diff --git a/.hgignore b/.hgignore --- a/.hgignore +++ b/.hgignore @@ -1,109 +1,111 @@ ~$ ^(anas|test|run).*$ \.orig$ \.(o|Po|lo|Plo|la|a|so|dylib|pyc|tar\.bz2|tar\.gz|fifo|hepmc)$ ^config\.guess$ ^config\.status$ ^config\.sub$ ^config\.log$ ^configure$ ^depcomp$ ^compile$ ^ar-lib$ ^install-sh$ ^INSTALL$ ^libtool$ ^test-driver$ ^ltmain\.sh$ ^m4/ltoptions\.m4$ ^m4/ltsugar\.m4$ ^m4/ltversion\.m4$ ^m4/lt~obsolete\.m4$ ^missing$ ^autom4te\.cache$ ^include/Rivet/Config/stamp-h.$ ^tmp$ ^rivet.pc$ Makefile$ Makefile\.in$ \.(pdf|toc|bbl|blg|sty|bib|html|tex)$ Doxyfile$ +doxy/html/.* +doxy/latex/.* \.libs$ \.deps$ #Rivet.yoda #.*/Rivet\.yoda ^bin/rivet-buildplugin$ ^bin/rivet-config$ ^bin/rivet-nopy$ ^aclocal\.m4$ ^pyext/build$ ^pyext/rivet/core.cpp$ ^pyext/rivet/rivetwrap\.py$ ^pyext/rivet/rivetwrap_wrap\.cc$ ^pyext/rivet/fix-out-of-source$ ^pyext/setup\.py$ ^rivetenv\.(sh|csh)$ ^test/test(Api|Cmp|NaN)$ ^include/Rivet/Config/DummyConfig\.hh\.in$ ^include/Rivet/Config/BuildOptions\.hh$ ^include/Rivet/Config/DummyConfig\.hh$ ^include/Rivet/Config/RivetConfig\.hh$ ^doc/.*\.(log|aux|out)$ ^doc/ana ^test/log$ ^test/.*\.log$ ^test/out\.yoda$ ^test/NaN.aida$ ^test/Rivet.yoda$ ^test/testBoost$ ^test/.*\.trs$ ^test/testMatVec$ ^test/testMath$ ^test/testBeams$ ^dev$ ^devval$ ^newanalyses$ ^.*plots$ ^a\.out$ ^a\.out\.dSYM$ ^Rivet-.\..\..$ ^local/.*$ ^(for|analyses)\d\d\d$ ^analyses/data$ # added by aHg on Mon Feb 25 14:51:05 2019 syntax: glob bin/LHC-13-Jets-0.hepmc.gz # added by aHg on Mon Feb 25 16:16:10 2019 syntax: glob bin/*.gz # added by aHg on Thu Feb 28 11:44:29 2019 syntax: glob bin/hepmc-compress # added by aHg on Tue Mar 5 14:30:12 2019 syntax: glob doc/rivet-manual.dvi # added by aHg on Tue Mar 5 14:30:21 2019 syntax: glob doc/rivet-manual.ps # added by aHg on Fri Mar 15 10:38:23 2019 syntax: glob bin/rivet-hepmz # added by aHg on Fri Mar 15 10:38:43 2019 syntax: glob bin/converall.log # added by aHg on Fri Mar 15 10:38:48 2019 syntax: glob bin/converall.sh ^doxy/.*$ # added by aHg on Tue May 28 11:20:16 2019 syntax: glob bin/hepmc-compress diff --git a/ChangeLog b/ChangeLog --- a/ChangeLog +++ b/ChangeLog @@ -1,6925 +1,6974 @@ +2019-06-01 Peter Richardson + * update yoda for ARGUS_1993_S2653028, improved y errors, still zero bin width issues + * update yoda for SND_2016_I1471515, ALEPH_1995_I382179, ALEPH_1999_S4193598 + * add analysis CLEO_1991_I29927, B* production in e+e- + +2019-05-31 Christian Gutschow + + * Skip beam particles when trying to determine promptness (thanks to Marek Schoenherr for pointing this out) + * Apple's CLANG compiler really doesn't like uninitialised variables ... sorry Peter! + + +2019-05-29 Andy Buckley + + * Use integer rather than overloaded Projection comparison at the + apply stage. Improves Smeared* projection reproducibility and may + speed up the apply step. Thanks to Xiangyang Ju. + +2019-05-29 Peter Richardson + * Move BABAR and BELLE analyses to separate plugin and add new mainly radiative + return analyses + + * new pluginNovosibirsk with analyses from SND, CMD, etc + + * new pluginOrsay with analyses from DM1 and DM2 + + * new PETRA analyses, mainly for R + + * move existing Tristan analyses to separate plugin and add new, mainy R + analyses + + * new pluginFrascati with analyses from ADONE and DAPHNE + + * move older SLAC e+e- analyses to separate plugin and add new analyses + + * move DORIS analysis to separate plugin and add new ones + + * move CLEO analyses to new CESR plugin and add more analyses + + * new plugin with analyses from the BES experiment + + * new MC analyses for hadron/tau decays based on Herwig internal ones + + * sync BABAR_2007_I729388, BABAR_2013_I1238276, BABAR_2005_S6181155 and all those + where no difference with yodadiff, similarly for BELLE + + * fix no of tracks plots in ATLAS_2016_I1424838, normalise to 100 not 1, agreed by Chris G + + * merge two versions of OPAL_2004_I631361, now using new options feature instead. + 2019-05-29 Leif Lönnblad * The GenEvents in rivet can now be stripped from (most) light quarks and gluons to speed up searching. * Status lines in info files can now contain words like NOTREENTRY, NOHEPDATA, SINGLEWEIGHT, and UNPHYSICAL. * Can now configured to use HepMC3 (3.1.1 or later). - + 2019-05-23 Andy Buckley * Fix Unicode and argparse bugs in bin/rivet. Thanks to Frank Siegert. 2019-05-21 Andy Buckley * Release version 2.7.2 * Fixes to CMS_2016_I1487288 jet selection and normalisation. Thanks to Peter Richardson for highlighting the issues. 2019-05-20 Andy Buckley * Improve Vector3::azimuthalAngle() (also used by FourMomentum and FourVector) to use exact rather than fuzzy is-zero check, to only check the perpendicular components, and to note that IEEE floating point implementations of atan2 should already be 'safe' unless we decide that this function should throw or return NaN in case of null or along-z vectors. Thanks to Louis Moureaux from CMS for the report and diagnosis. 2019-05-17 Andy Buckley * Tools/Utils.h: Add isum() functions, and mark other container functions as wanting a conversion to use std::function. 2019-05-16 Andy Buckley * Add super-generic (i)discardIfAny(particlebases, particlebases, bool(pb,pb)) functions. 2019-05-16 Christian Gutschow * Introduce TTMODE options for MC_TTBAR to pick the decay mode 2019-05-09 Christian Gutschow * Release version 2.7.1 2019-05-09 Christian Gutschow * add correlation information for those analyses that are compatible with HEPData * prevent Variations meta data from being copied * comment out redudnant code in MeasureDefinition.cc to suppress compiler warning 2019-05-08 Andy Buckley * Use an std::map rather than std::set to store analyses in AnalysisHandler, hopefully therefore fixing the analysis evaluation order and making multi-analysis runs with random numbers repeatable. 2019-05-07 Andy Buckley * Modify LorentzTransform::setBetaVec to behave better for boost along x, y, and z axes. * Attach bare lepton GenParticle pointers to output of DressedLeptons, to allow ancestry/decay navigation (request by Markus Seidel). * Add Particle::setGenParticle method and manual Particle constructors with the option to pass a GenParticle*. * Improve DressedLeptons constructor to deconstruct incoming particles into bare and dressing components (report by Markus Seidel). * Remove GSL includes and single remaining method (for now). 2019-05-06 Andy Buckley * First set of script conversions from optparse to argparse for Python3. 2019-05-06 Peter Richardson * Fix normalisation in ATLAS_2016_I1444991 after yoda update from HepData 2019-05-04 Christian Gutschow * default entry point of ATLAS_2014_I1319490 should be average of muon and electron channel * fix units in ATLAS_2014_I1319490 and apply Peter Richardson's plot updates 2019-05-04 Peter Richardson * Fix plot selection and labels in ATLAS_2016_I1419652 (due yoda update from HepData) * Fix to mode switch and plot labels in ATLAS_2014_I1319490 2019-05-03 Peter Richardson * Fix info text and plot labels in ATLAS_2013_I1217863 * Fix Zfinder test in ATLAS_2014_I1312627, size is now no of Z's not leptons 2019-05-02 Peter Richardson * Fix unicode in ATLAS_2014_I1312627,ATLAS_2016_I1424838,ATLAS_2016_I1426523 2019-05-02 Peter Richardson * Fix make-plots CustomMajorTicks and CustomMinorTicks 2019-04-30 Peter Richardson * Fix make-plots rendering when last point is NaN-valued. 2019-04-30 Christian Gutschow * path sign behaviour in deltaEta (MathUtils.hh) * add signed option for deltaRap 2019-04-29 Andy Buckley * Add tau mistag efficiency functions for jet smearing. * Make RIVET_RANDOM_SEED have effect outside OpenMP builds, too. 2019-04-29 Christian Gutschow * remove IsRef from output Histo1D * fix HEPData IDs in hist booking for ATLAS_2014_I1315949 2019-04-26 Christian Gutschow * use jet size rather than 4-momentum size (?) to fill in CDF_1996_S3108457 2019-04-25 Christian Gutschow * fix mapping to ref data in STAR_2006_S6500200, put bin width manually into ref data file 2019-04-24 Christian Gutschow * Patch weird behaviour in ATLAS_2017_I1589844 and ATLAS_2017_I1609448 when Cut argument is passed to VetoedFinalState constructor. In version 2.6.2 or prior, this would select the particles passing the cut, after that they are being vetoed. 2019-04-24 Andy Buckley * Add CMS_2016_I1487288 (CMS WZ differential cross-sections at 8 TeV) from Shehu AbdusSalam, refined and extended to jet distributions by AB. 2019-04-24 Jon Butterworth * Fix logic of call the vetoedFinalState in ATLAS_2017_I1609448 which was giving wrong met calculation. 2019-04-23 Chris Gutschow * Apply suggested corrections from Peter Richardson to ATLAS_2014_I1282441 (normalisation of second plot is in millibarn not microbarn), ATLAS_2015_I1387176 and ATLAS_2015_I1397635 (Unicode issues in the .info), ATLAS_2016_I1419070 (need more than 1 entry for a variance not just 1), CMS_2010_PAS_QCD_10_024 and CMS_2012_PAS_FSQ_12_020 (class names need to be consistent with file names to find the .yoda ref data), CMS_2013_I1261026 (need to ensure more than 1 entry in histos to avoid LowStats issues from YODA), CMS_2014_I1298810, CMS_2016_I1421646, CMS_2016_I1454211 (the polymarker command in the yoda caused make-plots to fail if there is more than 1 MC line), CMS_2017_I1467451 (cross sections in fb), CMS_2017_I1605749 (data fixed in HepData so don't need to divide by bin width anymore), ALEPH_1996_S3486095 (delete a lot of unused variables), ALEPH_2014_I1267648 (only worked if the final decay products were direct children of the tau, which is not the case in Herwig or Pythia -- rewritten to search down the decay tree), DELPHI_1996_S3430090, DELPHI_2000_S4328825, OPAL_1998_S374990, ARGUS_1993_S2669951, ALEPH_1996_S3486095 (switch ' to ^\prime in plots as it wasn't working as it was), ALEPH_2004_S5765862 (fix typo in plot label), BABAR_2003_I593379 and BELLE_2008_I786560 (switch to Rivet particle from genParticle), and to add the 2D case to the Sphericity projection so tranSphericity works. 2019-04-23 Andy Buckley * Add RIVET_CACHE_PROJECTIONS environment variable, for runtime disabling of the caching mechanism (for debugging and cross-checking). * Add optional only_physical and remove_duplicates args (passed through to the Particle methods) to hasParticleAncestorWith and hasParticleDescendantWith functors. 2019-04-08 Przemyslaw Karczmarczyk * Restored behaviour of getData function to return finalized plots by default 2019-04-03 Andy Buckley * Remove/protect against last Unicode .encode() calls that broke Python3 compatibility. * Remove last assert (for mod2() >= 0) from Vector classes. 2019-04-01 Andy Buckley * Move inline projections *inside* analysis classes, since our aggregated build mechanism means there's no longer a unique unnamed namespace for each analysis .cc file. * Adding analyses ATLAS_2018_I1677498 (WWbb), ATLAS_2018_I1711114 (g -> bb), and ATLAS_2019_I1720442 (4-lepton lineshape). 2019-03-19 Andy Buckley * Extend more deltaPhi(x,y) functions with an optional bool for signed dPhi. * Add Particle::isSame and isSame(Particle, Particle) functions in lieu of implicit (and wrong) Particle::operator==. * Reinstate Particle -> GenParticle as an explicit cast option. 2019-03-15 Leif Lönnblad * src/Projections/Sphericity.cc: Skip zero-momentum particles. * [Reader,Writer]CompressedAscii[cc,hh]: Introduced possibility to wead and write HepMC (v3) files in a compressed and stripped format. Also included a simple progra bin/rivet-hepmz to convert between this new format and othe HepMC fortmats. 2019-03-15 Andy Buckley * Add CMS_2018_I1686000.cc single-top plus photon analysis (with an info file warning about fiducial definition oddity) * Remove Particle -> GenParticle implicit cast. * analyses/pluginCMS/CMS_2018_I1682495.cc: Fix normalisation of final plots (patch from Sal Rappoccio, spot by Deepak Kar) 2019-02-27 Andy Buckley * bin/make-plots: Fix a few Py2/3 incompabilities in make-plots. Thanks to Leif Gellersen for the tip-off * analyses/Makefile.am: Adopt a more make-friendly plugin building rule. Thanks to Dima Konstantinov. 2019-02-24 Jon Butterworth * Fix multiple bugs in ATLAS_2017_I1514251 (Z+jets) including a problem with REF data having zero bin widths 2019-02-23 Jon Butterworth * Added first version of ZEUS_2012_I1116258 (dijet photoproduction). Currently works but unvalidated, need to check exact recombination scheme with ZEUS contacts. Note ZEUS_2001_S4815815 also needs the recombination scheme checking. (Now done; changed to Et scheme are checking original code, 27/2/19.) 2019-02-20 Andy Buckley * Move UnstableParticles to a consistently-named header, with UnstableFinalState.hh retained for backward compatibility. * Improve/fix UnstableParticles projection's Cut constructor argument to apply the cut on a Rivet::Particle rather than a HepMC::FourVector, meaning that PID cuts can now be used. 2019-02-17 Andy Buckley * Convert ATLAS_2013_I1217863 analysis variants to use the LMODE analysis option (from Jon Butterworth). 2019-02-20 James Monk * src/Tools/RivetHepMC_2.cc: implementation of HepMC helper funcs for HepMC2 * Add HepMCUtils namespace for helper funcs * Relatives class spoofs HepMC3::Relatives interface using HepMC2 iterator_ranges * Replace calls to particles_in() and particles_out() by HepMCUtils::particles * Fix pyext/setup.py.in for both HepMC2 and HepMC3 * Configures with either --with-hepmc=/blah or --with-hepmc3=/blah * Compiles for either HepMC2 or HepMC3 (3.1 or higher) 2019-02-17 James Monk * Update many build paths to cope with new HepMC3 include and lib paths :( * Use RivetHepMC namespace in place of HepMC:: RivetHepMC.hh should take care of it * configure.ac addes appropriate define to CPPFLAGS * wrangle rivet-buildplugin to cope with HePMC3 paths * HepMC::Reader is still a bit fubar :( 2018-12-10 James Monk * Merge from default 2018-12-06 James Monk * RivetHepMC.hh: Much simplified. Use only Const version of GenParticlePtr Only func delarations - two separate implementation files for HepMC2 or 3 * configure.ac: HepMC version dependence for building RivetHepMC_2.cc or RivetHepMC_3.cc * src/Makefile.am: HepMC version dependence * src/Tools/RivetHepMC_3.cc: implementations of funs for HepMC v3 * bin/rivet-nopy.cc: re-implement using HepMC3 reader interface (may need separate implementation for HepMC2) * Particle.hh, Event.cc, Jet.cc: const GenParticle replaced by ConstGenParticle * Projections Beam, DISLepton, FinalPartons, FinalState, HeavyHadrons, InitialQuarks, MergedFinalState, PrimaryHadrons, UnstableFinalState, VetoedFinalState: Use ConstGenParticlePtr and vector consistently * pluginATLAS: Start to fix some uses of const GenParticlePtr 2019-02-15 Leif Lönnblad * Release 2.7.0 2019-02-12 Christian Bierlich * Introduced CentralityProjection, allowing an analysis to cut on percentiles of single event quantities, preloaded from a user generated or supplied (by experiment) histogram. Notably used for the centrality definition in heavy ion analyses. User specifies the centrality definition as a special analysis option called cent, eg: "MyAnalysis:cent=GEN". Example usage: Calibration analysis: MC_Cent_pPb_Calib, Analysis using that calibration: MC_Cent_pPb_Eta. * Introduced EventMixingFinalState to provide simple event mixing functionality. Currently only works with unit event weights. Example usage: ALICE_2016_I1507157. * Introduced Correlators, a framework for calculating single event correlators based on the generic framework (arXiv: 1010.0233 and arXiv: 1312.3572), and perfoming all event averages giving flow coefficents. Implemented as new analysis base class. Example usage: ALICE_2016_I1419244. * Introduced a PrimaryParticle projection, replicating experimental definitions of stable particles through decay chains. Recommended for analyses which would otherwise have to require stable particles at generator level. * Introduced AliceCommon and AtlasCommon convenience tools, defining several triggers, primary particle definitions and acceptances. * Contributed, validated analyses using above features: ALICE_2010_I880049: Multiplicity at mid-rapidity, PbPb @ 2.76 TeV/nn. ALICE_2012_I1127497: Nuclear modification factor, PbPb @ 2.76 TeV/nn. ALICE_2012_I930312: Di-hadron correlations, PbPb @ 2.76 TeV/nn. * Contributed, unvalidated analyses using above features: BRAHMS_2004_I647076: pi, K, p spectra as function of rapidity, AuAu @ 200 GeV/nn ALICE_2012_I1126966: pi, K, p spectra, PbPb @ 2.76 TeV/nn. ALICE_2013_I1225979: Charged multiplicity, PbPb @ 2.76 TeV/nn. ALICE_2014_I1243865: Multi-strange baryons, PbPb @ 2.76 TeV/nn. ALICE_2014_I1244523: Multi-strange baryons, pPb @ 5.02 TeV/nn. ALICE_2015_PBPBCentrality: Centrality calibration for PbPb. Note that the included 5.02 TeV/nn data is not well defined at particle level, and cannot be compared to experiment without full detector simulation. ALICE_2016_I1394676: Charged multiplicity, PbPb @ 2.76 TeV/nn. ALICE_2016_I1419244: Multiparticle correlations (flow) using generic framework, PbPb @ 5.02 TeV/nn. ALICE_2016_I1471838: Multi-strange baryons, pp @ 7 TeV. ALICE_2016_I1507090: Charged multiplicity, PbPb @ 5.02 TeV/nn. ALICE_2016_I1507157: Angular correlations, pp @ 7 TeV. ATLAS_2015_I1386475: Charged multiplicity, pPb @ 5.02 TeV/nn. ATLAS_PBPB_CENTRALITY: Forward energy flow + centrality calibration, data not unfolded, but well defined at particle level, PbPb @ 2.76 TeV/nn. ATLAS_2015_I1360290: Charged multiplicity + spectra, PbPb @ 2.76 TeV/nn. ATLAS_pPb_Calib: Forward energy flow + centrality calibration, data not unfolded, but well defined at particle level, pPb @ 5.02 TeV/nn. STAR_2016_I1414638: Di-hadron correlations, AuAu @ 200 GeV/nn. CMS_2017_I1471287: Multiparticle correlations (flow) using generic framework, pp @ 7 TeV. * Contributed analyses without data: ALICE_2015_PPCentrality: ALICE pp centrality (multiplicity classes) calibration. BRAHMS_2004_CENTRALITY: BRAHMS centrality calibration. STAR_BES_CALIB: STAR centrality calibration. MC_Cent_pPb_Calib: Example analysis, centrality calibration. MC_Cent_pPb_Eta: Example analysis, centrality usage. 2019-01-29 Andy Buckley * 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 * 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 * Add setting of cross-section error in AnalysisHandler and Run. 2018-12-21 Andy Buckley * Add hasNoTag jet-classification functor, to complement hasBTag and hasCTag. 2018-12-20 Andy Buckley * 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 * Add a FIRST/LAST enum switch for PartonicTops, to choose which top quark clone to use. 2018-12-14 Andy Buckley * Add a FastJet clustering mode for DressedLeptons. 2018-12-10 Andy Buckley * 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 * 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 * 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 * Merge ATLAS_2017_I1517194_MU and ATLAS_2018_I1656578. * Add signed calculation optional bool argument on all deltaPhi functions. 2018-11-12 Andy Buckley * Fix CMS_2012_I1102908 efficiency calculation. Thanks to Anton Karneyeu! 2018-11-09 Andy Buckley * Remove doc dir from default top-level make 2018-09-20 Andy Buckley * 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 * Update embedded yaml-cpp to v0.6.0. 2018-08-29 Andy Buckley * Add RIVET_WEIGHT_INDEX=-1 -> ignore event weights behaviour. Slow, but sometimes useful for debug. 2018-08-29 Christian Gutschow * 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 * Version 2.6.1 release. 2018-08-08 Andy Buckley * Add a RIVET_RANDOM_SEED variable to fix the smearing random-seed engine for validation comparisons. 2018-07-19 Andy Buckley * 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 * Fix HepData tarball download handling: StringIO is *not* safe anymore 2018-07-08 Andy Buckley * Add LorentzTransform factory functions direct from FourMomentum, and operator()s 2018-06-20 Andy Buckley * 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 * Fix installation of (In)DirectFinalState.hh 2018-05-31 Andy Buckley * 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 * Include 'unphysical' photon parents in PartonicTops' veto of prompt leptons from photon conversions. 2018-05-20 Andy Buckley * 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 * Make CmpAnaHandle::operator() const, for GCC 8 (thanks to CMS) 2018-05-07 Andy Buckley * 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 * 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 * 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 * 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 * Add RatioPlotLogY key to make-plots. Thanks to Antonin Maire. 2018-02-22 Andy Buckley * 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 * 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 * Add highlighted source to HTML analysis metadata listings. 2017-12-21 Andy Buckley * Version 2.6.0 release. 2017-12-20 Andy Buckley * Typo fix in TOTEM_2012_I1220862 data -- thanks to Anton Karneyeu. 2017-12-19 Andy Buckley * Adding contributed analyses: 1 ALICE, 6 ATLAS, 1 CMS. * Fix bugged PID codes in MC_PRINTEVENT. 2017-12-13 Andy Buckley * Protect Run methods and rivet script against being told to run from a missing or unreadable file. 2017-12-11 Andy Buckley * Replace manual event count & weight handling with a YODA Counter object. 2017-11-28 Andy Buckley * 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 * Various improvements to DISKinematics, DISLepton, and the ZEUS 2001 analysis. 2017-11-06 Andy Buckley * Extend AOPath regex to allow dots and underscores in weight names. 2017-10-27 Andy Buckley * 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 * Embed zstr and enable transparent reading of gzipped HepMC streams. 2017-10-03 Andy Buckley * Use Lester MT2 bisection header, and expose a few more mT2 function signatures. 2017-09-26 Andy Buckley * 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 * Add deltaR2 functions for squared distances. 2017-09-10 Andy Buckley * Add white backgrounds to make-plots main and ratio plot frames. 2017-09-05 Andy Buckley * 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 * 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 * Protect make-plots against NaNs in error band values (patch from Dmitry Kalinkin). 2017-07-20 Andy Buckley * 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 * 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. 2017-07-18 Andy Buckley * Enable methods for booking of Histo2D and Profile2D from Scatter3D reference data. * Remove IsRef annotation from autobooked histogram objects. 2017-07-17 Andy Buckley * Add pair-smearing to SmearedJets. 2017-07-08 Andy Buckley * Add Event::centrality(), for non-HepMC access to the generator value if one has been recorded -- otherwise -1. 2017-06-28 Andy Buckley * Split the smearing functions into separate header files for generic/momentum, Particle, Jet, and experiment-specific smearings & efficiencies. 2017-06-27 Andy Buckley * Add 'JetFinder' alias for JetAlg, by analogy with ParticleFinder. 2017-06-26 Andy Buckley * 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 * Add portable OpenMP enabling flags to AM_CXXFLAGS. 2017-06-22 Andy Buckley * 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 * 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 * Fix normalisations in CMS_2016_I1454211. * Fix analysis name in ref histo paths for ATLAS_2017_I1591327. 2017-06-18 Andy Buckley * Move all standard plugin files into subdirs of src/Analyses, with some custom make rules driving rivet-buildplugin. 2017-06-18 David Grellscheid * Parallelise rivet-buildplugin, with source-file cat'ing and use of a temporary Makefile. 2016-06-18 Holger Schulz * Version 2.5.4 release! 2016-06-17 Holger Schulz * 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 * 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 * 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 * 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 * 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 * 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 * 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 * Tidy ALEPH_1999 charm fragmentation analysis and normalise to data integral. Added DSTARPLUS and DSTARMINUS to PID. 2017-05-16 Andy Buckley * 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 * 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 * Add ATLAS_2013_I1234228, high-mass Drell-Yan at 7 TeV. 2017-05-10 Andy Buckley * 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 * 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 * 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 * Replace non-template Analysis::refData functions with C++11 default T=Scatter2D. 2017-03-29 Andy Buckley * 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 * 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 * Add Cut and functor selection args to HeavyHadrons accessor methods. 2017-03-03 Andy Buckley * bin/rivet-mkanalysis: Add FastJets.hh include by default -- it's almost always used. 2017-03-02 Andy Buckley * 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 * 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 * Add BoolParticleAND, BoolJetOR, etc. functor combiners to Tools/ParticleUtils.hh and Tools/JetUtils.hh. 2017-02-24 Andy Buckley * 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 * Add aggregate signal regions to CMS_2016_PAS_SUS_16_14. 2017-02-18 Andy Buckley * Add getEnvParam function, for neater use of environment variable parameters with a required default. 2017-02-05 Andy Buckley * Add HasBTag and HasCTag jet functors, with lower-case aliases. 2017-01-31 Andy Buckley * Start making analyses HepMC3-compatible, including major tidying in ATLAS_2013_I1243871. * Add Cut-arg variants to HeavyHadrons particle-retrieving methods. * Convert core to be compatible with HepMC3. 2017-01-21 Andy Buckley * Removing lots of long-deprecated functions & methods. 2017-01-18 Andy Buckley * Use std::function in functor-expanded method signatures on JetAlg. 2017-01-16 Andy Buckley * 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 * Version 2.5.3 release. 2016-12-12 Holger Schulz * 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 * 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 * Require Cython 0.24 or later. 2016-12-02 Andy Buckley * 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 * Adding ALICE_2012_I1116147 (eta and pi0 pTs and ratio) and ATLAS_2011_I929691 (7 TeV jet frag) 2016-11-30 Andy Buckley * Fix bash bugs in rivet-buildplugin, including fixing the --cmd mode. 2016-11-28 Andy Buckley * 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 * Adding pTvec() function to 4-vectors and ParticleBase. * Fix --pwd option of the rivet script 2016-11-21 Andy Buckley * Add weights and scaling to Cutflow/s. 2016-11-19 Andy Buckley * Add Et(const ParticleBase&) unbound function. 2016-11-18 Andy Buckley * Fix missing YAML quote mark in rivet-mkanalysis. 2016-11-15 Andy Buckley * 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 * Add rough ATLAS and CMS photon reco efficiency functions from Delphes (ATLAS and CMS versions are identical, hmmm) 2016-10-12 Andy Buckley * Tidying/fixing make-plots custom z-ticks code. Thanks to Dmitry Kalinkin. 2016-10-03 Holger Schulz * Fix SpiresID -> InspireID in some analyses (show-analysis pointed to non-existing web page) 2016-09-29 Holger Schulz * Add Luminosity_fb to AnalysisInfo * Added some keywords and Lumi to ATLAS_2016_I1458270 2016-09-28 Andy Buckley * 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 * make-plots bugfix in y-axis labels for RatioPlotMode=deviation 2016-09-27 Andy Buckley * Add vector and scalar pT (rather than Et) to MissingMomentum. 2016-09-27 Holger Schulz * Analysis keyword machinery * rivet -a @semileptonic * rivet -a @semileptonic@^bdecays -a @semileptonic@^ddecays 2016-09-22 Holger Schulz * Release version 2.5.2 2016-09-21 Andy Buckley * 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 * 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 * 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 * 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 * Add CMS partonic top analysis (CMS_2015_I1397174) 2016-09-18 Holger Schulz * 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 * Add has{Ancestor,Parent,Child,Descendant}With functions and HasParticle{Ancestor,Parent,Child,Descendant}With functors. 2016-09-16 Holger Schulz * Add ATLAS 8TeV ttbar analysis from contrib (ATLAS_2015_I1404878) 2016-09-16 Andy Buckley * Add particles(GenParticlePtr) to RivetHepMC.hh * Add hasParent, hasParentWith, and hasAncestorWith to Particle. 2016-09-15 Holger Schulz * 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 * Explicit std::toupper and std::tolower to make clang happy 2016-09-14 Andy Buckley * Add ATLAS Run 2 0-lepton SUSY and monojet search papers (ATLAS_2016_I1452559, ATLAS_2016_I1458270) 2016-09-13 Andy Buckley * 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 * 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 * 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 * 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 * 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 * Add templated functor filtering args to the Particle parent/child/descendent methods. 2016-09-06 Andy Buckley * 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 * 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 * 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 * Add rapidity scheme arg to DeltaR functor constructors. 2016-08-23 Andy Buckley * 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 * Bugfix in rivet-mkhtml (NoneType: ana.spiresID() --> spiresid) * Added include to Rivet/Tools/Utils.h to make gcc6 happy 2016-08-22 Andy Buckley * Add efffilt() functions and Particle/JetEffFilt functors to SmearingFunctions.hh 2016-08-20 Andy Buckley * Adding filterBy methods for Particle and Jet which accept generic boolean functions as well as the Cut specialisation. 2016-08-18 Andy Buckley * 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 * Add convenience headers for including all final-state and smearing projections, to save user typing. 2016-08-12 Andy Buckley * 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 * 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 * 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 * Release 2.5.1 2016-08-08 Andy Buckley * Add a simple MC_MET analysis for out-of-the-box MET distribution testing. 2016-08-08 Holger Schulz * 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 * 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 * 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 * 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 * Add SmearedMET projection, wrapping MissingMomentum. * Include base truth-level projections in SmearedParticles/Jets compare() methods. 2016-07-29 Andy Buckley * 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 * Mark D0_2000... W pT analysis validated * Mark LHCB_2011_S919... phi meson analysis validated 2016-07-25 Andy Buckley * 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 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 * 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 * 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 * 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 * 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 * Fix the --nskip behaviour on the main rivet script. 2016-07-07 Andy Buckley * Release version 2.5.0 2016-07-01 Andy Buckley * Fix pandoc interface flag version detection. 2016-06-28 Andy Buckley * 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 * Add ATLAS_2016_I1457605 inclusive photon analysis at 8 TeV. 2016-06-15 Andy Buckley * 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 * 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 * Add and use projection handling methods declare(proj, pname) and apply(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 * 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 * 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 * 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 * Adding ATLAS 13 TeV minimum bias analysis, ATLAS_2016_I1419652. 2016-05-30 Andy Buckley * 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 * 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 * Mark ATLAS_2012_I1082009 as validated after exhaustive tests with Pythia8 and Sherpa in inclusive QCD mode. 2016-05-11 Andy Buckley * Specialise return error codes from the rivet script. 2016-05-11 Andy Buckley * 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 * 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 * Add CMS_2014_I1305624 event shapes analysis, with standalone variable calculation struct embedded in an unnamed namespace. 2016-04-19 Andy Buckley * Various clean-ups and fixes in ATLAS analyses using isolated photons with median pT density correction. 2016-04-18 Andy Buckley * Add transformBy(LT) methods to Particle and Jet. * Add mkObjectTransform and mkFrameTransform factory methods to LorentzTransform. 2016-04-17 Andy Buckley * Add null GenVertex protection in Particle children & descendants methods. 2016-04-15 Andy Buckley * Add ATLAS_2015_I1397637, ATLAS 8 TeV boosted top cross-section vs. pT 2016-04-14 Andy Buckley * Add a --no-histos argument to the rivet script. 2016-04-13 Andy Buckley * 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 * Patch PID utils for ordering issues in baryon decoding. 2016-04-11 Andy Buckley * Actually implement ZEUS_2001_S4815815... only 10 years late! 2016-04-08 Andy Buckley * 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 * 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 * 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 * 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 * 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 * 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 * Bug-fix in semi-leptonic top selection of CMS_2015_I1370682. 2016-03-12 Andy Buckley * 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 * Release 2.4.1 2016-03-03 Andy Buckley * 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 * Add ATLAS 7 TeV event shapes in Z+jets analysis (ATLAS_2016_I1424838) 2016-02-29 Andy Buckley * 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 * 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 * 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 * 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 * Update ParticleIdUtils.hh (i.e. PID:: functions) to use the functions from the latest version of MCUtils' PIDUtils.h. 2016-01-15 Andy Buckley * 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 * 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 * 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 * 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 * Pro-actively use -m/-M arguments when initially loading histograms in mkhtml, *before* passing them to cmphistos. 2015-12-03 Andy Buckley * 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 * 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 * 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 * Write out intermediate histogram files by default, with event interval of 10k. 2015-11-25 Andy Buckley * Protect make-plots against lock-up due to partial pstricks command when there are no data points. 2015-11-17 Andy Buckley * rivet-cmphistos: Use a ratio label that doesn't mention 'data' when plotting MC vs. MC. 2015-11-12 Andy Buckley * 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 * Handle 2D histograms better in rivet-cmphistos (since they can't be overlaid) 2015-11-05 Andy Buckley * 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 * Adding LHCB inelastic xsection measurement (LHCB_2015_I1333223) * Adding ATLAS colour flow in ttbar->semileptonic measurement (ATLAS_2015_I1376945) 2015-10-07 Chris Pollard * Release 2.4.0 2015-10-06 Holger Schulz * Adding CMS_2015_I1327224 dijet analysis (Mjj>2 TeV) 2015-10-03 Holger Schulz * Adding CMS_2015_I1346843 Z+gamma 2015-09-30 Andy Buckley * 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 * Adding D0_2000_I503361 ZPT at 1800 GeV 2015-09-29 Chris Pollard * Adding ATLAS_2015_CONF_2015_041 2015-09-29 Chris Pollard * Adding ATLAS_2015_I1387176 2015-09-29 Chris Pollard * Adding ATLAS_2014_I1327229 2015-09-28 Chris Pollard * Adding ATLAS_2014_I1326641 2015-09-28 Holger Schulz * Adding CMS_2013_I1122847 FB assymetry in DY analysis 2015-09-28 Andy Buckley * Adding CMS_2015_I1385107 LHA pp 2.76 TeV track-jet underlying event. 2015-09-27 Andy Buckley * Adding CMS_2015_I1384119 LHC Run 2 minimum bias dN/deta with no B field. 2015-09-25 Andy Buckley * Adding TOTEM_2014_I1328627 forward charged density in eta analysis. 2015-09-23 Andy Buckley * 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 * 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 * 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 * Allow access to MissingMomentum projection via WFinder. * Adding extra methods to MissingMomentum, to make it more user-friendly. 2015-09-09 Andy Buckley * Fix factor of 2 in LHCB_2013_I1218996 normalisation, thanks to Felix Riehn for the report. 2015-08-20 Frank Siegert * 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 * 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 * 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 * 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 * 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 * Version 2.3.0 release. 2015-07-02 Holger Schulz * 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 * 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 * 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 * 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 * 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 * 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 * Normalisation discussion concerning ATLAS_2014_I1325553 is resolved. Changed YLabel accordingly. 2015-05-19 Holger Schulz * 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 * Fix ATLAS_2014_I1325553 normalisation of histograms was wrong by factor of two |y| vs y problem 2015-05-01 Andy Buckley * 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 * 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 * Add CMS 7 TeV rapidity gap analysis (CMS_2015_I1356998). * Remove FinalState Projection. 2015-03-30 Holger Schulz * Add ATLAS 7 TeV photon + jets analysis (ATLAS_2013_I1244522). 2015-03-26 Andy Buckley * Updates for HepMC 2.07 interface constness improvements. 2015-03-25 Holger Schulz * Add ATLAS double parton scattering in W+2j analysis (ATLAS_2013_I1216670). 2015-03-24 Andy Buckley * 2.2.1 release! 2015-03-23 Holger Schulz * Add ATLAS differential Higgs analysis (ATLAS_2014_I1306615). 2015-03-19 Chris Pollard * Add ATLAS V+gamma analyses (ATLAS_2013_I1217863) 2015-03-20 Andy Buckley * 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 * Mark ATLAS_2012_I1083318 as VALIDATED and fix d25-x01-y02 ref data. 2015-03-19 Chris Pollard * Add ATLAS W and Z angular analyses (ATLAS_2011_I928289) 2015-03-19 Andy Buckley * 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 * 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 * Adding CMS_2014_I1298810 and CMS_2014_I1303894 analyses. 2015-03-18 Holger Schulz * 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 * Change UnstableFinalState duplicate resolution to use the last in a chain rather than the first. 2015-03-17 Holger Schulz * 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 * Removed fuzzyEquals() from Vector3::angle() 2015-03-16 Andy Buckley * Adding Cuts-based constructor to PrimaryHadrons. * Adding missing compare() method to HeavyHadrons projection. 2015-03-15 Chris Pollard * Adding FinalPartons projection which selects the quarks and gluons immediately before hadronization 2015-03-05 Andy Buckley * Adding Cuts-based constructors and other tidying in UnstableFinalState and HeavyHadrons 2015-03-03 Andy Buckley * Add support for a PLOT meta-file argument to rivet-cmphistos. 2015-02-27 Andy Buckley * Improved time reporting. 2015-02-24 Andy Buckley * 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 * 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 * Converting 'bitwise' to 'logical' Cuts combinations in all analyses. 2015-02-02 Andy Buckley * 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 * 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 * Interface improvements in DressedLeptons constructor. * Adding DEPRECATED macro to throw compiler deprecation warnings when using deprecated features. 2014-11-25 Andy Buckley * Adding Cut-based constructors, and various constructors with lists of PDG codes to IdentifiedFinalState. 2014-11-20 Andy Buckley * 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 * Fix a bug in the isCharmHadron(pid) function and remove isStrange* functions. 2014-09-30 Andy Buckley * 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 * 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 * 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) function and fixing the other stats functions to operate on vector rather than vector. 2014-09-03 Andy Buckley * Fix wrong behaviour of LorentzTransform with a null boost vector -- thanks to Michael Grosse. 2014-08-26 Andy Buckley * 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 * 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 * Version bump to 2.2.0beta1 for use at BOOST and MCnet school. 2014-08-13 Andy Buckley * 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 * Adding PromptFinalState, based on code submitted by Alex Grohsjean and Will Bell. Thanks! 2014-08-06 Andy Buckley * Adding MC_HFJETS and MC_JETTAGS analyses. 2014-08-05 Andy Buckley * 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 * 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 * Remove classifier functions accepting a Particle from the PID inner namespace. 2014-07-29 Andy Buckley * 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 * Fix to logspace: make sure that start and end values are exact, not the result of exp(log(x)). 2014-07-16 Andy Buckley * 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 * 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 * Add stupid missing include and std:: prefix in Rivet.hh 2014-06-20 Holger Schulz * 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 * pyext/rivet/Makefile.am: 'make distcheck' and out-of-source builds should work now. 2014-06-10 Andy Buckley * Fix use of the install command for bash completion installation on Macs. 2014-06-07 Andy Buckley * Removing direct includes of MathUtils.hh and others from analysis code files. 2014-06-02 Andy Buckley * Rivet 2.1.2 release! 2014-05-30 Andy Buckley * 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 * 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 * Re-enable 2D histo in MC_PDFS 2014-05-28 Andy Buckley * 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 * 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 * 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 * Adding any(iterable, fn) and all(iterable, fn) template functions for convenience. 2014-05-15 Holger Schulz * Fix some bugs in identified hadron PIDs in OPAL_1998_S3749908. 2014-05-13 Andy Buckley * Writing out [UNVALIDATED], [PRELIMINARY], etc. in the --list-analyses output if analysis is not VALIDATED. 2014-05-12 Andy Buckley * Adding CMS_2013_I1265659 colour coherence analysis. 2014-05-07 Andy Buckley * 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 * Fix missing abs() in Particle::abspid()!!!! 2014-04-14 Andy Buckley * 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 * 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 * Flattening PNG output of make-plots (i.e. no transparency) and other tweaks. 2014-03-23 Andy Buckley * 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 * Rivet 2.1.1 release. 2014-03-07 Andy Buckley * Adding ATLAS multilepton search (no ref data file), ATLAS_2012_I1204447. 2014-03-05 Andy Buckley * 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 * 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 * 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 * 2.1.0 release! 2014-02-05 Andy Buckley * Protect against invalid prefix value if the --prefix configure option is unused. 2014-02-03 Andy Buckley * 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 * 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 * Removing unused/overrestrictive Isolation* headers. 2014-01-27 Andy Buckley * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * Adding the GSL lib path to the library path in the env scripts and the rivet-config --ldflags output. 2013-10-25 Andy Buckley * 2.0.0 release!!!!!! 2013-10-24 Andy Buckley * Supporting zsh completion via bash completion compatibility. 2013-10-22 Andy Buckley * 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 * Several small fixes in jet shape analyses, SFM_1984, etc. found in the last H++ validation run. 2013-10-18 Andy Buckley * Updates to configure and the rivetenv scripts to try harder to discover YODA. 2013-09-26 Andy Buckley * Now bundling Cython-generated files in the tarballs, so Cython is not a build requirement for non-developers. 2013-09-24 Andy Buckley * 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 * Add the -avoid-version flag to libtool. * Final analysis histogramming issues resolved. 2013-08-16 Andy Buckley * 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 * 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 * 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 * 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 * 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 * 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 * 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 * Adding a new HeavyHadrons projection. * Adding optional extra include_end args to logspace() and linspace(). 2013-06-11 Andy Buckley * 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 * 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 * 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 * Releasing 2.0.0b2 beta version. 2013-06-05 Andy Buckley * 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 * 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 * 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 * 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 * 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 * Removing Constraints.hh header. * Minor bugfixes and improvements in Scatter2D booking and MC_JetAnalysis. 2013-05-28 Andy Buckley * Removing defunct HistoFormat.hh and HistoHandler.{hh,cc} 2013-05-27 Andy Buckley * 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 * 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 * 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 * Analysis histo booking improvements for Scatter2D, placeholders for 2D histos, and general tidying. 2013-05-12 Andy Buckley * Adding configure-time differentiation between yaml-cpp API versions 3 and 5. 2013-05-07 Andy Buckley * Converting info file reading to use the yaml-cpp 0.5.x API. 2013-04-12 Andy Buckley * Tagging as 2.0.0b1 2013-04-04 Andy Buckley * Removing bundling of yaml-cpp: it needs to be installed by the user / bootstrap script from now on. 2013-04-03 Andy Buckley * Removing svn:external m4 directory, and converting Boost detection to use better boost.m4 macros. 2013-03-22 Andy Buckley * Moving PID consts to the PID namespace and corresponding code updates and opportunistic clean-ups. * Adding Particle::fromDecay() method. 2013-03-09 Andy Buckley * 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 * 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 * 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 * 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 * 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 * include/Rivet/Math/MathUtils.hh: added BWspace bin edge method to give equal-area Breit-Wigner bins 2013-02-01 Andy Buckley * 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 * 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 * Fix TeX variable in the rivetenv scripts, especially for csh 2012-12-21 Andy Buckley * Version 1.8.2 release! 2012-12-20 Andy Buckley * Adding ATLAS_2012_I1119557 analysis (from Roman Lysak and Lily Asquith). 2012-12-18 Andy Buckley * Adding TOTEM_2012_002 analysis, from Sercan Sen. 2012-12-18 Hendrik Hoeth * Added CMS_2011_I954992 analysis 2012-12-17 Hendrik Hoeth * Added CMS_2012_I1193338 analysis * Fixed xi cut in ATLAS_2011_I894867 2012-12-17 Andy Buckley * Adding analysis descriptions to the HTML analysis page ToC. 2012-12-14 Hendrik Hoeth * Added CMS_2012_PAS_FWD_11_003 analysis * Added LHCB_2012_I1119400 analysis 2012-12-12 Andy Buckley * Correction to jet acceptance in CMS_2011_S9120041, from Sercan Sen: thanks! 2012-12-12 Hendrik Hoeth * Added CMS_2012_PAS_QCD_11_010 analysis 2012-12-07 Andy Buckley * 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 * Added ALICE_2012_I1181770 analysis * Bump version to 1.8.2 2012-12-06 Hendrik Hoeth * 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 * Converting CMS_2012_I1102908 analysis to use YODA. * Adding XLabel and YLabel setting in histo/profile/scatter booking. 2012-11-27 Hendrik Hoeth * Fix make-plots png creation for SL5 2012-11-23 Peter Richardson * Added ATLAS_2012_CONF_2012_153 4-lepton SUSY search 2012-11-17 Andy Buckley * 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 * Adding MC_PRINTEVENT, a convenient (but verbose!) analysis for printing out event details to stdout. 2012-11-15 Andy Buckley * Removing the long-unused/defunct autopackage system. 2012-11-15 Hendrik Hoeth * Added LHCF_2012_I1115479 analysis * Added ATLAS_2011_I894867 analysis 2012-11-14 Hendrik Hoeth * Added CMS_2012_I1102908 analysis 2012-11-14 Andy Buckley * 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 * 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 * Added CMS_2012_I1107658 analysis 2012-10-11 Hendrik Hoeth * Added CDF_2012_NOTE10874 analysis 2012-10-04 Hendrik Hoeth * Added ATLAS_2012_I1183818 analysis 2012-07-17 Hendrik Hoeth * 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 * Fixing aida2root command-line help message and converting to TH* rather than TGraph by default. 2012-07-24 Andy Buckley * Improvements/migrations to rivet-mkhtml, rivet-mkanalysis, and rivet-buildplugin. 2012-07-17 Hendrik Hoeth * Add CMS_2012_I1087342 2012-07-12 Andy Buckley * Fix rivet-mkanalysis a bit for YODA compatibility. 2012-07-05 Hendrik Hoeth * Version 1.8.1! 2012-07-05 Holger Schulz * Add ATLAS_2011_I945498 2012-07-03 Hendrik Hoeth * Bugfix for transverse mass (thanks to Gavin Hesketh) 2012-06-29 Hendrik Hoeth * Merge YODA branch into trunk. YODA is alive!!!!!! 2012-06-26 Holger Schulz * Add ATLAS_2012_I1091481 2012-06-20 Hendrik Hoeth * Added D0_2011_I895662: 3-jet mass 2012-04-24 Hendrik Hoeth * fixed a few bugs in rivet-rmgaps * Added new TOTEM dN/deta analysis 2012-03-19 Andy Buckley * 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 * 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 * Improve default plot behaviour for 2D histograms 2012-03-15 Hendrik Hoeth * 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 * Marking ATLAS_2011_I919017 as VALIDATED (this should have happened a long time ago) and adding more references. 2012-02-28 Hendrik Hoeth * lighthisto.py: Caching for re.compile(). This speeds up aida2flat and flat2aida by more than an order of magnitude. 2012-02-27 Andy Buckley * doc/mk-analysis-html: Adding more LaTeX/text -> HTML conversion replacements, including better <,> handling. 2012-02-26 Andy Buckley * 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 * Adding ATLAS Ks/Lambda analysis. 2012-02-20 Andy Buckley * src/Analyses/ATLAS_2011_I925932.cc: Using new overflow-aware normalize() in place of counters and scale(..., 1/count) 2012-02-14 Andy Buckley * 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 * DELPHI_1996_S3430090 and ALEPH_1996_S3486095: fix rapidity vs {Thrust,Sphericity}-axis. 2012-02-14 Andy Buckley * 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 * 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 * 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 * Fixed broken UnstableFS behaviour 2012-01-25 Frank Siegert * 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 * Add ATLAS diffractive gap analysis 2012-01-23 Andy Buckley * 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 * Tidying lighthisto, including fixing the order in which +- error values are passed to the Bin constructor in fromFlatHisto. 2012-01-16 Frank Siegert * 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 * Fixes to ATLAS_20111_S9225137 to include reference data 2012-01-13 Holger Schulz * Add ATLAS inclusive lepton analysis 2012-01-12 Hendrik Hoeth * Font selection support in rivet-mkhtml 2012-01-11 Peter Richardson * Added pi0 to list of particles. 2012-01-11 Andy Buckley * Removing references to Boost random numbers. 2011-12-30 Andy Buckley * 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 * Adding a command line completion function for rivet-mkhtml. 2011-12-12 Frank Siegert * 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 * Include underflow and overflow bins in the normalisation when calling Analysis::normalise(h) 2011-11-23 Andy Buckley * 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 * 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 * Adding a guide to compiling a new analysis template to the output message of rivet-mkanalysis. 2011-11-11 Andy Buckley * 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 * 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 * 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 * 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 * 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 * Add four CMS QCD analyses kindly provided by CMS. 2011-10-12 Andy Buckley * 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 * Removing SVertex. 2011-10-11 James Monk * 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 * Fix bug in ATLAS_2010_S8817804 that misidentified the akt4 jets as akt6 2011-09-29 Andy Buckley * Converting FinalStateHCM to a slightly more general DISFinalState. 2011-09-26 Andy Buckley * 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 * make-plots: Fixing regex for \physicscoor. Adding "FrameColor" option. 2011-09-17 Andy Buckley * 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 * Added ALICE_2011_S8909580 (strange particle production at 900 GeV) * Feed-down correction in ALICE_2011_S8945144 2011-09-16 Andy Buckley * 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 * 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 * 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 * 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 * lighthisto fixes from Christian Roehr. 2011-08-26 Andy Buckley * 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 * 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 * Added ATLAS_2011_S9126244 * Added ATLAS_2011_S9128077 2011-08-23 Hendrik Hoeth * 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 * 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 * Fix aida2flat to ignore empty dataPointSet 2011-08-07 Andy Buckley * 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 Version 1.6.0 release! 2011-08-01 Frank Siegert * 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 * Version 1.5.2 release! * New version of aida2root from James Monk. 2011-07-29 Frank Siegert * Fix implementation of --config file option in make-plots. 2011-07-27 David Mallows * Updated MC_TTBAR.plot to reflect updated analysis. 2011-07-25 Andy Buckley * 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 * 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 * Making MC_TTBAR work with semileptonic ttbar events and generally tidying the code. 2011-07-19 Andy Buckley * Version bump to 1.5.2.b01 in preparation for a release in the very near future. 2011-07-18 David Mallows * Replaced MC_TTBAR: Added t,tbar reconstruction. Not yet working. 2011-07-18 Andy Buckley * 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 * 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 * Rivet PDF manual updates, to not spread disinformation about bootstrapping a Genser repo. 2011-07-12 Andy Buckley * 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 * fix fromFlat() in lighthistos: It would ignore histogram paths before. * flat2aida: preserve histogram order from .dat files 2011-06-27 Andy Buckley * 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 * 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 * Bugfixes in WFinder. 2011-06-10 Andy Buckley * Adding \physicsxcoor and \physicsycoor treatment to make-plots. 2011-06-06 Hendrik Hoeth * 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 * 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 * Adding auto conversion of Histogram2D to DataPointSets in the AnalysisHandler _normalizeTree method. 2011-06-03 Andy Buckley * 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 * Add BeamThrust projection 2011-05-31 Hendrik Hoeth * 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 * 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 * 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 * 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 * 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 * 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 * Ignore duplicate files in compare-histos. 2011-04-25 Andy Buckley * 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 * Added ATLAS_2011_S9002537 W asymmetry analysis 2011-04-14 Hendrik Hoeth * 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 * added ATLAS 8983313: 0-lepton BSM 2011-04-01 Andy Buckley * 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 * 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 * 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 * src/Core/AnalysisHandler.cc (AnalysisHandler::removeAnalysis): Fixed strange shared pointer assignment that caused seg-fault. 2011-03-13 Hendrik Hoeth * filling of functions works now in a more intuitive way (I hope). 2011-03-09 Andy Buckley * Version 1.5.0 release! 2011-03-08 Andy Buckley * Adding some extra checks for external packages in make-plots. 2011-03-07 Andy Buckley * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * Adding the ATLAS 2011 transverse jet shapes analysis. 2011-02-18 Hendrik Hoeth * Support for transparency in make-plots 2011-02-18 Frank Siegert * Added ATLAS prompt photon analysis ATLAS_2010_S8914702 2011-02-10 Hendrik Hoeth * 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 * Add final version of ATLAS dijet azimuthal decorrelation 2011-02-10 Hendrik Hoeth * 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 * 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 * Adding ATLAS 2010 min bias and underlying event analyses and data. 2011-01-23 Andy Buckley * Make make-plots write out PDF rather than PS by default. 2011-01-12 Andy Buckley * 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 * Clean up ATLAS dijet analysis. 2010-12-30 Andy Buckley * 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 * Fix the cuts in the CDF 1994 colour coherence analysis. 2010-12-19 Andy Buckley * 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 * 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 * 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 * 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 * Fixing unbooked-histo segfault in UA1_1990_S2044935 at 63 GeV. 2010-12-08 Hendrik Hoeth * 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 * 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 * Change LegendXPos behaviour in make-plots. Now the top left corner of the legend is used as anchor point. 2010-12-03 Andy Buckley * 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 * Fix normalisation issues in UA5 and ALEPH analyses 2010-11-27 Andy Buckley * 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 * 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 * 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 * 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 * 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 * 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 * 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 * Adding ATLAS-CONF-2010-081 conference note. Data is read from plots. 2010-11-06 Andy Buckley * 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 * Adding ATLAS-CONF-2010-031 conference note. Data is read from plots. 2010-10-29 Andy Buckley * 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 * Adding a --with-root flag to rivet-buildplugin to add root-config --libs flags to the plugin build command. 2010-09-24 Andy Buckley * 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 * Fix error in N_effective definition for weighted profile errors. 2010-08-18 Andy Buckley * Adding MC_GENERIC analysis. NB. Frank Siegert also added MC_HJETS. 2010-08-03 Andy Buckley * Fixing compare-histos treatment of what is now a ref file, and speeding things up... again. What a mess! 2010-08-02 Andy Buckley * 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 * 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 * Adding an explicit library dependency declaration on libHepMC, and hence removing the -lHepMC from the rivet-config --libs output. 2010-07-14 Andy Buckley * 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 * 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 * 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 * 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 * Making rivet-buildplugin look in its own bin directory when trying to find rivet-config. 2010-06-23 Andy Buckley * 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 * 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 * 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 * 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 * Fixing factor-of-2 bug in the error calculation when scaling histograms. * Fixing D0_2001_S4674421 analysis. 2010-05-11 Andy Buckley * Replacing TotalVisibleMomentum with MissingMomentum in analyses and WFinder. Using vector ET rather than scalar ET in some places. 2010-05-07 Andy Buckley * 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 * Fixing LaTeX problems (make-plots) on ancient machines, like lxplus. 2010-04-29 Andy Buckley * Fixing (I hope!) the treatment of weighted profile bin errors in LWH. 2010-04-21 Andy Buckley * 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 * remove obsolete reference to InitialQuarks from DELPHI_2002 * fix normalisation in CDF_2000_S4155203 2010-04-20 Hendrik Hoeth * 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 * 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 * 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 * 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 * Tag as patch release 1.2.1. 2010-03-22 Andy Buckley * 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 * 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 * Tagging for 1.2.0 release... at last! 2010-03-01 Andy Buckley * 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 * Update WFinder to not place cuts and other restrictions on the neutrino. 2010-02-11 Andy Buckley * 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 * 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 * New option "RatioPlotMode=deviation" in make-plots. 2009-12-14 Hendrik Hoeth * 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 * 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 * 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 * 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 * Propagate SPECIAL and HISTOGRAM sections from .plot files through compare-histos * STAR_2006_S6860818: vs particle mass, validate analysis 2009-12-04 Andy Buckley * 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 * 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 * Adding parsing of beam types and pairs of energies from YAML. 2009-12-01 Hendrik Hoeth * Fixing trigger efficiency in CDF_2009_S8233977 2009-11-30 Andy Buckley * 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 * Fixing division by zero in Profile1D bin errors for bins with just a single entry. 2009-11-24 Hendrik Hoeth * First working version of STAR_2006_S6860818 2009-11-23 Hendrik Hoeth * 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 * Fixing our compare() for doubles. 2009-11-17 Hendrik Hoeth * Zeroth version of STAR_2006_S6860818 analysis (identified strange particles). Not working yet for unstable particles. 2009-11-11 Andy Buckley * 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 * Fixing last issues in STAR_2006_S6500200 and setting it to VALIDATED. * Noramlise STAR_2006_S6870392 to cross-section 2009-11-09 Andy Buckley * 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 * 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 * Adding Cmp specialisation, using fuzzyEquals(). 2009-11-05 Hendrik Hoeth * Fixing histogram division code. 2009-11-04 Hendrik Hoeth * 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 * Adding consistence checking on beam ID and sqrt(s) vs. those from first event. 2009-11-03 Andy Buckley * Adding more assertion checks to linear algebra testing. 2009-11-02 Hendrik Hoeth * Fixing normalisation issue with stacked histograms in make-plots. 2009-10-30 Hendrik Hoeth * CDF_2009_S8233977: Updating data and axes labels to match final paper. Normalise to cross-section instead of data. 2009-10-23 Andy Buckley * Fixing Cheese-3 plot in CDF 2004... at last! 2009-10-23 Hendrik Hoeth * Fix muon veto in CDF_1994_S2952106, CDF_2005_S6217184, CDF_2008_S7782535, and D0_2004_S5992206 2009-10-19 Andy Buckley * Adding analysis info files for MC SUSY and PHOTONJETUE analyses. * Adding MC UE analysis in photon+jet events. 2009-10-19 Hendrik Hoeth * 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 * 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 * 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 * 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 * 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 * Adding optional use of args as regex match expressions with -l/--list-analyses. 2009-09-03 Andy Buckley * 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 * 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 * 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 * 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 * 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 * Replacing in-source histo-booking metadata with .plot files. 2009-07-14 Andy Buckley * 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 * 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 * Adding Jet::neutralEnergy() (and Jet::totalEnergy() for convenience/symmetry). 2009-06-25 Andy Buckley * 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 * 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 * 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 * 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 * 1.1.3 release! * More doc building and SWIG robustness tweaks. 2009-06-07 Andy Buckley * Make doc build from metadata work even before the library is installed. 2009-06-07 Hendrik Hoeth * Fix phi rotation in CDF_2008_LEADINGJETS. 2009-06-07 Andy Buckley * 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 * 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 * 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 * Adding use of gsl-config in configure script. 2009-05-16 Andy Buckley * 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 * 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 * 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 * Adding event auto-rotation for events with one proton... more complete approach? 2009-05-09 Hendrik Hoeth * 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 * Adding rivet-mkanalysis script, to make generating new analysis source templates easier. 2009-05-07 Andy Buckley * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * Adding R=0.2 photon clustering to the electrons in the CDF 2000 Z pT analysis. 2009-03-04 Andy Buckley * 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 * 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 * 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 * 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 * Adding automatic generation of LaTeX manual entries for the standard analyses. 2009-01-20 Andy Buckley * Removing RivetGun and TCLAP source files! 2009-01-19 Andy Buckley * Added psyco Python optimiser to rivet, make-plots and compare-histos. * bin/aida2root: Added "-" -> "_" mangling, following requests. 2009-01-17 Andy Buckley * 1.1.2 release. 2009-01-15 Andy Buckley * Converting Python build system to bundle SWIG output in tarball. 2009-01-14 Andy Buckley * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * Replaced binreloc with an upgraded and symbol-independent copy. 2008-11-25 Andy Buckley * Added searching of $RIVET_REF_PATH for AIDA reference data files. 2008-11-24 Andy Buckley * Removing "get"s and other obsfucated syntax from ProjectionApplier (Projection and Analysis) interfaces. 2008-11-21 Andy Buckley * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * Adding native logger control from Python interface. 2008-11-03 Andy Buckley * Adding bash_completion for rivet executable. 2008-10-31 Andy Buckley * Clean-up of histo titles and analysis code review. * Added momentum construction functions from FastJet PseudoJets. 2008-10-28 Andy Buckley * 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 * 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 * 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 * 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 * 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 * 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 * 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 * 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 * New analysis: CDF_2000_S4155203 2008-09-23 Andy Buckley * rivetgun can now be built and run without AGILe. Based on a patch by Frank Siegert. 2008-09-23 Hendrik Hoeth * 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 * 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 * Allowing rivet-config to return combined flags. 2008-08-14 Andy Buckley * 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 * Tidying of FastJets and added new data files from HepData. 2008-08-10 James Monk * FastJets now uses user_index property of fastjet::PseudoJet to reconstruct PID information in jet contents. 2008-08-07 Andy Buckley * 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 * 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 * 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 * 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 * 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 * Fixed missing ROOT compile flags for libRivet. * Added command line repetition to logging. 2008-07-29 Hendrik Hoeth * Included the missing numbers and three more observables in the CDF_2008_NOTE_9351 analysis. 2008-07-29 Andy Buckley * Fixed wrong flags on rivet-config 2008-07-28 Hendrik Hoeth * 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 * Fixed polar angle calcuation to use atan2. * Added "mk" prefixes and x/setX convention to math classes. 2008-07-28 Hendrik Hoeth * Fixed definition of FourMomentum::pT (it had been returning pT2) 2008-07-27 Andy Buckley * Added better tests for Boost headers. * Added testing for -ansi, -pedantic and -Wall compiler flags. 2008-07-25 Hendrik Hoeth * updated DELPHI_2002_069_CONF_603 according to information from the author 2008-07-17 Andy Buckley * 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 * Fixed missing namespace in vector/matrix testing. * Removed Boost headers: now a system dependency. * Fixed polarRadius infinite loop. 2008-07-09 Andy Buckley * 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 * 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 * 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 * Modified FastJet to fix ysplit and split and filter. * Modified ExampleTree to show how to call them. 2008-06-19 Hendrik Hoeth * 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 * Added First versions of splitJet and filterJet methods to fastjet.cc. Not yet tested, buyer beware. 2008-06-18 Andy Buckley * 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 * Fixed processing of "RG" parameters to ensure that invalid iterators are never used. 2008-06-10 Andy Buckley * 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 * 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 * Added DELPHI_2002_069_CONF_603 analysis 2008-05-30 Hendrik Hoeth * Added InitialQuarks projection * Added OPAL_1998_S3780481 analysis 2008-05-29 Andy Buckley * distcheck compatibility fixes and autotools tweaks. 2008-05-28 Andy Buckley * 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 * 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 * 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 * New analysis PDG_Hadron_Multiplicities * flat2aida converter 2008-05-15 Andy Buckley * Removed unused mysterious Perl scripts! * Added RivetGun.HepMC logging of HepMC event details. 2008-05-14 Hendrik Hoeth * New analysis DELPHI_1995_S3137023. This analysis contains the xp spectra of Xi+- and Sigma(1385)+-. 2008-05-13 Andy Buckley * 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 * Improvements to robustness of ROOT checks. * Added --version flag on config scripts and rivetgun. 2008-05-06 Hendrik Hoeth * 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 * 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 * 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 * 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 * 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 * 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 * Profile histograms now use error computation with proper weighting, as described here: http://en.wikipedia.org/wiki/Weighted_average 2008-02-28 Andy Buckley * 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 * Vector 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 * 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 * 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 * Applied fixes and extensions to DIS classes, based on submissions by Dan Traynor. 2008-02-06 Andy Buckley * 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 * Fixed another misplaced factor of bin width in the Analysis::normalize() method. 2008-01-30 Andy Buckley * 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 * 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 * Added angle range fix to pseudorapidity function (thanks to Piergiulio Lenzi). 2008-01-10 Andy Buckley * 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 * 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 * 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 * 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 * include/LWH/ManagedObject.h: Fixed infinite loop in encodeForXML cf. ticket #135. 2007-12-20 Andy Buckley * 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 * Changed units header to set GeV = 1 (HepMC convention) and using units in CDF UE analysis. 2007-12-15 Andy Buckley * Introduced analysis metadata methods for all analyses (and made them part of the Analysis interface). 2007-12-11 Andy Buckley * Added JetAlg base projection for TrackJet, FastJet etc. 2007-12-06 Andy Buckley * 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 * 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 * 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 * 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 * 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 * Removed conditional HAVE_FASTJET bits: FastJet is now compulsory. * Merging appropriate RivetGun parts into Rivet. RivetGun currently broken. 2007-11-23 Andy Buckley * Renaming analyses to Spires-ID scheme: currently of form S, to become __. 2007-11-20 Andy Buckley * Merged replacement vectors, matrices and boosts into trunk. 2007-11-15 Leif Lonnblad * src/Analysis.cc, include/Rivet/Analysis.hh: Introduced normalize function. See ticket #126. 2007-10-31 Andy Buckley * Tagging as 1.0b2 for HERA-LHC meeting. 2007-10-25 Andy Buckley * 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 * 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 * Added new reference files. 2007-10-03 Andy Buckley * 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 * 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 * Fixed portable path to Rivet share directory. 2007-09-28 Andy Buckley * Added more functionality to the rivet-config script: now has libdir, includedir, cppflags, ldflags and ldlibs options. 2007-09-26 Andy Buckley * 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 * 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 * 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 * Added Hemispheres projection, which calculates event hemisphere masses and broadenings. 2007-09-19 Andy Buckley * 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 * 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 * Merged in a branch of pluggable analysis mechanisms. 2007-06-25 Jon Butterworth * Fixed some bugs in the root output for DataPoint.h 2007-06-25 Andy Buckley * 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 * 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 * 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 * 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 * 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 * Merged TotalVisibleMomentum and CalMET * Added pT ranges to Vetoed final state projection 2007-05-27 Jon Butterworth * Fixed initialization of VetoedFinalStateProjection in ExampleTree 2007-05-27 Leif Lonnblad * include/Rivet/Projections/KtJets.*: Make sure the KtEvent is deleted properly. 2007-05-26 Jon Butterworth * Added leptons to the ExampleTree. * Added TotalVisibleEnergy projection, and added output to ExampleTree. 2007-05-25 Jon Butterworth * Added a charged lepton projection 2007-05-23 Andy Buckley * 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 * src/Analysis/HepEx9506012.cc: Now uses the histogram booking function in the Analysis class. 2007-05-23 Jon Butterworth * Fixed bug in PRD65092002 (was failing on zero jets) 2007-05-23 Andy Buckley * 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 * 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::max() rather than min() * Added more control of logging presentation via static flag methods on Log. 2007-05-13 Andy Buckley * 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 * 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 * Added a preliminary version of the Rick Field UE analysis, under the name PRD65092002. 2007-04-19 Leif Lonnblad * 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 * 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 * Added "rivet" executable which can read in HepMC ASCII dump files and apply Rivet analyses on the events. 2007-02-24 Leif Lonnblad * 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 * 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 * 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 * 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 * 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 * 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 * Introduced log4cpp logging. * Added analysis enum, which can be used as input to an analysis factory by Rivet users. 2006-11-02 Andy Buckley * 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 * 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 * Moving things around: all sources now in directories under src 2006-06-04 Leif Lonnblad * 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 * 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 * 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/analyses/Makefile.am b/analyses/Makefile.am --- a/analyses/Makefile.am +++ b/analyses/Makefile.am @@ -1,54 +1,64 @@ AUTOMAKE_OPTIONS = -Wno-portability SHELL := bash -O extglob if ENABLE_ANALYSES PLUGIN_DIRS = $(shell ls -d $(srcdir)/plugin*) PLUGIN_NAMES = $(notdir $(subst plugin,,$(PLUGIN_DIRS))) PLUGIN_LIBS = $(patsubst %,Rivet%Analyses.so,$(PLUGIN_NAMES)) PLUGIN_DATAFILES = $(shell ls $(abs_srcdir)/plugin*/*.{info,plot,yoda}) CLEANFILES = $(PLUGIN_LIBS) EXTRA_DIST = $(PLUGIN_DIRS) %.so: @+echo && RIVET_BUILDPLUGIN_BEFORE_INSTALL=1 bash $(top_builddir)/bin/rivet-buildplugin -j2 $@ $^ -I$(top_builddir)/include RivetALICEAnalyses.so: $(filter-out $(srcdir)/pluginALICE/tmp*.cc, $(wildcard $(srcdir)/pluginALICE/*.cc)) RivetATLASAnalyses.so: $(filter-out $(srcdir)/pluginATLAS/tmp*.cc, $(wildcard $(srcdir)/pluginATLAS/*.cc)) +RivetBABARAnalyses.so: $(filter-out $(srcdir)/pluginBABAR/tmp*.cc, $(wildcard $(srcdir)/pluginBABAR/*.cc)) +RivetBELLEAnalyses.so: $(filter-out $(srcdir)/pluginBELLE/tmp*.cc, $(wildcard $(srcdir)/pluginBELLE/*.cc)) +RivetBESAnalyses.so: $(filter-out $(srcdir)/pluginBES/tmp*.cc, $(wildcard $(srcdir)/pluginBES/*.cc)) RivetCDFAnalyses.so: $(filter-out $(srcdir)/pluginCDF/tmp*.cc, $(wildcard $(srcdir)/pluginCDF/*.cc)) +RivetCESRAnalyses.so: $(filter-out $(srcdir)/pluginCESR/tmp*.cc, $(wildcard $(srcdir)/pluginCESR/*.cc)) RivetCMSAnalyses.so: $(filter-out $(srcdir)/pluginCMS/tmp*.cc, $(wildcard $(srcdir)/pluginCMS/*.cc)) RivetD0Analyses.so: $(filter-out $(srcdir)/pluginD0/tmp*.cc, $(wildcard $(srcdir)/pluginD0/*.cc)) +RivetDORISAnalyses.so: $(filter-out $(srcdir)/pluginDORIS/tmp*.cc, $(wildcard $(srcdir)/pluginDORIS/*.cc)) +RivetFrascatiAnalyses.so: $(filter-out $(srcdir)/pluginFrascati/tmp*.cc, $(wildcard $(srcdir)/pluginFrascati/*.cc)) RivetHERAAnalyses.so: $(filter-out $(srcdir)/pluginHERA/tmp*.cc, $(wildcard $(srcdir)/pluginHERA/*.cc)) RivetLEPAnalyses.so: $(filter-out $(srcdir)/pluginLEP/tmp*.cc, $(wildcard $(srcdir)/pluginLEP/*.cc)) RivetLHCbAnalyses.so: $(filter-out $(srcdir)/pluginLHCb/tmp*.cc, $(wildcard $(srcdir)/pluginLHCb/*.cc)) RivetLHCfAnalyses.so: $(filter-out $(srcdir)/pluginLHCf/tmp*.cc, $(wildcard $(srcdir)/pluginLHCf/*.cc)) RivetMCAnalyses.so: $(filter-out $(srcdir)/pluginMC/tmp*.cc, $(wildcard $(srcdir)/pluginMC/*.cc)) +RivetNovosibirskAnalyses.so: $(filter-out $(srcdir)/pluginNovosibirsk/tmp*.cc, $(wildcard $(srcdir)/pluginNovosibirsk/*.cc)) +RivetOrsayAnalyses.so: $(filter-out $(srcdir)/pluginOrsay/tmp*.cc, $(wildcard $(srcdir)/pluginOrsay/*.cc)) RivetMiscAnalyses.so: $(filter-out $(srcdir)/pluginMisc/tmp*.cc, $(wildcard $(srcdir)/pluginMisc/*.cc)) RivetPetraAnalyses.so: $(filter-out $(srcdir)/pluginPetra/tmp*.cc, $(wildcard $(srcdir)/pluginPetra/*.cc)) RivetRHICAnalyses.so: $(filter-out $(srcdir)/pluginRHIC/tmp*.cc, $(wildcard $(srcdir)/pluginRHIC/*.cc)) +RivetSLACAnalyses.so: $(filter-out $(srcdir)/pluginSLAC/tmp*.cc, $(wildcard $(srcdir)/pluginSLAC/*.cc)) RivetSPSAnalyses.so: $(filter-out $(srcdir)/pluginSPS/tmp*.cc, $(wildcard $(srcdir)/pluginSPS/*.cc)) RivetTOTEMAnalyses.so: $(filter-out $(srcdir)/pluginTOTEM/tmp*.cc, $(wildcard $(srcdir)/pluginTOTEM/*.cc)) +RivetTristanAnalyses.so: $(filter-out $(srcdir)/pluginTristan/tmp*.cc, $(wildcard $(srcdir)/pluginTristan/*.cc)) all-local: $(PLUGIN_LIBS) $(PLUGIN_DATAFILES) mkdir -p $(builddir)/data $(LN_S) -f $(abs_srcdir)/plugin*/*.{info,plot,yoda} $(builddir)/data clean-local: rm -rf data install-exec-local: $(PLUGIN_LIBS) $(INSTALL) $^ $(DESTDIR)$(libdir) install-data-local: $(PLUGIN_DATAFILES) @echo "Installing analysis data files..." $(mkdir_p) $(DESTDIR)$(pkgdatadir) cp $(abs_srcdir)/plugin*/*.{info,plot,yoda} $(DESTDIR)$(pkgdatadir)/ #@$(install_sh_DATA) $^ $(DESTDIR)$(pkgdatadir) uninstall-local: cd $(DESTDIR)$(libdir) && rm -f $(PLUGIN_LIBS) @echo "Uninstalling analysis data files..." rm -f $(DESTDIR)$(pkgdatadir)/*.{info,plot,yoda} endif diff --git a/analyses/pluginATLAS/ATLAS_2016_I1424838.cc b/analyses/pluginATLAS/ATLAS_2016_I1424838.cc --- a/analyses/pluginATLAS/ATLAS_2016_I1424838.cc +++ b/analyses/pluginATLAS/ATLAS_2016_I1424838.cc @@ -1,219 +1,219 @@ #include "Rivet/Analysis.hh" #include "Rivet/Projections/Thrust.hh" #include "Rivet/Projections/ZFinder.hh" #include "Rivet/Projections/FParameter.hh" #include "Rivet/Projections/Spherocity.hh" #include "Rivet/Projections/ChargedFinalState.hh" #include "Rivet/Projections/VetoedFinalState.hh" namespace Rivet { /// @brief Event shapes in leptonic $Z$-events class ATLAS_2016_I1424838 : public Analysis { public: /// Constructor DEFAULT_RIVET_ANALYSIS_CTOR(ATLAS_2016_I1424838); /// Book histograms and initialise projections before the run void init() { // Charged particles inside acceptance region const ChargedFinalState cfs(Cuts::abseta < 2.5 && Cuts::pT > 500*MeV); declare(cfs, "CFS"); // ZFinders ZFinder zfinder(cfs, Cuts::abseta<2.4 && Cuts::pT>20.0*GeV, PID::ELECTRON, 66*GeV, 116*GeV, 0.1, ZFinder::CLUSTERNODECAY); declare(zfinder, "ZFinder"); ZFinder zfinder_mu(cfs, Cuts::abseta<2.4 && Cuts::pT>20.0*GeV, PID::MUON, 66*GeV, 116*GeV, 0.1, ZFinder::CLUSTERNODECAY); declare(zfinder_mu, "ZFinderMu"); // This CFS only contains charged particles inside the acceptance excluding the leptons VetoedFinalState remfs(cfs); remfs.addVetoOnThisFinalState(zfinder); remfs.addVetoOnThisFinalState(zfinder_mu); declare(remfs, "REMFS"); const FParameter fparam(remfs); declare(fparam, "FParameter_"); const Spherocity sphero(remfs); declare(sphero, "Spherocity_"); // Booking of ES histos for (size_t alg = 0; alg < 5; ++alg) { // Book the inclusive histograms size_t offset = alg * 6; _h_Elec_Ntrk[alg] = bookHisto1D(offset + 1, 1, 1); _h_Elec_SumPt[alg] = bookHisto1D(offset + 2, 1, 1); _h_Elec_Beamthrust[alg] = bookHisto1D(offset + 3, 1, 1); _h_Elec_Thrust[alg] = bookHisto1D(offset + 4, 1, 1); _h_Elec_Spherocity[alg] = bookHisto1D(offset + 5, 1, 1); _h_Elec_FParam[alg] = bookHisto1D(offset + 6, 1, 1); _h_Muon_Ntrk[alg] = bookHisto1D(30 + offset + 1, 1, 1); _h_Muon_SumPt[alg] = bookHisto1D(30 + offset + 2, 1, 1); _h_Muon_Beamthrust[alg] = bookHisto1D(30 + offset + 3, 1, 1); _h_Muon_Thrust[alg] = bookHisto1D(30 + offset + 4, 1, 1); _h_Muon_Spherocity[alg] = bookHisto1D(30 + offset + 5, 1, 1); _h_Muon_FParam[alg] = bookHisto1D(30 + offset + 6, 1, 1); } } /// Perform the per-event analysis void analyze(const Event& event) { // Get generator weight const double weight = event.weight(); // Check for Z boson in event const ZFinder& zfinder = apply(event, "ZFinder"); MSG_DEBUG("Num e+ e- pairs found = " << zfinder.bosons().size()); const bool isElec = zfinder.bosons().size() == 1; const ZFinder& zfinder_mu = apply(event, "ZFinderMu"); MSG_DEBUG("Num mu+ mu- pairs found = " << zfinder_mu.bosons().size()); const bool isMuon = zfinder_mu.bosons().size() == 1; // Only accept events with exactly two electrons or exactly two muons if (isElec && isMuon) vetoEvent; if (!(isElec || isMuon)) vetoEvent; // This determines the Zpt phase-space double zpT = -1000; if (isElec) zpT = zfinder.bosons()[0].pT(); if (isMuon) zpT = zfinder_mu.bosons()[0].pT(); unsigned int alg = 4; //< for > 25 GeV if (zpT < 6*GeV) alg = 1; else if (inRange(zpT/GeV, 6, 12)) alg = 2; else if (inRange(zpT/GeV, 12, 25)) alg = 3; assert(alg < 5); assert(alg > 0); // All charged particles within |eta|<2.5 except the leptons from Z-decay const VetoedFinalState& remfs = apply(event, "REMFS"); // sumPt and Beamthrust (the latter will only be filled if the min Nch criterion is met) // and Thrust preparation double sumPt = 0.0, beamThrust = 0.0; vector momenta; for (const Particle& p : remfs.particles()) { const double pT = p.pT(); sumPt += pT; beamThrust += pT*exp(-p.abseta()); const Vector3 mom = p.mom().pTvec(); momenta.push_back(mom); } // Fill inclusive histos if (isElec) { _h_Elec_Ntrk[alg] ->fill(remfs.size(), weight); _h_Elec_Ntrk[0] ->fill(remfs.size(), weight); _h_Elec_SumPt[alg] ->fill(sumPt, weight); _h_Elec_SumPt[0] ->fill(sumPt, weight); } if (isMuon) { _h_Muon_Ntrk[alg] ->fill(remfs.size(), weight); _h_Muon_Ntrk[0] ->fill(remfs.size(), weight); _h_Muon_SumPt[alg] ->fill(sumPt, weight); _h_Muon_SumPt[0] ->fill(sumPt, weight); } // Skip event shape calculation if we don't match the minimum Nch criterion if (remfs.size() >=2) { // Eventshape calculations // Calculate transverse Thrust using all charged FS particles except the lepton // This is copied/inspired from the CMS_6000011_S8957746 analysis if (momenta.size() == 2) { // We need to use a ghost so that Thrust.calc() doesn't return 1. momenta.push_back(Vector3(1e-10*MeV, 0., 0.)); } Thrust thrustC; thrustC.calc(momenta); double thrust = thrustC.thrust(); // F-Parameter const FParameter& fparam = apply(event, "FParameter_"); // Spherocity const Spherocity& sphero = apply(event, "Spherocity_"); // Histos differential in NMPI // Fill inclusive histos if (isElec) { _h_Elec_Thrust[alg] ->fill(thrust, weight); _h_Elec_Thrust[0] ->fill(thrust, weight); _h_Elec_FParam[alg] ->fill(fparam.F(), weight); _h_Elec_FParam[0] ->fill(fparam.F(), weight); _h_Elec_Spherocity[alg] ->fill(sphero.spherocity(), weight); _h_Elec_Spherocity[0] ->fill(sphero.spherocity(), weight); _h_Elec_Beamthrust[alg] ->fill(beamThrust/GeV, weight); _h_Elec_Beamthrust[0] ->fill(beamThrust/GeV, weight); } if (isMuon) { _h_Muon_Thrust[alg] ->fill(thrust, weight); _h_Muon_Thrust[0] ->fill(thrust, weight); _h_Muon_FParam[alg] ->fill(fparam.F(), weight); _h_Muon_FParam[0] ->fill(fparam.F(), weight); _h_Muon_Spherocity[alg] ->fill(sphero.spherocity(), weight); _h_Muon_Spherocity[0] ->fill(sphero.spherocity(), weight); _h_Muon_Beamthrust[alg] ->fill(beamThrust/GeV, weight); _h_Muon_Beamthrust[0] ->fill(beamThrust/GeV, weight); } } } /// Normalise histograms etc., after the run void finalize() { for (size_t alg = 0; alg < 5; ++alg) { - normalize(_h_Elec_Ntrk[alg]); - normalize(_h_Elec_SumPt[alg]); - normalize(_h_Elec_Beamthrust[alg]); + normalize(_h_Elec_Ntrk[alg],100.); + normalize(_h_Elec_SumPt[alg],100.); + normalize(_h_Elec_Beamthrust[alg],100.); normalize(_h_Elec_Thrust[alg]); normalize(_h_Elec_FParam[alg]); normalize(_h_Elec_Spherocity[alg]); - normalize(_h_Muon_Ntrk[alg]); - normalize(_h_Muon_SumPt[alg]); - normalize(_h_Muon_Beamthrust[alg]); + normalize(_h_Muon_Ntrk[alg],100.); + normalize(_h_Muon_SumPt[alg],100.); + normalize(_h_Muon_Beamthrust[alg],100.); normalize(_h_Muon_Thrust[alg]); normalize(_h_Muon_FParam[alg]); normalize(_h_Muon_Spherocity[alg]); } } private: // Convenience method for histogram booking string _mkHistoName(int idDS, int channel, int i) { return "d0" + toString(idDS) + "-x0" + toString(channel) + "-y0" + toString(i+1); } Histo1DPtr _h_Elec_Ntrk[5]; Histo1DPtr _h_Elec_SumPt[5]; Histo1DPtr _h_Elec_Beamthrust[5]; Histo1DPtr _h_Elec_Thrust[5]; Histo1DPtr _h_Elec_FParam[5]; Histo1DPtr _h_Elec_Spherocity[5]; Histo1DPtr _h_Muon_Ntrk[5]; Histo1DPtr _h_Muon_SumPt[5]; Histo1DPtr _h_Muon_Beamthrust[5]; Histo1DPtr _h_Muon_Thrust[5]; Histo1DPtr _h_Muon_FParam[5]; Histo1DPtr _h_Muon_Spherocity[5]; }; DECLARE_RIVET_PLUGIN(ATLAS_2016_I1424838); } diff --git a/analyses/pluginATLAS/ATLAS_2016_I1424838.plot b/analyses/pluginATLAS/ATLAS_2016_I1424838.plot --- a/analyses/pluginATLAS/ATLAS_2016_I1424838.plot +++ b/analyses/pluginATLAS/ATLAS_2016_I1424838.plot @@ -1,434 +1,434 @@ # BEGIN PLOT /ATLAS_2016_I1424838/d01 Title=$N_\text{ch}$, $Z\to e^+e^-$ XLabel=$N_\text{ch}$ -YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}$ +YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch} \times 100$ LogY=0 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d07 Title=$N_\text{ch}$, $Z\to e^+e^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$N_\text{ch}$ -YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}$ +YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}\times 100$ LogY=0 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d13 Title=$N_\text{ch}$, $Z\to e^+e^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$N_\text{ch}$ -YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}$ +YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}\times 100$ LogY=0 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d19 Title=$N_\text{ch}$, $Z\to e^+e^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$N_\text{ch}$ -YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}$ +YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}\times 100$ LogY=0 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d25 Title=$N_\text{ch}$, $Z\to e^+e^-$, $p_\perp(Z) > 25$~GeV XLabel=$N_\text{ch}$ -YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}$ +YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}\times 100$ LogY=0 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d31 Title=$N_\text{ch}$, $Z\to \mu^+\mu^-$ XLabel=$N_\text{ch}$ -YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}$ +YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d37 Title=$N_\text{ch}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$N_\text{ch}$ -YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}$ +YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d43 Title=$N_\text{ch}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$N_\text{ch}$ -YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}$ +YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d49 Title=$N_\text{ch}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$N_\text{ch}$ -YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}$ +YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d55 Title=$N_\text{ch}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) > 25$~GeV XLabel=$N_\text{ch}$ -YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}$ +YLabel=$1/N~ \text{d}N /\text{d}N_\text{ch}\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d02 Title=$\sum p_\perp$, $Z\to e^+e^-$ XLabel=$\sum p_\perp$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp$ +YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d08 Title=$\sum p_\perp$, $Z\to e^+e^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$\sum p_\perp$ -YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp$ +YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d14 Title=$\sum p_\perp$, $Z\to e^+e^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$\sum p_\perp$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp$ +YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d20 Title=$\sum p_\perp$, $Z\to e^+e^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$\sum p_\perp$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp$ +YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d26 Title=$\sum p_\perp$, $Z\to e^+e^-$, $p_\perp(Z) > 25$~GeV XLabel=$\sum p_\perp$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp$ +YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d32 Title=$\sum p_\perp$, $Z\to \mu^+\mu^-$ XLabel=$\sum p_\perp$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp$ +YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d38 Title=$\sum p_\perp$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$\sum p_\perp$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp$ +YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d44 Title=$\sum p_\perp$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$\sum p_\perp$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp$ +YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d50 Title=$\sum p_\perp$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$\sum p_\perp$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp$ +YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d56 Title=$\sum p_\perp$, $Z\to \mu^+\mu^-$, $p_\perp(Z) > 25$~GeV XLabel=$\sum p_\perp$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp$ +YLabel=$1/N~ \text{d}N /\text{d}\sum p_\perp\times 100$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d03 Title=$\mathcal{B}$, $Z\to e^+e^-$ XLabel=$\mathcal{B}$~[GeV] YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] XMax=60 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d09 Title=$\mathcal{B}$, $Z\to e^+e^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$\mathcal{B}$~[GeV] YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] XMax=60 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d15 Title=$\mathcal{B}$, $Z\to e^+e^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$\mathcal{B}$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] +YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] $\times 100$ XMax=60 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d21 Title=$\mathcal{B}$, $Z\to e^+e^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$\mathcal{B}$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] +YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] $\times 100$ XMax=60 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d27 Title=$\mathcal{B}$, $Z\to e^+e^-$, $p_\perp(Z) > 25$~GeV XLabel=$\mathcal{B}$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] +YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] $\times 100$ XMax=60 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d33 Title=$\mathcal{B}$, $Z\to \mu^+\mu^-$ XLabel=$\mathcal{B}$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] +YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] $\times 100$ XMax=60 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d39 Title=$\mathcal{B}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$\mathcal{B}$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] +YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] $\times 100$ XMax=60 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d45 Title=$\mathcal{B}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$\mathcal{B}$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] +YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] $\times 100$ XMax=60 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d51 Title=$\mathcal{B}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$\mathcal{B}$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] +YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] $\times 100$ XMax=60 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d57 Title=$\mathcal{B}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) > 25$~GeV XLabel=$\mathcal{B}$~[GeV] -YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] +YLabel=$1/N~ \text{d}N /\text{d}\mathcal{B}$~[GeV] $\times 100$ XMax=60 LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d04 Title=$\mathcal{T}$, $Z\to e^+e^-$ XLabel=$\mathcal{T}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{T}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d10 Title=$\mathcal{T}$, $Z\to e^+e^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$\mathcal{T}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{T}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d16 Title=$\mathcal{T}$, $Z\to e^+e^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$\mathcal{T}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{T}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d22 Title=$\mathcal{T}$, $Z\to e^+e^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$\mathcal{T}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{T}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d28 Title=$\mathcal{T}$, $Z\to e^+e^-$, $p_\perp(Z) > 25$~GeV XLabel=$\mathcal{T}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{T}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d34 Title=$\mathcal{T}$, $Z\to \mu^+\mu^-$ XLabel=$\mathcal{T}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{T}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d40 Title=$\mathcal{T}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$\mathcal{T}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{T}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d46 Title=$\mathcal{T}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$\mathcal{T}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{T}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d52 Title=$\mathcal{T}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$\mathcal{T}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{T}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d58 Title=$\mathcal{T}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) > 25$~GeV XLabel=$\mathcal{T}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{T}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d06 Title=$\mathcal{F}$, $Z\to e^+e^-$ XLabel=$\mathcal{F}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{F}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d12 Title=$\mathcal{F}$, $Z\to e^+e^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$\mathcal{F}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{F}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d18 Title=$\mathcal{F}$, $Z\to e^+e^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$\mathcal{F}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{F}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d24 Title=$\mathcal{F}$, $Z\to e^+e^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$\mathcal{F}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{F}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d30 Title=$\mathcal{F}$, $Z\to e^+e^-$, $p_\perp(Z) > 25$~GeV XLabel=$\mathcal{F}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{F}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d36 Title=$\mathcal{F}$, $Z\to \mu^+\mu^-$ XLabel=$\mathcal{F}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{F}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d42 Title=$\mathcal{F}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$\mathcal{F}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{F}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d48 Title=$\mathcal{F}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$\mathcal{F}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{F}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d54 Title=$\mathcal{F}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$\mathcal{F}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{F}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d60 Title=$\mathcal{F}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) > 25$~GeV XLabel=$\mathcal{F}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{F}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d05 Title=$\mathcal{S}$, $Z\to e^+e^-$ XLabel=$\mathcal{S}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{S}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d11 Title=$\mathcal{S}$, $Z\to e^+e^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$\mathcal{S}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{S}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d17 Title=$\mathcal{S}$, $Z\to e^+e^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$\mathcal{S}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{S}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d23 Title=$\mathcal{S}$, $Z\to e^+e^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$\mathcal{S}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{S}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d29 Title=$\mathcal{S}$, $Z\to e^+e^-$, $p_\perp(Z) > 25$~GeV XLabel=$\mathcal{S}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{S}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d35 Title=$\mathcal{S}$, $Z\to \mu^+\mu^-$ XLabel=$\mathcal{S}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{S}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d41 Title=$\mathcal{S}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [0,6)$~GeV XLabel=$\mathcal{S}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{S}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d47 Title=$\mathcal{S}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [6,12)$~GeV XLabel=$\mathcal{S}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{S}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d53 Title=$\mathcal{S}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) \in [12,25)$~GeV XLabel=$\mathcal{S}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{S}$ LogY=0 # END PLOT # BEGIN PLOT /ATLAS_2016_I1424838/d59 Title=$\mathcal{S}$, $Z\to \mu^+\mu^-$, $p_\perp(Z) > 25$~GeV XLabel=$\mathcal{S}$ YLabel=$1/N~ \text{d}N /\text{d}\mathcal{S}$ LogY=0 # END PLOT diff --git a/analyses/pluginBABAR/BABAR_2001_I558091.cc b/analyses/pluginBABAR/BABAR_2001_I558091.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2001_I558091.cc @@ -0,0 +1,84 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2001_I558091 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2001_I558091); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(UnstableParticles(), "UFS"); + _c_jpsi = bookCounter("/TMP/jpsi"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const UnstableParticles& ufs = apply(event, "UFS"); + double nJsi=0.; + foreach (const Particle& p, ufs.particles()) { + if (p.pdgId()==443) { + bool fs = true; + foreach (const Particle & child, p.children()) { + if(child.pdgId()==443) { + fs = false; + break; + } + } + if(fs) nJsi += 1.; + } + } + _c_jpsi->fill(nJsi*event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /picobarn; + double sigma = _c_jpsi->val()*fact; + double error = _c_jpsi->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_jpsi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2001_I558091); + + +} diff --git a/analyses/pluginBABAR/BABAR_2001_I558091.info b/analyses/pluginBABAR/BABAR_2001_I558091.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2001_I558091.info @@ -0,0 +1,33 @@ +Name: BABAR_2001_I558091 +Year: 2001 +Summary: Inclusive $J/\psi$ cross section at 10.57 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 558091 +Status: VALIDATED +Authors: + - Your Name +References: + - PRL 87,162002 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of inclusive $J/psi$ production by BaBar for 10.57 GeV.' +BibKey: Aubert:2001pd +BibTeX: '@article{Aubert:2001pd, + author = "Aubert, Bernard and others", + title = "{Measurement of $J/\psi$ production in continuum $e^+e^-$ + annihilations near $\sqrt{s}=10.6$ GeV}", + collaboration = "BaBar", + journal = "Phys. Rev. Lett.", + volume = "87", + year = "2001", + pages = "162002", + doi = "10.1103/PhysRevLett.87.162002", + eprint = "hep-ex/0106044", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BABAR-PUB-01-12, SLAC-PUB-8854", + SLACcitation = "%%CITATION = HEP-EX/0106044;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2001_I558091.plot b/analyses/pluginBABAR/BABAR_2001_I558091.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2001_I558091.plot @@ -0,0 +1,9 @@ +BEGIN PLOT /BABAR_2001_I558091/d01-x01-y01 +Title=$\sigma(e^+e^-\to J/\psi+X)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to J/\psi+X)/pb$ +LogY=0 +ConnectGaps=1 +XMin=10. +XMax=11. +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2001_I558091.yoda b/analyses/pluginBABAR/BABAR_2001_I558091.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2001_I558091.yoda @@ -0,0 +1,12 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2001_I558091/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.21, up: 0.21}, sys: {dn: -0.21, up: 0.21}}} + +IsRef: 1 +Path: /REF/BABAR_2001_I558091/d01-x01-y01 +Title: doi:10.17182/hepdata.19450.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.057000e+01 0.000000e+00 0.000000e+00 2.520000e+00 2.969848e-01 2.969848e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2003_I593379.cc b/analyses/pluginBABAR/BABAR_2003_I593379.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2003_I593379.cc @@ -0,0 +1,186 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/Beam.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Babar charmonium spectra + /// @author Peter Richardson + class BABAR_2003_I593379 : public Analysis { + public: + + BABAR_2003_I593379() + : Analysis("BABAR_2003_I593379"), _weightSum(0.) + { } + + + void analyze(const Event& e) { + const double weight = e.weight(); + + // Find the charmonia + Particles upsilons; + // First in unstable final state + const UnstableParticles& ufs = apply(e, "UFS"); + foreach (const Particle& p, ufs.particles()) + if (p.pid() == 300553) upsilons.push_back(p); + // Then in whole event if fails + if (upsilons.empty()) { + for(ConstGenParticlePtr p: HepMCUtils::particles(e.genEvent())) { + if (p->pdg_id() != 300553) continue; + ConstGenVertexPtr pv = p->production_vertex(); + bool passed = true; + if (pv) { + for(ConstGenParticlePtr pp: HepMCUtils::particles(pv, Relatives::PARENTS)){ + if ( p->pdg_id() == pp->pdg_id() ) { + passed = false; + break; + } + } + } + if (passed) upsilons.push_back(Particle(p)); + } + } + + // Find upsilons + foreach (const Particle& p, upsilons) { + _weightSum += weight; + // Find the charmonium resonances + /// @todo Use Rivet::Particles + vector allJpsi, primaryJpsi, Psiprime, all_chi_c1, all_chi_c2, primary_chi_c1, primary_chi_c2; + findDecayProducts(p.genParticle(), allJpsi, primaryJpsi, Psiprime, + all_chi_c1, all_chi_c2, primary_chi_c1, primary_chi_c2); + const LorentzTransform cms_boost = LorentzTransform::mkFrameTransformFromBeta(p.mom().betaVec()); + for (size_t i = 0; i < allJpsi.size(); i++) { + const double pcm = cms_boost.transform(FourMomentum(allJpsi[i]->momentum())).p(); + _hist_all_Jpsi->fill(pcm, weight); + } + _mult_JPsi->fill(10.58, weight*double(allJpsi.size())); + for (size_t i = 0; i < primaryJpsi.size(); i++) { + const double pcm = cms_boost.transform(FourMomentum(primaryJpsi[i]->momentum())).p(); + _hist_primary_Jpsi->fill(pcm, weight); + } + _mult_JPsi_direct->fill(10.58, weight*double(primaryJpsi.size())); + for (size_t i=0; imomentum())).p(); + _hist_Psi_prime->fill(pcm, weight); + } + _mult_Psi2S->fill(10.58, weight*double(Psiprime.size())); + for (size_t i = 0; i < all_chi_c1.size(); i++) { + const double pcm = cms_boost.transform(FourMomentum(all_chi_c1[i]->momentum())).p(); + _hist_chi_c1->fill(pcm, weight); + } + _mult_chi_c1->fill(10.58, weight*double(all_chi_c1.size())); + _mult_chi_c1_direct->fill(10.58, weight*double(primary_chi_c1.size())); + for (size_t i = 0; i < all_chi_c2.size(); i++) { + const double pcm = cms_boost.transform(FourMomentum(all_chi_c2[i]->momentum())).p(); + _hist_chi_c2->fill(pcm, weight); + } + _mult_chi_c2->fill(10.58, weight*double(all_chi_c2.size())); + _mult_chi_c2_direct->fill(10.58, weight*double(primary_chi_c2.size())); + } + } // analyze + + + void finalize() { + scale(_hist_all_Jpsi , 0.5*0.1/_weightSum); + scale(_hist_chi_c1 , 0.5*0.1/_weightSum); + scale(_hist_chi_c2 , 0.5*0.1/_weightSum); + scale(_hist_Psi_prime , 0.5*0.1/_weightSum); + scale(_hist_primary_Jpsi , 0.5*0.1/_weightSum); + scale(_mult_JPsi , 0.5*100./_weightSum); + scale(_mult_JPsi_direct , 0.5*100./_weightSum); + scale(_mult_chi_c1 , 0.5*100./_weightSum); + scale(_mult_chi_c1_direct, 0.5*100./_weightSum); + scale(_mult_chi_c2 , 0.5*100./_weightSum); + scale(_mult_chi_c2_direct, 0.5*100./_weightSum); + scale(_mult_Psi2S , 0.5*100./_weightSum); + } // finalize + + + void init() { + declare(UnstableParticles(), "UFS"); + + _mult_JPsi = bookHisto1D(1, 1, 1); + _mult_JPsi_direct = bookHisto1D(1, 1, 2); + _mult_chi_c1 = bookHisto1D(1, 1, 3); + _mult_chi_c1_direct = bookHisto1D(1, 1, 4); + _mult_chi_c2 = bookHisto1D(1, 1, 5); + _mult_chi_c2_direct = bookHisto1D(1, 1, 6); + _mult_Psi2S = bookHisto1D(1, 1, 7); + _hist_all_Jpsi = bookHisto1D(6, 1, 1); + _hist_chi_c1 = bookHisto1D(7, 1, 1); + _hist_chi_c2 = bookHisto1D(7, 1, 2); + _hist_Psi_prime = bookHisto1D(8, 1, 1); + _hist_primary_Jpsi = bookHisto1D(10, 1, 1); + } // init + + private: + + //@{ + // count of weights + double _weightSum; + /// Histograms + Histo1DPtr _hist_all_Jpsi; + Histo1DPtr _hist_chi_c1; + Histo1DPtr _hist_chi_c2; + Histo1DPtr _hist_Psi_prime; + Histo1DPtr _hist_primary_Jpsi; + + Histo1DPtr _mult_JPsi; + Histo1DPtr _mult_JPsi_direct; + Histo1DPtr _mult_chi_c1; + Histo1DPtr _mult_chi_c1_direct; + Histo1DPtr _mult_chi_c2; + Histo1DPtr _mult_chi_c2_direct; + Histo1DPtr _mult_Psi2S; + //@} + + void findDecayProducts(ConstGenParticlePtr p, + vector& allJpsi, + vector& primaryJpsi, + vector& Psiprime, + vector& all_chi_c1, vector& all_chi_c2, + vector& primary_chi_c1, vector& primary_chi_c2) { + ConstGenVertexPtr dv = p->end_vertex(); + bool isOnium = false; + /// @todo Use better looping + for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::PARENTS)){ + int id = pp->pdg_id(); + id = id%1000; + id -= id%10; + id /= 10; + if (id==44) isOnium = true; + } + /// @todo Use better looping + for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ + int id = pp->pdg_id(); + if (id==100443) { + Psiprime.push_back(pp); + } + else if (id==20443) { + all_chi_c1.push_back(pp); + if (!isOnium) primary_chi_c1.push_back(pp); + } + else if (id==445) { + all_chi_c2.push_back(pp); + if (!isOnium) primary_chi_c2.push_back(pp); + } + else if (id==443) { + allJpsi.push_back(pp); + if (!isOnium) primaryJpsi.push_back(pp); + } + if (pp->end_vertex()) { + findDecayProducts(pp, allJpsi, primaryJpsi, Psiprime, all_chi_c1, all_chi_c2, primary_chi_c1, primary_chi_c2); + } + } + } + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2003_I593379); + +} diff --git a/analyses/pluginMisc/BABAR_2003_I593379.info b/analyses/pluginBABAR/BABAR_2003_I593379.info rename from analyses/pluginMisc/BABAR_2003_I593379.info rename to analyses/pluginBABAR/BABAR_2003_I593379.info diff --git a/analyses/pluginMisc/BABAR_2003_I593379.plot b/analyses/pluginBABAR/BABAR_2003_I593379.plot rename from analyses/pluginMisc/BABAR_2003_I593379.plot rename to analyses/pluginBABAR/BABAR_2003_I593379.plot diff --git a/analyses/pluginMisc/BABAR_2003_I593379.yoda b/analyses/pluginBABAR/BABAR_2003_I593379.yoda rename from analyses/pluginMisc/BABAR_2003_I593379.yoda rename to analyses/pluginBABAR/BABAR_2003_I593379.yoda diff --git a/analyses/pluginBABAR/BABAR_2004_I656680.cc b/analyses/pluginBABAR/BABAR_2004_I656680.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2004_I656680.cc @@ -0,0 +1,88 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2004_I656680 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2004_I656680); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + _num3pi = bookCounter("TMP/num3"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=3) vetoEvent; + if(nCount[-211]==1&&nCount[211]==1&&nCount[111]==1) + _num3pi->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _num3pi->val(); + double error = _num3pi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _num3pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2004_I656680); + + +} diff --git a/analyses/pluginBABAR/BABAR_2004_I656680.info b/analyses/pluginBABAR/BABAR_2004_I656680.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2004_I656680.info @@ -0,0 +1,35 @@ +Name: BABAR_2004_I656680 +Year: 2004 +Summary: Cross section for $e^+e^-\to$ $\pi^+\pi^-\pi^0$ between 1.05 and 2.325 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 656680 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D70 (2004) 072004, 2004 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ by BaBar using radiative return for + energies between 1.05 and 2.325 GeV.' +Keywords: +BibKey: Aubert:2004kj +BibTeX: '@article{Aubert:2004kj, + author = "Aubert, Bernard and others", + title = "{Study of $e^+e^- \to \pi^+ \pi^- \pi^0$ process using + initial state radiation with BaBar}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D70", + year = "2004", + pages = "072004", + doi = "10.1103/PhysRevD.70.072004", + eprint = "hep-ex/0408078", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-10624, BABAR-PUB-04-034", + SLACcitation = "%%CITATION = HEP-EX/0408078;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2004_I656680.plot b/analyses/pluginBABAR/BABAR_2004_I656680.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2004_I656680.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BABAR_2004_I656680/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2004_I656680.yoda b/analyses/pluginBABAR/BABAR_2004_I656680.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2004_I656680.yoda @@ -0,0 +1,89 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2004_I656680/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.53, up: 0.53}, sys: {dn: -0.13, up: 0.13}}, 1: {stat: {dn: -0.61, up: 0.61}, sys: {dn: -0.21, up: 0.21}}, 2: {stat: {dn: -0.63, up: 0.63}, sys: {dn: -0.21, up: 0.21}}, 3: {stat: {dn: -0.66, up: 0.66}, sys: {dn: -0.25, up: 0.25}}, 4: {stat: {dn: -0.62, up: 0.62}, sys: {dn: -0.22, up: 0.22}}, 5: {stat: {dn: -0.65, up: 0.65}, sys: {dn: -0.25, up: 0.25}}, 6: {stat: {dn: -0.65, up: 0.65}, sys: {dn: -0.26, up: 0.26}}, 7: {stat: {dn: -0.71, up: 0.71}, sys: {dn: -0.31, up: 0.31}}, 8: {stat: {dn: -0.65, up: 0.65}, sys: {dn: -0.27, up: 0.27}}, 9: {stat: {dn: -0.62, up: 0.62}, sys: {dn: -0.25, up: 0.25}}, 10: {stat: {dn: -0.65, up: 0.65}, sys: {dn: -0.31, up: 0.31}}, 11: {stat: {dn: -0.55, up: 0.55}, sys: {dn: -0.23, up: 0.23}}, 12: {stat: {dn: -0.56, up: 0.56}, sys: {dn: -0.24, up: 0.24}}, 13: {stat: {dn: -0.53, up: 0.53}, sys: {dn: -0.21, up: 0.21}}, 14: {stat: {dn: -0.54, up: 0.54}, sys: {dn: -0.24, up: 0.24}}, 15: {stat: {dn: -0.49, up: 0.49}, sys: {dn: -0.2, up: 0.2}}, 16: {stat: {dn: -0.54, up: 0.54}, sys: {dn: -0.21, up: 0.21}}, 17: {stat: {dn: -0.52, up: 0.52}, sys: {dn: -0.2, up: 0.2}}, 18: {stat: {dn: -0.53, up: 0.53}, sys: {dn: -0.22, up: 0.22}}, 19: {stat: {dn: -0.5, up: 0.5}, sys: {dn: -0.19, up: 0.19}}, 20: {stat: {dn: -0.56, up: 0.56}, sys: {dn: -0.28, up: 0.28}}, 21: {stat: {dn: -0.56, up: 0.56}, sys: {dn: -0.27, up: 0.27}}, 22: {stat: {dn: -0.58, up: 0.58}, sys: {dn: -0.31, up: 0.31}}, 23: {stat: {dn: -0.55, up: 0.55}, sys: {dn: -0.27, up: 0.27}}, 24: {stat: {dn: -0.5, up: 0.5}, sys: {dn: -0.24, up: 0.24}}, 25: {stat: {dn: -0.4, up: 0.4}, sys: {dn: -0.14, up: 0.14}}, 26: {stat: {dn: -0.36, up: 0.36}, sys: {dn: -0.12, up: 0.12}}, 27: {stat: {dn: -0.31, up: 0.31}, sys: {dn: -0.08, up: 0.08}}, 28: {stat: {dn: -0.31, up: 0.31}, sys: {dn: -0.09, up: 0.09}}, 29: {stat: {dn: -0.29, up: 0.29}, sys: {dn: -0.07, up: 0.07}}, 30: {stat: {dn: -0.26, up: 0.26}, sys: {dn: -0.06, up: 0.06}}, 31: {stat: {dn: -0.27, up: 0.27}, sys: {dn: -0.07, up: 0.07}}, 32: {stat: {dn: -0.26, up: 0.26}, sys: {dn: -0.07, up: 0.07}}, 33: {stat: {dn: -0.24, up: 0.24}, sys: {dn: -0.07, up: 0.07}}, 34: {stat: {dn: -0.22, up: 0.22}, sys: {dn: -0.06, up: 0.06}}, 35: {stat: {dn: -0.21, up: 0.21}, sys: {dn: -0.05, up: 0.05}}, 36: {stat: {dn: -0.19, up: 0.19}, sys: {dn: -0.04, up: 0.04}}, 37: {stat: {dn: -0.16, up: 0.16}, sys: {dn: -0.03, up: 0.03}}, 38: {stat: {dn: -0.18, up: 0.18}, sys: {dn: -0.04, up: 0.04}}, 39: {stat: {dn: -0.17, up: 0.17}, sys: {dn: -0.04, up: 0.04}}, 40: {stat: {dn: -0.15, up: 0.15}, sys: {dn: -0.02, up: 0.02}}, 41: {stat: {dn: -0.17, up: 0.17}, sys: {dn: -0.04, up: 0.04}}, 42: {stat: {dn: -0.16, up: 0.16}, sys: {dn: -0.03, up: 0.03}}, 43: {stat: {dn: -0.15, up: 0.15}, sys: {dn: -0.03, up: 0.03}}, 44: {stat: {dn: -0.16, up: 0.16}, sys: {dn: -0.03, up: 0.03}}, 45: {stat: {dn: -0.15, up: 0.15}, sys: {dn: -0.03, up: 0.03}}, 46: {stat: {dn: -0.14, up: 0.14}, sys: {dn: -0.02, up: 0.02}}, 47: {stat: {dn: -0.13, up: 0.13}, sys: {dn: -0.02, up: 0.02}}, 48: 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64: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.01, up: 0.01}}, 65: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.01, up: 0.01}}, 66: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.01, up: 0.01}}, 67: {stat: {dn: -0.08, up: 0.08}, sys: {dn: -0.01, up: 0.01}}, 68: {stat: {dn: -0.07, up: 0.07}, sys: {dn: -0.01, up: 0.01}}, 69: {stat: {dn: -0.07, up: 0.07}, sys: {dn: -0.01, up: 0.01}}, 70: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.01, up: 0.01}}, 71: {stat: {dn: -0.08, up: 0.08}, sys: {dn: -0.01, up: 0.01}}, 72: {stat: {dn: -0.07, up: 0.07}, sys: {dn: -0.01, up: 0.01}}, 73: {stat: {dn: -0.07, up: 0.07}, sys: {dn: -0.01, up: 0.01}}, 74: {stat: {dn: -0.07, up: 0.07}, sys: {dn: -0.01, up: 0.01}}, 75: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.02, up: 0.02}}, 76: {stat: {dn: -0.06, up: 0.06}, sys: {dn: -0.01, up: 0.01}}, 77: {stat: {dn: -0.08, up: 0.08}, sys: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2004_I656680/d01-x01-y01 +Title: doi:10.17182/hepdata.41884.v1/t1 +Type: Scatter2D +--- +# 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0.000000e+00 2.600000e-01 9.219544e-02 9.219544e-02 +2.962500e+00 0.000000e+00 0.000000e+00 -1.000000e-02 6.082763e-02 6.082763e-02 +2.987500e+00 0.000000e+00 0.000000e+00 2.000000e-01 8.062258e-02 8.062258e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2005_I676691.cc b/analyses/pluginBABAR/BABAR_2005_I676691.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2005_I676691.cc @@ -0,0 +1,107 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2005_I676691 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2005_I676691); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + _c2pip2pim = bookCounter("TMP/2pip2pim"); + _cKpKmpippim = bookCounter("TMP/KpKmpippim"); + _c2Kp2Km = bookCounter("TMP/2Kp2Km"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + if(ntotal!=4) vetoEvent; + + if( nCount[211]==2 && nCount[-211]==2) + _c2pip2pim->fill(event.weight()); + else if(nCount[321]==1 && nCount[-321]==1 && nCount[211]==1 && nCount[-211]==1) + _cKpKmpippim->fill(event.weight()); + else if( nCount[321]==2 && nCount[-321]==2) + _c2Kp2Km->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + + for(unsigned int ix=1;ix<4;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _c2pip2pim->val(); + error = _c2pip2pim->err(); + } + else if(ix==2) { + sigma = _cKpKmpippim->val(); + error = _cKpKmpippim->err(); + } + else if(ix==3) { + sigma = _c2Kp2Km->val(); + error = _c2Kp2Km->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c2pip2pim, _cKpKmpippim, _c2Kp2Km; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2005_I676691); + + +} diff --git a/analyses/pluginBABAR/BABAR_2005_I676691.info b/analyses/pluginBABAR/BABAR_2005_I676691.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2005_I676691.info @@ -0,0 +1,37 @@ +Name: BABAR_2005_I676691 +Year: 2005 +Summary: $e^+e^- \to$ $2\pi^+2\pi^-$, $K^+K^-\pi^+\pi^-$ and $2K^+2K^-$ cross-sections between the threshold to 4.5 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 676691 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D71 (2005) 052001, 2005 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + ' $e^+e^- \to$ $2\pi^+2\pi^-$, $K^+K^-\pi^+\pi^-$ and $2K^+2K^-$ cross-sections measured by BaBar using radiative return from threshold to 4.5 GeV.' +Keywords: [] +BibKey: Aubert:2005eg +BibTeX: '@article{Aubert:2005eg, + author = "Aubert, Bernard and others", + title = "{The $e^+e^- \to \pi^+ \pi^- \pi^+ \pi^-$, $K^+ K^- \pi^+ + \pi^-$, and $K^+ K^- K^+ K^-$ cross sections at + center-of-mass energies 0.5-GeV - 4.5-GeV measured with + initial-state radiation}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D71", + year = "2005", + pages = "052001", + doi = "10.1103/PhysRevD.71.052001", + eprint = "hep-ex/0502025", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-11026", + SLACcitation = "%%CITATION = HEP-EX/0502025;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2005_I676691.plot b/analyses/pluginBABAR/BABAR_2005_I676691.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2005_I676691.plot @@ -0,0 +1,18 @@ +BEGIN PLOT /BABAR_2005_I676691/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2005_I676691/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2005_I676691/d03-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-K^+K^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2005_I676691.yoda b/analyses/pluginBABAR/BABAR_2005_I676691.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2005_I676691.yoda @@ -0,0 +1,337 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_I676691/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.19, up: 0.19}}, 1: {error: {dn: -0.13, up: 0.13}}, 2: {error: {dn: -0.16, up: 0.16}}, 3: {error: {dn: -0.07, up: 0.07}}, 4: {error: {dn: -0.0, up: 0.0}}, 5: {error: {dn: -0.05, up: 0.05}}, 6: {error: {dn: -0.03, up: 0.03}}, 7: {error: {dn: -0.08, up: 0.08}}, 8: {error: {dn: -0.05, up: 0.05}}, 9: {error: {dn: -0.08, up: 0.08}}, 10: {error: {dn: -0.09, up: 0.09}}, 11: {error: {dn: -0.09, up: 0.09}}, 12: {error: {dn: -0.11, up: 0.11}}, 13: {error: {dn: -0.11, up: 0.11}}, 14: {error: {dn: -0.14, up: 0.14}}, 15: {error: {dn: -0.16, up: 0.16}}, 16: {error: {dn: -0.17, up: 0.17}}, 17: {error: {dn: -0.2, up: 0.2}}, 18: {error: {dn: 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+4.450000e+00 0.000000e+00 0.000000e+00 0.000000e+00 2.000000e-02 2.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_I676691/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.0, up: 0.0}, sys: {dn: -0.0, up: 0.0}}, 1: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.0045, up: 0.0045}}, 2: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.0165, up: 0.0165}}, 3: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.0435, up: 0.0435}}, 4: {error: {dn: -0.13, up: 0.13}, sys: {dn: -0.087, up: 0.087}}, 5: {error: {dn: -0.15, up: 0.15}, sys: {dn: -0.144, up: 0.144}}, 6: {error: {dn: -0.19, up: 0.19}, sys: {dn: -0.183, up: 0.183}}, 7: {error: {dn: -0.22, up: 0.22}, sys: {dn: -0.24, up: 0.24}}, 8: {error: {dn: -0.25, up: 0.25}, sys: {dn: -0.267, up: 0.267}}, 9: {error: {dn: -0.3, up: 0.3}, sys: {dn: -0.40049999999999997, up: 0.40049999999999997}}, 10: {error: {dn: -0.33, up: 0.33}, sys: {dn: -0.4215, up: 0.4215}}, 11: {error: {dn: -0.34, up: 0.34}, sys: {dn: -0.44850000000000007, up: 0.44850000000000007}}, 12: {error: {dn: -0.36, up: 0.36}, sys: {dn: -0.558, up: 0.558}}, 13: {error: {dn: -0.4, up: 0.4}, sys: {dn: -0.624, up: 0.624}}, 14: {error: {dn: -0.41, up: 0.41}, sys: {dn: -0.687, up: 0.687}}, 15: {error: {dn: -0.41, up: 0.41}, sys: {dn: -0.651, up: 0.651}}, 16: {error: {dn: -0.38, up: 0.38}, sys: {dn: -0.627, up: 0.627}}, 17: {error: {dn: -0.42, up: 0.42}, sys: {dn: -0.705, up: 0.705}}, 18: {error: {dn: -0.38, up: 0.38}, sys: {dn: -0.6014999999999999, up: 0.6014999999999999}}, 19: {error: {dn: -0.38, up: 0.38}, sys: {dn: -0.6165, up: 0.6165}}, 20: {error: {dn: -0.33, up: 0.33}, sys: {dn: -0.462, up: 0.462}}, 21: {error: {dn: -0.33, up: 0.33}, sys: {dn: -0.4785, up: 0.4785}}, 22: {error: {dn: -0.35, up: 0.35}, sys: {dn: -0.498, up: 0.498}}, 23: {error: {dn: -0.32, up: 0.32}, sys: {dn: -0.41850000000000004, up: 0.41850000000000004}}, 24: {error: {dn: -0.32, up: 0.32}, sys: {dn: -0.49649999999999994, up: 0.49649999999999994}}, 25: {error: {dn: -0.32, up: 0.32}, sys: {dn: -0.426, up: 0.426}}, 26: {error: {dn: -0.28, up: 0.28}, sys: {dn: -0.372, up: 0.372}}, 27: {error: {dn: -0.3, up: 0.3}, sys: {dn: -0.42450000000000004, up: 0.42450000000000004}}, 28: {error: {dn: -0.25, up: 0.25}, sys: {dn: -0.3, up: 0.3}}, 29: {error: {dn: -0.24, up: 0.24}, sys: {dn: -0.26849999999999996, up: 0.26849999999999996}}, 30: {error: {dn: -0.26, up: 0.26}, sys: {dn: -0.327, up: 0.327}}, 31: {error: {dn: -0.23, up: 0.23}, sys: {dn: -0.2295, up: 0.2295}}, 32: {error: {dn: -0.24, up: 0.24}, sys: {dn: -0.2865, up: 0.2865}}, 33: {error: {dn: -0.24, up: 0.24}, sys: {dn: -0.2595, up: 0.2595}}, 34: {error: {dn: -0.21, up: 0.21}, sys: {dn: -0.2655, up: 0.2655}}, 35: {error: {dn: -0.22, up: 0.22}, sys: {dn: -0.231, up: 0.231}}, 36: {error: {dn: -0.23, up: 0.23}, sys: {dn: -0.30149999999999993, up: 0.30149999999999993}}, 37: {error: {dn: -0.2, up: 0.2}, sys: {dn: -0.207, up: 0.207}}, 38: {error: {dn: -0.22, up: 0.22}, sys: {dn: -0.2415, up: 0.2415}}, 39: {error: {dn: -0.21, up: 0.21}, sys: {dn: -0.276, up: 0.276}}, 40: {error: {dn: -0.19, up: 0.19}, sys: {dn: -0.1905, up: 0.1905}}, 41: {error: {dn: -0.18, up: 0.18}, sys: {dn: -0.18, up: 0.18}}, 42: {error: {dn: -0.19, up: 0.19}, sys: {dn: -0.23700000000000002, up: 0.23700000000000002}}, 43: {error: {dn: -0.17, up: 0.17}, sys: {dn: -0.183, up: 0.183}}, 44: {error: {dn: -0.16, up: 0.16}, sys: {dn: -0.15300000000000002, up: 0.15300000000000002}}, 45: {error: {dn: -0.16, up: 0.16}, sys: {dn: -0.1545, up: 0.1545}}, 46: {error: {dn: -0.17, up: 0.17}, sys: {dn: -0.1245, up: 0.1245}}, 47: {error: {dn: -0.14, up: 0.14}, sys: {dn: -0.1035, up: 0.1035}}, 48: {error: {dn: -0.17, up: 0.17}, sys: {dn: -0.177, up: 0.177}}, 49: {error: {dn: -0.15, up: 0.15}, sys: {dn: -0.1005, up: 0.1005}}, 50: {error: {dn: -0.14, up: 0.14}, sys: {dn: -0.147, up: 0.147}}, 51: {error: {dn: -0.14, up: 0.14}, sys: {dn: -0.117, up: 0.117}}, 52: {error: {dn: -0.13, up: 0.13}, sys: {dn: -0.108, up: 0.108}}, 53: {error: {dn: -0.13, up: 0.13}, sys: {dn: -0.1155, up: 0.1155}}, 54: {error: {dn: -0.13, up: 0.13}, sys: {dn: -0.0945, up: 0.0945}}, 55: {error: {dn: -0.12, up: 0.12}, sys: {dn: -0.04200000000000001, up: 0.04200000000000001}}, 56: {error: {dn: -0.13, up: 0.13}, sys: {dn: -0.072, up: 0.072}}, 57: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.0795, up: 0.0795}}, 58: {error: {dn: -0.12, up: 0.12}, sys: {dn: -0.066, up: 0.066}}, 59: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.081, up: 0.081}}, 60: {error: {dn: -0.12, up: 0.12}, sys: {dn: -0.072, up: 0.072}}, 61: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.0585, up: 0.0585}}, 62: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.069, up: 0.069}}, 63: {error: {dn: -0.24, up: 0.24}, sys: {dn: -0.36, up: 0.36}}, 64: {error: {dn: -0.17, up: 0.17}, sys: {dn: -0.195, up: 0.195}}, 65: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.0885, up: 0.0885}}, 66: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.072, up: 0.072}}, 67: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.048, up: 0.048}}, 68: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.08549999999999999, up: 0.08549999999999999}}, 69: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.069, up: 0.069}}, 70: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.06, up: 0.06}}, 71: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.048, up: 0.048}}, 72: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.06, up: 0.06}}, 73: {error: {dn: -0.07, up: 0.07}, sys: {dn: -0.0375, up: 0.0375}}, 74: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.06, up: 0.06}}, 75: {error: {dn: -0.07, up: 0.07}, sys: {dn: -0.036, up: 0.036}}, 76: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.033, up: 0.033}}, 77: {error: {dn: -0.0, up: 0.0}, sys: {dn: -0.0, up: 0.0}}, 78: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.036, up: 0.036}}, 79: {error: {dn: -0.07, up: 0.07}, sys: {dn: -0.0315, up: 0.0315}}, 80: {error: {dn: -0.07, up: 0.07}, sys: {dn: -0.0495, up: 0.0495}}, 81: {error: {dn: -0.07, up: 0.07}, sys: {dn: -0.0435, up: 0.0435}}, 82: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.033, up: 0.033}}, 83: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.010500000000000002, up: 0.010500000000000002}}, 84: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.012, up: 0.012}}, 85: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.012, up: 0.012}}, 86: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.024, up: 0.024}}, 87: {error: {dn: -0.07, up: 0.07}, sys: {dn: -0.0315, up: 0.0315}}, 88: {error: {dn: -0.07, up: 0.07}, sys: {dn: -0.036, up: 0.036}}, 89: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.0165, up: 0.0165}}, 90: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.0345, up: 0.0345}}, 91: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.0195, up: 0.0195}}, 92: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.009, up: 0.009}}, 93: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.0195, up: 0.0195}}, 94: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.012, up: 0.012}}, 95: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.012, up: 0.012}}, 96: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.010500000000000002, up: 0.010500000000000002}}, 97: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.010500000000000002, up: 0.010500000000000002}}, 98: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.015, up: 0.015}}, 99: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.0045, up: 0.0045}}, 100: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.006, up: 0.006}}, 101: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.0195, up: 0.0195}}, 102: {error: {dn: -0.0, up: 0.0}, sys: {dn: -0.0, up: 0.0}}, 103: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.003, up: 0.003}}, 104: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.0075, up: 0.0075}}, 105: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.0, up: 0.0}}, 106: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.006, up: 0.006}}, 107: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.006, up: 0.006}}, 108: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.009, up: 0.009}}, 109: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.0015, up: 0.0015}}, 110: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.0195, up: 0.0195}}, 111: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.006, up: 0.006}}, 112: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.003, up: 0.003}}, 113: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.009, up: 0.009}}, 114: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.0, up: 0.0}}, 115: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.003, up: 0.003}}, 116: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.0075, up: 0.0075}}, 117: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.0075, up: 0.0075}}, 118: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.0075, up: 0.0075}}, 119: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.009, up: 0.009}}} + +IsRef: 1 +Path: /REF/BABAR_2005_I676691/d02-x01-y01 +Title: doi:10.17182/hepdata.22111.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.512500e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.537500e+00 0.000000e+00 0.000000e+00 3.000000e-02 5.020209e-02 5.020209e-02 +1.562500e+00 0.000000e+00 0.000000e+00 1.100000e-01 5.265216e-02 5.265216e-02 +1.587500e+00 0.000000e+00 0.000000e+00 2.900000e-01 9.106179e-02 9.106179e-02 +1.612500e+00 0.000000e+00 0.000000e+00 5.800000e-01 1.564257e-01 1.564257e-01 +1.637500e+00 0.000000e+00 0.000000e+00 9.600000e-01 2.079327e-01 2.079327e-01 +1.662500e+00 0.000000e+00 0.000000e+00 1.220000e+00 2.637973e-01 2.637973e-01 +1.687500e+00 0.000000e+00 0.000000e+00 1.600000e+00 3.255764e-01 3.255764e-01 +1.712500e+00 0.000000e+00 0.000000e+00 1.780000e+00 3.657718e-01 3.657718e-01 +1.737500e+00 0.000000e+00 0.000000e+00 2.670000e+00 5.004001e-01 5.004001e-01 +1.762500e+00 0.000000e+00 0.000000e+00 2.810000e+00 5.353151e-01 5.353151e-01 +1.787500e+00 0.000000e+00 0.000000e+00 2.990000e+00 5.628075e-01 5.628075e-01 +1.812500e+00 0.000000e+00 0.000000e+00 3.720000e+00 6.640512e-01 6.640512e-01 +1.837500e+00 0.000000e+00 0.000000e+00 4.160000e+00 7.411990e-01 7.411990e-01 +1.862500e+00 0.000000e+00 0.000000e+00 4.580000e+00 8.000431e-01 8.000431e-01 +1.887500e+00 0.000000e+00 0.000000e+00 4.340000e+00 7.693510e-01 7.693510e-01 +1.912500e+00 0.000000e+00 0.000000e+00 4.180000e+00 7.331637e-01 7.331637e-01 +1.937500e+00 0.000000e+00 0.000000e+00 4.700000e+00 8.206248e-01 8.206248e-01 +1.962500e+00 0.000000e+00 0.000000e+00 4.010000e+00 7.114789e-01 7.114789e-01 +1.987500e+00 0.000000e+00 0.000000e+00 4.110000e+00 7.242046e-01 7.242046e-01 +2.012500e+00 0.000000e+00 0.000000e+00 3.080000e+00 5.677535e-01 5.677535e-01 +2.037500e+00 0.000000e+00 0.000000e+00 3.190000e+00 5.812592e-01 5.812592e-01 +2.062500e+00 0.000000e+00 0.000000e+00 3.320000e+00 6.086904e-01 6.086904e-01 +2.087500e+00 0.000000e+00 0.000000e+00 2.790000e+00 5.268228e-01 5.268228e-01 +2.112500e+00 0.000000e+00 0.000000e+00 3.310000e+00 5.906879e-01 5.906879e-01 +2.137500e+00 0.000000e+00 0.000000e+00 2.840000e+00 5.328002e-01 5.328002e-01 +2.162500e+00 0.000000e+00 0.000000e+00 2.480000e+00 4.656007e-01 4.656007e-01 +2.187500e+00 0.000000e+00 0.000000e+00 2.830000e+00 5.198079e-01 5.198079e-01 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2.690544e-01 2.690544e-01 +2.537500e+00 0.000000e+00 0.000000e+00 1.200000e+00 2.545584e-01 2.545584e-01 +2.562500e+00 0.000000e+00 0.000000e+00 1.580000e+00 3.037581e-01 3.037581e-01 +2.587500e+00 0.000000e+00 0.000000e+00 1.220000e+00 2.497779e-01 2.497779e-01 +2.612500e+00 0.000000e+00 0.000000e+00 1.020000e+00 2.213798e-01 2.213798e-01 +2.637500e+00 0.000000e+00 0.000000e+00 1.030000e+00 2.224191e-01 2.224191e-01 +2.662500e+00 0.000000e+00 0.000000e+00 8.300000e-01 2.107137e-01 2.107137e-01 +2.687500e+00 0.000000e+00 0.000000e+00 6.900000e-01 1.741041e-01 1.741041e-01 +2.712500e+00 0.000000e+00 0.000000e+00 1.180000e+00 2.454160e-01 2.454160e-01 +2.737500e+00 0.000000e+00 0.000000e+00 6.700000e-01 1.805554e-01 1.805554e-01 +2.762500e+00 0.000000e+00 0.000000e+00 9.800000e-01 2.030000e-01 2.030000e-01 +2.787500e+00 0.000000e+00 0.000000e+00 7.800000e-01 1.824527e-01 1.824527e-01 +2.812500e+00 0.000000e+00 0.000000e+00 7.200000e-01 1.690089e-01 1.690089e-01 +2.837500e+00 0.000000e+00 0.000000e+00 7.700000e-01 1.738972e-01 1.738972e-01 +2.862500e+00 0.000000e+00 0.000000e+00 6.300000e-01 1.607179e-01 1.607179e-01 +2.887500e+00 0.000000e+00 0.000000e+00 2.800000e-01 1.271377e-01 1.271377e-01 +2.912500e+00 0.000000e+00 0.000000e+00 4.800000e-01 1.486069e-01 1.486069e-01 +2.937500e+00 0.000000e+00 0.000000e+00 5.300000e-01 1.357212e-01 1.357212e-01 +2.962500e+00 0.000000e+00 0.000000e+00 4.400000e-01 1.369525e-01 1.369525e-01 +2.987500e+00 0.000000e+00 0.000000e+00 5.400000e-01 1.366053e-01 1.366053e-01 +3.012500e+00 0.000000e+00 0.000000e+00 4.800000e-01 1.399428e-01 1.399428e-01 +3.037500e+00 0.000000e+00 0.000000e+00 3.900000e-01 1.245883e-01 1.245883e-01 +3.062500e+00 0.000000e+00 0.000000e+00 4.600000e-01 1.298499e-01 1.298499e-01 +3.087500e+00 0.000000e+00 0.000000e+00 2.400000e+00 4.326662e-01 4.326662e-01 +3.112500e+00 0.000000e+00 0.000000e+00 1.300000e+00 2.586987e-01 2.586987e-01 +3.137500e+00 0.000000e+00 0.000000e+00 5.900000e-01 1.411816e-01 1.411816e-01 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8.772685e-02 8.772685e-02 +3.487500e+00 0.000000e+00 0.000000e+00 2.100000e-01 7.676099e-02 7.676099e-02 +3.512500e+00 0.000000e+00 0.000000e+00 3.300000e-01 8.573360e-02 8.573360e-02 +3.537500e+00 0.000000e+00 0.000000e+00 2.900000e-01 8.241511e-02 8.241511e-02 +3.562500e+00 0.000000e+00 0.000000e+00 2.200000e-01 6.847627e-02 6.847627e-02 +3.587500e+00 0.000000e+00 0.000000e+00 7.000000e-02 6.091182e-02 6.091182e-02 +3.612500e+00 0.000000e+00 0.000000e+00 8.000000e-02 5.141984e-02 5.141984e-02 +3.637500e+00 0.000000e+00 0.000000e+00 8.000000e-02 5.141984e-02 5.141984e-02 +3.662500e+00 0.000000e+00 0.000000e+00 1.600000e-01 6.462198e-02 6.462198e-02 +3.687500e+00 0.000000e+00 0.000000e+00 2.100000e-01 7.676099e-02 7.676099e-02 +3.712500e+00 0.000000e+00 0.000000e+00 2.400000e-01 7.871467e-02 7.871467e-02 +3.737500e+00 0.000000e+00 0.000000e+00 1.100000e-01 6.222741e-02 6.222741e-02 +3.762500e+00 0.000000e+00 0.000000e+00 2.300000e-01 6.921163e-02 6.921163e-02 +3.787500e+00 0.000000e+00 0.000000e+00 1.300000e-01 5.366796e-02 5.366796e-02 +3.812500e+00 0.000000e+00 0.000000e+00 6.000000e-02 5.080354e-02 5.080354e-02 +3.837500e+00 0.000000e+00 0.000000e+00 1.300000e-01 6.308922e-02 6.308922e-02 +3.862500e+00 0.000000e+00 0.000000e+00 8.000000e-02 6.118823e-02 6.118823e-02 +3.887500e+00 0.000000e+00 0.000000e+00 8.000000e-02 5.141984e-02 5.141984e-02 +3.912500e+00 0.000000e+00 0.000000e+00 7.000000e-02 4.135517e-02 4.135517e-02 +3.937500e+00 0.000000e+00 0.000000e+00 7.000000e-02 5.109061e-02 5.109061e-02 +3.962500e+00 0.000000e+00 0.000000e+00 1.000000e-01 5.220153e-02 5.220153e-02 +3.987500e+00 0.000000e+00 0.000000e+00 3.000000e-02 5.020209e-02 5.020209e-02 +4.012500e+00 0.000000e+00 0.000000e+00 4.000000e-02 4.044750e-02 4.044750e-02 +4.037500e+00 0.000000e+00 0.000000e+00 1.300000e-01 5.366796e-02 5.366796e-02 +4.062500e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.087500e+00 0.000000e+00 0.000000e+00 2.000000e-02 4.011234e-02 4.011234e-02 +4.112500e+00 0.000000e+00 0.000000e+00 5.000000e-02 4.069705e-02 4.069705e-02 +4.137500e+00 0.000000e+00 0.000000e+00 0.000000e+00 4.000000e-02 4.000000e-02 +4.162500e+00 0.000000e+00 0.000000e+00 4.000000e-02 4.044750e-02 4.044750e-02 +4.187500e+00 0.000000e+00 0.000000e+00 4.000000e-02 5.035871e-02 5.035871e-02 +4.212500e+00 0.000000e+00 0.000000e+00 6.000000e-02 4.100000e-02 4.100000e-02 +4.237500e+00 0.000000e+00 0.000000e+00 1.000000e-02 4.002812e-02 4.002812e-02 +4.262500e+00 0.000000e+00 0.000000e+00 1.300000e-01 4.450000e-02 4.450000e-02 +4.287500e+00 0.000000e+00 0.000000e+00 4.000000e-02 4.044750e-02 4.044750e-02 +4.312500e+00 0.000000e+00 0.000000e+00 2.000000e-02 4.011234e-02 4.011234e-02 +4.337500e+00 0.000000e+00 0.000000e+00 6.000000e-02 3.132092e-02 3.132092e-02 +4.362500e+00 0.000000e+00 0.000000e+00 0.000000e+00 4.000000e-02 4.000000e-02 +4.387500e+00 0.000000e+00 0.000000e+00 2.000000e-02 4.011234e-02 4.011234e-02 +4.412500e+00 0.000000e+00 0.000000e+00 5.000000e-02 4.069705e-02 4.069705e-02 +4.437500e+00 0.000000e+00 0.000000e+00 5.000000e-02 3.092329e-02 3.092329e-02 +4.462500e+00 0.000000e+00 0.000000e+00 5.000000e-02 3.092329e-02 3.092329e-02 +4.487500e+00 0.000000e+00 0.000000e+00 6.000000e-02 4.100000e-02 4.100000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_I676691/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0, up: 0.0}}, 1: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.005, up: 0.005}}, 2: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0125, up: 0.0125}}, 3: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.02, up: 0.02}}, 4: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.0175, up: 0.0175}}, 5: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.02, up: 0.02}}, 6: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.0175, up: 0.0175}}, 7: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.02, up: 0.02}}, 8: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.0125, up: 0.0125}}, 9: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.0175, up: 0.0175}}, 10: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.025, up: 0.025}}, 11: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.0325, up: 0.0325}}, 12: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.02, up: 0.02}}, 13: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.025, up: 0.025}}, 14: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.0175, up: 0.0175}}, 15: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.02, up: 0.02}}, 16: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.015, up: 0.015}}, 17: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.0475, up: 0.0475}}, 18: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.0075, up: 0.0075}}, 19: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0125, up: 0.0125}}, 20: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0075, up: 0.0075}}, 21: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.01, up: 0.01}}, 22: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.0125, up: 0.0125}}, 23: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0075, up: 0.0075}}, 24: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0125, up: 0.0125}}, 25: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.005, up: 0.005}}, 26: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.005, up: 0.005}}, 27: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0, up: 0.0}}, 28: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0125, up: 0.0125}}, 29: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0075, up: 0.0075}}, 30: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0025, up: 0.0025}}, 31: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0025, up: 0.0025}}, 32: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0075, up: 0.0075}}, 33: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0025, up: 0.0025}}, 34: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.005, up: 0.005}}, 35: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.01, up: 0.01}}, 36: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0, up: 0.0}}, 37: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0025, up: 0.0025}}, 38: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0, up: 0.0}}, 39: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0, up: 0.0}}} + +IsRef: 1 +Path: /REF/BABAR_2005_I676691/d03-x01-y01 +Title: doi:10.17182/hepdata.22111.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.031200e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +2.093800e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.118034e-02 1.118034e-02 +2.156200e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.600781e-02 1.600781e-02 +2.218800e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.828427e-02 2.828427e-02 +2.281200e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.657536e-02 2.657536e-02 +2.343800e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.828427e-02 2.828427e-02 +2.406200e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.657536e-02 2.657536e-02 +2.468800e+00 0.000000e+00 0.000000e+00 8.000000e-02 3.605551e-02 3.605551e-02 +2.531200e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.358495e-02 2.358495e-02 +2.593800e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.657536e-02 2.657536e-02 +2.656200e+00 0.000000e+00 0.000000e+00 1.000000e-01 3.905125e-02 3.905125e-02 +2.718800e+00 0.000000e+00 0.000000e+00 1.300000e-01 4.422952e-02 4.422952e-02 +2.781200e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.828427e-02 2.828427e-02 +2.843800e+00 0.000000e+00 0.000000e+00 1.000000e-01 3.201562e-02 3.201562e-02 +2.906200e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.657536e-02 2.657536e-02 +2.968800e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.828427e-02 2.828427e-02 +3.031200e+00 0.000000e+00 0.000000e+00 6.000000e-02 2.500000e-02 2.500000e-02 +3.093800e+00 0.000000e+00 0.000000e+00 1.900000e-01 5.618051e-02 5.618051e-02 +3.156200e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.136001e-02 2.136001e-02 +3.218800e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.600781e-02 1.600781e-02 +3.281200e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.250000e-02 1.250000e-02 +3.343800e+00 0.000000e+00 0.000000e+00 4.000000e-02 2.236068e-02 2.236068e-02 +3.406200e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.358495e-02 2.358495e-02 +3.468800e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.250000e-02 1.250000e-02 +3.531200e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.600781e-02 1.600781e-02 +3.593800e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.118034e-02 1.118034e-02 +3.656200e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.118034e-02 1.118034e-02 +3.718800e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +3.781200e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.600781e-02 1.600781e-02 +3.843800e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.250000e-02 1.250000e-02 +3.906200e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.030776e-02 1.030776e-02 +3.968800e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.030776e-02 1.030776e-02 +4.031200e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.250000e-02 1.250000e-02 +4.093800e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.030776e-02 1.030776e-02 +4.156200e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.118034e-02 1.118034e-02 +4.218800e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.414214e-02 1.414214e-02 +4.281200e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +4.343800e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.030776e-02 1.030776e-02 +4.406200e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +4.468800e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2005_S6181155.cc b/analyses/pluginBABAR/BABAR_2005_S6181155.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2005_S6181155.cc @@ -0,0 +1,128 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/Beam.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief BABAR Xi_c baryons from fragmentation + /// @author Peter Richardson + class BABAR_2005_S6181155 : public Analysis { + public: + + BABAR_2005_S6181155() + : Analysis("BABAR_2005_S6181155") + { } + + void init() { + declare(Beam(), "Beams"); + declare(UnstableParticles(), "UFS"); + _histOnResonanceA = bookHisto1D(1,1,1); + _histOnResonanceB = bookHisto1D(2,1,1); + _histOffResonance = bookHisto1D(2,1,2); + _sigma = bookHisto1D(3,1,1); + } + + void analyze(const Event& e) { + const double weight = e.weight(); + + // Loop through unstable FS particles and look for charmed mesons/baryons + const UnstableParticles& ufs = apply(e, "UFS"); + + const Beam beamproj = apply(e, "Beams"); + const ParticlePair& beams = beamproj.beams(); + const FourMomentum mom_tot = beams.first.momentum() + beams.second.momentum(); + const LorentzTransform cms_boost = LorentzTransform::mkFrameTransformFromBeta(mom_tot.betaVec()); + const double s = sqr(beamproj.sqrtS()); + + const bool onresonance = fuzzyEquals(beamproj.sqrtS()/GeV, 10.58, 2E-3); + + foreach (const Particle& p, ufs.particles()) { + // 3-momentum in CMS frame + + const double mom = cms_boost.transform(p.momentum()).vector3().mod(); + // Only looking at Xi_c^0 + if (p.abspid() != 4132 ) continue; + MSG_DEBUG("mom = " << mom); + // off-resonance cross section + if (checkDecay(p.genParticle())) { + if (onresonance) { + _histOnResonanceA->fill(mom,weight); + _histOnResonanceB->fill(mom,weight); + } + else { + _histOffResonance->fill(mom,s/sqr(10.58)*weight); + _sigma->fill(10.58,weight); + } + } + } + } + + + void finalize() { + scale(_histOnResonanceA, crossSection()/femtobarn/sumOfWeights()*0.2); + scale(_histOnResonanceB, crossSection()/femtobarn/sumOfWeights()*0.45); + scale(_histOffResonance, crossSection()/femtobarn/sumOfWeights()*0.45); + scale(_sigma , crossSection()/femtobarn/sumOfWeights()); + } + + + private: + + //@{ + /// Histograms + Histo1DPtr _histOnResonanceA; + Histo1DPtr _histOnResonanceB; + Histo1DPtr _histOffResonance; + Histo1DPtr _sigma ; + //@} + + bool checkDecay(ConstGenParticlePtr p) { + unsigned int nstable = 0, npip = 0, npim = 0; + unsigned int nXim = 0, nXip = 0; + findDecayProducts(p, nstable, npip, npim, nXip, nXim); + int id = p->pdg_id(); + // Xi_c + if (id == 4132) { + if (nstable == 2 && nXim == 1 && npip == 1) return true; + } + else if (id == -4132) { + if (nstable == 2 && nXip == 1 && npim == 1) return true; + } + return false; + } + + void findDecayProducts(ConstGenParticlePtr p, + unsigned int& nstable, + unsigned int& npip, unsigned int& npim, + unsigned int& nXip, unsigned int& nXim) { + ConstGenVertexPtr dv = p->end_vertex(); + /// @todo Use better looping + for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ + int id = pp->pdg_id(); + if (id==3312) { + ++nXim; + ++nstable; + } else if (id == -3312) { + ++nXip; + ++nstable; + } else if(id == 111 || id == 221) { + ++nstable; + } else if (pp->end_vertex()) { + findDecayProducts(pp, nstable, npip, npim, nXip, nXim); + } else { + if (id != 22) ++nstable; + if (id == 211) ++npip; + else if(id == -211) ++npim; + } + } + } + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2005_S6181155); + +} diff --git a/analyses/pluginMisc/BABAR_2005_S6181155.info b/analyses/pluginBABAR/BABAR_2005_S6181155.info rename from analyses/pluginMisc/BABAR_2005_S6181155.info rename to analyses/pluginBABAR/BABAR_2005_S6181155.info diff --git a/analyses/pluginBABAR/BABAR_2005_S6181155.plot b/analyses/pluginBABAR/BABAR_2005_S6181155.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2005_S6181155.plot @@ -0,0 +1,24 @@ +# BEGIN PLOT /BABAR_2005_S6181155/d01-x01-y01 +Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ with $\Xi_c^0\to\Xi^-\pi^+$ at the $\Upsilon(4S)$ +XLabel=$p_{\Xi_c^0}$ [GeV] +YLabel=$\sigma$ [fb] +LogY=0 +# END PLOT +# BEGIN PLOT /BABAR_2005_S6181155/d02-x01-y01 +Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ with $\Xi_c^0\to\Xi^-\pi^+$ at the $\Upsilon(4S)$ +XLabel=$p_{\Xi_c^0}$ [GeV] +YLabel=$\sigma$ [fb] +LogY=0 +# END PLOT +# BEGIN PLOT /BABAR_2005_S6181155/d02-x01-y02 +Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ with $\Xi_c^0\to\Xi^-\pi^+$ in the continuum region +XLabel=$p_{\Xi_c^0}$ [GeV] +YLabel=$\sigma$ [fb] +LogY=0 +# END PLOT +# BEGIN PLOT /BABAR_2005_S6181155/d03-x01-y01 +Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ with $\Xi_c^0\to\Xi^-\pi^+$ +XLabel=$\sqrt{s}$ [GeV] +YLabel=$\sigma$ [fb] +LogY=0 +# END PLOT diff --git a/analyses/pluginBABAR/BABAR_2005_S6181155.yoda b/analyses/pluginBABAR/BABAR_2005_S6181155.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2005_S6181155.yoda @@ -0,0 +1,88 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -2.0, up: 2.0}, sys: {dn: -1.0, up: 1.0}}, 1: {stat: {dn: -4.0, up: 4.0}, sys: {dn: -5.0, up: 5.0}}, 2: {stat: {dn: -6.0, up: 6.0}, sys: {dn: -8.0, up: 8.0}}, 3: {stat: {dn: -6.0, up: 6.0}, sys: {dn: -8.0, up: 8.0}}, 4: {stat: {dn: -6.0, up: 6.0}, sys: {dn: -7.0, up: 7.0}}, 5: {stat: {dn: -5.0, up: 5.0}, sys: {dn: -5.0, up: 5.0}}, 6: {stat: {dn: -5.0, up: 5.0}, sys: {dn: -2.0, up: 2.0}}, 7: {stat: {dn: -4.0, up: 4.0}, sys: {dn: -2.0, up: 2.0}}, 8: {stat: {dn: -4.0, up: 4.0}, sys: {dn: -2.0, up: 2.0}}, 9: {stat: {dn: -3.0, up: 3.0}, sys: {dn: -2.0, up: 2.0}}, 10: {stat: {dn: -3.0, up: 3.0}, sys: {dn: -2.0, up: 2.0}}, 11: {stat: {dn: -3.0, up: 3.0}, sys: {dn: -2.0, up: 2.0}}, 12: {stat: {dn: -3.0, up: 3.0}, sys: {dn: -3.0, up: 3.0}}, 13: {stat: {dn: -3.0, up: 3.0}, sys: {dn: -3.0, up: 3.0}}, 14: {stat: {dn: -3.0, up: 3.0}, sys: {dn: -3.0, up: 3.0}}, 15: {stat: {dn: -2.0, up: 2.0}, sys: {dn: -4.0, up: 4.0}}, 16: {stat: {dn: -2.0, up: 2.0}, sys: {dn: -3.0, up: 3.0}}, 17: {stat: {dn: -2.0, up: 2.0}, sys: {dn: -3.0, up: 3.0}}, 18: {stat: {dn: -2.0, up: 2.0}, sys: {dn: -2.0, up: 2.0}}, 19: {stat: {dn: -1.0, up: 1.0}, sys: {dn: -2.0, up: 2.0}}, 20: {stat: {dn: -1.0, up: 1.0}, sys: {dn: -2.0, up: 2.0}}, 21: {stat: {dn: -0.5, up: 0.5}, sys: {dn: -0.3, up: 0.3}}, 22: {stat: {dn: -0.3, up: 0.3}, sys: {dn: -0.2, up: 0.2}}, 23: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.1, up: 0.1}}, 24: {stat: {dn: -0.2, up: 0.2}, sys: {dn: -0.1, up: 0.1}}} + +IsRef: 1 +Path: /REF/BABAR_2005_S6181155/d01-x01-y01 +Title: doi:10.17182/hepdata.27164.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000000e-01 1.000000e-01 1.000000e-01 1.000000e+01 2.236068e+00 2.236068e+00 +3.000000e-01 1.000000e-01 1.000000e-01 5.600000e+01 6.403124e+00 6.403124e+00 +5.000000e-01 1.000000e-01 1.000000e-01 1.010000e+02 1.000000e+01 1.000000e+01 +7.000000e-01 1.000000e-01 1.000000e-01 1.020000e+02 1.000000e+01 1.000000e+01 +9.000000e-01 1.000000e-01 1.000000e-01 8.400000e+01 9.219544e+00 9.219544e+00 +1.100000e+00 1.000000e-01 1.000000e-01 6.500000e+01 7.071068e+00 7.071068e+00 +1.300000e+00 1.000000e-01 1.000000e-01 2.800000e+01 5.385165e+00 5.385165e+00 +1.500000e+00 1.000000e-01 1.000000e-01 2.300000e+01 4.472136e+00 4.472136e+00 +1.700000e+00 1.000000e-01 1.000000e-01 2.100000e+01 4.472136e+00 4.472136e+00 +1.900000e+00 1.000000e-01 1.000000e-01 2.000000e+01 3.605551e+00 3.605551e+00 +2.100000e+00 1.000000e-01 1.000000e-01 2.300000e+01 3.605551e+00 3.605551e+00 +2.300000e+00 1.000000e-01 1.000000e-01 2.600000e+01 3.605551e+00 3.605551e+00 +2.500000e+00 1.000000e-01 1.000000e-01 3.400000e+01 4.242641e+00 4.242641e+00 +2.700000e+00 1.000000e-01 1.000000e-01 3.700000e+01 4.242641e+00 4.242641e+00 +2.900000e+00 1.000000e-01 1.000000e-01 4.400000e+01 4.242641e+00 4.242641e+00 +3.100000e+00 1.000000e-01 1.000000e-01 4.600000e+01 4.472136e+00 4.472136e+00 +3.300000e+00 1.000000e-01 1.000000e-01 4.200000e+01 3.605551e+00 3.605551e+00 +3.500000e+00 1.000000e-01 1.000000e-01 3.900000e+01 3.605551e+00 3.605551e+00 +3.700000e+00 1.000000e-01 1.000000e-01 2.200000e+01 2.828427e+00 2.828427e+00 +3.900000e+00 1.000000e-01 1.000000e-01 2.000000e+01 2.236068e+00 2.236068e+00 +4.100000e+00 1.000000e-01 1.000000e-01 1.100000e+01 2.236068e+00 2.236068e+00 +4.300000e+00 1.000000e-01 1.000000e-01 2.200000e+00 5.830952e-01 5.830952e-01 +4.500000e+00 1.000000e-01 1.000000e-01 8.000000e-01 3.605551e-01 3.605551e-01 +4.700000e+00 1.000000e-01 1.000000e-01 0.000000e+00 1.414214e-01 1.414214e-01 +4.900000e+00 1.000000e-01 1.000000e-01 2.000000e-01 2.236068e-01 2.236068e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -5.0, up: 5.0}, sys: {dn: -7.0, up: 7.0}}, 1: {stat: {dn: -9.0, up: 9.0}, sys: {dn: -17.0, up: 17.0}}, 2: {stat: {dn: -8.0, up: 8.0}, sys: {dn: -10.0, up: 10.0}}, 3: {stat: {dn: -6.0, up: 6.0}, sys: {dn: -4.0, up: 4.0}}, 4: {stat: {dn: -4.0, up: 4.0}, sys: {dn: -3.0, up: 3.0}}, 5: {stat: {dn: -5.0, up: 5.0}, sys: {dn: -6.0, up: 6.0}}, 6: {stat: {dn: -4.0, up: 4.0}, sys: {dn: -10.0, up: 10.0}}, 7: {stat: {dn: -3.0, up: 3.0}, sys: {dn: -8.0, up: 8.0}}, 8: {stat: {dn: -1.0, up: 1.0}, sys: {dn: -1.0, up: 1.0}}} + +IsRef: 1 +Path: /REF/BABAR_2005_S6181155/d02-x01-y01 +Title: doi:10.17182/hepdata.27164.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.250000e-01 2.250000e-01 2.250000e-01 8.800000e+01 8.602325e+00 8.602325e+00 +6.750000e-01 2.250000e-01 2.250000e-01 2.180000e+02 1.923538e+01 1.923538e+01 +1.125000e+00 2.250000e-01 2.250000e-01 1.280000e+02 1.280625e+01 1.280625e+01 +1.575000e+00 2.250000e-01 2.250000e-01 5.100000e+01 7.211103e+00 7.211103e+00 +1.975000e+00 1.750000e-01 1.750000e-01 3.700000e+01 5.000000e+00 5.000000e+00 +2.425000e+00 2.750000e-01 2.750000e-01 8.300000e+01 7.810250e+00 7.810250e+00 +3.000000e+00 3.000000e-01 3.000000e-01 1.330000e+02 1.077033e+01 1.077033e+01 +3.650000e+00 3.500000e-01 3.500000e-01 9.900000e+01 8.544004e+00 8.544004e+00 +4.350000e+00 3.500000e-01 3.500000e-01 1.400000e+01 1.414214e+00 1.414214e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d02-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -12.0, up: 12.0}, sys: {dn: -1.0, up: 1.0}}, 1: {stat: {dn: -21.0, up: 21.0}, sys: {dn: -2.0, up: 2.0}}, 2: {stat: {dn: -20.0, up: 20.0}, sys: {dn: -2.0, up: 2.0}}, 3: {stat: {dn: -18.0, up: 18.0}, sys: {dn: -2.0, up: 2.0}}, 4: {stat: {dn: -13.0, up: 13.0}, sys: {dn: -2.0, up: 2.0}}, 5: {stat: {dn: -16.0, up: 16.0}, sys: {dn: -7.0, up: 7.0}}, 6: {stat: {dn: -15.0, up: 15.0}, sys: {dn: -13.0, up: 13.0}}, 7: {stat: {dn: -10.0, up: 10.0}, sys: {dn: -7.0, up: 7.0}}, 8: {stat: {dn: -4.0, up: 4.0}, sys: {dn: -2.0, up: 2.0}}} + +IsRef: 1 +Path: /REF/BABAR_2005_S6181155/d02-x01-y02 +Title: doi:10.17182/hepdata.27164.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.250000e-01 2.250000e-01 2.250000e-01 1.000000e+01 1.204159e+01 1.204159e+01 +6.750000e-01 2.250000e-01 2.250000e-01 1.600000e+01 2.109502e+01 2.109502e+01 +1.125000e+00 2.250000e-01 2.250000e-01 -7.000000e+00 2.009975e+01 2.009975e+01 +1.575000e+00 2.250000e-01 2.250000e-01 1.600000e+01 1.811077e+01 1.811077e+01 +1.975000e+00 1.750000e-01 1.750000e-01 2.300000e+01 1.315295e+01 1.315295e+01 +2.425000e+00 2.750000e-01 2.750000e-01 9.100000e+01 1.746425e+01 1.746425e+01 +3.000000e+00 3.000000e-01 3.000000e-01 1.680000e+02 1.984943e+01 1.984943e+01 +3.650000e+00 3.500000e-01 3.500000e-01 8.900000e+01 1.220656e+01 1.220656e+01 +4.350000e+00 3.500000e-01 3.500000e-01 1.700000e+01 4.472136e+00 4.472136e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -39.0, up: 39.0}, sys: {dn: -41.0, up: 41.0}}} + +IsRef: 1 +Path: /REF/BABAR_2005_S6181155/d03-x01-y01 +Title: doi:10.17182/hepdata.27164.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 5.000000e-01 5.000000e-01 3.880000e+02 5.658622e+01 5.658622e+01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2006_I700020.cc b/analyses/pluginBABAR/BABAR_2006_I700020.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I700020.cc @@ -0,0 +1,83 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2006_I700020 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2006_I700020); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nproton = bookCounter("TMP/proton"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PROTON) vetoEvent; + } + _nproton->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _nproton->val(); + double error = _nproton->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nproton; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2006_I700020); + + +} diff --git a/analyses/pluginBABAR/BABAR_2006_I700020.info b/analyses/pluginBABAR/BABAR_2006_I700020.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I700020.info @@ -0,0 +1,34 @@ +Name: BABAR_2006_I700020 +Year: 2006 +Summary: Cross section for $e^+e^-\to$ proton and antiproton between threshold and 4.4 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 700020 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ using radiative + return for energies between threshold and 4.4 GeV.' +BibKey: Aubert:2005cb +BibTeX: '@article{Aubert:2005cb, + author = "Aubert, Bernard and others", + title = "{A Study of $e^{+} e^{-} \to p \bar{p}$ using initial + state radiation with BABAR}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D73", + year = "2006", + pages = "012005", + doi = "10.1103/PhysRevD.73.012005", + eprint = "hep-ex/0512023", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-11587, BABAR-PUB-05-050", + SLACcitation = "%%CITATION = HEP-EX/0512023;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2006_I700020.plot b/analyses/pluginBABAR/BABAR_2006_I700020.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I700020.plot @@ -0,0 +1,12 @@ +BEGIN PLOT /BABAR_2006_I700020/d01-x01-y01 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/pb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2006_I700020/d02-x01-y01 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2006_I700020.yoda b/analyses/pluginBABAR/BABAR_2006_I700020.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I700020.yoda @@ -0,0 +1,146 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I700020/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -68.0, up: 68.0}, sys: {dn: -43.0, up: 43.0}}, 1: {stat: {dn: -71.0, up: 71.0}, sys: {dn: -46.0, up: 46.0}}, 2: {stat: {dn: -68.0, up: 68.0}, sys: {dn: -43.0, up: 43.0}}, 3: {stat: {dn: -68.0, up: 68.0}, sys: {dn: -41.0, up: 41.0}}, 4: {stat: {dn: -68.0, up: 68.0}, sys: {dn: -44.0, up: 44.0}}, 5: {stat: {dn: -71.0, up: 71.0}, sys: {dn: -48.0, up: 48.0}}, 6: {stat: {dn: -68.0, up: 68.0}, sys: {dn: -45.0, up: 45.0}}, 7: {stat: {dn: -68.0, up: 68.0}, sys: {dn: -46.0, up: 46.0}}, 8: {stat: {dn: -66.0, up: 66.0}, sys: {dn: -40.0, up: 40.0}}, 9: {stat: {dn: -68.0, up: 68.0}, sys: {dn: -44.0, up: 44.0}}, 10: {stat: {dn: -66.0, up: 66.0}, sys: {dn: -40.0, up: 40.0}}, 11: {stat: {dn: -58.0, up: 58.0}, sys: {dn: -34.0, up: 34.0}}, 12: {stat: {dn: -56.0, up: 56.0}, sys: {dn: -31.0, up: 31.0}}, 13: {stat: {dn: -52.0, up: 52.0}, sys: {dn: -29.0, up: 29.0}}, 14: {stat: {dn: -47.0, up: 47.0}, sys: {dn: -21.0, up: 21.0}}, 15: {stat: {dn: -40.0, up: 40.0}, sys: {dn: -16.0, up: 16.0}}, 16: {stat: {dn: -39.0, up: 39.0}, sys: {dn: -20.0, up: 20.0}}, 17: {stat: {dn: -21.0, up: 21.0}, sys: {dn: -16.0, up: 16.0}}, 18: {stat: {dn: -19.0, up: 19.0}, sys: {dn: -13.0, up: 13.0}}, 19: {stat: {dn: -18.0, up: 18.0}, sys: {dn: -7.0, up: 7.0}}, 20: {stat: {dn: -15.0, up: 15.0}, sys: {dn: -5.0, up: 5.0}}, 21: {stat: {dn: -16.0, up: 16.0}, sys: {dn: -6.0, up: 6.0}}, 22: {stat: {dn: -13.0, up: 13.0}, sys: {dn: -4.0, up: 4.0}}, 23: {stat: {dn: -11.0, up: 11.0}, sys: {dn: -4.0, up: 4.0}}, 24: {stat: {dn: -10.0, up: 10.0}, sys: {dn: -4.0, up: 4.0}}, 25: {stat: {dn: -10.0, up: 10.0}, sys: {dn: -4.0, up: 4.0}}, 26: {stat: {dn: -10.0, up: 10.0}, sys: {dn: -4.0, up: 4.0}}, 27: {stat: {dn: -9.0, up: 9.0}, sys: {dn: -3.0, up: 3.0}}, 28: {stat: {dn: -9.0, up: 9.0}, sys: {dn: -3.0, up: 3.0}}, 29: {stat: {dn: -8.0, up: 8.0}, sys: {dn: -3.0, up: 3.0}}, 30: {stat: {dn: -7.0, up: 7.0}, sys: {dn: -3.0, up: 3.0}}, 31: {stat: {dn: -3.0, up: 3.0}, sys: {dn: -2.8, up: 2.8}}, 32: {stat: {dn: -1.6, up: 1.6}, sys: {dn: -2.0, up: 2.0}}, 33: {stat: {dn: -1.0, up: 1.0}, sys: {dn: -0.9, up: 0.9}}, 34: {stat: {dn: -1.1, up: 1.1}, sys: {dn: -0.8, up: 0.8}}, 35: {stat: {dn: -0.8, up: 0.8}, sys: {dn: -0.7, up: 0.7}}, 36: {stat: {dn: -0.5, up: 0.5}, sys: {dn: -0.5, up: 0.5}}, 37: {stat: {dn: -0.4, up: 0.4}, sys: {dn: -0.5, up: 0.5}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I700020/d01-x01-y01 +Title: doi:10.17182/hepdata.41831.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.888500e+00 1.150000e-02 1.150000e-02 8.020000e+02 8.045496e+01 8.045496e+01 +1.912500e+00 1.250000e-02 1.250000e-02 8.870000e+02 8.459905e+01 8.459905e+01 +1.937500e+00 1.250000e-02 1.250000e-02 8.190000e+02 8.045496e+01 8.045496e+01 +1.962500e+00 1.250000e-02 1.250000e-02 7.600000e+02 7.940403e+01 7.940403e+01 +1.987500e+00 1.250000e-02 1.250000e-02 7.650000e+02 8.099383e+01 8.099383e+01 +2.012500e+00 1.250000e-02 1.250000e-02 8.540000e+02 8.570298e+01 8.570298e+01 +2.037500e+00 1.250000e-02 1.250000e-02 7.480000e+02 8.154140e+01 8.154140e+01 +2.062500e+00 1.250000e-02 1.250000e-02 7.940000e+02 8.209750e+01 8.209750e+01 +2.087500e+00 1.250000e-02 1.250000e-02 7.150000e+02 7.717513e+01 7.717513e+01 +2.112500e+00 1.250000e-02 1.250000e-02 7.940000e+02 8.099383e+01 8.099383e+01 +2.137500e+00 1.250000e-02 1.250000e-02 7.210000e+02 7.717513e+01 7.717513e+01 +2.162500e+00 1.250000e-02 1.250000e-02 5.540000e+02 6.723095e+01 6.723095e+01 +2.187500e+00 1.250000e-02 1.250000e-02 4.770000e+02 6.400781e+01 6.400781e+01 +2.212500e+00 1.250000e-02 1.250000e-02 4.350000e+02 5.953990e+01 5.953990e+01 +2.237500e+00 1.250000e-02 1.250000e-02 3.920000e+02 5.147815e+01 5.147815e+01 +2.262500e+00 1.250000e-02 1.250000e-02 2.450000e+02 4.308132e+01 4.308132e+01 +2.287500e+00 1.250000e-02 1.250000e-02 2.440000e+02 4.382921e+01 4.382921e+01 +2.325000e+00 2.500000e-02 2.500000e-02 1.400000e+02 2.640076e+01 2.640076e+01 +2.375000e+00 2.500000e-02 2.500000e-02 1.330000e+02 2.302173e+01 2.302173e+01 +2.425000e+00 2.500000e-02 2.500000e-02 1.490000e+02 1.931321e+01 1.931321e+01 +2.475000e+00 2.500000e-02 2.500000e-02 8.300000e+01 1.581139e+01 1.581139e+01 +2.525000e+00 2.500000e-02 2.500000e-02 1.000000e+02 1.708801e+01 1.708801e+01 +2.575000e+00 2.500000e-02 2.500000e-02 6.000000e+01 1.360147e+01 1.360147e+01 +2.625000e+00 2.500000e-02 2.500000e-02 4.700000e+01 1.170470e+01 1.170470e+01 +2.675000e+00 2.500000e-02 2.500000e-02 3.700000e+01 1.077033e+01 1.077033e+01 +2.725000e+00 2.500000e-02 2.500000e-02 3.100000e+01 1.077033e+01 1.077033e+01 +2.775000e+00 2.500000e-02 2.500000e-02 3.700000e+01 1.077033e+01 1.077033e+01 +2.825000e+00 2.500000e-02 2.500000e-02 3.000000e+01 9.486833e+00 9.486833e+00 +2.875000e+00 2.500000e-02 2.500000e-02 2.700000e+01 9.486833e+00 9.486833e+00 +2.925000e+00 2.500000e-02 2.500000e-02 2.600000e+01 8.544004e+00 8.544004e+00 +2.975000e+00 2.500000e-02 2.500000e-02 1.200000e+01 7.615773e+00 7.615773e+00 +3.100000e+00 1.000000e-01 1.000000e-01 3.600000e+00 4.103657e+00 4.103657e+00 +3.300000e+00 1.000000e-01 1.000000e-01 2.300000e+00 2.561250e+00 2.561250e+00 +3.500000e+00 1.000000e-01 1.000000e-01 1.700000e+00 1.345362e+00 1.345362e+00 +3.700000e+00 1.000000e-01 1.000000e-01 2.200000e+00 1.360147e+00 1.360147e+00 +3.900000e+00 1.000000e-01 1.000000e-01 1.200000e+00 1.063015e+00 1.063015e+00 +4.125000e+00 1.250000e-01 1.250000e-01 7.000000e-01 7.071068e-01 7.071068e-01 +4.375000e+00 1.250000e-01 1.250000e-01 1.000000e-01 6.403124e-01 6.403124e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I700020/d01-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.025, up: 0.023}}, 1: {error: {dn: -0.017, up: 0.017}}, 2: {error: {dn: -0.015, up: 0.015}}, 3: {error: {dn: -0.015, up: 0.014}}, 4: {error: {dn: -0.015, up: 0.014}}, 5: {error: {dn: -0.014, up: 0.013}}, 6: {error: {dn: -0.014, up: 0.013}}, 7: {error: {dn: -0.014, up: 0.013}}, 8: {error: {dn: -0.013, up: 0.013}}, 9: {error: {dn: -0.013, up: 0.012}}, 10: {error: {dn: -0.013, up: 0.012}}, 11: {error: {dn: -0.013, up: 0.012}}, 12: {error: {dn: -0.013, up: 0.012}}, 13: {error: {dn: -0.013, up: 0.012}}, 14: {error: {dn: -0.012, up: 0.011}}, 15: {error: {dn: -0.013, up: 0.012}}, 16: {error: {dn: -0.013, up: 0.012}}, 17: {error: {dn: -0.01, up: 0.009}}, 18: {error: {dn: -0.009, up: 0.008}}, 19: {error: {dn: -0.008, up: 0.007}}, 20: {error: {dn: -0.008, up: 0.008}}, 21: {error: {dn: -0.008, up: 0.007}}, 22: {error: {dn: -0.008, up: 0.007}}, 23: {error: {dn: -0.009, up: 0.008}}, 24: {error: {dn: -0.009, up: 0.008}}, 25: {error: {dn: -0.01, up: 0.008}}, 26: {error: {dn: -0.01, up: 0.008}}, 27: {error: {dn: -0.009, up: 0.008}}, 28: {error: {dn: -0.01, up: 0.008}}, 29: {error: {dn: -0.009, up: 0.008}}, 30: {error: {dn: -0.014, up: 0.01}}, 31: {error: {dn: -0.021, up: 0.009}}, 32: {error: {dn: -0.017, up: 0.008}}, 33: {error: {dn: -0.009, up: 0.005}}, 34: {error: {dn: -0.008, up: 0.005}}, 35: {error: {dn: -0.009, up: 0.005}}, 36: {error: {dn: -0.01, up: 0.005}}, 37: {error: {dn: -0.005, up: 0.008}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I700020/d01-x01-y02 +Title: doi:10.17182/hepdata.41831.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.888500e+00 1.150000e-02 1.150000e-02 4.530000e-01 2.500000e-02 2.300000e-02 +1.912500e+00 1.250000e-02 1.250000e-02 3.540000e-01 1.700000e-02 1.700000e-02 +1.937500e+00 1.250000e-02 1.250000e-02 3.050000e-01 1.500000e-02 1.500000e-02 +1.962500e+00 1.250000e-02 1.250000e-02 2.760000e-01 1.500000e-02 1.400000e-02 +1.987500e+00 1.250000e-02 1.250000e-02 2.660000e-01 1.500000e-02 1.400000e-02 +2.012500e+00 1.250000e-02 1.250000e-02 2.730000e-01 1.400000e-02 1.300000e-02 +2.037500e+00 1.250000e-02 1.250000e-02 2.500000e-01 1.400000e-02 1.300000e-02 +2.062500e+00 1.250000e-02 1.250000e-02 2.540000e-01 1.400000e-02 1.300000e-02 +2.087500e+00 1.250000e-02 1.250000e-02 2.390000e-01 1.300000e-02 1.300000e-02 +2.112500e+00 1.250000e-02 1.250000e-02 2.500000e-01 1.300000e-02 1.200000e-02 +2.137500e+00 1.250000e-02 1.250000e-02 2.370000e-01 1.300000e-02 1.200000e-02 +2.162500e+00 1.250000e-02 1.250000e-02 2.070000e-01 1.300000e-02 1.200000e-02 +2.187500e+00 1.250000e-02 1.250000e-02 1.910000e-01 1.300000e-02 1.200000e-02 +2.212500e+00 1.250000e-02 1.250000e-02 1.830000e-01 1.300000e-02 1.200000e-02 +2.237500e+00 1.250000e-02 1.250000e-02 1.740000e-01 1.200000e-02 1.100000e-02 +2.262500e+00 1.250000e-02 1.250000e-02 1.370000e-01 1.300000e-02 1.200000e-02 +2.287500e+00 1.250000e-02 1.250000e-02 1.370000e-01 1.300000e-02 1.200000e-02 +2.325000e+00 2.500000e-02 2.500000e-02 1.050000e-01 1.000000e-02 9.000000e-03 +2.375000e+00 2.500000e-02 2.500000e-02 1.030000e-01 9.000000e-03 8.000000e-03 +2.425000e+00 2.500000e-02 2.500000e-02 1.100000e-01 8.000000e-03 7.000000e-03 +2.475000e+00 2.500000e-02 2.500000e-02 8.300000e-02 8.000000e-03 8.000000e-03 +2.525000e+00 2.500000e-02 2.500000e-02 9.200000e-02 8.000000e-03 7.000000e-03 +2.575000e+00 2.500000e-02 2.500000e-02 7.200000e-02 8.000000e-03 7.000000e-03 +2.625000e+00 2.500000e-02 2.500000e-02 6.500000e-02 9.000000e-03 8.000000e-03 +2.675000e+00 2.500000e-02 2.500000e-02 5.900000e-02 9.000000e-03 8.000000e-03 +2.725000e+00 2.500000e-02 2.500000e-02 5.400000e-02 1.000000e-02 8.000000e-03 +2.775000e+00 2.500000e-02 2.500000e-02 6.000000e-02 1.000000e-02 8.000000e-03 +2.825000e+00 2.500000e-02 2.500000e-02 5.400000e-02 9.000000e-03 8.000000e-03 +2.875000e+00 2.500000e-02 2.500000e-02 5.200000e-02 1.000000e-02 8.000000e-03 +2.925000e+00 2.500000e-02 2.500000e-02 5.200000e-02 9.000000e-03 8.000000e-03 +2.975000e+00 2.500000e-02 2.500000e-02 3.500000e-02 1.400000e-02 1.000000e-02 +3.100000e+00 1.000000e-01 1.000000e-01 2.100000e-02 2.100000e-02 9.000000e-03 +3.300000e+00 1.000000e-01 1.000000e-01 1.700000e-02 1.700000e-02 8.000000e-03 +3.500000e+00 1.000000e-01 1.000000e-01 1.600000e-02 9.000000e-03 5.000000e-03 +3.700000e+00 1.000000e-01 1.000000e-01 1.900000e-02 8.000000e-03 5.000000e-03 +3.900000e+00 1.000000e-01 1.000000e-01 1.500000e-02 9.000000e-03 5.000000e-03 +4.125000e+00 1.250000e-01 1.250000e-01 1.100000e-02 1.000000e-02 5.000000e-03 +4.375000e+00 1.250000e-01 1.250000e-01 5.000000e-03 5.000000e-03 8.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I700020/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -161.0, up: 161.0}, sys: {dn: -40.0, up: 40.0}}, 1: {stat: {dn: -155.0, up: 155.0}, sys: {dn: -43.0, up: 43.0}}, 2: {stat: {dn: -154.0, up: 154.0}, sys: {dn: -36.0, up: 36.0}}, 3: {stat: {dn: -174.0, up: 174.0}, sys: {dn: -48.0, up: 48.0}}, 4: {stat: {dn: -182.0, up: 182.0}, sys: {dn: -48.0, up: 48.0}}, 5: {stat: {dn: -207.0, up: 207.0}, sys: {dn: -56.0, up: 56.0}}, 6: {stat: {dn: -186.0, up: 186.0}, sys: {dn: -41.0, up: 41.0}}, 7: {stat: {dn: -210.0, up: 210.0}, sys: {dn: -60.0, up: 60.0}}, 8: {stat: {dn: -116.0, up: 116.0}, sys: {dn: -43.0, up: 43.0}}, 9: {stat: {dn: -102.0, up: 102.0}, sys: {dn: -44.0, up: 44.0}}, 10: {stat: {dn: -104.0, up: 104.0}, sys: {dn: -43.0, up: 43.0}}, 11: {stat: {dn: -105.0, up: 105.0}, sys: {dn: -42.0, up: 42.0}}, 12: {stat: {dn: -105.0, up: 105.0}, sys: {dn: -43.0, up: 43.0}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I700020/d02-x01-y01 +Title: doi:10.17182/hepdata.41831.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.878000e+00 2.000000e-03 2.000000e-03 6.560000e+02 1.658945e+02 1.658945e+02 +1.882500e+00 2.500000e-03 2.500000e-03 8.080000e+02 1.608540e+02 1.608540e+02 +1.887500e+00 2.500000e-03 2.500000e-03 6.560000e+02 1.581518e+02 1.581518e+02 +1.892500e+00 2.500000e-03 2.500000e-03 8.890000e+02 1.804993e+02 1.804993e+02 +1.897500e+00 2.500000e-03 2.500000e-03 9.010000e+02 1.882233e+02 1.882233e+02 +1.902500e+00 2.500000e-03 2.500000e-03 9.950000e+02 2.144411e+02 2.144411e+02 +1.907500e+00 2.500000e-03 2.500000e-03 7.260000e+02 1.904652e+02 1.904652e+02 +1.912500e+00 2.500000e-03 2.500000e-03 1.138000e+03 2.184033e+02 2.184033e+02 +1.920000e+00 5.000000e-03 5.000000e-03 7.980000e+02 1.237134e+02 1.237134e+02 +1.931250e+00 6.250000e-03 6.250000e-03 8.310000e+02 1.110856e+02 1.110856e+02 +1.943750e+00 6.250000e-03 6.250000e-03 8.170000e+02 1.125389e+02 1.125389e+02 +1.956250e+00 6.250000e-03 6.250000e-03 7.120000e+02 1.130885e+02 1.130885e+02 +1.968750e+00 6.250000e-03 6.250000e-03 8.020000e+02 1.134637e+02 1.134637e+02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I700020/d02-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.081, up: 0.071}}, 1: {error: {dn: -0.052, up: 0.047}}, 2: {error: {dn: -0.05, up: 0.045}}, 3: {error: {dn: -0.045, up: 0.041}}, 4: {error: {dn: -0.044, up: 0.04}}, 5: {error: {dn: -0.046, up: 0.041}}, 6: {error: {dn: -0.046, up: 0.04}}, 7: {error: {dn: -0.04, up: 0.036}}, 8: {error: {dn: -0.026, up: 0.024}}, 9: {error: {dn: -0.022, up: 0.02}}, 10: {error: {dn: -0.021, up: 0.02}}, 11: {error: {dn: -0.022, up: 0.021}}, 12: {error: {dn: -0.02, up: 0.019}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I700020/d02-x01-y02 +Title: doi:10.17182/hepdata.41831.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.878000e+00 2.000000e-03 2.000000e-03 5.740000e-01 8.100000e-02 7.100000e-02 +1.882500e+00 2.500000e-03 2.500000e-03 4.950000e-01 5.200000e-02 4.700000e-02 +1.887500e+00 2.500000e-03 2.500000e-03 3.900000e-01 5.000000e-02 4.500000e-02 +1.892500e+00 2.500000e-03 2.500000e-03 4.190000e-01 4.500000e-02 4.100000e-02 +1.897500e+00 2.500000e-03 2.500000e-03 3.980000e-01 4.400000e-02 4.000000e-02 +1.902500e+00 2.500000e-03 2.500000e-03 3.990000e-01 4.600000e-02 4.100000e-02 +1.907500e+00 2.500000e-03 2.500000e-03 3.260000e-01 4.600000e-02 4.000000e-02 +1.912500e+00 2.500000e-03 2.500000e-03 3.970000e-01 4.000000e-02 3.600000e-02 +1.920000e+00 5.000000e-03 5.000000e-03 3.210000e-01 2.600000e-02 2.400000e-02 +1.931250e+00 6.250000e-03 6.250000e-03 3.130000e-01 2.200000e-02 2.000000e-02 +1.943750e+00 6.250000e-03 6.250000e-03 2.980000e-01 2.100000e-02 2.000000e-02 +1.956250e+00 6.250000e-03 6.250000e-03 2.700000e-01 2.200000e-02 2.100000e-02 +1.968750e+00 6.250000e-03 6.250000e-03 2.800000e-01 2.000000e-02 1.900000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2006_I709730.cc b/analyses/pluginBABAR/BABAR_2006_I709730.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I709730.cc @@ -0,0 +1,101 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2006_I709730 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2006_I709730); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + _num3pip3pim = bookCounter("TMP/num3pip3pim" ); + _num2pip2pim2pi0 = bookCounter("TMP/num2pip2pim2pi0" ); + _num2pip2pim2KpKm = bookCounter("TMP/num2pip2pim2KpKm"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + if(ntotal!=6) vetoEvent; + if(nCount[-211]==3 && nCount[211]==3) + _num3pip3pim->fill(event.weight()); + else if(nCount[-211]==2 && nCount[211]==2 && nCount[111]==2) + _num2pip2pim2pi0->fill(event.weight()); + else if(nCount[-211]==2 && nCount[211]==2 && nCount[321]==1 && nCount[-321]==1) + _num2pip2pim2KpKm->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + + for(unsigned int ix=1; ix<4; ++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _num3pip3pim->val(); + error = _num3pip3pim->err(); + } + else if(ix==2) { + sigma = _num2pip2pim2pi0->val(); + error = _num2pip2pim2pi0->err(); + } + else if(ix==3) { + sigma = _num2pip2pim2KpKm->val(); + error = _num2pip2pim2KpKm->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + // just count the number of events of the types we're looking for + CounterPtr _num3pip3pim,_num2pip2pim2pi0,_num2pip2pim2KpKm; + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2006_I709730); + + +} diff --git a/analyses/pluginBABAR/BABAR_2006_I709730.info b/analyses/pluginBABAR/BABAR_2006_I709730.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I709730.info @@ -0,0 +1,39 @@ +Name: BABAR_2006_I709730 +Year: 2006 +Summary: Cross section for $e^+e^-\to$ $3\pi^+3\pi^-$, $2\pi^+2\pi^-2\pi^0$, $2\pi^+2\pi^-K^+K^-$ +Experiment: BABAR +Collider: PEP-II +InspireID: 709730 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D73.052003 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Luminosity_fb: 1 +Description: + 'Cross sections for $3\pi^+3\pi^-$, $2\pi^+2\pi^-2\pi^0$ and $2\pi^+2\pi^-K^+K^-$ measured by + BaBar using radiative return. Useful to compare hadronization and other non-perturbatuve models + at low energies between 1.3 and 4.5 GeV.' +Keywords: +BibKey: Aubert:2006jq +BibTeX: '@article{Aubert:2006jq, + author = "Aubert, Bernard and others", + title = "{The $e^+e^- \to 3(\pi^+ \pi^-), 2(\pi^+ \pi^- \pi^0)$ + and $K^+ K^- 2(\pi^+ \pi^-)$ cross sections at + center-of-mass energies from production threshold to + 4.5-GeV measured with initial-state radiation}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D73", + year = "2006", + pages = "052003", + doi = "10.1103/PhysRevD.73.052003", + eprint = "hep-ex/0602006", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-11663", + SLACcitation = "%%CITATION = HEP-EX/0602006;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2006_I709730.plot b/analyses/pluginBABAR/BABAR_2006_I709730.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I709730.plot @@ -0,0 +1,18 @@ +BEGIN PLOT /BABAR_2006_I709730/d01-x01-y01 +Title=$\sigma(e^+e^-\to 3\pi^+3\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 3\pi^+3\pi^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2006_I709730/d02-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-2\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2006_I709730/d03-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-K^+K^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2006_I709730.yoda b/analyses/pluginBABAR/BABAR_2006_I709730.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I709730.yoda @@ -0,0 +1,389 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I709730/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.01, up: 0.01}}, 1: {error: {dn: -0.01, up: 0.01}}, 2: {error: {dn: -0.01, up: 0.01}}, 3: {error: {dn: -0.01, up: 0.01}}, 4: {error: {dn: -0.02, up: 0.02}}, 5: {error: {dn: -0.01, up: 0.01}}, 6: {error: {dn: -0.02, up: 0.02}}, 7: {error: {dn: -0.02, up: 0.02}}, 8: {error: {dn: -0.03, up: 0.03}}, 9: {error: {dn: -0.03, up: 0.03}}, 10: {error: {dn: -0.03, up: 0.03}}, 11: {error: {dn: -0.05, up: 0.05}}, 12: {error: {dn: -0.05, up: 0.05}}, 13: {error: {dn: -0.06, up: 0.06}}, 14: {error: {dn: -0.06, up: 0.06}}, 15: {error: {dn: -0.07, up: 0.07}}, 16: {error: {dn: -0.09, up: 0.09}}, 17: {error: {dn: -0.09, up: 0.09}}, 18: {error: {dn: -0.11, up: 0.11}}, 19: {error: {dn: -0.11, up: 0.11}}, 20: {error: {dn: -0.11, up: 0.11}}, 21: {error: {dn: -0.12, up: 0.12}}, 22: {error: {dn: -0.12, up: 0.12}}, 23: {error: {dn: -0.11, up: 0.11}}, 24: {error: {dn: -0.1, up: 0.1}}, 25: {error: {dn: -0.1, up: 0.1}}, 26: {error: {dn: -0.1, up: 0.1}}, 27: {error: {dn: -0.1, up: 0.1}}, 28: {error: {dn: -0.11, up: 0.11}}, 29: {error: {dn: -0.11, up: 0.11}}, 30: {error: {dn: -0.11, up: 0.11}}, 31: {error: {dn: -0.11, up: 0.11}}, 32: {error: {dn: -0.12, up: 0.12}}, 33: {error: {dn: -0.11, up: 0.11}}, 34: {error: {dn: -0.12, up: 0.12}}, 35: {error: {dn: -0.11, up: 0.11}}, 36: {error: {dn: -0.12, up: 0.12}}, 37: {error: {dn: -0.11, up: 0.11}}, 38: {error: {dn: -0.11, up: 0.11}}, 39: {error: {dn: -0.12, up: 0.12}}, 40: {error: {dn: -0.11, up: 0.11}}, 41: {error: {dn: -0.11, up: 0.11}}, 42: {error: {dn: -0.1, up: 0.1}}, 43: {error: {dn: -0.1, up: 0.1}}, 44: {error: {dn: -0.11, up: 0.11}}, 45: {error: {dn: -0.1, up: 0.1}}, 46: {error: {dn: -0.1, up: 0.1}}, 47: {error: {dn: -0.1, up: 0.1}}, 48: {error: {dn: -0.1, up: 0.1}}, 49: {error: {dn: -0.09, up: 0.09}}, 50: {error: {dn: -0.1, up: 0.1}}, 51: {error: {dn: -0.1, up: 0.1}}, 52: {error: {dn: -0.1, up: 0.1}}, 53: {error: {dn: -0.1, up: 0.1}}, 54: {error: {dn: -0.09, up: 0.09}}, 55: {error: {dn: -0.09, up: 0.09}}, 56: {error: {dn: -0.09, up: 0.09}}, 57: {error: {dn: -0.1, up: 0.1}}, 58: {error: {dn: -0.09, up: 0.09}}, 59: {error: {dn: -0.09, up: 0.09}}, 60: {error: {dn: -0.09, up: 0.09}}, 61: {error: {dn: -0.08, up: 0.08}}, 62: {error: {dn: -0.08, up: 0.08}}, 63: {error: {dn: -0.09, up: 0.09}}, 64: {error: {dn: -0.08, up: 0.08}}, 65: {error: {dn: -0.08, up: 0.08}}, 66: {error: {dn: -0.08, up: 0.08}}, 67: {error: {dn: -0.08, up: 0.08}}, 68: {error: {dn: -0.07, up: 0.07}}, 69: {error: {dn: -0.07, up: 0.07}}, 70: {error: {dn: -0.07, up: 0.07}}, 71: {error: {dn: -0.1, up: 0.1}}, 72: {error: {dn: -0.1, up: 0.1}}, 73: {error: {dn: -0.07, up: 0.07}}, 74: {error: {dn: -0.07, up: 0.07}}, 75: {error: {dn: -0.06, up: 0.06}}, 76: {error: {dn: -0.07, up: 0.07}}, 77: {error: {dn: -0.07, up: 0.07}}, 78: {error: {dn: -0.06, up: 0.06}}, 79: {error: {dn: -0.06, up: 0.06}}, 80: {error: {dn: -0.06, up: 0.06}}, 81: {error: {dn: -0.06, up: 0.06}}, 82: {error: {dn: -0.06, up: 0.06}}, 83: {error: {dn: -0.06, up: 0.06}}, 84: {error: {dn: -0.06, up: 0.06}}, 85: {error: {dn: -0.06, up: 0.06}}, 86: {error: {dn: -0.06, up: 0.06}}, 87: {error: {dn: -0.05, up: 0.05}}, 88: {error: {dn: -0.05, up: 0.05}}, 89: {error: {dn: -0.05, up: 0.05}}, 90: {error: {dn: -0.06, up: 0.06}}, 91: {error: {dn: -0.06, up: 0.06}}, 92: {error: {dn: -0.05, up: 0.05}}, 93: {error: {dn: -0.05, up: 0.05}}, 94: {error: {dn: -0.05, up: 0.05}}, 95: {error: {dn: -0.05, up: 0.05}}, 96: {error: {dn: -0.06, up: 0.06}}, 97: {error: {dn: -0.05, up: 0.05}}, 98: {error: {dn: -0.05, up: 0.05}}, 99: {error: {dn: -0.05, up: 0.05}}, 100: {error: {dn: -0.05, up: 0.05}}, 101: {error: {dn: -0.05, up: 0.05}}, 102: {error: {dn: -0.05, up: 0.05}}, 103: {error: {dn: -0.05, up: 0.05}}, 104: {error: {dn: -0.04, up: 0.04}}, 105: {error: {dn: -0.05, up: 0.05}}, 106: {error: {dn: -0.05, up: 0.05}}, 107: {error: {dn: -0.04, up: 0.04}}, 108: {error: {dn: -0.04, up: 0.04}}, 109: {error: {dn: -0.04, up: 0.04}}, 110: {error: {dn: -0.04, up: 0.04}}, 111: {error: {dn: -0.04, up: 0.04}}, 112: {error: {dn: -0.04, up: 0.04}}, 113: {error: {dn: -0.04, up: 0.04}}, 114: {error: {dn: -0.04, up: 0.04}}, 115: {error: {dn: -0.04, up: 0.04}}, 116: {error: {dn: -0.04, up: 0.04}}, 117: {error: {dn: -0.04, up: 0.04}}, 118: {error: {dn: -0.04, up: 0.04}}, 119: {error: {dn: -0.04, up: 0.04}}, 120: {error: {dn: -0.04, up: 0.04}}, 121: {error: {dn: -0.04, up: 0.04}}, 122: {error: {dn: -0.04, up: 0.04}}, 123: {error: {dn: -0.04, up: 0.04}}, 124: {error: {dn: -0.04, up: 0.04}}, 125: {error: {dn: -0.04, up: 0.04}}, 126: {error: {dn: -0.03, up: 0.03}}, 127: {error: {dn: -0.04, up: 0.04}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I709730/d01-x01-y01 +Title: doi:10.17182/hepdata.41843.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.312500e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +1.337500e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +1.362500e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +1.387500e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +1.412500e+00 0.000000e+00 0.000000e+00 0.000000e+00 2.000000e-02 2.000000e-02 +1.437500e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +1.462500e+00 0.000000e+00 0.000000e+00 1.000000e-02 2.000000e-02 2.000000e-02 +1.487500e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +1.512500e+00 0.000000e+00 0.000000e+00 5.000000e-02 3.000000e-02 3.000000e-02 +1.537500e+00 0.000000e+00 0.000000e+00 1.000000e-01 3.000000e-02 3.000000e-02 +1.562500e+00 0.000000e+00 0.000000e+00 1.200000e-01 3.000000e-02 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1.090000e+00 1.100000e-01 1.100000e-01 +1.912500e+00 0.000000e+00 0.000000e+00 1.080000e+00 1.000000e-01 1.000000e-01 +1.937500e+00 0.000000e+00 0.000000e+00 9.100000e-01 1.000000e-01 1.000000e-01 +1.962500e+00 0.000000e+00 0.000000e+00 1.140000e+00 1.000000e-01 1.000000e-01 +1.987500e+00 0.000000e+00 0.000000e+00 1.010000e+00 1.000000e-01 1.000000e-01 +2.012500e+00 0.000000e+00 0.000000e+00 1.190000e+00 1.100000e-01 1.100000e-01 +2.037500e+00 0.000000e+00 0.000000e+00 1.540000e+00 1.100000e-01 1.100000e-01 +2.062500e+00 0.000000e+00 0.000000e+00 1.490000e+00 1.100000e-01 1.100000e-01 +2.087500e+00 0.000000e+00 0.000000e+00 1.480000e+00 1.100000e-01 1.100000e-01 +2.112500e+00 0.000000e+00 0.000000e+00 1.360000e+00 1.200000e-01 1.200000e-01 +2.137500e+00 0.000000e+00 0.000000e+00 1.350000e+00 1.100000e-01 1.100000e-01 +2.162500e+00 0.000000e+00 0.000000e+00 1.450000e+00 1.200000e-01 1.200000e-01 +2.187500e+00 0.000000e+00 0.000000e+00 1.170000e+00 1.100000e-01 1.100000e-01 +2.212500e+00 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/REF/BABAR_2006_I709730/d02-x01-y01 +Title: doi:10.17182/hepdata.41843.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.312500e+00 0.000000e+00 0.000000e+00 0.000000e+00 4.000000e-02 4.000000e-02 +1.337500e+00 0.000000e+00 0.000000e+00 0.000000e+00 5.000000e-02 5.000000e-02 +1.362500e+00 0.000000e+00 0.000000e+00 4.000000e-02 6.000000e-02 6.000000e-02 +1.387500e+00 0.000000e+00 0.000000e+00 6.000000e-02 7.000000e-02 7.000000e-02 +1.412500e+00 0.000000e+00 0.000000e+00 9.000000e-02 8.000000e-02 8.000000e-02 +1.437500e+00 0.000000e+00 0.000000e+00 0.000000e+00 6.000000e-02 6.000000e-02 +1.462500e+00 0.000000e+00 0.000000e+00 1.900000e-01 9.000000e-02 9.000000e-02 +1.487500e+00 0.000000e+00 0.000000e+00 4.000000e-02 9.000000e-02 9.000000e-02 +1.512500e+00 0.000000e+00 0.000000e+00 1.800000e-01 1.300000e-01 1.300000e-01 +1.537500e+00 0.000000e+00 0.000000e+00 3.000000e-01 1.500000e-01 1.500000e-01 +1.562500e+00 0.000000e+00 0.000000e+00 5.800000e-01 1.600000e-01 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4.370000e+00 3.900000e-01 3.900000e-01 +1.912500e+00 0.000000e+00 0.000000e+00 4.050000e+00 3.800000e-01 3.800000e-01 +1.937500e+00 0.000000e+00 0.000000e+00 4.440000e+00 3.900000e-01 3.900000e-01 +1.962500e+00 0.000000e+00 0.000000e+00 4.480000e+00 3.800000e-01 3.800000e-01 +1.987500e+00 0.000000e+00 0.000000e+00 4.850000e+00 4.000000e-01 4.000000e-01 +2.012500e+00 0.000000e+00 0.000000e+00 5.590000e+00 4.100000e-01 4.100000e-01 +2.037500e+00 0.000000e+00 0.000000e+00 5.150000e+00 4.000000e-01 4.000000e-01 +2.062500e+00 0.000000e+00 0.000000e+00 6.120000e+00 4.200000e-01 4.200000e-01 +2.087500e+00 0.000000e+00 0.000000e+00 5.970000e+00 4.200000e-01 4.200000e-01 +2.112500e+00 0.000000e+00 0.000000e+00 6.440000e+00 4.300000e-01 4.300000e-01 +2.137500e+00 0.000000e+00 0.000000e+00 5.450000e+00 4.200000e-01 4.200000e-01 +2.162500e+00 0.000000e+00 0.000000e+00 5.920000e+00 4.100000e-01 4.100000e-01 +2.187500e+00 0.000000e+00 0.000000e+00 4.810000e+00 4.000000e-01 4.000000e-01 +2.212500e+00 0.000000e+00 0.000000e+00 5.810000e+00 4.000000e-01 4.000000e-01 +2.237500e+00 0.000000e+00 0.000000e+00 5.450000e+00 3.900000e-01 3.900000e-01 +2.262500e+00 0.000000e+00 0.000000e+00 5.680000e+00 3.900000e-01 3.900000e-01 +2.287500e+00 0.000000e+00 0.000000e+00 5.040000e+00 3.900000e-01 3.900000e-01 +2.312500e+00 0.000000e+00 0.000000e+00 5.100000e+00 3.600000e-01 3.600000e-01 +2.337500e+00 0.000000e+00 0.000000e+00 4.990000e+00 3.700000e-01 3.700000e-01 +2.362500e+00 0.000000e+00 0.000000e+00 5.010000e+00 3.700000e-01 3.700000e-01 +2.387500e+00 0.000000e+00 0.000000e+00 4.880000e+00 3.600000e-01 3.600000e-01 +2.412500e+00 0.000000e+00 0.000000e+00 5.860000e+00 3.700000e-01 3.700000e-01 +2.437500e+00 0.000000e+00 0.000000e+00 4.070000e+00 3.300000e-01 3.300000e-01 +2.462500e+00 0.000000e+00 0.000000e+00 4.700000e+00 3.400000e-01 3.400000e-01 +2.487500e+00 0.000000e+00 0.000000e+00 4.370000e+00 3.300000e-01 3.300000e-01 +2.512500e+00 0.000000e+00 0.000000e+00 4.250000e+00 3.400000e-01 3.400000e-01 +2.537500e+00 0.000000e+00 0.000000e+00 4.390000e+00 3.300000e-01 3.300000e-01 +2.562500e+00 0.000000e+00 0.000000e+00 3.850000e+00 3.100000e-01 3.100000e-01 +2.587500e+00 0.000000e+00 0.000000e+00 4.130000e+00 3.100000e-01 3.100000e-01 +2.612500e+00 0.000000e+00 0.000000e+00 3.920000e+00 3.100000e-01 3.100000e-01 +2.637500e+00 0.000000e+00 0.000000e+00 3.490000e+00 3.100000e-01 3.100000e-01 +2.662500e+00 0.000000e+00 0.000000e+00 3.740000e+00 3.100000e-01 3.100000e-01 +2.687500e+00 0.000000e+00 0.000000e+00 3.410000e+00 3.000000e-01 3.000000e-01 +2.712500e+00 0.000000e+00 0.000000e+00 3.720000e+00 3.000000e-01 3.000000e-01 +2.737500e+00 0.000000e+00 0.000000e+00 2.940000e+00 2.900000e-01 2.900000e-01 +2.762500e+00 0.000000e+00 0.000000e+00 3.340000e+00 3.000000e-01 3.000000e-01 +2.787500e+00 0.000000e+00 0.000000e+00 3.110000e+00 2.900000e-01 2.900000e-01 +2.812500e+00 0.000000e+00 0.000000e+00 3.430000e+00 2.900000e-01 2.900000e-01 +2.837500e+00 0.000000e+00 0.000000e+00 2.810000e+00 2.800000e-01 2.800000e-01 +2.862500e+00 0.000000e+00 0.000000e+00 3.120000e+00 2.700000e-01 2.700000e-01 +2.887500e+00 0.000000e+00 0.000000e+00 2.450000e+00 2.600000e-01 2.600000e-01 +2.912500e+00 0.000000e+00 0.000000e+00 2.460000e+00 2.600000e-01 2.600000e-01 +2.937500e+00 0.000000e+00 0.000000e+00 2.490000e+00 2.600000e-01 2.600000e-01 +2.962500e+00 0.000000e+00 0.000000e+00 2.160000e+00 2.600000e-01 2.600000e-01 +2.987500e+00 0.000000e+00 0.000000e+00 2.640000e+00 2.600000e-01 2.600000e-01 +3.012500e+00 0.000000e+00 0.000000e+00 2.880000e+00 2.600000e-01 2.600000e-01 +3.037500e+00 0.000000e+00 0.000000e+00 2.010000e+00 2.600000e-01 2.600000e-01 +3.062500e+00 0.000000e+00 0.000000e+00 2.170000e+00 2.400000e-01 2.400000e-01 +3.087500e+00 0.000000e+00 0.000000e+00 6.940000e+00 3.400000e-01 3.400000e-01 +3.112500e+00 0.000000e+00 0.000000e+00 5.480000e+00 3.100000e-01 3.100000e-01 +3.137500e+00 0.000000e+00 0.000000e+00 2.410000e+00 2.300000e-01 2.300000e-01 +3.162500e+00 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1.700000e-01 +3.487500e+00 0.000000e+00 0.000000e+00 1.350000e+00 1.700000e-01 1.700000e-01 +3.512500e+00 0.000000e+00 0.000000e+00 1.060000e+00 1.700000e-01 1.700000e-01 +3.537500e+00 0.000000e+00 0.000000e+00 1.070000e+00 1.600000e-01 1.600000e-01 +3.562500e+00 0.000000e+00 0.000000e+00 8.700000e-01 1.500000e-01 1.500000e-01 +3.587500e+00 0.000000e+00 0.000000e+00 7.000000e-01 1.500000e-01 1.500000e-01 +3.612500e+00 0.000000e+00 0.000000e+00 7.000000e-01 1.600000e-01 1.600000e-01 +3.637500e+00 0.000000e+00 0.000000e+00 1.180000e+00 1.600000e-01 1.600000e-01 +3.662500e+00 0.000000e+00 0.000000e+00 7.400000e-01 1.500000e-01 1.500000e-01 +3.687500e+00 0.000000e+00 0.000000e+00 1.650000e+00 1.700000e-01 1.700000e-01 +3.712500e+00 0.000000e+00 0.000000e+00 7.400000e-01 1.500000e-01 1.500000e-01 +3.737500e+00 0.000000e+00 0.000000e+00 5.100000e-01 1.300000e-01 1.300000e-01 +3.762500e+00 0.000000e+00 0.000000e+00 6.000000e-01 1.400000e-01 1.400000e-01 +3.787500e+00 0.000000e+00 0.000000e+00 6.400000e-01 1.300000e-01 1.300000e-01 +3.812500e+00 0.000000e+00 0.000000e+00 8.600000e-01 1.400000e-01 1.400000e-01 +3.837500e+00 0.000000e+00 0.000000e+00 7.300000e-01 1.300000e-01 1.300000e-01 +3.862500e+00 0.000000e+00 0.000000e+00 5.300000e-01 1.300000e-01 1.300000e-01 +3.887500e+00 0.000000e+00 0.000000e+00 5.300000e-01 1.200000e-01 1.200000e-01 +3.912500e+00 0.000000e+00 0.000000e+00 7.000000e-01 1.300000e-01 1.300000e-01 +3.937500e+00 0.000000e+00 0.000000e+00 6.200000e-01 1.300000e-01 1.300000e-01 +3.962500e+00 0.000000e+00 0.000000e+00 5.000000e-01 1.200000e-01 1.200000e-01 +3.987500e+00 0.000000e+00 0.000000e+00 5.500000e-01 1.200000e-01 1.200000e-01 +4.012500e+00 0.000000e+00 0.000000e+00 4.700000e-01 1.200000e-01 1.200000e-01 +4.037500e+00 0.000000e+00 0.000000e+00 4.200000e-01 1.200000e-01 1.200000e-01 +4.062500e+00 0.000000e+00 0.000000e+00 6.000000e-01 1.200000e-01 1.200000e-01 +4.087500e+00 0.000000e+00 0.000000e+00 4.000000e-01 1.100000e-01 1.100000e-01 +4.112500e+00 0.000000e+00 0.000000e+00 5.000000e-01 1.100000e-01 1.100000e-01 +4.137500e+00 0.000000e+00 0.000000e+00 4.600000e-01 1.100000e-01 1.100000e-01 +4.162500e+00 0.000000e+00 0.000000e+00 3.200000e-01 1.100000e-01 1.100000e-01 +4.187500e+00 0.000000e+00 0.000000e+00 4.500000e-01 1.000000e-01 1.000000e-01 +4.212500e+00 0.000000e+00 0.000000e+00 1.700000e-01 1.000000e-01 1.000000e-01 +4.237500e+00 0.000000e+00 0.000000e+00 5.000000e-01 1.100000e-01 1.100000e-01 +4.262500e+00 0.000000e+00 0.000000e+00 1.400000e-01 1.000000e-01 1.000000e-01 +4.287500e+00 0.000000e+00 0.000000e+00 3.900000e-01 1.100000e-01 1.100000e-01 +4.312500e+00 0.000000e+00 0.000000e+00 2.600000e-01 1.000000e-01 1.000000e-01 +4.337500e+00 0.000000e+00 0.000000e+00 5.600000e-01 1.000000e-01 1.000000e-01 +4.362500e+00 0.000000e+00 0.000000e+00 2.600000e-01 1.100000e-01 1.100000e-01 +4.387500e+00 0.000000e+00 0.000000e+00 3.000000e-01 1.000000e-01 1.000000e-01 +4.412500e+00 0.000000e+00 0.000000e+00 3.400000e-01 1.000000e-01 1.000000e-01 +4.437500e+00 0.000000e+00 0.000000e+00 1.600000e-01 1.000000e-01 1.000000e-01 +4.462500e+00 0.000000e+00 0.000000e+00 3.200000e-01 1.000000e-01 1.000000e-01 +4.487500e+00 0.000000e+00 0.000000e+00 1.700000e-01 1.000000e-01 1.000000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I709730/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0015, up: 0.0015}}, 1: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0015, up: 0.0015}}, 2: {error: {dn: -0.0, up: 0.0}, sys: {dn: -0.0, up: 0.0}}, 3: {error: {dn: -0.01, up: 0.01}, sys: {dn: -0.0015, up: 0.0015}}, 4: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.003, up: 0.003}}, 5: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.003, up: 0.003}}, 6: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.012, up: 0.012}}, 7: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.0075, up: 0.0075}}, 8: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.018, up: 0.018}}, 9: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.015, up: 0.015}}, 10: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.003, up: 0.003}}, 11: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.027, up: 0.027}}, 12: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.0225, up: 0.0225}}, 13: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.0315, up: 0.0315}}, 14: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.012, up: 0.012}}, 15: {error: {dn: -0.07, up: 0.07}, sys: {dn: -0.0375, up: 0.0375}}, 16: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.051000000000000004, up: 0.051000000000000004}}, 17: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.0585, up: 0.0585}}, 18: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.057, up: 0.057}}, 19: {error: {dn: -0.07, up: 0.07}, sys: {dn: -0.0285, up: 0.0285}}, 20: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.054, up: 0.054}}, 21: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.036, up: 0.036}}, 22: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.045, up: 0.045}}, 23: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.048, up: 0.048}}, 24: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.039, up: 0.039}}, 25: {error: {dn: -0.08, up: 0.08}, sys: {dn: -0.0435, up: 0.0435}}, 26: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.066, up: 0.066}}, 27: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.0825, up: 0.0825}}, 28: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.04200000000000001, up: 0.04200000000000001}}, 29: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.0705, up: 0.0705}}, 30: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.0435, up: 0.0435}}, 31: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.081, up: 0.081}}, 32: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.0795, up: 0.0795}}, 33: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.0735, up: 0.0735}}, 34: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.048, up: 0.048}}, 35: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.0675, up: 0.0675}}, 36: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.0375, up: 0.0375}}, 37: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.10200000000000001, up: 0.10200000000000001}}, 38: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.063, up: 0.063}}, 39: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.078, up: 0.078}}, 40: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.051000000000000004, up: 0.051000000000000004}}, 41: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.0645, up: 0.0645}}, 42: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.1035, up: 0.1035}}, 43: {error: {dn: -0.2, up: 0.2}, sys: {dn: -0.3045, up: 0.3045}}, 44: {error: {dn: -0.16, up: 0.16}, sys: {dn: -0.17099999999999999, up: 0.17099999999999999}}, 45: {error: {dn: -0.13, up: 0.13}, sys: {dn: -0.063, up: 0.063}}, 46: {error: {dn: -0.12, up: 0.12}, sys: {dn: -0.093, up: 0.093}}, 47: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.0585, up: 0.0585}}, 48: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.08400000000000002, up: 0.08400000000000002}}, 49: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.0555, up: 0.0555}}, 50: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.054, up: 0.054}}, 51: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.081, up: 0.081}}, 52: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.0645, up: 0.0645}}, 53: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.021000000000000005, up: 0.021000000000000005}}, 54: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.057, up: 0.057}}, 55: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.0585, up: 0.0585}}, 56: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.025500000000000002, up: 0.025500000000000002}}, 57: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.0645, up: 0.0645}}, 58: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.051000000000000004, up: 0.051000000000000004}}, 59: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.06, up: 0.06}}, 60: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.0435, up: 0.0435}}, 61: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.015, up: 0.015}}, 62: {error: {dn: -0.1, up: 0.1}, sys: {dn: -0.025500000000000002, up: 0.025500000000000002}}, 63: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.025500000000000002, up: 0.025500000000000002}}, 64: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.027, up: 0.027}}, 65: {error: {dn: 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2.000000e-02 3.014963e-02 3.014963e-02 +2.162500e+00 0.000000e+00 0.000000e+00 8.000000e-02 4.176123e-02 4.176123e-02 +2.187500e+00 0.000000e+00 0.000000e+00 5.000000e-02 3.092329e-02 3.092329e-02 +2.212500e+00 0.000000e+00 0.000000e+00 1.200000e-01 4.386342e-02 4.386342e-02 +2.237500e+00 0.000000e+00 0.000000e+00 1.000000e-01 3.354102e-02 3.354102e-02 +2.262500e+00 0.000000e+00 0.000000e+00 2.000000e-02 3.014963e-02 3.014963e-02 +2.287500e+00 0.000000e+00 0.000000e+00 1.800000e-01 6.579514e-02 6.579514e-02 +2.312500e+00 0.000000e+00 0.000000e+00 1.500000e-01 5.482928e-02 5.482928e-02 +2.337500e+00 0.000000e+00 0.000000e+00 2.100000e-01 6.776614e-02 6.776614e-02 +2.362500e+00 0.000000e+00 0.000000e+00 8.000000e-02 5.141984e-02 5.141984e-02 +2.387500e+00 0.000000e+00 0.000000e+00 2.500000e-01 7.941190e-02 7.941190e-02 +2.412500e+00 0.000000e+00 0.000000e+00 3.400000e-01 9.487360e-02 9.487360e-02 +2.437500e+00 0.000000e+00 0.000000e+00 3.900000e-01 9.910727e-02 9.910727e-02 +2.462500e+00 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9.996124e-02 +2.787500e+00 0.000000e+00 0.000000e+00 5.400000e-01 1.286895e-01 1.286895e-01 +2.812500e+00 0.000000e+00 0.000000e+00 5.300000e-01 1.357212e-01 1.357212e-01 +2.837500e+00 0.000000e+00 0.000000e+00 4.900000e-01 1.241058e-01 1.241058e-01 +2.862500e+00 0.000000e+00 0.000000e+00 3.200000e-01 1.109234e-01 1.109234e-01 +2.887500e+00 0.000000e+00 0.000000e+00 4.500000e-01 1.290591e-01 1.290591e-01 +2.912500e+00 0.000000e+00 0.000000e+00 2.500000e-01 1.068000e-01 1.068000e-01 +2.937500e+00 0.000000e+00 0.000000e+00 6.800000e-01 1.500133e-01 1.500133e-01 +2.962500e+00 0.000000e+00 0.000000e+00 4.200000e-01 1.181905e-01 1.181905e-01 +2.987500e+00 0.000000e+00 0.000000e+00 5.200000e-01 1.348481e-01 1.348481e-01 +3.012500e+00 0.000000e+00 0.000000e+00 3.400000e-01 1.122542e-01 1.122542e-01 +3.037500e+00 0.000000e+00 0.000000e+00 4.300000e-01 1.275157e-01 1.275157e-01 +3.062500e+00 0.000000e+00 0.000000e+00 6.900000e-01 1.510372e-01 1.510372e-01 +3.087500e+00 0.000000e+00 0.000000e+00 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0.000000e+00 0.000000e+00 2.000000e-01 1.140175e-01 1.140175e-01 +4.387500e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.001798e-01 1.001798e-01 +4.412500e+00 0.000000e+00 0.000000e+00 1.400000e-01 1.021812e-01 1.021812e-01 +4.437500e+00 0.000000e+00 0.000000e+00 2.400000e-01 9.693297e-02 9.693297e-02 +4.462500e+00 0.000000e+00 0.000000e+00 3.100000e-01 1.194247e-01 1.194247e-01 +4.487500e+00 0.000000e+00 0.000000e+00 2.600000e-01 1.073359e-01 1.073359e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2006_I716277.cc b/analyses/pluginBABAR/BABAR_2006_I716277.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I716277.cc @@ -0,0 +1,132 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2006_I716277 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2006_I716277); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaGamma = bookCounter("TMP/EtaGamma"); + _numEtaPrimeGamma = bookCounter("TMP/EtaPrimeGamma"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the eta/eta prime + if(p.pdgId()!=221 && p.pdgId()!=331) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(val.first==22) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(p.pdgId()==221) + _numEtaGamma->fill(event.weight()); + else + _numEtaPrimeGamma->fill(event.weight()); + } + } + } + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma,error; + if(ix==1) { + sigma = _numEtaGamma->val(); + error = _numEtaGamma->err(); + } + else { + sigma = _numEtaPrimeGamma->val(); + error = _numEtaPrimeGamma->err(); + } + sigma *= crossSection()/ sumOfWeights() /femtobarn; + error *= crossSection()/ sumOfWeights() /femtobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numEtaGamma,_numEtaPrimeGamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2006_I716277); + + +} diff --git a/analyses/pluginBABAR/BABAR_2006_I716277.info b/analyses/pluginBABAR/BABAR_2006_I716277.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I716277.info @@ -0,0 +1,33 @@ +Name: BABAR_2006_I716277 +Year: 2006 +Summary: Cross section for $e^+e^-\to\eta\gamma$ and $\eta^\prime\gamma$ at 10.58 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 716277 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - PR D74,012002 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\eta\gamma$ and $\eta^\prime\gamma$ at 10.58 GeV' +BibKey: Aubert:2006cy +BibTeX: '@article{Aubert:2006cy, + author = "Aubert, Bernard and others", + title = "{Measurement of the eta and eta-prime transition + form-factors at q**2 = 112-GeV**2}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D74", + year = "2006", + pages = "012002", + doi = "10.1103/PhysRevD.74.012002", + eprint = "hep-ex/0605018", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-11849, BABAR-PUB-06-024", + SLACcitation = "%%CITATION = HEP-EX/0605018;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2006_I716277.plot b/analyses/pluginBABAR/BABAR_2006_I716277.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I716277.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /BABAR_2006_I716277/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\gamma)$/fb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +XMin=10.56 +XMax=10.60 +END PLOT + +BEGIN PLOT /BABAR_2006_I716277/d01-x01-y02 +Title=$\sigma(e^+e^-\to \eta^\prime\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta^\prime\gamma)$/fb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +XMin=10.56 +XMax=10.60 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2006_I716277.yoda b/analyses/pluginBABAR/BABAR_2006_I716277.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I716277.yoda @@ -0,0 +1,72 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I716277/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -1.1, up: 1.2}, sys: {dn: -0.3, up: 0.3}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I716277/d01-x01-y01 +Title: doi:10.17182/hepdata.22085.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 4.500000e+00 1.140175e+00 1.236932e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I716277/d01-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.8, up: 0.8}, sys: {dn: -0.3, up: 0.3}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I716277/d01-x01-y02 +Title: doi:10.17182/hepdata.22085.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 5.400000e+00 8.544004e-01 8.544004e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I716277/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -1.0, up: 1.2}, sys: {dn: -0.3, up: 0.3}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I716277/d02-x01-y01 +Title: doi:10.17182/hepdata.22085.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 4.200000e+00 1.044031e+00 1.236932e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I716277/d02-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.7, up: 0.8}, sys: {dn: -0.3, up: 0.3}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I716277/d02-x01-y02 +Title: doi:10.17182/hepdata.22085.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 5.000000e+00 7.615773e-01 8.544004e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I716277/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.03, up: 0.03}, sys: {dn: -0.008, up: 0.008}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I716277/d03-x01-y01 +Title: doi:10.17182/hepdata.22085.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 2.290000e-01 3.104835e-02 3.104835e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I716277/d03-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.019, up: 0.019}, sys: {dn: -0.008, up: 0.008}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I716277/d03-x01-y02 +Title: doi:10.17182/hepdata.22085.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 2.510000e-01 2.061553e-02 2.061553e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2006_I731865.cc b/analyses/pluginBABAR/BABAR_2006_I731865.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I731865.cc @@ -0,0 +1,117 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2006_I731865 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2006_I731865); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + _nPhiEta = bookCounter("TMP/phieta"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=333) continue; + map nRes=nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + foreach (const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=221) continue; + if(p2.parents()[0].isSame(p)) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=0) continue; + bool matched2 = true; + for(auto const & val : nResB) { + if(val.second!=0) { + matched2 = false; + break; + } + } + if(matched2) { + _nPhiEta->fill(event.weight()); + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nPhiEta->val(); + double error = _nPhiEta->err(); + sigma *= crossSection()/ sumOfWeights() /femtobarn; + error *= crossSection()/ sumOfWeights() /femtobarn; + + Scatter2D temphisto(refData(1, 1, 2)); + Scatter2DPtr mult = bookScatter2D(1, 1, 2); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + /// @name Histograms + //@{ + CounterPtr _nPhiEta; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2006_I731865); + +} diff --git a/analyses/pluginBABAR/BABAR_2006_I731865.info b/analyses/pluginBABAR/BABAR_2006_I731865.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I731865.info @@ -0,0 +1,35 @@ +Name: BABAR_2006_I731865 +Year: 2006 +Summary: Cross section for $\phi\eta$ at 10.58 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 731865 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - PR D74,111103 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $\phi\eta$ at 10.58 GeV' +Keywords: [] +BibKey: Aubert:2006xw +BibTeX: '@article{Aubert:2006xw, + author = "Aubert, Bernard and others", + title = "{Observation of the Exclusive Reaction $e^{+} e^{-} \to + \phi \eta$ at $\sqrt{s}$ = 10.58-GeV}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D74", + year = "2006", + pages = "111103", + doi = "10.1103/PhysRevD.74.111103", + eprint = "hep-ex/0611028", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-12200, BABAR-PUB-06-065", + SLACcitation = "%%CITATION = HEP-EX/0611028;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2006_I731865.plot b/analyses/pluginBABAR/BABAR_2006_I731865.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I731865.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /BABAR_2006_I731865/d01-x01-y02 +Title=$\sigma(e^+e^-\to \phi\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\eta)$/pb +ConnectGaps=1 +XMin = 10.56 +XMin = 10.60 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2006_I731865.yoda b/analyses/pluginBABAR/BABAR_2006_I731865.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2006_I731865.yoda @@ -0,0 +1,24 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I731865/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.4, up: 0.4}, sys: {dn: -0.1, up: 0.1}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I731865/d01-x01-y01 +Title: doi:10.17182/hepdata.52608.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 2.100000e+00 4.123106e-01 4.123106e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2006_I731865/d01-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.5, up: 0.5}, sys: {dn: -0.1, up: 0.1}}} + +IsRef: 1 +Path: /REF/BABAR_2006_I731865/d01-x01-y02 +Title: doi:10.17182/hepdata.52608.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 2.900000e+00 5.099020e-01 5.099020e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2007_I729388.cc b/analyses/pluginBABAR/BABAR_2007_I729388.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I729388.cc @@ -0,0 +1,118 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2007_I729388 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2007_I729388); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nPsi2s = bookCounter("TMP/psi2s"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the psi(2S) + if(p.pdgId()==100443) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // omega pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nPsi2s->fill(event.weight()); + break; + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nPsi2s->val(); + double error = _nPsi2s->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nPsi2s; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2007_I729388); + + +} diff --git a/analyses/pluginBABAR/BABAR_2007_I729388.info b/analyses/pluginBABAR/BABAR_2007_I729388.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I729388.info @@ -0,0 +1,38 @@ +Name: BABAR_2007_I729388 +Year: 2007 +Summary: Cross section for $e^+e^-\to \psi(2S)\pi^+\pi^-$ at energies between 4 and 8 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 729388 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 98 (2007) 212001 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to \psi(2S)\pi^+\pi^-$ at energies between 4 and 8 GeV using radiative return by BABAR.' +BibKey: Aubert:2007zz +BibTeX: '@article{Aubert:2007zz, + author = "Aubert, Bernard and others", + title = "{Evidence of a broad structure at an invariant mass of + 4.32- $GeV/c^{2}$ in the reaction $e^{+} e^{-} \to \pi^{+} + \pi^{-} \psi_{2S}$ measured at BaBar}", + booktitle = "{Proceedings of the 33rd International Conference on High + Energy Physics (ICHEP 06): Moscow, Russia, July 26-August + 2, 2006}", + collaboration = "BaBar", + journal = "Phys. Rev. Lett.", + volume = "98", + year = "2007", + pages = "212001", + doi = "10.1103/PhysRevLett.98.212001", + eprint = "hep-ex/0610057", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-12155, BABAR-PUB-06-38", + SLACcitation = "%%CITATION = HEP-EX/0610057;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2007_I729388.plot b/analyses/pluginBABAR/BABAR_2007_I729388.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I729388.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BABAR_2007_I729388/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\psi(2S))$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\psi(2S))$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2007_I729388.yoda b/analyses/pluginBABAR/BABAR_2007_I729388.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I729388.yoda @@ -0,0 +1,46 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I729388/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {3: {error: {dn: -10.0, up: 27.0}, 'sys,Overall additional systematic uncertainty.': {dn: -1.353, up: 1.353}}, 4: {error: {dn: -8.0, up: 22.0}, 'sys,Overall additional systematic uncertainty.': {dn: -1.107, up: 1.107}}, 5: {error: {dn: -11.0, up: 23.0}, 'sys,Overall additional systematic uncertainty.': {dn: -2.091, up: 2.091}}, 6: {error: {dn: -10.0, up: 20.0}, 'sys,Overall additional systematic uncertainty.': {dn: -1.845, up: 1.845}}, 7: {error: {dn: -17.0, up: 26.0}, 'sys,Overall additional systematic uncertainty.': {dn: -5.412, up: 5.412}}, 8: {error: {dn: -20.0, up: 28.0}, 'sys,Overall additional systematic uncertainty.': {dn: -7.503, up: 7.503}}, 9: {error: {dn: -15.0, up: 23.0}, 'sys,Overall additional systematic uncertainty.': {dn: -4.674, up: 4.674}}, 10: {error: {dn: -8.0, up: 16.0}, 'sys,Overall additional systematic uncertainty.': {dn: -1.476, up: 1.476}}, 12: {error: {dn: -9.0, up: 16.0}, 'sys,Overall additional systematic uncertainty.': {dn: -1.9680000000000002, up: 1.9680000000000002}}, 13: {error: {dn: -4.0, up: 12.0}, 'sys,Overall additional systematic uncertainty.': {dn: -0.6150000000000001, up: 0.6150000000000001}}, 14: {error: {dn: -13.0, up: 19.0}, 'sys,Overall additional systematic uncertainty.': {dn: -4.305, up: 4.305}}, 15: {error: {dn: -4.0, up: 11.0}, 'sys,Overall additional systematic uncertainty.': {dn: -0.49200000000000005, up: 0.49200000000000005}}, 16: {error: {dn: -8.0, up: 14.0}, 'sys,Overall additional systematic uncertainty.': {dn: -1.7220000000000002, up: 1.7220000000000002}}, 17: {error: {dn: -3.7, up: 10.4}, 'sys,Overall additional systematic uncertainty.': {dn: -0.4551000000000001, up: 0.4551000000000001}}, 18: {error: {dn: -3.6, up: 10.1}, 'sys,Overall additional systematic uncertainty.': {dn: -0.4551000000000001, up: 0.4551000000000001}}, 19: {error: {dn: -6.0, up: 11.0}, 'sys,Overall additional systematic uncertainty.': {dn: -0.9840000000000001, up: 0.9840000000000001}}, 20: {error: {dn: -7.0, up: 12.0}, 'sys,Overall additional systematic uncertainty.': {dn: -1.476, up: 1.476}}, 23: {error: {dn: -5.0, up: 10.0}, 'sys,Overall additional systematic uncertainty.': {dn: -0.8610000000000001, up: 0.8610000000000001}}, 24: {error: {dn: -3.0, up: 8.2}, 'sys,Overall additional systematic uncertainty.': {dn: -0.38130000000000003, up: 0.38130000000000003}}, 25: {error: {dn: -4.0, up: 9.0}, 'sys,Overall additional systematic uncertainty.': {dn: -0.738, up: 0.738}}, 27: {error: {dn: -2.7, up: 7.6}, 'sys,Overall additional systematic uncertainty.': {dn: -0.3444, up: 0.3444}}, 29: {error: {dn: -5.0, up: 9.0}, 'sys,Overall additional systematic uncertainty.': {dn: -1.107, up: 1.107}}, 30: {error: {dn: -4.0, up: 8.0}, 'sys,Overall additional systematic uncertainty.': {dn: -0.6150000000000001, up: 0.6150000000000001}}, 32: {error: {dn: -2.3, up: 6.3}, 'sys,Overall additional systematic uncertainty.': {dn: -0.2952, up: 0.2952}}, 33: {error: {dn: -3.0, up: 7.0}, 'sys,Overall additional systematic uncertainty.': {dn: -0.6150000000000001, up: 0.6150000000000001}}, 34: {error: {dn: -4.0, up: 8.0}, 'sys,Overall additional systematic uncertainty.': {dn: -0.9840000000000001, up: 0.9840000000000001}}, 43: {error: {dn: -1.7, up: 4.7}, 'sys,Overall additional systematic uncertainty.': {dn: -0.22140000000000004, up: 0.22140000000000004}}, 48: {error: {dn: -2.3, up: 4.7}, 'sys,Overall additional systematic uncertainty.': {dn: -0.41820000000000007, up: 0.41820000000000007}}, 51: {error: {dn: -1.4, up: 3.9}, 'sys,Overall additional systematic uncertainty.': {dn: -0.1968, up: 0.1968}}, 54: {error: {dn: -1.3, up: 3.6}, 'sys,Overall additional systematic uncertainty.': {dn: -0.1845, up: 0.1845}}, 57: {error: {dn: -1.2, up: 3.3}, 'sys,Overall additional systematic uncertainty.': {dn: -0.15990000000000001, up: 0.15990000000000001}}, 61: {error: {dn: -1.0, up: 2.9}, 'sys,Overall additional systematic uncertainty.': {dn: -0.1476, up: 0.1476}}, 63: {error: {dn: -1.0, up: 2.7}, 'sys,Overall additional systematic uncertainty.': {dn: -0.13530000000000003, up: 0.13530000000000003}}, 67: {error: {dn: -0.9, up: 2.4}, 'sys,Overall additional systematic uncertainty.': {dn: -0.12300000000000001, up: 0.12300000000000001}}, 70: {error: {dn: -0.8, up: 2.2}, 'sys,Overall additional systematic uncertainty.': {dn: -0.11070000000000002, up: 0.11070000000000002}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I729388/d01-x01-y01 +Title: doi:10.17182/hepdata.19344.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.135000e+00 2.500000e-02 2.500000e-02 1.100000e+01 1.009112e+01 2.703388e+01 +4.185000e+00 2.500000e-02 2.500000e-02 9.000000e+00 8.076227e+00 2.202783e+01 +4.235000e+00 2.500000e-02 2.500000e-02 1.700000e+01 1.119698e+01 2.309485e+01 +4.285000e+00 2.500000e-02 2.500000e-02 1.500000e+01 1.016878e+01 2.008492e+01 +4.335000e+00 2.500000e-02 2.500000e-02 4.400000e+01 1.784068e+01 2.655729e+01 +4.385000e+00 2.500000e-02 2.500000e-02 6.100000e+01 2.136106e+01 2.898784e+01 +4.435000e+00 2.500000e-02 2.500000e-02 3.800000e+01 1.571134e+01 2.347011e+01 +4.485000e+00 2.500000e-02 2.500000e-02 1.200000e+01 8.135022e+00 1.606794e+01 +4.585000e+00 2.500000e-02 2.500000e-02 1.600000e+01 9.212656e+00 1.612058e+01 +4.635000e+00 2.500000e-02 2.500000e-02 5.000000e+00 4.047002e+00 1.201575e+01 +4.685000e+00 2.500000e-02 2.500000e-02 3.500000e+01 1.369427e+01 1.948161e+01 +4.735000e+00 2.500000e-02 2.500000e-02 4.000000e+00 4.030144e+00 1.101100e+01 +4.785000e+00 2.500000e-02 2.500000e-02 1.400000e+01 8.183232e+00 1.410551e+01 +4.835000e+00 2.500000e-02 2.500000e-02 3.700000e+00 3.727884e+00 1.040995e+01 +4.885000e+00 2.500000e-02 2.500000e-02 3.700000e+00 3.628652e+00 1.011025e+01 +4.935000e+00 2.500000e-02 2.500000e-02 8.000000e+00 6.080153e+00 1.104392e+01 +4.985000e+00 2.500000e-02 2.500000e-02 1.200000e+01 7.153920e+00 1.209043e+01 +5.135000e+00 2.500000e-02 2.500000e-02 7.000000e+00 5.073591e+00 1.003700e+01 +5.185000e+00 2.500000e-02 2.500000e-02 3.100000e+00 3.024135e+00 8.208860e+00 +5.235000e+00 2.500000e-02 2.500000e-02 6.000000e+00 4.067511e+00 9.030207e+00 +5.335000e+00 2.500000e-02 2.500000e-02 2.800000e+00 2.721876e+00 7.607799e+00 +5.435000e+00 2.500000e-02 2.500000e-02 9.000000e+00 5.121079e+00 9.067825e+00 +5.485000e+00 2.500000e-02 2.500000e-02 5.000000e+00 4.047002e+00 8.023604e+00 +5.585000e+00 2.500000e-02 2.500000e-02 2.400000e+00 2.318867e+00 6.306912e+00 +5.635000e+00 2.500000e-02 2.500000e-02 5.000000e+00 3.062389e+00 7.026964e+00 +5.685000e+00 2.500000e-02 2.500000e-02 8.000000e+00 4.119254e+00 8.060289e+00 +6.135000e+00 2.500000e-02 2.500000e-02 1.800000e+00 1.714356e+00 4.705212e+00 +6.385000e+00 2.500000e-02 2.500000e-02 3.400000e+00 2.337711e+00 4.718569e+00 +6.535000e+00 2.500000e-02 2.500000e-02 1.600000e+00 1.413765e+00 3.904962e+00 +6.685000e+00 2.500000e-02 2.500000e-02 1.500000e+00 1.313027e+00 3.604725e+00 +6.835000e+00 2.500000e-02 2.500000e-02 1.300000e+00 1.210606e+00 3.303872e+00 +7.035000e+00 2.500000e-02 2.500000e-02 1.200000e+00 1.010834e+00 2.903754e+00 +7.135000e+00 2.500000e-02 2.500000e-02 1.100000e+00 1.009112e+00 2.703388e+00 +7.335000e+00 2.500000e-02 2.500000e-02 1.000000e+00 9.083661e-01 2.403150e+00 +7.485000e+00 2.500000e-02 2.500000e-02 9.000000e-01 8.076227e-01 2.202783e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2007_I747875.cc b/analyses/pluginBABAR/BABAR_2007_I747875.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I747875.cc @@ -0,0 +1,210 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2007_I747875 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2007_I747875); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + _cKpKmpippim = bookCounter("TMP/KpKmpippim"); + _cKstarKpi = bookCounter("TMP/KstarKpi"); + _cphipippim = bookCounter("TMP/phipippim"); + _cphif0 = bookCounter("TMP/phif0"); + _cKpKmpi0pi0 = bookCounter("TMP/KpKmpi0pi0"); + _cphif0pi0pi0 = bookCounter("TMP/phif0pi0pi0"); + _c2Kp2Km = bookCounter("TMP/2Kp2Km"); + + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // K*0 + if(abs(p.pdgId())==313) { + map nRes=nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // K* K+/- pi-/+ + if(ncount !=2 ) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==321 || abs(val.first)==211) { + continue; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched==false) continue; + if((nCount[321] == 1 && nCount[-321] ==0 && + nCount[211] == 0 && nCount[-211] == 1) || + (nCount[321] == 0 && nCount[-321] ==1 && + nCount[211] == 1 && nCount[-211] == 0)) + _cKstarKpi->fill(event.weight()); + } + else if(p.pdgId()==333) { + map nRes=nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // phi pi+pi- + if(ncount==2) { + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _cphipippim->fill(event.weight()); + } + foreach (const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=9010221) continue; + if(p2.parents()[0].isSame(p)) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=0) continue; + bool matched2 = true; + for(auto const & val : nResB) { + if(val.second!=0) { + matched2 = false; + break; + } + } + if(matched2) { + _cphif0pi0pi0->fill(event.weight()); + _cphif0 ->fill(event.weight()); + } + } + } + } + if(ntotal==4) { + if(nCount[321]==1 && nCount[-321]==1 && nCount[211]==1 && nCount[-211]==1) + _cKpKmpippim->fill(event.weight()); + else if( nCount[321]==1 && nCount[-321]==1 && nCount[111]==2) + _cKpKmpi0pi0->fill(event.weight()); + else if( nCount[321]==2 && nCount[-321]==2) + _c2Kp2Km->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1; ix<8; ++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _cKpKmpippim->val(); + error = _cKpKmpippim->err(); + } + else if(ix==2) { + sigma = _cKstarKpi->val(); + error = _cKstarKpi->err(); + } + else if(ix==3) { + sigma = _cphipippim->val(); + error = _cphipippim->err(); + } + else if(ix==4) { + sigma = _cphif0->val(); + error = _cphif0->err(); + } + else if(ix==5) { + sigma = _cKpKmpi0pi0->val(); + error = _cKpKmpi0pi0->err(); + } + else if(ix==6) { + sigma = _cphif0pi0pi0->val(); + error = _cphif0pi0pi0->err(); + } + else if(ix==7) { + sigma = _c2Kp2Km->val(); + error = _c2Kp2Km->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _cKpKmpippim, _cKstarKpi, _cphipippim, + _cphif0, _cKpKmpi0pi0, _cphif0pi0pi0, _c2Kp2Km; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2007_I747875); + + +} diff --git a/analyses/pluginBABAR/BABAR_2007_I747875.info b/analyses/pluginBABAR/BABAR_2007_I747875.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I747875.info @@ -0,0 +1,36 @@ +Name: BABAR_2007_I747875 +Year: 2007 +Summary: $e^+e^- \to$ $K^+K^-\pi^+\pi^-$, $K^+K^-\pi^0\pi^0$ and $K^+K^-K^+K^-$ cross-sections between 1.4 and 4 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 747875 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D76 (2007) 012008, 2007 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^- \to$ $K^+K^-\pi^+\pi^-$, $K^+K^-\pi^0\pi^0$ and $K^+K^-K^+K^-$ via radiative return, + including the identification of $K^{*0}$, $\phi$ and $f_0(980)$ mesons for energies between 1.4 and 4. GeV' +Keywords: +BibKey: Aubert:2007ur +BibTeX: '@article{Aubert:2007ur, + author = "Aubert, Bernard and others", + title = "{The e+ e- ---> K+ K- pi+ pi-, K+ K- pi0 pi0 and K+ K- K+ + K- cross-sections measured with initial-state radiation}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D76", + year = "2007", + pages = "012008", + doi = "10.1103/PhysRevD.76.012008", + eprint = "0704.0630", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-12435, BABAR-PUB-07-021", + SLACcitation = "%%CITATION = ARXIV:0704.0630;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2007_I747875.plot b/analyses/pluginBABAR/BABAR_2007_I747875.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I747875.plot @@ -0,0 +1,48 @@ +BEGIN PLOT /BABAR_2007_I747875/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I747875/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^{*0}K^+\pi^-+{\rm c.c.})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^{*0}K^+\pi^-+{\rm c.c.})$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I747875/d03-x01-y01 +Title=$\sigma(e^+e^-\to \phi\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I747875/d04-x01-y01 +Title=$\sigma(e^+e^-\to \phi f_0(980))$ extracted from $f_0\to\pi^+\pi^-$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi f_0(980))$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I747875/d05-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\pi^0\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^0\pi^0)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I747875/d06-x01-y01 +Title=$\sigma(e^+e^-\to \phi f_0(980))$ extracted from $f_0\to\pi^0\pi^0$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi f_0(980))$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I747875/d07-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-K^+K^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2007_I747875.yoda b/analyses/pluginBABAR/BABAR_2007_I747875.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I747875.yoda @@ -0,0 +1,567 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I747875/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.02, up: 0.02}}, 1: {error: {dn: -0.02, up: 0.02}}, 2: {error: {dn: -0.02, up: 0.02}}, 3: {error: {dn: -0.02, up: 0.02}}, 4: {error: {dn: -0.02, up: 0.02}}, 5: {error: {dn: -0.03, up: 0.03}}, 6: {error: {dn: -0.04, up: 0.04}}, 7: {error: {dn: -0.05, up: 0.05}}, 8: {error: {dn: -0.06, up: 0.06}}, 9: {error: {dn: -0.08, up: 0.08}}, 10: {error: {dn: -0.1, up: 0.1}}, 11: {error: {dn: -0.11, up: 0.11}}, 12: {error: {dn: -0.13, up: 0.13}}, 13: {error: {dn: -0.13, up: 0.13}}, 14: {error: {dn: -0.15, up: 0.15}}, 15: {error: {dn: -0.16, up: 0.16}}, 16: {error: {dn: -0.16, up: 0.16}}, 17: {error: {dn: -0.17, up: 0.17}}, 18: {error: {dn: -0.17, up: 0.17}}, 19: {error: {dn: -0.17, up: 0.17}}, 20: {error: {dn: -0.16, up: 0.16}}, 21: {error: {dn: -0.16, up: 0.16}}, 22: {error: {dn: -0.16, up: 0.16}}, 23: {error: {dn: -0.15, up: 0.15}}, 24: {error: {dn: -0.15, up: 0.15}}, 25: {error: {dn: -0.14, up: 0.14}}, 26: {error: {dn: -0.14, up: 0.14}}, 27: {error: {dn: -0.14, up: 0.14}}, 28: {error: {dn: -0.14, up: 0.14}}, 29: {error: {dn: -0.13, up: 0.13}}, 30: {error: {dn: -0.12, up: 0.12}}, 31: {error: {dn: -0.12, up: 0.12}}, 32: {error: {dn: -0.1, up: 0.1}}, 33: {error: {dn: -0.1, up: 0.1}}, 34: {error: {dn: -0.09, up: 0.09}}, 35: {error: {dn: -0.09, up: 0.09}}, 36: {error: {dn: -0.09, up: 0.09}}, 37: {error: {dn: -0.09, up: 0.09}}, 38: {error: {dn: -0.09, up: 0.09}}, 39: {error: {dn: -0.09, up: 0.09}}, 40: {error: {dn: -0.09, up: 0.09}}, 41: {error: {dn: -0.09, up: 0.09}}, 42: {error: {dn: -0.08, up: 0.08}}, 43: {error: {dn: -0.08, up: 0.08}}, 44: {error: {dn: -0.08, up: 0.08}}, 45: {error: {dn: -0.07, up: 0.07}}, 46: {error: {dn: -0.07, up: 0.07}}, 47: {error: {dn: -0.07, up: 0.07}}, 48: {error: {dn: -0.07, up: 0.07}}, 49: {error: {dn: -0.07, up: 0.07}}, 50: {error: {dn: -0.06, up: 0.06}}, 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/REF/BABAR_2007_I747875/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.11, up: 0.11}}, 1: {error: {dn: -0.08, up: 0.08}}, 2: {error: {dn: -0.13, up: 0.13}}, 3: {error: {dn: -0.12, up: 0.12}}, 4: {error: {dn: -0.15, up: 0.15}}, 5: {error: {dn: -0.15, up: 0.15}}, 6: {error: {dn: -0.14, up: 0.14}}, 7: {error: {dn: -0.17, up: 0.17}}, 8: {error: {dn: -0.2, up: 0.2}}, 9: {error: {dn: -0.21, up: 0.21}}, 10: {error: {dn: -0.2, up: 0.2}}, 11: {error: {dn: -0.2, up: 0.2}}, 12: {error: {dn: -0.23, up: 0.23}}, 13: {error: {dn: -0.2, up: 0.2}}, 14: {error: {dn: -0.2, up: 0.2}}, 15: {error: {dn: -0.21, up: 0.21}}, 16: {error: {dn: -0.18, up: 0.18}}, 17: {error: {dn: -0.17, up: 0.17}}, 18: {error: {dn: -0.16, up: 0.16}}, 19: {error: {dn: -0.16, up: 0.16}}, 20: {error: {dn: -0.16, up: 0.16}}, 21: {error: {dn: -0.16, up: 0.16}}, 22: {error: {dn: -0.14, up: 0.14}}, 23: {error: {dn: -0.15, up: 0.15}}, 24: {error: {dn: -0.14, up: 0.14}}, 25: {error: {dn: -0.11, up: 0.11}}, 26: {error: {dn: -0.1, up: 0.1}}, 27: {error: {dn: -0.11, up: 0.11}}, 28: {error: {dn: -0.1, up: 0.1}}, 29: {error: {dn: -0.09, up: 0.09}}, 30: {error: {dn: -0.11, up: 0.11}}, 31: {error: {dn: -0.09, up: 0.09}}, 32: {error: {dn: -0.09, up: 0.09}}, 33: {error: {dn: -0.09, up: 0.09}}, 34: {error: {dn: -0.09, up: 0.09}}, 35: {error: {dn: -0.08, up: 0.08}}, 36: {error: {dn: -0.09, up: 0.09}}, 37: {error: {dn: -0.07, up: 0.07}}, 38: {error: {dn: -0.07, up: 0.07}}, 39: {error: {dn: -0.07, up: 0.07}}, 40: {error: {dn: -0.07, up: 0.07}}, 41: {error: {dn: -0.06, up: 0.06}}, 42: {error: {dn: -0.06, up: 0.06}}, 43: {error: {dn: -0.06, up: 0.06}}, 44: {error: {dn: -0.06, up: 0.06}}, 45: {error: {dn: -0.06, up: 0.06}}, 46: {error: {dn: -0.06, up: 0.06}}, 47: {error: {dn: -0.06, up: 0.06}}, 48: {error: {dn: -0.06, up: 0.06}}, 49: {error: {dn: -0.05, up: 0.05}}, 50: {error: {dn: -0.05, up: 0.05}}, 51: {error: {dn: -0.04, up: 0.04}}, 52: {error: {dn: -0.05, up: 0.05}}, 53: {error: {dn: -0.05, up: 0.05}}, 54: {error: {dn: -0.04, up: 0.04}}, 55: {error: {dn: -0.04, up: 0.04}}, 56: {error: {dn: -0.05, up: 0.05}}, 57: {error: {dn: -0.04, up: 0.04}}, 58: {error: {dn: -0.04, up: 0.04}}, 59: {error: {dn: -0.04, up: 0.04}}, 60: {error: {dn: -0.1, up: 0.1}}, 61: {error: {dn: -0.07, up: 0.07}}, 62: {error: {dn: -0.04, up: 0.04}}, 63: {error: {dn: -0.04, up: 0.04}}, 64: {error: {dn: -0.03, up: 0.03}}, 65: {error: {dn: -0.03, up: 0.03}}, 66: {error: {dn: -0.04, up: 0.04}}, 67: {error: {dn: -0.03, up: 0.03}}, 68: {error: {dn: -0.03, up: 0.03}}, 69: {error: {dn: -0.03, up: 0.03}}, 70: {error: {dn: -0.03, up: 0.03}}, 71: {error: {dn: -0.06, up: 0.06}}, 72: {error: {dn: -0.03, up: 0.03}}, 73: {error: {dn: -0.03, up: 0.03}}, 74: {error: {dn: -0.03, up: 0.03}}, 75: {error: {dn: -0.05, up: 0.05}}, 76: {error: {dn: -0.03, up: 0.03}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I747875/d02-x01-y01 +Title: doi:10.17182/hepdata.50373.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.587500e+00 1.250000e-02 1.250000e-02 1.600000e-01 1.100000e-01 1.100000e-01 +1.612500e+00 1.250000e-02 1.250000e-02 3.100000e-01 8.000000e-02 8.000000e-02 +1.637500e+00 1.250000e-02 1.250000e-02 8.100000e-01 1.300000e-01 1.300000e-01 +1.662500e+00 1.250000e-02 1.250000e-02 7.900000e-01 1.200000e-01 1.200000e-01 +1.687500e+00 1.250000e-02 1.250000e-02 1.330000e+00 1.500000e-01 1.500000e-01 +1.712500e+00 1.250000e-02 1.250000e-02 1.630000e+00 1.500000e-01 1.500000e-01 +1.737500e+00 1.250000e-02 1.250000e-02 1.870000e+00 1.400000e-01 1.400000e-01 +1.762500e+00 1.250000e-02 1.250000e-02 2.120000e+00 1.700000e-01 1.700000e-01 +1.787500e+00 1.250000e-02 1.250000e-02 2.510000e+00 2.000000e-01 2.000000e-01 +1.812500e+00 1.250000e-02 1.250000e-02 2.960000e+00 2.100000e-01 2.100000e-01 +1.837500e+00 1.250000e-02 1.250000e-02 4.350000e+00 2.000000e-01 2.000000e-01 +1.862500e+00 1.250000e-02 1.250000e-02 4.110000e+00 2.000000e-01 2.000000e-01 +1.887500e+00 1.250000e-02 1.250000e-02 3.260000e+00 2.300000e-01 2.300000e-01 +1.912500e+00 1.250000e-02 1.250000e-02 3.900000e+00 2.000000e-01 2.000000e-01 +1.937500e+00 1.250000e-02 1.250000e-02 3.530000e+00 2.000000e-01 2.000000e-01 +1.962500e+00 1.250000e-02 1.250000e-02 3.420000e+00 2.100000e-01 2.100000e-01 +1.987500e+00 1.250000e-02 1.250000e-02 2.810000e+00 1.800000e-01 1.800000e-01 +2.012500e+00 1.250000e-02 1.250000e-02 2.470000e+00 1.700000e-01 1.700000e-01 +2.037500e+00 1.250000e-02 1.250000e-02 2.260000e+00 1.600000e-01 1.600000e-01 +2.062500e+00 1.250000e-02 1.250000e-02 2.000000e+00 1.600000e-01 1.600000e-01 +2.087500e+00 1.250000e-02 1.250000e-02 2.360000e+00 1.600000e-01 1.600000e-01 +2.112500e+00 1.250000e-02 1.250000e-02 1.920000e+00 1.600000e-01 1.600000e-01 +2.137500e+00 1.250000e-02 1.250000e-02 1.990000e+00 1.400000e-01 1.400000e-01 +2.162500e+00 1.250000e-02 1.250000e-02 1.190000e+00 1.500000e-01 1.500000e-01 +2.187500e+00 1.250000e-02 1.250000e-02 1.240000e+00 1.400000e-01 1.400000e-01 +2.212500e+00 1.250000e-02 1.250000e-02 1.250000e+00 1.100000e-01 1.100000e-01 +2.237500e+00 1.250000e-02 1.250000e-02 9.000000e-01 1.000000e-01 1.000000e-01 +2.262500e+00 1.250000e-02 1.250000e-02 7.900000e-01 1.100000e-01 1.100000e-01 +2.287500e+00 1.250000e-02 1.250000e-02 1.150000e+00 1.000000e-01 1.000000e-01 +2.312500e+00 1.250000e-02 1.250000e-02 9.900000e-01 9.000000e-02 9.000000e-02 +2.337500e+00 1.250000e-02 1.250000e-02 9.100000e-01 1.100000e-01 1.100000e-01 +2.362500e+00 1.250000e-02 1.250000e-02 1.110000e+00 9.000000e-02 9.000000e-02 +2.387500e+00 1.250000e-02 1.250000e-02 8.300000e-01 9.000000e-02 9.000000e-02 +2.412500e+00 1.250000e-02 1.250000e-02 8.700000e-01 9.000000e-02 9.000000e-02 +2.437500e+00 1.250000e-02 1.250000e-02 1.000000e+00 9.000000e-02 9.000000e-02 +2.462500e+00 1.250000e-02 1.250000e-02 8.600000e-01 8.000000e-02 8.000000e-02 +2.487500e+00 1.250000e-02 1.250000e-02 8.800000e-01 9.000000e-02 9.000000e-02 +2.512500e+00 1.250000e-02 1.250000e-02 6.900000e-01 7.000000e-02 7.000000e-02 +2.537500e+00 1.250000e-02 1.250000e-02 6.200000e-01 7.000000e-02 7.000000e-02 +2.562500e+00 1.250000e-02 1.250000e-02 5.500000e-01 7.000000e-02 7.000000e-02 +2.587500e+00 1.250000e-02 1.250000e-02 5.400000e-01 7.000000e-02 7.000000e-02 +2.612500e+00 1.250000e-02 1.250000e-02 6.300000e-01 6.000000e-02 6.000000e-02 +2.637500e+00 1.250000e-02 1.250000e-02 5.700000e-01 6.000000e-02 6.000000e-02 +2.662500e+00 1.250000e-02 1.250000e-02 4.600000e-01 6.000000e-02 6.000000e-02 +2.687500e+00 1.250000e-02 1.250000e-02 4.600000e-01 6.000000e-02 6.000000e-02 +2.712500e+00 1.250000e-02 1.250000e-02 6.400000e-01 6.000000e-02 6.000000e-02 +2.737500e+00 1.250000e-02 1.250000e-02 5.600000e-01 6.000000e-02 6.000000e-02 +2.762500e+00 1.250000e-02 1.250000e-02 4.600000e-01 6.000000e-02 6.000000e-02 +2.787500e+00 1.250000e-02 1.250000e-02 3.600000e-01 6.000000e-02 6.000000e-02 +2.812500e+00 1.250000e-02 1.250000e-02 3.100000e-01 5.000000e-02 5.000000e-02 +2.837500e+00 1.250000e-02 1.250000e-02 3.500000e-01 5.000000e-02 5.000000e-02 +2.862500e+00 1.250000e-02 1.250000e-02 2.700000e-01 4.000000e-02 4.000000e-02 +2.887500e+00 1.250000e-02 1.250000e-02 2.700000e-01 5.000000e-02 5.000000e-02 +2.912500e+00 1.250000e-02 1.250000e-02 3.400000e-01 5.000000e-02 5.000000e-02 +2.937500e+00 1.250000e-02 1.250000e-02 2.900000e-01 4.000000e-02 4.000000e-02 +2.962500e+00 1.250000e-02 1.250000e-02 2.500000e-01 4.000000e-02 4.000000e-02 +2.987500e+00 1.250000e-02 1.250000e-02 3.800000e-01 5.000000e-02 5.000000e-02 +3.012500e+00 1.250000e-02 1.250000e-02 2.100000e-01 4.000000e-02 4.000000e-02 +3.037500e+00 1.250000e-02 1.250000e-02 2.400000e-01 4.000000e-02 4.000000e-02 +3.062500e+00 1.250000e-02 1.250000e-02 2.200000e-01 4.000000e-02 4.000000e-02 +3.087500e+00 1.250000e-02 1.250000e-02 1.730000e+00 1.000000e-01 1.000000e-01 +3.112500e+00 1.250000e-02 1.250000e-02 9.200000e-01 7.000000e-02 7.000000e-02 +3.137500e+00 1.250000e-02 1.250000e-02 2.100000e-01 4.000000e-02 4.000000e-02 +3.162500e+00 1.250000e-02 1.250000e-02 2.400000e-01 4.000000e-02 4.000000e-02 +3.187500e+00 1.250000e-02 1.250000e-02 8.000000e-02 3.000000e-02 3.000000e-02 +3.212500e+00 1.250000e-02 1.250000e-02 1.500000e-01 3.000000e-02 3.000000e-02 +3.237500e+00 1.250000e-02 1.250000e-02 1.400000e-01 4.000000e-02 4.000000e-02 +3.262500e+00 1.250000e-02 1.250000e-02 1.600000e-01 3.000000e-02 3.000000e-02 +3.287500e+00 1.250000e-02 1.250000e-02 1.300000e-01 3.000000e-02 3.000000e-02 +3.312500e+00 1.250000e-02 1.250000e-02 1.200000e-01 3.000000e-02 3.000000e-02 +3.337500e+00 1.250000e-02 1.250000e-02 1.400000e-01 3.000000e-02 3.000000e-02 +3.362500e+00 1.250000e-02 1.250000e-02 1.200000e-01 6.000000e-02 6.000000e-02 +3.387500e+00 1.250000e-02 1.250000e-02 9.000000e-02 3.000000e-02 3.000000e-02 +3.412500e+00 1.250000e-02 1.250000e-02 1.000000e-01 3.000000e-02 3.000000e-02 +3.437500e+00 1.250000e-02 1.250000e-02 1.100000e-01 3.000000e-02 3.000000e-02 +3.462500e+00 1.250000e-02 1.250000e-02 1.000000e-01 5.000000e-02 5.000000e-02 +3.487500e+00 1.250000e-02 1.250000e-02 8.000000e-02 3.000000e-02 3.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I747875/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.02, up: 0.02}}, 1: {error: {dn: -0.03, up: 0.03}}, 2: {error: {dn: -0.04, up: 0.04}}, 3: {error: {dn: -0.04, up: 0.04}}, 4: {error: {dn: -0.06, up: 0.06}}, 5: {error: {dn: -0.06, up: 0.06}}, 6: {error: {dn: -0.08, up: 0.08}}, 7: {error: {dn: -0.09, up: 0.09}}, 8: {error: {dn: -0.1, up: 0.1}}, 9: {error: {dn: -0.09, up: 0.09}}, 10: {error: {dn: -0.1, up: 0.1}}, 11: {error: {dn: -0.11, up: 0.11}}, 12: {error: {dn: -0.11, up: 0.11}}, 13: {error: {dn: -0.09, up: 0.09}}, 14: {error: {dn: -0.1, up: 0.1}}, 15: {error: {dn: -0.1, up: 0.1}}, 16: {error: {dn: -0.08, up: 0.08}}, 17: {error: {dn: -0.09, up: 0.09}}, 18: {error: {dn: -0.08, up: 0.08}}, 19: {error: {dn: -0.08, up: 0.08}}, 20: {error: {dn: -0.07, up: 0.07}}, 21: {error: {dn: -0.07, up: 0.07}}, 22: {error: {dn: -0.07, up: 0.07}}, 23: {error: {dn: -0.07, up: 0.07}}, 24: {error: {dn: -0.06, up: 0.06}}, 25: {error: {dn: -0.07, up: 0.07}}, 26: {error: {dn: -0.06, up: 0.06}}, 27: {error: {dn: -0.07, up: 0.07}}, 28: {error: {dn: -0.06, up: 0.06}}, 29: {error: {dn: -0.05, up: 0.05}}, 30: {error: {dn: -0.04, up: 0.04}}, 31: {error: {dn: -0.03, up: 0.03}}, 32: {error: {dn: -0.04, up: 0.04}}, 33: {error: {dn: -0.03, up: 0.03}}, 34: {error: {dn: -0.03, up: 0.03}}, 35: {error: {dn: -0.04, up: 0.04}}, 36: {error: {dn: -0.04, up: 0.04}}, 37: {error: {dn: -0.04, up: 0.04}}, 38: {error: {dn: -0.04, up: 0.04}}, 39: {error: {dn: -0.03, up: 0.03}}, 40: {error: {dn: -0.03, up: 0.03}}, 41: {error: {dn: -0.03, up: 0.03}}, 42: {error: {dn: -0.03, up: 0.03}}, 43: {error: {dn: -0.02, up: 0.02}}, 44: {error: {dn: -0.02, up: 0.02}}, 45: {error: {dn: -0.02, up: 0.02}}, 46: {error: {dn: -0.03, up: 0.03}}, 47: {error: {dn: -0.02, up: 0.02}}, 48: {error: {dn: -0.02, up: 0.02}}, 49: {error: {dn: -0.03, up: 0.03}}, 50: {error: {dn: -0.02, up: 0.02}}, 51: {error: {dn: -0.02, up: 0.02}}, 52: {error: {dn: -0.02, up: 0.02}}, 53: {error: {dn: -0.02, up: 0.02}}, 54: {error: {dn: -0.02, up: 0.02}}, 55: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I747875/d03-x01-y01 +Title: doi:10.17182/hepdata.50373.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.487500e+00 1.250000e-02 1.250000e-02 1.000000e-02 2.000000e-02 2.000000e-02 +1.512500e+00 1.250000e-02 1.250000e-02 3.000000e-02 3.000000e-02 3.000000e-02 +1.537500e+00 1.250000e-02 1.250000e-02 9.000000e-02 4.000000e-02 4.000000e-02 +1.562500e+00 1.250000e-02 1.250000e-02 1.300000e-01 4.000000e-02 4.000000e-02 +1.587500e+00 1.250000e-02 1.250000e-02 2.100000e-01 6.000000e-02 6.000000e-02 +1.612500e+00 1.250000e-02 1.250000e-02 2.300000e-01 6.000000e-02 6.000000e-02 +1.637500e+00 1.250000e-02 1.250000e-02 5.400000e-01 8.000000e-02 8.000000e-02 +1.662500e+00 1.250000e-02 1.250000e-02 6.100000e-01 9.000000e-02 9.000000e-02 +1.687500e+00 1.250000e-02 1.250000e-02 6.400000e-01 1.000000e-01 1.000000e-01 +1.712500e+00 1.250000e-02 1.250000e-02 3.800000e-01 9.000000e-02 9.000000e-02 +1.737500e+00 1.250000e-02 1.250000e-02 6.400000e-01 1.000000e-01 1.000000e-01 +1.762500e+00 1.250000e-02 1.250000e-02 5.500000e-01 1.100000e-01 1.100000e-01 +1.787500e+00 1.250000e-02 1.250000e-02 5.500000e-01 1.100000e-01 1.100000e-01 +1.812500e+00 1.250000e-02 1.250000e-02 3.100000e-01 9.000000e-02 9.000000e-02 +1.837500e+00 1.250000e-02 1.250000e-02 3.900000e-01 1.000000e-01 1.000000e-01 +1.862500e+00 1.250000e-02 1.250000e-02 4.400000e-01 1.000000e-01 1.000000e-01 +1.887500e+00 1.250000e-02 1.250000e-02 2.300000e-01 8.000000e-02 8.000000e-02 +1.912500e+00 1.250000e-02 1.250000e-02 3.400000e-01 9.000000e-02 9.000000e-02 +1.937500e+00 1.250000e-02 1.250000e-02 3.700000e-01 8.000000e-02 8.000000e-02 +1.962500e+00 1.250000e-02 1.250000e-02 3.100000e-01 8.000000e-02 8.000000e-02 +1.987500e+00 1.250000e-02 1.250000e-02 3.600000e-01 7.000000e-02 7.000000e-02 +2.012500e+00 1.250000e-02 1.250000e-02 3.800000e-01 7.000000e-02 7.000000e-02 +2.037500e+00 1.250000e-02 1.250000e-02 2.900000e-01 7.000000e-02 7.000000e-02 +2.062500e+00 1.250000e-02 1.250000e-02 4.200000e-01 7.000000e-02 7.000000e-02 +2.087500e+00 1.250000e-02 1.250000e-02 3.000000e-01 6.000000e-02 6.000000e-02 +2.112500e+00 1.250000e-02 1.250000e-02 4.900000e-01 7.000000e-02 7.000000e-02 +2.137500e+00 1.250000e-02 1.250000e-02 3.000000e-01 6.000000e-02 6.000000e-02 +2.162500e+00 1.250000e-02 1.250000e-02 4.900000e-01 7.000000e-02 7.000000e-02 +2.187500e+00 1.250000e-02 1.250000e-02 3.200000e-01 6.000000e-02 6.000000e-02 +2.212500e+00 1.250000e-02 1.250000e-02 2.200000e-01 5.000000e-02 5.000000e-02 +2.237500e+00 1.250000e-02 1.250000e-02 1.500000e-01 4.000000e-02 4.000000e-02 +2.262500e+00 1.250000e-02 1.250000e-02 1.000000e-01 3.000000e-02 3.000000e-02 +2.287500e+00 1.250000e-02 1.250000e-02 1.100000e-01 4.000000e-02 4.000000e-02 +2.312500e+00 1.250000e-02 1.250000e-02 8.000000e-02 3.000000e-02 3.000000e-02 +2.337500e+00 1.250000e-02 1.250000e-02 1.300000e-01 3.000000e-02 3.000000e-02 +2.362500e+00 1.250000e-02 1.250000e-02 1.000000e-01 4.000000e-02 4.000000e-02 +2.387500e+00 1.250000e-02 1.250000e-02 1.300000e-01 4.000000e-02 4.000000e-02 +2.412500e+00 1.250000e-02 1.250000e-02 1.200000e-01 4.000000e-02 4.000000e-02 +2.437500e+00 1.250000e-02 1.250000e-02 1.500000e-01 4.000000e-02 4.000000e-02 +2.462500e+00 1.250000e-02 1.250000e-02 6.000000e-02 3.000000e-02 3.000000e-02 +2.487500e+00 1.250000e-02 1.250000e-02 9.000000e-02 3.000000e-02 3.000000e-02 +2.512500e+00 1.250000e-02 1.250000e-02 9.000000e-02 3.000000e-02 3.000000e-02 +2.537500e+00 1.250000e-02 1.250000e-02 9.000000e-02 3.000000e-02 3.000000e-02 +2.562500e+00 1.250000e-02 1.250000e-02 3.000000e-02 2.000000e-02 2.000000e-02 +2.587500e+00 1.250000e-02 1.250000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +2.612500e+00 1.250000e-02 1.250000e-02 7.000000e-02 2.000000e-02 2.000000e-02 +2.637500e+00 1.250000e-02 1.250000e-02 8.000000e-02 3.000000e-02 3.000000e-02 +2.662500e+00 1.250000e-02 1.250000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +2.687500e+00 1.250000e-02 1.250000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +2.712500e+00 1.250000e-02 1.250000e-02 8.000000e-02 3.000000e-02 3.000000e-02 +2.737500e+00 1.250000e-02 1.250000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +2.762500e+00 1.250000e-02 1.250000e-02 7.000000e-02 2.000000e-02 2.000000e-02 +2.787500e+00 1.250000e-02 1.250000e-02 2.000000e-02 2.000000e-02 2.000000e-02 +2.812500e+00 1.250000e-02 1.250000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +2.837500e+00 1.250000e-02 1.250000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +2.862500e+00 1.250000e-02 1.250000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I747875/d04-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.02, up: 0.02}}, 1: {error: {dn: -0.04, up: 0.04}}, 2: {error: {dn: -0.07, up: 0.07}}, 3: {error: {dn: -0.07, up: 0.07}}, 4: {error: {dn: -0.07, up: 0.07}}, 5: {error: {dn: -0.07, up: 0.07}}, 6: {error: {dn: -0.07, up: 0.07}}, 7: {error: {dn: -0.08, up: 0.08}}, 8: {error: {dn: -0.07, up: 0.07}}, 9: {error: {dn: -0.09, up: 0.09}}, 10: {error: {dn: -0.08, up: 0.08}}, 11: {error: {dn: -0.08, up: 0.08}}, 12: {error: {dn: -0.07, up: 0.07}}, 13: {error: {dn: -0.06, up: 0.06}}, 14: {error: {dn: -0.05, up: 0.05}}, 15: {error: {dn: -0.04, up: 0.04}}, 16: {error: {dn: -0.05, up: 0.05}}, 17: {error: {dn: -0.04, up: 0.04}}, 18: {error: {dn: -0.04, up: 0.04}}, 19: {error: {dn: -0.05, up: 0.05}}, 20: {error: {dn: -0.04, up: 0.04}}, 21: {error: {dn: -0.05, up: 0.05}}, 22: {error: {dn: -0.04, up: 0.04}}, 23: {error: {dn: -0.04, up: 0.04}}, 24: {error: {dn: -0.03, up: 0.03}}, 25: {error: {dn: -0.03, up: 0.03}}, 26: {error: {dn: -0.03, up: 0.03}}, 27: {error: {dn: -0.02, up: 0.02}}, 28: {error: {dn: -0.03, up: 0.03}}, 29: {error: {dn: -0.03, up: 0.03}}, 30: {error: {dn: -0.03, up: 0.03}}, 31: {error: {dn: -0.03, up: 0.03}}, 32: {error: {dn: -0.02, up: 0.02}}, 33: {error: {dn: -0.02, up: 0.02}}, 34: {error: {dn: -0.01, up: 0.01}}, 35: {error: {dn: -0.02, up: 0.02}}, 36: {error: {dn: -0.02, up: 0.02}}, 37: {error: {dn: -0.02, up: 0.02}}, 38: {error: {dn: -0.02, up: 0.02}}, 39: {error: {dn: -0.02, up: 0.02}}, 40: {error: {dn: -0.01, up: 0.01}}, 41: {error: {dn: -0.01, up: 0.01}}, 42: {error: {dn: -0.0, up: 0.0}}, 43: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I747875/d04-x01-y01 +Title: doi:10.17182/hepdata.50373.