RecursiveSymmetryCutBase.hh"
+
+//FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+
+namespace Rivet {
+ namespace fjcontrib {
+ using namespace fastjet;
+
+
+//------------------------------------------------------------------------
+/// \class SoftDrop
+/// An implementation of the SoftDrop from arXiv:1402.2657.
+///
+/// For the basic functionalities, we refer the reader to the
+/// documentation of the RecursiveSymmetryCutBase from which SoftDrop
+/// inherits. Here, we mostly put the emphasis on things specific to
+/// SoftDrop:
+///
+/// - the cut applied recursively is
+/// \f[
+/// z > z_{\rm cut} (\theta/R0)^\beta
+/// \f]
+/// with z the asymmetry measure and \f$\theta\f$ the geometrical
+/// distance between the two subjets. R0 is set to 1 by default.
+///
+/// - by default, we work in "grooming mode" i.s. if no substructure
+/// is found, we return a jet made of a single parton. Note that
+/// this behaviour differs from the mMDT (and can be a source of
+/// differences when running SoftDrop with beta=0.)
+///
+class SoftDrop : public RecursiveSymmetryCutBase {
+public:
+ /// Simplified constructor. This takes the value of the "beta"
+ /// parameter and the symmetry cut (applied by default on the
+ /// scalar_z variable, as for the mMDT). It also takes an optional
+ /// subtractor.
+ ///
+ /// If the (optional) pileup subtractor can be supplied, then see
+ /// also the documentation for the set_input_jet_is_subtracted() member
+ /// function.
+ ///
+ /// \param beta the value of the beta parameter
+ /// \param symmetry_cut the value of the cut on the symmetry measure
+ /// \param R0 the angular distance normalisation [1 by default]
+ SoftDrop(double beta,
+ double symmetry_cut,
+ double R0 = 1,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor = 0) :
+ RecursiveSymmetryCutBase(scalar_z, // the default SymmetryMeasure
+ std::numeric_limits<double>::infinity(), // default is no mass drop
+ larger_pt, // the default RecursionChoice
+ subtractor),
+ _beta(beta), _symmetry_cut(symmetry_cut), _R0sqr(R0*R0) {
+ // change the default: use grooming mode
+ set_grooming_mode();
+ }
+
+ /// Full constructor, which takes the following parameters:
+ ///
+ /// \param beta the value of the beta parameter
+ /// \param symmetry_cut the value of the cut on the symmetry measure
+ /// \param symmetry_measure the choice of measure to use to estimate the symmetry
+ /// \param R0 the angular distance normalisation [1 by default]
+ /// \param mu_cut the maximal allowed value of mass drop variable mu = m_heavy/m_parent
+ /// \param recursion_choice the strategy used to decide which subjet to recurse into
+ /// \param subtractor an optional pointer to a pileup subtractor (ignored if zero)
+ ///
+ /// The default values provided for this constructor are suited to
+ /// obtain the SoftDrop as discussed in arXiv:1402.2657:
+ /// - no mass drop is requested
+ /// - recursion follows the branch with the largest pt
+ /// The symmetry measure has to be specified (scalar_z is the recommended value)
+ ///
+ /// Notes:
+ ///
+ /// - by default, SoftDrop will recluster the jet with the
+ /// Cambridge/Aachen algorithm if it is not already the case. This
+ /// behaviour can be changed using the "set_reclustering" method
+ /// defined below
+ ///
+ SoftDrop(double beta,
+ double symmetry_cut,
+ SymmetryMeasure symmetry_measure,
+ double R0 = 1.0,
+ double mu_cut = std::numeric_limits<double>::infinity(),
+ RecursionChoice recursion_choice = larger_pt,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor = 0) :
+ RecursiveSymmetryCutBase(symmetry_measure, mu_cut, recursion_choice, subtractor),
+ _beta(beta), _symmetry_cut(symmetry_cut), _R0sqr(R0*R0)
+ {
+ // change the default: use grooming mode
+ set_grooming_mode();
+ }
+
+ /// default destructor
+ virtual ~SoftDrop(){}
+
+ //----------------------------------------------------------------------
+ // access to class info
+ double beta() const { return _beta; }
+ double symmetry_cut() const { return _symmetry_cut; }
+ double R0() const { return sqrt(_R0sqr); }
+
+protected:
+
+ // Unlike MMDT, the SoftDrop symmetry_cut_fn depends on the subjet kinematics
+ // since the symmetry condition depends on the DeltaR between subjets.
+ virtual double symmetry_cut_fn(const PseudoJet & p1,
+ const PseudoJet & p2,
+ void * optional_R0sqr_ptr = 0) const;
+ virtual std::string symmetry_cut_description() const;
+
+ //private:
+ double _beta; ///< the power of the angular distance to be used
+ ///< in the symmetry condition
+ double _symmetry_cut; ///< the value of zcut (the prefactor in the asymmetry cut)
+ double _R0sqr; ///< normalisation of the angular distance
+ ///< (typically set to the jet radius, 1 by default)
+};
+
+} } // namespace contrib
+
+ //FASTJET_END_NAMESPACE
+
+#endif // __FASTJET_CONTRIB_SOFTDROP_HH__
diff --git a/include/Rivet/Tools/fjcontrib/TauComponents.hh b/include/Rivet/Tools/fjcontrib/TauComponents.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/TauComponents.hh
@@ -0,0 +1,354 @@
+// Nsubjettiness Package
+// Questions/Comments? jthaler@jthaler.net
+//
+// Copyright (c) 2011-14
+// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
+//
+// $Id: MeasureFunction.hh 742 2014-08-23 15:43:29Z jthaler $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_TAUCOMPONENTS_HH__
+#define __FASTJET_CONTRIB_TAUCOMPONENTS_HH__
+
+#include "fastjet/PseudoJet.hh"
+#include "fastjet/ClusterSequence.hh"
+#include "fastjet/WrappedStructure.hh"
+
+
+#include <cmath>
+#include <vector>
+#include <list>
+#include <limits>
+
+
+namespace Rivet {
+namespace fjcontrib {
+
+namespace Nsubjettiness { using namespace fastjet;
+
+// Classes defined in this file.
+class TauComponents;
+class TauPartition;
+class NjettinessExtras;
+
+///------------------------------------------------------------------------
+/// \enum TauMode
+/// Specified whether tau value has beam region or denominators
+///------------------------------------------------------------------------
+enum TauMode {
+ UNDEFINED_SHAPE = -1, // Added so that constructor would default to some value
+ UNNORMALIZED_JET_SHAPE = 0,
+ NORMALIZED_JET_SHAPE = 1,
+ UNNORMALIZED_EVENT_SHAPE = 2,
+ NORMALIZED_EVENT_SHAPE = 3,
+};
+
+///////
+//
+// TauComponents
+//
+///////
+
+///------------------------------------------------------------------------
+/// \class TauComponents
+/// \brief Output wrapper for supplemental N-(sub)jettiness information
+///
+/// This class creates a wrapper for the various tau/subtau values calculated in Njettiness. This class allows Njettiness access to these variables
+/// without ever having to do the calculation itself. It takes in subtau numerators and tau denominator from MeasureFunction
+/// and outputs tau numerator, and normalized tau and subtau.
+///------------------------------------------------------------------------
+class TauComponents {
+
+public:
+
+ /// empty constructor necessary to initialize tau_components in Njettiness
+ /// later set correctly in Njettiness::getTau function
+ TauComponents() {}
+
+ /// This constructor takes input vector and double and calculates all necessary tau components
+ TauComponents(TauMode tau_mode,
+ const std::vector<double> & jet_pieces_numerator,
+ double beam_piece_numerator,
+ double denominator,
+ const std::vector<PseudoJet> & jets,
+ const std::vector<PseudoJet> & axes
+ );
+
+ /// Test for denominator
+ bool has_denominator() const;
+ /// Test for beam region
+ bool has_beam() const;
+
+ /// Return tau value
+ double tau() const { return _tau; }
+ /// Return jet regions
+ const std::vector<double>& jet_pieces() const { return _jet_pieces; }
+ /// Return beam region
+ double beam_piece() const { return _beam_piece; }
+
+ /// Return jet regions (no denominator)
+ std::vector<double> jet_pieces_numerator() const { return _jet_pieces_numerator; }
+ /// Return beam regions (no denominator)
+ double beam_piece_numerator() const { return _beam_piece_numerator; }
+ /// Return numerator
+ double numerator() const { return _numerator; }
+ /// Return denominator
+ double denominator() const { return _denominator; }
+
+ /// Four-vector of total jet (sum of clustered regions)
+ PseudoJet total_jet() const { return _total_jet;}
+ /// Four-vector of jet regions
+ const std::vector<PseudoJet>& jets() const { return _jets;}
+ /// Four-vector of axes
+ const std::vector<PseudoJet>& axes() const { return _axes;}
+
+ class StructureType;
+
+protected:
+
+ /// Defines whether there is a beam or denominator
+ TauMode _tau_mode;
+
+ std::vector<double> _jet_pieces_numerator; ///< Constructor input (jet region numerator)
+ double _beam_piece_numerator; ///< Constructor input (beam region numerator)
+ double _denominator; ///< Constructor input (denominator)
+
+ std::vector<double> _jet_pieces; ///< Derived value (jet regions)
+ double _beam_piece; ///< Derived value (beam region)
+ double _numerator; ///< Derived value (total numerator)
+ double _tau; ///< Derived value (final value)
+
+ PseudoJet _total_jet; ///< Total jet four-vector
+ std::vector<PseudoJet> _jets; ///< Jet four-vectors
+ std::vector<PseudoJet> _axes; ///< AXes four-vectors
+
+};
+
+///////
+//
+// TauPartition
+//
+///////
+
+///------------------------------------------------------------------------
+/// \class TauPartition
+/// \brief Output wrapper for N-(sub)jettiness partitioning information
+///
+/// Class for storing partitioning information.
+///------------------------------------------------------------------------
+class TauPartition {
+
+public:
+ /// empty constructor
+ TauPartition() {}
+
+ /// Make partition of size to hold n_jet partitions
+ TauPartition(int n_jet) {
+ _jets_list.resize(n_jet);
+ _jets_partition.resize(n_jet);
+ }
+
+ /// add a particle to the jet
+ void push_back_jet(int jet_num, const PseudoJet& part_to_add, int part_index) {
+ _jets_list[jet_num].push_back(part_index);
+ _jets_partition[jet_num].push_back(part_to_add);
+ }
+
+ /// add a particle to the beam
+ void push_back_beam(const PseudoJet& part_to_add, int part_index) {
+ _beam_list.push_back(part_index);
+ _beam_partition.push_back(part_to_add);
+ }
+
+ /// return jet regions
+ PseudoJet jet(int jet_num) const { return join(_jets_partition.at(jet_num)); }
+ /// return beam region
+ PseudoJet beam() const { return join(_beam_partition);}
+
+ /// return jets
+ std::vector<PseudoJet> jets() const {
+ std::vector<PseudoJet> jets;
+ for (unsigned int i = 0; i < _jets_partition.size(); i++) {
+ jets.push_back(jet(i));
+ }
+ return jets;
+ }
+
+ /// jets in list form
+ const std::list<int> & jet_list(int jet_num) const { return _jets_list.at(jet_num);}
+ /// beam in list form
+ const std::list<int> & beam_list() const { return _beam_list;}
+ /// all jets in list form
+ const std::vector<std::list<int> > & jets_list() const { return _jets_list;}
+
+private:
+
+ std::vector<std::list<int> > _jets_list; ///< jets in list form
+ std::list<int> _beam_list; ///< beam in list form
+
+ std::vector<std::vector<PseudoJet> > _jets_partition; ///< Partition in jet regions
+ std::vector<PseudoJet> _beam_partition; ///< Partition in beam region
+
+};
+
+
+///////
+//
+// NjettinessExtras
+//
+///////
+
+///------------------------------------------------------------------------
+/// \class NjettinessExtras
+/// \brief ClusterSequence add on for N-jettiness information
+///
+/// This class contains the same information as TauComponents, but adds additional ways of linking up
+/// the jets found in the ClusterSequence::Extras class.
+/// This is done in order to help improve the interface for the main NjettinessPlugin class.
+///------------------------------------------------------------------------
+class NjettinessExtras : public ClusterSequence::Extras, public TauComponents {
+
+public:
+ /// Constructor
+ NjettinessExtras(TauComponents tau_components,
+ std::vector<int> cluster_hist_indices)
+ : TauComponents(tau_components), _cluster_hist_indices(cluster_hist_indices) {}
+
+
+
+ /// Ask for tau of the whole event, but by querying a jet
+ double tau(const fastjet::PseudoJet& /*jet*/) const {return _tau;}
+
+ /// Ask for tau of an individual jet
+ double tau_piece(const fastjet::PseudoJet& jet) const {
+ if (labelOf(jet) == -1) return std::numeric_limits<double>::quiet_NaN(); // nonsense
+ return _jet_pieces[labelOf(jet)];
+ }
+
+ /// Find axis associated with jet
+ fastjet::PseudoJet axis(const fastjet::PseudoJet& jet) const {
+ return _axes[labelOf(jet)];
+ }
+
+ /// Check if extra information is available.
+ bool has_njettiness_extras(const fastjet::PseudoJet& jet) const {
+ return (labelOf(jet) >= 0);
+ }
+
+private:
+
+ /// Store cluster history indices to link up with ClusterSequence
+ std::vector<int> _cluster_hist_indices;
+
+ /// Figure out which jet things belonged to
+ int labelOf(const fastjet::PseudoJet& jet) const {
+ int thisJet = -1;
+ for (unsigned int i = 0; i < _jets.size(); i++) {
+ if (_cluster_hist_indices[i] == jet.cluster_hist_index()) {
+ thisJet = i;
+ break;
+ }
+ }
+ return thisJet;
+ }
+
+public:
+
+ // These are old methods for gaining this information
+ // The recommended interface is given in TauComponents
+
+ /// Tau value
+ double totalTau() const {return _tau;}
+ /// Jet regions
+ std::vector<double> subTaus() const {return _jet_pieces;}
+
+ /// Tau value
+ double totalTau(const fastjet::PseudoJet& /*jet*/) const {
+ return _tau;
+ }
+
+ /// Jet region
+ double subTau(const fastjet::PseudoJet& jet) const {
+ if (labelOf(jet) == -1) return std::numeric_limits<double>::quiet_NaN(); // nonsense
+ return _jet_pieces[labelOf(jet)];
+ }
+
+ /// beam region
+ double beamTau() const {
+ return _beam_piece;
+ }
+
+};
+
+
+/// Helper function to find out what njettiness_extras are (from jet)
+inline const NjettinessExtras * njettiness_extras(const fastjet::PseudoJet& jet) {
+ const ClusterSequence * myCS = jet.associated_cluster_sequence();
+ if (myCS == NULL) return NULL;
+ const NjettinessExtras* extras = dynamic_cast<const NjettinessExtras*>(myCS->extras());
+ return extras;
+}
+
+/// Helper function to find out what njettiness_extras are (from ClusterSequence)
+inline const NjettinessExtras * njettiness_extras(const fastjet::ClusterSequence& myCS) {
+ const NjettinessExtras* extras = dynamic_cast<const NjettinessExtras*>(myCS.extras());
+ return extras;
+}
+
+///////
+//
+// TauComponents::StructureType
+//
+///////
+
+
+///------------------------------------------------------------------------
+/// \class TauComponents::StructureType
+/// \brief Wrapped structure for jet-based N-(sub)jettiness information
+///
+/// Small wrapped structure to store tau information
+/// TODO: Can these be auto-joined?
+///------------------------------------------------------------------------
+class TauComponents::StructureType : public WrappedStructure {
+
+public:
+ /// Constructor
+ StructureType(const PseudoJet& j) :
+ WrappedStructure(j.structure_shared_ptr())
+ {}
+
+ /// tau associated with jet
+ double tau_piece() const { return _tau_piece; }
+
+ /// alternative call, though might be confusing
+ double tau() const { return _tau_piece; }
+
+private:
+ friend class TauComponents;
+ double _tau_piece; ///< tau value associated with jet
+};
+
+
+
+
+} //namespace Nsubjettiness
+
+}
+}
+
+#endif // __FASTJET_CONTRIB_TAUCOMPONENTS_HH__
diff --git a/include/Rivet/Tools/fjcontrib/XConePlugin.hh b/include/Rivet/Tools/fjcontrib/XConePlugin.hh
new file mode 100644
--- /dev/null
+++ b/include/Rivet/Tools/fjcontrib/XConePlugin.hh
@@ -0,0 +1,170 @@
+// Nsubjettiness Package
+// Questions/Comments? jthaler@jthaler.net
+//
+// Copyright (c) 2011-14
+// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
+//
+// $Id: XConePlugin.hh 748 2014-10-02 06:13:28Z tjwilk $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#ifndef __FASTJET_CONTRIB_XCONEPLUGIN_HH__
+#define __FASTJET_CONTRIB_XCONEPLUGIN_HH__
+
+#include <fastjet/config.h>
+
+#include "NjettinessPlugin.hh"
+
+#include "fastjet/ClusterSequence.hh"
+#include "fastjet/JetDefinition.hh"
+
+#include <string>
+#include <climits>
+
+namespace Rivet {
+namespace fjcontrib {
+
+namespace Nsubjettiness { using namespace fastjet;
+
+///------------------------------------------------------------------------
+/// \class XConePlugin
+/// \brief Implements the XCone Jet Algorithm
+/**
+ * An exclusive jet finder that identifies N jets. First N axes are found, then
+ * particles are assigned to the nearest (approximte DeltaR) axis and for each axis the
+ * corresponding jet is simply the four-momentum sum of these particles.
+ *
+ * The XConePlugin is based on NjettinessPlugin, but with sensible default
+ * values for the AxesDefinition and MeasureDefinition. There are three arguments
+ *
+ * int N: number of exclusive jets to be found
+ * double R0: approximate jet radius
+ * double beta: determines style of jet finding with the recommended values being:
+ * beta = 2: standard "mean" jets where jet momentum/axis align approximately.
+ * beta = 1: recoil-free "median" variant where jet axis points at hardest cluster.
+ *
+ * The AxesDefinition is OnePass_GenET_GenKT_Axes, which uses a generalized kT
+ * clustering algorithm matched to the beta value.
+ *
+ * The MeasureDefinition is the XConeMeasure, which is based on the
+ * ConicalGeometric measure.
+ */
+class XConePlugin : public NjettinessPlugin {
+public:
+
+ /// Constructor with N, R0, and beta as the options. beta = 2.0 is the default
+ /// All this does is use the NjettinessPlugin with OnePass_GenET_GenKT_Axes and the XConeMeasure.
+ /// For more advanced usage, call NjettinessPlugin directly
+ /// Note that the order of the R0 and beta values is reversed from the XConeMeasure to
+ /// standard usage for Plugins.
+ XConePlugin(int N, double R0, double beta = 2.0)
+ : NjettinessPlugin(N,
+ OnePass_GenET_GenKT_Axes(calc_delta(beta), calc_power(beta), R0), // use recommended axes method only
+ XConeMeasure(beta, R0) // use recommended XCone measure.
+ ),
+ _N(N), _R0(R0), _beta(beta)
+ {}
+
+ // The things that are required by base class.
+ virtual std::string description () const;
+ virtual double R() const {return _R0;}
+
+ // run_clustering is done by NjettinessPlugin
+
+ virtual ~XConePlugin() {}
+
+private:
+
+ /// Static call used within the constructor to set the recommended delta value
+ static double calc_delta(double beta) {
+ double delta;
+ if (beta > 1) delta = 1/(beta - 1);
+ else delta = std::numeric_limits<int>::max(); // use winner take all
+ return delta;
+ }
+
+ /// Static call used within the constructor to set the recommended p value
+ static double calc_power(double beta) {
+ return (double) 1.0/beta;
+ }
+
+ double _N; ///< Number of desired jets
+ double _R0; ///< Jet radius
+ double _beta; ///< Angular exponent (beta = 2.0 is dafault, beta = 1.0 is recoil-free)
+
+public:
+
+};
+
+
+/// \class PseudoXConePlugin
+/// \brief Implements a faster, non-optimal version of the XCone Jet Algorithm
+///
+/// A "poor man's" version of XCone with no minimization step
+/// Right now, used just for testing purposes by the developers
+class PseudoXConePlugin : public NjettinessPlugin {
+public:
+
+ /// Constructor with N, R0, and beta as the options. beta = 2.0 is the default
+ /// All this does is use the NjettinessPlugin with GenET_GenKT_Axes and the XConeMeasure.
+ PseudoXConePlugin(int N, double R0, double beta = 2.0)
+ : NjettinessPlugin(N,
+ GenET_GenKT_Axes(calc_delta(beta), calc_power(beta), R0), // poor man's axes
+ XConeMeasure(beta, R0) // use recommended XCone measure.
+ ),
+ _N(N), _R0(R0), _beta(beta)
+ {}
+
+ // The things that are required by base class.
+ virtual std::string description () const;
+ virtual double R() const {return _R0;}
+
+ // run_clustering is done by NjettinessPlugin
+
+ virtual ~PseudoXConePlugin() {}
+
+private:
+
+ /// Static call used within the constructor to set the recommended delta value
+ static double calc_delta(double beta) {
+ double delta;
+ if (beta > 1) delta = 1/(beta - 1);
+ else delta = std::numeric_limits<int>::max(); // use winner take all
+ return delta;
+ }
+
+ /// Static call used within the constructor to set the recommended p value
+ static double calc_power(double beta) {
+ return (double) 1.0/beta;
+ }
+
+ double _N; ///< Number of desired jets
+ double _R0; ///< Jet radius
+ double _beta; ///< Angular exponent (beta = 2.0 is dafault, beta = 1.0 is recoil-free)
+
+public:
+
+};
+
+
+
+} // namespace Nsubjettiness
+
+}
+}
+
+#endif // __FASTJET_CONTRIB_XConePlugin_HH__
diff --git a/src/Core/Analysis.cc b/src/Core/Analysis.cc
--- a/src/Core/Analysis.cc
+++ b/src/Core/Analysis.cc
@@ -1,936 +1,964 @@
// -*- C++ -*-
#include "Rivet/Config/RivetCommon.hh"
#include "Rivet/Analysis.hh"
#include "Rivet/AnalysisHandler.hh"
#include "Rivet/AnalysisInfo.hh"
#include "Rivet/Tools/BeamConstraint.hh"
#include "Rivet/Projections/ImpactParameterProjection.hh"
#include "Rivet/Projections/GeneratedPercentileProjection.hh"
#include "Rivet/Projections/UserCentEstimate.hh"
#include "Rivet/Projections/CentralityProjection.hh"
namespace Rivet {
Analysis::Analysis(const string& name)
: _crossSection(-1.0),
_gotCrossSection(false),
_analysishandler(NULL)
{
ProjectionApplier::_allowProjReg = false;
_defaultname = name;
unique_ptr<AnalysisInfo> ai = AnalysisInfo::make(name);
assert(ai);
_info = move(ai);
assert(_info);
}
double Analysis::sqrtS() const {
return handler().sqrtS();
}
const ParticlePair& Analysis::beams() const {
return handler().beams();
}
const PdgIdPair Analysis::beamIds() const {
return handler().beamIds();
}
const string Analysis::histoDir() const {
/// @todo Cache in a member variable
string _histoDir;
if (_histoDir.empty()) {
_histoDir = "/" + name();
if (handler().runName().length() > 0) {
_histoDir = "/" + handler().runName() + _histoDir;
}
replace_all(_histoDir, "//", "/"); //< iterates until none
}
return _histoDir;
}
const string Analysis::histoPath(const string& hname) const {
const string path = histoDir() + "/" + hname;
return path;
}
const string Analysis::histoPath(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const {
return histoDir() + "/" + mkAxisCode(datasetId, xAxisId, yAxisId);
}
const string Analysis::mkAxisCode(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId) const {
stringstream axisCode;
axisCode << "d";
if (datasetId < 10) axisCode << 0;
axisCode << datasetId;
axisCode << "-x";
if (xAxisId < 10) axisCode << 0;
axisCode << xAxisId;
axisCode << "-y";
if (yAxisId < 10) axisCode << 0;
axisCode << yAxisId;
return axisCode.str();
}
Log& Analysis::getLog() const {
string logname = "Rivet.Analysis." + name();
return Log::getLog(logname);
}
///////////////////////////////////////////
size_t Analysis::numEvents() const {
return handler().numEvents();
}
double Analysis::sumW() const {
return handler().sumW();
}
double Analysis::sumW2() const {
return handler().sumW2();
}
///////////////////////////////////////////
bool Analysis::isCompatible(const ParticlePair& beams) const {
return isCompatible(beams.first.pid(), beams.second.pid(),
beams.first.energy(), beams.second.energy());
}
bool Analysis::isCompatible(PdgId beam1, PdgId beam2, double e1, double e2) const {
PdgIdPair beams(beam1, beam2);
pair<double,double> energies(e1, e2);
return isCompatible(beams, energies);
}
+ // bool Analysis::beamIDsCompatible(const PdgIdPair& beams) const {
+ // bool beamIdsOk = false;
+ // for (const PdgIdPair& bp : requiredBeams()) {
+ // if (compatible(beams, bp)) {
+ // beamIdsOk = true;
+ // break;
+ // }
+ // }
+ // return beamIdsOk;
+ // }
+
+
+ // /// Check that the energies are compatible (within 1% or 1 GeV, whichever is larger, for a bit of UI forgiveness)
+ // bool Analysis::beamEnergiesCompatible(const pair<double,double>& energies) const {
+ // /// @todo Use some sort of standard ordering to improve comparisons, esp. when the two beams are different particles
+ // bool beamEnergiesOk = requiredEnergies().size() > 0 ? false : true;
+ // typedef pair<double,double> DoublePair;
+ // for (const DoublePair& ep : requiredEnergies()) {
+ // if ((fuzzyEquals(ep.first, energies.first, 0.01) && fuzzyEquals(ep.second, energies.second, 0.01)) ||
+ // (fuzzyEquals(ep.first, energies.second, 0.01) && fuzzyEquals(ep.second, energies.first, 0.01)) ||
+ // (abs(ep.first - energies.first) < 1*GeV && abs(ep.second - energies.second) < 1*GeV) ||
+ // (abs(ep.first - energies.second) < 1*GeV && abs(ep.second - energies.first) < 1*GeV)) {
+ // beamEnergiesOk = true;
+ // break;
+ // }
+ // }
+ // return beamEnergiesOk;
+ // }
+
+
+ // bool Analysis::beamsCompatible(const PdgIdPair& beams, const pair<double,double>& energies) const {
bool Analysis::isCompatible(const PdgIdPair& beams, const pair<double,double>& energies) const {
// First check the beam IDs
bool beamIdsOk = false;
for (const PdgIdPair& bp : requiredBeams()) {
if (compatible(beams, bp)) {
beamIdsOk = true;
break;
}
}
if (!beamIdsOk) return false;
// Next check that the energies are compatible (within 1% or 1 GeV, whichever is larger, for a bit of UI forgiveness)
/// @todo Use some sort of standard ordering to improve comparisons, esp. when the two beams are different particles
bool beamEnergiesOk = requiredEnergies().size() > 0 ? false : true;
typedef pair<double,double> DoublePair;
for (const DoublePair& ep : requiredEnergies()) {
if ((fuzzyEquals(ep.first, energies.first, 0.01) && fuzzyEquals(ep.second, energies.second, 0.01)) ||
(fuzzyEquals(ep.first, energies.second, 0.01) && fuzzyEquals(ep.second, energies.first, 0.01)) ||
(abs(ep.first - energies.first) < 1*GeV && abs(ep.second - energies.second) < 1*GeV) ||
(abs(ep.first - energies.second) < 1*GeV && abs(ep.second - energies.first) < 1*GeV)) {
beamEnergiesOk = true;
break;
}
}
return beamEnergiesOk;
-
- /// @todo Need to also check internal consistency of the analysis'
- /// beam requirements with those of the projections it uses.
}
///////////////////////////////////////////
Analysis& Analysis::setCrossSection(double xs) {
_crossSection = xs;
_gotCrossSection = true;
return *this;
}
double Analysis::crossSection() const {
if (!_gotCrossSection || std::isnan(_crossSection)) {
string errMsg = "You did not set the cross section for the analysis " + name();
throw Error(errMsg);
}
return _crossSection;
}
double Analysis::crossSectionPerEvent() const {
const double sumW = sumOfWeights();
assert(sumW != 0.0);
return _crossSection / sumW;
}
////////////////////////////////////////////////////////////
// Histogramming
void Analysis::_cacheRefData() const {
if (_refdata.empty()) {
MSG_TRACE("Getting refdata cache for paper " << name());
_refdata = getRefData(getRefDataName());
}
}
vector<AnalysisObjectPtr> Analysis::getAllData(bool includeorphans) const{
return handler().getData(includeorphans);
}
CounterPtr Analysis::bookCounter(const string& cname,
const string& title) {
return addOrGetCompatAO(make_shared<Counter>(histoPath(cname), title));
}
CounterPtr Analysis::bookCounter(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
const string& title) {
return bookCounter(mkAxisCode(datasetId, xAxisId, yAxisId), title);
}
Histo1DPtr Analysis::bookHisto1D(const string& hname,
size_t nbins, double lower, double upper,
const string& title,
const string& xtitle,
const string& ytitle) {
Histo1DPtr hist = make_shared<Histo1D>(nbins, lower, upper, histoPath(hname), title);
hist->setTitle(title);
hist->setAnnotation("XLabel", xtitle);
hist->setAnnotation("YLabel", ytitle);
return addOrGetCompatAO(hist);
}
Histo1DPtr Analysis::bookHisto1D(const string& hname,
const vector<double>& binedges,
const string& title,
const string& xtitle,
const string& ytitle) {
Histo1DPtr hist = make_shared<Histo1D>(binedges, histoPath(hname), title);
hist->setTitle(title);
hist->setAnnotation("XLabel", xtitle);
hist->setAnnotation("YLabel", ytitle);
return addOrGetCompatAO(hist);
}
Histo1DPtr Analysis::bookHisto1D(const string& hname,
const initializer_list<double>& binedges,
const string& title,
const string& xtitle,
const string& ytitle) {
return bookHisto1D(hname, vector<double>{binedges}, title, xtitle, ytitle);
}
Histo1DPtr Analysis::bookHisto1D(const string& hname,
const Scatter2D& refscatter,
const string& title,
const string& xtitle,
const string& ytitle) {
Histo1DPtr hist = make_shared<Histo1D>(refscatter, histoPath(hname));
hist->setTitle(title);
hist->setAnnotation("XLabel", xtitle);
hist->setAnnotation("YLabel", ytitle);
return addOrGetCompatAO(hist);
}
Histo1DPtr Analysis::bookHisto1D(const string& hname,
const string& title,
const string& xtitle,
const string& ytitle) {
const Scatter2D& refdata = refData(hname);
return bookHisto1D(hname, refdata, title, xtitle, ytitle);
}
Histo1DPtr Analysis::bookHisto1D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
const string& title,
const string& xtitle,
const string& ytitle) {
const string axisCode = mkAxisCode(datasetId, xAxisId, yAxisId);
return bookHisto1D(axisCode, title, xtitle, ytitle);
}
/// @todo Add booking methods which take a path, titles and *a reference Scatter from which to book*
/////////////////
Histo2DPtr Analysis::bookHisto2D(const string& hname,
size_t nxbins, double xlower, double xupper,
size_t nybins, double ylower, double yupper,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle)
{
const string path = histoPath(hname);
Histo2DPtr hist = make_shared<Histo2D>(nxbins, xlower, xupper, nybins, ylower, yupper, path, title);
hist->setAnnotation("XLabel", xtitle);
hist->setAnnotation("YLabel", ytitle);
hist->setAnnotation("ZLabel", ztitle);
return addOrGetCompatAO(hist);
}
Histo2DPtr Analysis::bookHisto2D(const string& hname,
const vector<double>& xbinedges,
const vector<double>& ybinedges,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle)
{
const string path = histoPath(hname);
Histo2DPtr hist = make_shared<Histo2D>(xbinedges, ybinedges, path, title);
hist->setAnnotation("XLabel", xtitle);
hist->setAnnotation("YLabel", ytitle);
hist->setAnnotation("ZLabel", ztitle);
return addOrGetCompatAO(hist);
}
Histo2DPtr Analysis::bookHisto2D(const string& hname,
const initializer_list<double>& xbinedges,
const initializer_list<double>& ybinedges,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle)
{
return bookHisto2D(hname, vector<double>{xbinedges}, vector<double>{ybinedges},
title, xtitle, ytitle, ztitle);
}
Histo2DPtr Analysis::bookHisto2D(const string& hname,
const Scatter3D& refscatter,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle) {
const string path = histoPath(hname);
Histo2DPtr hist( new Histo2D(refscatter, path) );
if (hist->hasAnnotation("IsRef")) hist->rmAnnotation("IsRef");
hist->setTitle(title);
hist->setAnnotation("XLabel", xtitle);
hist->setAnnotation("YLabel", ytitle);
hist->setAnnotation("ZLabel", ztitle);
return addOrGetCompatAO(hist);
}
Histo2DPtr Analysis::bookHisto2D(const string& hname,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle) {
const Scatter3D& refdata = refData<Scatter3D>(hname);
return bookHisto2D(hname, refdata, title, xtitle, ytitle, ztitle);
}
Histo2DPtr Analysis::bookHisto2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle) {
const string axisCode = mkAxisCode(datasetId, xAxisId, yAxisId);
return bookHisto2D(axisCode, title, xtitle, ytitle, ztitle);
}
/////////////////
Profile1DPtr Analysis::bookProfile1D(const string& hname,
size_t nbins, double lower, double upper,
const string& title,
const string& xtitle,
const string& ytitle) {
const string path = histoPath(hname);
Profile1DPtr prof = make_shared<Profile1D>(nbins, lower, upper, path, title);
prof->setAnnotation("XLabel", xtitle);
prof->setAnnotation("YLabel", ytitle);
return addOrGetCompatAO(prof);
}
Profile1DPtr Analysis::bookProfile1D(const string& hname,
const vector<double>& binedges,
const string& title,
const string& xtitle,
const string& ytitle) {
const string path = histoPath(hname);
Profile1DPtr prof = make_shared<Profile1D>(binedges, path, title);
prof->setAnnotation("XLabel", xtitle);
prof->setAnnotation("YLabel", ytitle);
return addOrGetCompatAO(prof);
}
Profile1DPtr Analysis::bookProfile1D(const string& hname,
const initializer_list<double>& binedges,
const string& title,
const string& xtitle,
const string& ytitle)
{
return bookProfile1D(hname, vector<double>{binedges}, title, xtitle, ytitle);
}
Profile1DPtr Analysis::bookProfile1D(const string& hname,
const Scatter2D& refscatter,
const string& title,
const string& xtitle,
const string& ytitle) {
const string path = histoPath(hname);
Profile1DPtr prof = make_shared<Profile1D>(refscatter, path);
if (prof->hasAnnotation("IsRef")) prof->rmAnnotation("IsRef");
prof->setTitle(title);
prof->setAnnotation("XLabel", xtitle);
prof->setAnnotation("YLabel", ytitle);
return addOrGetCompatAO(prof);
}
Profile1DPtr Analysis::bookProfile1D(const string& hname,
const string& title,
const string& xtitle,
const string& ytitle) {
const Scatter2D& refdata = refData(hname);
return bookProfile1D(hname, refdata, title, xtitle, ytitle);
}
Profile1DPtr Analysis::bookProfile1D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
const string& title,
const string& xtitle,
const string& ytitle) {
const string axisCode = mkAxisCode(datasetId, xAxisId, yAxisId);
return bookProfile1D(axisCode, title, xtitle, ytitle);
}
///////////////////
Profile2DPtr Analysis::bookProfile2D(const string& hname,
size_t nxbins, double xlower, double xupper,
size_t nybins, double ylower, double yupper,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle)
{
const string path = histoPath(hname);
Profile2DPtr prof = make_shared<Profile2D>(nxbins, xlower, xupper, nybins, ylower, yupper, path, title);
prof->setAnnotation("XLabel", xtitle);
prof->setAnnotation("YLabel", ytitle);
prof->setAnnotation("ZLabel", ztitle);
return addOrGetCompatAO(prof);
}
Profile2DPtr Analysis::bookProfile2D(const string& hname,
const vector<double>& xbinedges,
const vector<double>& ybinedges,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle)
{
const string path = histoPath(hname);
Profile2DPtr prof = make_shared<Profile2D>(xbinedges, ybinedges, path, title);
prof->setAnnotation("XLabel", xtitle);
prof->setAnnotation("YLabel", ytitle);
prof->setAnnotation("ZLabel", ztitle);
return addOrGetCompatAO(prof);
}
Profile2DPtr Analysis::bookProfile2D(const string& hname,
const initializer_list<double>& xbinedges,
const initializer_list<double>& ybinedges,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle)
{
return bookProfile2D(hname, vector<double>{xbinedges}, vector<double>{ybinedges},
title, xtitle, ytitle, ztitle);
}
Profile2DPtr Analysis::bookProfile2D(const string& hname,
const Scatter3D& refscatter,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle) {
const string path = histoPath(hname);
Profile2DPtr prof( new Profile2D(refscatter, path) );
if (prof->hasAnnotation("IsRef")) prof->rmAnnotation("IsRef");
prof->setTitle(title);
prof->setAnnotation("XLabel", xtitle);
prof->setAnnotation("YLabel", ytitle);
prof->setAnnotation("ZLabel", ztitle);
return addOrGetCompatAO(prof);
}
Profile2DPtr Analysis::bookProfile2D(const string& hname,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle) {
const Scatter3D& refdata = refData<Scatter3D>(hname);
return bookProfile2D(hname, refdata, title, xtitle, ytitle, ztitle);
}
Profile2DPtr Analysis::bookProfile2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
const string& title,
const string& xtitle,
const string& ytitle,
const string& ztitle) {
const string axisCode = mkAxisCode(datasetId, xAxisId, yAxisId);
return bookProfile2D(axisCode, title, xtitle, ytitle, ztitle);
}
/////////////////
Scatter2DPtr Analysis::bookScatter2D(unsigned int datasetId, unsigned int xAxisId, unsigned int yAxisId,
bool copy_pts,
const string& title,
const string& xtitle,
const string& ytitle) {
const string axisCode = mkAxisCode(datasetId, xAxisId, yAxisId);
return bookScatter2D(axisCode, copy_pts, title, xtitle, ytitle);
}
Scatter2DPtr Analysis::bookScatter2D(const string& hname,
bool copy_pts,
const string& title,
const string& xtitle,
const string& ytitle) {
Scatter2DPtr s;
const string path = histoPath(hname);
if (copy_pts) {
const Scatter2D& refdata = refData(hname);
s = make_shared<Scatter2D>(refdata, path);
for (Point2D& p : s->points()) p.setY(0, 0);
} else {
s = make_shared<Scatter2D>(path);
}
if (s->hasAnnotation("IsRef")) s->rmAnnotation("IsRef");
s->setTitle(title);
s->setAnnotation("XLabel", xtitle);
s->setAnnotation("YLabel", ytitle);
return addOrGetCompatAO(s);
}
Scatter2DPtr Analysis::bookScatter2D(const string& hname,
size_t npts, double lower, double upper,
const string& title,
const string& xtitle,
const string& ytitle) {
const string path = histoPath(hname);
Scatter2DPtr s = make_shared<Scatter2D>(path);
const double binwidth = (upper-lower)/npts;
for (size_t pt = 0; pt < npts; ++pt) {
const double bincentre = lower + (pt + 0.5) * binwidth;
s->addPoint(bincentre, 0, binwidth/2.0, 0);
}
s->setTitle(title);
s->setAnnotation("XLabel", xtitle);
s->setAnnotation("YLabel", ytitle);
return addOrGetCompatAO(s);
}
Scatter2DPtr Analysis::bookScatter2D(const string& hname,
const vector<double>& binedges,
const string& title,
const string& xtitle,
const string& ytitle) {
const string path = histoPath(hname);
Scatter2DPtr s = make_shared<Scatter2D>(path);
for (size_t pt = 0; pt < binedges.size()-1; ++pt) {
const double bincentre = (binedges[pt] + binedges[pt+1]) / 2.0;
const double binwidth = binedges[pt+1] - binedges[pt];
s->addPoint(bincentre, 0, binwidth/2.0, 0);
}
s->setTitle(title);
s->setAnnotation("XLabel", xtitle);
s->setAnnotation("YLabel", ytitle);
return addOrGetCompatAO(s);
}
Scatter2DPtr Analysis::bookScatter2D(const Scatter2DPtr scPtr,
const std::string& path, const std::string& title,
const std::string& xtitle, const std::string& ytitle ) {
Scatter2DPtr s = make_shared<Scatter2D>(*scPtr);
s->setPath(path);
s->setTitle(title);
s->setAnnotation("XLabel",xtitle);
s->setAnnotation("YLabel",ytitle);
return addOrGetCompatAO(s);
}
/////////////////////
void Analysis::divide(CounterPtr c1, CounterPtr c2, Scatter1DPtr s) const {
const string path = s->path();
*s = *c1 / *c2;
s->setPath(path);
}
void Analysis::divide(const Counter& c1, const Counter& c2, Scatter1DPtr s) const {
const string path = s->path();
*s = c1 / c2;
s->setPath(path);
}
void Analysis::divide(Histo1DPtr h1, Histo1DPtr h2, Scatter2DPtr s) const {
const string path = s->path();
*s = *h1 / *h2;
s->setPath(path);
}
void Analysis::divide(const Histo1D& h1, const Histo1D& h2, Scatter2DPtr s) const {
const string path = s->path();
*s = h1 / h2;
s->setPath(path);
}
void Analysis::divide(Profile1DPtr p1, Profile1DPtr p2, Scatter2DPtr s) const {
const string path = s->path();
*s = *p1 / *p2;
s->setPath(path);
}
void Analysis::divide(const Profile1D& p1, const Profile1D& p2, Scatter2DPtr s) const {
const string path = s->path();
*s = p1 / p2;
s->setPath(path);
}
void Analysis::divide(Histo2DPtr h1, Histo2DPtr h2, Scatter3DPtr s) const {
const string path = s->path();
*s = *h1 / *h2;
s->setPath(path);
}
void Analysis::divide(const Histo2D& h1, const Histo2D& h2, Scatter3DPtr s) const {
const string path = s->path();
*s = h1 / h2;
s->setPath(path);
}
void Analysis::divide(Profile2DPtr p1, Profile2DPtr p2, Scatter3DPtr s) const {
const string path = s->path();
*s = *p1 / *p2;
s->setPath(path);
}
void Analysis::divide(const Profile2D& p1, const Profile2D& p2, Scatter3DPtr s) const {
const string path = s->path();
*s = p1 / p2;
s->setPath(path);
}
/// @todo Counter and Histo2D efficiencies and asymms
void Analysis::efficiency(Histo1DPtr h1, Histo1DPtr h2, Scatter2DPtr s) const {
const string path = s->path();
*s = YODA::efficiency(*h1, *h2);
s->setPath(path);
}
void Analysis::efficiency(const Histo1D& h1, const Histo1D& h2, Scatter2DPtr s) const {
const string path = s->path();
*s = YODA::efficiency(h1, h2);
s->setPath(path);
}
void Analysis::asymm(Histo1DPtr h1, Histo1DPtr h2, Scatter2DPtr s) const {
const string path = s->path();
*s = YODA::asymm(*h1, *h2);
s->setPath(path);
}
void Analysis::asymm(const Histo1D& h1, const Histo1D& h2, Scatter2DPtr s) const {
const string path = s->path();
*s = YODA::asymm(h1, h2);
s->setPath(path);
}
void Analysis::scale(CounterPtr cnt, double factor) {
if (!cnt) {
MSG_WARNING("Failed to scale counter=NULL in analysis " << name() << " (scale=" << factor << ")");
return;
}
if (std::isnan(factor) || std::isinf(factor)) {
MSG_WARNING("Failed to scale counter=" << cnt->path() << " in analysis: " << name() << " (invalid scale factor = " << factor << ")");
factor = 0;
}
MSG_TRACE("Scaling counter " << cnt->path() << " by factor " << factor);
try {
cnt->scaleW(factor);
} catch (YODA::Exception& we) {
MSG_WARNING("Could not scale counter " << cnt->path());
return;
}
}
void Analysis::normalize(Histo1DPtr histo, double norm, bool includeoverflows) {
if (!histo) {
MSG_WARNING("Failed to normalize histo=NULL in analysis " << name() << " (norm=" << norm << ")");
return;
}
MSG_TRACE("Normalizing histo " << histo->path() << " to " << norm);
try {
const double hint = histo->integral(includeoverflows);
if (hint == 0) MSG_WARNING("Skipping histo with null area " << histo->path());
else histo->normalize(norm, includeoverflows);
} catch (YODA::Exception& we) {
MSG_WARNING("Could not normalize histo " << histo->path());
return;
}
}
void Analysis::scale(Histo1DPtr histo, double factor) {
if (!histo) {
MSG_WARNING("Failed to scale histo=NULL in analysis " << name() << " (scale=" << factor << ")");
return;
}
if (std::isnan(factor) || std::isinf(factor)) {
MSG_WARNING("Failed to scale histo=" << histo->path() << " in analysis: " << name() << " (invalid scale factor = " << factor << ")");
factor = 0;
}
MSG_TRACE("Scaling histo " << histo->path() << " by factor " << factor);
try {
histo->scaleW(factor);
} catch (YODA::Exception& we) {
MSG_WARNING("Could not scale histo " << histo->path());
return;
}
}
void Analysis::normalize(Histo2DPtr histo, double norm, bool includeoverflows) {
if (!histo) {
MSG_ERROR("Failed to normalize histo=NULL in analysis " << name() << " (norm=" << norm << ")");
return;
}
MSG_TRACE("Normalizing histo " << histo->path() << " to " << norm);
try {
const double hint = histo->integral(includeoverflows);
if (hint == 0) MSG_WARNING("Skipping histo with null area " << histo->path());
else histo->normalize(norm, includeoverflows);
} catch (YODA::Exception& we) {
MSG_WARNING("Could not normalize histo " << histo->path());
return;
}
}
void Analysis::scale(Histo2DPtr histo, double factor) {
if (!histo) {
MSG_ERROR("Failed to scale histo=NULL in analysis " << name() << " (scale=" << factor << ")");
return;
}
if (std::isnan(factor) || std::isinf(factor)) {
MSG_ERROR("Failed to scale histo=" << histo->path() << " in analysis: " << name() << " (invalid scale factor = " << factor << ")");
factor = 0;
}
MSG_TRACE("Scaling histo " << histo->path() << " by factor " << factor);
try {
histo->scaleW(factor);
} catch (YODA::Exception& we) {
MSG_WARNING("Could not scale histo " << histo->path());
return;
}
}
void Analysis::integrate(Histo1DPtr h, Scatter2DPtr s) const {
// preserve the path info
const string path = s->path();
*s = toIntegralHisto(*h);
s->setPath(path);
}
void Analysis::integrate(const Histo1D& h, Scatter2DPtr s) const {
// preserve the path info
const string path = s->path();
*s = toIntegralHisto(h);
s->setPath(path);
}
/// @todo 2D versions of integrate... defined how, exactly?!?
//////////////////////////////////
void Analysis::addAnalysisObject(AnalysisObjectPtr ao) {
_analysisobjects.push_back(ao);
}
void Analysis::removeAnalysisObject(const string& path) {
for (vector<AnalysisObjectPtr>::iterator it = _analysisobjects.begin(); it != _analysisobjects.end(); ++it) {
if ((*it)->path() == path) {
_analysisobjects.erase(it);
break;
}
}
}
void Analysis::removeAnalysisObject(AnalysisObjectPtr ao) {
for (vector<AnalysisObjectPtr>::iterator it = _analysisobjects.begin(); it != _analysisobjects.end(); ++it) {
if (*it == ao) {
_analysisobjects.erase(it);
break;
}
}
}
const CentralityProjection &
Analysis::declareCentrality(const SingleValueProjection &proj,
string calAnaName, string calHistName,
const string projName, bool increasing) {
CentralityProjection cproj;
// Select the centrality variable from option. Use REF as default.
// Other selections are "GEN", "IMP" and "USR" (USR only in HEPMC 3).
string sel = getOption<string>("cent","REF");
set<string> done;
if ( sel == "REF" ) {
Scatter2DPtr refscat;
auto refmap = getRefData(calAnaName);
if ( refmap.find(calHistName) != refmap.end() )
refscat =
dynamic_pointer_cast<Scatter2D>(refmap.find(calHistName)->second);
if ( !refscat ) {
MSG_WARNING("No reference calibration histogram for " <<
"CentralityProjection " << projName << " found " <<
"(requested histogram " << calHistName << " in " <<
calAnaName << ")");
}
else {
MSG_INFO("Found calibration histogram " << sel << " " << refscat->path());
cproj.add(PercentileProjection(proj, refscat, increasing), sel);
}
}
else if ( sel == "GEN" ) {
Histo1DPtr genhist;
string histpath = "/" + calAnaName + "/" + calHistName;
for ( AnalysisObjectPtr ao : handler().getData(true) ) {
if ( ao->path() == histpath )
genhist = dynamic_pointer_cast<Histo1D>(ao);
}
if ( !genhist || genhist->numEntries() <= 1 ) {
MSG_WARNING("No generated calibration histogram for " <<
"CentralityProjection " << projName << " found " <<
"(requested histogram " << calHistName << " in " <<
calAnaName << ")");
}
else {
MSG_INFO("Found calibration histogram " << sel << " " << genhist->path());
cproj.add(PercentileProjection(proj, genhist, increasing), sel);
}
}
else if ( sel == "IMP" ) {
Histo1DPtr imphist =
getAnalysisObject<Histo1D>(calAnaName, calHistName + "_IMP");
if ( !imphist || imphist->numEntries() <= 1 ) {
MSG_WARNING("No impact parameter calibration histogram for " <<
"CentralityProjection " << projName << " found " <<
"(requested histogram " << calHistName << "_IMP in " <<
calAnaName << ")");
}
else {
MSG_INFO("Found calibration histogram " << sel << " " << imphist->path());
cproj.add(PercentileProjection(ImpactParameterProjection(),
imphist, true), sel);
}
}
else if ( sel == "USR" ) {
#if HEPMC_VERSION_CODE >= 3000000
Histo1DPtr usrhist =
getAnalysisObject<Histo1D>(calAnaName, calHistName + "_USR");
if ( !usrhist || usrhist->numEntries() <= 1 ) {
MSG_WARNING("No user-defined calibration histogram for " <<
"CentralityProjection " << projName << " found " <<
"(requested histogram " << calHistName << "_USR in " <<
calAnaName << ")");
continue;
}
else {
MSG_INFO("Found calibration histogram " << sel << " " << usrhist->path());
cproj.add((UserCentEstimate(), usrhist, true), sel);
}
#else
MSG_WARNING("UserCentEstimate is only available with HepMC3.");
#endif
}
else if ( sel == "RAW" ) {
#if HEPMC_VERSION_CODE >= 3000000
cproj.add(GeneratedCentrality(), sel);
#else
MSG_WARNING("GeneratedCentrality is only available with HepMC3.");
#endif
}
else
MSG_WARNING("'" << sel << "' is not a valid PercentileProjection tag.");
if ( cproj.empty() )
MSG_WARNING("CentralityProjection " << projName
<< " did not contain any valid PercentileProjections.");
return declare(cproj, projName);
}
}
diff --git a/src/Core/AnalysisHandler.cc b/src/Core/AnalysisHandler.cc
--- a/src/Core/AnalysisHandler.cc
+++ b/src/Core/AnalysisHandler.cc
@@ -1,574 +1,575 @@
// -*- C++ -*-
#include "Rivet/Config/RivetCommon.hh"
#include "Rivet/AnalysisHandler.hh"
#include "Rivet/Analysis.hh"
#include "Rivet/Tools/ParticleName.hh"
#include "Rivet/Tools/BeamConstraint.hh"
#include "Rivet/Tools/Logging.hh"
#include "Rivet/Projections/Beam.hh"
#include "YODA/IO.h"
namespace Rivet {
AnalysisHandler::AnalysisHandler(const string& runname)
: _runname(runname),
_eventcounter("/_EVTCOUNT"),
_xs(NAN), _xserr(NAN),
_initialised(false), _ignoreBeams(false), _dumpPeriod(0), _dumping(false)
{ }
AnalysisHandler::~AnalysisHandler()
{ }
Log& AnalysisHandler::getLog() const {
return Log::getLog("Rivet.Analysis.Handler");
}
void AnalysisHandler::init(const GenEvent& ge) {
if (_initialised)
throw UserError("AnalysisHandler::init has already been called: cannot re-initialize!");
setRunBeams(Rivet::beams(ge));
MSG_DEBUG("Initialising the analysis handler");
_eventcounter.reset();
// Check that analyses are beam-compatible, and remove those that aren't
const size_t num_anas_requested = analysisNames().size();
vector<string> anamestodelete;
for (const AnaHandle a : _analyses) {
if (!_ignoreBeams && !a->isCompatible(beams())) {
//MSG_DEBUG(a->name() << " requires beams " << a->requiredBeams() << " @ " << a->requiredEnergies() << " GeV");
anamestodelete.push_back(a->name());
}
}
for (const string& aname : anamestodelete) {
MSG_WARNING("Analysis '" << aname << "' is incompatible with the provided beams: removing");
removeAnalysis(aname);
}
if (num_anas_requested > 0 && analysisNames().empty()) {
cerr << "All analyses were incompatible with the first event's beams\n"
<< "Exiting, since this probably wasn't intentional!" << endl;
exit(1);
}
// Warn if any analysis' status is not unblemished
for (const AnaHandle a : analyses()) {
if (toUpper(a->status()) == "PRELIMINARY") {
MSG_WARNING("Analysis '" << a->name() << "' is preliminary: be careful, it may change and/or be renamed!");
} else if (toUpper(a->status()) == "OBSOLETE") {
MSG_WARNING("Analysis '" << a->name() << "' is obsolete: please update!");
} else if (toUpper(a->status()).find("UNVALIDATED") != string::npos) {
MSG_WARNING("Analysis '" << a->name() << "' is unvalidated: be careful, it may be broken!");
}
}
// Initialize the remaining analyses
for (AnaHandle a : _analyses) {
MSG_DEBUG("Initialising analysis: " << a->name());
try {
// Allow projection registration in the init phase onwards
a->_allowProjReg = true;
a->init();
//MSG_DEBUG("Checking consistency of analysis: " << a->name());
//a->checkConsistency();
} catch (const Error& err) {
cerr << "Error in " << a->name() << "::init method: " << err.what() << endl;
exit(1);
}
MSG_DEBUG("Done initialising analysis: " << a->name());
}
_initialised = true;
MSG_DEBUG("Analysis handler initialised");
}
void AnalysisHandler::analyze(const GenEvent& ge) {
// Call init with event as template if not already initialised
if (!_initialised) init(ge);
assert(_initialised);
// Ensure that beam details match those from the first event (if we're checking beams)
if ( !_ignoreBeams ) {
const PdgIdPair beams = Rivet::beamIds(ge);
const double sqrts = Rivet::sqrtS(ge);
if (!compatible(beams, _beams) || !fuzzyEquals(sqrts, sqrtS())) {
cerr << "Event beams mismatch: "
<< PID::toBeamsString(beams) << " @ " << sqrts/GeV << " GeV" << " vs. first beams "
<< this->beams() << " @ " << this->sqrtS()/GeV << " GeV" << endl;
exit(1);
}
}
// Create the Rivet event wrapper
/// @todo Filter/normalize the event here
Event event(ge);
// Weights
/// @todo Drop this / just report first weight when we support multiweight events
_eventcounter.fill(event.weight());
MSG_DEBUG("Event #" << _eventcounter.numEntries() << " weight = " << event.weight());
// Cross-section
#ifdef HEPMC_HAS_CROSS_SECTION
if (ge.cross_section()) {
_xs = ge.cross_section()->cross_section();
_xserr = ge.cross_section()->cross_section_error();
}
#endif
// Run the analyses
for (AnaHandle a : _analyses) {
MSG_TRACE("About to run analysis " << a->name());
try {
a->analyze(event);
} catch (const Error& err) {
cerr << "Error in " << a->name() << "::analyze method: " << err.what() << endl;
exit(1);
}
MSG_TRACE("Finished running analysis " << a->name());
}
if ( _dumpPeriod > 0 && numEvents()%_dumpPeriod == 0 ) {
MSG_INFO("Dumping intermediate results to " << _dumpFile << ".");
_dumping = true;
finalize();
_dumping = false;
writeData(_dumpFile);
}
}
void AnalysisHandler::analyze(const GenEvent* ge) {
if (ge == nullptr) {
MSG_ERROR("AnalysisHandler received null pointer to GenEvent");
//throw Error("AnalysisHandler received null pointer to GenEvent");
}
analyze(*ge);
}
void AnalysisHandler::finalize() {
if (!_initialised) return;
// First we make copies of all analysis objects.
map<string,AnalysisObjectPtr> backupAOs;
for (auto ao : getData(false, true) )
backupAOs[ao->path()] = AnalysisObjectPtr(ao->newclone());
// Now we run the (re-entrant) finalize() functions for all analyses.
MSG_INFO("Finalising analyses");
for (AnaHandle a : _analyses) {
a->setCrossSection(_xs);
try {
if ( !_dumping || a->info().reentrant() ) a->finalize();
else if ( _dumping )
MSG_INFO("Skipping periodic dump of " << a->name()
<< " as it is not declared reentrant.");
} catch (const Error& err) {
cerr << "Error in " << a->name() << "::finalize method: " << err.what() << endl;
exit(1);
}
}
// Now we copy all analysis objects to the list of finalized
// ones, and restore the value to their original ones.
_finalizedAOs.clear();
for ( auto ao : getData() )
_finalizedAOs.push_back(AnalysisObjectPtr(ao->newclone()));
for ( auto ao : getData(false, true) ) {
// TODO: This should be possible to do in a nicer way, with a flag etc.
if (ao->path().find("/FINAL") != std::string::npos) continue;
auto aoit = backupAOs.find(ao->path());
if ( aoit == backupAOs.end() ) {
AnaHandle ana = analysis(split(ao->path(), "/")[0]);
if ( ana ) ana->removeAnalysisObject(ao->path());
} else
copyao(aoit->second, ao);
}
// Print out number of events processed
const int nevts = _eventcounter.numEntries();
MSG_INFO("Processed " << nevts << " event" << (nevts != 1 ? "s" : ""));
// // Delete analyses
// MSG_DEBUG("Deleting analyses");
// _analyses.clear();
// Print out MCnet boilerplate
cout << endl;
cout << "The MCnet usage guidelines apply to Rivet: see http://www.montecarlonet.org/GUIDELINES" << endl;
cout << "Please acknowledge plots made with Rivet analyses, and cite arXiv:1003.0694 (http://arxiv.org/abs/1003.0694)" << endl;
}
AnalysisHandler& AnalysisHandler::addAnalysis(const string& analysisname, std::map<string, string> pars) {
// Make an option handle.
std::string parHandle = "";
for (map<string, string>::iterator par = pars.begin(); par != pars.end(); ++par) {
parHandle +=":";
parHandle += par->first + "=" + par->second;
}
return addAnalysis(analysisname + parHandle);
}
AnalysisHandler& AnalysisHandler::addAnalysis(const string& analysisname) {
// Check for a duplicate analysis
/// @todo Might we want to be able to run an analysis twice, with different params?
/// Requires avoiding histo tree clashes, i.e. storing the histos on the analysis objects.
string ananame = analysisname;
vector<string> anaopt = split(analysisname, ":");
if ( anaopt.size() > 1 ) ananame = anaopt[0];
AnaHandle analysis( AnalysisLoader::getAnalysis(ananame) );
if (analysis.get() != 0) { // < Check for null analysis.
MSG_DEBUG("Adding analysis '" << analysisname << "'");
map<string,string> opts;
for ( int i = 1, N = anaopt.size(); i < N; ++i ) {
vector<string> opt = split(anaopt[i], "=");
if ( opt.size() != 2 ) {
MSG_WARNING("Error in option specification. Skipping analysis "
<< analysisname);
return *this;
}
if ( !analysis->info().validOption(opt[0], opt[1]) ) {
MSG_WARNING("Cannot set option '" << opt[0] << "' to '" << opt[1]
<< "'. Skipping analysis " << analysisname);
return *this;
}
opts[opt[0]] = opt[1];
}
for ( auto opt: opts) {
analysis->_options[opt.first] = opt.second;
analysis->_optstring += ":" + opt.first + "=" + opt.second;
}
for (const AnaHandle& a : _analyses) {
if (a->name() == analysis->name() ) {
MSG_WARNING("Analysis '" << analysisname << "' already registered: skipping duplicate");
return *this;
}
}
analysis->_analysishandler = this;
_analyses.insert(analysis);
} else {
MSG_WARNING("Analysis '" << analysisname << "' not found.");
}
// MSG_WARNING(_analyses.size());
// for (const AnaHandle& a : _analyses) MSG_WARNING(a->name());
return *this;
}
AnalysisHandler& AnalysisHandler::removeAnalysis(const string& analysisname) {
std::shared_ptr<Analysis> toremove;
for (const AnaHandle a : _analyses) {
if (a->name() == analysisname) {
toremove = a;
break;
}
}
if (toremove.get() != 0) {
MSG_DEBUG("Removing analysis '" << analysisname << "'");
_analyses.erase(toremove);
}
return *this;
}
/////////////////////////////
void AnalysisHandler::addData(const std::vector<AnalysisObjectPtr>& aos) {
for (const AnalysisObjectPtr ao : aos) {
string path = ao->path();
if ( path.substr(0, 5) != "/RAW/" ) {
_orphanedPreloads.push_back(ao);
continue;
}
path = path.substr(4);
ao->setPath(path);
if (path.size() > 1) { // path > "/"
try {
const string ananame = split(path, "/")[0];
AnaHandle a = analysis(ananame);
a->addAnalysisObject(ao); /// @todo Need to statistically merge...
} catch (const Error& e) {
MSG_TRACE("Adding analysis object " << path <<
" to the list of orphans.");
_orphanedPreloads.push_back(ao);
}
}
}
}
void AnalysisHandler::stripOptions(AnalysisObjectPtr ao,
const vector<string> & delopts) const {
string path = ao->path();
string ananame = split(path, "/")[0];
vector<string> anaopts = split(ananame, ":");
for ( int i = 1, N = anaopts.size(); i < N; ++i )
for ( auto opt : delopts )
if ( opt == "*" || anaopts[i].find(opt + "=") == 0 )
path.replace(path.find(":" + anaopts[i]), (":" + anaopts[i]).length(), "");
ao->setPath(path);
}
void AnalysisHandler::
mergeYodas(const vector<string> & aofiles, const vector<string> & delopts, bool equiv) {
vector< vector<AnalysisObjectPtr> > aosv;
vector<double> xsecs;
vector<double> xsecerrs;
vector<CounterPtr> sows;
set<string> ananames;
_eventcounter.reset();
// First scan all files and extract analysis objects and add the
// corresponding anayses..
for ( auto file : aofiles ) {
Scatter1DPtr xsec;
CounterPtr sow;
// For each file make sure that cross section and sum-of-weights
// objects are present and stor all RAW ones in a vector;
vector<AnalysisObjectPtr> aos;
try {
/// @todo Use new YODA SFINAE to fill the smart ptr vector directly
vector<YODA::AnalysisObject*> aos_raw;
YODA::read(file, aos_raw);
for (AnalysisObject* aor : aos_raw) {
AnalysisObjectPtr ao = AnalysisObjectPtr(aor);
if ( ao->path().substr(0, 5) != "/RAW/" ) continue;
ao->setPath(ao->path().substr(4));
if ( ao->path() == "/_XSEC" )
xsec = dynamic_pointer_cast<Scatter1D>(ao);
else if ( ao->path() == "/_EVTCOUNT" )
sow = dynamic_pointer_cast<Counter>(ao);
else {
stripOptions(ao, delopts);
string ananame = split(ao->path(), "/")[0];
if ( ananames.insert(ananame).second ) addAnalysis(ananame);
aos.push_back(ao);
}
}
if ( !xsec || !sow ) {
MSG_ERROR( "Error in AnalysisHandler::mergeYodas: The file " << file
<< " did not contain weights and cross section info.");
exit(1);
}
xsecs.push_back(xsec->point(0).x());
sows.push_back(sow);
xsecerrs.push_back(sqr(xsec->point(0).xErrAvg()));
_eventcounter += *sow;
sows.push_back(sow);
aosv.push_back(aos);
} catch (...) { //< YODA::ReadError&
throw UserError("Unexpected error in reading file: " + file);
}
}
// Now calculate the scale to be applied for all bins in a file
// and get the common cross section and sum of weights.
_xs = _xserr = 0.0;
for ( int i = 0, N = sows.size(); i < N; ++i ) {
double effnent = sows[i]->effNumEntries();
_xs += (equiv? effnent: 1.0)*xsecs[i];
_xserr += (equiv? sqr(effnent): 1.0)*xsecerrs[i];
}
vector<double> scales(sows.size(), 1.0);
if ( equiv ) {
_xs /= _eventcounter.effNumEntries();
_xserr = sqrt(_xserr)/_eventcounter.effNumEntries();
} else {
_xserr = sqrt(_xserr);
for ( int i = 0, N = sows.size(); i < N; ++i )
scales[i] = (_eventcounter.sumW()/sows[i]->sumW())*(xsecs[i]/_xs);
}
// Initialize the analyses allowing them to book analysis objects.
for (AnaHandle a : _analyses) {
MSG_DEBUG("Initialising analysis: " << a->name());
if ( !a->info().reentrant() )
MSG_WARNING("Analysis " << a->name() << " has not been validated to have "
<< "a reentrant finalize method. The result is unpredictable.");
try {
// Allow projection registration in the init phase onwards
a->_allowProjReg = true;
cerr << "sqrtS " << sqrtS() << endl;
a->init();
//MSG_DEBUG("Checking consistency of analysis: " << a->name());
//a->checkConsistency();
} catch (const Error& err) {
cerr << "Error in " << a->name() << "::init method: " << err.what() << endl;
exit(1);
}
MSG_DEBUG("Done initialising analysis: " << a->name());
}
_initialised = true;
// Get a list of all anaysis objects to handle.
map<string,AnalysisObjectPtr> current;
for ( auto ao : getData(false, true) ) current[ao->path()] = ao;
// Go through all objects to be merged and add them to current
// after appropriate scaling.
for ( int i = 0, N = aosv.size(); i < N; ++i)
for ( auto ao : aosv[i] ) {
if ( ao->path() == "/_XSEC" || ao->path() == "_EVTCOUNT" ) continue;
auto aoit = current.find(ao->path());
if ( aoit == current.end() ) {
MSG_WARNING("" << ao->path() << " was not properly booked.");
continue;
}
if ( !addaos(aoit->second, ao, scales[i]) )
MSG_WARNING("Cannot merge objects with path " << ao->path()
<<" of type " << ao->annotation("Type") );
}
// Now we can simply finalize() the analysis, leaving the
// controlling program to write it out some yoda-file.
finalize();
}
void AnalysisHandler::readData(const string& filename) {
vector<AnalysisObjectPtr> aos;
try {
/// @todo Use new YODA SFINAE to fill the smart ptr vector directly
vector<YODA::AnalysisObject*> aos_raw;
YODA::read(filename, aos_raw);
for (AnalysisObject* aor : aos_raw) aos.push_back(AnalysisObjectPtr(aor));
} catch (...) { //< YODA::ReadError&
throw UserError("Unexpected error in reading file: " + filename);
}
if (!aos.empty()) addData(aos);
}
vector<AnalysisObjectPtr> AnalysisHandler::
getData(bool includeorphans, bool includetmps) const {
vector<AnalysisObjectPtr> rtn;
// Event counter
rtn.push_back( make_shared<Counter>(_eventcounter) );
// Cross-section + err as scatter
YODA::Scatter1D::Points pts; pts.insert(YODA::Point1D(_xs, _xserr));
rtn.push_back( make_shared<Scatter1D>(pts, "/_XSEC") );
// Analysis histograms
for (const AnaHandle a : analyses()) {
vector<AnalysisObjectPtr> aos = a->analysisObjects();
// MSG_WARNING(a->name() << " " << aos.size());
for (const AnalysisObjectPtr ao : aos) {
// Exclude paths from final write-out if they contain a "TMP" layer (i.e. matching "/TMP/")
/// @todo This needs to be much more nuanced for re-entrant histogramming
if ( !includetmps && ao->path().find("/TMP/" ) != string::npos) continue;
rtn.push_back(ao);
}
}
// Sort histograms alphanumerically by path before write-out
sort(rtn.begin(), rtn.end(), [](AnalysisObjectPtr a, AnalysisObjectPtr b) {return a->path() < b->path();});
if ( includeorphans )
rtn.insert(rtn.end(), _orphanedPreloads.begin(), _orphanedPreloads.end());
return rtn;
}
void AnalysisHandler::writeData(const string& filename) const {
vector<AnalysisObjectPtr> out = _finalizedAOs;
out.reserve(2*out.size());
vector<AnalysisObjectPtr> aos = getData(false, true);
for ( auto ao : aos ) {
ao = AnalysisObjectPtr(ao->newclone());
ao->setPath("/RAW" + ao->path());
out.push_back(ao);
}
try {
YODA::write(filename, out.begin(), out.end());
} catch (...) { //< YODA::WriteError&
throw UserError("Unexpected error in writing file: " + filename);
}
}
std::vector<std::string> AnalysisHandler::analysisNames() const {
std::vector<std::string> rtn;
for (AnaHandle a : _analyses) {
rtn.push_back(a->name());
}
return rtn;
}
const AnaHandle AnalysisHandler::analysis(const std::string& analysisname) const {
for (const AnaHandle a : analyses())
if (a->name() == analysisname) return a;
throw Error("No analysis named '" + analysisname + "' registered in AnalysisHandler");
}
AnalysisHandler& AnalysisHandler::addAnalyses(const std::vector<std::string>& analysisnames) {
for (const string& aname : analysisnames) {
//MSG_DEBUG("Adding analysis '" << aname << "'");
addAnalysis(aname);
}
return *this;
}
AnalysisHandler& AnalysisHandler::removeAnalyses(const std::vector<std::string>& analysisnames) {
for (const string& aname : analysisnames) {
removeAnalysis(aname);
}
return *this;
}
bool AnalysisHandler::needCrossSection() const {
bool rtn = false;
for (const AnaHandle a : _analyses) {
if (!rtn) rtn = a->needsCrossSection();
if (rtn) break;
}
return rtn;
}
- AnalysisHandler& AnalysisHandler::setCrossSection(double xs) {
+ AnalysisHandler& AnalysisHandler::setCrossSection(double xs, double xserr) {
_xs = xs;
+ _xserr = xserr;
return *this;
}
bool AnalysisHandler::hasCrossSection() const {
return (!std::isnan(crossSection()));
}
AnalysisHandler& AnalysisHandler::addAnalysis(Analysis* analysis) {
analysis->_analysishandler = this;
_analyses.insert(AnaHandle(analysis));
return *this;
}
PdgIdPair AnalysisHandler::beamIds() const {
return Rivet::beamIds(beams());
}
double AnalysisHandler::sqrtS() const {
return Rivet::sqrtS(beams());
}
void AnalysisHandler::setIgnoreBeams(bool ignore) {
_ignoreBeams=ignore;
}
}
diff --git a/src/Core/Particle.cc b/src/Core/Particle.cc
--- a/src/Core/Particle.cc
+++ b/src/Core/Particle.cc
@@ -1,318 +1,327 @@
#include "Rivet/Particle.hh"
#include "Rivet/Tools/Cuts.hh"
#include "Rivet/Tools/ParticleIdUtils.hh"
#include "Rivet/Tools/ParticleUtils.hh"
namespace Rivet {
void Particle::setConstituents(const Particles& cs, bool setmom) {
_constituents = cs;
if (setmom) _momentum = sum(cs, p4, FourMomentum());
}
void Particle::addConstituent(const Particle& c, bool addmom) {
_constituents += c;
if (addmom) _momentum += c;
}
void Particle::addConstituents(const Particles& cs, bool addmom) {
_constituents += cs;
if (addmom)
for (const Particle& c : cs)
_momentum += c;
}
Particles Particle::rawConstituents() const {
if (!isComposite()) return Particles{*this};
Particles rtn;
for (const Particle& p : constituents()) rtn += p.rawConstituents();
return rtn;
}
Particle& Particle::transformBy(const LorentzTransform& lt) {
_momentum = lt.transform(_momentum);
return *this;
}
bool Particle::isVisible() const {
// Charged particles are visible
if ( PID::threeCharge(pid()) != 0 ) return true;
// Neutral hadrons are visible
if ( PID::isHadron(pid()) ) return true;
// Photons are visible
if ( pid() == PID::PHOTON ) return true;
// Gluons are visible (for parton level analyses)
if ( pid() == PID::GLUON ) return true;
// Everything else is invisible
return false;
}
bool Particle::isStable() const {
return genParticle() != NULL &&
genParticle()->status() == 1 &&
genParticle()->end_vertex() == NULL;
}
Particles Particle::ancestors(const Cut& c, bool physical_only) const {
Particles rtn;
// this case needed protecting against (at least for the latest Herwig... not sure why
// it didn't show up earlier
if (genParticle() == NULL) return rtn;
/// @todo Remove this const mess crap when HepMC doesn't suck
GenVertexPtr gv = const_cast<GenVertexPtr>( genParticle()->production_vertex() );
if (gv == NULL) return rtn;
/// @todo Would like to do this, but the range objects are broken
// foreach (const GenParticlePtr gp, gv->particles(HepMC::children))
// rtn += Particle(gp);
for (GenVertex::particle_iterator it = gv->particles_begin(HepMC::ancestors); it != gv->particles_end(HepMC::ancestors); ++it) {
if (physical_only && (*it)->status() != 1 && (*it)->status() != 2) continue;
const Particle p(*it);
if (c != Cuts::OPEN && !c->accept(p)) continue;
rtn += p;
}
return rtn;
}
Particles Particle::parents(const Cut& c) const {
Particles rtn;
/// @todo Remove this const mess crap when HepMC doesn't suck
GenVertexPtr gv = const_cast<GenVertexPtr>( genParticle()->production_vertex() );
if (gv == NULL) return rtn;
/// @todo Would like to do this, but the range objects are broken
// foreach (const GenParticlePtr gp, gv->particles(HepMC::children))
// rtn += Particle(gp);
for (GenVertex::particle_iterator it = gv->particles_begin(HepMC::parents); it != gv->particles_end(HepMC::parents); ++it) {
const Particle p(*it);
if (c != Cuts::OPEN && !c->accept(p)) continue;
rtn += p;
}
return rtn;
}
Particles Particle::children(const Cut& c) const {
Particles rtn;
/// @todo Something going wrong with taus -> GenParticle nullptr?
if (genParticle() == nullptr) return rtn;
if (isStable()) return rtn;
/// @todo Remove this const mess crap when HepMC doesn't suck
//cout << genParticle()->end_vertex() << endl;
GenVertexPtr gv = const_cast<GenVertexPtr>( genParticle()->end_vertex() );
if (gv == nullptr) return rtn;
/// @todo Would like to do this, but the range objects are broken
// foreach (const GenParticlePtr gp, gv->particles(HepMC::children))
// rtn += Particle(gp);
for (GenVertex::particle_iterator it = gv->particles_begin(HepMC::children); it != gv->particles_end(HepMC::children); ++it) {
const Particle p(*it);
if (c != Cuts::OPEN && !c->accept(p)) continue;
rtn += p;
}
return rtn;
}
/// @todo Insist that the current particle is post-hadronization, otherwise throw an exception?
/// @todo Use recursion through replica-avoiding functions to avoid bookkeeping duplicates
Particles Particle::allDescendants(const Cut& c, bool remove_duplicates) const {
Particles rtn;
if (isStable()) return rtn;
/// @todo Remove this const mess crap when HepMC doesn't suck
GenVertexPtr gv = const_cast<GenVertexPtr>( genParticle()->end_vertex() );
if (gv == NULL) return rtn;
/// @todo Would like to do this, but the range objects are broken
// foreach (const GenParticlePtr gp, gv->particles(HepMC::descendants))
for (GenVertex::particle_iterator it = gv->particles_begin(HepMC::descendants); it != gv->particles_end(HepMC::descendants); ++it) {
const Particle p(*it);
if (c != Cuts::OPEN && !c->accept(p)) continue;
if (remove_duplicates && (*it)->end_vertex() != NULL) {
// size_t n = 0; ///< @todo Only remove 1-to-1 duplicates?
bool dup = false;
/// @todo Yuck, HepMC
for (GenVertex::particle_iterator it2 = (*it)->end_vertex()->particles_begin(HepMC::children); it2 != (*it)->end_vertex()->particles_end(HepMC::children); ++it2) {
// n += 1; if (n > 1) break;
if ((*it)->pdg_id() == (*it2)->pdg_id()) { dup = true; break; }
}
if (dup) continue;
}
rtn += p;
}
return rtn;
}
/// @todo Insist that the current particle is post-hadronization, otherwise throw an exception?
Particles Particle::stableDescendants(const Cut& c) const {
Particles rtn;
if (isStable()) return rtn;
/// @todo Remove this const mess crap when HepMC doesn't suck
GenVertexPtr gv = const_cast<GenVertexPtr>( genParticle()->end_vertex() );
if (gv == NULL) return rtn;
/// @todo Would like to do this, but the range objects are broken
// foreach (const GenParticlePtr gp, gv->particles(HepMC::descendants))
for (GenVertex::particle_iterator it = gv->particles_begin(HepMC::descendants); it != gv->particles_end(HepMC::descendants); ++it) {
// if ((*it)->status() != 1 || (*it)->end_vertex() != NULL) continue;
const Particle p(*it);
if (!p.isStable()) continue;
if (c != Cuts::OPEN && !c->accept(p)) continue;
rtn += p;
}
return rtn;
}
double Particle::flightLength() const {
if (isStable()) return -1;
if (genParticle() == NULL) return 0;
if (genParticle()->production_vertex() == NULL) return 0;
const HepMC::FourVector v1 = genParticle()->production_vertex()->position();
const HepMC::FourVector v2 = genParticle()->end_vertex()->position();
return sqrt(sqr(v2.x()-v1.x()) + sqr(v2.y()-v1.y()) + sqr(v2.z()-v1.z()));
}
bool Particle::hasParent(PdgId pid) const {
return hasParentWith(hasPID(pid));
}
bool Particle::hasParentWith(const Cut& c) const {
return hasParentWith([&](const Particle& p){return c->accept(p);});
}
bool Particle::hasAncestor(PdgId pid, bool only_physical) const {
return hasAncestorWith(hasPID(pid), only_physical);
}
bool Particle::hasAncestorWith(const Cut& c, bool only_physical) const {
return hasAncestorWith([&](const Particle& p){return c->accept(p);}, only_physical);
}
bool Particle::hasChildWith(const Cut& c) const {
return hasChildWith([&](const Particle& p){return c->accept(p);});
}
bool Particle::hasDescendantWith(const Cut& c, bool remove_duplicates) const {
return hasDescendantWith([&](const Particle& p){return c->accept(p);}, remove_duplicates);
}
bool Particle::hasStableDescendantWith(const Cut& c) const {
return hasStableDescendantWith([&](const Particle& p){return c->accept(p);});
}
bool Particle::fromBottom() const {
return hasAncestorWith([](const Particle& p){
return p.genParticle()->status() == 2 && p.isHadron() && p.hasBottom();
});
}
bool Particle::fromCharm() const {
return hasAncestorWith([](const Particle& p){
return p.genParticle()->status() == 2 && p.isHadron() && p.hasCharm();
});
}
bool Particle::fromHadron() const {
return hasAncestorWith([](const Particle& p){
return p.genParticle()->status() == 2 && p.isHadron();
});
}
bool Particle::fromTau(bool prompt_taus_only) const {
if (prompt_taus_only && fromHadron()) return false;
return hasAncestorWith([](const Particle& p){
return p.genParticle()->status() == 2 && isTau(p);
});
}
bool Particle::fromHadronicTau(bool prompt_taus_only) const {
return hasAncestorWith([&](const Particle& p){
return p.genParticle()->status() == 2 && isTau(p) && (!prompt_taus_only || p.isPrompt()) && hasHadronicDecay(p);
});
}
bool Particle::isDirect(bool allow_from_direct_tau, bool allow_from_direct_mu) const {
- if (genParticle() == NULL) return false; // no HepMC connection, give up! Throw UserError exception?
- const GenVertexPtr prodVtx = genParticle()->production_vertex();
- if (prodVtx == NULL) return false; // orphaned particle, has to be assume false
- const pair<GenParticlePtr, GenParticlePtr> beams = prodVtx->parent_event()->beam_particles();
+ while (!_isDirect.second) { ///< @todo Replace awkward caching with C++17 std::optional
+ // Immediate short-circuit: hadrons can't be direct, and for partons we can't tell
+ if (isHadron() || isParton()) {
+ _isDirect = std::make_pair(false, true); break;
+ }
- /// @todo Would be nicer to be able to write this recursively up the chain, exiting as soon as a parton or string/cluster is seen
- for (const GenParticlePtr ancestor : Rivet::particles(prodVtx, HepMC::ancestors)) {
- const PdgId pid = ancestor->pdg_id();
- if (ancestor->status() != 2) continue; // no non-standard statuses or beams to be used in decision making
- if (ancestor == beams.first || ancestor == beams.second) continue; // PYTHIA6 uses status 2 for beams, I think... (sigh)
- if (PID::isParton(pid)) continue; // PYTHIA6 also uses status 2 for some partons, I think... (sigh)
- if (PID::isHadron(pid)) return false; // direct particles can't be from hadron decays
- if (abs(pid) == PID::TAU && abspid() != PID::TAU && !allow_from_direct_tau) return false; // allow or ban particles from tau decays (permitting tau copies)
- if (abs(pid) == PID::MUON && abspid() != PID::MUON && !allow_from_direct_mu) return false; // allow or ban particles from muon decays (permitting muon copies)
+ // Obtain links to parentage
+ if (genParticle() == nullptr) { _isDirect = std::make_pair(false, true); break; } // no HepMC connection, give up! Throw UserError exception?
+ const GenVertexPtr prodVtx = genParticle()->production_vertex();
+ if (prodVtx == nullptr) { _isDirect = std::make_pair(false, true); break; } // orphaned particle, has to be assume false
+ const pair<GenParticlePtr, GenParticlePtr> beams = prodVtx->parent_event()->beam_particles();
+
+ /// @todo Would be nicer to be able to write this recursively up the chain, exiting as soon as a parton or string/cluster is seen
+ for (const GenParticlePtr ancestor : Rivet::particles(prodVtx, HepMC::ancestors)) {
+ const PdgId pid = ancestor->pdg_id();
+ if (ancestor->status() != 2) continue; // no non-standard statuses or beams to be used in decision making
+ if (ancestor == beams.first || ancestor == beams.second) continue; // PYTHIA6 uses status 2 for beams, I think... (sigh)
+ if (PID::isParton(pid)) continue; // PYTHIA6 also uses status 2 for some partons, I think... (sigh)
+ if (PID::isHadron(pid)) { _isDirect = std::make_pair(false, true); break; } // direct particles can't be from hadron decays
+ if (abs(pid) == PID::TAU && abspid() != PID::TAU && !allow_from_direct_tau) { _isDirect = std::make_pair(false, true); break; } // allow or ban particles from tau decays (permitting tau copies)
+ if (abs(pid) == PID::MUON && abspid() != PID::MUON && !allow_from_direct_mu) { _isDirect = std::make_pair(false, true); break; } // allow or ban particles from muon decays (permitting muon copies)
+ }
+ if (!_isDirect.second) _isDirect = std::make_pair(true, true); //< guarantee loop exit
}
- return true;
+ return _isDirect.first;
}
///////////////////////
// DISABLED UNTIL VANILLA CC7 COMPATIBILITY NOT NEEDED
// /// Particles copy constructor from vector<Particle>
// Particles::Particles(const std::vector<Particle>& vps) : base(vps) {}
// /// Particles -> FourMomenta cast/conversion operator
// Particles::operator FourMomenta () const {
// // FourMomenta rtn(this->begin(), this->end());
// FourMomenta rtn; rtn.reserve(this->size());
// for (size_t i = 0; i < this->size(); ++i) rtn.push_back((*this)[i]);
// return rtn;
// }
// /// Particles concatenation operator
// Particles operator + (const Particles& a, const Particles& b) {
// Particles rtn(a);
// rtn += b;
// return rtn;
// }
//////////////////////////////////
/// Allow a Particle to be passed to an ostream.
std::ostream& operator << (std::ostream& os, const Particle& p) {
string pname;
try {
pname = PID::toParticleName(p.pid());
} catch (...) {
pname = "PID=" + to_str(p.pid());
}
os << "Particle<" << pname << " @ " << p.momentum()/GeV << " GeV>";
return os;
}
/// Allow ParticlePair to be passed to an ostream.
std::ostream& operator << (std::ostream& os, const ParticlePair& pp) {
os << "[" << pp.first << ", " << pp.second << "]";
return os;
}
}
diff --git a/src/Core/Run.cc b/src/Core/Run.cc
--- a/src/Core/Run.cc
+++ b/src/Core/Run.cc
@@ -1,162 +1,163 @@
// -*- C++ -*-
#include "Rivet/Run.hh"
#include "Rivet/AnalysisHandler.hh"
#include "HepMC/IO_GenEvent.h"
#include "Rivet/Math/MathUtils.hh"
#include "Rivet/Tools/RivetPaths.hh"
#include "zstr/zstr.hpp"
#include <limits>
namespace Rivet {
Run::Run(AnalysisHandler& ah)
: _ah(ah), _fileweight(1.0), _xs(NAN)
{ }
Run::~Run() { }
Run& Run::setCrossSection(const double xs) {
_xs = xs;
return *this;
}
double Run::crossSection() const {
return _ah.crossSection();
}
Run& Run::setListAnalyses(const bool dolist) {
_listAnalyses = dolist;
return *this;
}
// Fill event and check for a bad read state
bool Run::readEvent() {
/// @todo Clear rather than new the GenEvent object per-event?
_evt.reset(new GenEvent());
if (_io->rdstate() != 0 || !_io->fill_next_event(_evt.get()) ) {
Log::getLog("Rivet.Run") << Log::DEBUG << "Read failed. End of file?" << endl;
return false;
}
// Rescale event weights by file-level weight, if scaling is non-trivial
if (!fuzzyEquals(_fileweight, 1.0)) {
for (size_t i = 0; i < (size_t) _evt->weights().size(); ++i) {
_evt->weights()[i] *= _fileweight;
}
}
return true;
}
// Fill event and check for a bad read state --- to skip, maybe HEPMC3 will have a better way
bool Run::skipEvent() {
if (_io->rdstate() != 0 || !_io->fill_next_event(_evt.get()) ) {
Log::getLog("Rivet.Run") << Log::DEBUG << "Read failed. End of file?" << endl;
return false;
}
return true;
}
bool Run::openFile(const std::string& evtfile, double weight) {
// Set current weight-scaling member
_fileweight = weight;
// Set up HepMC input reader objects
if (evtfile == "-") {
_io.reset(new HepMC::IO_GenEvent(std::cin));
} else {
if (!fileexists(evtfile)) throw Error("Event file '" + evtfile + "' not found");
#ifdef HAVE_LIBZ
// NB. zstr auto-detects if file is deflated or plain-text
_istr.reset(new zstr::ifstream(evtfile.c_str()));
#else
_istr.reset(new std::fstream(evtfile.c_str(), std::ios::in));
#endif
_io.reset(new HepMC::IO_GenEvent(*_istr));
}
if (_io->rdstate() != 0) {
Log::getLog("Rivet.Run") << Log::ERROR << "Read error on file " << evtfile << endl;
return false;
}
return true;
}
bool Run::init(const std::string& evtfile, double weight) {
if (!openFile(evtfile, weight)) return false;
// Read first event to define run conditions
bool ok = readEvent();
if (!ok) return false;
if (_evt->particles_size() == 0) {
Log::getLog("Rivet.Run") << Log::ERROR << "Empty first event." << endl;
return false;
}
// Initialise AnalysisHandler with beam information from first event
_ah.init(*_evt);
// Set cross-section from command line
if (!std::isnan(_xs)) {
Log::getLog("Rivet.Run")
<< Log::DEBUG << "Setting user cross-section = " << _xs << " pb" << endl;
_ah.setCrossSection(_xs);
}
// List the chosen & compatible analyses if requested
if (_listAnalyses) {
for (const std::string& ana : _ah.analysisNames()) {
cout << ana << endl;
}
}
return true;
}
bool Run::processEvent() {
// Set cross-section if found in event and not from command line
#ifdef HEPMC_HAS_CROSS_SECTION
if (std::isnan(_xs) && _evt->cross_section()) {
- const double xs = _evt->cross_section()->cross_section(); ///< in pb
+ const double xs = _evt->cross_section()->cross_section()*picobarn;
+ const double xserr = _evt->cross_section()->cross_section_error()*picobarn;
Log::getLog("Rivet.Run")
- << Log::DEBUG << "Setting cross-section = " << xs << " pb" << endl;
- _ah.setCrossSection(xs);
+ << Log::DEBUG << "Setting cross-section = " << xs << " +- " << xserr << " pb" << endl;
+ _ah.setCrossSection(xs, xserr);
}
#endif
// Complain about absence of cross-section if required!
if (_ah.needCrossSection() && !_ah.hasCrossSection()) {
Log::getLog("Rivet.Run")
<< Log::ERROR
<< "Total cross-section needed for at least one of the analyses. "
<< "Please set it (on the command line with '-x' if using the 'rivet' program)" << endl;
return false;
}
// Analyze event
_ah.analyze(*_evt);
return true;
}
bool Run::finalize() {
_evt.reset();
_istr.reset();
_io.reset();
if (!std::isnan(_xs)) _ah.setCrossSection(_xs);
_ah.finalize();
return true;
}
}
diff --git a/src/Makefile.am b/src/Makefile.am
--- a/src/Makefile.am
+++ b/src/Makefile.am
@@ -1,17 +1,16 @@
SUBDIRS = Core Tools Projections AnalysisTools
lib_LTLIBRARIES = libRivet.la
libRivet_la_SOURCES =
libRivet_la_LDFLAGS = -export-dynamic -avoid-version -L$(YODALIBPATH) -L$(HEPMCLIBPATH)
libRivet_la_LIBADD = \
Core/libRivetCore.la \
Projections/libRivetProjections.la \
Tools/libRivetTools.la \
-Tools/Nsubjettiness/libRivetNsubjettiness.la \
AnalysisTools/libRivetAnalysisTools.la \
-lYODA -lHepMC -ldl -lm \
$(FASTJETCONFIGLIBADD) \
$(GSL_LDFLAGS)
diff --git a/src/Projections/DressedLeptons.cc b/src/Projections/DressedLeptons.cc
--- a/src/Projections/DressedLeptons.cc
+++ b/src/Projections/DressedLeptons.cc
@@ -1,134 +1,178 @@
// -*- C++ -*-
#include "Rivet/Projections/DressedLeptons.hh"
+#include "Rivet/Projections/PromptFinalState.hh"
+#include "Rivet/Projections/MergedFinalState.hh"
+#include "Rivet/Projections/FastJets.hh"
namespace Rivet {
// On DressedLepton helper class
//{
DressedLepton::DressedLepton(const Particle& dlepton)
: Particle(dlepton)
- {
+ {
setConstituents({{dlepton}}); //< bare lepton is first constituent
}
DressedLepton::DressedLepton(const Particle& lepton, const Particles& photons, bool momsum)
: Particle(lepton.pid(), lepton.momentum())
{
setConstituents({{lepton}}); //< bare lepton is first constituent
addConstituents(photons, momsum);
}
void DressedLepton::addPhoton(const Particle& p, bool momsum) {
if (p.pid() != PID::PHOTON) throw Error("Clustering a non-photon on to a DressedLepton:"+to_string(p.pid()));
addConstituent(p, momsum);
}
const Particle& DressedLepton::bareLepton() const {
const Particle& l = constituents().front();
if (!l.isChargedLepton()) throw Error("First constituent of a DressedLepton is not a bare lepton: oops");
return l;
}
//}
// Separate-FS version
DressedLeptons::DressedLeptons(const FinalState& photons, const FinalState& bareleptons,
- double dRmax, const Cut& cut, bool useDecayPhotons)
+ double dRmax, const Cut& cut,
+ bool useDecayPhotons, bool useJetClustering)
: FinalState(cut),
- _dRmax(dRmax), _fromDecay(useDecayPhotons)
+ _dRmax(dRmax), _fromDecay(useDecayPhotons), _useJetClustering(useJetClustering)
{
setName("DressedLeptons");
+ // Find photons -- specialising to prompt photons if decay photons are to be vetoed
IdentifiedFinalState photonfs(photons, PID::PHOTON);
- addProjection(photonfs, "Photons");
+ if (_fromDecay) {
+ addProjection(photonfs, "Photons");
+ } else {
+ addProjection(PromptFinalState(photonfs), "Photons");
+ }
+ // Find bare leptons
IdentifiedFinalState leptonfs(bareleptons);
- leptonfs.acceptIdPairs({PID::ELECTRON, PID::MUON, PID::TAU});
+ leptonfs.acceptIdPairs({PID::ELECTRON, PID::MUON, PID::TAU}); //< hmm, no final-state taus, so is this useful?
addProjection(leptonfs, "Leptons");
+
+ // Set up FJ clustering option
+ if (_useJetClustering) {
+ MergedFinalState mergedfs(photonfs, leptonfs);
+ FastJets leptonjets(mergedfs, FastJets::ANTIKT, dRmax);
+ addProjection(leptonjets, "LeptonJets");
+ }
}
// Single-FS version
DressedLeptons::DressedLeptons(const FinalState& barefs,
- double dRmax, const Cut& cut, bool useDecayPhotons)
- : DressedLeptons(barefs, barefs, dRmax, cut, useDecayPhotons)
+ double dRmax, const Cut& cut,
+ bool useDecayPhotons, bool useJetClustering)
+ : DressedLeptons(barefs, barefs, dRmax, cut, useDecayPhotons, useJetClustering)
{ }
int DressedLeptons::compare(const Projection& p) const {
// Compare the two as final states (for pT and eta cuts)
const DressedLeptons& other = dynamic_cast<const DressedLeptons&>(p);
int fscmp = FinalState::compare(other);
if (fscmp != EQUIVALENT) return fscmp;
const PCmp phcmp = mkNamedPCmp(p, "Photons");
if (phcmp != EQUIVALENT) return phcmp;
const PCmp sigcmp = mkNamedPCmp(p, "Leptons");
if (sigcmp != EQUIVALENT) return sigcmp;
return (cmp(_dRmax, other._dRmax) ||
- cmp(_fromDecay, other._fromDecay));
+ cmp(_fromDecay, other._fromDecay) ||
+ cmp(_useJetClustering, other._useJetClustering));
}
void DressedLeptons::project(const Event& e) {
_theParticles.clear();
// Get bare leptons
- const FinalState& signal = applyProjection<FinalState>(e, "Leptons");
+ const FinalState& signal = apply<FinalState>(e, "Leptons");
Particles bareleptons = signal.particles();
if (bareleptons.empty()) return;
// Initialise DL collection with bare leptons
vector<Particle> allClusteredLeptons;
allClusteredLeptons.reserve(bareleptons.size());
- for (const Particle& bl : bareleptons) {
- Particle dl(bl.pid(), bl.momentum());
- dl.setConstituents({bl});
- allClusteredLeptons += dl;
- }
// If the radius is 0 or negative, don't even attempt to cluster
- if (_dRmax > 0) {
- // Match each photon to its closest charged lepton within the dR cone
- const FinalState& photons = applyProjection<FinalState>(e, "Photons");
- for (const Particle& photon : photons.particles()) {
- // Ignore photon if it's from a hadron/tau decay and we're avoiding those
- if (!_fromDecay && photon.fromDecay()) continue;
- const FourMomentum& p_P = photon.momentum();
- double dRmin = _dRmax;
- int idx = -1;
- for (size_t i = 0; i < bareleptons.size(); ++i) {
- const Particle& bl = bareleptons[i];
- // Only cluster photons around *charged* signal particles
- if (bl.charge3() == 0) continue;
- // Find the closest lepton
- double dR = deltaR(bl, p_P);
- if (dR < dRmin) {
- dRmin = dR;
- idx = i;
+ if (_useJetClustering) {
+
+ if (_dRmax <= 0) {
+ for (const Particle& bl : bareleptons) {
+ Particle dl(bl.pid(), bl.momentum());
+ dl.setConstituents({bl});
+ allClusteredLeptons += dl;
+ }
+ } else {
+ const Jets& lepjets = apply<FastJets>(e, "LeptonJets").jets();
+ for (const Jet& lepjet : lepjets) {
+ const Particles leps = sortByPt(lepjet.particles(isChargedLepton));
+ if (leps.empty()) continue;
+ Particles constituents = {leps[0]}; //< note no dressing for subleading leptons
+ Particle dl(leps[0].pid(), leps[0].momentum());
+ constituents += lepjet.particles(isPhoton);
+ dl.setConstituents(constituents);
+ allClusteredLeptons += dl;
+ }
+ }
+
+ } else {
+
+ for (const Particle& bl : bareleptons) {
+ Particle dl(bl.pid(), bl.momentum());
+ dl.setConstituents({bl});
+ allClusteredLeptons += dl;
+ }
+ if (_dRmax > 0) {
+ // Match each photon to its closest charged lepton within the dR cone
+ const FinalState& photons = applyProjection<FinalState>(e, "Photons");
+ for (const Particle& photon : photons.particles()) {
+ // Ignore photon if it's from a hadron/tau decay and we're avoiding those
+ /// @todo Can remove via the PromptFinalState conversion above?
+ if (!_fromDecay && photon.fromDecay()) continue;
+ const FourMomentum& p_P = photon.momentum();
+ double dRmin = _dRmax;
+ int idx = -1;
+ for (size_t i = 0; i < bareleptons.size(); ++i) {
+ const Particle& bl = bareleptons[i];
+ // Only cluster photons around *charged* signal particles
+ if (bl.charge3() == 0) continue;
+ // Find the closest lepton
+ double dR = deltaR(bl, p_P);
+ if (dR < dRmin) {
+ dRmin = dR;
+ idx = i;
+ }
}
+ if (idx > -1) allClusteredLeptons[idx].addConstituent(photon, true);
}
- if (idx > -1) allClusteredLeptons[idx].addConstituent(photon, true);
}
}
// Fill the canonical particles collection with the composite DL Particles
for (const Particle& lepton : allClusteredLeptons) {
const bool acc = accept(lepton);
MSG_TRACE("Clustered lepton " << lepton << " with constituents = " << lepton.constituents() << ", cut-pass = " << boolalpha << acc);
if (acc) _theParticles.push_back(lepton);
}
MSG_DEBUG("#dressed leptons = " << allClusteredLeptons.size() << " -> " << _theParticles.size() << " after cuts");
}
}
diff --git a/src/Projections/VetoedFinalState.cc b/src/Projections/VetoedFinalState.cc
--- a/src/Projections/VetoedFinalState.cc
+++ b/src/Projections/VetoedFinalState.cc
@@ -1,144 +1,123 @@
// -*- C++ -*-
#include "Rivet/Projections/VetoedFinalState.hh"
namespace Rivet {
int VetoedFinalState::compare(const Projection& p) const {
const PCmp fscmp = mkNamedPCmp(p, "FS");
if (fscmp != EQUIVALENT) return fscmp;
/// @todo We can do better than this...
if (_vetofsnames.size() != 0) return UNDEFINED;
const VetoedFinalState& other = dynamic_cast<const VetoedFinalState&>(p);
return \
- cmp(_vetoCodes, other._vetoCodes) ||
+ cmp(_vetoCuts, other._vetoCuts) ||
cmp(_compositeVetoes, other._compositeVetoes) ||
cmp(_parentVetoes, other._parentVetoes);
}
void VetoedFinalState::project(const Event& e) {
const FinalState& fs = applyProjection<FinalState>(e, "FS");
_theParticles.clear();
_theParticles.reserve(fs.particles().size());
-
- // Veto by PID code
- if (getLog().isActive(Log::TRACE)) {
- /// @todo Should be PdgId, but _vetoCodes is currently a long
- vector<long> codes;
- for (auto& code : _vetoCodes) codes += code.first;
- MSG_TRACE("Veto codes = " << codes << " (" << codes.size() << ")");
- }
- if (_vetoCodes.empty()) {
+ // Veto by cut
+ if (_vetoCuts.empty()) {
_theParticles = fs.particles();
} else {
// Test every particle against the codes
for (const Particle& p : fs.particles()) {
- VetoDetails::iterator iter = _vetoCodes.find(p.pid());
- if (iter == _vetoCodes.end()) {
- // MSG_TRACE("Storing with PDG code = " << p.pid() << ", pT = " << p.pT());
+ bool match = false;
+ for (const Cut& c : _vetoCuts) {
+ if (c->accept(p)) {
+ match = true;
+ break;
+ }
+ }
+ if (!match) {
+ MSG_TRACE("Storing particle " << p);
_theParticles.push_back(p);
} else {
- // This particle code is listed as a possible veto... check pT.
- // Make sure that the pT range is sensible:
- BinaryCut ptrange = iter->second;
- assert(ptrange.first <= ptrange.second);
- stringstream rangess;
- if (ptrange.first < numeric_limits<double>::max()) rangess << ptrange.second;
- rangess << " - ";
- if (ptrange.second < numeric_limits<double>::max()) rangess << ptrange.second;
- MSG_TRACE("ID = " << p.pid() << ", pT range = " << rangess.str());
- stringstream debugline;
- debugline << "with PDG code = " << p.pid() << " pT = " << p.pT();
- if (p.pT() < ptrange.first || p.pT() > ptrange.second) {
- MSG_TRACE("Storing " << debugline.str());
- _theParticles.push_back(p);
- } else {
- MSG_TRACE("Vetoing " << debugline.str());
- }
+ MSG_TRACE("Vetoing particle " << p);
}
}
}
- /// @todo What is this block? Mass vetoing?
+ // Composite particle mass vetoing
+ /// @todo YUCK! Clean up...
set<Particles::iterator> toErase;
- for (set<int>::iterator nIt = _nCompositeDecays.begin(); nIt != _nCompositeDecays.end() && !_theParticles.empty(); ++nIt) {
+ for (auto nIt = _nCompositeDecays.begin(); nIt != _nCompositeDecays.end() && !_theParticles.empty(); ++nIt) {
map<set<Particles::iterator>, FourMomentum> oldMasses;
map<set<Particles::iterator>, FourMomentum> newMasses;
set<Particles::iterator> start;
start.insert(_theParticles.begin());
oldMasses.insert(pair<set<Particles::iterator>, FourMomentum>(start, _theParticles.begin()->momentum()));
for (int nParts = 1; nParts != *nIt; ++nParts) {
- for (map<set<Particles::iterator>, FourMomentum>::iterator mIt = oldMasses.begin();
- mIt != oldMasses.end(); ++mIt) {
+ for (auto mIt = oldMasses.begin(); mIt != oldMasses.end(); ++mIt) {
Particles::iterator pStart = *(mIt->first.rbegin());
- for (Particles::iterator pIt = pStart + 1; pIt != _theParticles.end(); ++pIt) {
+ for (auto pIt = pStart + 1; pIt != _theParticles.end(); ++pIt) {
FourMomentum cMom = mIt->second + pIt->momentum();
set<Particles::iterator> pList(mIt->first);
pList.insert(pIt);
newMasses[pList] = cMom;
}
}
oldMasses = newMasses;
newMasses.clear();
}
- for (map<set<Particles::iterator>, FourMomentum>::iterator mIt = oldMasses.begin();
- mIt != oldMasses.end(); ++mIt) {
+ for (auto mIt = oldMasses.begin(); mIt != oldMasses.end(); ++mIt) {
double mass2 = mIt->second.mass2();
if (mass2 >= 0.0) {
double mass = sqrt(mass2);
- for (CompositeVeto::iterator cIt = _compositeVetoes.lower_bound(*nIt);
- cIt != _compositeVetoes.upper_bound(*nIt); ++cIt) {
- BinaryCut massRange = cIt->second;
+ for (auto cIt = _compositeVetoes.lower_bound(*nIt); cIt != _compositeVetoes.upper_bound(*nIt); ++cIt) {
+ auto massRange = cIt->second;
if (mass < massRange.second && mass > massRange.first) {
- for (set<Particles::iterator>::iterator lIt = mIt->first.begin();
- lIt != mIt->first.end(); ++lIt) {
+ for (auto lIt = mIt->first.begin(); lIt != mIt->first.end(); ++lIt) {
toErase.insert(*lIt);
}
}
}
}
}
}
- for (set<Particles::iterator>::reverse_iterator p = toErase.rbegin(); p != toErase.rend(); ++p) {
+ for (auto p = toErase.rbegin(); p != toErase.rend(); ++p) {
_theParticles.erase(*p);
}
-
// Remove particles whose parents match entries in the parent veto PDG ID codes list
/// @todo There must be a nice way to do this -- an STL algorithm (or we provide a nicer wrapper)
for (PdgId vetoid : _parentVetoes) {
for (Particles::iterator ip = _theParticles.begin(); ip != _theParticles.end(); ++ip) {
const GenVertex* startVtx = ip->genParticle()->production_vertex();
if (startVtx == NULL) continue;
// Loop over parents and test their IDs
/// @todo Could use any() here?
for (const GenParticle* parent : Rivet::particles(startVtx, HepMC::ancestors)) {
if (vetoid == parent->pdg_id()) {
ip = _theParticles.erase(ip); --ip; //< Erase this _theParticles entry
break;
}
}
}
}
// Finally veto on the registered FSes
for (const string& ifs : _vetofsnames) {
const ParticleFinder& vfs = applyProjection<ParticleFinder>(e, ifs);
const Particles& pvetos = vfs.rawParticles();
ifilter_discard(_theParticles, [&](const Particle& pcheck) {
if (pcheck.genParticle() == nullptr) return false;
for (const Particle& pveto : pvetos) {
if (pveto.genParticle() == nullptr) continue;
if (pveto.genParticle() == pcheck.genParticle()) { MSG_TRACE("Vetoing: " << pcheck); return true; }
}
return false;
});
}
MSG_DEBUG("FS vetoing from #particles = " << fs.size() << " -> " << _theParticles.size());
}
}
diff --git a/src/Tools/Makefile.am b/src/Tools/Makefile.am
--- a/src/Tools/Makefile.am
+++ b/src/Tools/Makefile.am
@@ -1,23 +1,28 @@
-SUBDIRS = Nsubjettiness
+SUBDIRS = fjcontrib
noinst_LTLIBRARIES = libRivetTools.la
libRivetTools_la_SOURCES = \
BinnedHistogram.cc \
Correlators.cc \
Cuts.cc \
JetUtils.cc \
Random.cc \
Logging.cc \
ParticleUtils.cc \
ParticleName.cc \
Percentile.cc \
RivetYODA.cc \
RivetMT2.cc \
RivetPaths.cc \
Utils.cc \
binreloc.c
dist_noinst_HEADERS = binreloc.h lester_mt2_bisect.hh
libRivetTools_la_CPPFLAGS = $(AM_CPPFLAGS) -DENABLE_BINRELOC -DDEFAULTDATADIR=\"$(datadir)\" -DDEFAULTLIBDIR=\"$(libdir)\"
+
+libRivetTools_la_LIBADD = \
+ fjcontrib/EnergyCorrelator/libRivetEnergyCorrelator.la \
+ fjcontrib/Nsubjettiness/libRivetNsubjettiness.la \
+ fjcontrib/RecursiveTools/libRivetRecursiveTools.la
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/AUTHORS b/src/Tools/fjcontrib/EnergyCorrelator/AUTHORS
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/AUTHORS
@@ -0,0 +1,23 @@
+The EnergyCorrelator FastJet contrib was written and is maintained and developed by:
+
+ Andrew Larkoski <larkoski@mit.edu>
+ Lina Necib <lnecib@mit.edu>
+ Gavin Salam <gavin.salam@cern.ch>
+ Jesse Thaler <jthaler@jthaler.net>
+
+For physics details, see:
+
+ Energy Correlation Functions for Jet Substructure.
+ Andrew J. Larkoski, Gavin P. Salam, and Jesse Thaler.
+ JHEP 1306, 108 (2013)
+ arXiv:1305.0007.
+
+ Power Counting to Better Jet Observables.
+ Andrew J. Larkoski, Ian Moult, and Duff Neill.
+ JHEP 1412, 009 (2014)
+ arXiv:1409.6298.
+
+ New Angles on Energy Correlation Functions.
+ Ian Moult, Lina Necib, and Jesse Thaler.
+ arXiv:1609.07483.
+----------------------------------------------------------------------
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/COPYING b/src/Tools/fjcontrib/EnergyCorrelator/COPYING
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/COPYING
@@ -0,0 +1,360 @@
+The EnergyCorrelator contrib to FastJet is released
+under the terms of the GNU General Public License v2 (GPLv2).
+
+A copy of the GPLv2 is to be found at the end of this file.
+
+While the GPL license grants you considerable freedom, please bear in
+mind that this code's use falls under guidelines similar to those that
+are standard for Monte Carlo event generators
+(http://www.montecarlonet.org/GUIDELINES). In particular, if you use
+this code as part of work towards a scientific publication, whether
+directly or contained within another program you should include a citation
+to
+
+ arXiv:1305.0007
+ arXiv:1409.6298
+ arXiv:1609.07483
+
+======================================================================
+======================================================================
+======================================================================
+ GNU GENERAL PUBLIC LICENSE
+ Version 2, June 1991
+
+ Copyright (C) 1989, 1991 Free Software Foundation, Inc.
+ 59 Temple Place, Suite 330, Boston, MA 02111-1307 USA
+ Everyone is permitted to copy and distribute verbatim copies
+ of this license document, but changing it is not allowed.
+
+ Preamble
+
+ The licenses for most software are designed to take away your
+freedom to share and change it. By contrast, the GNU General Public
+License is intended to guarantee your freedom to share and change free
+software--to make sure the software is free for all its users. This
+General Public License applies to most of the Free Software
+Foundation's software and to any other program whose authors commit to
+using it. (Some other Free Software Foundation software is covered by
+the GNU Library General Public License instead.) You can apply it to
+your programs, too.
+
+ When we speak of free software, we are referring to freedom, not
+price. Our General Public Licenses are designed to make sure that you
+have the freedom to distribute copies of free software (and charge for
+this service if you wish), that you receive source code or can get it
+if you want it, that you can change the software or use pieces of it
+in new free programs; and that you know you can do these things.
+
+ To protect your rights, we need to make restrictions that forbid
+anyone to deny you these rights or to ask you to surrender the rights.
+These restrictions translate to certain responsibilities for you if you
+distribute copies of the software, or if you modify it.
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diff --git a/src/Tools/fjcontrib/EnergyCorrelator/ChangeLog b/src/Tools/fjcontrib/EnergyCorrelator/ChangeLog
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/ChangeLog
@@ -0,0 +1,307 @@
+2018-02-08 Jesse Thaler <jthaler@jthaler.net>
+
+ * NEWS
+ * VERSION
+ Making 1.3.1
+
+
+2018-02-08 Lina Necib <lnecib@caltech.edu>
+
+ * EnergyCorrelator.cc
+ Debugging memory allocation, deleting energyStore/angleStore properly this time
+
+
+2018-02-04 Lina Necib <lnecib@caltech.edu>
+
+ * EnergyCorrelator.cc
+ Debugging memory allocation, deleting energyStore/angleStore
+
+ * VERSION
+ Making 1.3.1-devel
+
+2018-01-09 Jesse Thaler <jthaler@jthaler.net>
+
+ * NEWS
+ * VERSION
+ Finalizing 1.3.0
+
+2018-01-09 Lina Necib <lnecib@caltech.edu>
+
+ * NEWS
+ Preparing for version candidate
+
+ * VERSION
+ Making 1.3.0-rc1
+
+2018-01-07 Lina Necib <lnecib@caltech.edu>
+
+ * EnergyCorrelator.hh/cc
+ Sped up evaluations of ECFs.
+ Functions are defined in ECFs and called to evaluate ECFGs.
+
+ * VERSION
+ Making 1.2.3-devel
+
+
+2018-01-04 Lina Necib <lnecib@caltech.edu>
+
+ * EnergyCorrelator.hh/cc
+ Sped up evaluations of ECFG by a factor of 4.
+ Refactored some of the code in functions
+
+ * VERSION
+ Making 1.2.2-devel
+
+ * example.cc
+ Added some timings tests for ECFGs, N2, and N3.
+
+
+2017-01-25 Jesse Thaler <jthaler@jthaler.net>
+
+ * EnergyCorrelator.hh/cc
+ Converting all _N to unsigned integers, removing _N < 0 warning
+ Added warning to constructors for N < 1 in some cases.
+
+ * VERSION
+ Making 1.2.1-devel
+
+ * Makefile
+ Added -Wextra to compiler flags
+
+2016-10-07 Jesse Thaler <jthaler@jthaler.net>
+
+ * AUTHORS/COPYING:
+ Updated the publication arXiv number to 1609.07483.
+
+ * EnergyCorrelator.hh
+ Fixed typo in EnergyCorrelatorGeneralized description
+
+ * NEWS
+ Added "USeries" to news.
+
+ * VERSION
+ Changed version to 1.2.0
+
+2016-09-27 Lina Necib <lnecib@mit.edu>
+
+ * EnergyCorrelator.hh/README
+ Updated the publication arXiv number to 1609.07483.
+
+2016-09-23 Lina Necib <lnecib@mit.edu>
+
+ * EnergyCorrelator.cc
+ Made the evaluation of ECFG faster by replacing sort -> partial_sort and simplified multiplication syntax
+ * example.cc/ref
+ Fixed minor typo
+ * VERSION
+ Changed version to 1.2.0-rc3
+
+2016-09-23 Lina Necib <lnecib@mit.edu>
+
+ * EnergyCorrelator.hh
+ Fixed minor doxygen typo
+ * example.cc/ref
+ Changed EnergyCorrelatorNormalized -> EnergyCorrelatorGeneralized in function explanations
+ * VERSION
+ Changed version to 1.2.0-rc2
+
+2016-09-22 Jesse Thaler <jthaler@jthaler.net>
+
+ * EnergyCorrelator.cc/hh
+ Renamed EnergyCorrelatorNormalized -> EnergyCorrelatorGeneralized
+ Changed order of arguments for EnergyCorrelatorGeneralized
+ Updated doxygen documentation
+ * example_basic_usage.cc
+ Changed EnergyCorrelatorNormalized -> EnergyCorrelatorGeneralized
+ * README
+ Updated for EnergyCorrelatorGeneralized
+
+2016-09-15 Lina Necib <lnecib@mit.edu>
+
+ *VERSION:
+ 1.2.0-rc1
+
+2016-08-24 Jesse Thaler <jthaler@jthaler.net>
+
+ Minor comment fixes throughout.
+
+ * EnergyCorrelator.cc/hh
+ Put in _helper_correlator when defining overall normalization
+ Removed angle error for result_all_angles()
+ *NEWS:
+ Made this more readable.
+ *README:
+ Clarified some of the documentation.
+
+2016-08-23 Lina Necib <lnecib@mit.edu>
+
+ *VERSION:
+ *NEWS:
+ *AUTHORS:
+ *COPYING:
+ *README:
+ *EnergyCorrelator.cc
+ Added if statement that the ECF and ECFNs return exactly zero
+ if the number of particles is less than N of the ECF.
+ *EnergyCorrelator.hh
+ *example.cc
+ *example_basic_usage.cc
+ Updated this example.
+
+2016-08-21 Lina Necib <lnecib@mit.edu>
+
+ *VERSION:
+ *NEWS:
+ *AUTHORS:
+ *COPYING:
+ *README:
+ *EnergyCorrelator.cc
+ Added Cseries.
+ *EnergyCorrelator.hh
+ Added Cseries.
+ *example.cc
+ Added example of Cseries
+ *example_basic_usage.cc
+ Simplified examples.
+
+2016-08-17 Lina Necib <lnecib@mit.edu>
+
+ *VERSION:
+ *NEWS:
+ *AUTHORS:
+ Added placeholder for new reference
+ *COPYING:
+ Added placeholder for new reference
+ *README:
+ added information on different measures E_inv
+ *EnergyCorrelator.cc
+ Minor text edits + added comments
+ *EnergyCorrelator.hh
+ Minor text edits + added comments
+ *example_basic_usage.cc
+ added a simplified example file that shows the use of the
+ different observables.
+
+
+2016-06-23 Lina Necib <lnecib@mit.edu>
+
+ *VERSION:
+ 1.2.0-alpha0
+ *NEWS:
+ *AUTHORS:
+ Lina Necib
+ *COPYING:
+ *README:
+ added descriptions of functions that will appear shortly
+ arXiv:160X.XXXXX
+
+ *EnergyCorrelator.cc
+ added code to calculate normalized ECFS.
+ *EnergyCorrelator.hh
+ added code to calculate normalized ECFS, Nseries, generalized
+ D2, N2, N3, and M2.
+
+ *example.cc
+ added calculation of normalized ECFS, Nseries, generalized
+ D2, N2, N3, and M2 to example file.
+
+
+2014-11-20 Jesse Thaler <jthaler@mit.edu>
+
+ * README:
+ Typos fixed
+
+2014-11-13 Andrew Larkoski <larkoski@mit.edu>
+
+ *VERSION:
+ *NEWS:
+ release of version 1.1.0
+
+ *AUTHORS:
+ *COPYING:
+ *README:
+ added reference to arXiv:1409.6298.
+
+ *EnergyCorrelator.cc
+ *EnergyCorrelator.hh
+ added code to calculate C1, C2, and D2 observables.
+
+ *example.cc
+ added calculation of C1, C2, and D2 to example file.
+
+2013-05-01 Gavin Salam <gavin.salam@cern.ch>
+
+ * VERSION:
+ * NEWS:
+ release of version 1.0.1
+
+ * README:
+ updated to reflect v1.0 interface.
+
+2013-05-01 Jesse Thaler
+
+ * EnergyCorrelator.cc
+ Switched from NAN to std::numeric_limits<double>::quiet_NaN()
+
+2013-04-30 Jesse Thaler
+
+ * EnergyCorrelator.cc
+ Implemented Gregory Soyez's suggestions on errors/asserts
+
+2013-04-30 Gavin Salam <gavin.salam@cern.ch>
+
+ * VERSION:
+ * NEWS:
+ released v. 1.0.0
+
+ * EnergyCorrelator.hh:
+ * example.cc
+ small changes to documentation to reflect the change below + an
+ gave an explicit command-line in the example.
+
+2013-04-29 Jesse Thaler
+
+ * EnergyCorrelator.cc
+ - Added support for N = 5
+
+ * example.cc|.ref
+ - Added N = 5 to test suite.
+
+2013-04-29 Gavin Salam <gavin.salam@cern.ch>
+
+ * EnergyCorrelator.hh|cc:
+ - reduced memory usage from roughly 8n^2 to 4n^2 bytes (note that
+ sums are now performed in a different order, so results may
+ change to within rounding error).
+
+ - Implemented description() for all three classes.
+
+ - Worked on doxygen-style comments and moved some bits of code into
+ the .cc file.
+
+ * Doxyfile: *** ADDED ***
+
+ * example.cc:
+ developers' timing component now uses clock(), to get
+ finer-grained timing, and also outputs a description for some of
+ the correlators being used.
+
+2013-04-26 + 04-27 Jesse Thaler <jthaler@MIT.EDU>
+
+ * EnergyCorrelator.hh|cc:
+ added temporary storage array for interparticle angles, to speed
+ up the energy correlator calculation for N>2
+
+ * example.cc
+ has internal option for printing out timing info.
+
+2013-04-26 Gavin Salam <gavin.salam@cern.ch> + Jesse & Andrew
+
+ * Makefile:
+ added explicit dependencies
+
+ * example.cc (analyze):
+ added a little bit of commented code for timing tests.
+
+2013-03-10 <jthaler>
+ Initial creation
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/EnergyCorrelator.cc b/src/Tools/fjcontrib/EnergyCorrelator/EnergyCorrelator.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/EnergyCorrelator.cc
@@ -0,0 +1,1093 @@
+// EnergyCorrelator Package
+// Questions/Comments? Email the authors:
+// larkoski@mit.edu, lnecib@mit.edu,
+// gavin.salam@cern.ch jthaler@jthaler.net
+//
+// Copyright (c) 2013-2016
+// Andrew Larkoski, Lina Necib, Gavin Salam, and Jesse Thaler
+//
+// $Id: EnergyCorrelator.cc 1106 2018-02-09 01:47:28Z linoush $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include "fjcontrib/EnergyCorrelator.hh"
+#include <sstream>
+#include <limits>
+using namespace std;
+
+namespace Rivet {
+// FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+ namespace fjcontrib {
+ using namespace fastjet;
+
+
+ double EnergyCorrelator::result(const PseudoJet& jet) const {
+
+ // if jet does not have constituents, throw error
+ if (!jet.has_constituents()) throw Error("EnergyCorrelator called on jet with no constituents.");
+
+ // get N = 0 case out of the way
+ if (_N == 0) return 1.0;
+
+ // find constituents
+ std::vector<fastjet::PseudoJet> particles = jet.constituents();
+
+ // return zero if the number of constituents is less than _N
+ if (particles.size() < _N) return 0.0 ;
+
+ double answer = 0.0;
+
+ // take care of N = 1 case.
+ if (_N == 1) {
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ answer += energy(particles[i]);
+ }
+ return answer;
+ }
+
+ double half_beta = _beta/2.0;
+
+ // take care of N = 2 case.
+ if (_N == 2) {
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) { //note offset by one so that angle is never called on identical pairs
+ answer += energy(particles[i])
+ * energy(particles[j])
+ * pow(angleSquared(particles[i],particles[j]), half_beta);
+ }
+ }
+ return answer;
+ }
+
+
+ // if N > 5, then throw error
+ if (_N > 5) {
+ throw Error("EnergyCorrelator is only hard coded for N = 0,1,2,3,4,5");
+ }
+
+
+ // Now deal with N = 3,4,5. Different options if storage array is used or not.
+ if (_strategy == storage_array) {
+
+ // For N > 2, fill static storage array to save computation time.
+ unsigned int nC = particles.size();
+ // Make energy storage
+ double *energyStore = new double[nC];
+
+ // Make angular storage
+ double **angleStore = new double*[nC];
+
+ precompute_energies_and_angles(particles, energyStore, angleStore);
+
+ // Define n_angles so it is the same function for ECFs and ECFGs
+ unsigned int n_angles = _N * (_N - 1) / 2;
+ // now do recursion
+ if (_N == 3) {
+ answer = evaluate_n3(nC, n_angles, energyStore, angleStore);
+ } else if (_N == 4) {
+ answer = evaluate_n4(nC, n_angles, energyStore, angleStore);
+ } else if (_N == 5) {
+ answer = evaluate_n5(nC, n_angles, energyStore, angleStore);
+ } else {
+ assert(_N <= 5);
+ }
+ // Deleting arrays
+ delete[] energyStore;
+
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ delete[] angleStore[i];
+ }
+ delete[] angleStore;
+
+ } else if (_strategy == slow) {
+ if (_N == 3) {
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) {
+ double ans_ij = energy(particles[i])
+ * energy(particles[j])
+ * pow(angleSquared(particles[i],particles[j]), half_beta);
+ for (unsigned int k = j + 1; k < particles.size(); k++) {
+ answer += ans_ij
+ * energy(particles[k])
+ * pow(angleSquared(particles[i],particles[k]), half_beta)
+ * pow(angleSquared(particles[j],particles[k]), half_beta);
+ }
+ }
+ }
+ } else if (_N == 4) {
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) {
+ double ans_ij = energy(particles[i])
+ * energy(particles[j])
+ * pow(angleSquared(particles[i],particles[j]), half_beta);
+ for (unsigned int k = j + 1; k < particles.size(); k++) {
+ double ans_ijk = ans_ij
+ * energy(particles[k])
+ * pow(angleSquared(particles[i],particles[k]), half_beta)
+ * pow(angleSquared(particles[j],particles[k]), half_beta);
+ for (unsigned int l = k + 1; l < particles.size(); l++) {
+ answer += ans_ijk
+ * energy(particles[l])
+ * pow(angleSquared(particles[i],particles[l]), half_beta)
+ * pow(angleSquared(particles[j],particles[l]), half_beta)
+ * pow(angleSquared(particles[k],particles[l]), half_beta);
+ }
+ }
+ }
+ }
+ } else if (_N == 5) {
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) {
+ double ans_ij = energy(particles[i])
+ * energy(particles[j])
+ * pow(angleSquared(particles[i],particles[j]), half_beta);
+ for (unsigned int k = j + 1; k < particles.size(); k++) {
+ double ans_ijk = ans_ij
+ * energy(particles[k])
+ * pow(angleSquared(particles[i],particles[k]), half_beta)
+ * pow(angleSquared(particles[j],particles[k]), half_beta);
+ for (unsigned int l = k + 1; l < particles.size(); l++) {
+ double ans_ijkl = ans_ijk
+ * energy(particles[l])
+ * pow(angleSquared(particles[i],particles[l]), half_beta)
+ * pow(angleSquared(particles[j],particles[l]), half_beta)
+ * pow(angleSquared(particles[k],particles[l]), half_beta);
+ for (unsigned int m = l + 1; m < particles.size(); m++) {
+ answer += ans_ijkl
+ * energy(particles[m])
+ * pow(angleSquared(particles[i],particles[m]), half_beta)
+ * pow(angleSquared(particles[j],particles[m]), half_beta)
+ * pow(angleSquared(particles[k],particles[m]), half_beta)
+ * pow(angleSquared(particles[l],particles[m]), half_beta);
+ }
+ }
+ }
+ }
+ }
+ } else {
+ assert(_N <= 5);
+ }
+ } else {
+ assert(_strategy == slow || _strategy == storage_array);
+ }
+
+ return answer;
+ }
+
+ double EnergyCorrelator::energy(const PseudoJet& jet) const {
+ if (_measure == pt_R) {
+ return jet.perp();
+ } else if (_measure == E_theta || _measure == E_inv) {
+ return jet.e();
+ } else {
+ assert(_measure==pt_R || _measure==E_theta || _measure==E_inv);
+ return std::numeric_limits<double>::quiet_NaN();
+ }
+ }
+
+ double EnergyCorrelator::angleSquared(const PseudoJet& jet1, const PseudoJet& jet2) const {
+ if (_measure == pt_R) {
+ return jet1.squared_distance(jet2);
+ } else if (_measure == E_theta) {
+ // doesn't seem to be a fastjet built in for this
+ double dot = jet1.px()*jet2.px() + jet1.py()*jet2.py() + jet1.pz()*jet2.pz();
+ double norm1 = jet1.px()*jet1.px() + jet1.py()*jet1.py() + jet1.pz()*jet1.pz();
+ double norm2 = jet2.px()*jet2.px() + jet2.py()*jet2.py() + jet2.pz()*jet2.pz();
+
+ double costheta = dot/(sqrt(norm1 * norm2));
+ if (costheta > 1.0) costheta = 1.0; // Need to handle case of numerical overflow
+ double theta = acos(costheta);
+ return theta*theta;
+
+ } else if (_measure == E_inv) {
+ if (jet1.E() < 0.0000001 || jet2.E() < 0.0000001) return 0.0;
+ else {
+ double dot4 = max(jet1.E()*jet2.E() - jet1.px()*jet2.px() - jet1.py()*jet2.py() - jet1.pz()*jet2.pz(),0.0);
+ return 2.0 * dot4 / jet1.E() / jet2.E();
+ }
+ } else {
+ assert(_measure==pt_R || _measure==E_theta || _measure==E_inv);
+ return std::numeric_limits<double>::quiet_NaN();
+ }
+ }
+
+
+ double EnergyCorrelator::multiply_angles(double angle_list[], int n_angles, unsigned int N_total) const {
+ // Compute the product of the n_angles smallest angles.
+ // std::partial_sort could also work, but since angle_list contains
+ // less than 10 elements, this way is usually faster.
+ double product = 1;
+
+ for (int a = 0; a < n_angles; a++) {
+ double cur_min = angle_list[0];
+ int cur_min_pos = 0;
+ for (unsigned int b = 1; b < N_total; b++) {
+ if (angle_list[b] < cur_min) {
+ cur_min = angle_list[b];
+ cur_min_pos = b;
+ }
+ }
+
+ // multiply it by the next smallest
+ product *= cur_min;
+ angle_list[cur_min_pos] = INT_MAX;
+ }
+ return product;
+ }
+
+ void EnergyCorrelator::precompute_energies_and_angles(std::vector<fastjet::PseudoJet> const &particles, double* energyStore, double** angleStore) const {
+ // Fill storage with energy/angle information
+ unsigned int nC = particles.size();
+ for (unsigned int i = 0; i < nC; i++) {
+ angleStore[i] = new double[i];
+ }
+
+ double half_beta = _beta/2.0;
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ energyStore[i] = energy(particles[i]);
+ for (unsigned int j = 0; j < i; j++) {
+ if (half_beta == 1.0){
+ angleStore[i][j] = angleSquared(particles[i], particles[j]);
+ } else {
+ angleStore[i][j] = pow(angleSquared(particles[i], particles[j]), half_beta);
+ }
+ }
+ }
+ }
+
+ double EnergyCorrelator::evaluate_n3(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const {
+ unsigned int N_total = 3;
+ double angle1, angle2, angle3;
+ double angle;
+ double answer = 0;
+
+ for (unsigned int i = 2; i < nC; i++) {
+ for (unsigned int j = 1; j < i; j++) {
+ double mult_energy_i_j = energyStore[i] * energyStore[j];
+
+ for (unsigned int k = 0; k < j; k++) {
+ angle1 = angleStore[i][j];
+ angle2 = angleStore[i][k];
+ angle3 = angleStore[j][k];
+
+ double angle_list[] = {angle1, angle2, angle3};
+
+ if (n_angles == N_total) {
+ angle = angle1 * angle2 * angle3;
+ } else {
+ angle = multiply_angles(angle_list, n_angles, N_total);
+ }
+
+ answer += mult_energy_i_j
+ * energyStore[k]
+ * angle;
+ }
+ }
+ }
+ return answer;
+ }
+
+ double EnergyCorrelator::evaluate_n4(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const {
+ double answer = 0;
+ double angle1, angle2, angle3, angle4, angle5, angle6;
+ unsigned int N_total = 6;
+ double angle;
+
+ for (unsigned int i = 3; i < nC; i++) {
+ for (unsigned int j = 2; j < i; j++) {
+ for (unsigned int k = 1; k < j; k++) {
+ for (unsigned int l = 0; l < k; l++) {
+
+ angle1 = angleStore[i][j];
+ angle2 = angleStore[i][k];
+ angle3 = angleStore[i][l];
+ angle4 = angleStore[j][k];
+ angle5 = angleStore[j][l];
+ angle6 = angleStore[k][l];
+
+ double angle_list[] = {angle1, angle2, angle3, angle4, angle5, angle6};
+
+ if (n_angles == N_total) {
+ angle = angle1 * angle2 * angle3 * angle4 * angle5 * angle6;
+ } else {
+ angle = multiply_angles(angle_list, n_angles, N_total);
+ }
+
+ answer += energyStore[i]
+ * energyStore[j]
+ * energyStore[k]
+ * energyStore[l]
+ * angle;
+ }
+ }
+ }
+ }
+ return answer;
+ }
+
+ double EnergyCorrelator::evaluate_n5(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const {
+
+ double answer = 0;
+ double angle1, angle2, angle3, angle4, angle5, angle6, angle7, angle8, angle9, angle10;
+ unsigned int N_total = 10;
+ double angle;
+
+ for (unsigned int i = 4; i < nC; i++) {
+ for (unsigned int j = 3; j < i; j++) {
+ for (unsigned int k = 2; k < j; k++) {
+ for (unsigned int l = 1; l < k; l++) {
+ for (unsigned int m = 0; m < l; m++) {
+
+ angle1 = angleStore[i][j];
+ angle2 = angleStore[i][k];
+ angle3 = angleStore[i][l];
+ angle4 = angleStore[i][m];
+ angle5 = angleStore[j][k];
+ angle6 = angleStore[j][l];
+ angle7 = angleStore[j][m];
+ angle8 = angleStore[k][l];
+ angle9 = angleStore[k][m];
+ angle10 = angleStore[l][m];
+
+ double angle_list[] = {angle1, angle2, angle3, angle4, angle5, angle6, angle7, angle8,
+ angle9, angle10};
+
+ angle = multiply_angles(angle_list, n_angles, N_total);
+
+ answer += energyStore[i]
+ * energyStore[j]
+ * energyStore[k]
+ * energyStore[l]
+ * energyStore[m]
+ * angle;
+ }
+ }
+ }
+ }
+ }
+ return answer;
+ }
+
+
+
+ double EnergyCorrelatorGeneralized::multiply_angles(double angle_list[], int n_angles, unsigned int N_total) const {
+
+ return _helper_correlator.multiply_angles(angle_list, n_angles, N_total);
+ }
+
+ void EnergyCorrelatorGeneralized::precompute_energies_and_angles(std::vector<fastjet::PseudoJet> const &particles, double* energyStore, double** angleStore) const {
+
+ return _helper_correlator.precompute_energies_and_angles(particles, energyStore, angleStore);
+ }
+
+ double EnergyCorrelatorGeneralized::evaluate_n3(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const {
+
+ return _helper_correlator.evaluate_n3(nC, n_angles, energyStore, angleStore);
+ }
+
+ double EnergyCorrelatorGeneralized::evaluate_n4(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const {
+
+ return _helper_correlator.evaluate_n4(nC, n_angles, energyStore, angleStore);
+ }
+
+ double EnergyCorrelatorGeneralized::evaluate_n5(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const {
+
+ return _helper_correlator.evaluate_n5(nC, n_angles, energyStore, angleStore);
+ }
+
+ double EnergyCorrelatorGeneralized::result(const PseudoJet& jet) const {
+
+ // if jet does not have constituents, throw error
+ if (!jet.has_constituents()) throw Error("EnergyCorrelator called on jet with no constituents.");
+
+ // Throw an error if N < 0
+ // Not needed if N is unsigned integer
+ //if (_N < 0 ) throw Error("N cannot be negative");
+ // get N = 0 case out of the way
+ if (_N == 0) return 1.0;
+
+ // take care of N = 1 case.