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.887500e+00 1.250000e-02 1.250000e-02 2.000000e-02 2.000000e-02 2.000000e-02 +1.912500e+00 1.250000e-02 1.250000e-02 7.000000e-02 4.000000e-02 4.000000e-02 +1.937500e+00 1.250000e-02 1.250000e-02 3.000000e-01 7.000000e-02 7.000000e-02 +1.962500e+00 1.250000e-02 1.250000e-02 2.700000e-01 7.000000e-02 7.000000e-02 +1.987500e+00 1.250000e-02 1.250000e-02 2.500000e-01 7.000000e-02 7.000000e-02 +2.012500e+00 1.250000e-02 1.250000e-02 2.500000e-01 7.000000e-02 7.000000e-02 +2.037500e+00 1.250000e-02 1.250000e-02 2.800000e-01 7.000000e-02 7.000000e-02 +2.062500e+00 1.250000e-02 1.250000e-02 4.300000e-01 8.000000e-02 8.000000e-02 +2.087500e+00 1.250000e-02 1.250000e-02 2.800000e-01 7.000000e-02 7.000000e-02 +2.112500e+00 1.250000e-02 1.250000e-02 5.400000e-01 9.000000e-02 9.000000e-02 +2.137500e+00 1.250000e-02 1.250000e-02 4.600000e-01 8.000000e-02 8.000000e-02 +2.162500e+00 1.250000e-02 1.250000e-02 5.600000e-01 8.000000e-02 8.000000e-02 +2.187500e+00 1.250000e-02 1.250000e-02 3.800000e-01 7.000000e-02 7.000000e-02 +2.212500e+00 1.250000e-02 1.250000e-02 2.100000e-01 6.000000e-02 6.000000e-02 +2.237500e+00 1.250000e-02 1.250000e-02 1.700000e-01 5.000000e-02 5.000000e-02 +2.262500e+00 1.250000e-02 1.250000e-02 1.200000e-01 4.000000e-02 4.000000e-02 +2.287500e+00 1.250000e-02 1.250000e-02 1.300000e-01 5.000000e-02 5.000000e-02 +2.312500e+00 1.250000e-02 1.250000e-02 1.200000e-01 4.000000e-02 4.000000e-02 +2.337500e+00 1.250000e-02 1.250000e-02 1.400000e-01 4.000000e-02 4.000000e-02 +2.362500e+00 1.250000e-02 1.250000e-02 1.300000e-01 5.000000e-02 5.000000e-02 +2.387500e+00 1.250000e-02 1.250000e-02 1.300000e-01 4.000000e-02 4.000000e-02 +2.412500e+00 1.250000e-02 1.250000e-02 1.400000e-01 5.000000e-02 5.000000e-02 +2.437500e+00 1.250000e-02 1.250000e-02 1.300000e-01 4.000000e-02 4.000000e-02 +2.462500e+00 1.250000e-02 1.250000e-02 9.000000e-02 4.000000e-02 4.000000e-02 +2.487500e+00 1.250000e-02 1.250000e-02 8.000000e-02 3.000000e-02 3.000000e-02 +2.512500e+00 1.250000e-02 1.250000e-02 9.000000e-02 3.000000e-02 3.000000e-02 +2.537500e+00 1.250000e-02 1.250000e-02 7.000000e-02 3.000000e-02 3.000000e-02 +2.562500e+00 1.250000e-02 1.250000e-02 2.000000e-02 2.000000e-02 2.000000e-02 +2.587500e+00 1.250000e-02 1.250000e-02 6.000000e-02 3.000000e-02 3.000000e-02 +2.612500e+00 1.250000e-02 1.250000e-02 7.000000e-02 3.000000e-02 3.000000e-02 +2.637500e+00 1.250000e-02 1.250000e-02 6.000000e-02 3.000000e-02 3.000000e-02 +2.662500e+00 1.250000e-02 1.250000e-02 5.000000e-02 3.000000e-02 3.000000e-02 +2.687500e+00 1.250000e-02 1.250000e-02 3.000000e-02 2.000000e-02 2.000000e-02 +2.712500e+00 1.250000e-02 1.250000e-02 5.000000e-02 2.000000e-02 2.000000e-02 +2.737500e+00 1.250000e-02 1.250000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +2.762500e+00 1.250000e-02 1.250000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +2.787500e+00 1.250000e-02 1.250000e-02 3.000000e-02 2.000000e-02 2.000000e-02 +2.812500e+00 1.250000e-02 1.250000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +2.837500e+00 1.250000e-02 1.250000e-02 5.000000e-02 2.000000e-02 2.000000e-02 +2.862500e+00 1.250000e-02 1.250000e-02 2.000000e-02 2.000000e-02 2.000000e-02 +2.887500e+00 1.250000e-02 1.250000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +2.912500e+00 1.250000e-02 1.250000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +2.937500e+00 1.250000e-02 1.250000e-02 0.000000e+00 0.000000e+00 0.000000e+00 +2.962500e+00 1.250000e-02 1.250000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I747875/d05-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.05, up: 0.05}}, 1: {error: {dn: -0.07, up: 0.07}}, 2: {error: {dn: -0.07, up: 0.07}}, 3: {error: {dn: -0.08, up: 0.08}}, 4: {error: {dn: -0.09, up: 0.09}}, 5: {error: {dn: -0.09, up: 0.09}}, 6: {error: {dn: -0.11, up: 0.11}}, 7: {error: {dn: -0.11, up: 0.11}}, 8: {error: {dn: -0.11, up: 0.11}}, 9: {error: {dn: -0.12, up: 0.12}}, 10: {error: {dn: -0.12, up: 0.12}}, 11: {error: {dn: -0.11, up: 0.11}}, 12: {error: {dn: -0.12, up: 0.12}}, 13: {error: {dn: -0.11, up: 0.11}}, 14: {error: {dn: -0.11, up: 0.11}}, 15: {error: {dn: -0.1, up: 0.1}}, 16: {error: {dn: -0.1, up: 0.1}}, 17: {error: {dn: -0.1, up: 0.1}}, 18: {error: {dn: -0.1, up: 0.1}}, 19: {error: {dn: -0.08, up: 0.08}}, 20: {error: {dn: -0.08, up: 0.08}}, 21: {error: {dn: -0.07, up: 0.07}}, 22: {error: {dn: -0.07, up: 0.07}}, 23: {error: {dn: -0.06, up: 0.06}}, 24: {error: {dn: -0.06, up: 0.06}}, 25: {error: {dn: -0.06, up: 0.06}}, 26: {error: {dn: -0.06, up: 0.06}}, 27: {error: {dn: -0.05, up: 0.05}}, 28: {error: {dn: -0.05, up: 0.05}}, 29: {error: {dn: -0.05, up: 0.05}}, 30: {error: {dn: -0.05, up: 0.05}}, 31: {error: {dn: -0.05, up: 0.05}}, 32: {error: {dn: -0.04, up: 0.04}}, 33: {error: {dn: -0.04, up: 0.04}}, 34: {error: {dn: -0.04, up: 0.04}}, 35: {error: {dn: -0.04, up: 0.04}}, 36: {error: {dn: -0.04, up: 0.04}}, 37: {error: {dn: -0.03, up: 0.03}}, 38: {error: {dn: -0.04, up: 0.04}}, 39: {error: {dn: -0.04, up: 0.04}}, 40: {error: {dn: -0.04, up: 0.04}}, 41: {error: {dn: -0.04, up: 0.04}}, 42: {error: {dn: -0.07, up: 0.07}}, 43: {error: {dn: -0.04, up: 0.04}}, 44: {error: {dn: -0.03, up: 0.03}}, 45: {error: {dn: -0.03, up: 0.03}}, 46: {error: {dn: -0.03, up: 0.03}}, 47: {error: {dn: -0.03, up: 0.03}}, 48: {error: {dn: -0.03, up: 0.03}}, 49: {error: {dn: -0.02, up: 0.02}}, 50: {error: {dn: -0.03, up: 0.03}}, 51: {error: {dn: -0.02, up: 0.02}}, 52: {error: {dn: -0.02, up: 0.02}}, 53: {error: {dn: -0.02, up: 0.02}}, 54: {error: {dn: -0.02, up: 0.02}}, 55: {error: {dn: -0.02, up: 0.02}}, 56: {error: {dn: -0.02, up: 0.02}}, 57: {error: {dn: -0.02, up: 0.02}}, 58: {error: {dn: -0.02, up: 0.02}}, 59: {error: {dn: -0.02, up: 0.02}}, 60: {error: {dn: -0.01, up: 0.01}}, 61: {error: {dn: -0.01, up: 0.01}}, 62: {error: {dn: -0.02, up: 0.02}}, 63: {error: {dn: -0.01, up: 0.01}}, 64: {error: {dn: -0.01, up: 0.01}}, 65: {error: {dn: -0.01, up: 0.01}}, 66: {error: {dn: -0.01, up: 0.01}}, 67: {error: {dn: -0.01, up: 0.01}}, 68: {error: {dn: -0.01, up: 0.01}}, 69: {error: {dn: -0.01, up: 0.01}}, 70: {error: {dn: -0.01, up: 0.01}}, 71: {error: {dn: -0.01, up: 0.01}}, 72: {error: {dn: -0.01, up: 0.01}}, 73: {error: {dn: -0.01, up: 0.01}}, 74: {error: {dn: -0.01, up: 0.01}}, 75: {error: {dn: -0.01, up: 0.01}}, 76: {error: {dn: -0.01, up: 0.01}}, 77: {error: {dn: -0.01, up: 0.01}}, 78: {error: {dn: -0.01, up: 0.01}}, 79: {error: {dn: -0.01, up: 0.01}}, 80: {error: {dn: -0.01, up: 0.01}}, 81: {error: {dn: -0.01, up: 0.01}}, 82: {error: {dn: -0.01, up: 0.01}}, 83: {error: {dn: -0.01, up: 0.01}}, 84: {error: {dn: -0.01, up: 0.01}}, 85: {error: {dn: -0.01, up: 0.01}}, 86: {error: {dn: -0.01, up: 0.01}}, 87: {error: {dn: -0.01, up: 0.01}}, 88: {error: {dn: -0.02, up: 0.02}}, 89: {error: {dn: -0.02, up: 0.02}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I747875/d05-x01-y01 +Title: doi:10.17182/hepdata.50373.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.420000e+00 2.000000e-02 2.000000e-02 0.000000e+00 5.000000e-02 5.000000e-02 +1.460000e+00 2.000000e-02 2.000000e-02 1.200000e-01 7.000000e-02 7.000000e-02 +1.500000e+00 2.000000e-02 2.000000e-02 0.000000e+00 7.000000e-02 7.000000e-02 +1.540000e+00 2.000000e-02 2.000000e-02 1.000000e-02 8.000000e-02 8.000000e-02 +1.580000e+00 2.000000e-02 2.000000e-02 3.000000e-02 9.000000e-02 9.000000e-02 +1.620000e+00 2.000000e-02 2.000000e-02 9.000000e-02 9.000000e-02 9.000000e-02 +1.660000e+00 2.000000e-02 2.000000e-02 3.100000e-01 1.100000e-01 1.100000e-01 +1.700000e+00 2.000000e-02 2.000000e-02 3.500000e-01 1.100000e-01 1.100000e-01 +1.740000e+00 2.000000e-02 2.000000e-02 4.900000e-01 1.100000e-01 1.100000e-01 +1.780000e+00 2.000000e-02 2.000000e-02 5.100000e-01 1.200000e-01 1.200000e-01 +1.820000e+00 2.000000e-02 2.000000e-02 8.400000e-01 1.200000e-01 1.200000e-01 +1.860000e+00 2.000000e-02 2.000000e-02 9.400000e-01 1.100000e-01 1.100000e-01 +1.900000e+00 2.000000e-02 2.000000e-02 9.500000e-01 1.200000e-01 1.200000e-01 +1.940000e+00 2.000000e-02 2.000000e-02 8.000000e-01 1.100000e-01 1.100000e-01 +1.980000e+00 2.000000e-02 2.000000e-02 8.700000e-01 1.100000e-01 1.100000e-01 +2.020000e+00 2.000000e-02 2.000000e-02 1.000000e+00 1.000000e-01 1.000000e-01 +2.060000e+00 2.000000e-02 2.000000e-02 9.600000e-01 1.000000e-01 1.000000e-01 +2.100000e+00 2.000000e-02 2.000000e-02 9.000000e-01 1.000000e-01 1.000000e-01 +2.140000e+00 2.000000e-02 2.000000e-02 8.200000e-01 1.000000e-01 1.000000e-01 +2.180000e+00 2.000000e-02 2.000000e-02 5.800000e-01 8.000000e-02 8.000000e-02 +2.220000e+00 2.000000e-02 2.000000e-02 5.600000e-01 8.000000e-02 8.000000e-02 +2.260000e+00 2.000000e-02 2.000000e-02 3.700000e-01 7.000000e-02 7.000000e-02 +2.300000e+00 2.000000e-02 2.000000e-02 4.300000e-01 7.000000e-02 7.000000e-02 +2.340000e+00 2.000000e-02 2.000000e-02 3.500000e-01 6.000000e-02 6.000000e-02 +2.380000e+00 2.000000e-02 2.000000e-02 2.900000e-01 6.000000e-02 6.000000e-02 +2.420000e+00 2.000000e-02 2.000000e-02 3.800000e-01 6.000000e-02 6.000000e-02 +2.460000e+00 2.000000e-02 2.000000e-02 3.800000e-01 6.000000e-02 6.000000e-02 +2.500000e+00 2.000000e-02 2.000000e-02 2.200000e-01 5.000000e-02 5.000000e-02 +2.540000e+00 2.000000e-02 2.000000e-02 2.500000e-01 5.000000e-02 5.000000e-02 +2.580000e+00 2.000000e-02 2.000000e-02 2.500000e-01 5.000000e-02 5.000000e-02 +2.620000e+00 2.000000e-02 2.000000e-02 2.500000e-01 5.000000e-02 5.000000e-02 +2.660000e+00 2.000000e-02 2.000000e-02 2.800000e-01 5.000000e-02 5.000000e-02 +2.700000e+00 2.000000e-02 2.000000e-02 1.600000e-01 4.000000e-02 4.000000e-02 +2.740000e+00 2.000000e-02 2.000000e-02 2.200000e-01 4.000000e-02 4.000000e-02 +2.780000e+00 2.000000e-02 2.000000e-02 2.100000e-01 4.000000e-02 4.000000e-02 +2.820000e+00 2.000000e-02 2.000000e-02 1.300000e-01 4.000000e-02 4.000000e-02 +2.860000e+00 2.000000e-02 2.000000e-02 2.100000e-01 4.000000e-02 4.000000e-02 +2.900000e+00 2.000000e-02 2.000000e-02 1.100000e-01 3.000000e-02 3.000000e-02 +2.940000e+00 2.000000e-02 2.000000e-02 1.200000e-01 4.000000e-02 4.000000e-02 +2.980000e+00 2.000000e-02 2.000000e-02 1.200000e-01 4.000000e-02 4.000000e-02 +3.020000e+00 2.000000e-02 2.000000e-02 2.100000e-01 4.000000e-02 4.000000e-02 +3.060000e+00 2.000000e-02 2.000000e-02 1.600000e-01 4.000000e-02 4.000000e-02 +3.100000e+00 2.000000e-02 2.000000e-02 9.200000e-01 7.000000e-02 7.000000e-02 +3.140000e+00 2.000000e-02 2.000000e-02 1.900000e-01 4.000000e-02 4.000000e-02 +3.180000e+00 2.000000e-02 2.000000e-02 1.200000e-01 3.000000e-02 3.000000e-02 +3.220000e+00 2.000000e-02 2.000000e-02 1.400000e-01 3.000000e-02 3.000000e-02 +3.260000e+00 2.000000e-02 2.000000e-02 1.300000e-01 3.000000e-02 3.000000e-02 +3.300000e+00 2.000000e-02 2.000000e-02 9.000000e-02 3.000000e-02 3.000000e-02 +3.340000e+00 2.000000e-02 2.000000e-02 9.000000e-02 3.000000e-02 3.000000e-02 +3.380000e+00 2.000000e-02 2.000000e-02 8.000000e-02 2.000000e-02 2.000000e-02 +3.420000e+00 2.000000e-02 2.000000e-02 1.100000e-01 3.000000e-02 3.000000e-02 +3.460000e+00 2.000000e-02 2.000000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +3.500000e+00 2.000000e-02 2.000000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +3.540000e+00 2.000000e-02 2.000000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +3.580000e+00 2.000000e-02 2.000000e-02 7.000000e-02 2.000000e-02 2.000000e-02 +3.620000e+00 2.000000e-02 2.000000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +3.660000e+00 2.000000e-02 2.000000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +3.700000e+00 2.000000e-02 2.000000e-02 8.000000e-02 2.000000e-02 2.000000e-02 +3.740000e+00 2.000000e-02 2.000000e-02 9.000000e-02 2.000000e-02 2.000000e-02 +3.780000e+00 2.000000e-02 2.000000e-02 2.000000e-02 2.000000e-02 2.000000e-02 +3.820000e+00 2.000000e-02 2.000000e-02 5.000000e-02 1.000000e-02 1.000000e-02 +3.860000e+00 2.000000e-02 2.000000e-02 4.000000e-02 1.000000e-02 1.000000e-02 +3.900000e+00 2.000000e-02 2.000000e-02 3.000000e-02 2.000000e-02 2.000000e-02 +3.940000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +3.980000e+00 2.000000e-02 2.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +4.020000e+00 2.000000e-02 2.000000e-02 5.000000e-02 1.000000e-02 1.000000e-02 +4.060000e+00 2.000000e-02 2.000000e-02 4.000000e-02 1.000000e-02 1.000000e-02 +4.100000e+00 2.000000e-02 2.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +4.140000e+00 2.000000e-02 2.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +4.180000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +4.220000e+00 2.000000e-02 2.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +4.260000e+00 2.000000e-02 2.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +4.300000e+00 2.000000e-02 2.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +4.340000e+00 2.000000e-02 2.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +4.380000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +4.420000e+00 2.000000e-02 2.000000e-02 5.000000e-02 1.000000e-02 1.000000e-02 +4.460000e+00 2.000000e-02 2.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +4.500000e+00 2.000000e-02 2.000000e-02 4.000000e-02 1.000000e-02 1.000000e-02 +4.540000e+00 2.000000e-02 2.000000e-02 0.000000e+00 1.000000e-02 1.000000e-02 +4.580000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +4.620000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +4.660000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +4.700000e+00 2.000000e-02 2.000000e-02 4.000000e-02 1.000000e-02 1.000000e-02 +4.740000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +4.780000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +4.820000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +4.860000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +4.900000e+00 2.000000e-02 2.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +4.940000e+00 2.000000e-02 2.000000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +4.980000e+00 2.000000e-02 2.000000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I747875/d06-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.053, up: 0.082}}, 1: {error: {dn: -0.085, up: 0.114}}, 2: {error: {dn: -0.075, up: 0.104}}, 3: {error: {dn: -0.131, up: 0.16}}, 4: {error: {dn: -0.113, up: 0.142}}, 5: {error: {dn: -0.137, up: 0.164}}, 6: {error: {dn: -0.118, up: 0.143}}, 7: {error: {dn: -0.042, up: 0.064}}, 8: {error: {dn: -0.071, up: 0.095}}, 9: {error: {dn: -0.03, up: 0.042}}, 10: {error: {dn: -0.042, up: 0.053}}, 11: {error: {dn: -0.019, up: 0.024}}, 12: {error: {dn: -0.012, up: 0.017}}, 13: {error: {dn: -0.011, up: 0.015}}, 14: {error: {dn: -0.013, up: 0.017}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I747875/d06-x01-y01 +Title: doi:10.17182/hepdata.50373.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.900000e+00 2.000000e-02 2.000000e-02 7.800000e-02 5.300000e-02 8.200000e-02 +1.940000e+00 2.000000e-02 2.000000e-02 2.200000e-01 8.500000e-02 1.140000e-01 +1.980000e+00 2.000000e-02 2.000000e-02 1.360000e-01 7.500000e-02 1.040000e-01 +2.020000e+00 2.000000e-02 2.000000e-02 4.460000e-01 1.310000e-01 1.600000e-01 +2.060000e+00 2.000000e-02 2.000000e-02 3.150000e-01 1.130000e-01 1.420000e-01 +2.140000e+00 2.000000e-02 2.000000e-02 3.970000e-01 1.370000e-01 1.640000e-01 +2.180000e+00 2.000000e-02 2.000000e-02 4.080000e-01 1.180000e-01 1.430000e-01 +2.220000e+00 2.000000e-02 2.000000e-02 7.000000e-02 4.200000e-02 6.400000e-02 +2.260000e+00 2.000000e-02 2.000000e-02 1.740000e-01 7.100000e-02 9.500000e-02 +2.320000e+00 4.000000e-02 4.000000e-02 6.900000e-02 3.000000e-02 4.200000e-02 +2.480000e+00 4.000000e-02 4.000000e-02 1.200000e-01 4.200000e-02 5.300000e-02 +2.600000e+00 8.000000e-02 8.000000e-02 5.000000e-02 1.900000e-02 2.400000e-02 +2.760000e+00 8.000000e-02 8.000000e-02 2.600000e-02 1.200000e-02 1.700000e-02 +2.920000e+00 8.000000e-02 8.000000e-02 2.600000e-02 1.100000e-02 1.500000e-02 +3.080000e+00 8.000000e-02 8.000000e-02 3.200000e-02 1.300000e-02 1.700000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I747875/d07-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.01, up: 0.01}}, 1: {error: {dn: -0.01, up: 0.01}}, 2: {error: {dn: -0.01, up: 0.01}}, 3: {error: {dn: -0.01, up: 0.01}}, 4: {error: {dn: -0.01, up: 0.01}}, 5: {error: {dn: -0.02, up: 0.02}}, 6: {error: {dn: -0.02, up: 0.02}}, 7: {error: {dn: -0.02, up: 0.02}}, 8: {error: {dn: -0.02, up: 0.02}}, 9: {error: {dn: -0.02, up: 0.02}}, 10: {error: {dn: -0.02, up: 0.02}}, 11: {error: {dn: -0.02, up: 0.02}}, 12: {error: {dn: -0.02, up: 0.02}}, 13: {error: {dn: -0.02, up: 0.02}}, 14: {error: {dn: -0.02, up: 0.02}}, 15: {error: {dn: -0.02, up: 0.02}}, 16: {error: {dn: -0.01, up: 0.01}}, 17: {error: {dn: -0.02, up: 0.02}}, 18: {error: {dn: -0.01, up: 0.01}}, 19: {error: {dn: -0.01, up: 0.01}}, 20: {error: {dn: -0.01, up: 0.01}}, 21: {error: {dn: -0.01, up: 0.01}}, 22: {error: {dn: -0.01, up: 0.01}}, 23: {error: {dn: -0.01, up: 0.01}}, 24: {error: {dn: -0.01, up: 0.01}}, 25: {error: {dn: -0.01, up: 0.01}}, 26: {error: {dn: -0.01, up: 0.01}}, 27: {error: {dn: -0.02, up: 0.02}}, 28: {error: {dn: -0.01, up: 0.01}}, 29: {error: {dn: -0.01, up: 0.01}}, 30: {error: {dn: -0.01, up: 0.01}}, 31: {error: {dn: -0.01, up: 0.01}}, 32: {error: {dn: -0.01, up: 0.01}}, 33: {error: {dn: -0.01, up: 0.01}}, 34: {error: {dn: -0.01, up: 0.01}}, 35: {error: {dn: -0.01, up: 0.01}}, 36: {error: {dn: -0.01, up: 0.01}}, 37: {error: {dn: -0.01, up: 0.01}}, 38: {error: {dn: -0.01, up: 0.01}}, 39: {error: {dn: -0.01, up: 0.01}}, 40: {error: {dn: -0.01, up: 0.01}}, 41: {error: {dn: -0.01, up: 0.01}}, 42: {error: {dn: -0.01, up: 0.01}}, 43: {error: {dn: -0.01, up: 0.01}}, 44: {error: {dn: -0.01, up: 0.01}}, 45: {error: {dn: -0.01, up: 0.01}}, 46: {error: {dn: -0.01, up: 0.01}}, 47: {error: {dn: -0.01, up: 0.01}}, 48: {error: {dn: -0.01, up: 0.01}}, 49: {error: {dn: -0.01, up: 0.01}}, 50: {error: {dn: -0.01, up: 0.01}}, 51: {error: {dn: -0.01, up: 0.01}}, 52: {error: {dn: -0.01, up: 0.01}}, 53: {error: {dn: -0.01, up: 0.01}}, 54: {error: {dn: -0.01, up: 0.01}}, 55: {error: {dn: -0.01, up: 0.01}}, 56: {error: {dn: -0.01, up: 0.01}}, 57: {error: {dn: -0.01, up: 0.01}}, 58: {error: {dn: -0.01, up: 0.01}}, 59: {error: {dn: -0.01, up: 0.01}}, 60: {error: {dn: -0.01, up: 0.01}}, 61: {error: {dn: -0.01, up: 0.01}}, 62: {error: {dn: -0.01, up: 0.01}}, 63: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I747875/d07-x01-y01 +Title: doi:10.17182/hepdata.50373.v1/t7 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.020000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +2.060000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +2.100000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +2.140000e+00 2.000000e-02 2.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +2.180000e+00 2.000000e-02 2.000000e-02 4.000000e-02 1.000000e-02 1.000000e-02 +2.220000e+00 2.000000e-02 2.000000e-02 9.000000e-02 2.000000e-02 2.000000e-02 +2.260000e+00 2.000000e-02 2.000000e-02 7.000000e-02 2.000000e-02 2.000000e-02 +2.300000e+00 2.000000e-02 2.000000e-02 9.000000e-02 2.000000e-02 2.000000e-02 +2.340000e+00 2.000000e-02 2.000000e-02 8.000000e-02 2.000000e-02 2.000000e-02 +2.380000e+00 2.000000e-02 2.000000e-02 8.000000e-02 2.000000e-02 2.000000e-02 +2.420000e+00 2.000000e-02 2.000000e-02 7.000000e-02 2.000000e-02 2.000000e-02 +2.460000e+00 2.000000e-02 2.000000e-02 9.000000e-02 2.000000e-02 2.000000e-02 +2.500000e+00 2.000000e-02 2.000000e-02 8.000000e-02 2.000000e-02 2.000000e-02 +2.540000e+00 2.000000e-02 2.000000e-02 9.000000e-02 2.000000e-02 2.000000e-02 +2.580000e+00 2.000000e-02 2.000000e-02 8.000000e-02 2.000000e-02 2.000000e-02 +2.620000e+00 2.000000e-02 2.000000e-02 9.000000e-02 2.000000e-02 2.000000e-02 +2.660000e+00 2.000000e-02 2.000000e-02 8.000000e-02 1.000000e-02 1.000000e-02 +2.700000e+00 2.000000e-02 2.000000e-02 1.000000e-01 2.000000e-02 2.000000e-02 +2.740000e+00 2.000000e-02 2.000000e-02 7.000000e-02 1.000000e-02 1.000000e-02 +2.780000e+00 2.000000e-02 2.000000e-02 6.000000e-02 1.000000e-02 1.000000e-02 +2.820000e+00 2.000000e-02 2.000000e-02 5.000000e-02 1.000000e-02 1.000000e-02 +2.860000e+00 2.000000e-02 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histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + // Book histograms + for(unsigned int ix=1;ix<12;++ix) { + stringstream ss; + ss << "TMP/n" << ix; + _nMeson[ix]= bookCounter(ss.str()); + } + } + + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=223 && p.pdgId()!=221&&p.pdgId()!=331&& p.pdgId()!=20223) + continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // omega + if(p.pdgId()==223) { + if(ncount==2) { + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nMeson[3]->fill(event.weight());matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==321) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nMeson[10]->fill(event.weight()); + } + foreach (const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=9010221) continue; + if(p2.parents()[0].isSame(p)) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=0) continue; + bool matched2 = true; + for(auto const & val : nResB) { + if(val.second!=0) { + matched2 = false; + break; + } + } + if(matched2) + _nMeson[4]->fill(event.weight()); + } + } + else if(p.pdgId()==221) { + if(ncount==2) { + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nMeson[2]->fill(event.weight()); + } + else if(ncount==4) { + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second!=2) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nMeson[5]->fill(event.weight()); + matched=true; + for(auto const & val : nRes) { + if(abs(val.first)==211 || abs(val.first)==321) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nMeson[11]->fill(event.weight()); + } + foreach(const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=333) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=0) continue; + bool matched2 = true; + for(auto const & val : nResB) { + if(val.second!=0) { + matched2 = false; + break; + } + } + if(matched2) + _nMeson[9]->fill(event.weight()); + } + } + else if(p.pdgId()==331 || p.pdgId()==20223) { + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(p.pdgId()==331) + _nMeson[6]->fill(event.weight()); + else + _nMeson[7]->fill(event.weight()); + } + } + } + + if(ntotal==5) { + if(nCount[211]==2&&nCount[-211]==2&&nCount[111]==1) + _nMeson[1]->fill(event.weight()); + else if(nCount[321]==1&&nCount[-321]==1&& + nCount[211]==1&&nCount[-211]==1&&nCount[111]==1) + _nMeson[8]->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<12;++ix) { + double sigma = _nMeson[ix]->val(); + double error = _nMeson[ix]->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nMeson[12]; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2007_I758568); + + +} diff --git a/analyses/pluginBABAR/BABAR_2007_I758568.info b/analyses/pluginBABAR/BABAR_2007_I758568.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I758568.info @@ -0,0 +1,38 @@ +Name: BABAR_2007_I758568 +Year: 2007 +Summary: Cross sections for $e^+e^-\to$ $2\pi^+2\pi^-\pi^0$, $2\pi^+2\pi^-\eta$, $K^+K^-\pi^+\pi^-\pi^0$ and $K^+K^-\pi^+\pi^-\eta$ from threshold to 5.0 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 758568 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D76 (2007) 092005, 2007 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^- \to$ $2\pi^+2\pi^-\pi^0$, $2\pi^+2\pi^-\eta$, $K^+K^-\pi^+\pi^-\pi^0$ + and $K^+K^-\pi^+\pi^-\eta$ via radiative return, for energies from the threshold to 5.0 GeV' +Keywords: +BibKey: Aubert:2007ef +BibTeX: '@article{Aubert:2007ef, + author = "Aubert, Bernard and others", + title = "{The e+ e- ---> 2(pi+ pi-) pi0, 2(pi+ pi-) eta, K+ K- pi+ + pi- pi0 and K+ K- pi+ pi- eta Cross Sections Measured with + Initial-State Radiation}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D76", + year = "2007", + pages = "092005", + doi = "10.1103/PhysRevD.77.119902, 10.1103/PhysRevD.76.092005", + note = "[Erratum: Phys. Rev.D77,119902(2008)]", + eprint = "0708.2461", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BABAR-PUB-07-045, SLAC-PUB-12753", + SLACcitation = "%%CITATION = ARXIV:0708.2461;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2007_I758568.plot b/analyses/pluginBABAR/BABAR_2007_I758568.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I758568.plot @@ -0,0 +1,76 @@ +BEGIN PLOT /BABAR_2007_I758568/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2007_I758568/d02-x01-y01 +Title=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$/nb +ConnectGaps=1 +LogY=0 +END PLOT + +BEGIN PLOT /BABAR_2007_I758568/d03-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I758568/d04-x01-y01 +Title=$\sigma(e^+e^-\to \omega f_0(980))$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega f_0(980))$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I758568/d05-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-\eta)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I758568/d06-x01-y01 +Title=$\sigma(e^+e^-\to \eta^\prime\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta^\prime\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I758568/d07-x01-y01 +Title=$\sigma(e^+e^-\to f_1(1285)\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to f_1(1285)\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I758568/d08-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I758568/d09-x01-y01 +Title=$\sigma(e^+e^-\to \phi\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\eta)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I758568/d10-x01-y01 +Title=$\sigma(e^+e^-\to \omega K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega K^+K^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2007_I758568/d11-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-\eta)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2007_I758568.yoda b/analyses/pluginBABAR/BABAR_2007_I758568.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I758568.yoda @@ -0,0 +1,873 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.03, up: 0.03}}, 1: {error: {dn: -0.04, up: 0.04}}, 2: {error: {dn: -0.05, up: 0.05}}, 3: {error: {dn: -0.05, up: 0.05}}, 4: {error: {dn: -0.06, up: 0.06}}, 5: {error: {dn: 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1.250000e-02 1.250000e-02 1.600000e-01 6.000000e-02 6.000000e-02 +4.187500e+00 1.250000e-02 1.250000e-02 1.800000e-01 6.000000e-02 6.000000e-02 +4.212500e+00 1.250000e-02 1.250000e-02 1.400000e-01 6.000000e-02 6.000000e-02 +4.237500e+00 1.250000e-02 1.250000e-02 1.100000e-01 6.000000e-02 6.000000e-02 +4.262500e+00 1.250000e-02 1.250000e-02 1.000000e-01 6.000000e-02 6.000000e-02 +4.287500e+00 1.250000e-02 1.250000e-02 5.000000e-02 6.000000e-02 6.000000e-02 +4.312500e+00 1.250000e-02 1.250000e-02 1.100000e-01 5.000000e-02 5.000000e-02 +4.337500e+00 1.250000e-02 1.250000e-02 8.000000e-02 5.000000e-02 5.000000e-02 +4.362500e+00 1.250000e-02 1.250000e-02 1.100000e-01 5.000000e-02 5.000000e-02 +4.387500e+00 1.250000e-02 1.250000e-02 8.000000e-02 5.000000e-02 5.000000e-02 +4.412500e+00 1.250000e-02 1.250000e-02 3.000000e-02 5.000000e-02 5.000000e-02 +4.437500e+00 1.250000e-02 1.250000e-02 1.100000e-01 5.000000e-02 5.000000e-02 +4.462500e+00 1.250000e-02 1.250000e-02 7.000000e-02 5.000000e-02 5.000000e-02 +4.487500e+00 1.250000e-02 1.250000e-02 1.500000e-01 6.000000e-02 6.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.05, up: 0.05}}, 1: {error: {dn: -0.08, up: 0.08}}, 2: {error: {dn: -0.1, up: 0.1}}, 3: {error: {dn: -0.13, up: 0.13}}, 4: {error: {dn: -0.13, up: 0.13}}, 5: {error: {dn: -0.18, up: 0.18}}, 6: {error: {dn: -0.24, up: 0.24}}, 7: {error: {dn: -0.26, up: 0.26}}, 8: {error: {dn: -0.33, up: 0.33}}, 9: {error: {dn: -0.34, up: 0.34}}, 10: {error: {dn: -0.37, up: 0.37}}, 11: {error: {dn: -0.34, up: 0.34}}, 12: {error: {dn: -0.35, up: 0.35}}, 13: {error: {dn: -0.29, up: 0.29}}, 14: {error: {dn: -0.28, up: 0.28}}, 15: {error: {dn: -0.25, up: 0.25}}, 16: {error: {dn: -0.23, up: 0.23}}, 17: {error: {dn: -0.18, up: 0.18}}, 18: {error: {dn: -0.17, up: 0.17}}, 19: {error: {dn: -0.15, up: 0.15}}, 20: {error: {dn: -0.14, up: 0.14}}, 21: {error: {dn: -0.15, up: 0.15}}, 22: {error: {dn: -0.12, up: 0.12}}, 23: {error: {dn: -0.12, up: 0.12}}, 24: {error: {dn: -0.11, up: 0.11}}, 25: {error: {dn: -0.1, up: 0.1}}, 26: {error: {dn: -0.1, up: 0.1}}, 27: {error: {dn: -0.09, up: 0.09}}, 28: {error: {dn: -0.08, up: 0.08}}, 29: {error: {dn: -0.09, up: 0.09}}, 30: {error: {dn: -0.07, up: 0.07}}, 31: {error: {dn: -0.07, up: 0.07}}, 32: {error: {dn: -0.07, up: 0.07}}, 33: {error: {dn: -0.07, up: 0.07}}, 34: {error: {dn: -0.06, up: 0.06}}, 35: {error: {dn: -0.06, up: 0.06}}, 36: {error: {dn: -0.06, up: 0.06}}, 37: {error: {dn: -0.05, up: 0.05}}, 38: {error: {dn: -0.06, up: 0.06}}, 39: {error: {dn: -0.05, up: 0.05}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I758568/d02-x01-y01 +Title: doi:10.17182/hepdata.51824.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.025000e+00 2.500000e-02 2.500000e-02 0.000000e+00 5.000000e-02 5.000000e-02 +1.075000e+00 2.500000e-02 2.500000e-02 1.100000e-01 8.000000e-02 8.000000e-02 +1.125000e+00 2.500000e-02 2.500000e-02 5.000000e-02 1.000000e-01 1.000000e-01 +1.175000e+00 2.500000e-02 2.500000e-02 2.000000e-01 1.300000e-01 1.300000e-01 +1.225000e+00 2.500000e-02 2.500000e-02 1.000000e-01 1.300000e-01 1.300000e-01 +1.275000e+00 2.500000e-02 2.500000e-02 6.600000e-01 1.800000e-01 1.800000e-01 +1.325000e+00 2.500000e-02 2.500000e-02 7.600000e-01 2.400000e-01 2.400000e-01 +1.375000e+00 2.500000e-02 2.500000e-02 1.370000e+00 2.600000e-01 2.600000e-01 +1.425000e+00 2.500000e-02 2.500000e-02 2.880000e+00 3.300000e-01 3.300000e-01 +1.475000e+00 2.500000e-02 2.500000e-02 3.590000e+00 3.400000e-01 3.400000e-01 +1.525000e+00 2.500000e-02 2.500000e-02 4.290000e+00 3.700000e-01 3.700000e-01 +1.575000e+00 2.500000e-02 2.500000e-02 3.130000e+00 3.400000e-01 3.400000e-01 +1.625000e+00 2.500000e-02 2.500000e-02 2.830000e+00 3.500000e-01 3.500000e-01 +1.675000e+00 2.500000e-02 2.500000e-02 2.130000e+00 2.900000e-01 2.900000e-01 +1.725000e+00 2.500000e-02 2.500000e-02 2.330000e+00 2.800000e-01 2.800000e-01 +1.775000e+00 2.500000e-02 2.500000e-02 1.900000e+00 2.500000e-01 2.500000e-01 +1.825000e+00 2.500000e-02 2.500000e-02 1.570000e+00 2.300000e-01 2.300000e-01 +1.875000e+00 2.500000e-02 2.500000e-02 8.000000e-01 1.800000e-01 1.800000e-01 +1.925000e+00 2.500000e-02 2.500000e-02 7.700000e-01 1.700000e-01 1.700000e-01 +1.975000e+00 2.500000e-02 2.500000e-02 6.900000e-01 1.500000e-01 1.500000e-01 +2.025000e+00 2.500000e-02 2.500000e-02 5.400000e-01 1.400000e-01 1.400000e-01 +2.075000e+00 2.500000e-02 2.500000e-02 5.000000e-01 1.500000e-01 1.500000e-01 +2.125000e+00 2.500000e-02 2.500000e-02 3.600000e-01 1.200000e-01 1.200000e-01 +2.175000e+00 2.500000e-02 2.500000e-02 6.400000e-01 1.200000e-01 1.200000e-01 +2.225000e+00 2.500000e-02 2.500000e-02 3.200000e-01 1.100000e-01 1.100000e-01 +2.275000e+00 2.500000e-02 2.500000e-02 4.200000e-01 1.000000e-01 1.000000e-01 +2.325000e+00 2.500000e-02 2.500000e-02 1.600000e-01 1.000000e-01 1.000000e-01 +2.375000e+00 2.500000e-02 2.500000e-02 1.500000e-01 9.000000e-02 9.000000e-02 +2.425000e+00 2.500000e-02 2.500000e-02 5.000000e-02 8.000000e-02 8.000000e-02 +2.475000e+00 2.500000e-02 2.500000e-02 2.500000e-01 9.000000e-02 9.000000e-02 +2.525000e+00 2.500000e-02 2.500000e-02 0.000000e+00 7.000000e-02 7.000000e-02 +2.575000e+00 2.500000e-02 2.500000e-02 6.000000e-02 7.000000e-02 7.000000e-02 +2.625000e+00 2.500000e-02 2.500000e-02 1.100000e-01 7.000000e-02 7.000000e-02 +2.675000e+00 2.500000e-02 2.500000e-02 2.000000e-02 7.000000e-02 7.000000e-02 +2.725000e+00 2.500000e-02 2.500000e-02 5.000000e-02 6.000000e-02 6.000000e-02 +2.775000e+00 2.500000e-02 2.500000e-02 0.000000e+00 6.000000e-02 6.000000e-02 +2.825000e+00 2.500000e-02 2.500000e-02 5.000000e-02 6.000000e-02 6.000000e-02 +2.875000e+00 2.500000e-02 2.500000e-02 0.000000e+00 5.000000e-02 5.000000e-02 +2.925000e+00 2.500000e-02 2.500000e-02 2.000000e-01 6.000000e-02 6.000000e-02 +2.975000e+00 2.500000e-02 2.500000e-02 0.000000e+00 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.09, up: 0.09}}, 1: {error: {dn: -0.05, up: 0.05}}, 2: {error: {dn: -0.08, up: 0.08}}, 3: {error: {dn: -0.12, up: 0.12}}, 4: {error: {dn: -0.14, up: 0.14}}, 5: {error: {dn: -0.14, up: 0.14}}, 6: {error: {dn: -0.15, up: 0.15}}, 7: {error: {dn: -0.16, up: 0.16}}, 8: {error: {dn: -0.2, up: 0.2}}, 9: {error: {dn: -0.2, up: 0.2}}, 10: {error: {dn: -0.22, up: 0.22}}, 11: {error: {dn: -0.24, up: 0.24}}, 12: {error: {dn: -0.23, up: 0.23}}, 13: {error: {dn: -0.25, up: 0.25}}, 14: {error: {dn: -0.25, up: 0.25}}, 15: {error: {dn: -0.24, up: 0.24}}, 16: {error: {dn: -0.27, up: 0.27}}, 17: {error: {dn: -0.27, up: 0.27}}, 18: {error: {dn: -0.28, up: 0.28}}, 19: {error: {dn: -0.29, up: 0.29}}, 20: {error: {dn: -0.3, up: 0.3}}, 21: {error: {dn: -0.28, up: 0.28}}, 22: {error: {dn: -0.26, up: 0.26}}, 23: {error: {dn: -0.25, up: 0.25}}, 24: {error: {dn: -0.24, up: 0.24}}, 25: {error: {dn: -0.23, up: 0.23}}, 26: {error: {dn: -0.23, up: 0.23}}, 27: {error: {dn: -0.21, up: 0.21}}, 28: {error: {dn: -0.2, up: 0.2}}, 29: {error: {dn: -0.2, up: 0.2}}, 30: {error: {dn: -0.2, up: 0.2}}, 31: {error: {dn: -0.19, up: 0.19}}, 32: {error: {dn: -0.18, up: 0.18}}, 33: {error: {dn: -0.17, up: 0.17}}, 34: {error: {dn: -0.17, up: 0.17}}, 35: {error: {dn: -0.16, up: 0.16}}, 36: {error: {dn: -0.15, up: 0.15}}, 37: {error: {dn: -0.15, up: 0.15}}, 38: {error: {dn: -0.15, up: 0.15}}, 39: {error: {dn: -0.14, up: 0.14}}, 40: {error: {dn: -0.14, up: 0.14}}, 41: {error: {dn: -0.14, up: 0.14}}, 42: {error: {dn: -0.14, up: 0.14}}, 43: {error: {dn: -0.14, up: 0.14}}, 44: {error: {dn: -0.13, up: 0.13}}, 45: {error: {dn: -0.12, up: 0.12}}, 46: {error: {dn: -0.12, up: 0.12}}, 47: {error: {dn: -0.11, up: 0.11}}, 48: {error: {dn: -0.1, up: 0.1}}, 49: {error: {dn: -0.1, up: 0.1}}, 50: {error: {dn: -0.1, up: 0.1}}, 51: {error: {dn: -0.1, up: 0.1}}, 52: {error: {dn: -0.09, up: 0.09}}, 53: {error: {dn: -0.1, up: 0.1}}, 54: {error: {dn: -0.1, up: 0.1}}, 55: {error: {dn: -0.09, up: 0.09}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I758568/d03-x01-y01 +Title: doi:10.17182/hepdata.51824.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.150000e+00 1.250000e-02 1.250000e-02 0.000000e+00 9.000000e-02 9.000000e-02 +1.175000e+00 1.250000e-02 1.250000e-02 0.000000e+00 5.000000e-02 5.000000e-02 +1.200000e+00 1.250000e-02 1.250000e-02 6.000000e-02 8.000000e-02 8.000000e-02 +1.225000e+00 1.250000e-02 1.250000e-02 0.000000e+00 1.200000e-01 1.200000e-01 +1.250000e+00 1.250000e-02 1.250000e-02 1.500000e-01 1.400000e-01 1.400000e-01 +1.275000e+00 1.250000e-02 1.250000e-02 2.300000e-01 1.400000e-01 1.400000e-01 +1.300000e+00 1.250000e-02 1.250000e-02 3.000000e-01 1.500000e-01 1.500000e-01 +1.325000e+00 1.250000e-02 1.250000e-02 3.300000e-01 1.600000e-01 1.600000e-01 +1.350000e+00 1.250000e-02 1.250000e-02 5.500000e-01 2.000000e-01 2.000000e-01 +1.375000e+00 1.250000e-02 1.250000e-02 8.800000e-01 2.000000e-01 2.000000e-01 +1.400000e+00 1.250000e-02 1.250000e-02 6.900000e-01 2.200000e-01 2.200000e-01 +1.425000e+00 1.250000e-02 1.250000e-02 8.300000e-01 2.400000e-01 2.400000e-01 +1.450000e+00 1.250000e-02 1.250000e-02 1.170000e+00 2.300000e-01 2.300000e-01 +1.475000e+00 1.250000e-02 1.250000e-02 9.500000e-01 2.500000e-01 2.500000e-01 +1.500000e+00 1.250000e-02 1.250000e-02 1.060000e+00 2.500000e-01 2.500000e-01 +1.525000e+00 1.250000e-02 1.250000e-02 1.330000e+00 2.400000e-01 2.400000e-01 +1.550000e+00 1.250000e-02 1.250000e-02 1.670000e+00 2.700000e-01 2.700000e-01 +1.575000e+00 1.250000e-02 1.250000e-02 1.300000e+00 2.700000e-01 2.700000e-01 +1.600000e+00 1.250000e-02 1.250000e-02 2.100000e+00 2.800000e-01 2.800000e-01 +1.625000e+00 1.250000e-02 1.250000e-02 2.210000e+00 2.900000e-01 2.900000e-01 +1.650000e+00 1.250000e-02 1.250000e-02 2.800000e+00 3.000000e-01 3.000000e-01 +1.675000e+00 1.250000e-02 1.250000e-02 2.190000e+00 2.800000e-01 2.800000e-01 +1.700000e+00 1.250000e-02 1.250000e-02 1.990000e+00 2.600000e-01 2.600000e-01 +1.725000e+00 1.250000e-02 1.250000e-02 1.380000e+00 2.500000e-01 2.500000e-01 +1.750000e+00 1.250000e-02 1.250000e-02 1.510000e+00 2.400000e-01 2.400000e-01 +1.775000e+00 1.250000e-02 1.250000e-02 1.450000e+00 2.300000e-01 2.300000e-01 +1.800000e+00 1.250000e-02 1.250000e-02 1.180000e+00 2.300000e-01 2.300000e-01 +1.825000e+00 1.250000e-02 1.250000e-02 1.190000e+00 2.100000e-01 2.100000e-01 +1.850000e+00 1.250000e-02 1.250000e-02 7.900000e-01 2.000000e-01 2.000000e-01 +1.875000e+00 1.250000e-02 1.250000e-02 8.400000e-01 2.000000e-01 2.000000e-01 +1.900000e+00 1.250000e-02 1.250000e-02 9.500000e-01 2.000000e-01 2.000000e-01 +1.925000e+00 1.250000e-02 1.250000e-02 6.100000e-01 1.900000e-01 1.900000e-01 +1.950000e+00 1.250000e-02 1.250000e-02 2.800000e-01 1.800000e-01 1.800000e-01 +1.975000e+00 1.250000e-02 1.250000e-02 6.900000e-01 1.700000e-01 1.700000e-01 +2.000000e+00 1.250000e-02 1.250000e-02 1.100000e-01 1.700000e-01 1.700000e-01 +2.025000e+00 1.250000e-02 1.250000e-02 4.900000e-01 1.600000e-01 1.600000e-01 +2.050000e+00 1.250000e-02 1.250000e-02 7.000000e-01 1.500000e-01 1.500000e-01 +2.075000e+00 1.250000e-02 1.250000e-02 4.000000e-01 1.500000e-01 1.500000e-01 +2.100000e+00 1.250000e-02 1.250000e-02 3.500000e-01 1.500000e-01 1.500000e-01 +2.125000e+00 1.250000e-02 1.250000e-02 2.600000e-01 1.400000e-01 1.400000e-01 +2.150000e+00 1.250000e-02 1.250000e-02 5.600000e-01 1.400000e-01 1.400000e-01 +2.175000e+00 1.250000e-02 1.250000e-02 4.300000e-01 1.400000e-01 1.400000e-01 +2.200000e+00 1.250000e-02 1.250000e-02 1.100000e-01 1.400000e-01 1.400000e-01 +2.225000e+00 1.250000e-02 1.250000e-02 5.200000e-01 1.400000e-01 1.400000e-01 +2.250000e+00 1.250000e-02 1.250000e-02 3.500000e-01 1.300000e-01 1.300000e-01 +2.275000e+00 1.250000e-02 1.250000e-02 2.700000e-01 1.200000e-01 1.200000e-01 +2.300000e+00 1.250000e-02 1.250000e-02 -4.000000e-02 1.200000e-01 1.200000e-01 +2.325000e+00 1.250000e-02 1.250000e-02 1.100000e-01 1.100000e-01 1.100000e-01 +2.350000e+00 1.250000e-02 1.250000e-02 -3.000000e-02 1.000000e-01 1.000000e-01 +2.375000e+00 1.250000e-02 1.250000e-02 0.000000e+00 1.000000e-01 1.000000e-01 +2.400000e+00 1.250000e-02 1.250000e-02 5.000000e-02 1.000000e-01 1.000000e-01 +2.425000e+00 1.250000e-02 1.250000e-02 2.000000e-02 1.000000e-01 1.000000e-01 +2.450000e+00 1.250000e-02 1.250000e-02 -4.000000e-02 9.000000e-02 9.000000e-02 +2.475000e+00 1.250000e-02 1.250000e-02 5.000000e-02 1.000000e-01 1.000000e-01 +2.500000e+00 1.250000e-02 1.250000e-02 2.000000e-02 1.000000e-01 1.000000e-01 +2.525000e+00 1.250000e-02 1.250000e-02 1.500000e-01 9.000000e-02 9.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d04-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.14, up: 0.14}}, 1: {error: {dn: -0.14, up: 0.14}}, 2: {error: {dn: -0.18, up: 0.18}}, 3: {error: {dn: -0.17, up: 0.17}}, 4: {error: {dn: -0.2, up: 0.2}}, 5: {error: {dn: -0.17, up: 0.17}}, 6: {error: {dn: -0.16, up: 0.16}}, 7: {error: {dn: -0.16, up: 0.16}}, 8: {error: {dn: -0.18, up: 0.18}}, 9: {error: {dn: -0.16, up: 0.16}}, 10: {error: {dn: -0.15, up: 0.15}}, 11: {error: {dn: -0.15, up: 0.15}}, 12: {error: {dn: -0.12, up: 0.12}}, 13: {error: {dn: -0.12, up: 0.12}}, 14: {error: {dn: -0.1, up: 0.1}}, 15: {error: {dn: -0.12, up: 0.12}}, 16: {error: {dn: -0.11, up: 0.11}}, 17: {error: {dn: -0.11, up: 0.11}}, 18: {error: {dn: -0.11, up: 0.11}}, 19: {error: {dn: -0.1, up: 0.1}}, 20: {error: {dn: -0.09, up: 0.09}}, 21: {error: {dn: -0.11, up: 0.11}}, 22: {error: {dn: -0.09, up: 0.09}}, 23: {error: {dn: -0.08, up: 0.08}}, 24: {error: {dn: -0.07, up: 0.07}}, 25: {error: {dn: -0.06, up: 0.06}}, 26: {error: {dn: -0.05, up: 0.05}}, 27: {error: {dn: -0.05, up: 0.05}}, 28: {error: {dn: -0.05, up: 0.05}}, 29: {error: {dn: -0.05, up: 0.05}}, 30: {error: {dn: -0.04, up: 0.04}}, 31: {error: {dn: -0.05, up: 0.05}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I758568/d04-x01-y01 +Title: doi:10.17182/hepdata.51824.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.700000e+00 1.250000e-02 1.250000e-02 2.000000e-02 1.400000e-01 1.400000e-01 +1.725000e+00 1.250000e-02 1.250000e-02 2.000000e-02 1.400000e-01 1.400000e-01 +1.750000e+00 1.250000e-02 1.250000e-02 1.000000e-01 1.800000e-01 1.800000e-01 +1.775000e+00 1.250000e-02 1.250000e-02 7.900000e-01 1.700000e-01 1.700000e-01 +1.800000e+00 1.250000e-02 1.250000e-02 8.900000e-01 2.000000e-01 2.000000e-01 +1.825000e+00 1.250000e-02 1.250000e-02 9.100000e-01 1.700000e-01 1.700000e-01 +1.850000e+00 1.250000e-02 1.250000e-02 4.500000e-01 1.600000e-01 1.600000e-01 +1.875000e+00 1.250000e-02 1.250000e-02 4.600000e-01 1.600000e-01 1.600000e-01 +1.900000e+00 1.250000e-02 1.250000e-02 5.100000e-01 1.800000e-01 1.800000e-01 +1.925000e+00 1.250000e-02 1.250000e-02 4.800000e-01 1.600000e-01 1.600000e-01 +1.950000e+00 1.250000e-02 1.250000e-02 3.200000e-01 1.500000e-01 1.500000e-01 +1.975000e+00 1.250000e-02 1.250000e-02 4.200000e-01 1.500000e-01 1.500000e-01 +2.000000e+00 1.250000e-02 1.250000e-02 1.700000e-01 1.200000e-01 1.200000e-01 +2.025000e+00 1.250000e-02 1.250000e-02 3.400000e-01 1.200000e-01 1.200000e-01 +2.050000e+00 1.250000e-02 1.250000e-02 2.700000e-01 1.000000e-01 1.000000e-01 +2.075000e+00 1.250000e-02 1.250000e-02 2.700000e-01 1.200000e-01 1.200000e-01 +2.100000e+00 1.250000e-02 1.250000e-02 3.900000e-01 1.100000e-01 1.100000e-01 +2.125000e+00 1.250000e-02 1.250000e-02 1.800000e-01 1.100000e-01 1.100000e-01 +2.150000e+00 1.250000e-02 1.250000e-02 3.100000e-01 1.100000e-01 1.100000e-01 +2.175000e+00 1.250000e-02 1.250000e-02 1.400000e-01 1.000000e-01 1.000000e-01 +2.200000e+00 1.250000e-02 1.250000e-02 1.700000e-01 9.000000e-02 9.000000e-02 +2.225000e+00 1.250000e-02 1.250000e-02 1.100000e-01 1.100000e-01 1.100000e-01 +2.250000e+00 1.250000e-02 1.250000e-02 3.000000e-02 9.000000e-02 9.000000e-02 +2.275000e+00 1.250000e-02 1.250000e-02 2.000000e-02 8.000000e-02 8.000000e-02 +2.300000e+00 1.250000e-02 1.250000e-02 6.000000e-02 7.000000e-02 7.000000e-02 +2.325000e+00 1.250000e-02 1.250000e-02 1.500000e-01 6.000000e-02 6.000000e-02 +2.350000e+00 1.250000e-02 1.250000e-02 2.000000e-02 5.000000e-02 5.000000e-02 +2.375000e+00 1.250000e-02 1.250000e-02 3.000000e-02 5.000000e-02 5.000000e-02 +2.400000e+00 1.250000e-02 1.250000e-02 6.000000e-02 5.000000e-02 5.000000e-02 +2.425000e+00 1.250000e-02 1.250000e-02 7.000000e-02 5.000000e-02 5.000000e-02 +2.450000e+00 1.250000e-02 1.250000e-02 1.000000e-02 4.000000e-02 4.000000e-02 +2.475000e+00 1.250000e-02 1.250000e-02 1.000000e-02 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d05-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.0, up: 0.0}}, 1: {error: {dn: -0.04, up: 0.04}}, 2: {error: {dn: -0.0, up: 0.0}}, 3: {error: {dn: -0.04, up: 0.04}}, 4: {error: {dn: -0.07, up: 0.07}}, 5: {error: {dn: -0.06, up: 0.06}}, 6: {error: {dn: -0.07, up: 0.07}}, 7: {error: {dn: -0.07, up: 0.07}}, 8: {error: {dn: -0.05, up: 0.05}}, 9: {error: {dn: -0.07, up: 0.07}}, 10: {error: {dn: -0.06, up: 0.06}}, 11: {error: {dn: -0.07, up: 0.07}}, 12: {error: {dn: -0.08, up: 0.08}}, 13: {error: {dn: -0.08, up: 0.08}}, 14: {error: {dn: -0.09, up: 0.09}}, 15: {error: {dn: -0.08, up: 0.08}}, 16: {error: {dn: -0.1, up: 0.1}}, 17: {error: {dn: -0.08, up: 0.08}}, 18: {error: {dn: -0.12, up: 0.12}}, 19: {error: {dn: -0.13, up: 0.13}}, 20: {error: {dn: -0.11, up: 0.11}}, 21: {error: {dn: -0.16, up: 0.16}}, 22: {error: {dn: -0.13, up: 0.13}}, 23: {error: {dn: -0.14, up: 0.14}}, 24: {error: {dn: -0.15, up: 0.15}}, 25: {error: {dn: -0.17, up: 0.17}}, 26: {error: {dn: -0.15, up: 0.15}}, 27: {error: {dn: -0.17, up: 0.17}}, 28: {error: {dn: -0.17, up: 0.17}}, 29: {error: {dn: -0.19, up: 0.19}}, 30: {error: {dn: -0.2, up: 0.2}}, 31: {error: {dn: -0.19, up: 0.19}}, 32: {error: {dn: -0.18, up: 0.18}}, 33: {error: {dn: -0.18, up: 0.18}}, 34: {error: {dn: -0.2, up: 0.2}}, 35: {error: {dn: -0.19, up: 0.19}}, 36: {error: {dn: -0.18, up: 0.18}}, 37: {error: {dn: -0.19, up: 0.19}}, 38: {error: {dn: -0.18, up: 0.18}}, 39: {error: {dn: -0.17, up: 0.17}}, 40: {error: {dn: -0.17, up: 0.17}}, 41: {error: {dn: -0.18, up: 0.18}}, 42: {error: {dn: -0.18, up: 0.18}}, 43: {error: {dn: -0.17, up: 0.17}}, 44: {error: {dn: -0.17, up: 0.17}}, 45: {error: {dn: -0.17, up: 0.17}}, 46: {error: {dn: -0.17, up: 0.17}}, 47: {error: {dn: -0.17, up: 0.17}}, 48: {error: {dn: -0.16, up: 0.16}}, 49: {error: {dn: -0.17, up: 0.17}}, 50: {error: {dn: -0.16, up: 0.16}}, 51: {error: {dn: -0.16, up: 0.16}}, 52: {error: {dn: -0.15, up: 0.15}}, 53: {error: {dn: -0.14, up: 0.14}}, 54: {error: {dn: -0.15, up: 0.15}}, 55: {error: {dn: -0.16, up: 0.16}}, 56: {error: {dn: -0.13, up: 0.13}}, 57: {error: {dn: -0.14, up: 0.14}}, 58: {error: {dn: -0.15, up: 0.15}}, 59: {error: {dn: -0.15, up: 0.15}}, 60: {error: {dn: -0.14, up: 0.14}}, 61: {error: {dn: -0.13, up: 0.13}}, 62: {error: {dn: -0.14, up: 0.14}}, 63: {error: {dn: -0.14, up: 0.14}}, 64: {error: {dn: -0.13, up: 0.13}}, 65: {error: {dn: -0.14, up: 0.14}}, 66: {error: {dn: -0.14, up: 0.14}}, 67: {error: {dn: -0.14, up: 0.14}}, 68: {error: {dn: -0.13, up: 0.13}}, 69: {error: {dn: -0.14, up: 0.14}}, 70: {error: {dn: -0.13, up: 0.13}}, 71: {error: {dn: -0.19, up: 0.19}}, 72: {error: {dn: -0.16, up: 0.16}}, 73: {error: {dn: -0.12, up: 0.12}}, 74: {error: {dn: -0.12, up: 0.12}}, 75: {error: {dn: -0.14, up: 0.14}}, 76: {error: {dn: -0.12, up: 0.12}}, 77: {error: {dn: -0.12, up: 0.12}}, 78: {error: {dn: -0.11, up: 0.11}}, 79: {error: {dn: -0.11, up: 0.11}}, 80: {error: {dn: -0.09, up: 0.09}}, 81: {error: {dn: -0.11, up: 0.11}}, 82: {error: {dn: -0.09, up: 0.09}}, 83: {error: {dn: -0.11, up: 0.11}}, 84: {error: {dn: -0.1, up: 0.1}}, 85: {error: {dn: -0.11, up: 0.11}}, 86: {error: {dn: -0.1, up: 0.1}}, 87: {error: {dn: -0.1, up: 0.1}}, 88: {error: {dn: -0.09, up: 0.09}}, 89: {error: {dn: -0.09, up: 0.09}}, 90: {error: {dn: -0.09, up: 0.09}}, 91: {error: {dn: -0.09, up: 0.09}}, 92: {error: {dn: -0.08, up: 0.08}}, 93: {error: {dn: -0.08, up: 0.08}}, 94: {error: {dn: -0.08, up: 0.08}}, 95: {error: {dn: -0.09, up: 0.09}}, 96: {error: {dn: -0.08, up: 0.08}}, 97: {error: {dn: -0.07, up: 0.07}}, 98: {error: {dn: -0.08, up: 0.08}}, 99: {error: {dn: -0.08, up: 0.08}}, 100: {error: {dn: -0.08, up: 0.08}}, 101: {error: {dn: -0.07, up: 0.07}}, 102: {error: {dn: -0.08, up: 0.08}}, 103: {error: {dn: -0.07, up: 0.07}}, 104: {error: {dn: -0.08, up: 0.08}}, 105: {error: {dn: -0.07, up: 0.07}}, 106: {error: {dn: -0.08, up: 0.08}}, 107: {error: {dn: -0.06, up: 0.06}}, 108: {error: {dn: -0.07, up: 0.07}}, 109: {error: {dn: -0.06, up: 0.06}}, 110: {error: {dn: -0.06, up: 0.06}}, 111: {error: {dn: -0.06, up: 0.06}}, 112: {error: {dn: -0.05, up: 0.05}}, 113: {error: {dn: -0.07, up: 0.07}}, 114: {error: {dn: -0.07, up: 0.07}}, 115: {error: {dn: -0.05, up: 0.05}}, 116: {error: {dn: -0.07, up: 0.07}}, 117: {error: {dn: -0.06, up: 0.06}}, 118: {error: {dn: -0.06, up: 0.06}}, 119: {error: {dn: -0.07, up: 0.07}}, 120: {error: {dn: -0.06, up: 0.06}}, 121: {error: {dn: -0.06, up: 0.06}}, 122: {error: {dn: -0.07, up: 0.07}}, 123: {error: {dn: -0.06, up: 0.06}}, 124: {error: {dn: -0.06, up: 0.06}}, 125: {error: {dn: -0.06, up: 0.06}}, 126: {error: {dn: -0.07, up: 0.07}}, 127: {error: {dn: -0.06, up: 0.06}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I758568/d05-x01-y01 +Title: doi:10.17182/hepdata.51824.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.312500e+00 1.250000e-02 1.250000e-02 0.000000e+00 0.000000e+00 0.000000e+00 +1.337500e+00 1.250000e-02 1.250000e-02 4.000000e-02 4.000000e-02 4.000000e-02 +1.362500e+00 1.250000e-02 1.250000e-02 0.000000e+00 0.000000e+00 0.000000e+00 +1.387500e+00 1.250000e-02 1.250000e-02 4.000000e-02 4.000000e-02 4.000000e-02 +1.412500e+00 1.250000e-02 1.250000e-02 1.100000e-01 7.000000e-02 7.000000e-02 +1.437500e+00 1.250000e-02 1.250000e-02 5.000000e-02 6.000000e-02 6.000000e-02 +1.462500e+00 1.250000e-02 1.250000e-02 0.000000e+00 7.000000e-02 7.000000e-02 +1.487500e+00 1.250000e-02 1.250000e-02 8.000000e-02 7.000000e-02 7.000000e-02 +1.512500e+00 1.250000e-02 1.250000e-02 7.000000e-02 5.000000e-02 5.000000e-02 +1.537500e+00 1.250000e-02 1.250000e-02 1.000000e-02 7.000000e-02 7.000000e-02 +1.562500e+00 1.250000e-02 1.250000e-02 -6.000000e-02 6.000000e-02 6.000000e-02 +1.587500e+00 1.250000e-02 1.250000e-02 6.000000e-02 7.000000e-02 7.000000e-02 +1.612500e+00 1.250000e-02 1.250000e-02 -1.000000e-02 8.000000e-02 8.000000e-02 +1.637500e+00 1.250000e-02 1.250000e-02 -8.000000e-02 8.000000e-02 8.000000e-02 +1.662500e+00 1.250000e-02 1.250000e-02 8.000000e-02 9.000000e-02 9.000000e-02 +1.687500e+00 1.250000e-02 1.250000e-02 9.000000e-02 8.000000e-02 8.000000e-02 +1.712500e+00 1.250000e-02 1.250000e-02 1.800000e-01 1.000000e-01 1.000000e-01 +1.737500e+00 1.250000e-02 1.250000e-02 -4.000000e-02 8.000000e-02 8.000000e-02 +1.762500e+00 1.250000e-02 1.250000e-02 2.200000e-01 1.200000e-01 1.200000e-01 +1.787500e+00 1.250000e-02 1.250000e-02 3.100000e-01 1.300000e-01 1.300000e-01 +1.812500e+00 1.250000e-02 1.250000e-02 3.900000e-01 1.100000e-01 1.100000e-01 +1.837500e+00 1.250000e-02 1.250000e-02 6.300000e-01 1.600000e-01 1.600000e-01 +1.862500e+00 1.250000e-02 1.250000e-02 3.100000e-01 1.300000e-01 1.300000e-01 +1.887500e+00 1.250000e-02 1.250000e-02 2.700000e-01 1.400000e-01 1.400000e-01 +1.912500e+00 1.250000e-02 1.250000e-02 6.900000e-01 1.500000e-01 1.500000e-01 +1.937500e+00 1.250000e-02 1.250000e-02 5.900000e-01 1.700000e-01 1.700000e-01 +1.962500e+00 1.250000e-02 1.250000e-02 5.000000e-01 1.500000e-01 1.500000e-01 +1.987500e+00 1.250000e-02 1.250000e-02 8.800000e-01 1.700000e-01 1.700000e-01 +2.012500e+00 1.250000e-02 1.250000e-02 5.400000e-01 1.700000e-01 1.700000e-01 +2.037500e+00 1.250000e-02 1.250000e-02 8.700000e-01 1.900000e-01 1.900000e-01 +2.062500e+00 1.250000e-02 1.250000e-02 1.320000e+00 2.000000e-01 2.000000e-01 +2.087500e+00 1.250000e-02 1.250000e-02 9.900000e-01 1.900000e-01 1.900000e-01 +2.112500e+00 1.250000e-02 1.250000e-02 8.400000e-01 1.800000e-01 1.800000e-01 +2.137500e+00 1.250000e-02 1.250000e-02 1.100000e+00 1.800000e-01 1.800000e-01 +2.162500e+00 1.250000e-02 1.250000e-02 1.030000e+00 2.000000e-01 2.000000e-01 +2.187500e+00 1.250000e-02 1.250000e-02 1.230000e+00 1.900000e-01 1.900000e-01 +2.212500e+00 1.250000e-02 1.250000e-02 9.600000e-01 1.800000e-01 1.800000e-01 +2.237500e+00 1.250000e-02 1.250000e-02 1.150000e+00 1.900000e-01 1.900000e-01 +2.262500e+00 1.250000e-02 1.250000e-02 1.210000e+00 1.800000e-01 1.800000e-01 +2.287500e+00 1.250000e-02 1.250000e-02 8.500000e-01 1.700000e-01 1.700000e-01 +2.312500e+00 1.250000e-02 1.250000e-02 1.000000e+00 1.700000e-01 1.700000e-01 +2.337500e+00 1.250000e-02 1.250000e-02 1.250000e+00 1.800000e-01 1.800000e-01 +2.362500e+00 1.250000e-02 1.250000e-02 1.280000e+00 1.800000e-01 1.800000e-01 +2.387500e+00 1.250000e-02 1.250000e-02 7.400000e-01 1.700000e-01 1.700000e-01 +2.412500e+00 1.250000e-02 1.250000e-02 9.900000e-01 1.700000e-01 1.700000e-01 +2.437500e+00 1.250000e-02 1.250000e-02 9.200000e-01 1.700000e-01 1.700000e-01 +2.462500e+00 1.250000e-02 1.250000e-02 9.100000e-01 1.700000e-01 1.700000e-01 +2.487500e+00 1.250000e-02 1.250000e-02 9.500000e-01 1.700000e-01 1.700000e-01 +2.512500e+00 1.250000e-02 1.250000e-02 6.800000e-01 1.600000e-01 1.600000e-01 +2.537500e+00 1.250000e-02 1.250000e-02 8.000000e-01 1.700000e-01 1.700000e-01 +2.562500e+00 1.250000e-02 1.250000e-02 8.600000e-01 1.600000e-01 1.600000e-01 +2.587500e+00 1.250000e-02 1.250000e-02 6.300000e-01 1.600000e-01 1.600000e-01 +2.612500e+00 1.250000e-02 1.250000e-02 5.300000e-01 1.500000e-01 1.500000e-01 +2.637500e+00 1.250000e-02 1.250000e-02 6.500000e-01 1.400000e-01 1.400000e-01 +2.662500e+00 1.250000e-02 1.250000e-02 8.100000e-01 1.500000e-01 1.500000e-01 +2.687500e+00 1.250000e-02 1.250000e-02 7.300000e-01 1.600000e-01 1.600000e-01 +2.712500e+00 1.250000e-02 1.250000e-02 4.300000e-01 1.300000e-01 1.300000e-01 +2.737500e+00 1.250000e-02 1.250000e-02 4.600000e-01 1.400000e-01 1.400000e-01 +2.762500e+00 1.250000e-02 1.250000e-02 6.400000e-01 1.500000e-01 1.500000e-01 +2.787500e+00 1.250000e-02 1.250000e-02 6.500000e-01 1.500000e-01 1.500000e-01 +2.812500e+00 1.250000e-02 1.250000e-02 6.100000e-01 1.400000e-01 1.400000e-01 +2.837500e+00 1.250000e-02 1.250000e-02 3.900000e-01 1.300000e-01 1.300000e-01 +2.862500e+00 1.250000e-02 1.250000e-02 5.400000e-01 1.400000e-01 1.400000e-01 +2.887500e+00 1.250000e-02 1.250000e-02 6.500000e-01 1.400000e-01 1.400000e-01 +2.912500e+00 1.250000e-02 1.250000e-02 3.000000e-01 1.300000e-01 1.300000e-01 +2.937500e+00 1.250000e-02 1.250000e-02 5.200000e-01 1.400000e-01 1.400000e-01 +2.962500e+00 1.250000e-02 1.250000e-02 3.300000e-01 1.400000e-01 1.400000e-01 +2.987500e+00 1.250000e-02 1.250000e-02 6.900000e-01 1.400000e-01 1.400000e-01 +3.012500e+00 1.250000e-02 1.250000e-02 1.300000e-01 1.300000e-01 1.300000e-01 +3.037500e+00 1.250000e-02 1.250000e-02 6.500000e-01 1.400000e-01 1.400000e-01 +3.062500e+00 1.250000e-02 1.250000e-02 4.300000e-01 1.300000e-01 1.300000e-01 +3.087500e+00 1.250000e-02 1.250000e-02 1.450000e+00 1.900000e-01 1.900000e-01 +3.112500e+00 1.250000e-02 1.250000e-02 8.900000e-01 1.600000e-01 1.600000e-01 +3.137500e+00 1.250000e-02 1.250000e-02 4.700000e-01 1.200000e-01 1.200000e-01 +3.162500e+00 1.250000e-02 1.250000e-02 4.800000e-01 1.200000e-01 1.200000e-01 +3.187500e+00 1.250000e-02 1.250000e-02 4.800000e-01 1.400000e-01 1.400000e-01 +3.212500e+00 1.250000e-02 1.250000e-02 5.800000e-01 1.200000e-01 1.200000e-01 +3.237500e+00 1.250000e-02 1.250000e-02 3.900000e-01 1.200000e-01 1.200000e-01 +3.262500e+00 1.250000e-02 1.250000e-02 2.500000e-01 1.100000e-01 1.100000e-01 +3.287500e+00 1.250000e-02 1.250000e-02 3.100000e-01 1.100000e-01 1.100000e-01 +3.312500e+00 1.250000e-02 1.250000e-02 1.600000e-01 9.000000e-02 9.000000e-02 +3.337500e+00 1.250000e-02 1.250000e-02 1.200000e-01 1.100000e-01 1.100000e-01 +3.362500e+00 1.250000e-02 1.250000e-02 1.400000e-01 9.000000e-02 9.000000e-02 +3.387500e+00 1.250000e-02 1.250000e-02 1.900000e-01 1.100000e-01 1.100000e-01 +3.412500e+00 1.250000e-02 1.250000e-02 1.200000e-01 1.000000e-01 1.000000e-01 +3.437500e+00 1.250000e-02 1.250000e-02 4.200000e-01 1.100000e-01 1.100000e-01 +3.462500e+00 1.250000e-02 1.250000e-02 3.200000e-01 1.000000e-01 1.000000e-01 +3.487500e+00 1.250000e-02 1.250000e-02 1.300000e-01 1.000000e-01 1.000000e-01 +3.512500e+00 1.250000e-02 1.250000e-02 1.200000e-01 9.000000e-02 9.000000e-02 +3.537500e+00 1.250000e-02 1.250000e-02 1.900000e-01 9.000000e-02 9.000000e-02 +3.562500e+00 1.250000e-02 1.250000e-02 2.200000e-01 9.000000e-02 9.000000e-02 +3.587500e+00 1.250000e-02 1.250000e-02 2.200000e-01 9.000000e-02 9.000000e-02 +3.612500e+00 1.250000e-02 1.250000e-02 1.300000e-01 8.000000e-02 8.000000e-02 +3.637500e+00 1.250000e-02 1.250000e-02 1.200000e-01 8.000000e-02 8.000000e-02 +3.662500e+00 1.250000e-02 1.250000e-02 1.900000e-01 8.000000e-02 8.000000e-02 +3.687500e+00 1.250000e-02 1.250000e-02 3.400000e-01 9.000000e-02 9.000000e-02 +3.712500e+00 1.250000e-02 1.250000e-02 2.100000e-01 8.000000e-02 8.000000e-02 +3.737500e+00 1.250000e-02 1.250000e-02 1.000000e-01 7.000000e-02 7.000000e-02 +3.762500e+00 1.250000e-02 1.250000e-02 4.000000e-02 8.000000e-02 8.000000e-02 +3.787500e+00 1.250000e-02 1.250000e-02 2.000000e-02 8.000000e-02 8.000000e-02 +3.812500e+00 1.250000e-02 1.250000e-02 1.300000e-01 8.000000e-02 8.000000e-02 +3.837500e+00 1.250000e-02 1.250000e-02 6.000000e-02 7.000000e-02 7.000000e-02 +3.862500e+00 1.250000e-02 1.250000e-02 1.300000e-01 8.000000e-02 8.000000e-02 +3.887500e+00 1.250000e-02 1.250000e-02 6.000000e-02 7.000000e-02 7.000000e-02 +3.912500e+00 1.250000e-02 1.250000e-02 1.800000e-01 8.000000e-02 8.000000e-02 +3.937500e+00 1.250000e-02 1.250000e-02 2.000000e-02 7.000000e-02 7.000000e-02 +3.962500e+00 1.250000e-02 1.250000e-02 1.500000e-01 8.000000e-02 8.000000e-02 +3.987500e+00 1.250000e-02 1.250000e-02 1.000000e-01 6.000000e-02 6.000000e-02 +4.012500e+00 1.250000e-02 1.250000e-02 1.000000e-01 7.000000e-02 7.000000e-02 +4.037500e+00 1.250000e-02 1.250000e-02 -2.000000e-02 6.000000e-02 6.000000e-02 +4.062500e+00 1.250000e-02 1.250000e-02 1.100000e-01 6.000000e-02 6.000000e-02 +4.087500e+00 1.250000e-02 1.250000e-02 1.000000e-01 6.000000e-02 6.000000e-02 +4.112500e+00 1.250000e-02 1.250000e-02 -2.000000e-02 5.000000e-02 5.000000e-02 +4.137500e+00 1.250000e-02 1.250000e-02 4.000000e-02 7.000000e-02 7.000000e-02 +4.162500e+00 1.250000e-02 1.250000e-02 5.000000e-02 7.000000e-02 7.000000e-02 +4.187500e+00 1.250000e-02 1.250000e-02 6.000000e-02 5.000000e-02 5.000000e-02 +4.212500e+00 1.250000e-02 1.250000e-02 6.000000e-02 7.000000e-02 7.000000e-02 +4.237500e+00 1.250000e-02 1.250000e-02 1.600000e-01 6.000000e-02 6.000000e-02 +4.262500e+00 1.250000e-02 1.250000e-02 4.000000e-02 6.000000e-02 6.000000e-02 +4.287500e+00 1.250000e-02 1.250000e-02 3.000000e-02 7.000000e-02 7.000000e-02 +4.312500e+00 1.250000e-02 1.250000e-02 4.000000e-02 6.000000e-02 6.000000e-02 +4.337500e+00 1.250000e-02 1.250000e-02 9.000000e-02 6.000000e-02 6.000000e-02 +4.362500e+00 1.250000e-02 1.250000e-02 -1.000000e-02 7.000000e-02 7.000000e-02 +4.387500e+00 1.250000e-02 1.250000e-02 -6.000000e-02 6.000000e-02 6.000000e-02 +4.412500e+00 1.250000e-02 1.250000e-02 -3.000000e-02 6.000000e-02 6.000000e-02 +4.437500e+00 1.250000e-02 1.250000e-02 1.000000e-01 6.000000e-02 6.000000e-02 +4.462500e+00 1.250000e-02 1.250000e-02 1.300000e-01 7.000000e-02 7.000000e-02 +4.487500e+00 1.250000e-02 1.250000e-02 7.000000e-02 6.000000e-02 6.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d06-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.05, up: 0.05}}, 1: {error: {dn: -0.03, up: 0.03}}, 2: {error: {dn: -0.06, up: 0.06}}, 3: {error: {dn: -0.06, up: 0.06}}, 4: {error: {dn: -0.07, up: 0.07}}, 5: {error: {dn: -0.06, up: 0.06}}, 6: {error: {dn: -0.08, up: 0.08}}, 7: {error: {dn: -0.06, up: 0.06}}, 8: {error: {dn: -0.05, up: 0.05}}, 9: {error: {dn: -0.05, up: 0.05}}, 10: {error: {dn: -0.04, up: 0.04}}, 11: {error: {dn: -0.05, up: 0.05}}, 12: {error: {dn: -0.04, up: 0.04}}, 13: {error: {dn: -0.03, up: 0.03}}, 14: {error: {dn: -0.02, up: 0.02}}, 15: {error: {dn: -0.02, up: 0.02}}, 16: {error: {dn: -0.02, up: 0.02}}, 17: {error: {dn: -0.02, up: 0.02}}, 18: {error: {dn: -0.03, up: 0.03}}, 19: {error: {dn: -0.03, up: 0.03}}, 20: {error: {dn: -0.02, up: 0.02}}, 21: {error: {dn: -0.02, up: 0.02}}, 22: {error: {dn: -0.02, up: 0.02}}, 23: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I758568/d06-x01-y01 +Title: doi:10.17182/hepdata.51824.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.580000e+00 4.000000e-02 4.000000e-02 2.000000e-02 5.000000e-02 5.000000e-02 +1.660000e+00 4.000000e-02 4.000000e-02 6.000000e-02 3.000000e-02 3.000000e-02 +1.740000e+00 4.000000e-02 4.000000e-02 1.000000e-02 6.000000e-02 6.000000e-02 +1.820000e+00 4.000000e-02 4.000000e-02 7.000000e-02 6.000000e-02 6.000000e-02 +1.900000e+00 4.000000e-02 4.000000e-02 1.100000e-01 7.000000e-02 7.000000e-02 +1.980000e+00 4.000000e-02 4.000000e-02 1.600000e-01 6.000000e-02 6.000000e-02 +2.060000e+00 4.000000e-02 4.000000e-02 2.400000e-01 8.000000e-02 8.000000e-02 +2.140000e+00 4.000000e-02 4.000000e-02 1.000000e-01 6.000000e-02 6.000000e-02 +2.220000e+00 4.000000e-02 4.000000e-02 1.100000e-01 5.000000e-02 5.000000e-02 +2.300000e+00 4.000000e-02 4.000000e-02 -5.000000e-02 5.000000e-02 5.000000e-02 +2.380000e+00 4.000000e-02 4.000000e-02 3.000000e-02 4.000000e-02 4.000000e-02 +2.460000e+00 4.000000e-02 4.000000e-02 9.000000e-02 5.000000e-02 5.000000e-02 +2.540000e+00 4.000000e-02 4.000000e-02 5.000000e-02 4.000000e-02 4.000000e-02 +2.620000e+00 4.000000e-02 4.000000e-02 3.000000e-02 3.000000e-02 3.000000e-02 +2.700000e+00 4.000000e-02 4.000000e-02 3.000000e-02 2.000000e-02 2.000000e-02 +2.780000e+00 4.000000e-02 4.000000e-02 -1.000000e-02 2.000000e-02 2.000000e-02 +2.860000e+00 4.000000e-02 4.000000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +2.940000e+00 4.000000e-02 4.000000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +3.020000e+00 4.000000e-02 4.000000e-02 7.000000e-02 3.000000e-02 3.000000e-02 +3.100000e+00 4.000000e-02 4.000000e-02 7.000000e-02 3.000000e-02 3.000000e-02 +3.180000e+00 4.000000e-02 4.000000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +3.260000e+00 4.000000e-02 4.000000e-02 7.000000e-02 2.000000e-02 2.000000e-02 +3.340000e+00 4.000000e-02 4.000000e-02 0.000000e+00 2.000000e-02 2.000000e-02 +3.420000e+00 4.000000e-02 4.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d07-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.0, up: 0.0}}, 1: {error: {dn: -0.11, up: 0.11}}, 2: {error: {dn: -0.18, up: 0.18}}, 3: {error: {dn: -0.2, up: 0.2}}, 4: {error: {dn: -0.23, up: 0.23}}, 5: {error: {dn: -0.24, up: 0.24}}, 6: {error: {dn: -0.24, up: 0.24}}, 7: {error: {dn: -0.24, up: 0.24}}, 8: {error: {dn: -0.21, up: 0.21}}, 9: {error: {dn: -0.17, up: 0.17}}, 10: {error: {dn: -0.16, up: 0.16}}, 11: {error: {dn: -0.12, up: 0.12}}, 12: {error: {dn: -0.12, up: 0.12}}, 13: {error: {dn: -0.1, up: 0.1}}, 14: {error: {dn: -0.1, up: 0.1}}, 15: {error: {dn: -0.08, up: 0.08}}, 16: {error: {dn: -0.06, up: 0.06}}, 17: {error: {dn: -0.08, up: 0.08}}, 18: {error: {dn: -0.08, up: 0.08}}, 19: {error: {dn: -0.05, up: 0.05}}, 20: {error: {dn: -0.04, up: 0.04}}, 21: {error: {dn: -0.03, up: 0.03}}, 22: {error: {dn: -0.05, up: 0.05}}, 23: {error: {dn: -0.04, up: 0.04}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I758568/d07-x01-y01 +Title: doi:10.17182/hepdata.51824.v1/t7 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.660000e+00 4.000000e-02 4.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 +1.740000e+00 4.000000e-02 4.000000e-02 1.000000e-02 1.100000e-01 1.100000e-01 +1.820000e+00 4.000000e-02 4.000000e-02 2.000000e-02 1.800000e-01 1.800000e-01 +1.900000e+00 4.000000e-02 4.000000e-02 3.500000e-01 2.000000e-01 2.000000e-01 +1.980000e+00 4.000000e-02 4.000000e-02 6.100000e-01 2.300000e-01 2.300000e-01 +2.060000e+00 4.000000e-02 4.000000e-02 5.900000e-01 2.400000e-01 2.400000e-01 +2.140000e+00 4.000000e-02 4.000000e-02 9.900000e-01 2.400000e-01 2.400000e-01 +2.220000e+00 4.000000e-02 4.000000e-02 8.900000e-01 2.400000e-01 2.400000e-01 +2.300000e+00 4.000000e-02 4.000000e-02 6.400000e-01 2.100000e-01 2.100000e-01 +2.380000e+00 4.000000e-02 4.000000e-02 5.400000e-01 1.700000e-01 1.700000e-01 +2.460000e+00 4.000000e-02 4.000000e-02 6.100000e-01 1.600000e-01 1.600000e-01 +2.540000e+00 4.000000e-02 4.000000e-02 2.500000e-01 1.200000e-01 1.200000e-01 +2.620000e+00 4.000000e-02 4.000000e-02 3.200000e-01 1.200000e-01 1.200000e-01 +2.700000e+00 4.000000e-02 4.000000e-02 1.300000e-01 1.000000e-01 1.000000e-01 +2.780000e+00 4.000000e-02 4.000000e-02 3.100000e-01 1.000000e-01 1.000000e-01 +2.860000e+00 4.000000e-02 4.000000e-02 2.500000e-01 8.000000e-02 8.000000e-02 +2.940000e+00 4.000000e-02 4.000000e-02 7.000000e-02 6.000000e-02 6.000000e-02 +3.020000e+00 4.000000e-02 4.000000e-02 2.400000e-01 8.000000e-02 8.000000e-02 +3.100000e+00 4.000000e-02 4.000000e-02 1.100000e-01 8.000000e-02 8.000000e-02 +3.180000e+00 4.000000e-02 4.000000e-02 8.000000e-02 5.000000e-02 5.000000e-02 +3.260000e+00 4.000000e-02 4.000000e-02 3.000000e-02 4.000000e-02 4.000000e-02 +3.340000e+00 4.000000e-02 4.000000e-02 2.000000e-02 3.000000e-02 3.000000e-02 +3.420000e+00 4.000000e-02 4.000000e-02 9.000000e-02 5.000000e-02 5.000000e-02 +3.500000e+00 4.000000e-02 4.000000e-02 5.000000e-02 4.000000e-02 4.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d08-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.04, up: 0.04}}, 1: {error: {dn: -0.06, up: 0.06}}, 2: {error: {dn: -0.08, up: 0.08}}, 3: {error: {dn: -0.1, up: 0.1}}, 4: {error: {dn: -0.08, up: 0.08}}, 5: {error: {dn: -0.06, up: 0.06}}, 6: {error: {dn: -0.1, up: 0.1}}, 7: {error: {dn: -0.07, up: 0.07}}, 8: {error: {dn: -0.09, up: 0.09}}, 9: {error: {dn: -0.09, up: 0.09}}, 10: {error: {dn: -0.09, up: 0.09}}, 11: {error: {dn: -0.09, up: 0.09}}, 12: {error: {dn: -0.11, up: 0.11}}, 13: {error: {dn: -0.11, up: 0.11}}, 14: {error: {dn: -0.11, up: 0.11}}, 15: {error: {dn: -0.11, up: 0.11}}, 16: {error: {dn: -0.1, up: 0.1}}, 17: {error: {dn: -0.11, up: 0.11}}, 18: {error: {dn: -0.13, up: 0.13}}, 19: {error: {dn: -0.11, up: 0.11}}, 20: {error: {dn: -0.12, up: 0.12}}, 21: {error: {dn: -0.12, up: 0.12}}, 22: {error: {dn: -0.12, up: 0.12}}, 23: {error: {dn: -0.13, up: 0.13}}, 24: {error: {dn: -0.11, up: 0.11}}, 25: {error: {dn: -0.12, up: 0.12}}, 26: {error: {dn: -0.11, up: 0.11}}, 27: {error: {dn: -0.13, up: 0.13}}, 28: {error: {dn: -0.12, up: 0.12}}, 29: {error: {dn: -0.13, up: 0.13}}, 30: {error: {dn: -0.13, up: 0.13}}, 31: {error: {dn: -0.13, up: 0.13}}, 32: {error: {dn: -0.13, up: 0.13}}, 33: {error: {dn: -0.13, up: 0.13}}, 34: {error: {dn: -0.13, up: 0.13}}, 35: {error: {dn: -0.14, up: 0.14}}, 36: {error: {dn: -0.14, up: 0.14}}, 37: {error: {dn: -0.15, up: 0.15}}, 38: {error: {dn: -0.14, up: 0.14}}, 39: {error: {dn: -0.12, up: 0.12}}, 40: {error: {dn: -0.15, up: 0.15}}, 41: {error: {dn: -0.13, up: 0.13}}, 42: {error: {dn: -0.12, up: 0.12}}, 43: {error: {dn: -0.14, up: 0.14}}, 44: {error: {dn: -0.13, up: 0.13}}, 45: {error: {dn: -0.13, up: 0.13}}, 46: {error: {dn: -0.13, up: 0.13}}, 47: {error: {dn: -0.14, up: 0.14}}, 48: {error: {dn: -0.13, up: 0.13}}, 49: {error: {dn: -0.13, up: 0.13}}, 50: {error: {dn: -0.13, up: 0.13}}, 51: {error: {dn: -0.14, up: 0.14}}, 52: {error: {dn: -0.13, up: 0.13}}, 53: {error: {dn: -0.14, up: 0.14}}, 54: {error: {dn: -0.13, up: 0.13}}, 55: {error: {dn: -0.15, up: 0.15}}, 56: {error: {dn: -0.14, up: 0.14}}, 57: {error: {dn: -0.13, up: 0.13}}, 58: {error: {dn: -0.15, up: 0.15}}, 59: {error: {dn: -0.34, up: 0.34}}, 60: {error: {dn: -0.28, up: 0.28}}, 61: {error: {dn: -0.15, up: 0.15}}, 62: {error: {dn: -0.15, up: 0.15}}, 63: {error: {dn: -0.13, up: 0.13}}, 64: {error: {dn: -0.13, up: 0.13}}, 65: {error: {dn: -0.14, up: 0.14}}, 66: {error: {dn: -0.12, up: 0.12}}, 67: {error: {dn: -0.13, up: 0.13}}, 68: {error: {dn: -0.13, up: 0.13}}, 69: {error: {dn: -0.13, up: 0.13}}, 70: {error: {dn: -0.12, up: 0.12}}, 71: {error: {dn: -0.11, up: 0.11}}, 72: {error: {dn: -0.11, up: 0.11}}, 73: {error: {dn: -0.12, up: 0.12}}, 74: {error: {dn: -0.11, up: 0.11}}, 75: {error: {dn: -0.12, up: 0.12}}, 76: {error: {dn: -0.11, up: 0.11}}, 77: {error: {dn: -0.1, up: 0.1}}, 78: {error: {dn: -0.1, up: 0.1}}, 79: {error: {dn: -0.11, up: 0.11}}, 80: {error: {dn: -0.09, up: 0.09}}, 81: {error: {dn: -0.11, up: 0.11}}, 82: {error: {dn: -0.1, up: 0.1}}, 83: {error: {dn: -0.12, up: 0.12}}, 84: {error: {dn: -0.1, up: 0.1}}, 85: {error: {dn: -0.1, up: 0.1}}, 86: {error: {dn: -0.1, up: 0.1}}, 87: {error: {dn: -0.1, up: 0.1}}, 88: {error: {dn: -0.08, up: 0.08}}, 89: {error: {dn: -0.09, up: 0.09}}, 90: {error: {dn: -0.08, up: 0.08}}, 91: {error: {dn: -0.08, up: 0.08}}, 92: {error: {dn: -0.08, up: 0.08}}, 93: {error: {dn: -0.07, up: 0.07}}, 94: {error: {dn: -0.08, up: 0.08}}, 95: {error: {dn: -0.08, up: 0.08}}, 96: {error: {dn: -0.07, up: 0.07}}, 97: {error: {dn: -0.07, up: 0.07}}, 98: {error: {dn: -0.08, up: 0.08}}, 99: {error: {dn: -0.07, up: 0.07}}, 100: {error: {dn: -0.07, up: 0.07}}, 101: {error: {dn: -0.07, up: 0.07}}, 102: {error: {dn: -0.07, up: 0.07}}, 103: {error: {dn: -0.08, up: 0.08}}, 104: {error: {dn: -0.06, up: 0.06}}, 105: {error: {dn: -0.06, up: 0.06}}, 106: {error: {dn: -0.08, up: 0.08}}, 107: {error: {dn: -0.06, up: 0.06}}, 108: {error: {dn: -0.07, up: 0.07}}, 109: {error: {dn: -0.07, up: 0.07}}, 110: {error: {dn: -0.07, up: 0.07}}, 111: {error: {dn: -0.06, up: 0.06}}, 112: {error: {dn: -0.08, up: 0.08}}, 113: {error: {dn: -0.09, up: 0.09}}, 114: {error: {dn: -0.06, up: 0.06}}, 115: {error: {dn: -0.07, up: 0.07}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I758568/d08-x01-y01 +Title: doi:10.17182/hepdata.51824.v1/t8 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.612500e+00 1.250000e-02 1.250000e-02 2.000000e-02 4.000000e-02 4.000000e-02 +1.637500e+00 1.250000e-02 1.250000e-02 8.000000e-02 6.000000e-02 6.000000e-02 +1.662500e+00 1.250000e-02 1.250000e-02 1.300000e-01 8.000000e-02 8.000000e-02 +1.687500e+00 1.250000e-02 1.250000e-02 2.700000e-01 1.000000e-01 1.000000e-01 +1.712500e+00 1.250000e-02 1.250000e-02 1.700000e-01 8.000000e-02 8.000000e-02 +1.737500e+00 1.250000e-02 1.250000e-02 9.000000e-02 6.000000e-02 6.000000e-02 +1.762500e+00 1.250000e-02 1.250000e-02 3.200000e-01 1.000000e-01 1.000000e-01 +1.787500e+00 1.250000e-02 1.250000e-02 1.600000e-01 7.000000e-02 7.000000e-02 +1.812500e+00 1.250000e-02 1.250000e-02 3.400000e-01 9.000000e-02 9.000000e-02 +1.837500e+00 1.250000e-02 1.250000e-02 3.600000e-01 9.000000e-02 9.000000e-02 +1.862500e+00 1.250000e-02 1.250000e-02 3.200000e-01 9.000000e-02 9.000000e-02 +1.887500e+00 1.250000e-02 1.250000e-02 2.000000e-01 9.000000e-02 9.000000e-02 +1.912500e+00 1.250000e-02 1.250000e-02 5.400000e-01 1.100000e-01 1.100000e-01 +1.937500e+00 1.250000e-02 1.250000e-02 5.400000e-01 1.100000e-01 1.100000e-01 +1.962500e+00 1.250000e-02 1.250000e-02 6.300000e-01 1.100000e-01 1.100000e-01 +1.987500e+00 1.250000e-02 1.250000e-02 5.700000e-01 1.100000e-01 1.100000e-01 +2.012500e+00 1.250000e-02 1.250000e-02 3.900000e-01 1.000000e-01 1.000000e-01 +2.037500e+00 1.250000e-02 1.250000e-02 4.900000e-01 1.100000e-01 1.100000e-01 +2.062500e+00 1.250000e-02 1.250000e-02 7.100000e-01 1.300000e-01 1.300000e-01 +2.087500e+00 1.250000e-02 1.250000e-02 5.600000e-01 1.100000e-01 1.100000e-01 +2.112500e+00 1.250000e-02 1.250000e-02 5.900000e-01 1.200000e-01 1.200000e-01 +2.137500e+00 1.250000e-02 1.250000e-02 5.900000e-01 1.200000e-01 1.200000e-01 +2.162500e+00 1.250000e-02 1.250000e-02 6.600000e-01 1.200000e-01 1.200000e-01 +2.187500e+00 1.250000e-02 1.250000e-02 6.000000e-01 1.300000e-01 1.300000e-01 +2.212500e+00 1.250000e-02 1.250000e-02 4.800000e-01 1.100000e-01 1.100000e-01 +2.237500e+00 1.250000e-02 1.250000e-02 6.100000e-01 1.200000e-01 1.200000e-01 +2.262500e+00 1.250000e-02 1.250000e-02 4.900000e-01 1.100000e-01 1.100000e-01 +2.287500e+00 1.250000e-02 1.250000e-02 8.400000e-01 1.300000e-01 1.300000e-01 +2.312500e+00 1.250000e-02 1.250000e-02 5.500000e-01 1.200000e-01 1.200000e-01 +2.337500e+00 1.250000e-02 1.250000e-02 8.900000e-01 1.300000e-01 1.300000e-01 +2.362500e+00 1.250000e-02 1.250000e-02 7.300000e-01 1.300000e-01 1.300000e-01 +2.387500e+00 1.250000e-02 1.250000e-02 8.200000e-01 1.300000e-01 1.300000e-01 +2.412500e+00 1.250000e-02 1.250000e-02 7.500000e-01 1.300000e-01 1.300000e-01 +2.437500e+00 1.250000e-02 1.250000e-02 8.500000e-01 1.300000e-01 1.300000e-01 +2.462500e+00 1.250000e-02 1.250000e-02 1.040000e+00 1.300000e-01 1.300000e-01 +2.487500e+00 1.250000e-02 1.250000e-02 1.020000e+00 1.400000e-01 1.400000e-01 +2.512500e+00 1.250000e-02 1.250000e-02 9.500000e-01 1.400000e-01 1.400000e-01 +2.537500e+00 1.250000e-02 1.250000e-02 8.500000e-01 1.500000e-01 1.500000e-01 +2.562500e+00 1.250000e-02 1.250000e-02 8.200000e-01 1.400000e-01 1.400000e-01 +2.587500e+00 1.250000e-02 1.250000e-02 6.300000e-01 1.200000e-01 1.200000e-01 +2.612500e+00 1.250000e-02 1.250000e-02 1.200000e+00 1.500000e-01 1.500000e-01 +2.637500e+00 1.250000e-02 1.250000e-02 7.300000e-01 1.300000e-01 1.300000e-01 +2.662500e+00 1.250000e-02 1.250000e-02 7.100000e-01 1.200000e-01 1.200000e-01 +2.687500e+00 1.250000e-02 1.250000e-02 9.300000e-01 1.400000e-01 1.400000e-01 +2.712500e+00 1.250000e-02 1.250000e-02 7.300000e-01 1.300000e-01 1.300000e-01 +2.737500e+00 1.250000e-02 1.250000e-02 8.000000e-01 1.300000e-01 1.300000e-01 +2.762500e+00 1.250000e-02 1.250000e-02 7.700000e-01 1.300000e-01 1.300000e-01 +2.787500e+00 1.250000e-02 1.250000e-02 6.400000e-01 1.400000e-01 1.400000e-01 +2.812500e+00 1.250000e-02 1.250000e-02 7.100000e-01 1.300000e-01 1.300000e-01 +2.837500e+00 1.250000e-02 1.250000e-02 8.200000e-01 1.300000e-01 1.300000e-01 +2.862500e+00 1.250000e-02 1.250000e-02 6.400000e-01 1.300000e-01 1.300000e-01 +2.887500e+00 1.250000e-02 1.250000e-02 8.300000e-01 1.400000e-01 1.400000e-01 +2.912500e+00 1.250000e-02 1.250000e-02 6.500000e-01 1.300000e-01 1.300000e-01 +2.937500e+00 1.250000e-02 1.250000e-02 7.600000e-01 1.400000e-01 1.400000e-01 +2.962500e+00 1.250000e-02 1.250000e-02 6.300000e-01 1.300000e-01 1.300000e-01 +2.987500e+00 1.250000e-02 1.250000e-02 9.300000e-01 1.500000e-01 1.500000e-01 +3.012500e+00 1.250000e-02 1.250000e-02 7.800000e-01 1.400000e-01 1.400000e-01 +3.037500e+00 1.250000e-02 1.250000e-02 6.200000e-01 1.300000e-01 1.300000e-01 +3.062500e+00 1.250000e-02 1.250000e-02 8.600000e-01 1.500000e-01 1.500000e-01 +3.087500e+00 1.250000e-02 1.250000e-02 7.010000e+00 3.400000e-01 3.400000e-01 +3.112500e+00 1.250000e-02 1.250000e-02 4.310000e+00 2.800000e-01 2.800000e-01 +3.137500e+00 1.250000e-02 1.250000e-02 8.300000e-01 1.500000e-01 1.500000e-01 +3.162500e+00 1.250000e-02 1.250000e-02 9.200000e-01 1.500000e-01 1.500000e-01 +3.187500e+00 1.250000e-02 1.250000e-02 7.500000e-01 1.300000e-01 1.300000e-01 +3.212500e+00 1.250000e-02 1.250000e-02 5.700000e-01 1.300000e-01 1.300000e-01 +3.237500e+00 1.250000e-02 1.250000e-02 6.200000e-01 1.400000e-01 1.400000e-01 +3.262500e+00 1.250000e-02 1.250000e-02 4.700000e-01 1.200000e-01 1.200000e-01 +3.287500e+00 1.250000e-02 1.250000e-02 4.300000e-01 1.300000e-01 1.300000e-01 +3.312500e+00 1.250000e-02 1.250000e-02 5.000000e-01 1.300000e-01 1.300000e-01 +3.337500e+00 1.250000e-02 1.250000e-02 5.500000e-01 1.300000e-01 1.300000e-01 +3.362500e+00 1.250000e-02 1.250000e-02 4.200000e-01 1.200000e-01 1.200000e-01 +3.387500e+00 1.250000e-02 1.250000e-02 4.800000e-01 1.100000e-01 1.100000e-01 +3.412500e+00 1.250000e-02 1.250000e-02 3.700000e-01 1.100000e-01 1.100000e-01 +3.437500e+00 1.250000e-02 1.250000e-02 5.000000e-01 1.200000e-01 1.200000e-01 +3.462500e+00 1.250000e-02 1.250000e-02 2.900000e-01 1.100000e-01 1.100000e-01 +3.487500e+00 1.250000e-02 1.250000e-02 5.200000e-01 1.200000e-01 1.200000e-01 +3.512500e+00 1.250000e-02 1.250000e-02 4.500000e-01 1.100000e-01 1.100000e-01 +3.537500e+00 1.250000e-02 1.250000e-02 4.200000e-01 1.000000e-01 1.000000e-01 +3.562500e+00 1.250000e-02 1.250000e-02 4.200000e-01 1.000000e-01 1.000000e-01 +3.587500e+00 1.250000e-02 1.250000e-02 5.300000e-01 1.100000e-01 1.100000e-01 +3.612500e+00 1.250000e-02 1.250000e-02 1.800000e-01 9.000000e-02 9.000000e-02 +3.637500e+00 1.250000e-02 1.250000e-02 2.500000e-01 1.100000e-01 1.100000e-01 +3.662500e+00 1.250000e-02 1.250000e-02 3.400000e-01 1.000000e-01 1.000000e-01 +3.687500e+00 1.250000e-02 1.250000e-02 6.000000e-01 1.200000e-01 1.200000e-01 +3.712500e+00 1.250000e-02 1.250000e-02 4.300000e-01 1.000000e-01 1.000000e-01 +3.737500e+00 1.250000e-02 1.250000e-02 3.600000e-01 1.000000e-01 1.000000e-01 +3.762500e+00 1.250000e-02 1.250000e-02 3.800000e-01 1.000000e-01 1.000000e-01 +3.787500e+00 1.250000e-02 1.250000e-02 3.800000e-01 1.000000e-01 1.000000e-01 +3.812500e+00 1.250000e-02 1.250000e-02 1.800000e-01 8.000000e-02 8.000000e-02 +3.837500e+00 1.250000e-02 1.250000e-02 3.600000e-01 9.000000e-02 9.000000e-02 +3.862500e+00 1.250000e-02 1.250000e-02 3.600000e-01 8.000000e-02 8.000000e-02 +3.887500e+00 1.250000e-02 1.250000e-02 2.000000e-01 8.000000e-02 8.000000e-02 +3.912500e+00 1.250000e-02 1.250000e-02 3.700000e-01 8.000000e-02 8.000000e-02 +3.937500e+00 1.250000e-02 1.250000e-02 2.000000e-01 7.000000e-02 7.000000e-02 +3.962500e+00 1.250000e-02 1.250000e-02 3.300000e-01 8.000000e-02 8.000000e-02 +3.987500e+00 1.250000e-02 1.250000e-02 1.800000e-01 8.000000e-02 8.000000e-02 +4.012500e+00 1.250000e-02 1.250000e-02 1.100000e-01 7.000000e-02 7.000000e-02 +4.037500e+00 1.250000e-02 1.250000e-02 1.400000e-01 7.000000e-02 7.000000e-02 +4.062500e+00 1.250000e-02 1.250000e-02 3.900000e-01 8.000000e-02 8.000000e-02 +4.087500e+00 1.250000e-02 1.250000e-02 1.300000e-01 7.000000e-02 7.000000e-02 +4.112500e+00 1.250000e-02 1.250000e-02 1.600000e-01 7.000000e-02 7.000000e-02 +4.137500e+00 1.250000e-02 1.250000e-02 1.900000e-01 7.000000e-02 7.000000e-02 +4.162500e+00 1.250000e-02 1.250000e-02 1.300000e-01 7.000000e-02 7.000000e-02 +4.187500e+00 1.250000e-02 1.250000e-02 1.300000e-01 8.000000e-02 8.000000e-02 +4.212500e+00 1.250000e-02 1.250000e-02 1.400000e-01 6.000000e-02 6.000000e-02 +4.237500e+00 1.250000e-02 1.250000e-02 2.100000e-01 6.000000e-02 6.000000e-02 +4.262500e+00 1.250000e-02 1.250000e-02 4.000000e-02 8.000000e-02 8.000000e-02 +4.287500e+00 1.250000e-02 1.250000e-02 1.000000e-01 6.000000e-02 6.000000e-02 +4.312500e+00 1.250000e-02 1.250000e-02 2.000000e-01 7.000000e-02 7.000000e-02 +4.337500e+00 1.250000e-02 1.250000e-02 1.400000e-01 7.000000e-02 7.000000e-02 +4.362500e+00 1.250000e-02 1.250000e-02 2.800000e-01 7.000000e-02 7.000000e-02 +4.387500e+00 1.250000e-02 1.250000e-02 5.000000e-02 6.000000e-02 6.000000e-02 +4.412500e+00 1.250000e-02 1.250000e-02 2.500000e-01 8.000000e-02 8.000000e-02 +4.437500e+00 1.250000e-02 1.250000e-02 4.100000e-01 9.000000e-02 9.000000e-02 +4.462500e+00 1.250000e-02 1.250000e-02 1.900000e-01 6.000000e-02 6.000000e-02 +4.487500e+00 1.250000e-02 1.250000e-02 1.000000e-01 7.000000e-02 7.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d09-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.41, up: 0.41}}, 1: {error: {dn: -0.33, up: 0.33}}, 2: {error: {dn: -0.35, up: 0.35}}, 3: {error: {dn: -0.61, up: 0.61}}, 4: {error: {dn: -0.48, up: 0.48}}, 5: {error: {dn: -0.54, up: 0.54}}, 6: {error: {dn: -0.41, up: 0.41}}, 7: {error: {dn: -0.29, up: 0.29}}, 8: {error: {dn: -0.28, up: 0.28}}, 9: {error: {dn: -0.32, up: 0.32}}, 10: {error: {dn: -0.26, up: 0.26}}, 11: {error: {dn: -0.25, up: 0.25}}, 12: {error: {dn: -0.16, up: 0.16}}, 13: {error: {dn: -0.24, up: 0.24}}, 14: {error: {dn: -0.26, up: 0.26}}, 15: {error: {dn: -0.18, up: 0.18}}, 16: {error: {dn: -0.18, up: 0.18}}, 17: {error: {dn: -0.2, up: 0.2}}, 18: {error: {dn: -0.14, up: 0.14}}, 19: {error: {dn: -0.1, up: 0.1}}, 20: {error: {dn: -0.17, up: 0.17}}, 21: {error: {dn: -0.1, up: 0.1}}, 22: {error: {dn: -0.13, up: 0.13}}, 23: {error: {dn: -0.19, up: 0.19}}, 24: {error: {dn: -0.16, up: 0.16}}, 25: {error: {dn: -0.19, up: 0.19}}, 26: {error: {dn: -0.13, up: 0.13}}, 27: {error: {dn: -0.09, up: 0.09}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I758568/d09-x01-y01 +Title: doi:10.17182/hepdata.51824.v1/t9 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.560000e+00 2.000000e-02 2.000000e-02 0.000000e+00 4.100000e-01 4.100000e-01 +1.600000e+00 2.000000e-02 2.000000e-02 5.700000e-01 3.300000e-01 3.300000e-01 +1.640000e+00 2.000000e-02 2.000000e-02 7.000000e-01 3.500000e-01 3.500000e-01 +1.680000e+00 2.000000e-02 2.000000e-02 2.280000e+00 6.100000e-01 6.100000e-01 +1.720000e+00 2.000000e-02 2.000000e-02 1.530000e+00 4.800000e-01 4.800000e-01 +1.760000e+00 2.000000e-02 2.000000e-02 2.020000e+00 5.400000e-01 5.400000e-01 +1.800000e+00 2.000000e-02 2.000000e-02 1.230000e+00 4.100000e-01 4.100000e-01 +1.840000e+00 2.000000e-02 2.000000e-02 6.500000e-01 2.900000e-01 2.900000e-01 +1.880000e+00 2.000000e-02 2.000000e-02 6.300000e-01 2.800000e-01 2.800000e-01 +1.920000e+00 2.000000e-02 2.000000e-02 8.500000e-01 3.200000e-01 3.200000e-01 +1.960000e+00 2.000000e-02 2.000000e-02 5.800000e-01 2.600000e-01 2.600000e-01 +2.000000e+00 2.000000e-02 2.000000e-02 5.700000e-01 2.500000e-01 2.500000e-01 +2.040000e+00 2.000000e-02 2.000000e-02 2.200000e-01 1.600000e-01 1.600000e-01 +2.080000e+00 2.000000e-02 2.000000e-02 5.400000e-01 2.400000e-01 2.400000e-01 +2.120000e+00 2.000000e-02 2.000000e-02 6.300000e-01 2.600000e-01 2.600000e-01 +2.160000e+00 2.000000e-02 2.000000e-02 3.100000e-01 1.800000e-01 1.800000e-01 +2.200000e+00 2.000000e-02 2.000000e-02 3.000000e-01 1.800000e-01 1.800000e-01 +2.240000e+00 2.000000e-02 2.000000e-02 0.000000e+00 2.000000e-01 2.000000e-01 +2.280000e+00 2.000000e-02 2.000000e-02 2.000000e-01 1.400000e-01 1.400000e-01 +2.320000e+00 2.000000e-02 2.000000e-02 1.000000e-01 1.000000e-01 1.000000e-01 +2.360000e+00 2.000000e-02 2.000000e-02 2.900000e-01 1.700000e-01 1.700000e-01 +2.400000e+00 2.000000e-02 2.000000e-02 1.000000e-01 1.000000e-01 1.000000e-01 +2.440000e+00 2.000000e-02 2.000000e-02 1.900000e-01 1.300000e-01 1.300000e-01 +2.480000e+00 2.000000e-02 2.000000e-02 0.000000e+00 1.900000e-01 1.900000e-01 +2.520000e+00 2.000000e-02 2.000000e-02 2.800000e-01 1.600000e-01 1.600000e-01 +2.560000e+00 2.000000e-02 2.000000e-02 0.000000e+00 1.900000e-01 1.900000e-01 +2.600000e+00 2.000000e-02 2.000000e-02 1.900000e-01 1.300000e-01 1.300000e-01 +2.640000e+00 2.000000e-02 2.000000e-02 9.000000e-02 9.000000e-02 9.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d10-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.04, up: 0.04}}, 1: {error: {dn: -0.08, up: 0.08}}, 2: {error: {dn: -0.06, up: 0.06}}, 3: {error: {dn: -0.09, up: 0.09}}, 4: {error: {dn: -0.1, up: 0.1}}, 5: {error: {dn: -0.09, up: 0.09}}, 6: {error: {dn: -0.09, up: 0.09}}, 7: {error: {dn: -0.1, up: 0.1}}, 8: {error: {dn: -0.08, up: 0.08}}, 9: {error: {dn: -0.07, up: 0.07}}, 10: {error: {dn: -0.08, up: 0.08}}, 11: {error: {dn: -0.08, up: 0.08}}, 12: {error: {dn: -0.06, up: 0.06}}, 13: {error: {dn: -0.06, up: 0.06}}, 14: {error: {dn: -0.07, up: 0.07}}, 15: {error: {dn: -0.06, up: 0.06}}, 16: {error: {dn: -0.06, up: 0.06}}, 17: {error: {dn: -0.07, up: 0.07}}, 18: {error: {dn: -0.06, up: 0.06}}, 19: {error: {dn: -0.05, up: 0.05}}, 20: {error: {dn: -0.05, up: 0.05}}, 21: {error: {dn: -0.05, up: 0.05}}, 22: {error: {dn: -0.06, up: 0.06}}, 23: {error: {dn: -0.04, up: 0.04}}, 24: {error: {dn: -0.05, up: 0.05}}, 25: {error: {dn: -0.05, up: 0.05}}, 26: {error: {dn: -0.05, up: 0.05}}, 27: {error: {dn: -0.05, up: 0.05}}, 28: {error: {dn: -0.05, up: 0.05}}, 29: {error: {dn: -0.05, up: 0.05}}, 30: {error: {dn: -0.05, up: 0.05}}, 31: {error: {dn: -0.04, up: 0.04}}, 32: {error: {dn: -0.09, up: 0.09}}, 33: {error: {dn: -0.06, up: 0.06}}, 34: {error: {dn: -0.04, up: 0.04}}, 35: {error: {dn: -0.04, up: 0.04}}, 36: {error: {dn: -0.05, up: 0.05}}, 37: {error: {dn: -0.04, up: 0.04}}, 38: {error: {dn: -0.04, up: 0.04}}, 39: {error: {dn: -0.03, up: 0.03}}, 40: {error: {dn: -0.02, up: 0.02}}, 41: {error: {dn: -0.03, up: 0.03}}, 42: {error: {dn: -0.02, up: 0.02}}, 43: {error: {dn: -0.03, up: 0.03}}, 44: {error: {dn: -0.03, up: 0.03}}, 45: {error: {dn: -0.03, up: 0.03}}, 46: {error: {dn: -0.03, up: 0.03}}, 47: {error: {dn: -0.04, up: 0.04}}, 48: {error: {dn: -0.03, up: 0.03}}, 49: {error: {dn: -0.02, up: 0.02}}, 50: {error: {dn: -0.02, up: 0.02}}, 51: {error: {dn: -0.02, up: 0.02}}, 52: {error: {dn: -0.01, up: 0.01}}, 53: {error: {dn: -0.01, up: 0.01}}, 54: {error: {dn: -0.01, up: 0.01}}, 55: {error: {dn: -0.01, up: 0.01}}, 56: {error: {dn: -0.01, up: 0.01}}, 57: {error: {dn: -0.01, up: 0.01}}, 58: {error: {dn: -0.01, up: 0.01}}, 59: {error: {dn: -0.01, up: 0.01}}, 60: {error: {dn: -0.01, up: 0.01}}, 61: {error: {dn: -0.01, up: 0.01}}, 62: {error: {dn: -0.01, up: 0.01}}, 63: {error: {dn: -0.02, up: 0.02}}, 64: {error: {dn: -0.01, up: 0.01}}, 65: {error: {dn: -0.01, up: 0.01}}, 66: {error: {dn: -0.01, up: 0.01}}, 67: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I758568/d10-x01-y01 +Title: doi:10.17182/hepdata.51824.v1/t10 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.800000e+00 2.000000e-02 2.000000e-02 9.000000e-02 4.000000e-02 4.000000e-02 +1.840000e+00 2.000000e-02 2.000000e-02 3.300000e-01 8.000000e-02 8.000000e-02 +1.880000e+00 2.000000e-02 2.000000e-02 2.500000e-01 6.000000e-02 6.000000e-02 +1.920000e+00 2.000000e-02 2.000000e-02 5.200000e-01 9.000000e-02 9.000000e-02 +1.960000e+00 2.000000e-02 2.000000e-02 6.000000e-01 1.000000e-01 1.000000e-01 +2.000000e+00 2.000000e-02 2.000000e-02 4.500000e-01 9.000000e-02 9.000000e-02 +2.040000e+00 2.000000e-02 2.000000e-02 4.300000e-01 9.000000e-02 9.000000e-02 +2.080000e+00 2.000000e-02 2.000000e-02 6.100000e-01 1.000000e-01 1.000000e-01 +2.120000e+00 2.000000e-02 2.000000e-02 3.700000e-01 8.000000e-02 8.000000e-02 +2.160000e+00 2.000000e-02 2.000000e-02 2.800000e-01 7.000000e-02 7.000000e-02 +2.200000e+00 2.000000e-02 2.000000e-02 3.900000e-01 8.000000e-02 8.000000e-02 +2.240000e+00 2.000000e-02 2.000000e-02 3.600000e-01 8.000000e-02 8.000000e-02 +2.280000e+00 2.000000e-02 2.000000e-02 1.700000e-01 6.000000e-02 6.000000e-02 +2.320000e+00 2.000000e-02 2.000000e-02 2.200000e-01 6.000000e-02 6.000000e-02 +2.360000e+00 2.000000e-02 2.000000e-02 3.400000e-01 7.000000e-02 7.000000e-02 +2.400000e+00 2.000000e-02 2.000000e-02 2.300000e-01 6.000000e-02 6.000000e-02 +2.440000e+00 2.000000e-02 2.000000e-02 1.900000e-01 6.000000e-02 6.000000e-02 +2.480000e+00 2.000000e-02 2.000000e-02 3.100000e-01 7.000000e-02 7.000000e-02 +2.520000e+00 2.000000e-02 2.000000e-02 2.700000e-01 6.000000e-02 6.000000e-02 +2.560000e+00 2.000000e-02 2.000000e-02 1.800000e-01 5.000000e-02 5.000000e-02 +2.600000e+00 2.000000e-02 2.000000e-02 2.000000e-01 5.000000e-02 5.000000e-02 +2.640000e+00 2.000000e-02 2.000000e-02 2.000000e-01 5.000000e-02 5.000000e-02 +2.680000e+00 2.000000e-02 2.000000e-02 1.800000e-01 6.000000e-02 6.000000e-02 +2.720000e+00 2.000000e-02 2.000000e-02 1.000000e-01 4.000000e-02 4.000000e-02 +2.760000e+00 2.000000e-02 2.000000e-02 1.600000e-01 5.000000e-02 5.000000e-02 +2.800000e+00 2.000000e-02 2.000000e-02 1.800000e-01 5.000000e-02 5.000000e-02 +2.840000e+00 2.000000e-02 2.000000e-02 1.200000e-01 5.000000e-02 5.000000e-02 +2.880000e+00 2.000000e-02 2.000000e-02 1.200000e-01 5.000000e-02 5.000000e-02 +2.920000e+00 2.000000e-02 2.000000e-02 1.700000e-01 5.000000e-02 5.000000e-02 +2.960000e+00 2.000000e-02 2.000000e-02 1.700000e-01 5.000000e-02 5.000000e-02 +3.000000e+00 2.000000e-02 2.000000e-02 1.600000e-01 5.000000e-02 5.000000e-02 +3.040000e+00 2.000000e-02 2.000000e-02 5.000000e-02 4.000000e-02 4.000000e-02 +3.080000e+00 2.000000e-02 2.000000e-02 5.100000e-01 9.000000e-02 9.000000e-02 +3.120000e+00 2.000000e-02 2.000000e-02 2.400000e-01 6.000000e-02 6.000000e-02 +3.160000e+00 2.000000e-02 2.000000e-02 7.000000e-02 4.000000e-02 4.000000e-02 +3.200000e+00 2.000000e-02 2.000000e-02 1.200000e-01 4.000000e-02 4.000000e-02 +3.240000e+00 2.000000e-02 2.000000e-02 1.700000e-01 5.000000e-02 5.000000e-02 +3.280000e+00 2.000000e-02 2.000000e-02 6.000000e-02 4.000000e-02 4.000000e-02 +3.320000e+00 2.000000e-02 2.000000e-02 7.000000e-02 4.000000e-02 4.000000e-02 +3.360000e+00 2.000000e-02 2.000000e-02 6.000000e-02 3.000000e-02 3.000000e-02 +3.400000e+00 2.000000e-02 2.000000e-02 1.000000e-02 2.000000e-02 2.000000e-02 +3.440000e+00 2.000000e-02 2.000000e-02 7.000000e-02 3.000000e-02 3.000000e-02 +3.480000e+00 2.000000e-02 2.000000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +3.520000e+00 2.000000e-02 2.000000e-02 7.000000e-02 3.000000e-02 3.000000e-02 +3.560000e+00 2.000000e-02 2.000000e-02 8.000000e-02 3.000000e-02 3.000000e-02 +3.600000e+00 2.000000e-02 2.000000e-02 7.000000e-02 3.000000e-02 3.000000e-02 +3.640000e+00 2.000000e-02 2.000000e-02 5.000000e-02 3.000000e-02 3.000000e-02 +3.680000e+00 2.000000e-02 2.000000e-02 1.400000e-01 4.000000e-02 4.000000e-02 +3.720000e+00 2.000000e-02 2.000000e-02 9.000000e-02 3.000000e-02 3.000000e-02 +3.760000e+00 2.000000e-02 2.000000e-02 2.000000e-02 2.000000e-02 2.000000e-02 +3.800000e+00 2.000000e-02 2.000000e-02 0.000000e+00 2.000000e-02 2.000000e-02 +3.840000e+00 2.000000e-02 2.000000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +3.880000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +3.920000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +3.960000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +4.000000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +4.040000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +4.080000e+00 2.000000e-02 2.000000e-02 0.000000e+00 1.000000e-02 1.000000e-02 +4.120000e+00 2.000000e-02 2.000000e-02 0.000000e+00 1.000000e-02 1.000000e-02 +4.160000e+00 2.000000e-02 2.000000e-02 0.000000e+00 1.000000e-02 1.000000e-02 +4.200000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +4.240000e+00 2.000000e-02 2.000000e-02 0.000000e+00 1.000000e-02 1.000000e-02 +4.280000e+00 2.000000e-02 2.000000e-02 0.000000e+00 1.000000e-02 1.000000e-02 +4.320000e+00 2.000000e-02 2.000000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +4.360000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +4.400000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +4.440000e+00 2.000000e-02 2.000000e-02 0.000000e+00 1.000000e-02 1.000000e-02 +4.480000e+00 2.000000e-02 2.000000e-02 0.000000e+00 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I758568/d11-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.0, up: 0.0}}, 1: {error: {dn: -0.06, up: 0.06}}, 2: {error: {dn: -0.05, up: 0.05}}, 3: {error: {dn: -0.0, up: 0.0}}, 4: {error: {dn: -0.04, up: 0.04}}, 5: {error: {dn: -0.04, up: 0.04}}, 6: {error: {dn: -0.02, up: 0.02}}, 7: {error: {dn: -0.04, up: 0.04}}, 8: {error: {dn: -0.0, up: 0.0}}, 9: {error: {dn: -0.0, up: 0.0}}, 10: {error: {dn: -0.02, up: 0.02}}, 11: {error: {dn: -0.05, up: 0.05}}, 12: {error: {dn: -0.05, up: 0.05}}, 13: {error: {dn: -0.0, up: 0.0}}, 14: {error: {dn: -0.09, up: 0.09}}, 15: {error: {dn: -0.04, up: 0.04}}, 16: {error: {dn: -0.06, up: 0.06}}, 17: {error: {dn: -0.08, up: 0.08}}, 18: {error: {dn: -0.06, up: 0.06}}, 19: {error: {dn: -0.08, up: 0.08}}, 20: {error: {dn: -0.05, up: 0.05}}, 21: {error: {dn: -0.1, up: 0.1}}, 22: {error: {dn: -0.07, up: 0.07}}, 23: {error: {dn: -0.06, up: 0.06}}, 24: {error: {dn: -0.06, up: 0.06}}, 25: {error: {dn: -0.07, up: 0.07}}, 26: {error: {dn: -0.08, up: 0.08}}, 27: {error: {dn: -0.11, up: 0.11}}, 28: {error: {dn: -0.09, up: 0.09}}, 29: {error: {dn: -0.08, up: 0.08}}, 30: {error: {dn: -0.07, up: 0.07}}, 31: {error: {dn: -0.07, up: 0.07}}, 32: {error: {dn: -0.08, up: 0.08}}, 33: {error: {dn: -0.12, up: 0.12}}, 34: {error: {dn: -0.1, up: 0.1}}, 35: {error: {dn: -0.13, up: 0.13}}, 36: {error: {dn: -0.09, up: 0.09}}, 37: {error: {dn: -0.1, up: 0.1}}, 38: {error: {dn: -0.13, up: 0.13}}, 39: {error: {dn: -0.26, up: 0.26}}, 40: {error: {dn: -0.22, up: 0.22}}, 41: {error: {dn: -0.1, up: 0.1}}, 42: {error: {dn: -0.11, up: 0.11}}, 43: {error: {dn: -0.08, up: 0.08}}, 44: {error: {dn: -0.14, up: 0.14}}, 45: {error: {dn: -0.13, up: 0.13}}, 46: {error: {dn: -0.11, up: 0.11}}, 47: {error: {dn: -0.09, up: 0.09}}, 48: {error: {dn: -0.08, up: 0.08}}, 49: {error: {dn: -0.09, up: 0.09}}, 50: {error: {dn: -0.09, up: 0.09}}, 51: {error: {dn: -0.09, up: 0.09}}, 52: {error: {dn: -0.05, up: 0.05}}, 53: {error: {dn: -0.1, up: 0.1}}, 54: {error: {dn: -0.08, up: 0.08}}, 55: {error: {dn: -0.1, up: 0.1}}, 56: {error: {dn: -0.05, up: 0.05}}, 57: {error: {dn: -0.11, up: 0.11}}, 58: {error: {dn: -0.08, up: 0.08}}, 59: {error: {dn: -0.08, up: 0.08}}, 60: {error: {dn: -0.09, up: 0.09}}, 61: {error: {dn: -0.1, up: 0.1}}, 62: {error: {dn: -0.07, up: 0.07}}, 63: {error: {dn: -0.1, up: 0.1}}, 64: {error: {dn: -0.09, up: 0.09}}, 65: {error: {dn: -0.05, up: 0.05}}, 66: {error: {dn: -0.08, up: 0.08}}, 67: {error: {dn: -0.07, up: 0.07}}, 68: {error: {dn: -0.08, up: 0.08}}, 69: {error: {dn: -0.09, up: 0.09}}, 70: {error: {dn: -0.07, up: 0.07}}, 71: {error: {dn: -0.07, up: 0.07}}, 72: {error: {dn: -0.08, up: 0.08}}, 73: {error: {dn: -0.06, up: 0.06}}, 74: {error: {dn: -0.06, up: 0.06}}, 75: {error: {dn: -0.06, up: 0.06}}, 76: {error: {dn: -0.06, up: 0.06}}, 77: {error: {dn: -0.07, up: 0.07}}, 78: {error: {dn: -0.07, up: 0.07}}, 79: {error: {dn: -0.07, up: 0.07}}, 80: {error: {dn: -0.06, up: 0.06}}, 81: {error: {dn: -0.05, up: 0.05}}, 82: {error: {dn: -0.05, up: 0.05}}, 83: {error: {dn: -0.06, up: 0.06}}, 84: {error: {dn: -0.05, up: 0.05}}, 85: {error: {dn: -0.08, up: 0.08}}, 86: {error: {dn: -0.04, up: 0.04}}, 87: {error: {dn: -0.08, up: 0.08}}, 88: {error: {dn: -0.06, up: 0.06}}, 89: {error: {dn: -0.07, up: 0.07}}, 90: {error: {dn: -0.07, up: 0.07}}, 91: {error: {dn: -0.07, up: 0.07}}, 92: {error: {dn: -0.07, up: 0.07}}, 93: {error: {dn: -0.08, up: 0.08}}, 94: {error: {dn: -0.06, up: 0.06}}, 95: {error: {dn: -0.11, up: 0.11}}} + +IsRef: 1 +Path: /REF/BABAR_2007_I758568/d11-x01-y01 +Title: doi:10.17182/hepdata.51824.v1/t11 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.112500e+00 1.250000e-02 1.250000e-02 0.000000e+00 0.000000e+00 0.000000e+00 +2.137500e+00 1.250000e-02 1.250000e-02 8.000000e-02 6.000000e-02 6.000000e-02 +2.162500e+00 1.250000e-02 1.250000e-02 8.000000e-02 5.000000e-02 5.000000e-02 +2.187500e+00 1.250000e-02 1.250000e-02 0.000000e+00 0.000000e+00 0.000000e+00 +2.212500e+00 1.250000e-02 1.250000e-02 4.000000e-02 4.000000e-02 4.000000e-02 +2.237500e+00 1.250000e-02 1.250000e-02 4.000000e-02 4.000000e-02 4.000000e-02 +2.262500e+00 1.250000e-02 1.250000e-02 -2.000000e-02 2.000000e-02 2.000000e-02 +2.287500e+00 1.250000e-02 1.250000e-02 4.000000e-02 4.000000e-02 4.000000e-02 +2.312500e+00 1.250000e-02 1.250000e-02 0.000000e+00 0.000000e+00 0.000000e+00 +2.337500e+00 1.250000e-02 1.250000e-02 0.000000e+00 0.000000e+00 0.000000e+00 +2.362500e+00 1.250000e-02 1.250000e-02 -2.000000e-02 2.000000e-02 2.000000e-02 +2.387500e+00 1.250000e-02 1.250000e-02 7.000000e-02 5.000000e-02 5.000000e-02 +2.412500e+00 1.250000e-02 1.250000e-02 -2.000000e-02 5.000000e-02 5.000000e-02 +2.437500e+00 1.250000e-02 1.250000e-02 0.000000e+00 0.000000e+00 0.000000e+00 +2.462500e+00 1.250000e-02 1.250000e-02 1.700000e-01 9.000000e-02 9.000000e-02 +2.487500e+00 1.250000e-02 1.250000e-02 2.000000e-02 4.000000e-02 4.000000e-02 +2.512500e+00 1.250000e-02 1.250000e-02 9.000000e-02 6.000000e-02 6.000000e-02 +2.537500e+00 1.250000e-02 1.250000e-02 8.000000e-02 8.000000e-02 8.000000e-02 +2.562500e+00 1.250000e-02 1.250000e-02 9.000000e-02 6.000000e-02 6.000000e-02 +2.587500e+00 1.250000e-02 1.250000e-02 1.600000e-01 8.000000e-02 8.000000e-02 +2.612500e+00 1.250000e-02 1.250000e-02 5.000000e-02 5.000000e-02 5.000000e-02 +2.637500e+00 1.250000e-02 1.250000e-02 2.600000e-01 1.000000e-01 1.000000e-01 +2.662500e+00 1.250000e-02 1.250000e-02 1.400000e-01 7.000000e-02 7.000000e-02 +2.687500e+00 1.250000e-02 1.250000e-02 -4.000000e-02 6.000000e-02 6.000000e-02 +2.712500e+00 1.250000e-02 1.250000e-02 9.000000e-02 6.000000e-02 6.000000e-02 +2.737500e+00 1.250000e-02 1.250000e-02 1.200000e-01 7.000000e-02 7.000000e-02 +2.762500e+00 1.250000e-02 1.250000e-02 1.400000e-01 8.000000e-02 8.000000e-02 +2.787500e+00 1.250000e-02 1.250000e-02 2.300000e-01 1.100000e-01 1.100000e-01 +2.812500e+00 1.250000e-02 1.250000e-02 1.700000e-01 9.000000e-02 9.000000e-02 +2.837500e+00 1.250000e-02 1.250000e-02 6.000000e-02 8.000000e-02 8.000000e-02 +2.862500e+00 1.250000e-02 1.250000e-02 5.000000e-02 7.000000e-02 7.000000e-02 +2.887500e+00 1.250000e-02 1.250000e-02 7.000000e-02 7.000000e-02 7.000000e-02 +2.912500e+00 1.250000e-02 1.250000e-02 3.000000e-02 8.000000e-02 8.000000e-02 +2.937500e+00 1.250000e-02 1.250000e-02 2.200000e-01 1.200000e-01 1.200000e-01 +2.962500e+00 1.250000e-02 1.250000e-02 6.000000e-02 1.000000e-01 1.000000e-01 +2.987500e+00 1.250000e-02 1.250000e-02 3.400000e-01 1.300000e-01 1.300000e-01 +3.012500e+00 1.250000e-02 1.250000e-02 1.000000e-01 9.000000e-02 9.000000e-02 +3.037500e+00 1.250000e-02 1.250000e-02 1.600000e-01 1.000000e-01 1.000000e-01 +3.062500e+00 1.250000e-02 1.250000e-02 2.500000e-01 1.300000e-01 1.300000e-01 +3.087500e+00 1.250000e-02 1.250000e-02 1.630000e+00 2.600000e-01 2.600000e-01 +3.112500e+00 1.250000e-02 1.250000e-02 9.500000e-01 2.200000e-01 2.200000e-01 +3.137500e+00 1.250000e-02 1.250000e-02 2.400000e-01 1.000000e-01 1.000000e-01 +3.162500e+00 1.250000e-02 1.250000e-02 2.000000e-01 1.100000e-01 1.100000e-01 +3.187500e+00 1.250000e-02 1.250000e-02 5.000000e-02 8.000000e-02 8.000000e-02 +3.212500e+00 1.250000e-02 1.250000e-02 3.600000e-01 1.400000e-01 1.400000e-01 +3.237500e+00 1.250000e-02 1.250000e-02 1.700000e-01 1.300000e-01 1.300000e-01 +3.262500e+00 1.250000e-02 1.250000e-02 2.000000e-01 1.100000e-01 1.100000e-01 +3.287500e+00 1.250000e-02 1.250000e-02 4.000000e-02 9.000000e-02 9.000000e-02 +3.312500e+00 1.250000e-02 1.250000e-02 1.100000e-01 8.000000e-02 8.000000e-02 +3.337500e+00 1.250000e-02 1.250000e-02 -8.000000e-02 9.000000e-02 9.000000e-02 +3.362500e+00 1.250000e-02 1.250000e-02 1.800000e-01 9.000000e-02 9.000000e-02 +3.387500e+00 1.250000e-02 1.250000e-02 1.200000e-01 9.000000e-02 9.000000e-02 +3.412500e+00 1.250000e-02 1.250000e-02 0.000000e+00 5.000000e-02 5.000000e-02 +3.437500e+00 1.250000e-02 1.250000e-02 0.000000e+00 1.000000e-01 1.000000e-01 +3.462500e+00 1.250000e-02 1.250000e-02 1.800000e-01 8.000000e-02 8.000000e-02 +3.487500e+00 1.250000e-02 1.250000e-02 1.700000e-01 1.000000e-01 1.000000e-01 +3.512500e+00 1.250000e-02 1.250000e-02 5.000000e-02 5.000000e-02 5.000000e-02 +3.537500e+00 1.250000e-02 1.250000e-02 1.300000e-01 1.100000e-01 1.100000e-01 +3.562500e+00 1.250000e-02 1.250000e-02 1.000000e-02 8.000000e-02 8.000000e-02 +3.587500e+00 1.250000e-02 1.250000e-02 -1.000000e-02 8.000000e-02 8.000000e-02 +3.612500e+00 1.250000e-02 1.250000e-02 9.000000e-02 9.000000e-02 9.000000e-02 +3.637500e+00 1.250000e-02 1.250000e-02 9.000000e-02 1.000000e-01 1.000000e-01 +3.662500e+00 1.250000e-02 1.250000e-02 1.000000e-01 7.000000e-02 7.000000e-02 +3.687500e+00 1.250000e-02 1.250000e-02 1.800000e-01 1.000000e-01 1.000000e-01 +3.712500e+00 1.250000e-02 1.250000e-02 2.100000e-01 9.000000e-02 9.000000e-02 +3.737500e+00 1.250000e-02 1.250000e-02 6.000000e-02 5.000000e-02 5.000000e-02 +3.762500e+00 1.250000e-02 1.250000e-02 -1.000000e-02 8.000000e-02 8.000000e-02 +3.787500e+00 1.250000e-02 1.250000e-02 0.000000e+00 7.000000e-02 7.000000e-02 +3.812500e+00 1.250000e-02 1.250000e-02 8.000000e-02 8.000000e-02 8.000000e-02 +3.837500e+00 1.250000e-02 1.250000e-02 -4.000000e-02 9.000000e-02 9.000000e-02 +3.862500e+00 1.250000e-02 1.250000e-02 1.500000e-01 7.000000e-02 7.000000e-02 +3.887500e+00 1.250000e-02 1.250000e-02 1.500000e-01 7.000000e-02 7.000000e-02 +3.912500e+00 1.250000e-02 1.250000e-02 8.000000e-02 8.000000e-02 8.000000e-02 +3.937500e+00 1.250000e-02 1.250000e-02 -3.000000e-02 6.000000e-02 6.000000e-02 +3.962500e+00 1.250000e-02 1.250000e-02 4.000000e-02 6.000000e-02 6.000000e-02 +3.987500e+00 1.250000e-02 1.250000e-02 -1.000000e-02 6.000000e-02 6.000000e-02 +4.012500e+00 1.250000e-02 1.250000e-02 8.000000e-02 6.000000e-02 6.000000e-02 +4.037500e+00 1.250000e-02 1.250000e-02 3.000000e-02 7.000000e-02 7.000000e-02 +4.062500e+00 1.250000e-02 1.250000e-02 1.100000e-01 7.000000e-02 7.000000e-02 +4.087500e+00 1.250000e-02 1.250000e-02 5.000000e-02 7.000000e-02 7.000000e-02 +4.112500e+00 1.250000e-02 1.250000e-02 5.000000e-02 6.000000e-02 6.000000e-02 +4.137500e+00 1.250000e-02 1.250000e-02 -3.000000e-02 5.000000e-02 5.000000e-02 +4.162500e+00 1.250000e-02 1.250000e-02 -7.000000e-02 5.000000e-02 5.000000e-02 +4.187500e+00 1.250000e-02 1.250000e-02 0.000000e+00 6.000000e-02 6.000000e-02 +4.212500e+00 1.250000e-02 1.250000e-02 0.000000e+00 5.000000e-02 5.000000e-02 +4.237500e+00 1.250000e-02 1.250000e-02 1.000000e-01 8.000000e-02 8.000000e-02 +4.262500e+00 1.250000e-02 1.250000e-02 6.000000e-02 4.000000e-02 4.000000e-02 +4.287500e+00 1.250000e-02 1.250000e-02 1.200000e-01 8.000000e-02 8.000000e-02 +4.312500e+00 1.250000e-02 1.250000e-02 4.000000e-02 6.000000e-02 6.000000e-02 +4.337500e+00 1.250000e-02 1.250000e-02 1.500000e-01 7.000000e-02 7.000000e-02 +4.362500e+00 1.250000e-02 1.250000e-02 2.000000e-02 7.000000e-02 7.000000e-02 +4.387500e+00 1.250000e-02 1.250000e-02 8.000000e-02 7.000000e-02 7.000000e-02 +4.412500e+00 1.250000e-02 1.250000e-02 6.000000e-02 7.000000e-02 7.000000e-02 +4.437500e+00 1.250000e-02 1.250000e-02 -2.000000e-02 8.000000e-02 8.000000e-02 +4.462500e+00 1.250000e-02 1.250000e-02 3.000000e-02 6.000000e-02 6.000000e-02 +4.487500e+00 1.250000e-02 1.250000e-02 4.000000e-02 1.100000e-01 1.100000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2007_I760730.cc b/analyses/pluginBABAR/BABAR_2007_I760730.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I760730.cc @@ -0,0 +1,159 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2007_I760730 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2007_I760730); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nLL = bookCounter( "/TMP/nLL" ); + _nSS = bookCounter( "/TMP/nSS" ); + _nLS = bookCounter( "/TMP/nLS" ); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + // total hadronic and muonic cross sections + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + // find the Lambdas and Sigmas + const FinalState& ufs = apply(event, "UFS"); + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + for(unsigned int iy=ix+1;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(abs(p1.pdgId())==3122 && abs(p2.pdgId())==3122) + _nLL->fill(event.weight()); + else if(abs(p1.pdgId())==3212 && abs(p2.pdgId())==3212) + _nSS->fill(event.weight()); + else + _nLS->fill(event.weight()); + break; + } + } + if(matched) break; + } + } + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /picobarn; + for(unsigned int ix=1;ix<4;++ix) { + double sigma,error; + if(ix==1) { + sigma = _nLL->val()*fact; + error = _nLL->err()*fact; + } + else if(ix==2) { + sigma = _nSS->val()*fact; + error = _nSS->err()*fact; + } + else { + sigma = _nLS->val()*fact; + error = _nLS->err()*fact; + } + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nLL,_nSS,_nLS; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2007_I760730); + + +} diff --git a/analyses/pluginBABAR/BABAR_2007_I760730.info b/analyses/pluginBABAR/BABAR_2007_I760730.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I760730.info @@ -0,0 +1,35 @@ +Name: BABAR_2007_I760730 +Year: 2007 +Summary: Cross section for $e^+e^-\to\Lambda\bar{\Lambda}$, $\Sigma^0\bar{\Sigma}^0$ and $\Lambda\bar{\Sigma}^0$ between threshold and 3 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 760730 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D76 (2007) 092006 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to\Lambda\bar{\Lambda}$ between threshold and 3 GeV.' +Keywords: +BibKey: Aubert:2007uf +BibTeX: '@article{Aubert:2007uf, + author = "Aubert, Bernard and others", + title = "{Study of $e^{+} e^{-} \to \Lambda \bar{\Lambda}$, + $\Lambda \bar{\Sigma}^0$, $\Sigma^0 \bar{\Sigma}^0$ using + initial state radiation with BABAR}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D76", + year = "2007", + pages = "092006", + doi = "10.1103/PhysRevD.76.092006", + eprint = "0709.1988", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-12806, BABAR-PUB-07-054", + SLACcitation = "%%CITATION = ARXIV:0709.1988;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2007_I760730.plot b/analyses/pluginBABAR/BABAR_2007_I760730.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I760730.plot @@ -0,0 +1,18 @@ +BEGIN PLOT /BABAR_2007_I760730/d01-x01-y01 +Title=$\sigma(e^+e^-\to \Lambda\bar{\Lambda})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \Lambda\bar{\Lambda})$/pb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2007_I760730/d02-x01-y01 +Title=$\sigma(e^+e^-\to \Sigma\bar{\Sigma}^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \Sigma\bar{\Sigma}^0)$/pb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2007_I760730/d03-x01-y01 +Title=$\sigma(e^+e^-\to \Lambda\bar{\Sigma}^0+\text{c.c})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \Lambda\bar{\Sigma}^0+\text{c.c.})$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2007_I760730.yoda b/analyses/pluginBABAR/BABAR_2007_I760730.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_I760730.yoda @@ -0,0 +1,41 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I760730/d01-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2007_I760730/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.25000 0.02000 0.02000 2.04000e+02 6.39062e+01 6.57875e+01 +2.28500 0.01500 0.01500 2.02000e+02 5.12640e+01 5.31413e+01 +2.32500 0.02500 0.02500 1.55000e+02 2.77308e+01 3.04631e+01 +2.37500 0.02500 0.02500 1.76000e+02 3.44384e+01 3.44384e+01 +2.42500 0.02500 0.02500 9.00000e+01 3.10483e+01 3.20156e+01 +2.47500 0.02500 0.02500 1.04000e+02 2.32594e+01 2.60000e+01 +2.55000 0.05000 0.05000 4.60000e+01 9.84886e+00 1.17047e+01 +2.65000 0.05000 0.05000 2.50000e+01 1.31529e+01 1.21655e+01 +2.75000 0.05000 0.05000 1.00000e+01 8.06226e+00 9.05539e+00 +2.90000 0.10000 0.10000 2.10000e+00 3.50571e+00 3.20624e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I760730/d02-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2007_I760730/d02-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.49250 0.10750 0.10750 3.00000e+01 1.33417e+01 1.33417e+01 +2.70000 0.10000 0.10000 1.70000e+01 1.01980e+01 8.24621e+00 +2.90000 0.10000 0.10000 3.40000e+00 7.81025e+00 8.50941e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2007_I760730/d03-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2007_I760730/d03-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.35400 0.04600 0.04600 4.70000e+01 2.15870e+01 2.35372e+01 +2.45000 0.05000 0.05000 3.20000e+01 1.84391e+01 1.94165e+01 +2.60000 0.10000 0.10000 7.10000e+00 7.53260e+00 8.22982e+00 +2.80000 0.10000 0.10000 2.90000e+00 3.71214e+00 4.31045e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/BABAR_2007_S6895344.cc b/analyses/pluginBABAR/BABAR_2007_S6895344.cc rename from analyses/pluginMisc/BABAR_2007_S6895344.cc rename to analyses/pluginBABAR/BABAR_2007_S6895344.cc diff --git a/analyses/pluginMisc/BABAR_2007_S6895344.info b/analyses/pluginBABAR/BABAR_2007_S6895344.info rename from analyses/pluginMisc/BABAR_2007_S6895344.info rename to analyses/pluginBABAR/BABAR_2007_S6895344.info diff --git a/analyses/pluginMisc/BABAR_2007_S6895344.plot b/analyses/pluginBABAR/BABAR_2007_S6895344.plot rename from analyses/pluginMisc/BABAR_2007_S6895344.plot rename to analyses/pluginBABAR/BABAR_2007_S6895344.plot diff --git a/analyses/pluginMisc/BABAR_2007_S6895344.yoda b/analyses/pluginBABAR/BABAR_2007_S6895344.yoda rename from analyses/pluginMisc/BABAR_2007_S6895344.yoda rename to analyses/pluginBABAR/BABAR_2007_S6895344.yoda diff --git a/analyses/pluginBABAR/BABAR_2007_S7266081.cc b/analyses/pluginBABAR/BABAR_2007_S7266081.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2007_S7266081.cc @@ -0,0 +1,174 @@ +// -*- C++ -*- +#include +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief BABAR tau lepton to three charged hadrons + /// @author Peter Richardson + class BABAR_2007_S7266081 : public Analysis { + public: + + BABAR_2007_S7266081() + : Analysis("BABAR_2007_S7266081"), + _weight_total(0), + _weight_pipipi(0), _weight_Kpipi(0), _weight_KpiK(0), _weight_KKK(0) + { } + + + void init() { + declare(UnstableParticles(), "UFS"); + _hist_pipipi_pipipi = bookHisto1D( 1, 1, 1); + _hist_pipipi_pipi = bookHisto1D( 2, 1, 1); + _hist_Kpipi_Kpipi = bookHisto1D( 3, 1, 1); + _hist_Kpipi_Kpi = bookHisto1D( 4, 1, 1); + _hist_Kpipi_pipi = bookHisto1D( 5, 1, 1); + _hist_KpiK_KpiK = bookHisto1D( 6, 1, 1); + _hist_KpiK_KK = bookHisto1D( 7, 1, 1); + _hist_KpiK_piK = bookHisto1D( 8, 1, 1); + _hist_KKK_KKK = bookHisto1D( 9, 1, 1); + _hist_KKK_KK = bookHisto1D(10, 1, 1); + } + + + void analyze(const Event& e) { + double weight = e.weight(); + // Find the taus + Particles taus; + foreach(const Particle& p, apply(e, "UFS").particles(Cuts::pid==PID::TAU)) { + _weight_total += weight; + Particles pip, pim, Kp, Km; + unsigned int nstable = 0; + // Find the decay products we want + findDecayProducts(p, nstable, pip, pim, Kp, Km); + if (p.pid() < 0) { + swap(pip, pim); + swap(Kp, Km ); + } + if (nstable != 4) continue; + // pipipi + if (pim.size() == 2 && pip.size() == 1) { + _weight_pipipi += weight; + _hist_pipipi_pipipi-> + fill((pip[0].momentum()+pim[0].momentum()+pim[1].momentum()).mass(), weight); + _hist_pipipi_pipi-> + fill((pip[0].momentum()+pim[0].momentum()).mass(), weight); + _hist_pipipi_pipi-> + fill((pip[0].momentum()+pim[1].momentum()).mass(), weight); + } + else if (pim.size() == 1 && pip.size() == 1 && Km.size() == 1) { + _weight_Kpipi += weight; + _hist_Kpipi_Kpipi-> + fill((pim[0].momentum()+pip[0].momentum()+Km[0].momentum()).mass(), weight); + _hist_Kpipi_Kpi-> + fill((pip[0].momentum()+Km[0].momentum()).mass(), weight); + _hist_Kpipi_pipi-> + fill((pim[0].momentum()+pip[0].momentum()).mass(), weight); + } + else if (Kp.size() == 1 && Km.size() == 1 && pim.size() == 1) { + _weight_KpiK += weight; + _hist_KpiK_KpiK-> + fill((Kp[0].momentum()+Km[0].momentum()+pim[0].momentum()).mass(), weight); + _hist_KpiK_KK-> + fill((Kp[0].momentum()+Km[0].momentum()).mass(), weight); + _hist_KpiK_piK-> + fill((Kp[0].momentum()+pim[0].momentum()).mass(), weight); + } + else if (Kp.size() == 1 && Km.size() == 2) { + _weight_KKK += weight; + _hist_KKK_KKK-> + fill((Kp[0].momentum()+Km[0].momentum()+Km[1].momentum()).mass(), weight); + _hist_KKK_KK-> + fill((Kp[0].momentum()+Km[0].momentum()).mass(), weight); + _hist_KKK_KK-> + fill((Kp[0].momentum()+Km[1].momentum()).mass(), weight); + } + } + } + + + void finalize() { + if (_weight_pipipi > 0.) { + scale(_hist_pipipi_pipipi, 1.0/_weight_pipipi); + scale(_hist_pipipi_pipi , 0.5/_weight_pipipi); + } + if (_weight_Kpipi > 0.) { + scale(_hist_Kpipi_Kpipi , 1.0/_weight_Kpipi); + scale(_hist_Kpipi_Kpi , 1.0/_weight_Kpipi); + scale(_hist_Kpipi_pipi , 1.0/_weight_Kpipi); + } + if (_weight_KpiK > 0.) { + scale(_hist_KpiK_KpiK , 1.0/_weight_KpiK); + scale(_hist_KpiK_KK , 1.0/_weight_KpiK); + scale(_hist_KpiK_piK , 1.0/_weight_KpiK); + } + if (_weight_KKK > 0.) { + scale(_hist_KKK_KKK , 1.0/_weight_KKK); + scale(_hist_KKK_KK , 0.5/_weight_KKK); + } + /// @note Using autobooking for these scatters since their x values are not really obtainable from the MC data + bookScatter2D(11, 1, 1, true)->point(0).setY(100*_weight_pipipi/_weight_total, 100*sqrt(_weight_pipipi)/_weight_total); + bookScatter2D(12, 1, 1, true)->point(0).setY(100*_weight_Kpipi/_weight_total, 100*sqrt(_weight_Kpipi)/_weight_total); + bookScatter2D(13, 1, 1, true)->point(0).setY(100*_weight_KpiK/_weight_total, 100*sqrt(_weight_KpiK)/_weight_total); + bookScatter2D(14, 1, 1, true)->point(0).setY(100*_weight_KKK/_weight_total, 100*sqrt(_weight_KKK)/_weight_total); + } + + + private: + + //@{ + + // Histograms + Histo1DPtr _hist_pipipi_pipipi, _hist_pipipi_pipi; + Histo1DPtr _hist_Kpipi_Kpipi, _hist_Kpipi_Kpi, _hist_Kpipi_pipi; + Histo1DPtr _hist_KpiK_KpiK, _hist_KpiK_KK, _hist_KpiK_piK; + Histo1DPtr _hist_KKK_KKK, _hist_KKK_KK; + + // Weights counters + double _weight_total, _weight_pipipi, _weight_Kpipi, _weight_KpiK, _weight_KKK; + + //@} + + void findDecayProducts(const Particle &mother, + unsigned int & nstable, + Particles& pip, Particles& pim, + Particles& Kp, Particles& Km) { + for (const Particle &p : mother.children()) { + long id = p.pdgId(); + if (id == PID::PI0 ) + ++nstable; + else if (id == PID::K0S) + ++nstable; + else if (id == PID::PIPLUS) { + pip.push_back(p); + ++nstable; + } + else if (id == PID::PIMINUS) { + pim.push_back(p); + ++nstable; + } + else if (id == PID::KPLUS) { + Kp.push_back(p); + ++nstable; + } + else if (id == PID::KMINUS) { + Km.push_back(p); + ++nstable; + } + else if (!p.children().empty()) { + findDecayProducts(p, nstable, pip, pim, Kp, Km); + } + else ++nstable; + } + } + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2007_S7266081); + +} diff --git a/analyses/pluginMisc/BABAR_2007_S7266081.info b/analyses/pluginBABAR/BABAR_2007_S7266081.info rename from analyses/pluginMisc/BABAR_2007_S7266081.info rename to analyses/pluginBABAR/BABAR_2007_S7266081.info diff --git a/analyses/pluginMisc/BABAR_2007_S7266081.plot b/analyses/pluginBABAR/BABAR_2007_S7266081.plot rename from analyses/pluginMisc/BABAR_2007_S7266081.plot rename to analyses/pluginBABAR/BABAR_2007_S7266081.plot diff --git a/analyses/pluginMisc/BABAR_2007_S7266081.yoda b/analyses/pluginBABAR/BABAR_2007_S7266081.yoda rename from analyses/pluginMisc/BABAR_2007_S7266081.yoda rename to analyses/pluginBABAR/BABAR_2007_S7266081.yoda diff --git a/analyses/pluginBABAR/BABAR_2008_I765258.cc b/analyses/pluginBABAR/BABAR_2008_I765258.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2008_I765258.cc @@ -0,0 +1,175 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2008_I765258 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2008_I765258); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + // Book histograms + for(unsigned int ix=1;ix<6;++ix) { + stringstream ss; + ss << "TMP/n" << ix; + _nMeson[ix]= bookCounter(ss.str()); + } + + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=221 && p.pdgId()!=333) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + + if(p.pdgId()==221) { + bool matchedKK = false; + if(ncount==2) { + matchedKK = true; + for(auto const & val : nRes) { + if(abs(val.first)==321) { + if(val.second!=1) { + matchedKK = false; + break; + } + } + else if(val.second!=0) { + matchedKK = false; + break; + } + } + } + foreach (const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=333) continue; + if(p2.parents()[0].isSame(p)) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=0) continue; + bool matched2 = true; + for(auto const & val : nResB) { + if(val.second!=0) { + matched2 = false; + break; + } + } + if(matched2) + _nMeson[5]->fill(event.weight()); + else if(matchedKK) + _nMeson[4]->fill(event.weight()); + } + } + else if(p.pdgId()==333) { + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(val.first==111) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nMeson[3]->fill(event.weight()); + } + } + + + if(ntotal==3 && nCount[310]==1 && + ((nCount[ 211]==1&&nCount[-321]==1)|| + (nCount[-211]==1&&nCount[ 321]==1))) + _nMeson[1]->fill(event.weight()); + else if(ntotal==3 && nCount[321]==1 && + nCount[-321]==1 && nCount[111]==1) + _nMeson[2]->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<6;++ix) { + double sigma = _nMeson[ix]->val(); + double error = _nMeson[ix]->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nMeson[6]; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2008_I765258); + + +} diff --git a/analyses/pluginBABAR/BABAR_2008_I765258.info b/analyses/pluginBABAR/BABAR_2008_I765258.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2008_I765258.info @@ -0,0 +1,37 @@ +Name: BABAR_2008_I765258 +Year: 2008 +Summary: Cross Section for $e^+e^-\to$ $K^+K^-\eta$, $K^+K^-\pi^0$ and $K^0_SK^\pm\pi^\mp$ from threshold to 4.6 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 765258 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D77 (2008) 092002, 2008 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to$ $K^+K^-\eta$, $K^+K^-\pi^0$ and $K^0_SK^\pm\pi^\mp$ via radiative return, + including the identification of $\phi$ and $\eta$ mesons for energies from threshold to 4.6 GeV.' +Keywords: +BibKey: Aubert:2007ym +BibTeX: '@article{Aubert:2007ym, + author = "Aubert, Bernard and others", + title = "{Measurements of $e^{+} e^{-} \to K^{+} K^{-} \eta$, + $K^{+} K^{-} \pi^0$ and $K^0_{s} K^\pm \pi^\mp$ cross- + sections using initial state radiation events}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D77", + year = "2008", + pages = "092002", + doi = "10.1103/PhysRevD.77.092002", + eprint = "0710.4451", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-12968, BABAR-PUB-07-052", + SLACcitation = "%%CITATION = ARXIV:0710.4451;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2008_I765258.plot b/analyses/pluginBABAR/BABAR_2008_I765258.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2008_I765258.plot @@ -0,0 +1,51 @@ +BEGIN PLOT /BABAR_2008_I765258/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^\pm \pi^\mp)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^\pm \pi^\mp)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2008_I765258/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^0)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2008_I765258/d03-x01-y01 +Title=$\sigma(e^+e^-\to \phi\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\pi^0)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2008_I765258/d04-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\eta)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2008_I765258/d05-x01-y01 +Title=$\sigma(e^+e^-\to \phi\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\eta)$/nb +ConnectGaps=1 +LogY=0 +END PLOT + +BEGIN PLOT /BABAR_2008_I765258/d06-x01-y01 +Title=$\sigma(e^+e^-\to KK^*)$ isoscalar +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to KK^*)$/nb +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2008_I765258/d07-x01-y01 +Title=$\sigma(e^+e^-\to KK^*)$ isovector +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to KK^*)$/nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2008_I765258.yoda b/analyses/pluginBABAR/BABAR_2008_I765258.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2008_I765258.yoda @@ -0,0 +1,589 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2008_I765258/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.034, up: 0.034}}, 1: {error: {dn: -0.024, up: 0.024}}, 2: {error: {dn: -0.014, up: 0.014}}, 3: {error: {dn: -0.054, up: 0.054}}, 4: {error: {dn: -0.059, up: 0.059}}, 5: {error: {dn: -0.111, up: 0.111}}, 6: {error: {dn: -0.118, up: 0.118}}, 7: {error: {dn: -0.167, up: 0.167}}, 8: {error: {dn: -0.187, up: 0.187}}, 9: {error: {dn: -0.18, up: 0.18}}, 10: {error: {dn: -0.205, up: 0.205}}, 11: {error: {dn: -0.22, up: 0.22}}, 12: {error: {dn: -0.249, up: 0.249}}, 13: {error: {dn: -0.253, up: 0.253}}, 14: {error: {dn: -0.282, up: 0.282}}, 15: {error: {dn: -0.283, up: 0.283}}, 16: {error: {dn: -0.268, up: 0.268}}, 17: {error: {dn: -0.302, up: 0.302}}, 18: {error: {dn: -0.291, up: 0.291}}, 19: {error: {dn: -0.284, up: 0.284}}, 20: {error: {dn: -0.262, up: 0.262}}, 21: {error: {dn: -0.247, up: 0.247}}, 22: {error: {dn: -0.223, up: 0.223}}, 23: {error: {dn: -0.181, up: 0.181}}, 24: {error: {dn: -0.187, up: 0.187}}, 25: {error: {dn: -0.17, up: 0.17}}, 26: {error: {dn: -0.136, up: 0.136}}, 27: {error: {dn: -0.137, up: 0.137}}, 28: {error: {dn: -0.119, up: 0.119}}, 29: {error: {dn: -0.122, up: 0.122}}, 30: {error: {dn: -0.099, up: 0.099}}, 31: {error: {dn: -0.111, up: 0.111}}, 32: {error: {dn: -0.105, up: 0.105}}, 33: {error: {dn: -0.105, up: 0.105}}, 34: {error: {dn: -0.098, up: 0.098}}, 35: {error: {dn: -0.109, up: 0.109}}, 36: {error: {dn: -0.093, up: 0.093}}, 37: {error: {dn: -0.107, up: 0.107}}, 38: {error: {dn: -0.095, up: 0.095}}, 39: {error: {dn: -0.102, up: 0.102}}, 40: {error: {dn: -0.107, up: 0.107}}, 41: {error: {dn: -0.104, up: 0.104}}, 42: {error: {dn: -0.099, up: 0.099}}, 43: {error: {dn: -0.091, up: 0.091}}, 44: {error: {dn: -0.1, up: 0.1}}, 45: {error: {dn: -0.085, up: 0.085}}, 46: {error: {dn: -0.076, up: 0.076}}, 47: {error: {dn: -0.095, up: 0.095}}, 48: {error: {dn: -0.067, up: 0.067}}, 49: {error: {dn: -0.077, up: 0.077}}, 50: {error: {dn: -0.086, up: 0.086}}, 51: {error: {dn: -0.069, up: 0.069}}, 52: {error: {dn: -0.076, up: 0.076}}, 53: {error: {dn: -0.077, up: 0.077}}, 54: {error: {dn: -0.064, up: 0.064}}, 55: {error: {dn: -0.064, up: 0.064}}, 56: {error: {dn: -0.059, up: 0.059}}, 57: {error: {dn: -0.067, up: 0.067}}, 58: {error: {dn: -0.047, up: 0.047}}, 59: {error: {dn: -0.049, up: 0.049}}, 60: {error: {dn: -0.047, up: 0.047}}, 61: {error: {dn: -0.058, up: 0.058}}, 62: {error: {dn: -0.051, up: 0.051}}, 63: {error: {dn: -0.057, up: 0.057}}, 64: {error: {dn: -0.053, up: 0.053}}, 65: {error: {dn: -0.054, up: 0.054}}, 66: {error: {dn: -0.044, up: 0.044}}, 67: {error: {dn: -0.036, up: 0.036}}, 68: {error: {dn: -0.044, up: 0.044}}, 69: {error: {dn: -0.037, up: 0.037}}, 70: {error: {dn: -0.04, up: 0.04}}, 71: {error: {dn: -0.05, up: 0.05}}, 72: {error: {dn: -0.033, up: 0.033}}, 73: {error: {dn: -0.041, up: 0.041}}, 74: {error: {dn: -0.048, up: 0.048}}, 75: {error: {dn: -0.041, up: 0.041}}, 76: {error: {dn: -0.029, up: 0.029}}, 77: {error: {dn: 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4.000000e-03 +4.420000e+00 4.000000e-02 4.000000e-02 1.400000e-02 6.000000e-03 6.000000e-03 +4.500000e+00 4.000000e-02 4.000000e-02 3.000000e-03 4.000000e-03 4.000000e-03 +4.580000e+00 4.000000e-02 4.000000e-02 1.100000e-02 5.000000e-03 5.000000e-03 +4.660000e+00 4.000000e-02 4.000000e-02 3.000000e-03 4.000000e-03 4.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2008_I765258/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.12, up: 0.12}}, 1: {error: {dn: -0.089, up: 0.089}}, 2: {error: {dn: -0.059, up: 0.059}}, 3: {error: {dn: -0.092, up: 0.092}}, 4: {error: {dn: -0.091, up: 0.091}}, 5: {error: {dn: -0.093, up: 0.093}}, 6: {error: {dn: -0.122, up: 0.122}}, 7: {error: {dn: -0.092, up: 0.092}}, 8: {error: {dn: -0.102, up: 0.102}}, 9: {error: {dn: -0.113, up: 0.113}}, 10: {error: {dn: -0.109, up: 0.109}}, 11: {error: {dn: -0.13, up: 0.13}}, 12: {error: {dn: -0.132, up: 0.132}}, 13: {error: {dn: -0.127, up: 0.127}}, 14: {error: {dn: -0.116, up: 0.116}}, 15: {error: {dn: -0.114, up: 0.114}}, 16: {error: {dn: -0.082, up: 0.082}}, 17: {error: {dn: -0.071, up: 0.071}}, 18: {error: {dn: -0.046, up: 0.046}}, 19: {error: {dn: -0.046, up: 0.046}}, 20: {error: {dn: -0.038, up: 0.038}}, 21: {error: {dn: -0.033, up: 0.033}}, 22: {error: {dn: -0.033, up: 0.033}}, 23: {error: {dn: -0.032, up: 0.032}}, 24: {error: {dn: -0.036, up: 0.036}}, 25: {error: {dn: -0.033, up: 0.033}}, 26: {error: {dn: -0.033, up: 0.033}}, 27: {error: {dn: -0.037, up: 0.037}}, 28: {error: {dn: -0.024, up: 0.024}}, 29: {error: {dn: -0.048, up: 0.048}}, 30: {error: {dn: -0.035, up: 0.035}}, 31: {error: {dn: -0.038, up: 0.038}}, 32: {error: {dn: -0.046, up: 0.046}}, 33: {error: {dn: -0.052, up: 0.052}}, 34: {error: {dn: -0.051, up: 0.051}}, 35: {error: {dn: -0.055, up: 0.055}}, 36: {error: {dn: -0.038, up: 0.038}}, 37: {error: {dn: -0.06, up: 0.06}}, 38: {error: {dn: -0.045, up: 0.045}}, 39: {error: {dn: -0.056, up: 0.056}}, 40: {error: {dn: -0.051, up: 0.051}}, 41: {error: {dn: -0.051, up: 0.051}}, 42: {error: {dn: -0.049, up: 0.049}}, 43: {error: {dn: -0.05, up: 0.05}}, 44: {error: {dn: -0.041, up: 0.041}}, 45: {error: {dn: -0.056, up: 0.056}}, 46: {error: {dn: -0.037, up: 0.037}}, 47: {error: {dn: -0.049, up: 0.049}}, 48: {error: {dn: -0.041, up: 0.041}}, 49: {error: {dn: -0.04, up: 0.04}}, 50: {error: {dn: -0.038, up: 0.038}}, 51: {error: {dn: -0.043, up: 0.043}}, 52: {error: {dn: -0.028, up: 0.028}}, 53: {error: {dn: -0.035, up: 0.035}}, 54: {error: {dn: -0.032, up: 0.032}}, 55: {error: {dn: -0.025, up: 0.025}}, 56: {error: {dn: -0.023, up: 0.023}}, 57: {error: {dn: -0.033, up: 0.033}}, 58: {error: {dn: -0.038, up: 0.038}}, 59: {error: {dn: -0.026, up: 0.026}}, 60: {error: {dn: -0.034, up: 0.034}}, 61: {error: {dn: -0.036, up: 0.036}}, 62: {error: {dn: -0.025, up: 0.025}}, 63: {error: {dn: -0.018, up: 0.018}}, 64: {error: {dn: -0.028, up: 0.028}}, 65: {error: {dn: -0.025, up: 0.025}}, 66: {error: {dn: -0.026, up: 0.026}}, 67: {error: {dn: -0.025, up: 0.025}}, 68: {error: {dn: -0.02, up: 0.02}}, 69: {error: {dn: -0.023, up: 0.023}}, 70: {error: {dn: -0.026, up: 0.026}}, 71: {error: {dn: -0.02, up: 0.02}}, 72: {error: {dn: -0.025, up: 0.025}}, 73: {error: {dn: -0.017, up: 0.017}}, 74: {error: {dn: -0.027, up: 0.027}}, 75: {error: {dn: -0.024, up: 0.024}}, 76: {error: {dn: -0.025, up: 0.025}}, 77: {error: {dn: -0.028, up: 0.028}}, 78: {error: {dn: -0.02, up: 0.02}}, 79: {error: {dn: -0.021, up: 0.021}}, 80: {error: {dn: -0.027, up: 0.027}}, 81: {error: {dn: -0.02, up: 0.02}}, 82: {error: {dn: -0.027, up: 0.027}}, 83: {error: {dn: -0.02, up: 0.02}}, 84: {error: {dn: -0.021, up: 0.021}}, 85: {error: {dn: -0.036, up: 0.036}}, 86: {error: {dn: -0.088, up: 0.088}}, 87: {error: {dn: -0.079, up: 0.079}}, 88: {error: {dn: -0.024, up: 0.024}}, 89: {error: {dn: -0.019, up: 0.019}}, 90: {error: {dn: -0.021, up: 0.021}}, 91: {error: {dn: -0.01, up: 0.01}}, 92: {error: {dn: -0.01, up: 0.01}}, 93: {error: {dn: -0.012, up: 0.012}}, 94: {error: {dn: -0.008, up: 0.008}}, 95: {error: {dn: -0.011, up: 0.011}}, 96: {error: {dn: -0.007, up: 0.007}}, 97: {error: {dn: -0.008, up: 0.008}}, 98: {error: {dn: -0.007, up: 0.007}}, 99: {error: {dn: -0.008, up: 0.008}}, 100: {error: {dn: -0.008, up: 0.008}}, 101: {error: {dn: -0.005, up: 0.005}}, 102: {error: {dn: -0.006, up: 0.006}}, 103: {error: {dn: -0.007, up: 0.007}}, 104: {error: {dn: -0.006, up: 0.006}}, 105: {error: {dn: -0.005, up: 0.005}}, 106: {error: {dn: -0.007, up: 0.007}}, 107: {error: {dn: -0.004, up: 0.004}}, 108: {error: {dn: -0.004, up: 0.004}}, 109: {error: {dn: -0.005, up: 0.005}}, 110: {error: {dn: -0.004, up: 0.004}}, 111: {error: {dn: -0.003, up: 0.003}}, 112: {error: {dn: -0.005, up: 0.005}}, 113: {error: {dn: -0.004, up: 0.004}}, 114: {error: {dn: -0.004, up: 0.004}}, 115: {error: {dn: -0.003, up: 0.003}}, 116: {error: {dn: -0.002, up: 0.002}}, 117: {error: {dn: -0.002, up: 0.002}}} + +IsRef: 1 +Path: /REF/BABAR_2008_I765258/d02-x01-y01 +Title: doi:10.17182/hepdata.50372.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.370000e+00 1.000000e-02 1.000000e-02 2.080000e-01 1.200000e-01 1.200000e-01 +1.390000e+00 1.000000e-02 1.000000e-02 1.000000e-01 8.900000e-02 8.900000e-02 +1.410000e+00 1.000000e-02 1.000000e-02 4.200000e-02 5.900000e-02 5.900000e-02 +1.430000e+00 1.000000e-02 1.000000e-02 2.410000e-01 9.200000e-02 9.200000e-02 +1.450000e+00 1.000000e-02 1.000000e-02 1.930000e-01 9.100000e-02 9.100000e-02 +1.470000e+00 1.000000e-02 1.000000e-02 3.700000e-01 9.300000e-02 9.300000e-02 +1.490000e+00 1.000000e-02 1.000000e-02 6.880000e-01 1.220000e-01 1.220000e-01 +1.510000e+00 1.000000e-02 1.000000e-02 3.850000e-01 9.200000e-02 9.200000e-02 +1.530000e+00 1.000000e-02 1.000000e-02 4.850000e-01 1.020000e-01 1.020000e-01 +1.550000e+00 1.000000e-02 1.000000e-02 6.100000e-01 1.130000e-01 1.130000e-01 +1.570000e+00 1.000000e-02 1.000000e-02 5.560000e-01 1.090000e-01 1.090000e-01 +1.590000e+00 1.000000e-02 1.000000e-02 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6.980000e-01 7.900000e-02 7.900000e-02 +3.130000e+00 1.000000e-02 1.000000e-02 4.900000e-02 2.400000e-02 2.400000e-02 +3.150000e+00 1.000000e-02 1.000000e-02 3.900000e-02 1.900000e-02 1.900000e-02 +3.170000e+00 1.000000e-02 1.000000e-02 4.700000e-02 2.100000e-02 2.100000e-02 +3.190000e+00 1.000000e-02 1.000000e-02 5.000000e-03 1.000000e-02 1.000000e-02 +3.220000e+00 2.000000e-02 2.000000e-02 1.600000e-02 1.000000e-02 1.000000e-02 +3.260000e+00 2.000000e-02 2.000000e-02 3.100000e-02 1.200000e-02 1.200000e-02 +3.300000e+00 2.000000e-02 2.000000e-02 7.000000e-03 8.000000e-03 8.000000e-03 +3.340000e+00 2.000000e-02 2.000000e-02 2.500000e-02 1.100000e-02 1.100000e-02 +3.380000e+00 2.000000e-02 2.000000e-02 1.000000e-02 7.000000e-03 7.000000e-03 +3.420000e+00 2.000000e-02 2.000000e-02 7.000000e-03 8.000000e-03 8.000000e-03 +3.460000e+00 2.000000e-02 2.000000e-02 2.000000e-03 7.000000e-03 7.000000e-03 +3.500000e+00 2.000000e-02 2.000000e-02 1.200000e-02 8.000000e-03 8.000000e-03 +3.540000e+00 2.000000e-02 2.000000e-02 1.300000e-02 8.000000e-03 8.000000e-03 +3.590000e+00 3.000000e-02 3.000000e-02 6.000000e-03 5.000000e-03 5.000000e-03 +3.650000e+00 3.000000e-02 3.000000e-02 6.000000e-03 6.000000e-03 6.000000e-03 +3.710000e+00 3.000000e-02 3.000000e-02 1.500000e-02 7.000000e-03 7.000000e-03 +3.770000e+00 3.000000e-02 3.000000e-02 1.300000e-02 6.000000e-03 6.000000e-03 +3.830000e+00 3.000000e-02 3.000000e-02 4.000000e-03 5.000000e-03 5.000000e-03 +3.890000e+00 3.000000e-02 3.000000e-02 1.800000e-02 7.000000e-03 7.000000e-03 +3.950000e+00 3.000000e-02 3.000000e-02 5.000000e-03 4.000000e-03 4.000000e-03 +4.010000e+00 3.000000e-02 3.000000e-02 3.000000e-03 4.000000e-03 4.000000e-03 +4.070000e+00 3.000000e-02 3.000000e-02 2.000000e-03 5.000000e-03 5.000000e-03 +4.130000e+00 3.000000e-02 3.000000e-02 5.000000e-03 4.000000e-03 4.000000e-03 +4.200000e+00 4.000000e-02 4.000000e-02 2.000000e-03 3.000000e-03 3.000000e-03 +4.280000e+00 4.000000e-02 4.000000e-02 1.200000e-02 5.000000e-03 5.000000e-03 +4.360000e+00 4.000000e-02 4.000000e-02 8.000000e-03 4.000000e-03 4.000000e-03 +4.440000e+00 4.000000e-02 4.000000e-02 6.000000e-03 4.000000e-03 4.000000e-03 +4.520000e+00 4.000000e-02 4.000000e-02 5.000000e-03 3.000000e-03 3.000000e-03 +4.600000e+00 4.000000e-02 4.000000e-02 2.000000e-03 2.000000e-03 2.000000e-03 +4.680000e+00 4.000000e-02 4.000000e-02 1.000000e-03 2.000000e-03 2.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2008_I765258/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.016, up: 0.016}, sys: {dn: -0.0012180000000000001, up: 0.0012180000000000001}}, 1: {error: {dn: -0.018, up: 0.018}, sys: {dn: -0.002175, up: 0.002175}}, 2: {error: {dn: -0.022, up: 0.022}, sys: {dn: -0.002871, up: 0.002871}}, 3: {error: {dn: -0.038, up: 0.038}, sys: {dn: -0.006350999999999999, up: 0.006350999999999999}}, 4: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.016617, up: 0.016617}}, 5: {error: {dn: -0.039, up: 0.039}, sys: {dn: -0.0075689999999999985, up: 0.0075689999999999985}}, 6: {error: {dn: -0.035, up: 0.035}, sys: {dn: -0.006263999999999999, up: 0.006263999999999999}}, 7: {error: {dn: -0.041, up: 0.041}, sys: {dn: -0.0087, up: 0.0087}}, 8: {error: {dn: -0.015, up: 0.015}, sys: {dn: -0.0013049999999999997, up: 0.0013049999999999997}}, 9: {error: {dn: -0.027, up: 0.027}, sys: {dn: -0.0040019999999999995, up: 0.0040019999999999995}}, 10: {error: {dn: -0.038, up: 0.038}, sys: {dn: -0.008091, up: 0.008091}}, 11: {error: {dn: -0.036, up: 0.036}, sys: {dn: -0.007742999999999999, up: 0.007742999999999999}}, 12: {error: {dn: -0.004, up: 0.004}, sys: {dn: -0.000174, up: 0.000174}}, 13: {error: {dn: -0.005, up: 0.005}, sys: {dn: -0.000522, up: 0.000522}}, 14: {error: {dn: -0.002, up: 0.002}, sys: {dn: -0.000174, up: 0.000174}}} + +IsRef: 1 +Path: /REF/BABAR_2008_I765258/d03-x01-y01 +Title: doi:10.17182/hepdata.50372.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.250000e+00 5.000000e-02 5.000000e-02 1.400000e-02 1.604629e-02 1.604629e-02 +1.350000e+00 5.000000e-02 5.000000e-02 2.500000e-02 1.813093e-02 1.813093e-02 +1.450000e+00 5.000000e-02 5.000000e-02 3.300000e-02 2.218654e-02 2.218654e-02 +1.525000e+00 2.500000e-02 2.500000e-02 7.300000e-02 3.852707e-02 3.852707e-02 +1.575000e+00 2.500000e-02 2.500000e-02 1.910000e-01 6.225853e-02 6.225853e-02 +1.625000e+00 2.500000e-02 2.500000e-02 8.700000e-02 3.972770e-02 3.972770e-02 +1.675000e+00 2.500000e-02 2.500000e-02 7.200000e-02 3.555612e-02 3.555612e-02 +1.725000e+00 2.500000e-02 2.500000e-02 1.000000e-01 4.191289e-02 4.191289e-02 +1.775000e+00 2.500000e-02 2.500000e-02 1.500000e-02 1.505666e-02 1.505666e-02 +1.825000e+00 2.500000e-02 2.500000e-02 4.600000e-02 2.729498e-02 2.729498e-02 +1.875000e+00 2.500000e-02 2.500000e-02 9.300000e-02 3.885182e-02 3.885182e-02 +1.925000e+00 2.500000e-02 2.500000e-02 8.900000e-02 3.682328e-02 3.682328e-02 +2.025000e+00 7.500000e-02 7.500000e-02 2.000000e-03 4.003783e-03 4.003783e-03 +2.200000e+00 1.000000e-01 1.000000e-01 6.000000e-03 5.027175e-03 5.027175e-03 +2.450000e+00 1.500000e-01 1.500000e-01 2.000000e-03 2.007555e-03 2.007555e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2008_I765258/d04-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.04, up: 0.04}}, 1: {error: {dn: -0.03, up: 0.03}}, 2: {error: {dn: -0.02, up: 0.02}}, 3: {error: {dn: -0.02, up: 0.02}}, 4: {error: {dn: -0.01, up: 0.01}}, 5: {error: {dn: -0.01, up: 0.01}}, 6: {error: {dn: -0.01, up: 0.01}}, 7: {error: {dn: -0.01, up: 0.01}}, 8: {error: {dn: -0.01, up: 0.01}}, 9: {error: {dn: -0.01, up: 0.01}}, 10: {error: {dn: -0.01, up: 0.01}}, 11: {error: {dn: -0.02, up: 0.02}}, 12: {error: {dn: -0.02, up: 0.02}}, 13: {error: {dn: -0.01, up: 0.01}}, 14: {error: {dn: -0.01, up: 0.01}}, 15: {error: {dn: -0.02, up: 0.02}}, 16: {error: {dn: -0.01, up: 0.01}}, 17: {error: {dn: -0.02, up: 0.02}}, 18: {error: {dn: -0.02, up: 0.02}}, 19: {error: {dn: -0.01, up: 0.01}}, 20: {error: {dn: -0.01, up: 0.01}}, 21: {error: {dn: -0.09, up: 0.09}}, 22: {error: {dn: -0.09, up: 0.09}}, 23: {error: {dn: -0.05, up: 0.05}}} + +IsRef: 1 +Path: /REF/BABAR_2008_I765258/d04-x01-y01 +Title: doi:10.17182/hepdata.50372.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.690000e+00 5.000000e-02 5.000000e-02 8.000000e-02 4.000000e-02 4.000000e-02 +1.790000e+00 5.000000e-02 5.000000e-02 1.000000e-02 3.000000e-02 3.000000e-02 +1.890000e+00 5.000000e-02 5.000000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +1.990000e+00 5.000000e-02 5.000000e-02 3.000000e-02 2.000000e-02 2.000000e-02 +2.090000e+00 5.000000e-02 5.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +2.190000e+00 5.000000e-02 5.000000e-02 0.000000e+00 1.000000e-02 1.000000e-02 +2.290000e+00 5.000000e-02 5.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +2.390000e+00 5.000000e-02 5.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +2.490000e+00 5.000000e-02 5.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +2.590000e+00 5.000000e-02 5.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +2.660000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +2.700000e+00 2.000000e-02 2.000000e-02 1.000000e-02 2.000000e-02 2.000000e-02 +2.740000e+00 2.000000e-02 2.000000e-02 2.000000e-02 2.000000e-02 2.000000e-02 +2.780000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +2.820000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +2.860000e+00 2.000000e-02 2.000000e-02 1.000000e-02 2.000000e-02 2.000000e-02 +2.900000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +2.940000e+00 2.000000e-02 2.000000e-02 2.000000e-02 2.000000e-02 2.000000e-02 +2.980000e+00 2.000000e-02 2.000000e-02 3.000000e-02 2.000000e-02 2.000000e-02 +3.020000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +3.060000e+00 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +3.090000e+00 1.000000e-02 1.000000e-02 2.700000e-01 9.000000e-02 9.000000e-02 +3.110000e+00 1.000000e-02 1.000000e-02 3.000000e-01 9.000000e-02 9.000000e-02 +3.130000e+00 1.000000e-02 1.000000e-02 1.100000e-01 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2008_I765258/d05-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.11, up: 0.11}, sys: {dn: -0.00583, up: 0.00583}}, 1: {error: {dn: -0.18, up: 0.18}, sys: {dn: -0.00848, up: 0.00848}}, 2: {error: {dn: -0.31, up: 0.31}, sys: {dn: -0.0424, up: 0.0424}}, 3: {error: {dn: -0.41, up: 0.41}, sys: {dn: -0.08003, up: 0.08003}}, 4: {error: {dn: -0.49, up: 0.49}, sys: {dn: -0.12401999999999998, up: 0.12401999999999998}}, 5: {error: {dn: -0.53, up: 0.53}, sys: {dn: -0.14734, up: 0.14734}}, 6: {error: {dn: -0.53, up: 0.53}, sys: {dn: -0.15423, up: 0.15423}}, 7: {error: {dn: -0.53, up: 0.53}, sys: {dn: -0.15582, up: 0.15582}}, 8: {error: {dn: -0.39, up: 0.39}, sys: {dn: -0.08850999999999999, up: 0.08850999999999999}}, 9: {error: {dn: -0.45, up: 0.45}, sys: {dn: -0.11553999999999999, up: 0.11553999999999999}}, 10: {error: {dn: -0.45, up: 0.45}, sys: {dn: -0.12295999999999999, up: 0.12295999999999999}}, 11: {error: {dn: -0.41, up: 0.41}, sys: {dn: -0.09487, up: 0.09487}}, 12: {error: {dn: -0.3, up: 0.3}, sys: {dn: -0.052469999999999996, up: 0.052469999999999996}}, 13: {error: {dn: -0.3, up: 0.3}, sys: {dn: -0.05141, up: 0.05141}}, 14: {error: {dn: -0.25, up: 0.25}, sys: {dn: -0.03975, up: 0.03975}}, 15: {error: {dn: -0.3, up: 0.3}, sys: {dn: -0.05618, up: 0.05618}}, 16: {error: {dn: -0.23, up: 0.23}, sys: {dn: -0.03392, up: 0.03392}}, 17: {error: {dn: -0.26, up: 0.26}, sys: {dn: -0.04611, up: 0.04611}}, 18: {error: {dn: -0.24, up: 0.24}, sys: {dn: -0.03763, up: 0.03763}}, 19: {error: {dn: -0.31, up: 0.31}, sys: {dn: -0.06572, up: 0.06572}}, 20: {error: {dn: -0.22, up: 0.22}, sys: {dn: -0.03233, up: 0.03233}}, 21: {error: {dn: -0.2, up: 0.2}, sys: {dn: -0.02809, up: 0.02809}}, 22: {error: {dn: -0.2, up: 0.2}, sys: {dn: -0.027559999999999998, up: 0.027559999999999998}}, 23: {error: {dn: -0.16, up: 0.16}, sys: {dn: -0.01961, up: 0.01961}}, 24: {error: {dn: -0.16, up: 0.16}, sys: {dn: -0.01908, up: 0.01908}}, 25: {error: {dn: -0.18, up: 0.18}, sys: {dn: -0.022789999999999998, up: 0.022789999999999998}}, 26: {error: {dn: -0.14, up: 0.14}, sys: {dn: -0.015369999999999998, up: 0.015369999999999998}}, 27: {error: {dn: -0.2, up: 0.2}, sys: {dn: -0.029680000000000005, up: 0.029680000000000005}}, 28: {error: {dn: -0.22, up: 0.22}, sys: {dn: -0.037099999999999994, up: 0.037099999999999994}}, 29: {error: {dn: -0.18, up: 0.18}, sys: {dn: -0.025439999999999997, up: 0.025439999999999997}}, 30: {error: {dn: -0.14, up: 0.14}, sys: {dn: -0.01431, up: 0.01431}}, 31: {error: {dn: -0.12, up: 0.12}, sys: {dn: -0.0106, up: 0.0106}}, 32: {error: {dn: -0.13, up: 0.13}, sys: {dn: -0.01431, up: 0.01431}}, 33: {error: {dn: -0.12, up: 0.12}, sys: {dn: -0.0106, up: 0.0106}}, 34: {error: {dn: -0.12, up: 0.12}, sys: {dn: -0.00848, up: 0.00848}}, 35: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.006889999999999999, up: 0.006889999999999999}}, 36: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.006889999999999999, up: 0.006889999999999999}}, 37: {error: {dn: -0.13, up: 0.13}, sys: {dn: -0.013779999999999999, up: 0.013779999999999999}}, 38: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.006889999999999999, up: 0.006889999999999999}}, 39: {error: {dn: -0.09, up: 0.09}, sys: {dn: -0.006889999999999999, up: 0.006889999999999999}}, 40: {error: {dn: -0.17, up: 0.17}, sys: {dn: -0.021729999999999996, up: 0.021729999999999996}}, 41: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.0031799999999999997, up: 0.0031799999999999997}}, 42: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.0031799999999999997, up: 0.0031799999999999997}}, 43: {error: {dn: -0.03, up: 0.03}, sys: {dn: -0.0015899999999999998, up: 0.0015899999999999998}}, 44: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.006359999999999999, up: 0.006359999999999999}}, 45: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.0031799999999999997, up: 0.0031799999999999997}}, 46: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.006359999999999999, up: 0.006359999999999999}}, 47: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.006359999999999999, up: 0.006359999999999999}}, 48: {error: {dn: -0.06, up: 0.06}, sys: {dn: -0.006359999999999999, up: 0.006359999999999999}}, 49: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.00477, up: 0.00477}}, 50: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.00477, up: 0.00477}}, 51: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.00424, up: 0.00424}}, 52: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.0037100000000000006, up: 0.0037100000000000006}}, 53: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.0031799999999999997, up: 0.0031799999999999997}}, 54: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.00477, up: 0.00477}}, 55: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.00106, up: 0.00106}}, 56: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.00106, up: 0.00106}}, 57: {error: {dn: -0.05, up: 0.05}, sys: {dn: -0.006889999999999999, up: 0.006889999999999999}}, 58: {error: {dn: -0.04, up: 0.04}, sys: {dn: -0.00424, up: 0.00424}}, 59: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.00106, up: 0.00106}}, 60: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.00106, up: 0.00106}}, 61: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.00053, up: 0.00053}}, 62: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.00106, up: 0.00106}}, 63: {error: {dn: -0.02, up: 0.02}, sys: {dn: -0.0015899999999999998, up: 0.0015899999999999998}}} + +IsRef: 1 +Path: /REF/BABAR_2008_I765258/d05-x01-y01 +Title: doi:10.17182/hepdata.50372.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.570000e+00 1.000000e-02 1.000000e-02 1.100000e-01 1.101544e-01 1.101544e-01 +1.590000e+00 1.000000e-02 1.000000e-02 1.600000e-01 1.801996e-01 1.801996e-01 +1.610000e+00 1.000000e-02 1.000000e-02 8.000000e-01 3.128862e-01 3.128862e-01 +1.630000e+00 1.000000e-02 1.000000e-02 1.510000e+00 4.177377e-01 4.177377e-01 +1.650000e+00 1.000000e-02 1.000000e-02 2.340000e+00 5.054512e-01 5.054512e-01 +1.670000e+00 1.000000e-02 1.000000e-02 2.780000e+00 5.500992e-01 5.500992e-01 +1.690000e+00 1.000000e-02 1.000000e-02 2.910000e+00 5.519845e-01 5.519845e-01 +1.710000e+00 1.000000e-02 1.000000e-02 2.940000e+00 5.524309e-01 5.524309e-01 +1.730000e+00 1.000000e-02 1.000000e-02 1.670000e+00 3.999175e-01 3.999175e-01 +1.750000e+00 1.000000e-02 1.000000e-02 2.180000e+00 4.645961e-01 4.645961e-01 +1.770000e+00 1.000000e-02 1.000000e-02 2.320000e+00 4.664967e-01 4.664967e-01 +1.790000e+00 1.000000e-02 1.000000e-02 1.790000e+00 4.208329e-01 4.208329e-01 +1.810000e+00 1.000000e-02 1.000000e-02 9.900000e-01 3.045539e-01 3.045539e-01 +1.830000e+00 1.000000e-02 1.000000e-02 9.700000e-01 3.043731e-01 3.043731e-01 +1.850000e+00 1.000000e-02 1.000000e-02 7.500000e-01 2.531404e-01 2.531404e-01 +1.870000e+00 1.000000e-02 1.000000e-02 1.060000e+00 3.052150e-01 3.052150e-01 +1.890000e+00 1.000000e-02 1.000000e-02 6.400000e-01 2.324878e-01 2.324878e-01 +1.910000e+00 1.000000e-02 1.000000e-02 8.700000e-01 2.640571e-01 2.640571e-01 +1.930000e+00 1.000000e-02 1.000000e-02 7.100000e-01 2.429321e-01 2.429321e-01 +1.950000e+00 1.000000e-02 1.000000e-02 1.240000e+00 3.168898e-01 3.168898e-01 +1.970000e+00 1.000000e-02 1.000000e-02 6.100000e-01 2.223628e-01 2.223628e-01 +1.990000e+00 1.000000e-02 1.000000e-02 5.300000e-01 2.019630e-01 2.019630e-01 +2.010000e+00 1.000000e-02 1.000000e-02 5.200000e-01 2.018900e-01 2.018900e-01 +2.030000e+00 1.000000e-02 1.000000e-02 3.700000e-01 1.611972e-01 1.611972e-01 +2.050000e+00 1.000000e-02 1.000000e-02 3.600000e-01 1.611336e-01 1.611336e-01 +2.070000e+00 1.000000e-02 1.000000e-02 4.300000e-01 1.814370e-01 1.814370e-01 +2.090000e+00 1.000000e-02 1.000000e-02 2.900000e-01 1.408412e-01 1.408412e-01 +2.110000e+00 1.000000e-02 1.000000e-02 5.600000e-01 2.021903e-01 2.021903e-01 +2.130000e+00 1.000000e-02 1.000000e-02 7.000000e-01 2.231063e-01 2.231063e-01 +2.150000e+00 1.000000e-02 1.000000e-02 4.800000e-01 1.817889e-01 1.817889e-01 +2.170000e+00 1.000000e-02 1.000000e-02 2.700000e-01 1.407294e-01 1.407294e-01 +2.190000e+00 1.000000e-02 1.000000e-02 2.000000e-01 1.204673e-01 1.204673e-01 +2.210000e+00 1.000000e-02 1.000000e-02 2.700000e-01 1.307852e-01 1.307852e-01 +2.230000e+00 1.000000e-02 1.000000e-02 2.000000e-01 1.204673e-01 1.204673e-01 +2.250000e+00 1.000000e-02 1.000000e-02 1.600000e-01 1.202993e-01 1.202993e-01 +2.270000e+00 1.000000e-02 1.000000e-02 1.300000e-01 9.026335e-02 9.026335e-02 +2.290000e+00 1.000000e-02 1.000000e-02 1.300000e-01 9.026335e-02 9.026335e-02 +2.310000e+00 1.000000e-02 1.000000e-02 2.600000e-01 1.307283e-01 1.307283e-01 +2.330000e+00 1.000000e-02 1.000000e-02 1.300000e-01 9.026335e-02 9.026335e-02 +2.350000e+00 1.000000e-02 1.000000e-02 1.300000e-01 9.026335e-02 9.026335e-02 +2.370000e+00 1.000000e-02 1.000000e-02 4.100000e-01 1.713832e-01 1.713832e-01 +2.390000e+00 1.000000e-02 1.000000e-02 6.000000e-02 6.008421e-02 6.008421e-02 +2.420000e+00 2.000000e-02 2.000000e-02 6.000000e-02 4.012621e-02 4.012621e-02 +2.460000e+00 2.000000e-02 2.000000e-02 3.000000e-02 3.004211e-02 3.004211e-02 +2.500000e+00 2.000000e-02 2.000000e-02 1.200000e-01 6.033614e-02 6.033614e-02 +2.540000e+00 2.000000e-02 2.000000e-02 6.000000e-02 4.012621e-02 4.012621e-02 +2.580000e+00 2.000000e-02 2.000000e-02 1.200000e-01 6.033614e-02 6.033614e-02 +2.620000e+00 2.000000e-02 2.000000e-02 1.200000e-01 6.033614e-02 6.033614e-02 +2.660000e+00 2.000000e-02 2.000000e-02 1.200000e-01 6.033614e-02 6.033614e-02 +2.700000e+00 2.000000e-02 2.000000e-02 9.000000e-02 5.022701e-02 5.022701e-02 +2.740000e+00 2.000000e-02 2.000000e-02 9.000000e-02 5.022701e-02 5.022701e-02 +2.780000e+00 2.000000e-02 2.000000e-02 8.000000e-02 5.017945e-02 5.017945e-02 +2.820000e+00 2.000000e-02 2.000000e-02 7.000000e-02 5.013745e-02 5.013745e-02 +2.860000e+00 2.000000e-02 2.000000e-02 6.000000e-02 4.012621e-02 4.012621e-02 +2.910000e+00 3.000000e-02 3.000000e-02 9.000000e-02 4.028341e-02 4.028341e-02 +2.970000e+00 3.000000e-02 3.000000e-02 2.000000e-02 2.002807e-02 2.002807e-02 +3.030000e+00 3.000000e-02 3.000000e-02 2.000000e-02 2.002807e-02 2.002807e-02 +3.090000e+00 3.000000e-02 3.000000e-02 1.300000e-01 5.047249e-02 5.047249e-02 +3.150000e+00 3.000000e-02 3.000000e-02 8.000000e-02 4.022409e-02 4.022409e-02 +3.210000e+00 3.000000e-02 3.000000e-02 2.000000e-02 2.002807e-02 2.002807e-02 +3.270000e+00 3.000000e-02 3.000000e-02 2.000000e-02 2.002807e-02 2.002807e-02 +3.330000e+00 3.000000e-02 3.000000e-02 1.000000e-02 2.000702e-02 2.000702e-02 +3.390000e+00 3.000000e-02 3.000000e-02 2.000000e-02 2.002807e-02 2.002807e-02 +3.450000e+00 3.000000e-02 3.000000e-02 3.000000e-02 2.006310e-02 2.006310e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2008_I765258/d06-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.75, up: 0.75}}, 1: {error: {dn: -0.36, up: 0.36}}, 2: {error: {dn: -0.42, up: 0.42}}, 3: {error: {dn: -0.48, up: 0.48}}, 4: {error: {dn: -0.39, up: 0.39}}, 5: {error: {dn: -0.51, up: 0.51}}, 6: {error: {dn: -0.57, up: 0.57}}, 7: {error: {dn: -0.69, up: 0.69}}, 8: {error: {dn: -0.66, up: 0.66}}, 9: {error: {dn: -0.75, up: 0.75}}, 10: {error: {dn: -0.81, up: 0.81}}, 11: {error: {dn: -0.75, up: 0.75}}, 12: {error: {dn: -0.84, up: 0.84}}, 13: {error: {dn: -0.78, up: 0.78}}, 14: {error: {dn: -0.75, up: 0.75}}, 15: {error: {dn: -0.72, up: 0.72}}, 16: {error: {dn: -0.69, up: 0.69}}, 17: {error: {dn: -0.57, up: 0.57}}, 18: {error: {dn: -0.45, up: 0.45}}, 19: {error: {dn: -0.45, up: 0.45}}, 20: {error: {dn: -0.48, up: 0.48}}, 21: {error: {dn: -0.3, up: 0.3}}, 22: {error: {dn: -0.3, up: 0.3}}, 23: {error: {dn: -0.3, up: 0.3}}, 24: {error: {dn: -0.36, up: 0.36}}, 25: {error: {dn: -0.27, up: 0.27}}, 26: {error: {dn: -0.18, up: 0.18}}, 27: {error: {dn: -0.18, up: 0.18}}, 28: {error: {dn: -0.18, up: 0.18}}, 29: {error: {dn: -0.15, up: 0.15}}, 30: {error: {dn: -0.18, up: 0.18}}, 31: {error: {dn: -0.18, up: 0.18}}, 32: {error: {dn: -0.12, up: 0.12}}, 33: {error: {dn: -0.15, up: 0.15}}, 34: {error: {dn: -0.06, up: 0.06}}, 35: {error: {dn: -0.15, up: 0.15}}, 36: {error: {dn: -0.09, up: 0.09}}, 37: {error: {dn: -0.09, up: 0.09}}, 38: {error: {dn: -0.06, up: 0.06}}, 39: {error: {dn: -0.09, up: 0.09}}, 40: {error: {dn: -0.09, up: 0.09}}, 41: {error: {dn: -0.06, up: 0.06}}, 42: {error: {dn: -0.06, up: 0.06}}, 43: {error: {dn: -0.03, up: 0.03}}, 44: {error: {dn: -0.03, up: 0.03}}, 45: {error: {dn: -0.06, up: 0.06}}, 46: {error: {dn: -0.03, up: 0.03}}, 47: {error: {dn: -0.03, up: 0.03}}, 48: {error: {dn: -0.15, up: 0.15}}} + +IsRef: 1 +Path: /REF/BABAR_2008_I765258/d06-x01-y01 +Title: doi:10.17182/hepdata.50372.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.410000e+00 1.000000e-02 1.000000e-02 1.260000e+00 7.500000e-01 7.500000e-01 +1.430000e+00 1.000000e-02 1.000000e-02 9.600000e-01 3.600000e-01 3.600000e-01 +1.450000e+00 1.000000e-02 1.000000e-02 1.620000e+00 4.200000e-01 4.200000e-01 +1.470000e+00 1.000000e-02 1.000000e-02 2.610000e+00 4.800000e-01 4.800000e-01 +1.490000e+00 1.000000e-02 1.000000e-02 1.380000e+00 3.900000e-01 3.900000e-01 +1.510000e+00 1.000000e-02 1.000000e-02 2.010000e+00 5.100000e-01 5.100000e-01 +1.530000e+00 1.000000e-02 1.000000e-02 3.060000e+00 5.700000e-01 5.700000e-01 +1.550000e+00 1.000000e-02 1.000000e-02 4.620000e+00 6.900000e-01 6.900000e-01 +1.570000e+00 1.000000e-02 1.000000e-02 5.280000e+00 6.600000e-01 6.600000e-01 +1.590000e+00 1.000000e-02 1.000000e-02 8.130000e+00 7.500000e-01 7.500000e-01 +1.610000e+00 1.000000e-02 1.000000e-02 6.630000e+00 8.100000e-01 8.100000e-01 +1.630000e+00 1.000000e-02 1.000000e-02 7.350000e+00 7.500000e-01 7.500000e-01 +1.650000e+00 1.000000e-02 1.000000e-02 9.480000e+00 8.400000e-01 8.400000e-01 +1.670000e+00 1.000000e-02 1.000000e-02 8.340000e+00 7.800000e-01 7.800000e-01 +1.690000e+00 1.000000e-02 1.000000e-02 8.400000e+00 7.500000e-01 7.500000e-01 +1.710000e+00 1.000000e-02 1.000000e-02 7.860000e+00 7.200000e-01 7.200000e-01 +1.730000e+00 1.000000e-02 1.000000e-02 6.450000e+00 6.900000e-01 6.900000e-01 +1.750000e+00 1.000000e-02 1.000000e-02 5.280000e+00 5.700000e-01 5.700000e-01 +1.770000e+00 1.000000e-02 1.000000e-02 2.970000e+00 4.500000e-01 4.500000e-01 +1.790000e+00 1.000000e-02 1.000000e-02 3.240000e+00 4.500000e-01 4.500000e-01 +1.810000e+00 1.000000e-02 1.000000e-02 3.570000e+00 4.800000e-01 4.800000e-01 +1.830000e+00 1.000000e-02 1.000000e-02 1.260000e+00 3.000000e-01 3.000000e-01 +1.850000e+00 1.000000e-02 1.000000e-02 1.560000e+00 3.000000e-01 3.000000e-01 +1.870000e+00 1.000000e-02 1.000000e-02 1.170000e+00 3.000000e-01 3.000000e-01 +1.890000e+00 1.000000e-02 1.000000e-02 1.590000e+00 3.600000e-01 3.600000e-01 +1.910000e+00 1.000000e-02 1.000000e-02 1.020000e+00 2.700000e-01 2.700000e-01 +1.940000e+00 2.000000e-02 2.000000e-02 1.110000e+00 1.800000e-01 1.800000e-01 +1.980000e+00 2.000000e-02 2.000000e-02 6.300000e-01 1.800000e-01 1.800000e-01 +2.020000e+00 2.000000e-02 2.000000e-02 8.400000e-01 1.800000e-01 1.800000e-01 +2.060000e+00 2.000000e-02 2.000000e-02 4.500000e-01 1.500000e-01 1.500000e-01 +2.100000e+00 2.000000e-02 2.000000e-02 5.700000e-01 1.800000e-01 1.800000e-01 +2.140000e+00 2.000000e-02 2.000000e-02 8.400000e-01 1.800000e-01 1.800000e-01 +2.180000e+00 2.000000e-02 2.000000e-02 4.200000e-01 1.200000e-01 1.200000e-01 +2.220000e+00 2.000000e-02 2.000000e-02 3.000000e-01 1.500000e-01 1.500000e-01 +2.260000e+00 2.000000e-02 2.000000e-02 1.200000e-01 6.000000e-02 6.000000e-02 +2.300000e+00 2.000000e-02 2.000000e-02 4.500000e-01 1.500000e-01 1.500000e-01 +2.340000e+00 2.000000e-02 2.000000e-02 1.500000e-01 9.000000e-02 9.000000e-02 +2.380000e+00 2.000000e-02 2.000000e-02 2.100000e-01 9.000000e-02 9.000000e-02 +2.420000e+00 2.000000e-02 2.000000e-02 1.500000e-01 6.000000e-02 6.000000e-02 +2.460000e+00 2.000000e-02 2.000000e-02 2.400000e-01 9.000000e-02 9.000000e-02 +2.500000e+00 2.000000e-02 2.000000e-02 2.100000e-01 9.000000e-02 9.000000e-02 +2.560000e+00 4.000000e-02 4.000000e-02 1.500000e-01 6.000000e-02 6.000000e-02 +2.640000e+00 4.000000e-02 4.000000e-02 1.800000e-01 6.000000e-02 6.000000e-02 +2.720000e+00 4.000000e-02 4.000000e-02 1.200000e-01 3.000000e-02 3.000000e-02 +2.800000e+00 4.000000e-02 4.000000e-02 9.000000e-02 3.000000e-02 3.000000e-02 +2.880000e+00 4.000000e-02 4.000000e-02 9.000000e-02 6.000000e-02 6.000000e-02 +2.960000e+00 4.000000e-02 4.000000e-02 1.500000e-01 3.000000e-02 3.000000e-02 +3.040000e+00 4.000000e-02 4.000000e-02 9.000000e-02 3.000000e-02 3.000000e-02 +3.120000e+00 4.000000e-02 4.000000e-02 1.950000e+00 1.500000e-01 1.500000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2008_I765258/d07-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.67, up: 0.67}}, 1: {error: {dn: -0.4, up: 0.4}}, 2: {error: {dn: -0.43, up: 0.43}}, 3: {error: {dn: -0.39, up: 0.39}}, 4: {error: {dn: -0.5, up: 0.5}}, 5: {error: {dn: -0.58, up: 0.58}}, 6: {error: {dn: -0.52, up: 0.52}}, 7: {error: {dn: -0.55, up: 0.55}}, 8: {error: {dn: -0.42, up: 0.42}}, 9: {error: {dn: -0.33, up: 0.33}}, 10: {error: {dn: -0.68, up: 0.68}}, 11: {error: {dn: -0.38, up: 0.38}}, 12: {error: {dn: -0.37, up: 0.37}}, 13: {error: {dn: -0.5, up: 0.5}}, 14: {error: {dn: -0.36, up: 0.36}}, 15: {error: {dn: -0.3, up: 0.3}}, 16: {error: {dn: -0.35, up: 0.35}}, 17: {error: {dn: -0.32, up: 0.32}}, 18: {error: {dn: -0.32, up: 0.32}}, 19: {error: {dn: -0.32, up: 0.32}}, 20: {error: {dn: -0.18, up: 0.18}}, 21: {error: {dn: -0.31, up: 0.31}}, 22: {error: {dn: -0.24, up: 0.24}}, 23: {error: {dn: -0.29, up: 0.29}}, 24: {error: {dn: -0.26, up: 0.26}}, 25: {error: {dn: -0.14, up: 0.14}}, 26: {error: {dn: -0.17, up: 0.17}}, 27: {error: {dn: -0.12, up: 0.12}}, 28: {error: {dn: -0.16, up: 0.16}}, 29: {error: {dn: -0.2, up: 0.2}}, 30: {error: {dn: -0.18, up: 0.18}}, 31: {error: {dn: -0.18, up: 0.18}}, 32: {error: {dn: -0.16, up: 0.16}}, 33: {error: {dn: -0.13, up: 0.13}}, 34: {error: {dn: -0.17, up: 0.17}}, 35: {error: {dn: -0.12, up: 0.12}}, 36: {error: {dn: -0.09, up: 0.09}}, 37: {error: {dn: -0.1, up: 0.1}}, 38: {error: {dn: -0.13, up: 0.13}}, 39: {error: {dn: -0.11, up: 0.11}}, 40: {error: {dn: -0.05, up: 0.05}}, 41: {error: {dn: -0.05, up: 0.05}}, 42: {error: {dn: -0.1, up: 0.1}}, 43: {error: {dn: -0.03, up: 0.03}}, 44: {error: {dn: -0.04, up: 0.04}}, 45: {error: {dn: -0.03, up: 0.03}}, 46: {error: {dn: -0.01, up: 0.01}}, 47: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2008_I765258/d07-x01-y01 +Title: doi:10.17182/hepdata.50372.v1/t7 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.410000e+00 1.000000e-02 1.000000e-02 3.200000e-01 6.700000e-01 6.700000e-01 +1.430000e+00 1.000000e-02 1.000000e-02 6.800000e-01 4.000000e-01 4.000000e-01 +1.450000e+00 1.000000e-02 1.000000e-02 1.400000e+00 4.300000e-01 4.300000e-01 +1.470000e+00 1.000000e-02 1.000000e-02 1.270000e+00 3.900000e-01 3.900000e-01 +1.490000e+00 1.000000e-02 1.000000e-02 2.330000e+00 5.000000e-01 5.000000e-01 +1.510000e+00 1.000000e-02 1.000000e-02 2.960000e+00 5.800000e-01 5.800000e-01 +1.530000e+00 1.000000e-02 1.000000e-02 2.830000e+00 5.200000e-01 5.200000e-01 +1.550000e+00 1.000000e-02 1.000000e-02 3.080000e+00 5.500000e-01 5.500000e-01 +1.570000e+00 1.000000e-02 1.000000e-02 2.050000e+00 4.200000e-01 4.200000e-01 +1.590000e+00 1.000000e-02 1.000000e-02 1.670000e+00 3.300000e-01 3.300000e-01 +1.610000e+00 1.000000e-02 1.000000e-02 3.460000e+00 6.800000e-01 6.800000e-01 +1.630000e+00 1.000000e-02 1.000000e-02 1.520000e+00 3.800000e-01 3.800000e-01 +1.650000e+00 1.000000e-02 1.000000e-02 1.830000e+00 3.700000e-01 3.700000e-01 +1.670000e+00 1.000000e-02 1.000000e-02 2.820000e+00 5.000000e-01 5.000000e-01 +1.690000e+00 1.000000e-02 1.000000e-02 2.100000e+00 3.600000e-01 3.600000e-01 +1.710000e+00 1.000000e-02 1.000000e-02 1.280000e+00 3.000000e-01 3.000000e-01 +1.730000e+00 1.000000e-02 1.000000e-02 1.530000e+00 3.500000e-01 3.500000e-01 +1.750000e+00 1.000000e-02 1.000000e-02 1.600000e+00 3.200000e-01 3.200000e-01 +1.770000e+00 1.000000e-02 1.000000e-02 1.440000e+00 3.200000e-01 3.200000e-01 +1.790000e+00 1.000000e-02 1.000000e-02 1.340000e+00 3.200000e-01 3.200000e-01 +1.810000e+00 1.000000e-02 1.000000e-02 5.800000e-01 1.800000e-01 1.800000e-01 +1.830000e+00 1.000000e-02 1.000000e-02 1.440000e+00 3.100000e-01 3.100000e-01 +1.850000e+00 1.000000e-02 1.000000e-02 1.020000e+00 2.400000e-01 2.400000e-01 +1.870000e+00 1.000000e-02 1.000000e-02 9.600000e-01 2.900000e-01 2.900000e-01 +1.890000e+00 1.000000e-02 1.000000e-02 5.900000e-01 2.600000e-01 2.600000e-01 +1.910000e+00 1.000000e-02 1.000000e-02 2.600000e-01 1.400000e-01 1.400000e-01 +1.930000e+00 1.000000e-02 1.000000e-02 5.100000e-01 1.700000e-01 1.700000e-01 +1.940000e+00 2.000000e-02 2.000000e-02 4.000000e-01 1.200000e-01 1.200000e-01 +1.980000e+00 2.000000e-02 2.000000e-02 7.500000e-01 1.600000e-01 1.600000e-01 +2.020000e+00 2.000000e-02 2.000000e-02 6.000000e-01 2.000000e-01 2.000000e-01 +2.060000e+00 2.000000e-02 2.000000e-02 9.300000e-01 1.800000e-01 1.800000e-01 +2.100000e+00 2.000000e-02 2.000000e-02 7.800000e-01 1.800000e-01 1.800000e-01 +2.140000e+00 2.000000e-02 2.000000e-02 5.500000e-01 1.600000e-01 1.600000e-01 +2.180000e+00 2.000000e-02 2.000000e-02 4.700000e-01 1.300000e-01 1.300000e-01 +2.220000e+00 2.000000e-02 2.000000e-02 4.500000e-01 1.700000e-01 1.700000e-01 +2.260000e+00 2.000000e-02 2.000000e-02 4.500000e-01 1.200000e-01 1.200000e-01 +2.300000e+00 2.000000e-02 2.000000e-02 2.500000e-01 9.000000e-02 9.000000e-02 +2.340000e+00 2.000000e-02 2.000000e-02 4.100000e-01 1.000000e-01 1.000000e-01 +2.380000e+00 2.000000e-02 2.000000e-02 3.800000e-01 1.300000e-01 1.300000e-01 +2.420000e+00 2.000000e-02 2.000000e-02 2.100000e-01 1.100000e-01 1.100000e-01 +2.460000e+00 2.000000e-02 2.000000e-02 1.300000e-01 5.000000e-02 5.000000e-02 +2.500000e+00 2.000000e-02 2.000000e-02 1.000000e-01 5.000000e-02 5.000000e-02 +2.560000e+00 4.000000e-02 4.000000e-02 2.700000e-01 1.000000e-01 1.000000e-01 +2.640000e+00 4.000000e-02 4.000000e-02 5.000000e-02 3.000000e-02 3.000000e-02 +2.720000e+00 4.000000e-02 4.000000e-02 1.100000e-01 4.000000e-02 4.000000e-02 +2.800000e+00 4.000000e-02 4.000000e-02 1.100000e-01 3.000000e-02 3.000000e-02 +2.880000e+00 4.000000e-02 4.000000e-02 4.000000e-02 1.000000e-02 1.000000e-02 +3.000000e+00 8.000000e-02 8.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2008_I765258/d08-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.036, up: 0.036}}, 1: {error: {dn: -0.033, up: 0.033}}, 2: {error: {dn: -0.051, up: 0.051}}, 3: {error: {dn: -0.088, up: 0.088}}, 4: {error: {dn: -0.089, up: 0.089}}, 5: {error: {dn: -0.018, up: 0.018}}, 6: {error: {dn: -0.1, up: 0.1}}, 7: {error: {dn: -0.06, up: 0.06}}, 8: {error: {dn: -0.037, up: 0.037}}, 9: {error: {dn: -0.023, up: 0.023}}, 10: {error: {dn: -0.028, up: 0.028}}, 11: {error: {dn: -0.055, up: 0.055}}, 12: {error: {dn: -0.007, up: 0.007}}, 13: {error: {dn: -0.066, up: 0.066}}, 14: {error: {dn: -0.004, up: 0.004}}, 15: {error: {dn: -0.031, up: 0.031}}, 16: {error: {dn: -0.012, up: 0.012}}, 17: {error: {dn: -0.003, up: 0.003}}, 18: {error: {dn: -0.009, up: 0.009}}, 19: {error: {dn: -0.012, up: 0.012}}, 20: {error: {dn: -0.019, up: 0.019}}, 21: {error: {dn: -0.025, up: 0.025}}} + +IsRef: 1 +Path: /REF/BABAR_2008_I765258/d08-x01-y01 +Title: doi:10.17182/hepdata.50372.v1/t8 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.940000e+00 2.000000e-02 2.000000e-02 6.900000e-02 3.600000e-02 3.600000e-02 +1.980000e+00 2.000000e-02 2.000000e-02 4.800000e-02 3.300000e-02 3.300000e-02 +2.020000e+00 2.000000e-02 2.000000e-02 8.300000e-02 5.100000e-02 5.100000e-02 +2.060000e+00 2.000000e-02 2.000000e-02 2.610000e-01 8.800000e-02 8.800000e-02 +2.100000e+00 2.000000e-02 2.000000e-02 1.720000e-01 8.900000e-02 8.900000e-02 +2.140000e+00 2.000000e-02 2.000000e-02 1.800000e-02 1.800000e-02 1.800000e-02 +2.180000e+00 2.000000e-02 2.000000e-02 2.520000e-01 1.000000e-01 1.000000e-01 +2.220000e+00 2.000000e-02 2.000000e-02 1.150000e-01 6.000000e-02 6.000000e-02 +2.260000e+00 2.000000e-02 2.000000e-02 5.900000e-02 3.700000e-02 3.700000e-02 +2.300000e+00 2.000000e-02 2.000000e-02 3.400000e-02 2.300000e-02 2.300000e-02 +2.340000e+00 2.000000e-02 2.000000e-02 4.500000e-02 2.800000e-02 2.800000e-02 +2.380000e+00 2.000000e-02 2.000000e-02 6.300000e-02 5.500000e-02 5.500000e-02 +2.420000e+00 2.000000e-02 2.000000e-02 1.400000e-02 7.000000e-03 7.000000e-03 +2.460000e+00 2.000000e-02 2.000000e-02 1.280000e-01 6.600000e-02 6.600000e-02 +2.500000e+00 2.000000e-02 2.000000e-02 8.000000e-03 4.000000e-03 4.000000e-03 +2.560000e+00 4.000000e-02 4.000000e-02 3.000000e-02 3.100000e-02 3.100000e-02 +2.640000e+00 4.000000e-02 4.000000e-02 1.200000e-02 1.200000e-02 1.200000e-02 +2.720000e+00 4.000000e-02 4.000000e-02 3.000000e-03 3.000000e-03 3.000000e-03 +2.800000e+00 4.000000e-02 4.000000e-02 9.000000e-03 9.000000e-03 9.000000e-03 +2.880000e+00 4.000000e-02 4.000000e-02 2.200000e-02 1.200000e-02 1.200000e-02 +2.960000e+00 4.000000e-02 4.000000e-02 6.500000e-02 1.900000e-02 1.900000e-02 +3.040000e+00 4.000000e-02 4.000000e-02 4.400000e-02 2.500000e-02 2.500000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2008_I765258/d09-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.07, up: 0.07}}, 1: {error: {dn: -0.09, up: 0.09}}, 2: {error: {dn: -0.05, up: 0.05}}, 3: {error: {dn: -0.09, up: 0.09}}, 4: {error: {dn: -0.1, up: 0.1}}, 5: {error: {dn: -0.1, up: 0.1}}, 6: {error: {dn: -0.07, up: 0.07}}, 7: {error: {dn: -0.1, up: 0.1}}, 8: {error: {dn: -0.11, up: 0.11}}, 9: {error: {dn: -0.07, up: 0.07}}, 10: {error: {dn: -0.05, up: 0.05}}, 11: {error: {dn: -0.07, up: 0.07}}, 12: {error: {dn: -0.03, up: 0.03}}, 13: {error: {dn: -0.01, up: 0.01}}, 14: {error: {dn: -0.03, up: 0.03}}, 15: {error: {dn: -0.03, up: 0.03}}, 16: {error: {dn: -0.03, up: 0.03}}, 17: {error: {dn: -0.02, up: 0.02}}, 18: {error: {dn: -0.02, up: 0.02}}, 19: {error: {dn: -0.02, up: 0.02}}, 20: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2008_I765258/d09-x01-y01 +Title: doi:10.17182/hepdata.50372.v1/t9 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.980000e+00 2.000000e-02 2.000000e-02 1.000000e-01 7.000000e-02 7.000000e-02 +2.020000e+00 2.000000e-02 2.000000e-02 2.300000e-01 9.000000e-02 9.000000e-02 +2.060000e+00 2.000000e-02 2.000000e-02 8.000000e-02 5.000000e-02 5.000000e-02 +2.100000e+00 2.000000e-02 2.000000e-02 1.900000e-01 9.000000e-02 9.000000e-02 +2.140000e+00 2.000000e-02 2.000000e-02 3.300000e-01 1.000000e-01 1.000000e-01 +2.180000e+00 2.000000e-02 2.000000e-02 2.700000e-01 1.000000e-01 1.000000e-01 +2.220000e+00 2.000000e-02 2.000000e-02 2.100000e-01 7.000000e-02 7.000000e-02 +2.260000e+00 2.000000e-02 2.000000e-02 4.200000e-01 1.000000e-01 1.000000e-01 +2.300000e+00 2.000000e-02 2.000000e-02 3.200000e-01 1.100000e-01 1.100000e-01 +2.340000e+00 2.000000e-02 2.000000e-02 1.500000e-01 7.000000e-02 7.000000e-02 +2.380000e+00 2.000000e-02 2.000000e-02 9.000000e-02 5.000000e-02 5.000000e-02 +2.420000e+00 2.000000e-02 2.000000e-02 1.800000e-01 7.000000e-02 7.000000e-02 +2.460000e+00 2.000000e-02 2.000000e-02 6.000000e-02 3.000000e-02 3.000000e-02 +2.500000e+00 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +2.560000e+00 4.000000e-02 4.000000e-02 6.000000e-02 3.000000e-02 3.000000e-02 +2.640000e+00 4.000000e-02 4.000000e-02 1.300000e-01 3.000000e-02 3.000000e-02 +2.720000e+00 4.000000e-02 4.000000e-02 8.000000e-02 3.000000e-02 3.000000e-02 +2.800000e+00 4.000000e-02 4.000000e-02 3.000000e-02 2.000000e-02 2.000000e-02 +2.880000e+00 4.000000e-02 4.000000e-02 4.000000e-02 2.000000e-02 2.000000e-02 +2.960000e+00 4.000000e-02 4.000000e-02 5.000000e-02 2.000000e-02 2.000000e-02 +3.040000e+00 4.000000e-02 4.000000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2008_I776519.cc b/analyses/pluginBABAR/BABAR_2008_I776519.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2008_I776519.cc @@ -0,0 +1,139 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2008_I776519 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2008_I776519); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nD0 = bookCounter("/TMP/nD0"); + _nDp = bookCounter("/TMP/nDp"); + + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + bool matched=false; + for(unsigned int iy=0;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) break; + } + if(matched) { + if(abs(p1.pdgId())==411) + _nDp->fill(event.weight()); + else if(abs(p1.pdgId())==421) + _nD0->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + for(unsigned int ix=1;ix<3;++ix) { + double sigma,error; + if(ix==1) { + sigma = _nD0->val(); + error = _nD0->err(); + } + else { + sigma = _nDp->val(); + error = _nDp->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nD0,_nDp; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2008_I776519); + + +} diff --git a/analyses/pluginBABAR/BABAR_2008_I776519.info b/analyses/pluginBABAR/BABAR_2008_I776519.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2008_I776519.info @@ -0,0 +1,30 @@ +Name: BABAR_2008_I776519 +Year: 2008 +Summary: Cross section for $e^+e^-\to D^+D^-$ and $D^0\bar{D}^0$ below 5 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 776519 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - arXiv:0710.1371 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to D^+D^-$ and $D^0\bar{D}^0$ below 5 GeV' +Keywords: [] +BibKey: Aubert:2008pa +BibTeX: '@article{Aubert:2008pa, + author = "Aubert, Bernard and others", + title = "{Study of the Exclusive Initial-State-Radiation + Production of the D anti-D System}", + collaboration = "BaBar", + year = "2008", + eprint = "0710.1371", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-12818, BABAR-PUB-07-060", + SLACcitation = "%%CITATION = ARXIV:0710.1371;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2008_I776519.plot b/analyses/pluginBABAR/BABAR_2008_I776519.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2008_I776519.plot @@ -0,0 +1,12 @@ +BEGIN PLOT /BABAR_2008_I776519/d01-x01-y01 +Title=$\sigma(e^+e^-\to D^0\bar{D}^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^0\bar{D}^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2008_I776519/d01-x01-y02 +Title=$\sigma(e^+e^-\to D^+D^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^+D^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2008_I776519.yoda b/analyses/pluginBABAR/BABAR_2008_I776519.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2008_I776519.yoda @@ -0,0 +1,180 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2008_I776519/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {1: {error: {dn: -0.12, up: 0.12}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00981, up: 0.00981}}, 2: {error: {dn: -0.32, up: 0.32}, 'sys,Additional overall systematic uncertainty.': {dn: -0.18094000000000002, up: 0.18094000000000002}}, 3: {error: {dn: -0.5, up: 0.5}, 'sys,Additional overall systematic uncertainty.': {dn: -0.45671000000000006, up: 0.45671000000000006}}, 4: {error: {dn: -0.34, up: 0.34}, 'sys,Additional overall systematic uncertainty.': {dn: -0.21364, up: 0.21364}}, 5: {error: {dn: -0.14, up: 0.14}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0218, up: 0.0218}}, 6: {error: {dn: -0.18, up: 0.18}, 'sys,Additional overall systematic uncertainty.': {dn: -0.050140000000000004, up: 0.050140000000000004}}, 7: {error: {dn: -0.13, up: 0.13}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01635, up: 0.01635}}, 8: {error: {dn: -0.14, up: 0.14}, 'sys,Additional overall systematic uncertainty.': {dn: -0.02725, up: 0.02725}}, 9: {error: {dn: -0.23, up: 0.23}, 'sys,Additional overall systematic uncertainty.': {dn: -0.10573, up: 0.10573}}, 10: {error: {dn: -0.17, up: 0.17}, 'sys,Additional overall systematic uncertainty.': {dn: -0.05232, up: 0.05232}}, 11: {error: {dn: -0.17, up: 0.17}, 'sys,Additional overall systematic uncertainty.': {dn: -0.05668, up: 0.05668}}, 12: {error: {dn: -0.2, up: 0.2}, 'sys,Additional overall systematic uncertainty.': {dn: -0.08502000000000001, up: 0.08502000000000001}}, 13: {error: {dn: -0.15, up: 0.15}, 'sys,Additional overall systematic uncertainty.': {dn: -0.040330000000000005, up: 0.040330000000000005}}, 14: {error: {dn: -0.11, up: 0.11}, 'sys,Additional overall systematic uncertainty.': {dn: -0.015260000000000003, up: 0.015260000000000003}}, 15: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00109, up: 0.00109}}, 16: {error: {dn: -0.16, up: 0.16}, 'sys,Additional overall systematic uncertainty.': {dn: -0.05668, up: 0.05668}}, 17: {error: {dn: -0.15, up: 0.15}, 'sys,Additional overall systematic uncertainty.': {dn: -0.04687, up: 0.04687}}, 18: {error: {dn: -0.18, up: 0.18}, 'sys,Additional overall systematic uncertainty.': {dn: -0.08066000000000001, up: 0.08066000000000001}}, 19: {error: {dn: -0.13, up: 0.13}, 'sys,Additional overall systematic uncertainty.': {dn: -0.03597, up: 0.03597}}, 20: {error: {dn: -0.13, up: 0.13}, 'sys,Additional overall systematic uncertainty.': {dn: -0.03597, up: 0.03597}}, 21: {error: {dn: -0.08, up: 0.08}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0109, up: 0.0109}}, 22: {error: {dn: -0.11, up: 0.11}, 'sys,Additional overall systematic uncertainty.': {dn: -0.02725, up: 0.02725}}, 23: {error: {dn: -0.09, up: 0.09}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01417, up: 0.01417}}, 24: {error: {dn: -0.12, up: 0.12}, 'sys,Additional overall systematic uncertainty.': {dn: -0.038149999999999996, up: 0.038149999999999996}}, 25: {error: {dn: -0.1, up: 0.1}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0218, up: 0.0218}}, 26: {error: {dn: -0.08, up: 0.08}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0109, up: 0.0109}}, 27: {error: {dn: -0.09, up: 0.09}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01744, up: 0.01744}}, 28: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00654, up: 0.00654}}, 29: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00654, up: 0.00654}}, 30: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00654, up: 0.00654}}, 31: {error: {dn: -0.09, up: 0.09}, 'sys,Additional overall systematic uncertainty.': {dn: -0.02071, up: 0.02071}}, 32: {error: {dn: -0.09, up: 0.09}, 'sys,Additional overall systematic uncertainty.': {dn: -0.02071, up: 0.02071}}, 33: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00109, up: 0.00109}}, 34: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01308, up: 0.01308}}, 35: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00436, up: 0.00436}}, 36: {error: {dn: -0.09, up: 0.09}, 'sys,Additional overall systematic uncertainty.': {dn: -0.025070000000000002, up: 0.025070000000000002}}, 37: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01635, up: 0.01635}}, 38: {error: {dn: -0.09, up: 0.09}, 'sys,Additional overall systematic uncertainty.': {dn: -0.025070000000000002, up: 0.025070000000000002}}, 39: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.015260000000000003, up: 0.015260000000000003}}, 40: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00981, up: 0.00981}}, 41: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00981, up: 0.00981}}, 42: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01744, up: 0.01744}}, 44: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00981, up: 0.00981}}, 45: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01417, up: 0.01417}}, 46: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00654, up: 0.00654}}, 47: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00981, up: 0.00981}}, 48: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00872, up: 0.00872}}, 49: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01199, up: 0.01199}}, 50: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00872, up: 0.00872}}, 51: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00872, up: 0.00872}}, 52: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0109, up: 0.0109}}, 54: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00654, up: 0.00654}}, 55: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00654, up: 0.00654}}, 56: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00872, up: 0.00872}}, 57: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00654, up: 0.00654}}, 58: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}, 59: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}, 60: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00436, up: 0.00436}}, 61: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00654, up: 0.00654}}, 62: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.015260000000000003, up: 0.015260000000000003}}, 63: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01308, up: 0.01308}}, 64: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}, 65: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00981, up: 0.00981}}, 68: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}, 69: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}, 71: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00545, up: 0.00545}}, 73: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00545, up: 0.00545}}, 74: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00327, up: 0.00327}}, 75: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00327, up: 0.00327}}, 76: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00327, up: 0.00327}}, 78: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00327, up: 0.00327}}, 79: {error: {dn: -0.01, up: 0.01}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00109, up: 0.00109}}, 80: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00327, up: 0.00327}}, 81: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00327, up: 0.00327}}, 82: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}, 83: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}, 84: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00436, up: 0.00436}}, 85: {error: {dn: -0.01, up: 0.01}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00109, up: 0.00109}}, 86: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}, 88: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00436, up: 0.00436}}, 89: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00436, up: 0.00436}}, 90: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00436, up: 0.00436}}, 91: {error: {dn: -0.01, up: 0.01}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00109, up: 0.00109}}, 92: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00545, up: 0.00545}}, 94: {error: {dn: -0.01, up: 0.01}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}, 95: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00327, up: 0.00327}}, 97: {error: {dn: -0.02, up: 0.02}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00327, up: 0.00327}}, 98: {error: {dn: -0.01, up: 0.01}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}, 99: {error: {dn: -0.01, up: 0.01}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00218, up: 0.00218}}} + +IsRef: 1 +Path: /REF/BABAR_2008_I776519/d01-x01-y01 +Title: doi:10.17182/hepdata.18803.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.730000e+00 1.000000e-02 1.000000e-02 9.000000e-02 1.204003e-01 1.204003e-01 +3.750000e+00 1.000000e-02 1.000000e-02 1.660000e+00 3.676130e-01 3.676130e-01 +3.770000e+00 1.000000e-02 1.000000e-02 4.190000e+00 6.771883e-01 6.771883e-01 +3.790000e+00 1.000000e-02 1.000000e-02 1.960000e+00 4.015496e-01 4.015496e-01 +3.810000e+00 1.000000e-02 1.000000e-02 2.000000e-01 1.416871e-01 1.416871e-01 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1.000000e-02 1.900000e-01 9.235207e-02 9.235207e-02 +4.350000e+00 1.000000e-02 1.000000e-02 1.900000e-01 9.235207e-02 9.235207e-02 +4.370000e+00 1.000000e-02 1.000000e-02 1.000000e-02 4.001485e-02 4.001485e-02 +4.390000e+00 1.000000e-02 1.000000e-02 1.200000e-01 7.121156e-02 7.121156e-02 +4.410000e+00 1.000000e-02 1.000000e-02 4.000000e-02 5.018974e-02 5.018974e-02 +4.430000e+00 1.000000e-02 1.000000e-02 2.300000e-01 9.342647e-02 9.342647e-02 +4.450000e+00 1.000000e-02 1.000000e-02 1.500000e-01 7.188409e-02 7.188409e-02 +4.470000e+00 1.000000e-02 1.000000e-02 2.300000e-01 9.342647e-02 9.342647e-02 +4.490000e+00 1.000000e-02 1.000000e-02 1.400000e-01 7.164403e-02 7.164403e-02 +4.510000e+00 1.000000e-02 1.000000e-02 9.000000e-02 6.079668e-02 6.079668e-02 +4.530000e+00 1.000000e-02 1.000000e-02 9.000000e-02 6.079668e-02 6.079668e-02 +4.550000e+00 1.000000e-02 1.000000e-02 1.600000e-01 7.213982e-02 7.213982e-02 +4.590000e+00 1.000000e-02 1.000000e-02 9.000000e-02 5.095327e-02 5.095327e-02 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0.23003999999999997}}, 4: {error: {dn: -0.3, up: 0.3}, 'sys,Additional overall systematic uncertainty.': {dn: -0.06075, up: 0.06075}}, 5: {error: {dn: -0.11, up: 0.11}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00648, up: 0.00648}}, 6: {error: {dn: -0.15, up: 0.15}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01458, up: 0.01458}}, 7: {error: {dn: -0.28, up: 0.28}, 'sys,Additional overall systematic uncertainty.': {dn: -0.05750999999999999, up: 0.05750999999999999}}, 8: {error: {dn: -0.25, up: 0.25}, 'sys,Additional overall systematic uncertainty.': {dn: -0.04779, up: 0.04779}}, 9: {error: {dn: -0.14, up: 0.14}, 'sys,Additional overall systematic uncertainty.': {dn: -0.013770000000000001, up: 0.013770000000000001}}, 10: {error: {dn: -0.24, up: 0.24}, 'sys,Additional overall systematic uncertainty.': {dn: -0.046169999999999996, up: 0.046169999999999996}}, 11: {error: {dn: -0.14, up: 0.14}, 'sys,Additional overall systematic uncertainty.': {dn: -0.013770000000000001, up: 0.013770000000000001}}, 12: {error: {dn: -0.17, up: 0.17}, 'sys,Additional overall systematic uncertainty.': {dn: -0.02106, up: 0.02106}}, 13: {error: {dn: -0.16, up: 0.16}, 'sys,Additional overall systematic uncertainty.': {dn: -0.02106, up: 0.02106}}, 15: {error: {dn: -0.09, up: 0.09}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0056700000000000006, up: 0.0056700000000000006}}, 16: {error: {dn: -0.13, up: 0.13}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01296, up: 0.01296}}, 17: {error: {dn: -0.15, up: 0.15}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01944, up: 0.01944}}, 18: {error: {dn: -0.17, up: 0.17}, 'sys,Additional overall systematic uncertainty.': {dn: -0.02592, up: 0.02592}}, 19: {error: {dn: -0.19, up: 0.19}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0324, up: 0.0324}}, 20: {error: {dn: -0.16, up: 0.16}, 'sys,Additional overall systematic uncertainty.': {dn: -0.025109999999999997, up: 0.025109999999999997}}, 21: {error: {dn: -0.21, up: 0.21}, 'sys,Additional overall systematic uncertainty.': {dn: -0.04455, up: 0.04455}}, 22: {error: {dn: -0.08, up: 0.08}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00486, up: 0.00486}}, 23: {error: {dn: -0.13, up: 0.13}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01782, up: 0.01782}}, 24: {error: {dn: -0.15, up: 0.15}, 'sys,Additional overall systematic uncertainty.': {dn: -0.023489999999999997, up: 0.023489999999999997}}, 25: {error: {dn: -0.08, up: 0.08}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00486, up: 0.00486}}, 26: {error: {dn: -0.13, up: 0.13}, 'sys,Additional overall systematic uncertainty.': {dn: -0.017009999999999997, up: 0.017009999999999997}}, 27: {error: {dn: -0.13, up: 0.13}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0162, up: 0.0162}}, 29: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00486, up: 0.00486}}, 32: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00486, up: 0.00486}}, 34: {error: {dn: -0.11, up: 0.11}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01458, up: 0.01458}}, 35: {error: {dn: -0.09, up: 0.09}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00972, up: 0.00972}}, 36: {error: {dn: -0.12, up: 0.12}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01944, up: 0.01944}}, 37: {error: {dn: -0.12, up: 0.12}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01944, up: 0.01944}}, 38: {error: {dn: -0.1, up: 0.1}, 'sys,Additional overall systematic uncertainty.': {dn: -0.013770000000000001, up: 0.013770000000000001}}, 39: {error: {dn: -0.12, up: 0.12}, 'sys,Additional overall systematic uncertainty.': {dn: -0.018629999999999997, up: 0.018629999999999997}}, 41: {error: {dn: -0.1, up: 0.1}, 'sys,Additional overall systematic uncertainty.': {dn: -0.01296, up: 0.01296}}, 42: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00405, up: 0.00405}}, 43: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00405, up: 0.00405}}, 44: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00405, up: 0.00405}}, 45: {error: {dn: -0.08, up: 0.08}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0081, up: 0.0081}}, 46: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0081, up: 0.0081}}, 49: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0081, up: 0.0081}}, 52: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00324, up: 0.00324}}, 54: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00324, up: 0.00324}}, 55: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00324, up: 0.00324}}, 56: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00729, up: 0.00729}}, 57: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00324, up: 0.00324}}, 58: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00324, up: 0.00324}}, 59: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00648, up: 0.00648}}, 60: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00648, up: 0.00648}}, 61: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00648, up: 0.00648}}, 64: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00324, up: 0.00324}}, 66: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00324, up: 0.00324}}, 67: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0056700000000000006, up: 0.0056700000000000006}}, 68: {error: {dn: -0.07, up: 0.07}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00891, up: 0.00891}}, 69: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0056700000000000006, up: 0.0056700000000000006}}, 70: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00243, up: 0.00243}}, 71: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00243, up: 0.00243}}, 73: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0056700000000000006, up: 0.0056700000000000006}}, 74: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0056700000000000006, up: 0.0056700000000000006}}, 75: {error: {dn: -0.06, up: 0.06}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0081, up: 0.0081}}, 77: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.0056700000000000006, up: 0.0056700000000000006}}, 80: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00243, up: 0.00243}}, 82: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00243, up: 0.00243}}, 83: {error: {dn: -0.05, up: 0.05}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00729, up: 0.00729}}, 84: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00243, up: 0.00243}}, 85: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00243, up: 0.00243}}, 86: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00243, up: 0.00243}}, 89: {error: {dn: -0.03, up: 0.03}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00243, up: 0.00243}}, 92: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00405, up: 0.00405}}, 93: {error: {dn: -0.04, up: 0.04}, 'sys,Additional overall systematic uncertainty.': {dn: -0.00405, up: 0.00405}}} + +IsRef: 1 +Path: /REF/BABAR_2008_I776519/d01-x01-y02 +Title: doi:10.17182/hepdata.18803.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.750000e+00 1.000000e-02 1.000000e-02 7.900000e-01 3.165355e-01 3.165355e-01 +3.770000e+00 1.000000e-02 1.000000e-02 2.840000e+00 6.146693e-01 6.146693e-01 +3.790000e+00 1.000000e-02 1.000000e-02 7.500000e-01 3.060891e-01 3.060891e-01 +3.810000e+00 1.000000e-02 1.000000e-02 8.000000e-02 1.101907e-01 1.101907e-01 +3.830000e+00 1.000000e-02 1.000000e-02 1.800000e-01 1.507069e-01 1.507069e-01 +3.850000e+00 1.000000e-02 1.000000e-02 7.100000e-01 2.858451e-01 2.858451e-01 +3.870000e+00 1.000000e-02 1.000000e-02 5.900000e-01 2.545268e-01 2.545268e-01 +3.890000e+00 1.000000e-02 1.000000e-02 1.700000e-01 1.406756e-01 1.406756e-01 +3.910000e+00 1.000000e-02 1.000000e-02 5.700000e-01 2.444006e-01 2.444006e-01 +3.930000e+00 1.000000e-02 1.000000e-02 1.700000e-01 1.406756e-01 1.406756e-01 +3.950000e+00 1.000000e-02 1.000000e-02 2.600000e-01 1.712995e-01 1.712995e-01 +3.970000e+00 1.000000e-02 1.000000e-02 2.600000e-01 1.613801e-01 1.613801e-01 +4.010000e+00 1.000000e-02 1.000000e-02 7.000000e-02 9.017843e-02 9.017843e-02 +4.030000e+00 1.000000e-02 1.000000e-02 1.600000e-01 1.306444e-01 1.306444e-01 +4.050000e+00 1.000000e-02 1.000000e-02 2.400000e-01 1.512545e-01 1.512545e-01 +4.070000e+00 1.000000e-02 1.000000e-02 3.200000e-01 1.719647e-01 1.719647e-01 +4.090000e+00 1.000000e-02 1.000000e-02 4.000000e-01 1.927427e-01 1.927427e-01 +4.110000e+00 1.000000e-02 1.000000e-02 3.100000e-01 1.619584e-01 1.619584e-01 +4.130000e+00 1.000000e-02 1.000000e-02 5.500000e-01 2.146735e-01 2.146735e-01 +4.150000e+00 1.000000e-02 1.000000e-02 6.000000e-02 8.014749e-02 8.014749e-02 +4.170000e+00 1.000000e-02 1.000000e-02 2.200000e-01 1.312157e-01 1.312157e-01 +4.190000e+00 1.000000e-02 1.000000e-02 2.900000e-01 1.518281e-01 1.518281e-01 +4.210000e+00 1.000000e-02 1.000000e-02 6.000000e-02 8.014749e-02 8.014749e-02 +4.230000e+00 1.000000e-02 1.000000e-02 2.100000e-01 1.311081e-01 1.311081e-01 +4.250000e+00 1.000000e-02 1.000000e-02 2.000000e-01 1.310055e-01 1.310055e-01 +4.290000e+00 1.000000e-02 1.000000e-02 6.000000e-02 7.016851e-02 7.016851e-02 +4.350000e+00 1.000000e-02 1.000000e-02 6.000000e-02 7.016851e-02 7.016851e-02 +4.390000e+00 1.000000e-02 1.000000e-02 1.800000e-01 1.109620e-01 1.109620e-01 +4.410000e+00 1.000000e-02 1.000000e-02 1.200000e-01 9.052336e-02 9.052336e-02 +4.430000e+00 1.000000e-02 1.000000e-02 2.400000e-01 1.215644e-01 1.215644e-01 +4.450000e+00 1.000000e-02 1.000000e-02 2.400000e-01 1.215644e-01 1.215644e-01 +4.470000e+00 1.000000e-02 1.000000e-02 1.700000e-01 1.009436e-01 1.009436e-01 +4.490000e+00 1.000000e-02 1.000000e-02 2.300000e-01 1.214375e-01 1.214375e-01 +4.530000e+00 1.000000e-02 1.000000e-02 1.600000e-01 1.008363e-01 1.008363e-01 +4.550000e+00 1.000000e-02 1.000000e-02 5.000000e-02 6.013653e-02 6.013653e-02 +4.570000e+00 1.000000e-02 1.000000e-02 5.000000e-02 6.013653e-02 6.013653e-02 +4.590000e+00 1.000000e-02 1.000000e-02 5.000000e-02 5.016376e-02 5.016376e-02 +4.610000e+00 1.000000e-02 1.000000e-02 1.000000e-01 8.040902e-02 8.040902e-02 +4.630000e+00 1.000000e-02 1.000000e-02 1.000000e-01 7.046708e-02 7.046708e-02 +4.690000e+00 1.000000e-02 1.000000e-02 1.000000e-01 7.046708e-02 7.046708e-02 +4.750000e+00 1.000000e-02 1.000000e-02 4.000000e-02 5.010487e-02 5.010487e-02 +4.790000e+00 1.000000e-02 1.000000e-02 4.000000e-02 5.010487e-02 5.010487e-02 +4.810000e+00 1.000000e-02 1.000000e-02 4.000000e-02 5.010487e-02 5.010487e-02 +4.830000e+00 1.000000e-02 1.000000e-02 9.000000e-02 6.044125e-02 6.044125e-02 +4.850000e+00 1.000000e-02 1.000000e-02 4.000000e-02 4.013101e-02 4.013101e-02 +4.870000e+00 1.000000e-02 1.000000e-02 4.000000e-02 4.013101e-02 4.013101e-02 +4.890000e+00 1.000000e-02 1.000000e-02 8.000000e-02 6.034891e-02 6.034891e-02 +4.910000e+00 1.000000e-02 1.000000e-02 8.000000e-02 6.034891e-02 6.034891e-02 +4.930000e+00 1.000000e-02 1.000000e-02 8.000000e-02 6.034891e-02 6.034891e-02 +4.990000e+00 1.000000e-02 1.000000e-02 4.000000e-02 4.013101e-02 4.013101e-02 +5.030000e+00 1.000000e-02 1.000000e-02 4.000000e-02 4.013101e-02 4.013101e-02 +5.050000e+00 1.000000e-02 1.000000e-02 7.000000e-02 5.032046e-02 5.032046e-02 +5.070000e+00 1.000000e-02 1.000000e-02 1.100000e-01 7.056478e-02 7.056478e-02 +5.090000e+00 1.000000e-02 1.000000e-02 7.000000e-02 5.032046e-02 5.032046e-02 +5.110000e+00 1.000000e-02 1.000000e-02 3.000000e-02 4.007374e-02 4.007374e-02 +5.130000e+00 1.000000e-02 1.000000e-02 3.000000e-02 4.007374e-02 4.007374e-02 +5.170000e+00 1.000000e-02 1.000000e-02 7.000000e-02 5.032046e-02 5.032046e-02 +5.190000e+00 1.000000e-02 1.000000e-02 7.000000e-02 5.032046e-02 5.032046e-02 +5.210000e+00 1.000000e-02 1.000000e-02 1.000000e-01 6.054428e-02 6.054428e-02 +5.250000e+00 1.000000e-02 1.000000e-02 7.000000e-02 5.032046e-02 5.032046e-02 +5.310000e+00 1.000000e-02 1.000000e-02 3.000000e-02 3.009825e-02 3.009825e-02 +5.350000e+00 1.000000e-02 1.000000e-02 3.000000e-02 3.009825e-02 3.009825e-02 +5.370000e+00 1.000000e-02 1.000000e-02 9.000000e-02 5.052865e-02 5.052865e-02 +5.390000e+00 1.000000e-02 1.000000e-02 3.000000e-02 3.009825e-02 3.009825e-02 +5.410000e+00 1.000000e-02 1.000000e-02 3.000000e-02 3.009825e-02 3.009825e-02 +5.430000e+00 1.000000e-02 1.000000e-02 3.000000e-02 3.009825e-02 3.009825e-02 +5.490000e+00 1.000000e-02 1.000000e-02 3.000000e-02 3.009825e-02 3.009825e-02 +5.550000e+00 1.000000e-02 1.000000e-02 5.000000e-02 4.020451e-02 4.020451e-02 +5.570000e+00 1.000000e-02 1.000000e-02 5.000000e-02 4.020451e-02 4.020451e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2009_I797507.cc b/analyses/pluginBABAR/BABAR_2009_I797507.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2009_I797507.cc @@ -0,0 +1,111 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2009_I797507 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2009_I797507); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + bool isBottom(false); + const UnstableParticles& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if (PID::isBottomHadron(p.pdgId())) { + isBottom = true; + break; + } + } + + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else if(isBottom) { + _c_hadrons->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2009_I797507); + + +} diff --git a/analyses/pluginBABAR/BABAR_2009_I797507.info b/analyses/pluginBABAR/BABAR_2009_I797507.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2009_I797507.info @@ -0,0 +1,35 @@ +Name: BABAR_2009_I797507 +Year: 2009 +Summary: Measurement of $R_b$ for energies between 10.541 and 11.206 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 797507 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - PRL 102,012001 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R_b$ in $e^+e^-$ collisions by BaBar for energies between 10.541 and 11.206 GeV. + The individual bottom hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Aubert:2008ab +BibTeX: '@article{Aubert:2008ab, + author = "Aubert, Bernard and others", + title = "{Measurement of the $e^{+} e^{-} \to b \bar{b}$ cross + section between $\sqrt{s}$ = 10.54-GeV and 11.20-GeV}", + collaboration = "BaBar", + journal = "Phys. Rev. Lett.", + volume = "102", + year = "2009", + pages = "012001", + doi = "10.1103/PhysRevLett.102.012001", + eprint = "0809.4120", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-13397, BABAR-PUB-08042", + SLACcitation = "%%CITATION = ARXIV:0809.4120;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2009_I797507.plot b/analyses/pluginBABAR/BABAR_2009_I797507.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2009_I797507.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /BABAR_2009_I797507/d01-x01-y01 +Title=$R_b=\sigma(e^+e^-\to b\bar{b})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R_b$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2009_I797507/sigma_hadrons +Title=$\sigma(e^+e^-\to b\bar{b})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to b\bar{b})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2009_I797507/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2009_I797507.yoda b/analyses/pluginBABAR/BABAR_2009_I797507.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2009_I797507.yoda @@ -0,0 +1,147 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2009_I797507/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.0, up: 0.0}, sys_1: {dn: -0.0, up: 0.0}, sys_2: {dn: -0.002, up: 0.002}}, 1: {stat: {dn: -0.019, up: 0.019}, sys_1: {dn: -0.0, up: 0.0}, sys_2: {dn: -0.003, up: 0.003}}, 2: {stat: {dn: -0.018, up: 0.018}, sys_1: {dn: -0.0, up: 0.0}, sys_2: {dn: -0.008, up: 0.008}}, 3: {stat: {dn: -0.021, up: 0.021}, sys_1: {dn: -0.0, up: 0.0}, sys_2: {dn: -0.017, up: 0.017}}, 4: {stat: {dn: -0.032, up: 0.032}, sys_1: {dn: -0.0, up: 0.0}, sys_2: {dn: -0.028, up: 0.028}}, 5: {stat: {dn: -0.034, up: 0.034}, sys_1: {dn: -0.0, up: 0.0}, sys_2: {dn: -0.033, up: 0.033}}, 6: {stat: {dn: -0.037, up: 0.037}, sys_1: {dn: -0.0, up: 0.0}, sys_2: 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/REF/BABAR_2009_I797507/d01-x01-y01 +Title: doi:10.17182/hepdata.18666.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.054080e+01 0.000000e+00 0.000000e+00 9.400000e-02 2.000000e-03 2.000000e-03 +1.055830e+01 0.000000e+00 0.000000e+00 1.280000e-01 1.923538e-02 1.923538e-02 +1.056280e+01 0.000000e+00 0.000000e+00 3.260000e-01 1.969772e-02 1.969772e-02 +1.056730e+01 0.000000e+00 0.000000e+00 7.220000e-01 2.701851e-02 2.701851e-02 +1.057230e+01 0.000000e+00 0.000000e+00 1.180000e+00 4.252058e-02 4.252058e-02 +1.057380e+01 0.000000e+00 0.000000e+00 1.386000e+00 4.738143e-02 4.738143e-02 +1.057880e+01 0.000000e+00 0.000000e+00 1.552000e+00 5.232590e-02 5.232590e-02 +1.059030e+01 0.000000e+00 0.000000e+00 1.017000e+00 3.189044e-02 3.189044e-02 +1.059830e+01 0.000000e+00 0.000000e+00 4.880000e-01 2.163331e-02 2.163331e-02 +1.060180e+01 0.000000e+00 0.000000e+00 3.150000e-01 1.700000e-02 1.700000e-02 +1.060630e+01 0.000000e+00 0.000000e+00 2.470000e-01 1.720465e-02 1.720465e-02 +1.061180e+01 0.000000e+00 0.000000e+00 3.040000e-01 2.507987e-02 2.507987e-02 +1.061280e+01 0.000000e+00 0.000000e+00 2.790000e-01 2.412468e-02 2.412468e-02 +1.061780e+01 0.000000e+00 0.000000e+00 2.870000e-01 1.757840e-02 1.757840e-02 +1.062730e+01 0.000000e+00 0.000000e+00 3.340000e-01 1.711724e-02 1.711724e-02 +1.063080e+01 0.000000e+00 0.000000e+00 3.200000e-01 1.889444e-02 1.889444e-02 +1.063530e+01 0.000000e+00 0.000000e+00 3.250000e-01 1.889444e-02 1.889444e-02 +1.064130e+01 0.000000e+00 0.000000e+00 2.870000e-01 1.749286e-02 1.749286e-02 +1.064580e+01 0.000000e+00 0.000000e+00 2.130000e-01 1.584298e-02 1.584298e-02 +1.065180e+01 0.000000e+00 0.000000e+00 2.670000e-01 1.772005e-02 1.772005e-02 +1.065530e+01 0.000000e+00 0.000000e+00 2.960000e-01 1.772005e-02 1.772005e-02 +1.066130e+01 0.000000e+00 0.000000e+00 2.540000e-01 1.920937e-02 1.920937e-02 +1.066590e+01 0.000000e+00 0.000000e+00 3.230000e-01 1.726268e-02 1.726268e-02 +1.067240e+01 0.000000e+00 0.000000e+00 3.200000e-01 1.813836e-02 1.813836e-02 +1.067740e+01 0.000000e+00 0.000000e+00 3.340000e-01 1.902630e-02 1.902630e-02 +1.068190e+01 0.000000e+00 0.000000e+00 3.480000e-01 1.902630e-02 1.902630e-02 +1.068690e+01 0.000000e+00 0.000000e+00 3.120000e-01 1.813836e-02 1.813836e-02 +1.068840e+01 0.000000e+00 0.000000e+00 3.440000e-01 1.902630e-02 1.902630e-02 +1.069640e+01 0.000000e+00 0.000000e+00 3.370000e-01 1.813836e-02 1.813836e-02 +1.070090e+01 0.000000e+00 0.000000e+00 3.420000e-01 1.813836e-02 1.813836e-02 +1.070440e+01 0.000000e+00 0.000000e+00 3.450000e-01 1.902630e-02 1.902630e-02 +1.070990e+01 0.000000e+00 0.000000e+00 3.230000e-01 1.800000e-02 1.800000e-02 +1.071640e+01 0.000000e+00 0.000000e+00 3.370000e-01 1.889444e-02 1.889444e-02 +1.071890e+01 0.000000e+00 0.000000e+00 3.180000e-01 1.800000e-02 1.800000e-02 +1.072490e+01 0.000000e+00 0.000000e+00 3.300000e-01 1.800000e-02 1.800000e-02 +1.072940e+01 0.000000e+00 0.000000e+00 3.540000e-01 1.933908e-02 1.933908e-02 +1.073440e+01 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1.886796e-02 +1.115820e+01 0.000000e+00 0.000000e+00 3.800000e-01 2.549510e-02 2.549510e-02 +1.116070e+01 0.000000e+00 0.000000e+00 3.250000e-01 2.416609e-02 2.416609e-02 +1.116770e+01 0.000000e+00 0.000000e+00 3.290000e-01 1.886796e-02 1.886796e-02 +1.116970e+01 0.000000e+00 0.000000e+00 3.610000e-01 1.941649e-02 1.941649e-02 +1.117870e+01 0.000000e+00 0.000000e+00 3.780000e-01 1.941649e-02 1.941649e-02 +1.118120e+01 0.000000e+00 0.000000e+00 3.230000e-01 1.802776e-02 1.802776e-02 +1.118470e+01 0.000000e+00 0.000000e+00 3.520000e-01 1.941649e-02 1.941649e-02 +1.119120e+01 0.000000e+00 0.000000e+00 3.480000e-01 1.941649e-02 1.941649e-02 +1.119420e+01 0.000000e+00 0.000000e+00 3.310000e-01 1.802776e-02 1.802776e-02 +1.120170e+01 0.000000e+00 0.000000e+00 3.680000e-01 1.860108e-02 1.860108e-02 +1.120620e+01 0.000000e+00 0.000000e+00 3.560000e-01 1.860108e-02 1.860108e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2009_I829441.cc b/analyses/pluginBABAR/BABAR_2009_I829441.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2009_I829441.cc @@ -0,0 +1,80 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2009_I829441 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2009_I829441); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2009_I829441); + + +} diff --git a/analyses/pluginBABAR/BABAR_2009_I829441.info b/analyses/pluginBABAR/BABAR_2009_I829441.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2009_I829441.info @@ -0,0 +1,38 @@ +Name: BABAR_2009_I829441 +Year: 2009 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ below 3 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 829441 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 103 (2009) 231801 + - Phys.Rev. D86 (2012) 032013 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies near the $\rho$ mass.' +Keywords: [] +BibKey: Aubert:2009ad +BibTeX: '@article{Aubert:2009ad, + author = "Aubert, Bernard and others", + title = "{Precise measurement of the e+ e- ---> pi+ pi- (gamma) + cross section with the Initial State Radiation method at + BABAR}", + collaboration = "BaBar", + journal = "Phys. Rev. Lett.", + volume = "103", + year = "2009", + pages = "231801", + doi = "10.1103/PhysRevLett.103.231801", + eprint = "0908.3589", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-13754, BABAR-PUB-09-027", + SLACcitation = "%%CITATION = ARXIV:0908.3589;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2009_I829441.plot b/analyses/pluginBABAR/BABAR_2009_I829441.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2009_I829441.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BABAR_2009_I829441/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2009_I829441.yoda b/analyses/pluginBABAR/BABAR_2009_I829441.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2009_I829441.yoda @@ -0,0 +1,345 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2009_I829441/d01-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2009_I829441/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.30500 0.00500 0.00500 2.54904e+01 2.69943e+00 2.69943e+00 +0.31500 0.00500 0.00500 3.54801e+01 2.91464e+00 2.91464e+00 +0.32500 0.00500 0.00500 4.54858e+01 3.04669e+00 3.04669e+00 +0.33500 0.00500 0.00500 5.17825e+01 3.13355e+00 3.13355e+00 +0.34500 0.00500 0.00500 6.44156e+01 3.49953e+00 3.49953e+00 +0.35500 0.00500 0.00500 7.52105e+01 3.86247e+00 3.86247e+00 +0.36500 0.00500 0.00500 8.01998e+01 3.87376e+00 3.87376e+00 +0.37500 0.00500 0.00500 8.63805e+01 4.02805e+00 4.02805e+00 +0.38500 0.00500 0.00500 1.02438e+02 4.31976e+00 4.31976e+00 +0.39500 0.00500 0.00500 1.04710e+02 3.96803e+00 3.96803e+00 +0.40500 0.00500 0.00500 1.18252e+02 4.09898e+00 4.09898e+00 +0.41500 0.00500 0.00500 1.18000e+02 3.90209e+00 3.90209e+00 +0.42500 0.00500 0.00500 1.27675e+02 4.17054e+00 4.17054e+00 +0.43500 0.00500 0.00500 1.29278e+02 3.83703e+00 3.83703e+00 +0.44500 0.00500 0.00500 1.37056e+02 4.08884e+00 4.08884e+00 +0.45500 0.00500 0.00500 1.38780e+02 3.80708e+00 3.80708e+00 +0.46500 0.00500 0.00500 1.49933e+02 4.05805e+00 4.05805e+00 +0.47500 0.00500 0.00500 1.61274e+02 4.29024e+00 4.29024e+00 +0.48500 0.00500 0.00500 1.67659e+02 4.29975e+00 4.29975e+00 +0.49500 0.00500 0.00500 1.70777e+02 4.09567e+00 4.09567e+00 +0.50100 0.00100 0.00100 1.70490e+02 4.94587e+00 4.94587e+00 +0.50300 0.00100 0.00100 1.73419e+02 4.53398e+00 4.53398e+00 +0.50500 0.00100 0.00100 1.77172e+02 4.50925e+00 4.50925e+00 +0.50700 0.00100 0.00100 1.75923e+02 4.79673e+00 4.79673e+00 +0.50900 0.00100 0.00100 1.76444e+02 5.32704e+00 5.32704e+00 +0.51100 0.00100 0.00100 1.78940e+02 5.10733e+00 5.10733e+00 +0.51300 0.00100 0.00100 1.88560e+02 5.72383e+00 5.72383e+00 +0.51500 0.00100 0.00100 1.85026e+02 5.34796e+00 5.34796e+00 +0.51700 0.00100 0.00100 1.87884e+02 4.52075e+00 4.52075e+00 +0.51900 0.00100 0.00100 1.91173e+02 4.83832e+00 4.83832e+00 +0.52100 0.00100 0.00100 1.86696e+02 4.97632e+00 4.97632e+00 +0.52300 0.00100 0.00100 1.93177e+02 5.58947e+00 5.58947e+00 +0.52500 0.00100 0.00100 1.99509e+02 5.91304e+00 5.91304e+00 +0.52700 0.00100 0.00100 1.97814e+02 4.73803e+00 4.73803e+00 +0.52900 0.00100 0.00100 2.02529e+02 4.70092e+00 4.70092e+00 +0.53100 0.00100 0.00100 2.01567e+02 5.89086e+00 5.89086e+00 +0.53300 0.00100 0.00100 2.05391e+02 5.87140e+00 5.87140e+00 +0.53500 0.00100 0.00100 2.12441e+02 5.04889e+00 5.04889e+00 +0.53700 0.00100 0.00100 2.17834e+02 4.88096e+00 4.88096e+00 +0.53900 0.00100 0.00100 2.16395e+02 5.23306e+00 5.23306e+00 +0.54100 0.00100 0.00100 2.22313e+02 6.02197e+00 6.02197e+00 +0.54300 0.00100 0.00100 2.27740e+02 5.73655e+00 5.73655e+00 +0.54500 0.00100 0.00100 2.25003e+02 5.73778e+00 5.73778e+00 +0.54700 0.00100 0.00100 2.34542e+02 6.23250e+00 6.23250e+00 +0.54900 0.00100 0.00100 2.35788e+02 5.23052e+00 5.23052e+00 +0.55100 0.00100 0.00100 2.36245e+02 5.65545e+00 5.65545e+00 +0.55300 0.00100 0.00100 2.35052e+02 6.10188e+00 6.10188e+00 +0.55500 0.00100 0.00100 2.44258e+02 6.03505e+00 6.03505e+00 +0.55700 0.00100 0.00100 2.41296e+02 6.26508e+00 6.26508e+00 +0.55900 0.00100 0.00100 2.38944e+02 4.88960e+00 4.88960e+00 +0.56100 0.00100 0.00100 2.47561e+02 5.95113e+00 5.95113e+00 +0.56300 0.00100 0.00100 2.52729e+02 6.22876e+00 6.22876e+00 +0.56500 0.00100 0.00100 2.54064e+02 6.29356e+00 6.29356e+00 +0.56700 0.00100 0.00100 2.51711e+02 5.89993e+00 5.89993e+00 +0.56900 0.00100 0.00100 2.63511e+02 6.23737e+00 6.23737e+00 +0.57100 0.00100 0.00100 2.58408e+02 5.95967e+00 5.95967e+00 +0.57300 0.00100 0.00100 2.57723e+02 6.36086e+00 6.36086e+00 +0.57500 0.00100 0.00100 2.66283e+02 5.16458e+00 5.16458e+00 +0.57700 0.00100 0.00100 2.76459e+02 6.53556e+00 6.53556e+00 +0.57900 0.00100 0.00100 2.68516e+02 6.16405e+00 6.16405e+00 +0.58100 0.00100 0.00100 2.78692e+02 6.61913e+00 6.61913e+00 +0.58300 0.00100 0.00100 2.79647e+02 5.81224e+00 5.81224e+00 +0.58500 0.00100 0.00100 2.87129e+02 6.07523e+00 6.07523e+00 +0.58700 0.00100 0.00100 2.90007e+02 5.74166e+00 5.74166e+00 +0.58900 0.00100 0.00100 2.89457e+02 6.42293e+00 6.42293e+00 +0.59100 0.00100 0.00100 2.88048e+02 5.95134e+00 5.95134e+00 +0.59300 0.00100 0.00100 3.01113e+02 5.52231e+00 5.52231e+00 +0.59500 0.00100 0.00100 3.09435e+02 6.95643e+00 6.95643e+00 +0.59700 0.00100 0.00100 3.21707e+02 6.80183e+00 6.80183e+00 +0.59900 0.00100 0.00100 3.30973e+02 7.60966e+00 7.60966e+00 +0.60100 0.00100 0.00100 3.25413e+02 6.06285e+00 6.06285e+00 +0.60300 0.00100 0.00100 3.32822e+02 5.21301e+00 5.21301e+00 +0.60500 0.00100 0.00100 3.36632e+02 5.88944e+00 5.88944e+00 +0.60700 0.00100 0.00100 3.41428e+02 6.67362e+00 6.67362e+00 +0.60900 0.00100 0.00100 3.44518e+02 6.71287e+00 6.71287e+00 +0.61100 0.00100 0.00100 3.49659e+02 5.70493e+00 5.70493e+00 +0.61300 0.00100 0.00100 3.53204e+02 5.30912e+00 5.30912e+00 +0.61500 0.00100 0.00100 3.57844e+02 6.82366e+00 6.82366e+00 +0.61700 0.00100 0.00100 3.66571e+02 7.12967e+00 7.12967e+00 +0.61900 0.00100 0.00100 3.73152e+02 5.35323e+00 5.35323e+00 +0.62100 0.00100 0.00100 3.77674e+02 6.75055e+00 6.75055e+00 +0.62300 0.00100 0.00100 3.92495e+02 6.66409e+00 6.66409e+00 +0.62500 0.00100 0.00100 3.89935e+02 6.72768e+00 6.72768e+00 +0.62700 0.00100 0.00100 4.03266e+02 7.19893e+00 7.19893e+00 +0.62900 0.00100 0.00100 4.09291e+02 6.64353e+00 6.64353e+00 +0.63100 0.00100 0.00100 4.32872e+02 7.16007e+00 7.16007e+00 +0.63300 0.00100 0.00100 4.32317e+02 6.74057e+00 6.74057e+00 +0.63500 0.00100 0.00100 4.41693e+02 7.32202e+00 7.32202e+00 +0.63700 0.00100 0.00100 4.47307e+02 7.55775e+00 7.55775e+00 +0.63900 0.00100 0.00100 4.40543e+02 7.26787e+00 7.26787e+00 +0.64100 0.00100 0.00100 4.62622e+02 6.96407e+00 6.96407e+00 +0.64300 0.00100 0.00100 4.69842e+02 7.75651e+00 7.75651e+00 +0.64500 0.00100 0.00100 4.73894e+02 6.26555e+00 6.26555e+00 +0.64700 0.00100 0.00100 4.81965e+02 7.71686e+00 7.71686e+00 +0.64900 0.00100 0.00100 5.06772e+02 7.42557e+00 7.42557e+00 +0.65100 0.00100 0.00100 5.15120e+02 7.32130e+00 7.32130e+00 +0.65300 0.00100 0.00100 5.21883e+02 7.97169e+00 7.97169e+00 +0.65500 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1.15454e+01 +0.72100 0.00100 0.00100 1.07526e+03 1.27249e+01 1.27249e+01 +0.72300 0.00100 0.00100 1.10393e+03 1.29544e+01 1.29544e+01 +0.72500 0.00100 0.00100 1.10533e+03 1.26579e+01 1.26579e+01 +0.72700 0.00100 0.00100 1.13328e+03 1.16202e+01 1.16202e+01 +0.72900 0.00100 0.00100 1.14954e+03 1.31084e+01 1.31084e+01 +0.73100 0.00100 0.00100 1.15838e+03 1.24490e+01 1.24490e+01 +0.73300 0.00100 0.00100 1.19523e+03 1.25723e+01 1.25723e+01 +0.73500 0.00100 0.00100 1.20812e+03 1.36549e+01 1.36549e+01 +0.73700 0.00100 0.00100 1.23571e+03 1.23235e+01 1.23235e+01 +0.73900 0.00100 0.00100 1.26629e+03 1.42119e+01 1.42119e+01 +0.74100 0.00100 0.00100 1.26664e+03 1.24516e+01 1.24516e+01 +0.74300 0.00100 0.00100 1.27859e+03 1.42056e+01 1.42056e+01 +0.74500 0.00100 0.00100 1.28014e+03 1.25097e+01 1.25097e+01 +0.74700 0.00100 0.00100 1.29324e+03 1.43521e+01 1.43521e+01 +0.74900 0.00100 0.00100 1.31638e+03 1.42986e+01 1.42986e+01 +0.75100 0.00100 0.00100 1.31756e+03 1.30731e+01 1.30731e+01 +0.75300 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2.37278e+00 2.32561e-01 2.32561e-01 +1.42500 0.02500 0.02500 1.91735e+00 1.46111e-01 1.46111e-01 +1.47500 0.02500 0.02500 7.13561e-01 1.02489e-01 1.02489e-01 +1.52500 0.02500 0.02500 1.29645e-01 6.35916e-02 6.35916e-02 +1.57500 0.02500 0.02500 4.41370e-02 5.98525e-02 5.98525e-02 +1.62500 0.02500 0.02500 1.62515e-01 6.06476e-02 6.06476e-02 +1.67500 0.02500 0.02500 6.15551e-01 7.83663e-02 7.83663e-02 +1.72500 0.02500 0.02500 1.08982e+00 9.16829e-02 9.16829e-02 +1.77500 0.02500 0.02500 1.29044e+00 9.77287e-02 9.77287e-02 +1.82500 0.02500 0.02500 1.31079e+00 1.02564e-01 1.02564e-01 +1.87500 0.02500 0.02500 1.21806e+00 9.53119e-02 9.53119e-02 +1.92500 0.02500 0.02500 8.61740e-01 7.95639e-02 7.95639e-02 +1.97500 0.02500 0.02500 6.18126e-01 6.72227e-02 6.72227e-02 +2.02500 0.02500 0.02500 2.88671e-01 4.66405e-02 4.66405e-02 +2.07500 0.02500 0.02500 2.09002e-01 4.32806e-02 4.32806e-02 +2.12500 0.02500 0.02500 1.32147e-01 3.98234e-02 3.98234e-02 +2.17500 0.02500 0.02500 8.86300e-02 3.73953e-02 3.73953e-02 +2.22500 0.02500 0.02500 1.13896e-01 3.44593e-02 3.44593e-02 +2.27500 0.02500 0.02500 2.02709e-01 4.36286e-02 4.36286e-02 +2.32500 0.02500 0.02500 1.04124e-01 3.10663e-02 3.10663e-02 +2.37500 0.02500 0.02500 1.28319e-01 3.56242e-02 3.56242e-02 +2.42500 0.02500 0.02500 8.12150e-02 2.90157e-02 2.90157e-02 +2.47500 0.02500 0.02500 4.30790e-02 3.22583e-02 3.22583e-02 +2.55000 0.05000 0.05000 4.76500e-02 1.86345e-02 1.86345e-02 +2.65000 0.05000 0.05000 2.42110e-02 1.36672e-02 1.36672e-02 +2.75000 0.05000 0.05000 1.39450e-02 1.41180e-02 1.41180e-02 +2.85000 0.05000 0.05000 9.18100e-03 1.32598e-02 1.32598e-02 +2.95000 0.05000 0.05000 1.02280e-02 1.23726e-02 1.23726e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2012_I1086164.cc b/analyses/pluginBABAR/BABAR_2012_I1086164.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2012_I1086164.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2012_I1086164 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2012_I1086164); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=4) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2012_I1086164); + + +} diff --git a/analyses/pluginBABAR/BABAR_2012_I1086164.info b/analyses/pluginBABAR/BABAR_2012_I1086164.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2012_I1086164.info @@ -0,0 +1,34 @@ +Name: BABAR_2012_I1086164 +Year: 2012 +Summary: Cross section for $e^+e^-\to 2\pi^+2\pi^-$ between 0.6 and 4.5 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 1086164 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D85 (2012) 112009, 2012 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to 2\pi^+2\pi^-$ using ISR by BaBar between 0.6 and 4.5 GeV.' +Keywords: +BibKey: Lees:2012cr +BibTeX: '@article{Lees:2012cr, + author = "Lees, J. P. and others", + title = "{Initial-State Radiation Measurement of the $e^+e^- -> + \pi^+\pi^-\pi^+\pi^-$ Cross Section}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D85", + year = "2012", + pages = "112009", + doi = "10.1103/PhysRevD.85.112009", + eprint = "1201.5677", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-14857, BABAR-PUB-11-016", + SLACcitation = "%%CITATION = ARXIV:1201.5677;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2012_I1086164.plot b/analyses/pluginBABAR/BABAR_2012_I1086164.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2012_I1086164.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /BABAR_2012_I1086164/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +LogY=0 +ConnectGaps=1 +LegendXPos=0.8 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2012_I1086164.yoda b/analyses/pluginBABAR/BABAR_2012_I1086164.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2012_I1086164.yoda @@ -0,0 +1,334 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2012_I1086164/d01-x01-y01 +Variations: [""] 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1.000000e-02 +4.387500e+03 0.000000e+00 0.000000e+00 1.000000e-01 1.000000e-02 1.000000e-02 +4.412500e+03 0.000000e+00 0.000000e+00 1.000000e-01 1.000000e-02 1.000000e-02 +4.437500e+03 0.000000e+00 0.000000e+00 9.000000e-02 1.000000e-02 1.000000e-02 +4.462500e+03 0.000000e+00 0.000000e+00 8.000000e-02 1.000000e-02 1.000000e-02 +4.487500e+03 0.000000e+00 0.000000e+00 9.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2012_I892684.cc b/analyses/pluginBABAR/BABAR_2012_I892684.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2012_I892684.cc @@ -0,0 +1,219 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2012_I892684 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2012_I892684); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + _cKpKmpippim = bookCounter("TMP/KpKmpippim"); + _cKstarKpi = bookCounter("TMP/KstarKpi"); + _cphipippim = bookCounter("TMP/phipippim"); + _cphif0_980 = bookCounter("TMP/phif0_980"); + _cphif0_600 = bookCounter("TMP/phif0_600"); + _cKpKmpi0pi0 = bookCounter("TMP/KpKmpi0pi0"); + _cphif0pi0pi0 = bookCounter("TMP/phif0pi0pi0"); + _c2Kp2Km = bookCounter("TMP/2Kp2Km"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // K*0 + if(abs(p.pdgId())==313) { + map nRes=nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // K* K+/- pi-/+ + if(ncount !=2 ) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==321 || abs(val.first)==211) { + continue; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched==false) continue; + if((nCount[321] == 1 && nCount[-321] ==0 && + nCount[211] == 0 && nCount[-211] == 1) || + (nCount[321] == 0 && nCount[-321] ==1 && + nCount[211] == 1 && nCount[-211] == 0)) + _cKstarKpi->fill(event.weight()); + } + else if(p.pdgId()==333) { + map nRes=nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // phi pi+pi- + if(ncount==2) { + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _cphipippim->fill(event.weight()); + } + foreach (const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=9010221&&p2.pdgId()!=9000221) continue; + if(p2.parents()[0].isSame(p)) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=0) continue; + bool matched2 = true; + for(auto const & val : nResB) { + if(val.second!=0) { + matched2 = false; + break; + } + } + if(matched2) { + if(p2.pdgId()==9010221) { + _cphif0pi0pi0->fill(event.weight()); + _cphif0_980 ->fill(event.weight()); + } + else { + _cphif0_600 ->fill(event.weight()); + } + } + } + } + } + if(ntotal==4) { + if(nCount[321]==1 && nCount[-321]==1 && nCount[211]==1 && nCount[-211]==1) + _cKpKmpippim->fill(event.weight()); + else if( nCount[321]==1 && nCount[-321]==1 && nCount[111]==2) + _cKpKmpi0pi0->fill(event.weight()); + else if( nCount[321]==2 && nCount[-321]==2) + _c2Kp2Km->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<9;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _cKpKmpippim->val(); + error = _cKpKmpippim->err(); + } + else if(ix==2) { + sigma = _cKstarKpi->val(); + error = _cKstarKpi->err(); + } + else if(ix==3) { + sigma = _cphipippim->val(); + error = _cphipippim->err(); + } + else if(ix==4) { + sigma = _cphif0_980->val(); + error = _cphif0_980->err(); + } + else if(ix==5) { + sigma = _cphif0_600->val(); + error = _cphif0_600->err(); + } + else if(ix==6) { + sigma = _cKpKmpi0pi0->val(); + error = _cKpKmpi0pi0->err(); + } + else if(ix==7) { + sigma = _cphif0pi0pi0->val(); + error = _cphif0pi0pi0->err(); + } + else if(ix==8) { + sigma = _c2Kp2Km->val(); + error = _c2Kp2Km->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _cKpKmpippim, _cKstarKpi, _cphipippim, + _cphif0_980,_cphif0_600, _cKpKmpi0pi0, _cphif0pi0pi0, _c2Kp2Km; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2012_I892684); + + +} diff --git a/analyses/pluginBABAR/BABAR_2012_I892684.info b/analyses/pluginBABAR/BABAR_2012_I892684.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2012_I892684.info @@ -0,0 +1,37 @@ +Name: BABAR_2012_I892684 +Year: 2012 +Summary: Cross sections for $e^+e^-\to$ $K^+K^-\pi^+\pi^-$, $K^+K^-\pi^0\pi^0$, and $K^+K^-K^+K^-$ between 1.28 and 5.0 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 892684 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D86 (2012) 012008, 2012 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^- \to$ $K^+K^-\pi^+\pi^-$, $K^+K^-\pi^0\pi^0$ and $K^+K^-K^+K^-$ via radiative return, + including the identification of $K^{*0}$, $\phi$ and $f_0(980)$ mesons for energies between 1.28 and 5.0 GeV' +Keywords: +BibKey: Lees:2011zi +BibTeX: '@article{Lees:2011zi, + author = "Lees, J. P. and others", + title = "{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}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D86", + year = "2012", + pages = "012008", + doi = "10.1103/PhysRevD.86.012008", + eprint = "1103.3001", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-14403", + SLACcitation = "%%CITATION = ARXIV:1103.3001;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2012_I892684.plot b/analyses/pluginBABAR/BABAR_2012_I892684.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2012_I892684.plot @@ -0,0 +1,55 @@ +BEGIN PLOT /BABAR_2012_I892684/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2012_I892684/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^{*0}K^+\pi^-+{\rm c.c.})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^{*0}K^+\pi^-+{\rm c.c.})$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2012_I892684/d03-x01-y01 +Title=$\sigma(e^+e^-\to \phi\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2012_I892684/d04-x01-y01 +Title=$\sigma(e^+e^-\to \phi f_0(980))$ extracted from $f_0\to\pi^+\pi^-$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi f_0(980))$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2012_I892684/d05-x01-y01 +Title=$\sigma(e^+e^-\to \phi f_0(600))$ extracted from $f_0\to\pi^+\pi^-$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi f_0(600))$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2012_I892684/d06-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\pi^0\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^0\pi^0)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2012_I892684/d07-x01-y01 +Title=$\sigma(e^+e^-\to \phi f_0(980))$ extracted from $f_0\to\pi^0\pi^0$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi f_0(980))$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2012_I892684/d08-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-K^+K^-)$/nb +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginBABAR/BABAR_2012_I892684.yoda b/analyses/pluginBABAR/BABAR_2012_I892684.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2012_I892684.yoda @@ -0,0 +1,679 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2012_I892684/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.004, up: 0.004}}, 1: {error: {dn: -0.008, up: 0.008}}, 2: {error: {dn: -0.008, up: 0.008}}, 3: {error: {dn: -0.01, up: 0.01}}, 4: {error: {dn: -0.017, up: 0.017}}, 5: {error: {dn: -0.018, up: 0.018}}, 6: {error: {dn: -0.022, up: 0.022}}, 7: {error: {dn: -0.03, up: 0.03}}, 8: {error: {dn: -0.04, up: 0.04}}, 9: {error: {dn: -0.053, up: 0.053}}, 10: {error: {dn: -0.061, up: 0.061}}, 11: {error: {dn: -0.069, up: 0.069}}, 12: {error: {dn: -0.078, up: 0.078}}, 13: {error: {dn: -0.083, up: 0.083}}, 14: {error: {dn: -0.094, up: 0.094}}, 15: {error: {dn: -0.099, up: 0.099}}, 16: 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6.000000e-03 +4.887500e+00 0.000000e+00 0.000000e+00 2.800000e-02 5.000000e-03 5.000000e-03 +4.912500e+00 0.000000e+00 0.000000e+00 3.000000e-02 5.000000e-03 5.000000e-03 +4.937500e+00 0.000000e+00 0.000000e+00 2.800000e-02 5.000000e-03 5.000000e-03 +4.962500e+00 0.000000e+00 0.000000e+00 3.000000e-02 5.000000e-03 5.000000e-03 +4.987500e+00 0.000000e+00 0.000000e+00 3.700000e-02 5.000000e-03 5.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2012_I892684/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.0, up: 0.0}}, 1: {error: {dn: -0.04, up: 0.04}}, 2: {error: {dn: -0.07, up: 0.07}}, 3: {error: {dn: -0.08, up: 0.08}}, 4: {error: {dn: -0.1, up: 0.1}}, 5: {error: {dn: -0.11, up: 0.11}}, 6: {error: {dn: -0.11, up: 0.11}}, 7: {error: {dn: -0.13, up: 0.13}}, 8: {error: {dn: -0.15, up: 0.15}}, 9: {error: {dn: -0.16, up: 0.16}}, 10: {error: {dn: -0.17, up: 0.17}}, 11: {error: {dn: -0.17, up: 0.17}}, 12: {error: {dn: -0.15, up: 0.15}}, 13: {error: {dn: -0.15, up: 0.15}}, 14: {error: {dn: -0.16, up: 0.16}}, 15: {error: {dn: -0.15, up: 0.15}}, 16: {error: {dn: -0.14, up: 0.14}}, 17: {error: {dn: -0.13, up: 0.13}}, 18: {error: {dn: -0.11, up: 0.11}}, 19: {error: {dn: -0.12, up: 0.12}}, 20: {error: {dn: -0.11, up: 0.11}}, 21: {error: {dn: -0.11, up: 0.11}}, 22: {error: {dn: -0.1, up: 0.1}}, 23: {error: {dn: -0.1, up: 0.1}}, 24: {error: {dn: -0.09, up: 0.09}}, 25: {error: {dn: -0.08, up: 0.08}}, 26: {error: {dn: -0.08, up: 0.08}}, 27: {error: {dn: -0.07, up: 0.07}}, 28: {error: {dn: -0.07, up: 0.07}}, 29: {error: {dn: -0.07, up: 0.07}}, 30: {error: {dn: -0.07, up: 0.07}}, 31: {error: {dn: -0.06, up: 0.06}}, 32: {error: {dn: -0.06, up: 0.06}}, 33: {error: {dn: -0.06, up: 0.06}}, 34: {error: {dn: -0.06, up: 0.06}}, 35: {error: {dn: -0.06, up: 0.06}}, 36: {error: {dn: -0.05, up: 0.05}}, 37: {error: {dn: -0.05, up: 0.05}}, 38: {error: {dn: -0.05, up: 0.05}}, 39: {error: {dn: -0.04, up: 0.04}}, 40: {error: {dn: -0.04, up: 0.04}}, 41: {error: {dn: -0.04, up: 0.04}}, 42: {error: {dn: -0.04, up: 0.04}}, 43: {error: {dn: -0.04, up: 0.04}}, 44: {error: {dn: -0.04, up: 0.04}}, 45: {error: {dn: -0.04, up: 0.04}}, 46: {error: {dn: -0.04, up: 0.04}}, 47: {error: {dn: -0.04, up: 0.04}}, 48: {error: {dn: -0.03, up: 0.03}}, 49: {error: {dn: -0.03, up: 0.03}}, 50: {error: {dn: -0.03, up: 0.03}}, 51: {error: {dn: -0.03, up: 0.03}}, 52: {error: {dn: -0.03, up: 0.03}}, 53: {error: {dn: -0.03, up: 0.03}}, 54: {error: {dn: -0.03, up: 0.03}}, 55: {error: {dn: -0.03, up: 0.03}}, 56: {error: {dn: -0.03, up: 0.03}}, 57: {error: {dn: -0.03, up: 0.03}}, 58: {error: {dn: -0.03, up: 0.03}}, 59: {error: {dn: -0.02, up: 0.02}}, 60: {error: {dn: -0.06, up: 0.06}}, 61: {error: {dn: -0.05, up: 0.05}}, 62: {error: {dn: -0.02, up: 0.02}}, 63: {error: {dn: -0.02, up: 0.02}}, 64: {error: {dn: -0.02, up: 0.02}}, 65: {error: {dn: -0.02, up: 0.02}}, 66: {error: {dn: -0.02, up: 0.02}}, 67: {error: {dn: -0.02, up: 0.02}}, 68: {error: {dn: -0.02, up: 0.02}}, 69: {error: {dn: -0.02, up: 0.02}}, 70: {error: {dn: -0.02, up: 0.02}}, 71: {error: {dn: -0.02, up: 0.02}}, 72: {error: {dn: -0.02, up: 0.02}}, 73: {error: {dn: -0.02, up: 0.02}}, 74: {error: {dn: -0.02, up: 0.02}}, 75: {error: {dn: -0.02, up: 0.02}}, 76: {error: {dn: -0.02, up: 0.02}}, 77: {error: {dn: -0.02, up: 0.02}}, 78: {error: {dn: -0.01, up: 0.01}}, 79: {error: {dn: -0.01, up: 0.01}}, 80: {error: {dn: -0.01, up: 0.01}}, 81: {error: {dn: -0.01, up: 0.01}}, 82: {error: {dn: -0.02, up: 0.02}}, 83: {error: {dn: -0.01, up: 0.01}}, 84: {error: {dn: -0.02, up: 0.02}}, 85: {error: {dn: -0.01, up: 0.01}}, 86: {error: {dn: -0.01, up: 0.01}}, 87: {error: {dn: -0.01, up: 0.01}}, 88: {error: {dn: -0.01, up: 0.01}}, 89: {error: {dn: -0.01, up: 0.01}}, 90: {error: {dn: -0.01, up: 0.01}}, 91: {error: {dn: -0.01, up: 0.01}}, 92: {error: {dn: -0.01, up: 0.01}}, 93: {error: {dn: -0.01, up: 0.01}}, 94: {error: {dn: -0.01, up: 0.01}}, 95: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2012_I892684/d02-x01-y01 +Title: doi:10.17182/hepdata.62222.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.587500e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.612500e+00 0.000000e+00 0.000000e+00 1.900000e-01 4.000000e-02 4.000000e-02 +1.637500e+00 0.000000e+00 0.000000e+00 4.800000e-01 7.000000e-02 7.000000e-02 +1.662500e+00 0.000000e+00 0.000000e+00 1.010000e+00 8.000000e-02 8.000000e-02 +1.687500e+00 0.000000e+00 0.000000e+00 1.290000e+00 1.000000e-01 1.000000e-01 +1.712500e+00 0.000000e+00 0.000000e+00 1.580000e+00 1.100000e-01 1.100000e-01 +1.737500e+00 0.000000e+00 0.000000e+00 1.820000e+00 1.100000e-01 1.100000e-01 +1.762500e+00 0.000000e+00 0.000000e+00 2.240000e+00 1.300000e-01 1.300000e-01 +1.787500e+00 0.000000e+00 0.000000e+00 2.750000e+00 1.500000e-01 1.500000e-01 +1.812500e+00 0.000000e+00 0.000000e+00 3.610000e+00 1.600000e-01 1.600000e-01 +1.837500e+00 0.000000e+00 0.000000e+00 4.220000e+00 1.700000e-01 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0.000000e+00 0.000000e+00 1.200000e-01 2.000000e-02 2.000000e-02 +3.462500e+00 0.000000e+00 0.000000e+00 1.500000e-01 2.000000e-02 2.000000e-02 +3.487500e+00 0.000000e+00 0.000000e+00 1.300000e-01 2.000000e-02 2.000000e-02 +3.512500e+00 0.000000e+00 0.000000e+00 1.500000e-01 2.000000e-02 2.000000e-02 +3.537500e+00 0.000000e+00 0.000000e+00 8.000000e-02 1.000000e-02 1.000000e-02 +3.562500e+00 0.000000e+00 0.000000e+00 1.200000e-01 1.000000e-02 1.000000e-02 +3.587500e+00 0.000000e+00 0.000000e+00 1.200000e-01 1.000000e-02 1.000000e-02 +3.612500e+00 0.000000e+00 0.000000e+00 9.000000e-02 1.000000e-02 1.000000e-02 +3.637500e+00 0.000000e+00 0.000000e+00 1.200000e-01 2.000000e-02 2.000000e-02 +3.662500e+00 0.000000e+00 0.000000e+00 9.000000e-02 1.000000e-02 1.000000e-02 +3.687500e+00 0.000000e+00 0.000000e+00 1.500000e-01 2.000000e-02 2.000000e-02 +3.712500e+00 0.000000e+00 0.000000e+00 8.000000e-02 1.000000e-02 1.000000e-02 +3.737500e+00 0.000000e+00 0.000000e+00 7.000000e-02 1.000000e-02 1.000000e-02 +3.762500e+00 0.000000e+00 0.000000e+00 1.100000e-01 1.000000e-02 1.000000e-02 +3.787500e+00 0.000000e+00 0.000000e+00 9.000000e-02 1.000000e-02 1.000000e-02 +3.812500e+00 0.000000e+00 0.000000e+00 9.000000e-02 1.000000e-02 1.000000e-02 +3.837500e+00 0.000000e+00 0.000000e+00 6.000000e-02 1.000000e-02 1.000000e-02 +3.862500e+00 0.000000e+00 0.000000e+00 6.000000e-02 1.000000e-02 1.000000e-02 +3.887500e+00 0.000000e+00 0.000000e+00 8.000000e-02 1.000000e-02 1.000000e-02 +3.912500e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.000000e-02 1.000000e-02 +3.937500e+00 0.000000e+00 0.000000e+00 6.000000e-02 1.000000e-02 1.000000e-02 +3.962500e+00 0.000000e+00 0.000000e+00 6.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2012_I892684/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.01, up: 0.01}}, 1: {error: {dn: -0.03, up: 0.03}}, 2: {error: {dn: -0.03, up: 0.03}}, 3: {error: {dn: -0.03, up: 0.03}}, 4: {error: {dn: -0.04, up: 0.04}}, 5: {error: {dn: -0.05, up: 0.05}}, 6: {error: {dn: -0.06, up: 0.06}}, 7: {error: {dn: -0.06, up: 0.06}}, 8: {error: {dn: -0.07, up: 0.07}}, 9: {error: {dn: -0.07, up: 0.07}}, 10: {error: {dn: -0.07, up: 0.07}}, 11: {error: {dn: -0.08, up: 0.08}}, 12: {error: {dn: -0.07, up: 0.07}}, 13: {error: {dn: -0.07, up: 0.07}}, 14: {error: {dn: -0.07, up: 0.07}}, 15: {error: {dn: -0.07, up: 0.07}}, 16: {error: {dn: -0.06, up: 0.06}}, 17: {error: {dn: -0.06, up: 0.06}}, 18: {error: {dn: -0.06, up: 0.06}}, 19: {error: {dn: -0.05, up: 0.05}}, 20: {error: {dn: -0.05, up: 0.05}}, 21: {error: {dn: -0.05, up: 0.05}}, 22: {error: {dn: -0.05, up: 0.05}}, 23: {error: {dn: -0.05, up: 0.05}}, 24: {error: {dn: -0.05, up: 0.05}}, 25: {error: {dn: -0.05, up: 0.05}}, 26: {error: {dn: -0.05, up: 0.05}}, 27: {error: {dn: -0.05, up: 0.05}}, 28: {error: {dn: -0.04, up: 0.04}}, 29: {error: {dn: -0.04, up: 0.04}}, 30: {error: {dn: -0.03, up: 0.03}}, 31: {error: {dn: -0.04, up: 0.04}}, 32: {error: {dn: -0.03, up: 0.03}}, 33: {error: {dn: -0.03, up: 0.03}}, 34: {error: {dn: -0.03, up: 0.03}}, 35: {error: {dn: -0.03, up: 0.03}}, 36: {error: {dn: -0.03, up: 0.03}}, 37: {error: {dn: -0.02, up: 0.02}}, 38: {error: {dn: -0.02, up: 0.02}}, 39: {error: {dn: -0.02, up: 0.02}}, 40: {error: {dn: -0.02, up: 0.02}}, 41: {error: {dn: -0.02, up: 0.02}}, 42: {error: {dn: -0.02, up: 0.02}}, 43: {error: {dn: -0.02, up: 0.02}}, 44: {error: {dn: -0.02, up: 0.02}}, 45: {error: {dn: -0.02, up: 0.02}}, 46: {error: {dn: -0.02, up: 0.02}}, 47: {error: {dn: -0.02, up: 0.02}}, 48: {error: {dn: -0.01, up: 0.01}}, 49: {error: {dn: -0.01, up: 0.01}}, 50: {error: {dn: -0.01, up: 0.01}}, 51: {error: {dn: -0.01, up: 0.01}}, 52: {error: {dn: -0.01, up: 0.01}}, 53: {error: {dn: -0.01, up: 0.01}}, 54: {error: {dn: -0.01, up: 0.01}}, 55: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2012_I892684/d03-x01-y01 +Title: doi:10.17182/hepdata.62222.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.487500e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +1.512500e+00 0.000000e+00 0.000000e+00 8.000000e-02 3.000000e-02 3.000000e-02 +1.537500e+00 0.000000e+00 0.000000e+00 1.000000e-01 3.000000e-02 3.000000e-02 +1.562500e+00 0.000000e+00 0.000000e+00 1.200000e-01 3.000000e-02 3.000000e-02 +1.587500e+00 0.000000e+00 0.000000e+00 2.100000e-01 4.000000e-02 4.000000e-02 +1.612500e+00 0.000000e+00 0.000000e+00 3.300000e-01 5.000000e-02 5.000000e-02 +1.637500e+00 0.000000e+00 0.000000e+00 4.800000e-01 6.000000e-02 6.000000e-02 +1.662500e+00 0.000000e+00 0.000000e+00 4.900000e-01 6.000000e-02 6.000000e-02 +1.687500e+00 0.000000e+00 0.000000e+00 5.400000e-01 7.000000e-02 7.000000e-02 +1.712500e+00 0.000000e+00 0.000000e+00 5.300000e-01 7.000000e-02 7.000000e-02 +1.737500e+00 0.000000e+00 0.000000e+00 4.800000e-01 7.000000e-02 7.000000e-02 +1.762500e+00 0.000000e+00 0.000000e+00 6.100000e-01 8.000000e-02 8.000000e-02 +1.787500e+00 0.000000e+00 0.000000e+00 4.800000e-01 7.000000e-02 7.000000e-02 +1.812500e+00 0.000000e+00 0.000000e+00 3.400000e-01 7.000000e-02 7.000000e-02 +1.837500e+00 0.000000e+00 0.000000e+00 2.900000e-01 7.000000e-02 7.000000e-02 +1.862500e+00 0.000000e+00 0.000000e+00 3.600000e-01 7.000000e-02 7.000000e-02 +1.887500e+00 0.000000e+00 0.000000e+00 3.400000e-01 6.000000e-02 6.000000e-02 +1.912500e+00 0.000000e+00 0.000000e+00 2.900000e-01 6.000000e-02 6.000000e-02 +1.937500e+00 0.000000e+00 0.000000e+00 3.200000e-01 6.000000e-02 6.000000e-02 +1.962500e+00 0.000000e+00 0.000000e+00 2.800000e-01 5.000000e-02 5.000000e-02 +1.987500e+00 0.000000e+00 0.000000e+00 3.200000e-01 5.000000e-02 5.000000e-02 +2.012500e+00 0.000000e+00 0.000000e+00 3.700000e-01 5.000000e-02 5.000000e-02 +2.037500e+00 0.000000e+00 0.000000e+00 3.100000e-01 5.000000e-02 5.000000e-02 +2.062500e+00 0.000000e+00 0.000000e+00 3.900000e-01 5.000000e-02 5.000000e-02 +2.087500e+00 0.000000e+00 0.000000e+00 3.200000e-01 5.000000e-02 5.000000e-02 +2.112500e+00 0.000000e+00 0.000000e+00 5.100000e-01 5.000000e-02 5.000000e-02 +2.137500e+00 0.000000e+00 0.000000e+00 4.100000e-01 5.000000e-02 5.000000e-02 +2.162500e+00 0.000000e+00 0.000000e+00 4.300000e-01 5.000000e-02 5.000000e-02 +2.187500e+00 0.000000e+00 0.000000e+00 3.300000e-01 4.000000e-02 4.000000e-02 +2.212500e+00 0.000000e+00 0.000000e+00 2.100000e-01 4.000000e-02 4.000000e-02 +2.237500e+00 0.000000e+00 0.000000e+00 1.900000e-01 3.000000e-02 3.000000e-02 +2.262500e+00 0.000000e+00 0.000000e+00 1.000000e-01 4.000000e-02 4.000000e-02 +2.287500e+00 0.000000e+00 0.000000e+00 1.300000e-01 3.000000e-02 3.000000e-02 +2.312500e+00 0.000000e+00 0.000000e+00 1.300000e-01 3.000000e-02 3.000000e-02 +2.337500e+00 0.000000e+00 0.000000e+00 1.500000e-01 3.000000e-02 3.000000e-02 +2.362500e+00 0.000000e+00 0.000000e+00 1.200000e-01 3.000000e-02 3.000000e-02 +2.387500e+00 0.000000e+00 0.000000e+00 1.000000e-01 3.000000e-02 3.000000e-02 +2.412500e+00 0.000000e+00 0.000000e+00 1.200000e-01 2.000000e-02 2.000000e-02 +2.437500e+00 0.000000e+00 0.000000e+00 1.200000e-01 2.000000e-02 2.000000e-02 +2.462500e+00 0.000000e+00 0.000000e+00 1.000000e-01 2.000000e-02 2.000000e-02 +2.487500e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.000000e-02 2.000000e-02 +2.512500e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.000000e-02 2.000000e-02 +2.537500e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +2.562500e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.000000e-02 2.000000e-02 +2.587500e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +2.612500e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +2.637500e+00 0.000000e+00 0.000000e+00 1.000000e-01 2.000000e-02 2.000000e-02 +2.662500e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +2.687500e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +2.712500e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.000000e-02 1.000000e-02 +2.737500e+00 0.000000e+00 0.000000e+00 6.000000e-02 1.000000e-02 1.000000e-02 +2.762500e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +2.787500e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +2.812500e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +2.837500e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +2.862500e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2012_I892684/d04-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.01, up: 0.01}}, 1: {error: {dn: -0.02, up: 0.02}}, 2: {error: {dn: -0.04, up: 0.04}}, 3: {error: {dn: -0.04, up: 0.04}}, 4: {error: {dn: -0.04, up: 0.04}}, 5: {error: {dn: -0.05, up: 0.05}}, 6: {error: {dn: -0.05, up: 0.05}}, 7: {error: {dn: -0.06, up: 0.06}}, 8: {error: {dn: -0.05, up: 0.05}}, 9: {error: {dn: -0.06, up: 0.06}}, 10: {error: {dn: -0.07, up: 0.07}}, 11: {error: {dn: -0.06, up: 0.06}}, 12: {error: {dn: -0.05, up: 0.05}}, 13: {error: {dn: -0.04, up: 0.04}}, 14: {error: {dn: -0.04, up: 0.04}}, 15: {error: {dn: -0.04, up: 0.04}}, 16: {error: {dn: -0.03, up: 0.03}}, 17: {error: {dn: -0.03, up: 0.03}}, 18: {error: {dn: -0.03, up: 0.03}}, 19: {error: {dn: -0.03, up: 0.03}}, 20: {error: {dn: -0.03, up: 0.03}}, 21: {error: {dn: -0.03, up: 0.03}}, 22: {error: {dn: -0.02, up: 0.02}}, 23: {error: {dn: -0.03, up: 0.03}}, 24: {error: {dn: -0.02, up: 0.02}}, 25: {error: {dn: -0.02, up: 0.02}}, 26: {error: {dn: -0.02, up: 0.02}}, 27: {error: {dn: -0.02, up: 0.02}}, 28: {error: {dn: -0.02, up: 0.02}}, 29: {error: {dn: -0.02, up: 0.02}}, 30: {error: {dn: -0.02, up: 0.02}}, 31: {error: {dn: -0.02, up: 0.02}}, 32: {error: {dn: -0.02, up: 0.02}}, 33: {error: {dn: -0.03, up: 0.03}}, 34: {error: {dn: -0.02, up: 0.02}}, 35: {error: {dn: -0.02, up: 0.02}}, 36: {error: {dn: -0.02, up: 0.02}}, 37: {error: {dn: -0.02, up: 0.02}}, 38: {error: {dn: -0.02, up: 0.02}}, 39: {error: {dn: -0.02, up: 0.02}}, 40: {error: {dn: -0.02, up: 0.02}}, 41: {error: {dn: -0.02, up: 0.02}}, 42: {error: {dn: -0.02, up: 0.02}}, 43: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2012_I892684/d04-x01-y01 +Title: doi:10.17182/hepdata.62222.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.887500e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +1.912500e+00 0.000000e+00 0.000000e+00 1.000000e-02 2.000000e-02 2.000000e-02 +1.937500e+00 0.000000e+00 0.000000e+00 1.600000e-01 4.000000e-02 4.000000e-02 +1.962500e+00 0.000000e+00 0.000000e+00 1.500000e-01 4.000000e-02 4.000000e-02 +1.987500e+00 0.000000e+00 0.000000e+00 1.900000e-01 4.000000e-02 4.000000e-02 +2.012500e+00 0.000000e+00 0.000000e+00 3.200000e-01 5.000000e-02 5.000000e-02 +2.037500e+00 0.000000e+00 0.000000e+00 2.800000e-01 5.000000e-02 5.000000e-02 +2.062500e+00 0.000000e+00 0.000000e+00 3.800000e-01 6.000000e-02 6.000000e-02 +2.087500e+00 0.000000e+00 0.000000e+00 3.500000e-01 5.000000e-02 5.000000e-02 +2.112500e+00 0.000000e+00 0.000000e+00 6.000000e-01 6.000000e-02 6.000000e-02 +2.137500e+00 0.000000e+00 0.000000e+00 5.000000e-01 7.000000e-02 7.000000e-02 +2.162500e+00 0.000000e+00 0.000000e+00 5.400000e-01 6.000000e-02 6.000000e-02 +2.187500e+00 0.000000e+00 0.000000e+00 3.800000e-01 5.000000e-02 5.000000e-02 +2.212500e+00 0.000000e+00 0.000000e+00 1.900000e-01 4.000000e-02 4.000000e-02 +2.237500e+00 0.000000e+00 0.000000e+00 1.900000e-01 4.000000e-02 4.000000e-02 +2.262500e+00 0.000000e+00 0.000000e+00 1.000000e-01 4.000000e-02 4.000000e-02 +2.287500e+00 0.000000e+00 0.000000e+00 1.500000e-01 3.000000e-02 3.000000e-02 +2.312500e+00 0.000000e+00 0.000000e+00 1.400000e-01 3.000000e-02 3.000000e-02 +2.337500e+00 0.000000e+00 0.000000e+00 1.600000e-01 3.000000e-02 3.000000e-02 +2.362500e+00 0.000000e+00 0.000000e+00 1.400000e-01 3.000000e-02 3.000000e-02 +2.387500e+00 0.000000e+00 0.000000e+00 7.000000e-02 3.000000e-02 3.000000e-02 +2.412500e+00 0.000000e+00 0.000000e+00 1.100000e-01 3.000000e-02 3.000000e-02 +2.437500e+00 0.000000e+00 0.000000e+00 1.100000e-01 2.000000e-02 2.000000e-02 +2.462500e+00 0.000000e+00 0.000000e+00 1.100000e-01 3.000000e-02 3.000000e-02 +2.487500e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.000000e-02 2.000000e-02 +2.512500e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +2.537500e+00 0.000000e+00 0.000000e+00 6.000000e-02 2.000000e-02 2.000000e-02 +2.562500e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.000000e-02 2.000000e-02 +2.587500e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +2.612500e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +2.637500e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +2.662500e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +2.687500e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +2.712500e+00 0.000000e+00 0.000000e+00 4.000000e-02 3.000000e-02 3.000000e-02 +2.737500e+00 0.000000e+00 0.000000e+00 4.000000e-02 2.000000e-02 2.000000e-02 +2.762500e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +2.787500e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +2.812500e+00 0.000000e+00 0.000000e+00 2.000000e-02 2.000000e-02 2.000000e-02 +2.837500e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.000000e-02 2.000000e-02 +2.862500e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +2.887500e+00 0.000000e+00 0.000000e+00 2.000000e-02 2.000000e-02 2.000000e-02 +2.912500e+00 0.000000e+00 0.000000e+00 4.000000e-02 2.000000e-02 2.000000e-02 +2.937500e+00 0.000000e+00 0.000000e+00 1.000000e-02 2.000000e-02 2.000000e-02 +2.962500e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2012_I892684/d05-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.01, up: 0.01}}, 1: {error: {dn: -0.01, up: 0.01}}, 2: {error: {dn: -0.01, up: 0.01}}, 3: {error: {dn: -0.01, up: 0.01}}, 4: {error: {dn: -0.01, up: 0.01}}, 5: {error: {dn: -0.01, up: 0.01}}, 6: {error: {dn: -0.01, up: 0.01}}, 7: {error: {dn: -0.02, up: 0.02}}, 8: {error: {dn: -0.02, up: 0.02}}, 9: {error: {dn: -0.04, up: 0.04}}, 10: {error: {dn: -0.04, up: 0.04}}, 11: {error: {dn: -0.04, up: 0.04}}, 12: {error: {dn: -0.06, up: 0.06}}, 13: {error: {dn: -0.08, up: 0.08}}, 14: {error: {dn: -0.09, up: 0.09}}, 15: {error: {dn: -0.09, up: 0.09}}, 16: {error: {dn: -0.1, up: 0.1}}, 17: {error: {dn: -0.11, up: 0.11}}, 18: {error: {dn: -0.1, up: 0.1}}, 19: {error: {dn: -0.12, up: 0.12}}, 20: {error: {dn: -0.11, up: 0.11}}, 21: {error: {dn: -0.1, up: 0.1}}, 22: {error: {dn: -0.1, up: 0.1}}, 23: {error: {dn: -0.11, up: 0.11}}, 24: {error: {dn: -0.09, up: 0.09}}, 25: {error: {dn: -0.09, up: 0.09}}, 26: {error: {dn: -0.08, up: 0.08}}, 27: {error: {dn: -0.07, up: 0.07}}, 28: {error: {dn: -0.07, up: 0.07}}, 29: {error: {dn: -0.06, up: 0.06}}, 30: {error: {dn: -0.05, up: 0.05}}, 31: {error: {dn: -0.05, up: 0.05}}, 32: {error: {dn: -0.05, up: 0.05}}, 33: {error: {dn: -0.05, up: 0.05}}, 34: {error: {dn: -0.04, up: 0.04}}, 35: {error: {dn: -0.04, up: 0.04}}, 36: {error: {dn: -0.03, up: 0.03}}, 37: {error: {dn: -0.03, up: 0.03}}, 38: {error: {dn: -0.03, up: 0.03}}, 39: {error: {dn: -0.02, up: 0.02}}, 40: {error: {dn: -0.02, up: 0.02}}, 41: {error: {dn: -0.02, up: 0.02}}, 42: {error: {dn: -0.02, up: 0.02}}, 43: {error: {dn: -0.02, up: 0.02}}, 44: {error: {dn: -0.02, up: 0.02}}, 45: {error: {dn: -0.02, up: 0.02}}, 46: {error: {dn: -0.02, up: 0.02}}, 47: {error: {dn: -0.01, up: 0.01}}, 48: {error: {dn: -0.01, up: 0.01}}, 49: {error: {dn: -0.01, up: 0.01}}, 50: {error: {dn: -0.01, up: 0.01}}, 51: {error: {dn: -0.01, up: 0.01}}, 52: {error: {dn: -0.01, up: 0.01}}, 53: {error: {dn: -0.01, up: 0.01}}, 54: {error: {dn: -0.02, up: 0.02}}, 55: {error: {dn: -0.01, up: 0.01}}, 56: {error: {dn: -0.02, up: 0.02}}, 57: {error: {dn: -0.02, up: 0.02}}, 58: {error: {dn: -0.03, up: 0.03}}, 59: {error: {dn: -0.02, up: 0.02}}, 60: {error: {dn: -0.01, up: 0.01}}, 61: {error: {dn: -0.02, up: 0.02}}, 62: {error: {dn: -0.02, up: 0.02}}, 63: {error: {dn: -0.02, up: 0.02}}, 64: {error: {dn: -0.02, up: 0.02}}, 65: {error: {dn: -0.02, up: 0.02}}, 66: {error: {dn: -0.01, up: 0.01}}, 67: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2012_I892684/d05-x01-y01 +Title: doi:10.17182/hepdata.62222.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.287500e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +1.312500e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +1.337500e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +1.362500e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +1.387500e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +1.412500e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +1.437500e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +1.462500e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.000000e-02 2.000000e-02 +1.487500e+00 0.000000e+00 0.000000e+00 6.000000e-02 2.000000e-02 2.000000e-02 +1.512500e+00 0.000000e+00 0.000000e+00 1.200000e-01 4.000000e-02 4.000000e-02 +1.537500e+00 0.000000e+00 0.000000e+00 1.500000e-01 4.000000e-02 4.000000e-02 +1.562500e+00 0.000000e+00 0.000000e+00 1.800000e-01 4.000000e-02 4.000000e-02 +1.587500e+00 0.000000e+00 0.000000e+00 3.100000e-01 6.000000e-02 6.000000e-02 +1.612500e+00 0.000000e+00 0.000000e+00 4.800000e-01 8.000000e-02 8.000000e-02 +1.637500e+00 0.000000e+00 0.000000e+00 7.000000e-01 9.000000e-02 9.000000e-02 +1.662500e+00 0.000000e+00 0.000000e+00 7.200000e-01 9.000000e-02 9.000000e-02 +1.687500e+00 0.000000e+00 0.000000e+00 8.000000e-01 1.000000e-01 1.000000e-01 +1.712500e+00 0.000000e+00 0.000000e+00 7.900000e-01 1.100000e-01 1.100000e-01 +1.737500e+00 0.000000e+00 0.000000e+00 7.200000e-01 1.000000e-01 1.000000e-01 +1.762500e+00 0.000000e+00 0.000000e+00 9.100000e-01 1.200000e-01 1.200000e-01 +1.787500e+00 0.000000e+00 0.000000e+00 7.200000e-01 1.100000e-01 1.100000e-01 +1.812500e+00 0.000000e+00 0.000000e+00 5.100000e-01 1.000000e-01 1.000000e-01 +1.837500e+00 0.000000e+00 0.000000e+00 4.300000e-01 1.000000e-01 1.000000e-01 +1.862500e+00 0.000000e+00 0.000000e+00 5.400000e-01 1.100000e-01 1.100000e-01 +1.887500e+00 0.000000e+00 0.000000e+00 5.000000e-01 9.000000e-02 9.000000e-02 +1.912500e+00 0.000000e+00 0.000000e+00 4.000000e-01 9.000000e-02 9.000000e-02 +1.937500e+00 0.000000e+00 0.000000e+00 3.200000e-01 8.000000e-02 8.000000e-02 +1.962500e+00 0.000000e+00 0.000000e+00 2.600000e-01 7.000000e-02 7.000000e-02 +1.987500e+00 0.000000e+00 0.000000e+00 2.700000e-01 7.000000e-02 7.000000e-02 +2.012500e+00 0.000000e+00 0.000000e+00 2.500000e-01 6.000000e-02 6.000000e-02 +2.037500e+00 0.000000e+00 0.000000e+00 1.800000e-01 5.000000e-02 5.000000e-02 +2.062500e+00 0.000000e+00 0.000000e+00 2.500000e-01 5.000000e-02 5.000000e-02 +2.087500e+00 0.000000e+00 0.000000e+00 1.500000e-01 5.000000e-02 5.000000e-02 +2.112500e+00 0.000000e+00 0.000000e+00 1.800000e-01 5.000000e-02 5.000000e-02 +2.137500e+00 0.000000e+00 0.000000e+00 1.000000e-01 4.000000e-02 4.000000e-02 +2.162500e+00 0.000000e+00 0.000000e+00 1.000000e-01 4.000000e-02 4.000000e-02 +2.187500e+00 0.000000e+00 0.000000e+00 5.000000e-02 3.000000e-02 3.000000e-02 +2.212500e+00 0.000000e+00 0.000000e+00 5.000000e-02 3.000000e-02 3.000000e-02 +2.237500e+00 0.000000e+00 0.000000e+00 6.000000e-02 3.000000e-02 3.000000e-02 +2.262500e+00 0.000000e+00 0.000000e+00 4.000000e-02 2.000000e-02 2.000000e-02 +2.287500e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +2.312500e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +2.337500e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.000000e-02 2.000000e-02 +2.362500e+00 0.000000e+00 0.000000e+00 4.000000e-02 2.000000e-02 2.000000e-02 +2.387500e+00 0.000000e+00 0.000000e+00 6.000000e-02 2.000000e-02 2.000000e-02 +2.412500e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.000000e-02 2.000000e-02 +2.437500e+00 0.000000e+00 0.000000e+00 4.000000e-02 2.000000e-02 2.000000e-02 +2.462500e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +2.487500e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +2.512500e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +2.537500e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +2.562500e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +2.587500e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +2.612500e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +2.637500e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +2.662500e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +2.687500e+00 0.000000e+00 0.000000e+00 2.000000e-02 2.000000e-02 2.000000e-02 +2.712500e+00 0.000000e+00 0.000000e+00 2.000000e-02 2.000000e-02 2.000000e-02 +2.737500e+00 0.000000e+00 0.000000e+00 3.000000e-02 3.000000e-02 3.000000e-02 +2.762500e+00 0.000000e+00 0.000000e+00 1.000000e-02 2.000000e-02 2.000000e-02 +2.787500e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +2.812500e+00 0.000000e+00 0.000000e+00 1.000000e-02 2.000000e-02 2.000000e-02 +2.837500e+00 0.000000e+00 0.000000e+00 1.000000e-02 2.000000e-02 2.000000e-02 +2.862500e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +2.887500e+00 0.000000e+00 0.000000e+00 1.000000e-02 2.000000e-02 2.000000e-02 +2.912500e+00 0.000000e+00 0.000000e+00 2.000000e-02 2.000000e-02 2.000000e-02 +2.937500e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +2.962500e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2012_I892684/d06-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.04, up: 0.04}}, 1: {error: {dn: -0.05, up: 0.05}}, 2: {error: {dn: -0.05, up: 0.05}}, 3: {error: {dn: -0.06, up: 0.06}}, 4: {error: {dn: -0.08, up: 0.08}}, 5: {error: {dn: -0.07, up: 0.07}}, 6: {error: {dn: -0.07, up: 0.07}}, 7: {error: {dn: -0.08, up: 0.08}}, 8: {error: {dn: -0.08, up: 0.08}}, 9: {error: {dn: -0.08, up: 0.08}}, 10: {error: {dn: -0.08, up: 0.08}}, 11: {error: {dn: -0.08, up: 0.08}}, 12: {error: {dn: -0.08, up: 0.08}}, 13: {error: {dn: -0.08, up: 0.08}}, 14: {error: {dn: -0.08, up: 0.08}}, 15: {error: {dn: -0.07, up: 0.07}}, 16: {error: {dn: -0.07, up: 0.07}}, 17: {error: {dn: -0.06, up: 0.06}}, 18: {error: {dn: -0.05, up: 0.05}}, 19: {error: {dn: -0.05, up: 0.05}}, 20: {error: {dn: -0.05, up: 0.05}}, 21: {error: {dn: -0.04, up: 0.04}}, 22: {error: {dn: -0.05, up: 0.05}}, 23: {error: {dn: -0.04, up: 0.04}}, 24: {error: {dn: -0.04, up: 0.04}}, 25: {error: {dn: -0.04, up: 0.04}}, 26: {error: {dn: -0.04, up: 0.04}}, 27: {error: {dn: -0.04, up: 0.04}}, 28: {error: {dn: -0.03, up: 0.03}}, 29: {error: {dn: -0.03, up: 0.03}}, 30: {error: {dn: -0.03, up: 0.03}}, 31: {error: {dn: -0.03, up: 0.03}}, 32: {error: {dn: -0.03, up: 0.03}}, 33: {error: {dn: -0.03, up: 0.03}}, 34: {error: {dn: -0.03, up: 0.03}}, 35: {error: {dn: -0.02, up: 0.02}}, 36: {error: {dn: -0.03, up: 0.03}}, 37: {error: {dn: -0.03, up: 0.03}}, 38: {error: {dn: -0.02, up: 0.02}}, 39: {error: {dn: -0.03, up: 0.03}}, 40: {error: {dn: -0.04, up: 0.04}}, 41: {error: {dn: -0.03, up: 0.03}}, 42: {error: {dn: -0.03, up: 0.03}}, 43: {error: {dn: -0.02, up: 0.02}}, 44: {error: {dn: -0.02, up: 0.02}}, 45: {error: {dn: -0.02, up: 0.02}}, 46: {error: {dn: -0.02, up: 0.02}}, 47: {error: {dn: -0.02, up: 0.02}}, 48: {error: {dn: -0.02, up: 0.02}}, 49: {error: {dn: -0.02, up: 0.02}}, 50: {error: {dn: -0.02, up: 0.02}}, 51: {error: {dn: -0.02, up: 0.02}}, 52: {error: {dn: -0.01, up: 0.01}}, 53: {error: {dn: -0.02, up: 0.02}}, 54: {error: {dn: -0.02, up: 0.02}}, 55: {error: {dn: -0.02, up: 0.02}}, 56: {error: {dn: -0.01, up: 0.01}}, 57: {error: {dn: -0.01, up: 0.01}}, 58: {error: {dn: -0.01, up: 0.01}}, 59: {error: {dn: -0.01, up: 0.01}}, 60: {error: {dn: -0.01, up: 0.01}}, 61: {error: {dn: -0.01, up: 0.01}}, 62: {error: {dn: -0.01, up: 0.01}}, 63: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2012_I892684/d06-x01-y01 +Title: doi:10.17182/hepdata.62222.