+ if (_N == 1) return 1.0;
+
+ // find constituents
+ std::vector<fastjet::PseudoJet> particles = jet.constituents();
+ double answer = 0.0;
+
+ // return zero if the number of constituents is less than _N for the ECFG
+ if (particles.size() < _N) return 0.0 ;
+
+ // The normalization is the energy or pt of the jet, which is also ECF(1, beta)
+ double EJ = _helper_correlator.result(jet);
+
+ // The overall normalization
+ double norm = pow(EJ, _N);
+
+ // Find the max number of angles and throw an error if unsuitable
+ int N_total = int(_N*(_N-1)/2);
+ if (_angles > N_total) throw Error("Requested number of angles for EnergyCorrelatorGeneralized is larger than number of angles available");
+ if (_angles < -1) throw Error("Negative number of angles called for EnergyCorrelatorGeneralized");
+
+ double half_beta = _beta/2.0;
+
+ // take care of N = 2 case.
+ if (_N == 2) {
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) { //note offset by one so that angle is never called on identical pairs
+ answer += energy(particles[i])
+ * energy(particles[j])
+ * pow(angleSquared(particles[i],particles[j]), half_beta)/norm;
+ }
+ }
+ return answer;
+ }
+
+
+ // if N > 4, then throw error
+ if (_N > 5) {
+ throw Error("EnergyCorrelatorGeneralized is only hard coded for N = 0,1,2,3,4,5");
+ }
+
+ // Now deal with N = 3,4,5. Different options if storage array is used or not.
+ if (_strategy == EnergyCorrelator::storage_array) {
+
+ // For N > 2, fill static storage array to save computation time.
+
+ unsigned int nC = particles.size();
+ // Make energy storage
+// double energyStore[nC];
+ double *energyStore = new double[nC];
+
+ // Make angular storage
+// double angleStore[nC][nC];
+ double **angleStore = new double*[nC];
+
+ precompute_energies_and_angles(particles, energyStore, angleStore);
+
+ unsigned int n_angles = _angles;
+ if (_angles < 0) {
+ n_angles = N_total;
+ }
+
+ // now do recursion
+ if (_N == 3) {
+ answer = evaluate_n3(nC, n_angles, energyStore, angleStore) / norm;
+ } else if (_N == 4) {
+ answer = evaluate_n4(nC, n_angles, energyStore, angleStore) / norm;
+ } else if (_N == 5) {
+ answer = evaluate_n5(nC, n_angles, energyStore, angleStore) / norm;
+ } else {
+ assert(_N <= 5);
+ }
+ // Deleting arrays
+ delete[] energyStore;
+
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ delete[] angleStore[i];
+ }
+ delete[] angleStore;
+ } else if (_strategy == EnergyCorrelator::slow) {
+ if (_N == 3) {
+ unsigned int N_total = 3;
+ double angle1, angle2, angle3;
+ double angle;
+
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) {
+ for (unsigned int k = j + 1; k < particles.size(); k++) {
+
+ angle1 = angleSquared(particles[i], particles[j]);
+ angle2 = angleSquared(particles[i], particles[k]);
+ angle3 = angleSquared(particles[j], particles[k]);
+
+ if (_angles == -1){
+ angle = angle1*angle2*angle3;
+ } else {
+ double angle_list[] = {angle1, angle2, angle3};
+ std::vector<double> angle_vector(angle_list, angle_list + N_total);
+ std::sort(angle_vector.begin(), angle_vector.begin() + N_total);
+
+ angle = angle_vector[0];
+ for ( int l = 1; l < _angles; l++) { angle = angle * angle_vector[l]; }
+ }
+ answer += energy(particles[i])
+ * energy(particles[j])
+ * energy(particles[k])
+ * pow(angle, half_beta) /norm;
+ }
+ }
+ }
+ } else if (_N == 4) {
+ double angle1, angle2, angle3, angle4, angle5, angle6;
+ unsigned int N_total = 6;
+ double angle;
+
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) {
+ for (unsigned int k = j + 1; k < particles.size(); k++) {
+ for (unsigned int l = k + 1; l < particles.size(); l++) {
+
+ angle1 = angleSquared(particles[i], particles[j]);
+ angle2 = angleSquared(particles[i], particles[k]);
+ angle3 = angleSquared(particles[i], particles[l]);
+ angle4 = angleSquared(particles[j], particles[k]);
+ angle5 = angleSquared(particles[j], particles[l]);
+ angle6 = angleSquared(particles[k], particles[l]);
+
+ if(_angles == -1) {
+ angle = angle1*angle2*angle3*angle4*angle5*angle6;
+ } else {
+
+ double angle_list[] = {angle1, angle2, angle3, angle4, angle5, angle6};
+ std::vector<double> angle_vector(angle_list, angle_list + N_total);
+ std::sort(angle_vector.begin(), angle_vector.begin() + N_total);
+
+ angle = angle_vector[0];
+ for ( int s = 1; s < _angles; s++) { angle = angle * angle_vector[s]; }
+
+ }
+ answer += energy(particles[i])
+ * energy(particles[j])
+ * energy(particles[k])
+ * energy(particles[l])
+ * pow(angle, half_beta)/norm;
+ }
+ }
+ }
+ }
+ } else if (_N == 5) {
+ double angle1, angle2, angle3, angle4, angle5, angle6, angle7, angle8, angle9, angle10;
+ unsigned int N_total = 10;
+ double angle;
+
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) {
+ for (unsigned int k = j + 1; k < particles.size(); k++) {
+ for (unsigned int l = k + 1; l < particles.size(); l++) {
+ for (unsigned int m = l + 1; m < particles.size(); m++) {
+
+ angle1 = angleSquared(particles[i], particles[j]);
+ angle2 = angleSquared(particles[i], particles[k]);
+ angle3 = angleSquared(particles[i], particles[l]);
+ angle4 = angleSquared(particles[j], particles[k]);
+ angle5 = angleSquared(particles[j], particles[l]);
+ angle6 = angleSquared(particles[k], particles[l]);
+ angle7 = angleSquared(particles[m], particles[i]);
+ angle8 = angleSquared(particles[m], particles[j]);
+ angle9 = angleSquared(particles[m], particles[k]);
+ angle10 = angleSquared(particles[m], particles[l]);
+
+ if (_angles == -1){
+ angle = angle1*angle2*angle3*angle4*angle5*angle6*angle7*angle8*angle9*angle10;
+ } else {
+ double angle_list[] = {angle1, angle2, angle3, angle4, angle5, angle6,
+ angle7, angle8, angle9, angle10};
+ std::vector<double> angle_vector(angle_list, angle_list + N_total);
+ std::sort(angle_vector.begin(), angle_vector.begin() + N_total);
+
+ angle = angle_vector[0];
+ for ( int s = 1; s < _angles; s++) { angle = angle * angle_vector[s]; }
+ }
+ answer += energy(particles[i])
+ * energy(particles[j])
+ * energy(particles[k])
+ * energy(particles[l])
+ * energy(particles[m])
+ * pow(angle, half_beta) /norm;
+ }
+ }
+ }
+ }
+ }
+ } else {
+ assert(_N <= 5);
+ }
+ } else {
+ assert(_strategy == EnergyCorrelator::slow || _strategy == EnergyCorrelator::storage_array);
+ }
+ return answer;
+ }
+
+
+ std::vector<double> EnergyCorrelatorGeneralized::result_all_angles(const PseudoJet& jet) const {
+
+ // if jet does not have constituents, throw error
+ if (!jet.has_constituents()) throw Error("EnergyCorrelator called on jet with no constituents.");
+
+ // Throw an error if N < 1
+ if (_N < 1 ) throw Error("N cannot be negative or zero");
+
+ // get the N = 1 case out of the way
+ if (_N == 1) {
+ std::vector<double> ans (1, 1.0);
+ return ans;
+ }
+
+ // find constituents
+ std::vector<fastjet::PseudoJet> particles = jet.constituents();
+
+ // return zero if the number of constituents is less than _N for the ECFG
+ if (particles.size() < _N) {
+ std::vector<double> ans (_N, 0.0);
+ return ans;
+ }
+
+ // The normalization is the energy or pt of the jet, which is also ECF(1, beta)
+ double EJ = _helper_correlator.result(jet);
+
+ // The overall normalization
+ double norm = pow(EJ, _N);
+
+ // Find the max number of angles and throw an error if it unsuitable
+ int N_total = _N * (_N - 1)/2;
+
+ double half_beta = _beta/2.0;
+
+ // take care of N = 2 case.
+ if (_N == 2) {
+ double answer = 0.0;
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) { //note offset by one so that angle is never called on identical pairs
+ answer += energy(particles[i])
+ * energy(particles[j])
+ * pow(angleSquared(particles[i],particles[j]), half_beta)/norm;
+ }
+ }
+ std::vector<double> ans(N_total, answer);
+ return ans;
+ }
+
+ // Prepare the answer vector
+ std::vector<double> ans (N_total, 0.0);
+ // if N > 4, then throw error
+ if (_N > 5) {
+ throw Error("EnergyCorrelatorGeneralized is only hard coded for N = 0,1,2,3,4,5");
+ }
+
+ // Now deal with N = 3,4,5. Different options if storage array is used or not.
+ if (_strategy == EnergyCorrelator::storage_array) {
+
+ // For N > 2, fill static storage array to save computation time.
+
+ // Make energy storage
+ std::vector<double> energyStore;
+ energyStore.resize(particles.size());
+
+ // Make angular storage
+ std::vector < std::vector<double> > angleStore;
+ angleStore.resize(particles.size());
+ for (unsigned int i = 0; i < angleStore.size(); i++) {
+ angleStore[i].resize(i);
+ }
+
+ // Fill storage with energy/angle information
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ energyStore[i] = energy(particles[i]);
+ for (unsigned int j = 0; j < i; j++) {
+ if (half_beta == 1){
+ angleStore[i][j] = angleSquared(particles[i], particles[j]);
+ } else {
+ angleStore[i][j] = pow(angleSquared(particles[i], particles[j]), half_beta);
+ }
+ }
+ }
+
+ // now do recursion
+ if (_N == 3) {
+ double angle1, angle2, angle3;
+
+ for (unsigned int i = 2; i < particles.size(); i++) {
+ for (unsigned int j = 1; j < i; j++) {
+ for (unsigned int k = 0; k < j; k++) {
+
+ angle1 = angleStore[i][j];
+ angle2 = angleStore[i][k];
+ angle3 = angleStore[j][k];
+
+ double angle_list[] = {angle1, angle2, angle3};
+ std::vector<double> angle_vector(angle_list, angle_list + N_total);
+ std::sort(angle_vector.begin(), angle_vector.begin() + N_total);
+
+ std::vector<double> final_angles (N_total, angle_vector[0]);
+
+ double z_product = energyStore[i] * energyStore[j] * energyStore[k]/norm;
+ ans[0] += z_product * final_angles[0];
+ for ( int s=1 ; s<N_total; s++){
+ final_angles[s] = final_angles[s-1]*angle_vector[s];
+ ans[s] += z_product * final_angles[s];
+ }
+ }
+ }
+ }
+ } else if (_N == 4) {
+ double angle1, angle2, angle3, angle4, angle5, angle6;
+
+ for (unsigned int i = 3; i < particles.size(); i++) {
+ for (unsigned int j = 2; j < i; j++) {
+ for (unsigned int k = 1; k < j; k++) {
+ for (unsigned int l = 0; l < k; l++) {
+
+ angle1 = angleStore[i][j];
+ angle2 = angleStore[i][k];
+ angle3 = angleStore[i][l];
+ angle4 = angleStore[j][k];
+ angle5 = angleStore[j][l];
+ angle6 = angleStore[k][l];
+
+ double angle_list[] = {angle1, angle2, angle3, angle4, angle5, angle6};
+ std::vector<double> angle_vector(angle_list, angle_list + N_total);
+ std::sort(angle_vector.begin(), angle_vector.begin() + N_total);
+
+ std::vector<double> final_angles (N_total, angle_vector[0]);
+
+ double z_product = energyStore[i] * energyStore[j] * energyStore[k] * energyStore [l]/norm;
+ ans[0] += z_product * final_angles[0];
+ for ( int s=1 ; s<N_total; s++){
+ final_angles[s] = final_angles[s-1]*angle_vector[s];
+ ans[s] += z_product * final_angles[s];
+ }
+ }
+ }
+ }
+ }
+ } else if (_N == 5) {
+ double angle1, angle2, angle3, angle4, angle5, angle6, angle7, angle8, angle9, angle10;
+
+ for (unsigned int i = 4; i < particles.size(); i++) {
+ for (unsigned int j = 3; j < i; j++) {
+ for (unsigned int k = 2; k < j; k++) {
+ for (unsigned int l = 1; l < k; l++) {
+ for (unsigned int m = 0; m < l; m++) {
+
+ angle1 = angleStore[i][j];
+ angle2 = angleStore[i][k];
+ angle3 = angleStore[i][l];
+ angle4 = angleStore[i][m];
+ angle5 = angleStore[j][k];
+ angle6 = angleStore[j][l];
+ angle7 = angleStore[j][m];
+ angle8 = angleStore[k][l];
+ angle9 = angleStore[k][m];
+ angle10 = angleStore[l][m];
+
+
+ double angle_list[] = {angle1, angle2, angle3, angle4, angle5, angle6,
+ angle7, angle8, angle9, angle10};
+ std::vector<double> angle_vector(angle_list, angle_list + N_total);
+ std::sort(angle_vector.begin(), angle_vector.begin() + N_total);
+
+ std::vector<double> final_angles (N_total, angle_vector[0]);
+
+ double z_product = energyStore[i] * energyStore[j] * energyStore[k]
+ * energyStore[l] * energyStore[m]/norm;
+ ans[0] += z_product * final_angles[0];
+ for ( int s=1 ; s<N_total; s++){
+ final_angles[s] = final_angles[s-1]*angle_vector[s];
+ ans[s] += z_product * final_angles[s];
+ }
+ }
+ }
+ }
+ }
+ }
+
+ } else {
+ assert(_N <= 5);
+ }
+ } else if (_strategy == EnergyCorrelator::slow) {
+ if (_N == 3) {
+ double angle1, angle2, angle3;
+
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) {
+ for (unsigned int k = j + 1; k < particles.size(); k++) {
+
+ angle1 = pow(angleSquared(particles[i], particles[j]), half_beta);
+ angle2 = pow(angleSquared(particles[i], particles[k]), half_beta);
+ angle3 = pow(angleSquared(particles[j], particles[k]), half_beta);
+
+ double angle_list[] = {angle1, angle2, angle3};
+ std::vector<double> angle_vector(angle_list, angle_list + N_total);
+ std::sort(angle_vector.begin(), angle_vector.begin() + N_total);
+
+ std::vector<double> final_angles (N_total, angle_vector[0]);
+
+ double z_product = energy(particles[i])
+ * energy(particles[j])
+ * energy(particles[k])/norm;
+
+ ans[0] += z_product * final_angles[0];
+ for ( int s=1 ; s<N_total; s++){
+ final_angles[s] = final_angles[s-1]*angle_vector[s];
+ ans[s] += z_product * final_angles[s];
+ }
+ }
+ }
+ }
+ } else if (_N == 4) {
+ double angle1, angle2, angle3, angle4, angle5, angle6;
+
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) {
+ for (unsigned int k = j + 1; k < particles.size(); k++) {
+ for (unsigned int l = k + 1; l < particles.size(); l++) {
+
+ angle1 = pow(angleSquared(particles[i], particles[j]), half_beta);
+ angle2 = pow(angleSquared(particles[i], particles[k]), half_beta);
+ angle3 = pow(angleSquared(particles[i], particles[l]), half_beta);
+ angle4 = pow(angleSquared(particles[j], particles[k]), half_beta);
+ angle5 = pow(angleSquared(particles[j], particles[l]), half_beta);
+ angle6 = pow(angleSquared(particles[k], particles[l]), half_beta);
+
+ double angle_list[] = {angle1, angle2, angle3, angle4, angle5, angle6};
+ std::vector<double> angle_vector(angle_list, angle_list + N_total);
+ std::sort(angle_vector.begin(), angle_vector.begin() + N_total);
+
+ std::vector<double> final_angles (N_total, angle_vector[0]);
+
+ double z_product = energy(particles[i])
+ * energy(particles[j])
+ * energy(particles[k])
+ * energy(particles[l])/norm;
+ ans[0] += z_product * final_angles[0];
+ for ( int s=1 ; s<N_total; s++){
+ final_angles[s] = final_angles[s-1]*angle_vector[s];
+ ans[s] += z_product * final_angles[s];
+ }
+ }
+ }
+ }
+ }
+ } else if (_N == 5) {
+ double angle1, angle2, angle3, angle4, angle5, angle6, angle7, angle8, angle9, angle10;
+
+ for (unsigned int i = 0; i < particles.size(); i++) {
+ for (unsigned int j = i + 1; j < particles.size(); j++) {
+ for (unsigned int k = j + 1; k < particles.size(); k++) {
+ for (unsigned int l = k + 1; l < particles.size(); l++) {
+ for (unsigned int m = l + 1; m < particles.size(); m++) {
+
+ angle1 = pow(angleSquared(particles[i], particles[j]), half_beta);
+ angle2 = pow(angleSquared(particles[i], particles[k]), half_beta);
+ angle3 = pow(angleSquared(particles[i], particles[l]), half_beta);
+ angle4 = pow(angleSquared(particles[j], particles[k]), half_beta);
+ angle5 = pow(angleSquared(particles[j], particles[l]), half_beta);
+ angle6 = pow(angleSquared(particles[k], particles[l]), half_beta);
+ angle7 = pow(angleSquared(particles[m], particles[i]), half_beta);
+ angle8 = pow(angleSquared(particles[m], particles[j]), half_beta);
+ angle9 = pow(angleSquared(particles[m], particles[k]), half_beta);
+ angle10 = pow(angleSquared(particles[m], particles[l]), half_beta);
+
+ double angle_list[] = {angle1, angle2, angle3, angle4, angle5, angle6,
+ angle7, angle8, angle9, angle10};
+ std::vector<double> angle_vector(angle_list, angle_list + N_total);
+ std::sort(angle_vector.begin(), angle_vector.begin() + N_total);
+
+ std::vector<double> final_angles (N_total, angle_vector[0]);
+
+ double z_product = energy(particles[i])
+ * energy(particles[j])
+ * energy(particles[k])
+ * energy(particles[l])
+ * energy(particles[m])/norm;
+
+ ans[0] += z_product * final_angles[0];
+ for ( int s=1 ; s<N_total; s++){
+ final_angles[s] = final_angles[s-1]*angle_vector[s];
+ ans[s] += z_product * final_angles[s];
+ }
+ }
+ }
+ }
+ }
+ }
+ } else {
+ assert(_N <= 5);
+ }
+ } else {
+ assert(_strategy == EnergyCorrelator::slow || _strategy == EnergyCorrelator::storage_array);
+ }
+
+ return ans;
+ }
+
+
+ // call _helper_correlator to get energy information
+ double EnergyCorrelatorGeneralized::energy(const PseudoJet& jet) const {
+ return _helper_correlator.energy(jet);
+ }
+
+ // call _helper_correlator to get angle information
+ double EnergyCorrelatorGeneralized::angleSquared(const PseudoJet& jet1, const PseudoJet& jet2) const {
+ return _helper_correlator.angleSquared(jet1, jet2);
+ }
+
+ string EnergyCorrelator::description_parameters() const {
+ ostringstream oss;
+ oss << "N=" << _N << ", beta=" << _beta;
+
+ if (_measure == pt_R) oss << ", pt_R measure";
+ else if (_measure == E_theta) oss << ", E_theta measure";
+ else if (_measure == E_inv) oss << ", E_inv measure";
+ else throw Error("unrecognized measure");
+
+ if (_strategy == slow) oss << " and 'slow' strategy";
+ else if (_strategy == storage_array) oss << " and 'storage_array' strategy";
+ else throw Error("unrecognized strategy");
+
+ return oss.str();
+ }
+
+ string EnergyCorrelator::description_no_N() const {
+ ostringstream oss;
+ oss << "beta=" << _beta;
+
+ if (_measure == pt_R) oss << ", pt_R measure";
+ else if (_measure == E_theta) oss << ", E_theta measure";
+ else if (_measure == E_inv) oss << ", E_inv measure";
+ else throw Error("unrecognized measure");
+
+ if (_strategy == slow) oss << " and 'slow' strategy";
+ else if (_strategy == storage_array) oss << " and 'storage_array' strategy";
+ else throw Error("unrecognized strategy");
+
+ return oss.str();
+ }
+
+ string EnergyCorrelator::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator ECF(N,beta) for ";
+ oss << description_parameters();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorRatio::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator ratio ECF(N+1,beta)/ECF(N,beta) for ";
+ oss << EnergyCorrelator(_N,_beta,_measure,_strategy).description_parameters();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorDoubleRatio::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator double ratio ECF(N-1,beta)ECF(N+1,beta)/ECF(N,beta)^2 for ";
+ oss << EnergyCorrelator(_N,_beta,_measure,_strategy).description_parameters();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorC1::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable C1 ECF(2,beta)/ECF(1,beta)^2 for ";
+ oss << EnergyCorrelator(2,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorC2::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable C2 ECF(3,beta)*ECF(1,beta)/ECF(2,beta)^2 for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorD2::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable D2 ECF(3,beta)*ECF(1,beta)^3/ECF(2,beta)^3 for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorGeneralizedD2::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable D2 ECFN(3,alpha)/ECFN(2,beta)^(3 alpha/beta) for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorNseries::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable N_n ECFG(2,n+1,beta)/ECFG(1,n,beta)^2 for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorMseries::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable M_n ECFG(1,n+1,beta)/ECFG(1,n,beta) for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorN2::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable N2 ECFG(2,3,beta)/ECFG(1,2,beta)^2 for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+
+ string EnergyCorrelatorN3::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable N3 ECFG(2,4,beta)/ECFG(1,3,beta)^2 for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorM2::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable M2 ECFG(1,3,beta)/ECFG(1,2,beta) for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorCseries::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator double ratio ECFN(N-1,beta)ECFN(N+1,beta)/ECFN(N,beta)^2 for ";
+ oss << EnergyCorrelator(_N,_beta,_measure,_strategy).description_parameters();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorUseries::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable U_n ECFG(1,n+1,beta) for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorU1::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable U_1 ECFG(1,2,beta) for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorU2::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable U_2 ECFG(1,3,beta) for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+ string EnergyCorrelatorU3::description() const {
+ ostringstream oss;
+ oss << "Energy Correlator observable U_3 ECFG(1,4,beta) for ";
+ oss << EnergyCorrelator(3,_beta,_measure,_strategy).description_no_N();
+ return oss.str();
+ }
+
+
+} // namespace fjcontrib
+ //FASTJET_END_NAMESPACE
+} // namespace Rivet
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/EnergyCorrelator.hh b/src/Tools/fjcontrib/EnergyCorrelator/EnergyCorrelator.hh
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/EnergyCorrelator.hh
@@ -0,0 +1,1078 @@
+#ifndef __FASTJET_CONTRIB_ENERGYCORRELATOR_HH__
+#define __FASTJET_CONTRIB_ENERGYCORRELATOR_HH__
+
+// EnergyCorrelator Package
+// Questions/Comments? Email the authors.
+// larkoski@mit.edu, lnecib@mit.edu,
+// gavin.salam@cern.ch jthaler@jthaler.net
+//
+// Copyright (c) 2013-2016
+// Andrew Larkoski, Lina Necib Gavin Salam, and Jesse Thaler
+//
+// $Id: EnergyCorrelator.hh 1098 2018-01-07 20:17:52Z linoush $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <fastjet/internal/base.hh>
+#include "fastjet/FunctionOfPseudoJet.hh"
+
+#include <string>
+#include <climits>
+
+FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+namespace contrib{
+
+/// \mainpage EnergyCorrelator contrib
+///
+/// The EnergyCorrelator contrib provides an implementation of energy
+/// correlators and their ratios as described in arXiv:1305.0007 by
+/// Larkoski, Salam and Thaler. Additionally, the ratio observable
+/// D2 described in arXiv:1409.6298 by Larkoski, Moult and Neill
+/// is also included in this contrib. Finally, a generalized version of
+/// the energy correlation functions is added, defined in
+/// arXiv:1609.07483 by Moult, Necib and Thaler, which allow the
+/// definition of the M series, N series, and U series observables.
+/// There is also a generalized version of D2.
+///
+///
+/// <p>There are 4 main classes:
+///
+/// - EnergyCorrelator
+/// - EnergyCorrelatorRatio
+/// - EnergyCorrelatorDoubleRatio
+/// - EnergyCorrelatorGeneralized
+///
+/// <p>There are five classes that define useful combinations of the ECFs.
+///
+/// - EnergyCorrelatorNseries
+/// - EnergyCorrelatorMseries
+/// - EnergyCorrelatorUseries
+/// - EnergyCorrelatorD2
+/// - EnergyCorrelatorGeneralizedD2
+///
+/// <p> There are also aliases for easier access:
+/// - EnergyCorrelatorCseries (same as EnergyCorrelatorDoubleRatio)
+/// - EnergyCorrelatorC1 (EnergyCorrelatorCseries with i=1)
+/// - EnergyCorrelatorC2 (EnergyCorrelatorCseries with i=2)
+/// - EnergyCorrelatorN2 (EnergyCorrelatorNseries with i=2)
+/// - EnergyCorrelatorN3 (EnergyCorrelatorNseries with i=3)
+/// - EnergyCorrelatorM2 (EnergyCorrelatorMseries with i=2)
+/// - EnergyCorrelatorU1 (EnergyCorrelatorUseries with i=1)
+/// - EnergyCorrelatorU2 (EnergyCorrelatorUseries with i=2)
+/// - EnergyCorrelatorU3 (EnergyCorrelatorUseries with i=3)
+///
+/// Each of these classes is a FastJet FunctionOfPseudoJet.
+/// EnergyCorrelatorDoubleRatio (which is equivalent to EnergyCorrelatorCseries)
+/// is in particular is useful for quark/gluon discrimination and boosted
+/// object tagging.
+///
+/// Using the original 2- and 3-point correlators, EnergyCorrelationD2 has
+/// been shown to be the optimal combination for boosted 2-prong tagging.
+///
+/// The EnergyCorrelatorNseries and EnergyCorrelatorMseries use
+/// generalized correlation functions with different angular scaling,
+/// and are intended for use on 2-prong and 3-prong jets.
+/// The EnergyCorrelatorUseries is useful for quark/gluon discrimimation.
+///
+/// See the file example.cc for an illustration of usage and
+/// example_basic_usage.cc for the most commonly used functions.
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelator
+/// ECF(N,beta) is the N-point energy correlation function, with an angular exponent beta.
+///
+/// It is defined as follows
+///
+/// - \f$ \mathrm{ECF}(1,\beta) = \sum_i E_i \f$
+/// - \f$ \mathrm{ECF}(2,\beta) = \sum_{i<j} E_i E_j \theta_{ij}^\beta \f$
+/// - \f$ \mathrm{ECF}(3,\beta) = \sum_{i<j<k} E_i E_j E_k (\theta_{ij} \theta_{ik} \theta_{jk})^\beta \f$
+/// - \f$ \mathrm{ECF}(4,\beta) = \sum_{i<j<k<l} E_i E_j E_k E_l (\theta_{ij} \theta_{ik} \theta_{il} \theta_{jk} \theta_{jl} \theta_{kl})^\beta \f$
+/// - ...
+///
+/// The correlation can be determined with energies and angles (as
+/// given above) or with transverse momenta and boost invariant angles
+/// (the code's default). The choice is controlled by
+/// EnergyCorrelator::Measure provided in the constructor.
+///
+/// The current implementation handles values of N up to and including 5.
+/// Run times scale as n^N/N!, where n is the number of particles in a jet.
+
+ class EnergyCorrelator : public FunctionOfPseudoJet<double> {
+ friend class EnergyCorrelatorGeneralized; ///< This allow ECFG to access the energy and angle definitions
+ ///< of this class, which are otherwise private.
+ public:
+
+ enum Measure {
+ pt_R, ///< use transverse momenta and boost-invariant angles,
+ ///< eg \f$\mathrm{ECF}(2,\beta) = \sum_{i<j} p_{ti} p_{tj} \Delta R_{ij}^{\beta} \f$
+ E_theta, /// use energies and angles,
+ /// eg \f$\mathrm{ECF}(2,\beta) = \sum_{i<j} E_{i} E_{j} \theta_{ij}^{\beta} \f$
+ E_inv /// use energies and invariant mass,
+ /// eg \f$\mathrm{ECF}(2,\beta) = \sum_{i<j} E_{i} E_{j} (\frac{2 p_{i} \cdot p_{j}}{E_{i} E_{j}})^{\beta/2} \f$
+ };
+
+ enum Strategy {
+ slow, ///< interparticle angles are not cached.
+ ///< For N>=3 this leads to many expensive recomputations,
+ ///< but has only O(n) memory usage for n particles
+
+ storage_array /// the interparticle angles are cached. This gives a significant speed
+ /// improvement for N>=3, but has a memory requirement of (4n^2) bytes.
+ };
+
+ public:
+
+ /// constructs an N-point correlator with angular exponent beta,
+ /// using the specified choice of energy and angular measure as well
+ /// one of two possible underlying computational Strategy
+ EnergyCorrelator(unsigned int N,
+ double beta,
+ Measure measure = pt_R,
+ Strategy strategy = storage_array) :
+ _N(N), _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ /// destructor
+ virtual ~EnergyCorrelator(){}
+
+ /// returns the value of the energy correlator for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ /// returns the the part of the description related to the parameters
+ std::string description_parameters() const;
+ std::string description_no_N() const;
+
+ private:
+
+ unsigned int _N;
+ double _beta;
+ Measure _measure;
+ Strategy _strategy;
+
+ double energy(const PseudoJet& jet) const;
+ double angleSquared(const PseudoJet& jet1, const PseudoJet& jet2) const;
+ double multiply_angles(double angles[], int n_angles, unsigned int N_total) const;
+ void precompute_energies_and_angles(std::vector<fastjet::PseudoJet> const &particles, double* energyStore, double** angleStore) const;
+ double evaluate_n3(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ double evaluate_n4(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ double evaluate_n5(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ };
+
+// core EnergyCorrelator::result code in .cc file.
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorRatio
+/// A class to calculate the ratio of (N+1)-point to N-point energy correlators,
+/// ECF(N+1,beta)/ECF(N,beta),
+/// called \f$ r_N^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorRatio : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an (N+1)-point to N-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorRatio(unsigned int N,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _N(N), _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorRatio() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _N;
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+ inline double EnergyCorrelatorRatio::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelator(_N + 1, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelator(_N, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorDoubleRatio
+/// Calculates the double ratio of energy correlators, ECF(N-1,beta)*ECF(N+1)/ECF(N,beta)^2.
+///
+/// A class to calculate a double ratio of energy correlators,
+/// ECF(N-1,beta)*ECF(N+1,beta)/ECF(N,beta)^2,
+/// called \f$C_N^{(\beta)}\f$ in the publication, and equal to
+/// \f$ r_N^{(\beta)}/r_{N-1}^{(\beta)} \f$.
+///
+
+ class EnergyCorrelatorDoubleRatio : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ EnergyCorrelatorDoubleRatio(unsigned int N,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _N(N), _beta(beta), _measure(measure), _strategy(strategy) {
+
+ if (_N < 1) throw Error("EnergyCorrelatorDoubleRatio: N must be 1 or greater.");
+
+ };
+
+ virtual ~EnergyCorrelatorDoubleRatio() {}
+
+
+ /// returns the value of the energy correlator double-ratio for a
+ /// jet's constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _N;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorDoubleRatio::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelator(_N - 1, _beta, _measure, _strategy).result(jet) * EnergyCorrelator(_N + 1, _beta, _measure, _strategy).result(jet);
+ double denominator = pow(EnergyCorrelator(_N, _beta, _measure, _strategy).result(jet), 2.0);
+
+ return numerator/denominator;
+
+ }
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorC1
+/// A class to calculate the normalized 2-point energy correlators,
+/// ECF(2,beta)/ECF(1,beta)^2,
+/// called \f$ C_1^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorC1 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorC1(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorC1() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorC1::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelator(2, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelator(1, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorC2
+/// A class to calculate the double ratio of 3-point to 2-point
+/// energy correlators,
+/// ECF(3,beta)*ECF(1,beta)/ECF(2,beta)^2,
+/// called \f$ C_2^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorC2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a 3-point to 2-point correlator double ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorC2(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorC2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorC2::result(const PseudoJet& jet) const {
+
+ double numerator3 = EnergyCorrelator(3, _beta, _measure, _strategy).result(jet);
+ double numerator1 = EnergyCorrelator(1, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelator(2, _beta, _measure, _strategy).result(jet);
+
+ return numerator3*numerator1/denominator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorD2
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// ECF(3,beta)*ECF(1,beta)^3/ECF(2,beta)^3,
+/// called \f$ D_2^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorD2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorD2(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorD2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorD2::result(const PseudoJet& jet) const {
+
+ double numerator3 = EnergyCorrelator(3, _beta, _measure, _strategy).result(jet);
+ double numerator1 = EnergyCorrelator(1, _beta, _measure, _strategy).result(jet);
+ double denominator2 = EnergyCorrelator(2, _beta, _measure, _strategy).result(jet);
+
+ return numerator3*numerator1*numerator1*numerator1/denominator2/denominator2/denominator2;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorGeneralized
+/// A generalized and normalized version of the N-point energy correlators, with
+/// angular exponent beta and v number of pairwise angles. When \f$v = {N \choose 2}\f$
+/// (or, for convenience, \f$v = -1\f$), EnergyCorrelatorGeneralized just gives normalized
+/// versions of EnergyCorrelator:
+/// - \f$ \mathrm{ECFG}(-1,1,\beta) = \mathrm{ECFN}(N,\beta) = \mathrm{ECF}(N,\beta)/\mathrm{ECF}(1,\beta)\f$
+///
+/// Note that there is no separate class that implements ECFN, though it is a
+/// notation that we will use in this documentation. Examples of the low-point normalized
+/// correlators are:
+/// - \f$\mathrm{ECFN}(1,\beta) = 1\f$
+/// - \f$\mathrm{ECFN}(2,\beta) = \sum_{i<j} z_i z_j \theta_{ij}^\beta \f$
+/// - \f$\mathrm{ECFN}(3,\beta) = \sum_{i<j<k} z_i z_j z_k (\theta_{ij} \theta_{ik} \theta_{jk})^\beta \f$
+/// - \f$\mathrm{ECFN}(4,\beta) = \sum_{i<j<k<l} z_i z_j z_k z_l (\theta_{ij} \theta_{ik} \theta_{il} \theta_{jk} \theta_{jl} \theta_{kl})^\beta \f$
+/// - ...
+/// where the \f$z_i\f$'s are the energy fractions.
+///
+/// When a new value of v is given, the generalized energy correlators are defined as
+/// - \f$\mathrm{ECFG}(0,1,\beta) = 1\f$
+/// - \f$\mathrm{ECFG}(1,2,\beta) = \sum_{i<j} z_i z_j \theta_{ij}^\beta \f$
+/// - \f$\mathrm{ECFG}(v,3,\beta) = \sum_{i<j<k} z_i z_j z_k \prod_{m = 1}^{v} \min^{(m)} \{ \theta_{ij}, \theta_{jk}, \theta_{ki} \}^\beta \f$
+/// - \f$\mathrm{ECFG}(v,4,\beta) = \sum_{i<j<k<l} z_i z_j z_k z_l \prod_{m = 1}^{v} \min^{(m)} \{ \theta_{ij}, \theta_{ik}, \theta_{il}, \theta_{jk}, \theta_{jl}, \theta_{kl} \}^\beta \f$
+/// - \f$\mathrm{ECFG}(v,n,\beta) = \sum_{i_1 < i_2 < \dots < i_n} z_{i_1} z_{i_2} \dots z_{i_n} \prod_{m = 1}^{v} \min^{(m)}_{s < t \in \{i_1, i_2 , \dots, i_n \}} \{ \theta_{st}^{\beta} \}\f$,
+///
+/// where \f$\min^{(m)}\f$ means the m-th smallest element of the list.
+///
+/// The correlation can be determined with energies and angles (as
+/// given above) or with transverse momenta and boost invariant angles
+/// (the code's default). The choice is controlled by
+/// EnergyCorrelator::Measure provided in the constructor.
+///
+/// The current implementation handles values of N up to and including 5.
+///
+ class EnergyCorrelatorGeneralized : public FunctionOfPseudoJet<double> {
+ public:
+
+ /// constructs an N-point correlator with v_angles pairwise angles
+ /// and angular exponent beta,
+ /// using the specified choice of energy and angular measure as well
+ /// one of two possible underlying computational Strategy
+ EnergyCorrelatorGeneralized(int v_angles,
+ unsigned int N,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _angles(v_angles), _N(N), _beta(beta), _measure(measure), _strategy(strategy), _helper_correlator(1,_beta, _measure, _strategy) {};
+
+ /// destructor
+ virtual ~EnergyCorrelatorGeneralized(){}
+
+ /// returns the value of the normalized energy correlator for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+
+ double result(const PseudoJet& jet) const;
+ std::vector<double> result_all_angles(const PseudoJet& jet) const;
+
+ private:
+
+ int _angles;
+ unsigned int _N;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+ EnergyCorrelator _helper_correlator;
+
+ double energy(const PseudoJet& jet) const;
+ double angleSquared(const PseudoJet& jet1, const PseudoJet& jet2) const;
+ double multiply_angles(double angles[], int n_angles, unsigned int N_total) const;
+ void precompute_energies_and_angles(std::vector<fastjet::PseudoJet> const &particles, double* energyStore, double** angleStore) const;
+ double evaluate_n3(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ double evaluate_n4(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ double evaluate_n5(unsigned int nC, unsigned int n_angles, double* energyStore, double** angleStore) const;
+ };
+
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorGeneralizedD2
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// ECFN(3,alpha)/ECFN(2,beta)^3 alpha/beta,
+/// called \f$ D_2^{(\alpha, \beta)} \f$ in the publication.
+ class EnergyCorrelatorGeneralizedD2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorGeneralizedD2(
+ double alpha,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _alpha(alpha), _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorGeneralizedD2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _alpha;
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorGeneralizedD2::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelatorGeneralized(-1, 3, _alpha, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(-1, 2, _beta, _measure, _strategy).result(jet);
+
+ return numerator/pow(denominator, 3.0*_alpha/_beta);
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorNseries
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// N_n = ECFG(2,n+1,beta)/ECFG(1,n,beta)^2,
+/// called \f$ N_i^{(\alpha, \beta)} \f$ in the publication.
+/// By definition, N_1^{beta} = ECFG(1, 2, 2*beta), where the angular exponent
+/// is twice as big since the N series should involve two pairwise angles.
+ class EnergyCorrelatorNseries : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a n 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorNseries(
+ unsigned int n,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _n(n), _beta(beta), _measure(measure), _strategy(strategy) {
+
+ if (_n < 1) throw Error("EnergyCorrelatorNseries: n must be 1 or greater.");
+
+ };
+
+ virtual ~EnergyCorrelatorNseries() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _n;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+ };
+
+
+ inline double EnergyCorrelatorNseries::result(const PseudoJet& jet) const {
+
+ if (_n == 1) return EnergyCorrelatorGeneralized(1, 2, 2*_beta, _measure, _strategy).result(jet);
+ // By definition, N1 = ECFN(2, 2 beta)
+ double numerator = EnergyCorrelatorGeneralized(2, _n + 1, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(1, _n, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator/denominator;
+
+ }
+
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorN2
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// ECFG(2,3,beta)/ECFG(1,2,beta)^2,
+/// called \f$ N_2^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorN2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorN2(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorN2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorN2::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelatorGeneralized(2, 3, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(1, 2, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorN3
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// ECFG(2,4,beta)/ECFG(1,3,beta)^2,
+/// called \f$ N_3^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorN3 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorN3(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorN3() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorN3::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelatorGeneralized(2, 4, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(1, 3, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorMseries
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// M_n = ECFG(1,n+1,beta)/ECFG(1,n,beta),
+/// called \f$ M_i^{(\alpha, \beta)} \f$ in the publication.
+/// By definition, M_1^{beta} = ECFG(1,2,beta)
+ class EnergyCorrelatorMseries : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a n 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorMseries(
+ unsigned int n,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _n(n), _beta(beta), _measure(measure), _strategy(strategy) {
+
+ if (_n < 1) throw Error("EnergyCorrelatorMseries: n must be 1 or greater.");
+
+ };
+
+ virtual ~EnergyCorrelatorMseries() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _n;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+ };
+
+
+ inline double EnergyCorrelatorMseries::result(const PseudoJet& jet) const {
+
+ if (_n == 1) return EnergyCorrelatorGeneralized(1, 2, _beta, _measure, _strategy).result(jet);
+
+ double numerator = EnergyCorrelatorGeneralized(1, _n + 1, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(1, _n, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator;
+
+ }
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorM2
+/// A class to calculate the observable formed from the ratio of the
+/// 3-point and 2-point energy correlators,
+/// ECFG(1,3,beta)/ECFG(1,2,beta),
+/// called \f$ M_2^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorM2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs an 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorM2(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorM2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorM2::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelatorGeneralized(1, 3, _beta, _measure, _strategy).result(jet);
+ double denominator = EnergyCorrelatorGeneralized(1, 2, _beta, _measure, _strategy).result(jet);
+
+ return numerator/denominator;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorCseries
+/// Calculates the C series energy correlators, ECFN(N-1,beta)*ECFN(N+1,beta)/ECFN(N,beta)^2.
+/// This is equivalent to EnergyCorrelatorDoubleRatio
+///
+/// A class to calculate a double ratio of energy correlators,
+/// ECFN(N-1,beta)*ECFN(N+1,beta)/ECFN(N,beta)^2,
+/// called \f$C_N^{(\beta)}\f$ in the publication, and equal to
+/// \f$ r_N^{(\beta)}/r_{N-1}^{(\beta)} \f$.
+///
+
+ class EnergyCorrelatorCseries : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ EnergyCorrelatorCseries(unsigned int N,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _N(N), _beta(beta), _measure(measure), _strategy(strategy) {
+
+ if (_N < 1) throw Error("EnergyCorrelatorCseries: N must be 1 or greater.");
+
+ };
+
+ virtual ~EnergyCorrelatorCseries() {}
+
+
+ /// returns the value of the energy correlator double-ratio for a
+ /// jet's constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _N;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorCseries::result(const PseudoJet& jet) const {
+
+ double numerator = EnergyCorrelatorGeneralized(-1, _N - 1, _beta, _measure, _strategy).result(jet) * EnergyCorrelatorGeneralized(-1, _N + 1, _beta, _measure, _strategy).result(jet);
+ double denominator = pow(EnergyCorrelatorGeneralized(-1, _N, _beta, _measure, _strategy).result(jet), 2.0);
+
+ return numerator/denominator;
+
+ }
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorUseries
+/// A class to calculate the observable used for quark versus gluon discrimination
+/// U_n = ECFG(1,n+1,beta),
+/// called \f$ U_i^{(\beta)} \f$ in the publication.
+
+ class EnergyCorrelatorUseries : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a n 3-point to 2-point correlator ratio with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorUseries(
+ unsigned int n,
+ double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _n(n), _beta(beta), _measure(measure), _strategy(strategy) {
+
+ if (_n < 1) throw Error("EnergyCorrelatorUseries: n must be 1 or greater.");
+
+ };
+
+ virtual ~EnergyCorrelatorUseries() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ unsigned int _n;
+ double _beta;
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+ };
+
+
+ inline double EnergyCorrelatorUseries::result(const PseudoJet& jet) const {
+
+ double answer = EnergyCorrelatorGeneralized(1, _n + 1, _beta, _measure, _strategy).result(jet);
+ return answer;
+
+ }
+
+
+//------------------------------------------------------------------------
+/// \class EnergyCorrelatorU1
+/// A class to calculate the observable formed from
+/// ECFG(1,2,beta),
+/// called \f$ U_1^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorU1 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a 2-point correlator with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorU1(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorU1() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorU1::result(const PseudoJet& jet) const {
+
+ double answer = EnergyCorrelatorGeneralized(1, 2, _beta, _measure, _strategy).result(jet);
+
+ return answer;
+
+ }
+
+
+ //------------------------------------------------------------------------
+ /// \class EnergyCorrelatorU2
+ /// A class to calculate the observable formed from
+ /// ECFG(1,3,beta),
+ /// called \f$ U_2^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorU2 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a 3-point correlator with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorU2(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorU2() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorU2::result(const PseudoJet& jet) const {
+
+ double answer = EnergyCorrelatorGeneralized(1, 3, _beta, _measure, _strategy).result(jet);
+
+ return answer;
+
+ }
+
+
+ //------------------------------------------------------------------------
+ /// \class EnergyCorrelatorU3
+ /// A class to calculate the observable formed from
+ /// ECFG(1,4,beta),
+ /// called \f$ U_3^{(\beta)} \f$ in the publication.
+ class EnergyCorrelatorU3 : public FunctionOfPseudoJet<double> {
+
+ public:
+
+ /// constructs a 4-point correlator with
+ /// angular exponent beta, using the specified choice of energy and
+ /// angular measure as well one of two possible underlying
+ /// computational strategies
+ EnergyCorrelatorU3(double beta,
+ EnergyCorrelator::Measure measure = EnergyCorrelator::pt_R,
+ EnergyCorrelator::Strategy strategy = EnergyCorrelator::storage_array)
+ : _beta(beta), _measure(measure), _strategy(strategy) {};
+
+ virtual ~EnergyCorrelatorU3() {}
+
+ /// returns the value of the energy correlator ratio for a jet's
+ /// constituents. (Normally accessed by the parent class's
+ /// operator()).
+ double result(const PseudoJet& jet) const;
+
+ std::string description() const;
+
+ private:
+
+ double _beta;
+
+ EnergyCorrelator::Measure _measure;
+ EnergyCorrelator::Strategy _strategy;
+
+
+ };
+
+
+ inline double EnergyCorrelatorU3::result(const PseudoJet& jet) const {
+
+ double answer = EnergyCorrelatorGeneralized(1, 4, _beta, _measure, _strategy).result(jet);
+
+ return answer;
+
+ }
+
+
+
+} // namespace contrib
+
+FASTJET_END_NAMESPACE
+
+#endif // __FASTJET_CONTRIB_ENERGYCORRELATOR_HH__
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/Makefile.am b/src/Tools/fjcontrib/EnergyCorrelator/Makefile.am
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/Makefile.am
@@ -0,0 +1,3 @@
+noinst_LTLIBRARIES = libRivetEnergyCorrelator.la
+libRivetEnergyCorrelator_la_SOURCES = EnergyCorrelator.cc
+libRivetEnergyCorrelator_la_CPPFLAGS = $(AM_CPPFLAGS) -I${top_srcdir}/include/Rivet/Tools
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/NEWS b/src/Tools/fjcontrib/EnergyCorrelator/NEWS
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/NEWS
@@ -0,0 +1,14 @@
+2018-02-08: Release of version 1.3.1:
+ Fixing memory leak, functionality unchanged.
+2018-01-09: Release of version 1.3.0:
+ Speed up of core ECF code, functionality unchanged.
+2016-10-07: Release of version 1.2.0:
+ Incorporates the generalized energy correlation functions
+ and adds the NSeries, MSeries, USeries, and GeneralizedD2
+ observables.
+2014-11-13: Release of version 1.1.0:
+ Added the C1, C2, and D2 observables
+2013-05-01: Release of version 1.0.1:
+ Improved error reporting
+2013-04-30: Release of version 1.0.0:
+ Initial release
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/README b/src/Tools/fjcontrib/EnergyCorrelator/README
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/README
@@ -0,0 +1,190 @@
+The EnergyCorrelator package is based on the physics described in:
+
+ Energy Correlation Functions for Jet Substructure.
+ Andrew J. Larkoski, Gavin Salam, and Jesse Thaler.
+ JHEP 1306, 108 (2013)
+ arXiv:1305.0007.
+
+Additional information and a new observable formed from the
+energy correlation functions was described in
+
+ Power Counting to Better Jet Observables.
+ Andrew J. Larkoski, Ian Moult, and Duff Neill.
+ JHEP 1412, 009 (2014)
+ arXiv:1409.6298.
+
+Additional observables based on generalizations of the energy
+correlation functions are described in
+
+ New Angles on Energy Correlation Functions.
+ Ian Moult, Lina Necib, and Jesse Thaler.
+ arXiv:1609.07483.
+
+This FastJet-contrib package contains a number of classes derived from
+FunctionOfPseudoJet<double>.
+
+----------------------------------------------------------------------------
+
+The core classes from 1305.0007, and defined since version 1.0, are:
+
+EnergyCorrelator(int N, double beta, Measure measure)
+
+ Called ECF(N,beta) in arXiv:1305.0007. Corresponds to the N-point
+ correlation function, with beta the angular exponent, while measure
+ = pt_R (default) or E_theta sets how energies and angles are
+ determined.
+
+EnergyCorrelatorRatio(int N, double beta, Measure measure)
+
+ Called r_N^(beta) in arXiv:1305.0007.
+ Equals ECF(N+1,beta)/ECF(N,beta).
+
+EnergyCorrelatorDoubleRatio(int N, double beta, Measure measure)
+
+ Called C_N^(beta) in arXiv:1305.0007. Equals r_N/r_{N-1}. This
+ observable provides good boosted N-prong object discrimination.
+ (N=1 for quark/gluon, N=2 for boosted W/Z/H, N=3 for boosted top)
+ Also given in EnergyCorrelatorCseries as of version 1.2.
+
+----------------------------------------------------------------------------
+
+The D2 observable from 1409.6298, as well as C1 and C2 alias classes, were
+added in version 1.1:
+
+EnergyCorrelatorC1(double beta, Measure measure)
+
+ This calculates the double ratio observable C_1^(beta) which is
+ useful for quark versus gluon discrimination.
+
+EnergyCorrelatorC2(double beta, Measure measure)
+
+ This calculates the double ratio observable C_2^(beta) which is
+ useful for boosted W/Z/H identification.
+
+EnergyCorrelatorD2(double beta, Measure measure)
+
+ Called D_2^(beta) in arXiv:1409.6298.
+ Equals ECF(3,beta)*ECF(1,beta)^3/ECF(2,beta)^3.
+ This is the recommended function for boosted 2-prong object
+ discrimination (boosted W/Z/H).
+
+----------------------------------------------------------------------------
+
+Generalized energy correlators were introduced in 1609.07483 and appear in
+version 1.2. They are defined in the class:
+
+EnergyCorrelatorGeneralized(int angles, int N, double beta, Measure measure)
+
+ Called {}_v e_n^{(beta)} in 1609.07483, but will be denoted here as
+ ECFG(angles,N,beta), where v=angles and n=N. As for EnergyCorrelator,
+ beta is the angular exponent, while measure = pt_R (default) or E_theta
+ sets how energies and angles are determined. The integer angles
+ determines the number of angles in the observable. The choice angles=-1
+ sets angles = N choose 2, which corresponds to the N-point
+ normalized (dimensionless) correlation function, with
+ ECFN(N,beta) = ECFG(N choose 2,N,beta) = ECF(N,beta)/ECF(1,beta)^N
+
+From the generalized correlators, a variety of useful ratios are defined.
+They are mainly organized by series, with special values highlighted for
+recommended usage.
+
+----------------------------------------------------------------------------
+
+EnergyCorrelatorGeneralizedD2(double alpha, double beta, Measure measure)
+
+ Called D_2^(alpha, beta) in arXiv:1609.07483
+ Equals ECFN(3,alpha)/ECFN(2,beta)^(3 alpha/beta).
+ Useful for groomed 2-prong object tagging. We recommend the use of alpha=1
+ and beta=2.
+
+----------------------------------------------------------------------------
+
+EnergyCorrelatorNseries(int i, double beta, Measure measure)
+
+ Called N_i^(beta) in arXiv:1609.07483
+ Equals ECFG(2,n+1,beta)/ECFN(1,n,beta)^2.
+
+EnergyCorrelatorN2(double beta, Measure measure)
+
+ Called N_2^(beta) in arXiv:1609.07483
+ Equals ECFG(2,3,beta)/ECFG(1,2,beta)^2.
+ Useful for groomed and ungroomed 2-prong object tagging.
+
+EnergyCorrelatorN3(double beta, Measure measure)
+
+ Called N_3^(beta) in arXiv:1609.07483
+ Equals ECFG(2,4,beta)/ECFG(1,3,beta)^2.
+ Useful for groomed 3-prong object tagging.
+
+----------------------------------------------------------------------------
+
+EnergyCorrelatorMseries(int i, double beta, Measure measure)
+
+ Called M_i^(beta) in arXiv:1609.07483
+ Equals ECFG(1,n+1,beta)/ECFG(1,n,beta).
+
+EnergyCorrelatorM2(double beta, Measure measure)
+
+ Called M_2^(beta) in arXiv:1609.07483
+ Equals ECFG(1,3,beta)/ECFG(1,2,beta).
+ Useful for groomed 2-prong object tagging.
+
+
+----------------------------------------------------------------------------
+
+EnergyCorrelatorUseries(int i, double beta, Measure measure)
+
+ Called U_i^(beta) in arXiv:1609.07483
+ Equals ECFG(1,n+1,beta).
+
+EnergyCorrelatorU1(double beta, Measure measure)
+
+ Called U_1^(beta) in arXiv:1609.07483
+ Equals ECFG(1,2,beta).
+ Useful for quark vs. gluon discrimination.
+
+EnergyCorrelatorU2(double beta, Measure measure)
+
+ Called U_2^(beta) in arXiv:1609.07483
+ Equals ECFG(1,3,beta).
+ Useful for quark vs. gluon discrimination.
+
+EnergyCorrelatorU3(double beta, Measure measure)
+
+ Called U_3^(beta) in arXiv:1609.07483
+ Equals ECFG(1,4,beta).
+ Useful for quark vs. gluon discrimination.
+----------------------------------------------------------------------------
+
+The argument Measure in each of the above functions sets how energies
+and angles are defined in the observable. The measure
+
+ pt_R
+
+uses hadron collider coordinates (transverse momenta and boost-invariant
+angles). The "energy" in this case is defined as the pT of the jet,
+and the "angle" is the distance between the jets in phi, eta space.
+
+The measure
+
+ E_theta
+
+uses particle energies and angles and is appropriate for e+e-
+collider applications. The "energy" is the jet energy and the angle
+between 2 jets is computed from the dot product of the 3 vectors p1 and p2.
+
+The measure
+
+ E_inv
+
+uses particle energies and angles and is also appropriate for e+e-
+collider applications. In this case “theta” is replaced by Mandelstam
+invariants with the same behavior in the collinear limits, leading to a more
+calculation friendly observables. The "energy" is defined as the jet energy
+and the "angle squared" is defined as (2p_i \cdot p_j/E_i E_j),
+where p_i,p_j are the momenta of the jets i adn j, and E_i, E_j are their
+respective energies.
+
+General usage is shown in the example.cc program, and recommended usage
+is shown in example_basic_usage.cc.
+
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/VERSION b/src/Tools/fjcontrib/EnergyCorrelator/VERSION
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/VERSION
@@ -0,0 +1,1 @@
+1.3.1
\ No newline at end of file
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/example.cc b/src/Tools/fjcontrib/EnergyCorrelator/example.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/example.cc
@@ -0,0 +1,686 @@
+// Example showing usage of energy correlator classes.
+//
+// Compile it with "make example" and run it with
+//
+// ./example < ../data/single-event.dat
+//
+// Copyright (c) 2013-2016
+// Andrew Larkoski, Lina Necib, Gavin Salam, and Jesse Thaler
+//
+// $Id: example.cc 1097 2018-01-05 00:04:20Z linoush $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iomanip>
+#include <stdlib.h>
+#include <stdio.h>
+#include <ctime>
+#include <iostream>
+#include <istream>
+#include <fstream>
+#include <sstream>
+#include <string>
+
+#include "fastjet/PseudoJet.hh"
+#include "fastjet/ClusterSequence.hh"
+#include "fastjet/JetDefinition.hh"
+
+#include <sstream>
+#include "EnergyCorrelator.hh" // In external code, this should be fastjet/contrib/EnergyCorrelator.hh
+
+using namespace std;
+using namespace fastjet;
+using namespace fastjet::contrib;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &event);
+void analyze(const vector<PseudoJet> & input_particles);
+
+//----------------------------------------------------------------------
+int main(){
+
+ //----------------------------------------------------------
+ // read in input particles
+ vector<PseudoJet> event;
+ read_event(event);
+ cout << "# read an event with " << event.size() << " particles" << endl;
+
+ //----------------------------------------------------------
+ // illustrate how this EnergyCorrelator contrib works
+
+ analyze(event);
+
+ return 0;
+}
+
+// read in input particles
+void read_event(vector<PseudoJet> &event){
+ string line;
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {return;}
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ event.push_back(particle);
+ }
+}
+
+////////
+//
+// Main Routine for Analysis
+//
+///////
+
+void analyze(const vector<PseudoJet> & input_particles) {
+
+ /////// EnergyCorrelator /////////////////////////////
+
+ // Initial clustering with anti-kt algorithm
+ JetAlgorithm algorithm = antikt_algorithm;
+ double jet_rad = 1.00; // jet radius for anti-kt algorithm
+ JetDefinition jetDef = JetDefinition(algorithm,jet_rad,E_scheme,Best);
+ ClusterSequence clust_seq(input_particles,jetDef);
+ vector<PseudoJet> antikt_jets = sorted_by_pt(clust_seq.inclusive_jets());
+
+ for (int j = 0; j < 2; j++) { // Two hardest jets per event
+ if (antikt_jets[j].perp() > 200) {
+
+ PseudoJet myJet = antikt_jets[j];
+
+ // various values of beta
+ vector<double> betalist;
+ betalist.push_back(0.1);
+ betalist.push_back(0.2);
+ betalist.push_back(0.5);
+ betalist.push_back(1.0);
+ betalist.push_back(1.5);
+ betalist.push_back(2.0);
+
+ // various values of alpha
+ vector<double> alphalist;
+ alphalist.push_back(0.1);
+ alphalist.push_back(0.2);
+ alphalist.push_back(0.5);
+ alphalist.push_back(1.0);
+
+
+ // checking the two energy/angle modes
+ vector<EnergyCorrelator::Measure> measurelist;
+ measurelist.push_back(EnergyCorrelator::pt_R);
+ measurelist.push_back(EnergyCorrelator::E_theta);
+ //measurelist.push_back(EnergyCorrelator::E_inv);
+
+ vector<string> modename;
+ modename.push_back("pt_R");
+ modename.push_back("E_theta");
+ //modename.push_back("E_inv");
+
+ for (unsigned int M = 0; M < measurelist.size(); M++) {
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelator: ECF(N,beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s %14s %14s %14s %15s\n","beta", "N=1 (GeV)", "N=2 (GeV^2)", "N=3 (GeV^3)", "N=4 (GeV^4)", "N=5 (GeV^5)");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelator ECF0(0,beta,measurelist[M]);
+ EnergyCorrelator ECF1(1,beta,measurelist[M]);
+ EnergyCorrelator ECF2(2,beta,measurelist[M]);
+ EnergyCorrelator ECF3(3,beta,measurelist[M]);
+ EnergyCorrelator ECF4(4,beta,measurelist[M]);
+ EnergyCorrelator ECF5(5,beta,measurelist[M]);
+
+ printf("%7.3f %14.2f %14.2f %14.2f %14.2f %15.2f \n",beta,ECF1(myJet),ECF2(myJet),ECF3(myJet),ECF4(myJet),ECF5(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorRatio: r_N^(beta) = ECF(N+1,beta)/ECF(N,beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s %14s %14s %14s %15s \n","beta", "N=0 (GeV)", "N=1 (GeV)", "N=2 (GeV)", "N=3 (GeV)","N=4 (GeV)");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorRatio r0(0,beta,measurelist[M]);
+ EnergyCorrelatorRatio r1(1,beta,measurelist[M]);
+ EnergyCorrelatorRatio r2(2,beta,measurelist[M]);
+ EnergyCorrelatorRatio r3(3,beta,measurelist[M]);
+ EnergyCorrelatorRatio r4(4,beta,measurelist[M]);
+
+ printf("%7.3f %14.4f %14.4f %14.4f %14.4f %15.4f \n",beta,r0(myJet),r1(myJet),r2(myJet),r3(myJet),r4(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorDoubleRatio: C_N^(beta) = r_N^(beta)/r_{N-1}^(beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s %14s %14s %14s \n","beta", "N=1", "N=2", "N=3", "N=4");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorDoubleRatio C1(1,beta,measurelist[M]);
+ EnergyCorrelatorDoubleRatio C2(2,beta,measurelist[M]);
+ EnergyCorrelatorDoubleRatio C3(3,beta,measurelist[M]);
+ EnergyCorrelatorDoubleRatio C4(4,beta,measurelist[M]);
+
+ printf("%7.3f %14.6f %14.6f %14.6f %14.6f \n",beta,C1(myJet),C2(myJet),C3(myJet),C4(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorC1: C_1^(beta) = ECF(2,beta)/ECF(1,beta)^2 with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s \n","beta","C1 obs");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorC1 c1(beta,measurelist[M]);
+
+ printf("%7.3f %14.6f \n",beta,c1(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorC2: C_2^(beta) = ECF(3,beta)*ECF(1,beta)/ECF(2,beta)^2 with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s \n","beta","C2 obs");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorC2 c2(beta,measurelist[M]);
+
+ printf("%7.3f %14.6f \n",beta,c2(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorD2: D_2^(beta) = ECF(3,beta)*ECF(1,beta)^3/ECF(2,beta)^3 with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s \n","beta","D2 obs");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorD2 d2(beta,measurelist[M]);
+
+ printf("%7.3f %14.6f \n",beta,d2(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorGeneralizedD2: D_2^(alpha, beta) = ECFN(3,alpha)/ECFN(2,beta)^(3*alpha/beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %18s %18s %18s %18s\n","beta","alpha = 0.100","alpha = 0.200","alpha = 0.500","alpha = 1.000");
+
+ for (unsigned int B = 1; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ printf("%7.3f ", beta);
+ for (unsigned int A = 0; A < alphalist.size(); A++) {
+ double alpha = alphalist[A];
+
+ EnergyCorrelatorGeneralizedD2 d2(alpha, beta, measurelist[M]);
+
+ printf("%18.4f ", d2(myJet));
+ }
+ printf("\n");
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorGeneralized (angles = N Choose 2): ECFN(N, beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %7s %14s %14s %14s\n","beta", "N=1", "N=2", "N=3", "N=4");
+
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorGeneralized ECF1(-1,1, beta, measurelist[M]);
+ EnergyCorrelatorGeneralized ECF2(-1,2, beta, measurelist[M]);
+ EnergyCorrelatorGeneralized ECF3(-1,3, beta, measurelist[M]);
+ EnergyCorrelatorGeneralized ECF4(-1,4, beta, measurelist[M]);
+ //EnergyCorrelatorGeneralized ECF5(-1, 5, beta, measurelist[M]);
+
+ printf("%7.3f %7.2f %14.10f %14.10f %14.10f \n", beta, ECF1(myJet), ECF2(myJet), ECF3(myJet),
+ ECF4(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" <<
+ endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorGeneralized: ECFG(angles, N, beta=1) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %7s %14s %14s %14s\n","angles", "N=1", "N=2", "N=3", "N=4");
+
+ double beta = 1.0;
+ for (unsigned int A = 1; A < 2; A++) {
+ double angle = A;
+
+ EnergyCorrelatorGeneralized ECF1(angle, 1, beta, measurelist[M]);
+ EnergyCorrelatorGeneralized ECF2(angle, 2, beta, measurelist[M]);
+ EnergyCorrelatorGeneralized ECF3(angle, 3, beta, measurelist[M]);
+ EnergyCorrelatorGeneralized ECF4(angle, 4, beta, measurelist[M], EnergyCorrelator::slow);
+
+ printf("%7.0f %7.2f %14.10f %14.10f %14.10f \n", angle, ECF1(myJet), ECF2(myJet), ECF3(myJet),
+ ECF4(myJet));
+
+ }
+
+ for (unsigned int A = 2; A < 4; A++) {
+ double angle = A;
+
+ EnergyCorrelatorGeneralized ECF3(angle, 3, beta, measurelist[M]);
+ EnergyCorrelatorGeneralized ECF4(angle, 4, beta, measurelist[M]);
+
+ printf("%7.0f %7s %14s %14.10f %14.10f \n", angle, " " , " " ,ECF3(myJet), ECF4(myJet));
+ }
+
+ for (unsigned int A = 4; A < 7; A++) {
+ double angle = A;
+
+ EnergyCorrelatorGeneralized ECF4(angle, 4, beta, measurelist[M]);
+ printf("%7.0f %7s %14s %14s %14.10f \n", angle, " ", " ", " ", ECF4(myJet) );
+ }
+ cout << "-------------------------------------------------------------------------------------" <<
+ endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorNseries: N_i(beta) = ECFG(i+1, 2, beta)/ECFG(i, 1, beta)^2 with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s %14s %14s \n","beta", "N=1", "N=2", "N=3");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorNseries N1(1,beta,measurelist[M]);
+ EnergyCorrelatorNseries N2(2,beta,measurelist[M]);
+ EnergyCorrelatorNseries N3(3,beta,measurelist[M]);
+
+ printf("%7.3f %14.6f %14.6f %14.6f \n",beta,N1(myJet),N2(myJet),N3(myJet));
+
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorN2: N2(beta) = ECFG(3, 2, beta)/ECFG(2, 1, beta)^2 with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s \n","beta", "N2 obs");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorN2 N2(beta,measurelist[M]);
+
+ printf("%7.3f %14.6f \n",beta,N2(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorN3: N3(beta) = ECFG(4, 2, beta)/ECFG(3, 1, beta)^2 with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s \n","beta", "N3 obs");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorN3 N3(beta,measurelist[M]);
+
+ printf("%7.3f %14.6f \n",beta,N3(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorMseries: M_i(beta) = ECFG(i+1, 1, beta)/ECFN(i, 1, beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s %14s %14s \n","beta", "N=1", "N=2", "N=3");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorMseries M1(1,beta,measurelist[M]);
+ EnergyCorrelatorMseries M2(2,beta,measurelist[M]);
+ EnergyCorrelatorMseries M3(3,beta,measurelist[M]);
+
+
+ printf("%7.3f %14.6f %14.6f %14.6f \n",beta,M1(myJet),M2(myJet),M3(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorM2: M2(beta) = ECFG(3, 1, beta)/ECFG(3, 1, beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s \n","beta", "M2 obs");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorM2 M2(beta,measurelist[M]);
+
+ printf("%7.3f %14.6f \n",beta,M2(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorCseries: C_i(beta) = ECFN(i-1, beta)*ECFN(i+1, beta)/ECFN(i, beta)^2 with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %20s %20s %20s \n","beta", "N=1", "N=2", "N=3");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorCseries C1(1,beta,measurelist[M]);
+ EnergyCorrelatorCseries C2(2,beta,measurelist[M]);
+ EnergyCorrelatorCseries C3(3,beta,measurelist[M]);
+
+
+ printf("%7.3f %20.10f %20.10f %20.10f \n",beta,C1(myJet),C2(myJet),C3(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorUseries: U_i(beta) = ECFG(i+1, 1, beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %20s %20s %20s \n","beta", "N=1", "N=2", "N=3");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorUseries U1(1,beta,measurelist[M]);
+ EnergyCorrelatorUseries U2(2,beta,measurelist[M]);
+ EnergyCorrelatorUseries U3(3,beta,measurelist[M]);
+
+
+ printf("%7.3f %20.10f %20.10f %20.10f \n",beta,U1(myJet),U2(myJet),U3(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorU1: U1(beta) = ECFG(2, 1, beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s \n","beta", "U1 obs");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorU1 U1(beta,measurelist[M]);
+
+ printf("%7.3f %14.10f \n",beta,U1(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorU2: U2(beta) = ECFG(3, 1, beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s \n","beta", "U2 obs");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorU2 U2(beta,measurelist[M]);
+
+ printf("%7.3f %14.10f \n",beta,U2(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelatorU3: U3(beta) = ECFG(4, 1, beta) with " << modename[M] << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s \n","beta", "U3 obs");
+
+ for (unsigned int B = 0; B < betalist.size(); B++) {
+ double beta = betalist[B];
+
+ EnergyCorrelatorU3 U3(beta,measurelist[M]);
+
+ printf("%7.3f %14.10f \n",beta,U3(myJet));
+ }
+ cout << "-------------------------------------------------------------------------------------" << endl << endl;
+
+
+ // timing tests for the developers
+ double do_timing_test = false;
+ if (do_timing_test) {
+
+ cout << "jet with pt = " << myJet.pt() << " and " << myJet.constituents().size() << " constituents" << endl;
+
+ clock_t clock_begin, clock_end;
+ double num_iter;
+ double beta = 0.5;
+
+ cout << setprecision(6);
+
+ // test C1
+ num_iter = 20000;
+ clock_begin = clock();
+ EnergyCorrelatorDoubleRatio C1s(1,beta,measurelist[M],EnergyCorrelator::slow);
+ EnergyCorrelatorDoubleRatio C1f(1,beta,measurelist[M],EnergyCorrelator::storage_array);
+ cout << "timing " << C1s.description() << endl;
+ cout << "timing " << C1f.description() << endl;
+ for (int t = 0; t < num_iter; t++) {
+ C1s(myJet);
+ }
+ clock_end = clock();
+ cout << "Slow method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per C1"<< endl;
+
+ num_iter = 20000;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ C1f(myJet);
+ }
+ clock_end = clock();
+ cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per C1"<< endl;
+
+
+ // test C2
+ num_iter = 1000;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorDoubleRatio C2(2,beta,measurelist[M],EnergyCorrelator::slow);
+ C2(myJet);
+ }
+ clock_end = clock();
+ cout << "Slow method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per C2"<< endl;
+
+ num_iter = 10000;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorDoubleRatio C2(2,beta,measurelist[M],EnergyCorrelator::storage_array);
+ C2(myJet);
+ }
+ clock_end = clock();
+ cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per C2"<< endl;
+
+ // test C3
+ num_iter = 100;
+ clock_begin = clock();
+
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorDoubleRatio C3(3,beta,measurelist[M],EnergyCorrelator::slow);
+ C3(myJet);
+ }
+ clock_end = clock();
+ cout << "Slow method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per C3"<< endl;
+
+ num_iter = 3000;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorDoubleRatio C3(3,beta,measurelist[M],EnergyCorrelator::storage_array);
+ C3(myJet);
+ }
+ clock_end = clock();
+ cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per C3"<< endl;
+
+ // test C4
+ num_iter = 10;
+ clock_begin = clock();
+
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorDoubleRatio C4(4,beta,measurelist[M],EnergyCorrelator::slow);
+ C4(myJet);
+ }
+ clock_end = clock();
+ cout << "Slow method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per C4"<< endl;
+
+ num_iter = 300;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorDoubleRatio C4(4,beta,measurelist[M],EnergyCorrelator::storage_array);
+ C4(myJet);
+ }
+ clock_end = clock();
+ cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per C4"<< endl;
+
+ // test N2
+ num_iter = 10;
+ clock_begin = clock();
+
+ num_iter = 300;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorN2 N2(beta,measurelist[M],EnergyCorrelator::storage_array);
+ N2(myJet);
+ }
+ clock_end = clock();
+ EnergyCorrelatorN2 N2test(beta,measurelist[M],EnergyCorrelator::storage_array);
+ cout << "Beta is: "<< beta << endl;
+ cout << "Result of N2: "<< N2test(myJet) << endl;
+ cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per N2"<< endl;
+
+
+ num_iter = 300;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorN3 N3(beta,measurelist[M],EnergyCorrelator::storage_array);
+ N3(myJet);
+ }
+ clock_end = clock();
+ EnergyCorrelatorN3 N3test(beta,measurelist[M],EnergyCorrelator::storage_array);
+ cout << "Beta is: "<< beta << endl;
+ cout << "Result of N3: "<< N3test(myJet) << endl;
+ cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per N3"<< endl;
+
+
+
+
+ num_iter = 300;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorGeneralized ECF1(2,3, beta, measurelist[M]);
+ ECF1(myJet);
+ }
+ clock_end = clock();
+ EnergyCorrelatorGeneralized ECF1test(2,3, beta, measurelist[M]);
+ cout << "Beta is: "<< beta << endl;
+ cout << "Result of 2e3: "<< ECF1test(myJet) << endl;
+ cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per 2e3"<< endl;
+
+
+ num_iter = 300;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorGeneralized ECF3(2,4, beta, measurelist[M]);
+ ECF3(myJet);
+ }
+ clock_end = clock();
+ EnergyCorrelatorGeneralized ECF2test(2,4, beta, measurelist[M]);
+ cout << "Beta is: "<< beta << endl;
+ cout << "Result of 2e4: "<< ECF2test(myJet) << endl;
+ cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per 2e4"<< endl;
+
+
+// num_iter = 300;
+// clock_begin = clock();
+// for (int t = 0; t < num_iter; t++) {
+// EnergyCorrelatorGeneralized ECF5(2,5, beta, measurelist[M]);
+// ECF5(myJet);
+// }
+// clock_end = clock();
+// EnergyCorrelatorGeneralized ECF5test(2,5, beta, measurelist[M]);
+// cout << "Beta is: "<< beta << endl;
+// cout << "Result of 2e5: "<< ECF5test(myJet) << endl;
+// cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per 2e5"<< endl;
+//
+
+ // test M2
+ num_iter = 10;
+ clock_begin = clock();
+
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorM2 M2(beta,measurelist[M],EnergyCorrelator::slow);
+ M2(myJet);
+ }
+ clock_end = clock();
+ cout << "Slow method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per M2"<< endl;
+
+ num_iter = 300;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorM2 M2(beta,measurelist[M],EnergyCorrelator::storage_array);
+ M2(myJet);
+ }
+ clock_end = clock();
+ cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per M2"<< endl;
+
+ // test M3
+ num_iter = 10;
+ clock_begin = clock();
+
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorMseries M3(3,beta,measurelist[M],EnergyCorrelator::slow);
+ M3(myJet);
+ }
+ clock_end = clock();
+ cout << "Slow method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per M3"<< endl;
+
+ num_iter = 300;
+ clock_begin = clock();
+ for (int t = 0; t < num_iter; t++) {
+ EnergyCorrelatorMseries M3(3,beta,measurelist[M],EnergyCorrelator::storage_array);
+ M3(myJet);
+ }
+ clock_end = clock();
+ cout << "Storage array method: " << (clock_end-clock_begin)/double(CLOCKS_PER_SEC*num_iter)*1000 << " ms per M3"<< endl;
+
+
+ }
+ }
+ }
+ }
+}
+
+
+
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/example.ref b/src/Tools/fjcontrib/EnergyCorrelator/example.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/example.ref
@@ -0,0 +1,922 @@
+# read an event with 354 particles
+#--------------------------------------------------------------------------
+# FastJet release 3.2.0
+# M. Cacciari, G.P. Salam and G. Soyez
+# A software package for jet finding and analysis at colliders
+# http://fastjet.fr
+#
+# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package
+# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210].
+#
+# FastJet is provided without warranty under the terms of the GNU GPLv2.
+# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code
+# and 3rd party plugin jet algorithms. See COPYING file for details.
+#--------------------------------------------------------------------------
+-------------------------------------------------------------------------------------
+EnergyCorrelator: ECF(N,beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 (GeV) N=2 (GeV^2) N=3 (GeV^3) N=4 (GeV^4) N=5 (GeV^5)
+ 0.100 983.64 265690.56 27540663.76 1287213926.38 30113720909.66
+ 0.200 983.64 172787.11 8222752.45 134175168.40 888560847.26
+ 0.500 983.64 52039.98 364021.49 608244.06 356259.05
+ 1.000 983.64 10006.49 9934.06 2670.10 271.98
+ 1.500 983.64 3001.20 1066.15 118.17 4.24
+ 2.000 983.64 1272.64 260.18 14.88 0.22
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorRatio: r_N^(beta) = ECF(N+1,beta)/ECF(N,beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=0 (GeV) N=1 (GeV) N=2 (GeV) N=3 (GeV) N=4 (GeV)
+ 0.100 983.6369 270.1104 103.6569 46.7387 23.3945
+ 0.200 983.6369 175.6615 47.5889 16.3175 6.6224
+ 0.500 983.6369 52.9057 6.9950 1.6709 0.5857
+ 1.000 983.6369 10.1730 0.9928 0.2688 0.1019
+ 1.500 983.6369 3.0511 0.3552 0.1108 0.0359
+ 2.000 983.6369 1.2938 0.2044 0.0572 0.0151
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorDoubleRatio: C_N^(beta) = r_N^(beta)/r_{N-1}^(beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3 N=4
+ 0.100 0.274604 0.383758 0.450898 0.500538
+ 0.200 0.178584 0.270913 0.342885 0.405845
+ 0.500 0.053786 0.132217 0.238870 0.350540
+ 1.000 0.010342 0.097588 0.270742 0.378972
+ 1.500 0.003102 0.116430 0.312016 0.323906
+ 2.000 0.001315 0.158011 0.279675 0.263310
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorC1: C_1^(beta) = ECF(2,beta)/ECF(1,beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta C1 obs
+ 0.100 0.274604
+ 0.200 0.178584
+ 0.500 0.053786
+ 1.000 0.010342
+ 1.500 0.003102
+ 2.000 0.001315
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorC2: C_2^(beta) = ECF(3,beta)*ECF(1,beta)/ECF(2,beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta C2 obs
+ 0.100 0.383758
+ 0.200 0.270913
+ 0.500 0.132217
+ 1.000 0.097588
+ 1.500 0.116430
+ 2.000 0.158011
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorD2: D_2^(beta) = ECF(3,beta)*ECF(1,beta)^3/ECF(2,beta)^3 with pt_R
+-------------------------------------------------------------------------------------
+ beta D2 obs
+ 0.100 1.397496
+ 0.200 1.517007
+ 0.500 2.458216
+ 1.000 9.435950
+ 1.500 37.535182
+ 2.000 120.129760
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralizedD2: D_2^(alpha, beta) = ECFN(3,alpha)/ECFN(2,beta)^(3*alpha/beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta alpha = 0.100 alpha = 0.200 alpha = 0.500 alpha = 1.000
+ 0.200 0.3834 1.5170 156.2463 1741793.7615
+ 0.500 0.1671 0.2882 2.4582 431.1389
+ 1.000 0.1140 0.1342 0.3637 9.4359
+ 1.500 0.0919 0.0871 0.1233 1.0849
+ 2.000 0.0783 0.0632 0.0554 0.2188
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralized (angles = N Choose 2): ECFN(N, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3 N=4
+ 0.100 1.00 0.2746037664 0.0289380967 0.0013750278
+ 0.200 1.00 0.1785836568 0.0086399808 0.0001433286
+ 0.500 1.00 0.0537857869 0.0003824922 0.0000006497
+ 1.000 1.00 0.0103421840 0.0000104381 0.0000000029
+ 1.500 1.00 0.0031018827 0.0000011202 0.0000000001
+ 2.000 1.00 0.0013153375 0.0000002734 0.0000000000
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralized: ECFG(angles, N, beta=1) with pt_R
+-------------------------------------------------------------------------------------
+ angles N=1 N=2 N=3 N=4
+ 1 1.00 0.0103421840 0.0007353402 0.0000733472
+ 2 0.0000460939 0.0000010704
+ 3 0.0000104381 0.0000000552
+ 4 0.0000000114
+ 5 0.0000000045
+ 6 0.0000000029
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorNseries: N_i(beta) = ECFG(i+1, 2, beta)/ECFG(i, 1, beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.178584 0.551898 1.506618
+ 0.200 0.078954 0.534774 1.521976
+ 0.500 0.010342 0.487547 1.601014
+ 1.000 0.001315 0.430942 1.979487
+ 1.500 0.000437 0.391935 3.250084
+ 2.000 0.000220 0.365859 6.700247
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorN2: N2(beta) = ECFG(3, 2, beta)/ECFG(2, 1, beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta N2 obs
+ 0.100 0.551898
+ 0.200 0.534774
+ 0.500 0.487547
+ 1.000 0.430942
+ 1.500 0.391935
+ 2.000 0.365859
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorN3: N3(beta) = ECFG(4, 2, beta)/ECFG(3, 1, beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta N3 obs
+ 0.100 1.506618
+ 0.200 1.521976
+ 0.500 1.601014
+ 1.000 1.979487
+ 1.500 3.250084
+ 2.000 6.700247
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorMseries: M_i(beta) = ECFG(i+1, 1, beta)/ECFN(i, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.274604 0.225158 0.151396
+ 0.200 0.178584 0.206357 0.146715
+ 0.500 0.053786 0.149827 0.130985
+ 1.000 0.010342 0.071101 0.099746
+ 1.500 0.003102 0.027603 0.065806
+ 2.000 0.001315 0.010448 0.036511
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorM2: M2(beta) = ECFG(3, 1, beta)/ECFG(3, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta M2 obs
+ 0.100 0.225158
+ 0.200 0.206357
+ 0.500 0.149827
+ 1.000 0.071101
+ 1.500 0.027603
+ 2.000 0.010448
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorCseries: C_i(beta) = ECFN(i-1, beta)*ECFN(i+1, beta)/ECFN(i, beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.2746037664 0.3837575950 0.4508977207
+ 0.200 0.1785836568 0.2709126926 0.3428854490
+ 0.500 0.0537857869 0.1322170711 0.2388696533
+ 1.000 0.0103421840 0.0975883303 0.2707417692
+ 1.500 0.0031018827 0.1164297328 0.3120164994
+ 2.000 0.0013153375 0.1580111821 0.2796746959
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorUseries: U_i(beta) = ECFG(i+1, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.2746037664 0.0618292258 0.0093606928
+ 0.200 0.1785836568 0.0368519186 0.0054067344
+ 0.500 0.0537857869 0.0080585540 0.0010555469
+ 1.000 0.0103421840 0.0007353402 0.0000733472
+ 1.500 0.0031018827 0.0000856204 0.0000056343
+ 2.000 0.0013153375 0.0000137425 0.0000005017
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU1: U1(beta) = ECFG(2, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta U1 obs
+ 0.100 0.2746037664
+ 0.200 0.1785836568
+ 0.500 0.0537857869
+ 1.000 0.0103421840
+ 1.500 0.0031018827
+ 2.000 0.0013153375
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU2: U2(beta) = ECFG(3, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta U2 obs
+ 0.100 0.0618292258
+ 0.200 0.0368519186
+ 0.500 0.0080585540
+ 1.000 0.0007353402
+ 1.500 0.0000856204
+ 2.000 0.0000137425
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU3: U3(beta) = ECFG(4, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta U3 obs
+ 0.100 0.0093606928
+ 0.200 0.0054067344
+ 0.500 0.0010555469
+ 1.000 0.0000733472
+ 1.500 0.0000056343
+ 2.000 0.0000005017
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelator: ECF(N,beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 (GeV) N=2 (GeV^2) N=3 (GeV^3) N=4 (GeV^4) N=5 (GeV^5)
+ 0.100 1378.16 504056.94 68362746.10 4040636656.75 115642116882.67
+ 0.200 1378.16 316828.68 18441161.70 345185274.86 2475861856.72
+ 0.500 1378.16 86243.22 614652.00 941844.70 459093.24
+ 1.000 1378.16 14186.79 11682.63 2060.77 92.98
+ 1.500 1378.16 3751.90 907.11 39.34 0.27
+ 2.000 1378.16 1439.57 152.71 1.84 0.00
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorRatio: r_N^(beta) = ECF(N+1,beta)/ECF(N,beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=0 (GeV) N=1 (GeV) N=2 (GeV) N=3 (GeV) N=4 (GeV)
+ 0.100 1378.1622 365.7457 135.6250 59.1058 28.6198
+ 0.200 1378.1622 229.8922 58.2055 18.7182 7.1726
+ 0.500 1378.1622 62.5784 7.1270 1.5323 0.4874
+ 1.000 1378.1622 10.2940 0.8235 0.1764 0.0451
+ 1.500 1378.1622 2.7224 0.2418 0.0434 0.0069
+ 2.000 1378.1622 1.0446 0.1061 0.0121 0.0013
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorDoubleRatio: C_N^(beta) = r_N^(beta)/r_{N-1}^(beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3 N=4
+ 0.100 0.265387 0.370818 0.435803 0.484212
+ 0.200 0.166811 0.253186 0.321588 0.383186
+ 0.500 0.045407 0.113888 0.215004 0.318106
+ 1.000 0.007469 0.079997 0.214207 0.255786
+ 1.500 0.001975 0.088810 0.179360 0.160180
+ 2.000 0.000758 0.101555 0.113867 0.106401
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorC1: C_1^(beta) = ECF(2,beta)/ECF(1,beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta C1 obs
+ 0.100 0.265387
+ 0.200 0.166811
+ 0.500 0.045407
+ 1.000 0.007469
+ 1.500 0.001975
+ 2.000 0.000758
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorC2: C_2^(beta) = ECF(3,beta)*ECF(1,beta)/ECF(2,beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta C2 obs
+ 0.100 0.370818
+ 0.200 0.253186
+ 0.500 0.113888
+ 1.000 0.079997
+ 1.500 0.088810
+ 2.000 0.101555
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorD2: D_2^(beta) = ECF(3,beta)*ECF(1,beta)^3/ECF(2,beta)^3 with E_theta
+-------------------------------------------------------------------------------------
+ beta D2 obs
+ 0.100 1.397274
+ 0.200 1.517804
+ 0.500 2.508161
+ 1.000 10.709981
+ 1.500 44.958245
+ 2.000 133.988418
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralizedD2: D_2^(alpha, beta) = ECFN(3,alpha)/ECFN(2,beta)^(3*alpha/beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta alpha = 0.100 alpha = 0.200 alpha = 0.500 alpha = 1.000
+ 0.200 0.3833 1.5178 159.9740 2071485.6064
+ 0.500 0.1670 0.2880 2.5082 509.2064
+ 1.000 0.1135 0.1330 0.3637 10.7100
+ 1.500 0.0907 0.0850 0.1189 1.1438
+ 2.000 0.0767 0.0608 0.0514 0.2139
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralized (angles = N Choose 2): ECFN(N, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3 N=4
+ 0.100 1.00 0.2653865755 0.0261167137 0.0011200786
+ 0.200 1.00 0.1668106769 0.0070451023 0.0000956866
+ 0.500 1.00 0.0454071552 0.0002348163 0.0000002611
+ 1.000 1.00 0.0074693640 0.0000044631 0.0000000006
+ 1.500 1.00 0.0019753776 0.0000003465 0.0000000000
+ 2.000 1.00 0.0007579352 0.0000000583 0.0000000000
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralized: ECFG(angles, N, beta=1) with E_theta
+-------------------------------------------------------------------------------------
+ angles N=1 N=2 N=3 N=4
+ 1 1.00 0.0074693640 0.0005219446 0.0000521319
+ 2 0.0000242551 0.0000005388
+ 3 0.0000044631 0.0000000205
+ 4 0.0000000035
+ 5 0.0000000011
+ 6 0.0000000006
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorNseries: N_i(beta) = ECFG(i+1, 2, beta)/ECFG(i, 1, beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.166811 0.551800 1.506192
+ 0.200 0.068920 0.534652 1.521253
+ 0.500 0.007469 0.487710 1.598907
+ 1.000 0.000758 0.434746 1.977674
+ 1.500 0.000207 0.401351 3.333270
+ 2.000 0.000082 0.372570 7.518334
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorN2: N2(beta) = ECFG(3, 2, beta)/ECFG(2, 1, beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta N2 obs
+ 0.100 0.551800
+ 0.200 0.534652
+ 0.500 0.487710
+ 1.000 0.434746
+ 1.500 0.401351
+ 2.000 0.372570
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorN3: N3(beta) = ECFG(4, 2, beta)/ECFG(3, 1, beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta N3 obs
+ 0.100 1.506192
+ 0.200 1.521253
+ 0.500 1.598907
+ 1.000 1.977674
+ 1.500 3.333270
+ 2.000 7.518334
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorMseries: M_i(beta) = ECFG(i+1, 1, beta)/ECFN(i, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.265387 0.225134 0.151350
+ 0.200 0.166811 0.206335 0.146685
+ 0.500 0.045407 0.149607 0.131015
+ 1.000 0.007469 0.069878 0.099880
+ 1.500 0.001975 0.025930 0.065823
+ 2.000 0.000758 0.009248 0.036027
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorM2: M2(beta) = ECFG(3, 1, beta)/ECFG(3, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta M2 obs
+ 0.100 0.225134
+ 0.200 0.206335
+ 0.500 0.149607
+ 1.000 0.069878
+ 1.500 0.025930
+ 2.000 0.009248
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorCseries: C_i(beta) = ECFN(i-1, beta)*ECFN(i+1, beta)/ECFN(i, beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.2653865755 0.3708178471 0.4358031826
+ 0.200 0.1668106769 0.2531859580 0.3215882713
+ 0.500 0.0454071552 0.1138884647 0.2150035566
+ 1.000 0.0074693640 0.0799967491 0.2142068062
+ 1.500 0.0019753776 0.0888095113 0.1793603915
+ 2.000 0.0007579352 0.1015545382 0.1138668084
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorUseries: U_i(beta) = ECFG(i+1, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.2653865755 0.0597476192 0.0090428096
+ 0.200 0.1668106769 0.0344188111 0.0050487063
+ 0.500 0.0454071552 0.0067932369 0.0008900155
+ 1.000 0.0074693640 0.0005219446 0.0000521319
+ 1.500 0.0019753776 0.0000512213 0.0000033715
+ 2.000 0.0007579352 0.0000070092 0.0000002525
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU1: U1(beta) = ECFG(2, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta U1 obs
+ 0.100 0.2653865755
+ 0.200 0.1668106769
+ 0.500 0.0454071552
+ 1.000 0.0074693640
+ 1.500 0.0019753776
+ 2.000 0.0007579352
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU2: U2(beta) = ECFG(3, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta U2 obs
+ 0.100 0.0597476192
+ 0.200 0.0344188111
+ 0.500 0.0067932369
+ 1.000 0.0005219446
+ 1.500 0.0000512213
+ 2.000 0.0000070092
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU3: U3(beta) = ECFG(4, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta U3 obs
+ 0.100 0.0090428096
+ 0.200 0.0050487063
+ 0.500 0.0008900155
+ 1.000 0.0000521319
+ 1.500 0.0000033715
+ 2.000 0.0000002525
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelator: ECF(N,beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 (GeV) N=2 (GeV^2) N=3 (GeV^3) N=4 (GeV^4) N=5 (GeV^5)
+ 0.100 910.03 163661.63 10858223.95 340994615.02 5907941830.38
+ 0.200 910.03 111307.49 3950123.18 59638399.31 478368362.42
+ 0.500 910.03 40470.38 446453.20 2147680.90 5564873.72
+ 1.000 910.03 13863.90 65435.19 142222.94 166409.02
+ 1.500 910.03 8417.59 26548.97 39560.12 31484.21
+ 2.000 910.03 6328.24 16871.11 21081.97 13743.58
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorRatio: r_N^(beta) = ECF(N+1,beta)/ECF(N,beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=0 (GeV) N=1 (GeV) N=2 (GeV) N=3 (GeV) N=4 (GeV)
+ 0.100 910.0320 179.8416 66.3456 31.4043 17.3256
+ 0.200 910.0320 122.3116 35.4884 15.0979 8.0211
+ 0.500 910.0320 44.4714 11.0316 4.8105 2.5911
+ 1.000 910.0320 15.2345 4.7198 2.1735 1.1701
+ 1.500 910.0320 9.2498 3.1540 1.4901 0.7959
+ 2.000 910.0320 6.9539 2.6660 1.2496 0.6519
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorDoubleRatio: C_N^(beta) = r_N^(beta)/r_{N-1}^(beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3 N=4
+ 0.100 0.197621 0.368911 0.473344 0.551696
+ 0.200 0.134404 0.290147 0.425431 0.531277
+ 0.500 0.048868 0.248061 0.436069 0.538632
+ 1.000 0.016741 0.309811 0.460503 0.538330
+ 1.500 0.010164 0.340980 0.472444 0.534103
+ 2.000 0.007641 0.383385 0.468712 0.521701
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorC1: C_1^(beta) = ECF(2,beta)/ECF(1,beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta C1 obs
+ 0.100 0.197621
+ 0.200 0.134404
+ 0.500 0.048868
+ 1.000 0.016741
+ 1.500 0.010164
+ 2.000 0.007641
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorC2: C_2^(beta) = ECF(3,beta)*ECF(1,beta)/ECF(2,beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta C2 obs
+ 0.100 0.368911
+ 0.200 0.290147
+ 0.500 0.248061
+ 1.000 0.309811
+ 1.500 0.340980
+ 2.000 0.383385
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorD2: D_2^(beta) = ECF(3,beta)*ECF(1,beta)^3/ECF(2,beta)^3 with pt_R
+-------------------------------------------------------------------------------------
+ beta D2 obs
+ 0.100 1.866758
+ 0.200 2.158775
+ 0.500 5.076145
+ 1.000 18.506536
+ 1.500 33.547049
+ 2.000 50.172493
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralizedD2: D_2^(alpha, beta) = ECFN(3,alpha)/ECFN(2,beta)^(3*alpha/beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta alpha = 0.100 alpha = 0.200 alpha = 0.500 alpha = 1.000
+ 0.200 0.2924 2.1588 2039.4962 1029141861.7962
+ 0.500 0.0881 0.1962 5.0761 6375.2544
+ 1.000 0.0491 0.0610 0.2735 18.5065
+ 1.500 0.0361 0.0329 0.0583 0.8404
+ 2.000 0.0299 0.0226 0.0229 0.1300
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralized (angles = N Choose 2): ECFN(N, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3 N=4
+ 0.100 1.00 0.1976212201 0.0144075072 0.0004971883
+ 0.200 1.00 0.1344036550 0.0052413202 0.0000869560
+ 0.500 1.00 0.0488679347 0.0005923876 0.0000031314
+ 1.000 1.00 0.0167406417 0.0000868243 0.0000002074
+ 1.500 1.00 0.0101642297 0.0000352272 0.0000000577
+ 2.000 1.00 0.0076413374 0.0000223859 0.0000000307
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralized: ECFG(angles, N, beta=1) with pt_R
+-------------------------------------------------------------------------------------
+ angles N=1 N=2 N=3 N=4
+ 1 1.00 0.0167406417 0.0005149099 0.0000275956
+ 2 0.0001201519 0.0000010521
+ 3 0.0000868243 0.0000003239
+ 4 0.0000002207
+ 5 0.0000001864
+ 6 0.0000002074
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorNseries: N_i(beta) = ECFG(i+1, 2, beta)/ECFG(i, 1, beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.134404 0.501515 2.093230
+ 0.200 0.066590 0.490962 2.107355
+ 0.500 0.016741 0.472128 2.270271
+ 1.000 0.007641 0.428733 3.968204
+ 1.500 0.005197 0.367850 11.456776
+ 2.000 0.003938 0.329248 20.513687
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorN2: N2(beta) = ECFG(3, 2, beta)/ECFG(2, 1, beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta N2 obs
+ 0.100 0.501515
+ 0.200 0.490962
+ 0.500 0.472128
+ 1.000 0.428733
+ 1.500 0.367850
+ 2.000 0.329248
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorN3: N3(beta) = ECFG(4, 2, beta)/ECFG(3, 1, beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta N3 obs
+ 0.100 2.093230
+ 0.200 2.107355
+ 0.500 2.270271
+ 1.000 3.968204
+ 1.500 11.456776
+ 2.000 20.513687
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorMseries: M_i(beta) = ECFG(i+1, 1, beta)/ECFN(i, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.197621 0.140440 0.090587
+ 0.200 0.134404 0.127907 0.086996
+ 0.500 0.048868 0.087042 0.076041
+ 1.000 0.016741 0.030758 0.053593
+ 1.500 0.010164 0.010637 0.025871
+ 2.000 0.007641 0.005839 0.009492
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorM2: M2(beta) = ECFG(3, 1, beta)/ECFG(3, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta M2 obs
+ 0.100 0.140440
+ 0.200 0.127907
+ 0.500 0.087042
+ 1.000 0.030758
+ 1.500 0.010637
+ 2.000 0.005839
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorCseries: C_i(beta) = ECFN(i-1, beta)*ECFN(i+1, beta)/ECFN(i, beta)^2 with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.1976212201 0.3689110739 0.4733439247
+ 0.200 0.1344036550 0.2901472976 0.4254309496
+ 0.500 0.0488679347 0.2480607340 0.4360689366
+ 1.000 0.0167406417 0.3098112813 0.4605028221
+ 1.500 0.0101642297 0.3409799143 0.4724436009
+ 2.000 0.0076413374 0.3833849510 0.4687122507
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorUseries: U_i(beta) = ECFG(i+1, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.1976212201 0.0277540195 0.0025141656
+ 0.200 0.1344036550 0.0171911179 0.0014955586
+ 0.500 0.0488679347 0.0042535497 0.0003234433
+ 1.000 0.0167406417 0.0005149099 0.0000275956
+ 1.500 0.0101642297 0.0001081211 0.0000027972
+ 2.000 0.0076413374 0.0000446167 0.0000004235
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU1: U1(beta) = ECFG(2, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta U1 obs
+ 0.100 0.1976212201
+ 0.200 0.1344036550
+ 0.500 0.0488679347
+ 1.000 0.0167406417
+ 1.500 0.0101642297
+ 2.000 0.0076413374
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU2: U2(beta) = ECFG(3, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta U2 obs
+ 0.100 0.0277540195
+ 0.200 0.0171911179
+ 0.500 0.0042535497
+ 1.000 0.0005149099
+ 1.500 0.0001081211
+ 2.000 0.0000446167
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU3: U3(beta) = ECFG(4, 1, beta) with pt_R
+-------------------------------------------------------------------------------------
+ beta U3 obs
+ 0.100 0.0025141656
+ 0.200 0.0014955586
+ 0.500 0.0003234433
+ 1.000 0.0000275956
+ 1.500 0.0000027972
+ 2.000 0.0000004235
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelator: ECF(N,beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 (GeV) N=2 (GeV^2) N=3 (GeV^3) N=4 (GeV^4) N=5 (GeV^5)
+ 0.100 934.39 173035.93 11869881.64 387687952.45 7030672399.84
+ 0.200 934.39 117791.85 4351824.23 69148951.24 587495287.84
+ 0.500 934.39 43220.34 507378.92 2589996.65 7002091.93
+ 1.000 934.39 15182.02 75656.66 165115.95 178354.07
+ 1.500 934.39 9296.03 30143.02 40417.01 24563.71
+ 2.000 934.39 6943.30 18259.83 17679.34 7116.38
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorRatio: r_N^(beta) = ECF(N+1,beta)/ECF(N,beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=0 (GeV) N=1 (GeV) N=2 (GeV) N=3 (GeV) N=4 (GeV)
+ 0.100 934.3868 185.1866 68.5978 32.6615 18.1349
+ 0.200 934.3868 126.0633 36.9450 15.8896 8.4961
+ 0.500 934.3868 46.2553 11.7394 5.1047 2.7035
+ 1.000 934.3868 16.2481 4.9833 2.1824 1.0802
+ 1.500 934.3868 9.9488 3.2426 1.3408 0.6078
+ 2.000 934.3868 7.4309 2.6299 0.9682 0.4025
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorDoubleRatio: C_N^(beta) = r_N^(beta)/r_{N-1}^(beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3 N=4
+ 0.100 0.198191 0.370425 0.476130 0.555237
+ 0.200 0.134916 0.293067 0.430089 0.534693
+ 0.500 0.049503 0.253795 0.434833 0.529617
+ 1.000 0.017389 0.306701 0.437950 0.494940
+ 1.500 0.010647 0.325926 0.413512 0.453265
+ 2.000 0.007953 0.353909 0.368161 0.415742
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorC1: C_1^(beta) = ECF(2,beta)/ECF(1,beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta C1 obs
+ 0.100 0.198191
+ 0.200 0.134916
+ 0.500 0.049503
+ 1.000 0.017389
+ 1.500 0.010647
+ 2.000 0.007953
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorC2: C_2^(beta) = ECF(3,beta)*ECF(1,beta)/ECF(2,beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta C2 obs
+ 0.100 0.370425
+ 0.200 0.293067
+ 0.500 0.253795
+ 1.000 0.306701
+ 1.500 0.325926
+ 2.000 0.353909
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorD2: D_2^(beta) = ECF(3,beta)*ECF(1,beta)^3/ECF(2,beta)^3 with E_theta
+-------------------------------------------------------------------------------------
+ beta D2 obs
+ 0.100 1.869035
+ 0.200 2.172229
+ 0.500 5.126818
+ 1.000 17.637552
+ 1.500 30.610782
+ 2.000 44.502015
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralizedD2: D_2^(alpha, beta) = ECFN(3,alpha)/ECFN(2,beta)^(3*alpha/beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta alpha = 0.100 alpha = 0.200 alpha = 0.500 alpha = 1.000
+ 0.200 0.2936 2.1722 2081.0777 1038338617.9694
+ 0.500 0.0883 0.1966 5.1268 6301.7080
+ 1.000 0.0491 0.0607 0.2712 17.6376
+ 1.500 0.0361 0.0328 0.0584 0.8180
+ 2.000 0.0300 0.0227 0.0234 0.1308
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralized (angles = N Choose 2): ECFN(N, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3 N=4
+ 0.100 1.00 0.1981905437 0.0145501117 0.0005085991
+ 0.200 1.00 0.1349155085 0.0053344701 0.0000907149
+ 0.500 1.00 0.0495033749 0.0006219455 0.0000033978
+ 1.000 1.00 0.0173890665 0.0000927400 0.0000002166
+ 1.500 1.00 0.0106474132 0.0000369493 0.0000000530
+ 2.000 1.00 0.0079526591 0.0000223829 0.0000000232
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorGeneralized: ECFG(angles, N, beta=1) with E_theta
+-------------------------------------------------------------------------------------
+ angles N=1 N=2 N=3 N=4
+ 1 1.00 0.0173890665 0.0005243822 0.0000276026
+ 2 0.0001290539 0.0000011436
+ 3 0.0000927400 0.0000003720
+ 4 0.0000002479
+ 5 0.0000002021
+ 6 0.0000002166
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorNseries: N_i(beta) = ECFG(i+1, 2, beta)/ECFG(i, 1, beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.134916 0.502292 2.091587
+ 0.200 0.067180 0.491827 2.107891
+ 0.500 0.017389 0.472830 2.289141
+ 1.000 0.007953 0.426794 4.159019
+ 1.500 0.005251 0.366194 11.630367
+ 2.000 0.003828 0.328039 19.240170
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorN2: N2(beta) = ECFG(3, 2, beta)/ECFG(2, 1, beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta N2 obs
+ 0.100 0.502292
+ 0.200 0.491827
+ 0.500 0.472830
+ 1.000 0.426794
+ 1.500 0.366194
+ 2.000 0.328039
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorN3: N3(beta) = ECFG(4, 2, beta)/ECFG(3, 1, beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta N3 obs
+ 0.100 2.091587
+ 0.200 2.107891
+ 0.500 2.289141
+ 1.000 4.159019
+ 1.500 11.630367
+ 2.000 19.240170
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorMseries: M_i(beta) = ECFG(i+1, 1, beta)/ECFN(i, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.198191 0.140807 0.091081
+ 0.200 0.134916 0.127947 0.087436
+ 0.500 0.049503 0.086121 0.076197
+ 1.000 0.017389 0.030156 0.052638
+ 1.500 0.010647 0.010921 0.024416
+ 2.000 0.007953 0.006325 0.009110
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorM2: M2(beta) = ECFG(3, 1, beta)/ECFG(3, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta M2 obs
+ 0.100 0.140807
+ 0.200 0.127947
+ 0.500 0.086121
+ 1.000 0.030156
+ 1.500 0.010921
+ 2.000 0.006325
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorCseries: C_i(beta) = ECFN(i-1, beta)*ECFN(i+1, beta)/ECFN(i, beta)^2 with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.1981905437 0.3704251544 0.4761303115
+ 0.200 0.1349155085 0.2930674174 0.4300888197
+ 0.500 0.0495033749 0.2537948134 0.4348330516
+ 1.000 0.0173890665 0.3067005727 0.4379497669
+ 1.500 0.0106474132 0.3259256469 0.4135119649
+ 2.000 0.0079526591 0.3539093501 0.3681613681
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorUseries: U_i(beta) = ECFG(i+1, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta N=1 N=2 N=3
+ 0.100 0.1981905437 0.0279066279 0.0025417550
+ 0.200 0.1349155085 0.0172619856 0.0015093221
+ 0.500 0.0495033749 0.0042632685 0.0003248489
+ 1.000 0.0173890665 0.0005243822 0.0000276026
+ 1.500 0.0106474132 0.0001162849 0.0000028392
+ 2.000 0.0079526591 0.0000503042 0.0000004582
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU1: U1(beta) = ECFG(2, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta U1 obs
+ 0.100 0.1981905437
+ 0.200 0.1349155085
+ 0.500 0.0495033749
+ 1.000 0.0173890665
+ 1.500 0.0106474132
+ 2.000 0.0079526591
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU2: U2(beta) = ECFG(3, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta U2 obs
+ 0.100 0.0279066279
+ 0.200 0.0172619856
+ 0.500 0.0042632685
+ 1.000 0.0005243822
+ 1.500 0.0001162849
+ 2.000 0.0000503042
+-------------------------------------------------------------------------------------
+
+-------------------------------------------------------------------------------------
+EnergyCorrelatorU3: U3(beta) = ECFG(4, 1, beta) with E_theta
+-------------------------------------------------------------------------------------
+ beta U3 obs
+ 0.100 0.0025417550
+ 0.200 0.0015093221
+ 0.500 0.0003248489
+ 1.000 0.0000276026
+ 1.500 0.0000028392
+ 2.000 0.0000004582
+-------------------------------------------------------------------------------------
+
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/example_basic_usage.cc b/src/Tools/fjcontrib/EnergyCorrelator/example_basic_usage.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/example_basic_usage.cc
@@ -0,0 +1,234 @@
+// Example showing basic usage of energy correlator classes.
+//
+// Compile it with "make example" and run it with
+//
+// ./example_basic_usage < ../data/single-event.dat
+//
+// Copyright (c) 2013-2016
+// Andrew Larkoski, Lina Necib, Gavin Salam, and Jesse Thaler
+//
+// $Id: example.cc 958 2016-08-17 00:25:14Z linoush $
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iomanip>
+#include <stdlib.h>
+#include <stdio.h>
+#include <ctime>
+#include <iostream>
+#include <istream>
+#include <fstream>
+#include <sstream>
+#include <string>
+
+#include "fastjet/PseudoJet.hh"
+#include "fastjet/ClusterSequence.hh"
+#include "fastjet/JetDefinition.hh"
+
+#include <sstream>
+#include "EnergyCorrelator.hh" // In external code, this should be fastjet/contrib/EnergyCorrelator.hh
+
+using namespace std;
+using namespace fastjet;
+using namespace fastjet::contrib;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &event);
+void analyze(const vector<PseudoJet> & input_particles);
+
+//----------------------------------------------------------------------
+int main(){
+
+ //----------------------------------------------------------
+ // read in input particles
+ vector<PseudoJet> event;
+ read_event(event);
+ cout << "# read an event with " << event.size() << " particles" << endl;
+
+ //----------------------------------------------------------
+ // illustrate how this EnergyCorrelator contrib works
+
+ analyze(event);
+
+ return 0;
+}
+
+// read in input particles
+void read_event(vector<PseudoJet> &event){
+ string line;
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {return;}
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ event.push_back(particle);
+ }
+}
+
+////////
+//
+// Main Routine for Analysis
+//
+///////
+
+void analyze(const vector<PseudoJet> & input_particles) {
+
+ /////// EnergyCorrelator /////////////////////////////
+
+ // Initial clustering with anti-kt algorithm
+ JetAlgorithm algorithm = antikt_algorithm;
+ double jet_rad = 1.00; // jet radius for anti-kt algorithm
+ JetDefinition jetDef = JetDefinition(algorithm,jet_rad,E_scheme,Best);
+ ClusterSequence clust_seq(input_particles,jetDef);
+ vector<PseudoJet> antikt_jets = sorted_by_pt(clust_seq.inclusive_jets());
+
+ for (int j = 0; j < 1; j++) { // Hardest jet per event
+ if (antikt_jets[j].perp() > 200) {
+
+ PseudoJet myJet = antikt_jets[j];
+
+
+ // The angularity is set by the value of beta
+ double beta;
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelator: C series " << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s %14s %14s\n","beta", "C1", "C2", "C3");
+
+
+ beta = 1.0;
+ //Defining the Cseries for beta= 1.0
+ EnergyCorrelatorC1 C1s(beta);
+ EnergyCorrelatorC2 C2s(beta);
+ EnergyCorrelatorCseries C3s(3, beta);
+
+
+ printf("%7.3f %14.6f %14.6f %14.6f\n",beta,C1s(myJet),C2s(myJet),C3s(myJet));
+
+ beta = 2.0;
+ //Defining the Cseries for beta= 2.0
+ EnergyCorrelatorC1 C1s_2(beta);
+ EnergyCorrelatorC2 C2s_2(beta);
+ EnergyCorrelatorCseries C3s_2(3, beta);
+
+
+ printf("%7.3f %14.6f %14.6f %14.6f\n",beta,C1s_2(myJet),C2s_2(myJet),C3s_2(myJet));
+
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelator: D2, orignal (alpha=beta) and generalized " << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s %14s %14s\n","beta","D2", "D2(alpha=1)", "D2(alpha=2)");
+
+
+ beta = 1.0;
+ EnergyCorrelatorD2 d2(beta);
+ double alpha = 1.0;
+ EnergyCorrelatorGeneralizedD2 d2_generalized(alpha, beta);
+ alpha = 2.0;
+ EnergyCorrelatorGeneralizedD2 d2_generalized_2(alpha, beta);
+
+ printf("%7.3f %14.6f %14.6f %14.6f\n",beta,d2(myJet), d2_generalized(myJet), d2_generalized_2(myJet));
+ beta = 2.0;
+ EnergyCorrelatorD2 d2_2(beta);
+ alpha = 1.0;
+ EnergyCorrelatorGeneralizedD2 d2_generalized_3(alpha, beta);
+ alpha = 2.0;
+ EnergyCorrelatorGeneralizedD2 d2_generalized_4(alpha, beta);
+ printf("%7.3f %14.6f %14.6f %14.6f\n",beta,d2_2(myJet), d2_generalized_3(myJet), d2_generalized_4(myJet));
+
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelator: N series " << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s %14s\n","beta", "N2", "N3");
+
+
+ beta = 1.0;
+ // Directly defining the EnergyCorrelator N2 and N3
+ EnergyCorrelatorN2 N2(beta);
+ EnergyCorrelatorN3 N3(beta);
+ printf("%7.3f %14.6f %14.6f\n",beta, N2(myJet), N3(myJet));
+
+ beta = 2.0;
+ EnergyCorrelatorN2 N2_2(beta);
+ EnergyCorrelatorN3 N3_2(beta);
+ printf("%7.3f %14.6f %14.6f\n",beta, N2_2(myJet), N3_2(myJet));
+
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelator: M series " << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s %14s\n","beta", "M2", "M3");
+
+ beta = 1.0;
+ //Directly defining M2
+ EnergyCorrelatorM2 M2(beta);
+ EnergyCorrelatorMseries M3(3, beta);
+ printf("%7.3f %14.6f %14.6f\n", beta, M2(myJet), M3(myJet));
+
+ beta = 2.0;
+ EnergyCorrelatorM2 M2_2(beta);
+ EnergyCorrelatorMseries M3_2(3, beta);
+ printf("%7.3f %14.6f %14.6f\n", beta, M2_2(myJet), M3_2(myJet));
+
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ cout << "EnergyCorrelator: U series " << endl;
+ cout << "-------------------------------------------------------------------------------------" << endl;
+ printf("%7s %14s %14s %14s\n","beta", "U1", "U2", "U3");
+
+
+ beta = 0.5;
+ //Defining the Useries for beta= 0.5
+ EnergyCorrelatorU1 U1s(beta);
+ EnergyCorrelatorU2 U2s(beta);
+ EnergyCorrelatorU3 U3s(beta);
+
+
+ printf("%7.3f %14.8f %14.8f %14.8f\n",beta,U1s(myJet),U2s(myJet),U3s(myJet));
+
+ beta = 1.0;
+ //Defining the Useries for beta= 1.0
+ EnergyCorrelatorU1 U1s_2(beta);
+ EnergyCorrelatorU2 U2s_2(beta);
+ EnergyCorrelatorU3 U3s_2(beta);
+
+
+ printf("%7.3f %14.8f %14.8f %14.8f\n",beta,U1s_2(myJet),U2s_2(myJet),U3s_2(myJet));
+
+ beta = 2.0;
+ //Defining the Useries for beta= 2.0
+ EnergyCorrelatorU1 U1s_3(beta);
+ EnergyCorrelatorU2 U2s_3(beta);
+ EnergyCorrelatorU3 U3s_3(beta);
+
+
+ printf("%7.3f %14.8f %14.8f %14.8f\n",beta,U1s_3(myJet),U2s_3(myJet),U3s_3(myJet));
+ }
+ }
+}
+
+
+
+
diff --git a/src/Tools/fjcontrib/EnergyCorrelator/example_basic_usage.ref b/src/Tools/fjcontrib/EnergyCorrelator/example_basic_usage.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/EnergyCorrelator/example_basic_usage.ref
@@ -0,0 +1,45 @@
+# read an event with 354 particles
+#--------------------------------------------------------------------------
+# FastJet release 3.2.0
+# M. Cacciari, G.P. Salam and G. Soyez
+# A software package for jet finding and analysis at colliders
+# http://fastjet.fr
+#
+# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package
+# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210].
+#
+# FastJet is provided without warranty under the terms of the GNU GPLv2.
+# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code
+# and 3rd party plugin jet algorithms. See COPYING file for details.
+#--------------------------------------------------------------------------
+-------------------------------------------------------------------------------------
+EnergyCorrelator: C series
+-------------------------------------------------------------------------------------
+ beta C1 C2 C3
+ 1.000 0.010342 0.097588 0.270742
+ 2.000 0.001315 0.158011 0.279675
+-------------------------------------------------------------------------------------
+EnergyCorrelator: D2, orignal (alpha=beta) and generalized
+-------------------------------------------------------------------------------------
+ beta D2 D2(alpha=1) D2(alpha=2)
+ 1.000 9.435950 9.435950 223402.841831
+ 2.000 120.129760 0.218810 120.129760
+-------------------------------------------------------------------------------------
+EnergyCorrelator: N series
+-------------------------------------------------------------------------------------
+ beta N2 N3
+ 1.000 0.430942 1.979487
+ 2.000 0.365859 6.700247
+-------------------------------------------------------------------------------------
+EnergyCorrelator: M series
+-------------------------------------------------------------------------------------
+ beta M2 M3
+ 1.000 0.071101 0.099746
+ 2.000 0.010448 0.036511
+-------------------------------------------------------------------------------------
+EnergyCorrelator: U series
+-------------------------------------------------------------------------------------
+ beta U1 U2 U3
+ 0.500 0.05378579 0.00805855 0.00105555
+ 1.000 0.01034218 0.00073534 0.00007335
+ 2.000 0.00131534 0.00001374 0.00000050
diff --git a/src/Tools/fjcontrib/Makefile.am b/src/Tools/fjcontrib/Makefile.am
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/Makefile.am
@@ -0,0 +1,1 @@
+SUBDIRS = EnergyCorrelator Nsubjettiness RecursiveTools
diff --git a/src/Tools/Nsubjettiness/AUTHORS b/src/Tools/fjcontrib/Nsubjettiness/AUTHORS
rename from src/Tools/Nsubjettiness/AUTHORS
rename to src/Tools/fjcontrib/Nsubjettiness/AUTHORS
diff --git a/src/Tools/Nsubjettiness/AxesDefinition.cc b/src/Tools/fjcontrib/Nsubjettiness/AxesDefinition.cc
rename from src/Tools/Nsubjettiness/AxesDefinition.cc
rename to src/Tools/fjcontrib/Nsubjettiness/AxesDefinition.cc
--- a/src/Tools/Nsubjettiness/AxesDefinition.cc
+++ b/src/Tools/fjcontrib/Nsubjettiness/AxesDefinition.cc
@@ -1,95 +1,97 @@
// Nsubjettiness Package
// Questions/Comments? jthaler@jthaler.net
//
// Copyright (c) 2011-14
// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
//
// $Id: AxesDefinition.cc 833 2015-07-23 14:35:23Z jthaler $
//----------------------------------------------------------------------
// This file is part of FastJet contrib.
//
// It is free software; you can redistribute it and/or modify it under
// the terms of the GNU General Public License as published by the
// Free Software Foundation; either version 2 of the License, or (at
// your option) any later version.
//
// It is distributed in the hope that it will be useful, but WITHOUT
// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
// License for more details.
//
// You should have received a copy of the GNU General Public License
// along with this code. If not, see <http://www.gnu.org/licenses/>.
//----------------------------------------------------------------------
#include "AxesDefinition.hh"
-namespace Rivet {
+namespace Rivet {
+namespace fjcontrib {
namespace Nsubjettiness { using namespace fastjet;
-
+
// Repeatedly calls the one pass finder to try to find global minimum
std::vector<fastjet::PseudoJet> AxesDefinition::get_multi_pass_axes(int n_jets,
const std::vector <fastjet::PseudoJet> & inputJets,
const std::vector <fastjet::PseudoJet> & seedAxes,
const MeasureDefinition* measure) const {
-
+
assert(n_jets == (int)seedAxes.size()); //added int casting to get rid of compiler warning
-
+
// first iteration
std::vector<fastjet::PseudoJet> bestAxes = measure->get_one_pass_axes(n_jets, inputJets, seedAxes,_nAttempts,_accuracy);
-
+
double bestTau = measure->result(inputJets,bestAxes);
-
+
for (int l = 1; l < _Npass; l++) { // Do minimization procedure multiple times (l = 1 to start since first iteration is done already)
-
+
// Add noise to current best axes
std::vector< PseudoJet > noiseAxes(n_jets, PseudoJet(0,0,0,0));
for (int k = 0; k < n_jets; k++) {
noiseAxes[k] = jiggle(bestAxes[k]);
}
-
+
std::vector<fastjet::PseudoJet> testAxes = measure->get_one_pass_axes(n_jets, inputJets, noiseAxes,_nAttempts,_accuracy);
double testTau = measure->result(inputJets,testAxes);
-
+
if (testTau < bestTau) {
bestTau = testTau;
bestAxes = testAxes;
}
}
-
+
return bestAxes;
}
-
+
// Used by multi-pass minimization to jiggle axes with noise range.
PseudoJet AxesDefinition::jiggle(const PseudoJet& axis) const {
double phi_noise = ((double)rand()/(double)RAND_MAX) * _noise_range * 2.0 - _noise_range;
double rap_noise = ((double)rand()/(double)RAND_MAX) * _noise_range * 2.0 - _noise_range;
-
+
double new_phi = axis.phi() + phi_noise;
if (new_phi >= 2.0*M_PI) new_phi -= 2.0*M_PI;
if (new_phi <= -2.0*M_PI) new_phi += 2.0*M_PI;
-
+
PseudoJet newAxis(0,0,0,0);
newAxis.reset_PtYPhiM(axis.perp(),axis.rap() + rap_noise,new_phi);
return newAxis;
}
-
+
LimitedWarning HardestJetAxes::_too_few_axes_warning;
LimitedWarning ExclusiveJetAxes::_too_few_axes_warning;
LimitedWarning ExclusiveCombinatorialJetAxes::_too_few_axes_warning;
std::vector<fastjet::PseudoJet> Manual_Axes::get_starting_axes(int,
const std::vector<fastjet::PseudoJet>&,
const MeasureDefinition *) const {
// This is a function dummy and should never be called
assert(false);
std::vector<fastjet::PseudoJet> dummy;
return dummy;
}
} // namespace Nsubjettiness
}
+}
diff --git a/src/Tools/Nsubjettiness/COPYING b/src/Tools/fjcontrib/Nsubjettiness/COPYING
rename from src/Tools/Nsubjettiness/COPYING
rename to src/Tools/fjcontrib/Nsubjettiness/COPYING
diff --git a/src/Tools/Nsubjettiness/ChangeLog b/src/Tools/fjcontrib/Nsubjettiness/ChangeLog
rename from src/Tools/Nsubjettiness/ChangeLog
rename to src/Tools/fjcontrib/Nsubjettiness/ChangeLog
diff --git a/src/Tools/Nsubjettiness/ExtraRecombiners.cc b/src/Tools/fjcontrib/Nsubjettiness/ExtraRecombiners.cc
rename from src/Tools/Nsubjettiness/ExtraRecombiners.cc
rename to src/Tools/fjcontrib/Nsubjettiness/ExtraRecombiners.cc
--- a/src/Tools/Nsubjettiness/ExtraRecombiners.cc
+++ b/src/Tools/fjcontrib/Nsubjettiness/ExtraRecombiners.cc
@@ -1,103 +1,105 @@
// Nsubjettiness Package
// Questions/Comments? jthaler@jthaler.net
//
// Copyright (c) 2011-14
// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
//
// $Id: ExtraRecombiners.cc 842 2015-08-20 13:44:31Z jthaler $
//----------------------------------------------------------------------
// This file is part of FastJet contrib.
//
// It is free software; you can redistribute it and/or modify it under
// the terms of the GNU General Public License as published by the
// Free Software Foundation; either version 2 of the License, or (at
// your option) any later version.
//
// It is distributed in the hope that it will be useful, but WITHOUT
// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
// License for more details.
//
// You should have received a copy of the GNU General Public License
// along with this code. If not, see <http://www.gnu.org/licenses/>.
//----------------------------------------------------------------------
#include "ExtraRecombiners.hh"
-namespace Rivet {
+namespace Rivet {
+namespace fjcontrib {
namespace Nsubjettiness{
-
+
std::string GeneralEtSchemeRecombiner::description() const {
return "General Et-scheme recombination";
}
// recombine pa and pb according to a generalized Et-scheme parameterized by the power delta
void GeneralEtSchemeRecombiner::recombine(const fastjet::PseudoJet & pa, const fastjet::PseudoJet & pb, fastjet::PseudoJet & pab) const {
-
+
// Define new weights for recombination according to delta
// definition of ratio done so that we do not encounter issues about numbers being too large for huge values of delta
double ratio;
if (std::abs(_delta - 1.0) < std::numeric_limits<double>::epsilon()) ratio = pb.perp()/pa.perp(); // save computation time of pow()
else ratio = pow(pb.perp()/pa.perp(), _delta);
double weighta = 1.0/(1.0 + ratio);
double weightb = 1.0/(1.0 + 1.0/ratio);
-
+
double perp_ab = pa.perp() + pb.perp();
// reweight the phi and rap sums according to the weights above
if (perp_ab != 0.0) {
double y_ab = (weighta * pa.rap() + weightb * pb.rap());
-
+
double phi_a = pa.phi(), phi_b = pb.phi();
if (phi_a - phi_b > pi) phi_b += twopi;
if (phi_a - phi_b < -pi) phi_b -= twopi;
double phi_ab = (weighta * phi_a + weightb * phi_b);
-
+
pab.reset_PtYPhiM(perp_ab, y_ab, phi_ab);
-
+
}
else {
pab.reset(0.0,0.0,0.0,0.0);
}
}
std::string WinnerTakeAllRecombiner::description() const {
return "Winner-Take-All recombination";
}
// recombine pa and pb by creating pab with energy of the sum of particle energies in the direction of the harder particle
// updated recombiner to use more general form of a metric equal to E*(pT/E)^(alpha), which reduces to pT*cosh(rap)^(1-alpha)
-// alpha is specified by the user. The default is alpha = 1, which is the typical behavior. alpha = 2 provides a metric which more
+// alpha is specified by the user. The default is alpha = 1, which is the typical behavior. alpha = 2 provides a metric which more
// favors central jets
void WinnerTakeAllRecombiner::recombine(const fastjet::PseudoJet & pa, const fastjet::PseudoJet & pb, fastjet::PseudoJet & pab) const {
double a_pt = pa.perp(), b_pt = pb.perp(), a_rap = pa.rap(), b_rap = pb.rap();
-
+
// special case of alpha = 1, everything is just pt (made separate so that pow function isn't called)
if (_alpha == 1.0) {
if (a_pt >= b_pt) {
pab.reset_PtYPhiM(a_pt + b_pt, a_rap, pa.phi());
}
else if (b_pt > a_pt) {
pab.reset_PtYPhiM(a_pt + b_pt, b_rap, pb.phi());
}
}
// every other case uses additional cosh(rap) term
else {
double a_metric = a_pt*pow(cosh(a_rap), 1.0-_alpha);
double b_metric = b_pt*pow(cosh(b_rap), 1.0-_alpha);
if (a_metric >= b_metric) {
double new_pt = a_pt + b_pt*pow(cosh(b_rap)/cosh(a_rap), 1.0-_alpha);
pab.reset_PtYPhiM(new_pt, a_rap, pa.phi());
}
if (b_metric > a_metric) {
double new_pt = b_pt + a_pt*pow(cosh(a_rap)/cosh(b_rap), 1.0-_alpha);
pab.reset_PtYPhiM(new_pt, b_rap, pb.phi());
}
}
}
} //namespace Nsubjettiness
}
+}
diff --git a/src/Tools/Nsubjettiness/Makefile.am b/src/Tools/fjcontrib/Nsubjettiness/Makefile.am
rename from src/Tools/Nsubjettiness/Makefile.am
rename to src/Tools/fjcontrib/Nsubjettiness/Makefile.am
--- a/src/Tools/Nsubjettiness/Makefile.am
+++ b/src/Tools/fjcontrib/Nsubjettiness/Makefile.am
@@ -1,15 +1,13 @@
noinst_LTLIBRARIES = libRivetNsubjettiness.la
libRivetNsubjettiness_la_SOURCES = \
-Nsubjettiness.cc \
-Njettiness.cc \
-NjettinessPlugin.cc \
-XConePlugin.cc \
-MeasureDefinition.cc \
-ExtraRecombiners.cc \
-AxesDefinition.cc \
-TauComponents.cc
+ Nsubjettiness.cc \
+ Njettiness.cc \
+ NjettinessPlugin.cc \
+ XConePlugin.cc \
+ MeasureDefinition.cc \
+ ExtraRecombiners.cc \
+ AxesDefinition.cc \
+ TauComponents.cc
-libRivetNsubjettiness_la_CPPFLAGS = \
-$(AM_CPPFLAGS) \
--I${top_srcdir}/include/Rivet/Tools/Nsubjettiness
\ No newline at end of file
+libRivetNsubjettiness_la_CPPFLAGS = $(AM_CPPFLAGS) -I${top_srcdir}/include/Rivet/Tools/fjcontrib
diff --git a/src/Tools/Nsubjettiness/MeasureDefinition.cc b/src/Tools/fjcontrib/Nsubjettiness/MeasureDefinition.cc
rename from src/Tools/Nsubjettiness/MeasureDefinition.cc
rename to src/Tools/fjcontrib/Nsubjettiness/MeasureDefinition.cc
--- a/src/Tools/Nsubjettiness/MeasureDefinition.cc
+++ b/src/Tools/fjcontrib/Nsubjettiness/MeasureDefinition.cc
@@ -1,628 +1,630 @@
// Nsubjettiness Package
// Questions/Comments? jthaler@jthaler.net
//
// Copyright (c) 2011-14
// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
//
// $Id: MeasureDefinition.cc 946 2016-06-14 19:11:27Z jthaler $
//----------------------------------------------------------------------
// This file is part of FastJet contrib.
//
// It is free software; you can redistribute it and/or modify it under
// the terms of the GNU General Public License as published by the
// Free Software Foundation; either version 2 of the License, or (at
// your option) any later version.
//
// It is distributed in the hope that it will be useful, but WITHOUT
// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
// License for more details.
//
// You should have received a copy of the GNU General Public License
// along with this code. If not, see <http://www.gnu.org/licenses/>.