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 4.000000e-02 4.000000e-02 +1.540000e+00 0.000000e+00 0.000000e+00 1.000000e-02 5.000000e-02 5.000000e-02 +1.580000e+00 0.000000e+00 0.000000e+00 0.000000e+00 5.000000e-02 5.000000e-02 +1.620000e+00 0.000000e+00 0.000000e+00 1.000000e-02 6.000000e-02 6.000000e-02 +1.660000e+00 0.000000e+00 0.000000e+00 1.400000e-01 8.000000e-02 8.000000e-02 +1.700000e+00 0.000000e+00 0.000000e+00 1.400000e-01 7.000000e-02 7.000000e-02 +1.740000e+00 0.000000e+00 0.000000e+00 3.500000e-01 7.000000e-02 7.000000e-02 +1.780000e+00 0.000000e+00 0.000000e+00 5.900000e-01 8.000000e-02 8.000000e-02 +1.820000e+00 0.000000e+00 0.000000e+00 6.600000e-01 8.000000e-02 8.000000e-02 +1.860000e+00 0.000000e+00 0.000000e+00 4.800000e-01 8.000000e-02 8.000000e-02 +1.900000e+00 0.000000e+00 0.000000e+00 6.400000e-01 8.000000e-02 8.000000e-02 +1.940000e+00 0.000000e+00 0.000000e+00 5.400000e-01 8.000000e-02 8.000000e-02 +1.980000e+00 0.000000e+00 0.000000e+00 7.400000e-01 8.000000e-02 8.000000e-02 +2.020000e+00 0.000000e+00 0.000000e+00 8.400000e-01 8.000000e-02 8.000000e-02 +2.060000e+00 0.000000e+00 0.000000e+00 6.300000e-01 8.000000e-02 8.000000e-02 +2.100000e+00 0.000000e+00 0.000000e+00 7.800000e-01 7.000000e-02 7.000000e-02 +2.140000e+00 0.000000e+00 0.000000e+00 6.500000e-01 7.000000e-02 7.000000e-02 +2.180000e+00 0.000000e+00 0.000000e+00 6.500000e-01 6.000000e-02 6.000000e-02 +2.220000e+00 0.000000e+00 0.000000e+00 4.700000e-01 5.000000e-02 5.000000e-02 +2.260000e+00 0.000000e+00 0.000000e+00 3.700000e-01 5.000000e-02 5.000000e-02 +2.300000e+00 0.000000e+00 0.000000e+00 3.800000e-01 5.000000e-02 5.000000e-02 +2.340000e+00 0.000000e+00 0.000000e+00 2.600000e-01 4.000000e-02 4.000000e-02 +2.380000e+00 0.000000e+00 0.000000e+00 2.600000e-01 5.000000e-02 5.000000e-02 +2.420000e+00 0.000000e+00 0.000000e+00 3.200000e-01 4.000000e-02 4.000000e-02 +2.460000e+00 0.000000e+00 0.000000e+00 2.600000e-01 4.000000e-02 4.000000e-02 +2.500000e+00 0.000000e+00 0.000000e+00 2.100000e-01 4.000000e-02 4.000000e-02 +2.540000e+00 0.000000e+00 0.000000e+00 2.100000e-01 4.000000e-02 4.000000e-02 +2.580000e+00 0.000000e+00 0.000000e+00 1.700000e-01 4.000000e-02 4.000000e-02 +2.620000e+00 0.000000e+00 0.000000e+00 1.500000e-01 3.000000e-02 3.000000e-02 +2.660000e+00 0.000000e+00 0.000000e+00 1.900000e-01 3.000000e-02 3.000000e-02 +2.700000e+00 0.000000e+00 0.000000e+00 1.400000e-01 3.000000e-02 3.000000e-02 +2.740000e+00 0.000000e+00 0.000000e+00 2.000000e-01 3.000000e-02 3.000000e-02 +2.780000e+00 0.000000e+00 0.000000e+00 1.900000e-01 3.000000e-02 3.000000e-02 +2.820000e+00 0.000000e+00 0.000000e+00 1.100000e-01 3.000000e-02 3.000000e-02 +2.860000e+00 0.000000e+00 0.000000e+00 9.000000e-02 3.000000e-02 3.000000e-02 +2.900000e+00 0.000000e+00 0.000000e+00 9.000000e-02 2.000000e-02 2.000000e-02 +2.940000e+00 0.000000e+00 0.000000e+00 9.000000e-02 3.000000e-02 3.000000e-02 +2.980000e+00 0.000000e+00 0.000000e+00 1.000000e-01 3.000000e-02 3.000000e-02 +3.020000e+00 0.000000e+00 0.000000e+00 1.200000e-01 2.000000e-02 2.000000e-02 +3.060000e+00 0.000000e+00 0.000000e+00 1.800000e-01 3.000000e-02 3.000000e-02 +3.100000e+00 0.000000e+00 0.000000e+00 7.100000e-01 4.000000e-02 4.000000e-02 +3.140000e+00 0.000000e+00 0.000000e+00 1.200000e-01 3.000000e-02 3.000000e-02 +3.180000e+00 0.000000e+00 0.000000e+00 6.000000e-02 3.000000e-02 3.000000e-02 +3.220000e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.000000e-02 2.000000e-02 +3.260000e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.000000e-02 2.000000e-02 +3.300000e+00 0.000000e+00 0.000000e+00 1.000000e-01 2.000000e-02 2.000000e-02 +3.340000e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.000000e-02 2.000000e-02 +3.380000e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +3.420000e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.000000e-02 2.000000e-02 +3.460000e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.000000e-02 2.000000e-02 +3.500000e+00 0.000000e+00 0.000000e+00 2.000000e-02 2.000000e-02 2.000000e-02 +3.540000e+00 0.000000e+00 0.000000e+00 6.000000e-02 2.000000e-02 2.000000e-02 +3.580000e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +3.620000e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +3.660000e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +3.700000e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.000000e-02 2.000000e-02 +3.740000e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +3.780000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +3.820000e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +3.860000e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +3.900000e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +3.940000e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +3.980000e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +4.020000e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2012_I892684/d07-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.07, up: 0.07}}, 1: {error: {dn: -0.06, up: 0.06}}, 2: {error: {dn: -0.09, up: 0.09}}, 3: {error: {dn: -0.11, up: 0.11}}, 4: {error: {dn: -0.08, up: 0.08}}, 5: {error: {dn: -0.11, up: 0.11}}, 6: {error: {dn: -0.11, up: 0.11}}, 7: {error: {dn: -0.1, up: 0.1}}, 8: {error: {dn: -0.05, up: 0.05}}, 9: {error: {dn: -0.05, up: 0.05}}, 10: {error: {dn: -0.06, up: 0.06}}, 11: {error: {dn: -0.03, up: 0.03}}, 12: {error: {dn: -0.03, up: 0.03}}, 13: {error: {dn: -0.01, up: 0.01}}, 14: {error: {dn: -0.01, up: 0.01}}, 15: {error: {dn: -0.01, up: 0.01}}, 16: {error: {dn: -0.01, up: 0.01}}, 17: {error: {dn: -0.01, up: 0.01}}, 18: {error: {dn: -0.0, up: 0.0}}} + +IsRef: 1 +Path: /REF/BABAR_2012_I892684/d07-x01-y01 +Title: doi:10.17182/hepdata.62222.v1/t7 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.900000e+00 0.000000e+00 0.000000e+00 1.500000e-01 7.000000e-02 7.000000e-02 +1.940000e+00 0.000000e+00 0.000000e+00 1.400000e-01 6.000000e-02 6.000000e-02 +1.980000e+00 0.000000e+00 0.000000e+00 1.900000e-01 9.000000e-02 9.000000e-02 +2.020000e+00 0.000000e+00 0.000000e+00 4.700000e-01 1.100000e-01 1.100000e-01 +2.060000e+00 0.000000e+00 0.000000e+00 2.200000e-01 8.000000e-02 8.000000e-02 +2.100000e+00 0.000000e+00 0.000000e+00 4.500000e-01 1.100000e-01 1.100000e-01 +2.140000e+00 0.000000e+00 0.000000e+00 4.700000e-01 1.100000e-01 1.100000e-01 +2.180000e+00 0.000000e+00 0.000000e+00 5.500000e-01 1.000000e-01 1.000000e-01 +2.220000e+00 0.000000e+00 0.000000e+00 1.100000e-01 5.000000e-02 5.000000e-02 +2.260000e+00 0.000000e+00 0.000000e+00 1.300000e-01 5.000000e-02 5.000000e-02 +2.320000e+00 0.000000e+00 0.000000e+00 1.200000e-01 6.000000e-02 6.000000e-02 +2.400000e+00 0.000000e+00 0.000000e+00 1.400000e-01 3.000000e-02 3.000000e-02 +2.480000e+00 0.000000e+00 0.000000e+00 1.200000e-01 3.000000e-02 3.000000e-02 +2.600000e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +2.760000e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +2.920000e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +3.080000e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.000000e-02 1.000000e-02 +3.240000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +3.400000e+00 0.000000e+00 0.000000e+00 1.000000e-02 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2012_I892684/d08-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.002, up: 0.002}}, 1: {error: {dn: -0.004, up: 0.004}}, 2: {error: {dn: -0.005, up: 0.005}}, 3: {error: {dn: -0.007, up: 0.007}}, 4: {error: {dn: -0.01, up: 0.01}}, 5: {error: {dn: -0.01, up: 0.01}}, 6: {error: {dn: -0.01, up: 0.01}}, 7: {error: {dn: -0.012, up: 0.012}}, 8: {error: {dn: -0.013, up: 0.013}}, 9: {error: {dn: -0.016, up: 0.016}}, 10: {error: {dn: -0.014, up: 0.014}}, 11: {error: {dn: -0.015, up: 0.015}}, 12: {error: {dn: -0.016, up: 0.016}}, 13: {error: {dn: -0.014, up: 0.014}}, 14: {error: {dn: -0.014, up: 0.014}}, 15: {error: {dn: -0.015, up: 0.015}}, 16: {error: {dn: -0.016, up: 0.016}}, 17: {error: {dn: -0.014, up: 0.014}}, 18: {error: {dn: -0.016, up: 0.016}}, 19: {error: {dn: -0.015, up: 0.015}}, 20: {error: {dn: -0.016, up: 0.016}}, 21: {error: {dn: -0.014, up: 0.014}}, 22: {error: {dn: -0.015, up: 0.015}}, 23: {error: {dn: -0.015, up: 0.015}}, 24: {error: {dn: -0.013, up: 0.013}}, 25: {error: {dn: -0.016, up: 0.016}}, 26: {error: {dn: -0.013, up: 0.013}}, 27: {error: {dn: -0.014, up: 0.014}}, 28: {error: {dn: -0.013, up: 0.013}}, 29: {error: {dn: -0.012, up: 0.012}}, 30: {error: {dn: -0.012, up: 0.012}}, 31: {error: {dn: -0.014, up: 0.014}}, 32: {error: {dn: -0.012, up: 0.012}}, 33: {error: {dn: -0.012, up: 0.012}}, 34: {error: {dn: -0.011, up: 0.011}}, 35: {error: {dn: -0.011, up: 0.011}}, 36: {error: {dn: -0.013, up: 0.013}}, 37: {error: {dn: -0.011, up: 0.011}}, 38: {error: {dn: -0.01, up: 0.01}}, 39: {error: {dn: -0.01, up: 0.01}}, 40: {error: {dn: -0.01, up: 0.01}}, 41: {error: {dn: -0.01, up: 0.01}}, 42: {error: {dn: -0.01, up: 0.01}}, 43: {error: {dn: -0.023, up: 0.023}}, 44: {error: {dn: -0.017, up: 0.017}}, 45: {error: {dn: -0.01, up: 0.01}}, 46: {error: {dn: -0.01, up: 0.01}}, 47: {error: {dn: -0.01, up: 0.01}}, 48: {error: {dn: -0.009, up: 0.009}}, 49: {error: {dn: -0.009, up: 0.009}}, 50: {error: {dn: -0.008, up: 0.008}}, 51: {error: {dn: -0.009, up: 0.009}}, 52: {error: {dn: -0.008, up: 0.008}}, 53: {error: {dn: -0.008, up: 0.008}}, 54: {error: {dn: -0.008, up: 0.008}}, 55: {error: {dn: -0.009, up: 0.009}}, 56: {error: {dn: -0.009, up: 0.009}}, 57: {error: {dn: -0.008, up: 0.008}}, 58: {error: {dn: -0.008, up: 0.008}}, 59: {error: {dn: -0.007, up: 0.007}}, 60: {error: {dn: -0.007, up: 0.007}}, 61: {error: {dn: -0.008, up: 0.008}}, 62: {error: {dn: -0.008, up: 0.008}}, 63: {error: {dn: -0.007, up: 0.007}}, 64: {error: {dn: -0.006, up: 0.006}}, 65: {error: {dn: -0.007, up: 0.007}}, 66: {error: {dn: -0.007, up: 0.007}}, 67: {error: {dn: -0.008, up: 0.008}}, 68: {error: {dn: -0.006, up: 0.006}}, 69: {error: {dn: -0.006, up: 0.006}}, 70: {error: {dn: -0.006, up: 0.006}}, 71: {error: {dn: -0.007, up: 0.007}}, 72: {error: {dn: -0.006, up: 0.006}}, 73: {error: {dn: -0.005, up: 0.005}}, 74: {error: {dn: -0.006, up: 0.006}}, 75: {error: {dn: -0.005, up: 0.005}}, 76: {error: {dn: -0.005, up: 0.005}}, 77: {error: {dn: -0.005, up: 0.005}}, 78: {error: {dn: -0.006, up: 0.006}}, 79: {error: {dn: -0.005, up: 0.005}}, 80: {error: {dn: -0.005, up: 0.005}}, 81: {error: {dn: -0.005, up: 0.005}}, 82: {error: {dn: -0.004, up: 0.004}}, 83: {error: {dn: -0.005, up: 0.005}}, 84: {error: {dn: -0.004, up: 0.004}}, 85: {error: {dn: -0.005, up: 0.005}}, 86: {error: {dn: -0.004, up: 0.004}}, 87: {error: {dn: -0.005, up: 0.005}}, 88: {error: {dn: -0.004, up: 0.004}}, 89: {error: {dn: -0.005, up: 0.005}}, 90: {error: {dn: -0.003, up: 0.003}}, 91: {error: {dn: -0.005, up: 0.005}}, 92: {error: {dn: -0.004, up: 0.004}}, 93: {error: {dn: -0.004, up: 0.004}}, 94: {error: {dn: -0.004, up: 0.004}}, 95: {error: {dn: -0.004, up: 0.004}}, 96: {error: {dn: -0.004, up: 0.004}}, 97: {error: {dn: -0.004, up: 0.004}}, 98: {error: {dn: -0.004, up: 0.004}}, 99: {error: {dn: -0.003, up: 0.003}}} + +IsRef: 1 +Path: /REF/BABAR_2012_I892684/d08-x01-y01 +Title: doi:10.17182/hepdata.62222.v1/t8 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.012500e+00 0.000000e+00 0.000000e+00 2.000000e-03 2.000000e-03 2.000000e-03 +2.037500e+00 0.000000e+00 0.000000e+00 3.000000e-03 4.000000e-03 4.000000e-03 +2.062500e+00 0.000000e+00 0.000000e+00 1.300000e-02 5.000000e-03 5.000000e-03 +2.087500e+00 0.000000e+00 0.000000e+00 2.100000e-02 7.000000e-03 7.000000e-03 +2.112500e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +2.137500e+00 0.000000e+00 0.000000e+00 4.600000e-02 1.000000e-02 1.000000e-02 +2.162500e+00 0.000000e+00 0.000000e+00 2.100000e-02 1.000000e-02 1.000000e-02 +2.187500e+00 0.000000e+00 0.000000e+00 5.700000e-02 1.200000e-02 1.200000e-02 +2.212500e+00 0.000000e+00 0.000000e+00 6.600000e-02 1.300000e-02 1.300000e-02 +2.237500e+00 0.000000e+00 0.000000e+00 1.120000e-01 1.600000e-02 1.600000e-02 +2.262500e+00 0.000000e+00 0.000000e+00 8.600000e-02 1.400000e-02 1.400000e-02 +2.287500e+00 0.000000e+00 0.000000e+00 6.300000e-02 1.500000e-02 1.500000e-02 +2.312500e+00 0.000000e+00 0.000000e+00 8.300000e-02 1.600000e-02 1.600000e-02 +2.337500e+00 0.000000e+00 0.000000e+00 6.000000e-02 1.400000e-02 1.400000e-02 +2.362500e+00 0.000000e+00 0.000000e+00 7.000000e-02 1.400000e-02 1.400000e-02 +2.387500e+00 0.000000e+00 0.000000e+00 8.300000e-02 1.500000e-02 1.500000e-02 +2.412500e+00 0.000000e+00 0.000000e+00 8.700000e-02 1.600000e-02 1.600000e-02 +2.437500e+00 0.000000e+00 0.000000e+00 7.100000e-02 1.400000e-02 1.400000e-02 +2.462500e+00 0.000000e+00 0.000000e+00 7.900000e-02 1.600000e-02 1.600000e-02 +2.487500e+00 0.000000e+00 0.000000e+00 8.000000e-02 1.500000e-02 1.500000e-02 +2.512500e+00 0.000000e+00 0.000000e+00 9.300000e-02 1.600000e-02 1.600000e-02 +2.537500e+00 0.000000e+00 0.000000e+00 7.900000e-02 1.400000e-02 1.400000e-02 +2.562500e+00 0.000000e+00 0.000000e+00 8.600000e-02 1.500000e-02 1.500000e-02 +2.587500e+00 0.000000e+00 0.000000e+00 1.100000e-01 1.500000e-02 1.500000e-02 +2.612500e+00 0.000000e+00 0.000000e+00 7.700000e-02 1.300000e-02 1.300000e-02 +2.637500e+00 0.000000e+00 0.000000e+00 1.000000e-01 1.600000e-02 1.600000e-02 +2.662500e+00 0.000000e+00 0.000000e+00 8.300000e-02 1.300000e-02 1.300000e-02 +2.687500e+00 0.000000e+00 0.000000e+00 9.700000e-02 1.400000e-02 1.400000e-02 +2.712500e+00 0.000000e+00 0.000000e+00 9.400000e-02 1.300000e-02 1.300000e-02 +2.737500e+00 0.000000e+00 0.000000e+00 6.400000e-02 1.200000e-02 1.200000e-02 +2.762500e+00 0.000000e+00 0.000000e+00 6.100000e-02 1.200000e-02 1.200000e-02 +2.787500e+00 0.000000e+00 0.000000e+00 9.100000e-02 1.400000e-02 1.400000e-02 +2.812500e+00 0.000000e+00 0.000000e+00 7.400000e-02 1.200000e-02 1.200000e-02 +2.837500e+00 0.000000e+00 0.000000e+00 6.700000e-02 1.200000e-02 1.200000e-02 +2.862500e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.100000e-02 1.100000e-02 +2.887500e+00 0.000000e+00 0.000000e+00 5.400000e-02 1.100000e-02 1.100000e-02 +2.912500e+00 0.000000e+00 0.000000e+00 7.300000e-02 1.300000e-02 1.300000e-02 +2.937500e+00 0.000000e+00 0.000000e+00 4.200000e-02 1.100000e-02 1.100000e-02 +2.962500e+00 0.000000e+00 0.000000e+00 4.800000e-02 1.000000e-02 1.000000e-02 +2.987500e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.000000e-02 1.000000e-02 +3.012500e+00 0.000000e+00 0.000000e+00 6.200000e-02 1.000000e-02 1.000000e-02 +3.037500e+00 0.000000e+00 0.000000e+00 3.700000e-02 1.000000e-02 1.000000e-02 +3.062500e+00 0.000000e+00 0.000000e+00 5.700000e-02 1.000000e-02 1.000000e-02 +3.087500e+00 0.000000e+00 0.000000e+00 3.340000e-01 2.300000e-02 2.300000e-02 +3.112500e+00 0.000000e+00 0.000000e+00 1.510000e-01 1.700000e-02 1.700000e-02 +3.137500e+00 0.000000e+00 0.000000e+00 4.500000e-02 1.000000e-02 1.000000e-02 +3.162500e+00 0.000000e+00 0.000000e+00 5.300000e-02 1.000000e-02 1.000000e-02 +3.187500e+00 0.000000e+00 0.000000e+00 4.100000e-02 1.000000e-02 1.000000e-02 +3.212500e+00 0.000000e+00 0.000000e+00 5.100000e-02 9.000000e-03 9.000000e-03 +3.237500e+00 0.000000e+00 0.000000e+00 4.600000e-02 9.000000e-03 9.000000e-03 +3.262500e+00 0.000000e+00 0.000000e+00 3.500000e-02 8.000000e-03 8.000000e-03 +3.287500e+00 0.000000e+00 0.000000e+00 3.000000e-02 9.000000e-03 9.000000e-03 +3.312500e+00 0.000000e+00 0.000000e+00 2.700000e-02 8.000000e-03 8.000000e-03 +3.337500e+00 0.000000e+00 0.000000e+00 4.000000e-02 8.000000e-03 8.000000e-03 +3.362500e+00 0.000000e+00 0.000000e+00 3.200000e-02 8.000000e-03 8.000000e-03 +3.387500e+00 0.000000e+00 0.000000e+00 2.100000e-02 9.000000e-03 9.000000e-03 +3.412500e+00 0.000000e+00 0.000000e+00 3.700000e-02 9.000000e-03 9.000000e-03 +3.437500e+00 0.000000e+00 0.000000e+00 3.100000e-02 8.000000e-03 8.000000e-03 +3.462500e+00 0.000000e+00 0.000000e+00 3.500000e-02 8.000000e-03 8.000000e-03 +3.487500e+00 0.000000e+00 0.000000e+00 3.400000e-02 7.000000e-03 7.000000e-03 +3.512500e+00 0.000000e+00 0.000000e+00 2.500000e-02 7.000000e-03 7.000000e-03 +3.537500e+00 0.000000e+00 0.000000e+00 3.300000e-02 8.000000e-03 8.000000e-03 +3.562500e+00 0.000000e+00 0.000000e+00 3.500000e-02 8.000000e-03 8.000000e-03 +3.587500e+00 0.000000e+00 0.000000e+00 2.500000e-02 7.000000e-03 7.000000e-03 +3.612500e+00 0.000000e+00 0.000000e+00 8.000000e-03 6.000000e-03 6.000000e-03 +3.637500e+00 0.000000e+00 0.000000e+00 2.000000e-02 7.000000e-03 7.000000e-03 +3.662500e+00 0.000000e+00 0.000000e+00 3.100000e-02 7.000000e-03 7.000000e-03 +3.687500e+00 0.000000e+00 0.000000e+00 2.800000e-02 8.000000e-03 8.000000e-03 +3.712500e+00 0.000000e+00 0.000000e+00 2.300000e-02 6.000000e-03 6.000000e-03 +3.737500e+00 0.000000e+00 0.000000e+00 1.400000e-02 6.000000e-03 6.000000e-03 +3.762500e+00 0.000000e+00 0.000000e+00 2.600000e-02 6.000000e-03 6.000000e-03 +3.787500e+00 0.000000e+00 0.000000e+00 3.100000e-02 7.000000e-03 7.000000e-03 +3.812500e+00 0.000000e+00 0.000000e+00 2.100000e-02 6.000000e-03 6.000000e-03 +3.837500e+00 0.000000e+00 0.000000e+00 1.300000e-02 5.000000e-03 5.000000e-03 +3.862500e+00 0.000000e+00 0.000000e+00 1.800000e-02 6.000000e-03 6.000000e-03 +3.887500e+00 0.000000e+00 0.000000e+00 2.000000e-02 5.000000e-03 5.000000e-03 +3.912500e+00 0.000000e+00 0.000000e+00 1.100000e-02 5.000000e-03 5.000000e-03 +3.937500e+00 0.000000e+00 0.000000e+00 1.700000e-02 5.000000e-03 5.000000e-03 +3.962500e+00 0.000000e+00 0.000000e+00 2.300000e-02 6.000000e-03 6.000000e-03 +3.987500e+00 0.000000e+00 0.000000e+00 1.500000e-02 5.000000e-03 5.000000e-03 +4.012500e+00 0.000000e+00 0.000000e+00 1.200000e-02 5.000000e-03 5.000000e-03 +4.037500e+00 0.000000e+00 0.000000e+00 1.500000e-02 5.000000e-03 5.000000e-03 +4.062500e+00 0.000000e+00 0.000000e+00 1.200000e-02 4.000000e-03 4.000000e-03 +4.087500e+00 0.000000e+00 0.000000e+00 8.000000e-03 5.000000e-03 5.000000e-03 +4.112500e+00 0.000000e+00 0.000000e+00 8.000000e-03 4.000000e-03 4.000000e-03 +4.137500e+00 0.000000e+00 0.000000e+00 1.500000e-02 5.000000e-03 5.000000e-03 +4.162500e+00 0.000000e+00 0.000000e+00 1.000000e-02 4.000000e-03 4.000000e-03 +4.187500e+00 0.000000e+00 0.000000e+00 1.800000e-02 5.000000e-03 5.000000e-03 +4.212500e+00 0.000000e+00 0.000000e+00 3.000000e-03 4.000000e-03 4.000000e-03 +4.237500e+00 0.000000e+00 0.000000e+00 1.200000e-02 5.000000e-03 5.000000e-03 +4.262500e+00 0.000000e+00 0.000000e+00 4.000000e-03 3.000000e-03 3.000000e-03 +4.287500e+00 0.000000e+00 0.000000e+00 9.000000e-03 5.000000e-03 5.000000e-03 +4.312500e+00 0.000000e+00 0.000000e+00 3.000000e-03 4.000000e-03 4.000000e-03 +4.337500e+00 0.000000e+00 0.000000e+00 6.000000e-03 4.000000e-03 4.000000e-03 +4.362500e+00 0.000000e+00 0.000000e+00 9.000000e-03 4.000000e-03 4.000000e-03 +4.387500e+00 0.000000e+00 0.000000e+00 8.000000e-03 4.000000e-03 4.000000e-03 +4.412500e+00 0.000000e+00 0.000000e+00 1.000000e-03 4.000000e-03 4.000000e-03 +4.437500e+00 0.000000e+00 0.000000e+00 1.200000e-02 4.000000e-03 4.000000e-03 +4.462500e+00 0.000000e+00 0.000000e+00 1.000000e-02 4.000000e-03 4.000000e-03 +4.487500e+00 0.000000e+00 0.000000e+00 6.000000e-03 3.000000e-03 3.000000e-03 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/BABAR_2013_I1116411.cc b/analyses/pluginBABAR/BABAR_2013_I1116411.cc rename from analyses/pluginMisc/BABAR_2013_I1116411.cc rename to analyses/pluginBABAR/BABAR_2013_I1116411.cc diff --git a/analyses/pluginMisc/BABAR_2013_I1116411.info b/analyses/pluginBABAR/BABAR_2013_I1116411.info rename from analyses/pluginMisc/BABAR_2013_I1116411.info rename to analyses/pluginBABAR/BABAR_2013_I1116411.info diff --git a/analyses/pluginMisc/BABAR_2013_I1116411.plot b/analyses/pluginBABAR/BABAR_2013_I1116411.plot rename from analyses/pluginMisc/BABAR_2013_I1116411.plot rename to analyses/pluginBABAR/BABAR_2013_I1116411.plot diff --git a/analyses/pluginMisc/BABAR_2013_I1116411.yoda b/analyses/pluginBABAR/BABAR_2013_I1116411.yoda rename from analyses/pluginMisc/BABAR_2013_I1116411.yoda rename to analyses/pluginBABAR/BABAR_2013_I1116411.yoda diff --git a/analyses/pluginBABAR/BABAR_2013_I1217421.cc b/analyses/pluginBABAR/BABAR_2013_I1217421.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2013_I1217421.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2013_I1217421 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2013_I1217421); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nproton = bookCounter("TMP/proton"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PROTON) vetoEvent; + } + _nproton->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nproton->val(); + double error = _nproton->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nproton; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2013_I1217421); + + +} diff --git a/analyses/pluginBABAR/BABAR_2013_I1217421.info b/analyses/pluginBABAR/BABAR_2013_I1217421.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2013_I1217421.info @@ -0,0 +1,35 @@ +Name: BABAR_2013_I1217421 +Year: 2013 +Summary: Cross section for $e^+e^-\to$ proton and antiproton between 1.877 and 4.25 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 1217421 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- 'Phys.Rev. D87 (2013) 092005, 2013 ' +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ using radiative + return for energies between 1.877 and 4.25 GeV.' +BibKey: Lees:2013ebn +BibTeX: '@article{Lees:2013ebn, + author = "Lees, J. P. and others", + title = "{Study of $e^+e^- \to p \bar{p}$ via initial-state + radiation at BABAR}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D87", + year = "2013", + number = "9", + pages = "092005", + doi = "10.1103/PhysRevD.87.092005", + eprint = "1302.0055", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BABAR-PUB-12-030, SLAC-PUB-15324", + SLACcitation = "%%CITATION = ARXIV:1302.0055;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2013_I1217421.plot b/analyses/pluginBABAR/BABAR_2013_I1217421.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2013_I1217421.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BABAR_2013_I1217421/d01-x01-y01 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2013_I1217421.yoda b/analyses/pluginBABAR/BABAR_2013_I1217421.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2013_I1217421.yoda @@ -0,0 +1,96 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1217421/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -46.0, up: 46.0}, sys: {dn: -30.0, up: 30.0}}, 1: {stat: {dn: -50.0, up: 50.0}, sys: {dn: -32.0, up: 32.0}}, 2: {stat: {dn: -47.0, up: 47.0}, sys: {dn: -31.0, up: 31.0}}, 3: {stat: {dn: -46.0, up: 46.0}, sys: {dn: -30.0, up: 30.0}}, 4: {stat: {dn: -48.0, up: 48.0}, sys: {dn: -31.0, up: 31.0}}, 5: {stat: {dn: -48.0, up: 48.0}, sys: {dn: -30.0, up: 30.0}}, 6: {stat: {dn: -48.0, up: 48.0}, sys: {dn: -31.0, up: 31.0}}, 7: {stat: {dn: -45.0, up: 45.0}, sys: {dn: -28.0, up: 28.0}}, 8: {stat: {dn: -46.0, up: 46.0}, sys: {dn: -29.0, up: 29.0}}, 9: {stat: {dn: -45.0, up: 45.0}, sys: {dn: -29.0, up: 29.0}}, 10: {stat: {dn: -43.0, up: 43.0}, sys: {dn: -27.0, up: 27.0}}, 11: {stat: {dn: -41.0, up: 41.0}, sys: {dn: -24.0, up: 24.0}}, 12: {stat: {dn: -35.0, up: 35.0}, sys: {dn: -20.0, up: 20.0}}, 13: {stat: {dn: -33.0, up: 33.0}, sys: {dn: -19.0, up: 19.0}}, 14: {stat: {dn: -32.0, up: 32.0}, sys: {dn: -16.0, up: 16.0}}, 15: {stat: {dn: -27.0, up: 27.0}, sys: {dn: -13.0, up: 13.0}}, 16: {stat: {dn: -25.0, up: 25.0}, sys: {dn: -12.0, up: 12.0}}, 17: {stat: {dn: -14.0, up: 14.0}, sys: {dn: -12.0, up: 12.0}}, 18: {stat: {dn: -12.0, up: 12.0}, sys: {dn: -11.0, up: 11.0}}, 19: {stat: {dn: -12.0, up: 12.0}, sys: {dn: -6.0, up: 6.0}}, 20: {stat: {dn: -11.0, up: 11.0}, sys: {dn: -5.0, up: 5.0}}, 21: {stat: {dn: -10.0, up: 10.0}, sys: {dn: -4.0, up: 4.0}}, 22: {stat: {dn: -8.0, up: 8.0}, sys: {dn: -3.0, up: 3.0}}, 23: {stat: {dn: -8.0, up: 8.0}, sys: {dn: -3.0, up: 3.0}}, 24: {stat: {dn: -6.0, up: 6.0}, sys: {dn: -3.0, up: 3.0}}, 25: {stat: {dn: -7.0, up: 7.0}, sys: {dn: -3.0, up: 3.0}}, 26: {stat: {dn: -6.0, up: 6.0}, sys: {dn: -3.0, up: 3.0}}, 27: {stat: {dn: -5.0, up: 5.0}, sys: {dn: -1.0, up: 1.0}}, 28: {stat: {dn: -6.0, up: 6.0}, sys: {dn: -2.0, up: 2.0}}, 29: {stat: {dn: -5.0, up: 5.0}, sys: {dn: -2.0, up: 2.0}}, 30: {stat: {dn: -5.0, up: 5.0}, sys: {dn: -2.0, up: 2.0}}, 31: {stat: {dn: -2.0, up: 2.0}, sys: {dn: -1.6, up: 1.6}}, 32: {stat: {dn: -1.2, up: 1.2}, sys: {dn: -1.1, up: 1.1}}, 33: {stat: {dn: -0.6, up: 0.6}, sys: {dn: -0.3, up: 0.3}}, 34: {stat: {dn: -0.8, up: 0.8}, sys: {dn: -0.3, up: 0.3}}, 35: {stat: {dn: -0.4, up: 0.4}, sys: {dn: -0.2, up: 0.2}}, 36: {stat: {dn: -0.3, up: 0.3}, sys: {dn: -0.2, up: 0.2}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1217421/d01-x01-y01 +Title: doi:10.17182/hepdata.62678.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.888500e+00 1.150000e-02 1.150000e-02 8.060000e+02 5.491812e+01 5.491812e+01 +1.912500e+00 1.250000e-02 1.250000e-02 9.060000e+02 5.936329e+01 5.936329e+01 +1.937500e+00 1.250000e-02 1.250000e-02 8.450000e+02 5.630275e+01 5.630275e+01 +1.962500e+00 1.250000e-02 1.250000e-02 8.170000e+02 5.491812e+01 5.491812e+01 +1.987500e+00 1.250000e-02 1.250000e-02 8.540000e+02 5.714018e+01 5.714018e+01 +2.012500e+00 1.250000e-02 1.250000e-02 8.420000e+02 5.660389e+01 5.660389e+01 +2.037500e+00 1.250000e-02 1.250000e-02 8.460000e+02 5.714018e+01 5.714018e+01 +2.062500e+00 1.250000e-02 1.250000e-02 7.500000e+02 5.300000e+01 5.300000e+01 +2.087500e+00 1.250000e-02 1.250000e-02 7.960000e+02 5.437830e+01 5.437830e+01 +2.112500e+00 1.250000e-02 1.250000e-02 7.790000e+02 5.353504e+01 5.353504e+01 +2.137500e+00 1.250000e-02 1.250000e-02 6.660000e+02 5.077401e+01 5.077401e+01 +2.162500e+00 1.250000e-02 1.250000e-02 5.510000e+02 4.750789e+01 4.750789e+01 +2.187500e+00 1.250000e-02 1.250000e-02 4.290000e+02 4.031129e+01 4.031129e+01 +2.212500e+00 1.250000e-02 1.250000e-02 3.900000e+02 3.807887e+01 3.807887e+01 +2.237500e+00 1.250000e-02 1.250000e-02 3.790000e+02 3.577709e+01 3.577709e+01 +2.262500e+00 1.250000e-02 1.250000e-02 2.340000e+02 2.996665e+01 2.996665e+01 +2.287500e+00 1.250000e-02 1.250000e-02 2.010000e+02 2.773085e+01 2.773085e+01 +2.325000e+00 2.500000e-02 2.500000e-02 1.430000e+02 1.843909e+01 1.843909e+01 +2.375000e+00 2.500000e-02 2.500000e-02 1.050000e+02 1.627882e+01 1.627882e+01 +2.425000e+00 2.500000e-02 2.500000e-02 1.150000e+02 1.341641e+01 1.341641e+01 +2.475000e+00 2.500000e-02 2.500000e-02 1.010000e+02 1.208305e+01 1.208305e+01 +2.525000e+00 2.500000e-02 2.500000e-02 8.400000e+01 1.077033e+01 1.077033e+01 +2.575000e+00 2.500000e-02 2.500000e-02 5.500000e+01 8.544004e+00 8.544004e+00 +2.625000e+00 2.500000e-02 2.500000e-02 4.000000e+01 8.544004e+00 8.544004e+00 +2.675000e+00 2.500000e-02 2.500000e-02 2.800000e+01 6.708204e+00 6.708204e+00 +2.725000e+00 2.500000e-02 2.500000e-02 3.600000e+01 7.615773e+00 7.615773e+00 +2.775000e+00 2.500000e-02 2.500000e-02 2.900000e+01 6.708204e+00 6.708204e+00 +2.825000e+00 2.500000e-02 2.500000e-02 1.800000e+01 5.099020e+00 5.099020e+00 +2.875000e+00 2.500000e-02 2.500000e-02 2.700000e+01 6.324555e+00 6.324555e+00 +2.925000e+00 2.500000e-02 2.500000e-02 1.900000e+01 5.385165e+00 5.385165e+00 +2.975000e+00 2.500000e-02 2.500000e-02 2.000000e+01 5.385165e+00 5.385165e+00 +3.100000e+00 1.000000e-01 1.000000e-01 4.200000e+00 2.561250e+00 2.561250e+00 +3.300000e+00 1.000000e-01 1.000000e-01 5.400000e+00 1.627882e+00 1.627882e+00 +3.500000e+00 1.000000e-01 1.000000e-01 1.600000e+00 6.708204e-01 6.708204e-01 +3.700000e+00 1.000000e-01 1.000000e-01 1.900000e+00 8.544004e-01 8.544004e-01 +3.900000e+00 1.000000e-01 1.000000e-01 2.000000e-01 4.472136e-01 4.472136e-01 +4.125000e+00 1.250000e-01 1.250000e-01 3.000000e-01 3.605551e-01 3.605551e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1217421/d01-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.014, up: 0.014}}, 1: {error: {dn: -0.012, up: 0.012}}, 2: {error: {dn: -0.01, up: 0.01}}, 3: {error: {dn: -0.01, up: 0.01}}, 4: {error: {dn: -0.009, up: 0.009}}, 5: {error: {dn: -0.009, up: 0.009}}, 6: {error: {dn: -0.009, up: 0.009}}, 7: {error: {dn: -0.009, up: 0.009}}, 8: {error: {dn: -0.009, up: 0.009}}, 9: {error: {dn: -0.008, up: 0.008}}, 10: {error: {dn: -0.009, up: 0.009}}, 11: {error: {dn: -0.009, up: 0.009}}, 12: {error: {dn: -0.009, up: 0.009}}, 13: {error: {dn: -0.008, up: 0.008}}, 14: {error: {dn: -0.008, up: 0.008}}, 15: {error: {dn: -0.009, up: 0.009}}, 16: {error: {dn: -0.009, up: 0.009}}, 17: {error: {dn: -0.007, up: 0.007}}, 18: {error: {dn: -0.007, up: 0.007}}, 19: {error: {dn: -0.006, up: 0.006}}, 20: {error: {dn: -0.006, up: 0.006}}, 21: {error: {dn: -0.005, up: 0.005}}, 22: {error: {dn: -0.006, up: 0.006}}, 23: {error: {dn: -0.006, up: 0.006}}, 24: {error: {dn: -0.006, up: 0.006}}, 25: {error: {dn: -0.006, up: 0.006}}, 26: {error: {dn: -0.006, up: 0.006}}, 27: {error: {dn: -0.006, up: 0.006}}, 28: {error: {dn: -0.006, up: 0.006}}, 29: {error: {dn: -0.006, up: 0.006}}, 30: {error: {dn: -0.006, up: 0.006}}, 31: {error: {dn: -0.007, up: 0.007}}, 32: {error: {dn: -0.004, up: 0.004}}, 33: {error: {dn: -0.003, up: 0.003}}, 34: {error: {dn: -0.004, up: 0.004}}, 35: {error: {dn: -0.005, up: 0.005}}, 36: {error: {dn: -0.008, up: 0.004}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1217421/d01-x01-y02 +Title: doi:10.17182/hepdata.62678.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ 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9.000000e-03 9.000000e-03 +2.212500e+00 1.250000e-02 1.250000e-02 1.730000e-01 8.000000e-03 8.000000e-03 +2.237500e+00 1.250000e-02 1.250000e-02 1.710000e-01 8.000000e-03 8.000000e-03 +2.262500e+00 1.250000e-02 1.250000e-02 1.340000e-01 9.000000e-03 9.000000e-03 +2.287500e+00 1.250000e-02 1.250000e-02 1.250000e-01 9.000000e-03 9.000000e-03 +2.325000e+00 2.500000e-02 2.500000e-02 1.060000e-01 7.000000e-03 7.000000e-03 +2.375000e+00 2.500000e-02 2.500000e-02 9.100000e-02 7.000000e-03 7.000000e-03 +2.425000e+00 2.500000e-02 2.500000e-02 9.600000e-02 6.000000e-03 6.000000e-03 +2.475000e+00 2.500000e-02 2.500000e-02 9.100000e-02 6.000000e-03 6.000000e-03 +2.525000e+00 2.500000e-02 2.500000e-02 8.400000e-02 5.000000e-03 5.000000e-03 +2.575000e+00 2.500000e-02 2.500000e-02 6.900000e-02 6.000000e-03 6.000000e-03 +2.625000e+00 2.500000e-02 2.500000e-02 6.000000e-02 6.000000e-03 6.000000e-03 +2.675000e+00 2.500000e-02 2.500000e-02 5.000000e-02 6.000000e-03 6.000000e-03 +2.725000e+00 2.500000e-02 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b/analyses/pluginBABAR/BABAR_2013_I1238276.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2013_I1238276.cc @@ -0,0 +1,118 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/Beam.hh" +#include "Rivet/Projections/ChargedFinalState.hh" + +namespace Rivet { + + + /// @brief BaBar pion, kaon and proton production in the continuum + /// @author Peter Richardson + class BABAR_2013_I1238276 : public Analysis { + public: + + BABAR_2013_I1238276() + : Analysis("BABAR_2013_I1238276") + { } + + + void init() { + declare(Beam(), "Beams"); + declare(ChargedFinalState(), "FS"); + + _histPion_no_dec = bookHisto1D(1,1,1); + _histKaon_no_dec = bookHisto1D(1,1,2); + _histProton_no_dec = bookHisto1D(1,1,3); + _histPion_dec = bookHisto1D(2,1,1); + _histKaon_dec = bookHisto1D(2,1,2); + _histProton_dec = bookHisto1D(2,1,3); + } + + + void analyze(const Event& e) { + const double weight = e.weight(); + + // Loop through charged FS particles and look for charmed mesons/baryons + const ChargedFinalState& fs = apply(e, "FS"); + + const Beam beamproj = apply(e, "Beams"); + const ParticlePair& beams = beamproj.beams(); + const FourMomentum mom_tot = beams.first.momentum() + beams.second.momentum(); + const LorentzTransform cms_boost = LorentzTransform::mkFrameTransformFromBeta(mom_tot.betaVec()); + MSG_DEBUG("CMS Energy sqrt s = " << beamproj.sqrtS()); + + foreach (const Particle& p, fs.particles()) { + // check if prompt or not + ConstGenParticlePtr pmother = p.genParticle(); + ConstGenVertexPtr ivertex = pmother->production_vertex(); + bool prompt = true; + while (ivertex) { + vector inparts = HepMCUtils::particles(ivertex, Relatives::PARENTS); + int n_inparts = inparts.size(); + if (n_inparts < 1) break; + pmother = inparts[0]; // first mother particle + int mother_pid = abs(pmother->pdg_id()); + if (mother_pid==PID::K0S || mother_pid==PID::LAMBDA) { + prompt = false; + break; + } + else if (mother_pid<6) { + break; + } + ivertex = pmother->production_vertex(); + } + + // momentum in CMS frame + const double mom = cms_boost.transform(p.momentum()).vector3().mod(); + const int PdgId = p.abspid(); + MSG_DEBUG("pdgID = " << PdgId << " Momentum = " << mom); + switch (PdgId) { + case PID::PIPLUS: + if(prompt) _histPion_no_dec->fill(mom,weight); + _histPion_dec ->fill(mom,weight); + break; + case PID::KPLUS: + if(prompt) _histKaon_no_dec->fill(mom,weight); + _histKaon_dec ->fill(mom,weight); + break; + case PID::PROTON: + if(prompt) _histProton_no_dec->fill(mom,weight); + _histProton_dec ->fill(mom,weight); + default : + break; + } + } + } + + + void finalize() { + scale(_histPion_no_dec ,1./sumOfWeights()); + scale(_histKaon_no_dec ,1./sumOfWeights()); + scale(_histProton_no_dec,1./sumOfWeights()); + scale(_histPion_dec ,1./sumOfWeights()); + scale(_histKaon_dec ,1./sumOfWeights()); + scale(_histProton_dec ,1./sumOfWeights()); + } + + + private: + + //@{ + // Histograms for continuum data (sqrt(s) = 10.52 GeV) + // no K_S and Lambda decays + Histo1DPtr _histPion_no_dec; + Histo1DPtr _histKaon_no_dec; + Histo1DPtr _histProton_no_dec; + // including decays + Histo1DPtr _histPion_dec; + Histo1DPtr _histKaon_dec; + Histo1DPtr _histProton_dec; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2013_I1238276); + +} diff --git a/analyses/pluginMisc/BABAR_2013_I1238276.info b/analyses/pluginBABAR/BABAR_2013_I1238276.info rename from analyses/pluginMisc/BABAR_2013_I1238276.info rename to analyses/pluginBABAR/BABAR_2013_I1238276.info diff --git a/analyses/pluginMisc/BABAR_2013_I1238276.plot b/analyses/pluginBABAR/BABAR_2013_I1238276.plot rename from analyses/pluginMisc/BABAR_2013_I1238276.plot rename to analyses/pluginBABAR/BABAR_2013_I1238276.plot diff --git a/analyses/pluginBABAR/BABAR_2013_I1238276.yoda b/analyses/pluginBABAR/BABAR_2013_I1238276.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2013_I1238276.yoda @@ -0,0 +1,408 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.02, up: 0.02}, sys: {dn: -0.22, up: 0.22}, 'sys,normalization uncertainty': {dn: -0.078498, up: 0.078498}}, 1: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.21, up: 0.21}, 'sys,normalization uncertainty': {dn: -0.08085, up: 0.08085}}, 2: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.17, up: 0.17}, 'sys,normalization uncertainty': {dn: -0.07879199999999999, up: 0.07879199999999999}}, 3: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.14, up: 0.14}, 'sys,normalization uncertainty': {dn: -0.07369599999999998, up: 0.07369599999999998}}, 4: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.11, up: 0.11}, 'sys,normalization uncertainty': {dn: -0.067914, up: 0.067914}}, 5: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.1, up: 0.1}, 'sys,normalization uncertainty': {dn: -0.062328, up: 0.062328}}, 6: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.08, up: 0.08}, 'sys,normalization uncertainty': {dn: -0.056644, up: 0.056644}}, 7: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.07, up: 0.07}, 'sys,normalization uncertainty': {dn: -0.051058, up: 0.051058}}, 8: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.06, up: 0.06}, 'sys,normalization uncertainty': {dn: -0.045962, up: 0.045962}}, 9: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.05, up: 0.05}, 'sys,normalization uncertainty': {dn: -0.041257999999999996, up: 0.041257999999999996}}, 10: {stat: {dn: -0.005, up: 0.005}, sys: {dn: -0.048, up: 0.048}, 'sys,normalization uncertainty': {dn: -0.037053800000000005, up: 0.037053800000000005}}, 11: {stat: {dn: -0.004, up: 0.004}, sys: {dn: -0.043, up: 0.043}, 'sys,normalization uncertainty': {dn: -0.033339600000000004, up: 0.033339600000000004}}, 12: {stat: {dn: -0.004, up: 0.004}, sys: {dn: -0.039, up: 0.039}, 'sys,normalization uncertainty': {dn: -0.030037, up: 0.030037}}, 13: {stat: {dn: -0.004, up: 0.004}, sys: {dn: -0.035, up: 0.035}, 'sys,normalization uncertainty': {dn: -0.027097, up: 0.027097}}, 14: {stat: {dn: -0.003, up: 0.003}, sys: {dn: -0.032, up: 0.032}, 'sys,normalization uncertainty': {dn: -0.024451, up: 0.024451}}, 15: {stat: {dn: -0.003, up: 0.003}, sys: {dn: -0.03, up: 0.03}, 'sys,normalization uncertainty': {dn: -0.0221284, up: 0.0221284}}, 16: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.027, up: 0.027}, 'sys,normalization uncertainty': {dn: -0.0190904, up: 0.0190904}}, 17: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.023, up: 0.023}, 'sys,normalization uncertainty': {dn: -0.0157094, up: 0.0157094}}, 18: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.02, up: 0.02}, 'sys,normalization uncertainty': {dn: -0.0130536, up: 0.0130536}}, 19: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.018, up: 0.018}, 'sys,normalization uncertainty': {dn: -0.0108388, up: 0.0108388}}, 20: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.016, up: 0.016}, 'sys,normalization uncertainty': {dn: -0.009074800000000001, up: 0.009074800000000001}}, 21: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.014, up: 0.014}, 'sys,normalization uncertainty': {dn: -0.007644000000000001, up: 0.007644000000000001}}, 22: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.013, up: 0.013}, 'sys,normalization uncertainty': {dn: -0.0064582, up: 0.0064582}}, 23: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.012, up: 0.012}, 'sys,normalization uncertainty': {dn: -0.0054782, up: 0.0054782}}, 24: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.01, up: 0.01}, 'sys,normalization uncertainty': {dn: -0.004654999999999999, up: 0.004654999999999999}}, 25: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.009, up: 0.009}, 'sys,normalization uncertainty': {dn: -0.0039592, up: 0.0039592}}, 26: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.008, up: 0.008}, 'sys,normalization uncertainty': {dn: -0.0033614, up: 0.0033614}}, 27: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0028812, up: 0.0028812}}, 28: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0024598, up: 0.0024598}}, 29: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.0021168, up: 0.0021168}}, 30: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.005, up: 0.005}, 'sys,normalization uncertainty': {dn: -0.0018227999999999999, up: 0.0018227999999999999}}, 31: {stat: {dn: -0.0006, up: 0.0006}, sys: {dn: -0.0048, up: 0.0048}, 'sys,normalization uncertainty': {dn: -0.0015778, up: 0.0015778}}, 32: {stat: {dn: -0.0005, up: 0.0005}, sys: {dn: -0.0043, up: 0.0043}, 'sys,normalization uncertainty': {dn: -0.00136612, up: 0.00136612}}, 33: {stat: {dn: -0.0005, up: 0.0005}, sys: {dn: -0.0038, up: 0.0038}, 'sys,normalization uncertainty': {dn: -0.00118874, up: 0.00118874}}, 34: {stat: {dn: -0.0005, up: 0.0005}, sys: {dn: -0.0034, up: 0.0034}, 'sys,normalization uncertainty': {dn: -0.0010270400000000001, up: 0.0010270400000000001}}, 35: {stat: {dn: -0.0004, up: 0.0004}, sys: {dn: -0.003, up: 0.003}, 'sys,normalization uncertainty': {dn: -0.0008918, up: 0.0008918}}, 36: {stat: {dn: -0.0004, up: 0.0004}, sys: {dn: -0.0024, up: 0.0024}, 'sys,normalization uncertainty': {dn: -0.0006918799999999999, up: 0.0006918799999999999}}, 37: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0018, up: 0.0018}, 'sys,normalization uncertainty': {dn: -0.00048706000000000004, up: 0.00048706000000000004}}, 38: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0014, up: 0.0014}, 'sys,normalization uncertainty': {dn: -0.00034300000000000004, up: 0.00034300000000000004}}, 39: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.001, up: 0.001}, 'sys,normalization uncertainty': {dn: -0.00024108000000000002, up: 0.00024108000000000002}}, 40: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0008, up: 0.0008}, 'sys,normalization uncertainty': {dn: -0.00016366, up: 0.00016366}}, 41: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0005, up: 0.0005}, 'sys,normalization uncertainty': {dn: -0.00010486, up: 0.00010486}}, 42: {stat: {dn: -0.00017, up: 0.00017}, sys: {dn: -0.00036, up: 0.00036}, 'sys,normalization uncertainty': {dn: -6.6738e-05, up: 6.6738e-05}}, 43: {stat: {dn: -0.00015, up: 0.00015}, sys: {dn: -0.00024, up: 0.00024}, 'sys,normalization uncertainty': {dn: -4.0963999999999996e-05, up: 4.0963999999999996e-05}}, 44: {stat: {dn: -0.0001, up: 0.0001}, sys: {dn: -0.00011, up: 0.00011}, 'sys,normalization uncertainty': {dn: -1.4993999999999999e-05, up: 1.4993999999999999e-05}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1238276/d01-x01-y01 +Title: doi:10.17182/hepdata.62088.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.250000e-01 2.500000e-02 2.500000e-02 8.010000e+00 2.344396e-01 2.344396e-01 +2.750000e-01 2.500000e-02 2.500000e-02 8.250000e+00 2.252481e-01 2.252481e-01 +3.250000e-01 2.500000e-02 2.500000e-02 8.040000e+00 1.876384e-01 1.876384e-01 +3.750000e-01 2.500000e-02 2.500000e-02 7.520000e+00 1.585279e-01 1.585279e-01 +4.250000e-01 2.500000e-02 2.500000e-02 6.930000e+00 1.296623e-01 1.296623e-01 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sys: {dn: -0.008, up: 0.008}, 'sys,normalization uncertainty': {dn: -0.0062328, up: 0.0062328}}, 13: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.008, up: 0.008}, 'sys,normalization uncertainty': {dn: -0.006036799999999999, up: 0.006036799999999999}}, 14: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.008, up: 0.008}, 'sys,normalization uncertainty': {dn: -0.0058113999999999996, up: 0.0058113999999999996}}, 15: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.005566399999999999, up: 0.005566399999999999}}, 16: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.005203800000000001, up: 0.005203800000000001}}, 17: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.0047236, up: 0.0047236}}, 18: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.004262999999999999, up: 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15: {stat: {dn: -0.0008, up: 0.0008}, sys: {dn: -0.0041, up: 0.0041}, 'sys,normalization uncertainty': {dn: -0.0011122999999999999, up: 0.0011122999999999999}}, 16: {stat: {dn: -0.0007, up: 0.0007}, sys: {dn: -0.004, up: 0.004}, 'sys,normalization uncertainty': {dn: -0.00101234, up: 0.00101234}}, 17: {stat: {dn: -0.0006, up: 0.0006}, sys: {dn: -0.0038, up: 0.0038}, 'sys,normalization uncertainty': {dn: -0.00090062, up: 0.00090062}}, 18: {stat: {dn: -0.0006, up: 0.0006}, sys: {dn: -0.0035, up: 0.0035}, 'sys,normalization uncertainty': {dn: -0.0008065399999999999, up: 0.0008065399999999999}}, 19: {stat: {dn: -0.0005, up: 0.0005}, sys: {dn: -0.0032, up: 0.0032}, 'sys,normalization uncertainty': {dn: -0.0007193200000000001, up: 0.0007193200000000001}}, 20: {stat: {dn: -0.0005, up: 0.0005}, sys: {dn: -0.0029, up: 0.0029}, 'sys,normalization uncertainty': {dn: -0.0006418999999999999, up: 0.0006418999999999999}}, 21: {stat: {dn: -0.0005, up: 0.0005}, sys: {dn: -0.0026, up: 0.0026}, 'sys,normalization uncertainty': {dn: -0.00057624, up: 0.00057624}}, 22: {stat: {dn: -0.0004, up: 0.0004}, sys: {dn: -0.0023, up: 0.0023}, 'sys,normalization uncertainty': {dn: -0.00051548, up: 0.00051548}}, 23: {stat: {dn: -0.0004, up: 0.0004}, sys: {dn: -0.002, up: 0.002}, 'sys,normalization uncertainty': {dn: -0.00045668000000000005, up: 0.00045668000000000005}}, 24: {stat: {dn: -0.0004, up: 0.0004}, sys: {dn: -0.0017, up: 0.0017}, 'sys,normalization uncertainty': {dn: -0.00040767999999999995, up: 0.00040767999999999995}}, 25: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0015, up: 0.0015}, 'sys,normalization uncertainty': {dn: -0.00036652, up: 0.00036652}}, 26: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0013, up: 0.0013}, 'sys,normalization uncertainty': {dn: -0.00032438, up: 0.00032438}}, 27: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0012, up: 0.0012}, 'sys,normalization uncertainty': {dn: -0.00028714, up: 0.00028714}}, 28: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.001, up: 0.001}, 'sys,normalization uncertainty': {dn: -0.00025382, up: 0.00025382}}, 29: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0009, up: 0.0009}, 'sys,normalization uncertainty': {dn: -0.00022246, up: 0.00022246}}, 30: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0008, up: 0.0008}, 'sys,normalization uncertainty': {dn: -0.00019698, up: 0.00019698}}, 31: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0007, up: 0.0007}, 'sys,normalization uncertainty': {dn: -0.00017248000000000003, up: 0.00017248000000000003}}, 32: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0006, up: 0.0006}, 'sys,normalization uncertainty': {dn: -0.00015092, up: 0.00015092}}, 33: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0005, up: 0.0005}, 'sys,normalization uncertainty': {dn: -0.00013033999999999998, up: 0.00013033999999999998}}, 34: {stat: {dn: -0.00015, up: 0.00015}, sys: {dn: -0.00044, up: 0.00044}, 'sys,normalization uncertainty': {dn: -0.000112308, up: 0.000112308}}, 35: {stat: {dn: -0.00014, up: 0.00014}, sys: {dn: -0.00038, up: 0.00038}, 'sys,normalization uncertainty': {dn: -9.5942e-05, up: 9.5942e-05}}, 36: {stat: {dn: -0.00011, up: 0.00011}, sys: {dn: -0.00029, up: 0.00029}, 'sys,normalization uncertainty': {dn: -7.183399999999999e-05, up: 7.183399999999999e-05}}, 37: {stat: {dn: -9.0e-05, up: 9.0e-05}, sys: {dn: -0.00019, up: 0.00019}, 'sys,normalization uncertainty': {dn: -4.3904e-05, up: 4.3904e-05}}, 38: {stat: {dn: -7.0e-05, up: 7.0e-05}, sys: {dn: -0.00012, up: 0.00012}, 'sys,normalization uncertainty': {dn: -2.5479999999999997e-05, up: 2.5479999999999997e-05}}, 39: {stat: {dn: -5.0e-05, up: 5.0e-05}, sys: {dn: -8.0e-05, up: 8.0e-05}, 'sys,normalization uncertainty': {dn: -1.4014e-05, up: 1.4014e-05}}, 40: {stat: {dn: -4.0e-05, up: 4.0e-05}, sys: {dn: -5.0e-05, up: 5.0e-05}, 'sys,normalization uncertainty': {dn: -7.154e-06, up: 7.154e-06}}, 41: {stat: {dn: -3.0e-05, up: 3.0e-05}, sys: {dn: -3.0e-05, up: 3.0e-05}, 'sys,normalization uncertainty': {dn: -3.5280000000000004e-06, up: 3.5280000000000004e-06}}, 42: {stat: {dn: -2.0e-05, up: 2.0e-05}, sys: {dn: -2.0e-05, up: 2.0e-05}, 'sys,normalization uncertainty': {dn: -1.666e-06, up: 1.666e-06}}, 43: {stat: {dn: -2.0e-05, up: 2.0e-05}, sys: {dn: -1.0e-05, up: 1.0e-05}, 'sys,normalization uncertainty': {dn: -6.86e-07, up: 6.86e-07}}, 44: {stat: {dn: -1.0e-05, up: 1.0e-05}, sys: {dn: -1.0e-05, up: 1.0e-05}, 'sys,normalization uncertainty': {dn: -9.8e-08, up: 9.8e-08}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1238276/d01-x01-y03 +Title: doi:10.17182/hepdata.62088.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.250000e-01 2.500000e-02 2.500000e-02 4.790000e-02 3.836712e-03 3.836712e-03 +2.750000e-01 2.500000e-02 2.500000e-02 6.720000e-02 4.358176e-03 4.358176e-03 +3.250000e-01 2.500000e-02 2.500000e-02 8.790000e-02 4.951974e-03 4.951974e-03 +3.750000e-01 2.500000e-02 2.500000e-02 1.046000e-01 5.243166e-03 5.243166e-03 +4.250000e-01 2.500000e-02 2.500000e-02 1.167000e-01 5.341157e-03 5.341157e-03 +4.750000e-01 2.500000e-02 2.500000e-02 1.237000e-01 5.071447e-03 5.071447e-03 +5.250000e-01 2.500000e-02 2.500000e-02 1.296000e-01 4.781538e-03 4.781538e-03 +5.750000e-01 2.500000e-02 2.500000e-02 1.356000e-01 4.777648e-03 4.777648e-03 +6.250000e-01 2.500000e-02 2.500000e-02 1.380000e-01 4.690308e-03 4.690308e-03 +6.750000e-01 2.500000e-02 2.500000e-02 1.384000e-01 4.879509e-03 4.879509e-03 +7.250000e-01 2.500000e-02 2.500000e-02 1.363000e-01 4.779561e-03 4.779561e-03 +7.750000e-01 2.500000e-02 2.500000e-02 1.331000e-01 4.770892e-03 4.770892e-03 +8.250000e-01 2.500000e-02 2.500000e-02 1.292000e-01 4.647920e-03 4.647920e-03 +8.750000e-01 2.500000e-02 2.500000e-02 1.256000e-01 4.543684e-03 4.543684e-03 +9.250000e-01 2.500000e-02 2.500000e-02 1.200000e-01 4.434295e-03 4.434295e-03 +9.750000e-01 2.500000e-02 2.500000e-02 1.135000e-01 4.322871e-03 4.322871e-03 +1.050000e+00 5.000000e-02 5.000000e-02 1.033000e-01 4.185073e-03 4.185073e-03 +1.150000e+00 5.000000e-02 5.000000e-02 9.190000e-02 3.951091e-03 3.951091e-03 +1.250000e+00 5.000000e-02 5.000000e-02 8.230000e-02 3.641498e-03 3.641498e-03 +1.350000e+00 5.000000e-02 5.000000e-02 7.340000e-02 3.317743e-03 3.317743e-03 +1.450000e+00 5.000000e-02 5.000000e-02 6.550000e-02 3.011982e-03 3.011982e-03 +1.550000e+00 5.000000e-02 5.000000e-02 5.880000e-02 2.709622e-03 2.709622e-03 +1.650000e+00 5.000000e-02 5.000000e-02 5.260000e-02 2.390757e-03 2.390757e-03 +1.750000e+00 5.000000e-02 5.000000e-02 4.660000e-02 2.090109e-03 2.090109e-03 +1.850000e+00 5.000000e-02 5.000000e-02 4.160000e-02 1.793378e-03 1.793378e-03 +1.950000e+00 5.000000e-02 5.000000e-02 3.740000e-02 1.573003e-03 1.573003e-03 +2.050000e+00 5.000000e-02 5.000000e-02 3.310000e-02 1.373034e-03 1.373034e-03 +2.150000e+00 5.000000e-02 5.000000e-02 2.930000e-02 1.269823e-03 1.269823e-03 +2.250000e+00 5.000000e-02 5.000000e-02 2.590000e-02 1.074442e-03 1.074442e-03 +2.350000e+00 5.000000e-02 5.000000e-02 2.270000e-02 9.484137e-04 9.484137e-04 +2.450000e+00 5.000000e-02 5.000000e-02 2.010000e-02 8.478214e-04 8.478214e-04 +2.550000e+00 5.000000e-02 5.000000e-02 1.760000e-02 7.481640e-04 7.481640e-04 +2.650000e+00 5.000000e-02 5.000000e-02 1.540000e-02 6.502129e-04 6.502129e-04 +2.750000e+00 5.000000e-02 5.000000e-02 1.330000e-02 5.540654e-04 5.540654e-04 +2.850000e+00 5.000000e-02 5.000000e-02 1.146000e-02 4.782396e-04 4.782396e-04 +2.950000e+00 5.000000e-02 5.000000e-02 9.790000e-03 4.161789e-04 4.161789e-04 +3.125000e+00 1.250000e-01 1.250000e-01 7.330000e-03 3.183710e-04 3.183710e-04 +3.375000e+00 1.250000e-01 1.250000e-01 4.480000e-03 2.147733e-04 2.147733e-04 +3.625000e+00 1.250000e-01 1.250000e-01 2.600000e-03 1.412417e-04 1.412417e-04 +3.875000e+00 1.250000e-01 1.250000e-01 1.430000e-03 9.537501e-05 9.537501e-05 +4.125000e+00 1.250000e-01 1.250000e-01 7.300000e-04 6.442965e-05 6.442965e-05 +4.375000e+00 1.250000e-01 1.250000e-01 3.600000e-04 4.257284e-05 4.257284e-05 +4.625000e+00 1.250000e-01 1.250000e-01 1.700000e-04 2.833329e-05 2.833329e-05 +4.875000e+00 1.250000e-01 1.250000e-01 7.000000e-05 2.237120e-05 2.237120e-05 +5.135000e+00 1.350000e-01 1.350000e-01 1.000000e-05 1.414248e-05 1.414248e-05 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.02, up: 0.02}, sys: {dn: -0.24, up: 0.24}, 'sys,normalization uncertainty': {dn: -0.09065, up: 0.09065}}, 1: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.23, up: 0.23}, 'sys,normalization uncertainty': {dn: -0.09260999999999998, up: 0.09260999999999998}}, 2: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.2, up: 0.2}, 'sys,normalization uncertainty': {dn: -0.08957200000000001, up: 0.08957200000000001}}, 3: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.16, up: 0.16}, 'sys,normalization uncertainty': {dn: -0.083398, up: 0.083398}}, 4: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.14, up: 0.14}, 'sys,normalization uncertainty': {dn: -0.07663600000000001, up: 0.07663600000000001}}, 5: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.11, up: 0.11}, 'sys,normalization uncertainty': {dn: -0.07007000000000001, up: 0.07007000000000001}}, 6: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.1, up: 0.1}, 'sys,normalization uncertainty': {dn: -0.06340599999999999, up: 0.06340599999999999}}, 7: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.08, up: 0.08}, 'sys,normalization uncertainty': {dn: -0.057134, up: 0.057134}}, 8: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.07, up: 0.07}, 'sys,normalization uncertainty': {dn: -0.05125400000000001, up: 0.05125400000000001}}, 9: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.06, up: 0.06}, 'sys,normalization uncertainty': {dn: -0.045962, up: 0.045962}}, 10: {stat: {dn: -0.01, up: 0.01}, sys: {dn: -0.05, up: 0.05}, 'sys,normalization uncertainty': {dn: -0.041257999999999996, up: 0.041257999999999996}}, 11: {stat: {dn: -0.004, up: 0.004}, sys: {dn: -0.049, up: 0.049}, 'sys,normalization uncertainty': {dn: -0.0370244, up: 0.0370244}}, 12: {stat: {dn: -0.004, up: 0.004}, sys: {dn: -0.044, up: 0.044}, 'sys,normalization uncertainty': {dn: -0.0333298, up: 0.0333298}}, 13: {stat: {dn: -0.004, up: 0.004}, sys: {dn: -0.041, up: 0.041}, 'sys,normalization uncertainty': {dn: -0.030056600000000003, up: 0.030056600000000003}}, 14: {stat: {dn: -0.003, up: 0.003}, sys: {dn: -0.038, up: 0.038}, 'sys,normalization uncertainty': {dn: -0.027126399999999995, up: 0.027126399999999995}}, 15: {stat: {dn: -0.003, up: 0.003}, sys: {dn: -0.035, up: 0.035}, 'sys,normalization uncertainty': {dn: -0.0245392, up: 0.0245392}}, 16: {stat: {dn: -0.003, up: 0.003}, sys: {dn: -0.031, up: 0.031}, 'sys,normalization uncertainty': {dn: -0.0211582, up: 0.0211582}}, 17: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.027, up: 0.027}, 'sys,normalization uncertainty': {dn: -0.017394999999999997, up: 0.017394999999999997}}, 18: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.024, up: 0.024}, 'sys,normalization uncertainty': {dn: -0.0144256, up: 0.0144256}}, 19: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.021, up: 0.021}, 'sys,normalization uncertainty': {dn: -0.0119658, up: 0.0119658}}, 20: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.018, up: 0.018}, 'sys,normalization uncertainty': {dn: -0.009996, up: 0.009996}}, 21: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.016, up: 0.016}, 'sys,normalization uncertainty': {dn: -0.008398599999999999, up: 0.008398599999999999}}, 22: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.015, up: 0.015}, 'sys,normalization uncertainty': {dn: -0.0070853999999999995, up: 0.0070853999999999995}}, 23: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.013, up: 0.013}, 'sys,normalization uncertainty': {dn: -0.0059878, up: 0.0059878}}, 24: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.012, up: 0.012}, 'sys,normalization uncertainty': {dn: -0.005076400000000001, up: 0.005076400000000001}}, 25: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.011, up: 0.011}, 'sys,normalization uncertainty': {dn: -0.0043022, up: 0.0043022}}, 26: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.009, up: 0.009}, 'sys,normalization uncertainty': {dn: -0.0036455999999999997, up: 0.0036455999999999997}}, 27: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.008, up: 0.008}, 'sys,normalization uncertainty': {dn: -0.0031066, up: 0.0031066}}, 28: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.008, up: 0.008}, 'sys,normalization uncertainty': {dn: -0.002646, up: 0.002646}}, 29: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0022638, up: 0.0022638}}, 30: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.0019404, up: 0.0019404}}, 31: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.005, up: 0.005}, 'sys,normalization uncertainty': {dn: -0.0016660000000000002, up: 0.0016660000000000002}}, 32: {stat: {dn: -0.0006, up: 0.0006}, sys: {dn: -0.0048, up: 0.0048}, 'sys,normalization uncertainty': {dn: -0.00144158, up: 0.00144158}}, 33: {stat: {dn: -0.0005, up: 0.0005}, sys: {dn: -0.0042, up: 0.0042}, 'sys,normalization uncertainty': {dn: -0.00125048, up: 0.00125048}}, 34: {stat: {dn: -0.0005, up: 0.0005}, sys: {dn: -0.0037, up: 0.0037}, 'sys,normalization uncertainty': {dn: -0.00107702, up: 0.00107702}}, 35: {stat: {dn: -0.0004, up: 0.0004}, sys: {dn: -0.0033, up: 0.0033}, 'sys,normalization uncertainty': {dn: -0.000931, up: 0.000931}}, 36: {stat: {dn: -0.0004, up: 0.0004}, sys: {dn: -0.0026, up: 0.0026}, 'sys,normalization uncertainty': {dn: -0.0007193200000000001, up: 0.0007193200000000001}}, 37: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0019, up: 0.0019}, 'sys,normalization uncertainty': {dn: -0.00050274, up: 0.00050274}}, 38: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0014, up: 0.0014}, 'sys,normalization uncertainty': {dn: -0.00035182, up: 0.00035182}}, 39: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0011, up: 0.0011}, 'sys,normalization uncertainty': {dn: -0.00024598, up: 0.00024598}}, 40: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0008, up: 0.0008}, 'sys,normalization uncertainty': {dn: -0.00016561999999999998, up: 0.00016561999999999998}}, 41: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0005, up: 0.0005}, 'sys,normalization uncertainty': {dn: -0.00010584, up: 0.00010584}}, 42: {stat: {dn: -0.00017, up: 0.00017}, sys: {dn: -0.00036, up: 0.00036}, 'sys,normalization uncertainty': {dn: -6.6836e-05, up: 6.6836e-05}}, 43: {stat: {dn: -0.00015, up: 0.00015}, sys: {dn: -0.00024, up: 0.00024}, 'sys,normalization uncertainty': {dn: -4.0963999999999996e-05, up: 4.0963999999999996e-05}}, 44: {stat: {dn: -0.0001, up: 0.0001}, sys: {dn: -0.00011, up: 0.00011}, 'sys,normalization uncertainty': {dn: -1.4993999999999999e-05, up: 1.4993999999999999e-05}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1238276/d02-x01-y01 +Title: doi:10.17182/hepdata.62088.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.250000e-01 2.500000e-02 2.500000e-02 9.250000e+00 2.573275e-01 2.573275e-01 +2.750000e-01 2.500000e-02 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+BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d02-x01-y03 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.0006664, up: 0.0006664}}, 1: {stat: {dn: -0.002, up: 0.002}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0009212, up: 0.0009212}}, 2: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.008, up: 0.008}, 'sys,normalization uncertainty': {dn: -0.0011956, up: 0.0011956}}, 3: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.009, up: 0.009}, 'sys,normalization uncertainty': {dn: -0.001421, up: 0.001421}}, 4: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.008, up: 0.008}, 'sys,normalization uncertainty': {dn: -0.0015778, up: 0.0015778}}, 5: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0016758, up: 0.0016758}}, 6: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.001764, up: 0.001764}}, 7: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0018424, up: 0.0018424}}, 8: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.0018816, up: 0.0018816}}, 9: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0018914000000000001, up: 0.0018914000000000001}}, 10: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0018718, up: 0.0018718}}, 11: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0018326, up: 0.0018326}}, 12: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0017934, up: 0.0017934}}, 13: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.007, up: 0.007}, 'sys,normalization uncertainty': {dn: -0.0017541999999999998, up: 0.0017541999999999998}}, 14: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.0016953999999999997, up: 0.0016953999999999997}}, 15: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.001617, up: 0.001617}}, 16: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.0014994, up: 0.0014994}}, 17: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.0013622, up: 0.0013622}}, 18: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.006, up: 0.006}, 'sys,normalization uncertainty': {dn: -0.0012348, up: 0.0012348}}, 19: {stat: {dn: -0.001, up: 0.001}, sys: {dn: -0.005, up: 0.005}, 'sys,normalization uncertainty': {dn: -0.0011074, up: 0.0011074}}, 20: {stat: {dn: -0.0005, up: 0.0005}, sys: {dn: -0.0046, up: 0.0046}, 'sys,normalization uncertainty': {dn: -0.00098588, up: 0.00098588}}, 21: {stat: {dn: -0.0005, up: 0.0005}, sys: {dn: -0.0042, up: 0.0042}, 'sys,normalization uncertainty': {dn: -0.000882, up: 0.000882}}, 22: {stat: {dn: -0.0004, up: 0.0004}, sys: {dn: -0.0037, up: 0.0037}, 'sys,normalization uncertainty': {dn: -0.00078302, up: 0.00078302}}, 23: {stat: {dn: -0.0004, up: 0.0004}, sys: {dn: -0.0032, up: 0.0032}, 'sys,normalization uncertainty': {dn: -0.0006899200000000001, up: 0.0006899200000000001}}, 24: {stat: {dn: -0.0004, up: 0.0004}, sys: {dn: -0.0028, up: 0.0028}, 'sys,normalization uncertainty': {dn: -0.0006076, up: 0.0006076}}, 25: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0024, up: 0.0024}, 'sys,normalization uncertainty': {dn: -0.00053704, up: 0.00053704}}, 26: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0021, up: 0.0021}, 'sys,normalization uncertainty': {dn: -0.0004704, up: 0.0004704}}, 27: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0018, up: 0.0018}, 'sys,normalization uncertainty': {dn: -0.00041062, up: 0.00041062}}, 28: {stat: {dn: -0.0003, up: 0.0003}, sys: {dn: -0.0016, up: 0.0016}, 'sys,normalization uncertainty': {dn: -0.00035672, up: 0.00035672}}, 29: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0014, up: 0.0014}, 'sys,normalization uncertainty': {dn: -0.0003087, up: 0.0003087}}, 30: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0012, up: 0.0012}, 'sys,normalization uncertainty': {dn: -0.0002695, up: 0.0002695}}, 31: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0011, up: 0.0011}, 'sys,normalization uncertainty': {dn: -0.00023225999999999998, up: 0.00023225999999999998}}, 32: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.001, up: 0.001}, 'sys,normalization uncertainty': {dn: -0.00020187999999999998, up: 0.00020187999999999998}}, 33: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0009, up: 0.0009}, 'sys,normalization uncertainty': {dn: -0.00017248000000000003, up: 0.00017248000000000003}}, 34: {stat: {dn: -0.0002, up: 0.0002}, sys: {dn: -0.0008, up: 0.0008}, 'sys,normalization uncertainty': {dn: -0.000147, up: 0.000147}}, 35: {stat: {dn: -0.0001, up: 0.0001}, sys: {dn: -0.0007, up: 0.0007}, 'sys,normalization uncertainty': {dn: -0.00012544, up: 0.00012544}}, 36: {stat: {dn: -0.00012, up: 0.00012}, sys: {dn: -0.00049, up: 0.00049}, 'sys,normalization uncertainty': {dn: -9.074799999999999e-05, up: 9.074799999999999e-05}}, 37: {stat: {dn: -9.0e-05, up: 9.0e-05}, sys: {dn: -0.00034, up: 0.00034}, 'sys,normalization uncertainty': {dn: -5.5272e-05, up: 5.5272e-05}}, 38: {stat: {dn: -7.0e-05, up: 7.0e-05}, sys: {dn: -0.00021, up: 0.00021}, 'sys,normalization uncertainty': {dn: -3.1752000000000004e-05, up: 3.1752000000000004e-05}}, 39: {stat: {dn: -5.0e-05, up: 5.0e-05}, sys: {dn: -0.00012, up: 0.00012}, 'sys,normalization uncertainty': {dn: -1.6954e-05, up: 1.6954e-05}}, 40: {stat: {dn: -4.0e-05, up: 4.0e-05}, sys: {dn: -6.0e-05, up: 6.0e-05}, 'sys,normalization uncertainty': {dn: -8.526e-06, up: 8.526e-06}}, 41: {stat: {dn: -3.0e-05, up: 3.0e-05}, sys: {dn: -3.0e-05, up: 3.0e-05}, 'sys,normalization uncertainty': {dn: -3.92e-06, up: 3.92e-06}}, 42: {stat: {dn: -2.0e-05, up: 2.0e-05}, sys: {dn: -2.0e-05, up: 2.0e-05}, 'sys,normalization uncertainty': {dn: -1.666e-06, up: 1.666e-06}}, 43: {stat: {dn: -2.0e-05, up: 2.0e-05}, sys: {dn: -1.0e-05, up: 1.0e-05}, 'sys,normalization uncertainty': {dn: -6.86e-07, up: 6.86e-07}}, 44: {stat: {dn: -1.0e-05, up: 1.0e-05}, sys: {dn: -1.0e-05, up: 1.0e-05}, 'sys,normalization uncertainty': {dn: -9.8e-08, up: 9.8e-08}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1238276/d02-x01-y03 +Title: doi:10.17182/hepdata.62088.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.250000e-01 2.500000e-02 2.500000e-02 6.800000e-02 6.359567e-03 6.359567e-03 +2.750000e-01 2.500000e-02 2.500000e-02 9.400000e-02 7.338161e-03 7.338161e-03 +3.250000e-01 2.500000e-02 2.500000e-02 1.220000e-01 8.150427e-03 8.150427e-03 +3.750000e-01 2.500000e-02 2.500000e-02 1.450000e-01 9.166201e-03 9.166201e-03 +4.250000e-01 2.500000e-02 2.500000e-02 1.610000e-01 8.215196e-03 8.215196e-03 +4.750000e-01 2.500000e-02 2.500000e-02 1.710000e-01 7.266932e-03 7.266932e-03 +5.250000e-01 2.500000e-02 2.500000e-02 1.800000e-01 7.287777e-03 7.287777e-03 +5.750000e-01 2.500000e-02 2.500000e-02 1.880000e-01 7.307150e-03 7.307150e-03 +6.250000e-01 2.500000e-02 2.500000e-02 1.920000e-01 6.367136e-03 6.367136e-03 +6.750000e-01 2.500000e-02 2.500000e-02 1.930000e-01 7.319658e-03 7.319658e-03 +7.250000e-01 2.500000e-02 2.500000e-02 1.910000e-01 7.314618e-03 7.314618e-03 +7.750000e-01 2.500000e-02 2.500000e-02 1.870000e-01 7.304685e-03 7.304685e-03 +8.250000e-01 2.500000e-02 2.500000e-02 1.830000e-01 7.294949e-03 7.294949e-03 +8.750000e-01 2.500000e-02 2.500000e-02 1.790000e-01 7.285411e-03 7.285411e-03 +9.250000e-01 2.500000e-02 2.500000e-02 1.730000e-01 6.314616e-03 6.314616e-03 +9.750000e-01 2.500000e-02 2.500000e-02 1.650000e-01 6.294020e-03 6.294020e-03 +1.050000e+00 5.000000e-02 5.000000e-02 1.530000e-01 6.264838e-03 6.264838e-03 +1.150000e+00 5.000000e-02 5.000000e-02 1.390000e-01 6.233425e-03 6.233425e-03 +1.250000e+00 5.000000e-02 5.000000e-02 1.260000e-01 6.206829e-03 6.206829e-03 +1.350000e+00 5.000000e-02 5.000000e-02 1.130000e-01 5.217886e-03 5.217886e-03 +1.450000e+00 5.000000e-02 5.000000e-02 1.006000e-01 4.730958e-03 4.730958e-03 +1.550000e+00 5.000000e-02 5.000000e-02 9.000000e-02 4.320639e-03 4.320639e-03 +1.650000e+00 5.000000e-02 5.000000e-02 7.990000e-02 3.803041e-03 3.803041e-03 +1.750000e+00 5.000000e-02 5.000000e-02 7.040000e-02 3.297877e-03 3.297877e-03 +1.850000e+00 5.000000e-02 5.000000e-02 6.200000e-02 2.892953e-03 2.892953e-03 +1.950000e+00 5.000000e-02 5.000000e-02 5.480000e-02 2.477582e-03 2.477582e-03 +2.050000e+00 5.000000e-02 5.000000e-02 4.800000e-02 2.172850e-03 2.172850e-03 +2.150000e+00 5.000000e-02 5.000000e-02 4.190000e-02 1.870457e-03 1.870457e-03 +2.250000e+00 5.000000e-02 5.000000e-02 3.640000e-02 1.666508e-03 1.666508e-03 +2.350000e+00 5.000000e-02 5.000000e-02 3.150000e-02 1.447514e-03 1.447514e-03 +2.450000e+00 5.000000e-02 5.000000e-02 2.750000e-02 1.246046e-03 1.246046e-03 +2.550000e+00 5.000000e-02 5.000000e-02 2.370000e-02 1.141904e-03 1.141904e-03 +2.650000e+00 5.000000e-02 5.000000e-02 2.060000e-02 1.039594e-03 1.039594e-03 +2.750000e+00 5.000000e-02 5.000000e-02 1.760000e-02 9.379495e-04 9.379495e-04 +2.850000e+00 5.000000e-02 5.000000e-02 1.500000e-02 8.376210e-04 8.376210e-04 +2.950000e+00 5.000000e-02 5.000000e-02 1.280000e-02 7.181471e-04 7.181471e-04 +3.125000e+00 1.250000e-01 1.250000e-01 9.260000e-03 5.125770e-04 5.125770e-04 +3.375000e+00 1.250000e-01 1.250000e-01 5.640000e-03 3.560267e-04 3.560267e-04 +3.625000e+00 1.250000e-01 1.250000e-01 3.240000e-03 2.236251e-04 2.236251e-04 +3.875000e+00 1.250000e-01 1.250000e-01 1.730000e-03 1.311009e-04 1.311009e-04 +4.125000e+00 1.250000e-01 1.250000e-01 8.700000e-04 7.261331e-05 7.261331e-05 +4.375000e+00 1.250000e-01 1.250000e-01 4.000000e-04 4.260712e-05 4.260712e-05 +4.625000e+00 1.250000e-01 1.250000e-01 1.700000e-04 2.833329e-05 2.833329e-05 +4.875000e+00 1.250000e-01 1.250000e-01 7.000000e-05 2.237120e-05 2.237120e-05 +5.135000e+00 1.350000e-01 1.350000e-01 1.000000e-05 1.414248e-05 1.414248e-05 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.002, up: 0.002}, sys_1: {dn: -0.08, up: 0.08}, sys_2: {dn: -0.019, up: 0.019}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1238276/d03-x01-y01 +Title: doi:10.17182/hepdata.62088.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.735000e+00 2.535000e+00 2.535000e+00 5.364000e+00 8.224962e-02 8.224962e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d03-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.001, up: 0.001}, sys_1: {dn: -0.012, up: 0.012}, sys_2: {dn: -0.016, up: 0.016}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1238276/d03-x01-y02 +Title: doi:10.17182/hepdata.62088.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.735000e+00 2.535000e+00 2.535000e+00 9.460000e-01 2.002498e-02 2.002498e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d03-x01-y03 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.0003, up: 0.0003}, sys_1: {dn: -0.0058, up: 0.0058}, sys_2: {dn: -0.007, up: 0.007}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1238276/d03-x01-y03 +Title: doi:10.17182/hepdata.62088.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.735000e+00 2.535000e+00 2.535000e+00 1.819000e-01 9.095603e-03 9.095603e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d04-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.002, up: 0.002}, sys_1: {dn: -0.092, up: 0.092}, sys_2: {dn: -0.02, up: 0.02}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1238276/d04-x01-y01 +Title: doi:10.17182/hepdata.62088.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.735000e+00 2.535000e+00 2.535000e+00 6.002000e+00 9.417006e-02 9.417006e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d04-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.001, up: 0.001}, sys_1: {dn: -0.012, up: 0.012}, sys_2: {dn: -0.016, up: 0.016}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1238276/d04-x01-y02 +Title: doi:10.17182/hepdata.62088.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.735000e+00 2.535000e+00 2.535000e+00 9.460000e-01 2.002498e-02 2.002498e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d04-x01-y03 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.0003, up: 0.0003}, sys_1: {dn: -0.0095, up: 0.0095}, sys_2: {dn: -0.008, up: 0.008}}} + +IsRef: 1 +Path: /REF/BABAR_2013_I1238276/d04-x01-y03 +Title: doi:10.17182/hepdata.62088.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.735000e+00 2.535000e+00 2.535000e+00 2.612000e-01 1.242337e-02 1.242337e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2013_I1238807.cc b/analyses/pluginBABAR/BABAR_2013_I1238807.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2013_I1238807.cc @@ -0,0 +1,84 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2013_I1238807 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2013_I1238807); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nkaon = bookCounter("TMP/kaon"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::KPLUS) vetoEvent; + } + _nkaon->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nkaon->val(); + double error = _nkaon->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nkaon; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2013_I1238807); + + +} diff --git a/analyses/pluginBABAR/BABAR_2013_I1238807.info b/analyses/pluginBABAR/BABAR_2013_I1238807.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2013_I1238807.info @@ -0,0 +1,39 @@ +Name: BABAR_2013_I1238807 +Year: 2013 +Summary: Cross section for $e^+e^-\to K^+K^-$ between threshold and 5 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 1238807 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D88 (2013) no.3, 032013 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-$ at energies between threshold and 5 GeV using radiative return' +Keywords: +BibKey: Lees:2013gzt +BibTeX: '%%% contains utf-8, see: http://inspirehep.net/info/faq/general#utf8 +%%% add \usepackage[utf8]{inputenc} to your latex preamble + +@article{Lees:2013gzt, + author = "Lees, J. P. and others", + title = "{Precision measurement of the $e^+e^- → K^+K^-(\gamma)$ + cross section with the initial-state radiation method at + BABAR}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D88", + year = "2013", + number = "3", + pages = "032013", + doi = "10.1103/PhysRevD.88.032013", + eprint = "1306.3600", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BABAR-PUB-13-006, SLAC-PUB-15487", + SLACcitation = "%%CITATION = ARXIV:1306.3600;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2013_I1238807.plot b/analyses/pluginBABAR/BABAR_2013_I1238807.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2013_I1238807.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BABAR_2013_I1238807/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2013_I1238807.yoda b/analyses/pluginBABAR/BABAR_2013_I1238807.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2013_I1238807.yoda @@ -0,0 +1,166 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238807/d01-x01-y01IsRef: 1 +Path: /REF/BABAR_2013_I1238807/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.98750 0.00250 0.00250 0.03404 0.05198 0.05198 +0.99250 0.00250 0.00250 0.52023 0.20054 0.20054 +0.99750 0.00250 0.00250 3.19217 0.40650 0.40650 +1.00050 0.00050 0.00050 7.76484 1.51642 1.51642 +1.00150 0.00050 0.00050 5.94779 1.38601 1.38601 +1.00250 0.00050 0.00050 10.59020 1.80259 1.80259 +1.00350 0.00050 0.00050 9.63146 1.86215 1.86215 +1.00450 0.00050 0.00050 13.94398 2.23428 2.23428 +1.00550 0.00050 0.00050 20.33949 2.70745 2.70745 +1.00650 0.00050 0.00050 29.08580 3.12644 3.12644 +1.00750 0.00050 0.00050 30.13583 3.33408 3.33408 +1.00850 0.00050 0.00050 40.40224 3.86399 3.86399 +1.00950 0.00050 0.00050 52.32349 4.47783 4.47783 +1.01050 0.00050 0.00050 67.42239 4.78165 4.78165 +1.01150 0.00050 0.00050 104.99093 5.90879 5.90879 +1.01250 0.00050 0.00050 132.71958 7.17124 7.17124 +1.01350 0.00050 0.00050 182.32391 8.32592 8.32592 +1.01450 0.00050 0.00050 274.11728 10.53492 10.53492 +1.01550 0.00050 0.00050 444.48373 13.64209 13.64209 +1.01650 0.00050 0.00050 695.80222 17.75332 17.75332 +1.01750 0.00050 0.00050 1211.07223 21.79731 21.79731 +1.01850 0.00050 0.00050 1815.48296 28.84015 28.84015 +1.01950 0.00050 0.00050 2009.06013 29.20881 29.20881 +1.02050 0.00050 0.00050 1510.64308 24.19325 24.19325 +1.02150 0.00050 0.00050 949.83482 16.44565 16.44565 +1.02250 0.00050 0.00050 675.07793 13.31370 13.31370 +1.02350 0.00050 0.00050 455.07878 12.23909 12.23909 +1.02450 0.00050 0.00050 363.97604 10.76803 10.76803 +1.02550 0.00050 0.00050 278.69647 9.80299 9.80299 +1.02650 0.00050 0.00050 230.22939 8.37779 8.37779 +1.02750 0.00050 0.00050 171.82932 6.73530 6.73530 +1.02850 0.00050 0.00050 155.89575 7.28194 7.28194 +1.02950 0.00050 0.00050 133.72340 6.77856 6.77856 +1.03050 0.00050 0.00050 126.68812 5.96282 5.96282 +1.03150 0.00050 0.00050 101.37972 5.81777 5.81777 +1.03250 0.00050 0.00050 94.47374 5.60552 5.60552 +1.03350 0.00050 0.00050 78.97748 5.15112 5.15112 +1.03450 0.00050 0.00050 74.62534 5.07906 5.07906 +1.03550 0.00050 0.00050 65.20443 4.63823 4.63823 +1.03650 0.00050 0.00050 60.89312 4.45762 4.45762 +1.03750 0.00050 0.00050 64.81491 4.18438 4.18438 +1.03850 0.00050 0.00050 51.66602 4.08711 4.08711 +1.03950 0.00050 0.00050 45.79948 3.76907 3.76907 +1.04250 0.00250 0.00250 43.40466 1.57036 1.57036 +1.04750 0.00250 0.00250 34.99578 1.45252 1.45252 +1.05250 0.00250 0.00250 27.42988 1.27134 1.27134 +1.05750 0.00250 0.00250 22.91198 1.17089 1.17089 +1.06250 0.00250 0.00250 21.09122 1.09872 1.09872 +1.06750 0.00250 0.00250 19.21957 1.03872 1.03872 +1.07250 0.00250 0.00250 16.65472 0.95991 0.95991 +1.07750 0.00250 0.00250 16.67370 0.97234 0.97234 +1.08250 0.00250 0.00250 16.07066 0.93845 0.93845 +1.08750 0.00250 0.00250 13.80418 0.86376 0.86376 +1.09250 0.00250 0.00250 13.87001 0.88342 0.88342 +1.09750 0.00250 0.00250 12.74153 0.85121 0.85121 +1.11000 0.01000 0.01000 11.50355 0.36345 0.36345 +1.13000 0.01000 0.01000 9.76316 0.33553 0.33553 +1.15000 0.01000 0.01000 8.88819 0.32304 0.32304 +1.17000 0.01000 0.01000 7.91165 0.30661 0.30661 +1.19000 0.01000 0.01000 7.61149 0.30212 0.30212 +1.21000 0.01000 0.01000 7.27651 0.30303 0.30303 +1.23000 0.01000 0.01000 6.32698 0.28422 0.28422 +1.25000 0.01000 0.01000 7.25539 0.29315 0.29315 +1.27000 0.01000 0.01000 6.24005 0.27201 0.27201 +1.29000 0.01000 0.01000 6.02363 0.26125 0.26125 +1.31000 0.01000 0.01000 5.66601 0.25118 0.25118 +1.33000 0.01000 0.01000 5.50158 0.24554 0.24554 +1.35000 0.01000 0.01000 5.00275 0.22984 0.22984 +1.37000 0.01000 0.01000 4.75062 0.22128 0.22128 +1.39000 0.01000 0.01000 5.06118 0.22529 0.22529 +1.41000 0.01000 0.01000 4.33639 0.20842 0.20842 +1.43000 0.01000 0.01000 4.25246 0.20244 0.20244 +1.45000 0.01000 0.01000 4.10792 0.19887 0.19887 +1.47000 0.01000 0.01000 3.75452 0.18989 0.18989 +1.49000 0.01000 0.01000 3.46905 0.18099 0.18099 +1.51000 0.01000 0.01000 3.61010 0.18348 0.18348 +1.53000 0.01000 0.01000 3.22218 0.17507 0.17507 +1.55000 0.01000 0.01000 3.06929 0.17213 0.17213 +1.57000 0.01000 0.01000 3.30626 0.17399 0.17399 +1.59000 0.01000 0.01000 3.23367 0.17013 0.17013 +1.61000 0.01000 0.01000 2.91618 0.16424 0.16424 +1.63000 0.01000 0.01000 2.69413 0.15741 0.15741 +1.65000 0.01000 0.01000 2.52585 0.15017 0.15017 +1.67000 0.01000 0.01000 1.90007 0.13284 0.13284 +1.69000 0.01000 0.01000 1.18224 0.10676 0.10676 +1.71000 0.01000 0.01000 0.84654 0.08840 0.08840 +1.73000 0.01000 0.01000 0.86783 0.08836 0.08836 +1.75000 0.01000 0.01000 0.54285 0.07274 0.07274 +1.77000 0.01000 0.01000 0.33428 0.05854 0.05854 +1.79000 0.01000 0.01000 0.13643 0.04163 0.04163 +1.81000 0.01000 0.01000 0.21617 0.04525 0.04525 +1.83000 0.01000 0.01000 0.30144 0.05383 0.05383 +1.85000 0.01000 0.01000 0.20391 0.04581 0.04581 +1.87000 0.01000 0.01000 0.32506 0.05411 0.05411 +1.89000 0.01000 0.01000 0.23759 0.04843 0.04843 +1.91000 0.01000 0.01000 0.33583 0.05767 0.05767 +1.93000 0.01000 0.01000 0.33025 0.05690 0.05690 +1.95000 0.01000 0.01000 0.33111 0.05679 0.05679 +1.97000 0.01000 0.01000 0.34416 0.05801 0.05801 +1.99000 0.01000 0.01000 0.28873 0.05412 0.05412 +2.01000 0.01000 0.01000 0.37396 0.05773 0.05773 +2.03000 0.01000 0.01000 0.32173 0.05253 0.05253 +2.05000 0.01000 0.01000 0.19299 0.04382 0.04382 +2.07000 0.01000 0.01000 0.29156 0.04940 0.04940 +2.09000 0.01000 0.01000 0.15410 0.04044 0.04044 +2.11000 0.01000 0.01000 0.19067 0.04199 0.04199 +2.13000 0.01000 0.01000 0.22421 0.04437 0.04437 +2.15000 0.01000 0.01000 0.14127 0.03491 0.03491 +2.17000 0.01000 0.01000 0.09976 0.03196 0.03196 +2.19000 0.01000 0.01000 0.22013 0.04426 0.04426 +2.21000 0.01000 0.01000 0.23219 0.04380 0.04380 +2.23000 0.01000 0.01000 0.25413 0.04675 0.04675 +2.25000 0.01000 0.01000 0.31236 0.04700 0.04700 +2.27000 0.01000 0.01000 0.13028 0.03197 0.03197 +2.29000 0.01000 0.01000 0.26799 0.04314 0.04314 +2.31000 0.01000 0.01000 0.21411 0.04027 0.04027 +2.33000 0.01000 0.01000 0.15053 0.03497 0.03497 +2.35000 0.01000 0.01000 0.10188 0.02936 0.02936 +2.37000 0.01000 0.01000 0.15979 0.03388 0.03388 +2.39000 0.01000 0.01000 0.07784 0.02430 0.02430 +2.41000 0.01000 0.01000 0.11294 0.02826 0.02826 +2.43000 0.01000 0.01000 0.11989 0.03027 0.03027 +2.45000 0.01000 0.01000 0.05867 0.02199 0.02199 +2.47000 0.01000 0.01000 0.05324 0.02115 0.02115 +2.49000 0.01000 0.01000 0.10564 0.02690 0.02690 +2.51000 0.01000 0.01000 0.07906 0.02565 0.02565 +2.53000 0.01000 0.01000 0.09094 0.02659 0.02659 +2.55000 0.01000 0.01000 0.10364 0.02810 0.02810 +2.57000 0.01000 0.01000 0.05557 0.02203 0.02203 +2.59000 0.01000 0.01000 0.08155 0.02418 0.02418 +2.62000 0.02000 0.02000 0.06594 0.01464 0.01464 +2.66000 0.02000 0.02000 0.04467 0.01276 0.01276 +2.70000 0.02000 0.02000 0.04615 0.01199 0.01199 +2.74000 0.02000 0.02000 0.03700 0.01072 0.01072 +2.78000 0.02000 0.02000 0.03738 0.01095 0.01095 +2.82000 0.02000 0.02000 0.03908 0.01044 0.01044 +2.86000 0.02000 0.02000 0.02904 0.00925 0.00925 +2.90000 0.02000 0.02000 0.03853 0.01094 0.01094 +2.94000 0.02000 0.02000 0.04467 0.01061 0.01061 +2.98000 0.02000 0.02000 0.02110 0.00791 0.00791 +3.02000 0.02000 0.02000 0.02358 0.00794 0.00794 +3.06000 0.02000 0.02000 0.03378 0.00928 0.00928 +3.10000 0.02000 0.02000 0.02013 0.00692 0.00692 +3.14000 0.02000 0.02000 0.03313 0.00927 0.00927 +3.18000 0.02000 0.02000 0.01784 0.00722 0.00722 +3.22000 0.02000 0.02000 0.02287 0.00757 0.00757 +3.26000 0.02000 0.02000 0.02440 0.00793 0.00793 +3.30000 0.02000 0.02000 0.01005 0.00547 0.00547 +3.34000 0.02000 0.02000 0.03010 0.00775 0.00775 +3.38000 0.02000 0.02000 0.01215 0.00584 0.00584 +3.44000 0.04000 0.04000 0.01232 0.00357 0.00357 +3.52000 0.04000 0.04000 0.00768 0.00275 0.00275 +3.60000 0.04000 0.04000 0.00823 0.00293 0.00293 +3.68000 0.04000 0.04000 0.01103 0.00323 0.00323 +3.76000 0.04000 0.04000 0.00536 0.00246 0.00246 +3.95000 0.15000 0.15000 0.00250 0.00096 0.00096 +4.25000 0.15000 0.15000 0.00390 0.00088 0.00088 +4.55000 0.15000 0.15000 0.00158 0.00062 0.00062 +4.85000 0.15000 0.15000 0.00116 0.00053 0.00053 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2014_I1287920.cc b/analyses/pluginBABAR/BABAR_2014_I1287920.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2014_I1287920.cc @@ -0,0 +1,114 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2014_I1287920 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2014_I1287920); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nKSKL = bookCounter("TMP/nKSKL"); + _nKSKLpipi = bookCounter("TMP/nKSKLpipi"); + _nKSKSpipi = bookCounter("TMP/nKSKSpipi"); + _nKSKSKpKm = bookCounter("TMP/nKSKSKpKm"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + if(ntotal==2 && nCount[130]==1 && nCount[310]==1) + _nKSKL->fill(event.weight()); + else if( ntotal==4 && nCount[130]==1 && nCount[310]==1 && nCount[211]==1 && nCount[-211]==1) + _nKSKLpipi->fill(event.weight()); + else if( ntotal==4 && nCount[310]==2 && nCount[211]==1 && nCount[-211]==1 ) + _nKSKSpipi->fill(event.weight()); + else if( ntotal==4 && nCount[310]==2 && nCount[321]==1 && nCount[-321]==1) + _nKSKSKpKm->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + for(unsigned int ix=9;ix<13;++ix) { + double sigma = 0., error = 0.; + if(ix==9) { + sigma = _nKSKL->val(); + error = _nKSKL->err(); + } + else if(ix==10) { + sigma = _nKSKLpipi->val(); + error = _nKSKLpipi->err(); + } + else if(ix==11) { + sigma = _nKSKSpipi->val(); + error = _nKSKSpipi->err(); + } + else if(ix==12) { + sigma = _nKSKSKpKm->val(); + error = _nKSKSKpKm->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nKSKL,_nKSKLpipi,_nKSKSpipi,_nKSKSKpKm; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2014_I1287920); + + +} diff --git a/analyses/pluginBABAR/BABAR_2014_I1287920.info b/analyses/pluginBABAR/BABAR_2014_I1287920.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2014_I1287920.info @@ -0,0 +1,39 @@ +Name: BABAR_2014_I1287920 +Year: 2014 +Summary: Cross section for $e^+e^-\to$ $K_S^0K_L^0$, $K_S^0K_L^0\pi^+\pi^-$, $K_S^0K_S^0\pi^+\pi^-$, $K_S^0K_S^0K^+K^-$ between 1.06 and 2.2 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 1287920 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D89 (2014) 092002, 2014 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to$ $K_S^0K_L^0$, $K_S^0K_L^0\pi^+\pi^-$, $K_S^0K_S^0\pi^+\pi^-$, $K_S^0K_S^0K^+K^-$ via radiative return, + including for energies between 1.06 and 2.2 GeV' +Keywords: +BibKey: Lees:2014xsh +BibTeX: '@article{Lees:2014xsh, + author = "Lees, J. P. and others", + title = "{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}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D89", + year = "2014", + number = "9", + pages = "092002", + doi = "10.1103/PhysRevD.89.092002", + eprint = "1403.7593", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-15934", + SLACcitation = "%%CITATION = ARXIV:1403.7593;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2014_I1287920.plot b/analyses/pluginBABAR/BABAR_2014_I1287920.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2014_I1287920.plot @@ -0,0 +1,27 @@ +BEGIN PLOT /BABAR_2014_I1287920/d09-x01-y01 +Title=$\sigma(e^+e^-\to K_S^0K_L^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K_L^0)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2014_I1287920/d10-x01-y01 +Title=$\sigma(e^+e^-\to K_S^0K_L^0\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K_L^0\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2014_I1287920/d11-x01-y01 +Title=$\sigma(e^+e^-\to K_S^0K_S^0\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K_S^0\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BABAR_2014_I1287920/d12-x01-y01 +Title=$\sigma(e^+e^-\to K_S^0K_S^0K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K_S^0K^+K^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2014_I1287920.yoda b/analyses/pluginBABAR/BABAR_2014_I1287920.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2014_I1287920.yoda @@ -0,0 +1,531 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -33.0, up: 33.0}, 'sys,model': {dn: -15.0, up: 15.0}, 'sys,syst': {dn: -42.0, up: 42.0}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d01-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.620000e+00 5.400000e-01 5.400000e-01 1.409000e+03 5.547973e+01 5.547973e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.042, up: 0.042}, 'sys,model': {dn: -0.025, up: 0.025}, 'sys,syst': {dn: -0.05, up: 0.05}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d02-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.620000e+00 5.400000e-01 5.400000e-01 1.019462e+03 6.992138e-02 6.992138e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.103, up: 0.103}, 'sys,model': {dn: -0.045, up: 0.045}, 'sys,syst': {dn: -0.05, up: 0.05}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d03-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.620000e+00 5.400000e-01 5.400000e-01 4.205000e+00 1.230203e-01 1.230203e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d04-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.0033, up: 0.0033}, 'sys,model': {dn: -0.0019, up: 0.0019}, 'sys,syst': {dn: -0.0122, up: 0.0122}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d04-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.620000e+00 5.400000e-01 5.400000e-01 4.200000e-01 1.278045e-02 1.278045e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d05-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.05, up: 0.05}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d05-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.620000e+00 5.400000e-01 5.400000e-01 4.600000e-01 1.118034e-01 1.118034e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d06-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -12.0, up: 12.0}, sys: {dn: -6.0, up: 6.0}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d06-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.620000e+00 5.400000e-01 5.400000e-01 1.674000e+03 1.341641e+01 1.341641e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d07-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -38.0, up: 38.0}, sys: {dn: -70.0, up: 70.0}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d07-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t7 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.620000e+00 5.400000e-01 5.400000e-01 1.650000e+02 7.964923e+01 7.964923e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d08-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -2.4, up: 2.4}, 'sys,model': {dn: -6.0, up: 6.0}, 'sys,syst': {dn: -1.5, up: 1.5}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d08-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t8 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.620000e+00 5.400000e-01 5.400000e-01 1.430000e+01 6.634003e+00 6.634003e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d09-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.43, up: 0.43}}, 1: {error: {dn: -0.3, up: 0.3}}, 2: {error: {dn: -0.24, up: 0.24}}, 3: {error: {dn: -0.23, up: 0.23}}, 4: {error: {dn: -0.18, up: 0.18}}, 5: {error: {dn: -0.14, up: 0.14}}, 6: {error: {dn: -0.15, up: 0.15}}, 7: {error: {dn: -0.13, up: 0.13}}, 8: {error: {dn: -0.11, up: 0.11}}, 9: {error: {dn: -0.12, up: 0.12}}, 10: {error: {dn: -0.11, up: 0.11}}, 11: {error: {dn: -0.13, up: 0.13}}, 12: {error: {dn: -0.13, up: 0.13}}, 13: {error: {dn: -0.12, up: 0.12}}, 14: {error: {dn: -0.13, up: 0.13}}, 15: {error: {dn: -0.11, up: 0.11}}, 16: {error: {dn: -0.11, up: 0.11}}, 17: {error: {dn: -0.07, up: 0.07}}, 18: {error: {dn: -0.05, up: 0.05}}, 19: {error: {dn: -0.04, up: 0.04}}, 20: {error: {dn: -0.04, up: 0.04}}, 21: {error: {dn: -0.05, up: 0.05}}, 22: {error: {dn: -0.05, up: 0.05}}, 23: {error: {dn: -0.03, up: 0.03}}, 24: {error: {dn: -0.03, up: 0.03}}, 25: {error: {dn: -0.03, up: 0.03}}, 26: {error: {dn: -0.02, up: 0.02}}, 27: {error: {dn: -0.03, up: 0.03}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d09-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t9 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.080000e+00 0.000000e+00 0.000000e+00 6.860000e+00 4.300000e-01 4.300000e-01 +1.120000e+00 0.000000e+00 0.000000e+00 2.860000e+00 3.000000e-01 3.000000e-01 +1.160000e+00 0.000000e+00 0.000000e+00 1.780000e+00 2.400000e-01 2.400000e-01 +1.200000e+00 0.000000e+00 0.000000e+00 1.480000e+00 2.300000e-01 2.300000e-01 +1.240000e+00 0.000000e+00 0.000000e+00 8.700000e-01 1.800000e-01 1.800000e-01 +1.280000e+00 0.000000e+00 0.000000e+00 5.400000e-01 1.400000e-01 1.400000e-01 +1.320000e+00 0.000000e+00 0.000000e+00 5.400000e-01 1.500000e-01 1.500000e-01 +1.360000e+00 0.000000e+00 0.000000e+00 4.000000e-01 1.300000e-01 1.300000e-01 +1.400000e+00 0.000000e+00 0.000000e+00 2.200000e-01 1.100000e-01 1.100000e-01 +1.440000e+00 0.000000e+00 0.000000e+00 3.200000e-01 1.200000e-01 1.200000e-01 +1.480000e+00 0.000000e+00 0.000000e+00 3.600000e-01 1.100000e-01 1.100000e-01 +1.520000e+00 0.000000e+00 0.000000e+00 6.600000e-01 1.300000e-01 1.300000e-01 +1.560000e+00 0.000000e+00 0.000000e+00 6.700000e-01 1.300000e-01 1.300000e-01 +1.600000e+00 0.000000e+00 0.000000e+00 8.400000e-01 1.200000e-01 1.200000e-01 +1.640000e+00 0.000000e+00 0.000000e+00 8.300000e-01 1.300000e-01 1.300000e-01 +1.680000e+00 0.000000e+00 0.000000e+00 5.100000e-01 1.100000e-01 1.100000e-01 +1.720000e+00 0.000000e+00 0.000000e+00 2.600000e-01 1.100000e-01 1.100000e-01 +1.760000e+00 0.000000e+00 0.000000e+00 1.100000e-01 7.000000e-02 7.000000e-02 +1.800000e+00 0.000000e+00 0.000000e+00 3.000000e-02 5.000000e-02 5.000000e-02 +1.840000e+00 0.000000e+00 0.000000e+00 4.000000e-02 4.000000e-02 4.000000e-02 +1.880000e+00 0.000000e+00 0.000000e+00 2.000000e-02 4.000000e-02 4.000000e-02 +1.920000e+00 0.000000e+00 0.000000e+00 7.000000e-02 5.000000e-02 5.000000e-02 +1.960000e+00 0.000000e+00 0.000000e+00 9.000000e-02 5.000000e-02 5.000000e-02 +2.000000e+00 0.000000e+00 0.000000e+00 2.000000e-02 3.000000e-02 3.000000e-02 +2.040000e+00 0.000000e+00 0.000000e+00 2.000000e-02 3.000000e-02 3.000000e-02 +2.080000e+00 0.000000e+00 0.000000e+00 0.000000e+00 3.000000e-02 3.000000e-02 +2.120000e+00 0.000000e+00 0.000000e+00 1.000000e-02 2.000000e-02 2.000000e-02 +2.160000e+00 0.000000e+00 0.000000e+00 2.000000e-02 3.000000e-02 3.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d10-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.02, up: 0.02}}, 1: {error: {dn: -0.04, up: 0.04}}, 2: {error: {dn: -0.04, up: 0.04}}, 3: {error: {dn: -0.05, up: 0.05}}, 4: {error: {dn: -0.05, up: 0.05}}, 5: {error: {dn: -0.06, up: 0.06}}, 6: {error: {dn: -0.06, up: 0.06}}, 7: {error: {dn: -0.07, up: 0.07}}, 8: {error: {dn: -0.08, up: 0.08}}, 9: {error: {dn: -0.08, up: 0.08}}, 10: {error: {dn: -0.09, up: 0.09}}, 11: {error: {dn: -0.09, up: 0.09}}, 12: {error: {dn: -0.09, up: 0.09}}, 13: {error: {dn: -0.09, up: 0.09}}, 14: {error: {dn: -0.08, up: 0.08}}, 15: {error: {dn: -0.08, up: 0.08}}, 16: {error: {dn: -0.08, up: 0.08}}, 17: {error: {dn: -0.07, up: 0.07}}, 18: {error: {dn: -0.07, up: 0.07}}, 19: {error: {dn: -0.07, up: 0.07}}, 20: {error: {dn: -0.06, up: 0.06}}, 21: {error: {dn: -0.06, up: 0.06}}, 22: {error: {dn: -0.06, up: 0.06}}, 23: {error: {dn: -0.06, up: 0.06}}, 24: {error: {dn: -0.06, up: 0.06}}, 25: {error: {dn: -0.05, up: 0.05}}, 26: {error: {dn: -0.05, up: 0.05}}, 27: {error: {dn: -0.05, up: 0.05}}, 28: {error: {dn: -0.05, up: 0.05}}, 29: {error: {dn: -0.05, up: 0.05}}, 30: {error: {dn: -0.05, up: 0.05}}, 31: {error: {dn: -0.05, up: 0.05}}, 32: {error: {dn: -0.05, up: 0.05}}, 33: {error: {dn: -0.06, up: 0.06}}, 34: {error: {dn: -0.05, up: 0.05}}, 35: {error: {dn: -0.05, up: 0.05}}, 36: {error: {dn: -0.04, up: 0.04}}, 37: {error: {dn: -0.04, up: 0.04}}, 38: {error: {dn: -0.04, up: 0.04}}, 39: {error: {dn: -0.04, up: 0.04}}, 40: {error: {dn: -0.04, up: 0.04}}, 41: {error: {dn: -0.03, up: 0.03}}, 42: {error: {dn: -0.03, up: 0.03}}, 43: {error: {dn: -0.03, up: 0.03}}, 44: {error: {dn: -0.03, up: 0.03}}, 45: {error: {dn: -0.03, up: 0.03}}, 46: {error: {dn: -0.03, up: 0.03}}, 47: {error: {dn: -0.03, up: 0.03}}, 48: {error: {dn: -0.03, up: 0.03}}, 49: {error: {dn: -0.03, up: 0.03}}, 50: {error: {dn: -0.03, up: 0.03}}, 51: {error: {dn: -0.03, up: 0.03}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d10-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t10 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.425000e+00 0.000000e+00 0.000000e+00 3.000000e-02 2.000000e-02 2.000000e-02 +1.475000e+00 0.000000e+00 0.000000e+00 1.200000e-01 4.000000e-02 4.000000e-02 +1.525000e+00 0.000000e+00 0.000000e+00 1.500000e-01 4.000000e-02 4.000000e-02 +1.575000e+00 0.000000e+00 0.000000e+00 1.700000e-01 5.000000e-02 5.000000e-02 +1.625000e+00 0.000000e+00 0.000000e+00 2.000000e-01 5.000000e-02 5.000000e-02 +1.675000e+00 0.000000e+00 0.000000e+00 2.700000e-01 6.000000e-02 6.000000e-02 +1.725000e+00 0.000000e+00 0.000000e+00 3.900000e-01 6.000000e-02 6.000000e-02 +1.775000e+00 0.000000e+00 0.000000e+00 5.800000e-01 7.000000e-02 7.000000e-02 +1.825000e+00 0.000000e+00 0.000000e+00 6.000000e-01 8.000000e-02 8.000000e-02 +1.875000e+00 0.000000e+00 0.000000e+00 8.300000e-01 8.000000e-02 8.000000e-02 +1.925000e+00 0.000000e+00 0.000000e+00 1.090000e+00 9.000000e-02 9.000000e-02 +1.975000e+00 0.000000e+00 0.000000e+00 1.030000e+00 9.000000e-02 9.000000e-02 +2.025000e+00 0.000000e+00 0.000000e+00 9.400000e-01 9.000000e-02 9.000000e-02 +2.075000e+00 0.000000e+00 0.000000e+00 9.900000e-01 9.000000e-02 9.000000e-02 +2.125000e+00 0.000000e+00 0.000000e+00 8.100000e-01 8.000000e-02 8.000000e-02 +2.175000e+00 0.000000e+00 0.000000e+00 6.900000e-01 8.000000e-02 8.000000e-02 +2.225000e+00 0.000000e+00 0.000000e+00 5.600000e-01 8.000000e-02 8.000000e-02 +2.275000e+00 0.000000e+00 0.000000e+00 5.100000e-01 7.000000e-02 7.000000e-02 +2.325000e+00 0.000000e+00 0.000000e+00 4.000000e-01 7.000000e-02 7.000000e-02 +2.375000e+00 0.000000e+00 0.000000e+00 4.300000e-01 7.000000e-02 7.000000e-02 +2.425000e+00 0.000000e+00 0.000000e+00 3.100000e-01 6.000000e-02 6.000000e-02 +2.475000e+00 0.000000e+00 0.000000e+00 2.700000e-01 6.000000e-02 6.000000e-02 +2.525000e+00 0.000000e+00 0.000000e+00 2.200000e-01 6.000000e-02 6.000000e-02 +2.575000e+00 0.000000e+00 0.000000e+00 1.700000e-01 6.000000e-02 6.000000e-02 +2.625000e+00 0.000000e+00 0.000000e+00 2.300000e-01 6.000000e-02 6.000000e-02 +2.675000e+00 0.000000e+00 0.000000e+00 1.800000e-01 5.000000e-02 5.000000e-02 +2.725000e+00 0.000000e+00 0.000000e+00 1.100000e-01 5.000000e-02 5.000000e-02 +2.775000e+00 0.000000e+00 0.000000e+00 2.400000e-01 5.000000e-02 5.000000e-02 +2.825000e+00 0.000000e+00 0.000000e+00 2.100000e-01 5.000000e-02 5.000000e-02 +2.875000e+00 0.000000e+00 0.000000e+00 1.500000e-01 5.000000e-02 5.000000e-02 +2.925000e+00 0.000000e+00 0.000000e+00 2.200000e-01 5.000000e-02 5.000000e-02 +2.975000e+00 0.000000e+00 0.000000e+00 1.700000e-01 5.000000e-02 5.000000e-02 +3.025000e+00 0.000000e+00 0.000000e+00 1.800000e-01 5.000000e-02 5.000000e-02 +3.075000e+00 0.000000e+00 0.000000e+00 6.000000e-01 6.000000e-02 6.000000e-02 +3.125000e+00 0.000000e+00 0.000000e+00 4.400000e-01 5.000000e-02 5.000000e-02 +3.175000e+00 0.000000e+00 0.000000e+00 1.600000e-01 5.000000e-02 5.000000e-02 +3.225000e+00 0.000000e+00 0.000000e+00 5.000000e-02 4.000000e-02 4.000000e-02 +3.275000e+00 0.000000e+00 0.000000e+00 8.000000e-02 4.000000e-02 4.000000e-02 +3.325000e+00 0.000000e+00 0.000000e+00 5.000000e-02 4.000000e-02 4.000000e-02 +3.375000e+00 0.000000e+00 0.000000e+00 7.000000e-02 4.000000e-02 4.000000e-02 +3.425000e+00 0.000000e+00 0.000000e+00 1.000000e-02 4.000000e-02 4.000000e-02 +3.475000e+00 0.000000e+00 0.000000e+00 -1.000000e-02 3.000000e-02 3.000000e-02 +3.525000e+00 0.000000e+00 0.000000e+00 3.000000e-02 3.000000e-02 3.000000e-02 +3.575000e+00 0.000000e+00 0.000000e+00 3.000000e-02 3.000000e-02 3.000000e-02 +3.625000e+00 0.000000e+00 0.000000e+00 0.000000e+00 3.000000e-02 3.000000e-02 +3.675000e+00 0.000000e+00 0.000000e+00 -1.000000e-02 3.000000e-02 3.000000e-02 +3.725000e+00 0.000000e+00 0.000000e+00 -6.000000e-02 3.000000e-02 3.000000e-02 +3.775000e+00 0.000000e+00 0.000000e+00 2.000000e-02 3.000000e-02 3.000000e-02 +3.825000e+00 0.000000e+00 0.000000e+00 -3.000000e-02 3.000000e-02 3.000000e-02 +3.875000e+00 0.000000e+00 0.000000e+00 0.000000e+00 3.000000e-02 3.000000e-02 +3.925000e+00 0.000000e+00 0.000000e+00 4.000000e-02 3.000000e-02 3.000000e-02 +3.975000e+00 0.000000e+00 0.000000e+00 1.000000e-02 3.000000e-02 3.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d11-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.01, up: 0.01}}, 1: {error: {dn: -0.01, up: 0.01}}, 2: {error: {dn: -0.02, up: 0.02}}, 3: {error: {dn: -0.03, up: 0.03}}, 4: {error: {dn: -0.03, up: 0.03}}, 5: {error: {dn: -0.03, up: 0.03}}, 6: {error: {dn: -0.04, up: 0.04}}, 7: {error: {dn: -0.04, up: 0.04}}, 8: {error: {dn: -0.05, up: 0.05}}, 9: {error: {dn: -0.04, up: 0.04}}, 10: {error: {dn: -0.04, up: 0.04}}, 11: {error: {dn: -0.03, up: 0.03}}, 12: {error: {dn: -0.03, up: 0.03}}, 13: {error: {dn: -0.03, up: 0.03}}, 14: {error: {dn: -0.02, up: 0.02}}, 15: {error: {dn: -0.02, up: 0.02}}, 16: {error: {dn: -0.02, up: 0.02}}, 17: {error: {dn: -0.02, up: 0.02}}, 18: {error: {dn: -0.02, up: 0.02}}, 19: {error: {dn: -0.02, up: 0.02}}, 20: {error: {dn: -0.02, up: 0.02}}, 21: {error: {dn: -0.02, up: 0.02}}, 22: {error: {dn: -0.02, up: 0.02}}, 23: {error: {dn: -0.01, up: 0.01}}, 24: {error: {dn: -0.01, up: 0.01}}, 25: {error: {dn: -0.01, up: 0.01}}, 26: {error: {dn: -0.01, up: 0.01}}, 27: {error: {dn: -0.02, up: 0.02}}, 28: {error: {dn: -0.01, up: 0.01}}, 29: {error: {dn: -0.03, up: 0.03}}, 30: {error: {dn: -0.02, up: 0.02}}, 31: {error: {dn: -0.01, up: 0.01}}, 32: {error: {dn: -0.01, up: 0.01}}, 33: {error: {dn: -0.01, up: 0.01}}, 34: {error: {dn: -0.01, up: 0.01}}, 35: {error: {dn: -0.01, up: 0.01}}, 36: {error: {dn: -0.01, up: 0.01}}, 37: {error: {dn: -0.01, up: 0.01}}, 38: {error: {dn: -0.01, up: 0.01}}, 39: {error: {dn: -0.01, up: 0.01}}, 40: {error: {dn: -0.01, up: 0.01}}, 41: {error: {dn: -0.01, up: 0.01}}, 42: {error: {dn: -0.01, up: 0.01}}, 43: {error: {dn: -0.01, up: 0.01}}, 44: {error: {dn: -0.01, up: 0.01}}, 45: {error: {dn: -0.01, up: 0.01}}, 46: {error: {dn: -0.01, up: 0.01}}, 47: {error: {dn: -0.01, up: 0.01}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d11-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t11 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.630000e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +1.670000e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +1.730000e+00 0.000000e+00 0.000000e+00 5.000000e-02 2.000000e-02 2.000000e-02 +1.770000e+00 0.000000e+00 0.000000e+00 1.300000e-01 3.000000e-02 3.000000e-02 +1.830000e+00 0.000000e+00 0.000000e+00 2.200000e-01 3.000000e-02 3.000000e-02 +1.880000e+00 0.000000e+00 0.000000e+00 2.400000e-01 3.000000e-02 3.000000e-02 +1.920000e+00 0.000000e+00 0.000000e+00 2.700000e-01 4.000000e-02 4.000000e-02 +1.980000e+00 0.000000e+00 0.000000e+00 3.800000e-01 4.000000e-02 4.000000e-02 +2.030000e+00 0.000000e+00 0.000000e+00 4.700000e-01 5.000000e-02 5.000000e-02 +2.080000e+00 0.000000e+00 0.000000e+00 3.700000e-01 4.000000e-02 4.000000e-02 +2.130000e+00 0.000000e+00 0.000000e+00 3.800000e-01 4.000000e-02 4.000000e-02 +2.170000e+00 0.000000e+00 0.000000e+00 2.500000e-01 3.000000e-02 3.000000e-02 +2.220000e+00 0.000000e+00 0.000000e+00 2.200000e-01 3.000000e-02 3.000000e-02 +2.280000e+00 0.000000e+00 0.000000e+00 2.500000e-01 3.000000e-02 3.000000e-02 +2.330000e+00 0.000000e+00 0.000000e+00 1.300000e-01 2.000000e-02 2.000000e-02 +2.380000e+00 0.000000e+00 0.000000e+00 1.200000e-01 2.000000e-02 2.000000e-02 +2.420000e+00 0.000000e+00 0.000000e+00 1.000000e-01 2.000000e-02 2.000000e-02 +2.470000e+00 0.000000e+00 0.000000e+00 1.200000e-01 2.000000e-02 2.000000e-02 +2.530000e+00 0.000000e+00 0.000000e+00 1.100000e-01 2.000000e-02 2.000000e-02 +2.580000e+00 0.000000e+00 0.000000e+00 1.200000e-01 2.000000e-02 2.000000e-02 +2.630000e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +2.670000e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.000000e-02 2.000000e-02 +2.720000e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.000000e-02 2.000000e-02 +2.780000e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.000000e-02 1.000000e-02 +2.830000e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +2.880000e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +2.920000e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.000000e-02 1.000000e-02 +2.970000e+00 0.000000e+00 0.000000e+00 7.000000e-02 2.000000e-02 2.000000e-02 +3.030000e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.000000e-02 1.000000e-02 +3.080000e+00 0.000000e+00 0.000000e+00 2.800000e-01 3.000000e-02 3.000000e-02 +3.130000e+00 0.000000e+00 0.000000e+00 1.900000e-01 2.000000e-02 2.000000e-02 +3.170000e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +3.220000e+00 0.000000e+00 0.000000e+00 7.000000e-02 1.000000e-02 1.000000e-02 +3.280000e+00 0.000000e+00 0.000000e+00 5.000000e-02 1.000000e-02 1.000000e-02 +3.330000e+00 0.000000e+00 0.000000e+00 3.000000e-02 1.000000e-02 1.000000e-02 +3.380000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +3.420000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +3.470000e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +3.530000e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +3.580000e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +3.630000e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +3.670000e+00 0.000000e+00 0.000000e+00 4.000000e-02 1.000000e-02 1.000000e-02 +3.720000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +3.780000e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +3.830000e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +3.880000e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 +3.920000e+00 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 1.000000e-02 +3.970000e+00 0.000000e+00 0.000000e+00 2.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d12-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.003, up: 0.003}}, 1: {error: {dn: -0.003, up: 0.003}}, 2: {error: {dn: -0.004, up: 0.004}}, 3: {error: {dn: -0.005, up: 0.005}}, 4: {error: {dn: -0.004, up: 0.004}}, 5: {error: {dn: -0.004, up: 0.004}}, 6: {error: {dn: -0.006, up: 0.006}}, 7: {error: {dn: -0.004, up: 0.004}}, 8: {error: {dn: -0.004, up: 0.004}}, 9: {error: {dn: -0.005, up: 0.005}}, 10: {error: {dn: -0.005, up: 0.005}}, 11: {error: {dn: -0.003, up: 0.003}}, 12: {error: {dn: -0.004, up: 0.004}}, 13: {error: {dn: -0.004, up: 0.004}}, 14: {error: {dn: -0.004, up: 0.004}}, 15: {error: {dn: -0.003, up: 0.003}}, 16: {error: {dn: -0.002, up: 0.002}}, 17: {error: {dn: -0.003, up: 0.003}}, 18: {error: {dn: -0.003, up: 0.003}}, 19: {error: {dn: -0.002, up: 0.002}}, 20: {error: {dn: -0.002, up: 0.002}}, 21: {error: {dn: -0.002, up: 0.002}}, 22: {error: {dn: -0.003, up: 0.003}}, 23: {error: {dn: -0.001, up: 0.001}}, 24: {error: {dn: -0.002, up: 0.002}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d12-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t12 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.050000e+00 0.000000e+00 0.000000e+00 3.000000e-03 3.000000e-03 3.000000e-03 +2.150000e+00 0.000000e+00 0.000000e+00 0.000000e+00 3.000000e-03 3.000000e-03 +2.250000e+00 0.000000e+00 0.000000e+00 8.000000e-03 4.000000e-03 4.000000e-03 +2.350000e+00 0.000000e+00 0.000000e+00 1.000000e-02 5.000000e-03 5.000000e-03 +2.450000e+00 0.000000e+00 0.000000e+00 7.000000e-03 4.000000e-03 4.000000e-03 +2.550000e+00 0.000000e+00 0.000000e+00 7.000000e-03 4.000000e-03 4.000000e-03 +2.650000e+00 0.000000e+00 0.000000e+00 1.700000e-02 6.000000e-03 6.000000e-03 +2.750000e+00 0.000000e+00 0.000000e+00 1.000000e-02 4.000000e-03 4.000000e-03 +2.850000e+00 0.000000e+00 0.000000e+00 1.000000e-02 4.000000e-03 4.000000e-03 +2.950000e+00 0.000000e+00 0.000000e+00 1.100000e-02 5.000000e-03 5.000000e-03 +3.050000e+00 0.000000e+00 0.000000e+00 1.200000e-02 5.000000e-03 5.000000e-03 +3.150000e+00 0.000000e+00 0.000000e+00 5.000000e-03 3.000000e-03 3.000000e-03 +3.250000e+00 0.000000e+00 0.000000e+00 1.000000e-02 4.000000e-03 4.000000e-03 +3.350000e+00 0.000000e+00 0.000000e+00 9.000000e-03 4.000000e-03 4.000000e-03 +3.450000e+00 0.000000e+00 0.000000e+00 1.300000e-02 4.000000e-03 4.000000e-03 +3.550000e+00 0.000000e+00 0.000000e+00 6.000000e-03 3.000000e-03 3.000000e-03 +3.650000e+00 0.000000e+00 0.000000e+00 4.000000e-03 2.000000e-03 2.000000e-03 +3.750000e+00 0.000000e+00 0.000000e+00 5.000000e-03 3.000000e-03 3.000000e-03 +3.850000e+00 0.000000e+00 0.000000e+00 9.000000e-03 3.000000e-03 3.000000e-03 +3.950000e+00 0.000000e+00 0.000000e+00 2.000000e-03 2.000000e-03 2.000000e-03 +4.050000e+00 0.000000e+00 0.000000e+00 4.000000e-03 2.000000e-03 2.000000e-03 +4.150000e+00 0.000000e+00 0.000000e+00 3.000000e-03 2.000000e-03 2.000000e-03 +4.250000e+00 0.000000e+00 0.000000e+00 0.000000e+00 3.000000e-03 3.000000e-03 +4.350000e+00 0.000000e+00 0.000000e+00 1.000000e-03 1.000000e-03 1.000000e-03 +4.450000e+00 0.000000e+00 0.000000e+00 3.000000e-03 2.000000e-03 2.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d13-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -2.3, up: 2.3}, sys: {dn: -2.1, up: 2.1}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d13-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t13 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.700000e+00 1.275000e+00 1.275000e+00 2.080000e+01 3.114482e+00 3.114482e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d13-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.6, up: 0.6}, sys: {dn: -0.4, up: 0.4}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d13-x01-y02 +Title: doi:10.17182/hepdata.64506.v1/t13 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.700000e+00 1.275000e+00 1.275000e+00 3.700000e+00 7.211103e-01 7.211103e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d14-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.9, up: 0.9}, sys: {dn: -0.5, up: 0.5}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d14-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t14 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.800000e+00 1.170000e+00 1.170000e+00 9.300000e+00 1.029563e+00 1.029563e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d14-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.16, up: 0.16}, sys: {dn: -0.08, up: 0.08}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d14-x01-y02 +Title: doi:10.17182/hepdata.64506.v1/t14 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.800000e+00 1.170000e+00 1.170000e+00 1.680000e+00 1.788854e-01 1.788854e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d15-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.4, up: 0.4}, sys: {dn: -0.1, up: 0.1}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d15-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t15 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.250000e+00 1.200000e+00 1.200000e+00 2.300000e+00 4.123106e-01 4.123106e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d15-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.08, up: 0.08}, sys: {dn: -0.02, up: 0.02}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d15-x01-y02 +Title: doi:10.17182/hepdata.64506.v1/t15 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.250000e+00 1.200000e+00 1.200000e+00 4.200000e-01 8.246211e-02 8.246211e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d16-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -1.2, up: 1.2}, sys: {dn: -0.3, up: 0.3}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d16-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t16 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.800000e+00 1.170000e+00 1.170000e+00 3.700000e+00 1.236932e+00 1.236932e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d16-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.9, up: 0.9}, sys: {dn: -0.2, up: 0.2}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d16-x01-y02 +Title: doi:10.17182/hepdata.64506.v1/t16 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.800000e+00 1.170000e+00 1.170000e+00 2.600000e+00 9.219544e-01 9.219544e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d17-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -1.2, up: 1.2}, sys: {dn: -0.2, up: 0.2}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d17-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t17 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.800000e+00 1.170000e+00 1.170000e+00 2.500000e+00 1.216553e+00 1.216553e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d17-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -1.7, up: 1.7}, sys: {dn: -0.3, up: 0.3}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d17-x01-y02 +Title: doi:10.17182/hepdata.64506.v1/t17 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.800000e+00 1.170000e+00 1.170000e+00 3.600000e+00 1.726268e+00 1.726268e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d18-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.03, up: 0.03}, sys: {dn: -0.02, up: 0.02}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d18-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t18 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.800000e+00 1.170000e+00 1.170000e+00 5.000000e-02 3.605551e-02 3.605551e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d18-x01-y02 +Variations: [] +ErrorBreakdown: {} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d18-x01-y02 +Title: doi:10.17182/hepdata.64506.v1/t18 +Type: Scatter2D +--- +# xval xerr- xerr+ yval +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d19-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.5, up: 0.5}, sys: {dn: -0.02, up: 0.02}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d19-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t19 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.800000e+00 1.170000e+00 1.170000e+00 5.800000e-01 5.003998e-01 5.003998e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d19-x01-y02 +Variations: [] +ErrorBreakdown: {} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d19-x01-y02 +Title: doi:10.17182/hepdata.64506.v1/t19 +Type: Scatter2D +--- +# xval xerr- xerr+ yval +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d20-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.4, up: 0.4}, sys: {dn: -0.1, up: 0.1}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d20-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t20 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.250000e+00 1.200000e+00 1.200000e+00 1.600000e+00 4.123106e-01 4.123106e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d20-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.14, up: 0.14}, sys: {dn: -0.03, up: 0.03}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d20-x01-y02 +Title: doi:10.17182/hepdata.64506.v1/t20 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.250000e+00 1.200000e+00 1.200000e+00 5.800000e-01 1.431782e-01 1.431782e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d21-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.34, up: 0.34}, sys: {dn: -0.04, up: 0.04}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d21-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t21 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.250000e+00 1.200000e+00 1.200000e+00 8.800000e-01 3.423449e-01 3.423449e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d21-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.17, up: 0.17}, sys: {dn: -0.02, up: 0.02}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d21-x01-y02 +Title: doi:10.17182/hepdata.64506.v1/t21 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.250000e+00 1.200000e+00 1.200000e+00 4.500000e-01 1.711724e-01 1.711724e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d22-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.42, up: 0.42}, sys: {dn: -0.05, up: 0.05}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d22-x01-y01 +Title: doi:10.17182/hepdata.64506.v1/t22 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.250000e+00 1.200000e+00 1.200000e+00 1.280000e+00 4.229657e-01 4.229657e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2014_I1287920/d22-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.11, up: 0.11}, sys: {dn: -0.02, up: 0.02}}} + +IsRef: 1 +Path: /REF/BABAR_2014_I1287920/d22-x01-y02 +Title: doi:10.17182/hepdata.64506.v1/t22 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.250000e+00 1.200000e+00 1.200000e+00 3.200000e-01 1.118034e-01 1.118034e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/BABAR_2015_I1334693.cc b/analyses/pluginBABAR/BABAR_2015_I1334693.cc rename from analyses/pluginMisc/BABAR_2015_I1334693.cc rename to analyses/pluginBABAR/BABAR_2015_I1334693.cc diff --git a/analyses/pluginMisc/BABAR_2015_I1334693.info b/analyses/pluginBABAR/BABAR_2015_I1334693.info rename from analyses/pluginMisc/BABAR_2015_I1334693.info rename to analyses/pluginBABAR/BABAR_2015_I1334693.info diff --git a/analyses/pluginMisc/BABAR_2015_I1334693.plot b/analyses/pluginBABAR/BABAR_2015_I1334693.plot rename from analyses/pluginMisc/BABAR_2015_I1334693.plot rename to analyses/pluginBABAR/BABAR_2015_I1334693.plot diff --git a/analyses/pluginMisc/BABAR_2015_I1334693.yoda b/analyses/pluginBABAR/BABAR_2015_I1334693.yoda rename from analyses/pluginMisc/BABAR_2015_I1334693.yoda rename to analyses/pluginBABAR/BABAR_2015_I1334693.yoda diff --git a/analyses/pluginBABAR/BABAR_2015_I1383130.cc b/analyses/pluginBABAR/BABAR_2015_I1383130.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2015_I1383130.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2015_I1383130 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2015_I1383130); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nkaon = bookCounter("TMP/kaon"); + + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::KPLUS) vetoEvent; + } + _nkaon->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nkaon->val(); + double error = _nkaon->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 4)); + Scatter2DPtr mult = bookScatter2D(1, 1, 4); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nkaon; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2015_I1383130); + + +} diff --git a/analyses/pluginBABAR/BABAR_2015_I1383130.info b/analyses/pluginBABAR/BABAR_2015_I1383130.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2015_I1383130.info @@ -0,0 +1,34 @@ +Name: BABAR_2015_I1383130 +Year: 2015 +Summary: Cross section for $e^+e^-\to K^+K^-$ between 2.6 and 8 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 1383130 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- 'Phys.Rev. D92 (2015) no.7, 072008' +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-$ at energies between 2.6 and 8 GeV' +BibKey: Lees:2015iba +BibTeX: '@article{Lees:2015iba, + author = "Lees, J. P. and others", + title = "{Study of the $e^+e^-\to K^+K^-$ reaction in the energy + range from 2.6 to 8.0 GeV}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D92", + year = "2015", + number = "7", + pages = "072008", + doi = "10.1103/PhysRevD.92.072008", + eprint = "1507.04638", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BABAR-PUB-15-004, SLAC-PUB-16333", + SLACcitation = "%%CITATION = ARXIV:1507.04638;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2015_I1383130.plot b/analyses/pluginBABAR/BABAR_2015_I1383130.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2015_I1383130.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BABAR_2015_I1383130/d01-x01-y04 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2015_I1383130.yoda b/analyses/pluginBABAR/BABAR_2015_I1383130.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2015_I1383130.yoda @@ -0,0 +1,158 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2015_I1383130/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -9.0, up: 9.0}, sys: {dn: -2.0, up: 2.0}}, 1: {stat: {dn: -11.0, up: 11.0}, sys: {dn: -2.0, up: 2.0}}, 2: {stat: {dn: -13.0, up: 13.0}, sys: {dn: -2.0, up: 2.0}}, 3: {stat: {dn: -13.0, up: 13.0}, sys: {dn: -2.0, up: 2.0}}, 4: {stat: {dn: -22.0, up: 22.0}, sys: {dn: -3.0, up: 3.0}}, 5: {stat: {dn: -17.0, up: 17.0}, sys: {dn: -2.0, up: 2.0}}, 6: {stat: {dn: -16.0, up: 16.0}, sys: {dn: -2.0, up: 2.0}}, 7: {stat: {dn: -16.0, up: 16.0}, sys: {dn: -1.0, up: 1.0}}, 8: {stat: {dn: -13.0, up: 13.0}, sys: {dn: -1.0, up: 1.0}}, 9: {stat: {dn: -11.0, up: 11.0}, sys: {dn: -1.0, up: 1.0}}, 10: {stat: {dn: -9.0, up: 9.0}, sys: {dn: -1.0, up: 1.0}}, 11: {stat: {dn: -6.9, up: 6.9}, sys: {dn: -0.6, up: 0.6}}, 12: {stat: {dn: -6.6, up: 6.6}, sys: {dn: -0.3, up: 0.3}}, 13: {stat: {dn: -6.2, up: 6.2}, sys: {dn: -0.5, up: 0.5}}, 14: {stat: {dn: -5.3, up: 5.3}, sys: {dn: -0.3, up: 0.3}}, 15: {stat: {dn: -6.9, up: 6.9}, sys: {dn: -0.6, up: 0.6}}, 16: {stat: {dn: -6.6, up: 6.6}, sys: {dn: -0.7, up: 0.7}}, 17: {stat: {dn: -4.5, up: 4.5}, sys: {dn: -1.2, up: 1.2}}, 18: {stat: {dn: -5.3, up: 5.3}, sys: {dn: -0.7, up: 0.7}}, 19: {stat: {dn: -5.3, up: 5.3}, sys: {dn: -1.9, up: 1.9}}, 20: {stat: {dn: -6.9, up: 6.9}, sys: {dn: -2.0, up: 2.0}}} + +IsRef: 1 +Path: /REF/BABAR_2015_I1383130/d01-x01-y01 +Title: doi:10.17182/hepdata.73784.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.650000e+00 5.000000e-02 5.000000e-02 7.500000e+01 9.219544e+00 9.219544e+00 +2.750000e+00 5.000000e-02 5.000000e-02 1.210000e+02 1.118034e+01 1.118034e+01 +2.850000e+00 5.000000e-02 5.000000e-02 1.570000e+02 1.315295e+01 1.315295e+01 +2.950000e+00 5.000000e-02 5.000000e-02 1.520000e+02 1.315295e+01 1.315295e+01 +3.100000e+00 1.000000e-01 1.000000e-01 2.970000e+02 2.220360e+01 2.220360e+01 +3.300000e+00 1.000000e-01 1.000000e-01 2.790000e+02 1.711724e+01 1.711724e+01 +3.500000e+00 1.000000e-01 1.000000e-01 1.940000e+02 1.612452e+01 1.612452e+01 +3.700000e+00 1.000000e-01 1.000000e-01 1.620000e+02 1.603122e+01 1.603122e+01 +3.900000e+00 1.000000e-01 1.000000e-01 1.520000e+02 1.303840e+01 1.303840e+01 +4.100000e+00 1.000000e-01 1.000000e-01 1.050000e+02 1.104536e+01 1.104536e+01 +4.300000e+00 1.000000e-01 1.000000e-01 8.100000e+01 9.055385e+00 9.055385e+00 +4.500000e+00 1.000000e-01 1.000000e-01 4.470000e+01 6.926038e+00 6.926038e+00 +4.700000e+00 1.000000e-01 1.000000e-01 4.120000e+01 6.606815e+00 6.606815e+00 +4.900000e+00 1.000000e-01 1.000000e-01 3.620000e+01 6.220129e+00 6.220129e+00 +5.100000e+00 1.000000e-01 1.000000e-01 2.680000e+01 5.308484e+00 5.308484e+00 +5.350000e+00 1.500000e-01 1.500000e-01 4.520000e+01 6.926038e+00 6.926038e+00 +5.750000e+00 2.500000e-01 2.500000e-01 3.460000e+01 6.637017e+00 6.637017e+00 +6.250000e+00 2.500000e-01 2.500000e-01 1.070000e+01 4.657252e+00 4.657252e+00 +6.750000e+00 2.500000e-01 2.500000e-01 1.360000e+01 5.346027e+00 5.346027e+00 +7.250000e+00 2.500000e-01 2.500000e-01 7.400000e+00 5.630275e+00 5.630275e+00 +7.750000e+00 2.500000e-01 2.500000e-01 0.000000e+00 7.184010e+00 7.184010e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2015_I1383130/d01-x01-y02 +Variations: [""] +ErrorBreakdown: {} + +IsRef: 1 +Path: /REF/BABAR_2015_I1383130/d01-x01-y02 +Title: doi:10.17182/hepdata.73784.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.650000e+00 5.000000e-02 5.000000e-02 9.600000e-01 0.000000e+00 0.000000e+00 +2.750000e+00 5.000000e-02 5.000000e-02 1.940000e+00 0.000000e+00 0.000000e+00 +2.850000e+00 5.000000e-02 5.000000e-02 3.030000e+00 0.000000e+00 0.000000e+00 +2.950000e+00 5.000000e-02 5.000000e-02 3.690000e+00 0.000000e+00 0.000000e+00 +3.100000e+00 1.000000e-01 1.000000e-01 5.070000e+00 0.000000e+00 0.000000e+00 +3.300000e+00 1.000000e-01 1.000000e-01 6.430000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 1.000000e-01 1.000000e-01 7.810000e+00 0.000000e+00 0.000000e+00 +3.700000e+00 1.000000e-01 1.000000e-01 9.150000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 1.000000e-01 1.000000e-01 9.800000e+00 0.000000e+00 0.000000e+00 +4.100000e+00 1.000000e-01 1.000000e-01 1.080000e+01 0.000000e+00 0.000000e+00 +4.300000e+00 1.000000e-01 1.000000e-01 1.100000e+01 0.000000e+00 0.000000e+00 +4.500000e+00 1.000000e-01 1.000000e-01 1.190000e+01 0.000000e+00 0.000000e+00 +4.700000e+00 1.000000e-01 1.000000e-01 1.250000e+01 0.000000e+00 0.000000e+00 +4.900000e+00 1.000000e-01 1.000000e-01 1.310000e+01 0.000000e+00 0.000000e+00 +5.100000e+00 1.000000e-01 1.000000e-01 1.290000e+01 0.000000e+00 0.000000e+00 +5.350000e+00 1.500000e-01 1.500000e-01 1.440000e+01 0.000000e+00 0.000000e+00 +5.750000e+00 2.500000e-01 2.500000e-01 1.350000e+01 0.000000e+00 0.000000e+00 +6.250000e+00 2.500000e-01 2.500000e-01 1.060000e+01 0.000000e+00 0.000000e+00 +6.750000e+00 2.500000e-01 2.500000e-01 1.160000e+01 0.000000e+00 0.000000e+00 +7.250000e+00 2.500000e-01 2.500000e-01 1.190000e+01 0.000000e+00 0.000000e+00 +7.750000e+00 2.500000e-01 2.500000e-01 9.360000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2015_I1383130/d01-x01-y03 +Variations: [""] +ErrorBreakdown: {} + +IsRef: 1 +Path: /REF/BABAR_2015_I1383130/d01-x01-y03 +Title: doi:10.17182/hepdata.73784.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.650000e+00 5.000000e-02 5.000000e-02 1.130000e+02 0.000000e+00 0.000000e+00 +2.750000e+00 5.000000e-02 5.000000e-02 1.180000e+02 0.000000e+00 0.000000e+00 +2.850000e+00 5.000000e-02 5.000000e-02 1.220000e+02 0.000000e+00 0.000000e+00 +2.950000e+00 5.000000e-02 5.000000e-02 1.270000e+02 0.000000e+00 0.000000e+00 +3.100000e+00 1.000000e-01 1.000000e-01 2.710000e+02 0.000000e+00 0.000000e+00 +3.300000e+00 1.000000e-01 1.000000e-01 2.920000e+02 0.000000e+00 0.000000e+00 +3.500000e+00 1.000000e-01 1.000000e-01 3.130000e+02 0.000000e+00 0.000000e+00 +3.700000e+00 1.000000e-01 1.000000e-01 3.360000e+02 0.000000e+00 0.000000e+00 +3.900000e+00 1.000000e-01 1.000000e-01 3.610000e+02 0.000000e+00 0.000000e+00 +4.100000e+00 1.000000e-01 1.000000e-01 3.860000e+02 0.000000e+00 0.000000e+00 +4.300000e+00 1.000000e-01 1.000000e-01 4.130000e+02 0.000000e+00 0.000000e+00 +4.500000e+00 1.000000e-01 1.000000e-01 4.420000e+02 0.000000e+00 0.000000e+00 +4.700000e+00 1.000000e-01 1.000000e-01 4.730000e+02 0.000000e+00 0.000000e+00 +4.900000e+00 1.000000e-01 1.000000e-01 5.070000e+02 0.000000e+00 0.000000e+00 +5.100000e+00 1.000000e-01 1.000000e-01 5.430000e+02 0.000000e+00 0.000000e+00 +5.350000e+00 1.500000e-01 1.500000e-01 8.880000e+02 0.000000e+00 0.000000e+00 +5.750000e+00 2.500000e-01 2.500000e-01 1.710000e+03 0.000000e+00 0.000000e+00 +6.250000e+00 2.500000e-01 2.500000e-01 2.062000e+03 0.000000e+00 0.000000e+00 +6.750000e+00 2.500000e-01 2.500000e-01 2.523000e+03 0.000000e+00 0.000000e+00 +7.250000e+00 2.500000e-01 2.500000e-01 3.144000e+03 0.000000e+00 0.000000e+00 +7.750000e+00 2.500000e-01 2.500000e-01 4.015000e+03 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2015_I1383130/d01-x01-y04 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -8.1, up: 8.1}, sys: {dn: -3.7, up: 3.7}}, 1: {stat: {dn: -4.9, up: 4.9}, sys: {dn: -2.4, up: 2.4}}, 2: {stat: {dn: -3.4, up: 3.4}, sys: {dn: -1.6, up: 1.6}}, 3: {stat: {dn: -2.7, up: 2.7}, sys: {dn: -1.2, up: 1.2}}, 4: {stat: {dn: -1.6, up: 1.6}, sys: {dn: -0.6, up: 0.6}}, 5: {stat: {dn: -0.9, up: 0.9}, sys: {dn: -0.4, up: 0.4}}, 6: {stat: {dn: -0.63, up: 0.63}, sys: {dn: -0.24, up: 0.24}}, 7: {stat: {dn: -0.51, up: 0.51}, sys: {dn: -0.16, up: 0.16}}, 8: {stat: {dn: -0.36, up: 0.36}, sys: {dn: -0.13, up: 0.13}}, 9: {stat: {dn: -0.25, up: 0.25}, sys: {dn: -0.08, up: 0.08}}, 10: {stat: {dn: -0.2, up: 0.2}, sys: {dn: -0.06, up: 0.06}}, 11: {stat: {dn: -0.13, up: 0.13}, sys: {dn: -0.03, up: 0.03}}, 12: {stat: {dn: -0.11, up: 0.11}, sys: {dn: -0.03, up: 0.03}}, 13: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.02, up: 0.02}}, 14: {stat: {dn: -0.08, up: 0.08}, sys: {dn: -0.02, up: 0.02}}, 15: {stat: {dn: -0.05, up: 0.05}, sys: {dn: -0.01, up: 0.01}}, 16: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.006, up: 0.006}}, 17: {stat: {dn: -0.021, up: 0.021}, sys: {dn: -0.006, up: 0.006}}, 18: {stat: {dn: -0.018, up: 0.018}, sys: {dn: -0.004, up: 0.004}}, 19: {stat: {dn: -0.014, up: 0.014}, sys: {dn: -0.004, up: 0.004}}} + +IsRef: 1 +Path: /REF/BABAR_2015_I1383130/d01-x01-y04 +Title: doi:10.17182/hepdata.73784.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.650000e+00 5.000000e-02 5.000000e-02 6.930000e+01 8.905055e+00 8.905055e+00 +2.750000e+00 5.000000e-02 5.000000e-02 5.290000e+01 5.456189e+00 5.456189e+00 +2.850000e+00 5.000000e-02 5.000000e-02 4.200000e+01 3.757659e+00 3.757659e+00 +2.950000e+00 5.000000e-02 5.000000e-02 3.220000e+01 2.954657e+00 2.954657e+00 +3.100000e+00 1.000000e-01 1.000000e-01 2.170000e+01 1.708801e+00 1.708801e+00 +3.300000e+00 1.000000e-01 1.000000e-01 1.480000e+01 9.848858e-01 9.848858e-01 +3.500000e+00 1.000000e-01 1.000000e-01 7.920000e+00 6.741662e-01 6.741662e-01 +3.700000e+00 1.000000e-01 1.000000e-01 5.260000e+00 5.345091e-01 5.345091e-01 +3.900000e+00 1.000000e-01 1.000000e-01 4.300000e+00 3.827532e-01 3.827532e-01 +4.100000e+00 1.000000e-01 1.000000e-01 2.520000e+00 2.624881e-01 2.624881e-01 +4.300000e+00 1.000000e-01 1.000000e-01 1.790000e+00 2.088061e-01 2.088061e-01 +4.500000e+00 1.000000e-01 1.000000e-01 8.500000e-01 1.334166e-01 1.334166e-01 +4.700000e+00 1.000000e-01 1.000000e-01 7.000000e-01 1.140175e-01 1.140175e-01 +4.900000e+00 1.000000e-01 1.000000e-01 5.500000e-01 9.219544e-02 9.219544e-02 +5.100000e+00 1.000000e-01 1.000000e-01 3.800000e-01 8.246211e-02 8.246211e-02 +5.350000e+00 1.500000e-01 1.500000e-01 3.500000e-01 5.099020e-02 5.099020e-02 +5.750000e+00 2.500000e-01 2.500000e-01 1.500000e-01 2.961419e-02 2.961419e-02 +6.250000e+00 2.500000e-01 2.500000e-01 4.900000e-02 2.184033e-02 2.184033e-02 +6.750000e+00 2.500000e-01 2.500000e-01 4.700000e-02 1.843909e-02 1.843909e-02 +7.250000e+00 2.500000e-01 2.500000e-01 2.000000e-02 1.456022e-02 1.456022e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2015_I1383130/d01-x01-y05 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -1.1, up: 1.1}}, 1: {error: {dn: -0.8, up: 0.8}}, 2: {error: {dn: -0.6, up: 0.6}}, 3: {error: {dn: -0.6, up: 0.6}}, 4: {error: {dn: -0.4, up: 0.4}}, 5: {error: {dn: -0.3, up: 0.3}}, 6: {error: {dn: -0.3, up: 0.3}}, 7: {error: {dn: -0.3, up: 0.3}}, 8: {error: {dn: -0.3, up: 0.3}}, 9: {error: {dn: -0.25, up: 0.25}}, 10: {error: {dn: -0.25, up: 0.25}}, 11: {error: {dn: -0.23, up: 0.23}}, 12: {error: {dn: -0.23, up: 0.23}}, 13: {error: {dn: -0.22, up: 0.22}}, 14: {error: {dn: -0.22, up: 0.22}}, 15: {error: {dn: -0.18, up: 0.18}}, 16: {error: {dn: -0.15, up: 0.15}}, 17: {error: {dn: -0.22, up: 0.22}}, 18: {error: {dn: -0.2, up: 0.2}}, 19: {error: {dn: -0.36, up: 0.23}}} + +IsRef: 1 +Path: /REF/BABAR_2015_I1383130/d01-x01-y05 +Title: doi:10.17182/hepdata.73784.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.650000e+00 5.000000e-02 5.000000e-02 1.670000e+01 1.100000e+00 1.100000e+00 +2.750000e+00 5.000000e-02 5.000000e-02 1.500000e+01 8.000000e-01 8.000000e-01 +2.850000e+00 5.000000e-02 5.000000e-02 1.370000e+01 6.000000e-01 6.000000e-01 +2.950000e+00 5.000000e-02 5.000000e-02 1.240000e+01 6.000000e-01 6.000000e-01 +3.100000e+00 1.000000e-01 1.000000e-01 1.060000e+01 4.000000e-01 4.000000e-01 +3.300000e+00 1.000000e-01 1.000000e-01 9.200000e+00 3.000000e-01 3.000000e-01 +3.500000e+00 1.000000e-01 1.000000e-01 7.100000e+00 3.000000e-01 3.000000e-01 +3.700000e+00 1.000000e-01 1.000000e-01 6.100000e+00 3.000000e-01 3.000000e-01 +3.900000e+00 1.000000e-01 1.000000e-01 5.700000e+00 3.000000e-01 3.000000e-01 +4.100000e+00 1.000000e-01 1.000000e-01 4.600000e+00 2.500000e-01 2.500000e-01 +4.300000e+00 1.000000e-01 1.000000e-01 4.050000e+00 2.500000e-01 2.500000e-01 +4.500000e+00 1.000000e-01 1.000000e-01 2.910000e+00 2.300000e-01 2.300000e-01 +4.700000e+00 1.000000e-01 1.000000e-01 2.740000e+00 2.300000e-01 2.300000e-01 +4.900000e+00 1.000000e-01 1.000000e-01 2.520000e+00 2.200000e-01 2.200000e-01 +5.100000e+00 1.000000e-01 1.000000e-01 2.190000e+00 2.200000e-01 2.200000e-01 +5.350000e+00 1.500000e-01 1.500000e-01 2.210000e+00 1.800000e-01 1.800000e-01 +5.750000e+00 2.500000e-01 2.500000e-01 1.540000e+00 1.500000e-01 1.500000e-01 +6.250000e+00 2.500000e-01 2.500000e-01 9.500000e-01 2.200000e-01 2.200000e-01 +6.750000e+00 2.500000e-01 2.500000e-01 1.000000e+00 2.000000e-01 2.000000e-01 +7.250000e+00 2.500000e-01 2.500000e-01 7.000000e-01 3.600000e-01 2.300000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2017_I1511276.cc b/analyses/pluginBABAR/BABAR_2017_I1511276.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1511276.cc @@ -0,0 +1,164 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2017_I1511276 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2017_I1511276); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + _nKKpi = bookCounter("TMP/KKpi"); + _nPhipi = bookCounter("TMP/Phipi"); + _nKKeta = bookCounter("TMP/KKeta"); + _nKKpipi = bookCounter("TMP/KKpipi");; + + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // stable histos + if( ntotal == 3 && nCount[130] == 1 && + nCount[310] == 1 && nCount[111] == 1) + _nKKpi->fill(event.weight()); + else if( ntotal == 4 && nCount[130] == 1 && + nCount[310] == 1 && nCount[111] == 2) + _nKKpipi->fill(event.weight()); + // unstable particles + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=333 && p.pdgId()!=221) continue; + map nRes=nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + bool matched = true; + if(p.pdgId()==333 && ncount==1) { + for(auto const & val : nRes) { + if(val.first==111) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nPhipi->fill(event.weight()); + } + else if(p.pdgId()==221 && ncount==2) { + for(auto const & val : nRes) { + if(val.first==130 || val.first==310) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nKKeta->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<5;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _nKKpi->val(); + error = _nKKpi->err(); + } + else if (ix==2) { + sigma = _nPhipi->val(); + error = _nPhipi->err(); + } + else if (ix==3) { + sigma = _nKKeta->val(); + error = _nKKeta->err(); + } + else if (ix==4) { + sigma = _nKKpipi->val(); + error = _nKKpipi->err(); + } + + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nKKpi,_nPhipi,_nKKeta,_nKKpipi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2017_I1511276); + + +} diff --git a/analyses/pluginBABAR/BABAR_2017_I1511276.info b/analyses/pluginBABAR/BABAR_2017_I1511276.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1511276.info @@ -0,0 +1,37 @@ +Name: BABAR_2017_I1511276 +Year: 2017 +Summary: Cross section for $e^+e^-\to K_S^0K_L^0$ with $\pi^0$, $\eta$ and $\pi^0\pi^0$ between threshold and 4 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 1511276 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D95 (2017) no.5, 052001 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Cross section for $e^+e^-\to K_S^0K_L^0$ with $\pi^0$, $\eta$ and $\pi^0\pi^0$ between threshold and 4 GeV using radiative events.' +Keywords: +BibKey: TheBABAR:2017vgl +BibTeX: '@article{TheBABAR:2017vgl, + author = "Lees, J. P. and others", + title = "{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}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D95", + year = "2017", + number = "5", + pages = "052001", + doi = "10.1103/PhysRevD.95.052001", + eprint = "1701.08297", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BABAR-PUB-16-004, SLAC-PUB-16918", + SLACcitation = "%%CITATION = ARXIV:1701.08297;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2017_I1511276.plot b/analyses/pluginBABAR/BABAR_2017_I1511276.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1511276.plot @@ -0,0 +1,25 @@ +BEGIN PLOT /BABAR_2017_I1511276/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2017_I1511276/d02-x01-y01 +Title=$\sigma(e^+e^-\to \phi\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2017_I1511276/d03-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L\eta)$/nb +ConnectGaps=1 +LogY=0 +END PLOT +BEGIN PLOT /BABAR_2017_I1511276/d04-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L\pi^0\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L\pi^0\pi^0)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2017_I1511276.yoda b/analyses/pluginBABAR/BABAR_2017_I1511276.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1511276.yoda @@ -0,0 +1,177 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2017_I1511276/d01-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2017_I1511276/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.42500 0.00000 0.00000 2.80000e-01 7.00000e-02 7.00000e-02 +1.47500 0.00000 0.00000 9.40000e-01 1.50000e-01 1.50000e-01 +1.52500 0.00000 0.00000 1.68000e+00 2.20000e-01 2.20000e-01 +1.57500 0.00000 0.00000 2.60000e+00 2.80000e-01 2.80000e-01 +1.62500 0.00000 0.00000 2.89000e+00 2.60000e-01 2.60000e-01 +1.67500 0.00000 0.00000 3.15000e+00 3.00000e-01 3.00000e-01 +1.72500 0.00000 0.00000 2.79000e+00 2.90000e-01 2.90000e-01 +1.77500 0.00000 0.00000 1.96000e+00 2.30000e-01 2.30000e-01 +1.82500 0.00000 0.00000 1.30000e+00 1.80000e-01 1.80000e-01 +1.87500 0.00000 0.00000 1.12000e+00 1.80000e-01 1.80000e-01 +1.92500 0.00000 0.00000 7.90000e-01 1.20000e-01 1.20000e-01 +1.97500 0.00000 0.00000 5.50000e-01 1.00000e-01 1.00000e-01 +2.02500 0.00000 0.00000 5.80000e-01 1.10000e-01 1.10000e-01 +2.07500 0.00000 0.00000 5.50000e-01 1.10000e-01 1.10000e-01 +2.12500 0.00000 0.00000 4.40000e-01 9.00000e-02 9.00000e-02 +2.17500 0.00000 0.00000 4.20000e-01 9.00000e-02 9.00000e-02 +2.22500 0.00000 0.00000 3.60000e-01 8.00000e-02 8.00000e-02 +2.27500 0.00000 0.00000 4.80000e-01 9.00000e-02 9.00000e-02 +2.32500 0.00000 0.00000 3.10000e-01 7.00000e-02 7.00000e-02 +2.37500 0.00000 0.00000 1.80000e-01 7.00000e-02 7.00000e-02 +2.42500 0.00000 0.00000 2.60000e-01 7.00000e-02 7.00000e-02 +2.47500 0.00000 0.00000 2.50000e-01 8.00000e-02 8.00000e-02 +2.52500 0.00000 0.00000 1.90000e-01 6.00000e-02 6.00000e-02 +2.57500 0.00000 0.00000 9.00000e-02 4.00000e-02 4.00000e-02 +2.62500 0.00000 0.00000 1.40000e-01 5.00000e-02 5.00000e-02 +2.67500 0.00000 0.00000 7.00000e-02 3.00000e-02 3.00000e-02 +2.72500 0.00000 0.00000 1.20000e-01 5.00000e-02 5.00000e-02 +2.77500 0.00000 0.00000 1.20000e-01 8.00000e-02 8.00000e-02 +2.82500 0.00000 0.00000 1.00000e-01 6.00000e-02 6.00000e-02 +2.87500 0.00000 0.00000 1.50000e-01 1.00000e-01 1.00000e-01 +2.92500 0.00000 0.00000 4.00000e-02 3.00000e-02 3.00000e-02 +2.97500 0.00000 0.00000 1.00000e-01 1.00000e-01 1.00000e-01 +3.02500 0.00000 0.00000 6.00000e-02 3.00000e-02 3.00000e-02 +3.07500 0.00000 0.00000 3.10000e-01 9.00000e-02 9.00000e-02 +3.12500 0.00000 0.00000 2.40000e-01 1.20000e-01 1.20000e-01 +3.17500 0.00000 0.00000 5.00000e-02 4.00000e-02 4.00000e-02 +3.22500 0.00000 0.00000 2.00000e-02 3.00000e-02 3.00000e-02 +3.27500 0.00000 0.00000 4.00000e-02 3.00000e-02 3.00000e-02 +3.32500 0.00000 0.00000 5.00000e-02 4.00000e-02 4.00000e-02 +3.37500 0.00000 0.00000 3.00000e-02 4.00000e-02 4.00000e-02 +3.42500 0.00000 0.00000 2.00000e-02 1.00000e-02 1.00000e-02 +3.47500 0.00000 0.00000 5.00000e-02 3.00000e-02 3.00000e-02 +3.52500 0.00000 0.00000 1.00000e-02 3.00000e-02 3.00000e-02 +3.57500 0.00000 0.00000 4.00000e-02 3.00000e-02 3.00000e-02 +3.62500 0.00000 0.00000 3.00000e-02 3.00000e-02 3.00000e-02 +3.67500 0.00000 0.00000 0.00000e+00 1.00000e-02 1.00000e-02 +3.72500 0.00000 0.00000 4.00000e-02 4.00000e-02 4.00000e-02 +3.77500 0.00000 0.00000 1.00000e-02 1.00000e-02 1.00000e-02 +3.82500 0.00000 0.00000 3.00000e-02 2.00000e-02 2.00000e-02 +3.87500 0.00000 0.00000 0.00000e+00 1.00000e-02 1.00000e-02 +3.92500 0.00000 0.00000 2.00000e-02 2.00000e-02 2.00000e-02 +3.97500 0.00000 0.00000 1.00000e-02 1.00000e-02 1.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2017_I1511276/d02-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2017_I1511276/d02-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.25000 0.00000 0.00000 0.00000e+00 2.00000e-02 2.00000e-02 +1.35000 0.00000 0.00000 0.00000e+00 2.00000e-02 2.00000e-02 +1.45000 0.00000 0.00000 6.00000e-02 6.00000e-02 6.00000e-02 +1.55000 0.00000 0.00000 1.70000e-01 6.00000e-02 6.00000e-02 +1.65000 0.00000 0.00000 4.00000e-02 3.00000e-02 3.00000e-02 +1.75000 0.00000 0.00000 5.00000e-02 3.00000e-02 3.00000e-02 +1.85000 0.00000 0.00000 2.00000e-02 2.00000e-02 2.00000e-02 +1.95000 0.00000 0.00000 0.00000e+00 1.00000e-02 1.00000e-02 +2.05000 0.00000 0.00000 3.00000e-02 2.00000e-02 2.00000e-02 +2.15000 0.00000 0.00000 0.00000e+00 1.00000e-02 1.00000e-02 +2.25000 0.00000 0.00000 1.00000e-02 1.00000e-02 1.00000e-02 +2.35000 0.00000 0.00000 2.00000e-02 2.00000e-02 2.00000e-02 +2.45000 0.00000 0.00000 2.00000e-02 1.00000e-02 1.00000e-02 +2.55000 0.00000 0.00000 0.00000e+00 1.00000e-02 1.00000e-02 +2.65000 0.00000 0.00000 1.00000e-02 1.00000e-02 1.00000e-02 +2.75000 0.00000 0.00000 0.00000e+00 1.00000e-02 1.00000e-02 +2.85000 0.00000 0.00000 0.00000e+00 1.00000e-02 1.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2017_I1511276/d03-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2017_I1511276/d03-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.57500 0.00000 0.00000 1.20000e-01 1.40000e-01 1.40000e-01 +1.62500 0.00000 0.00000 5.20000e-01 1.40000e-01 1.40000e-01 +1.67500 0.00000 0.00000 7.80000e-01 1.80000e-01 1.80000e-01 +1.72500 0.00000 0.00000 1.01000e+00 2.30000e-01 2.30000e-01 +1.77500 0.00000 0.00000 5.00000e-01 1.40000e-01 1.40000e-01 +1.82500 0.00000 0.00000 5.30000e-01 1.40000e-01 1.40000e-01 +1.87500 0.00000 0.00000 4.10000e-01 1.20000e-01 1.20000e-01 +1.92500 0.00000 0.00000 3.60000e-01 1.20000e-01 1.20000e-01 +1.97500 0.00000 0.00000 2.80000e-01 9.00000e-02 9.00000e-02 +2.02500 0.00000 0.00000 4.60000e-01 1.10000e-01 1.10000e-01 +2.07500 0.00000 0.00000 4.10000e-01 1.20000e-01 1.20000e-01 +2.12500 0.00000 0.00000 4.50000e-01 1.20000e-01 1.20000e-01 +2.17500 0.00000 0.00000 4.40000e-01 1.10000e-01 1.10000e-01 +2.22500 0.00000 0.00000 4.90000e-01 1.20000e-01 1.20000e-01 +2.27500 0.00000 0.00000 3.00000e-01 1.10000e-01 1.10000e-01 +2.32500 0.00000 0.00000 3.10000e-01 9.00000e-02 9.00000e-02 +2.37500 0.00000 0.00000 3.00000e-01 1.00000e-01 1.00000e-01 +2.42500 0.00000 0.00000 3.20000e-01 1.00000e-01 1.00000e-01 +2.47500 0.00000 0.00000 1.90000e-01 7.00000e-02 7.00000e-02 +2.52500 0.00000 0.00000 1.20000e-01 6.00000e-02 6.00000e-02 +2.57500 0.00000 0.00000 2.90000e-01 9.00000e-02 9.00000e-02 +2.62500 0.00000 0.00000 1.10000e-01 6.00000e-02 6.00000e-02 +2.67500 0.00000 0.00000 1.90000e-01 8.00000e-02 8.00000e-02 +2.72500 0.00000 0.00000 1.50000e-01 6.00000e-02 6.00000e-02 +2.77500 0.00000 0.00000 1.00000e-01 5.00000e-02 5.00000e-02 +2.82500 0.00000 0.00000 8.00000e-02 5.00000e-02 5.00000e-02 +2.87500 0.00000 0.00000 1.40000e-01 6.00000e-02 6.00000e-02 +2.92500 0.00000 0.00000 5.00000e-02 4.00000e-02 4.00000e-02 +2.97500 0.00000 0.00000 5.00000e-02 6.00000e-02 6.00000e-02 +3.02500 0.00000 0.00000 1.40000e-01 6.00000e-02 6.00000e-02 +3.07500 0.00000 0.00000 2.20000e-01 6.00000e-02 6.00000e-02 +3.12500 0.00000 0.00000 9.00000e-02 5.00000e-02 5.00000e-02 +3.17500 0.00000 0.00000 3.00000e-02 4.00000e-02 4.00000e-02 +3.22500 0.00000 0.00000 -1.00000e-02 3.00000e-02 3.00000e-02 +3.27500 0.00000 0.00000 4.00000e-02 4.00000e-02 4.00000e-02 +3.32500 0.00000 0.00000 5.00000e-02 3.00000e-02 3.00000e-02 +3.37500 0.00000 0.00000 1.00000e-02 2.00000e-02 2.00000e-02 +3.42500 0.00000 0.00000 2.00000e-02 3.00000e-02 3.00000e-02 +3.47500 0.00000 0.00000 1.00000e-02 2.00000e-02 2.00000e-02 +3.52500 0.00000 0.00000 2.00000e-02 2.00000e-02 2.00000e-02 +3.57500 0.00000 0.00000 -1.00000e-02 2.00000e-02 2.00000e-02 +3.62500 0.00000 0.00000 -1.00000e-02 1.00000e-02 1.00000e-02 +3.67500 0.00000 0.00000 7.00000e-02 3.00000e-02 3.00000e-02 +3.72500 0.00000 0.00000 4.00000e-02 3.00000e-02 3.00000e-02 +3.77500 0.00000 0.00000 7.00000e-02 4.00000e-02 4.00000e-02 +3.82500 0.00000 0.00000 1.00000e-02 2.00000e-02 2.00000e-02 +3.87500 0.00000 0.00000 1.00000e-02 2.00000e-02 2.00000e-02 +3.92500 0.00000 0.00000 1.00000e-02 2.00000e-02 2.00000e-02 +3.97500 0.00000 0.00000 2.00000e-02 2.00000e-02 2.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2017_I1511276/d04-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2017_I1511276/d04-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.35000 0.00000 0.00000 1.80000e-02 2.90000e-02 2.90000e-02 +1.45000 0.00000 0.00000 5.90000e-02 7.00000e-02 7.00000e-02 +1.55000 0.00000 0.00000 3.34000e-01 1.08000e-01 1.08000e-01 +1.65000 0.00000 0.00000 3.50000e-01 1.15000e-01 1.15000e-01 +1.75000 0.00000 0.00000 5.49000e-01 1.62000e-01 1.62000e-01 +1.85000 0.00000 0.00000 2.90000e-01 1.13000e-01 1.13000e-01 +1.95000 0.00000 0.00000 1.13000e-01 1.03000e-01 1.03000e-01 +2.05000 0.00000 0.00000 1.85000e-01 1.04000e-01 1.04000e-01 +2.15000 0.00000 0.00000 1.41000e-01 9.80000e-02 9.80000e-02 +2.25000 0.00000 0.00000 3.80000e-02 8.80000e-02 8.80000e-02 +2.35000 0.00000 0.00000 8.00000e-03 8.10000e-02 8.10000e-02 +2.45000 0.00000 0.00000 -2.20000e-02 7.30000e-02 7.30000e-02 +2.55000 0.00000 0.00000 8.00000e-02 7.40000e-02 7.40000e-02 +2.65000 0.00000 0.00000 -1.90000e-02 6.20000e-02 6.20000e-02 +2.75000 0.00000 0.00000 2.90000e-02 5.90000e-02 5.90000e-02 +2.85000 0.00000 0.00000 2.80000e-02 5.40000e-02 5.40000e-02 +2.95000 0.00000 0.00000 5.10000e-02 8.30000e-02 8.30000e-02 +3.05000 0.00000 0.00000 2.13000e-01 8.10000e-02 8.10000e-02 +3.15000 0.00000 0.00000 -2.00000e-03 7.10000e-02 7.10000e-02 +3.25000 0.00000 0.00000 2.00000e-03 3.30000e-02 3.30000e-02 +3.35000 0.00000 0.00000 -2.00000e-03 2.90000e-02 2.90000e-02 +3.45000 0.00000 0.00000 3.10000e-02 2.90000e-02 2.90000e-02 +3.55000 0.00000 0.00000 1.50000e-02 2.50000e-02 2.50000e-02 +3.65000 0.00000 0.00000 -1.50000e-02 2.00000e-02 2.00000e-02 +3.75000 0.00000 0.00000 5.20000e-02 2.40000e-02 2.40000e-02 +3.85000 0.00000 0.00000 2.00000e-03 1.80000e-02 1.80000e-02 +3.95000 0.00000 0.00000 -1.60000e-02 1.60000e-02 1.60000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2017_I1591716.cc b/analyses/pluginBABAR/BABAR_2017_I1591716.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1591716.cc @@ -0,0 +1,143 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2017_I1591716 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2017_I1591716); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + _nKKpipi = bookCounter("TMP/KKpipi"); + _nKKpieta = bookCounter("TMP/KKpieta"); + + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // stable histos + if( ntotal == 4 && nCount[310] == 1 && nCount[111] == 1 && + ( (nCount[ 321]==1 && nCount[-211]==1) || + (nCount[-321]==1 && nCount[ 211]==1))) + _nKKpipi->fill(event.weight()); + + // unstable particles + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=221) continue; + map nRes=nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + bool matched = true; + if(p.pdgId()==221 && ncount==3) { + for(auto const & val : nRes) { + if(val.first==310 || val.first==111) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(abs(val.first)==321 || abs(val.first)==211) + continue; + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if((nRes[321]==1 && nRes[-211]==1 && nRes[-321]==0 && nRes[211]==0) || + (nRes[321]==0 && nRes[-211]==0 && nRes[-321]==1 && nRes[211]==1)) + _nKKpieta->fill(event.weight()); + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _nKKpipi->val(); + error = _nKKpipi->err(); + } + else if (ix==2) { + sigma = _nKKpieta->val(); + error = _nKKpieta->err(); + } + + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nKKpipi,_nKKpieta; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2017_I1591716); + + +} diff --git a/analyses/pluginBABAR/BABAR_2017_I1591716.info b/analyses/pluginBABAR/BABAR_2017_I1591716.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1591716.info @@ -0,0 +1,40 @@ +Name: BABAR_2017_I1591716 +Year: 2017 +Summary: Cross section for $e^+e^-\to K_S^0K^\pm\pi^\mp$ with $\pi^0$, $\eta$ between threshold and 4 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 1591716 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D95 (2017) no.9, 092005 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Cross section for $e^+e^-\to K_S^0K^\pm\pi^\mp$ with $\pi^0$, $\eta$ between threshold and 4 GeV using radiative events.' +Keywords: +BibKey: TheBABAR:2017aph +BibTeX: '@article{TheBABAR:2017aph, + author = "Lees, J. P. and others", + title = "{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}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D95", + year = "2017", + number = "9", + pages = "092005", + doi = "10.1103/PhysRevD.95.092005", + eprint = "1704.05009", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BABAR-PUB-15-005, SLAC-PUB-16940", + SLACcitation = "%%CITATION = ARXIV:1704.05009;%%" +}' +ToDo: + - Implement the analysis, test it, remove this ToDo, and mark as VALIDATED :-) + diff --git a/analyses/pluginBABAR/BABAR_2017_I1591716.plot b/analyses/pluginBABAR/BABAR_2017_I1591716.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1591716.plot @@ -0,0 +1,12 @@ +BEGIN PLOT /BABAR_2017_I1591716/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^\pm\pi^\mp\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^\pm\pi^\mp\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BABAR_2017_I1591716/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^\pm\pi^\mp\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^\pm\pi^\mp\eta)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2017_I1591716.yoda b/analyses/pluginBABAR/BABAR_2017_I1591716.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1591716.yoda @@ -0,0 +1,241 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2017_I1591716/d01-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2017_I1591716/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.51000 0.00000 0.00000 5.00000e-02 3.00000e-02 3.00000e-02 +1.53000 0.00000 0.00000 5.00000e-02 3.00000e-02 3.00000e-02 +1.55000 0.00000 0.00000 2.00000e-02 2.00000e-02 2.00000e-02 +1.57000 0.00000 0.00000 6.00000e-02 4.00000e-02 4.00000e-02 +1.59000 0.00000 0.00000 1.90000e-01 6.00000e-02 6.00000e-02 +1.61000 0.00000 0.00000 1.60000e-01 6.00000e-02 6.00000e-02 +1.63000 0.00000 0.00000 3.60000e-01 9.00000e-02 9.00000e-02 +1.65000 0.00000 0.00000 5.30000e-01 1.00000e-01 1.00000e-01 +1.67000 0.00000 0.00000 5.20000e-01 1.00000e-01 1.00000e-01 +1.69000 0.00000 0.00000 7.20000e-01 1.20000e-01 1.20000e-01 +1.71000 0.00000 0.00000 7.00000e-01 1.20000e-01 1.20000e-01 +1.73000 0.00000 0.00000 1.09000e+00 1.40000e-01 1.40000e-01 +1.75000 0.00000 0.00000 9.10000e-01 1.30000e-01 1.30000e-01 +1.77000 0.00000 0.00000 1.11000e+00 1.40000e-01 1.40000e-01 +1.79000 0.00000 0.00000 1.48000e+00 1.60000e-01 1.60000e-01 +1.81000 0.00000 0.00000 1.35000e+00 1.50000e-01 1.50000e-01 +1.83000 0.00000 0.00000 1.67000e+00 1.70000e-01 1.70000e-01 +1.85000 0.00000 0.00000 1.73000e+00 1.70000e-01 1.70000e-01 +1.87000 0.00000 0.00000 1.98000e+00 1.80000e-01 1.80000e-01 +1.89000 0.00000 0.00000 2.12000e+00 1.90000e-01 1.90000e-01 +1.91000 0.00000 0.00000 1.99000e+00 1.80000e-01 1.80000e-01 +1.93000 0.00000 0.00000 2.31000e+00 1.90000e-01 1.90000e-01 +1.95000 0.00000 0.00000 2.05000e+00 1.80000e-01 1.80000e-01 +1.97000 0.00000 0.00000 2.32000e+00 1.90000e-01 1.90000e-01 +1.99000 0.00000 0.00000 2.00000e+00 1.80000e-01 1.80000e-01 +2.01000 0.00000 0.00000 1.65000e+00 1.60000e-01 1.60000e-01 +2.03000 0.00000 0.00000 1.67000e+00 1.60000e-01 1.60000e-01 +2.05000 0.00000 0.00000 1.62000e+00 1.60000e-01 1.60000e-01 +2.07000 0.00000 0.00000 1.91000e+00 1.70000e-01 1.70000e-01 +2.09000 0.00000 0.00000 1.44000e+00 1.50000e-01 1.50000e-01 +2.11000 0.00000 0.00000 1.90000e+00 1.70000e-01 1.70000e-01 +2.13000 0.00000 0.00000 1.78000e+00 1.60000e-01 1.60000e-01 +2.15000 0.00000 0.00000 1.73000e+00 1.60000e-01 1.60000e-01 +2.17000 0.00000 0.00000 1.36000e+00 1.40000e-01 1.40000e-01 +2.19000 0.00000 0.00000 1.49000e+00 1.40000e-01 1.40000e-01 +2.21000 0.00000 0.00000 1.42000e+00 1.40000e-01 1.40000e-01 +2.23000 0.00000 0.00000 1.36000e+00 1.40000e-01 1.40000e-01 +2.25000 0.00000 0.00000 1.36000e+00 1.40000e-01 1.40000e-01 +2.27000 0.00000 0.00000 1.15000e+00 1.20000e-01 1.20000e-01 +2.29000 0.00000 0.00000 9.90000e-01 1.20000e-01 1.20000e-01 +2.31000 0.00000 0.00000 9.50000e-01 1.10000e-01 1.10000e-01 +2.33000 0.00000 0.00000 1.25000e+00 1.30000e-01 1.30000e-01 +2.35000 0.00000 0.00000 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2.00000e-02 2.00000e-02 +3.89000 0.00000 0.00000 8.00000e-02 4.00000e-02 4.00000e-02 +3.91000 0.00000 0.00000 0.00000e+00 1.00000e-02 1.00000e-02 +3.93000 0.00000 0.00000 3.00000e-02 2.00000e-02 2.00000e-02 +3.95000 0.00000 0.00000 1.00000e-02 1.00000e-02 1.00000e-02 +3.97000 0.00000 0.00000 5.00000e-02 3.00000e-02 3.00000e-02 +3.99000 0.00000 0.00000 0.00000e+00 0.00000e+00 0.00000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2017_I1621593.cc b/analyses/pluginBABAR/BABAR_2017_I1621593.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1621593.cc @@ -0,0 +1,87 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2017_I1621593 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2017_I1621593); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + _num4pi = bookCounter("TMP/num4"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=4) vetoEvent; + if(nCount[-211]==1&&nCount[211]==1&&nCount[111]==2) + _num4pi->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _num4pi->val(); + double error = _num4pi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + /// @name Histograms + //@{ + CounterPtr _num4pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2017_I1621593); + + +} diff --git a/analyses/pluginBABAR/BABAR_2017_I1621593.info b/analyses/pluginBABAR/BABAR_2017_I1621593.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1621593.info @@ -0,0 +1,36 @@ +Name: BABAR_2017_I1621593 +Year: 2017 +Summary: $e^+e^-\to \pi^+\pi^-\pi^0\pi^0$ cross section from 0.85 to 4.5 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 1621593 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D96 (2017) no.9, 092009 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-\pi^0\pi^0$ between 0.85 to 4.5 GeV using radiative return.' +Keywords: [] +BibKey: TheBaBar:2017vzo +BibTeX: '@article{TheBaBar:2017vzo, + author = "Lees, J. P. and others", + title = "{Measurement of the + ${e}^{+}{e}^{{-}}{\rightarrow}{{\pi}}^{+}{{\pi}}^{{-}}{{\pi}}^{0}{{\pi}}^{0}$ + cross section using initial-state radiation at BABAR}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D96", + year = "2017", + number = "9", + pages = "092009", + doi = "10.1103/PhysRevD.96.092009", + eprint = "1709.01171", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-17147, BABAR-PUB-17-002", + SLACcitation = "%%CITATION = ARXIV:1709.01171;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2017_I1621593.plot b/analyses/pluginBABAR/BABAR_2017_I1621593.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1621593.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /BABAR_2017_I1621593/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0\pi^0)$/nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2017_I1621593.yoda b/analyses/pluginBABAR/BABAR_2017_I1621593.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2017_I1621593.yoda @@ -0,0 +1,382 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2017_I1621593/d01-x01-y01 +IsRef: 1 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0.01000 0.01000 0.13000 0.03000 0.03000 +4.37000 0.01000 0.01000 0.11000 0.02000 0.02000 +4.39000 0.01000 0.01000 0.08000 0.02000 0.02000 +4.41000 0.01000 0.01000 0.10000 0.02000 0.02000 +4.43000 0.01000 0.01000 0.11000 0.02000 0.02000 +4.45000 0.01000 0.01000 0.07000 0.02000 0.02000 +4.47000 0.01000 0.01000 0.07000 0.02000 0.02000 +4.49000 0.01000 0.01000 0.08000 0.02000 0.02000 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2018_I1647139.cc b/analyses/pluginBABAR/BABAR_2018_I1647139.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1647139.cc @@ -0,0 +1,122 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2018_I1647139 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2018_I1647139); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaPiPi = bookCounter("TMP/EtaPiPi"); + + } + + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaPiPi->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _numEtaPiPi->val(); + double error = _numEtaPiPi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numEtaPiPi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2018_I1647139); + + +} diff --git a/analyses/pluginBABAR/BABAR_2018_I1647139.info b/analyses/pluginBABAR/BABAR_2018_I1647139.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1647139.info @@ -0,0 +1,34 @@ +Name: BABAR_2018_I1647139 +Year: 2018 +Summary: Cross section for $e^+e^-\to\eta\pi^+\pi^-$ between 1.2 and 3.5 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 1647139 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D97 (2018) 052007 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to\eta\pi^+\pi^-$ at energies between 1.2 and 3.5 GeV using radiative events.' +Keywords: +BibKey: TheBABAR:2018vvb +BibTeX: '@article{TheBABAR:2018vvb, + author = "Lees, J. P. and others", + title = "{Study of the process $e^+e^- \to \pi^+\pi^-\eta $ using + initial state radiation}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D97", + year = "2018", + pages = "052007", + doi = "10.1103/PhysRevD.97.052007", + eprint = "1801.02960", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BABAR-PUB-17-003, SLAC-PUB-17204", + SLACcitation = "%%CITATION = ARXIV:1801.02960;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2018_I1647139.plot b/analyses/pluginBABAR/BABAR_2018_I1647139.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1647139.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /BABAR_2018_I1647139/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$/nb +LogY=0 +ConnectGaps=1 +LegendXPos=0.7 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2018_I1647139.yoda b/analyses/pluginBABAR/BABAR_2018_I1647139.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1647139.yoda @@ -0,0 +1,65 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2018_I1647139/d01-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2018_I1647139/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.21250 0.01250 0.01250 0.23100 0.08300 0.08300 +1.23750 0.01250 0.01250 0.05800 0.05200 0.05200 +1.26250 0.01250 0.01250 0.22800 0.08100 0.08100 +1.28750 0.01250 0.01250 0.58300 0.11200 0.11200 +1.31250 0.01250 0.01250 0.44400 0.10300 0.10300 +1.33750 0.01250 0.01250 0.91400 0.13400 0.13400 +1.36250 0.01250 0.01250 1.28000 0.15400 0.15400 +1.38750 0.01250 0.01250 1.62800 0.17000 0.17000 +1.41250 0.01250 0.01250 2.10300 0.18900 0.18900 +1.43750 0.01250 0.01250 2.92000 0.21600 0.21600 +1.46250 0.01250 0.01250 3.58200 0.23500 0.23500 +1.48750 0.01250 0.01250 3.69900 0.23700 0.23700 +1.51250 0.01250 0.01250 3.97000 0.24100 0.24100 +1.53750 0.01250 0.01250 4.03500 0.24000 0.24000 +1.56250 0.01250 0.01250 3.82600 0.23100 0.23100 +1.58750 0.01250 0.01250 3.47600 0.21800 0.21800 +1.61250 0.01250 0.01250 3.06500 0.20300 0.20300 +1.63750 0.01250 0.01250 2.73200 0.18900 0.18900 +1.66250 0.01250 0.01250 2.52800 0.17900 0.17900 +1.68750 0.01250 0.01250 2.16100 0.16600 0.16600 +1.71250 0.01250 0.01250 2.23300 0.16400 0.16400 +1.73750 0.01250 0.01250 2.13000 0.15900 0.15900 +1.76250 0.01250 0.01250 2.09100 0.15500 0.15500 +1.78750 0.01250 0.01250 1.96500 0.14900 0.14900 +1.81250 0.01250 0.01250 2.00500 0.14600 0.14600 +1.83750 0.01250 0.01250 1.26200 0.11800 0.11800 +1.86250 0.01250 0.01250 0.98700 0.10100 0.10100 +1.88750 0.01250 0.01250 0.57500 0.08100 0.08100 +1.91250 0.01250 0.01250 0.88800 0.09200 0.09200 +1.93750 0.01250 0.01250 0.72800 0.08600 0.08600 +1.96250 0.01250 0.01250 0.73600 0.08500 0.08500 +1.98750 0.01250 0.01250 0.64800 0.08100 0.08100 +2.02500 0.02500 0.02500 0.63200 0.05700 0.05700 +2.07500 0.02500 0.02500 0.54400 0.05000 0.05000 +2.12500 0.02500 0.02500 0.33700 0.03900 0.03900 +2.17500 0.02500 0.02500 0.31700 0.03800 0.03800 +2.22500 0.02500 0.02500 0.23600 0.03300 0.03300 +2.27500 0.02500 0.02500 0.20900 0.03100 0.03100 +2.32500 0.02500 0.02500 0.31700 0.03600 0.03600 +2.37500 0.02500 0.02500 0.28100 0.03300 0.03300 +2.42500 0.02500 0.02500 0.22300 0.03000 0.03000 +2.47500 0.02500 0.02500 0.28700 0.03200 0.03200 +2.52500 0.02500 0.02500 0.17300 0.02600 0.02600 +2.57500 0.02500 0.02500 0.09600 0.01900 0.01900 +2.62500 0.02500 0.02500 0.14700 0.02300 0.02300 +2.67500 0.02500 0.02500 0.09500 0.01800 0.01800 +2.72500 0.02500 0.02500 0.09700 0.01800 0.01800 +2.77500 0.02500 0.02500 0.08800 0.01700 0.01700 +2.82500 0.02500 0.02500 0.10100 0.01800 0.01800 +2.87500 0.02500 0.02500 0.07900 0.01500 0.01500 +2.92500 0.02500 0.02500 0.04400 0.01200 0.01200 +2.97500 0.02500 0.02500 0.06300 0.01400 0.01400 +3.02500 0.02500 0.02500 0.05800 0.01400 0.01400 +3.17500 0.02500 0.02500 0.03000 0.01000 0.01000 +3.25000 0.05000 0.05000 0.03300 0.00700 0.00700 +3.35000 0.05000 0.05000 0.01700 0.00500 0.00500 +3.45000 0.05000 0.05000 0.00800 0.00300 0.00300 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2018_I1679886.cc b/analyses/pluginBABAR/BABAR_2018_I1679886.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1679886.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2018_I1679886 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2018_I1679886); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + declare(UnstableParticles(), "UFS"); + _h_KK = bookHisto1D( 1, 1, 1); + + } + + void findDecayProducts(const Particle & mother, unsigned int & nstable, + unsigned int & nK0, unsigned int & nKp, + unsigned int & nKm, FourMomentum & ptot) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::KPLUS ) { + ++nKp; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::KMINUS ) { + ++nKm; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::K0S) { + ++nK0; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::PI0 || id == PID::PIPLUS || id == PID::PIMINUS) { + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p, nstable, nK0, nKp, nKm, ptot); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + // Loop over taus + for(const Particle& tau : apply(event, "UFS").particles(Cuts::abspid==PID::TAU)) { + unsigned int nstable(0),nK0(0),nKp(0),nKm(0); + FourMomentum p_tot(0,0,0,0); + findDecayProducts(tau, nstable, nK0, nKp, nKm, p_tot); + if (tau.pdgId() < 0) { + swap(nKp,nKm); + } + if(nstable!=3) continue; + if(nKm==1 && nK0==1 ) + _h_KK->fill(p_tot.mass(), event.weight()); + } + + + } + + + /// Normalise histograms etc., after the run + void finalize() { + normalize(_h_KK); + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _h_KK; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2018_I1679886); + + +} diff --git a/analyses/pluginBABAR/BABAR_2018_I1679886.info b/analyses/pluginBABAR/BABAR_2018_I1679886.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1679886.info @@ -0,0 +1,34 @@ +Name: BABAR_2018_I1679886 +Year: 2018 +Summary: Mass spectrum for $K^-K_S^0$ decays of the $\tau^-$ lepton +Experiment: BABAR +Collider: PEP-II +InspireID: 1679886 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D98 (2018) no.3, 032010 +RunInfo: e+ e- > tau+ tau-, or any process producing tau leptons +Description: + 'Mass spectra for $K^-K_S^0$ in tau decays + measured by BaBar. Useful for testing models of the hadronic current in $\tau$ decays.' +Keywords: [] +BibKey: BaBar:2018qry +BibTeX: '@article{BaBar:2018qry, + author = "Lees, J. P. and others", + title = "{Measurement of the spectral function for the $\tau^-\to + K^-K_S\nu_{\tau}$ decay}", + collaboration = "BaBar", + journal = "Phys. Rev.", + volume = "D98", + year = "2018", + number = "3", + pages = "032010", + doi = "10.1103/PhysRevD.98.032010", + eprint = "1806.10280", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BABAR-PUB-18/005, SLAC-PUB-17286, BABAR-PUB-18-005", + SLACcitation = "%%CITATION = ARXIV:1806.10280;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2018_I1679886.plot b/analyses/pluginBABAR/BABAR_2018_I1679886.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1679886.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BABAR_2018_I1679886/d01-x01-y01 +Title=$K^-K^0_S$ mass in $\tau^-\to K^-K^0_S\nu_\tau$ decays +XLabel=$m_{K^-K^0_S}$ [$\text{GeV}$] +YLabel=$1/\Gamma\text{d}\Gamma/\text{d}m_{K^-K^0_S}$ [ $\text{GeV}^{-1}$] +LogY=0 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2018_I1679886.yoda b/analyses/pluginBABAR/BABAR_2018_I1679886.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1679886.yoda @@ -0,0 +1,24 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2018_I1679886/d01-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2018_I1679886/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.00000 0.02000 0.02000 1.40000e-01 3.50000e-02 3.50000e-02 +1.04000 0.02000 0.02000 6.50000e-01 6.75000e-02 6.75000e-02 +1.08000 0.02000 0.02000 1.15000e+00 8.00000e-02 8.00000e-02 +1.12000 0.02000 0.02000 1.77000e+00 8.75000e-02 8.75000e-02 +1.16000 0.02000 0.02000 2.11000e+00 8.50000e-02 8.50000e-02 +1.20000 0.02000 0.02000 2.30750e+00 8.25000e-02 8.25000e-02 +1.24000 0.02000 0.02000 2.45500e+00 8.00000e-02 8.00000e-02 +1.28000 0.02000 0.02000 2.46000e+00 8.00000e-02 8.00000e-02 +1.32000 0.02000 0.02000 2.40750e+00 7.50000e-02 7.50000e-02 +1.36000 0.02000 0.02000 2.25500e+00 7.25000e-02 7.25000e-02 +1.40000 0.02000 0.02000 2.19500e+00 7.75000e-02 7.75000e-02 +1.44000 0.02000 0.02000 1.62750e+00 6.50000e-02 6.50000e-02 +1.48000 0.02000 0.02000 1.43250e+00 6.25000e-02 6.25000e-02 +1.52000 0.02000 0.02000 9.52500e-01 6.25000e-02 6.25000e-02 +1.60000 0.06000 0.06000 3.07500e-01 2.00000e-02 2.00000e-02 +1.72000 0.06000 0.06000 5.50000e-02 8.50000e-02 8.50000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBABAR/BABAR_2018_I1700745.cc b/analyses/pluginBABAR/BABAR_2018_I1700745.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1700745.cc @@ -0,0 +1,215 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BABAR_2018_I1700745 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BABAR_2018_I1700745); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _num5Pi = bookCounter("TMP/5Pi"); + _num2PiEta = bookCounter("TMP/2PiEta"); + _numOmegaPiPi = bookCounter("TMP/OmegaPiPi"); + _num4PiEta = bookCounter("TMP/4PiEta"); + _numOmegaPiEta = bookCounter("TMP/OmegaPiEta"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==5 && nCount[211]==1 && nCount[-211]==1 && nCount[111]==3) + _num5Pi->fill(event.weight()); + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find eta/omegas + if(p.pdgId()==221 || p.pdgId()==223 ) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta + if(p.pdgId()==221) { + // 2 pi eta + if(ncount==2) { + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _num2PiEta->fill(event.weight()); + } + // 4 pi eta + else if(ncount==4) { + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(abs(val.first)==111) { + if(val.second !=2) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _num4PiEta->fill(event.weight()); + } + // pi0 omega eta + foreach (const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=223) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=1) continue; + bool matched = true; + for(auto const & val : nResB) { + if(abs(val.first)==111) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _numOmegaPiEta->fill(event.weight()); + break; + } + } + } + else { + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==111) { + if(val.second !=2) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numOmegaPiPi->fill(event.weight()); + } + } + } + } + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<6;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _num5Pi->val(); + error = _num5Pi->err(); + } + else if(ix==2) { + sigma = _num2PiEta->val(); + error = _num2PiEta->err(); + } + else if(ix==3) { + sigma = _numOmegaPiPi->val(); + error = _numOmegaPiPi->err(); + } + else if(ix==4) { + sigma = _num4PiEta->val(); + error = _num4PiEta->err(); + } + else if(ix==5) { + sigma = _numOmegaPiEta->val(); + error = _numOmegaPiEta->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + //@} + + + /// @name Histograms + //@{ + CounterPtr _num5Pi,_num2PiEta,_numOmegaPiPi, + _num4PiEta,_numOmegaPiEta; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BABAR_2018_I1700745); + + +} diff --git a/analyses/pluginBABAR/BABAR_2018_I1700745.info b/analyses/pluginBABAR/BABAR_2018_I1700745.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1700745.info @@ -0,0 +1,34 @@ +Name: BABAR_2018_I1700745 +Year: 2018 +Summary: Cross section for $e^+e^-\to\pi^+\pi^-3\pi^0$ and $\pi^+\pi^-2\pi^0\eta$ between threshold and 4.35 GeV +Experiment: BABAR +Collider: PEP-II +InspireID: 1700745 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - arXiv:1810.11962 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^-3\pi^0$ and $\pi^+\pi^-2\pi^0\eta$ between threshold and 4.35 GeV. + The cross sections for the $\pi^+\pi^-\eta$, $\omega\pi^0\pi^0$ and $\omega\pi^0\eta$ resonant contributions are also measured' +Keywords: +BibKey: Lees:2018dnv +BibTeX: '@article{Lees:2018dnv, + author = "Lees, J. P.", + title = "{Study of the reactions + $e^+e^-\to\pi^+\pi^-\pi^0\pi^0\pi^0\gamma$ and + $\pi^+\pi^-\pi^0\pi^0\eta\gamma$ at center-of-mass + energies from threshold to 4.35 GeV using initial-state + radiation}", + collaboration = "BaBar", + year = "2018", + eprint = "1810.11962", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-17344", + SLACcitation = "%%CITATION = ARXIV:1810.11962;%%" +}' diff --git a/analyses/pluginBABAR/BABAR_2018_I1700745.plot b/analyses/pluginBABAR/BABAR_2018_I1700745.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1700745.plot @@ -0,0 +1,40 @@ +BEGIN PLOT /BABAR_2018_I1700745/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-3\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-3\pi^0)$/nb +LogY=0 +ConnectGaps=1 +LegendXPos=0.6 +END PLOT +BEGIN PLOT /BABAR_2018_I1700745/d02-x01-y01 +Title=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$/nb +LogY=0 +ConnectGaps=1 +LegendXPos=0.6 +END PLOT +BEGIN PLOT /BABAR_2018_I1700745/d03-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^0\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0\pi^0)$/nb +LogY=0 +ConnectGaps=1 +LegendXPos=0.6 +END PLOT +BEGIN PLOT /BABAR_2018_I1700745/d04-x01-y01 +Title=$\sigma(e^+e^-\to \eta\pi^+\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta\pi^+\pi^-2\pi^0)$/nb +LogY=0 +ConnectGaps=1 +LegendXPos=0.6 +END PLOT +BEGIN PLOT /BABAR_2018_I1700745/d05-x01-y01 +Title=$\sigma(e^+e^-\to \eta\omega\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta\omega\pi^0)$/nb +LogY=0 +ConnectGaps=1 +LegendXPos=0.6 +END PLOT diff --git a/analyses/pluginBABAR/BABAR_2018_I1700745.yoda b/analyses/pluginBABAR/BABAR_2018_I1700745.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBABAR/BABAR_2018_I1700745.yoda @@ -0,0 +1,322 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2018_I1700745/d01-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2018_I1700745/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.12500 0.00000 0.00000 0.00000e+00 2.00000e-02 2.00000e-02 +1.17500 0.00000 0.00000 0.00000e+00 3.00000e-02 3.00000e-02 +1.22500 0.00000 0.00000 -3.00000e-02 5.00000e-02 5.00000e-02 +1.27500 0.00000 0.00000 2.10000e-01 1.20000e-01 1.20000e-01 +1.32500 0.00000 0.00000 5.10000e-01 1.20000e-01 1.20000e-01 +1.37500 0.00000 0.00000 1.17000e+00 2.00000e-01 2.00000e-01 +1.42500 0.00000 0.00000 1.68000e+00 1.50000e-01 1.50000e-01 +1.47500 0.00000 0.00000 2.10000e+00 2.60000e-01 2.60000e-01 +1.52500 0.00000 0.00000 1.92000e+00 2.80000e-01 2.80000e-01 +1.57500 0.00000 0.00000 2.49000e+00 2.70000e-01 2.70000e-01 +1.62500 0.00000 0.00000 2.36000e+00 2.70000e-01 2.70000e-01 +1.67500 0.00000 0.00000 2.81000e+00 2.00000e-01 2.00000e-01 +1.72500 0.00000 0.00000 2.20000e+00 2.50000e-01 2.50000e-01 +1.77500 0.00000 0.00000 2.20000e+00 2.30000e-01 2.30000e-01 +1.82500 0.00000 0.00000 2.03000e+00 1.70000e-01 1.70000e-01 +1.87500 0.00000 0.00000 1.65000e+00 1.50000e-01 1.50000e-01 +1.92500 0.00000 0.00000 1.23000e+00 1.50000e-01 1.50000e-01 +1.97500 0.00000 0.00000 1.46000e+00 1.90000e-01 1.90000e-01 +2.02500 0.00000 0.00000 1.41000e+00 1.40000e-01 1.40000e-01 +2.07500 0.00000 0.00000 1.42000e+00 1.40000e-01 1.40000e-01 +2.12500 0.00000 0.00000 1.30000e+00 1.20000e-01 1.20000e-01 +2.17500 0.00000 0.00000 1.12000e+00 1.30000e-01 1.30000e-01 +2.22500 0.00000 0.00000 1.16000e+00 1.30000e-01 1.30000e-01 +2.27500 0.00000 0.00000 1.03000e+00 1.20000e-01 1.20000e-01 +2.32500 0.00000 0.00000 8.20000e-01 1.10000e-01 1.10000e-01 +2.37500 0.00000 0.00000 6.80000e-01 1.00000e-01 1.00000e-01 +2.42500 0.00000 0.00000 9.20000e-01 1.00000e-01 1.00000e-01 +2.47500 0.00000 0.00000 6.10000e-01 9.00000e-02 9.00000e-02 +2.52500 0.00000 0.00000 4.50000e-01 8.00000e-02 8.00000e-02 +2.57500 0.00000 0.00000 7.10000e-01 1.00000e-01 1.00000e-01 +2.62500 0.00000 0.00000 4.50000e-01 8.00000e-02 8.00000e-02 +2.67500 0.00000 0.00000 5.60000e-01 9.00000e-02 9.00000e-02 +2.72500 0.00000 0.00000 2.20000e-01 8.00000e-02 8.00000e-02 +2.77500 0.00000 0.00000 4.00000e-01 8.00000e-02 8.00000e-02 +2.82500 0.00000 0.00000 2.90000e-01 8.00000e-02 8.00000e-02 +2.87500 0.00000 0.00000 6.20000e-01 8.00000e-02 8.00000e-02 +2.92500 0.00000 0.00000 5.50000e-01 8.00000e-02 8.00000e-02 +2.97500 0.00000 0.00000 6.00000e-01 9.00000e-02 9.00000e-02 +3.02500 0.00000 0.00000 8.50000e-01 1.00000e-01 1.00000e-01 +3.07500 0.00000 0.00000 4.36000e+00 1.30000e-01 1.30000e-01 +3.12500 0.00000 0.00000 2.66000e+00 1.10000e-01 1.10000e-01 +3.17500 0.00000 0.00000 6.00000e-01 6.00000e-02 6.00000e-02 +3.22500 0.00000 0.00000 3.30000e-01 5.00000e-02 5.00000e-02 +3.27500 0.00000 0.00000 3.10000e-01 5.00000e-02 5.00000e-02 +3.32500 0.00000 0.00000 2.00000e-01 5.00000e-02 5.00000e-02 +3.37500 0.00000 0.00000 3.50000e-01 5.00000e-02 5.00000e-02 +3.42500 0.00000 0.00000 2.20000e-01 5.00000e-02 5.00000e-02 +3.47500 0.00000 0.00000 1.90000e-01 5.00000e-02 5.00000e-02 +3.52500 0.00000 0.00000 2.60000e-01 5.00000e-02 5.00000e-02 +3.57500 0.00000 0.00000 1.20000e-01 5.00000e-02 5.00000e-02 +3.62500 0.00000 0.00000 3.80000e-01 5.00000e-02 5.00000e-02 +3.67500 0.00000 0.00000 4.10000e-01 6.00000e-02 6.00000e-02 +3.72500 0.00000 0.00000 2.90000e-01 5.00000e-02 5.00000e-02 +3.77500 0.00000 0.00000 1.50000e-01 4.00000e-02 4.00000e-02 +3.82500 0.00000 0.00000 2.00000e-01 4.00000e-02 4.00000e-02 +3.87500 0.00000 0.00000 1.80000e-01 4.00000e-02 4.00000e-02 +3.92500 0.00000 0.00000 1.40000e-01 4.00000e-02 4.00000e-02 +3.97500 0.00000 0.00000 2.20000e-01 4.00000e-02 4.00000e-02 +4.02500 0.00000 0.00000 1.40000e-01 4.00000e-02 4.00000e-02 +4.07500 0.00000 0.00000 1.40000e-01 3.00000e-02 3.00000e-02 +4.12500 0.00000 0.00000 4.00000e-02 3.00000e-02 3.00000e-02 +4.17500 0.00000 0.00000 8.00000e-02 3.00000e-02 3.00000e-02 +4.22500 0.00000 0.00000 9.00000e-02 3.00000e-02 3.00000e-02 +4.27500 0.00000 0.00000 1.20000e-01 3.00000e-02 3.00000e-02 +4.32500 0.00000 0.00000 9.00000e-02 3.00000e-02 3.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2018_I1700745/d02-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2018_I1700745/d02-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.07500 0.00000 0.00000 6.00000e-02 3.00000e-02 3.00000e-02 +1.12500 0.00000 0.00000 2.90000e-01 2.30000e-01 2.30000e-01 +1.17500 0.00000 0.00000 0.00000e+00 1.20000e-01 1.20000e-01 +1.22500 0.00000 0.00000 2.30000e-01 2.50000e-01 2.50000e-01 +1.27500 0.00000 0.00000 5.70000e-01 2.70000e-01 2.70000e-01 +1.32500 0.00000 0.00000 1.15000e+00 3.40000e-01 3.40000e-01 +1.37500 0.00000 0.00000 1.83000e+00 3.60000e-01 3.60000e-01 +1.42500 0.00000 0.00000 2.74000e+00 4.00000e-01 4.00000e-01 +1.47500 0.00000 0.00000 3.74000e+00 4.30000e-01 4.30000e-01 +1.52500 0.00000 0.00000 4.14000e+00 4.40000e-01 4.40000e-01 +1.57500 0.00000 0.00000 3.48000e+00 4.00000e-01 4.00000e-01 +1.62500 0.00000 0.00000 2.67000e+00 3.60000e-01 3.60000e-01 +1.67500 0.00000 0.00000 2.52000e+00 3.20000e-01 3.20000e-01 +1.72500 0.00000 0.00000 2.20000e+00 3.00000e-01 3.00000e-01 +1.77500 0.00000 0.00000 2.38000e+00 2.90000e-01 2.90000e-01 +1.82500 0.00000 0.00000 1.39000e+00 2.30000e-01 2.30000e-01 +1.87500 0.00000 0.00000 1.16000e+00 2.10000e-01 2.10000e-01 +1.92500 0.00000 0.00000 1.00000e+00 1.90000e-01 1.90000e-01 +1.97500 0.00000 0.00000 6.50000e-01 1.60000e-01 1.60000e-01 +2.02500 0.00000 0.00000 7.80000e-01 1.60000e-01 1.60000e-01 +2.07500 0.00000 0.00000 5.10000e-01 1.30000e-01 1.30000e-01 +2.12500 0.00000 0.00000 5.00000e-01 1.30000e-01 1.30000e-01 +2.17500 0.00000 0.00000 7.50000e-01 1.30000e-01 1.30000e-01 +2.22500 0.00000 0.00000 2.30000e-01 1.10000e-01 1.10000e-01 +2.27500 0.00000 0.00000 3.50000e-01 1.00000e-01 1.00000e-01 +2.32500 0.00000 0.00000 2.20000e-01 9.00000e-02 9.00000e-02 +2.37500 0.00000 0.00000 3.30000e-01 9.00000e-02 9.00000e-02 +2.42500 0.00000 0.00000 2.20000e-01 7.00000e-02 7.00000e-02 +2.47500 0.00000 0.00000 5.10000e-01 1.00000e-01 1.00000e-01 +2.52500 0.00000 0.00000 2.70000e-01 9.00000e-02 9.00000e-02 +2.57500 0.00000 0.00000 8.00000e-02 5.00000e-02 5.00000e-02 +2.62500 0.00000 0.00000 1.20000e-01 6.00000e-02 6.00000e-02 +2.67500 0.00000 0.00000 2.70000e-01 7.00000e-02 7.00000e-02 +2.72500 0.00000 0.00000 1.10000e-01 5.00000e-02 5.00000e-02 +2.77500 0.00000 0.00000 9.00000e-02 5.00000e-02 5.00000e-02 +2.82500 0.00000 0.00000 3.00000e-02 4.00000e-02 4.00000e-02 +2.87500 0.00000 0.00000 5.00000e-02 4.00000e-02 4.00000e-02 +2.92500 0.00000 0.00000 2.00000e-02 4.00000e-02 4.00000e-02 +2.97500 0.00000 0.00000 9.00000e-02 5.00000e-02 5.00000e-02 +3.02500 0.00000 0.00000 5.00000e-02 5.00000e-02 5.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2018_I1700745/d03-x01-y01 +IsRef: 1 +Path: /REF/BABAR_2018_I1700745/d03-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.12500 0.00000 0.00000 4.00000e-02 8.00000e-02 8.00000e-02 +1.17500 0.00000 0.00000 3.00000e-02 1.00000e-01 1.00000e-01 +1.22500 0.00000 0.00000 -2.00000e-02 1.00000e-01 1.00000e-01 +1.27500 0.00000 0.00000 1.30000e-01 1.10000e-01 1.10000e-01 +1.32500 0.00000 0.00000 4.10000e-01 1.30000e-01 1.30000e-01 +1.37500 0.00000 0.00000 6.90000e-01 1.80000e-01 1.80000e-01 +1.42500 0.00000 0.00000 2.90000e-01 1.80000e-01 1.80000e-01 +1.47500 0.00000 0.00000 6.80000e-01 1.90000e-01 1.90000e-01 +1.52500 0.00000 0.00000 1.05000e+00 2.10000e-01 2.10000e-01 +1.57500 0.00000 0.00000 1.44000e+00 2.20000e-01 2.20000e-01 +1.62500 0.00000 0.00000 1.40000e+00 2.10000e-01 2.10000e-01 +1.67500 0.00000 0.00000 1.55000e+00 2.00000e-01 2.00000e-01 +1.72500 0.00000 0.00000 9.60000e-01 1.80000e-01 1.80000e-01 +1.77500 0.00000 0.00000 8.80000e-01 1.60000e-01 1.60000e-01 +1.82500 0.00000 0.00000 6.20000e-01 1.40000e-01 1.40000e-01 +1.87500 0.00000 0.00000 9.60000e-01 1.40000e-01 1.40000e-01 +1.92500 0.00000 0.00000 6.10000e-01 1.30000e-01 1.30000e-01 +1.97500 0.00000 0.00000 4.50000e-01 1.10000e-01 1.10000e-01 +2.02500 0.00000 0.00000 4.70000e-01 1.00000e-01 1.00000e-01 +2.07500 0.00000 0.00000 3.30000e-01 9.00000e-02 9.00000e-02 +2.12500 0.00000 0.00000 2.90000e-01 9.00000e-02 9.00000e-02 +2.17500 0.00000 0.00000 2.60000e-01 8.00000e-02 8.00000e-02 +2.22500 0.00000 0.00000 4.00000e-01 8.00000e-02 8.00000e-02 +2.27500 0.00000 0.00000 3.10000e-01 7.00000e-02 7.00000e-02 +2.32500 0.00000 0.00000 2.10000e-01 6.00000e-02 6.00000e-02 +2.37500 0.00000 0.00000 2.30000e-01 6.00000e-02 6.00000e-02 +2.42500 0.00000 0.00000 7.00000e-02 5.00000e-02 5.00000e-02 +2.47500 0.00000 0.00000 1.20000e-01 5.00000e-02 5.00000e-02 +2.52500 0.00000 0.00000 2.10000e-01 5.00000e-02 5.00000e-02 +2.57500 0.00000 0.00000 1.50000e-01 4.00000e-02 4.00000e-02 +2.62500 0.00000 0.00000 1.30000e-01 4.00000e-02 4.00000e-02 +2.67500 0.00000 0.00000 1.20000e-01 4.00000e-02 4.00000e-02 +2.72500 0.00000 0.00000 1.70000e-01 4.00000e-02 4.00000e-02 +2.77500 0.00000 0.00000 1.00000e-01 4.00000e-02 4.00000e-02 +2.82500 0.00000 0.00000 1.10000e-01 4.00000e-02 4.00000e-02 +2.87500 0.00000 0.00000 1.80000e-01 4.00000e-02 4.00000e-02 +2.92500 0.00000 0.00000 1.00000e-01 3.00000e-02 3.00000e-02 +2.97500 0.00000 0.00000 1.40000e-01 6.00000e-02 6.00000e-02 +3.02500 0.00000 0.00000 2.50000e-01 4.00000e-02 4.00000e-02 +3.07500 0.00000 0.00000 8.30000e-01 7.00000e-02 7.00000e-02 +3.12500 0.00000 0.00000 5.20000e-01 5.00000e-02 5.00000e-02 +3.17500 0.00000 0.00000 1.10000e-01 3.00000e-02 3.00000e-02 +3.22500 0.00000 0.00000 8.00000e-02 2.00000e-02 2.00000e-02 +3.27500 0.00000 0.00000 8.00000e-02 2.00000e-02 2.00000e-02 +3.32500 0.00000 0.00000 7.00000e-02 2.00000e-02 2.00000e-02 +3.37500 0.00000 0.00000 6.00000e-02 2.00000e-02 2.00000e-02 +3.42500 0.00000 0.00000 7.00000e-02 2.00000e-02 2.00000e-02 +3.47500 0.00000 0.00000 3.00000e-02 2.00000e-02 2.00000e-02 +3.52500 0.00000 0.00000 7.00000e-02 2.00000e-02 2.00000e-02 +3.57500 0.00000 0.00000 4.00000e-02 2.00000e-02 2.00000e-02 +3.62500 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+Path: /REF/BABAR_2018_I1700745/d04-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.62500 0.00000 0.00000 1.00000e-02 1.00000e-01 1.00000e-01 +1.67500 0.00000 0.00000 -5.00000e-02 8.00000e-02 8.00000e-02 +1.72500 0.00000 0.00000 2.00000e-01 1.00000e-01 1.00000e-01 +1.77500 0.00000 0.00000 5.10000e-01 1.20000e-01 1.20000e-01 +1.82500 0.00000 0.00000 7.10000e-01 1.40000e-01 1.40000e-01 +1.87500 0.00000 0.00000 7.30000e-01 1.40000e-01 1.40000e-01 +1.92500 0.00000 0.00000 1.22000e+00 1.60000e-01 1.60000e-01 +1.97500 0.00000 0.00000 2.22000e+00 2.00000e-01 2.00000e-01 +2.02500 0.00000 0.00000 2.01000e+00 1.90000e-01 1.90000e-01 +2.07500 0.00000 0.00000 1.61000e+00 1.80000e-01 1.80000e-01 +2.12500 0.00000 0.00000 1.90000e+00 1.80000e-01 1.80000e-01 +2.17500 0.00000 0.00000 1.59000e+00 1.60000e-01 1.60000e-01 +2.22500 0.00000 0.00000 1.66000e+00 1.80000e-01 1.80000e-01 +2.27500 0.00000 0.00000 1.29000e+00 1.60000e-01 1.60000e-01 +2.32500 0.00000 0.00000 1.27000e+00 1.50000e-01 1.50000e-01 +2.37500 0.00000 0.00000 1.70000e+00 1.80000e-01 1.80000e-01 +2.42500 0.00000 0.00000 1.30000e+00 1.50000e-01 1.50000e-01 +2.47500 0.00000 0.00000 1.27000e+00 1.60000e-01 1.60000e-01 +2.52500 0.00000 0.00000 1.00000e+00 1.30000e-01 1.30000e-01 +2.57500 0.00000 0.00000 9.50000e-01 1.50000e-01 1.50000e-01 +2.62500 0.00000 0.00000 1.11000e+00 1.60000e-01 1.60000e-01 +2.67500 0.00000 0.00000 6.70000e-01 1.40000e-01 1.40000e-01 +2.72500 0.00000 0.00000 1.07000e+00 1.30000e-01 1.30000e-01 +2.77500 0.00000 0.00000 9.70000e-01 1.40000e-01 1.40000e-01 +2.82500 0.00000 0.00000 6.80000e-01 1.40000e-01 1.40000e-01 +2.87500 0.00000 0.00000 1.00000e+00 1.30000e-01 1.30000e-01 +2.92500 0.00000 0.00000 8.10000e-01 1.30000e-01 1.30000e-01 +2.97500 0.00000 0.00000 9.60000e-01 1.30000e-01 1.30000e-01 +3.02500 0.00000 0.00000 6.10000e-01 1.40000e-01 1.40000e-01 +3.07500 0.00000 0.00000 1.21000e+00 1.60000e-01 1.60000e-01 +3.12500 0.00000 0.00000 1.06000e+00 1.50000e-01 1.50000e-01 +3.17500 0.00000 0.00000 5.00000e-01 1.20000e-01 1.20000e-01 +3.22500 0.00000 0.00000 5.20000e-01 1.10000e-01 1.10000e-01 +3.27500 0.00000 0.00000 2.60000e-01 9.00000e-02 9.00000e-02 +3.32500 0.00000 0.00000 1.50000e-01 1.10000e-01 1.10000e-01 +3.37500 0.00000 0.00000 5.00000e-01 1.00000e-01 1.00000e-01 +3.42500 0.00000 0.00000 1.50000e-01 1.10000e-01 1.10000e-01 +3.47500 0.00000 0.00000 3.40000e-01 1.00000e-01 1.00000e-01 +3.52500 0.00000 0.00000 3.00000e-01 8.00000e-02 8.00000e-02 +3.57500 0.00000 0.00000 1.80000e-01 9.00000e-02 9.00000e-02 +3.62500 0.00000 0.00000 2.00000e-01 1.10000e-01 1.10000e-01 +3.67500 0.00000 0.00000 1.80000e-01 9.00000e-02 9.00000e-02 +3.72500 0.00000 0.00000 2.80000e-01 9.00000e-02 9.00000e-02 +3.77500 0.00000 0.00000 6.00000e-02 9.00000e-02 9.00000e-02 +3.82500 0.00000 0.00000 2.00000e-02 7.00000e-02 7.00000e-02 +3.87500 0.00000 0.00000 8.00000e-02 8.00000e-02 8.00000e-02 +3.92500 0.00000 0.00000 1.20000e-01 7.00000e-02 7.00000e-02 +3.97500 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3.00000e-02 +3.42500 0.00000 0.00000 1.30000e-01 4.00000e-02 4.00000e-02 +3.47500 0.00000 0.00000 9.00000e-02 3.00000e-02 3.00000e-02 +3.52500 0.00000 0.00000 6.00000e-02 3.00000e-02 3.00000e-02 +3.57500 0.00000 0.00000 1.00000e-01 3.00000e-02 3.00000e-02 +3.62500 0.00000 0.00000 2.00000e-02 2.00000e-02 2.00000e-02 +3.67500 0.00000 0.00000 6.00000e-02 3.00000e-02 3.00000e-02 +3.72500 0.00000 0.00000 5.00000e-02 3.00000e-02 3.00000e-02 +3.77500 0.00000 0.00000 8.00000e-02 2.00000e-02 2.00000e-02 +3.82500 0.00000 0.00000 4.00000e-02 3.00000e-02 3.00000e-02 +3.87500 0.00000 0.00000 7.00000e-02 2.00000e-02 2.00000e-02 +3.92500 0.00000 0.00000 8.00000e-02 3.00000e-02 3.00000e-02 +3.97500 0.00000 0.00000 0.00000e+00 3.00000e-02 3.00000e-02 +4.02500 0.00000 0.00000 5.00000e-02 2.00000e-02 2.00000e-02 +4.07500 0.00000 0.00000 0.00000e+00 3.00000e-02 3.00000e-02 +4.12500 0.00000 0.00000 4.00000e-02 2.00000e-02 2.00000e-02 +4.17500 0.00000 0.00000 3.00000e-02 2.00000e-02 2.00000e-02 +4.22500 0.00000 0.00000 3.00000e-02 2.00000e-02 2.00000e-02 +4.27500 0.00000 0.00000 0.00000e+00 3.00000e-02 3.00000e-02 +4.32500 0.00000 0.00000 2.00000e-02 1.00000e-02 1.00000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2001_S4598261.cc b/analyses/pluginBELLE/BELLE_2001_S4598261.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2001_S4598261.cc @@ -0,0 +1,104 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/Beam.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief BELLE pi0 spectrum at Upsilon(4S) + /// @author Peter Richardson + class BELLE_2001_S4598261 : public Analysis { + public: + + BELLE_2001_S4598261() + : Analysis("BELLE_2001_S4598261"), _weightSum(0.) + { } + + + void init() { + declare(UnstableParticles(), "UFS"); + _histdSigDp = bookHisto1D(1, 1, 1); // spectrum + _histMult = bookHisto1D(2, 1, 1); // multiplicity + } + + + void analyze(const Event& e) { + const double weight = e.weight(); + + // Find the upsilons + Particles upsilons; + // First in unstable final state + const UnstableParticles& ufs = apply(e, "UFS"); + foreach (const Particle& p, ufs.particles()) + if (p.pid()==300553) upsilons.push_back(p); + // Then in whole event if fails + if (upsilons.empty()) { + for(ConstGenParticlePtr p: HepMCUtils::particles(e.genEvent())) { + if (p->pdg_id() != 300553) continue; + ConstGenVertexPtr pv = p->production_vertex(); + bool passed = true; + if (pv) { + for (ConstGenParticlePtr pp: HepMCUtils::particles(pv, Relatives::PARENTS)){ + if ( p->pdg_id() == pp->pdg_id() ) { + passed = false; + break; + } + } + } + if (passed) upsilons.push_back(Particle(p)); + } + } + + // Find upsilons + foreach (const Particle& p, upsilons) { + _weightSum += weight; + // Find the neutral pions from the decay + vector pions; + findDecayProducts(p.genParticle(), pions); + const LorentzTransform cms_boost = LorentzTransform::mkFrameTransformFromBeta(p.momentum().betaVec()); + for (size_t ix=0; ixmomentum())).p(); + _histdSigDp->fill(pcm,weight); + } + _histMult->fill(0., pions.size()*weight); + } + } + + + void finalize() { + scale(_histdSigDp, 1./_weightSum); + scale(_histMult , 1./_weightSum); + } + + + private: + + //@{ + // count of weights + double _weightSum; + /// Histograms + Histo1DPtr _histdSigDp; + Histo1DPtr _histMult; + //@} + + + void findDecayProducts(ConstGenParticlePtr p, vector& pions) { + ConstGenVertexPtr dv = p->end_vertex(); + for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ + const int id = pp->pdg_id(); + if (id == 111) { + pions.push_back(pp); + } else if (pp->end_vertex()) + findDecayProducts(pp, pions); + } + } + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2001_S4598261); + +} diff --git a/analyses/pluginMisc/BELLE_2001_S4598261.info b/analyses/pluginBELLE/BELLE_2001_S4598261.info rename from analyses/pluginMisc/BELLE_2001_S4598261.info rename to analyses/pluginBELLE/BELLE_2001_S4598261.info diff --git a/analyses/pluginMisc/BELLE_2001_S4598261.plot b/analyses/pluginBELLE/BELLE_2001_S4598261.plot rename from analyses/pluginMisc/BELLE_2001_S4598261.plot rename to analyses/pluginBELLE/BELLE_2001_S4598261.plot diff --git a/analyses/pluginMisc/BELLE_2001_S4598261.yoda b/analyses/pluginBELLE/BELLE_2001_S4598261.yoda rename from analyses/pluginMisc/BELLE_2001_S4598261.yoda rename to analyses/pluginBELLE/BELLE_2001_S4598261.yoda diff --git a/analyses/pluginBELLE/BELLE_2007_I723333.cc b/analyses/pluginBELLE/BELLE_2007_I723333.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I723333.cc @@ -0,0 +1,141 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2007_I723333 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2007_I723333); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nDSS = bookCounter("/TMP/nDSS"); + _nDS = bookCounter("/TMP/nDS"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + bool matched=false; + int sign = -p1.pdgId()/abs(p1.pdgId()); + for(unsigned int iy=0;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + sign = abs(p2.pdgId()); + break; + } + } + if(matched) { + if(sign==411) + _nDS->fill(event.weight()); + else if(sign==413) + _nDSS->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma,error; + if(ix==1) { + sigma = _nDSS->val(); + error = _nDSS->err(); + } + else { + sigma = _nDS->val(); + error = _nDS->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nDSS,_nDS; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2007_I723333); + + +} diff --git a/analyses/pluginBELLE/BELLE_2007_I723333.info b/analyses/pluginBELLE/BELLE_2007_I723333.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I723333.info @@ -0,0 +1,33 @@ +Name: BELLE_2007_I723333 +Year: 2007 +Summary: Cross section for $e^+e^-\to D^{*+}D^{*-}$ and $D^\pm D^{*\mp}$ below 5 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 723333 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 98 (2007) 092001 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to D^{*+}D^{*-}$ and $D^\pm D^{*\mp}$ below 5 GeV' +Keywords: [] +BibKey: Abe:2006fj +BibTeX: '@article{Abe:2006fj, + author = "Abe, Kazuo and others", + title = "{Measurement of the near-threshold e+ e- ---> D(*)+- + D(*)-+ cross section using initial-state radiation}", + collaboration = "Belle", + journal = "Phys. Rev. Lett.", + volume = "98", + year = "2007", + pages = "092001", + doi = "10.1103/PhysRevLett.98.092001", + eprint = "hep-ex/0608018", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0608018;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2007_I723333.plot b/analyses/pluginBELLE/BELLE_2007_I723333.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I723333.plot @@ -0,0 +1,13 @@ +BEGIN PLOT /BELLE_2007_I723333/d01-x01-y01 +Title=$\sigma(e^+e^-\to D^{*+}D^{*-})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^{*+}D^{*-})$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2007_I723333/d02-x01-y01 +Title=$\sigma(e^+e^-\to D^\pm D^{*\mp})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^\pm D^{*\mp})$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2007_I723333.yoda b/analyses/pluginBELLE/BELLE_2007_I723333.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I723333.yoda @@ -0,0 +1,128 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2007_I723333/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.302, up: 0.302}, sys: {dn: -0.2, up: 0.2}}, 1: {stat: {dn: -0.36, up: 0.36}, sys: {dn: -0.335, up: 0.335}}, 2: {stat: {dn: -0.377, up: 0.377}, sys: {dn: -0.359, up: 0.359}}, 3: {stat: {dn: -0.359, up: 0.359}, sys: {dn: -0.309, up: 0.309}}, 4: {stat: {dn: -0.341, up: 0.341}, sys: {dn: -0.271, up: 0.271}}, 5: {stat: {dn: -0.352, up: 0.352}, sys: {dn: -0.326, up: 0.326}}, 6: {stat: {dn: -0.373, up: 0.373}, sys: {dn: -0.364, up: 0.364}}, 7: {stat: {dn: -0.348, up: 0.348}, sys: {dn: -0.342, up: 0.342}}, 8: {stat: {dn: -0.353, up: 0.353}, sys: {dn: -0.331, up: 0.331}}, 9: {stat: {dn: -0.274, up: 0.274}, sys: {dn: -0.186, up: 0.186}}, 10: {stat: {dn: -0.158, up: 0.158}, sys: {dn: -0.072, up: 0.072}}, 11: {stat: {dn: -0.144, up: 0.144}, sys: {dn: -0.059, up: 0.059}}, 12: {stat: {dn: -0.151, up: 0.151}, sys: {dn: -0.068, up: 0.068}}, 13: {stat: {dn: -0.181, up: 0.181}, sys: {dn: -0.08, up: 0.08}}, 14: {stat: {dn: -0.198, up: 0.198}, sys: {dn: -0.112, up: 0.112}}, 15: {stat: {dn: -0.2, up: 0.2}, sys: {dn: -0.112, up: 0.112}}, 16: {stat: {dn: -0.209, up: 0.209}, sys: {dn: -0.127, up: 0.127}}, 17: {stat: {dn: -0.199, up: 0.199}, sys: {dn: -0.115, up: 0.115}}, 18: {stat: {dn: -0.202, up: 0.202}, sys: {dn: -0.12, up: 0.12}}, 19: {stat: {dn: -0.197, up: 0.197}, sys: {dn: -0.111, up: 0.111}}, 20: {stat: {dn: -0.165, up: 0.165}, sys: {dn: -0.085, up: 0.085}}, 21: {stat: {dn: -0.156, up: 0.156}, sys: {dn: -0.071, up: 0.071}}, 22: {stat: {dn: -0.142, up: 0.142}, sys: {dn: -0.043, up: 0.043}}, 23: {stat: {dn: -0.155, up: 0.155}, sys: {dn: -0.064, up: 0.064}}, 24: {stat: {dn: -0.15, up: 0.15}, sys: {dn: -0.077, up: 0.077}}, 25: {stat: {dn: -0.146, up: 0.146}, sys: {dn: -0.073, up: 0.073}}, 26: {stat: {dn: -0.163, up: 0.163}, sys: {dn: -0.09, up: 0.09}}, 27: {stat: {dn: -0.136, up: 0.136}, sys: {dn: -0.062, up: 0.062}}, 28: {stat: {dn: -0.139, up: 0.139}, sys: {dn: -0.063, up: 0.063}}, 29: {stat: {dn: -0.133, up: 0.133}, sys: {dn: -0.052, up: 0.052}}, 30: {stat: {dn: -0.123, up: 0.123}, sys: {dn: -0.049, up: 0.049}}, 31: {stat: {dn: -0.138, up: 0.138}, sys: {dn: -0.057, up: 0.057}}, 32: {stat: {dn: -0.127, up: 0.127}, sys: {dn: -0.057, up: 0.057}}, 33: {stat: {dn: -0.144, up: 0.144}, sys: {dn: -0.068, up: 0.068}}, 34: {stat: {dn: -0.136, up: 0.136}, sys: {dn: -0.064, up: 0.064}}, 35: {stat: {dn: -0.131, up: 0.131}, sys: {dn: -0.062, up: 0.062}}, 36: {stat: {dn: -0.114, up: 0.114}, sys: {dn: -0.044, up: 0.044}}, 37: {stat: {dn: -0.101, up: 0.101}, sys: {dn: -0.036, up: 0.036}}, 38: {stat: {dn: -0.121, up: 0.121}, sys: {dn: -0.056, up: 0.056}}, 39: {stat: {dn: -0.129, up: 0.129}, sys: {dn: -0.053, up: 0.053}}, 40: {stat: {dn: -0.061, up: 0.061}, sys: {dn: -0.007, up: 0.007}}, 41: {stat: {dn: -0.077, up: 0.077}, sys: {dn: -0.018, up: 0.018}}, 42: {stat: {dn: -0.084, up: 0.084}, sys: {dn: -0.026, up: 0.026}}, 43: {stat: {dn: -0.094, up: 0.094}, sys: {dn: -0.028, up: 0.028}}, 44: {stat: {dn: -0.083, up: 0.083}, sys: {dn: -0.025, up: 0.025}}, 45: {stat: {dn: -0.086, up: 0.086}, sys: {dn: -0.027, up: 0.027}}, 46: {stat: {dn: -0.104, up: 0.104}, sys: {dn: -0.042, up: 0.042}}, 47: {stat: {dn: -0.103, up: 0.103}, sys: {dn: -0.04, up: 0.04}}, 48: {stat: {dn: -0.096, up: 0.096}, sys: {dn: -0.033, up: 0.033}}} + +IsRef: 1 +Path: /REF/BELLE_2007_I723333/d01-x01-y01 +Title: doi:10.17182/hepdata.19336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.030000e+00 1.000000e-02 1.000000e-02 1.823000e+00 3.622209e-01 3.622209e-01 +4.050000e+00 1.000000e-02 1.000000e-02 3.046000e+00 4.917571e-01 4.917571e-01 +4.070000e+00 1.000000e-02 1.000000e-02 3.267000e+00 5.205862e-01 5.205862e-01 +4.090000e+00 1.000000e-02 1.000000e-02 2.810000e+00 4.736687e-01 4.736687e-01 +4.110000e+00 1.000000e-02 1.000000e-02 2.471000e+00 4.355709e-01 4.355709e-01 +4.130000e+00 1.000000e-02 1.000000e-02 2.968000e+00 4.797708e-01 4.797708e-01 +4.150000e+00 1.000000e-02 1.000000e-02 3.309000e+00 5.211766e-01 5.211766e-01 +4.170000e+00 1.000000e-02 1.000000e-02 3.110000e+00 4.879221e-01 4.879221e-01 +4.190000e+00 1.000000e-02 1.000000e-02 3.013000e+00 4.839111e-01 4.839111e-01 +4.210000e+00 1.000000e-02 1.000000e-02 1.695000e+00 3.311676e-01 3.311676e-01 +4.230000e+00 1.000000e-02 1.000000e-02 6.550000e-01 1.736318e-01 1.736318e-01 +4.250000e+00 1.000000e-02 1.000000e-02 5.440000e-01 1.556181e-01 1.556181e-01 +4.270000e+00 1.000000e-02 1.000000e-02 6.180000e-01 1.656050e-01 1.656050e-01 +4.290000e+00 1.000000e-02 1.000000e-02 7.340000e-01 1.978914e-01 1.978914e-01 +4.310000e+00 1.000000e-02 1.000000e-02 1.019000e+00 2.274819e-01 2.274819e-01 +4.330000e+00 1.000000e-02 1.000000e-02 1.020000e+00 2.292248e-01 2.292248e-01 +4.350000e+00 1.000000e-02 1.000000e-02 1.155000e+00 2.445608e-01 2.445608e-01 +4.370000e+00 1.000000e-02 1.000000e-02 1.054000e+00 2.298391e-01 2.298391e-01 +4.390000e+00 1.000000e-02 1.000000e-02 1.095000e+00 2.349553e-01 2.349553e-01 +4.410000e+00 1.000000e-02 1.000000e-02 1.012000e+00 2.261194e-01 2.261194e-01 +4.430000e+00 1.000000e-02 1.000000e-02 7.750000e-01 1.856071e-01 1.856071e-01 +4.450000e+00 1.000000e-02 1.000000e-02 6.470000e-01 1.713972e-01 1.713972e-01 +4.470000e+00 1.000000e-02 1.000000e-02 3.930000e-01 1.483678e-01 1.483678e-01 +4.490000e+00 1.000000e-02 1.000000e-02 5.890000e-01 1.676932e-01 1.676932e-01 +4.510000e+00 1.000000e-02 1.000000e-02 7.030000e-01 1.686090e-01 1.686090e-01 +4.530000e+00 1.000000e-02 1.000000e-02 6.660000e-01 1.632330e-01 1.632330e-01 +4.550000e+00 1.000000e-02 1.000000e-02 8.240000e-01 1.861961e-01 1.861961e-01 +4.570000e+00 1.000000e-02 1.000000e-02 5.710000e-01 1.494657e-01 1.494657e-01 +4.590000e+00 1.000000e-02 1.000000e-02 5.740000e-01 1.526106e-01 1.526106e-01 +4.610000e+00 1.000000e-02 1.000000e-02 4.780000e-01 1.428041e-01 1.428041e-01 +4.630000e+00 1.000000e-02 1.000000e-02 4.510000e-01 1.324009e-01 1.324009e-01 +4.650000e+00 1.000000e-02 1.000000e-02 5.220000e-01 1.493084e-01 1.493084e-01 +4.670000e+00 1.000000e-02 1.000000e-02 5.180000e-01 1.392049e-01 1.392049e-01 +4.690000e+00 1.000000e-02 1.000000e-02 6.240000e-01 1.592482e-01 1.592482e-01 +4.710000e+00 1.000000e-02 1.000000e-02 5.830000e-01 1.503064e-01 1.503064e-01 +4.730000e+00 1.000000e-02 1.000000e-02 5.640000e-01 1.449310e-01 1.449310e-01 +4.750000e+00 1.000000e-02 1.000000e-02 4.010000e-01 1.221966e-01 1.221966e-01 +4.770000e+00 1.000000e-02 1.000000e-02 3.270000e-01 1.072241e-01 1.072241e-01 +4.790000e+00 1.000000e-02 1.000000e-02 5.150000e-01 1.333304e-01 1.333304e-01 +4.810000e+00 1.000000e-02 1.000000e-02 4.900000e-01 1.394633e-01 1.394633e-01 +4.830000e+00 1.000000e-02 1.000000e-02 6.900000e-02 6.140033e-02 6.140033e-02 +4.850000e+00 1.000000e-02 1.000000e-02 1.650000e-01 7.907591e-02 7.907591e-02 +4.870000e+00 1.000000e-02 1.000000e-02 2.390000e-01 8.793179e-02 8.793179e-02 +4.890000e+00 1.000000e-02 1.000000e-02 2.570000e-01 9.808160e-02 9.808160e-02 +4.910000e+00 1.000000e-02 1.000000e-02 2.350000e-01 8.668333e-02 8.668333e-02 +4.930000e+00 1.000000e-02 1.000000e-02 2.530000e-01 9.013878e-02 9.013878e-02 +4.950000e+00 1.000000e-02 1.000000e-02 3.900000e-01 1.121606e-01 1.121606e-01 +4.970000e+00 1.000000e-02 1.000000e-02 3.670000e-01 1.104943e-01 1.104943e-01 +4.990000e+00 1.000000e-02 1.000000e-02 3.050000e-01 1.015135e-01 1.015135e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2007_I723333/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.106, up: 0.106}, sys: {dn: -0.025, up: 0.025}}, 1: {stat: {dn: -0.354, up: 0.354}, sys: {dn: -0.053, up: 0.053}}, 2: {stat: {dn: -0.48, up: 0.48}, sys: {dn: -0.217, up: 0.217}}, 3: {stat: {dn: -0.519, up: 0.519}, sys: {dn: -0.26, up: 0.26}}, 4: {stat: {dn: -0.522, up: 0.522}, sys: {dn: -0.295, up: 0.295}}, 5: {stat: {dn: -0.573, up: 0.573}, sys: {dn: -0.46, up: 0.46}}, 6: {stat: {dn: -0.577, up: 0.577}, sys: {dn: -0.476, up: 0.476}}, 7: {stat: {dn: -0.583, up: 0.583}, sys: {dn: -0.44, up: 0.44}}, 8: {stat: {dn: -0.552, up: 0.552}, sys: {dn: -0.508, up: 0.508}}, 9: {stat: {dn: -0.483, up: 0.483}, sys: {dn: -0.345, up: 0.345}}, 10: {stat: {dn: -0.425, up: 0.425}, sys: {dn: -0.222, up: 0.222}}, 11: {stat: {dn: -0.407, up: 0.407}, sys: {dn: -0.294, up: 0.294}}, 12: {stat: {dn: -0.39, up: 0.39}, sys: {dn: -0.167, up: 0.167}}, 13: {stat: {dn: -0.369, up: 0.369}, sys: {dn: -0.201, up: 0.201}}, 14: {stat: {dn: -0.336, up: 0.336}, sys: {dn: -0.136, up: 0.136}}, 15: {stat: {dn: -0.321, up: 0.321}, sys: {dn: -0.152, up: 0.152}}, 16: {stat: {dn: -0.286, up: 0.286}, sys: {dn: -0.12, up: 0.12}}, 17: {stat: {dn: -0.304, up: 0.304}, sys: {dn: -0.119, up: 0.119}}, 18: {stat: {dn: -0.275, up: 0.275}, sys: {dn: -0.106, up: 0.106}}, 19: {stat: {dn: -0.278, up: 0.278}, sys: {dn: -0.126, up: 0.126}}, 20: {stat: {dn: -0.279, up: 0.279}, sys: {dn: -0.138, up: 0.138}}, 21: {stat: {dn: -0.273, up: 0.273}, sys: {dn: -0.13, up: 0.13}}, 22: {stat: {dn: -0.229, up: 0.229}, sys: {dn: -0.07, up: 0.07}}, 23: {stat: {dn: -0.272, up: 0.272}, sys: {dn: -0.112, up: 0.112}}, 24: {stat: {dn: -0.244, up: 0.244}, sys: {dn: -0.105, up: 0.105}}, 25: {stat: {dn: -0.238, up: 0.238}, sys: {dn: -0.075, up: 0.075}}, 26: {stat: {dn: -0.225, up: 0.225}, sys: {dn: -0.073, up: 0.073}}, 27: {stat: {dn: -0.241, up: 0.241}, sys: {dn: -0.087, up: 0.087}}, 28: {stat: {dn: -0.209, up: 0.209}, sys: {dn: -0.076, up: 0.076}}, 29: {stat: {dn: -0.22, up: 0.22}, sys: {dn: -0.071, up: 0.071}}, 30: {stat: {dn: -0.199, up: 0.199}, sys: {dn: -0.062, up: 0.062}}, 31: {stat: {dn: -0.198, up: 0.198}, sys: {dn: -0.081, up: 0.081}}, 32: {stat: {dn: -0.196, up: 0.196}, sys: {dn: -0.056, up: 0.056}}, 33: {stat: {dn: -0.194, up: 0.194}, sys: {dn: -0.068, up: 0.068}}, 34: {stat: {dn: -0.161, up: 0.161}, sys: {dn: -0.038, up: 0.038}}, 35: {stat: {dn: -0.213, up: 0.213}, sys: {dn: -0.11, up: 0.11}}, 36: {stat: {dn: -0.163, up: 0.163}, sys: {dn: -0.038, up: 0.038}}, 37: {stat: {dn: -0.176, up: 0.176}, sys: {dn: -0.074, up: 0.074}}, 38: {stat: {dn: -0.187, up: 0.187}, sys: {dn: -0.068, up: 0.068}}, 39: {stat: {dn: -0.163, up: 0.163}, sys: {dn: -0.06, up: 0.06}}, 40: {stat: {dn: -0.159, up: 0.159}, sys: {dn: -0.05, up: 0.05}}, 41: {stat: {dn: -0.156, up: 0.156}, sys: {dn: -0.047, up: 0.047}}, 42: {stat: {dn: -0.139, up: 0.139}, sys: {dn: -0.044, up: 0.044}}, 43: {stat: {dn: -0.181, up: 0.181}, sys: {dn: -0.07, up: 0.07}}, 44: {stat: {dn: -0.13, up: 0.13}, sys: {dn: -0.018, up: 0.018}}, 45: {stat: {dn: -0.141, up: 0.141}, sys: {dn: -0.041, up: 0.041}}, 46: {stat: {dn: -0.17, up: 0.17}, sys: {dn: -0.072, up: 0.072}}, 47: {stat: {dn: -0.174, up: 0.174}, sys: {dn: -0.042, up: 0.042}}, 48: {stat: {dn: -0.192, up: 0.192}, sys: {dn: -0.084, up: 0.084}}, 49: {stat: {dn: -0.112, up: 0.112}, sys: {dn: -0.007, up: 0.007}}, 50: {stat: {dn: -0.141, up: 0.141}, sys: {dn: -0.043, up: 0.043}}, 51: {stat: {dn: -0.097, up: 0.097}, sys: {dn: -0.025, up: 0.025}}, 52: {stat: {dn: -0.138, up: 0.138}, sys: {dn: -0.04, up: 0.04}}, 53: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.022, up: 0.022}}, 54: {stat: {dn: -0.129, up: 0.129}, sys: {dn: -0.029, up: 0.029}}, 55: {stat: {dn: -0.143, up: 0.143}, sys: {dn: -0.05, up: 0.05}}, 56: {stat: {dn: -0.14, up: 0.14}, sys: {dn: -0.049, up: 0.049}}} + +IsRef: 1 +Path: /REF/BELLE_2007_I723333/d02-x01-y01 +Title: doi:10.17182/hepdata.19336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.870000e+00 1.000000e-02 1.000000e-02 -2.360000e-01 1.089082e-01 1.089082e-01 +3.890000e+00 1.000000e-02 1.000000e-02 4.820000e-01 3.579455e-01 3.579455e-01 +3.910000e+00 1.000000e-02 1.000000e-02 1.980000e+00 5.267722e-01 5.267722e-01 +3.930000e+00 1.000000e-02 1.000000e-02 2.372000e+00 5.804834e-01 5.804834e-01 +3.950000e+00 1.000000e-02 1.000000e-02 2.682000e+00 5.995907e-01 5.995907e-01 +3.970000e+00 1.000000e-02 1.000000e-02 4.187000e+00 7.347986e-01 7.347986e-01 +3.990000e+00 1.000000e-02 1.000000e-02 4.332000e+00 7.480007e-01 7.480007e-01 +4.010000e+00 1.000000e-02 1.000000e-02 4.005000e+00 7.304033e-01 7.304033e-01 +4.030000e+00 1.000000e-02 1.000000e-02 4.627000e+00 7.501786e-01 7.501786e-01 +4.050000e+00 1.000000e-02 1.000000e-02 3.142000e+00 5.935604e-01 5.935604e-01 +4.070000e+00 1.000000e-02 1.000000e-02 2.018000e+00 4.794883e-01 4.794883e-01 +4.090000e+00 1.000000e-02 1.000000e-02 2.679000e+00 5.020807e-01 5.020807e-01 +4.110000e+00 1.000000e-02 1.000000e-02 1.519000e+00 4.242511e-01 4.242511e-01 +4.130000e+00 1.000000e-02 1.000000e-02 1.834000e+00 4.201928e-01 4.201928e-01 +4.150000e+00 1.000000e-02 1.000000e-02 1.240000e+00 3.624803e-01 3.624803e-01 +4.170000e+00 1.000000e-02 1.000000e-02 1.390000e+00 3.551690e-01 3.551690e-01 +4.190000e+00 1.000000e-02 1.000000e-02 1.097000e+00 3.101548e-01 3.101548e-01 +4.210000e+00 1.000000e-02 1.000000e-02 1.081000e+00 3.264613e-01 3.264613e-01 +4.230000e+00 1.000000e-02 1.000000e-02 9.640000e-01 2.947219e-01 2.947219e-01 +4.250000e+00 1.000000e-02 1.000000e-02 1.145000e+00 3.052212e-01 3.052212e-01 +4.270000e+00 1.000000e-02 1.000000e-02 1.262000e+00 3.112636e-01 3.112636e-01 +4.290000e+00 1.000000e-02 1.000000e-02 1.184000e+00 3.023723e-01 3.023723e-01 +4.310000e+00 1.000000e-02 1.000000e-02 6.430000e-01 2.394598e-01 2.394598e-01 +4.330000e+00 1.000000e-02 1.000000e-02 1.020000e+00 2.941564e-01 2.941564e-01 +4.350000e+00 1.000000e-02 1.000000e-02 9.580000e-01 2.656332e-01 2.656332e-01 +4.370000e+00 1.000000e-02 1.000000e-02 6.860000e-01 2.495376e-01 2.495376e-01 +4.390000e+00 1.000000e-02 1.000000e-02 6.660000e-01 2.365460e-01 2.365460e-01 +4.410000e+00 1.000000e-02 1.000000e-02 7.990000e-01 2.562226e-01 2.562226e-01 +4.430000e+00 1.000000e-02 1.000000e-02 6.910000e-01 2.223893e-01 2.223893e-01 +4.450000e+00 1.000000e-02 1.000000e-02 6.510000e-01 2.311731e-01 2.311731e-01 +4.470000e+00 1.000000e-02 1.000000e-02 5.640000e-01 2.084346e-01 2.084346e-01 +4.490000e+00 1.000000e-02 1.000000e-02 7.360000e-01 2.139276e-01 2.139276e-01 +4.510000e+00 1.000000e-02 1.000000e-02 5.170000e-01 2.038431e-01 2.038431e-01 +4.530000e+00 1.000000e-02 1.000000e-02 6.250000e-01 2.055724e-01 2.055724e-01 +4.550000e+00 1.000000e-02 1.000000e-02 3.500000e-01 1.654237e-01 1.654237e-01 +4.570000e+00 1.000000e-02 1.000000e-02 1.007000e+00 2.397269e-01 2.397269e-01 +4.590000e+00 1.000000e-02 1.000000e-02 3.470000e-01 1.673708e-01 1.673708e-01 +4.610000e+00 1.000000e-02 1.000000e-02 6.800000e-01 1.909241e-01 1.909241e-01 +4.630000e+00 1.000000e-02 1.000000e-02 6.260000e-01 1.989799e-01 1.989799e-01 +4.650000e+00 1.000000e-02 1.000000e-02 5.510000e-01 1.736923e-01 1.736923e-01 +4.670000e+00 1.000000e-02 1.000000e-02 4.550000e-01 1.666763e-01 1.666763e-01 +4.690000e+00 1.000000e-02 1.000000e-02 4.280000e-01 1.629264e-01 1.629264e-01 +4.710000e+00 1.000000e-02 1.000000e-02 4.000000e-01 1.457978e-01 1.457978e-01 +4.730000e+00 1.000000e-02 1.000000e-02 6.400000e-01 1.940644e-01 1.940644e-01 +4.750000e+00 1.000000e-02 1.000000e-02 1.720000e-01 1.312402e-01 1.312402e-01 +4.770000e+00 1.000000e-02 1.000000e-02 3.740000e-01 1.468400e-01 1.468400e-01 +4.790000e+00 1.000000e-02 1.000000e-02 6.620000e-01 1.846185e-01 1.846185e-01 +4.810000e+00 1.000000e-02 1.000000e-02 3.840000e-01 1.789972e-01 1.789972e-01 +4.830000e+00 1.000000e-02 1.000000e-02 7.700000e-01 2.095710e-01 2.095710e-01 +4.850000e+00 1.000000e-02 1.000000e-02 6.300000e-02 1.122185e-01 1.122185e-01 +4.870000e+00 1.000000e-02 1.000000e-02 3.990000e-01 1.474110e-01 1.474110e-01 +4.890000e+00 1.000000e-02 1.000000e-02 2.340000e-01 1.001699e-01 1.001699e-01 +4.910000e+00 1.000000e-02 1.000000e-02 3.660000e-01 1.436802e-01 1.436802e-01 +4.930000e+00 1.000000e-02 1.000000e-02 2.090000e-01 1.023914e-01 1.023914e-01 +4.950000e+00 1.000000e-02 1.000000e-02 2.650000e-01 1.322195e-01 1.322195e-01 +4.970000e+00 1.000000e-02 1.000000e-02 4.570000e-01 1.514893e-01 1.514893e-01 +4.990000e+00 1.000000e-02 1.000000e-02 4.460000e-01 1.483273e-01 1.483273e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2007_I753243.cc b/analyses/pluginBELLE/BELLE_2007_I753243.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I753243.cc @@ -0,0 +1,96 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2007_I753243 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2007_I753243); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + declare(UnstableParticles(), "UFS"); + _hist_Kpi = bookHisto1D( 1, 1, 1); + + } + + void findDecayProducts(const Particle & mother, unsigned int & nstable, + unsigned int & npip, unsigned int & npim, + unsigned int & nK, FourMomentum & ptot) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if (id == PID::K0S ) { + ++nK; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::PIPLUS) { + ++npip; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::PIMINUS) { + ++npim; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::PI0 || id == PID::KPLUS || + id == PID::KMINUS) { + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p, nstable, npip, npim, nK,ptot); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + // Loop over taus + for(const Particle& tau : apply(event, "UFS").particles(Cuts::abspid==PID::TAU)) { + unsigned int nstable(0),npip(0),npim(0),nK(0); + FourMomentum p_tot(0,0,0,0); + findDecayProducts(tau, nstable, npip, npim, nK, p_tot); + if (tau.pdgId() < 0) swap(npip, npim); + if(nstable==3 && npim==1 && nK==1) + _hist_Kpi->fill(p_tot.mass(), event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + normalize(_hist_Kpi); + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _hist_Kpi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2007_I753243); + + +} diff --git a/analyses/pluginBELLE/BELLE_2007_I753243.info b/analyses/pluginBELLE/BELLE_2007_I753243.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I753243.info @@ -0,0 +1,32 @@ +Name: BELLE_2007_I753243 +Year: 2007 +Summary: $K_S^0\pi^-$ spectrum in $\tau$ decays +Experiment: BELLE +Collider: KEKB +InspireID: 753243 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B654 (2007) 65-73 +RunInfo: e+ e- > tau+ tau-, or any process producing tau leptons +NeedCrossSection: no +Description: + 'Measurement of the spectrum of $K_S^0\pi^-$ spectrum in $\tau$ decays by BELLE. Useful for testing models of the hadronic current in $\tau$ decays.' +Keywords: [] +BibKey: Epifanov:2007rf +BibTeX: '@article{Epifanov:2007rf, + author = "Epifanov, D. and others", + title = "{Study of tau- ---> K(S) pi- nu(tau) decay at Belle}", + collaboration = "Belle", + journal = "Phys. Lett.", + volume = "B654", + year = "2007", + pages = "65-73", + doi = "10.1016/j.physletb.2007.08.045", + eprint = "0706.2231", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-PREPRINT-2007-28, KEK-PREPRINT-2007-17", + SLACcitation = "%%CITATION = ARXIV:0706.2231;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2007_I753243.plot b/analyses/pluginBELLE/BELLE_2007_I753243.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I753243.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BELLE_2007_I753243/d01-x01-y01 +Title=$K^0_S\pi^-$ mass in $\tau^-\to K^0_S\pi^-\nu_\tau$ decays +XLabel=$m_{K^0_S\pi^-}$ [$\text{GeV}$] +YLabel=$1/\Gamma\text{d}\Gamma/\text{d}m_{K^0_S\pi^-}$ [ $\text{GeV}^{-1}$] +LogY=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2007_I753243.yoda b/analyses/pluginBELLE/BELLE_2007_I753243.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I753243.yoda @@ -0,0 +1,108 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2007_I753243/d01-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2007_I753243/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.63575 0.00575 0.00575 0.01118 0.00989 0.00989 +0.64725 0.00575 0.00575 0.05067 0.03556 0.03556 +0.65875 0.00575 0.00575 0.07109 0.02664 0.02664 +0.67025 0.00575 0.00575 0.05823 0.03188 0.03188 +0.68175 0.00575 0.00575 0.19600 0.04730 0.04730 +0.69325 0.00575 0.00575 0.18412 0.03433 0.03433 +0.70475 0.00575 0.00575 0.18844 0.03728 0.03728 +0.71625 0.00575 0.00575 0.12470 0.03171 0.03171 +0.72775 0.00575 0.00575 0.16022 0.04072 0.04072 +0.73925 0.00575 0.00575 0.19650 0.03887 0.03887 +0.75075 0.00575 0.00575 0.24746 0.04612 0.04612 +0.76225 0.00575 0.00575 0.31197 0.04596 0.04596 +0.77375 0.00575 0.00575 0.38061 0.04412 0.04412 +0.78525 0.00575 0.00575 0.43765 0.04725 0.04725 +0.79675 0.00575 0.00575 0.50624 0.04884 0.04884 +0.80825 0.00575 0.00575 0.61154 0.05151 0.05151 +0.81975 0.00575 0.00575 1.02886 0.05833 0.05833 +0.83125 0.00575 0.00575 1.25126 0.06410 0.06410 +0.84275 0.00575 0.00575 1.94741 0.07446 0.07446 +0.85425 0.00575 0.00575 3.20032 0.08952 0.08952 +0.86575 0.00575 0.00575 5.68674 0.11573 0.11573 +0.87725 0.00575 0.00575 9.57489 0.14900 0.14900 +0.88875 0.00575 0.00575 13.07850 0.17615 0.17615 +0.90025 0.00575 0.00575 12.83146 0.17565 0.17565 +0.91175 0.00575 0.00575 8.97121 0.14504 0.14504 +0.92325 0.00575 0.00575 5.39607 0.11174 0.11174 +0.93475 0.00575 0.00575 3.61815 0.09145 0.09145 +0.94625 0.00575 0.00575 2.68666 0.07986 0.07986 +0.95775 0.00575 0.00575 1.95676 0.06907 0.06907 +0.96925 0.00575 0.00575 1.40083 0.05899 0.05899 +0.98075 0.00575 0.00575 1.12485 0.05463 0.05463 +0.99225 0.00575 0.00575 0.94942 0.05118 0.05118 +1.00375 0.00575 0.00575 0.76553 0.04555 0.04555 +1.01525 0.00575 0.00575 0.67588 0.04322 0.04322 +1.02675 0.00575 0.00575 0.55311 0.04000 0.04000 +1.03825 0.00575 0.00575 0.52194 0.03923 0.03923 +1.04975 0.00575 0.00575 0.46156 0.03831 0.03831 +1.06125 0.00575 0.00575 0.44322 0.03838 0.03838 +1.07275 0.00575 0.00575 0.41175 0.03551 0.03551 +1.08425 0.00575 0.00575 0.30183 0.03243 0.03243 +1.09575 0.00575 0.00575 0.30376 0.03286 0.03286 +1.10725 0.00575 0.00575 0.26531 0.03017 0.03017 +1.11875 0.00575 0.00575 0.24433 0.03066 0.03066 +1.13025 0.00575 0.00575 0.19872 0.02788 0.02788 +1.14175 0.00575 0.00575 0.18220 0.02451 0.02451 +1.15325 0.00575 0.00575 0.18210 0.02652 0.02652 +1.16475 0.00575 0.00575 0.15722 0.02510 0.02510 +1.17625 0.00575 0.00575 0.17267 0.02433 0.02433 +1.18775 0.00575 0.00575 0.15465 0.02361 0.02361 +1.19925 0.00575 0.00575 0.13474 0.02073 0.02073 +1.21075 0.00575 0.00575 0.13006 0.02084 0.02084 +1.22225 0.00575 0.00575 0.10691 0.02127 0.02127 +1.23375 0.00575 0.00575 0.10972 0.01986 0.01986 +1.24525 0.00575 0.00575 0.11256 0.01896 0.01896 +1.25675 0.00575 0.00575 0.10571 0.01875 0.01875 +1.26825 0.00575 0.00575 0.13117 0.02174 0.02174 +1.27975 0.00575 0.00575 0.10552 0.01853 0.01853 +1.29125 0.00575 0.00575 0.09014 0.01830 0.01830 +1.30275 0.00575 0.00575 0.08052 0.01627 0.01627 +1.31425 0.00575 0.00575 0.08823 0.01596 0.01596 +1.32575 0.00575 0.00575 0.10054 0.01884 0.01884 +1.33725 0.00575 0.00575 0.09984 0.01740 0.01740 +1.34875 0.00575 0.00575 0.10679 0.01789 0.01789 +1.36025 0.00575 0.00575 0.08720 0.01676 0.01676 +1.37175 0.00575 0.00575 0.06626 0.01662 0.01662 +1.38325 0.00575 0.00575 0.08654 0.01562 0.01562 +1.39475 0.00575 0.00575 0.06626 0.01693 0.01693 +1.40625 0.00575 0.00575 0.07366 0.01365 0.01365 +1.41775 0.00575 0.00575 0.06830 0.01275 0.01275 +1.42925 0.00575 0.00575 0.04540 0.01336 0.01336 +1.44075 0.00575 0.00575 0.05905 0.01288 0.01288 +1.45225 0.00575 0.00575 0.03358 0.01074 0.01074 +1.46375 0.00575 0.00575 0.04876 0.01063 0.01063 +1.47525 0.00575 0.00575 0.03150 0.00927 0.00927 +1.48675 0.00575 0.00575 0.04062 0.00938 0.00938 +1.49825 0.00575 0.00575 0.03528 0.01521 0.01521 +1.50975 0.00575 0.00575 0.03857 0.01017 0.01017 +1.52125 0.00575 0.00575 0.02896 0.01049 0.01049 +1.53275 0.00575 0.00575 0.02570 0.00933 0.00933 +1.54425 0.00575 0.00575 0.03242 0.01212 0.01212 +1.55575 0.00575 0.00575 0.01449 0.00676 0.00676 +1.56725 0.00575 0.00575 0.00946 0.00530 0.00530 +1.57875 0.00575 0.00575 0.00832 0.00414 0.00414 +1.59025 0.00575 0.00575 0.01655 0.00586 0.00586 +1.60175 0.00575 0.00575 0.01696 0.00607 0.00607 +1.61325 0.00575 0.00575 0.02772 0.00810 0.00810 +1.62475 0.00575 0.00575 0.00445 0.00295 0.00295 +1.63625 0.00575 0.00575 0.00268 0.00255 0.00255 +1.64775 0.00575 0.00575 0.00730 0.00437 0.00437 +1.65925 0.00575 0.00575 0.01125 0.00727 0.00727 +1.67075 0.00575 0.00575 0.00359 0.00401 0.00401 +1.68225 0.00575 0.00575 0.00435 0.00287 0.00287 +1.69375 0.00575 0.00575 0.00327 0.00637 0.00637 +1.70525 0.00575 0.00575 0.00164 0.00287 0.00287 +1.71675 0.00575 0.00575 0.00246 0.00260 0.00260 +1.72825 0.00575 0.00575 0.00164 0.00138 0.00138 +1.73975 0.00575 0.00575 0.00000 0.00047 0.00047 +1.75125 0.00575 0.00575 0.00627 0.00327 0.00327 +1.76275 0.00575 0.00575 0.00290 0.00236 0.00236 +1.77425 0.00575 0.00575 0.00491 0.00285 0.00285 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2007_I756012.cc b/analyses/pluginBELLE/BELLE_2007_I756012.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I756012.cc @@ -0,0 +1,117 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2007_I756012 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2007_I756012); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nJPsi = bookCounter("TMP/jpsi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=443) continue; + // find the J/psi + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // J/psi pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nJPsi->fill(event.weight()); + break; + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nJPsi->val(); + double error = _nJPsi->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nJPsi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2007_I756012); + + +} diff --git a/analyses/pluginBELLE/BELLE_2007_I756012.info b/analyses/pluginBELLE/BELLE_2007_I756012.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I756012.info @@ -0,0 +1,34 @@ +Name: BELLE_2007_I756012 +Year: 2007 +Summary: Cross section for $e^+e^-\to J\psi\pi^+\pi^-$ at energies between 3.8 and 5.5 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 756012 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 99 (2007) 182004, 2007 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to J\psi\pi^+\pi^-$ at energies between 3.8 and 5.5 GeV using radiative return by BELLE.' +BibKey: Yuan:2007sj +BibTeX: '@article{Yuan:2007sj, + author = "Yuan, C. Z. and others", + title = "{Measurement of e+ e- ---> pi+ pi- J/psi cross-section + via initial state radiation at Belle}", + collaboration = "Belle", + journal = "Phys. Rev. Lett.", + volume = "99", + year = "2007", + pages = "182004", + doi = "10.1103/PhysRevLett.99.182004", + eprint = "0707.2541", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-PREPRINT-2007-31, KEK-PREPRINT-2007-23", + SLACcitation = "%%CITATION = ARXIV:0707.2541;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2007_I756012.plot b/analyses/pluginBELLE/BELLE_2007_I756012.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I756012.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BELLE_2007_I756012/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-J/\psi)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-J/\psi)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2007_I756012.yoda b/analyses/pluginBELLE/BELLE_2007_I756012.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I756012.yoda @@ -0,0 +1,96 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2007_I756012/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -9.206, up: 9.206}, 'sys,Additional systematic error.': {dn: -0.9732000000000001, up: 0.9732000000000001}}, 1: {error: {dn: -8.35, up: 8.35}, 'sys,Additional systematic error.': {dn: -0.42315, up: 0.42315}}, 2: {error: {dn: -10.738, up: 10.738}, 'sys,Additional systematic error.': {dn: -1.7006999999999999, up: 1.7006999999999999}}, 3: {error: {dn: -8.427, up: 8.427}, 'sys,Additional systematic error.': {dn: -0.467775, up: 0.467775}}, 4: {error: {dn: -7.872, up: 7.872}, 'sys,Additional systematic error.': {dn: -0.75045, up: 0.75045}}, 5: {error: {dn: -9.007, up: 9.007}, 'sys,Additional systematic error.': {dn: -1.521525, up: 1.521525}}, 6: {error: {dn: -8.868, up: 8.868}, 'sys,Additional systematic error.': {dn: -1.2626249999999999, up: 1.2626249999999999}}, 7: {error: {dn: -9.155, up: 9.155}, 'sys,Additional systematic error.': {dn: -1.2246750000000002, up: 1.2246750000000002}}, 8: {error: {dn: -9.686, up: 9.686}, 'sys,Additional systematic error.': {dn: -1.51995, up: 1.51995}}, 9: {error: {dn: -9.227, up: 9.227}, 'sys,Additional systematic error.': {dn: -1.799775, up: 1.799775}}, 10: {error: {dn: -7.65, up: 7.65}, 'sys,Additional systematic error.': {dn: -0.7520249999999999, up: 0.7520249999999999}}, 11: {error: {dn: -10.679, up: 10.679}, 'sys,Additional systematic error.': {dn: -2.687925, up: 2.687925}}, 12: {error: {dn: -7.461, up: 7.461}, 'sys,Additional systematic error.': {dn: -1.1934749999999998, up: 1.1934749999999998}}, 13: {error: {dn: -8.625, up: 8.625}, 'sys,Additional systematic error.': {dn: -1.9251750000000003, up: 1.9251750000000003}}, 14: {error: {dn: -8.337, up: 8.337}, 'sys,Additional systematic error.': {dn: -1.370775, up: 1.370775}}, 15: {error: {dn: -9.92, up: 9.92}, 'sys,Additional systematic error.': {dn: -2.8526249999999997, up: 2.8526249999999997}}, 16: {error: {dn: -6.779, up: 6.779}, 'sys,Additional systematic error.': {dn: -0.54915, up: 0.54915}}, 17: {error: {dn: -6.805, up: 6.805}, 'sys,Additional systematic error.': {dn: -0.32384999999999997, up: 0.32384999999999997}}, 18: {error: {dn: -6.794, up: 6.794}, 'sys,Additional systematic error.': {dn: -0.7932750000000001, up: 0.7932750000000001}}, 19: {error: {dn: -8.394, up: 8.394}, 'sys,Additional systematic error.': {dn: -1.7142000000000002, up: 1.7142000000000002}}, 20: {error: {dn: -9.959, up: 9.959}, 'sys,Additional systematic error.': {dn: -3.16605, up: 3.16605}}, 21: {error: {dn: -12.019, up: 12.019}, 'sys,Additional systematic error.': {dn: -4.9235999999999995, up: 4.9235999999999995}}, 22: {error: {dn: -12.769, up: 12.769}, 'sys,Additional systematic error.': {dn: -5.193525, up: 5.193525}}, 23: {error: {dn: -12.063, up: 12.063}, 'sys,Additional systematic error.': {dn: -4.822875000000001, up: 4.822875000000001}}, 24: {error: {dn: -11.304, up: 11.304}, 'sys,Additional systematic error.': {dn: -4.03275, up: 4.03275}}, 25: {error: {dn: -10.271, up: 10.271}, 'sys,Additional systematic error.': {dn: -3.3604499999999997, up: 3.3604499999999997}}, 26: {error: {dn: -9.66, up: 9.66}, 'sys,Additional systematic error.': {dn: -2.754375, up: 2.754375}}, 27: {error: {dn: -9.938, up: 9.938}, 'sys,Additional systematic error.': {dn: -3.40815, up: 3.40815}}, 28: {error: {dn: -7.97, up: 7.97}, 'sys,Additional systematic error.': {dn: -1.4099249999999999, up: 1.4099249999999999}}, 29: {error: {dn: -6.388, up: 6.388}, 'sys,Additional systematic error.': {dn: -0.8085, up: 0.8085}}, 30: {error: {dn: -7.092, up: 7.092}, 'sys,Additional systematic error.': {dn: -1.5962250000000002, up: 1.5962250000000002}}, 31: {error: {dn: -7.68, up: 7.68}, 'sys,Additional systematic error.': {dn: -1.8837, up: 1.8837}}, 32: {error: {dn: -5.413, up: 5.413}, 'sys,Additional systematic error.': {dn: -0.86595, up: 0.86595}}, 33: {error: {dn: -5.472, up: 5.472}, 'sys,Additional systematic error.': {dn: -0.685125, up: 0.685125}}, 34: {error: {dn: -5.996, up: 5.996}, 'sys,Additional systematic error.': {dn: -0.8044500000000001, up: 0.8044500000000001}}, 35: {error: {dn: -5.143, up: 5.143}, 'sys,Additional systematic error.': {dn: -0.460875, up: 0.460875}}, 36: {error: {dn: -6.121, up: 6.121}, 'sys,Additional systematic error.': {dn: -0.8699999999999999, up: 0.8699999999999999}}, 37: {error: {dn: -3.976, up: 3.976}, 'sys,Additional systematic error.': {dn: -0.2871, up: 0.2871}}, 38: {error: {dn: -6.234, up: 6.234}, 'sys,Additional systematic error.': {dn: -1.419225, up: 1.419225}}, 39: {error: {dn: -5.132, up: 5.132}, 'sys,Additional systematic error.': {dn: -0.642525, up: 0.642525}}, 40: {error: {dn: -4.708, up: 4.708}, 'sys,Additional systematic error.': {dn: -0.675675, up: 0.675675}}, 41: {error: {dn: -4.892, up: 4.892}, 'sys,Additional systematic error.': {dn: -0.826425, up: 0.826425}}, 42: {error: {dn: -4.873, up: 4.873}, 'sys,Additional systematic error.': {dn: -0.7795500000000001, up: 0.7795500000000001}}, 43: {error: {dn: -3.952, up: 3.952}, 'sys,Additional systematic error.': {dn: -0.03915, up: 0.03915}}, 44: {error: {dn: -3.71, up: 3.71}, 'sys,Additional systematic error.': {dn: 0.1905, up: -0.1905}}, 45: {error: {dn: -4.46, up: 4.46}, 'sys,Additional systematic error.': {dn: -0.22784999999999997, up: 0.22784999999999997}}, 46: {error: {dn: -4.305, up: 4.305}, 'sys,Additional systematic error.': {dn: -0.375825, up: 0.375825}}, 47: {error: {dn: -4.572, up: 4.572}, 'sys,Additional systematic error.': {dn: -0.409725, up: 0.409725}}, 48: {error: {dn: -3.612, up: 3.612}, 'sys,Additional systematic error.': {dn: -0.22155, up: 0.22155}}, 49: {error: {dn: -3.867, up: 3.867}, 'sys,Additional systematic error.': {dn: -0.32924999999999993, up: 0.32924999999999993}}, 50: {error: {dn: -2.938, up: 2.938}, 'sys,Additional systematic error.': {dn: 0.03584999999999999, up: -0.03584999999999999}}, 51: {error: {dn: -4.643, up: 4.643}, 'sys,Additional systematic error.': {dn: -0.5034, up: 0.5034}}, 52: {error: {dn: -4.22, up: 4.22}, 'sys,Additional systematic error.': {dn: -0.17865, up: 0.17865}}, 53: {error: {dn: -3.708, up: 3.708}, 'sys,Additional systematic error.': {dn: -0.353475, up: 0.353475}}, 54: {error: {dn: -3.463, up: 3.463}, 'sys,Additional systematic error.': {dn: -0.1755, up: 0.1755}}, 55: {error: {dn: -2.493, up: 2.493}, 'sys,Additional systematic error.': {dn: 0.17332499999999998, up: -0.17332499999999998}}, 56: {error: {dn: -3.897, up: 3.897}, 'sys,Additional systematic error.': {dn: -0.4137, up: 0.4137}}, 57: {error: {dn: -3.317, up: 3.317}, 'sys,Additional systematic error.': {dn: -0.239475, up: 0.239475}}, 58: {error: {dn: -4.191, up: 4.191}, 'sys,Additional systematic error.': {dn: -0.33945, up: 0.33945}}, 59: {error: {dn: -4.133, up: 4.133}, 'sys,Additional systematic error.': {dn: -0.37035, up: 0.37035}}, 60: {error: {dn: -3.64, up: 3.64}, 'sys,Additional systematic error.': {dn: -0.16725, up: 0.16725}}, 61: {error: {dn: -3.557, up: 3.557}, 'sys,Additional systematic error.': {dn: -0.23204999999999998, up: 0.23204999999999998}}, 62: {error: {dn: -3.791, up: 3.791}, 'sys,Additional systematic error.': {dn: 0.09780000000000001, up: -0.09780000000000001}}, 63: {error: {dn: -4.576, up: 4.576}, 'sys,Additional systematic error.': {dn: -0.6846, up: 0.6846}}, 64: {error: {dn: -4.288, up: 4.288}, 'sys,Additional systematic error.': {dn: -0.679125, up: 0.679125}}, 65: {error: {dn: -3.312, up: 3.312}, 'sys,Additional systematic error.': {dn: -0.00045, up: 0.00045}}, 66: {error: {dn: -3.499, up: 3.499}, 'sys,Additional systematic error.': {dn: -0.1278, up: 0.1278}}, 67: {error: {dn: -3.498, up: 3.498}, 'sys,Additional systematic error.': {dn: -0.09525, up: 0.09525}}, 68: {error: {dn: -3.154, up: 3.154}, 'sys,Additional systematic error.': {dn: 0.28147500000000003, up: -0.28147500000000003}}, 69: {error: {dn: -3.823, up: 3.823}, 'sys,Additional systematic error.': {dn: -0.3426, up: 0.3426}}, 70: {error: {dn: -2.635, up: 2.635}, 'sys,Additional systematic error.': {dn: 0.1539, up: -0.1539}}, 71: {error: {dn: -3.676, up: 3.676}, 'sys,Additional systematic error.': {dn: -0.092475, up: 0.092475}}, 72: {error: {dn: -3.217, up: 3.217}, 'sys,Additional systematic error.': {dn: 0.090675, up: -0.090675}}, 73: {error: {dn: -3.507, up: 3.507}, 'sys,Additional systematic error.': {dn: -0.24180000000000004, up: 0.24180000000000004}}, 74: {error: {dn: -3.144, up: 3.144}, 'sys,Additional systematic error.': {dn: 0.0594, up: -0.0594}}, 75: {error: {dn: -4.081, up: 4.081}, 'sys,Additional systematic error.': {dn: -0.41669999999999996, up: 0.41669999999999996}}, 76: {error: {dn: -4.503, up: 4.503}, 'sys,Additional systematic error.': {dn: -0.7381500000000001, up: 0.7381500000000001}}, 77: {error: {dn: -2.469, up: 2.469}, 'sys,Additional systematic error.': {dn: 0.11677499999999999, up: -0.11677499999999999}}, 78: {error: {dn: -2.599, up: 2.599}, 'sys,Additional systematic error.': {dn: 0.26115000000000005, up: -0.26115000000000005}}, 79: {error: {dn: -3.462, up: 3.462}, 'sys,Additional systematic error.': {dn: -0.087075, up: 0.087075}}, 80: {error: {dn: -2.59, up: 2.59}, 'sys,Additional systematic error.': {dn: -0.0576, up: 0.0576}}, 81: {error: {dn: -3.26, up: 3.26}, 'sys,Additional systematic error.': {dn: -0.28462499999999996, up: 0.28462499999999996}}, 82: {error: {dn: -2.686, up: 2.686}, 'sys,Additional systematic error.': {dn: 0.08422500000000001, up: -0.08422500000000001}}, 83: {error: {dn: -3.361, up: 3.361}, 'sys,Additional systematic error.': {dn: -0.084525, up: 0.084525}}, 84: {error: {dn: -2.621, up: 2.621}, 'sys,Additional systematic error.': {dn: 0.0552, up: -0.0552}}} + +IsRef: 1 +Path: /REF/BELLE_2007_I756012/d01-x01-y01 +Title: doi:10.17182/hepdata.50926.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 1.000000e-02 1.000000e-02 1.297600e+01 9.257297e+00 9.257297e+00 +3.830000e+00 1.000000e-02 1.000000e-02 5.642000e+00 8.360715e+00 8.360715e+00 +3.850000e+00 1.000000e-02 1.000000e-02 2.267600e+01 1.087185e+01 1.087185e+01 +3.870000e+00 1.000000e-02 1.000000e-02 6.237000e+00 8.439973e+00 8.439973e+00 +3.890000e+00 1.000000e-02 1.000000e-02 1.000600e+01 7.907690e+00 7.907690e+00 +3.910000e+00 1.000000e-02 1.000000e-02 2.028700e+01 9.134609e+00 9.134609e+00 +3.930000e+00 1.000000e-02 1.000000e-02 1.683500e+01 8.957435e+00 8.957435e+00 +3.950000e+00 1.000000e-02 1.000000e-02 1.632900e+01 9.236550e+00 9.236550e+00 +3.970000e+00 1.000000e-02 1.000000e-02 2.026600e+01 9.804532e+00 9.804532e+00 +3.990000e+00 1.000000e-02 1.000000e-02 2.399700e+01 9.400889e+00 9.400889e+00 +4.010000e+00 1.000000e-02 1.000000e-02 1.002700e+01 7.686875e+00 7.686875e+00 +4.030000e+00 1.000000e-02 1.000000e-02 3.583900e+01 1.101208e+01 1.101208e+01 +4.050000e+00 1.000000e-02 1.000000e-02 1.591300e+01 7.555852e+00 7.555852e+00 +4.070000e+00 1.000000e-02 1.000000e-02 2.566900e+01 8.837246e+00 8.837246e+00 +4.090000e+00 1.000000e-02 1.000000e-02 1.827700e+01 8.448940e+00 8.448940e+00 +4.110000e+00 1.000000e-02 1.000000e-02 3.803500e+01 1.032201e+01 1.032201e+01 +4.130000e+00 1.000000e-02 1.000000e-02 7.322000e+00 6.801206e+00 6.801206e+00 +4.150000e+00 1.000000e-02 1.000000e-02 4.318000e+00 6.812702e+00 6.812702e+00 +4.170000e+00 1.000000e-02 1.000000e-02 1.057700e+01 6.840155e+00 6.840155e+00 +4.190000e+00 1.000000e-02 1.000000e-02 2.285600e+01 8.567247e+00 8.567247e+00 +4.210000e+00 1.000000e-02 1.000000e-02 4.221400e+01 1.045015e+01 1.045015e+01 +4.230000e+00 1.000000e-02 1.000000e-02 6.564800e+01 1.298839e+01 1.298839e+01 +4.250000e+00 1.000000e-02 1.000000e-02 6.924700e+01 1.378478e+01 1.378478e+01 +4.270000e+00 1.000000e-02 1.000000e-02 6.430500e+01 1.299139e+01 1.299139e+01 +4.290000e+00 1.000000e-02 1.000000e-02 5.377000e+01 1.200181e+01 1.200181e+01 +4.310000e+00 1.000000e-02 1.000000e-02 4.480600e+01 1.080676e+01 1.080676e+01 +4.330000e+00 1.000000e-02 1.000000e-02 3.672500e+01 1.004501e+01 1.004501e+01 +4.350000e+00 1.000000e-02 1.000000e-02 4.544200e+01 1.050616e+01 1.050616e+01 +4.370000e+00 1.000000e-02 1.000000e-02 1.879900e+01 8.093750e+00 8.093750e+00 +4.390000e+00 1.000000e-02 1.000000e-02 1.078000e+01 6.438961e+00 6.438961e+00 +4.410000e+00 1.000000e-02 1.000000e-02 2.128300e+01 7.269415e+00 7.269415e+00 +4.430000e+00 1.000000e-02 1.000000e-02 2.511600e+01 7.907637e+00 7.907637e+00 +4.450000e+00 1.000000e-02 1.000000e-02 1.154600e+01 5.481828e+00 5.481828e+00 +4.470000e+00 1.000000e-02 1.000000e-02 9.135000e+00 5.514724e+00 5.514724e+00 +4.490000e+00 1.000000e-02 1.000000e-02 1.072600e+01 6.049724e+00 6.049724e+00 +4.510000e+00 1.000000e-02 1.000000e-02 6.145000e+00 5.163609e+00 5.163609e+00 +4.530000e+00 1.000000e-02 1.000000e-02 1.160000e+01 6.182519e+00 6.182519e+00 +4.550000e+00 1.000000e-02 1.000000e-02 3.828000e+00 3.986352e+00 3.986352e+00 +4.570000e+00 1.000000e-02 1.000000e-02 1.892300e+01 6.393509e+00 6.393509e+00 +4.590000e+00 1.000000e-02 1.000000e-02 8.567000e+00 5.172066e+00 5.172066e+00 +4.610000e+00 1.000000e-02 1.000000e-02 9.009000e+00 4.756238e+00 4.756238e+00 +4.630000e+00 1.000000e-02 1.000000e-02 1.101900e+01 4.961315e+00 4.961315e+00 +4.650000e+00 1.000000e-02 1.000000e-02 1.039400e+01 4.934960e+00 4.934960e+00 +4.670000e+00 1.000000e-02 1.000000e-02 5.220000e-01 3.952194e+00 3.952194e+00 +4.690000e+00 1.000000e-02 1.000000e-02 -2.540000e+00 3.714888e+00 3.714888e+00 +4.710000e+00 1.000000e-02 1.000000e-02 3.038000e+00 4.465816e+00 4.465816e+00 +4.730000e+00 1.000000e-02 1.000000e-02 5.011000e+00 4.321374e+00 4.321374e+00 +4.750000e+00 1.000000e-02 1.000000e-02 5.463000e+00 4.590322e+00 4.590322e+00 +4.770000e+00 1.000000e-02 1.000000e-02 2.954000e+00 3.618788e+00 3.618788e+00 +4.790000e+00 1.000000e-02 1.000000e-02 4.390000e+00 3.880991e+00 3.880991e+00 +4.810000e+00 1.000000e-02 1.000000e-02 -4.780000e-01 2.938219e+00 2.938219e+00 +4.830000e+00 1.000000e-02 1.000000e-02 6.712000e+00 4.670210e+00 4.670210e+00 +4.850000e+00 1.000000e-02 1.000000e-02 2.382000e+00 4.223780e+00 4.223780e+00 +4.870000e+00 1.000000e-02 1.000000e-02 4.713000e+00 3.724810e+00 3.724810e+00 +4.890000e+00 1.000000e-02 1.000000e-02 2.340000e+00 3.467444e+00 3.467444e+00 +4.910000e+00 1.000000e-02 1.000000e-02 -2.311000e+00 2.499018e+00 2.499018e+00 +4.930000e+00 1.000000e-02 1.000000e-02 5.516000e+00 3.918897e+00 3.918897e+00 +4.950000e+00 1.000000e-02 1.000000e-02 3.193000e+00 3.325633e+00 3.325633e+00 +4.970000e+00 1.000000e-02 1.000000e-02 4.526000e+00 4.204724e+00 4.204724e+00 +4.990000e+00 1.000000e-02 1.000000e-02 4.938000e+00 4.149560e+00 4.149560e+00 +5.010000e+00 1.000000e-02 1.000000e-02 2.230000e+00 3.643840e+00 3.643840e+00 +5.030000e+00 1.000000e-02 1.000000e-02 3.094000e+00 3.564561e+00 3.564561e+00 +5.050000e+00 1.000000e-02 1.000000e-02 -1.304000e+00 3.792261e+00 3.792261e+00 +5.070000e+00 1.000000e-02 1.000000e-02 9.128000e+00 4.626927e+00 4.626927e+00 +5.090000e+00 1.000000e-02 1.000000e-02 9.055000e+00 4.341446e+00 4.341446e+00 +5.110000e+00 1.000000e-02 1.000000e-02 6.000000e-03 3.312000e+00 3.312000e+00 +5.130000e+00 1.000000e-02 1.000000e-02 1.704000e+00 3.501333e+00 3.501333e+00 +5.150000e+00 1.000000e-02 1.000000e-02 1.270000e+00 3.499297e+00 3.499297e+00 +5.170000e+00 1.000000e-02 1.000000e-02 -3.753000e+00 3.166535e+00 3.166535e+00 +5.190000e+00 1.000000e-02 1.000000e-02 4.568000e+00 3.838320e+00 3.838320e+00 +5.210000e+00 1.000000e-02 1.000000e-02 -2.052000e+00 2.639491e+00 2.639491e+00 +5.230000e+00 1.000000e-02 1.000000e-02 1.233000e+00 3.677163e+00 3.677163e+00 +5.250000e+00 1.000000e-02 1.000000e-02 -1.209000e+00 3.218278e+00 3.218278e+00 +5.270000e+00 1.000000e-02 1.000000e-02 3.224000e+00 3.515326e+00 3.515326e+00 +5.290000e+00 1.000000e-02 1.000000e-02 -7.920000e-01 3.144561e+00 3.144561e+00 +5.310000e+00 1.000000e-02 1.000000e-02 5.556000e+00 4.102219e+00 4.102219e+00 +5.330000e+00 1.000000e-02 1.000000e-02 9.842000e+00 4.563099e+00 4.563099e+00 +5.350000e+00 1.000000e-02 1.000000e-02 -1.557000e+00 2.471760e+00 2.471760e+00 +5.370000e+00 1.000000e-02 1.000000e-02 -3.482000e+00 2.612087e+00 2.612087e+00 +5.390000e+00 1.000000e-02 1.000000e-02 1.161000e+00 3.463095e+00 3.463095e+00 +5.410000e+00 1.000000e-02 1.000000e-02 7.680000e-01 2.590640e+00 2.590640e+00 +5.430000e+00 1.000000e-02 1.000000e-02 3.795000e+00 3.272401e+00 3.272401e+00 +5.450000e+00 1.000000e-02 1.000000e-02 -1.123000e+00 2.687320e+00 2.687320e+00 +5.470000e+00 1.000000e-02 1.000000e-02 1.127000e+00 3.362063e+00 3.362063e+00 +5.490000e+00 1.000000e-02 1.000000e-02 -7.360000e-01 2.621581e+00 2.621581e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2007_I756643.cc b/analyses/pluginBELLE/BELLE_2007_I756643.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I756643.cc @@ -0,0 +1,118 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2007_I756643 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2007_I756643); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nPsi2s = bookCounter("TMP/psi2s"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the psi(2S) + if(p.pdgId()==100443) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // omega pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nPsi2s->fill(event.weight()); + break; + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nPsi2s->val(); + double error = _nPsi2s->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nPsi2s; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2007_I756643); + + +} diff --git a/analyses/pluginBELLE/BELLE_2007_I756643.info b/analyses/pluginBELLE/BELLE_2007_I756643.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I756643.info @@ -0,0 +1,34 @@ +Name: BELLE_2007_I756643 +Year: 2007 +Summary: Cross section for $e^+e^-\to \psi(2S)\pi^+\pi^-$ at energies between 4.025 and 5.475 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 756643 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 99 (2007) 142002, 2007 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to \psi(2S)\pi^+\pi^-$ at energies between 4.025 and 5.475 GeV using radiative return by BELLE.' +BibKey: Wang:2007ea +BibTeX: '@article{Wang:2007ea, + author = "Wang, X. L. and others", + title = "{Observation of Two Resonant Structures in e+e- to pi+ + pi- psi(2S) via Initial State Radiation at Belle}", + collaboration = "Belle", + journal = "Phys. Rev. Lett.", + volume = "99", + year = "2007", + pages = "142002", + doi = "10.1103/PhysRevLett.99.142002", + eprint = "0707.3699", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-2007-33, KEK-2007-27", + SLACcitation = "%%CITATION = ARXIV:0707.3699;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2007_I756643.plot b/analyses/pluginBELLE/BELLE_2007_I756643.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I756643.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BELLE_2007_I756643/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\psi(2S))$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\psi(2S))$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2007_I756643.yoda b/analyses/pluginBELLE/BELLE_2007_I756643.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2007_I756643.yoda @@ -0,0 +1,41 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2007_I756643/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: 0.0, up: 99.412}, 'sys,Additional systematic error.': {dn: -0.0, up: 0.0}}, 1: {error: {dn: 0.0, up: 26.531}, 'sys,Additional systematic error.': {dn: -0.0, up: 0.0}}, 2: {error: {dn: -18.06, up: 30.29}, 'sys,Additional systematic error.': {dn: -2.391245, up: 2.391245}}, 3: {error: {dn: 0.0, up: 11.265}, 'sys,Additional systematic error.': {dn: -0.0, up: 0.0}}, 4: {error: {dn: -10.279, up: 17.239}, 'sys,Additional systematic error.': {dn: -1.3608749999999998, up: 1.3608749999999998}}, 5: {error: {dn: -11.28, up: 18.44}, 'sys,Additional systematic error.': {dn: -2.419175, up: 2.419175}}, 6: {error: {dn: -19.1, up: 21.787}, 'sys,Additional systematic error.': {dn: -5.42146, up: 5.42146}}, 7: {error: {dn: -19.012, up: 22.431}, 'sys,Additional systematic error.': {dn: -7.760834999999999, up: 7.760834999999999}}, 8: {error: {dn: -15.305, up: 19.33}, 'sys,Additional systematic error.': {dn: -5.233265000000001, up: 5.233265000000001}}, 9: {error: {dn: -7.163, up: 11.709}, 'sys,Additional systematic error.': {dn: -1.5361500000000001, up: 1.5361500000000001}}, 10: {error: {dn: -5.05, up: 8.469}, 'sys,Additional systematic error.': {dn: -0.6686099999999999, up: 0.6686099999999999}}, 11: {error: {dn: -2.491, up: 6.433}, 'sys,Additional systematic error.': {dn: -0.271985, up: 0.271985}}, 12: {error: {dn: -7.952, up: 9.563}, 'sys,Additional systematic error.': {dn: -1.58745, up: 1.58745}}, 13: {error: {dn: -12.184, up: 14.375}, 'sys,Additional systematic error.': {dn: -4.973535, up: 4.973535}}, 14: {error: {dn: -8.442, up: 11.794}, 'sys,Additional systematic error.': {dn: -2.63435, up: 2.63435}}, 15: {error: {dn: -5.652, up: 6.438}, 'sys,Additional systematic error.': {dn: -0.795435, up: 0.795435}}, 16: {error: {dn: -5.42, up: 6.173}, 'sys,Additional systematic error.': {dn: -0.76266, up: 0.76266}}, 17: {error: {dn: -1.867, up: 4.82}, 'sys,Additional systematic error.': {dn: -0.203775, up: 0.203775}}, 18: {error: {dn: -3.406, up: 5.713}, 'sys,Additional systematic error.': {dn: -0.450965, up: 0.450965}}, 19: {error: {dn: -4.835, up: 7.059}, 'sys,Additional systematic error.': {dn: -0.92606, up: 0.92606}}, 20: {error: {dn: -1.671, up: 4.315}, 'sys,Additional systematic error.': {dn: -0.18249500000000002, up: 0.18249500000000002}}, 21: {error: {dn: -1.612, up: 4.163}, 'sys,Additional systematic error.': {dn: -0.17603500000000002, up: 0.17603500000000002}}, 22: {error: {dn: 0.0, up: 2.553}, 'sys,Additional systematic error.': {dn: -0.0, up: 0.0}}, 23: {error: {dn: -4.182, up: 4.764}, 'sys,Additional systematic error.': {dn: -0.5885250000000001, up: 0.5885250000000001}}, 24: {error: {dn: -1.442, up: 3.724}, 'sys,Additional systematic error.': {dn: -0.15750999999999998, up: 0.15750999999999998}}, 25: {error: {dn: -2.628, up: 4.407}, 'sys,Additional systematic error.': {dn: -0.34789, up: 0.34789}}, 26: {error: {dn: -1.33, up: 3.435}, 'sys,Additional systematic error.': {dn: -0.145255, up: 0.145255}}, 27: {error: {dn: -2.414, up: 4.049}, 'sys,Additional systematic error.': {dn: -0.319675, up: 0.319675}}, 28: {error: {dn: -1.217, up: 3.141}, 'sys,Additional systematic error.': {dn: -0.13280999999999998, up: 0.13280999999999998}}, 29: {error: {dn: -2.198, up: 3.686}, 'sys,Additional systematic error.': {dn: -0.290985, up: 0.290985}}} + +IsRef: 1 +Path: /REF/BELLE_2007_I756643/d01-x01-y01 +Title: doi:10.17182/hepdata.51373.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.025000e+00 2.500000e-02 2.500000e-02 0.000000e+00 0.000000e+00 9.941200e+01 +4.075000e+00 2.500000e-02 2.500000e-02 0.000000e+00 0.000000e+00 2.653100e+01 +4.125000e+00 2.500000e-02 2.500000e-02 2.517100e+01 1.821762e+01 3.038424e+01 +4.175000e+00 2.500000e-02 2.500000e-02 0.000000e+00 0.000000e+00 1.126500e+01 +4.225000e+00 2.500000e-02 2.500000e-02 1.432500e+01 1.036869e+01 1.729263e+01 +4.275000e+00 2.500000e-02 2.500000e-02 2.546500e+01 1.153650e+01 1.859801e+01 +4.325000e+00 2.500000e-02 2.500000e-02 5.706800e+01 1.985453e+01 2.245141e+01 +4.375000e+00 2.500000e-02 2.500000e-02 8.169300e+01 2.053501e+01 2.373563e+01 +4.425000e+00 2.500000e-02 2.500000e-02 5.508700e+01 1.617498e+01 2.002588e+01 +4.475000e+00 2.500000e-02 2.500000e-02 1.617000e+01 7.325867e+00 1.180934e+01 +4.525000e+00 2.500000e-02 2.500000e-02 7.038000e+00 5.094069e+00 8.495352e+00 +4.575000e+00 2.500000e-02 2.500000e-02 2.863000e+00 2.505805e+00 6.438747e+00 +4.625000e+00 2.500000e-02 2.500000e-02 1.671000e+01 8.108903e+00 9.693862e+00 +4.675000e+00 2.500000e-02 2.500000e-02 5.235300e+01 1.316001e+01 1.521107e+01 +4.725000e+00 2.500000e-02 2.500000e-02 2.773000e+01 8.843481e+00 1.208463e+01 +4.775000e+00 2.500000e-02 2.500000e-02 8.373000e+00 5.707698e+00 6.486953e+00 +4.825000e+00 2.500000e-02 2.500000e-02 8.028000e+00 5.473395e+00 6.219934e+00 +4.875000e+00 2.500000e-02 2.500000e-02 2.145000e+00 1.878088e+00 4.824306e+00 +4.925000e+00 2.500000e-02 2.500000e-02 4.747000e+00 3.435725e+00 5.730771e+00 +4.975000e+00 2.500000e-02 2.500000e-02 9.748000e+00 4.922887e+00 7.119485e+00 +5.025000e+00 2.500000e-02 2.500000e-02 1.921000e+00 1.680936e+00 4.318857e+00 +5.075000e+00 2.500000e-02 2.500000e-02 1.853000e+00 1.621583e+00 4.166720e+00 +5.125000e+00 2.500000e-02 2.500000e-02 0.000000e+00 0.000000e+00 2.553000e+00 +5.175000e+00 2.500000e-02 2.500000e-02 6.195000e+00 4.223208e+00 4.800214e+00 +5.225000e+00 2.500000e-02 2.500000e-02 1.658000e+00 1.450577e+00 3.727330e+00 +5.275000e+00 2.500000e-02 2.500000e-02 3.662000e+00 2.650927e+00 4.420710e+00 +5.325000e+00 2.500000e-02 2.500000e-02 1.529000e+00 1.337908e+00 3.438070e+00 +5.375000e+00 2.500000e-02 2.500000e-02 3.365000e+00 2.435075e+00 4.061600e+00 +5.425000e+00 2.500000e-02 2.500000e-02 1.398000e+00 1.224225e+00 3.143807e+00 +5.475000e+00 2.500000e-02 2.500000e-02 3.063000e+00 2.217178e+00 3.697468e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2008_I757220.cc b/analyses/pluginBELLE/BELLE_2008_I757220.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I757220.cc @@ -0,0 +1,136 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2008_I757220 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2008_I757220); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nD0 = bookCounter("/TMP/nD0"); + _nDp = bookCounter("/TMP/nDp"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + bool matched=false; + for(unsigned int iy=0;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) break; + } + if(matched) { + if(abs(p1.pdgId())==411) + _nDp->fill(event.weight()); + else if(abs(p1.pdgId())==421) + _nD0->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma,error; + if(ix==1) { + sigma = _nD0->val(); + error = _nD0->err(); + } + else { + sigma = _nDp->val(); + error = _nDp->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nD0,_nDp; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2008_I757220); + + +} diff --git a/analyses/pluginBELLE/BELLE_2008_I757220.info b/analyses/pluginBELLE/BELLE_2008_I757220.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I757220.info @@ -0,0 +1,37 @@ +Name: BELLE_2008_I757220 +Year: 2008 +Summary: Cross section for $e^+e^-\to D^+D^-$ and $D^0\bar{D}^0$ below 5 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 757220 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys. Rev. D77, 011103 (2008) +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to D^+D^-$ and $D^0\bar{D}^0$ below 5 GeV' +Keywords: [] +BibKey: Pakhlova:2008zza +BibTeX: '@article{Pakhlova:2008zza, + author = "Pakhlova, G. and others", + title = "{Measurement of the near-threshold e+ e- ---> D anti-D + cross section using initial-state radiation}", + booktitle = "{Lepton and photon interactions at high energies. + Proceedings, 23rd International Symposium, LP2007, Daegu, + South Korea, August 13-18, 2007}", + collaboration = "Belle", + journal = "Phys. Rev.", + volume = "D77", + year = "2008", + pages = "011103", + doi = "10.1103/PhysRevD.77.011103", + eprint = "0708.0082", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-CONF-0704", + SLACcitation = "%%CITATION = ARXIV:0708.0082;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2008_I757220.plot b/analyses/pluginBELLE/BELLE_2008_I757220.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I757220.plot @@ -0,0 +1,13 @@ +BEGIN PLOT /BELLE_2008_I757220/d01-x01-y01 +Title=$\sigma(e^+e^-\to D^0\bar{D}^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^0\bar{D}^0)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2008_I757220/d02-x01-y01 +Title=$\sigma(e^+e^-\to D^+D^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^+D^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2008_I757220.yoda b/analyses/pluginBELLE/BELLE_2008_I757220.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I757220.yoda @@ -0,0 +1,152 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2008_I757220/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.096, up: 0.096}, sys: {dn: -0.016, up: 0.016}}, 1: {stat: {dn: -0.131, up: 0.131}, sys: {dn: -0.01, up: 0.01}}, 2: {stat: {dn: -0.31, up: 0.31}, sys: {dn: -0.157, up: 0.157}}, 3: {stat: {dn: -0.547, up: 0.547}, sys: {dn: -0.542, up: 0.542}}, 4: {stat: {dn: -0.303, up: 0.303}, sys: {dn: -0.162, up: 0.162}}, 5: {stat: {dn: -0.098, up: 0.098}, sys: {dn: -0.006, up: 0.006}}, 6: {stat: {dn: -0.134, up: 0.134}, sys: {dn: -0.025, up: 0.025}}, 7: {stat: {dn: -0.136, up: 0.136}, sys: {dn: -0.028, up: 0.028}}, 8: {stat: {dn: -0.157, up: 0.157}, sys: {dn: -0.032, up: 0.032}}, 9: {stat: {dn: -0.159, up: 0.159}, sys: {dn: -0.038, up: 0.038}}, 10: {stat: {dn: -0.159, up: 0.159}, sys: {dn: -0.046, up: 0.046}}, 11: {stat: {dn: -0.139, up: 0.139}, sys: {dn: -0.036, up: 0.036}}, 12: {stat: {dn: -0.127, up: 0.127}, sys: {dn: -0.023, up: 0.023}}, 13: {stat: {dn: -0.101, up: 0.101}, sys: {dn: -0.014, up: 0.014}}, 14: {stat: {dn: -0.093, up: 0.093}, sys: {dn: -0.009, up: 0.009}}, 15: {stat: {dn: -0.104, up: 0.104}, sys: {dn: -0.013, up: 0.013}}, 16: {stat: {dn: -0.109, up: 0.109}, sys: {dn: -0.026, up: 0.026}}, 17: {stat: {dn: -0.104, up: 0.104}, sys: {dn: -0.031, up: 0.031}}, 18: {stat: {dn: -0.122, up: 0.122}, sys: {dn: -0.049, up: 0.049}}, 19: {stat: {dn: -0.118, up: 0.118}, sys: {dn: -0.045, up: 0.045}}, 20: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.031, up: 0.031}}, 21: {stat: {dn: -0.125, up: 0.125}, sys: {dn: -0.056, up: 0.056}}, 22: {stat: {dn: -0.083, up: 0.083}, sys: {dn: -0.024, up: 0.024}}, 23: {stat: {dn: -0.061, up: 0.061}, sys: {dn: -0.007, up: 0.007}}, 24: {stat: {dn: -0.069, up: 0.069}, sys: {dn: -0.014, up: 0.014}}, 25: {stat: {dn: -0.067, up: 0.067}, sys: {dn: -0.015, up: 0.015}}, 26: {stat: {dn: -0.068, up: 0.068}, sys: {dn: -0.014, up: 0.014}}, 27: {stat: {dn: -0.048, up: 0.048}, sys: {dn: -0.006, up: 0.006}}, 28: {stat: {dn: -0.051, up: 0.051}, sys: {dn: -0.008, up: 0.008}}, 29: {stat: {dn: -0.049, up: 0.049}, sys: {dn: -0.006, up: 0.006}}, 30: {stat: {dn: -0.04, up: 0.04}, sys: {dn: -0.005, up: 0.005}}, 31: {stat: {dn: -0.053, up: 0.053}, sys: {dn: -0.009, up: 0.009}}, 32: {stat: {dn: -0.046, up: 0.046}, sys: {dn: -0.006, up: 0.006}}, 33: {stat: {dn: -0.046, up: 0.046}, sys: {dn: -0.01, up: 0.01}}, 34: {stat: {dn: -0.043, up: 0.043}, sys: {dn: -0.006, up: 0.006}}, 35: {stat: {dn: -0.061, up: 0.061}, sys: {dn: -0.016, up: 0.016}}, 36: {stat: {dn: -0.058, up: 0.058}, sys: {dn: -0.021, up: 0.021}}, 37: {stat: {dn: -0.049, up: 0.049}, sys: {dn: -0.011, up: 0.011}}, 38: {stat: {dn: -0.041, up: 0.041}, sys: {dn: -0.006, up: 0.006}}, 39: {stat: {dn: -0.045, up: 0.045}, sys: {dn: -0.015, up: 0.015}}, 40: {stat: {dn: -0.044, up: 0.044}, sys: {dn: -0.007, up: 0.007}}, 41: {stat: {dn: -0.052, up: 0.052}, sys: {dn: -0.014, up: 0.014}}, 42: {stat: {dn: -0.05, up: 0.05}, sys: {dn: -0.016, up: 0.016}}, 43: {stat: {dn: -0.036, up: 0.036}, sys: {dn: -0.005, up: 0.005}}, 44: {stat: {dn: -0.024, up: 0.024}, sys: {dn: -0.005, up: 0.005}}, 45: {stat: {dn: -0.034, up: 0.034}, sys: {dn: -0.006, up: 0.006}}, 46: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.005, up: 0.005}}, 47: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.006, up: 0.006}}, 48: {stat: {dn: -0.032, up: 0.032}, sys: {dn: -0.006, up: 0.006}}, 49: {stat: {dn: -0.028, up: 0.028}, sys: {dn: -0.005, up: 0.005}}, 50: {stat: {dn: -0.03, up: 0.03}, sys: {dn: -0.006, up: 0.006}}, 51: {stat: {dn: -0.035, up: 0.035}, sys: {dn: -0.008, up: 0.008}}, 52: {stat: {dn: -0.026, up: 0.026}, sys: {dn: -0.006, up: 0.006}}, 53: {stat: {dn: -0.028, up: 0.028}, sys: {dn: -0.006, up: 0.006}}, 54: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.006, up: 0.006}}, 55: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.006, up: 0.006}}, 56: {stat: {dn: -0.02, up: 0.02}, sys: {dn: -0.005, up: 0.005}}, 57: {stat: {dn: -0.026, up: 0.026}, sys: {dn: -0.005, up: 0.005}}, 58: {stat: {dn: -0.028, up: 0.028}, sys: {dn: -0.007, up: 0.007}}, 59: {stat: {dn: -0.015, up: 0.015}, sys: {dn: -0.006, up: 0.006}}, 60: {stat: {dn: -0.026, up: 0.026}, sys: {dn: -0.008, up: 0.008}}, 61: {stat: {dn: -0.016, up: 0.016}, sys: {dn: -0.005, up: 0.005}}, 62: {stat: {dn: -0.026, up: 0.026}, sys: {dn: -0.007, up: 0.007}}, 63: {stat: {dn: -0.011, up: 0.011}, sys: {dn: -0.005, up: 0.005}}, 64: {stat: {dn: -0.028, up: 0.028}, sys: {dn: -0.009, up: 0.009}}} + +IsRef: 1 +Path: /REF/BELLE_2008_I757220/d01-x01-y01 +Title: doi:10.17182/hepdata.22082.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.710000e+00 1.000000e-02 1.000000e-02 -1.580000e-01 9.732420e-02 9.732420e-02 +3.730000e+00 1.000000e-02 1.000000e-02 1.000000e-01 1.313811e-01 1.313811e-01 +3.750000e+00 1.000000e-02 1.000000e-02 1.568000e+00 3.474896e-01 3.474896e-01 +3.770000e+00 1.000000e-02 1.000000e-02 5.424000e+00 7.700474e-01 7.700474e-01 +3.790000e+00 1.000000e-02 1.000000e-02 1.619000e+00 3.435884e-01 3.435884e-01 +3.810000e+00 1.000000e-02 1.000000e-02 2.200000e-02 9.818350e-02 9.818350e-02 +3.830000e+00 1.000000e-02 1.000000e-02 2.510000e-01 1.363121e-01 1.363121e-01 +3.850000e+00 1.000000e-02 1.000000e-02 2.770000e-01 1.388524e-01 1.388524e-01 +3.870000e+00 1.000000e-02 1.000000e-02 3.220000e-01 1.602280e-01 1.602280e-01 +3.890000e+00 1.000000e-02 1.000000e-02 3.810000e-01 1.634778e-01 1.634778e-01 +3.910000e+00 1.000000e-02 1.000000e-02 4.620000e-01 1.655204e-01 1.655204e-01 +3.930000e+00 1.000000e-02 1.000000e-02 3.610000e-01 1.435862e-01 1.435862e-01 +3.950000e+00 1.000000e-02 1.000000e-02 2.340000e-01 1.290659e-01 1.290659e-01 +3.970000e+00 1.000000e-02 1.000000e-02 1.440000e-01 1.019657e-01 1.019657e-01 +3.990000e+00 1.000000e-02 1.000000e-02 9.300000e-02 9.343447e-02 9.343447e-02 +4.010000e+00 1.000000e-02 1.000000e-02 1.270000e-01 1.048094e-01 1.048094e-01 +4.030000e+00 1.000000e-02 1.000000e-02 2.620000e-01 1.120580e-01 1.120580e-01 +4.050000e+00 1.000000e-02 1.000000e-02 3.120000e-01 1.085219e-01 1.085219e-01 +4.070000e+00 1.000000e-02 1.000000e-02 4.920000e-01 1.314724e-01 1.314724e-01 +4.090000e+00 1.000000e-02 1.000000e-02 4.520000e-01 1.262894e-01 1.262894e-01 +4.110000e+00 1.000000e-02 1.000000e-02 3.060000e-01 1.046948e-01 1.046948e-01 +4.130000e+00 1.000000e-02 1.000000e-02 5.570000e-01 1.369708e-01 1.369708e-01 +4.150000e+00 1.000000e-02 1.000000e-02 2.410000e-01 8.640023e-02 8.640023e-02 +4.170000e+00 1.000000e-02 1.000000e-02 6.900000e-02 6.140033e-02 6.140033e-02 +4.190000e+00 1.000000e-02 1.000000e-02 1.400000e-01 7.040597e-02 7.040597e-02 +4.210000e+00 1.000000e-02 1.000000e-02 1.460000e-01 6.865858e-02 6.865858e-02 +4.230000e+00 1.000000e-02 1.000000e-02 1.380000e-01 6.942622e-02 6.942622e-02 +4.250000e+00 1.000000e-02 1.000000e-02 5.800000e-02 4.837355e-02 4.837355e-02 +4.270000e+00 1.000000e-02 1.000000e-02 8.100000e-02 5.162364e-02 5.162364e-02 +4.290000e+00 1.000000e-02 1.000000e-02 6.000000e-02 4.936598e-02 4.936598e-02 +4.310000e+00 1.000000e-02 1.000000e-02 3.100000e-02 4.031129e-02 4.031129e-02 +4.330000e+00 1.000000e-02 1.000000e-02 9.200000e-02 5.375872e-02 5.375872e-02 +4.350000e+00 1.000000e-02 1.000000e-02 4.900000e-02 4.638965e-02 4.638965e-02 +4.370000e+00 1.000000e-02 1.000000e-02 9.800000e-02 4.707441e-02 4.707441e-02 +4.390000e+00 1.000000e-02 1.000000e-02 5.600000e-02 4.341659e-02 4.341659e-02 +4.410000e+00 1.000000e-02 1.000000e-02 1.580000e-01 6.306346e-02 6.306346e-02 +4.430000e+00 1.000000e-02 1.000000e-02 2.100000e-01 6.168468e-02 6.168468e-02 +4.450000e+00 1.000000e-02 1.000000e-02 1.130000e-01 5.021952e-02 5.021952e-02 +4.470000e+00 1.000000e-02 1.000000e-02 5.300000e-02 4.143670e-02 4.143670e-02 +4.490000e+00 1.000000e-02 1.000000e-02 1.450000e-01 4.743416e-02 4.743416e-02 +4.510000e+00 1.000000e-02 1.000000e-02 6.900000e-02 4.455334e-02 4.455334e-02 +4.530000e+00 1.000000e-02 1.000000e-02 1.440000e-01 5.385165e-02 5.385165e-02 +4.550000e+00 1.000000e-02 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up: 0.169}, sys: {dn: -0.005, up: 0.005}}, 2: {stat: {dn: -0.286, up: 0.286}, sys: {dn: -0.06, up: 0.06}}, 3: {stat: {dn: -0.721, up: 0.721}, sys: {dn: -0.392, up: 0.392}}, 4: {stat: {dn: -0.458, up: 0.458}, sys: {dn: -0.168, up: 0.168}}, 5: {stat: {dn: -0.175, up: 0.175}, sys: {dn: -0.019, up: 0.019}}, 6: {stat: {dn: -0.205, up: 0.205}, sys: {dn: -0.029, up: 0.029}}, 7: {stat: {dn: -0.122, up: 0.122}, sys: {dn: -0.006, up: 0.006}}, 8: {stat: {dn: -0.236, up: 0.236}, sys: {dn: -0.049, up: 0.049}}, 9: {stat: {dn: -0.282, up: 0.282}, sys: {dn: -0.078, up: 0.078}}, 10: {stat: {dn: -0.258, up: 0.258}, sys: {dn: -0.057, up: 0.057}}, 11: {stat: {dn: -0.163, up: 0.163}, sys: {dn: -0.021, up: 0.021}}, 12: {stat: {dn: -0.177, up: 0.177}, sys: {dn: -0.035, up: 0.035}}, 13: {stat: {dn: -0.15, up: 0.15}, sys: {dn: -0.022, up: 0.022}}, 14: {stat: {dn: -0.12, up: 0.12}, sys: {dn: -0.013, up: 0.013}}, 15: {stat: {dn: -0.112, up: 0.112}, sys: {dn: -0.014, up: 0.014}}, 16: {stat: {dn: -0.154, up: 0.154}, sys: {dn: -0.026, up: 0.026}}, 17: {stat: {dn: -0.082, up: 0.082}, sys: {dn: -0.005, up: 0.005}}, 18: {stat: {dn: -0.172, up: 0.172}, sys: {dn: -0.041, up: 0.041}}, 19: {stat: {dn: -0.136, up: 0.136}, sys: {dn: -0.027, up: 0.027}}, 20: {stat: {dn: -0.134, up: 0.134}, sys: {dn: -0.024, up: 0.024}}, 21: {stat: {dn: -0.168, up: 0.168}, sys: {dn: -0.042, up: 0.042}}, 22: {stat: {dn: -0.126, up: 0.126}, sys: {dn: -0.019, up: 0.019}}, 23: {stat: {dn: -0.119, up: 0.119}, sys: {dn: -0.023, up: 0.023}}, 24: {stat: {dn: -0.101, up: 0.101}, sys: {dn: -0.019, up: 0.019}}, 25: {stat: {dn: -0.177, up: 0.177}, sys: {dn: -0.053, up: 0.053}}, 26: {stat: {dn: -0.097, up: 0.097}, sys: {dn: -0.011, up: 0.011}}, 27: {stat: {dn: -0.118, up: 0.118}, sys: {dn: -0.024, up: 0.024}}, 28: {stat: {dn: -0.089, up: 0.089}, sys: {dn: -0.015, up: 0.015}}, 29: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.018, up: 0.018}}, 30: {stat: {dn: -0.086, up: 0.086}, sys: {dn: -0.01, up: 0.01}}, 31: {stat: {dn: -0.049, up: 0.049}, sys: {dn: -0.006, up: 0.006}}, 32: {stat: {dn: -0.08, up: 0.08}, sys: {dn: -0.012, up: 0.012}}, 33: {stat: {dn: -0.077, up: 0.077}, sys: {dn: -0.013, up: 0.013}}, 34: {stat: {dn: -0.087, up: 0.087}, sys: {dn: -0.018, up: 0.018}}, 35: {stat: {dn: -0.103, up: 0.103}, sys: {dn: -0.025, up: 0.025}}, 36: {stat: {dn: -0.082, up: 0.082}, sys: {dn: -0.017, up: 0.017}}, 37: {stat: {dn: -0.098, up: 0.098}, sys: {dn: -0.024, up: 0.024}}, 38: {stat: {dn: -0.079, up: 0.079}, sys: {dn: -0.014, up: 0.014}}, 39: {stat: {dn: -0.085, up: 0.085}, sys: {dn: -0.017, up: 0.017}}, 40: {stat: {dn: -0.053, up: 0.053}, sys: {dn: -0.007, up: 0.007}}, 41: {stat: {dn: -0.052, up: 0.052}, sys: {dn: -0.008, up: 0.008}}, 42: {stat: {dn: -0.038, up: 0.038}, sys: {dn: -0.005, up: 0.005}}, 43: {stat: {dn: -0.051, up: 0.051}, sys: {dn: -0.006, up: 0.006}}, 44: {stat: {dn: -0.083, up: 0.083}, sys: {dn: -0.017, up: 0.017}}, 45: {stat: {dn: -0.047, up: 0.047}, sys: {dn: -0.007, up: 0.007}}, 46: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.006, up: 0.006}}, 47: {stat: {dn: -0.035, up: 0.035}, sys: {dn: -0.005, up: 0.005}}, 48: {stat: {dn: -0.044, up: 0.044}, sys: {dn: -0.005, up: 0.005}}, 49: {stat: {dn: -0.053, up: 0.053}, sys: {dn: -0.008, up: 0.008}}, 50: {stat: {dn: -0.031, up: 0.031}, sys: {dn: -0.006, up: 0.006}}, 51: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.006, up: 0.006}}, 52: {stat: {dn: -0.04, up: 0.04}, sys: {dn: -0.006, up: 0.006}}, 53: {stat: {dn: -0.039, up: 0.039}, sys: {dn: -0.006, up: 0.006}}, 54: {stat: {dn: -0.027, up: 0.027}, sys: {dn: -0.006, up: 0.006}}, 55: {stat: {dn: -0.046, up: 0.046}, sys: {dn: -0.008, up: 0.008}}, 56: {stat: {dn: -0.037, up: 0.037}, sys: {dn: -0.006, up: 0.006}}, 57: {stat: {dn: -0.051, up: 0.051}, sys: {dn: -0.009, up: 0.009}}, 58: {stat: {dn: -0.055, up: 0.055}, sys: {dn: -0.012, up: 0.012}}, 59: {stat: {dn: -0.025, up: 0.025}, sys: {dn: -0.006, up: 0.006}}, 60: {stat: {dn: -0.026, up: 0.026}, sys: {dn: -0.005, up: 0.005}}, 61: {stat: {dn: -0.026, up: 0.026}, sys: {dn: -0.005, up: 0.005}}, 62: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.006, up: 0.006}}, 63: {stat: {dn: -0.032, up: 0.032}, sys: {dn: -0.006, up: 0.006}}, 64: {stat: {dn: -0.022, up: 0.022}, sys: {dn: -0.006, up: 0.006}}} + +IsRef: 1 +Path: /REF/BELLE_2008_I757220/d02-x01-y01 +Title: doi:10.17182/hepdata.22082.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.710000e+00 1.000000e-02 1.000000e-02 -2.900000e-02 1.801000e-01 1.801000e-01 +3.730000e+00 1.000000e-02 1.000000e-02 -1.800000e-02 1.690739e-01 1.690739e-01 +3.750000e+00 1.000000e-02 1.000000e-02 6.010000e-01 2.922259e-01 2.922259e-01 +3.770000e+00 1.000000e-02 1.000000e-02 3.919000e+00 8.206735e-01 8.206735e-01 +3.790000e+00 1.000000e-02 1.000000e-02 1.679000e+00 4.878401e-01 4.878401e-01 +3.810000e+00 1.000000e-02 1.000000e-02 1.880000e-01 1.760284e-01 1.760284e-01 +3.830000e+00 1.000000e-02 1.000000e-02 2.930000e-01 2.070411e-01 2.070411e-01 +3.850000e+00 1.000000e-02 1.000000e-02 3.400000e-02 1.221475e-01 1.221475e-01 +3.870000e+00 1.000000e-02 1.000000e-02 4.940000e-01 2.410332e-01 2.410332e-01 +3.890000e+00 1.000000e-02 1.000000e-02 7.840000e-01 2.925884e-01 2.925884e-01 +3.910000e+00 1.000000e-02 1.000000e-02 5.720000e-01 2.642215e-01 2.642215e-01 +3.930000e+00 1.000000e-02 1.000000e-02 2.110000e-01 1.643472e-01 1.643472e-01 +3.950000e+00 1.000000e-02 1.000000e-02 3.500000e-01 1.804273e-01 1.804273e-01 +3.970000e+00 1.000000e-02 1.000000e-02 2.150000e-01 1.516047e-01 1.516047e-01 +3.990000e+00 1.000000e-02 1.000000e-02 1.310000e-01 1.207021e-01 1.207021e-01 +4.010000e+00 1.000000e-02 1.000000e-02 1.410000e-01 1.128716e-01 1.128716e-01 +4.030000e+00 1.000000e-02 1.000000e-02 2.580000e-01 1.561794e-01 1.561794e-01 +4.050000e+00 1.000000e-02 1.000000e-02 4.000000e-03 8.215230e-02 8.215230e-02 +4.070000e+00 1.000000e-02 1.000000e-02 4.100000e-01 1.768191e-01 1.768191e-01 +4.090000e+00 1.000000e-02 1.000000e-02 2.700000e-01 1.386542e-01 1.386542e-01 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8.089499e-02 8.089499e-02 +4.370000e+00 1.000000e-02 1.000000e-02 1.290000e-01 7.808969e-02 7.808969e-02 +4.390000e+00 1.000000e-02 1.000000e-02 1.800000e-01 8.884256e-02 8.884256e-02 +4.410000e+00 1.000000e-02 1.000000e-02 2.490000e-01 1.059906e-01 1.059906e-01 +4.430000e+00 1.000000e-02 1.000000e-02 1.710000e-01 8.374366e-02 8.374366e-02 +4.450000e+00 1.000000e-02 1.000000e-02 2.390000e-01 1.008960e-01 1.008960e-01 +4.470000e+00 1.000000e-02 1.000000e-02 1.430000e-01 8.023092e-02 8.023092e-02 +4.490000e+00 1.000000e-02 1.000000e-02 1.700000e-01 8.668333e-02 8.668333e-02 +4.510000e+00 1.000000e-02 1.000000e-02 7.300000e-02 5.346027e-02 5.346027e-02 +4.530000e+00 1.000000e-02 1.000000e-02 7.800000e-02 5.261179e-02 5.261179e-02 +4.550000e+00 1.000000e-02 1.000000e-02 8.000000e-03 3.832754e-02 3.832754e-02 +4.570000e+00 1.000000e-02 1.000000e-02 3.600000e-02 5.135173e-02 5.135173e-02 +4.590000e+00 1.000000e-02 1.000000e-02 1.720000e-01 8.472308e-02 8.472308e-02 +4.610000e+00 1.000000e-02 1.000000e-02 6.900000e-02 4.751842e-02 4.751842e-02 +4.630000e+00 1.000000e-02 1.000000e-02 2.800000e-02 3.354102e-02 3.354102e-02 +4.650000e+00 1.000000e-02 1.000000e-02 -7.000000e-03 3.535534e-02 3.535534e-02 +4.670000e+00 1.000000e-02 1.000000e-02 5.100000e-02 4.428318e-02 4.428318e-02 +4.690000e+00 1.000000e-02 1.000000e-02 7.800000e-02 5.360037e-02 5.360037e-02 +4.710000e+00 1.000000e-02 1.000000e-02 1.600000e-02 3.157531e-02 3.157531e-02 +4.730000e+00 1.000000e-02 1.000000e-02 3.000000e-02 2.961419e-02 2.961419e-02 +4.750000e+00 1.000000e-02 1.000000e-02 5.600000e-02 4.044750e-02 4.044750e-02 +4.770000e+00 1.000000e-02 1.000000e-02 4.800000e-02 3.945884e-02 3.945884e-02 +4.790000e+00 1.000000e-02 1.000000e-02 2.000000e-02 2.765863e-02 2.765863e-02 +4.810000e+00 1.000000e-02 1.000000e-02 8.000000e-02 4.669047e-02 4.669047e-02 +4.830000e+00 1.000000e-02 1.000000e-02 5.100000e-02 3.748333e-02 3.748333e-02 +4.850000e+00 1.000000e-02 1.000000e-02 9.100000e-02 5.178803e-02 5.178803e-02 +4.870000e+00 1.000000e-02 1.000000e-02 1.180000e-01 5.629387e-02 5.629387e-02 +4.890000e+00 1.000000e-02 1.000000e-02 2.700000e-02 2.570992e-02 2.570992e-02 +4.910000e+00 1.000000e-02 1.000000e-02 1.000000e-03 2.647640e-02 2.647640e-02 +4.930000e+00 1.000000e-02 1.000000e-02 1.000000e-03 2.647640e-02 2.647640e-02 +4.950000e+00 1.000000e-02 1.000000e-02 3.500000e-02 3.354102e-02 3.354102e-02 +4.970000e+00 1.000000e-02 1.000000e-02 4.600000e-02 3.255764e-02 3.255764e-02 +4.990000e+00 1.000000e-02 1.000000e-02 2.400000e-02 2.280351e-02 2.280351e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2008_I759073.cc b/analyses/pluginBELLE/BELLE_2008_I759073.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I759073.cc @@ -0,0 +1,128 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2008_I759073 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2008_I759073); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nD0 = bookCounter("/TMP/nD0"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + + + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + bool matched=false; + int id2 = p1.pdgId()>0 ? -411 : 411; + int ipi = p1.pdgId()>0 ? 211 : -211; + for(unsigned int iy=0;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=1) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.first==ipi) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) break; + } + if(matched) + _nD0->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nD0->val(); + double error = _nD0->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + /// @name Histograms + //@{ + CounterPtr _nD0; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2008_I759073); + + +} diff --git a/analyses/pluginBELLE/BELLE_2008_I759073.info b/analyses/pluginBELLE/BELLE_2008_I759073.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I759073.info @@ -0,0 +1,32 @@ +Name: BELLE_2008_I759073 +Year: 2008 +Summary: Cross section for $e^+e^-\to D^0D^-\pi^++\text{c.c.}$ below 5 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 759073 +Status: VALIDATED +Authors: + - Peter Richardson +References: +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to D^0D^-\pi^++\text{c.c.}$ below 5 GeV' +Keywords: [] +BibKey: Pakhlova:2007fq +BibTeX: '@article{Pakhlova:2007fq, + author = "Pakhlova, G. and others", + title = "{Observation of psi (4415) ---> D anti-D*(2)(2460) decay + using initial-state radiation}", + collaboration = "Belle", + journal = "Phys. Rev. Lett.", + volume = "100", + year = "2008", + pages = "062001", + doi = "10.1103/PhysRevLett.100.062001", + eprint = "0708.3313", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0708.3313;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2008_I759073.plot b/analyses/pluginBELLE/BELLE_2008_I759073.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I759073.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BELLE_2008_I759073/d01-x01-y01 +Title=$\sigma(e^+e^-\to D^0D^-\pi^++\text{c.c.})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^0D^-\pi^++\text{c.c.})$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2008_I759073.yoda b/analyses/pluginBELLE/BELLE_2008_I759073.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I759073.yoda @@ -0,0 +1,36 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2008_I759073/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.089, up: 0.089}, sys: {dn: -0.005, up: 0.005}}, 1: {stat: {dn: -0.08, up: 0.08}, sys: {dn: -0.005, up: 0.005}}, 2: {stat: {dn: -0.072, up: 0.072}, sys: {dn: -0.006, up: 0.006}}, 3: {stat: {dn: -0.058, up: 0.058}, sys: {dn: -0.01, up: 0.01}}, 4: {stat: {dn: -0.093, up: 0.093}, sys: {dn: -0.008, up: 0.008}}, 5: {stat: {dn: -0.065, up: 0.065}, sys: {dn: -0.006, up: 0.006}}, 6: {stat: {dn: -0.069, up: 0.069}, sys: {dn: -0.006, up: 0.006}}, 7: {stat: {dn: -0.062, up: 0.062}, sys: {dn: -0.006, up: 0.006}}, 8: {stat: {dn: -0.081, up: 0.081}, sys: {dn: -0.01, up: 0.01}}, 9: {stat: {dn: -0.119, up: 0.119}, sys: {dn: -0.048, up: 0.048}}, 10: {stat: {dn: -0.135, up: 0.135}, sys: {dn: -0.062, up: 0.062}}, 11: {stat: {dn: -0.103, up: 0.103}, sys: {dn: -0.036, up: 0.036}}, 12: {stat: {dn: -0.084, up: 0.084}, sys: {dn: -0.014, up: 0.014}}, 13: {stat: {dn: -0.073, up: 0.073}, sys: {dn: -0.01, up: 0.01}}, 14: {stat: {dn: -0.073, up: 0.073}, sys: {dn: -0.012, up: 0.012}}, 15: {stat: {dn: -0.074, up: 0.074}, sys: {dn: -0.018, up: 0.018}}, 16: {stat: {dn: -0.068, up: 0.068}, sys: {dn: -0.011, up: 0.011}}, 17: {stat: {dn: -0.066, up: 0.066}, sys: {dn: -0.01, up: 0.01}}, 18: {stat: {dn: -0.062, up: 0.062}, sys: {dn: -0.01, up: 0.01}}, 19: {stat: {dn: -0.068, up: 0.068}, sys: {dn: -0.018, up: 0.018}}, 20: {stat: {dn: -0.076, up: 0.076}, sys: {dn: -0.031, up: 0.031}}, 21: {stat: {dn: -0.054, up: 0.054}, sys: {dn: -0.011, up: 0.011}}, 22: {stat: {dn: -0.057, up: 0.057}, sys: {dn: -0.016, up: 0.016}}, 23: {stat: {dn: -0.048, up: 0.048}, sys: {dn: -0.01, up: 0.01}}, 24: {stat: {dn: -0.063, up: 0.063}, sys: {dn: -0.027, up: 0.027}}} + +IsRef: 1 +Path: /REF/BELLE_2008_I759073/d01-x01-y01 +Title: doi:10.17182/hepdata.21846.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.020000e+00 2.000000e-02 2.000000e-02 2.900000e-02 8.914034e-02 8.914034e-02 +4.060000e+00 2.000000e-02 2.000000e-02 2.000000e-02 8.015610e-02 8.015610e-02 +4.100000e+00 2.000000e-02 2.000000e-02 6.000000e-02 7.224957e-02 7.224957e-02 +4.140000e+00 2.000000e-02 2.000000e-02 -9.900000e-02 5.885576e-02 5.885576e-02 +4.180000e+00 2.000000e-02 2.000000e-02 7.500000e-02 9.334345e-02 9.334345e-02 +4.220000e+00 2.000000e-02 2.000000e-02 -2.500000e-02 6.527634e-02 6.527634e-02 +4.260000e+00 2.000000e-02 2.000000e-02 -1.700000e-02 6.926038e-02 6.926038e-02 +4.300000e+00 2.000000e-02 2.000000e-02 5.000000e-03 6.228965e-02 6.228965e-02 +4.340000e+00 2.000000e-02 2.000000e-02 9.800000e-02 8.161495e-02 8.161495e-02 +4.380000e+00 2.000000e-02 2.000000e-02 4.820000e-01 1.283160e-01 1.283160e-01 +4.420000e+00 2.000000e-02 2.000000e-02 6.190000e-01 1.485564e-01 1.485564e-01 +4.460000e+00 2.000000e-02 2.000000e-02 3.600000e-01 1.091100e-01 1.091100e-01 +4.500000e+00 2.000000e-02 2.000000e-02 1.350000e-01 8.515868e-02 8.515868e-02 +4.540000e+00 2.000000e-02 2.000000e-02 3.800000e-02 7.368175e-02 7.368175e-02 +4.580000e+00 2.000000e-02 2.000000e-02 1.180000e-01 7.397973e-02 7.397973e-02 +4.620000e+00 2.000000e-02 2.000000e-02 1.810000e-01 7.615773e-02 7.615773e-02 +4.660000e+00 2.000000e-02 2.000000e-02 9.400000e-02 6.888396e-02 6.888396e-02 +4.700000e+00 2.000000e-02 2.000000e-02 6.300000e-02 6.675328e-02 6.675328e-02 +4.740000e+00 2.000000e-02 2.000000e-02 9.500000e-02 6.280127e-02 6.280127e-02 +4.780000e+00 2.000000e-02 2.000000e-02 1.830000e-01 7.034202e-02 7.034202e-02 +4.820000e+00 2.000000e-02 2.000000e-02 3.060000e-01 8.207923e-02 8.207923e-02 +4.860000e+00 2.000000e-02 2.000000e-02 6.200000e-02 5.510898e-02 5.510898e-02 +4.900000e+00 2.000000e-02 2.000000e-02 1.580000e-01 5.920304e-02 5.920304e-02 +4.940000e+00 2.000000e-02 2.000000e-02 6.000000e-02 4.903060e-02 4.903060e-02 +4.980000e+00 2.000000e-02 2.000000e-02 2.660000e-01 6.854196e-02 6.854196e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2008_I764099.cc b/analyses/pluginBELLE/BELLE_2008_I764099.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I764099.cc @@ -0,0 +1,139 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2008_I764099 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2008_I764099); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nUps1pipi = bookCounter("TMP/nUps1pipi"); + _nUps2pipi = bookCounter("TMP/nUps2pipi"); + _nUps3pipi = bookCounter("TMP/nUps3pipi"); + _nUps1KK = bookCounter("TMP/nUps1KK"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId() != 553 && + p.pdgId() != 100553 && + p.pdgId() != 200553 ) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==321 || abs(val.first)==211) { + continue; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(nRes[211]==1 && nRes[-211]==1 ) { + if(p.pdgId()==553) + _nUps1pipi->fill(event.weight()); + if(p.pdgId()==100553) + _nUps2pipi->fill(event.weight()); + if(p.pdgId()==200553) + _nUps3pipi->fill(event.weight()); + } + else if(nRes[321]==1 && nRes[-321]==1) { + if(p.pdgId()==553) + _nUps1KK->fill(event.weight()); + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /picobarn; + for(unsigned int ix=1;ix<5;++ix) { + double sigma,error; + if(ix==1) { + sigma = _nUps1pipi->val()*fact; + error = _nUps1pipi->err()*fact; + } + else if(ix==2) { + sigma = _nUps2pipi->val()*fact; + error = _nUps2pipi->err()*fact; + } + else if(ix==3) { + sigma = _nUps3pipi->val()*fact; + error = _nUps3pipi->err()*fact; + } + else if(ix==4) { + sigma = _nUps1KK->val()*fact; + error = _nUps1KK->err()*fact; + } + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + /// @name Histograms + //@{ + CounterPtr _nUps1pipi,_nUps2pipi,_nUps3pipi,_nUps1KK; + //@} + + }; + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2008_I764099); + +} diff --git a/analyses/pluginBELLE/BELLE_2008_I764099.info b/analyses/pluginBELLE/BELLE_2008_I764099.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I764099.info @@ -0,0 +1,36 @@ +Name: BELLE_2008_I764099 +Year: 2008 +Summary: Cross Section for $e^+e^-\to\Upsilon(1,2,3S)\pi^+\pi^-$ and $\Upsilon(1S)K^+K^-$ at 10.87 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 764099 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 100 (2008) 112001, 2008 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\Upsilon(1,2,3S)\pi^+\pi^-$ and $\Upsilon(1S)K^+K^-$ at 10.87 GeV measured by BELLE.' +Keywords: [] +BibKey: Abe:2007tk +BibTeX: '@article{Abe:2007tk, + author = "Chen, K. F. and others", + title = "{Observation of anomalous Upsilon(1S) pi+ pi- and + Upsilon(2S) pi+ pi- production near the Upsilon(5S) + resonance}", + collaboration = "Belle", + journal = "Phys. Rev. Lett.", + volume = "100", + year = "2008", + pages = "112001", + doi = "10.1103/PhysRevLett.100.112001", + eprint = "0710.2577", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-CONF-0774", + SLACcitation = "%%CITATION = ARXIV:0710.2577;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2008_I764099.plot b/analyses/pluginBELLE/BELLE_2008_I764099.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I764099.plot @@ -0,0 +1,32 @@ +BEGIN PLOT /BELLE_2008_I764099/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\Upsilon(1S))$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\Upsilon(1S))$/pb +ConnectGaps=1 +XMin=10. +XMax=11. +END PLOT +BEGIN PLOT /BELLE_2008_I764099/d02-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\Upsilon(2S))$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\Upsilon(2S))$/pb +ConnectGaps=1 +XMin=10. +XMax=11. +END PLOT +BEGIN PLOT /BELLE_2008_I764099/d03-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\Upsilon(3S))$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\Upsilon(3S))$/pb +ConnectGaps=1 +XMin=10. +XMax=11. +END PLOT +BEGIN PLOT /BELLE_2008_I764099/d04-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\Upsilon(1S))$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\Upsilon(1S))$/pb +ConnectGaps=1 +XMin=10. +XMax=11. +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2008_I764099.yoda b/analyses/pluginBELLE/BELLE_2008_I764099.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I764099.yoda @@ -0,0 +1,48 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2008_I764099/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.12, up: 0.12}}} + +IsRef: 1 +Path: /REF/BELLE_2008_I764099/d01-x01-y01 +Title: doi:10.17182/hepdata.50307.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.087000e+01 0.000000e+00 0.000000e+00 1.610000e+00 1.562050e-01 1.562050e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2008_I764099/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.19, up: 0.19}, sys: {dn: -0.32, up: 0.32}}} + +IsRef: 1 +Path: /REF/BELLE_2008_I764099/d02-x01-y01 +Title: doi:10.17182/hepdata.50307.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.087000e+01 0.000000e+00 0.000000e+00 2.350000e+00 3.721559e-01 3.721559e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2008_I764099/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.45, up: 0.55}, sys: {dn: -0.19, up: 0.19}}} + +IsRef: 1 +Path: /REF/BELLE_2008_I764099/d03-x01-y01 +Title: doi:10.17182/hepdata.50307.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.087000e+01 0.000000e+00 0.000000e+00 1.440000e+00 4.884670e-01 5.818935e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2008_I764099/d04-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.041, up: 0.048}, sys: {dn: -0.028, up: 0.028}}} + +IsRef: 1 +Path: /REF/BELLE_2008_I764099/d04-x01-y01 +Title: doi:10.17182/hepdata.50307.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.087000e+01 0.000000e+00 0.000000e+00 1.850000e-01 4.964877e-02 5.556978e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2008_I786560.cc b/analyses/pluginBELLE/BELLE_2008_I786560.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I786560.cc @@ -0,0 +1,104 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief BELLE tau lepton to pi pi + /// @author Peter Richardson + class BELLE_2008_I786560 : public Analysis { + public: + + BELLE_2008_I786560() + : Analysis("BELLE_2008_I786560"), + _weight_total(0), + _weight_pipi(0) + { } + + + void init() { + declare(UnstableParticles(), "UFS"); + _hist_pipi = bookHisto1D( 1, 1, 1); + } + + + void analyze(const Event& e) { + // Find the taus + Particles taus; + const UnstableParticles& ufs = apply(e, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if (p.abspid() != PID::TAU) continue; + _weight_total += 1.; + Particles pip, pim, pi0; + unsigned int nstable = 0; + // find the decay products we want + findDecayProducts(p, nstable, pip, pim, pi0); + if (p.pid() < 0) { + swap(pip, pim); + } + if (nstable != 3) continue; + // pipi + if (pim.size() == 1 && pi0.size() == 1) { + _weight_pipi += 1.; + _hist_pipi->fill((pi0[0].momentum()+pim[0].momentum()).mass2(),1.); + } + } + } + + + void finalize() { + if (_weight_pipi > 0.) scale(_hist_pipi, 1./_weight_pipi); + } + + + private: + + //@{ + + // Histograms + Histo1DPtr _hist_pipi; + + // Weights counters + double _weight_total, _weight_pipi; + + //@} + + void findDecayProducts(const Particle &mother, + unsigned int & nstable, + Particles& pip, Particles& pim, + Particles& pi0) { + for (const Particle &p : mother.children()) { + long id = p.pdgId(); + if (id == PID::PI0 ) { + pi0.push_back(p); + ++nstable; + } + else if (id == PID::K0S) + ++nstable; + else if (id == PID::PIPLUS) { + pip.push_back(p); + ++nstable; + } + else if (id == PID::PIMINUS) { + pim.push_back(p); + ++nstable; + } + else if (id == PID::KPLUS) { + ++nstable; + } + else if (id == PID::KMINUS) { + ++nstable; + } + else if (!p.children().empty()) { + findDecayProducts(p, nstable, pip, pim, pi0); + } + else ++nstable; + } + } + }; + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2008_I786560); + +} diff --git a/analyses/pluginMisc/BELLE_2008_I786560.info b/analyses/pluginBELLE/BELLE_2008_I786560.info rename from analyses/pluginMisc/BELLE_2008_I786560.info rename to analyses/pluginBELLE/BELLE_2008_I786560.info diff --git a/analyses/pluginMisc/BELLE_2008_I786560.plot b/analyses/pluginBELLE/BELLE_2008_I786560.plot rename from analyses/pluginMisc/BELLE_2008_I786560.plot rename to analyses/pluginBELLE/BELLE_2008_I786560.plot diff --git a/analyses/pluginMisc/BELLE_2008_I786560.yoda b/analyses/pluginBELLE/BELLE_2008_I786560.yoda rename from analyses/pluginMisc/BELLE_2008_I786560.yoda rename to analyses/pluginBELLE/BELLE_2008_I786560.yoda diff --git a/analyses/pluginBELLE/BELLE_2008_I791660.cc b/analyses/pluginBELLE/BELLE_2008_I791660.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I791660.cc @@ -0,0 +1,126 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2008_I791660 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2008_I791660); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nLambda = bookCounter("/TMP/nLambda"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + bool matched=false; + for(unsigned int iy=0;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + break; + } + } + if(matched) { + _nLambda->fill(event.weight()); + break; + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _nLambda->val(); + double error = _nLambda->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nLambda; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2008_I791660); + + +} diff --git a/analyses/pluginBELLE/BELLE_2008_I791660.info b/analyses/pluginBELLE/BELLE_2008_I791660.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I791660.info @@ -0,0 +1,37 @@ +Name: BELLE_2008_I791660 +Year: 2008 +Summary: Cross section for $e^+e^-\to \Lambda_c^+\bar{\Lambda}_c^-$ below 5.4 GeV. +Experiment: BELLE +Collider: KEKB +InspireID: 791660 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 101 (2008) 172001 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to \Lambda_c^+\bar{\Lambda}_c^-$ below 5.4 GeV.' +Keywords: [] +BibKey: Pakhlova:2008vn +BibTeX: '@article{Pakhlova:2008vn, + author = "Pakhlova, G. and others", + title = "{Observation of a near-threshold enhancement in the e+e- + ---> Lambda+(c) Lambda-(c) cross section using + initial-state radiation}", + booktitle = "{Proceedings, 34th International Conference on High + Energy Physics (ICHEP 2008): Philadelphia, Pennsylvania, + July 30-August 5, 2008}", + collaboration = "Belle", + journal = "Phys. Rev. Lett.", + volume = "101", + year = "2008", + pages = "172001", + doi = "10.1103/PhysRevLett.101.172001", + eprint = "0807.4458", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0807.4458;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2008_I791660.plot b/analyses/pluginBELLE/BELLE_2008_I791660.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I791660.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BELLE_2008_I791660/d01-x01-y01 +Title=$\sigma(e^+e^-\to \Lambda_c^+\bar{\Lambda}_c^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \Lambda_c^+\bar{\Lambda}_c^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2008_I791660.yoda b/analyses/pluginBELLE/BELLE_2008_I791660.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2008_I791660.yoda @@ -0,0 +1,53 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2008_I791660/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.047, up: 0.047}, sys: {dn: -0.007, up: 0.007}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.02112, up: 0.02112}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.01716, up: 0.01716}}, 1: {stat: {dn: -0.088, up: 0.088}, sys: {dn: -0.028, up: 0.028}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.08928000000000001, up: 0.08928000000000001}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.07254000000000001, up: 0.07254000000000001}}, 2: {stat: {dn: -0.109, up: 0.109}, sys: {dn: -0.038, up: 0.038}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.12128, up: 0.12128}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.09854, up: 0.09854}}, 3: {stat: {dn: -0.122, up: 0.122}, sys: {dn: -0.047, up: 0.047}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.15136, up: 0.15136}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.12297999999999999, up: 0.12297999999999999}}, 4: {stat: {dn: -0.117, up: 0.117}, sys: {dn: -0.055, up: 0.055}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.17504, up: 0.17504}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.14222, up: 0.14222}}, 5: {stat: {dn: -0.098, up: 0.098}, sys: {dn: -0.025, up: 0.025}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.07968, up: 0.07968}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.06474, up: 0.06474}}, 6: {stat: {dn: -0.091, up: 0.091}, sys: {dn: -0.019, up: 0.019}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.06176, up: 0.06176}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.05018, up: 0.05018}}, 7: {stat: {dn: -0.087, up: 0.087}, sys: {dn: -0.015, up: 0.015}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.04896, up: 0.04896}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.039779999999999996, up: 0.039779999999999996}}, 8: {stat: {dn: -0.082, up: 0.082}, sys: {dn: -0.011, up: 0.011}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.03616, up: 0.03616}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.029379999999999996, up: 0.029379999999999996}}, 9: {stat: {dn: -0.069, up: 0.069}, sys: {dn: -0.009, up: 0.009}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.02656, up: 0.02656}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.021580000000000002, up: 0.021580000000000002}}, 10: {stat: {dn: -0.085, up: 0.085}, sys: {dn: -0.016, up: 0.016}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.05152, up: 0.05152}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.04186, up: 0.04186}}, 11: {stat: {dn: -0.089, up: 0.089}, sys: {dn: -0.019, up: 0.019}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.06048, up: 0.06048}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.049139999999999996, up: 0.049139999999999996}}, 12: {stat: {dn: -0.081, up: 0.081}, sys: {dn: -0.018, up: 0.018}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.05728, up: 0.05728}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.04654, up: 0.04654}}, 13: {stat: {dn: -0.069, up: 0.069}, sys: {dn: -0.008, up: 0.008}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.02144, up: 0.02144}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.01742, up: 0.01742}}, 14: {stat: {dn: -0.074, up: 0.074}, sys: {dn: -0.011, up: 0.011}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.032, up: 0.032}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.026000000000000002, up: 0.026000000000000002}}, 15: {stat: {dn: -0.08, up: 0.08}, sys: {dn: -0.016, up: 0.016}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.05024, up: 0.05024}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.04082, up: 0.04082}}, 16: {stat: {dn: -0.076, up: 0.076}, sys: {dn: -0.011, up: 0.011}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.03648, up: 0.03648}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.02964, up: 0.02964}}, 17: {stat: {dn: -0.064, up: 0.064}, sys: {dn: -0.009, up: 0.009}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.024, up: 0.024}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.0195, up: 0.0195}}, 18: {stat: {dn: -0.064, up: 0.064}, sys: {dn: -0.007, up: 0.007}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.01504, up: 0.01504}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.01222, up: 0.01222}}, 19: {stat: {dn: -0.071, up: 0.071}, sys: {dn: -0.013, up: 0.013}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.04032, up: 0.04032}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.032760000000000004, up: 0.032760000000000004}}, 20: {stat: {dn: -0.082, up: 0.082}, sys: {dn: -0.023, up: 0.023}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.07296, up: 0.07296}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.05928, up: 0.05928}}, 21: {stat: {dn: -0.07, up: 0.07}, sys: {dn: -0.015, up: 0.015}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.04896, up: 0.04896}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.039779999999999996, up: 0.039779999999999996}}, 22: {stat: {dn: -0.062, up: 0.062}, sys: {dn: -0.009, up: 0.009}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.02496, up: 0.02496}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.02028, up: 0.02028}}, 23: {stat: {dn: -0.071, up: 0.071}, sys: {dn: -0.017, up: 0.017}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.054400000000000004, up: 0.054400000000000004}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.0442, up: 0.0442}}, 24: {stat: {dn: -0.069, up: 0.069}, sys: {dn: -0.015, up: 0.015}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.04672, up: 0.04672}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.03796, up: 0.03796}}, 25: {stat: {dn: -0.073, up: 0.073}, sys: {dn: -0.02, up: 0.02}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.06272, up: 0.06272}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.05096, up: 0.05096}}, 26: {stat: {dn: -0.036, up: 0.036}, sys: {dn: -0.02, up: 0.02}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: 0.007039999999999999, up: -0.007039999999999999}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: 0.005719999999999999, up: -0.005719999999999999}}, 27: {stat: {dn: -0.074, up: 0.074}, sys: {dn: -0.021, up: 0.021}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.06784, up: 0.06784}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.055119999999999995, up: 0.055119999999999995}}, 28: {stat: {dn: -0.049, up: 0.049}, sys: {dn: -0.008, up: 0.008}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.024319999999999998, up: 0.024319999999999998}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.01976, up: 0.01976}}, 29: {stat: {dn: -0.062, up: 0.062}, sys: {dn: -0.011, up: 0.011}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.035840000000000004, up: 0.035840000000000004}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.029120000000000004, up: 0.029120000000000004}}, 30: {stat: {dn: -0.049, up: 0.049}, sys: {dn: -0.008, up: 0.008}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.02112, up: 0.02112}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.01716, up: 0.01716}}, 31: {stat: {dn: -0.056, up: 0.056}, sys: {dn: -0.009, up: 0.009}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.028159999999999998, up: 0.028159999999999998}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.022879999999999998, up: 0.022879999999999998}}, 32: {stat: {dn: -0.072, up: 0.072}, sys: {dn: -0.021, up: 0.021}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.06784, up: 0.06784}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.055119999999999995, up: 0.055119999999999995}}, 33: {stat: {dn: -0.052, up: 0.052}, sys: {dn: -0.008, up: 0.008}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.02368, up: 0.02368}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.01924, up: 0.01924}}, 34: {stat: {dn: -0.054, up: 0.054}, sys: {dn: -0.007, up: 0.007}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.011200000000000002, up: 0.011200000000000002}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.0091, up: 0.0091}}, 35: {stat: {dn: -0.052, up: 0.052}, sys: {dn: -0.009, up: 0.009}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.02496, up: 0.02496}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.02028, up: 0.02028}}, 36: {stat: {dn: -0.054, up: 0.054}, sys: {dn: -0.01, up: 0.01}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.0304, up: 0.0304}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.0247, up: 0.0247}}, 37: {stat: {dn: -0.054, up: 0.054}, sys: {dn: -0.01, up: 0.01}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.02752, up: 0.02752}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.022359999999999998, up: 0.022359999999999998}}, 38: {stat: {dn: -0.061, up: 0.061}, sys: {dn: -0.008, up: 0.008}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.02464, up: 0.02464}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.02002, up: 0.02002}}, 39: {stat: {dn: -0.035, up: 0.035}, sys: {dn: -0.006, up: 0.006}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.01344, up: 0.01344}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.010920000000000001, up: 0.010920000000000001}}, 40: {stat: {dn: -0.047, up: 0.047}, sys: {dn: -0.006, up: 0.006}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.02048, up: 0.02048}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.016640000000000002, up: 0.016640000000000002}}, 41: {stat: {dn: -0.058, up: 0.058}, sys: {dn: -0.013, up: 0.013}, 'sys,Additional uncertainty from the Branching Ratio of LAMBDA/CBAR-.': {dn: -0.04064, up: 0.04064}, 'sys,Additional uncertainty from the Branching Ration of LAMBDA/C+.': {dn: -0.03302, up: 0.03302}}} + +IsRef: 1 +Path: /REF/BELLE_2008_I791660/d01-x01-y01 +Title: doi:10.17182/hepdata.21861.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.570000e+00 1.000000e-02 1.000000e-02 6.600000e-02 5.475874e-02 5.475874e-02 +4.590000e+00 1.000000e-02 1.000000e-02 2.790000e-01 1.475160e-01 1.475160e-01 +4.610000e+00 1.000000e-02 1.000000e-02 3.790000e-01 1.942781e-01 1.942781e-01 +4.630000e+00 1.000000e-02 1.000000e-02 4.730000e-01 2.347912e-01 2.347912e-01 +4.650000e+00 1.000000e-02 1.000000e-02 5.470000e-01 2.599606e-01 2.599606e-01 +4.670000e+00 1.000000e-02 1.000000e-02 2.490000e-01 1.441151e-01 1.441151e-01 +4.690000e+00 1.000000e-02 1.000000e-02 1.930000e-01 1.223696e-01 1.223696e-01 +4.710000e+00 1.000000e-02 1.000000e-02 1.530000e-01 1.085059e-01 1.085059e-01 +4.730000e+00 1.000000e-02 1.000000e-02 1.130000e-01 9.495120e-02 9.495120e-02 +4.750000e+00 1.000000e-02 1.000000e-02 8.300000e-02 7.754437e-02 7.754437e-02 +4.770000e+00 1.000000e-02 1.000000e-02 1.610000e-01 1.090301e-01 1.090301e-01 +4.790000e+00 1.000000e-02 1.000000e-02 1.890000e-01 1.198106e-01 1.198106e-01 +4.810000e+00 1.000000e-02 1.000000e-02 1.790000e-01 1.110494e-01 1.110494e-01 +4.830000e+00 1.000000e-02 1.000000e-02 6.700000e-02 7.475380e-02 7.475380e-02 +4.850000e+00 1.000000e-02 1.000000e-02 1.000000e-01 8.542248e-02 8.542248e-02 +4.870000e+00 1.000000e-02 1.000000e-02 1.570000e-01 1.041457e-01 1.041457e-01 +4.890000e+00 1.000000e-02 1.000000e-02 1.140000e-01 9.003510e-02 9.003510e-02 +4.910000e+00 1.000000e-02 1.000000e-02 7.500000e-02 7.164670e-02 7.164670e-02 +4.930000e+00 1.000000e-02 1.000000e-02 4.700000e-02 6.723489e-02 6.723489e-02 +4.950000e+00 1.000000e-02 1.000000e-02 1.260000e-01 8.893211e-02 8.893211e-02 +4.970000e+00 1.000000e-02 1.000000e-02 2.280000e-01 1.268475e-01 1.268475e-01 +4.990000e+00 1.000000e-02 1.000000e-02 1.530000e-01 9.541766e-02 9.541766e-02 +5.010000e+00 1.000000e-02 1.000000e-02 7.800000e-02 7.042216e-02 7.042216e-02 +5.030000e+00 1.000000e-02 1.000000e-02 1.700000e-01 1.012077e-01 1.012077e-01 +5.050000e+00 1.000000e-02 1.000000e-02 1.460000e-01 9.278858e-02 9.278858e-02 +5.070000e+00 1.000000e-02 1.000000e-02 1.960000e-01 1.107236e-01 1.107236e-01 +5.090000e+00 1.000000e-02 1.000000e-02 -2.200000e-02 4.216966e-02 4.216966e-02 +5.110000e+00 1.000000e-02 1.000000e-02 2.120000e-01 1.164366e-01 1.164366e-01 +5.130000e+00 1.000000e-02 1.000000e-02 7.600000e-02 5.871048e-02 5.871048e-02 +5.150000e+00 1.000000e-02 1.000000e-02 1.120000e-01 7.808636e-02 7.808636e-02 +5.170000e+00 1.000000e-02 1.000000e-02 6.600000e-02 5.661731e-02 5.661731e-02 +5.190000e+00 1.000000e-02 1.000000e-02 8.800000e-02 6.733112e-02 6.733112e-02 +5.210000e+00 1.000000e-02 1.000000e-02 2.120000e-01 1.151759e-01 1.151759e-01 +5.230000e+00 1.000000e-02 1.000000e-02 7.400000e-02 6.081875e-02 6.081875e-02 +5.250000e+00 1.000000e-02 1.000000e-02 3.500000e-02 5.633161e-02 5.633161e-02 +5.270000e+00 1.000000e-02 1.000000e-02 7.800000e-02 6.180032e-02 6.180032e-02 +5.290000e+00 1.000000e-02 1.000000e-02 9.500000e-02 6.745554e-02 6.745554e-02 +5.310000e+00 1.000000e-02 1.000000e-02 8.600000e-02 6.537064e-02 6.537064e-02 +5.330000e+00 1.000000e-02 1.000000e-02 7.700000e-02 6.923099e-02 6.923099e-02 +5.350000e+00 1.000000e-02 1.000000e-02 4.200000e-02 3.950797e-02 3.950797e-02 +5.370000e+00 1.000000e-02 1.000000e-02 6.400000e-02 5.423394e-02 5.423394e-02 +5.390000e+00 1.000000e-02 1.000000e-02 1.270000e-01 7.921446e-02 7.921446e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2009_I809630.cc b/analyses/pluginBELLE/BELLE_2009_I809630.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2009_I809630.cc @@ -0,0 +1,149 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2009_I809630 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2009_I809630); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _cphipippim = bookCounter("TMP/phipippim"); + _cphif0 = bookCounter("TMP/phif0"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // phi + if(p.pdgId()!=333) continue; + map nRes=nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // phi pi+pi- + if(ncount==2) { + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _cphipippim->fill(event.weight()); + } + foreach (const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=9010221) continue; + if(p2.parents()[0].isSame(p)) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=0) continue; + bool matched2 = true; + for(auto const & val : nResB) { + if(val.second!=0) { + matched2 = false; + break; + } + } + if(matched2) { + _cphif0 ->fill(event.weight()); + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma,error; + if(ix==1) { + sigma = _cphipippim->val(); + error = _cphipippim->err(); + } + else { + sigma = _cphif0->val(); + error = _cphif0->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + //@} + + + /// @name Histograms + //@{ + CounterPtr _cphipippim; + CounterPtr _cphif0; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2009_I809630); + + +} diff --git a/analyses/pluginBELLE/BELLE_2009_I809630.info b/analyses/pluginBELLE/BELLE_2009_I809630.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2009_I809630.info @@ -0,0 +1,35 @@ +Name: BELLE_2009_I809630 +Year: 2009 +Summary: Cross Section for $e^+e^-\to\phi\pi^+\pi^-$ between 1.488 and 2.987 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 809630 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D80 (2009) 031101, 2009 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\phi\pi^+\pi^-$ between 1.488 and 2.987 GeV' +Keywords: [] +BibKey: Shen:2009zze +BibTeX: '@article{Shen:2009zze, + author = "Shen, C. P. and others", + title = "{Observation of the phi(1680) and the Y(2175) in e+e- + ---> phi pi+ pi-}", + collaboration = "Belle", + journal = "Phys. Rev.", + volume = "D80", + year = "2009", + pages = "031101", + doi = "10.1103/PhysRevD.80.031101", + eprint = "0808.0006", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-CONF-0865", + SLACcitation = "%%CITATION = ARXIV:0808.0006;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2009_I809630.plot b/analyses/pluginBELLE/BELLE_2009_I809630.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2009_I809630.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BELLE_2009_I809630/d01-x01-y01 +Title=$\sigma(e^+e^-\to \phi\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2009_I809630.yoda b/analyses/pluginBELLE/BELLE_2009_I809630.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2009_I809630.yoda @@ -0,0 +1,127 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2009_I809630/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.012, up: 0.012}, sys: {dn: -0.005, up: 0.005}}, 1: {stat: {dn: -0.024, up: 0.024}, sys: {dn: -0.005, up: 0.005}}, 2: {stat: {dn: -0.027, up: 0.027}, sys: {dn: -0.007, up: 0.007}}, 3: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.011, up: 0.011}}, 4: {stat: {dn: -0.041, up: 0.041}, sys: {dn: -0.016, up: 0.016}}, 5: {stat: {dn: -0.057, up: 0.057}, sys: {dn: -0.033, up: 0.033}}, 6: {stat: {dn: -0.068, up: 0.068}, sys: {dn: -0.05, up: 0.05}}, 7: {stat: {dn: -0.069, up: 0.069}, sys: {dn: -0.046, up: 0.046}}, 8: {stat: {dn: -0.078, up: 0.078}, sys: {dn: -0.056, up: 0.056}}, 9: {stat: {dn: -0.085, up: 0.085}, sys: {dn: -0.073, up: 0.073}}, 10: {stat: {dn: -0.085, up: 0.085}, sys: {dn: -0.079, up: 0.079}}, 11: {stat: {dn: -0.088, up: 0.088}, sys: {dn: -0.082, up: 0.082}}, 12: {stat: {dn: -0.089, up: 0.089}, sys: {dn: -0.073, up: 0.073}}, 13: {stat: {dn: -0.084, up: 0.084}, sys: {dn: -0.06, up: 0.06}}, 14: {stat: {dn: -0.079, up: 0.079}, sys: {dn: -0.046, up: 0.046}}, 15: {stat: {dn: -0.077, up: 0.077}, sys: {dn: -0.046, up: 0.046}}, 16: {stat: {dn: -0.076, up: 0.076}, sys: {dn: -0.049, up: 0.049}}, 17: {stat: {dn: -0.075, up: 0.075}, sys: {dn: -0.055, up: 0.055}}, 18: {stat: {dn: -0.071, up: 0.071}, sys: {dn: -0.043, up: 0.043}}, 19: {stat: {dn: -0.067, up: 0.067}, sys: {dn: -0.037, up: 0.037}}, 20: {stat: {dn: -0.068, up: 0.068}, sys: {dn: -0.042, up: 0.042}}, 21: {stat: {dn: -0.065, up: 0.065}, sys: {dn: -0.04, up: 0.04}}, 22: {stat: {dn: -0.067, up: 0.067}, sys: {dn: -0.054, up: 0.054}}, 23: {stat: {dn: -0.059, up: 0.059}, sys: {dn: -0.035, up: 0.035}}, 24: {stat: {dn: -0.062, up: 0.062}, sys: {dn: -0.045, up: 0.045}}, 25: {stat: {dn: -0.06, up: 0.06}, sys: {dn: -0.042, up: 0.042}}, 26: {stat: {dn: -0.057, up: 0.057}, sys: {dn: -0.042, up: 0.042}}, 27: {stat: {dn: -0.053, up: 0.053}, sys: {dn: -0.034, up: 0.034}}, 28: {stat: {dn: -0.05, up: 0.05}, sys: {dn: -0.04, up: 0.04}}, 29: {stat: {dn: -0.043, up: 0.043}, sys: {dn: -0.024, up: 0.024}}, 30: {stat: {dn: -0.038, up: 0.038}, sys: {dn: -0.018, up: 0.018}}, 31: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.013, up: 0.013}}, 32: {stat: {dn: -0.034, up: 0.034}, sys: {dn: -0.013, up: 0.013}}, 33: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.014, up: 0.014}}, 34: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.011, up: 0.011}}, 35: {stat: {dn: -0.031, up: 0.031}, sys: {dn: -0.013, up: 0.013}}, 36: {stat: {dn: -0.032, up: 0.032}, sys: {dn: -0.016, up: 0.016}}, 37: {stat: {dn: -0.03, up: 0.03}, sys: {dn: -0.015, up: 0.015}}, 38: {stat: {dn: -0.028, up: 0.028}, sys: {dn: -0.013, up: 0.013}}, 39: {stat: {dn: -0.026, up: 0.026}, sys: {dn: -0.012, up: 0.012}}, 40: {stat: {dn: -0.026, up: 0.026}, sys: {dn: -0.011, up: 0.011}}, 41: {stat: {dn: -0.023, up: 0.023}, sys: {dn: -0.009, up: 0.009}}, 42: {stat: {dn: -0.023, up: 0.023}, sys: {dn: -0.008, up: 0.008}}, 43: {stat: {dn: -0.02, up: 0.02}, sys: {dn: -0.007, up: 0.007}}, 44: {stat: {dn: -0.019, up: 0.019}, sys: {dn: -0.006, up: 0.006}}, 45: {stat: {dn: -0.019, up: 0.019}, sys: {dn: -0.006, up: 0.006}}, 46: {stat: {dn: -0.022, up: 0.022}, sys: {dn: -0.009, up: 0.009}}, 47: {stat: {dn: -0.019, up: 0.019}, sys: {dn: -0.007, up: 0.007}}, 48: {stat: {dn: -0.022, up: 0.022}, sys: {dn: -0.012, up: 0.012}}, 49: {stat: {dn: -0.017, up: 0.017}, sys: {dn: -0.004, up: 0.004}}, 50: {stat: {dn: -0.017, up: 0.017}, sys: {dn: -0.006, up: 0.006}}, 51: {stat: {dn: -0.016, up: 0.016}, sys: {dn: -0.005, up: 0.005}}, 52: {stat: {dn: -0.017, up: 0.017}, sys: {dn: -0.006, up: 0.006}}, 53: {stat: {dn: -0.013, up: 0.013}, sys: {dn: -0.004, up: 0.004}}, 54: {stat: {dn: -0.016, up: 0.016}, sys: {dn: -0.006, up: 0.006}}, 55: {stat: {dn: -0.014, up: 0.014}, sys: {dn: -0.005, up: 0.005}}, 56: {stat: {dn: -0.016, up: 0.016}, sys: {dn: -0.006, up: 0.006}}, 57: {stat: {dn: -0.014, up: 0.014}, sys: {dn: -0.004, up: 0.004}}, 58: {stat: {dn: -0.014, up: 0.014}, sys: {dn: -0.004, up: 0.004}}, 59: {stat: {dn: -0.015, up: 0.015}, sys: {dn: -0.005, up: 0.005}}, 60: {stat: {dn: -0.012, up: 0.012}, sys: {dn: -0.003, up: 0.003}}} + +IsRef: 1 +Path: /REF/BELLE_2009_I809630/d01-x01-y01 +Title: doi:10.17182/hepdata.52399.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.487500e+00 1.250000e-02 1.250000e-02 5.400000e-02 1.300000e-02 1.300000e-02 +1.512500e+00 1.250000e-02 1.250000e-02 5.800000e-02 2.451530e-02 2.451530e-02 +1.537500e+00 1.250000e-02 1.250000e-02 7.400000e-02 2.789265e-02 2.789265e-02 +1.562500e+00 1.250000e-02 1.250000e-02 1.200000e-01 3.478505e-02 3.478505e-02 +1.587500e+00 1.250000e-02 1.250000e-02 1.680000e-01 4.401136e-02 4.401136e-02 +1.612500e+00 1.250000e-02 1.250000e-02 3.370000e-01 6.586350e-02 6.586350e-02 +1.637500e+00 1.250000e-02 1.250000e-02 5.040000e-01 8.440379e-02 8.440379e-02 +1.662500e+00 1.250000e-02 1.250000e-02 4.480000e-01 8.292768e-02 8.292768e-02 +1.687500e+00 1.250000e-02 1.250000e-02 5.400000e-01 9.602083e-02 9.602083e-02 +1.712500e+00 1.250000e-02 1.250000e-02 6.790000e-01 1.120446e-01 1.120446e-01 +1.737500e+00 1.250000e-02 1.250000e-02 7.060000e-01 1.160431e-01 1.160431e-01 +1.762500e+00 1.250000e-02 1.250000e-02 6.990000e-01 1.202830e-01 1.202830e-01 +1.787500e+00 1.250000e-02 1.250000e-02 5.970000e-01 1.151086e-01 1.151086e-01 +1.812500e+00 1.250000e-02 1.250000e-02 4.640000e-01 1.032279e-01 1.032279e-01 +1.837500e+00 1.250000e-02 1.250000e-02 3.420000e-01 9.141663e-02 9.141663e-02 +1.862500e+00 1.250000e-02 1.250000e-02 3.340000e-01 8.969392e-02 8.969392e-02 +1.887500e+00 1.250000e-02 1.250000e-02 3.580000e-01 9.042677e-02 9.042677e-02 +1.912500e+00 1.250000e-02 1.250000e-02 4.200000e-01 9.300538e-02 9.300538e-02 +1.937500e+00 1.250000e-02 1.250000e-02 3.500000e-01 8.300602e-02 8.300602e-02 +1.962500e+00 1.250000e-02 1.250000e-02 3.310000e-01 7.653757e-02 7.653757e-02 +1.987500e+00 1.250000e-02 1.250000e-02 4.060000e-01 7.992496e-02 7.992496e-02 +2.012500e+00 1.250000e-02 1.250000e-02 4.020000e-01 7.632169e-02 7.632169e-02 +2.037500e+00 1.250000e-02 1.250000e-02 5.730000e-01 8.605231e-02 8.605231e-02 +2.062500e+00 1.250000e-02 1.250000e-02 3.830000e-01 6.860029e-02 6.860029e-02 +2.087500e+00 1.250000e-02 1.250000e-02 5.030000e-01 7.660940e-02 7.660940e-02 +2.112500e+00 1.250000e-02 1.250000e-02 4.790000e-01 7.323933e-02 7.323933e-02 +2.137500e+00 1.250000e-02 1.250000e-02 4.750000e-01 7.080254e-02 7.080254e-02 +2.162500e+00 1.250000e-02 1.250000e-02 3.900000e-01 6.296825e-02 6.296825e-02 +2.187500e+00 1.250000e-02 1.250000e-02 4.610000e-01 6.403124e-02 6.403124e-02 +2.212500e+00 1.250000e-02 1.250000e-02 2.780000e-01 4.924429e-02 4.924429e-02 +2.237500e+00 1.250000e-02 1.250000e-02 2.060000e-01 4.204759e-02 4.204759e-02 +2.262500e+00 1.250000e-02 1.250000e-02 1.480000e-01 3.546830e-02 3.546830e-02 +2.287500e+00 1.250000e-02 1.250000e-02 1.530000e-01 3.640055e-02 3.640055e-02 +2.312500e+00 1.250000e-02 1.250000e-02 1.620000e-01 3.584690e-02 3.584690e-02 +2.337500e+00 1.250000e-02 1.250000e-02 1.220000e-01 3.101612e-02 3.101612e-02 +2.362500e+00 1.250000e-02 1.250000e-02 1.540000e-01 3.361547e-02 3.361547e-02 +2.387500e+00 1.250000e-02 1.250000e-02 1.840000e-01 3.577709e-02 3.577709e-02 +2.412500e+00 1.250000e-02 1.250000e-02 1.690000e-01 3.354102e-02 3.354102e-02 +2.437500e+00 1.250000e-02 1.250000e-02 1.450000e-01 3.087070e-02 3.087070e-02 +2.462500e+00 1.250000e-02 1.250000e-02 1.350000e-01 2.863564e-02 2.863564e-02 +2.487500e+00 1.250000e-02 1.250000e-02 1.280000e-01 2.823119e-02 2.823119e-02 +2.512500e+00 1.250000e-02 1.250000e-02 1.080000e-01 2.469818e-02 2.469818e-02 +2.537500e+00 1.250000e-02 1.250000e-02 9.700000e-02 2.435159e-02 2.435159e-02 +2.562500e+00 1.250000e-02 1.250000e-02 7.800000e-02 2.118962e-02 2.118962e-02 +2.587500e+00 1.250000e-02 1.250000e-02 7.000000e-02 1.992486e-02 1.992486e-02 +2.612500e+00 1.250000e-02 1.250000e-02 6.600000e-02 1.992486e-02 1.992486e-02 +2.637500e+00 1.250000e-02 1.250000e-02 1.050000e-01 2.376973e-02 2.376973e-02 +2.662500e+00 1.250000e-02 1.250000e-02 8.200000e-02 2.024846e-02 2.024846e-02 +2.687500e+00 1.250000e-02 1.250000e-02 1.380000e-01 2.505993e-02 2.505993e-02 +2.712500e+00 1.250000e-02 1.250000e-02 4.600000e-02 1.746425e-02 1.746425e-02 +2.737500e+00 1.250000e-02 1.250000e-02 6.700000e-02 1.802776e-02 1.802776e-02 +2.762500e+00 1.250000e-02 1.250000e-02 5.800000e-02 1.676305e-02 1.676305e-02 +2.787500e+00 1.250000e-02 1.250000e-02 7.200000e-02 1.802776e-02 1.802776e-02 +2.812500e+00 1.250000e-02 1.250000e-02 4.600000e-02 1.360147e-02 1.360147e-02 +2.837500e+00 1.250000e-02 1.250000e-02 6.800000e-02 1.708801e-02 1.708801e-02 +2.862500e+00 1.250000e-02 1.250000e-02 5.400000e-02 1.486607e-02 1.486607e-02 +2.887500e+00 1.250000e-02 1.250000e-02 6.700000e-02 1.708801e-02 1.708801e-02 +2.912500e+00 1.250000e-02 1.250000e-02 5.000000e-02 1.456022e-02 1.456022e-02 +2.937500e+00 1.250000e-02 1.250000e-02 5.100000e-02 1.456022e-02 1.456022e-02 +2.962500e+00 1.250000e-02 1.250000e-02 5.800000e-02 1.581139e-02 1.581139e-02 +2.987500e+00 1.250000e-02 1.250000e-02 2.900000e-02 1.236932e-02 1.236932e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2009_I809630/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.013, up: 0.013}, sys: {dn: -0.003, up: 0.003}}, 1: {stat: {dn: -0.035, up: 0.035}, sys: {dn: -0.017, up: 0.017}}, 2: {stat: {dn: -0.038, up: 0.038}, sys: {dn: -0.017, up: 0.017}}, 3: {stat: {dn: -0.047, up: 0.047}, sys: {dn: -0.023, up: 0.023}}, 4: {stat: {dn: -0.053, up: 0.053}, sys: {dn: -0.03, up: 0.03}}, 5: {stat: {dn: -0.056, up: 0.056}, sys: {dn: -0.031, up: 0.031}}, 6: {stat: {dn: -0.062, up: 0.062}, sys: {dn: -0.04, up: 0.04}}, 7: {stat: {dn: -0.059, up: 0.059}, sys: {dn: -0.03, up: 0.03}}, 8: {stat: {dn: -0.064, up: 0.064}, sys: {dn: -0.037, up: 0.037}}, 9: {stat: {dn: -0.065, up: 0.065}, sys: {dn: -0.04, up: 0.04}}, 10: {stat: {dn: -0.068, up: 0.068}, sys: {dn: -0.046, up: 0.046}}, 11: {stat: {dn: -0.059, up: 0.059}, sys: {dn: -0.032, up: 0.032}}, 12: {stat: {dn: -0.056, up: 0.056}, sys: {dn: -0.032, up: 0.032}}, 13: {stat: {dn: -0.049, up: 0.049}, sys: {dn: -0.024, up: 0.024}}, 14: {stat: {dn: -0.041, up: 0.041}, sys: {dn: -0.014, up: 0.014}}, 15: {stat: {dn: -0.032, up: 0.032}, sys: {dn: -0.007, up: 0.007}}, 16: {stat: {dn: -0.037, up: 0.037}, sys: {dn: -0.012, up: 0.012}}, 17: {stat: {dn: -0.038, up: 0.038}, sys: {dn: -0.013, up: 0.013}}, 18: {stat: {dn: -0.03, up: 0.03}, sys: {dn: -0.008, up: 0.008}}, 19: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.007, up: 0.007}}, 20: {stat: {dn: -0.034, up: 0.034}, sys: {dn: -0.011, up: 0.011}}, 21: {stat: {dn: -0.035, up: 0.035}, sys: {dn: -0.012, up: 0.012}}, 22: {stat: {dn: -0.034, up: 0.034}, sys: {dn: -0.011, up: 0.011}}, 23: {stat: {dn: -0.025, up: 0.025}, sys: {dn: -0.006, up: 0.006}}, 24: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.009, up: 0.009}}, 25: {stat: {dn: -0.022, up: 0.022}, sys: {dn: -0.005, up: 0.005}}, 26: {stat: {dn: -0.022, up: 0.022}, sys: {dn: -0.006, up: 0.006}}, 27: {stat: {dn: -0.021, up: 0.021}, sys: {dn: -0.005, up: 0.005}}, 28: {stat: {dn: -0.016, up: 0.016}, sys: {dn: -0.002, up: 0.002}}, 29: {stat: {dn: -0.019, up: 0.019}, sys: {dn: -0.003, up: 0.003}}, 30: {stat: {dn: -0.022, up: 0.022}, sys: {dn: -0.004, up: 0.004}}, 31: {stat: {dn: -0.02, up: 0.02}, sys: {dn: -0.005, up: 0.005}}, 32: {stat: {dn: -0.023, up: 0.023}, sys: {dn: -0.008, up: 0.008}}, 33: {stat: {dn: -0.018, up: 0.018}, sys: {dn: -0.004, up: 0.004}}, 34: {stat: {dn: -0.019, up: 0.019}, sys: {dn: -0.004, up: 0.004}}, 35: {stat: {dn: -0.015, up: 0.015}, sys: {dn: -0.003, up: 0.003}}, 36: {stat: {dn: -0.017, up: 0.017}, sys: {dn: -0.003, up: 0.003}}, 37: {stat: {dn: -0.016, up: 0.016}, sys: {dn: -0.003, up: 0.003}}, 38: {stat: {dn: -0.016, up: 0.016}, sys: {dn: -0.003, up: 0.003}}, 39: {stat: {dn: -0.016, up: 0.016}, sys: {dn: -0.003, up: 0.003}}, 40: {stat: {dn: -0.014, up: 0.014}, sys: {dn: -0.002, up: 0.002}}, 41: {stat: {dn: -0.013, up: 0.013}, sys: {dn: -0.003, up: 0.003}}, 42: {stat: {dn: -0.013, up: 0.013}, sys: {dn: -0.003, up: 0.003}}, 43: {stat: {dn: -0.014, up: 0.014}, sys: {dn: -0.003, up: 0.003}}} + +IsRef: 1 +Path: /REF/BELLE_2009_I809630/d02-x01-y01 +Title: doi:10.17182/hepdata.52399.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.887500e+00 1.250000e-02 1.250000e-02 2.000000e-02 1.334166e-02 1.334166e-02 +1.912500e+00 1.250000e-02 1.250000e-02 1.380000e-01 3.891015e-02 3.891015e-02 +1.937500e+00 1.250000e-02 1.250000e-02 1.520000e-01 4.162932e-02 4.162932e-02 +1.962500e+00 1.250000e-02 1.250000e-02 2.310000e-01 5.232590e-02 5.232590e-02 +1.987500e+00 1.250000e-02 1.250000e-02 3.310000e-01 6.090156e-02 6.090156e-02 +2.012500e+00 1.250000e-02 1.250000e-02 3.670000e-01 6.400781e-02 6.400781e-02 +2.037500e+00 1.250000e-02 1.250000e-02 5.020000e-01 7.378347e-02 7.378347e-02 +2.062500e+00 1.250000e-02 1.250000e-02 4.010000e-01 6.618912e-02 6.618912e-02 +2.087500e+00 1.250000e-02 1.250000e-02 5.020000e-01 7.392564e-02 7.392564e-02 +2.112500e+00 1.250000e-02 1.250000e-02 5.570000e-01 7.632169e-02 7.632169e-02 +2.137500e+00 1.250000e-02 1.250000e-02 6.460000e-01 8.209750e-02 8.209750e-02 +2.162500e+00 1.250000e-02 1.250000e-02 4.560000e-01 6.711930e-02 6.711930e-02 +2.187500e+00 1.250000e-02 1.250000e-02 4.610000e-01 6.449806e-02 6.449806e-02 +2.212500e+00 1.250000e-02 1.250000e-02 3.430000e-01 5.456189e-02 5.456189e-02 +2.237500e+00 1.250000e-02 1.250000e-02 2.000000e-01 4.332436e-02 4.332436e-02 +2.262500e+00 1.250000e-02 1.250000e-02 1.020000e-01 3.275668e-02 3.275668e-02 +2.287500e+00 1.250000e-02 1.250000e-02 1.780000e-01 3.889730e-02 3.889730e-02 +2.312500e+00 1.250000e-02 1.250000e-02 1.890000e-01 4.016217e-02 4.016217e-02 +2.337500e+00 1.250000e-02 1.250000e-02 1.210000e-01 3.104835e-02 3.104835e-02 +2.362500e+00 1.250000e-02 1.250000e-02 9.600000e-02 2.983287e-02 2.983287e-02 +2.387500e+00 1.250000e-02 1.250000e-02 1.640000e-01 3.573514e-02 3.573514e-02 +2.412500e+00 1.250000e-02 1.250000e-02 1.670000e-01 3.700000e-02 3.700000e-02 +2.437500e+00 1.250000e-02 1.250000e-02 1.640000e-01 3.573514e-02 3.573514e-02 +2.462500e+00 1.250000e-02 1.250000e-02 8.200000e-02 2.570992e-02 2.570992e-02 +2.487500e+00 1.250000e-02 1.250000e-02 1.230000e-01 3.036445e-02 3.036445e-02 +2.512500e+00 1.250000e-02 1.250000e-02 7.500000e-02 2.256103e-02 2.256103e-02 +2.537500e+00 1.250000e-02 1.250000e-02 8.000000e-02 2.280351e-02 2.280351e-02 +2.562500e+00 1.250000e-02 1.250000e-02 6.500000e-02 2.158703e-02 2.158703e-02 +2.587500e+00 1.250000e-02 1.250000e-02 3.200000e-02 1.612452e-02 1.612452e-02 +2.612500e+00 1.250000e-02 1.250000e-02 4.400000e-02 1.923538e-02 1.923538e-02 +2.637500e+00 1.250000e-02 1.250000e-02 5.300000e-02 2.236068e-02 2.236068e-02 +2.662500e+00 1.250000e-02 1.250000e-02 6.900000e-02 2.061553e-02 2.061553e-02 +2.687500e+00 1.250000e-02 1.250000e-02 1.170000e-01 2.435159e-02 2.435159e-02 +2.712500e+00 1.250000e-02 1.250000e-02 5.400000e-02 1.843909e-02 1.843909e-02 +2.737500e+00 1.250000e-02 1.250000e-02 5.800000e-02 1.941649e-02 1.941649e-02 +2.762500e+00 1.250000e-02 1.250000e-02 4.200000e-02 1.529706e-02 1.529706e-02 +2.787500e+00 1.250000e-02 1.250000e-02 4.800000e-02 1.726268e-02 1.726268e-02 +2.812500e+00 1.250000e-02 1.250000e-02 4.900000e-02 1.627882e-02 1.627882e-02 +2.837500e+00 1.250000e-02 1.250000e-02 4.700000e-02 1.627882e-02 1.627882e-02 +2.862500e+00 1.250000e-02 1.250000e-02 5.000000e-02 1.627882e-02 1.627882e-02 +2.887500e+00 1.250000e-02 1.250000e-02 2.800000e-02 1.414214e-02 1.414214e-02 +2.912500e+00 1.250000e-02 1.250000e-02 3.900000e-02 1.334166e-02 1.334166e-02 +2.937500e+00 1.250000e-02 1.250000e-02 3.800000e-02 1.334166e-02 1.334166e-02 +2.962500e+00 1.250000e-02 1.250000e-02 3.600000e-02 1.431782e-02 1.431782e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2009_I823878.cc b/analyses/pluginBELLE/BELLE_2009_I823878.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2009_I823878.cc @@ -0,0 +1,127 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2009_I823878 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2009_I823878); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + _nMeson[1] = bookCounter("TMP/phieta"); + _nMeson[2] = bookCounter("TMP/phietaprime"); + _nMeson[3] = bookCounter("TMP/rhoeta"); + _nMeson[4] = bookCounter("TMP/rhoetaprime"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=333 && p.pdgId()!=113) continue; + map nRes=nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + foreach (const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=221 && p2.pdgId()!=331 ) continue; + if(p2.parents()[0].isSame(p)) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=0) continue; + bool matched2 = true; + for(auto const & val : nResB) { + if(val.second!=0) { + matched2 = false; + break; + } + } + if(matched2) { + unsigned int iloc=1; + if(p.pdgId()==113 ) iloc+=2; + if(p2.pdgId()==331) iloc+=1; + _nMeson[iloc]->fill(event.weight()); + } + } + } + } + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<5;++ix) { + double sigma = _nMeson[ix]->val(); + double error = _nMeson[ix]->err(); + sigma *= crossSection()/ sumOfWeights() /femtobarn; + error *= crossSection()/ sumOfWeights() /femtobarn; + + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nMeson[5]; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2009_I823878); + + +} diff --git a/analyses/pluginBELLE/BELLE_2009_I823878.info b/analyses/pluginBELLE/BELLE_2009_I823878.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2009_I823878.info @@ -0,0 +1,34 @@ +Name: BELLE_2009_I823878 +Year: 2009 +Summary: Cross section for $\phi\eta$, $\phi\eta^\prime$, $\rho^0\eta$, $\rho^0\eta^\prime$ at 10.58 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 823878 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B681 (2009) 400-405, 2009 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $\phi\eta$, $\phi\eta^\prime$, $\rho^0\eta$, $\rho^0\eta^\prime$ at 10.58 GeV' +Keywords: [] +BibKey: Belous:2009yp +BibTeX: '@article{Belous:2009yp, + author = "Belous, K. and others", + title = "{Measurement of cross sections of exclusive e+ e- ---> VP + processes at s**(1/2) = 10.58-GeV}", + collaboration = "Belle", + journal = "Phys. Lett.", + volume = "B681", + year = "2009", + pages = "400-405", + doi = "10.1016/j.physletb.2009.10.037", + eprint = "0906.4214", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0906.4214;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2009_I823878.plot b/analyses/pluginBELLE/BELLE_2009_I823878.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2009_I823878.plot @@ -0,0 +1,32 @@ +BEGIN PLOT /BELLE_2009_I823878/d01-x01-y01 +Title=$\sigma(e^+e^-\to \phi\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\eta)$/pb +ConnectGaps=1 +XMin = 10.56 +XMin = 10.60 +END PLOT +BEGIN PLOT /BELLE_2009_I823878/d01-x01-y02 +Title=$\sigma(e^+e^-\to \phi\eta^\prime)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\eta^\prime)$/pb +ConnectGaps=1 +XMin = 10.56 +XMin = 10.60 +END PLOT +BEGIN PLOT /BELLE_2009_I823878/d01-x01-y03 +Title=$\sigma(e^+e^-\to \rho^0\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \rho^0\eta)$/pb +ConnectGaps=1 +XMin = 10.56 +XMin = 10.60 +END PLOT +BEGIN PLOT /BELLE_2009_I823878/d01-x01-y04 +Title=$\sigma(e^+e^-\to \rho^0\eta^\prime)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \rho^0\eta^\prime)$/pb +ConnectGaps=1 +XMin = 10.56 +XMin = 10.60 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2009_I823878.yoda b/analyses/pluginBELLE/BELLE_2009_I823878.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2009_I823878.yoda @@ -0,0 +1,48 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2009_I823878/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.4, up: 0.4}, sys: {dn: -0.1, up: 0.1}}} + +IsRef: 1 +Path: /REF/BELLE_2009_I823878/d01-x01-y01 +Title: doi:10.17182/hepdata.52944.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 1.400000e+00 4.123106e-01 4.123106e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2009_I823878/d01-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -1.1, up: 1.1}, sys: {dn: -0.4, up: 0.4}}} + +IsRef: 1 +Path: /REF/BELLE_2009_I823878/d01-x01-y02 +Title: doi:10.17182/hepdata.52944.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 5.300000e+00 1.170470e+00 1.170470e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2009_I823878/d01-x01-y03 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.5, up: 0.5}, sys: {dn: -0.1, up: 0.1}}} + +IsRef: 1 +Path: /REF/BELLE_2009_I823878/d01-x01-y03 +Title: doi:10.17182/hepdata.52944.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 3.100000e+00 5.099020e-01 5.099020e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2009_I823878/d01-x01-y04 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.6, up: 0.6}, sys: {dn: -0.2, up: 0.2}}} + +IsRef: 1 +Path: /REF/BELLE_2009_I823878/d01-x01-y04 +Title: doi:10.17182/hepdata.52944.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 3.300000e+00 6.324555e-01 6.324555e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2010_I841618.cc b/analyses/pluginBELLE/BELLE_2010_I841618.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2010_I841618.cc @@ -0,0 +1,117 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2010_I841618 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2010_I841618); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + declare(UnstableParticles(), "UFS"); + _h_3pi = bookHisto1D( 1, 1, 1); + _h_Kpipi = bookHisto1D( 2, 1, 1); + _h_KKpi = bookHisto1D( 3, 1, 1); + _h_3K = bookHisto1D( 4, 1, 1); + + } + + void findDecayProducts(const Particle & mother, unsigned int & nstable, + unsigned int & npip, unsigned int & npim, + unsigned int & nKp, unsigned int & nKm, FourMomentum & ptot) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::KPLUS ) { + ++nKp; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::KMINUS ) { + ++nKm; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::PIPLUS) { + ++npip; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::PIMINUS) { + ++npim; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::PI0 || id == PID::K0S) { + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p, nstable, npip, npim, nKp, nKm,ptot); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + // Loop over taus + for(const Particle& tau : apply(event, "UFS").particles(Cuts::abspid==PID::TAU)) { + unsigned int nstable(0),npip(0),npim(0),nKp(0),nKm(0); + FourMomentum p_tot(0,0,0,0); + findDecayProducts(tau, nstable, npip, npim, nKp, nKm, p_tot); + if (tau.pdgId() < 0) { + swap(npip, npim); + swap(nKp,nKm); + } + if(nstable!=4) continue; + if(npim==2 && npip==1 ) + _h_3pi->fill(p_tot.mass(), event.weight()); + else if(npim==1 && npip==1 && nKm==1) + _h_Kpipi->fill(p_tot.mass(), event.weight()); + else if(nKm==1 && nKp==1 && npim==1) + _h_KKpi->fill(p_tot.mass(), event.weight()); + else if(nKm==2 && nKp==1 ) + _h_3K->fill(p_tot.mass(), event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + normalize(_h_3pi); + normalize(_h_Kpipi); + normalize(_h_KKpi); + normalize(_h_3K); + + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _h_3pi, _h_Kpipi, _h_KKpi, _h_3K; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2010_I841618); + + +} diff --git a/analyses/pluginBELLE/BELLE_2010_I841618.info b/analyses/pluginBELLE/BELLE_2010_I841618.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2010_I841618.info @@ -0,0 +1,35 @@ +Name: BELLE_2010_I841618 +Year: 2010 +Summary: Mass spectra for $h^-h^-h^+$ decays of the $\tau^-$ lepton +Experiment: BELLE +Collider: KEKB +InspireID: 841618 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D81 (2010) 113007 +RunInfo: e+ e- > tau+ tau-, or any process producing tau leptons +NeedCrossSection: no +Description: + 'Mass spectra for $\pi^+\pi^-\pi^+$, $K^-\pi^+\pi^-$, $K^+K^-\pi^-$ and $K^-K^-K^+$ in tau decays + measured by BELLE. Useful for testing models of the hadronic current in $\tau$ decays.' +Keywords: [] +BibKey: Lee:2010tc +BibTeX: '@article{Lee:2010tc, + author = "Lee, M. J. and others", + title = "{Measurement of the branching fractions and the invariant + mass distributions for $\tau^- \to h^-h^+h^-\nu_{\tau}$ + decays}", + collaboration = "Belle", + journal = "Phys. Rev.", + volume = "D81", + year = "2010", + pages = "113007", + doi = "10.1103/PhysRevD.81.113007", + eprint = "1001.0083", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-PREPRINT-2009-23, KEK-PREPRINT-2009-26", + SLACcitation = "%%CITATION = ARXIV:1001.0083;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2010_I841618.plot b/analyses/pluginBELLE/BELLE_2010_I841618.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2010_I841618.plot @@ -0,0 +1,24 @@ +BEGIN PLOT /BELLE_2010_I841618/d01-x01-y01 +Title=$\pi^-\pi^-\pi^+$ mass in $\tau^-\to \pi^-\pi^-\pi^+\nu_\tau$ decays +XLabel=$m_{\pi^-\pi^-\pi^+}$ [$\text{GeV}$] +YLabel=$1/\Gamma\text{d}\Gamma/\text{d}m_{\pi^-\pi^-\pi^+}$ [ $\text{GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /BELLE_2010_I841618/d02-x01-y01 +Title=$K^-\pi^-\pi^+$ mass in $\tau^-\to K^-\pi^-\pi^+\nu_\tau$ decays +XLabel=$m_{K^-\pi^-\pi^+}$ [$\text{GeV}$] +YLabel=$1/\Gamma\text{d}\Gamma/\text{d}m_{K^-\pi^-\pi^+}$ [ $\text{GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /BELLE_2010_I841618/d03-x01-y01 +Title=$K^-K^+\pi^-$ mass in $\tau^-\to K^-K^+\pi^-\nu_\tau$ decays +XLabel=$m_{K^-K^+\pi^-}$ [$\text{GeV}$] +YLabel=$1/\Gamma\text{d}\Gamma/\text{d}m_{K^-K^+\pi^-}$ [ $\text{GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /BELLE_2010_I841618/d04-x01-y01 +Title=$K^-K^+K^-$ mass in $\tau^-\to K^-K^+K^-\nu_\tau$ decays +XLabel=$m_{K^-K^+K^-}$ [$\text{GeV}$] +YLabel=$1/\Gamma\text{d}\Gamma/\text{d}m_{K^-K^+K^-}$ [ $\text{GeV}^{-1}$] +LogY=0 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2010_I841618.yoda b/analyses/pluginBELLE/BELLE_2010_I841618.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2010_I841618.yoda @@ -0,0 +1,371 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2010_I841618/d01-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2010_I841618/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.44500 0.00500 0.00500 -1.38200e-05 9.27285e-06 9.27285e-06 +0.45500 0.00500 0.00500 -2.51300e-05 1.73646e-05 1.73646e-05 +0.46500 0.00500 0.00500 -5.09500e-05 3.66793e-05 3.66793e-05 +0.47500 0.00500 0.00500 -7.90900e-05 6.02195e-05 6.02195e-05 +0.48500 0.00500 0.00500 -1.18000e-04 9.70096e-05 9.70096e-05 +0.49500 0.00500 0.00500 -1.57300e-04 1.43573e-04 1.43573e-04 +0.50500 0.00500 0.00500 -1.89900e-04 2.00203e-04 2.00203e-04 +0.51500 0.00500 0.00500 -2.11500e-04 2.73258e-04 2.73258e-04 +0.52500 0.00500 0.00500 -2.04200e-04 3.58958e-04 3.58958e-04 +0.53500 0.00500 0.00500 -1.41800e-04 4.34675e-04 4.34675e-04 +0.54500 0.00500 0.00500 -1.73000e-05 5.17404e-04 5.17404e-04 +0.55500 0.00500 0.00500 1.97400e-04 5.94862e-04 5.94862e-04 +0.56500 0.00500 0.00500 5.41500e-04 6.64486e-04 6.64486e-04 +0.57500 0.00500 0.00500 1.02900e-03 6.73202e-04 6.73202e-04 +0.58500 0.00500 0.00500 1.67300e-03 6.25927e-04 6.25927e-04 +0.59500 0.00500 0.00500 2.61800e-03 5.90146e-04 5.90146e-04 +0.60500 0.00500 0.00500 3.68600e-03 5.61363e-04 5.61363e-04 +0.61500 0.00500 0.00500 5.05600e-03 6.00403e-04 6.00403e-04 +0.62500 0.00500 0.00500 6.76700e-03 6.68027e-04 6.68027e-04 +0.63500 0.00500 0.00500 8.85300e-03 7.33108e-04 7.33108e-04 +0.64500 0.00500 0.00500 1.11300e-02 7.67531e-04 7.67531e-04 +0.65500 0.00500 0.00500 1.44000e-02 8.28550e-04 8.28550e-04 +0.66500 0.00500 0.00500 1.76400e-02 8.53037e-04 8.53037e-04 +0.67500 0.00500 0.00500 2.18300e-02 9.11295e-04 9.11295e-04 +0.68500 0.00500 0.00500 2.62200e-02 9.77070e-04 9.77070e-04 +0.69500 0.00500 0.00500 3.19100e-02 1.07764e-03 1.07764e-03 +0.70500 0.00500 0.00500 3.78800e-02 1.14495e-03 1.14495e-03 +0.71500 0.00500 0.00500 4.59100e-02 1.21733e-03 1.21733e-03 +0.72500 0.00500 0.00500 5.35400e-02 1.25969e-03 1.25969e-03 +0.73500 0.00500 0.00500 6.26600e-02 1.34778e-03 1.34778e-03 +0.74500 0.00500 0.00500 7.32600e-02 1.40934e-03 1.40934e-03 +0.75500 0.00500 0.00500 8.52500e-02 1.44950e-03 1.44950e-03 +0.76500 0.00500 0.00500 9.85100e-02 1.56730e-03 1.56730e-03 +0.77500 0.00500 0.00500 1.13400e-01 1.72748e-03 1.72748e-03 +0.78500 0.00500 0.00500 1.32200e-01 1.96733e-03 1.96733e-03 +0.79500 0.00500 0.00500 1.52500e-01 2.21157e-03 2.21157e-03 +0.80500 0.00500 0.00500 1.77400e-01 2.33812e-03 2.33812e-03 +0.81500 0.00500 0.00500 2.06300e-01 2.31910e-03 2.31910e-03 +0.82500 0.00500 0.00500 2.41300e-01 2.45767e-03 2.45767e-03 +0.83500 0.00500 0.00500 2.80000e-01 2.80132e-03 2.80132e-03 +0.84500 0.00500 0.00500 3.24300e-01 3.22219e-03 3.22219e-03 +0.85500 0.00500 0.00500 3.78500e-01 3.48916e-03 3.48916e-03 +0.86500 0.00500 0.00500 4.41200e-01 3.71298e-03 3.71298e-03 +0.87500 0.00500 0.00500 5.12800e-01 4.09783e-03 4.09783e-03 +0.88500 0.00500 0.00500 5.98400e-01 4.73535e-03 4.73535e-03 +0.89500 0.00500 0.00500 6.95200e-01 5.61756e-03 5.61756e-03 +0.90500 0.00500 0.00500 8.01000e-01 6.22687e-03 6.22687e-03 +0.91500 0.00500 0.00500 9.13000e-01 6.29005e-03 6.29005e-03 +0.92500 0.00500 0.00500 1.02800e+00 6.68353e-03 6.68353e-03 +0.93500 0.00500 0.00500 1.14800e+00 7.51685e-03 7.51685e-03 +0.94500 0.00500 0.00500 1.27300e+00 8.74356e-03 8.74356e-03 +0.95500 0.00500 0.00500 1.39500e+00 9.33349e-03 9.33349e-03 +0.96500 0.00500 0.00500 1.52200e+00 9.49977e-03 9.49977e-03 +0.97500 0.00500 0.00500 1.64300e+00 1.02477e-02 1.02477e-02 +0.98500 0.00500 0.00500 1.75500e+00 1.21206e-02 1.21206e-02 +0.99500 0.00500 0.00500 1.86300e+00 1.40406e-02 1.40406e-02 +1.00500 0.00500 0.00500 1.96100e+00 1.42921e-02 1.42921e-02 +1.01500 0.00500 0.00500 2.05500e+00 1.41508e-02 1.41508e-02 +1.02500 0.00500 0.00500 2.13900e+00 1.52102e-02 1.52102e-02 +1.03500 0.00500 0.00500 2.21800e+00 1.79498e-02 1.79498e-02 +1.04500 0.00500 0.00500 2.29200e+00 1.85373e-02 1.85373e-02 +1.05500 0.00500 0.00500 2.34700e+00 1.76894e-02 1.76894e-02 +1.06500 0.00500 0.00500 2.39800e+00 1.86658e-02 1.86658e-02 +1.07500 0.00500 0.00500 2.44300e+00 1.87015e-02 1.87015e-02 +1.08500 0.00500 0.00500 2.46800e+00 2.01276e-02 2.01276e-02 +1.09500 0.00500 0.00500 2.48500e+00 2.20436e-02 2.20436e-02 +1.10500 0.00500 0.00500 2.49600e+00 1.89596e-02 1.89596e-02 +1.11500 0.00500 0.00500 2.50300e+00 1.89711e-02 1.89711e-02 +1.12500 0.00500 0.00500 2.49400e+00 2.05676e-02 2.05676e-02 +1.13500 0.00500 0.00500 2.47400e+00 2.13987e-02 2.13987e-02 +1.14500 0.00500 0.00500 2.44900e+00 2.05736e-02 2.05736e-02 +1.15500 0.00500 0.00500 2.42700e+00 1.95528e-02 1.95528e-02 +1.16500 0.00500 0.00500 2.39700e+00 2.19660e-02 2.19660e-02 +1.17500 0.00500 0.00500 2.35000e+00 2.08373e-02 2.08373e-02 +1.18500 0.00500 0.00500 2.30100e+00 1.94963e-02 1.94963e-02 +1.19500 0.00500 0.00500 2.23900e+00 1.96005e-02 1.96005e-02 +1.20500 0.00500 0.00500 2.17800e+00 1.91898e-02 1.91898e-02 +1.21500 0.00500 0.00500 2.11400e+00 2.10819e-02 2.10819e-02 +1.22500 0.00500 0.00500 2.04100e+00 2.23148e-02 2.23148e-02 +1.23500 0.00500 0.00500 1.96600e+00 2.18711e-02 2.18711e-02 +1.24500 0.00500 0.00500 1.88900e+00 2.01005e-02 2.01005e-02 +1.25500 0.00500 0.00500 1.81900e+00 1.76217e-02 1.76217e-02 +1.26500 0.00500 0.00500 1.74100e+00 1.65963e-02 1.65963e-02 +1.27500 0.00500 0.00500 1.66300e+00 1.56822e-02 1.56822e-02 +1.28500 0.00500 0.00500 1.57700e+00 1.60829e-02 1.60829e-02 +1.29500 0.00500 0.00500 1.49600e+00 1.57821e-02 1.57821e-02 +1.30500 0.00500 0.00500 1.41500e+00 1.47673e-02 1.47673e-02 +1.31500 0.00500 0.00500 1.33500e+00 1.40072e-02 1.40072e-02 +1.32500 0.00500 0.00500 1.25800e+00 1.34814e-02 1.34814e-02 +1.33500 0.00500 0.00500 1.17900e+00 1.28776e-02 1.28776e-02 +1.34500 0.00500 0.00500 1.09900e+00 1.33991e-02 1.33991e-02 +1.35500 0.00500 0.00500 1.01400e+00 1.28443e-02 1.28443e-02 +1.36500 0.00500 0.00500 9.34100e-01 1.17906e-02 1.17906e-02 +1.37500 0.00500 0.00500 8.54400e-01 1.09026e-02 1.09026e-02 +1.38500 0.00500 0.00500 7.88600e-01 1.07064e-02 1.07064e-02 +1.39500 0.00500 0.00500 6.84500e-01 9.22957e-03 9.22957e-03 +1.40500 0.00500 0.00500 6.10500e-01 8.06834e-03 8.06834e-03 +1.41500 0.00500 0.00500 5.50300e-01 6.88882e-03 6.88882e-03 +1.42500 0.00500 0.00500 4.97200e-01 6.08521e-03 6.08521e-03 +1.43500 0.00500 0.00500 4.46300e-01 5.65360e-03 5.65360e-03 +1.44500 0.00500 0.00500 4.00400e-01 5.63395e-03 5.63395e-03 +1.45500 0.00500 0.00500 3.59100e-01 5.70863e-03 5.70863e-03 +1.46500 0.00500 0.00500 3.24700e-01 5.45374e-03 5.45374e-03 +1.47500 0.00500 0.00500 2.93300e-01 4.92950e-03 4.92950e-03 +1.48500 0.00500 0.00500 2.66000e-01 4.43768e-03 4.43768e-03 +1.49500 0.00500 0.00500 2.42200e-01 4.06021e-03 4.06021e-03 +1.50500 0.00500 0.00500 2.18900e-01 3.84848e-03 3.84848e-03 +1.51500 0.00500 0.00500 1.96000e-01 3.79477e-03 3.79477e-03 +1.52500 0.00500 0.00500 1.76800e-01 3.84828e-03 3.84828e-03 +1.53500 0.00500 0.00500 1.59100e-01 3.80327e-03 3.80327e-03 +1.54500 0.00500 0.00500 1.41800e-01 3.50632e-03 3.50632e-03 +1.55500 0.00500 0.00500 1.27500e-01 3.10028e-03 3.10028e-03 +1.56500 0.00500 0.00500 1.13500e-01 2.68528e-03 2.68528e-03 +1.57500 0.00500 0.00500 1.02700e-01 2.38588e-03 2.38588e-03 +1.58500 0.00500 0.00500 9.02800e-02 2.15130e-03 2.15130e-03 +1.59500 0.00500 0.00500 8.02500e-02 2.05794e-03 2.05794e-03 +1.60500 0.00500 0.00500 7.04100e-02 1.97562e-03 1.97562e-03 +1.61500 0.00500 0.00500 6.19100e-02 1.85499e-03 1.85499e-03 +1.62500 0.00500 0.00500 5.44400e-02 1.67820e-03 1.67820e-03 +1.63500 0.00500 0.00500 4.64900e-02 1.44065e-03 1.44065e-03 +1.64500 0.00500 0.00500 4.00800e-02 1.27496e-03 1.27496e-03 +1.65500 0.00500 0.00500 3.38900e-02 1.17031e-03 1.17031e-03 +1.66500 0.00500 0.00500 2.79800e-02 1.11583e-03 1.11583e-03 +1.67500 0.00500 0.00500 2.32200e-02 1.12566e-03 1.12566e-03 +1.68500 0.00500 0.00500 1.87300e-02 1.13558e-03 1.13558e-03 +1.69500 0.00500 0.00500 1.45200e-02 1.10420e-03 1.10420e-03 +1.70500 0.00500 0.00500 1.08600e-02 1.01894e-03 1.01894e-03 +1.71500 0.00500 0.00500 8.15300e-03 9.20246e-04 9.20246e-04 +1.72500 0.00500 0.00500 5.57700e-03 7.35926e-04 7.35926e-04 +1.73500 0.00500 0.00500 3.51700e-03 5.28201e-04 5.28201e-04 +1.74500 0.00500 0.00500 2.07700e-03 3.45843e-04 3.45843e-04 +1.75500 0.00500 0.00500 8.89000e-04 1.60333e-04 1.60333e-04 +1.76500 0.00500 0.00500 1.72100e-04 3.29419e-05 3.29419e-05 +1.77500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +1.78500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +1.79500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2010_I841618/d02-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2010_I841618/d02-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.77500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +0.78500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +0.79500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +0.80500 0.00500 0.00500 4.59800e-05 6.45127e-06 6.45127e-06 +0.81500 0.00500 0.00500 4.58900e-05 6.38167e-06 6.38167e-06 +0.82500 0.00500 0.00500 2.28900e-04 3.14772e-05 3.14772e-05 +0.83500 0.00500 0.00500 2.28200e-04 3.09609e-05 3.09609e-05 +0.84500 0.00500 0.00500 3.18400e-04 4.24981e-05 4.24981e-05 +0.85500 0.00500 0.00500 1.04200e-03 1.36451e-04 1.36451e-04 +0.86500 0.00500 0.00500 1.03800e-03 1.32883e-04 1.32883e-04 +0.87500 0.00500 0.00500 2.20000e-03 2.74708e-04 2.74708e-04 +0.88500 0.00500 0.00500 4.91100e-03 5.95935e-04 5.95935e-04 +0.89500 0.00500 0.00500 5.32500e-03 6.25362e-04 6.25362e-04 +0.90500 0.00500 0.00500 7.22900e-03 8.17987e-04 8.17987e-04 +0.91500 0.00500 0.00500 8.18300e-03 8.87632e-04 8.87632e-04 +0.92500 0.00500 0.00500 8.81300e-03 9.11037e-04 9.11037e-04 +0.93500 0.00500 0.00500 1.11500e-02 1.09117e-03 1.09117e-03 +0.94500 0.00500 0.00500 1.31700e-02 1.21288e-03 1.21288e-03 +0.95500 0.00500 0.00500 1.76800e-02 1.51963e-03 1.51963e-03 +0.96500 0.00500 0.00500 2.31600e-02 1.84609e-03 1.84609e-03 +0.97500 0.00500 0.00500 3.23600e-02 2.37628e-03 2.37628e-03 +0.98500 0.00500 0.00500 4.54800e-02 3.05629e-03 3.05629e-03 +0.99500 0.00500 0.00500 6.10000e-02 3.72635e-03 3.72635e-03 +1.00500 0.00500 0.00500 8.31100e-02 4.58684e-03 4.58684e-03 +1.01500 0.00500 0.00500 1.24900e-01 6.19240e-03 6.19240e-03 +1.02500 0.00500 0.00500 1.86900e-01 8.27170e-03 8.27170e-03 +1.03500 0.00500 0.00500 2.79700e-01 1.09680e-02 1.09680e-02 +1.04500 0.00500 0.00500 3.72400e-01 1.28409e-02 1.28409e-02 +1.05500 0.00500 0.00500 4.71400e-01 1.42167e-02 1.42167e-02 +1.06500 0.00500 0.00500 5.85400e-01 1.54081e-02 1.54081e-02 +1.07500 0.00500 0.00500 7.03500e-01 1.61955e-02 1.61955e-02 +1.08500 0.00500 0.00500 8.08600e-01 1.64397e-02 1.64397e-02 +1.09500 0.00500 0.00500 9.24400e-01 1.70127e-02 1.70127e-02 +1.10500 0.00500 0.00500 1.02400e+00 1.77558e-02 1.77558e-02 +1.11500 0.00500 0.00500 1.13600e+00 1.92642e-02 1.92642e-02 +1.12500 0.00500 0.00500 1.24300e+00 2.09942e-02 2.09942e-02 +1.13500 0.00500 0.00500 1.36200e+00 2.29395e-02 2.29395e-02 +1.14500 0.00500 0.00500 1.48000e+00 2.48506e-02 2.48506e-02 +1.15500 0.00500 0.00500 1.59100e+00 2.66593e-02 2.66593e-02 +1.16500 0.00500 0.00500 1.73300e+00 2.90454e-02 2.90454e-02 +1.17500 0.00500 0.00500 1.85100e+00 3.12191e-02 3.12191e-02 +1.18500 0.00500 0.00500 2.00000e+00 3.40032e-02 3.40032e-02 +1.19500 0.00500 0.00500 2.16500e+00 3.62841e-02 3.62841e-02 +1.20500 0.00500 0.00500 2.32600e+00 3.61531e-02 3.61531e-02 +1.21500 0.00500 0.00500 2.52600e+00 3.46598e-02 3.46598e-02 +1.22500 0.00500 0.00500 2.72600e+00 3.65415e-02 3.65415e-02 +1.23500 0.00500 0.00500 2.95500e+00 4.88702e-02 4.88702e-02 +1.24500 0.00500 0.00500 3.20800e+00 6.72746e-02 6.72746e-02 +1.25500 0.00500 0.00500 3.39700e+00 7.76767e-02 7.76767e-02 +1.26500 0.00500 0.00500 3.47000e+00 7.01283e-02 7.01283e-02 +1.27500 0.00500 0.00500 3.35000e+00 5.25232e-02 5.25232e-02 +1.28500 0.00500 0.00500 3.08800e+00 4.37627e-02 4.37627e-02 +1.29500 0.00500 0.00500 2.78000e+00 5.68059e-02 5.68059e-02 +1.30500 0.00500 0.00500 2.53600e+00 7.54969e-02 7.54969e-02 +1.31500 0.00500 0.00500 2.37100e+00 8.67786e-02 8.67786e-02 +1.32500 0.00500 0.00500 2.27400e+00 8.86502e-02 8.86502e-02 +1.33500 0.00500 0.00500 2.25900e+00 8.13340e-02 8.13340e-02 +1.34500 0.00500 0.00500 2.27100e+00 6.75006e-02 6.75006e-02 +1.35500 0.00500 0.00500 2.28800e+00 5.33424e-02 5.33424e-02 +1.36500 0.00500 0.00500 2.30100e+00 4.56854e-02 4.56854e-02 +1.37500 0.00500 0.00500 2.29500e+00 4.71304e-02 4.71304e-02 +1.38500 0.00500 0.00500 2.27000e+00 5.12284e-02 5.12284e-02 +1.39500 0.00500 0.00500 2.20300e+00 5.22551e-02 5.22551e-02 +1.40500 0.00500 0.00500 2.11500e+00 5.08797e-02 5.08797e-02 +1.41500 0.00500 0.00500 2.01200e+00 4.78818e-02 4.78818e-02 +1.42500 0.00500 0.00500 1.87100e+00 4.33674e-02 4.33674e-02 +1.43500 0.00500 0.00500 1.74300e+00 3.97278e-02 3.97278e-02 +1.44500 0.00500 0.00500 1.62300e+00 3.78275e-02 3.78275e-02 +1.45500 0.00500 0.00500 1.50900e+00 3.75841e-02 3.75841e-02 +1.46500 0.00500 0.00500 1.39400e+00 3.80702e-02 3.80702e-02 +1.47500 0.00500 0.00500 1.29600e+00 3.92849e-02 3.92849e-02 +1.48500 0.00500 0.00500 1.20700e+00 4.05195e-02 4.05195e-02 +1.49500 0.00500 0.00500 1.11900e+00 4.09933e-02 4.09933e-02 +1.50500 0.00500 0.00500 1.03900e+00 4.06999e-02 4.06999e-02 +1.51500 0.00500 0.00500 9.76300e-01 3.98592e-02 3.98592e-02 +1.52500 0.00500 0.00500 9.00100e-01 3.72654e-02 3.72654e-02 +1.53500 0.00500 0.00500 8.52200e-01 3.53140e-02 3.53140e-02 +1.54500 0.00500 0.00500 7.99100e-01 3.34783e-02 3.34783e-02 +1.55500 0.00500 0.00500 7.42600e-01 3.24306e-02 3.24306e-02 +1.56500 0.00500 0.00500 6.85400e-01 3.23406e-02 3.23406e-02 +1.57500 0.00500 0.00500 6.37600e-01 3.34387e-02 3.34387e-02 +1.58500 0.00500 0.00500 5.77500e-01 3.41325e-02 3.41325e-02 +1.59500 0.00500 0.00500 5.28700e-01 3.52686e-02 3.52686e-02 +1.60500 0.00500 0.00500 4.84800e-01 3.62737e-02 3.62737e-02 +1.61500 0.00500 0.00500 4.31200e-01 3.58758e-02 3.58758e-02 +1.62500 0.00500 0.00500 3.85700e-01 3.52966e-02 3.52966e-02 +1.63500 0.00500 0.00500 3.33000e-01 3.32029e-02 3.32029e-02 +1.64500 0.00500 0.00500 2.95200e-01 3.17531e-02 3.17531e-02 +1.65500 0.00500 0.00500 2.69100e-01 3.09780e-02 3.09780e-02 +1.66500 0.00500 0.00500 2.13400e-01 2.60741e-02 2.60741e-02 +1.67500 0.00500 0.00500 1.77800e-01 2.28881e-02 2.28881e-02 +1.68500 0.00500 0.00500 1.42100e-01 1.91240e-02 1.91240e-02 +1.69500 0.00500 0.00500 1.17100e-01 1.63896e-02 1.63896e-02 +1.70500 0.00500 0.00500 9.08700e-02 1.31441e-02 1.31441e-02 +1.71500 0.00500 0.00500 7.04600e-02 1.04889e-02 1.04889e-02 +1.72500 0.00500 0.00500 4.51700e-02 6.88498e-03 6.88498e-03 +1.73500 0.00500 0.00500 3.00500e-02 4.67043e-03 4.67043e-03 +1.74500 0.00500 0.00500 1.50000e-02 2.37014e-03 2.37014e-03 +1.75500 0.00500 0.00500 7.74500e-03 1.23996e-03 1.23996e-03 +1.76500 0.00500 0.00500 1.30300e-03 2.10680e-04 2.10680e-04 +1.77500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +1.78500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +1.79500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2010_I841618/d03-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2010_I841618/d03-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.12500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +1.13500 0.00500 0.00500 4.43500e-05 1.49376e-05 1.49376e-05 +1.14500 0.00500 0.00500 1.91200e-04 6.39112e-05 6.39112e-05 +1.15500 0.00500 0.00500 5.98000e-04 1.97689e-04 1.97689e-04 +1.16500 0.00500 0.00500 1.54400e-03 5.02576e-04 5.02576e-04 +1.17500 0.00500 0.00500 2.91800e-03 9.30992e-04 9.30992e-04 +1.18500 0.00500 0.00500 5.05300e-03 1.57229e-03 1.57229e-03 +1.19500 0.00500 0.00500 8.15300e-03 2.45887e-03 2.45887e-03 +1.20500 0.00500 0.00500 1.23100e-02 3.57115e-03 3.57115e-03 +1.21500 0.00500 0.00500 1.71700e-02 4.75442e-03 4.75442e-03 +1.22500 0.00500 0.00500 2.34100e-02 6.12272e-03 6.12272e-03 +1.23500 0.00500 0.00500 3.09000e-02 7.54527e-03 7.54527e-03 +1.24500 0.00500 0.00500 3.94200e-02 8.88927e-03 8.88927e-03 +1.25500 0.00500 0.00500 5.17300e-02 1.06325e-02 1.06325e-02 +1.26500 0.00500 0.00500 6.27500e-02 1.15785e-02 1.15785e-02 +1.27500 0.00500 0.00500 7.82200e-02 1.27184e-02 1.27184e-02 +1.28500 0.00500 0.00500 9.39600e-02 1.31559e-02 1.31559e-02 +1.29500 0.00500 0.00500 1.14400e-01 1.33214e-02 1.33214e-02 +1.30500 0.00500 0.00500 1.38300e-01 1.28048e-02 1.28048e-02 +1.31500 0.00500 0.00500 1.70400e-01 1.20002e-02 1.20002e-02 +1.32500 0.00500 0.00500 2.10900e-01 1.15303e-02 1.15303e-02 +1.33500 0.00500 0.00500 2.63800e-01 1.32335e-02 1.32335e-02 +1.34500 0.00500 0.00500 3.41800e-01 1.84700e-02 1.84700e-02 +1.35500 0.00500 0.00500 4.49500e-01 2.57335e-02 2.57335e-02 +1.36500 0.00500 0.00500 6.32400e-01 3.39619e-02 3.39619e-02 +1.37500 0.00500 0.00500 9.13800e-01 3.96600e-02 3.96600e-02 +1.38500 0.00500 0.00500 1.32400e+00 4.01032e-02 4.01032e-02 +1.39500 0.00500 0.00500 1.77800e+00 3.67327e-02 3.67327e-02 +1.40500 0.00500 0.00500 2.26100e+00 4.51209e-02 4.51209e-02 +1.41500 0.00500 0.00500 2.74600e+00 6.04090e-02 6.04090e-02 +1.42500 0.00500 0.00500 3.19600e+00 7.08201e-02 7.08201e-02 +1.43500 0.00500 0.00500 3.58400e+00 7.28556e-02 7.28556e-02 +1.44500 0.00500 0.00500 3.90200e+00 7.01416e-02 7.01416e-02 +1.45500 0.00500 0.00500 4.14900e+00 6.84391e-02 6.84391e-02 +1.46500 0.00500 0.00500 4.33800e+00 7.23487e-02 7.23487e-02 +1.47500 0.00500 0.00500 4.45700e+00 7.72827e-02 7.72827e-02 +1.48500 0.00500 0.00500 4.52500e+00 8.22589e-02 8.22589e-02 +1.49500 0.00500 0.00500 4.53800e+00 8.60984e-02 8.60984e-02 +1.50500 0.00500 0.00500 4.52600e+00 8.58079e-02 8.58079e-02 +1.51500 0.00500 0.00500 4.47700e+00 8.00884e-02 8.00884e-02 +1.52500 0.00500 0.00500 4.36800e+00 7.37307e-02 7.37307e-02 +1.53500 0.00500 0.00500 4.26100e+00 7.03195e-02 7.03195e-02 +1.54500 0.00500 0.00500 4.09900e+00 6.97423e-02 6.97423e-02 +1.55500 0.00500 0.00500 3.88800e+00 7.12950e-02 7.12950e-02 +1.56500 0.00500 0.00500 3.65800e+00 7.39229e-02 7.39229e-02 +1.57500 0.00500 0.00500 3.39900e+00 7.59900e-02 7.59900e-02 +1.58500 0.00500 0.00500 3.14500e+00 7.78794e-02 7.78794e-02 +1.59500 0.00500 0.00500 2.83800e+00 7.75612e-02 7.75612e-02 +1.60500 0.00500 0.00500 2.54700e+00 7.63901e-02 7.63901e-02 +1.61500 0.00500 0.00500 2.25500e+00 7.39768e-02 7.39768e-02 +1.62500 0.00500 0.00500 1.99800e+00 7.15300e-02 7.15300e-02 +1.63500 0.00500 0.00500 1.75400e+00 6.79003e-02 6.79003e-02 +1.64500 0.00500 0.00500 1.50700e+00 6.26924e-02 6.26924e-02 +1.65500 0.00500 0.00500 1.29600e+00 5.80050e-02 5.80050e-02 +1.66500 0.00500 0.00500 1.10300e+00 5.33428e-02 5.33428e-02 +1.67500 0.00500 0.00500 9.45200e-01 4.96375e-02 4.96375e-02 +1.68500 0.00500 0.00500 8.11400e-01 4.63603e-02 4.63603e-02 +1.69500 0.00500 0.00500 6.85000e-01 4.24662e-02 4.24662e-02 +1.70500 0.00500 0.00500 5.73800e-01 3.83589e-02 3.83589e-02 +1.71500 0.00500 0.00500 4.80900e-01 3.43412e-02 3.43412e-02 +1.72500 0.00500 0.00500 3.78700e-01 2.85967e-02 2.85967e-02 +1.73500 0.00500 0.00500 2.71700e-01 2.14996e-02 2.14996e-02 +1.74500 0.00500 0.00500 1.71600e-01 1.41094e-02 1.41094e-02 +1.75500 0.00500 0.00500 8.27700e-02 7.01701e-03 7.01701e-03 +1.76500 0.00500 0.00500 1.56700e-02 1.36061e-03 1.36061e-03 +1.77500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +1.78500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +1.79500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2010_I841618/d04-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2010_I841618/d04-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.48500 0.00500 0.00500 2.15300e-02 3.05341e-03 3.05341e-03 +1.49500 0.00500 0.00500 1.83800e-01 2.58436e-02 2.58436e-02 +1.50500 0.00500 0.00500 8.12700e-01 1.12250e-01 1.12250e-01 +1.51500 0.00500 0.00500 1.52800e+00 2.05463e-01 2.05463e-01 +1.52500 0.00500 0.00500 2.88800e+00 3.73661e-01 3.73661e-01 +1.53500 0.00500 0.00500 3.58500e+00 4.40864e-01 4.40864e-01 +1.54500 0.00500 0.00500 5.02000e+00 5.78170e-01 5.78170e-01 +1.55500 0.00500 0.00500 5.25700e+00 5.58129e-01 5.58129e-01 +1.56500 0.00500 0.00500 6.15800e+00 5.92585e-01 5.92585e-01 +1.57500 0.00500 0.00500 6.09100e+00 5.24612e-01 5.24612e-01 +1.58500 0.00500 0.00500 7.45200e+00 5.72648e-01 5.72648e-01 +1.59500 0.00500 0.00500 7.08000e+00 4.95929e-01 4.95929e-01 +1.60500 0.00500 0.00500 6.75300e+00 4.57297e-01 4.57297e-01 +1.61500 0.00500 0.00500 6.80800e+00 4.85206e-01 4.85206e-01 +1.62500 0.00500 0.00500 6.79000e+00 5.46123e-01 5.46123e-01 +1.63500 0.00500 0.00500 5.54800e+00 5.19924e-01 5.19924e-01 +1.64500 0.00500 0.00500 4.96700e+00 5.48267e-01 5.48267e-01 +1.65500 0.00500 0.00500 4.94000e+00 6.43780e-01 6.43780e-01 +1.66500 0.00500 0.00500 4.10200e+00 6.32126e-01 6.32126e-01 +1.67500 0.00500 0.00500 3.38100e+00 6.16767e-01 6.16767e-01 +1.68500 0.00500 0.00500 2.75700e+00 5.94978e-01 5.94978e-01 +1.69500 0.00500 0.00500 2.35100e+00 5.97622e-01 5.97622e-01 +1.70500 0.00500 0.00500 1.82500e+00 5.44315e-01 5.44315e-01 +1.71500 0.00500 0.00500 1.52300e+00 5.31133e-01 5.31133e-01 +1.72500 0.00500 0.00500 1.01500e+00 4.10732e-01 4.10732e-01 +1.73500 0.00500 0.00500 5.79800e-01 2.69949e-01 2.69949e-01 +1.74500 0.00500 0.00500 3.57700e-01 1.89348e-01 1.89348e-01 +1.75500 0.00500 0.00500 1.65200e-01 9.79094e-02 9.79094e-02 +1.76500 0.00500 0.00500 5.77800e-02 3.76844e-02 3.76844e-02 +1.77500 0.00500 0.00500 2.47800e-03 1.74184e-03 1.74184e-03 +1.78500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +1.79500 0.00500 0.00500 0.00000e+00 0.00000e+00 0.00000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/BELLE_2011_I878990.cc b/analyses/pluginBELLE/BELLE_2011_I878990.cc rename from analyses/pluginMisc/BELLE_2011_I878990.cc rename to analyses/pluginBELLE/BELLE_2011_I878990.cc diff --git a/analyses/pluginMisc/BELLE_2011_I878990.info b/analyses/pluginBELLE/BELLE_2011_I878990.info rename from analyses/pluginMisc/BELLE_2011_I878990.info rename to analyses/pluginBELLE/BELLE_2011_I878990.info diff --git a/analyses/pluginMisc/BELLE_2011_I878990.plot b/analyses/pluginBELLE/BELLE_2011_I878990.plot rename from analyses/pluginMisc/BELLE_2011_I878990.plot rename to analyses/pluginBELLE/BELLE_2011_I878990.plot diff --git a/analyses/pluginMisc/BELLE_2011_I878990.yoda b/analyses/pluginBELLE/BELLE_2011_I878990.yoda rename from analyses/pluginMisc/BELLE_2011_I878990.yoda rename to analyses/pluginBELLE/BELLE_2011_I878990.yoda diff --git a/analyses/pluginMisc/BELLE_2013_I1216515.cc b/analyses/pluginBELLE/BELLE_2013_I1216515.cc rename from analyses/pluginMisc/BELLE_2013_I1216515.cc rename to analyses/pluginBELLE/BELLE_2013_I1216515.cc diff --git a/analyses/pluginMisc/BELLE_2013_I1216515.info b/analyses/pluginBELLE/BELLE_2013_I1216515.info rename from analyses/pluginMisc/BELLE_2013_I1216515.info rename to analyses/pluginBELLE/BELLE_2013_I1216515.info diff --git a/analyses/pluginMisc/BELLE_2013_I1216515.plot b/analyses/pluginBELLE/BELLE_2013_I1216515.plot rename from analyses/pluginMisc/BELLE_2013_I1216515.plot rename to analyses/pluginBELLE/BELLE_2013_I1216515.plot diff --git a/analyses/pluginBELLE/BELLE_2013_I1216515.yoda b/analyses/pluginBELLE/BELLE_2013_I1216515.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2013_I1216515.yoda @@ -0,0 +1,178 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2013_I1216515/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -7000.0, up: 7000.0}, sys: {dn: -384400.0, up: 384600.0}, 'sys,normalization uncertainty': {dn: -285290.6, up: 285290.6}}, 1: {stat: {dn: -6600.0, up: 6600.0}, sys: {dn: -356000.0, up: 356200.0}, 'sys,normalization uncertainty': {dn: -256544.4, up: 256544.4}}, 2: {stat: {dn: -6300.0, up: 6300.0}, sys: {dn: -331700.0, up: 331800.0}, 'sys,normalization uncertainty': {dn: -231130.19999999998, up: 231130.19999999998}}, 3: {stat: {dn: -5900.0, up: 5900.0}, sys: {dn: -296300.0, up: 296400.0}, 'sys,normalization uncertainty': {dn: -208304.59999999998, up: 208304.59999999998}}, 4: {stat: {dn: -5600.0, up: 5600.0}, sys: {dn: -276800.0, up: 276900.0}, 'sys,normalization uncertainty': {dn: -188209.0, up: 188209.0}}, 5: {stat: {dn: -5400.0, up: 5400.0}, sys: {dn: -256900.0, up: 257000.0}, 'sys,normalization uncertainty': {dn: -170710.4, up: 170710.4}}, 6: {stat: {dn: -5100.0, up: 5100.0}, sys: {dn: -242700.0, up: 242800.0}, 'sys,normalization uncertainty': {dn: -155131.19999999998, up: 155131.19999999998}}, 7: {stat: {dn: -4900.0, up: 4900.0}, sys: {dn: -222800.0, up: 222900.0}, 'sys,normalization uncertainty': {dn: -141169.0, up: 141169.0}}, 8: {stat: {dn: -4600.0, up: 4600.0}, sys: {dn: -207000.0, up: 207100.0}, 'sys,normalization uncertainty': {dn: -128503.2, up: 128503.2}}, 9: {stat: {dn: -4400.0, up: 4400.0}, sys: {dn: -190600.0, up: 190600.0}, 'sys,normalization uncertainty': {dn: -117125.4, up: 117125.4}}, 10: {stat: {dn: -4200.0, up: 4200.0}, sys: {dn: -187600.0, up: 187600.0}, 'sys,normalization uncertainty': {dn: -106954.4, up: 106954.4}}, 11: {stat: {dn: -4000.0, up: 4000.0}, sys: {dn: -177400.0, up: 177400.0}, 'sys,normalization uncertainty': {dn: -97850.2, up: 97850.2}}, 12: {stat: {dn: -3800.0, up: 3800.0}, sys: {dn: -165100.0, up: 165200.0}, 'sys,normalization uncertainty': {dn: -89628.0, up: 89628.0}}, 13: {stat: {dn: -3700.0, up: 3700.0}, sys: {dn: -155300.0, up: 155300.0}, 'sys,normalization uncertainty': {dn: -82047.0, up: 82047.0}}, 14: {stat: {dn: -3500.0, up: 3500.0}, sys: {dn: -149200.0, up: 149300.0}, 'sys,normalization uncertainty': {dn: -75201.0, up: 75201.0}}, 15: {stat: {dn: -3400.0, up: 3400.0}, sys: {dn: -133900.0, up: 134000.0}, 'sys,normalization uncertainty': {dn: -68943.0, up: 68943.0}}, 16: {stat: {dn: -3200.0, up: 3200.0}, sys: {dn: -124100.0, up: 124200.0}, 'sys,normalization uncertainty': {dn: -63317.799999999996, up: 63317.799999999996}}, 17: {stat: {dn: -3100.0, up: 3100.0}, sys: {dn: -117700.0, up: 117700.0}, 'sys,normalization uncertainty': {dn: -58118.2, up: 58118.2}}, 18: {stat: {dn: -2900.0, up: 2900.0}, sys: {dn: -108600.0, up: 108700.0}, 'sys,normalization uncertainty': {dn: -53389.0, up: 53389.0}}, 19: {stat: {dn: -2800.0, up: 2800.0}, sys: {dn: -104100.0, up: 104200.0}, 'sys,normalization uncertainty': {dn: -49060.2, up: 49060.2}}, 20: {stat: {dn: -2700.0, up: 2700.0}, sys: {dn: -95500.0, up: 95600.0}, 'sys,normalization uncertainty': {dn: -45144.399999999994, up: 45144.399999999994}}, 21: {stat: {dn: -2600.0, up: 2600.0}, sys: {dn: -89500.0, up: 89500.0}, 'sys,normalization uncertainty': {dn: -41601.0, up: 41601.0}}, 22: {stat: {dn: -2500.0, up: 2500.0}, sys: {dn: -83900.0, up: 84000.0}, 'sys,normalization uncertainty': {dn: -38336.2, up: 38336.2}}, 23: {stat: {dn: -2400.0, up: 2400.0}, sys: {dn: -79400.0, up: 79400.0}, 'sys,normalization uncertainty': {dn: -35414.399999999994, up: 35414.399999999994}}, 24: {stat: {dn: -2300.0, up: 2300.0}, sys: {dn: -76500.0, up: 76500.0}, 'sys,normalization uncertainty': {dn: -32729.199999999997, up: 32729.199999999997}}, 25: {stat: {dn: -2200.0, up: 2200.0}, sys: {dn: -68300.0, up: 68300.0}, 'sys,normalization uncertainty': {dn: -30209.199999999997, up: 30209.199999999997}}, 26: {stat: {dn: -2100.0, up: 2100.0}, sys: {dn: -65500.0, up: 65500.0}, 'sys,normalization uncertainty': {dn: -27958.0, up: 27958.0}}, 27: {stat: {dn: -2000.0, up: 2000.0}, sys: {dn: -57800.0, up: 57800.0}, 'sys,normalization uncertainty': {dn: -25804.8, up: 25804.8}}, 28: {stat: {dn: -2000.0, up: 2000.0}, sys: {dn: -57800.0, up: 57800.0}, 'sys,normalization uncertainty': {dn: -23906.399999999998, up: 23906.399999999998}}, 29: {stat: {dn: -1900.0, up: 1900.0}, sys: {dn: -53100.0, up: 53100.0}, 'sys,normalization uncertainty': {dn: -22143.8, up: 22143.8}}, 30: {stat: {dn: -1800.0, up: 1800.0}, sys: {dn: -49200.0, up: 49200.0}, 'sys,normalization uncertainty': {dn: -20507.199999999997, up: 20507.199999999997}}, 31: {stat: {dn: -1700.0, up: 1700.0}, sys: {dn: -47800.0, up: 47800.0}, 'sys,normalization uncertainty': {dn: -18995.199999999997, up: 18995.199999999997}}, 32: {stat: {dn: -1700.0, up: 1700.0}, sys: {dn: -44100.0, up: 44100.0}, 'sys,normalization uncertainty': {dn: -17591.0, up: 17591.0}}, 33: {stat: {dn: -1600.0, up: 1600.0}, sys: {dn: -40800.0, up: 40800.0}, 'sys,normalization uncertainty': {dn: -16281.999999999998, up: 16281.999999999998}}, 34: {stat: {dn: -1600.0, up: 1600.0}, sys: {dn: -39400.0, up: 39400.0}, 'sys,normalization uncertainty': {dn: -15100.4, up: 15100.4}}, 35: {stat: {dn: -1500.0, up: 1500.0}, sys: {dn: -38800.0, up: 38800.0}, 'sys,normalization uncertainty': {dn: -14014.0, up: 14014.0}}, 36: {stat: {dn: -1400.0, up: 1400.0}, sys: {dn: -35400.0, up: 35400.0}, 'sys,normalization uncertainty': {dn: -12982.199999999999, up: 12982.199999999999}}, 37: {stat: {dn: -1400.0, up: 1400.0}, sys: {dn: -32800.0, up: 32800.0}, 'sys,normalization uncertainty': {dn: -12037.199999999999, up: 12037.199999999999}}, 38: {stat: {dn: -1300.0, up: 1300.0}, sys: {dn: -32600.0, up: 32600.0}, 'sys,normalization uncertainty': {dn: -11162.199999999999, up: 11162.199999999999}}, 39: {stat: {dn: -1300.0, up: 1300.0}, sys: {dn: -29500.0, up: 29500.0}, 'sys,normalization uncertainty': {dn: -10367.0, up: 10367.0}}, 40: {stat: {dn: -1200.0, up: 1200.0}, sys: {dn: -27800.0, up: 27800.0}, 'sys,normalization uncertainty': {dn: -9620.8, up: 9620.8}}, 41: {stat: {dn: -1200.0, up: 1200.0}, sys: {dn: -26800.0, up: 26900.0}, 'sys,normalization uncertainty': {dn: -8926.4, up: 8926.4}}, 42: {stat: {dn: -1200.0, up: 1200.0}, sys: {dn: -24000.0, up: 24000.0}, 'sys,normalization uncertainty': {dn: -8310.4, up: 8310.4}}, 43: {stat: {dn: -1100.0, up: 1100.0}, sys: {dn: -23700.0, up: 23700.0}, 'sys,normalization uncertainty': {dn: -7716.799999999999, up: 7716.799999999999}}, 44: {stat: {dn: -1100.0, up: 1100.0}, sys: {dn: -21600.0, up: 21700.0}, 'sys,normalization uncertainty': {dn: -7163.799999999999, up: 7163.799999999999}}, 45: {stat: {dn: -1000.0, up: 1000.0}, sys: {dn: -19600.0, up: 19600.0}, 'sys,normalization uncertainty': {dn: -6631.799999999999, up: 6631.799999999999}}, 46: {stat: {dn: -1000.0, up: 1000.0}, sys: {dn: -20200.0, up: 20300.0}, 'sys,normalization uncertainty': {dn: -6181.0, up: 6181.0}}, 47: {stat: {dn: -970.0, up: 970.0}, sys: 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uncertainty': {dn: -1841.6999999999998, up: 1841.6999999999998}}, 62: {stat: {dn: -570.0, up: 570.0}, sys: {dn: -8810.0, up: 8860.0}, 'sys,normalization uncertainty': {dn: -1674.68, up: 1674.68}}, 63: {stat: {dn: -540.0, up: 540.0}, sys: {dn: -10500.0, up: 10530.0}, 'sys,normalization uncertainty': {dn: -1515.2199999999998, up: 1515.2199999999998}}, 64: {stat: {dn: -520.0, up: 520.0}, sys: {dn: -8060.0, up: 8090.0}, 'sys,normalization uncertainty': {dn: -1354.08, up: 1354.08}}, 65: {stat: {dn: -490.0, up: 490.0}, sys: {dn: -8270.0, up: 8290.0}, 'sys,normalization uncertainty': {dn: -1205.26, up: 1205.26}}, 66: {stat: {dn: -470.0, up: 470.0}, sys: {dn: -7900.0, up: 7910.0}, 'sys,normalization uncertainty': {dn: -1065.9599999999998, up: 1065.9599999999998}}, 67: {stat: {dn: -450.0, up: 450.0}, sys: {dn: -7260.0, up: 7260.0}, 'sys,normalization uncertainty': {dn: -943.3199999999998, up: 943.3199999999998}}, 68: {stat: {dn: -420.0, up: 420.0}, sys: {dn: -6960.0, up: 6960.0}, 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5.000000e-03 4.915000e+04 7.750463e+03 7.740516e+03 +9.050000e-01 5.000000e-03 5.000000e-03 4.200000e+04 6.417713e+03 6.407772e+03 +9.150000e-01 5.000000e-03 5.000000e-03 3.497000e+04 5.046017e+03 5.026160e+03 +9.250000e-01 5.000000e-03 5.000000e-03 2.946000e+04 6.182605e+03 6.162679e+03 +9.350000e-01 5.000000e-03 5.000000e-03 2.470000e+04 4.842972e+03 4.823067e+03 +9.450000e-01 5.000000e-03 5.000000e-03 1.915000e+04 5.434370e+03 5.414423e+03 +9.550000e-01 5.000000e-03 5.000000e-03 1.376000e+04 3.775329e+03 3.755411e+03 +9.650000e-01 5.000000e-03 5.000000e-03 9.910000e+03 4.940471e+03 4.920513e+03 +9.750000e-01 5.000000e-03 5.000000e-03 1.170000e+04 6.504524e+03 6.454714e+03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2013_I1216515/d01-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -4000.0, up: 4000.0}, sys: {dn: -143200.0, up: 143100.0}, 'sys,normalization uncertainty': {dn: -89233.2, up: 89233.2}}, 1: {stat: {dn: -3900.0, up: 3900.0}, sys: {dn: -139700.0, 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{dn: -51224.6, up: 51224.6}}, 9: {stat: {dn: -2900.0, up: 2900.0}, sys: {dn: -90600.0, up: 90700.0}, 'sys,normalization uncertainty': {dn: -47544.0, up: 47544.0}}, 10: {stat: {dn: -2700.0, up: 2700.0}, sys: {dn: -85800.0, up: 85900.0}, 'sys,normalization uncertainty': {dn: -44216.2, up: 44216.2}}, 11: {stat: {dn: -2600.0, up: 2600.0}, sys: {dn: -85800.0, up: 85800.0}, 'sys,normalization uncertainty': {dn: -41272.0, up: 41272.0}}, 12: {stat: {dn: -2600.0, up: 2600.0}, sys: {dn: -78500.0, up: 78500.0}, 'sys,normalization uncertainty': {dn: -38530.799999999996, up: 38530.799999999996}}, 13: {stat: {dn: -2500.0, up: 2500.0}, sys: {dn: -75700.0, up: 75800.0}, 'sys,normalization uncertainty': {dn: -35925.399999999994, up: 35925.399999999994}}, 14: {stat: {dn: -2400.0, up: 2400.0}, sys: {dn: -71800.0, up: 71900.0}, 'sys,normalization uncertainty': {dn: -33544.0, up: 33544.0}}, 15: {stat: {dn: -2300.0, up: 2300.0}, sys: {dn: -68800.0, up: 68800.0}, 'sys,normalization uncertainty': {dn: -31344.6, up: 31344.6}}, 16: {stat: {dn: -2200.0, up: 2200.0}, sys: {dn: -64200.0, up: 64300.0}, 'sys,normalization uncertainty': {dn: -29283.8, up: 29283.8}}, 17: {stat: {dn: -2100.0, up: 2100.0}, sys: {dn: -62900.0, up: 62900.0}, 'sys,normalization uncertainty': {dn: -27281.8, up: 27281.8}}, 18: {stat: {dn: -2100.0, up: 2100.0}, sys: {dn: -60300.0, up: 60300.0}, 'sys,normalization uncertainty': {dn: -25405.8, up: 25405.8}}, 19: {stat: {dn: -2000.0, up: 2000.0}, sys: {dn: -56400.0, up: 56400.0}, 'sys,normalization uncertainty': {dn: -23668.399999999998, up: 23668.399999999998}}, 20: {stat: {dn: -1900.0, up: 1900.0}, sys: {dn: -52900.0, up: 53000.0}, 'sys,normalization uncertainty': {dn: -22125.6, up: 22125.6}}, 21: {stat: {dn: -1900.0, up: 1900.0}, sys: {dn: -53000.0, up: 53100.0}, 'sys,normalization uncertainty': {dn: -20722.8, up: 20722.8}}, 22: {stat: {dn: -1800.0, up: 1800.0}, sys: {dn: -51000.0, up: 51000.0}, 'sys,normalization uncertainty': {dn: -19446.0, up: 19446.0}}, 23: {stat: {dn: -1700.0, up: 1700.0}, sys: {dn: -48500.0, up: 48500.0}, 'sys,normalization uncertainty': {dn: -18200.0, up: 18200.0}}, 24: {stat: {dn: -1700.0, up: 1700.0}, sys: {dn: -46500.0, up: 46500.0}, 'sys,normalization uncertainty': {dn: -17003.0, up: 17003.0}}, 25: {stat: {dn: -1600.0, up: 1600.0}, sys: {dn: -44200.0, up: 44200.0}, 'sys,normalization uncertainty': {dn: -15873.199999999999, up: 15873.199999999999}}, 26: {stat: {dn: -1600.0, up: 1600.0}, sys: {dn: -40600.0, up: 40600.0}, 'sys,normalization uncertainty': {dn: -14823.199999999999, up: 14823.199999999999}}, 27: {stat: {dn: -1500.0, up: 1500.0}, sys: {dn: -40100.0, up: 40000.0}, 'sys,normalization uncertainty': {dn: -13804.0, up: 13804.0}}, 28: {stat: {dn: -1500.0, up: 1500.0}, sys: {dn: -37200.0, up: 37100.0}, 'sys,normalization uncertainty': {dn: -12870.199999999999, up: 12870.199999999999}}, 29: {stat: {dn: -1400.0, up: 1400.0}, sys: {dn: -36200.0, up: 36100.0}, 'sys,normalization uncertainty': {dn: -12003.599999999999, up: 12003.599999999999}}, 30: {stat: {dn: -1400.0, up: 1400.0}, sys: {dn: -31900.0, up: 31900.0}, 'sys,normalization uncertainty': {dn: -11198.599999999999, up: 11198.599999999999}}, 31: {stat: {dn: -1300.0, up: 1300.0}, sys: {dn: -31000.0, up: 30900.0}, 'sys,normalization uncertainty': {dn: -10480.4, up: 10480.4}}, 32: {stat: {dn: -1300.0, up: 1300.0}, sys: {dn: -30000.0, up: 29900.0}, 'sys,normalization uncertainty': {dn: -9807.0, up: 9807.0}}, 33: {stat: {dn: -1200.0, up: 1200.0}, sys: {dn: -27300.0, up: 27200.0}, 'sys,normalization uncertainty': {dn: -9185.4, up: 9185.4}}, 34: {stat: {dn: -1200.0, up: 1200.0}, sys: {dn: -25700.0, up: 25600.0}, 'sys,normalization uncertainty': {dn: -8589.0, up: 8589.0}}, 35: {stat: {dn: -1200.0, up: 1200.0}, sys: {dn: -23700.0, up: 23600.0}, 'sys,normalization uncertainty': {dn: -8033.2, up: 8033.2}}, 36: {stat: {dn: -1100.0, up: 1100.0}, sys: {dn: -23000.0, up: 22900.0}, 'sys,normalization uncertainty': {dn: -7489.999999999999, up: 7489.999999999999}}, 37: {stat: {dn: -1100.0, up: 1100.0}, sys: {dn: -20500.0, up: 20400.0}, 'sys,normalization uncertainty': {dn: -6970.599999999999, up: 6970.599999999999}}, 38: {stat: {dn: -1000.0, up: 1000.0}, sys: {dn: -19400.0, up: 19300.0}, 'sys,normalization uncertainty': {dn: -6479.2, up: 6479.2}}, 39: {stat: {dn: -1000.0, up: 1000.0}, sys: {dn: -20700.0, up: 20700.0}, 'sys,normalization uncertainty': {dn: -6028.4, up: 6028.4}}, 40: {stat: {dn: -970.0, up: 970.0}, sys: {dn: -16430.0, up: 16370.0}, 'sys,normalization uncertainty': {dn: -5616.099999999999, up: 5616.099999999999}}, 41: {stat: {dn: -940.0, up: 940.0}, sys: {dn: -15590.0, up: 15540.0}, 'sys,normalization uncertainty': {dn: -5211.78, up: 5211.78}}, 42: {stat: {dn: -910.0, up: 910.0}, sys: {dn: -13600.0, up: 13550.0}, 'sys,normalization uncertainty': {dn: -4843.72, up: 4843.72}}, 43: {stat: {dn: -880.0, up: 880.0}, sys: {dn: -14260.0, up: 14200.0}, 'sys,normalization uncertainty': {dn: -4495.26, up: 4495.26}}, 44: {stat: {dn: -850.0, up: 850.0}, sys: {dn: -13050.0, up: 12940.0}, 'sys,normalization uncertainty': {dn: -4162.9, up: 4162.9}}, 45: {stat: {dn: -810.0, up: 810.0}, sys: {dn: -13410.0, up: 13270.0}, 'sys,normalization uncertainty': {dn: -3846.3599999999997, up: 3846.3599999999997}}, 46: {stat: {dn: -780.0, up: 780.0}, sys: {dn: -13850.0, up: 13660.0}, 'sys,normalization uncertainty': {dn: -3552.92, up: 3552.92}}, 47: {stat: {dn: -760.0, up: 760.0}, sys: {dn: -12190.0, up: 11920.0}, 'sys,normalization uncertainty': {dn: -3285.24, up: 3285.24}}, 48: {stat: {dn: -730.0, up: 730.0}, sys: {dn: -12920.0, up: 12620.0}, 'sys,normalization uncertainty': {dn: -3033.52, up: 3033.52}}, 49: {stat: {dn: -700.0, up: 700.0}, sys: {dn: -11820.0, up: 11450.0}, 'sys,normalization uncertainty': {dn: -2787.12, up: 2787.12}}, 50: {stat: {dn: -680.0, up: 680.0}, sys: {dn: -12710.0, up: 12330.0}, 'sys,normalization uncertainty': {dn: -2578.66, up: 2578.66}}, 51: {stat: {dn: -650.0, up: 650.0}, sys: {dn: -12780.0, up: 12390.0}, 'sys,normalization uncertainty': {dn: -2366.0, up: 2366.0}}, 52: {stat: {dn: -630.0, up: 630.0}, sys: {dn: -11800.0, up: 11370.0}, 'sys,normalization uncertainty': {dn: -2182.3199999999997, up: 2182.3199999999997}}, 53: {stat: {dn: -610.0, up: 610.0}, sys: {dn: -11670.0, up: 11220.0}, 'sys,normalization uncertainty': {dn: -2003.96, up: 2003.96}}, 54: {stat: {dn: -580.0, up: 580.0}, sys: {dn: -11970.0, up: 11550.0}, 'sys,normalization uncertainty': {dn: -1836.66, up: 1836.66}}, 55: {stat: {dn: -560.0, up: 560.0}, sys: {dn: -11360.0, up: 10940.0}, 'sys,normalization uncertainty': {dn: -1678.46, up: 1678.46}}, 56: {stat: {dn: -540.0, up: 540.0}, sys: {dn: -11160.0, up: 10750.0}, 'sys,normalization uncertainty': {dn: -1540.56, up: 1540.56}}, 57: {stat: {dn: -510.0, up: 510.0}, sys: {dn: -10310.0, up: 9890.0}, 'sys,normalization uncertainty': {dn: -1396.2199999999998, up: 1396.2199999999998}}, 58: {stat: {dn: -500.0, up: 500.0}, sys: {dn: -9380.0, up: 8950.0}, 'sys,normalization uncertainty': {dn: -1274.56, up: 1274.56}}, 59: {stat: {dn: -480.0, up: 480.0}, sys: {dn: -9530.0, up: 9140.0}, 'sys,normalization uncertainty': {dn: -1160.18, up: 1160.18}}, 60: {stat: {dn: -460.0, up: 460.0}, sys: {dn: -9240.0, up: 8870.0}, 'sys,normalization uncertainty': {dn: -1047.34, up: 1047.34}}, 61: {stat: {dn: -440.0, up: 440.0}, sys: {dn: -8540.0, up: 8170.0}, 'sys,normalization uncertainty': {dn: -945.56, up: 945.56}}, 62: {stat: {dn: -420.0, up: 420.0}, sys: {dn: -8240.0, up: 7900.0}, 'sys,normalization uncertainty': {dn: -851.1999999999999, up: 851.1999999999999}}, 63: {stat: {dn: -400.0, up: 400.0}, sys: {dn: -7510.0, up: 7160.0}, 'sys,normalization uncertainty': {dn: -760.34, up: 760.34}}, 64: {stat: {dn: -370.0, up: 370.0}, sys: {dn: -7180.0, up: 6870.0}, 'sys,normalization uncertainty': {dn: -663.4599999999999, up: 663.4599999999999}}, 65: {stat: {dn: -360.0, up: 360.0}, sys: {dn: -6980.0, up: 6690.0}, 'sys,normalization uncertainty': {dn: -590.52, up: 590.52}}, 66: {stat: {dn: -340.0, up: 340.0}, sys: {dn: -6490.0, up: 6210.0}, 'sys,normalization uncertainty': {dn: -517.72, up: 517.72}}, 67: {stat: {dn: -320.0, up: 320.0}, sys: {dn: -5970.0, up: 5700.0}, 'sys,normalization uncertainty': {dn: -453.32, up: 453.32}}, 68: {stat: {dn: -310.0, up: 310.0}, sys: {dn: -5390.0, up: 5120.0}, 'sys,normalization uncertainty': {dn: -390.17999999999995, up: 390.17999999999995}}, 69: {stat: {dn: -280.0, up: 280.0}, sys: {dn: -5320.0, up: 5090.0}, 'sys,normalization uncertainty': {dn: -327.59999999999997, up: 327.59999999999997}}, 70: {stat: {dn: -270.0, up: 270.0}, sys: {dn: -4810.0, up: 4590.0}, 'sys,normalization uncertainty': {dn: -280.42, up: 280.42}}, 71: {stat: {dn: -260.0, up: 260.0}, sys: {dn: -4830.0, up: 4620.0}, 'sys,normalization uncertainty': {dn: -237.99999999999997, up: 237.99999999999997}}, 72: {stat: {dn: -240.0, up: 240.0}, sys: {dn: -4220.0, up: 4010.0}, 'sys,normalization uncertainty': {dn: -199.35999999999999, up: 199.35999999999999}}, 73: {stat: {dn: -240.0, up: 240.0}, sys: {dn: -4010.0, up: 3810.0}, 'sys,normalization uncertainty': {dn: -164.5, up: 164.5}}, 74: {stat: {dn: -220.0, up: 220.0}, sys: {dn: -3750.0, up: 3560.0}, 'sys,normalization uncertainty': {dn: -123.33999999999999, up: 123.33999999999999}}, 75: {stat: {dn: -210.0, up: 210.0}, sys: {dn: -3590.0, up: 3400.0}, 'sys,normalization uncertainty': {dn: -89.17999999999999, up: 89.17999999999999}}, 76: {stat: {dn: -220.0, up: 220.0}, sys: {dn: -3690.0, up: 3500.0}, 'sys,normalization uncertainty': {dn: -65.38, up: 65.38}}, 77: {stat: {dn: -440.0, up: 440.0}, sys: {dn: -7720.0, up: 7340.0}, 'sys,normalization uncertainty': {dn: -82.88, up: 82.88}}} + +IsRef: 1 +Path: /REF/BELLE_2013_I1216515/d01-x01-y02 +Title: doi:10.17182/hepdata.62276.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.050000e-01 5.000000e-03 5.000000e-03 6.373800e+06 1.687744e+05 1.686896e+05 +2.150000e-01 5.000000e-03 5.000000e-03 5.981600e+06 1.629236e+05 1.629236e+05 +2.250000e-01 5.000000e-03 5.000000e-03 5.591300e+06 1.501692e+05 1.501692e+05 +2.350000e-01 5.000000e-03 5.000000e-03 5.234300e+06 1.416771e+05 1.416771e+05 +2.450000e-01 5.000000e-03 5.000000e-03 4.906600e+06 1.371016e+05 1.371016e+05 +2.550000e-01 5.000000e-03 5.000000e-03 4.578400e+06 1.330099e+05 1.329224e+05 +2.650000e-01 5.000000e-03 5.000000e-03 4.256800e+06 1.228682e+05 1.227808e+05 +2.750000e-01 5.000000e-03 5.000000e-03 3.947500e+06 1.154362e+05 1.154362e+05 +2.850000e-01 5.000000e-03 5.000000e-03 3.658900e+06 1.045570e+05 1.046442e+05 +2.950000e-01 5.000000e-03 5.000000e-03 3.396000e+06 1.023582e+05 1.024467e+05 +3.050000e-01 5.000000e-03 5.000000e-03 3.158300e+06 9.656087e+04 9.664974e+04 +3.150000e-01 5.000000e-03 5.000000e-03 2.948000e+06 9.524588e+04 9.524588e+04 +3.250000e-01 5.000000e-03 5.000000e-03 2.752200e+06 8.748504e+04 8.748504e+04 +3.350000e-01 5.000000e-03 5.000000e-03 2.566100e+06 8.382944e+04 8.391975e+04 +3.450000e-01 5.000000e-03 5.000000e-03 2.396000e+06 7.928556e+04 7.937613e+04 +3.550000e-01 5.000000e-03 5.000000e-03 2.238900e+06 7.563871e+04 7.563871e+04 +3.650000e-01 5.000000e-03 5.000000e-03 2.091700e+06 7.059760e+04 7.068855e+04 +3.750000e-01 5.000000e-03 5.000000e-03 1.948700e+06 6.859385e+04 6.859385e+04 +3.850000e-01 5.000000e-03 5.000000e-03 1.814700e+06 6.546720e+04 6.546720e+04 +3.950000e-01 5.000000e-03 5.000000e-03 1.690600e+06 6.119766e+04 6.119766e+04 +4.050000e-01 5.000000e-03 5.000000e-03 1.580400e+06 5.737214e+04 5.746436e+04 +4.150000e-01 5.000000e-03 5.000000e-03 1.480200e+06 5.693895e+04 5.703205e+04 +4.250000e-01 5.000000e-03 5.000000e-03 1.389000e+06 5.461123e+04 5.461123e+04 +4.350000e-01 5.000000e-03 5.000000e-03 1.300000e+06 5.183030e+04 5.183030e+04 +4.450000e-01 5.000000e-03 5.000000e-03 1.214500e+06 4.954031e+04 4.954031e+04 +4.550000e-01 5.000000e-03 5.000000e-03 1.133800e+06 4.699105e+04 4.699105e+04 +4.650000e-01 5.000000e-03 5.000000e-03 1.058800e+06 4.325098e+04 4.325098e+04 +4.750000e-01 5.000000e-03 5.000000e-03 9.860000e+05 4.243596e+04 4.234147e+04 +4.850000e-01 5.000000e-03 5.000000e-03 9.193000e+05 3.939203e+04 3.929761e+04 +4.950000e-01 5.000000e-03 5.000000e-03 8.574000e+05 3.816394e+04 3.806910e+04 +5.050000e-01 5.000000e-03 5.000000e-03 7.999000e+05 3.383753e+04 3.383753e+04 +5.150000e-01 5.000000e-03 5.000000e-03 7.486000e+05 3.274949e+04 3.265484e+04 +5.250000e-01 5.000000e-03 5.000000e-03 7.005000e+05 3.158904e+04 3.149408e+04 +5.350000e-01 5.000000e-03 5.000000e-03 6.561000e+05 2.882883e+04 2.873415e+04 +5.450000e-01 5.000000e-03 5.000000e-03 6.135000e+05 2.712381e+04 2.702908e+04 +5.550000e-01 5.000000e-03 5.000000e-03 5.738000e+05 2.505319e+04 2.495861e+04 +5.650000e-01 5.000000e-03 5.000000e-03 5.350000e+05 2.421384e+04 2.411887e+04 +5.750000e-01 5.000000e-03 5.000000e-03 4.979000e+05 2.168062e+04 2.158609e+04 +5.850000e-01 5.000000e-03 5.000000e-03 4.628000e+05 2.047779e+04 2.038308e+04 +5.950000e-01 5.000000e-03 5.000000e-03 4.306000e+05 2.158313e+04 2.158313e+04 +6.050000e-01 5.000000e-03 5.000000e-03 4.011500e+05 1.739041e+04 1.733374e+04 +6.150000e-01 5.000000e-03 5.000000e-03 3.722700e+05 1.646494e+04 1.641761e+04 +6.250000e-01 5.000000e-03 5.000000e-03 3.459800e+05 1.446547e+04 1.441847e+04 +6.350000e-01 5.000000e-03 5.000000e-03 3.210900e+05 1.497763e+04 1.492051e+04 +6.450000e-01 5.000000e-03 5.000000e-03 2.973500e+05 1.372424e+04 1.361969e+04 +6.550000e-01 5.000000e-03 5.000000e-03 2.747400e+05 1.397422e+04 1.383992e+04 +6.650000e-01 5.000000e-03 5.000000e-03 2.537800e+05 1.431971e+04 1.413603e+04 +6.750000e-01 5.000000e-03 5.000000e-03 2.346600e+05 1.264779e+04 1.238777e+04 +6.850000e-01 5.000000e-03 5.000000e-03 2.166800e+05 1.329141e+04 1.299998e+04 +6.950000e-01 5.000000e-03 5.000000e-03 1.990800e+05 1.216431e+04 1.180511e+04 +7.050000e-01 5.000000e-03 5.000000e-03 1.841900e+05 1.298676e+04 1.261510e+04 +7.150000e-01 5.000000e-03 5.000000e-03 1.690000e+05 1.301341e+04 1.263062e+04 +7.250000e-01 5.000000e-03 5.000000e-03 1.558800e+05 1.201663e+04 1.159467e+04 +7.350000e-01 5.000000e-03 5.000000e-03 1.431400e+05 1.185651e+04 1.141387e+04 +7.450000e-01 5.000000e-03 5.000000e-03 1.311900e+05 1.212397e+04 1.170949e+04 +7.550000e-01 5.000000e-03 5.000000e-03 1.198900e+05 1.149697e+04 1.108217e+04 +7.650000e-01 5.000000e-03 5.000000e-03 1.100400e+05 1.127876e+04 1.087324e+04 +7.750000e-01 5.000000e-03 5.000000e-03 9.973000e+04 1.041660e+04 1.000108e+04 +7.850000e-01 5.000000e-03 5.000000e-03 9.104000e+04 9.479394e+03 9.054115e+03 +7.950000e-01 5.000000e-03 5.000000e-03 8.287000e+04 9.612352e+03 9.225834e+03 +8.050000e-01 5.000000e-03 5.000000e-03 7.481000e+04 9.310538e+03 8.943457e+03 +8.150000e-01 5.000000e-03 5.000000e-03 6.754000e+04 8.603446e+03 8.236297e+03 +8.250000e-01 5.000000e-03 5.000000e-03 6.080000e+04 8.294489e+03 7.956817e+03 +8.350000e-01 5.000000e-03 5.000000e-03 5.431000e+04 7.558983e+03 7.211360e+03 +8.450000e-01 5.000000e-03 5.000000e-03 4.739000e+04 7.220075e+03 6.911872e+03 +8.550000e-01 5.000000e-03 5.000000e-03 4.218000e+04 7.014179e+03 6.725653e+03 +8.650000e-01 5.000000e-03 5.000000e-03 3.698000e+04 6.519489e+03 6.240812e+03 +8.750000e-01 5.000000e-03 5.000000e-03 3.238000e+04 5.995732e+03 5.726945e+03 +8.850000e-01 5.000000e-03 5.000000e-03 2.787000e+04 5.412988e+03 5.144195e+03 +8.950000e-01 5.000000e-03 5.000000e-03 2.340000e+04 5.337427e+03 5.108211e+03 +9.050000e-01 5.000000e-03 5.000000e-03 2.003000e+04 4.825726e+03 4.606478e+03 +9.150000e-01 5.000000e-03 5.000000e-03 1.700000e+04 4.842845e+03 4.633427e+03 +9.250000e-01 5.000000e-03 5.000000e-03 1.424000e+04 4.231518e+03 4.022119e+03 +9.350000e-01 5.000000e-03 5.000000e-03 1.175000e+04 4.020542e+03 3.821094e+03 +9.450000e-01 5.000000e-03 5.000000e-03 8.810000e+03 3.758472e+03 3.568923e+03 +9.550000e-01 5.000000e-03 5.000000e-03 6.370000e+03 3.597242e+03 3.407646e+03 +9.650000e-01 5.000000e-03 5.000000e-03 4.670000e+03 3.697131e+03 3.507517e+03 +9.750000e-01 5.000000e-03 5.000000e-03 5.920000e+03 7.732973e+03 7.353643e+03 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2013_I1225975.cc b/analyses/pluginBELLE/BELLE_2013_I1225975.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2013_I1225975.cc @@ -0,0 +1,116 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2013_I1225975 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2013_I1225975); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nJPsi = bookCounter("TMP/jpsi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==443) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // omega pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nJPsi->fill(event.weight()); + break; + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nJPsi->val(); + double error = _nJPsi->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nJPsi; + //@} + + + }; + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2013_I1225975); + +} diff --git a/analyses/pluginBELLE/BELLE_2013_I1225975.info b/analyses/pluginBELLE/BELLE_2013_I1225975.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2013_I1225975.info @@ -0,0 +1,38 @@ +Name: BELLE_2013_I1225975 +Year: 2013 +Summary: Cross section for $e^+e^-\to J/\psi\pi^+\pi^-$ at energies between 3.8 and 4.82 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 1225975 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 110 (2013) 252002, 2013 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to J/\psi\pi^+\pi^-$ at energies between 3.8 and 4.82 GeV using radiative return by BELLE.' +Keywords: [] +BibKey: Liu:2013dau +BibTeX: '%%% contains utf-8, see: http://inspirehep.net/info/faq/general#utf8 +%%% add \usepackage[utf8]{inputenc} to your latex preamble + +@article{Liu:2013dau, + author = "Liu, Z. Q. and others", + title = "{Study of $e^+e^- → π^+ π^- J/ψ$ and Observation of + a Charged Charmoniumlike State at Belle}", + collaboration = "Belle", + journal = "Phys. Rev. Lett.", + volume = "110", + year = "2013", + pages = "252002", + doi = "10.1103/PhysRevLett.110.252002", + eprint = "1304.0121", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-PREPRINT-2013-6, KEK-PREPRINT-2013-2", + SLACcitation = "%%CITATION = ARXIV:1304.0121;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2013_I1225975.plot b/analyses/pluginBELLE/BELLE_2013_I1225975.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2013_I1225975.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BELLE_2013_I1225975/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-J/\psi)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-J/\psi)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2013_I1225975.yoda b/analyses/pluginBELLE/BELLE_2013_I1225975.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2013_I1225975.yoda @@ -0,0 +1,96 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2013_I1225975/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -9.15, up: 9.15}, 'sys,overall uncertainty': {dn: -1.5455999999999999, up: 1.5455999999999999}}, 1: {error: {dn: -7.93, up: 7.93}, 'sys,overall uncertainty': {dn: -0.9961000000000001, up: 0.9961000000000001}}, 2: {error: {dn: -8.05, up: 8.05}, 'sys,overall uncertainty': {dn: -1.1494, up: 1.1494}}, 3: {error: {dn: -8.8, up: 8.8}, 'sys,overall uncertainty': {dn: -2.2995, up: 2.2995}}, 4: {error: {dn: -7.17, up: 7.17}, 'sys,overall uncertainty': {dn: -1.1508, up: 1.1508}}, 5: {error: {dn: -7.11, up: 7.11}, 'sys,overall uncertainty': {dn: -1.2201, up: 1.2201}}, 6: {error: {dn: -7.34, up: 7.34}, 'sys,overall uncertainty': {dn: -1.6814, up: 1.6814}}, 7: {error: {dn: -5.78, up: 5.78}, 'sys,overall uncertainty': {dn: -0.6097000000000001, up: 0.6097000000000001}}, 8: {error: {dn: -8.16, up: 8.16}, 'sys,overall uncertainty': {dn: -1.7836000000000003, up: 1.7836000000000003}}, 9: {error: {dn: -7.16, up: 7.16}, 'sys,overall uncertainty': {dn: -1.4650999999999998, up: 1.4650999999999998}}, 10: {error: {dn: -7.03, up: 7.03}, 'sys,overall uncertainty': {dn: -1.5792, up: 1.5792}}, 11: {error: {dn: -7.89, up: 7.89}, 'sys,overall uncertainty': {dn: -2.0965, up: 2.0965}}, 12: {error: {dn: -6.06, up: 6.06}, 'sys,overall uncertainty': {dn: -0.6265, up: 0.6265}}, 13: {error: {dn: -6.79, up: 6.79}, 'sys,overall uncertainty': {dn: -1.477, up: 1.477}}, 14: {error: {dn: -6.58, up: 6.58}, 'sys,overall uncertainty': {dn: -1.0093999999999999, up: 1.0093999999999999}}, 15: {error: {dn: -6.65, up: 6.65}, 'sys,overall uncertainty': {dn: -1.4707000000000001, up: 1.4707000000000001}}, 16: {error: {dn: -6.45, up: 6.45}, 'sys,overall uncertainty': {dn: -1.022, up: 1.022}}, 17: {error: {dn: -5.83, up: 5.83}, 'sys,overall uncertainty': {dn: -0.46270000000000006, up: 0.46270000000000006}}, 18: {error: {dn: -6.05, up: 6.05}, 'sys,overall uncertainty': {dn: -1.1101999999999999, up: 1.1101999999999999}}, 19: {error: {dn: -6.86, up: 6.86}, 'sys,overall uncertainty': {dn: -1.8088000000000002, up: 1.8088000000000002}}, 20: {error: {dn: -7.78, up: 7.78}, 'sys,overall uncertainty': {dn: -3.2381999999999995, up: 3.2381999999999995}}, 21: {error: {dn: -9.42, up: 9.42}, 'sys,overall uncertainty': {dn: -5.1443, up: 5.1443}}, 22: {error: {dn: -8.98, up: 8.98}, 'sys,overall uncertainty': {dn: -4.2819, up: 4.2819}}, 23: {error: {dn: -8.61, up: 8.61}, 'sys,overall uncertainty': {dn: -4.0733, up: 4.0733}}, 24: {error: {dn: -8.93, up: 8.93}, 'sys,overall uncertainty': {dn: -3.9851, up: 3.9851}}, 25: {error: {dn: -7.4, up: 7.4}, 'sys,overall uncertainty': {dn: -2.7349, up: 2.7349}}, 26: {error: {dn: -7.41, up: 7.41}, 'sys,overall uncertainty': {dn: -2.5605999999999995, up: 2.5605999999999995}}, 27: {error: {dn: -7.44, up: 7.44}, 'sys,overall uncertainty': {dn: -3.0226, up: 3.0226}}, 28: {error: {dn: -6.02, up: 6.02}, 'sys,overall uncertainty': {dn: -1.4784, up: 1.4784}}, 29: {error: {dn: -6.03, up: 6.03}, 'sys,overall uncertainty': {dn: -1.4994000000000003, up: 1.4994000000000003}}, 30: {error: {dn: -5.45, up: 5.45}, 'sys,overall uncertainty': {dn: -1.0409, up: 1.0409}}, 31: {error: {dn: -5.75, up: 5.75}, 'sys,overall uncertainty': {dn: -1.0681999999999998, up: 1.0681999999999998}}, 32: {error: {dn: -4.07, up: 4.07}, 'sys,overall uncertainty': {dn: -0.6076, up: 0.6076}}, 33: {error: {dn: -4.45, up: 4.45}, 'sys,overall uncertainty': {dn: -0.7798, up: 0.7798}}, 34: {error: {dn: -4.53, up: 4.53}, 'sys,overall uncertainty': {dn: -0.6706, up: 0.6706}}, 35: {error: {dn: -4.99, up: 4.99}, 'sys,overall uncertainty': {dn: -0.9541000000000001, up: 0.9541000000000001}}, 36: {error: {dn: -4.41, up: 4.41}, 'sys,overall uncertainty': {dn: -0.4228, up: 0.4228}}, 37: {error: {dn: -4.07, up: 4.07}, 'sys,overall uncertainty': {dn: -0.5131, up: 0.5131}}, 38: {error: {dn: -5.04, up: 5.04}, 'sys,overall uncertainty': {dn: -1.0507, up: 1.0507}}, 39: {error: {dn: -4.23, up: 4.23}, 'sys,overall uncertainty': {dn: -0.42629999999999996, up: 0.42629999999999996}}, 40: {error: {dn: -3.85, up: 3.85}, 'sys,overall uncertainty': {dn: -0.3297, up: 0.3297}}, 41: {error: {dn: -3.93, up: 3.93}, 'sys,overall uncertainty': {dn: -0.45289999999999997, up: 0.45289999999999997}}, 42: {error: {dn: -3.91, up: 3.91}, 'sys,overall uncertainty': {dn: -0.7518, up: 0.7518}}, 43: {error: {dn: -3.84, up: 3.84}, 'sys,overall uncertainty': {dn: -0.2303, up: 0.2303}}, 44: {error: {dn: -3.67, up: 3.67}, 'sys,overall uncertainty': {dn: -0.0, up: 0.0}}, 45: {error: {dn: -3.68, up: 3.68}, 'sys,overall uncertainty': {dn: -0.3808, up: 0.3808}}, 46: {error: {dn: -3.67, up: 3.67}, 'sys,overall uncertainty': {dn: -0.462, up: 0.462}}, 47: {error: {dn: -3.86, up: 3.86}, 'sys,overall uncertainty': {dn: -0.3892, up: 0.3892}}, 48: {error: {dn: -2.99, up: 2.99}, 'sys,overall uncertainty': {dn: -0.23450000000000001, up: 0.23450000000000001}}, 49: {error: {dn: -3.33, up: 3.33}, 'sys,overall uncertainty': {dn: -0.19879999999999998, up: 0.19879999999999998}}, 50: {error: {dn: -3.09, up: 3.09}, 'sys,overall uncertainty': {dn: -0.13090000000000002, up: 0.13090000000000002}}, 51: {error: {dn: -3.94, up: 3.94}, 'sys,overall uncertainty': {dn: -0.48719999999999997, up: 0.48719999999999997}}, 52: {error: {dn: -3.56, up: 3.56}, 'sys,overall uncertainty': {dn: -0.0644, up: 0.0644}}, 53: {error: {dn: -3.05, up: 3.05}, 'sys,overall uncertainty': {dn: -0.38220000000000004, up: 0.38220000000000004}}, 54: {error: {dn: -3.09, up: 3.09}, 'sys,overall uncertainty': {dn: -0.23659999999999998, up: 0.23659999999999998}}, 55: {error: {dn: -2.81, up: 2.81}, 'sys,overall uncertainty': {dn: -0.0154, up: 0.0154}}, 56: {error: {dn: -3.08, up: 3.08}, 'sys,overall uncertainty': {dn: -0.38639999999999997, up: 0.38639999999999997}}, 57: {error: {dn: -3.28, up: 3.28}, 'sys,overall uncertainty': {dn: -0.22959999999999997, up: 0.22959999999999997}}, 58: {error: {dn: -3.16, up: 3.16}, 'sys,overall uncertainty': {dn: -0.2877, up: 0.2877}}, 59: {error: {dn: -3.42, up: 3.42}, 'sys,overall uncertainty': {dn: -0.2555, up: 0.2555}}, 60: {error: {dn: -2.9, up: 2.9}, 'sys,overall uncertainty': {dn: -0.059500000000000004, up: 0.059500000000000004}}, 61: {error: {dn: -2.82, up: 2.82}, 'sys,overall uncertainty': {dn: -0.0882, up: 0.0882}}, 62: {error: {dn: -2.84, up: 2.84}, 'sys,overall uncertainty': {dn: -0.0581, up: 0.0581}}, 63: {error: {dn: -3.28, up: 3.28}, 'sys,overall uncertainty': {dn: -0.2604, up: 0.2604}}, 64: {error: {dn: -3.47, up: 3.47}, 'sys,overall uncertainty': {dn: -0.5159, up: 0.5159}}, 65: {error: {dn: -3.14, up: 3.14}, 'sys,overall uncertainty': {dn: -0.05670000000000001, up: 0.05670000000000001}}, 66: {error: {dn: -2.83, up: 2.83}, 'sys,overall uncertainty': {dn: -0.2534, up: 0.2534}}, 67: {error: {dn: -2.85, up: 2.85}, 'sys,overall uncertainty': {dn: -0.056, up: 0.056}}, 68: {error: {dn: -2.67, up: 2.67}, 'sys,overall uncertainty': {dn: 0.17989999999999998, up: -0.17989999999999998}}, 69: {error: {dn: -3.18, up: 3.18}, 'sys,overall uncertainty': {dn: -0.3563, up: 0.3563}}, 70: {error: {dn: -2.56, up: 2.56}, 'sys,overall uncertainty': {dn: 0.0546, up: -0.0546}}, 71: {error: {dn: -3.33, up: 3.33}, 'sys,overall uncertainty': {dn: -0.1078, up: 0.1078}}, 72: {error: {dn: -2.94, up: 2.94}, 'sys,overall uncertainty': {dn: 0.0133, up: -0.0133}}, 73: {error: {dn: -2.56, up: 2.56}, 'sys,overall uncertainty': {dn: -0.0665, up: 0.0665}}, 74: {error: {dn: -3.39, up: 3.39}, 'sys,overall uncertainty': {dn: -0.38009999999999994, up: 0.38009999999999994}}, 75: {error: {dn: -3.02, up: 3.02}, 'sys,overall uncertainty': {dn: -0.1043, up: 0.1043}}, 76: {error: {dn: -2.84, up: 2.84}, 'sys,overall uncertainty': {dn: -0.2968, up: 0.2968}}, 77: {error: {dn: -2.41, up: 2.41}, 'sys,overall uncertainty': {dn: 0.1281, up: -0.1281}}, 78: {error: {dn: -2.64, up: 2.64}, 'sys,overall uncertainty': {dn: -0.0126, up: 0.0126}}, 79: {error: {dn: -3.03, up: 3.03}, 'sys,overall uncertainty': {dn: -0.0126, up: 0.0126}}, 80: {error: {dn: -2.65, up: 2.65}, 'sys,overall uncertainty': {dn: 0.0252, up: -0.0252}}, 81: {error: {dn: -2.12, up: 2.12}, 'sys,overall uncertainty': {dn: -0.0, up: 0.0}}, 82: {error: {dn: -2.46, up: 2.46}, 'sys,overall uncertainty': {dn: -0.0, up: 0.0}}, 83: {error: {dn: -2.77, up: 2.77}, 'sys,overall uncertainty': {dn: -0.060899999999999996, up: 0.060899999999999996}}, 84: {error: {dn: -2.42, up: 2.42}, 'sys,overall uncertainty': {dn: -0.0, up: 0.0}}} + +IsRef: 1 +Path: /REF/BELLE_2013_I1225975/d01-x01-y01 +Title: doi:10.17182/hepdata.61431.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 1.000000e-02 1.000000e-02 2.208000e+01 9.279622e+00 9.279622e+00 +3.830000e+00 1.000000e-02 1.000000e-02 1.423000e+01 7.992316e+00 7.992316e+00 +3.850000e+00 1.000000e-02 1.000000e-02 1.642000e+01 8.131643e+00 8.131643e+00 +3.870000e+00 1.000000e-02 1.000000e-02 3.285000e+01 9.095477e+00 9.095477e+00 +3.890000e+00 1.000000e-02 1.000000e-02 1.644000e+01 7.261766e+00 7.261766e+00 +3.910000e+00 1.000000e-02 1.000000e-02 1.743000e+01 7.213927e+00 7.213927e+00 +3.930000e+00 1.000000e-02 1.000000e-02 2.402000e+01 7.530120e+00 7.530120e+00 +3.950000e+00 1.000000e-02 1.000000e-02 8.710000e+00 5.812068e+00 5.812068e+00 +3.970000e+00 1.000000e-02 1.000000e-02 2.548000e+01 8.352654e+00 8.352654e+00 +3.990000e+00 1.000000e-02 1.000000e-02 2.093000e+01 7.308359e+00 7.308359e+00 +4.010000e+00 1.000000e-02 1.000000e-02 2.256000e+01 7.205191e+00 7.205191e+00 +4.030000e+00 1.000000e-02 1.000000e-02 2.995000e+01 8.163787e+00 8.163787e+00 +4.050000e+00 1.000000e-02 1.000000e-02 8.950000e+00 6.092299e+00 6.092299e+00 +4.070000e+00 1.000000e-02 1.000000e-02 2.110000e+01 6.948786e+00 6.948786e+00 +4.090000e+00 1.000000e-02 1.000000e-02 1.442000e+01 6.656973e+00 6.656973e+00 +4.110000e+00 1.000000e-02 1.000000e-02 2.101000e+01 6.810687e+00 6.810687e+00 +4.130000e+00 1.000000e-02 1.000000e-02 1.460000e+01 6.530466e+00 6.530466e+00 +4.150000e+00 1.000000e-02 1.000000e-02 6.610000e+00 5.848332e+00 5.848332e+00 +4.170000e+00 1.000000e-02 1.000000e-02 1.586000e+01 6.151020e+00 6.151020e+00 +4.190000e+00 1.000000e-02 1.000000e-02 2.584000e+01 7.094460e+00 7.094460e+00 +4.210000e+00 1.000000e-02 1.000000e-02 4.626000e+01 8.427001e+00 8.427001e+00 +4.230000e+00 1.000000e-02 1.000000e-02 7.349000e+01 1.073314e+01 1.073314e+01 +4.250000e+00 1.000000e-02 1.000000e-02 6.117000e+01 9.948621e+00 9.948621e+00 +4.270000e+00 1.000000e-02 1.000000e-02 5.819000e+01 9.524908e+00 9.524908e+00 +4.290000e+00 1.000000e-02 1.000000e-02 5.693000e+01 9.778851e+00 9.778851e+00 +4.310000e+00 1.000000e-02 1.000000e-02 3.907000e+01 7.889213e+00 7.889213e+00 +4.330000e+00 1.000000e-02 1.000000e-02 3.658000e+01 7.839947e+00 7.839947e+00 +4.350000e+00 1.000000e-02 1.000000e-02 4.318000e+01 8.030549e+00 8.030549e+00 +4.370000e+00 1.000000e-02 1.000000e-02 2.112000e+01 6.198876e+00 6.198876e+00 +4.390000e+00 1.000000e-02 1.000000e-02 2.142000e+01 6.213622e+00 6.213622e+00 +4.410000e+00 1.000000e-02 1.000000e-02 1.487000e+01 5.548511e+00 5.548511e+00 +4.430000e+00 1.000000e-02 1.000000e-02 1.526000e+01 5.848380e+00 5.848380e+00 +4.450000e+00 1.000000e-02 1.000000e-02 8.680000e+00 4.115104e+00 4.115104e+00 +4.470000e+00 1.000000e-02 1.000000e-02 1.114000e+01 4.517808e+00 4.517808e+00 +4.490000e+00 1.000000e-02 1.000000e-02 9.580000e+00 4.579367e+00 4.579367e+00 +4.510000e+00 1.000000e-02 1.000000e-02 1.363000e+01 5.080394e+00 5.080394e+00 +4.530000e+00 1.000000e-02 1.000000e-02 6.040000e+00 4.430221e+00 4.430221e+00 +4.550000e+00 1.000000e-02 1.000000e-02 7.330000e+00 4.102215e+00 4.102215e+00 +4.570000e+00 1.000000e-02 1.000000e-02 1.501000e+01 5.148356e+00 5.148356e+00 +4.590000e+00 1.000000e-02 1.000000e-02 6.090000e+00 4.251427e+00 4.251427e+00 +4.610000e+00 1.000000e-02 1.000000e-02 4.710000e+00 3.864091e+00 3.864091e+00 +4.630000e+00 1.000000e-02 1.000000e-02 6.470000e+00 3.956010e+00 3.956010e+00 +4.650000e+00 1.000000e-02 1.000000e-02 1.074000e+01 3.981621e+00 3.981621e+00 +4.670000e+00 1.000000e-02 1.000000e-02 3.290000e+00 3.846900e+00 3.846900e+00 +4.690000e+00 1.000000e-02 1.000000e-02 0.000000e+00 3.670000e+00 3.670000e+00 +4.710000e+00 1.000000e-02 1.000000e-02 5.440000e+00 3.699650e+00 3.699650e+00 +4.730000e+00 1.000000e-02 1.000000e-02 6.600000e+00 3.698965e+00 3.698965e+00 +4.750000e+00 1.000000e-02 1.000000e-02 5.560000e+00 3.879572e+00 3.879572e+00 +4.770000e+00 1.000000e-02 1.000000e-02 3.350000e+00 2.999182e+00 2.999182e+00 +4.790000e+00 1.000000e-02 1.000000e-02 2.840000e+00 3.335929e+00 3.335929e+00 +4.810000e+00 1.000000e-02 1.000000e-02 1.870000e+00 3.092771e+00 3.092771e+00 +4.830000e+00 1.000000e-02 1.000000e-02 6.960000e+00 3.970008e+00 3.970008e+00 +4.850000e+00 1.000000e-02 1.000000e-02 9.200000e-01 3.560582e+00 3.560582e+00 +4.870000e+00 1.000000e-02 1.000000e-02 5.460000e+00 3.073854e+00 3.073854e+00 +4.890000e+00 1.000000e-02 1.000000e-02 3.380000e+00 3.099045e+00 3.099045e+00 +4.910000e+00 1.000000e-02 1.000000e-02 2.200000e-01 2.810042e+00 2.810042e+00 +4.930000e+00 1.000000e-02 1.000000e-02 5.520000e+00 3.104143e+00 3.104143e+00 +4.950000e+00 1.000000e-02 1.000000e-02 3.280000e+00 3.288026e+00 3.288026e+00 +4.970000e+00 1.000000e-02 1.000000e-02 4.110000e+00 3.173070e+00 3.173070e+00 +4.990000e+00 1.000000e-02 1.000000e-02 3.650000e+00 3.429531e+00 3.429531e+00 +5.010000e+00 1.000000e-02 1.000000e-02 8.500000e-01 2.900610e+00 2.900610e+00 +5.030000e+00 1.000000e-02 1.000000e-02 1.260000e+00 2.821379e+00 2.821379e+00 +5.050000e+00 1.000000e-02 1.000000e-02 8.300000e-01 2.840594e+00 2.840594e+00 +5.070000e+00 1.000000e-02 1.000000e-02 3.720000e+00 3.290320e+00 3.290320e+00 +5.090000e+00 1.000000e-02 1.000000e-02 7.370000e+00 3.508141e+00 3.508141e+00 +5.110000e+00 1.000000e-02 1.000000e-02 8.100000e-01 3.140512e+00 3.140512e+00 +5.130000e+00 1.000000e-02 1.000000e-02 3.620000e+00 2.841322e+00 2.841322e+00 +5.150000e+00 1.000000e-02 1.000000e-02 8.000000e-01 2.850550e+00 2.850550e+00 +5.170000e+00 1.000000e-02 1.000000e-02 -2.570000e+00 2.676054e+00 2.676054e+00 +5.190000e+00 1.000000e-02 1.000000e-02 5.090000e+00 3.199898e+00 3.199898e+00 +5.210000e+00 1.000000e-02 1.000000e-02 -7.800000e-01 2.560582e+00 2.560582e+00 +5.230000e+00 1.000000e-02 1.000000e-02 1.540000e+00 3.331744e+00 3.331744e+00 +5.250000e+00 1.000000e-02 1.000000e-02 -1.900000e-01 2.940030e+00 2.940030e+00 +5.270000e+00 1.000000e-02 1.000000e-02 9.500000e-01 2.560864e+00 2.560864e+00 +5.290000e+00 1.000000e-02 1.000000e-02 5.430000e+00 3.411243e+00 3.411243e+00 +5.310000e+00 1.000000e-02 1.000000e-02 1.490000e+00 3.021801e+00 3.021801e+00 +5.330000e+00 1.000000e-02 1.000000e-02 4.240000e+00 2.855467e+00 2.855467e+00 +5.350000e+00 1.000000e-02 1.000000e-02 -1.830000e+00 2.413402e+00 2.413402e+00 +5.370000e+00 1.000000e-02 1.000000e-02 1.800000e-01 2.640030e+00 2.640030e+00 +5.390000e+00 1.000000e-02 1.000000e-02 1.800000e-01 3.030026e+00 3.030026e+00 +5.410000e+00 1.000000e-02 1.000000e-02 -3.600000e-01 2.650120e+00 2.650120e+00 +5.430000e+00 1.000000e-02 1.000000e-02 0.000000e+00 2.120000e+00 2.120000e+00 +5.450000e+00 1.000000e-02 1.000000e-02 0.000000e+00 2.460000e+00 2.460000e+00 +5.470000e+00 1.000000e-02 1.000000e-02 8.700000e-01 2.770669e+00 2.770669e+00 +5.490000e+00 1.000000e-02 1.000000e-02 0.000000e+00 2.420000e+00 2.420000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/BELLE_2013_I1238273.cc b/analyses/pluginBELLE/BELLE_2013_I1238273.cc rename from analyses/pluginMisc/BELLE_2013_I1238273.cc rename to analyses/pluginBELLE/BELLE_2013_I1238273.cc diff --git a/analyses/pluginMisc/BELLE_2013_I1238273.info b/analyses/pluginBELLE/BELLE_2013_I1238273.info rename from analyses/pluginMisc/BELLE_2013_I1238273.info rename to analyses/pluginBELLE/BELLE_2013_I1238273.info diff --git a/analyses/pluginMisc/BELLE_2013_I1238273.plot b/analyses/pluginBELLE/BELLE_2013_I1238273.plot rename from analyses/pluginMisc/BELLE_2013_I1238273.plot rename to analyses/pluginBELLE/BELLE_2013_I1238273.plot diff --git a/analyses/pluginMisc/BELLE_2013_I1238273.yoda b/analyses/pluginBELLE/BELLE_2013_I1238273.yoda rename from analyses/pluginMisc/BELLE_2013_I1238273.yoda rename to analyses/pluginBELLE/BELLE_2013_I1238273.yoda diff --git a/analyses/pluginBELLE/BELLE_2014_I1282602.cc b/analyses/pluginBELLE/BELLE_2014_I1282602.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2014_I1282602.cc @@ -0,0 +1,119 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2014_I1282602 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2014_I1282602); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nJPsi = bookCounter("TMP/jpsi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the j/psi + if(p.pdgId()==443) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // J/psi pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==321) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nJPsi->fill(event.weight()); + break; + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nJPsi->val(); + double error = _nJPsi->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nJPsi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2014_I1282602); + + +} diff --git a/analyses/pluginBELLE/BELLE_2014_I1282602.info b/analyses/pluginBELLE/BELLE_2014_I1282602.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2014_I1282602.info @@ -0,0 +1,38 @@ +Name: BELLE_2014_I1282602 +Year: 2014 +Summary: Cross section for $e^+e^-\to J/\psi K^+K^-$ at energies between 4.175 and 5.975 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 1282602 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D89 (2014) 072015, 2014 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to J/\psiK^+K^-$ at energies between 4.175 and 5.975 GeV using radiative return by BELLE. + The paper also includes $J\psiK^0_SK^0_S$ but the data is a confidence limit and is therefore not implemented' +Keywords: [] +BibKey: Shen:2014gdm +BibTeX: '@article{Shen:2014gdm, + author = "Shen, C. P. and others", + title = "{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}", + collaboration = "Belle", + journal = "Phys. Rev.", + volume = "D89", + year = "2014", + number = "7", + pages = "072015", + doi = "10.1103/PhysRevD.89.072015", + eprint = "1402.6578", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-PREPRINT-2014-2, KEK-PREPRINT-2013-61", + SLACcitation = "%%CITATION = ARXIV:1402.6578;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2014_I1282602.plot b/analyses/pluginBELLE/BELLE_2014_I1282602.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2014_I1282602.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BELLE_2014_I1282602/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-J/\psi)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-J/\psi)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2014_I1282602.yoda b/analyses/pluginBELLE/BELLE_2014_I1282602.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2014_I1282602.yoda @@ -0,0 +1,152 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2014_I1282602/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -2.6, up: 6.2}, sys: {dn: -0.3, up: 0.3}}, 1: {stat: {dn: -1.3, up: 3.1}, sys: {dn: -0.2, up: 0.2}}, 5: {stat: {dn: -1.2, up: 1.8}, sys: {dn: -0.3, up: 0.3}}, 6: {stat: {dn: -2.0, up: 2.6}, sys: {dn: -0.6, up: 0.6}}, 7: {stat: {dn: -1.6, up: 1.8}, sys: {dn: -0.4, up: 0.4}}, 8: {stat: {dn: -0.8, up: 1.1}, sys: {dn: -0.1, up: 0.1}}, 9: {stat: {dn: -1.3, up: 1.8}, sys: {dn: -0.3, up: 0.3}}, 10: {stat: {dn: -1.2, up: 1.4}, sys: {dn: -0.3, up: 0.3}}, 11: {stat: {dn: -0.6, up: 1.0}, sys: {dn: -0.1, up: 0.1}}, 12: {stat: {dn: -1.5, up: 1.7}, sys: {dn: -0.5, up: 0.5}}, 13: {stat: {dn: -0.5, up: 0.8}, sys: {dn: -0.1, up: 0.1}}, 14: {stat: {dn: -0.8, up: 1.0}, sys: {dn: -0.2, up: 0.2}}, 15: {stat: {dn: -1.1, up: 1.2}, sys: {dn: -0.2, up: 0.2}}, 16: {stat: {dn: -1.1, up: 1.3}, sys: {dn: -0.3, up: 0.3}}, 17: {stat: {dn: -0.9, up: 1.0}, sys: {dn: -0.2, up: 0.2}}, 18: {stat: {dn: -1.0, up: 1.1}, sys: {dn: -0.3, up: 0.3}}, 19: {stat: {dn: -0.8, up: 1.0}, sys: {dn: -0.2, up: 0.2}}, 20: {stat: {dn: -0.6, up: 0.8}, sys: {dn: -0.1, up: 0.1}}, 21: {stat: {dn: -0.6, up: 0.7}, sys: {dn: -0.1, up: 0.1}}, 22: {stat: {dn: -0.8, up: 0.9}, sys: {dn: -0.2, up: 0.2}}, 23: {stat: {dn: -0.6, up: 0.8}, sys: {dn: -0.1, up: 0.1}}, 24: {stat: {dn: -1.0, up: 1.0}, sys: {dn: -0.3, up: 0.3}}, 25: {stat: {dn: -0.6, up: 0.7}, sys: {dn: -0.1, up: 0.1}}, 26: {stat: {dn: -0.3, up: 0.5}, sys: {dn: -0.1, up: 0.1}}, 27: {stat: {dn: -0.6, up: 0.7}, sys: {dn: -0.1, up: 0.1}}, 28: {stat: {dn: -0.4, up: 0.6}, sys: {dn: -0.1, up: 0.1}}, 30: {stat: {dn: -0.3, up: 0.5}, sys: {dn: -0.1, up: 0.1}}, 31: {stat: {dn: -0.2, up: 0.4}, sys: {dn: -0.1, up: 0.1}}, 32: {stat: {dn: -0.3, up: 0.5}, sys: {dn: -0.1, up: 0.1}}, 33: {stat: {dn: -0.3, up: 0.4}, sys: {dn: -0.1, up: 0.1}}, 34: {stat: {dn: -0.4, up: 0.5}, sys: {dn: -0.1, up: 0.1}}, 35: {stat: {dn: -0.3, up: 0.5}, sys: {dn: -0.1, up: 0.1}}, 36: {stat: {dn: -0.2, up: 0.4}, sys: {dn: -0.1, up: 0.1}}} + +IsRef: 1 +Path: /REF/BELLE_2014_I1282602/d01-x01-y01 +Title: doi:10.17182/hepdata.64381.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.175000e+00 0.000000e+00 0.000000e+00 3.600000e+00 2.617250e+00 6.207254e+00 +4.225000e+00 0.000000e+00 0.000000e+00 1.800000e+00 1.315295e+00 3.106445e+00 +4.425000e+00 0.000000e+00 0.000000e+00 2.700000e+00 1.236932e+00 1.824829e+00 +4.475000e+00 0.000000e+00 0.000000e+00 7.100000e+00 2.088061e+00 2.668333e+00 +4.525000e+00 0.000000e+00 0.000000e+00 3.900000e+00 1.649242e+00 1.843909e+00 +4.575000e+00 0.000000e+00 0.000000e+00 1.100000e+00 8.062258e-01 1.104536e+00 +4.625000e+00 0.000000e+00 0.000000e+00 3.800000e+00 1.334166e+00 1.824829e+00 +4.675000e+00 0.000000e+00 0.000000e+00 2.800000e+00 1.236932e+00 1.431782e+00 +4.725000e+00 0.000000e+00 0.000000e+00 8.000000e-01 6.082763e-01 1.004988e+00 +4.775000e+00 0.000000e+00 0.000000e+00 5.900000e+00 1.581139e+00 1.772005e+00 +4.825000e+00 0.000000e+00 0.000000e+00 7.000000e-01 5.099020e-01 8.062258e-01 +4.875000e+00 0.000000e+00 0.000000e+00 1.500000e+00 8.246211e-01 1.019804e+00 +4.925000e+00 0.000000e+00 0.000000e+00 2.500000e+00 1.118034e+00 1.216553e+00 +4.975000e+00 0.000000e+00 0.000000e+00 3.400000e+00 1.140175e+00 1.334166e+00 +5.025000e+00 0.000000e+00 0.000000e+00 1.700000e+00 9.219544e-01 1.019804e+00 +5.075000e+00 0.000000e+00 0.000000e+00 2.900000e+00 1.044031e+00 1.140175e+00 +5.125000e+00 0.000000e+00 0.000000e+00 2.200000e+00 8.246211e-01 1.019804e+00 +5.175000e+00 0.000000e+00 0.000000e+00 1.300000e+00 6.082763e-01 8.062258e-01 +5.225000e+00 0.000000e+00 0.000000e+00 1.000000e+00 6.082763e-01 7.071068e-01 +5.275000e+00 0.000000e+00 0.000000e+00 1.600000e+00 8.246211e-01 9.219544e-01 +5.325000e+00 0.000000e+00 0.000000e+00 8.000000e-01 6.082763e-01 8.062258e-01 +5.375000e+00 0.000000e+00 0.000000e+00 3.500000e+00 1.044031e+00 1.044031e+00 +5.425000e+00 0.000000e+00 0.000000e+00 1.000000e+00 6.082763e-01 7.071068e-01 +5.475000e+00 0.000000e+00 0.000000e+00 4.000000e-01 3.162278e-01 5.099020e-01 +5.525000e+00 0.000000e+00 0.000000e+00 1.100000e+00 6.082763e-01 7.071068e-01 +5.575000e+00 0.000000e+00 0.000000e+00 7.000000e-01 4.123106e-01 6.082763e-01 +5.675000e+00 0.000000e+00 0.000000e+00 6.000000e-01 3.162278e-01 5.099020e-01 +5.725000e+00 0.000000e+00 0.000000e+00 2.000000e-01 2.236068e-01 4.123106e-01 +5.775000e+00 0.000000e+00 0.000000e+00 3.000000e-01 3.162278e-01 5.099020e-01 +5.825000e+00 0.000000e+00 0.000000e+00 4.000000e-01 3.162278e-01 4.123106e-01 +5.875000e+00 0.000000e+00 0.000000e+00 5.000000e-01 4.123106e-01 5.099020e-01 +5.925000e+00 0.000000e+00 0.000000e+00 3.000000e-01 3.162278e-01 5.099020e-01 +5.975000e+00 0.000000e+00 0.000000e+00 2.000000e-01 2.236068e-01 4.123106e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER3D_V2 /REF/BELLE_2014_I1282602/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {} + +IsRef: 1 +Path: /REF/BELLE_2014_I1282602/d02-x01-y01 +Title: doi:10.17182/hepdata.64381.v1/t2 +Type: Scatter3D +--- +# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+ +4.175000e+00 0.000000e+00 0.000000e+00 1.050000e+01 1.050000e+01 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 +4.225000e+00 0.000000e+00 0.000000e+00 9.000000e+00 9.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.275000e+00 0.000000e+00 0.000000e+00 8.000000e+00 8.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.325000e+00 0.000000e+00 0.000000e+00 5.000000e+00 5.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.375000e+00 0.000000e+00 0.000000e+00 6.500000e+00 6.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.425000e+00 0.000000e+00 0.000000e+00 1.275000e+01 1.025000e+01 1.025000e+01 1.000000e+00 0.000000e+00 0.000000e+00 +4.475000e+00 0.000000e+00 0.000000e+00 5.000000e+00 5.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.525000e+00 0.000000e+00 0.000000e+00 4.600000e+00 4.600000e+00 4.600000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 4.200000e+00 4.200000e+00 4.200000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.625000e+00 0.000000e+00 0.000000e+00 3.900000e+00 3.900000e+00 3.900000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.675000e+00 0.000000e+00 0.000000e+00 2.500000e+00 2.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.725000e+00 0.000000e+00 0.000000e+00 1.125000e+01 8.750000e+00 8.750000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.775000e+00 0.000000e+00 0.000000e+00 3.100000e+00 3.100000e+00 3.100000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.825000e+00 0.000000e+00 0.000000e+00 4.250000e+00 4.250000e+00 4.250000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.875000e+00 0.000000e+00 0.000000e+00 3.950000e+00 3.950000e+00 3.950000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.925000e+00 0.000000e+00 0.000000e+00 6.050000e+00 4.950000e+00 4.950000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.975000e+00 0.000000e+00 0.000000e+00 1.650000e+00 1.650000e+00 1.650000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.025000e+00 0.000000e+00 0.000000e+00 5.200000e+00 4.200000e+00 4.200000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.075000e+00 0.000000e+00 0.000000e+00 2.150000e+00 2.150000e+00 2.150000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.125000e+00 0.000000e+00 0.000000e+00 2.000000e+00 2.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.175000e+00 0.000000e+00 0.000000e+00 3.350000e+00 3.350000e+00 3.350000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.225000e+00 0.000000e+00 0.000000e+00 1.800000e+00 1.800000e+00 1.800000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.275000e+00 0.000000e+00 0.000000e+00 3.900000e+00 3.200000e+00 3.200000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.325000e+00 0.000000e+00 0.000000e+00 4.700000e+00 4.000000e+00 4.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +5.375000e+00 0.000000e+00 0.000000e+00 1.100000e+00 1.100000e+00 1.100000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.425000e+00 0.000000e+00 0.000000e+00 1.500000e+00 1.500000e+00 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.475000e+00 0.000000e+00 0.000000e+00 1.000000e+00 1.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.525000e+00 0.000000e+00 0.000000e+00 2.350000e+00 2.350000e+00 2.350000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.575000e+00 0.000000e+00 0.000000e+00 1.700000e+00 1.700000e+00 1.700000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.625000e+00 0.000000e+00 0.000000e+00 5.000000e-01 5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 +5.675000e+00 0.000000e+00 0.000000e+00 6.500000e-01 6.500000e-01 6.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 +5.725000e+00 0.000000e+00 0.000000e+00 1.950000e+00 1.950000e+00 1.950000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.775000e+00 0.000000e+00 0.000000e+00 6.000000e-01 6.000000e-01 6.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 +5.825000e+00 0.000000e+00 0.000000e+00 5.500000e-01 5.500000e-01 5.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 +5.875000e+00 0.000000e+00 0.000000e+00 5.500000e-01 5.500000e-01 5.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 +5.925000e+00 0.000000e+00 0.000000e+00 1.250000e+00 1.250000e+00 1.250000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.975000e+00 0.000000e+00 0.000000e+00 3.500000e-01 3.500000e-01 3.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER3D_V2 +BEGIN YODA_SCATTER3D_V2 /REF/BELLE_2014_I1282602/d02-x01-y02 +Variations: [""] +ErrorBreakdown: {} + +IsRef: 1 +Path: /REF/BELLE_2014_I1282602/d02-x01-y02 +Title: doi:10.17182/hepdata.64381.v1/t2 +Type: Scatter3D +--- +# xval xerr- xerr+ yval yerr- yerr+ zval zerr- zerr+ +4.175000e+00 0.000000e+00 0.000000e+00 1.050000e+01 1.050000e+01 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 +4.225000e+00 0.000000e+00 0.000000e+00 9.000000e+00 9.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.275000e+00 0.000000e+00 0.000000e+00 8.000000e+00 8.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.325000e+00 0.000000e+00 0.000000e+00 5.000000e+00 5.000000e+00 5.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.375000e+00 0.000000e+00 0.000000e+00 6.500000e+00 6.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.425000e+00 0.000000e+00 0.000000e+00 1.275000e+01 1.025000e+01 1.025000e+01 0.000000e+00 0.000000e+00 0.000000e+00 +4.475000e+00 0.000000e+00 0.000000e+00 5.000000e+00 5.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.525000e+00 0.000000e+00 0.000000e+00 4.600000e+00 4.600000e+00 4.600000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 4.200000e+00 4.200000e+00 4.200000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.625000e+00 0.000000e+00 0.000000e+00 3.900000e+00 3.900000e+00 3.900000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.675000e+00 0.000000e+00 0.000000e+00 2.500000e+00 2.500000e+00 2.500000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.725000e+00 0.000000e+00 0.000000e+00 1.125000e+01 8.750000e+00 8.750000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.775000e+00 0.000000e+00 0.000000e+00 3.100000e+00 3.100000e+00 3.100000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.825000e+00 0.000000e+00 0.000000e+00 4.250000e+00 4.250000e+00 4.250000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.875000e+00 0.000000e+00 0.000000e+00 3.950000e+00 3.950000e+00 3.950000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.925000e+00 0.000000e+00 0.000000e+00 6.050000e+00 4.950000e+00 4.950000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.975000e+00 0.000000e+00 0.000000e+00 1.650000e+00 1.650000e+00 1.650000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.025000e+00 0.000000e+00 0.000000e+00 5.200000e+00 4.200000e+00 4.200000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.075000e+00 0.000000e+00 0.000000e+00 2.150000e+00 2.150000e+00 2.150000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.125000e+00 0.000000e+00 0.000000e+00 2.000000e+00 2.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.175000e+00 0.000000e+00 0.000000e+00 3.350000e+00 3.350000e+00 3.350000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.225000e+00 0.000000e+00 0.000000e+00 1.800000e+00 1.800000e+00 1.800000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.275000e+00 0.000000e+00 0.000000e+00 3.900000e+00 3.200000e+00 3.200000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.325000e+00 0.000000e+00 0.000000e+00 4.700000e+00 4.000000e+00 4.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +5.375000e+00 0.000000e+00 0.000000e+00 1.100000e+00 1.100000e+00 1.100000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.425000e+00 0.000000e+00 0.000000e+00 1.500000e+00 1.500000e+00 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.475000e+00 0.000000e+00 0.000000e+00 1.000000e+00 1.000000e+00 1.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.525000e+00 0.000000e+00 0.000000e+00 2.350000e+00 2.350000e+00 2.350000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.575000e+00 0.000000e+00 0.000000e+00 1.700000e+00 1.700000e+00 1.700000e+00 3.000000e+00 0.000000e+00 0.000000e+00 +5.625000e+00 0.000000e+00 0.000000e+00 5.000000e-01 5.000000e-01 5.000000e-01 5.000000e+00 0.000000e+00 0.000000e+00 +5.675000e+00 0.000000e+00 0.000000e+00 6.500000e-01 6.500000e-01 6.500000e-01 2.000000e+00 0.000000e+00 0.000000e+00 +5.725000e+00 0.000000e+00 0.000000e+00 1.950000e+00 1.950000e+00 1.950000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +5.775000e+00 0.000000e+00 0.000000e+00 6.000000e-01 6.000000e-01 6.000000e-01 2.000000e+00 0.000000e+00 0.000000e+00 +5.825000e+00 0.000000e+00 0.000000e+00 5.500000e-01 5.500000e-01 5.500000e-01 2.000000e+00 0.000000e+00 0.000000e+00 +5.875000e+00 0.000000e+00 0.000000e+00 5.500000e-01 5.500000e-01 5.500000e-01 2.000000e+00 0.000000e+00 0.000000e+00 +5.925000e+00 0.000000e+00 0.000000e+00 1.250000e+00 1.250000e+00 1.250000e+00 4.000000e+00 0.000000e+00 0.000000e+00 +5.975000e+00 0.000000e+00 0.000000e+00 3.500000e-01 3.500000e-01 3.500000e-01 3.000000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER3D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2014_I1282602/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.6, up: 0.6}, sys: {dn: -0.3, up: 0.3}}} + +IsRef: 1 +Path: /REF/BELLE_2014_I1282602/d03-x01-y01 +Title: doi:10.17182/hepdata.64381.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.825000e+00 4.250000e-01 4.250000e-01 1.800000e+00 6.708204e-01 6.708204e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2015_I1324785.cc b/analyses/pluginBELLE/BELLE_2015_I1324785.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2015_I1324785.cc @@ -0,0 +1,118 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2015_I1324785 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2015_I1324785); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nPsi2s = bookCounter("TMP/psi2s"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the psi(2S) + if(p.pdgId()==100443) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // omega pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nPsi2s->fill(event.weight()); + break; + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nPsi2s->val(); + double error = _nPsi2s->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nPsi2s; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2015_I1324785); + + +} diff --git a/analyses/pluginBELLE/BELLE_2015_I1324785.info b/analyses/pluginBELLE/BELLE_2015_I1324785.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2015_I1324785.info @@ -0,0 +1,33 @@ +Name: BELLE_2015_I1324785 +Year: 2015 +Summary: Cross section for $e^+e^-\to \psi(2S)\pi^+\pi^-$ at energies between 4.0 and 5.5 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 1324785 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D91 (2015) 112007, 2015 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to \psi(2S)\pi^+\pi^-$ at energies between 4.0 and 5.5 GeV using radiative return by BELLE.' +BibKey: Wang:2014hta +BibTeX: '@article{Wang:2014hta, + author = "Wang, X. L. and others", + title = "{Measurement of $e^+e^- \to \pi^+\pi^-\psi(2S)$ via + Initial State Radiation at Belle}", + collaboration = "Belle", + journal = "Phys. Rev.", + volume = "D91", + year = "2015", + pages = "112007", + doi = "10.1103/PhysRevD.91.112007", + eprint = "1410.7641", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1410.7641;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2015_I1324785.plot b/analyses/pluginBELLE/BELLE_2015_I1324785.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2015_I1324785.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BELLE_2015_I1324785/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\psi(2S))$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\psi(2S))$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2015_I1324785.yoda b/analyses/pluginBELLE/BELLE_2015_I1324785.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2015_I1324785.yoda @@ -0,0 +1,86 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2015_I1324785/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -31.4, up: 31.4}}, 1: {error: {dn: -24.9, up: 24.9}}, 2: {error: {dn: -20.7, up: 20.7}}, 3: {error: {dn: -17.8, up: 17.8}}, 4: {error: {dn: -15.7, up: 15.7}}, 5: {error: {dn: -12.9, up: 12.9}}, 6: {error: {dn: -11.7, up: 11.7}}, 7: {error: {dn: -10.7, up: 10.7}}, 8: {error: {dn: -9.0, up: 9.0}}, 9: {error: {dn: -11.0, up: 11.0}}, 10: {error: {dn: -9.4, up: 9.4}}, 11: {error: {dn: -11.7, up: 11.7}}, 12: {error: {dn: -13.1, up: 13.1}}, 13: {error: {dn: -9.9, up: 9.9}}, 14: {error: {dn: -11.9, up: 11.9}}, 15: {error: {dn: -11.4, up: 11.4}}, 16: {error: {dn: -16.5, up: 16.5}}, 17: {error: {dn: -16.9, up: 16.9}}, 18: {error: {dn: -18.0, up: 18.0}}, 19: {error: {dn: -12.9, up: 12.9}}, 20: {error: {dn: -13.0, up: 13.0}}, 21: {error: {dn: -11.0, up: 11.0}}, 22: {error: {dn: -6.8, up: 6.8}}, 23: {error: {dn: -7.4, up: 7.4}}, 24: {error: {dn: -5.6, up: 5.6}}, 25: {error: {dn: -8.4, up: 8.4}}, 26: {error: {dn: -7.6, up: 7.6}}, 27: {error: {dn: -5.2, up: 5.2}}, 28: {error: {dn: -4.6, up: 4.6}}, 29: {error: {dn: -5.8, up: 5.8}}, 30: {error: {dn: -6.4, up: 6.4}}, 31: {error: {dn: -10.2, up: 10.2}}, 32: {error: {dn: -9.6, up: 9.6}}, 33: {error: {dn: -10.6, up: 10.6}}, 34: {error: {dn: -10.1, up: 10.1}}, 35: {error: {dn: -7.9, up: 7.9}}, 36: {error: {dn: -8.2, up: 8.2}}, 37: {error: {dn: -5.7, up: 5.7}}, 38: {error: {dn: -6.7, up: 6.7}}, 39: {error: {dn: -5.6, up: 5.6}}, 40: {error: {dn: -5.2, up: 5.2}}, 41: {error: {dn: -4.5, up: 4.5}}, 42: {error: {dn: -4.8, up: 4.8}}, 43: {error: {dn: -4.7, up: 4.7}}, 44: {error: {dn: -5.7, up: 5.7}}, 45: {error: {dn: -4.6, up: 4.6}}, 46: {error: {dn: -4.0, up: 4.0}}, 47: {error: {dn: -3.8, up: 3.8}}, 48: {error: {dn: -4.1, up: 4.1}}, 49: {error: {dn: -4.4, up: 4.4}}, 50: {error: {dn: -4.6, up: 4.6}}, 51: {error: {dn: -5.3, up: 5.3}}, 52: {error: {dn: -4.3, up: 4.3}}, 53: {error: {dn: -3.6, up: 3.6}}, 54: {error: {dn: -3.6, up: 3.6}}, 55: {error: {dn: -3.5, up: 3.5}}, 56: {error: {dn: -3.4, up: 3.4}}, 57: {error: {dn: -4.5, up: 4.5}}, 58: {error: {dn: -4.4, up: 4.4}}, 59: {error: {dn: -3.9, up: 3.9}}, 60: {error: {dn: -3.0, up: 3.0}}, 61: {error: {dn: -3.8, up: 3.8}}, 62: {error: {dn: -5.0, up: 5.0}}, 63: {error: {dn: -2.9, up: 2.9}}, 64: {error: {dn: -2.6, up: 2.6}}, 65: {error: {dn: -4.0, up: 4.0}}, 66: {error: {dn: -2.7, up: 2.7}}, 67: {error: {dn: -4.0, up: 4.0}}, 68: {error: {dn: -2.6, up: 2.6}}, 69: {error: {dn: -2.9, up: 2.9}}, 70: {error: {dn: -2.6, up: 2.6}}, 71: {error: {dn: -3.4, up: 3.4}}, 72: {error: {dn: -3.2, up: 3.2}}, 73: {error: {dn: -3.5, up: 3.5}}, 74: {error: {dn: -2.4, up: 2.4}}} + +IsRef: 1 +Path: /REF/BELLE_2015_I1324785/d01-x01-y01 +Title: doi:10.17182/hepdata.71501.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.010000e+00 0.000000e+00 0.000000e+00 -1.910000e+01 3.140000e+01 3.140000e+01 +4.030000e+00 0.000000e+00 0.000000e+00 -1.530000e+01 2.490000e+01 2.490000e+01 +4.050000e+00 0.000000e+00 0.000000e+00 -1.280000e+01 2.070000e+01 2.070000e+01 +4.070000e+00 0.000000e+00 0.000000e+00 -1.100000e+01 1.780000e+01 1.780000e+01 +4.090000e+00 0.000000e+00 0.000000e+00 -9.700000e+00 1.570000e+01 1.570000e+01 +4.110000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.290000e+01 1.290000e+01 +4.130000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.170000e+01 1.170000e+01 +4.150000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.070000e+01 1.070000e+01 +4.170000e+00 0.000000e+00 0.000000e+00 5.900000e+00 9.000000e+00 9.000000e+00 +4.190000e+00 0.000000e+00 0.000000e+00 5.400000e+00 1.100000e+01 1.100000e+01 +4.210000e+00 0.000000e+00 0.000000e+00 -6.000000e+00 9.400000e+00 9.400000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 2.040000e+01 1.170000e+01 1.170000e+01 +4.250000e+00 0.000000e+00 0.000000e+00 2.920000e+01 1.310000e+01 1.310000e+01 +4.270000e+00 0.000000e+00 0.000000e+00 8.900000e+00 9.900000e+00 9.900000e+00 +4.290000e+00 0.000000e+00 0.000000e+00 2.650000e+01 1.190000e+01 1.190000e+01 +4.310000e+00 0.000000e+00 0.000000e+00 2.530000e+01 1.140000e+01 1.140000e+01 +4.330000e+00 0.000000e+00 0.000000e+00 6.150000e+01 1.650000e+01 1.650000e+01 +4.350000e+00 0.000000e+00 0.000000e+00 6.710000e+01 1.690000e+01 1.690000e+01 +4.370000e+00 0.000000e+00 0.000000e+00 8.010000e+01 1.800000e+01 1.800000e+01 +4.390000e+00 0.000000e+00 0.000000e+00 4.040000e+01 1.290000e+01 1.290000e+01 +4.410000e+00 0.000000e+00 0.000000e+00 4.270000e+01 1.300000e+01 1.300000e+01 +4.430000e+00 0.000000e+00 0.000000e+00 3.100000e+01 1.100000e+01 1.100000e+01 +4.450000e+00 0.000000e+00 0.000000e+00 9.700000e+00 6.800000e+00 6.800000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 1.280000e+01 7.400000e+00 7.400000e+00 +4.490000e+00 0.000000e+00 0.000000e+00 6.000000e+00 5.600000e+00 5.600000e+00 +4.510000e+00 0.000000e+00 0.000000e+00 1.840000e+01 8.400000e+00 8.400000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 1.490000e+01 7.600000e+00 7.600000e+00 +4.550000e+00 0.000000e+00 0.000000e+00 5.500000e+00 5.200000e+00 5.200000e+00 +4.570000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 4.600000e+00 4.600000e+00 +4.590000e+00 0.000000e+00 0.000000e+00 8.200000e+00 5.800000e+00 5.800000e+00 +4.610000e+00 0.000000e+00 0.000000e+00 1.090000e+01 6.400000e+00 6.400000e+00 +4.630000e+00 0.000000e+00 0.000000e+00 3.300000e+01 1.020000e+01 1.020000e+01 +4.650000e+00 0.000000e+00 0.000000e+00 2.970000e+01 9.600000e+00 9.600000e+00 +4.670000e+00 0.000000e+00 0.000000e+00 3.730000e+01 1.060000e+01 1.060000e+01 +4.690000e+00 0.000000e+00 0.000000e+00 3.410000e+01 1.010000e+01 1.010000e+01 +4.710000e+00 0.000000e+00 0.000000e+00 2.040000e+01 7.900000e+00 7.900000e+00 +4.730000e+00 0.000000e+00 0.000000e+00 2.270000e+01 8.200000e+00 8.200000e+00 +4.750000e+00 0.000000e+00 0.000000e+00 9.600000e+00 5.700000e+00 5.700000e+00 +4.770000e+00 0.000000e+00 0.000000e+00 1.450000e+01 6.700000e+00 6.700000e+00 +4.790000e+00 0.000000e+00 0.000000e+00 9.400000e+00 5.600000e+00 5.600000e+00 +4.810000e+00 0.000000e+00 0.000000e+00 4.300000e+00 5.200000e+00 5.200000e+00 +4.830000e+00 0.000000e+00 0.000000e+00 1.900000e+00 4.500000e+00 4.500000e+00 +4.850000e+00 0.000000e+00 0.000000e+00 6.600000e+00 4.800000e+00 4.800000e+00 +4.870000e+00 0.000000e+00 0.000000e+00 6.500000e+00 4.700000e+00 4.700000e+00 +4.890000e+00 0.000000e+00 0.000000e+00 1.110000e+01 5.700000e+00 5.700000e+00 +4.910000e+00 0.000000e+00 0.000000e+00 6.300000e+00 4.600000e+00 4.600000e+00 +4.930000e+00 0.000000e+00 0.000000e+00 4.000000e+00 4.000000e+00 4.000000e+00 +4.950000e+00 0.000000e+00 0.000000e+00 -2.800000e+00 3.800000e+00 3.800000e+00 +4.970000e+00 0.000000e+00 0.000000e+00 1.600000e+00 4.100000e+00 4.100000e+00 +4.990000e+00 0.000000e+00 0.000000e+00 6.000000e+00 4.400000e+00 4.400000e+00 +5.010000e+00 0.000000e+00 0.000000e+00 3.700000e+00 4.600000e+00 4.600000e+00 +5.030000e+00 0.000000e+00 0.000000e+00 1.010000e+01 5.300000e+00 5.300000e+00 +5.050000e+00 0.000000e+00 0.000000e+00 5.800000e+00 4.300000e+00 4.300000e+00 +5.070000e+00 0.000000e+00 0.000000e+00 3.600000e+00 3.600000e+00 3.600000e+00 +5.090000e+00 0.000000e+00 0.000000e+00 3.500000e+00 3.600000e+00 3.600000e+00 +5.110000e+00 0.000000e+00 0.000000e+00 -2.600000e+00 3.500000e+00 3.500000e+00 +5.130000e+00 0.000000e+00 0.000000e+00 -2.600000e+00 3.400000e+00 3.400000e+00 +5.150000e+00 0.000000e+00 0.000000e+00 7.400000e+00 4.500000e+00 4.500000e+00 +5.170000e+00 0.000000e+00 0.000000e+00 7.300000e+00 4.400000e+00 4.400000e+00 +5.190000e+00 0.000000e+00 0.000000e+00 5.200000e+00 3.900000e+00 3.900000e+00 +5.210000e+00 0.000000e+00 0.000000e+00 -6.000000e-01 3.000000e+00 3.000000e+00 +5.230000e+00 0.000000e+00 0.000000e+00 5.000000e+00 3.800000e+00 3.800000e+00 +5.250000e+00 0.000000e+00 0.000000e+00 1.050000e+01 5.000000e+00 5.000000e+00 +5.270000e+00 0.000000e+00 0.000000e+00 -6.000000e-01 2.900000e+00 2.900000e+00 +5.290000e+00 0.000000e+00 0.000000e+00 1.200000e+00 2.600000e+00 2.600000e+00 +5.310000e+00 0.000000e+00 0.000000e+00 6.500000e+00 4.000000e+00 4.000000e+00 +5.330000e+00 0.000000e+00 0.000000e+00 -6.000000e-01 2.700000e+00 2.700000e+00 +5.350000e+00 0.000000e+00 0.000000e+00 4.600000e+00 4.000000e+00 4.000000e+00 +5.370000e+00 0.000000e+00 0.000000e+00 -6.000000e-01 2.600000e+00 2.600000e+00 +5.390000e+00 0.000000e+00 0.000000e+00 2.700000e+00 2.900000e+00 2.900000e+00 +5.410000e+00 0.000000e+00 0.000000e+00 -6.000000e-01 2.600000e+00 2.600000e+00 +5.430000e+00 0.000000e+00 0.000000e+00 2.600000e+00 3.400000e+00 3.400000e+00 +5.450000e+00 0.000000e+00 0.000000e+00 4.100000e+00 3.200000e+00 3.200000e+00 +5.470000e+00 0.000000e+00 0.000000e+00 5.600000e+00 3.500000e+00 3.500000e+00 +5.490000e+00 0.000000e+00 0.000000e+00 -6.000000e-01 2.400000e+00 2.400000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2015_I1330289.cc b/analyses/pluginBELLE/BELLE_2015_I1330289.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2015_I1330289.cc @@ -0,0 +1,119 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" +#include "Rivet/Projections/FastJets.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2015_I1330289 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2015_I1330289); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(), "UFS"); + + // Book histograms + _h_spectrum = bookHisto1D(1, 1, 2); + _nBottom = 0.; + } + + + void findDecayProducts(const Particle & mother, unsigned int & nK0, + unsigned int & nKp, unsigned int & nKm, + FourMomentum & ptot) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::KPLUS ) { + ++nKp; + ptot += p.momentum(); + } + else if (id == PID::KMINUS ) { + ++nKm; + ptot += p.momentum(); + } + else if (id == PID::K0S) { + ++nK0; + ptot += p.momentum(); + } + else if (id == PID::PI0 || id == PID::PIPLUS || id == PID::PIMINUS) { + ptot += p.momentum(); + } + else if ( !p.children().empty() ) { + findDecayProducts(p, nK0, nKp, nKm, ptot); + } + else + ptot += p.momentum(); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + // Loop over bottoms + for(const Particle& bottom : apply(event, "UFS").particles()) { + if(bottom.pdgId()!=-521 && bottom.pdgId()!=-511) continue; + FourMomentum pgamma(0.,0.,0.,0.); + unsigned int ngamma = 0; + bool fs = true; + foreach(const Particle & child, bottom.children()) { + if(child.pdgId()==bottom.pdgId()) { + fs = false; + break; + } + else if(child.pdgId()==22) { + ngamma += 1; + pgamma += child.momentum(); + } + } + if(!fs) continue; + _nBottom += event.weight(); + if(ngamma!=1) continue; + unsigned int nK0(0),nKp(0),nKm(0); + FourMomentum p_tot(0,0,0,0); + findDecayProducts(bottom, nK0, nKp, nKm, p_tot); + unsigned int nk = nKp-nKm+nK0; + if(nk%2==1) { + p_tot -= pgamma; + _h_spectrum->fill(p_tot.mass()/GeV,event.weight()); + } + } + + } + + + /// Normalise histograms etc., after the run + void finalize() { + scale(_h_spectrum, 1e6/_nBottom); + // multiply by the bin width + for (unsigned int ix=0;ix<_h_spectrum->numBins();++ix) { + _h_spectrum->bins()[ix].scaleW(_h_spectrum->bins()[ix].xWidth()); + } + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _h_spectrum; + double _nBottom; + //@} + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2015_I1330289); + + +} diff --git a/analyses/pluginBELLE/BELLE_2015_I1330289.info b/analyses/pluginBELLE/BELLE_2015_I1330289.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2015_I1330289.info @@ -0,0 +1,34 @@ +Name: BELLE_2015_I1330289 +Year: 2015 +Summary: Measurement of the spectrum for $\bar{B}\to X_s \gamma$ +Experiment: BELLE +Collider: KEKB +InspireID: 1330289 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - PR D91,052004 +RunInfo: any process making $B^-$ and $\bar{B}^0$ mesons, eg. particle gun or $\Upslion(4S)$ decay. +NeedCrossSection: no +Description: + 'Mass spectrum in $B\to s\gamma$ decays measured by BELLE. Useful for testing the implementation of these decays' +Keywords: [] +BibKey: Saito:2014das +BibTeX: '@article{Saito:2014das, + author = "Saito, T. and others", + title = "{Measurement of the $\bar{B} \rightarrow X_s \gamma$ + Branching Fraction with a Sum of Exclusive Decays}", + collaboration = "Belle", + journal = "Phys. Rev.", + volume = "D91", + year = "2015", + number = "5", + pages = "052004", + doi = "10.1103/PhysRevD.91.052004", + eprint = "1411.7198", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-PREPRINT-2014-15, KEK-PREPRINT-2014-26", + SLACcitation = "%%CITATION = ARXIV:1411.7198;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2015_I1330289.plot b/analyses/pluginBELLE/BELLE_2015_I1330289.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2015_I1330289.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BELLE_2015_I1330289/d01-x01-y02 +Title=Mass spectrum for $\bar{B}\to X_s\gamma$ +XLabel=$M_{X_s}$/GeV +YLabel=$\text{Br}\times10^{-6}$ +LogY=0 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2015_I1330289.yoda b/analyses/pluginBELLE/BELLE_2015_I1330289.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2015_I1330289.yoda @@ -0,0 +1,60 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2015_I1330289/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -10.0, up: 10.0}}, 1: {error: {dn: -14.0, up: 14.0}}, 2: {error: {dn: -54.0, up: 54.0}}, 3: {error: {dn: -49.0, up: 49.0}}, 4: {error: {dn: -27.0, up: 27.0}}, 5: {error: {dn: -31.0, up: 31.0}}, 6: {error: {dn: -46.0, up: 46.0}}, 7: {error: {dn: -50.0, up: 50.0}}, 8: {error: {dn: -52.0, up: 52.0}}, 9: {error: {dn: -50.0, up: 50.0}}, 10: {error: {dn: -37.0, up: 37.0}}, 11: {error: {dn: -37.0, up: 37.0}}, 12: {error: {dn: -54.0, up: 54.0}}, 13: {error: {dn: -60.0, up: 60.0}}, 14: {error: {dn: -54.0, up: 54.0}}, 15: {error: {dn: -35.0, up: 35.0}}, 16: {error: {dn: -80.0, up: 80.0}}, 17: {error: {dn: -84.0, up: 84.0}}, 18: {error: {dn: -82.0, up: 82.0}}} + +IsRef: 1 +Path: /REF/BELLE_2015_I1330289/d01-x01-y01 +Title: doi:10.17182/hepdata.72902.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.500000e-01 5.000000e-02 5.000000e-02 -6.000000e+00 1.000000e+01 1.000000e+01 +7.500000e-01 5.000000e-02 5.000000e-02 3.600000e+01 1.400000e+01 1.400000e+01 +8.500000e-01 5.000000e-02 5.000000e-02 2.032000e+03 5.400000e+01 5.400000e+01 +9.500000e-01 5.000000e-02 5.000000e-02 1.689000e+03 4.900000e+01 4.900000e+01 +1.050000e+00 5.000000e-02 5.000000e-02 3.010000e+02 2.700000e+01 2.700000e+01 +1.150000e+00 5.000000e-02 5.000000e-02 3.100000e+02 3.100000e+01 3.100000e+01 +1.250000e+00 5.000000e-02 5.000000e-02 1.019000e+03 4.600000e+01 4.600000e+01 +1.350000e+00 5.000000e-02 5.000000e-02 1.117000e+03 5.000000e+01 5.000000e+01 +1.450000e+00 5.000000e-02 5.000000e-02 1.090000e+03 5.200000e+01 5.200000e+01 +1.550000e+00 5.000000e-02 5.000000e-02 8.060000e+02 5.000000e+01 5.000000e+01 +1.650000e+00 5.000000e-02 5.000000e-02 7.230000e+02 3.700000e+01 3.700000e+01 +1.750000e+00 5.000000e-02 5.000000e-02 6.640000e+02 3.700000e+01 3.700000e+01 +1.850000e+00 5.000000e-02 5.000000e-02 6.520000e+02 5.400000e+01 5.400000e+01 +1.950000e+00 5.000000e-02 5.000000e-02 5.420000e+02 6.000000e+01 6.000000e+01 +2.050000e+00 5.000000e-02 5.000000e-02 4.030000e+02 5.400000e+01 5.400000e+01 +2.150000e+00 5.000000e-02 5.000000e-02 2.850000e+02 3.500000e+01 3.500000e+01 +2.300000e+00 1.000000e-01 1.000000e-01 4.490000e+02 8.000000e+01 8.000000e+01 +2.500000e+00 1.000000e-01 1.000000e-01 2.730000e+02 8.400000e+01 8.400000e+01 +2.700000e+00 1.000000e-01 1.000000e-01 8.700000e+01 8.200000e+01 8.200000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2015_I1330289/d01-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.0, up: 0.0}}, 1: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.1, up: 0.1}}, 2: {stat: {dn: -0.5, up: 0.5}, sys: {dn: -0.9, up: 0.9}}, 3: {stat: {dn: -0.5, up: 0.5}, sys: {dn: -0.7, up: 0.7}}, 4: {stat: {dn: -0.3, up: 0.3}, sys: {dn: -0.2, up: 0.2}}, 5: {stat: {dn: -0.5, up: 0.5}, sys: {dn: -1.5, up: 1.5}}, 6: {stat: {dn: -0.8, up: 0.8}, sys: {dn: -1.1, up: 1.1}}, 7: {stat: {dn: -1.0, up: 1.0}, sys: {dn: -1.3, up: 1.3}}, 8: {stat: {dn: -1.0, up: 1.0}, sys: {dn: -1.4, up: 1.4}}, 9: {stat: {dn: -1.4, up: 1.4}, sys: {dn: -1.3, up: 1.3}}, 10: {stat: {dn: -1.1, up: 1.1}, sys: {dn: -1.5, up: 1.5}}, 11: {stat: {dn: -1.4, up: 1.4}, sys: {dn: -1.7, up: 1.7}}, 12: {stat: {dn: -2.2, up: 2.2}, sys: {dn: -1.9, up: 1.9}}, 13: {stat: {dn: -2.9, up: 2.9}, sys: {dn: -2.3, up: 2.3}}, 14: {stat: {dn: -3.1, up: 3.1}, sys: {dn: -4.5, up: 4.5}}, 15: {stat: {dn: -2.6, up: 2.6}, sys: {dn: -4.9, up: 4.9}}, 16: {stat: {dn: -7.2, up: 7.2}, sys: {dn: -11.0, up: 11.0}}, 17: {stat: {dn: -8.6, up: 8.6}, sys: {dn: -11.0, up: 11.0}}, 18: {stat: {dn: -11.0, up: 11.0}, sys: {dn: -13.0, up: 13.0}}} + +IsRef: 1 +Path: /REF/BELLE_2015_I1330289/d01-x01-y02 +Title: doi:10.17182/hepdata.72902.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.500000e-01 5.000000e-02 5.000000e-02 -1.000000e-01 1.000000e-01 1.000000e-01 +7.500000e-01 5.000000e-02 5.000000e-02 3.000000e-01 1.414214e-01 1.414214e-01 +8.500000e-01 5.000000e-02 5.000000e-02 1.980000e+01 1.029563e+00 1.029563e+00 +9.500000e-01 5.000000e-02 5.000000e-02 1.570000e+01 8.602325e-01 8.602325e-01 +1.050000e+00 5.000000e-02 5.000000e-02 2.900000e+00 3.605551e-01 3.605551e-01 +1.150000e+00 5.000000e-02 5.000000e-02 4.800000e+00 1.581139e+00 1.581139e+00 +1.250000e+00 5.000000e-02 5.000000e-02 1.870000e+01 1.360147e+00 1.360147e+00 +1.350000e+00 5.000000e-02 5.000000e-02 2.180000e+01 1.640122e+00 1.640122e+00 +1.450000e+00 5.000000e-02 5.000000e-02 2.120000e+01 1.720465e+00 1.720465e+00 +1.550000e+00 5.000000e-02 5.000000e-02 2.200000e+01 1.910497e+00 1.910497e+00 +1.650000e+00 5.000000e-02 5.000000e-02 2.240000e+01 1.860108e+00 1.860108e+00 +1.750000e+00 5.000000e-02 5.000000e-02 2.480000e+01 2.202272e+00 2.202272e+00 +1.850000e+00 5.000000e-02 5.000000e-02 2.670000e+01 2.906888e+00 2.906888e+00 +1.950000e+00 5.000000e-02 5.000000e-02 2.630000e+01 3.701351e+00 3.701351e+00 +2.050000e+00 5.000000e-02 5.000000e-02 2.330000e+01 5.464430e+00 5.464430e+00 +2.150000e+00 5.000000e-02 5.000000e-02 2.100000e+01 5.547071e+00 5.547071e+00 +2.300000e+00 1.000000e-01 1.000000e-01 4.030000e+01 1.314686e+01 1.314686e+01 +2.500000e+00 1.000000e-01 1.000000e-01 2.790000e+01 1.396281e+01 1.396281e+01 +2.700000e+00 1.000000e-01 1.000000e-01 1.150000e+01 1.702939e+01 1.702939e+01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/BELLE_2015_I1397632.cc b/analyses/pluginBELLE/BELLE_2015_I1397632.cc rename from analyses/pluginMisc/BELLE_2015_I1397632.cc rename to analyses/pluginBELLE/BELLE_2015_I1397632.cc diff --git a/analyses/pluginMisc/BELLE_2015_I1397632.info b/analyses/pluginBELLE/BELLE_2015_I1397632.info rename from analyses/pluginMisc/BELLE_2015_I1397632.info rename to analyses/pluginBELLE/BELLE_2015_I1397632.info diff --git a/analyses/pluginMisc/BELLE_2015_I1397632.plot b/analyses/pluginBELLE/BELLE_2015_I1397632.plot rename from analyses/pluginMisc/BELLE_2015_I1397632.plot rename to analyses/pluginBELLE/BELLE_2015_I1397632.plot diff --git a/analyses/pluginMisc/BELLE_2015_I1397632.yoda b/analyses/pluginBELLE/BELLE_2015_I1397632.yoda rename from analyses/pluginMisc/BELLE_2015_I1397632.yoda rename to analyses/pluginBELLE/BELLE_2015_I1397632.yoda diff --git a/analyses/pluginBELLE/BELLE_2016_I1389855.cc b/analyses/pluginBELLE/BELLE_2016_I1389855.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2016_I1389855.cc @@ -0,0 +1,131 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2016_I1389855 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2016_I1389855); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nhb1 = bookCounter("TMP/hb1"); + _nhb2 = bookCounter("TMP/hb2"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()== 10553|| p.pdgId()==110553) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // omega pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(p.pdgId()== 10553) + _nhb1->fill(event.weight()); + else + _nhb2->fill(event.weight()); + break; + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=2;ix<4;++ix) { + double sigma,error; + if(ix==2) { + sigma = _nhb1->val(); + error = _nhb1->err(); + } + else { + sigma = _nhb2->val(); + error = _nhb2->err(); + } + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + //@} + + + /// @name Histograms + //@{ + CounterPtr _nhb1,_nhb2; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2016_I1389855); + + +} diff --git a/analyses/pluginBELLE/BELLE_2016_I1389855.info b/analyses/pluginBELLE/BELLE_2016_I1389855.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2016_I1389855.info @@ -0,0 +1,37 @@ +Name: BELLE_2016_I1389855 +Year: 2016 +Summary: Cross section for $e^+e^-\to h_b(n=1,2)\pi^+\pi^-$ at energies between 10.77 and 11.02 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 1389855 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 117 (2016) no.14, 142001 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to h_b(n=1,2)\pi^+\pi^-$ at energies between 10.77 and 11.02 GeV by BELLE.' +BibKey: Abdesselam:2015zza +BibTeX: '@article{Abdesselam:2015zza, + author = "Abdesselam, A. and others", + title = "{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}", + collaboration = "Belle", + journal = "Phys. Rev. Lett.", + volume = "117", + year = "2016", + number = "14", + pages = "142001", + doi = "10.1103/PhysRevLett.117.142001", + eprint = "1508.06562", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-CONF-1503", + SLACcitation = "%%CITATION = ARXIV:1508.06562;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2016_I1389855.plot b/analyses/pluginBELLE/BELLE_2016_I1389855.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2016_I1389855.plot @@ -0,0 +1,13 @@ +BEGIN PLOT /BELLE_2016_I1389855/d01-x01-y02 +Title=$\sigma(e^+e^-\to \pi^+\pi^-h_b(n=1))$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-h_b(n=1))$/pb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2016_I1389855/d01-x01-y03 +Title=$\sigma(e^+e^-\to \pi^+\pi^-h_b(n=2))$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-h_b(n=2))$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2016_I1389855.yoda b/analyses/pluginBELLE/BELLE_2016_I1389855.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2016_I1389855.yoda @@ -0,0 +1,90 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2016_I1389855/d01-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2016_I1389855/d01-x01-y02 +Title: doi:10.17182/hepdata.74710.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.102200e+04 5.393515e+00 1.077033e+00 9.800000e-01 0.000000e+00 0.000000e+00 +1.101750e+04 4.123106e+00 4.123106e+00 8.600000e-01 0.000000e+00 0.000000e+00 +1.101640e+04 4.707441e+00 1.077033e+00 7.700000e-01 0.000000e+00 0.000000e+00 +1.100680e+04 4.026164e+00 1.077033e+00 9.800000e-01 0.000000e+00 0.000000e+00 +1.099190e+04 1.077033e+00 1.077033e+00 9.900000e-01 0.000000e+00 0.000000e+00 +1.097750e+04 1.077033e+00 1.077033e+00 1.000000e+00 0.000000e+00 0.000000e+00 +1.095750e+04 4.123106e+00 4.123106e+00 9.700000e-01 0.000000e+00 0.000000e+00 +1.092750e+04 4.123106e+00 4.123106e+00 1.150000e+00 0.000000e+00 0.000000e+00 +1.090770e+04 5.001000e+00 1.077033e+00 9.800000e-01 0.000000e+00 0.000000e+00 +1.090110e+04 5.001000e+00 1.486607e+00 1.420000e+00 0.000000e+00 0.000000e+00 +1.089850e+04 4.123106e+00 1.077033e+00 9.800000e-01 0.000000e+00 0.000000e+00 +1.088890e+04 2.236068e+00 1.077033e+00 9.900000e-01 0.000000e+00 0.000000e+00 +1.088360e+04 2.325941e+00 1.345362e+00 1.850000e+00 0.000000e+00 0.000000e+00 +1.087850e+04 1.720465e+00 1.077033e+00 9.800000e-01 0.000000e+00 0.000000e+00 +1.086950e+04 2.236068e+00 1.077033e+00 9.800000e-01 0.000000e+00 0.000000e+00 +1.086860e+04 5.385165e-01 5.385165e-01 2.294000e+01 0.000000e+00 0.000000e+00 +1.086670e+04 5.385165e-01 5.385165e-01 5.047000e+01 0.000000e+00 0.000000e+00 +1.086330e+04 5.385165e-01 5.385165e-01 4.765000e+01 0.000000e+00 0.000000e+00 +1.085890e+04 2.236068e+00 1.077033e+00 9.900000e-01 0.000000e+00 0.000000e+00 +1.084970e+04 1.562050e+00 1.077033e+00 9.900000e-01 0.000000e+00 0.000000e+00 +1.082050e+04 1.077033e+00 6.576473e+00 1.700000e+00 0.000000e+00 0.000000e+00 +1.077110e+04 2.059126e+00 2.059126e+00 9.500000e-01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2016_I1389855/d01-x01-y02 +IsRef: 1 +Path: /REF/BELLE_2016_I1389855/d01-x01-y03 +Title: doi:10.17182/hepdata.74710.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.102200e+04 5.393515e+00 1.077033e+00 -3.900000e-01 9.619771e-01 9.619771e-01 +1.101750e+04 4.123106e+00 4.123106e+00 1.870000e+00 9.792855e-01 9.792855e-01 +1.101640e+04 4.707441e+00 1.077033e+00 1.250000e+00 9.818859e-01 9.818859e-01 +1.100680e+04 4.026164e+00 1.077033e+00 2.570000e+00 9.021086e-01 9.021086e-01 +1.099190e+04 1.077033e+00 1.077033e+00 2.250000e+00 9.345052e-01 9.345052e-01 +1.097750e+04 1.077033e+00 1.077033e+00 3.800000e-01 9.588013e-01 9.588013e-01 +1.095750e+04 4.123106e+00 4.123106e+00 1.050000e+00 9.029396e-01 9.029396e-01 +1.092750e+04 4.123106e+00 4.123106e+00 -1.600000e-01 8.994999e-01 8.994999e-01 +1.090770e+04 5.001000e+00 1.077033e+00 9.700000e-01 9.990495e-01 9.990495e-01 +1.090110e+04 5.001000e+00 1.486607e+00 1.720000e+00 8.122192e-01 8.122192e-01 +1.089850e+04 4.123106e+00 1.077033e+00 2.630000e+00 1.010000e+00 1.010000e+00 +1.088890e+04 2.236068e+00 1.077033e+00 1.940000e+00 1.115706e+00 1.115706e+00 +1.088360e+04 2.325941e+00 1.345362e+00 3.890000e+00 8.164558e-01 8.164558e-01 +1.087850e+04 1.720465e+00 1.077033e+00 2.890000e+00 1.078610e+00 1.078610e+00 +1.086950e+04 2.236068e+00 1.077033e+00 2.220000e+00 1.063438e+00 1.063438e+00 +1.086860e+04 5.385165e-01 5.385165e-01 1.360000e+00 2.282542e-01 2.282542e-01 +1.086670e+04 5.385165e-01 5.385165e-01 1.810000e+00 1.902630e-01 1.902630e-01 +1.086330e+04 5.385165e-01 5.385165e-01 1.660000e+00 1.827567e-01 1.827567e-01 +1.085890e+04 2.236068e+00 1.077033e+00 4.400000e-01 1.036291e+00 1.036291e+00 +1.084970e+04 1.562050e+00 1.077033e+00 1.540000e+00 1.032182e+00 1.032182e+00 +1.082050e+04 1.077033e+00 6.576473e+00 5.000000e-01 7.770457e-01 7.770457e-01 +1.077110e+04 2.059126e+00 2.059126e+00 2.800000e-01 8.809654e-01 8.809654e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2016_I1389855/d01-x01-y03 +IsRef: 1 +Path: /REF/BELLE_2016_I1389855/d01-x01-y04 +Title: doi:10.17182/hepdata.74710.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.102200e+04 5.393515e+00 1.077033e+00 2.210000e+00 1.176903e+00 1.176903e+00 +1.101750e+04 4.123106e+00 4.123106e+00 2.050000e+00 1.124856e+00 1.118839e+00 +1.101640e+04 4.707441e+00 1.077033e+00 3.420000e+00 1.179958e+00 1.182328e+00 +1.100680e+04 4.026164e+00 1.077033e+00 3.450000e+00 1.068971e+00 1.068971e+00 +1.099190e+04 1.077033e+00 1.077033e+00 2.450000e+00 1.130442e+00 1.130442e+00 +1.097750e+04 1.077033e+00 1.077033e+00 8.300000e-01 1.265148e+00 1.265148e+00 +1.095750e+04 4.123106e+00 4.123106e+00 6.000000e-01 1.452618e+00 1.467856e+00 +1.092750e+04 4.123106e+00 4.123106e+00 2.920000e+00 1.636154e+00 1.636154e+00 +1.090770e+04 5.001000e+00 1.077033e+00 -4.000000e-02 1.751371e+00 1.751371e+00 +1.090110e+04 5.001000e+00 1.486607e+00 2.760000e+00 1.472175e+00 1.466186e+00 +1.089850e+04 4.123106e+00 1.077033e+00 3.890000e+00 1.765673e+00 1.755021e+00 +1.088890e+04 2.236068e+00 1.077033e+00 5.410000e+00 1.909398e+00 1.909398e+00 +1.088360e+04 2.325941e+00 1.345362e+00 5.550000e+00 1.491241e+00 1.491241e+00 +1.087850e+04 1.720465e+00 1.077033e+00 5.340000e+00 2.128333e+00 2.128333e+00 +1.086950e+04 2.236068e+00 1.077033e+00 4.260000e+00 2.038750e+00 2.038750e+00 +1.086860e+04 5.385165e-01 5.385165e-01 3.010000e+00 4.455334e-01 4.455334e-01 +1.086670e+04 5.385165e-01 5.385165e-01 2.910000e+00 3.376389e-01 3.376389e-01 +1.086330e+04 5.385165e-01 5.385165e-01 2.330000e+00 3.325658e-01 3.325658e-01 +1.085890e+04 2.236068e+00 1.077033e+00 3.630000e+00 2.043404e+00 2.040858e+00 +1.084970e+04 1.562050e+00 1.077033e+00 2.570000e+00 2.185452e+00 2.194972e+00 +1.082050e+04 1.077033e+00 6.576473e+00 1.830000e+00 1.569841e+00 1.569841e+00 +1.077110e+04 2.059126e+00 2.059126e+00 4.700000e-01 1.525025e+00 1.525025e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/BELLE_2017_I1512299.cc b/analyses/pluginBELLE/BELLE_2017_I1512299.cc rename from analyses/pluginMisc/BELLE_2017_I1512299.cc rename to analyses/pluginBELLE/BELLE_2017_I1512299.cc diff --git a/analyses/pluginMisc/BELLE_2017_I1512299.info b/analyses/pluginBELLE/BELLE_2017_I1512299.info rename from analyses/pluginMisc/BELLE_2017_I1512299.info rename to analyses/pluginBELLE/BELLE_2017_I1512299.info diff --git a/analyses/pluginMisc/BELLE_2017_I1512299.plot b/analyses/pluginBELLE/BELLE_2017_I1512299.plot rename from analyses/pluginMisc/BELLE_2017_I1512299.plot rename to analyses/pluginBELLE/BELLE_2017_I1512299.plot diff --git a/analyses/pluginMisc/BELLE_2017_I1512299.yoda b/analyses/pluginBELLE/BELLE_2017_I1512299.yoda rename from analyses/pluginMisc/BELLE_2017_I1512299.yoda rename to analyses/pluginBELLE/BELLE_2017_I1512299.yoda diff --git a/analyses/pluginBELLE/BELLE_2017_I1606201.cc b/analyses/pluginBELLE/BELLE_2017_I1606201.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2017_I1606201.cc @@ -0,0 +1,115 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2017_I1606201 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2017_I1606201); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(UnstableParticles(), "UFS"); + // Book histograms + for(unsigned int ix=1;ix<16;++ix) + _h[ix] = bookHisto1D(ix, 1, 1); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const UnstableParticles& ufs = apply(event, "UFS"); + + foreach (const Particle& p, ufs.particles()) { + const Vector3 mom3 = p.p3(); + double pp = mom3.mod(); + double xp = 2.*pp/sqrtS(); + int id = abs(p.pdgId()); + if(id==3122) + _h[ 1]->fill(xp,event.weight()); + else if(id==3212) + _h[ 2]->fill(xp,event.weight()); + else if(id==3224) + _h[ 3]->fill(xp,event.weight()); + else if(id==3124) + _h[ 4]->fill(xp,event.weight()); + else if(id==3312) + _h[ 5]->fill(xp,event.weight()); + else if(id==3334) + _h[ 6]->fill(xp,event.weight()); + else if(id==3324) + _h[ 7]->fill(xp,event.weight()); + else if(id==4122) + _h[ 8]->fill(xp,event.weight()); + else if(id==14122) + _h[ 9]->fill(xp,event.weight()); + else if(id==4124) + _h[10]->fill(xp,event.weight()); + else if(id==4112) + _h[11]->fill(xp,event.weight()); + else if(id==4114) + _h[12]->fill(xp,event.weight()); + else if(id==4332) { + if(isDecay(p,{3334,-211})) + _h[13]->fill(xp,event.weight()); + } + else if(id==4132) { + if(isDecay(p,{3312,211})) + _h[14]->fill(xp,event.weight()); + else if(isDecay(p,{3334,321})) + _h[15]->fill(xp,event.weight()); + } + } + } + + // Check for explicit decay into pdgids + bool isDecay(const Particle& mother, vector ids) { + if(mother.pdgId()<0) { + for(unsigned int ix=0;ix=8 &&ix<=12) ) + scale(_h[ix], crossSection()/nanobarn/sumOfWeights()); + else + scale(_h[ix], crossSection()/picobarn/sumOfWeights()); + } + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _h[16]; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2017_I1606201); + + +} diff --git a/analyses/pluginBELLE/BELLE_2017_I1606201.info b/analyses/pluginBELLE/BELLE_2017_I1606201.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2017_I1606201.info @@ -0,0 +1,40 @@ +Name: BELLE_2017_I1606201 +Year: 2017 +Summary: Baryon spectra in $e^+e^-$ collisions at 10.52 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 1606201 +Status: VALIDATED +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D97 (2018) no.7, 072005 +RunInfo: e+ e- to hadrons and e+ e- +NeedCrossSection: yes +Beams: [e-, e+] +Energies: [10.52] +Description: + 'Measurement of spectra for hyperon and charm baryon production in $e^+e^-$ collisions at 10.52 GeV by BELLE. + The spectra for $\Lambda^0$, $\Sigma^0$, $\Sigma^{*+}$, $\Lambda^0(1520)$, $\Xi^-$, $\Omega^-$ + and $\Xi^{*0}$ hyperons are measured. The spectra for the $\Lambda_c^+$, $\Lambda_c(2595)^+$, $\Lambda_c(2625)^+$, + $\Sigma_c(2455)^0$, $\Sigma_c(2520)^0$, $\Omega_c^0$ and $\Xi_c^0$ charm baryons are also measured.' +BibKey: Niiyama:2017wpp +BibTeX: '@article{Niiyama:2017wpp, + author = "Niiyama, M. and others", + title = "{Production cross sections of hyperons and charmed + baryons from $e^+e^-$ annihilation near $\sqrt{s} = + 10.52$~GeV}", + collaboration = "Belle", + journal = "Phys. Rev.", + volume = "D97", + year = "2018", + number = "7", + pages = "072005", + doi = "10.1103/PhysRevD.97.072005", + eprint = "1706.06791", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-PREPRINT-2017-14, KEK-PREPRINT-2017-15", + SLACcitation = "%%CITATION = ARXIV:1706.06791;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2017_I1606201.plot b/analyses/pluginBELLE/BELLE_2017_I1606201.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2017_I1606201.plot @@ -0,0 +1,119 @@ +BEGIN PLOT /BELLE_2017_I1606201/d01-x01-y01 +Title=$\Lambda^0$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$nb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d02-x01-y01 +Title=$\Sigma^0$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$nb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d03-x01-y01 +Title=$\Sigma^{*+}$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$nb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d04-x01-y01 +Title=$\Lambda^0(1520)$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$nb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d05-x01-y01 +Title=$\Xi^-$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$pb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d06-x01-y01 +Title=$\Omega^-$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$pb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d07-x01-y01 +Title=$\Xi^{*0}$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$pb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d08-x01-y01 +Title=$\Lambda_c^+$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$nb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d09-x01-y01 +Title=$\Lambda_c(2595)^+$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$nb +LogY=1 +ConnectGaps=1 +END PLOT + , +BEGIN PLOT /BELLE_2017_I1606201/d10-x01-y01 +Title=$\Lambda_c(2625)^+$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$nb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d11-x01-y01 +Title=$\Sigma_c(2455)^0$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$nb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d12-x01-y01 +Title=$\Sigma_c(2520)^0$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$nb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d13-x01-y01 +Title=$\Omega^0_c\to\Omega^-\pi^+$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$pb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d14-x01-y01 +Title=$\Xi_c^0\to\Xi^-\pi^+$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$pb +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /BELLE_2017_I1606201/d15-x01-y01 +Title=$\Xi_c^0\to\Omega^-K^+$ Momentum Spectra +XLabel=$x_p$ +YLabel=$\frac{\text{d}\sigma}{\text{d}x_p}/$pb +LogY=1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2017_I1606201.yoda b/analyses/pluginBELLE/BELLE_2017_I1606201.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2017_I1606201.yoda @@ -0,0 +1,373 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d01-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.12500 0.02500 0.02500 0.77600 0.04214 0.04214 +0.17500 0.02500 0.02500 0.78800 0.04307 0.04307 +0.22500 0.02500 0.02500 0.72100 0.03906 0.03906 +0.27500 0.02500 0.02500 0.63500 0.03405 0.03405 +0.32500 0.02500 0.02500 0.51900 0.02805 0.02805 +0.37500 0.02500 0.02500 0.39900 0.02204 0.02204 +0.42500 0.02500 0.02500 0.28900 0.01604 0.01604 +0.47500 0.02500 0.02500 0.19800 0.01103 0.01103 +0.52500 0.02500 0.02500 0.13200 0.00714 0.00714 +0.57500 0.02500 0.02500 0.08660 0.00474 0.00474 +0.62500 0.02500 0.02500 0.05080 0.00274 0.00274 +0.67500 0.02500 0.02500 0.02920 0.00164 0.00164 +0.72500 0.02500 0.02500 0.01500 0.00085 0.00085 +0.77500 0.02500 0.02500 0.00779 0.00047 0.00047 +0.82500 0.02500 0.02500 0.00284 0.00019 0.00019 +0.87500 0.02500 0.02500 0.00081 0.00008 0.00008 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d02-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d02-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.15000 0.05000 0.05000 0.16300 0.00836 0.00836 +0.25000 0.05000 0.05000 0.14900 0.00742 0.00742 +0.35000 0.05000 0.05000 0.11200 0.00553 0.00553 +0.45000 0.05000 0.05000 0.07090 0.00349 0.00349 +0.55000 0.05000 0.05000 0.03690 0.00187 0.00187 +0.65000 0.05000 0.05000 0.01500 0.00078 0.00078 +0.75000 0.05000 0.05000 0.00482 0.00029 0.00029 +0.85000 0.05000 0.05000 0.00091 0.00009 0.00009 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d03-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d03-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.25000 0.05000 0.05000 0.05290 0.00575 0.00575 +0.35000 0.05000 0.05000 0.04490 0.00478 0.00478 +0.45000 0.05000 0.05000 0.03380 0.00356 0.00356 +0.55000 0.05000 0.05000 0.01370 0.00145 0.00145 +0.65000 0.05000 0.05000 0.00449 0.00051 0.00051 +0.75000 0.05000 0.05000 0.00107 0.00016 0.00016 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d04-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d04-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.05000 0.05000 0.05000 0.01810 0.00179 0.00179 +0.15000 0.05000 0.05000 0.03250 0.00239 0.00239 +0.25000 0.05000 0.05000 0.02920 0.00204 0.00204 +0.35000 0.05000 0.05000 0.02010 0.00156 0.00156 +0.45000 0.05000 0.05000 0.01350 0.00130 0.00130 +0.55000 0.05000 0.05000 0.00685 0.00100 0.00100 +0.65000 0.05000 0.05000 0.00341 0.00069 0.00069 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d05-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d05-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.05000 0.05000 0.05000 12.30000 0.62169 0.62169 +0.15000 0.05000 0.05000 38.80000 1.84835 1.84835 +0.25000 0.05000 0.05000 38.30000 1.77775 1.77775 +0.35000 0.05000 0.05000 30.80000 1.45602 1.45602 +0.45000 0.05000 0.05000 18.40000 0.86585 0.86585 +0.55000 0.05000 0.05000 9.25000 0.44272 0.44272 +0.65000 0.05000 0.05000 3.86000 0.19172 0.19172 +0.75000 0.05000 0.05000 1.22000 0.14155 0.14155 +0.85000 0.05000 0.05000 0.20900 0.03147 0.03147 +0.95000 0.05000 0.05000 0.00000 0.00000 0.00000 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d06-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d06-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.05000 0.05000 0.05000 0.58200 0.09396 0.09396 +0.15000 0.05000 0.05000 1.75000 0.12343 0.12343 +0.25000 0.05000 0.05000 1.93000 0.11307 0.11307 +0.35000 0.05000 0.05000 1.75000 0.09596 0.09596 +0.45000 0.05000 0.05000 1.39000 0.07767 0.07767 +0.55000 0.05000 0.05000 0.87400 0.06720 0.06720 +0.65000 0.05000 0.05000 0.36400 0.02941 0.02941 +0.75000 0.05000 0.05000 0.14700 0.01374 0.01374 +0.85000 0.05000 0.05000 0.04540 0.00866 0.00866 +0.95000 0.05000 0.05000 0.01680 0.00933 0.00933 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d07-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d07-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.05000 0.05000 0.05000 2.71000 0.36056 0.36056 +0.15000 0.05000 0.05000 7.56000 0.42202 0.42202 +0.25000 0.05000 0.05000 8.23000 0.42544 0.42544 +0.35000 0.05000 0.05000 7.44000 0.37577 0.37577 +0.45000 0.05000 0.05000 4.96000 0.26420 0.26420 +0.55000 0.05000 0.05000 2.86000 0.16101 0.16101 +0.65000 0.05000 0.05000 1.04000 0.07701 0.07701 +0.75000 0.05000 0.05000 0.24000 0.03195 0.03195 +0.85000 0.05000 0.05000 0.06180 0.01624 0.01624 +0.95000 0.05000 0.05000 0.00248 0.00350 0.00350 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d08-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d08-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.01000 0.01000 0.01000 0.00007 0.00007 0.00007 +0.03000 0.01000 0.01000 0.00000 0.00000 0.00000 +0.05000 0.01000 0.01000 0.00200 0.00270 0.00270 +0.07000 0.01000 0.01000 0.00546 0.00571 0.00571 +0.09000 0.01000 0.01000 0.00684 0.00671 0.00671 +0.11000 0.01000 0.01000 0.00563 0.00291 0.00291 +0.13000 0.01000 0.01000 0.01130 0.00443 0.00443 +0.15000 0.01000 0.01000 0.01080 0.00374 0.00374 +0.17000 0.01000 0.01000 0.01730 0.00616 0.00616 +0.19000 0.01000 0.01000 0.01650 0.00349 0.00349 +0.21000 0.01000 0.01000 0.02320 0.00348 0.00348 +0.23000 0.01000 0.01000 0.02770 0.00392 0.00392 +0.25000 0.01000 0.01000 0.03580 0.00416 0.00416 +0.27000 0.01000 0.01000 0.03780 0.00420 0.00420 +0.29000 0.01000 0.01000 0.05480 0.00483 0.00483 +0.31000 0.01000 0.01000 0.05930 0.00510 0.00510 +0.33000 0.01000 0.01000 0.08200 0.00587 0.00587 +0.35000 0.01000 0.01000 0.09630 0.00637 0.00637 +0.37000 0.01000 0.01000 0.10800 0.00681 0.00681 +0.39000 0.01000 0.01000 0.12800 0.00766 0.00766 +0.41000 0.01000 0.01000 0.14300 0.00832 0.00832 +0.43000 0.01000 0.01000 0.16900 0.00940 0.00940 +0.45000 0.01000 0.01000 0.19600 0.01060 0.01060 +0.47000 0.01000 0.01000 0.22100 0.01200 0.01200 +0.49000 0.01000 0.01000 0.25900 0.01386 0.01386 +0.51000 0.01000 0.01000 0.27200 0.01310 0.01310 +0.53000 0.01000 0.01000 0.30700 0.01510 0.01510 +0.55000 0.01000 0.01000 0.34000 0.01609 0.01609 +0.57000 0.01000 0.01000 0.35900 0.01708 0.01708 +0.59000 0.01000 0.01000 0.37900 0.01808 0.01808 +0.61000 0.01000 0.01000 0.39100 0.01908 0.01908 +0.63000 0.01000 0.01000 0.39400 0.01907 0.01907 +0.65000 0.01000 0.01000 0.39100 0.01907 0.01907 +0.67000 0.01000 0.01000 0.37800 0.01807 0.01807 +0.69000 0.01000 0.01000 0.35200 0.01707 0.01707 +0.71000 0.01000 0.01000 0.32800 0.01607 0.01607 +0.73000 0.01000 0.01000 0.29600 0.01407 0.01407 +0.75000 0.01000 0.01000 0.26100 0.01308 0.01308 +0.77000 0.01000 0.01000 0.21800 0.01108 0.01108 +0.79000 0.01000 0.01000 0.18300 0.00898 0.00898 +0.81000 0.01000 0.01000 0.14700 0.00718 0.00718 +0.83000 0.01000 0.01000 0.11800 0.00581 0.00581 +0.85000 0.01000 0.01000 0.08740 0.00431 0.00431 +0.87000 0.01000 0.01000 0.06600 0.00333 0.00333 +0.89000 0.01000 0.01000 0.04490 0.00236 0.00236 +0.91000 0.01000 0.01000 0.03000 0.00186 0.00186 +0.93000 0.01000 0.01000 0.01730 0.00109 0.00109 +0.95000 0.01000 0.01000 0.00980 0.00086 0.00086 +0.97000 0.01000 0.01000 0.00335 0.00089 0.00089 +0.99000 0.01000 0.01000 0.00013 0.00020 0.00020 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d09-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d09-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.45000 0.01000 0.01000 0.00480 0.00080 0.00080 +0.47000 0.01000 0.01000 0.00501 0.00080 0.00080 +0.49000 0.01000 0.01000 0.00646 0.00071 0.00071 +0.51000 0.01000 0.01000 0.00803 0.00086 0.00086 +0.53000 0.01000 0.01000 0.01090 0.00096 0.00096 +0.55000 0.01000 0.01000 0.01160 0.00097 0.00097 +0.57000 0.01000 0.01000 0.01360 0.00105 0.00105 +0.59000 0.01000 0.01000 0.01450 0.00108 0.00108 +0.61000 0.01000 0.01000 0.01590 0.00113 0.00113 +0.63000 0.01000 0.01000 0.01710 0.00119 0.00119 +0.65000 0.01000 0.01000 0.01900 0.00126 0.00126 +0.67000 0.01000 0.01000 0.02210 0.00143 0.00143 +0.69000 0.01000 0.01000 0.02400 0.00152 0.00152 +0.71000 0.01000 0.01000 0.02630 0.00161 0.00161 +0.73000 0.01000 0.01000 0.02870 0.00171 0.00171 +0.75000 0.01000 0.01000 0.02900 0.00178 0.00178 +0.77000 0.01000 0.01000 0.02690 0.00159 0.00159 +0.79000 0.01000 0.01000 0.02950 0.00178 0.00178 +0.81000 0.01000 0.01000 0.02700 0.00158 0.00158 +0.83000 0.01000 0.01000 0.02820 0.00168 0.00168 +0.85000 0.01000 0.01000 0.02600 0.00157 0.00157 +0.87000 0.01000 0.01000 0.02310 0.00138 0.00138 +0.89000 0.01000 0.01000 0.01860 0.00117 0.00117 +0.91000 0.01000 0.01000 0.01520 0.00097 0.00097 +0.93000 0.01000 0.01000 0.01140 0.00077 0.00077 +0.95000 0.01000 0.01000 0.00627 0.00052 0.00052 +0.97000 0.01000 0.01000 0.00448 0.00039 0.00039 +0.99000 0.01000 0.01000 0.00260 0.00029 0.00029 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d10-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d10-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.45000 0.01000 0.01000 0.00881 0.00100 0.00100 +0.47000 0.01000 0.01000 0.01130 0.00094 0.00094 +0.49000 0.01000 0.01000 0.01420 0.00110 0.00110 +0.51000 0.01000 0.01000 0.01400 0.00110 0.00110 +0.53000 0.01000 0.01000 0.01730 0.00134 0.00134 +0.55000 0.01000 0.01000 0.01890 0.00140 0.00140 +0.57000 0.01000 0.01000 0.02160 0.00150 0.00150 +0.59000 0.01000 0.01000 0.02530 0.00168 0.00168 +0.61000 0.01000 0.01000 0.02780 0.00186 0.00186 +0.63000 0.01000 0.01000 0.03160 0.00205 0.00205 +0.65000 0.01000 0.01000 0.03430 0.00224 0.00224 +0.67000 0.01000 0.01000 0.03680 0.00243 0.00243 +0.69000 0.01000 0.01000 0.03930 0.00253 0.00253 +0.71000 0.01000 0.01000 0.04010 0.00262 0.00262 +0.73000 0.01000 0.01000 0.04060 0.00262 0.00262 +0.75000 0.01000 0.01000 0.04060 0.00262 0.00262 +0.77000 0.01000 0.01000 0.03790 0.00241 0.00241 +0.79000 0.01000 0.01000 0.03750 0.00241 0.00241 +0.81000 0.01000 0.01000 0.03590 0.00231 0.00231 +0.83000 0.01000 0.01000 0.03450 0.00221 0.00221 +0.85000 0.01000 0.01000 0.03120 0.00201 0.00201 +0.87000 0.01000 0.01000 0.02920 0.00191 0.00191 +0.89000 0.01000 0.01000 0.02480 0.00161 0.00161 +0.91000 0.01000 0.01000 0.02200 0.00151 0.00151 +0.93000 0.01000 0.01000 0.01390 0.00097 0.00097 +0.95000 0.01000 0.01000 0.01290 0.00092 0.00092 +0.97000 0.01000 0.01000 0.00844 0.00065 0.00065 +0.99000 0.01000 0.01000 0.00452 0.00040 0.00040 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d11-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d11-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.45000 0.01000 0.01000 0.00904 0.00086 0.00086 +0.47000 0.01000 0.01000 0.00966 0.00087 0.00087 +0.49000 0.01000 0.01000 0.01110 0.00097 0.00097 +0.51000 0.01000 0.01000 0.01200 0.00103 0.00103 +0.53000 0.01000 0.01000 0.01440 0.00121 0.00121 +0.55000 0.01000 0.01000 0.01450 0.00120 0.00120 +0.57000 0.01000 0.01000 0.01600 0.00130 0.00130 +0.59000 0.01000 0.01000 0.01750 0.00140 0.00140 +0.61000 0.01000 0.01000 0.01840 0.00149 0.00149 +0.63000 0.01000 0.01000 0.01960 0.00157 0.00157 +0.65000 0.01000 0.01000 0.02050 0.00167 0.00167 +0.67000 0.01000 0.01000 0.02140 0.00168 0.00168 +0.69000 0.01000 0.01000 0.02090 0.00167 0.00167 +0.71000 0.01000 0.01000 0.02000 0.00157 0.00157 +0.73000 0.01000 0.01000 0.01960 0.00156 0.00156 +0.75000 0.01000 0.01000 0.01880 0.00149 0.00149 +0.77000 0.01000 0.01000 0.01570 0.00126 0.00126 +0.79000 0.01000 0.01000 0.01480 0.00116 0.00116 +0.81000 0.01000 0.01000 0.01250 0.00102 0.00102 +0.83000 0.01000 0.01000 0.01030 0.00085 0.00085 +0.85000 0.01000 0.01000 0.00852 0.00071 0.00071 +0.87000 0.01000 0.01000 0.00634 0.00055 0.00055 +0.89000 0.01000 0.01000 0.00407 0.00036 0.00036 +0.91000 0.01000 0.01000 0.00300 0.00028 0.00028 +0.93000 0.01000 0.01000 0.00163 0.00018 0.00018 +0.95000 0.01000 0.01000 0.00079 0.00011 0.00011 +0.97000 0.01000 0.01000 0.00034 0.00006 0.00006 +0.99000 0.01000 0.01000 0.00009 0.00005 0.00005 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d12-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d12-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.45000 0.01000 0.01000 0.00956 0.00156 0.00156 +0.47000 0.01000 0.01000 0.01010 0.00163 0.00163 +0.49000 0.01000 0.01000 0.01140 0.00170 0.00170 +0.51000 0.01000 0.01000 0.01370 0.00192 0.00192 +0.53000 0.01000 0.01000 0.01470 0.00200 0.00200 +0.55000 0.01000 0.01000 0.01560 0.00208 0.00208 +0.57000 0.01000 0.01000 0.01440 0.00192 0.00192 +0.59000 0.01000 0.01000 0.02020 0.00251 0.00251 +0.61000 0.01000 0.01000 0.02200 0.00268 0.00268 +0.63000 0.01000 0.01000 0.02100 0.00255 0.00255 +0.65000 0.01000 0.01000 0.02130 0.00255 0.00255 +0.67000 0.01000 0.01000 0.01980 0.00237 0.00237 +0.69000 0.01000 0.01000 0.01820 0.00222 0.00222 +0.71000 0.01000 0.01000 0.01840 0.00221 0.00221 +0.73000 0.01000 0.01000 0.01880 0.00219 0.00219 +0.75000 0.01000 0.01000 0.01610 0.00196 0.00196 +0.77000 0.01000 0.01000 0.01370 0.00170 0.00170 +0.79000 0.01000 0.01000 0.01160 0.00140 0.00140 +0.81000 0.01000 0.01000 0.00927 0.00120 0.00120 +0.83000 0.01000 0.01000 0.00744 0.00102 0.00102 +0.85000 0.01000 0.01000 0.00665 0.00091 0.00091 +0.87000 0.01000 0.01000 0.00424 0.00069 0.00069 +0.89000 0.01000 0.01000 0.00324 0.00058 0.00058 +0.91000 0.01000 0.01000 0.00282 0.00051 0.00051 +0.93000 0.01000 0.01000 0.00130 0.00043 0.00043 +0.95000 0.01000 0.01000 0.00086 0.00049 0.00049 +0.97000 0.01000 0.01000 0.00055 0.00026 0.00026 +0.99000 0.01000 0.01000 0.00013 0.00044 0.00044 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d13-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d13-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.30000 0.10000 0.10000 0.00396 0.00181 0.00181 +0.50000 0.10000 0.10000 0.01030 0.00215 0.00215 +0.70000 0.10000 0.10000 0.01160 0.00207 0.00207 +0.90000 0.10000 0.10000 0.00234 0.00089 0.00089 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d14-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d14-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.05000 0.05000 0.05000 0.00087 0.01100 0.01100 +0.15000 0.05000 0.05000 0.04600 0.00830 0.00830 +0.25000 0.05000 0.05000 0.09600 0.02246 0.02246 +0.35000 0.05000 0.05000 0.17200 0.02915 0.02915 +0.45000 0.05000 0.05000 0.36500 0.03712 0.03712 +0.55000 0.05000 0.05000 0.61900 0.04469 0.04469 +0.65000 0.05000 0.05000 0.85500 0.05315 0.05315 +0.75000 0.05000 0.05000 0.75100 0.04610 0.04610 +0.85000 0.05000 0.05000 0.36800 0.02780 0.02780 +0.95000 0.05000 0.05000 0.05130 0.01019 0.01019 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1606201/d15-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1606201/d15-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.05000 0.05000 0.05000 0.00000 0.00170 0.00170 +0.15000 0.05000 0.05000 0.00174 0.00170 0.00170 +0.25000 0.05000 0.05000 0.04110 0.01215 0.01215 +0.35000 0.05000 0.05000 0.05000 0.01222 0.01222 +0.45000 0.05000 0.05000 0.11200 0.01490 0.01490 +0.55000 0.05000 0.05000 0.20000 0.02107 0.02107 +0.65000 0.05000 0.05000 0.26100 0.02247 0.02247 +0.75000 0.05000 0.05000 0.21300 0.02045 0.02045 +0.85000 0.05000 0.05000 0.07410 0.01247 0.01247 +0.95000 0.05000 0.05000 0.01760 0.00655 0.00655 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBELLE/BELLE_2017_I1613517.cc b/analyses/pluginBELLE/BELLE_2017_I1613517.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2017_I1613517.cc @@ -0,0 +1,167 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BELLE_2017_I1613517 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BELLE_2017_I1613517); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + // Book histograms + _c_DpDmS = bookCounter("/TMP/sigma_DpDmS"); + _c_DpSDmS = bookCounter("/TMP/sigma_DpSDmS"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + // total hadronic and muonic cross sections + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + vetoEvent; + // unstable charm analysis + const FinalState& ufs = apply(event, "UFS"); + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + bool matched=false; + int sign = p1.pdgId()/id1; + // loop over the other fs particles + for(unsigned int iy=ix+1;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(id1==413 && id2==413) { + _c_DpSDmS->fill(event.weight()); + } + else if((id1==411 && id2==413) || + (id1==413 && id2==411)) { + _c_DpDmS->fill(event.weight()); + } + break; + } + } + if(matched) break; + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights()/nanobarn; + for(unsigned int iy=1;iy<3;++iy) { + double sigma,error; + if(iy==1) { + sigma = _c_DpDmS->val()*fact; + error = _c_DpDmS->err()*fact; + } + else if(iy==2) { + sigma = _c_DpSDmS->val()*fact; + error = _c_DpSDmS->err()*fact; + } + Scatter2D temphisto(refData(1, 1, iy)); + Scatter2DPtr mult = bookScatter2D(1,1,iy); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_DpDmS, _c_DpSDmS; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BELLE_2017_I1613517); + + +} diff --git a/analyses/pluginBELLE/BELLE_2017_I1613517.info b/analyses/pluginBELLE/BELLE_2017_I1613517.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2017_I1613517.info @@ -0,0 +1,35 @@ +Name: BELLE_2017_I1613517 +Year: 2017 +Summary: Cross Section for $e^+e^-\to D^\pm D^{*\mp}$ and $D^{*+}D^{*-}$ from threshold to 6 GeV +Experiment: BELLE +Collider: KEKB +InspireID: 1613517 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D97 (2018) no.1, 012002 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of the cross section for $e^+e^-\to D^\pm D^{*\mp}$ and $D^{*+}D^{*-}$ from threshold to 6 GeV.' +BibKey: Zhukova:2017pen +BibTeX: '@article{Zhukova:2017pen, + author = "Zhukova, V. and others", + title = "{Angular analysis of the $e^+ e^- \to D^{(*) \pm} D^{* + \mp}$ process near the open charm threshold using + initial-state radiation}", + collaboration = "Belle", + journal = "Phys. Rev.", + volume = "D97", + year = "2018", + number = "1", + pages = "012002", + doi = "10.1103/PhysRevD.97.012002", + eprint = "1707.09167", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BELLE-PREPRINT-2017-15, KEK-PREPRINT-2017-16", + SLACcitation = "%%CITATION = ARXIV:1707.09167;%%" +}' diff --git a/analyses/pluginBELLE/BELLE_2017_I1613517.plot b/analyses/pluginBELLE/BELLE_2017_I1613517.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2017_I1613517.plot @@ -0,0 +1,14 @@ +BEGIN PLOT /BELLE_2017_I1613517/d01-x01-y01 +Title=$\sigma(e^+e^-\to D^+D^{*-} +\text{c.c})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^+D^{*-} +\text{c.c} )/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BELLE_2017_I1613517/d01-x01-y02 +Title=$\sigma(e^+e^-\to D^{*+}D^{*-})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^{*-}D^{*+})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBELLE/BELLE_2017_I1613517.yoda b/analyses/pluginBELLE/BELLE_2017_I1613517.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBELLE/BELLE_2017_I1613517.yoda @@ -0,0 +1,427 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1613517/d01-x01-y01 +IsRef: 1 +Path: /REF/BELLE_2017_I1613517/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.87500 0.00500 0.00500 0.01800 0.02800 0.02800 +3.88500 0.00500 0.00500 0.57900 0.31277 0.31277 +3.89500 0.00500 0.00500 0.89800 0.39763 0.39763 +3.90500 0.00500 0.00500 1.55600 0.45921 0.45921 +3.91500 0.00500 0.00500 1.47000 0.46329 0.46329 +3.92500 0.00500 0.00500 2.89300 0.53573 0.53573 +3.93500 0.00500 0.00500 1.65400 0.50324 0.50324 +3.94500 0.00500 0.00500 2.13500 0.50976 0.50976 +3.95500 0.00500 0.00500 2.61700 0.49578 0.49578 +3.96500 0.00500 0.00500 4.01400 0.56314 0.56314 +3.97500 0.00500 0.00500 2.79600 0.52050 0.52050 +3.98500 0.00500 0.00500 2.83700 0.53782 0.53782 +3.99500 0.00500 0.00500 3.03000 0.53881 0.53881 +4.00500 0.00500 0.00500 3.53200 0.53100 0.53100 +4.01500 0.00500 0.00500 4.42400 0.56820 0.56820 +4.02500 0.00500 0.00500 4.64200 0.56297 0.56297 +4.03500 0.00500 0.00500 3.95300 0.52737 0.52737 +4.04500 0.00500 0.00500 2.71900 0.48067 0.48067 +4.05500 0.00500 0.00500 2.37200 0.44608 0.44608 +4.06500 0.00500 0.00500 1.82500 0.40465 0.40465 +4.07500 0.00500 0.00500 1.46000 0.37964 0.37964 +4.08500 0.00500 0.00500 2.68100 0.39110 0.39110 +4.09500 0.00500 0.00500 1.62900 0.37459 0.37459 +4.10500 0.00500 0.00500 2.36400 0.36911 0.36911 +4.11500 0.00500 0.00500 1.76800 0.36535 0.36535 +4.12500 0.00500 0.00500 2.02200 0.38347 0.38347 +4.13500 0.00500 0.00500 0.82800 0.32450 0.32450 +4.14500 0.00500 0.00500 1.12200 0.32949 0.32949 +4.15500 0.00500 0.00500 1.49200 0.35745 0.35745 +4.16500 0.00500 0.00500 1.32700 0.34147 0.34147 +4.17500 0.00500 0.00500 1.08700 0.33885 0.33885 +4.18500 0.00500 0.00500 0.56200 0.33011 0.33011 +4.19500 0.00500 0.00500 1.03800 0.32150 0.32150 +4.20500 0.00500 0.00500 0.68300 0.29444 0.29444 +4.21500 0.00500 0.00500 0.79300 0.29034 0.29034 +4.22500 0.00500 0.00500 1.08100 0.32162 0.32162 +4.23500 0.00500 0.00500 0.85600 0.29743 0.29743 +4.24500 0.00500 0.00500 0.89400 0.29044 0.29044 +4.25500 0.00500 0.00500 0.46000 0.26748 0.26748 +4.26500 0.00500 0.00500 1.34400 0.29317 0.29317 +4.27500 0.00500 0.00500 0.64700 0.25424 0.25424 +4.28500 0.00500 0.00500 0.92000 0.26112 0.26112 +4.29500 0.00500 0.00500 0.45200 0.25245 0.25245 +4.30500 0.00500 0.00500 0.90300 0.25819 0.25819 +4.31500 0.00500 0.00500 0.96100 0.25612 0.25612 +4.32500 0.00500 0.00500 1.22800 0.27318 0.27318 +4.33500 0.00500 0.00500 0.64600 0.23721 0.23721 +4.34500 0.00500 0.00500 0.68800 0.25039 0.25039 +4.35500 0.00500 0.00500 1.07400 0.24910 0.24910 +4.36500 0.00500 0.00500 1.06400 0.23302 0.23302 +4.37500 0.00500 0.00500 0.82900 0.24529 0.24529 +4.38500 0.00500 0.00500 0.83700 0.24117 0.24117 +4.39500 0.00500 0.00500 0.85200 0.24221 0.24221 +4.40500 0.00500 0.00500 0.29900 0.21340 0.21340 +4.41500 0.00500 0.00500 0.97900 0.22002 0.22002 +4.42500 0.00500 0.00500 0.67000 0.22123 0.22123 +4.43500 0.00500 0.00500 0.52500 0.21119 0.21119 +4.44500 0.00500 0.00500 0.72800 0.21311 0.21311 +4.45500 0.00500 0.00500 0.34000 0.20735 0.20735 +4.46500 0.00500 0.00500 0.61200 0.19509 0.19509 +4.47500 0.00500 0.00500 0.74500 0.21112 0.21112 +4.48500 0.00500 0.00500 0.42300 0.19721 0.19721 +4.49500 0.00500 0.00500 0.24800 0.18527 0.18527 +4.50500 0.00500 0.00500 0.72500 0.20009 0.20009 +4.51500 0.00500 0.00500 0.56400 0.17904 0.17904 +4.52500 0.00500 0.00500 0.29500 0.17623 0.17623 +4.53500 0.00500 0.00500 0.53500 0.19217 0.19217 +4.54500 0.00500 0.00500 0.75700 0.19406 0.19406 +4.55500 0.00500 0.00500 0.43900 0.17410 0.17410 +4.56500 0.00500 0.00500 0.51900 0.18513 0.18513 +4.57500 0.00500 0.00500 0.46000 0.17914 0.17914 +4.58500 0.00500 0.00500 0.46400 0.17314 0.17314 +4.59500 0.00500 0.00500 0.59300 0.17005 0.17005 +4.60500 0.00500 0.00500 0.50600 0.17814 0.17814 +4.61500 0.00500 0.00500 0.35100 0.15711 0.15711 +4.62500 0.00500 0.00500 0.47400 0.15805 0.15805 +4.63500 0.00500 0.00500 0.55800 0.17107 0.17107 +4.64500 0.00500 0.00500 0.33300 0.14506 0.14506 +4.65500 0.00500 0.00500 0.72400 0.16200 0.16200 +4.66500 0.00500 0.00500 0.46000 0.15203 0.15203 +4.67500 0.00500 0.00500 0.46000 0.14705 0.14705 +4.68500 0.00500 0.00500 0.48500 0.15205 0.15205 +4.69500 0.00500 0.00500 0.36500 0.13603 0.13603 +4.70500 0.00500 0.00500 0.31200 0.13203 0.13203 +4.71500 0.00500 0.00500 0.41900 0.13701 0.13701 +4.72500 0.00500 0.00500 0.30300 0.13706 0.13706 +4.73500 0.00500 0.00500 0.32700 0.13809 0.13809 +4.74500 0.00500 0.00500 0.30100 0.12903 0.12903 +4.75500 0.00500 0.00500 0.43000 0.14805 0.14805 +4.76500 0.00500 0.00500 0.15500 0.11204 0.11204 +4.77500 0.00500 0.00500 0.48200 0.14403 0.14403 +4.78500 0.00500 0.00500 0.84600 0.15900 0.15900 +4.79500 0.00500 0.00500 0.42700 0.11900 0.11900 +4.80500 0.00500 0.00500 0.43900 0.14509 0.14509 +4.81500 0.00500 0.00500 0.31000 0.12906 0.12906 +4.82500 0.00500 0.00500 0.39700 0.12704 0.12704 +4.83500 0.00500 0.00500 0.62800 0.14601 0.14601 +4.84500 0.00500 0.00500 0.41600 0.12804 0.12804 +4.85500 0.00500 0.00500 0.44300 0.12500 0.12500 +4.86500 0.00500 0.00500 0.36800 0.11400 0.11400 +4.87500 0.00500 0.00500 0.31100 0.11402 0.11402 +4.88500 0.00500 0.00500 0.22600 0.10602 0.10602 +4.89500 0.00500 0.00500 0.18700 0.11007 0.11007 +4.90500 0.00500 0.00500 0.22500 0.10404 0.10404 +4.91500 0.00500 0.00500 0.33000 0.11804 0.11804 +4.92500 0.00500 0.00500 0.16900 0.08301 0.08301 +4.93500 0.00500 0.00500 0.13500 0.10408 0.10408 +4.94500 0.00500 0.00500 0.34100 0.11002 0.11002 +4.95500 0.00500 0.00500 0.35900 0.09800 0.09800 +4.96500 0.00500 0.00500 0.33400 0.11804 0.11804 +4.97500 0.00500 0.00500 0.33800 0.09800 0.09800 +4.98500 0.00500 0.00500 0.34700 0.10400 0.10400 +4.99500 0.00500 0.00500 0.19700 0.09002 0.09002 +5.00500 0.00500 0.00500 0.21500 0.09302 0.09302 +5.01500 0.00500 0.00500 0.33000 0.10100 0.10100 +5.02500 0.00500 0.00500 0.11300 0.07803 0.07803 +5.03500 0.00500 0.00500 0.28100 0.09902 0.09902 +5.04500 0.00500 0.00500 0.30000 0.09501 0.09501 +5.05500 0.00500 0.00500 0.28900 0.10302 0.10302 +5.06500 0.00500 0.00500 0.26400 0.09302 0.09302 +5.07500 0.00500 0.00500 0.21200 0.09302 0.09302 +5.08500 0.00500 0.00500 0.33400 0.09501 0.09501 +5.09500 0.00500 0.00500 0.33000 0.09801 0.09801 +5.10500 0.00500 0.00500 0.31100 0.09702 0.09702 +5.11500 0.00500 0.00500 0.28300 0.08200 0.08200 +5.12500 0.00500 0.00500 0.43800 0.10400 0.10400 +5.13500 0.00500 0.00500 0.36400 0.09801 0.09801 +5.14500 0.00500 0.00500 0.26200 0.08601 0.08601 +5.15500 0.00500 0.00500 0.16300 0.07301 0.07301 +5.16500 0.00500 0.00500 0.14200 0.07301 0.07301 +5.17500 0.00500 0.00500 0.02800 0.06303 0.06303 +5.18500 0.00500 0.00500 0.20400 0.07100 0.07100 +5.19500 0.00500 0.00500 0.15800 0.07603 0.07603 +5.20500 0.00500 0.00500 0.24000 0.08301 0.08301 +5.21500 0.00500 0.00500 0.15500 0.06400 0.06400 +5.22500 0.00500 0.00500 0.08100 0.06603 0.06603 +5.23500 0.00500 0.00500 0.22300 0.07801 0.07801 +5.24500 0.00500 0.00500 0.15200 0.07503 0.07503 +5.25500 0.00500 0.00500 0.22500 0.07701 0.07701 +5.26500 0.00500 0.00500 0.03800 0.06303 0.06303 +5.27500 0.00500 0.00500 0.06400 0.05401 0.05401 +5.28500 0.00500 0.00500 0.28600 0.08001 0.08001 +5.29500 0.00500 0.00500 0.18400 0.06800 0.06800 +5.30500 0.00500 0.00500 0.34200 0.08000 0.08000 +5.31500 0.00500 0.00500 0.25100 0.07601 0.07601 +5.32500 0.00500 0.00500 0.18500 0.07703 0.07703 +5.33500 0.00500 0.00500 0.26500 0.07801 0.07801 +5.34500 0.00500 0.00500 0.17800 0.05800 0.05800 +5.35500 0.00500 0.00500 0.08400 0.05801 0.05801 +5.36500 0.00500 0.00500 0.14300 0.05600 0.05600 +5.37500 0.00500 0.00500 0.07400 0.06003 0.06003 +5.38500 0.00500 0.00500 0.13500 0.06401 0.06401 +5.39500 0.00500 0.00500 0.13300 0.05701 0.05701 +5.40500 0.00500 0.00500 0.08700 0.05201 0.05201 +5.41500 0.00500 0.00500 0.10900 0.05801 0.05801 +5.42500 0.00500 0.00500 0.16600 0.05400 0.05400 +5.43500 0.00500 0.00500 0.16000 0.06201 0.06201 +5.44500 0.00500 0.00500 0.16900 0.05700 0.05700 +5.45500 0.00500 0.00500 0.16500 0.06001 0.06001 +5.46500 0.00500 0.00500 0.18000 0.05700 0.05700 +5.47500 0.00500 0.00500 0.17000 0.05700 0.05700 +5.48500 0.00500 0.00500 0.16800 0.05400 0.05400 +5.49500 0.00500 0.00500 0.08600 0.05704 0.05704 +5.50500 0.00500 0.00500 0.15800 0.05500 0.05500 +5.51500 0.00500 0.00500 0.21500 0.06701 0.06701 +5.52500 0.00500 0.00500 0.10000 0.04100 0.04100 +5.53500 0.00500 0.00500 0.12000 0.04200 0.04200 +5.54500 0.00500 0.00500 0.14800 0.05801 0.05801 +5.55500 0.00500 0.00500 0.14000 0.05100 0.05100 +5.56500 0.00500 0.00500 0.17300 0.05500 0.05500 +5.57500 0.00500 0.00500 0.11700 0.04900 0.04900 +5.58500 0.00500 0.00500 0.10300 0.05201 0.05201 +5.59500 0.00500 0.00500 0.07500 0.04501 0.04501 +5.60500 0.00500 0.00500 0.10400 0.05001 0.05001 +5.61500 0.00500 0.00500 0.20600 0.05900 0.05900 +5.62500 0.00500 0.00500 0.10000 0.04701 0.04701 +5.63500 0.00500 0.00500 0.19900 0.05600 0.05600 +5.64500 0.00500 0.00500 0.17300 0.05801 0.05801 +5.65500 0.00500 0.00500 0.07800 0.05001 0.05001 +5.66500 0.00500 0.00500 0.07500 0.04000 0.04000 +5.67500 0.00500 0.00500 0.09200 0.04601 0.04601 +5.68500 0.00500 0.00500 0.10400 0.04901 0.04901 +5.69500 0.00500 0.00500 0.17700 0.05401 0.05401 +5.70500 0.00500 0.00500 0.13000 0.04700 0.04700 +5.71500 0.00500 0.00500 0.12700 0.04300 0.04300 +5.72500 0.00500 0.00500 0.15700 0.04900 0.04900 +5.73500 0.00500 0.00500 0.02000 0.03002 0.03002 +5.74500 0.00500 0.00500 0.09700 0.04000 0.04000 +5.75500 0.00500 0.00500 0.18200 0.04700 0.04700 +5.76500 0.00500 0.00500 0.11100 0.04501 0.04501 +5.77500 0.00500 0.00500 0.07600 0.04101 0.04101 +5.78500 0.00500 0.00500 0.12400 0.04400 0.04400 +5.79500 0.00500 0.00500 0.04900 0.03200 0.03200 +5.80500 0.00500 0.00500 0.04300 0.03601 0.03601 +5.81500 0.00500 0.00500 0.11100 0.04301 0.04301 +5.82500 0.00500 0.00500 0.06400 0.03400 0.03400 +5.83500 0.00500 0.00500 0.16700 0.04500 0.04500 +5.84500 0.00500 0.00500 0.04800 0.03200 0.03200 +5.85500 0.00500 0.00500 0.04200 0.03401 0.03401 +5.86500 0.00500 0.00500 0.07200 0.03200 0.03200 +5.87500 0.00500 0.00500 0.04000 0.03202 0.03202 +5.88500 0.00500 0.00500 0.04600 0.03302 0.03302 +5.89500 0.00500 0.00500 0.07000 0.03100 0.03100 +5.90500 0.00500 0.00500 -0.01300 0.02502 0.02502 +5.91500 0.00500 0.00500 0.13500 0.04200 0.04200 +5.92500 0.00500 0.00500 0.07800 0.03601 0.03601 +5.93500 0.00500 0.00500 0.05300 0.03200 0.03200 +5.94500 0.00500 0.00500 0.10600 0.03700 0.03700 +5.95500 0.00500 0.00500 0.05900 0.03000 0.03000 +5.96500 0.00500 0.00500 0.04600 0.02800 0.02800 +5.97500 0.00500 0.00500 0.06000 0.03200 0.03200 +5.98500 0.00500 0.00500 0.07000 0.03300 0.03300 +5.99500 0.00500 0.00500 0.09800 0.03200 0.03200 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2017_I1613517/d01-x01-y02 +IsRef: 1 +Path: /REF/BELLE_2017_I1613517/d01-x01-y02 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.02500 0.00500 0.00500 0.78800 0.15799 0.15799 +4.03500 0.00500 0.00500 2.70200 0.26311 0.26311 +4.04500 0.00500 0.00500 2.95800 0.28778 0.28778 +4.05500 0.00500 0.00500 3.13700 0.28640 0.28640 +4.06500 0.00500 0.00500 2.93200 0.27716 0.27716 +4.07500 0.00500 0.00500 3.62900 0.31385 0.31385 +4.08500 0.00500 0.00500 3.51400 0.30438 0.30438 +4.09500 0.00500 0.00500 2.91900 0.27225 0.27225 +4.10500 0.00500 0.00500 2.57400 0.26565 0.26565 +4.11500 0.00500 0.00500 3.43600 0.29558 0.29558 +4.12500 0.00500 0.00500 3.10000 0.29788 0.29788 +4.13500 0.00500 0.00500 2.94300 0.28898 0.28898 +4.14500 0.00500 0.00500 3.10200 0.28562 0.28562 +4.15500 0.00500 0.00500 2.95600 0.28597 0.28597 +4.16500 0.00500 0.00500 3.17800 0.29954 0.29954 +4.17500 0.00500 0.00500 3.06000 0.29062 0.29062 +4.18500 0.00500 0.00500 2.78000 0.27427 0.27427 +4.19500 0.00500 0.00500 2.57000 0.25775 0.25775 +4.20500 0.00500 0.00500 2.22600 0.24042 0.24042 +4.21500 0.00500 0.00500 1.49500 0.20096 0.20096 +4.22500 0.00500 0.00500 1.10000 0.17293 0.17293 +4.23500 0.00500 0.00500 0.67400 0.13533 0.13533 +4.24500 0.00500 0.00500 0.30300 0.12249 0.12249 +4.25500 0.00500 0.00500 0.37400 0.12678 0.12678 +4.26500 0.00500 0.00500 0.61400 0.14303 0.14303 +4.27500 0.00500 0.00500 0.65000 0.14812 0.14812 +4.28500 0.00500 0.00500 0.74100 0.14983 0.14983 +4.29500 0.00500 0.00500 0.50700 0.12560 0.12560 +4.30500 0.00500 0.00500 0.89700 0.16867 0.16867 +4.31500 0.00500 0.00500 0.73500 0.14591 0.14591 +4.32500 0.00500 0.00500 0.95900 0.15377 0.15377 +4.33500 0.00500 0.00500 1.19100 0.17349 0.17349 +4.34500 0.00500 0.00500 1.07800 0.17051 0.17051 +4.35500 0.00500 0.00500 1.22100 0.17596 0.17596 +4.36500 0.00500 0.00500 1.12700 0.16813 0.16813 +4.37500 0.00500 0.00500 1.24100 0.17624 0.17624 +4.38500 0.00500 0.00500 1.06900 0.15893 0.15893 +4.39500 0.00500 0.00500 1.28500 0.17109 0.17109 +4.40500 0.00500 0.00500 0.91900 0.16130 0.16130 +4.41500 0.00500 0.00500 1.27200 0.17940 0.17940 +4.42500 0.00500 0.00500 0.83100 0.14504 0.14504 +4.43500 0.00500 0.00500 0.95100 0.14822 0.14822 +4.44500 0.00500 0.00500 0.67700 0.13200 0.13200 +4.45500 0.00500 0.00500 0.54500 0.12889 0.12889 +4.46500 0.00500 0.00500 0.72500 0.13147 0.13147 +4.47500 0.00500 0.00500 0.41200 0.10341 0.10341 +4.48500 0.00500 0.00500 0.44000 0.10850 0.10850 +4.49500 0.00500 0.00500 0.75400 0.12491 0.12491 +4.50500 0.00500 0.00500 0.63500 0.11790 0.11790 +4.51500 0.00500 0.00500 0.58400 0.12140 0.12140 +4.52500 0.00500 0.00500 0.57300 0.10651 0.10651 +4.53500 0.00500 0.00500 0.37800 0.10607 0.10607 +4.54500 0.00500 0.00500 0.65200 0.12202 0.12202 +4.55500 0.00500 0.00500 0.27500 0.09166 0.09166 +4.56500 0.00500 0.00500 0.56600 0.12317 0.12317 +4.57500 0.00500 0.00500 0.77600 0.12782 0.12782 +4.58500 0.00500 0.00500 0.45200 0.09767 0.09767 +4.59500 0.00500 0.00500 0.39600 0.09240 0.09240 +4.60500 0.00500 0.00500 0.32300 0.08896 0.08896 +4.61500 0.00500 0.00500 0.38700 0.09535 0.09535 +4.62500 0.00500 0.00500 0.50700 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0.00500 0.24400 0.06140 0.06140 +5.04500 0.00500 0.00500 0.28200 0.06549 0.06549 +5.05500 0.00500 0.00500 0.26100 0.06239 0.06239 +5.06500 0.00500 0.00500 0.18500 0.05423 0.05423 +5.07500 0.00500 0.00500 0.26500 0.06239 0.06239 +5.08500 0.00500 0.00500 0.16000 0.05315 0.05315 +5.09500 0.00500 0.00500 0.18200 0.06313 0.06313 +5.10500 0.00500 0.00500 0.17800 0.05515 0.05515 +5.11500 0.00500 0.00500 0.22100 0.05722 0.05722 +5.12500 0.00500 0.00500 0.25000 0.06129 0.06129 +5.13500 0.00500 0.00500 0.17000 0.05315 0.05315 +5.14500 0.00500 0.00500 0.18300 0.05515 0.05515 +5.15500 0.00500 0.00500 0.04200 0.04201 0.04201 +5.16500 0.00500 0.00500 0.10800 0.04305 0.04305 +5.17500 0.00500 0.00500 0.24500 0.05324 0.05324 +5.18500 0.00500 0.00500 0.22000 0.05415 0.05415 +5.19500 0.00500 0.00500 0.08000 0.03606 0.03606 +5.20500 0.00500 0.00500 0.19600 0.05016 0.05016 +5.21500 0.00500 0.00500 0.07000 0.03801 0.03801 +5.22500 0.00500 0.00500 0.12100 0.04604 0.04604 +5.23500 0.00500 0.00500 0.16600 0.04410 0.04410 +5.24500 0.00500 0.00500 0.14900 0.05104 0.05104 +5.25500 0.00500 0.00500 0.12600 0.04205 0.04205 +5.26500 0.00500 0.00500 0.10800 0.04205 0.04205 +5.27500 0.00500 0.00500 0.19700 0.04909 0.04909 +5.28500 0.00500 0.00500 0.14200 0.04804 0.04804 +5.29500 0.00500 0.00500 0.14500 0.04704 0.04704 +5.30500 0.00500 0.00500 0.07000 0.03202 0.03202 +5.31500 0.00500 0.00500 0.16900 0.04504 0.04504 +5.32500 0.00500 0.00500 0.15300 0.04305 0.04305 +5.33500 0.00500 0.00500 0.19900 0.04704 0.04704 +5.34500 0.00500 0.00500 0.17900 0.04405 0.04405 +5.35500 0.00500 0.00500 0.10400 0.03601 0.03601 +5.36500 0.00500 0.00500 0.24500 0.05104 0.05104 +5.37500 0.00500 0.00500 0.20500 0.05004 0.05004 +5.38500 0.00500 0.00500 0.20100 0.04704 0.04704 +5.39500 0.00500 0.00500 0.11200 0.03701 0.03701 +5.40500 0.00500 0.00500 0.15600 0.04101 0.04101 +5.41500 0.00500 0.00500 0.14700 0.04401 0.04401 +5.42500 0.00500 0.00500 0.13400 0.03901 0.03901 +5.43500 0.00500 0.00500 0.13300 0.03801 0.03801 +5.44500 0.00500 0.00500 0.15200 0.04101 0.04101 +5.45500 0.00500 0.00500 0.16500 0.04101 0.04101 +5.46500 0.00500 0.00500 0.06600 0.02900 0.02900 +5.47500 0.00500 0.00500 0.13800 0.03800 0.03800 +5.48500 0.00500 0.00500 0.19200 0.04200 0.04200 +5.49500 0.00500 0.00500 0.18100 0.04300 0.04300 +5.50500 0.00500 0.00500 0.15800 0.03900 0.03900 +5.51500 0.00500 0.00500 0.11000 0.03700 0.03700 +5.52500 0.00500 0.00500 0.17600 0.04200 0.04200 +5.53500 0.00500 0.00500 0.16300 0.03900 0.03900 +5.54500 0.00500 0.00500 0.07200 0.02800 0.02800 +5.55500 0.00500 0.00500 0.07400 0.03000 0.03000 +5.56500 0.00500 0.00500 0.04200 0.02800 0.02800 +5.57500 0.00500 0.00500 0.08900 0.03200 0.03200 +5.58500 0.00500 0.00500 0.06900 0.03000 0.03000 +5.59500 0.00500 0.00500 0.15600 0.03801 0.03801 +5.60500 0.00500 0.00500 0.03900 0.02100 0.02100 +5.61500 0.00500 0.00500 0.06300 0.02600 0.02600 +5.62500 0.00500 0.00500 0.03500 0.02500 0.02500 +5.63500 0.00500 0.00500 0.10600 0.03701 0.03701 +5.64500 0.00500 0.00500 0.07700 0.02602 0.02602 +5.65500 0.00500 0.00500 0.09400 0.02902 0.02902 +5.66500 0.00500 0.00500 0.05100 0.02100 0.02100 +5.67500 0.00500 0.00500 0.05500 0.02602 0.02602 +5.68500 0.00500 0.00500 0.12300 0.03202 0.03202 +5.69500 0.00500 0.00500 0.09800 0.02802 0.02802 +5.70500 0.00500 0.00500 0.14200 0.03406 0.03406 +5.71500 0.00500 0.00500 0.10200 0.03002 0.03002 +5.72500 0.00500 0.00500 0.08500 0.02902 0.02902 +5.73500 0.00500 0.00500 0.10200 0.02802 0.02802 +5.74500 0.00500 0.00500 0.05900 0.02502 0.02502 +5.75500 0.00500 0.00500 0.09700 0.02802 0.02802 +5.76500 0.00500 0.00500 0.08800 0.02902 0.02902 +5.77500 0.00500 0.00500 0.07100 0.02302 0.02302 +5.78500 0.00500 0.00500 0.05500 0.02502 0.02502 +5.79500 0.00500 0.00500 0.07800 0.02502 0.02502 +5.80500 0.00500 0.00500 0.10300 0.02807 0.02807 +5.81500 0.00500 0.00500 0.08500 0.02508 0.02508 +5.82500 0.00500 0.00500 0.08800 0.02608 0.02608 +5.83500 0.00500 0.00500 0.11400 0.02807 0.02807 +5.84500 0.00500 0.00500 0.05800 0.02102 0.02102 +5.85500 0.00500 0.00500 0.09500 0.02907 0.02907 +5.86500 0.00500 0.00500 0.04100 0.01903 0.01903 +5.87500 0.00500 0.00500 0.04100 0.01803 0.01803 +5.88500 0.00500 0.00500 0.10300 0.02707 0.02707 +5.89500 0.00500 0.00500 0.07000 0.02209 0.02209 +5.90500 0.00500 0.00500 0.08000 0.02309 0.02309 +5.91500 0.00500 0.00500 0.07300 0.02209 0.02209 +5.92500 0.00500 0.00500 0.07900 0.02309 0.02309 +5.93500 0.00500 0.00500 0.06500 0.02010 0.02010 +5.94500 0.00500 0.00500 0.03000 0.01603 0.01603 +5.95500 0.00500 0.00500 0.05600 0.02302 0.02302 +5.96500 0.00500 0.00500 0.10700 0.02518 0.02518 +5.97500 0.00500 0.00500 0.05600 0.01910 0.01910 +5.98500 0.00500 0.00500 0.04200 0.01703 0.01703 +5.99500 0.00500 0.00500 0.03800 0.01503 0.01503 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2014_I1286898.cc b/analyses/pluginBES/BESIII_2014_I1286898.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2014_I1286898.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2014_I1286898 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2014_I1286898); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nproton = bookCounter("TMP/proton"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PROTON) vetoEvent; + } + _nproton->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nproton->val(); + double error = _nproton->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 6)); + Scatter2DPtr mult = bookScatter2D(1, 1, 6); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nproton; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2014_I1286898); + + +} diff --git a/analyses/pluginBES/BESIII_2014_I1286898.info b/analyses/pluginBES/BESIII_2014_I1286898.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2014_I1286898.info @@ -0,0 +1,36 @@ +Name: BESIII_2014_I1286898 +Year: 2014 +Summary: Cross section for $e^+e^-\to$ proton and antiproton between 3.65 and 3.9 GeV +Experiment: BESIII +Collider: BEPC +InspireID: 1286898 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Lett. B735 (2014) 101-107, 2014 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ for energies between 3.65 and 3.9 GeV' +Keywords: +BibKey: Ablikim:2014jrz +BibTeX: '%%% contains utf-8, see: http://inspirehep.net/info/faq/general#utf8 +%%% add \usepackage[utf8]{inputenc} to your latex preamble + +@article{Ablikim:2014jrz, + author = "Ablikim, M. and others", + title = "{Study of $e^+e^−$ → $p\bar{p}$ in the vicinity of + ψ(3770)}", + collaboration = "BESIII", + journal = "Phys. Lett.", + volume = "B735", + year = "2014", + pages = "101-107", + doi = "10.1016/j.physletb.2014.06.013", + eprint = "1403.6011", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1403.6011;%%" +}' diff --git a/analyses/pluginBES/BESIII_2014_I1286898.plot b/analyses/pluginBES/BESIII_2014_I1286898.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2014_I1286898.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BESIII_2014_I1286898/d01-x01-y06 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESIII_2014_I1286898.yoda b/analyses/pluginBES/BESIII_2014_I1286898.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2014_I1286898.yoda @@ -0,0 +1,204 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d01-x01-y01 +Title: doi:10.17182/hepdata.64597.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 2.600000e+01 5.100000e+00 5.100000e+00 +3.748000e+00 0.000000e+00 0.000000e+00 1.000000e+00 6.000000e-01 1.800000e+00 +3.752000e+00 0.000000e+00 0.000000e+00 3.000000e+00 1.900000e+00 2.300000e+00 +3.755000e+00 0.000000e+00 0.000000e+00 4.000000e+00 1.700000e+00 2.800000e+00 +3.760000e+00 0.000000e+00 0.000000e+00 4.000000e+00 1.700000e+00 2.800000e+00 +3.766000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.300000e+00 +3.772000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.300000e+00 +3.773000e+00 0.000000e+00 0.000000e+00 6.840000e+02 2.600000e+01 2.600000e+01 +3.778000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.300000e+00 +3.784000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.300000e+00 +3.791000e+00 0.000000e+00 0.000000e+00 1.000000e+00 6.000000e-01 1.800000e+00 +3.798000e+00 0.000000e+00 0.000000e+00 3.000000e+00 1.900000e+00 2.300000e+00 +3.805000e+00 0.000000e+00 0.000000e+00 1.000000e+00 6.000000e-01 1.800000e+00 +3.810000e+00 0.000000e+00 0.000000e+00 2.000000e+01 4.500000e+00 4.500000e+00 +3.819000e+00 0.000000e+00 0.000000e+00 1.000000e+00 6.000000e-01 1.800000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 1.200000e+01 3.200000e+00 4.300000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d01-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d01-x01-y02 +Title: doi:10.17182/hepdata.64597.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 6.260000e+01 4.000000e-01 4.000000e-01 +3.748000e+00 0.000000e+00 0.000000e+00 6.120000e+01 4.000000e-01 4.000000e-01 +3.752000e+00 0.000000e+00 0.000000e+00 6.080000e+01 4.000000e-01 4.000000e-01 +3.755000e+00 0.000000e+00 0.000000e+00 6.170000e+01 4.000000e-01 4.000000e-01 +3.760000e+00 0.000000e+00 0.000000e+00 6.240000e+01 4.000000e-01 4.000000e-01 +3.766000e+00 0.000000e+00 0.000000e+00 6.240000e+01 4.000000e-01 4.000000e-01 +3.772000e+00 0.000000e+00 0.000000e+00 6.250000e+01 4.000000e-01 4.000000e-01 +3.773000e+00 0.000000e+00 0.000000e+00 6.230000e+01 4.000000e-01 4.000000e-01 +3.778000e+00 0.000000e+00 0.000000e+00 6.260000e+01 4.000000e-01 4.000000e-01 +3.784000e+00 0.000000e+00 0.000000e+00 6.240000e+01 4.000000e-01 4.000000e-01 +3.791000e+00 0.000000e+00 0.000000e+00 6.210000e+01 4.000000e-01 4.000000e-01 +3.798000e+00 0.000000e+00 0.000000e+00 6.190000e+01 4.000000e-01 4.000000e-01 +3.805000e+00 0.000000e+00 0.000000e+00 6.150000e+01 4.000000e-01 4.000000e-01 +3.810000e+00 0.000000e+00 0.000000e+00 6.240000e+01 4.000000e-01 4.000000e-01 +3.819000e+00 0.000000e+00 0.000000e+00 6.140000e+01 4.000000e-01 4.000000e-01 +3.900000e+00 0.000000e+00 0.000000e+00 6.170000e+01 4.000000e-01 4.000000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d01-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d01-x01-y03 +Title: doi:10.17182/hepdata.64597.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 4.450000e+01 0.000000e+00 0.000000e+00 +3.748000e+00 0.000000e+00 0.000000e+00 3.570000e+00 0.000000e+00 0.000000e+00 +3.752000e+00 0.000000e+00 0.000000e+00 6.050000e+00 0.000000e+00 0.000000e+00 +3.755000e+00 0.000000e+00 0.000000e+00 7.010000e+00 0.000000e+00 0.000000e+00 +3.760000e+00 0.000000e+00 0.000000e+00 8.650000e+00 0.000000e+00 0.000000e+00 +3.766000e+00 0.000000e+00 0.000000e+00 5.570000e+00 0.000000e+00 0.000000e+00 +3.772000e+00 0.000000e+00 0.000000e+00 3.680000e+00 0.000000e+00 0.000000e+00 +3.773000e+00 0.000000e+00 0.000000e+00 2.917000e+03 0.000000e+00 0.000000e+00 +3.778000e+00 0.000000e+00 0.000000e+00 3.610000e+00 0.000000e+00 0.000000e+00 +3.784000e+00 0.000000e+00 0.000000e+00 4.570000e+00 0.000000e+00 0.000000e+00 +3.791000e+00 0.000000e+00 0.000000e+00 6.100000e+00 0.000000e+00 0.000000e+00 +3.798000e+00 0.000000e+00 0.000000e+00 7.640000e+00 0.000000e+00 0.000000e+00 +3.805000e+00 0.000000e+00 0.000000e+00 4.340000e+00 0.000000e+00 0.000000e+00 +3.810000e+00 0.000000e+00 0.000000e+00 5.260000e+01 0.000000e+00 0.000000e+00 +3.819000e+00 0.000000e+00 0.000000e+00 1.050000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 5.261000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d01-x01-y04 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d01-x01-y04 +Title: doi:10.17182/hepdata.64597.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 7.600000e-01 0.000000e+00 0.000000e+00 +3.748000e+00 0.000000e+00 0.000000e+00 7.600000e-01 0.000000e+00 0.000000e+00 +3.752000e+00 0.000000e+00 0.000000e+00 7.600000e-01 0.000000e+00 0.000000e+00 +3.755000e+00 0.000000e+00 0.000000e+00 7.700000e-01 0.000000e+00 0.000000e+00 +3.760000e+00 0.000000e+00 0.000000e+00 7.700000e-01 0.000000e+00 0.000000e+00 +3.766000e+00 0.000000e+00 0.000000e+00 7.900000e-01 0.000000e+00 0.000000e+00 +3.772000e+00 0.000000e+00 0.000000e+00 8.000000e-01 0.000000e+00 0.000000e+00 +3.773000e+00 0.000000e+00 0.000000e+00 8.000000e-01 0.000000e+00 0.000000e+00 +3.778000e+00 0.000000e+00 0.000000e+00 7.800000e-01 0.000000e+00 0.000000e+00 +3.784000e+00 0.000000e+00 0.000000e+00 7.500000e-01 0.000000e+00 0.000000e+00 +3.791000e+00 0.000000e+00 0.000000e+00 7.400000e-01 0.000000e+00 0.000000e+00 +3.798000e+00 0.000000e+00 0.000000e+00 7.500000e-01 0.000000e+00 0.000000e+00 +3.805000e+00 0.000000e+00 0.000000e+00 7.500000e-01 0.000000e+00 0.000000e+00 +3.810000e+00 0.000000e+00 0.000000e+00 7.500000e-01 0.000000e+00 0.000000e+00 +3.819000e+00 0.000000e+00 0.000000e+00 7.500000e-01 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 7.600000e-01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d01-x01-y05 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d01-x01-y05 +Title: doi:10.17182/hepdata.64597.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 9.000000e-01 1.897367e-01 1.897367e-01 +3.748000e+00 0.000000e+00 0.000000e+00 4.600000e-01 2.816026e-01 8.305420e-01 +3.752000e+00 0.000000e+00 0.000000e+00 8.200000e-01 5.234501e-01 6.328507e-01 +3.755000e+00 0.000000e+00 0.000000e+00 9.300000e-01 3.945884e-01 6.527634e-01 +3.760000e+00 0.000000e+00 0.000000e+00 7.400000e-01 3.238827e-01 5.223983e-01 +3.766000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 3.700000e-01 +3.772000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 5.600000e-01 +3.773000e+00 0.000000e+00 0.000000e+00 3.800000e-01 3.162278e-02 3.162278e-02 +3.778000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 5.700000e-01 +3.784000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 4.500000e-01 +3.791000e+00 0.000000e+00 0.000000e+00 2.600000e-01 1.612452e-01 4.804165e-01 +3.798000e+00 0.000000e+00 0.000000e+00 6.300000e-01 4.019950e-01 4.916299e-01 +3.805000e+00 0.000000e+00 0.000000e+00 3.700000e-01 2.220360e-01 6.706713e-01 +3.810000e+00 0.000000e+00 0.000000e+00 6.100000e-01 1.456022e-01 1.456022e-01 +3.819000e+00 0.000000e+00 0.000000e+00 1.550000e+00 9.364828e-01 2.792168e+00 +3.900000e+00 0.000000e+00 0.000000e+00 3.700000e-01 1.044031e-01 1.334166e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d01-x01-y06 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d01-x01-y06 +Title: doi:10.17182/hepdata.64597.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.190000e+00 2.529822e-01 2.529822e-01 +3.748000e+00 0.000000e+00 0.000000e+00 6.000000e-01 3.622154e-01 1.080740e+00 +3.752000e+00 0.000000e+00 0.000000e+00 1.070000e+00 6.846897e-01 8.238932e-01 +3.755000e+00 0.000000e+00 0.000000e+00 1.210000e+00 5.178803e-01 8.547514e-01 +3.760000e+00 0.000000e+00 0.000000e+00 9.600000e-01 4.159327e-01 6.736468e-01 +3.766000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 4.700000e-01 +3.772000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 7.000000e-01 +3.773000e+00 0.000000e+00 0.000000e+00 4.700000e-01 4.472136e-02 4.472136e-02 +3.778000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 7.400000e-01 +3.784000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 6.000000e-01 +3.791000e+00 0.000000e+00 0.000000e+00 3.500000e-01 2.109502e-01 6.403124e-01 +3.798000e+00 0.000000e+00 0.000000e+00 8.500000e-01 5.433231e-01 6.527634e-01 +3.805000e+00 0.000000e+00 0.000000e+00 5.000000e-01 3.026549e-01 9.008885e-01 +3.810000e+00 0.000000e+00 0.000000e+00 8.100000e-01 1.897367e-01 1.897367e-01 +3.819000e+00 0.000000e+00 0.000000e+00 2.060000e+00 1.237942e+00 3.702648e+00 +3.900000e+00 0.000000e+00 0.000000e+00 4.900000e-01 1.334166e-01 1.726268e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d01-x01-y07 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d01-x01-y07 +Title: doi:10.17182/hepdata.64597.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.120000e+00 2.340940e-01 2.340940e-01 +3.748000e+00 0.000000e+00 0.000000e+00 5.400000e-01 3.224903e-01 9.708244e-01 +3.752000e+00 0.000000e+00 0.000000e+00 9.600000e-01 6.140033e-01 7.433034e-01 +3.755000e+00 0.000000e+00 0.000000e+00 1.090000e+00 4.669047e-01 7.641989e-01 +3.760000e+00 0.000000e+00 0.000000e+00 8.700000e-01 3.748333e-01 6.129437e-01 +3.766000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 4.300000e-01 +3.772000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 6.400000e-01 +3.773000e+00 0.000000e+00 0.000000e+00 4.300000e-01 3.605551e-02 3.605551e-02 +3.778000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 6.600000e-01 +3.784000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 5.400000e-01 +3.791000e+00 0.000000e+00 0.000000e+00 3.200000e-01 1.910497e-01 5.703508e-01 +3.798000e+00 0.000000e+00 0.000000e+00 7.700000e-01 4.825971e-01 5.921149e-01 +3.805000e+00 0.000000e+00 0.000000e+00 4.500000e-01 2.716616e-01 8.105554e-01 +3.810000e+00 0.000000e+00 0.000000e+00 7.300000e-01 1.676305e-01 1.676305e-01 +3.819000e+00 0.000000e+00 0.000000e+00 1.850000e+00 1.117587e+00 3.342529e+00 +3.900000e+00 0.000000e+00 0.000000e+00 4.400000e-01 1.236932e-01 1.627882e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d02-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d02-x01-y01 +Title: doi:10.17182/hepdata.64597.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.775000e+00 1.250000e-01 1.250000e-01 5.900000e-02 3.417601e-02 3.417601e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d02-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d02-x01-y02 +Title: doi:10.17182/hepdata.64597.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.775000e+00 1.250000e-01 1.250000e-01 2.558000e+02 3.820275e+01 3.820275e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d02-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d02-x01-y03 +Title: doi:10.17182/hepdata.64597.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.775000e+00 1.250000e-01 1.250000e-01 2.570000e+00 1.697056e-01 1.697056e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2014_I1286898/d02-x01-y04 +IsRef: 1 +Path: /REF/BESIII_2014_I1286898/d02-x01-y04 +Title: doi:10.17182/hepdata.64597.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.775000e+00 1.250000e-01 1.250000e-01 2.669000e+02 6.166036e+00 6.166036e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2015_I1355215.cc b/analyses/pluginBES/BESIII_2015_I1355215.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1355215.cc @@ -0,0 +1,121 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2015_I1355215 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2015_I1355215); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nJPsi = bookCounter("TMP/jpsi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p1, ufs.particles()) { + if(p1.children().empty()) continue; + bool matched=false; + // find the j/psi + if(p1.pdgId()!=443) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + + foreach (const Particle& p2, ufs.particles()) { + if(p2.children().empty()) continue; + // find the j/psi + if(p2.pdgId()!=331) continue; + map nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nJPsi->fill(event.weight()); + break; + } + } + if(matched) break; + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _nJPsi->val(); + double error = _nJPsi->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 10)); + Scatter2DPtr mult = bookScatter2D(1, 1, 10); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nJPsi; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2015_I1355215); + + +} diff --git a/analyses/pluginBES/BESIII_2015_I1355215.info b/analyses/pluginBES/BESIII_2015_I1355215.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1355215.info @@ -0,0 +1,39 @@ +Name: BESIII_2015_I1355215 +Year: 2015 +Summary: Cross section for $e^+e^-\to J/\psi \eta$ at energies between 3.82 and 4.6 GeV +Experiment: BESIII +Collider: BEPC +InspireID: 1355215 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D91 (2015) 112005, 2015 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to J/\psi \eta$ at energies between 3.82 and 4.6 GeV' +Keywords: [] +BibKey: Ablikim:2015xhk +BibTeX: '%%% contains utf-8, see: http://inspirehep.net/info/faq/general#utf8 +%%% add \usepackage[utf8]{inputenc} to your latex preamble + +@article{Ablikim:2015xhk, + author = "Ablikim, M. and others", + title = "{Measurement of the $e^{+}e^{-} \to \eta J/\psi$ cross + section and search for $e^{+}e^{-} \to \pi^{0} J/\psi$ at + center-of-mass energies between 3.810 and 4.600 GeV}", + collaboration = "BESIII", + journal = "Phys. Rev.", + volume = "D91", + year = "2015", + number = "11", + pages = "112005", + doi = "10.1103/PhysRevD.91.112005", + eprint = "1503.06644", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1503.06644;%%" +}' diff --git a/analyses/pluginBES/BESIII_2015_I1355215.plot b/analyses/pluginBES/BESIII_2015_I1355215.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1355215.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BESIII_2015_I1355215/d01-x01-y10 +Title=$\sigma(e^+e^-\to \eta J/\psi)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta J/\psi)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESIII_2015_I1355215.yoda b/analyses/pluginBES/BESIII_2015_I1355215.