//----------------------------------------------------------------------
// #include "AxesRefiner.hh"
#include "MeasureDefinition.hh"
#include <iomanip>
namespace Rivet {
+namespace fjcontrib {
namespace Nsubjettiness { using namespace fastjet;
///////
//
// Measure Function
//
///////
//descriptions updated to include measure type
std::string DefaultMeasure::description() const {
std::stringstream stream;
stream << std::fixed << std::setprecision(2)
<< "Default Measure (should not be used directly)";
return stream.str();
}
std::string NormalizedMeasure::description() const {
std::stringstream stream;
stream << std::fixed << std::setprecision(2)
<< "Normalized Measure (beta = " << _beta << ", R0 = " << _R0 << ")";
return stream.str();
}
std::string UnnormalizedMeasure::description() const {
std::stringstream stream;
stream << std::fixed << std::setprecision(2)
<< "Unnormalized Measure (beta = " << _beta << ", in GeV)";
return stream.str();
}
std::string NormalizedCutoffMeasure::description() const {
std::stringstream stream;
stream << std::fixed << std::setprecision(2)
<< "Normalized Cutoff Measure (beta = " << _beta << ", R0 = " << _R0 << ", Rcut = " << _Rcutoff << ")";
return stream.str();
}
std::string UnnormalizedCutoffMeasure::description() const {
std::stringstream stream;
stream << std::fixed << std::setprecision(2)
<< "Unnormalized Cutoff Measure (beta = " << _beta << ", Rcut = " << _Rcutoff << ", in GeV)";
return stream.str();
}
//std::string DeprecatedGeometricMeasure::description() const {
// std::stringstream stream;
// stream << std::fixed << std::setprecision(2)
// << "Deprecated Geometric Measure (beta = " << _jet_beta << ", in GeV)";
// return stream.str();
//}
//std::string DeprecatedGeometricCutoffMeasure::description() const {
// std::stringstream stream;
// stream << std::fixed << std::setprecision(2)
// << "Deprecated Geometric Cutoff Measure (beta = " << _jet_beta << ", Rcut = " << _Rcutoff << ", in GeV)";
// return stream.str();
//}
std::string ConicalMeasure::description() const {
std::stringstream stream;
stream << std::fixed << std::setprecision(2)
<< "Conical Measure (beta = " << _beta << ", Rcut = " << _Rcutoff << ", in GeV)";
return stream.str();
}
std::string OriginalGeometricMeasure::description() const {
std::stringstream stream;
stream << std::fixed << std::setprecision(2)
<< "Original Geometric Measure (Rcut = " << _Rcutoff << ", in GeV)";
return stream.str();
}
std::string ModifiedGeometricMeasure::description() const {
std::stringstream stream;
stream << std::fixed << std::setprecision(2)
<< "Modified Geometric Measure (Rcut = " << _Rcutoff << ", in GeV)";
return stream.str();
}
std::string ConicalGeometricMeasure::description() const {
std::stringstream stream;
stream << std::fixed << std::setprecision(2)
<< "Conical Geometric Measure (beta = " << _jet_beta << ", gamma = " << _beam_gamma << ", Rcut = " << _Rcutoff << ", in GeV)";
return stream.str();
}
std::string XConeMeasure::description() const {
std::stringstream stream;
stream << std::fixed << std::setprecision(2)
<< "XCone Measure (beta = " << _jet_beta << ", Rcut = " << _Rcutoff << ", in GeV)";
return stream.str();
}
// Return all of the necessary TauComponents for specific input particles and axes
TauComponents MeasureDefinition::component_result(const std::vector<fastjet::PseudoJet>& particles,
const std::vector<fastjet::PseudoJet>& axes) const {
// first find partition
TauPartition partition = get_partition(particles,axes);
// then return result calculated from partition
return component_result_from_partition(partition,axes);
}
TauPartition MeasureDefinition::get_partition(const std::vector<fastjet::PseudoJet>& particles,
const std::vector<fastjet::PseudoJet>& axes) const {
TauPartition myPartition(axes.size());
// Figures out the partiting of the input particles into the various jet pieces
// Based on which axis the parition is closest to
for (unsigned i = 0; i < particles.size(); i++) {
// find minimum distance; start with beam (-1) for reference
int j_min = -1;
double minRsq;
if (has_beam()) minRsq = beam_distance_squared(particles[i]);
else minRsq = std::numeric_limits<double>::max(); // make it large value
// check to see which axis the particle is closest to
for (unsigned j = 0; j < axes.size(); j++) {
double tempRsq = jet_distance_squared(particles[i],axes[j]); // delta R distance
if (tempRsq < minRsq) {
minRsq = tempRsq;
j_min = j;
}
}
if (j_min == -1) {
assert(has_beam()); // should have beam for this to make sense.
myPartition.push_back_beam(particles[i],i);
} else {
myPartition.push_back_jet(j_min,particles[i],i);
}
}
return myPartition;
}
// Uses existing partition and calculates result
// TODO: Can we cache this for speed up when doing area subtraction?
TauComponents MeasureDefinition::component_result_from_partition(const TauPartition& partition,
const std::vector<fastjet::PseudoJet>& axes) const {
std::vector<double> jetPieces(axes.size(), 0.0);
double beamPiece = 0.0;
double tauDen = 0.0;
if (!has_denominator()) tauDen = 1.0; // if no denominator, then 1.0 for no normalization factor
// first find jet pieces
for (unsigned j = 0; j < axes.size(); j++) {
std::vector<PseudoJet> thisPartition = partition.jet(j).constituents();
for (unsigned i = 0; i < thisPartition.size(); i++) {
jetPieces[j] += jet_numerator(thisPartition[i],axes[j]); //numerator jet piece
if (has_denominator()) tauDen += denominator(thisPartition[i]); // denominator
}
}
// then find beam piece
if (has_beam()) {
std::vector<PseudoJet> beamPartition = partition.beam().constituents();
for (unsigned i = 0; i < beamPartition.size(); i++) {
beamPiece += beam_numerator(beamPartition[i]); //numerator beam piece
if (has_denominator()) tauDen += denominator(beamPartition[i]); // denominator
}
}
// create jets for storage in TauComponents
std::vector<PseudoJet> jets = partition.jets();
return TauComponents(_tau_mode, jetPieces, beamPiece, tauDen, jets, axes);
}
// new methods added to generalize energy and angle squared for different measure types
double DefaultMeasure::energy(const PseudoJet& jet) const {
double energy;
switch (_measure_type) {
case pt_R :
case perp_lorentz_dot :
energy = jet.perp();
break;
case E_theta :
case lorentz_dot :
energy = jet.e();
break;
default : {
assert(_measure_type == pt_R || _measure_type == E_theta || _measure_type == lorentz_dot || _measure_type == perp_lorentz_dot);
energy = std::numeric_limits<double>::quiet_NaN();
break;
}
}
return energy;
}
double DefaultMeasure::angleSquared(const PseudoJet& jet1, const PseudoJet& jet2) const {
double pseudoRsquared;
switch(_measure_type) {
case pt_R : {
pseudoRsquared = jet1.squared_distance(jet2);
break;
}
case E_theta : {
// doesn't seem to be a fastjet built in for this
double dot = jet1.px()*jet2.px() + jet1.py()*jet2.py() + jet1.pz()*jet2.pz();
double norm1 = sqrt(jet1.px()*jet1.px() + jet1.py()*jet1.py() + jet1.pz()*jet1.pz());
double norm2 = sqrt(jet2.px()*jet2.px() + jet2.py()*jet2.py() + jet2.pz()*jet2.pz());
double costheta = dot/(norm1 * norm2);
if (costheta > 1.0) costheta = 1.0; // Need to handle case of numerical overflow
double theta = acos(costheta);
pseudoRsquared = theta*theta;
break;
}
case lorentz_dot : {
double dotproduct = dot_product(jet1,jet2);
pseudoRsquared = 2.0 * dotproduct / (jet1.e() * jet2.e());
break;
}
case perp_lorentz_dot : {
PseudoJet lightJet = lightFrom(jet2); // assuming jet2 is the axis
double dotproduct = dot_product(jet1,lightJet);
pseudoRsquared = 2.0 * dotproduct / (lightJet.pt() * jet1.pt());
break;
}
default : {
assert(_measure_type == pt_R || _measure_type == E_theta || _measure_type == lorentz_dot || _measure_type == perp_lorentz_dot);
pseudoRsquared = std::numeric_limits<double>::quiet_NaN();
break;
}
}
return pseudoRsquared;
}
///////
//
// Axes Refining
//
///////
// uses minimization of N-jettiness to continually update axes until convergence.
// The function returns the axes found at the (local) minimum
// This is the general axes refiner that can be used for a generic measure (but is
// overwritten in the case of the conical measure and the deprecated geometric measure)
std::vector<fastjet::PseudoJet> MeasureDefinition::get_one_pass_axes(int n_jets,
const std::vector <fastjet::PseudoJet> & particles,
const std::vector<fastjet::PseudoJet>& currentAxes,
int nAttempts,
double accuracy) const {
assert(n_jets == (int)currentAxes.size());
std::vector<fastjet::PseudoJet> seedAxes = currentAxes;
std::vector<fastjet::PseudoJet> temp_axes(seedAxes.size(),fastjet::PseudoJet(0,0,0,0));
for (unsigned int k = 0; k < seedAxes.size(); k++) {
seedAxes[k] = lightFrom(seedAxes[k]) * seedAxes[k].E(); // making light-like, but keeping energy
}
double seedTau = result(particles, seedAxes);
std::vector<fastjet::PseudoJet> bestAxesSoFar = seedAxes;
double bestTauSoFar = seedTau;
for (int i_att = 0; i_att < nAttempts; i_att++) {
std::vector<fastjet::PseudoJet> newAxes(seedAxes.size(),fastjet::PseudoJet(0,0,0,0));
std::vector<fastjet::PseudoJet> summed_jets(seedAxes.size(), fastjet::PseudoJet(0,0,0,0));
// find closest axis and assign to that
for (unsigned int i = 0; i < particles.size(); i++) {
// start from unclustered beam measure
int minJ = -1;
double minDist = beam_distance_squared(particles[i]);
// which axis am I closest to?
for (unsigned int j = 0; j < seedAxes.size(); j++) {
double tempDist = jet_distance_squared(particles[i],seedAxes[j]);
if (tempDist < minDist) {
minDist = tempDist;
minJ = j;
}
}
// if not unclustered, then cluster
if (minJ != -1) {
summed_jets[minJ] += particles[i]; // keep track of energy to use later.
if (_useAxisScaling) {
double pseudoMomentum = dot_product(lightFrom(seedAxes[minJ]),particles[i]) + accuracy; // need small offset to avoid potential divide by zero issues
double axis_scaling = (double)jet_numerator(particles[i], seedAxes[minJ])/pseudoMomentum;
newAxes[minJ] += particles[i]*axis_scaling;
}
}
}
if (!_useAxisScaling) newAxes = summed_jets;
// convert the axes to LightLike and then back to PseudoJet
for (unsigned int k = 0; k < newAxes.size(); k++) {
if (newAxes[k].perp() > 0) {
newAxes[k] = lightFrom(newAxes[k]);
newAxes[k] *= summed_jets[k].E(); // scale by energy to get sensible result
}
}
// calculate tau on new axes
double newTau = result(particles, newAxes);
// find the smallest value of tau (and the corresponding axes) so far
if (newTau < bestTauSoFar) {
bestAxesSoFar = newAxes;
bestTauSoFar = newTau;
}
if (fabs(newTau - seedTau) < accuracy) {// close enough for jazz
seedAxes = newAxes;
seedTau = newTau;
break;
}
seedAxes = newAxes;
seedTau = newTau;
}
// return the axes corresponding to the smallest tau found throughout all iterations
// this is to prevent the minimization from returning a non-minimized of tau due to potential oscillations around the minimum
return bestAxesSoFar;
}
// One pass minimization for the DefaultMeasure
// Given starting axes, update to find better axes by using Kmeans clustering around the old axes
template <int N>
std::vector<LightLikeAxis> DefaultMeasure::UpdateAxesFast(const std::vector <LightLikeAxis> & old_axes,
const std::vector <fastjet::PseudoJet> & inputJets,
double accuracy
) const {
assert(old_axes.size() == N);
// some storage, declared static to save allocation/re-allocation costs
static LightLikeAxis new_axes[N];
static fastjet::PseudoJet new_jets[N];
for (int n = 0; n < N; ++n) {
new_axes[n].reset(0.0,0.0,0.0,0.0);
new_jets[n].reset_momentum(0.0,0.0,0.0,0.0);
}
double precision = accuracy; //TODO: actually cascade this in
/////////////// Assignment Step //////////////////////////////////////////////////////////
std::vector<int> assignment_index(inputJets.size());
int k_assign = -1;
for (unsigned i = 0; i < inputJets.size(); i++){
double smallestDist = std::numeric_limits<double>::max(); //large number
for (int k = 0; k < N; k++) {
double thisDist = old_axes[k].DistanceSq(inputJets[i]);
if (thisDist < smallestDist) {
smallestDist = thisDist;
k_assign = k;
}
}
if (smallestDist > sq(_Rcutoff)) {k_assign = -1;}
assignment_index[i] = k_assign;
}
//////////////// Update Step /////////////////////////////////////////////////////////////
double distPhi, old_dist;
for (unsigned i = 0; i < inputJets.size(); i++) {
int old_jet_i = assignment_index[i];
if (old_jet_i == -1) {continue;}
const fastjet::PseudoJet& inputJet_i = inputJets[i];
LightLikeAxis& new_axis_i = new_axes[old_jet_i];
double inputPhi_i = inputJet_i.phi();
double inputRap_i = inputJet_i.rap();
// optimize pow() call
// add noise (the precision term) to make sure we don't divide by zero
if (_beta == 1.0) {
double DR = std::sqrt(sq(precision) + old_axes[old_jet_i].DistanceSq(inputJet_i));
old_dist = 1.0/DR;
} else if (_beta == 2.0) {
old_dist = 1.0;
} else if (_beta == 0.0) {
double DRSq = sq(precision) + old_axes[old_jet_i].DistanceSq(inputJet_i);
old_dist = 1.0/DRSq;
} else {
old_dist = sq(precision) + old_axes[old_jet_i].DistanceSq(inputJet_i);
old_dist = std::pow(old_dist, (0.5*_beta-1.0));
}
// TODO: Put some of these addition functions into light-like axes
// rapidity sum
new_axis_i.set_rap(new_axis_i.rap() + inputJet_i.perp() * inputRap_i * old_dist);
// phi sum
distPhi = inputPhi_i - old_axes[old_jet_i].phi();
if (fabs(distPhi) <= M_PI){
new_axis_i.set_phi( new_axis_i.phi() + inputJet_i.perp() * inputPhi_i * old_dist );
} else if (distPhi > M_PI) {
new_axis_i.set_phi( new_axis_i.phi() + inputJet_i.perp() * (-2*M_PI + inputPhi_i) * old_dist );
} else if (distPhi < -M_PI) {
new_axis_i.set_phi( new_axis_i.phi() + inputJet_i.perp() * (+2*M_PI + inputPhi_i) * old_dist );
}
// weights sum
new_axis_i.set_weight( new_axis_i.weight() + inputJet_i.perp() * old_dist );
// momentum magnitude sum
new_jets[old_jet_i] += inputJet_i;
}
// normalize sums
for (int k = 0; k < N; k++) {
if (new_axes[k].weight() == 0) {
// no particles were closest to this axis! Return to old axis instead of (0,0,0,0)
new_axes[k] = old_axes[k];
} else {
new_axes[k].set_rap( new_axes[k].rap() / new_axes[k].weight() );
new_axes[k].set_phi( new_axes[k].phi() / new_axes[k].weight() );
new_axes[k].set_phi( std::fmod(new_axes[k].phi() + 2*M_PI, 2*M_PI) );
new_axes[k].set_mom( std::sqrt(new_jets[k].modp2()) );
}
}
std::vector<LightLikeAxis> new_axes_vec(N);
for (unsigned k = 0; k < N; ++k) new_axes_vec[k] = new_axes[k];
return new_axes_vec;
}
// Given N starting axes, this function updates all axes to find N better axes.
// (This is just a wrapper for the templated version above.)
// TODO: Consider removing this in a future version
std::vector<LightLikeAxis> DefaultMeasure::UpdateAxes(const std::vector <LightLikeAxis> & old_axes,
const std::vector <fastjet::PseudoJet> & inputJets,
double accuracy) const {
int N = old_axes.size();
switch (N) {
case 1: return UpdateAxesFast<1>(old_axes, inputJets, accuracy);
case 2: return UpdateAxesFast<2>(old_axes, inputJets, accuracy);
case 3: return UpdateAxesFast<3>(old_axes, inputJets, accuracy);
case 4: return UpdateAxesFast<4>(old_axes, inputJets, accuracy);
case 5: return UpdateAxesFast<5>(old_axes, inputJets, accuracy);
case 6: return UpdateAxesFast<6>(old_axes, inputJets, accuracy);
case 7: return UpdateAxesFast<7>(old_axes, inputJets, accuracy);
case 8: return UpdateAxesFast<8>(old_axes, inputJets, accuracy);
case 9: return UpdateAxesFast<9>(old_axes, inputJets, accuracy);
case 10: return UpdateAxesFast<10>(old_axes, inputJets, accuracy);
case 11: return UpdateAxesFast<11>(old_axes, inputJets, accuracy);
case 12: return UpdateAxesFast<12>(old_axes, inputJets, accuracy);
case 13: return UpdateAxesFast<13>(old_axes, inputJets, accuracy);
case 14: return UpdateAxesFast<14>(old_axes, inputJets, accuracy);
case 15: return UpdateAxesFast<15>(old_axes, inputJets, accuracy);
case 16: return UpdateAxesFast<16>(old_axes, inputJets, accuracy);
case 17: return UpdateAxesFast<17>(old_axes, inputJets, accuracy);
case 18: return UpdateAxesFast<18>(old_axes, inputJets, accuracy);
case 19: return UpdateAxesFast<19>(old_axes, inputJets, accuracy);
case 20: return UpdateAxesFast<20>(old_axes, inputJets, accuracy);
default: std::cout << "N-jettiness is hard-coded to only allow up to 20 jets!" << std::endl;
return std::vector<LightLikeAxis>();
}
}
// uses minimization of N-jettiness to continually update axes until convergence.
// The function returns the axes found at the (local) minimum
std::vector<fastjet::PseudoJet> DefaultMeasure::get_one_pass_axes(int n_jets,
const std::vector <fastjet::PseudoJet> & inputJets,
const std::vector<fastjet::PseudoJet>& seedAxes,
int nAttempts,
double accuracy
) const {
// if the measure type doesn't use the pt_R metric, then the standard minimization scheme should be used
if (_measure_type != pt_R) {
return MeasureDefinition::get_one_pass_axes(n_jets, inputJets, seedAxes, nAttempts, accuracy);
}
// convert from PseudoJets to LightLikeAxes
std::vector< LightLikeAxis > old_axes(n_jets, LightLikeAxis(0,0,0,0));
for (int k = 0; k < n_jets; k++) {
old_axes[k].set_rap( seedAxes[k].rap() );
old_axes[k].set_phi( seedAxes[k].phi() );
old_axes[k].set_mom( seedAxes[k].modp() );
}
// Find new axes by iterating (only one pass here)
std::vector< LightLikeAxis > new_axes(n_jets, LightLikeAxis(0,0,0,0));
double cmp = std::numeric_limits<double>::max(); //large number
int h = 0;
while (cmp > accuracy && h < nAttempts) { // Keep updating axes until near-convergence or too many update steps
cmp = 0.0;
h++;
new_axes = UpdateAxes(old_axes, inputJets,accuracy); // Update axes
for (int k = 0; k < n_jets; k++) {
cmp += old_axes[k].Distance(new_axes[k]);
}
cmp = cmp / ((double) n_jets);
old_axes = new_axes;
}
// Convert from internal LightLikeAxes to PseudoJet
std::vector<fastjet::PseudoJet> outputAxes;
for (int k = 0; k < n_jets; k++) {
fastjet::PseudoJet temp = old_axes[k].ConvertToPseudoJet();
outputAxes.push_back(temp);
}
// this is used to debug the minimization routine to make sure that it works.
bool do_debug = false;
if (do_debug) {
// get this information to make sure that minimization is working properly
double seed_tau = result(inputJets, seedAxes);
double outputTau = result(inputJets, outputAxes);
assert(outputTau <= seed_tau);
}
return outputAxes;
}
//// One-pass minimization for the Deprecated Geometric Measure
//// Uses minimization of the geometric distance in order to find the minimum axes.
//// It continually updates until it reaches convergence or it reaches the maximum number of attempts.
//// This is essentially the same as a stable cone finder.
//std::vector<fastjet::PseudoJet> DeprecatedGeometricCutoffMeasure::get_one_pass_axes(int n_jets,
// const std::vector <fastjet::PseudoJet> & particles,
// const std::vector<fastjet::PseudoJet>& currentAxes,
// int nAttempts,
// double accuracy) const {
//
// assert(n_jets == (int)currentAxes.size()); //added int casting to get rid of compiler warning
//
// std::vector<fastjet::PseudoJet> seedAxes = currentAxes;
// double seedTau = result(particles, seedAxes);
//
// for (int i = 0; i < nAttempts; i++) {
//
// std::vector<fastjet::PseudoJet> newAxes(seedAxes.size(),fastjet::PseudoJet(0,0,0,0));
//
// // find closest axis and assign to that
// for (unsigned int i = 0; i < particles.size(); i++) {
//
// // start from unclustered beam measure
// int minJ = -1;
// double minDist = beam_distance_squared(particles[i]);
//
// // which axis am I closest to?
// for (unsigned int j = 0; j < seedAxes.size(); j++) {
// double tempDist = jet_distance_squared(particles[i],seedAxes[j]);
// if (tempDist < minDist) {
// minDist = tempDist;
// minJ = j;
// }
// }
//
// // if not unclustered, then cluster
// if (minJ != -1) newAxes[minJ] += particles[i];
// }
//
// // calculate tau on new axes
// seedAxes = newAxes;
// double tempTau = result(particles, newAxes);
//
// // close enough to stop?
// if (fabs(tempTau - seedTau) < accuracy) break;
// seedTau = tempTau;
// }
//
// return seedAxes;
//}
// Go from internal LightLikeAxis to PseudoJet
fastjet::PseudoJet LightLikeAxis::ConvertToPseudoJet() {
double px, py, pz, E;
E = _mom;
pz = (std::exp(2.0*_rap) - 1.0) / (std::exp(2.0*_rap) + 1.0) * E;
px = std::cos(_phi) * std::sqrt( std::pow(E,2) - std::pow(pz,2) );
py = std::sin(_phi) * std::sqrt( std::pow(E,2) - std::pow(pz,2) );
return fastjet::PseudoJet(px,py,pz,E);
}
} //namespace Nsubjettiness
}
+}
diff --git a/src/Tools/Nsubjettiness/NEWS b/src/Tools/fjcontrib/Nsubjettiness/NEWS
rename from src/Tools/Nsubjettiness/NEWS
rename to src/Tools/fjcontrib/Nsubjettiness/NEWS
diff --git a/src/Tools/Nsubjettiness/Njettiness.cc b/src/Tools/fjcontrib/Nsubjettiness/Njettiness.cc
rename from src/Tools/Nsubjettiness/Njettiness.cc
rename to src/Tools/fjcontrib/Nsubjettiness/Njettiness.cc
--- a/src/Tools/Nsubjettiness/Njettiness.cc
+++ b/src/Tools/fjcontrib/Nsubjettiness/Njettiness.cc
@@ -1,223 +1,225 @@
// Nsubjettiness Package
// Questions/Comments? jthaler@jthaler.net
//
// Copyright (c) 2011-14
// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
//
// $Id: Njettiness.cc 933 2016-04-04 22:23:32Z jthaler $
//----------------------------------------------------------------------
// This file is part of FastJet contrib.
//
// It is free software; you can redistribute it and/or modify it under
// the terms of the GNU General Public License as published by the
// Free Software Foundation; either version 2 of the License, or (at
// your option) any later version.
//
// It is distributed in the hope that it will be useful, but WITHOUT
// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
// License for more details.
//
// You should have received a copy of the GNU General Public License
// along with this code. If not, see <http://www.gnu.org/licenses/>.
//----------------------------------------------------------------------
#include "Njettiness.hh"
-namespace Rivet {
+namespace Rivet {
+namespace fjcontrib {
namespace Nsubjettiness { using namespace fastjet;
///////
//
// Main Njettiness Class
//
///////
LimitedWarning Njettiness::_old_measure_warning;
LimitedWarning Njettiness::_old_axes_warning;
-
+
// Constructor
Njettiness::Njettiness(const AxesDefinition & axes_def, const MeasureDefinition & measure_def)
: _axes_def(axes_def.create()), _measure_def(measure_def.create()) {}
-
+
// setAxes for Manual mode
void Njettiness::setAxes(const std::vector<fastjet::PseudoJet> & myAxes) {
if (_axes_def->needsManualAxes()) {
_currentAxes = myAxes;
} else {
throw Error("You can only use setAxes for manual AxesDefinitions");
}
}
-
+
// Calculates and returns all TauComponents that user would want.
// This information is stored in _current_tau_components for later access as well.
TauComponents Njettiness::getTauComponents(unsigned n_jets, const std::vector<fastjet::PseudoJet> & inputJets) const {
if (inputJets.size() <= n_jets) { //if not enough particles, return zero
_currentAxes = inputJets;
_currentAxes.resize(n_jets,fastjet::PseudoJet(0.0,0.0,0.0,0.0));
-
+
// Put in empty tau components
std::vector<double> dummy_jet_pieces;
_current_tau_components = TauComponents(UNDEFINED_SHAPE,
dummy_jet_pieces,
0.0,
1.0,
_currentAxes,
_currentAxes
);
_seedAxes = _currentAxes;
_currentPartition = TauPartition(n_jets); // empty partition
} else {
assert(_axes_def); // this should never fail.
-
+
if (_axes_def->needsManualAxes()) { // if manual mode
// take current axes as seeds
_seedAxes = _currentAxes;
-
+
// refine axes if requested
_currentAxes = _axes_def->get_refined_axes(n_jets,inputJets,_seedAxes, _measure_def.get());
} else { // non-manual axes
-
+
//set starting point for minimization
_seedAxes = _axes_def->get_starting_axes(n_jets,inputJets,_measure_def.get());
-
+
// refine axes as needed
_currentAxes = _axes_def->get_refined_axes(n_jets,inputJets,_seedAxes, _measure_def.get());
-
+
// NOTE: The above two function calls are combined in "AxesDefinition::get_axes"
// but are separated here to allow seed axes to be stored.
}
-
+
// Find and store partition
_currentPartition = _measure_def->get_partition(inputJets,_currentAxes);
-
+
// Find and store tau value
_current_tau_components = _measure_def->component_result_from_partition(_currentPartition, _currentAxes); // sets current Tau Values
}
return _current_tau_components;
}
-
+
///////
//
// Below is code for backward compatibility to use the old interface.
// May be deleted in a future version
//
///////
-
+
Njettiness::Njettiness(AxesMode axes_mode, const MeasureDefinition & measure_def)
: _axes_def(createAxesDef(axes_mode)), _measure_def(measure_def.create()) {}
// Convert from MeasureMode enum to MeasureDefinition
// This returns a pointer that will be claimed by a SharedPtr
MeasureDefinition* Njettiness::createMeasureDef(MeasureMode measure_mode, int num_para, double para1, double para2, double para3) const {
-
+
_old_measure_warning.warn("Njettiness::createMeasureDef: You are using the old MeasureMode way of specifying N-subjettiness measures. This is deprecated as of v2.1 and will be removed in v3.0. Please use MeasureDefinition instead.");
-
+
// definition of maximum Rcutoff for non-cutoff measures, changed later by other measures
double Rcutoff = std::numeric_limits<double>::max(); //large number
// Most (but not all) measures have some kind of beta value
double beta = std::numeric_limits<double>::quiet_NaN();
// The normalized measures have an R0 value.
double R0 = std::numeric_limits<double>::quiet_NaN();
-
+
// Find the MeasureFunction and set the parameters.
switch (measure_mode) {
case normalized_measure:
beta = para1;
R0 = para2;
if(num_para == 2) {
return new NormalizedMeasure(beta,R0);
} else {
throw Error("normalized_measure needs 2 parameters (beta and R0)");
}
break;
case unnormalized_measure:
beta = para1;
if(num_para == 1) {
return new UnnormalizedMeasure(beta);
} else {
throw Error("unnormalized_measure needs 1 parameter (beta)");
}
break;
case geometric_measure:
throw Error("This class has been removed. Please use OriginalGeometricMeasure, ModifiedGeometricMeasure, or ConicalGeometricMeasure with the new Njettiness constructor.");
break;
case normalized_cutoff_measure:
beta = para1;
R0 = para2;
Rcutoff = para3; //Rcutoff parameter is 3rd parameter in normalized_cutoff_measure
if (num_para == 3) {
return new NormalizedCutoffMeasure(beta,R0,Rcutoff);
} else {
throw Error("normalized_cutoff_measure has 3 parameters (beta, R0, Rcutoff)");
}
break;
case unnormalized_cutoff_measure:
beta = para1;
Rcutoff = para2; //Rcutoff parameter is 2nd parameter in normalized_cutoff_measure
if (num_para == 2) {
return new UnnormalizedCutoffMeasure(beta,Rcutoff);
} else {
throw Error("unnormalized_cutoff_measure has 2 parameters (beta, Rcutoff)");
}
break;
case geometric_cutoff_measure:
throw Error("This class has been removed. Please use OriginalGeometricMeasure, ModifiedGeometricMeasure, or ConicalGeometricMeasure with the new Njettiness constructor.");
default:
assert(false);
break;
}
return NULL;
}
// Convert from AxesMode enum to AxesDefinition
// This returns a pointer that will be claimed by a SharedPtr
AxesDefinition* Njettiness::createAxesDef(Njettiness::AxesMode axes_mode) const {
-
+
_old_axes_warning.warn("Njettiness::createAxesDef: You are using the old AxesMode way of specifying N-subjettiness axes. This is deprecated as of v2.1 and will be removed in v3.0. Please use AxesDefinition instead.");
-
-
+
+
switch (axes_mode) {
case wta_kt_axes:
return new WTA_KT_Axes();
case wta_ca_axes:
return new WTA_CA_Axes();
case kt_axes:
return new KT_Axes();
case ca_axes:
return new CA_Axes();
case antikt_0p2_axes:
return new AntiKT_Axes(0.2);
case onepass_wta_kt_axes:
return new OnePass_WTA_KT_Axes();
case onepass_wta_ca_axes:
return new OnePass_WTA_CA_Axes();
case onepass_kt_axes:
return new OnePass_KT_Axes();
case onepass_ca_axes:
return new OnePass_CA_Axes();
case onepass_antikt_0p2_axes:
return new OnePass_AntiKT_Axes(0.2);
case onepass_manual_axes:
return new OnePass_Manual_Axes();
case min_axes:
return new MultiPass_Axes(100);
case manual_axes:
return new Manual_Axes();
default:
assert(false);
return NULL;
}
}
-
-
-
+
+
+
} // namespace Nsubjettiness
}
+}
diff --git a/src/Tools/Nsubjettiness/NjettinessPlugin.cc b/src/Tools/fjcontrib/Nsubjettiness/NjettinessPlugin.cc
rename from src/Tools/Nsubjettiness/NjettinessPlugin.cc
rename to src/Tools/fjcontrib/Nsubjettiness/NjettinessPlugin.cc
--- a/src/Tools/Nsubjettiness/NjettinessPlugin.cc
+++ b/src/Tools/fjcontrib/Nsubjettiness/NjettinessPlugin.cc
@@ -1,96 +1,98 @@
// Nsubjettiness Package
// Questions/Comments? jthaler@jthaler.net
//
// Copyright (c) 2011-14
// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
//
// $Id: NjettinessPlugin.cc 821 2015-06-15 18:50:53Z jthaler $
//----------------------------------------------------------------------
// This file is part of FastJet contrib.
//
// It is free software; you can redistribute it and/or modify it under
// the terms of the GNU General Public License as published by the
// Free Software Foundation; either version 2 of the License, or (at
// your option) any later version.
//
// It is distributed in the hope that it will be useful, but WITHOUT
// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
// License for more details.
//
// You should have received a copy of the GNU General Public License
// along with this code. If not, see <http://www.gnu.org/licenses/>.
//----------------------------------------------------------------------
#include "NjettinessPlugin.hh"
-namespace Rivet {
+namespace Rivet {
+namespace fjcontrib {
namespace Nsubjettiness{
LimitedWarning NjettinessPlugin::_old_constructor_warning;
std::string NjettinessPlugin::description() const {return "N-jettiness jet finder";}
// Clusters the particles according to the Njettiness jet algorithm
// Apologies for the complication with this code, but we need to make
// a fake jet clustering tree. The partitioning is done by getPartitionList
void NjettinessPlugin::run_clustering(ClusterSequence& cs) const
{
std::vector<fastjet::PseudoJet> particles = cs.jets();
// HACK: remove area information from particles (in case this is called by
// a ClusterSequenceArea. Will be fixed in a future FastJet release)
for (unsigned i = 0; i < particles.size(); i++) {
particles[i].set_structure_shared_ptr(SharedPtr<PseudoJetStructureBase>());
}
-
-
+
+
TauComponents tau_components = _njettinessFinder.getTauComponents(_N, particles);
TauPartition tau_partition = _njettinessFinder.currentPartition();
std::vector<std::list<int> > partition = tau_partition.jets_list();
-
+
std::vector<int> jet_indices_for_extras;
// output clusterings for each jet
for (size_t i0 = 0; i0 < partition.size(); ++i0) {
size_t i = partition.size() - 1 - i0; // reversed order of reading to match axes order
std::list<int>& indices = partition[i];
if (indices.size() == 0) continue;
while (indices.size() > 1) {
int merge_i = indices.back(); indices.pop_back();
int merge_j = indices.back(); indices.pop_back();
int newIndex;
double fakeDij = -1.0;
-
+
cs.plugin_record_ij_recombination(merge_i, merge_j, fakeDij, newIndex);
indices.push_back(newIndex);
}
double fakeDib = -1.0;
-
+
int finalJet = indices.back();
cs.plugin_record_iB_recombination(finalJet, fakeDib);
jet_indices_for_extras.push_back(cs.jets()[finalJet].cluster_hist_index()); // Get the four vector for the final jets to compare later.
}
//HACK: Re-reverse order of reading to match CS order
reverse(jet_indices_for_extras.begin(),jet_indices_for_extras.end());
- // Store extra information about jets
+ // Store extra information about jets
NjettinessExtras * extras = new NjettinessExtras(tau_components,jet_indices_for_extras);
#if FASTJET_VERSION_NUMBER>=30100
cs.plugin_associate_extras(extras);
#else
// auto_ptr no longer supported, apparently
cs.plugin_associate_extras(std::auto_ptr<ClusterSequence::Extras>(extras));
#endif
-
+
}
} // namespace Nsubjettiness
}
+}
diff --git a/src/Tools/Nsubjettiness/Nsubjettiness.cc b/src/Tools/fjcontrib/Nsubjettiness/Nsubjettiness.cc
rename from src/Tools/Nsubjettiness/Nsubjettiness.cc
rename to src/Tools/fjcontrib/Nsubjettiness/Nsubjettiness.cc
--- a/src/Tools/Nsubjettiness/Nsubjettiness.cc
+++ b/src/Tools/fjcontrib/Nsubjettiness/Nsubjettiness.cc
@@ -1,54 +1,58 @@
// Nsubjettiness Package
// Questions/Comments? jthaler@jthaler.net
//
// Copyright (c) 2011-14
// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
//
// $Id: Nsubjettiness.cc 821 2015-06-15 18:50:53Z jthaler $
//----------------------------------------------------------------------
// This file is part of FastJet contrib.
//
// It is free software; you can redistribute it and/or modify it under
// the terms of the GNU General Public License as published by the
// Free Software Foundation; either version 2 of the License, or (at
// your option) any later version.
//
// It is distributed in the hope that it will be useful, but WITHOUT
// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
// License for more details.
//
// You should have received a copy of the GNU General Public License
// along with this code. If not, see <http://www.gnu.org/licenses/>.
//----------------------------------------------------------------------
#include "Nsubjettiness.hh"
-namespace Rivet {
+namespace Rivet {
+namespace fjcontrib {
-namespace Nsubjettiness { using namespace fastjet;
+namespace Nsubjettiness {
+
+using namespace fastjet;
LimitedWarning Nsubjettiness::_old_constructor_warning;
-
-
+
+
//result returns tau_N with normalization dependent on what is specified in constructor
double Nsubjettiness::result(const PseudoJet& jet) const {
std::vector<fastjet::PseudoJet> particles = jet.constituents();
return _njettinessFinder.getTau(_N, particles);
}
TauComponents Nsubjettiness::component_result(const PseudoJet& jet) const {
std::vector<fastjet::PseudoJet> particles = jet.constituents();
return _njettinessFinder.getTauComponents(_N, particles);
}
//ratio result uses Nsubjettiness result to find the ratio tau_N/tau_M, where N and M are specified by user
double NsubjettinessRatio::result(const PseudoJet& jet) const {
double numerator = _nsub_numerator.result(jet);
double denominator = _nsub_denominator.result(jet);
return numerator/denominator;
}
} // namespace Nsubjettiness
}
+}
diff --git a/src/Tools/Nsubjettiness/README b/src/Tools/fjcontrib/Nsubjettiness/README
rename from src/Tools/Nsubjettiness/README
rename to src/Tools/fjcontrib/Nsubjettiness/README
diff --git a/src/Tools/Nsubjettiness/TauComponents.cc b/src/Tools/fjcontrib/Nsubjettiness/TauComponents.cc
rename from src/Tools/Nsubjettiness/TauComponents.cc
rename to src/Tools/fjcontrib/Nsubjettiness/TauComponents.cc
--- a/src/Tools/Nsubjettiness/TauComponents.cc
+++ b/src/Tools/fjcontrib/Nsubjettiness/TauComponents.cc
@@ -1,89 +1,91 @@
// Nsubjettiness Package
// Questions/Comments? jthaler@jthaler.net
//
// Copyright (c) 2011-14
// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
//
// $Id: NjettinessDefinition.cc 704 2014-07-07 14:30:43Z jthaler $
//----------------------------------------------------------------------
// This file is part of FastJet contrib.
//
// It is free software; you can redistribute it and/or modify it under
// the terms of the GNU General Public License as published by the
// Free Software Foundation; either version 2 of the License, or (at
// your option) any later version.
//
// It is distributed in the hope that it will be useful, but WITHOUT
// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
// License for more details.
//
// You should have received a copy of the GNU General Public License
// along with this code. If not, see <http://www.gnu.org/licenses/>.
//----------------------------------------------------------------------
#include "TauComponents.hh"
#include "MeasureDefinition.hh"
-namespace Rivet {
+namespace Rivet {
+namespace fjcontrib {
namespace Nsubjettiness { using namespace fastjet;
// This constructor takes input vector and double and calculates all necessary tau components
TauComponents::TauComponents(TauMode tau_mode,
const std::vector<double> & jet_pieces_numerator,
double beam_piece_numerator,
double denominator,
const std::vector<PseudoJet> & jets,
const std::vector<PseudoJet> & axes
)
: _tau_mode(tau_mode),
_jet_pieces_numerator(jet_pieces_numerator),
_beam_piece_numerator(beam_piece_numerator),
_denominator(denominator),
_jets(jets),
_axes(axes)
{
-
+
if (!has_denominator()) assert(_denominator == 1.0); //make sure no effect from _denominator if _has_denominator is false
if (!has_beam()) assert (_beam_piece_numerator == 0.0); //make sure no effect from _beam_piece_numerator if _has_beam is false
-
+
// Put the pieces together
_numerator = _beam_piece_numerator;
_jet_pieces.resize(_jet_pieces_numerator.size(),0.0);
for (unsigned j = 0; j < _jet_pieces_numerator.size(); j++) {
_jet_pieces[j] = _jet_pieces_numerator[j]/_denominator;
_numerator += _jet_pieces_numerator[j];
-
+
// Add structural information to jets
StructureType * structure = new StructureType(_jets[j]);
structure->_tau_piece = _jet_pieces[j];
_jets[j].set_structure_shared_ptr(SharedPtr<PseudoJetStructureBase>(structure));
}
-
+
_beam_piece = _beam_piece_numerator/_denominator;
_tau = _numerator/_denominator;
-
+
// Add total_jet with structural information
_total_jet = join(_jets);
StructureType * total_structure = new StructureType(_total_jet);
total_structure->_tau_piece = _tau;
_total_jet.set_structure_shared_ptr(SharedPtr<PseudoJetStructureBase>(total_structure));
}
-
-
-
+
+
+
// test for denominator/beams
bool TauComponents::has_denominator() const {
return (_tau_mode == NORMALIZED_JET_SHAPE
|| _tau_mode == NORMALIZED_EVENT_SHAPE);
}
bool TauComponents::has_beam() const {
return (_tau_mode == UNNORMALIZED_EVENT_SHAPE
|| _tau_mode == NORMALIZED_EVENT_SHAPE);
}
} // namespace Nsubjettiness
}
+}
diff --git a/src/Tools/Nsubjettiness/VERSION b/src/Tools/fjcontrib/Nsubjettiness/VERSION
rename from src/Tools/Nsubjettiness/VERSION
rename to src/Tools/fjcontrib/Nsubjettiness/VERSION
diff --git a/src/Tools/Nsubjettiness/XConePlugin.cc b/src/Tools/fjcontrib/Nsubjettiness/XConePlugin.cc
rename from src/Tools/Nsubjettiness/XConePlugin.cc
rename to src/Tools/fjcontrib/Nsubjettiness/XConePlugin.cc
--- a/src/Tools/Nsubjettiness/XConePlugin.cc
+++ b/src/Tools/fjcontrib/Nsubjettiness/XConePlugin.cc
@@ -1,46 +1,48 @@
// Nsubjettiness Package
// Questions/Comments? jthaler@jthaler.net
//
// Copyright (c) 2011-14
// Jesse Thaler, Ken Van Tilburg, Christopher K. Vermilion, and TJ Wilkason
//
// $Id: XConePlugin.cc 745 2014-08-26 23:51:48Z jthaler $
//----------------------------------------------------------------------
// This file is part of FastJet contrib.
//
// It is free software; you can redistribute it and/or modify it under
// the terms of the GNU General Public License as published by the
// Free Software Foundation; either version 2 of the License, or (at
// your option) any later version.
//
// It is distributed in the hope that it will be useful, but WITHOUT
// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
// License for more details.
//
// You should have received a copy of the GNU General Public License
// along with this code. If not, see <http://www.gnu.org/licenses/>.
//----------------------------------------------------------------------
#include "XConePlugin.hh"
-namespace Rivet {
+namespace Rivet {
+namespace fjcontrib {
namespace Nsubjettiness{
std::string XConePlugin::description() const {
std::stringstream stream;
stream << "XCone Jet Algorithm with N = " << _N << std::fixed << std::setprecision(2) << ", Rcut = " << _R0 << ", beta = " << _beta;
return stream.str();
}
std::string PseudoXConePlugin::description() const {
std::stringstream stream;
stream
<< "PseudoXCone Jet Algorithm with N = " << _N << std::fixed << std::setprecision(2) << ", Rcut = " << _R0 << ", beta = " << _beta;
return stream.str();
}
-
+
} // namespace Nsubjettiness
}
+}
diff --git a/src/Tools/fjcontrib/RecursiveTools/AUTHORS b/src/Tools/fjcontrib/RecursiveTools/AUTHORS
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/AUTHORS
@@ -0,0 +1,31 @@
+The RecursiveTools FastJet contrib is developed and maintained by:
+
+ Gavin P. Salam <gavin.salam@cern.ch>
+ Gregory Soyez <soyez@fastjet.fr>
+ Jesse Thaler <jthaler@jthaler.net>
+ Kevin Zhou <knzhou@mit.edu>
+ Frederic Dreyer <fdreyer@mit.edu>
+
+The physics is based on:
+
+ [ModifiedMassDropTagger]
+ Towards an understanding of jet substructure.
+ Mrinal Dasgupta, Alessandro Fregoso, Simone Marzani, and Gavin P. Salam.
+ JHEP 1309:029 (2013), arXiv:1307.0007.
+
+ [SoftDrop]
+ Soft Drop.
+ Andrew J. Larkoski, Simone Marzani, Gregory Soyez, and Jesse Thaler.
+ JHEP 1405:146 (2014), arXiv:1402.2657
+
+ [IteratedSoftDrop]
+ Casimir Meets Poisson: Improved Quark/Gluon Discrimination with Counting Observables.
+ Christopher Frye, Andrew J. Larkoski, Jesse Thaler, Kevin Zhou.
+ JHEP 1709:083 (2017), arXiv:1704.06266
+
+ [RecursiveSoftDrop]
+ [BottomUpSoftDrop]
+ Recursive Soft Drop.
+ Frederic A. Dreyer, Lina Necib, Gregory Soyez, and Jesse Thaler
+ arXiv:1804.03657
+
\ No newline at end of file
diff --git a/src/Tools/fjcontrib/RecursiveTools/BottomUpSoftDrop.cc b/src/Tools/fjcontrib/RecursiveTools/BottomUpSoftDrop.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/BottomUpSoftDrop.cc
@@ -0,0 +1,329 @@
+// $Id: BottomUpSoftDrop.cc 1064 2017-09-08 09:19:57Z gsoyez $
+//
+// Copyright (c) 2017-, Gavin P. Salam, Gregory Soyez, Jesse Thaler,
+// Kevin Zhou, Frederic Dreyer
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include "BottomUpSoftDrop.hh"
+#include <cassert>
+#include <algorithm>
+#include <sstream>
+#include <typeinfo>
+#include "fastjet/ClusterSequenceActiveAreaExplicitGhosts.hh"
+#include "fastjet/Selector.hh"
+#include "fastjet/config.h"
+
+
+using namespace std;
+
+
+//FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+//namespace contrib{
+
+namespace Rivet{
+ namespace fjcontrib{
+
+
+
+//----------------------------------------------------------------------
+// BottomUpSoftDrop class
+//----------------------------------------------------------------------
+
+// action on a single jet
+PseudoJet BottomUpSoftDrop::result(const PseudoJet &jet) const{
+ // soft drop can only be applied to jets that have constituents
+ if (!jet.has_constituents()){
+ throw Error("BottomUpSoftDrop: trying to apply the Soft Drop transformer to a jet that has no constituents");
+ }
+
+ // if the jet has area support and there are explicit ghosts, we can
+ // transfer that support to the internal re-clustering
+ //
+ // Note that this is just meant to maintain the information since
+ // all the jes will have a 0 area
+ bool do_areas = jet.has_area() && _check_explicit_ghosts(jet);
+
+ // build the soft drop plugin
+ BottomUpSoftDropPlugin * softdrop_plugin;
+
+ // for some constructors, we get the recombiner from the
+ // input jet -- some acrobatics are needed
+ if (_get_recombiner_from_jet) {
+ JetDefinition jet_def = _jet_def;
+
+ // if all the pieces have a shared recombiner, we'll use that
+ // one. Otherwise, use the one from _jet_def as a fallback.
+ JetDefinition jet_def_for_recombiner;
+ if (_check_common_recombiner(jet, jet_def_for_recombiner)){
+#if FASTJET_VERSION_NUMBER >= 30100
+ // Note that this is better than the option directly passing the
+ // recombiner (for cases where th ejet def own its recombiner)
+ // but it's only available in FJ>=3.1
+ jet_def.set_recombiner(jet_def_for_recombiner);
+#else
+ jet_def.set_recombiner(jet_def_for_recombiner.recombiner());
+#endif
+ }
+ softdrop_plugin = new BottomUpSoftDropPlugin(jet_def, _beta, _symmetry_cut, _R0);
+ } else {
+ softdrop_plugin = new BottomUpSoftDropPlugin(_jet_def, _beta, _symmetry_cut, _R0);
+ }
+
+ // now recluster the constituents of the jet with that plugin
+ JetDefinition internal_jet_def(softdrop_plugin);
+ // flag the plugin for automatic deletion _before_ we make
+ // copies (so that as long as the copies are also present
+ // it doesn't get deleted).
+ internal_jet_def.delete_plugin_when_unused();
+
+ ClusterSequence * cs;
+ if (do_areas){
+ vector<PseudoJet> particles, ghosts;
+ SelectorIsPureGhost().sift(jet.constituents(), ghosts, particles);
+ // determine the ghost area from the 1st ghost (if none, any value
+ // will do, as the area will be 0 and subtraction will have
+ // no effect!)
+ double ghost_area = (ghosts.size()) ? ghosts[0].area() : 0.01;
+ cs = new ClusterSequenceActiveAreaExplicitGhosts(particles, internal_jet_def,
+ ghosts, ghost_area);
+ } else {
+ cs = new ClusterSequence(jet.constituents(), internal_jet_def);
+ }
+
+ PseudoJet result_local = SelectorNHardest(1)(cs->inclusive_jets())[0];
+ BottomUpSoftDropStructure * s = new BottomUpSoftDropStructure(result_local);
+ s->_beta = _beta;
+ s->_symmetry_cut = _symmetry_cut;
+ s->_R0 = _R0;
+ result_local.set_structure_shared_ptr(SharedPtr<PseudoJetStructureBase>(s));
+
+ // make sure things remain persistent -- i.e. tell the jet definition
+ // and the cluster sequence that it is their responsibility to clean
+ // up memory once the "result" reaches the end of its life in the user's
+ // code. (The CS deletes itself when the result goes out of scope and
+ // that also triggers deletion of the plugin)
+ cs->delete_self_when_unused();
+
+ return result_local;
+}
+
+// global grooming on a full event
+// note: does not support jet areas
+vector<PseudoJet> BottomUpSoftDrop::global_grooming(const vector<PseudoJet> & event) const {
+ // start by reclustering the event into one very large jet
+ ClusterSequence cs(event, _jet_def);
+ std::vector<PseudoJet> global_jet = SelectorNHardest(1)(cs.inclusive_jets());
+ // if the event is empty, do nothing
+ if (global_jet.size() == 0) return vector<PseudoJet>();
+
+ // apply the groomer to the large jet
+ PseudoJet result = this->result(global_jet[0]);
+ return result.constituents();
+}
+
+// check if the jet has explicit_ghosts (knowing that there is an
+// area support)
+bool BottomUpSoftDrop::_check_explicit_ghosts(const PseudoJet &jet) const {
+ // if the jet comes from a Clustering check explicit ghosts in that
+ // clustering
+ if (jet.has_associated_cluster_sequence())
+ return jet.validated_csab()->has_explicit_ghosts();
+
+ // if the jet has pieces, recurse in the pieces
+ if (jet.has_pieces()){
+ vector<PseudoJet> pieces = jet.pieces();
+ for (unsigned int i=0;i<pieces.size(); i++)
+ if (!_check_explicit_ghosts(pieces[i])) return false;
+ // never returned false, so we're OK.
+ return true;
+ }
+
+ // return false for any other (unknown) structure
+ return false;
+}
+
+// see if there is a common recombiner among the pieces; if there
+// is return true and set jet_def_for_recombiner so that the
+// recombiner can be taken from that JetDefinition. Otherwise,
+// return false. 'assigned' is initially false; when true, each
+// time we meet a new jet definition, we'll check it shares the
+// same recombiner as jet_def_for_recombiner.
+bool BottomUpSoftDrop::_check_common_recombiner(const PseudoJet &jet,
+ JetDefinition &jet_def_for_recombiner,
+ bool assigned) const {
+ if (jet.has_associated_cluster_sequence()){
+ // if the jet def for recombination has already been assigned, check if we have the same
+ if (assigned)
+ return jet.validated_cs()->jet_def().has_same_recombiner(jet_def_for_recombiner);
+
+ // otherwise, assign it.
+ jet_def_for_recombiner = jet.validated_cs()->jet_def();
+ assigned = true;
+ return true;
+ }
+
+ // if the jet has pieces, recurse in the pieces
+ if (jet.has_pieces()){
+ vector<PseudoJet> pieces = jet.pieces();
+ if (pieces.size() == 0) return false;
+ for (unsigned int i=0;i<pieces.size(); i++)
+ if (!_check_common_recombiner(pieces[i], jet_def_for_recombiner, assigned)) return false;
+ // never returned false, so we're OK.
+ return true;
+ }
+ // return false for any other (unknown) structure
+ return false;
+}
+
+
+// description
+string BottomUpSoftDrop::description() const{
+ ostringstream oss;
+ oss << "BottomUpSoftDrop with jet_definition = (" << _jet_def.description() << ")"
+ << ", symmetry_cut = " << _symmetry_cut << ", beta = " << _beta << ", R0 = " << _R0;
+ return oss.str();
+}
+
+//----------------------------------------------------------------------
+// BottomUpSoftDropRecombiner class
+//----------------------------------------------------------------------
+
+// perform a recombination taking into account the Soft Drop
+// conditions
+void BottomUpSoftDropRecombiner::recombine(const PseudoJet &pa,
+ const PseudoJet &pb,
+ PseudoJet &pab) const {
+ PseudoJet p;
+ _recombiner->recombine(pa, pb, p);
+
+ // calculate symmetry parameter
+ double symmetry_cut_fn =_symmetry_cut * pow(pa.squared_distance(pb)/_R0sqr, 0.5*_beta);
+ double pta = pa.pt();
+ double ptb = pb.pt();
+ // make sure denominator is non-zero
+ double sym = pta + ptb;
+ if (sym == 0){
+ pab = p;
+ return;
+ }
+ sym = min(pta, ptb) / sym;
+
+ // if the 2 particles pass the soft drop condition, do the
+ // recombination
+ if (sym > symmetry_cut_fn){
+ pab=p;
+ return;
+ }
+
+ // if the soft drop condition is not passed, return the particle
+ // with largest pt
+ if (pta < ptb) {
+ pab = pb;
+ _rejected.push_back(pa.cluster_hist_index());
+ } else {
+ pab = pa;
+ _rejected.push_back(pb.cluster_hist_index());
+ }
+}
+
+//----------------------------------------------------------------------
+// BottomUpSoftDropPlugin class
+//----------------------------------------------------------------------
+
+// the actual clustering work for the plugin
+void BottomUpSoftDropPlugin::run_clustering(ClusterSequence &input_cs) const {
+ // declare a soft drop recombiner
+ BottomUpSoftDropRecombiner softdrop_recombiner(_beta, _symmetry_cut, _R0, _jet_def.recombiner());
+ JetDefinition jet_def = _jet_def;
+ jet_def.set_recombiner(&softdrop_recombiner);
+
+ // cluster the particles using that recombiner
+ ClusterSequence internal_cs(input_cs.jets(), jet_def);
+ const vector<ClusterSequence::history_element> & internal_hist = internal_cs.history();
+
+ // transfer the list of "childless" elements into a bool vector
+ vector<bool> kept(internal_hist.size(), true);
+ const vector<unsigned int> &sd_rej = softdrop_recombiner.rejected();
+ for (unsigned int i=0;i<sd_rej.size(); i++) kept[sd_rej[i]]=false;
+
+ // browse the history, keeping only the elements that have not been
+ // vetoed.
+ //
+ // In the process we build a map for the history indices
+ vector<unsigned int> internal2input(internal_hist.size());
+ for (unsigned int i=0; i<input_cs.jets().size(); i++)
+ internal2input[i] = i;
+
+ for (unsigned int i=input_cs.jets().size(); i<internal_hist.size(); i++){
+ const ClusterSequence::history_element &he = internal_hist[i];
+
+ // deal with recombinations with the beam
+ if (he.parent2 == ClusterSequence::BeamJet){
+ int internal_jetp_index = internal_hist[he.parent1].jetp_index;
+ int internal_hist_index = internal_cs.jets()[internal_jetp_index].cluster_hist_index();
+
+ int input_jetp_index = input_cs.history()[internal2input[internal_hist_index]].jetp_index;
+
+ // cout << "Beam recomb for internal " << internal_hist_index
+ // << " (input jet index=" << input_jetp_index << endl;
+
+ input_cs.plugin_record_iB_recombination(input_jetp_index, he.dij);
+ continue;
+ }
+
+ // now, deal with two-body recombinations
+ if (!kept[he.parent1]){ // 1 is rejected, we keep only 2
+ internal2input[i]=internal2input[he.parent2];
+ // cout << "rejecting internal " << he.parent1
+ // << ", mapping internal " << i
+ // << " to internal " << he.parent2
+ // << " i.e. " << internal2input[i] << endl;
+ } else if (!kept[he.parent2]){ // 2 is rejected, we keep only 1
+ internal2input[i]=internal2input[he.parent1];
+ // cout << "rejecting internal " << he.parent2
+ // << ", mapping internal " << i
+ // << " to internal " << he.parent1
+ // << " i.e. " << internal2input[i] << endl;
+ } else { // do the recombination
+ int new_index;
+ input_cs.plugin_record_ij_recombination(input_cs.history()[internal2input[he.parent1]].jetp_index,
+ input_cs.history()[internal2input[he.parent2]].jetp_index,
+ he.dij, internal_cs.jets()[he.jetp_index], new_index);
+ internal2input[i]=input_cs.jets()[new_index].cluster_hist_index();
+ // cout << "merging " << internal2input[he.parent1] << " (int: " << he.parent1 << ")"
+ // << " and " << internal2input[he.parent2] << " (int: " << he.parent2 << ")"
+ // << " into " << internal2input[i] << " (int: " << i << ")" << endl;
+ }
+ }
+}
+
+// description of the plugin
+string BottomUpSoftDropPlugin::description() const {
+ ostringstream oss;
+ oss << "BottomUpSoftDropPlugin with jet_definition = (" << _jet_def.description()
+ <<"), symmetry_cut = " << _symmetry_cut << ", beta = "
+ << _beta << ", R0 = " << _R0;
+ return oss.str();
+}
+
+
+ } }
+
+ //FASTJET_END_NAMESPACE
diff --git a/src/Tools/fjcontrib/RecursiveTools/COPYING b/src/Tools/fjcontrib/RecursiveTools/COPYING
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/COPYING
@@ -0,0 +1,360 @@
+The RecursiveTools contrib to FastJet is released
+under the terms of the GNU General Public License v2 (GPLv2).
+
+A copy of the GPLv2 is to be found at the end of this file.
+
+While the GPL license grants you considerable freedom, please bear in
+mind that this code's use falls under guidelines similar to those that
+are standard for Monte Carlo event generators
+(http://www.montecarlonet.org/GUIDELINES). In particular, if you use
+this code as part of work towards a scientific publication, whether
+directly or contained within another program you should include a
+citation to
+
+ arXiv:1307.0007
+ arXiv:1402.2657
+ arXiv:1704.06266
+
+======================================================================
+======================================================================
+======================================================================
+ GNU GENERAL PUBLIC LICENSE
+ Version 2, June 1991
+
+ Copyright (C) 1989, 1991 Free Software Foundation, Inc.
+ 59 Temple Place, Suite 330, Boston, MA 02111-1307 USA
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+
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+
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+possible use to the public, the best way to achieve this is to make it
+free software which everyone can redistribute and change under these terms.
+
+ To do so, attach the following notices to the program. It is safest
+to attach them to the start of each source file to most effectively
+convey the exclusion of warranty; and each file should have at least
+the "copyright" line and a pointer to where the full notice is found.
+
+ <one line to give the program's name and a brief idea of what it does.>
+ Copyright (C) <year> <name of author>
+
+ This program is free software; you can redistribute it and/or modify
+ it under the terms of the GNU General Public License as published by
+ the Free Software Foundation; either version 2 of the License, or
+ (at your option) any later version.
+
+ This program is distributed in the hope that it will be useful,
+ but WITHOUT ANY WARRANTY; without even the implied warranty of
+ MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
+ GNU General Public License for more details.
+
+ You should have received a copy of the GNU General Public License
+ along with this program; if not, write to the Free Software
+ Foundation, Inc., 59 Temple Place, Suite 330, Boston, MA 02111-1307 USA
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+when it starts in an interactive mode:
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+ Gnomovision version 69, Copyright (C) year name of author
+ Gnomovision comes with ABSOLUTELY NO WARRANTY; for details type `show w'.
+ This is free software, and you are welcome to redistribute it
+ under certain conditions; type `show c' for details.
+
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+parts of the General Public License. Of course, the commands you use may
+be called something other than `show w' and `show c'; they could even be
+mouse-clicks or menu items--whatever suits your program.
+
+You should also get your employer (if you work as a programmer) or your
+school, if any, to sign a "copyright disclaimer" for the program, if
+necessary. Here is a sample; alter the names:
+
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+ `Gnomovision' (which makes passes at compilers) written by James Hacker.
+
+ <signature of Ty Coon>, 1 April 1989
+ Ty Coon, President of Vice
+
+This General Public License does not permit incorporating your program into
+proprietary programs. If your program is a subroutine library, you may
+consider it more useful to permit linking proprietary applications with the
+library. If this is what you want to do, use the GNU Library General
+Public License instead of this License.
diff --git a/src/Tools/fjcontrib/RecursiveTools/ChangeLog b/src/Tools/fjcontrib/RecursiveTools/ChangeLog
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/ChangeLog
@@ -0,0 +1,674 @@
+2018-05-29 Jesse Thaler <jthaler@jthaler.net>
+
+ * VERSION
+ * NEWS
+ Changed to 2.0.0-beta2, noted in news
+
+2018-04-21 Jesse Thaler <jthaler@jthaler.net>
+
+ * AUTHORS: updated arxiv number for RecursiveSoftDrop
+
+2018-04-21 Gavin Salam <gavin.salam@cern.ch>
+
+ * README: updated arxiv number for RecursiveSoftDrop & Bottom-up
+ Soft Drop.
+
+2018-04-04 Gregory Soyez <soyez@fastjet.fr>
+
+ * RecursiveSoftDrop.cc (contrib):
+ fixed syntax of calls to structure_of<...>
+ (thanks to Attila Krasznahorkay)
+
+2018-01-24 Gregory Soyez <soyez@fastjet.fr>
+
+ * RecursiveSoftDrop.cc:
+ for the (dafault) dynamical R0 implementation, the dynamical R0 is
+ evolved independently in each branch.
+
+2017-10-10 Jesse Thaler <jthaler@jthaler.net>
+ * AUTHORS
+ Added mention of BUSD
+
+ * README
+ Some tweaks to the wording
+
+2017-10-11 Gregory Soyez <soyez@fastjet.fr>
+
+ * IteratedSoftDrop.hh:
+ IteratedSoftDropInfo::size() and multiplicity() now return an
+ unsigned int instead of a double
+
+2017-10-10 Jesse Thaler <jthaler@jthaler.net>
+ * AUTHORS
+ Updated journal reference for ISD
+
+ * example_isd.{cc,ref}:
+ Included soft drop multiplicity in example
+
+ * README
+ Added warning at top that documentation has not been updated
+
+ * VERSION
+ Changed to 2.0.0-beta1
+
+2017-10-10 Gregory Soyez <soyez@fastjet.fr>
+
+ * example_isd.ref:
+ updated to reflect the bugfix below
+
+ * IteratedSoftDrop.cc:
+ fixed issue in description (was taking sqrt of -ve number when
+ there were no angular cut)
+
+ * NEWS:
+ drafted for RecursiveTools-2.0.0-beta1
+
+ * TODO:
+ updated list in view of a beta release
+
+ * example_isd.cc:
+ pointed to the right header for IteratedSoftDrop
+
+ * RecursiveSoftDrop.{hh,cc}:
+ * IteratedSoftDrop.{hh,cc}:
+ moved IteratedSoftDrop to its own file (replacing the old
+ implementation)
+
+ * example_advanced_usage.ref:
+ updated reference file following the fix below.
+
+2017-09-28 Gregory Soyez <soyez@fastjet.fr>
+
+ * RecursiveSymmetryCutBase.cc:
+ when no substructure is found, keep the _symmetry, _delta_R and
+ _mu structure variables at -1. This for example allows one to
+ trigger on substructure by checking if delta_R>=0.
+
+ Note: we could set it to 0 (as it was before) and trigger using
+ _delta_R>0 but there might be some genuine substructure exactly
+ collinear.
+
+2017-09-19 Gregory Soyez <soyez@fastjet.fr>
+
+ * example_isd.ref:
+ updated to the latest version of the example
+
+2017-09-18 Gregory Soyez <soyez@fastjet.fr>
+
+ * Makefile:
+ updating make check to use all the examples (failing on ISD as
+ expected, see below)
+
+ * example_bottomup_softdrop.cc:
+ fixed typo
+
+ * example_bottomup_softdrop.ref:
+ * example_recursive_softdrop.ref:
+ added reference output for this example
+
+ * RecursiveSoftDrop.{hh,cc}:
+ * RecursiveSymmetryCutBase.{cc,hh}:
+ moved the "all_prongs" method from the base structure t oa
+ standalone function in RecursiveSoftDrop.hh
+
+ In practice, this is irrelevant for mMDT and SD (since pieces()
+ gets the job done, and the substructure class does not have (as
+ is) reliable info to get the full structure)
+
+ * RecursiveSymmetryCutBase.cc:
+ revamped a series of requests for substructure info to better
+ handle possible recursion into deeper jet substructure.
+
+ * RecursiveSoftDrop.{hh,cc}:
+ updated "description" to reuse the info from the base class
+
+ * example_isd.cc:
+ updated to use the newer implementation of ISD. Checked that it
+ gives the same results as the former implementation.
+
+ Note: make check still needs fixing because the example now
+ computes a different set of angularities
+
+ * RecursiveSoftDrop.hh:
+ added a few helpers to IteratedSoftDropInfo ([] operator and size,
+ meaning it can be used as a vector<pair<double,double> >)
+
+ * RecursiveSymmetryCutBase.cc:
+ . fixed bugs in the calculation of the geometric distances for ee
+ coordinates
+ . fixed bug in the computation of the (zg,thetag) pairs [it was
+ returning the groomed ones instead of the ones passing the
+ condition]
+
+ * example_recursive_softdrop.cc:
+ set the R0 parameter to the original jet radius
+
+2017-09-13 Gregory Soyez <soyez@fastjet.fr>
+
+ * example_recursive_softdrop.cc:
+ tied up a few comments and the code output
+
+ * RecursiveSymmetryCutBase.{hh,cc}:
+ removed the unneeded _is_composite
+
+ * RecursiveSoftDrop.cc:
+ fixed issue with "verbose" dropped info on branches with no
+ further substructure
+
+2017-09-11 Gregory Soyez <soyez@fastjet.fr>
+
+ * RecursiveSoftDrop.{hh,cc}:
+ have IteratedSoftDDrop returning by default an object of type
+ IteratedSoftDropInfo; added several helpers
+
+2017-09-08 Gregory Soyez <soyez@fastjet.fr>
+
+ * RecursiveSoftDrop.{hh,cc}:
+ updated IteratedSoftDrop to give it the flexibility of
+ RecursiveSoftDrop
+
+ * RecursiveSymmetryCutBase.hh:
+ fixed typo in comment
+
+ * example_mmdt_ee.cc: *** ADDED ***
+ added an example to illustrat usage in ee collisions
+
+ * example_isd.cc:
+ * BottomUpSoftDrop.cc:
+ * IteratedSoftDrop.cc:
+ * RecursiveSoftDrop.cc:
+ Fixed compilation issues with FJ 3.0 (mostly the usage of features
+ introduced only in FJ3.1)
+
+ * RecursiveSymmetryCutBase.{hh,cc}:
+ used the internal Recluster class for FJ<3.1.0 and the FJ antive
+ one for FJ>=3.1.0
+
+ * BottomUpSoftDrop.{hh,cc}:
+ moved the implementation of global_grooming to the source file and
+ fixed a few trivial compilation errors
+
+2017-09-08 Frédéric Dreyer <frederic.dreyer@gmail.com>
+
+ * BottomUpSoftDrop.hh:
+ added the global_grooming method to process full event
+
+2017-09-07 Gregory Soyez <soyez@fastjet.fr>
+
+ * RecursiveSoftDrop.cc:
+ cleaned (mostly by removing older commented-out code)
+
+ * RecursiveSoftDrop.{hh,cc}:
+ * RecursiveSymmetryCutBase.{hh,cc}:
+ * SoftDrop.cc:
+
+ added support for ee coordinates. For that, the symmetry measure
+ has to be set to either theta_E (which uses the 3-vector angle
+ theta) or to cos_theta_E which uses sqrt(2*[1-cos(theta)])
+
+ Accordingly, the recursion_choice can be set to larger_E to
+ recurse into the branch with the largest energy. The larger_m
+ mode, recorsing into the larger-mass branch is also possible but
+ not advised (for the same reason as the pp version).
+
+ * RecursiveSymmetryCutBase.{hh,cc}:
+ switched to the Recluster class provided with FastJet. ASlso
+ included the recluster description to RecursiveSymmetryCutBase
+ when it is user-defined.
+
+2017-09-06 Gregory Soyez <soyez@fastjet.fr>
+
+ * BottomUpSoftDrop.{hh,cc}:
+ . renamed SoftDropStructure -> BottomUpSoftDropStructure
+ SoftDropRecombiner -> BottomUpSoftDropRecombiner
+ SoftDropPlugin -> BottomUpSoftDropPlugin
+ . moved 'description' to source file (instead of header)
+ . kept the "area" information when available (jets will just
+ appear as having a 0 area)
+ . added most class description (main class still missing)
+
+ * RecursiveSoftDrop.cc:
+ . put internal classes to handle CS history in an internal namespace
+ . replaced the "switch" in the mail loop by a series of if (allows
+ us a few simplificatins/cleaning)
+ . more uniform treatment of issues in the presence of an angular cut
+ (as part of the above reorganisation)
+
+ * example_advanced_usage.ref:
+ updated reference output file following the bugfix (missing
+ "grooming mode" initialisation in one of the SoftDrop ctors) on
+ 2017-08-01
+
+ * RecursiveSymmetryCutBase.cc:
+ removed redundent code
+
+2017-08-10 Gregory Soyez <soyez@fastjet.fr>
+
+ * RecursiveSoftDrop.cc:
+ fixed trivial typo in variable name
+
+>>>>>>> .r1071
+2017-08-04 Gregory Soyez <soyez@fastjet.fr>
+
+ * RecursiveSoftDrop.cc:
+ do not impose an angular cut in IterativeSD if it is -ve.
+
+2017-08-01 Gregory Soyez <soyez@fastjet.fr>
+
+ * example_recursive_softdrop.cc:
+ added a series of optional flags
+
+ * RecursiveSoftDrop.cc:
+ fixed a few issues with the fixed depth version
+
+ * RecursiveSymmetryCutBase.hh:
+ a jet is now considered as havig substructure if deltaR>0
+ (coherent with released version)
+
+ * SoftDrop.hh:
+ bugfix: set the "grooming mode" by default in all ctors
+ EDIT: caused issue with make check, fixed on 2017-09-069 (see
+ above)
+
+ * RecursiveSoftDrop.{hh,cc}:
+ added support for the "same depth" variant
+
+ * RecursiveSymmetryCutBase.cc:
+ also associate a RecursiveSymmetryCutBase::StructureType structure
+ to the result jet in case it is just a single particle (in
+ grooming mode)
+
+2017-07-31 Gregory Soyez <soyez@fastjet.fr>
+
+ * RecursiveSymmetryCutBase.{hh,cc}:
+ added the option to pass an extra parameter to the symmetry cut
+ function
+
+ * RecursiveSymmetryCutBase.{hh,cc}:
+ * ModifiedMassDropTagger.hh
+ * SoftDrop.hh:
+ minor adaptions due to the above change + added a few methods to
+ query the class information (symmetry cut, beta, ...)
+
+ * RecursiveSoftDrop.{hh,cc}:
+ Added support for
+ - a dynamical R0
+ - recursing only in the hardest branch
+ - imposing a min deltaR cut
+
+ Added a tentative IterativeSoftDrop class
+
+2017-07-28 Gregory Soyez <soyez@fastjet.fr>
+
+ * RecursiveSoftDrop.cc:
+ adapted to the latest changes in RecursiveSymmetryCutBase
+
+ * RecursiveSymmetryCutBase.{hh,cc}:
+ reorganised the output of the recursion step (recurse_one_step)
+ using an enum to make iot more readable (and to fix issues where
+ the dropped prong is actually 0, e.g. after subtraction)
+
+2017-07-26 Gregory Soyez <soyez@fastjet.fr>
+
+ * example_recursive_softdrop.cc: *** ADDED ***
+ added a draft example for the use of RecursiveSoftDrop
+
+ * RecursiveSoftDrop.{hh,cc}: *** ADDED ***
+ added a first pass at an implementation of RecursiveSoftDrop.
+
+ This is based on Frederic's initial version but keeps the
+ branching structure of the jet. Some of the features, like
+ dynamical R0, direct access to the substructure or the same depth
+ variant, are still unsupported.
+
+ * SoftDrop.hh:
+ declared _beta, _symmetry_cut and _R0sqr as protected (was
+ private) so they ca n be used by RecursiveSoftDrop
+
+ * RecursiveSymmetryCutBase.{hh,cc}:
+ extracted from result() the part that performs one step of the
+ resursion (implemented as recurse_one_step()). This is repeatedly
+ called by result(). It has specific conventions to indicate
+ whether or not some substructure has been found or if one ran into
+ some issue.
+
+2017-04-25 Kevin Zhou <knzhou@mit.edu>
+
+ * IteratedSoftDrop.hh
+ . Added Doxygen documentation
+
+ * RecursiveSymmetryCutBase.hh
+ . Added references to ISD
+
+2017-04-25 Jesse Thaler <jthaler@jthaler.net>
+ * AUTHORS, COPYING:
+ . Added ISD arXiv number
+
+ * example_isd.{cc,ref}
+ . Added ISD arXiv number
+ . Changing z_cut to be optimal value (with Lambda = 1 GeV)
+ . Tweaked formatting
+
+ * IteratedSoftDrop.{hh,cc}
+ . Added ISD arXiv number
+ . Assert added if recluster does not return one jet.
+
+ * README
+ . Added ISD arXiv number and tweaked wording
+
+
+2017-04-20 Kevin Zhou <knzhou@mit.edu>
+
+ * example_isd.{cc,ref} ** ADDED **
+ * IteratedSoftDrop.{cc,hh} ** ADDED **
+
+ * Makefile
+ . Added IteratedSoftDrop (ISD) as appropriate
+
+ * AUTHORS
+ . Added myself to author list
+ . Added placeholder for ISD paper
+
+ * COPYING
+ . Added placeholder for ISD paper
+
+ * README
+ . Added description of ISD
+
+ * TODO
+ . Added tasks to integrate ISD with other classes, e.g. SD,
+ Recluster, and the future RecursiveSoftDrop (RSD)
+
+ * NEWS
+ . Added dummy for release of 1.1.0
+
+ * VERSION:
+ . Switched version number to 1.1.0-dev
+
+ * example_advanced_usage.cc:
+ . Added $Id$ tag, didn't change anything else
+
+2014-07-30 Gregory Soyez <soyez@fastjet.fr>
+
+ * Recluster.hh: fixed the name of the #define for the header
+
+2014-07-09 Gregory Soyez <soyez@fastjet.fr> + Jesse
+
+ * NEWS:
+ release of RecursiveTools v1.0.0
+
+ * VERSION:
+ switched version number to 1.0.0
+
+2014-07-08 Gavin Salam <gavin.salam@cern.ch>
+
+ * README (RecursionChoice):
+ added ref to .hh for constness specs of virtual functions (to
+ reduce risk of failed overloading due to wrong constness).
+
+2014-07-08 Gregory Soyez <soyez@fastjet.fr> + Jesse
+
+ * README:
+ partially rewrote the description of set_subtractor
+
+2014-07-07 Gregory Soyez <soyez@fastjet.fr> + Jesse
+
+ * example_advanced_usage.cc:
+ * example_softdrop.cc:
+ a few small fixed in the header of the files
+
+ * VERSION:
+ switched over to 1.0.0-alpha2-devel
+
+ * README:
+ Reordered a few things and added a few details.
+
+ * Makefile (check):
+ Be quiter during "make check"
+
+ * Recluster.cc (contrib):
+ Documented the "single" ctor argument
+
+ * RecursiveSymmetryCutBase.cc (contrib):
+ If the user sets himself the reclustering, disable the "non-CA"
+ warning (we assume that he knows what he is doing). Mentioned in
+ the comments that non-CA reclustering has to be used at the user's
+ risk. Also throw when th input jet has no constituents or when
+ there is no cluster sequence after reclustering.
+
+ * Recluster.cc (contrib):
+ replaced a remaining mention to "filtering" by reclustering
+
+2014-07-04 Jesse Thaler <jthaler@jthaler.net>
+ * VERSION
+ . Ready for alpha release
+
+2014-06-17 Jesse Thaler <jthaler@jthaler.net>
+ * example_advanced_usage.{cc,ref} ** ADDED **
+ * Makefile
+ . New example file to test a bunch of soft drop options
+ . Put in makefile as well
+ . Fixed nasty memory bug with pointers to Recluster
+
+ * RecursiveSymmetryCutBase.cc
+ * example_softdrop.ref
+ . description() now says Groomer vs. Tagger
+
+ * RecursiveSymmetryCutBase.{cc,hh}
+ . Added optional verbose logging information about
+ kinematics of dropped branches
+
+ * example_softdrop.cc
+ * example_advanced_usage.cc
+ . Fixed
+
+
+2014-06-16 Gregory Soyez <soyez@fastjet.fr>
+
+ * Makefile:
+ also install the RecursiveSymmetryuCutBase.hh header
+
+2014-06-13 Jesse Thaler <jthaler@jthaler.net>
+ * AUTHORS
+ . Added myself to author list
+ . Put complete bibliographic details on papers
+
+ * COPYING
+ . Added boilerplate MC/GPLv2 statement
+
+ * example.cc: ** REMOVED ** renamed to...
+ * example_mmdt.cc ** ADDED **
+ * Makefile
+ . Made name change for consistency
+ . Made corresponding changes in Makefile
+
+ * example_mmdt_sub.cc:
+ * example_mmdt.cc:
+ * example_recluster.cc:
+ . light editing of comments
+
+ * example_softdrop.cc:
+ . light editing of comments
+ . added assert for sdjet != 0, since SoftDrop is a groomer
+
+ * ModifiedMassDropTagger.hh
+ * Recluster.{cc,hh}
+ * RecursiveSymmetryCutBase.{cc,hh}
+ * SoftDrop.hh
+ . Updated some comments
+
+ * README
+ . Updated to include basic usage description and some
+ technical details
+
+ * TODO:
+ . Added some discussion points.
+
+2014-06-13 Gregory Soyez <soyez@fastjet.fr>
+
+ * example_softdrop.{cc,ref}:
+ added an example for SoftDrop
+
+ * SoftDrop.{hh,cc}:
+ * ModifiedMassDropTagger.{hh,cc}:
+ * RecursiveSymmetryCutBase.{hh,cc}: *** ADDED ***
+ . added a base class for both the mMDT and SoftDrop
+ . made mMDT and SoftDrop inherit from RecursiveSymmetryCutBase
+ . moved the reclustering to the base class. By default, both
+ mMDT and SoftDrop now recluster the jet with C/A
+ . added set_grooming_mode and set_tagging_mode methods to the
+ base class
+
+ * Merging the development branch 1.0-beta1-softdrop-addition back
+ into the trunk (will correspond to revision 682)
+
+ * VERSION:
+ switched back to 1.0.0-devel
+
+ * SoftDrop.{hh,cc}:
+ added support for re-clustering through set_reclustering(bool,
+ Recluster*). By default, reclustering is done with
+ Cambridge/Aachen.
+
+ * example_recluster.{cc,ref}: *** ADDED ***
+ added an example of reclustering
+
+ * Recluster.{hh,cc}:
+ added a 'single' ctor argument [true by default]. When true, the
+ hardest jet after reclustering is returned, otherwise, the result
+ is a composite jet with all the subjets as its pieces.
+
+2014-05-15 Gregory Soyez <soyez@fastjet.fr>
+
+ * VERSION:
+ set version number to 1.0-alpha-PUWS14.1 in preparation for a
+ fastjet-contrib release for the pileup-workshop at CERN on May
+ 2014.
+
+2014-04-25 Gregory Soyez <soyez@fastjet.fr>
+
+ * ModifiedMassDropTagger.hh:
+ * ModifiedMassDropTagger.cc:
+ Added comments at various places
+
+ * AUTHORS:
+ * README:
+ Updated info about what is now included in this contrib
+
+ * SoftDrop.hh: *** ADDED ***
+ * SoftDrop.cc: *** ADDED ***
+ * Recluster.hh: *** ADDED ***
+ * Recluster.cc; *** ADDED ***
+ Added tools for reclustering and softDrop
+
+2014-04-25 Gregory Soyez <soyez@fastjet.fr>
+
+ branch started at revision 611 to start including SoftDrop in the
+ Recursivetols contrib
+
+2014-04-24 Gregory Soyez <soyez@fastjet.fr>
+
+ * ModifiedMassDropTagger.hh:
+ added a mention of the fact that when result is called in the
+ presence of a subtractor, then the output is a subtracted
+ PseudoJet.
+
+ * ModifiedMassDropTagger.hh:
+ declared _symmetry_cut as protected (rather than provate) so it
+ can be accessed if symmetry_cut_description() is overloaded.
+
+ * example.cc:
+ trivial typo fixed in a comment
+
+2014-02-04 Gavin Salam <gavin.salam@cern.ch>
+
+ * VERSION:
+ upped it to 1.0-beta1
+
+ * example_mmdt_sub.cc (main):
+ added an #if to make sure FJ3.1 features are only used if FJ3.1
+ is available. (Currently FJ3.1 is only available to FJ developers).
+
+2014-01-26 Gavin Salam <gavin.salam@cern.ch>
+
+ * VERSION:
+ renamed to 1.0-beta0
+
+ * ModifiedMassDropTagger.hh:
+ * README:
+ added info on author names
+
+ * example_mmdt_sub.ref: *** ADDED ***
+ added reference output for the pileup test.
+
+2014-01-25 Gavin Salam <gavin.salam@cern.ch>
+
+ * example_mmdt_sub.cc:
+ * Makefile:
+ added an extra example illustrating functionality with pileup
+ subtraction.
+
+2014-01-24 Gavin Salam <gavin.salam@cern.ch>
+
+ * ModifiedMassDropTagger.cc:
+
+ Reorganised code so that (sub)jet.m2()>0 check is only used when
+ absolutely necessary: so if using a scalar_z symmetry measure,
+ whenever scalar_z < zcut, then there is no point checking the mu
+ condition. This means that there's no issue if the (sub)jet mass
+ is negative, and one simply recurses down into the jet. (Whereas
+ before it would bail out, reducing the tagging efficiency).
+
+ Also removed the verbose code.
+
+2014-01-23 Gavin Salam <gavin.salam@cern.ch>
+
+ * ModifiedMassDropTagger.cc|hh:
+ * example.cc
+ replaced "asymmetry" with "symmetry" in a number of places;
+ implemented the structural information and added it to the example;
+ added a new simplified constructor;
+ improved doxygen documentation;
+ started renaming -> RecursiveTools
+
+ * README
+ some tidying
+
+ * VERSION
+ 1.0-b0
+
+2014-01-22 Gavin Salam <gavin.salam@cern.ch>
+
+ * ModifiedMassDropTagger.cc (contrib):
+ -ve mass now bails out also when using the "y" asymmetry measure.
+ Also, default my is now infinite.
+
+2014-01-20 Gavin Salam <gavin.salam@cern.ch> + Gregory
+
+
+ * ModifiedMassDropTagger.cc|hh:
+ introduced a virtual asymmetry_cut_fn (essentially a
+ dummy function returning a constant), to allow for derived classes
+ to do fancier things.
+
+ added warning about non-C/A clustering.
+ explicitly labelled some (inherited) virtual functions as
+ virtual.
+
+2014-01-20 Gavin Salam <gavin.salam@cern.ch>
+
+ * example.ref:
+ * example.cc (main):
+ got a first working example and make check setup.
+
+ * ModifiedMassDropTagger.cc|hh:
+ improved doxygen comments;
+ added option whereby input jet is assumed already subtracted
+
+2014-01-19 Gavin Salam <gavin.salam@cern.ch>
+
+ * ModifiedMassDropTagger.cc|hh:
+ * many other files
+
+ Initial creation, with basic code for MMDT
+
diff --git a/src/Tools/fjcontrib/RecursiveTools/IteratedSoftDrop.cc b/src/Tools/fjcontrib/RecursiveTools/IteratedSoftDrop.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/IteratedSoftDrop.cc
@@ -0,0 +1,132 @@
+// $Id: IteratedSoftDrop.cc 1084 2017-10-10 20:36:50Z gsoyez $
+//
+// Copyright (c) 2017-, Jesse Thaler, Kevin Zhou, Gavin P. Salam
+// andGregory Soyez
+//
+// based on arXiv:1704.06266 by Christopher Frye, Andrew J. Larkoski,
+// Jesse Thaler, Kevin Zhou
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include "IteratedSoftDrop.hh"
+#include <sstream>
+#include <cmath>
+#include <fastjet/ClusterSequence.hh>
+
+using namespace std;
+
+//FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+ //namespace contrib{
+
+ namespace Rivet{
+ namespace fjcontrib{
+
+
+//========================================================================
+// implementation of IteratedSoftDropInfo
+//========================================================================
+
+// returns the angularity with angular exponent alpha and z
+// exponent kappa calculated on the zg's and thetag's found by
+// iterated SoftDrop
+//
+// returns 0 if no substructure was found
+double IteratedSoftDropInfo::angularity(double alpha, double kappa) const{
+ double sum = 0.0;
+ for (unsigned int i=0; i< _all_zg_thetag.size(); ++i)
+ sum += pow(_all_zg_thetag[i].first, kappa) * pow(_all_zg_thetag[i].second, alpha);
+ return sum;
+}
+
+//========================================================================
+// implementation of IteratedSoftDrop
+//========================================================================
+
+// Constructor. Takes in the standard Soft Drop parameters, an angular cut \f$\theta_{\rm cut}\f$,
+// and a choice of angular and symmetry measure.
+//
+// - beta the Soft Drop beta parameter
+// - symmetry_cut the Soft Drop symmetry cut
+// - angular_cut the angular cutoff to halt Iterated Soft Drop
+// - R0 the angular distance normalization
+IteratedSoftDrop::IteratedSoftDrop(double beta, double symmetry_cut, double angular_cut, double R0,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor) :
+ _rsd(beta, symmetry_cut, -1, R0, subtractor){
+ _rsd.set_hardest_branch_only(true);
+ if (angular_cut>0)
+ _rsd.set_min_deltaR_squared(angular_cut*angular_cut);
+}
+
+
+// Full constructor, which takes the following parameters:
+//
+// \param beta the value of the beta parameter
+// \param symmetry_cut the value of the cut on the symmetry measure
+// \param symmetry_measure the choice of measure to use to estimate the symmetry
+// \param angular_cut the angular cutoff to halt Iterated Soft Drop
+// \param R0 the angular distance normalisation [1 by default]
+// \param mu_cut the maximal allowed value of mass drop variable mu = m_heavy/m_parent
+// \param recursion_choice the strategy used to decide which subjet to recurse into
+// \param subtractor an optional pointer to a pileup subtractor (ignored if zero)
+IteratedSoftDrop::IteratedSoftDrop(double beta,
+ double symmetry_cut,
+ RecursiveSoftDrop::SymmetryMeasure symmetry_measure,
+ double angular_cut,
+ double R0,
+ double mu_cut,
+ RecursiveSoftDrop::RecursionChoice recursion_choice,
+ const FunctionOfPseudoJet<PseudoJet> * subtractor)
+ : _rsd(beta, symmetry_cut, symmetry_measure, -1, R0, mu_cut, recursion_choice, subtractor){
+ _rsd.set_hardest_branch_only(true);
+ if (angular_cut>0)
+ _rsd.set_min_deltaR_squared(angular_cut*angular_cut);
+}
+
+
+// returns vector of ISD symmetry factors and splitting angles
+IteratedSoftDropInfo IteratedSoftDrop::result(const PseudoJet& jet) const{
+ PseudoJet rsd_jet = _rsd(jet);
+ if (! rsd_jet.has_structure_of<RecursiveSoftDrop>())
+ return IteratedSoftDropInfo();
+ return IteratedSoftDropInfo(rsd_jet.structure_of<RecursiveSoftDrop>().sorted_zg_and_thetag());
+}
+
+
+std::string IteratedSoftDrop::description() const{
+ std::ostringstream oss;
+ oss << "IteratedSoftDrop with beta =" << _rsd.beta()
+ << ", symmetry_cut=" << _rsd.symmetry_cut()
+ << ", R0=" << _rsd.R0();
+
+ if (_rsd.min_deltaR_squared() >= 0){
+ oss << " and angular_cut=" << sqrt(_rsd.min_deltaR_squared());
+ } else {
+ oss << " and no angular_cut";
+ }
+
+ if (_rsd.subtractor()){
+ oss << ", and with internal subtraction using [" << _rsd.subtractor()->description() << "]";
+ }
+ return oss.str();
+}
+
+
+ } } // namespace contrib
+
+ //FASTJET_END_NAMESPACE
diff --git a/src/Tools/fjcontrib/RecursiveTools/Makefile.am b/src/Tools/fjcontrib/RecursiveTools/Makefile.am
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/Makefile.am
@@ -0,0 +1,12 @@
+noinst_LTLIBRARIES = libRivetRecursiveTools.la
+
+libRivetRecursiveTools_la_SOURCES = \
+ BottomUpSoftDrop.cc \
+ IteratedSoftDrop.cc \
+ ModifiedMassDropTagger.cc \
+ Recluster.cc \
+ RecursiveSoftDrop.cc \
+ RecursiveSymmetryCutBase.cc \
+ SoftDrop.cc
+
+libRivetRecursiveTools_la_CPPFLAGS = -I${top_srcdir}/include/Rivet/Tools/fjcontrib $(AM_CPPFLAGS)
diff --git a/src/Tools/fjcontrib/RecursiveTools/ModifiedMassDropTagger.cc b/src/Tools/fjcontrib/RecursiveTools/ModifiedMassDropTagger.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/ModifiedMassDropTagger.cc
@@ -0,0 +1,48 @@
+// $Id: ModifiedMassDropTagger.cc 683 2014-06-13 14:38:38Z gsoyez $
+//
+// Copyright (c) 2014-, Gavin P. Salam
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include "ModifiedMassDropTagger.hh"
+#include "fastjet/JetDefinition.hh"
+#include "fastjet/ClusterSequenceAreaBase.hh"
+#include <algorithm>
+#include <cstdlib>
+
+using namespace std;
+
+//FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+ //namespace contrib{
+
+ namespace Rivet{
+ namespace fjcontrib{
+
+
+//----------------------------------------------------------------------
+string ModifiedMassDropTagger::symmetry_cut_description() const {
+ ostringstream ostr;
+ ostr << _symmetry_cut << " [ModifiedMassDropTagger]";
+ return ostr.str();
+}
+
+
+ } } // namespace contrib
+
+ //FASTJET_END_NAMESPACE
diff --git a/src/Tools/fjcontrib/RecursiveTools/NEWS b/src/Tools/fjcontrib/RecursiveTools/NEWS
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/NEWS
@@ -0,0 +1,11 @@
+2018/05/31: release of version 2.0.0-beta2 with corrected syntax
+
+2017/10/10: release of version 2.0.0-beta1 including implementations of
+
+* RecursiveSoftDrop (see example_rsd.hh for usage)
+* IteratedSoftDrop (see example_isd.hh for usage)
+* e+e- version of the recursive tools (see example_mmdt_ee.hh for usage)
+* BottomUpSoftDrop (see example_bottomup_softdrop.cc for usage)
+
+2014/07/09: release of version 1.0.0 of RecursiveTools including
+ ModifiedMassDropTagger and SoftDrop (as well as Recluster)
diff --git a/src/Tools/fjcontrib/RecursiveTools/README b/src/Tools/fjcontrib/RecursiveTools/README
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/README
@@ -0,0 +1,346 @@
+------------------------------------------------------------------------
+RecursiveTools FastJet contrib
+------------------------------------------------------------------------
+
+The RecursiveTools FastJet contrib aims to provide a common contrib
+for a number of tools that involve recursive reclustering/declustering
+of a jet for tagging or grooming purposes.
+
+Currently it contains:
+
+- ModifiedMassDropTagger
+ This corresponds to arXiv:1307.0007 by Mrinal Dasgupta, Alessandro
+ Fregoso, Simone Marzani and Gavin P. Salam
+
+- SoftDrop
+ This corresponds to arXiv:1402.2657 by Andrew J. Larkoski, Simone
+ Marzani, Gregory Soyez, Jesse Thaler
+
+- RecursiveSoftDrop
+- BottomUpSoftDrop
+ This corresponds to arXiv:1804.03657 by Frederic Dreyer, Lina
+ Necib, Gregory Soyez and Jesse Thaler
+
+- IteratedSoftDrop
+ This corresponds to arXiv:1704.06266 by Christopher Frye, Andrew J.
+ Larkoski, Jesse Thaler, Kevin Zhou
+
+- Recluster
+ A generic tool to recluster a given jet into subjets
+ Note: a Recluster class is available natively in FastJet since v3.1.
+ Users are therefore encouraged to use the FastJet version
+ rather than this one which is mostly provided for
+ compatibility of this contrib with older versions of FastJet.
+
+The interface for these tools is described in more detail below, with
+all of the available options documented in the header files.
+
+One note about nomenclature. A groomer is a procedure that takes a
+PseudoJet and always returns another (non-zero) PseudoJet. A tagger is
+a procedure that takes a PseudoJet, and either returns another PseudoJet
+(i.e. tags it) or returns an empty PseudoJet (i.e. doesn't tag it).
+
+------------------------------------------------------------------------
+ModifiedMassDropTagger
+------------------------------------------------------------------------
+
+The Modified Mass Drop Tagger (mMDT) recursively declusters a jet,
+following the largest pT subjet until a pair of subjets is found that
+satisfy the symmetry condition on the energy sharing
+
+ z > z_cut
+
+where z_cut is a predetermined value. By default, z is calculated as
+the scalar pT fraction of the softest subjet. Note that larger values
+of z_cut correspond to a more restrictive tagging criteria.
+
+By default, mMDT will first recluster the jet using the CA clustering
+algorithm, which means that mMDT can be called on any jet, regardless
+of the original jet finding measure.
+
+A default mMDT can be created via
+
+ double z_cut = 0.10;
+ ModifiedMassDropTagger mMDT(z_cut);
+
+More options are available in the full constructor. To apply mMDT,
+one simply calls it on the jet of interest.
+
+ PseudoJet tagged_jet = mMDT(original_jet);
+
+Note that mMDT is a tagger, such that tagged_jet will only be non-zero
+if the symmetry cut z > z_cut is satisfied by some branching of the
+clustering tree.
+
+To gain additional information about the mMDT procedure, one can use
+
+ tagged_jet.structure_of<ModifiedMassDropTagger>()
+
+which gives access to information about the delta_R between the tagged
+subjets, their z value, etc.
+
+------------------------------------------------------------------------
+SoftDrop
+------------------------------------------------------------------------
+
+The SoftDrop procedure is very similar to mMDT, albeit with a
+generalised symmetry condition:
+
+ z > z_cut * (R / R0)^beta
+
+Note that larger z_cut and smaller beta correspond to more aggressive
+grooming of the jet.
+
+SoftDrop is intended to be used as a groomer (instead of as a tagger),
+such that if the symmetry condition fails throughout the whole
+clustering tree, SoftDrop will still return a single particle in the
+end. Apart from the tagger/groomer distinction, SoftDrop with beta=0 is
+the same as mMDT.
+
+A default SoftDrop groomer can be created via:
+
+ double z_cut = 0.10;
+ double beta = 2.0;
+ double R0 = 1.0; // this is the default value
+ SoftDrop sd(z_cut,beta,R0);
+
+and acts on a desired jet as
+
+ PseudoJet groomed_jet = sd(original_jet);
+
+and additional information can be obtained via
+
+ groomed_jet.structure_of<SoftDrop>()
+
+SoftDrop is typically called with beta > 0, though beta < 0 is still a
+viable option. Because beta < 0 is infrared-collinear unsafe in
+grooming mode, one probably wants to switch to tagging mode for negative
+beta, via set_tagging_mode().
+
+------------------------------------------------------------------------
+RecursiveSoftDrop
+------------------------------------------------------------------------
+
+The RecursiveSoftDrop procedure applies the Soft Drop procedure N times
+in a jet in order to find up to N+1 prongs. N=0 makes no modification
+to the jet, and N=1 is equivalent to the original SoftDrop.
+
+Once one has more than one prong, one has to decide which will be
+declustered next. At each step of the declustering procedure, one
+undoes the clustering which has the largest declustering angle
+(amongst all the branches that are searched for substructure). [see
+"set_fixed_depth" below for an alternative]
+
+Compared to SoftDrop, RecursiveSoftDrop takes an extra argument N
+specifying the number of times the SoftDrop procedure is recursively
+applied. Negative N means that the procedure is applied until no
+further substructure is found (i.e. corresponds to taking N=infinity).
+
+ double z_cut = 0.10;
+ double beta = 2.0;
+ double R0 = 1.0; // this is the default value
+ int N = -1;
+ RecursiveSoftDrop rsd(z_cut, beta, N, R0);
+
+One then acts on a jet as
+
+ PseudoJet groomed_jet = rsd(jet)
+
+and get additional information via
+
+ groomed_jet.structure_of<RecursiveSoftDrop>()
+
+------------------------------------------------------------------------
+IteratedSoftDrop
+------------------------------------------------------------------------
+
+Iterated Soft Drop (ISD) is a repeated variant of SoftDrop. After
+performing the Soft Drop procedure once, it logs the groomed symmetry
+factor, then recursively performs Soft Drop again on the harder
+branch. This procedure is repeated down to an (optional) angular cut
+theta_cut, yielding a set of symmetry factors from which observables
+can be built.
+
+An IteratedSoftDrop tool can be created as follows:
+
+ double beta = -1.0;
+ double z_cut = 0.005;
+ double theta_cut = 0.0;
+ double R0 = 0.5; // characteristic radius of jet algorithm
+ IteratedSoftDrop isd(beta, z_cut, double theta_cut, R0);
+
+By default, ISD applied on a jet gives a result of type
+IteratedSoftDropInfo that can then be probed to obtain physical
+observables
+
+ IteratedSoftDropInfo isd_info = isd(jet);
+
+ unsigned int multiplicity = isd_info.multiplicity();
+ double kappa = 1.0; // changes angular scale of ISD angularity
+ double isd_width = isd_info.angularity(kappa);
+ vector<pair<double,double> > zg_thetags = isd_info.all_zg_thetag();
+ vector<pair<double,double> > zg_thetags = isd_info();
+ for (unsigned int i=0; i< isd_info.size(); ++i){
+ cout << "(zg, theta_g)_" << i << " = "
+ << isd_info[i].first << " " << isd_info[i].second << endl;
+ }
+
+Alternatively, one can directly get the multiplicity, angularity, and
+(zg,thetag) pairs from the IteratedSoftDrop class, at the expense of
+re-running the declustering procedure:
+
+ unsigned int multiplicity = isd.multiplicity(jet);
+ double isd_width = isd.angularity(jet, 1.0);
+ vector<pair<double,double> > zg_thetags = isd.all_zg_thetag(jet);
+
+
+Note: the iterative declustering procedure is the same as what one
+ would obtain with RecursiveSoftDrop with an (optional) angular cut
+ and recursing only in the hardest branch [see the "Changing
+ behaviour" section below for details], except that it returns some
+ information about the jet instead of a modified jet as RSD does.
+
+
+------------------------------------------------------------------------
+BottomUpSoftDrop
+------------------------------------------------------------------------
+
+This is a bottom-up version of the RecursiveSoftDrop procedure, in a
+similar way as Pruning can be seen as a bottom-up version of Trimming.
+
+In practice, the jet is reclustered and at each step of the clustering
+one checks the SoftDrop condition
+
+ z > z_cut * (R / R0)^beta
+
+If the condition is met, the pair is recombined. If the condition is
+not met, only the hardest of the two objects is kept for further
+clustering and the softest is rejected.
+
+------------------------------------------------------------------------
+Recluster
+------------------------------------------------------------------------
+
+ *** NOTE: this is provided only for backwards compatibility ***
+ *** with FastJet <3.1. For FastJet >=3.1, the native ***
+ *** fastjet::Recluster is used instead ***
+
+The Recluster class allows the constituents of a jet to be reclustered
+with a different recursive clustering algorithm. This is used
+internally in the mMDT/SoftDrop/RecursiveSoftDrop/IteratedSoftDrop
+code in order to recluster the jet using the CA algorithm. This is
+achieved via
+
+ Recluster ca_reclusterer(cambridge_algorithm,
+ JetDefinition::max_allowable_R);
+ PseudoJet reclustered_jet = ca_reclusterer(original_jet);
+
+Note that reclustered_jet creates a new ClusterSequence that knows to
+delete_self_when_unused.
+
+------------------------------------------------------------------------
+Changing behaviour
+------------------------------------------------------------------------
+
+The behaviour of the all the tools provided here
+(ModifiedMassDropTagger, SoftDrop, RecursiveSoftDrop and
+IteratedSoftDrop) can be tweaked using the following options:
+
+SymmetryMeasure = {scalar_z, vector_z, y, theta_E, cos_theta_E}
+ [constructor argument]
+ : The definition of the energy sharing between subjets, with 0
+ corresponding to the most asymmetric.
+ . scalar_z = min(pt1,pt2)/(pt1+pt2) [default]
+ . vector_z = min(pt1,pt2)/pt_{1+2}
+ . y = min(pt1^2,pt2^2)/m_{12}^2 (original y from MDT)
+ . theta_E = min(E1,E2)/(E1+E2),
+ with angular measure theta_{12}^2
+ . cos_theta_E = min(E1,E2)/(E1+E2),
+ with angular measure 2[1-cos(theta_{12})]
+ The last two variants are meant for use in e+e- collisions,
+ together with the "larger_E" recursion choice (see below)
+
+RecursionChoice = {larger_pt, larger_mt, larger_m, larger_E}
+ [constructor argument]
+ : The path to recurse through the tree after the symmetry condition
+ fails. Options refer to transverse momentum (pt), transverse mass
+ (mt=sqrt(pt^2+m^2), mass (m) or energy (E). the latter is meant
+ for use in e+e- collisions
+
+mu_cut [constructor argument]
+ : An optional mass drop condition
+
+set_subtractor(subtractor*) [or subtractor as a constructor argument]
+ : provide a subtractor. When a subtractor is supplied, the
+ kinematic constraints are applied on subtracted 4-vectors. In
+ this case, the result of the ModifiedMassDropTagger/SoftDrop is a
+ subtracted PseudoJet, and it is assumed that
+ ModifiedMassDropTagger/SoftDrop is applied to an unsubtracted jet.
+ The latter default can be changed by calling
+ set_input_jet_is_subtracted().
+
+set_reclustering(bool, Recluster*)
+ : An optional setting to recluster a jet with a different jet
+ recursive jet algorithm. The code is only designed to give sensible
+ results with the CA algorithm, but other reclustering algorithm
+ (especially kT) may be appropriate in certain contexts.
+ Use at your own risk.
+
+set_grooming_mode()/set_tagging_mode()
+ : In grooming mode, the algorithm will return a single particle if the
+ symmetry condition fails for the whole tree. In tagging mode, the
+ algorithm will return an zero PseudoJet if no symmetry conditions
+ passes. Note that ModifiedMassDropTagger defaults to tagging mode
+ and SoftDrop defaults to grooming mode.
+
+set_verbose_structure(bool)
+ : when set to true, additional information will be stored in the jet
+ structure. This includes in particular values of symmetry,
+ delta_R, and mu of dropped branches
+
+For the specific case of RecursiveSoftDrop, additional tweaking is
+possible via the following methods
+
+set_fixed_depth_mode(bool)
+ : when this is true, RSD will recurse (N times) into all the
+ branches found during the previous iteration [instead of recursing
+ through the largest declustering angle until N prongs have been
+ found]. This yields at most 2^N prong. For infinite N, the two
+ options are equivalent.
+
+set_dynamical_R0(bool)
+ : By default the angles in the SD condition are normalised to the
+ parameter R0. With "dynamical R0", RSD will dynamically adjust R0
+ to be the angle between the two prongs found during the previous
+ iteration.
+
+set_hardest_branch_only(bool)
+ : When substructure is found, only recurse into the hardest of the
+ two branches for further substructure search. This uses the class
+ RecursionChoice.
+
+set_min_deltaR_squared(double):
+ : set a minimal angle (squared) at which we stop the declustering
+ procedure. This cut is ineffective for negative values of the
+ argument.
+
+------------------------------------------------------------------------
+Technical Details
+------------------------------------------------------------------------
+
+Both ModifiedMassDropTagger and SoftDrop inherit from
+RecursiveSymmetryCutBase, which provides a common codebase for recursive
+declustering of a jet with a symmetry cut condition. A generic
+RecursiveSymmetryCutBase depends on the following (virtual) functions
+(see header file for exact full specs, including constness):
+
+double symmetry_cut_fn(PseudoJet &, PseudoJet &)
+ : The function that defines the symmetry cut. This is what actually
+ defines different recursive declustering schemes, and all classes
+ that inherit from RecursiveSymmetryCutBase must define this
+ function.
+
+string symmetry_cut_description()
+ : the string description of the symmetry cut.
+
+------------------------------------------------------------------------
diff --git a/src/Tools/fjcontrib/RecursiveTools/Recluster.cc b/src/Tools/fjcontrib/RecursiveTools/Recluster.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/Recluster.cc
@@ -0,0 +1,394 @@
+// $Id: Recluster.cc 699 2014-07-07 09:58:12Z gsoyez $
+//
+// Copyright (c) 2014-, Matteo Cacciari, Gavin P. Salam and Gregory Soyez
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include "Recluster.hh"
+#include <fastjet/ClusterSequenceActiveAreaExplicitGhosts.hh>
+#include <sstream>
+#include <typeinfo>
+
+using namespace std;
+
+// Comments:
+//
+// - If the jet comes from a C/A clustering (or is a composite jet
+// made of C/A clusterings) and we recluster it with a C/A
+// algorithm, we just use exclusive jets instead of doing the
+// clustering explicitly. In this specific case, we need to make
+// sure that all the pieces share the same cluster sequence.
+//
+// - If the recombiner has to be taken from the original jet and that
+// jet is composite, we need to check that all the pieces were
+// obtained with the same recombiner.
+//
+// TODO:
+//
+// - check this actually works!!!
+
+//FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+ //namespace contrib{
+
+ namespace Rivet{
+ namespace fjcontrib{
+
+
+LimitedWarning Recluster::_explicit_ghost_warning;
+
+// class description
+string Recluster::description() const {
+ ostringstream ostr;
+ ostr << "Recluster with subjet_def = ";
+ if (_use_full_def) {
+ ostr << _subjet_def.description();
+ } else {
+ if (_subjet_alg == kt_algorithm) {
+ ostr << "Longitudinally invariant kt algorithm with R = " << _subjet_radius;
+ } else if (_subjet_alg == cambridge_algorithm) {
+ ostr << "Longitudinally invariant Cambridge/Aachen algorithm with R = " << _subjet_radius;
+ } else if (_subjet_alg == antikt_algorithm) {
+ ostr << "Longitudinally invariant anti-kt algorithm with R = " << _subjet_radius;
+ } else if (_subjet_alg == genkt_algorithm) {
+ ostr << "Longitudinally invariant generalised kt algorithm with R = " << _subjet_radius
+ << ", p = " << _subjet_extra;
+ } else if (_subjet_alg == cambridge_for_passive_algorithm) {
+ ostr << "Longitudinally invariant Cambridge/Aachen algorithm with R = " << _subjet_radius
+ << " and a special hack whereby particles with kt < "
+ << _subjet_extra << "are treated as passive ghosts";
+ } else if (_subjet_alg == ee_kt_algorithm) {
+ ostr << "e+e- kt (Durham) algorithm";
+ } else if (_subjet_alg == ee_genkt_algorithm) {
+ ostr << "e+e- generalised kt algorithm with R = " << _subjet_radius
+ << ", p = " << _subjet_extra;
+ } else if (_subjet_alg == undefined_jet_algorithm) {
+ ostr << "uninitialised JetDefinition (jet_algorithm=undefined_jet_algorithm)" ;
+ } else {
+ ostr << "unrecognized jet_algorithm";
+ }
+ ostr << ", a recombiner obtained from the jet being reclustered";
+ }
+
+ if (_single)
+ ostr << " and keeping the hardest subjet";
+ else
+ ostr << " and joining all subjets in a composite jet";
+
+ return ostr.str();
+}
+
+// return a vector of subjets, which are the ones that would be kept
+// by the filtering
+PseudoJet Recluster::result(const PseudoJet &jet) const {
+ // generic sanity checks
+ //-------------------------------------------------------------------
+ // make sure that the jet has constituents
+ if (! jet.has_constituents())
+ throw Error("Filter can only be applied on jets having constituents");
+
+ // tests particular to certain configurations
+ //-------------------------------------------------------------------
+
+ // for a whole variety of checks, we shall need the "recursive"
+ // pieces of the jet (the jet itself or recursing down to its most
+ // fundamental pieces). So we do compute these once and for all.
+ //
+ // Note that the pieces are always needed (either for C/A or for the
+ // area checks)
+ vector<PseudoJet> all_pieces; //.clear();
+ if ((!_get_all_pieces(jet, all_pieces)) || (all_pieces.size()==0)){
+ throw Error("Recluster: failed to retrieve all the pieces composing the jet.");
+ }
+
+ // decide which jet definition to use
+ //-------------------------------------------------------------------
+ JetDefinition subjet_def;
+ if (_use_full_def){
+ subjet_def = _subjet_def;
+ } else {
+ _build_jet_def_with_recombiner(all_pieces, subjet_def);
+ }
+
+
+ // the vector that will ultimately hold the subjets
+ vector<PseudoJet> subjets;
+
+ // check if we can apply the simplification for C/A jets reclustered
+ // with C/A
+ //
+ // we apply C/A clustering iff
+ // - the request subjet_def is C/A
+ // - the jet is either directly coming from C/A or if it is a
+ // superposition of C/A jets from the same cluster sequence
+ // - the pieces agree with the recombination scheme of subjet_def
+ //
+ // Note that in this case area support will be automatically
+ // inherted so we can only worry about this later
+ //-------------------------------------------------------------------
+ if (_check_ca(all_pieces, subjet_def)){
+ _recluster_cafilt(all_pieces, subjets, subjet_def.R());
+ subjets = sorted_by_pt(subjets);
+ return _single
+ ? subjets[0]
+ : join(subjets, *(subjet_def.recombiner()));
+ }
+
+ // decide if area support has to be kept
+ //-------------------------------------------------------------------
+ bool include_area_support = jet.has_area();
+ if ((include_area_support) && (!_check_explicit_ghosts(all_pieces))){
+ _explicit_ghost_warning.warn("Recluster: the original cluster sequence is lacking explicit ghosts; area support will no longer be available after re-clustering");
+ include_area_support = false;
+ }
+
+ // extract the subjets
+ //-------------------------------------------------------------------
+ _recluster_generic(jet, subjets, subjet_def, include_area_support);
+ subjets = sorted_by_pt(subjets);
+
+ return _single
+ ? subjets[0]
+ : join(subjets, *(subjet_def.recombiner()));
+}
+
+//----------------------------------------------------------------------
+// the parts that really do the reclustering
+//----------------------------------------------------------------------
+
+// get the subjets in the simple case of C/A+C/A
+void Recluster::_recluster_cafilt(const vector<PseudoJet> & all_pieces,
+ vector<PseudoJet> & subjets,
+ double Rfilt) const{
+ subjets.clear();
+
+ // each individual piece should have a C/A cluster sequence
+ // associated to it. So a simple loop would do the job
+ for (vector<PseudoJet>::const_iterator piece_it = all_pieces.begin();
+ piece_it!=all_pieces.end(); piece_it++){
+ // just extract the exclusive subjets of 'jet'
+ const ClusterSequence *cs = piece_it->associated_cluster_sequence();
+ vector<PseudoJet> local_subjets;
+
+ double dcut = Rfilt / cs->jet_def().R();
+ if (dcut>=1.0){
+ local_subjets.push_back(*piece_it);
+ } else {
+ local_subjets = piece_it->exclusive_subjets(dcut*dcut);
+ }
+
+ copy(local_subjets.begin(), local_subjets.end(), back_inserter(subjets));
+ }
+}
+
+
+// set the filtered elements in the generic re-clustering case (w/o
+// subtraction)
+void Recluster::_recluster_generic(const PseudoJet & jet,
+ vector<PseudoJet> & subjets,
+ const JetDefinition & subjet_def,
+ bool do_areas) const{
+ // create a new, internal, ClusterSequence from the jet constituents
+ // get the subjets directly from there
+ //
+ // If the jet has area support then we separate the ghosts from the
+ // "regular" particles so the subjets will also have area
+ // support. Note that we do this regardless of whether rho is zero
+ // or not.
+ //
+ // Note that to be able to separate the ghosts, one needs explicit
+ // ghosts!!
+ // ---------------------------------------------------------------
+ if (do_areas){
+ vector<PseudoJet> all_constituents = jet.constituents();
+ vector<PseudoJet> regular_constituents, ghosts;
+
+ for (vector<PseudoJet>::iterator it = all_constituents.begin();
+ it != all_constituents.end(); it++){
+ if (it->is_pure_ghost())
+ ghosts.push_back(*it);
+ else
+ regular_constituents.push_back(*it);
+ }
+
+ // figure out the ghost area from the 1st ghost (if none, any value
+ // would probably do as the area will be 0 and subtraction will have
+ // no effect!)
+ double ghost_area = (ghosts.size()) ? ghosts[0].area() : 0.01;
+ ClusterSequenceActiveAreaExplicitGhosts * csa
+ = new ClusterSequenceActiveAreaExplicitGhosts(regular_constituents,
+ subjet_def,
+ ghosts, ghost_area);
+
+ subjets = csa->inclusive_jets();
+
+ // allow the cs to be deleted when it's no longer used
+ //
+ // Note that there is at least one constituent in the jet so there
+ // is in principle at least one subjet But one may have used a
+ // nasty recombiner that left an empty set of subjets, so we'd
+ // rather play it safe
+ if (subjets.size())
+ csa->delete_self_when_unused();
+ else
+ delete csa;
+ } else {
+ ClusterSequence * cs = new ClusterSequence(jet.constituents(), subjet_def);
+ subjets = cs->inclusive_jets();
+ // allow the cs to be deleted when it's no longer used (again, we
+ // add an extra safety check)
+ if (subjets.size())
+ cs->delete_self_when_unused();
+ else
+ delete cs;
+ }
+}
+
+
+//----------------------------------------------------------------------
+// various checks and internal constructs
+//----------------------------------------------------------------------
+
+// fundamental info for CompositeJets
+//----------------------------------------------------------------------
+
+// get the pieces down to the fundamental pieces
+//
+// Note that this just checks that there is an associated CS to the
+// fundamental pieces, not that it is still valid
+bool Recluster::_get_all_pieces(const PseudoJet &jet, vector<PseudoJet> &all_pieces) const{
+ if (jet.has_associated_cluster_sequence()){
+ all_pieces.push_back(jet);
+ return true;
+ }
+
+ if (jet.has_pieces()){
+ const vector<PseudoJet> pieces = jet.pieces();
+ for (vector<PseudoJet>::const_iterator it=pieces.begin(); it!=pieces.end(); it++)
+ if (!_get_all_pieces(*it, all_pieces)) return false;
+ return true;
+ }
+
+ return false;
+}
+
+// treatment of recombiners
+//----------------------------------------------------------------------
+// get the common recombiner to all pieces (NULL if none)
+//
+// Note that if the jet has an associated cluster sequence that is no
+// longer valid, an error will be thrown (needed since it could be the
+// 1st check called after the enumeration of the pieces)
+const JetDefinition::Recombiner* Recluster::_get_common_recombiner(const vector<PseudoJet> &all_pieces) const{
+ const JetDefinition & jd_ref = all_pieces[0].validated_cs()->jet_def();
+ for (unsigned int i=1; i<all_pieces.size(); i++)
+ if (!all_pieces[i].validated_cs()->jet_def().has_same_recombiner(jd_ref)) return NULL;
+
+ return jd_ref.recombiner();
+}
+
+void Recluster::_build_jet_def_with_recombiner(const vector<PseudoJet> &all_pieces,
+ JetDefinition &subjet_def) const{
+ // the recombiner has to be guessed from the pieces
+ const JetDefinition::Recombiner * common_recombiner = _get_common_recombiner(all_pieces);
+ if (common_recombiner) {
+ if (typeid(*common_recombiner) == typeid(JetDefinition::DefaultRecombiner)) {
+ RecombinationScheme scheme =
+ static_cast<const JetDefinition::DefaultRecombiner *>(common_recombiner)->scheme();
+ if (_has_subjet_extra)
+ subjet_def = JetDefinition(_subjet_alg, _subjet_radius, _subjet_extra, scheme);
+ else if (_has_subjet_radius)
+ subjet_def = JetDefinition(_subjet_alg, _subjet_radius, scheme);
+ else
+ subjet_def = JetDefinition(_subjet_alg, scheme);
+ } else {
+ if (_has_subjet_extra)
+ subjet_def = JetDefinition(_subjet_alg, _subjet_radius, _subjet_extra, common_recombiner);
+ else if (_has_subjet_radius)
+ subjet_def = JetDefinition(_subjet_alg, _subjet_radius, common_recombiner);
+ else
+ subjet_def = JetDefinition(_subjet_alg, common_recombiner);
+ }
+ } else {
+ throw Error("Recluster: requested to guess the recombination scheme (or recombiner) from the original jet but an inconsistency was found between the pieces constituing that jet.");
+ }
+}
+
+// area support
+//----------------------------------------------------------------------
+
+// check if the jet (or all its pieces) have explicit ghosts
+// (assuming the jet has area support).
+//
+// Note that if the jet has an associated cluster sequence that is no
+// longer valid, an error will be thrown (needed since it could be the
+// 1st check called after the enumeration of the pieces)
+bool Recluster::_check_explicit_ghosts(const vector<PseudoJet> &all_pieces) const{
+ for (vector<PseudoJet>::const_iterator it=all_pieces.begin(); it!=all_pieces.end(); it++)
+ if (! it->validated_csab()->has_explicit_ghosts()) return false;
+ return true;
+}
+
+// C/A specific tests
+//----------------------------------------------------------------------
+
+// check if one can apply the simplification for C/A subjets
+//
+// This includes:
+// - the subjet definition asks for C/A subjets
+// - all the pieces share the same CS
+// - that CS is C/A with the same recombiner as the subjet def
+// - the filtering radius is not larger than any of the pairwise
+// distance between the pieces
+//
+// Note that if the jet has an associated cluster sequence that is no
+// longer valid, an error will be thrown (needed since it could be the
+// 1st check called after the enumeration of the pieces)
+bool Recluster::_check_ca(const vector<PseudoJet> &all_pieces,
+ const JetDefinition &subjet_def) const{
+ if (subjet_def.jet_algorithm() != cambridge_algorithm) return false;
+
+ // check that the 1st of all the pieces (we're sure there is at
+ // least one) is coming from a C/A clustering. Then check that all
+ // the following pieces share the same ClusterSequence
+ const ClusterSequence * cs_ref = all_pieces[0].validated_cs();
+ if (cs_ref->jet_def().jet_algorithm() != cambridge_algorithm) return false;
+ for (unsigned int i=1; i<all_pieces.size(); i++)
+ if (all_pieces[i].validated_cs() != cs_ref) return false;
+
+ // check that the 1st peice has the same recombiner as the one used
+ // for the subjet clustering
+ // Note that since they share the same CS, checking the 1st one is enough
+ if (!cs_ref->jet_def().has_same_recombiner(subjet_def)) return false;
+
+ // we also have to make sure that the reclustering radius is not larger
+ // than any of the inter-pieces distance
+ double Rsub2 = subjet_def.R();
+ Rsub2 *= Rsub2;
+ for (unsigned int i=0; i<all_pieces.size()-1; i++){
+ for (unsigned int j=i+1; j<all_pieces.size(); j++){
+ if (all_pieces[i].squared_distance(all_pieces[j]) < Rsub2) return false;
+ }
+ }
+
+ return true;
+}
+
+ } } // contrib namespace
+
+ //FASTJET_END_NAMESPACE // defined in fastjet/internal/base.hh
diff --git a/src/Tools/fjcontrib/RecursiveTools/RecursiveSoftDrop.cc b/src/Tools/fjcontrib/RecursiveTools/RecursiveSoftDrop.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/RecursiveSoftDrop.cc
@@ -0,0 +1,486 @@
+// $Id: RecursiveSoftDrop.cc 1111 2018-04-04 10:06:11Z gsoyez $
+//
+// Copyright (c) 2017-, Gavin P. Salam, Gregory Soyez, Jesse Thaler,
+// Kevin Zhou, Frederic Dreyer
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include "RecursiveSoftDrop.hh"
+#include "fastjet/ClusterSequence.hh"
+
+using namespace std;
+
+// FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+ //namespace contrib{
+
+ namespace Rivet{
+ namespace fjcontrib{
+
+
+namespace internal_recursive_softdrop{
+
+//========================================================================
+/// \class RSDHistoryElement
+/// a helper class to help keeping track od the RSD tree
+///
+/// The element is created at the top of a branch and updated each
+/// time one grooms something away.
+class RSDHistoryElement{
+public:
+ RSDHistoryElement(const PseudoJet &jet, const RecursiveSoftDrop* rsd_ptr, double R0sqr) :
+ R0_squared(R0sqr),
+ child1_in_history(-1), child2_in_history(-1), symmetry(-1.0), mu2(-1.0){
+ reset(jet, rsd_ptr);
+ }
+
+ void reset(const PseudoJet &jet, const RecursiveSoftDrop* rsd_ptr){
+ current_in_ca_tree = jet.cluster_hist_index();
+ PseudoJet piece1, piece2;
+ theta_squared = (jet.has_parents(piece1, piece2))
+ ? rsd_ptr->squared_geometric_distance(piece1,piece2) : 0.0;
+ }
+
+ int current_in_ca_tree; ///< (history) index of the current particle in the C/A tree
+ double theta_squared; ///< squared angle at which this decays
+ double R0_squared; ///< squared angle at the top of the branch
+ ///< (used for RSD with dynamic_R0)
+ int child1_in_history; ///< hardest of the 2 decay products (-1 if untagged)
+ int child2_in_history; ///< softest of the 2 decay products (-1 if untagged)
+
+ // info about what has been dropped and the local substructure
+ vector<double> dropped_delta_R;
+ vector<double> dropped_symmetry;
+ vector<double> dropped_mu;
+ double symmetry, mu2;
+};
+
+
+/// \class OrderRSDHistoryElements
+/// angular ordering of (pointers to) the history elements
+///
+/// our priority queue will use pointers to these elements that are
+/// ordered in angle (of the objects they point to)
+class OrderRSDHistoryElements{
+public:
+ bool operator()(const RSDHistoryElement *e1, const RSDHistoryElement *e2) const {
+ return e1->theta_squared < e2->theta_squared;
+ }
+};
+
+} // internal_recursive_softdrop
+
+//========================================================================
+
+// initialise all the flags and parameters to their default value
+void RecursiveSoftDrop::set_defaults(){
+ set_fixed_depth_mode(false);
+ set_dynamical_R0(false);
+ set_hardest_branch_only(false);
+ set_min_deltaR_squared(-1.0);
+}
+
+// description of the tool
+string RecursiveSoftDrop::description() const{
+ ostringstream res;
+ res << "recursive application of ["
+ << RecursiveSymmetryCutBase::description()
+ << "]";
+
+ if (_fixed_depth){
+ res << ", recursively applied down to a maximal depth of N=";
+ if (_n==-1) res << "infinity"; else res << _n;
+ } else {
+ res << ", applied N=";
+ if (_n==-1) res << "infinity"; else res << _n;
+ res << " times";
+ }
+
+ if (_dynamical_R0)
+ res << ", with R0 dynamically scaled";
+ else
+ res << ", with R0 kept fixed";
+
+ if (_hardest_branch_only)
+ res << ", following only the hardest branch";
+
+ if (_min_dR2>0)
+ res << ", with minimal angle (squared) = " << _min_dR2;
+
+ return res.str();
+}
+
+
+// action on a single jet with RecursiveSoftDrop.
+//
+// uses "result_fixed_tags" by default (i.e. recurse from R0 to
+// smaller angles until n SD conditions have been met), or
+// "result_fixed_depth" where each of the previous SD branches are
+// recirsed into down to a depth of n.
+PseudoJet RecursiveSoftDrop::result(const PseudoJet &jet) const{
+ return _fixed_depth ? result_fixed_depth(jet) : result_fixed_tags(jet);
+}
+
+// this routine applies the Soft Drop criterion recursively on the
+// CA tree until we find n subjets (or until it converges), and
+// adds them together into a groomed PseudoJet
+PseudoJet RecursiveSoftDrop::result_fixed_tags(const PseudoJet &jet) const {
+ // start by reclustering jet with C/A algorithm
+ PseudoJet ca_jet = _recluster_if_needed(jet);
+
+ if (! ca_jet.has_valid_cluster_sequence()){
+ throw Error("RecursiveSoftDrop can only be applied to jets associated to a (valid) cluster sequence");
+ }
+
+ const ClusterSequence *cs = ca_jet.validated_cluster_sequence();
+ const vector<ClusterSequence::history_element> &cs_history = cs->history();
+ const vector<PseudoJet> &cs_jets = cs->jets();
+
+ // initialize counter to 1 subjet (i.e. the full ca_jet)
+ int n_tagged = 0;
+ int max_njet = ca_jet.constituents().size();
+
+ // create the list of branches
+ unsigned int max_history_size = 2*max_njet;
+ if ((_n>0) && (_n<max_njet-1)){ max_history_size = 2*(_n+1); }
+
+ // we need to pre-allocate the space for the vector so that the
+ // pointers are not invalidated
+ vector<internal_recursive_softdrop::RSDHistoryElement> history;
+ history.reserve(max_history_size); // could be one shorter
+ history.push_back(internal_recursive_softdrop::RSDHistoryElement(ca_jet, this, _R0sqr));
+
+ // create a priority queue containing the subjets and a comparison definition
+ // initialise to the full ca_jet
+ priority_queue<internal_recursive_softdrop::RSDHistoryElement*, vector<internal_recursive_softdrop::RSDHistoryElement*>, internal_recursive_softdrop::OrderRSDHistoryElements> active_branches;
+ active_branches.push(& (history[0]));
+
+ PseudoJet parent, piece1, piece2;
+ double sym, mu2;
+
+ // which R0 to use
+ //double R0sqr = _R0sqr;
+
+ // loop over C/A tree until we reach the appropriate number of subjets
+ while ((continue_grooming(n_tagged)) && (active_branches.size())) {
+ // get the element corresponding to the max dR
+ // and the associated PJ
+ internal_recursive_softdrop::RSDHistoryElement * elm = active_branches.top();
+ PseudoJet parent = cs_jets[cs_history[elm->current_in_ca_tree].jetp_index];
+
+ // do one step of SD
+ RecursionStatus status = recurse_one_step(parent, piece1, piece2, sym, mu2, &elm->R0_squared);
+
+ // check if we passed the SD condition
+ if (status==recursion_success){
+ // check for the optional angular cut
+ if ((_min_dR2 > 0) && (squared_geometric_distance(piece1,piece2) < _min_dR2))
+ break;
+
+ // both subjets are kept in the list for potential further de-clustering
+ elm->child1_in_history = history.size();
+ elm->child2_in_history = history.size()+1;
+ elm->symmetry = sym;
+ elm->mu2 = mu2;
+ active_branches.pop();
+
+ // update the history
+ double next_R0_squared = (_dynamical_R0)
+ ? piece1.squared_distance(piece2) : elm->R0_squared;
+
+ internal_recursive_softdrop::RSDHistoryElement elm1(piece1, this, next_R0_squared);
+ history.push_back(elm1);
+ active_branches.push(&(history.back()));
+ internal_recursive_softdrop::RSDHistoryElement elm2(piece2, this, next_R0_squared);
+ history.push_back(elm2);
+ if (!_hardest_branch_only){
+ active_branches.push(&(history.back()));
+ }
+
+ ++n_tagged;
+ } else if (status==recursion_dropped){
+ // check for the optional angular cut
+ if ((_min_dR2 > 0) && (squared_geometric_distance(piece1,piece2) < _min_dR2))
+ break;
+
+ active_branches.pop();
+ // tagging failed and the softest branch should be dropped
+ // keep track of what has een groomed away
+ max_njet -= piece2.constituents().size();
+ elm->dropped_delta_R .push_back((elm->theta_squared >= 0) ? sqrt(elm->theta_squared) : -sqrt(elm->theta_squared));
+ elm->dropped_symmetry.push_back(sym);
+ elm->dropped_mu .push_back((mu2>=0) ? sqrt(mu2) : -sqrt(mu2));
+
+ // keep the hardest bhanch in the recursion
+ elm->reset(piece1, this);
+ active_branches.push(elm);
+ } else if (status==recursion_no_parents){
+ if (_min_dR2 > 0) break;
+ active_branches.pop();
+ // nothing specific to do: we just keep the curent jet as a "leaf"
+ } else { // recursion_issue
+ active_branches.pop();
+ // we've met an issue
+ // if the piece2 is null as well, it means we've had a critical problem.
+ // In that case, return an empty PseudoJet
+ if (piece2 == 0) return PseudoJet();
+
+ // otherwise, we should consider "piece2" as a final particle
+ // not to be recursed into
+ if (_min_dR2 > 0) break;
+ max_njet -= (piece2.constituents().size()-1);
+ break;
+ }
+
+ // If the missing number of tags is exactly the number of objects
+ // we have left in the recursion, stop
+ if (n_tagged == max_njet) break;
+ }
+
+ // now we have a bunch of history elements that we can use to build the final jet
+ vector<PseudoJet> mapped_to_history(history.size());
+ unsigned int history_index = history.size();
+ do {
+ --history_index;
+ const internal_recursive_softdrop::RSDHistoryElement & elm = history[history_index];
+
+ // two kinds of events: either just a final leave, poteitially with grooming
+ // or a brandhing (also with potential grooming at the end)
+ if (elm.child1_in_history<0){
+ // this is a leaf, i.e. with no further sustructure
+ PseudoJet & subjet = mapped_to_history[history_index]
+ = cs_jets[cs_history[elm.current_in_ca_tree].jetp_index];
+
+ StructureType * structure = new StructureType(subjet);
+ if (has_verbose_structure()){
+ structure->set_verbose(true);
+ structure->set_dropped_delta_R (elm.dropped_delta_R);
+ structure->set_dropped_symmetry(elm.dropped_symmetry);
+ structure->set_dropped_mu (elm.dropped_mu);
+ }
+ subjet.set_structure_shared_ptr(SharedPtr<PseudoJetStructureBase>(structure));
+ } else {
+ PseudoJet & subjet = mapped_to_history[history_index]
+ = join(mapped_to_history[elm.child1_in_history], mapped_to_history[elm.child2_in_history]);
+ StructureType * structure = new StructureType(subjet, sqrt(elm.theta_squared), elm.symmetry, sqrt(elm.mu2));
+ if (has_verbose_structure()){
+ structure->set_verbose(true);
+ structure->set_dropped_delta_R (elm.dropped_delta_R);
+ structure->set_dropped_symmetry(elm.dropped_symmetry);
+ structure->set_dropped_mu (elm.dropped_mu);
+ }
+ subjet.set_structure_shared_ptr(SharedPtr<PseudoJetStructureBase>(structure));
+ }
+ } while (history_index>0);
+
+ return mapped_to_history[0];
+}
+
+// this routine applies the Soft Drop criterion recursively on the
+// CA tree, recursing into all the branches found during the previous iteration
+// until n layers have been found (or until it converges)
+PseudoJet RecursiveSoftDrop::result_fixed_depth(const PseudoJet &jet) const {
+ // start by reclustering jet with C/A algorithm
+ PseudoJet ca_jet = _recluster_if_needed(jet);
+
+ if (! ca_jet.has_valid_cluster_sequence()){
+ throw Error("RecursiveSoftDrop can only be applied to jets associated to a (valid) cluster sequence");
+ }
+
+ const ClusterSequence *cs = ca_jet.validated_cluster_sequence();
+ const vector<ClusterSequence::history_element> &cs_history = cs->history();
+ const vector<PseudoJet> &cs_jets = cs->jets();
+
+ // initialize counter to 1 subjet (i.e. the full ca_jet)
+ int n_depth = 0;
+ int max_njet = ca_jet.constituents().size();
+
+ // create the list of branches
+ unsigned int max_history_size = 2*max_njet;
+ //if ((_n>0) && (_n<max_njet-1)){ max_history_size = 2*(_n+1); }
+
+ // we need to pre-allocate the space for the vector so that the
+ // pointers are not invalidated
+ vector<internal_recursive_softdrop::RSDHistoryElement> history;
+ history.reserve(max_history_size); // could be one shorter
+ history.push_back(internal_recursive_softdrop::RSDHistoryElement(ca_jet, this, _R0sqr));
+ history.back().theta_squared = _R0sqr;
+
+ // create a priority queue containing the subjets and a comparison definition
+ // initialize counter to 1 subjet (i.e. the full ca_jet)
+ list<internal_recursive_softdrop::RSDHistoryElement*> active_branches;
+ active_branches.push_back(& (history[0]));
+
+ PseudoJet parent, piece1, piece2;
+
+ while ((continue_grooming(n_depth)) && (active_branches.size())) {
+ // loop over all the branches and look for substructure
+ list<internal_recursive_softdrop::RSDHistoryElement*>::iterator hist_it=active_branches.begin();
+ while (hist_it!=active_branches.end()){
+ // get the element corresponding to the max dR
+ // and the associated PJ
+ internal_recursive_softdrop::RSDHistoryElement * elm = (*hist_it);
+ PseudoJet parent = cs_jets[cs_history[elm->current_in_ca_tree].jetp_index];
+
+ // we need to iterate this branch until we find some substructure
+ PseudoJet result_sd;
+ if (_dynamical_R0){
+ SoftDrop sd(_beta, _symmetry_cut, symmetry_measure(), sqrt(elm->theta_squared),
+ mu_cut(), recursion_choice(), subtractor());
+ sd.set_reclustering(false);
+ sd.set_verbose_structure(has_verbose_structure());
+ result_sd = sd(parent);
+ } else {
+ result_sd = SoftDrop::result(parent);
+ }
+
+ // if we had an empty PJ, that means we ran into some problems.