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1355215.yoda @@ -0,0 +1,478 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d01-x01-y01 +Title: doi:10.17182/hepdata.73336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 4.310000e+01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 5.460000e+01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 5.410000e+01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 1.091700e+03 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 5.560000e+01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 8.257000e+02 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 5.398000e+02 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.074700e+03 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d01-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d01-x01-y02 +Title: doi:10.17182/hepdata.73336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 1.750000e+01 4.300000e+00 4.300000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 2.570000e+01 5.100000e+00 5.100000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 3.260000e+01 5.800000e+00 5.800000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 3.943000e+02 2.090000e+01 2.090000e+01 +4.245000e+00 0.000000e+00 0.000000e+00 9.300000e+00 3.300000e+00 3.300000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 9.440000e+01 1.050000e+01 1.050000e+01 +4.360000e+00 0.000000e+00 0.000000e+00 1.980000e+01 5.300000e+00 5.300000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 5.690000e+01 8.200000e+00 8.200000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d01-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d01-x01-y03 +Title: doi:10.17182/hepdata.73336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 1.040000e+01 3.600000e+00 3.600000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 1.480000e+01 4.500000e+00 4.500000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 1.140000e+01 3.900000e+00 3.900000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 2.749000e+02 2.010000e+01 2.010000e+01 +4.245000e+00 0.000000e+00 0.000000e+00 9.700000e+00 3.600000e+00 3.600000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 7.590000e+01 1.190000e+01 1.190000e+01 +4.360000e+00 0.000000e+00 0.000000e+00 2.390000e+01 7.700000e+00 7.700000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 4.260000e+01 9.900000e+00 9.900000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d01-x01-y04 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d01-x01-y04 +Title: doi:10.17182/hepdata.73336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 3.520000e+01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 3.370000e+01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 3.310000e+01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 3.240000e+01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 3.140000e+01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 3.030000e+01 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 2.570000e+01 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 2.420000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d01-x01-y05 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d01-x01-y05 +Title: doi:10.17182/hepdata.73336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 2.410000e+01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 2.310000e+01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 2.280000e+01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 2.230000e+01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 2.170000e+01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 2.090000e+01 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.770000e+01 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.670000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d01-x01-y06 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d01-x01-y06 +Title: doi:10.17182/hepdata.73336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 8.660000e-01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 9.140000e-01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 9.370000e-01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 9.600000e-01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 9.920000e-01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 1.021000e+00 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.168000e+00 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.225000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d01-x01-y07 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d01-x01-y07 +Title: doi:10.17182/hepdata.73336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 1.057000e+00 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 1.057000e+00 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 1.054000e+00 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.051000e+00 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.053000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d01-x01-y08 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d01-x01-y08 +Title: doi:10.17182/hepdata.73336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 5.370000e+01 1.355913e+01 1.355913e+01 +4.210000e+00 0.000000e+00 0.000000e+00 6.160000e+01 1.287051e+01 1.287051e+01 +4.220000e+00 0.000000e+00 0.000000e+00 7.820000e+01 1.477193e+01 1.477193e+01 +4.230000e+00 0.000000e+00 0.000000e+00 4.680000e+01 3.535534e+00 3.535534e+00 +4.245000e+00 0.000000e+00 0.000000e+00 2.160000e+01 8.065358e+00 8.065358e+00 +4.260000e+00 0.000000e+00 0.000000e+00 1.490000e+01 2.024846e+00 2.024846e+00 +4.360000e+00 0.000000e+00 0.000000e+00 4.900000e+00 1.476482e+00 1.476482e+00 +4.420000e+00 0.000000e+00 0.000000e+00 7.300000e+00 1.360147e+00 1.360147e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d01-x01-y09 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d01-x01-y09 +Title: doi:10.17182/hepdata.73336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 4.660000e+01 1.618950e+01 1.618950e+01 +4.210000e+00 0.000000e+00 0.000000e+00 5.170000e+01 1.633218e+01 1.633218e+01 +4.220000e+00 0.000000e+00 0.000000e+00 3.960000e+01 1.390575e+01 1.390575e+01 +4.230000e+00 0.000000e+00 0.000000e+00 4.730000e+01 4.879549e+00 4.879549e+00 +4.245000e+00 0.000000e+00 0.000000e+00 3.260000e+01 1.259603e+01 1.259603e+01 +4.260000e+00 0.000000e+00 0.000000e+00 1.740000e+01 2.954657e+00 2.954657e+00 +4.360000e+00 0.000000e+00 0.000000e+00 8.700000e+00 3.008322e+00 3.008322e+00 +4.420000e+00 0.000000e+00 0.000000e+00 7.800000e+00 1.931321e+00 1.931321e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d01-x01-y10 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d01-x01-y10 +Title: doi:10.17182/hepdata.73336.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 5.080000e+01 1.041393e+01 1.041393e+01 +4.210000e+00 0.000000e+00 0.000000e+00 5.780000e+01 1.011929e+01 1.011929e+01 +4.220000e+00 0.000000e+00 0.000000e+00 5.770000e+01 1.015332e+01 1.015332e+01 +4.230000e+00 0.000000e+00 0.000000e+00 4.700000e+01 2.973214e+00 2.973214e+00 +4.245000e+00 0.000000e+00 0.000000e+00 2.480000e+01 6.800735e+00 6.800735e+00 +4.260000e+00 0.000000e+00 0.000000e+00 1.570000e+01 1.664332e+00 1.664332e+00 +4.360000e+00 0.000000e+00 0.000000e+00 5.600000e+00 1.341641e+00 1.341641e+00 +4.420000e+00 0.000000e+00 0.000000e+00 7.500000e+00 1.081665e+00 1.081665e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d02-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d02-x01-y01 +Title: doi:10.17182/hepdata.73336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 5.050000e+01 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 5.260000e+01 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 5.260000e+01 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 4.490000e+01 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 5.520000e+01 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 1.099000e+02 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 1.100000e+02 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 4.770000e+01 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 5.700000e+02 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d02-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d02-x01-y02 +Title: doi:10.17182/hepdata.73336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d02-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d02-x01-y03 +Title: doi:10.17182/hepdata.73336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 1.200000e+01 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 6.000000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 3.400000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d02-x01-y04 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d02-x01-y04 +Title: doi:10.17182/hepdata.73336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 1.900000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d02-x01-y05 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d02-x01-y05 +Title: doi:10.17182/hepdata.73336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 3.230000e+01 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 3.830000e+01 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 3.100000e+01 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 2.740000e+01 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 2.500000e+01 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 2.350000e+01 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 2.280000e+01 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 2.260000e+01 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 2.240000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d02-x01-y06 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d02-x01-y06 +Title: doi:10.17182/hepdata.73336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d02-x01-y07 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d02-x01-y07 +Title: doi:10.17182/hepdata.73336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 1.243000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 7.750000e-01 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 1.087000e+00 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 1.105000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.198000e+00 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 1.258000e+00 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 1.295000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 1.314000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 1.323000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d02-x01-y08 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d02-x01-y08 +Title: doi:10.17182/hepdata.73336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 1.049000e+00 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 1.052000e+00 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 1.053000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.051000e+00 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d02-x01-y09 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d02-x01-y09 +Title: doi:10.17182/hepdata.73336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 5.500000e+00 4.604346e+00 7.102816e+00 +3.900000e+00 0.000000e+00 0.000000e+00 7.900000e+00 5.907622e+00 9.204890e+00 +4.090000e+00 0.000000e+00 0.000000e+00 1.220000e+01 6.264982e+00 9.044888e+00 +4.310000e+00 0.000000e+00 0.000000e+00 0.000000e+00 2.900000e+00 7.200000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.170000e+01 5.433231e+00 8.521150e+00 +4.470000e+00 0.000000e+00 0.000000e+00 -1.200000e+00 1.902630e+00 3.501428e+00 +4.530000e+00 0.000000e+00 0.000000e+00 4.300000e+00 2.807134e+00 4.304649e+00 +4.575000e+00 0.000000e+00 0.000000e+00 4.300000e+00 3.805260e+00 7.702597e+00 +4.600000e+00 0.000000e+00 0.000000e+00 -8.000000e-01 6.082763e-01 9.055385e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d02-x01-y10 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d02-x01-y10 +Title: doi:10.17182/hepdata.73336.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d03-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d03-x01-y01 +Title: doi:10.17182/hepdata.73336.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.190000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d03-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d03-x01-y02 +Title: doi:10.17182/hepdata.73336.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.190000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 8.000000e+00 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 5.000000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d03-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d03-x01-y03 +Title: doi:10.17182/hepdata.73336.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.190000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 1.000000e+01 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 2.000000e+01 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d03-x01-y04 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d03-x01-y04 +Title: doi:10.17182/hepdata.73336.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 1.690000e+01 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 2.920000e+01 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 2.570000e+01 0.000000e+00 0.000000e+00 +4.190000e+00 0.000000e+00 0.000000e+00 2.990000e+01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 2.900000e+01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 2.850000e+01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 2.810000e+01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 2.730000e+01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 2.650000e+01 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 2.460000e+01 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 2.350000e+01 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 2.310000e+01 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 2.270000e+01 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 2.230000e+01 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 2.180000e+01 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 2.170000e+01 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 2.160000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d03-x01-y05 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d03-x01-y05 +Title: doi:10.17182/hepdata.73336.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d03-x01-y06 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d03-x01-y06 +Title: doi:10.17182/hepdata.73336.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 1.243000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 7.750000e-01 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 1.078000e+00 0.000000e+00 0.000000e+00 +4.190000e+00 0.000000e+00 0.000000e+00 8.660000e-01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 9.140000e-01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 9.370000e-01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 9.600000e-01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 9.920000e-01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 1.021000e+00 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 1.105000e+00 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.168000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.198000e+00 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.225000e+00 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 1.258000e+00 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 1.295000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 1.314000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 1.323000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d03-x01-y07 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d03-x01-y07 +Title: doi:10.17182/hepdata.73336.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.810000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +3.900000e+00 0.000000e+00 0.000000e+00 1.049000e+00 0.000000e+00 0.000000e+00 +4.090000e+00 0.000000e+00 0.000000e+00 1.052000e+00 0.000000e+00 0.000000e+00 +4.190000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 1.057000e+00 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 1.057000e+00 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 1.054000e+00 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 1.053000e+00 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.051000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.051000e+00 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.053000e+00 0.000000e+00 0.000000e+00 +4.470000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +4.530000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1355215/d03-x01-y08 +IsRef: 1 +Path: /REF/BESIII_2015_I1355215/d03-x01-y08 +Title: doi:10.17182/hepdata.73336.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2015_I1358937.cc b/analyses/pluginBES/BESIII_2015_I1358937.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1358937.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2015_I1358937 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2015_I1358937); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nproton = bookCounter("TMP/proton"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PROTON) vetoEvent; + } + _nproton->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nproton->val(); + double error = _nproton->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 5)); + Scatter2DPtr mult = bookScatter2D(1, 1, 5); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nproton; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2015_I1358937); + + +} diff --git a/analyses/pluginBES/BESIII_2015_I1358937.info b/analyses/pluginBES/BESIII_2015_I1358937.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1358937.info @@ -0,0 +1,34 @@ +Name: BESIII_2015_I1358937 +Year: 2015 +Summary: Cross section for $e^+e^-\to$ proton and antiproton between 2.2324 and 3.671 GeV +Experiment: BESIII +Collider: BEPC II +InspireID: 1358937 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D91 (2015) 112004, 2015 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ for energies between 2.2324 and 3.671 GeV' +Keywords: +BibKey: Ablikim:2015vga +BibTeX: '@article{Ablikim:2015vga, + author = "Ablikim, M. and others", + title = "{Measurement of the proton form factor by studying $e^{+} + e^{-}\rightarrow p\bar{p}$}", + collaboration = "BESIII", + journal = "Phys. Rev.", + volume = "D91", + year = "2015", + number = "11", + pages = "112004", + doi = "10.1103/PhysRevD.91.112004", + eprint = "1504.02680", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1504.02680;%%" +}' diff --git a/analyses/pluginBES/BESIII_2015_I1358937.plot b/analyses/pluginBES/BESIII_2015_I1358937.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1358937.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BESIII_2015_I1358937/d01-x01-y05 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESIII_2015_I1358937.yoda b/analyses/pluginBES/BESIII_2015_I1358937.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1358937.yoda @@ -0,0 +1,120 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1358937/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2015_I1358937/d01-x01-y01 +Title: doi:10.17182/hepdata.73442.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.232400e+00 0.000000e+00 0.000000e+00 6.140000e+02 2.500000e+01 2.500000e+01 +2.400000e+00 0.000000e+00 0.000000e+00 2.970000e+02 1.700000e+01 1.700000e+01 +2.800000e+00 0.000000e+00 0.000000e+00 5.300000e+01 7.000000e+00 7.000000e+00 +3.050000e+00 0.000000e+00 0.000000e+00 9.100000e+01 1.000000e+01 1.000000e+01 +3.060000e+00 0.000000e+00 0.000000e+00 7.800000e+01 9.000000e+00 9.000000e+00 +3.080000e+00 0.000000e+00 0.000000e+00 1.620000e+02 1.300000e+01 1.300000e+01 +3.400000e+00 0.000000e+00 0.000000e+00 2.000000e+00 1.000000e+00 1.000000e+00 +3.500000e+00 0.000000e+00 0.000000e+00 5.000000e+00 2.000000e+00 2.000000e+00 +3.550700e+00 0.000000e+00 0.000000e+00 2.400000e+01 5.000000e+00 5.000000e+00 +3.600200e+00 0.000000e+00 0.000000e+00 1.400000e+01 4.000000e+00 4.000000e+00 +3.650000e+00 0.000000e+00 0.000000e+00 3.600000e+01 6.000000e+00 6.000000e+00 +3.671000e+00 0.000000e+00 0.000000e+00 6.000000e+00 2.000000e+00 2.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1358937/d01-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2015_I1358937/d01-x01-y02 +Title: doi:10.17182/hepdata.73442.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.232400e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +2.400000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +2.800000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +3.050000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +3.060000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +3.080000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +3.400000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.550700e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +3.600200e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +3.650000e+00 0.000000e+00 0.000000e+00 4.000000e+00 0.000000e+00 0.000000e+00 +3.671000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1358937/d01-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2015_I1358937/d01-x01-y03 +Title: doi:10.17182/hepdata.73442.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.232400e+00 0.000000e+00 0.000000e+00 6.600000e+01 0.000000e+00 0.000000e+00 +2.400000e+00 0.000000e+00 0.000000e+00 6.579000e+01 0.000000e+00 0.000000e+00 +2.800000e+00 0.000000e+00 0.000000e+00 6.508000e+01 0.000000e+00 0.000000e+00 +3.050000e+00 0.000000e+00 0.000000e+00 5.911000e+01 0.000000e+00 0.000000e+00 +3.060000e+00 0.000000e+00 0.000000e+00 5.921000e+01 0.000000e+00 0.000000e+00 +3.080000e+00 0.000000e+00 0.000000e+00 5.897000e+01 0.000000e+00 0.000000e+00 +3.400000e+00 0.000000e+00 0.000000e+00 6.334000e+01 0.000000e+00 0.000000e+00 +3.500000e+00 0.000000e+00 0.000000e+00 6.370000e+01 0.000000e+00 0.000000e+00 +3.550700e+00 0.000000e+00 0.000000e+00 6.223000e+01 0.000000e+00 0.000000e+00 +3.600200e+00 0.000000e+00 0.000000e+00 6.224000e+01 0.000000e+00 0.000000e+00 +3.650000e+00 0.000000e+00 0.000000e+00 6.120000e+01 0.000000e+00 0.000000e+00 +3.671000e+00 0.000000e+00 0.000000e+00 5.117000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1358937/d01-x01-y04 +IsRef: 1 +Path: /REF/BESIII_2015_I1358937/d01-x01-y04 +Title: doi:10.17182/hepdata.73442.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.232400e+00 0.000000e+00 0.000000e+00 2.630000e+00 0.000000e+00 0.000000e+00 +2.400000e+00 0.000000e+00 0.000000e+00 3.420000e+00 0.000000e+00 0.000000e+00 +2.800000e+00 0.000000e+00 0.000000e+00 3.750000e+00 0.000000e+00 0.000000e+00 +3.050000e+00 0.000000e+00 0.000000e+00 1.490000e+01 0.000000e+00 0.000000e+00 +3.060000e+00 0.000000e+00 0.000000e+00 1.506000e+01 0.000000e+00 0.000000e+00 +3.080000e+00 0.000000e+00 0.000000e+00 3.073000e+01 0.000000e+00 0.000000e+00 +3.400000e+00 0.000000e+00 0.000000e+00 1.730000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 0.000000e+00 0.000000e+00 3.610000e+00 0.000000e+00 0.000000e+00 +3.550700e+00 0.000000e+00 0.000000e+00 1.815000e+01 0.000000e+00 0.000000e+00 +3.600200e+00 0.000000e+00 0.000000e+00 9.550000e+00 0.000000e+00 0.000000e+00 +3.650000e+00 0.000000e+00 0.000000e+00 4.882000e+01 0.000000e+00 0.000000e+00 +3.671000e+00 0.000000e+00 0.000000e+00 4.590000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1358937/d01-x01-y05 +IsRef: 1 +Path: /REF/BESIII_2015_I1358937/d01-x01-y05 +Title: doi:10.17182/hepdata.73442.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.232400e+00 0.000000e+00 0.000000e+00 3.530000e+02 2.108886e+01 2.108886e+01 +2.400000e+00 0.000000e+00 0.000000e+00 1.327000e+02 1.117587e+01 1.117587e+01 +2.800000e+00 0.000000e+00 0.000000e+00 2.130000e+01 4.103657e+00 4.103657e+00 +3.050000e+00 0.000000e+00 0.000000e+00 1.010000e+01 1.252996e+00 1.252996e+00 +3.060000e+00 0.000000e+00 0.000000e+00 8.500000e+00 1.166190e+00 1.166190e+00 +3.080000e+00 0.000000e+00 0.000000e+00 8.900000e+00 8.602325e-01 8.602325e-01 +3.400000e+00 0.000000e+00 0.000000e+00 1.800000e+00 1.360147e+00 1.360147e+00 +3.500000e+00 0.000000e+00 0.000000e+00 2.200000e+00 1.166190e+00 1.166190e+00 +3.550700e+00 0.000000e+00 0.000000e+00 2.000000e+00 7.211103e-01 7.211103e-01 +3.600200e+00 0.000000e+00 0.000000e+00 2.200000e+00 1.081665e+00 1.081665e+00 +3.650000e+00 0.000000e+00 0.000000e+00 1.100000e+00 2.236068e-01 2.236068e-01 +3.671000e+00 0.000000e+00 0.000000e+00 2.200000e+00 1.204159e+00 1.204159e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1358937/d01-x01-y06 +IsRef: 1 +Path: /REF/BESIII_2015_I1358937/d01-x01-y06 +Title: doi:10.17182/hepdata.73442.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.232400e+00 0.000000e+00 0.000000e+00 1.610000e+01 4.742362e-01 4.742362e-01 +2.400000e+00 0.000000e+00 0.000000e+00 1.007000e+01 4.244997e-01 4.244997e-01 +2.800000e+00 0.000000e+00 0.000000e+00 4.450000e+00 4.244997e-01 4.244997e-01 +3.050000e+00 0.000000e+00 0.000000e+00 3.290000e+00 1.923538e-01 1.923538e-01 +3.060000e+00 0.000000e+00 0.000000e+00 3.030000e+00 1.972308e-01 1.972308e-01 +3.080000e+00 0.000000e+00 0.000000e+00 3.110000e+00 1.442221e-01 1.442221e-01 +3.400000e+00 0.000000e+00 0.000000e+00 1.540000e+00 5.787055e-01 5.787055e-01 +3.500000e+00 0.000000e+00 0.000000e+00 1.730000e+00 4.477723e-01 4.477723e-01 +3.550700e+00 0.000000e+00 0.000000e+00 1.670000e+00 2.860070e-01 2.860070e-01 +3.600200e+00 0.000000e+00 0.000000e+00 1.780000e+00 4.301163e-01 4.301163e-01 +3.650000e+00 0.000000e+00 0.000000e+00 1.260000e+00 1.303840e-01 1.303840e-01 +3.671000e+00 0.000000e+00 0.000000e+00 1.840000e+00 4.957822e-01 4.957822e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2015_I1364494.cc b/analyses/pluginBES/BESIII_2015_I1364494.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1364494.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2015_I1364494 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2015_I1364494); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(), "UFS"); + + // Book histograms + _h_m = bookHisto1D(1, 1, 3); + _netap = 0.; + } + + void findDecayProducts(const Particle & mother, unsigned int & nstable, unsigned int & ngamma, + unsigned int & nep, unsigned int & nem, FourMomentum & ptot) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if (id == PID::EMINUS ) { + ++nem; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::EPLUS) { + ++nep; + ++nstable; + ptot += p.momentum(); + } + else if ( !p.children().empty() ) { + findDecayProducts(p, nstable, ngamma,nep,nem,ptot); + } + else if (id == PID::GAMMA) { + ++ngamma; + ++nstable; + } + else + ++nstable; + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + // Loop over eta' mesons + foreach(const Particle& p, apply(event, "UFS").particles(Cuts::pid==331)) { + unsigned nstable(0),ngamma(0),nep(0),nem(0); + FourMomentum ptot; + findDecayProducts(p,nstable,ngamma,nep,nem,ptot); + if(nstable==3 && nem==1 && nem==1 && ngamma==1) + _h_m->fill(ptot.mass(),event.weight()); + else if(nstable==2 &&ngamma==2) + _netap+=event.weight(); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + // divide by no so BR and mult by bin width + // and 100 as in % + scale(_h_m,1./_netap*0.1*100.); + + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _h_m; + double _netap; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2015_I1364494); + + +} diff --git a/analyses/pluginBES/BESIII_2015_I1364494.info b/analyses/pluginBES/BESIII_2015_I1364494.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1364494.info @@ -0,0 +1,35 @@ +Name: BESIII_2015_I1364494 +Year: 2015 +Summary: $\eta^\prime\to e^+e^-\gamma$ decays +Experiment: BESIII +Collider: BEPC +InspireID: 1364494 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D92 (2015) 012001, 2015 +RunInfo: + Events with eta prime decays, either particle guns or collisions. +NumEvents: 10000 +NeedCrossSection: no +Description: + 'Differential decay rates for $\eta^\prime\to e^+e^-\gamma$ decays' +Keywords: [] +BibKey: Ablikim:2015wnx +BibTeX: '@article{Ablikim:2015wnx, + author = "Ablikim, M. and others", + title = "{Observation of the Dalitz Decay $\eta^\prime \to \gamma + e^+e^-$}", + collaboration = "BESIII", + journal = "Phys. Rev.", + volume = "D92", + year = "2015", + number = "1", + pages = "012001", + doi = "10.1103/PhysRevD.92.012001", + eprint = "1504.06016", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1504.06016;%%" +}' diff --git a/analyses/pluginBES/BESIII_2015_I1364494.plot b/analyses/pluginBES/BESIII_2015_I1364494.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1364494.plot @@ -0,0 +1,5 @@ +BEGIN PLOT /BESIII_2015_I1364494/d01-x01-y03 +Title=Differential $\eta^\prime\to e^+e^-\gamma$ decay +XLabel=$M(e^+e^-)$/GeV +YLabel=$\Gamma(e^+e^-\gamma)/\Gamma(\gamma\gamma)$/\% +END PLOT diff --git a/analyses/pluginBES/BESIII_2015_I1364494.yoda b/analyses/pluginBES/BESIII_2015_I1364494.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1364494.yoda @@ -0,0 +1,64 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1364494/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2015_I1364494/d01-x01-y01 +Title: doi:10.17182/hepdata.73672.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-02 5.000000e-02 5.000000e-02 5.450000e+02 2.700000e+01 2.700000e+01 +1.500000e-01 5.000000e-02 5.000000e-02 8.650000e+01 1.070000e+01 1.070000e+01 +2.500000e-01 5.000000e-02 5.000000e-02 6.210000e+01 9.800000e+00 9.800000e+00 +3.500000e-01 5.000000e-02 5.000000e-02 4.560000e+01 9.700000e+00 9.700000e+00 +4.500000e-01 5.000000e-02 5.000000e-02 4.540000e+01 9.000000e+00 9.000000e+00 +5.500000e-01 5.000000e-02 5.000000e-02 2.990000e+01 8.000000e+00 8.000000e+00 +6.500000e-01 5.000000e-02 5.000000e-02 2.800000e+01 7.800000e+00 7.800000e+00 +7.500000e-01 5.000000e-02 5.000000e-02 2.500000e+01 6.900000e+00 6.900000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1364494/d01-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2015_I1364494/d01-x01-y02 +Title: doi:10.17182/hepdata.73672.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-02 5.000000e-02 5.000000e-02 2.380000e+03 1.200000e+02 1.200000e+02 +1.500000e-01 5.000000e-02 5.000000e-02 3.680000e+02 4.600000e+01 4.600000e+01 +2.500000e-01 5.000000e-02 5.000000e-02 1.940000e+02 3.100000e+01 3.100000e+01 +3.500000e-01 5.000000e-02 5.000000e-02 1.280000e+02 2.700000e+01 2.700000e+01 +4.500000e-01 5.000000e-02 5.000000e-02 1.350000e+02 2.700000e+01 2.700000e+01 +5.500000e-01 5.000000e-02 5.000000e-02 9.330000e+01 2.500000e+01 2.500000e+01 +6.500000e-01 5.000000e-02 5.000000e-02 9.620000e+01 2.680000e+01 2.680000e+01 +7.500000e-01 5.000000e-02 5.000000e-02 1.090000e+02 3.000000e+01 3.000000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1364494/d01-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2015_I1364494/d01-x01-y03 +Title: doi:10.17182/hepdata.73672.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-02 5.000000e-02 5.000000e-02 1.440000e+00 7.000000e-02 7.000000e-02 +1.500000e-01 5.000000e-02 5.000000e-02 2.200000e-01 3.000000e-02 3.000000e-02 +2.500000e-01 5.000000e-02 5.000000e-02 1.200000e-01 2.000000e-02 2.000000e-02 +3.500000e-01 5.000000e-02 5.000000e-02 8.000000e-02 2.000000e-02 2.000000e-02 +4.500000e-01 5.000000e-02 5.000000e-02 8.000000e-02 2.000000e-02 2.000000e-02 +5.500000e-01 5.000000e-02 5.000000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +6.500000e-01 5.000000e-02 5.000000e-02 6.000000e-02 2.000000e-02 2.000000e-02 +7.500000e-01 5.000000e-02 5.000000e-02 7.000000e-02 2.000000e-02 2.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1364494/d02-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2015_I1364494/d02-x01-y01 +Title: doi:10.17182/hepdata.73672.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-02 5.000000e-02 5.000000e-02 1.050000e+00 5.830952e-02 5.830952e-02 +1.500000e-01 5.000000e-02 5.000000e-02 1.120000e+00 1.456022e-01 1.456022e-01 +2.500000e-01 5.000000e-02 5.000000e-02 1.160000e+00 1.868154e-01 1.868154e-01 +3.500000e-01 5.000000e-02 5.000000e-02 1.330000e+00 2.844293e-01 2.844293e-01 +4.500000e-01 5.000000e-02 5.000000e-02 2.480000e+00 5.500909e-01 5.500909e-01 +5.500000e-01 5.000000e-02 5.000000e-02 3.300000e+00 9.330059e-01 9.330059e-01 +6.500000e-01 5.000000e-02 5.000000e-02 7.660000e+00 2.308463e+00 2.308463e+00 +7.500000e-01 5.000000e-02 5.000000e-02 2.660000e+01 7.543209e+00 7.543209e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2015_I1377204.cc b/analyses/pluginBES/BESIII_2015_I1377204.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1377204.cc @@ -0,0 +1,119 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2015_I1377204 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2015_I1377204); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nJPsi = bookCounter("TMP/jpsi"); + } + + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the j/psi + if(p.pdgId()==443) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // J/psi pi0pi0 + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==111) { + if(val.second !=2) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nJPsi->fill(event.weight()); + break; + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nJPsi->val(); + double error = _nJPsi->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 12)); + Scatter2DPtr mult = bookScatter2D(1, 1, 12); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nJPsi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2015_I1377204); + + +} diff --git a/analyses/pluginBES/BESIII_2015_I1377204.info b/analyses/pluginBES/BESIII_2015_I1377204.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1377204.info @@ -0,0 +1,35 @@ +Name: BESIII_2015_I1377204 +Year: 2015 +Summary: Cross section for $e^+e^-\to J/\psi \pi^0\pi^0$ at energies between 4.19 and 4.42 GeV +Experiment: BESIII +Collider: BEPC +InspireID: 1377204 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 115 (2015) 112003, 2015 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to J/\psi \pi^0\pi^0$ at energies between 4.19 and 4.42 GeV' +Keywords: [] +BibKey: Ablikim:2015tbp +BibTeX: '@article{Ablikim:2015tbp, + author = "Ablikim, M. and others", + title = "{Observation of $Z_c(3900)^{0}$ in $e^+e^-\to\pi^0\pi^0 + J/\psi$}", + collaboration = "BESIII", + journal = "Phys. Rev. Lett.", + volume = "115", + year = "2015", + number = "11", + pages = "112003", + doi = "10.1103/PhysRevLett.115.112003", + eprint = "1506.06018", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1506.06018;%%" +}' diff --git a/analyses/pluginBES/BESIII_2015_I1377204.plot b/analyses/pluginBES/BESIII_2015_I1377204.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1377204.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BESIII_2015_I1377204/d01-x01-y12 +Title=$\sigma(e^+e^-\to \pi^0\pi^0 J/\psi)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^0\pi^0 J/\psi)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESIII_2015_I1377204.yoda b/analyses/pluginBES/BESIII_2015_I1377204.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1377204.yoda @@ -0,0 +1,199 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y01 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 4.310000e+01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 5.460000e+01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 5.410000e+01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 1.091700e+03 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 5.560000e+01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 8.257000e+02 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 4.490000e+01 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 5.398000e+02 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 5.520000e+01 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 4.470000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y02 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 2.080000e+01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 2.150000e+01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 2.160000e+01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 2.200000e+01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 2.230000e+01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 2.260000e+01 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 2.250000e+01 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 2.150000e+01 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 2.140000e+01 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 2.170000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y03 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 2.040000e+01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 2.100000e+01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 2.120000e+01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 2.110000e+01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 2.160000e+01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 2.120000e+01 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 2.040000e+01 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.880000e+01 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.770000e+01 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.680000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y04 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y04 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 2.010000e+01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 2.080000e+01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 2.080000e+01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 2.100000e+01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 2.110000e+01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 2.140000e+01 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 2.070000e+01 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.910000e+01 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.840000e+01 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.790000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y05 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y05 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 2.020000e+01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 2.090000e+01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 2.110000e+01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 2.100000e+01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 2.150000e+01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 2.120000e+01 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 2.050000e+01 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.890000e+01 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.770000e+01 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.680000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y06 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y06 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.230000e+00 0.000000e+00 0.000000e+00 2.368000e+02 2.500000e+01 2.500000e+01 +4.260000e+00 0.000000e+00 0.000000e+00 7.310000e+01 1.650000e+01 1.650000e+01 +4.360000e+00 0.000000e+00 0.000000e+00 4.180000e+01 1.080000e+01 1.080000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y07 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y07 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 8.200000e+00 3.000000e+00 3.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 2.660000e+01 5.400000e+00 5.400000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 3.190000e+01 5.700000e+00 5.700000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 8.251000e+02 2.980000e+01 2.980000e+01 +4.245000e+00 0.000000e+00 0.000000e+00 4.900000e+01 7.100000e+00 7.100000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 5.073000e+02 2.340000e+01 2.340000e+01 +4.310000e+00 0.000000e+00 0.000000e+00 2.550000e+01 5.100000e+00 5.100000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.828000e+02 1.420000e+01 1.420000e+01 +4.390000e+00 0.000000e+00 0.000000e+00 6.200000e+00 2.600000e+00 2.600000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 2.900000e+00 2.100000e+00 2.100000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y08 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y08 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 7.100000e-01 4.517743e-01 4.517743e-01 +4.210000e+00 0.000000e+00 0.000000e+00 4.200000e-01 2.121320e-01 2.121320e-01 +4.220000e+00 0.000000e+00 0.000000e+00 1.800000e-01 1.414214e-01 1.414214e-01 +4.230000e+00 0.000000e+00 0.000000e+00 2.800000e-01 3.605551e-02 3.605551e-02 +4.245000e+00 0.000000e+00 0.000000e+00 1.500000e-01 1.019804e-01 1.019804e-01 +4.260000e+00 0.000000e+00 0.000000e+00 1.400000e-01 3.162278e-02 3.162278e-02 +4.310000e+00 0.000000e+00 0.000000e+00 7.000000e-02 1.204159e-01 1.204159e-01 +4.360000e+00 0.000000e+00 0.000000e+00 2.000000e-01 5.385165e-02 5.385165e-02 +4.390000e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.020000e+00 1.020000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 0.000000e+00 5.600000e-01 5.600000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y09 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y09 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y10 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y10 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 8.280000e-01 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 8.130000e-01 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 8.100000e-01 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 8.050000e-01 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 8.060000e-01 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 8.150000e-01 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 9.160000e-01 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.038000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.088000e+00 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.132000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y11 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y11 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.210000e+00 0.000000e+00 0.000000e+00 1.057000e+00 0.000000e+00 0.000000e+00 +4.220000e+00 0.000000e+00 0.000000e+00 1.057000e+00 0.000000e+00 0.000000e+00 +4.230000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.245000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.260000e+00 0.000000e+00 0.000000e+00 1.054000e+00 0.000000e+00 0.000000e+00 +4.310000e+00 0.000000e+00 0.000000e+00 1.052000e+00 0.000000e+00 0.000000e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.051000e+00 0.000000e+00 0.000000e+00 +4.390000e+00 0.000000e+00 0.000000e+00 1.051000e+00 0.000000e+00 0.000000e+00 +4.420000e+00 0.000000e+00 0.000000e+00 1.053000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1377204/d01-x01-y12 +IsRef: 1 +Path: /REF/BESIII_2015_I1377204/d01-x01-y12 +Title: doi:10.17182/hepdata.73771.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.190000e+00 0.000000e+00 0.000000e+00 9.000000e+00 3.354102e+00 3.354102e+00 +4.210000e+00 0.000000e+00 0.000000e+00 2.270000e+01 4.838388e+00 4.838388e+00 +4.220000e+00 0.000000e+00 0.000000e+00 2.740000e+01 5.220153e+00 5.220153e+00 +4.230000e+00 0.000000e+00 0.000000e+00 3.540000e+01 2.555386e+00 2.555386e+00 +4.245000e+00 0.000000e+00 0.000000e+00 4.030000e+01 6.397656e+00 6.397656e+00 +4.260000e+00 0.000000e+00 0.000000e+00 2.830000e+01 2.220360e+00 2.220360e+00 +4.310000e+00 0.000000e+00 0.000000e+00 2.410000e+01 5.154610e+00 5.154610e+00 +4.360000e+00 0.000000e+00 0.000000e+00 1.380000e+01 1.421267e+00 1.421267e+00 +4.390000e+00 0.000000e+00 0.000000e+00 4.700000e+00 1.923538e+00 1.923538e+00 +4.420000e+00 0.000000e+00 0.000000e+00 2.700000e+00 1.910497e+00 1.910497e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2015_I1391138.cc b/analyses/pluginBES/BESIII_2015_I1391138.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1391138.cc @@ -0,0 +1,85 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Based on BABAR_2015_I1334693 + class BESIII_2015_I1391138 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2015_I1391138); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(), "UFS"); + + // Book histograms + _h_q2_K = bookHisto1D(1, 1, 3); + _h_q2_pi = bookHisto1D(2, 1, 3); + nD0 = 0.; + } + + // Calculate the Q2 using mother and daugher meson + double q2(const Particle& B, int mesonID) { + FourMomentum q = B.mom() - filter_select(B.children(), Cuts::pid==mesonID)[0]; + return q*q; + } + + // Check for explicit decay into pdgids + bool isSemileptonicDecay(const Particle& mother, vector ids) { + // Trivial check to ignore any other decays but the one in question modulo photons + const Particles children = mother.children(Cuts::pid!=PID::PHOTON); + if (children.size()!=ids.size()) return false; + // Check for the explicit decay + return all(ids, [&](int i){return count(children, hasPID(i))==1;}); + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + // Loop over D0 mesons + foreach(const Particle& p, apply(event, "UFS").particles(Cuts::pid==PID::D0)) { + nD0 += event.weight(); + if (isSemileptonicDecay(p, {PID::PIMINUS, PID::POSITRON, PID::NU_E})) { + _h_q2_pi->fill(q2(p, PID::PIMINUS), event.weight()); + } + else if(isSemileptonicDecay(p, {PID::KMINUS, PID::POSITRON, PID::NU_E})) { + _h_q2_K ->fill(q2(p, PID::KMINUS), event.weight()); + } + } + } + + /// Normalise histograms etc., after the run + void finalize() { + // scale by D0 lifetime = 410.1e-6 ps (from PDG 2014 used in paper) + // and bin width 0.1 K and 0.2 pi + scale(_h_q2_K , 1./nD0/410.1e-6*0.1); + scale(_h_q2_pi, 1./nD0/410.1e-6*0.2); + } + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _h_q2_K,_h_q2_pi; + double nD0; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2015_I1391138); + + +} diff --git a/analyses/pluginBES/BESIII_2015_I1391138.info b/analyses/pluginBES/BESIII_2015_I1391138.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1391138.info @@ -0,0 +1,35 @@ +Name: BESIII_2015_I1391138 +Year: 2015 +Summary: Exclusive $D^0\to K^-,\pi^-e^+\nu_e$ decays +Experiment: BESIII +Collider: BEPC +InspireID: 1391138 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D92 (2015) 072012, 2015 +RunInfo: + Events with D-decays, either particle guns or collisions. +NumEvents: 10000 +NeedCrossSection: no +Description: + 'Differential decay rates for semileptonic $D^0\to K^-,\pi^-e^+\nu_e$ decays' +Keywords: [] +BibKey: Ablikim:2015ixa +BibTeX: '@article{Ablikim:2015ixa, + author = "Ablikim, M. and others", + title = "{Study of Dynamics of $D^0 \to K^- e^+ \nu_{e}$ and + $D^0\to\pi^- e^+ \nu_{e}$ Decays}", + collaboration = "BESIII", + journal = "Phys. Rev.", + volume = "D92", + year = "2015", + number = "7", + pages = "072012", + doi = "10.1103/PhysRevD.92.072012", + eprint = "1508.07560", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1508.07560;%%" +}' diff --git a/analyses/pluginBES/BESIII_2015_I1391138.plot b/analyses/pluginBES/BESIII_2015_I1391138.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1391138.plot @@ -0,0 +1,10 @@ +BEGIN PLOT /BESIII_2015_I1391138/d01-x01-y03 +Title=$D^0\to K^- e^+ \nu_e$ +XLabel=$q^2/$GeV$^2$ +YLabel=$\Delta\Gamma/$ns$^{-1}$ +END PLOT +BEGIN PLOT /BESIII_2015_I1391138/d02-x01-y03 +Title=$D^0\to \pi^- e^+ \nu_e$ +XLabel=$q^2/$GeV$^2$ +YLabel=$\Delta\Gamma/$ns$^{-1}$ +END PLOT diff --git a/analyses/pluginBES/BESIII_2015_I1391138.yoda b/analyses/pluginBES/BESIII_2015_I1391138.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2015_I1391138.yoda @@ -0,0 +1,144 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1391138/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2015_I1391138/d01-x01-y01 +Title: doi:10.17182/hepdata.74726.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.050000e+00 5.000000e-02 5.000000e-02 7.876100e+03 9.420000e+01 9.420000e+01 +0.150000e+00 5.000000e-02 5.000000e-02 7.504300e+03 9.050000e+01 9.050000e+01 +0.250000e+00 5.000000e-02 5.000000e-02 6.940500e+03 8.720000e+01 8.720000e+01 +0.350000e+00 5.000000e-02 5.000000e-02 6.376000e+03 8.340000e+01 8.340000e+01 +0.450000e+00 5.000000e-02 5.000000e-02 6.139800e+03 8.190000e+01 8.190000e+01 +0.550000e+00 5.000000e-02 5.000000e-02 5.460500e+03 7.710000e+01 7.710000e+01 +0.650000e+00 5.000000e-02 5.000000e-02 5.120300e+03 7.470000e+01 7.470000e+01 +0.750000e+00 5.000000e-02 5.000000e-02 4.545500e+03 7.050000e+01 7.050000e+01 +0.850000e+00 5.000000e-02 5.000000e-02 4.159400e+03 6.710000e+01 6.710000e+01 +0.950000e+00 5.000000e-02 5.000000e-02 3.680700e+03 6.320000e+01 6.320000e+01 +1.050000e+00 5.000000e-02 5.000000e-02 3.199600e+03 5.890000e+01 5.890000e+01 +1.150000e+00 5.000000e-02 5.000000e-02 2.637100e+03 5.350000e+01 5.350000e+01 +1.250000e+00 5.000000e-02 5.000000e-02 2.239100e+03 4.940000e+01 4.940000e+01 +1.350000e+00 5.000000e-02 5.000000e-02 1.752100e+03 4.390000e+01 4.390000e+01 +1.450000e+00 5.000000e-02 5.000000e-02 1.301000e+03 3.770000e+01 3.770000e+01 +1.550000e+00 5.000000e-02 5.000000e-02 9.275000e+02 3.200000e+01 3.200000e+01 +1.650000e+00 5.000000e-02 5.000000e-02 5.413000e+02 2.460000e+01 2.460000e+01 +1.750000e+00 5.000000e-02 5.000000e-02 1.882000e+02 1.510000e+01 1.510000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1391138/d01-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2015_I1391138/d01-x01-y02 +Title: doi:10.17182/hepdata.74726.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.050000e+00 5.000000e-02 5.000000e-02 1.009490e+04 1.323000e+02 1.323000e+02 +0.150000e+00 5.000000e-02 5.000000e-02 1.001540e+04 1.408000e+02 1.408000e+02 +0.250000e+00 5.000000e-02 5.000000e-02 9.502600e+03 1.420000e+02 1.420000e+02 +0.350000e+00 5.000000e-02 5.000000e-02 8.667900e+03 1.386000e+02 1.386000e+02 +0.450000e+00 5.000000e-02 5.000000e-02 8.575900e+03 1.377000e+02 1.377000e+02 +0.550000e+00 5.000000e-02 5.000000e-02 7.384000e+03 1.281000e+02 1.281000e+02 +0.650000e+00 5.000000e-02 5.000000e-02 7.101800e+03 1.258000e+02 1.258000e+02 +0.750000e+00 5.000000e-02 5.000000e-02 6.322200e+03 1.202000e+02 1.202000e+02 +0.850000e+00 5.000000e-02 5.000000e-02 5.760300e+03 1.133000e+02 1.133000e+02 +0.950000e+00 5.000000e-02 5.000000e-02 5.183500e+03 1.076000e+02 1.076000e+02 +1.050000e+00 5.000000e-02 5.000000e-02 4.550000e+03 1.002000e+02 1.002000e+02 +1.150000e+00 5.000000e-02 5.000000e-02 3.810200e+03 9.240000e+01 9.240000e+01 +1.250000e+00 5.000000e-02 5.000000e-02 3.239100e+03 8.430000e+01 8.430000e+01 +1.350000e+00 5.000000e-02 5.000000e-02 2.621200e+03 7.730000e+01 7.730000e+01 +1.450000e+00 5.000000e-02 5.000000e-02 1.989400e+03 6.740000e+01 6.740000e+01 +1.550000e+00 5.000000e-02 5.000000e-02 1.505100e+03 5.900000e+01 5.900000e+01 +1.650000e+00 5.000000e-02 5.000000e-02 9.834000e+02 5.030000e+01 5.030000e+01 +1.750000e+00 5.000000e-02 5.000000e-02 4.342000e+02 3.960000e+01 3.960000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1391138/d01-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2015_I1391138/d01-x01-y03 +Title: doi:10.17182/hepdata.74726.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.050000e+00 5.000000e-02 5.000000e-02 8.812000e+00 1.160000e-01 1.160000e-01 +0.150000e+00 5.000000e-02 5.000000e-02 8.743000e+00 1.230000e-01 1.230000e-01 +0.250000e+00 5.000000e-02 5.000000e-02 8.295000e+00 1.240000e-01 1.240000e-01 +0.350000e+00 5.000000e-02 5.000000e-02 7.567000e+00 1.210000e-01 1.210000e-01 +0.450000e+00 5.000000e-02 5.000000e-02 7.486000e+00 1.200000e-01 1.200000e-01 +0.550000e+00 5.000000e-02 5.000000e-02 6.446000e+00 1.120000e-01 1.120000e-01 +0.650000e+00 5.000000e-02 5.000000e-02 6.200000e+00 1.100000e-01 1.100000e-01 +0.750000e+00 5.000000e-02 5.000000e-02 5.519000e+00 1.050000e-01 1.050000e-01 +0.850000e+00 5.000000e-02 5.000000e-02 5.028000e+00 9.900000e-02 9.900000e-02 +0.950000e+00 5.000000e-02 5.000000e-02 4.525000e+00 9.400000e-02 9.400000e-02 +1.050000e+00 5.000000e-02 5.000000e-02 3.972000e+00 8.700000e-02 8.700000e-02 +1.150000e+00 5.000000e-02 5.000000e-02 3.326000e+00 8.100000e-02 8.100000e-02 +1.250000e+00 5.000000e-02 5.000000e-02 2.828000e+00 7.400000e-02 7.400000e-02 +1.350000e+00 5.000000e-02 5.000000e-02 2.288000e+00 6.700000e-02 6.700000e-02 +1.450000e+00 5.000000e-02 5.000000e-02 1.737000e+00 5.900000e-02 5.900000e-02 +1.550000e+00 5.000000e-02 5.000000e-02 1.314000e+00 5.200000e-02 5.200000e-02 +1.650000e+00 5.000000e-02 5.000000e-02 8.580000e-01 4.400000e-02 4.400000e-02 +1.750000e+00 5.000000e-02 5.000000e-02 3.790000e-01 3.500000e-02 3.500000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1391138/d02-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2015_I1391138/d02-x01-y01 +Title: doi:10.17182/hepdata.74726.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.100000e+00 1.000000e-01 1.000000e-01 8.144000e+02 3.090000e+01 3.090000e+01 +0.300000e+00 1.000000e-01 1.000000e-01 6.972000e+02 2.870000e+01 2.870000e+01 +0.500000e+00 1.000000e-01 1.000000e-01 6.346000e+02 2.770000e+01 2.770000e+01 +0.700000e+00 1.000000e-01 1.000000e-01 6.546000e+02 2.780000e+01 2.780000e+01 +0.900000e+00 1.000000e-01 1.000000e-01 6.432000e+02 2.730000e+01 2.730000e+01 +1.100000e+00 1.000000e-01 1.000000e-01 5.786000e+02 2.630000e+01 2.630000e+01 +1.300000e+00 1.000000e-01 1.000000e-01 5.099000e+02 2.470000e+01 2.470000e+01 +1.500000e+00 1.000000e-01 1.000000e-01 4.386000e+02 2.320000e+01 2.320000e+01 +1.700000e+00 1.000000e-01 1.000000e-01 4.126000e+02 2.230000e+01 2.230000e+01 +1.900000e+00 1.000000e-01 1.000000e-01 3.209000e+02 1.980000e+01 1.980000e+01 +2.100000e+00 1.000000e-01 1.000000e-01 2.458000e+02 1.700000e+01 1.700000e+01 +2.300000e+00 1.000000e-01 1.000000e-01 1.654000e+02 1.410000e+01 1.410000e+01 +2.500000e+00 1.000000e-01 1.000000e-01 9.360000e+01 1.070000e+01 1.070000e+01 +2.700000e+00 1.000000e-01 1.000000e-01 7.580000e+01 1.000000e+01 1.000000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1391138/d02-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2015_I1391138/d02-x01-y02 +Title: doi:10.17182/hepdata.74726.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.100000e+00 1.000000e-01 1.000000e-01 1.066900e+03 4.320000e+01 4.320000e+01 +0.300000e+00 1.000000e-01 1.000000e-01 9.351000e+02 4.280000e+01 4.280000e+01 +0.500000e+00 1.000000e-01 1.000000e-01 8.366000e+02 4.130000e+01 4.130000e+01 +0.700000e+00 1.000000e-01 1.000000e-01 8.501000e+02 4.060000e+01 4.060000e+01 +0.900000e+00 1.000000e-01 1.000000e-01 8.402000e+02 3.990000e+01 3.990000e+01 +1.100000e+00 1.000000e-01 1.000000e-01 7.446000e+02 3.770000e+01 3.770000e+01 +1.300000e+00 1.000000e-01 1.000000e-01 6.511000e+02 3.510000e+01 3.510000e+01 +1.500000e+00 1.000000e-01 1.000000e-01 5.516000e+02 3.280000e+01 3.280000e+01 +1.700000e+00 1.000000e-01 1.000000e-01 5.347000e+02 3.170000e+01 3.170000e+01 +1.900000e+00 1.000000e-01 1.000000e-01 4.206000e+02 2.860000e+01 2.860000e+01 +2.100000e+00 1.000000e-01 1.000000e-01 3.240000e+02 2.470000e+01 2.470000e+01 +2.300000e+00 1.000000e-01 1.000000e-01 2.299000e+02 2.170000e+01 2.170000e+01 +2.500000e+00 1.000000e-01 1.000000e-01 1.292000e+02 1.670000e+01 1.670000e+01 +2.700000e+00 1.000000e-01 1.000000e-01 1.072000e+02 1.500000e+01 1.500000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2015_I1391138/d02-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2015_I1391138/d02-x01-y03 +Title: doi:10.17182/hepdata.74726.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.100000e+00 1.000000e-01 1.000000e-01 9.310000e-01 3.800000e-02 3.800000e-02 +0.300000e+00 1.000000e-01 1.000000e-01 8.160000e-01 3.700000e-02 3.700000e-02 +0.500000e+00 1.000000e-01 1.000000e-01 7.300000e-01 3.600000e-02 3.600000e-02 +0.700000e+00 1.000000e-01 1.000000e-01 7.420000e-01 3.500000e-02 3.500000e-02 +0.900000e+00 1.000000e-01 1.000000e-01 7.330000e-01 3.500000e-02 3.500000e-02 +1.100000e+00 1.000000e-01 1.000000e-01 6.500000e-01 3.300000e-02 3.300000e-02 +1.300000e+00 1.000000e-01 1.000000e-01 5.680000e-01 3.100000e-02 3.100000e-02 +1.500000e+00 1.000000e-01 1.000000e-01 4.810000e-01 2.900000e-02 2.900000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 4.670000e-01 2.800000e-02 2.800000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 3.670000e-01 2.500000e-02 2.500000e-02 +2.100000e+00 1.000000e-01 1.000000e-01 2.830000e-01 2.200000e-02 2.200000e-02 +2.300000e+00 1.000000e-01 1.000000e-01 2.010000e-01 1.900000e-02 1.900000e-02 +2.500000e+00 1.000000e-01 1.000000e-01 1.130000e-01 1.500000e-02 1.500000e-02 +2.700000e+00 1.000000e-01 1.000000e-01 9.400000e-02 1.300000e-02 1.300000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2016_I1385603.cc b/analyses/pluginBES/BESIII_2016_I1385603.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1385603.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2016_I1385603 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2016_I1385603); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2016_I1385603); + + +} diff --git a/analyses/pluginBES/BESIII_2016_I1385603.info b/analyses/pluginBES/BESIII_2016_I1385603.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1385603.info @@ -0,0 +1,36 @@ +Name: BESIII_2016_I1385603 +Year: 2016 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ between 0.6 and 0.9 GeV +Experiment: BES III +Collider: BEPC II +InspireID: 1385603 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys. Lett. B753 (2016) 629-638 +RunInfo: e+ e- to hadrons below 0.6 and 0.9 GeV +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies between 0.6 and 0.9 GeV. Useful for comparing models of the pion form factor.' +Keywords: +BibTeX: '%%% contains utf-8, see: http://inspirehep.net/info/faq/general#utf8 +%%% add \usepackage[utf8]{inputenc} to your latex preamble + +@article{Ablikim:2015orh, + author = "Ablikim, M. and others", + title = "{Measurement of the $e^+ e^− \to \pi^+ \pi^−$ cross + section between 600 and 900 MeV using initial state + radiation}", + collaboration = "BESIII", + journal = "Phys. Lett.", + volume = "B753", + year = "2016", + pages = "629-638", + doi = "10.1016/j.physletb.2015.11.043", + eprint = "1507.08188", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1507.08188;%%" +}' diff --git a/analyses/pluginBES/BESIII_2016_I1385603.plot b/analyses/pluginBES/BESIII_2016_I1385603.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1385603.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /BESIII_2016_I1385603/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESIII_2016_I1385603.yoda b/analyses/pluginBES/BESIII_2016_I1385603.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1385603.yoda @@ -0,0 +1,136 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1385603/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2016_I1385603/d01-x01-y01 +Title: doi:10.17182/hepdata.73898.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.025000e+02 0.000000e+00 0.000000e+00 2.883000e+02 1.520000e+01 1.520000e+01 +6.075000e+02 0.000000e+00 0.000000e+00 3.066000e+02 1.550000e+01 1.550000e+01 +6.125000e+02 0.000000e+00 0.000000e+00 3.328000e+02 1.630000e+01 1.630000e+01 +6.175000e+02 0.000000e+00 0.000000e+00 3.525000e+02 1.630000e+01 1.630000e+01 +6.225000e+02 0.000000e+00 0.000000e+00 3.677000e+02 1.660000e+01 1.660000e+01 +6.275000e+02 0.000000e+00 0.000000e+00 3.901000e+02 1.770000e+01 1.770000e+01 +6.325000e+02 0.000000e+00 0.000000e+00 4.080000e+02 1.800000e+01 1.800000e+01 +6.375000e+02 0.000000e+00 0.000000e+00 4.266000e+02 1.810000e+01 1.810000e+01 +6.425000e+02 0.000000e+00 0.000000e+00 4.535000e+02 1.900000e+01 1.900000e+01 +6.475000e+02 0.000000e+00 0.000000e+00 4.777000e+02 1.850000e+01 1.850000e+01 +6.525000e+02 0.000000e+00 0.000000e+00 4.974000e+02 1.950000e+01 1.950000e+01 +6.575000e+02 0.000000e+00 0.000000e+00 5.092000e+02 1.940000e+01 1.940000e+01 +6.625000e+02 0.000000e+00 0.000000e+00 5.434000e+02 1.990000e+01 1.990000e+01 +6.675000e+02 0.000000e+00 0.000000e+00 5.850000e+02 2.050000e+01 2.050000e+01 +6.725000e+02 0.000000e+00 0.000000e+00 6.427000e+02 2.220000e+01 2.220000e+01 +6.775000e+02 0.000000e+00 0.000000e+00 6.405000e+02 2.100000e+01 2.100000e+01 +6.825000e+02 0.000000e+00 0.000000e+00 6.680000e+02 2.190000e+01 2.190000e+01 +6.875000e+02 0.000000e+00 0.000000e+00 7.244000e+02 2.290000e+01 2.290000e+01 +6.925000e+02 0.000000e+00 0.000000e+00 7.835000e+02 2.320000e+01 2.320000e+01 +6.975000e+02 0.000000e+00 0.000000e+00 8.586000e+02 2.530000e+01 2.530000e+01 +7.025000e+02 0.000000e+00 0.000000e+00 8.938000e+02 2.540000e+01 2.540000e+01 +7.075000e+02 0.000000e+00 0.000000e+00 8.978000e+02 2.500000e+01 2.500000e+01 +7.125000e+02 0.000000e+00 0.000000e+00 9.786000e+02 2.660000e+01 2.660000e+01 +7.175000e+02 0.000000e+00 0.000000e+00 1.059100e+03 2.790000e+01 2.790000e+01 +7.225000e+02 0.000000e+00 0.000000e+00 1.086000e+03 2.830000e+01 2.830000e+01 +7.275000e+02 0.000000e+00 0.000000e+00 1.088400e+03 2.770000e+01 2.770000e+01 +7.325000e+02 0.000000e+00 0.000000e+00 1.158800e+03 2.920000e+01 2.920000e+01 +7.375000e+02 0.000000e+00 0.000000e+00 1.206500e+03 2.960000e+01 2.960000e+01 +7.425000e+02 0.000000e+00 0.000000e+00 1.229900e+03 2.900000e+01 2.900000e+01 +7.475000e+02 0.000000e+00 0.000000e+00 1.263300e+03 3.030000e+01 3.030000e+01 +7.525000e+02 0.000000e+00 0.000000e+00 1.276100e+03 2.980000e+01 2.980000e+01 +7.575000e+02 0.000000e+00 0.000000e+00 1.315900e+03 3.130000e+01 3.130000e+01 +7.625000e+02 0.000000e+00 0.000000e+00 1.339300e+03 3.090000e+01 3.090000e+01 +7.675000e+02 0.000000e+00 0.000000e+00 1.331900e+03 3.080000e+01 3.080000e+01 +7.725000e+02 0.000000e+00 0.000000e+00 1.327000e+03 3.060000e+01 3.060000e+01 +7.775000e+02 0.000000e+00 0.000000e+00 1.272700e+03 2.920000e+01 2.920000e+01 +7.825000e+02 0.000000e+00 0.000000e+00 1.031500e+03 2.670000e+01 2.670000e+01 +7.875000e+02 0.000000e+00 0.000000e+00 8.107000e+02 2.420000e+01 2.420000e+01 +7.925000e+02 0.000000e+00 0.000000e+00 8.197000e+02 2.380000e+01 2.380000e+01 +7.975000e+02 0.000000e+00 0.000000e+00 8.031000e+02 2.330000e+01 2.330000e+01 +8.025000e+02 0.000000e+00 0.000000e+00 7.324000e+02 2.210000e+01 2.210000e+01 +8.075000e+02 0.000000e+00 0.000000e+00 6.799000e+02 2.060000e+01 2.060000e+01 +8.125000e+02 0.000000e+00 0.000000e+00 6.636000e+02 2.100000e+01 2.100000e+01 +8.175000e+02 0.000000e+00 0.000000e+00 6.222000e+02 1.990000e+01 1.990000e+01 +8.225000e+02 0.000000e+00 0.000000e+00 5.850000e+02 1.950000e+01 1.950000e+01 +8.275000e+02 0.000000e+00 0.000000e+00 5.408000e+02 1.810000e+01 1.810000e+01 +8.325000e+02 0.000000e+00 0.000000e+00 4.964000e+02 1.770000e+01 1.770000e+01 +8.375000e+02 0.000000e+00 0.000000e+00 4.504000e+02 1.680000e+01 1.680000e+01 +8.425000e+02 0.000000e+00 0.000000e+00 4.047000e+02 1.520000e+01 1.520000e+01 +8.475000e+02 0.000000e+00 0.000000e+00 3.913000e+02 1.540000e+01 1.540000e+01 +8.525000e+02 0.000000e+00 0.000000e+00 3.640000e+02 1.500000e+01 1.500000e+01 +8.575000e+02 0.000000e+00 0.000000e+00 3.396000e+02 1.400000e+01 1.400000e+01 +8.625000e+02 0.000000e+00 0.000000e+00 3.100000e+02 1.370000e+01 1.370000e+01 +8.675000e+02 0.000000e+00 0.000000e+00 2.838000e+02 1.300000e+01 1.300000e+01 +8.725000e+02 0.000000e+00 0.000000e+00 2.565000e+02 1.240000e+01 1.240000e+01 +8.775000e+02 0.000000e+00 0.000000e+00 2.373000e+02 1.140000e+01 1.140000e+01 +8.825000e+02 0.000000e+00 0.000000e+00 2.297000e+02 1.160000e+01 1.160000e+01 +8.875000e+02 0.000000e+00 0.000000e+00 2.240000e+02 1.160000e+01 1.160000e+01 +8.925000e+02 0.000000e+00 0.000000e+00 1.961000e+02 1.050000e+01 1.050000e+01 +8.975000e+02 0.000000e+00 0.000000e+00 1.759000e+02 9.700000e+00 9.700000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1385603/d01-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2016_I1385603/d01-x01-y02 +Title: doi:10.17182/hepdata.73898.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.025000e+02 0.000000e+00 0.000000e+00 6.900000e+00 4.000000e-01 4.000000e-01 +6.075000e+02 0.000000e+00 0.000000e+00 7.400000e+00 4.000000e-01 4.000000e-01 +6.125000e+02 0.000000e+00 0.000000e+00 8.200000e+00 4.000000e-01 4.000000e-01 +6.175000e+02 0.000000e+00 0.000000e+00 8.700000e+00 4.000000e-01 4.000000e-01 +6.225000e+02 0.000000e+00 0.000000e+00 9.200000e+00 4.000000e-01 4.000000e-01 +6.275000e+02 0.000000e+00 0.000000e+00 9.800000e+00 4.000000e-01 4.000000e-01 +6.325000e+02 0.000000e+00 0.000000e+00 1.040000e+01 5.000000e-01 5.000000e-01 +6.375000e+02 0.000000e+00 0.000000e+00 1.100000e+01 5.000000e-01 5.000000e-01 +6.425000e+02 0.000000e+00 0.000000e+00 1.180000e+01 5.000000e-01 5.000000e-01 +6.475000e+02 0.000000e+00 0.000000e+00 1.250000e+01 5.000000e-01 5.000000e-01 +6.525000e+02 0.000000e+00 0.000000e+00 1.320000e+01 5.000000e-01 5.000000e-01 +6.575000e+02 0.000000e+00 0.000000e+00 1.360000e+01 5.000000e-01 5.000000e-01 +6.625000e+02 0.000000e+00 0.000000e+00 1.470000e+01 5.000000e-01 5.000000e-01 +6.675000e+02 0.000000e+00 0.000000e+00 1.600000e+01 6.000000e-01 6.000000e-01 +6.725000e+02 0.000000e+00 0.000000e+00 1.770000e+01 6.000000e-01 6.000000e-01 +6.775000e+02 0.000000e+00 0.000000e+00 1.780000e+01 6.000000e-01 6.000000e-01 +6.825000e+02 0.000000e+00 0.000000e+00 1.880000e+01 6.000000e-01 6.000000e-01 +6.875000e+02 0.000000e+00 0.000000e+00 2.060000e+01 6.000000e-01 6.000000e-01 +6.925000e+02 0.000000e+00 0.000000e+00 2.250000e+01 7.000000e-01 7.000000e-01 +6.975000e+02 0.000000e+00 0.000000e+00 2.490000e+01 7.000000e-01 7.000000e-01 +7.025000e+02 0.000000e+00 0.000000e+00 2.620000e+01 7.000000e-01 7.000000e-01 +7.075000e+02 0.000000e+00 0.000000e+00 2.660000e+01 7.000000e-01 7.000000e-01 +7.125000e+02 0.000000e+00 0.000000e+00 2.930000e+01 8.000000e-01 8.000000e-01 +7.175000e+02 0.000000e+00 0.000000e+00 3.200000e+01 8.000000e-01 8.000000e-01 +7.225000e+02 0.000000e+00 0.000000e+00 3.320000e+01 9.000000e-01 9.000000e-01 +7.275000e+02 0.000000e+00 0.000000e+00 3.360000e+01 9.000000e-01 9.000000e-01 +7.325000e+02 0.000000e+00 0.000000e+00 3.620000e+01 9.000000e-01 9.000000e-01 +7.375000e+02 0.000000e+00 0.000000e+00 3.820000e+01 9.000000e-01 9.000000e-01 +7.425000e+02 0.000000e+00 0.000000e+00 3.930000e+01 9.000000e-01 9.000000e-01 +7.475000e+02 0.000000e+00 0.000000e+00 4.090000e+01 1.000000e+00 1.000000e+00 +7.525000e+02 0.000000e+00 0.000000e+00 4.180000e+01 1.000000e+00 1.000000e+00 +7.575000e+02 0.000000e+00 0.000000e+00 4.360000e+01 1.000000e+00 1.000000e+00 +7.625000e+02 0.000000e+00 0.000000e+00 4.480000e+01 1.000000e+00 1.000000e+00 +7.675000e+02 0.000000e+00 0.000000e+00 4.500000e+01 1.000000e+00 1.000000e+00 +7.725000e+02 0.000000e+00 0.000000e+00 4.520000e+01 1.000000e+00 1.000000e+00 +7.775000e+02 0.000000e+00 0.000000e+00 4.370000e+01 1.000000e+00 1.000000e+00 +7.825000e+02 0.000000e+00 0.000000e+00 3.710000e+01 9.000000e-01 9.000000e-01 +7.875000e+02 0.000000e+00 0.000000e+00 3.030000e+01 8.000000e-01 8.000000e-01 +7.925000e+02 0.000000e+00 0.000000e+00 3.060000e+01 8.000000e-01 8.000000e-01 +7.975000e+02 0.000000e+00 0.000000e+00 3.010000e+01 8.000000e-01 8.000000e-01 +8.025000e+02 0.000000e+00 0.000000e+00 2.770000e+01 8.000000e-01 8.000000e-01 +8.075000e+02 0.000000e+00 0.000000e+00 2.590000e+01 7.000000e-01 7.000000e-01 +8.125000e+02 0.000000e+00 0.000000e+00 2.550000e+01 8.000000e-01 8.000000e-01 +8.175000e+02 0.000000e+00 0.000000e+00 2.410000e+01 7.000000e-01 7.000000e-01 +8.225000e+02 0.000000e+00 0.000000e+00 2.290000e+01 7.000000e-01 7.000000e-01 +8.275000e+02 0.000000e+00 0.000000e+00 2.140000e+01 7.000000e-01 7.000000e-01 +8.325000e+02 0.000000e+00 0.000000e+00 1.980000e+01 7.000000e-01 7.000000e-01 +8.375000e+02 0.000000e+00 0.000000e+00 1.810000e+01 6.000000e-01 6.000000e-01 +8.425000e+02 0.000000e+00 0.000000e+00 1.640000e+01 6.000000e-01 6.000000e-01 +8.475000e+02 0.000000e+00 0.000000e+00 1.600000e+01 6.000000e-01 6.000000e-01 +8.525000e+02 0.000000e+00 0.000000e+00 1.500000e+01 6.000000e-01 6.000000e-01 +8.575000e+02 0.000000e+00 0.000000e+00 1.420000e+01 6.000000e-01 6.000000e-01 +8.625000e+02 0.000000e+00 0.000000e+00 1.300000e+01 6.000000e-01 6.000000e-01 +8.675000e+02 0.000000e+00 0.000000e+00 1.210000e+01 5.000000e-01 5.000000e-01 +8.725000e+02 0.000000e+00 0.000000e+00 1.100000e+01 5.000000e-01 5.000000e-01 +8.775000e+02 0.000000e+00 0.000000e+00 1.030000e+01 5.000000e-01 5.000000e-01 +8.825000e+02 0.000000e+00 0.000000e+00 1.000000e+01 5.000000e-01 5.000000e-01 +8.875000e+02 0.000000e+00 0.000000e+00 9.900000e+00 5.000000e-01 5.000000e-01 +8.925000e+02 0.000000e+00 0.000000e+00 8.700000e+00 4.000000e-01 4.000000e-01 +8.975000e+02 0.000000e+00 0.000000e+00 7.900000e+00 4.000000e-01 4.000000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2016_I1457597.cc b/analyses/pluginBES/BESIII_2016_I1457597.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1457597.cc @@ -0,0 +1,120 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2016_I1457597 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2016_I1457597); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nJPsi = bookCounter("TMP/jpsi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p1, ufs.particles()) { + bool matched=false; + if(p1.children().empty()) continue; + // find the j/psi + if(p1.pdgId()!=443) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + + foreach (const Particle& p2, ufs.particles()) { + if(p2.children().empty()) continue; + // find the j/psi + if(p2.pdgId()!=331) continue; + map nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nJPsi->fill(event.weight()); + break; + } + } + if(matched) break; + } + } + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nJPsi->val(); + double error = _nJPsi->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 7)); + Scatter2DPtr mult = bookScatter2D(1, 1, 7); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nJPsi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2016_I1457597); + + +} diff --git a/analyses/pluginBES/BESIII_2016_I1457597.info b/analyses/pluginBES/BESIII_2016_I1457597.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1457597.info @@ -0,0 +1,35 @@ +Name: BESIII_2016_I1457597 +Year: 2016 +Summary: Cross section for $e^+e^-\to J/\psi \eta^\prime$ at energies between 4.189 and 4.6 GeV +Experiment: BESIII +Collider: BEPC +InspireID: 1457597 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D94 (2016) 032009, 2016 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to J/\psi \eta^\prime$ at energies between 4.189 and 4.6 GeV' +Keywords: [] +BibKey: Ablikim:2016ymr +BibTeX: '@article{Ablikim:2016ymr, + author = "Ablikim, Medina and others", + title = "{Observation of $e^{+}e^{-} \to \eta^{\prime} J/\psi$ at + center-of-mass energies between 4.189 and 4.600 GeV}", + collaboration = "BESIII", + journal = "Phys. Rev.", + volume = "D94", + year = "2016", + number = "3", + pages = "032009", + doi = "10.1103/PhysRevD.94.032009", + eprint = "1605.03256", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1605.03256;%%" +}' diff --git a/analyses/pluginBES/BESIII_2016_I1457597.plot b/analyses/pluginBES/BESIII_2016_I1457597.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1457597.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BESIII_2016_I1457597/d01-x01-y07 +Title=$\sigma(e^+e^-\to \eta^\prime J/\psi)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta^\prime J/\psi)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESIII_2016_I1457597.yoda b/analyses/pluginBES/BESIII_2016_I1457597.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1457597.yoda @@ -0,0 +1,172 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1457597/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2016_I1457597/d01-x01-y01 +Title: doi:10.17182/hepdata.78543.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.189000e+00 0.000000e+00 0.000000e+00 3.800000e+00 2.300000e+00 2.300000e+00 +4.208000e+00 0.000000e+00 0.000000e+00 2.600000e+00 3.200000e+00 3.200000e+00 +4.217000e+00 0.000000e+00 0.000000e+00 1.000000e+00 1.700000e+00 1.700000e+00 +4.226000e+00 0.000000e+00 0.000000e+00 3.650000e+01 6.900000e+00 6.900000e+00 +4.242000e+00 0.000000e+00 0.000000e+00 8.000000e-01 1.400000e+00 1.400000e+00 +4.258000e+00 0.000000e+00 0.000000e+00 3.000000e+01 6.200000e+00 6.200000e+00 +4.308000e+00 0.000000e+00 0.000000e+00 2.200000e+00 1.500000e+00 1.500000e+00 +4.358000e+00 0.000000e+00 0.000000e+00 3.000000e+00 2.300000e+00 2.300000e+00 +4.387000e+00 0.000000e+00 0.000000e+00 2.100000e+00 2.100000e+00 2.100000e+00 +4.416000e+00 0.000000e+00 0.000000e+00 1.080000e+01 4.100000e+00 4.100000e+00 +4.467000e+00 0.000000e+00 0.000000e+00 5.900000e+00 4.100000e+00 4.100000e+00 +4.527000e+00 0.000000e+00 0.000000e+00 1.400000e+00 1.300000e+00 1.300000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 0.000000e+00 1.700000e+00 1.700000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 1.200000e+00 2.300000e+00 2.300000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1457597/d01-x01-y02 +IsRef: 1 +Path: /REF/BESIII_2016_I1457597/d01-x01-y02 +Title: doi:10.17182/hepdata.78543.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.189000e+00 0.000000e+00 0.000000e+00 8.700000e+00 0.000000e+00 0.000000e+00 +4.208000e+00 0.000000e+00 0.000000e+00 1.330000e+01 0.000000e+00 0.000000e+00 +4.217000e+00 0.000000e+00 0.000000e+00 6.200000e+00 0.000000e+00 0.000000e+00 +4.242000e+00 0.000000e+00 0.000000e+00 5.300000e+00 0.000000e+00 0.000000e+00 +4.308000e+00 0.000000e+00 0.000000e+00 5.900000e+00 0.000000e+00 0.000000e+00 +4.358000e+00 0.000000e+00 0.000000e+00 7.900000e+00 0.000000e+00 0.000000e+00 +4.387000e+00 0.000000e+00 0.000000e+00 8.300000e+00 0.000000e+00 0.000000e+00 +4.416000e+00 0.000000e+00 0.000000e+00 1.590000e+01 0.000000e+00 0.000000e+00 +4.467000e+00 0.000000e+00 0.000000e+00 1.480000e+01 0.000000e+00 0.000000e+00 +4.527000e+00 0.000000e+00 0.000000e+00 5.300000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 9.000000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 7.900000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1457597/d01-x01-y03 +IsRef: 1 +Path: /REF/BESIII_2016_I1457597/d01-x01-y03 +Title: doi:10.17182/hepdata.78543.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.189000e+00 0.000000e+00 0.000000e+00 4.310000e+01 0.000000e+00 0.000000e+00 +4.208000e+00 0.000000e+00 0.000000e+00 5.460000e+01 0.000000e+00 0.000000e+00 +4.217000e+00 0.000000e+00 0.000000e+00 5.410000e+01 0.000000e+00 0.000000e+00 +4.226000e+00 0.000000e+00 0.000000e+00 1.047300e+03 0.000000e+00 0.000000e+00 +4.242000e+00 0.000000e+00 0.000000e+00 5.560000e+01 0.000000e+00 0.000000e+00 +4.258000e+00 0.000000e+00 0.000000e+00 8.257000e+02 0.000000e+00 0.000000e+00 +4.308000e+00 0.000000e+00 0.000000e+00 4.490000e+01 0.000000e+00 0.000000e+00 +4.358000e+00 0.000000e+00 0.000000e+00 5.398000e+02 0.000000e+00 0.000000e+00 +4.387000e+00 0.000000e+00 0.000000e+00 5.520000e+01 0.000000e+00 0.000000e+00 +4.416000e+00 0.000000e+00 0.000000e+00 1.028900e+03 0.000000e+00 0.000000e+00 +4.467000e+00 0.000000e+00 0.000000e+00 1.099000e+02 0.000000e+00 0.000000e+00 +4.527000e+00 0.000000e+00 0.000000e+00 1.100000e+02 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 4.770000e+01 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 5.669000e+02 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1457597/d01-x01-y04 +IsRef: 1 +Path: /REF/BESIII_2016_I1457597/d01-x01-y04 +Title: doi:10.17182/hepdata.78543.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.189000e+00 0.000000e+00 0.000000e+00 8.570000e-01 0.000000e+00 0.000000e+00 +4.208000e+00 0.000000e+00 0.000000e+00 8.850000e-01 0.000000e+00 0.000000e+00 +4.217000e+00 0.000000e+00 0.000000e+00 9.020000e-01 0.000000e+00 0.000000e+00 +4.226000e+00 0.000000e+00 0.000000e+00 9.190000e-01 0.000000e+00 0.000000e+00 +4.242000e+00 0.000000e+00 0.000000e+00 9.450000e-01 0.000000e+00 0.000000e+00 +4.258000e+00 0.000000e+00 0.000000e+00 9.690000e-01 0.000000e+00 0.000000e+00 +4.308000e+00 0.000000e+00 0.000000e+00 1.036000e+00 0.000000e+00 0.000000e+00 +4.358000e+00 0.000000e+00 0.000000e+00 1.114000e+00 0.000000e+00 0.000000e+00 +4.387000e+00 0.000000e+00 0.000000e+00 1.162000e+00 0.000000e+00 0.000000e+00 +4.416000e+00 0.000000e+00 0.000000e+00 1.191000e+00 0.000000e+00 0.000000e+00 +4.467000e+00 0.000000e+00 0.000000e+00 1.161000e+00 0.000000e+00 0.000000e+00 +4.527000e+00 0.000000e+00 0.000000e+00 1.002000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 9.070000e-01 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 8.800000e-01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1457597/d01-x01-y05 +IsRef: 1 +Path: /REF/BESIII_2016_I1457597/d01-x01-y05 +Title: doi:10.17182/hepdata.78543.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.189000e+00 0.000000e+00 0.000000e+00 1.010000e+00 0.000000e+00 0.000000e+00 +4.208000e+00 0.000000e+00 0.000000e+00 1.040000e+00 0.000000e+00 0.000000e+00 +4.217000e+00 0.000000e+00 0.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +4.226000e+00 0.000000e+00 0.000000e+00 9.800000e-01 0.000000e+00 0.000000e+00 +4.242000e+00 0.000000e+00 0.000000e+00 9.500000e-01 0.000000e+00 0.000000e+00 +4.258000e+00 0.000000e+00 0.000000e+00 9.100000e-01 0.000000e+00 0.000000e+00 +4.308000e+00 0.000000e+00 0.000000e+00 8.100000e-01 0.000000e+00 0.000000e+00 +4.358000e+00 0.000000e+00 0.000000e+00 7.700000e-01 0.000000e+00 0.000000e+00 +4.387000e+00 0.000000e+00 0.000000e+00 7.300000e-01 0.000000e+00 0.000000e+00 +4.416000e+00 0.000000e+00 0.000000e+00 7.100000e-01 0.000000e+00 0.000000e+00 +4.467000e+00 0.000000e+00 0.000000e+00 7.200000e-01 0.000000e+00 0.000000e+00 +4.527000e+00 0.000000e+00 0.000000e+00 8.100000e-01 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 9.000000e-01 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 9.200000e-01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1457597/d01-x01-y06 +IsRef: 1 +Path: /REF/BESIII_2016_I1457597/d01-x01-y06 +Title: doi:10.17182/hepdata.78543.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.189000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.208000e+00 0.000000e+00 0.000000e+00 1.057000e+00 0.000000e+00 0.000000e+00 +4.217000e+00 0.000000e+00 0.000000e+00 1.057000e+00 0.000000e+00 0.000000e+00 +4.226000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.242000e+00 0.000000e+00 0.000000e+00 1.056000e+00 0.000000e+00 0.000000e+00 +4.258000e+00 0.000000e+00 0.000000e+00 1.054000e+00 0.000000e+00 0.000000e+00 +4.308000e+00 0.000000e+00 0.000000e+00 1.052000e+00 0.000000e+00 0.000000e+00 +4.358000e+00 0.000000e+00 0.000000e+00 1.051000e+00 0.000000e+00 0.000000e+00 +4.387000e+00 0.000000e+00 0.000000e+00 1.051000e+00 0.000000e+00 0.000000e+00 +4.416000e+00 0.000000e+00 0.000000e+00 1.053000e+00 0.000000e+00 0.000000e+00 +4.467000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +4.527000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 1.055000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1457597/d01-x01-y07 +IsRef: 1 +Path: /REF/BESIII_2016_I1457597/d01-x01-y07 +Title: doi:10.17182/hepdata.78543.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.189000e+00 0.000000e+00 0.000000e+00 9.700000e+00 5.830952e+00 5.830952e+00 +4.208000e+00 0.000000e+00 0.000000e+00 4.900000e+00 6.113101e+00 6.113101e+00 +4.217000e+00 0.000000e+00 0.000000e+00 1.900000e+00 3.306055e+00 3.306055e+00 +4.226000e+00 0.000000e+00 0.000000e+00 3.700000e+00 7.615773e-01 7.615773e-01 +4.242000e+00 0.000000e+00 0.000000e+00 1.500000e+00 2.707397e+00 2.707397e+00 +4.258000e+00 0.000000e+00 0.000000e+00 3.900000e+00 8.544004e-01 8.544004e-01 +4.308000e+00 0.000000e+00 0.000000e+00 5.600000e+00 3.811824e+00 3.811824e+00 +4.358000e+00 0.000000e+00 0.000000e+00 6.000000e-01 5.099020e-01 5.099020e-01 +4.387000e+00 0.000000e+00 0.000000e+00 4.300000e+00 4.310452e+00 4.310452e+00 +4.416000e+00 0.000000e+00 0.000000e+00 1.200000e+00 5.099020e-01 5.099020e-01 +4.467000e+00 0.000000e+00 0.000000e+00 6.100000e+00 4.229657e+00 4.229657e+00 +4.527000e+00 0.000000e+00 0.000000e+00 1.500000e+00 1.403567e+00 1.403567e+00 +4.575000e+00 0.000000e+00 0.000000e+00 0.000000e+00 4.219005e+00 4.219005e+00 +4.600000e+00 0.000000e+00 0.000000e+00 3.000000e-01 5.099020e-01 5.099020e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1457597/d01-x01-y08 +IsRef: 1 +Path: /REF/BESIII_2016_I1457597/d01-x01-y08 +Title: doi:10.17182/hepdata.78543.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.189000e+00 0.000000e+00 0.000000e+00 2.400000e+01 0.000000e+00 0.000000e+00 +4.208000e+00 0.000000e+00 0.000000e+00 2.700000e+01 0.000000e+00 0.000000e+00 +4.217000e+00 0.000000e+00 0.000000e+00 1.300000e+01 0.000000e+00 0.000000e+00 +4.242000e+00 0.000000e+00 0.000000e+00 1.100000e+01 0.000000e+00 0.000000e+00 +4.308000e+00 0.000000e+00 0.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 +4.358000e+00 0.000000e+00 0.000000e+00 1.700000e+00 0.000000e+00 0.000000e+00 +4.387000e+00 0.000000e+00 0.000000e+00 1.800000e+01 0.000000e+00 0.000000e+00 +4.416000e+00 0.000000e+00 0.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +4.467000e+00 0.000000e+00 0.000000e+00 1.700000e+01 0.000000e+00 0.000000e+00 +4.527000e+00 0.000000e+00 0.000000e+00 6.100000e+00 0.000000e+00 0.000000e+00 +4.575000e+00 0.000000e+00 0.000000e+00 2.400000e+01 0.000000e+00 0.000000e+00 +4.600000e+00 0.000000e+00 0.000000e+00 2.100000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2016_I1495838.cc b/analyses/pluginBES/BESIII_2016_I1495838.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1495838.cc @@ -0,0 +1,119 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2016_I1495838 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2016_I1495838); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nPsi = bookCounter("TMP/psi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the psi + if(p.pdgId()==443) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // psi pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nPsi->fill(event.weight()); + break; + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /picobarn; + double sigma = _nPsi->val()*fact; + double error = _nPsi->err()*fact; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nPsi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2016_I1495838); + + +} diff --git a/analyses/pluginBES/BESIII_2016_I1495838.info b/analyses/pluginBES/BESIII_2016_I1495838.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1495838.info @@ -0,0 +1,36 @@ +Name: BESIII_2016_I1495838 +Year: 2016 +Summary: Cross section for $e^+e^-\to J/\psi\pi^+\pi^-$ at energies between 3.77 and 4.6 GeV +Experiment: BESIII +Collider: BEPC +InspireID: 1495838 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 118 (2017) no.9, 092001 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to J/\psi\pi^+\pi^-$ at energies between 3.77 and 4.6 GeV.' +Keywords: [] +BibKey: Ablikim:2016qzw +BibTeX: '@article{Ablikim:2016qzw, + author = "Ablikim, Medina and others", + title = "{Precise measurement of the $e^+e^-\to \pi^+\pi^-J/\psi$ + cross section at center-of-mass energies from 3.77 to 4.60 + GeV}", + collaboration = "BESIII", + journal = "Phys. Rev. Lett.", + volume = "118", + year = "2017", + number = "9", + pages = "092001", + doi = "10.1103/PhysRevLett.118.092001", + eprint = "1611.01317", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1611.01317;%%" +}' diff --git a/analyses/pluginBES/BESIII_2016_I1495838.plot b/analyses/pluginBES/BESIII_2016_I1495838.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1495838.plot @@ -0,0 +1,12 @@ +BEGIN PLOT /BESIII_2016_I1495838/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-J/\psi)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-J/\psi)$/pb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESIII_2016_I1495838/d02-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-J/\psi)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-J/\psi)$/pb +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginBES/BESIII_2016_I1495838.yoda b/analyses/pluginBES/BESIII_2016_I1495838.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2016_I1495838.yoda @@ -0,0 +1,138 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1495838/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2016_I1495838/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.77300 0.00000 0.00000 2.85000e+01 1.80278e+00 1.80278e+00 +3.80770 0.00000 0.00000 1.67000e+01 3.44819e+00 3.44819e+00 +3.89620 0.00000 0.00000 1.71000e+01 3.54401e+00 3.54401e+00 +4.00760 0.00000 0.00000 1.60000e+01 1.48661e+00 1.48661e+00 +4.08550 0.00000 0.00000 1.50000e+01 3.22800e+00 3.22800e+00 +4.18860 0.00000 0.00000 1.55000e+01 3.90512e+00 3.90512e+00 +4.20770 0.00000 0.00000 5.34000e+01 6.22656e+00 6.22656e+00 +4.21710 0.00000 0.00000 6.03000e+01 6.68880e+00 6.68880e+00 +4.22630 0.00000 0.00000 8.51000e+01 5.12445e+00 5.12445e+00 +4.24170 0.00000 0.00000 8.44000e+01 7.98123e+00 7.98123e+00 +4.25800 0.00000 0.00000 5.95000e+01 3.67696e+00 3.67696e+00 +4.30790 0.00000 0.00000 5.20000e+01 6.44127e+00 6.44127e+00 +4.35830 0.00000 0.00000 2.54000e+01 1.92094e+00 1.92094e+00 +4.38740 0.00000 0.00000 2.00000e+01 3.41760e+00 3.41760e+00 +4.41560 0.00000 0.00000 1.21000e+01 9.21954e-01 9.21954e-01 +4.46710 0.00000 0.00000 1.33000e+01 2.24722e+00 2.24722e+00 +4.52710 0.00000 0.00000 1.06000e+01 1.99249e+00 1.99249e+00 +4.57450 0.00000 0.00000 1.34000e+01 3.29848e+00 3.29848e+00 +4.59950 0.00000 0.00000 6.40000e+00 8.06226e-01 8.06226e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2016_I1495838/d02-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2016_I1495838/d02-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.88740 0.00000 0.00000 3.88740e+00 1.31137e+01 9.11976e+00 +3.89240 0.00000 0.00000 3.89240e+00 1.38232e+01 9.83260e+00 +3.89740 0.00000 0.00000 3.89740e+00 1.34536e+01 9.37710e+00 +3.90240 0.00000 0.00000 3.90240e+00 1.42425e+01 1.02591e+01 +3.90740 0.00000 0.00000 3.90740e+00 1.28316e+01 8.54751e+00 +3.91240 0.00000 0.00000 3.91240e+00 1.34183e+01 9.22659e+00 +3.91740 0.00000 0.00000 3.91740e+00 1.14018e+01 6.60303e+00 +3.92240 0.00000 0.00000 3.92240e+00 1.71747e+01 1.27012e+01 +3.92740 0.00000 0.00000 3.92740e+00 1.56627e+01 1.11879e+01 +3.93240 0.00000 0.00000 3.93240e+00 1.24064e+01 8.10987e+00 +3.93740 0.00000 0.00000 3.93740e+00 1.27252e+01 8.53756e+00 +3.94240 0.00000 0.00000 3.94240e+00 1.26396e+01 8.65794e+00 +3.94740 0.00000 0.00000 3.94740e+00 1.48570e+01 1.10766e+01 +3.95240 0.00000 0.00000 3.95240e+00 1.30384e+01 9.35361e+00 +3.95740 0.00000 0.00000 3.95740e+00 1.39517e+01 1.04690e+01 +3.96240 0.00000 0.00000 3.96240e+00 1.23329e+01 8.44808e+00 +3.96740 0.00000 0.00000 3.96740e+00 1.32242e+01 9.13510e+00 +3.97240 0.00000 0.00000 3.97240e+00 1.27142e+01 9.01998e+00 +3.97740 0.00000 0.00000 3.97740e+00 1.17107e+01 7.91581e+00 +3.98240 0.00000 0.00000 3.98240e+00 1.45774e+01 1.09037e+01 +3.98740 0.00000 0.00000 3.98740e+00 8.42140e+00 1.21149e+01 +3.99240 0.00000 0.00000 3.99240e+00 6.60076e+00 1.05005e+01 +3.99740 0.00000 0.00000 3.99740e+00 8.96772e+00 1.27475e+01 +4.00240 0.00000 0.00000 4.00240e+00 1.10653e+01 1.49482e+01 +4.00740 0.00000 0.00000 4.00740e+00 1.43503e+01 1.02703e+01 +4.00940 0.00000 0.00000 4.00940e+00 1.33135e+01 8.92020e+00 +4.01140 0.00000 0.00000 4.01140e+00 1.53639e+01 1.09895e+01 +4.01340 0.00000 0.00000 4.01340e+00 1.38232e+01 9.23472e+00 +4.01540 0.00000 0.00000 4.01540e+00 1.36297e+01 9.34345e+00 +4.01740 0.00000 0.00000 4.01740e+00 1.73277e+01 1.31685e+01 +4.02240 0.00000 0.00000 4.02240e+00 1.67084e+01 1.23471e+01 +4.02740 0.00000 0.00000 4.02740e+00 7.71622e+00 6.02080e+00 +4.03240 0.00000 0.00000 4.03240e+00 1.52555e+01 1.09772e+01 +4.03740 0.00000 0.00000 4.03740e+00 1.17004e+01 7.00071e+00 +4.04740 0.00000 0.00000 4.04740e+00 1.26004e+01 8.00062e+00 +4.05240 0.00000 0.00000 4.05240e+00 1.44679e+01 1.02956e+01 +4.05740 0.00000 0.00000 4.05740e+00 1.39291e+01 9.24392e+00 +4.06240 0.00000 0.00000 4.06240e+00 1.34239e+01 9.23472e+00 +4.06740 0.00000 0.00000 4.06740e+00 1.23146e+01 8.22192e+00 +4.07740 0.00000 0.00000 4.07740e+00 1.36444e+01 9.96092e+00 +4.08740 0.00000 0.00000 4.08740e+00 1.29190e+01 9.12688e+00 +4.09740 0.00000 0.00000 4.09740e+00 1.17068e+01 7.61052e+00 +4.10740 0.00000 0.00000 4.10740e+00 1.26143e+01 8.52115e+00 +4.11740 0.00000 0.00000 4.11740e+00 1.12071e+01 7.31095e+00 +4.12740 0.00000 0.00000 4.12740e+00 1.27142e+01 8.52115e+00 +4.13740 0.00000 0.00000 4.13740e+00 1.51954e+01 1.12294e+01 +4.14240 0.00000 0.00000 4.14240e+00 1.25196e+01 8.62844e+00 +4.14740 0.00000 0.00000 4.14740e+00 1.14158e+01 7.32462e+00 +4.15740 0.00000 0.00000 4.15740e+00 1.55929e+01 1.19218e+01 +4.16740 0.00000 0.00000 4.16740e+00 6.51230e+00 4.81664e+00 +4.17740 0.00000 0.00000 4.17740e+00 1.44779e+01 1.03097e+01 +4.18740 0.00000 0.00000 4.18740e+00 1.12040e+01 7.00643e+00 +4.19240 0.00000 0.00000 4.19240e+00 1.46874e+01 1.07201e+01 +4.19740 0.00000 0.00000 4.19740e+00 1.56285e+01 1.16726e+01 +4.20040 0.00000 0.00000 4.20040e+00 2.00960e+01 1.58493e+01 +4.20340 0.00000 0.00000 4.20340e+00 1.59706e+01 1.19942e+01 +4.20740 0.00000 0.00000 4.20740e+00 1.51954e+01 1.12294e+01 +4.21240 0.00000 0.00000 4.21240e+00 2.02000e+01 1.65895e+01 +4.21740 0.00000 0.00000 4.21740e+00 1.98479e+01 1.63248e+01 +4.22240 0.00000 0.00000 4.22240e+00 2.05915e+01 1.73081e+01 +4.22740 0.00000 0.00000 4.22740e+00 2.40052e+01 2.09745e+01 +4.23240 0.00000 0.00000 4.23240e+00 1.86344e+01 1.55242e+01 +4.23740 0.00000 0.00000 4.23740e+00 2.21721e+01 1.89114e+01 +4.24040 0.00000 0.00000 4.24040e+00 1.87984e+01 1.57965e+01 +4.24240 0.00000 0.00000 4.24240e+00 1.57334e+01 1.25929e+01 +4.24540 0.00000 0.00000 4.24540e+00 1.68671e+01 1.39463e+01 +4.24740 0.00000 0.00000 4.24740e+00 1.70294e+01 1.40246e+01 +4.25240 0.00000 0.00000 4.25240e+00 1.49459e+01 1.20075e+01 +4.25740 0.00000 0.00000 4.25740e+00 1.76570e+01 1.49616e+01 +4.26240 0.00000 0.00000 4.26240e+00 1.62595e+01 1.33405e+01 +4.26740 0.00000 0.00000 4.26740e+00 1.77539e+01 1.49616e+01 +4.27240 0.00000 0.00000 4.27240e+00 1.62975e+01 1.33645e+01 +4.27740 0.00000 0.00000 4.27740e+00 1.42706e+01 1.12178e+01 +4.28240 0.00000 0.00000 4.28240e+00 1.69650e+01 1.40431e+01 +4.28740 0.00000 0.00000 4.28740e+00 1.60854e+01 1.32699e+01 +4.29740 0.00000 0.00000 4.29740e+00 1.44257e+01 1.12614e+01 +4.30740 0.00000 0.00000 4.30740e+00 1.68122e+01 1.38051e+01 +4.31740 0.00000 0.00000 4.31740e+00 1.34974e+01 1.06513e+01 +4.32740 0.00000 0.00000 4.32740e+00 1.32966e+01 1.01272e+01 +4.33740 0.00000 0.00000 4.33740e+00 1.34213e+01 1.03576e+01 +4.34740 0.00000 0.00000 4.34740e+00 1.14280e+01 8.23893e+00 +4.35740 0.00000 0.00000 4.35740e+00 1.49626e+01 1.18068e+01 +4.36740 0.00000 0.00000 4.36740e+00 1.38452e+01 1.07870e+01 +4.37740 0.00000 0.00000 4.37740e+00 1.22409e+01 8.95600e+00 +4.38740 0.00000 0.00000 4.38740e+00 1.32544e+01 9.67471e+00 +4.39240 0.00000 0.00000 4.39240e+00 1.32740e+01 9.60260e+00 +4.39740 0.00000 0.00000 4.39740e+00 1.21413e+01 8.26075e+00 +4.40740 0.00000 0.00000 4.40740e+00 1.10041e+01 6.20725e+00 +4.41740 0.00000 0.00000 4.41740e+00 1.23406e+01 8.65794e+00 +4.42240 0.00000 0.00000 4.42240e+00 1.24487e+01 8.67006e+00 +4.42740 0.00000 0.00000 4.42740e+00 1.19151e+01 7.62365e+00 +4.43740 0.00000 0.00000 4.43740e+00 1.21499e+01 8.47172e+00 +4.44740 0.00000 0.00000 4.44740e+00 1.02020e+01 6.40312e+00 +4.45740 0.00000 0.00000 4.45740e+00 9.40851e+00 6.11310e+00 +4.47740 0.00000 0.00000 4.47740e+00 1.12219e+01 7.73175e+00 +4.49740 0.00000 0.00000 4.49740e+00 8.30060e+00 4.30116e+00 +4.51740 0.00000 0.00000 4.51740e+00 1.02240e+01 6.73647e+00 +4.53740 0.00000 0.00000 4.53740e+00 1.06301e+01 7.54255e+00 +4.54740 0.00000 0.00000 4.54740e+00 1.08374e+01 7.45453e+00 +4.55740 0.00000 0.00000 4.55740e+00 1.00045e+01 6.20725e+00 +4.56740 0.00000 0.00000 4.56740e+00 1.06118e+01 6.81836e+00 +4.57740 0.00000 0.00000 4.57740e+00 1.11113e+01 7.51665e+00 +4.58740 0.00000 0.00000 4.58740e+00 8.70057e+00 4.40114e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2018_I1627871.cc b/analyses/pluginBES/BESIII_2018_I1627871.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1627871.cc @@ -0,0 +1,136 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2018_I1627871 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2018_I1627871); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nLambda= bookCounter( "/TMP/nLambda" ); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + // total hadronic and muonic cross sections + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // find the Lambdas + const FinalState& ufs = apply(event, "UFS"); + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + for(unsigned int iy=ix+1;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nLambda->fill(event.weight()); + break; + } + } + if(matched) break; + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nLambda->val(); + double error = _nLambda->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + //@} + + /// @name Histograms + //@{ + CounterPtr _nLambda; + //@} + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2018_I1627871); + + +} diff --git a/analyses/pluginBES/BESIII_2018_I1627871.info b/analyses/pluginBES/BESIII_2018_I1627871.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1627871.info @@ -0,0 +1,34 @@ +Name: BESIII_2018_I1627871 +Year: 2018 +Summary: Cross section for $e^+e^-\to\Lambda\bar{\Lambda}$ between threshold and 3.08 GeV +Experiment: BESIII +Collider: BEPC II +InspireID: 1627871 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D97 (2018) no.3, 032013 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to\Lambda\bar{\Lambda}$ between threshold and 3.08 GeV.' +Keywords: +BibKey: Ablikim:2017pyl +BibTeX: '@article{Ablikim:2017pyl, + author = "Ablikim, Medina and others", + title = "{Observation of a cross-section enhancement near mass + threshold in $e^{+}e^{-}\rightarrow\Lambda\bar{\Lambda}$}", + collaboration = "BESIII", + journal = "Phys. Rev.", + volume = "D97", + year = "2018", + number = "3", + pages = "032013", + doi = "10.1103/PhysRevD.97.032013", + eprint = "1709.10236", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1709.10236;%%" +}' diff --git a/analyses/pluginBES/BESIII_2018_I1627871.plot b/analyses/pluginBES/BESIII_2018_I1627871.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1627871.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BESIII_2018_I1627871/d01-x01-y01 +Title=$\sigma(e^+e^-\to \Lambda\bar{\Lambda})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \Lambda\bar{\Lambda})$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESIII_2018_I1627871.yoda b/analyses/pluginBES/BESIII_2018_I1627871.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1627871.yoda @@ -0,0 +1,12 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2018_I1627871/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2018_I1627871/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.23240 0.00000 0.00000 3.05000e+02 5.76281e+01 7.98812e+01 +2.40000 0.00000 0.00000 1.28000e+02 2.61725e+01 2.61725e+01 +2.80000 0.00000 0.00000 1.48000e+01 5.53624e+00 5.53624e+00 +3.08000 0.00000 0.00000 4.20000e+00 1.30000e+00 1.30000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2018_I1691798.cc b/analyses/pluginBES/BESIII_2018_I1691798.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1691798.cc @@ -0,0 +1,84 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2018_I1691798 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2018_I1691798); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + _nKKpi= bookCounter( "/TMP/nKKpi" ); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + if(ntotal==3 && nCount[310]==1 && + ((nCount[ 321]=1 && nCount[-211] ==1) || + (nCount[-321]=1 && nCount[ 211] ==1))) + _nKKpi->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nKKpi->val(); + double error = _nKKpi->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nKKpi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2018_I1691798); + + +} diff --git a/analyses/pluginBES/BESIII_2018_I1691798.info b/analyses/pluginBES/BESIII_2018_I1691798.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1691798.info @@ -0,0 +1,31 @@ +Name: BESIII_2018_I1691798 +Year: 2018 +Summary: Cross Section for $K^0_SK^\pm\pi^\mp$ between 3.8 and 4.6 GeV +Experiment: BESIII +Collider: BEPC II +InspireID: 1691798 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - arXiv:1808.08733 [hep-ex] +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $K^0_SK^\pm\pi^\mp$ between 3.8 and 4.6 GeV.' +Keywords: +BibKey: Ablikim:2018lmx +BibTeX: '@article{Ablikim:2018lmx, + author = "Ablikim, Medina and others", + title = "{Precision measurements of $\sigma_{B}(e^+e^- \to + K_{S}^{0}K^{\pm}\pi^{\mp})$ at center-of-mass energies + between 3.8 and 4.6 GeV}", + collaboration = "BESIII", + year = "2018", + eprint = "1808.08733", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1808.08733;%%" +}' diff --git a/analyses/pluginBES/BESIII_2018_I1691798.plot b/analyses/pluginBES/BESIII_2018_I1691798.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1691798.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BESIII_2018_I1691798/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^\pm \pi^\mp)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^\pm \pi^\mp)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESIII_2018_I1691798.yoda b/analyses/pluginBES/BESIII_2018_I1691798.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1691798.yoda @@ -0,0 +1,23 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2018_I1691798/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2018_I1691798/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.80800 0.00000 0.00000 1.74000e+01 1.89568e+00 1.88053e+00 +3.89600 0.00000 0.00000 1.01100e+01 1.44568e+00 1.42299e+00 +4.00800 0.00000 0.00000 9.08000e+00 9.53362e-01 9.53362e-01 +4.08600 0.00000 0.00000 8.91000e+00 1.37971e+00 1.35680e+00 +4.18900 0.00000 0.00000 9.32000e+00 1.48741e+00 1.45588e+00 +4.20800 0.00000 0.00000 7.92000e+00 1.27342e+00 1.25841e+00 +4.21700 0.00000 0.00000 8.59000e+00 1.31913e+00 1.30419e+00 +4.22600 0.00000 0.00000 7.69000e+00 8.53464e-01 8.53464e-01 +4.24200 0.00000 0.00000 7.28000e+00 1.26507e+00 1.23434e+00 +4.25800 0.00000 0.00000 6.79000e+00 8.08022e-01 8.08022e-01 +4.30800 0.00000 0.00000 5.22000e+00 1.11104e+00 1.08743e+00 +4.35800 0.00000 0.00000 5.90000e+00 7.70000e-01 7.70000e-01 +4.38700 0.00000 0.00000 5.39000e+00 1.09659e+00 1.06588e+00 +4.41600 0.00000 0.00000 5.59000e+00 7.15821e-01 7.15821e-01 +4.60000 0.00000 0.00000 4.18000e+00 6.39062e-01 6.39062e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2018_I1699641.cc b/analyses/pluginBES/BESIII_2018_I1699641.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1699641.cc @@ -0,0 +1,138 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/FastJets.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2018_I1699641 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2018_I1699641); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + // Book histograms + _cKKpipi = bookCounter("TMP/2Kpipi" ); + _cKKpieta = bookCounter("TMP/2Kpieta"); + } + + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // K K pi pi + if(ntotal==4 && nCount[310]==1 && nCount[111]==1 && + ((nCount[ 321]==1 &&nCount[-211]==1) || + (nCount[-321]==1 &&nCount[ 211]==1) )) + _cKKpipi->fill(event.weight()); + // eta resonance + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=221) continue; + map nRes=nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + if(ncount!=3) continue; + bool matched=true; + for(auto const & val : nRes) { + if(abs(val.first)==321 || abs(val.first)==211) { + continue; + } + else if(abs(val.first)==310) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched==false) continue; + if((nCount[ 321] == 1 && nCount[-211] ==1) || + (nCount[-321] == 1 && nCount[ 211] ==1)) + _cKKpieta->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _cKKpipi->val(); + error = _cKKpipi->err(); + } + else if(ix==2) { + sigma = _cKKpieta->val(); + error = _cKKpieta->err(); + } + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _cKKpipi,_cKKpieta; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2018_I1699641); + + +} diff --git a/analyses/pluginBES/BESIII_2018_I1699641.info b/analyses/pluginBES/BESIII_2018_I1699641.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1699641.info @@ -0,0 +1,31 @@ +Name: BESIII_2018_I1699641 +Year: 2018 +Summary: Cross section for $e^+e^-\to K^0_SK^\pm\pi^\mp\pi^0$ and $K^0_SK^\pm\pi^\mp\eta$ between 3.90 to 4.60 GeV +Experiment: BESIII +Collider: BEPC II +InspireID: 1699641 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - arXiv:1810.09395 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^0_SK^\pm\pi^\mp\pi^0$ and $K^0_SK^\pm\pi^\mp\eta$ between 3.90 to 4.60 GeV.' +Keywords: +BibKey: Ablikim:2018ddb +BibTeX: '@article{Ablikim:2018ddb, + author = "Ablikim, Medina and others", + title = "{Measurements of $e^+e^- \to + K_{S}^{0}K^{\pm}\pi^{\mp}\pi^0$ and + $K_{S}^{0}K^{\pm}\pi^{\mp}\eta$ at center-of-mass energies + from $3.90$ to $4.60~\mathrm{GeV}$}", + collaboration = "BESIII", + year = "2018", + eprint = "1810.09395", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1810.09395;%%" +}' diff --git a/analyses/pluginBES/BESIII_2018_I1699641.plot b/analyses/pluginBES/BESIII_2018_I1699641.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1699641.plot @@ -0,0 +1,12 @@ +BEGIN PLOT /BESIII_2018_I1699641/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^\pm\pi^\mp\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^\pm\pi^\mp\pi^0)$/pb +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESIII_2018_I1699641/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^\pm\pi^\mp\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^\pm\pi^\mp\eta)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESIII_2018_I1699641.yoda b/analyses/pluginBES/BESIII_2018_I1699641.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1699641.yoda @@ -0,0 +1,50 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2018_I1699641/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2018_I1699641/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.89600 0.00000 0.00000 7.44100e+01 4.32908e+00 4.32908e+00 +4.00800 0.00000 0.00000 5.80200e+01 2.49802e+00 2.49802e+00 +4.08600 0.00000 0.00000 4.75200e+01 3.42533e+00 3.42533e+00 +4.18900 0.00000 0.00000 4.53800e+01 3.56702e+00 3.56702e+00 +4.20800 0.00000 0.00000 4.09500e+01 3.15119e+00 3.15119e+00 +4.21700 0.00000 0.00000 3.82800e+01 3.03315e+00 3.03315e+00 +4.22600 0.00000 0.00000 3.92300e+01 1.96023e+00 1.96023e+00 +4.24200 0.00000 0.00000 3.74600e+01 2.98371e+00 2.98371e+00 +4.25800 0.00000 0.00000 3.86500e+01 1.96898e+00 1.96898e+00 +4.30800 0.00000 0.00000 3.68600e+01 3.19130e+00 3.19130e+00 +4.35800 0.00000 0.00000 3.35300e+01 1.88106e+00 1.88106e+00 +4.38700 0.00000 0.00000 3.36800e+01 2.80713e+00 2.80713e+00 +4.41600 0.00000 0.00000 3.03800e+01 1.72630e+00 1.72630e+00 +4.46700 0.00000 0.00000 2.67000e+01 2.07470e+00 2.07470e+00 +4.52700 0.00000 0.00000 2.65100e+01 2.08327e+00 2.08327e+00 +4.57500 0.00000 0.00000 2.48700e+01 2.54629e+00 2.54629e+00 +4.60000 0.00000 0.00000 2.27100e+01 1.53782e+00 1.53782e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2018_I1699641/d02-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2018_I1699641/d02-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.89600 0.00000 0.00000 2.72300e+01 3.59004e+00 3.59004e+00 +4.00800 0.00000 0.00000 1.98800e+01 1.65118e+00 1.65118e+00 +4.08500 0.00000 0.00000 1.47100e+01 2.72075e+00 2.72075e+00 +4.18900 0.00000 0.00000 1.77500e+01 3.16735e+00 3.16735e+00 +4.20800 0.00000 0.00000 1.42000e+01 2.56049e+00 2.56049e+00 +4.21700 0.00000 0.00000 1.00500e+01 2.15000e+00 2.15000e+00 +4.22600 0.00000 0.00000 1.56100e+01 1.24101e+00 1.24101e+00 +4.24200 0.00000 0.00000 1.46300e+01 2.52951e+00 2.52951e+00 +4.25800 0.00000 0.00000 1.43500e+01 1.28254e+00 1.28254e+00 +4.30800 0.00000 0.00000 1.26700e+01 2.60085e+00 2.60085e+00 +4.35800 0.00000 0.00000 1.13800e+01 1.18507e+00 1.18507e+00 +4.38700 0.00000 0.00000 1.30500e+01 2.25424e+00 2.25424e+00 +4.41600 0.00000 0.00000 1.06200e+01 1.07931e+00 1.07931e+00 +4.46700 0.00000 0.00000 1.06200e+01 1.64441e+00 1.64441e+00 +4.52700 0.00000 0.00000 7.27000e+00 1.56719e+00 1.56719e+00 +4.57500 0.00000 0.00000 9.23000e+00 2.08940e+00 2.08940e+00 +4.60000 0.00000 0.00000 8.67000e+00 1.07313e+00 1.07313e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2018_I1704558.cc b/analyses/pluginBES/BESIII_2018_I1704558.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1704558.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2018_I1704558 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2018_I1704558); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nkaon = bookCounter("TMP/kaon"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::KPLUS) vetoEvent; + } + _nkaon->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nkaon->val(); + double error = _nkaon->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nkaon; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2018_I1704558); + + +} diff --git a/analyses/pluginBES/BESIII_2018_I1704558.info b/analyses/pluginBES/BESIII_2018_I1704558.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1704558.info @@ -0,0 +1,29 @@ +Name: BESIII_2018_I1704558 +Year: 2018 +Summary: Cross section for $e^+e^-\to K^+K^-$ between 2.00 and 3.08 GeV +Experiment: BESIII +Collider: BEPC II +InspireID: 1704558 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - arXiv:1811.08742 +RunInfo: e+ e- to hadrons between 2.00 and 3.08 GeV +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-$ at energies between 2.00 and 3.08 GeV. Useful for comparing models of the kaon form factor.' +Keywords: [] +BibKey: Ablikim:2018iyx +BibTeX: '@article{Ablikim:2018iyx, + author = "Ablikim, M. and others", + title = "{Measurement of $e^{+} e^{-} \rightarrow K^{+} K^{-}$ + cross section at $\sqrt{s} = 2.00 - 3.08$ GeV}", + collaboration = "BESIII", + year = "2018", + eprint = "1811.08742", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1811.08742;%%" +}' diff --git a/analyses/pluginBES/BESIII_2018_I1704558.plot b/analyses/pluginBES/BESIII_2018_I1704558.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1704558.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BESIII_2018_I1704558/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESIII_2018_I1704558.yoda b/analyses/pluginBES/BESIII_2018_I1704558.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2018_I1704558.yoda @@ -0,0 +1,30 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2018_I1704558/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2018_I1704558/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.00000 0.00000 0.00000 3.51500e+02 9.23255e+00 9.23255e+00 +2.05000 0.00000 0.00000 2.96100e+02 1.36605e+01 1.36605e+01 +2.10000 0.00000 0.00000 2.20600e+02 6.76831e+00 6.76831e+00 +2.12500 0.00000 0.00000 1.92000e+02 3.55528e+00 3.55528e+00 +2.15000 0.00000 0.00000 1.71700e+02 1.10856e+01 1.10856e+01 +2.17500 0.00000 0.00000 1.84200e+02 6.45678e+00 6.45678e+00 +2.20000 0.00000 0.00000 2.31400e+02 6.67008e+00 6.67008e+00 +2.23240 0.00000 0.00000 2.53200e+02 7.24500e+00 7.24500e+00 +2.30940 0.00000 0.00000 1.84000e+02 5.05964e+00 5.05964e+00 +2.38640 0.00000 0.00000 1.01500e+02 3.74299e+00 3.74299e+00 +2.39600 0.00000 0.00000 1.02600e+02 2.94788e+00 2.94788e+00 +2.50000 0.00000 0.00000 8.81000e+01 1.24274e+01 1.24274e+01 +2.64440 0.00000 0.00000 5.66000e+01 2.80000e+00 2.80000e+00 +2.64640 0.00000 0.00000 5.67000e+01 2.61534e+00 2.61534e+00 +2.70000 0.00000 0.00000 3.63000e+01 8.55336e+00 8.55336e+00 +2.80000 0.00000 0.00000 3.79000e+01 8.99111e+00 8.99111e+00 +2.90000 0.00000 0.00000 3.04000e+01 1.90788e+00 1.90788e+00 +2.95000 0.00000 0.00000 2.53000e+01 2.53180e+00 2.53180e+00 +2.98100 0.00000 0.00000 2.80000e+01 2.40000e+00 2.40000e+00 +3.00000 0.00000 0.00000 2.44000e+01 2.49800e+00 2.49800e+00 +3.02000 0.00000 0.00000 2.48000e+01 2.49800e+00 2.49800e+00 +3.08000 0.00000 0.00000 2.53000e+01 2.21133e+00 2.21133e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESIII_2019_I1718337.cc b/analyses/pluginBES/BESIII_2019_I1718337.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2019_I1718337.cc @@ -0,0 +1,80 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESIII_2019_I1718337 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESIII_2019_I1718337); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nproton = bookCounter("TMP/proton"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PROTON) vetoEvent; + } + _nproton->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nproton->val(); + double error = _nproton->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nproton; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESIII_2019_I1718337); + + +} diff --git a/analyses/pluginBES/BESIII_2019_I1718337.info b/analyses/pluginBES/BESIII_2019_I1718337.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2019_I1718337.info @@ -0,0 +1,29 @@ +Name: BESIII_2019_I1718337 +Year: 2019 +Summary: Cross section for $e^+e^-\to$ proton and antiproton between 2. and 3.8GeV using ISR +Experiment: BESIII +Collider: BEPC II +InspireID: 1718337 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - arXiv:1902.00665 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ for energies between 2. and 3.8 GeV using initial-state radiation.' +Keywords: [] +BibKey: Ablikim:2019njl +BibTeX: '@article{Ablikim:2019njl, + author = "Ablikim, M. and others", + title = "{Study of $e^+ e^- \to p \bar p$ via initial state + radiation at BESIII}", + collaboration = "BESIII", + year = "2019", + eprint = "1902.00665", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1902.00665;%%" +}' diff --git a/analyses/pluginBES/BESIII_2019_I1718337.plot b/analyses/pluginBES/BESIII_2019_I1718337.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2019_I1718337.plot @@ -0,0 +1,5 @@ +BEGIN PLOT /BESIII_2019_I1718337/d01-x01-y01 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/pb +END PLOT diff --git a/analyses/pluginBES/BESIII_2019_I1718337.yoda b/analyses/pluginBES/BESIII_2019_I1718337.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESIII_2019_I1718337.yoda @@ -0,0 +1,38 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESIII_2019_I1718337/d01-x01-y01 +IsRef: 1 +Path: /REF/BESIII_2019_I1718337/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.01250 0.01250 0.01250 7.97000e+02 9.36002e+01 9.36002e+01 +2.03750 0.01250 0.01250 8.33000e+02 8.29277e+01 8.29277e+01 +2.06250 0.01250 0.01250 7.23000e+02 6.76757e+01 6.76757e+01 +2.08750 0.01250 0.01250 7.49000e+02 5.78014e+01 5.78014e+01 +2.11250 0.01250 0.01250 6.54000e+02 5.63028e+01 5.63028e+01 +2.13750 0.01250 0.01250 6.37000e+02 4.94065e+01 4.94065e+01 +2.16250 0.01250 0.01250 5.57000e+02 4.74342e+01 4.74342e+01 +2.18750 0.01250 0.01250 4.67000e+02 3.92046e+01 3.92046e+01 +2.21250 0.01250 0.01250 3.71000e+02 3.42053e+01 3.42053e+01 +2.23750 0.01250 0.01250 3.10000e+02 2.90689e+01 2.90689e+01 +2.26250 0.01250 0.01250 2.25000e+02 2.26274e+01 2.26274e+01 +2.28750 0.01250 0.01250 1.92000e+02 1.97990e+01 1.97990e+01 +2.32500 0.02500 0.02500 1.36100e+02 1.13146e+01 1.13146e+01 +2.37500 0.02500 0.02500 1.16300e+02 1.21037e+01 1.21037e+01 +2.42500 0.02500 0.02500 1.26100e+02 9.56713e+00 9.56713e+00 +2.47500 0.02500 0.02500 1.00100e+02 9.12853e+00 9.12853e+00 +2.52500 0.02500 0.02500 6.74000e+01 6.86222e+00 6.86222e+00 +2.57500 0.02500 0.02500 6.11000e+01 5.90339e+00 5.90339e+00 +2.62500 0.02500 0.02500 4.10000e+01 4.70106e+00 4.70106e+00 +2.67500 0.02500 0.02500 3.36000e+01 3.94081e+00 3.94081e+00 +2.72500 0.02500 0.02500 3.07000e+01 4.24264e+00 4.24264e+00 +2.77500 0.02500 0.02500 2.68000e+01 3.61248e+00 3.61248e+00 +2.82500 0.02500 0.02500 2.16000e+01 3.25269e+00 3.25269e+00 +2.87500 0.02500 0.02500 2.04000e+01 2.84253e+00 2.84253e+00 +2.92500 0.02500 0.02500 1.02000e+01 2.72029e+00 2.72029e+00 +2.97500 0.02500 0.02500 1.41000e+01 2.64008e+00 2.64008e+00 +3.10000 0.10000 0.10000 1.11000e+01 1.69706e+00 1.69706e+00 +3.30000 0.10000 0.10000 3.59000e+00 6.51153e-01 6.51153e-01 +3.50000 0.10000 0.10000 2.18000e+00 3.92046e-01 3.92046e-01 +3.70000 0.10000 0.10000 6.40000e-01 2.62488e-01 2.62488e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2000_I505323.cc b/analyses/pluginBES/BESII_2000_I505323.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2000_I505323.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2000_I505323 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2000_I505323); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2000_I505323); + + +} diff --git a/analyses/pluginBES/BESII_2000_I505323.info b/analyses/pluginBES/BESII_2000_I505323.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2000_I505323.info @@ -0,0 +1,36 @@ +Name: BESII_2000_I505323 +Year: 2000 +Summary: Measurement of $R$ for energies between 2.6 and 5 GeV +Experiment: BESII +Collider: BEPC +InspireID: 505323 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 84 (2000) 594-597, 2000 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by BESII for energies between 2.6 and 5 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Bai:1999pk +BibTeX: '@article{Bai:1999pk, + author = "Bai, J. Z. and others", + title = "{Measurement of the total cross-section for hadronic + production by e+ e- annihilation at energies between + 2.6-GeV - 5-GeV}", + collaboration = "BES", + journal = "Phys. Rev. Lett.", + volume = "84", + year = "2000", + pages = "594-597", + doi = "10.1103/PhysRevLett.84.594", + eprint = "hep-ex/9908046", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-REPRINT-1999-087", + SLACcitation = "%%CITATION = HEP-EX/9908046;%%" +}' diff --git a/analyses/pluginBES/BESII_2000_I505323.plot b/analyses/pluginBES/BESII_2000_I505323.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2000_I505323.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /BESII_2000_I505323/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2000_I505323/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2000_I505323/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESII_2000_I505323.yoda b/analyses/pluginBES/BESII_2000_I505323.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2000_I505323.yoda @@ -0,0 +1,14 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2000_I505323/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2000_I505323/d01-x01-y01 +Title: doi:10.17182/hepdata.41611.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.600000e+00 0.000000e+00 0.000000e+00 2.640000e+00 1.964688e-01 1.964688e-01 +3.200000e+00 0.000000e+00 0.000000e+00 2.210000e+00 1.476482e-01 1.476482e-01 +3.400000e+00 0.000000e+00 0.000000e+00 2.380000e+00 1.746425e-01 1.746425e-01 +3.550000e+00 0.000000e+00 0.000000e+00 2.230000e+00 1.708801e-01 1.708801e-01 +4.600000e+00 0.000000e+00 0.000000e+00 3.580000e+00 3.522783e-01 3.522783e-01 +5.000000e+00 0.000000e+00 0.000000e+00 3.470000e+00 4.318565e-01 4.318565e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2002_I552757.cc b/analyses/pluginBES/BESII_2002_I552757.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2002_I552757.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2002_I552757 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2002_I552757); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2002_I552757); + + +} diff --git a/analyses/pluginBES/BESII_2002_I552757.info b/analyses/pluginBES/BESII_2002_I552757.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2002_I552757.info @@ -0,0 +1,35 @@ +Name: BESII_2002_I552757 +Year: 2002 +Summary: Measurement of $R$ for energies between 2.2 and 4.8 GeV +Experiment: BESII +Collider: BEPC +InspireID: 552757 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 88 (2002) 101802, 2002 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by BESII for energies between 2.2 and 4.8 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Bai:2001ct +BibTeX: '@article{Bai:2001ct, + author = "Bai, J. Z. and others", + title = "{Measurements of the cross-section for e+ e ---> hadrons + at center-of-mass energies from 2-GeV to 5-GeV}", + collaboration = "BES", + journal = "Phys. Rev. Lett.", + volume = "88", + year = "2002", + pages = "101802", + doi = "10.1103/PhysRevLett.88.101802", + eprint = "hep-ex/0102003", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-8938", + SLACcitation = "%%CITATION = HEP-EX/0102003;%%" +}' diff --git a/analyses/pluginBES/BESII_2002_I552757.plot b/analyses/pluginBES/BESII_2002_I552757.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2002_I552757.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /BESII_2002_I552757/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2002_I552757/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2002_I552757/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESII_2002_I552757.yoda b/analyses/pluginBES/BESII_2002_I552757.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2002_I552757.yoda @@ -0,0 +1,93 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2002_I552757/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2002_I552757/d01-x01-y01 +Title: doi:10.17182/hepdata.41990.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.000000e+00 0.000000e+00 0.000000e+00 2.180000e+00 1.931321e-01 1.931321e-01 +2.200000e+00 0.000000e+00 0.000000e+00 2.380000e+00 1.838478e-01 1.838478e-01 +2.400000e+00 0.000000e+00 0.000000e+00 2.380000e+00 1.565248e-01 1.565248e-01 +2.500000e+00 0.000000e+00 0.000000e+00 2.390000e+00 1.700000e-01 1.700000e-01 +2.600000e+00 0.000000e+00 0.000000e+00 2.380000e+00 1.615549e-01 1.615549e-01 +2.700000e+00 0.000000e+00 0.000000e+00 2.300000e+00 1.476482e-01 1.476482e-01 +2.800000e+00 0.000000e+00 0.000000e+00 2.170000e+00 1.523155e-01 1.523155e-01 +2.900000e+00 0.000000e+00 0.000000e+00 2.220000e+00 1.476482e-01 1.476482e-01 +3.000000e+00 0.000000e+00 0.000000e+00 2.210000e+00 1.208305e-01 1.208305e-01 +3.700000e+00 0.000000e+00 0.000000e+00 2.230000e+00 1.131371e-01 1.131371e-01 +3.730000e+00 0.000000e+00 0.000000e+00 2.100000e+00 1.612452e-01 1.612452e-01 +3.750000e+00 0.000000e+00 0.000000e+00 2.470000e+00 1.500000e-01 1.500000e-01 +3.760000e+00 0.000000e+00 0.000000e+00 2.770000e+00 1.702939e-01 1.702939e-01 +3.764000e+00 0.000000e+00 0.000000e+00 3.290000e+00 3.962323e-01 3.962323e-01 +3.768000e+00 0.000000e+00 0.000000e+00 3.800000e+00 4.140048e-01 4.140048e-01 +3.770000e+00 0.000000e+00 0.000000e+00 3.550000e+00 2.360085e-01 2.360085e-01 +3.772000e+00 0.000000e+00 0.000000e+00 3.120000e+00 3.324154e-01 3.324154e-01 +3.776000e+00 0.000000e+00 0.000000e+00 3.260000e+00 3.220248e-01 3.220248e-01 +3.780000e+00 0.000000e+00 0.000000e+00 3.280000e+00 1.697056e-01 1.697056e-01 +3.790000e+00 0.000000e+00 0.000000e+00 2.620000e+00 1.486607e-01 1.486607e-01 +3.810000e+00 0.000000e+00 0.000000e+00 2.380000e+00 1.562050e-01 1.562050e-01 +3.850000e+00 0.000000e+00 0.000000e+00 2.470000e+00 1.702939e-01 1.702939e-01 +3.890000e+00 0.000000e+00 0.000000e+00 2.640000e+00 1.860108e-01 1.860108e-01 +3.930000e+00 0.000000e+00 0.000000e+00 3.180000e+00 2.202272e-01 2.202272e-01 +3.940000e+00 0.000000e+00 0.000000e+00 2.940000e+00 2.302173e-01 2.302173e-01 +3.950000e+00 0.000000e+00 0.000000e+00 2.970000e+00 2.140093e-01 2.140093e-01 +3.960000e+00 0.000000e+00 0.000000e+00 2.790000e+00 2.080865e-01 2.080865e-01 +3.970000e+00 0.000000e+00 0.000000e+00 3.290000e+00 1.838478e-01 1.838478e-01 +3.980000e+00 0.000000e+00 0.000000e+00 3.130000e+00 2.126029e-01 2.126029e-01 +3.990000e+00 0.000000e+00 0.000000e+00 3.060000e+00 2.343075e-01 2.343075e-01 +4.000000e+00 0.000000e+00 0.000000e+00 3.160000e+00 2.051828e-01 2.051828e-01 +4.010000e+00 0.000000e+00 0.000000e+00 3.530000e+00 2.561250e-01 2.561250e-01 +4.020000e+00 0.000000e+00 0.000000e+00 4.430000e+00 2.640076e-01 2.640076e-01 +4.027000e+00 0.000000e+00 0.000000e+00 4.580000e+00 2.765863e-01 2.765863e-01 +4.030000e+00 0.000000e+00 0.000000e+00 4.580000e+00 3.047950e-01 3.047950e-01 +4.033000e+00 0.000000e+00 0.000000e+00 4.320000e+00 2.780288e-01 2.780288e-01 +4.040000e+00 0.000000e+00 0.000000e+00 4.400000e+00 2.549510e-01 2.549510e-01 +4.050000e+00 0.000000e+00 0.000000e+00 4.230000e+00 2.780288e-01 2.780288e-01 +4.060000e+00 0.000000e+00 0.000000e+00 4.650000e+00 2.687006e-01 2.687006e-01 +4.070000e+00 0.000000e+00 0.000000e+00 4.140000e+00 2.758623e-01 2.758623e-01 +4.080000e+00 0.000000e+00 0.000000e+00 4.240000e+00 2.765863e-01 2.765863e-01 +4.090000e+00 0.000000e+00 0.000000e+00 4.060000e+00 2.475884e-01 2.475884e-01 +4.100000e+00 0.000000e+00 0.000000e+00 3.970000e+00 2.408319e-01 2.408319e-01 +4.110000e+00 0.000000e+00 0.000000e+00 3.920000e+00 2.483948e-01 2.483948e-01 +4.120000e+00 0.000000e+00 0.000000e+00 4.110000e+00 3.324154e-01 3.324154e-01 +4.130000e+00 0.000000e+00 0.000000e+00 3.990000e+00 2.267157e-01 2.267157e-01 +4.140000e+00 0.000000e+00 0.000000e+00 3.830000e+00 2.343075e-01 2.343075e-01 +4.150000e+00 0.000000e+00 0.000000e+00 4.210000e+00 2.617250e-01 2.617250e-01 +4.160000e+00 0.000000e+00 0.000000e+00 4.120000e+00 2.193171e-01 2.193171e-01 +4.170000e+00 0.000000e+00 0.000000e+00 4.120000e+00 2.420744e-01 2.420744e-01 +4.180000e+00 0.000000e+00 0.000000e+00 4.180000e+00 2.475884e-01 2.475884e-01 +4.190000e+00 0.000000e+00 0.000000e+00 4.010000e+00 1.979899e-01 1.979899e-01 +4.200000e+00 0.000000e+00 0.000000e+00 3.870000e+00 2.262742e-01 2.262742e-01 +4.210000e+00 0.000000e+00 0.000000e+00 3.200000e+00 2.334524e-01 2.334524e-01 +4.220000e+00 0.000000e+00 0.000000e+00 3.620000e+00 2.500000e-01 2.500000e-01 +4.230000e+00 0.000000e+00 0.000000e+00 3.210000e+00 1.984943e-01 1.984943e-01 +4.240000e+00 0.000000e+00 0.000000e+00 3.240000e+00 1.920937e-01 1.920937e-01 +4.245000e+00 0.000000e+00 0.000000e+00 2.970000e+00 1.780449e-01 1.780449e-01 +4.250000e+00 0.000000e+00 0.000000e+00 2.710000e+00 1.769181e-01 1.769181e-01 +4.255000e+00 0.000000e+00 0.000000e+00 2.880000e+00 1.780449e-01 1.780449e-01 +4.260000e+00 0.000000e+00 0.000000e+00 2.970000e+00 1.780449e-01 1.780449e-01 +4.265000e+00 0.000000e+00 0.000000e+00 3.040000e+00 1.910497e-01 1.910497e-01 +4.270000e+00 0.000000e+00 0.000000e+00 3.260000e+00 2.000000e-01 2.000000e-01 +4.280000e+00 0.000000e+00 0.000000e+00 3.080000e+00 1.920937e-01 1.920937e-01 +4.300000e+00 0.000000e+00 0.000000e+00 3.110000e+00 1.697056e-01 1.697056e-01 +4.320000e+00 0.000000e+00 0.000000e+00 2.960000e+00 1.843909e-01 1.843909e-01 +4.340000e+00 0.000000e+00 0.000000e+00 3.270000e+00 2.343075e-01 2.343075e-01 +4.350000e+00 0.000000e+00 0.000000e+00 3.490000e+00 1.979899e-01 1.979899e-01 +4.360000e+00 0.000000e+00 0.000000e+00 3.470000e+00 2.220360e-01 2.220360e-01 +4.380000e+00 0.000000e+00 0.000000e+00 3.500000e+00 2.267157e-01 2.267157e-01 +4.390000e+00 0.000000e+00 0.000000e+00 3.480000e+00 2.262742e-01 2.262742e-01 +4.400000e+00 0.000000e+00 0.000000e+00 3.910000e+00 2.483948e-01 2.483948e-01 +4.410000e+00 0.000000e+00 0.000000e+00 3.790000e+00 2.500000e-01 2.500000e-01 +4.420000e+00 0.000000e+00 0.000000e+00 3.680000e+00 2.202272e-01 2.202272e-01 +4.430000e+00 0.000000e+00 0.000000e+00 4.020000e+00 2.561250e-01 2.561250e-01 +4.440000e+00 0.000000e+00 0.000000e+00 3.850000e+00 2.404163e-01 2.404163e-01 +4.450000e+00 0.000000e+00 0.000000e+00 3.750000e+00 2.267157e-01 2.267157e-01 +4.460000e+00 0.000000e+00 0.000000e+00 3.660000e+00 2.334524e-01 2.334524e-01 +4.480000e+00 0.000000e+00 0.000000e+00 3.540000e+00 2.475884e-01 2.475884e-01 +4.500000e+00 0.000000e+00 0.000000e+00 3.490000e+00 2.051828e-01 2.051828e-01 +4.520000e+00 0.000000e+00 0.000000e+00 3.250000e+00 1.984943e-01 1.984943e-01 +4.540000e+00 0.000000e+00 0.000000e+00 3.230000e+00 2.280351e-01 2.280351e-01 +4.560000e+00 0.000000e+00 0.000000e+00 3.620000e+00 2.061553e-01 2.061553e-01 +4.600000e+00 0.000000e+00 0.000000e+00 3.310000e+00 1.941649e-01 1.941649e-01 +4.800000e+00 0.000000e+00 0.000000e+00 3.660000e+00 2.360085e-01 2.360085e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2004_I622224.cc b/analyses/pluginBES/BESII_2004_I622224.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2004_I622224.cc @@ -0,0 +1,80 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/ChargedFinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2004_I622224 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2004_I622224); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + const ChargedFinalState fs; + declare(fs, "FS"); + unsigned int iloc(0); + if(fuzzyEquals(sqrtS()/GeV, 2.2 , 1E-3)) + iloc = 1; + else if(fuzzyEquals(sqrtS()/GeV, 2.6 , 1E-3)) + iloc = 2; + else if(fuzzyEquals(sqrtS()/GeV, 3.0 , 1E-3)) + iloc = 3; + else if(fuzzyEquals(sqrtS()/GeV, 3.2 , 1E-3)) + iloc = 4; + else if(fuzzyEquals(sqrtS()/GeV, 4.6 , 1E-3)) + iloc = 5; + else if(fuzzyEquals(sqrtS()/GeV, 4.8 , 1E-3)) + iloc = 6; + assert(iloc!=0); + _h_ln = bookHisto1D( iloc ,1,1); + _h_weight = 0.; + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const ChargedFinalState& fs = apply(event, "FS"); + if(fs.particles().size()==2 && + abs(fs.particles()[0].pdgId())==13 && + abs(fs.particles()[1].pdgId())==13) vetoEvent; + foreach (const Particle& p, fs.particles()) { + const Vector3 mom3 = p.p3(); + double pp = mom3.mod(); + double xi = -log(2.*pp/sqrtS()); + _h_ln->fill(xi,event.weight()); + } + _h_weight+= event.weight(); + } + + + /// Normalise histograms etc., after the run + void finalize() { + scale(_h_ln,1./_h_weight); + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _h_ln; + double _h_weight; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2004_I622224); + + +} diff --git a/analyses/pluginBES/BESII_2004_I622224.info b/analyses/pluginBES/BESII_2004_I622224.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2004_I622224.info @@ -0,0 +1,36 @@ +Name: BESII_2004_I622224 +Year: 2004 +Summary: Charged particle momentum distributions for energies between 2.2 and 4.8 GeV +Experiment: BESII +Collider: BEPC +InspireID: 622224 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D69 (2004) 072002, 2004 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Energies: [2.2,2.6,3.0,3.2,4.6,4.8] +Luminosity_fb: +Description: + 'Charged particle momentum distributions for energies between 2.2 and 4.8 GeV' +BibKey: Dunwoodie:2003xt +BibTeX: '@article{Dunwoodie:2003xt, + author = "Dunwoodie, W. and others", + title = "{Measurement of inclusive momentum spectra and + multiplicity distributions of charged particles at S**1/2 + sim 2-5 GeV}", + collaboration = "BES", + journal = "Phys. Rev.", + volume = "D69", + year = "2004", + pages = "072002", + doi = "10.1103/PhysRevD.69.072002", + eprint = "hep-ex/0306055", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-10095", + SLACcitation = "%%CITATION = HEP-EX/0306055;%%" +}' diff --git a/analyses/pluginBES/BESII_2004_I622224.plot b/analyses/pluginBES/BESII_2004_I622224.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2004_I622224.plot @@ -0,0 +1,42 @@ +BEGIN PLOT /BESII_2004_I622224/d01-x01-y01 +Title=Charged Particle Momentum at 2.2 GeV +XLabel=$\xi$ +YLabel=$\frac1{N}\frac{\text{d}N}{\text{d}\xi}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2004_I622224/d02-x01-y01 +Title=Charged Particle Momentum at 2.6 GeV +XLabel=$\xi$ +YLabel=$\frac1{N}\frac{\text{d}N}{\text{d}\xi}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2004_I622224/d03-x01-y01 +Title=Charged Particle Momentum at 3.0 GeV +XLabel=$\xi$ +YLabel=$\frac1{N}\frac{\text{d}N}{\text{d}\xi}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2004_I622224/d04-x01-y01 +Title=Charged Particle Momentum at 3.2 GeV +XLabel=$\xi$ +YLabel=$\frac1{N}\frac{\text{d}N}{\text{d}\xi}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2004_I622224/d05-x01-y01 +Title=Charged Particle Momentum at 4.6 GeV +XLabel=$\xi$ +YLabel=$\frac1{N}\frac{\text{d}N}{\text{d}\xi}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2004_I622224/d06-x01-y01 +Title=Charged Particle Momentum at 4.8 GeV +XLabel=$\xi$ +YLabel=$\frac1{N}\frac{\text{d}N}{\text{d}\xi}$ +LogY=1 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginBES/BESII_2004_I622224.yoda b/analyses/pluginBES/BESII_2004_I622224.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2004_I622224.yoda @@ -0,0 +1,402 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d01-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-01 0.250000e+00 0.200000e+00 6.966900e-01 1.026500e-01 1.026500e-01 +5.250000e-01 0.075000e+00 0.075000e+00 1.175220e+00 1.241500e-01 1.241500e-01 +6.500000e-01 0.050000e+00 0.050000e+00 1.477710e+00 1.502200e-01 1.502200e-01 +7.500000e-01 0.050000e+00 0.050000e+00 1.966460e+00 2.033500e-01 2.033500e-01 +8.500000e-01 0.050000e+00 0.050000e+00 1.726810e+00 1.589200e-01 1.589200e-01 +9.500000e-01 0.050000e+00 0.050000e+00 1.841690e+00 1.528200e-01 1.528200e-01 +1.050000e+00 0.050000e+00 0.050000e+00 1.940160e+00 1.553900e-01 1.553900e-01 +1.150000e+00 0.050000e+00 0.050000e+00 1.787370e+00 1.752200e-01 1.752200e-01 +1.250000e+00 0.050000e+00 0.050000e+00 1.872280e+00 1.584500e-01 1.584500e-01 +1.350000e+00 0.050000e+00 0.050000e+00 1.800140e+00 1.482800e-01 1.482800e-01 +1.450000e+00 0.050000e+00 0.050000e+00 1.570240e+00 1.269700e-01 1.269700e-01 +1.550000e+00 0.050000e+00 0.050000e+00 1.226020e+00 1.034900e-01 1.034900e-01 +1.650000e+00 0.050000e+00 0.050000e+00 1.172940e+00 1.175800e-01 1.175800e-01 +1.750000e+00 0.050000e+00 0.050000e+00 8.000700e-01 8.446000e-02 8.446000e-02 +1.850000e+00 0.050000e+00 0.050000e+00 7.597300e-01 8.050000e-02 8.050000e-02 +1.950000e+00 0.050000e+00 0.050000e+00 6.599400e-01 7.504000e-02 7.504000e-02 +2.050000e+00 0.050000e+00 0.050000e+00 4.915100e-01 7.032000e-02 7.032000e-02 +2.150000e+00 0.050000e+00 0.050000e+00 3.071300e-01 7.672000e-02 7.672000e-02 +2.250000e+00 0.050000e+00 0.050000e+00 3.957100e-01 1.001900e-01 1.001900e-01 +2.350000e+00 0.050000e+00 0.050000e+00 2.118100e-01 6.572000e-02 6.572000e-02 +2.450000e+00 0.050000e+00 0.050000e+00 2.078300e-01 7.213000e-02 7.213000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d02-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d02-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-01 0.250000e+00 0.200000e+00 6.241700e-01 1.082600e-01 1.082600e-01 +5.250000e-01 0.075000e+00 0.075000e+00 1.057570e+00 8.123000e-02 8.123000e-02 +6.500000e-01 0.050000e+00 0.050000e+00 1.247730e+00 7.713000e-02 7.713000e-02 +7.500000e-01 0.050000e+00 0.050000e+00 1.531760e+00 6.671000e-02 6.671000e-02 +8.500000e-01 0.050000e+00 0.050000e+00 1.807230e+00 7.415000e-02 7.415000e-02 +9.500000e-01 0.050000e+00 0.050000e+00 1.982960e+00 1.012300e-01 1.012300e-01 +1.050000e+00 0.050000e+00 0.050000e+00 2.095060e+00 9.078000e-02 9.078000e-02 +1.150000e+00 0.050000e+00 0.050000e+00 2.056010e+00 9.643000e-02 9.643000e-02 +1.250000e+00 0.050000e+00 0.050000e+00 2.045640e+00 8.862000e-02 8.862000e-02 +1.350000e+00 0.050000e+00 0.050000e+00 2.041740e+00 8.949000e-02 8.949000e-02 +1.450000e+00 0.050000e+00 0.050000e+00 1.934960e+00 9.212000e-02 9.212000e-02 +1.550000e+00 0.050000e+00 0.050000e+00 1.658560e+00 1.022300e-01 1.022300e-01 +1.650000e+00 0.050000e+00 0.050000e+00 1.494150e+00 9.205000e-02 9.205000e-02 +1.750000e+00 0.050000e+00 0.050000e+00 1.380630e+00 8.992000e-02 8.992000e-02 +1.850000e+00 0.050000e+00 0.050000e+00 1.061060e+00 8.572000e-02 8.572000e-02 +1.950000e+00 0.050000e+00 0.050000e+00 9.049100e-01 6.068000e-02 6.068000e-02 +2.050000e+00 0.050000e+00 0.050000e+00 7.603700e-01 4.902000e-02 4.902000e-02 +2.150000e+00 0.050000e+00 0.050000e+00 6.323300e-01 4.249000e-02 4.249000e-02 +2.250000e+00 0.050000e+00 0.050000e+00 5.688000e-01 4.668000e-02 4.668000e-02 +2.350000e+00 0.050000e+00 0.050000e+00 4.108200e-01 3.663000e-02 3.663000e-02 +2.450000e+00 0.050000e+00 0.050000e+00 2.977100e-01 4.803000e-02 4.803000e-02 +2.550000e+00 0.050000e+00 0.050000e+00 2.967400e-01 4.322000e-02 4.322000e-02 +2.650000e+00 0.050000e+00 0.050000e+00 1.972800e-01 4.204000e-02 4.204000e-02 +2.750000e+00 0.050000e+00 0.050000e+00 1.612300e-01 6.237000e-02 6.237000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d03-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d03-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-01 0.250000e+00 0.200000e+00 4.740300e-01 8.037000e-02 8.037000e-02 +5.250000e-01 0.075000e+00 0.075000e+00 9.760700e-01 8.079000e-02 8.079000e-02 +6.500000e-01 0.050000e+00 0.050000e+00 1.288380e+00 1.045400e-01 1.045400e-01 +7.500000e-01 0.050000e+00 0.050000e+00 1.459130e+00 1.234600e-01 1.234600e-01 +8.500000e-01 0.050000e+00 0.050000e+00 1.749810e+00 1.509400e-01 1.509400e-01 +9.500000e-01 0.050000e+00 0.050000e+00 2.081620e+00 1.435500e-01 1.435500e-01 +1.050000e+00 0.050000e+00 0.050000e+00 2.077880e+00 1.291000e-01 1.291000e-01 +1.150000e+00 0.050000e+00 0.050000e+00 2.094710e+00 1.363700e-01 1.363700e-01 +1.250000e+00 0.050000e+00 0.050000e+00 2.261780e+00 1.529900e-01 1.529900e-01 +1.350000e+00 0.050000e+00 0.050000e+00 2.238840e+00 1.380500e-01 1.380500e-01 +1.450000e+00 0.050000e+00 0.050000e+00 2.238630e+00 1.293700e-01 1.293700e-01 +1.550000e+00 0.050000e+00 0.050000e+00 2.063880e+00 1.142200e-01 1.142200e-01 +1.650000e+00 0.050000e+00 0.050000e+00 2.108150e+00 1.325800e-01 1.325800e-01 +1.750000e+00 0.050000e+00 0.050000e+00 1.655760e+00 1.280700e-01 1.280700e-01 +1.850000e+00 0.050000e+00 0.050000e+00 1.518560e+00 9.854000e-02 9.854000e-02 +1.950000e+00 0.050000e+00 0.050000e+00 1.280100e+00 1.108400e-01 1.108400e-01 +2.050000e+00 0.050000e+00 0.050000e+00 1.146910e+00 9.304000e-02 9.304000e-02 +2.150000e+00 0.050000e+00 0.050000e+00 9.340500e-01 9.029000e-02 9.029000e-02 +2.250000e+00 0.050000e+00 0.050000e+00 7.740900e-01 8.908000e-02 8.908000e-02 +2.350000e+00 0.050000e+00 0.050000e+00 6.221600e-01 9.724000e-02 9.724000e-02 +2.450000e+00 0.050000e+00 0.050000e+00 5.870600e-01 9.631000e-02 9.631000e-02 +2.550000e+00 0.050000e+00 0.050000e+00 4.005100e-01 7.759000e-02 7.759000e-02 +2.650000e+00 0.050000e+00 0.050000e+00 3.260400e-01 8.877000e-02 8.877000e-02 +2.750000e+00 0.050000e+00 0.050000e+00 2.784000e-01 6.271000e-02 6.271000e-02 +2.850000e+00 0.050000e+00 0.050000e+00 2.238400e-01 6.857000e-02 6.857000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d04-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d04-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-01 0.250000e+00 0.200000e+00 3.753200e-01 6.535000e-02 6.535000e-02 +5.250000e-01 0.075000e+00 0.075000e+00 7.654500e-01 7.733000e-02 7.733000e-02 +6.500000e-01 0.050000e+00 0.050000e+00 1.119380e+00 1.540400e-01 1.540400e-01 +7.500000e-01 0.050000e+00 0.050000e+00 1.200400e+00 1.081900e-01 1.081900e-01 +8.500000e-01 0.050000e+00 0.050000e+00 1.574770e+00 1.339200e-01 1.339200e-01 +9.500000e-01 0.050000e+00 0.050000e+00 1.871230e+00 1.352500e-01 1.352500e-01 +1.050000e+00 0.050000e+00 0.050000e+00 2.084230e+00 1.442300e-01 1.442300e-01 +1.150000e+00 0.050000e+00 0.050000e+00 2.132300e+00 1.569200e-01 1.569200e-01 +1.250000e+00 0.050000e+00 0.050000e+00 2.362560e+00 1.468600e-01 1.468600e-01 +1.350000e+00 0.050000e+00 0.050000e+00 2.679340e+00 1.583500e-01 1.583500e-01 +1.450000e+00 0.050000e+00 0.050000e+00 2.300830e+00 1.533700e-01 1.533700e-01 +1.550000e+00 0.050000e+00 0.050000e+00 2.097060e+00 1.493500e-01 1.493500e-01 +1.650000e+00 0.050000e+00 0.050000e+00 2.117490e+00 1.518500e-01 1.518500e-01 +1.750000e+00 0.050000e+00 0.050000e+00 2.020670e+00 1.304900e-01 1.304900e-01 +1.850000e+00 0.050000e+00 0.050000e+00 1.635450e+00 1.308700e-01 1.308700e-01 +1.950000e+00 0.050000e+00 0.050000e+00 1.336350e+00 1.317600e-01 1.317600e-01 +2.050000e+00 0.050000e+00 0.050000e+00 1.227010e+00 9.873000e-02 9.873000e-02 +2.150000e+00 0.050000e+00 0.050000e+00 1.036600e+00 1.117200e-01 1.117200e-01 +2.250000e+00 0.050000e+00 0.050000e+00 8.345600e-01 1.052600e-01 1.052600e-01 +2.350000e+00 0.050000e+00 0.050000e+00 6.490300e-01 1.050800e-01 1.050800e-01 +2.450000e+00 0.050000e+00 0.050000e+00 5.885800e-01 8.516000e-02 8.516000e-02 +2.550000e+00 0.050000e+00 0.050000e+00 5.542600e-01 1.107400e-01 1.107400e-01 +2.650000e+00 0.050000e+00 0.050000e+00 4.764600e-01 1.130400e-01 1.130400e-01 +2.750000e+00 0.050000e+00 0.050000e+00 1.827900e-01 6.391000e-02 6.391000e-02 +2.850000e+00 0.050000e+00 0.050000e+00 2.295800e-01 6.547000e-02 6.547000e-02 +2.950000e+00 0.050000e+00 0.050000e+00 1.754200e-01 7.104000e-02 7.104000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d05-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d05-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-01 0.250000e+00 0.200000e+00 1.523000e-01 3.635000e-02 3.635000e-02 +5.250000e-01 0.075000e+00 0.075000e+00 4.144400e-01 8.089000e-02 8.089000e-02 +6.500000e-01 0.050000e+00 0.050000e+00 5.325900e-01 1.334600e-01 1.334600e-01 +7.500000e-01 0.050000e+00 0.050000e+00 9.639600e-01 1.574600e-01 1.574600e-01 +8.500000e-01 0.050000e+00 0.050000e+00 1.337820e+00 1.783800e-01 1.783800e-01 +9.500000e-01 0.050000e+00 0.050000e+00 1.797590e+00 1.847000e-01 1.847000e-01 +1.050000e+00 0.050000e+00 0.050000e+00 1.621910e+00 1.716500e-01 1.716500e-01 +1.150000e+00 0.050000e+00 0.050000e+00 2.035620e+00 2.066400e-01 2.066400e-01 +1.250000e+00 0.050000e+00 0.050000e+00 2.430140e+00 2.350400e-01 2.350400e-01 +1.350000e+00 0.050000e+00 0.050000e+00 2.694270e+00 2.425100e-01 2.425100e-01 +1.450000e+00 0.050000e+00 0.050000e+00 2.580740e+00 2.235400e-01 2.235400e-01 +1.550000e+00 0.050000e+00 0.050000e+00 2.922790e+00 2.771700e-01 2.771700e-01 +1.650000e+00 0.050000e+00 0.050000e+00 2.862950e+00 2.526300e-01 2.526300e-01 +1.750000e+00 0.050000e+00 0.050000e+00 2.793870e+00 2.396900e-01 2.396900e-01 +1.850000e+00 0.050000e+00 0.050000e+00 2.738200e+00 2.308300e-01 2.308300e-01 +1.950000e+00 0.050000e+00 0.050000e+00 2.585370e+00 2.917800e-01 2.917800e-01 +2.050000e+00 0.050000e+00 0.050000e+00 2.213140e+00 2.091000e-01 2.091000e-01 +2.150000e+00 0.050000e+00 0.050000e+00 2.146770e+00 2.255400e-01 2.255400e-01 +2.250000e+00 0.050000e+00 0.050000e+00 1.450660e+00 1.808200e-01 1.808200e-01 +2.350000e+00 0.050000e+00 0.050000e+00 1.530150e+00 2.312700e-01 2.312700e-01 +2.450000e+00 0.050000e+00 0.050000e+00 1.429520e+00 2.242400e-01 2.242400e-01 +2.550000e+00 0.050000e+00 0.050000e+00 1.117320e+00 2.015100e-01 2.015100e-01 +2.650000e+00 0.050000e+00 0.050000e+00 1.063170e+00 2.094400e-01 2.094400e-01 +2.750000e+00 0.050000e+00 0.050000e+00 1.017040e+00 1.880400e-01 1.880400e-01 +2.850000e+00 0.050000e+00 0.050000e+00 6.515600e-01 1.344500e-01 1.344500e-01 +2.950000e+00 0.050000e+00 0.050000e+00 7.414700e-01 1.753900e-01 1.753900e-01 +3.250000e+00 0.050000e+00 0.050000e+00 3.868600e-01 1.001500e-01 1.001500e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d06-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d06-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-01 0.250000e+00 0.200000e+00 2.123300e-01 5.481000e-02 5.481000e-02 +5.250000e-01 0.075000e+00 0.075000e+00 5.373100e-01 9.395000e-02 9.395000e-02 +6.500000e-01 0.050000e+00 0.050000e+00 6.215100e-01 1.349400e-01 1.349400e-01 +7.500000e-01 0.050000e+00 0.050000e+00 1.000070e+00 1.626400e-01 1.626400e-01 +8.500000e-01 0.050000e+00 0.050000e+00 1.044930e+00 1.514700e-01 1.514700e-01 +9.500000e-01 0.050000e+00 0.050000e+00 1.534650e+00 1.727200e-01 1.727200e-01 +1.050000e+00 0.050000e+00 0.050000e+00 1.614270e+00 1.895300e-01 1.895300e-01 +1.150000e+00 0.050000e+00 0.050000e+00 1.871630e+00 2.281100e-01 2.281100e-01 +1.250000e+00 0.050000e+00 0.050000e+00 2.579310e+00 2.138200e-01 2.138200e-01 +1.350000e+00 0.050000e+00 0.050000e+00 2.576730e+00 2.514100e-01 2.514100e-01 +1.450000e+00 0.050000e+00 0.050000e+00 2.831690e+00 2.862600e-01 2.862600e-01 +1.550000e+00 0.050000e+00 0.050000e+00 2.793350e+00 2.459000e-01 2.459000e-01 +1.650000e+00 0.050000e+00 0.050000e+00 2.828420e+00 3.209100e-01 3.209100e-01 +1.750000e+00 0.050000e+00 0.050000e+00 3.199510e+00 2.907100e-01 2.907100e-01 +1.850000e+00 0.050000e+00 0.050000e+00 2.900540e+00 2.391500e-01 2.391500e-01 +1.950000e+00 0.050000e+00 0.050000e+00 2.546210e+00 2.559500e-01 2.559500e-01 +2.050000e+00 0.050000e+00 0.050000e+00 2.214820e+00 3.007500e-01 3.007500e-01 +2.150000e+00 0.050000e+00 0.050000e+00 2.152230e+00 2.313900e-01 2.313900e-01 +2.250000e+00 0.050000e+00 0.050000e+00 2.025490e+00 2.459800e-01 2.459800e-01 +2.350000e+00 0.050000e+00 0.050000e+00 1.450650e+00 2.457800e-01 2.457800e-01 +2.450000e+00 0.050000e+00 0.050000e+00 1.664090e+00 2.177300e-01 2.177300e-01 +2.550000e+00 0.050000e+00 0.050000e+00 1.141290e+00 2.330200e-01 2.330200e-01 +2.650000e+00 0.050000e+00 0.050000e+00 1.016370e+00 1.899700e-01 1.899700e-01 +2.750000e+00 0.050000e+00 0.050000e+00 9.391300e-01 1.842200e-01 1.842200e-01 +2.850000e+00 0.050000e+00 0.050000e+00 1.031030e+00 2.040200e-01 2.040200e-01 +2.950000e+00 0.050000e+00 0.050000e+00 5.478900e-01 1.660600e-01 1.660600e-01 +3.250000e+00 0.050000e+00 0.050000e+00 3.166800e-01 8.155000e-02 8.155000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d07-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d07-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t7 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.492000e-02 0.000000e+00 0.000000e+00 1.933681e+01 6.711080e+00 6.711080e+00 +1.049100e-01 0.000000e+00 0.000000e+00 1.459938e+01 4.529870e+00 4.529870e+00 +1.159400e-01 0.000000e+00 0.000000e+00 2.020584e+01 5.115930e+00 5.115930e+00 +1.281300e-01 0.000000e+00 0.000000e+00 1.161806e+01 2.902150e+00 2.902150e+00 +1.416100e-01 0.000000e+00 0.000000e+00 1.377385e+01 1.970620e+00 1.970620e+00 +1.565000e-01 0.000000e+00 0.000000e+00 1.370059e+01 1.557860e+00 1.557860e+00 +1.729600e-01 0.000000e+00 0.000000e+00 1.168438e+01 1.238060e+00 1.238060e+00 +1.911500e-01 0.000000e+00 0.000000e+00 9.115620e+00 9.623000e-01 9.623000e-01 +2.112500e-01 0.000000e+00 0.000000e+00 9.900240e+00 9.924400e-01 9.924400e-01 +2.334700e-01 0.000000e+00 0.000000e+00 7.666180e+00 6.471100e-01 6.471100e-01 +2.580300e-01 0.000000e+00 0.000000e+00 7.273770e+00 5.881600e-01 5.881600e-01 +2.851600e-01 0.000000e+00 0.000000e+00 6.177480e+00 5.088500e-01 5.088500e-01 +3.151600e-01 0.000000e+00 0.000000e+00 4.759780e+00 4.028200e-01 4.028200e-01 +3.483000e-01 0.000000e+00 0.000000e+00 3.366220e+00 3.300000e-01 3.300000e-01 +3.849300e-01 0.000000e+00 0.000000e+00 2.706930e+00 2.168000e-01 2.168000e-01 +4.254200e-01 0.000000e+00 0.000000e+00 1.903570e+00 1.579500e-01 1.579500e-01 +4.701600e-01 0.000000e+00 0.000000e+00 1.322230e+00 1.216900e-01 1.216900e-01 +5.196000e-01 0.000000e+00 0.000000e+00 1.115480e+00 1.153500e-01 1.153500e-01 +5.742500e-01 0.000000e+00 0.000000e+00 6.209800e-01 6.313000e-02 6.313000e-02 +6.507100e-01 0.000000e+00 0.000000e+00 3.394300e-01 3.586000e-02 3.586000e-02 +8.566800e-01 0.000000e+00 0.000000e+00 8.818000e-02 1.299000e-02 1.299000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d08-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d08-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t8 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.041000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.804000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.520000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.311000e-02 0.000000e+00 0.000000e+00 2.235298e+01 8.647000e+00 8.647000e+00 +9.185000e-02 0.000000e+00 0.000000e+00 2.026210e+01 4.317820e+00 4.317820e+00 +1.015100e-01 0.000000e+00 0.000000e+00 2.257818e+01 3.288500e+00 3.288500e+00 +1.121800e-01 0.000000e+00 0.000000e+00 1.678101e+01 2.707310e+00 2.707310e+00 +1.239800e-01 0.000000e+00 0.000000e+00 1.715488e+01 1.529580e+00 1.529580e+00 +1.370200e-01 0.000000e+00 0.000000e+00 1.759574e+01 1.444040e+00 1.444040e+00 +1.514300e-01 0.000000e+00 0.000000e+00 1.449117e+01 9.737500e-01 9.737500e-01 +1.673600e-01 0.000000e+00 0.000000e+00 1.290911e+01 8.322300e-01 8.322300e-01 +1.849600e-01 0.000000e+00 0.000000e+00 1.138121e+01 7.631800e-01 7.631800e-01 +2.044100e-01 0.000000e+00 0.000000e+00 9.886320e+00 7.986900e-01 7.986900e-01 +2.259100e-01 0.000000e+00 0.000000e+00 9.529800e+00 6.206700e-01 6.206700e-01 +2.496600e-01 0.000000e+00 0.000000e+00 7.640330e+00 4.707000e-01 4.707000e-01 +2.759200e-01 0.000000e+00 0.000000e+00 6.282910e+00 3.872600e-01 3.872600e-01 +3.049400e-01 0.000000e+00 0.000000e+00 5.430170e+00 2.585200e-01 2.585200e-01 +3.370100e-01 0.000000e+00 0.000000e+00 4.244760e+00 1.860500e-01 1.860500e-01 +3.724600e-01 0.000000e+00 0.000000e+00 3.150600e+00 1.364900e-01 1.364900e-01 +4.116300e-01 0.000000e+00 0.000000e+00 2.345860e+00 1.100200e-01 1.100200e-01 +4.549200e-01 0.000000e+00 0.000000e+00 1.770860e+00 7.673000e-02 7.673000e-02 +5.027600e-01 0.000000e+00 0.000000e+00 1.241690e+00 6.339000e-02 6.339000e-02 +5.556400e-01 0.000000e+00 0.000000e+00 8.383500e-01 3.440000e-02 3.440000e-02 +6.140800e-01 0.000000e+00 0.000000e+00 5.264000e-01 2.293000e-02 2.293000e-02 +6.786600e-01 0.000000e+00 0.000000e+00 3.176500e-01 1.964000e-02 1.964000e-02 +7.690200e-01 0.000000e+00 0.000000e+00 1.850500e-01 1.421000e-02 1.421000e-02 +1.012440e+00 0.000000e+00 0.000000e+00 4.786000e-02 8.300000e-03 8.300000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d09-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d09-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t9 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.816000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.851000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.677000e-02 0.000000e+00 0.000000e+00 2.726916e+01 8.353500e+00 8.353500e+00 +9.589000e-02 0.000000e+00 0.000000e+00 2.512552e+01 5.659560e+00 5.659560e+00 +1.059800e-01 0.000000e+00 0.000000e+00 2.179860e+01 5.935040e+00 5.935040e+00 +1.171200e-01 0.000000e+00 0.000000e+00 1.983730e+01 3.843040e+00 3.843040e+00 +1.294400e-01 0.000000e+00 0.000000e+00 2.154088e+01 3.533880e+00 3.533880e+00 +1.430500e-01 0.000000e+00 0.000000e+00 1.691198e+01 2.643240e+00 2.643240e+00 +1.581000e-01 0.000000e+00 0.000000e+00 1.558819e+01 1.793840e+00 1.793840e+00 +1.747300e-01 0.000000e+00 0.000000e+00 1.393433e+01 1.346960e+00 1.346960e+00 +1.931000e-01 0.000000e+00 0.000000e+00 1.267526e+01 1.028250e+00 1.028250e+00 +2.134100e-01 0.000000e+00 0.000000e+00 1.048053e+01 9.074800e-01 9.074800e-01 +2.358600e-01 0.000000e+00 0.000000e+00 9.210490e+00 5.976700e-01 5.976700e-01 +2.606600e-01 0.000000e+00 0.000000e+00 7.439770e+00 5.754500e-01 5.754500e-01 +2.880700e-01 0.000000e+00 0.000000e+00 7.017390e+00 4.413200e-01 4.413200e-01 +3.183700e-01 0.000000e+00 0.000000e+00 5.089440e+00 2.816600e-01 2.816600e-01 +3.518600e-01 0.000000e+00 0.000000e+00 4.089590e+00 2.363400e-01 2.363400e-01 +3.888600e-01 0.000000e+00 0.000000e+00 3.029930e+00 1.868300e-01 1.868300e-01 +4.297600e-01 0.000000e+00 0.000000e+00 2.267620e+00 1.533900e-01 1.533900e-01 +4.749600e-01 0.000000e+00 0.000000e+00 1.555810e+00 1.012900e-01 1.012900e-01 +5.249100e-01 0.000000e+00 0.000000e+00 1.143310e+00 7.103000e-02 7.103000e-02 +5.801100e-01 0.000000e+00 0.000000e+00 8.485100e-01 5.851000e-02 5.851000e-02 +6.411200e-01 0.000000e+00 0.000000e+00 5.283900e-01 4.558000e-02 4.558000e-02 +7.085500e-01 0.000000e+00 0.000000e+00 3.264200e-01 2.762000e-02 2.762000e-02 +7.830700e-01 0.000000e+00 0.000000e+00 2.135200e-01 1.732000e-02 1.732000e-02 +8.873300e-01 0.000000e+00 0.000000e+00 1.111800e-01 9.200000e-03 9.200000e-03 +1.168200e+00 0.000000e+00 0.000000e+00 2.366000e-02 4.010000e-03 4.010000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d10-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d10-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t10 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.204000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.374000e-02 0.000000e+00 0.000000e+00 2.376925e+01 9.625860e+00 9.625860e+00 +9.255000e-02 0.000000e+00 0.000000e+00 2.304528e+01 6.571890e+00 6.571890e+00 +1.022800e-01 0.000000e+00 0.000000e+00 1.359290e+01 4.752570e+00 4.752570e+00 +1.130400e-01 0.000000e+00 0.000000e+00 2.624810e+01 6.227360e+00 6.227360e+00 +1.249300e-01 0.000000e+00 0.000000e+00 2.262020e+01 4.519470e+00 4.519470e+00 +1.380700e-01 0.000000e+00 0.000000e+00 1.779509e+01 2.574720e+00 2.574720e+00 +1.525900e-01 0.000000e+00 0.000000e+00 1.453687e+01 2.353570e+00 2.353570e+00 +1.686400e-01 0.000000e+00 0.000000e+00 1.384763e+01 1.746550e+00 1.746550e+00 +1.863700e-01 0.000000e+00 0.000000e+00 1.274209e+01 1.373280e+00 1.373280e+00 +2.059800e-01 0.000000e+00 0.000000e+00 1.117350e+01 8.990600e-01 8.990600e-01 +2.276400e-01 0.000000e+00 0.000000e+00 9.015150e+00 8.888700e-01 8.888700e-01 +2.515800e-01 0.000000e+00 0.000000e+00 8.173380e+00 6.540400e-01 6.540400e-01 +2.780400e-01 0.000000e+00 0.000000e+00 7.481210e+00 4.831200e-01 4.831200e-01 +3.072800e-01 0.000000e+00 0.000000e+00 5.807770e+00 4.164900e-01 4.164900e-01 +3.396000e-01 0.000000e+00 0.000000e+00 4.260990e+00 3.034600e-01 3.034600e-01 +3.753100e-01 0.000000e+00 0.000000e+00 3.463350e+00 2.308600e-01 2.308600e-01 +4.147800e-01 0.000000e+00 0.000000e+00 2.987790e+00 1.765800e-01 1.765800e-01 +4.584100e-01 0.000000e+00 0.000000e+00 1.951720e+00 1.213200e-01 1.213200e-01 +5.066200e-01 0.000000e+00 0.000000e+00 1.304950e+00 9.603000e-02 9.603000e-02 +5.599000e-01 0.000000e+00 0.000000e+00 9.449400e-01 6.539000e-02 6.539000e-02 +6.187900e-01 0.000000e+00 0.000000e+00 6.284900e-01 4.543000e-02 4.543000e-02 +6.838600e-01 0.000000e+00 0.000000e+00 3.918300e-01 3.332000e-02 3.332000e-02 +7.557900e-01 0.000000e+00 0.000000e+00 2.212700e-01 1.994000e-02 1.994000e-02 +8.352700e-01 0.000000e+00 0.000000e+00 1.528600e-01 2.103000e-02 2.103000e-02 +9.464900e-01 0.000000e+00 0.000000e+00 7.184000e-02 7.260000e-03 7.260000e-03 +1.246080e+00 0.000000e+00 0.000000e+00 1.544000e-02 2.690000e-03 2.690000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d11-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d11-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t11 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +8.918000e-02 0.000000e+00 0.000000e+00 4.340419e+01 1.123083e+01 1.123083e+01 +1.203800e-01 0.000000e+00 0.000000e+00 3.382256e+01 7.996410e+00 7.996410e+00 +1.330400e-01 0.000000e+00 0.000000e+00 2.201805e+01 4.541750e+00 4.541750e+00 +1.470300e-01 0.000000e+00 0.000000e+00 2.546093e+01 4.706460e+00 4.706460e+00 +1.625000e-01 0.000000e+00 0.000000e+00 1.971744e+01 3.883510e+00 3.883510e+00 +1.795900e-01 0.000000e+00 0.000000e+00 1.535101e+01 2.768440e+00 2.768440e+00 +1.984800e-01 0.000000e+00 0.000000e+00 1.454995e+01 2.281950e+00 2.281950e+00 +2.193500e-01 0.000000e+00 0.000000e+00 1.153763e+01 1.743290e+00 1.743290e+00 +2.424200e-01 0.000000e+00 0.000000e+00 8.103260e+00 1.009930e+00 1.009930e+00 +2.679100e-01 0.000000e+00 0.000000e+00 8.883650e+00 9.331500e-01 9.331500e-01 +2.960900e-01 0.000000e+00 0.000000e+00 6.784640e+00 6.410200e-01 6.410200e-01 +3.272300e-01 0.000000e+00 0.000000e+00 5.871540e+00 6.624700e-01 6.624700e-01 +3.616500e-01 0.000000e+00 0.000000e+00 4.606870e+00 3.883100e-01 3.883100e-01 +3.996800e-01 0.000000e+00 0.000000e+00 3.482240e+00 2.986300e-01 2.986300e-01 +4.417100e-01 0.000000e+00 0.000000e+00 2.643490e+00 2.332400e-01 2.332400e-01 +4.881700e-01 0.000000e+00 0.000000e+00 1.999280e+00 1.895500e-01 1.895500e-01 +5.395100e-01 0.000000e+00 0.000000e+00 1.307770e+00 1.132600e-01 1.132600e-01 +5.962500e-01 0.000000e+00 0.000000e+00 1.011440e+00 9.104000e-02 9.104000e-02 +6.589600e-01 0.000000e+00 0.000000e+00 6.758400e-01 6.535000e-02 6.535000e-02 +7.282600e-01 0.000000e+00 0.000000e+00 4.193900e-01 4.257000e-02 4.257000e-02 +8.048600e-01 0.000000e+00 0.000000e+00 2.475500e-01 2.619000e-02 2.619000e-02 +8.895000e-01 0.000000e+00 0.000000e+00 2.032500e-01 2.088000e-02 2.088000e-02 +9.830500e-01 0.000000e+00 0.000000e+00 1.120600e-01 1.494000e-02 1.494000e-02 +1.086440e+00 0.000000e+00 0.000000e+00 5.982000e-02 9.770000e-03 9.770000e-03 +1.200710e+00 0.000000e+00 0.000000e+00 2.448000e-02 6.130000e-03 6.130000e-03 +1.360580e+00 0.000000e+00 0.000000e+00 1.309000e-02 2.550000e-03 2.550000e-03 +1.791240e+00 0.000000e+00 0.000000e+00 2.110000e-03 5.000000e-04 5.000000e-04 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2004_I622224/d12-x01-y01 +IsRef: 1 +Path: /REF/BESII_2004_I622224/d12-x01-y01 +Title: doi:10.17182/hepdata.22183.v1/t12 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.306000e-02 0.000000e+00 0.000000e+00 3.127147e+01 8.052890e+00 8.052890e+00 +1.256200e-01 0.000000e+00 0.000000e+00 2.199663e+01 6.666960e+00 6.666960e+00 +1.388300e-01 0.000000e+00 0.000000e+00 3.066517e+01 6.068020e+00 6.068020e+00 +1.534300e-01 0.000000e+00 0.000000e+00 2.069243e+01 4.059030e+00 4.059030e+00 +1.695600e-01 0.000000e+00 0.000000e+00 1.659012e+01 3.100860e+00 3.100860e+00 +1.874000e-01 0.000000e+00 0.000000e+00 1.380083e+01 2.817750e+00 2.817750e+00 +2.071000e-01 0.000000e+00 0.000000e+00 1.490726e+01 1.950470e+00 1.950470e+00 +2.288900e-01 0.000000e+00 0.000000e+00 9.627090e+00 1.631090e+00 1.631090e+00 +2.529600e-01 0.000000e+00 0.000000e+00 9.958050e+00 1.209330e+00 1.209330e+00 +2.795600e-01 0.000000e+00 0.000000e+00 7.838710e+00 8.427500e-01 8.427500e-01 +3.089600e-01 0.000000e+00 0.000000e+00 5.975940e+00 8.114700e-01 8.114700e-01 +3.414600e-01 0.000000e+00 0.000000e+00 5.089480e+00 5.116000e-01 5.116000e-01 +3.773700e-01 0.000000e+00 0.000000e+00 4.295060e+00 3.541300e-01 3.541300e-01 +4.170600e-01 0.000000e+00 0.000000e+00 3.509830e+00 3.189100e-01 3.189100e-01 +4.609200e-01 0.000000e+00 0.000000e+00 2.298570e+00 2.607900e-01 2.607900e-01 +5.094000e-01 0.000000e+00 0.000000e+00 1.681710e+00 1.480400e-01 1.480400e-01 +5.629700e-01 0.000000e+00 0.000000e+00 1.262940e+00 1.276700e-01 1.276700e-01 +6.221800e-01 0.000000e+00 0.000000e+00 8.513700e-01 8.307000e-02 8.307000e-02 +6.876100e-01 0.000000e+00 0.000000e+00 6.313400e-01 5.234000e-02 5.234000e-02 +7.599300e-01 0.000000e+00 0.000000e+00 3.393800e-01 4.136000e-02 4.136000e-02 +8.398500e-01 0.000000e+00 0.000000e+00 2.168500e-01 2.546000e-02 2.546000e-02 +9.281800e-01 0.000000e+00 0.000000e+00 1.527200e-01 1.719000e-02 1.719000e-02 +1.025800e+00 0.000000e+00 0.000000e+00 7.704000e-02 1.117000e-02 1.117000e-02 +1.133680e+00 0.000000e+00 0.000000e+00 5.462000e-02 8.880000e-03 8.880000e-03 +1.252910e+00 0.000000e+00 0.000000e+00 2.515000e-02 5.460000e-03 5.460000e-03 +1.419730e+00 0.000000e+00 0.000000e+00 1.494000e-02 2.610000e-03 2.610000e-03 +1.869120e+00 0.000000e+00 0.000000e+00 2.590000e-03 6.700000e-04 6.700000e-04 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2005_I685906.cc b/analyses/pluginBES/BESII_2005_I685906.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2005_I685906.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2005_I685906 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2005_I685906); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nproton = bookCounter("TMP/proton"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PROTON) vetoEvent; + } + _nproton->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nproton->val(); + double error = _nproton->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nproton; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2005_I685906); + + +} diff --git a/analyses/pluginBES/BESII_2005_I685906.info b/analyses/pluginBES/BESII_2005_I685906.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2005_I685906.info @@ -0,0 +1,31 @@ +Name: BESII_2005_I685906 +Year: 2005 +Summary: Cross section for $e^+e^-\to$ proton and antiproton between 2 and 3.07 GeV +Experiment: BESII +Collider: BEPC +Authors: + - Peter Richardson +References: +- Phys.Rev. D91 (2015) 112004, 2015 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ for energies between 2 and 3.07 GeV' +InspireID: 685906 +BibKey: Ablikim:2005nn +BibTeX: '@article{Ablikim:2005nn, + author = "Ablikim, M. and others", + title = "{Measurement of the cross section for e+ e- ---> p anti-p + at center-of-mass energies from 2.0-GeV to 3.07-GeV}", + collaboration = "BES", + journal = "Phys. Lett.", + volume = "B630", + year = "2005", + pages = "14-20", + doi = "10.1016/j.physletb.2005.09.044", + eprint = "hep-ex/0506059", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0506059;%%" +}' diff --git a/analyses/pluginBES/BESII_2005_I685906.plot b/analyses/pluginBES/BESII_2005_I685906.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2005_I685906.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /BESII_2005_I685906/d01-x01-y01 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESII_2005_I685906.yoda b/analyses/pluginBES/BESII_2005_I685906.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2005_I685906.yoda @@ -0,0 +1,34 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2005_I685906/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2005_I685906/d01-x01-y01 +Title: doi:10.17182/hepdata.41880.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.000000e+00 0.000000e+00 0.000000e+00 3.300000e+02 2.103735e+02 2.541358e+02 +2.200000e+00 0.000000e+00 0.000000e+00 4.080000e+02 7.912016e+01 7.912016e+01 +2.400000e+00 0.000000e+00 0.000000e+00 6.400000e+01 4.119466e+01 7.310951e+01 +2.500000e+00 0.000000e+00 0.000000e+00 2.010000e+02 9.192388e+01 1.137453e+02 +2.600000e+00 0.000000e+00 0.000000e+00 3.300000e+01 7.280110e+00 7.280110e+00 +2.700000e+00 0.000000e+00 0.000000e+00 5.100000e+01 3.238827e+01 5.821512e+01 +2.800000e+00 0.000000e+00 0.000000e+00 4.000000e+01 2.531798e+01 4.517743e+01 +3.000000e+00 0.000000e+00 0.000000e+00 7.000000e+00 3.162278e+00 5.099020e+00 +3.070000e+00 0.000000e+00 0.000000e+00 7.000000e+00 2.236068e+00 3.162278e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2005_I685906/d01-x01-y02 +IsRef: 1 +Path: /REF/BESII_2005_I685906/d01-x01-y02 +Title: doi:10.17182/hepdata.41880.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.000000e+00 0.000000e+00 0.000000e+00 1.750000e+02 5.532630e+01 6.726812e+01 +2.200000e+00 0.000000e+00 0.000000e+00 1.790000e+02 1.772005e+01 1.772005e+01 +2.400000e+00 0.000000e+00 0.000000e+00 7.200000e+01 2.308679e+01 4.104875e+01 +2.500000e+00 0.000000e+00 0.000000e+00 1.310000e+02 2.927456e+01 3.721559e+01 +2.600000e+00 0.000000e+00 0.000000e+00 5.400000e+01 6.324555e+00 6.324555e+00 +2.700000e+00 0.000000e+00 0.000000e+00 7.000000e+01 2.220360e+01 3.911521e+01 +2.800000e+00 0.000000e+00 0.000000e+00 6.300000e+01 2.022375e+01 3.612478e+01 +3.000000e+00 0.000000e+00 0.000000e+00 2.800000e+01 6.082763e+00 1.004988e+01 +3.070000e+00 0.000000e+00 0.000000e+00 2.700000e+01 4.123106e+00 6.082763e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2006_I717665.cc b/analyses/pluginBES/BESII_2006_I717665.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2006_I717665.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2006_I717665 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2006_I717665); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(2,1,1); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(2, 1, 2); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2006_I717665); + + +} diff --git a/analyses/pluginBES/BESII_2006_I717665.info b/analyses/pluginBES/BESII_2006_I717665.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2006_I717665.info @@ -0,0 +1,35 @@ +Name: BESII_2006_I717665 +Year: 2006 +Summary: Measurement of $R$ for energies betweenv 3.65 and 3.773 GeV +Experiment: BESII +Collider: BEPC +InspireID: 717665 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B641 (2006) 145-155, 2006 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ and the hadronic cross section in $e^+e^-$ collisions by BESII for energies between 3.65 and 3.773, in the vicinity of the $\psi(3770)$. + The muonic cross section is also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Ablikim:2006aj +BibTeX: '@article{Ablikim:2006aj, + author = "Ablikim, M. and others", + title = "{Measurements of the cross-sections for e+ e- ---> + hadrons at 3.650-GeV, 3.6648-GeV, 3.773-GeV and the + branching fraction for psi(3770) ---> non - D anti-D}", + collaboration = "BES", + journal = "Phys. Lett.", + volume = "B641", + year = "2006", + pages = "145-155", + doi = "10.1016/j.physletb.2006.08.049", + eprint = "hep-ex/0605105", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0605105;%%" +}' diff --git a/analyses/pluginBES/BESII_2006_I717665.plot b/analyses/pluginBES/BESII_2006_I717665.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2006_I717665.plot @@ -0,0 +1,22 @@ +BEGIN PLOT /BESII_2006_I717665/d02-x01-y02 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2006_I717665/d02-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2006_I717665/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT + diff --git a/analyses/pluginBES/BESII_2006_I717665.yoda b/analyses/pluginBES/BESII_2006_I717665.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2006_I717665.yoda @@ -0,0 +1,60 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2006_I717665/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2006_I717665/d01-x01-y01 +Title: doi:10.17182/hepdata.41802.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.898300e+01 2.017251e-01 2.017251e-01 +3.664800e+00 0.000000e+00 0.000000e+00 1.829900e+01 2.656633e-01 2.656633e-01 +3.773000e+00 0.000000e+00 0.000000e+00 2.768000e+01 2.718308e-01 2.718308e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2006_I717665/d02-x01-y01 +IsRef: 1 +Path: /REF/BESII_2006_I717665/d02-x01-y01 +Title: doi:10.17182/hepdata.41802.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.457800e+01 6.083700e-01 6.083700e-01 +3.664800e+00 0.000000e+00 0.000000e+00 1.412800e+01 6.169968e-01 6.169968e-01 +3.773000e+00 0.000000e+00 0.000000e+00 2.285500e+01 1.165870e+00 1.165870e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2006_I717665/d02-x01-y02 +IsRef: 1 +Path: /REF/BESII_2006_I717665/d02-x01-y02 +Title: doi:10.17182/hepdata.41802.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 2.236000e+00 9.222256e-02 9.222256e-02 +3.664800e+00 0.000000e+00 0.000000e+00 2.185000e+00 9.289241e-02 9.289241e-02 +3.773000e+00 0.000000e+00 0.000000e+00 3.746000e+00 1.906017e-01 1.906017e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2006_I717665/d03-x01-y01 +IsRef: 1 +Path: /REF/BESII_2006_I717665/d03-x01-y01 +Title: doi:10.17182/hepdata.41802.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 3.664800e+00 3.664800e+00 2.218000e+00 9.100549e-02 9.100549e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2006_I717665/d04-x01-y01 +IsRef: 1 +Path: /REF/BESII_2006_I717665/d04-x01-y01 +Title: doi:10.17182/hepdata.41802.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.773000e+00 0.000000e+00 0.000000e+00 1.528000e+00 1.375682e-01 1.375682e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2006_I717665/d05-x01-y01 +IsRef: 1 +Path: /REF/BESII_2006_I717665/d05-x01-y01 +Title: doi:10.17182/hepdata.41802.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.773000e+00 0.000000e+00 0.000000e+00 9.323000e+00 8.400060e-01 8.400060e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2007_I750713.cc b/analyses/pluginBES/BESII_2007_I750713.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I750713.cc @@ -0,0 +1,180 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2007_I750713 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2007_I750713); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + // Book histograms + for(unsigned int ix=1;ix<19;++ix) { + stringstream ss; + ss << "TMP/n" << ix; + _nMeson[ix]= bookCounter(ss.str()); + } + + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=221 && p.pdgId()!=333) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta + if(p.pdgId()==221) { + if(ncount==4) { + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second!=2) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) _nMeson[12]->fill(event.weight()); + } + } + else if(p.pdgId()==333) { + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==321) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nMeson[7]->fill(event.weight()); + } + } + if(ntotal==3 && nCount[111]==1 && + nCount[-2212] == 1 && nCount[ 2212]==1) + _nMeson[16]->fill(event.weight()); + else if(ntotal==4) { + if(nCount[-211] == 2 && nCount[ 211]==2) + _nMeson[3]->fill(event.weight()); + else if(nCount[-211] == 1 && nCount[ 211]==1 && + nCount[-321] == 1 && nCount[ 321]==1) + _nMeson[4]->fill(event.weight()); + else if(nCount[-321] == 2 && nCount[ 321]==2) + _nMeson[6]->fill(event.weight()); + else if(nCount[-211 ] == 1 && nCount[ 211 ]==1 && + nCount[-2212] == 1 && nCount[ 2212]==1) + _nMeson[8]->fill(event.weight()); + else if(nCount[-321 ] == 1 && nCount[ 321 ]==1 && + nCount[-2212] == 1 && nCount[ 2212]==1) + _nMeson[9]->fill(event.weight()); + } + else if(ntotal==5 && nCount[111]==1) { + if(nCount[-211] == 2 && nCount[ 211]==2) + _nMeson[13]->fill(event.weight()); + else if(nCount[-211] == 1 && nCount[ 211]==1 && + nCount[-321] == 1 && nCount[ 321]==1) + _nMeson[14]->fill(event.weight()); + else if(nCount[-321] == 2 && nCount[ 321]==2) + _nMeson[15]->fill(event.weight()); + else if(nCount[-211 ] == 1 && nCount[ 211 ]==1 && + nCount[-2212] == 1 && nCount[ 2212]==1) + _nMeson[17]->fill(event.weight()); + } + else if(ntotal==6 && nCount[211]==3 && nCount[-211]==3) + _nMeson[11]->fill(event.weight()); + else if(ntotal==7 && nCount[111]==1 && + nCount[211]==3 && nCount[-211]==3) + _nMeson[18]->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=3;ix<19;++ix) { + if(ix==5 || ix==10) continue; + double sigma = _nMeson[ix]->val(); + double error = _nMeson[ix]->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + //@} + + /// @name Histograms + //@{ + CounterPtr _nMeson[19]; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2007_I750713); + + +} diff --git a/analyses/pluginBES/BESII_2007_I750713.info b/analyses/pluginBES/BESII_2007_I750713.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I750713.info @@ -0,0 +1,36 @@ +Name: BESII_2007_I750713 +Year: 2007 +Summary: Cross sections for light hadrons at 3.773, 3.650 GeV +Experiment: BESII +Collider: BEPC II +InspireID: 750713 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B650 (2007) 111-118, 2007 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to 2\pi^+2\pi^-$, $K^+K^-\pi^+\pi^-$, $2K^+2K^-$, $\phi K^+K^-$, + $p\bar{p}\pi^+\pi^-$, $p\bar{p}K^+K^-$, $3\pi^+3\pi^-$, $2\pi^+2\pi^-\eta$, $2\pi^+2\pi^-\pi^0$, + $K^+K^-\pi^+\pi^-\pi^0$, $2K^+2K^-\pi^0$, $p\bar{p}\pi^0$, $p\bar{p}\pi^+\pi^-\pi^0$, $3\pi^+3\pi^-\pi^0$ + at 3.773 and 3.650 GeV.' +Keywords: [] +BibKey: Ablikim:2007ss +BibTeX: '@article{Ablikim:2007ss, + author = "Ablikim, M. and others", + title = "{Measurements of the observed cross-sections for e+ e- + ---> light hadrons at s**(1/2) = 3.773-GeV and 3.650-GeV}", + collaboration = "BES", + journal = "Phys. Lett.", + volume = "B650", + year = "2007", + pages = "111-118", + doi = "10.1016/j.physletb.2007.05.011", + eprint = "0705.2276", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0705.2276;%%" +}' diff --git a/analyses/pluginBES/BESII_2007_I750713.plot b/analyses/pluginBES/BESII_2007_I750713.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I750713.plot @@ -0,0 +1,112 @@ +BEGIN PLOT /BESII_2007_I750713/d01-x01-y03 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y04 +Title=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y06 +Title=$\sigma(e^+e^-\to 2K^+2K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2K^+2K^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y07 +Title=$\sigma(e^+e^-\to \phi K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi K^+K^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y08 +Title=$\sigma(e^+e^-\to p\bar{p}\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p}\pi^+\pi^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y09 +Title=$\sigma(e^+e^-\to p\bar{p}K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p}K^+K^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y11 +Title=$\sigma(e^+e^-\to 3\pi^+3\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 3\pi^+3\pi^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y12 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-\eta)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y13 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y14 +Title=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y15 +Title=$\sigma(e^+e^-\to 2K^+2K^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2K^+2K^-\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y16 +Title=$\sigma(e^+e^-\to p\bar{p}\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p}\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y17 +Title=$\sigma(e^+e^-\to p\bar{p}\pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p}\pi^+\pi^-\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I750713/d01-x01-y18 +Title=$\sigma(e^+e^-\to 3\pi^+3\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 3\pi^+3\pi^-\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT diff --git a/analyses/pluginBES/BESII_2007_I750713.yoda b/analyses/pluginBES/BESII_2007_I750713.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I750713.yoda @@ -0,0 +1,171 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y01 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y02 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y02 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y03 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y03 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.777000e+02 2.302889e+01 2.302889e+01 +3.773000e+00 0.000000e+00 0.000000e+00 1.737000e+02 2.022672e+01 2.022672e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y04 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y04 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.617000e+02 2.475520e+01 2.475520e+01 +3.773000e+00 0.000000e+00 0.000000e+00 1.317000e+02 1.734416e+01 1.734416e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y05 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y05 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y06 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y06 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 2.410000e+01 7.000714e+00 7.000714e+00 +3.773000e+00 0.000000e+00 0.000000e+00 1.990000e+01 4.167733e+00 4.167733e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y07 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y07 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.740000e+01 9.414882e+00 9.414882e+00 +3.773000e+00 0.000000e+00 0.000000e+00 1.580000e+01 5.408327e+00 5.408327e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y08 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y08 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 4.210000e+01 7.762087e+00 7.762087e+00 +3.773000e+00 0.000000e+00 0.000000e+00 3.320000e+01 5.099020e+00 5.099020e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y09 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y09 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 6.100000e+00 3.178050e+00 3.178050e+00 +3.773000e+00 0.000000e+00 0.000000e+00 7.100000e+00 2.154066e+00 2.154066e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y10 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y10 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y11 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y11 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 2.349000e+02 4.076825e+01 4.076825e+01 +3.773000e+00 0.000000e+00 0.000000e+00 2.367000e+02 3.649178e+01 3.649178e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y12 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y12 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 8.660000e+01 4.162031e+01 4.162031e+01 +3.773000e+00 0.000000e+00 0.000000e+00 1.537000e+02 4.411995e+01 4.411995e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y13 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y13 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.243000e+02 2.632299e+01 2.632299e+01 +3.773000e+00 0.000000e+00 0.000000e+00 8.090000e+01 1.712338e+01 1.712338e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y14 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y14 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 2.228000e+02 4.648796e+01 4.648796e+01 +3.773000e+00 0.000000e+00 0.000000e+00 1.716000e+02 3.335881e+01 3.335881e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y15 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y15 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.773000e+00 0.000000e+00 0.000000e+00 1.810000e+01 7.981228e+00 7.981228e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y16 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y16 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 9.200000e+00 3.544009e+00 3.544009e+00 +3.773000e+00 0.000000e+00 0.000000e+00 1.010000e+01 2.416609e+00 2.416609e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y17 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y17 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 2.900000e+01 1.170043e+01 1.170043e+01 +3.773000e+00 0.000000e+00 0.000000e+00 5.310000e+01 1.144028e+01 1.144028e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I750713/d01-x01-y18 +IsRef: 1 +Path: /REF/BESII_2007_I750713/d01-x01-y18 +Title: doi:10.17182/hepdata.26996.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.266000e+02 5.086305e+01 5.086305e+01 +3.773000e+00 0.000000e+00 0.000000e+00 1.058000e+02 3.832714e+01 3.832714e+01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2007_I762901.cc b/analyses/pluginBES/BESII_2007_I762901.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I762901.cc @@ -0,0 +1,175 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2007_I762901 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2007_I762901); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + // Book histograms + for(unsigned int ix=1;ix<11;++ix) { + stringstream ss; + ss << "TMP/n" << ix; + _nMeson[ix]= bookCounter(ss.str()); + } + + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==6) { + if(nCount[211]==2 && nCount[-211]==2 && nCount[321]==1 && nCount[-321]==1) + _nMeson[1]->fill(event.weight()); + else if(nCount[211]==1 && nCount[-211]==1 && nCount[321]==2 && nCount[-321]==2) + _nMeson[2]->fill(event.weight()); + else if(nCount[211]==2 && nCount[-211]==2 && nCount[2212]==1 && nCount[-2212]==1) + _nMeson[3]->fill(event.weight()); + else if(nCount[211]==3 && nCount[-211]==3) + _nMeson[4]->fill(event.weight()); + } + else if(ntotal==7) { + if(nCount[211]==2 && nCount[-211]==2 && nCount[321]==1 && nCount[-321]==1 && nCount[111]==1) + _nMeson[5]->fill(event.weight()); + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=113 && abs(p.pdgId())!=313) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + if(p.pdgId()==113) { + if(ncount!=2) continue; + unsigned int nPi(0),nK(0),nProt(0); + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211 && val.second==1) { + nPi+=1; + } + else if(abs(val.first)==321 && val.second==1) { + nK+=1; + } + else if(abs(val.first)==2212 && val.second==1) { + nProt+=1; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(nProt==2 && nPi==0 && nK==0) + _nMeson[9]->fill(event.weight()); + else if(nProt==0 && nPi==2 && nK==0) + _nMeson[7]->fill(event.weight()); + else if(nProt==0 && nPi==0 && nK==2) + _nMeson[8]->fill(event.weight()); + } + } + else if(abs(p.pdgId())==313) { + if(ncount!=2) continue; + unsigned int npi(0),nK(0); + bool matched = true; + int ipi = p.pdgId()==313 ? 211 : -211; + int iK = p.pdgId()==313 ? -321 : 321; + for(auto const & val : nRes) { + if(abs(val.first)== ipi && val.second==1) { + npi+=1; + } + else if(abs(val.first)==iK && val.second==1) { + nK+=1; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(npi==1&&nK==1) + _nMeson[10]->fill(event.weight()); + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<11;++ix) { + if(ix==6) continue; + double sigma = _nMeson[ix]->val(); + double error = _nMeson[ix]->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nMeson[11]; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2007_I762901); + + +} diff --git a/analyses/pluginBES/BESII_2007_I762901.info b/analyses/pluginBES/BESII_2007_I762901.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I762901.info @@ -0,0 +1,36 @@ +Name: BESII_2007_I762901 +Year: 2007 +Summary: Cross sections for light hadrons at 3.650 and 3.773 GeV +Experiment: BESII +Collider: BEPC +InspireID: 762901 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B656 (2007) 30-37, 2007 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to 2\pi^+2\pi^-K^+K^-$, $\pi^+\pi^-2K^+2K^-$, + $2\pi^+2\pi^-p\bar{p}$, $3\pi^+3\pi^-$, $2\pi^+2\pi^-K^+K^-\pi^0$, + $\rho^0\pi^+\pi^-$, $\rho^0K^+K^-$, $\rho^0p\bar{p}$, $K^{*0}K^-\pi^++\text{c.c.}$ at 3.650 and 3.773 GeV.' +Keywords: [] +BibKey: Ablikim:2007af +BibTeX: '@article{Ablikim:2007af, + author = "Ablikim, M. and others", + title = "{Measurements of the observed cross-sections for + exclusive light hadron production in e+ e- annihilation at + s**(1/2) = 3.773-GeV and 3.650- GeV}", + collaboration = "BES", + journal = "Phys. Lett.", + volume = "B656", + year = "2007", + pages = "30-37", + doi = "10.1016/j.physletb.2007.10.001", + eprint = "0710.0786", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0710.0786;%%" +}' diff --git a/analyses/pluginBES/BESII_2007_I762901.plot b/analyses/pluginBES/BESII_2007_I762901.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I762901.plot @@ -0,0 +1,73 @@ +BEGIN PLOT /BESII_2007_I762901/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-K^+K^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I762901/d01-x01-y02 +Title=$\sigma(e^+e^-\to \pi^+\pi^-2K^+2K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-2K^+2K^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I762901/d01-x01-y03 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-p\bar{p})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +END PLOT +BEGIN PLOT /BESII_2007_I762901/d01-x01-y04 +Title=$\sigma(e^+e^-\to 3\pi^+3\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 3\pi^+3\pi^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I762901/d01-x01-y05 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-K^+K^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-K^+K^-\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I762901/d01-x01-y07 +Title=$\sigma(e^+e^-\to \rho^0 \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \rho^0 \pi^+\pi^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I762901/d01-x01-y08 +Title=$\sigma(e^+e^-\to \rho^0 K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \rho^0 K^+K^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I762901/d01-x01-y09 +Title=$\sigma(e^+e^-\to \rho^0 p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \rho^0 p\bar{p})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /BESII_2007_I762901/d01-x01-y10 +Title=$\sigma(e^+e^-\to K^{*0}K^-\pi^++\text{c.c.})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^{*0}K^-\pi^++\text{c.c.})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT diff --git a/analyses/pluginBES/BESII_2007_I762901.yoda b/analyses/pluginBES/BESII_2007_I762901.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I762901.yoda @@ -0,0 +1,113 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y01 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.649000e+02 3.816189e+01 3.816189e+01 +3.773000e+00 0.000000e+00 0.000000e+00 1.680000e+02 2.988193e+01 2.988193e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y02 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y02 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.773000e+00 0.000000e+00 0.000000e+00 1.190000e+01 6.044005e+00 6.044005e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y03 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y03 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 2.280000e+01 9.062009e+00 9.062009e+00 +3.773000e+00 0.000000e+00 0.000000e+00 2.350000e+01 6.103278e+00 6.103278e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y04 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y04 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 7.620000e+01 2.793421e+01 2.793421e+01 +3.773000e+00 0.000000e+00 0.000000e+00 1.318000e+02 3.061389e+01 3.061389e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y05 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y05 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.502000e+02 7.305135e+01 7.305135e+01 +3.773000e+00 0.000000e+00 0.000000e+00 2.315000e+02 7.357962e+01 7.357962e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y06 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y06 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y07 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y07 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.136000e+02 2.500600e+01 2.500600e+01 +3.773000e+00 0.000000e+00 0.000000e+00 1.119000e+02 1.852620e+01 1.852620e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y08 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y08 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 5.760000e+01 1.897630e+01 1.897630e+01 +3.773000e+00 0.000000e+00 0.000000e+00 3.420000e+01 1.231300e+01 1.231300e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y09 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y09 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.770000e+01 6.802941e+00 6.802941e+00 +3.773000e+00 0.000000e+00 0.000000e+00 1.310000e+01 3.671512e+00 3.671512e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y10 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y10 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 8.550000e+01 2.998416e+01 2.998416e+01 +3.773000e+00 0.000000e+00 0.000000e+00 9.470000e+01 1.866574e+01 1.866574e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y11 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y11 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I762901/d01-x01-y12 +IsRef: 1 +Path: /REF/BESII_2007_I762901/d01-x01-y12 +Title: doi:10.17182/hepdata.26970.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2007_I763880.cc b/analyses/pluginBES/BESII_2007_I763880.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I763880.cc @@ -0,0 +1,204 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2007_I763880 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2007_I763880); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + // Book histograms + for(unsigned int ix=1;ix<8;++ix) { + stringstream ss; + ss << "TMP/n" << ix; + _nMeson[ix]= bookCounter(ss.str()); + } + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=223 && p.pdgId()!=113&&abs(p.pdgId())!=313&& abs(p.pdgId())!=323) + continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + if(p.pdgId()==113) { + if(ncount!=3) continue; + unsigned int npi(0),nK(0); + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==111 && val.second==1) { + npi+=1; + } + else if(abs(val.first)==321 && val.second==1) { + nK+=1; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(npi==1&&nK==2) + _nMeson[4]->fill(event.weight()); + } + } + else if(abs(p.pdgId())==213) { + if(ncount!=3) continue; + unsigned int npi(0),nK(0); + bool matched = true; + int ipi = p.pdgId()==213 ? -211 : 211; + for(auto const & val : nRes) { + if(abs(val.first)== ipi && val.second==1) { + npi+=1; + } + else if(abs(val.first)==321 && val.second==1) { + nK+=1; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(npi==1&&nK==2) + _nMeson[5]->fill(event.weight()); + } + } + else if(abs(p.pdgId())==313) { + if(ncount!=3) continue; + unsigned int npi(0),nK(0),npi0(0); + bool matched = true; + int ipi = p.pdgId()==313 ? 211 : -211; + int iK = p.pdgId()==313 ? -321 : 321; + for(auto const & val : nRes) { + if(abs(val.first)== ipi && val.second==1) { + npi+=1; + } + else if(abs(val.first)==iK && val.second==1) { + nK+=1; + } + if(abs(val.first)== 111 && val.second==1) { + npi0+=1; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(npi==1&&nK==1&&npi0==1) + _nMeson[6]->fill(event.weight()); + } + } + else if(abs(p.pdgId())==323) { + if(ncount!=3) continue; + unsigned int npi(0),nK(0),npi0(0); + bool matched = true; + int ipi = p.pdgId()==323 ? 211 : -211; + int iK = p.pdgId()==323 ? -321 : 321; + for(auto const & val : nRes) { + if(abs(val.first)== ipi && val.second==1) { + npi+=1; + } + else if(abs(val.first)==iK && val.second==1) { + nK+=1; + } + if(abs(val.first)== 111 && val.second==1) { + npi0+=1; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(npi==1&&nK==1&&npi0==1) + _nMeson[7]->fill(event.weight()); + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=4;ix<8;++ix) { + double sigma = _nMeson[ix]->val(); + double error = _nMeson[ix]->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nMeson[8]; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2007_I763880); + + +} diff --git a/analyses/pluginBES/BESII_2007_I763880.info b/analyses/pluginBES/BESII_2007_I763880.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I763880.info @@ -0,0 +1,37 @@ +Name: BESII_2007_I763880 +Year: 2007 +Summary: Cross sections for light hadrons at 3.773 and 3.650 GeV +Experiment: BESII +Collider: BEPC +InspireID: 763880 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B670 (2008) 184-189, 2008 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to \omega \pi^+\pi^-$, $\omega K^+K^-$, $\omega p\bar{p}$, + $K^+K^-\rho^0\pi^0$, $K^+K^-\rho^+\pi^-+\text{c.c.}$, + $K^{*0}K^-\pi^+\pi^0+\text{c.c.}$ and $K^{*+}K^-\pi^+\pi^-+\text{c.c.}$ at 3.773 and 3.650 GeV.' +Keywords: [] +BibKey: Ablikim:2007ae +BibTeX: '@article{Ablikim:2007ae, + author = "Ablikim, M. and others", + title = "{Experimental studies of the $\pi^+\pi^-\pi^+\pi^-\pi^0$, + $K^+K^-\pi^+\pi^-\pi^0$ and $p\bar p\pi^+\pi^-\pi^0$ final + states produced in $e^+e^-$ annihilation at $\sqrt{s}=$ + 3.773 and 3.650 GeV}", + collaboration = "BES", + journal = "Eur. Phys. J.", + volume = "C52", + year = "2007", + pages = "805-811", + doi = "10.1140/epjc/s10052-007-0438-9", + eprint = "0710.2176", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0710.2176;%%" +}' diff --git a/analyses/pluginBES/BESII_2007_I763880.plot b/analyses/pluginBES/BESII_2007_I763880.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I763880.plot @@ -0,0 +1,62 @@ +BEGIN PLOT /BESII_2007_I763880/d01-x01-y01 +Title=$\sigma(e^+e^-\to \omega \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega \pi^+\pi^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2007_I763880/d01-x01-y02 +Title=$\sigma(e^+e^-\to \omega K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega K^+K^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2007_I763880/d01-x01-y03 +Title=$\sigma(e^+e^-\to \omega p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega p\bar{p})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2007_I763880/d01-x01-y04 +Title=$\sigma(e^+e^-\to K^+K^-\rho^0\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\rho^0\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2007_I763880/d01-x01-y05 +Title=$\sigma(e^+e^-\to K^+K^-\rho^+\pi^-+\text{c.c.})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\rho^+\pi^-+\text{c.c.})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2007_I763880/d01-x01-y06 +Title=$\sigma(e^+e^-\to K^{*0}K^-\pi^+\pi^0+\text{c.c.})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^{*0}K^-\pi^+\pi^0+\text{c.c.})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2007_I763880/d01-x01-y07 +Title=$\sigma(e^+e^-\to K^{*+}K^-\pi^+\pi^-+\text{c.c.})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^{*+}K^-\pi^+\pi^-+\text{c.c.})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT \ No newline at end of file diff --git a/analyses/pluginBES/BESII_2007_I763880.yoda b/analyses/pluginBES/BESII_2007_I763880.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2007_I763880.yoda @@ -0,0 +1,79 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I763880/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2007_I763880/d01-x01-y01 +Title: doi:10.17182/hepdata.43093.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I763880/d01-x01-y02 +IsRef: 1 +Path: /REF/BESII_2007_I763880/d01-x01-y02 +Title: doi:10.17182/hepdata.43093.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I763880/d01-x01-y03 +IsRef: 1 +Path: /REF/BESII_2007_I763880/d01-x01-y03 +Title: doi:10.17182/hepdata.43093.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I763880/d01-x01-y04 +IsRef: 1 +Path: /REF/BESII_2007_I763880/d01-x01-y04 +Title: doi:10.17182/hepdata.43093.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 4.760000e+01 3.507207e+01 3.507207e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I763880/d01-x01-y05 +IsRef: 1 +Path: /REF/BESII_2007_I763880/d01-x01-y05 +Title: doi:10.17182/hepdata.43093.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.419000e+02 5.682411e+01 5.682411e+01 +3.773000e+00 0.000000e+00 0.000000e+00 9.420000e+01 3.369644e+01 3.369644e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I763880/d01-x01-y06 +IsRef: 1 +Path: /REF/BESII_2007_I763880/d01-x01-y06 +Title: doi:10.17182/hepdata.43093.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.281000e+02 6.213421e+01 6.213421e+01 +3.773000e+00 0.000000e+00 0.000000e+00 1.163000e+02 3.833132e+01 3.833132e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I763880/d01-x01-y07 +IsRef: 1 +Path: /REF/BESII_2007_I763880/d01-x01-y07 +Title: doi:10.17182/hepdata.43093.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.890000e+02 1.196701e+02 1.196701e+02 +3.773000e+00 0.000000e+00 0.000000e+00 1.739000e+02 7.780810e+01 7.780810e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I763880/d01-x01-y08 +IsRef: 1 +Path: /REF/BESII_2007_I763880/d01-x01-y08 +Title: doi:10.17182/hepdata.43093.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2007_I763880/d01-x01-y09 +IsRef: 1 +Path: /REF/BESII_2007_I763880/d01-x01-y09 +Title: doi:10.17182/hepdata.43093.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2008_I801208.cc b/analyses/pluginBES/BESII_2008_I801208.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2008_I801208.cc @@ -0,0 +1,117 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2008_I801208 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2008_I801208); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + for(unsigned int ix=1;ix<7;++ix) { + stringstream ss; + ss << "TMP/n" << ix; + _nMeson[ix]= bookCounter(ss.str()); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(nCount[310]!=1) vetoEvent; + + if(ntotal==3) { + if((nCount[ 211]==1 && nCount[-321]==1) || + (nCount[-211]==1 && nCount[ 321]==1) ) + _nMeson[1]->fill(event.weight()); + } + else if(ntotal==4&&nCount[111]==1) { + if((nCount[ 211]==1 && nCount[-321]==1) || + (nCount[-211]==1 && nCount[ 321]==1) ) + _nMeson[2]->fill(event.weight()); + } + else if(ntotal==5) { + if((nCount[ 211]==2 && nCount[-211]==1 && nCount[-321]==1) || + (nCount[-211]==2 && nCount[ 211]==1 && nCount[ 321]==1) ) + _nMeson[3]->fill(event.weight()); + if(((nCount[ 211]==1 && nCount[-321]==1) || + (nCount[-211]==1 && nCount[ 321]==1) ) && nCount[111]==2) + _nMeson[6]->fill(event.weight()); + } + else if(ntotal==6&&nCount[111]==1) { + if((nCount[ 211]==2 && nCount[-211]==1 && nCount[-321]==1) || + (nCount[-211]==2 && nCount[ 211]==1 && nCount[ 321]==1) ) + _nMeson[4]->fill(event.weight()); + } + else if(ntotal==7) { + if((nCount[ 211]==3 && nCount[-211]==2 && nCount[-321]==1) || + (nCount[-211]==3 && nCount[ 211]==2 && nCount[ 321]==1) ) + _nMeson[5]->fill(event.weight()); + } + } + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<7;++ix) { + double sigma = _nMeson[ix]->val(); + double error = _nMeson[ix]->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nMeson[7]; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2008_I801208); + + +} diff --git a/analyses/pluginBES/BESII_2008_I801208.info b/analyses/pluginBES/BESII_2008_I801208.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2008_I801208.info @@ -0,0 +1,34 @@ +Name: BESII_2008_I801208 +Year: 2008 +Summary: Cross sections for light hadrons at 3.773 and 3.650 GeV +Experiment: BESII +Collider: BEPC II +InspireID: 801208 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B670 (2008) 179-183, 2008 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to K^-\pi^+$, $K^-\pi^+\pi^0$, $K^-\pi^+\pi^+\pi^-$, $K^-\pi^+\pi^+\pi^-\pi^0$ + and $K^-\pi^+\pi^0\pi^0$ together with a $K_S^0$ meson at 3.773 and 3.650 GeV.' +BibKey: Ablikim:2008aa +BibTeX: '@article{Ablikim:2008aa, + author = "Ablikim, M. and others", + title = "{Measurements of the observed cross sections for e+ e- + ---> exclusive light hadrons containing K0(S) meson at + s**(1/2) = 3.773-GeV and 3.650-GeV}", + collaboration = "BES", + journal = "Phys. Lett.", + volume = "B670", + year = "2008", + pages = "179-183", + doi = "10.1016/j.physletb.2008.10.050", + eprint = "0810.5608", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0810.5608;%%" +}' diff --git a/analyses/pluginBES/BESII_2008_I801208.plot b/analyses/pluginBES/BESII_2008_I801208.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2008_I801208.plot @@ -0,0 +1,53 @@ +BEGIN PLOT /BESII_2008_I801208/d01-x01-y01 +Title=$\sigma(e^+e^-\to K_S^0K^-\pi^++\text{c.c})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K^-\pi^++\text{c.c})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2008_I801208/d01-x01-y02 +Title=$\sigma(e^+e^-\to K_S^0+K^-\pi^+\pi^0+\text{c.c})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K^-\pi^+\pi^0+\text{c.c})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2008_I801208/d01-x01-y03 +Title=$\sigma(e^+e^-\to K_S^0K^-\pi^+\pi^+\pi^-+\text{c.c})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K^-\pi^+\pi^+\pi^-+\text{c.c})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2008_I801208/d01-x01-y04 +Title=$\sigma(e^+e^-\to K_S^0K^-\pi^+\pi^+\pi^-\pi^0+\text{c.c})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K^-\pi^+\pi^+\pi^-\pi^0+\text{c.c})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2008_I801208/d01-x01-y05 +Title=$\sigma(e^+e^-\to K_S^0K^-\pi^+\pi^+\pi^+\pi^-\pi^-+\text{c.c})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K^-\pi^+\pi^+\pi^+\pi^-\pi^-+\text{c.c})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2008_I801208/d01-x01-y06 +Title=$\sigma(e^+e^-\to K_S^0K^-\pi^+\pi^0\pi^0+\text{c.c})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K^-\pi^+\pi^0\pi^0+\text{c.c})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT diff --git a/analyses/pluginBES/BESII_2008_I801208.yoda b/analyses/pluginBES/BESII_2008_I801208.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2008_I801208.yoda @@ -0,0 +1,58 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801208/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2008_I801208/d01-x01-y01 +Title: doi:10.17182/hepdata.50468.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.773000e+00 0.000000e+00 0.000000e+00 1.520000e+01 4.123106e+00 4.123106e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801208/d01-x01-y02 +IsRef: 1 +Path: /REF/BESII_2008_I801208/d01-x01-y02 +Title: doi:10.17182/hepdata.50468.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 4.790000e+01 1.885099e+01 1.885099e+01 +3.773000e+00 0.000000e+00 0.000000e+00 9.620000e+01 1.939124e+01 1.939124e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801208/d01-x01-y03 +IsRef: 1 +Path: /REF/BESII_2008_I801208/d01-x01-y03 +Title: doi:10.17182/hepdata.50468.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 8.140000e+01 2.580426e+01 2.580426e+01 +3.773000e+00 0.000000e+00 0.000000e+00 9.150000e+01 2.007710e+01 2.007710e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801208/d01-x01-y04 +IsRef: 1 +Path: /REF/BESII_2008_I801208/d01-x01-y04 +Title: doi:10.17182/hepdata.50468.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.190000e+02 6.787002e+01 6.787002e+01 +3.773000e+00 0.000000e+00 0.000000e+00 2.530000e+02 6.881112e+01 6.881112e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801208/d01-x01-y05 +IsRef: 1 +Path: /REF/BESII_2008_I801208/d01-x01-y05 +Title: doi:10.17182/hepdata.50468.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.773000e+00 0.000000e+00 0.000000e+00 4.440000e+01 2.338482e+01 2.338482e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801208/d01-x01-y06 +IsRef: 1 +Path: /REF/BESII_2008_I801208/d01-x01-y06 +Title: doi:10.17182/hepdata.50468.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 6.710000e+01 4.179402e+01 4.179402e+01 +3.773000e+00 0.000000e+00 0.000000e+00 1.470000e+02 4.731554e+01 4.731554e+01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2008_I801210.cc b/analyses/pluginBES/BESII_2008_I801210.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2008_I801210.cc @@ -0,0 +1,108 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2008_I801210 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2008_I801210); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + for(unsigned int ix=1;ix<6;++ix) { + stringstream ss; + ss << "TMP/n" << ix; + _nMeson[ix]= bookCounter(ss.str()); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(nCount[111]!=2) vetoEvent; + + if(ntotal==4) { + if(nCount[211]==1 && nCount[-211]==1) + _nMeson[1]->fill(event.weight()); + else if(nCount[321]==1 && nCount[-321]==1) + _nMeson[2]->fill(event.weight()); + } + else if(ntotal==6) { + if(nCount[211]==2 && nCount[-211]==2) + _nMeson[3]->fill(event.weight()); + else if(nCount[321]==1 && nCount[-321]==1 && + nCount[211]==1 && nCount[-211]==1) + _nMeson[4]->fill(event.weight()); + } + else if(ntotal==8) { + if(nCount[211]==3 && nCount[-211]==3) + _nMeson[5]->fill(event.weight()); + } + + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<6;++ix) { + double sigma = _nMeson[ix]->val(); + double error = _nMeson[ix]->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nMeson[6]; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2008_I801210); + + +} diff --git a/analyses/pluginBES/BESII_2008_I801210.info b/analyses/pluginBES/BESII_2008_I801210.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2008_I801210.info @@ -0,0 +1,34 @@ +Name: BESII_2008_I801210 +Year: 2008 +Summary: Cross sections for light hadrons at 3.773, 3.650 and 3.6648 GeV +Experiment: BESII +Collider: BEPC II +InspireID: 801210 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B670 (2008) 184-189, 2008 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to \pi^+\pi^-$, $K^+K^-$, $2\pi^+2\pi^-$, $K^+K^-\pi^+\pi^-$ and $3\pi^+3\pi^-$ + together with a $\pi^0\pi^0$ pair at 3.773, 3.650 and 3.6648 GeV.' +BibKey: Ablikim:2008vk +BibTeX: '@article{Ablikim:2008vk, + author = "Ablikim, M. and others", + title = "{Measurements of the observed cross sections for e+e- + ---> exclusive light hadrons containing pi0 pi0 at s**(1/) + = 3.773, 3.650 and 3.6648-GeV}", + collaboration = "BES", + journal = "Phys. Lett.", + volume = "B670", + year = "2008", + pages = "184-189", + doi = "10.1016/j.physletb.2008.10.051", + eprint = "0810.5611", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0810.5611;%%" +}' diff --git a/analyses/pluginBES/BESII_2008_I801210.plot b/analyses/pluginBES/BESII_2008_I801210.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2008_I801210.plot @@ -0,0 +1,44 @@ +BEGIN PLOT /BESII_2008_I801210/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2008_I801210/d01-x01-y02 +Title=$\sigma(e^+e^-\to K^+K^-2\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-2\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2008_I801210/d01-x01-y03 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-2\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2008_I801210/d01-x01-y04 +Title=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-2\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT + +BEGIN PLOT /BESII_2008_I801210/d01-x01-y05 +Title=$\sigma(e^+e^-\to 3\pi^+3\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 3\pi^+3\pi^-2\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT diff --git a/analyses/pluginBES/BESII_2008_I801210.yoda b/analyses/pluginBES/BESII_2008_I801210.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2008_I801210.yoda @@ -0,0 +1,52 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801210/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2008_I801210/d01-x01-y01 +Title: doi:10.17182/hepdata.50497.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 2.922000e+02 5.861672e+01 5.861672e+01 +3.664800e+00 0.000000e+00 0.000000e+00 3.973000e+02 1.045299e+02 1.045299e+02 +3.773000e+00 0.000000e+00 0.000000e+00 2.148000e+02 3.746211e+01 3.746211e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801210/d01-x01-y02 +IsRef: 1 +Path: /REF/BESII_2008_I801210/d01-x01-y02 +Title: doi:10.17182/hepdata.50497.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 5.430000e+01 2.350340e+01 2.350340e+01 +3.773000e+00 0.000000e+00 0.000000e+00 2.670000e+01 1.302920e+01 1.302920e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801210/d01-x01-y03 +IsRef: 1 +Path: /REF/BESII_2008_I801210/d01-x01-y03 +Title: doi:10.17182/hepdata.50497.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 1.077300e+03 2.426492e+02 2.426492e+02 +3.664800e+00 0.000000e+00 0.000000e+00 8.764000e+02 3.201725e+02 3.201725e+02 +3.773000e+00 0.000000e+00 0.000000e+00 1.051500e+03 1.902670e+02 1.902670e+02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801210/d01-x01-y04 +IsRef: 1 +Path: /REF/BESII_2008_I801210/d01-x01-y04 +Title: doi:10.17182/hepdata.50497.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 3.791000e+02 1.504016e+02 1.504016e+02 +3.773000e+00 0.000000e+00 0.000000e+00 1.860000e+02 9.186076e+01 9.186076e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2008_I801210/d01-x01-y05 +IsRef: 1 +Path: /REF/BESII_2008_I801210/d01-x01-y05 +Title: doi:10.17182/hepdata.50497.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.650000e+00 0.000000e+00 0.000000e+00 8.421000e+02 3.501997e+02 3.501997e+02 +3.773000e+00 0.000000e+00 0.000000e+00 9.738000e+02 3.186470e+02 3.186470e+02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BESII_2009_I814778.cc b/analyses/pluginBES/BESII_2009_I814778.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2009_I814778.cc @@ -0,0 +1,98 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BESII_2009_I814778 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BESII_2009_I814778); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BESII_2009_I814778); + + +} diff --git a/analyses/pluginBES/BESII_2009_I814778.info b/analyses/pluginBES/BESII_2009_I814778.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2009_I814778.info @@ -0,0 +1,34 @@ +Name: BESII_2009_I814778 +Year: 2009 +Summary: Measurement of $R$ for energies between 2.6 and 3.65 GeV +Experiment: BESII +Collider: BEPC +InspireID: 814778 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B677 (2009) 239-245, 2009 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by BESII for energies between 2.6 and 3.65 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Ablikim:2009ad +BibTeX: '@article{Ablikim:2009ad, + author = "Ablikim, M. and others", + title = "{R value measurements for e+ e- annihilation at 2.60-GeV, + 3.07-GeV and 3.65-GeV}", + collaboration = "BES", + journal = "Phys. Lett.", + volume = "B677", + year = "2009", + pages = "239-245", + doi = "10.1016/j.physletb.2009.05.055", + eprint = "0903.0900", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0903.0900;%%" +}' diff --git a/analyses/pluginBES/BESII_2009_I814778.plot b/analyses/pluginBES/BESII_2009_I814778.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2009_I814778.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /BESII_2009_I814778/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2009_I814778/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BESII_2009_I814778/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BESII_2009_I814778.yoda b/analyses/pluginBES/BESII_2009_I814778.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BESII_2009_I814778.yoda @@ -0,0 +1,11 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BESII_2009_I814778/d01-x01-y01 +IsRef: 1 +Path: /REF/BESII_2009_I814778/d01-x01-y01 +Title: doi:10.17182/hepdata.51953.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.600000e+00 0.000000e+00 0.000000e+00 2.180000e+00 8.246211e-02 8.246211e-02 +3.070000e+00 0.000000e+00 0.000000e+00 2.130000e+00 7.280110e-02 7.280110e-02 +3.650000e+00 0.000000e+00 0.000000e+00 2.140000e+00 7.071068e-02 7.071068e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginBES/BES_1995_I39870.cc b/analyses/pluginBES/BES_1995_I39870.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BES_1995_I39870.cc @@ -0,0 +1,88 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BES_1995_I39870 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BES_1995_I39870); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + vetoEvent; + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + } + else { + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BES_1995_I39870); + + +} diff --git a/analyses/pluginBES/BES_1995_I39870.info b/analyses/pluginBES/BES_1995_I39870.info new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BES_1995_I39870.info @@ -0,0 +1,31 @@ +Name: BES_1995_I39870 +Year: 1995 +Summary: Measurement of the hadronic cross section for energies between 3.08 and 3.116 GeV +Experiment: BES +Collider: BEPC +InspireID: 39870 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B355 (1995) 374-380, 1995 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of the hadronic cross section in $e^+e^-$ collisions by BES for energies between 3.08 and 3.116 GeV.' +BibKey: Bai:1995ik +BibTeX: '@article{Bai:1995ik, + author = "Bai, J. Z. and others", + title = "{A Measurement of J / psi decay widths}", + collaboration = "BES", + journal = "Phys. Lett.", + volume = "B355", + year = "1995", + pages = "374-380", + doi = "10.1016/0370-2693(95)01220-2, + 10.1016/0370-2693(95)00712-T", + note = "[Erratum: Phys. Lett.B363,267(1995)]", + reportNumber = "BIHEP-EP1-95-03", + SLACcitation = "%%CITATION = PHLTA,B355,374;%%" +}' diff --git a/analyses/pluginBES/BES_1995_I39870.plot b/analyses/pluginBES/BES_1995_I39870.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BES_1995_I39870.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /BES_1995_I39870/d01-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginBES/BES_1995_I39870.yoda b/analyses/pluginBES/BES_1995_I39870.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginBES/BES_1995_I39870.yoda @@ -0,0 +1,31 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BES_1995_I39870/d01-x01-y01 +IsRef: 1 +Path: /REF/BES_1995_I39870/d01-x01-y01 +Title: doi:10.17182/hepdata.28500.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.080490e+00 0.000000e+00 0.000000e+00 2.000000e+01 2.813468e+00 2.813468e+00 +3.085540e+00 0.000000e+00 0.000000e+00 1.750000e+01 2.926992e+00 2.926992e+00 +3.090630e+00 0.000000e+00 0.000000e+00 2.070000e+01 2.908528e+00 2.908528e+00 +3.092580e+00 0.000000e+00 0.000000e+00 2.940000e+01 4.370130e+00 4.370130e+00 +3.093730e+00 0.000000e+00 0.000000e+00 1.070000e+02 1.052134e+01 1.052134e+01 +3.094520e+00 0.000000e+00 0.000000e+00 4.360000e+02 3.509683e+01 3.509683e+01 +3.095300e+00 0.000000e+00 0.000000e+00 1.230000e+03 9.358514e+01 9.358514e+01 +3.095670e+00 0.000000e+00 0.000000e+00 1.840000e+03 1.382366e+02 1.382366e+02 +3.096070e+00 0.000000e+00 0.000000e+00 2.130000e+03 1.626267e+02 1.626267e+02 +3.096470e+00 0.000000e+00 0.000000e+00 2.428000e+03 1.814529e+02 1.814529e+02 +3.096860e+00 0.000000e+00 0.000000e+00 2.450000e+03 1.830955e+02 1.830955e+02 +3.097630e+00 0.000000e+00 0.000000e+00 1.498000e+03 1.122461e+02 1.122461e+02 +3.098020e+00 0.000000e+00 0.000000e+00 1.002000e+03 7.572699e+01 7.572699e+01 +3.098420e+00 0.000000e+00 0.000000e+00 6.560000e+02 5.226060e+01 5.226060e+01 +3.098800e+00 0.000000e+00 0.000000e+00 3.880000e+02 3.342950e+01 3.342950e+01 +3.099190e+00 0.000000e+00 0.000000e+00 3.010000e+02 2.710607e+01 2.710607e+01 +3.099600e+00 0.000000e+00 0.000000e+00 2.220000e+02 2.116227e+01 2.116227e+01 +3.099980e+00 0.000000e+00 0.000000e+00 1.940000e+02 1.805631e+01 1.805631e+01 +3.100750e+00 0.000000e+00 0.000000e+00 1.540000e+02 1.549727e+01 1.549727e+01 +3.102780e+00 0.000000e+00 0.000000e+00 1.070000e+02 9.646692e+00 9.646692e+00 +3.105490e+00 0.000000e+00 0.000000e+00 9.360000e+01 8.324831e+00 8.324831e+00 +3.110140e+00 0.000000e+00 0.000000e+00 6.420000e+01 6.379774e+00 6.379774e+00 +3.116360e+00 0.000000e+00 0.000000e+00 5.080000e+01 5.396023e+00 5.396023e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEOC_2005_I693873.cc b/analyses/pluginCESR/CLEOC_2005_I693873.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEOC_2005_I693873.cc @@ -0,0 +1,108 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEOC_2005_I693873 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEOC_2005_I693873); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npipi = bookCounter("TMP/npipi"); + _nKK = bookCounter("TMP/nKK"); + _nppbar = bookCounter("TMP/nppbar"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=2) vetoEvent; + + if(nCount[211]==1 && nCount[-211]==1) + _npipi->fill(event.weight()); + else if(nCount[321]==1 && nCount[-321]==1) + _nKK->fill(event.weight()); + else if(nCount[2212]==1 && nCount[-2212]==1) + _nppbar->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + + for(unsigned int ix=1;ix<4;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _npipi->val(); + error = _npipi->err(); + } + else if(ix==2) { + sigma = _nKK->val(); + error = _nKK->err(); + } + else if(ix==3) { + sigma = _nppbar->val(); + error = _nppbar->err(); + } + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npipi,_nKK,_nppbar; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEOC_2005_I693873); + + +} diff --git a/analyses/pluginCESR/CLEOC_2005_I693873.info b/analyses/pluginCESR/CLEOC_2005_I693873.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEOC_2005_I693873.info @@ -0,0 +1,36 @@ +Name: CLEOC_2005_I693873 +Year: 2005 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$, $K^+K^-$ and $p\bar{p}$ at 3.671 GeV +Experiment: CLEOC +Collider: CESR +InspireID: 693873 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 95 (2005) 261803 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e-, e+] +Energies: [3.671] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$, $K^+K^-$ and $p\bar{p}$ at 3.671 GeV by CLEO-c.' +Keywords: [] +BibKey: Pedlar:2005sj +BibTeX: '@article{Pedlar:2005sj, + author = "Pedlar, T. K. and others", + title = "{Precision measurements of the timelike electromagnetic + form-factors of pion, kaon, and proton}", + collaboration = "CLEO", + journal = "Phys. Rev. Lett.", + volume = "95", + year = "2005", + pages = "261803", + doi = "10.1103/PhysRevLett.95.261803", + eprint = "hep-ex/0510005", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "CLNS-05-1936, CLEO-05-24", + SLACcitation = "%%CITATION = HEP-EX/0510005;%%" +}' diff --git a/analyses/pluginCESR/CLEOC_2005_I693873.plot b/analyses/pluginCESR/CLEOC_2005_I693873.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEOC_2005_I693873.plot @@ -0,0 +1,24 @@ +BEGIN PLOT /CLEOC_2005_I693873/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.7 +END PLOT +BEGIN PLOT /CLEOC_2005_I693873/d01-x01-y02 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.7 +END PLOT +BEGIN PLOT /CLEOC_2005_I693873/d01-x01-y03 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.7 +END PLOT diff --git a/analyses/pluginCESR/CLEOC_2005_I693873.yoda b/analyses/pluginCESR/CLEOC_2005_I693873.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEOC_2005_I693873.yoda @@ -0,0 +1,27 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2005_I693873/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEOC_2005_I693873/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.67100 0.00000 0.00000 9.00000e+00 2.22036e+00 2.22036e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2005_I693873/d01-x01-y02 +IsRef: 1 +Path: /REF/CLEOC_2005_I693873/d01-x01-y02 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.67100 0.00000 0.00000 5.70000e+00 7.61577e-01 7.61577e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2005_I693873/d01-x01-y03 +IsRef: 1 +Path: /REF/CLEOC_2005_I693873/d01-x01-y03 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.67100 0.00000 0.00000 1.20000e+00 4.12311e-01 4.12311e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEOC_2008_I777917.cc b/analyses/pluginCESR/CLEOC_2008_I777917.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEOC_2008_I777917.cc @@ -0,0 +1,363 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEOC_2008_I777917 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEOC_2008_I777917); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + _c_D0D0 = bookCounter("/TMP/sigma_D0D0"); + _c_DpDm = bookCounter("/TMP/sigma_DpDm"); + _c_DsDs = bookCounter("/TMP/sigma_DsDs"); + _c_D0D0S = bookCounter("/TMP/sigma_D0D0S"); + _c_DpDmS = bookCounter("/TMP/sigma_DpDmS"); + _c_DsDsS = bookCounter("/TMP/sigma_DsDsS"); + _c_D0SD0S = bookCounter("/TMP/sigma_D0SD0S"); + _c_DpSDmS = bookCounter("/TMP/sigma_DpSDmS"); + _c_DsSDsS = bookCounter("/TMP/sigma_DsSDsS"); + _c_DD = bookCounter("/TMP/sigma_DD"); + _c_DDX = bookCounter("/TMP/sigma_DDX"); + _c_DSDpi = bookCounter("/TMP/sigma_DSDpi"); + _c_DSDSpi = bookCounter("/TMP/sigma_DSDSpi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + // total hadronic and muonic cross sections + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + // identified final state with D mesons + const FinalState& ufs = apply(event, "UFS"); + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + bool matched=false; + int sign = p1.pdgId()/id1; + // loop over the other fs particles + for(unsigned int iy=ix+1;iyfill(event.weight()); + map nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2==0) { + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(id1==411 && id2==411) { + _c_DpDm->fill(event.weight()); + _c_DD ->fill(event.weight()); + } + else if(id1==421&& id2==421) { + _c_D0D0->fill(event.weight()); + _c_DD ->fill(event.weight()); + } + else if(id1==431&& id2==431) { + _c_DsDs->fill(event.weight()); + } + else if(id1==413 && id2==413) { + _c_DpSDmS->fill(event.weight()); + } + else if(id1==423&& id2==423) { + _c_D0SD0S->fill(event.weight()); + } + else if(id1==433&& id2==433) { + _c_DsSDsS->fill(event.weight()); + } + else if((id1==421 && id2==423) || + (id1==423 && id2==421)) { + _c_D0D0S->fill(event.weight()); + } + else if((id1==411 && id2==413) || + (id1==413 && id2==411)) { + _c_DpDmS->fill(event.weight()); + } + else if((id1==431 && id2==433) || + (id1==433 && id2==431)) { + _c_DsDsS->fill(event.weight()); + } + } + } + else if(ncount2==1) { + int ipi=0; + if(nRes2[111]==1 && nRes2[211]==0 && nRes[-211]==0 ) + ipi = 111; + else if(nRes2[111]==0 && nRes2[211]==1 && nRes[-211]==0 ) + ipi = 211; + else if(nRes2[111]==0 && nRes2[211]==0 && nRes[-211]==1 ) + ipi =-211; + if(ipi==0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.first==ipi) + continue; + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + bool Ddecay = false; + Particle mother = p1; + while (!mother.parents().empty()) { + mother = mother.parents()[0]; + if(PID::isCharmMeson(mother.pdgId()) && mother.pdgId()!=p1.pdgId()) { + Ddecay = true; + break; + } + } + mother = p2; + while (!mother.parents().empty()) { + mother = mother.parents()[0]; + if(PID::isCharmMeson(mother.pdgId()) && mother.pdgId()!=p1.pdgId()) { + Ddecay = true; + break; + } + } + if(Ddecay) continue; + if((id1==413 || id1==423 ) && + (id2==413 || id2==423 )) { + _c_DSDSpi->fill(event.weight()); + } + else if((id1==411 || id1==421 ) && + (id2==413 || id2==423 )) { + _c_DSDpi->fill(event.weight()); + } + else if((id1==413 || id1==423 ) && + (id2==411 || id2==421 )) { + _c_DSDpi->fill(event.weight()); + } + } + } + } + } + } + + /// Normalise histograms etc., after the run + void finalize() { + // R + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_c = _c_DDX->val()*fact; + double err_c = _c_DDX->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(6, 1, 2)); + Scatter2DPtr charm = bookScatter2D(6,1,1); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(6,1,2); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + charm ->addPoint(x, sig_c, ex, make_pair(err_c,err_c)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + charm ->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + for(unsigned int ix=1;ix<6;++ix) { + unsigned int imax(0); + if (ix<=3) imax = 4; + else imax = 3; + for(unsigned int iy=1;iyval()/picobarn; + error = _c_D0D0->err()/picobarn; + } + else if(iy==2) { + sigma = _c_D0D0S->val()/picobarn; + error = _c_D0D0S->err()/picobarn; + } + else if(iy==3) { + sigma = _c_D0SD0S->val()/picobarn; + error = _c_D0SD0S->err()/picobarn; + } + } + else if(ix==2) { + if(iy==1) { + sigma = _c_DpDm->val()/picobarn; + error = _c_DpDm->err()/picobarn; + } + else if(iy==2) { + sigma = _c_DpDmS->val()/picobarn; + error = _c_DpDmS->err()/picobarn; + } + else if(iy==3) { + sigma = _c_DpSDmS->val()/picobarn; + error = _c_DpSDmS->err()/picobarn; + } + } + else if(ix==3) { + if(iy==1) { + sigma = _c_DsDs->val()/picobarn; + error = _c_DsDs->err()/picobarn; + } + else if(iy==2) { + sigma = _c_DsDsS->val()/picobarn; + error = _c_DsDsS->err()/picobarn; + } + else if(iy==3) { + sigma = _c_DsSDsS->val()/picobarn; + error = _c_DsSDsS->err()/picobarn; + } + } + else if(ix==4) { + if(iy==1) { + sigma = _c_DSDpi->val()/picobarn; + error = _c_DSDpi->err()/picobarn; + } + else if(iy==2) { + sigma = _c_DSDSpi->val()/picobarn; + error = _c_DSDSpi->err()/picobarn; + } + } + else if(ix==5) { + if(iy==1) { + sigma = _c_DD->val()/nanobarn; + error = _c_DD->err()/nanobarn; + } + else if(iy==2) { + sigma = _c_DDX->val()/nanobarn; + error = _c_DDX->err()/nanobarn; + } + } + sigma *= crossSection()/ sumOfWeights(); + error *= crossSection()/ sumOfWeights(); + Scatter2D temphisto(refData(ix, 1, iy)); + Scatter2DPtr mult = bookScatter2D(ix,1,iy); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_D0D0, _c_DpDm,_c_DsDs; + CounterPtr _c_D0D0S, _c_DpDmS,_c_DsDsS; + CounterPtr _c_D0SD0S, _c_DpSDmS,_c_DsSDsS; + CounterPtr _c_DD, _c_DDX; + CounterPtr _c_DSDpi, _c_DSDSpi; + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEOC_2008_I777917); + + +} diff --git a/analyses/pluginCESR/CLEOC_2008_I777917.info b/analyses/pluginCESR/CLEOC_2008_I777917.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEOC_2008_I777917.info @@ -0,0 +1,36 @@ +Name: CLEOC_2008_I777917 +Year: 2008 +Summary: Measurement of charm final-states, the total hadronic cross section and $R$ for energies between 3.92 and 4.26 GeV +Experiment: CLEOC +Collider: CESR +InspireID: 777917 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D80 (2009) 072001, 2009 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of charm final-states, the total hadronic cross section + and $R$ for energies between 3.92 and 4.26 GeV + The muonic cross section is also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: CroninHennessy:2008yi +BibTeX: '@article{CroninHennessy:2008yi, + author = "Cronin-Hennessy, D. and others", + title = "{Measurement of Charm Production Cross Sections in e+e- + Annihilation at Energies between 3.97 and 4.26-GeV}", + collaboration = "CLEO", + journal = "Phys. Rev.", + volume = "D80", + year = "2009", + pages = "072001", + doi = "10.1103/PhysRevD.80.072001", + eprint = "0801.3418", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "CLNS07-2015, CLEO-07-19", + SLACcitation = "%%CITATION = ARXIV:0801.3418;%%" +}' diff --git a/analyses/pluginCESR/CLEOC_2008_I777917.plot b/analyses/pluginCESR/CLEOC_2008_I777917.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEOC_2008_I777917.plot @@ -0,0 +1,138 @@ +BEGIN PLOT /CLEOC_2008_I777917/d06-x01-y01 +Title=$\sigma(e^+e^-\to \text{charm})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \text{charm})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /CLEOC_2008_I777917/d06-x01-y02 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /CLEOC_2008_I777917/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CLEOC_2008_I777917/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /CLEOC_2008_I777917/d01-x01-y01 +Title=$\sigma(e^+e^-\to D^0\bar{D}^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D^0\bar{D}^0)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CLEOC_2008_I777917/d01-x01-y02 +Title=$\sigma(e^+e^-\to D^0\bar{D}^{*0} +\text{c.c})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D^0\bar{D}^{*0} +\text{c.c} )/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CLEOC_2008_I777917/d01-x01-y03 +Title=$\sigma(e^+e^-\to D^{*0}\bar{D}^{*0})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D^{*0}\bar{D}^{*0})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /CLEOC_2008_I777917/d02-x01-y01 +Title=$\sigma(e^+e^-\to D^+D^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D^+D^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CLEOC_2008_I777917/d02-x01-y02 +Title=$\sigma(e^+e^-\to D^+D^{*-} +\text{c.c})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D^+D^{*-} +\text{c.c} )/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CLEOC_2008_I777917/d02-x01-y03 +Title=$\sigma(e^+e^-\to D^{*+}D^{*-})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D^{*-}D^{*+})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /CLEOC_2008_I777917/d03-x01-y01 +Title=$\sigma(e^+e^-\to D_s^+D_s^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D_s^+D_s^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /CLEOC_2008_I777917/d03-x01-y02 +Title=$\sigma(e^+e^-\to D_s^+D_s^{*-} +\text{c.c})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D_s^+D_s^{*-} +\text{c.c} )/pb$ +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /CLEOC_2008_I777917/d03-x01-y03 +Title=$\sigma(e^+e^-\to D_s^{*+}D_s^{*-})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D_s^{*-}D_s^{*+})/pb$ +LogY=0 +ConnectGaps=1 +XMin=3920 +XMax=4260 +END PLOT + + + +BEGIN PLOT /CLEOC_2008_I777917/d04-x01-y01 +Title=$\sigma(e^+e^-\to DD^{*}\pi )$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to DD^{*}\pi)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CLEOC_2008_I777917/d04-x01-y02 +Title=$\sigma(e^+e^-\to D^{*}D^{*}\pi)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D^{*}D^{*}\pi)/pb$ +LogY=0 +ConnectGaps=1 +XMin=3920 +XMax=4260 +END PLOT + + + + +BEGIN PLOT /CLEOC_2008_I777917/d05-x01-y01 +Title=$\sigma(e^+e^-\to D\bar{D})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D\bar{D})/$nb +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /CLEOC_2008_I777917/d05-x01-y02 +Title=$\sigma(e^+e^-\to D\bar{D}+X)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to D\bar{D}+X)/$nb +LogY=0 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginCESR/CLEOC_2008_I777917.yoda b/analyses/pluginCESR/CLEOC_2008_I777917.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEOC_2008_I777917.yoda @@ -0,0 +1,271 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d01-x01-y01 +Title: doi:10.17182/hepdata.47185.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.970000e+03 0.000000e+00 0.000000e+00 8.600000e+01 2.927456e+01 2.927456e+01 +3.990000e+03 0.000000e+00 0.000000e+00 1.330000e+02 4.143670e+01 4.143670e+01 +4.010000e+03 0.000000e+00 0.000000e+00 7.600000e+01 2.517936e+01 2.517936e+01 +4.030000e+03 0.000000e+00 0.000000e+00 3.340000e+02 7.158911e+01 7.158911e+01 +4.060000e+03 0.000000e+00 0.000000e+00 4.100000e+02 7.421590e+01 7.421590e+01 +4.120000e+03 0.000000e+00 0.000000e+00 3.030000e+02 7.138627e+01 7.138627e+01 +4.140000e+03 0.000000e+00 0.000000e+00 1.770000e+02 4.079216e+01 4.079216e+01 +4.160000e+03 0.000000e+00 0.000000e+00 1.670000e+02 2.912044e+01 2.912044e+01 +4.170000e+03 0.000000e+00 0.000000e+00 1.770000e+02 1.063015e+01 1.063015e+01 +4.180000e+03 0.000000e+00 0.000000e+00 1.790000e+02 3.981206e+01 3.981206e+01 +4.200000e+03 0.000000e+00 0.000000e+00 1.800000e+02 5.557877e+01 5.557877e+01 +4.260000e+03 0.000000e+00 0.000000e+00 8.600000e+01 1.843909e+01 1.843909e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d01-x01-y02 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d01-x01-y02 +Title: doi:10.17182/hepdata.47185.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.970000e+03 0.000000e+00 0.000000e+00 2.280000e+03 1.550484e+02 1.550484e+02 +3.990000e+03 0.000000e+00 0.000000e+00 2.740000e+03 1.824774e+02 1.824774e+02 +4.010000e+03 0.000000e+00 0.000000e+00 3.320000e+03 1.137453e+02 1.137453e+02 +4.015000e+03 0.000000e+00 0.000000e+00 3.840000e+03 3.118493e+02 3.118493e+02 +4.030000e+03 0.000000e+00 0.000000e+00 3.200000e+03 2.130023e+02 2.130023e+02 +4.060000e+03 0.000000e+00 0.000000e+00 2.230000e+03 1.654841e+02 1.654841e+02 +4.120000e+03 0.000000e+00 0.000000e+00 1.400000e+03 1.432794e+02 1.432794e+02 +4.140000e+03 0.000000e+00 0.000000e+00 1.350000e+03 1.100727e+02 1.100727e+02 +4.160000e+03 0.000000e+00 0.000000e+00 1.252000e+03 8.130191e+01 8.130191e+01 +4.170000e+03 0.000000e+00 0.000000e+00 1.272000e+03 4.701064e+01 4.701064e+01 +4.180000e+03 0.000000e+00 0.000000e+00 1.211000e+03 1.007224e+02 1.007224e+02 +4.200000e+03 0.000000e+00 0.000000e+00 1.030000e+03 1.278828e+02 1.278828e+02 +4.260000e+03 0.000000e+00 0.000000e+00 1.080000e+03 6.964194e+01 6.964194e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d01-x01-y03 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d01-x01-y03 +Title: doi:10.17182/hepdata.47185.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.015000e+03 0.000000e+00 0.000000e+00 2.130000e+02 7.653104e+01 7.653104e+01 +4.030000e+03 0.000000e+00 0.000000e+00 2.000000e+03 1.564001e+02 1.564001e+02 +4.060000e+03 0.000000e+00 0.000000e+00 2.290000e+03 1.705520e+02 1.705520e+02 +4.120000e+03 0.000000e+00 0.000000e+00 2.550000e+03 1.952332e+02 1.952332e+02 +4.140000e+03 0.000000e+00 0.000000e+00 2.443000e+03 1.633432e+02 1.633432e+02 +4.160000e+03 0.000000e+00 0.000000e+00 2.566000e+03 1.472990e+02 1.472990e+02 +4.170000e+03 0.000000e+00 0.000000e+00 2.363000e+03 1.126144e+02 1.126144e+02 +4.180000e+03 0.000000e+00 0.000000e+00 2.173000e+03 1.456709e+02 1.456709e+02 +4.200000e+03 0.000000e+00 0.000000e+00 1.830000e+03 1.634534e+02 1.634534e+02 +4.260000e+03 0.000000e+00 0.000000e+00 2.690000e+02 4.396590e+01 4.396590e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d02-x01-y01 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d02-x01-y01 +Title: doi:10.17182/hepdata.47185.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.970000e+03 0.000000e+00 0.000000e+00 1.370000e+02 2.668333e+01 2.668333e+01 +3.990000e+03 0.000000e+00 0.000000e+00 9.000000e+01 2.236068e+01 2.236068e+01 +4.010000e+03 0.000000e+00 0.000000e+00 1.350000e+02 2.280351e+01 2.280351e+01 +4.015000e+03 0.000000e+00 0.000000e+00 3.800000e+01 2.009975e+01 2.009975e+01 +4.030000e+03 0.000000e+00 0.000000e+00 1.960000e+02 3.613862e+01 3.613862e+01 +4.060000e+03 0.000000e+00 0.000000e+00 4.800000e+02 5.923681e+01 5.923681e+01 +4.120000e+03 0.000000e+00 0.000000e+00 3.100000e+02 5.192302e+01 5.192302e+01 +4.140000e+03 0.000000e+00 0.000000e+00 2.000000e+02 3.036445e+01 3.036445e+01 +4.160000e+03 0.000000e+00 0.000000e+00 2.000000e+02 2.284732e+01 2.284732e+01 +4.170000e+03 0.000000e+00 0.000000e+00 1.820000e+02 1.000000e+01 1.000000e+01 +4.180000e+03 0.000000e+00 0.000000e+00 1.970000e+02 2.846050e+01 2.846050e+01 +4.200000e+03 0.000000e+00 0.000000e+00 1.810000e+02 3.687818e+01 3.687818e+01 +4.260000e+03 0.000000e+00 0.000000e+00 9.400000e+01 1.360147e+01 1.360147e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d02-x01-y02 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d02-x01-y02 +Title: doi:10.17182/hepdata.47185.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.970000e+03 0.000000e+00 0.000000e+00 2.230000e+03 1.514497e+02 1.514497e+02 +3.990000e+03 0.000000e+00 0.000000e+00 2.750000e+03 1.821318e+02 1.821318e+02 +4.010000e+03 0.000000e+00 0.000000e+00 3.300000e+03 1.731127e+02 1.731127e+02 +4.015000e+03 0.000000e+00 0.000000e+00 3.703000e+03 3.015825e+02 3.015825e+02 +4.030000e+03 0.000000e+00 0.000000e+00 3.300000e+03 2.128497e+02 2.128497e+02 +4.060000e+03 0.000000e+00 0.000000e+00 2.170000e+03 1.610124e+02 1.610124e+02 +4.120000e+03 0.000000e+00 0.000000e+00 1.560000e+03 1.459623e+02 1.459623e+02 +4.140000e+03 0.000000e+00 0.000000e+00 1.376000e+03 1.086876e+02 1.086876e+02 +4.160000e+03 0.000000e+00 0.000000e+00 1.376000e+03 8.348653e+01 8.348653e+01 +4.170000e+03 0.000000e+00 0.000000e+00 1.285000e+03 4.753946e+01 4.753946e+01 +4.180000e+03 0.000000e+00 0.000000e+00 1.296000e+03 9.749359e+01 9.749359e+01 +4.200000e+03 0.000000e+00 0.000000e+00 1.070000e+03 1.214578e+02 1.214578e+02 +4.260000e+03 0.000000e+00 0.000000e+00 1.022000e+03 6.435060e+01 6.435060e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d02-x01-y03 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d02-x01-y03 +Title: doi:10.17182/hepdata.47185.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.030000e+03 0.000000e+00 0.000000e+00 1.400000e+03 1.823623e+02 1.823623e+02 +4.060000e+03 0.000000e+00 0.000000e+00 2.390000e+03 2.486524e+02 2.486524e+02 +4.120000e+03 0.000000e+00 0.000000e+00 2.280000e+03 2.554858e+02 2.554858e+02 +4.140000e+03 0.000000e+00 0.000000e+00 2.556000e+03 2.298173e+02 2.298173e+02 +4.160000e+03 0.000000e+00 0.000000e+00 2.479000e+03 1.786449e+02 1.786449e+02 +4.170000e+03 0.000000e+00 0.000000e+00 2.357000e+03 1.126144e+02 1.126144e+02 +4.180000e+03 0.000000e+00 0.000000e+00 2.145000e+03 1.994618e+02 1.994618e+02 +4.200000e+03 0.000000e+00 0.000000e+00 1.564000e+03 2.273785e+02 2.273785e+02 +4.260000e+03 0.000000e+00 0.000000e+00 2.370000e+02 5.510898e+01 5.510898e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d03-x01-y01 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d03-x01-y01 +Title: doi:10.17182/hepdata.47185.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.970000e+03 0.000000e+00 0.000000e+00 1.020000e+02 2.668333e+01 2.668333e+01 +3.990000e+03 0.000000e+00 0.000000e+00 1.330000e+02 3.178050e+01 3.178050e+01 +4.010000e+03 0.000000e+00 0.000000e+00 2.690000e+02 3.354102e+01 3.354102e+01 +4.015000e+03 0.000000e+00 0.000000e+00 2.500000e+02 6.063827e+01 6.063827e+01 +4.030000e+03 0.000000e+00 0.000000e+00 1.740000e+02 3.736308e+01 3.736308e+01 +4.060000e+03 0.000000e+00 0.000000e+00 5.100000e+01 2.816026e+01 2.816026e+01 +4.120000e+03 0.000000e+00 0.000000e+00 2.600000e+01 2.601922e+01 2.601922e+01 +4.140000e+03 0.000000e+00 0.000000e+00 2.500000e+01 2.002498e+01 2.002498e+01 +4.170000e+03 0.000000e+00 0.000000e+00 3.400000e+01 3.605551e+00 3.605551e+00 +4.180000e+03 0.000000e+00 0.000000e+00 7.000000e+00 1.603122e+01 1.603122e+01 +4.200000e+03 0.000000e+00 0.000000e+00 1.500000e+01 2.202272e+01 2.202272e+01 +4.260000e+03 0.000000e+00 0.000000e+00 4.700000e+01 2.220360e+01 2.220360e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d03-x01-y02 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d03-x01-y02 +Title: doi:10.17182/hepdata.47185.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.120000e+03 0.000000e+00 0.000000e+00 4.780000e+02 6.870953e+01 6.870953e+01 +4.140000e+03 0.000000e+00 0.000000e+00 6.840000e+02 6.911584e+01 6.911584e+01 +4.160000e+03 0.000000e+00 0.000000e+00 9.050000e+02 4.924429e+01 4.924429e+01 +4.170000e+03 0.000000e+00 0.000000e+00 9.160000e+02 5.021952e+01 5.021952e+01 +4.180000e+03 0.000000e+00 0.000000e+00 8.890000e+02 7.543209e+01 7.543209e+01 +4.200000e+03 0.000000e+00 0.000000e+00 8.120000e+02 9.259050e+01 9.259050e+01 +4.260000e+03 0.000000e+00 0.000000e+00 3.400000e+01 9.219544e+00 9.219544e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d03-x01-y03 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d03-x01-y03 +Title: doi:10.17182/hepdata.47185.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.260000e+03 0.000000e+00 0.000000e+00 4.400000e+02 4.036087e+01 4.036087e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d04-x01-y01 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d04-x01-y01 +Title: doi:10.17182/hepdata.47185.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.060000e+03 0.000000e+00 0.000000e+00 1.440000e+02 9.552487e+01 9.552487e+01 +4.120000e+03 0.000000e+00 0.000000e+00 4.500000e+01 8.315047e+01 8.315047e+01 +4.140000e+03 0.000000e+00 0.000000e+00 4.120000e+02 9.984989e+01 9.984989e+01 +4.160000e+03 0.000000e+00 0.000000e+00 3.890000e+02 7.621680e+01 7.621680e+01 +4.170000e+03 0.000000e+00 0.000000e+00 4.400000e+02 5.664804e+01 5.664804e+01 +4.180000e+03 0.000000e+00 0.000000e+00 5.750000e+02 1.150000e+02 1.150000e+02 +4.200000e+03 0.000000e+00 0.000000e+00 7.350000e+02 1.561570e+02 1.561570e+02 +4.260000e+03 0.000000e+00 0.000000e+00 6.380000e+02 1.207394e+02 1.207394e+02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d04-x01-y02 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d04-x01-y02 +Title: doi:10.17182/hepdata.47185.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.260000e+03 0.000000e+00 0.000000e+00 3.220000e+02 1.043504e+02 1.043504e+02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d05-x01-y01 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d05-x01-y01 +Title: doi:10.17182/hepdata.47185.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.970000e+03 0.000000e+00 0.000000e+00 4.830000e+00 2.420744e-01 2.420744e-01 +3.990000e+03 0.000000e+00 0.000000e+00 5.850000e+00 2.983287e-01 2.983287e-01 +4.010000e+03 0.000000e+00 0.000000e+00 7.100000e+00 2.692582e-01 2.692582e-01 +4.015000e+03 0.000000e+00 0.000000e+00 7.940000e+00 4.854894e-01 4.854894e-01 +4.030000e+03 0.000000e+00 0.000000e+00 1.060000e+01 4.341659e-01 4.341659e-01 +4.060000e+03 0.000000e+00 0.000000e+00 1.016000e+01 4.500000e-01 4.500000e-01 +4.120000e+03 0.000000e+00 0.000000e+00 8.950000e+00 4.465423e-01 4.465423e-01 +4.140000e+03 0.000000e+00 0.000000e+00 9.220000e+00 3.894868e-01 3.894868e-01 +4.160000e+03 0.000000e+00 0.000000e+00 9.330000e+00 3.280244e-01 3.280244e-01 +4.170000e+03 0.000000e+00 0.000000e+00 9.030000e+00 2.531798e-01 2.531798e-01 +4.180000e+03 0.000000e+00 0.000000e+00 8.670000e+00 3.612478e-01 3.612478e-01 +4.200000e+03 0.000000e+00 0.000000e+00 7.420000e+00 4.031129e-01 4.031129e-01 +4.260000e+03 0.000000e+00 0.000000e+00 4.270000e+00 2.126029e-01 2.126029e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d05-x01-y02 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d05-x01-y02 +Title: doi:10.17182/hepdata.47185.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.970000e+03 0.000000e+00 0.000000e+00 4.910000e+00 2.408319e-01 2.408319e-01 +3.990000e+03 0.000000e+00 0.000000e+00 5.930000e+00 2.831960e-01 2.831960e-01 +4.010000e+03 0.000000e+00 0.000000e+00 7.050000e+00 2.860070e-01 2.860070e-01 +4.015000e+03 0.000000e+00 0.000000e+00 7.620000e+00 4.220190e-01 4.220190e-01 +4.030000e+03 0.000000e+00 0.000000e+00 1.087000e+01 4.640043e-01 4.640043e-01 +4.060000e+03 0.000000e+00 0.000000e+00 9.980000e+00 4.280187e-01 4.280187e-01 +4.120000e+03 0.000000e+00 0.000000e+00 9.130000e+00 4.177320e-01 4.177320e-01 +4.140000e+03 0.000000e+00 0.000000e+00 9.110000e+00 3.720215e-01 3.720215e-01 +4.160000e+03 0.000000e+00 0.000000e+00 9.100000e+00 3.354102e-01 3.354102e-01 +4.170000e+03 0.000000e+00 0.000000e+00 9.090000e+00 3.080584e-01 3.080584e-01 +4.180000e+03 0.000000e+00 0.000000e+00 8.700000e+00 3.522783e-01 3.522783e-01 +4.200000e+03 0.000000e+00 0.000000e+00 7.450000e+00 3.606938e-01 3.606938e-01 +4.260000e+03 0.000000e+00 0.000000e+00 4.200000e+00 1.720465e-01 1.720465e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d06-x01-y01 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d06-x01-y01 +Title: doi:10.17182/hepdata.47185.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.970000e+03 0.000000e+00 0.000000e+00 4.910000e+00 3.269557e-01 3.269557e-01 +3.990000e+03 0.000000e+00 0.000000e+00 5.870000e+00 3.676955e-01 3.676955e-01 +4.010000e+03 0.000000e+00 0.000000e+00 7.210000e+00 4.176123e-01 4.176123e-01 +4.015000e+03 0.000000e+00 0.000000e+00 7.880000e+00 4.661545e-01 4.661545e-01 +4.030000e+03 0.000000e+00 0.000000e+00 1.130000e+01 6.087693e-01 6.087693e-01 +4.060000e+03 0.000000e+00 0.000000e+00 9.980000e+00 5.481788e-01 5.481788e-01 +4.120000e+03 0.000000e+00 0.000000e+00 9.430000e+00 5.124451e-01 5.124451e-01 +4.140000e+03 0.000000e+00 0.000000e+00 9.580000e+00 5.546170e-01 5.546170e-01 +4.160000e+03 0.000000e+00 0.000000e+00 9.620000e+00 5.281098e-01 5.281098e-01 +4.170000e+03 0.000000e+00 0.000000e+00 9.450000e+00 4.981967e-01 4.981967e-01 +4.180000e+03 0.000000e+00 0.000000e+00 9.070000e+00 4.850773e-01 4.850773e-01 +4.200000e+03 0.000000e+00 0.000000e+00 8.370000e+00 4.522168e-01 4.522168e-01 +4.260000e+03 0.000000e+00 0.000000e+00 4.340000e+00 2.801785e-01 2.801785e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEOC_2008_I777917/d06-x01-y02 +IsRef: 1 +Path: /REF/CLEOC_2008_I777917/d06-x01-y02 +Title: doi:10.17182/hepdata.47185.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.970000e+03 0.000000e+00 0.000000e+00 3.360000e+00 6.403124e-02 6.403124e-02 +3.990000e+03 0.000000e+00 0.000000e+00 3.550000e+00 7.810250e-02 7.810250e-02 +4.010000e+03 0.000000e+00 0.000000e+00 3.880000e+00 8.944272e-02 8.944272e-02 +4.015000e+03 0.000000e+00 0.000000e+00 3.950000e+00 1.131371e-01 1.131371e-01 +4.030000e+03 0.000000e+00 0.000000e+00 4.740000e+00 1.389244e-01 1.389244e-01 +4.060000e+03 0.000000e+00 0.000000e+00 4.340000e+00 1.118034e-01 1.118034e-01 +4.120000e+03 0.000000e+00 0.000000e+00 4.210000e+00 1.166190e-01 1.166190e-01 +4.140000e+03 0.000000e+00 0.000000e+00 4.180000e+00 1.077033e-01 1.077033e-01 +4.160000e+03 0.000000e+00 0.000000e+00 4.180000e+00 1.044031e-01 1.044031e-01 +4.170000e+03 0.000000e+00 0.000000e+00 4.200000e+00 1.004988e-01 1.004988e-01 +4.180000e+03 0.000000e+00 0.000000e+00 4.170000e+00 1.077033e-01 1.077033e-01 +4.200000e+03 0.000000e+00 0.000000e+00 3.770000e+00 9.433981e-02 9.433981e-02 +4.260000e+03 0.000000e+00 0.000000e+00 3.060000e+00 4.472136e-02 4.472136e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEO_1983_I188803.cc b/analyses/pluginCESR/CLEO_1983_I188803.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1983_I188803.cc @@ -0,0 +1,87 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEO_1983_I188803 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEO_1983_I188803); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + vetoEvent; + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(2, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEO_1983_I188803); + + +} diff --git a/analyses/pluginCESR/CLEO_1983_I188803.info b/analyses/pluginCESR/CLEO_1983_I188803.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1983_I188803.info @@ -0,0 +1,33 @@ +Name: CLEO_1983_I188803 +Year: 1983 +Summary: Measurement of hadronic cross section at the $\Upsilon(1S)$, 9.461 GeV +Experiment: CLEO +Collider: CESR +InspireID: 188803 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D57 (1998) 1350-1358, 1998 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of the hadronic cross section in $e^+e^-$ collisions by CLEO at the $\Upsilon(1S)$, 9.461 GeV.' +BibKey: Giles:1983eq +BibTeX: '@article{Giles:1983eq, + author = "Giles, R. and others", + title = "{A Measurement of the Branching Fraction of the Decay + $\Upsilon$ (1s) $\to \tau^+ \tau^-$}", + booktitle = "{11th International Symposium on Lepton and Photon + Interactions at High Energies Ithaca, New York, August + 4-9, 1983}", + collaboration = "CLEO", + journal = "Phys. Rev. Lett.", + volume = "50", + year = "1983", + pages = "877", + doi = "10.1103/PhysRevLett.50.877", + reportNumber = "CLNS-83-556, CLEO-83-02", + SLACcitation = "%%CITATION = PRLTA,50,877;%%" +}' diff --git a/analyses/pluginCESR/CLEO_1983_I188803.plot b/analyses/pluginCESR/CLEO_1983_I188803.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1983_I188803.plot @@ -0,0 +1,9 @@ +BEGIN PLOT /CLEO_1983_I188803/d02-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +XMin=9 +XMax=10 +END PLOT diff --git a/analyses/pluginCESR/CLEO_1983_I188803.yoda b/analyses/pluginCESR/CLEO_1983_I188803.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1983_I188803.yoda @@ -0,0 +1,19 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1983_I188803/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEO_1983_I188803/d01-x01-y01 +Title: doi:10.17182/hepdata.20525.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.460000e+00 0.000000e+00 0.000000e+00 1.628000e+02 7.900000e+00 7.900000e+00 +1.057700e+01 0.000000e+00 0.000000e+00 7.500000e+01 1.600000e+00 1.600000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1983_I188803/d02-x01-y01 +IsRef: 1 +Path: /REF/CLEO_1983_I188803/d02-x01-y01 +Title: doi:10.17182/hepdata.20525.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.460000e+00 0.000000e+00 0.000000e+00 2.160000e+01 1.303840e+00 1.303840e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEO_1983_I188805.cc b/analyses/pluginCESR/CLEO_1983_I188805.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1983_I188805.cc @@ -0,0 +1,86 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEO_1983_I188805 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEO_1983_I188805); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + vetoEvent; + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + // R + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(1,1,1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + } + else { + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEO_1983_I188805); + + +} diff --git a/analyses/pluginCESR/CLEO_1983_I188805.info b/analyses/pluginCESR/CLEO_1983_I188805.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1983_I188805.info @@ -0,0 +1,33 @@ +Name: CLEO_1983_I188805 +Year: 1983 +Summary: Measurement of the hadronic cross section between9.46 and 10.355 GeV +Experiment: CLEO +Collider: CESR +InspireID: 188805 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 50 (1983) 807 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of the hadronic cross section between 9.46 and 10.355 GeV' +BibKey: Andrews:1983es +BibTeX: '@article{Andrews:1983es, + author = "Andrews, D. and others", + title = "{A Measurement of the Leptonic Branching Ratios of the + $\Upsilon$ (1s), $\Upsilon$ (2s), and $\Upsilon$ (3s)}", + booktitle = "{11th International Symposium on Lepton and Photon + Interactions at High Energies Ithaca, New York, August + 4-9, 1983}", + collaboration = "CLEO", + journal = "Phys. Rev. Lett.", + volume = "50", + year = "1983", + pages = "807", + doi = "10.1103/PhysRevLett.50.807", + reportNumber = "CLNS-83-555, CLEO-83-01", + SLACcitation = "%%CITATION = PRLTA,50,807;%%" +}' diff --git a/analyses/pluginCESR/CLEO_1983_I188805.plot b/analyses/pluginCESR/CLEO_1983_I188805.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1983_I188805.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /CLEO_1983_I188805/d01-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/$nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginCESR/CLEO_1983_I188805.yoda b/analyses/pluginCESR/CLEO_1983_I188805.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1983_I188805.yoda @@ -0,0 +1,11 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1983_I188805/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEO_1983_I188805/d01-x01-y01 +Title: doi:10.17182/hepdata.20536.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.460000e+00 0.000000e+00 0.000000e+00 2.150000e+01 8.246211e-01 8.246211e-01 +1.002300e+01 0.000000e+00 0.000000e+00 7.060000e+00 3.023243e-01 3.023243e-01 +1.035500e+01 0.000000e+00 0.000000e+00 4.810000e+00 1.931321e-01 1.931321e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEO_1984_I193577.cc b/analyses/pluginCESR/CLEO_1984_I193577.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1984_I193577.cc @@ -0,0 +1,98 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEO_1984_I193577 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEO_1984_I193577); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEO_1984_I193577); + + +} diff --git a/analyses/pluginCESR/CLEO_1984_I193577.info b/analyses/pluginCESR/CLEO_1984_I193577.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1984_I193577.info @@ -0,0 +1,34 @@ +Name: CLEO_1984_I193577 +Year: 1984 +Summary: Measurement of $R$ for 10.49 GeV +Experiment: CLEO +Collider: CESR +InspireID: 193577 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.D29 (1984) 1285 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by CLEO for 10.49 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Giles:1983vq +BibTeX: '@article{Giles:1983vq, + author = "Giles, R. and others", + title = "{The Total Cross-section for Electron - Positron + Annihilation Into Hadron Final States in the $\Upsilon$ + Energy Region}", + collaboration = "CLEO", + journal = "Phys. Rev.", + volume = "D29", + year = "1984", + pages = "1285", + doi = "10.1103/PhysRevD.29.1285", + reportNumber = "CLNS-83/586, CLEO-83-10", + SLACcitation = "%%CITATION = PHRVA,D29,1285;%%" +}' diff --git a/analyses/pluginCESR/CLEO_1984_I193577.plot b/analyses/pluginCESR/CLEO_1984_I193577.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1984_I193577.plot @@ -0,0 +1,27 @@ +BEGIN PLOT /CLEO_1984_I193577/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +XMin=10. +XMax=11. +END PLOT +BEGIN PLOT /CLEO_1984_I193577/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=10. +XMax=11. +END PLOT +BEGIN PLOT /CLEO_1984_I193577/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +XMin=10. +XMax=11. +END PLOT diff --git a/analyses/pluginCESR/CLEO_1984_I193577.yoda b/analyses/pluginCESR/CLEO_1984_I193577.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1984_I193577.yoda @@ -0,0 +1,9 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1984_I193577/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEO_1984_I193577/d01-x01-y01 +Title: doi:10.17182/hepdata.23768.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.049000e+01 0.000000e+00 0.000000e+00 3.770000e+00 3.429446e-01 3.429446e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEO_1991_I29927.cc b/analyses/pluginCESR/CLEO_1991_I29927.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1991_I29927.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/FastJets.