+ // just return an empty PJ ourselves
+ if (result_sd == 0) return PseudoJet();
+
+ // update the history element to reflect our iteration
+ elm->current_in_ca_tree = result_sd.cluster_hist_index();
+
+ if (has_verbose_structure()){
+ elm->dropped_delta_R = result_sd.structure_of<SoftDrop>().dropped_delta_R();
+ elm->dropped_symmetry = result_sd.structure_of<SoftDrop>().dropped_symmetry();
+ elm->dropped_mu = result_sd.structure_of<SoftDrop>().dropped_mu();
+ }
+
+ // if some substructure was found:
+ if (result_sd.structure_of<SoftDrop>().has_substructure()){
+ // update the history element to reflect our iteration
+ elm->child1_in_history = history.size();
+ elm->child2_in_history = history.size()+1;
+ elm->theta_squared = result_sd.structure_of<SoftDrop>().delta_R();
+ elm->theta_squared *= elm->theta_squared;
+ elm->symmetry = result_sd.structure_of<SoftDrop>().symmetry();
+ elm->mu2 = result_sd.structure_of<SoftDrop>().mu();
+ elm->mu2 *= elm->mu2;
+
+ // the next iteration will have to handle 2 new history
+ // elements (the R0squared argument here is unused)
+ result_sd.has_parents(piece1, piece2);
+ internal_recursive_softdrop::RSDHistoryElement elm1(piece1, this, _R0sqr);
+ history.push_back(elm1);
+ // insert it in the active branches if needed
+ if (elm1.theta_squared>0)
+ active_branches.insert(hist_it,&(history.back())); // insert just before
+
+ internal_recursive_softdrop::RSDHistoryElement elm2(piece2, this, _R0sqr);
+ history.push_back(elm2);
+ if ((!_hardest_branch_only) && (elm2.theta_squared>0)){
+ active_branches.insert(hist_it,&(history.back())); // insert just before
+ }
+ }
+ // otherwise we've just reached the end of the recursion the
+ // history information has been updated above
+ //
+ // we just need to make sure that we do not recurse into that
+ // element any longer
+
+ list<internal_recursive_softdrop::RSDHistoryElement*>::iterator current = hist_it;
+ ++hist_it;
+ active_branches.erase(current);
+ } // loop over branches at current depth
+ ++n_depth;
+ } // loop over depth
+
+ // now we have a bunch of history elements that we can use to build the final jet
+ vector<PseudoJet> mapped_to_history(history.size());
+ unsigned int history_index = history.size();
+ do {
+ --history_index;
+ const internal_recursive_softdrop::RSDHistoryElement & elm = history[history_index];
+
+ // two kinds of events: either just a final leave, poteitially with grooming
+ // or a brandhing (also with potential grooming at the end)
+ if (elm.child1_in_history<0){
+ // this is a leaf, i.e. with no further sustructure
+ PseudoJet & subjet = mapped_to_history[history_index]
+ = cs_jets[cs_history[elm.current_in_ca_tree].jetp_index];
+
+ StructureType * structure = new StructureType(subjet);
+ if (has_verbose_structure()){
+ structure->set_verbose(true);
+ }
+ subjet.set_structure_shared_ptr(SharedPtr<PseudoJetStructureBase>(structure));
+ } else {
+ PseudoJet & subjet = mapped_to_history[history_index]
+ = join(mapped_to_history[elm.child1_in_history], mapped_to_history[elm.child2_in_history]);
+ StructureType * structure = new StructureType(subjet, sqrt(elm.theta_squared), elm.symmetry, sqrt(elm.mu2));
+ if (has_verbose_structure()){
+ structure->set_verbose(true);
+ structure->set_dropped_delta_R (elm.dropped_delta_R);
+ structure->set_dropped_symmetry(elm.dropped_symmetry);
+ structure->set_dropped_mu (elm.dropped_mu);
+ }
+ subjet.set_structure_shared_ptr(SharedPtr<PseudoJetStructureBase>(structure));
+ }
+ } while (history_index>0);
+
+ return mapped_to_history[0];
+}
+
+
+//========================================================================
+// implementation of the helpers
+//========================================================================
+
+// helper to get all the prongs in a jet that has been obtained using
+// RecursiveSoftDrop (instead of recursively parsing the 1->2
+// composite jet structure)
+vector<PseudoJet> recursive_soft_drop_prongs(const PseudoJet & rsd_jet){
+ // make sure that the jet has the appropriate RecursiveSoftDrop structure
+ if (!rsd_jet.has_structure_of<RecursiveSoftDrop>())
+ return vector<PseudoJet>();
+
+ // if this jet has no substructure, just return a 1-prong object
+ if (!rsd_jet.structure_of<RecursiveSoftDrop>().has_substructure())
+ return vector<PseudoJet>(1, rsd_jet);
+
+ // otherwise fill a vector with all the prongs (no specific ordering)
+ vector<PseudoJet> prongs;
+
+ // parse the list of PseudoJet we still need to deal with
+ vector<PseudoJet> to_parse = rsd_jet.pieces(); // valid both for a C/A recombination step or a RSD join
+ unsigned int i_parse = 0;
+ while (i_parse<to_parse.size()){
+ const PseudoJet &current = to_parse[i_parse];
+
+ if ((current.has_structure_of<RecursiveSymmetryCutBase>()) &&
+ (current.structure_of<RecursiveSymmetryCutBase>().has_substructure())){
+ // if this has some deeper substructure, add it to the list of
+ // things to further process
+ vector<PseudoJet> pieces = current.pieces();
+ assert(pieces.size() == 2);
+ to_parse[i_parse] = pieces[0];
+ to_parse.push_back(pieces[1]);
+ } else {
+ // no further substructure, just add this as a branch
+ prongs.push_back(current);
+ ++i_parse;
+ }
+ }
+
+ return prongs;
+}
+
+ } }
+
+ //FASTJET_END_NAMESPACE
diff --git a/src/Tools/fjcontrib/RecursiveTools/RecursiveSymmetryCutBase.cc b/src/Tools/fjcontrib/RecursiveTools/RecursiveSymmetryCutBase.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/RecursiveSymmetryCutBase.cc
@@ -0,0 +1,646 @@
+// $Id: RecursiveSymmetryCutBase.cc 1080 2017-09-28 07:51:37Z gsoyez $
+//
+// Copyright (c) 2014-, Gavin P. Salam, Gregory Soyez, Jesse Thaler
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include "RecursiveSymmetryCutBase.hh"
+#include "fastjet/JetDefinition.hh"
+#include "fastjet/ClusterSequenceAreaBase.hh"
+#include <cassert>
+#include <algorithm>
+#include <cstdlib>
+
+using namespace std;
+
+//FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+ //namespace contrib{
+
+ namespace Rivet{
+ namespace fjcontrib{
+
+
+LimitedWarning RecursiveSymmetryCutBase::_negative_mass_warning;
+LimitedWarning RecursiveSymmetryCutBase::_mu2_gt1_warning;
+//LimitedWarning RecursiveSymmetryCutBase::_nonca_warning;
+LimitedWarning RecursiveSymmetryCutBase::_explicit_ghost_warning;
+
+bool RecursiveSymmetryCutBase::_verbose = false;
+
+//----------------------------------------------------------------------
+PseudoJet RecursiveSymmetryCutBase::result(const PseudoJet & jet) const {
+ // construct the input jet (by default, recluster with C/A)
+ if (! jet.has_constituents()){
+ throw Error("RecursiveSymmetryCutBase can only be applied to jets with constituents");
+ }
+
+ PseudoJet j = _recluster_if_needed(jet);
+
+ // sanity check: the jet must have a valid CS
+ if (! j.has_valid_cluster_sequence()){
+ throw Error("RecursiveSymmetryCutBase can only be applied to jets associated to a (valid) cluster sequence");
+ }
+
+ // check that area information is there in case we have a subtractor
+ // GS: do we really need this since subtraction may not require areas?
+ if (_subtractor) {
+ const ClusterSequenceAreaBase * csab =
+ dynamic_cast<const ClusterSequenceAreaBase *>(j.associated_cs());
+ if (csab == 0 || (!csab->has_explicit_ghosts()))
+ _explicit_ghost_warning.warn("RecursiveSymmetryCutBase: there is no clustering sequence, or it lacks explicit ghosts: subtraction is not guaranteed to function properly");
+ }
+
+ // establish the first subjet and optionally subtract it
+ PseudoJet subjet = j;
+ if (_subtractor && (!_input_jet_is_subtracted)) {
+ subjet = (*_subtractor)(subjet);
+ }
+
+ // variables for tracking what will happen
+ PseudoJet piece1, piece2;
+
+ // vectors for storing optional verbose structure
+ // these hold the deltaR, symmetry, and mu values of dropped branches
+ std::vector<double> dropped_delta_R;
+ std::vector<double> dropped_symmetry;
+ std::vector<double> dropped_mu;
+
+ double sym, mu2;
+
+ // now recurse into the jet's structure
+ RecursionStatus status;
+ while ((status=recurse_one_step(subjet, piece1, piece2, sym, mu2)) != recursion_success) {
+ // start with sanity checks:
+ if ((status == recursion_issue) || (status == recursion_no_parents)) {
+ // we should return piece1 by our convention for recurse_one_step
+ PseudoJet result;
+ if (status == recursion_issue){
+ result = piece1;
+ if (_verbose) cout << "reached end; returning null jet " << endl;
+ } else {
+ result = _result_no_substructure(piece1);
+ if (_verbose) cout << "no parents found; returning last PJ or empty jet" << endl;
+ }
+
+ if (result != 0) {
+ // if in grooming mode, add dummy structure information
+ StructureType * structure = new StructureType(result);
+ // structure->_symmetry = 0.0;
+ // structure->_mu = 0.0;
+ // structure->_delta_R = 0.0;
+ if (_verbose_structure) { // still want to store verbose information about dropped branches
+ structure->_has_verbose = true;
+ structure->_dropped_symmetry = dropped_symmetry;
+ structure->_dropped_mu = dropped_mu;
+ structure->_dropped_delta_R = dropped_delta_R;
+ }
+ result.set_structure_shared_ptr(SharedPtr<PseudoJetStructureBase>(structure));
+ }
+
+ return result;
+ }
+
+ assert(status == recursion_dropped);
+
+ // if desired, store information about dropped branches before recursing
+ if (_verbose_structure) {
+ dropped_delta_R.push_back(piece1.delta_R(piece2));
+ dropped_symmetry.push_back(sym);
+ dropped_mu.push_back((mu2 >= 0) ? sqrt(mu2) : -sqrt(-mu2));
+ }
+
+ subjet = piece1;
+ }
+
+
+ // we've tagged the splitting, return the jet with its substructure
+ StructureType * structure = new StructureType(subjet);
+ structure->_symmetry = sym;
+ structure->_mu = (mu2 >= 0) ? sqrt(mu2) : -sqrt(-mu2);
+ structure->_delta_R = sqrt(squared_geometric_distance(piece1, piece2));
+ if (_verbose_structure) {
+ structure->_has_verbose = true;
+ structure->_dropped_symmetry = dropped_symmetry;
+ structure->_dropped_mu = dropped_mu;
+ structure->_dropped_delta_R = dropped_delta_R;
+ }
+ subjet.set_structure_shared_ptr(SharedPtr<PseudoJetStructureBase>(structure));
+ return subjet;
+}
+
+
+
+//----------------------------------------------------------------------
+// the method below is the one actually performing one step of the
+// recursion.
+//
+// It returns a status code (defined above)
+//
+// In case of success, all the information is filled
+// In case of "no parents", piee1 is the same subjet
+// In case of trouble, piece2 will be a 0 PJ and piece1 is the PJ we
+// should return (either 0 itself if the issue was critical, or
+// non-wero in case of a minor issue just causing the recursion to
+// stop)
+RecursiveSymmetryCutBase::RecursionStatus
+ RecursiveSymmetryCutBase::recurse_one_step(const PseudoJet & subjet,
+ PseudoJet &piece1, PseudoJet &piece2,
+ double &sym, double &mu2,
+ void *extra_parameters) const {
+ if (!subjet.has_parents(piece1, piece2)){
+ piece1 = subjet;
+ piece2 = PseudoJet();
+ return recursion_no_parents;
+ }
+
+ // first sanity check:
+ // - zero or negative pts are not allowed for the input subjet
+ // - zero or negative masses are not allowed for configurations
+ // in which the mass will effectively appear in a denominator
+ // (The masses will be checked later)
+ if (subjet.pt2() <= 0){ // this is a critical problem, return an empty PJ
+ piece1 = piece2 = PseudoJet();
+ return recursion_issue;
+ }
+
+ if (_subtractor) {
+ piece1 = (*_subtractor)(piece1);
+ piece2 = (*_subtractor)(piece2);
+ }
+
+ // determine the symmetry parameter
+ if (_symmetry_measure == y) {
+ // the original d_{ij}/m^2 choice from MDT
+ // first make sure the mass is sensible
+ if (subjet.m2() <= 0) {
+ _negative_mass_warning.warn("RecursiveSymmetryCutBase: cannot calculate y, because (sub)jet mass is negative; bailing out");
+ // since rounding errors can give -ve masses, be a it more
+ // tolerant and consider that no substructure has been found
+ piece1 = _result_no_substructure(subjet);
+ piece2 = PseudoJet();
+ return recursion_issue;
+ }
+ sym = piece1.kt_distance(piece2) / subjet.m2();
+
+ } else if (_symmetry_measure == vector_z) {
+ // min(pt1, pt2)/(pt), where the denominator is a vector sum
+ // of the two subjets
+ sym = min(piece1.pt(), piece2.pt()) / subjet.pt();
+ } else if (_symmetry_measure == scalar_z) {
+ // min(pt1, pt2)/(pt1+pt2), where the denominator is a scalar sum
+ // of the two subjets
+ double pt1 = piece1.pt();
+ double pt2 = piece2.pt();
+ // make sure denominator is non-zero
+ sym = pt1 + pt2;
+ if (sym == 0){ // this is a critical problem, return an empty PJ
+ piece1 = piece2 = PseudoJet();
+ return recursion_issue;
+ }
+ sym = min(pt1, pt2) / sym;
+ } else if ((_symmetry_measure == theta_E) || (_symmetry_measure == cos_theta_E)){
+ // min(E1, E2)/(E1+E2)
+ double E1 = piece1.E();
+ double E2 = piece2.E();
+ // make sure denominator is non-zero
+ sym = E1 + E2;
+ if (sym == 0){ // this is a critical problem, return an empty PJ
+ piece1 = piece2 = PseudoJet();
+ return recursion_issue;
+ }
+ sym = min(E1, E2) / sym;
+ } else {
+ throw Error ("Unrecognized choice of symmetry_measure");
+ }
+
+ // determine the symmetry cut
+ // (This function is specified in the derived classes)
+ double this_symmetry_cut = symmetry_cut_fn(piece1, piece2, extra_parameters);
+
+ // and make a first tagging decision based on symmetry cut
+ bool tagged = (sym > this_symmetry_cut);
+
+ // if tagged based on symmetry cut, then check the mu cut (if relevant)
+ // and update the tagging decision. Calculate mu^2 regardless, for cases
+ // of users not cutting on mu2, but still interested in its value.
+ bool use_mu_cut = (_mu_cut != numeric_limits<double>::infinity());
+ mu2 = max(piece1.m2(), piece2.m2())/subjet.m2();
+ if (tagged && use_mu_cut) {
+ // first a sanity check -- mu2 won't be sensible if the subjet mass
+ // is negative, so we can't then trust the mu cut - bail out
+ if (subjet.m2() <= 0) {
+ _negative_mass_warning.warn("RecursiveSymmetryCutBase: cannot trust mu, because (sub)jet mass is negative; bailing out");
+ piece1 = piece2 = PseudoJet();
+ return recursion_issue;
+ }
+ if (mu2 > 1) _mu2_gt1_warning.warn("RecursiveSymmetryCutBase encountered mu^2 value > 1");
+ if (mu2 > pow(_mu_cut,2)) tagged = false;
+ }
+
+ // we'll continue unclustering, allowing for the different
+ // ways of choosing which parent to look into
+ if (_recursion_choice == larger_pt) {
+ if (piece1.pt2() < piece2.pt2()) std::swap(piece1, piece2);
+ } else if (_recursion_choice == larger_mt) {
+ if (piece1.mt2() < piece2.mt2()) std::swap(piece1, piece2);
+ } else if (_recursion_choice == larger_m) {
+ if (piece1.m2() < piece2.m2()) std::swap(piece1, piece2);
+ } else if (_recursion_choice == larger_E) {
+ if (piece1.E() < piece2.E()) std::swap(piece1, piece2);
+ } else {
+ throw Error ("Unrecognized value for recursion_choice");
+ }
+
+ return tagged ? recursion_success : recursion_dropped;
+}
+
+
+//----------------------------------------------------------------------
+string RecursiveSymmetryCutBase::description() const {
+ ostringstream ostr;
+ ostr << "Recursive " << (_grooming_mode ? "Groomer" : "Tagger") << " with a symmetry cut ";
+
+ switch(_symmetry_measure) {
+ case y:
+ ostr << "y"; break;
+ case scalar_z:
+ ostr << "scalar_z"; break;
+ case vector_z:
+ ostr << "vector_z"; break;
+ case theta_E:
+ ostr << "theta_E"; break;
+ case cos_theta_E:
+ ostr << "cos_theta_E"; break;
+ default:
+ cerr << "failed to interpret symmetry_measure" << endl; exit(-1);
+ }
+ ostr << " > " << symmetry_cut_description();
+
+ if (_mu_cut != numeric_limits<double>::infinity()) {
+ ostr << ", mass-drop cut mu=max(m1,m2)/m < " << _mu_cut;
+ } else {
+ ostr << ", no mass-drop requirement";
+ }
+
+ ostr << ", recursion into the subjet with larger ";
+ switch(_recursion_choice) {
+ case larger_pt:
+ ostr << "pt"; break;
+ case larger_mt:
+ ostr << "mt(=sqrt(m^2+pt^2))"; break;
+ case larger_m:
+ ostr << "mass"; break;
+ case larger_E:
+ ostr << "energy"; break;
+ default:
+ cerr << "failed to interpret recursion_choice" << endl; exit(-1);
+ }
+
+ if (_subtractor) {
+ ostr << ", subtractor: " << _subtractor->description();
+ if (_input_jet_is_subtracted) {ostr << " (input jet is assumed already subtracted)";}
+ }
+
+ if (_recluster) {
+ ostr << " and reclustering using " << _recluster->description();
+ }
+
+ return ostr.str();
+}
+
+//----------------------------------------------------------------------
+// helper for handling the reclustering
+PseudoJet RecursiveSymmetryCutBase::_recluster_if_needed(const PseudoJet &jet) const{
+ if (! _do_reclustering) return jet;
+ if (_recluster) return (*_recluster)(jet);
+ if (is_ee()){
+#if FASTJET_VERSION_NUMBER >= 30100
+ return Recluster(JetDefinition(ee_genkt_algorithm, JetDefinition::max_allowable_R, 0.0), true)(jet);
+#else
+ return Recluster(JetDefinition(ee_genkt_algorithm, JetDefinition::max_allowable_R, 0.0))(jet);
+#endif
+ }
+
+ return Recluster(cambridge_algorithm, JetDefinition::max_allowable_R)(jet);
+}
+
+//----------------------------------------------------------------------
+// decide what to return when no substructure has been found
+double RecursiveSymmetryCutBase::squared_geometric_distance(const PseudoJet &j1,
+ const PseudoJet &j2) const{
+ if (_symmetry_measure == theta_E){
+ double dot_3d = j1.px()*j2.px() + j1.py()*j2.py() + j1.pz()*j2.pz();
+ double cos_theta = max(-1.0,min(1.0, dot_3d/sqrt(j1.modp2()*j2.modp2())));
+ double theta = acos(cos_theta);
+ return theta*theta;
+ } else if (_symmetry_measure == cos_theta_E){
+ double dot_3d = j1.px()*j2.px() + j1.py()*j2.py() + j1.pz()*j2.pz();
+ return max(0.0, 2*(1-dot_3d/sqrt(j1.modp2()*j2.modp2())));
+ }
+
+ return j1.squared_distance(j2);
+}
+
+//----------------------------------------------------------------------
+PseudoJet RecursiveSymmetryCutBase::_result_no_substructure(const PseudoJet &last_parent) const{
+ if (_grooming_mode){
+ // in grooming mode, return the last parent
+ return last_parent;
+ } else {
+ // in tagging mode, return an empty PseudoJet
+ return PseudoJet();
+ }
+}
+
+
+//========================================================================
+// implementation of the details of the structure
+
+// the number of dropped subjets
+int RecursiveSymmetryCutBase::StructureType::dropped_count(bool global) const {
+ check_verbose("dropped_count()");
+
+ // if this jet has no substructure, just return an empty vector
+ if (!has_substructure()) return _dropped_delta_R.size();
+
+ // deal with the non-global case
+ if (!global) return _dropped_delta_R.size();
+
+ // for the global case, we've unfolded the recursion (likely more
+ // efficient as it requires less copying)
+ unsigned int count = 0;
+ vector<const RecursiveSymmetryCutBase::StructureType*> to_parse;
+ to_parse.push_back(this);
+
+ unsigned int i_parse = 0;
+ while (i_parse<to_parse.size()){
+ const RecursiveSymmetryCutBase::StructureType *current = to_parse[i_parse];
+ count += current->_dropped_delta_R.size();
+
+ // check if we need to recurse deeper in the substructure
+ //
+ // we can have 2 situations here for the underlying structure (the
+ // one we've wrapped around):
+ // - it's of the clustering type
+ // - it's a composite jet
+ // only in the 2nd case do we have to recurse deeper
+ const CompositeJetStructure *css = dynamic_cast<const CompositeJetStructure*>(current->_structure.get());
+ if (css == 0){ ++i_parse; continue; }
+
+ vector<PseudoJet> prongs = css->pieces(PseudoJet()); // argument irrelevant
+ assert(prongs.size() == 2);
+ for (unsigned int i_prong=0; i_prong<2; ++i_prong){
+ if (prongs[i_prong].has_structure_of<RecursiveSymmetryCutBase>()){
+ RecursiveSymmetryCutBase::StructureType* prong_structure
+ = (RecursiveSymmetryCutBase::StructureType*) prongs[i_prong].structure_ptr();
+ if (prong_structure->has_substructure())
+ to_parse.push_back(prong_structure);
+ }
+ }
+
+ ++i_parse;
+ }
+ return count;
+}
+
+// the delta_R of all the dropped subjets
+vector<double> RecursiveSymmetryCutBase::StructureType::dropped_delta_R(bool global) const {
+ check_verbose("dropped_delta_R()");
+
+ // if this jet has no substructure, just return an empty vector
+ if (!has_substructure()) return vector<double>();
+
+ // deal with the non-global case
+ if (!global) return _dropped_delta_R;
+
+ // for the global case, we've unfolded the recursion (likely more
+ // efficient as it requires less copying)
+ vector<double> all_dropped;
+ vector<const RecursiveSymmetryCutBase::StructureType*> to_parse;
+ to_parse.push_back(this);
+
+ unsigned int i_parse = 0;
+ while (i_parse<to_parse.size()){
+ const RecursiveSymmetryCutBase::StructureType *current = to_parse[i_parse];
+ all_dropped.insert(all_dropped.end(), current->_dropped_delta_R.begin(), current->_dropped_delta_R.end());
+
+ // check if we need to recurse deeper in the substructure
+ //
+ // we can have 2 situations here for the underlying structure (the
+ // one we've wrapped around):
+ // - it's of the clustering type
+ // - it's a composite jet
+ // only in the 2nd case do we have to recurse deeper
+ const CompositeJetStructure *css = dynamic_cast<const CompositeJetStructure*>(current->_structure.get());
+ if (css == 0){ ++i_parse; continue; }
+
+ vector<PseudoJet> prongs = css->pieces(PseudoJet()); // argument irrelevant
+ assert(prongs.size() == 2);
+ for (unsigned int i_prong=0; i_prong<2; ++i_prong){
+ if (prongs[i_prong].has_structure_of<RecursiveSymmetryCutBase>()){
+ RecursiveSymmetryCutBase::StructureType* prong_structure
+ = (RecursiveSymmetryCutBase::StructureType*) prongs[i_prong].structure_ptr();
+ if (prong_structure->has_substructure())
+ to_parse.push_back(prong_structure);
+ }
+ }
+
+ ++i_parse;
+ }
+ return all_dropped;
+}
+
+// the symmetry of all the dropped subjets
+vector<double> RecursiveSymmetryCutBase::StructureType::dropped_symmetry(bool global) const {
+ check_verbose("dropped_symmetry()");
+
+ // if this jet has no substructure, just return an empty vector
+ if (!has_substructure()) return vector<double>();
+
+ // deal with the non-global case
+ if (!global) return _dropped_symmetry;
+
+ // for the global case, we've unfolded the recursion (likely more
+ // efficient as it requires less copying)
+ vector<double> all_dropped;
+ vector<const RecursiveSymmetryCutBase::StructureType*> to_parse;
+ to_parse.push_back(this);
+
+ unsigned int i_parse = 0;
+ while (i_parse<to_parse.size()){
+ const RecursiveSymmetryCutBase::StructureType *current = to_parse[i_parse];
+ all_dropped.insert(all_dropped.end(), current->_dropped_symmetry.begin(), current->_dropped_symmetry.end());
+
+ // check if we need to recurse deeper in the substructure
+ //
+ // we can have 2 situations here for the underlying structure (the
+ // one we've wrapped around):
+ // - it's of the clustering type
+ // - it's a composite jet
+ // only in the 2nd case do we have to recurse deeper
+ const CompositeJetStructure *css = dynamic_cast<const CompositeJetStructure*>(current->_structure.get());
+ if (css == 0){ ++i_parse; continue; }
+
+ vector<PseudoJet> prongs = css->pieces(PseudoJet()); // argument irrelevant
+ assert(prongs.size() == 2);
+ for (unsigned int i_prong=0; i_prong<2; ++i_prong){
+ if (prongs[i_prong].has_structure_of<RecursiveSymmetryCutBase>()){
+ RecursiveSymmetryCutBase::StructureType* prong_structure
+ = (RecursiveSymmetryCutBase::StructureType*) prongs[i_prong].structure_ptr();
+ if (prong_structure->has_substructure())
+ to_parse.push_back(prong_structure);
+ }
+ }
+
+ ++i_parse;
+ }
+ return all_dropped;
+}
+
+// the mu of all the dropped subjets
+vector<double> RecursiveSymmetryCutBase::StructureType::dropped_mu(bool global) const {
+ check_verbose("dropped_mu()");
+
+ // if this jet has no substructure, just return an empty vector
+ if (!has_substructure()) return vector<double>();
+
+ // deal with the non-global case
+ if (!global) return _dropped_mu;
+
+ // for the global case, we've unfolded the recursion (likely more
+ // efficient as it requires less copying)
+ vector<double> all_dropped;
+ vector<const RecursiveSymmetryCutBase::StructureType*> to_parse;
+ to_parse.push_back(this);
+
+ unsigned int i_parse = 0;
+ while (i_parse<to_parse.size()){
+ const RecursiveSymmetryCutBase::StructureType *current = to_parse[i_parse];
+ all_dropped.insert(all_dropped.end(), current->_dropped_mu.begin(), current->_dropped_mu.end());
+
+ // check if we need to recurse deeper in the substructure
+ //
+ // we can have 2 situations here for the underlying structure (the
+ // one we've wrapped around):
+ // - it's of the clustering type
+ // - it's a composite jet
+ // only in the 2nd case do we have to recurse deeper
+ const CompositeJetStructure *css = dynamic_cast<const CompositeJetStructure*>(current->_structure.get());
+ if (css == 0){ ++i_parse; continue; }
+
+ vector<PseudoJet> prongs = css->pieces(PseudoJet()); // argument irrelevant
+ assert(prongs.size() == 2);
+ for (unsigned int i_prong=0; i_prong<2; ++i_prong){
+ if (prongs[i_prong].has_structure_of<RecursiveSymmetryCutBase>()){
+ RecursiveSymmetryCutBase::StructureType* prong_structure
+ = (RecursiveSymmetryCutBase::StructureType*) prongs[i_prong].structure_ptr();
+ if (prong_structure->has_substructure())
+ to_parse.push_back(prong_structure);
+ }
+ }
+
+ ++i_parse;
+ }
+ return all_dropped;
+}
+
+// the maximum of the symmetry over the dropped subjets
+double RecursiveSymmetryCutBase::StructureType::max_dropped_symmetry(bool global) const {
+ check_verbose("max_dropped_symmetry()");
+
+ // if there is no substructure, just exit
+ if (!has_substructure()){ return 0.0; }
+
+ // local value of the max_dropped_symmetry
+ double local_max = (_dropped_symmetry.size() == 0)
+ ? 0.0 : *max_element(_dropped_symmetry.begin(),_dropped_symmetry.end());
+
+ // recurse down the structure if instructed to do so
+ if (global){
+ // we can have 2 situations here for the underlying structure (the
+ // one we've wrapped around):
+ // - it's of the clustering type
+ // - it's a composite jet
+ // only in the 2nd case do we have to recurse deeper
+ const CompositeJetStructure *css = dynamic_cast<const CompositeJetStructure*>(_structure.get());
+ if (css == 0) return local_max;
+
+ vector<PseudoJet> prongs = css->pieces(PseudoJet()); // argument irrelevant
+ assert(prongs.size() == 2);
+ for (unsigned int i_prong=0; i_prong<2; ++i_prong){
+ // check if the prong has further substructure
+ if (prongs[i_prong].has_structure_of<RecursiveSymmetryCutBase>()){
+ RecursiveSymmetryCutBase::StructureType* prong_structure
+ = (RecursiveSymmetryCutBase::StructureType*) prongs[i_prong].structure_ptr();
+ local_max = max(local_max, prong_structure->max_dropped_symmetry(true));
+ }
+ }
+ }
+
+ return local_max;
+}
+
+//------------------------------------------------------------------------
+// helper class to sort by decreasing thetag
+class SortRecursiveSoftDropStructureZgThetagPair{
+public:
+ bool operator()(const pair<double, double> &p1, const pair<double, double> &p2) const{
+ return p1.second > p2.second;
+ }
+};
+//------------------------------------------------------------------------
+
+// the (zg,thetag) pairs of all the splitting that were found and passed the SD condition
+vector<pair<double,double> > RecursiveSymmetryCutBase::StructureType::sorted_zg_and_thetag() const {
+ //check_verbose("sorted_zg_and_thetag()");
+
+ // if this jet has no substructure, just return an empty vector
+ if (!has_substructure()) return vector<pair<double,double> >();
+
+ // otherwise fill a vector with all the prongs (no specific ordering)
+ vector<pair<double,double> > all;
+ vector<const RecursiveSymmetryCutBase::StructureType*> to_parse;
+ to_parse.push_back(this);
+
+ unsigned int i_parse = 0;
+ while (i_parse<to_parse.size()){
+ const RecursiveSymmetryCutBase::StructureType *current = to_parse[i_parse];
+ all.push_back(pair<double,double>(current->_symmetry, current->_delta_R));
+
+ vector<PseudoJet> prongs = current->pieces(PseudoJet());
+ assert(prongs.size() == 2);
+ for (unsigned int i_prong=0; i_prong<2; ++i_prong){
+ if (prongs[i_prong].has_structure_of<RecursiveSymmetryCutBase>()){
+ RecursiveSymmetryCutBase::StructureType* prong_structure
+ = (RecursiveSymmetryCutBase::StructureType*) prongs[i_prong].structure_ptr();
+ if (prong_structure->has_substructure())
+ to_parse.push_back(prong_structure);
+ }
+ }
+
+ ++i_parse;
+ }
+
+ sort(all.begin(), all.end(), SortRecursiveSoftDropStructureZgThetagPair());
+ return all;
+}
+
+ } } // namespace contrib
+
+ //FASTJET_END_NAMESPACE
diff --git a/src/Tools/fjcontrib/RecursiveTools/SoftDrop.cc b/src/Tools/fjcontrib/RecursiveTools/SoftDrop.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/SoftDrop.cc
@@ -0,0 +1,78 @@
+// $Id: SoftDrop.cc 1059 2017-09-07 20:48:00Z gsoyez $
+//
+// Copyright (c) 2014-, Gregory Soyez, Jesse. Thaler
+// based on arXiv:1402.2657 by Andrew J. Larkoski, Simone Marzani,
+// Gregory Soyez, Jesse Thaler
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include "SoftDrop.hh"
+#include <cmath>
+#include <sstream>
+
+using namespace std;
+
+//FASTJET_BEGIN_NAMESPACE // defined in fastjet/internal/base.hh
+
+ //namespace contrib{
+
+ namespace Rivet{
+ namespace fjcontrib{
+
+
+//----------------------------------------------------------------------
+// TODO:
+//
+// - implement reclustering (at the moment we assume it's C/A as for mMDT
+//
+// - what is returned if no substructure is found? [and for negativeve
+// pt, m2 or other situations where mMDT currentlty returns an empty
+// PseudoJet]
+//
+// GS.: mMDT seeks substructure so it makes sense for it to return
+// an empry PseudoJet when no substructure is found (+ it is the
+// original behaviour). For SoftDrop, in grooming mode (beta>0), if
+// would make sense to return a jet with a single particle. In
+// tagging mode (beta<0), the situation is less clear. At the level
+// of the implementation, having a virtual function could work
+// (with a bit of care to cover the -ve pt or m2 cases)
+//
+// - Do we include Andrew and Simone in the "contrib-author" list
+// since they are on the paper? Do we include Gavin in the author's
+// list since he started this contrib?
+//
+//----------------------------------------------------------------------
+
+//----------------------------------------------------------------------
+double SoftDrop::symmetry_cut_fn(const PseudoJet & p1,
+ const PseudoJet & p2,
+ void *optional_R0sqr_ptr) const{
+ double R0sqr = (optional_R0sqr_ptr == 0) ? _R0sqr : *((double*) optional_R0sqr_ptr);
+ return _symmetry_cut * pow(squared_geometric_distance(p1,p2)/R0sqr, 0.5*_beta);
+}
+
+//----------------------------------------------------------------------
+string SoftDrop::symmetry_cut_description() const {
+ ostringstream ostr;
+ ostr << _symmetry_cut << " (theta/" << sqrt(_R0sqr) << ")^" << _beta << " [SoftDrop]";
+ return ostr.str();
+}
+
+ } } // namespace contrib
+
+//FASTJET_END_NAMESPACE
diff --git a/src/Tools/fjcontrib/RecursiveTools/TODO b/src/Tools/fjcontrib/RecursiveTools/TODO
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/TODO
@@ -0,0 +1,26 @@
+For v2.0
+--------
+
+- CHECK: lines 100-102 of RecursiveSymmetryCutBase.hh: this was
+ initially setting the structure members to 0. I think it's highly
+ preferable to set them to their default of -1, signalling the
+ absence of substructure. [0 dR might happen with a perfectly
+ collinear splitting]
+
+- CHECK: are we happy with how the structure info is stored and the
+ recursive_soft_drop_prongs(...) function in RecursiveSoftDrop.hh?
+
+- QUESTION: do we move set_min_deltaR_squared in the base class?
+
+- Add option to define z wrt to original jet?
+
+For future releases?
+--------------------
+- JDT: In Recluster, change "single" to an enum for user clarity?
+ [do we have any other option that "sungle" or "subjets"]
+- JDT: Should we have a FASTJET_CONTRIB_BEGIN_NAMESPACE? It would
+ help those of us who use XCode to edit, which is aggressive about
+ auto-indenting. [Consider this for the full contrib??]
+- More generic kinematic cuts?
+- KZ: common base class for IteratedSoftDrop and RecursiveSoftDrop?
+- KZ: make IteratedSoftDrop use Recluster
\ No newline at end of file
diff --git a/src/Tools/fjcontrib/RecursiveTools/VERSION b/src/Tools/fjcontrib/RecursiveTools/VERSION
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/VERSION
@@ -0,0 +1,1 @@
+2.0.0-beta2
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_advanced_usage.cc b/src/Tools/fjcontrib/RecursiveTools/example_advanced_usage.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_advanced_usage.cc
@@ -0,0 +1,362 @@
+//----------------------------------------------------------------------
+/// \file example_advanced_usage.cc
+///
+/// This example program is meant to illustrate some advanced features
+/// of the fastjet::contrib::SoftDrop class is used.
+///
+/// Run this example with
+///
+/// \verbatim
+/// ./example_advanced_usage < ../data/single-event.dat
+/// \endverbatim
+//----------------------------------------------------------------------
+
+// $Id: example_advanced_usage.cc 1016 2017-04-20 16:51:52Z knzhou $
+//
+// Copyright (c) 2014, Gavin P. Salam
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iostream>
+#include <sstream>
+
+#include <sstream>
+#include <iomanip>
+#include <cmath>
+#include "fastjet/ClusterSequence.hh"
+#include "SoftDrop.hh" // In external code, this should be fastjet/contrib/SoftDrop.hh
+
+#define MY_INF std::numeric_limits<double>::infinity()
+
+using namespace std;
+using namespace fastjet;
+using namespace fastjet::contrib;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &event);
+ostream & operator<<(ostream &, const PseudoJet &);
+
+// Simple class to store SoftDrop objects along with display information
+class SoftDropStruct {
+
+private:
+ string _name;
+ double _beta;
+ double _z_cut;
+ SoftDrop::SymmetryMeasure _symmetry_measure;
+ double _R0;
+ double _mu; //mass drop
+ SoftDrop::RecursionChoice _recursion_choice;
+ JetAlgorithm _recluster_algorithm;
+ bool _tagging_mode;
+ SoftDrop _soft_drop;
+ Recluster _reclusterer;
+
+public:
+ SoftDropStruct(string name,
+ double beta,
+ double z_cut,
+ SoftDrop::SymmetryMeasure symmetry_measure,
+ double R0,
+ double mu,
+ SoftDrop::RecursionChoice recursion_choice,
+ JetAlgorithm recluster_algorithm,
+ bool tagging_mode = false)
+ : _name(name),
+ _beta(beta),
+ _z_cut(z_cut),
+ _symmetry_measure(symmetry_measure),
+ _R0(R0),
+ _mu(mu),
+ _recursion_choice(recursion_choice),
+ _recluster_algorithm(recluster_algorithm),
+ _tagging_mode(tagging_mode),
+ _soft_drop(beta,z_cut,symmetry_measure,R0,mu,recursion_choice),
+ _reclusterer(recluster_algorithm,JetDefinition::max_allowable_R)
+ {
+ // no need to recluser if already CA algorithm
+ if (recluster_algorithm != cambridge_algorithm) {
+ _soft_drop.set_reclustering(true,&_reclusterer);
+ }
+
+ // if beta is negative, typically want to use in tagging mode
+ // MMDT behavior is also tagging mode
+ // set this option here
+ if (tagging_mode) {
+ _soft_drop.set_tagging_mode();
+ }
+
+ //turn verbose structure on (off by default)
+ _soft_drop.set_verbose_structure();
+ }
+
+ const SoftDrop& soft_drop() const { return _soft_drop;}
+ string name() const { return _name;}
+ double beta() const { return _beta;}
+ double z_cut() const { return _z_cut;}
+ string symmetry_measure_name() const {
+ switch (_symmetry_measure) {
+ case SoftDrop::scalar_z:
+ return "scalar_z";
+ case SoftDrop::vector_z:
+ return "vector_z";
+ case SoftDrop::y:
+ return "y";
+ default:
+ return "unknown";
+ }
+ }
+ double R0() const { return _R0;}
+ double mu() const { return _mu;}
+
+ string recursion_choice_name() const {
+ switch (_recursion_choice) {
+ case SoftDrop::larger_pt:
+ return "larger_pt";
+ case SoftDrop::larger_mt:
+ return "larger_mt";
+ case SoftDrop::larger_m:
+ return "larger_m";
+ default:
+ return "unknown";
+ }
+ }
+
+ string reclustering_name() const {
+ switch (_recluster_algorithm) {
+ case kt_algorithm:
+ return "KT";
+ case cambridge_algorithm:
+ return "CA";
+ default:
+ return "unknown";
+ }
+ }
+
+ string tag_or_groom() const {
+ return (_tagging_mode ? "tag" : "groom");
+ }
+
+};
+
+
+//----------------------------------------------------------------------
+int main(){
+
+ //----------------------------------------------------------
+ // read in input particles
+ vector<PseudoJet> event;
+ read_event(event);
+ cout << "# read an event with " << event.size() << " particles" << endl;
+
+ // first get some anti-kt jets
+ double R = 1.0, ptmin = 20.0;
+ JetDefinition jet_def(antikt_algorithm, R);
+ ClusterSequence cs(event, jet_def);
+ vector<PseudoJet> jets = sorted_by_pt(cs.inclusive_jets(ptmin));
+
+
+ //----------------------------------------------------------
+ // Make vector of structs to store a bunch of different SoftDrop options
+ // This is a vector of pointers because SoftDropStruct doesn't
+ // have a valid copy constructor
+ vector<SoftDropStruct *> sd_vec;
+
+ // make some standard SoftDrop
+ sd_vec.push_back(new SoftDropStruct("beta=2.0 zcut=.1", 2.0,0.10,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("beta=1.0 zcut=.1", 1.0,0.10,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("beta=0.5 zcut=.1", 0.5,0.10,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("beta=2.0 zcut=.2", 2.0,0.20,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("beta=1.0 zcut=.2", 1.0,0.20,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("beta=0.5 zcut=.2", 0.5,0.20,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+
+ // make a mMDT-like tagger using SoftDrop
+ sd_vec.push_back(new SoftDropStruct("MMDT-like zcut=.1", 0.0,0.10,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm,true));
+ sd_vec.push_back(new SoftDropStruct("MMDT-like zcut=.2", 0.0,0.20,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm,true));
+ sd_vec.push_back(new SoftDropStruct("MMDT-like zcut=.3", 0.0,0.30,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm,true));
+ sd_vec.push_back(new SoftDropStruct("MMDT-like zcut=.4", 0.0,0.40,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm,true));
+
+ // make some tagging SoftDrop (negative beta)
+ sd_vec.push_back(new SoftDropStruct("beta=-2.0 zcut=.05", -2.0,0.05,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm,true));
+ sd_vec.push_back(new SoftDropStruct("beta=-1.0 zcut=.05", -1.0,0.05,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm,true));
+ sd_vec.push_back(new SoftDropStruct("beta=-0.5 zcut=.05", -0.5,0.05,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm,true));
+
+ // make a SoftDrop with R0 parameter
+ sd_vec.push_back(new SoftDropStruct("b=.5 z=.3 R0=1.0", 0.5,0.30,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=.5 z=.3 R0=0.5", 0.5,0.30,SoftDrop::scalar_z,0.5,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=.5 z=.3 R0=0.2", 0.5,0.30,SoftDrop::scalar_z,0.2,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+
+ // make a SoftDrop with different symmetry measure
+ sd_vec.push_back(new SoftDropStruct("b=2 z=.4 scalar_z", 2.0,0.4,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=2 z=.4 vector_z", 2.0,0.4,SoftDrop::vector_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=2 z=.4 y", 2.0,0.4,SoftDrop::y, 1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+
+ // make a SoftDrop with different recursion choice
+ sd_vec.push_back(new SoftDropStruct("b=3 z=.2 larger_pt", 3.0,0.20,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=3 z=.2 larger_mt", 3.0,0.20,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_mt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=3 z=.2 larger_m", 3.0,0.20,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_m,cambridge_algorithm));
+
+ // make a SoftDrop with mass drop
+ sd_vec.push_back(new SoftDropStruct("b=2 z=.1 mu=1.0", 2.0,0.10,SoftDrop::scalar_z,1.0,1.0,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=2 z=.1 mu=0.8", 2.0,0.10,SoftDrop::scalar_z,1.0,0.8,SoftDrop::larger_pt,cambridge_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=2 z=.1 mu=0.5", 2.0,0.10,SoftDrop::scalar_z,1.0,0.5,SoftDrop::larger_pt,cambridge_algorithm));
+
+ // make a SoftDrop with a different clustering scheme (kT instead of default CA)
+ sd_vec.push_back(new SoftDropStruct("b=2.0 z=.2 kT", 2.0,0.20,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,kt_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=1.0 z=.2 kT", 1.0,0.20,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,kt_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=0.5 z=.2 kT", 0.5,0.20,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,kt_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=2.0 z=.4 kT", 2.0,0.40,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,kt_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=1.0 z=.4 kT", 1.0,0.40,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,kt_algorithm));
+ sd_vec.push_back(new SoftDropStruct("b=0.5 z=.4 kT", 0.5,0.40,SoftDrop::scalar_z,1.0,MY_INF,SoftDrop::larger_pt,kt_algorithm));
+
+ //----------------------------------------------------------
+ // Output information about the various Soft Drop algorithms
+
+
+ // header lines
+ cout << "---------------------------------------------------------------------------------------------" << endl;
+ cout << "Soft Drops to be tested:" << endl;
+ cout << "---------------------------------------------------------------------------------------------" << endl;
+ cout << std::setw(18) << "name"
+ << std::setw(8) << "beta"
+ << std::setw(8) << "z_cut"
+ << std::setw(9) << "sym"
+ << std::setw(8) << "R0"
+ << std::setw(8) << "mu"
+ << std::setw(10)<< "recurse"
+ << std::setw(8) << "reclust"
+ << std::setw(8) << "mode"
+ << endl;
+
+ // set precision for display
+ cout << setprecision(3) << fixed;
+
+ // line for each SoftDrop
+ for (unsigned i_sd = 0; i_sd < sd_vec.size(); i_sd++) {
+ cout << std::setw(18) << sd_vec[i_sd]->name()
+ << std::setw(8) << sd_vec[i_sd]->beta()
+ << std::setw(8) << sd_vec[i_sd]->z_cut()
+ << std::setw(9) << sd_vec[i_sd]->symmetry_measure_name()
+ << std::setw(8) << sd_vec[i_sd]->R0()
+ << std::setw(8) << sd_vec[i_sd]->mu()
+ << std::setw(10)<< sd_vec[i_sd]->recursion_choice_name()
+ << std::setw(8) << sd_vec[i_sd]->reclustering_name()
+ << std::setw(8) << sd_vec[i_sd]->tag_or_groom()
+ << endl;
+ }
+ cout << "---------------------------------------------------------------------------------------------" << endl;
+
+
+
+ for (unsigned ijet = 0; ijet < jets.size(); ijet++) {
+
+ cout << "---------------------------------------------------------------------------------------------" << endl;
+ cout << "Analyzing Jet " << ijet + 1 << ":" << endl;
+ cout << "---------------------------------------------------------------------------------------------" << endl;
+
+ cout << std::setw(18) << "name"
+ << std::setw(10) << "pt"
+ << std::setw(9) << "m"
+ << std::setw(8) << "y"
+ << std::setw(8) << "phi"
+ << std::setw(8) << "constit"
+ << std::setw(8) << "delta_R"
+ << std::setw(8) << "sym"
+ << std::setw(8) << "mu"
+ << std::setw(8) << "mxdropz" // max_dropped_z from verbose logging
+
+ << endl;
+
+ PseudoJet original_jet = jets[ijet];
+
+ // set precision for display
+ cout << setprecision(4) << fixed;
+
+ cout << std::setw(18) << "Original Jet"
+ << std::setw(10) << original_jet.pt()
+ << std::setw(9) << original_jet.m()
+ << std::setw(8) << original_jet.rap()
+ << std::setw(8) << original_jet.phi()
+ << std::setw(8) << original_jet.constituents().size()
+ << endl;
+
+ for (unsigned i_sd = 0; i_sd < sd_vec.size(); i_sd++) {
+ // the current Soft Drop
+ const SoftDrop & sd = (*sd_vec[i_sd]).soft_drop();
+ PseudoJet sd_jet = sd(jets[ijet]);
+
+ cout << std::setw(18) << sd_vec[i_sd]->name();
+ if (sd_jet != 0.0) {
+ cout << std::setw(10) << sd_jet.pt()
+ << std::setw(9) << sd_jet.m()
+ << std::setw(8) << sd_jet.rap()
+ << std::setw(8) << sd_jet.phi()
+ << std::setw(8) << sd_jet.constituents().size()
+ << std::setw(8) << sd_jet.structure_of<contrib::SoftDrop>().delta_R()
+ << std::setw(8) << sd_jet.structure_of<contrib::SoftDrop>().symmetry()
+ << std::setw(8) << sd_jet.structure_of<contrib::SoftDrop>().mu()
+ // the next line is part of the verbose information that is off by default
+ << std::setw(8) << sd_jet.structure_of<contrib::SoftDrop>().max_dropped_symmetry();
+ } else {
+ cout << " ---- untagged jet ----";
+ }
+ cout << endl;
+
+ }
+ }
+
+ // clean up
+ for (unsigned i_sd = 0; i_sd < sd_vec.size(); i_sd++) {
+ delete sd_vec[i_sd];
+ }
+
+ return 0;
+}
+
+//----------------------------------------------------------------------
+/// read in input particles
+void read_event(vector<PseudoJet> &event){
+ string line;
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {return;}
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ event.push_back(particle);
+ }
+}
+
+//----------------------------------------------------------------------
+/// overloaded jet info output
+ostream & operator<<(ostream & ostr, const PseudoJet & jet) {
+ if (jet == 0) {
+ ostr << " 0 ";
+ } else {
+ ostr << " pt = " << jet.pt()
+ << " m = " << jet.m()
+ << " y = " << jet.rap()
+ << " phi = " << jet.phi();
+ }
+ return ostr;
+}
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_advanced_usage.ref b/src/Tools/fjcontrib/RecursiveTools/example_advanced_usage.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_advanced_usage.ref
@@ -0,0 +1,144 @@
+---------------------------------------------------------------------------------------------
+Soft Drops to be tested:
+---------------------------------------------------------------------------------------------
+ name beta z_cut sym R0 mu recurse reclust mode
+ beta=2.0 zcut=.1 2.000 0.100 scalar_z 1.000 inf larger_pt CA groom
+ beta=1.0 zcut=.1 1.000 0.100 scalar_z 1.000 inf larger_pt CA groom
+ beta=0.5 zcut=.1 0.500 0.100 scalar_z 1.000 inf larger_pt CA groom
+ beta=2.0 zcut=.2 2.000 0.200 scalar_z 1.000 inf larger_pt CA groom
+ beta=1.0 zcut=.2 1.000 0.200 scalar_z 1.000 inf larger_pt CA groom
+ beta=0.5 zcut=.2 0.500 0.200 scalar_z 1.000 inf larger_pt CA groom
+ MMDT-like zcut=.1 0.000 0.100 scalar_z 1.000 inf larger_pt CA tag
+ MMDT-like zcut=.2 0.000 0.200 scalar_z 1.000 inf larger_pt CA tag
+ MMDT-like zcut=.3 0.000 0.300 scalar_z 1.000 inf larger_pt CA tag
+ MMDT-like zcut=.4 0.000 0.400 scalar_z 1.000 inf larger_pt CA tag
+beta=-2.0 zcut=.05 -2.000 0.050 scalar_z 1.000 inf larger_pt CA tag
+beta=-1.0 zcut=.05 -1.000 0.050 scalar_z 1.000 inf larger_pt CA tag
+beta=-0.5 zcut=.05 -0.500 0.050 scalar_z 1.000 inf larger_pt CA tag
+ b=.5 z=.3 R0=1.0 0.500 0.300 scalar_z 1.000 inf larger_pt CA groom
+ b=.5 z=.3 R0=0.5 0.500 0.300 scalar_z 0.500 inf larger_pt CA groom
+ b=.5 z=.3 R0=0.2 0.500 0.300 scalar_z 0.200 inf larger_pt CA groom
+ b=2 z=.4 scalar_z 2.000 0.400 scalar_z 1.000 inf larger_pt CA groom
+ b=2 z=.4 vector_z 2.000 0.400 vector_z 1.000 inf larger_pt CA groom
+ b=2 z=.4 y 2.000 0.400 y 1.000 inf larger_pt CA groom
+b=3 z=.2 larger_pt 3.000 0.200 scalar_z 1.000 inf larger_pt CA groom
+b=3 z=.2 larger_mt 3.000 0.200 scalar_z 1.000 inf larger_mt CA groom
+ b=3 z=.2 larger_m 3.000 0.200 scalar_z 1.000 inf larger_m CA groom
+ b=2 z=.1 mu=1.0 2.000 0.100 scalar_z 1.000 1.000 larger_pt CA groom
+ b=2 z=.1 mu=0.8 2.000 0.100 scalar_z 1.000 0.800 larger_pt CA groom
+ b=2 z=.1 mu=0.5 2.000 0.100 scalar_z 1.000 0.500 larger_pt CA groom
+ b=2.0 z=.2 kT 2.000 0.200 scalar_z 1.000 inf larger_pt KT groom
+ b=1.0 z=.2 kT 1.000 0.200 scalar_z 1.000 inf larger_pt KT groom
+ b=0.5 z=.2 kT 0.500 0.200 scalar_z 1.000 inf larger_pt KT groom
+ b=2.0 z=.4 kT 2.000 0.400 scalar_z 1.000 inf larger_pt KT groom
+ b=1.0 z=.4 kT 1.000 0.400 scalar_z 1.000 inf larger_pt KT groom
+ b=0.5 z=.4 kT 0.500 0.400 scalar_z 1.000 inf larger_pt KT groom
+---------------------------------------------------------------------------------------------
+---------------------------------------------------------------------------------------------
+Analyzing Jet 1:
+---------------------------------------------------------------------------------------------
+ name pt m y phi constit delta_R sym mu mxdropz
+ Original Jet 983.3873 39.9912 -0.8673 2.9051 35
+ beta=2.0 zcut=.1 980.4398 27.1382 -0.8675 2.9053 25 0.2092 0.0047 0.8353 0.0014
+ beta=1.0 zcut=.1 971.5229 20.8426 -0.8686 2.9051 22 0.0954 0.0294 0.5476 0.0047
+ beta=0.5 zcut=.1 933.8859 9.9073 -0.8697 2.9075 13 0.0217 0.0174 0.8786 0.0294
+ beta=2.0 zcut=.2 975.8387 22.6675 -0.8684 2.9057 23 0.1316 0.0045 0.9195 0.0047
+ beta=1.0 zcut=.2 971.5229 20.8426 -0.8686 2.9051 22 0.0954 0.0294 0.5476 0.0047
+ beta=0.5 zcut=.2 917.6736 8.7048 -0.8696 2.9079 12 0.0200 0.1543 0.5576 0.0294
+ MMDT-like zcut=.1 917.6736 8.7048 -0.8696 2.9079 12 0.0200 0.1543 0.5576 0.0294
+ MMDT-like zcut=.2 669.6354 1.9839 -0.8677 2.9075 4 0.0044 0.2031 0.7051 0.1543
+ MMDT-like zcut=.3 446.5813 1.0182 -0.8678 2.9069 2 0.0030 0.4251 0.4848 0.2031
+ MMDT-like zcut=.4 446.5813 1.0182 -0.8678 2.9069 2 0.0030 0.4251 0.4848 0.2031
+beta=-2.0 zcut=.05 ---- untagged jet ----
+beta=-1.0 zcut=.05 ---- untagged jet ----
+beta=-0.5 zcut=.05 ---- untagged jet ----
+ b=.5 z=.3 R0=1.0 917.6736 8.7048 -0.8696 2.9079 12 0.0200 0.1543 0.5576 0.0294
+ b=.5 z=.3 R0=0.5 917.6736 8.7048 -0.8696 2.9079 12 0.0200 0.1543 0.5576 0.0294
+ b=.5 z=.3 R0=0.2 917.6736 8.7048 -0.8696 2.9079 12 0.0200 0.1543 0.5576 0.0294
+ b=2 z=.4 scalar_z 971.5229 20.8426 -0.8686 2.9051 22 0.0954 0.0294 0.5476 0.0047
+ b=2 z=.4 vector_z 971.5229 20.8426 -0.8686 2.9051 22 0.0954 0.0294 0.5476 0.0047
+ b=2 z=.4 y 971.5229 20.8426 -0.8686 2.9051 22 0.0954 0.0171 0.5476 0.0013
+b=3 z=.2 larger_pt 980.4398 27.1382 -0.8675 2.9053 25 0.2092 0.0047 0.8353 0.0014
+b=3 z=.2 larger_mt 980.4398 27.1382 -0.8675 2.9053 25 0.2092 0.0047 0.8353 0.0014
+ b=3 z=.2 larger_m 980.4398 27.1382 -0.8675 2.9053 25 0.2092 0.0047 0.8353 0.0014
+ b=2 z=.1 mu=1.0 980.4398 27.1382 -0.8675 2.9053 25 0.2092 0.0047 0.8353 0.0014
+ b=2 z=.1 mu=0.8 971.5229 20.8426 -0.8686 2.9051 22 0.0954 0.0294 0.5476 0.0047
+ b=2 z=.1 mu=0.5 446.5813 1.0182 -0.8678 2.9069 2 0.0030 0.4251 0.4848 0.2031
+ b=2.0 z=.2 kT 983.3873 39.9912 -0.8673 2.9051 35 0.1119 0.0377 0.5030 0.0000
+ b=1.0 z=.2 kT 983.3873 39.9912 -0.8673 2.9051 35 0.1119 0.0377 0.5030 0.0000
+ b=0.5 z=.2 kT 946.4934 20.1170 -0.8699 2.9084 21 0.0233 0.1579 0.5951 0.0377
+ b=2.0 z=.4 kT 983.3873 39.9912 -0.8673 2.9051 35 0.1119 0.0377 0.5030 0.0000
+ b=1.0 z=.4 kT 946.4934 20.1170 -0.8699 2.9084 21 0.0233 0.1579 0.5951 0.0377
+ b=0.5 z=.4 kT 946.4934 20.1170 -0.8699 2.9084 21 0.0233 0.1579 0.5951 0.0377
+---------------------------------------------------------------------------------------------
+Analyzing Jet 2:
+---------------------------------------------------------------------------------------------
+ name pt m y phi constit delta_R sym mu mxdropz
+ Original Jet 908.0979 87.7124 0.2195 6.0349 47
+ beta=2.0 zcut=.1 887.9353 11.3171 0.2232 6.0303 15 0.1116 0.0044 0.7910 0.0104
+ beta=1.0 zcut=.1 884.0262 8.9520 0.2228 6.0306 14 0.0570 0.0067 0.8862 0.0104
+ beta=0.5 zcut=.1 872.2856 7.0426 0.2230 6.0308 12 0.0346 0.0232 0.7445 0.0104
+ beta=2.0 zcut=.2 887.9353 11.3171 0.2232 6.0303 15 0.1116 0.0044 0.7910 0.0104
+ beta=1.0 zcut=.2 872.2856 7.0426 0.2230 6.0308 12 0.0346 0.0232 0.7445 0.0104
+ beta=0.5 zcut=.2 852.0552 5.2435 0.2230 6.0300 10 0.0154 0.0608 0.7701 0.0232
+ MMDT-like zcut=.1 800.2694 4.0381 0.2230 6.0310 9 0.0101 0.2350 0.2291 0.0608
+ MMDT-like zcut=.2 800.2694 4.0381 0.2230 6.0310 9 0.0101 0.2350 0.2291 0.0608
+ MMDT-like zcut=.3 ---- untagged jet ----
+ MMDT-like zcut=.4 ---- untagged jet ----
+beta=-2.0 zcut=.05 ---- untagged jet ----
+beta=-1.0 zcut=.05 ---- untagged jet ----
+beta=-0.5 zcut=.05 ---- untagged jet ----
+ b=.5 z=.3 R0=1.0 852.0552 5.2435 0.2230 6.0300 10 0.0154 0.0608 0.7701 0.0232
+ b=.5 z=.3 R0=0.5 852.0552 5.2435 0.2230 6.0300 10 0.0154 0.0608 0.7701 0.0232
+ b=.5 z=.3 R0=0.2 800.2694 4.0381 0.2230 6.0310 9 0.0101 0.2350 0.2291 0.0608
+ b=2 z=.4 scalar_z 884.0262 8.9520 0.2228 6.0306 14 0.0570 0.0067 0.8862 0.0104
+ b=2 z=.4 vector_z 884.0262 8.9520 0.2228 6.0306 14 0.0570 0.0067 0.8862 0.0104
+ b=2 z=.4 y 884.0262 8.9520 0.2228 6.0306 14 0.0570 0.0014 0.8862 0.0050
+b=3 z=.2 larger_pt 887.9353 11.3171 0.2232 6.0303 15 0.1116 0.0044 0.7910 0.0104
+b=3 z=.2 larger_mt 887.9353 11.3171 0.2232 6.0303 15 0.1116 0.0044 0.7910 0.0104
+ b=3 z=.2 larger_m 887.9353 11.3171 0.2232 6.0303 15 0.1116 0.0044 0.7910 0.0104
+ b=2 z=.1 mu=1.0 887.9353 11.3171 0.2232 6.0303 15 0.1116 0.0044 0.7910 0.0104
+ b=2 z=.1 mu=0.8 887.9353 11.3171 0.2232 6.0303 15 0.1116 0.0044 0.7910 0.0104
+ b=2 z=.1 mu=0.5 800.2694 4.0381 0.2230 6.0310 9 0.0101 0.2350 0.2291 0.0608
+ b=2.0 z=.2 kT 900.1551 59.2173 0.2190 6.0292 31 0.0176 0.2314 0.8689 0.0104
+ b=1.0 z=.2 kT 900.1551 59.2173 0.2190 6.0292 31 0.0176 0.2314 0.8689 0.0104
+ b=0.5 z=.2 kT 900.1551 59.2173 0.2190 6.0292 31 0.0176 0.2314 0.8689 0.0104
+ b=2.0 z=.4 kT 900.1551 59.2173 0.2190 6.0292 31 0.0176 0.2314 0.8689 0.0104
+ b=1.0 z=.4 kT 900.1551 59.2173 0.2190 6.0292 31 0.0176 0.2314 0.8689 0.0104
+ b=0.5 z=.4 kT 900.1551 59.2173 0.2190 6.0292 31 0.0176 0.2314 0.8689 0.0104
+---------------------------------------------------------------------------------------------
+Analyzing Jet 3:
+---------------------------------------------------------------------------------------------
+ name pt m y phi constit delta_R sym mu mxdropz
+ Original Jet 72.9429 23.4022 -1.1908 6.1199 43
+ beta=2.0 zcut=.1 71.5847 20.0943 -1.1761 6.1254 37 0.6803 0.0730 0.5627 0.0111
+ beta=1.0 zcut=.1 71.5847 20.0943 -1.1761 6.1254 37 0.6803 0.0730 0.5627 0.0111
+ beta=0.5 zcut=.1 67.3730 11.3061 -1.1810 6.0789 29 0.3790 0.0855 0.6966 0.0730
+ beta=2.0 zcut=.2 67.3730 11.3061 -1.1810 6.0789 29 0.3790 0.0855 0.6966 0.0730
+ beta=1.0 zcut=.2 67.3730 11.3061 -1.1810 6.0789 29 0.3790 0.0855 0.6966 0.0730
+ beta=0.5 zcut=.2 57.6019 5.9671 -1.1998 6.1138 16 0.1161 0.2463 0.7416 0.0855
+ MMDT-like zcut=.1 57.6019 5.9671 -1.1998 6.1138 16 0.1161 0.2463 0.7416 0.0855
+ MMDT-like zcut=.2 57.6019 5.9671 -1.1998 6.1138 16 0.1161 0.2463 0.7416 0.0855
+ MMDT-like zcut=.3 43.4356 4.4251 -1.2213 6.0950 13 0.1136 0.4598 0.5944 0.2463
+ MMDT-like zcut=.4 43.4356 4.4251 -1.2213 6.0950 13 0.1136 0.4598 0.5944 0.2463
+beta=-2.0 zcut=.05 ---- untagged jet ----
+beta=-1.0 zcut=.05 43.4356 4.4251 -1.2213 6.0950 13 0.1136 0.4598 0.5944 0.2463
+beta=-0.5 zcut=.05 71.5847 20.0943 -1.1761 6.1254 37 0.6803 0.0730 0.5627 0.0111
+ b=.5 z=.3 R0=1.0 57.6019 5.9671 -1.1998 6.1138 16 0.1161 0.2463 0.7416 0.0855
+ b=.5 z=.3 R0=0.5 57.6019 5.9671 -1.1998 6.1138 16 0.1161 0.2463 0.7416 0.0855
+ b=.5 z=.3 R0=0.2 57.6019 5.9671 -1.1998 6.1138 16 0.1161 0.2463 0.7416 0.0855
+ b=2 z=.4 scalar_z 67.3730 11.3061 -1.1810 6.0789 29 0.3790 0.0855 0.6966 0.0730
+ b=2 z=.4 vector_z 67.3730 11.3061 -1.1810 6.0789 29 0.3790 0.0859 0.6966 0.0741
+ b=2 z=.4 y 57.6019 5.9671 -1.1998 6.1138 16 0.1161 0.0763 0.7416 0.0376
+b=3 z=.2 larger_pt 71.5847 20.0943 -1.1761 6.1254 37 0.6803 0.0730 0.5627 0.0111
+b=3 z=.2 larger_mt 71.5847 20.0943 -1.1761 6.1254 37 0.6803 0.0730 0.5627 0.0111
+ b=3 z=.2 larger_m 71.5847 20.0943 -1.1761 6.1254 37 0.6803 0.0730 0.5627 0.0111
+ b=2 z=.1 mu=1.0 71.5847 20.0943 -1.1761 6.1254 37 0.6803 0.0730 0.5627 0.0111
+ b=2 z=.1 mu=0.8 71.5847 20.0943 -1.1761 6.1254 37 0.6803 0.0730 0.5627 0.0111
+ b=2 z=.1 mu=0.5 10.2806 0.1396 -1.1761 6.0554 1 -1.0000 -1.0000 -1.0000 0.0000
+ b=2.0 z=.2 kT 72.9429 23.4022 -1.1908 6.1199 43 0.2517 0.3453 0.4508 0.0000
+ b=1.0 z=.2 kT 72.9429 23.4022 -1.1908 6.1199 43 0.2517 0.3453 0.4508 0.0000
+ b=0.5 z=.2 kT 72.9429 23.4022 -1.1908 6.1199 43 0.2517 0.3453 0.4508 0.0000
+ b=2.0 z=.4 kT 72.9429 23.4022 -1.1908 6.1199 43 0.2517 0.3453 0.4508 0.0000
+ b=1.0 z=.4 kT 72.9429 23.4022 -1.1908 6.1199 43 0.2517 0.3453 0.4508 0.0000
+ b=0.5 z=.4 kT 72.9429 23.4022 -1.1908 6.1199 43 0.2517 0.3453 0.4508 0.0000
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_bottomup_softdrop.cc b/src/Tools/fjcontrib/RecursiveTools/example_bottomup_softdrop.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_bottomup_softdrop.cc
@@ -0,0 +1,123 @@
+//----------------------------------------------------------------------
+/// \file example_bottomup_softdrop.cc
+///
+/// This example program is meant to illustrate how the
+/// fastjet::contrib::BottomUpSoftDrop class is used.