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEO_1991_I29927 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEO_1991_I29927); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(), "UFS"); + + // Book histograms + _c_B = bookCounter("/TMP/sigma_B"); + _c_Bstar = bookCounter("/TMP/sigma_Bstar"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& ufs = apply(event, "UFS"); + unsigned int nBstar(0); + // Get Bottom hadrons + const Particles bhads = filter_select(ufs.particles(), isBottomHadron); + // find the Bstars + foreach (const Particle& p, bhads) { + if(abs(p.pdgId())==513 || abs(p.pdgId())==523) { + if(!p.hasDescendantWith(Cuts::pid == p.pdgId())) ++nBstar; + } + } + if(!bhads.empty()) + _c_B->fill(event.weight()); + if(nBstar!=0) + _c_Bstar->fill(nBstar*event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /picobarn; + for(unsigned int ix=1;ix<3;++ix) { + double sig(0.),err(0.); + if(ix==1) { + sig = _c_B->val()*fact; + err = _c_B->err()*fact; + } + else { + sig = _c_Bstar->val()*fact; + err = _c_Bstar->err()*fact; + } + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sig, ex, make_pair(err,err)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_B, _c_Bstar; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEO_1991_I29927); + + +} diff --git a/analyses/pluginCESR/CLEO_1991_I29927.info b/analyses/pluginCESR/CLEO_1991_I29927.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1991_I29927.info @@ -0,0 +1,32 @@ +Name: CLEO_1991_I29927 +Year: 1991 +Summary: Inclusive $B^*$ cross-section above the $\Upsilon(4S)$ +Experiment: CLEO +Collider: CESR +InspireID: 29927 +Status: VALIDATED NOTREENTRY HEPDATA SINGLEWEIGHT +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 67 (1991) 1692-1695 +RunInfo: e+e- collisions +NeedCrossSection: yes +Beams: [e-, e+] +Energies: [10.58,10.61,10.62,10.63,10.64,10.65,10.7] +Description: + 'Measurement of the inclusive cross section for $B^*$ production at energies above the $\Upsilon(4S)$ mass.' +Keywords: [] +BibKey: Akerib:1991eq +BibTeX: '@article{Akerib:1991eq, + author = "Akerib, D. S. and others", + title = "{Measurement of the inclusive B* cross-section above the + Upsilon (4S)}", + collaboration = "CLEO-II", + journal = "Phys. Rev. Lett.", + volume = "67", + year = "1991", + pages = "1692-1695", + doi = "10.1103/PhysRevLett.67.1692", + reportNumber = "CLNS-91-1089, CLEO-91-5", + SLACcitation = "%%CITATION = PRLTA,67,1692;%%" +}' diff --git a/analyses/pluginCESR/CLEO_1991_I29927.plot b/analyses/pluginCESR/CLEO_1991_I29927.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1991_I29927.plot @@ -0,0 +1,19 @@ +BEGIN PLOT /CLEO_1991_I29927/d01-x01-y01 +Title=Cross Section for $b\bar{b}$ +XLabel=$\sqrt{s}$ [GeV] +YLabel=$\sigma_B$ [pb] +XMajorTickMarks=10 +XMin=10.57 +XMax=10.71 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CLEO_1991_I29927/d02-x01-y01 +Title=Cross Section for $B^*$ production +XLabel=$\sqrt{s}$ [GeV] +YLabel=$\sigma_B$ [pb] +XMajorTickMarks=10 +XMin=10.57 +XMax=10.71 +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginCESR/CLEO_1991_I29927.yoda b/analyses/pluginCESR/CLEO_1991_I29927.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1991_I29927.yoda @@ -0,0 +1,36 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1991_I29927/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {1: {stat: {dn: -13.0, up: 13.0}, sys: {dn: -46.0, up: 46.0}}, 2: {stat: {dn: -12.0, up: 12.0}, sys: {dn: -9.0, up: 9.0}}, 3: {stat: {dn: -12.0, up: 12.0}, sys: {dn: -15.0, up: 15.0}}, 4: {stat: {dn: -13.0, up: 13.0}, sys: {dn: -18.0, up: 18.0}}, 5: {stat: {dn: -11.0, up: 11.0}, sys: {dn: -21.0, up: 21.0}}, 6: {stat: {dn: -17.0, up: 17.0}, sys: {dn: -28.0, up: 28.0}}} + +IsRef: 1 +Path: /REF/CLEO_1991_I29927/d01-x01-y01 +Title: doi:10.17182/hepdata.19887.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 1.150000e+03 0.000000e+00 0.000000e+00 +1.061000e+01 0.000000e+00 0.000000e+00 2.150000e+02 4.780167e+01 4.780167e+01 +1.062000e+01 0.000000e+00 0.000000e+00 2.430000e+02 1.500000e+01 1.500000e+01 +1.063000e+01 0.000000e+00 0.000000e+00 2.430000e+02 1.920937e+01 1.920937e+01 +1.064000e+01 0.000000e+00 0.000000e+00 2.180000e+02 2.220360e+01 2.220360e+01 +1.065000e+01 0.000000e+00 0.000000e+00 1.560000e+02 2.370654e+01 2.370654e+01 +1.070000e+01 0.000000e+00 0.000000e+00 2.260000e+02 3.275668e+01 3.275668e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1991_I29927/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -15.0, up: 15.0}, sys: {dn: -10.0, up: 10.0}}, 1: {stat: {dn: -18.0, up: 18.0}, sys: {dn: -17.0, up: 17.0}}, 2: {stat: {dn: -20.0, up: 20.0}, sys: {dn: -30.0, up: 30.0}}, 3: {stat: {dn: -23.0, up: 23.0}, sys: {dn: -22.0, up: 22.0}}, 4: {stat: {dn: -21.0, up: 21.0}, sys: {dn: -21.0, up: 21.0}}, 5: {stat: {dn: -18.0, up: 18.0}, sys: {dn: -17.0, up: 17.0}}, 6: {stat: {dn: -34.0, up: 34.0}, sys: {dn: -46.0, up: 46.0}}} + +IsRef: 1 +Path: /REF/CLEO_1991_I29927/d02-x01-y01 +Title: doi:10.17182/hepdata.19887.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 0.000000e+00 0.000000e+00 -1.500000e+01 1.802776e+01 1.802776e+01 +1.061000e+01 0.000000e+00 0.000000e+00 5.800000e+01 2.475884e+01 2.475884e+01 +1.062000e+01 0.000000e+00 0.000000e+00 1.510000e+02 3.605551e+01 3.605551e+01 +1.063000e+01 0.000000e+00 0.000000e+00 1.640000e+02 3.182766e+01 3.182766e+01 +1.064000e+01 0.000000e+00 0.000000e+00 1.210000e+02 2.969848e+01 2.969848e+01 +1.065000e+01 0.000000e+00 0.000000e+00 1.510000e+02 2.475884e+01 2.475884e+01 +1.070000e+01 0.000000e+00 0.000000e+00 3.460000e+02 5.720140e+01 5.720140e+01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEO_1998_I445351.cc b/analyses/pluginCESR/CLEO_1998_I445351.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1998_I445351.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEO_1998_I445351 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEO_1998_I445351); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEO_1998_I445351); + + +} diff --git a/analyses/pluginCESR/CLEO_1998_I445351.info b/analyses/pluginCESR/CLEO_1998_I445351.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1998_I445351.info @@ -0,0 +1,35 @@ +Name: CLEO_1998_I445351 +Year: 1998 +Summary: Measurement of $R$ at 10.52 GeV +Experiment: CLEO +Collider: CESR +InspireID: 445351 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D57 (1998) 1350-1358, 1998 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by CLEO for 10.52 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Ammar:1997sk +BibTeX: '@article{Ammar:1997sk, + author = "Ammar, R. and others", + title = "{A Measurement of the total cross-section for e+ e- ---> + hadrons at s**(1/2) = 10.52-GeV}", + collaboration = "CLEO", + journal = "Phys. Rev.", + volume = "D57", + year = "1998", + pages = "1350-1358", + doi = "10.1103/PhysRevD.57.1350", + eprint = "hep-ex/9707018", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-PUB-9765, CLNS-97-1493, CLEO-97-14", + SLACcitation = "%%CITATION = HEP-EX/9707018;%%" +}' diff --git a/analyses/pluginCESR/CLEO_1998_I445351.plot b/analyses/pluginCESR/CLEO_1998_I445351.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1998_I445351.plot @@ -0,0 +1,27 @@ +BEGIN PLOT /CLEO_1998_I445351/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +XMin=10 +XMax=11 +END PLOT +BEGIN PLOT /CLEO_1998_I445351/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=10 +XMax=11 +END PLOT +BEGIN PLOT /CLEO_1998_I445351/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +XMin=10 +XMax=11 +END PLOT \ No newline at end of file diff --git a/analyses/pluginCESR/CLEO_1998_I445351.yoda b/analyses/pluginCESR/CLEO_1998_I445351.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1998_I445351.yoda @@ -0,0 +1,19 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1998_I445351/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEO_1998_I445351/d01-x01-y01 +Title: doi:10.17182/hepdata.47132.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.052000e+01 0.000000e+00 0.000000e+00 3.560000e+00 7.071068e-02 7.071068e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1998_I445351/d02-x01-y01 +IsRef: 1 +Path: /REF/CLEO_1998_I445351/d02-x01-y01 +Title: doi:10.17182/hepdata.47132.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.052000e+01 0.000000e+00 0.000000e+00 2.000000e-01 6.082763e-02 6.082763e-02 +9.120000e+01 0.000000e+00 0.000000e+00 1.300000e-01 3.041381e-02 3.041381e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEO_1999_I474676.cc b/analyses/pluginCESR/CLEO_1999_I474676.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1999_I474676.cc @@ -0,0 +1,124 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEO_1999_I474676 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEO_1999_I474676); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nUps2pipi = bookCounter("TMP/nUps2pipi"); + _nUps3pipi = bookCounter("TMP/nUps3pipi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId() != 100553 && + p.pdgId() != 200553 ) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(p.pdgId()==100553) + _nUps2pipi->fill(event.weight()); + if(p.pdgId()==200553) + _nUps3pipi->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /picobarn; + for(unsigned int ix=1;ix<3;++ix) { + double sigma,error; + if(ix==1) { + sigma = _nUps3pipi->val()*fact; + error = _nUps3pipi->err()*fact; + } + else if(ix==2) { + sigma = _nUps2pipi->val()*fact; + error = _nUps2pipi->err()*fact; + } + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + //@} + + /// @name Histograms + //@{ + CounterPtr _nUps2pipi,_nUps3pipi; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEO_1999_I474676); + + +} diff --git a/analyses/pluginCESR/CLEO_1999_I474676.info b/analyses/pluginCESR/CLEO_1999_I474676.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1999_I474676.info @@ -0,0 +1,35 @@ +Name: CLEO_1999_I474676 +Year: 1999 +Summary: Cross Section for $e^+e^-\to\Upsilon(2,3S)\pi^+\pi^-$ at 10.52, 10.58 GeV +Experiment: CLEO +Collider: CESR +InspireID: 474676 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D59 (1999) 052003, 1999 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\Upsilon(2,3S)\pi^+\pi^-$ at 10.52 and 10.58 by CLEO.' +Keywords: [] +BibKey: Glenn:1998bd +BibTeX: '@article{Glenn:1998bd, + author = "Glenn, S. and others", + title = "{Upsilon dipion transitions at energies near the + upsilon(4S)}", + collaboration = "CLEO", + journal = "Phys. Rev.", + volume = "D59", + year = "1999", + pages = "052003", + doi = "10.1103/PhysRevD.59.052003", + eprint = "hep-ex/9808008", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-REPRINT-1998-097, CLNS-98-1576, CLEO-98-12", + SLACcitation = "%%CITATION = HEP-EX/9808008;%%" +}' diff --git a/analyses/pluginCESR/CLEO_1999_I474676.plot b/analyses/pluginCESR/CLEO_1999_I474676.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1999_I474676.plot @@ -0,0 +1,16 @@ +BEGIN PLOT /CLEO_1999_I474676/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\Upsilon(3S))$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\Upsilon(3S))$/pb +ConnectGaps=1 +XMin=10. +XMax=11. +END PLOT +BEGIN PLOT /CLEO_1999_I474676/d01-x01-y02 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\Upsilon(2S))$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\Upsilon(2S))$/pb +ConnectGaps=1 +XMin=10. +XMax=11. +END PLOT \ No newline at end of file diff --git a/analyses/pluginCESR/CLEO_1999_I474676.yoda b/analyses/pluginCESR/CLEO_1999_I474676.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1999_I474676.yoda @@ -0,0 +1,20 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1999_I474676/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEO_1999_I474676/d01-x01-y01 +Title: doi:10.17182/hepdata.47202.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.052000e+01 0.000000e+00 0.000000e+00 2.730000e+01 5.590170e+00 5.590170e+00 +1.058000e+01 0.000000e+00 0.000000e+00 1.750000e+01 3.400000e+00 3.400000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1999_I474676/d01-x01-y02 +IsRef: 1 +Path: /REF/CLEO_1999_I474676/d01-x01-y02 +Title: doi:10.17182/hepdata.47202.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.052000e+01 0.000000e+00 0.000000e+00 1.630000e+01 2.220360e+00 2.220360e+00 +1.058000e+01 0.000000e+00 0.000000e+00 1.550000e+01 1.838478e+00 1.838478e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEO_1999_I508944.cc b/analyses/pluginCESR/CLEO_1999_I508944.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1999_I508944.cc @@ -0,0 +1,101 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEO_1999_I508944 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEO_1999_I508944); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(UnstableParticles(), "UFS"); + _hist_pipi = bookHisto1D( 1, 1, 1); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + // Find the taus + Particles taus; + const UnstableParticles& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if (p.abspid() != PID::TAU) continue; + Particles pip, pim, pi0; + unsigned int nstable = 0; + // get the boost to the rest frame + // find the decay products we want + findDecayProducts(p, nstable, pip, pim, pi0); + if (p.pid() < 0) { + swap(pip, pim); + } + if (nstable != 3) continue; + // pipi + if (pim.size() == 1 && pi0.size() == 1) + _hist_pipi->fill((pi0[0].momentum()+pim[0].momentum()).mass(),event.weight()); + } + } + + void findDecayProducts(const Particle & mother, + unsigned int & nstable, + Particles& pip, Particles& pim, + Particles& pi0) { + for(const Particle & p : mother.children()) { + long id = p.pdgId(); + if (id == PID::PI0 ) { + pi0.push_back(p); + ++nstable; + } + else if (id == PID::PIPLUS) { + pip.push_back(p); + ++nstable; + } + else if (id == PID::PIMINUS) { + pim.push_back(p); + ++nstable; + } + else if (id == PID::K0S || id == PID::KPLUS || + id == PID::KMINUS) { + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p, nstable, pip, pim, pi0); + } + else + ++nstable; + } + } + + /// Normalise histograms etc., after the run + void finalize() { + + normalize(_hist_pipi); + + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _hist_pipi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEO_1999_I508944); + + +} diff --git a/analyses/pluginCESR/CLEO_1999_I508944.info b/analyses/pluginCESR/CLEO_1999_I508944.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1999_I508944.info @@ -0,0 +1,35 @@ +Name: CLEO_1999_I508944 +Year: 1999 +Summary: Measurement of Semi-Leptonic Tau Decays into $\pi^\pm\pi^0$ +Experiment: CLEO +Collider: CESR +InspireID: 508944 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D61 (2000) 112002 + - hep-ex/9910046 +RunInfo: + Tau production, can be any process but original data was in + $e^+ e^-$ at the $\Upsilon(4S)$ resonance +Description: + 'Measurement of the invariant mass spectrum of the $\pi^-\pi^0$ system in $\tau\to\pi^-\pi^0\nu_\tau$ measured by CLEO at CESR.' +Keywords: [] +BibKey: Anderson:1999ui +BibTeX: '@article{Anderson:1999ui, + author = "Anderson, S. and others", + title = "{Hadronic structure in the decay tau- ---> pi- pi0 + neutrino(tau)}", + collaboration = "CLEO", + journal = "Phys. Rev.", + volume = "D61", + year = "2000", + pages = "112002", + doi = "10.1103/PhysRevD.61.112002", + eprint = "hep-ex/9910046", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "SLAC-REPRINT-1999-116, CLNS-99-1635, CLEO-99-13", + SLACcitation = "%%CITATION = HEP-EX/9910046;%%" +}' diff --git a/analyses/pluginCESR/CLEO_1999_I508944.plot b/analyses/pluginCESR/CLEO_1999_I508944.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1999_I508944.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /CLEO_1999_I508944/d01-x01-y01 +Title=$\pi^-\pi^0$ mass in $\tau^-\to\pi^-\pi^0\nu_\tau$ decays +XLabel=$m_{\pi^-\pi^0}$ [$\text{GeV}$] +YLabel=$1/\Gamma\text{d}\Gamma/\text{d}m_{\pi^-\pi^0}$ [ $\text{GeV}^{-1}$] +LogY=1 +END PLOT diff --git a/analyses/pluginCESR/CLEO_1999_I508944.yoda b/analyses/pluginCESR/CLEO_1999_I508944.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_1999_I508944.yoda @@ -0,0 +1,51 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_1999_I508944/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEO_1999_I508944/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.28750 0.01250 0.01250 6.00000e-03 5.60000e-03 5.60000e-03 +0.31250 0.01250 0.01250 3.20000e-02 1.00000e-02 1.00000e-02 +0.33750 0.01250 0.01250 2.40000e-02 1.04000e-02 1.04000e-02 +0.36250 0.01250 0.01250 3.40000e-02 9.20000e-03 9.20000e-03 +0.38750 0.01250 0.01250 6.24000e-02 1.04000e-02 1.04000e-02 +0.41250 0.01250 0.01250 6.48000e-02 1.16000e-02 1.16000e-02 +0.43750 0.01250 0.01250 9.96000e-02 1.24000e-02 1.24000e-02 +0.46250 0.01250 0.01250 1.65600e-01 1.36000e-02 1.36000e-02 +0.48750 0.01250 0.01250 2.02400e-01 1.48000e-02 1.48000e-02 +0.51250 0.01250 0.01250 2.43600e-01 1.60000e-02 1.60000e-02 +0.53750 0.01250 0.01250 3.19200e-01 1.76000e-02 1.76000e-02 +0.56250 0.01250 0.01250 4.29600e-01 1.88000e-02 1.88000e-02 +0.58750 0.01250 0.01250 5.77200e-01 2.08000e-02 2.08000e-02 +0.61250 0.01250 0.01250 8.18000e-01 2.36000e-02 2.36000e-02 +0.63750 0.01250 0.01250 1.07640e+00 2.60000e-02 2.60000e-02 +0.66250 0.01250 0.01250 1.54320e+00 3.00000e-02 3.00000e-02 +0.68750 0.01250 0.01250 2.28600e+00 3.48000e-02 3.48000e-02 +0.71250 0.01250 0.01250 3.30720e+00 4.04000e-02 4.04000e-02 +0.73750 0.01250 0.01250 4.31360e+00 4.52000e-02 4.52000e-02 +0.76250 0.01250 0.01250 4.91240e+00 4.72000e-02 4.72000e-02 +0.78750 0.01250 0.01250 4.45880e+00 4.40000e-02 4.40000e-02 +0.81250 0.01250 0.01250 3.51240e+00 3.84000e-02 3.84000e-02 +0.83750 0.01250 0.01250 2.51720e+00 3.16000e-02 3.16000e-02 +0.86250 0.01250 0.01250 1.78680e+00 2.64000e-02 2.64000e-02 +0.88750 0.01250 0.01250 1.30480e+00 2.20000e-02 2.20000e-02 +0.91250 0.01250 0.01250 1.04840e+00 1.96000e-02 1.96000e-02 +0.93750 0.01250 0.01250 8.29200e-01 1.72000e-02 1.72000e-02 +0.96250 0.01250 0.01250 6.35200e-01 1.48000e-02 1.48000e-02 +0.98750 0.01250 0.01250 5.18400e-01 1.36000e-02 1.36000e-02 +1.02500 0.02500 0.02500 4.05600e-01 9.60000e-03 9.60000e-03 +1.07500 0.02500 0.02500 3.02000e-01 8.20000e-03 8.20000e-03 +1.12500 0.02500 0.02500 2.22000e-01 6.80000e-03 6.80000e-03 +1.17500 0.02500 0.02500 1.74000e-01 6.00000e-03 6.00000e-03 +1.22500 0.02500 0.02500 1.27800e-01 5.00000e-03 5.00000e-03 +1.27500 0.02500 0.02500 8.54000e-02 4.00000e-03 4.00000e-03 +1.32500 0.02500 0.02500 5.84000e-02 3.40000e-03 3.40000e-03 +1.37500 0.02500 0.02500 3.62000e-02 2.60000e-03 2.60000e-03 +1.42500 0.02500 0.02500 1.39600e-02 1.68000e-03 1.68000e-03 +1.47500 0.02500 0.02500 5.82000e-03 1.18000e-03 1.18000e-03 +1.52500 0.02500 0.02500 1.42000e-03 6.40000e-04 6.40000e-04 +1.57500 0.02500 0.02500 1.18000e-03 5.00000e-04 5.00000e-04 +1.62500 0.02500 0.02500 1.36000e-03 5.20000e-04 5.20000e-04 +1.67500 0.02500 0.02500 5.60000e-04 4.20000e-04 4.20000e-04 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/CLEO_2004_S5809304.cc b/analyses/pluginCESR/CLEO_2004_S5809304.cc rename from analyses/pluginMisc/CLEO_2004_S5809304.cc rename to analyses/pluginCESR/CLEO_2004_S5809304.cc diff --git a/analyses/pluginMisc/CLEO_2004_S5809304.info b/analyses/pluginCESR/CLEO_2004_S5809304.info rename from analyses/pluginMisc/CLEO_2004_S5809304.info rename to analyses/pluginCESR/CLEO_2004_S5809304.info diff --git a/analyses/pluginMisc/CLEO_2004_S5809304.plot b/analyses/pluginCESR/CLEO_2004_S5809304.plot rename from analyses/pluginMisc/CLEO_2004_S5809304.plot rename to analyses/pluginCESR/CLEO_2004_S5809304.plot diff --git a/analyses/pluginMisc/CLEO_2004_S5809304.yoda b/analyses/pluginCESR/CLEO_2004_S5809304.yoda rename from analyses/pluginMisc/CLEO_2004_S5809304.yoda rename to analyses/pluginCESR/CLEO_2004_S5809304.yoda diff --git a/analyses/pluginCESR/CLEO_2006_I691720.cc b/analyses/pluginCESR/CLEO_2006_I691720.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2006_I691720.cc @@ -0,0 +1,223 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FastJets.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEO_2006_I691720 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEO_2006_I691720); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + // Book histograms + for(unsigned int ix=1;ix<18;++ix) { + stringstream ss; + ss << "TMP/n" << ix; + _nMeson[ix]= bookCounter(ss.str()); + } + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==3) { + if(nCount[211]==1 && nCount[-211]==1 && nCount[111]==1) + _nMeson[1]->fill(event.weight()); + } + const FinalState& ufs = apply(event, "UFS"); + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + if(p1.pdgId()==113 || p1.pdgId()==223 || p1.pdgId()==10113) { + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==111 && val.second!=1) { + matched = false; + break; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(p1.pdgId()==113) { + _nMeson[2]->fill(event.weight()); + _nMeson[3]->fill(event.weight()); + } + else if(p1.pdgId()==223) { + _nMeson[5]->fill(event.weight()); + } + else if(p1.pdgId()==10113) { + _nMeson[15]->fill(event.weight()); + } + } + } + else if(p1.pdgId()==abs(113) || abs(p1.pdgId())==10113) { + if(ncount!=1) continue; + bool matched = true; + int ipi = p1.pdgId()>0 ? -211 : 211; + for(auto const & val : nRes) { + if(abs(val.first)==ipi && val.second!=1) { + matched = false; + break; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + if(p1.pdgId()==abs(113)) { + _nMeson[2]->fill(event.weight()); + _nMeson[4]->fill(event.weight()); + } + else { + _nMeson[15]->fill(event.weight()); + _nMeson[17]->fill(event.weight()); + } + } + } + else if(p1.pdgId()==abs(323)) { + if(ncount!=1) continue; + bool matched = true; + int iK = p1.pdgId()==323 ? -321 : 321; + for(auto const & val : nRes) { + if(abs(val.first)==iK && val.second!=1) { + matched = false; + break; + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nMeson[14]->fill(event.weight()); + } + } + // second unstable particle + if(abs(p1.pdgId())!=313 && p1.pdgId()!=113 && p1.pdgId()!=223 && + p1.pdgId()!=333 && p1.pdgId()!=221 && p1.pdgId()!=331) + continue; + for(unsigned int iy=ix+1;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount!=0) continue; + bool matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(!matched) continue; + if( (p1.pdgId()==113 && p2.pdgId()==221) || + (p2.pdgId()==113 && p1.pdgId()==221) ) + _nMeson[7]->fill(event.weight()); + else if( (p1.pdgId()==223 && p2.pdgId()==221) || + (p2.pdgId()==223 && p1.pdgId()==221) ) + _nMeson[8]->fill(event.weight()); + else if( (p1.pdgId()==333 && p2.pdgId()==221) || + (p2.pdgId()==333 && p1.pdgId()==221) ) + _nMeson[9]->fill(event.weight()); + else if( (p1.pdgId()==113 && p2.pdgId()==331) || + (p2.pdgId()==113 && p1.pdgId()==331) ) + _nMeson[10]->fill(event.weight()); + else if( (p1.pdgId()==223 && p2.pdgId()==331) || + (p2.pdgId()==223 && p1.pdgId()==331) ) + _nMeson[11]->fill(event.weight()); + else if( (p1.pdgId()==333 && p2.pdgId()==331) || + (p2.pdgId()==333 && p1.pdgId()==331) ) + _nMeson[12]->fill(event.weight()); + else if( (p1.pdgId()==313 && p2.pdgId()==-313) || + (p2.pdgId()==313 && p1.pdgId()==-313) ) + _nMeson[13]->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<18;++ix) { + if(ix==6||ix==16) continue; + double sigma = _nMeson[ix]->val(); + double error = _nMeson[ix]->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nMeson[18]; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEO_2006_I691720); + + +} diff --git a/analyses/pluginCESR/CLEO_2006_I691720.info b/analyses/pluginCESR/CLEO_2006_I691720.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2006_I691720.info @@ -0,0 +1,36 @@ +Name: CLEO_2006_I691720 +Year: 2006 +Summary: Cross section for light hadron production at 3.671 and 3.773 GeV +Experiment: CLEO +Collider: CESR +InspireID: 691720 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D73 (2006) 012002, 2006 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to \pi^+\pi^-\pi^0$, $\rho^0\pi^0$, $\rho^\pm\pi^\mp$, + $\omega\pi^0$, $\rho^0\eta$, $\omega\eta$, $\phi\eta$, $\rho^0\eta^\prime$, + $\omega\eta^\prime$, $\phi\eta^\prime$, $K^{*0}\bar{K}^{*0}$, + $K^{*\pm} K^\mp$, $b_1^0\pi^0$, $b_1^\pm\pi^\mp$ at 3.671 and 3.773 GeV' +Keywords: [] +BibKey: Adams:2005ks +BibTeX: '@article{Adams:2005ks, + author = "Adams, G. S. and others", + title = "{Decay of the psi(3770) to light hadrons}", + collaboration = "CLEO", + journal = "Phys. Rev.", + volume = "D73", + year = "2006", + pages = "012002", + doi = "10.1103/PhysRevD.73.012002", + eprint = "hep-ex/0509011", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "CLNS-05-1933, CLEO-05-21", + SLACcitation = "%%CITATION = HEP-EX/0509011;%%" +}' diff --git a/analyses/pluginCESR/CLEO_2006_I691720.plot b/analyses/pluginCESR/CLEO_2006_I691720.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2006_I691720.plot @@ -0,0 +1,120 @@ +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y02 +Title=$\sigma(e^+e^-\to \rho^0\pi^0,\rho^\pm\pi^\mp)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \rho^0\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y03 +Title=$\sigma(e^+e^-\to \rho^0\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \rho^0\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y04 +Title=$\sigma(e^+e^-\to \rho^\pm\pi^\mp)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \rho^\pm\pi^\mp)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y05 +Title=$\sigma(e^+e^-\to \omega\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y07 +Title=$\sigma(e^+e^-\to \rho^0\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \rho^0\eta)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y08 +Title=$\sigma(e^+e^-\to \omega\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega\eta)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y09 +Title=$\sigma(e^+e^-\to \phi\eta)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\eta)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y10 +Title=$\sigma(e^+e^-\to \rho^0\eta^\prime)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \rho^0\eta^\prime)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y11 +Title=$\sigma(e^+e^-\to \omega\eta^\prime)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega\eta^\prime)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y12 +Title=$\sigma(e^+e^-\to \phi\eta^\prime)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \phi\eta^\prime)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y13 +Title=$\sigma(e^+e^-\to K^{*0}\bar{K}^{*0})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^{*0}\bar{K}^{*0})$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y14 +Title=$\sigma(e^+e^-\to K^{*\pm} K^\mp)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^{*\pm} K^\mp)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y15 +Title=$\sigma(e^+e^-\to b_1^0\pi^0, b_1^\pm\pi^\mp)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to )$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT +BEGIN PLOT /CLEO_2006_I691720/d01-x01-y17 +Title=$\sigma(e^+e^-\to b_1^\pm\pi^\mp)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to b_1^\pm\pi^\mp)$/pb +ConnectGaps=1 +XMin=3.6 +XMax=3.8 +END PLOT diff --git a/analyses/pluginCESR/CLEO_2006_I691720.yoda b/analyses/pluginCESR/CLEO_2006_I691720.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2006_I691720.yoda @@ -0,0 +1,163 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y01 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 1.310000e+01 2.701851e+00 2.831960e+00 +3.773000e+00 0.000000e+00 0.000000e+00 7.400000e+00 1.264911e+00 1.264911e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y02 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y02 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 8.000000e+00 1.664332e+00 1.923538e+00 +3.773000e+00 0.000000e+00 0.000000e+00 4.400000e+00 5.830952e-01 5.830952e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y03 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y03 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 3.100000e+00 8.944272e-01 1.077033e+00 +3.773000e+00 0.000000e+00 0.000000e+00 1.300000e+00 2.828427e-01 2.828427e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y04 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y04 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 4.800000e+00 1.300000e+00 1.581139e+00 +3.773000e+00 0.000000e+00 0.000000e+00 3.200000e+00 4.242641e-01 4.242641e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y05 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y05 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 1.520000e+01 2.830194e+00 3.176476e+00 +3.773000e+00 0.000000e+00 0.000000e+00 1.460000e+01 1.615549e+00 1.615549e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y06 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y06 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y07 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y07 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 1.000000e+01 2.147091e+00 2.416609e+00 +3.773000e+00 0.000000e+00 0.000000e+00 1.030000e+01 1.118034e+00 1.118034e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y08 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y08 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 2.300000e+00 1.118034e+00 1.868154e+00 +3.773000e+00 0.000000e+00 0.000000e+00 4.000000e-01 2.236068e-01 2.236068e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y09 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y09 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 2.100000e+00 1.216553e+00 1.910497e+00 +3.773000e+00 0.000000e+00 0.000000e+00 4.500000e+00 7.071068e-01 7.071068e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y10 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y10 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 2.100000e+00 1.612452e+00 4.704253e+00 +3.773000e+00 0.000000e+00 0.000000e+00 3.800000e+00 8.944272e-01 9.848858e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y11 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y11 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.773000e+00 0.000000e+00 0.000000e+00 6.000000e-01 6.708204e-01 1.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y12 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y12 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.773000e+00 0.000000e+00 0.000000e+00 2.500000e+00 1.170470e+00 1.552417e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y13 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y13 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 2.350000e+01 4.981967e+00 5.547071e+00 +3.773000e+00 0.000000e+00 0.000000e+00 2.350000e+01 3.289377e+00 3.289377e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y14 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y14 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 1.000000e+00 8.602325e-01 1.208305e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y15 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y15 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 7.900000e+00 3.080584e+00 3.584690e+00 +3.773000e+00 0.000000e+00 0.000000e+00 6.300000e+00 1.655295e+00 1.655295e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y16 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y16 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I691720/d01-x01-y17 +IsRef: 1 +Path: /REF/CLEO_2006_I691720/d01-x01-y17 +Title: doi:10.17182/hepdata.52474.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.671000e+00 0.000000e+00 0.000000e+00 4.200000e+00 1.341641e+00 1.708801e+00 +3.773000e+00 0.000000e+00 0.000000e+00 4.700000e+00 7.211103e-01 7.211103e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEO_2006_I700665.cc b/analyses/pluginCESR/CLEO_2006_I700665.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2006_I700665.cc @@ -0,0 +1,87 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEO_2006_I700665 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEO_2006_I700665); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + vetoEvent; + // everything else + else { + _c_hadrons->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + } + else { + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEO_2006_I700665); + + +} diff --git a/analyses/pluginCESR/CLEO_2006_I700665.info b/analyses/pluginCESR/CLEO_2006_I700665.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2006_I700665.info @@ -0,0 +1,37 @@ +Name: CLEO_2006_I700665 +Year: 2006 +Summary: Hadronic cross section at 3.773 GeV +Experiment: CLEO +Collider: CESR +InspireID: 700665 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 96 (2006) 092002, 2006 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Haronic cross section at 3.773 measured by CLEO.' +Keywords: [] +BibKey: Besson:2005kzr +BibTeX: '@article{Besson:2005kzr, + author = "Besson, D. and others", + title = "{Measurement of $\sigma(e^+e^- \to \psi(3770) \to + hadrons)$ at $E_{c.m.}$ = 3773 MeV}", + collaboration = "CLEO", + journal = "Phys. Rev. Lett.", + volume = "96", + year = "2006", + pages = "092002", + doi = "10.1103/PhysRevLett.96.092002, + 10.1103/PhysRevLett.104.159901", + note = "[Erratum: Phys. Rev. Lett.104,159901(2010)]", + eprint = "1004.1358", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "CLNS-05-1939, CLEO-05-27, hep-ex/0512038", + SLACcitation = "%%CITATION = ARXIV:1004.1358;%%" +} +' diff --git a/analyses/pluginCESR/CLEO_2006_I700665.plot b/analyses/pluginCESR/CLEO_2006_I700665.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2006_I700665.plot @@ -0,0 +1,9 @@ +BEGIN PLOT /CLEO_2006_I700665/d01-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=3. +XMax=4. +END PLOT diff --git a/analyses/pluginCESR/CLEO_2006_I700665.yoda b/analyses/pluginCESR/CLEO_2006_I700665.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2006_I700665.yoda @@ -0,0 +1,9 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2006_I700665/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEO_2006_I700665/d01-x01-y01 +Title: doi:10.17182/hepdata.47194.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.773000e+00 0.000000e+00 0.000000e+00 6.380000e+00 3.104835e-01 4.177320e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CLEO_2007_I753556.cc b/analyses/pluginCESR/CLEO_2007_I753556.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2007_I753556.cc @@ -0,0 +1,101 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CLEO_2007_I753556 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CLEO_2007_I753556); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CLEO_2007_I753556); + + +} diff --git a/analyses/pluginCESR/CLEO_2007_I753556.info b/analyses/pluginCESR/CLEO_2007_I753556.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2007_I753556.info @@ -0,0 +1,36 @@ +Name: CLEO_2007_I753556 +Year: 2007 +Summary: Measurement of $R$ for energies between 6.964 and 10.538 GeV +Experiment: CLEO +Collider: CESR +InspireID: 753556 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D76 (2007) 072008, 2007 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by CLEO for energies between 6.964 and 10.538 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Besson:2007aa +BibTeX: '@article{Besson:2007aa, + author = "Besson, D. and others", + title = "{Measurement of the Total Hadronic Cross Section in e+e- + Annihilations below 10.56-GeV}", + collaboration = "CLEO", + journal = "Phys. Rev.", + volume = "D76", + year = "2007", + pages = "072008", + doi = "10.1103/PhysRevD.76.072008", + eprint = "0706.2813", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "CLNS-07-1998, CLEO-07-7", + SLACcitation = "%%CITATION = ARXIV:0706.2813;%%" +}' diff --git a/analyses/pluginCESR/CLEO_2007_I753556.plot b/analyses/pluginCESR/CLEO_2007_I753556.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2007_I753556.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /CLEO_2007_I753556/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CLEO_2007_I753556/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CLEO_2007_I753556/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginCESR/CLEO_2007_I753556.yoda b/analyses/pluginCESR/CLEO_2007_I753556.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CLEO_2007_I753556.yoda @@ -0,0 +1,15 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CLEO_2007_I753556/d01-x01-y01 +IsRef: 1 +Path: /REF/CLEO_2007_I753556/d01-x01-y01 +Title: doi:10.17182/hepdata.47183.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.964000e+00 0.000000e+00 0.000000e+00 3.597000e+00 6.883313e-02 6.883313e-02 +7.380000e+00 0.000000e+00 0.000000e+00 3.550000e+00 6.422616e-02 6.422616e-02 +8.380000e+00 0.000000e+00 0.000000e+00 3.576000e+00 6.756478e-02 6.756478e-02 +9.432000e+00 0.000000e+00 0.000000e+00 3.510000e+00 7.582875e-02 7.582875e-02 +9.996000e+00 0.000000e+00 0.000000e+00 3.497000e+00 7.720751e-02 7.720751e-02 +1.033000e+01 0.000000e+00 0.000000e+00 3.491000e+00 8.015610e-02 8.015610e-02 +1.053800e+01 0.000000e+00 0.000000e+00 3.591000e+00 8.306022e-02 8.306022e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginCESR/CUSB_1982_I180613.cc b/analyses/pluginCESR/CUSB_1982_I180613.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CUSB_1982_I180613.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CUSB_1982_I180613 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CUSB_1982_I180613); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(3, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(3, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CUSB_1982_I180613); + + +} diff --git a/analyses/pluginCESR/CUSB_1982_I180613.info b/analyses/pluginCESR/CUSB_1982_I180613.info new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CUSB_1982_I180613.info @@ -0,0 +1,31 @@ +Name: CUSB_1982_I180613 +Year: 1982 +Summary: Measurement of $R$ for energies between 10.34 and 11.6 GeV +Experiment: CUSB +Collider: CESR +InspireID: 180613 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 48 (1982) 906-910, 1982 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by CUSB for energies between 10.34 and 11.6 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Rice:1982br +BibTeX: '@article{Rice:1982br, + author = "Rice, E. and others", + title = "{SEARCH FOR STRUCTURE IN SIGMA (E+ E- ---> HADRONS) + BETWEEN S**(1/2) = 10.34-GEV AND 11.6-GEV}", + journal = "Phys. Rev. Lett.", + volume = "48", + year = "1982", + pages = "906-910", + doi = "10.1103/PhysRevLett.48.906", + SLACcitation = "%%CITATION = PRLTA,48,906;%%" +}' diff --git a/analyses/pluginCESR/CUSB_1982_I180613.plot b/analyses/pluginCESR/CUSB_1982_I180613.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CUSB_1982_I180613.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /CUSB_1982_I180613/d03-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CUSB_1982_I180613/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CUSB_1982_I180613/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginCESR/CUSB_1982_I180613.yoda b/analyses/pluginCESR/CUSB_1982_I180613.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginCESR/CUSB_1982_I180613.yoda @@ -0,0 +1,39 @@ +BEGIN YODA_SCATTER1D_V2 /REF/CUSB_1982_I180613/d01-x01-y01 +IsRef: 1 +Path: /REF/CUSB_1982_I180613/d01-x01-y01 +Title: doi:10.17182/hepdata.20593.v1/t1 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CUSB_1982_I180613/d02-x01-y01 +IsRef: 1 +Path: /REF/CUSB_1982_I180613/d02-x01-y01 +Title: doi:10.17182/hepdata.20593.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.043000e+01 9.000000e-02 9.000000e-02 2.290000e+00 2.576669e-01 2.576669e-01 +1.109000e+01 5.100000e-01 5.100000e-01 2.540000e+00 2.867839e-01 2.867839e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CUSB_1982_I180613/d03-x01-y01 +IsRef: 1 +Path: /REF/CUSB_1982_I180613/d03-x01-y01 +Title: doi:10.17182/hepdata.20593.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.043000e+01 9.000000e-02 9.000000e-02 3.540000e+00 3.989298e-01 3.989298e-01 +1.109000e+01 5.100000e-01 5.100000e-01 3.850000e+00 4.333373e-01 4.333373e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CUSB_1982_I180613/d04-x01-y01 +IsRef: 1 +Path: /REF/CUSB_1982_I180613/d04-x01-y01 +Title: doi:10.17182/hepdata.20593.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.043000e+01 9.000000e-02 9.000000e-02 8.194000e-01 1.000000e-03 1.000000e-03 +1.055000e+01 3.000000e-02 3.000000e-02 7.353000e-01 4.300000e-03 4.300000e-03 +1.109000e+01 5.100000e-01 5.100000e-01 8.135000e-01 1.300000e-03 1.300000e-03 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginDORIS/ARGUS_1992_I319102.cc b/analyses/pluginDORIS/ARGUS_1992_I319102.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/ARGUS_1992_I319102.cc @@ -0,0 +1,114 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class ARGUS_1992_I319102 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(ARGUS_1992_I319102); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + if(fuzzyEquals(sqrtS()/GeV, 10.47 , 1E-3)) + _h_N = bookHisto1D(2, 1, 1); + else if(fuzzyEquals(sqrtS()/GeV, 10.575, 1E-3)) + _h_N = bookHisto1D(3, 1, 1); + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else { + _c_hadrons->fill(event.weight()); + if(_h_N) + _h_N->fill(nCharged,event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + if(_h_N) { + normalize(_h_N,200.); + } + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _h_N; + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(ARGUS_1992_I319102); + + +} diff --git a/analyses/pluginDORIS/ARGUS_1992_I319102.info b/analyses/pluginDORIS/ARGUS_1992_I319102.info new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/ARGUS_1992_I319102.info @@ -0,0 +1,34 @@ +Name: ARGUS_1992_I319102 +Year: 1992 +Summary: Measurement of $R$ at 9.36 GeV and charged particle multiplcities in continuum and at the $\Upsilon(4S)$ +Experiment: ARGUS +Collider: DORIS +InspireID: 319102 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C54 (1992) 13-20, 1992 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ at 9.36 GeV and charged particle multiplcities in continuum and at the $\Upsilon(4S)$. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Albrecht:1991vp +BibTeX: '@article{Albrecht:1991vp, + author = "Albrecht, H. and others", + title = "{Measurement of R and determination of the charged + particle multiplicity in e+ e- annihilation at s**(1/2) + around 10-GeV}", + collaboration = "ARGUS", + journal = "Z. Phys.", + volume = "C54", + year = "1992", + pages = "13-20", + doi = "10.1007/BF01881704", + reportNumber = "DESY-91-092", + SLACcitation = "%%CITATION = ZEPYA,C54,13;%%" +}' diff --git a/analyses/pluginDORIS/ARGUS_1992_I319102.plot b/analyses/pluginDORIS/ARGUS_1992_I319102.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/ARGUS_1992_I319102.plot @@ -0,0 +1,41 @@ +BEGIN PLOT /ARGUS_1992_I319102/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +XMin=9. +XMax=10. +END PLOT +BEGIN PLOT /ARGUS_1992_I319102/d02-x01-y01 +Title=Charged Multiplicity at 10.47 GeV +XLabel=$N$ +YLabel=Probability/\% +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /ARGUS_1992_I319102/d03-x01-y01 +Title=Charged Multiplicity at 10.47 GeV +XLabel=$N$ +YLabel=Probability/\% +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /ARGUS_1992_I319102/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=9. +XMax=10. +END PLOT +BEGIN PLOT /ARGUS_1992_I319102/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +XMin=9. +XMax=10. +END PLOT diff --git a/analyses/pluginDORIS/ARGUS_1992_I319102.yoda b/analyses/pluginDORIS/ARGUS_1992_I319102.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/ARGUS_1992_I319102.yoda @@ -0,0 +1,178 @@ +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d01-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d01-x01-y01 +Title: doi:10.17182/hepdata.14708.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.360000e+00 0.000000e+00 0.000000e+00 3.460000e+00 1.334166e-01 1.334166e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d02-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d02-x01-y01 +Title: doi:10.17182/hepdata.14708.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.000000e+00 1.000000e+00 1.000000e+00 1.100000e+00 2.236068e-01 2.236068e-01 +4.000000e+00 1.000000e+00 1.000000e+00 8.600000e+00 7.280110e-01 7.280110e-01 +6.000000e+00 1.000000e+00 1.000000e+00 2.240000e+01 1.264911e+00 1.264911e+00 +8.000000e+00 1.000000e+00 1.000000e+00 2.920000e+01 2.024846e+00 2.024846e+00 +1.000000e+01 1.000000e+00 1.000000e+00 2.290000e+01 2.024846e+00 2.024846e+00 +1.200000e+01 1.000000e+00 1.000000e+00 1.080000e+01 2.109502e+00 2.109502e+00 +1.400000e+01 1.000000e+00 1.000000e+00 3.800000e+00 2.404163e+00 2.404163e+00 +1.600000e+01 1.000000e+00 1.000000e+00 9.000000e-01 1.878829e+00 1.878829e+00 +1.800000e+01 1.000000e+00 1.000000e+00 2.000000e-01 1.280625e+00 1.280625e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d03-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d03-x01-y01 +Title: doi:10.17182/hepdata.14708.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.000000e+00 1.000000e+00 1.000000e+00 8.000000e-01 9.899495e-01 9.899495e-01 +6.000000e+00 1.000000e+00 1.000000e+00 8.800000e+00 2.193171e+00 2.193171e+00 +8.000000e+00 1.000000e+00 1.000000e+00 1.880000e+01 3.612478e+00 3.612478e+00 +1.000000e+01 1.000000e+00 1.000000e+00 2.670000e+01 5.108816e+00 5.108816e+00 +1.200000e+01 1.000000e+00 1.000000e+00 2.300000e+01 6.000000e+00 6.000000e+00 +1.400000e+01 1.000000e+00 1.000000e+00 1.320000e+01 5.300000e+00 5.300000e+00 +1.600000e+01 1.000000e+00 1.000000e+00 5.900000e+00 3.721559e+00 3.721559e+00 +1.800000e+01 1.000000e+00 1.000000e+00 2.600000e+00 2.996665e+00 2.996665e+00 +2.000000e+01 1.000000e+00 1.000000e+00 2.000000e-01 1.019804e+00 1.019804e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d04-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d04-x01-y01 +Title: doi:10.17182/hepdata.14708.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.047000e+01 0.000000e+00 0.000000e+00 8.350000e+00 2.009975e-01 2.009975e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d04-x01-y02 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d04-x01-y02 +Title: doi:10.17182/hepdata.14708.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.047000e+01 0.000000e+00 0.000000e+00 2.710000e+00 1.019804e-01 1.019804e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d04-x01-y03 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d04-x01-y03 +Title: doi:10.17182/hepdata.14708.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.047000e+01 0.000000e+00 0.000000e+00 3.080000e+00 9.219544e-02 9.219544e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d04-x01-y04 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d04-x01-y04 +Title: doi:10.17182/hepdata.14708.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.047000e+01 0.000000e+00 0.000000e+00 1.110000e+00 1.414214e-02 1.414214e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d04-x01-y05 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d04-x01-y05 +Title: doi:10.17182/hepdata.14708.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.047000e+01 0.000000e+00 0.000000e+00 1.330000e+00 3.162278e-02 3.162278e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d04-x01-y06 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d04-x01-y06 +Title: doi:10.17182/hepdata.14708.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.047000e+01 0.000000e+00 0.000000e+00 1.710000e+00 9.219544e-02 9.219544e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d04-x01-y07 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d04-x01-y07 +Title: doi:10.17182/hepdata.14708.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.047000e+01 0.000000e+00 0.000000e+00 2.340000e+00 2.570992e-01 2.570992e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d05-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d05-x01-y01 +Title: doi:10.17182/hepdata.14708.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.057500e+01 0.000000e+00 0.000000e+00 1.081000e+01 2.353720e-01 2.353720e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d05-x01-y02 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d05-x01-y02 +Title: doi:10.17182/hepdata.14708.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.057500e+01 0.000000e+00 0.000000e+00 2.980000e+00 1.264911e-01 1.264911e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d05-x01-y03 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d05-x01-y03 +Title: doi:10.17182/hepdata.14708.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.057500e+01 0.000000e+00 0.000000e+00 3.630000e+00 1.523155e-01 1.523155e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d05-x01-y04 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d05-x01-y04 +Title: doi:10.17182/hepdata.14708.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.057500e+01 0.000000e+00 0.000000e+00 1.080000e+00 1.414214e-02 1.414214e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d05-x01-y05 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d05-x01-y05 +Title: doi:10.17182/hepdata.14708.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.057500e+01 0.000000e+00 0.000000e+00 1.240000e+00 2.236068e-02 2.236068e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d05-x01-y06 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d05-x01-y06 +Title: doi:10.17182/hepdata.14708.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.057500e+01 0.000000e+00 0.000000e+00 1.500000e+00 4.472136e-02 4.472136e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d05-x01-y07 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d05-x01-y07 +Title: doi:10.17182/hepdata.14708.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.057500e+01 0.000000e+00 0.000000e+00 1.910000e+00 9.848858e-02 9.848858e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1992_I319102/d06-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1992_I319102/d06-x01-y01 +Title: doi:10.17182/hepdata.14708.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.360000e+00 0.000000e+00 0.000000e+00 1.550000e-01 6.500000e-02 6.500000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginDORIS/ARGUS_1993_S2653028.cc b/analyses/pluginDORIS/ARGUS_1993_S2653028.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/ARGUS_1993_S2653028.cc @@ -0,0 +1,177 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief BELLE pi+/-, K+/- and proton/antiproton spectrum at Upsilon(4S) + /// @author Peter Richardson + class ARGUS_1993_S2653028 : public Analysis { + public: + + ARGUS_1993_S2653028() + : Analysis("ARGUS_1993_S2653028"), + _weightSum(0.) + { } + + + void analyze(const Event& e) { + const double weight = e.weight(); + + // Find the upsilons + Particles upsilons; + // First in unstable final state + const UnstableParticles& ufs = apply(e, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if (p.pid() == 300553) upsilons.push_back(p); + } + // Then in whole event if that failed + if (upsilons.empty()) { + for(ConstGenParticlePtr p: HepMCUtils::particles(e.genEvent())) { + if (p->pdg_id() != 300553) continue; + ConstGenVertexPtr pv = p->production_vertex(); + bool passed = true; + if (pv) { + for(ConstGenParticlePtr pp: HepMCUtils::particles(pv, Relatives::PARENTS)){ + if ( p->pdg_id() == pp->pdg_id() ) { + passed = false; + break; + } + } + } + if (passed) upsilons.push_back(Particle(*p)); + } + } + + // Find an upsilon + foreach (const Particle& p, upsilons) { + _weightSum += weight; + vector pionsA,pionsB,protonsA,protonsB,kaons; + // Find the decay products we want + findDecayProducts(p.genParticle(), pionsA, pionsB, protonsA, protonsB, kaons); + LorentzTransform cms_boost; + if (p.p3().mod() > 1*MeV) + cms_boost = LorentzTransform::mkFrameTransformFromBeta(p.momentum().betaVec()); + for (size_t ix = 0; ix < pionsA.size(); ++ix) { + FourMomentum ptemp(pionsA[ix]->momentum()); + FourMomentum p2 = cms_boost.transform(ptemp); + double pcm = cms_boost.transform(ptemp).vector3().mod(); + _histPiA->fill(pcm,weight); + } + _multPiA->fill(10.58,double(pionsA.size())*weight); + for (size_t ix = 0; ix < pionsB.size(); ++ix) { + double pcm = cms_boost.transform(FourMomentum(pionsB[ix]->momentum())).vector3().mod(); + _histPiB->fill(pcm,weight); + } + _multPiB->fill(10.58,double(pionsB.size())*weight); + for (size_t ix = 0; ix < protonsA.size(); ++ix) { + double pcm = cms_boost.transform(FourMomentum(protonsA[ix]->momentum())).vector3().mod(); + _histpA->fill(pcm,weight); + } + _multpA->fill(10.58,double(protonsA.size())*weight); + for (size_t ix = 0; ix < protonsB.size(); ++ix) { + double pcm = cms_boost.transform(FourMomentum(protonsB[ix]->momentum())).vector3().mod(); + _histpB->fill(pcm,weight); + } + _multpB->fill(10.58,double(protonsB.size())*weight); + for (size_t ix = 0 ;ix < kaons.size(); ++ix) { + double pcm = cms_boost.transform(FourMomentum(kaons[ix]->momentum())).vector3().mod(); + _histKA->fill(pcm,weight); + _histKB->fill(pcm,weight); + } + _multK->fill(10.58,double(kaons.size())*weight); + } + } + + + void finalize() { + if (_weightSum > 0.) { + scale(_histPiA, 1./_weightSum); + scale(_histPiB, 1./_weightSum); + scale(_histKA , 1./_weightSum); + scale(_histKB , 1./_weightSum); + scale(_histpA , 1./_weightSum); + scale(_histpB , 1./_weightSum); + scale(_multPiA, 1./_weightSum); + scale(_multPiB, 1./_weightSum); + scale(_multK , 1./_weightSum); + scale(_multpA , 1./_weightSum); + scale(_multpB , 1./_weightSum); + } + } + + + void init() { + declare(UnstableParticles(), "UFS"); + + // spectra + _histPiA = bookHisto1D(1, 1, 1); + _histPiB = bookHisto1D(2, 1, 1); + _histKA = bookHisto1D(3, 1, 1); + _histKB = bookHisto1D(6, 1, 1); + _histpA = bookHisto1D(4, 1, 1); + _histpB = bookHisto1D(5, 1, 1); + // multiplicities + _multPiA = bookHisto1D( 7, 1, 1); + _multPiB = bookHisto1D( 8, 1, 1); + _multK = bookHisto1D( 9, 1, 1); + _multpA = bookHisto1D(10, 1, 1); + _multpB = bookHisto1D(11, 1, 1); + } // init + + + private: + + //@{ + /// Count of weights + double _weightSum; + /// Spectra + Histo1DPtr _histPiA, _histPiB, _histKA, _histKB, _histpA, _histpB; + /// Multiplicities + Histo1DPtr _multPiA, _multPiB, _multK, _multpA, _multpB; + //@} + + + void findDecayProducts(ConstGenParticlePtr p, + vector& pionsA, vector& pionsB, + vector& protonsA, vector& protonsB, + vector& kaons) + { + int parentId = p->pdg_id(); + ConstGenVertexPtr dv = p->end_vertex(); + /// @todo Use better looping + for(ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ + int id = abs(pp->pdg_id()); + if (id == PID::PIPLUS) { + if (parentId != PID::LAMBDA && parentId != PID::K0S) { + pionsA.push_back(pp); + pionsB.push_back(pp); + } + else + pionsB.push_back(pp); + } + else if (id == PID::PROTON) { + if (parentId != PID::LAMBDA && parentId != PID::K0S) { + protonsA.push_back(pp); + protonsB.push_back(pp); + } + else + protonsB.push_back(pp); + } + else if (id == PID::KPLUS) { + kaons.push_back(pp); + } + else if (pp->end_vertex()) + findDecayProducts(pp, pionsA, pionsB, protonsA, protonsB, kaons); + } + } + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(ARGUS_1993_S2653028); + +} diff --git a/analyses/pluginMisc/ARGUS_1993_S2653028.info b/analyses/pluginDORIS/ARGUS_1993_S2653028.info rename from analyses/pluginMisc/ARGUS_1993_S2653028.info rename to analyses/pluginDORIS/ARGUS_1993_S2653028.info diff --git a/analyses/pluginMisc/ARGUS_1993_S2653028.plot b/analyses/pluginDORIS/ARGUS_1993_S2653028.plot rename from analyses/pluginMisc/ARGUS_1993_S2653028.plot rename to analyses/pluginDORIS/ARGUS_1993_S2653028.plot diff --git a/analyses/pluginDORIS/ARGUS_1993_S2653028.yoda b/analyses/pluginDORIS/ARGUS_1993_S2653028.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/ARGUS_1993_S2653028.yoda @@ -0,0 +1,323 @@ +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.255, up: 0.255}, sys: {dn: -0.332, up: 0.332}, 'sys,Additional scale uncertainty.': {dn: -0.08914399999999999, up: 0.08914399999999999}}, 1: {stat: {dn: -0.273, up: 0.273}, sys: {dn: -0.239, up: 0.239}, 'sys,Additional scale uncertainty.': {dn: -0.103829, up: 0.103829}}, 2: {stat: {dn: -0.283, up: 0.283}, sys: {dn: -0.385, up: 0.385}, 'sys,Additional scale uncertainty.': {dn: -0.10963700000000001, up: 0.10963700000000001}}, 3: {stat: {dn: -0.31, up: 0.31}, sys: {dn: -0.376, up: 0.376}, 'sys,Additional scale uncertainty.': {dn: -0.123618, up: 0.123618}}, 4: {stat: {dn: -0.335, up: 0.335}, sys: {dn: -0.307, up: 0.307}, 'sys,Additional scale uncertainty.': {dn: -0.12338700000000001, up: 0.12338700000000001}}, 5: {stat: {dn: -0.351, up: 0.351}, sys: {dn: -0.337, up: 0.337}, 'sys,Additional scale uncertainty.': {dn: -0.13428800000000002, up: 0.13428800000000002}}, 6: {stat: {dn: -0.365, up: 0.365}, sys: {dn: -0.292, up: 0.292}, 'sys,Additional scale uncertainty.': {dn: -0.133683, up: 0.133683}}, 7: {stat: {dn: -0.369, up: 0.369}, sys: {dn: -0.293, up: 0.293}, 'sys,Additional scale uncertainty.': {dn: -0.133628, up: 0.133628}}, 8: {stat: {dn: -0.367, up: 0.367}, sys: {dn: -0.366, up: 0.366}, 'sys,Additional scale uncertainty.': {dn: -0.13413400000000003, up: 0.13413400000000003}}, 9: {stat: {dn: -0.363, up: 0.363}, sys: {dn: -0.248, up: 0.248}, 'sys,Additional scale uncertainty.': {dn: -0.129921, up: 0.129921}}, 10: {stat: {dn: -0.358, up: 0.358}, sys: {dn: -0.325, up: 0.325}, 'sys,Additional scale uncertainty.': {dn: -0.12815000000000001, up: 0.12815000000000001}}, 11: {stat: {dn: -0.351, up: 0.351}, sys: {dn: -0.286, up: 0.286}, 'sys,Additional scale uncertainty.': {dn: -0.12111000000000001, up: 0.12111000000000001}}, 12: {stat: {dn: -0.344, up: 0.344}, sys: {dn: -0.232, up: 0.232}, 'sys,Additional scale uncertainty.': {dn: -0.11093500000000002, up: 0.11093500000000002}}, 13: {stat: {dn: -0.335, up: 0.335}, sys: {dn: -0.188, up: 0.188}, 'sys,Additional scale uncertainty.': {dn: -0.11176, up: 0.11176}}, 14: {stat: {dn: -0.325, up: 0.325}, sys: {dn: -0.182, up: 0.182}, 'sys,Additional scale uncertainty.': {dn: -0.10315800000000001, up: 0.10315800000000001}}, 15: {stat: {dn: -0.317, up: 0.317}, sys: {dn: -0.231, up: 0.231}, 'sys,Additional scale uncertainty.': {dn: -0.09852700000000002, up: 0.09852700000000002}}, 16: {stat: {dn: -0.307, up: 0.307}, sys: {dn: -0.145, up: 0.145}, 'sys,Additional scale uncertainty.': {dn: -0.09017800000000001, up: 0.09017800000000001}}, 17: {stat: {dn: -0.301, up: 0.301}, sys: {dn: -0.262, up: 0.262}, 'sys,Additional scale uncertainty.': {dn: -0.085811, up: 0.085811}}, 18: {stat: {dn: -0.293, up: 0.293}, sys: {dn: -0.103, up: 0.103}, 'sys,Additional scale uncertainty.': {dn: -0.074866, up: 0.074866}}, 19: {stat: {dn: -0.284, up: 0.284}, sys: {dn: -0.056, up: 0.056}, 'sys,Additional scale uncertainty.': {dn: -0.067925, up: 0.067925}}, 20: {stat: {dn: -0.273, up: 0.273}, sys: {dn: -0.151, up: 0.151}, 'sys,Additional scale uncertainty.': {dn: -0.06844200000000002, up: 0.06844200000000002}}, 21: {stat: {dn: -0.267, up: 0.267}, sys: {dn: -0.073, up: 0.073}, 'sys,Additional scale uncertainty.': {dn: -0.05918, up: 0.05918}}, 22: {stat: {dn: -0.258, up: 0.258}, sys: {dn: -0.091, up: 0.091}, 'sys,Additional scale uncertainty.': {dn: -0.058399, up: 0.058399}}, 23: {stat: {dn: -0.251, up: 0.251}, sys: {dn: -0.105, up: 0.105}, 'sys,Additional scale uncertainty.': {dn: -0.056056, up: 0.056056}}, 24: {stat: {dn: -0.247, up: 0.247}, sys: {dn: -0.129, up: 0.129}, 'sys,Additional scale uncertainty.': {dn: -0.046123, up: 0.046123}}, 25: {stat: {dn: -0.238, up: 0.238}, sys: {dn: -0.215, up: 0.215}, 'sys,Additional scale uncertainty.': {dn: -0.042702000000000004, up: 0.042702000000000004}}, 26: {stat: {dn: -0.232, up: 0.232}, sys: {dn: -0.134, up: 0.134}, 'sys,Additional scale uncertainty.': {dn: -0.043329000000000006, up: 0.043329000000000006}}, 27: {stat: {dn: -0.224, up: 0.224}, sys: {dn: -0.148, up: 0.148}, 'sys,Additional scale uncertainty.': {dn: -0.041635000000000005, up: 0.041635000000000005}}, 28: {stat: {dn: -0.222, up: 0.222}, sys: {dn: -0.116, up: 0.116}, 'sys,Additional scale uncertainty.': {dn: -0.037070000000000006, up: 0.037070000000000006}}, 29: {stat: {dn: -0.112, up: 0.112}, sys: {dn: -0.098, up: 0.098}, 'sys,Additional scale uncertainty.': {dn: -0.030052000000000002, up: 0.030052000000000002}}, 30: {stat: {dn: -0.105, up: 0.105}, sys: {dn: -0.072, up: 0.072}, 'sys,Additional scale uncertainty.': {dn: -0.020471000000000003, up: 0.020471000000000003}}, 31: {stat: {dn: -0.105, up: 0.105}, sys: {dn: -0.089, up: 0.089}, 'sys,Additional scale uncertainty.': {dn: -0.01276, up: 0.01276}}, 32: {stat: {dn: -0.11, up: 0.11}, sys: {dn: -0.089, up: 0.089}, 'sys,Additional scale uncertainty.': {dn: -0.008921000000000002, up: 0.008921000000000002}}, 33: {stat: {dn: -0.115, up: 0.115}, sys: {dn: -0.136, up: 0.136}, 'sys,Additional scale uncertainty.': {dn: -0.006842, up: 0.006842}}, 34: {stat: {dn: -0.11, up: 0.11}, sys: {dn: -0.064, up: 0.064}, 'sys,Additional scale uncertainty.': {dn: -0.004763, up: 0.004763}}, 35: {stat: {dn: -0.096, up: 0.096}, sys: {dn: -0.075, up: 0.075}, 'sys,Additional scale uncertainty.': {dn: -0.004994, up: 0.004994}}, 36: {stat: {dn: -0.08, up: 0.08}, sys: {dn: -0.072, up: 0.072}, 'sys,Additional scale uncertainty.': {dn: -0.002288, up: 0.002288}}, 37: {stat: {dn: -0.071, up: 0.071}, sys: {dn: -0.058, up: 0.058}, 'sys,Additional scale uncertainty.': {dn: -0.0015509999999999999, up: 0.0015509999999999999}}, 38: {stat: {dn: -0.064, up: 0.064}, sys: {dn: -0.043, up: 0.043}, 'sys,Additional scale uncertainty.': {dn: -0.001925, up: 0.001925}}, 39: {stat: {dn: -0.059, up: 0.059}, sys: {dn: -0.028, up: 0.028}, 'sys,Additional scale uncertainty.': {dn: -0.001122, up: 0.001122}}, 40: {stat: {dn: -0.053, up: 0.053}, sys: {dn: -0.029, up: 0.029}, 'sys,Additional scale uncertainty.': {dn: -0.00099, up: 0.00099}}, 41: {stat: {dn: -0.049, up: 0.049}, sys: {dn: -0.029, up: 0.029}, 'sys,Additional scale uncertainty.': {dn: -0.001353, up: 0.001353}}, 42: {stat: {dn: -0.044, up: 0.044}, sys: {dn: -0.033, up: 0.033}, 'sys,Additional scale uncertainty.': {dn: -0.0007260000000000001, up: 0.0007260000000000001}}, 43: {stat: {dn: -0.038, up: 0.038}, sys: {dn: -0.017, up: 0.017}, 'sys,Additional scale uncertainty.': {dn: -0.0015400000000000004, up: 0.0015400000000000004}}, 44: {stat: {dn: -0.035, up: 0.035}, sys: {dn: -0.027, up: 0.027}, 'sys,Additional scale uncertainty.': {dn: -0.00011000000000000002, up: 0.00011000000000000002}}, 45: {stat: {dn: -0.031, up: 0.031}, sys: {dn: -0.034, up: 0.034}, 'sys,Additional scale uncertainty.': {dn: -0.00023100000000000003, up: 0.00023100000000000003}}, 46: {stat: {dn: -0.027, up: 0.027}, sys: {dn: -0.014, up: 0.014}, 'sys,Additional scale uncertainty.': {dn: -0.000286, up: 0.000286}}, 47: {stat: {dn: -0.025, up: 0.025}, sys: {dn: -0.025, up: 0.025}, 'sys,Additional scale uncertainty.': {dn: 0.000165, up: -0.000165}}, 48: {stat: {dn: -0.024, up: 0.024}, sys: {dn: -0.016, up: 0.016}, 'sys,Additional scale uncertainty.': {dn: 0.000121, up: -0.000121}}} + +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d01-x01-y01 +Title: doi:10.17182/hepdata.14424.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +8.750000e-02 1.250000e-02 1.250000e-02 8.104000e+00 4.280136e-01 4.280136e-01 +1.125000e-01 1.250000e-02 1.250000e-02 9.439000e+00 3.773996e-01 3.773996e-01 +1.375000e-01 1.250000e-02 1.250000e-02 9.967000e+00 4.902390e-01 4.902390e-01 +1.625000e-01 1.250000e-02 1.250000e-02 1.123800e+01 5.027498e-01 5.027498e-01 +1.875000e-01 1.250000e-02 1.250000e-02 1.121700e+01 4.708485e-01 4.708485e-01 +2.125000e-01 1.250000e-02 1.250000e-02 1.220800e+01 5.047804e-01 5.047804e-01 +2.375000e-01 1.250000e-02 1.250000e-02 1.215300e+01 4.861688e-01 4.861688e-01 +2.625000e-01 1.250000e-02 1.250000e-02 1.214800e+01 4.897616e-01 4.897616e-01 +2.875000e-01 1.250000e-02 1.250000e-02 1.219400e+01 5.353848e-01 5.353848e-01 +3.125000e-01 1.250000e-02 1.250000e-02 1.181100e+01 4.584239e-01 4.584239e-01 +3.375000e-01 1.250000e-02 1.250000e-02 1.165000e+01 5.002114e-01 5.002114e-01 +3.625000e-01 1.250000e-02 1.250000e-02 1.101000e+01 4.686839e-01 4.686839e-01 +3.875000e-01 1.250000e-02 1.250000e-02 1.008500e+01 4.294957e-01 4.294957e-01 +4.125000e-01 1.250000e-02 1.250000e-02 1.016000e+01 4.000741e-01 4.000741e-01 +4.375000e-01 1.250000e-02 1.250000e-02 9.378000e+00 3.865108e-01 3.865108e-01 +4.625000e-01 1.250000e-02 1.250000e-02 8.957000e+00 4.044225e-01 4.044225e-01 +4.875000e-01 1.250000e-02 1.250000e-02 8.198000e+00 3.512920e-01 3.512920e-01 +5.125000e-01 1.250000e-02 1.250000e-02 7.801000e+00 4.081771e-01 4.081771e-01 +5.375000e-01 1.250000e-02 1.250000e-02 6.806000e+00 3.194729e-01 3.194729e-01 +5.625000e-01 1.250000e-02 1.250000e-02 6.175000e+00 2.973311e-01 2.973311e-01 +5.875000e-01 1.250000e-02 1.250000e-02 6.222000e+00 3.193968e-01 3.193968e-01 +6.125000e-01 1.250000e-02 1.250000e-02 5.380000e+00 2.830552e-01 2.830552e-01 +6.375000e-01 1.250000e-02 1.250000e-02 5.309000e+00 2.797417e-01 2.797417e-01 +6.625000e-01 1.250000e-02 1.250000e-02 5.096000e+00 2.777918e-01 2.777918e-01 +6.875000e-01 1.250000e-02 1.250000e-02 4.193000e+00 2.824488e-01 2.824488e-01 +7.125000e-01 1.250000e-02 1.250000e-02 3.882000e+00 3.235621e-01 3.235621e-01 +7.375000e-01 1.250000e-02 1.250000e-02 3.939000e+00 2.713990e-01 2.713990e-01 +7.625000e-01 1.250000e-02 1.250000e-02 3.785000e+00 2.716864e-01 2.716864e-01 +7.875000e-01 1.250000e-02 1.250000e-02 3.370000e+00 2.532078e-01 2.532078e-01 +8.500000e-01 5.000000e-02 5.000000e-02 2.732000e+00 1.518260e-01 1.518260e-01 +9.500000e-01 5.000000e-02 5.000000e-02 1.861000e+00 1.289498e-01 1.289498e-01 +1.050000e+00 5.000000e-02 5.000000e-02 1.160000e+00 1.382346e-01 1.382346e-01 +1.150000e+00 5.000000e-02 5.000000e-02 8.110000e-01 1.417765e-01 1.417765e-01 +1.250000e+00 5.000000e-02 5.000000e-02 6.220000e-01 1.782353e-01 1.782353e-01 +1.350000e+00 5.000000e-02 5.000000e-02 4.330000e-01 1.273526e-01 1.273526e-01 +1.450000e+00 5.000000e-02 5.000000e-02 4.540000e-01 1.219260e-01 1.219260e-01 +1.550000e+00 5.000000e-02 5.000000e-02 2.080000e-01 1.076533e-01 1.076533e-01 +1.650000e+00 5.000000e-02 5.000000e-02 1.410000e-01 9.169191e-02 9.169191e-02 +1.750000e+00 5.000000e-02 5.000000e-02 1.750000e-01 7.712785e-02 7.712785e-02 +1.850000e+00 5.000000e-02 5.000000e-02 1.020000e-01 6.531660e-02 6.531660e-02 +1.950000e+00 5.000000e-02 5.000000e-02 9.000000e-02 6.042334e-02 6.042334e-02 +2.050000e+00 5.000000e-02 5.000000e-02 1.230000e-01 5.695464e-02 5.695464e-02 +2.150000e+00 5.000000e-02 5.000000e-02 6.600000e-02 5.500479e-02 5.500479e-02 +2.250000e+00 5.000000e-02 5.000000e-02 1.400000e-01 4.165779e-02 4.165779e-02 +2.350000e+00 5.000000e-02 5.000000e-02 1.000000e-02 4.420421e-02 4.420421e-02 +2.450000e+00 5.000000e-02 5.000000e-02 2.100000e-02 4.601145e-02 4.601145e-02 +2.550000e+00 5.000000e-02 5.000000e-02 2.600000e-02 3.041516e-02 3.041516e-02 +2.650000e+00 5.000000e-02 5.000000e-02 -1.500000e-02 3.535572e-02 3.535572e-02 +2.750000e+00 5.000000e-02 5.000000e-02 -1.100000e-02 2.884466e-02 2.884466e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.255, up: 0.255}, sys: {dn: -0.383, up: 0.383}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.10291600000000001, up: 0.10291600000000001}, 'sys,Additional scale uncertainty.': {dn: -0.10291600000000001, up: 0.10291600000000001}}, 1: {stat: {dn: -0.273, up: 0.273}, sys: {dn: -0.281, up: 0.281}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.12233100000000001, up: 0.12233100000000001}, 'sys,Additional scale uncertainty.': {dn: -0.12233100000000001, up: 0.12233100000000001}}, 2: {stat: {dn: -0.283, up: 0.283}, sys: {dn: -0.465, up: 0.465}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.132396, up: 0.132396}, 'sys,Additional scale uncertainty.': {dn: -0.132396, up: 0.132396}}, 3: {stat: {dn: -0.31, up: 0.31}, sys: {dn: -0.455, up: 0.455}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.14932499999999999, up: 0.14932499999999999}, 'sys,Additional scale uncertainty.': {dn: -0.14932499999999999, up: 0.14932499999999999}}, 4: {stat: {dn: -0.335, up: 0.335}, sys: {dn: -0.377, up: 0.377}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.15149200000000002, up: 0.15149200000000002}, 'sys,Additional scale uncertainty.': {dn: -0.15149200000000002, up: 0.15149200000000002}}, 5: {stat: {dn: -0.351, up: 0.351}, sys: {dn: -0.408, up: 0.408}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.162646, up: 0.162646}, 'sys,Additional scale uncertainty.': {dn: -0.162646, up: 0.162646}}, 6: {stat: {dn: -0.365, up: 0.365}, sys: {dn: -0.348, up: 0.348}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.159654, up: 0.159654}, 'sys,Additional scale uncertainty.': {dn: -0.159654, up: 0.159654}}, 7: {stat: {dn: -0.369, up: 0.369}, sys: {dn: -0.344, up: 0.344}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.156948, up: 0.156948}, 'sys,Additional scale uncertainty.': {dn: -0.156948, up: 0.156948}}, 8: {stat: {dn: -0.367, up: 0.367}, sys: {dn: -0.426, up: 0.426}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.15596900000000002, up: 0.15596900000000002}, 'sys,Additional scale uncertainty.': {dn: -0.15596900000000002, up: 0.15596900000000002}}, 9: {stat: {dn: -0.363, up: 0.363}, sys: {dn: -0.286, up: 0.286}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.150238, up: 0.150238}, 'sys,Additional scale uncertainty.': {dn: -0.150238, up: 0.150238}}, 10: {stat: {dn: -0.358, up: 0.358}, sys: {dn: -0.373, up: 0.373}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.14703700000000003, up: 0.14703700000000003}, 'sys,Additional scale uncertainty.': {dn: -0.14703700000000003, up: 0.14703700000000003}}, 11: {stat: {dn: -0.351, up: 0.351}, sys: {dn: -0.328, up: 0.328}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.139139, up: 0.139139}, 'sys,Additional scale uncertainty.': {dn: -0.139139, up: 0.139139}}, 12: {stat: {dn: -0.344, up: 0.344}, sys: {dn: -0.266, up: 0.266}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.12718200000000002, up: 0.12718200000000002}, 'sys,Additional scale uncertainty.': {dn: -0.12718200000000002, up: 0.12718200000000002}}, 13: {stat: {dn: -0.335, up: 0.335}, sys: {dn: -0.213, up: 0.213}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.126654, up: 0.126654}, 'sys,Additional scale uncertainty.': {dn: -0.126654, up: 0.126654}}, 14: {stat: {dn: -0.325, up: 0.325}, sys: {dn: -0.207, up: 0.207}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.11715, up: 0.11715}, 'sys,Additional scale uncertainty.': {dn: -0.11715, up: 0.11715}}, 15: {stat: {dn: -0.317, up: 0.317}, sys: {dn: -0.261, up: 0.261}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.11123200000000001, up: 0.11123200000000001}, 'sys,Additional scale uncertainty.': {dn: -0.11123200000000001, up: 0.11123200000000001}}, 16: {stat: {dn: -0.307, up: 0.307}, sys: {dn: -0.164, up: 0.164}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.10198100000000003, up: 0.10198100000000003}, 'sys,Additional scale uncertainty.': {dn: -0.10198100000000003, up: 0.10198100000000003}}, 17: {stat: {dn: -0.301, up: 0.301}, sys: {dn: -0.294, up: 0.294}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.09638200000000001, up: 0.09638200000000001}, 'sys,Additional scale uncertainty.': {dn: -0.09638200000000001, up: 0.09638200000000001}}, 18: {stat: {dn: -0.293, up: 0.293}, sys: {dn: -0.116, up: 0.116}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.08409499999999999, up: 0.08409499999999999}, 'sys,Additional scale uncertainty.': {dn: -0.08409499999999999, up: 0.08409499999999999}}, 19: {stat: {dn: -0.284, up: 0.284}, sys: {dn: -0.063, up: 0.063}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.076527, up: 0.076527}, 'sys,Additional scale uncertainty.': {dn: -0.076527, up: 0.076527}}, 20: {stat: {dn: -0.273, up: 0.273}, sys: {dn: -0.168, up: 0.168}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.07616400000000002, up: 0.07616400000000002}, 'sys,Additional scale uncertainty.': {dn: -0.07616400000000002, up: 0.07616400000000002}}, 21: {stat: {dn: -0.267, up: 0.267}, sys: {dn: -0.082, up: 0.082}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.066231, up: 0.066231}, 'sys,Additional scale uncertainty.': {dn: -0.066231, up: 0.066231}}, 22: {stat: {dn: -0.258, up: 0.258}, sys: {dn: -0.1, up: 0.1}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.064647, up: 0.064647}, 'sys,Additional scale uncertainty.': {dn: -0.064647, up: 0.064647}}, 23: {stat: {dn: -0.251, up: 0.251}, sys: {dn: -0.116, up: 0.116}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.061996, up: 0.061996}, 'sys,Additional scale uncertainty.': {dn: -0.061996, up: 0.061996}}, 24: {stat: {dn: -0.247, up: 0.247}, sys: {dn: -0.144, up: 0.144}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.051381, up: 0.051381}, 'sys,Additional scale uncertainty.': {dn: -0.051381, up: 0.051381}}, 25: {stat: {dn: -0.238, up: 0.238}, sys: {dn: -0.239, up: 0.239}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.04746500000000001, up: 0.04746500000000001}, 'sys,Additional scale uncertainty.': {dn: -0.04746500000000001, up: 0.04746500000000001}}, 26: {stat: {dn: -0.232, up: 0.232}, sys: {dn: -0.147, up: 0.147}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.04775100000000001, up: 0.04775100000000001}, 'sys,Additional scale uncertainty.': {dn: -0.04775100000000001, up: 0.04775100000000001}}, 27: {stat: {dn: -0.224, up: 0.224}, sys: {dn: -0.162, up: 0.162}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.045727000000000004, up: 0.045727000000000004}, 'sys,Additional scale uncertainty.': {dn: -0.045727000000000004, up: 0.045727000000000004}}, 28: {stat: {dn: -0.222, up: 0.222}, sys: {dn: -0.127, up: 0.127}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.040579000000000004, up: 0.040579000000000004}, 'sys,Additional scale uncertainty.': {dn: -0.040579000000000004, up: 0.040579000000000004}}, 29: {stat: {dn: -0.112, up: 0.112}, sys: {dn: -0.107, up: 0.107}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.032813, up: 0.032813}, 'sys,Additional scale uncertainty.': {dn: -0.032813, up: 0.032813}}, 30: {stat: {dn: -0.105, up: 0.105}, sys: {dn: -0.079, up: 0.079}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.022462, up: 0.022462}, 'sys,Additional scale uncertainty.': {dn: -0.022462, up: 0.022462}}, 31: {stat: {dn: -0.105, up: 0.105}, sys: {dn: -0.099, up: 0.099}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.014080000000000002, up: 0.014080000000000002}, 'sys,Additional scale uncertainty.': {dn: -0.014080000000000002, up: 0.014080000000000002}}, 32: {stat: {dn: -0.11, up: 0.11}, sys: {dn: -0.098, up: 0.098}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.009801, up: 0.009801}, 'sys,Additional scale uncertainty.': {dn: -0.009801, up: 0.009801}}, 33: {stat: {dn: -0.115, up: 0.115}, sys: {dn: -0.148, up: 0.148}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.007436000000000001, up: 0.007436000000000001}, 'sys,Additional scale uncertainty.': {dn: -0.007436000000000001, up: 0.007436000000000001}}, 34: {stat: {dn: -0.11, up: 0.11}, sys: {dn: -0.07, up: 0.07}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.005203, up: 0.005203}, 'sys,Additional scale uncertainty.': {dn: -0.005203, up: 0.005203}}, 35: {stat: {dn: -0.096, up: 0.096}, sys: {dn: -0.079, up: 0.079}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.005247, up: 0.005247}, 'sys,Additional scale uncertainty.': {dn: -0.005247, up: 0.005247}}, 36: {stat: {dn: -0.08, up: 0.08}, sys: {dn: -0.077, up: 0.077}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0024530000000000003, up: 0.0024530000000000003}, 'sys,Additional scale uncertainty.': {dn: -0.0024530000000000003, up: 0.0024530000000000003}}, 37: {stat: {dn: -0.071, up: 0.071}, sys: {dn: -0.061, up: 0.061}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0016500000000000002, up: 0.0016500000000000002}, 'sys,Additional scale uncertainty.': {dn: -0.0016500000000000002, up: 0.0016500000000000002}}, 38: {stat: {dn: -0.064, up: 0.064}, sys: {dn: -0.045, up: 0.045}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.001991, up: 0.001991}, 'sys,Additional scale uncertainty.': {dn: -0.001991, up: 0.001991}}, 39: {stat: {dn: -0.059, up: 0.059}, sys: {dn: -0.029, up: 0.029}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.001155, up: 0.001155}, 'sys,Additional scale uncertainty.': {dn: -0.001155, up: 0.001155}}, 40: {stat: {dn: -0.053, up: 0.053}, sys: {dn: -0.03, up: 0.03}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0010010000000000002, up: 0.0010010000000000002}, 'sys,Additional scale uncertainty.': {dn: -0.0010010000000000002, up: 0.0010010000000000002}}, 41: {stat: {dn: -0.049, up: 0.049}, sys: {dn: -0.03, up: 0.03}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0013750000000000001, up: 0.0013750000000000001}, 'sys,Additional scale uncertainty.': {dn: -0.0013750000000000001, up: 0.0013750000000000001}}, 42: {stat: {dn: -0.044, up: 0.044}, sys: {dn: -0.033, up: 0.033}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0007370000000000001, up: 0.0007370000000000001}, 'sys,Additional scale uncertainty.': {dn: -0.0007370000000000001, up: 0.0007370000000000001}}, 43: {stat: {dn: -0.038, up: 0.038}, sys: {dn: -0.017, up: 0.017}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0015400000000000004, up: 0.0015400000000000004}, 'sys,Additional scale uncertainty.': {dn: -0.0015400000000000004, up: 0.0015400000000000004}}, 44: {stat: {dn: -0.035, up: 0.035}, sys: {dn: -0.027, up: 0.027}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00011000000000000002, up: 0.00011000000000000002}, 'sys,Additional scale uncertainty.': {dn: -0.00011000000000000002, up: 0.00011000000000000002}}, 45: {stat: {dn: -0.031, up: 0.031}, sys: {dn: -0.034, up: 0.034}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00023100000000000003, up: 0.00023100000000000003}, 'sys,Additional scale uncertainty.': {dn: -0.00023100000000000003, up: 0.00023100000000000003}}, 46: {stat: {dn: -0.027, up: 0.027}, sys: {dn: -0.014, up: 0.014}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.000286, up: 0.000286}, 'sys,Additional scale uncertainty.': {dn: -0.000286, up: 0.000286}}, 47: {stat: {dn: -0.025, up: 0.025}, sys: {dn: -0.025, up: 0.025}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.000165, up: -0.000165}, 'sys,Additional scale uncertainty.': {dn: 0.000165, up: -0.000165}}, 48: {stat: {dn: -0.024, up: 0.024}, sys: {dn: -0.016, up: 0.016}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.000121, up: -0.000121}, 'sys,Additional scale uncertainty.': {dn: 0.000121, up: -0.000121}}} + +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d02-x01-y01 +Title: doi:10.17182/hepdata.14424.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +8.750000e-02 1.250000e-02 1.250000e-02 9.356000e+00 4.825945e-01 4.825945e-01 +1.125000e-01 1.250000e-02 1.250000e-02 1.112100e+01 4.282753e-01 4.282753e-01 +1.375000e-01 1.250000e-02 1.250000e-02 1.203600e+01 5.756487e-01 5.756487e-01 +1.625000e-01 1.250000e-02 1.250000e-02 1.357500e+01 5.896787e-01 5.896787e-01 +1.875000e-01 1.250000e-02 1.250000e-02 1.377200e+01 5.479541e-01 5.479541e-01 +2.125000e-01 1.250000e-02 1.250000e-02 1.478600e+01 5.852969e-01 5.852969e-01 +2.375000e-01 1.250000e-02 1.250000e-02 1.451400e+01 5.525466e-01 5.525466e-01 +2.625000e-01 1.250000e-02 1.250000e-02 1.426800e+01 5.511464e-01 5.511464e-01 +2.875000e-01 1.250000e-02 1.250000e-02 1.417900e+01 6.040014e-01 6.040014e-01 +3.125000e-01 1.250000e-02 1.250000e-02 1.365800e+01 5.086334e-01 5.086334e-01 +3.375000e-01 1.250000e-02 1.250000e-02 1.336700e+01 5.572547e-01 5.572547e-01 +3.625000e-01 1.250000e-02 1.250000e-02 1.264900e+01 5.191381e-01 5.191381e-01 +3.875000e-01 1.250000e-02 1.250000e-02 1.156200e+01 4.705768e-01 4.705768e-01 +4.125000e-01 1.250000e-02 1.250000e-02 1.151400e+01 4.355186e-01 4.355186e-01 +4.375000e-01 1.250000e-02 1.250000e-02 1.065000e+01 4.194309e-01 4.194309e-01 +4.625000e-01 1.250000e-02 1.250000e-02 1.011200e+01 4.397216e-01 4.397216e-01 +4.875000e-01 1.250000e-02 1.250000e-02 9.271000e+00 3.767562e-01 3.767562e-01 +5.125000e-01 1.250000e-02 1.250000e-02 8.762000e+00 4.422850e-01 4.422850e-01 +5.375000e-01 1.250000e-02 1.250000e-02 7.645000e+00 3.368218e-01 3.368218e-01 +5.625000e-01 1.250000e-02 1.250000e-02 6.957000e+00 3.103833e-01 3.103833e-01 +5.875000e-01 1.250000e-02 1.250000e-02 6.924000e+00 3.381640e-01 3.381640e-01 +6.125000e-01 1.250000e-02 1.250000e-02 6.021000e+00 2.945948e-01 2.945948e-01 +6.375000e-01 1.250000e-02 1.250000e-02 5.877000e+00 2.914146e-01 2.914146e-01 +6.625000e-01 1.250000e-02 1.250000e-02 5.636000e+00 2.900759e-01 2.900759e-01 +6.875000e-01 1.250000e-02 1.250000e-02 4.671000e+00 2.950000e-01 2.950000e-01 +7.125000e-01 1.250000e-02 1.250000e-02 4.315000e+00 3.439053e-01 3.439053e-01 +7.375000e-01 1.250000e-02 1.250000e-02 4.341000e+00 2.828309e-01 2.828309e-01 +7.625000e-01 1.250000e-02 1.250000e-02 4.157000e+00 2.839048e-01 2.839048e-01 +7.875000e-01 1.250000e-02 1.250000e-02 3.689000e+00 2.621189e-01 2.621189e-01 +8.500000e-01 5.000000e-02 5.000000e-02 2.983000e+00 1.616984e-01 1.616984e-01 +9.500000e-01 5.000000e-02 5.000000e-02 2.042000e+00 1.351854e-01 1.351854e-01 +1.050000e+00 5.000000e-02 5.000000e-02 1.280000e+00 1.456794e-01 1.456794e-01 +1.150000e+00 5.000000e-02 5.000000e-02 8.910000e-01 1.479734e-01 1.479734e-01 +1.250000e+00 5.000000e-02 5.000000e-02 6.760000e-01 1.877221e-01 1.877221e-01 +1.350000e+00 5.000000e-02 5.000000e-02 4.730000e-01 1.305915e-01 1.305915e-01 +1.450000e+00 5.000000e-02 5.000000e-02 4.770000e-01 1.245474e-01 1.245474e-01 +1.550000e+00 5.000000e-02 5.000000e-02 2.230000e-01 1.110902e-01 1.110902e-01 +1.650000e+00 5.000000e-02 5.000000e-02 1.500000e-01 9.363464e-02 9.363464e-02 +1.750000e+00 5.000000e-02 5.000000e-02 1.810000e-01 7.828747e-02 7.828747e-02 +1.850000e+00 5.000000e-02 5.000000e-02 1.050000e-01 6.576221e-02 6.576221e-02 +1.950000e+00 5.000000e-02 5.000000e-02 9.100000e-02 6.091801e-02 6.091801e-02 +2.050000e+00 5.000000e-02 5.000000e-02 1.250000e-01 5.748723e-02 5.748723e-02 +2.150000e+00 5.000000e-02 5.000000e-02 6.700000e-02 5.500987e-02 5.500987e-02 +2.250000e+00 5.000000e-02 5.000000e-02 1.400000e-01 4.168625e-02 4.168625e-02 +2.350000e+00 5.000000e-02 5.000000e-02 1.000000e-02 4.420435e-02 4.420435e-02 +2.450000e+00 5.000000e-02 5.000000e-02 2.100000e-02 4.601203e-02 4.601203e-02 +2.550000e+00 5.000000e-02 5.000000e-02 2.600000e-02 3.041650e-02 3.041650e-02 +2.650000e+00 5.000000e-02 5.000000e-02 -1.500000e-02 3.535611e-02 3.535611e-02 +2.750000e+00 5.000000e-02 5.000000e-02 -1.100000e-02 2.884492e-02 2.884492e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.081, up: 0.081}, sys: {dn: -0.097, up: 0.097}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.007458000000000001, up: 0.007458000000000001}}, 1: {stat: {dn: -0.086, up: 0.086}, sys: {dn: -0.095, up: 0.095}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.011352000000000003, up: 0.011352000000000003}}, 2: {stat: {dn: -0.087, up: 0.087}, sys: {dn: -0.108, up: 0.108}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.013640000000000001, up: 0.013640000000000001}}, 3: {stat: {dn: -0.087, up: 0.087}, sys: {dn: -0.071, up: 0.071}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.015246000000000001, up: 0.015246000000000001}}, 4: {stat: {dn: -0.093, up: 0.093}, sys: {dn: -0.126, up: 0.126}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.015653, up: 0.015653}}, 5: {stat: {dn: -0.092, up: 0.092}, sys: {dn: -0.071, up: 0.071}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.016511, up: 0.016511}}, 6: {stat: {dn: -0.094, up: 0.094}, sys: {dn: -0.096, up: 0.096}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.017721, up: 0.017721}}, 7: {stat: {dn: -0.098, up: 0.098}, sys: {dn: -0.084, up: 0.084}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.020823, up: 0.020823}}, 8: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.057, up: 0.057}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.020174000000000004, up: 0.020174000000000004}}, 9: {stat: {dn: -0.099, up: 0.099}, sys: {dn: -0.075, up: 0.075}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.022913000000000003, up: 0.022913000000000003}}, 10: {stat: {dn: -0.103, up: 0.103}, sys: {dn: -0.068, up: 0.068}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.022099, up: 0.022099}}, 11: {stat: {dn: -0.103, up: 0.103}, sys: {dn: -0.056, up: 0.056}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.022000000000000002, up: 0.022000000000000002}}, 12: {stat: {dn: -0.104, up: 0.104}, sys: {dn: -0.084, up: 0.084}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.023430000000000003, up: 0.023430000000000003}}, 13: {stat: {dn: -0.106, up: 0.106}, sys: {dn: -0.094, up: 0.094}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.021472, up: 0.021472}}, 14: {stat: {dn: -0.107, up: 0.107}, sys: {dn: -0.086, up: 0.086}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.020757000000000005, up: 0.020757000000000005}}, 15: {stat: {dn: -0.108, up: 0.108}, sys: {dn: -0.086, up: 0.086}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.020042, up: 0.020042}}, 16: {stat: {dn: -0.108, up: 0.108}, sys: {dn: -0.072, up: 0.072}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.019899, up: 0.019899}}, 17: {stat: {dn: -0.109, up: 0.109}, sys: {dn: -0.071, up: 0.071}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.020944, up: 0.020944}}, 18: {stat: {dn: -0.111, up: 0.111}, sys: {dn: -0.086, up: 0.086}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.019052, up: 0.019052}}, 19: {stat: {dn: -0.113, up: 0.113}, sys: {dn: -0.063, up: 0.063}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.017281, up: 0.017281}}, 20: {stat: {dn: -0.112, up: 0.112}, sys: {dn: -0.06, up: 0.06}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.016731, up: 0.016731}}, 21: {stat: {dn: -0.113, up: 0.113}, sys: {dn: -0.133, up: 0.133}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.015455000000000002, up: 0.015455000000000002}}, 22: {stat: {dn: -0.114, up: 0.114}, sys: {dn: -0.091, up: 0.091}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.015312, up: 0.015312}}, 23: {stat: {dn: -0.112, up: 0.112}, sys: {dn: -0.156, up: 0.156}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.015169000000000002, up: 0.015169000000000002}}, 24: {stat: {dn: -0.118, up: 0.118}, sys: {dn: -0.115, up: 0.115}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.013200000000000002, up: 0.013200000000000002}}, 25: {stat: {dn: -0.06, up: 0.06}, sys: {dn: -0.051, up: 0.051}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.010087000000000002, up: 0.010087000000000002}}, 26: {stat: {dn: -0.066, up: 0.066}, sys: {dn: -0.054, up: 0.054}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.010527000000000002, up: 0.010527000000000002}}, 27: {stat: {dn: -0.079, up: 0.079}, sys: {dn: -0.092, up: 0.092}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.007249000000000001, up: 0.007249000000000001}}, 28: {stat: {dn: -0.094, up: 0.094}, sys: {dn: -0.063, up: 0.063}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.004433000000000001, up: 0.004433000000000001}}, 29: {stat: {dn: -0.103, up: 0.103}, sys: {dn: -0.131, up: 0.131}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.006292, up: 0.006292}}, 30: {stat: {dn: -0.101, up: 0.101}, sys: {dn: -0.029, up: 0.029}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.005885000000000001, up: 0.005885000000000001}}, 31: {stat: {dn: -0.084, up: 0.084}, sys: {dn: -0.074, up: 0.074}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.002288, up: 0.002288}}, 32: {stat: {dn: -0.067, up: 0.067}, sys: {dn: -0.042, up: 0.042}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.003432, up: 0.003432}}, 33: {stat: {dn: -0.056, up: 0.056}, sys: {dn: -0.019, up: 0.019}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0017600000000000003, up: 0.0017600000000000003}}, 34: {stat: {dn: -0.049, up: 0.049}, sys: {dn: -0.024, up: 0.024}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0013640000000000002, up: 0.0013640000000000002}}, 35: {stat: {dn: -0.044, up: 0.044}, sys: {dn: -0.03, up: 0.03}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.000143, up: 0.000143}}, 36: {stat: {dn: -0.039, up: 0.039}, sys: {dn: -0.011, up: 0.011}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.000715, up: 0.000715}}, 37: {stat: {dn: -0.039, up: 0.039}, sys: {dn: -0.021, up: 0.021}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.0006820000000000001, up: -0.0006820000000000001}}, 38: {stat: {dn: -0.037, up: 0.037}, sys: {dn: -0.01, up: 0.01}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.000286, up: -0.000286}}, 39: {stat: {dn: -0.035, up: 0.035}, sys: {dn: -0.027, up: 0.027}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.000264, up: 0.000264}}, 40: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.023, up: 0.023}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.00023100000000000003, up: -0.00023100000000000003}}, 41: {stat: {dn: -0.036, up: 0.036}, sys: {dn: -0.023, up: 0.023}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00015400000000000003, up: 0.00015400000000000003}}, 42: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.023, up: 0.023}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.00035200000000000005, up: -0.00035200000000000005}}, 43: {stat: {dn: -0.034, up: 0.034}, sys: {dn: -0.011, up: 0.011}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00044000000000000007, up: 0.00044000000000000007}}, 44: {stat: {dn: -0.037, up: 0.037}, sys: {dn: -0.022, up: 0.022}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.000506, up: 0.000506}}} + +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d03-x01-y01 +Title: doi:10.17182/hepdata.14424.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.875000e-01 1.250000e-02 1.250000e-02 6.780000e-01 1.265923e-01 1.265923e-01 +2.125000e-01 1.250000e-02 1.250000e-02 1.032000e+00 1.286463e-01 1.286463e-01 +2.375000e-01 1.250000e-02 1.250000e-02 1.240000e+00 1.393523e-01 1.393523e-01 +2.625000e-01 1.250000e-02 1.250000e-02 1.386000e+00 1.133245e-01 1.133245e-01 +2.875000e-01 1.250000e-02 1.250000e-02 1.423000e+00 1.573849e-01 1.573849e-01 +3.125000e-01 1.250000e-02 1.250000e-02 1.501000e+00 1.173781e-01 1.173781e-01 +3.375000e-01 1.250000e-02 1.250000e-02 1.611000e+00 1.355213e-01 1.355213e-01 +3.625000e-01 1.250000e-02 1.250000e-02 1.893000e+00 1.307425e-01 1.307425e-01 +3.875000e-01 1.250000e-02 1.250000e-02 1.834000e+00 1.168588e-01 1.168588e-01 +4.125000e-01 1.250000e-02 1.250000e-02 2.083000e+00 1.262973e-01 1.262973e-01 +4.375000e-01 1.250000e-02 1.250000e-02 2.009000e+00 1.253849e-01 1.253849e-01 +4.625000e-01 1.250000e-02 1.250000e-02 2.000000e+00 1.192854e-01 1.192854e-01 +4.875000e-01 1.250000e-02 1.250000e-02 2.130000e+00 1.357239e-01 1.357239e-01 +5.125000e-01 1.250000e-02 1.250000e-02 1.952000e+00 1.432936e-01 1.432936e-01 +5.375000e-01 1.250000e-02 1.250000e-02 1.887000e+00 1.388375e-01 1.388375e-01 +5.625000e-01 1.250000e-02 1.250000e-02 1.822000e+00 1.395051e-01 1.395051e-01 +5.875000e-01 1.250000e-02 1.250000e-02 1.809000e+00 1.313163e-01 1.313163e-01 +6.125000e-01 1.250000e-02 1.250000e-02 1.904000e+00 1.317598e-01 1.317598e-01 +6.375000e-01 1.250000e-02 1.250000e-02 1.732000e+00 1.417038e-01 1.417038e-01 +6.625000e-01 1.250000e-02 1.250000e-02 1.571000e+00 1.305245e-01 1.305245e-01 +6.875000e-01 1.250000e-02 1.250000e-02 1.521000e+00 1.281559e-01 1.281559e-01 +7.125000e-01 1.250000e-02 1.250000e-02 1.405000e+00 1.752052e-01 1.752052e-01 +7.375000e-01 1.250000e-02 1.250000e-02 1.392000e+00 1.466678e-01 1.466678e-01 +7.625000e-01 1.250000e-02 1.250000e-02 1.379000e+00 1.926398e-01 1.926398e-01 +7.875000e-01 1.250000e-02 1.250000e-02 1.200000e+00 1.652974e-01 1.652974e-01 +8.500000e-01 5.000000e-02 5.000000e-02 9.170000e-01 7.938985e-02 7.938985e-02 +9.500000e-01 5.000000e-02 5.000000e-02 9.570000e-01 8.592332e-02 8.592332e-02 +1.050000e+00 5.000000e-02 5.000000e-02 6.590000e-01 1.214806e-01 1.214806e-01 +1.150000e+00 5.000000e-02 5.000000e-02 4.030000e-01 1.132460e-01 1.132460e-01 +1.250000e+00 5.000000e-02 5.000000e-02 5.720000e-01 1.667621e-01 1.667621e-01 +1.350000e+00 5.000000e-02 5.000000e-02 5.350000e-01 1.052456e-01 1.052456e-01 +1.450000e+00 5.000000e-02 5.000000e-02 2.080000e-01 1.119698e-01 1.119698e-01 +1.550000e+00 5.000000e-02 5.000000e-02 3.120000e-01 7.915035e-02 7.915035e-02 +1.650000e+00 5.000000e-02 5.000000e-02 1.600000e-01 5.916162e-02 5.916162e-02 +1.750000e+00 5.000000e-02 5.000000e-02 1.240000e-01 5.457894e-02 5.457894e-02 +1.850000e+00 5.000000e-02 5.000000e-02 1.300000e-02 5.325430e-02 5.325430e-02 +1.950000e+00 5.000000e-02 5.000000e-02 6.500000e-02 4.052791e-02 4.052791e-02 +2.050000e+00 5.000000e-02 5.000000e-02 -6.200000e-02 4.429972e-02 4.429972e-02 +2.150000e+00 5.000000e-02 5.000000e-02 -2.600000e-02 3.832860e-02 3.832860e-02 +2.250000e+00 5.000000e-02 5.000000e-02 2.400000e-02 4.420486e-02 4.420486e-02 +2.350000e+00 5.000000e-02 5.000000e-02 -2.100000e-02 4.022503e-02 4.022503e-02 +2.450000e+00 5.000000e-02 5.000000e-02 1.400000e-02 4.272030e-02 4.272030e-02 +2.550000e+00 5.000000e-02 5.000000e-02 -3.200000e-02 4.022591e-02 4.022591e-02 +2.650000e+00 5.000000e-02 5.000000e-02 4.000000e-02 3.573785e-02 3.573785e-02 +2.750000e+00 5.000000e-02 5.000000e-02 4.600000e-02 4.304946e-02 4.304946e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d04-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.025, up: 0.025}, sys: {dn: -0.012, up: 0.012}}, 1: {stat: {dn: -0.032, up: 0.032}, sys: {dn: -0.002, up: 0.002}}, 2: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.005, up: 0.005}}, 3: {stat: {dn: -0.035, up: 0.035}, sys: {dn: -0.008, up: 0.008}}, 4: {stat: {dn: -0.034, up: 0.034}, sys: {dn: -0.01, up: 0.01}}, 5: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.011, up: 0.011}}, 6: {stat: {dn: -0.031, up: 0.031}, sys: {dn: -0.001, up: 0.001}}, 7: {stat: {dn: -0.031, up: 0.031}, sys: {dn: -0.009, up: 0.009}}, 8: {stat: {dn: -0.03, up: 0.03}, sys: {dn: -0.003, up: 0.003}}, 9: {stat: {dn: -0.022, up: 0.022}, sys: {dn: -0.019, up: 0.019}}, 10: {stat: {dn: -0.022, up: 0.022}, sys: {dn: -0.029, up: 0.029}}, 11: {stat: {dn: -0.023, up: 0.023}, sys: {dn: -0.013, up: 0.013}}, 12: {stat: {dn: -0.025, up: 0.025}, sys: {dn: -0.014, up: 0.014}}, 13: {stat: {dn: -0.027, up: 0.027}, sys: {dn: -0.013, up: 0.013}}, 14: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.014, up: 0.014}}, 15: {stat: {dn: -0.032, up: 0.032}, sys: {dn: -0.016, up: 0.016}}, 16: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.027, up: 0.027}}, 17: {stat: {dn: -0.038, up: 0.038}, sys: {dn: -0.015, up: 0.015}}, 18: {stat: {dn: -0.038, up: 0.038}, sys: {dn: -0.025, up: 0.025}}} + +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d04-x01-y01 +Title: doi:10.17182/hepdata.14424.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.500000e-01 5.000000e-02 5.000000e-02 1.170000e-01 2.773085e-02 2.773085e-02 +4.500000e-01 5.000000e-02 5.000000e-02 1.150000e-01 3.206244e-02 3.206244e-02 +5.500000e-01 5.000000e-02 5.000000e-02 2.010000e-01 3.337664e-02 3.337664e-02 +6.500000e-01 5.000000e-02 5.000000e-02 1.200000e-01 3.590265e-02 3.590265e-02 +7.500000e-01 5.000000e-02 5.000000e-02 1.250000e-01 3.544009e-02 3.544009e-02 +8.500000e-01 5.000000e-02 5.000000e-02 8.800000e-02 3.478505e-02 3.478505e-02 +9.500000e-01 5.000000e-02 5.000000e-02 1.120000e-01 3.101612e-02 3.101612e-02 +1.050000e+00 5.000000e-02 5.000000e-02 5.400000e-02 3.228002e-02 3.228002e-02 +1.150000e+00 5.000000e-02 5.000000e-02 6.000000e-02 3.014963e-02 3.014963e-02 +1.250000e+00 5.000000e-02 5.000000e-02 -1.200000e-02 2.906888e-02 2.906888e-02 +1.350000e+00 5.000000e-02 5.000000e-02 1.000000e-02 3.640055e-02 3.640055e-02 +1.450000e+00 5.000000e-02 5.000000e-02 -2.100000e-02 2.641969e-02 2.641969e-02 +1.550000e+00 5.000000e-02 5.000000e-02 -2.100000e-02 2.865310e-02 2.865310e-02 +1.650000e+00 5.000000e-02 5.000000e-02 -1.100000e-02 2.996665e-02 2.996665e-02 +1.750000e+00 5.000000e-02 5.000000e-02 -1.600000e-02 3.220248e-02 3.220248e-02 +1.850000e+00 5.000000e-02 5.000000e-02 3.400000e-02 3.577709e-02 3.577709e-02 +1.950000e+00 5.000000e-02 5.000000e-02 -2.000000e-02 4.263801e-02 4.263801e-02 +2.050000e+00 5.000000e-02 5.000000e-02 3.100000e-02 4.085340e-02 4.085340e-02 +2.150000e+00 5.000000e-02 5.000000e-02 -3.000000e-03 4.548626e-02 4.548626e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d05-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.025, up: 0.025}, sys: {dn: -0.017, up: 0.017}}, 1: {stat: {dn: -0.032, up: 0.032}, sys: {dn: -0.003, up: 0.003}}, 2: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.007, up: 0.007}}, 3: {stat: {dn: -0.035, up: 0.035}, sys: {dn: -0.013, up: 0.013}}, 4: {stat: {dn: -0.034, up: 0.034}, sys: {dn: -0.013, up: 0.013}}, 5: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.016, up: 0.016}}, 6: {stat: {dn: -0.031, up: 0.031}, sys: {dn: -0.001, up: 0.001}}, 7: {stat: {dn: -0.031, up: 0.031}, sys: {dn: -0.012, up: 0.012}}, 8: {stat: {dn: -0.03, up: 0.03}, sys: {dn: -0.003, up: 0.003}}, 9: {stat: {dn: -0.022, up: 0.022}, sys: {dn: -0.019, up: 0.019}}, 10: {stat: {dn: -0.022, up: 0.022}, sys: {dn: -0.04, up: 0.04}}, 11: {stat: {dn: -0.023, up: 0.023}, sys: {dn: -0.013, up: 0.013}}, 12: {stat: {dn: -0.025, up: 0.025}, sys: {dn: -0.014, up: 0.014}}, 13: {stat: {dn: -0.027, up: 0.027}, sys: {dn: -0.013, up: 0.013}}, 14: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.014, up: 0.014}}, 15: {stat: {dn: -0.032, up: 0.032}, sys: {dn: -0.016, up: 0.016}}, 16: {stat: {dn: -0.033, up: 0.033}, sys: {dn: -0.027, up: 0.027}}, 17: {stat: {dn: -0.038, up: 0.038}, sys: {dn: -0.015, up: 0.015}}, 18: {stat: {dn: -0.038, up: 0.038}, sys: {dn: -0.025, up: 0.025}}} + +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d05-x01-y01 +Title: doi:10.17182/hepdata.14424.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.500000e-01 5.000000e-02 5.000000e-02 1.720000e-01 3.023243e-02 3.023243e-02 +4.500000e-01 5.000000e-02 5.000000e-02 1.880000e-01 3.214032e-02 3.214032e-02 +5.500000e-01 5.000000e-02 5.000000e-02 2.740000e-01 3.373426e-02 3.373426e-02 +6.500000e-01 5.000000e-02 5.000000e-02 1.900000e-01 3.733631e-02 3.733631e-02 +7.500000e-01 5.000000e-02 5.000000e-02 1.750000e-01 3.640055e-02 3.640055e-02 +8.500000e-01 5.000000e-02 5.000000e-02 1.240000e-01 3.667424e-02 3.667424e-02 +9.500000e-01 5.000000e-02 5.000000e-02 1.360000e-01 3.101612e-02 3.101612e-02 +1.050000e+00 5.000000e-02 5.000000e-02 7.700000e-02 3.324154e-02 3.324154e-02 +1.150000e+00 5.000000e-02 5.000000e-02 7.200000e-02 3.014963e-02 3.014963e-02 +1.250000e+00 5.000000e-02 5.000000e-02 -4.000000e-03 2.906888e-02 2.906888e-02 +1.350000e+00 5.000000e-02 5.000000e-02 1.400000e-02 4.565085e-02 4.565085e-02 +1.450000e+00 5.000000e-02 5.000000e-02 -1.800000e-02 2.641969e-02 2.641969e-02 +1.550000e+00 5.000000e-02 5.000000e-02 -2.000000e-02 2.865310e-02 2.865310e-02 +1.650000e+00 5.000000e-02 5.000000e-02 -1.000000e-02 2.996665e-02 2.996665e-02 +1.750000e+00 5.000000e-02 5.000000e-02 -1.600000e-02 3.220248e-02 3.220248e-02 +1.850000e+00 5.000000e-02 5.000000e-02 3.400000e-02 3.577709e-02 3.577709e-02 +1.950000e+00 5.000000e-02 5.000000e-02 -2.000000e-02 4.263801e-02 4.263801e-02 +2.050000e+00 5.000000e-02 5.000000e-02 3.100000e-02 4.085340e-02 4.085340e-02 +2.150000e+00 5.000000e-02 5.000000e-02 -3.000000e-03 4.548626e-02 4.548626e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d06-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.13, up: 0.13}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.17060999999999998, up: 0.17060999999999998}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.01331, up: 0.01331}}, 1: {stat: {dn: -0.12, up: 0.12}, sys: {dn: -0.17, up: 0.17}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.24111, up: 0.24111}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.018810000000000004, up: 0.018810000000000004}}, 2: {stat: {dn: -0.15, up: 0.15}, sys: {dn: -0.17, up: 0.17}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.24675000000000002, up: 0.24675000000000002}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.019250000000000003, up: 0.019250000000000003}}, 3: {stat: {dn: -0.18, up: 0.18}, sys: {dn: -0.2, up: 0.2}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.28340999999999994, up: 0.28340999999999994}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.022109999999999998, up: 0.022109999999999998}}, 4: {stat: {dn: -0.18, up: 0.18}, sys: {dn: -0.14, up: 0.14}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.20445, up: 0.20445}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.01595, up: 0.01595}}, 5: {stat: {dn: -0.18, up: 0.18}, sys: {dn: -0.12, up: 0.12}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.1692, up: 0.1692}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.013200000000000002, up: 0.013200000000000002}}, 6: {stat: {dn: -0.18, up: 0.18}, sys: {dn: -0.09, up: 0.09}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.13818, up: 0.13818}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.010780000000000001, up: 0.010780000000000001}}, 7: {stat: {dn: -0.2, up: 0.2}, sys: {dn: -0.09, up: 0.09}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.13677, up: 0.13677}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.01067, up: 0.01067}}, 8: {stat: {dn: -0.17, up: 0.17}, sys: {dn: -0.06, up: 0.06}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.09024, up: 0.09024}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.007040000000000001, up: 0.007040000000000001}}, 9: {stat: {dn: -0.17, up: 0.17}, sys: {dn: -0.06, up: 0.06}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.01833, up: 0.01833}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00143, up: 0.00143}}, 10: {stat: {dn: -0.16, up: 0.16}, sys: {dn: -0.05, up: 0.05}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.07896000000000002, up: 0.07896000000000002}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.006160000000000001, up: 0.006160000000000001}}, 11: {stat: {dn: -0.17, up: 0.17}, sys: {dn: -0.03, up: 0.03}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.03243, up: 0.03243}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00253, up: 0.00253}}, 12: {stat: {dn: -0.13, up: 0.13}, sys: {dn: -0.02, up: 0.02}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.01269, up: 0.01269}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00099, up: 0.00099}}, 13: {stat: {dn: -0.15, up: 0.15}, sys: {dn: -0.02, up: 0.02}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.02115, up: 0.02115}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0016500000000000002, up: 0.0016500000000000002}}, 14: {stat: {dn: -0.13, up: 0.13}, sys: {dn: -0.01, up: 0.01}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.01269, up: 0.01269}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00099, up: 0.00099}}, 15: {stat: {dn: -0.17, up: 0.17}, sys: {dn: -0.03, up: 0.03}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: 0.015510000000000001, up: -0.015510000000000001}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.0012100000000000001, up: -0.0012100000000000001}}, 16: {stat: {dn: -0.15, up: 0.15}, sys: {dn: -0.02, up: 0.02}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.00141, up: 0.00141}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00011000000000000002, up: 0.00011000000000000002}}, 17: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.01, up: 0.01}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: 0.009870000000000002, up: -0.009870000000000002}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.0007700000000000002, up: -0.0007700000000000002}}, 18: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.01, up: 0.01}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: 0.004229999999999999, up: -0.004229999999999999}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.00033, up: -0.00033}}, 19: {stat: {dn: -0.19, up: 0.19}, sys: {dn: -0.02, up: 0.02}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.026789999999999998, up: 0.026789999999999998}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0020900000000000003, up: 0.0020900000000000003}}, 20: {stat: {dn: -0.29, up: 0.29}, sys: {dn: -0.04, up: 0.04}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.03807, up: 0.03807}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0029700000000000004, up: 0.0029700000000000004}}, 21: {stat: {dn: -0.19, up: 0.19}, sys: {dn: -0.01, up: 0.01}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.02115, up: 0.02115}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.0016500000000000002, up: 0.0016500000000000002}}, 22: {stat: {dn: -0.16, up: 0.16}, sys: {dn: -0.01, up: 0.01}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: 0.015510000000000001, up: -0.015510000000000001}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.0012100000000000001, up: -0.0012100000000000001}}, 23: {stat: {dn: -0.14, up: 0.14}, sys: {dn: -0.01, up: 0.01}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: 0.008459999999999999, up: -0.008459999999999999}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: 0.00066, up: -0.00066}}, 24: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.0, up: 0.0}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.00564, up: 0.00564}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00044000000000000007, up: 0.00044000000000000007}}, 25: {stat: {dn: -0.04, up: 0.04}, sys: {dn: -0.02, up: 0.02}, ? 'sys,Additional scale uncertainty in inclusive kaon spectra determined from kaon decays in-flight. Only decays into one charged plus neutral particles was taken into accountDECAY-BR(BRN=K+ --> CHARGED+ NEUTRAL (NEUTRALS),BRV=94.4 PCT,C=RPP-92)' : {dn: -0.00282, up: 0.00282}, 'sys,Additional scale uncertainty in inclusive kaon spectrum determined from particle identification.': {dn: -0.00022000000000000003, up: 0.00022000000000000003}}} + +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d06-x01-y01 +Title: doi:10.17182/hepdata.14424.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-01 5.000000e-02 5.000000e-02 1.210000e+00 2.329913e-01 2.329913e-01 +3.500000e-01 5.000000e-02 5.000000e-02 1.710000e+00 3.190421e-01 3.190421e-01 +4.500000e-01 5.000000e-02 5.000000e-02 1.750000e+00 3.356429e-01 3.356429e-01 +5.500000e-01 5.000000e-02 5.000000e-02 2.010000e+00 3.914206e-01 3.914206e-01 +6.500000e-01 5.000000e-02 5.000000e-02 1.450000e+00 3.066826e-01 3.066826e-01 +7.500000e-01 5.000000e-02 5.000000e-02 1.200000e+00 2.749598e-01 2.749598e-01 +8.500000e-01 5.000000e-02 5.000000e-02 9.800000e-01 2.443561e-01 2.443561e-01 +9.500000e-01 5.000000e-02 5.000000e-02 9.700000e-01 2.586888e-01 2.586888e-01 +1.050000e+00 5.000000e-02 5.000000e-02 6.400000e-01 2.017246e-01 2.017246e-01 +1.150000e+00 5.000000e-02 5.000000e-02 1.300000e-01 1.812127e-01 1.812127e-01 +1.250000e+00 5.000000e-02 5.000000e-02 5.600000e-01 1.853986e-01 1.853986e-01 +1.350000e+00 5.000000e-02 5.000000e-02 2.300000e-01 1.756648e-01 1.756648e-01 +1.450000e+00 5.000000e-02 5.000000e-02 9.000000e-02 1.321439e-01 1.321439e-01 +1.550000e+00 5.000000e-02 5.000000e-02 1.500000e-01 1.528072e-01 1.528072e-01 +1.650000e+00 5.000000e-02 5.000000e-02 9.000000e-02 1.310039e-01 1.310039e-01 +1.750000e+00 5.000000e-02 5.000000e-02 -1.100000e-01 1.733264e-01 1.733264e-01 +1.850000e+00 5.000000e-02 5.000000e-02 1.000000e-02 1.513341e-01 1.513341e-01 +1.950000e+00 5.000000e-02 5.000000e-02 -7.000000e-02 9.109341e-02 9.109341e-02 +2.050000e+00 5.000000e-02 5.000000e-02 -3.000000e-02 9.065320e-02 9.065320e-02 +2.150000e+00 5.000000e-02 5.000000e-02 1.900000e-01 1.929302e-01 1.929302e-01 +2.250000e+00 5.000000e-02 5.000000e-02 2.700000e-01 2.952256e-01 2.952256e-01 +2.350000e+00 5.000000e-02 5.000000e-02 1.500000e-01 1.914420e-01 1.914420e-01 +2.450000e+00 5.000000e-02 5.000000e-02 -1.100000e-01 1.610653e-01 1.610653e-01 +2.550000e+00 5.000000e-02 5.000000e-02 -6.000000e-02 1.406130e-01 1.406130e-01 +2.650000e+00 5.000000e-02 5.000000e-02 4.000000e-02 9.017762e-02 9.017762e-02 +2.750000e+00 5.000000e-02 5.000000e-02 2.000000e-02 4.481072e-02 4.481072e-02 +END YODA_SCATTER2D_V2 + +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d07-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d07-x01-y01 +Title: ~ +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 5.000000e-01 5.000000e-01 7.170000e+00 1.486607e-01 1.486607e-01 +END YODA_SCATTER2D_V2 + +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d08-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d08-x01-y01 +Title: ~ +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 5.000000e-01 5.000000e-01 8.210000e+00 1.676305e-01 1.676305e-01 +END YODA_SCATTER2D_V2 + +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d09-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d09-x01-y01 +Title: ~ +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 5.000000e-01 5.000000e-01 1.550000e+00 5.830952e-02 5.830952e-02 +END YODA_SCATTER2D_V2 + +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d10-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d10-x01-y01 +Title: ~ +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 5.000000e-01 5.000000e-01 1.100000e-01 1.220656e-02 1.220656e-02 +END YODA_SCATTER2D_V2 + +BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d11-x01-y01 +IsRef: 1 +Path: /REF/ARGUS_1993_S2653028/d11-x01-y01 +Title: ~ +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.058000e+01 5.000000e-01 5.000000e-01 1.600000e-01 1.414214e-02 1.414214e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginDORIS/ARGUS_1993_S2669951.cc b/analyses/pluginDORIS/ARGUS_1993_S2669951.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/ARGUS_1993_S2669951.cc @@ -0,0 +1,191 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Production of the $\eta'(958)$ and $f_0(980)$ in $e^+e^-$ annihilation in the Upsilon region + /// @author Peter Richardson + class ARGUS_1993_S2669951 : public Analysis { + public: + + ARGUS_1993_S2669951() + : Analysis("ARGUS_1993_S2669951"), + _count_etaPrime_highZ(2, 0.), + _count_etaPrime_allZ(3, 0.), + _count_f0(3, 0.), + _weightSum_cont(0.), + _weightSum_Ups1(0.), + _weightSum_Ups2(0.) + { } + + + void init() { + declare(UnstableParticles(), "UFS"); + + _hist_cont_f0 = bookHisto1D(2, 1, 1); + _hist_Ups1_f0 = bookHisto1D(3, 1, 1); + _hist_Ups2_f0 = bookHisto1D(4, 1, 1); + } + + + void analyze(const Event& e) { + + // Find the Upsilons among the unstables + const UnstableParticles& ufs = apply(e, "UFS"); + Particles upsilons; + + // First in unstable final state + foreach (const Particle& p, ufs.particles()) + if (p.pid() == 553 || p.pid() == 100553) + upsilons.push_back(p); + // Then in whole event if fails + if (upsilons.empty()) { + /// @todo Replace HepMC digging with Particle::descendents etc. calls + for(ConstGenParticlePtr p: HepMCUtils::particles(e.genEvent())) { + if ( p->pdg_id() != 553 && p->pdg_id() != 100553 ) continue; + // Discard it if its parent has the same PDG ID code (avoid duplicates) + ConstGenVertexPtr pv = p->production_vertex(); + bool passed = true; + if (pv) { + for(ConstGenParticlePtr pp: HepMCUtils::particles(pv, Relatives::PARENTS)){ + if ( p->pdg_id() == pp->pdg_id() ) { + passed = false; + break; + } + } + } + if (passed) upsilons.push_back(Particle(*p)); + } + } + + + // Finding done, now fill counters + const double weight = e.weight(); + if (upsilons.empty()) { // Continuum + MSG_DEBUG("No Upsilons found => continuum event"); + + _weightSum_cont += weight; + unsigned int nEtaA(0), nEtaB(0), nf0(0); + foreach (const Particle& p, ufs.particles()) { + const int id = p.abspid(); + const double xp = 2.*p.E()/sqrtS(); + const double beta = p.p3().mod() / p.E(); + if (id == 9010221) { + _hist_cont_f0->fill(xp, weight/beta); + nf0 += 1; + } else if (id == 331) { + if (xp > 0.35) nEtaA += 1; + nEtaB += 1; + } + } + _count_f0[2] += nf0*weight; + _count_etaPrime_highZ[1] += nEtaA*weight; + _count_etaPrime_allZ[2] += nEtaB*weight; + + } else { // Upsilon(s) found + MSG_DEBUG("Upsilons found => resonance event"); + + foreach (const Particle& ups, upsilons) { + const int parentId = ups.pid(); + ((parentId == 553) ? _weightSum_Ups1 : _weightSum_Ups2) += weight; + Particles unstable; + // Find the decay products we want + findDecayProducts(ups.genParticle(), unstable); + LorentzTransform cms_boost; + if (ups.p3().mod() > 1*MeV) + cms_boost = LorentzTransform::mkFrameTransformFromBeta(ups.momentum().betaVec()); + const double mass = ups.mass(); + unsigned int nEtaA(0), nEtaB(0), nf0(0); + foreach(const Particle& p, unstable) { + const int id = p.abspid(); + const FourMomentum p2 = cms_boost.transform(p.momentum()); + const double xp = 2.*p2.E()/mass; + const double beta = p2.p3().mod()/p2.E(); + if (id == 9010221) { //< ? + ((parentId == 553) ? _hist_Ups1_f0 : _hist_Ups2_f0)->fill(xp, weight/beta); + nf0 += 1; + } else if (id == 331) { //< ? + if (xp > 0.35) nEtaA += 1; + nEtaB += 1; + } + } + if (parentId == 553) { + _count_f0[0] += nf0*weight; + _count_etaPrime_highZ[0] += nEtaA*weight; + _count_etaPrime_allZ[0] += nEtaB*weight; + } else { + _count_f0[1] += nf0*weight; + _count_etaPrime_allZ[1] += nEtaB*weight; + } + } + } + } + + + void finalize() { + + // High-Z eta' multiplicity + Scatter2DPtr s111 = bookScatter2D(1, 1, 1, true); + if (_weightSum_Ups1 > 0) // Point at 9.460 + s111->point(0).setY(_count_etaPrime_highZ[0] / _weightSum_Ups1, 0); + if (_weightSum_cont > 0) // Point at 9.905 + s111->point(1).setY(_count_etaPrime_highZ[1] / _weightSum_cont, 0); + + // All-Z eta' multiplicity + Scatter2DPtr s112 = bookScatter2D(1, 1, 2, true); + if (_weightSum_Ups1 > 0) // Point at 9.460 + s112->point(0).setY(_count_etaPrime_allZ[0] / _weightSum_Ups1, 0); + if (_weightSum_cont > 0) // Point at 9.905 + s112->point(1).setY(_count_etaPrime_allZ[2] / _weightSum_cont, 0); + if (_weightSum_Ups2 > 0) // Point at 10.02 + s112->point(2).setY(_count_etaPrime_allZ[1] / _weightSum_Ups2, 0); + + // f0 multiplicity + Scatter2DPtr s511 = bookScatter2D(5, 1, 1, true); + if (_weightSum_Ups1 > 0) // Point at 9.46 + s511->point(0).setY(_count_f0[0] / _weightSum_Ups1, 0); + if (_weightSum_Ups2 > 0) // Point at 10.02 + s511->point(1).setY(_count_f0[1] / _weightSum_Ups2, 0); + if (_weightSum_cont > 0) // Point at 10.45 + s511->point(2).setY(_count_f0[2] / _weightSum_cont, 0); + + // Scale histos + if (_weightSum_cont > 0.) scale(_hist_cont_f0, 1./_weightSum_cont); + if (_weightSum_Ups1 > 0.) scale(_hist_Ups1_f0, 1./_weightSum_Ups1); + if (_weightSum_Ups2 > 0.) scale(_hist_Ups2_f0, 1./_weightSum_Ups2); + } + + + private: + + /// @name Counters + //@{ + vector _count_etaPrime_highZ, _count_etaPrime_allZ, _count_f0; + double _weightSum_cont,_weightSum_Ups1,_weightSum_Ups2; + //@} + + + /// Histos + Histo1DPtr _hist_cont_f0, _hist_Ups1_f0, _hist_Ups2_f0; + + + /// Recursively walk the HepMC tree to find decay products of @a p + void findDecayProducts(ConstGenParticlePtr p, Particles& unstable) { + ConstGenVertexPtr dv = p->end_vertex(); + for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ + const int id = abs(pp->pdg_id()); + if (id == 331 || id == 9010221) unstable.push_back(Particle(pp)); + else if (pp->end_vertex()) findDecayProducts(pp, unstable); + } + } + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(ARGUS_1993_S2669951); + +} diff --git a/analyses/pluginMisc/ARGUS_1993_S2669951.info b/analyses/pluginDORIS/ARGUS_1993_S2669951.info rename from analyses/pluginMisc/ARGUS_1993_S2669951.info rename to analyses/pluginDORIS/ARGUS_1993_S2669951.info diff --git a/analyses/pluginMisc/ARGUS_1993_S2669951.plot b/analyses/pluginDORIS/ARGUS_1993_S2669951.plot rename from analyses/pluginMisc/ARGUS_1993_S2669951.plot rename to analyses/pluginDORIS/ARGUS_1993_S2669951.plot diff --git a/analyses/pluginMisc/ARGUS_1993_S2669951.yoda b/analyses/pluginDORIS/ARGUS_1993_S2669951.yoda rename from analyses/pluginMisc/ARGUS_1993_S2669951.yoda rename to analyses/pluginDORIS/ARGUS_1993_S2669951.yoda diff --git a/analyses/pluginDORIS/ARGUS_1993_S2789213.cc b/analyses/pluginDORIS/ARGUS_1993_S2789213.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/ARGUS_1993_S2789213.cc @@ -0,0 +1,256 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief ARGUS vector meson production + /// @author Peter Richardson + class ARGUS_1993_S2789213 : public Analysis { + public: + + ARGUS_1993_S2789213() + : Analysis("ARGUS_1993_S2789213"), + _weightSum_cont(0.),_weightSum_Ups1(0.),_weightSum_Ups4(0.) + { } + + + void init() { + declare(UnstableParticles(), "UFS"); + + _mult_cont_Omega = bookHisto1D( 1, 1, 1); + _mult_cont_Rho0 = bookHisto1D( 1, 1, 2); + _mult_cont_KStar0 = bookHisto1D( 1, 1, 3); + _mult_cont_KStarPlus = bookHisto1D( 1, 1, 4); + _mult_cont_Phi = bookHisto1D( 1, 1, 5); + + _mult_Ups1_Omega = bookHisto1D( 2, 1, 1); + _mult_Ups1_Rho0 = bookHisto1D( 2, 1, 2); + _mult_Ups1_KStar0 = bookHisto1D( 2, 1, 3); + _mult_Ups1_KStarPlus = bookHisto1D( 2, 1, 4); + _mult_Ups1_Phi = bookHisto1D( 2, 1, 5); + + _mult_Ups4_Omega = bookHisto1D( 3, 1, 1); + _mult_Ups4_Rho0 = bookHisto1D( 3, 1, 2); + _mult_Ups4_KStar0 = bookHisto1D( 3, 1, 3); + _mult_Ups4_KStarPlus = bookHisto1D( 3, 1, 4); + _mult_Ups4_Phi = bookHisto1D( 3, 1, 5); + + _hist_cont_KStarPlus = bookHisto1D( 4, 1, 1); + _hist_Ups1_KStarPlus = bookHisto1D( 5, 1, 1); + _hist_Ups4_KStarPlus = bookHisto1D( 6, 1, 1); + + _hist_cont_KStar0 = bookHisto1D( 7, 1, 1); + _hist_Ups1_KStar0 = bookHisto1D( 8, 1, 1); + _hist_Ups4_KStar0 = bookHisto1D( 9, 1, 1); + + _hist_cont_Rho0 = bookHisto1D(10, 1, 1); + _hist_Ups1_Rho0 = bookHisto1D(11, 1, 1); + _hist_Ups4_Rho0 = bookHisto1D(12, 1, 1); + + _hist_cont_Omega = bookHisto1D(13, 1, 1); + _hist_Ups1_Omega = bookHisto1D(14, 1, 1); + } + + + void analyze(const Event& e) { + const double weight = e.weight(); + + // Find the upsilons + Particles upsilons; + // First in unstable final state + const UnstableParticles& ufs = apply(e, "UFS"); + foreach (const Particle& p, ufs.particles()) + if (p.pid() == 300553 || p.pid() == 553) upsilons.push_back(p); + // Then in whole event if that failed + if (upsilons.empty()) { + for(ConstGenParticlePtr p: HepMCUtils::particles(e.genEvent())) { + if (p->pdg_id() != 300553 && p->pdg_id() != 553) continue; + ConstGenVertexPtr pv = p->production_vertex(); + bool passed = true; + if (pv) { + for(ConstGenParticlePtr pp: HepMCUtils::particles(pv, Relatives::PARENTS)){ + if ( p->pdg_id() == pp->pdg_id() ) { + passed = false; + break; + } + } + } + if (passed) upsilons.push_back(Particle(*p)); + } + } + + if (upsilons.empty()) { // continuum + + _weightSum_cont += weight; + unsigned int nOmega(0), nRho0(0), nKStar0(0), nKStarPlus(0), nPhi(0); + foreach (const Particle& p, ufs.particles()) { + int id = p.abspid(); + double xp = 2.*p.E()/sqrtS(); + double beta = p.p3().mod()/p.E(); + if (id == 113) { + _hist_cont_Rho0->fill(xp, weight/beta); + ++nRho0; + } + else if (id == 313) { + _hist_cont_KStar0->fill(xp, weight/beta); + ++nKStar0; + } + else if (id == 223) { + _hist_cont_Omega->fill(xp, weight/beta); + ++nOmega; + } + else if (id == 323) { + _hist_cont_KStarPlus->fill(xp,weight/beta); + ++nKStarPlus; + } + else if (id == 333) { + ++nPhi; + } + } + /// @todo Replace with Counters and fill one-point Scatters at the end + _mult_cont_Omega ->fill(10.45, weight*nOmega ); + _mult_cont_Rho0 ->fill(10.45, weight*nRho0 ); + _mult_cont_KStar0 ->fill(10.45, weight*nKStar0 ); + _mult_cont_KStarPlus->fill(10.45, weight*nKStarPlus); + _mult_cont_Phi ->fill(10.45, weight*nPhi ); + + } else { // found an upsilon + + foreach (const Particle& ups, upsilons) { + const int parentId = ups.pid(); + (parentId == 553 ? _weightSum_Ups1 : _weightSum_Ups4) += weight; + Particles unstable; + // Find the decay products we want + findDecayProducts(ups.genParticle(),unstable); + /// @todo Update to new LT mk* functions + LorentzTransform cms_boost; + if (ups.p3().mod() > 0.001) + cms_boost = LorentzTransform::mkFrameTransformFromBeta(ups.momentum().betaVec()); + double mass = ups.mass(); + unsigned int nOmega(0),nRho0(0),nKStar0(0),nKStarPlus(0),nPhi(0); + foreach(const Particle & p , unstable) { + int id = p.abspid(); + FourMomentum p2 = cms_boost.transform(p.momentum()); + double xp = 2.*p2.E()/mass; + double beta = p2.p3().mod()/p2.E(); + if (id == 113) { + if (parentId == 553) _hist_Ups1_Rho0->fill(xp,weight/beta); + else _hist_Ups4_Rho0->fill(xp,weight/beta); + ++nRho0; + } + else if (id == 313) { + if (parentId == 553) _hist_Ups1_KStar0->fill(xp,weight/beta); + else _hist_Ups4_KStar0->fill(xp,weight/beta); + ++nKStar0; + } + else if (id == 223) { + if (parentId == 553) _hist_Ups1_Omega->fill(xp,weight/beta); + ++nOmega; + } + else if (id == 323) { + if (parentId == 553) _hist_Ups1_KStarPlus->fill(xp,weight/beta); + else _hist_Ups4_KStarPlus->fill(xp,weight/beta); + ++nKStarPlus; + } + else if (id == 333) { + ++nPhi; + } + } + if (parentId == 553) { + _mult_Ups1_Omega ->fill(9.46,weight*nOmega ); + _mult_Ups1_Rho0 ->fill(9.46,weight*nRho0 ); + _mult_Ups1_KStar0 ->fill(9.46,weight*nKStar0 ); + _mult_Ups1_KStarPlus->fill(9.46,weight*nKStarPlus); + _mult_Ups1_Phi ->fill(9.46,weight*nPhi ); + } + else { + _mult_Ups4_Omega ->fill(10.58,weight*nOmega ); + _mult_Ups4_Rho0 ->fill(10.58,weight*nRho0 ); + _mult_Ups4_KStar0 ->fill(10.58,weight*nKStar0 ); + _mult_Ups4_KStarPlus->fill(10.58,weight*nKStarPlus); + _mult_Ups4_Phi ->fill(10.58,weight*nPhi ); + } + } + } + + } + + + void finalize() { + if (_weightSum_cont > 0.) { + /// @todo Replace with Counters and fill one-point Scatters at the end + scale(_mult_cont_Omega , 1./_weightSum_cont); + scale(_mult_cont_Rho0 , 1./_weightSum_cont); + scale(_mult_cont_KStar0 , 1./_weightSum_cont); + scale(_mult_cont_KStarPlus, 1./_weightSum_cont); + scale(_mult_cont_Phi , 1./_weightSum_cont); + scale(_hist_cont_KStarPlus, 1./_weightSum_cont); + scale(_hist_cont_KStar0 , 1./_weightSum_cont); + scale(_hist_cont_Rho0 , 1./_weightSum_cont); + scale(_hist_cont_Omega , 1./_weightSum_cont); + } + if (_weightSum_Ups1 > 0.) { + /// @todo Replace with Counters and fill one-point Scatters at the end + scale(_mult_Ups1_Omega , 1./_weightSum_Ups1); + scale(_mult_Ups1_Rho0 , 1./_weightSum_Ups1); + scale(_mult_Ups1_KStar0 , 1./_weightSum_Ups1); + scale(_mult_Ups1_KStarPlus, 1./_weightSum_Ups1); + scale(_mult_Ups1_Phi , 1./_weightSum_Ups1); + scale(_hist_Ups1_KStarPlus, 1./_weightSum_Ups1); + scale(_hist_Ups1_KStar0 , 1./_weightSum_Ups1); + scale(_hist_Ups1_Rho0 , 1./_weightSum_Ups1); + scale(_hist_Ups1_Omega , 1./_weightSum_Ups1); + } + if (_weightSum_Ups4 > 0.) { + /// @todo Replace with Counters and fill one-point Scatters at the end + scale(_mult_Ups4_Omega , 1./_weightSum_Ups4); + scale(_mult_Ups4_Rho0 , 1./_weightSum_Ups4); + scale(_mult_Ups4_KStar0 , 1./_weightSum_Ups4); + scale(_mult_Ups4_KStarPlus, 1./_weightSum_Ups4); + scale(_mult_Ups4_Phi , 1./_weightSum_Ups4); + scale(_hist_Ups4_KStarPlus, 1./_weightSum_Ups4); + scale(_hist_Ups4_KStar0 , 1./_weightSum_Ups4); + scale(_hist_Ups4_Rho0 , 1./_weightSum_Ups4); + } + } + + + private: + + //@{ + Histo1DPtr _mult_cont_Omega, _mult_cont_Rho0, _mult_cont_KStar0, _mult_cont_KStarPlus, _mult_cont_Phi; + Histo1DPtr _mult_Ups1_Omega, _mult_Ups1_Rho0, _mult_Ups1_KStar0, _mult_Ups1_KStarPlus, _mult_Ups1_Phi; + Histo1DPtr _mult_Ups4_Omega, _mult_Ups4_Rho0, _mult_Ups4_KStar0, _mult_Ups4_KStarPlus, _mult_Ups4_Phi; + Histo1DPtr _hist_cont_KStarPlus, _hist_Ups1_KStarPlus, _hist_Ups4_KStarPlus; + Histo1DPtr _hist_cont_KStar0, _hist_Ups1_KStar0, _hist_Ups4_KStar0 ; + Histo1DPtr _hist_cont_Rho0, _hist_Ups1_Rho0, _hist_Ups4_Rho0; + Histo1DPtr _hist_cont_Omega, _hist_Ups1_Omega; + + double _weightSum_cont,_weightSum_Ups1,_weightSum_Ups4; + //@} + + + void findDecayProducts(ConstGenParticlePtr p, Particles& unstable) { + ConstGenVertexPtr dv = p->end_vertex(); + /// @todo Use better looping + for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ + int id = abs(pp->pdg_id()); + if (id == 113 || id == 313 || id == 323 || + id == 333 || id == 223 ) { + unstable.push_back(Particle(pp)); + } + else if (pp->end_vertex()) + findDecayProducts(pp, unstable); + } + } + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(ARGUS_1993_S2789213); + +} diff --git a/analyses/pluginMisc/ARGUS_1993_S2789213.info b/analyses/pluginDORIS/ARGUS_1993_S2789213.info rename from analyses/pluginMisc/ARGUS_1993_S2789213.info rename to analyses/pluginDORIS/ARGUS_1993_S2789213.info diff --git a/analyses/pluginMisc/ARGUS_1993_S2789213.plot b/analyses/pluginDORIS/ARGUS_1993_S2789213.plot rename from analyses/pluginMisc/ARGUS_1993_S2789213.plot rename to analyses/pluginDORIS/ARGUS_1993_S2789213.plot diff --git a/analyses/pluginMisc/ARGUS_1993_S2789213.yoda b/analyses/pluginDORIS/ARGUS_1993_S2789213.yoda rename from analyses/pluginMisc/ARGUS_1993_S2789213.yoda rename to analyses/pluginDORIS/ARGUS_1993_S2789213.yoda diff --git a/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.cc b/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.cc @@ -0,0 +1,98 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CRYSTAL_BALL_1988_I261078 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CRYSTAL_BALL_1988_I261078); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CRYSTAL_BALL_1988_I261078); + + +} diff --git a/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.info b/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.info new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.info @@ -0,0 +1,35 @@ +Name: CRYSTAL_BALL_1988_I261078 +Year: 1988 +Summary: Measurement of $R$ for energies between 9.39 GeV +Experiment: CRYSTAL_BALL +Collider: DORIS +InspireID: 261078 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B234 (1990) 525-533, 1990 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by the Crystal Ball experiment + for 9.39 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Jakubowski:1988cd +BibTeX: '@article{Jakubowski:1988cd, + author = "Jakubowski, Z. and others", + title = "{Determination of $\gamma (e e$) of the $\Upsilon$ (1s) + and $\Upsilon$ (2s) Resonances and Measurement of R at + $W=9$.39-{GeV}}", + collaboration = "Crystal Ball", + journal = "Z. Phys.", + volume = "C40", + year = "1988", + pages = "49", + doi = "10.1007/BF01559717", + reportNumber = "SLAC-PUB-4567, DESY-88-032", + SLACcitation = "%%CITATION = ZEPYA,C40,49;%%" +}' diff --git a/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.plot b/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.plot @@ -0,0 +1,27 @@ +BEGIN PLOT /CRYSTAL_BALL_1988_I261078/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +XMin=9. +XMax=10. +END PLOT +BEGIN PLOT /CRYSTAL_BALL_1988_I261078/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=9. +XMax=10. +END PLOT +BEGIN PLOT /CRYSTAL_BALL_1988_I261078/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +XMin=9. +XMax=10. +END PLOT \ No newline at end of file diff --git a/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.yoda b/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/CRYSTAL_BALL_1988_I261078.yoda @@ -0,0 +1,9 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CRYSTAL_BALL_1988_I261078/d01-x01-y01 +IsRef: 1 +Path: /REF/CRYSTAL_BALL_1988_I261078/d01-x01-y01 +Title: doi:10.17182/hepdata.15560.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.390000e+00 0.000000e+00 0.000000e+00 3.480000e+00 4.000000e-02 4.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginDORIS/DASP_1978_I129715.cc b/analyses/pluginDORIS/DASP_1978_I129715.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DASP_1978_I129715.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DASP_1978_I129715 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DASP_1978_I129715); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DASP_1978_I129715); + + +} diff --git a/analyses/pluginDORIS/DASP_1978_I129715.info b/analyses/pluginDORIS/DASP_1978_I129715.info new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DASP_1978_I129715.info @@ -0,0 +1,34 @@ +Name: DASP_1978_I129715 +Year: 1978 +Summary: Measurement of $R$ for energies between 3.603 and 5.195 GeV +Experiment: DASP +Collider: DORIS +InspireID: 129715 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D76 (2007) 072008, 2007 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by DASP for energies between 3.603 and 5.195 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Brandelik:1978ei +BibTeX: '@article{Brandelik:1978ei, + author = "Brandelik, R. and others", + title = "{Total Cross-section for Hadron Production by $e^+ e^-$ + Annihilation at Center-of-mass Energies Between 3.6-{GeV} + and 5.2-{GeV}}", + collaboration = "DASP", + journal = "Phys. Lett.", + volume = "76B", + year = "1978", + pages = "361", + doi = "10.1016/0370-2693(78)90807-9", + reportNumber = "DESY-78-18", + SLACcitation = "%%CITATION = PHLTA,76B,361;%%" +}' diff --git a/analyses/pluginDORIS/DASP_1978_I129715.plot b/analyses/pluginDORIS/DASP_1978_I129715.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DASP_1978_I129715.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /DASP_1978_I129715/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DASP_1978_I129715/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DASP_1978_I129715/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginDORIS/DASP_1978_I129715.yoda b/analyses/pluginDORIS/DASP_1978_I129715.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DASP_1978_I129715.yoda @@ -0,0 +1,160 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DASP_1978_I129715/d01-x01-y01 +IsRef: 1 +Path: /REF/DASP_1978_I129715/d01-x01-y01 +Title: doi:10.17182/hepdata.27431.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.602500e+00 0.000000e+00 0.000000e+00 2.304600e+00 3.497066e-01 3.497066e-01 +3.612500e+00 0.000000e+00 0.000000e+00 2.267000e+00 4.029328e-01 4.029328e-01 +3.625000e+00 0.000000e+00 0.000000e+00 2.110400e+00 3.390079e-01 3.390079e-01 +3.650000e+00 0.000000e+00 0.000000e+00 2.390300e+00 3.740734e-01 3.740734e-01 +3.845000e+00 0.000000e+00 0.000000e+00 2.661200e+00 4.661136e-01 4.661136e-01 +3.885000e+00 0.000000e+00 0.000000e+00 2.462100e+00 4.855614e-01 4.855614e-01 +3.930000e+00 0.000000e+00 0.000000e+00 2.682900e+00 5.787717e-01 5.787717e-01 +3.950000e+00 0.000000e+00 0.000000e+00 3.533500e+00 6.994741e-01 6.994741e-01 +3.977500e+00 0.000000e+00 0.000000e+00 2.938200e+00 5.388981e-01 5.388981e-01 +4.000000e+00 0.000000e+00 0.000000e+00 3.618600e+00 5.750504e-01 5.750504e-01 +4.010000e+00 0.000000e+00 0.000000e+00 3.833100e+00 5.967988e-01 5.967988e-01 +4.020000e+00 0.000000e+00 0.000000e+00 4.251700e+00 6.468016e-01 6.468016e-01 +4.030000e+00 0.000000e+00 0.000000e+00 4.928200e+00 7.436610e-01 7.436610e-01 +4.040000e+00 0.000000e+00 0.000000e+00 4.425300e+00 6.857546e-01 6.857546e-01 +4.050000e+00 0.000000e+00 0.000000e+00 4.452300e+00 7.008951e-01 7.008951e-01 +4.060000e+00 0.000000e+00 0.000000e+00 4.176700e+00 6.630182e-01 6.630182e-01 +4.070000e+00 0.000000e+00 0.000000e+00 3.917600e+00 6.297298e-01 6.297298e-01 +4.080000e+00 0.000000e+00 0.000000e+00 3.981900e+00 6.439648e-01 6.439648e-01 +4.090000e+00 0.000000e+00 0.000000e+00 3.643200e+00 5.855085e-01 5.855085e-01 +4.100000e+00 0.000000e+00 0.000000e+00 3.334600e+00 5.362847e-01 5.362847e-01 +4.110000e+00 0.000000e+00 0.000000e+00 3.619900e+00 5.759012e-01 5.759012e-01 +4.120000e+00 0.000000e+00 0.000000e+00 3.480000e+00 6.173867e-01 6.173867e-01 +4.130000e+00 0.000000e+00 0.000000e+00 3.809100e+00 7.154238e-01 7.154238e-01 +4.140000e+00 0.000000e+00 0.000000e+00 4.387000e+00 7.224673e-01 7.224673e-01 +4.155000e+00 0.000000e+00 0.000000e+00 4.606300e+00 7.339557e-01 7.339557e-01 +4.170000e+00 0.000000e+00 0.000000e+00 4.219600e+00 6.408754e-01 6.408754e-01 +4.180000e+00 0.000000e+00 0.000000e+00 4.485100e+00 8.055911e-01 8.055911e-01 +4.192500e+00 0.000000e+00 0.000000e+00 3.818200e+00 5.847797e-01 5.847797e-01 +4.212500e+00 0.000000e+00 0.000000e+00 3.953400e+00 6.488722e-01 6.488722e-01 +4.230000e+00 0.000000e+00 0.000000e+00 3.348100e+00 7.124666e-01 7.124666e-01 +4.240000e+00 0.000000e+00 0.000000e+00 3.103500e+00 5.452899e-01 5.452899e-01 +4.255000e+00 0.000000e+00 0.000000e+00 3.125700e+00 4.728908e-01 4.728908e-01 +4.282500e+00 0.000000e+00 0.000000e+00 3.342700e+00 5.567460e-01 5.567460e-01 +4.305000e+00 0.000000e+00 0.000000e+00 3.769600e+00 6.826685e-01 6.826685e-01 +4.315000e+00 0.000000e+00 0.000000e+00 3.538400e+00 6.544430e-01 6.544430e-01 +4.325000e+00 0.000000e+00 0.000000e+00 3.552300e+00 6.395802e-01 6.395802e-01 +4.335000e+00 0.000000e+00 0.000000e+00 3.587400e+00 5.914748e-01 5.914748e-01 +4.345000e+00 0.000000e+00 0.000000e+00 3.390100e+00 6.543634e-01 6.543634e-01 +4.355000e+00 0.000000e+00 0.000000e+00 4.253600e+00 6.914872e-01 6.914872e-01 +4.365000e+00 0.000000e+00 0.000000e+00 3.799900e+00 6.489467e-01 6.489467e-01 +4.375000e+00 0.000000e+00 0.000000e+00 4.111400e+00 6.657830e-01 6.657830e-01 +4.387500e+00 0.000000e+00 0.000000e+00 4.145900e+00 6.713603e-01 6.713603e-01 +4.400000e+00 0.000000e+00 0.000000e+00 4.635400e+00 6.973134e-01 6.973134e-01 +4.410000e+00 0.000000e+00 0.000000e+00 4.756700e+00 7.191076e-01 7.191076e-01 +4.420000e+00 0.000000e+00 0.000000e+00 4.787900e+00 7.290438e-01 7.290438e-01 +4.430000e+00 0.000000e+00 0.000000e+00 4.522700e+00 7.168260e-01 7.168260e-01 +4.440000e+00 0.000000e+00 0.000000e+00 4.723400e+00 7.727445e-01 7.727445e-01 +4.450000e+00 0.000000e+00 0.000000e+00 4.267200e+00 7.599013e-01 7.599013e-01 +4.460000e+00 0.000000e+00 0.000000e+00 4.189200e+00 6.821046e-01 6.821046e-01 +4.472500e+00 0.000000e+00 0.000000e+00 3.803000e+00 5.863775e-01 5.863775e-01 +4.490000e+00 0.000000e+00 0.000000e+00 4.376500e+00 6.901161e-01 6.901161e-01 +4.505000e+00 0.000000e+00 0.000000e+00 3.990100e+00 6.806328e-01 6.806328e-01 +4.515000e+00 0.000000e+00 0.000000e+00 3.839600e+00 6.329276e-01 6.329276e-01 +4.525000e+00 0.000000e+00 0.000000e+00 3.517600e+00 6.175344e-01 6.175344e-01 +4.535000e+00 0.000000e+00 0.000000e+00 4.145900e+00 7.429174e-01 7.429174e-01 +4.545000e+00 0.000000e+00 0.000000e+00 4.372700e+00 7.546157e-01 7.546157e-01 +4.555000e+00 0.000000e+00 0.000000e+00 4.196300e+00 6.768878e-01 6.768878e-01 +4.565000e+00 0.000000e+00 0.000000e+00 4.198000e+00 7.411171e-01 7.411171e-01 +4.575000e+00 0.000000e+00 0.000000e+00 4.311900e+00 7.665167e-01 7.665167e-01 +4.590000e+00 0.000000e+00 0.000000e+00 4.330800e+00 7.004268e-01 7.004268e-01 +4.605000e+00 0.000000e+00 0.000000e+00 4.137200e+00 7.454009e-01 7.454009e-01 +4.620000e+00 0.000000e+00 0.000000e+00 4.143100e+00 7.356808e-01 7.356808e-01 +4.635000e+00 0.000000e+00 0.000000e+00 4.974600e+00 8.110856e-01 8.110856e-01 +4.645000e+00 0.000000e+00 0.000000e+00 4.066900e+00 7.406027e-01 7.406027e-01 +4.660000e+00 0.000000e+00 0.000000e+00 4.027300e+00 7.325073e-01 7.325073e-01 +4.675000e+00 0.000000e+00 0.000000e+00 4.104400e+00 6.975542e-01 6.975542e-01 +4.690000e+00 0.000000e+00 0.000000e+00 4.288200e+00 7.524289e-01 7.524289e-01 +4.720000e+00 0.000000e+00 0.000000e+00 4.387700e+00 7.040085e-01 7.040085e-01 +4.760000e+00 0.000000e+00 0.000000e+00 4.488000e+00 7.248471e-01 7.248471e-01 +4.790000e+00 0.000000e+00 0.000000e+00 4.005900e+00 8.132648e-01 8.132648e-01 +5.000000e+00 0.000000e+00 0.000000e+00 4.244300e+00 6.389083e-01 6.389083e-01 +5.195000e+00 0.000000e+00 0.000000e+00 4.278100e+00 6.444777e-01 6.444777e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DASP_1978_I129715/d02-x01-y01 +IsRef: 1 +Path: /REF/DASP_1978_I129715/d02-x01-y01 +Title: doi:10.17182/hepdata.27431.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.602500e+00 0.000000e+00 0.000000e+00 2.360400e+00 3.579827e-01 3.579827e-01 +3.612500e+00 0.000000e+00 0.000000e+00 2.391300e+00 4.187874e-01 4.187874e-01 +3.625000e+00 0.000000e+00 0.000000e+00 2.285400e+00 3.638082e-01 3.638082e-01 +3.650000e+00 0.000000e+00 0.000000e+00 2.635500e+00 4.094609e-01 4.094609e-01 +3.845000e+00 0.000000e+00 0.000000e+00 3.166400e+00 5.324512e-01 5.324512e-01 +3.885000e+00 0.000000e+00 0.000000e+00 2.999400e+00 5.493590e-01 5.493590e-01 +3.930000e+00 0.000000e+00 0.000000e+00 3.252300e+00 6.411049e-01 6.411049e-01 +3.950000e+00 0.000000e+00 0.000000e+00 4.115900e+00 7.677901e-01 7.677901e-01 +3.977500e+00 0.000000e+00 0.000000e+00 3.537600e+00 6.146113e-01 6.146113e-01 +4.000000e+00 0.000000e+00 0.000000e+00 4.231000e+00 6.624520e-01 6.624520e-01 +4.010000e+00 0.000000e+00 0.000000e+00 4.451100e+00 6.865570e-01 6.865570e-01 +4.020000e+00 0.000000e+00 0.000000e+00 4.875100e+00 7.391680e-01 7.391680e-01 +4.030000e+00 0.000000e+00 0.000000e+00 5.557000e+00 8.374821e-01 8.374821e-01 +4.040000e+00 0.000000e+00 0.000000e+00 6.059300e+00 9.250545e-01 9.250545e-01 +4.050000e+00 0.000000e+00 0.000000e+00 5.091400e+00 7.927709e-01 7.927709e-01 +4.060000e+00 0.000000e+00 0.000000e+00 4.820800e+00 7.549750e-01 7.549750e-01 +4.070000e+00 0.000000e+00 0.000000e+00 4.566600e+00 7.214223e-01 7.214223e-01 +4.080000e+00 0.000000e+00 0.000000e+00 4.635600e+00 7.358254e-01 7.358254e-01 +4.090000e+00 0.000000e+00 0.000000e+00 4.301700e+00 6.786264e-01 6.786264e-01 +4.100000e+00 0.000000e+00 0.000000e+00 3.997600e+00 6.300630e-01 6.300630e-01 +4.110000e+00 0.000000e+00 0.000000e+00 4.287400e+00 6.711333e-01 6.711333e-01 +4.120000e+00 0.000000e+00 0.000000e+00 4.152000e+00 7.046717e-01 7.046717e-01 +4.130000e+00 0.000000e+00 0.000000e+00 4.485400e+00 7.987782e-01 7.987782e-01 +4.140000e+00 0.000000e+00 0.000000e+00 5.067500e+00 8.165288e-01 8.165288e-01 +4.155000e+00 0.000000e+00 0.000000e+00 5.293000e+00 8.316505e-01 8.316505e-01 +4.170000e+00 0.000000e+00 0.000000e+00 4.912400e+00 7.436874e-01 7.436874e-01 +4.180000e+00 0.000000e+00 0.000000e+00 5.181700e+00 8.947008e-01 8.947008e-01 +4.192500e+00 0.000000e+00 0.000000e+00 4.519600e+00 6.881499e-01 6.881499e-01 +4.212500e+00 0.000000e+00 0.000000e+00 4.662400e+00 7.473143e-01 7.473143e-01 +4.230000e+00 0.000000e+00 0.000000e+00 4.063400e+00 7.918923e-01 7.918923e-01 +4.240000e+00 0.000000e+00 0.000000e+00 3.822200e+00 6.397929e-01 6.397929e-01 +4.255000e+00 0.000000e+00 0.000000e+00 3.849600e+00 5.807217e-01 5.807217e-01 +4.282500e+00 0.000000e+00 0.000000e+00 4.075700e+00 6.575060e-01 6.575060e-01 +4.305000e+00 0.000000e+00 0.000000e+00 4.509700e+00 7.771134e-01 7.771134e-01 +4.315000e+00 0.000000e+00 0.000000e+00 4.281600e+00 6.831549e-01 6.831549e-01 +4.325000e+00 0.000000e+00 0.000000e+00 4.298500e+00 7.354413e-01 7.354413e-01 +4.335000e+00 0.000000e+00 0.000000e+00 4.336600e+00 6.952822e-01 6.952822e-01 +4.345000e+00 0.000000e+00 0.000000e+00 4.142200e+00 7.454226e-01 7.454226e-01 +4.355000e+00 0.000000e+00 0.000000e+00 5.008600e+00 7.971802e-01 7.971802e-01 +4.365000e+00 0.000000e+00 0.000000e+00 4.557800e+00 7.507686e-01 7.507686e-01 +4.375000e+00 0.000000e+00 0.000000e+00 4.872100e+00 7.726748e-01 7.726748e-01 +4.387500e+00 0.000000e+00 0.000000e+00 4.910000e+00 7.787271e-01 7.787271e-01 +4.400000e+00 0.000000e+00 0.000000e+00 5.402800e+00 8.121395e-01 8.121395e-01 +4.410000e+00 0.000000e+00 0.000000e+00 5.526700e+00 8.338319e-01 8.338319e-01 +4.420000e+00 0.000000e+00 0.000000e+00 5.560500e+00 8.434431e-01 8.434431e-01 +4.430000e+00 0.000000e+00 0.000000e+00 5.297900e+00 8.277260e-01 8.277260e-01 +4.440000e+00 0.000000e+00 0.000000e+00 5.501100e+00 8.809341e-01 8.809341e-01 +4.450000e+00 0.000000e+00 0.000000e+00 5.047400e+00 8.607922e-01 8.607922e-01 +4.460000e+00 0.000000e+00 0.000000e+00 6.971800e+00 1.078907e+00 1.078907e+00 +4.472500e+00 0.000000e+00 0.000000e+00 4.588600e+00 7.015472e-01 7.015472e-01 +4.490000e+00 0.000000e+00 0.000000e+00 5.166200e+00 8.036276e-01 8.036276e-01 +4.505000e+00 0.000000e+00 0.000000e+00 4.783200e+00 7.872854e-01 7.872854e-01 +4.515000e+00 0.000000e+00 0.000000e+00 4.635000e+00 7.431440e-01 7.431440e-01 +4.525000e+00 0.000000e+00 0.000000e+00 4.315200e+00 7.224376e-01 7.224376e-01 +4.535000e+00 0.000000e+00 0.000000e+00 4.945700e+00 8.458925e-01 8.458925e-01 +4.545000e+00 0.000000e+00 0.000000e+00 5.174600e+00 8.612226e-01 8.612226e-01 +4.555000e+00 0.000000e+00 0.000000e+00 5.000300e+00 7.902807e-01 7.902807e-01 +4.565000e+00 0.000000e+00 0.000000e+00 5.004100e+00 8.462596e-01 8.462596e-01 +4.575000e+00 0.000000e+00 0.000000e+00 5.120000e+00 8.712296e-01 8.712296e-01 +4.590000e+00 0.000000e+00 0.000000e+00 5.141900e+00 8.145380e-01 8.145380e-01 +4.605000e+00 0.000000e+00 0.000000e+00 4.951300e+00 8.497640e-01 8.497640e-01 +4.620000e+00 0.000000e+00 0.000000e+00 4.960200e+00 8.417768e-01 8.417768e-01 +4.635000e+00 0.000000e+00 0.000000e+00 4.794400e+00 7.862897e-01 7.862897e-01 +4.645000e+00 0.000000e+00 0.000000e+00 4.388600e+00 7.808299e-01 7.808299e-01 +4.660000e+00 0.000000e+00 0.000000e+00 4.851800e+00 8.374278e-01 8.374278e-01 +4.675000e+00 0.000000e+00 0.000000e+00 4.931500e+00 8.091586e-01 8.091586e-01 +4.690000e+00 0.000000e+00 0.000000e+00 5.118000e+00 8.612593e-01 8.612593e-01 +4.720000e+00 0.000000e+00 0.000000e+00 5.222500e+00 8.222751e-01 8.222751e-01 +4.760000e+00 0.000000e+00 0.000000e+00 5.329300e+00 8.433489e-01 8.433489e-01 +4.790000e+00 0.000000e+00 0.000000e+00 4.851900e+00 9.110477e-01 9.110477e-01 +5.000000e+00 0.000000e+00 0.000000e+00 5.118100e+00 7.695929e-01 7.695929e-01 +5.195000e+00 0.000000e+00 0.000000e+00 5.172200e+00 7.781167e-01 7.781167e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginDORIS/DASP_1982_I178613.cc b/analyses/pluginDORIS/DASP_1982_I178613.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DASP_1982_I178613.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DASP_1982_I178613 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DASP_1982_I178613); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(2, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(2, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DASP_1982_I178613); + + +} diff --git a/analyses/pluginDORIS/DASP_1982_I178613.info b/analyses/pluginDORIS/DASP_1982_I178613.info new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DASP_1982_I178613.info @@ -0,0 +1,32 @@ +Name: DASP_1982_I178613 +Year: 1982 +Summary: Measurement of $R$ in the $\Upsilon$ region, 9.42 GeV +Experiment: DASP +Collider: DORIS +InspireID: 178613 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B116 (1982) 383-386, 1982 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by DASP in the $\Upsilon$ region, 9.42 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Albrecht:1982bq +BibTeX: '@article{Albrecht:1982bq, + author = "Albrecht, H. and others", + title = "{The Hadronic Cross-section of Electron - Positron + Annihilation at 9.5-{GeV} and the $\Upsilon$ and + $\Upsilon^\prime$ Resonance Parameters}", + journal = "Phys. Lett.", + volume = "116B", + year = "1982", + pages = "383-386", + doi = "10.1016/0370-2693(82)90305-7", + reportNumber = "DESY-82-037", + SLACcitation = "%%CITATION = PHLTA,116B,383;%%" +}' diff --git a/analyses/pluginDORIS/DASP_1982_I178613.plot b/analyses/pluginDORIS/DASP_1982_I178613.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DASP_1982_I178613.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /DASP_1982_I178613/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DASP_1982_I178613/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DASP_1982_I178613/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginDORIS/DASP_1982_I178613.yoda b/analyses/pluginDORIS/DASP_1982_I178613.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DASP_1982_I178613.yoda @@ -0,0 +1,17 @@ +BEGIN YODA_SCATTER1D_V2 /REF/DASP_1982_I178613/d01-x01-y01 +IsRef: 1 +Path: /REF/DASP_1982_I178613/d01-x01-y01 +Title: doi:10.17182/hepdata.30881.v1/t1 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DASP_1982_I178613/d02-x01-y01 +IsRef: 1 +Path: /REF/DASP_1982_I178613/d02-x01-y01 +Title: doi:10.17182/hepdata.30881.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.420000e+00 2.000000e-02 2.000000e-02 3.730000e+00 3.222733e-01 3.222733e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginDORIS/DESY147_1978_I131524.cc b/analyses/pluginDORIS/DESY147_1978_I131524.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DESY147_1978_I131524.cc @@ -0,0 +1,103 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DESY147_1978_I131524 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DESY147_1978_I131524); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + ostringstream title; + title << "d0" << ix << "_sigma"; + Scatter2DPtr hadrons = bookScatter2D(title.str() + "_hadrons"); + Scatter2DPtr muons = bookScatter2D(title.str() + "_muons" ); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DESY147_1978_I131524); + + +} diff --git a/analyses/pluginDORIS/DESY147_1978_I131524.info b/analyses/pluginDORIS/DESY147_1978_I131524.info new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DESY147_1978_I131524.info @@ -0,0 +1,32 @@ +Name: DESY147_1978_I131524 +Year: 1978 +Summary: Measurement of $R$ for energies between 9.41 and 10.63 GeV +Experiment: DESY147 +Collider: DORIS +InspireID: 131524 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B78 (1978) 360-363, 1978 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 9.41 and 9.51, and 9.98 and 10.63 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Bienlein:1978bg +BibTeX: '@article{Bienlein:1978bg, + author = "Bienlein, J. K. and others", + title = "{Observation of a Narrow Resonance at 10.02-GeV in e+ e- + Annihilations}", + journal = "Phys. Lett.", + volume = "78B", + year = "1978", + pages = "360-363", + doi = "10.1016/0370-2693(78)90040-0", + reportNumber = "DESY-78-45", + SLACcitation = "%%CITATION = PHLTA,78B,360;%%" +}' diff --git a/analyses/pluginDORIS/DESY147_1978_I131524.plot b/analyses/pluginDORIS/DESY147_1978_I131524.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DESY147_1978_I131524.plot @@ -0,0 +1,43 @@ +BEGIN PLOT /DESY147_1978_I131524/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DESY147_1978_I131524/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DESY147_1978_I131524/d01_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DESY147_1978_I131524/d01_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DESY147_1978_I131524/d02_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DESY147_1978_I131524/d02_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT + diff --git a/analyses/pluginDORIS/DESY147_1978_I131524.yoda b/analyses/pluginDORIS/DESY147_1978_I131524.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DESY147_1978_I131524.yoda @@ -0,0 +1,41 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DESY147_1978_I131524/d01-x01-y01 +IsRef: 1 +Path: /REF/DESY147_1978_I131524/d01-x01-y01 +Title: doi:10.17182/hepdata.45244.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.410000e+00 0.000000e+00 0.000000e+00 4.100000e+00 8.112336e-01 8.112336e-01 +9.425000e+00 0.000000e+00 0.000000e+00 4.600000e+00 7.560423e-01 7.560423e-01 +9.440000e+00 0.000000e+00 0.000000e+00 3.900000e+00 6.341136e-01 6.341136e-01 +9.450000e+00 0.000000e+00 0.000000e+00 7.800000e+00 1.153646e+00 1.153646e+00 +9.455000e+00 0.000000e+00 0.000000e+00 1.260000e+01 1.395564e+00 1.395564e+00 +9.460000e+00 0.000000e+00 0.000000e+00 1.380000e+01 1.686802e+00 1.686802e+00 +9.470000e+00 0.000000e+00 0.000000e+00 8.600000e+00 1.396281e+00 1.396281e+00 +9.480000e+00 0.000000e+00 0.000000e+00 5.100000e+00 8.905055e-01 8.905055e-01 +9.490000e+00 0.000000e+00 0.000000e+00 5.600000e+00 9.200543e-01 9.200543e-01 +9.500000e+00 0.000000e+00 0.000000e+00 4.230000e+00 7.341178e-01 7.341178e-01 +9.510000e+00 0.000000e+00 0.000000e+00 4.350000e+00 7.410972e-01 7.410972e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DESY147_1978_I131524/d02-x01-y01 +IsRef: 1 +Path: /REF/DESY147_1978_I131524/d02-x01-y01 +Title: doi:10.17182/hepdata.45244.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.980000e+00 0.000000e+00 0.000000e+00 2.500000e+00 5.679789e-01 5.679789e-01 +1.000000e+01 0.000000e+00 0.000000e+00 3.040000e+00 5.184747e-01 5.184747e-01 +1.000500e+01 0.000000e+00 0.000000e+00 2.680000e+00 5.761285e-01 5.761285e-01 +1.001000e+01 0.000000e+00 0.000000e+00 4.600000e+00 8.544004e-01 8.544004e-01 +1.002000e+01 0.000000e+00 0.000000e+00 3.480000e+00 5.848111e-01 5.848111e-01 +1.002800e+01 0.000000e+00 0.000000e+00 3.500000e+00 8.005623e-01 8.005623e-01 +1.003300e+01 0.000000e+00 0.000000e+00 3.040000e+00 7.085309e-01 7.085309e-01 +1.004400e+01 0.000000e+00 0.000000e+00 2.230000e+00 5.934888e-01 5.934888e-01 +1.005300e+01 0.000000e+00 0.000000e+00 2.560000e+00 6.523312e-01 6.523312e-01 +1.007000e+01 0.000000e+00 0.000000e+00 2.320000e+00 5.785534e-01 5.785534e-01 +1.008000e+01 0.000000e+00 0.000000e+00 2.410000e+00 6.745228e-01 6.745228e-01 +1.009000e+01 0.000000e+00 0.000000e+00 2.410000e+00 5.281865e-01 5.281865e-01 +1.010000e+01 0.000000e+00 0.000000e+00 2.140000e+00 5.164262e-01 5.164262e-01 +1.063000e+01 0.000000e+00 0.000000e+00 2.150000e+00 5.719484e-01 5.719484e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginDORIS/DESY147_1980_I153896.cc b/analyses/pluginDORIS/DESY147_1980_I153896.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DESY147_1980_I153896.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DESY147_1980_I153896 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DESY147_1980_I153896); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DESY147_1980_I153896); + + +} diff --git a/analyses/pluginDORIS/DESY147_1980_I153896.info b/analyses/pluginDORIS/DESY147_1980_I153896.info new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DESY147_1980_I153896.info @@ -0,0 +1,33 @@ +Name: DESY147_1980_I153896 +Year: 1980 +Summary: Measurement of $R$ between 9.4 and 10.1 GeV +Experiment: DESY147 +Collider: DORIS +InspireID: 153896 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C6 (1980) 125, 1980 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 9.4 and 10.1 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Bock:1980ag +BibTeX: '@article{Bock:1980ag, + author = "Bock, P. and others", + title = "{Total Cross-section for Hadron Production by $e^+ e^-$ + Annihilation Between 9.4-{GeV} and 9.5-{GeV}}", + collaboration = "DESY-Hamburg-Heidelberg-Munich", + journal = "Z. Phys.", + volume = "C6", + year = "1980", + pages = "125", + doi = "10.1007/BF01588838", + reportNumber = "DESY-80-58", + SLACcitation = "%%CITATION = ZEPYA,C6,125;%%" +}' diff --git a/analyses/pluginDORIS/DESY147_1980_I153896.plot b/analyses/pluginDORIS/DESY147_1980_I153896.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DESY147_1980_I153896.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /DESY147_1980_I153896/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DESY147_1980_I153896/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /DESY147_1980_I153896/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginDORIS/DESY147_1980_I153896.yoda b/analyses/pluginDORIS/DESY147_1980_I153896.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/DESY147_1980_I153896.yoda @@ -0,0 +1,10 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DESY147_1980_I153896/d01-x01-y01 +IsRef: 1 +Path: /REF/DESY147_1980_I153896/d01-x01-y01 +Title: doi:10.17182/hepdata.14364.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.450000e+00 5.000000e-02 5.000000e-02 3.800000e+00 8.153061e-01 8.153061e-01 +1.004000e+01 6.000000e-02 6.000000e-02 3.600000e+00 6.489992e-01 6.489992e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginDORIS/LENA_1982_I179431.cc b/analyses/pluginDORIS/LENA_1982_I179431.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/LENA_1982_I179431.cc @@ -0,0 +1,103 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class LENA_1982_I179431 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(LENA_1982_I179431); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + for(unsigned int ix=1;ix<4;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + ostringstream title; + title << "d0" << ix << "_sigma"; + Scatter2DPtr hadrons = bookScatter2D(title.str() + "_hadrons"); + Scatter2DPtr muons = bookScatter2D(title.str() + "_muons" ); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(LENA_1982_I179431); + + +} diff --git a/analyses/pluginDORIS/LENA_1982_I179431.info b/analyses/pluginDORIS/LENA_1982_I179431.info new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/LENA_1982_I179431.info @@ -0,0 +1,33 @@ +Name: LENA_1982_I179431 +Year: 1982 +Summary: Measurement of $R$ between 7.4 and 9.4 GeV +Experiment: LENA +Collider: DORIS +InspireID: 179431 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C15 (1982) 299, 1982 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by LENA for energies between .4 and 9.4 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Niczyporuk:1982ya +BibTeX: '@article{Niczyporuk:1982ya, + author = "Niczyporuk, B. and others", + title = "{Measurement of R in $e^+ e^-$ Annihilation for + $\sqrt{s}$ Between 7.4-{GeV} and 9.4-{GeV}}", + collaboration = "LENA", + journal = "Z. Phys.", + volume = "C15", + year = "1982", + pages = "299", + doi = "10.1007/BF01614421", + reportNumber = "DESY-82-052", + SLACcitation = "%%CITATION = ZEPYA,C15,299;%%" +}' diff --git a/analyses/pluginDORIS/LENA_1982_I179431.plot b/analyses/pluginDORIS/LENA_1982_I179431.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/LENA_1982_I179431.plot @@ -0,0 +1,64 @@ +BEGIN PLOT /LENA_1982_I179431/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /LENA_1982_I179431/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /LENA_1982_I179431/d03-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /LENA_1982_I179431/d01_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /LENA_1982_I179431/d01_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /LENA_1982_I179431/d02_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /LENA_1982_I179431/d02_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /LENA_1982_I179431/d03_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /LENA_1982_I179431/d03_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT + diff --git a/analyses/pluginDORIS/LENA_1982_I179431.yoda b/analyses/pluginDORIS/LENA_1982_I179431.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginDORIS/LENA_1982_I179431.yoda @@ -0,0 +1,212 @@ +BEGIN YODA_SCATTER2D_V2 /REF/LENA_1982_I179431/d01-x01-y01 +IsRef: 1 +Path: /REF/LENA_1982_I179431/d01-x01-y01 +Title: doi:10.17182/hepdata.16412.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +8.400000e+00 1.000000e+00 1.000000e+00 3.370000e+00 3.278431e-01 3.278431e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/LENA_1982_I179431/d02-x01-y01 +IsRef: 1 +Path: /REF/LENA_1982_I179431/d02-x01-y01 +Title: doi:10.17182/hepdata.16412.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.440000e+00 4.000000e-02 4.000000e-02 3.370000e+00 2.605401e-01 2.605401e-01 +8.910000e+00 2.400000e-01 2.400000e-01 3.420000e+00 2.500103e-01 2.500103e-01 +9.280000e+00 1.300000e-01 1.300000e-01 3.310000e+00 2.393364e-01 2.393364e-01 +9.415000e+00 1.500000e-02 1.500000e-02 3.570000e+00 3.607102e-01 3.607102e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/LENA_1982_I179431/d03-x01-y01 +IsRef: 1 +Path: /REF/LENA_1982_I179431/d03-x01-y01 +Title: doi:10.17182/hepdata.16412.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.4 0. 0. 3.880000e+00 5.635417e-01 5.635417e-01 +7.406 0. 0. 3.970000e+00 6.563160e-01 6.563160e-01 +7.412 0. 0. 3.390000e+00 5.220039e-01 5.220039e-01 +7.418 0. 0. 2.760000e+00 4.680763e-01 4.680763e-01 +7.424 0. 0. 3.250000e+00 5.362043e-01 5.362043e-01 +7.43 0. 0. 4.720000e+00 7.499385e-01 7.499385e-01 +7.435 0. 0. 3.220000e+00 4.990428e-01 4.990428e-01 +7.442 0. 0. 3.350000e+00 5.663725e-01 5.663725e-01 +7.448 0. 0. 3.300000e+00 5.103775e-01 5.103775e-01 +7.454 0. 0. 3.590000e+00 6.743550e-01 6.743550e-01 +7.46 0. 0. 2.390000e+00 4.031645e-01 4.031645e-01 +7.466 0. 0. 3.260000e+00 5.182734e-01 5.182734e-01 +7.472 0. 0. 3.680000e+00 5.485361e-01 5.485361e-01 +7.478 0. 0. 2.790000e+00 4.872811e-01 4.872811e-01 +8.67 0. 0. 5.090000e+00 1.538279e+00 1.538279e+00 +8.678 0. 0. 4.800000e+00 1.012436e+00 1.012436e+00 +8.686 0. 0. 3.880000e+00 8.506934e-01 8.506934e-01 +8.694 0. 0. 4.680000e+00 1.114998e+00 1.114998e+00 +8.702 0. 0. 2.240000e+00 4.933802e-01 4.933802e-01 +8.71 0. 0. 3.030000e+00 5.396416e-01 5.396416e-01 +8.718 0. 0. 3.780000e+00 8.010872e-01 8.010872e-01 +8.726 0. 0. 3.960000e+00 9.287059e-01 9.287059e-01 +8.734 0. 0. 3.660000e+00 7.134654e-01 7.134654e-01 +8.742 0. 0. 2.760000e+00 6.374131e-01 6.374131e-01 +8.75 0. 0. 3.470000e+00 7.091908e-01 7.091908e-01 +8.757 0. 0. 3.130000e+00 6.355929e-01 6.355929e-01 +8.766 0. 0. 4.670000e+00 9.812238e-01 9.812238e-01 +8.77 0. 0. 3.080000e+00 5.224791e-01 5.224791e-01 +8.774 0. 0. 3.050000e+00 5.587118e-01 5.587118e-01 +8.782 0. 0. 2.810000e+00 8.218550e-01 8.218550e-01 +8.79 0. 0. 3.510000e+00 7.574331e-01 7.574331e-01 +8.8 0. 0. 4.700000e+00 1.038875e+00 1.038875e+00 +8.808 0. 0. 3.360000e+00 7.639234e-01 7.639234e-01 +8.818 0. 0. 3.530000e+00 9.015747e-01 9.015747e-01 +8.827 0. 0. 3.630000e+00 7.599678e-01 7.599678e-01 +8.836 0. 0. 3.400000e+00 1.084201e+00 1.084201e+00 +8.845 0. 0. 4.320000e+00 1.002684e+00 1.002684e+00 +8.854 0. 0. 2.990000e+00 6.706207e-01 6.706207e-01 +8.863 0. 0. 3.990000e+00 7.962194e-01 7.962194e-01 +8.872 0. 0. 2.600000e+00 6.247765e-01 6.247765e-01 +8.881 0. 0. 3.150000e+00 7.983997e-01 7.983997e-01 +8.891 0. 0. 2.110000e+00 5.099858e-01 5.099858e-01 +8.908 0. 0. 2.710000e+00 6.268713e-01 6.268713e-01 +8.916 0. 0. 4.050000e+00 8.069887e-01 8.069887e-01 +8.926 0. 0. 3.320000e+00 7.249687e-01 7.249687e-01 +8.94 0. 0. 3.100000e+00 7.975207e-01 7.975207e-01 +8.962 0. 0. 3.240000e+00 8.579183e-01 8.579183e-01 +8.971 0. 0. 4.650000e+00 1.076087e+00 1.076087e+00 +8.98 0. 0. 2.080000e+00 5.770799e-01 5.770799e-01 +8.989 0. 0. 4.110000e+00 9.891050e-01 9.891050e-01 +8.998 0. 0. 3.770000e+00 8.675838e-01 8.675838e-01 +9.007 0. 0. 2.650000e+00 6.257188e-01 6.257188e-01 +9.016 0. 0. 2.740000e+00 6.466078e-01 6.466078e-01 +9.025 0. 0. 5.000000e+00 1.092623e+00 1.092623e+00 +9.038 0. 0. 3.130000e+00 5.886241e-01 5.886241e-01 +9.052 0. 0. 3.540000e+00 8.728427e-01 8.728427e-01 +9.061 0. 0. 5.230000e+00 1.202201e+00 1.202201e+00 +9.074 0. 0. 2.030000e+00 4.892839e-01 4.892839e-01 +9.093 0. 0. 3.590000e+00 6.837066e-01 6.837066e-01 +9.106 0. 0. 4.460000e+00 1.082078e+00 1.082078e+00 +9.115 0. 0. 3.420000e+00 8.225601e-01 8.225601e-01 +9.124 0. 0. 3.530000e+00 9.015747e-01 9.015747e-01 +9.133 0. 0. 3.360000e+00 9.763089e-01 9.763089e-01 +9.142 0. 0. 2.850000e+00 6.966792e-01 6.966792e-01 +9.15 0. 0. 2.240000e+00 5.508394e-01 5.508394e-01 +9.16 0. 0. 3.250000e+00 5.270816e-01 5.270816e-01 +9.17 0. 0. 3.230000e+00 5.265295e-01 5.265295e-01 +9.18 0. 0. 3.100000e+00 4.596078e-01 4.596078e-01 +9.19 0. 0. 3.450000e+00 5.417844e-01 5.417844e-01 +9.2 0. 0. 3.250000e+00 5.362043e-01 5.362043e-01 +9.21 0. 0. 3.710000e+00 6.218417e-01 6.218417e-01 +9.219 0. 0. 2.880000e+00 4.896259e-01 4.896259e-01 +9.23 0. 0. 2.070000e+00 3.487620e-01 3.487620e-01 +9.24 0. 0. 3.000000e+00 5.019970e-01 5.019970e-01 +9.25 0. 0. 3.240000e+00 4.639221e-01 4.639221e-01 +9.26 0. 0. 3.440000e+00 5.505643e-01 5.505643e-01 +9.27 0. 0. 3.570000e+00 5.906030e-01 5.906030e-01 +9.28 0. 0. 3.550000e+00 5.267567e-01 5.267567e-01 +9.29 0. 0. 3.620000e+00 5.557208e-01 5.557208e-01 +9.3 0. 0. 4.440000e+00 6.341091e-01 6.341091e-01 +9.31 0. 0. 3.560000e+00 5.449695e-01 5.449695e-01 +9.32 0. 0. 3.220000e+00 5.353912e-01 5.353912e-01 +9.33 0. 0. 2.930000e+00 5.278614e-01 5.278614e-01 +9.34 0. 0. 3.370000e+00 5.395193e-01 5.395193e-01 +9.35 0. 0. 3.030000e+00 4.396738e-01 4.396738e-01 +9.36 0. 0. 4.480000e+00 6.708920e-01 6.708920e-01 +9.37 0. 0. 3.470000e+00 5.333400e-01 5.333400e-01 +9.38 0. 0. 3.010000e+00 5.022657e-01 5.022657e-01 +9.39 0. 0. 3.110000e+00 5.788074e-01 5.788074e-01 +9.4 0. 0. 3.450000e+00 5.237655e-01 5.237655e-01 +9.41 0. 0. 4.290000e+00 9.638548e-01 9.638548e-01 +9.4 0. 0. 3.910000e+00 5.556332e-01 5.556332e-01 +END YODA_SCATTER2D_V2 + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + diff --git a/analyses/pluginFrascati/BBAR_1980_I152630.cc b/analyses/pluginFrascati/BBAR_1980_I152630.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/BBAR_1980_I152630.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class BBAR_1980_I152630 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(BBAR_1980_I152630); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(BBAR_1980_I152630); + + +} diff --git a/analyses/pluginFrascati/BBAR_1980_I152630.info b/analyses/pluginFrascati/BBAR_1980_I152630.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/BBAR_1980_I152630.info @@ -0,0 +1,31 @@ +Name: BBAR_1980_I152630 +Year: 1980 +Summary: Measurement of $R$ between 1.427 and 1.946 +Experiment: BBAR +Collider: ADONE +InspireID: 152630 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B91 (1980) 155-160, 1980 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by the baryon-antibaryon experiment between 1.427 and 1.946 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Ambrosio:1980mf +BibTeX: '@article{Ambrosio:1980mf, + author = "Ambrosio, M. and others", + title = "{Total Cross-section for Hadron Production by Electron - + Positron Annihilation at Adone}", + journal = "Phys. Lett.", + volume = "91B", + year = "1980", + pages = "155-160", + doi = "10.1016/0370-2693(80)90683-8", + reportNumber = "LNF-80-4-P", + SLACcitation = "%%CITATION = PHLTA,91B,155;%%" +}' diff --git a/analyses/pluginFrascati/BBAR_1980_I152630.plot b/analyses/pluginFrascati/BBAR_1980_I152630.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/BBAR_1980_I152630.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /BBAR_1980_I152630/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BBAR_1980_I152630/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /BBAR_1980_I152630/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginFrascati/BBAR_1980_I152630.yoda b/analyses/pluginFrascati/BBAR_1980_I152630.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/BBAR_1980_I152630.yoda @@ -0,0 +1,27 @@ +BEGIN YODA_SCATTER2D_V2 /REF/BBAR_1980_I152630/d01-x01-y01 +IsRef: 1 +Path: /REF/BBAR_1980_I152630/d01-x01-y01 +Title: doi:10.17182/hepdata.27239.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.427000e+00 1.500000e-02 1.000000e-02 1.840000e+00 3.190235e-01 3.190235e-01 +1.452000e+00 1.500000e-02 1.000000e-02 1.800000e+00 2.996665e-01 2.996665e-01 +1.472000e+00 1.000000e-02 1.500000e-02 2.410000e+00 3.953255e-01 3.953255e-01 +1.501000e+00 1.400000e-02 1.100000e-02 2.390000e+00 3.696245e-01 3.696245e-01 +1.523000e+00 1.100000e-02 1.400000e-02 2.660000e+00 4.508891e-01 4.508891e-01 +1.550000e+00 1.300000e-02 1.200000e-02 1.990000e+00 3.768319e-01 3.768319e-01 +1.574000e+00 1.200000e-02 1.300000e-02 1.730000e+00 3.276282e-01 3.276282e-01 +1.599000e+00 1.200000e-02 1.300000e-02 1.970000e+00 4.070875e-01 4.070875e-01 +1.624000e+00 1.200000e-02 1.300000e-02 1.940000e+00 3.902320e-01 3.902320e-01 +1.650000e+00 1.300000e-02 1.200000e-02 2.470000e+00 4.469567e-01 4.469567e-01 +1.673000e+00 1.100000e-02 1.400000e-02 2.100000e+00 3.900320e-01 3.900320e-01 +1.700000e+00 1.300000e-02 1.200000e-02 2.280000e+00 4.178086e-01 4.178086e-01 +1.722000e+00 1.000000e-02 1.500000e-02 2.310000e+00 4.518432e-01 4.518432e-01 +1.746000e+00 9.000000e-03 1.600000e-02 2.370000e+00 5.059449e-01 5.059449e-01 +1.799000e+00 1.200000e-02 1.300000e-02 2.440000e+00 4.322684e-01 4.322684e-01 +1.826000e+00 1.400000e-02 1.100000e-02 2.710000e+00 4.720617e-01 4.720617e-01 +1.845000e+00 8.000000e-03 1.700000e-02 2.820000e+00 6.473245e-01 6.473245e-01 +1.874000e+00 1.200000e-02 1.300000e-02 1.460000e+00 4.213799e-01 4.213799e-01 +1.946000e+00 9.000000e-03 1.600000e-02 1.410000e+00 3.509021e-01 3.509021e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/FENICE_1994_I377833.cc b/analyses/pluginFrascati/FENICE_1994_I377833.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/FENICE_1994_I377833.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class FENICE_1994_I377833 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(FENICE_1994_I377833); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nProton= bookCounter( "/TMP/nProton" ); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + // total hadronic and muonic cross sections + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && nCount[2212]==1 && nCount[-2212]==1) + _nProton->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sigma = _nProton->val()*fact; + double error = _nProton->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqr(sqrtS()/GeV), x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nProton; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(FENICE_1994_I377833); + + +} diff --git a/analyses/pluginFrascati/FENICE_1994_I377833.info b/analyses/pluginFrascati/FENICE_1994_I377833.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/FENICE_1994_I377833.info @@ -0,0 +1,30 @@ +Name: FENICE_1994_I377833 +Year: 1994 +Summary: Cross section for $e^+e^-\to p\bar{p}$ between 1.9 and 2.44 GeV +Experiment: FENICE +Collider: ADONE +InspireID: 377833 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B334 (1994) 431-434, 1994 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ between 1.9 and 2.44 GeV.' +Keywords: +BibKey: Antonelli:1994kq +BibTeX: '@article{Antonelli:1994kq, + author = "Antonelli, A. and others", + title = "{Measurement of the electromagnetic form-factor of the + proton in the timelike region}", + journal = "Phys. Lett.", + volume = "B334", + year = "1994", + pages = "431-434", + doi = "10.1016/0370-2693(94)90710-2", + reportNumber = "LNF-94-032-P", + SLACcitation = "%%CITATION = PHLTA,B334,431;%%" +}' diff --git a/analyses/pluginFrascati/FENICE_1994_I377833.plot b/analyses/pluginFrascati/FENICE_1994_I377833.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/FENICE_1994_I377833.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /FENICE_1994_I377833/d01-x01-y01 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$s/\text{GeV}^2$ +YLabel=$\sigma(e^+e^-\to p\bar{p})$/nb +ConnectGaps=1 +XMin=3.5 +XMax=6.0 +END PLOT diff --git a/analyses/pluginFrascati/FENICE_1994_I377833.yoda b/analyses/pluginFrascati/FENICE_1994_I377833.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/FENICE_1994_I377833.yoda @@ -0,0 +1,24 @@ +BEGIN YODA_SCATTER2D_V2 /REF/FENICE_1994_I377833/d01-x01-y01 +IsRef: 1 +Path: /REF/FENICE_1994_I377833/d01-x01-y01 +Title: doi:10.17182/hepdata.28572.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.690000e+00 0.000000e+00 0.000000e+00 9.600000e-01 2.731300e-01 2.731300e-01 +4.000000e+00 0.000000e+00 0.000000e+00 6.200000e-01 1.708801e-01 1.708801e-01 +4.410000e+00 0.000000e+00 0.000000e+00 6.200000e-01 1.208305e-01 1.208305e-01 +5.950000e+00 0.000000e+00 0.000000e+00 2.800000e-01 1.208305e-01 1.208305e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/FENICE_1994_I377833/d02-x01-y01 +IsRef: 1 +Path: /REF/FENICE_1994_I377833/d02-x01-y01 +Title: doi:10.17182/hepdata.28572.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.690000e+00 0.000000e+00 0.000000e+00 3.600000e-01 5.385165e-02 5.385165e-02 +4.000000e+00 0.000000e+00 0.000000e+00 2.400000e-01 3.162278e-02 3.162278e-02 +4.410000e+00 0.000000e+00 0.000000e+00 2.200000e-01 2.236068e-02 2.236068e-02 +5.950000e+00 0.000000e+00 0.000000e+00 1.500000e-01 3.162278e-02 3.162278e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/FENICE_1998_I471263.cc b/analyses/pluginFrascati/FENICE_1998_I471263.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/FENICE_1998_I471263.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class FENICE_1998_I471263 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(FENICE_1998_I471263); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nNeutron= bookCounter( "/TMP/nNeutron" ); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + // total hadronic and muonic cross sections + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && nCount[2112]==1 && nCount[-2112]==1) + _nNeutron->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sigma = _nNeutron->val()*fact; + double error = _nNeutron->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nNeutron; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(FENICE_1998_I471263); + + +} diff --git a/analyses/pluginFrascati/FENICE_1998_I471263.info b/analyses/pluginFrascati/FENICE_1998_I471263.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/FENICE_1998_I471263.info @@ -0,0 +1,29 @@ +Name: FENICE_1998_I471263 +Year: 1998 +Summary: Cross section for $e^+e^-\to n\bar{n}$ between 1.9 and 2.44 GeV +Experiment: FENICE +Collider: ADONE +InspireID: 471263 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Nucl.Phys. B517 (1998) 3-35, 1998 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to n\bar{n}$ between 1.9 and 2.44 GeV.' +Keywords: +BibKey: Antonelli:1998fv +BibTeX: '@article{Antonelli:1998fv, + author = "Antonelli, A. and others", + title = "{The first measurement of the neutron electromagnetic + form-factors in the timelike region}", + journal = "Nucl. Phys.", + volume = "B517", + year = "1998", + pages = "3-35", + doi = "10.1016/S0550-3213(98)00083-2", + SLACcitation = "%%CITATION = NUPHA,B517,3;%%" +}' diff --git a/analyses/pluginFrascati/FENICE_1998_I471263.plot b/analyses/pluginFrascati/FENICE_1998_I471263.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/FENICE_1998_I471263.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /FENICE_1998_I471263/d01-x01-y01 +Title=$\sigma(e^+e^-\to n\bar{n})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to n\bar{n})$/nb +ConnectGaps=1 +XMin=1.8 +XMax=2.5 +END PLOT diff --git a/analyses/pluginFrascati/FENICE_1998_I471263.yoda b/analyses/pluginFrascati/FENICE_1998_I471263.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/FENICE_1998_I471263.yoda @@ -0,0 +1,65 @@ +BEGIN YODA_SCATTER2D_V2 /REF/FENICE_1998_I471263/d01-x01-y01 +IsRef: 1 +Path: /REF/FENICE_1998_I471263/d01-x01-y01 +Title: doi:10.17182/hepdata.32681.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.900000e+00 0.000000e+00 0.000000e+00 1.100000e+00 8.000000e-01 8.000000e-01 +1.920000e+00 0.000000e+00 0.000000e+00 1.060000e+00 4.400000e-01 4.400000e-01 +2.000000e+00 0.000000e+00 0.000000e+00 8.800000e-01 3.400000e-01 3.400000e-01 +2.100000e+00 0.000000e+00 0.000000e+00 1.000000e+00 2.800000e-01 2.800000e-01 +2.440000e+00 0.000000e+00 0.000000e+00 6.500000e-01 2.900000e-01 2.900000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/FENICE_1998_I471263/d02-x01-y01 +IsRef: 1 +Path: /REF/FENICE_1998_I471263/d02-x01-y01 +Title: doi:10.17182/hepdata.32681.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.640000e+00 0.000000e+00 0.000000e+00 4.500000e-01 1.600000e-01 1.600000e-01 +3.690000e+00 0.000000e+00 0.000000e+00 3.900000e-01 8.000000e-02 8.000000e-02 +4.000000e+00 0.000000e+00 0.000000e+00 2.900000e-01 5.000000e-02 5.000000e-02 +4.410000e+00 0.000000e+00 0.000000e+00 2.800000e-01 4.000000e-02 4.000000e-02 +5.950000e+00 0.000000e+00 0.000000e+00 2.300000e-01 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/FENICE_1998_I471263/d02-x01-y02 +IsRef: 1 +Path: /REF/FENICE_1998_I471263/d02-x01-y02 +Title: doi:10.17182/hepdata.32681.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.640000e+00 0.000000e+00 0.000000e+00 5.500000e-01 2.000000e-01 2.000000e-01 +3.690000e+00 0.000000e+00 0.000000e+00 4.700000e-01 1.000000e-01 1.000000e-01 +4.000000e+00 0.000000e+00 0.000000e+00 3.400000e-01 6.000000e-02 6.000000e-02 +4.410000e+00 0.000000e+00 0.000000e+00 3.400000e-01 5.000000e-02 5.000000e-02 +5.950000e+00 0.000000e+00 0.000000e+00 2.600000e-01 6.000000e-02 6.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/FENICE_1998_I471263/d03-x01-y01 +IsRef: 1 +Path: /REF/FENICE_1998_I471263/d03-x01-y01 +Title: doi:10.17182/hepdata.32681.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.610000e+00 0.000000e+00 0.000000e+00 9.700000e-01 4.400000e-01 5.300000e-01 +3.690000e+00 0.000000e+00 0.000000e+00 9.600000e-01 2.700000e-01 2.700000e-01 +4.000000e+00 0.000000e+00 0.000000e+00 6.200000e-01 1.700000e-01 1.700000e-01 +4.420000e+00 0.000000e+00 0.000000e+00 6.200000e-01 1.200000e-01 1.200000e-01 +5.950000e+00 0.000000e+00 0.000000e+00 2.800000e-01 1.200000e-01 1.200000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/FENICE_1998_I471263/d03-x01-y02 +IsRef: 1 +Path: /REF/FENICE_1998_I471263/d03-x01-y02 +Title: doi:10.17182/hepdata.32681.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.610000e+00 0.000000e+00 0.000000e+00 4.100000e-01 9.000000e-02 1.100000e-01 +3.690000e+00 0.000000e+00 0.000000e+00 3.600000e-01 5.000000e-02 5.000000e-02 +4.000000e+00 0.000000e+00 0.000000e+00 2.400000e-01 3.000000e-02 3.000000e-02 +4.420000e+00 0.000000e+00 0.000000e+00 2.200000e-01 2.000000e-02 2.000000e-02 +5.950000e+00 0.000000e+00 0.000000e+00 1.500000e-01 3.000000e-02 3.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.cc b/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class GAMMAGAMMA_1973_I84794 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(GAMMAGAMMA_1973_I84794); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(3, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(3,1,1); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(4,1,1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(GAMMAGAMMA_1973_I84794); + + +} diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.info b/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.info @@ -0,0 +1,32 @@ +Name: GAMMAGAMMA_1973_I84794 +Year: 1973 +Summary: Measurement of $R$ and the hadronic cross section for energies between 1.35 and 3 GeV +Experiment: GAMMAGAMMA +Collider: ADONE +InspireID: 84794 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B44 (1973) 533-536, 1973 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ and the hadronic cross section in $e^+e^-$ collisions by the GAMMA-GAMMA group for energies between 1.35 and 3 GeV. + The muonic cross section is also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Bacci:1973fb +BibTeX: '@article{Bacci:1973fb, + author = "Bacci, C. and Penson, G. and Salvini, G. and Stella, B. + and Baldini-Celio, R. and Capon, G. and Mencuccini, C. and + Murtas, G. P. and Spinetti, M. and Zallo, A.", + title = "{Multihadronic cross-sections from e+ e- annihilation up + to 3 gev center-of-mass energy}", + journal = "Phys. Lett.", + volume = "44B", + year = "1973", + pages = "533-536", + doi = "10.1016/0370-2693(73)90016-6", + SLACcitation = "%%CITATION = PHLTA,44B,533;%%" +}' diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.plot b/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /GAMMAGAMMA_1973_I84794/d04-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1973_I84794/d03-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1973_I84794/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.yoda b/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1973_I84794.yoda @@ -0,0 +1,60 @@ +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1973_I84794/d01-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1973_I84794/d01-x01-y01 +Title: doi:10.17182/hepdata.6496.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.350000e+00 0.000000e+00 0.000000e+00 4.500000e+01 1.800000e+01 1.800000e+01 +1.450000e+00 0.000000e+00 0.000000e+00 5.500000e+01 1.500000e+01 1.500000e+01 +1.650000e+00 0.000000e+00 0.000000e+00 3.600000e+01 7.000000e+00 7.000000e+00 +1.900000e+00 0.000000e+00 0.000000e+00 1.550000e+01 4.000000e+00 4.000000e+00 +1.980000e+00 0.000000e+00 0.000000e+00 3.000000e+01 1.000000e+01 1.000000e+01 +2.100000e+00 0.000000e+00 0.000000e+00 1.700000e+01 4.000000e+00 4.000000e+00 +2.400000e+00 0.000000e+00 0.000000e+00 3.400000e+01 1.200000e+01 1.200000e+01 +2.800000e+00 0.000000e+00 0.000000e+00 1.500000e+01 3.500000e+00 3.500000e+00 +3.000000e+00 0.000000e+00 0.000000e+00 2.800000e+01 4.500000e+00 4.500000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1973_I84794/d02-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1973_I84794/d02-x01-y01 +Title: doi:10.17182/hepdata.6496.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.000000e+00 0.000000e+00 0.000000e+00 5.000000e+00 3.000000e+00 3.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1973_I84794/d03-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1973_I84794/d03-x01-y01 +Title: doi:10.17182/hepdata.6496.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.350000e+00 0.000000e+00 0.000000e+00 4.500000e+01 2.163331e+01 2.163331e+01 +1.450000e+00 0.000000e+00 0.000000e+00 5.500000e+01 2.051828e+01 2.051828e+01 +1.650000e+00 0.000000e+00 0.000000e+00 3.600000e+01 1.140175e+01 1.140175e+01 +1.900000e+00 0.000000e+00 0.000000e+00 1.550000e+01 5.656854e+00 5.656854e+00 +1.980000e+00 0.000000e+00 0.000000e+00 3.000000e+01 1.280625e+01 1.280625e+01 +2.100000e+00 0.000000e+00 0.000000e+00 1.700000e+01 5.656854e+00 5.656854e+00 +2.400000e+00 0.000000e+00 0.000000e+00 3.400000e+01 1.500000e+01 1.500000e+01 +2.800000e+00 0.000000e+00 0.000000e+00 1.500000e+01 4.609772e+00 4.609772e+00 +3.000000e+00 0.000000e+00 0.000000e+00 2.800000e+01 8.746428e+00 8.746428e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1973_I84794/d04-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1973_I84794/d04-x01-y01 +Title: doi:10.17182/hepdata.6496.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.350000e+00 0.000000e+00 0.000000e+00 9.400000e-01 4.548626e-01 4.548626e-01 +1.450000e+00 0.000000e+00 0.000000e+00 1.330000e+00 4.951767e-01 4.951767e-01 +1.650000e+00 0.000000e+00 0.000000e+00 1.130000e+00 3.560899e-01 3.560899e-01 +1.900000e+00 0.000000e+00 0.000000e+00 6.400000e-01 2.404163e-01 2.404163e-01 +1.980000e+00 0.000000e+00 0.000000e+00 1.350000e+00 5.762812e-01 5.762812e-01 +2.100000e+00 0.000000e+00 0.000000e+00 8.600000e-01 2.828427e-01 2.828427e-01 +2.400000e+00 0.000000e+00 0.000000e+00 2.250000e+00 1.000000e+00 1.000000e+00 +2.800000e+00 0.000000e+00 0.000000e+00 1.350000e+00 4.186884e-01 4.186884e-01 +3.000000e+00 0.000000e+00 0.000000e+00 2.900000e+00 9.106591e-01 9.106591e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.cc b/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class GAMMAGAMMA_1975_I100016 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(GAMMAGAMMA_1975_I100016); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(1,1,1); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 2); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(GAMMAGAMMA_1975_I100016); + + +} diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.info b/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.info @@ -0,0 +1,32 @@ +Name: GAMMAGAMMA_1975_I100016 +Year: 1975 +Summary: Measurement of $R$ and the hadronic cross section for energies between 1.91 and 2.97 GeV +Experiment: GAMMAGAMMA +Collider: ADONE +InspireID: 100016 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B58 (1975) 481-483, 1975 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ and the hadronic cross section in $e^+e^-$ collisions by the GAMMA-GAMMA group for energies between 1.91 and 2.97 GeV. + The muonic cross section is also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Bacci:1975eb +BibTeX: '@article{Bacci:1975eb, + author = "Bacci, C. and others", + title = "{Search for Narrow Resonances in e+ e- Annihilation Into + Hadrons in the Mass Regions 1910-MeV-2545-MeV and + 2970-MeV-3090-MeV}", + journal = "Phys. Lett.", + volume = "58B", + year = "1975", + pages = "481-483", + doi = "10.1016/0370-2693(75)90707-8", + reportNumber = "LNF-75/38-P", + SLACcitation = "%%CITATION = PHLTA,58B,481;%%" +}' diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.plot b/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /GAMMAGAMMA_1975_I100016/d01-x01-y02 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1975_I100016/d01-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1975_I100016/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.yoda b/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1975_I100016.yoda @@ -0,0 +1,22 @@ +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1975_I100016/d01-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1975_I100016/d01-x01-y01 +Title: doi:10.17182/hepdata.27776.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.055000e+00 1.450000e-01 1.450000e-01 2.900000e+01 1.040829e+01 1.040829e+01 +2.372500e+00 1.725000e-01 1.725000e-01 3.000000e+01 1.050000e+01 1.050000e+01 +3.030000e+00 6.000000e-02 6.000000e-02 2.500000e+01 9.182184e+00 9.182184e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1975_I100016/d01-x01-y02 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1975_I100016/d01-x01-y02 +Title: doi:10.17182/hepdata.27776.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.055000e+00 1.450000e-01 1.450000e-01 1.400000e+00 4.729693e-01 4.729693e-01 +2.372500e+00 1.725000e-01 1.725000e-01 1.900000e+00 6.908871e-01 6.908871e-01 +3.030000e+00 6.000000e-02 6.000000e-02 2.600000e+00 9.272001e-01 9.272001e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.cc b/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class GAMMAGAMMA_1979_I133588 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(GAMMAGAMMA_1979_I133588); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(1,1,2); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(GAMMAGAMMA_1979_I133588); + + +} diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.info b/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.info @@ -0,0 +1,32 @@ +Name: GAMMAGAMMA_1979_I133588 +Year: 1979 +Summary: Measurement of $R$ and the hadronic cross section for energies between 1.92 and 3.09 GeV +Experiment: GAMMAGAMMA +Collider: ADONE +InspireID: 133588 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Lett.Nuovo Cim. 24 (1979) 324, 1979 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ and the hadronic cross section in $e^+e^-$ collisions by the GAMMA-GAMMA group for energies between 1.92 and 3.09 GeV. + The muonic cross section is also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Bacci:1978mq +BibTeX: '@article{Bacci:1978mq, + author = "Bacci, C. and others", + title = "{Total Hadronic Cross-section From $e^+ e^-$ Annihilation + in the Total Center-of-mass Energy Range 1920-{MeV} - + 3090-{MeV}}", + journal = "Lett. Nuovo Cim.", + volume = "24", + year = "1979", + pages = "324", + doi = "10.1007/BF02724851", + reportNumber = "LNF-78/56-P", + SLACcitation = "%%CITATION = NCLTA,24,324;%%" +}' diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.plot b/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /GAMMAGAMMA_1979_I133588/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1979_I133588/d01-x01-y02 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1979_I133588/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.yoda b/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1979_I133588.yoda @@ -0,0 +1,32 @@ +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1979_I133588/d01-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1979_I133588/d01-x01-y01 +Title: doi:10.17182/hepdata.37911.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.960000e+00 4.000000e-02 4.000000e-02 1.740000e+00 1.700000e-01 1.700000e-01 +2.050000e+00 5.000000e-02 5.000000e-02 1.860000e+00 1.900000e-01 1.900000e-01 +2.150000e+00 5.000000e-02 5.000000e-02 2.090000e+00 1.300000e-01 1.300000e-01 +2.370000e+00 1.700000e-01 1.700000e-01 2.690000e+00 2.700000e-01 2.700000e-01 +2.590000e+00 5.000000e-02 5.000000e-02 2.890000e+00 2.900000e-01 2.900000e-01 +2.700000e+00 6.000000e-02 6.000000e-02 2.990000e+00 3.000000e-01 3.000000e-01 +2.870000e+00 1.100000e-01 1.100000e-01 2.380000e+00 1.900000e-01 1.900000e-01 +3.035000e+00 5.500000e-02 5.500000e-02 2.460000e+00 2.700000e-01 2.700000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1979_I133588/d01-x01-y02 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1979_I133588/d01-x01-y02 +Title: doi:10.17182/hepdata.37911.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.960000e+00 4.000000e-02 4.000000e-02 3.930000e+01 3.800000e+00 3.800000e+00 +2.050000e+00 5.000000e-02 5.000000e-02 3.840000e+01 3.900000e+00 3.900000e+00 +2.150000e+00 5.000000e-02 5.000000e-02 3.930000e+01 2.400000e+00 2.400000e+00 +2.370000e+00 1.700000e-01 1.700000e-01 4.160000e+01 4.200000e+00 4.200000e+00 +2.590000e+00 5.000000e-02 5.000000e-02 3.740000e+01 3.800000e+00 3.800000e+00 +2.700000e+00 6.000000e-02 6.000000e-02 3.560000e+01 3.600000e+00 3.600000e+00 +2.870000e+00 1.100000e-01 1.100000e-01 2.510000e+01 2.000000e+00 2.000000e+00 +3.035000e+00 5.500000e-02 5.500000e-02 2.320000e+01 2.500000e+00 2.500000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.cc b/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.cc @@ -0,0 +1,140 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class GAMMAGAMMA_1979_I141722 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(GAMMAGAMMA_1979_I141722); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + _c_charged = bookCounter("/TMP/Ncharged"); + _c_neutral = bookCounter("/TMP/Nneutral"); + _nHadrons = 0.; + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0),ncharged(0),nneutral(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) + ncharged += 1; + else + nneutral += 1; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else { + if(ntotal==2) vetoEvent; + _c_hadrons->fill(event.weight()); + _c_charged->fill(ncharged*event.weight()); + _c_neutral->fill(nneutral*event.weight()); + _nHadrons += event.weight(); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + scale(_c_charged, 1./_nHadrons); + scale(_c_neutral, 1./_nHadrons); + for(unsigned int iy=1; iy<3;++iy) { + double aver(0.),error(0.); + if(iy==1) { + aver = _c_charged->val(); + error = _c_charged->err(); + } + else { + aver = _c_neutral->val(); + error = _c_neutral->err(); + } + Scatter2D temphisto(refData(2, 1, iy)); + Scatter2DPtr mult = bookScatter2D(2, 1, iy); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, aver, ex, make_pair(error,error)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons,_c_neutral,_c_charged; + double _nHadrons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(GAMMAGAMMA_1979_I141722); + + +} diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.info b/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.info @@ -0,0 +1,33 @@ +Name: GAMMAGAMMA_1979_I141722 +Year: 1979 +Summary: Measurement of $R$ and the hadron multiplicity between 1.42 and 3.09 GeV +Experiment: GAMMAGAMMA +Collider: ADONE +InspireID: 141722 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B86 (1979) 234-238, 1979 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by Gamma-Gamma-2 for energies between 1.42 and 3.09 GeV. + The average charged and neutral particle multiplicity is also measured. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Bacci:1979ab +BibTeX: '@article{Bacci:1979ab, + author = "Bacci, C. and others", + title = "{Total Cross-Section for Hadronic Production by e+ e- + Annihilation in the Total Center-Of-Mass Energy Range + 1.42-GeV - 3.09-GeV}", + journal = "Phys. Lett.", + volume = "86B", + year = "1979", + pages = "234-238", + doi = "10.1016/0370-2693(79)90828-1", + reportNumber = "LNF-79/34-P", + SLACcitation = "%%CITATION = PHLTA,86B,234;%%" +}' diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.plot b/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.plot @@ -0,0 +1,35 @@ +BEGIN PLOT /GAMMAGAMMA_1979_I141722/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1979_I141722/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1979_I141722/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1979_I141722/d02-x01-y01 +Title=Average Charged particle Multiplicity +XLabel=$\sqrt{s}$/GeV +YLabel=$N_{\text{charged}}$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1979_I141722/d02-x01-y02 +Title=Average Neutral particle Multiplicity +XLabel=$\sqrt{s}$/GeV +YLabel=$N_{\text{neutral}}$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.yoda b/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1979_I141722.yoda @@ -0,0 +1,91 @@ +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1979_I141722/d01-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1979_I141722/d01-x01-y01 +Title: doi:10.17182/hepdata.27311.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.435000e+00 1.600000e-02 1.500000e-02 1.460000e+00 3.456776e-01 3.456776e-01 +1.464000e+00 1.400000e-02 1.100000e-02 1.580000e+00 3.721519e-01 3.721519e-01 +1.491000e+00 1.600000e-02 9.000000e-03 1.930000e+00 4.102539e-01 4.102539e-01 +1.506000e+00 6.000000e-03 1.800000e-02 2.040000e+00 4.322823e-01 4.322823e-01 +1.525000e+00 0.000000e+00 0.000000e+00 2.380000e+00 5.750974e-01 5.750974e-01 +1.539000e+00 1.300000e-02 1.000000e-02 2.280000e+00 5.576128e-01 5.576128e-01 +1.550000e+00 0.000000e+00 0.000000e+00 2.200000e+00 5.550676e-01 5.550676e-01 +1.560000e+00 9.000000e-03 1.400000e-02 2.200000e+00 6.181424e-01 6.181424e-01 +1.575000e+00 0.000000e+00 0.000000e+00 2.090000e+00 5.138524e-01 5.138524e-01 +1.587000e+00 1.100000e-02 1.300000e-02 1.860000e+00 4.994327e-01 4.994327e-01 +1.610000e+00 1.000000e-02 1.500000e-02 2.070000e+00 4.945789e-01 4.945789e-01 +1.638000e+00 1.300000e-02 1.200000e-02 1.780000e+00 4.330785e-01 4.330785e-01 +1.663000e+00 1.300000e-02 1.200000e-02 2.350000e+00 5.698300e-01 5.698300e-01 +1.687000e+00 1.200000e-02 1.300000e-02 2.100000e+00 5.267115e-01 5.267115e-01 +1.713000e+00 1.300000e-02 1.200000e-02 2.100000e+00 5.210806e-01 5.210806e-01 +1.738000e+00 1.300000e-02 1.200000e-02 1.940000e+00 5.060168e-01 5.060168e-01 +1.764000e+00 1.400000e-02 1.100000e-02 1.680000e+00 4.271440e-01 4.271440e-01 +1.790000e+00 1.500000e-02 1.000000e-02 1.820000e+00 4.803925e-01 4.803925e-01 +1.812000e+00 1.200000e-02 1.300000e-02 1.700000e+00 4.035158e-01 4.035158e-01 +1.834000e+00 9.000000e-03 1.600000e-02 1.910000e+00 4.611337e-01 4.611337e-01 +1.859000e+00 9.000000e-03 1.600000e-02 1.550000e+00 4.382993e-01 4.382993e-01 +1.886000e+00 1.100000e-02 1.400000e-02 1.740000e+00 4.874146e-01 4.874146e-01 +1.930000e+00 3.000000e-02 4.200000e-02 1.580000e+00 3.987443e-01 3.987443e-01 +1.960000e+00 4.000000e-02 4.000000e-02 1.610000e+00 3.684620e-01 3.684620e-01 +2.050000e+00 5.000000e-02 5.000000e-02 1.760000e+00 4.050284e-01 4.050284e-01 +2.150000e+00 5.000000e-02 5.000000e-02 2.000000e+00 4.294182e-01 4.294182e-01 +2.370000e+00 1.700000e-01 1.700000e-01 2.610000e+00 5.975904e-01 5.975904e-01 +2.590000e+00 5.000000e-02 5.000000e-02 2.770000e+00 6.360018e-01 6.360018e-01 +2.700000e+00 6.000000e-02 6.000000e-02 2.850000e+00 6.552147e-01 6.552147e-01 +2.870000e+00 1.100000e-01 1.100000e-01 2.260000e+00 4.994727e-01 4.994727e-01 +3.035000e+00 5.500000e-02 5.500000e-02 2.320000e+00 5.396777e-01 5.396777e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1979_I141722/d02-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1979_I141722/d02-x01-y01 +Title: doi:10.17182/hepdata.27311.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.435000e+00 1.600000e-02 1.500000e-02 3.050000e+00 1.300000e-01 1.300000e-01 +1.485000e+00 3.500000e-02 1.500000e-02 3.040000e+00 5.000000e-02 5.000000e-02 +1.511000e+00 1.100000e-02 3.900000e-02 3.150000e+00 5.000000e-02 5.000000e-02 +1.570000e+00 2.000000e-02 3.000000e-02 3.120000e+00 9.000000e-02 9.000000e-02 +1.624000e+00 2.400000e-02 2.600000e-02 3.250000e+00 1.000000e-01 1.000000e-01 +1.675000e+00 2.500000e-02 2.500000e-02 3.070000e+00 1.100000e-01 1.100000e-01 +1.725000e+00 2.500000e-02 2.500000e-02 3.140000e+00 1.200000e-01 1.200000e-01 +1.776000e+00 2.600000e-02 2.400000e-02 3.000000e+00 1.300000e-01 1.300000e-01 +1.822000e+00 2.200000e-02 2.800000e-02 3.240000e+00 1.000000e-01 1.000000e-01 +1.872000e+00 2.200000e-02 2.800000e-02 3.180000e+00 1.500000e-01 1.500000e-01 +1.930000e+00 3.000000e-02 4.200000e-02 3.090000e+00 1.700000e-01 1.700000e-01 +1.960000e+00 4.000000e-02 4.000000e-02 3.200000e+00 1.100000e-01 1.100000e-01 +2.050000e+00 5.000000e-02 5.000000e-02 3.350000e+00 1.100000e-01 1.100000e-01 +2.150000e+00 5.000000e-02 5.000000e-02 3.530000e+00 7.000000e-02 7.000000e-02 +2.370000e+00 1.700000e-01 1.700000e-01 3.380000e+00 1.100000e-01 1.100000e-01 +2.590000e+00 5.000000e-02 5.000000e-02 3.400000e+00 1.200000e-01 1.200000e-01 +2.700000e+00 6.000000e-02 5.000000e-02 3.630000e+00 1.200000e-01 1.200000e-01 +2.870000e+00 1.100000e-01 1.100000e-01 3.600000e+00 1.100000e-01 1.100000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1979_I141722/d02-x01-y02 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1979_I141722/d02-x01-y02 +Title: doi:10.17182/hepdata.27311.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.435000e+00 1.600000e-02 1.500000e-02 1.340000e+00 1.300000e-01 1.300000e-01 +1.485000e+00 3.500000e-02 1.500000e-02 1.170000e+00 5.000000e-02 5.000000e-02 +1.511000e+00 1.100000e-02 3.900000e-02 1.310000e+00 5.000000e-02 5.000000e-02 +1.570000e+00 2.000000e-02 3.000000e-02 1.340000e+00 9.000000e-02 9.000000e-02 +1.624000e+00 2.400000e-02 2.600000e-02 1.280000e+00 1.000000e-01 1.000000e-01 +1.675000e+00 2.500000e-02 2.500000e-02 1.340000e+00 1.100000e-01 1.100000e-01 +1.725000e+00 2.500000e-02 2.500000e-02 1.620000e+00 1.200000e-01 1.200000e-01 +1.776000e+00 2.600000e-02 2.400000e-02 1.440000e+00 1.300000e-01 1.300000e-01 +1.822000e+00 2.200000e-02 2.800000e-02 1.610000e+00 1.000000e-01 1.000000e-01 +1.872000e+00 2.200000e-02 2.800000e-02 1.420000e+00 1.500000e-01 1.500000e-01 +1.930000e+00 3.000000e-02 4.200000e-02 1.730000e+00 1.700000e-01 1.700000e-01 +1.960000e+00 4.000000e-02 4.000000e-02 1.750000e+00 1.500000e-01 1.500000e-01 +2.050000e+00 5.000000e-02 5.000000e-02 1.850000e+00 1.500000e-01 1.500000e-01 +2.150000e+00 5.000000e-02 5.000000e-02 1.900000e+00 1.000000e-01 1.000000e-01 +2.370000e+00 1.700000e-01 1.700000e-01 1.900000e+00 1.500000e-01 1.500000e-01 +2.590000e+00 5.000000e-02 5.000000e-02 2.350000e+00 1.600000e-01 1.600000e-01 +2.700000e+00 6.000000e-02 5.000000e-02 2.400000e+00 1.600000e-01 1.600000e-01 +2.870000e+00 1.100000e-01 1.100000e-01 2.250000e+00 1.500000e-01 1.500000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.cc b/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.cc @@ -0,0 +1,78 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class GAMMAGAMMA_1980_I153382 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(GAMMAGAMMA_1980_I153382); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=4) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(GAMMAGAMMA_1980_I153382); + + +} diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.info b/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.info @@ -0,0 +1,31 @@ +Name: GAMMAGAMMA_1980_I153382 +Year: 1980 +Summary: Cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ between 1.456 and 2.15 GeV +Experiment: GAMMAGAMMA +Collider: ADONE +InspireID: 153382 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B95 (1980) 139-142, 1980 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ for energies between 1.456 and 2.15 GeV' +Keywords: +BibKey: Bacci:1980ru +BibTeX: '@article{Bacci:1980ru, + author = "Bacci, C. and others", + title = "{Measurement of the $e^+ e^- \to \pi^+ \pi^- \pi^+ \pi^-$ + Cross-section in the $\rho^\prime$ (1600) Energy Region}", + journal = "Phys. Lett.", + volume = "95B", + year = "1980", + pages = "139-142", + doi = "10.1016/0370-2693(80)90418-9", + reportNumber = "LNF-80/25-P", + SLACcitation = "%%CITATION = PHLTA,95B,139;%%" +}' diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.plot b/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /GAMMAGAMMA_1980_I153382/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.yoda b/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1980_I153382.yoda @@ -0,0 +1,23 @@ +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1980_I153382/d01-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1980_I153382/d01-x01-y01 +Title: doi:10.17182/hepdata.27154.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.456000e+00 3.700000e-02 1.900000e-02 2.260000e+01 5.319972e+00 5.319972e+00 +1.491000e+00 1.600000e-02 9.000000e-03 3.060000e+01 5.134014e+00 5.134014e+00 +1.507000e+00 7.000000e-03 1.800000e-02 2.340000e+01 4.490000e+00 4.490000e+00 +1.546000e+00 2.100000e-02 2.900000e-02 2.630000e+01 5.273806e+00 5.273806e+00 +1.600000e+00 2.500000e-02 1.500000e-02 2.440000e+01 5.064148e+00 5.064148e+00 +1.633000e+00 1.800000e-02 1.700000e-02 2.240000e+01 4.438423e+00 4.438423e+00 +1.660000e+00 1.000000e-02 1.000000e-02 2.930000e+01 6.010493e+00 6.010493e+00 +1.701000e+00 3.100000e-02 2.400000e-02 1.730000e+01 3.402062e+00 3.402062e+00 +1.752000e+00 2.700000e-02 2.300000e-02 1.680000e+01 3.480000e+00 3.480000e+00 +1.794000e+00 1.900000e-02 1.100000e-02 1.320000e+01 3.189106e+00 3.189106e+00 +1.821000e+00 1.600000e-02 1.400000e-02 1.010000e+01 2.589445e+00 2.589445e+00 +1.851000e+00 1.600000e-02 2.400000e-02 1.190000e+01 2.911396e+00 2.911396e+00 +1.935000e+00 6.000000e-02 6.500000e-02 8.200000e+00 1.863572e+00 1.863572e+00 +2.050000e+00 5.000000e-02 5.000000e-02 8.300000e+00 2.441316e+00 2.441316e+00 +2.150000e+00 5.000000e-02 5.000000e-02 5.300000e+00 1.523819e+00 1.523819e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.cc b/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.cc @@ -0,0 +1,177 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class GAMMAGAMMA_1981_I158474 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(GAMMAGAMMA_1981_I158474); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + _n3pi = bookCounter("TMP/n3pi"); + _n4pi = bookCounter("TMP/n4pi"); + _n5pi = bookCounter("TMP/n5pi"); + _n6pi = bookCounter("TMP/n6pi"); + _n35pi = bookCounter("TMP/n35pi"); + _n46pi = bookCounter("TMP/n46pi"); + _nC2 = bookCounter("TMP/nC2"); + _nC4 = bookCounter("TMP/nC4"); + _nmu = bookCounter("TMP/nmu"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _nmu->fill(event.weight()); + else { + if(ntotal==3 && nCount[211] == 1 && nCount[-211]==1 && nCount[111]==1 ) { + _n3pi->fill(event.weight()); + } + if(ntotal==4 && nCount[211] == 1 && nCount[-211]==1 && nCount[111]==2 ) { + _n4pi->fill(event.weight()); + } + if(ntotal==5 && nCount[211] == 2 && nCount[-211]==2 && nCount[111]==1 ) { + _n5pi->fill(event.weight()); + } + if(ntotal==6 && nCount[211] == 2 && nCount[-211]==2 && nCount[111]==2 ) { + _n6pi->fill(event.weight()); + } + if(nCount[211] == 1 && nCount[-211]==1 && ntotal == 2+nCount[111]) { + _nC2->fill(event.weight()); + } + if(nCount[211] == 2 && nCount[-211]==2 && ntotal == 4+nCount[111]) { + _nC4->fill(event.weight()); + } + if((nCount[211]+nCount[-211]+nCount[111])==ntotal ) { + if(ntotal==3 || ntotal ==5) + _n35pi->fill(event.weight()); + else if(ntotal==4 || ntotal==6) + _n46pi ->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /nanobarn; + for(unsigned int ix=1;ix<7;++ix) { + double sigma,error; + if(ix==1) { + sigma = _n3pi->val()*fact; + error = _n3pi->err()*fact; + } + else if(ix==2) { + sigma = _n4pi->val()*fact; + error = _n4pi->err()*fact; + } + else if(ix==3) { + sigma = _n5pi->val()*fact; + error = _n5pi->err()*fact; + } + else if(ix==4) { + sigma = _n6pi->val()*fact; + error = _n6pi->err()*fact; + } + else if(ix==5) { + sigma = _n35pi->val()*fact; + error = _n35pi->err()*fact; + } + else if(ix==6) { + sigma = _n46pi->val()*fact; + error = _n46pi->err()*fact; + } + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + for(unsigned int ix=1;ix<3;++ix) { + Scatter1D R = (ix==1? *_nC2 : *_nC4)/ *_nmu; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double sig_h = (ix ==1 ? _nC2 : _nC4)->val()*fact; + double err_h = (ix ==1 ? _nC2 : _nC4)->err()*fact; + double sig_m = _nmu->val()*fact; + double err_m = _nmu->err()*fact; + Scatter2D temphisto(refData(2, 1, ix)); + ostringstream title; + if(ix==1) + title << "sigma_2pi"; + else + title << "sigma_4pi"; + Scatter2DPtr hadrons = bookScatter2D(title.str()); + Scatter2DPtr muons; + if(ix==1) muons = bookScatter2D("sigma_muons"); + Scatter2DPtr mult = bookScatter2D(2,1,ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + if(ix==1) muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + if(ix==1) muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _n3pi,_n4pi,_n5pi,_n6pi,_n35pi,_n46pi,_nC2,_nC4,_nmu; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(GAMMAGAMMA_1981_I158474); + + +} diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.info b/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.info @@ -0,0 +1,31 @@ +Name: GAMMAGAMMA_1981_I158474 +Year: 1981 +Summary: Multi pion cross sections for energies between 1.44 and 2.15 GeV +Experiment: GAMMAGAMMA +Collider: ADONE +InspireID: 158474 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Nucl.Phys. B184 (1981) 31-39, 1981 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to$pions for energies between 1.44 and 2.15 GeV' +Keywords: +BibKey: Bacci:1980zs +BibTeX: '@article{Bacci:1980zs, + author = "Bacci, C. and others", + title = "{Measurement of Hadronic Exclusive Cross-sections in $e^+ + e^-$ Annihilation From 1.42-{GeV} to 2.20-{GeV}}", + journal = "Nucl. Phys.", + volume = "B184", + year = "1981", + pages = "31-39", + doi = "10.1016/0550-3213(81)90208-X", + reportNumber = "LNF-80/72-P", + SLACcitation = "%%CITATION = NUPHA,B184,31;%%" +}' diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.plot b/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.plot @@ -0,0 +1,77 @@ +BEGIN PLOT /GAMMAGAMMA_1981_I158474/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1981_I158474/d01-x01-y02 +Title=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$/nb +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1981_I158474/d01-x01-y03 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-\pi^0)$/nb +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1981_I158474/d01-x01-y04 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-2\pi^0)$/nb +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1981_I158474/d01-x01-y05 +Title=$\sigma(e^+e^-\to 3\pi+5\pi)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 3\pi+5\pi)$/nb +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1981_I158474/d01-x01-y06 +Title=$\sigma(e^+e^-\to 4\pi+6\pi)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 4\pi^+6\pi^-)$/nb +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1981_I158474/d02-x01-y01 +Title==$R=\sigma(e^+e^-\to \pi^+\pi^-+n\pi^0)/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1981_I158474/d02-x01-y02 +Title==$R=\sigma(e^+e^-\to 2\pi^+2\pi^-+n\pi^0)/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1981_I158474/sigma_2pi +Title=$\sigma(e^+e^-\to \pi^+\pi^-+n\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-+n\pi^0)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1981_I158474/sigma_4pi +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-+n\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-+n\pi^0)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /GAMMAGAMMA_1981_I158474/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.yoda b/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/GAMMAGAMMA_1981_I158474.yoda @@ -0,0 +1,192 @@ +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1981_I158474/d01-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1981_I158474/d01-x01-y01 +Title: doi:10.17182/hepdata.34278.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.437000e+00 1.700000e-02 3.800000e-02 5.200000e+00 3.400000e+00 3.400000e+00 +1.491000e+00 1.600000e-02 9.000000e-03 0.000000e+00 1.200000e+00 1.200000e+00 +1.505000e+00 5.000000e-03 2.000000e-02 4.000000e-01 1.100000e+00 1.100000e+00 +1.549000e+00 2.400000e-02 2.600000e-02 1.000000e-01 1.300000e+00 1.300000e+00 +1.600000e+00 2.500000e-02 1.500000e-02 0.000000e+00 2.600000e+00 2.600000e+00 +1.633000e+00 1.800000e-02 1.700000e-02 0.000000e+00 3.600000e+00 3.600000e+00 +1.660000e+00 1.000000e-02 1.000000e-02 1.220000e+01 8.000000e+00 8.000000e+00 +1.701000e+00 3.100000e-02 2.400000e-02 0.000000e+00 1.500000e+00 1.500000e+00 +1.752000e+00 2.700000e-02 2.300000e-02 0.000000e+00 2.400000e+00 2.400000e+00 +1.794000e+00 1.900000e-02 1.100000e-02 0.000000e+00 3.200000e+00 3.200000e+00 +1.821000e+00 1.600000e-02 1.400000e-02 6.000000e-01 4.800000e+00 4.800000e+00 +1.851000e+00 1.600000e-02 2.400000e-02 4.900000e+00 5.000000e+00 5.000000e+00 +1.935000e+00 6.000000e-02 6.500000e-02 0.000000e+00 1.700000e+00 1.700000e+00 +2.050000e+00 5.000000e-02 5.000000e-02 0.000000e+00 3.000000e+00 3.000000e+00 +2.150000e+00 5.000000e-02 5.000000e-02 0.000000e+00 2.000000e+00 2.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1981_I158474/d01-x01-y02 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1981_I158474/d01-x01-y02 +Title: doi:10.17182/hepdata.34278.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.437000e+00 1.700000e-02 3.800000e-02 1.670000e+01 4.700000e+00 4.700000e+00 +1.491000e+00 1.600000e-02 9.000000e-03 3.160000e+01 2.700000e+00 2.700000e+00 +1.505000e+00 5.000000e-03 2.000000e-02 2.800000e+01 3.100000e+00 3.100000e+00 +1.549000e+00 2.400000e-02 2.600000e-02 3.120000e+01 3.400000e+00 3.400000e+00 +1.600000e+00 2.500000e-02 1.500000e-02 1.690000e+01 5.800000e+00 5.800000e+00 +1.633000e+00 1.800000e-02 1.700000e-02 2.000000e+01 4.900000e+00 4.900000e+00 +1.660000e+00 1.000000e-02 1.000000e-02 2.010000e+01 8.100000e+00 8.100000e+00 +1.701000e+00 3.100000e-02 2.400000e-02 2.730000e+01 4.400000e+00 4.400000e+00 +1.752000e+00 2.700000e-02 2.300000e-02 2.210000e+01 4.500000e+00 4.500000e+00 +1.794000e+00 1.900000e-02 1.100000e-02 2.710000e+01 5.400000e+00 5.400000e+00 +1.821000e+00 1.600000e-02 1.400000e-02 1.630000e+01 4.900000e+00 4.900000e+00 +1.851000e+00 1.600000e-02 2.400000e-02 1.040000e+01 5.500000e+00 5.500000e+00 +1.935000e+00 6.000000e-02 6.500000e-02 1.690000e+01 3.200000e+00 3.200000e+00 +2.050000e+00 5.000000e-02 5.000000e-02 1.660000e+01 4.000000e+00 4.000000e+00 +2.150000e+00 5.000000e-02 5.000000e-02 1.500000e+01 2.700000e+00 2.700000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1981_I158474/d01-x01-y03 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1981_I158474/d01-x01-y03 +Title: doi:10.17182/hepdata.34278.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.437000e+00 1.700000e-02 3.800000e-02 4.400000e+00 2.400000e+00 2.400000e+00 +1.491000e+00 1.600000e-02 9.000000e-03 6.200000e+00 1.500000e+00 1.500000e+00 +1.505000e+00 5.000000e-03 2.000000e-02 6.100000e+00 1.900000e+00 1.900000e+00 +1.549000e+00 2.400000e-02 2.600000e-02 7.100000e+00 2.400000e+00 2.400000e+00 +1.600000e+00 2.500000e-02 1.500000e-02 6.700000e+00 4.900000e+00 4.900000e+00 +1.633000e+00 1.800000e-02 1.700000e-02 3.900000e+00 3.900000e+00 3.900000e+00 +1.660000e+00 1.000000e-02 1.000000e-02 0.000000e+00 5.000000e+00 5.000000e+00 +1.701000e+00 3.100000e-02 2.400000e-02 0.000000e+00 4.000000e+00 4.000000e+00 +1.752000e+00 2.700000e-02 2.300000e-02 3.400000e+00 3.400000e+00 3.400000e+00 +1.794000e+00 1.900000e-02 1.100000e-02 4.100000e+00 2.800000e+00 2.800000e+00 +1.821000e+00 1.600000e-02 1.400000e-02 6.700000e+00 3.400000e+00 3.400000e+00 +1.851000e+00 1.600000e-02 2.400000e-02 1.000000e-01 3.200000e+00 3.200000e+00 +1.935000e+00 6.000000e-02 6.500000e-02 2.500000e+00 2.300000e+00 2.300000e+00 +2.050000e+00 5.000000e-02 5.000000e-02 2.400000e+00 3.200000e+00 3.200000e+00 +2.150000e+00 5.000000e-02 5.000000e-02 2.700000e+00 1.600000e+00 1.600000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1981_I158474/d01-x01-y04 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1981_I158474/d01-x01-y04 +Title: doi:10.17182/hepdata.34278.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.437000e+00 1.700000e-02 3.800000e-02 6.600000e+00 2.900000e+00 2.900000e+00 +1.491000e+00 1.600000e-02 9.000000e-03 2.900000e+00 1.800000e+00 1.800000e+00 +1.505000e+00 5.000000e-03 2.000000e-02 8.700000e+00 2.100000e+00 2.100000e+00 +1.549000e+00 2.400000e-02 2.600000e-02 1.150000e+01 3.000000e+00 3.000000e+00 +1.600000e+00 2.500000e-02 1.500000e-02 1.210000e+01 6.300000e+00 6.300000e+00 +1.633000e+00 1.800000e-02 1.700000e-02 8.700000e+00 4.600000e+00 4.600000e+00 +1.660000e+00 1.000000e-02 1.000000e-02 1.350000e+01 4.600000e+00 4.600000e+00 +1.701000e+00 3.100000e-02 2.400000e-02 1.380000e+01 2.600000e+00 2.600000e+00 +1.752000e+00 2.700000e-02 2.300000e-02 6.500000e+00 3.200000e+00 3.200000e+00 +1.794000e+00 1.900000e-02 1.100000e-02 2.400000e+00 2.500000e+00 2.500000e+00 +1.821000e+00 1.600000e-02 1.400000e-02 1.260000e+01 3.200000e+00 3.200000e+00 +1.851000e+00 1.600000e-02 2.400000e-02 1.020000e+01 2.900000e+00 2.900000e+00 +1.935000e+00 6.000000e-02 6.500000e-02 1.020000e+01 2.300000e+00 2.300000e+00 +2.050000e+00 5.000000e-02 5.000000e-02 9.700000e+00 2.800000e+00 2.800000e+00 +2.150000e+00 5.000000e-02 5.000000e-02 1.340000e+01 1.700000e+00 1.700000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1981_I158474/d01-x01-y05 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1981_I158474/d01-x01-y05 +Title: doi:10.17182/hepdata.34278.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.437000e+00 1.700000e-02 3.800000e-02 1.170000e+01 4.900000e+00 4.900000e+00 +1.491000e+00 1.600000e-02 9.000000e-03 9.300000e+00 2.600000e+00 2.600000e+00 +1.505000e+00 5.000000e-03 2.000000e-02 9.300000e+00 3.100000e+00 3.100000e+00 +1.549000e+00 2.400000e-02 2.600000e-02 1.030000e+01 3.800000e+00 3.800000e+00 +1.600000e+00 2.500000e-02 1.500000e-02 1.000000e+01 7.800000e+00 7.800000e+00 +1.633000e+00 1.800000e-02 1.700000e-02 5.900000e+00 6.900000e+00 6.900000e+00 +1.660000e+00 1.000000e-02 1.000000e-02 8.900000e+00 1.100000e+01 1.100000e+01 +1.701000e+00 3.100000e-02 2.400000e-02 0.000000e+00 6.200000e+00 6.200000e+00 +1.752000e+00 2.700000e-02 2.300000e-02 5.000000e+00 5.600000e+00 5.600000e+00 +1.794000e+00 1.900000e-02 1.100000e-02 6.100000e+00 5.300000e+00 5.300000e+00 +1.821000e+00 1.600000e-02 1.400000e-02 1.060000e+01 7.000000e+00 7.000000e+00 +1.851000e+00 1.600000e-02 2.400000e-02 5.100000e+00 6.900000e+00 6.900000e+00 +1.935000e+00 6.000000e-02 6.500000e-02 3.600000e+00 4.000000e+00 4.000000e+00 +2.050000e+00 5.000000e-02 5.000000e-02 3.600000e+00 5.700000e+00 5.700000e+00 +2.150000e+00 5.000000e-02 5.000000e-02 4.100000e+00 3.100000e+00 3.100000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1981_I158474/d01-x01-y06 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1981_I158474/d01-x01-y06 +Title: doi:10.17182/hepdata.34278.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.437000e+00 1.700000e-02 3.800000e-02 4.590000e+01 5.600000e+00 5.600000e+00 +1.491000e+00 1.600000e-02 9.000000e-03 6.510000e+01 3.300000e+00 3.300000e+00 +1.505000e+00 5.000000e-03 2.000000e-02 6.070000e+01 3.800000e+00 3.800000e+00 +1.549000e+00 2.400000e-02 2.600000e-02 7.010000e+01 4.700000e+00 4.700000e+00 +1.600000e+00 2.500000e-02 1.500000e-02 5.340000e+01 8.900000e+00 8.900000e+00 +1.633000e+00 1.800000e-02 1.700000e-02 5.110000e+01 7.000000e+00 7.000000e+00 +1.660000e+00 1.000000e-02 1.000000e-02 6.290000e+01 9.500000e+00 9.500000e+00 +1.701000e+00 3.100000e-02 2.400000e-02 5.840000e+01 5.200000e+00 5.200000e+00 +1.752000e+00 2.700000e-02 2.300000e-02 4.540000e+01 5.700000e+00 5.700000e+00 +1.794000e+00 1.900000e-02 1.100000e-02 4.270000e+01 6.000000e+00 6.000000e+00 +1.821000e+00 1.600000e-02 1.400000e-02 3.990000e+01 5.900000e+00 5.900000e+00 +1.851000e+00 1.600000e-02 2.400000e-02 3.250000e+01 6.200000e+00 6.200000e+00 +1.935000e+00 6.000000e-02 6.500000e-02 3.560000e+01 4.000000e+00 4.000000e+00 +2.050000e+00 5.000000e-02 5.000000e-02 3.460000e+01 5.200000e+00 5.200000e+00 +2.150000e+00 5.000000e-02 5.000000e-02 3.510000e+01 3.300000e+00 3.300000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1981_I158474/d02-x01-y01 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1981_I158474/d02-x01-y01 +Title: doi:10.17182/hepdata.34278.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.437000e+00 1.700000e-02 3.800000e-02 5.800000e-01 1.300000e-01 1.300000e-01 +1.491000e+00 1.600000e-02 9.000000e-03 9.000000e-01 7.000000e-02 7.000000e-02 +1.505000e+00 5.000000e-03 2.000000e-02 8.300000e-01 7.000000e-02 7.000000e-02 +1.549000e+00 2.400000e-02 2.600000e-02 9.700000e-01 1.000000e-01 1.000000e-01 +1.600000e+00 2.500000e-02 1.500000e-02 6.000000e-01 1.700000e-01 1.700000e-01 +1.633000e+00 1.800000e-02 1.700000e-02 6.800000e-01 1.900000e-01 1.900000e-01 +1.660000e+00 1.000000e-02 1.000000e-02 1.030000e+00 2.200000e-01 2.200000e-01 +1.701000e+00 3.100000e-02 2.400000e-02 9.200000e-01 1.400000e-01 1.400000e-01 +1.752000e+00 2.700000e-02 2.300000e-02 8.500000e-01 1.700000e-01 1.700000e-01 +1.794000e+00 1.900000e-02 1.100000e-02 1.100000e+00 2.200000e-01 2.200000e-01 +1.821000e+00 1.600000e-02 1.400000e-02 7.800000e-01 2.400000e-01 2.400000e-01 +1.851000e+00 1.600000e-02 2.400000e-02 6.200000e-01 2.900000e-01 2.900000e-01 +1.935000e+00 6.000000e-02 6.500000e-02 7.900000e-01 1.500000e-01 1.500000e-01 +2.050000e+00 5.000000e-02 5.000000e-02 8.800000e-01 2.200000e-01 2.200000e-01 +2.150000e+00 5.000000e-02 5.000000e-02 8.800000e-01 1.600000e-01 1.600000e-01 +2.370000e+00 1.700000e-01 1.700000e-01 1.230000e+00 3.600000e-01 3.600000e-01 +2.590000e+00 5.000000e-02 5.000000e-02 1.300000e+00 3.800000e-01 3.800000e-01 +2.700000e+00 6.000000e-02 6.000000e-02 9.600000e-01 2.000000e-01 2.000000e-01 +2.870000e+00 1.100000e-01 1.100000e-01 8.300000e-01 1.900000e-01 1.900000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/GAMMAGAMMA_1981_I158474/d02-x01-y02 +IsRef: 1 +Path: /REF/GAMMAGAMMA_1981_I158474/d02-x01-y02 +Title: doi:10.17182/hepdata.34278.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.437000e+00 1.700000e-02 3.800000e-02 7.400000e-01 6.000000e-02 6.000000e-02 +1.491000e+00 1.600000e-02 9.000000e-03 9.100000e-01 4.000000e-02 4.000000e-02 +1.505000e+00 5.000000e-03 2.000000e-02 9.900000e-01 5.000000e-02 5.000000e-02 +1.549000e+00 2.400000e-02 2.600000e-02 1.130000e+00 7.000000e-02 7.000000e-02 +1.600000e+00 2.500000e-02 1.500000e-02 1.280000e+00 1.400000e-01 1.400000e-01 +1.633000e+00 1.800000e-02 1.700000e-02 1.080000e+00 1.100000e-01 1.100000e-01 +1.660000e+00 1.000000e-02 1.000000e-02 1.370000e+00 1.300000e-01 1.300000e-01 +1.701000e+00 3.100000e-02 2.400000e-02 1.050000e+00 9.000000e-02 9.000000e-02 +1.752000e+00 2.700000e-02 2.300000e-02 9.500000e-01 9.000000e-02 9.000000e-02 +1.794000e+00 1.900000e-02 1.100000e-02 7.400000e-01 9.000000e-02 9.000000e-02 +1.821000e+00 1.600000e-02 1.400000e-02 1.130000e+00 9.000000e-02 9.000000e-02 +1.851000e+00 1.600000e-02 2.400000e-02 8.900000e-01 1.000000e-01 1.000000e-01 +1.935000e+00 6.000000e-02 6.500000e-02 9.500000e-01 7.000000e-02 7.000000e-02 +2.050000e+00 5.000000e-02 5.000000e-02 9.900000e-01 1.100000e-01 1.100000e-01 +2.150000e+00 5.000000e-02 5.000000e-02 1.140000e+00 8.000000e-02 8.000000e-02 +2.370000e+00 1.700000e-01 1.700000e-01 1.160000e+00 1.500000e-01 1.500000e-01 +2.590000e+00 5.000000e-02 5.000000e-02 1.070000e+00 1.400000e-01 1.400000e-01 +2.700000e+00 6.000000e-02 6.000000e-02 1.630000e+00 2.500000e-01 2.500000e-01 +2.870000e+00 1.100000e-01 1.100000e-01 1.090000e+00 1.000000e-01 1.000000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/KLOE_2005_I655225.cc b/analyses/pluginFrascati/KLOE_2005_I655225.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2005_I655225.cc @@ -0,0 +1,79 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class KLOE_2005_I655225 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(KLOE_2005_I655225); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(2, 1, 1)); + Scatter2DPtr mult = bookScatter2D(2, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqr(sqrtS()/GeV), x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(KLOE_2005_I655225); + + +} diff --git a/analyses/pluginFrascati/KLOE_2005_I655225.info b/analyses/pluginFrascati/KLOE_2005_I655225.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2005_I655225.info @@ -0,0 +1,34 @@ +Name: KLOE_2005_I655225 +Year: 2005 +Summary: Cross section for $e^+e^-\to\pi^+\pi^-$ below 1 GeV +Experiment: KLOE +Collider: DAPHNE +InspireID: 655225 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B606 (2005) 12-24, 2005 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^-$ below 1 GeV' +BibKey: Aloisio:2004bu +BibTeX: '@article{Aloisio:2004bu, + author = "Aloisio, A. and others", + title = "{Measurement of $\sigma(e^+e^- \to \pi^+ \pi^- \gamma$) + and extraction of $\sigma(e^+e^- \to \pi^+ \pi^-$) below + 1-GeV with the KLOE detector}", + collaboration = "KLOE", + journal = "Phys. Lett.", + volume = "B606", + year = "2005", + pages = "12-24", + doi = "10.1016/j.physletb.2004.11.068", + eprint = "hep-ex/0407048", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0407048;%%" +}' diff --git a/analyses/pluginFrascati/KLOE_2005_I655225.plot b/analyses/pluginFrascati/KLOE_2005_I655225.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2005_I655225.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /KLOE_2005_I655225/d02-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$s/\text{GeV}^2$ +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginFrascati/KLOE_2005_I655225.yoda b/analyses/pluginFrascati/KLOE_2005_I655225.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2005_I655225.yoda @@ -0,0 +1,204 @@ +BEGIN YODA_SCATTER2D_V2 /REF/KLOE_2005_I655225/d01-x01-y01 +IsRef: 1 +Path: /REF/KLOE_2005_I655225/d01-x01-y01 +Title: doi:10.17182/hepdata.41901.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.500000e-01 0.000000e+00 0.000000e+00 1.340000e+01 2.944295e-01 2.944295e-01 +3.600000e-01 0.000000e+00 0.000000e+00 1.459000e+01 3.034545e-01 3.034545e-01 +3.700000e-01 0.000000e+00 0.000000e+00 1.578000e+01 3.129526e-01 3.129526e-01 +3.800000e-01 0.000000e+00 0.000000e+00 1.704000e+01 3.234789e-01 3.234789e-01 +3.900000e-01 0.000000e+00 0.000000e+00 1.863000e+01 3.303429e-01 3.303429e-01 +4.000000e-01 0.000000e+00 0.000000e+00 2.034000e+01 3.740614e-01 3.740614e-01 +4.100000e-01 0.000000e+00 0.000000e+00 2.264000e+01 3.750150e-01 3.750150e-01 +4.200000e-01 0.000000e+00 0.000000e+00 2.456000e+01 4.130585e-01 4.130585e-01 +4.300000e-01 0.000000e+00 0.000000e+00 2.707000e+01 4.439720e-01 4.439720e-01 +4.400000e-01 0.000000e+00 0.000000e+00 2.999000e+01 4.675498e-01 4.675498e-01 +4.500000e-01 0.000000e+00 0.000000e+00 3.265000e+01 5.010944e-01 5.010944e-01 +4.600000e-01 0.000000e+00 0.000000e+00 3.624000e+01 5.344723e-01 5.344723e-01 +4.700000e-01 0.000000e+00 0.000000e+00 4.010000e+01 5.870244e-01 5.870244e-01 +4.800000e-01 0.000000e+00 0.000000e+00 4.434000e+01 6.438927e-01 6.438927e-01 +4.900000e-01 0.000000e+00 0.000000e+00 4.894000e+01 6.829422e-01 6.829422e-01 +5.000000e-01 0.000000e+00 0.000000e+00 5.410000e+01 7.963311e-01 7.963311e-01 +5.100000e-01 0.000000e+00 0.000000e+00 5.977000e+01 8.253105e-01 8.253105e-01 +5.200000e-01 0.000000e+00 0.000000e+00 6.493000e+01 8.862148e-01 8.862148e-01 +5.300000e-01 0.000000e+00 0.000000e+00 7.024000e+01 9.600794e-01 9.600794e-01 +5.400000e-01 0.000000e+00 0.000000e+00 7.560000e+01 1.042060e+00 1.042060e+00 +5.500000e-01 0.000000e+00 0.000000e+00 8.020000e+01 1.096353e+00 1.096353e+00 +5.600000e-01 0.000000e+00 0.000000e+00 8.347000e+01 1.118567e+00 1.118567e+00 +5.700000e-01 0.000000e+00 0.000000e+00 8.606000e+01 1.146920e+00 1.146920e+00 +5.800000e-01 0.000000e+00 0.000000e+00 8.785000e+01 1.168698e+00 1.168698e+00 +5.900000e-01 0.000000e+00 0.000000e+00 8.950000e+01 1.207336e+00 1.207336e+00 +6.000000e-01 0.000000e+00 0.000000e+00 9.031000e+01 1.201564e+00 1.201564e+00 +6.100000e-01 0.000000e+00 0.000000e+00 7.420000e+01 1.007181e+00 1.007181e+00 +6.200000e-01 0.000000e+00 0.000000e+00 6.549000e+01 8.793226e-01 8.793226e-01 +6.300000e-01 0.000000e+00 0.000000e+00 6.414000e+01 8.630517e-01 8.630517e-01 +6.400000e-01 0.000000e+00 0.000000e+00 6.209000e+01 8.319479e-01 8.319479e-01 +6.500000e-01 0.000000e+00 0.000000e+00 5.940000e+01 8.062223e-01 8.062223e-01 +6.600000e-01 0.000000e+00 0.000000e+00 5.638000e+01 7.566704e-01 7.566704e-01 +6.700000e-01 0.000000e+00 0.000000e+00 5.304000e+01 7.131936e-01 7.131936e-01 +6.800000e-01 0.000000e+00 0.000000e+00 4.987000e+01 6.859276e-01 6.859276e-01 +6.900000e-01 0.000000e+00 0.000000e+00 4.698000e+01 6.371448e-01 6.371448e-01 +7.000000e-01 0.000000e+00 0.000000e+00 4.416000e+01 6.000143e-01 6.000143e-01 +7.100000e-01 0.000000e+00 0.000000e+00 4.154000e+01 5.618208e-01 5.618208e-01 +7.200000e-01 0.000000e+00 0.000000e+00 3.905000e+01 5.395685e-01 5.395685e-01 +7.300000e-01 0.000000e+00 0.000000e+00 3.687000e+01 4.991215e-01 4.991215e-01 +7.400000e-01 0.000000e+00 0.000000e+00 3.520000e+01 4.828297e-01 4.828297e-01 +7.500000e-01 0.000000e+00 0.000000e+00 3.322000e+01 4.520819e-01 4.520819e-01 +7.600000e-01 0.000000e+00 0.000000e+00 3.199000e+01 4.374750e-01 4.374750e-01 +7.700000e-01 0.000000e+00 0.000000e+00 3.051000e+01 4.239096e-01 4.239096e-01 +7.800000e-01 0.000000e+00 0.000000e+00 2.960000e+01 4.093140e-01 4.093140e-01 +7.900000e-01 0.000000e+00 0.000000e+00 2.852000e+01 3.855765e-01 3.855765e-01 +8.000000e-01 0.000000e+00 0.000000e+00 2.753000e+01 3.773327e-01 3.773327e-01 +8.100000e-01 0.000000e+00 0.000000e+00 2.700000e+01 3.710768e-01 3.710768e-01 +8.200000e-01 0.000000e+00 0.000000e+00 2.648000e+01 3.612379e-01 3.612379e-01 +8.300000e-01 0.000000e+00 0.000000e+00 2.584000e+01 3.614807e-01 3.614807e-01 +8.400000e-01 0.000000e+00 0.000000e+00 2.545000e+01 3.490384e-01 3.490384e-01 +8.500000e-01 0.000000e+00 0.000000e+00 2.516000e+01 3.456156e-01 3.456156e-01 +8.600000e-01 0.000000e+00 0.000000e+00 2.496000e+01 3.395972e-01 3.395972e-01 +8.700000e-01 0.000000e+00 0.000000e+00 2.481000e+01 3.495953e-01 3.495953e-01 +8.800000e-01 0.000000e+00 0.000000e+00 2.509000e+01 3.486837e-01 3.486837e-01 +8.900000e-01 0.000000e+00 0.000000e+00 2.517000e+01 3.420989e-01 3.420989e-01 +9.000000e-01 0.000000e+00 0.000000e+00 2.537000e+01 3.480936e-01 3.480936e-01 +9.100000e-01 0.000000e+00 0.000000e+00 2.586000e+01 3.503367e-01 3.503367e-01 +9.200000e-01 0.000000e+00 0.000000e+00 2.687000e+01 3.695450e-01 3.695450e-01 +9.300000e-01 0.000000e+00 0.000000e+00 2.794000e+01 3.821835e-01 3.821835e-01 +9.400000e-01 0.000000e+00 0.000000e+00 2.949000e+01 4.080257e-01 4.080257e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/KLOE_2005_I655225/d02-x01-y01 +IsRef: 1 +Path: /REF/KLOE_2005_I655225/d02-x01-y01 +Title: doi:10.17182/hepdata.41901.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.500000e-01 0.000000e+00 0.000000e+00 3.300000e+02 8.163443e+00 8.163443e+00 +3.600000e-01 0.000000e+00 0.000000e+00 3.490000e+02 8.290462e+00 8.290462e+00 +3.700000e-01 0.000000e+00 0.000000e+00 3.700000e+02 8.436694e+00 8.436694e+00 +3.800000e-01 0.000000e+00 0.000000e+00 3.920000e+02 7.803433e+00 7.803433e+00 +3.900000e-01 0.000000e+00 0.000000e+00 4.160000e+02 8.002192e+00 8.002192e+00 +4.000000e-01 0.000000e+00 0.000000e+00 4.500000e+02 9.044612e+00 9.044612e+00 +4.100000e-01 0.000000e+00 0.000000e+00 4.890000e+02 8.645091e+00 8.645091e+00 +4.200000e-01 0.000000e+00 0.000000e+00 5.210000e+02 9.642274e+00 9.642274e+00 +4.300000e-01 0.000000e+00 0.000000e+00 5.640000e+02 1.002654e+01 1.002654e+01 +4.400000e-01 0.000000e+00 0.000000e+00 6.080000e+02 1.043482e+01 1.043482e+01 +4.500000e-01 0.000000e+00 0.000000e+00 6.490000e+02 1.082749e+01 1.082749e+01 +4.600000e-01 0.000000e+00 0.000000e+00 7.100000e+02 1.143084e+01 1.143084e+01 +4.700000e-01 0.000000e+00 0.000000e+00 7.690000e+02 1.203331e+01 1.203331e+01 +4.800000e-01 0.000000e+00 0.000000e+00 8.300000e+02 1.267288e+01 1.267288e+01 +4.900000e-01 0.000000e+00 0.000000e+00 8.950000e+02 1.337034e+01 1.337034e+01 +5.000000e-01 0.000000e+00 0.000000e+00 9.670000e+02 1.467939e+01 1.467939e+01 +5.100000e-01 0.000000e+00 0.000000e+00 1.041000e+03 1.498520e+01 1.498520e+01 +5.200000e-01 0.000000e+00 0.000000e+00 1.102000e+03 1.567589e+01 1.567589e+01 +5.300000e-01 0.000000e+00 0.000000e+00 1.171000e+03 1.691570e+01 1.691570e+01 +5.400000e-01 0.000000e+00 0.000000e+00 1.226000e+03 1.753563e+01 1.753563e+01 +5.500000e-01 0.000000e+00 0.000000e+00 1.279000e+03 1.813853e+01 1.813853e+01 +5.600000e-01 0.000000e+00 0.000000e+00 1.288000e+03 1.782551e+01 1.782551e+01 +5.700000e-01 0.000000e+00 0.000000e+00 1.302000e+03 1.798953e+01 1.798953e+01 +5.800000e-01 0.000000e+00 0.000000e+00 1.297000e+03 1.793092e+01 1.793092e+01 +5.900000e-01 0.000000e+00 0.000000e+00 1.282000e+03 1.775531e+01 1.775531e+01 +6.000000e-01 0.000000e+00 0.000000e+00 1.266000e+03 1.756834e+01 1.756834e+01 +6.100000e-01 0.000000e+00 0.000000e+00 1.006000e+03 1.414036e+01 1.414036e+01 +6.200000e-01 0.000000e+00 0.000000e+00 8.570000e+02 1.199920e+01 1.199920e+01 +6.300000e-01 0.000000e+00 0.000000e+00 8.170000e+02 1.153834e+01 1.153834e+01 +6.400000e-01 0.000000e+00 0.000000e+00 7.720000e+02 1.060893e+01 1.060893e+01 +6.500000e-01 0.000000e+00 0.000000e+00 7.140000e+02 9.929096e+00 9.929096e+00 +6.600000e-01 0.000000e+00 0.000000e+00 6.570000e+02 9.269689e+00 9.269689e+00 +6.700000e-01 0.000000e+00 0.000000e+00 5.950000e+02 8.564581e+00 8.564581e+00 +6.800000e-01 0.000000e+00 0.000000e+00 5.430000e+02 7.985333e+00 7.985333e+00 +6.900000e-01 0.000000e+00 0.000000e+00 4.932000e+02 7.001135e+00 7.001135e+00 +7.000000e-01 0.000000e+00 0.000000e+00 4.470000e+02 6.385848e+00 6.385848e+00 +7.100000e-01 0.000000e+00 0.000000e+00 4.050000e+02 5.773392e+00 5.773392e+00 +7.200000e-01 0.000000e+00 0.000000e+00 3.671000e+02 5.347103e+00 5.347103e+00 +7.300000e-01 0.000000e+00 0.000000e+00 3.333000e+02 4.778745e+00 4.778745e+00 +7.400000e-01 0.000000e+00 0.000000e+00 3.046000e+02 4.362402e+00 4.362402e+00 +7.500000e-01 0.000000e+00 0.000000e+00 2.778000e+02 3.967619e+00 3.967619e+00 +7.600000e-01 0.000000e+00 0.000000e+00 2.572000e+02 3.688712e+00 3.688712e+00 +7.700000e-01 0.000000e+00 0.000000e+00 2.338000e+02 3.427144e+00 3.427144e+00 +7.800000e-01 0.000000e+00 0.000000e+00 2.177000e+02 3.199643e+00 3.199643e+00 +7.900000e-01 0.000000e+00 0.000000e+00 2.003000e+02 2.861722e+00 2.861722e+00 +8.000000e-01 0.000000e+00 0.000000e+00 1.845000e+02 2.684124e+00 2.684124e+00 +8.100000e-01 0.000000e+00 0.000000e+00 1.721000e+02 2.497635e+00 2.497635e+00 +8.200000e-01 0.000000e+00 0.000000e+00 1.600000e+02 2.314563e+00 2.314563e+00 +8.300000e-01 0.000000e+00 0.000000e+00 1.484000e+02 2.185785e+00 2.185785e+00 +8.400000e-01 0.000000e+00 0.000000e+00 1.385000e+02 2.026703e+00 2.026703e+00 +8.500000e-01 0.000000e+00 0.000000e+00 1.292000e+02 1.874622e+00 1.874622e+00 +8.600000e-01 0.000000e+00 0.000000e+00 1.203000e+02 1.727564e+00 1.727564e+00 +8.700000e-01 0.000000e+00 0.000000e+00 1.118000e+02 1.683709e+00 1.683709e+00 +8.800000e-01 0.000000e+00 0.000000e+00 1.063000e+02 1.571798e+00 1.571798e+00 +8.900000e-01 0.000000e+00 0.000000e+00 9.950000e+01 1.447011e+00 1.447011e+00 +9.000000e-01 0.000000e+00 0.000000e+00 9.310000e+01 1.328214e+00 1.328214e+00 +9.100000e-01 0.000000e+00 0.000000e+00 8.760000e+01 1.266155e+00 1.266155e+00 +9.200000e-01 0.000000e+00 0.000000e+00 8.300000e+01 1.214915e+00 1.214915e+00 +9.300000e-01 0.000000e+00 0.000000e+00 7.910000e+01 1.124101e+00 1.124101e+00 +9.400000e-01 0.000000e+00 0.000000e+00 7.530000e+01 1.080997e+00 1.080997e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/KLOE_2005_I655225/d03-x01-y01 +IsRef: 1 +Path: /REF/KLOE_2005_I655225/d03-x01-y01 +Title: doi:10.17182/hepdata.41901.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.500000e-01 0.000000e+00 0.000000e+00 7.680000e+00 1.600000e-01 1.600000e-01 +3.600000e-01 0.000000e+00 0.000000e+00 8.260000e+00 1.600000e-01 1.600000e-01 +3.700000e-01 0.000000e+00 0.000000e+00 8.920000e+00 1.600000e-01 1.600000e-01 +3.800000e-01 0.000000e+00 0.000000e+00 9.600000e+00 1.600000e-01 1.600000e-01 +3.900000e-01 0.000000e+00 0.000000e+00 1.035000e+01 1.500000e-01 1.500000e-01 +4.000000e-01 0.000000e+00 0.000000e+00 1.140000e+01 1.700000e-01 1.700000e-01 +4.100000e-01 0.000000e+00 0.000000e+00 1.259000e+01 1.600000e-01 1.600000e-01 +4.200000e-01 0.000000e+00 0.000000e+00 1.363000e+01 1.800000e-01 1.800000e-01 +4.300000e-01 0.000000e+00 0.000000e+00 1.501000e+01 1.800000e-01 1.800000e-01 +4.400000e-01 0.000000e+00 0.000000e+00 1.643000e+01 1.800000e-01 1.800000e-01 +4.500000e-01 0.000000e+00 0.000000e+00 1.782000e+01 1.900000e-01 1.900000e-01 +4.600000e-01 0.000000e+00 0.000000e+00 1.979000e+01 1.800000e-01 1.800000e-01 +4.700000e-01 0.000000e+00 0.000000e+00 2.178000e+01 2.000000e-01 2.000000e-01 +4.800000e-01 0.000000e+00 0.000000e+00 2.386000e+01 2.000000e-01 2.000000e-01 +4.900000e-01 0.000000e+00 0.000000e+00 2.611000e+01 2.000000e-01 2.000000e-01 +5.000000e-01 0.000000e+00 0.000000e+00 2.860000e+01 2.300000e-01 2.300000e-01 +5.100000e-01 0.000000e+00 0.000000e+00 3.123000e+01 2.200000e-01 2.200000e-01 +5.200000e-01 0.000000e+00 0.000000e+00 3.350000e+01 2.200000e-01 2.200000e-01 +5.300000e-01 0.000000e+00 0.000000e+00 3.605000e+01 2.300000e-01 2.300000e-01 +5.400000e-01 0.000000e+00 0.000000e+00 3.820000e+01 2.600000e-01 2.600000e-01 +5.500000e-01 0.000000e+00 0.000000e+00 4.032000e+01 2.400000e-01 2.400000e-01 +5.600000e-01 0.000000e+00 0.000000e+00 4.107000e+01 2.400000e-01 2.400000e-01 +5.700000e-01 0.000000e+00 0.000000e+00 4.198000e+01 2.300000e-01 2.300000e-01 +5.800000e-01 0.000000e+00 0.000000e+00 4.236000e+01 2.300000e-01 2.300000e-01 +5.900000e-01 0.000000e+00 0.000000e+00 4.246000e+01 2.400000e-01 2.400000e-01 +6.000000e-01 0.000000e+00 0.000000e+00 4.258000e+01 2.300000e-01 2.300000e-01 +6.100000e-01 0.000000e+00 0.000000e+00 3.243000e+01 2.000000e-01 2.000000e-01 +6.200000e-01 0.000000e+00 0.000000e+00 2.799000e+01 1.600000e-01 1.600000e-01 +6.300000e-01 0.000000e+00 0.000000e+00 2.732000e+01 1.600000e-01 1.600000e-01 +6.400000e-01 0.000000e+00 0.000000e+00 2.627000e+01 1.500000e-01 1.500000e-01 +6.500000e-01 0.000000e+00 0.000000e+00 2.469000e+01 1.500000e-01 1.500000e-01 +6.600000e-01 0.000000e+00 0.000000e+00 2.305000e+01 1.400000e-01 1.400000e-01 +6.700000e-01 0.000000e+00 0.000000e+00 2.118000e+01 1.300000e-01 1.300000e-01 +6.800000e-01 0.000000e+00 0.000000e+00 1.957000e+01 1.300000e-01 1.300000e-01 +6.900000e-01 0.000000e+00 0.000000e+00 1.802000e+01 1.100000e-01 1.100000e-01 +7.000000e-01 0.000000e+00 0.000000e+00 1.654000e+01 1.100000e-01 1.100000e-01 +7.100000e-01 0.000000e+00 0.000000e+00 1.517000e+01 1.000000e-01 1.000000e-01 +7.200000e-01 0.000000e+00 0.000000e+00 1.392000e+01 1.000000e-01 1.000000e-01 +7.300000e-01 0.000000e+00 0.000000e+00 1.278000e+01 8.000000e-02 8.000000e-02 +7.400000e-01 0.000000e+00 0.000000e+00 1.181000e+01 8.000000e-02 8.000000e-02 +7.500000e-01 0.000000e+00 0.000000e+00 1.089000e+01 7.000000e-02 7.000000e-02 +7.600000e-01 0.000000e+00 0.000000e+00 1.019000e+01 7.000000e-02 7.000000e-02 +7.700000e-01 0.000000e+00 0.000000e+00 9.370000e+00 7.000000e-02 7.000000e-02 +7.800000e-01 0.000000e+00 0.000000e+00 8.820000e+00 6.000000e-02 6.000000e-02 +7.900000e-01 0.000000e+00 0.000000e+00 8.200000e+00 5.000000e-02 5.000000e-02 +8.000000e-01 0.000000e+00 0.000000e+00 7.630000e+00 5.000000e-02 5.000000e-02 +8.100000e-01 0.000000e+00 0.000000e+00 7.200000e+00 5.000000e-02 5.000000e-02 +8.200000e-01 0.000000e+00 0.000000e+00 6.760000e+00 5.000000e-02 5.000000e-02 +8.300000e-01 0.000000e+00 0.000000e+00 6.330000e+00 5.000000e-02 5.000000e-02 +8.400000e-01 0.000000e+00 0.000000e+00 5.970000e+00 4.000000e-02 4.000000e-02 +8.500000e-01 0.000000e+00 0.000000e+00 5.630000e+00 4.000000e-02 4.000000e-02 +8.600000e-01 0.000000e+00 0.000000e+00 5.290000e+00 4.000000e-02 4.000000e-02 +8.700000e-01 0.000000e+00 0.000000e+00 4.970000e+00 4.000000e-02 4.000000e-02 +8.800000e-01 0.000000e+00 0.000000e+00 4.774000e+00 3.500000e-02 3.500000e-02 +8.900000e-01 0.000000e+00 0.000000e+00 4.516000e+00 3.000000e-02 3.000000e-02 +9.000000e-01 0.000000e+00 0.000000e+00 4.269000e+00 3.000000e-02 3.000000e-02 +9.100000e-01 0.000000e+00 0.000000e+00 4.059000e+00 2.700000e-02 2.700000e-02 +9.200000e-01 0.000000e+00 0.000000e+00 3.886000e+00 2.600000e-02 2.600000e-02 +9.300000e-01 0.000000e+00 0.000000e+00 3.741000e+00 2.500000e-02 2.500000e-02 +9.400000e-01 0.000000e+00 0.000000e+00 3.599000e+00 2.500000e-02 2.500000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/KLOE_2008_I791841.cc b/analyses/pluginFrascati/KLOE_2008_I791841.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2008_I791841.cc @@ -0,0 +1,95 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class KLOE_2008_I791841 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(KLOE_2008_I791841); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + _n4pi = bookCounter("TMP/4pi"); + _n2pigamma = bookCounter("TMP/2pigamma"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(nCount[111]==2) { + if( nCount[211] == 1 && nCount[-211] == 1 ) + _n4pi->fill(event.weight()); + else if( nCount[22] == 1) + _n2pigamma->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _n4pi->val(); + error = _n4pi->err(); + } + else if(ix==2) { + sigma = _n2pigamma->val(); + error = _n2pigamma->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _n4pi,_n2pigamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(KLOE_2008_I791841); + + +} diff --git a/analyses/pluginFrascati/KLOE_2008_I791841.info b/analyses/pluginFrascati/KLOE_2008_I791841.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2008_I791841.info @@ -0,0 +1,34 @@ +Name: KLOE_2008_I791841 +Year: 2008 +Summary: Cross section for $\pi^+\pi^-2\pi^0$ and $2\pi^0\gamma$ near the $\phi$ mass +Experiment: KLOE +Collider: DAPHNE +InspireID: 791841 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B669 (2008) 223-228, 2008 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $\pi^+\pi^-2\pi^0$ and $2\pi^0\gamma$ near the $\phi$ mass' +Keywords: [] +BibKey: Ambrosino:2008gb +BibTeX: '@article{Ambrosino:2008gb, + author = "Ambrosino, F. and others", + title = "{Study of the process $e^+ e^- \to \omega \pi^0$ in the + $\phi$-meson mass region with the KLOE detector}", + collaboration = "KLOE", + journal = "Phys. Lett.", + volume = "B669", + year = "2008", + pages = "223-228", + doi = "10.1016/j.physletb.2008.09.056", + eprint = "0807.4909", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0807.4909;%%" +}' diff --git a/analyses/pluginFrascati/KLOE_2008_I791841.plot b/analyses/pluginFrascati/KLOE_2008_I791841.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2008_I791841.plot @@ -0,0 +1,16 @@ +BEGIN PLOT /KLOE_2008_I791841/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT +BEGIN PLOT /KLOE_2008_I791841/d02-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^0\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to 2\pi^0\gamma)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginFrascati/KLOE_2008_I791841.yoda b/analyses/pluginFrascati/KLOE_2008_I791841.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2008_I791841.yoda @@ -0,0 +1,50 @@ +BEGIN YODA_SCATTER2D_V2 /REF/KLOE_2008_I791841/d01-x01-y01 +IsRef: 1 +Path: /REF/KLOE_2008_I791841/d01-x01-y01 +Title: doi:10.17182/hepdata.50498.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000100e+03 0.000000e+00 0.000000e+00 5.720000e+00 5.000000e-02 5.000000e-02 +1.009900e+03 0.000000e+00 0.000000e+00 6.200000e+00 6.000000e-02 6.000000e-02 +1.017200e+03 0.000000e+00 0.000000e+00 5.710000e+00 8.000000e-02 8.000000e-02 +1.018150e+03 0.000000e+00 0.000000e+00 5.600000e+00 6.000000e-02 6.000000e-02 +1.019300e+03 0.000000e+00 0.000000e+00 5.880000e+00 1.200000e-01 1.200000e-01 +1.019450e+03 0.000000e+00 0.000000e+00 5.890000e+00 6.000000e-02 6.000000e-02 +1.019550e+03 0.000000e+00 0.000000e+00 5.930000e+00 5.000000e-02 5.000000e-02 +1.019650e+03 0.000000e+00 0.000000e+00 5.980000e+00 5.000000e-02 5.000000e-02 +1.019750e+03 0.000000e+00 0.000000e+00 6.040000e+00 5.000000e-02 5.000000e-02 +1.019850e+03 0.000000e+00 0.000000e+00 6.080000e+00 5.000000e-02 5.000000e-02 +1.019950e+03 0.000000e+00 0.000000e+00 6.200000e+00 7.000000e-02 7.000000e-02 +1.020050e+03 0.000000e+00 0.000000e+00 6.210000e+00 8.000000e-02 8.000000e-02 +1.020150e+03 0.000000e+00 0.000000e+00 6.230000e+00 1.100000e-01 1.100000e-01 +1.020450e+03 0.000000e+00 0.000000e+00 6.410000e+00 9.000000e-02 9.000000e-02 +1.022300e+03 0.000000e+00 0.000000e+00 7.240000e+00 8.000000e-02 8.000000e-02 +1.023000e+03 0.000000e+00 0.000000e+00 7.410000e+00 7.000000e-02 7.000000e-02 +1.029950e+03 0.000000e+00 0.000000e+00 7.840000e+00 7.000000e-02 7.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/KLOE_2008_I791841/d02-x01-y01 +IsRef: 1 +Path: /REF/KLOE_2008_I791841/d02-x01-y01 +Title: doi:10.17182/hepdata.50498.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000100e+03 0.000000e+00 0.000000e+00 5.500000e-01 5.000000e-03 5.000000e-03 +1.009900e+03 0.000000e+00 0.000000e+00 5.810000e-01 1.200000e-02 1.200000e-02 +1.017200e+03 0.000000e+00 0.000000e+00 5.640000e-01 1.800000e-02 1.800000e-02 +1.018150e+03 0.000000e+00 0.000000e+00 5.410000e-01 1.400000e-02 1.400000e-02 +1.019300e+03 0.000000e+00 0.000000e+00 4.800000e-01 3.400000e-02 3.400000e-02 +1.019450e+03 0.000000e+00 0.000000e+00 4.970000e-01 9.000000e-03 9.000000e-03 +1.019550e+03 0.000000e+00 0.000000e+00 4.870000e-01 8.000000e-03 8.000000e-03 +1.019650e+03 0.000000e+00 0.000000e+00 5.090000e-01 7.000000e-03 7.000000e-03 +1.019750e+03 0.000000e+00 0.000000e+00 5.050000e-01 6.000000e-03 6.000000e-03 +1.019850e+03 0.000000e+00 0.000000e+00 5.080000e-01 6.000000e-03 6.000000e-03 +1.019950e+03 0.000000e+00 0.000000e+00 4.910000e-01 1.100000e-02 1.100000e-02 +1.020050e+03 0.000000e+00 0.000000e+00 5.160000e-01 1.600000e-02 1.600000e-02 +1.020150e+03 0.000000e+00 0.000000e+00 5.010000e-01 2.400000e-02 2.400000e-02 +1.020450e+03 0.000000e+00 0.000000e+00 4.880000e-01 2.400000e-02 2.400000e-02 +1.022300e+03 0.000000e+00 0.000000e+00 6.120000e-01 1.800000e-02 1.800000e-02 +1.023000e+03 0.000000e+00 0.000000e+00 6.190000e-01 1.300000e-02 1.300000e-02 +1.029950e+03 0.000000e+00 0.000000e+00 6.890000e-01 1.300000e-02 1.300000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/KLOE_2009_I797438.cc b/analyses/pluginFrascati/KLOE_2009_I797438.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2009_I797438.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class KLOE_2009_I797438 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(KLOE_2009_I797438); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(2, 1, 1)); + Scatter2DPtr mult = bookScatter2D(2, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqr(sqrtS()/GeV), x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(KLOE_2009_I797438); + + +} diff --git a/analyses/pluginFrascati/KLOE_2009_I797438.info b/analyses/pluginFrascati/KLOE_2009_I797438.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2009_I797438.info @@ -0,0 +1,35 @@ +Name: KLOE_2009_I797438 +Year: 2009 +Summary: Cross section for $e^+e^-\to\pi^+\pi^-$ below 0.93 GeV +Experiment: KLOE +Collider: DAPHNE +InspireID: 797438 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B670 (2009) 285-291, 2009 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^-$ below 0.93 GeV' +Keywords: [] +BibKey: Ambrosino:2008aa +BibTeX: '@article{Ambrosino:2008aa, + author = "Ambrosino, F. and others", + title = "{Measurement of $\sigma(e^+ e^- \to \pi^+ \pi^- + \gamma(\gamma)$ and the dipion contribution to the muon + anomaly with the KLOE detector}", + collaboration = "KLOE", + journal = "Phys. Lett.", + volume = "B670", + year = "2009", + pages = "285-291", + doi = "10.1016/j.physletb.2008.10.060", + eprint = "0809.3950", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0809.3950;%%" +}' diff --git a/analyses/pluginFrascati/KLOE_2009_I797438.plot b/analyses/pluginFrascati/KLOE_2009_I797438.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2009_I797438.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /KLOE_2009_I797438/d02-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$s/\text{GeV}^2$ +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +LogY=0 +END PLOT diff --git a/analyses/pluginFrascati/KLOE_2009_I797438.yoda b/analyses/pluginFrascati/KLOE_2009_I797438.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2009_I797438.yoda @@ -0,0 +1,204 @@ +BEGIN YODA_SCATTER2D_V2 /REF/KLOE_2009_I797438/d01-x01-y01 +IsRef: 1 +Path: /REF/KLOE_2009_I797438/d01-x01-y01 +Title: doi:10.17182/hepdata.57088.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.550000e-01 5.000000e-03 5.000000e-03 1.307000e+01 1.937982e-01 1.937982e-01 +3.650000e-01 5.000000e-03 5.000000e-03 1.421000e+01 1.983200e-01 1.983200e-01 +3.750000e-01 5.000000e-03 5.000000e-03 1.520000e+01 1.963116e-01 1.963116e-01 +3.850000e-01 5.000000e-03 5.000000e-03 1.660000e+01 2.005110e-01 2.005110e-01 +3.950000e-01 5.000000e-03 5.000000e-03 1.823000e+01 2.094158e-01 2.094158e-01 +4.050000e-01 5.000000e-03 5.000000e-03 1.997000e+01 2.057903e-01 2.057903e-01 +4.150000e-01 5.000000e-03 5.000000e-03 2.200000e+01 2.251222e-01 2.251222e-01 +4.250000e-01 5.000000e-03 5.000000e-03 2.409000e+01 2.308111e-01 2.308111e-01 +4.350000e-01 5.000000e-03 5.000000e-03 2.657000e+01 2.222003e-01 2.222003e-01 +4.450000e-01 5.000000e-03 5.000000e-03 2.926000e+01 2.337944e-01 2.337944e-01 +4.550000e-01 5.000000e-03 5.000000e-03 3.256000e+01 2.437691e-01 2.437691e-01 +4.650000e-01 5.000000e-03 5.000000e-03 3.560000e+01 2.529465e-01 2.529465e-01 +4.750000e-01 5.000000e-03 5.000000e-03 3.918000e+01 2.784725e-01 2.784725e-01 +4.850000e-01 5.000000e-03 5.000000e-03 4.428000e+01 2.779454e-01 2.779454e-01 +4.950000e-01 5.000000e-03 5.000000e-03 4.973000e+01 2.935000e-01 2.935000e-01 +5.050000e-01 5.000000e-03 5.000000e-03 5.417000e+01 3.360901e-01 3.360901e-01 +5.150000e-01 5.000000e-03 5.000000e-03 5.920000e+01 3.390990e-01 3.390990e-01 +5.250000e-01 5.000000e-03 5.000000e-03 6.390000e+01 3.127544e-01 3.127544e-01 +5.350000e-01 5.000000e-03 5.000000e-03 6.982000e+01 3.185490e-01 3.185490e-01 +5.450000e-01 5.000000e-03 5.000000e-03 7.468000e+01 4.044316e-01 4.044316e-01 +5.550000e-01 5.000000e-03 5.000000e-03 7.920000e+01 3.813358e-01 3.813358e-01 +5.650000e-01 5.000000e-03 5.000000e-03 8.379000e+01 4.009872e-01 4.009872e-01 +5.750000e-01 5.000000e-03 5.000000e-03 8.579000e+01 3.588026e-01 3.588026e-01 +5.850000e-01 5.000000e-03 5.000000e-03 8.866000e+01 5.089351e-01 5.089351e-01 +5.950000e-01 5.000000e-03 5.000000e-03 9.024000e+01 4.997949e-01 4.997949e-01 +6.050000e-01 5.000000e-03 5.000000e-03 9.138000e+01 1.948098e+00 1.948098e+00 +6.150000e-01 5.000000e-03 5.000000e-03 7.010000e+01 2.824060e+00 2.824060e+00 +6.250000e-01 5.000000e-03 5.000000e-03 6.502000e+01 4.084458e-01 4.084458e-01 +6.350000e-01 5.000000e-03 5.000000e-03 6.492000e+01 2.791621e-01 2.791621e-01 +6.450000e-01 5.000000e-03 5.000000e-03 6.240000e+01 2.667397e-01 2.667397e-01 +6.550000e-01 5.000000e-03 5.000000e-03 5.962000e+01 2.868956e-01 2.868956e-01 +6.650000e-01 5.000000e-03 5.000000e-03 5.628000e+01 2.712503e-01 2.712503e-01 +6.750000e-01 5.000000e-03 5.000000e-03 5.343000e+01 2.636512e-01 2.636512e-01 +6.850000e-01 5.000000e-03 5.000000e-03 4.984000e+01 2.208443e-01 2.208443e-01 +6.950000e-01 5.000000e-03 5.000000e-03 4.722000e+01 2.336375e-01 2.336375e-01 +7.050000e-01 5.000000e-03 5.000000e-03 4.465000e+01 2.269738e-01 2.269738e-01 +7.150000e-01 5.000000e-03 5.000000e-03 4.140000e+01 1.990970e-01 1.990970e-01 +7.250000e-01 5.000000e-03 5.000000e-03 3.940000e+01 2.144531e-01 2.144531e-01 +7.350000e-01 5.000000e-03 5.000000e-03 3.780000e+01 1.840880e-01 1.840880e-01 +7.450000e-01 5.000000e-03 5.000000e-03 3.605000e+01 1.805437e-01 1.805437e-01 +7.550000e-01 5.000000e-03 5.000000e-03 3.413000e+01 1.689632e-01 1.689632e-01 +7.650000e-01 5.000000e-03 5.000000e-03 3.250000e+01 1.866983e-01 1.866983e-01 +7.750000e-01 5.000000e-03 5.000000e-03 3.114000e+01 1.552321e-01 1.552321e-01 +7.850000e-01 5.000000e-03 5.000000e-03 3.001000e+01 1.529902e-01 1.529902e-01 +7.950000e-01 5.000000e-03 5.000000e-03 2.923000e+01 1.436800e-01 1.436800e-01 +8.050000e-01 5.000000e-03 5.000000e-03 2.846000e+01 1.608400e-01 1.608400e-01 +8.150000e-01 5.000000e-03 5.000000e-03 2.779000e+01 1.588359e-01 1.588359e-01 +8.250000e-01 5.000000e-03 5.000000e-03 2.706000e+01 1.393644e-01 1.393644e-01 +8.350000e-01 5.000000e-03 5.000000e-03 2.643000e+01 1.678159e-01 1.678159e-01 +8.450000e-01 5.000000e-03 5.000000e-03 2.602000e+01 1.466618e-01 1.466618e-01 +8.550000e-01 5.000000e-03 5.000000e-03 2.563000e+01 1.645580e-01 1.645580e-01 +8.650000e-01 5.000000e-03 5.000000e-03 2.563000e+01 1.454897e-01 1.454897e-01 +8.750000e-01 5.000000e-03 5.000000e-03 2.563000e+01 1.454897e-01 1.454897e-01 +8.850000e-01 5.000000e-03 5.000000e-03 2.563000e+01 1.645580e-01 1.645580e-01 +8.950000e-01 5.000000e-03 5.000000e-03 2.563000e+01 1.645580e-01 1.645580e-01 +9.050000e-01 5.000000e-03 5.000000e-03 2.563000e+01 1.645580e-01 1.645580e-01 +9.150000e-01 5.000000e-03 5.000000e-03 2.563000e+01 1.852166e-01 1.852166e-01 +9.250000e-01 5.000000e-03 5.000000e-03 2.563000e+01 1.852166e-01 1.852166e-01 +9.350000e-01 5.000000e-03 5.000000e-03 2.857000e+01 2.005020e-01 2.005020e-01 +9.450000e-01 5.000000e-03 5.000000e-03 2.986000e+01 2.336257e-01 2.336257e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/KLOE_2009_I797438/d02-x01-y01 +IsRef: 1 +Path: /REF/KLOE_2009_I797438/d02-x01-y01 +Title: doi:10.17182/hepdata.57088.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.550000e-01 5.000000e-03 5.000000e-03 3.090000e+02 4.762738e+00 4.762738e+00 +3.650000e-01 5.000000e-03 5.000000e-03 3.350000e+02 4.861204e+00 4.861204e+00 +3.750000e-01 5.000000e-03 5.000000e-03 3.540000e+02 4.797676e+00 4.797676e+00 +3.850000e-01 5.000000e-03 5.000000e-03 3.800000e+02 4.863456e+00 4.863456e+00 +3.950000e-01 5.000000e-03 5.000000e-03 4.050000e+02 4.835403e+00 4.835403e+00 +4.050000e-01 5.000000e-03 5.000000e-03 4.390000e+02 4.908593e+00 4.908593e+00 +4.150000e-01 5.000000e-03 5.000000e-03 4.720000e+02 5.101498e+00 5.101498e+00 +4.250000e-01 5.000000e-03 5.000000e-03 5.110000e+02 5.192984e+00 5.192984e+00 +4.350000e-01 5.000000e-03 5.000000e-03 5.480000e+02 4.970796e+00 4.970796e+00 +4.450000e-01 5.000000e-03 5.000000e-03 5.920000e+02 5.011194e+00 5.011194e+00 +4.550000e-01 5.000000e-03 5.000000e-03 6.480000e+02 5.023732e+00 5.023732e+00 +4.650000e-01 5.000000e-03 5.000000e-03 6.950000e+02 5.160092e+00 5.160092e+00 +4.750000e-01 5.000000e-03 5.000000e-03 7.490000e+02 5.580952e+00 5.580952e+00 +4.850000e-01 5.000000e-03 5.000000e-03 8.260000e+02 6.161432e+00 6.161432e+00 +4.950000e-01 5.000000e-03 5.000000e-03 9.080000e+02 6.246270e+00 6.246270e+00 +5.050000e-01 5.000000e-03 5.000000e-03 9.630000e+02 6.738109e+00 6.738109e+00 +5.150000e-01 5.000000e-03 5.000000e-03 1.035000e+03 6.734484e+00 6.734484e+00 +5.250000e-01 5.000000e-03 5.000000e-03 1.085000e+03 6.160315e+00 6.160315e+00 +5.350000e-01 5.000000e-03 5.000000e-03 1.158000e+03 6.088405e+00 6.088405e+00 +5.450000e-01 5.000000e-03 5.000000e-03 1.209000e+03 7.264430e+00 7.264430e+00 +5.550000e-01 5.000000e-03 5.000000e-03 1.242000e+03 6.826119e+00 6.826119e+00 +5.650000e-01 5.000000e-03 5.000000e-03 1.289000e+03 6.947035e+00 6.947035e+00 +5.750000e-01 5.000000e-03 5.000000e-03 1.276000e+03 6.297109e+00 6.297109e+00 +5.850000e-01 5.000000e-03 5.000000e-03 1.285000e+03 8.141291e+00 8.141291e+00 +5.950000e-01 5.000000e-03 5.000000e-03 1.282000e+03 7.924711e+00 7.924711e+00 +6.050000e-01 5.000000e-03 5.000000e-03 1.262000e+03 2.714612e+01 2.714612e+01 +6.150000e-01 5.000000e-03 5.000000e-03 8.981000e+02 3.625019e+01 3.625019e+01 +6.250000e-01 5.000000e-03 5.000000e-03 8.017000e+02 5.433386e+00 5.433386e+00 +6.350000e-01 5.000000e-03 5.000000e-03 7.857000e+02 3.894345e+00 3.894345e+00 +6.450000e-01 5.000000e-03 5.000000e-03 7.342000e+02 3.566847e+00 3.566847e+00 +6.550000e-01 5.000000e-03 5.000000e-03 6.838000e+02 3.656306e+00 3.656306e+00 +6.650000e-01 5.000000e-03 5.000000e-03 6.269000e+02 3.370319e+00 3.370319e+00 +6.750000e-01 5.000000e-03 5.000000e-03 5.735000e+02 3.167922e+00 3.167922e+00 +6.850000e-01 5.000000e-03 5.000000e-03 5.208000e+02 2.647614e+00 2.647614e+00 +6.950000e-01 5.000000e-03 5.000000e-03 4.760000e+02 2.635429e+00 2.635429e+00 +7.050000e-01 5.000000e-03 5.000000e-03 4.358000e+02 2.465559e+00 2.465559e+00 +7.150000e-01 5.000000e-03 5.000000e-03 3.895000e+02 2.099310e+00 2.099310e+00 +7.250000e-01 5.000000e-03 5.000000e-03 3.607000e+02 2.184440e+00 2.184440e+00 +7.350000e-01 5.000000e-03 5.000000e-03 3.311000e+02 1.829282e+00 1.829282e+00 +7.450000e-01 5.000000e-03 5.000000e-03 3.026000e+02 1.695779e+00 1.695779e+00 +7.550000e-01 5.000000e-03 5.000000e-03 2.760000e+02 1.565810e+00 1.565810e+00 +7.650000e-01 5.000000e-03 5.000000e-03 2.514000e+02 1.585696e+00 1.585696e+00 +7.750000e-01 5.000000e-03 5.000000e-03 2.302000e+02 1.319060e+00 1.319060e+00 +7.850000e-01 5.000000e-03 5.000000e-03 2.123000e+02 1.204455e+00 1.204455e+00 +7.950000e-01 5.000000e-03 5.000000e-03 1.974000e+02 1.095293e+00 1.095293e+00 +8.050000e-01 5.000000e-03 5.000000e-03 1.837000e+02 1.176298e+00 1.176298e+00 +8.150000e-01 5.000000e-03 5.000000e-03 1.713000e+02 1.067166e+00 1.067166e+00 +8.250000e-01 5.000000e-03 5.000000e-03 1.584000e+02 9.438780e-01 9.438780e-01 +8.350000e-01 5.000000e-03 5.000000e-03 1.470000e+02 1.025590e+00 1.025590e+00 +8.450000e-01 5.000000e-03 5.000000e-03 1.375000e+02 8.254733e-01 8.254733e-01 +8.550000e-01 5.000000e-03 5.000000e-03 1.274000e+02 8.843075e-01 8.843075e-01 +8.650000e-01 5.000000e-03 5.000000e-03 1.192000e+02 7.755945e-01 7.755945e-01 +8.750000e-01 5.000000e-03 5.000000e-03 1.115000e+02 6.792262e-01 6.792262e-01 +8.850000e-01 5.000000e-03 5.000000e-03 1.049000e+02 7.321914e-01 7.321914e-01 +8.950000e-01 5.000000e-03 5.000000e-03 9.870000e+01 6.428716e-01 6.428716e-01 +9.050000e-01 5.000000e-03 5.000000e-03 9.310000e+01 6.207720e-01 6.207720e-01 +9.150000e-01 5.000000e-03 5.000000e-03 8.760000e+01 6.662801e-01 6.662801e-01 +9.250000e-01 5.000000e-03 5.000000e-03 8.280000e+01 6.431688e-01 6.431688e-01 +9.350000e-01 5.000000e-03 5.000000e-03 7.874000e+01 5.816352e-01 5.816352e-01 +9.450000e-01 5.000000e-03 5.000000e-03 7.474000e+01 6.127017e-01 6.127017e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/KLOE_2009_I797438/d03-x01-y01 +IsRef: 1 +Path: /REF/KLOE_2009_I797438/d03-x01-y01 +Title: doi:10.17182/hepdata.57088.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.550000e-01 5.000000e-03 5.000000e-03 7.350000e+00 1.260221e-01 1.260221e-01 +3.650000e-01 5.000000e-03 5.000000e-03 8.090000e+00 1.286486e-01 1.286486e-01 +3.750000e-01 5.000000e-03 5.000000e-03 8.680000e+00 1.277465e-01 1.277465e-01 +3.850000e-01 5.000000e-03 5.000000e-03 9.450000e+00 1.297422e-01 1.297422e-01 +3.950000e-01 5.000000e-03 5.000000e-03 1.023000e+01 1.296510e-01 1.296510e-01 +4.050000e-01 5.000000e-03 5.000000e-03 1.128000e+01 1.320758e-01 1.320758e-01 +4.150000e-01 5.000000e-03 5.000000e-03 1.230000e+01 1.375065e-01 1.375065e-01 +4.250000e-01 5.000000e-03 5.000000e-03 1.351000e+01 1.405911e-01 1.405911e-01 +4.350000e-01 5.000000e-03 5.000000e-03 1.470000e+01 1.355235e-01 1.355235e-01 +4.450000e-01 5.000000e-03 5.000000e-03 1.613000e+01 1.454806e-01 1.454806e-01 +4.550000e-01 5.000000e-03 5.000000e-03 1.791000e+01 1.464817e-01 1.464817e-01 +4.650000e-01 5.000000e-03 5.000000e-03 1.949000e+01 1.508540e-01 1.508540e-01 +4.750000e-01 5.000000e-03 5.000000e-03 2.131000e+01 1.707663e-01 1.707663e-01 +4.850000e-01 5.000000e-03 5.000000e-03 2.385000e+01 1.664561e-01 1.664561e-01 +4.950000e-01 5.000000e-03 5.000000e-03 2.661000e+01 1.778695e-01 1.778695e-01 +5.050000e-01 5.000000e-03 5.000000e-03 2.865000e+01 1.940569e-01 1.940569e-01 +5.150000e-01 5.000000e-03 5.000000e-03 3.125000e+01 2.026196e-01 2.026196e-01 +5.250000e-01 5.000000e-03 5.000000e-03 3.325000e+01 1.861752e-01 1.861752e-01 +5.350000e-01 5.000000e-03 5.000000e-03 3.605000e+01 1.931228e-01 1.931228e-01 +5.450000e-01 5.000000e-03 5.000000e-03 3.822000e+01 2.309861e-01 2.309861e-01 +5.550000e-01 5.000000e-03 5.000000e-03 3.988000e+01 2.187825e-01 2.187825e-01 +5.650000e-01 5.000000e-03 5.000000e-03 4.206000e+01 2.244251e-01 2.244251e-01 +5.750000e-01 5.000000e-03 5.000000e-03 4.227000e+01 2.041587e-01 2.041587e-01 +5.850000e-01 5.000000e-03 5.000000e-03 4.318000e+01 2.687244e-01 2.687244e-01 +5.950000e-01 5.000000e-03 5.000000e-03 4.361000e+01 2.633290e-01 2.633290e-01 +6.050000e-01 5.000000e-03 5.000000e-03 4.337000e+01 9.307995e-01 9.307995e-01 +6.150000e-01 5.000000e-03 5.000000e-03 3.303000e+01 1.333320e+00 1.333320e+00 +6.250000e-01 5.000000e-03 5.000000e-03 2.984000e+01 2.027628e-01 2.027628e-01 +6.350000e-01 5.000000e-03 5.000000e-03 2.931000e+01 1.487672e-01 1.487672e-01 +6.450000e-01 5.000000e-03 5.000000e-03 2.757000e+01 1.348363e-01 1.348363e-01 +6.550000e-01 5.000000e-03 5.000000e-03 2.590000e+01 1.368230e-01 1.368230e-01 +6.650000e-01 5.000000e-03 5.000000e-03 2.398000e+01 1.321950e-01 1.321950e-01 +6.750000e-01 5.000000e-03 5.000000e-03 2.216000e+01 1.203489e-01 1.203489e-01 +6.850000e-01 5.000000e-03 5.000000e-03 2.033000e+01 1.068011e-01 1.068011e-01 +6.950000e-01 5.000000e-03 5.000000e-03 1.878000e+01 1.048091e-01 1.048091e-01 +7.050000e-01 5.000000e-03 5.000000e-03 1.738000e+01 1.016210e-01 1.016210e-01 +7.150000e-01 5.000000e-03 5.000000e-03 1.570000e+01 8.581900e-02 8.581900e-02 +7.250000e-01 5.000000e-03 5.000000e-03 1.469000e+01 9.256637e-02 9.256637e-02 +7.350000e-01 5.000000e-03 5.000000e-03 1.363000e+01 7.387671e-02 7.387671e-02 +7.450000e-01 5.000000e-03 5.000000e-03 1.260000e+01 7.202500e-02 7.202500e-02 +7.550000e-01 5.000000e-03 5.000000e-03 1.163000e+01 6.206907e-02 6.206907e-02 +7.650000e-01 5.000000e-03 5.000000e-03 1.070000e+01 6.668081e-02 6.668081e-02 +7.750000e-01 5.000000e-03 5.000000e-03 9.910000e+00 5.900916e-02 5.900916e-02 +7.850000e-01 5.000000e-03 5.000000e-03 9.240000e+00 4.953560e-02 4.953560e-02 +7.950000e-01 5.000000e-03 5.000000e-03 8.680000e+00 4.851210e-02 4.851210e-02 +8.050000e-01 5.000000e-03 5.000000e-03 8.160000e+00 5.226811e-02 5.226811e-02 +8.150000e-01 5.000000e-03 5.000000e-03 7.690000e+00 5.104227e-02 5.104227e-02 +8.250000e-01 5.000000e-03 5.000000e-03 7.180000e+00 4.171959e-02 4.171959e-02 +8.350000e-01 5.000000e-03 5.000000e-03 6.732000e+00 4.692883e-02 4.692883e-02 +8.450000e-01 5.000000e-03 5.000000e-03 6.358000e+00 3.983981e-02 3.983981e-02 +8.550000e-01 5.000000e-03 5.000000e-03 5.948000e+00 4.127767e-02 4.127767e-02 +8.650000e-01 5.000000e-03 5.000000e-03 5.621000e+00 3.482996e-02 3.482996e-02 +8.750000e-01 5.000000e-03 5.000000e-03 5.304000e+00 3.321522e-02 3.321522e-02 +8.850000e-01 5.000000e-03 5.000000e-03 5.038000e+00 3.448068e-02 3.448068e-02 +8.950000e-01 5.000000e-03 5.000000e-03 4.784000e+00 3.284894e-02 3.284894e-02 +9.050000e-01 5.000000e-03 5.000000e-03 4.550000e+00 3.063111e-02 3.063111e-02 +9.150000e-01 5.000000e-03 5.000000e-03 4.322000e+00 3.243684e-02 3.243684e-02 +9.250000e-01 5.000000e-03 5.000000e-03 4.117000e+00 3.084053e-02 3.084053e-02 +9.350000e-01 5.000000e-03 5.000000e-03 3.950000e+00 2.943285e-02 2.943285e-02 +9.450000e-01 5.000000e-03 5.000000e-03 3.780000e+00 3.115156e-02 3.115156e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/KLOE_2009_I818106.cc b/analyses/pluginFrascati/KLOE_2009_I818106.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2009_I818106.cc @@ -0,0 +1,98 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class KLOE_2009_I818106 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(KLOE_2009_I818106); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(UnstableParticles(), "UFS"); + _h_etapi = bookHisto1D( 1, 1, 1); + _nPhi=0.; + } + + void findDecayProducts(const Particle & mother, unsigned int & nstable, + unsigned int & neta, unsigned int & npi, + unsigned int & ngamma, FourMomentum & ptot) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::ETA ) { + ++neta; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::PI0) { + ++npi; + ++nstable; + ptot += p.momentum(); + } + else if (id == PID::GAMMA) { + ++ngamma; + ++nstable; + } + else if (id == PID::PIPLUS || id == PID::PIMINUS) { + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p, nstable, neta, npi, ngamma, ptot); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + // Loop over phis + for(const Particle& phi : apply(event, "UFS").particles(Cuts::abspid==PID::PHI)) { + _nPhi+=event.weight(); + unsigned int nstable(0),neta(0),npi(0),ngamma(0); + FourMomentum p_tot(0,0,0,0); + findDecayProducts(phi, nstable, neta, npi, ngamma, p_tot); + if(nstable!=3) continue; + if(neta==1 && npi==1 && ngamma==1 ) { + _h_etapi->fill(p_tot.mass()/MeV, event.weight()); + } + } + + } + + + /// Normalise histograms etc., after the run + void finalize() { + // normalise to total no of phi mesons + // and mult by 10^7 due normalisation in paper + scale( _h_etapi, 1./_nPhi*1e7); + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _h_etapi; + double _nPhi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(KLOE_2009_I818106); + + +} diff --git a/analyses/pluginFrascati/KLOE_2009_I818106.info b/analyses/pluginFrascati/KLOE_2009_I818106.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2009_I818106.info @@ -0,0 +1,32 @@ +Name: KLOE_2009_I818106 +Year: 2009 +Summary: Mass spectrum of $\eta\pi$ in $\phi\to\eta\pi^0\gamma$ decays +Experiment: KLOE +Collider: DAPHNE +InspireID: 818106 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B681 (2009) 5-13 +RunInfo: Any process producing phi mesons +Description: + 'Mass spectra for $\eta\pi$ in $\phi$ decays to $\eta\pi^0\gamma$ + measured by KLOE. Useful for teting he treatment of the a_0(980) meson.' +Keywords: [] +BibKey: Ambrosino:2009py +BibTeX: '@article{Ambrosino:2009py, + author = "Ambrosino, F. and others", + title = "{Study of the a(0)(980) meson via the radiative decay + $\phi \to \eta \pi_0 \gamma$ with the KLOE detector}", + collaboration = "KLOE", + journal = "Phys. Lett.", + volume = "B681", + year = "2009", + pages = "5-13", + doi = "10.1016/j.physletb.2009.09.022", + eprint = "0904.2539", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0904.2539;%%" +}' diff --git a/analyses/pluginFrascati/KLOE_2009_I818106.plot b/analyses/pluginFrascati/KLOE_2009_I818106.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2009_I818106.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /KLOE_2009_I818106/d01-x01-y01 +Title=$\eta\pi^0$ mass in $\phi^0\to\eta\pi^0\gamma$ decays +XLabel=$m_{\eta\pi^0}$ [$\text{MeV}$] +YLabel=$1/\Gamma\text{d}\Gamma/\text{d}m_{\eta\pi^0}\times10^7$ [$\text{MeV}^{-1}$] +LogY=0 +END PLOT diff --git a/analyses/pluginFrascati/KLOE_2009_I818106.yoda b/analyses/pluginFrascati/KLOE_2009_I818106.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/KLOE_2009_I818106.yoda @@ -0,0 +1,57 @@ +BEGIN YODA_SCATTER2D_V2 /REF/KLOE_2009_I818106/d01-x01-y01 +IsRef: 1 +Path: /REF/KLOE_2009_I818106/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +691.53000 3.17500 3.17500 6.00000e-02 7.00000e-02 7.00000e-02 +697.88000 3.17500 3.17500 1.80000e-01 1.00000e-01 1.00000e-01 +704.24000 3.17500 3.17500 1.80000e-01 1.20000e-01 1.20000e-01 +710.59000 3.17500 3.17500 3.10000e-01 1.30000e-01 1.30000e-01 +716.94000 3.17500 3.17500 3.00000e-01 8.00000e-02 8.00000e-02 +723.29000 3.17500 3.17500 3.80000e-01 1.10000e-01 1.10000e-01 +729.65000 3.17500 3.17500 5.30000e-01 1.70000e-01 1.70000e-01 +736.00000 3.17500 3.17500 5.10000e-01 1.30000e-01 1.30000e-01 +742.35000 3.17500 3.17500 5.30000e-01 5.00000e-02 5.00000e-02 +748.71000 3.17500 3.17500 6.70000e-01 7.00000e-02 7.00000e-02 +755.06000 3.17500 3.17500 8.10000e-01 7.00000e-02 7.00000e-02 +761.41000 3.17500 3.17500 9.40000e-01 1.00000e-01 1.00000e-01 +767.76000 3.17500 3.17500 9.90000e-01 1.10000e-01 1.10000e-01 +774.12000 3.17500 3.17500 9.90000e-01 8.00000e-02 8.00000e-02 +780.47000 3.17500 3.17500 1.08000e+00 9.00000e-02 9.00000e-02 +786.82000 3.17500 3.17500 1.30000e+00 1.00000e-01 1.00000e-01 +793.18000 3.17500 3.17500 1.27000e+00 1.30000e-01 1.30000e-01 +799.53000 3.17500 3.17500 1.42000e+00 2.80000e-01 2.80000e-01 +805.88000 3.17500 3.17500 1.63000e+00 2.80000e-01 2.80000e-01 +812.24000 3.17500 3.17500 1.71000e+00 1.40000e-01 1.40000e-01 +818.59000 3.17500 3.17500 1.79000e+00 1.60000e-01 1.60000e-01 +824.94000 3.17500 3.17500 1.66000e+00 1.80000e-01 1.80000e-01 +831.29000 3.17500 3.17500 1.82000e+00 1.50000e-01 1.50000e-01 +837.65000 3.17500 3.17500 1.96000e+00 1.20000e-01 1.20000e-01 +844.00000 3.17500 3.17500 2.13000e+00 1.30000e-01 1.30000e-01 +850.35000 3.17500 3.17500 2.25000e+00 1.30000e-01 1.30000e-01 +856.71000 3.17500 3.17500 2.35000e+00 1.40000e-01 1.40000e-01 +863.06000 3.17500 3.17500 2.27000e+00 1.30000e-01 1.30000e-01 +869.41000 3.17500 3.17500 2.35000e+00 1.30000e-01 1.30000e-01 +875.76000 3.17500 3.17500 2.42000e+00 1.60000e-01 1.60000e-01 +882.12000 3.17500 3.17500 2.59000e+00 1.60000e-01 1.60000e-01 +888.47000 3.17500 3.17500 2.80000e+00 1.40000e-01 1.40000e-01 +894.82000 3.17500 3.17500 2.92000e+00 1.90000e-01 1.90000e-01 +901.18000 3.17500 3.17500 3.18000e+00 2.00000e-01 2.00000e-01 +907.53000 3.17500 3.17500 3.37000e+00 1.70000e-01 1.70000e-01 +913.88000 3.17500 3.17500 3.48000e+00 1.70000e-01 1.70000e-01 +920.24000 3.17500 3.17500 3.67000e+00 1.70000e-01 1.70000e-01 +926.59000 3.17500 3.17500 3.94000e+00 1.70000e-01 1.70000e-01 +932.94000 3.17500 3.17500 4.29000e+00 2.50000e-01 2.50000e-01 +939.29000 3.17500 3.17500 4.63000e+00 2.50000e-01 2.50000e-01 +945.65000 3.17500 3.17500 4.89000e+00 2.10000e-01 2.10000e-01 +952.00000 3.17500 3.17500 5.20000e+00 2.20000e-01 2.20000e-01 +958.35000 3.17500 3.17500 5.40000e+00 2.80000e-01 2.80000e-01 +964.71000 3.17500 3.17500 5.44000e+00 3.30000e-01 3.30000e-01 +971.06000 3.17500 3.17500 5.35000e+00 2.20000e-01 2.20000e-01 +977.41000 3.17500 3.17500 4.94000e+00 2.10000e-01 2.10000e-01 +983.76000 3.17500 3.17500 4.02000e+00 1.90000e-01 1.90000e-01 +990.12000 3.17500 3.17500 2.80000e+00 2.70000e-01 2.70000e-01 +996.47000 3.17500 3.17500 1.51000e+00 3.20000e-01 3.20000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/MUPI_1972_I84978.cc b/analyses/pluginFrascati/MUPI_1972_I84978.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/MUPI_1972_I84978.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MUPI_1972_I84978 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MUPI_1972_I84978); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(1, 1, 1); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(2, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MUPI_1972_I84978); + + +} diff --git a/analyses/pluginFrascati/MUPI_1972_I84978.info b/analyses/pluginFrascati/MUPI_1972_I84978.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/MUPI_1972_I84978.info @@ -0,0 +1,36 @@ +Name: MUPI_1972_I84978 +Year: 1972 +Summary: Measurement of $R$ and the hadronic cross section for energies between 1.2 and 2.1 GeV +Experiment: MUPI +Collider: ADONE +InspireID: 84978 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B218 (1989) 499-507, 1989 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ and the hadronic cross seection in $e^+e^-$ collisions by + the Mu-Pi group for energies between 1.2 and 2.1 GeV. + The muonic cross section is also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +InspireID: 84978 +BibKey: Ceradini:1973pr +BibTeX: '@article{Ceradini:1973pr, + author = "Ceradini, F. and Santonico, R. and Conversi, M. and + Paoluzi, L. and Grilli, M. and Iarocci, E. and + Spillantini, P. and Valente, V. and Visentin, R. and + Nigro, M.", + title = "{Multiplicity in hadron production by e+ e- colliding + beams}", + journal = "Phys. Lett.", + volume = "42B", + year = "1972", + pages = "501-503", + doi = "10.1016/0370-2693(72)90116-5", + SLACcitation = "%%CITATION = PHLTA,42B,501;%%" +}' diff --git a/analyses/pluginFrascati/MUPI_1972_I84978.plot b/analyses/pluginFrascati/MUPI_1972_I84978.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/MUPI_1972_I84978.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /MUPI_1972_I84978/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MUPI_1972_I84978/d01-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MUPI_1972_I84978/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginFrascati/MUPI_1972_I84978.yoda b/analyses/pluginFrascati/MUPI_1972_I84978.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/MUPI_1972_I84978.yoda @@ -0,0 +1,24 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MUPI_1972_I84978/d01-x01-y01 +IsRef: 1 +Path: /REF/MUPI_1972_I84978/d01-x01-y01 +Title: doi:10.17182/hepdata.28188.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+00 0.000000e+00 0.000000e+00 3.400000e+01 1.612452e+01 1.612452e+01 +1.500000e+00 0.000000e+00 0.000000e+00 6.600000e+01 9.000000e+00 9.000000e+00 +1.900000e+00 0.000000e+00 0.000000e+00 3.600000e+01 5.000000e+00 5.000000e+00 +2.100000e+00 0.000000e+00 0.000000e+00 3.600000e+01 4.000000e+00 4.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MUPI_1972_I84978/d02-x01-y01 +IsRef: 1 +Path: /REF/MUPI_1972_I84978/d02-x01-y01 +Title: doi:10.17182/hepdata.28188.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+00 0.000000e+00 0.000000e+00 5.600000e-01 2.716616e-01 2.716616e-01 +1.500000e+00 0.000000e+00 0.000000e+00 1.710000e+00 2.300000e-01 2.300000e-01 +1.900000e+00 0.000000e+00 0.000000e+00 1.500000e+00 2.100000e-01 2.100000e-01 +2.100000e+00 0.000000e+00 0.000000e+00 1.830000e+00 2.000000e-01 2.000000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginFrascati/MUPI_1973_I95215.cc b/analyses/pluginFrascati/MUPI_1973_I95215.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/MUPI_1973_I95215.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MUPI_1973_I95215 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MUPI_1973_I95215); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(1, 1, 1); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 2); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MUPI_1973_I95215); + + +} diff --git a/analyses/pluginFrascati/MUPI_1973_I95215.info b/analyses/pluginFrascati/MUPI_1973_I95215.info new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/MUPI_1973_I95215.info @@ -0,0 +1,33 @@ +Name: MUPI_1973_I95215 +Year: 1973 +Summary: Measurement of $R$ and the hadronic cross section for energies betwee 2.6 and 3 GeV +Experiment: MUPI +Collider: ADONE +InspireID: 95215 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B47 (1973) 80-84, 1973 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ and the hadronic cross seection in $e^+e^-$ collisions by + the Mu-Pi group for energies between 2.6 and 3 GeV. + The muonic cross section is also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Ceradini:1974nt +BibTeX: '@article{Ceradini:1974nt, + author = "Ceradini, F. and Conversi, M. and D Angelo, S. and + Paoluzi, L. and Santonico, R. and Visentin, R.", + title = "{Multihadron production in e+ e- collisions up to 3 gev + total center-of-mass energy}", + journal = "Phys. Lett.", + volume = "47B", + year = "1973", + pages = "80-84", + doi = "10.1016/0370-2693(73)90574-1", + SLACcitation = "%%CITATION = PHLTA,47B,80;%%" +}' diff --git a/analyses/pluginFrascati/MUPI_1973_I95215.plot b/analyses/pluginFrascati/MUPI_1973_I95215.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/MUPI_1973_I95215.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /MUPI_1973_I95215/d01-x01-y02 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MUPI_1973_I95215/d01-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/$nb +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MUPI_1973_I95215/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/$nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginFrascati/MUPI_1973_I95215.yoda b/analyses/pluginFrascati/MUPI_1973_I95215.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginFrascati/MUPI_1973_I95215.yoda @@ -0,0 +1,22 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MUPI_1973_I95215/d01-x01-y01 +IsRef: 1 +Path: /REF/MUPI_1973_I95215/d01-x01-y01 +Title: doi:10.17182/hepdata.28037.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.600000e+00 0.000000e+00 0.000000e+00 1.830000e+01 4.700000e+00 4.700000e+00 +2.800000e+00 0.000000e+00 0.000000e+00 1.700000e+01 5.000000e+00 5.000000e+00 +3.000000e+00 0.000000e+00 0.000000e+00 1.390000e+01 5.000000e+00 5.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MUPI_1973_I95215/d01-x01-y02 +IsRef: 1 +Path: /REF/MUPI_1973_I95215/d01-x01-y02 +Title: doi:10.17182/hepdata.28037.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.600000e+00 0.000000e+00 0.000000e+00 1.470000e+00 3.800000e-01 3.800000e-01 +2.800000e+00 0.000000e+00 0.000000e+00 1.580000e+00 4.700000e-01 4.700000e-01 +3.000000e+00 0.000000e+00 0.000000e+00 1.490000e+00 5.400000e-01 5.400000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginLEP/ALEPH_1995_I382179.yoda b/analyses/pluginLEP/ALEPH_1995_I382179.yoda --- a/analyses/pluginLEP/ALEPH_1995_I382179.yoda +++ b/analyses/pluginLEP/ALEPH_1995_I382179.yoda @@ -1,120 +1,127 @@ BEGIN YODA_SCATTER2D_V2 /REF/ALEPH_1995_I382179/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -5.9, up: 5.9}, sys_1: {dn: -1.3, up: 1.3}, sys_2: {dn: -14.486999999999998, up: 14.486999999999998}}, 1: {stat: {dn: -4.8, up: 4.8}, sys_1: {dn: -0.9, up: 0.9}, sys_2: {dn: -13.878, up: 13.878}}, 2: {stat: {dn: -4.6, up: 4.6}, sys_1: {dn: -0.8, up: 0.8}, sys_2: {dn: -14.895, up: 14.895}}, 3: {stat: {dn: -4.4, up: 4.4}, sys_1: {dn: -0.8, up: 0.8}, sys_2: {dn: -15.336, up: 15.336}}, 4: {stat: {dn: -4.2, up: 4.2}, sys_1: {dn: -0.7, up: 0.7}, sys_2: {dn: -15.231, up: 15.231}}, 5: {stat: {dn: -4.4, up: 4.4}, sys_1: {dn: -0.7, up: 0.7}, sys_2: {dn: -16.155, up: 16.155}}, 6: {stat: {dn: -3.9, up: 3.9}, sys_1: {dn: -0.6, up: 0.6}, sys_2: {dn: -14.526, up: 14.526}}, 7: {stat: {dn: -3.9, up: 3.9}, sys_1: {dn: -0.7, up: 0.7}, sys_2: {dn: -14.991, up: 14.991}}, 8: {stat: {dn: -3.8, up: 3.8}, sys_1: {dn: -0.6, up: 0.6}, sys_2: {dn: -14.838000000000001, up: 14.838000000000001}}, 9: {stat: {dn: -3.6, up: 3.6}, sys_1: {dn: -0.5, up: 0.5}, sys_2: {dn: -14.216999999999999, up: 14.216999999999999}}, 10: {stat: {dn: -2.5, up: 2.5}, sys_1: {dn: -0.5, up: 0.5}, sys_2: {dn: -13.827, up: 13.827}}, 11: {stat: {dn: -2.3, up: 2.3}, sys_1: {dn: -0.5, up: 0.5}, sys_2: {dn: -12.768, up: 12.768}}, 12: {stat: {dn: -2.3, up: 2.3}, sys_1: {dn: -0.4, up: 0.4}, sys_2: {dn: -12.620999999999999, up: 12.620999999999999}}, 13: {stat: {dn: -2.2, up: 2.2}, sys_1: {dn: -0.4, up: 0.4}, sys_2: {dn: -11.415000000000001, up: 11.415000000000001}}, 14: {stat: {dn: -1.5, up: 1.5}, sys_1: {dn: -0.6, up: 0.6}, sys_2: {dn: -10.824, up: 10.824}}, 15: {stat: {dn: -1.4, up: 1.4}, sys_1: {dn: -1.8, up: 1.8}, sys_2: {dn: -9.72, up: 9.72}}, 16: {stat: {dn: -0.61, up: 0.61}, sys_1: {dn: -2.09, up: 2.09}, sys_2: {dn: -3.1187999999999994, up: 3.1187999999999994}}, 17: {stat: {dn: -0.53, up: 0.53}, sys_1: {dn: -1.02, up: 1.02}, sys_2: {dn: -2.6985, up: 2.6985}}, 18: {stat: {dn: -0.5, up: 0.5}, sys_1: {dn: -0.9, up: 0.9}, sys_2: {dn: -2.3688, up: 2.3688}}, 19: {stat: {dn: -0.35, up: 0.35}, sys_1: {dn: -0.72, up: 0.72}, sys_2: {dn: -2.0808, up: 2.0808}}, 20: {stat: {dn: -0.33, up: 0.33}, sys_1: {dn: -0.6, up: 0.6}, sys_2: {dn: -1.8405, up: 1.8405}}, 21: {stat: {dn: -0.32, up: 0.32}, sys_1: {dn: -0.49, up: 0.49}, sys_2: {dn: -1.6581000000000001, up: 1.6581000000000001}}, 22: {stat: {dn: -0.3, up: 0.3}, sys_1: {dn: -0.44, up: 0.44}, sys_2: {dn: -1.4973, up: 1.4973}}, 23: {stat: {dn: -0.29, up: 0.29}, sys_1: {dn: -0.38, up: 0.38}, sys_2: {dn: -1.3298999999999999, up: 1.3298999999999999}}, 24: {stat: {dn: -0.27, up: 0.27}, sys_1: {dn: -0.34, up: 0.34}, sys_2: {dn: -1.2072, up: 1.2072}}, 25: {stat: {dn: -0.18, up: 0.18}, sys_1: {dn: -0.3, up: 0.3}, sys_2: {dn: -1.0614, up: 1.0614}}, 26: {stat: {dn: -0.17, up: 0.17}, sys_1: {dn: -0.25, up: 0.25}, sys_2: {dn: -0.8853000000000001, up: 0.8853000000000001}}, 27: {stat: {dn: -0.16, up: 0.16}, sys_1: {dn: -0.22, up: 0.22}, sys_2: {dn: -0.7473, up: 0.7473}}, 28: {stat: {dn: -0.14, up: 0.14}, sys_1: {dn: -0.18, up: 0.18}, sys_2: {dn: -0.6317999999999999, up: 0.6317999999999999}}, 29: {stat: {dn: -0.13, up: 0.13}, sys_1: {dn: -0.16, up: 0.16}, sys_2: {dn: -0.5448000000000001, up: 0.5448000000000001}}, 30: {stat: {dn: -0.12, up: 0.12}, sys_1: {dn: -0.15, up: 0.15}, sys_2: {dn: -0.46380000000000005, up: 0.46380000000000005}}, 31: {stat: {dn: -0.12, up: 0.12}, sys_1: {dn: -0.13, up: 0.13}, sys_2: {dn: -0.4092, up: 0.4092}}, 32: {stat: {dn: -0.07, up: 0.07}, sys_1: {dn: -0.11, up: 0.11}, sys_2: {dn: -0.33, up: 0.33}}, 33: {stat: {dn: -0.066, up: 0.066}, sys_1: {dn: -0.094, up: 0.094}, sys_2: {dn: -0.25451999999999997, up: 0.25451999999999997}}, 34: {stat: {dn: -0.035, up: 0.035}, sys_1: {dn: -0.071, up: 0.071}, sys_2: {dn: -0.16863, up: 0.16863}}, 35: {stat: {dn: -0.026, up: 0.026}, sys_1: {dn: -0.047, up: 0.047}, sys_2: {dn: -0.09542999999999999, up: 0.09542999999999999}}, 36: {stat: {dn: -0.013, up: 0.013}, sys_1: {dn: -0.028, up: 0.028}, sys_2: {dn: -0.046889999999999994, up: 0.046889999999999994}}, 37: {stat: {dn: -0.0051, up: 0.0051}, sys_1: {dn: -0.01, up: 0.01}, sys_2: {dn: -0.013485, up: 0.013485}}, 38: {stat: {dn: -0.0021, up: 0.0021}, sys_1: {dn: -0.0021, up: 0.0021}, sys_2: {dn: -0.002301, up: 0.002301}}} + IsRef: 1 Path: /REF/ALEPH_1995_I382179/d01-x01-y01 -Title: ~ +Title: doi:10.17182/hepdata.48315.v1/t1 Type: Scatter2D --- -# xval xerr- xerr+ yval yerr- yerr+ -5.260000e-03 2.600000e-04 2.400000e-04 4.829000e+02 6.041523e+00 6.041523e+00 -5.740000e-03 2.400000e-04 2.600000e-04 4.626000e+02 4.883646e+00 4.883646e+00 -6.220000e-03 2.200000e-04 2.800000e-04 4.965000e+02 4.669047e+00 4.669047e+00 -6.730000e-03 2.300000e-04 2.700000e-04 5.112000e+02 4.472136e+00 4.472136e+00 -7.220000e-03 2.200000e-04 2.800000e-04 5.077000e+02 4.257934e+00 4.257934e+00 -7.730000e-03 2.300000e-04 2.700000e-04 5.385000e+02 4.455334e+00 4.455334e+00 -8.220000e-03 2.200000e-04 2.800000e-04 4.842000e+02 3.945884e+00 3.945884e+00 -8.710000e-03 2.100000e-04 2.900000e-04 4.997000e+02 3.962323e+00 3.962323e+00 -9.220000e-03 2.200000e-04 2.800000e-04 4.946000e+02 3.847077e+00 3.847077e+00 -9.720000e-03 2.200000e-04 2.800000e-04 4.739000e+02 3.634556e+00 3.634556e+00 -1.050000e-02 5.000000e-04 5.000000e-04 4.609000e+02 2.549510e+00 2.549510e+00 -1.150000e-02 5.000000e-04 5.000000e-04 4.256000e+02 2.353720e+00 2.353720e+00 -1.250000e-02 5.000000e-04 5.000000e-04 4.207000e+02 2.334524e+00 2.334524e+00 -1.350000e-02 5.000000e-04 5.000000e-04 3.805000e+02 2.236068e+00 2.236068e+00 -1.470000e-02 7.000000e-04 1.300000e-03 3.608000e+02 1.615549e+00 1.615549e+00 -1.670000e-02 7.000000e-04 1.300000e-03 3.240000e+02 2.280351e+00 2.280351e+00 -4.700000e-02 2.000000e-03 3.000000e-03 1.039600e+02 2.177200e+00 2.177200e+00 -5.200000e-02 2.000000e-03 3.000000e-03 8.995000e+01 1.149478e+00 1.149478e+00 -5.700000e-02 2.000000e-03 3.000000e-03 7.896000e+01 1.029563e+00 1.029563e+00 -6.190000e-02 1.900000e-03 3.100000e-03 6.936000e+01 8.005623e-01 8.005623e-01 -6.690000e-02 1.900000e-03 3.100000e-03 6.135000e+01 6.847627e-01 6.847627e-01 -7.190000e-02 1.900000e-03 3.100000e-03 5.527000e+01 5.852350e-01 5.852350e-01 -7.690000e-02 1.900000e-03 3.100000e-03 4.991000e+01 5.325411e-01 5.325411e-01 -8.190000e-02 1.900000e-03 3.100000e-03 4.433000e+01 4.780167e-01 4.780167e-01 -8.700000e-02 2.000000e-03 3.000000e-03 4.024000e+01 4.341659e-01 4.341659e-01 -9.420000e-02 4.200000e-03 5.800000e-03 3.538000e+01 3.498571e-01 3.498571e-01 -1.040000e-01 4.000000e-03 6.000000e-03 2.951000e+01 3.023243e-01 3.023243e-01 -1.140000e-01 4.000000e-03 6.000000e-03 2.491000e+01 2.720294e-01 2.720294e-01 -1.240000e-01 4.000000e-03 6.000000e-03 2.106000e+01 2.280351e-01 2.280351e-01 -1.340000e-01 4.000000e-03 6.000000e-03 1.816000e+01 2.061553e-01 2.061553e-01 -1.440000e-01 4.000000e-03 6.000000e-03 1.546000e+01 1.920937e-01 1.920937e-01 -1.540000e-01 4.000000e-03 6.000000e-03 1.364000e+01 1.769181e-01 1.769181e-01 -1.690000e-01 9.000000e-03 1.100000e-02 1.100000e+01 1.303840e-01 1.303840e-01 -1.890000e-01 9.000000e-03 1.100000e-02 8.484000e+00 1.148564e-01 1.148564e-01 -2.220000e-01 2.200000e-02 2.800000e-02 5.621000e+00 7.915807e-02 7.915807e-02 -2.720000e-01 2.200000e-02 2.800000e-02 3.181000e+00 5.371220e-02 5.371220e-02 -3.420000e-01 4.200000e-02 5.800000e-02 1.563000e+00 3.087070e-02 3.087070e-02 -4.760000e-01 7.600000e-02 1.240000e-01 4.495000e-01 1.122542e-02 1.122542e-02 -6.740000e-01 7.400000e-02 1.260000e-01 7.670000e-02 2.969848e-03 2.969848e-03 +# xval xerr- xerr+ yval yerr- yerr+ +5.260000e-03 2.600000e-04 2.400000e-04 4.829000e+02 1.569628e+01 1.569628e+01 +5.740000e-03 2.400000e-04 2.600000e-04 4.626000e+02 1.471220e+01 1.471220e+01 +6.220000e-03 2.200000e-04 2.800000e-04 4.965000e+02 1.560965e+01 1.560965e+01 +6.730000e-03 2.300000e-04 2.700000e-04 5.112000e+02 1.597476e+01 1.597476e+01 +7.220000e-03 2.200000e-04 2.800000e-04 5.077000e+02 1.581497e+01 1.581497e+01 +7.730000e-03 2.300000e-04 2.700000e-04 5.385000e+02 1.675810e+01 1.675810e+01 +8.220000e-03 2.200000e-04 2.800000e-04 4.842000e+02 1.505240e+01 1.505240e+01 +8.710000e-03 2.100000e-04 2.900000e-04 4.997000e+02 1.550581e+01 1.550581e+01 +9.220000e-03 2.200000e-04 2.800000e-04 4.946000e+02 1.532861e+01 1.532861e+01 +9.720000e-03 2.200000e-04 2.800000e-04 4.739000e+02 1.467423e+01 1.467423e+01 +1.050000e-02 5.000000e-04 5.000000e-04 4.609000e+02 1.406008e+01 1.406008e+01 +1.150000e-02 5.000000e-04 5.000000e-04 4.256000e+02 1.298314e+01 1.298314e+01 +1.250000e-02 5.000000e-04 5.000000e-04 4.207000e+02 1.283509e+01 1.283509e+01 +1.350000e-02 5.000000e-04 5.000000e-04 3.805000e+02 1.163195e+01 1.163195e+01 +1.470000e-02 7.000000e-04 1.300000e-03 3.608000e+02 1.094390e+01 1.094390e+01 +1.670000e-02 7.000000e-04 1.300000e-03 3.240000e+02 9.983907e+00 9.983907e+00 +4.700000e-02 2.000000e-03 3.000000e-03 1.039600e+02 3.803566e+00 3.803566e+00 +5.200000e-02 2.000000e-03 3.000000e-03 8.995000e+01 2.933122e+00 2.933122e+00 +5.700000e-02 2.000000e-03 3.000000e-03 7.896000e+01 2.582869e+00 2.582869e+00 +6.190000e-02 1.900000e-03 3.100000e-03 6.936000e+01 2.229491e+00 2.229491e+00 +6.690000e-02 1.900000e-03 3.100000e-03 6.135000e+01 1.963757e+00 1.963757e+00 +7.190000e-02 1.900000e-03 3.100000e-03 5.527000e+01 1.758350e+00 1.758350e+00 +7.690000e-02 1.900000e-03 3.100000e-03 4.991000e+01 1.589184e+00 1.589184e+00 +8.190000e-02 1.900000e-03 3.100000e-03 4.433000e+01 1.413200e+00 1.413200e+00 +8.700000e-02 2.000000e-03 3.000000e-03 4.024000e+01 1.282900e+00 1.282900e+00 +9.420000e-02 4.200000e-03 5.800000e-03 3.538000e+01 1.117573e+00 1.117573e+00 +1.040000e-01 4.000000e-03 6.000000e-03 2.951000e+01 9.354978e-01 9.354978e-01 +1.140000e-01 4.000000e-03 6.000000e-03 2.491000e+01 7.952718e-01 7.952718e-01 +1.240000e-01 4.000000e-03 6.000000e-03 2.106000e+01 6.716928e-01 6.716928e-01 +1.340000e-01 4.000000e-03 6.000000e-03 1.816000e+01 5.825007e-01 5.825007e-01 +1.440000e-01 4.000000e-03 6.000000e-03 1.546000e+01 5.020064e-01 5.020064e-01 +1.540000e-01 4.000000e-03 6.000000e-03 1.364000e+01 4.458079e-01 4.458079e-01 +1.690000e-01 9.000000e-03 1.100000e-02 1.100000e+01 3.548239e-01 3.548239e-01 +1.890000e-01 9.000000e-03 1.100000e-02 8.484000e+00 2.792354e-01 2.792354e-01 +2.220000e-01 2.200000e-02 2.800000e-02 5.621000e+00 1.862849e-01 1.862849e-01 +2.720000e-01 2.200000e-02 2.800000e-02 3.181000e+00 1.095075e-01 1.095075e-01 +3.420000e-01 4.200000e-02 5.800000e-02 1.563000e+00 5.613976e-02 5.613976e-02 +4.760000e-01 7.600000e-02 1.240000e-01 4.495000e-01 1.754580e-02 1.754580e-02 +6.740000e-01 7.400000e-02 1.260000e-01 7.670000e-02 3.756940e-03 3.756940e-03 END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ALEPH_1995_I382179/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -1.12, up: 1.12}, sys: {dn: -0.01, up: 0.01}}, 1: {stat: {dn: -0.91, up: 0.91}, sys: {dn: -0.01, up: 0.01}}, 2: {stat: {dn: -0.9, up: 0.9}, sys: {dn: -0.01, up: 0.01}}, 3: {stat: {dn: -0.92, up: 0.92}, sys: {dn: -0.02, up: 0.02}}, 4: {stat: {dn: -0.88, up: 0.88}, sys: {dn: -0.02, up: 0.02}}, 5: {stat: {dn: -0.9, up: 0.9}, sys: {dn: -0.02, up: 0.02}}, 6: {stat: {dn: -0.86, up: 0.86}, sys: {dn: -0.05, up: 0.05}}, 7: {stat: {dn: -0.88, up: 0.88}, sys: {dn: -0.12, up: 0.12}}, 8: {stat: {dn: -0.66, up: 0.66}, sys: {dn: -0.5, up: 0.5}}, 9: {stat: {dn: -0.47, up: 0.47}, sys: {dn: -0.68, up: 0.68}}, 10: {stat: {dn: -0.53, up: 0.53}, sys: {dn: -2.2, up: 2.2}}, 11: {stat: {dn: -0.3, up: 0.3}, sys: {dn: -1.28, up: 1.28}}, 12: {stat: {dn: -0.26, up: 0.26}, sys: {dn: -0.98, up: 0.98}}, 13: {stat: {dn: -0.23, up: 0.23}, sys: {dn: -0.83, up: 0.83}}, 14: {stat: {dn: -0.21, up: 0.21}, sys: {dn: -0.71, up: 0.71}}, 15: {stat: {dn: -0.14, up: 0.14}, sys: {dn: -0.56, up: 0.56}}, 16: {stat: {dn: -0.13, up: 0.13}, sys: {dn: -0.47, up: 0.47}}, 17: {stat: {dn: -0.11, up: 0.11}, sys: {dn: -0.37, up: 0.37}}, 18: {stat: {dn: -0.11, up: 0.11}, sys: {dn: -0.32, up: 0.32}}, 19: {stat: {dn: -0.1, up: 0.1}, sys: {dn: -0.28, up: 0.28}}, 20: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.24, up: 0.24}}, 21: {stat: {dn: -0.09, up: 0.09}, sys: {dn: -0.22, up: 0.22}}, 22: {stat: {dn: -0.06, up: 0.06}, sys: {dn: -0.18, up: 0.18}}, 23: {stat: {dn: -0.05, up: 0.05}, sys: {dn: -0.15, up: 0.15}}, 24: {stat: {dn: -0.029, up: 0.029}, sys: {dn: -0.109, up: 0.109}}, 25: {stat: {dn: -0.025, up: 0.025}, sys: {dn: -0.076, up: 0.076}}, 26: {stat: {dn: -0.013, up: 0.013}, sys: {dn: -0.043, up: 0.043}}, 27: {stat: {dn: -0.0053, up: 0.0053}, sys: {dn: -0.0146, up: 0.0146}}, 28: {stat: {dn: -0.0022, up: 0.0022}, sys: {dn: -0.0031, up: 0.0031}}} -BEGIN YODA_SCATTER2D_V2 /REF/ALEPH_1995_I382179/d02-x01-y01 IsRef: 1 Path: /REF/ALEPH_1995_I382179/d02-x01-y01 -Title: ~ +Title: doi:10.17182/hepdata.48315.v1/t2 Type: Scatter2D --- -# xval xerr- xerr+ yval yerr- yerr+ +# xval xerr- xerr+ yval yerr- yerr+ 5.740000e-03 2.400000e-04 2.600000e-04 1.240000e+01 1.120045e+00 1.120045e+00 6.220000e-03 2.200000e-04 2.800000e-04 1.327000e+01 9.100549e-01 9.100549e-01 6.730000e-03 2.300000e-04 2.700000e-04 1.533000e+01 9.000556e-01 9.000556e-01 7.220000e-03 2.200000e-04 2.800000e-04 1.743000e+01 9.202174e-01 9.202174e-01 7.730000e-03 2.300000e-04 2.700000e-04 1.833000e+01 8.802272e-01 8.802272e-01 8.220000e-03 2.200000e-04 2.800000e-04 1.962000e+01 9.002222e-01 9.002222e-01 8.710000e-03 2.100000e-04 2.900000e-04 2.002000e+01 8.614523e-01 8.614523e-01 9.220000e-03 2.200000e-04 2.800000e-04 2.166000e+01 8.881441e-01 8.881441e-01 1.350000e-02 5.000000e-04 5.000000e-04 2.584000e+01 8.280097e-01 8.280097e-01 1.470000e-02 7.000000e-04 1.300000e-03 2.746000e+01 8.266196e-01 8.266196e-01 1.670000e-02 7.000000e-04 1.300000e-03 2.763000e+01 2.262941e+00 2.262941e+00 7.190000e-02 1.900000e-03 3.100000e-03 1.060000e+01 1.314686e+00 1.314686e+00 7.690000e-02 1.900000e-03 3.100000e-03 9.530000e+00 1.013903e+00 1.013903e+00 8.190000e-02 1.900000e-03 3.100000e-03 9.150000e+00 8.612781e-01 8.612781e-01 8.700000e-02 2.000000e-03 3.000000e-03 8.410000e+00 7.404053e-01 7.404053e-01 9.420000e-02 4.200000e-03 5.800000e-03 7.960000e+00 5.772348e-01 5.772348e-01 1.040000e-01 4.000000e-03 6.000000e-03 7.260000e+00 4.876474e-01 4.876474e-01 1.140000e-01 4.000000e-03 6.000000e-03 6.340000e+00 3.860052e-01 3.860052e-01 1.240000e-01 4.000000e-03 6.000000e-03 5.630000e+00 3.383785e-01 3.383785e-01 1.340000e-01 4.000000e-03 6.000000e-03 4.940000e+00 2.973214e-01 2.973214e-01 1.440000e-01 4.000000e-03 6.000000e-03 4.390000e+00 2.563201e-01 2.563201e-01 1.540000e-01 4.000000e-03 6.000000e-03 4.220000e+00 2.376973e-01 2.376973e-01 1.690000e-01 9.000000e-03 1.100000e-02 3.630000e+00 1.897367e-01 1.897367e-01 1.890000e-01 9.000000e-03 1.100000e-02 3.100000e+00 1.581139e-01 1.581139e-01 2.220000e-01 2.200000e-02 2.800000e-02 2.245000e+00 1.127918e-01 1.127918e-01 2.720000e-01 2.200000e-02 2.800000e-02 1.538000e+00 8.000625e-02 8.000625e-02 3.420000e-01 4.200000e-02 5.800000e-02 8.410000e-01 4.492215e-02 4.492215e-02 4.760000e-01 7.600000e-02 1.240000e-01 2.936000e-01 1.553222e-02 1.553222e-02 6.740000e-01 7.400000e-02 1.260000e-01 5.960000e-02 3.801316e-03 3.801316e-03 END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ALEPH_1995_I382179/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.35, up: 0.35}, sys: {dn: -0.0, up: 0.0}}, 1: {stat: {dn: -0.36, up: 0.36}, sys: {dn: -0.0, up: 0.0}}, 2: {stat: {dn: -0.36, up: 0.36}, sys: {dn: -0.01, up: 0.01}}, 3: {stat: {dn: -0.38, up: 0.38}, sys: {dn: -0.01, up: 0.01}}, 4: {stat: {dn: -0.26, up: 0.26}, sys: {dn: -0.01, up: 0.01}}, 5: {stat: {dn: -0.27, up: 0.27}, sys: {dn: -0.04, up: 0.04}}, 6: {stat: {dn: -0.18, up: 0.18}, sys: {dn: -0.23, up: 0.23}}, 7: {stat: {dn: -0.18, up: 0.18}, sys: {dn: -0.44, up: 0.44}}, 8: {stat: {dn: -0.216, up: 0.216}, sys: {dn: -0.876, up: 0.876}}, 9: {stat: {dn: -0.183, up: 0.183}, sys: {dn: -0.639, up: 0.639}}, 10: {stat: {dn: -0.162, up: 0.162}, sys: {dn: -0.549, up: 0.549}}, 11: {stat: {dn: -0.154, up: 0.154}, sys: {dn: -0.474, up: 0.474}}, 12: {stat: {dn: -0.092, up: 0.092}, sys: {dn: -0.355, up: 0.355}}, 13: {stat: {dn: -0.084, up: 0.084}, sys: {dn: -0.292, up: 0.292}}, 14: {stat: {dn: -0.077, up: 0.077}, sys: {dn: -0.232, up: 0.232}}, 15: {stat: {dn: -0.072, up: 0.072}, sys: {dn: -0.205, up: 0.205}}, 16: {stat: {dn: -0.068, up: 0.068}, sys: {dn: -0.178, up: 0.178}}, 17: {stat: {dn: -0.064, up: 0.064}, sys: {dn: -0.162, up: 0.162}}, 18: {stat: {dn: -0.061, up: 0.061}, sys: {dn: -0.146, up: 0.146}}, 19: {stat: {dn: -0.041, up: 0.041}, sys: {dn: -0.118, up: 0.118}}, 20: {stat: {dn: -0.036, up: 0.036}, sys: {dn: -0.099, up: 0.099}}, 21: {stat: {dn: -0.02, up: 0.02}, sys: {dn: -0.073, up: 0.073}}, 22: {stat: {dn: -0.017, up: 0.017}, sys: {dn: -0.054, up: 0.054}}, 23: {stat: {dn: -0.009, up: 0.009}, sys: {dn: -0.031, up: 0.031}}, 24: {stat: {dn: -0.0034, up: 0.0034}, sys: {dn: -0.011, up: 0.011}}, 25: {stat: {dn: -0.0011, up: 0.0011}, sys: {dn: -0.0022, up: 0.0022}}} -BEGIN YODA_SCATTER2D_V2 /REF/ALEPH_1995_I382179/d03-x01-y01 IsRef: 1 Path: /REF/ALEPH_1995_I382179/d03-x01-y01 -Title: ~ +Title: doi:10.17182/hepdata.48315.v1/t3 Type: Scatter2D --- -# xval xerr- xerr+ yval yerr- yerr+ +# xval xerr- xerr+ yval yerr- yerr+ 1.050000e-02 5.000000e-04 5.000000e-04 8.320000e+00 3.500000e-01 3.500000e-01 1.150000e-02 5.000000e-04 5.000000e-04 8.950000e+00 3.600000e-01 3.600000e-01 1.250000e-02 5.000000e-04 5.000000e-04 9.800000e+00 3.601389e-01 3.601389e-01 1.350000e-02 5.000000e-04 5.000000e-04 1.030000e+01 3.801316e-01 3.801316e-01 1.470000e-02 7.000000e-04 1.300000e-03 1.070000e+01 2.601922e-01 2.601922e-01 1.670000e-02 7.000000e-04 1.300000e-03 1.158000e+01 2.729469e-01 2.729469e-01 2.470000e-02 7.000000e-04 1.300000e-03 1.237000e+01 2.920616e-01 2.920616e-01 2.680000e-02 8.000000e-04 1.200000e-03 1.246000e+01 4.753946e-01 4.753946e-01 7.190000e-02 1.900000e-03 3.100000e-03 5.315000e+00 9.022372e-01 9.022372e-01 7.690000e-02 1.900000e-03 3.100000e-03 5.008000e+00 6.646879e-01 6.646879e-01 8.190000e-02 1.900000e-03 3.100000e-03 4.445000e+00 5.724028e-01 5.724028e-01 8.700000e-02 2.000000e-03 3.000000e-03 4.555000e+00 4.983894e-01 4.983894e-01 9.420000e-02 4.200000e-03 5.800000e-03 3.742000e+00 3.667274e-01 3.667274e-01 1.040000e-01 4.000000e-03 6.000000e-03 3.355000e+00 3.038421e-01 3.038421e-01 1.140000e-01 4.000000e-03 6.000000e-03 2.905000e+00 2.444443e-01 2.444443e-01 1.240000e-01 4.000000e-03 6.000000e-03 2.653000e+00 2.172763e-01 2.172763e-01 1.340000e-01 4.000000e-03 6.000000e-03 2.371000e+00 1.905466e-01 1.905466e-01 1.440000e-01 4.000000e-03 6.000000e-03 2.137000e+00 1.741838e-01 1.741838e-01 1.540000e-01 4.000000e-03 6.000000e-03 1.878000e+00 1.582308e-01 1.582308e-01 1.690000e-01 9.000000e-03 1.100000e-02 1.696000e+00 1.249200e-01 1.249200e-01 1.890000e-01 9.000000e-03 1.100000e-02 1.299000e+00 1.053423e-01 1.053423e-01 2.220000e-01 2.200000e-02 2.800000e-02 9.660000e-01 7.569016e-02 7.569016e-02 2.720000e-01 2.200000e-02 2.800000e-02 6.140000e-01 5.661272e-02 5.661272e-02 3.420000e-01 4.200000e-02 5.800000e-02 3.050000e-01 3.228002e-02 3.228002e-02 4.760000e-01 7.600000e-02 1.240000e-01 7.840000e-02 1.151347e-02 1.151347e-02 6.740000e-01 7.400000e-02 1.260000e-01 5.400000e-03 2.459675e-03 2.459675e-03 END YODA_SCATTER2D_V2 diff --git a/analyses/pluginLEP/ALEPH_1999_S4193598.cc b/analyses/pluginLEP/ALEPH_1999_S4193598.cc --- a/analyses/pluginLEP/ALEPH_1999_S4193598.cc +++ b/analyses/pluginLEP/ALEPH_1999_S4193598.cc @@ -1,78 +1,78 @@ // -*- C++ -*- #include "Rivet/Analysis.hh" #include "Rivet/Projections/Beam.hh" #include "Rivet/Projections/ChargedFinalState.hh" #include "Rivet/Projections/UnstableParticles.hh" namespace Rivet { class ALEPH_1999_S4193598 : public Analysis { public: /// @name Constructors etc. //@{ /// Constructor ALEPH_1999_S4193598() : Analysis("ALEPH_1999_S4193598") { } //@} public: /// Book histograms and initialise projections before the run void init() { declare(Beam(), "Beams"); declare(UnstableParticles(), "UFS"); declare(ChargedFinalState(), "CFS"); _h_Xe_Ds = bookHisto1D(1, 1, 1); } /// Perform the per-event analysis void analyze(const Event& event) { const double weight = event.weight(); // Trigger condition const ChargedFinalState& cfs = apply(event, "CFS"); if (cfs.size() < 5) vetoEvent; const UnstableParticles& ufs = apply(event, "UFS"); // Get beams and average beam momentum const ParticlePair& beams = apply(event, "Beams").beams(); const double meanBeamMom = ( beams.first.p3().mod() + beams.second.p3().mod() ) / 2.0/GeV; // Accept all D*+- decays. Normalisation to data in finalize for (const Particle& p : filter_select(ufs.particles(), Cuts::abspid==PID::DSTARPLUS)) { // Scaled energy. const double energy = p.E()/GeV; const double scaledEnergy = energy/meanBeamMom; _h_Xe_Ds->fill(scaledEnergy, weight); } } /// Normalise histograms etc., after the run void finalize() { // Normalize to data integral - normalize(_h_Xe_Ds, 0.00498); + normalize(_h_Xe_Ds, 4.98); } private: Histo1DPtr _h_Xe_Ds; }; // The hook for the plugin system DECLARE_RIVET_PLUGIN(ALEPH_1999_S4193598); } diff --git a/analyses/pluginLEP/ALEPH_1999_S4193598.plot b/analyses/pluginLEP/ALEPH_1999_S4193598.plot --- a/analyses/pluginLEP/ALEPH_1999_S4193598.plot +++ b/analyses/pluginLEP/ALEPH_1999_S4193598.plot @@ -1,6 +1,6 @@ # BEGIN PLOT /ALEPH_1999_S4193598/d01-x01-y01 Title=Scaled energy of $D^{*\pm}$ in $e^+e^-\to Z\to\text{hadronic}$ at $\sqrt{s}=91.2$~GeV XLabel=$X_E$ -YLabel=$1/N_\text{Zhad} \text{d}N(D^{*})/\text{d}X_E$ +YLabel=$1000/N_\text{Zhad} \text{d}N(D^{*})/\text{d}X_E$ LogY=0 # END PLOT diff --git a/analyses/pluginLEP/ALEPH_1999_S4193598.yoda b/analyses/pluginLEP/ALEPH_1999_S4193598.yoda --- a/analyses/pluginLEP/ALEPH_1999_S4193598.yoda +++ b/analyses/pluginLEP/ALEPH_1999_S4193598.yoda @@ -1,46 +1,53 @@ BEGIN YODA_SCATTER2D_V2 /REF/ALEPH_1999_S4193598/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {error: {dn: -0.63, up: 0.63}}, 1: {error: {dn: -0.49, up: 0.49}}, 2: {error: {dn: -0.44, up: 0.44}}, 3: {error: {dn: -0.43, up: 0.43}}, 4: {error: {dn: -0.38, up: 0.38}}, 5: {error: {dn: -0.35, up: 0.35}}, 6: {error: {dn: -0.32, up: 0.32}}, 7: {error: {dn: -0.28, up: 0.28}}, 8: {error: {dn: -0.27, up: 0.27}}, 9: {error: {dn: -0.24, up: 0.24}}, 10: {error: {dn: -0.22, up: 0.22}}, 11: {error: {dn: -0.18, up: 0.18}}, 12: {error: {dn: -0.17, up: 0.17}}, 13: {error: {dn: -0.14, up: 0.14}}, 14: {error: {dn: -0.11, up: 0.11}}, 15: {error: {dn: -0.07, up: 0.07}}, 16: {error: {dn: -0.05, up: 0.05}}, 17: {error: {dn: -0.03, up: 0.03}}} + IsRef: 1 Path: /REF/ALEPH_1999_S4193598/d01-x01-y01 -Title: ~ +Title: doi:10.17182/hepdata.49183.v1/t1 Type: Scatter2D --- -# xval xerr- xerr+ yval yerr- yerr+ -1.250000e-01 2.500000e-02 2.500000e-02 7.470000e-03 6.300000e-04 6.300000e-04 -1.750000e-01 2.500000e-02 2.500000e-02 9.030000e-03 4.900000e-04 4.900000e-04 -2.250000e-01 2.500000e-02 2.500000e-02 1.042000e-02 4.400000e-04 4.400000e-04 -2.750000e-01 2.500000e-02 2.500000e-02 1.076000e-02 4.300000e-04 4.300000e-04 -3.250000e-01 2.500000e-02 2.500000e-02 9.890000e-03 3.800000e-04 3.800000e-04 -3.750000e-01 2.500000e-02 2.500000e-02 8.970000e-03 3.500000e-04 3.500000e-04 -4.250000e-01 2.500000e-02 2.500000e-02 8.170000e-03 3.200000e-04 3.200000e-04 -4.750000e-01 2.500000e-02 2.500000e-02 6.940000e-03 2.800000e-04 2.800000e-04 -5.250000e-01 2.500000e-02 2.500000e-02 6.730000e-03 2.700000e-04 2.700000e-04 -5.750000e-01 2.500000e-02 2.500000e-02 5.560000e-03 2.400000e-04 2.400000e-04 -6.250000e-01 2.500000e-02 2.500000e-02 4.940000e-03 2.200000e-04 2.200000e-04 -6.750000e-01 2.500000e-02 2.500000e-02 3.490000e-03 1.800000e-04 1.800000e-04 -7.250000e-01 2.500000e-02 2.500000e-02 3.130000e-03 1.700000e-04 1.700000e-04 -7.750000e-01 2.500000e-02 2.500000e-02 2.000000e-03 1.400000e-04 1.400000e-04 -8.250000e-01 2.500000e-02 2.500000e-02 1.270000e-03 1.100000e-04 1.100000e-04 -8.750000e-01 2.500000e-02 2.500000e-02 5.000000e-04 7.000000e-05 7.000000e-05 -9.250000e-01 2.500000e-02 2.500000e-02 2.700000e-04 5.000000e-05 5.000000e-05 -9.750000e-01 2.500000e-02 2.500000e-02 6.000000e-05 3.000000e-05 3.000000e-05 +# xval xerr- xerr+ yval yerr- yerr+ +1.250000e-01 2.500000e-02 2.500000e-02 7.470000e+00 6.300000e-01 6.300000e-01 +1.750000e-01 2.500000e-02 2.500000e-02 9.030000e+00 4.900000e-01 4.900000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.042000e+01 4.400000e-01 4.400000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 1.076000e+01 4.300000e-01 4.300000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 9.890000e+00 3.800000e-01 3.800000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 8.970000e+00 3.500000e-01 3.500000e-01 +4.250000e-01 2.500000e-02 2.500000e-02 8.170000e+00 3.200000e-01 3.200000e-01 +4.750000e-01 2.500000e-02 2.500000e-02 6.940000e+00 2.800000e-01 2.800000e-01 +5.250000e-01 2.500000e-02 2.500000e-02 6.730000e+00 2.700000e-01 2.700000e-01 +5.750000e-01 2.500000e-02 2.500000e-02 5.560000e+00 2.400000e-01 2.400000e-01 +6.250000e-01 2.500000e-02 2.500000e-02 4.940000e+00 2.200000e-01 2.200000e-01 +6.750000e-01 2.500000e-02 2.500000e-02 3.490000e+00 1.800000e-01 1.800000e-01 +7.250000e-01 2.500000e-02 2.500000e-02 3.130000e+00 1.700000e-01 1.700000e-01 +7.750000e-01 2.500000e-02 2.500000e-02 2.000000e+00 1.400000e-01 1.400000e-01 +8.250000e-01 2.500000e-02 2.500000e-02 1.270000e+00 1.100000e-01 1.100000e-01 +8.750000e-01 2.500000e-02 2.500000e-02 5.000000e-01 7.000000e-02 7.000000e-02 +9.250000e-01 2.500000e-02 2.500000e-02 2.700000e-01 5.000000e-02 5.000000e-02 +9.750000e-01 2.500000e-02 2.500000e-02 6.000000e-02 3.000000e-02 3.000000e-02 END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ALEPH_1999_S4193598/d02-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -6.7e-05, up: 6.7e-05}, sys: {dn: -7.2e-05, up: 7.2e-05}}} -BEGIN YODA_SCATTER2D_V2 /REF/ALEPH_1999_S4193598/d02-x01-y01 IsRef: 1 Path: /REF/ALEPH_1999_S4193598/d02-x01-y01 -Title: ~ +Title: doi:10.17182/hepdata.49183.v1/t2 Type: Scatter2D --- -# xval xerr- xerr+ yval yerr- yerr+ +# xval xerr- xerr+ yval yerr- yerr+ 5.000000e-01 5.000000e-01 5.000000e-01 5.114000e-03 9.835141e-05 9.835141e-05 END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/ALEPH_1999_S4193598/d03-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {stat: {dn: -0.0047, up: 0.0047}, sys_1: {dn: -0.0088, up: 0.0088}, sys_2: {dn: -0.0075, up: 0.0075}}} -BEGIN YODA_SCATTER2D_V2 /REF/ALEPH_1999_S4193598/d03-x01-y01 IsRef: 1 Path: /REF/ALEPH_1999_S4193598/d03-x01-y01 -Title: ~ +Title: doi:10.17182/hepdata.49183.v1/t3 Type: Scatter2D --- -# xval xerr- xerr+ yval yerr- yerr+ -9.120000e+01 5.000000e-01 5.000000e-01 1.738000e-01 1.248119e-02 1.248119e-02 +# xval xerr- xerr+ yval yerr- yerr+ +9.120000e+01 0.000000e+00 0.000000e+00 1.738000e-01 1.248119e-02 1.248119e-02 END YODA_SCATTER2D_V2 diff --git a/analyses/pluginLEP/OPAL_2004_I631361.cc b/analyses/pluginLEP/OPAL_2004_I631361.cc --- a/analyses/pluginLEP/OPAL_2004_I631361.cc +++ b/analyses/pluginLEP/OPAL_2004_I631361.cc @@ -1,119 +1,336 @@ // -*- C++ -*- #include "Rivet/Analysis.hh" #include "Rivet/Projections/FinalState.hh" #include "Rivet/Projections/ChargedFinalState.hh" +#include "Rivet/Projections/FastJets.hh" +#include "Rivet/Projections/HadronicFinalState.hh" +#include "Rivet/Jet.hh" +#include "Rivet/Tools/BinnedHistogram.hh" +#include "fastjet/JetDefinition.hh" + +namespace fastjet { + +class P_scheme : public JetDefinition::Recombiner { + public: + std::string description() const {return "";} + void recombine(const PseudoJet & pa, const PseudoJet & pb, + PseudoJet & pab) const { + PseudoJet tmp = pa + pb; + double E = sqrt(tmp.px()*tmp.px() + tmp.py()*tmp.py() + tmp.pz()*tmp.pz()); + pab.reset_momentum(tmp.px(), tmp.py(), tmp.pz(), E); + } + void preprocess(PseudoJet & p) const { + double E = sqrt(p.px()*p.px() + p.py()*p.py() + p.pz()*p.pz()); + p.reset_momentum(p.px(), p.py(), p.pz(), E); + } + ~P_scheme() { } +}; + +} namespace Rivet { class OPAL_2004_I631361 : public Analysis { public: /// Constructor OPAL_2004_I631361() - : Analysis("OPAL_2004_I631361"), _sumW(0.0) + : Analysis("OPAL_2004_I631361"), _mode(0), _sumW(0.0), _sumWEbin(7,0.) { } /// @name Analysis methods //@{ + int getEbin(double E_glue) { + int ih = -1; + if (inRange(E_glue/GeV, 5.0, 5.5)) { + ih = 0; + } else if (inRange(E_glue/GeV, 5.5, 6.5)) { + ih = 1; + } else if (inRange(E_glue/GeV, 6.5, 7.5)) { + ih = 2; + } else if (inRange(E_glue/GeV, 7.5, 9.5)) { + ih = 3; + } else if (inRange(E_glue/GeV, 9.5, 13.0)) { + ih = 4; + } else if (inRange(E_glue/GeV, 13.0, 16.0)) { + ih = 5; + } else if (inRange(E_glue/GeV, 16.0, 20.0)) { + ih = 6; + } + assert(ih >= 0); + return ih; + } + void init() { - declare(FinalState(), "FS"); - declare(ChargedFinalState(), "CFS"); - int ih(0), iy(0); - if (inRange(0.5*sqrtS()/GeV, 5.0, 5.5)) { - ih = 1; - iy = 1; - } else if (inRange(0.5*sqrtS()/GeV, 5.5, 6.5)) { - ih = 1; - iy = 2; - } else if (inRange(0.5*sqrtS()/GeV, 6.5, 7.5)) { - ih = 1; - iy = 3; - } else if (inRange(0.5*sqrtS()/GeV, 7.5, 9.5)) { - ih = 2; - iy = 1; - } else if (inRange(0.5*sqrtS()/GeV, 9.5, 13.0)) { - ih = 2; - iy = 2; - } else if (inRange(0.5*sqrtS()/GeV, 13.0, 16.0)) { - ih = 3; - iy = 1; - } else if (inRange(0.5*sqrtS()/GeV, 16.0, 20.0)) { - ih = 3; - iy = 2; + // Get options from the new option system + _mode = 0; + if ( getOption("PROCESS") == "GG" ) _mode = 0; + if ( getOption("PROCESS") == "QQ" ) _mode = 1; + // projections we need for both cases + const FinalState fs; + addProjection(fs, "FS"); + const ChargedFinalState cfs; + addProjection(cfs, "CFS"); + // additional projections for q qbar + if(_mode==1) { + addProjection(HadronicFinalState(fs), "HFS"); + addProjection(HadronicFinalState(cfs), "HCFS"); } - assert(ih>0); - _h_chMult = bookHisto1D(ih,1,iy); - if(ih==3) - _h_chFragFunc = bookHisto1D(5,1,iy); - else - _h_chFragFunc = nullptr; + // book the histograms + if(_mode==0) { + int ih(0), iy(0); + if (inRange(0.5*sqrtS()/GeV, 5.0, 5.5)) { + ih = 1; + iy = 1; + } else if (inRange(0.5*sqrtS()/GeV, 5.5, 6.5)) { + ih = 1; + iy = 2; + } else if (inRange(0.5*sqrtS()/GeV, 6.5, 7.5)) { + ih = 1; + iy = 3; + } else if (inRange(0.5*sqrtS()/GeV, 7.5, 9.5)) { + ih = 2; + iy = 1; + } else if (inRange(0.5*sqrtS()/GeV, 9.5, 13.0)) { + ih = 2; + iy = 2; + } else if (inRange(0.5*sqrtS()/GeV, 13.0, 16.0)) { + ih = 3; + iy = 1; + } else if (inRange(0.5*sqrtS()/GeV, 16.0, 20.0)) { + ih = 3; + iy = 2; + } + assert(ih>0); + _h_chMult_gg = bookHisto1D(ih,1,iy); + if(ih==3) + _h_chFragFunc_gg = bookHisto1D(5,1,iy); + else + _h_chFragFunc_gg = nullptr; + } + else { + _h_chMult_qq.addHistogram(5.0, 5.5, bookHisto1D(1,1,1)); + _h_chMult_qq.addHistogram(5.5, 6.5, bookHisto1D(1,1,2)); + _h_chMult_qq.addHistogram(6.5, 7.5, bookHisto1D(1,1,3)); + _h_chMult_qq.addHistogram(7.5, 9.5, bookHisto1D(2,1,1)); + _h_chMult_qq.addHistogram(9.5, 13.0, bookHisto1D(2,1,2)); + _h_chMult_qq.addHistogram(13.0, 16.0, bookHisto1D(3,1,1)); + _h_chMult_qq.addHistogram(16.0, 20.0, bookHisto1D(3,1,2)); + + _h_chFragFunc_qq.addHistogram(13.0, 16.0, bookHisto1D(5,1,1)); + _h_chFragFunc_qq.addHistogram(16.0, 20.0, bookHisto1D(5,1,2)); + } } /// Perform the per-event analysis void analyze(const Event& event) { const double weight = event.weight(); - // find the initial gluons - ParticleVector initial; - for (ConstGenParticlePtr p : HepMCUtils::particles(event.genEvent())) { - ConstGenVertexPtr pv = p->production_vertex(); - const PdgId pid = p->pdg_id(); - if(pid!=21) continue; - bool passed = false; - for (ConstGenParticlePtr pp : HepMCUtils::particles(pv, Relatives::PARENTS)) { - const PdgId ppid = abs(pp->pdg_id()); - passed = (ppid == PID::ELECTRON || ppid == PID::HIGGS || - ppid == PID::ZBOSON || ppid == PID::GAMMA); - if(passed) break; - } - if(passed) initial.push_back(Particle(*p)); + // gg mode + if(_mode==0) { + // find the initial gluons + ParticleVector initial; + for (ConstGenParticlePtr p : HepMCUtils::particles(event.genEvent())) { + ConstGenVertexPtr pv = p->production_vertex(); + const PdgId pid = p->pdg_id(); + if(pid!=21) continue; + bool passed = false; + for (ConstGenParticlePtr pp : HepMCUtils::particles(pv, Relatives::PARENTS)) { + const PdgId ppid = abs(pp->pdg_id()); + passed = (ppid == PID::ELECTRON || ppid == PID::HIGGS || + ppid == PID::ZBOSON || ppid == PID::GAMMA); + if(passed) break; + } + if(passed) initial.push_back(Particle(*p)); + } + if(initial.size()!=2) vetoEvent; + // use the direction for the event axis + Vector3 axis = initial[0].momentum().p3().unit(); + // fill histograms + const Particles& chps = applyProjection(event, "CFS").particles(); + unsigned int nMult[2] = {0,0}; + _sumW += 2.*weight; + // distribution + foreach(const Particle& p, chps) { + double xE = 2.*p.E()/sqrtS(); + if(_h_chFragFunc_gg) _h_chFragFunc_gg->fill(xE, weight); + if(p.momentum().p3().dot(axis)>0.) + ++nMult[0]; + else + ++nMult[1]; + } + // multiplcities in jet + _h_chMult_gg->fill(nMult[0],weight); + _h_chMult_gg->fill(nMult[1],weight); } - if(initial.size()!=2) vetoEvent; - // use the direction for the event axis - Vector3 axis = initial[0].momentum().p3().unit(); - // fill histograms - const Particles& chps = applyProjection(event, "CFS").particles(); - unsigned int nMult[2] = {0,0}; - _sumW += 2.*weight; - // distribution - foreach(const Particle& p, chps) { - double xE = 2.*p.E()/sqrtS(); - if(_h_chFragFunc) _h_chFragFunc->fill(xE, weight); - if(p.momentum().p3().dot(axis)>0.) - ++nMult[0]; - else - ++nMult[1]; + // qqbar mode + else { + // cut on the number of charged particles + const Particles& chParticles = applyProjection(event, "CFS").particles(); + if(chParticles.size() < 5) vetoEvent; + // cluster the jets + const Particles& particles = applyProjection(event, "FS").particles(); + fastjet::JetDefinition ee_kt_def(fastjet::ee_kt_algorithm, &p_scheme); + PseudoJets pParticles; + foreach(Particle p, particles) { + PseudoJet temp = p.pseudojet(); + if(p.fromBottom()) { + temp.set_user_index(5); + } + pParticles.push_back(temp); + } + fastjet::ClusterSequence cluster(pParticles, ee_kt_def); + // rescale energys to just keep the directions of the jets + // and keep track of b tags + PseudoJets pJets = sorted_by_E(cluster.exclusive_jets_up_to(3)); + if(pJets.size() < 3) vetoEvent; + array dirs; + for(int i=0; i<3; i++) { + dirs[i] = Vector3(pJets[i].px(),pJets[i].py(),pJets[i].pz()).unit(); + } + array bTagged; + Jets jets; + for(int i=0; i<3; i++) { + double Ejet = sqrtS()*sin(angle(dirs[(i+1)%3],dirs[(i+2)%3])) / + (sin(angle(dirs[i],dirs[(i+1)%3])) + sin(angle(dirs[i],dirs[(i+2)%3])) + sin(angle(dirs[(i+1)%3],dirs[(i+2)%3]))); + jets.push_back(FourMomentum(Ejet,Ejet*dirs[i].x(),Ejet*dirs[i].y(),Ejet*dirs[i].z())); + bTagged[i] = false; + foreach(PseudoJet particle, pJets[i].constituents()) { + if(particle.user_index() > 1 and !bTagged[i]) { + bTagged[i] = true; + } + } + } + + int QUARK1 = 0, QUARK2 = 1, GLUON = 2; + + if(jets[QUARK2].E() > jets[QUARK1].E()) swap(QUARK1, QUARK2); + if(jets[GLUON].E() > jets[QUARK1].E()) swap(QUARK1, GLUON); + if(!bTagged[QUARK2]) { + if(!bTagged[GLUON]) vetoEvent; + else swap(QUARK2, GLUON); + } + if(bTagged[GLUON]) vetoEvent; + + // exclude collinear or soft jets + double k1 = jets[QUARK1].E()*min(angle(jets[QUARK1].momentum(),jets[QUARK2].momentum()), + angle(jets[QUARK1].momentum(),jets[GLUON].momentum())); + double k2 = jets[QUARK2].E()*min(angle(jets[QUARK2].momentum(),jets[QUARK1].momentum()), + angle(jets[QUARK2].momentum(),jets[GLUON].momentum())); + if(k1<8.0*GeV || k2<8.0*GeV) vetoEvent; + + double sqg = (jets[QUARK1].momentum()+jets[GLUON].momentum()).mass2(); + double sgq = (jets[QUARK2].momentum()+jets[GLUON].momentum()).mass2(); + double s = (jets[QUARK1].momentum()+jets[QUARK2].momentum()+jets[GLUON].momentum()).mass2(); + + double Eg = 0.5*sqrt(sqg*sgq/s); + + if(Eg < 5.0 || Eg > 20.0) { vetoEvent; } + else if(Eg > 9.5) { + //requirements for experimental reconstructability raise as energy raises + if(!bTagged[QUARK1]) { + vetoEvent; + } + } + + // all cuts applied, increment sum of weights + _sumWEbin[getEbin(Eg)] += weight; + + + // transform to frame with event in y-z and glue jet in z direction + Matrix3 glueTOz(jets[GLUON].momentum().vector3(), Vector3(0,0,1)); + Vector3 transQuark = glueTOz*jets[QUARK2].momentum().vector3(); + Matrix3 quarksTOyz(Vector3(transQuark.x(), transQuark.y(), 0), Vector3(0,1,0)); + + // work out transformation to symmetric frame + array x_cm; + array x_cm_y; + array x_cm_z; + array x_pr; + for(int i=0; i<3; i++) { + x_cm[i] = 2*jets[i].E()/sqrt(s); + Vector3 p_transf = quarksTOyz*glueTOz*jets[i].p3(); + x_cm_y[i] = 2*p_transf.y()/sqrt(s); + x_cm_z[i] = 2*p_transf.z()/sqrt(s); + } + x_pr[GLUON] = sqrt(4*(1-x_cm[QUARK1])*(1-x_cm[QUARK2])/(3+x_cm[GLUON])); + x_pr[QUARK1] = x_pr[GLUON]/(1-x_cm[QUARK1]); + x_pr[QUARK2] = x_pr[GLUON]/(1-x_cm[QUARK2]); + double gamma = (x_pr[QUARK1] + x_pr[GLUON] + x_pr[QUARK2])/2; + double beta_z = x_pr[GLUON]/(gamma*x_cm[GLUON]) - 1; + double beta_y = (x_pr[QUARK2]/gamma - x_cm[QUARK2] - beta_z*x_cm_z[QUARK2])/x_cm_y[QUARK2]; + + LorentzTransform toSymmetric = LorentzTransform::mkObjTransformFromBeta(Vector3(0.,beta_y,beta_z)). + postMult(quarksTOyz*glueTOz); + + FourMomentum transGlue = toSymmetric.transform(jets[GLUON].momentum()); + double cutAngle = angle(toSymmetric.transform(jets[QUARK2].momentum()), transGlue)/2; + + int nCh = 0; + foreach(const Particle& chP, chParticles ) { + FourMomentum pSymmFrame = toSymmetric.transform(FourMomentum(chP.p3().mod(), chP.px(), chP.py(), chP.pz())); + if(angle(pSymmFrame, transGlue) < cutAngle) { + _h_chFragFunc_qq.fill(Eg, pSymmFrame.E()*sin(cutAngle)/Eg, weight); + nCh++; + } + } + _h_chMult_qq.fill(Eg, nCh, weight); } - // multiplcities in jet - _h_chMult->fill(nMult[0],weight); - _h_chMult->fill(nMult[1],weight); } /// Normalise histograms etc., after the run void finalize() { - normalize(_h_chMult); - if(_h_chFragFunc) scale(_h_chFragFunc, 1./_sumW); + if(_mode==0) { + normalize(_h_chMult_gg); + if(_h_chFragFunc_gg) scale(_h_chFragFunc_gg, 1./_sumW); + } + else { + foreach(Histo1DPtr hist, _h_chMult_qq.getHistograms()) { + normalize(hist); + } + for(int i=0; i<2; i++) { + if(!isZero(_sumWEbin[i+5])) { + scale(_h_chFragFunc_qq.getHistograms()[i], 1./_sumWEbin[i+5]); + } + } + } } //@} private: + // the mode + unsigned int _mode; + double _sumW; /// @name Histograms //@{ - Histo1DPtr _h_chMult; - Histo1DPtr _h_chFragFunc; + Histo1DPtr _h_chMult_gg; + Histo1DPtr _h_chFragFunc_gg; + //@} + + + // Data members like post-cuts event weight counters go here + vector _sumWEbin; + + // p scheme jet definition + fastjet::P_scheme p_scheme; + + /// @name Histograms + //@{ + BinnedHistogram _h_chMult_qq; + BinnedHistogram _h_chFragFunc_qq; //@} }; // The hook for the plugin system DECLARE_RIVET_PLUGIN(OPAL_2004_I631361); } diff --git a/analyses/pluginLEP/OPAL_2004_I631361.info b/analyses/pluginLEP/OPAL_2004_I631361.info --- a/analyses/pluginLEP/OPAL_2004_I631361.info +++ b/analyses/pluginLEP/OPAL_2004_I631361.info @@ -1,48 +1,54 @@ Name: OPAL_2004_I631361 Year: 2004 Summary: Gluon jet charged multiplicities and fragmentation functions Experiment: OPAL Collider: LEP InspireID: 631361 Status: VALIDATED Authors: - Daniel Reichelt References: - Phys. Rev. D69, 032002,2004 - hep-ex/0310048 RunInfo: - The fictional $e^+e^-\to gg$ process is required. + The fictional $e^+e^-\to gg$ process NumEvents: 100000 NeedCrossSection: no Beams: [e+, e- ] -Energies: [10.50,11.96,13.96,16.86,21.84,28.48,35.44] +Energies: [10.50,11.96,13.96,16.86,21.84,28.48,35.44,91,2] +Options: + - PROCESS=GG,QQ NeedCrossSection: False Description: - ' Measurement of gluon jet properties using the jet boost algorithm, a technique to select unbiased samples of gluon jets in $e^+e^-$ annihilation, i.e. gluon jets free of biases introduced by event selection or jet finding criteria. This analysis requires the fictional $e^+e^-\to g g $ process to be used due to the corrections applied to the data. It allows the study of gluon jet properties. This analysis can be used for tuning etc..' + ' Measurement of gluon jet properties using the jet boost algorithm, a technique to select unbiased samples of gluon jets in $e^+e^-$ annihilation, i.e. gluon jets free of biases introduced by event selection or jet finding criteria. +Two modes are provided, the prefer option is to produce the fictional $e^+e^-\to g g $ process to be used due to the corrections applied to the data, PROCESS=GG. +The original analysis technique to extract gluon jets from hadronic $e^+e^-$ events using $e^+e^-\to q\bar{q}$ events, PROCESS=QQ, +is also provided but cannot be used for tuning as the data has been corrected for impurities, however it is still useful qualitatively in order to check the properties of gluon jets in the original way in which there were measured rather than using a fictitious process.' BibKey: Abbiendi:2004gh BibTeX: '@article{Abbiendi:2004gh, author = "Abbiendi, G. and others", title = "{Experimental studies of unbiased gluon jets from $e^{+} e^{-}$ annihilations using the jet boost algorithm}", collaboration = "OPAL", journal = "Phys. Rev.", volume = "D69", year = "2004", pages = "032002", doi = "10.1103/PhysRevD.69.032002", eprint = "hep-ex/0310048", archivePrefix = "arXiv", primaryClass = "hep-ex", reportNumber = "CERN-EP-2004-067", SLACcitation = "%%CITATION = HEP-EX/0310048;%%" }' Validation: - $A LEP-10.5-gg - $A-2 LEP-11.96-gg - $A-3 LEP-13.96-gg - $A-4 LEP-16.86-gg - $A-5 LEP-21.84-gg - $A-6 LEP-28.48-gg - $A-7 LEP-35.44-gg + - $A-8 LEP-91; rivet $< -a $A:PROCESS=QQ -o $@ diff --git a/analyses/pluginLEP/OPAL_2004_I631361_qq.cc b/analyses/pluginLEP/OPAL_2004_I631361_qq.cc deleted file mode 100644 --- a/analyses/pluginLEP/OPAL_2004_I631361_qq.cc +++ /dev/null @@ -1,241 +0,0 @@ -// -*- C++ -*- -#include "Rivet/Analysis.hh" -#include "Rivet/Projections/FinalState.hh" -#include "Rivet/Projections/ChargedFinalState.hh" -#include "Rivet/Projections/FastJets.hh" -#include "Rivet/Projections/HadronicFinalState.hh" -#include "Rivet/Jet.hh" -#include "Rivet/Tools/BinnedHistogram.hh" -#include "fastjet/JetDefinition.hh" - -namespace fastjet { - -class P_scheme : public JetDefinition::Recombiner { - public: - std::string description() const {return "";} - void recombine(const PseudoJet & pa, const PseudoJet & pb, - PseudoJet & pab) const { - PseudoJet tmp = pa + pb; - double E = sqrt(tmp.px()*tmp.px() + tmp.py()*tmp.py() + tmp.pz()*tmp.pz()); - pab.reset_momentum(tmp.px(), tmp.py(), tmp.pz(), E); - } - void preprocess(PseudoJet & p) const { - double E = sqrt(p.px()*p.px() + p.py()*p.py() + p.pz()*p.pz()); - p.reset_momentum(p.px(), p.py(), p.pz(), E); - } - ~P_scheme() { } -}; - -} - -namespace Rivet { - - class OPAL_2004_I631361_qq : public Analysis { - public: - - /// Constructor - OPAL_2004_I631361_qq() - : Analysis("OPAL_2004_I631361_qq"), _sumWEbin(7,0.) - { } - - /// @name Analysis methods - //@{ - int getEbin(double E_glue) { - int ih = -1; - if (inRange(E_glue/GeV, 5.0, 5.5)) { - ih = 0; - } else if (inRange(E_glue/GeV, 5.5, 6.5)) { - ih = 1; - } else if (inRange(E_glue/GeV, 6.5, 7.5)) { - ih = 2; - } else if (inRange(E_glue/GeV, 7.5, 9.5)) { - ih = 3; - } else if (inRange(E_glue/GeV, 9.5, 13.0)) { - ih = 4; - } else if (inRange(E_glue/GeV, 13.0, 16.0)) { - ih = 5; - } else if (inRange(E_glue/GeV, 16.0, 20.0)) { - ih = 6; - } - assert(ih >= 0); - return ih; - } - - /// Book histograms and initialise projections before the run - void init() { - - const FinalState fs; - addProjection(fs, "FS"); - addProjection(HadronicFinalState(fs), "HFS"); - - const ChargedFinalState cfs; - addProjection(cfs, "CFS"); - addProjection(HadronicFinalState(cfs), "HCFS"); - - _h_chMult.addHistogram(5.0, 5.5, bookHisto1D(1,1,1)); - _h_chMult.addHistogram(5.5, 6.5, bookHisto1D(1,1,2)); - _h_chMult.addHistogram(6.5, 7.5, bookHisto1D(1,1,3)); - _h_chMult.addHistogram(7.5, 9.5, bookHisto1D(2,1,1)); - _h_chMult.addHistogram(9.5, 13.0, bookHisto1D(2,1,2)); - _h_chMult.addHistogram(13.0, 16.0, bookHisto1D(3,1,1)); - _h_chMult.addHistogram(16.0, 20.0, bookHisto1D(3,1,2)); - - _h_chFragFunc.addHistogram(13.0, 16.0, bookHisto1D(5,1,1)); - _h_chFragFunc.addHistogram(16.0, 20.0, bookHisto1D(5,1,2)); - - } - - - /// Perform the per-event analysis - void analyze(const Event& event) { - // cut on the number of charged particles - const Particles& chParticles = applyProjection(event, "CFS").particles(); - if(chParticles.size() < 5) vetoEvent; - // cluster the jets - const Particles& particles = applyProjection(event, "FS").particles(); - fastjet::JetDefinition ee_kt_def(fastjet::ee_kt_algorithm, &p_scheme); - PseudoJets pParticles; - foreach(Particle p, particles) { - PseudoJet temp = p.pseudojet(); - if(p.fromBottom()) { - temp.set_user_index(5); - } - pParticles.push_back(temp); - } - fastjet::ClusterSequence cluster(pParticles, ee_kt_def); - // rescale energys to just keep the directions of the jets - // and keep track of b tags - PseudoJets pJets = sorted_by_E(cluster.exclusive_jets_up_to(3)); - if(pJets.size() < 3) vetoEvent; - array dirs; - for(int i=0; i<3; i++) { - dirs[i] = Vector3(pJets[i].px(),pJets[i].py(),pJets[i].pz()).unit(); - } - array bTagged; - Jets jets; - for(int i=0; i<3; i++) { - double Ejet = sqrtS()*sin(angle(dirs[(i+1)%3],dirs[(i+2)%3])) / - (sin(angle(dirs[i],dirs[(i+1)%3])) + sin(angle(dirs[i],dirs[(i+2)%3])) + sin(angle(dirs[(i+1)%3],dirs[(i+2)%3]))); - jets.push_back(FourMomentum(Ejet,Ejet*dirs[i].x(),Ejet*dirs[i].y(),Ejet*dirs[i].z())); - bTagged[i] = false; - foreach(PseudoJet particle, pJets[i].constituents()) { - if(particle.user_index() > 1 and !bTagged[i]) { - bTagged[i] = true; - } - } - } - - int QUARK1 = 0, QUARK2 = 1, GLUON = 2; - - if(jets[QUARK2].E() > jets[QUARK1].E()) swap(QUARK1, QUARK2); - if(jets[GLUON].E() > jets[QUARK1].E()) swap(QUARK1, GLUON); - if(!bTagged[QUARK2]) { - if(!bTagged[GLUON]) vetoEvent; - else swap(QUARK2, GLUON); - } - if(bTagged[GLUON]) vetoEvent; - - // exclude collinear or soft jets - double k1 = jets[QUARK1].E()*min(angle(jets[QUARK1].momentum(),jets[QUARK2].momentum()), - angle(jets[QUARK1].momentum(),jets[GLUON].momentum())); - double k2 = jets[QUARK2].E()*min(angle(jets[QUARK2].momentum(),jets[QUARK1].momentum()), - angle(jets[QUARK2].momentum(),jets[GLUON].momentum())); - if(k1<8.0*GeV || k2<8.0*GeV) vetoEvent; - - double sqg = (jets[QUARK1].momentum()+jets[GLUON].momentum()).mass2(); - double sgq = (jets[QUARK2].momentum()+jets[GLUON].momentum()).mass2(); - double s = (jets[QUARK1].momentum()+jets[QUARK2].momentum()+jets[GLUON].momentum()).mass2(); - - double Eg = 0.5*sqrt(sqg*sgq/s); - - if(Eg < 5.0 || Eg > 20.0) { vetoEvent; } - else if(Eg > 9.5) { - //requirements for experimental reconstructability raise as energy raises - if(!bTagged[QUARK1]) { - vetoEvent; - } - } - - // all cuts applied, increment sum of weights - const double weight = event.weight(); - _sumWEbin[getEbin(Eg)] += weight; - - - // transform to frame with event in y-z and glue jet in z direction - Matrix3 glueTOz(jets[GLUON].momentum().vector3(), Vector3(0,0,1)); - Vector3 transQuark = glueTOz*jets[QUARK2].momentum().vector3(); - Matrix3 quarksTOyz(Vector3(transQuark.x(), transQuark.y(), 0), Vector3(0,1,0)); - - // work out transformation to symmetric frame - array x_cm; - array x_cm_y; - array x_cm_z; - array x_pr; - for(int i=0; i<3; i++) { - x_cm[i] = 2*jets[i].E()/sqrt(s); - Vector3 p_transf = quarksTOyz*glueTOz*jets[i].p3(); - x_cm_y[i] = 2*p_transf.y()/sqrt(s); - x_cm_z[i] = 2*p_transf.z()/sqrt(s); - } - x_pr[GLUON] = sqrt(4*(1-x_cm[QUARK1])*(1-x_cm[QUARK2])/(3+x_cm[GLUON])); - x_pr[QUARK1] = x_pr[GLUON]/(1-x_cm[QUARK1]); - x_pr[QUARK2] = x_pr[GLUON]/(1-x_cm[QUARK2]); - double gamma = (x_pr[QUARK1] + x_pr[GLUON] + x_pr[QUARK2])/2; - double beta_z = x_pr[GLUON]/(gamma*x_cm[GLUON]) - 1; - double beta_y = (x_pr[QUARK2]/gamma - x_cm[QUARK2] - beta_z*x_cm_z[QUARK2])/x_cm_y[QUARK2]; - - LorentzTransform toSymmetric = LorentzTransform::mkObjTransformFromBeta(Vector3(0.,beta_y,beta_z)). - postMult(quarksTOyz*glueTOz); - - FourMomentum transGlue = toSymmetric.transform(jets[GLUON].momentum()); - double cutAngle = angle(toSymmetric.transform(jets[QUARK2].momentum()), transGlue)/2; - - int nCh = 0; - foreach(const Particle& chP, chParticles ) { - FourMomentum pSymmFrame = toSymmetric.transform(FourMomentum(chP.p3().mod(), chP.px(), chP.py(), chP.pz())); - if(angle(pSymmFrame, transGlue) < cutAngle) { - _h_chFragFunc.fill(Eg, pSymmFrame.E()*sin(cutAngle)/Eg, weight); - nCh++; - } - } - _h_chMult.fill(Eg, nCh, weight); - } - - /// Normalise histograms etc., after the run - void finalize() { - - foreach(Histo1DPtr hist, _h_chMult.getHistograms()) { - normalize(hist); - } - for(int i=0; i<2; i++) { - if(!isZero(_sumWEbin[i+5])) { - scale(_h_chFragFunc.getHistograms()[i], 1./_sumWEbin[i+5]); - } - } - } - - //@} - - - private: - - // Data members like post-cuts event weight counters go here - vector _sumWEbin; - - // p scheme jet definition - fastjet::P_scheme p_scheme; - - /// @name Histograms - //@{ - BinnedHistogram _h_chMult; - BinnedHistogram _h_chFragFunc; - //@} - - - }; - - - - // The hook for the plugin system - DECLARE_RIVET_PLUGIN(OPAL_2004_I631361_qq); -} diff --git a/analyses/pluginLEP/OPAL_2004_I631361_qq.info b/analyses/pluginLEP/OPAL_2004_I631361_qq.info deleted file mode 100644 --- a/analyses/pluginLEP/OPAL_2004_I631361_qq.info +++ /dev/null @@ -1,42 +0,0 @@ -Name: OPAL_2004_I631361_qq -Year: 2004 -Summary: Gluon jet charged multiplicities and fragmentation functions -Experiment: OPAL -Collider: LEP -InspireID: 631361 -Status: VALIDATED -Authors: - - Daniel Reichelt -References: - - Phys. Rev. D69, 032002,2004 - - hep-ex/0310048 -RunInfo: - $e^+e^-\to q\bar q$. -NumEvents: 100000 -NeedCrossSection: no -Beams: [e+, e- ] -Energies: [91.2] -NeedCrossSection: False -Description: - ' Measurement of gluon jet properties using the jet boost algorithm, a technique to select unbiased samples of gluon jets in $e^+e^-$ annihilation, i.e. gluon jets free of biases introduced by event selection or jet finding criteria. This analysis uses the original analysis technique to extract gluon jets from hadronic $e^+e^-$ events. It cannot therefore be used for tuning as the data has been corrected for impurities, however it is still useful qualitatively in order to check the properties of gluon jets in the original way in which there were measured rather than using a fictitious process.' -BibKey: Abbiendi:2004gh -BibTeX: '@article{Abbiendi:2004gh, - author = "Abbiendi, G. and others", - title = "{Experimental studies of unbiased gluon jets from $e^{+} - e^{-}$ annihilations using the jet boost algorithm}", - collaboration = "OPAL", - journal = "Phys. Rev.", - volume = "D69", - year = "2004", - pages = "032002", - doi = "10.1103/PhysRevD.69.032002", - eprint = "hep-ex/0310048", - archivePrefix = "arXiv", - primaryClass = "hep-ex", - reportNumber = "CERN-EP-2004-067", - SLACcitation = "%%CITATION = HEP-EX/0310048;%%" -}' - -Validation: - - $A LEP-91 - diff --git a/analyses/pluginLEP/OPAL_2004_I631361_qq.plot b/analyses/pluginLEP/OPAL_2004_I631361_qq.plot deleted file mode 100644 --- a/analyses/pluginLEP/OPAL_2004_I631361_qq.plot +++ /dev/null @@ -1,75 +0,0 @@ -# BEGIN PLOT /OPAL_2004_I631361_qq/d01-x01-y01 -Title=Charged particle multiplicity, $E^*_g=5.25~\mathrm{GeV}$ -XLabel=$n^\mathrm{ch.}_\mathrm{gluon}$ -YLabel=$P(n^\mathrm{ch.}_\mathrm{gluon})$ -LogX=0 -LogY=0 -LogZ=0 -# END PLOT - -# BEGIN PLOT /OPAL_2004_I631361_qq/d01-x01-y02 -Title=Charged particle multiplicity, $E^*_g=5.98~\mathrm{GeV}$ -XLabel=$n^\mathrm{ch.}_\mathrm{gluon}$ -YLabel=$P(n^\mathrm{ch.}_\mathrm{gluon})$ -LogX=0 -LogY=0 -LogZ=0 -# END PLOT - -# BEGIN PLOT /OPAL_2004_I631361_qq/d01-x01-y03 -Title=Charged particle multiplicity, $E^*_g=6.98~\mathrm{GeV}$ -XLabel=$n^\mathrm{ch.}_\mathrm{gluon}$ -YLabel=$P(n^\mathrm{ch.}_\mathrm{gluon})$ -LogX=0 -LogY=0 -LogZ=0 -# END PLOT - -# BEGIN PLOT /OPAL_2004_I631361_qq/d02-x01-y01 -Title=Charged particle multiplicity, $E^*_g=8.43~\mathrm{GeV}$ -XLabel=$n^\mathrm{ch.}_\mathrm{gluon}$ -YLabel=$P(n^\mathrm{ch.}_\mathrm{gluon})$ -LogX=0 -LogY=0 -LogZ=0 -# END PLOT - -# BEGIN PLOT /OPAL_2004_I631361_qq/d02-x01-y02 -Title=Charged particle multiplicity, $E^*_g=10.92~\mathrm{GeV}$ -XLabel=$n^\mathrm{ch.}_\mathrm{gluon}$ -YLabel=$P(n^\mathrm{ch.}_\mathrm{gluon})$ -LogX=0 -LogY=0 -LogZ=0 -# END PLOT - -# BEGIN PLOT /OPAL_2004_I631361_qq/d03-x01-y01 -Title=Charged particle multiplicity, $E^*_g=14.24~\mathrm{GeV}$ -XLabel=$n^\mathrm{ch.}_\mathrm{gluon}$ -YLabel=$P(n^\mathrm{ch.}_\mathrm{gluon})$ -LogX=0 -LogY=0 -LogZ=0 -# END PLOT - -# BEGIN PLOT /OPAL_2004_I631361_qq/d03-x01-y02 -Title=Charged particle multiplicity, $E^*_g=17.72~\mathrm{GeV}$ -XLabel=$n^\mathrm{ch.}_\mathrm{gluon}$ -YLabel=$P(n^\mathrm{ch.}_\mathrm{gluon})$ -LogX=0 -LogY=0 -LogZ=0 -# END PLOT - -# BEGIN PLOT /OPAL_2004_I631361_qq/d05-x01-y01 -Title=Charged particle fragmentation function, $E^*_g=14.24~\mathrm{GeV}$ -XLabel=$x^*_\mathrm{E}$ -YLabel=$\frac{1}{N}\frac{\mathop{dn^\mathrm{ch.}_\mathrm{gluon}}}{\mathop{dx^*_\mathrm{E}}}$ -# END PLOT - -# BEGIN PLOT /OPAL_2004_I631361_qq/d05-x01-y02 -Title=Charged particle fragmentation function, $E^*_g=17.72~\mathrm{GeV}$ -XLabel=$x^*_\mathrm{E}$ -YLabel=$\frac{1}{N}\frac{\mathop{dn^\mathrm{ch.}_\mathrm{gluon}}}{\mathop{dx^*_\mathrm{E}}}$ -# END PLOT - diff --git a/analyses/pluginLEP/OPAL_2004_I631361_qq.yoda b/analyses/pluginLEP/OPAL_2004_I631361_qq.yoda deleted file mode 100644 --- a/analyses/pluginLEP/OPAL_2004_I631361_qq.yoda +++ /dev/null @@ -1,284 +0,0 @@ -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d01-x01-y01 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d01-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -0.000000e+00 5.000000e-01 5.000000e-01 3.600000e-03 3.710795e-03 3.710795e-03 -1.000000e+00 5.000000e-01 5.000000e-01 2.660000e-02 7.116881e-03 7.116881e-03 -2.000000e+00 5.000000e-01 5.000000e-01 8.080000e-02 1.037545e-02 1.037545e-02 -3.000000e+00 5.000000e-01 5.000000e-01 1.490000e-01 1.028251e-02 1.028251e-02 -4.000000e+00 5.000000e-01 5.000000e-01 1.982000e-01 8.563294e-03 8.563294e-03 -5.000000e+00 5.000000e-01 5.000000e-01 1.990000e-01 1.341641e-02 1.341641e-02 -6.000000e+00 5.000000e-01 5.000000e-01 1.540000e-01 1.166190e-02 1.166190e-02 -7.000000e+00 5.000000e-01 5.000000e-01 1.000000e-01 7.481310e-03 7.481310e-03 -8.000000e+00 5.000000e-01 5.000000e-01 5.450000e-02 5.693856e-03 5.693856e-03 -9.000000e+00 5.000000e-01 5.000000e-01 2.300000e-02 2.418677e-03 2.418677e-03 -1.000000e+01 5.000000e-01 5.000000e-01 7.900000e-03 1.697056e-03 1.697056e-03 -1.100000e+01 5.000000e-01 5.000000e-01 2.320000e-03 8.459905e-04 8.459905e-04 -1.200000e+01 5.000000e-01 5.000000e-01 4.100000e-04 4.964877e-04 4.964877e-04 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d01-x01-y02 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d01-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -0.000000e+00 5.000000e-01 5.000000e-01 2.500000e-03 2.549510e-03 2.549510e-03 -1.000000e+00 5.000000e-01 5.000000e-01 1.900000e-02 4.237924e-03 4.237924e-03 -2.000000e+00 5.000000e-01 5.000000e-01 6.180000e-02 5.458938e-03 5.458938e-03 -3.000000e+00 5.000000e-01 5.000000e-01 1.186000e-01 6.365532e-03 6.365532e-03 -4.000000e+00 5.000000e-01 5.000000e-01 1.794000e-01 6.395311e-03 6.395311e-03 -5.000000e+00 5.000000e-01 5.000000e-01 1.935000e-01 6.660330e-03 6.660330e-03 -6.000000e+00 5.000000e-01 5.000000e-01 1.769000e-01 7.294518e-03 7.294518e-03 -7.000000e+00 5.000000e-01 5.000000e-01 1.236000e-01 6.010824e-03 6.010824e-03 -8.000000e+00 5.000000e-01 5.000000e-01 7.100000e-02 3.764306e-03 3.764306e-03 -9.000000e+00 5.000000e-01 5.000000e-01 3.300000e-02 2.758623e-03 2.758623e-03 -1.000000e+01 5.000000e-01 5.000000e-01 1.390000e-02 2.109502e-03 2.109502e-03 -1.100000e+01 5.000000e-01 5.000000e-01 5.000000e-03 1.565248e-03 1.565248e-03 -1.200000e+01 5.000000e-01 5.000000e-01 1.290000e-03 8.586617e-04 8.586617e-04 -1.300000e+01 5.000000e-01 5.000000e-01 3.400000e-04 3.488553e-04 3.488553e-04 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d01-x01-y03 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d01-x01-y03 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -0.000000e+00 5.000000e-01 5.000000e-01 1.900000e-03 1.941649e-03 1.941649e-03 -1.000000e+00 5.000000e-01 5.000000e-01 1.170000e-02 6.987131e-03 6.987131e-03 -2.000000e+00 5.000000e-01 5.000000e-01 4.270000e-02 6.109828e-03 6.109828e-03 -3.000000e+00 5.000000e-01 5.000000e-01 9.430000e-02 8.628441e-03 8.628441e-03 -4.000000e+00 5.000000e-01 5.000000e-01 1.494000e-01 1.118258e-02 1.118258e-02 -5.000000e+00 5.000000e-01 5.000000e-01 1.857000e-01 1.053945e-02 1.053945e-02 -6.000000e+00 5.000000e-01 5.000000e-01 1.803000e-01 9.264988e-03 9.264988e-03 -7.000000e+00 5.000000e-01 5.000000e-01 1.422000e-01 8.405355e-03 8.405355e-03 -8.000000e+00 5.000000e-01 5.000000e-01 9.610000e-02 7.766595e-03 7.766595e-03 -9.000000e+00 5.000000e-01 5.000000e-01 5.430000e-02 6.041523e-03 6.041523e-03 -1.000000e+01 5.000000e-01 5.000000e-01 2.560000e-02 4.031129e-03 4.031129e-03 -1.100000e+01 5.000000e-01 5.000000e-01 1.060000e-02 2.282542e-03 2.282542e-03 -1.200000e+01 5.000000e-01 5.000000e-01 3.900000e-03 1.220656e-03 1.220656e-03 -1.300000e+01 5.000000e-01 5.000000e-01 9.400000e-04 6.981404e-04 6.981404e-04 -1.400000e+01 5.000000e-01 5.000000e-01 1.700000e-04 2.404163e-04 2.404163e-04 -1.500000e+01 5.000000e-01 5.000000e-01 1.700000e-04 1.802776e-04 1.802776e-04 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d02-x01-y01 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d02-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -0.000000e+00 5.000000e-01 5.000000e-01 1.200000e-03 1.236932e-03 1.236932e-03 -1.000000e+00 5.000000e-01 5.000000e-01 6.900000e-03 6.675328e-03 6.675328e-03 -2.000000e+00 5.000000e-01 5.000000e-01 2.800000e-02 7.736924e-03 7.736924e-03 -3.000000e+00 5.000000e-01 5.000000e-01 6.460000e-02 8.321658e-03 8.321658e-03 -4.000000e+00 5.000000e-01 5.000000e-01 1.157000e-01 8.276473e-03 8.276473e-03 -5.000000e+00 5.000000e-01 5.000000e-01 1.621000e-01 9.964437e-03 9.964437e-03 -6.000000e+00 5.000000e-01 5.000000e-01 1.783000e-01 9.082401e-03 9.082401e-03 -7.000000e+00 5.000000e-01 5.000000e-01 1.632000e-01 9.706184e-03 9.706184e-03 -8.000000e+00 5.000000e-01 5.000000e-01 1.207000e-01 8.276473e-03 8.276473e-03 -9.000000e+00 5.000000e-01 5.000000e-01 7.560000e-02 7.111259e-03 7.111259e-03 -1.000000e+01 5.000000e-01 5.000000e-01 4.430000e-02 5.700877e-03 5.700877e-03 -1.100000e+01 5.000000e-01 5.000000e-01 2.260000e-02 3.257299e-03 3.257299e-03 -1.200000e+01 5.000000e-01 5.000000e-01 1.030000e-02 2.154066e-03 2.154066e-03 -1.300000e+01 5.000000e-01 5.000000e-01 4.400000e-03 1.341641e-03 1.341641e-03 -1.400000e+01 5.000000e-01 5.000000e-01 1.410000e-03 8.300602e-04 8.300602e-04 -1.500000e+01 5.000000e-01 5.000000e-01 4.800000e-04 3.883298e-04 3.883298e-04 -1.600000e+01 5.000000e-01 5.000000e-01 1.900000e-04 1.655295e-04 1.655295e-04 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d02-x01-y02 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d02-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -0.000000e+00 5.000000e-01 5.000000e-01 8.000000e-04 8.944272e-04 8.944272e-04 -1.000000e+00 5.000000e-01 5.000000e-01 4.700000e-03 4.850773e-03 4.850773e-03 -2.000000e+00 5.000000e-01 5.000000e-01 1.520000e-02 5.470832e-03 5.470832e-03 -3.000000e+00 5.000000e-01 5.000000e-01 3.730000e-02 6.747592e-03 6.747592e-03 -4.000000e+00 5.000000e-01 5.000000e-01 7.490000e-02 8.627862e-03 8.627862e-03 -5.000000e+00 5.000000e-01 5.000000e-01 1.083000e-01 9.492102e-03 9.492102e-03 -6.000000e+00 5.000000e-01 5.000000e-01 1.419000e-01 1.145600e-02 1.145600e-02 -7.000000e+00 5.000000e-01 5.000000e-01 1.530000e-01 1.062544e-02 1.062544e-02 -8.000000e+00 5.000000e-01 5.000000e-01 1.428000e-01 1.058017e-02 1.058017e-02 -9.000000e+00 5.000000e-01 5.000000e-01 1.173000e-01 9.990495e-03 9.990495e-03 -1.000000e+01 5.000000e-01 5.000000e-01 8.620000e-02 8.780091e-03 8.780091e-03 -1.100000e+01 5.000000e-01 5.000000e-01 5.500000e-02 6.414047e-03 6.414047e-03 -1.200000e+01 5.000000e-01 5.000000e-01 3.200000e-02 4.669047e-03 4.669047e-03 -1.300000e+01 5.000000e-01 5.000000e-01 1.720000e-02 4.313931e-03 4.313931e-03 -1.400000e+01 5.000000e-01 5.000000e-01 7.400000e-03 2.483948e-03 2.483948e-03 -1.500000e+01 5.000000e-01 5.000000e-01 4.200000e-03 1.702939e-03 1.702939e-03 -1.600000e+01 5.000000e-01 5.000000e-01 1.100000e-03 1.208305e-03 1.208305e-03 -1.700000e+01 5.000000e-01 5.000000e-01 4.000000e-04 5.656854e-04 5.656854e-04 -1.800000e+01 5.000000e-01 5.000000e-01 1.800000e-04 2.545584e-04 2.545584e-04 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d03-x01-y01 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d03-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -0.000000e+00 5.000000e-01 5.000000e-01 1.000000e-04 1.414214e-04 1.414214e-04 -1.000000e+00 5.000000e-01 5.000000e-01 5.000000e-04 7.071068e-04 7.071068e-04 -2.000000e+00 5.000000e-01 5.000000e-01 6.800000e-03 4.560702e-03 4.560702e-03 -3.000000e+00 5.000000e-01 5.000000e-01 1.790000e-02 7.780103e-03 7.780103e-03 -4.000000e+00 5.000000e-01 5.000000e-01 3.630000e-02 1.110180e-02 1.110180e-02 -5.000000e+00 5.000000e-01 5.000000e-01 7.200000e-02 1.360147e-02 1.360147e-02 -6.000000e+00 5.000000e-01 5.000000e-01 9.900000e-02 1.431782e-02 1.431782e-02 -7.000000e+00 5.000000e-01 5.000000e-01 1.310000e-01 1.886796e-02 1.886796e-02 -8.000000e+00 5.000000e-01 5.000000e-01 1.370000e-01 1.720465e-02 1.720465e-02 -9.000000e+00 5.000000e-01 5.000000e-01 1.320000e-01 1.476482e-02 1.476482e-02 -1.000000e+01 5.000000e-01 5.000000e-01 1.160000e-01 1.708801e-02 1.708801e-02 -1.100000e+01 5.000000e-01 5.000000e-01 9.240000e-02 1.431782e-02 1.431782e-02 -1.200000e+01 5.000000e-01 5.000000e-01 6.700000e-02 1.341641e-02 1.341641e-02 -1.300000e+01 5.000000e-01 5.000000e-01 4.700000e-02 1.166190e-02 1.166190e-02 -1.400000e+01 5.000000e-01 5.000000e-01 2.500000e-02 9.219544e-03 9.219544e-03 -1.500000e+01 5.000000e-01 5.000000e-01 1.447000e-02 4.472136e-03 4.472136e-03 -1.600000e+01 5.000000e-01 5.000000e-01 5.100000e-03 4.338202e-03 4.338202e-03 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d03-x01-y02 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d03-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -0.000000e+00 5.000000e-01 5.000000e-01 4.000000e-05 4.123106e-05 4.123106e-05 -1.000000e+00 5.000000e-01 5.000000e-01 4.000000e-04 5.656854e-04 5.656854e-04 -2.000000e+00 5.000000e-01 5.000000e-01 1.300000e-03 1.838478e-03 1.838478e-03 -3.000000e+00 5.000000e-01 5.000000e-01 8.000000e-03 9.183137e-03 9.183137e-03 -4.000000e+00 5.000000e-01 5.000000e-01 1.800000e-02 1.702939e-02 1.702939e-02 -5.000000e+00 5.000000e-01 5.000000e-01 4.700000e-02 2.280351e-02 2.280351e-02 -6.000000e+00 5.000000e-01 5.000000e-01 6.700000e-02 2.983287e-02 2.983287e-02 -7.000000e+00 5.000000e-01 5.000000e-01 1.020000e-01 3.667424e-02 3.667424e-02 -8.000000e+00 5.000000e-01 5.000000e-01 1.030000e-01 3.701351e-02 3.701351e-02 -9.000000e+00 5.000000e-01 5.000000e-01 1.250000e-01 4.341659e-02 4.341659e-02 -1.000000e+01 5.000000e-01 5.000000e-01 1.430000e-01 3.860052e-02 3.860052e-02 -1.100000e+01 5.000000e-01 5.000000e-01 1.280000e-01 3.764306e-02 3.764306e-02 -1.200000e+01 5.000000e-01 5.000000e-01 1.530000e-01 5.968249e-02 5.968249e-02 -1.300000e+01 5.000000e-01 5.000000e-01 5.400000e-02 5.015974e-02 5.015974e-02 -1.400000e+01 5.000000e-01 5.000000e-01 2.200000e-02 2.842534e-02 2.842534e-02 -1.500000e+01 5.000000e-01 5.000000e-01 1.700000e-02 2.140093e-02 2.140093e-02 -1.600000e+01 5.000000e-01 5.000000e-01 1.000000e-02 1.345362e-02 1.345362e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d04-x01-y01 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d04-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -5.250000e+00 0.000000e+00 0.000000e+00 4.803000e+00 5.575841e-02 5.575841e-02 -5.980000e+00 0.000000e+00 0.000000e+00 5.190000e+00 6.887670e-02 6.887670e-02 -6.980000e+00 0.000000e+00 0.000000e+00 5.677000e+00 7.984986e-02 7.984986e-02 -8.430000e+00 0.000000e+00 0.000000e+00 6.291000e+00 9.486833e-02 9.486833e-02 -1.092000e+01 0.000000e+00 0.000000e+00 7.378000e+00 9.885848e-02 9.885848e-02 -1.424000e+01 0.000000e+00 0.000000e+00 8.620000e+00 1.640122e-01 1.640122e-01 -1.772000e+01 0.000000e+00 0.000000e+00 9.520000e+00 4.459821e-01 4.459821e-01 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d04-x01-y02 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d04-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -5.250000e+00 0.000000e+00 0.000000e+00 9.528000e-01 9.202717e-03 9.202717e-03 -5.980000e+00 0.000000e+00 0.000000e+00 9.560000e-01 1.118034e-02 1.118034e-02 -6.980000e+00 0.000000e+00 0.000000e+00 9.630000e-01 1.118034e-02 1.118034e-02 -8.430000e+00 0.000000e+00 0.000000e+00 9.700000e-01 1.118034e-02 1.118034e-02 -1.092000e+01 0.000000e+00 0.000000e+00 9.890000e-01 1.170470e-02 1.170470e-02 -1.424000e+01 0.000000e+00 0.000000e+00 9.880000e-01 1.581139e-02 1.581139e-02 -1.772000e+01 0.000000e+00 0.000000e+00 9.730000e-01 2.983287e-02 2.983287e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d04-x01-y03 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d04-x01-y03 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -5.250000e+00 0.000000e+00 0.000000e+00 8.630000e-01 2.154066e-02 2.154066e-02 -5.980000e+00 0.000000e+00 0.000000e+00 8.700000e-01 2.765863e-02 2.765863e-02 -6.980000e+00 0.000000e+00 0.000000e+00 8.910000e-01 2.668333e-02 2.668333e-02 -8.430000e+00 0.000000e+00 0.000000e+00 9.150000e-01 2.745906e-02 2.745906e-02 -1.092000e+01 0.000000e+00 0.000000e+00 9.640000e-01 2.863564e-02 2.863564e-02 -1.424000e+01 0.000000e+00 0.000000e+00 9.600000e-01 4.401136e-02 4.401136e-02 -1.772000e+01 0.000000e+00 0.000000e+00 9.140000e-01 8.077747e-02 8.077747e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d05-x01-y01 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d05-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -5.000000e-03 5.000000e-03 5.000000e-03 4.900000e+00 4.850773e+00 4.850773e+00 -1.500000e-02 5.000000e-03 5.000000e-03 1.047000e+02 6.519202e+00 6.519202e+00 -2.500000e-02 5.000000e-03 5.000000e-03 1.314000e+02 8.765843e+00 8.765843e+00 -3.500000e-02 5.000000e-03 5.000000e-03 9.340000e+01 8.417244e+00 8.417244e+00 -4.500000e-02 5.000000e-03 5.000000e-03 8.900000e+01 7.615773e+00 7.615773e+00 -5.500000e-02 5.000000e-03 5.000000e-03 6.180000e+01 9.213577e+00 9.213577e+00 -6.500000e-02 5.000000e-03 5.000000e-03 5.540000e+01 8.149233e+00 8.149233e+00 -7.500000e-02 5.000000e-03 5.000000e-03 5.470000e+01 6.449806e+00 6.449806e+00 -8.500000e-02 5.000000e-03 5.000000e-03 4.110000e+01 5.420332e+00 5.420332e+00 -9.500000e-02 5.000000e-03 5.000000e-03 3.390000e+01 4.545327e+00 4.545327e+00 -1.100000e-01 1.000000e-02 1.000000e-02 2.700000e+01 4.071855e+00 4.071855e+00 -1.300000e-01 1.000000e-02 1.000000e-02 1.590000e+01 3.224903e+00 3.224903e+00 -1.500000e-01 1.000000e-02 1.000000e-02 1.470000e+01 3.162278e+00 3.162278e+00 -1.700000e-01 1.000000e-02 1.000000e-02 1.020000e+01 2.236068e+00 2.236068e+00 -1.900000e-01 1.000000e-02 1.000000e-02 7.600000e+00 1.389244e+00 1.389244e+00 -2.250000e-01 2.500000e-02 2.500000e-02 4.750000e+00 9.666437e-01 9.666437e-01 -2.750000e-01 2.500000e-02 2.500000e-02 1.960000e+00 7.130919e-01 7.130919e-01 -3.500000e-01 5.000000e-02 5.000000e-02 6.600000e-01 5.080354e-01 5.080354e-01 -4.500000e-01 5.000000e-02 5.000000e-02 1.900000e-01 1.523155e-01 1.523155e-01 -5.500000e-01 5.000000e-02 5.000000e-02 1.600000e-01 1.188276e-01 1.188276e-01 -7.000000e-01 1.000000e-01 1.000000e-01 1.400000e-02 1.664332e-02 1.664332e-02 -9.000000e-01 1.000000e-01 1.000000e-01 2.000000e-04 2.828427e-04 2.828427e-04 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/OPAL_2004_I631361_qq/d05-x01-y02 -IsRef: 1 -Path: /REF/OPAL_2004_I631361_qq/d05-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -5.000000e-03 5.000000e-03 5.000000e-03 2.710000e+01 9.021086e+00 9.021086e+00 -1.500000e-02 5.000000e-03 5.000000e-03 1.550000e+02 2.140093e+01 2.140093e+01 -2.500000e-02 5.000000e-03 5.000000e-03 1.280000e+02 2.024846e+01 2.024846e+01 -3.500000e-02 5.000000e-03 5.000000e-03 1.100000e+02 1.835756e+01 1.835756e+01 -4.500000e-02 5.000000e-03 5.000000e-03 1.060000e+02 2.624881e+01 2.624881e+01 -5.500000e-02 5.000000e-03 5.000000e-03 8.300000e+01 2.247221e+01 2.247221e+01 -6.500000e-02 5.000000e-03 5.000000e-03 7.600000e+01 1.746425e+01 1.746425e+01 -7.500000e-02 5.000000e-03 5.000000e-03 4.600000e+01 1.615549e+01 1.615549e+01 -8.500000e-02 5.000000e-03 5.000000e-03 5.000000e+01 1.523155e+01 1.523155e+01 -9.500000e-02 5.000000e-03 5.000000e-03 4.800000e+01 1.868154e+01 1.868154e+01 -1.100000e-01 1.000000e-02 1.000000e-02 2.400000e+01 1.529706e+01 1.529706e+01 -1.300000e-01 1.000000e-02 1.000000e-02 1.820000e+01 6.462198e+00 6.462198e+00 -1.500000e-01 1.000000e-02 1.000000e-02 1.110000e+01 3.580503e+00 3.580503e+00 -1.700000e-01 1.000000e-02 1.000000e-02 1.050000e+01 3.858756e+00 3.858756e+00 -1.900000e-01 1.000000e-02 1.000000e-02 5.400000e+00 4.554119e+00 4.554119e+00 -2.250000e-01 2.500000e-02 2.500000e-02 4.200000e+00 3.178050e+00 3.178050e+00 -2.750000e-01 2.500000e-02 2.500000e-02 2.600000e+00 1.431782e+00 1.431782e+00 -3.500000e-01 5.000000e-02 5.000000e-02 7.100000e-01 7.300685e-01 7.300685e-01 -4.500000e-01 5.000000e-02 5.000000e-02 1.400000e-01 1.523155e-01 1.523155e-01 -5.500000e-01 5.000000e-02 5.000000e-02 2.900000e-02 3.178050e-02 3.178050e-02 -7.000000e-01 1.000000e-01 1.000000e-01 1.200000e-02 1.697056e-02 1.697056e-02 -END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMC/MC_D_Dalitz.cc b/analyses/pluginMC/MC_D_Dalitz.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_D_Dalitz.cc @@ -0,0 +1,272 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/FastJets.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MC_D_Dalitz : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MC_D_Dalitz); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(), "UFS"); + + // Book histograms + _h_plus1 = bookHisto1D("h_plus1" ,200,0.,3. ); + _h_minus1 = bookHisto1D("h_minus1" ,200,0.,3.2 ); + _h_pipi1 = bookHisto1D("h_pipi1" ,200,0.,2. ); + _h_minus2 = bookHisto1D("h_minus2" ,200,0.,3.2 ); + _h_neutral2 = bookHisto1D("h_neutral2",200,0.,3.2 ); + _h_pipi2 = bookHisto1D("h_pipi2" ,200,0.,2. ); + _h_Kpilow3 = bookHisto1D("h_Kpilow3" ,200,0.,2. ); + _h_Kpihigh3 = bookHisto1D("h_Kpihigh3" ,200,0.,3.2 ); + _h_Kpiall3 = bookHisto1D("h_Kpiall3" ,200,0.,3. ); + _h_pipi3 = bookHisto1D("h_pipi3" ,200,0.,2. ); + _h_Kpip4 = bookHisto1D("h_Kpip4" ,200,0.,3.2 ); + _h_pipi4 = bookHisto1D("h_pipi4" ,200,0.,2. ); + _h_Kpi04 = bookHisto1D("h_Kpi04" ,200,0.,3.2); + _h_kppim5 = bookHisto1D("h_kppim5" ,200,0.,3. ); + _h_kppip5 = bookHisto1D("h_kppip5" ,200,0.,3.1 ); + _h_pippim5 = bookHisto1D("h_pippim5" ,200,0.,2. ); + _h_kppim6 = bookHisto1D("h_kppim6" ,200,0.,3.5); + _h_kppip6 = bookHisto1D("h_kppip6" ,200,0.,3.5); + _h_pippim6 = bookHisto1D("h_pippim6" ,200,0.,2.5); + _dalitz1 = bookHisto2D("dalitz1" ,50,0.3,3.2,50,0.3,3.2); + _dalitz2 = bookHisto2D("dalitz2" ,50,0.3,3. ,50,0.3,3. ); + _dalitz3 = bookHisto2D("dalitz3" ,50,0.3,2. ,50,0.07,2. ); + _dalitz4 = bookHisto2D("dalitz4" ,50,0.3,3.1 ,50,0.07,2. ); + _dalitz5 = bookHisto2D("dalitz5" ,50,0.,3. ,50,0.,2. ); + _dalitz6 = bookHisto2D("dalitz6" ,50,0.3,3.5,50,0.07,2.5); + } + + void findDecayProducts(const Particle & mother, unsigned int & nstable, + Particles & pip , Particles & pim , Particles & pi0 , + Particles & Kp , Particles & Km , Particles & K0) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::KPLUS ) { + Kp.push_back(p); + ++nstable; + } + else if (id == PID::KMINUS ) { + Km.push_back(p); + ++nstable; + } + else if (id == PID::PIPLUS) { + pip.push_back(p); + ++nstable; + } + else if (id == PID::PIMINUS) { + pim.push_back(p); + ++nstable; + } + else if (id == PID::PI0) { + pi0.push_back(p); + ++nstable; + } + else if (id == PID::K0S||id == PID::K0L) { + K0.push_back(p); + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p, nstable, pip, pim, pi0, Kp , Km, K0); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + double weight = event.weight(); + for(const Particle& meson : apply(event, "UFS"). + particles(Cuts::abspid== 411 ||Cuts::abspid== 421 ||Cuts::abspid== 431 )) { + unsigned int nstable(0); + Particles pip, pim, pi0, Kp , Km, K0; + findDecayProducts(meson, nstable, pip, pim, pi0, Kp , Km, K0); + if(meson.pdgId()<0) { + swap(pim,pip); + swap(Kp,Km); + } + if(abs(meson.pdgId())==421) { + if(pim.size()==1&&pip.size()==1&&K0.size()==1) { + double mminus = (pim[0].momentum()+K0[0].momentum() ).mass2(); + double mplus = (pip[0].momentum()+K0[0].momentum() ).mass2(); + double mpipi = (pip[0].momentum()+pim[0].momentum()).mass2(); + _h_plus1 ->fill(mplus,weight); + _h_minus1 ->fill(mminus,weight); + _h_pipi1 ->fill(mpipi,weight); + _dalitz1 ->fill(mplus,mminus,weight); + } + else if (pip.size()==1&&Km.size()==1&&pi0.size()==1) { + double mneut = (Km[0].momentum()+pip[0].momentum()).mass2(); + double mminus = (Km[0].momentum()+pi0[0].momentum()).mass2(); + double mpipi = (pip[0].momentum()+pi0[0].momentum()).mass2(); + _h_neutral2 ->fill(mneut,weight); + _h_minus2 ->fill(mminus,weight); + _h_pipi2 ->fill(mpipi,weight); + _dalitz2->fill(mminus,mneut,weight); + } + } + else if(abs(meson.pdgId())==411) { + if(pip.size()==2&&Km.size()==1) { + double mplus = (Km[0].momentum() +pip[0].momentum()).mass2(); + double mminus = (Km[0].momentum() +pip[1].momentum()).mass2(); + double mpipi = (pip[0].momentum()+pip[1].momentum()).mass2(); + if(mplusfill( mminus,weight); + _h_Kpihigh3->fill( mplus,weight); + _h_Kpiall3 ->fill( mminus,weight); + _h_Kpiall3 ->fill( mplus,weight); + _h_pipi3 ->fill( mpipi,weight); + _dalitz3->fill(mminus,mpipi, weight); + } + else if (pip.size()==1&&pi0.size()==1&&K0.size()==1) { + double mminus = (K0[0].momentum()+pip[0].momentum()).mass2(); + double mplus = (K0[0].momentum()+pi0[0].momentum()).mass2(); + double mpipi = (pip[0].momentum()+pi0[0].momentum()).mass2(); + _h_Kpip4 ->fill( mminus, weight); + _h_pipi4 ->fill( mpipi , weight); + _h_Kpi04 ->fill( mplus , weight); + _dalitz4->fill(mplus,mpipi, weight); + } + else if (pim.size()==1&&Kp.size()==1&&pip.size()==1) { + double mplus = (Kp [0].momentum()+pip[0].momentum()).mass2(); + double mminus = (Kp [0].momentum()+pim[0].momentum()).mass2(); + double mpipi = (pip[0].momentum()+pim[0].momentum()).mass2(); + _h_kppim5 ->fill(mminus,weight); + _h_kppip5 ->fill(mplus ,weight); + _h_pippim5->fill(mpipi ,weight); + _dalitz5->fill(mminus,mpipi, weight); + } + } + else if(abs(meson.pdgId())==431) { + if (pim.size()==1&&Kp.size()==1&&pip.size()==1) { + double mplus = (Kp [0].momentum()+pip[0].momentum()).mass2(); + double mminus = (Kp [0].momentum()+pim[0].momentum()).mass2(); + double mpipi = (pip[0].momentum()+pim[0].momentum()).mass2(); + _h_kppim6 ->fill(mminus,weight); + _h_kppip6 ->fill(mplus ,weight); + _h_pippim6->fill(mpipi ,weight); + _dalitz6->fill(mminus,mpipi, weight); + } + } + } + } + + /// Normalise histograms etc., after the run + void finalize() { + normalize(_h_plus1); + normalize(_h_minus1); + normalize(_h_pipi1); + normalize(_dalitz1); + normalize(_h_minus2); + normalize(_h_pipi2); + normalize(_h_neutral2); + normalize(_dalitz2); + normalize(_h_Kpilow3); + normalize(_h_Kpihigh3); + normalize(_h_Kpiall3); + normalize(_h_pipi3); + normalize(_dalitz3); + normalize(_h_Kpip4); + normalize(_h_pipi4); + normalize(_h_Kpi04); + normalize(_dalitz4); + normalize(_h_kppim5); + normalize(_h_kppip5); + normalize(_h_pippim5); + normalize(_dalitz5); + normalize(_h_kppim6); + normalize(_h_kppip6); + normalize(_h_pippim6); + normalize(_dalitz6); + } + //@} + + /// @name Histograms + //@{ + // Histograms for D^0\to \bar{K}^0\pi^+\pi^- + //m^2_+ + Histo1DPtr _h_plus1; + //m^2_+ + Histo1DPtr _h_minus1; + //m^2_{\pi\pi} + Histo1DPtr _h_pipi1; + // Dalitz plot + Histo2DPtr _dalitz1; + + // Histograms for D^0\to K^-\pi^+\pi^0 + // Histogram for the K^-\pi^+ mass + Histo1DPtr _h_minus2; + // Histogram for the \pi^+\pi^0 mass + Histo1DPtr _h_pipi2; + // Histogram for the K^-\pi^0 mass + Histo1DPtr _h_neutral2; + // Dalitz plot + Histo2DPtr _dalitz2; + + // Histograms for D^+\to K^-\pi^+\pi^+ + // Histogram for K^-\pi^+ low + Histo1DPtr _h_Kpilow3; + // Histogram for K^-\pi^+ high + Histo1DPtr _h_Kpihigh3; + // Histogram for K^-\pi^+ all + Histo1DPtr _h_Kpiall3; + // Histogram for \pi^+\pi^- + Histo1DPtr _h_pipi3; + // Dalitz plot + Histo2DPtr _dalitz3; + + // Histograms for D^+\to\bar{K}^0\pi^+\pi^0 + // Histogram for the \bar{K}^0\pi^+ mass + Histo1DPtr _h_Kpip4; + // Histogram for the \pi^+\pi^0 mass + Histo1DPtr _h_pipi4; + // Histogram for the \bar{K}^0\pi^0 mass + Histo1DPtr _h_Kpi04; + // Dalitz plot + Histo2DPtr _dalitz4; + + // Histograms for D^+\to K^+\pi^-\pi^+ + // Histogram for K^+\pi^- + Histo1DPtr _h_kppim5; + // Histogram for K^+\pi^+ + Histo1DPtr _h_kppip5; + // Histogram for \pi^+\pi^- + Histo1DPtr _h_pippim5; + // Dalitz plot + Histo2DPtr _dalitz5; + + // Histograms for D_s^+\to K^+\pi^-\pi^+ + // Histogram for K^+\pi^- + Histo1DPtr _h_kppim6; + // Histogram for K^+\pi^+ + Histo1DPtr _h_kppip6; + // Histogram for \pi^+\pi^- + Histo1DPtr _h_pippim6; + // Dalitz plot + Histo2DPtr _dalitz6; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MC_D_Dalitz); + + +} diff --git a/analyses/pluginMC/MC_D_Dalitz.info b/analyses/pluginMC/MC_D_Dalitz.info new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_D_Dalitz.info @@ -0,0 +1,8 @@ +Name: MC_D_Dalitz +Summary: MC analysis of Dalitz plots in three-body $D$-meson decays +Status: VALIDATED +Authors: + - Peter Richardson +RunInfo: Any process producing D mesons +Description: + 'Monte Carlo analysis of $D^0\to \bar{K}^0\pi^+\pi^-$, $D^0\to K^-\pi^+\pi^0$, $D^+\to K^-\pi^+\pi^+$, $D^+\to\bar{K}^0\pi^+\pi^0$, $D^+\to K^+\pi^-\pi^+$ and $D_s^+\to K^+\pi^-\pi^+$ including kinematic distributions and Dalitz plots.' diff --git a/analyses/pluginMC/MC_D_Dalitz.plot b/analyses/pluginMC/MC_D_Dalitz.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_D_Dalitz.plot @@ -0,0 +1,136 @@ +BEGIN PLOT /MC_D_Dalitz/h_plus1 +Title=$\bar{K}^0\pi^+$ mass distribution in $D^0\to \bar{K}^0\pi^+\pi^-$ +XLabel=$m^2_{\bar{K}^0\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m^2_{\bar{K}^0\pi^+}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_minus1 +Title=$\bar{K}^0\pi^-$ mass distribution in $D^0\to \bar{K}^0\pi^+\pi^-$ +XLabel=$m^2_{\bar{K}^0\pi^-}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m^2_{\bar{K}^0\pi^-}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_pipi1 +Title=$\pi^+\pi^-$ mass distribution in $D^0\to \bar{K}^0\pi^+\pi^-$ +XLabel=$m^2_{\pi^+\pi^-}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m^2_{\pi^+\pi^-}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/dalitz1 +Title=Dalitz plot for $D^0\to \bar{K}^0\pi^+\pi^-$ +XLabel=$m^2_{\bar{K}^0\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$m^2_{\bar{K}^0\pi^-}$ [$\rm{GeV}^{-2}$] +ZLabel=$1/\Gamma{\rm d}^2 \Gamma/{\rm d}m^2_{\bar{K}^0\pi^+}/{\rm d}m^2_{\bar{K}^0\pi^-}$ [$\rm{GeV}^{-4}$] +END PLOT + +BEGIN PLOT /MC_D_Dalitz/h_minus2 +Title=$K^-\pi^0$ mass distribution in $D^0\to K^-\pi^+\pi^0$ +XLabel=$m^2_{K^-\pi^0}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m^2_{K^-\pi^0}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_neutral2 +Title=$K^-\pi^+$ mass distribution in $D^0\to K^-\pi^+\pi^0$ +XLabel=$m^2_{K^-\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m^2_{K^-\pi^+}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_pipi2 +Title=$\pi^+\pi^0$ mass distribution in $D^0\to K^-\pi^+\pi^0$ +XLabel=$m^2_{\pi^+\pi^0}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m^2_{\pi^+\pi^0}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/dalitz2 +Title=Dalitz plot for $D^0\to K^-\pi^+\pi^0$ +XLabel=$m^2_{K^-\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$m^2_{K^-\pi^0}$ [$\rm{GeV}^{-2}$] +ZLabel=$1/\Gamma{\rm d}^2 \Gamma/{\rm d}m^2_{K^-\pi^+}/{\rm d}m^2_{K^-\pi^0}$ [$\rm{GeV}^{-4}$] +END PLOT + +BEGIN PLOT /MC_D_Dalitz/h_Kpilow3 +Title=Lower $K^-\pi^+$ mass distribution in $D^+\to K^-\pi^+\pi^+$ +XLabel=${m^{\rm low}_{K^-\pi^+}}^2$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}{m^{\rm low}_{K^-\pi^+}}^2$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_Kpihigh3 +Title=Higher $K^-\pi^+$ mass distribution in $D^+\to K^-\pi^+\pi^+$ +XLabel=${m^{\rm high}_{K^-\pi^+}}^2$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}{m^{\rm high}_{K^-\pi^+}}^$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_Kpiall3 +Title=All $K^-\pi^+$ mass distribution in $D^+\to K^-\pi^+\pi^+$ +XLabel=${m^{\rm all}_{K^-\pi^+}}^2$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}{m^{\rm all}_{K^-\pi^+}}^2$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_pipi3 +Title=$\pi^+\pi^+$ mass distribution in $D^+\to K^-\pi^+\pi^+$ +XLabel=$m^2_{\pi^+\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m^2_{\pi^+\pi^+}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/dalitz3 +Title=Dalitz plot for $D^+\to K^-\pi^+\pi^+$ +XLabel=${m^{\rm low}_{K^-\pi^+}}^2$ [$\rm{GeV}^{-2}$] +YLabel=$m^2_{\pi^+\pi^+}$ [$\rm{GeV}^{-2}$] +ZLabel=$1/\Gamma{\rm d}^2 \Gamma/{\rm d}{m^{\rm low}_{K^-\pi^+}}^2/{\rm d}m^2_{\pi^+\pi^+}$ [$\rm{GeV}^{-4}$] +END PLOT + +BEGIN PLOT /MC_D_Dalitz/h_Kpip4 +Title=$\bar{K}^0\pi^+$ mass distribution in $D^+\to \bar{K}^0\pi^+\pi^0$ +XLabel=$m^2_{\bar{K}^0\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}^{\rm low}_{\bar{K}^0\pi^+}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_pipi4 +Title=$\pi^0\pi^+$ mass distribution in $D^+\to \bar{K}^0\pi^+\pi^0$ +XLabel=$m^2_{\pi^0\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}^{\rm low}_{\pi^0\pi^+}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_Kpi04 +Title=$\bar{K}^0\pi^0$ mass distribution in $D^+\to \bar{K}^0\pi^+\pi^0$ +XLabel=$m^2_{\bar{K}^0\pi^0}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}^{\rm low}_{\bar{K}^0\pi^0}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/dalitz4 +Title=Dalitz plot for $D^+\to \bar{K}^0\pi^+\pi^0$ +XLabel=$m^2_{\bar{K}^0\pi^0}$ [$\rm{GeV}^{-2}$] +YLabel=$m^2_{\pi^+\pi^0}$ [$\rm{GeV}^{-2}$] +ZLabel=$1/\Gamma{\rm d}^2 \Gamma/{\rm d}m^2_{\bar{K}^0\pi^0}/{\rm d}m^2_{\pi^+\pi^0}$ [$\rm{GeV}^{-4}$] +END PLOT + +BEGIN PLOT /MC_D_Dalitz/h_kppim5 +Title=$K^+\pi^-$ mass distribution in $D^+\to K^+\pi^-\pi^+$ +XLabel=$m^2_{K^+\pi^-}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}^{\rm low}_{K^+\pi^-}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_kppip5 +Title=$K^+\pi^+$ mass distribution in $D^+\to K^+\pi^-\pi^+$ +XLabel=$m^2_{K^+\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}^{\rm low}_{K^+\pi^+}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_pippim5 +Title=$\pi^-\pi^+$ mass distribution in $D^+\to K^+\pi^-\pi^+$ +XLabel=$m^2_{\pi^-\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}^{\rm low}_{\pi^-\pi^+}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/dalitz5 +Title=Dalitz plot for $D^+\to K^+\pi^-\pi^+$ +XLabel=$m^2_{K^+\pi^-}$ [$\rm{GeV}^{-2}$] +YLabel=$m^2_{\pi^+\pi^-}$ [$\rm{GeV}^{-2}$] +ZLabel=$1/\Gamma{\rm d}^2 \Gamma/{\rm d}m^2_{K^+\pi^-}/{\rm d}m^2_{\pi^+\pi^-}$ [$\rm{GeV}^{-4}$] +END PLOT + +BEGIN PLOT /MC_D_Dalitz/h_kppim6 +Title=$K^+\pi^-$ mass distribution in $D_s^+\to K^+\pi^-\pi^+$ +XLabel=$m^2_{K^+\pi^-}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}^{\rm low}_{K^+\pi^-}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_kppip6 +Title=$K^+\pi^+$ mass distribution in $D_s^+\to K^+\pi^-\pi^+$ +XLabel=$m^2_{K^+\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}^{\rm low}_{K^+\pi^+}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/h_pippim6 +Title=$\pi^-\pi^+$ mass distribution in $D_s^+\to K^+\pi^-\pi^+$ +XLabel=$m^2_{\pi^-\pi^+}$ [$\rm{GeV}^{-2}$] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}^{\rm low}_{\pi^-\pi^+}$ [$\rm{GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_D_Dalitz/dalitz6 +Title=Dalitz plot for $D_s^+\to K^+\pi^-\pi^+$ +XLabel=$m^2_{K^+\pi^-}$ [$\rm{GeV}^{-2}$] +YLabel=$m^2_{\pi^+\pi^-}$ [$\rm{GeV}^{-2}$] +ZLabel=$1/\Gamma{\rm d}^2 \Gamma/{\rm d}m^2_{K^+\pi^-}/{\rm d}m^2_{\pi^+\pi^-}$ [$\rm{GeV}^{-4}$] +END PLOT diff --git a/analyses/pluginMC/MC_Eta_Decay.cc b/analyses/pluginMC/MC_Eta_Decay.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Eta_Decay.cc @@ -0,0 +1,247 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MC_Eta_Decay : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MC_Eta_Decay); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(), "UFS"); + + // Book histograms + double meta[2]={547.45, 957.78}; + for(unsigned int ix=0;ix<2;++ix) { + ostringstream title; title << "_" << ix; + _mgammagamma .push_back(bookHisto1D("mgammagamma" +title.str(),200,0.,meta[ix]) ); + _mpi0gamma .push_back(bookHisto1D("mpi0gamma" +title.str(),200,0.,meta[ix])) ; + _mpipgamma .push_back(bookHisto1D("mpipgamma" +title.str(),200,0.,meta[ix])); + _mpimgamma .push_back(bookHisto1D("mpimgamma" +title.str(),200,0.,meta[ix])); + _photonenergy.push_back(bookHisto1D("photonenergy"+title.str(),200,0.,meta[ix])); + _mpippim .push_back(bookHisto1D("mpippim" +title.str(),200,0.,meta[ix])); + _dpippim .push_back(bookHisto1D("dpippim" +title.str(),200,200.,meta[ix])); + _dpi0pi0 .push_back(bookHisto1D("dpi0pi0" +title.str(),200,200.,meta[ix])); + _dpi0pip .push_back(bookHisto1D("dpi0pip" +title.str(),200,200.,meta[ix])); + _dpi0pim .push_back(bookHisto1D("dpi0pim" +title.str(),200,200.,meta[ix])); + } + _dpi0pi0.push_back(bookHisto1D("dpi0pi0_2",200,200.,500. )); + _dpippim.push_back(bookHisto1D("dpippim_2",200,200.,500. )); + _dpipeta=bookHisto1D("dpipeta",200,500.,meta[1]) ; + _dpimeta=bookHisto1D("dpimeta",200,500.,meta[1]) ; + _dpi0eta=bookHisto1D("dpi0eta",200,500.,meta[1]) ; + } + + void findDecayProducts(const Particle & mother, + unsigned int & nstable, + Particles& pip, Particles& pim, + Particles& pi0, Particles& eta, + Particles& gamma) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::ETA ) { + eta.push_back(p); + ++nstable; + } + else if ( id == PID::PHOTON ) { + gamma.push_back(p); + ++nstable; + } + else if (id == PID::PIPLUS) { + pip.push_back(p); + ++nstable; + } + else if (id == PID::PIMINUS) { + pim.push_back(p); + ++nstable; + } + else if (id == PID::PI0 ) { + pi0.push_back(p); + ++nstable; + } + else if (id == PID::K0S || id == PID::K0L || + id == PID::KPLUS || id == PID::KMINUS) + ++nstable; + else if ( !p.children().empty() ) { + findDecayProducts(p,nstable,pip,pim,pi0,eta,gamma); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + double weight = event.weight(); + // Loop over f_1 mesons + for(const Particle& meson : apply(event, "UFS"). + particles(Cuts::pid==221||Cuts::pid==331)) { + unsigned int nstable(0); + Particles pip, pim, pi0, eta, gamma; + findDecayProducts(meson,nstable,pip, pim, pi0, eta, gamma); + unsigned int imeson = meson.pdgId()==221 ? 0 : 1; + // pi0 gamma gamma + if(nstable==3 && pi0.size()==1 && gamma.size()==2) { + _mgammagamma[imeson]->fill((gamma[0].momentum()+gamma[1].momentum()).mass()/MeV,weight); + _mpi0gamma [imeson]->fill(( pi0[0].momentum()+gamma[0].momentum()).mass()/MeV,weight); + _mpi0gamma [imeson]->fill(( pi0[0].momentum()+gamma[1].momentum()).mass()/MeV,weight); + } // pi+pi-gamma analysis + else if(nstable==3 && pip.size()==1 && pim.size()==1 && gamma.size()==1) { + FourMomentum ptemp = pip[0].momentum()+pim[0].momentum(); + double mpipi = ptemp.mass(); + _mpippim[imeson]->fill(mpipi/MeV,weight); + double egamma = 0.5*(meson.mass()*meson.mass()-mpipi*mpipi)/meson.mass(); + _photonenergy[imeson]->fill(egamma/MeV,weight); + _mpipgamma[imeson]->fill((pip[0].momentum()+gamma[0].momentum()).mass()/MeV,weight); + _mpimgamma[imeson]->fill((pim[0].momentum()+gamma[0].momentum()).mass()/MeV,weight); + } + else if(nstable==3&& pi0.size()==3) { + _dpi0pi0[imeson]->fill((pi0[0].momentum()+pi0[1].momentum()).mass()/MeV,weight); + _dpi0pi0[imeson]->fill((pi0[0].momentum()+pi0[2].momentum()).mass()/MeV,weight); + _dpi0pi0[imeson]->fill((pi0[1].momentum()+pi0[2].momentum()).mass()/MeV,weight); + } + else if(nstable==3&& pip.size()==1&&pim.size()==1&&pi0.size()==1) { + _dpi0pip[imeson]->fill((pi0[0].momentum()+pip[0].momentum()).mass()/MeV,weight); + _dpi0pim[imeson]->fill((pi0[0].momentum()+pim[0].momentum()).mass()/MeV,weight); + _dpippim[imeson]->fill((pip[0].momentum()+pim[0].momentum()).mass()/MeV,weight); + } + else if(nstable==3&& pi0.size()==2&&eta.size()==1) { + _dpi0pi0[2]->fill((pi0[0].momentum()+pi0[1].momentum()).mass()/MeV,weight); + _dpi0eta ->fill((pi0[0].momentum()+eta[0].momentum()).mass()/MeV,weight); + _dpi0eta ->fill((pi0[1].momentum()+eta[0].momentum()).mass()/MeV,weight); + } + else if(nstable==3&& pip.size()==1&&pim.size()==1&&eta.size()==1) { + _dpippim[2]->fill((pip[0].momentum()+pim[0].momentum()).mass()/MeV,weight); + _dpipeta ->fill((pip[0].momentum()+eta[0].momentum()).mass()/MeV,weight); + _dpimeta ->fill((pim[0].momentum()+eta[0].momentum()).mass()/MeV,weight); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + // normalize to unity + for(unsigned int ix=0;ix<2;++ix) { + normalize(_mgammagamma[ix]); + normalize(_mpi0gamma[ix]); + normalize(_mpipgamma[ix]); + normalize(_mpimgamma[ix]); + normalize(_mpippim[ix]); + normalize(_photonenergy[ix]); + normalize(_dpippim[ix]); + normalize(_dpi0pi0[ix]); + normalize(_dpi0pip[ix]); + normalize(_dpi0pim[ix]); + } + normalize(_dpi0pi0[2]); + normalize(_dpippim[2]); + normalize(_dpipeta); + normalize(_dpimeta); + normalize(_dpi0eta); + } + //@} + + + /** + * Histograms for the decay \f$\eta\to\pi^0\gamma\gamma\f$ + */ + //@{ + /** + * Histogram for the mass of \f$\gamma\gamma\f$ + */ + vector _mgammagamma; + + /** + * Histogrma for the mass of \f$\pi^0\gamma\f$ + */ + vector _mpi0gamma; + //@} + + /** + * Histograms for the decay \f$\eta\to\pi^+\pi^-\gamma\f$ + */ + //@{ + /** + * Histogram for the mass of \f$\pi^+\gamma\f$ + */ + vector _mpipgamma; + + /** + * Histogram for the mass of \f$\pi^-\gamma\f$ + */ + vector _mpimgamma; + + /** + * Histogram for the mass of \f$\pi^+\pi^-\f$ + */ + vector _mpippim; + + /** + * Histogram for the photon energy + */ + vector _photonenergy; + //@} + + /** + * Histograms for the decay \f$\eta\pi\pi\pi\f$ and \f$\eta'\to\eta\pi\pi\f$. + */ + //@{ + /** + * Histogram for the mass of \f$\pi^+\pi^-\f$ + */ + vector _dpippim; + + /** + * Histogram for the mass of \f$\pi^0\pi^0\f$ + */ + vector _dpi0pi0; + + /** + * Histogram for the mass of \f$\pi^0\pi^+\f$ + */ + vector _dpi0pip; + + /** + * Histogram for the mass of \f$\pi^0\pi^-\f$ + */ + vector _dpi0pim; + + /** + * Histogram for the mass of \f$\pi^+\eta\f$ + */ + Histo1DPtr _dpipeta; + + /** + * Histogram for the mass of \f$\pi^-\eta\f$ + */ + Histo1DPtr _dpimeta; + + /** + * Histogram for the mass of \f$\pi^0\eta\f$ + */ + Histo1DPtr _dpi0eta; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MC_Eta_Decay); + + +} diff --git a/analyses/pluginMC/MC_Eta_Decay.info b/analyses/pluginMC/MC_Eta_Decay.info new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Eta_Decay.info @@ -0,0 +1,9 @@ +Name: MC_Eta_Decay +Summary: Analysis of Kinematic distributions in $\eta$ and $\eta^\prime$ meson decays +Status: VALIDATED +Authors: + - Peter Richardson +RunInfo: Any type of process producing eta/eta prime mesons +NeedCrossSection: no +Description: + ' Analysis of Kinematic distributions in $\eta$ and $\eta^\prime$ meson decays. The mass distributions in the decays $\eta,\eta^\prime\to \gamma\pi^+\pi^-$, $\gamma\gamma\pi^0$, $\pi^0\pi^0\pi^0$, $\pi^+\pi^-\pi^0$ and $\eta^\prime\to\pi^+\pi^-\eta$, $\pi^0\pi^0\eta$ are produced. Based on an +old Herwig++ internal analysis.' diff --git a/analyses/pluginMC/MC_Eta_Decay.plot b/analyses/pluginMC/MC_Eta_Decay.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Eta_Decay.plot @@ -0,0 +1,134 @@ +BEGIN PLOT /MC_Eta_Decay/dpi0eta +Title=Distribution of the $\eta\pi^0$ mass in the decay $\eta^\prime\to\eta\pi^0\pi^0$ +XLabel=$m_{\eta\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\eta\pi^0}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/dpi0pi0_2 +Title=Distribution of the $\pi^0\pi^0$ mass in the decay $\eta^\prime\to\eta\pi^0\pi^0$ +XLabel=$m_{\pi^0\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^0\pi^0}$ [${\rm MeV}^{-1}$] +END PLOT + +BEGIN PLOT /MC_Eta_Decay/dpipeta +Title=Distribution of the $\eta\pi^+$ mass in the decay $\eta^\prime\to\eta\pi^+\pi^-$ +XLabel=$m_{\eta\pi^+}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\eta\pi^+}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/dpimeta +Title=Distribution of the $\eta\pi^-$ mass in the decay $\eta^\prime\to\eta\pi^+\pi^-$ +XLabel=$m_{\eta\pi^-}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\eta\pi^-}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/dpippim_2 +Title=Distribution of the $\pi^+\pi^-$ mass in the decay $\eta^\prime\to\eta\pi^+\pi^-$ +XLabel=$m_{\pi^+\pi^-}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^+\pi^-}$ [${\rm MeV}^{-1}$] +END PLOT + +BEGIN PLOT /MC_Eta_Decay/mpipgamma_0 +Title=Distribution of the $\gamma\pi^+$ mass in the decay $\eta\to\gamma\pi^+\pi^-$ +XLabel=$m_{\gamma\pi^+}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\gamma\pi^+}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/mpimgamma_0 +Title=Distribution of the $\gamma\pi^-$ mass in the decay $\eta\to\gamma\pi^+\pi^-$ +XLabel=$m_{\gamma\pi^-}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\gamma\pi^-}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/mpippim_0 +Title=Distribution of the $\pi^+\pi^-$ mass in the decay $\eta\to\gamma\pi^+\pi^-$ +XLabel=$m_{\pi^+\pi^-}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^+\pi^-}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/photonenergy_0 +Title=Distribution of the photon energy in the decay $\eta\to\gamma\pi^+\pi^-$ +XLabel=$E_\gamma$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} E_\gamma$ [${\rm MeV}^{-1}$] +END PLOT + +BEGIN PLOT /MC_Eta_Decay/mpipgamma_1 +Title=Distribution of the $\gamma\pi^+$ mass in the decay $\eta^\prime\to\gamma\pi^+\pi^-$ +XLabel=$m_{\gamma\pi^+}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\gamma\pi^+}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/mpimgamma_1 +Title=Distribution of the $\gamma\pi^-$ mass in the decay $\eta^\prime\to\gamma\pi^+\pi^-$ +XLabel=$m_{\gamma\pi^-}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\gamma\pi^-}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/mpippim_1 +Title=Distribution of the $\pi^+\pi^-$ mass in the decay $\eta^\prime\to\gamma\pi^+\pi^-$ +XLabel=$m_{\pi^+\pi^-}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^+\pi^-}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/photonenergy_1 +Title=Distribution of the photon energy in the decay $\eta^\prime\to\gamma\pi^+\pi^-$ +XLabel=$E_\gamma$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} E_\gamma$ [${\rm MeV}^{-1}$] +END PLOT + + +BEGIN PLOT /MC_Eta_Decay/mgammagamma_1 +Title=Distribution of the $\gamma\gamma$ mass in the decay $\eta^\prime\to\gamma\gamma\pi^0$ +XLabel=$m_{\gamma\gamma}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\gamma\gamma}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/mpi0gamma_1 +Title=Distribution of the $\gamma\pi^0$ mass in the decay $\eta^\prime\to\gamma\gamma\pi^0$ +XLabel=$m_{\gamma\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\gamma\pi^0}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/mgammagamma_0 +Title=Distribution of the $\gamma\gamma$ mass in the decay $\eta\to\gamma\gamma\pi^0$ +XLabel=$m_{\gamma\gamma}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\gamma\gamma}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/mpi0gamma_0 +Title=Distribution of the $\gamma\pi^0$ mass in the decay $\eta\to\gamma\gamma\pi^0$ +XLabel=$m_{\gamma\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\gamma\pi^0}$ [${\rm MeV}^{-1}$] +END PLOT + +BEGIN PLOT /MC_Eta_Decay/dpi0pi0_0 +Title=Distribution of the $\pi\pi^0$ mass in the decay $\eta\to\pi^0\pi^0\pi^0$ +XLabel=$m_{\pi^0\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^0\pi^0}$ [${\rm MeV}^{-1}$] +END PLOT + +BEGIN PLOT /MC_Eta_Decay/dpi0pi0_1 +Title=Distribution of the $\pi\pi^0$ mass in the decay $\eta^\prime\to\pi^0\pi^0\pi^0$ +XLabel=$m_{\pi^0\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^0\pi^0}$ [${\rm MeV}^{-1}$] +END PLOT + +BEGIN PLOT /MC_Eta_Decay/dpi0pip_0 +Title=Distribution of the $\pi^+\pi^0$ mass in the decay $\eta\to\pi^+\pi^-\pi^0$ +XLabel=$m_{\pi^+\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^+\pi^0}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/dpi0pim_0 +Title=Distribution of the $\pi^-\pi^0$ mass in the decay $\eta\to\pi^+\pi^-\pi^0$ +XLabel=$m_{\pi^-\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^-\pi^0}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/dpippim_0 +Title=Distribution of the $\pi^+\pi^-$ mass in the decay $\eta\to\pi^+\pi^-\pi^0$ +XLabel=$m_{\pi^+\pi^-}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^+\pi^-}$ [${\rm MeV}^{-1}$] +END PLOT + +BEGIN PLOT /MC_Eta_Decay/dpi0pip_1 +Title=Distribution of the $\pi^+\pi^0$ mass in the decay $\eta^\prime\to\pi^+\pi^-\pi^0$ +XLabel=$m_{\pi^+\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^+\pi^0}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/dpi0pim_1 +Title=Distribution of the $\pi^-\pi^0$ mass in the decay $\eta^\prime\to\pi^+\pi^-\pi^0$ +XLabel=$m_{\pi^-\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^-\pi^0}$ [${\rm MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Eta_Decay/dpippim_1 +Title=Distribution of the $\pi^+\pi^-$ mass in the decay $\eta^\prime\to\pi^+\pi^-\pi^0$ +XLabel=$m_{\pi^+\pi^-}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\pi^+\pi^-}$ [${\rm MeV}^{-1}$] +END PLOT \ No newline at end of file diff --git a/analyses/pluginMC/MC_F1_Decay.cc b/analyses/pluginMC/MC_F1_Decay.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_F1_Decay.cc @@ -0,0 +1,185 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MC_F1_Decay : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MC_F1_Decay); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(),"UFS"); + + // eta pi0 pi0 mode + _h_eta0_etapi0 = bookHisto1D("eta0_etapi0" , 70, 0.66, 1.36); + _h_eta0_pi0pi0 = bookHisto1D("eta0_pi0pi0" , 80, 0.2, 1.0); + _h_eta0_etapi0pi0 = bookHisto1D("eta0_etapi0pi0", 70, 1.0, 1.7); + // eta pi+pi- mode + _h_eta1_etapip = bookHisto1D("eta1_etapip" , 70, 0.66, 1.36); + _h_eta1_etapim = bookHisto1D("eta1_etapim" , 70, 0.66, 1.36); + _h_eta1_pippim = bookHisto1D("eta1_pippim" , 80, 0.2, 1.0); + _h_eta1_etapippim = bookHisto1D("eta1_etapippim", 70, 1.0, 1.7); + // pi+pi-2pi0 + _h_4pi0_pi0pi0 = bookHisto1D("4pi0_pi0pi0" , 80, 0.2, 1.0); + _h_4pi0_pippi0 = bookHisto1D("4pi0_pippi0" , 80, 0.2, 1.0); + _h_4pi0_pimpi0 = bookHisto1D("4pi0_pimpi0" , 80, 0.2, 1.0); + _h_4pi0_pippim = bookHisto1D("4pi0_pippim" , 80, 0.2, 1.0); + _h_4pi0_pippimpi0 = bookHisto1D("4pi0_pippimpi0",100, 0.4, 1.4); + _h_4pi0_pippi0pi0 = bookHisto1D("4pi0_pippi0pi0",100, 0.4, 1.4); + _h_4pi0_pimpi0pi0 = bookHisto1D("4pi0_pimpi0pi0",100, 0.4, 1.4); + _h_4pi0_4pi = bookHisto1D("4pi0_4pi" , 70, 1.0, 1.7); + // 2pi+ 2pi- mode + _h_4pi1_pippip = bookHisto1D("4pi1_pippip" , 80, 0.2, 1.0); + _h_4pi1_pimpim = bookHisto1D("4pi1_pimpim" , 80, 0.2, 1.0); + _h_4pi1_pippim = bookHisto1D("4pi1_pippim" , 80, 0.2, 1.0); + _h_4pi1_pimpimpip = bookHisto1D("4pi1_pimpimpip",100, 0.4, 1.4); + _h_4pi1_pippippim = bookHisto1D("4pi1_pippippim",100, 0.4, 1.4); + _h_4pi1_4pi = bookHisto1D("4pi1_4pi" , 70, 1.0, 1.7); + } + + void findDecayProducts(const Particle & mother, + unsigned int & nstable, + Particles& pip, Particles& pim, + Particles& pi0, Particles& eta) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::ETA ) { + eta.push_back(p); + ++nstable; + } + else if (id == PID::PIPLUS) { + pip.push_back(p); + ++nstable; + } + else if (id == PID::PIMINUS) { + pim.push_back(p); + ++nstable; + } + else if (id == PID::PI0 ) { + pi0.push_back(p); + ++nstable; + } + else if (id == PID::K0S || id == PID::K0L || + id == PID::KPLUS || id == PID::KMINUS) + ++nstable; + else if ( !p.children().empty() ) { + findDecayProducts(p,nstable,pip,pim,pi0,eta); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + // Loop over f_1 mesons + for(const Particle& f1 : apply(event, "UFS").particles(Cuts::abspid==20223)) { + unsigned int nstable(0); + Particles pip, pim, pi0, eta; + findDecayProducts(f1,nstable,pip, pim, pi0, eta); + // pi+ pi- pi0 pi0 + if(nstable==4 && pip.size()==1 && pim.size()==1 && pi0.size()==2) { + _h_4pi0_pi0pi0->fill((pi0[0].momentum()+pi0[1].momentum()).mass(),1.); + _h_4pi0_pippi0->fill((pip[0].momentum()+pi0[0].momentum()).mass(),1.); + _h_4pi0_pippi0->fill((pip[0].momentum()+pi0[1].momentum()).mass(),1.); + _h_4pi0_pimpi0->fill((pim[0].momentum()+pi0[0].momentum()).mass(),1.); + _h_4pi0_pimpi0->fill((pim[0].momentum()+pi0[1].momentum()).mass(),1.); + _h_4pi0_pippim->fill((pip[0].momentum()+pim[0].momentum()).mass(),1.); + _h_4pi0_pippimpi0->fill((pip[0].momentum()+pim[0].momentum()+pi0[0].momentum()).mass(),1.); + _h_4pi0_pippimpi0->fill((pip[0].momentum()+pim[0].momentum()+pi0[1].momentum()).mass(),1.); + _h_4pi0_pippi0pi0->fill((pi0[0].momentum()+pi0[1].momentum()+pip[0].momentum()).mass(),1.); + _h_4pi0_pimpi0pi0->fill((pi0[0].momentum()+pi0[1].momentum()+pim[0].momentum()).mass(),1.); + _h_4pi0_4pi->fill((pi0[0].momentum()+pi0[1].momentum()+pim[0].momentum()+pip[0].momentum()).mass(),1.); + } + else if(nstable==4 && pip.size()==2 && pim.size()==2) { + _h_4pi1_pippip ->fill((pip[0].momentum()+pip[1].momentum()).mass(),1.); + _h_4pi1_pimpim ->fill((pim[0].momentum()+pim[1].momentum()).mass(),1.); + _h_4pi1_pippim ->fill((pip[0].momentum()+pim[0].momentum()).mass(),1.); + _h_4pi1_pippim ->fill((pip[0].momentum()+pim[1].momentum()).mass(),1.); + _h_4pi1_pippim ->fill((pip[1].momentum()+pim[0].momentum()).mass(),1.); + _h_4pi1_pippim ->fill((pip[1].momentum()+pim[1].momentum()).mass(),1.); + _h_4pi1_pimpimpip->fill((pim[0].momentum()+pim[1].momentum()+pip[0].momentum()).mass(),1.); + _h_4pi1_pimpimpip->fill((pim[0].momentum()+pim[1].momentum()+pip[1].momentum()).mass(),1.); + _h_4pi1_pippippim->fill((pip[0].momentum()+pip[1].momentum()+pim[0].momentum()).mass(),1.); + _h_4pi1_pippippim->fill((pip[0].momentum()+pip[1].momentum()+pim[1].momentum()).mass(),1.); + _h_4pi1_4pi ->fill((pip[0].momentum()+pip[1].momentum()+ + pim[0].momentum()+pim[1].momentum()).mass(),1.); + } + else if(nstable==3 && eta.size()==1 && pip.size()==1 && pim.size()==1) { + _h_eta1_etapip ->fill((eta[0].momentum()+pip[0].momentum()).mass(),1.); + _h_eta1_etapim ->fill((eta[0].momentum()+pim[0].momentum()).mass(),1.); + _h_eta1_pippim ->fill((pim[0].momentum()+pip[0].momentum()).mass(),1.); + _h_eta1_etapippim->fill((eta[0].momentum()+pim[0].momentum()+pip[0].momentum()).mass(),1.); + } + else if(nstable==3 && eta.size()==1 && pi0.size()==2 ) { + _h_eta0_etapi0 ->fill((eta[0].momentum()+pi0[0].momentum()).mass(),1.); + _h_eta0_etapi0 ->fill((eta[0].momentum()+pi0[1].momentum()).mass(),1.); + _h_eta0_pi0pi0 ->fill((pi0[0].momentum()+pi0[1].momentum()).mass(),1.); + _h_eta0_etapi0pi0->fill((eta[0].momentum()+pi0[0].momentum()+pi0[1].momentum()).mass(),1.); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + normalize(_h_eta0_etapi0 ); + normalize(_h_eta0_pi0pi0 ); + normalize(_h_eta0_etapi0pi0); + + normalize(_h_eta1_etapip); + normalize(_h_eta1_etapim); + normalize(_h_eta1_pippim); + normalize(_h_eta1_etapippim); + + normalize(_h_4pi0_pi0pi0); + normalize(_h_4pi0_pippi0); + normalize(_h_4pi0_pimpi0); + normalize(_h_4pi0_pippim); + normalize(_h_4pi0_pippimpi0); + normalize(_h_4pi0_pippi0pi0); + normalize(_h_4pi0_pimpi0pi0); + normalize(_h_4pi0_4pi); + + normalize(_h_4pi1_pippip); + normalize(_h_4pi1_pimpim); + normalize(_h_4pi1_pippim); + normalize(_h_4pi1_pimpimpip); + normalize(_h_4pi1_pippippim); + normalize(_h_4pi1_4pi); + } + + //@} + + + // @name Histograms + //@{ + Histo1DPtr _h_eta0_etapi0,_h_eta0_pi0pi0,_h_eta0_etapi0pi0; + Histo1DPtr _h_eta1_etapip,_h_eta1_etapim,_h_eta1_pippim,_h_eta1_etapippim; + Histo1DPtr _h_4pi0_pi0pi0,_h_4pi0_pippi0,_h_4pi0_pimpi0,_h_4pi0_pippim,_h_4pi0_pippimpi0,_h_4pi0_pippi0pi0, + _h_4pi0_pimpi0pi0,_h_4pi0_4pi; + Histo1DPtr _h_4pi1_pippip,_h_4pi1_pimpim,_h_4pi1_pippim,_h_4pi1_pimpimpip,_h_4pi1_pippippim,_h_4pi1_4pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MC_F1_Decay); + + +} diff --git a/analyses/pluginMC/MC_F1_Decay.info b/analyses/pluginMC/MC_F1_Decay.info new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_F1_Decay.info @@ -0,0 +1,9 @@ +Name: MC_F1_Decay +Summary: Analysis of Kinematic distributions of $f_1$ meson decays +Status: VALIDATED +Authors: + - Peter Richardson +RunInfo: Any type of process producing f_1 mesons +NeedCrossSection: no +Description: + 'Simple analysis of kinematic distributions in f_1 meson decays.' diff --git a/analyses/pluginMC/MC_F1_Decay.plot b/analyses/pluginMC/MC_F1_Decay.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_F1_Decay.plot @@ -0,0 +1,131 @@ +BEGIN PLOT /MC_F1_Decay/eta0_etapi0 +Title=$\eta\pi^0$ mass distribution in $f_1\to \eta\pi^0\pi^0$ +XLabel=$m_{\eta\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\eta\pi^0}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/eta0_etapi0pi0 +Title=$\eta\pi^0\pi^0$ mass distribution in $f_1\to \eta\pi^0\pi^0$ +XLabel=$m_{\eta\pi^0\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\eta\pi^0\pi^0}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/eta0_pi0pi0 +Title=$\pi^0\pi^0$ mass distribution in $f_1\to \eta\pi^0\pi^0$ +XLabel=$m_{\pi^0\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^0\pi^0}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT + +BEGIN PLOT /MC_F1_Decay/eta1_etapip +Title=$\eta\pi^+$ mass distribution in $f_1\to \eta\pi^+\pi^-$ +XLabel=$m_{\eta\pi^+}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\eta\pi^+}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/eta1_etapippim +Title=$\eta\pi^+\pi^-$ mass distribution in $f_1\to \eta\pi^+\pi^-$ +XLabel=$m_{\eta\pi^+\pi^-}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\eta\pi^+\pi^-}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/eta1_etapim +Title=$\eta\pi^-$ mass distribution in $f_1\to \eta\pi^+\pi^-$ +XLabel=$m_{\eta\pi^-}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\eta\pi^-}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/eta1_pippim +Title=$\pi^+\pi^-$ mass distribution in $f_1\to \eta\pi^+\pi^-$ +XLabel=$m_{\pi^+\pi^-}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^-}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT + + +BEGIN PLOT /MC_F1_Decay/4pi1_pippim +Title=$\pi^+\pi^-$ mass distribution in $f_1\to 2\pi^+2\pi^-$ +XLabel=$m_{\pi^+\pi^-}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^-}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi1_pippip +Title=$\pi^+\pi^+$ mass distribution in $f_1\to 2\pi^+2\pi^-$ +XLabel=$m_{\pi^+\pi^+}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^+}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi1_pimpim +Title=$\pi^-\pi^-$ mass distribution in $f_1\to 2\pi^+2\pi^-$ +XLabel=$m_{\pi^-\pi^-}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^-\pi^-}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi1_pippippim +Title=$\pi^+\pi^+\pi^-$ mass distribution in $f_1\to 2\pi^+2\pi^-$ +XLabel=$m_{\pi^+\pi^+\pi^-}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^+\pi^-}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi1_pimpimpip +Title=$\pi^-\pi^-\pi^+$ mass distribution in $f_1\to 2\pi^+2\pi^-$ +XLabel=$m_{\pi^-\pi^-\pi^+}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^-\pi^-\pi^+}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi1_4pi +Title=$2\pi^-2\pi^+$ mass distribution in $f_1\to 2\pi^+2\pi^-$ +XLabel=$m_{2\pi^-2\pi^+}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{2\pi^-2\pi^+}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT + +BEGIN PLOT /MC_F1_Decay/4pi0_pippim +Title=$\pi^+\pi^-$ mass distribution in $f_1\to \pi^+\pi^-2\pi^0$ +XLabel=$m_{\pi^+\pi^-}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^-}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi0_pippi0 +Title=$\pi^+\pi^0$ mass distribution in $f_1\to \pi^+\pi^-2\pi^0$ +XLabel=$m_{\pi^+\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^0}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi0_pimpi0 +Title=$\pi^-\pi^0$ mass distribution in $f_1\to \pi^+\pi^-2\pi^0$ +XLabel=$m_{\pi^-\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^-\pi^0}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi0_pi0pi0 +Title=$\pi^0\pi^0$ mass distribution in $f_1\to \pi^+\pi^-2\pi^0$ +XLabel=$m_{\pi^0\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^0\pi^0}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT + +BEGIN PLOT /MC_F1_Decay/4pi0_pippimpi0 +Title=$\pi^-\pi^+\pi^0$ mass distribution in $f_1\to \pi^+\pi^-2\pi^0$ +XLabel=$m_{\pi^-\pi^+\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^-\pi^+\pi^0}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi0_pippi0pi0 +Title=$\pi^+2\pi^0$ mass distribution in $f_1\to \pi^+\pi^-2\pi^0$ +XLabel=$m_{\pi^+2\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+2\pi^0}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi0_pimpi0pi0 +Title=$\pi^-2\pi^0$ mass distribution in $f_1\to \pi^+\pi^-2\pi^0$ +XLabel=$m_{\pi^-2\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^-2\pi^0}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_F1_Decay/4pi0_4pi +Title=$\pi^-\pi^+2\pi^0$ mass distribution in $f_1\to \pi^+\pi^-2\pi^0$ +XLabel=$m_{\pi^-\pi^+2\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^-\pi^+2\pi^0}$ [${\rm GeV}^{-1}$] +LogY=0 +END PLOT diff --git a/analyses/pluginMC/MC_Meson_Meson_Leptons_Decay.cc b/analyses/pluginMC/MC_Meson_Meson_Leptons_Decay.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Meson_Meson_Leptons_Decay.cc @@ -0,0 +1,241 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" +#include "Rivet/Tools/ParticleIdUtils.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MC_Meson_Meson_Leptons_Decay : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MC_Meson_Meson_Leptons_Decay); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(),"UFS"); + + } + + void findDecayProducts(const Particle & mother, + unsigned int & nstable, + Particles& lp, Particles& lm, + Particles& scalar, + Particles& vector) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::EMINUS || id == PID::MUON ) { + lm.push_back(p); + ++nstable; + } + else if (id == PID::EPLUS || id == PID::ANTIMUON) { + lp.push_back(p); + ++nstable; + } + else if (abs(id)%10==1 && PID::isMeson(id)) { + scalar.push_back(p); + ++nstable; + } + else if ((abs(id)%10==3 && PID::isMeson(id)) || + id==PID::PHOTON ) { + vector.push_back(p); + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p,nstable,lp,lm,scalar,vector); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + // loop over unstable particles + for(const Particle& iMeson : apply(event, "UFS").particles()) { + // only consider scalar/vector mesons + long pid = iMeson.pdgId(); + if(!PID::isMeson(pid)) continue; + if(abs(pid)%10!=3 and abs(pid)%10!=1 ) continue; + Particles lp,lm,scalar,vector; + unsigned int nstable(0); + findDecayProducts(iMeson,nstable,lp,lm,scalar,vector); + if(nstable!=3 || lp.size()!=1 || lm.size()!=1 || lp[0].pdgId()!=-lm[0].pdgId()) continue; + if(scalar.size()==1) { + // check if we already have this decay + unsigned int ix=0; bool found(false); + while(!found&&ix<_incomingV.size()) { + if(_incomingV[ix]==pid && _outgoingP[ix]==scalar[0].pdgId() && + _outgoingf_V[ix]==lm[0].pdgId()) { + found=true; + } + else { + ++ix; + } + } + // create a new graph if needed + if(!found) { + ix=_incomingV.size(); + _incomingV.push_back(pid); + _outgoingP.push_back(scalar[0].pdgId()); + _outgoingf_V.push_back(lm[0].pdgId()); + ostringstream title; + title << "h_" << abs(pid); + if(pid>0) title << "p"; + else title << "m"; + title << "_" << abs(scalar[0].pdgId()); + if(scalar[0].pdgId()>0) title << "p"; + else title << "m"; + title << "_" << lm[0].pdgId() << "_"; + _mff_V .push_back(bookHisto1D(title.str()+"mff" , 200, 0., iMeson.mass())); + _mPf .push_back(bookHisto1D(title.str()+"mPf" , 200, 0., iMeson.mass())); + _mPfbar.push_back(bookHisto1D(title.str()+"mPfbar", 200, 0., iMeson.mass())); + } + // add the results to the histogram + _mff_V [ix]->fill((lm [0].momentum()+lp[0].momentum()).mass(),event.weight()); + _mPf [ix]->fill((scalar[0].momentum()+lm[0].momentum()).mass(),event.weight()); + _mPfbar[ix]->fill((scalar[0].momentum()+lp[0].momentum()).mass(),event.weight()); + } + else if(vector.size()==1) { + // check if we already have this decay + unsigned int ix=0; bool found(false); + while(!found&&ix<_incoming_P.size()) { + if(_incoming_P[ix]==pid && _outgoingV[ix]==vector[0].pdgId() && + _outgoingf_P[ix]==lm[0].pdgId()) { + found=true; + } + else { + ++ix; + } + } + // create a new graph if needed + if(!found) { + ix=_incoming_P.size(); + _incoming_P.push_back(pid); + _outgoingV.push_back(vector[0].pdgId()); + _outgoingf_P.push_back(lm[0].pdgId()); + ostringstream title; + title << "h2_" << abs(pid); + if(pid>0) title << "p"; + else title << "m"; + title << "_" << abs(vector[0].pdgId()); + if(vector[0].pdgId()>0) title << "p"; + else title << "m"; + title << "_" << lm[0].pdgId() << "_"; + _mff_P .push_back(bookHisto1D(title.str()+"mff" , 200, 0., iMeson.mass())); + _mVf .push_back(bookHisto1D(title.str()+"mVf" , 200, 0., iMeson.mass())); + _mVfbar.push_back(bookHisto1D(title.str()+"mVfbar", 200, 0., iMeson.mass())); + } + // add the results to the histogram + _mff_P [ix]->fill((lm [0].momentum()+lp[0].momentum()).mass(),event.weight()); + _mVf [ix]->fill((vector[0].momentum()+lm[0].momentum()).mass(),event.weight()); + _mVfbar[ix]->fill((vector[0].momentum()+lp[0].momentum()).mass(),event.weight()); + } + } + } + + /// Normalise histograms etc., after the run + void finalize() { + + // normalize to unity V->P + for(unsigned int ix=0;ix<_mff_V.size();++ix) { + normalize(_mff_V); + normalize(_mPf); + normalize(_mPfbar); + } + // normalize to unity P->V + for(unsigned int ix=0;ix<_mff_P.size();++ix) { + normalize(_mff_P); + normalize(_mVf); + normalize(_mVfbar); + } + + } + + //@} + + + + /// @name Histograms for V -> P + //@{ + /** + * PDG codes of the incoming particles + */ + vector _incomingV; + + /** + * PDG codes of the outgoing pseudoscalar mesons + */ + vector _outgoingP; + + /** + * PDG codes of the outgoing fermion + */ + vector _outgoingf_V; + + /** + * Histograms for the mass of the fermion-antifermion pair + */ + vector _mff_V; + + /** + * Histograms for the masses of the pseudoscalar and the fermion + */ + vector _mPf; + + /** + * Histograms for the masses of the pseudoscalar and the antifermion + */ + vector _mPfbar; + //@} + + /// @name Histograms P->V + //@{ + /** + * PDG codes of the incoming_P particles + */ + vector _incoming_P; + + /** + * PDG codes of the outgoing vector mesons + */ + vector _outgoingV; + + /** + * PDG codes of the outgoing fermion + */ + vector _outgoingf_P; + + /** + * Histograms for the mass of the fermion-antifermion pair + */ + vector _mff_P; + + /** + * Histograms for the masses of the vector and the fermion + */ + vector _mVf; + + /** + * Histograms for the masses of the vector and the antifermion + */ + vector _mVfbar; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MC_Meson_Meson_Leptons_Decay); + + +} diff --git a/analyses/pluginMC/MC_Meson_Meson_Leptons_Decay.info b/analyses/pluginMC/MC_Meson_Meson_Leptons_Decay.info new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Meson_Meson_Leptons_Decay.info @@ -0,0 +1,9 @@ +Name: MC_Meson_Meson_Leptons_Decay +Summary: MC analyis of $V\to P \ell^+\ell^-$ and $P\to V \ell^+\ell^-$ decays +Status: VALIDATED +Authors: + - Peter Richardson +RunInfo: Any process producing vector or scalar meson decays +NeedCrossSection: no +Description: + 'A Monte Carlo analysis for the decay of vector mesons to a pseudoscalar meson, or a pseudoscalar meson to a vector meson, and an $e^+e^-$ or $\mu^+\mu^-$ pair. All such decays are automatically identified. Based on old Herwig++ internal analysis.' diff --git a/analyses/pluginMC/MC_Meson_Meson_Leptons_Decay.plot b/analyses/pluginMC/MC_Meson_Meson_Leptons_Decay.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Meson_Meson_Leptons_Decay.plot @@ -0,0 +1,368 @@ +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/d01-x01-y01 +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_.*_13_mff +XLabel=$m_{\mu^+\mu^-}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\mu^+\mu^-}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_.*_13_mPf +XLabel=$m_{P\mu^-}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{P\mu^-}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_.*_13_mPfbar +XLabel=$m_{P\mu^+}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{P\mu^+}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_.*_11_mff +XLabel=$m_{e^+e^-}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{e^+e^-}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_.*_11_mPf +XLabel=$m_{Pe^-}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{Pe^-}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_.*_11_mPfbar +XLabel=$m_{Pe^+}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{Pe^+}$ [${\rm GeV}^{-1}$] +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_223p_111p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\omega\to\pi^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_223p_111p_13_mPf +Title=$\pi^0\mu^-$ mass distribution in the decay $\omega\to\pi^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_223p_111p_13_mPfbar +Title=$\pi^0\mu^+$ mass distribution in the decay $\omega\to\pi^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_223p_111p_11_mff +Title=$e^+e^-$ mass distribution in the decay $\omega\to\pi^0e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_223p_111p_11_mPf +Title=$\pi^0e^-$ mass distribution in the decay $\omega\to\pi^0e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_223p_111p_11_mPfbar +Title=$\pi^0e^+$ mass distribution in the decay $\omega\to\pi^0e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_111p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\phi\to\pi^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_111p_13_mPf +Title=$\pi^0\mu^-$ mass distribution in the decay $\phi\to\pi^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_111p_13_mPfbar +Title=$\pi^0\mu^+$ mass distribution in the decay $\phi\to\pi^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_111p_11_mff +Title=$e^+e^-$ mass distribution in the decay $\phi\to\pi^0e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_111p_11_mPf +Title=$\pi^0e^-$ mass distribution in the decay $\phi\to\pi^0e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_111p_11_mPfbar +Title=$\pi^0e^+$ mass distribution in the decay $\phi\to\pi^0e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_221p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\phi\to\eta\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_221p_13_mPf +Title=$\eta\mu^-$ mass distribution in the decay $\phi\to\eta\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_221p_13_mPfbar +Title=$\eta\mu^+$ mass distribution in the decay $\phi\to\eta\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_221p_11_mff +Title=$e^+e^-$ mass distribution in the decay $\phi\to\eta e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_221p_11_mPf +Title=$\eta e^-$ mass distribution in the decay $\phi\to\eta e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_333p_221p_11_mPfbar +Title=$\eta e^+$ mass distribution in the decay $\phi\to\eta e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_221p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\psi(2S)\to\eta\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_221p_13_mPf +Title=$\eta\mu^-$ mass distribution in the decay $\psi(2S)\to\eta\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_221p_13_mPfbar +Title=$\eta\mu^+$ mass distribution in the decay $\psi(2S)\to\eta\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_221p_11_mff +Title=$e^+e^-$ mass distribution in the decay $\psi(2S)\to\eta e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_221p_11_mPf +Title=$\eta e^-$ mass distribution in the decay $\psi(2S)\to\eta e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_221p_11_mPfbar +Title=$\eta e^+$ mass distribution in the decay $\psi(2S)\to\eta e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_111p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\psi(2S)\to\pi^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_111p_13_mPf +Title=$\pi^0\mu^-$ mass distribution in the decay $\psi(2S)\to\pi^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_111p_13_mPfbar +Title=$\pi^0\mu^+$ mass distribution in the decay $\psi(2S)\to\pi^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_111p_11_mff +Title=$e^+e^-$ mass distribution in the decay $\psi(2S)\to\pi^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_111p_11_mPf +Title=$\pi^0 e^-$ mass distribution in the decay $\psi(2S)\to\pi^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h_100443p_111p_11_mPfbar +Title=$\pi^0 e^+$ mass distribution in the decay $\psi(2S)\to\pi^0 e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_.*_13_mff +XLabel=$m_{\mu^+\mu^-}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{\mu^+\mu^-}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_.*_13_mVf +XLabel=$m_{V\mu^-}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{V\mu^-}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_.*_13_mVfbar +XLabel=$m_{V\mu^+}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{V\mu^+}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_.*_11_mff +XLabel=$m_{e^+e^-}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{e^+e^-}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_.*_11_mVf +XLabel=$m_{Ve^-}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{Ve^-}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_.*_11_mVfbar +XLabel=$m_{Ve^+}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d} m_{Ve^+}$ [${\rm GeV}^{-1}$] +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\eta\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_13_mVf +Title=$\gamma\mu^-$ mass distribution in the decay $\eta\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_13_mVfbar +Title=$\gamma\mu^+$ mass distribution in the decay $\eta\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_11_mff +Title=$e^+e^-$ mass distribution in the decay $\eta\to\gamma e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_11_mVf +Title=$\gamma e^-$ mass distribution in the decay $\eta\to\gamma e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_11_mVfbar +Title=$\gamma e^+$ mass distribution in the decay $\eta\to\gamma e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\eta\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_13_mVf +Title=$\gamma\mu^-$ mass distribution in the decay $\eta\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_13_mVfbar +Title=$\gamma\mu^+$ mass distribution in the decay $\eta\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_11_mff +Title=$e^+e^-$ mass distribution in the decay $\eta\to\gamma e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_11_mVf +Title=$\gamma e^-$ mass distribution in the decay $\eta\to\gamma e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_221p_22p_11_mVfbar +Title=$\gamma e^+$ mass distribution in the decay $\eta\to\gamma e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_111p_22p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\pi^0\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_111p_22p_13_mVf +Title=$\gamma\mu^-$ mass distribution in the decay $\pi^0\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_111p_22p_13_mVfbar +Title=$\gamma\mu^+$ mass distribution in the decay $\pi^0\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_111p_22p_11_mff +Title=$e^+e^-$ mass distribution in the decay $\pi^0\to\gamma e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_111p_22p_11_mVf +Title=$\gamma e^-$ mass distribution in the decay $\pi^0\to\gamma e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_111p_22p_11_mVfbar +Title=$\gamma e^+$ mass distribution in the decay $\pi^0\to\gamma e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_331p_22p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\eta^\prime\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_331p_22p_13_mVf +Title=$\gamma\mu^-$ mass distribution in the decay $\eta^\prime\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_331p_22p_13_mVfbar +Title=$\gamma\mu^+$ mass distribution in the decay $\eta^\prime\to\gamma\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_331p_22p_11_mff +Title=$e^+e^-$ mass distribution in the decay $\eta^\prime\to\gamma e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_331p_22p_11_mVf +Title=$\gamma e^-$ mass distribution in the decay $\eta^\prime\to\gamma e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_331p_22p_11_mVfbar +Title=$\gamma e^+$ mass distribution in the decay $\eta^\prime\to\gamma e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431p_213p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $D_s^+\to\rho^+\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431p_213p_13_mVf +Title=$\rho^+\mu^-$ mass distribution in the decay $D_s^+\to\rho^+\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431p_213p_13_mVfbar +Title=$\rho^+\mu^+$ mass distribution in the decay $D_s^+\to\rho^+\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431p_213p_11_mff +Title=$e^+e^-$ mass distribution in the decay $D_s^+\to\rho^+ e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431p_213p_11_mVf +Title=$\rho^+e^-$ mass distribution in the decay $D_s^+\to\rho^+ e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431p_213p_11_mVfbar +Title=$\rho^+e^+$ mass distribution in the decay $D_s^+\to\rho^+ e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431m_213m_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $D_s^-\to\rho^-\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431m_213m_13_mVf +Title=$\rho^-\mu^-$ mass distribution in the decay $D_s^-\to\rho^-\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431m_213m_13_mVfbar +Title=$\rho^-\mu^+$ mass distribution in the decay $D_s^-\to\rho^-\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431m_213m_11_mff +Title=$e^+e^-$ mass distribution in the decay $D_s^-\to\rho^- e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431m_213m_11_mVf +Title=$\rho^-e^-$ mass distribution in the decay $D_s^-\to\rho^- e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_431m_213m_11_mVfbar +Title=$\rho^-e^+$ mass distribution in the decay $D_s^-\to\rho^- e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521p_323p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $B^+\to{K^*}^+\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521p_323p_13_mVf +Title=${K^*}^+\mu^-$ mass distribution in the decay $B^+\to{K^*}^+\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521p_323p_13_mVfbar +Title=${K^*}^+\mu^+$ mass distribution in the decay $B^+\to{K^*}^+\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521p_323p_11_mff +Title=$e^+e^-$ mass distribution in the decay $B^+\to{K^*}^+ e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521p_323p_11_mVf +Title=${K^*}^+e^-$ mass distribution in the decay $B^+\to{K^*}^+ e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521p_323p_11_mVfbar +Title=${K^*}^+e^+$ mass distribution in the decay $B^+\to{K^*}^+ e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521m_323m_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $B^-\to{K^*}^-\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521m_323m_13_mVf +Title=${K^*}^-\mu^-$ mass distribution in the decay $B^-\to{K^*}^-\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521m_323m_13_mVfbar +Title=${K^*}^-\mu^+$ mass distribution in the decay $B^-\to{K^*}^-\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521m_323m_11_mff +Title=$e^+e^-$ mass distribution in the decay $B^-\to{K^*}^- e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521m_323m_11_mVf +Title=${K^*}^-e^-$ mass distribution in the decay $B^-\to{K^*}^- e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_521m_323m_11_mVfbar +Title=${K^*}^-e^+$ mass distribution in the decay $B^-\to{K^*}^- e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511p_313p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $B^0\to{K^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511p_313p_13_mVf +Title=${K^*}^0\mu^-$ mass distribution in the decay $B^0\to{K^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511p_313p_13_mVfbar +Title=${K^*}^0\mu^+$ mass distribution in the decay $B^0\to{K^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511p_313p_11_mff +Title=$e^+e^-$ mass distribution in the decay $B^0\to{K^*}^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511p_313p_11_mVf +Title=${K^*}^0e^-$ mass distribution in the decay $B^0\to{K^*}^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511p_313p_11_mVfbar +Title=${K^*}^0e^+$ mass distribution in the decay $B^0\to{K^*}^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511m_313m_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\bar{B}^0\to{\bar{K}^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511m_313m_13_mVf +Title=${\bar{K}^*}^0\mu^-$ mass distribution in the decay $\bar{B}^0\to{\bar{K}^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511m_313m_13_mVfbar +Title=${\bar{K}^*}^0\mu^+$ mass distribution in the decay $\bar{B}^0\to{\bar{K}^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511m_313m_11_mff +Title=$e^+e^-$ mass distribution in the decay $\bar{B}^0\to{\bar{K}^*}^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511m_313m_11_mVf +Title=${\bar{K}^*}^0e^-$ mass distribution in the decay $\bar{B}^0\to{\bar{K}^*}^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_511m_313m_11_mVfbar +Title=${\bar{K}^*}^0e^+$ mass distribution in the decay $\bar{B}^0\to{\bar{K}^*}^0 e^+e^-$ +END PLOT + +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421m_313p_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $\bar{D}^0\to{K^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421m_313p_13_mVf +Title=${K^*}^0\mu^-$ mass distribution in the decay $\bar{D}^0\to{K^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421m_313p_13_mVfbar +Title=${K^*}^0\mu^+$ mass distribution in the decay $\bar{D}^0\to{K^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421m_313p_11_mff +Title=$e^+e^-$ mass distribution in the decay $\bar{D}^0\to{K^*}^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421m_313p_11_mVf +Title=${K^*}^0e^-$ mass distribution in the decay $\bar{D}^0\to{K^*}^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421m_313p_11_mVfbar +Title=${K^*}^0e^+$ mass distribution in the decay $\bar{D}^0\to{K^*}^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421p_313m_13_mff +Title=$\mu^+\mu^-$ mass distribution in the decay $D^0\to{\bar{K}^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421p_313m_13_mVf +Title=${\bar{K}^*}^0\mu^-$ mass distribution in the decay $D^0\to{\bar{K}^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421p_313m_13_mVfbar +Title=${\bar{K}^*}^0\mu^+$ mass distribution in the decay $D^0\to{\bar{K}^*}^0\mu^+\mu^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421p_313m_11_mff +Title=$e^+e^-$ mass distribution in the decay $D^0\to{\bar{K}^*}^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421p_313m_11_mVf +Title=${\bar{K}^*}^0e^-$ mass distribution in the decay $D^0\to{\bar{K}^*}^0 e^+e^-$ +END PLOT +BEGIN PLOT /MC_Meson_Meson_Leptons_Decay/h2_421p_313m_11_mVfbar +Title=${\bar{K}^*}^0e^+$ mass distribution in the decay $D^0\to{\bar{K}^*}^0 e^+e^-$ +END PLOT diff --git a/analyses/pluginMC/MC_OmegaPhia1_3Pion_Decay.cc b/analyses/pluginMC/MC_OmegaPhia1_3Pion_Decay.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_OmegaPhia1_3Pion_Decay.cc @@ -0,0 +1,248 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MC_OmegaPhia1_3Pion_Decay : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MC_OmegaPhia1_3Pion_Decay); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(), "UFS"); + // book histograms a_1 + // Histograms for a_10 -> pi0pi0pi0 + _hist0 = bookHisto1D("hist0",200,0.2,1.5); + // // dalitz plot + _dalitz0 = bookHisto2D("dalitz0",50,0.2,1.5,50,0.2,1.5); + // Histograms for a_1+ -> pi0pi0pi+ + // Mass of the pi0pi0 pair + _hist1A = bookHisto1D("hist1A",200,0.2,1.5); + // Mass of the pi0pi+ pair + _hist1B = bookHisto1D("hist1B",200,0.2,1.5); + // dalitz plot + _dalitz1 = bookHisto2D("dalitz1",50,0.2,1.5,50,0.2,1.5); + // Histograms for a_10 -> pi+pi-pi0 + // Mass of the pi+pi- pair + _hist2A = bookHisto1D("hist2A",200,0.2,1.5); + // Mass of the pi+pi0 pair + _hist2B = bookHisto1D("hist2B",200,0.2,1.5); + // Mass of the pi-pi0 pair + _hist2C = bookHisto1D("hist2C",200,0.2,1.5); + // dalitz plot + _dalitz2 = bookHisto2D("dalitz2",50,0.2,1.5,50,0.2,1.5); + // Histograms for a_1+ -> pi+pi+pi- + // Mass of the pi+pi+ pair + _hist3A = bookHisto1D("hist3A",200,0.2,1.5); + // Mass of the pi+pi- pair + _hist3B = bookHisto1D("hist3B",200,0.2,1.5); + // dalitz plot + _dalitz3 = bookHisto2D("dalitz3",50,0.2,1.5,50,0.2,1.5); + + // Book histograms omega/phi + for(unsigned int ix=0;ix<2;++ix) { + double mmax = ix==0 ? 0.8 : 1.0; + ostringstream title1; title1 << "xhist_" << ix+1; + _h_xhist .push_back(bookHisto1D(title1.str(),200,-300.,300. )); + ostringstream title2; title2 << "yhist_" << ix+1; + _h_yhist .push_back(bookHisto1D(title2.str(),200,0. ,400. )); + ostringstream title3; title3 << "mplus_" << ix+1; + _h_mplus .push_back(bookHisto1D(title3.str(),200,200.,mmax*1000.)); + ostringstream title4; title4 << "mminus_" << ix+1; + _h_mminus .push_back(bookHisto1D(title4.str(),200,200.,mmax*1000.)); + ostringstream title5; title5 << "m0_" << ix+1; + _h_m0 .push_back(bookHisto1D(title5.str(),200,200.,mmax*1000.)); + ostringstream title6; title6 << "dalitz_" << ix+1; + _h_dalitz.push_back(bookHisto2D(title6.str(),50,0.2,mmax,50,0.2,mmax)); + } + } + + + void findDecayProducts(const Particle & mother, unsigned int & nstable, + Particles & pip , Particles & pim , Particles & pi0) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if (id == PID::PIPLUS) { + pip.push_back(p); + ++nstable; + } + else if (id == PID::PIMINUS) { + pim.push_back(p); + ++nstable; + } + else if (id == PID::PI0) { + pi0.push_back(p); + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p, nstable, pip, pim, pi0); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + double weight = event.weight(); + for(const Particle& meson : + apply(event, "UFS").particles(Cuts::pid==PID::PHI || Cuts::pid==PID::OMEGA || + Cuts::abspid==20213 || Cuts::pid==20113 )) { + unsigned int nstable(0); + Particles pip, pim, pi0; + findDecayProducts(meson, nstable, pip, pim, pi0); + if(nstable !=3) continue; + if(meson.pdgId()<0) { + swap(pim,pip); + } + if(meson.pdgId()== PID::PHI || meson.pdgId()==PID::OMEGA) { + if(pip.size()!=1 || pim.size()!=1 || pi0.size()!=1) continue; + unsigned int iloc = meson.pdgId() == PID::OMEGA ? 0 : 1; + LorentzTransform boost = LorentzTransform::mkFrameTransformFromBeta(meson.momentum().betaVec()); + FourMomentum pp = boost.transform(pip[0].momentum()); + FourMomentum pm = boost.transform(pim[0].momentum()); + FourMomentum p0 = boost.transform(pi0[0].momentum()); + double mp = (pp+p0).mass(), mm = (pm+pp).mass(); + _h_mplus [iloc]->fill(mp/MeV,weight); + _h_mminus[iloc]->fill((pm+p0).mass()/MeV,weight); + _h_m0 [iloc]->fill(mm/MeV,weight); + double x = pp.t()-pm.t(); + double y = p0.t()-p0.mass(); + _h_xhist[iloc]->fill(x/MeV,weight); + _h_yhist[iloc]->fill(y/MeV,weight); + _h_dalitz[iloc]->fill(mp,mm,weight); + } + else { + // a_1+ -> pi+pi+pi- + if(pip.size()==2&&pim.size()==1) { + _hist3A->fill((pip[0].momentum()+pip[1].momentum()).mass(),weight); + _hist3B->fill((pip[0].momentum()+pim[0].momentum()).mass(),weight); + _hist3B->fill((pip[1].momentum()+pim[0].momentum()).mass(),weight); + _dalitz3->fill((pip[0].momentum()+pim[0].momentum()).mass(),(pip[1].momentum()+pim[0].momentum()).mass(),weight); + _dalitz3->fill((pip[1].momentum()+pim[0].momentum()).mass(),(pip[0].momentum()+pim[0].momentum()).mass(),weight); + } + // a_1+ -> pi0pi0pi+ + else if(pip.size()==1&&pi0.size()==2) { + _hist1A->fill((pi0[0].momentum()+pi0[1].momentum()).mass(),weight); + _hist1B->fill((pip[0].momentum()+pi0[0].momentum()).mass(),weight); + _hist1B->fill((pip[0].momentum()+pi0[1].momentum()).mass(),weight); + _dalitz1->fill((pip[0].momentum()+pi0[0].momentum()).mass(),(pip[0].momentum()+pi0[1].momentum()).mass(),weight); + _dalitz1->fill((pip[0].momentum()+pi0[1].momentum()).mass(),(pip[0].momentum()+pi0[0].momentum()).mass(),weight); + } + // a_10 -> pi0pi0pi0 + else if(pi0.size()==3) { + _hist0->fill((pi0[0].momentum()+pi0[1].momentum()).mass(),weight); + _hist0->fill((pi0[0].momentum()+pi0[2].momentum()).mass(),weight); + _hist0->fill((pi0[1].momentum()+pi0[2].momentum()).mass(),weight); + _dalitz0->fill((pi0[0].momentum()+pi0[1].momentum()).mass(),(pi0[0].momentum()+pi0[2].momentum()).mass(),weight); + _dalitz0->fill((pi0[0].momentum()+pi0[1].momentum()).mass(),(pi0[1].momentum()+pi0[2].momentum()).mass(),weight); + _dalitz0->fill((pi0[0].momentum()+pi0[2].momentum()).mass(),(pi0[1].momentum()+pi0[2].momentum()).mass(),weight); + _dalitz0->fill((pi0[0].momentum()+pi0[2].momentum()).mass(),(pi0[0].momentum()+pi0[1].momentum()).mass(),weight); + _dalitz0->fill((pi0[1].momentum()+pi0[2].momentum()).mass(),(pi0[0].momentum()+pi0[1].momentum()).mass(),weight); + _dalitz0->fill((pi0[1].momentum()+pi0[2].momentum()).mass(),(pi0[0].momentum()+pi0[2].momentum()).mass(),weight); + } + // a_10 -> pi+pi-pi0 + else if(pi0.size()==1&&pip.size()==1&&pim.size()==1) { + _hist2A->fill((pim[0].momentum()+pip[0].momentum()).mass(),weight); + _hist2B->fill((pip[0].momentum()+pi0[0].momentum()).mass(),weight); + _hist2C->fill((pim[0].momentum()+pi0[0].momentum()).mass(),weight); + _dalitz2->fill((pim[0].momentum()+pi0[0].momentum()).mass(),(pip[0].momentum()+pi0[0].momentum()).mass(),weight); + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + // a_1 + normalize(_hist0); + normalize(_dalitz0); + normalize(_hist1A); + normalize(_hist1B); + normalize(_dalitz1); + normalize(_hist2A); + normalize(_hist2B); + normalize(_hist2C); + normalize(_dalitz2); + normalize(_hist3A); + normalize(_hist3B); + normalize(_dalitz3); + // omega/phi + for(unsigned int ix=0;ix<2;++ix) { + normalize(_h_xhist [ix]); + normalize(_h_yhist [ix]); + normalize(_h_mplus [ix]); + normalize(_h_mminus[ix]); + normalize(_h_m0 [ix]); + normalize(_h_dalitz[ix]); + } + } + + //@} + + /// @name Histograms a_1 + //@{ + // Histograms for a_10 -> pi0pi0pi0 + Histo1DPtr _hist0; + // dalitz plot + Histo2DPtr _dalitz0; + // Histograms for a_1+ -> pi0pi0pi+ + // Mass of the pi0pi0 pair + Histo1DPtr _hist1A; + // Mass of the pi0pi+ pair + Histo1DPtr _hist1B; + // dalitz plot + Histo2DPtr _dalitz1; + // Histograms for a_10 -> pi+pi-pi0 + // Mass of the pi+pi- pair + Histo1DPtr _hist2A; + // Mass of the pi+pi0 pair + Histo1DPtr _hist2B; + // Mass of the pi-pi0 pair + Histo1DPtr _hist2C; + // dalitz plot + Histo2DPtr _dalitz2; + // Histograms for a_1+ -> pi+pi+pi- + // Mass of the pi+pi+ pair + Histo1DPtr _hist3A; + // Mass of the pi+pi- pair + Histo1DPtr _hist3B; + // dalitz plot + Histo2DPtr _dalitz3; + //@} + + /// @name Histograms omega/phi + //@{ + // Histogram for the x-values + vector _h_xhist; + // Histogram for the y-values + vector _h_yhist; + // The mass of the \rho^+ + vector _h_mplus; + // The mass of the \rho^- + vector _h_mminus; + // The mass of the \rho^0 + vector _h_m0; + // Dalitz plot + vector _h_dalitz; + //@} + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MC_OmegaPhia1_3Pion_Decay); + + +} diff --git a/analyses/pluginMC/MC_OmegaPhia1_3Pion_Decay.info b/analyses/pluginMC/MC_OmegaPhia1_3Pion_Decay.info new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_OmegaPhia1_3Pion_Decay.info @@ -0,0 +1,10 @@ +Name: MC_OmegaPhia1_3Pion_Decay +Summary: MC analysis of $\omega$, $\phi$ and $a_1\to3\pi$ decays +Status: VALIDATED +Authors: + - Peter Richardson +RunInfo: Any process producing a1, omega or phi mesons +NeedCrossSection: no +Description: + 'Analysis of the mass distributions and Dalitz plots in $a_1\to3\pi$ and $\omega,\phi\to\pi^+\pi^-\pi^0$ decays. + Based on old Herwig++ internal analysis.' diff --git a/analyses/pluginMC/MC_OmegaPhia1_3Pion_Decay.plot b/analyses/pluginMC/MC_OmegaPhia1_3Pion_Decay.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_OmegaPhia1_3Pion_Decay.plot @@ -0,0 +1,130 @@ +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/hist0 +Title=$\pi^0\pi^0$ mass distribution in $a_1^0\to3\pi^0$ decays +XLabel=$m_{\pi^0\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^0}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/dalitz0 +Title=Dalitz plot for $a_1^0\to3\pi^0$ decays +XLabel=$m_{\pi^0\pi^0}$ [GeV] +YLabel=$m_{\pi^0\pi^0}$ [GeV] +ZLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^0}/{\rm d}m_{\pi^0\pi^0}$ [${\rm GeV}^{-2}$] +END PLOT + +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/hist1A +Title=$\pi^0\pi^0$ mass distribution in $a_1^+\to\pi^+2\pi^0$ decays +XLabel=$m_{\pi^0\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^0}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/hist1B +Title=$\pi^0\pi^+$ mass distribution in $a_1^+\to\pi^+2\pi^0$ decays +XLabel=$m_{\pi^0\pi^+}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^+}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/dalitz1 +Title=Dalitz plot for $a_1^+\to\pi^+2\pi^0$ decays +XLabel=$m_{\pi^+\pi^0}$ [GeV] +YLabel=$m_{\pi^+\pi^0}$ [GeV] +ZLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^0}/{\rm d}m_{\pi^+\pi^0}$ [${\rm GeV}^{-2}$] +END PLOT + +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/hist2A +Title=$\pi^+\pi^-$ mass distribution in $a_1^0\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^+\pi^-}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^-}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/hist2B +Title=$\pi^+\pi^0$ mass distribution in $a_1^0\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^+\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^0}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/hist2C +Title=$\pi^-\pi^0$ mass distribution in $a_1^0\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^-\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^0}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/dalitz2 +Title=Dalitz plot for $a_1^0\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^-\pi^0}$ [GeV] +YLabel=$m_{\pi^+\pi^0}$ [GeV] +ZLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^0}/{\rm d}m_{\pi^+\pi^0}$ [${\rm GeV}^{-2}$] +END PLOT + +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/hist3A +Title=$\pi^+\pi^+$ mass distribution in $a_1^+\to2\pi^+\pi^-$ decays +XLabel=$m_{\pi^+\pi^+}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^+}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/hist3B +Title=$\pi^-\pi^+$ mass distribution in $a_1^+\to2\pi^+\pi^-$ decays +XLabel=$m_{\pi^-\pi^+}$ [GeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^+}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/dalitz3 +Title=Dalitz plot for $a_1^+\to2\pi^+\pi^-$ decays +XLabel=$m_{\pi^+\pi^-}$ [GeV] +YLabel=$m_{\pi^+\pi^-}$ [GeV] +ZLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^0}/{\rm d}m_{\pi^+\pi^0}$ [${\rm GeV}^{-2}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/xhist_1 +Title=$x$ distribution in $\omega\to\pi^0\pi^+\pi^-$ decays +XLabel=$x$ [MeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} x$ [$\rm{MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/yhist_1 +Title=$y$ distribution in $\omega\to\pi^0\pi^+\pi^-$ decays +XLabel=$y$ [MeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} y$ [$\rm{MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/mminus_1 +Title=$\pi^-\pi^0$ mass distribution in $\omega\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^-\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^-\pi^0}$ [$\rm{MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/mplus_1 +Title=$\pi^+\pi^0$ mass distribution in $\omega\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^+\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^0}$ [$\rm{MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/m0_1 +Title=$\pi^+\pi^-$ mass distribution in $\omega\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^+\pi^-}$ [MeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^-}$ [$\rm{MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/dalitz_1 +Title=Dalitz plot for $\omega\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^+\pi^0}$ [GeV] +YLabel=$m_{\pi^+-\pi^0}$ [GeV] +ZLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^0}/{\rm d} m_{\pi^-\pi^0}$ [$\rm{GeV}^{-2}$] +END PLOT + +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/xhist_2 +Title=$x$ distribution in $\phi\to\pi^0\pi^+\pi^-$ decays +XLabel=$x$ [MeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} x$ [$\rm{MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/yhist_2 +Title=$y$ distribution in $\phi\to\pi^0\pi^+\pi^-$ decays +XLabel=$y$ [MeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} y$ [$\rm{MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/mminus_2 +Title=$\pi^-\pi^0$ mass distribution in $\phi\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^-\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^-\pi^0}$ [$\rm{MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/mplus_2 +Title=$\pi^+\pi^0$ mass distribution in $\phi\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^+\pi^0}$ [MeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^0}$ [$\rm{MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/m0_2 +Title=$\pi^+\pi^-$ mass distribution in $\phi\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^+\pi^-}$ [MeV] +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^-}$ [$\rm{MeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_OmegaPhia1_3Pion_Decay/dalitz_2 +Title=Dalitz plot for $\phi\to\pi^0\pi^+\pi^-$ decays +XLabel=$m_{\pi^+\pi^0}$ [GeV] +YLabel=$m_{\pi^+-\pi^0}$ [GeV] +ZLabel=$1/\Gamma{\rm d}\Gamma/{\rm d} m_{\pi^+\pi^0}/{\rm d} m_{\pi^-\pi^0}$ [$\rm{GeV}^{-2}$] +END PLOT diff --git a/analyses/pluginMC/MC_Onium_PiPi_Decay.cc b/analyses/pluginMC/MC_Onium_PiPi_Decay.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Onium_PiPi_Decay.cc @@ -0,0 +1,152 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MC_Onium_PiPi_Decay : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MC_Onium_PiPi_Decay); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(),"UFS"); + + } + + void findDecayProducts(const Particle & mother, + unsigned int & nstable, + Particles& pip, Particles& pim, + Particles& pi0, Particles & onium) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::PIMINUS) { + pim.push_back(p); + ++nstable; + } + else if (id == PID::PIPLUS) { + pim.push_back(p); + ++nstable; + } + else if (id == PID::PI0) { + pi0.push_back(p); + ++nstable; + } + else if (abs(id)%1000==443 || abs(id)%1000==553) { + onium.push_back(p); + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p,nstable,pip,pim,pi0,onium); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + double weight = event.weight(); + // loop over unstable particles + for(const Particle& vMeson : apply(event, "UFS").particles()) { + int id = vMeson.pdgId(); + if(id%1000!=443 && id%1000!=553) continue; + unsigned int nstable(0); + Particles pip, pim, pi0, onium; + findDecayProducts(vMeson,nstable,pip,pim,pi0,onium); + // check for onium + if(onium.size() !=1 || nstable !=3) continue; + // check for pipi + if( ! ((pip.size()==1 && pim.size() ==1) || pi0.size()==2)) continue; + // check if histos already made + unsigned int iloc=0; bool found(false); + while(!found&&iloc<_incoming.size()) { + if(_incoming[iloc]==vMeson.pdgId()&&_outgoing[iloc]==onium[0].pdgId()) found=true; + else ++iloc; + } + // if histos not made, make them + if(!found) { + double twompi = 0.378; + double upp = vMeson.mass()-onium[0].mass(); + iloc=_incoming.size(); + _incoming.push_back(vMeson.pdgId()); + _outgoing.push_back(onium[0].pdgId()); + ostringstream title; + title << "h_" << vMeson.pdgId() << "_" << onium[0].pdgId() << "_"; + _mpipi.push_back(make_pair(bookHisto1D(title.str()+"mpippim",200,twompi/GeV,upp/GeV), + bookHisto1D(title.str()+"mpi0pi0",200,twompi/GeV,upp/GeV))); + _hel .push_back(make_pair(bookHisto1D(title.str()+"hpippim",200,-1.,1.), + bookHisto1D(title.str()+"hpi0pi0",200, 0.,1.))); + } + // boost to rest frame of the pion pair + FourMomentum q = vMeson.momentum()-onium[0].momentum(); + LorentzTransform boost = LorentzTransform::mkFrameTransformFromBeta(q.betaVec()); + FourMomentum qp = onium[0].momentum(); + FourMomentum ppi= pip.size()==1 ? pip[0].momentum() : pi0[0].momentum(); + qp = boost.transform(qp); + ppi = boost.transform(ppi); + double cX=-ppi.p3().unit().dot(qp.p3().unit()); + if(pi0.size()==2) { + _mpipi[iloc].second->fill(q.mass(),weight); + _hel [iloc].second->fill(abs(cX),weight); + } + else { + _mpipi[iloc].first->fill(q.mass(),weight); + _hel [iloc].first->fill(cX,weight); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + // normalize to unity + for(unsigned int ix=0;ix<_mpipi.size();++ix) { + normalize(_mpipi[ix].first ); + normalize(_mpipi[ix].second); + normalize(_hel[ix].first ); + normalize(_hel[ix].second); + } + } + + //@} + + /** + * Incoming onium states + */ + vector _incoming; + + /** + * Outgoing onium states + */ + vector _outgoing; + + /** + * Histograms for the \f$\pi^+\pi^-\f$ masses + */ + vector > _mpipi; + + /** + * Histmgrams for the helicity angles + */ + vector > _hel; + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MC_Onium_PiPi_Decay); + + +} diff --git a/analyses/pluginMC/MC_Onium_PiPi_Decay.info b/analyses/pluginMC/MC_Onium_PiPi_Decay.info new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Onium_PiPi_Decay.info @@ -0,0 +1,10 @@ +Name: MC_Onium_PiPi_Decay +Summary: Analysis of kinematics in $\mathcal{O}\to\mathcal{O}^\prime\pi\pi$ decays +Status: VALIDATED +Authors: + - Peter Richardson +RunInfo: Any type of process producing bottom or charmonium mesons +NeedCrossSection: no +Description: + 'Analysis of the kinematics in the decay of bottom and charmonium resonances to lighter resonances and $\pi\pi$' + \ No newline at end of file diff --git a/analyses/pluginMC/MC_Onium_PiPi_Decay.plot b/analyses/pluginMC/MC_Onium_PiPi_Decay.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Onium_PiPi_Decay.plot @@ -0,0 +1,108 @@ +BEGIN PLOT /MC_Onium_PiPi_Decay/h_.*_mpi0pi0 +XLabel=$m_{\pi^0\pi^0}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m_{\pi^0\pi^0}$ [${\rm GeV}^{-1}$] +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_.*_mpippim +XLabel=$m_{\pi^+\pi^-}$ [GeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m_{\pi^+\pi^-}$ [${\rm GeV}^{-1}$] +END PLOT + +BEGIN PLOT /MC_Onium_PiPi_Decay/h_.*_hpi0pi0 +XLabel=$\cos\chi$ +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}\cos\chi$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_.*_hpippim +XLabel=$\cos\chi$ +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}\cos\chi$ +END PLOT + +BEGIN PLOT /MC_Onium_PiPi_Decay/h_100443_443_mpi0pi0 +Title=$m_{\pi^0\pi^0}$ in the decay $\psi(2S)\to J/\psi\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_100443_443_mpippim +Title=$m_{\pi^+\pi^-}$ in the decay $\psi(2S)\to J/\psi\pi^+\pi^-$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_100443_443_hpi0pi0 +Title=Helicity angle in the decay $\psi(2S)\to J/\psi\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_100443_443_hpippim +Title=Helicity angle in the decay $\psi(2S)\to J/\psi\pi^+\pi^-$ +END PLOT + +BEGIN PLOT /MC_Onium_PiPi_Decay/h_30443_443_mpi0pi0 +Title=$m_{\pi^0\pi^0}$ in the decay $\psi(3770)\to J/\psi\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_30443_443_mpippim +Title=$m_{\pi^+\pi^-}$ in the decay $\psi(3770)\to J/\psi\pi^+\pi^-$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_30443_443_hpi0pi0 +Title=Helicity angle in the decay $\psi(3770)\to J/\psi\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_30443_443_hpippim +Title=Helicity angle in the decay $\psi(3770)\to J/\psi\pi^+\pi^-$ +END PLOT + +BEGIN PLOT /MC_Onium_PiPi_Decay/h_100553_553_mpi0pi0 +Title=$m_{\pi^0\pi^0}$ in the decay $\Upsilon(2S)\to \Upsilon\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_100553_553_mpippim +Title=$m_{\pi^+\pi^-}$ in the decay $\Upsilon(2S)\to \Upsilon\pi^+\pi^-$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_100553_553_hpi0pi0 +Title=Helicity angle in the decay $\Upsilon(2S)\to \Upsilon\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_100553_553_hpippim +Title=Helicity angle in the decay $\Upsilon(2S)\to \Upsilon\pi^+\pi^-$ +END PLOT + +BEGIN PLOT /MC_Onium_PiPi_Decay/h_200553_553_mpi0pi0 +Title=$m_{\pi^0\pi^0}$ in the decay $\Upsilon(3S)\to \Upsilon\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_200553_553_mpippim +Title=$m_{\pi^+\pi^-}$ in the decay $\Upsilon(3S)\to \Upsilon\pi^+\pi^-$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_200553_553_hpi0pi0 +Title=Helicity angle in the decay $\Upsilon(3S)\to \Upsilon\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_200553_553_hpippim +Title=Helicity angle in the decay $\Upsilon(3S)\to \Upsilon\pi^+\pi^-$ +END PLOT + +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_553_mpi0pi0 +Title=$m_{\pi^0\pi^0}$ in the decay $\Upsilon(4S)\to \Upsilon\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_553_mpippim +Title=$m_{\pi^+\pi^-}$ in the decay $\Upsilon(4S)\to \Upsilon\pi^+\pi^-$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_553_hpi0pi0 +Title=Helicity angle in the decay $\Upsilon(4S)\to \Upsilon\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_553_hpippim +Title=Helicity angle in the decay $\Upsilon(4S)\to \Upsilon\pi^+\pi^-$ +END PLOT + +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_100553_mpi0pi0 +Title=$m_{\pi^0\pi^0}$ in the decay $\Upsilon(4S)\to \Upsilon(2S)\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_100553_mpippim +Title=$m_{\pi^+\pi^-}$ in the decay $\Upsilon(4S)\to \Upsilon(2S)\pi^+\pi^-$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_100553_hpi0pi0 +Title=Helicity angle in the decay $\Upsilon(4S)\to \Upsilon(2S)\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_100553_hpippim +Title=Helicity angle in the decay $\Upsilon(4S)\to \Upsilon(2S)\pi^+\pi^-$ +END PLOT + +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_200553_mpi0pi0 +Title=$m_{\pi^0\pi^0}$ in the decay $\Upsilon(4S)\to \Upsilon(3S)\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_200553_mpippim +Title=$m_{\pi^+\pi^-}$ in the decay $\Upsilon(4S)\to \Upsilon(3S)\pi^+\pi^-$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_200553_hpi0pi0 +Title=Helicity angle in the decay $\Upsilon(4S)\to \Upsilon(3S)\pi^0\pi^0$ +END PLOT +BEGIN PLOT /MC_Onium_PiPi_Decay/h_300553_200553_hpippim +Title=Helicity angle in the decay $\Upsilon(4S)\to \Upsilon(3S)\pi^+\pi^-$ +END PLOT \ No newline at end of file diff --git a/analyses/pluginMC/MC_Semi_Leptonic_Decay.cc b/analyses/pluginMC/MC_Semi_Leptonic_Decay.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Semi_Leptonic_Decay.cc @@ -0,0 +1,180 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MC_Semi_Leptonic_Decay : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MC_Semi_Leptonic_Decay); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(), "UFS"); + + } + + void findDecayProducts(const Particle & mother, + unsigned int & nstable, + Particles& lp, Particles& lm, + Particles& nu, Particles& nub, + Particles& out) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::EMINUS || id == PID::MUON ) { + lm .push_back(p); + ++nstable; + } + else if (id == PID::EPLUS || id == PID::ANTIMUON) { + lp .push_back(p); + ++nstable; + } + else if ( id == PID::NU_E || id == PID::NU_EBAR ) { + nu .push_back(p); + ++nstable; + } + else if (id == PID::NU_MU || id == PID::NU_MUBAR ) { + nub.push_back(p); + ++nstable; + } + else if (PID::isMeson(id)) { + out.push_back(p); + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p,nstable,lp,lm,nu,nub,out); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + double weight = event.weight(); + // loop over unstable particles + for(const Particle& meson : apply(event, "UFS").particles()) { + int id = meson.pdgId(); + // spin 0 mesons + if(!PID::isMeson(id)) continue; + if(abs(id)%10!=1) continue; + unsigned int nstable(0); + Particles lp, lm, nu, nub, out; + findDecayProducts(meson,nstable,lp,lm,nu,nub,out); + if(nstable!=3 || out.size()!=1) continue; + int ilep=0; + FourMomentum plep,pmnu=out[0].momentum(); + double me2(0.); + if( lp.size()==1 && nu.size()==1 && out.size()==1 ) { + if(nu[0].pdgId() != -lp[0].pdgId()+1) continue; + ilep = lp[0].pdgId(); + plep = nu[0].momentum()+lp[0].momentum(); + pmnu += nu[0].momentum(); + me2 = lp[0].mass2(); + } + else if( lm.size()==1 && nub.size()==1 && out.size()==1 ) { + if(nub[0].pdgId() != -lm[0].pdgId()-1) continue; + ilep = lm[0].pdgId(); + plep = nub[0].momentum()+lm[0].momentum(); + pmnu += nub[0].momentum(); + me2 = lm[0].mass2(); + } + else + continue; + // check if histos already exist + unsigned int iloc=0; bool found(false); + while(!found&&iloc<_incoming.size()) { + if(_incoming[iloc] == id && + _outgoing[iloc] == out[0].pdgId() && + ilep==_outgoingL[iloc]) found=true; + else ++iloc; + } + if(!found) { + iloc=_incoming.size(); + _incoming.push_back(id); + _outgoing.push_back(out[0].pdgId()); + _outgoingL.push_back(ilep); + ostringstream title; + title << "h_" << abs(id); + if(id>0) title << "p"; + else title << "m"; + title << "_" << abs(out[0].pdgId()); + if(out[0].pdgId()>0) title << "p"; + else title << "m"; + title << "_" << abs(ilep); + if(ilep>0) title << "p"; + else title << "m"; + title << "_"; + _energy.push_back(bookHisto1D(title.str()+"energy", + 200,0.0,0.5*meson.mass()/MeV)); + _scale .push_back(bookHisto1D(title.str()+"scale", + 200,0.0,meson.mass()/MeV)); + } + // add the results to the histogram + _scale[iloc]->fill(plep.mass()/MeV,weight); + double ee = 0.5/meson.mass()*(meson.mass2()-pmnu.mass2()+me2); + _energy[iloc]->fill(ee/MeV,weight); + } + } + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=0;ix<_energy.size();++ix) { + normalize(_energy); + normalize(_scale ); + } + } + + //@} + + + /// @name Histograms + //@{ + /** + * PDG codes of the decaying mesons + */ + vector _incoming; + + /** + * PDG codes of the decay products + */ + vector _outgoing; + + /** + * Identidies of the leptons + */ + vector _outgoingL; + + /** + * Histograms + */ + //@{ + /** + * The lepton energy + */ + vector _energy; + + /** + * The \f$q\f$ value + */ + vector _scale; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MC_Semi_Leptonic_Decay); + + +} diff --git a/analyses/pluginMC/MC_Semi_Leptonic_Decay.info b/analyses/pluginMC/MC_Semi_Leptonic_Decay.info new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Semi_Leptonic_Decay.info @@ -0,0 +1,9 @@ +Name: MC_Semi_Leptonic_Decay +Summary: MC analysis of the Kinematics in Semi-Leptonic Meson decays +Status: VALIDATED +Authors: + - Peter Richardson +RunInfo: Any type of process producing mesons which decay semi-leptonically +NeedCrossSection: no +Description: + 'Analysis of the kinematics in semileptonic meson decays.' diff --git a/analyses/pluginMC/MC_Semi_Leptonic_Decay.plot b/analyses/pluginMC/MC_Semi_Leptonic_Decay.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_Semi_Leptonic_Decay.plot @@ -0,0 +1,972 @@ +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_.*_13m_energy +XLabel=$E_{\mu^+}$ [Me]V +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}E_{\mu^+}$ [${\rm MeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_.*_13m_scale +XLabel=$m_{\mu^+\nu_\mu}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m_{\mu^+\nu_\mu}$ [${\rm MeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_.*_13p_energy +XLabel=$E_{\mu^-}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}E_{\mu^-}$ [${\rm MeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_.*_13p_scale +XLabel=$m_{\mu^-\bar\nu_\mu}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m_{\mu^-\bar\nu_\mu}$ [${\rm MeV}^{-1}$] +LogY=0 +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_.*_11m_energy +XLabel=$E_{e^+}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}E_{e^+}$ [${\rm MeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_.*_11m_scale +XLabel=$m_{e^+\nu_e}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m_{e^+\nu_e}$ [${\rm MeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_.*_11p_energy +XLabel=$E_{e^-}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}E_{e^-}$ [${\rm MeV}^{-1}$] +LogY=0 +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_.*_11p_scale +XLabel=$m_{e^-\bar\nu_e}$ [MeV] +YLabel=$1/\Gamma{\rm d} \Gamma/{\rm d}m_{e^-\bar\nu_e}$ [${\rm MeV}^{-1}$] +LogY=0 +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_10313p_13p_energy +Title=$\mu^-$ energy in the decay $D^-\to K_1(1270)^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_10313p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^-\to K_1(1270)^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_10313p_11p_energy +Title=$e^-$ energy in the decay $D^-\to K_1(1270)^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_10313p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^-\to K_1(1270)^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_10313m_13m_energy +Title=$\mu^+$ energy in the decay $D^+\to \bar{K}_1(1270)^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_10313m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D^+\to \bar{K}_1(1270)^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_10313m_11m_energy +Title=$e^+$ energy in the decay $D^+\to \bar{K}_1(1270)^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_10313m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D^+\to \bar{K}_1(1270)^0 e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_313p_13p_energy +Title=$\mu^-$ energy in the decay $D^-\to K^{*0} \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_313p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^-\to K^{*0} \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_313p_11p_energy +Title=$e^-$ energy in the decay $D^-\to K^{*0} e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_313p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^-\to K^{*0} e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_313m_13m_energy +Title=$\mu^+$ energy in the decay $D^+\to \bar{K}^{*0} \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_313m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D^+\to \bar{K}^{*0} \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_313m_11m_energy +Title=$e^+$ energy in the decay $D^+\to \bar{K}^{*0} e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_313m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D^+\to \bar{K}^{*0} e^+\nu_e$ +END PLOT + + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_311p_13p_energy +Title=$\mu^-$ energy in the decay $D^-\to K^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_311p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^-\to K^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_311p_11p_energy +Title=$e^-$ energy in the decay $D^-\to K^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_311p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^-\to K^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_311m_13m_energy +Title=$\mu^+$ energy in the decay $D^+\to \bar{K}^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_311m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D^+\to \bar{K}^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_311m_11m_energy +Title=$e^+$ energy in the decay $D^+\to \bar{K}^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_311m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D^+\to \bar{K}^0 e^+\nu_e$ +END PLOT + + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_111p_13p_energy +Title=$\mu^-$ energy in the decay $D^-\to \pi^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_111p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^-\to \pi^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_111p_11p_energy +Title=$e^-$ energy in the decay $D^-\to \pi^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_111p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^-\to \pi^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_111p_13m_energy +Title=$\mu^+$ energy in the decay $D^+\to \pi^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_111p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D^+\to \pi^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_111p_11m_energy +Title=$e^+$ energy in the decay $D^+\to \pi^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_111p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D^+\to \pi^0 e^+\nu_e$ +END PLOT + + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_221p_13p_energy +Title=$\mu^-$ energy in the decay $D^-\to \eta \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_221p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^-\to \eta \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_221p_11p_energy +Title=$e^-$ energy in the decay $D^-\to \eta e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_221p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^-\to \eta e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_221p_13m_energy +Title=$\mu^+$ energy in the decay $D^+\to \eta \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_221p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D^+\to \eta \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_221p_11m_energy +Title=$e^+$ energy in the decay $D^+\to \eta e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_221p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D^+\to \eta e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_223p_13p_energy +Title=$\mu^-$ energy in the decay $D^-\to \omega \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_223p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^-\to \omega \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_223p_11p_energy +Title=$e^-$ energy in the decay $D^-\to \omega e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_223p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^-\to \omega e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_223p_13m_energy +Title=$\mu^+$ energy in the decay $D^+\to \omega \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_223p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D^+\to \omega \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_223p_11m_energy +Title=$e^+$ energy in the decay $D^+\to \omega e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_223p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D^+\to \omega e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_113p_13p_energy +Title=$\mu^-$ energy in the decay $D^-\to \rho^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_113p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^-\to \rho^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_113p_11p_energy +Title=$e^-$ energy in the decay $D^-\to \rho^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411m_113p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^-\to \rho^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_113p_13m_energy +Title=$\mu^+$ energy in the decay $D^+\to \rho^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_113p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D^+\to \rho^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_113p_11m_energy +Title=$e^+$ energy in the decay $D^+\to \rho^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_411p_113p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D^+\to \rho^0 e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_10323p_13p_energy +Title=$\mu^-$ energy in the decay $D^0\to K_1(1270)^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_10323p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^0\to K_1(1270)^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_10323p_11p_energy +Title=$e^-$ energy in the decay $D^0\to K_1(1270)^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_10323p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^0\to K_1(1270)^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_10323m_13m_energy +Title=$\mu^+$ energy in the decay $\bar{D}^0\to K_1(1270)^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_10323m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $\bar{D}^0\to K_1(1270)^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_10323m_11m_energy +Title=$e^+$ energy in the decay $\bar{D}^0\to K_1(1270)^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_10323m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $\bar{D}^0\to K_1(1270)^- e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_323p_13p_energy +Title=$\mu^-$ energy in the decay $D^0\to K^{*+} \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_323p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^0\to K^{*+} \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_323p_11p_energy +Title=$e^-$ energy in the decay $D^0\to K^{*+} e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_323p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^0\to K^{*+} e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_323m_13m_energy +Title=$\mu^+$ energy in the decay $\bar{D}^0\to K^{*-} \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_323m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $\bar{D}^0\to K^{*-} \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_323m_11m_energy +Title=$e^+$ energy in the decay $\bar{D}^0\to K^{*-} e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_323m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $\bar{D}^0\to K^{*-} e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_321p_13p_energy +Title=$\mu^-$ energy in the decay $D^0\to K^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_321p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^0\to K^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_321p_11p_energy +Title=$e^-$ energy in the decay $D^0\to K^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_321p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^0\to K^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_321m_13m_energy +Title=$\mu^+$ energy in the decay $\bar{D}^0\to K^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_321m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $\bar{D}^0\to K^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_321m_11m_energy +Title=$e^+$ energy in the decay $\bar{D}^0\to K^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_321m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $\bar{D}^0\to K^- e^+\nu_e$ +END PLOT + + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_211p_13p_energy +Title=$\mu^-$ energy in the decay $D^0\to \pi^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_211p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^0\to \pi^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_211p_11p_energy +Title=$e^-$ energy in the decay $D^0\to \pi^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_211p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^0\to \pi^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_211m_13m_energy +Title=$\mu^+$ energy in the decay $\bar{D}^0\to \pi^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_211m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $\bar{D}^0\to \pi^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_211m_11m_energy +Title=$e^+$ energy in the decay $\bar{D}^0\to \pi^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_211m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $\bar{D}^0\to \pi^- e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_213p_13p_energy +Title=$\mu^-$ energy in the decay $D^0\to \rho^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_213p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D^0\to \rho^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_213p_11p_energy +Title=$e^-$ energy in the decay $D^0\to \rho^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421m_213p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D^0\to \rho^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_213m_13m_energy +Title=$\mu^+$ energy in the decay $\bar{D}^0\to \rho^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_213m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $\bar{D}^0\to \rho^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_213m_11m_energy +Title=$e^+$ energy in the decay $\bar{D}^0\to \rho^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_421p_213m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $\bar{D}^0\to \rho^- e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_311m_13p_energy +Title=$\mu^-$ energy in the decay $D_s^-\to \bar{K}^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_311m_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D_s^-\to \bar{K}^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_311m_11p_energy +Title=$e^-$ energy in the decay $D_s^-\to \bar{K}^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_311m_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D_s^-\to \bar{K}^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_311p_13m_energy +Title=$\mu^+$ energy in the decay $D_s^+\to K^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_311p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D_s^+\to K^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_311p_11m_energy +Title=$e^+$ energy in the decay $D_s^+\to K^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_311p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D_s^+\to K^0 e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_313m_13p_energy +Title=$\mu^-$ energy in the decay $D_s^-\to \bar{K}^{*0} \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_313m_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D_s^-\to \bar{K}^{*0} \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_313m_11p_energy +Title=$e^-$ energy in the decay $D_s^-\to \bar{K}^{*0} e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_313m_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D_s^-\to \bar{K}^{*0} e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_313p_13m_energy +Title=$\mu^+$ energy in the decay $D_s^+\to K^{*0} \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_313p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D_s^+\to K^{*0} \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_313p_11m_energy +Title=$e^+$ energy in the decay $D_s^+\to K^{*0} e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_313p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D_s^+\to K^{*0} e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_221p_13p_energy +Title=$\mu^-$ energy in the decay $D_s^-\to \eta \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_221p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D_s^-\to \eta \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_221p_11p_energy +Title=$e^-$ energy in the decay $D_s^-\to \eta e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_221p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D_s^-\to \eta e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_221p_13m_energy +Title=$\mu^+$ energy in the decay $D_s^+\to \eta \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_221p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D_s^+\to \eta \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_221p_11m_energy +Title=$e^+$ energy in the decay $D_s^+\to \eta e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_221p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D_s^+\to \eta e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_331p_13p_energy +Title=$\mu^-$ energy in the decay $D_s^-\to \eta^\prime \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_331p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D_s^-\to \eta^\prime \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_331p_11p_energy +Title=$e^-$ energy in the decay $D_s^-\to \eta^\prime e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_331p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D_s^-\to \eta^\prime e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_331p_13m_energy +Title=$\mu^+$ energy in the decay $D_s^+\to \eta^\prime \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_331p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D_s^+\to \eta^\prime \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_331p_11m_energy +Title=$e^+$ energy in the decay $D_s^+\to \eta^\prime e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_331p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D_s^+\to \eta^\prime e^+\nu_e$ +END PLOT + + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_223p_13p_energy +Title=$\mu^-$ energy in the decay $D_s^-\to \omega \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_223p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D_s^-\to \omega \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_223p_11p_energy +Title=$e^-$ energy in the decay $D_s^-\to \omega e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_223p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D_s^-\to \omega e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_223p_13m_energy +Title=$\mu^+$ energy in the decay $D_s^+\to \omega \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_223p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D_s^+\to \omega \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_223p_11m_energy +Title=$e^+$ energy in the decay $D_s^+\to \omega e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_223p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D_s^+\to \omega e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_333p_13p_energy +Title=$\mu^-$ energy in the decay $D_s^-\to \phi \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_333p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $D_s^-\to \phi \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_333p_11p_energy +Title=$e^-$ energy in the decay $D_s^-\to \phi e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431m_333p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $D_s^-\to \phi e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_333p_13m_energy +Title=$\mu^+$ energy in the decay $D_s^+\to \phi \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_333p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $D_s^+\to \phi \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_333p_11m_energy +Title=$e^+$ energy in the decay $D_s^+\to \phi e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_431p_333p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $D_s^+\to \phi e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_10411p_13p_energy +Title=$\mu^-$ energy in the decay $\bar{B}^0\to D^*_0(2400)^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_10411p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $\bar{B}^0\to D^*_0(2400)^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_10411p_11p_energy +Title=$e^-$ energy in the decay $\bar{B}^0\to D^*_0(2400)^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_10411p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $\bar{B}^0\to D^*_0(2400)^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_10411m_13m_energy +Title=$\mu^+$ energy in the decay $B^0\to D^*_0(2400)^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_10411m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^0\to D^*_0(2400)^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_10411m_11m_energy +Title=$e^+$ energy in the decay $B^0\to D^*_0(2400)^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_10411m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^0\to D^*_0(2400)^- e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_20413p_13p_energy +Title=$\mu^-$ energy in the decay $\bar{B}^0\to D_1(2430)^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_20413p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $\bar{B}^0\to D_1(2430)^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_20413p_11p_energy +Title=$e^-$ energy in the decay $\bar{B}^0\to D_1(2430)^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_20413p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $\bar{B}^0\to D_1(2430)^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_20413m_13m_energy +Title=$\mu^+$ energy in the decay $B^0\to D_1(2430)^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_20413m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^0\to D_1(2430)^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_20413m_11m_energy +Title=$e^+$ energy in the decay $B^0\to D_1(2430)^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_20413m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^0\to D_1(2430)^- e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_10413p_13p_energy +Title=$\mu^-$ energy in the decay $\bar{B}^0\to D_1(2420)^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_10413p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $\bar{B}^0\to D_1(2420)^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_10413p_11p_energy +Title=$e^-$ energy in the decay $\bar{B}^0\to D_1(2420)^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_10413p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $\bar{B}^0\to D_1(2420)^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_10413m_13m_energy +Title=$\mu^+$ energy in the decay $B^0\to D_1(2420)^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_10413m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^0\to D_1(2420)^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_10413m_11m_energy +Title=$e^+$ energy in the decay $B^0\to D_1(2420)^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_10413m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^0\to D_1(2420)^- e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_411p_13p_energy +Title=$\mu^-$ energy in the decay $\bar{B}^0\to D^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_411p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $\bar{B}^0\to D^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_411p_11p_energy +Title=$e^-$ energy in the decay $\bar{B}^0\to D^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_411p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $\bar{B}^0\to D^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_411m_13m_energy +Title=$\mu^+$ energy in the decay $B^0\to D^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_411m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^0\to D^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_411m_11m_energy +Title=$e^+$ energy in the decay $B^0\to D^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_411m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^0\to D^- e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_415p_13p_energy +Title=$\mu^-$ energy in the decay $\bar{B}^0\to D_2^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_415p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $\bar{B}^0\to D_2^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_415p_11p_energy +Title=$e^-$ energy in the decay $\bar{B}^0\to D_2^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_415p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $\bar{B}^0\to D_2^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_415m_13m_energy +Title=$\mu^+$ energy in the decay $B^0\to D_2^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_415m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^0\to D_2^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_415m_11m_energy +Title=$e^+$ energy in the decay $B^0\to D_2^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_415m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^0\to D_2^- e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_413p_13p_energy +Title=$\mu^-$ energy in the decay $\bar{B}^0\to D^{*+} \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_413p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $\bar{B}^0\to D^{*+} \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_413p_11p_energy +Title=$e^-$ energy in the decay $\bar{B}^0\to D^{*+} e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_413p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $\bar{B}^0\to D^{*+} e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_413m_13m_energy +Title=$\mu^+$ energy in the decay $B^0\to D^{*-} \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_413m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^0\to D^{*-} \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_413m_11m_energy +Title=$e^+$ energy in the decay $B^0\to D^{*-} e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_413m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^0\to D^{*-} e^+\nu_e$ +END PLOT + + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_211p_13p_energy +Title=$\mu^-$ energy in the decay $\bar{B}^0\to \pi^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_211p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $\bar{B}^0\to \pi^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_211p_11p_energy +Title=$e^-$ energy in the decay $\bar{B}^0\to \pi^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_211p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $\bar{B}^0\to \pi^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_211m_13m_energy +Title=$\mu^+$ energy in the decay $B^0\to \pi^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_211m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^0\to \pi^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_211m_11m_energy +Title=$e^+$ energy in the decay $B^0\to \pi^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_211m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^0\to \pi^- e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_213p_13p_energy +Title=$\mu^-$ energy in the decay $\bar{B}^0\to \rho^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_213p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $\bar{B}^0\to \rho^+ \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_213p_11p_energy +Title=$e^-$ energy in the decay $\bar{B}^0\to \rho^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511m_213p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $\bar{B}^0\to \rho^+ e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_213m_13m_energy +Title=$\mu^+$ energy in the decay $B^0\to \rho^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_213m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^0\to \rho^- \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_213m_11m_energy +Title=$e^+$ energy in the decay $B^0\to \rho^- e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_511p_213m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^0\to \rho^- e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_10421p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to D^*_0(2400)^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_10421p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to D^*_0(2400)^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_10421p_11p_energy +Title=$e^-$ energy in the decay $B^-\to D^*_0(2400)^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_10421p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to D^*_0(2400)^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_10421m_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \bar{D}^*_0(2400)^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_10421m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \bar{D}^*_0(2400)^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_10421m_11m_energy +Title=$e^+$ energy in the decay $B^+\to \bar{D}^*_0(2400)^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_10421m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \bar{D}^*_0(2400)^0 e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_10423p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to D_1(2420)^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_10423p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to D_1(2420)^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_10423p_11p_energy +Title=$e^-$ energy in the decay $B^-\to D_1(2420)^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_10423p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to D_1(2420)^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_10423m_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \bar{D}_1(2420)^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_10423m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \bar{D}_1(2420)^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_10423m_11m_energy +Title=$e^+$ energy in the decay $B^+\to \bar{D}_1(2420)^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_10423m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \bar{D}_1(2420)^0 e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_20423p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to D_1(2430)^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_20423p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to D_1(2430)^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_20423p_11p_energy +Title=$e^-$ energy in the decay $B^-\to D_1(2430)^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_20423p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to D_1(2430)^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_20423m_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \bar{D}_1(2430)^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_20423m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \bar{D}_1(2430)^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_20423m_11m_energy +Title=$e^+$ energy in the decay $B^+\to \bar{D}_1(2430)^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_20423m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \bar{D}_1(2430)^0 e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_421p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to D^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_421p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to D^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_421p_11p_energy +Title=$e^-$ energy in the decay $B^-\to D^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_421p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to D^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_421m_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \bar{D}^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_421m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \bar{D}^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_421m_11m_energy +Title=$e^+$ energy in the decay $B^+\to \bar{D}^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_421m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \bar{D}^0 e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_425p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to D_2^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_425p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to D_2^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_425p_11p_energy +Title=$e^-$ energy in the decay $B^-\to D_2^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_425p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to D_2^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_425m_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \bar{D}_2^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_425m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \bar{D}_2^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_425m_11m_energy +Title=$e^+$ energy in the decay $B^+\to \bar{D}_2^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_425m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \bar{D}_2^0 e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_423p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to D^{*0} \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_423p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to D^{*0} \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_423p_11p_energy +Title=$e^-$ energy in the decay $B^-\to D^{*0} e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_423p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to D^{*0} e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_423m_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \bar{D}^{*0} \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_423m_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \bar{D}^{*0} \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_423m_11m_energy +Title=$e^+$ energy in the decay $B^+\to \bar{D}^{*0} e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_423m_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \bar{D}^{*0} e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_113p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to \rho^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_113p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to \rho^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_113p_11p_energy +Title=$e^-$ energy in the decay $B^-\to \rho^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_113p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to \rho^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_113p_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \rho^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_113p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \rho^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_113p_11m_energy +Title=$e^+$ energy in the decay $B^+\to \rho^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_113p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \rho^0 e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_223p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to \omega \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_223p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to \omega \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_223p_11p_energy +Title=$e^-$ energy in the decay $B^-\to \omega e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_223p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to \omega e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_223p_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \omega \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_223p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \omega \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_223p_11m_energy +Title=$e^+$ energy in the decay $B^+\to \omega e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_223p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \omega e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_111p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to \pi^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_111p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to \pi^0 \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_111p_11p_energy +Title=$e^-$ energy in the decay $B^-\to \pi^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_111p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to \pi^0 e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_111p_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \pi^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_111p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \pi^0 \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_111p_11m_energy +Title=$e^+$ energy in the decay $B^+\to \pi^0 e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_111p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \pi^0 e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_221p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to \eta \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_221p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to \eta \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_221p_11p_energy +Title=$e^-$ energy in the decay $B^-\to \eta e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_221p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to \eta e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_221p_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \eta \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_221p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \eta \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_221p_11m_energy +Title=$e^+$ energy in the decay $B^+\to \eta e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_221p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \eta e^+\nu_e$ +END PLOT + +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_331p_13p_energy +Title=$\mu^-$ energy in the decay $B^-\to \eta^\prime \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_331p_13p_scale +Title=Mass of $\mu^-\bar\nu_\mu$ in the decay $B^-\to \eta^\prime \mu^-\bar\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_331p_11p_energy +Title=$e^-$ energy in the decay $B^-\to \eta^\prime e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521m_331p_11p_scale +Title=Mass of $e^-\bar\nu_e$ in the decay $B^-\to \eta^\prime e^-\bar\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_331p_13m_energy +Title=$\mu^+$ energy in the decay $B^+\to \eta^\prime \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_331p_13m_scale +Title=Mass of $\mu^+\nu_\mu$ in the decay $B^+\to \eta^\prime \mu^+\nu_\mu$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_331p_11m_energy +Title=$e^+$ energy in the decay $B^+\to \eta^\prime e^+\nu_e$ +END PLOT +BEGIN PLOT /MC_Semi_Leptonic_Decay/h_521p_331p_11m_scale +Title=Mass of $e^+\nu_e$ in the decay $B^+\to \eta^\prime e^+\nu_e$ +END PLOT diff --git a/analyses/pluginMC/MC_TAU_Decay.cc b/analyses/pluginMC/MC_TAU_Decay.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_TAU_Decay.cc @@ -0,0 +1,645 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/FastJets.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MC_TAU_Decay : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MC_TAU_Decay); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(),"UFS"); + + // Book histograms + // leptonic + _h_2B_m2enu=bookHisto1D("h_2B_m2enu", 200,0.,3.15); + _h_2B_menu =bookHisto1D("h_2B_menu" , 200,0.,1.8 ); + // hadronic + // 2 hadrons + _h_2B_m2pipi=bookHisto1D("h_2B_m2pipi", 200,0.,3.15); + _h_2B_mpipi =bookHisto1D("h_2B_mpipi" , 200,0.,1.8 ); + _h_2B_m2munu=bookHisto1D("h_2B_m2munu", 200,0.,3.15); + _h_2B_mmunu =bookHisto1D("h_2B_mmunu" , 200,0.,1.8 ); + _h_2B_m2KpiA=bookHisto1D("h_2B_m2KpiA", 200,0.,3.15); + _h_2B_mKpiA =bookHisto1D("h_2B_mKpiA" , 200,0.,1.8 ); + _h_2B_m2KpiB=bookHisto1D("h_2B_m2KpiB", 200,0.,3.15); + _h_2B_mKpiB =bookHisto1D("h_2B_mKpiB" , 200,0.,1.8 ); + _h_2B_m2Keta=bookHisto1D("h_2B_m2Keta", 200,0.,3.15); + _h_2B_mKeta =bookHisto1D("h_2B_mKeta" , 200,0.,1.8 ); + _h_2B_m2KK =bookHisto1D("h_2B_m2KK" , 200,0.,3.15); + _h_2B_mKK =bookHisto1D("h_2B_mKK" , 200,0.,1.8 ); + // 3 hadrons + for(unsigned int ix=0;ix<4;++ix) { + if(ix<3) { + ostringstream title1 ; title1 << "h_3B_pippimpim_" << ix+1; + _h_3B_pippimpim .push_back(bookHisto1D(title1 .str(),200,0.,1.8)); + ostringstream title2 ; title2 << "h_3B_pi0pi0pim_" << ix+1; + _h_3B_pi0pi0pim .push_back(bookHisto1D(title2 .str(),200,0.,1.8)); + ostringstream title5 ; title5 << "h_3B_pi0pi0km_" << ix+1; + _h_3B_pi0pi0km .push_back(bookHisto1D(title5 .str(),200,0.,1.8)); + ostringstream title10; title10 << "h_3B_kspimks_" << ix+1; + _h_3B_kspimks .push_back(bookHisto1D(title10.str(),200,0.,1.8)); + ostringstream title11; title11 << "h_3B_klpimkl_" << ix+1; + _h_3B_klpimkl .push_back(bookHisto1D(title11.str(),200,0.,1.8)); + } + ostringstream title3 ; title3 << "h_3B_kmpimkp_" << ix+1; + _h_3B_kmpimkp .push_back(bookHisto1D(title3 .str(),200,0.,1.8)); + ostringstream title4 ; title4 << "h_3B_kmpi0k0_" << ix+1; + _h_3B_kmpi0k0 .push_back(bookHisto1D(title4 .str(),200,0.,1.8)); + ostringstream title6 ; title6 << "h_3B_kmpimpip_" << ix+1; + _h_3B_kmpimpip .push_back(bookHisto1D(title6 .str(),200,0.,1.8)); + ostringstream title7 ; title7 << "h_3B_pimk0pi0_" << ix+1; + _h_3B_pimk0pi0 .push_back(bookHisto1D(title7 .str(),200,0.,1.8)); + ostringstream title8 ; title8 << "h_3B_pimpi0eta_" << ix+1; + _h_3B_pimpi0eta .push_back(bookHisto1D(title8 .str(),200,0.,1.8)); + ostringstream title9 ; title9 << "h_3B_pimpi0gamma_" << ix+1; + _h_3B_pimpi0gamma .push_back(bookHisto1D(title9 .str(),200,0.,1.8)); + ostringstream title12; title12 << "h_3B_kspimkl_" << ix+1; + _h_3B_kspimkl .push_back(bookHisto1D(title12.str(),200,0.,1.8)); + } + // 4 pion decays + for(unsigned int ix=0;ix<5;++ix) { + ostringstream title1 ; title1 << "h_4B_pipi_" << ix+1; + _h_4B_pipi .push_back(bookHisto1D(title1.str(),200,0.,1.8)); + ostringstream title2 ; title2 << "h_4B_pipipi_" << ix+1; + _h_4B_pipipi.push_back(bookHisto1D(title2.str(),200,0.,1.8)); + } + _h_4B_pipi .push_back(bookHisto1D("h_4B_pipi_6",200,0.,1.8)); + for(unsigned int ix=0;ix<2;++ix) { + ostringstream title ; title << "h_4B_pipipipi_" << ix+1; + _h_4B_pipipipi.push_back(bookHisto1D(title.str(),200,0.,1.8)); + } + // 5 pion decays + // 2 pi0 2pi- pi+ + _h_5B_q1 = bookHisto1D("h_5B_q1",200,0.,1.8); + for(unsigned int ix=0;ix<5;++ix) { + ostringstream title; + title << "h_5B_pipi1_" << ix+1; + _h_5B_pipi1.push_back(bookHisto1D(title.str(), 200,0.,1.8 )); + } + for(unsigned int ix=0;ix<5;++ix) { + ostringstream title; + title << "h_5B_pipipi1_" << ix+1; + _h_5B_pipipi1.push_back(bookHisto1D(title.str(), 200,0.,1.8 )); + } + for(unsigned int ix=0;ix<3;++ix) { + ostringstream title; + title << "h_5B_pipipipi1_" << ix+1; + _h_5B_pipipipi1.push_back(bookHisto1D(title.str(), 200,0.,1.8 )); + } + // 4 pi0 pi- + _h_5B_q2 = bookHisto1D("h_5B_q2",200,0.,1.8); + for(unsigned int ix=0;ix<2;++ix) { + ostringstream title; + title << "h_5B_pipi2_" << ix+1; + _h_5B_pipi2.push_back(bookHisto1D(title.str(), 200,0.,1.8 )); + } + for(unsigned int ix=0;ix<2;++ix) { + ostringstream title; + title << "h_5B_pipipi2_" << ix+1; + _h_5B_pipipi2.push_back(bookHisto1D(title.str(), 200,0.,1.8 )); + } + for(unsigned int ix=0;ix<2;++ix) { + ostringstream title; + title << "h_5B_pipipipi2_" << ix+1; + _h_5B_pipipipi2.push_back(bookHisto1D(title.str(), 200,0.,1.8 )); + } + // 3 pi- 2 pi+ + _h_5B_q3 = bookHisto1D("h_5B_q3",200,0.,1.8); + for(unsigned int ix=0;ix<3;++ix) { + ostringstream title; + title << "h_5B_pipi3_" << ix+1; + _h_5B_pipi3.push_back(bookHisto1D(title.str(), 200,0.,1.8 )); + } + for(unsigned int ix=0;ix<3;++ix) { + ostringstream title; + title << "h_5B_pipipi3_" << ix+1; + _h_5B_pipipi3.push_back(bookHisto1D(title.str(), 200,0.,1.8 )); + } + for(unsigned int ix=0;ix<2;++ix) { + ostringstream title; + title << "h_5B_pipipipi3_" << ix+1; + _h_5B_pipipipi3.push_back(bookHisto1D(title.str(), 200,0.,1.8 )); + } + } + + void findDecayProducts(const Particle & mother, unsigned int & nstable, + Particles & ep , Particles & em , Particles & nu_e , Particles & nu_ebar, + Particles & mup , Particles & mum , Particles & nu_mu, Particles & nu_mubar, + Particles & pip , Particles & pim , Particles & pi0 , + Particles & Kp , Particles & Km , Particles & K0S , Particles & K0L, + Particles & eta , Particles & gamma) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if ( id == PID::KPLUS ) { + Kp.push_back(p); + ++nstable; + } + else if (id == PID::KMINUS ) { + Km.push_back(p); + ++nstable; + } + else if (id == PID::PIPLUS) { + pip.push_back(p); + ++nstable; + } + else if (id == PID::PIMINUS) { + pim.push_back(p); + ++nstable; + } + else if (id == PID::EPLUS) { + ep.push_back(p); + ++nstable; + } + else if (id == PID::EMINUS) { + em.push_back(p); + ++nstable; + } + else if (id == PID::NU_E) { + nu_e.push_back(p); + ++nstable; + } + else if (id == PID::NU_EBAR) { + nu_ebar.push_back(p); + ++nstable; + } + else if (id == PID::NU_MU) { + nu_mu.push_back(p); + ++nstable; + } + else if (id == PID::NU_MUBAR) { + nu_mubar.push_back(p); + ++nstable; + } + else if (id == PID::ANTIMUON) { + mup.push_back(p); + ++nstable; + } + else if (id == PID::MUON) { + mum.push_back(p); + ++nstable; + } + else if (id == PID::PI0) { + pi0.push_back(p); + ++nstable; + } + else if (id == PID::K0S) { + K0S.push_back(p); + ++nstable; + } + else if (id == PID::K0L) { + K0L.push_back(p); + ++nstable; + } + else if (id == PID::ETA) { + eta.push_back(p); + ++nstable; + } + else if (id == PID::PHOTON) { + gamma.push_back(p); + ++nstable; + } + else if ( !p.children().empty() ) { + findDecayProducts(p, nstable,ep,em,nu_e,nu_ebar,mup,mum,nu_mu,nu_mubar, + pip, pim, pi0,Kp , Km, K0S, K0L,eta,gamma); + } + else + ++nstable; + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + double weight = event.weight(); + for(const Particle& tau : apply(event, "UFS").particles(Cuts::abspid==PID::TAU)) { + unsigned int nstable(0); + Particles ep,em,nu_e,nu_ebar,mup,mum,nu_mu,nu_mubar; + Particles pip, pim, pi0, Kp , Km, K0S, K0L, eta,gamma; + findDecayProducts(tau, nstable,ep,em,nu_e,nu_ebar,mup,mum,nu_mu,nu_mubar, + pip, pim, pi0,Kp , Km, K0S, K0L,eta,gamma); + if(tau.pdgId()<0) { + swap(pim,pip); + swap(Kp,Km); + swap(em,ep); + swap(mum,mup); + swap(nu_e ,nu_ebar ); + swap(nu_mu,nu_mubar); + } + // cerr << "testing before loop " << nstable << " " + // << pip.size() << " " << pim.size() << " " << pi0.size() << " " + // << Kp.size() << " " << Km.size() << " " << K0S.size() << " " << K0L.size() << "\n"; + // 2 hadrons + if(nstable==3 ) { + if(em.size()==1 && nu_ebar.size()==1) { + FourMomentum ptot = em[0].momentum()+nu_ebar[0].momentum(); + double mass2 = ptot.mass2(); + _h_2B_m2enu->fill( mass2 ,weight); + _h_2B_menu ->fill(sqrt(mass2),weight); + } + else if(mum.size()==1 && nu_mubar.size()==1) { + FourMomentum ptot = mum[0].momentum()+nu_mubar[0].momentum(); + double mass2 = ptot.mass2(); + _h_2B_m2munu->fill( mass2 ,weight); + _h_2B_mmunu ->fill(sqrt(mass2),weight); + } + else if(pim.size()==1 && pi0.size()==1) { + FourMomentum ptot = pim[0].momentum()+pi0[0].momentum(); + double mass2 = ptot.mass2(); + _h_2B_m2pipi->fill( mass2 ,weight); + _h_2B_mpipi ->fill(sqrt(mass2),weight); + } + else if(Km.size()==1 && pi0.size()==1) { + FourMomentum ptot = Km[0].momentum()+pi0[0].momentum(); + double mass2 = ptot.mass2(); + _h_2B_m2KpiA->fill( mass2 ,weight); + _h_2B_mKpiA ->fill(sqrt(mass2),weight); + } + else if(K0S.size()==1&&pim.size()==1) { + FourMomentum ptot = K0S[0].momentum()+pim[0].momentum(); + double mass2 = ptot.mass2(); + _h_2B_m2KpiB->fill( mass2 ,weight); + _h_2B_mKpiB ->fill(sqrt(mass2),weight); + } + else if(K0L.size()==1&&pim.size()==1) { + FourMomentum ptot = K0L[0].momentum()+pim[0].momentum(); + double mass2 = ptot.mass2(); + _h_2B_m2KpiB->fill( mass2 ,weight); + _h_2B_mKpiB ->fill(sqrt(mass2),weight); + } + else if(K0S.size()==1&&Km.size()==1) { + FourMomentum ptot = K0S[0].momentum()+Km[0].momentum(); + double mass2 = ptot.mass2(); + _h_2B_m2KK->fill( mass2 ,weight); + _h_2B_mKK ->fill(sqrt(mass2),weight); + } + else if(K0L.size()==1&&Km.size()==1) { + FourMomentum ptot = K0L[0].momentum()+Km[0].momentum(); + double mass2 = ptot.mass2(); + _h_2B_m2KK->fill( mass2 ,weight); + _h_2B_mKK ->fill(sqrt(mass2),weight); + } + else if(eta.size()==1&&Km.size()==1) { + FourMomentum ptot = eta[0].momentum()+Km[0].momentum(); + double mass2 = ptot.mass2(); + _h_2B_m2Keta->fill( mass2 ,weight); + _h_2B_mKeta ->fill(sqrt(mass2),weight); + } + } + else if(nstable==4) { + if(pim.size()==2&&pip.size()==1) { + _h_3B_pippimpim[0]->fill((pim[0].momentum()+pim[1].momentum()+pip[0].momentum()).mass(),weight); + _h_3B_pippimpim[1]->fill((pim[0].momentum()+pim[1].momentum()).mass(),weight); + _h_3B_pippimpim[2]->fill((pim[0].momentum()+pip[0].momentum()).mass(),weight); + _h_3B_pippimpim[2]->fill((pim[1].momentum()+pip[0].momentum()).mass(),weight); + } + else if(pim.size()==1&&pi0.size()==2) { + _h_3B_pi0pi0pim[0]->fill((pi0[0].momentum()+pi0[1].momentum()+pim[0].momentum()).mass(),weight); + _h_3B_pi0pi0pim[1]->fill((pi0[0].momentum()+pi0[1].momentum()).mass(),weight); + _h_3B_pi0pi0pim[2]->fill((pi0[0].momentum()+pim[0].momentum()).mass(),weight); + _h_3B_pi0pi0pim[2]->fill((pi0[1].momentum()+pim[0].momentum()).mass(),weight); + } + else if(Km.size()==1&&Kp.size()==1&&pim.size()==1) { + _h_3B_kmpimkp[0]->fill((Km[0].momentum()+pim[0].momentum()+Kp[0].momentum()).mass(),weight); + _h_3B_kmpimkp[1]->fill((Km[0].momentum()+pim[0].momentum()).mass(),weight); + _h_3B_kmpimkp[2]->fill((Km[0].momentum()+ Kp[0].momentum()).mass(),weight); + _h_3B_kmpimkp[3]->fill((Kp[0].momentum()+pim[0].momentum()).mass(),weight); + } + else if((K0S.size()==1||K0L.size()==1)&&Km.size()==1&&pi0.size()==1) { + FourMomentum pk = K0L.size()==1 ? K0L[0].momentum() : K0S[0].momentum(); + _h_3B_kmpi0k0[0]->fill((Km[0].momentum()+pi0[0].momentum()+pk).mass(),weight); + _h_3B_kmpi0k0[1]->fill((Km[0].momentum()+pi0[0].momentum()).mass(),weight); + _h_3B_kmpi0k0[2]->fill((Km[0].momentum()+pk ).mass(),weight); + _h_3B_kmpi0k0[3]->fill((pk+pi0[0].momentum()).mass(),weight); + } + else if(pi0.size()==2&&Km.size()==1) { + _h_3B_pi0pi0km[0]->fill((pi0[0].momentum()+pi0[1].momentum()+Km[0].momentum()).mass(),weight); + _h_3B_pi0pi0km[1]->fill((pi0[0].momentum()+pi0[1].momentum()).mass(),weight); + _h_3B_pi0pi0km[2]->fill((pi0[0].momentum()+Km[0].momentum() ).mass(),weight); + _h_3B_pi0pi0km[2]->fill((pi0[1].momentum()+Km[0].momentum() ).mass(),weight); + } + else if(Km.size()==1&&pim.size()==1&&pip.size()==1) { + _h_3B_kmpimpip[0]->fill((pip[0].momentum()+pim[0].momentum()+Km[0].momentum()).mass(),weight); + _h_3B_kmpimpip[1]->fill((Km[0].momentum()+pim[0].momentum()).mass(),weight); + _h_3B_kmpimpip[2]->fill((Km[0].momentum()+pip[0].momentum() ).mass(),weight); + _h_3B_kmpimpip[3]->fill((pip[0].momentum()+pim[0].momentum() ).mass(),weight); + } + else if(pim.size()==1&&(K0S.size()==1||K0L.size()==1)&&pi0.size()==1) { + FourMomentum pk = K0L.size()==1 ? K0L[0].momentum() : K0S[0].momentum(); + _h_3B_pimk0pi0[0]->fill((pim[0].momentum()+pi0[0].momentum()+pk).mass(),weight); + _h_3B_pimk0pi0[1]->fill((pim[0].momentum()+pk).mass(),weight); + _h_3B_pimk0pi0[2]->fill((pim[0].momentum()+pi0[0].momentum() ).mass(),weight); + _h_3B_pimk0pi0[3]->fill((pk+pi0[0].momentum()).mass(),weight); + } + else if(pim.size()==1&&pi0.size()==1&&eta.size()==1) { + _h_3B_pimpi0eta[0]->fill((pim[0].momentum()+pi0[0].momentum()+eta[0].momentum()).mass(),weight); + _h_3B_pimpi0eta[1]->fill((pim[0].momentum()+pi0[0].momentum()).mass(),weight); + _h_3B_pimpi0eta[2]->fill((pim[0].momentum()+eta[0].momentum()).mass(),weight); + _h_3B_pimpi0eta[3]->fill((pi0[0].momentum()+eta[0].momentum()).mass(),weight); + } + else if(pim.size()==1&&pi0.size()==1&&gamma.size()==1) { + _h_3B_pimpi0gamma[0]->fill((pim[0].momentum()+pi0[0].momentum()+gamma[0].momentum()).mass(),weight); + _h_3B_pimpi0gamma[1]->fill((pim[0].momentum()+pi0[0].momentum()).mass(),weight); + _h_3B_pimpi0gamma[2]->fill((pim[0].momentum()+gamma[0].momentum()).mass(),weight); + _h_3B_pimpi0gamma[3]->fill((pi0[0].momentum()+gamma[0].momentum()).mass(),weight); + } + else if(K0S.size()==2&&pim.size()==1) { + _h_3B_kspimks[0]->fill((pim[0].momentum()+K0S[0].momentum()+K0S[1].momentum()).mass(),weight); + _h_3B_kspimks[1]->fill((pim[0].momentum()+K0S[0].momentum()).mass(),weight); + _h_3B_kspimks[1]->fill((pim[0].momentum()+K0S[1].momentum()).mass(),weight); + _h_3B_kspimks[2]->fill((K0S [0].momentum()+K0S[1].momentum()).mass(),weight); + } + else if(K0L.size()==2&&pim.size()==1) { + _h_3B_klpimkl[0]->fill((pim[0].momentum()+K0L[0].momentum()+K0L[1].momentum()).mass(),weight); + _h_3B_klpimkl[1]->fill((pim[0].momentum()+K0L[0].momentum()).mass(),weight); + _h_3B_klpimkl[1]->fill((pim[0].momentum()+K0L[1].momentum()).mass(),weight); + _h_3B_klpimkl[2]->fill((K0L [0].momentum()+K0L[1].momentum()).mass(),weight); + } + else if(K0S.size()==1&&K0L.size()==1&&pim.size()==1) { + _h_3B_kspimkl[0]->fill((pim[0].momentum()+K0S[0].momentum()+K0L[0].momentum()).mass(),weight); + _h_3B_kspimkl[1]->fill((pim[0].momentum()+K0S[0].momentum()).mass(),weight); + _h_3B_kspimkl[2]->fill((K0S[0].momentum() +K0L[0].momentum()).mass(),weight); + _h_3B_kspimkl[3]->fill((pim[0].momentum()+K0L[0].momentum()).mass(),weight); + } + } + else if(nstable==5) { + if(pi0.size()==3&&pim.size()==1) { + _h_4B_pipi[0] ->fill( (pi0[0].momentum()+pim[0].momentum()).mass(),weight); + _h_4B_pipi[0] ->fill( (pi0[1].momentum()+pim[0].momentum()).mass(),weight); + _h_4B_pipi[0] ->fill( (pi0[2].momentum()+pim[0].momentum()).mass(),weight); + _h_4B_pipi[1] ->fill( (pi0[0].momentum()+pi0[1].momentum()).mass(),weight); + _h_4B_pipi[1] ->fill( (pi0[0].momentum()+pi0[2].momentum()).mass(),weight); + _h_4B_pipi[1] ->fill( (pi0[1].momentum()+pi0[2].momentum()).mass(),weight); + _h_4B_pipipi[0] ->fill( (pi0[0].momentum()+pi0[1].momentum()+pi0[2].momentum()).mass(),weight); + _h_4B_pipipi[1] ->fill( (pi0[0].momentum()+pi0[1].momentum()+pim[0].momentum()).mass(),weight); + _h_4B_pipipi[1] ->fill( (pi0[0].momentum()+pi0[2].momentum()+pim[0].momentum()).mass(),weight); + _h_4B_pipipi[1] ->fill( (pi0[1].momentum()+pi0[2].momentum()+pim[0].momentum()).mass(),weight); + _h_4B_pipipipi[0] ->fill( (pi0[0].momentum()+pi0[1].momentum()+pi0[2].momentum()+pim[0].momentum()).mass(),weight); + } + else if(pi0.size()==1&&pip.size()==1&&pim.size()==2) { + _h_4B_pipi[2] ->fill((pi0[0].momentum()+pip[0].momentum()).mass(),weight); + _h_4B_pipi[3] ->fill((pi0[0].momentum()+pim[0].momentum()).mass(),weight); + _h_4B_pipi[3] ->fill((pi0[0].momentum()+pim[1].momentum()).mass(),weight); + _h_4B_pipi[4] ->fill((pip[0].momentum()+pim[0].momentum()).mass(),weight); + _h_4B_pipi[4] ->fill((pip[0].momentum()+pim[1].momentum()).mass(),weight); + _h_4B_pipi[5] ->fill((pim[0].momentum()+pim[1].momentum()).mass(),weight); + _h_4B_pipipi[2] ->fill( (pi0[0].momentum()+pip[0].momentum()+pim[0].momentum()).mass(),weight); + _h_4B_pipipi[2] ->fill( (pi0[0].momentum()+pip[0].momentum()+pim[1].momentum()).mass(),weight); + _h_4B_pipipi[3] ->fill( (pip[0].momentum()+pim[0].momentum()+pim[1].momentum()).mass(),weight); + _h_4B_pipipi[4] ->fill( (pi0[0].momentum()+pim[0].momentum()+pim[1].momentum()).mass(),weight); + _h_4B_pipipipi[1] ->fill( (pi0[0].momentum()+pip[0].momentum()+pim[0].momentum()+pim[1].momentum()).mass(),weight); + } + } + else if(nstable==6) { + // 2 pi0 2pi- pi+ + if(pi0.size()==2&&pim.size()==2&&pip.size()==1) { + FourMomentum ptotal = pim[0].momentum()+pim[1].momentum()+ + pip[0].momentum()+pi0[0].momentum()+pi0[1].momentum(); + _h_5B_pipi1[0]->fill((pim[0].momentum()+pim[1].momentum()).mass(),weight); + _h_5B_pipi1[1]->fill((pim[0].momentum()+pip[0].momentum()).mass(),weight); + _h_5B_pipi1[1]->fill((pim[1].momentum()+pip[0].momentum()).mass(),weight); + _h_5B_pipi1[2]->fill((pim[0].momentum()+pi0[0].momentum()).mass(),weight); + _h_5B_pipi1[2]->fill((pim[0].momentum()+pi0[1].momentum()).mass(),weight); + _h_5B_pipi1[2]->fill((pim[1].momentum()+pi0[0].momentum()).mass(),weight); + _h_5B_pipi1[2]->fill((pim[1].momentum()+pi0[1].momentum()).mass(),weight); + _h_5B_pipi1[3]->fill((pip[0].momentum()+pi0[0].momentum()).mass(),weight); + _h_5B_pipi1[3]->fill((pip[0].momentum()+pi0[1].momentum()).mass(),weight); + _h_5B_pipi1[4]->fill((pi0[0].momentum()+pi0[1].momentum()).mass(),weight); + _h_5B_pipipi1[0]->fill((pim[0].momentum()+pim[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi1[1]->fill((pim[0].momentum()+pip[0].momentum()-ptotal).mass(),weight); + _h_5B_pipipi1[1]->fill((pim[1].momentum()+pip[0].momentum()-ptotal).mass(),weight); + _h_5B_pipipi1[2]->fill((pim[0].momentum()+pi0[0].momentum()-ptotal).mass(),weight); + _h_5B_pipipi1[2]->fill((pim[0].momentum()+pi0[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi1[2]->fill((pim[1].momentum()+pi0[0].momentum()-ptotal).mass(),weight); + _h_5B_pipipi1[2]->fill((pim[1].momentum()+pi0[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi1[3]->fill((pip[0].momentum()+pi0[0].momentum()-ptotal).mass(),weight); + _h_5B_pipipi1[3]->fill((pip[0].momentum()+pi0[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi1[4]->fill((pi0[0].momentum()+pi0[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipipi1[0]->fill((ptotal-pim[0].momentum()).mass(),weight); + _h_5B_pipipipi1[0]->fill((ptotal-pim[1].momentum()).mass(),weight); + _h_5B_pipipipi1[1]->fill((ptotal-pip[0].momentum()).mass(),weight); + _h_5B_pipipipi1[2]->fill((ptotal-pi0[0].momentum()).mass(),weight); + _h_5B_pipipipi1[2]->fill((ptotal-pi0[1].momentum()).mass(),weight); + _h_5B_q1->fill(ptotal.mass(),weight); + } + // 4 pi0 pi- + else if(pi0.size()==4&&pim.size()==1) { + FourMomentum ptotal = pi0[0].momentum()+pi0[1].momentum()+pi0[2].momentum()+ + pi0[3].momentum()+pim[0].momentum(); + _h_5B_pipi2[0]->fill((pim[0].momentum()+pi0[0].momentum()).mass(),weight); + _h_5B_pipi2[0]->fill((pim[0].momentum()+pi0[1].momentum()).mass(),weight); + _h_5B_pipi2[0]->fill((pim[0].momentum()+pi0[2].momentum()).mass(),weight); + _h_5B_pipi2[0]->fill((pim[0].momentum()+pi0[3].momentum()).mass(),weight); + _h_5B_pipi2[1]->fill((pi0[0].momentum()+pi0[1].momentum()).mass(),weight); + _h_5B_pipi2[1]->fill((pi0[0].momentum()+pi0[2].momentum()).mass(),weight); + _h_5B_pipi2[1]->fill((pi0[0].momentum()+pi0[3].momentum()).mass(),weight); + _h_5B_pipi2[1]->fill((pi0[1].momentum()+pi0[2].momentum()).mass(),weight); + _h_5B_pipi2[1]->fill((pi0[1].momentum()+pi0[3].momentum()).mass(),weight); + _h_5B_pipi2[1]->fill((pi0[2].momentum()+pi0[3].momentum()).mass(),weight); + _h_5B_pipipi2[0]->fill((pim[0].momentum()+pi0[0].momentum()-ptotal).mass(),weight); + _h_5B_pipipi2[0]->fill((pim[0].momentum()+pi0[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi2[0]->fill((pim[0].momentum()+pi0[2].momentum()-ptotal).mass(),weight); + _h_5B_pipipi2[0]->fill((pim[0].momentum()+pi0[3].momentum()-ptotal).mass(),weight); + _h_5B_pipipi2[1]->fill((pi0[0].momentum()+pi0[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi2[1]->fill((pi0[0].momentum()+pi0[2].momentum()-ptotal).mass(),weight); + _h_5B_pipipi2[1]->fill((pi0[0].momentum()+pi0[3].momentum()-ptotal).mass(),weight); + _h_5B_pipipi2[1]->fill((pi0[1].momentum()+pi0[2].momentum()-ptotal).mass(),weight); + _h_5B_pipipi2[1]->fill((pi0[1].momentum()+pi0[3].momentum()-ptotal).mass(),weight); + _h_5B_pipipi2[1]->fill((pi0[2].momentum()+pi0[3].momentum()-ptotal).mass(),weight); + _h_5B_pipipipi2[0]->fill((ptotal-pim[0].momentum()).mass(),weight); + _h_5B_pipipipi2[1]->fill((ptotal-pi0[0].momentum()).mass(),weight); + _h_5B_pipipipi2[1]->fill((ptotal-pi0[1].momentum()).mass(),weight); + _h_5B_pipipipi2[1]->fill((ptotal-pi0[2].momentum()).mass(),weight); + _h_5B_pipipipi2[1]->fill((ptotal-pi0[3].momentum()).mass(),weight); + _h_5B_q2->fill(ptotal.mass(),weight); + } + // 3 pi- 2pi+ + else if(pim.size()==3&&pip.size()==2) { + FourMomentum ptotal = pim[0].momentum()+pim[1].momentum()+ + pim[2].momentum()+pip[0].momentum()+pip[1].momentum(); + _h_5B_pipi3[0]->fill((pip[0].momentum()+pip[1].momentum()).mass(),weight); + _h_5B_pipi3[1]->fill((pim[0].momentum()+pip[0].momentum()).mass(),weight); + _h_5B_pipi3[1]->fill((pim[0].momentum()+pip[1].momentum()).mass(),weight); + _h_5B_pipi3[1]->fill((pim[1].momentum()+pip[0].momentum()).mass(),weight); + _h_5B_pipi3[1]->fill((pim[1].momentum()+pip[1].momentum()).mass(),weight); + _h_5B_pipi3[1]->fill((pim[2].momentum()+pip[0].momentum()).mass(),weight); + _h_5B_pipi3[1]->fill((pim[2].momentum()+pip[1].momentum()).mass(),weight); + _h_5B_pipi3[2]->fill((pim[0].momentum()+pim[1].momentum()).mass(),weight); + _h_5B_pipi3[2]->fill((pim[0].momentum()+pim[2].momentum()).mass(),weight); + _h_5B_pipi3[2]->fill((pim[1].momentum()+pim[2].momentum()).mass(),weight); + _h_5B_pipipi3[0]->fill((pip[0].momentum()+pip[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi3[1]->fill((pim[0].momentum()+pip[0].momentum()-ptotal).mass(),weight); + _h_5B_pipipi3[1]->fill((pim[0].momentum()+pip[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi3[1]->fill((pim[1].momentum()+pip[0].momentum()-ptotal).mass(),weight); + _h_5B_pipipi3[1]->fill((pim[1].momentum()+pip[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi3[1]->fill((pim[2].momentum()+pip[0].momentum()-ptotal).mass(),weight); + _h_5B_pipipi3[1]->fill((pim[2].momentum()+pip[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi3[2]->fill((pim[0].momentum()+pim[1].momentum()-ptotal).mass(),weight); + _h_5B_pipipi3[2]->fill((pim[0].momentum()+pim[2].momentum()-ptotal).mass(),weight); + _h_5B_pipipi3[2]->fill((pim[1].momentum()+pim[2].momentum()-ptotal).mass(),weight); + _h_5B_pipipipi3[0]->fill((ptotal-pim[0].momentum()).mass(),weight); + _h_5B_pipipipi3[0]->fill((ptotal-pim[1].momentum()).mass(),weight); + _h_5B_pipipipi3[0]->fill((ptotal-pim[2].momentum()).mass(),weight); + _h_5B_pipipipi3[1]->fill((ptotal-pip[0].momentum()).mass(),weight); + _h_5B_pipipipi3[1]->fill((ptotal-pip[1].momentum()).mass(),weight); + _h_5B_q3->fill(ptotal.mass(),weight); + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + // leptonic + normalize(_h_2B_m2enu); + normalize(_h_2B_menu ); + // 2 hadrons + normalize(_h_2B_m2pipi); + normalize(_h_2B_mpipi ); + normalize(_h_2B_m2munu); + normalize(_h_2B_mmunu ); + normalize(_h_2B_m2KpiA); + normalize(_h_2B_mKpiA ); + normalize(_h_2B_m2KpiB); + normalize(_h_2B_mKpiB ); + normalize(_h_2B_m2Keta); + normalize(_h_2B_mKeta ); + normalize(_h_2B_m2KK ); + normalize(_h_2B_mKK ); + // 3 hadrons + for(unsigned int ix=0;ix<4;++ix) { + if(ix<3) { + normalize(_h_3B_pippimpim [ix]); + normalize(_h_3B_pi0pi0pim [ix]); + normalize(_h_3B_pi0pi0km [ix]); + normalize(_h_3B_kspimks [ix]); + normalize(_h_3B_klpimkl [ix]); + } + normalize(_h_3B_kmpimkp [ix]); + normalize(_h_3B_kmpi0k0 [ix]); + normalize(_h_3B_kmpimpip [ix]); + normalize(_h_3B_pimk0pi0 [ix]); + normalize(_h_3B_pimpi0eta [ix]); + normalize(_h_3B_pimpi0gamma[ix]); + normalize(_h_3B_kspimkl [ix]); + } + // 4 pion decays + for(unsigned int ix=0;ix<5;++ix) { + normalize(_h_4B_pipi [ix]); + normalize(_h_4B_pipipi[ix]); + } + normalize(_h_4B_pipi[5]); + for(unsigned int ix=0;ix<2;++ix) { + normalize(_h_4B_pipipipi[ix]); + } + // 5 pions + normalize(_h_5B_q1); + for(unsigned int ix=0;ix<5;++ix) { + normalize(_h_5B_pipi1); + normalize(_h_5B_pipipi1); + } + for(unsigned int ix=0;ix<3;++ix) { + normalize(_h_5B_pipipipi1); + } + // 4 pi0 pi- + normalize(_h_5B_q2); + for(unsigned int ix=0;ix<2;++ix) { + normalize(_h_5B_pipi2); + normalize(_h_5B_pipipi2); + normalize(_h_5B_pipipipi2); + } + // 3 pi- 2 pi+ + normalize(_h_5B_q3); + for(unsigned int ix=0;ix<3;++ix) { + normalize(_h_5B_pipi3); + normalize(_h_5B_pipipi3); + } + for(unsigned int ix=0;ix<2;++ix) { + normalize(_h_5B_pipipipi3); + } + } + + //@} + + + /// @name Histograms + //@{ + // histograms for leptonic decay + Histo1DPtr _h_2B_m2enu,_h_2B_menu; + Histo1DPtr _h_2B_m2munu,_h_2B_mmunu; + // histograms for 2 hadron decay + Histo1DPtr _h_2B_m2pipi,_h_2B_mpipi; + Histo1DPtr _h_2B_m2KpiA,_h_2B_m2KpiB,_h_2B_mKpiA,_h_2B_mKpiB; + Histo1DPtr _h_2B_m2Keta,_h_2B_mKeta; + Histo1DPtr _h_2B_m2KK,_h_2B_mKK; + // histograms for 3 hadronc decay + // Histograms for tau^- -> nu_tau pi^+pi^-pi^- + vector _h_3B_pippimpim; + //Histograms for tau^- -> nu_tau pi^0pi^0pi^- + vector _h_3B_pi0pi0pim; + // Histograms for tau^- -> nu_tau K^-K^+pi^- + vector _h_3B_kmpimkp; + // Histograms for tau^- -> nu_tau K^-K^0pi^0 + vector _h_3B_kmpi0k0; + // Histograms for tau^- -> nu_tau pi^0pi^0K^- + vector _h_3B_pi0pi0km; + // Histograms for tau^- -> nu_tau K^-pi^-pi^+ + vector _h_3B_kmpimpip; + // Histograms for tau^- -> nu_tau pi^-K^0pi^0 + vector _h_3B_pimk0pi0; + // Histograms for tau^- -> nu_tau pi^-pi^0eta + vector _h_3B_pimpi0eta; + // Histograms for tau^- -> nu_tau pi^-pi^0gamma + vector _h_3B_pimpi0gamma; + // Histograms for tau^- -> nu_tau K^0_SK^0_Spi^- + vector _h_3B_kspimks; + // Histograms for tau^- -> nu_tau K^0_LK^0_Lpi^- + vector _h_3B_klpimkl; + // Histograms for tau^- -> nu_tau K^0_SK^0_Lpi^- + vector _h_3B_kspimkl; + // histograms for 4 pion decay + // Histograms for the pipi mass distributions + vector _h_4B_pipi; + // Histograms for the pipipi mass distributions + vector _h_4B_pipipi; + // Histograms for the pipipipi mass distributions + vector _h_4B_pipipipi; + // histograms for 5 pion decay + // 2 pi0 2 pi- pi+ + Histo1DPtr _h_5B_q1; + vector _h_5B_pipi1; + vector _h_5B_pipipi1; + vector _h_5B_pipipipi1; + // 4 pi0 pi- + Histo1DPtr _h_5B_q2; + vector _h_5B_pipi2; + vector _h_5B_pipipi2; + vector _h_5B_pipipipi2; + // 3 pi- 2 pi+ + Histo1DPtr _h_5B_q3; + vector _h_5B_pipi3; + vector _h_5B_pipipi3; + vector _h_5B_pipipipi3; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MC_TAU_Decay); + + +} diff --git a/analyses/pluginMC/MC_TAU_Decay.info b/analyses/pluginMC/MC_TAU_Decay.info new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_TAU_Decay.info @@ -0,0 +1,20 @@ +Name: MC_TAU_Decay +Summary: Analysis of Kinematic distributions for $\tau$ lepton decays +Status: VALIDATED +Authors: + - Peter Richardson +RunInfo: Any type of process producing tau leptons +NeedCrossSection: no +Description: + 'Simple analysis of kinematic distributions in tau lepton decays. + This includes the mass distribution of the hadronic decay products of the $\tau$ in the 2, 3, 4 and 5 hadron decays. + The two hadron modes included are $\tau^-\to\nu_\tau\{\pi^-\pi^0,K^-\pi^0,K^0\pi^-,K^-\eta,K^-K^0\}$. + The three hadron modes included are $\tau^-\to\nu_\tau \pi^+\pi^-\pi^-$, + $\tau^-\to\nu_\tau \pi^0\pi^0\pi^-$, $\tau^-\to\nu_\tau K^-K^+\pi^-$, + $\tau^-\to\nu_\tau K^0\bar{K}^0\pi^-$, $\tau^-\to\nu_\tau K^-K^0\pi^0$, + $\tau^-\to\nu_\tau \pi^0-\pi^0K^-$,$\tau^-\to\nu_\tau K^-\pi^-\pi^+$, + $\tau^-\to\nu_\tau \pi^-K^0\pi^0$, $\tau^-\to\nu_\tau \pi^-\pi^0\eta$, + $\tau^-\to\nu_\tau \pi^-\pi^0\gamma$. + The mass distributions in the four and five pion decays are included. + The leptonic modes are also included. + Charge conjugate modes are combined. This is based on a number of old Herwig internal analyses.' diff --git a/analyses/pluginMC/MC_TAU_Decay.plot b/analyses/pluginMC/MC_TAU_Decay.