+///
+/// Run this example with
+///
+/// \verbatim
+/// ./example_bottomup_softdrop < ../data/single-event.dat
+/// \endverbatim
+//----------------------------------------------------------------------
+
+// $Id: example_bottomup_softdrop.cc 1075 2017-09-18 15:27:09Z gsoyez $
+//
+// Copyright (c) 2017-, Gavin P. Salam, Gregory Soyez, Jesse Thaler,
+// Kevin Zhou, Frederic Dreyer
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iostream>
+#include <sstream>
+
+#include <iomanip>
+#include <cmath>
+#include "fastjet/ClusterSequence.hh"
+#include "BottomUpSoftDrop.hh" // In external code, this should be fastjet/contrib/BottomUpSoftDrop.hh
+
+using namespace std;
+using namespace fastjet;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &event);
+void print_prongs(const PseudoJet &jet, const string &pprefix);
+ostream & operator<<(ostream &, const PseudoJet &);
+
+//----------------------------------------------------------------------
+int main(){
+
+ //----------------------------------------------------------
+ // read in input particles
+ vector<PseudoJet> event;
+ read_event(event);
+ cout << "# read an event with " << event.size() << " particles" << endl;
+
+ // first get some anti-kt jets
+ double R = 1.0, ptmin = 100.0;
+ JetDefinition jet_def(antikt_algorithm, R);
+ ClusterSequence cs(event, jet_def);
+ vector<PseudoJet> jets = sorted_by_pt(cs.inclusive_jets(ptmin));
+
+ //----------------------------------------------------------------------
+ // give the soft drop groomer a short name
+ // Use a symmetry cut z > z_cut R^beta
+ // By default, there is no mass-drop requirement
+ double z_cut = 0.2;
+ double beta = 1.0;
+ contrib::BottomUpSoftDrop busd(beta, z_cut);
+
+ //----------------------------------------------------------------------
+ cout << "BottomUpSoftDrop groomer is: " << busd.description() << endl;
+
+ for (unsigned ijet = 0; ijet < jets.size(); ijet++) {
+ // Run SoftDrop and examine the output
+ PseudoJet busd_jet = busd(jets[ijet]);
+ cout << endl;
+ cout << "original jet: " << jets[ijet] << endl;
+ cout << "BottomUpSoftDropped jet: " << busd_jet << endl;
+
+ assert(busd_jet != 0); //because bottom-up soft drop is a groomer (not a tagger), it should always return a soft-dropped jet
+
+ }
+
+ return 0;
+}
+
+//----------------------------------------------------------------------
+/// read in input particles
+void read_event(vector<PseudoJet> &event){
+ string line;
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {return;}
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ event.push_back(particle);
+ }
+}
+
+//----------------------------------------------------------------------
+/// overloaded jet info output
+ostream & operator<<(ostream & ostr, const PseudoJet & jet) {
+ if (jet == 0) {
+ ostr << " 0 ";
+ } else {
+ ostr << " pt = " << jet.pt()
+ << " m = " << jet.m()
+ << " y = " << jet.rap()
+ << " phi = " << jet.phi();
+ }
+ return ostr;
+}
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_bottomup_softdrop.ref b/src/Tools/fjcontrib/RecursiveTools/example_bottomup_softdrop.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_bottomup_softdrop.ref
@@ -0,0 +1,21 @@
+# read an event with 354 particles
+#--------------------------------------------------------------------------
+# FastJet release 3.3.1-devel
+# M. Cacciari, G.P. Salam and G. Soyez
+# A software package for jet finding and analysis at colliders
+# http://fastjet.fr
+#
+# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package
+# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210].
+#
+# FastJet is provided without warranty under the terms of the GNU GPLv2.
+# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code
+# and 3rd party plugin jet algorithms. See COPYING file for details.
+#--------------------------------------------------------------------------
+BottomUpSoftDrop groomer is: BottomUpSoftDrop with jet_definition = (Longitudinally invariant Cambridge/Aachen algorithm with R = 1000 and E scheme recombination), symmetry_cut = 0.2, beta = 1, R0 = 1
+
+original jet: pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511
+BottomUpSoftDropped jet: pt = 962.379 m = 19.9368 y = -0.868399 phi = 2.90497
+
+original jet: pt = 908.098 m = 87.7124 y = 0.219482 phi = 6.03487
+BottomUpSoftDropped jet: pt = 872.286 m = 7.04265 y = 0.223045 phi = 6.03083
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_isd.cc b/src/Tools/fjcontrib/RecursiveTools/example_isd.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_isd.cc
@@ -0,0 +1,170 @@
+//----------------------------------------------------------------------
+/// \file example_isd.cc
+///
+/// This example program is meant to illustrate how the
+/// fastjet::contrib::IteratedSoftDrop class is used.
+///
+/// Run this example with
+///
+/// \verbatim
+/// ./example_isd < ../data/single-event.dat
+/// \endverbatim
+//----------------------------------------------------------------------
+
+// $Id: example_isd.cc 1115 2018-04-21 13:37:04Z jthaler $
+//
+// Copyright (c) 2017, Jesse Thaler, Kevin Zhou
+// based on arXiv:1704.06266 by Christopher Frye, Andrew J. Larkoski,
+// Jesse Thaler, Kevin Zhou
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iostream>
+#include <sstream>
+
+#include <sstream>
+#include <iomanip>
+#include <cmath>
+#include "fastjet/ClusterSequence.hh"
+
+#include "IteratedSoftDrop.hh" // In external code, this should be fastjet/contrib/IteratedSoftDrop.hh
+
+using namespace std;
+using namespace fastjet;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &event);
+
+//----------------------------------------------------------------------
+int main(){
+
+ //----------------------------------------------------------
+ // read in input particles
+ vector<PseudoJet> event;
+ read_event(event);
+ cout << "# read an event with " << event.size() << " particles" << endl;
+
+ // first get some anti-kt jets
+ double R = 0.5;
+ JetDefinition jet_def(antikt_algorithm, R);
+ double ptmin = 200.0;
+ Selector pt_min_selector = SelectorPtMin(ptmin);
+
+ ClusterSequence cs(event,jet_def);
+ vector<PseudoJet> jets = pt_min_selector(sorted_by_pt(cs.inclusive_jets()));
+
+ // Determine optimal scale from 1704.06266 for beta = -1
+ double expected_jet_pt = 1000; // in GeV
+ double NP_scale = 1; // approximately Lambda_QCD in GeV
+ double optimal_z_cut = (NP_scale / expected_jet_pt / R);
+
+ // set up iterated soft drop objects
+ double z_cut = optimal_z_cut;
+ double beta = -1.0;
+ double theta_cut = 0.0;
+
+ contrib::IteratedSoftDrop isd(beta, z_cut, theta_cut, R);
+ contrib::IteratedSoftDrop isd_ee(beta, z_cut, contrib::RecursiveSoftDrop::theta_E,
+ theta_cut, R, std::numeric_limits<double>::infinity(),
+ contrib::RecursiveSoftDrop::larger_E);
+
+ cout << "---------------------------------------------------" << endl;
+ cout << "Iterated Soft Drop" << endl;
+ cout << "---------------------------------------------------" << endl;
+
+ cout << endl;
+ cout << "Computing with:" << endl;
+ cout << " " << isd.description() << endl;
+ cout << " " << isd_ee.description() << endl;
+ cout << endl;
+
+ for (unsigned ijet = 0; ijet < jets.size(); ijet++) {
+
+ cout << "---------------------------------------------------" << endl;
+ cout << "Processing Jet " << ijet << endl;
+ cout << "---------------------------------------------------" << endl;
+
+
+ cout << endl;
+ cout << "Jet pT: " << jets[ijet].pt() << " GeV" << endl;
+ cout << endl;
+
+
+ // Run full iterated soft drop
+ //
+ // Instead of asking for an IteratedSoftDropInfo which contains
+ // all the information to calculate physics observables, one can
+ // use
+ // isd.all_zg_thetag(jet) for the list of symmetry factors and angles
+ // isd.multiplicity(jet) for the ISD multiplicity
+ // isd.angularity(jet,alpha) for the angularity obtained from the (zg, thetag)
+ //
+ contrib::IteratedSoftDropInfo syms = isd(jets[ijet]);
+
+ cout << "Soft Drop Multiplicity (pt_R measure, beta=" << beta << ", z_cut=" << z_cut << "):" << endl;
+ cout << syms.multiplicity() << endl;
+ cout << endl;
+
+ cout << "Symmetry Factors (pt_R measure, beta=" << beta << ", z_cut=" << z_cut << "):" << endl;
+ for (unsigned i = 0; i < syms.size(); i++){
+ cout << syms[i].first << " ";
+ }
+ cout << endl;
+ cout << endl;
+
+ cout << "Soft Drop Angularities (pt_R measure, beta=" << beta << ", z_cut=" << z_cut << "):" << endl;
+ cout << " alpha = 0, kappa = 0 : " << syms.angularity(0.0, 0.0) << endl;
+ cout << " alpha = 0, kappa = 2 : " << syms.angularity(0.0, 2.0) << endl;
+ cout << " alpha = 0.5, kappa = 1 : " << syms.angularity(0.5) << endl;
+ cout << " alpha = 1, kappa = 1 : " << syms.angularity(1.0) << endl;
+ cout << " alpha = 2, kappa = 1 : " << syms.angularity(2.0) << endl;
+ cout << endl;
+
+ // Alternative version with e+e- measure
+ contrib::IteratedSoftDropInfo syms_ee = isd_ee(jets[ijet]);
+ cout << "Symmetry Factors (E_theta measure, beta=" << beta << ", z_cut=" << z_cut << "):" << endl;
+ for (unsigned i = 0; i < syms_ee.size(); i++){
+ cout << syms_ee[i].first << " ";
+ }
+ cout << endl;
+ cout << endl;
+
+
+ }
+
+ return 0;
+}
+
+//----------------------------------------------------------------------
+/// read in input particles
+void read_event(vector<PseudoJet> &event){
+ string line;
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {return;}
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ event.push_back(particle);
+ }
+}
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_isd.ref b/src/Tools/fjcontrib/RecursiveTools/example_isd.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_isd.ref
@@ -0,0 +1,66 @@
+# read an event with 354 particles
+#--------------------------------------------------------------------------
+# FastJet release 3.2.0
+# M. Cacciari, G.P. Salam and G. Soyez
+# A software package for jet finding and analysis at colliders
+# http://fastjet.fr
+#
+# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package
+# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210].
+#
+# FastJet is provided without warranty under the terms of the GNU GPLv2.
+# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code
+# and 3rd party plugin jet algorithms. See COPYING file for details.
+#--------------------------------------------------------------------------
+---------------------------------------------------
+Iterated Soft Drop
+---------------------------------------------------
+
+Computing with:
+ IteratedSoftDrop with beta =-1, symmetry_cut=0.002, R0=0.5 and no angular_cut
+ IteratedSoftDrop with beta =-1, symmetry_cut=0.002, R0=0.5 and no angular_cut
+
+---------------------------------------------------
+Processing Jet 0
+---------------------------------------------------
+
+Jet pT: 982.342 GeV
+
+Soft Drop Multiplicity (pt_R measure, beta=-1, z_cut=0.002):
+3
+
+Symmetry Factors (pt_R measure, beta=-1, z_cut=0.002):
+0.0294298 0.154333 0.42512
+
+Soft Drop Angularities (pt_R measure, beta=-1, z_cut=0.002):
+ alpha = 0, kappa = 0 : 3
+ alpha = 0, kappa = 2 : 0.205411
+ alpha = 0.5, kappa = 1 : 0.0541032
+ alpha = 1, kappa = 1 : 0.0071635
+ alpha = 2, kappa = 1 : 0.000333819
+
+Symmetry Factors (E_theta measure, beta=-1, z_cut=0.002):
+0.0286322 0.156129
+
+---------------------------------------------------
+Processing Jet 1
+---------------------------------------------------
+
+Jet pT: 899.993 GeV
+
+Soft Drop Multiplicity (pt_R measure, beta=-1, z_cut=0.002):
+4
+
+Symmetry Factors (pt_R measure, beta=-1, z_cut=0.002):
+0.00357435 0.0033004 0.00518061 0.235041
+
+Soft Drop Angularities (pt_R measure, beta=-1, z_cut=0.002):
+ alpha = 0, kappa = 0 : 4
+ alpha = 0, kappa = 2 : 0.0552947
+ alpha = 0.5, kappa = 1 : 0.0307531
+ alpha = 1, kappa = 1 : 0.00657501
+ alpha = 2, kappa = 1 : 0.00151741
+
+Symmetry Factors (E_theta measure, beta=-1, z_cut=0.002):
+0.00367919 0.00338026 0.00506002 0.235347
+
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_mmdt.cc b/src/Tools/fjcontrib/RecursiveTools/example_mmdt.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_mmdt.cc
@@ -0,0 +1,131 @@
+//----------------------------------------------------------------------
+/// \file example_mmdt.cc
+///
+/// This example program is meant to illustrate how the
+/// fastjet::contrib::ModifiedMassDropTagger class is used.
+///
+/// Run this example with
+///
+/// \verbatim
+/// ./example_mmdt < ../data/single-event.dat
+/// \endverbatim
+///
+/// It also shows operation in conjunction with a Filter.
+//----------------------------------------------------------------------
+
+// $Id: example_mmdt.cc 686 2014-06-14 03:25:09Z jthaler $
+//
+// Copyright (c) 2014, Gavin P. Salam
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iostream>
+#include <sstream>
+
+#include <sstream>
+#include <iomanip>
+#include <cmath>
+#include "fastjet/ClusterSequence.hh"
+#include "fastjet/tools/Filter.hh"
+#include "ModifiedMassDropTagger.hh" // In external code, this should be fastjet/contrib/ModifiedMassDropTagger.hh
+
+using namespace std;
+using namespace fastjet;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &event);
+ostream & operator<<(ostream &, const PseudoJet &);
+
+//----------------------------------------------------------------------
+int main(){
+
+ //----------------------------------------------------------
+ // read in input particles
+ vector<PseudoJet> event;
+ read_event(event);
+ cout << "# read an event with " << event.size() << " particles" << endl;
+
+ // first get some Cambridge/Aachen jets
+ double R = 1.0, ptmin = 20.0;
+ JetDefinition jet_def(cambridge_algorithm, R);
+ ClusterSequence cs(event, jet_def);
+ vector<PseudoJet> jets = sorted_by_pt(cs.inclusive_jets(ptmin));
+
+ // give the tagger a short name
+ typedef contrib::ModifiedMassDropTagger MMDT;
+ // use just a symmetry cut, with no mass-drop requirement
+ double z_cut = 0.10;
+ MMDT tagger(z_cut);
+ cout << "tagger is: " << tagger.description() << endl;
+
+ for (unsigned ijet = 0; ijet < jets.size(); ijet++) {
+ // first run MMDT and examine the output
+ PseudoJet tagged_jet = tagger(jets[ijet]);
+ cout << endl;
+ cout << "original jet: " << jets[ijet] << endl;
+ cout << "tagged jet: " << tagged_jet << endl;
+ if (tagged_jet == 0) continue; // If symmetry condition not satisified, jet is not tagged
+ cout << " delta_R between subjets: " << tagged_jet.structure_of<MMDT>().delta_R() << endl;
+ cout << " symmetry measure(z): " << tagged_jet.structure_of<MMDT>().symmetry() << endl;
+ cout << " mass drop(mu): " << tagged_jet.structure_of<MMDT>().mu() << endl;
+
+ // then filter the jet (useful for studies at moderate pt)
+ // with a dynamic Rfilt choice (as in arXiv:0802.2470)
+ double Rfilt = min(0.3, tagged_jet.structure_of<MMDT>().delta_R()*0.5);
+ int nfilt = 3;
+ Filter filter(Rfilt, SelectorNHardest(nfilt));
+ PseudoJet filtered_jet = filter(tagged_jet);
+ cout << "filtered jet: " << filtered_jet << endl;
+ cout << endl;
+ }
+
+ return 0;
+}
+
+//----------------------------------------------------------------------
+/// read in input particles
+void read_event(vector<PseudoJet> &event){
+ string line;
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {return;}
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ event.push_back(particle);
+ }
+}
+
+//----------------------------------------------------------------------
+/// overloaded jet info output
+ostream & operator<<(ostream & ostr, const PseudoJet & jet) {
+ if (jet == 0) {
+ ostr << " 0 ";
+ } else {
+ ostr << " pt = " << jet.pt()
+ << " m = " << jet.m()
+ << " y = " << jet.rap()
+ << " phi = " << jet.phi();
+ }
+ return ostr;
+}
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_mmdt.ref b/src/Tools/fjcontrib/RecursiveTools/example_mmdt.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_mmdt.ref
@@ -0,0 +1,39 @@
+# read an event with 354 particles
+#--------------------------------------------------------------------------
+# FastJet release 3.1.0-devel
+# M. Cacciari, G.P. Salam and G. Soyez
+# A software package for jet finding and analysis at colliders
+# http://fastjet.fr
+#
+# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package
+# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210].
+#
+# FastJet is provided without warranty under the terms of the GNU GPLv2.
+# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code,
+# CGAL and 3rd party plugin jet algorithms. See COPYING file for details.
+#--------------------------------------------------------------------------
+tagger is: Recursive Tagger with a symmetry cut scalar_z > 0.1 [ModifiedMassDropTagger], no mass-drop requirement, recursion into the subjet with larger pt
+
+original jet: pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511
+tagged jet: pt = 917.674 m = 8.70484 y = -0.869593 phi = 2.90788
+ delta_R between subjets: 0.0200353
+ symmetry measure(z): 0.154333
+ mass drop(mu): 0.557579
+filtered jet: pt = 917.674 m = 8.70484 y = -0.869593 phi = 2.90788
+
+
+original jet: pt = 910.164 m = 122.615 y = 0.223738 phi = 6.04265
+tagged jet: pt = 800.269 m = 4.03811 y = 0.223011 phi = 6.03096
+ delta_R between subjets: 0.0101382
+ symmetry measure(z): 0.235041
+ mass drop(mu): 0.229134
+filtered jet: pt = 778.731 m = 3.66481 y = 0.223066 phi = 6.0309
+
+
+original jet: pt = 73.2118 m = 21.4859 y = -1.16399 phi = 6.11977
+tagged jet: pt = 57.6019 m = 5.96709 y = -1.19982 phi = 6.11382
+ delta_R between subjets: 0.116062
+ symmetry measure(z): 0.246343
+ mass drop(mu): 0.741581
+filtered jet: pt = 46.7389 m = 4.6395 y = -1.19991 phi = 6.12566
+
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_mmdt_ee.cc b/src/Tools/fjcontrib/RecursiveTools/example_mmdt_ee.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_mmdt_ee.cc
@@ -0,0 +1,142 @@
+//----------------------------------------------------------------------
+/// \file example_ee.cc
+///
+/// This example program is meant to illustrate how to use
+/// RecursiveTools for e+e- events. It is done using the
+/// ModifiedMassDropTagger class but the same strategy would work as
+/// well for SoftDrop, RecursiveSoftDrop and IteratedSoftDrop
+///
+/// Run this example with
+///
+/// \verbatim
+/// ./example_ee < ../data/single-ee-event.dat
+/// \endverbatim
+//----------------------------------------------------------------------
+
+// $Id: example_mmdt_ee.cc 1064 2017-09-08 09:19:57Z gsoyez $
+//
+// Copyright (c) 2017-, Gavin P. Salam, Gregory Soyez, Jesse Thaler,
+// Kevin Zhou, Frederic Dreyer
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iostream>
+#include <sstream>
+
+#include <sstream>
+#include <iomanip>
+#include <cmath>
+#include "fastjet/ClusterSequence.hh"
+#include "fastjet/tools/Filter.hh"
+#include "ModifiedMassDropTagger.hh" // In external code, this should be fastjet/contrib/ModifiedMassDropTagger.hh
+
+using namespace std;
+using namespace fastjet;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &event);
+ostream & operator<<(ostream &, const PseudoJet &);
+
+//----------------------------------------------------------------------
+int main(){
+
+ //----------------------------------------------------------
+ // read in input particles
+ vector<PseudoJet> event;
+ read_event(event);
+ cout << "# read an event with " << event.size() << " particles" << endl;
+
+ // first get some Cambridge/Aachen jets
+ double R = 1.0;
+ JetDefinition jet_def(ee_genkt_algorithm, R, 0.0);
+ ClusterSequence cs(event, jet_def);
+
+ double Emin = 10.0;
+ Selector sel_jets = SelectorEMin(Emin);
+ vector<PseudoJet> jets = sorted_by_E(sel_jets(cs.inclusive_jets()));
+
+ // give the tagger a short name
+ typedef contrib::ModifiedMassDropTagger MMDT;
+
+ // This version uses the following setup:
+ // - use energy for the symmetry measure
+ // Note: since the mMDT does not require angular information,
+ // here we could use either theta_E or cos_theta_E (it would
+ // only change the value of DeltaR). For
+ // SoftDrop/RecursiveSoftDrop/IteratedSoftDrop, this would make
+ // a difference and we have
+ // DeltaR_{ij}^2 = theta_{ij}^2 (theta_E)
+ // DeltaR_{ij}^2 = 2 [1-cos(theta_{ij}^2)] (cos_theta_E)
+ //
+ // - recurse into the branch with the largest energy
+ //
+ // - use a symmetry cut, with no mass-drop requirement
+ double z_cut = 0.20;
+ MMDT tagger(z_cut,
+ MMDT::cos_theta_E,
+ std::numeric_limits<double>::infinity(),
+ MMDT::larger_E);
+ cout << "tagger is: " << tagger.description() << endl;
+
+ for (unsigned ijet = 0; ijet < jets.size(); ijet++) {
+ // first run MMDT and examine the output
+ PseudoJet tagged_jet = tagger(jets[ijet]);
+ cout << endl;
+ cout << "original jet: " << jets[ijet] << endl;
+ cout << "tagged jet: " << tagged_jet << endl;
+ if (tagged_jet == 0) continue; // If symmetry condition not satisified, jet is not tagged
+ cout << " delta_R between subjets: " << tagged_jet.structure_of<MMDT>().delta_R() << endl;
+ cout << " symmetry measure(z): " << tagged_jet.structure_of<MMDT>().symmetry() << endl;
+ cout << " mass drop(mu): " << tagged_jet.structure_of<MMDT>().mu() << endl;
+
+ cout << endl;
+ }
+
+ return 0;
+}
+
+//----------------------------------------------------------------------
+/// read in input particles
+void read_event(vector<PseudoJet> &event){
+ string line;
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {return;}
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ event.push_back(particle);
+ }
+}
+
+//----------------------------------------------------------------------
+/// overloaded jet info output
+ostream & operator<<(ostream & ostr, const PseudoJet & jet) {
+ if (jet == 0) {
+ ostr << " 0 ";
+ } else {
+ ostr << " E = " << jet.pt()
+ << " m = " << jet.m();
+ }
+ return ostr;
+}
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_mmdt_ee.ref b/src/Tools/fjcontrib/RecursiveTools/example_mmdt_ee.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_mmdt_ee.ref
@@ -0,0 +1,36 @@
+# read an event with 70 particles
+#--------------------------------------------------------------------------
+# FastJet release 3.3.1-devel
+# M. Cacciari, G.P. Salam and G. Soyez
+# A software package for jet finding and analysis at colliders
+# http://fastjet.fr
+#
+# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package
+# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210].
+#
+# FastJet is provided without warranty under the terms of the GNU GPLv2.
+# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code
+# and 3rd party plugin jet algorithms. See COPYING file for details.
+#--------------------------------------------------------------------------
+tagger is: Recursive Tagger with a symmetry cut cos_theta_E > 0.2 [ModifiedMassDropTagger], no mass-drop requirement, recursion into the subjet with larger energy
+
+original jet: E = 11.7799 m = 19.2957
+tagged jet: E = 6.02018 m = 6.52181
+ delta_R between subjets: 0.270322
+ symmetry measure(z): 0.49629
+ mass drop(mu): 0.403395
+
+
+original jet: E = 15.9528 m = 7.28134
+tagged jet: E = 8.08779 m = 0.992053
+ delta_R between subjets: 0.113801
+ symmetry measure(z): 0.289966
+ mass drop(mu): 0.413689
+
+
+original jet: E = 10.3356 m = 9.53801
+tagged jet: E = 10.3356 m = 9.53801
+ delta_R between subjets: 0.779204
+ symmetry measure(z): 0.35827
+ mass drop(mu): 0.331619
+
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_mmdt_sub.cc b/src/Tools/fjcontrib/RecursiveTools/example_mmdt_sub.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_mmdt_sub.cc
@@ -0,0 +1,211 @@
+// $Id: example_mmdt_sub.cc 686 2014-06-14 03:25:09Z jthaler $
+//
+// Copyright (c) 2014, Gavin Salam
+//
+/// \file example_mmdt_sub.cc
+///
+/// An example to illustrate how to use the ModifiedMassDropTagger
+/// together with pileup subtraction.
+///
+/// Usage:
+///
+/// \verbatim
+/// ./example_mmdt_sub < ../data/Pythia-Zp2jets-lhc-pileup-1ev.dat
+/// \endverbatim
+///
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iostream>
+#include <sstream>
+
+#include <sstream>
+#include <iomanip>
+#include "fastjet/ClusterSequenceArea.hh"
+#include "fastjet/tools/GridMedianBackgroundEstimator.hh"
+#include "fastjet/tools/Subtractor.hh"
+#include "fastjet/tools/Filter.hh"
+#include "fastjet/config.h"
+#include "ModifiedMassDropTagger.hh" // In external code, this should be fastjet/contrib/ModifiedMassDropTagger.hh
+
+using namespace std;
+using namespace fastjet;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &hard_event, vector<PseudoJet> &full_event);
+void do_analysis(const vector<PseudoJet> & jets, const Subtractor * subtractor);
+ostream & operator<<(ostream &, const PseudoJet &);
+
+// give the tagger a short name
+typedef contrib::ModifiedMassDropTagger MMDT;
+
+//----------------------------------------------------------------------
+int main(){
+
+ // Specify our basic jet tools:
+ // jet definition & area definition
+ double R = 1.0, rapmax = 5.0, ghost_area = 0.01;
+ int repeat = 1;
+ JetDefinition jet_def(cambridge_algorithm, R);
+ AreaDefinition area_def(active_area_explicit_ghosts,
+ GhostedAreaSpec(SelectorAbsRapMax(rapmax),repeat,ghost_area));
+ cout << "# " << jet_def.description() << endl;
+ cout << "# " << area_def.description() << endl;
+
+ // then our background estimator: use the (fast) grid-median method,
+ // and manually include reasonable rapidity dependence for
+ // particle-level 14 TeV events.
+ double grid_size = 0.55;
+ GridMedianBackgroundEstimator bge(rapmax, grid_size);
+ BackgroundRescalingYPolynomial rescaling (1.1685397, 0, -0.0246807, 0, 5.94119e-05);
+ bge.set_rescaling_class(&rescaling);
+ // define a corresponding subtractor
+ Subtractor subtractor(&bge);
+
+
+ //----------------------------------------------------------
+ // next read in input particles and get corresponding jets
+ // for the hard event (no pileup) and full event (with pileup)
+ vector<PseudoJet> hard_event, full_event;
+ read_event(hard_event, full_event);
+ cout << "# read a hard event with " << hard_event.size() << " particles" ;
+#if (FASTJET_VERSION_NUMBER >= 30100) // Selector.sum(..) works only for FJ >= 3.1
+ cout << ", centre-of-mass energy = " << SelectorIdentity().sum(hard_event).m();
+#endif
+ cout << endl;
+ cout << "# read a full event with " << full_event.size() << " particles" << endl;
+
+ // then get the CS and jets for both hard and full events
+ ClusterSequenceArea csa_hard(hard_event, jet_def, area_def);
+ ClusterSequenceArea csa_full(full_event, jet_def, area_def);
+ vector<PseudoJet> hard_jets = SelectorNHardest(2)(csa_hard.inclusive_jets());
+ vector<PseudoJet> full_jets = SelectorNHardest(2)(csa_full.inclusive_jets());
+ hard_jets = sorted_by_rapidity(hard_jets);
+ full_jets = sorted_by_rapidity(full_jets);
+
+ // estimate the background (the subtractor is automatically tied to this)
+ bge.set_particles(full_event);
+
+ // then do analyses with and without PU, and with and without subtraction
+ cout << endl << "-----------------------------------------" << endl
+ << "No pileup, no subtraction" << endl;
+ do_analysis(hard_jets, 0);
+ cout << endl << "-----------------------------------------" << endl
+ << "Pileup, no subtraction" << endl;
+ do_analysis(full_jets, 0);
+ cout << endl << "-----------------------------------------" << endl
+ << "Pileup, with subtraction" << endl;
+ do_analysis(full_jets, &subtractor);
+
+ return 0;
+}
+
+
+//----------------------------------------------------------------------
+/// do a simple MMDT + filter analysis, optionally with a subtractor
+void do_analysis(const vector<PseudoJet> & jets, const Subtractor * subtractor) {
+
+ // use just a symmetry cut for the tagger, with no mass-drop requirement
+ double z_cut = 0.10;
+ MMDT tagger(z_cut);
+ cout << "tagger is: " << tagger.description() << endl;
+ // tell the tagger that we will subtract the input jet ourselves
+ tagger.set_subtractor(subtractor);
+ tagger.set_input_jet_is_subtracted(true);
+
+
+ PseudoJet jet;
+ for (unsigned ijet = 0; ijet < jets.size(); ijet++) {
+ if (subtractor) {
+ jet = (*subtractor)(jets[ijet]);
+ } else {
+ jet = jets[ijet];
+ }
+ PseudoJet tagged_jet = tagger(jet);
+ cout << endl;
+ cout << "original jet" << jet << endl;
+ cout << "tagged jet" << tagged_jet << endl;
+ if (tagged_jet != 0) { // get additional informaition about satisified symmetry condition
+ cout << " delta_R between subjets: " << tagged_jet.structure_of<MMDT>().delta_R() << endl;
+ cout << " symmetry measure(z): " << tagged_jet.structure_of<MMDT>().symmetry() << endl;
+ cout << " mass drop(mu): " << tagged_jet.structure_of<MMDT>().mu() << endl;
+ }
+
+ // then filter the jet (useful for studies at moderate pt)
+ // with a dynamic Rfilt choice (as in arXiv:0802.2470)
+ double Rfilt = min(0.3, tagged_jet.structure_of<MMDT>().delta_R()*0.5);
+ int nfilt = 3;
+ Filter filter(Rfilt, SelectorNHardest(nfilt));
+ filter.set_subtractor(subtractor);
+ PseudoJet filtered_jet = filter(tagged_jet);
+ cout << "filtered jet: " << filtered_jet << endl;
+ cout << endl;
+ }
+
+
+}
+
+
+//------------------------------------------------------------------------
+// read the event with and without pileup
+void read_event(vector<PseudoJet> &hard_event, vector<PseudoJet> &full_event){
+ string line;
+ int nsub = 0; // counter to keep track of which sub-event we're reading
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {break;}
+ if (line.substr(0,9) == "#SUBSTART") {
+ // if more sub events follow, make copy of first one (the hard one) here
+ if (nsub == 1) hard_event = full_event;
+ nsub += 1;
+ }
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ full_event.push_back(particle);
+ }
+
+ // if we have read in only one event, copy it across here...
+ if (nsub == 1) hard_event = full_event;
+
+ // if there was nothing in the event
+ if (nsub == 0) {
+ cerr << "Error: read empty event\n";
+ exit(-1);
+ }
+
+ cout << "# " << nsub-1 << " pileup events on top of the hard event" << endl;
+}
+
+//----------------------------------------------------------------------
+/// overloaded jet info output
+ostream & operator<<(ostream & ostr, const PseudoJet & jet) {
+ if (jet == 0) {
+ ostr << " 0 ";
+ } else {
+ ostr << " pt = " << jet.pt()
+ << " m = " << jet.m()
+ << " y = " << jet.rap()
+ << " phi = " << jet.phi();
+ }
+ return ostr;
+}
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_mmdt_sub.ref b/src/Tools/fjcontrib/RecursiveTools/example_mmdt_sub.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_mmdt_sub.ref
@@ -0,0 +1,78 @@
+# Longitudinally invariant Cambridge/Aachen algorithm with R = 1 and E scheme recombination
+# Active area (explicit ghosts) with ghosts of area 0.00997331 (had requested 0.01), placed according to selector (|rap| <= 5), scattered wrt to perfect grid by (rel) 1, mean_ghost_pt = 1e-100, rel pt_scatter = 0.1, n repetitions of ghost distributions = 1
+# 20 pileup events on top of the hard event
+# read a hard event with 309 particles, centre-of-mass energy = 14000
+# read a full event with 3109 particles
+#--------------------------------------------------------------------------
+# FastJet release 3.1.0-devel
+# M. Cacciari, G.P. Salam and G. Soyez
+# A software package for jet finding and analysis at colliders
+# http://fastjet.fr
+#
+# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package
+# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210].
+#
+# FastJet is provided without warranty under the terms of the GNU GPLv2.
+# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code,
+# CGAL and 3rd party plugin jet algorithms. See COPYING file for details.
+#--------------------------------------------------------------------------
+
+-----------------------------------------
+No pileup, no subtraction
+tagger is: Recursive Tagger with a symmetry cut scalar_z > 0.1 [ModifiedMassDropTagger], no mass-drop requirement, recursion into the subjet with larger pt
+
+original jet pt = 221.812 m = 32.2905 y = -1.05822 phi = 0.0756913
+tagged jet pt = 206.662 m = 6.022 y = -1.07399 phi = 0.074484
+ delta_R between subjets: 0.0625986
+ symmetry measure(z): 0.10081
+ mass drop(mu): 0.629535
+filtered jet: pt = 198.618 m = 5.00366 y = -1.07664 phi = 0.0741277
+
+
+original jet pt = 147.272 m = 32.4736 y = 0.684444 phi = 3.45888
+tagged jet pt = 125.59 m = 9.00653 y = 0.673318 phi = 3.44347
+ delta_R between subjets: 0.0732829
+ symmetry measure(z): 0.348016
+ mass drop(mu): 0.604284
+filtered jet: pt = 72.4046 m = 4.32252 y = 0.668029 phi = 3.44446
+
+
+-----------------------------------------
+Pileup, no subtraction
+tagger is: Recursive Tagger with a symmetry cut scalar_z > 0.1 [ModifiedMassDropTagger], no mass-drop requirement, recursion into the subjet with larger pt
+
+original jet pt = 238.971 m = 82.4889 y = -1.07084 phi = 0.0430975
+tagged jet pt = 206.662 m = 6.022 y = -1.07399 phi = 0.074484
+ delta_R between subjets: 0.0625986
+ symmetry measure(z): 0.10081
+ mass drop(mu): 0.629535
+filtered jet: pt = 198.618 m = 5.00366 y = -1.07664 phi = 0.0741277
+
+
+original jet pt = 173.75 m = 74.6701 y = 0.73638 phi = 3.48392
+tagged jet pt = 133.133 m = 13.4499 y = 0.667906 phi = 3.44217
+ delta_R between subjets: 0.10831
+ symmetry measure(z): 0.107147
+ mass drop(mu): 0.862327
+filtered jet: pt = 109.81 m = 7.14298 y = 0.676746 phi = 3.43921
+
+
+-----------------------------------------
+Pileup, with subtraction
+tagger is: Recursive Tagger with a symmetry cut scalar_z > 0.1 [ModifiedMassDropTagger], no mass-drop requirement, recursion into the subjet with larger pt
+
+original jet pt = 203.782 m = -0.967618 y = -1.05353 phi = 0.0821247
+tagged jet pt = 206.662 m = 6.022 y = -1.07399 phi = 0.074484
+ delta_R between subjets: 0.0625986
+ symmetry measure(z): 0.10081
+ mass drop(mu): 0.629535
+filtered jet: pt = 198.618 m = 5.00366 y = -1.07664 phi = 0.0741277
+
+
+original jet pt = 146.109 m = 51.1929 y = 0.705189 phi = 3.44819
+tagged jet pt = 132.536 m = 13.3758 y = 0.668335 phi = 3.44231
+ delta_R between subjets: 0.107608
+ symmetry measure(z): 0.104244
+ mass drop(mu): 0.866401
+filtered jet: pt = 109.661 m = 7.13553 y = 0.676798 phi = 3.43925
+
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_recluster.cc b/src/Tools/fjcontrib/RecursiveTools/example_recluster.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_recluster.cc
@@ -0,0 +1,173 @@
+//----------------------------------------------------------------------
+/// \file example_recluster.cc
+///
+/// This example program is meant to illustrate how the
+/// fastjet::contrib::ModifiedMassDropTagger class is used.
+///
+/// Run this example with
+///
+/// \verbatim
+/// ./example_recluster < ../data/single-event.dat
+/// \endverbatim
+//----------------------------------------------------------------------
+
+// $Id: example_recluster.cc 705 2014-07-07 14:37:03Z gsoyez $
+//
+// Copyright (c) 2014, Gavin P. Salam
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iostream>
+#include <sstream>
+
+#include <sstream>
+#include <iomanip>
+#include <cmath>
+#include "fastjet/ClusterSequence.hh"
+
+#include "Recluster.hh" // In external code, this should be fastjet/contrib/Recluster.hh
+
+using namespace std;
+using namespace fastjet;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &event);
+ostream & operator<<(ostream &, const PseudoJet &);
+
+//----------------------------------------------------------------------
+int main(){
+
+ //----------------------------------------------------------
+ // read in input particles
+ vector<PseudoJet> event;
+ read_event(event);
+ cout << "# read an event with " << event.size() << " particles" << endl;
+
+ double R = 1.0;
+ double ptmin = 20.0;
+ double Rsub = 0.3;
+
+ //----------------------------------------------------------
+ // start with an example from anti-kt jets
+ cout << "--------------------------------------------------" << endl;
+ JetDefinition jet_def_akt(antikt_algorithm, R);
+ ClusterSequence cs_akt(event, jet_def_akt);
+ vector<PseudoJet> jets_akt = sorted_by_pt(cs_akt.inclusive_jets(ptmin));
+ PseudoJet jet_akt = jets_akt[0];
+ cout << "Starting from a jet obtained from: " << jet_def_akt.description() << endl
+ << " " << jet_akt << endl << endl;
+
+ // recluster with C/A ("infinite" radius)
+ contrib::Recluster recluster_ca_inf(cambridge_algorithm, JetDefinition::max_allowable_R);
+ PseudoJet rec_jet_ca_inf = recluster_ca_inf(jet_akt);
+ cout << "Reclustering with: " << recluster_ca_inf.description() << endl
+ << " " << rec_jet_ca_inf << endl << endl;;
+
+ // recluster with C/A (small radius), keeping all subjets
+ contrib::Recluster recluster_ca_sub(cambridge_algorithm, Rsub, false);
+ PseudoJet rec_jet_ca_sub = recluster_ca_sub(jet_akt);
+ cout << "Reclustering with: " << recluster_ca_sub.description() << endl
+ << " " << rec_jet_ca_sub << endl;
+ vector<PseudoJet> pieces = rec_jet_ca_sub.pieces();
+ cout << " subjets: " << endl;
+ for (unsigned int i=0;i<pieces.size();i++)
+ cout << " " << pieces[i] << endl;
+ cout << endl;
+
+ // recluster with kt (small radius), keeping all subjets
+ contrib::Recluster recluster_kt_sub(kt_algorithm, Rsub, false);
+ PseudoJet rec_jet_kt_sub = recluster_kt_sub(jet_akt);
+ cout << "Reclustering with: " << recluster_kt_sub.description() << endl
+ << " " << rec_jet_kt_sub << endl;
+ pieces = rec_jet_kt_sub.pieces();
+ cout << " subjets: " << endl;
+ for (unsigned int i=0;i<pieces.size();i++)
+ cout << " " << pieces[i] << endl;
+ cout << endl;
+
+ //----------------------------------------------------------
+ // now an example starting from C/A jets
+ cout << "--------------------------------------------------" << endl;
+ JetDefinition jet_def_ca(cambridge_algorithm, R);
+ ClusterSequence cs_ca(event, jet_def_ca);
+ vector<PseudoJet> jets_ca = sorted_by_pt(cs_ca.inclusive_jets(ptmin));
+ PseudoJet jet_ca = jets_ca[0];
+ cout << "Starting from a jet obtained from: " << jet_def_ca.description() << endl
+ << " " << jet_ca << endl << endl;
+
+ // recluster with C/A ("infinite" radius)
+ rec_jet_ca_inf = recluster_ca_inf(jet_ca);
+ cout << "Reclustering with: " << recluster_ca_inf.description() << endl
+ << " " << rec_jet_ca_inf << endl << endl;
+
+ // recluster with C/A (small radius), keeping all subjets
+ rec_jet_ca_sub = recluster_ca_sub(jet_ca);
+ cout << "Reclustering with: " << recluster_ca_sub.description() << endl
+ << " " << rec_jet_ca_sub << endl;
+ pieces = rec_jet_ca_sub.pieces();
+ cout << " subjets: " << endl;
+ for (unsigned int i=0;i<pieces.size();i++)
+ cout << " " << pieces[i] << endl;
+ cout << endl;
+
+ // recluster with kt (small radius), keeping all subjets
+ rec_jet_kt_sub = recluster_kt_sub(jet_ca);
+ cout << "Reclustering with: " << recluster_kt_sub.description() << endl
+ << " " << rec_jet_kt_sub << endl;
+ pieces = rec_jet_kt_sub.pieces();
+ cout << " subjets: " << endl;
+ for (unsigned int i=0;i<pieces.size();i++)
+ cout << " " << pieces[i] << endl;
+ cout << endl;
+
+ return 0;
+}
+
+//----------------------------------------------------------------------
+/// read in input particles
+void read_event(vector<PseudoJet> &event){
+ string line;
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {return;}
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ event.push_back(particle);
+ }
+}
+
+//----------------------------------------------------------------------
+/// overloaded jet info output
+ostream & operator<<(ostream & ostr, const PseudoJet & jet) {
+ if (jet == 0) {
+ ostr << " 0 ";
+ } else {
+ ostr << " pt = " << jet.pt()
+ << " m = " << jet.m()
+ << " y = " << jet.rap()
+ << " phi = " << jet.phi()
+ << " ClusSeq = " << (jet.has_associated_cs() ? "yes" : "no");
+ }
+ return ostr;
+}
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_recluster.ref b/src/Tools/fjcontrib/RecursiveTools/example_recluster.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_recluster.ref
@@ -0,0 +1,64 @@
+# read an event with 354 particles
+--------------------------------------------------
+#--------------------------------------------------------------------------
+# FastJet release 3.1.0-devel
+# M. Cacciari, G.P. Salam and G. Soyez
+# A software package for jet finding and analysis at colliders
+# http://fastjet.fr
+#
+# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package
+# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210].
+#
+# FastJet is provided without warranty under the terms of the GNU GPLv2.
+# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code,
+# CGAL and 3rd party plugin jet algorithms. See COPYING file for details.
+#--------------------------------------------------------------------------
+Starting from a jet obtained from: Longitudinally invariant anti-kt algorithm with R = 1 and E scheme recombination
+ pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511 ClusSeq = yes
+
+Reclustering with: Recluster with subjet_def = Longitudinally invariant Cambridge/Aachen algorithm with R = 1000, a recombiner obtained from the jet being reclustered and keeping the hardest subjet
+ pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511 ClusSeq = yes
+
+Reclustering with: Recluster with subjet_def = Longitudinally invariant Cambridge/Aachen algorithm with R = 0.3, a recombiner obtained from the jet being reclustered and joining all subjets in a composite jet
+ pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511 ClusSeq = no
+ subjets:
+ pt = 980.937 m = 27.6178 y = -0.86753 phi = 2.90527 ClusSeq = yes
+ pt = 1.34048 m = 0.13498 y = -0.448775 phi = 2.76161 ClusSeq = yes
+ pt = 0.461349 m = 0.13957 y = -1.31787 phi = 3.17806 ClusSeq = yes
+ pt = 0.362421 m = 0.0359117 y = -0.593531 phi = 3.08425 ClusSeq = yes
+ pt = 0.241708 m = -3.12684e-06 y = -1.16407 phi = 2.42725 ClusSeq = yes
+ pt = 0.115239 m = 0.13957 y = -1.6844 phi = 2.54038 ClusSeq = yes
+
+Reclustering with: Recluster with subjet_def = Longitudinally invariant kt algorithm with R = 0.3, a recombiner obtained from the jet being reclustered and joining all subjets in a composite jet
+ pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511 ClusSeq = no
+ subjets:
+ pt = 982.621 m = 32.8883 y = -0.866837 phi = 2.90514 ClusSeq = yes
+ pt = 0.461349 m = 0.13957 y = -1.31787 phi = 3.17806 ClusSeq = yes
+ pt = 0.241708 m = -3.12684e-06 y = -1.16407 phi = 2.42725 ClusSeq = yes
+ pt = 0.115239 m = 0.13957 y = -1.6844 phi = 2.54038 ClusSeq = yes
+
+--------------------------------------------------
+Starting from a jet obtained from: Longitudinally invariant Cambridge/Aachen algorithm with R = 1 and E scheme recombination
+ pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511 ClusSeq = yes
+
+Reclustering with: Recluster with subjet_def = Longitudinally invariant Cambridge/Aachen algorithm with R = 1000, a recombiner obtained from the jet being reclustered and keeping the hardest subjet
+ pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511 ClusSeq = yes
+
+Reclustering with: Recluster with subjet_def = Longitudinally invariant Cambridge/Aachen algorithm with R = 0.3, a recombiner obtained from the jet being reclustered and joining all subjets in a composite jet
+ pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511 ClusSeq = no
+ subjets:
+ pt = 980.937 m = 27.6178 y = -0.86753 phi = 2.90527 ClusSeq = yes
+ pt = 1.34048 m = 0.13498 y = -0.448775 phi = 2.76161 ClusSeq = yes
+ pt = 0.461349 m = 0.13957 y = -1.31787 phi = 3.17806 ClusSeq = yes
+ pt = 0.362421 m = 0.0359117 y = -0.593531 phi = 3.08425 ClusSeq = yes
+ pt = 0.241708 m = -3.12684e-06 y = -1.16407 phi = 2.42725 ClusSeq = yes
+ pt = 0.115239 m = 0.13957 y = -1.6844 phi = 2.54038 ClusSeq = yes
+
+Reclustering with: Recluster with subjet_def = Longitudinally invariant kt algorithm with R = 0.3, a recombiner obtained from the jet being reclustered and joining all subjets in a composite jet
+ pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511 ClusSeq = no
+ subjets:
+ pt = 982.621 m = 32.8883 y = -0.866837 phi = 2.90514 ClusSeq = yes
+ pt = 0.461349 m = 0.13957 y = -1.31787 phi = 3.17806 ClusSeq = yes
+ pt = 0.241708 m = -3.12684e-06 y = -1.16407 phi = 2.42725 ClusSeq = yes
+ pt = 0.115239 m = 0.13957 y = -1.6844 phi = 2.54038 ClusSeq = yes
+
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_recursive_softdrop.cc b/src/Tools/fjcontrib/RecursiveTools/example_recursive_softdrop.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_recursive_softdrop.cc
@@ -0,0 +1,240 @@
+//----------------------------------------------------------------------
+/// \file example_recursive_softdrop.cc
+///
+/// This example program is meant to illustrate how the
+/// fastjet::contrib::RecursiveSoftDrop class is used.
+///
+/// Run this example with
+///
+/// \verbatim
+/// ./example_recursive_softdrop < ../data/single-event.dat
+/// \endverbatim
+//----------------------------------------------------------------------
+
+// $Id: example_recursive_softdrop.cc 1074 2017-09-18 15:15:20Z gsoyez $
+//
+// Copyright (c) 2017-, Gavin P. Salam, Gregory Soyez, Jesse Thaler,
+// Kevin Zhou, Frederic Dreyer
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iostream>
+#include <sstream>
+
+#include <iomanip>
+#include <cmath>
+#include "fastjet/ClusterSequence.hh"
+#include "RecursiveSoftDrop.hh" // In external code, this should be fastjet/contrib/RecursiveSoftDrop.hh
+
+using namespace std;
+using namespace fastjet;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &event);
+
+void print_prongs_with_clustering_info(const PseudoJet &jet, const string &pprefix);
+void print_raw_prongs(const PseudoJet &jet);
+
+ostream & operator<<(ostream &, const PseudoJet &);
+
+//----------------------------------------------------------------------
+int main(){
+
+ //----------------------------------------------------------
+ // read in input particles
+ vector<PseudoJet> event;
+ read_event(event);
+ cout << "# read an event with " << event.size() << " particles" << endl;
+
+ // first get some anti-kt jets
+ double R = 1.0, ptmin = 100.0;
+ JetDefinition jet_def(antikt_algorithm, R);
+ ClusterSequence cs(event, jet_def);
+ vector<PseudoJet> jets = sorted_by_pt(cs.inclusive_jets(ptmin));
+
+ //----------------------------------------------------------------------
+ // give the soft drop groomer a short name
+ // Use a symmetry cut z > z_cut R^beta
+ // By default, there is no mass-drop requirement
+ double z_cut = 0.2;
+ double beta = 0.5;
+ int n=4; // number of layers (-1 <> infinite)
+ contrib::RecursiveSoftDrop rsd(beta, z_cut, n, R);
+
+ // keep addittional structure info (used below)
+ rsd.set_verbose_structure(true);
+
+ // (optionally) use the same-depth variant
+ //
+ // instead of recursing into the largest Delta R branch until "n+1"
+ // branches hav ebeen found, the same-depth variant recurses n times
+ // into all the branches found in the previous iteration
+ //
+ //rsd.set_fixed_depth_mode();
+
+ // (optionally) use a dynamical R0
+ //
+ // Instead of being normalised by the initial jet radios R0, angles
+ // are notrmalised by the delta R of the previous iteration
+ //
+ rsd.set_dynamical_R0();
+
+ // (optionally) recurse only in the hardest branch
+ //
+ // Instead of recursing into both branches found by the previous
+ // iteration, only keep recursing into the hardest one
+ //
+ //rsd.set_hardest_branch_only();
+
+
+ //----------------------------------------------------------------------
+ cout << "RecursiveSoftDrop groomer is: " << rsd.description() << endl;
+
+ for (unsigned ijet = 0; ijet < jets.size(); ijet++) {
+ // Run SoftDrop and examine the output
+ PseudoJet rsd_jet = rsd(jets[ijet]);
+ cout << endl;
+ cout << "original jet: " << jets[ijet] << endl;
+ cout << "RecursiveSoftDropped jet: " << rsd_jet << endl;
+
+ assert(rsd_jet != 0); //because soft drop is a groomer (not a tagger), it should always return a soft-dropped jet
+
+ // print the prong structure of the jet
+ //
+ // This can be done in 2 ways:
+ //
+ // - either keeping the clustering information and get the
+ // branches as a succession of 2->1 recombinations (this is
+ // done calling "pieces" recursively)
+ cout << endl
+ << "Prongs with clustering information" << endl
+ << "----------------------------------" << endl;
+ print_prongs_with_clustering_info(rsd_jet, " ");
+ //
+ // - or getting all the branches in a single go (done directly
+ // through the jet associated structure)
+ cout << endl
+ << "Prongs without clustering information" << endl
+ << "-------------------------------------" << endl;
+ print_raw_prongs(rsd_jet);
+
+ cout << "Groomed prongs information:" << endl;
+ cout << "index zg thetag" << endl;
+ vector<pair<double, double> > ztg = rsd_jet.structure_of<contrib::RecursiveSoftDrop>().sorted_zg_and_thetag();
+ for (unsigned int i=0; i<ztg.size();++i)
+ cout << setw(5) << i+1
+ << setw(14) << ztg[i].first << setw(14) << ztg[i].second << endl;
+
+ }
+
+ return 0;
+}
+
+//----------------------------------------------------------------------
+// print the prongs inside the jet, showing the clustering info
+void print_prongs_with_clustering_info(const PseudoJet &jet, const string &prefix){
+ if (prefix.size() == 1){
+ cout << " " << setw(14) << " "
+ << setw(8) << "branch" << setw(14) << "branch"
+ << setw(10) << "N_groomed"
+ << setw(11) << "max loc"
+ << setw(22) << "substructure" << endl;
+ cout << " " << setw(14) << " "
+ << setw(8) << "pt" << setw(14) << "mass"
+ << setw(5) << "loc"
+ << setw(5) << "tot"
+ << setw(11) << "zdrop"
+ << setw(11) << "zg"
+ << setw(11) << "thetag"<< endl;
+ }
+ const contrib::RecursiveSoftDrop::StructureType &structure = jet.structure_of<contrib::RecursiveSoftDrop>();
+ double dR = structure.delta_R();
+ cout << " " << left << setw(14) << (prefix.substr(0, prefix.size()-1)+"+--> ") << right
+ << setw(8) << jet.pt() << setw(14) << jet.m()
+ << setw(5) << structure.dropped_count(false)
+ << setw(5) << structure.dropped_count()
+ << setw(11) << structure.max_dropped_symmetry(false);
+
+ if (structure.has_substructure()){
+ cout << setw(11) << structure.symmetry()
+ << setw(11) << structure.delta_R();
+ }
+ cout << endl;
+
+ if (dR>=0){
+ vector<PseudoJet> pieces = jet.pieces();
+ assert(pieces.size()==2);
+ print_prongs_with_clustering_info(pieces[0], prefix+" |");
+ print_prongs_with_clustering_info(pieces[1], prefix+" ");
+ }
+}
+
+//----------------------------------------------------------------------
+// print all the prongs inside the jet (no clustering info)
+void print_raw_prongs(const PseudoJet &jet){
+ cout << "(Raw) list of prongs:" << endl;
+ if (!jet.has_structure_of<contrib::RecursiveSoftDrop>()){
+ cout << " None (bad structure)" << endl;
+ return;
+ }
+
+ cout << setw(5) << " " << setw(11) << "pt" << setw(14) << "mass" << endl;
+
+ vector<PseudoJet> prongs = contrib::recursive_soft_drop_prongs(jet);
+ for (unsigned int iprong=0; iprong<prongs.size(); ++iprong){
+ const PseudoJet & prong = prongs[iprong];
+ const contrib::RecursiveSoftDrop::StructureType &structure = prong.structure_of<contrib::RecursiveSoftDrop>();
+ cout << setw(5) << iprong << setw(11) << prong.pt() << setw(14) << prong.m() << endl;
+
+ assert(!structure.has_substructure());
+ }
+ cout << endl;
+}
+
+//----------------------------------------------------------------------
+/// read in input particles
+void read_event(vector<PseudoJet> &event){
+ string line;
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {return;}
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ event.push_back(particle);
+ }
+}
+
+//----------------------------------------------------------------------
+/// overloaded jet info output
+ostream & operator<<(ostream & ostr, const PseudoJet & jet) {
+ if (jet == 0) {
+ ostr << " 0 ";
+ } else {
+ ostr << " pt = " << jet.pt()
+ << " m = " << jet.m()
+ << " y = " << jet.rap()
+ << " phi = " << jet.phi();
+ }
+ return ostr;
+}
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_recursive_softdrop.ref b/src/Tools/fjcontrib/RecursiveTools/example_recursive_softdrop.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_recursive_softdrop.ref
@@ -0,0 +1,83 @@
+# read an event with 354 particles
+#--------------------------------------------------------------------------
+# FastJet release 3.3.1-devel
+# M. Cacciari, G.P. Salam and G. Soyez
+# A software package for jet finding and analysis at colliders
+# http://fastjet.fr
+#
+# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package
+# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210].
+#
+# FastJet is provided without warranty under the terms of the GNU GPLv2.
+# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code
+# and 3rd party plugin jet algorithms. See COPYING file for details.
+#--------------------------------------------------------------------------
+RecursiveSoftDrop groomer is: recursive application of [Recursive Groomer with a symmetry cut scalar_z > 0.2 (theta/1)^0.5 [SoftDrop], no mass-drop requirement, recursion into the subjet with larger pt], applied N=4 times, with R0 dynamically scaled
+
+original jet: pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511
+RecursiveSoftDropped jet: pt = 811.261 m = 6.45947 y = -0.87094 phi = 2.9083
+
+Prongs with clustering information
+----------------------------------
+ branch branch N_groomed max loc substructure
+ pt mass loc tot zdrop zg thetag
+ +--> 811.261 6.45947 13 13 0.0294298 0.154333 0.0200353
+ +--> 669.635 1.98393 2 2 0
+ +--> 141.627 0.765329 0 0 0 0.199906 0.00734861
+ +--> 113.316 0.462946 0 0 0 0.208947 0.00550512
+ | +--> 89.6387 0.211913 0 0 0
+ | +--> 23.6769 0.13957 0 0 0
+ +--> 28.3123 0.170026 0 0 0 0.248173 0.00447786
+ +--> 21.286 0.13957 0 0 0
+ +--> 7.02636 -3.21461e-05 0 0 0
+
+Prongs without clustering information
+-------------------------------------
+(Raw) list of prongs:
+ pt mass
+ 0 669.635 1.98393
+ 1 89.6387 0.211913
+ 2 21.286 0.13957
+ 3 23.6769 0.13957
+ 4 7.02636 -3.21461e-05
+
+Groomed prongs information:
+index zg thetag
+ 1 0.154333 0.0200353
+ 2 0.199906 0.00734861
+ 3 0.208947 0.00550512
+ 4 0.248173 0.00447786
+
+original jet: pt = 908.098 m = 87.7124 y = 0.219482 phi = 6.03487
+RecursiveSoftDropped jet: pt = 830.517 m = 4.91035 y = 0.223054 phi = 6.02995
+
+Prongs with clustering information
+----------------------------------
+ branch branch N_groomed max loc substructure
+ pt mass loc tot zdrop zg thetag
+ +--> 830.517 4.91035 12 13 0.0232056 0.060784 0.0153863
+ +--> 778.731 3.66481 0 1 0 0.235041 0.0101382
+ | +--> 599.106 0.403809 1 1 0
+ | +--> 179.628 0.853363 0 1 0 0.25773 0.00871739
+ | +--> 131.15 0.378456 1 1 0.0606587 0.315246 0.00417298
+ | | +--> 89.8058 0.107191 0 0 0
+ | | +--> 41.3448 0.13957 0 0 0
+ | +--> 48.4785 0.13957 0 0 0
+ +--> 51.7916 0.13957 0 0 0
+
+Prongs without clustering information
+-------------------------------------
+(Raw) list of prongs:
+ pt mass
+ 0 599.106 0.403809
+ 1 51.7916 0.13957
+ 2 89.8058 0.107191
+ 3 48.4785 0.13957
+ 4 41.3448 0.13957
+
+Groomed prongs information:
+index zg thetag
+ 1 0.060784 0.0153863
+ 2 0.235041 0.0101382
+ 3 0.25773 0.00871739
+ 4 0.315246 0.00417298
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_softdrop.cc b/src/Tools/fjcontrib/RecursiveTools/example_softdrop.cc
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_softdrop.cc
@@ -0,0 +1,122 @@
+//----------------------------------------------------------------------
+/// \file example_softdrop.cc
+///
+/// This example program is meant to illustrate how the
+/// fastjet::contrib::SoftDrop class is used.
+///
+/// Run this example with
+///
+/// \verbatim
+/// ./example_softdrop < ../data/single-event.dat
+/// \endverbatim
+//----------------------------------------------------------------------
+
+// $Id: example_softdrop.cc 705 2014-07-07 14:37:03Z gsoyez $
+//
+// Copyright (c) 2014, Gavin P. Salam
+//
+//----------------------------------------------------------------------
+// This file is part of FastJet contrib.
+//
+// It is free software; you can redistribute it and/or modify it under
+// the terms of the GNU General Public License as published by the
+// Free Software Foundation; either version 2 of the License, or (at
+// your option) any later version.
+//
+// It is distributed in the hope that it will be useful, but WITHOUT
+// ANY WARRANTY; without even the implied warranty of MERCHANTABILITY
+// or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
+// License for more details.
+//
+// You should have received a copy of the GNU General Public License
+// along with this code. If not, see <http://www.gnu.org/licenses/>.
+//----------------------------------------------------------------------
+
+#include <iostream>
+#include <sstream>
+
+#include <sstream>
+#include <iomanip>
+#include <cmath>
+#include "fastjet/ClusterSequence.hh"
+#include "SoftDrop.hh" // In external code, this should be fastjet/contrib/SoftDrop.hh
+
+using namespace std;
+using namespace fastjet;
+
+// forward declaration to make things clearer
+void read_event(vector<PseudoJet> &event);
+ostream & operator<<(ostream &, const PseudoJet &);
+
+//----------------------------------------------------------------------
+int main(){
+
+ //----------------------------------------------------------
+ // read in input particles
+ vector<PseudoJet> event;
+ read_event(event);
+ cout << "# read an event with " << event.size() << " particles" << endl;
+
+ // first get some anti-kt jets
+ double R = 1.0, ptmin = 20.0;
+ JetDefinition jet_def(antikt_algorithm, R);
+ ClusterSequence cs(event, jet_def);
+ vector<PseudoJet> jets = sorted_by_pt(cs.inclusive_jets(ptmin));
+
+ // give the soft drop groomer a short name
+ // Use a symmetry cut z > z_cut R^beta
+ // By default, there is no mass-drop requirement
+ double z_cut = 0.10;
+ double beta = 2.0;
+ contrib::SoftDrop sd(beta, z_cut);
+ cout << "SoftDrop groomer is: " << sd.description() << endl;
+
+ for (unsigned ijet = 0; ijet < jets.size(); ijet++) {
+ // Run SoftDrop and examine the output
+ PseudoJet sd_jet = sd(jets[ijet]);
+ cout << endl;
+ cout << "original jet: " << jets[ijet] << endl;
+ cout << "SoftDropped jet: " << sd_jet << endl;
+
+ assert(sd_jet != 0); //because soft drop is a groomer (not a tagger), it should always return a soft-dropped jet
+
+ cout << " delta_R between subjets: " << sd_jet.structure_of<contrib::SoftDrop>().delta_R() << endl;
+ cout << " symmetry measure(z): " << sd_jet.structure_of<contrib::SoftDrop>().symmetry() << endl;
+ cout << " mass drop(mu): " << sd_jet.structure_of<contrib::SoftDrop>().mu() << endl;
+ }
+
+ return 0;
+}
+
+//----------------------------------------------------------------------
+/// read in input particles
+void read_event(vector<PseudoJet> &event){
+ string line;
+ while (getline(cin, line)) {
+ istringstream linestream(line);
+ // take substrings to avoid problems when there are extra "pollution"
+ // characters (e.g. line-feed).
+ if (line.substr(0,4) == "#END") {return;}
+ if (line.substr(0,1) == "#") {continue;}
+ double px,py,pz,E;
+ linestream >> px >> py >> pz >> E;
+ PseudoJet particle(px,py,pz,E);
+
+ // push event onto back of full_event vector
+ event.push_back(particle);
+ }
+}
+
+//----------------------------------------------------------------------
+/// overloaded jet info output
+ostream & operator<<(ostream & ostr, const PseudoJet & jet) {
+ if (jet == 0) {
+ ostr << " 0 ";
+ } else {
+ ostr << " pt = " << jet.pt()
+ << " m = " << jet.m()
+ << " y = " << jet.rap()
+ << " phi = " << jet.phi();
+ }
+ return ostr;
+}
diff --git a/src/Tools/fjcontrib/RecursiveTools/example_softdrop.ref b/src/Tools/fjcontrib/RecursiveTools/example_softdrop.ref
new file mode 100644
--- /dev/null
+++ b/src/Tools/fjcontrib/RecursiveTools/example_softdrop.ref
@@ -0,0 +1,33 @@
+# read an event with 354 particles
+#--------------------------------------------------------------------------
+# FastJet release 3.0.6
+# M. Cacciari, G.P. Salam and G. Soyez
+# A software package for jet finding and analysis at colliders
+# http://fastjet.fr
+#
+# Please cite EPJC72(2012)1896 [arXiv:1111.6097] if you use this package
+# for scientific work and optionally PLB641(2006)57 [hep-ph/0512210].
+#
+# FastJet is provided without warranty under the terms of the GNU GPLv2.
+# It uses T. Chan's closest pair algorithm, S. Fortune's Voronoi code
+# and 3rd party plugin jet algorithms. See COPYING file for details.
+#--------------------------------------------------------------------------
+SoftDrop groomer is: Recursive Groomer with a symmetry cut scalar_z > 0.1 (theta/1)^2 [SoftDrop], no mass-drop requirement, recursion into the subjet with larger pt
+
+original jet: pt = 983.387 m = 39.9912 y = -0.867307 phi = 2.90511
+SoftDropped jet: pt = 980.44 m = 27.1382 y = -0.867485 phi = 2.90532
+ delta_R between subjets: 0.209158
+ symmetry measure(z): 0.0047049
+ mass drop(mu): 0.835262
+
+original jet: pt = 908.098 m = 87.7124 y = 0.219482 phi = 6.03487
+SoftDropped jet: pt = 887.935 m = 11.3171 y = 0.223247 phi = 6.03034
+ delta_R between subjets: 0.111631
+ symmetry measure(z): 0.00440752
+ mass drop(mu): 0.791013
+
+original jet: pt = 72.9429 m = 23.4022 y = -1.19083 phi = 6.1199
+SoftDropped jet: pt = 71.5847 m = 20.0943 y = -1.1761 phi = 6.12539
+ delta_R between subjets: 0.680305
+ symmetry measure(z): 0.0730158
+ mass drop(mu): 0.56265

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