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginMC/MC_TAU_Decay.plot @@ -0,0 +1,556 @@ +BEGIN PLOT /MC_TAU_Decay/h_2B_mpipi +Title=Mass distribution of the hadrons for $\tau^-\to\pi^-\pi^0\nu_\tau$ +XLabel=$m_{\pi^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_2B_m2pipi +Title=Mass distribution of the hadrons for $\tau^-\to\pi^-\pi^0\nu_\tau$ +XLabel=$m^2_{\pi^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m^2_{\pi^-\pi^0}$\,$[{\rm GeV}^{-2}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_2B_menu +Title=Mass distribution of the electron/neutrino for $\tau^-\to e^-\bar{\nu}_e\nu_\tau$ +XLabel=$m_{e^-\bar{\nu}_e}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{e^-\bar{\nu}_e}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_2B_m2enu +Title=Mass distribution of the hadrons for $\tau^-\to e^-\bar{\nu}_e\nu_\tau$ +XLabel=$m^2_{e^-\bar{\nu}_e}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m^2_{e^-\bar{\nu}_e}$\,$[{\rm GeV}^{-2}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_2B_m2munu +Title=Mass distribution of the muon/neutrino for $\tau^-\to \mu^-\bar{\nu}_\mu\nu_\tau$ +XLabel=$m_{\mu^-\bar{\nu}_\mu}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\mu^-\bar{\nu}_\mu}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_2B_mmunu +Title=Mass distribution of the hadrons for $\tau^-\to\mu^-\bar{\nu}_\mu\nu_\tau$ +XLabel=$m^2_{\mu^-\bar{\nu}_\mu}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m^2_{\mu^-\bar{\nu}_\mu}$\,$[{\rm GeV}^{-2}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_2B_m2KpiA +Title=Mass distribution of the hadrons for $\tau^-\to K^-\pi^0$ +XLabel=$m_{K^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^-\pi^0}$\,$[{\rm GeV}^{-1}]\nu_\tau$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_2B_mKpiA +Title=Mass distribution of the hadrons for $\tau^-\toK^-\pi^0\nu_\tau$ +XLabel=$m^2_{K^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m^2_{K^-\pi^0}$\,$[{\rm GeV}^{-2}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_2B_m2KpiB +Title=Mass distribution of the hadrons for $\tau^-\to K^0_{S,L}\pi^-\nu_\tau$ +XLabel=$m_{K^0_{S,L}\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^0_{S,L}\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_2B_mKpiB +Title=Mass distribution of the hadrons for $\tau^-\to K^0_{S,L}\pi^-\nu_\tau$ +XLabel=$m^2_{K^0_{S,L}\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m^2_{K^0_{S,L}\pi^-}$\,$[{\rm GeV}^{-2}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_2B_m2Keta +Title=Mass distribution of the hadrons for $\tau^-\to K^-\eta\nu_\tau$ +XLabel=$m_{ K^-\eta}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ K^-\eta}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_2B_mKeta +Title=Mass distribution of the hadrons for $\tau^-\to K^-\eta\nu_\tau$ +XLabel=$m^2_{ K^-\eta}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m^2_{ K^-\eta}$\,$[{\rm GeV}^{-2}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_2B_m2KK +Title=Mass distribution of the hadrons for $\tau^-\to K^0_{S,L}K^-\nu_\tau$ +XLabel=$m_{K^0_{S,L}K^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^0_{S,L}K^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_2B_mKK +Title=Mass distribution of the hadrons for $\tau^-\to K^0_{S,L}K^-\nu_\tau$ +XLabel=$m^2_{K^0_{S,L}K^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m^2_{K^0_{S,L}K^-}$\,$[{\rm GeV}^{-2}]$ +END PLOT + + +BEGIN PLOT /MC_TAU_Decay/h_5B_q1 +Title=Mass distribution of the hadrons for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{2\pi^02\pi^-\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{2\pi^02\pi^-\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_5B_pipi1_1 +Title=Distribution of the $\pi^-\pi^-$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^-\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipi1_2 +Title=Distribution of the $\pi^-\pi^+$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^-\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipi1_3 +Title=Distribution of the $\pi^-\pi^0$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipi1_4 +Title=Distribution of the $\pi^+\pi^0$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^+\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipi1_5 +Title=Distribution of the $\pi^0\pi^0$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^0\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipi1_1 +Title=Distribution of the $\pi^+\pi^0\pi^0$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^+\pi^0\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^0\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipi1_2 +Title=Distribution of the $\pi^-\pi^0\pi^0$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^-\pi^0\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^0\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipi1_3 +Title=Distribution of the $\pi^+\pi^-\pi^0$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^+\pi^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^-\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipi1_4 +Title=Distribution of the $\pi^-\pi^-\pi^0$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^-\pi^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^-\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipi1_5 +Title=Distribution of the $\pi^+\pi^-\pi^-$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^+\pi^-\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^-\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipipi1_1 +Title=Distribution of the $\pi^-\pi^+2\pi^0$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^-\pi^+2\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^+2\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipipi1_2 +Title=Distribution of the $2\pi^-2\pi^0$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{2\pi^-2\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{2\pi^-2\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipipi1_3 +Title=Distribution of the $2\pi^-\pi^+\pi^0$ mass for $\tau^-\to 2\pi^02\pi^-\pi^+\nu_\tau$ +XLabel=$m_{2\pi^-\pi^+\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{2\pi^-\pi^+\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_5B_q2 +Title=Mass distribution of the hadrons for $\tau^-\to 4\pi^0\pi^-\nu_\tau$ +XLabel=$m_{4\pi^0\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{4\pi^0\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_5B_pipi2_1 +Title=Distribution of the $\pi^-\pi^0$ mass for $\tau^-\to 4\pi^0\pi^-\nu_\tau$ +XLabel=$m_{\pi^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipi2_2 +Title=Distribution of the $\pi^0\pi^0$ mass for $\tau^-\to 4\pi^0\pi^-\nu_\tau$ +XLabel=$m_{\pi^0\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipi2_1 +Title=Distribution of the $3\pi^0$ mass for $\tau^-\to 4\pi^0\pi^-\nu_\tau$ +XLabel=$m_{3\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{3\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipi2_2 +Title=Distribution of the $\pi^-2\pi^0$ mass for $\tau^-\to 4\pi^0\pi^-\nu_\tau$ +XLabel=$m_{\pi^-2\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-2\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipipi2_1 +Title=Distribution of the $4\pi^0$ mass for $\tau^-\to 4\pi^0\pi^-\nu_\tau$ +XLabel=$m_{4\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{4\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipipi2_2 +Title=Distribution of the $\pi^-3\pi^0$ mass for $\tau^-\to 4\pi^0\pi^-\nu_\tau$ +XLabel=$m_{\pi^-3\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-3\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_5B_q3 +Title=Mass distribution of the hadrons for $\tau^-\to 3\pi^-2\pi^+\nu_\tau$ +XLabel=$m_{3\pi^-2\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{3\pi^-2\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_5B_pipi3_1 +Title=Distribution of the $\pi^+\pi^+$ mass for $\tau^-\to 3\pi^-2\pi^+\nu_\tau$ +XLabel=$m_{\pi^+\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipi3_2 +Title=Distribution of the $\pi^+\pi^-$ mass for $\tau^-\to 3\pi^-2\pi^+\nu_\tau$ +XLabel=$m_{\pi^+\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipi3_3 +Title=Distribution of the $\pi^-\pi^-$ mass for $\tau^-\to 3\pi^-2\pi^+\nu_\tau$ +XLabel=$m_{\pi^-\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipi3_1 +Title=Distribution of the $3\pi^-$ mass for $\tau^-\to 3\pi^-2\pi^+\nu_\tau$ +XLabel=$m_{3\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{3\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipi3_2 +Title=Distribution of the $2\pi^-\pi^+$ mass for $\tau^-\to 3\pi^-2\pi^+\nu_\tau$ +XLabel=$m_{2\pi^-\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{2\pi^-\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipi3_3 +Title=Distribution of the $\pi^-2\pi^+$ mass for $\tau^-\to 3\pi^-2\pi^+\nu_\tau$ +XLabel=$m_{\pi^-2\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-2\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipipi3_1 +Title=Distribution of the $2\pi^-2\pi^+$ mass for $\tau^-\to 3\pi^-2\pi^+\nu_\tau$ +XLabel=$m_{2\pi^-2\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{2\pi^-2\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_5B_pipipipi3_2 +Title=Distribution of the $3\pi^-\pi^+$ mass for $\tau^-\to 3\pi^-2\pi^+\nu_\tau$ +XLabel=$m_{3\pi^-\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{3\pi^-\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_pippimpim_1 +Title=Distribution of the hadronic mass in $\tau^-\to2\pi^-\pi^+\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{2\pi^-\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{2\pi^-\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pippimpim_2 +Title=Distribution of the $\pi^-\pi^-$ mass in $\tau^-\to2\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^-\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pippimpim_3 +Title=Distribution of the $\pi^-\pi^+$ mass in $\tau^-\to2\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^-\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_pi0pi0pim_1 +Title=Distribution of the hadronic mass in $\tau^-\to2\pi^0\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{2\pi^0\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{2\pi^0\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pi0pi0pim_2 +Title=Distribution of the $\pi^0\pi^0$ mass in $\tau^-\to2\pi^0\pi^-\nu_\tau$ +XLabel=$m_{\pi^0\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pi0pi0pim_3 +Title=Distribution of the $\pi^0\pi^-$ mass in $\tau^-\to2\pi^0\pi^-\nu_\tau$ +XLabel=$m_{\pi^0\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpimkp_1 +Title=Distribution of the hadronic mass in $\tau^-\to K^-\pi^-K^+\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ K^-\pi^-K^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ K^-\pi^-K^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpimkp_2 +Title=Distribution of the $K^-\pi^-$ mass in $\tau^-\to K^-\pi^-K^+\nu_\tau$ +XLabel=$m_{K^-\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^-\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpimkp_3 +Title=Distribution of the $K^-K^+$ mass in $\tau^-\to K^-\pi^-K^+\nu_\tau$ +XLabel=$m_{K^-K^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^-K^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpimkp_4 +Title=Distribution of the $\pi^-K^+$ mass in $\tau^-\to K^-\pi^-K^+\nu_\tau$ +XLabel=$m_{\pi^-K^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-K^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpi0k0_1 +Title=Distribution of the hadronic mass in $\tau^-\to K^-\pi^0K^0\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ K^-\pi^0K^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ K^-\pi^0K^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpi0k0_2 +Title=Distribution of the $K^-\pi^0$ mass in $\tau^-\to K^-\pi^0K^0\nu_\tau$ +XLabel=$m_{K^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^-\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpi0k0_3 +Title=Distribution of the $K^-K^0$ mass in $\tau^-\to K^-\pi^0K^0\nu_\tau$ +XLabel=$m_{K^-K^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^-K^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpi0k0_4 +Title=Distribution of the $\pi^0K^0$ mass in $\tau^-\to K^-\pi^0K^0\nu_\tau$ +XLabel=$m_{\pi^0K^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0K^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_pi0pi0km_1 +Title=Distribution of the hadronic mass in $\tau^-\to 2\pi^0K^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ 2\pi^0K^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ 2\pi^0K^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pi0pi0km_2 +Title=Distribution of the $\pi^0\pi^0$ mass in $\tau^-\to 2\pi^0K^-\nu_\tau$ +XLabel=$m_{\pi^0\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pi0pi0km_3 +Title=Distribution of the $K^-\pi^0$ mass in $\tau^-\to 2\pi^0K^-\nu_\tau$ +XLabel=$m_{K^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^-\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpimpip_1 +Title=Distribution of the hadronic mass in $\tau^-\to K^-\pi^-\pi^+\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ K^-\pi^-\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ K^-\pi^-\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpimpip_2 +Title=Distribution of the $K^-\pi^-$ mass in $\tau^-\to K^-\pi^-\pi^+\nu_\tau$ +XLabel=$m_{K^-\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^-\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpimpip_3 +Title=Distribution of the $K^-\pi^+$ mass in $\tau^-\to K^-\pi^-\pi^+\nu_\tau$ +XLabel=$m_{K^-\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^-\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kmpimpip_4 +Title=Distribution of the $\pi^+\pi^-$ mass in $\tau^-\to K^-\pi^-\pi^+\nu_\tau$ +XLabel=$m_{\pi^+\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_pimk0pi0_1 +Title=Distribution of the hadronic mass in $\tau^-\to \pi^-\pi^0\bar{K}^0\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ \pi^-\pi^0\bar{K}^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ \pi^-\pi^0\bar{K}^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pimk0pi0_2 +Title=Distribution of the $\bar{K}^0\pi^-$ mass in $\tau^-\to \pi^-\pi^0\bar{K}^0\nu_\tau$ +XLabel=$m_{\bar{K}^0\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\bar{K}^0\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pimk0pi0_3 +Title=Distribution of the $\pi^0\pi^-$ mass in $\tau^-\to \pi^-\pi^0\bar{K}^0\nu_\tau$ +XLabel=$m_{\pi^0\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pimk0pi0_4 +Title=Distribution of the $\bar{K}^0\pi^0$ mass in $\tau^-\to \pi^-\pi^0\bar{K}^0\nu_\tau$ +XLabel=$m_{\bar{K}^0\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\bar{K}^0\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_pimpi0eta_1 +Title=Distribution of the hadronic mass in $\tau^-\to \pi^-\pi^0\eta\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ \pi^-\pi^0\eta}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ \pi^-\pi^0\eta}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pimpi0eta_2 +Title=Distribution of the $\pi^-\pi^0$ mass in $\tau^-\to \pi^-\pi^0\eta\nu_\tau$ +XLabel=$m_{\pi^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pimpi0eta_3 +Title=Distribution of the $\eta\pi^-$ mass in $\tau^-\to \pi^-\pi^0\eta\nu_\tau$ +XLabel=$m_{\eta\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\eta\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pimpi0eta_4 +Title=Distribution of the $\eta\pi^0$ mass in $\tau^-\to \pi^-\pi^0\eta\nu_\tau$ +XLabel=$m_{\eta\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\eta\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_pimpi0gamma_1 +Title=Distribution of the hadronic mass in $\tau^-\to \pi^-\pi^0\gamma\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ \pi^-\pi^0\gamma}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ \pi^-\pi^0\gamma}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pimpi0gamma_2 +Title=Distribution of the $\pi^-\pi^0$ mass in $\tau^-\to \pi^-\pi^0\gamma\nu_\tau$ +XLabel=$m_{\pi^-\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pimpi0gamma_3 +Title=Distribution of the $\gamma\pi^-$ mass in $\tau^-\to \pi^-\pi^0\gamma\nu_\tau$ +XLabel=$m_{\gamma\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\gamma\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_pimpi0gamma_4 +Title=Distribution of the $\gamma\pi^0$ mass in $\tau^-\to \pi^-\pi^0\gamma\nu_\tau$ +XLabel=$m_{\gamma\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\gamma\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_kspimks_1 +Title=Distribution of the hadronic mass in $\tau^-\to K^0_S\pi^-K^0_S\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ K^0_S\pi^-K^0_S}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ K^0_S\pi^-K^0_S}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kspimks_2 +Title=Distribution of the $K^0_S\pi^-$ mass in $\tau^-\to K^0_S\pi^-K^0_S\nu_\tau$ +XLabel=$m_{K^0_S\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^0_S\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kspimks_3 +Title=Distribution of the $K^0_SK^0_S$ mass in $\tau^-\to K^0_S\pi^-K^0_S\nu_\tau$ +XLabel=$m_{K^0_SK^0_S}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^0_SK^0_S}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_klpimkl_1 +Title=Distribution of the hadronic mass in $\tau^-\to K^0_L\pi^-K^0_L\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ K^0_L\pi^-K^0_L}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ K^0_L\pi^-K^0_L}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_klpimkl_2 +Title=Distribution of the $K^0_L\pi^-$ mass in $\tau^-\to K^0_L\pi^-K^0_L\nu_\tau$ +XLabel=$m_{K^0_L\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^0_L\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_klpimkl_3 +Title=Distribution of the $K^0_LK^0_L$ mass in $\tau^-\to K^0_L\pi^-K^0_L\nu_\tau$ +XLabel=$m_{K^0_LK^0_L}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^0_LK^0_L}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_3B_kspimkl_1 +Title=Distribution of the hadronic mass in $\tau^-\to K^0_S\pi^-K^0_L\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ K^0_S\pi^-K^0_L}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ K^0_S\pi^-K^0_L}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kspimkl_2 +Title=Distribution of the $K^0_S\pi^-$ mass in $\tau^-\to K^0_S\pi^-K^0_L\nu_\tau$ +XLabel=$m_{K^0_S\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^0_S\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kspimkl_3 +Title=Distribution of the $K^0_SK^0_L$ mass in $\tau^-\to K^0_S\pi^-K^0_L\nu_\tau$ +XLabel=$m_{K^0_SK^0_L}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^0_SK^0_L}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_3B_kspimkl_4 +Title=Distribution of the $K^0_L\pi^-$ mass in $\tau^-\to K^0_S\pi^-K^0_L\nu_\tau$ +XLabel=$m_{K^0_L\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{K^0_L\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT + +BEGIN PLOT /MC_TAU_Decay/h_4B_pipi_1 +Title=Distribution of the $\pi^0\pi^-$ mass in $\tau^-\to 3\pi^0\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ \pi^0\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ \pi^0\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipi_2 +Title=Distribution of the $\pi^0\pi^0$ mass in $\tau^-\to 3\pi^0\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{\pi^0\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipipi_1 +Title=Distribution of the $\pi^0\pi^0\pi^0$ mass in $\tau^-\to 3\pi^0\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{\pi^0\pi^0\pi^0}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^0\pi^0}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipipi_2 +Title=Distribution of the $\pi^0\pi^0\pi^-$ mass in $\tau^-\to 3\pi^0\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ \pi^0\pi^0\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ \pi^0\pi^0\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipipipi_1 +Title=Distribution of the hadronic mass in $\tau^-\to 3\pi^0\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ 3\pi^0\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ 3\pi^0\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipi_3 +Title=Distribution of the $\pi^0\pi^+$ mass in $\tau^-\to \pi^0\pi^+2\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ \pi^0\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ \pi^0\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipi_4 +Title=Distribution of the $\pi^0\pi^-$ mass in $\tau^-\to \pi^0\pi^+2\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{\pi^0\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipi_5 +Title=Distribution of the $\pi^+\pi^-$ mass in $\tau^-\to \pi^0\pi^+2\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{\pi^+\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^+\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipi_6 +Title=Distribution of the $\pi^-\pi^-$ mass in $\tau^-\to \pi^0\pi^+2\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{\pi^-\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^-\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipipi_3 +Title=Distribution of the $\pi^0\pi^-\pi^+$ mass in $\tau^-\to \pi^0\pi^+2\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ \pi^0\pi^-\pi^+}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ \pi^0\pi^-\pi^+}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipipi_4 +Title=Distribution of the $\pi^+\pi^-\pi^-$ mass in $\tau^-\to \pi^0\pi^+2\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ \pi^+\pi^-\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ \pi^+\pi^-\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipipi_5 +Title=Distribution of the $\pi^0\pi^-\pi^-$ mass in $\tau^-\to \pi^0\pi^+2\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{ \pi^0\pi^-\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{ \pi^0\pi^-\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT +BEGIN PLOT /MC_TAU_Decay/h_4B_pipipipi_2 +Title=Distribution of the $\pi^0\pi^+2\pi^-$ mass in $\tau^-\to \pi^0\pi^+2\pi^-\nu_\tau$ +LegendXPos=0.1 +XLabel=$m_{\pi^0\pi^+2\pi^-}$/GeV +YLabel=$1/\Gamma{\rm d}\Gamma/{\rm d}m_{\pi^0\pi^+2\pi^-}$\,$[{\rm GeV}^{-1}]$ +END PLOT diff --git a/analyses/pluginMisc/ARGUS_1993_S2653028.cc b/analyses/pluginMisc/ARGUS_1993_S2653028.cc deleted file mode 100644 --- a/analyses/pluginMisc/ARGUS_1993_S2653028.cc +++ /dev/null @@ -1,177 +0,0 @@ -// -*- C++ -*- -#include "Rivet/Analysis.hh" -#include "Rivet/Projections/UnstableParticles.hh" - -namespace Rivet { - - - /// @brief BELLE pi+/-, K+/- and proton/antiproton spectrum at Upsilon(4S) - /// @author Peter Richardson - class ARGUS_1993_S2653028 : public Analysis { - public: - - ARGUS_1993_S2653028() - : Analysis("ARGUS_1993_S2653028"), - _weightSum(0.) - { } - - - void analyze(const Event& e) { - const double weight = e.weight(); - - // Find the upsilons - Particles upsilons; - // First in unstable final state - const UnstableParticles& ufs = apply(e, "UFS"); - foreach (const Particle& p, ufs.particles()) { - if (p.pid() == 300553) upsilons.push_back(p); - } - // Then in whole event if that failed - if (upsilons.empty()) { - for(ConstGenParticlePtr p: HepMCUtils::particles(e.genEvent())) { - if (p->pdg_id() != 300553) continue; - ConstGenVertexPtr pv = p->production_vertex(); - bool passed = true; - if (pv) { - for(ConstGenParticlePtr pp: HepMCUtils::particles(pv, Relatives::PARENTS)){ - if ( p->pdg_id() == pp->pdg_id() ) { - passed = false; - break; - } - } - } - if (passed) upsilons.push_back(Particle(*p)); - } - } - - // Find an upsilon - foreach (const Particle& p, upsilons) { - _weightSum += weight; - vector pionsA,pionsB,protonsA,protonsB,kaons; - // Find the decay products we want - findDecayProducts(p.genParticle(), pionsA, pionsB, protonsA, protonsB, kaons); - LorentzTransform cms_boost; - if (p.p3().mod() > 1*MeV) - cms_boost = LorentzTransform::mkFrameTransformFromBeta(p.momentum().betaVec()); - for (size_t ix = 0; ix < pionsA.size(); ++ix) { - FourMomentum ptemp(pionsA[ix]->momentum()); - FourMomentum p2 = cms_boost.transform(ptemp); - double pcm = cms_boost.transform(ptemp).vector3().mod(); - _histPiA->fill(pcm,weight); - } - _multPiA->fill(10.58,double(pionsA.size())*weight); - for (size_t ix = 0; ix < pionsB.size(); ++ix) { - double pcm = cms_boost.transform(FourMomentum(pionsB[ix]->momentum())).vector3().mod(); - _histPiB->fill(pcm,weight); - } - _multPiB->fill(10.58,double(pionsB.size())*weight); - for (size_t ix = 0; ix < protonsA.size(); ++ix) { - double pcm = cms_boost.transform(FourMomentum(protonsA[ix]->momentum())).vector3().mod(); - _histpA->fill(pcm,weight); - } - _multpA->fill(10.58,double(protonsA.size())*weight); - for (size_t ix = 0; ix < protonsB.size(); ++ix) { - double pcm = cms_boost.transform(FourMomentum(protonsB[ix]->momentum())).vector3().mod(); - _histpB->fill(pcm,weight); - } - _multpB->fill(10.58,double(protonsB.size())*weight); - for (size_t ix = 0 ;ix < kaons.size(); ++ix) { - double pcm = cms_boost.transform(FourMomentum(kaons[ix]->momentum())).vector3().mod(); - _histKA->fill(pcm,weight); - _histKB->fill(pcm,weight); - } - _multK->fill(10.58,double(kaons.size())*weight); - } - } - - - void finalize() { - if (_weightSum > 0.) { - scale(_histPiA, 1./_weightSum); - scale(_histPiB, 1./_weightSum); - scale(_histKA , 1./_weightSum); - scale(_histKB , 1./_weightSum); - scale(_histpA , 1./_weightSum); - scale(_histpB , 1./_weightSum); - scale(_multPiA, 1./_weightSum); - scale(_multPiB, 1./_weightSum); - scale(_multK , 1./_weightSum); - scale(_multpA , 1./_weightSum); - scale(_multpB , 1./_weightSum); - } - } - - - void init() { - declare(UnstableParticles(), "UFS"); - - // spectra - _histPiA = bookHisto1D(1, 1, 1); - _histPiB = bookHisto1D(2, 1, 1); - _histKA = bookHisto1D(3, 1, 1); - _histKB = bookHisto1D(6, 1, 1); - _histpA = bookHisto1D(4, 1, 1); - _histpB = bookHisto1D(5, 1, 1); - // multiplicities - _multPiA = bookHisto1D( 7, 1, 1); - _multPiB = bookHisto1D( 8, 1, 1); - _multK = bookHisto1D( 9, 1, 1); - _multpA = bookHisto1D(10, 1, 1); - _multpB = bookHisto1D(11, 1, 1); - } // init - - - private: - - //@{ - /// Count of weights - double _weightSum; - /// Spectra - Histo1DPtr _histPiA, _histPiB, _histKA, _histKB, _histpA, _histpB; - /// Multiplicities - Histo1DPtr _multPiA, _multPiB, _multK, _multpA, _multpB; - //@} - - - void findDecayProducts(ConstGenParticlePtr p, - vector& pionsA, vector& pionsB, - vector& protonsA, vector& protonsB, - vector& kaons) - { - int parentId = p->pdg_id(); - ConstGenVertexPtr dv = p->end_vertex(); - /// @todo Use better looping - for(ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ - int id = abs(pp->pdg_id()); - if (id == PID::PIPLUS) { - if (parentId != PID::LAMBDA && parentId != PID::K0S) { - pionsA.push_back(pp); - pionsB.push_back(pp); - } - else - pionsB.push_back(pp); - } - else if (id == PID::PROTON) { - if (parentId != PID::LAMBDA && parentId != PID::K0S) { - protonsA.push_back(pp); - protonsB.push_back(pp); - } - else - protonsB.push_back(pp); - } - else if (id == PID::KPLUS) { - kaons.push_back(pp); - } - else if (pp->end_vertex()) - findDecayProducts(pp, pionsA, pionsB, protonsA, protonsB, kaons); - } - } - - - }; - - - // The hook for the plugin system - DECLARE_RIVET_PLUGIN(ARGUS_1993_S2653028); - -} diff --git a/analyses/pluginMisc/ARGUS_1993_S2653028.yoda b/analyses/pluginMisc/ARGUS_1993_S2653028.yoda deleted file mode 100644 --- a/analyses/pluginMisc/ARGUS_1993_S2653028.yoda +++ /dev/null @@ -1,310 +0,0 @@ -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d01-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d01-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -8.750000e-02 1.250000e-02 1.250000e-02 8.104000e+00 4.186275e-01 4.186275e-01 -1.125000e-01 1.250000e-02 1.250000e-02 9.439000e+00 3.628361e-01 3.628361e-01 -1.375000e-01 1.250000e-02 1.250000e-02 9.967000e+00 4.778221e-01 4.778221e-01 -1.625000e-01 1.250000e-02 1.250000e-02 1.123800e+01 4.873151e-01 4.873151e-01 -1.875000e-01 1.250000e-02 1.250000e-02 1.121700e+01 4.543941e-01 4.543941e-01 -2.125000e-01 1.250000e-02 1.250000e-02 1.220800e+01 4.865902e-01 4.865902e-01 -2.375000e-01 1.250000e-02 1.250000e-02 1.215300e+01 4.674281e-01 4.674281e-01 -2.625000e-01 1.250000e-02 1.250000e-02 1.214800e+01 4.711794e-01 4.711794e-01 -2.875000e-01 1.250000e-02 1.250000e-02 1.219400e+01 5.183098e-01 5.183098e-01 -3.125000e-01 1.250000e-02 1.250000e-02 1.181100e+01 4.396283e-01 4.396283e-01 -3.375000e-01 1.250000e-02 1.250000e-02 1.165000e+01 4.835173e-01 4.835173e-01 -3.625000e-01 1.250000e-02 1.250000e-02 1.101000e+01 4.527659e-01 4.527659e-01 -3.875000e-01 1.250000e-02 1.250000e-02 1.008500e+01 4.149217e-01 4.149217e-01 -4.125000e-01 1.250000e-02 1.250000e-02 1.016000e+01 3.841471e-01 3.841471e-01 -4.375000e-01 1.250000e-02 1.250000e-02 9.378000e+00 3.724903e-01 3.724903e-01 -4.625000e-01 1.250000e-02 1.250000e-02 8.957000e+00 3.922372e-01 3.922372e-01 -4.875000e-01 1.250000e-02 1.250000e-02 8.198000e+00 3.395202e-01 3.395202e-01 -5.125000e-01 1.250000e-02 1.250000e-02 7.801000e+00 3.990551e-01 3.990551e-01 -5.375000e-01 1.250000e-02 1.250000e-02 6.806000e+00 3.105769e-01 3.105769e-01 -5.625000e-01 1.250000e-02 1.250000e-02 6.175000e+00 2.894685e-01 2.894685e-01 -5.875000e-01 1.250000e-02 1.250000e-02 6.222000e+00 3.119776e-01 3.119776e-01 -6.125000e-01 1.250000e-02 1.250000e-02 5.380000e+00 2.767996e-01 2.767996e-01 -6.375000e-01 1.250000e-02 1.250000e-02 5.309000e+00 2.735781e-01 2.735781e-01 -6.625000e-01 1.250000e-02 1.250000e-02 5.096000e+00 2.720772e-01 2.720772e-01 -6.875000e-01 1.250000e-02 1.250000e-02 4.193000e+00 2.786575e-01 2.786575e-01 -7.125000e-01 1.250000e-02 1.250000e-02 3.882000e+00 3.207320e-01 3.207320e-01 -7.375000e-01 1.250000e-02 1.250000e-02 3.939000e+00 2.679179e-01 2.679179e-01 -7.625000e-01 1.250000e-02 1.250000e-02 3.785000e+00 2.684772e-01 2.684772e-01 -7.875000e-01 1.250000e-02 1.250000e-02 3.370000e+00 2.504795e-01 2.504795e-01 -8.500000e-01 5.000000e-02 5.000000e-02 2.732000e+00 1.488220e-01 1.488220e-01 -9.500000e-01 5.000000e-02 5.000000e-02 1.861000e+00 1.273146e-01 1.273146e-01 -1.050000e+00 5.000000e-02 5.000000e-02 1.160000e+00 1.376445e-01 1.376445e-01 -1.150000e+00 5.000000e-02 5.000000e-02 8.110000e-01 1.414956e-01 1.414956e-01 -1.250000e+00 5.000000e-02 5.000000e-02 6.220000e-01 1.781039e-01 1.781039e-01 -1.350000e+00 5.000000e-02 5.000000e-02 4.330000e-01 1.272635e-01 1.272635e-01 -1.450000e+00 5.000000e-02 5.000000e-02 4.540000e-01 1.218236e-01 1.218236e-01 -1.550000e+00 5.000000e-02 5.000000e-02 2.080000e-01 1.076290e-01 1.076290e-01 -1.650000e+00 5.000000e-02 5.000000e-02 1.410000e-01 9.167879e-02 9.167879e-02 -1.750000e+00 5.000000e-02 5.000000e-02 1.750000e-01 7.710383e-02 7.710383e-02 -1.850000e+00 5.000000e-02 5.000000e-02 1.020000e-01 6.530697e-02 6.530697e-02 -1.950000e+00 5.000000e-02 5.000000e-02 9.000000e-02 6.041523e-02 6.041523e-02 -2.050000e+00 5.000000e-02 5.000000e-02 1.230000e-01 5.693856e-02 5.693856e-02 -2.150000e+00 5.000000e-02 5.000000e-02 6.600000e-02 5.500000e-02 5.500000e-02 -2.250000e+00 5.000000e-02 5.000000e-02 1.400000e-01 4.162932e-02 4.162932e-02 -2.350000e+00 5.000000e-02 5.000000e-02 1.000000e-02 4.420407e-02 4.420407e-02 -2.450000e+00 5.000000e-02 5.000000e-02 2.100000e-02 4.601087e-02 4.601087e-02 -2.550000e+00 5.000000e-02 5.000000e-02 2.600000e-02 3.041381e-02 3.041381e-02 -2.650000e+00 5.000000e-02 5.000000e-02 -1.500000e-02 3.535534e-02 3.535534e-02 -2.750000e+00 5.000000e-02 5.000000e-02 -1.100000e-02 2.884441e-02 2.884441e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d02-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d02-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -8.750000e-02 1.250000e-02 1.250000e-02 9.356000e+00 4.601239e-01 4.601239e-01 -1.125000e-01 1.250000e-02 1.250000e-02 1.112100e+01 3.917780e-01 3.917780e-01 -1.375000e-01 1.250000e-02 1.250000e-02 1.203600e+01 5.443473e-01 5.443473e-01 -1.625000e-01 1.250000e-02 1.250000e-02 1.357500e+01 5.505679e-01 5.505679e-01 -1.875000e-01 1.250000e-02 1.250000e-02 1.377200e+01 5.043352e-01 5.043352e-01 -2.125000e-01 1.250000e-02 1.250000e-02 1.478600e+01 5.382054e-01 5.382054e-01 -2.375000e-01 1.250000e-02 1.250000e-02 1.451400e+01 5.043104e-01 5.043104e-01 -2.625000e-01 1.250000e-02 1.250000e-02 1.426800e+01 5.044770e-01 5.044770e-01 -2.875000e-01 1.250000e-02 1.250000e-02 1.417900e+01 5.622855e-01 5.622855e-01 -3.125000e-01 1.250000e-02 1.250000e-02 1.365800e+01 4.621309e-01 4.621309e-01 -3.375000e-01 1.250000e-02 1.250000e-02 1.336700e+01 5.170039e-01 5.170039e-01 -3.625000e-01 1.250000e-02 1.250000e-02 1.264900e+01 4.804009e-01 4.804009e-01 -3.875000e-01 1.250000e-02 1.250000e-02 1.156200e+01 4.348471e-01 4.348471e-01 -4.125000e-01 1.250000e-02 1.250000e-02 1.151400e+01 3.969811e-01 3.969811e-01 -4.375000e-01 1.250000e-02 1.250000e-02 1.065000e+01 3.853232e-01 3.853232e-01 -4.625000e-01 1.250000e-02 1.250000e-02 1.011200e+01 4.106215e-01 4.106215e-01 -4.875000e-01 1.250000e-02 1.250000e-02 9.271000e+00 3.480589e-01 3.480589e-01 -5.125000e-01 1.250000e-02 1.250000e-02 8.762000e+00 4.207576e-01 4.207576e-01 -5.375000e-01 1.250000e-02 1.250000e-02 7.645000e+00 3.151270e-01 3.151270e-01 -5.625000e-01 1.250000e-02 1.250000e-02 6.957000e+00 2.909038e-01 2.909038e-01 -5.875000e-01 1.250000e-02 1.250000e-02 6.924000e+00 3.205511e-01 3.205511e-01 -6.125000e-01 1.250000e-02 1.250000e-02 6.021000e+00 2.793081e-01 2.793081e-01 -6.375000e-01 1.250000e-02 1.250000e-02 5.877000e+00 2.767020e-01 2.767020e-01 -6.625000e-01 1.250000e-02 1.250000e-02 5.636000e+00 2.765086e-01 2.765086e-01 -6.875000e-01 1.250000e-02 1.250000e-02 4.671000e+00 2.859108e-01 2.859108e-01 -7.125000e-01 1.250000e-02 1.250000e-02 4.315000e+00 3.372907e-01 3.372907e-01 -7.375000e-01 1.250000e-02 1.250000e-02 4.341000e+00 2.746507e-01 2.746507e-01 -7.625000e-01 1.250000e-02 1.250000e-02 4.157000e+00 2.764417e-01 2.764417e-01 -7.875000e-01 1.250000e-02 1.250000e-02 3.689000e+00 2.557597e-01 2.557597e-01 -8.500000e-01 5.000000e-02 5.000000e-02 2.983000e+00 1.548967e-01 1.548967e-01 -9.500000e-01 5.000000e-02 5.000000e-02 2.042000e+00 1.314002e-01 1.314002e-01 -1.050000e+00 5.000000e-02 5.000000e-02 1.280000e+00 1.443122e-01 1.443122e-01 -1.150000e+00 5.000000e-02 5.000000e-02 8.910000e-01 1.473228e-01 1.473228e-01 -1.250000e+00 5.000000e-02 5.000000e-02 6.760000e-01 1.874273e-01 1.874273e-01 -1.350000e+00 5.000000e-02 5.000000e-02 4.730000e-01 1.303840e-01 1.303840e-01 -1.450000e+00 5.000000e-02 5.000000e-02 4.770000e-01 1.243262e-01 1.243262e-01 -1.550000e+00 5.000000e-02 5.000000e-02 2.230000e-01 1.110360e-01 1.110360e-01 -1.650000e+00 5.000000e-02 5.000000e-02 1.500000e-01 9.360556e-02 9.360556e-02 -1.750000e+00 5.000000e-02 5.000000e-02 1.810000e-01 7.823682e-02 7.823682e-02 -1.850000e+00 5.000000e-02 5.000000e-02 1.050000e-01 6.574192e-02 6.574192e-02 -1.950000e+00 5.000000e-02 5.000000e-02 9.100000e-02 6.090156e-02 6.090156e-02 -2.050000e+00 5.000000e-02 5.000000e-02 1.250000e-01 5.745433e-02 5.745433e-02 -2.150000e+00 5.000000e-02 5.000000e-02 6.700000e-02 5.500000e-02 5.500000e-02 -2.250000e+00 5.000000e-02 5.000000e-02 1.400000e-01 4.162932e-02 4.162932e-02 -2.350000e+00 5.000000e-02 5.000000e-02 1.000000e-02 4.420407e-02 4.420407e-02 -2.450000e+00 5.000000e-02 5.000000e-02 2.100000e-02 4.601087e-02 4.601087e-02 -2.550000e+00 5.000000e-02 5.000000e-02 2.600000e-02 3.041381e-02 3.041381e-02 -2.650000e+00 5.000000e-02 5.000000e-02 -1.500000e-02 3.535534e-02 3.535534e-02 -2.750000e+00 5.000000e-02 5.000000e-02 -1.100000e-02 2.884441e-02 2.884441e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d03-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d03-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -1.875000e-01 1.250000e-02 1.250000e-02 6.780000e-01 1.263725e-01 1.263725e-01 -2.125000e-01 1.250000e-02 1.250000e-02 1.032000e+00 1.281444e-01 1.281444e-01 -2.375000e-01 1.250000e-02 1.250000e-02 1.240000e+00 1.386831e-01 1.386831e-01 -2.625000e-01 1.250000e-02 1.250000e-02 1.386000e+00 1.122943e-01 1.122943e-01 -2.875000e-01 1.250000e-02 1.250000e-02 1.423000e+00 1.566046e-01 1.566046e-01 -3.125000e-01 1.250000e-02 1.250000e-02 1.501000e+00 1.162110e-01 1.162110e-01 -3.375000e-01 1.250000e-02 1.250000e-02 1.611000e+00 1.343577e-01 1.343577e-01 -3.625000e-01 1.250000e-02 1.250000e-02 1.893000e+00 1.290736e-01 1.290736e-01 -3.875000e-01 1.250000e-02 1.250000e-02 1.834000e+00 1.151043e-01 1.151043e-01 -4.125000e-01 1.250000e-02 1.250000e-02 2.083000e+00 1.242014e-01 1.242014e-01 -4.375000e-01 1.250000e-02 1.250000e-02 2.009000e+00 1.234220e-01 1.234220e-01 -4.625000e-01 1.250000e-02 1.250000e-02 2.000000e+00 1.172391e-01 1.172391e-01 -4.875000e-01 1.250000e-02 1.250000e-02 2.130000e+00 1.336862e-01 1.336862e-01 -5.125000e-01 1.250000e-02 1.250000e-02 1.952000e+00 1.416757e-01 1.416757e-01 -5.375000e-01 1.250000e-02 1.250000e-02 1.887000e+00 1.372771e-01 1.372771e-01 -5.625000e-01 1.250000e-02 1.250000e-02 1.822000e+00 1.380580e-01 1.380580e-01 -5.875000e-01 1.250000e-02 1.250000e-02 1.809000e+00 1.297998e-01 1.297998e-01 -6.125000e-01 1.250000e-02 1.250000e-02 1.904000e+00 1.300846e-01 1.300846e-01 -6.375000e-01 1.250000e-02 1.250000e-02 1.732000e+00 1.404172e-01 1.404172e-01 -6.625000e-01 1.250000e-02 1.250000e-02 1.571000e+00 1.293754e-01 1.293754e-01 -6.875000e-01 1.250000e-02 1.250000e-02 1.521000e+00 1.270590e-01 1.270590e-01 -7.125000e-01 1.250000e-02 1.250000e-02 1.405000e+00 1.745222e-01 1.745222e-01 -7.375000e-01 1.250000e-02 1.250000e-02 1.392000e+00 1.458664e-01 1.458664e-01 -7.625000e-01 1.250000e-02 1.250000e-02 1.379000e+00 1.920417e-01 1.920417e-01 -7.875000e-01 1.250000e-02 1.250000e-02 1.200000e+00 1.647695e-01 1.647695e-01 -8.500000e-01 5.000000e-02 5.000000e-02 9.170000e-01 7.874643e-02 7.874643e-02 -9.500000e-01 5.000000e-02 5.000000e-02 9.570000e-01 8.527602e-02 8.527602e-02 -1.050000e+00 5.000000e-02 5.000000e-02 6.590000e-01 1.212642e-01 1.212642e-01 -1.150000e+00 5.000000e-02 5.000000e-02 4.030000e-01 1.131592e-01 1.131592e-01 -1.250000e+00 5.000000e-02 5.000000e-02 5.720000e-01 1.666433e-01 1.666433e-01 -1.350000e+00 5.000000e-02 5.000000e-02 5.350000e-01 1.050809e-01 1.050809e-01 -1.450000e+00 5.000000e-02 5.000000e-02 2.080000e-01 1.119464e-01 1.119464e-01 -1.550000e+00 5.000000e-02 5.000000e-02 3.120000e-01 7.907591e-02 7.907591e-02 -1.650000e+00 5.000000e-02 5.000000e-02 1.600000e-01 5.913544e-02 5.913544e-02 -1.750000e+00 5.000000e-02 5.000000e-02 1.240000e-01 5.456189e-02 5.456189e-02 -1.850000e+00 5.000000e-02 5.000000e-02 1.300000e-02 5.325411e-02 5.325411e-02 -1.950000e+00 5.000000e-02 5.000000e-02 6.500000e-02 4.052160e-02 4.052160e-02 -2.050000e+00 5.000000e-02 5.000000e-02 -6.200000e-02 4.429447e-02 4.429447e-02 -2.150000e+00 5.000000e-02 5.000000e-02 -2.600000e-02 3.832754e-02 3.832754e-02 -2.250000e+00 5.000000e-02 5.000000e-02 2.400000e-02 4.420407e-02 4.420407e-02 -2.350000e+00 5.000000e-02 5.000000e-02 -2.100000e-02 4.022437e-02 4.022437e-02 -2.450000e+00 5.000000e-02 5.000000e-02 1.400000e-02 4.272002e-02 4.272002e-02 -2.550000e+00 5.000000e-02 5.000000e-02 -3.200000e-02 4.022437e-02 4.022437e-02 -2.650000e+00 5.000000e-02 5.000000e-02 4.000000e-02 3.573514e-02 3.573514e-02 -2.750000e+00 5.000000e-02 5.000000e-02 4.600000e-02 4.304649e-02 4.304649e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d04-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d04-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -3.500000e-01 5.000000e-02 5.000000e-02 1.170000e-01 2.773085e-02 2.773085e-02 -4.500000e-01 5.000000e-02 5.000000e-02 1.150000e-01 3.206244e-02 3.206244e-02 -5.500000e-01 5.000000e-02 5.000000e-02 2.010000e-01 3.337664e-02 3.337664e-02 -6.500000e-01 5.000000e-02 5.000000e-02 1.200000e-01 3.590265e-02 3.590265e-02 -7.500000e-01 5.000000e-02 5.000000e-02 1.250000e-01 3.544009e-02 3.544009e-02 -8.500000e-01 5.000000e-02 5.000000e-02 8.800000e-02 3.478505e-02 3.478505e-02 -9.500000e-01 5.000000e-02 5.000000e-02 1.120000e-01 3.101612e-02 3.101612e-02 -1.050000e+00 5.000000e-02 5.000000e-02 5.400000e-02 3.228002e-02 3.228002e-02 -1.150000e+00 5.000000e-02 5.000000e-02 6.000000e-02 3.014963e-02 3.014963e-02 -1.250000e+00 5.000000e-02 5.000000e-02 -1.200000e-02 2.906888e-02 2.906888e-02 -1.350000e+00 5.000000e-02 5.000000e-02 1.000000e-02 3.640055e-02 3.640055e-02 -1.450000e+00 5.000000e-02 5.000000e-02 -2.100000e-02 2.641969e-02 2.641969e-02 -1.550000e+00 5.000000e-02 5.000000e-02 -2.100000e-02 2.865310e-02 2.865310e-02 -1.650000e+00 5.000000e-02 5.000000e-02 -1.100000e-02 2.996665e-02 2.996665e-02 -1.750000e+00 5.000000e-02 5.000000e-02 -1.600000e-02 3.220248e-02 3.220248e-02 -1.850000e+00 5.000000e-02 5.000000e-02 3.400000e-02 3.577709e-02 3.577709e-02 -1.950000e+00 5.000000e-02 5.000000e-02 -2.000000e-02 4.263801e-02 4.263801e-02 -2.050000e+00 5.000000e-02 5.000000e-02 3.100000e-02 4.085340e-02 4.085340e-02 -2.150000e+00 5.000000e-02 5.000000e-02 -3.000000e-03 4.548626e-02 4.548626e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d05-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d05-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -3.500000e-01 5.000000e-02 5.000000e-02 1.720000e-01 3.023243e-02 3.023243e-02 -4.500000e-01 5.000000e-02 5.000000e-02 1.880000e-01 3.214032e-02 3.214032e-02 -5.500000e-01 5.000000e-02 5.000000e-02 2.740000e-01 3.373426e-02 3.373426e-02 -6.500000e-01 5.000000e-02 5.000000e-02 1.900000e-01 3.733631e-02 3.733631e-02 -7.500000e-01 5.000000e-02 5.000000e-02 1.750000e-01 3.640055e-02 3.640055e-02 -8.500000e-01 5.000000e-02 5.000000e-02 1.240000e-01 3.667424e-02 3.667424e-02 -9.500000e-01 5.000000e-02 5.000000e-02 1.360000e-01 3.101612e-02 3.101612e-02 -1.050000e+00 5.000000e-02 5.000000e-02 7.700000e-02 3.324154e-02 3.324154e-02 -1.150000e+00 5.000000e-02 5.000000e-02 7.200000e-02 3.014963e-02 3.014963e-02 -1.250000e+00 5.000000e-02 5.000000e-02 -4.000000e-03 2.906888e-02 2.906888e-02 -1.350000e+00 5.000000e-02 5.000000e-02 1.400000e-02 4.565085e-02 4.565085e-02 -1.450000e+00 5.000000e-02 5.000000e-02 -1.800000e-02 2.641969e-02 2.641969e-02 -1.550000e+00 5.000000e-02 5.000000e-02 -2.000000e-02 2.865310e-02 2.865310e-02 -1.650000e+00 5.000000e-02 5.000000e-02 -1.000000e-02 2.996665e-02 2.996665e-02 -1.750000e+00 5.000000e-02 5.000000e-02 -1.600000e-02 3.220248e-02 3.220248e-02 -1.850000e+00 5.000000e-02 5.000000e-02 3.400000e-02 3.577709e-02 3.577709e-02 -1.950000e+00 5.000000e-02 5.000000e-02 -2.000000e-02 4.263801e-02 4.263801e-02 -2.050000e+00 5.000000e-02 5.000000e-02 3.100000e-02 4.085340e-02 4.085340e-02 -2.150000e+00 5.000000e-02 5.000000e-02 -3.000000e-03 4.548626e-02 4.548626e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d06-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d06-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.500000e-01 5.000000e-02 5.000000e-02 1.210000e+00 1.581139e-01 1.581139e-01 -3.500000e-01 5.000000e-02 5.000000e-02 1.710000e+00 2.080865e-01 2.080865e-01 -4.500000e-01 5.000000e-02 5.000000e-02 1.750000e+00 2.267157e-01 2.267157e-01 -5.500000e-01 5.000000e-02 5.000000e-02 2.010000e+00 2.690725e-01 2.690725e-01 -6.500000e-01 5.000000e-02 5.000000e-02 1.450000e+00 2.280351e-01 2.280351e-01 -7.500000e-01 5.000000e-02 5.000000e-02 1.200000e+00 2.163331e-01 2.163331e-01 -8.500000e-01 5.000000e-02 5.000000e-02 9.800000e-01 2.012461e-01 2.012461e-01 -9.500000e-01 5.000000e-02 5.000000e-02 9.700000e-01 2.193171e-01 2.193171e-01 -1.050000e+00 5.000000e-02 5.000000e-02 6.400000e-01 1.802776e-01 1.802776e-01 -1.150000e+00 5.000000e-02 5.000000e-02 1.300000e-01 1.802776e-01 1.802776e-01 -1.250000e+00 5.000000e-02 5.000000e-02 5.600000e-01 1.676305e-01 1.676305e-01 -1.350000e+00 5.000000e-02 5.000000e-02 2.300000e-01 1.726268e-01 1.726268e-01 -1.450000e+00 5.000000e-02 5.000000e-02 9.000000e-02 1.315295e-01 1.315295e-01 -1.550000e+00 5.000000e-02 5.000000e-02 1.500000e-01 1.513275e-01 1.513275e-01 -1.650000e+00 5.000000e-02 5.000000e-02 9.000000e-02 1.303840e-01 1.303840e-01 -1.750000e+00 5.000000e-02 5.000000e-02 -1.100000e-01 1.726268e-01 1.726268e-01 -1.850000e+00 5.000000e-02 5.000000e-02 1.000000e-02 1.513275e-01 1.513275e-01 -1.950000e+00 5.000000e-02 5.000000e-02 -7.000000e-02 9.055385e-02 9.055385e-02 -2.050000e+00 5.000000e-02 5.000000e-02 -3.000000e-02 9.055385e-02 9.055385e-02 -2.150000e+00 5.000000e-02 5.000000e-02 1.900000e-01 1.910497e-01 1.910497e-01 -2.250000e+00 5.000000e-02 5.000000e-02 2.700000e-01 2.927456e-01 2.927456e-01 -2.350000e+00 5.000000e-02 5.000000e-02 1.500000e-01 1.902630e-01 1.902630e-01 -2.450000e+00 5.000000e-02 5.000000e-02 -1.100000e-01 1.603122e-01 1.603122e-01 -2.550000e+00 5.000000e-02 5.000000e-02 -6.000000e-02 1.403567e-01 1.403567e-01 -2.650000e+00 5.000000e-02 5.000000e-02 4.000000e-02 9.000000e-02 9.000000e-02 -2.750000e+00 5.000000e-02 5.000000e-02 2.000000e-02 4.472136e-02 4.472136e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d07-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d07-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -1.058000e+01 5.000000e-01 5.000000e-01 7.170000e+00 1.486607e-01 1.486607e-01 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d08-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d08-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -1.058000e+01 5.000000e-01 5.000000e-01 8.210000e+00 1.676305e-01 1.676305e-01 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d09-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d09-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -1.058000e+01 5.000000e-01 5.000000e-01 1.550000e+00 5.830952e-02 5.830952e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d10-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d10-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -1.058000e+01 5.000000e-01 5.000000e-01 1.100000e-01 1.220656e-02 1.220656e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/ARGUS_1993_S2653028/d11-x01-y01 -IsRef: 1 -Path: /REF/ARGUS_1993_S2653028/d11-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -1.058000e+01 5.000000e-01 5.000000e-01 1.600000e-01 1.414214e-02 1.414214e-02 -END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/ARGUS_1993_S2669951.cc b/analyses/pluginMisc/ARGUS_1993_S2669951.cc deleted file mode 100644 --- a/analyses/pluginMisc/ARGUS_1993_S2669951.cc +++ /dev/null @@ -1,191 +0,0 @@ -// -*- C++ -*- -#include "Rivet/Analysis.hh" -#include "Rivet/Projections/UnstableParticles.hh" - -namespace Rivet { - - - /// @brief Production of the $\eta'(958)$ and $f_0(980)$ in $e^+e^-$ annihilation in the Upsilon region - /// @author Peter Richardson - class ARGUS_1993_S2669951 : public Analysis { - public: - - ARGUS_1993_S2669951() - : Analysis("ARGUS_1993_S2669951"), - _count_etaPrime_highZ(2, 0.), - _count_etaPrime_allZ(3, 0.), - _count_f0(3, 0.), - _weightSum_cont(0.), - _weightSum_Ups1(0.), - _weightSum_Ups2(0.) - { } - - - void init() { - declare(UnstableParticles(), "UFS"); - - _hist_cont_f0 = bookHisto1D(2, 1, 1); - _hist_Ups1_f0 = bookHisto1D(3, 1, 1); - _hist_Ups2_f0 = bookHisto1D(4, 1, 1); - } - - - void analyze(const Event& e) { - - // Find the Upsilons among the unstables - const UnstableParticles& ufs = apply(e, "UFS"); - Particles upsilons; - - // First in unstable final state - foreach (const Particle& p, ufs.particles()) - if (p.pid() == 553 || p.pid() == 100553) - upsilons.push_back(p); - // Then in whole event if fails - if (upsilons.empty()) { - /// @todo Replace HepMC digging with Particle::descendents etc. calls - for(ConstGenParticlePtr p: HepMCUtils::particles(e.genEvent())) { - if ( p->pdg_id() != 553 && p->pdg_id() != 100553 ) continue; - // Discard it if its parent has the same PDG ID code (avoid duplicates) - ConstGenVertexPtr pv = p->production_vertex(); - bool passed = true; - if (pv) { - for(ConstGenParticlePtr pp: HepMCUtils::particles(pv, Relatives::PARENTS)){ - if ( p->pdg_id() == pp->pdg_id() ) { - passed = false; - break; - } - } - } - if (passed) upsilons.push_back(Particle(*p)); - } - } - - - // Finding done, now fill counters - const double weight = e.weight(); - if (upsilons.empty()) { // Continuum - MSG_DEBUG("No Upsilons found => continuum event"); - - _weightSum_cont += weight; - unsigned int nEtaA(0), nEtaB(0), nf0(0); - foreach (const Particle& p, ufs.particles()) { - const int id = p.abspid(); - const double xp = 2.*p.E()/sqrtS(); - const double beta = p.p3().mod() / p.E(); - if (id == 9010221) { - _hist_cont_f0->fill(xp, weight/beta); - nf0 += 1; - } else if (id == 331) { - if (xp > 0.35) nEtaA += 1; - nEtaB += 1; - } - } - _count_f0[2] += nf0*weight; - _count_etaPrime_highZ[1] += nEtaA*weight; - _count_etaPrime_allZ[2] += nEtaB*weight; - - } else { // Upsilon(s) found - MSG_DEBUG("Upsilons found => resonance event"); - - foreach (const Particle& ups, upsilons) { - const int parentId = ups.pid(); - ((parentId == 553) ? _weightSum_Ups1 : _weightSum_Ups2) += weight; - Particles unstable; - // Find the decay products we want - findDecayProducts(ups.genParticle(), unstable); - LorentzTransform cms_boost; - if (ups.p3().mod() > 1*MeV) - cms_boost = LorentzTransform::mkFrameTransformFromBeta(ups.momentum().betaVec()); - const double mass = ups.mass(); - unsigned int nEtaA(0), nEtaB(0), nf0(0); - foreach(const Particle& p, unstable) { - const int id = p.abspid(); - const FourMomentum p2 = cms_boost.transform(p.momentum()); - const double xp = 2.*p2.E()/mass; - const double beta = p2.p3().mod()/p2.E(); - if (id == 9010221) { //< ? - ((parentId == 553) ? _hist_Ups1_f0 : _hist_Ups2_f0)->fill(xp, weight/beta); - nf0 += 1; - } else if (id == 331) { //< ? - if (xp > 0.35) nEtaA += 1; - nEtaB += 1; - } - } - if (parentId == 553) { - _count_f0[0] += nf0*weight; - _count_etaPrime_highZ[0] += nEtaA*weight; - _count_etaPrime_allZ[0] += nEtaB*weight; - } else { - _count_f0[1] += nf0*weight; - _count_etaPrime_allZ[1] += nEtaB*weight; - } - } - } - } - - - void finalize() { - - // High-Z eta' multiplicity - Scatter2DPtr s111 = bookScatter2D(1, 1, 1, true); - if (_weightSum_Ups1 > 0) // Point at 9.460 - s111->point(0).setY(_count_etaPrime_highZ[0] / _weightSum_Ups1, 0); - if (_weightSum_cont > 0) // Point at 9.905 - s111->point(1).setY(_count_etaPrime_highZ[1] / _weightSum_cont, 0); - - // All-Z eta' multiplicity - Scatter2DPtr s112 = bookScatter2D(1, 1, 2, true); - if (_weightSum_Ups1 > 0) // Point at 9.460 - s112->point(0).setY(_count_etaPrime_allZ[0] / _weightSum_Ups1, 0); - if (_weightSum_cont > 0) // Point at 9.905 - s112->point(1).setY(_count_etaPrime_allZ[2] / _weightSum_cont, 0); - if (_weightSum_Ups2 > 0) // Point at 10.02 - s112->point(2).setY(_count_etaPrime_allZ[1] / _weightSum_Ups2, 0); - - // f0 multiplicity - Scatter2DPtr s511 = bookScatter2D(5, 1, 1, true); - if (_weightSum_Ups1 > 0) // Point at 9.46 - s511->point(0).setY(_count_f0[0] / _weightSum_Ups1, 0); - if (_weightSum_Ups2 > 0) // Point at 10.02 - s511->point(1).setY(_count_f0[1] / _weightSum_Ups2, 0); - if (_weightSum_cont > 0) // Point at 10.45 - s511->point(2).setY(_count_f0[2] / _weightSum_cont, 0); - - // Scale histos - if (_weightSum_cont > 0.) scale(_hist_cont_f0, 1./_weightSum_cont); - if (_weightSum_Ups1 > 0.) scale(_hist_Ups1_f0, 1./_weightSum_Ups1); - if (_weightSum_Ups2 > 0.) scale(_hist_Ups2_f0, 1./_weightSum_Ups2); - } - - - private: - - /// @name Counters - //@{ - vector _count_etaPrime_highZ, _count_etaPrime_allZ, _count_f0; - double _weightSum_cont,_weightSum_Ups1,_weightSum_Ups2; - //@} - - - /// Histos - Histo1DPtr _hist_cont_f0, _hist_Ups1_f0, _hist_Ups2_f0; - - - /// Recursively walk the HepMC tree to find decay products of @a p - void findDecayProducts(ConstGenParticlePtr p, Particles& unstable) { - ConstGenVertexPtr dv = p->end_vertex(); - for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ - const int id = abs(pp->pdg_id()); - if (id == 331 || id == 9010221) unstable.push_back(Particle(pp)); - else if (pp->end_vertex()) findDecayProducts(pp, unstable); - } - } - - - }; - - - // The hook for the plugin system - DECLARE_RIVET_PLUGIN(ARGUS_1993_S2669951); - -} diff --git a/analyses/pluginMisc/ARGUS_1993_S2789213.cc b/analyses/pluginMisc/ARGUS_1993_S2789213.cc deleted file mode 100644 --- a/analyses/pluginMisc/ARGUS_1993_S2789213.cc +++ /dev/null @@ -1,256 +0,0 @@ -// -*- C++ -*- -#include "Rivet/Analysis.hh" -#include "Rivet/Projections/UnstableParticles.hh" - -namespace Rivet { - - - /// @brief ARGUS vector meson production - /// @author Peter Richardson - class ARGUS_1993_S2789213 : public Analysis { - public: - - ARGUS_1993_S2789213() - : Analysis("ARGUS_1993_S2789213"), - _weightSum_cont(0.),_weightSum_Ups1(0.),_weightSum_Ups4(0.) - { } - - - void init() { - declare(UnstableParticles(), "UFS"); - - _mult_cont_Omega = bookHisto1D( 1, 1, 1); - _mult_cont_Rho0 = bookHisto1D( 1, 1, 2); - _mult_cont_KStar0 = bookHisto1D( 1, 1, 3); - _mult_cont_KStarPlus = bookHisto1D( 1, 1, 4); - _mult_cont_Phi = bookHisto1D( 1, 1, 5); - - _mult_Ups1_Omega = bookHisto1D( 2, 1, 1); - _mult_Ups1_Rho0 = bookHisto1D( 2, 1, 2); - _mult_Ups1_KStar0 = bookHisto1D( 2, 1, 3); - _mult_Ups1_KStarPlus = bookHisto1D( 2, 1, 4); - _mult_Ups1_Phi = bookHisto1D( 2, 1, 5); - - _mult_Ups4_Omega = bookHisto1D( 3, 1, 1); - _mult_Ups4_Rho0 = bookHisto1D( 3, 1, 2); - _mult_Ups4_KStar0 = bookHisto1D( 3, 1, 3); - _mult_Ups4_KStarPlus = bookHisto1D( 3, 1, 4); - _mult_Ups4_Phi = bookHisto1D( 3, 1, 5); - - _hist_cont_KStarPlus = bookHisto1D( 4, 1, 1); - _hist_Ups1_KStarPlus = bookHisto1D( 5, 1, 1); - _hist_Ups4_KStarPlus = bookHisto1D( 6, 1, 1); - - _hist_cont_KStar0 = bookHisto1D( 7, 1, 1); - _hist_Ups1_KStar0 = bookHisto1D( 8, 1, 1); - _hist_Ups4_KStar0 = bookHisto1D( 9, 1, 1); - - _hist_cont_Rho0 = bookHisto1D(10, 1, 1); - _hist_Ups1_Rho0 = bookHisto1D(11, 1, 1); - _hist_Ups4_Rho0 = bookHisto1D(12, 1, 1); - - _hist_cont_Omega = bookHisto1D(13, 1, 1); - _hist_Ups1_Omega = bookHisto1D(14, 1, 1); - } - - - void analyze(const Event& e) { - const double weight = e.weight(); - - // Find the upsilons - Particles upsilons; - // First in unstable final state - const UnstableParticles& ufs = apply(e, "UFS"); - foreach (const Particle& p, ufs.particles()) - if (p.pid() == 300553 || p.pid() == 553) upsilons.push_back(p); - // Then in whole event if that failed - if (upsilons.empty()) { - for(ConstGenParticlePtr p: HepMCUtils::particles(e.genEvent())) { - if (p->pdg_id() != 300553 && p->pdg_id() != 553) continue; - ConstGenVertexPtr pv = p->production_vertex(); - bool passed = true; - if (pv) { - for(ConstGenParticlePtr pp: HepMCUtils::particles(pv, Relatives::PARENTS)){ - if ( p->pdg_id() == pp->pdg_id() ) { - passed = false; - break; - } - } - } - if (passed) upsilons.push_back(Particle(*p)); - } - } - - if (upsilons.empty()) { // continuum - - _weightSum_cont += weight; - unsigned int nOmega(0), nRho0(0), nKStar0(0), nKStarPlus(0), nPhi(0); - foreach (const Particle& p, ufs.particles()) { - int id = p.abspid(); - double xp = 2.*p.E()/sqrtS(); - double beta = p.p3().mod()/p.E(); - if (id == 113) { - _hist_cont_Rho0->fill(xp, weight/beta); - ++nRho0; - } - else if (id == 313) { - _hist_cont_KStar0->fill(xp, weight/beta); - ++nKStar0; - } - else if (id == 223) { - _hist_cont_Omega->fill(xp, weight/beta); - ++nOmega; - } - else if (id == 323) { - _hist_cont_KStarPlus->fill(xp,weight/beta); - ++nKStarPlus; - } - else if (id == 333) { - ++nPhi; - } - } - /// @todo Replace with Counters and fill one-point Scatters at the end - _mult_cont_Omega ->fill(10.45, weight*nOmega ); - _mult_cont_Rho0 ->fill(10.45, weight*nRho0 ); - _mult_cont_KStar0 ->fill(10.45, weight*nKStar0 ); - _mult_cont_KStarPlus->fill(10.45, weight*nKStarPlus); - _mult_cont_Phi ->fill(10.45, weight*nPhi ); - - } else { // found an upsilon - - foreach (const Particle& ups, upsilons) { - const int parentId = ups.pid(); - (parentId == 553 ? _weightSum_Ups1 : _weightSum_Ups4) += weight; - Particles unstable; - // Find the decay products we want - findDecayProducts(ups.genParticle(),unstable); - /// @todo Update to new LT mk* functions - LorentzTransform cms_boost; - if (ups.p3().mod() > 0.001) - cms_boost = LorentzTransform::mkFrameTransformFromBeta(ups.momentum().betaVec()); - double mass = ups.mass(); - unsigned int nOmega(0),nRho0(0),nKStar0(0),nKStarPlus(0),nPhi(0); - foreach(const Particle & p , unstable) { - int id = p.abspid(); - FourMomentum p2 = cms_boost.transform(p.momentum()); - double xp = 2.*p2.E()/mass; - double beta = p2.p3().mod()/p2.E(); - if (id == 113) { - if (parentId == 553) _hist_Ups1_Rho0->fill(xp,weight/beta); - else _hist_Ups4_Rho0->fill(xp,weight/beta); - ++nRho0; - } - else if (id == 313) { - if (parentId == 553) _hist_Ups1_KStar0->fill(xp,weight/beta); - else _hist_Ups4_KStar0->fill(xp,weight/beta); - ++nKStar0; - } - else if (id == 223) { - if (parentId == 553) _hist_Ups1_Omega->fill(xp,weight/beta); - ++nOmega; - } - else if (id == 323) { - if (parentId == 553) _hist_Ups1_KStarPlus->fill(xp,weight/beta); - else _hist_Ups4_KStarPlus->fill(xp,weight/beta); - ++nKStarPlus; - } - else if (id == 333) { - ++nPhi; - } - } - if (parentId == 553) { - _mult_Ups1_Omega ->fill(9.46,weight*nOmega ); - _mult_Ups1_Rho0 ->fill(9.46,weight*nRho0 ); - _mult_Ups1_KStar0 ->fill(9.46,weight*nKStar0 ); - _mult_Ups1_KStarPlus->fill(9.46,weight*nKStarPlus); - _mult_Ups1_Phi ->fill(9.46,weight*nPhi ); - } - else { - _mult_Ups4_Omega ->fill(10.58,weight*nOmega ); - _mult_Ups4_Rho0 ->fill(10.58,weight*nRho0 ); - _mult_Ups4_KStar0 ->fill(10.58,weight*nKStar0 ); - _mult_Ups4_KStarPlus->fill(10.58,weight*nKStarPlus); - _mult_Ups4_Phi ->fill(10.58,weight*nPhi ); - } - } - } - - } - - - void finalize() { - if (_weightSum_cont > 0.) { - /// @todo Replace with Counters and fill one-point Scatters at the end - scale(_mult_cont_Omega , 1./_weightSum_cont); - scale(_mult_cont_Rho0 , 1./_weightSum_cont); - scale(_mult_cont_KStar0 , 1./_weightSum_cont); - scale(_mult_cont_KStarPlus, 1./_weightSum_cont); - scale(_mult_cont_Phi , 1./_weightSum_cont); - scale(_hist_cont_KStarPlus, 1./_weightSum_cont); - scale(_hist_cont_KStar0 , 1./_weightSum_cont); - scale(_hist_cont_Rho0 , 1./_weightSum_cont); - scale(_hist_cont_Omega , 1./_weightSum_cont); - } - if (_weightSum_Ups1 > 0.) { - /// @todo Replace with Counters and fill one-point Scatters at the end - scale(_mult_Ups1_Omega , 1./_weightSum_Ups1); - scale(_mult_Ups1_Rho0 , 1./_weightSum_Ups1); - scale(_mult_Ups1_KStar0 , 1./_weightSum_Ups1); - scale(_mult_Ups1_KStarPlus, 1./_weightSum_Ups1); - scale(_mult_Ups1_Phi , 1./_weightSum_Ups1); - scale(_hist_Ups1_KStarPlus, 1./_weightSum_Ups1); - scale(_hist_Ups1_KStar0 , 1./_weightSum_Ups1); - scale(_hist_Ups1_Rho0 , 1./_weightSum_Ups1); - scale(_hist_Ups1_Omega , 1./_weightSum_Ups1); - } - if (_weightSum_Ups4 > 0.) { - /// @todo Replace with Counters and fill one-point Scatters at the end - scale(_mult_Ups4_Omega , 1./_weightSum_Ups4); - scale(_mult_Ups4_Rho0 , 1./_weightSum_Ups4); - scale(_mult_Ups4_KStar0 , 1./_weightSum_Ups4); - scale(_mult_Ups4_KStarPlus, 1./_weightSum_Ups4); - scale(_mult_Ups4_Phi , 1./_weightSum_Ups4); - scale(_hist_Ups4_KStarPlus, 1./_weightSum_Ups4); - scale(_hist_Ups4_KStar0 , 1./_weightSum_Ups4); - scale(_hist_Ups4_Rho0 , 1./_weightSum_Ups4); - } - } - - - private: - - //@{ - Histo1DPtr _mult_cont_Omega, _mult_cont_Rho0, _mult_cont_KStar0, _mult_cont_KStarPlus, _mult_cont_Phi; - Histo1DPtr _mult_Ups1_Omega, _mult_Ups1_Rho0, _mult_Ups1_KStar0, _mult_Ups1_KStarPlus, _mult_Ups1_Phi; - Histo1DPtr _mult_Ups4_Omega, _mult_Ups4_Rho0, _mult_Ups4_KStar0, _mult_Ups4_KStarPlus, _mult_Ups4_Phi; - Histo1DPtr _hist_cont_KStarPlus, _hist_Ups1_KStarPlus, _hist_Ups4_KStarPlus; - Histo1DPtr _hist_cont_KStar0, _hist_Ups1_KStar0, _hist_Ups4_KStar0 ; - Histo1DPtr _hist_cont_Rho0, _hist_Ups1_Rho0, _hist_Ups4_Rho0; - Histo1DPtr _hist_cont_Omega, _hist_Ups1_Omega; - - double _weightSum_cont,_weightSum_Ups1,_weightSum_Ups4; - //@} - - - void findDecayProducts(ConstGenParticlePtr p, Particles& unstable) { - ConstGenVertexPtr dv = p->end_vertex(); - /// @todo Use better looping - for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ - int id = abs(pp->pdg_id()); - if (id == 113 || id == 313 || id == 323 || - id == 333 || id == 223 ) { - unstable.push_back(Particle(pp)); - } - else if (pp->end_vertex()) - findDecayProducts(pp, unstable); - } - } - - - }; - - - // The hook for the plugin system - DECLARE_RIVET_PLUGIN(ARGUS_1993_S2789213); - -} diff --git a/analyses/pluginMisc/BABAR_2003_I593379.cc b/analyses/pluginMisc/BABAR_2003_I593379.cc deleted file mode 100644 --- a/analyses/pluginMisc/BABAR_2003_I593379.cc +++ /dev/null @@ -1,186 +0,0 @@ -// -*- C++ -*- -#include "Rivet/Analysis.hh" -#include "Rivet/Projections/Beam.hh" -#include "Rivet/Projections/UnstableParticles.hh" - -namespace Rivet { - - - /// @brief Babar charmonium spectra - /// @author Peter Richardson - class BABAR_2003_I593379 : public Analysis { - public: - - BABAR_2003_I593379() - : Analysis("BABAR_2003_I593379"), _weightSum(0.) - { } - - - void analyze(const Event& e) { - const double weight = e.weight(); - - // Find the charmonia - Particles upsilons; - // First in unstable final state - const UnstableParticles& ufs = apply(e, "UFS"); - foreach (const Particle& p, ufs.particles()) - if (p.pid() == 300553) upsilons.push_back(p); - // Then in whole event if fails - if (upsilons.empty()) { - for(ConstGenParticlePtr p: HepMCUtils::particles(e.genEvent())) { - if (p->pdg_id() != 300553) continue; - ConstGenVertexPtr pv = p->production_vertex(); - bool passed = true; - if (pv) { - for(ConstGenParticlePtr pp: HepMCUtils::particles(pv, Relatives::PARENTS)){ - if ( p->pdg_id() == pp->pdg_id() ) { - passed = false; - break; - } - } - } - if (passed) upsilons.push_back(Particle(p)); - } - } - - // Find upsilons - foreach (const Particle& p, upsilons) { - _weightSum += weight; - // Find the charmonium resonances - /// @todo Use Rivet::Particles - vector allJpsi, primaryJpsi, Psiprime, all_chi_c1, all_chi_c2, primary_chi_c1, primary_chi_c2; - findDecayProducts(p.genParticle(), allJpsi, primaryJpsi, Psiprime, - all_chi_c1, all_chi_c2, primary_chi_c1, primary_chi_c2); - const LorentzTransform cms_boost = LorentzTransform::mkFrameTransformFromBeta(p.mom().betaVec()); - for (size_t i = 0; i < allJpsi.size(); i++) { - const double pcm = cms_boost.transform(FourMomentum(allJpsi[i]->momentum())).p(); - _hist_all_Jpsi->fill(pcm, weight); - } - _mult_JPsi->fill(10.58, weight*double(allJpsi.size())); - for (size_t i = 0; i < primaryJpsi.size(); i++) { - const double pcm = cms_boost.transform(FourMomentum(primaryJpsi[i]->momentum())).p(); - _hist_primary_Jpsi->fill(pcm, weight); - } - _mult_JPsi_direct->fill(10.58, weight*double(primaryJpsi.size())); - for (size_t i=0; imomentum())).p(); - _hist_Psi_prime->fill(pcm, weight); - } - _mult_Psi2S->fill(10.58, weight*double(Psiprime.size())); - for (size_t i = 0; i < all_chi_c1.size(); i++) { - const double pcm = cms_boost.transform(FourMomentum(all_chi_c1[i]->momentum())).p(); - _hist_chi_c1->fill(pcm, weight); - } - _mult_chi_c1->fill(10.58, weight*double(all_chi_c1.size())); - _mult_chi_c1_direct->fill(10.58, weight*double(primary_chi_c1.size())); - for (size_t i = 0; i < all_chi_c2.size(); i++) { - const double pcm = cms_boost.transform(FourMomentum(all_chi_c2[i]->momentum())).p(); - _hist_chi_c2->fill(pcm, weight); - } - _mult_chi_c2->fill(10.58, weight*double(all_chi_c2.size())); - _mult_chi_c2_direct->fill(10.58, weight*double(primary_chi_c2.size())); - } - } // analyze - - - void finalize() { - scale(_hist_all_Jpsi , 0.5*0.1/_weightSum); - scale(_hist_chi_c1 , 0.5*0.1/_weightSum); - scale(_hist_chi_c2 , 0.5*0.1/_weightSum); - scale(_hist_Psi_prime , 0.5*0.1/_weightSum); - scale(_hist_primary_Jpsi , 0.5*0.1/_weightSum); - scale(_mult_JPsi , 0.5*100./_weightSum); - scale(_mult_JPsi_direct , 0.5*100./_weightSum); - scale(_mult_chi_c1 , 0.5*100./_weightSum); - scale(_mult_chi_c1_direct, 0.5*100./_weightSum); - scale(_mult_chi_c2 , 0.5*100./_weightSum); - scale(_mult_chi_c2_direct, 0.5*100./_weightSum); - scale(_mult_Psi2S , 0.5*100./_weightSum); - } // finalize - - - void init() { - declare(UnstableParticles(), "UFS"); - - _mult_JPsi = bookHisto1D(1, 1, 1); - _mult_JPsi_direct = bookHisto1D(1, 1, 2); - _mult_chi_c1 = bookHisto1D(1, 1, 3); - _mult_chi_c1_direct = bookHisto1D(1, 1, 4); - _mult_chi_c2 = bookHisto1D(1, 1, 5); - _mult_chi_c2_direct = bookHisto1D(1, 1, 6); - _mult_Psi2S = bookHisto1D(1, 1, 7); - _hist_all_Jpsi = bookHisto1D(6, 1, 1); - _hist_chi_c1 = bookHisto1D(7, 1, 1); - _hist_chi_c2 = bookHisto1D(7, 1, 2); - _hist_Psi_prime = bookHisto1D(8, 1, 1); - _hist_primary_Jpsi = bookHisto1D(10, 1, 1); - } // init - - private: - - //@{ - // count of weights - double _weightSum; - /// Histograms - Histo1DPtr _hist_all_Jpsi; - Histo1DPtr _hist_chi_c1; - Histo1DPtr _hist_chi_c2; - Histo1DPtr _hist_Psi_prime; - Histo1DPtr _hist_primary_Jpsi; - - Histo1DPtr _mult_JPsi; - Histo1DPtr _mult_JPsi_direct; - Histo1DPtr _mult_chi_c1; - Histo1DPtr _mult_chi_c1_direct; - Histo1DPtr _mult_chi_c2; - Histo1DPtr _mult_chi_c2_direct; - Histo1DPtr _mult_Psi2S; - //@} - - void findDecayProducts(ConstGenParticlePtr p, - vector& allJpsi, - vector& primaryJpsi, - vector& Psiprime, - vector& all_chi_c1, vector& all_chi_c2, - vector& primary_chi_c1, vector& primary_chi_c2) { - ConstGenVertexPtr dv = p->end_vertex(); - bool isOnium = false; - /// @todo Use better looping - for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::PARENTS)){ - int id = pp->pdg_id(); - id = id%1000; - id -= id%10; - id /= 10; - if (id==44) isOnium = true; - } - /// @todo Use better looping - for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ - int id = pp->pdg_id(); - if (id==100443) { - Psiprime.push_back(pp); - } - else if (id==20443) { - all_chi_c1.push_back(pp); - if (!isOnium) primary_chi_c1.push_back(pp); - } - else if (id==445) { - all_chi_c2.push_back(pp); - if (!isOnium) primary_chi_c2.push_back(pp); - } - else if (id==443) { - allJpsi.push_back(pp); - if (!isOnium) primaryJpsi.push_back(pp); - } - if (pp->end_vertex()) { - findDecayProducts(pp, allJpsi, primaryJpsi, Psiprime, all_chi_c1, all_chi_c2, primary_chi_c1, primary_chi_c2); - } - } - } - - }; - - - // The hook for the plugin system - DECLARE_RIVET_PLUGIN(BABAR_2003_I593379); - -} diff --git a/analyses/pluginMisc/BABAR_2005_S6181155.cc b/analyses/pluginMisc/BABAR_2005_S6181155.cc deleted file mode 100644 --- a/analyses/pluginMisc/BABAR_2005_S6181155.cc +++ /dev/null @@ -1,145 +0,0 @@ -// -*- C++ -*- -#include "Rivet/Analysis.hh" -#include "Rivet/Projections/Beam.hh" -#include "Rivet/Projections/UnstableParticles.hh" - -namespace Rivet { - - - /// @brief BABAR Xi_c baryons from fragmentation - /// @author Peter Richardson - class BABAR_2005_S6181155 : public Analysis { - public: - - BABAR_2005_S6181155() - : Analysis("BABAR_2005_S6181155") - { } - - void init() { - declare(Beam(), "Beams"); - declare(UnstableParticles(), "UFS"); - _histOnResonanceA = bookHisto1D(1,1,1); - _histOnResonanceB = bookHisto1D(2,1,1); - _histOffResonance = bookHisto1D(2,1,2); - _sigma = bookHisto1D(3,1,1); - _histOnResonanceA_norm = bookHisto1D(4,1,1); - _histOnResonanceB_norm = bookHisto1D(5,1,1); - _histOffResonance_norm = bookHisto1D(5,1,2); - - } - - void analyze(const Event& e) { - const double weight = e.weight(); - - // Loop through unstable FS particles and look for charmed mesons/baryons - const UnstableParticles& ufs = apply(e, "UFS"); - - const Beam beamproj = apply(e, "Beams"); - const ParticlePair& beams = beamproj.beams(); - const FourMomentum mom_tot = beams.first.momentum() + beams.second.momentum(); - const LorentzTransform cms_boost = LorentzTransform::mkFrameTransformFromBeta(mom_tot.betaVec()); - const double s = sqr(beamproj.sqrtS()); - - const bool onresonance = fuzzyEquals(beamproj.sqrtS()/GeV, 10.58, 2E-3); - - foreach (const Particle& p, ufs.particles()) { - // 3-momentum in CMS frame - - const double mom = cms_boost.transform(p.momentum()).vector3().mod(); - // Only looking at Xi_c^0 - if (p.abspid() != 4132 ) continue; - if (onresonance) { - _histOnResonanceA_norm->fill(mom,weight); - _histOnResonanceB_norm->fill(mom,weight); - } - else { - _histOffResonance_norm->fill(mom,s/sqr(10.58)*weight); - } - MSG_DEBUG("mom = " << mom); - // off-resonance cross section - if (checkDecay(p.genParticle())) { - if (onresonance) { - _histOnResonanceA->fill(mom,weight); - _histOnResonanceB->fill(mom,weight); - } - else { - _histOffResonance->fill(mom,s/sqr(10.58)*weight); - _sigma->fill(10.6,weight); - } - } - } - } - - - void finalize() { - scale(_histOnResonanceA, crossSection()/femtobarn/sumOfWeights()); - scale(_histOnResonanceB, crossSection()/femtobarn/sumOfWeights()); - scale(_histOffResonance, crossSection()/femtobarn/sumOfWeights()); - scale(_sigma , crossSection()/femtobarn/sumOfWeights()); - normalize(_histOnResonanceA_norm); - normalize(_histOnResonanceB_norm); - normalize(_histOffResonance_norm); - } - - - private: - - //@{ - /// Histograms - Histo1DPtr _histOnResonanceA; - Histo1DPtr _histOnResonanceB; - Histo1DPtr _histOffResonance; - Histo1DPtr _sigma ; - Histo1DPtr _histOnResonanceA_norm; - Histo1DPtr _histOnResonanceB_norm; - Histo1DPtr _histOffResonance_norm; - //@} - - bool checkDecay(ConstGenParticlePtr p) { - unsigned int nstable = 0, npip = 0, npim = 0; - unsigned int nXim = 0, nXip = 0; - findDecayProducts(p, nstable, npip, npim, nXip, nXim); - int id = p->pdg_id(); - // Xi_c - if (id == 4132) { - if (nstable == 2 && nXim == 1 && npip == 1) return true; - } - else if (id == -4132) { - if (nstable == 2 && nXip == 1 && npim == 1) return true; - } - return false; - } - - void findDecayProducts(ConstGenParticlePtr p, - unsigned int& nstable, - unsigned int& npip, unsigned int& npim, - unsigned int& nXip, unsigned int& nXim) { - ConstGenVertexPtr dv = p->end_vertex(); - /// @todo Use better looping - for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ - int id = pp->pdg_id(); - if (id==3312) { - ++nXim; - ++nstable; - } else if (id == -3312) { - ++nXip; - ++nstable; - } else if(id == 111 || id == 221) { - ++nstable; - } else if (pp->end_vertex()) { - findDecayProducts(pp, nstable, npip, npim, nXip, nXim); - } else { - if (id != 22) ++nstable; - if (id == 211) ++npip; - else if(id == -211) ++npim; - } - } - } - - }; - - - // The hook for the plugin system - DECLARE_RIVET_PLUGIN(BABAR_2005_S6181155); - -} diff --git a/analyses/pluginMisc/BABAR_2005_S6181155.plot b/analyses/pluginMisc/BABAR_2005_S6181155.plot deleted file mode 100644 --- a/analyses/pluginMisc/BABAR_2005_S6181155.plot +++ /dev/null @@ -1,42 +0,0 @@ -# BEGIN PLOT /BABAR_2005_S6181155/d01-x01-y01 -Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ with $\Xi_c^0\to\Xi^-\pi^+$ at the $\Upsilon(4S)$ -XLabel=$p_{\Xi_c^0}$ [GeV] -YLabel=$\text{d}\sigma/\text{d}p_{\Xi_c^0}$ [fb/GeV] -LogY=0 -# END PLOT -# BEGIN PLOT /BABAR_2005_S6181155/d02-x01-y01 -Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ with $\Xi_c^0\to\Xi^-\pi^+$ at the $\Upsilon(4S)$ -XLabel=$p_{\Xi_c^0}$ [GeV] -YLabel=$\text{d}\sigma/\text{d}p_{\Xi_c^0}$ [fb/GeV] -LogY=0 -# END PLOT -# BEGIN PLOT /BABAR_2005_S6181155/d02-x01-y02 -Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ with $\Xi_c^0\to\Xi^-\pi^+$ in the continuum region -XLabel=$p_{\Xi_c^0}$ [GeV] -YLabel=$\text{d}\sigma/\text{d}p_{\Xi_c^0}$ [fb/GeV] -LogY=0 -# END PLOT -# BEGIN PLOT /BABAR_2005_S6181155/d03-x01-y01 -Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ with $\Xi_c^0\to\Xi^-\pi^+$ -XLabel=$\sqrt{s}$ [GeV] -YLabel=$\sigma$ [fb] -LogY=0 -# END PLOT -# BEGIN PLOT /BABAR_2005_S6181155/d04-x01-y01 -Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ at the $\Upsilon(4S)$ -XLabel=$p_{\Xi_c^0}$ [GeV] -YLabel=$1/\sigma\text{d}\sigma/\text{d}p_{\Xi_c^0}$ [$\text{GeV}^{-1}$] -LogY=0 -# END PLOT -# BEGIN PLOT /BABAR_2005_S6181155/d05-x01-y01 -Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ at the $\Upsilon(4S)$ -XLabel=$p_{\Xi_c^0}$ [GeV] -YLabel=$1/\sigma\text{d}\sigma/\text{d}p_{\Xi_c^0}$ [$\text{GeV}^{-1}$] -LogY=0 -# END PLOT -# BEGIN PLOT /BABAR_2005_S6181155/d05-x01-y02 -Title=$\sigma(e^+e^-\to \Xi_c^0+\bar{\Xi}_c^0+X)$ in the continuum region -XLabel=$p_{\Xi_c^0}$ [GeV] -YLabel=$1/\sigma\text{d}\sigma/\text{d}p_{\Xi_c^0}$ [$\text{GeV}^{-1}$] -LogY=0 -# END PLOT diff --git a/analyses/pluginMisc/BABAR_2005_S6181155.yoda b/analyses/pluginMisc/BABAR_2005_S6181155.yoda deleted file mode 100644 --- a/analyses/pluginMisc/BABAR_2005_S6181155.yoda +++ /dev/null @@ -1,149 +0,0 @@ -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d01-x01-y01 -IsRef: 1 -Path: /REF/BABAR_2005_S6181155/d01-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -1.000000e-01 1.000000e-01 1.000000e-01 5.000000e+01 1.118034e+01 1.118034e+01 -3.000000e-01 1.000000e-01 1.000000e-01 2.800000e+02 3.201562e+01 3.201562e+01 -5.000000e-01 1.000000e-01 1.000000e-01 5.050000e+02 5.000000e+01 5.000000e+01 -7.000000e-01 1.000000e-01 1.000000e-01 5.100000e+02 5.000000e+01 5.000000e+01 -9.000000e-01 1.000000e-01 1.000000e-01 4.200000e+02 4.609772e+01 4.609772e+01 -1.100000e+00 1.000000e-01 1.000000e-01 3.250000e+02 3.535534e+01 3.535534e+01 -1.300000e+00 1.000000e-01 1.000000e-01 1.400000e+02 2.692582e+01 2.692582e+01 -1.500000e+00 1.000000e-01 1.000000e-01 1.150000e+02 2.236068e+01 2.236068e+01 -1.700000e+00 1.000000e-01 1.000000e-01 1.050000e+02 2.236068e+01 2.236068e+01 -1.900000e+00 1.000000e-01 1.000000e-01 1.000000e+02 1.802776e+01 1.802776e+01 -2.100000e+00 1.000000e-01 1.000000e-01 1.150000e+02 1.802776e+01 1.802776e+01 -2.300000e+00 1.000000e-01 1.000000e-01 1.300000e+02 1.802776e+01 1.802776e+01 -2.500000e+00 1.000000e-01 1.000000e-01 1.700000e+02 2.121320e+01 2.121320e+01 -2.700000e+00 1.000000e-01 1.000000e-01 1.850000e+02 2.121320e+01 2.121320e+01 -2.900000e+00 1.000000e-01 1.000000e-01 2.200000e+02 2.121320e+01 2.121320e+01 -3.100000e+00 1.000000e-01 1.000000e-01 2.300000e+02 2.236068e+01 2.236068e+01 -3.300000e+00 1.000000e-01 1.000000e-01 2.100000e+02 1.802776e+01 1.802776e+01 -3.500000e+00 1.000000e-01 1.000000e-01 1.950000e+02 1.802776e+01 1.802776e+01 -3.700000e+00 1.000000e-01 1.000000e-01 1.100000e+02 1.414214e+01 1.414214e+01 -3.900000e+00 1.000000e-01 1.000000e-01 1.000000e+02 1.118034e+01 1.118034e+01 -4.100000e+00 1.000000e-01 1.000000e-01 5.500000e+01 1.118034e+01 1.118034e+01 -4.300000e+00 1.000000e-01 1.000000e-01 1.100000e+01 2.915476e+00 2.915476e+00 -4.500000e+00 1.000000e-01 1.000000e-01 4.000000e+00 1.802776e+00 1.802776e+00 -4.700000e+00 1.000000e-01 1.000000e-01 0.000000e+00 7.071068e-01 7.071068e-01 -4.900000e+00 1.000000e-01 1.000000e-01 1.000000e+00 1.118034e+00 1.118034e+00 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d02-x01-y01 -IsRef: 1 -Path: /REF/BABAR_2005_S6181155/d02-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.250000e-01 2.250000e-01 2.250000e-01 1.955556e+02 1.911628e+01 1.911628e+01 -6.750000e-01 2.250000e-01 2.250000e-01 4.844444e+02 4.274530e+01 4.274530e+01 -1.125000e+00 2.250000e-01 2.250000e-01 2.844444e+02 2.845833e+01 2.845833e+01 -1.575000e+00 2.250000e-01 2.250000e-01 1.133333e+02 1.602467e+01 1.602467e+01 -1.975000e+00 1.750000e-01 1.750000e-01 1.057143e+02 1.428571e+01 1.428571e+01 -2.425000e+00 2.750000e-01 2.750000e-01 1.509091e+02 1.420045e+01 1.420045e+01 -3.000000e+00 3.000000e-01 3.000000e-01 2.216667e+02 1.795055e+01 1.795055e+01 -3.650000e+00 3.500000e-01 3.500000e-01 1.414286e+02 1.220572e+01 1.220572e+01 -4.350000e+00 3.500000e-01 3.500000e-01 2.000000e+01 2.020305e+00 2.020305e+00 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d02-x01-y02 -IsRef: 1 -Path: /REF/BABAR_2005_S6181155/d02-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.250000e-01 2.250000e-01 2.250000e-01 2.222222e+01 2.675910e+01 2.675910e+01 -6.750000e-01 2.250000e-01 2.250000e-01 3.555556e+01 4.687783e+01 4.687783e+01 -1.125000e+00 2.250000e-01 2.250000e-01 -1.555556e+01 4.466611e+01 4.466611e+01 -1.575000e+00 2.250000e-01 2.250000e-01 3.555556e+01 4.024616e+01 4.024616e+01 -1.975000e+00 1.750000e-01 1.750000e-01 6.571429e+01 3.757985e+01 3.757985e+01 -2.425000e+00 2.750000e-01 2.750000e-01 1.654545e+02 3.175318e+01 3.175318e+01 -3.000000e+00 3.000000e-01 3.000000e-01 2.800000e+02 3.308239e+01 3.308239e+01 -3.650000e+00 3.500000e-01 3.500000e-01 1.271429e+02 1.743794e+01 1.743794e+01 -4.350000e+00 3.500000e-01 3.500000e-01 2.428571e+01 6.388766e+00 6.388766e+00 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d03-x01-y01 -IsRef: 1 -Path: /REF/BABAR_2005_S6181155/d03-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -1.058000e+01 5.000000e-01 5.000000e-01 3.880000e+02 5.658622e+01 5.658622e+01 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d04-x01-y01 -IsRef: 1 -Path: /REF/BABAR_2005_S6181155/d04-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -1.000000e-01 1.000000e-01 1.000000e-01 5.832944e-02 1.304286e-02 1.304286e-02 -3.000000e-01 1.000000e-01 1.000000e-01 3.266449e-01 3.734907e-02 3.734907e-02 -5.000000e-01 1.000000e-01 1.000000e-01 5.891274e-01 5.832944e-02 5.832944e-02 -7.000000e-01 1.000000e-01 1.000000e-01 5.949603e-01 5.832944e-02 5.832944e-02 -9.000000e-01 1.000000e-01 1.000000e-01 4.899673e-01 5.377709e-02 5.377709e-02 -1.100000e+00 1.000000e-01 1.000000e-01 3.791414e-01 4.124515e-02 4.124515e-02 -1.300000e+00 1.000000e-01 1.000000e-01 1.633224e-01 3.141136e-02 3.141136e-02 -1.500000e+00 1.000000e-01 1.000000e-01 1.341577e-01 2.608572e-02 2.608572e-02 -1.700000e+00 1.000000e-01 1.000000e-01 1.224918e-01 2.608572e-02 2.608572e-02 -1.900000e+00 1.000000e-01 1.000000e-01 1.166589e-01 2.103098e-02 2.103098e-02 -2.100000e+00 1.000000e-01 1.000000e-01 1.341577e-01 2.103098e-02 2.103098e-02 -2.300000e+00 1.000000e-01 1.000000e-01 1.516566e-01 2.103098e-02 2.103098e-02 -2.500000e+00 1.000000e-01 1.000000e-01 1.983201e-01 2.474708e-02 2.474708e-02 -2.700000e+00 1.000000e-01 1.000000e-01 2.158189e-01 2.474708e-02 2.474708e-02 -2.900000e+00 1.000000e-01 1.000000e-01 2.566496e-01 2.474708e-02 2.474708e-02 -3.100000e+00 1.000000e-01 1.000000e-01 2.683154e-01 2.608572e-02 2.608572e-02 -3.300000e+00 1.000000e-01 1.000000e-01 2.449837e-01 2.103098e-02 2.103098e-02 -3.500000e+00 1.000000e-01 1.000000e-01 2.274848e-01 2.103098e-02 2.103098e-02 -3.700000e+00 1.000000e-01 1.000000e-01 1.283248e-01 1.649806e-02 1.649806e-02 -3.900000e+00 1.000000e-01 1.000000e-01 1.166589e-01 1.304286e-02 1.304286e-02 -4.100000e+00 1.000000e-01 1.000000e-01 6.416239e-02 1.304286e-02 1.304286e-02 -4.300000e+00 1.000000e-01 1.000000e-01 1.283248e-02 3.401162e-03 3.401162e-03 -4.500000e+00 1.000000e-01 1.000000e-01 4.666356e-03 2.103098e-03 2.103098e-03 -4.700000e+00 1.000000e-01 1.000000e-01 0.000000e+00 8.249029e-04 8.249029e-04 -4.900000e+00 1.000000e-01 1.000000e-01 1.166589e-03 1.304286e-03 1.304286e-03 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d05-x01-y01 -IsRef: 1 -Path: /REF/BABAR_2005_S6181155/d05-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.250000e-01 2.250000e-01 2.250000e-01 2.297951e-01 2.246331e-02 2.246331e-02 -6.750000e-01 2.250000e-01 2.250000e-01 5.692649e-01 5.022949e-02 5.022949e-02 -1.125000e+00 2.250000e-01 2.250000e-01 3.342472e-01 3.344105e-02 3.344105e-02 -1.575000e+00 2.250000e-01 2.250000e-01 1.331766e-01 1.883040e-02 1.883040e-02 -1.975000e+00 1.750000e-01 1.750000e-01 1.242236e-01 1.678697e-02 1.678697e-02 -2.425000e+00 2.750000e-01 2.750000e-01 1.773315e-01 1.668678e-02 1.668678e-02 -3.000000e+00 3.000000e-01 3.000000e-01 2.604779e-01 2.109348e-02 2.109348e-02 -3.650000e+00 3.500000e-01 3.500000e-01 1.661911e-01 1.434280e-02 1.434280e-02 -4.350000e+00 3.500000e-01 3.500000e-01 2.350176e-02 2.374036e-03 2.374036e-03 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2005_S6181155/d05-x01-y02 -IsRef: 1 -Path: /REF/BABAR_2005_S6181155/d05-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.250000e-01 2.250000e-01 2.250000e-01 5.253480e-02 6.326028e-02 6.326028e-02 -6.750000e-01 2.250000e-01 2.250000e-01 8.405570e-02 1.108223e-01 1.108223e-01 -1.125000e+00 2.250000e-01 2.250000e-01 -3.677437e-02 1.055936e-01 1.055936e-01 -1.575000e+00 2.250000e-01 2.250000e-01 8.405570e-02 9.514459e-02 9.514459e-02 -1.975000e+00 1.750000e-01 1.750000e-01 1.553529e-01 8.884125e-02 8.884125e-02 -2.425000e+00 2.750000e-01 2.750000e-01 3.911454e-01 7.506662e-02 7.506662e-02 -3.000000e+00 3.000000e-01 3.000000e-01 6.619385e-01 7.820896e-02 7.820896e-02 -3.650000e+00 3.500000e-01 3.500000e-01 3.005742e-01 4.122444e-02 4.122444e-02 -4.350000e+00 3.500000e-01 3.500000e-01 5.741303e-02 1.510347e-02 1.510347e-02 -END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/BABAR_2007_S7266081.cc b/analyses/pluginMisc/BABAR_2007_S7266081.cc deleted file mode 100644 --- a/analyses/pluginMisc/BABAR_2007_S7266081.cc +++ /dev/null @@ -1,174 +0,0 @@ -// -*- C++ -*- -#include -#include "Rivet/Analysis.hh" -#include "Rivet/Projections/UnstableParticles.hh" - -namespace Rivet { - - - /// @brief BABAR tau lepton to three charged hadrons - /// @author Peter Richardson - class BABAR_2007_S7266081 : public Analysis { - public: - - BABAR_2007_S7266081() - : Analysis("BABAR_2007_S7266081"), - _weight_total(0), - _weight_pipipi(0), _weight_Kpipi(0), _weight_KpiK(0), _weight_KKK(0) - { } - - - void init() { - declare(UnstableParticles(), "UFS"); - _hist_pipipi_pipipi = bookHisto1D( 1, 1, 1); - _hist_pipipi_pipi = bookHisto1D( 2, 1, 1); - _hist_Kpipi_Kpipi = bookHisto1D( 3, 1, 1); - _hist_Kpipi_Kpi = bookHisto1D( 4, 1, 1); - _hist_Kpipi_pipi = bookHisto1D( 5, 1, 1); - _hist_KpiK_KpiK = bookHisto1D( 6, 1, 1); - _hist_KpiK_KK = bookHisto1D( 7, 1, 1); - _hist_KpiK_piK = bookHisto1D( 8, 1, 1); - _hist_KKK_KKK = bookHisto1D( 9, 1, 1); - _hist_KKK_KK = bookHisto1D(10, 1, 1); - } - - - void analyze(const Event& e) { - double weight = e.weight(); - // Find the taus - Particles taus; - foreach(const Particle& p, apply(e, "UFS").particles(Cuts::pid==PID::TAU)) { - _weight_total += weight; - Particles pip, pim, Kp, Km; - unsigned int nstable = 0; - // Find the decay products we want - findDecayProducts(p, nstable, pip, pim, Kp, Km); - if (p.pid() < 0) { - swap(pip, pim); - swap(Kp, Km ); - } - if (nstable != 4) continue; - // pipipi - if (pim.size() == 2 && pip.size() == 1) { - _weight_pipipi += weight; - _hist_pipipi_pipipi-> - fill((pip[0].momentum()+pim[0].momentum()+pim[1].momentum()).mass(), weight); - _hist_pipipi_pipi-> - fill((pip[0].momentum()+pim[0].momentum()).mass(), weight); - _hist_pipipi_pipi-> - fill((pip[0].momentum()+pim[1].momentum()).mass(), weight); - } - else if (pim.size() == 1 && pip.size() == 1 && Km.size() == 1) { - _weight_Kpipi += weight; - _hist_Kpipi_Kpipi-> - fill((pim[0].momentum()+pip[0].momentum()+Km[0].momentum()).mass(), weight); - _hist_Kpipi_Kpi-> - fill((pip[0].momentum()+Km[0].momentum()).mass(), weight); - _hist_Kpipi_pipi-> - fill((pim[0].momentum()+pip[0].momentum()).mass(), weight); - } - else if (Kp.size() == 1 && Km.size() == 1 && pim.size() == 1) { - _weight_KpiK += weight; - _hist_KpiK_KpiK-> - fill((Kp[0].momentum()+Km[0].momentum()+pim[0].momentum()).mass(), weight); - _hist_KpiK_KK-> - fill((Kp[0].momentum()+Km[0].momentum()).mass(), weight); - _hist_KpiK_piK-> - fill((Kp[0].momentum()+pim[0].momentum()).mass(), weight); - } - else if (Kp.size() == 1 && Km.size() == 2) { - _weight_KKK += weight; - _hist_KKK_KKK-> - fill((Kp[0].momentum()+Km[0].momentum()+Km[1].momentum()).mass(), weight); - _hist_KKK_KK-> - fill((Kp[0].momentum()+Km[0].momentum()).mass(), weight); - _hist_KKK_KK-> - fill((Kp[0].momentum()+Km[1].momentum()).mass(), weight); - } - } - } - - - void finalize() { - if (_weight_pipipi > 0.) { - scale(_hist_pipipi_pipipi, 1.0/_weight_pipipi); - scale(_hist_pipipi_pipi , 0.5/_weight_pipipi); - } - if (_weight_Kpipi > 0.) { - scale(_hist_Kpipi_Kpipi , 1.0/_weight_Kpipi); - scale(_hist_Kpipi_Kpi , 1.0/_weight_Kpipi); - scale(_hist_Kpipi_pipi , 1.0/_weight_Kpipi); - } - if (_weight_KpiK > 0.) { - scale(_hist_KpiK_KpiK , 1.0/_weight_KpiK); - scale(_hist_KpiK_KK , 1.0/_weight_KpiK); - scale(_hist_KpiK_piK , 1.0/_weight_KpiK); - } - if (_weight_KKK > 0.) { - scale(_hist_KKK_KKK , 1.0/_weight_KKK); - scale(_hist_KKK_KK , 0.5/_weight_KKK); - } - /// @note Using autobooking for these scatters since their x values are not really obtainable from the MC data - bookScatter2D(11, 1, 1, true)->point(0).setY(100*_weight_pipipi/_weight_total, 100*sqrt(_weight_pipipi)/_weight_total); - bookScatter2D(12, 1, 1, true)->point(0).setY(100*_weight_Kpipi/_weight_total, 100*sqrt(_weight_Kpipi)/_weight_total); - bookScatter2D(13, 1, 1, true)->point(0).setY(100*_weight_KpiK/_weight_total, 100*sqrt(_weight_KpiK)/_weight_total); - bookScatter2D(14, 1, 1, true)->point(0).setY(100*_weight_KKK/_weight_total, 100*sqrt(_weight_KKK)/_weight_total); - } - - - private: - - //@{ - - // Histograms - Histo1DPtr _hist_pipipi_pipipi, _hist_pipipi_pipi; - Histo1DPtr _hist_Kpipi_Kpipi, _hist_Kpipi_Kpi, _hist_Kpipi_pipi; - Histo1DPtr _hist_KpiK_KpiK, _hist_KpiK_KK, _hist_KpiK_piK; - Histo1DPtr _hist_KKK_KKK, _hist_KKK_KK; - - // Weights counters - double _weight_total, _weight_pipipi, _weight_Kpipi, _weight_KpiK, _weight_KKK; - - //@} - - void findDecayProducts(const Particle &mother, - unsigned int & nstable, - Particles& pip, Particles& pim, - Particles& Kp, Particles& Km) { - for (const Particle &p : mother.children()) { - long id = p.pdgId(); - if (id == PID::PI0 ) - ++nstable; - else if (id == PID::K0S) - ++nstable; - else if (id == PID::PIPLUS) { - pip.push_back(p); - ++nstable; - } - else if (id == PID::PIMINUS) { - pim.push_back(p); - ++nstable; - } - else if (id == PID::KPLUS) { - Kp.push_back(p); - ++nstable; - } - else if (id == PID::KMINUS) { - Km.push_back(p); - ++nstable; - } - else if (!p.children().empty()) { - findDecayProducts(p, nstable, pip, pim, Kp, Km); - } - else ++nstable; - } - } - - - }; - - - // The hook for the plugin system - DECLARE_RIVET_PLUGIN(BABAR_2007_S7266081); - -} diff --git a/analyses/pluginMisc/BABAR_2013_I1238276.cc b/analyses/pluginMisc/BABAR_2013_I1238276.cc deleted file mode 100644 --- a/analyses/pluginMisc/BABAR_2013_I1238276.cc +++ /dev/null @@ -1,118 +0,0 @@ -// -*- C++ -*- -#include "Rivet/Analysis.hh" -#include "Rivet/Projections/Beam.hh" -#include "Rivet/Projections/ChargedFinalState.hh" - -namespace Rivet { - - - /// @brief BaBar pion, kaon and proton production in the continuum - /// @author Peter Richardson - class BABAR_2013_I1238276 : public Analysis { - public: - - BABAR_2013_I1238276() - : Analysis("BABAR_2013_I1238276") - { } - - - void init() { - declare(Beam(), "Beams"); - declare(ChargedFinalState(), "FS"); - - _histPion_no_dec = bookHisto1D(1,1,1); - _histKaon_no_dec = bookHisto1D(1,1,2); - _histProton_no_dec = bookHisto1D(1,1,3); - _histPion_dec = bookHisto1D(2,1,1); - _histKaon_dec = bookHisto1D(2,1,2); - _histProton_dec = bookHisto1D(2,1,3); - } - - - void analyze(const Event& e) { - const double weight = e.weight(); - - // Loop through charged FS particles and look for charmed mesons/baryons - const ChargedFinalState& fs = apply(e, "FS"); - - const Beam beamproj = apply(e, "Beams"); - const ParticlePair& beams = beamproj.beams(); - const FourMomentum mom_tot = beams.first.momentum() + beams.second.momentum(); - const LorentzTransform cms_boost = LorentzTransform::mkFrameTransformFromBeta(mom_tot.betaVec()); - MSG_DEBUG("CMS Energy sqrt s = " << beamproj.sqrtS()); - - foreach (const Particle& p, fs.particles()) { - // check if prompt or not - ConstGenParticlePtr pmother = p.genParticle(); - ConstGenVertexPtr ivertex = pmother->production_vertex(); - bool prompt = true; - while (ivertex) { - vector inparts = HepMCUtils::particles(ivertex, Relatives::PARENTS); - int n_inparts = inparts.size(); - if (n_inparts < 1) break; - pmother = inparts[0]; // first mother particle - int mother_pid = abs(pmother->pdg_id()); - if (mother_pid==PID::K0S || mother_pid==PID::LAMBDA) { - prompt = false; - break; - } - else if (mother_pid<6) { - break; - } - ivertex = pmother->production_vertex(); - } - - // momentum in CMS frame - const double mom = cms_boost.transform(p.momentum()).vector3().mod(); - const int PdgId = p.abspid(); - MSG_DEBUG("pdgID = " << PdgId << " Momentum = " << mom); - switch (PdgId) { - case PID::PIPLUS: - if(prompt) _histPion_no_dec->fill(mom,weight); - _histPion_dec ->fill(mom,weight); - break; - case PID::KPLUS: - if(prompt) _histKaon_no_dec->fill(mom,weight); - _histKaon_dec ->fill(mom,weight); - break; - case PID::PROTON: - if(prompt) _histProton_no_dec->fill(mom,weight); - _histProton_dec ->fill(mom,weight); - default : - break; - } - } - } - - - void finalize() { - scale(_histPion_no_dec ,1./sumOfWeights()); - scale(_histKaon_no_dec ,1./sumOfWeights()); - scale(_histProton_no_dec,1./sumOfWeights()); - scale(_histPion_dec ,1./sumOfWeights()); - scale(_histKaon_dec ,1./sumOfWeights()); - scale(_histProton_dec ,1./sumOfWeights()); - } - - - private: - - //@{ - // Histograms for continuum data (sqrt(s) = 10.52 GeV) - // no K_S and Lambda decays - Histo1DPtr _histPion_no_dec; - Histo1DPtr _histKaon_no_dec; - Histo1DPtr _histProton_no_dec; - // including decays - Histo1DPtr _histPion_dec; - Histo1DPtr _histKaon_dec; - Histo1DPtr _histProton_dec; - //@} - - }; - - - // The hook for the plugin system - DECLARE_RIVET_PLUGIN(BABAR_2013_I1238276); - -} diff --git a/analyses/pluginMisc/BABAR_2013_I1238276.yoda b/analyses/pluginMisc/BABAR_2013_I1238276.yoda deleted file mode 100644 --- a/analyses/pluginMisc/BABAR_2013_I1238276.yoda +++ /dev/null @@ -1,383 +0,0 @@ -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d01-x01-y01 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d01-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.250000e-01 2.500000e-02 2.500000e-02 8.010000e+00 2.209072e-01 2.209072e-01 -2.750000e-01 2.500000e-02 2.500000e-02 8.250000e+00 2.102380e-01 2.102380e-01 -3.250000e-01 2.500000e-02 2.500000e-02 8.040000e+00 1.702939e-01 1.702939e-01 -3.750000e-01 2.500000e-02 2.500000e-02 7.520000e+00 1.403567e-01 1.403567e-01 -4.250000e-01 2.500000e-02 2.500000e-02 6.930000e+00 1.104536e-01 1.104536e-01 -4.750000e-01 2.500000e-02 2.500000e-02 6.360000e+00 1.004988e-01 1.004988e-01 -5.250000e-01 2.500000e-02 2.500000e-02 5.780000e+00 8.062258e-02 8.062258e-02 -5.750000e-01 2.500000e-02 2.500000e-02 5.210000e+00 7.071068e-02 7.071068e-02 -6.250000e-01 2.500000e-02 2.500000e-02 4.690000e+00 6.082763e-02 6.082763e-02 -6.750000e-01 2.500000e-02 2.500000e-02 4.210000e+00 5.099020e-02 5.099020e-02 -7.250000e-01 2.500000e-02 2.500000e-02 3.781000e+00 4.825971e-02 4.825971e-02 -7.750000e-01 2.500000e-02 2.500000e-02 3.402000e+00 4.318565e-02 4.318565e-02 -8.250000e-01 2.500000e-02 2.500000e-02 3.065000e+00 3.920459e-02 3.920459e-02 -8.750000e-01 2.500000e-02 2.500000e-02 2.765000e+00 3.522783e-02 3.522783e-02 -9.250000e-01 2.500000e-02 2.500000e-02 2.495000e+00 3.214032e-02 3.214032e-02 -9.750000e-01 2.500000e-02 2.500000e-02 2.258000e+00 3.014963e-02 3.014963e-02 -1.050000e+00 5.000000e-02 5.000000e-02 1.948000e+00 2.707397e-02 2.707397e-02 -1.150000e+00 5.000000e-02 5.000000e-02 1.603000e+00 2.308679e-02 2.308679e-02 -1.250000e+00 5.000000e-02 5.000000e-02 1.332000e+00 2.009975e-02 2.009975e-02 -1.350000e+00 5.000000e-02 5.000000e-02 1.106000e+00 1.811077e-02 1.811077e-02 -1.450000e+00 5.000000e-02 5.000000e-02 9.260000e-01 1.612452e-02 1.612452e-02 -1.550000e+00 5.000000e-02 5.000000e-02 7.800000e-01 1.414214e-02 1.414214e-02 -1.650000e+00 5.000000e-02 5.000000e-02 6.590000e-01 1.303840e-02 1.303840e-02 -1.750000e+00 5.000000e-02 5.000000e-02 5.590000e-01 1.204159e-02 1.204159e-02 -1.850000e+00 5.000000e-02 5.000000e-02 4.750000e-01 1.004988e-02 1.004988e-02 -1.950000e+00 5.000000e-02 5.000000e-02 4.040000e-01 9.055385e-03 9.055385e-03 -2.050000e+00 5.000000e-02 5.000000e-02 3.430000e-01 8.062258e-03 8.062258e-03 -2.150000e+00 5.000000e-02 5.000000e-02 2.940000e-01 7.071068e-03 7.071068e-03 -2.250000e+00 5.000000e-02 5.000000e-02 2.510000e-01 7.071068e-03 7.071068e-03 -2.350000e+00 5.000000e-02 5.000000e-02 2.160000e-01 6.082763e-03 6.082763e-03 -2.450000e+00 5.000000e-02 5.000000e-02 1.860000e-01 5.099020e-03 5.099020e-03 -2.550000e+00 5.000000e-02 5.000000e-02 1.610000e-01 4.837355e-03 4.837355e-03 -2.650000e+00 5.000000e-02 5.000000e-02 1.394000e-01 4.328972e-03 4.328972e-03 -2.750000e+00 5.000000e-02 5.000000e-02 1.213000e-01 3.832754e-03 3.832754e-03 -2.850000e+00 5.000000e-02 5.000000e-02 1.048000e-01 3.436568e-03 3.436568e-03 -2.950000e+00 5.000000e-02 5.000000e-02 9.100000e-02 3.026549e-03 3.026549e-03 -3.125000e+00 1.250000e-01 1.250000e-01 7.060000e-02 2.433105e-03 2.433105e-03 -3.375000e+00 1.250000e-01 1.250000e-01 4.970000e-02 1.824829e-03 1.824829e-03 -3.625000e+00 1.250000e-01 1.250000e-01 3.500000e-02 1.431782e-03 1.431782e-03 -3.875000e+00 1.250000e-01 1.250000e-01 2.460000e-02 1.044031e-03 1.044031e-03 -4.125000e+00 1.250000e-01 1.250000e-01 1.670000e-02 8.246211e-04 8.246211e-04 -4.375000e+00 1.250000e-01 1.250000e-01 1.070000e-02 5.385165e-04 5.385165e-04 -4.625000e+00 1.250000e-01 1.250000e-01 6.810000e-03 3.981206e-04 3.981206e-04 -4.875000e+00 1.250000e-01 1.250000e-01 4.180000e-03 2.830194e-04 2.830194e-04 -5.135000e+00 1.350000e-01 1.350000e-01 1.530000e-03 1.486607e-04 1.486607e-04 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d01-x01-y02 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d01-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.250000e-01 2.500000e-02 2.500000e-02 2.910000e-01 7.615773e-03 7.615773e-03 -2.750000e-01 2.500000e-02 2.500000e-02 3.820000e-01 7.615773e-03 7.615773e-03 -3.250000e-01 2.500000e-02 2.500000e-02 4.680000e-01 8.544004e-03 8.544004e-03 -3.750000e-01 2.500000e-02 2.500000e-02 5.380000e-01 9.486833e-03 9.486833e-03 -4.250000e-01 2.500000e-02 2.500000e-02 5.910000e-01 9.219544e-03 9.219544e-03 -4.750000e-01 2.500000e-02 2.500000e-02 6.330000e-01 9.219544e-03 9.219544e-03 -5.250000e-01 2.500000e-02 2.500000e-02 6.690000e-01 9.219544e-03 9.219544e-03 -5.750000e-01 2.500000e-02 2.500000e-02 6.820000e-01 9.219544e-03 9.219544e-03 -6.250000e-01 2.500000e-02 2.500000e-02 6.890000e-01 9.219544e-03 9.219544e-03 -6.750000e-01 2.500000e-02 2.500000e-02 6.870000e-01 9.219544e-03 9.219544e-03 -7.250000e-01 2.500000e-02 2.500000e-02 6.760000e-01 9.219544e-03 9.219544e-03 -7.750000e-01 2.500000e-02 2.500000e-02 6.580000e-01 8.246211e-03 8.246211e-03 -8.250000e-01 2.500000e-02 2.500000e-02 6.360000e-01 8.246211e-03 8.246211e-03 -8.750000e-01 2.500000e-02 2.500000e-02 6.160000e-01 8.246211e-03 8.246211e-03 -9.250000e-01 2.500000e-02 2.500000e-02 5.930000e-01 8.246211e-03 8.246211e-03 -9.750000e-01 2.500000e-02 2.500000e-02 5.680000e-01 7.280110e-03 7.280110e-03 -1.050000e+00 5.000000e-02 5.000000e-02 5.310000e-01 7.071068e-03 7.071068e-03 -1.150000e+00 5.000000e-02 5.000000e-02 4.820000e-01 6.082763e-03 6.082763e-03 -1.250000e+00 5.000000e-02 5.000000e-02 4.350000e-01 6.082763e-03 6.082763e-03 -1.350000e+00 5.000000e-02 5.000000e-02 3.890000e-01 6.082763e-03 6.082763e-03 -1.450000e+00 5.000000e-02 5.000000e-02 3.470000e-01 5.099020e-03 5.099020e-03 -1.550000e+00 5.000000e-02 5.000000e-02 3.080000e-01 4.785394e-03 4.785394e-03 -1.650000e+00 5.000000e-02 5.000000e-02 2.731000e-01 4.373786e-03 4.373786e-03 -1.750000e+00 5.000000e-02 5.000000e-02 2.427000e-01 4.079216e-03 4.079216e-03 -1.850000e+00 5.000000e-02 5.000000e-02 2.161000e-01 3.765634e-03 3.765634e-03 -1.950000e+00 5.000000e-02 5.000000e-02 1.921000e-01 3.471311e-03 3.471311e-03 -2.050000e+00 5.000000e-02 5.000000e-02 1.698000e-01 3.157531e-03 3.157531e-03 -2.150000e+00 5.000000e-02 5.000000e-02 1.503000e-01 2.961419e-03 2.961419e-03 -2.250000e+00 5.000000e-02 5.000000e-02 1.323000e-01 2.647640e-03 2.647640e-03 -2.350000e+00 5.000000e-02 5.000000e-02 1.167000e-01 2.451530e-03 2.451530e-03 -2.450000e+00 5.000000e-02 5.000000e-02 1.031000e-01 2.256103e-03 2.256103e-03 -2.550000e+00 5.000000e-02 5.000000e-02 9.090000e-02 2.039608e-03 2.039608e-03 -2.650000e+00 5.000000e-02 5.000000e-02 8.020000e-02 1.843909e-03 1.843909e-03 -2.750000e+00 5.000000e-02 5.000000e-02 7.040000e-02 1.649242e-03 1.649242e-03 -2.850000e+00 5.000000e-02 5.000000e-02 6.220000e-02 1.552417e-03 1.552417e-03 -2.950000e+00 5.000000e-02 5.000000e-02 5.460000e-02 1.431782e-03 1.431782e-03 -3.125000e+00 1.250000e-01 1.250000e-01 4.360000e-02 1.140175e-03 1.140175e-03 -3.375000e+00 1.250000e-01 1.250000e-01 3.060000e-02 9.486833e-04 9.486833e-04 -3.625000e+00 1.250000e-01 1.250000e-01 2.090000e-02 7.280110e-04 7.280110e-04 -3.875000e+00 1.250000e-01 1.250000e-01 1.390000e-02 5.385165e-04 5.385165e-04 -4.125000e+00 1.250000e-01 1.250000e-01 9.100000e-03 4.518849e-04 4.518849e-04 -4.375000e+00 1.250000e-01 1.250000e-01 5.680000e-03 3.448188e-04 3.448188e-04 -4.625000e+00 1.250000e-01 1.250000e-01 3.240000e-03 2.580698e-04 2.580698e-04 -4.875000e+00 1.250000e-01 1.250000e-01 1.490000e-03 1.920937e-04 1.920937e-04 -5.135000e+00 1.350000e-01 1.350000e-01 5.000000e-04 9.899495e-05 9.899495e-05 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d01-x01-y03 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d01-x01-y03 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.250000e-01 2.500000e-02 2.500000e-02 4.790000e-02 3.807887e-03 3.807887e-03 -2.750000e-01 2.500000e-02 2.500000e-02 6.720000e-02 4.308132e-03 4.308132e-03 -3.250000e-01 2.500000e-02 2.500000e-02 8.790000e-02 4.876474e-03 4.876474e-03 -3.750000e-01 2.500000e-02 2.500000e-02 1.046000e-01 5.141984e-03 5.141984e-03 -4.250000e-01 2.500000e-02 2.500000e-02 1.167000e-01 5.217279e-03 5.217279e-03 -4.750000e-01 2.500000e-02 2.500000e-02 1.237000e-01 4.924429e-03 4.924429e-03 -5.250000e-01 2.500000e-02 2.500000e-02 1.296000e-01 4.609772e-03 4.609772e-03 -5.750000e-01 2.500000e-02 2.500000e-02 1.356000e-01 4.589118e-03 4.589118e-03 -6.250000e-01 2.500000e-02 2.500000e-02 1.380000e-01 4.491102e-03 4.491102e-03 -6.750000e-01 2.500000e-02 2.500000e-02 1.384000e-01 4.687217e-03 4.687217e-03 -7.250000e-01 2.500000e-02 2.500000e-02 1.363000e-01 4.589118e-03 4.589118e-03 -7.750000e-01 2.500000e-02 2.500000e-02 1.331000e-01 4.589118e-03 4.589118e-03 -8.250000e-01 2.500000e-02 2.500000e-02 1.292000e-01 4.472136e-03 4.472136e-03 -8.750000e-01 2.500000e-02 2.500000e-02 1.256000e-01 4.373786e-03 4.373786e-03 -9.250000e-01 2.500000e-02 2.500000e-02 1.200000e-01 4.275512e-03 4.275512e-03 -9.750000e-01 2.500000e-02 2.500000e-02 1.135000e-01 4.177320e-03 4.177320e-03 -1.050000e+00 5.000000e-02 5.000000e-02 1.033000e-01 4.060788e-03 4.060788e-03 -1.150000e+00 5.000000e-02 5.000000e-02 9.190000e-02 3.847077e-03 3.847077e-03 -1.250000e+00 5.000000e-02 5.000000e-02 8.230000e-02 3.551056e-03 3.551056e-03 -1.350000e+00 5.000000e-02 5.000000e-02 7.340000e-02 3.238827e-03 3.238827e-03 -1.450000e+00 5.000000e-02 5.000000e-02 6.550000e-02 2.942788e-03 2.942788e-03 -1.550000e+00 5.000000e-02 5.000000e-02 5.880000e-02 2.647640e-03 2.647640e-03 -1.650000e+00 5.000000e-02 5.000000e-02 5.260000e-02 2.334524e-03 2.334524e-03 -1.750000e+00 5.000000e-02 5.000000e-02 4.660000e-02 2.039608e-03 2.039608e-03 -1.850000e+00 5.000000e-02 5.000000e-02 4.160000e-02 1.746425e-03 1.746425e-03 -1.950000e+00 5.000000e-02 5.000000e-02 3.740000e-02 1.529706e-03 1.529706e-03 -2.050000e+00 5.000000e-02 5.000000e-02 3.310000e-02 1.334166e-03 1.334166e-03 -2.150000e+00 5.000000e-02 5.000000e-02 2.930000e-02 1.236932e-03 1.236932e-03 -2.250000e+00 5.000000e-02 5.000000e-02 2.590000e-02 1.044031e-03 1.044031e-03 -2.350000e+00 5.000000e-02 5.000000e-02 2.270000e-02 9.219544e-04 9.219544e-04 -2.450000e+00 5.000000e-02 5.000000e-02 2.010000e-02 8.246211e-04 8.246211e-04 -2.550000e+00 5.000000e-02 5.000000e-02 1.760000e-02 7.280110e-04 7.280110e-04 -2.650000e+00 5.000000e-02 5.000000e-02 1.540000e-02 6.324555e-04 6.324555e-04 -2.750000e+00 5.000000e-02 5.000000e-02 1.330000e-02 5.385165e-04 5.385165e-04 -2.850000e+00 5.000000e-02 5.000000e-02 1.146000e-02 4.648656e-04 4.648656e-04 -2.950000e+00 5.000000e-02 5.000000e-02 9.790000e-03 4.049691e-04 4.049691e-04 -3.125000e+00 1.250000e-01 1.250000e-01 7.330000e-03 3.101612e-04 3.101612e-04 -3.375000e+00 1.250000e-01 1.250000e-01 4.480000e-03 2.102380e-04 2.102380e-04 -3.625000e+00 1.250000e-01 1.250000e-01 2.600000e-03 1.389244e-04 1.389244e-04 -3.875000e+00 1.250000e-01 1.250000e-01 1.430000e-03 9.433981e-05 9.433981e-05 -4.125000e+00 1.250000e-01 1.250000e-01 7.300000e-04 6.403124e-05 6.403124e-05 -4.375000e+00 1.250000e-01 1.250000e-01 3.600000e-04 4.242641e-05 4.242641e-05 -4.625000e+00 1.250000e-01 1.250000e-01 1.700000e-04 2.828427e-05 2.828427e-05 -4.875000e+00 1.250000e-01 1.250000e-01 7.000000e-05 2.236068e-05 2.236068e-05 -5.135000e+00 1.350000e-01 1.350000e-01 1.000000e-05 1.414214e-05 1.414214e-05 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d02-x01-y01 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d02-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.250000e-01 2.500000e-02 2.500000e-02 9.250000e+00 2.408319e-01 2.408319e-01 -2.750000e-01 2.500000e-02 2.500000e-02 9.450000e+00 2.302173e-01 2.302173e-01 -3.250000e-01 2.500000e-02 2.500000e-02 9.140000e+00 2.002498e-01 2.002498e-01 -3.750000e-01 2.500000e-02 2.500000e-02 8.510000e+00 1.603122e-01 1.603122e-01 -4.250000e-01 2.500000e-02 2.500000e-02 7.820000e+00 1.403567e-01 1.403567e-01 -4.750000e-01 2.500000e-02 2.500000e-02 7.150000e+00 1.104536e-01 1.104536e-01 -5.250000e-01 2.500000e-02 2.500000e-02 6.470000e+00 1.004988e-01 1.004988e-01 -5.750000e-01 2.500000e-02 2.500000e-02 5.830000e+00 8.062258e-02 8.062258e-02 -6.250000e-01 2.500000e-02 2.500000e-02 5.230000e+00 7.071068e-02 7.071068e-02 -6.750000e-01 2.500000e-02 2.500000e-02 4.690000e+00 6.082763e-02 6.082763e-02 -7.250000e-01 2.500000e-02 2.500000e-02 4.210000e+00 5.099020e-02 5.099020e-02 -7.750000e-01 2.500000e-02 2.500000e-02 3.778000e+00 4.916299e-02 4.916299e-02 -8.250000e-01 2.500000e-02 2.500000e-02 3.401000e+00 4.418144e-02 4.418144e-02 -8.750000e-01 2.500000e-02 2.500000e-02 3.067000e+00 4.119466e-02 4.119466e-02 -9.250000e-01 2.500000e-02 2.500000e-02 2.768000e+00 3.811824e-02 3.811824e-02 -9.750000e-01 2.500000e-02 2.500000e-02 2.504000e+00 3.512834e-02 3.512834e-02 -1.050000e+00 5.000000e-02 5.000000e-02 2.159000e+00 3.114482e-02 3.114482e-02 -1.150000e+00 5.000000e-02 5.000000e-02 1.775000e+00 2.707397e-02 2.707397e-02 -1.250000e+00 5.000000e-02 5.000000e-02 1.472000e+00 2.408319e-02 2.408319e-02 -1.350000e+00 5.000000e-02 5.000000e-02 1.221000e+00 2.109502e-02 2.109502e-02 -1.450000e+00 5.000000e-02 5.000000e-02 1.020000e+00 1.811077e-02 1.811077e-02 -1.550000e+00 5.000000e-02 5.000000e-02 8.570000e-01 1.612452e-02 1.612452e-02 -1.650000e+00 5.000000e-02 5.000000e-02 7.230000e-01 1.503330e-02 1.503330e-02 -1.750000e+00 5.000000e-02 5.000000e-02 6.110000e-01 1.303840e-02 1.303840e-02 -1.850000e+00 5.000000e-02 5.000000e-02 5.180000e-01 1.204159e-02 1.204159e-02 -1.950000e+00 5.000000e-02 5.000000e-02 4.390000e-01 1.104536e-02 1.104536e-02 -2.050000e+00 5.000000e-02 5.000000e-02 3.720000e-01 9.055385e-03 9.055385e-03 -2.150000e+00 5.000000e-02 5.000000e-02 3.170000e-01 8.062258e-03 8.062258e-03 -2.250000e+00 5.000000e-02 5.000000e-02 2.700000e-01 8.062258e-03 8.062258e-03 -2.350000e+00 5.000000e-02 5.000000e-02 2.310000e-01 7.071068e-03 7.071068e-03 -2.450000e+00 5.000000e-02 5.000000e-02 1.980000e-01 6.082763e-03 6.082763e-03 -2.550000e+00 5.000000e-02 5.000000e-02 1.700000e-01 5.099020e-03 5.099020e-03 -2.650000e+00 5.000000e-02 5.000000e-02 1.471000e-01 4.837355e-03 4.837355e-03 -2.750000e+00 5.000000e-02 5.000000e-02 1.276000e-01 4.229657e-03 4.229657e-03 -2.850000e+00 5.000000e-02 5.000000e-02 1.099000e-01 3.733631e-03 3.733631e-03 -2.950000e+00 5.000000e-02 5.000000e-02 9.500000e-02 3.324154e-03 3.324154e-03 -3.125000e+00 1.250000e-01 1.250000e-01 7.340000e-02 2.630589e-03 2.630589e-03 -3.375000e+00 1.250000e-01 1.250000e-01 5.130000e-02 1.923538e-03 1.923538e-03 -3.625000e+00 1.250000e-01 1.250000e-01 3.590000e-02 1.431782e-03 1.431782e-03 -3.875000e+00 1.250000e-01 1.250000e-01 2.510000e-02 1.140175e-03 1.140175e-03 -4.125000e+00 1.250000e-01 1.250000e-01 1.690000e-02 8.246211e-04 8.246211e-04 -4.375000e+00 1.250000e-01 1.250000e-01 1.080000e-02 5.385165e-04 5.385165e-04 -4.625000e+00 1.250000e-01 1.250000e-01 6.820000e-03 3.981206e-04 3.981206e-04 -4.875000e+00 1.250000e-01 1.250000e-01 4.180000e-03 2.830194e-04 2.830194e-04 -5.135000e+00 1.350000e-01 1.350000e-01 1.530000e-03 1.486607e-04 1.486607e-04 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d02-x01-y02 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d02-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.250000e-01 2.500000e-02 2.500000e-02 2.910000e-01 7.615773e-03 7.615773e-03 -2.750000e-01 2.500000e-02 2.500000e-02 3.830000e-01 7.615773e-03 7.615773e-03 -3.250000e-01 2.500000e-02 2.500000e-02 4.680000e-01 8.544004e-03 8.544004e-03 -3.750000e-01 2.500000e-02 2.500000e-02 5.380000e-01 9.486833e-03 9.486833e-03 -4.250000e-01 2.500000e-02 2.500000e-02 5.910000e-01 9.219544e-03 9.219544e-03 -4.750000e-01 2.500000e-02 2.500000e-02 6.330000e-01 9.219544e-03 9.219544e-03 -5.250000e-01 2.500000e-02 2.500000e-02 6.690000e-01 9.219544e-03 9.219544e-03 -5.750000e-01 2.500000e-02 2.500000e-02 6.830000e-01 9.219544e-03 9.219544e-03 -6.250000e-01 2.500000e-02 2.500000e-02 6.890000e-01 9.219544e-03 9.219544e-03 -6.750000e-01 2.500000e-02 2.500000e-02 6.870000e-01 9.219544e-03 9.219544e-03 -7.250000e-01 2.500000e-02 2.500000e-02 6.770000e-01 9.219544e-03 9.219544e-03 -7.750000e-01 2.500000e-02 2.500000e-02 6.580000e-01 8.246211e-03 8.246211e-03 -8.250000e-01 2.500000e-02 2.500000e-02 6.360000e-01 8.246211e-03 8.246211e-03 -8.750000e-01 2.500000e-02 2.500000e-02 6.160000e-01 8.246211e-03 8.246211e-03 -9.250000e-01 2.500000e-02 2.500000e-02 5.930000e-01 8.246211e-03 8.246211e-03 -9.750000e-01 2.500000e-02 2.500000e-02 5.680000e-01 7.280110e-03 7.280110e-03 -1.050000e+00 5.000000e-02 5.000000e-02 5.310000e-01 7.071068e-03 7.071068e-03 -1.150000e+00 5.000000e-02 5.000000e-02 4.820000e-01 6.082763e-03 6.082763e-03 -1.250000e+00 5.000000e-02 5.000000e-02 4.350000e-01 6.082763e-03 6.082763e-03 -1.350000e+00 5.000000e-02 5.000000e-02 3.890000e-01 6.082763e-03 6.082763e-03 -1.450000e+00 5.000000e-02 5.000000e-02 3.470000e-01 5.099020e-03 5.099020e-03 -1.550000e+00 5.000000e-02 5.000000e-02 3.080000e-01 4.785394e-03 4.785394e-03 -1.650000e+00 5.000000e-02 5.000000e-02 2.731000e-01 4.373786e-03 4.373786e-03 -1.750000e+00 5.000000e-02 5.000000e-02 2.427000e-01 4.079216e-03 4.079216e-03 -1.850000e+00 5.000000e-02 5.000000e-02 2.161000e-01 3.765634e-03 3.765634e-03 -1.950000e+00 5.000000e-02 5.000000e-02 1.921000e-01 3.471311e-03 3.471311e-03 -2.050000e+00 5.000000e-02 5.000000e-02 1.698000e-01 3.157531e-03 3.157531e-03 -2.150000e+00 5.000000e-02 5.000000e-02 1.503000e-01 2.961419e-03 2.961419e-03 -2.250000e+00 5.000000e-02 5.000000e-02 1.323000e-01 2.647640e-03 2.647640e-03 -2.350000e+00 5.000000e-02 5.000000e-02 1.167000e-01 2.451530e-03 2.451530e-03 -2.450000e+00 5.000000e-02 5.000000e-02 1.031000e-01 2.256103e-03 2.256103e-03 -2.550000e+00 5.000000e-02 5.000000e-02 9.090000e-02 2.039608e-03 2.039608e-03 -2.650000e+00 5.000000e-02 5.000000e-02 8.020000e-02 1.843909e-03 1.843909e-03 -2.750000e+00 5.000000e-02 5.000000e-02 7.040000e-02 1.649242e-03 1.649242e-03 -2.850000e+00 5.000000e-02 5.000000e-02 6.220000e-02 1.552417e-03 1.552417e-03 -2.950000e+00 5.000000e-02 5.000000e-02 5.460000e-02 1.431782e-03 1.431782e-03 -3.125000e+00 1.250000e-01 1.250000e-01 4.360000e-02 1.140175e-03 1.140175e-03 -3.375000e+00 1.250000e-01 1.250000e-01 3.060000e-02 9.486833e-04 9.486833e-04 -3.625000e+00 1.250000e-01 1.250000e-01 2.090000e-02 7.280110e-04 7.280110e-04 -3.875000e+00 1.250000e-01 1.250000e-01 1.390000e-02 5.385165e-04 5.385165e-04 -4.125000e+00 1.250000e-01 1.250000e-01 9.100000e-03 4.518849e-04 4.518849e-04 -4.375000e+00 1.250000e-01 1.250000e-01 5.680000e-03 3.448188e-04 3.448188e-04 -4.625000e+00 1.250000e-01 1.250000e-01 3.240000e-03 2.580698e-04 2.580698e-04 -4.875000e+00 1.250000e-01 1.250000e-01 1.490000e-03 1.920937e-04 1.920937e-04 -5.135000e+00 1.350000e-01 1.350000e-01 5.000000e-04 9.899495e-05 9.899495e-05 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d02-x01-y03 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d02-x01-y03 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.250000e-01 2.500000e-02 2.500000e-02 6.800000e-02 6.324555e-03 6.324555e-03 -2.750000e-01 2.500000e-02 2.500000e-02 9.400000e-02 7.280110e-03 7.280110e-03 -3.250000e-01 2.500000e-02 2.500000e-02 1.220000e-01 8.062258e-03 8.062258e-03 -3.750000e-01 2.500000e-02 2.500000e-02 1.450000e-01 9.055385e-03 9.055385e-03 -4.250000e-01 2.500000e-02 2.500000e-02 1.610000e-01 8.062258e-03 8.062258e-03 -4.750000e-01 2.500000e-02 2.500000e-02 1.710000e-01 7.071068e-03 7.071068e-03 -5.250000e-01 2.500000e-02 2.500000e-02 1.800000e-01 7.071068e-03 7.071068e-03 -5.750000e-01 2.500000e-02 2.500000e-02 1.880000e-01 7.071068e-03 7.071068e-03 -6.250000e-01 2.500000e-02 2.500000e-02 1.920000e-01 6.082763e-03 6.082763e-03 -6.750000e-01 2.500000e-02 2.500000e-02 1.930000e-01 7.071068e-03 7.071068e-03 -7.250000e-01 2.500000e-02 2.500000e-02 1.910000e-01 7.071068e-03 7.071068e-03 -7.750000e-01 2.500000e-02 2.500000e-02 1.870000e-01 7.071068e-03 7.071068e-03 -8.250000e-01 2.500000e-02 2.500000e-02 1.830000e-01 7.071068e-03 7.071068e-03 -8.750000e-01 2.500000e-02 2.500000e-02 1.790000e-01 7.071068e-03 7.071068e-03 -9.250000e-01 2.500000e-02 2.500000e-02 1.730000e-01 6.082763e-03 6.082763e-03 -9.750000e-01 2.500000e-02 2.500000e-02 1.650000e-01 6.082763e-03 6.082763e-03 -1.050000e+00 5.000000e-02 5.000000e-02 1.530000e-01 6.082763e-03 6.082763e-03 -1.150000e+00 5.000000e-02 5.000000e-02 1.390000e-01 6.082763e-03 6.082763e-03 -1.250000e+00 5.000000e-02 5.000000e-02 1.260000e-01 6.082763e-03 6.082763e-03 -1.350000e+00 5.000000e-02 5.000000e-02 1.130000e-01 5.099020e-03 5.099020e-03 -1.450000e+00 5.000000e-02 5.000000e-02 1.006000e-01 4.627094e-03 4.627094e-03 -1.550000e+00 5.000000e-02 5.000000e-02 9.000000e-02 4.229657e-03 4.229657e-03 -1.650000e+00 5.000000e-02 5.000000e-02 7.990000e-02 3.721559e-03 3.721559e-03 -1.750000e+00 5.000000e-02 5.000000e-02 7.040000e-02 3.224903e-03 3.224903e-03 -1.850000e+00 5.000000e-02 5.000000e-02 6.200000e-02 2.828427e-03 2.828427e-03 -1.950000e+00 5.000000e-02 5.000000e-02 5.480000e-02 2.418677e-03 2.418677e-03 -2.050000e+00 5.000000e-02 5.000000e-02 4.800000e-02 2.121320e-03 2.121320e-03 -2.150000e+00 5.000000e-02 5.000000e-02 4.190000e-02 1.824829e-03 1.824829e-03 -2.250000e+00 5.000000e-02 5.000000e-02 3.640000e-02 1.627882e-03 1.627882e-03 -2.350000e+00 5.000000e-02 5.000000e-02 3.150000e-02 1.414214e-03 1.414214e-03 -2.450000e+00 5.000000e-02 5.000000e-02 2.750000e-02 1.216553e-03 1.216553e-03 -2.550000e+00 5.000000e-02 5.000000e-02 2.370000e-02 1.118034e-03 1.118034e-03 -2.650000e+00 5.000000e-02 5.000000e-02 2.060000e-02 1.019804e-03 1.019804e-03 -2.750000e+00 5.000000e-02 5.000000e-02 1.760000e-02 9.219544e-04 9.219544e-04 -2.850000e+00 5.000000e-02 5.000000e-02 1.500000e-02 8.246211e-04 8.246211e-04 -2.950000e+00 5.000000e-02 5.000000e-02 1.280000e-02 7.071068e-04 7.071068e-04 -3.125000e+00 1.250000e-01 1.250000e-01 9.260000e-03 5.044799e-04 5.044799e-04 -3.375000e+00 1.250000e-01 1.250000e-01 5.640000e-03 3.517101e-04 3.517101e-04 -3.625000e+00 1.250000e-01 1.250000e-01 3.240000e-03 2.213594e-04 2.213594e-04 -3.875000e+00 1.250000e-01 1.250000e-01 1.730000e-03 1.300000e-04 1.300000e-04 -4.125000e+00 1.250000e-01 1.250000e-01 8.700000e-04 7.211103e-05 7.211103e-05 -4.375000e+00 1.250000e-01 1.250000e-01 4.000000e-04 4.242641e-05 4.242641e-05 -4.625000e+00 1.250000e-01 1.250000e-01 1.700000e-04 2.828427e-05 2.828427e-05 -4.875000e+00 1.250000e-01 1.250000e-01 7.000000e-05 2.236068e-05 2.236068e-05 -5.135000e+00 1.350000e-01 1.350000e-01 1.000000e-05 1.414214e-05 1.414214e-05 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d03-x01-y01 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d03-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.735000e+00 2.535000e+00 2.535000e+00 5.364000e+00 8.224962e-02 8.224962e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d03-x01-y02 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d03-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.735000e+00 2.535000e+00 2.535000e+00 9.460000e-01 2.002498e-02 2.002498e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d03-x01-y03 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d03-x01-y03 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.735000e+00 2.535000e+00 2.535000e+00 1.819000e-01 9.095603e-03 9.095603e-03 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d04-x01-y01 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d04-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.735000e+00 2.535000e+00 2.535000e+00 6.002000e+00 9.417006e-02 9.417006e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d04-x01-y02 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d04-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.735000e+00 2.535000e+00 2.535000e+00 9.460000e-01 2.002498e-02 2.002498e-02 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BABAR_2013_I1238276/d04-x01-y03 -IsRef: 1 -Path: /REF/BABAR_2013_I1238276/d04-x01-y03 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.735000e+00 2.535000e+00 2.535000e+00 2.612000e-01 1.242337e-02 1.242337e-02 -END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/BELLE_2001_S4598261.cc b/analyses/pluginMisc/BELLE_2001_S4598261.cc deleted file mode 100644 --- a/analyses/pluginMisc/BELLE_2001_S4598261.cc +++ /dev/null @@ -1,104 +0,0 @@ -// -*- C++ -*- -#include "Rivet/Analysis.hh" -#include "Rivet/Projections/Beam.hh" -#include "Rivet/Projections/UnstableParticles.hh" - -namespace Rivet { - - - /// @brief BELLE pi0 spectrum at Upsilon(4S) - /// @author Peter Richardson - class BELLE_2001_S4598261 : public Analysis { - public: - - BELLE_2001_S4598261() - : Analysis("BELLE_2001_S4598261"), _weightSum(0.) - { } - - - void init() { - declare(UnstableParticles(), "UFS"); - _histdSigDp = bookHisto1D(1, 1, 1); // spectrum - _histMult = bookHisto1D(2, 1, 1); // multiplicity - } - - - void analyze(const Event& e) { - const double weight = e.weight(); - - // Find the upsilons - Particles upsilons; - // First in unstable final state - const UnstableParticles& ufs = apply(e, "UFS"); - foreach (const Particle& p, ufs.particles()) - if (p.pid()==300553) upsilons.push_back(p); - // Then in whole event if fails - if (upsilons.empty()) { - for(ConstGenParticlePtr p: HepMCUtils::particles(e.genEvent())) { - if (p->pdg_id() != 300553) continue; - ConstGenVertexPtr pv = p->production_vertex(); - bool passed = true; - if (pv) { - for (ConstGenParticlePtr pp: HepMCUtils::particles(pv, Relatives::PARENTS)){ - if ( p->pdg_id() == pp->pdg_id() ) { - passed = false; - break; - } - } - } - if (passed) upsilons.push_back(Particle(p)); - } - } - - // Find upsilons - foreach (const Particle& p, upsilons) { - _weightSum += weight; - // Find the neutral pions from the decay - vector pions; - findDecayProducts(p.genParticle(), pions); - const LorentzTransform cms_boost = LorentzTransform::mkFrameTransformFromBeta(p.momentum().betaVec()); - for (size_t ix=0; ixmomentum())).p(); - _histdSigDp->fill(pcm,weight); - } - _histMult->fill(0., pions.size()*weight); - } - } - - - void finalize() { - scale(_histdSigDp, 1./_weightSum); - scale(_histMult , 1./_weightSum); - } - - - private: - - //@{ - // count of weights - double _weightSum; - /// Histograms - Histo1DPtr _histdSigDp; - Histo1DPtr _histMult; - //@} - - - void findDecayProducts(ConstGenParticlePtr p, vector& pions) { - ConstGenVertexPtr dv = p->end_vertex(); - for (ConstGenParticlePtr pp: HepMCUtils::particles(dv, Relatives::CHILDREN)){ - const int id = pp->pdg_id(); - if (id == 111) { - pions.push_back(pp); - } else if (pp->end_vertex()) - findDecayProducts(pp, pions); - } - } - - - }; - - - // The hook for the plugin system - DECLARE_RIVET_PLUGIN(BELLE_2001_S4598261); - -} diff --git a/analyses/pluginMisc/BELLE_2008_I786560.cc b/analyses/pluginMisc/BELLE_2008_I786560.cc deleted file mode 100644 --- a/analyses/pluginMisc/BELLE_2008_I786560.cc +++ /dev/null @@ -1,104 +0,0 @@ -// -*- C++ -*- -#include "Rivet/Analysis.hh" -#include "Rivet/Projections/UnstableParticles.hh" - -namespace Rivet { - - - /// @brief BELLE tau lepton to pi pi - /// @author Peter Richardson - class BELLE_2008_I786560 : public Analysis { - public: - - BELLE_2008_I786560() - : Analysis("BELLE_2008_I786560"), - _weight_total(0), - _weight_pipi(0) - { } - - - void init() { - declare(UnstableParticles(), "UFS"); - _hist_pipi = bookHisto1D( 1, 1, 1); - } - - - void analyze(const Event& e) { - // Find the taus - Particles taus; - const UnstableParticles& ufs = apply(e, "UFS"); - foreach (const Particle& p, ufs.particles()) { - if (p.abspid() != PID::TAU) continue; - _weight_total += 1.; - Particles pip, pim, pi0; - unsigned int nstable = 0; - // find the decay products we want - findDecayProducts(p, nstable, pip, pim, pi0); - if (p.pid() < 0) { - swap(pip, pim); - } - if (nstable != 3) continue; - // pipi - if (pim.size() == 1 && pi0.size() == 1) { - _weight_pipi += 1.; - _hist_pipi->fill((pi0[0].momentum()+pim[0].momentum()).mass2(),1.); - } - } - } - - - void finalize() { - if (_weight_pipi > 0.) scale(_hist_pipi, 1./_weight_pipi); - } - - - private: - - //@{ - - // Histograms - Histo1DPtr _hist_pipi; - - // Weights counters - double _weight_total, _weight_pipi; - - //@} - - void findDecayProducts(const Particle &mother, - unsigned int & nstable, - Particles& pip, Particles& pim, - Particles& pi0) { - for (const Particle &p : mother.children()) { - long id = p.pdgId(); - if (id == PID::PI0 ) { - pi0.push_back(p); - ++nstable; - } - else if (id == PID::K0S) - ++nstable; - else if (id == PID::PIPLUS) { - pip.push_back(p); - ++nstable; - } - else if (id == PID::PIMINUS) { - pim.push_back(p); - ++nstable; - } - else if (id == PID::KPLUS) { - ++nstable; - } - else if (id == PID::KMINUS) { - ++nstable; - } - else if (!p.children().empty()) { - findDecayProducts(p, nstable, pip, pim, pi0); - } - else ++nstable; - } - } - }; - - // The hook for the plugin system - DECLARE_RIVET_PLUGIN(BELLE_2008_I786560); - -} diff --git a/analyses/pluginMisc/BELLE_2013_I1216515.yoda b/analyses/pluginMisc/BELLE_2013_I1216515.yoda deleted file mode 100644 --- a/analyses/pluginMisc/BELLE_2013_I1216515.yoda +++ /dev/null @@ -1,173 +0,0 @@ -BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2013_I1216515/d01-x01-y01 -IsRef: 1 -Path: /REF/BELLE_2013_I1216515/d01-x01-y01 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.050000e-01 5.000000e-03 5.000000e-03 2.037790e+07 3.844637e+05 3.846637e+05 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1.682149e+04 1.687143e+04 -7.250000e-01 5.000000e-03 5.000000e-03 2.812600e+05 1.500243e+04 1.506234e+04 -7.350000e-01 5.000000e-03 5.000000e-03 2.594300e+05 1.528044e+04 1.533037e+04 -7.450000e-01 5.000000e-03 5.000000e-03 2.404800e+05 1.438010e+04 1.443003e+04 -7.550000e-01 5.000000e-03 5.000000e-03 2.218000e+05 1.356021e+04 1.361013e+04 -7.650000e-01 5.000000e-03 5.000000e-03 2.036400e+05 1.280969e+04 1.286960e+04 -7.750000e-01 5.000000e-03 5.000000e-03 1.878500e+05 1.192940e+04 1.198930e+04 -7.850000e-01 5.000000e-03 5.000000e-03 1.721800e+05 1.096987e+04 1.102976e+04 -7.950000e-01 5.000000e-03 5.000000e-03 1.577200e+05 1.074848e+04 1.080838e+04 -8.050000e-01 5.000000e-03 5.000000e-03 1.446600e+05 1.085715e+04 1.090707e+04 -8.150000e-01 5.000000e-03 5.000000e-03 1.315500e+05 1.120554e+04 1.125547e+04 -8.250000e-01 5.000000e-03 5.000000e-03 1.196200e+05 8.828420e+03 8.878316e+03 -8.350000e-01 5.000000e-03 5.000000e-03 1.082300e+05 1.051388e+04 1.054384e+04 -8.450000e-01 5.000000e-03 5.000000e-03 9.672000e+04 8.076757e+03 8.106695e+03 -8.550000e-01 5.000000e-03 5.000000e-03 8.609000e+04 8.284504e+03 8.304469e+03 -8.650000e-01 5.000000e-03 5.000000e-03 7.614000e+04 7.913969e+03 7.923951e+03 -8.750000e-01 5.000000e-03 5.000000e-03 6.738000e+04 7.273933e+03 7.273933e+03 -8.850000e-01 5.000000e-03 5.000000e-03 5.811000e+04 6.972661e+03 6.972661e+03 -8.950000e-01 5.000000e-03 5.000000e-03 4.915000e+04 7.719858e+03 7.709870e+03 -9.050000e-01 5.000000e-03 5.000000e-03 4.200000e+04 6.390720e+03 6.380737e+03 -9.150000e-01 5.000000e-03 5.000000e-03 3.497000e+04 5.022211e+03 5.002259e+03 -9.250000e-01 5.000000e-03 5.000000e-03 2.946000e+04 6.168833e+03 6.148862e+03 -9.350000e-01 5.000000e-03 5.000000e-03 2.470000e+04 4.830611e+03 4.810655e+03 -9.450000e-01 5.000000e-03 5.000000e-03 1.915000e+04 5.427753e+03 5.407781e+03 -9.550000e-01 5.000000e-03 5.000000e-03 1.376000e+04 3.770411e+03 3.750467e+03 -9.650000e-01 5.000000e-03 5.000000e-03 9.910000e+03 4.938522e+03 4.918557e+03 -9.750000e-01 5.000000e-03 5.000000e-03 1.170000e+04 6.502461e+03 6.452635e+03 -END YODA_SCATTER2D_V2 - -BEGIN YODA_SCATTER2D_V2 /REF/BELLE_2013_I1216515/d01-x01-y02 -IsRef: 1 -Path: /REF/BELLE_2013_I1216515/d01-x01-y02 -Title: ~ -Type: Scatter2D ---- -# xval xerr- xerr+ yval yerr- yerr+ -2.050000e-01 5.000000e-03 5.000000e-03 6.373800e+06 1.432559e+05 1.431559e+05 -2.150000e-01 5.000000e-03 5.000000e-03 5.981600e+06 1.397544e+05 1.397544e+05 -2.250000e-01 5.000000e-03 5.000000e-03 5.591300e+06 1.281534e+05 1.281534e+05 -2.350000e-01 5.000000e-03 5.000000e-03 5.234300e+06 1.212535e+05 1.212535e+05 -2.450000e-01 5.000000e-03 5.000000e-03 4.906600e+06 1.186516e+05 1.186516e+05 -2.550000e-01 5.000000e-03 5.000000e-03 4.578400e+06 1.165467e+05 1.164468e+05 -2.650000e-01 5.000000e-03 5.000000e-03 4.256800e+06 1.074477e+05 1.073477e+05 -2.750000e-01 5.000000e-03 5.000000e-03 3.947500e+06 1.013474e+05 1.013474e+05 -2.850000e-01 5.000000e-03 5.000000e-03 3.658900e+06 9.114938e+04 9.124933e+04 -2.950000e-01 5.000000e-03 5.000000e-03 3.396000e+06 9.064640e+04 9.074635e+04 -3.050000e-01 5.000000e-03 5.000000e-03 3.158300e+06 8.584247e+04 8.594242e+04 -3.150000e-01 5.000000e-03 5.000000e-03 2.948000e+06 8.583938e+04 8.583938e+04 -3.250000e-01 5.000000e-03 5.000000e-03 2.752200e+06 7.854305e+04 7.854305e+04 -3.350000e-01 5.000000e-03 5.000000e-03 2.566100e+06 7.574127e+04 7.584122e+04 -3.450000e-01 5.000000e-03 5.000000e-03 2.396000e+06 7.184010e+04 7.194004e+04 -3.550000e-01 5.000000e-03 5.000000e-03 2.238900e+06 6.883843e+04 6.883843e+04 -3.650000e-01 5.000000e-03 5.000000e-03 2.091700e+06 6.423768e+04 6.433763e+04 -3.750000e-01 5.000000e-03 5.000000e-03 1.948700e+06 6.293505e+04 6.293505e+04 -3.850000e-01 5.000000e-03 5.000000e-03 1.814700e+06 6.033656e+04 6.033656e+04 -3.950000e-01 5.000000e-03 5.000000e-03 1.690600e+06 5.643545e+04 5.643545e+04 -4.050000e-01 5.000000e-03 5.000000e-03 1.580400e+06 5.293411e+04 5.303405e+04 -4.150000e-01 5.000000e-03 5.000000e-03 1.480200e+06 5.303405e+04 5.313398e+04 -4.250000e-01 5.000000e-03 5.000000e-03 1.389000e+06 5.103175e+04 5.103175e+04 -4.350000e-01 5.000000e-03 5.000000e-03 1.300000e+06 4.852978e+04 4.852978e+04 -4.450000e-01 5.000000e-03 5.000000e-03 1.214500e+06 4.653106e+04 4.653106e+04 -4.550000e-01 5.000000e-03 5.000000e-03 1.133800e+06 4.422895e+04 4.422895e+04 -4.650000e-01 5.000000e-03 5.000000e-03 1.058800e+06 4.063151e+04 4.063151e+04 -4.750000e-01 5.000000e-03 5.000000e-03 9.860000e+05 4.012805e+04 4.002812e+04 -4.850000e-01 5.000000e-03 5.000000e-03 9.193000e+05 3.723023e+04 3.713031e+04 -4.950000e-01 5.000000e-03 5.000000e-03 8.574000e+05 3.622706e+04 3.612714e+04 -5.050000e-01 5.000000e-03 5.000000e-03 7.999000e+05 3.193071e+04 3.193071e+04 -5.150000e-01 5.000000e-03 5.000000e-03 7.486000e+05 3.102725e+04 3.092733e+04 -5.250000e-01 5.000000e-03 5.000000e-03 7.005000e+05 3.002815e+04 2.992825e+04 -5.350000e-01 5.000000e-03 5.000000e-03 6.561000e+05 2.732636e+04 2.722646e+04 -5.450000e-01 5.000000e-03 5.000000e-03 6.135000e+05 2.572800e+04 2.562811e+04 -5.550000e-01 5.000000e-03 5.000000e-03 5.738000e+05 2.373036e+04 2.363049e+04 -5.650000e-01 5.000000e-03 5.000000e-03 5.350000e+05 2.302629e+04 2.292640e+04 -5.750000e-01 5.000000e-03 5.000000e-03 4.979000e+05 2.052949e+04 2.042964e+04 -5.850000e-01 5.000000e-03 5.000000e-03 4.628000e+05 1.942576e+04 1.932589e+04 -5.950000e-01 5.000000e-03 5.000000e-03 4.306000e+05 2.072414e+04 2.072414e+04 -6.050000e-01 5.000000e-03 5.000000e-03 4.011500e+05 1.645861e+04 1.639871e+04 -6.150000e-01 5.000000e-03 5.000000e-03 3.722700e+05 1.561831e+04 1.556840e+04 -6.250000e-01 5.000000e-03 5.000000e-03 3.459800e+05 1.363041e+04 1.358052e+04 -6.350000e-01 5.000000e-03 5.000000e-03 3.210900e+05 1.428713e+04 1.422724e+04 -6.450000e-01 5.000000e-03 5.000000e-03 2.973500e+05 1.307765e+04 1.296789e+04 -6.550000e-01 5.000000e-03 5.000000e-03 2.747400e+05 1.343444e+04 1.329470e+04 -6.650000e-01 5.000000e-03 5.000000e-03 2.537800e+05 1.387195e+04 1.368225e+04 -6.750000e-01 5.000000e-03 5.000000e-03 2.346600e+05 1.221367e+04 1.194420e+04 -6.850000e-01 5.000000e-03 5.000000e-03 2.166800e+05 1.294061e+04 1.264110e+04 -6.950000e-01 5.000000e-03 5.000000e-03 1.990800e+05 1.184071e+04 1.147138e+04 -7.050000e-01 5.000000e-03 5.000000e-03 1.841900e+05 1.272818e+04 1.234874e+04 -7.150000e-01 5.000000e-03 5.000000e-03 1.690000e+05 1.279652e+04 1.240704e+04 -7.250000e-01 5.000000e-03 5.000000e-03 1.558800e+05 1.181681e+04 1.138744e+04 -7.350000e-01 5.000000e-03 5.000000e-03 1.431400e+05 1.168593e+04 1.123657e+04 -7.450000e-01 5.000000e-03 5.000000e-03 1.311900e+05 1.198404e+04 1.156455e+04 -7.550000e-01 5.000000e-03 5.000000e-03 1.198900e+05 1.137379e+04 1.095432e+04 -7.650000e-01 5.000000e-03 5.000000e-03 1.100400e+05 1.117306e+04 1.076355e+04 -7.750000e-01 5.000000e-03 5.000000e-03 9.973000e+04 1.032261e+04 9.903141e+03 -7.850000e-01 5.000000e-03 5.000000e-03 9.104000e+04 9.393317e+03 8.963956e+03 -7.950000e-01 5.000000e-03 5.000000e-03 8.287000e+04 9.542080e+03 9.152595e+03 -8.050000e-01 5.000000e-03 5.000000e-03 7.481000e+04 9.251443e+03 8.881920e+03 -8.150000e-01 5.000000e-03 5.000000e-03 6.754000e+04 8.551327e+03 8.181840e+03 -8.250000e-01 5.000000e-03 5.000000e-03 6.080000e+04 8.250697e+03 7.911157e+03 -8.350000e-01 5.000000e-03 5.000000e-03 5.431000e+04 7.520645e+03 7.171164e+03 -8.450000e-01 5.000000e-03 5.000000e-03 4.739000e+04 7.189527e+03 6.879956e+03 -8.550000e-01 5.000000e-03 5.000000e-03 4.218000e+04 6.989278e+03 6.699679e+03 -8.650000e-01 5.000000e-03 5.000000e-03 3.698000e+04 6.498900e+03 6.219301e+03 -8.750000e-01 5.000000e-03 5.000000e-03 3.238000e+04 5.978570e+03 5.708975e+03 -8.850000e-01 5.000000e-03 5.000000e-03 2.787000e+04 5.398907e+03 5.129376e+03 -8.950000e-01 5.000000e-03 5.000000e-03 2.340000e+04 5.327363e+03 5.097696e+03 -9.050000e-01 5.000000e-03 5.000000e-03 2.003000e+04 4.817572e+03 4.597934e+03 -9.150000e-01 5.000000e-03 5.000000e-03 1.700000e+04 4.836993e+03 4.627310e+03 -9.250000e-01 5.000000e-03 5.000000e-03 1.424000e+04 4.226819e+03 4.017176e+03 -9.350000e-01 5.000000e-03 5.000000e-03 1.175000e+04 4.017176e+03 3.817552e+03 -9.450000e-01 5.000000e-03 5.000000e-03 8.810000e+03 3.756448e+03 3.566791e+03 -9.550000e-01 5.000000e-03 5.000000e-03 6.370000e+03 3.596137e+03 3.406479e+03 -9.650000e-01 5.000000e-03 5.000000e-03 4.670000e+03 3.696552e+03 3.506907e+03 -9.750000e-01 5.000000e-03 5.000000e-03 5.920000e+03 7.732529e+03 7.353176e+03 -END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/NMD_1974_I745.cc b/analyses/pluginMisc/NMD_1974_I745.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginMisc/NMD_1974_I745.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class NMD_1974_I745 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(NMD_1974_I745); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(1, 1, 1); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 2); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(NMD_1974_I745); + + +} diff --git a/analyses/pluginMisc/NMD_1974_I745.info b/analyses/pluginMisc/NMD_1974_I745.info new file mode 100644 --- /dev/null +++ b/analyses/pluginMisc/NMD_1974_I745.info @@ -0,0 +1,35 @@ +Name: NMD_1974_I745 +Year: 1974 +Summary: Measurement of $R$ and the hadronic cross section for 4 GeV +Experiment: NMD +Collider: CEA +InspireID: 745 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 32 (1974) 432-435, 1974 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ and the hadronic cross seection in $e^+e^-$ collisions by + the Non-Magnetic Detector at 4 GeV. + The muonic cross section is also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Tarnopolsky:1974xb +BibTeX: '@article{Tarnopolsky:1974xb, + author = "Tarnopolsky, G. and Eshelman, J. and Law, M. E. and + Leong, J. and Newman, H. and Little, R. and Strauch, K. + and Wilson, R.", + title = "{Hadron Production by electron-Positron Annihilation at + 5-GeV Center-Of-Mass Energy}", + journal = "Phys. Rev. Lett.", + volume = "32", + year = "1974", + pages = "432-435", + doi = "10.1103/PhysRevLett.32.432", + reportNumber = "PRINT-74-0434 (CEA)", + SLACcitation = "%%CITATION = PRLTA,32,432;%%" +}' diff --git a/analyses/pluginMisc/NMD_1974_I745.plot b/analyses/pluginMisc/NMD_1974_I745.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginMisc/NMD_1974_I745.plot @@ -0,0 +1,27 @@ +BEGIN PLOT /NMD_1974_I745/d01-x01-y02 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +XMin=3.5 +XMax=4.5 +END PLOT +BEGIN PLOT /NMD_1974_I745/d01-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=3.5 +XMax=4.5 +END PLOT +BEGIN PLOT /NMD_1974_I745/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +XMin=3.5 +XMax=4.5 +END PLOT diff --git a/analyses/pluginMisc/NMD_1974_I745.yoda b/analyses/pluginMisc/NMD_1974_I745.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginMisc/NMD_1974_I745.yoda @@ -0,0 +1,18 @@ +BEGIN YODA_SCATTER2D_V2 /REF/NMD_1974_I745/d01-x01-y01 +IsRef: 1 +Path: /REF/NMD_1974_I745/d01-x01-y01 +Title: doi:10.17182/hepdata.21302.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.000000e+00 0.000000e+00 0.000000e+00 2.100000e+01 5.000000e+00 5.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/NMD_1974_I745/d01-x01-y02 +IsRef: 1 +Path: /REF/NMD_1974_I745/d01-x01-y02 +Title: doi:10.17182/hepdata.21302.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.000000e+00 0.000000e+00 0.000000e+00 6.000000e+00 1.500000e+00 1.500000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.cc b/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.cc @@ -0,0 +1,120 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Tools/Cuts.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class PDG_Upsilon_4S_HADRON_MULTIPLICITIES : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(PDG_Upsilon_4S_HADRON_MULTIPLICITIES); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(UnstableParticles(), "UFS"); + + for(int ix : _ihistos) + _histos[ix] = bookHisto1D(ix, 1, 1); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + double weight = event.weight(); + for(const Particle& meson : apply(event, "UFS").particles(Cuts::pid==300553)) { + _wSum += weight; + map ncount; + findDecayProducts(meson,ncount); + _histos[29]->fill(10.579,double(ncount[411]+ncount[-411])*weight); + _histos[30]->fill(10.579,double(ncount[421]+ncount[-421])*weight); + _histos[31]->fill(10.579,double(ncount[413]+ncount[-413])*weight); + _histos[32]->fill(10.579,double(ncount[423]+ncount[-423])*weight); + _histos[33]->fill(10.579,double(ncount[431]+ncount[-431])*weight); + _histos[34]->fill(10.579,double(ncount[433]+ncount[-433])*weight); + _histos[48]->fill(10.579,double(ncount[443])*weight); + _histos[50]->fill(10.579,double(ncount[100443])*weight); + _histos[51]->fill(10.579,double(ncount[20443])*weight); + _histos[53]->fill(10.579,double(ncount[445])*weight); + _histos[60]->fill(10.579,double(ncount[321]+ncount[-321])*weight); + _histos[61]->fill(10.579,double(ncount[321])*weight); + _histos[62]->fill(10.579,double(ncount[-321])*weight); + _histos[63]->fill(10.579,double(ncount[130]+ncount[310])*weight); + _histos[64]->fill(10.579,double(ncount[323]+ncount[-323])*weight); + _histos[65]->fill(10.579,double(ncount[313]+ncount[-313])*weight); + _histos[87]->fill(10.579,double(ncount[211]+ncount[-211])*weight); + _histos[88]->fill(10.579,double(ncount[111])*weight); + _histos[89]->fill(10.579,double(ncount[221])*weight); + _histos[90]->fill(10.579,double(ncount[113])*weight); + _histos[92]->fill(10.579,double(ncount[333])*weight); + _histos[96]->fill(10.579,double(ncount[4122]+ncount[-4122])*weight); + _histos[104]->fill(10.579,double(ncount[-4222])*weight); + _histos[106]->fill(10.579,double(ncount[-4112])*weight); + _histos[110]->fill(10.579,double(ncount[2212]+ncount[-2212])*weight); + _histos[113]->fill(10.579,double(ncount[3122]+ncount[-3122])*weight); + _histos[116]->fill(10.579,double(ncount[3312]+ncount[-3312])*weight); + } + } + + void findDecayProducts(const Particle & mother, + map & ncount) { + for(const Particle & p : mother.children()) { + int id = p.pdgId(); + if(p.children().empty()) { + ncount[id] += 1; + } + else { + // check particle is not a child or itself, eg copy or from photon radiation + bool isChild(false); + for(const Particle & p2 : p.children()) { + if(p2.pdgId()==id) { + isChild = true; + break; + } + } + if(!isChild) ncount[id] += 1; + findDecayProducts(p,ncount); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + for(auto hist : _histos) { + scale(hist.second, 1./_wSum); + } + + } + + //@} + + + /// @name Histograms + //@{ + vector _ihistos={29 ,30 ,31 ,32 ,33 ,34 ,48 ,50 ,51 ,53 ,60 ,61 ,62 ,63 , + 64 ,65 ,87 ,88 ,89 ,90 ,92 ,96 ,104,106,110,113,116}; + map _histos; + double _wSum = 0.; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(PDG_Upsilon_4S_HADRON_MULTIPLICITIES); + + +} diff --git a/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.info b/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.info new file mode 100644 --- /dev/null +++ b/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.info @@ -0,0 +1,28 @@ +Name: PDG_Upsilon_4S_HADRON_MULTIPLICITIES +Year: 2018 +Summary: Hadron multiplicities in $\Upsilon(4S)$ decays +Experiment: PDG +Collider: Various +InspireID: 1688995 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D98 (2018) no.3, 030001 +RunInfo: Any process producing Upsilon(4S) mesons +NeedCrossSection: no +Description: + 'Hadron multiplicities in $\Upsilon(4S)$ decays. In the PDG these are quoted as the $B^\pm/B^0$ admixture, however in fact the quoted numbers are half the multplicity in $\Upsilon(4S)$ decays.' +BibKey: Tanabashi:2018oca +BibTeX: '@article{Tanabashi:2018oca, + author = "Tanabashi, M. and others", + title = "{Review of Particle Physics}", + collaboration = "Particle Data Group", + journal = "Phys. Rev.", + volume = "D98", + year = "2018", + number = "3", + pages = "030001", + doi = "10.1103/PhysRevD.98.030001", + SLACcitation = "%%CITATION = PHRVA,D98,030001;%%" +}' diff --git a/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.plot b/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.plot @@ -0,0 +1,92 @@ +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d +XLabel= +YLabel=Multiplicity +LogY=0 +# END PLOT + + +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d29-x01-y01 +Title=Mean $D^\pm$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d30-x01-y01 +Title=Mean $D^0/\bar{D}^0$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d31-x01-y01 +Title=Mean $D^{*\pm}$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d32-x01-y01 +Title=Mean $D^{*0}/\bar{D}^{*0}$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d33-x01-y01 +Title=Mean $D_s^\pm$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d34-x01-y01 +Title=Mean $D_s^{*\pm}$ multiplicity +# END PLOT + + +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d48-x01-y01 +Title=Mean $J/\psi$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d50-x01-y01 +Title=Mean $\psi(2S)$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d51-x01-y01 +Title=Mean $\chi_{c1}(1P)$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d53-x01-y01 +Title=Mean $\chi_{c2}(1P)$ multiplicity +# END PLOT + +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d60-x01-y01 +Title=Mean $K^{\pm}$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d61-x01-y01 +Title=Mean $K^+$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d62-x01-y01 +Title=Mean $K^-$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d63-x01-y01 +Title=Mean $K^0/\bar{K}^0$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d64-x01-y01 +Title=Mean $K^{*\pm}$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d65-x01-y01 +Title=Mean $K^{*0}/\bar{K}^{*0}$ multiplicity +# END PLOT + +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d87-x01-y01 +Title=Mean $\pi^\pm$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d88-x01-y01 +Title=Mean $\pi^0$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d89-x01-y01 +Title=Mean $\eta$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d90-x01-y01 +Title=Mean $\rho^0$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d92-x01-y01 +Title=Mean $\phi$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d96-x01-y01 +Title=Mean $\Lambda_c^+/\bar{\Lambda}_c^-$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d104-x01-y01 +Title=Mean $\bar{\Sigma}_c^{++}$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d106-x01-y01 +Title=Mean $\bar{\Sigma}_c^{0}$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d110-x01-y01 +Title=Mean $p/\bar{p}$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d113-x01-y01 +Title=Mean $\Lambda/\bar{\Lambda}$ multiplicity +# END PLOT +# BEGIN PLOT /PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d116-x01-y01 +Title=Mean $\Xi^-/\bar{\Xi}^+$ multiplicity +# END PLOT \ No newline at end of file diff --git a/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.yoda b/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginMisc/PDG_Upsilon_4S_HADRON_MULTIPLICITIES.yoda @@ -0,0 +1,243 @@ +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d29-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d29-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 4.82000e-01 2.80000e-02 2.80000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d30-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d30-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 1.24800e+00 5.80000e-02 5.80000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d31-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d31-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 4.50000e-01 3.00000e-02 3.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d32-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d32-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 5.20000e-01 5.40000e-02 5.40000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d33-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d33-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 1.66000e-01 1.60000e-02 1.60000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d34-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d34-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 1.26000e-01 2.00000e-02 2.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d48-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d48-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 2.18800e-02 6.40000e-04 6.40000e-04 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d50-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d50-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 6.14000e-03 4.20000e-04 4.20000e-04 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d51-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d51-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 7.10000e-03 5.40000e-04 5.40000e-04 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d53-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d53-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 2.00000e-03 3.40000e-04 3.40000e-04 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d60-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d60-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 1.57800e+00 5.00000e-02 5.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d61-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d61-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 1.32000e+00 1.00000e-01 1.00000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d62-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d62-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 2.60000e-01 8.00000e-02 8.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d63-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d63-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 1.28000e+00 8.00000e-02 8.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d64-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d64-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 3.60000e-01 1.20000e-01 1.20000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d65-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d65-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 2.92000e-01 5.20000e-02 5.20000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d87-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d87-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 7.16000e+00 1.40000e-01 1.40000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d88-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d88-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 4.70000e+00 2.20000e-01 2.20000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d89-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d89-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 3.52000e-01 3.20000e-02 3.20000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d90-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d90-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 4.20000e-01 1.00000e-01 1.00000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d92-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d92-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 6.86000e-02 2.40000e-03 2.40000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d96-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d96-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 7.20000e-02 8.00000e-03 8.00000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d104-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d104-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 6.80000e-03 3.40000e-03 3.40000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d106-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d106-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 7.40000e-03 3.40000e-03 3.40000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d110-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d110-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 1.60000e-01 8.00000e-03 8.00000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d113-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d113-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 8.00000e-02 1.00000e-02 1.00000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d116-x01-y01 +IsRef: 1 +Path: /REF/PDG_Upsilon_4S_HADRON_MULTIPLICITIES/d116-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +10.57900 0.50000 0.50000 5.40000e-03 1.20000e-03 1.20000e-03 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_1995_I406880.cc b/analyses/pluginNovosibirsk/CMD2_1995_I406880.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1995_I406880.cc @@ -0,0 +1,147 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_1995_I406880 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_1995_I406880); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nKpKm = bookCounter("TMP/KpKm"); + _nK0K0 = bookCounter("TMP/K0K0"); + _n3pi = bookCounter("TMP/3pi"); + _numEtaGamma = bookCounter("TMP/EtaGamma"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2) { + if(nCount[321]==1 && nCount[-321]==1) + _nKpKm->fill(event.weight()); + else if(nCount[130]==1 && nCount[310]==1) + _nK0K0->fill(event.weight()); + } + else if(ntotal==3 && nCount[211] == 1 && nCount[-211] == 1 && nCount[111] == 1) + _n3pi->fill(event.weight()); + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(val.first==22) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaGamma->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<5;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _nKpKm->val(); + error = _nKpKm->err(); + } + else if(ix==2) { + sigma = _nK0K0->val(); + error = _nK0K0->err(); + } + else if(ix==3) { + sigma = _n3pi->val(); + error = _n3pi->err(); + } + else if(ix==4) { + sigma = _numEtaGamma->val(); + error = _numEtaGamma->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + //@} + + + /// @name Histograms + //@{ + CounterPtr _nKpKm,_nK0K0,_n3pi,_numEtaGamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_1995_I406880); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_1995_I406880.info b/analyses/pluginNovosibirsk/CMD2_1995_I406880.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1995_I406880.info @@ -0,0 +1,31 @@ +Name: CMD2_1995_I406880 +Year: 1995 +Summary: Cross section for $e^+e^-\to$ $K^+K^-$, $K_S^0K_L^0$, $\pi^+\pi^-\pi^0$ and $\eta\gamma$ near the $\phi$ resonance +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 406880 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Lett. B364 (1995) 199-206, 1995 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to$ $K^+K^-$, $K_S^0K_L^0$, $\pi^+\pi^-\pi^0$ and $\eta\gamma$ near the $\phi$ resonance' +Keywords: +BibKey: Akhmetshin:1995vz +BibTeX: '@article{Akhmetshin:1995vz, + author = "Akhmetshin, R. R. and others", + title = "{Measurement of phi meson parameters with CMD-2 detector + at VEPP-2M collider}", + journal = "Phys. Lett.", + volume = "B364", + year = "1995", + pages = "199-206", + doi = "10.1016/0370-2693(95)01394-6", + SLACcitation = "%%CITATION = PHLTA,B364,199;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_1995_I406880.plot b/analyses/pluginNovosibirsk/CMD2_1995_I406880.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1995_I406880.plot @@ -0,0 +1,24 @@ +BEGIN PLOT /CMD2_1995_I406880/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_1995_I406880/d01-x01-y02 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_1995_I406880/d01-x01-y03 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_1995_I406880/d01-x01-y04 +Title=$\sigma(e^+e^-\to \eta\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\gamma)$/nb +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginNovosibirsk/CMD2_1995_I406880.yoda b/analyses/pluginNovosibirsk/CMD2_1995_I406880.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1995_I406880.yoda @@ -0,0 +1,93 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1995_I406880/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1995_I406880/d01-x01-y01 +Title: doi:10.17182/hepdata.28437.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.008624e+03 4.020000e-01 4.020000e-01 5.000000e+01 5.000000e+01 5.000000e+01 +1.013882e+03 1.820000e-01 1.820000e-01 2.220000e+02 5.400000e+01 5.400000e+01 +1.016726e+03 9.000000e-02 9.000000e-02 7.130000e+02 1.140000e+02 1.140000e+02 +1.017264e+03 9.600000e-02 9.600000e-02 8.970000e+02 1.340000e+02 1.340000e+02 +1.017654e+03 8.200000e-02 8.200000e-02 1.224000e+03 1.350000e+02 1.350000e+02 +1.017934e+03 8.200000e-02 8.200000e-02 1.236000e+03 1.340000e+02 1.340000e+02 +1.017992e+03 6.600000e-02 6.600000e-02 1.477000e+03 8.600000e+01 8.600000e+01 +1.018322e+03 6.600000e-02 6.600000e-02 1.844000e+03 1.430000e+02 1.430000e+02 +1.018806e+03 7.400000e-02 7.400000e-02 1.852000e+03 2.190000e+02 2.190000e+02 +1.019070e+03 7.000000e-02 7.000000e-02 2.317000e+03 1.660000e+02 1.660000e+02 +1.019468e+03 1.040000e-01 1.040000e-01 2.152000e+03 2.720000e+02 2.720000e+02 +1.019636e+03 9.400000e-02 9.400000e-02 1.939000e+03 3.470000e+02 3.470000e+02 +1.021762e+03 8.400000e-02 8.400000e-02 9.730000e+02 1.260000e+02 1.260000e+02 +1.022072e+03 9.600000e-02 9.600000e-02 7.190000e+02 1.040000e+02 1.040000e+02 +1.027996e+03 1.240000e-01 1.240000e-01 1.610000e+02 2.500000e+01 2.500000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1995_I406880/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD2_1995_I406880/d01-x01-y02 +Title: doi:10.17182/hepdata.28437.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.008624e+03 4.020000e-01 4.020000e-01 1.800000e+01 5.000000e+00 5.000000e+00 +1.013882e+03 1.820000e-01 1.820000e-01 1.380000e+02 1.400000e+01 1.400000e+01 +1.016726e+03 9.000000e-02 9.000000e-02 5.040000e+02 3.600000e+01 3.600000e+01 +1.017264e+03 9.600000e-02 9.600000e-02 7.390000e+02 4.900000e+01 4.900000e+01 +1.017654e+03 8.200000e-02 8.200000e-02 8.310000e+02 4.700000e+01 4.700000e+01 +1.017934e+03 8.200000e-02 8.200000e-02 9.370000e+02 5.300000e+01 5.300000e+01 +1.017992e+03 6.600000e-02 6.600000e-02 9.850000e+02 4.000000e+01 4.000000e+01 +1.018322e+03 6.600000e-02 6.600000e-02 1.118000e+03 4.600000e+01 4.600000e+01 +1.018806e+03 7.400000e-02 7.400000e-02 1.277000e+03 5.200000e+01 5.200000e+01 +1.019070e+03 7.000000e-02 7.000000e-02 1.303000e+03 4.600000e+01 4.600000e+01 +1.019468e+03 1.040000e-01 1.040000e-01 1.411000e+03 6.200000e+01 6.200000e+01 +1.019636e+03 9.400000e-02 9.400000e-02 1.334000e+03 6.800000e+01 6.800000e+01 +1.021762e+03 8.400000e-02 8.400000e-02 6.690000e+02 3.600000e+01 3.600000e+01 +1.022072e+03 9.600000e-02 9.600000e-02 5.790000e+02 3.000000e+01 3.000000e+01 +1.027996e+03 1.240000e-01 1.240000e-01 1.100000e+02 6.000000e+00 6.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1995_I406880/d01-x01-y03 +IsRef: 1 +Path: /REF/CMD2_1995_I406880/d01-x01-y03 +Title: doi:10.17182/hepdata.28437.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.939560e+02 6.000000e-01 6.000000e-01 3.100000e+01 7.000000e+00 7.000000e+00 +1.008624e+03 4.020000e-01 4.020000e-01 5.400000e+01 9.000000e+00 9.000000e+00 +1.013882e+03 1.820000e-01 1.820000e-01 1.580000e+02 1.600000e+01 1.600000e+01 +1.016726e+03 9.000000e-02 9.000000e-02 3.730000e+02 2.700000e+01 2.700000e+01 +1.017264e+03 9.600000e-02 9.600000e-02 4.470000e+02 3.100000e+01 3.100000e+01 +1.017654e+03 8.200000e-02 8.200000e-02 4.730000e+02 2.900000e+01 2.900000e+01 +1.017934e+03 8.200000e-02 8.200000e-02 5.550000e+02 3.000000e+01 3.000000e+01 +1.017992e+03 6.600000e-02 6.600000e-02 5.450000e+02 2.000000e+01 2.000000e+01 +1.018322e+03 6.600000e-02 6.600000e-02 5.700000e+02 2.800000e+01 2.800000e+01 +1.018806e+03 7.400000e-02 7.400000e-02 6.310000e+02 3.700000e+01 3.700000e+01 +1.019070e+03 7.000000e-02 7.000000e-02 6.620000e+02 3.200000e+01 3.200000e+01 +1.019468e+03 1.040000e-01 1.040000e-01 5.750000e+02 4.400000e+01 4.400000e+01 +1.019636e+03 9.400000e-02 9.400000e-02 6.210000e+02 5.100000e+01 5.100000e+01 +1.021762e+03 8.400000e-02 8.400000e-02 2.520000e+02 2.200000e+01 2.200000e+01 +1.022072e+03 9.600000e-02 9.600000e-02 1.870000e+02 1.600000e+01 1.600000e+01 +1.027996e+03 1.240000e-01 1.240000e-01 2.100000e+01 3.000000e+00 3.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1995_I406880/d01-x01-y04 +IsRef: 1 +Path: /REF/CMD2_1995_I406880/d01-x01-y04 +Title: doi:10.17182/hepdata.28437.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.008624e+03 4.020000e-01 4.020000e-01 5.000000e+00 3.000000e+00 3.000000e+00 +1.013882e+03 1.820000e-01 1.820000e-01 5.000000e+00 3.000000e+00 3.000000e+00 +1.016726e+03 9.000000e-02 9.000000e-02 3.200000e+01 1.100000e+01 1.100000e+01 +1.017264e+03 9.600000e-02 9.600000e-02 1.900000e+01 6.000000e+00 6.000000e+00 +1.017654e+03 8.200000e-02 8.200000e-02 3.700000e+01 9.000000e+00 9.000000e+00 +1.017934e+03 8.200000e-02 8.200000e-02 2.700000e+01 8.000000e+00 8.000000e+00 +1.017992e+03 6.600000e-02 6.600000e-02 4.600000e+01 7.000000e+00 7.000000e+00 +1.018322e+03 6.600000e-02 6.600000e-02 3.400000e+01 8.000000e+00 8.000000e+00 +1.018806e+03 7.400000e-02 7.400000e-02 4.600000e+01 1.400000e+01 1.400000e+01 +1.019070e+03 7.000000e-02 7.000000e-02 5.600000e+01 1.000000e+01 1.000000e+01 +1.019468e+03 1.040000e-01 1.040000e-01 6.000000e+01 2.000000e+01 2.000000e+01 +1.019636e+03 9.400000e-02 9.400000e-02 3.600000e+01 1.800000e+01 1.800000e+01 +1.021762e+03 8.400000e-02 8.400000e-02 2.800000e+01 8.000000e+00 8.000000e+00 +1.022072e+03 9.600000e-02 9.600000e-02 2.400000e+01 7.000000e+00 7.000000e+00 +1.027996e+03 1.240000e-01 1.240000e-01 3.000000e+00 1.000000e+00 1.000000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_1998_I480170.cc b/analyses/pluginNovosibirsk/CMD2_1998_I480170.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1998_I480170.cc @@ -0,0 +1,85 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_1998_I480170 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_1998_I480170); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + _num3pi = bookCounter("TMP/num3"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=3) vetoEvent; + if(nCount[-211]==1&&nCount[211]==1&&nCount[111]==1) + _num3pi->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _num3pi->val(); + double error = _num3pi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _num3pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_1998_I480170); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_1998_I480170.info b/analyses/pluginNovosibirsk/CMD2_1998_I480170.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1998_I480170.info @@ -0,0 +1,29 @@ +Name: CMD2_1998_I480170 +Year: 1998 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ near the $\phi$ mass +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 480170 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B434 (1998) 426-436, 1998 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ for energies near the $\phi$ mass.' +Keywords: +BibKey: Akhmetshin:1998se +BibTeX: '@article{Akhmetshin:1998se, + author = "Akhmetshin, R. R. and others", + title = "{Study of dynamics of Phi --> pi+ pi- pi0 decay with + CMD-2 detector}", + journal = "Phys. Lett.", + volume = "B434", + year = "1998", + pages = "426-436", + doi = "10.1016/S0370-2693(98)00826-0", + SLACcitation = "%%CITATION = PHLTA,B434,426;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_1998_I480170.plot b/analyses/pluginNovosibirsk/CMD2_1998_I480170.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1998_I480170.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /CMD2_1998_I480170/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +LegendXPos=0.1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_1998_I480170.yoda b/analyses/pluginNovosibirsk/CMD2_1998_I480170.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1998_I480170.yoda @@ -0,0 +1,22 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1998_I480170/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1998_I480170/d01-x01-y01 +Title: doi:10.17182/hepdata.28172.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.940000e+02 2.000000e-01 2.000000e-01 1.800000e+01 3.000000e+00 3.000000e+00 +1.012760e+03 6.000000e-02 6.000000e-02 1.080000e+02 1.000000e+01 1.000000e+01 +1.016540e+03 7.000000e-02 7.000000e-02 2.980000e+02 1.600000e+01 1.600000e+01 +1.018260e+03 6.000000e-02 6.000000e-02 5.330000e+02 2.300000e+01 2.300000e+01 +1.018870e+03 6.000000e-02 6.000000e-02 6.500000e+02 2.500000e+01 2.500000e+01 +1.019510e+03 6.000000e-02 6.000000e-02 6.270000e+02 2.100000e+01 2.100000e+01 +1.020760e+03 6.000000e-02 6.000000e-02 3.690000e+02 1.600000e+01 1.600000e+01 +1.021350e+03 6.000000e-02 6.000000e-02 2.650000e+02 1.600000e+01 1.600000e+01 +1.021540e+03 6.000000e-02 6.000000e-02 2.740000e+02 1.800000e+01 1.800000e+01 +1.022230e+03 6.000000e-02 6.000000e-02 1.640000e+02 1.600000e+01 1.600000e+01 +1.022940e+03 6.000000e-02 6.000000e-02 1.030000e+02 1.100000e+01 1.100000e+01 +1.025350e+03 7.000000e-02 7.000000e-02 3.700000e+01 6.000000e+00 6.000000e+00 +1.029200e+03 7.000000e-02 7.000000e-02 7.000000e+00 4.000000e+00 4.000000e+00 +1.040000e+03 2.000000e-01 2.000000e-01 1.000000e-01 1.000000e-01 4.000000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I483994.cc b/analyses/pluginNovosibirsk/CMD2_1999_I483994.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I483994.cc @@ -0,0 +1,142 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_1999_I483994 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_1999_I483994); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _ncharged = bookCounter("TMP/charged"); + _nneutral = bookCounter("TMP/neutral"); + _nomega = bookCounter("TMP/omega"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==4) { + if( nCount[211] == 2 && nCount[-211] == 2 ) + _ncharged->fill(event.weight()); + else if( nCount[211] == 1 && nCount[-211] == 1 && nCount[111] == 2) + _nneutral->fill(event.weight()); + } + + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==223) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // omega pi+pi- + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==111) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nomega->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<4;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _ncharged->val(); + error = _ncharged->err(); + } + else if(ix==2) { + sigma = _nneutral->val(); + error = _nneutral->err(); + } + else if(ix==3) { + sigma = _nomega->val(); + error = _nomega->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _ncharged,_nneutral,_nomega; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_1999_I483994); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I483994.info b/analyses/pluginNovosibirsk/CMD2_1999_I483994.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I483994.info @@ -0,0 +1,35 @@ +Name: CMD2_1999_I483994 +Year: 1999 +Summary: Cross section for $e^+e^-\to2\pi^+2\pi^-$ and $\pi^+\pi^-2\pi^0$ below 1.38 GeV +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 483994 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B466 (1999) 392-402, 199 9 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to2\pi^+2\pi^-$ and $\pi^+\pi^-2\pi^0$ below 1.38 GeV' +Keywords: +BibKey: Akhmetshin:1998df +BibTeX: '@article{Akhmetshin:1998df, + author = "Akhmetshin, R. R. and others", + title = "{a(1)(1260) pi dominance in the process e+ e- ---> 4 pi + at energies 1.05-GeV - 1.38-GeV}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B466", + year = "1999", + pages = "392-402", + doi = "10.1016/S0370-2693(99)01080-1", + eprint = "hep-ex/9904024", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BUDKER-INP-1998-83", + SLACcitation = "%%CITATION = HEP-EX/9904024;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I483994.plot b/analyses/pluginNovosibirsk/CMD2_1999_I483994.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I483994.plot @@ -0,0 +1,24 @@ +BEGIN PLOT /CMD2_1999_I483994/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_1999_I483994/d02-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_1999_I483994/d03-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I483994.yoda b/analyses/pluginNovosibirsk/CMD2_1999_I483994.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I483994.yoda @@ -0,0 +1,81 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I483994/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1999_I483994/d01-x01-y01 +Title: doi:10.17182/hepdata.50145.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.800000e+02 0.000000e+00 0.000000e+00 2.100000e-01 9.535329e-02 9.535329e-02 +1.046000e+03 0.000000e+00 0.000000e+00 1.200000e+00 2.109502e-01 2.109502e-01 +1.065000e+03 0.000000e+00 0.000000e+00 2.130000e+00 3.573237e-01 3.573237e-01 +1.086000e+03 0.000000e+00 0.000000e+00 2.190000e+00 3.794895e-01 3.794895e-01 +1.106000e+03 0.000000e+00 0.000000e+00 2.860000e+00 4.776411e-01 4.776411e-01 +1.127000e+03 0.000000e+00 0.000000e+00 3.180000e+00 5.295555e-01 5.295555e-01 +1.143000e+03 0.000000e+00 0.000000e+00 4.270000e+00 6.875611e-01 6.875611e-01 +1.164000e+03 0.000000e+00 0.000000e+00 4.620000e+00 7.333819e-01 7.333819e-01 +1.186000e+03 0.000000e+00 0.000000e+00 6.130000e+00 9.528800e-01 9.528800e-01 +1.204000e+03 0.000000e+00 0.000000e+00 8.310000e+00 1.273327e+00 1.273327e+00 +1.225000e+03 0.000000e+00 0.000000e+00 9.060000e+00 1.393909e+00 1.393909e+00 +1.246000e+03 0.000000e+00 0.000000e+00 1.016000e+01 1.547733e+00 1.547733e+00 +1.266000e+03 0.000000e+00 0.000000e+00 1.156000e+01 1.753384e+00 1.753384e+00 +1.286000e+03 0.000000e+00 0.000000e+00 1.244000e+01 1.881371e+00 1.881371e+00 +1.305000e+03 0.000000e+00 0.000000e+00 1.454000e+01 2.197649e+00 2.197649e+00 +1.327000e+03 0.000000e+00 0.000000e+00 1.483000e+01 2.239643e+00 2.239643e+00 +1.346000e+03 0.000000e+00 0.000000e+00 1.692000e+01 2.556862e+00 2.556862e+00 +1.362000e+03 0.000000e+00 0.000000e+00 1.711000e+01 2.586372e+00 2.586372e+00 +1.380000e+03 0.000000e+00 0.000000e+00 1.980000e+01 2.985113e+00 2.985113e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I483994/d02-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1999_I483994/d02-x01-y01 +Title: doi:10.17182/hepdata.50145.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.800000e+02 0.000000e+00 0.000000e+00 3.600000e+00 9.404786e-01 9.404786e-01 +1.046000e+03 0.000000e+00 0.000000e+00 8.980000e+00 1.487047e+00 1.487047e+00 +1.065000e+03 0.000000e+00 0.000000e+00 9.040000e+00 1.530633e+00 1.530633e+00 +1.086000e+03 0.000000e+00 0.000000e+00 1.014000e+01 1.718558e+00 1.718558e+00 +1.106000e+03 0.000000e+00 0.000000e+00 1.116000e+01 1.855337e+00 1.855337e+00 +1.127000e+03 0.000000e+00 0.000000e+00 1.144000e+01 1.910564e+00 1.910564e+00 +1.143000e+03 0.000000e+00 0.000000e+00 1.278000e+01 2.085015e+00 2.085015e+00 +1.164000e+03 0.000000e+00 0.000000e+00 1.413000e+01 2.261942e+00 2.261942e+00 +1.186000e+03 0.000000e+00 0.000000e+00 1.374000e+01 2.179867e+00 2.179867e+00 +1.204000e+03 0.000000e+00 0.000000e+00 1.519000e+01 2.372164e+00 2.372164e+00 +1.225000e+03 0.000000e+00 0.000000e+00 1.734000e+01 2.721250e+00 2.721250e+00 +1.246000e+03 0.000000e+00 0.000000e+00 1.793000e+01 2.771698e+00 2.771698e+00 +1.266000e+03 0.000000e+00 0.000000e+00 1.936000e+01 2.973687e+00 2.973687e+00 +1.286000e+03 0.000000e+00 0.000000e+00 2.021000e+01 3.086485e+00 3.086485e+00 +1.305000e+03 0.000000e+00 0.000000e+00 2.226000e+01 3.396074e+00 3.396074e+00 +1.327000e+03 0.000000e+00 0.000000e+00 2.031000e+01 3.099365e+00 3.099365e+00 +1.346000e+03 0.000000e+00 0.000000e+00 2.036000e+01 3.120339e+00 3.120339e+00 +1.362000e+03 0.000000e+00 0.000000e+00 2.143000e+01 3.285637e+00 3.285637e+00 +1.380000e+03 0.000000e+00 0.000000e+00 2.589000e+01 3.937521e+00 3.937521e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I483994/d03-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1999_I483994/d03-x01-y01 +Title: doi:10.17182/hepdata.50145.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.800000e+02 0.000000e+00 0.000000e+00 4.150000e+00 9.670089e-01 9.670089e-01 +1.046000e+03 0.000000e+00 0.000000e+00 1.021000e+01 1.679760e+00 1.679760e+00 +1.065000e+03 0.000000e+00 0.000000e+00 1.013000e+01 1.698964e+00 1.698964e+00 +1.086000e+03 0.000000e+00 0.000000e+00 1.094000e+01 1.843497e+00 1.843497e+00 +1.106000e+03 0.000000e+00 0.000000e+00 1.141000e+01 1.906524e+00 1.906524e+00 +1.127000e+03 0.000000e+00 0.000000e+00 1.213000e+01 2.025507e+00 2.025507e+00 +1.143000e+03 0.000000e+00 0.000000e+00 1.230000e+01 2.039835e+00 2.039835e+00 +1.164000e+03 0.000000e+00 0.000000e+00 1.303000e+01 2.127362e+00 2.127362e+00 +1.186000e+03 0.000000e+00 0.000000e+00 1.325000e+01 2.127852e+00 2.127852e+00 +1.204000e+03 0.000000e+00 0.000000e+00 1.315000e+01 2.093026e+00 2.093026e+00 +1.225000e+03 0.000000e+00 0.000000e+00 1.437000e+01 2.313392e+00 2.313392e+00 +1.246000e+03 0.000000e+00 0.000000e+00 1.566000e+01 2.448244e+00 2.448244e+00 +1.266000e+03 0.000000e+00 0.000000e+00 1.513000e+01 2.358014e+00 2.358014e+00 +1.286000e+03 0.000000e+00 0.000000e+00 1.640000e+01 2.525173e+00 2.525173e+00 +1.305000e+03 0.000000e+00 0.000000e+00 1.641000e+01 2.531221e+00 2.531221e+00 +1.327000e+03 0.000000e+00 0.000000e+00 1.494000e+01 2.302820e+00 2.302820e+00 +1.346000e+03 0.000000e+00 0.000000e+00 1.435000e+01 2.229273e+00 2.229273e+00 +1.362000e+03 0.000000e+00 0.000000e+00 1.556000e+01 2.412396e+00 2.412396e+00 +1.380000e+03 0.000000e+00 0.000000e+00 1.861000e+01 2.851118e+00 2.851118e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I498859.cc b/analyses/pluginNovosibirsk/CMD2_1999_I498859.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I498859.cc @@ -0,0 +1,80 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_1999_I498859 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_1999_I498859); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_1999_I498859); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I498859.info b/analyses/pluginNovosibirsk/CMD2_1999_I498859.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I498859.info @@ -0,0 +1,32 @@ +Name: CMD2_1999_I498859 +Year: 1999 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ at near the $\rho$ mass. +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 498859 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B527 (2002) 161-172, 2002 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies near the $\rho$ mass.' +Keywords: [] +BibKey: Akhmetshin:1999uj +BibTeX: '@article{Akhmetshin:1999uj, + author = "Akhmetshin, R. R. and others", + title = "{Measurement of e+ e- ---> pi+ pi- cross-section with + CMD-2 around rho meson}", + collaboration = "CMD-2", + year = "1999", + eprint = "hep-ex/9904027", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BUDKER-INP-1999-10", + SLACcitation = "%%CITATION = HEP-EX/9904027;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I498859.plot b/analyses/pluginNovosibirsk/CMD2_1999_I498859.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I498859.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /CMD2_1999_I498859/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I498859.yoda b/analyses/pluginNovosibirsk/CMD2_1999_I498859.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I498859.yoda @@ -0,0 +1,104 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I498859/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1999_I498859/d01-x01-y01 +Title: doi:10.17182/hepdata.50143.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.105000e+02 0.000000e+00 0.000000e+00 3.336000e+02 3.917368e+01 3.917368e+01 +6.205000e+02 0.000000e+00 0.000000e+00 3.780000e+02 2.730703e+01 2.730703e+01 +6.305000e+02 0.000000e+00 0.000000e+00 4.228000e+02 2.841059e+01 2.841059e+01 +6.405100e+02 0.000000e+00 0.000000e+00 4.363000e+02 2.727836e+01 2.727836e+01 +6.504900e+02 0.000000e+00 0.000000e+00 4.922000e+02 3.096052e+01 3.096052e+01 +6.605000e+02 0.000000e+00 0.000000e+00 5.494000e+02 2.728357e+01 2.728357e+01 +6.705000e+02 0.000000e+00 0.000000e+00 6.026000e+02 2.902689e+01 2.902689e+01 +6.805900e+02 0.000000e+00 0.000000e+00 6.979000e+02 3.152009e+01 3.152009e+01 +6.904300e+02 0.000000e+00 0.000000e+00 7.178000e+02 2.718484e+01 2.718484e+01 +7.005200e+02 0.000000e+00 0.000000e+00 8.451000e+02 2.661457e+01 2.661457e+01 +7.104700e+02 0.000000e+00 0.000000e+00 9.460000e+02 2.938561e+01 2.938561e+01 +7.202500e+02 0.000000e+00 0.000000e+00 1.018300e+03 3.333364e+01 3.333364e+01 +7.302400e+02 0.000000e+00 0.000000e+00 1.111900e+03 4.072670e+01 4.072670e+01 +7.402000e+02 0.000000e+00 0.000000e+00 1.181500e+03 4.110123e+01 4.110123e+01 +7.502800e+02 0.000000e+00 0.000000e+00 1.315900e+03 4.151814e+01 4.151814e+01 +7.601800e+02 0.000000e+00 0.000000e+00 1.337800e+03 4.499582e+01 4.499582e+01 +7.641700e+02 0.000000e+00 0.000000e+00 1.301800e+03 3.432228e+01 3.432228e+01 +7.701100e+02 0.000000e+00 0.000000e+00 1.301100e+03 3.874944e+01 3.874944e+01 +7.743800e+02 0.000000e+00 0.000000e+00 1.250500e+03 3.977286e+01 3.977286e+01 +7.781700e+02 0.000000e+00 0.000000e+00 1.313600e+03 4.213436e+01 4.213436e+01 +7.801700e+02 0.000000e+00 0.000000e+00 1.253900e+03 3.970346e+01 3.970346e+01 +7.822300e+02 0.000000e+00 0.000000e+00 1.080700e+03 2.434911e+01 2.434911e+01 +7.842400e+02 0.000000e+00 0.000000e+00 9.869000e+02 2.788355e+01 2.788355e+01 +7.860400e+02 0.000000e+00 0.000000e+00 8.696000e+02 3.270094e+01 3.270094e+01 +7.901000e+02 0.000000e+00 0.000000e+00 8.863000e+02 2.633840e+01 2.633840e+01 +7.941400e+02 0.000000e+00 0.000000e+00 8.365000e+02 2.575555e+01 2.575555e+01 +8.000200e+02 0.000000e+00 0.000000e+00 8.196000e+02 2.405026e+01 2.405026e+01 +8.099800e+02 0.000000e+00 0.000000e+00 6.965000e+02 1.783652e+01 1.783652e+01 +8.101400e+02 0.000000e+00 0.000000e+00 6.992000e+02 1.827882e+01 1.827882e+01 +8.200200e+02 0.000000e+00 0.000000e+00 6.482000e+02 2.357777e+01 2.357777e+01 +8.299700e+02 0.000000e+00 0.000000e+00 5.427000e+02 2.127342e+01 2.127342e+01 +8.391000e+02 0.000000e+00 0.000000e+00 4.503000e+02 1.961866e+01 1.961866e+01 +8.492400e+02 0.000000e+00 0.000000e+00 3.622000e+02 1.534400e+01 1.534400e+01 +8.596000e+02 0.000000e+00 0.000000e+00 3.643000e+02 1.735054e+01 1.735054e+01 +8.695000e+02 0.000000e+00 0.000000e+00 2.748000e+02 1.220897e+01 1.220897e+01 +8.798400e+02 0.000000e+00 0.000000e+00 2.606000e+02 1.943834e+01 1.943834e+01 +8.897200e+02 0.000000e+00 0.000000e+00 2.034000e+02 8.860211e+00 8.860211e+00 +9.000400e+02 0.000000e+00 0.000000e+00 1.820000e+02 7.440417e+00 7.440417e+00 +9.100200e+02 0.000000e+00 0.000000e+00 1.564000e+02 7.614887e+00 7.614887e+00 +9.195600e+02 0.000000e+00 0.000000e+00 1.356000e+02 7.151250e+00 7.151250e+00 +9.301100e+02 0.000000e+00 0.000000e+00 1.278000e+02 8.193650e+00 8.193650e+00 +9.421900e+02 0.000000e+00 0.000000e+00 1.161000e+02 5.634537e+00 5.634537e+00 +9.518400e+02 0.000000e+00 0.000000e+00 9.630000e+01 5.271674e+00 5.271674e+00 +9.615200e+02 0.000000e+00 0.000000e+00 9.160000e+01 5.061718e+00 5.061718e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I498859/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD2_1999_I498859/d01-x01-y02 +Title: doi:10.17182/hepdata.50143.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.105000e+02 0.000000e+00 0.000000e+00 8.140000e+00 9.566723e-01 9.566723e-01 +6.205000e+02 0.000000e+00 0.000000e+00 9.410000e+00 6.825696e-01 6.825696e-01 +6.305000e+02 0.000000e+00 0.000000e+00 1.074000e+01 7.254287e-01 7.254287e-01 +6.405100e+02 0.000000e+00 0.000000e+00 1.131000e+01 7.075732e-01 7.075732e-01 +6.504900e+02 0.000000e+00 0.000000e+00 1.302000e+01 8.200902e-01 8.200902e-01 +6.605000e+02 0.000000e+00 0.000000e+00 1.483000e+01 7.391389e-01 7.391389e-01 +6.705000e+02 0.000000e+00 0.000000e+00 1.660000e+01 8.036215e-01 8.036215e-01 +6.805900e+02 0.000000e+00 0.000000e+00 1.963000e+01 8.829409e-01 8.829409e-01 +6.904300e+02 0.000000e+00 0.000000e+00 2.059000e+01 7.837717e-01 7.837717e-01 +7.005200e+02 0.000000e+00 0.000000e+00 2.476000e+01 7.795557e-01 7.795557e-01 +7.104700e+02 0.000000e+00 0.000000e+00 2.828000e+01 8.818467e-01 8.818467e-01 +7.202500e+02 0.000000e+00 0.000000e+00 3.106000e+01 1.015690e+00 1.015690e+00 +7.302400e+02 0.000000e+00 0.000000e+00 3.461000e+01 1.264471e+00 1.264471e+00 +7.402000e+02 0.000000e+00 0.000000e+00 3.753000e+01 1.307835e+00 1.307835e+00 +7.502800e+02 0.000000e+00 0.000000e+00 4.266000e+01 1.346669e+00 1.346669e+00 +7.601800e+02 0.000000e+00 0.000000e+00 4.424000e+01 1.491770e+00 1.491770e+00 +7.641700e+02 0.000000e+00 0.000000e+00 4.340000e+01 1.141290e+00 1.141290e+00 +7.701100e+02 0.000000e+00 0.000000e+00 4.390000e+01 1.309818e+00 1.309818e+00 +7.743800e+02 0.000000e+00 0.000000e+00 4.255000e+01 1.354997e+00 1.354997e+00 +7.781700e+02 0.000000e+00 0.000000e+00 4.504000e+01 1.442044e+00 1.442044e+00 +7.801700e+02 0.000000e+00 0.000000e+00 4.317000e+01 1.367743e+00 1.367743e+00 +7.822300e+02 0.000000e+00 0.000000e+00 3.736000e+01 8.388014e-01 8.388014e-01 +7.842400e+02 0.000000e+00 0.000000e+00 3.425000e+01 9.647943e-01 9.647943e-01 +7.860400e+02 0.000000e+00 0.000000e+00 3.029000e+01 1.140069e+00 1.140069e+00 +7.901000e+02 0.000000e+00 0.000000e+00 3.112000e+01 9.264682e-01 9.264682e-01 +7.941400e+02 0.000000e+00 0.000000e+00 2.961000e+01 9.079848e-01 9.079848e-01 +8.000200e+02 0.000000e+00 0.000000e+00 2.935000e+01 8.619705e-01 8.619705e-01 +8.099800e+02 0.000000e+00 0.000000e+00 2.544000e+01 6.532696e-01 6.532696e-01 +8.101400e+02 0.000000e+00 0.000000e+00 2.555000e+01 6.709978e-01 6.709978e-01 +8.200200e+02 0.000000e+00 0.000000e+00 2.415000e+01 8.764010e-01 8.764010e-01 +8.299700e+02 0.000000e+00 0.000000e+00 2.061000e+01 8.118844e-01 8.118844e-01 +8.391000e+02 0.000000e+00 0.000000e+00 1.741000e+01 7.593397e-01 7.593397e-01 +8.492400e+02 0.000000e+00 0.000000e+00 1.428000e+01 6.033675e-01 6.033675e-01 +8.596000e+02 0.000000e+00 0.000000e+00 1.465000e+01 7.000768e-01 7.000768e-01 +8.695000e+02 0.000000e+00 0.000000e+00 1.126000e+01 5.047209e-01 5.047209e-01 +8.798400e+02 0.000000e+00 0.000000e+00 1.089000e+01 8.141067e-01 8.141067e-01 +8.897200e+02 0.000000e+00 0.000000e+00 8.660000e+00 3.794722e-01 3.794722e-01 +9.000400e+02 0.000000e+00 0.000000e+00 7.900000e+00 3.193473e-01 3.193473e-01 +9.100200e+02 0.000000e+00 0.000000e+00 6.920000e+00 3.340572e-01 3.340572e-01 +9.195600e+02 0.000000e+00 0.000000e+00 6.110000e+00 3.213530e-01 3.213530e-01 +9.301100e+02 0.000000e+00 0.000000e+00 5.870000e+00 3.788347e-01 3.788347e-01 +9.421900e+02 0.000000e+00 0.000000e+00 5.450000e+00 2.707450e-01 2.707450e-01 +9.518400e+02 0.000000e+00 0.000000e+00 4.600000e+00 2.483198e-01 2.483198e-01 +9.615200e+02 0.000000e+00 0.000000e+00 4.450000e+00 2.477944e-01 2.477944e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I502164.cc b/analyses/pluginNovosibirsk/CMD2_1999_I502164.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I502164.cc @@ -0,0 +1,88 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_1999_I502164 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_1999_I502164); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + _nK0K0 = bookCounter("TMP/K0K0"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && + nCount[130]==1 && nCount[310]==1) + _nK0K0->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _nK0K0->val(); + double error = _nK0K0->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + for(unsigned int ix=1;ix<5;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nK0K0; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_1999_I502164); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I502164.info b/analyses/pluginNovosibirsk/CMD2_1999_I502164.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I502164.info @@ -0,0 +1,37 @@ +Name: CMD2_1999_I502164 +Year: 1999 +Summary: Cross section for $e^+e^-\to K^0_SK^0_L$ at energies near the $\phi$ mass +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 502164 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B466 (1999) 385, 1999 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to K^0_SK^0_L$ at energies near the $\phi$ mass.' +Keywords: [] +BibKey: Akhmetshin:1999ym +BibTeX: '@article{Akhmetshin:1999ym, + author = "Akhmetshin, R. R. and others", + title = "{Measurement of $\phi$ meson parameters in K$^0_L$ + K$^0_S$ decay mode with CMD-2}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B466", + year = "1999", + pages = "385", + doi = "10.1016/S0370-2693(99)00973-9, + 10.1016/S0370-2693(01)00511-1", + note = "[Erratum: Phys. Lett.B508,217(2001)]", + eprint = "hep-ex/9906032", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/9906032;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I502164.plot b/analyses/pluginNovosibirsk/CMD2_1999_I502164.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I502164.plot @@ -0,0 +1,25 @@ +BEGIN PLOT /CMD2_1999_I502164/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_1999_I502164/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_1999_I502164/d03-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_1999_I502164/d04-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT + diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I502164.yoda b/analyses/pluginNovosibirsk/CMD2_1999_I502164.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I502164.yoda @@ -0,0 +1,152 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I502164/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1999_I502164/d01-x01-y01 +Title: doi:10.17182/hepdata.41645.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.010270e+03 3.000000e-02 3.000000e-02 4.221000e+01 5.209655e+00 5.209655e+00 +1.017090e+03 2.000000e-02 2.000000e-02 6.028500e+02 1.809251e+01 1.809251e+01 +1.018140e+03 2.000000e-02 2.000000e-02 9.996800e+02 3.876391e+01 3.876391e+01 +1.018960e+03 2.000000e-02 2.000000e-02 1.278750e+03 3.890920e+01 3.890920e+01 +1.019210e+03 2.000000e-02 2.000000e-02 1.328940e+03 4.489808e+01 4.489808e+01 +1.019990e+03 2.000000e-02 2.000000e-02 1.325080e+03 3.642957e+01 3.642957e+01 +1.020130e+03 2.000000e-02 2.000000e-02 1.342710e+03 4.770536e+01 4.770536e+01 +1.021850e+03 2.000000e-02 2.000000e-02 6.228200e+02 3.549590e+01 3.549590e+01 +1.023970e+03 2.000000e-02 2.000000e-02 2.922600e+02 1.571602e+01 1.571602e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I502164/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD2_1999_I502164/d01-x01-y02 +Title: doi:10.17182/hepdata.41645.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.010270e+03 3.000000e-02 3.000000e-02 4.289000e+01 5.290485e+00 5.290485e+00 +1.017090e+03 2.000000e-02 2.000000e-02 6.583100e+02 1.975558e+01 1.975558e+01 +1.018140e+03 2.000000e-02 2.000000e-02 1.069660e+03 4.147848e+01 4.147848e+01 +1.018960e+03 2.000000e-02 2.000000e-02 1.277470e+03 3.887217e+01 3.887217e+01 +1.019210e+03 2.000000e-02 2.000000e-02 1.291730e+03 4.363783e+01 4.363783e+01 +1.019990e+03 2.000000e-02 2.000000e-02 1.189920e+03 3.271394e+01 3.271394e+01 +1.020130e+03 2.000000e-02 2.000000e-02 1.193670e+03 4.240989e+01 4.240989e+01 +1.021850e+03 2.000000e-02 2.000000e-02 5.368700e+02 3.059311e+01 3.059311e+01 +1.023970e+03 2.000000e-02 2.000000e-02 2.580700e+02 1.388151e+01 1.388151e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I502164/d02-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1999_I502164/d02-x01-y01 +Title: doi:10.17182/hepdata.41645.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004250e+03 1.700000e-01 1.700000e-01 1.851000e+01 9.855025e+00 9.855025e+00 +1.010860e+03 1.300000e-01 1.300000e-01 5.296000e+01 7.583632e+00 7.583632e+00 +1.016370e+03 8.000000e-02 8.000000e-02 3.995400e+02 3.592787e+01 3.592787e+01 +1.017190e+03 8.000000e-02 8.000000e-02 6.002200e+02 4.690335e+01 4.690335e+01 +1.018060e+03 8.000000e-02 8.000000e-02 9.306600e+02 5.373205e+01 5.373205e+01 +1.019000e+03 8.000000e-02 8.000000e-02 1.329000e+03 3.375574e+01 3.375574e+01 +1.020000e+03 8.000000e-02 8.000000e-02 1.282510e+03 5.484030e+01 5.484030e+01 +1.020960e+03 8.000000e-02 8.000000e-02 9.413800e+02 4.964042e+01 4.964042e+01 +1.021880e+03 9.000000e-02 9.000000e-02 6.207000e+02 4.164885e+01 4.164885e+01 +1.027700e+03 1.100000e-01 1.100000e-01 1.267400e+02 1.057188e+01 1.057188e+01 +1.033630e+03 1.700000e-01 1.700000e-01 6.633000e+01 8.643865e+00 8.643865e+00 +1.039480e+03 1.700000e-01 1.700000e-01 3.792000e+01 6.263263e+00 6.263263e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I502164/d02-x01-y02 +IsRef: 1 +Path: /REF/CMD2_1999_I502164/d02-x01-y02 +Title: doi:10.17182/hepdata.41645.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004250e+03 1.700000e-01 1.700000e-01 1.840000e+01 9.794996e+00 9.794996e+00 +1.010860e+03 1.300000e-01 1.300000e-01 5.397000e+01 7.724680e+00 7.724680e+00 +1.016370e+03 8.000000e-02 8.000000e-02 4.335000e+02 3.898292e+01 3.898292e+01 +1.017190e+03 8.000000e-02 8.000000e-02 6.554400e+02 5.121674e+01 5.121674e+01 +1.018060e+03 8.000000e-02 8.000000e-02 9.995300e+02 5.770833e+01 5.770833e+01 +1.019000e+03 8.000000e-02 8.000000e-02 1.322360e+03 3.358360e+01 3.358360e+01 +1.020000e+03 8.000000e-02 8.000000e-02 1.150410e+03 4.919446e+01 4.919446e+01 +1.020960e+03 8.000000e-02 8.000000e-02 8.114700e+02 4.279441e+01 4.279441e+01 +1.021880e+03 9.000000e-02 9.000000e-02 5.350400e+02 3.590131e+01 3.590131e+01 +1.027700e+03 1.100000e-01 1.100000e-01 1.154600e+02 9.632111e+00 9.632111e+00 +1.033630e+03 1.700000e-01 1.700000e-01 6.169000e+01 8.038702e+00 8.038702e+00 +1.039480e+03 1.700000e-01 1.700000e-01 3.561000e+01 5.881239e+00 5.881239e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I502164/d03-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1999_I502164/d03-x01-y01 +Title: doi:10.17182/hepdata.41645.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004640e+03 1.700000e-01 1.700000e-01 1.358000e+01 4.595802e+00 4.595802e+00 +1.011300e+03 9.000000e-02 9.000000e-02 5.297000e+01 3.594619e+00 3.594619e+00 +1.015990e+03 8.000000e-02 8.000000e-02 3.507900e+02 2.893127e+01 2.893127e+01 +1.016930e+03 8.000000e-02 8.000000e-02 5.605800e+02 4.389693e+01 4.389693e+01 +1.017910e+03 8.000000e-02 8.000000e-02 9.316100e+02 5.171475e+01 5.171475e+01 +1.019040e+03 7.000000e-02 7.000000e-02 1.354290e+03 3.414088e+01 3.414088e+01 +1.019950e+03 7.000000e-02 7.000000e-02 1.251840e+03 5.403704e+01 5.403704e+01 +1.020860e+03 8.000000e-02 8.000000e-02 8.914800e+02 4.799553e+01 4.799553e+01 +1.021740e+03 8.000000e-02 8.000000e-02 6.069600e+02 3.842145e+01 3.842145e+01 +1.022670e+03 9.000000e-02 9.000000e-02 4.193100e+02 3.172129e+01 3.172129e+01 +1.028360e+03 1.200000e-01 1.200000e-01 1.023800e+02 9.904125e+00 9.904125e+00 +1.034060e+03 1.700000e-01 1.700000e-01 5.404000e+01 7.834052e+00 7.834052e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I502164/d03-x01-y02 +IsRef: 1 +Path: /REF/CMD2_1999_I502164/d03-x01-y02 +Title: doi:10.17182/hepdata.41645.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004640e+03 1.700000e-01 1.700000e-01 1.351000e+01 4.575768e+00 4.575768e+00 +1.011300e+03 9.000000e-02 9.000000e-02 5.414000e+01 3.677050e+00 3.677050e+00 +1.015990e+03 8.000000e-02 8.000000e-02 3.785000e+02 3.122027e+01 3.122027e+01 +1.016930e+03 8.000000e-02 8.000000e-02 6.115900e+02 4.789218e+01 4.789218e+01 +1.017910e+03 8.000000e-02 8.000000e-02 1.006140e+03 5.585346e+01 5.585346e+01 +1.019040e+03 7.000000e-02 7.000000e-02 1.342100e+03 3.383130e+01 3.383130e+01 +1.019950e+03 7.000000e-02 7.000000e-02 1.127910e+03 4.868493e+01 4.868493e+01 +1.020860e+03 8.000000e-02 8.000000e-02 7.702400e+02 4.147140e+01 4.147140e+01 +1.021740e+03 8.000000e-02 8.000000e-02 5.225900e+02 3.308509e+01 3.308509e+01 +1.022670e+03 9.000000e-02 9.000000e-02 3.643800e+02 2.756503e+01 2.756503e+01 +1.028360e+03 1.200000e-01 1.200000e-01 9.358000e+01 9.050908e+00 9.050908e+00 +1.034060e+03 1.700000e-01 1.700000e-01 5.031000e+01 7.290342e+00 7.290342e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I502164/d04-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1999_I502164/d04-x01-y01 +Title: doi:10.17182/hepdata.41645.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004190e+03 1.700000e-01 1.700000e-01 1.239000e+01 1.782488e+00 1.782488e+00 +1.011300e+03 1.000000e-01 1.000000e-01 5.662000e+01 6.937102e+00 6.937102e+00 +1.015910e+03 8.000000e-02 8.000000e-02 3.439500e+02 2.725461e+01 2.725461e+01 +1.016940e+03 8.000000e-02 8.000000e-02 6.016500e+02 4.677203e+01 4.677203e+01 +1.017920e+03 8.000000e-02 8.000000e-02 9.985000e+02 5.411135e+01 5.411135e+01 +1.018760e+03 8.000000e-02 8.000000e-02 1.317090e+03 3.224965e+01 3.224965e+01 +1.019680e+03 7.000000e-02 7.000000e-02 1.321090e+03 5.066914e+01 5.066914e+01 +1.020680e+03 8.000000e-02 8.000000e-02 9.993000e+02 5.228669e+01 5.228669e+01 +1.021600e+03 8.000000e-02 8.000000e-02 6.485400e+02 3.782257e+01 3.782257e+01 +1.022590e+03 8.000000e-02 8.000000e-02 4.280500e+02 2.830150e+01 2.830150e+01 +1.028410e+03 1.000000e-01 1.000000e-01 1.025700e+02 8.598654e+00 8.598654e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I502164/d04-x01-y02 +IsRef: 1 +Path: /REF/CMD2_1999_I502164/d04-x01-y02 +Title: doi:10.17182/hepdata.41645.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004190e+03 1.700000e-01 1.700000e-01 1.232000e+01 1.772418e+00 1.772418e+00 +1.011300e+03 1.000000e-01 1.000000e-01 5.787000e+01 7.088599e+00 7.088599e+00 +1.015910e+03 8.000000e-02 8.000000e-02 3.707800e+02 2.938403e+01 2.938403e+01 +1.016940e+03 8.000000e-02 8.000000e-02 6.564000e+02 5.102512e+01 5.102512e+01 +1.017920e+03 8.000000e-02 8.000000e-02 1.078380e+03 5.843988e+01 5.843988e+01 +1.018760e+03 8.000000e-02 8.000000e-02 1.344750e+03 3.292877e+01 3.292877e+01 +1.019680e+03 7.000000e-02 7.000000e-02 1.219370e+03 4.676526e+01 4.676526e+01 +1.020680e+03 8.000000e-02 8.000000e-02 8.663900e+02 4.532956e+01 4.532956e+01 +1.021600e+03 8.000000e-02 8.000000e-02 5.583900e+02 3.256428e+01 3.256428e+01 +1.022590e+03 8.000000e-02 8.000000e-02 3.719800e+02 2.459678e+01 2.459678e+01 +1.028410e+03 1.000000e-01 1.000000e-01 9.375000e+01 7.863208e+00 7.863208e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I503154.cc b/analyses/pluginNovosibirsk/CMD2_1999_I503154.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I503154.cc @@ -0,0 +1,123 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_1999_I503154 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_1999_I503154); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaGamma = bookCounter("TMP/EtaGamma"); + } + + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(val.first==22) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaGamma->fill(event.weight()); + } + } + + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _numEtaGamma->val(); + double error = _numEtaGamma->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numEtaGamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_1999_I503154); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I503154.info b/analyses/pluginNovosibirsk/CMD2_1999_I503154.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I503154.info @@ -0,0 +1,32 @@ +Name: CMD2_1999_I503154 +Year: 1999 +Summary: Cross section for $e^+e^-\to\eta\gamma$ for energies near the $\phi$ mass +Collider: VEPP-2M +InspireID: 503154 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B460 (1999) 242-247, 1999 +RunInfo: e+ e- to hadrons below 0.6 and 1.38 GeV +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\eta\gamma$ for energies near the $\phi$ mass.' +Keywords: +BibKey: Akhmetshin:1999zv +BibTeX: '@article{Akhmetshin:1999zv, + author = "Akhmetshin, R. R. and others", + title = "{Study of the radiative decay phi ---> eta gamma with + CMD-2 detector}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B460", + year = "1999", + pages = "242-247", + doi = "10.1016/S0370-2693(99)00748-0", + eprint = "hep-ex/9907003", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/9907003;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I503154.plot b/analyses/pluginNovosibirsk/CMD2_1999_I503154.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I503154.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /CMD2_1999_I503154/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\gamma)$/nb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_1999_I503154.yoda b/analyses/pluginNovosibirsk/CMD2_1999_I503154.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_1999_I503154.yoda @@ -0,0 +1,26 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_1999_I503154/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_1999_I503154/d01-x01-y01 +Title: doi:10.17182/hepdata.27081.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.858000e+02 2.000000e-01 2.000000e-01 8.000000e-01 9.008188e-01 9.008188e-01 +1.004800e+03 2.000000e-01 2.000000e-01 1.800000e+00 1.003726e+00 1.003726e+00 +1.011440e+03 2.000000e-01 2.000000e-01 2.500000e+00 1.007174e+00 1.007174e+00 +1.016140e+03 2.000000e-01 2.000000e-01 2.170000e+01 2.524862e+00 2.524862e+00 +1.017080e+03 6.000000e-02 6.000000e-02 2.630000e+01 2.365091e+00 2.365091e+00 +1.018040e+03 6.000000e-02 6.000000e-02 3.740000e+01 2.839497e+00 2.839497e+00 +1.018880e+03 4.000000e-02 4.000000e-02 4.840000e+01 4.625717e+00 4.625717e+00 +1.019040e+03 4.000000e-02 4.000000e-02 4.850000e+01 5.155539e+00 5.155539e+00 +1.019200e+03 4.000000e-02 4.000000e-02 5.500000e+01 4.627051e+00 4.627051e+00 +1.019840e+03 4.000000e-02 4.000000e-02 4.920000e+01 4.474053e+00 4.474053e+00 +1.020080e+03 4.000000e-02 4.000000e-02 4.490000e+01 3.377112e+00 3.377112e+00 +1.020720e+03 4.000000e-02 4.000000e-02 3.060000e+01 4.733643e+00 4.733643e+00 +1.020980e+03 6.000000e-02 6.000000e-02 3.050000e+01 2.726407e+00 2.726407e+00 +1.021800e+03 6.000000e-02 6.000000e-02 1.680000e+01 2.064045e+00 2.064045e+00 +1.022720e+03 6.000000e-02 6.000000e-02 1.330000e+01 2.099418e+00 2.099418e+00 +1.028260e+03 1.000000e-01 1.000000e-01 1.500000e+00 6.043046e-01 6.043046e-01 +1.033700e+03 1.800000e-01 1.800000e-01 1.000000e+00 1.101047e+00 1.101047e+00 +1.038960e+03 1.200000e-01 1.200000e-01 2.100000e+00 2.901751e+00 2.901751e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I511375.cc b/analyses/pluginNovosibirsk/CMD2_2000_I511375.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I511375.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2000_I511375 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2000_I511375); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=4) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2000_I511375); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I511375.info b/analyses/pluginNovosibirsk/CMD2_2000_I511375.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I511375.info @@ -0,0 +1,34 @@ +Name: CMD2_2000_I511375 +Year: 2000 +Summary: Cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ below 1 GeV +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 511375 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B475 (2000) 190-197, 2000 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ below 1 GeV' +Keywords: +BibKey: Akhmetshin:1999ty +BibTeX: '@article{Akhmetshin:1999ty, + author = "Akhmetshin, R. R. and others", + title = "{Cross-section of the reaction e+ e- ---> pi+ pi- pi+ pi- + below 1-GeV at CMD-2}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B475", + year = "2000", + pages = "190-197", + doi = "10.1016/S0370-2693(00)00043-5", + eprint = "hep-ex/9912020", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/9912020;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I511375.plot b/analyses/pluginNovosibirsk/CMD2_2000_I511375.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I511375.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /CMD2_2000_I511375/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I511375.yoda b/analyses/pluginNovosibirsk/CMD2_2000_I511375.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I511375.yoda @@ -0,0 +1,19 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2000_I511375/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2000_I511375/d01-x01-y01 +Title: doi:10.17182/hepdata.27052.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.650000e-01 1.500000e-02 1.500000e-02 3.600000e-02 2.600000e-02 2.600000e-02 +7.905000e-01 9.500000e-03 9.500000e-03 1.500000e-02 1.100000e-02 1.100000e-02 +8.100000e-01 0.000000e+00 0.000000e+00 1.500000e-01 1.100000e-01 1.100000e-01 +8.200000e-01 0.000000e+00 0.000000e+00 1.400000e-01 8.000000e-02 8.000000e-02 +8.400000e-01 0.000000e+00 0.000000e+00 1.400000e-01 7.000000e-02 7.000000e-02 +8.800000e-01 0.000000e+00 0.000000e+00 2.300000e-01 8.000000e-02 8.000000e-02 +9.200000e-01 0.000000e+00 0.000000e+00 3.700000e-01 7.000000e-02 7.000000e-02 +9.400000e-01 0.000000e+00 0.000000e+00 3.000000e-01 9.000000e-02 9.000000e-02 +9.500000e-01 0.000000e+00 0.000000e+00 3.100000e-01 7.000000e-02 7.000000e-02 +9.580000e-01 0.000000e+00 0.000000e+00 5.300000e-01 9.000000e-02 9.000000e-02 +9.700000e-01 0.000000e+00 0.000000e+00 7.000000e-01 1.100000e-01 1.100000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I523691.cc b/analyses/pluginNovosibirsk/CMD2_2000_I523691.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I523691.cc @@ -0,0 +1,85 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2000_I523691 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2000_I523691); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + _num3pi = bookCounter("TMP/num3"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=3) vetoEvent; + if(nCount[-211]==1&&nCount[211]==1&&nCount[111]==1) + _num3pi->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _num3pi->val(); + double error = _num3pi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _num3pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2000_I523691); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I523691.info b/analyses/pluginNovosibirsk/CMD2_2000_I523691.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I523691.info @@ -0,0 +1,33 @@ +Name: CMD2_2000_I523691 +Year: 2000 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ near the $\omega$ mass +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 523691 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B434 (1998) 426-436, 1998 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ for energies near the $\omega$ mass.' +Keywords: +BibKey: Akhmetshin:2000ca +BibTeX: '@article{Akhmetshin:2000ca, + author = "Akhmetshin, R. R. and others", + title = "{Measurement of omega meson parameters in pi+ pi- pi0 + decay mode with CMD-2}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B476", + year = "2000", + pages = "33-39", + doi = "10.1016/S0370-2693(00)00123-4", + eprint = "hep-ex/0002017", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0002017;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I523691.plot b/analyses/pluginNovosibirsk/CMD2_2000_I523691.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I523691.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /CMD2_2000_I523691/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +LegendXPos=0.1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I523691.yoda b/analyses/pluginNovosibirsk/CMD2_2000_I523691.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I523691.yoda @@ -0,0 +1,42 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2000_I523691/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2000_I523691/d01-x01-y01 +Title: doi:10.17182/hepdata.27036.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.601800e+02 0.000000e+00 0.000000e+00 6.900000e+01 1.103651e+01 1.103651e+01 +7.641700e+02 0.000000e+00 0.000000e+00 7.100000e+01 8.053070e+00 8.053070e+00 +7.701100e+02 0.000000e+00 0.000000e+00 1.790000e+02 1.517942e+01 1.517942e+01 +7.743800e+02 0.000000e+00 0.000000e+00 2.790000e+02 2.229698e+01 2.229698e+01 +7.781700e+02 0.000000e+00 0.000000e+00 7.900000e+02 4.226669e+01 4.226669e+01 +7.801700e+02 0.000000e+00 0.000000e+00 1.193000e+03 5.330599e+01 5.330599e+01 +7.822300e+02 0.000000e+00 0.000000e+00 1.490000e+03 3.655403e+01 3.655403e+01 +7.842400e+02 0.000000e+00 0.000000e+00 1.338000e+03 4.824470e+01 4.824470e+01 +7.860400e+02 0.000000e+00 0.000000e+00 9.030000e+02 4.553904e+01 4.553904e+01 +7.900900e+02 0.000000e+00 0.000000e+00 4.170000e+02 1.975822e+01 1.975822e+01 +7.941400e+02 0.000000e+00 0.000000e+00 1.970000e+02 1.129419e+01 1.129419e+01 +8.000000e+02 0.000000e+00 0.000000e+00 1.270000e+02 8.168586e+00 8.168586e+00 +8.101400e+02 0.000000e+00 0.000000e+00 5.600000e+01 4.065708e+00 4.065708e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2000_I523691/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD2_2000_I523691/d01-x01-y02 +Title: doi:10.17182/hepdata.27036.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.601800e+02 0.000000e+00 0.000000e+00 6.800000e+01 1.083612e+01 1.083612e+01 +7.641700e+02 0.000000e+00 0.000000e+00 7.000000e+01 7.952239e+00 7.952239e+00 +7.701100e+02 0.000000e+00 0.000000e+00 1.766000e+02 1.497701e+01 1.497701e+01 +7.743800e+02 0.000000e+00 0.000000e+00 2.759000e+02 2.209309e+01 2.209309e+01 +7.781700e+02 0.000000e+00 0.000000e+00 7.818000e+02 4.185277e+01 4.185277e+01 +7.801700e+02 0.000000e+00 0.000000e+00 1.149100e+03 5.266311e+01 5.266311e+01 +7.822300e+02 0.000000e+00 0.000000e+00 1.427800e+03 3.502307e+01 3.502307e+01 +7.842400e+02 0.000000e+00 0.000000e+00 1.254800e+03 4.524306e+01 4.524306e+01 +7.860400e+02 0.000000e+00 0.000000e+00 8.428000e+02 4.253531e+01 4.253531e+01 +7.900900e+02 0.000000e+00 0.000000e+00 3.914000e+02 1.851296e+01 1.851296e+01 +7.941400e+02 0.000000e+00 0.000000e+00 1.859000e+02 1.067710e+01 1.067710e+01 +8.000000e+02 0.000000e+00 0.000000e+00 1.203000e+02 7.759239e+00 7.759239e+00 +8.101400e+02 0.000000e+00 0.000000e+00 5.320000e+01 3.862423e+00 3.862423e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I531667.cc b/analyses/pluginNovosibirsk/CMD2_2000_I531667.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I531667.cc @@ -0,0 +1,80 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2000_I531667 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2000_I531667); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=4) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2000_I531667); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I531667.info b/analyses/pluginNovosibirsk/CMD2_2000_I531667.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I531667.info @@ -0,0 +1,33 @@ +Name: CMD2_2000_I531667 +Year: 2000 +Summary: Cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ hear the $\phi$ mass +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 531667 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B491 (2000) 81-89, 2000 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ hear the $\phi$ mass.' +Keywords: +BibKey: Akhmetshin:2000it +BibTeX: '@article{Akhmetshin:2000it, + author = "Akhmetshin, R. R. and others", + title = "{Observation of the phi ---> pi+ pi- pi+ pi- decay}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B491", + year = "2000", + pages = "81-89", + doi = "10.1016/S0370-2693(00)01001-7", + eprint = "hep-ex/0008019", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0008019;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I531667.plot b/analyses/pluginNovosibirsk/CMD2_2000_I531667.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I531667.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /CMD2_2000_I531667/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I531667.yoda b/analyses/pluginNovosibirsk/CMD2_2000_I531667.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I531667.yoda @@ -0,0 +1,24 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2000_I531667/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2000_I531667/d01-x01-y01 +Title: doi:10.17182/hepdata.41735.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.840000e-01 0.000000e+00 0.000000e+00 6.800000e-01 1.182141e-01 1.182141e-01 +1.004000e+00 0.000000e+00 0.000000e+00 9.000000e-01 1.461801e-01 1.461801e-01 +1.010300e+00 0.000000e+00 0.000000e+00 9.800000e-01 1.543772e-01 1.543772e-01 +1.015700e+00 0.000000e+00 0.000000e+00 9.200000e-01 1.482055e-01 1.482055e-01 +1.016800e+00 0.000000e+00 0.000000e+00 9.400000e-01 1.344405e-01 1.344405e-01 +1.017800e+00 0.000000e+00 0.000000e+00 1.010000e+00 1.386011e-01 1.386011e-01 +1.018700e+00 0.000000e+00 0.000000e+00 9.600000e-01 1.326527e-01 1.326527e-01 +1.019700e+00 0.000000e+00 0.000000e+00 1.260000e+00 1.720653e-01 1.720653e-01 +1.020600e+00 0.000000e+00 0.000000e+00 1.270000e+00 1.811654e-01 1.811654e-01 +1.021500e+00 0.000000e+00 0.000000e+00 1.170000e+00 1.800665e-01 1.800665e-01 +1.022700e+00 0.000000e+00 0.000000e+00 1.250000e+00 1.835628e-01 1.835628e-01 +1.027800e+00 0.000000e+00 0.000000e+00 1.290000e+00 1.930275e-01 1.930275e-01 +1.034000e+00 0.000000e+00 0.000000e+00 1.450000e+00 2.157338e-01 2.157338e-01 +1.040000e+00 0.000000e+00 0.000000e+00 1.530000e+00 2.246025e-01 2.246025e-01 +1.050000e+00 0.000000e+00 0.000000e+00 1.640000e+00 2.523060e-01 2.523060e-01 +1.060000e+00 0.000000e+00 0.000000e+00 1.920000e+00 2.828196e-01 2.828196e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I532970.cc b/analyses/pluginNovosibirsk/CMD2_2000_I532970.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I532970.cc @@ -0,0 +1,165 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2000_I532970 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2000_I532970); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numOmegaPiPi = bookCounter("TMP/OmegaPiPi"); + _numEtaPiPi = bookCounter("TMP/EtaPiPi"); + _num5Pi = bookCounter("TMP/5Pi"); + + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + bool foundRes = false; + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the eta + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _numEtaPiPi->fill(event.weight()); + foundRes = true; + } + } + // find the eta + else if(p.pdgId()==223) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _numOmegaPiPi->fill(event.weight()); + foundRes = true; + } + } + } + + if(foundRes) vetoEvent; + if(nCount[-211]==2&&nCount[211]==2&&nCount[111]==1) + _num5Pi->fill(event.weight()); + } + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<4;++ix) { + double sigma,error; + if(ix==1) { + sigma = _numOmegaPiPi->val(); + error = _numOmegaPiPi->err(); + } + else if(ix==2) { + sigma = _numEtaPiPi->val(); + error = _numEtaPiPi->err(); + } + else { + sigma = _num5Pi->val(); + error = _num5Pi->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + /// @name Histograms + //@{ + CounterPtr _numEtaPiPi,_numOmegaPiPi,_num5Pi; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2000_I532970); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I532970.info b/analyses/pluginNovosibirsk/CMD2_2000_I532970.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I532970.info @@ -0,0 +1,34 @@ +Name: CMD2_2000_I532970 +Year: 2000 +Summary: Cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+\pi^0$ between 1.28 and 1.38 GeV +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 532970 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B489 (2000) 125-130, 2000 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+\pi^0$ between 1.28 and 1.38 GeV.' +Keywords: +BibKey: Akhmetshin:2000wv +BibTeX: '@article{Akhmetshin:2000wv, + author = "Akhmetshin, R. R. and others", + title = "{Study of the process e+ e- ---> pi+ pi- pi+ pi- pi0 with + CMD-2 detector}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B489", + year = "2000", + pages = "125-130", + doi = "10.1016/S0370-2693(00)00937-0", + eprint = "hep-ex/0009013", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0009013;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I532970.plot b/analyses/pluginNovosibirsk/CMD2_2000_I532970.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I532970.plot @@ -0,0 +1,24 @@ +BEGIN PLOT /CMD2_2000_I532970/d01-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega\pi^+\pi^-)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_2000_I532970/d02-x01-y01 +Title=$\sigma(e^+e^-\to \eta \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_2000_I532970/d03-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-\pi^0)$ non-resonant +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-\pi^0)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginNovosibirsk/CMD2_2000_I532970.yoda b/analyses/pluginNovosibirsk/CMD2_2000_I532970.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2000_I532970.yoda @@ -0,0 +1,36 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2000_I532970/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2000_I532970/d01-x01-y01 +Title: doi:10.17182/hepdata.28019.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.285000e+00 0.000000e+00 0.000000e+00 7.000000e-02 5.000000e-02 5.000000e-02 +1.305000e+00 0.000000e+00 0.000000e+00 2.000000e-01 6.000000e-02 6.000000e-02 +1.325000e+00 0.000000e+00 0.000000e+00 2.100000e-01 6.000000e-02 6.000000e-02 +1.345000e+00 0.000000e+00 0.000000e+00 3.200000e-01 8.000000e-02 8.000000e-02 +1.365000e+00 0.000000e+00 0.000000e+00 4.000000e-01 8.000000e-02 8.000000e-02 +1.380000e+00 0.000000e+00 0.000000e+00 5.300000e-01 9.000000e-02 9.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2000_I532970/d02-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2000_I532970/d02-x01-y01 +Title: doi:10.17182/hepdata.28019.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.285000e+00 0.000000e+00 0.000000e+00 1.100000e-01 1.300000e-01 1.300000e-01 +1.305000e+00 0.000000e+00 0.000000e+00 4.200000e-01 1.300000e-01 1.300000e-01 +1.325000e+00 0.000000e+00 0.000000e+00 5.400000e-01 1.300000e-01 1.300000e-01 +1.345000e+00 0.000000e+00 0.000000e+00 8.400000e-01 1.300000e-01 1.300000e-01 +1.365000e+00 0.000000e+00 0.000000e+00 8.800000e-01 1.300000e-01 1.300000e-01 +1.380000e+00 0.000000e+00 0.000000e+00 1.810000e+00 1.300000e-01 1.300000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2000_I532970/d03-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2000_I532970/d03-x01-y01 +Title: doi:10.17182/hepdata.28019.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2001_I554522.cc b/analyses/pluginNovosibirsk/CMD2_2001_I554522.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2001_I554522.cc @@ -0,0 +1,123 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2001_I554522 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2001_I554522); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaGamma = bookCounter("TMP/EtaGamma"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(val.first==22) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaGamma->fill(event.weight()); + } + } + + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _numEtaGamma->val(); + double error = _numEtaGamma->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numEtaGamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2001_I554522); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2001_I554522.info b/analyses/pluginNovosibirsk/CMD2_2001_I554522.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2001_I554522.info @@ -0,0 +1,33 @@ +Name: CMD2_2001_I554522 +Year: 2001 +Summary: Cross section for $e^+e^-\to\eta\gamma$ for energies between 600 MeV and 1380 MeV +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 554522 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B509 (2001) 217-226, 2001 +RunInfo: e+ e- to hadrons below 0.6 and 1.38 GeV +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\eta\gamma$ for energies between 600 MeV and 1380 MeV' +Keywords: +BibKey: Akhmetshin:2001hm +BibTeX: '@article{Akhmetshin:2001hm, + author = "Akhmetshin, R. R. and others", + title = "{Study of the process e+ e- ---> eta gamma in + center-of-mass energy range 600-MeV to 1380-MeV at CMD-2}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B509", + year = "2001", + pages = "217-226", + doi = "10.1016/S0370-2693(01)00567-6", + eprint = "hep-ex/0103043", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0103043;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2001_I554522.plot b/analyses/pluginNovosibirsk/CMD2_2001_I554522.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2001_I554522.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /CMD2_2001_I554522/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\gamma)$/nb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2001_I554522.yoda b/analyses/pluginNovosibirsk/CMD2_2001_I554522.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2001_I554522.yoda @@ -0,0 +1,53 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2001_I554522/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2001_I554522/d01-x01-y01 +Title: doi:10.17182/hepdata.27025.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.900000e+02 0.000000e+00 0.000000e+00 8.000000e-02 6.000000e-02 1.000000e-01 +7.200000e+02 0.000000e+00 0.000000e+00 3.200000e-01 1.100000e-01 1.100000e-01 +7.500000e+02 0.000000e+00 0.000000e+00 4.700000e-01 1.800000e-01 1.800000e-01 +7.600000e+02 0.000000e+00 0.000000e+00 3.400000e-01 1.500000e-01 1.500000e-01 +7.640000e+02 0.000000e+00 0.000000e+00 3.500000e-01 2.500000e-01 4.600000e-01 +7.700000e+02 0.000000e+00 0.000000e+00 2.600000e-01 1.400000e-01 2.300000e-01 +7.740000e+02 0.000000e+00 0.000000e+00 1.020000e+00 2.700000e-01 2.700000e-01 +7.780000e+02 0.000000e+00 0.000000e+00 1.640000e+00 3.500000e-01 3.500000e-01 +7.800000e+02 0.000000e+00 0.000000e+00 1.790000e+00 3.700000e-01 3.700000e-01 +7.810000e+02 0.000000e+00 0.000000e+00 1.840000e+00 3.300000e-01 3.300000e-01 +7.820000e+02 0.000000e+00 0.000000e+00 2.450000e+00 2.400000e-01 2.400000e-01 +7.830000e+02 0.000000e+00 0.000000e+00 2.560000e+00 3.700000e-01 3.700000e-01 +7.840000e+02 0.000000e+00 0.000000e+00 2.280000e+00 3.100000e-01 3.100000e-01 +7.850000e+02 0.000000e+00 0.000000e+00 1.660000e+00 3.400000e-01 3.400000e-01 +7.860000e+02 0.000000e+00 0.000000e+00 2.310000e+00 4.000000e-01 4.000000e-01 +7.900000e+02 0.000000e+00 0.000000e+00 8.200000e-01 2.600000e-01 2.600000e-01 +7.940000e+02 0.000000e+00 0.000000e+00 9.200000e-01 2.500000e-01 2.500000e-01 +8.000000e+02 0.000000e+00 0.000000e+00 5.700000e-01 1.600000e-01 1.600000e-01 +8.100000e+02 0.000000e+00 0.000000e+00 4.600000e-01 1.500000e-01 1.500000e-01 +8.200000e+02 0.000000e+00 0.000000e+00 3.000000e-01 1.100000e-01 1.100000e-01 +8.400000e+02 0.000000e+00 0.000000e+00 4.700000e-01 9.000000e-02 9.000000e-02 +8.800000e+02 0.000000e+00 0.000000e+00 3.700000e-01 1.000000e-01 1.000000e-01 +9.200000e+02 0.000000e+00 0.000000e+00 2.300000e-01 7.000000e-02 7.000000e-02 +9.400000e+02 0.000000e+00 0.000000e+00 2.600000e-01 9.000000e-02 9.000000e-02 +9.500000e+02 0.000000e+00 0.000000e+00 1.400000e-01 8.000000e-02 8.000000e-02 +9.580000e+02 0.000000e+00 0.000000e+00 3.000000e-01 1.100000e-01 1.100000e-01 +9.700000e+02 0.000000e+00 0.000000e+00 2.300000e-01 2.000000e-01 2.000000e-01 +9.840000e+02 0.000000e+00 0.000000e+00 5.000000e-01 1.700000e-01 1.700000e-01 +1.004000e+03 0.000000e+00 0.000000e+00 1.700000e+00 2.800000e-01 2.800000e-01 +1.010300e+03 0.000000e+00 0.000000e+00 3.320000e+00 3.500000e-01 3.500000e-01 +1.015700e+03 0.000000e+00 0.000000e+00 1.597000e+01 8.800000e-01 8.800000e-01 +1.016780e+03 0.000000e+00 0.000000e+00 2.564000e+01 8.000000e-01 8.000000e-01 +1.017820e+03 0.000000e+00 0.000000e+00 3.671000e+01 9.000000e-01 9.000000e-01 +1.018680e+03 0.000000e+00 0.000000e+00 5.214000e+01 9.300000e-01 9.300000e-01 +1.019690e+03 0.000000e+00 0.000000e+00 5.010000e+01 9.600000e-01 9.600000e-01 +1.020580e+03 0.000000e+00 0.000000e+00 3.645000e+01 1.020000e+00 1.020000e+00 +1.021510e+03 0.000000e+00 0.000000e+00 2.149000e+01 9.700000e-01 9.700000e-01 +1.022740e+03 0.000000e+00 0.000000e+00 1.209000e+01 7.200000e-01 7.200000e-01 +1.027800e+03 0.000000e+00 0.000000e+00 2.450000e+00 3.900000e-01 3.900000e-01 +1.033700e+03 0.000000e+00 0.000000e+00 7.500000e-01 2.800000e-01 2.800000e-01 +1.039600e+03 0.000000e+00 0.000000e+00 3.100000e-01 2.200000e-01 2.200000e-01 +1.049700e+03 0.000000e+00 0.000000e+00 1.200000e-01 1.200000e-01 2.100000e-01 +1.060000e+03 0.000000e+00 0.000000e+00 4.000000e-02 4.000000e-02 1.700000e-01 +1.100000e+03 0.000000e+00 0.000000e+00 1.000000e-02 1.000000e-02 8.000000e-02 +1.354000e+03 0.000000e+00 0.000000e+00 5.000000e-02 3.000000e-02 4.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2002_I568807.cc b/analyses/pluginNovosibirsk/CMD2_2002_I568807.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2002_I568807.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2002_I568807 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2002_I568807); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 2)); + Scatter2DPtr mult = bookScatter2D(1, 1, 2); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2002_I568807); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2002_I568807.info b/analyses/pluginNovosibirsk/CMD2_2002_I568807.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2002_I568807.info @@ -0,0 +1,33 @@ +Name: CMD2_2002_I568807 +Year: 2002 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ at near the $\rho$ mass. +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 568807 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B527 (2002) 161-172, 2002 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies near the $\rho$ mass.' +Keywords: [] +BibKey: Akhmetshin:2001ig +BibTeX: '@article{Akhmetshin:2001ig, + author = "Akhmetshin, R. R. and others", + title = "{Measurement of e+ e- ---> pi+ pi- cross-section with + CMD-2 around rho meson}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B527", + year = "2002", + pages = "161-172", + doi = "10.1016/S0370-2693(02)01168-1", + eprint = "hep-ex/0112031", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0112031;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2002_I568807.plot b/analyses/pluginNovosibirsk/CMD2_2002_I568807.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2002_I568807.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /CMD2_2002_I568807/d01-x01-y02 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2002_I568807.yoda b/analyses/pluginNovosibirsk/CMD2_2002_I568807.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2002_I568807.yoda @@ -0,0 +1,102 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2002_I568807/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2002_I568807/d01-x01-y01 +Title: doi:10.17182/hepdata.27037.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.105000e+02 0.000000e+00 0.000000e+00 8.180000e+00 1.151047e+00 1.151047e+00 +6.205000e+02 0.000000e+00 0.000000e+00 9.950000e+00 7.424043e-01 7.424043e-01 +6.305000e+02 0.000000e+00 0.000000e+00 1.112000e+01 7.430017e-01 7.430017e-01 +6.405100e+02 0.000000e+00 0.000000e+00 1.130000e+01 7.331418e-01 7.331418e-01 +6.504900e+02 0.000000e+00 0.000000e+00 1.302000e+01 8.535823e-01 8.535823e-01 +6.605000e+02 0.000000e+00 0.000000e+00 1.377000e+01 7.744198e-01 7.744198e-01 +6.705000e+02 0.000000e+00 0.000000e+00 1.579000e+01 8.453258e-01 8.453258e-01 +6.805900e+02 0.000000e+00 0.000000e+00 2.002000e+01 9.377253e-01 9.377253e-01 +6.904300e+02 0.000000e+00 0.000000e+00 2.103000e+01 7.506806e-01 7.506806e-01 +7.005200e+02 0.000000e+00 0.000000e+00 2.446000e+01 6.566114e-01 6.566114e-01 +7.104700e+02 0.000000e+00 0.000000e+00 2.837000e+01 1.024244e+00 1.024244e+00 +7.202500e+02 0.000000e+00 0.000000e+00 3.274000e+01 8.724040e-01 8.724040e-01 +7.302400e+02 0.000000e+00 0.000000e+00 3.529000e+01 1.228387e+00 1.228387e+00 +7.402000e+02 0.000000e+00 0.000000e+00 3.881000e+01 1.222384e+00 1.222384e+00 +7.502800e+02 0.000000e+00 0.000000e+00 4.352000e+01 1.198784e+00 1.198784e+00 +7.601800e+02 0.000000e+00 0.000000e+00 4.471000e+01 1.219862e+00 1.219862e+00 +7.641700e+02 0.000000e+00 0.000000e+00 4.448000e+01 1.083386e+00 1.083386e+00 +7.701100e+02 0.000000e+00 0.000000e+00 4.548000e+01 1.201401e+00 1.201401e+00 +7.743800e+02 0.000000e+00 0.000000e+00 4.429000e+01 1.199799e+00 1.199799e+00 +7.781700e+02 0.000000e+00 0.000000e+00 4.668000e+01 1.359171e+00 1.359171e+00 +7.801700e+02 0.000000e+00 0.000000e+00 4.404000e+01 1.248288e+00 1.248288e+00 +7.822300e+02 0.000000e+00 0.000000e+00 3.755000e+01 7.163519e-01 7.163519e-01 +7.842400e+02 0.000000e+00 0.000000e+00 3.524000e+01 1.022109e+00 1.022109e+00 +7.860400e+02 0.000000e+00 0.000000e+00 3.092000e+01 1.115535e+00 1.115535e+00 +7.901000e+02 0.000000e+00 0.000000e+00 3.303000e+01 1.157098e+00 1.157098e+00 +7.941400e+02 0.000000e+00 0.000000e+00 3.090000e+01 8.895354e-01 8.895354e-01 +8.000200e+02 0.000000e+00 0.000000e+00 3.025000e+01 7.522249e-01 7.522249e-01 +8.101400e+02 0.000000e+00 0.000000e+00 2.633000e+01 5.818571e-01 5.818571e-01 +8.200200e+02 0.000000e+00 0.000000e+00 2.478000e+01 8.038692e-01 8.038692e-01 +8.299700e+02 0.000000e+00 0.000000e+00 2.115000e+01 7.705216e-01 7.705216e-01 +8.391000e+02 0.000000e+00 0.000000e+00 1.729000e+01 7.274352e-01 7.274352e-01 +8.492400e+02 0.000000e+00 0.000000e+00 1.457000e+01 7.252877e-01 7.252877e-01 +8.596000e+02 0.000000e+00 0.000000e+00 1.491000e+01 7.056933e-01 7.056933e-01 +8.695000e+02 0.000000e+00 0.000000e+00 1.141000e+01 4.749598e-01 4.749598e-01 +8.798400e+02 0.000000e+00 0.000000e+00 1.047000e+01 8.124324e-01 8.124324e-01 +8.897200e+02 0.000000e+00 0.000000e+00 8.690000e+00 3.538624e-01 3.538624e-01 +9.000400e+02 0.000000e+00 0.000000e+00 8.040000e+00 3.038537e-01 3.038537e-01 +9.100200e+02 0.000000e+00 0.000000e+00 7.050000e+00 3.227837e-01 3.227837e-01 +9.195600e+02 0.000000e+00 0.000000e+00 6.230000e+00 3.122455e-01 3.122455e-01 +9.301100e+02 0.000000e+00 0.000000e+00 5.910000e+00 3.716953e-01 3.716953e-01 +9.421900e+02 0.000000e+00 0.000000e+00 5.350000e+00 2.520524e-01 2.520524e-01 +9.518400e+02 0.000000e+00 0.000000e+00 4.720000e+00 2.416651e-01 2.416651e-01 +9.615200e+02 0.000000e+00 0.000000e+00 4.440000e+00 2.315377e-01 2.315377e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2002_I568807/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD2_2002_I568807/d01-x01-y02 +Title: doi:10.17182/hepdata.27037.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.105000e+02 0.000000e+00 0.000000e+00 3.352000e+02 4.724283e+01 4.724283e+01 +6.205000e+02 0.000000e+00 0.000000e+00 4.002000e+02 2.979691e+01 2.979691e+01 +6.305000e+02 0.000000e+00 0.000000e+00 4.387000e+02 2.921880e+01 2.921880e+01 +6.405100e+02 0.000000e+00 0.000000e+00 4.373000e+02 2.842137e+01 2.842137e+01 +6.504900e+02 0.000000e+00 0.000000e+00 4.939000e+02 3.253524e+01 3.253524e+01 +6.605000e+02 0.000000e+00 0.000000e+00 5.122000e+02 2.886407e+01 2.886407e+01 +6.705000e+02 0.000000e+00 0.000000e+00 5.760000e+02 3.089391e+01 3.089391e+01 +6.805900e+02 0.000000e+00 0.000000e+00 7.160000e+02 3.337762e+01 3.337762e+01 +6.904300e+02 0.000000e+00 0.000000e+00 7.374000e+02 2.647235e+01 2.647235e+01 +7.005200e+02 0.000000e+00 0.000000e+00 8.402000e+02 2.266768e+01 2.266768e+01 +7.104700e+02 0.000000e+00 0.000000e+00 9.546000e+02 3.447906e+01 3.447906e+01 +7.202500e+02 0.000000e+00 0.000000e+00 1.078800e+03 2.864100e+01 2.864100e+01 +7.302400e+02 0.000000e+00 0.000000e+00 1.137100e+03 3.959227e+01 3.959227e+01 +7.402000e+02 0.000000e+00 0.000000e+00 1.222200e+03 3.860293e+01 3.860293e+01 +7.502800e+02 0.000000e+00 0.000000e+00 1.338400e+03 3.678719e+01 3.678719e+01 +7.601800e+02 0.000000e+00 0.000000e+00 1.343600e+03 3.659890e+01 3.659890e+01 +7.641700e+02 0.000000e+00 0.000000e+00 1.325600e+03 3.239166e+01 3.239166e+01 +7.701100e+02 0.000000e+00 0.000000e+00 1.340300e+03 3.542486e+01 3.542486e+01 +7.743800e+02 0.000000e+00 0.000000e+00 1.297500e+03 3.526991e+01 3.526991e+01 +7.781700e+02 0.000000e+00 0.000000e+00 1.358000e+03 3.954845e+01 3.954845e+01 +7.801700e+02 0.000000e+00 0.000000e+00 1.265500e+03 3.591189e+01 3.591189e+01 +7.822300e+02 0.000000e+00 0.000000e+00 1.049300e+03 1.992102e+01 1.992102e+01 +7.842400e+02 0.000000e+00 0.000000e+00 9.598000e+02 2.790078e+01 2.790078e+01 +7.860400e+02 0.000000e+00 0.000000e+00 8.350000e+02 3.011960e+01 3.011960e+01 +7.901000e+02 0.000000e+00 0.000000e+00 8.900000e+02 3.125949e+01 3.125949e+01 +7.941400e+02 0.000000e+00 0.000000e+00 8.301000e+02 2.392418e+01 2.392418e+01 +8.000200e+02 0.000000e+00 0.000000e+00 8.062000e+02 2.018808e+01 2.018808e+01 +8.101400e+02 0.000000e+00 0.000000e+00 6.897000e+02 1.536765e+01 1.536765e+01 +8.200200e+02 0.000000e+00 0.000000e+00 6.373000e+02 2.075528e+01 2.075528e+01 +8.299700e+02 0.000000e+00 0.000000e+00 5.339000e+02 1.936677e+01 1.936677e+01 +8.391000e+02 0.000000e+00 0.000000e+00 4.292000e+02 1.808429e+01 1.808429e+01 +8.492400e+02 0.000000e+00 0.000000e+00 3.550000e+02 1.762915e+01 1.762915e+01 +8.596000e+02 0.000000e+00 0.000000e+00 3.565000e+02 1.683643e+01 1.683643e+01 +8.695000e+02 0.000000e+00 0.000000e+00 2.680000e+02 1.111691e+01 1.111691e+01 +8.798400e+02 0.000000e+00 0.000000e+00 2.414000e+02 1.875601e+01 1.875601e+01 +8.897200e+02 0.000000e+00 0.000000e+00 1.970000e+02 7.987936e+00 7.987936e+00 +9.000400e+02 0.000000e+00 0.000000e+00 1.789000e+02 6.785439e+00 6.785439e+00 +9.100200e+02 0.000000e+00 0.000000e+00 1.541000e+02 7.060799e+00 7.060799e+00 +9.195600e+02 0.000000e+00 0.000000e+00 1.340000e+02 6.748068e+00 6.748068e+00 +9.301100e+02 0.000000e+00 0.000000e+00 1.249000e+02 7.935465e+00 7.935465e+00 +9.421900e+02 0.000000e+00 0.000000e+00 1.108000e+02 5.341532e+00 5.341532e+00 +9.518400e+02 0.000000e+00 0.000000e+00 9.620000e+01 4.933879e+00 4.933879e+00 +9.615200e+02 0.000000e+00 0.000000e+00 8.910000e+01 4.730306e+00 4.730306e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2003_I601222.cc b/analyses/pluginNovosibirsk/CMD2_2003_I601222.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2003_I601222.cc @@ -0,0 +1,86 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2003_I601222 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2003_I601222); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + declare(FinalState(), "FS"); + _nK0K0 = bookCounter("TMP/K0K0"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && + nCount[130]==1 && nCount[310]==1) + _nK0K0->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _nK0K0->val(); + double error = _nK0K0->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nK0K0; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2003_I601222); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2003_I601222.info b/analyses/pluginNovosibirsk/CMD2_2003_I601222.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2003_I601222.info @@ -0,0 +1,34 @@ +Name: CMD2_2003_I601222 +Year: 2003 +Summary: Cross section for $e^+e^-\to K^0_SK^0_L$ at energies between 1.05 and 1.38 GeV +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 601222 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B551 (2003) 27-34, 2003 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to K^0_SK^0_L$ at energies between 1.05 and 1.38 GeV.' +Keywords: +BibKey: Akhmetshin:2002vj +BibTeX: '@article{Akhmetshin:2002vj, + author = "Akhmetshin, R. R. and others", + title = "{Study of the process e+ e- ---> K0(L) K0(S) in the CM + energy range 1.05-GeV to 1.38-GeV with CMD-2}", + journal = "Phys. Lett.", + volume = "B551", + year = "2003", + pages = "27-34", + doi = "10.1016/S0370-2693(02)02985-4", + eprint = "hep-ex/0211004", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0211004;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2003_I601222.plot b/analyses/pluginNovosibirsk/CMD2_2003_I601222.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2003_I601222.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /CMD2_2003_I601222/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2003_I601222.yoda b/analyses/pluginNovosibirsk/CMD2_2003_I601222.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2003_I601222.yoda @@ -0,0 +1,60 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2003_I601222/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2003_I601222/d01-x01-y01 +Title: doi:10.17182/hepdata.41971.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.050000e+00 0.000000e+00 0.000000e+00 1.756000e+01 2.209276e+00 2.209276e+00 +1.060000e+00 0.000000e+00 0.000000e+00 1.165000e+01 1.238225e+00 1.238225e+00 +1.070000e+00 0.000000e+00 0.000000e+00 7.130000e+00 9.100000e-01 9.100000e-01 +1.080000e+00 0.000000e+00 0.000000e+00 5.300000e+00 9.368031e-01 9.368031e-01 +1.090000e+00 0.000000e+00 0.000000e+00 5.180000e+00 7.716217e-01 7.716217e-01 +1.100000e+00 0.000000e+00 0.000000e+00 4.350000e+00 8.367795e-01 8.367795e-01 +1.110000e+00 0.000000e+00 0.000000e+00 3.580000e+00 7.117584e-01 7.117584e-01 +1.120000e+00 0.000000e+00 0.000000e+00 2.820000e+00 6.894926e-01 7.844743e-01 +1.130000e+00 0.000000e+00 0.000000e+00 2.230000e+00 5.787055e-01 6.552099e-01 +1.140000e+00 0.000000e+00 0.000000e+00 2.850000e+00 5.869412e-01 6.519202e-01 +1.150000e+00 0.000000e+00 0.000000e+00 2.850000e+00 6.612866e-01 7.749194e-01 +1.160000e+00 0.000000e+00 0.000000e+00 1.580000e+00 3.956008e-01 4.617359e-01 +1.170000e+00 0.000000e+00 0.000000e+00 2.070000e+00 5.281098e-01 6.140033e-01 +1.180000e+00 0.000000e+00 0.000000e+00 1.450000e+00 3.794733e-01 4.368066e-01 +1.190000e+00 0.000000e+00 0.000000e+00 1.790000e+00 3.992493e-01 4.648656e-01 +1.205000e+00 0.000000e+00 0.000000e+00 8.500000e-01 2.213594e-01 2.404163e-01 +1.225000e+00 0.000000e+00 0.000000e+00 1.160000e+00 2.370654e-01 2.640076e-01 +1.251000e+00 0.000000e+00 0.000000e+00 5.700000e-01 1.486607e-01 1.486607e-01 +1.275000e+00 0.000000e+00 0.000000e+00 5.500000e-01 1.486607e-01 1.772005e-01 +1.296000e+00 0.000000e+00 0.000000e+00 5.000000e-01 1.300000e-01 1.486607e-01 +1.325000e+00 0.000000e+00 0.000000e+00 1.700000e-01 8.246211e-02 9.219544e-02 +1.368000e+00 0.000000e+00 0.000000e+00 2.500000e-01 7.280110e-02 8.246211e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2003_I601222/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD2_2003_I601222/d01-x01-y02 +Title: doi:10.17182/hepdata.41971.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.050000e+00 0.000000e+00 0.000000e+00 1.665000e+01 2.097475e+00 2.097475e+00 +1.060000e+00 0.000000e+00 0.000000e+00 1.110000e+01 1.145862e+00 1.145862e+00 +1.070000e+00 0.000000e+00 0.000000e+00 6.820000e+00 8.653901e-01 8.653901e-01 +1.080000e+00 0.000000e+00 0.000000e+00 5.080000e+00 8.956004e-01 8.956004e-01 +1.090000e+00 0.000000e+00 0.000000e+00 4.970000e+00 7.400000e-01 7.400000e-01 +1.100000e+00 0.000000e+00 0.000000e+00 4.190000e+00 8.052329e-01 8.052329e-01 +1.110000e+00 0.000000e+00 0.000000e+00 3.440000e+00 6.802941e-01 6.802941e-01 +1.120000e+00 0.000000e+00 0.000000e+00 2.710000e+00 6.578754e-01 7.528612e-01 +1.130000e+00 0.000000e+00 0.000000e+00 2.150000e+00 5.597321e-01 6.360031e-01 +1.140000e+00 0.000000e+00 0.000000e+00 2.750000e+00 5.646238e-01 6.296825e-01 +1.150000e+00 0.000000e+00 0.000000e+00 2.750000e+00 6.356886e-01 7.404053e-01 +1.160000e+00 0.000000e+00 0.000000e+00 1.520000e+00 3.827532e-01 4.396590e-01 +1.170000e+00 0.000000e+00 0.000000e+00 2.000000e+00 5.059644e-01 5.920304e-01 +1.180000e+00 0.000000e+00 0.000000e+00 1.400000e+00 3.700000e-01 4.272002e-01 +1.190000e+00 0.000000e+00 0.000000e+00 1.720000e+00 3.862642e-01 4.427189e-01 +1.205000e+00 0.000000e+00 0.000000e+00 8.200000e-01 2.213594e-01 2.404163e-01 +1.225000e+00 0.000000e+00 0.000000e+00 1.120000e+00 2.370654e-01 2.640076e-01 +1.251000e+00 0.000000e+00 0.000000e+00 5.500000e-01 1.486607e-01 1.486607e-01 +1.275000e+00 0.000000e+00 0.000000e+00 5.300000e-01 1.486607e-01 1.772005e-01 +1.296000e+00 0.000000e+00 0.000000e+00 4.800000e-01 1.300000e-01 1.486607e-01 +1.325000e+00 0.000000e+00 0.000000e+00 1.600000e-01 8.246211e-02 9.219544e-02 +1.368000e+00 0.000000e+00 0.000000e+00 2.400000e-01 7.280110e-02 8.246211e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2003_I616446.cc b/analyses/pluginNovosibirsk/CMD2_2003_I616446.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2003_I616446.cc @@ -0,0 +1,108 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2003_I616446 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2003_I616446); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numOmegaPi = bookCounter("TMP/OmegaPi"); + } + + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]+=1; + ++ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // three particles (pi0 pi0 gamma) + if(ntotal!=3) vetoEvent; + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==223) { + map nRes; + int ncount(0); + findChildren(p,nRes,ncount); + // only omega to pi0 gamma mode + if(ncount!=2) continue; + if(nRes[111]!=1 || nRes[22]!=1) continue; + // omega pi0 + if(nCount[111]-nRes[111]==1) + _numOmegaPi->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + Scatter2D temphisto(refData(1, 1, 1)); + double sigma = _numOmegaPi->val(); + double error = _numOmegaPi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + /// @name Histograms + //@{ + CounterPtr _numOmegaPi; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2003_I616446); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2003_I616446.info b/analyses/pluginNovosibirsk/CMD2_2003_I616446.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2003_I616446.info @@ -0,0 +1,34 @@ +Name: CMD2_2003_I616446 +Year: 2003 +Summary: Cross section for $e^+e^-\to\omega\pi^0\to\pi^0\pi^0\gamma$ between 0.92 and 1.38 GeV +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 616446 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B562 (2003) 173-181, 2003 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\omega\pi^0\to\pi^0\pi^0\gamma$ at energies 0.92 and 1.38 GeV.' +Keywords: +BibKey: Akhmetshin:2003ag +BibTeX: '@article{Akhmetshin:2003ag, + author = "Akhmetshin, R. R. and others", + title = "{Study of the process e+ e- ---> omega pi0 ---> pi0 pi0 + gamma in c.m. energy range 920-MeV - 1380-MeV at CMD-2}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B562", + year = "2003", + pages = "173-181", + doi = "10.1016/S0370-2693(03)00595-1", + eprint = "hep-ex/0304009", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0304009;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2003_I616446.plot b/analyses/pluginNovosibirsk/CMD2_2003_I616446.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2003_I616446.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /CMD2_2003_I616446/d01-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^0\to \pi^0\pi^0\gamma)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0\to \pi^0\pi^0\gamma)$/nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2003_I616446.yoda b/analyses/pluginNovosibirsk/CMD2_2003_I616446.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2003_I616446.yoda @@ -0,0 +1,84 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2003_I616446/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2003_I616446/d01-x01-y01 +Title: doi:10.17182/hepdata.41951.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.200000e+02 0.000000e+00 0.000000e+00 6.000000e-02 3.026023e-02 3.026023e-02 +9.400000e+02 0.000000e+00 0.000000e+00 1.200000e-01 4.077654e-02 4.077654e-02 +9.500000e+02 0.000000e+00 0.000000e+00 3.700000e-01 9.325415e-02 9.325415e-02 +9.600000e+02 0.000000e+00 0.000000e+00 4.200000e-01 9.417217e-02 9.417217e-02 +9.700000e+02 0.000000e+00 0.000000e+00 5.400000e-01 1.061612e-01 1.061612e-01 +9.840000e+02 0.000000e+00 0.000000e+00 5.900000e-01 8.897372e-02 8.897372e-02 +1.004000e+03 0.000000e+00 0.000000e+00 6.300000e-01 9.016039e-02 9.016039e-02 +1.034000e+03 0.000000e+00 0.000000e+00 1.100000e+00 1.317982e-01 1.317982e-01 +1.044000e+03 0.000000e+00 0.000000e+00 9.200000e-01 8.536345e-02 8.536345e-02 +1.061000e+03 0.000000e+00 0.000000e+00 8.300000e-01 9.695797e-02 9.695797e-02 +1.083000e+03 0.000000e+00 0.000000e+00 1.230000e+00 1.532651e-01 1.532651e-01 +1.103000e+03 0.000000e+00 0.000000e+00 8.600000e-01 1.237808e-01 1.237808e-01 +1.123000e+03 0.000000e+00 0.000000e+00 1.270000e+00 1.546796e-01 1.546796e-01 +1.142000e+03 0.000000e+00 0.000000e+00 1.180000e+00 1.515430e-01 1.515430e-01 +1.163000e+03 0.000000e+00 0.000000e+00 1.430000e+00 1.688419e-01 1.688419e-01 +1.183000e+03 0.000000e+00 0.000000e+00 1.260000e+00 1.300599e-01 1.300599e-01 +1.204000e+03 0.000000e+00 0.000000e+00 1.300000e+00 1.557615e-01 1.557615e-01 +1.226000e+03 0.000000e+00 0.000000e+00 1.300000e+00 1.642000e-01 1.642000e-01 +1.246000e+03 0.000000e+00 0.000000e+00 1.570000e+00 1.662441e-01 1.662441e-01 +1.266000e+03 0.000000e+00 0.000000e+00 1.470000e+00 1.543142e-01 1.543142e-01 +1.286000e+03 0.000000e+00 0.000000e+00 1.350000e+00 1.339358e-01 1.339358e-01 +1.304000e+03 0.000000e+00 0.000000e+00 1.400000e+00 1.361534e-01 1.361534e-01 +1.326000e+03 0.000000e+00 0.000000e+00 1.410000e+00 1.366022e-01 1.366022e-01 +1.345000e+03 0.000000e+00 0.000000e+00 1.410000e+00 1.440839e-01 1.440839e-01 +1.364000e+03 0.000000e+00 0.000000e+00 1.510000e+00 1.484322e-01 1.484322e-01 +1.380000e+03 0.000000e+00 0.000000e+00 1.310000e+00 1.321943e-01 1.321943e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2003_I616446/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD2_2003_I616446/d01-x01-y02 +Title: doi:10.17182/hepdata.41951.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.200000e+02 0.000000e+00 0.000000e+00 6.000000e-02 3.026023e-02 3.026023e-02 +9.400000e+02 0.000000e+00 0.000000e+00 1.200000e-01 4.077654e-02 4.077654e-02 +9.500000e+02 0.000000e+00 0.000000e+00 3.500000e-01 8.326830e-02 8.326830e-02 +9.600000e+02 0.000000e+00 0.000000e+00 4.100000e-01 8.445261e-02 8.445261e-02 +9.700000e+02 0.000000e+00 0.000000e+00 5.200000e-01 1.057254e-01 1.057254e-01 +9.840000e+02 0.000000e+00 0.000000e+00 5.800000e-01 8.868686e-02 8.868686e-02 +1.004000e+03 0.000000e+00 0.000000e+00 6.300000e-01 9.016039e-02 9.016039e-02 +1.034000e+03 0.000000e+00 0.000000e+00 1.020000e+00 1.205487e-01 1.205487e-01 +1.044000e+03 0.000000e+00 0.000000e+00 8.700000e-01 8.304852e-02 8.304852e-02 +1.061000e+03 0.000000e+00 0.000000e+00 7.900000e-01 9.549125e-02 9.549125e-02 +1.083000e+03 0.000000e+00 0.000000e+00 1.180000e+00 1.430570e-01 1.430570e-01 +1.103000e+03 0.000000e+00 0.000000e+00 8.300000e-01 1.228855e-01 1.228855e-01 +1.123000e+03 0.000000e+00 0.000000e+00 1.230000e+00 1.532651e-01 1.532651e-01 +1.142000e+03 0.000000e+00 0.000000e+00 1.140000e+00 1.416371e-01 1.416371e-01 +1.163000e+03 0.000000e+00 0.000000e+00 1.370000e+00 1.583533e-01 1.583533e-01 +1.183000e+03 0.000000e+00 0.000000e+00 1.220000e+00 1.283880e-01 1.283880e-01 +1.204000e+03 0.000000e+00 0.000000e+00 1.260000e+00 1.543230e-01 1.543230e-01 +1.226000e+03 0.000000e+00 0.000000e+00 1.250000e+00 1.625000e-01 1.625000e-01 +1.246000e+03 0.000000e+00 0.000000e+00 1.520000e+00 1.642075e-01 1.642075e-01 +1.266000e+03 0.000000e+00 0.000000e+00 1.430000e+00 1.449399e-01 1.449399e-01 +1.286000e+03 0.000000e+00 0.000000e+00 1.310000e+00 1.321943e-01 1.321943e-01 +1.304000e+03 0.000000e+00 0.000000e+00 1.350000e+00 1.339358e-01 1.339358e-01 +1.326000e+03 0.000000e+00 0.000000e+00 1.370000e+00 1.348176e-01 1.348176e-01 +1.345000e+03 0.000000e+00 0.000000e+00 1.360000e+00 1.419748e-01 1.419748e-01 +1.364000e+03 0.000000e+00 0.000000e+00 1.460000e+00 1.388713e-01 1.388713e-01 +1.380000e+03 0.000000e+00 0.000000e+00 1.270000e+00 1.229870e-01 1.229870e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2003_I616446/d02-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2003_I616446/d02-x01-y01 +Title: doi:10.17182/hepdata.41951.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2003_I616446/d03-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2003_I616446/d03-x01-y01 +Title: doi:10.17182/hepdata.41951.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2004_I630009.cc b/analyses/pluginNovosibirsk/CMD2_2004_I630009.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2004_I630009.cc @@ -0,0 +1,87 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2004_I630009 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2004_I630009); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + _numPiPiGamma = bookCounter("TMP/PiPiGamma"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // three particles (pi0 pi0 gamma) + if(ntotal!=3) vetoEvent; + if(nCount[111]==2 && nCount[22]==1) + _numPiPiGamma->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _numPiPiGamma->val(); + double error = _numPiPiGamma->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numPiPiGamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2004_I630009); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2004_I630009.info b/analyses/pluginNovosibirsk/CMD2_2004_I630009.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2004_I630009.info @@ -0,0 +1,35 @@ +Name: CMD2_2004_I630009 +Year: 2004 +Summary: Cross section for $e^+e^-\to\pi^0\pi^0\gamma$ at energies between 0.6 and 0.97 GeV. +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 630009 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B580 (2004) 119-128, 2004 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^0\pi^0\gamma$ at energies between 0.6 and 0.97 GeV.' +Keywords: [] +BibKey: Akhmetshin:2003rg +BibTeX: '@article{Akhmetshin:2003rg, + author = "Akhmetshin, R. R. and others", + title = "{Study of the process e+ e- ---> pi0 pi0 gamma in c.m. + energy range 600-MeV to 970-MeV at CMD2}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B580", + year = "2004", + pages = "119-128", + doi = "10.1016/j.physletb.2003.11.046", + eprint = "hep-ex/0310012", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0310012;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2004_I630009.plot b/analyses/pluginNovosibirsk/CMD2_2004_I630009.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2004_I630009.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /CMD2_2004_I630009/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^0\pi^0\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^0\pi^0\gamma)$/pb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2004_I630009.yoda b/analyses/pluginNovosibirsk/CMD2_2004_I630009.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2004_I630009.yoda @@ -0,0 +1,64 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2004_I630009/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2004_I630009/d01-x01-y01 +Title: doi:10.17182/hepdata.41906.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.500000e+02 0.000000e+00 0.000000e+00 1.060000e+02 6.917947e+01 8.495763e+01 +7.600000e+02 0.000000e+00 0.000000e+00 6.200000e+01 3.872149e+01 8.233683e+01 +7.640000e+02 0.000000e+00 0.000000e+00 1.910000e+02 1.221693e+02 3.347855e+02 +7.740000e+02 0.000000e+00 0.000000e+00 1.230000e+02 6.763030e+01 1.109858e+02 +7.780000e+02 0.000000e+00 0.000000e+00 1.900000e+02 9.090567e+01 1.339546e+02 +7.800000e+02 0.000000e+00 0.000000e+00 4.170000e+02 1.047282e+02 1.685972e+02 +7.810000e+02 0.000000e+00 0.000000e+00 1.120000e+02 4.314665e+01 9.099799e+01 +7.820000e+02 0.000000e+00 0.000000e+00 3.220000e+02 7.052694e+01 7.305511e+01 +7.830000e+02 0.000000e+00 0.000000e+00 3.610000e+02 1.154367e+02 1.332390e+02 +7.840000e+02 0.000000e+00 0.000000e+00 2.950000e+02 9.207692e+01 1.165082e+02 +7.850000e+02 0.000000e+00 0.000000e+00 2.830000e+02 1.075048e+02 1.489237e+02 +7.860000e+02 0.000000e+00 0.000000e+00 3.320000e+02 1.302429e+02 1.523031e+02 +7.900000e+02 0.000000e+00 0.000000e+00 1.530000e+02 7.721457e+01 1.263412e+02 +7.940000e+02 0.000000e+00 0.000000e+00 1.300000e+02 6.199484e+01 1.012095e+02 +8.000000e+02 0.000000e+00 0.000000e+00 3.200000e+01 2.430526e+01 5.513389e+01 +8.100000e+02 0.000000e+00 0.000000e+00 5.100000e+01 4.046547e+01 5.931656e+01 +8.200000e+02 0.000000e+00 0.000000e+00 4.900000e+01 3.450470e+01 4.935154e+01 +8.400000e+02 0.000000e+00 0.000000e+00 1.240000e+02 4.080949e+01 4.644798e+01 +8.800000e+02 0.000000e+00 0.000000e+00 5.400000e+01 2.679534e+01 3.756315e+01 +9.200000e+02 0.000000e+00 0.000000e+00 6.500000e+01 3.003065e+01 4.468602e+01 +9.400000e+02 0.000000e+00 0.000000e+00 2.190000e+02 6.550296e+01 8.610829e+01 +9.500000e+02 0.000000e+00 0.000000e+00 3.690000e+02 1.093651e+02 1.250988e+02 +9.580000e+02 0.000000e+00 0.000000e+00 4.020000e+02 1.119290e+02 1.256308e+02 +9.700000e+02 0.000000e+00 0.000000e+00 5.160000e+02 1.184698e+02 1.314918e+02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2004_I630009/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD2_2004_I630009/d01-x01-y02 +Title: doi:10.17182/hepdata.41906.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.500000e+02 0.000000e+00 0.000000e+00 1.050000e+02 6.915750e+01 8.395094e+01 +7.600000e+02 0.000000e+00 0.000000e+00 6.200000e+01 3.872149e+01 8.134097e+01 +7.640000e+02 0.000000e+00 0.000000e+00 1.890000e+02 1.211420e+02 3.317761e+02 +7.740000e+02 0.000000e+00 0.000000e+00 1.220000e+02 6.760421e+01 1.099788e+02 +7.780000e+02 0.000000e+00 0.000000e+00 1.890000e+02 8.990763e+01 1.329488e+02 +7.800000e+02 0.000000e+00 0.000000e+00 4.100000e+02 1.025702e+02 1.654831e+02 +7.810000e+02 0.000000e+00 0.000000e+00 1.090000e+02 4.208428e+01 8.797776e+01 +7.820000e+02 0.000000e+00 0.000000e+00 3.090000e+02 6.799946e+01 7.053316e+01 +7.830000e+02 0.000000e+00 0.000000e+00 3.420000e+02 1.090196e+02 1.258780e+02 +7.840000e+02 0.000000e+00 0.000000e+00 2.760000e+02 8.658484e+01 1.091464e+02 +7.850000e+02 0.000000e+00 0.000000e+00 2.640000e+02 1.001430e+02 1.386673e+02 +7.860000e+02 0.000000e+00 0.000000e+00 3.090000e+02 1.217823e+02 1.419293e+02 +7.900000e+02 0.000000e+00 0.000000e+00 1.440000e+02 7.210131e+01 1.182692e+02 +7.940000e+02 0.000000e+00 0.000000e+00 1.230000e+02 5.888003e+01 9.515176e+01 +8.000000e+02 0.000000e+00 0.000000e+00 3.000000e+01 2.328003e+01 5.212447e+01 +8.100000e+02 0.000000e+00 0.000000e+00 4.800000e+01 3.843407e+01 5.629545e+01 +8.200000e+02 0.000000e+00 0.000000e+00 4.600000e+01 3.247261e+01 4.633002e+01 +8.400000e+02 0.000000e+00 0.000000e+00 1.180000e+02 3.868469e+01 4.432274e+01 +8.800000e+02 0.000000e+00 0.000000e+00 5.100000e+01 2.573819e+01 3.553103e+01 +9.200000e+02 0.000000e+00 0.000000e+00 6.300000e+01 2.900265e+01 4.267498e+01 +9.400000e+02 0.000000e+00 0.000000e+00 2.120000e+02 6.333398e+01 8.299514e+01 +9.500000e+02 0.000000e+00 0.000000e+00 3.570000e+02 1.060390e+02 1.208481e+02 +9.580000e+02 0.000000e+00 0.000000e+00 3.900000e+02 1.086013e+02 1.213847e+02 +9.700000e+02 0.000000e+00 0.000000e+00 5.020000e+02 1.150342e+02 1.271726e+02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2004_I648023.cc b/analyses/pluginNovosibirsk/CMD2_2004_I648023.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2004_I648023.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2004_I648023 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2004_I648023); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=4) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2004_I648023); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2004_I648023.info b/analyses/pluginNovosibirsk/CMD2_2004_I648023.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2004_I648023.info @@ -0,0 +1,34 @@ +Name: CMD2_2004_I648023 +Year: 2004 +Summary: Cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ between 0.98 and 1.38 GeV +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 648023 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B595 (2004) 101-108, 2004 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ between 0.98 and 1.38 GeV.' +Keywords: +BibKey: Akhmetshin:2004dy +BibTeX: '@article{Akhmetshin:2004dy, + author = "Akhmetshin, R. R. and others", + title = "{Total cross section of the process e+ e- ---> pi+ pi- + pi+ pi- in the C.M. energy range 980-MeV to 1380-MeV}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B595", + year = "2004", + pages = "101-108", + doi = "10.1016/j.physletb.2004.05.056", + eprint = "hep-ex/0404019", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0404019;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2004_I648023.plot b/analyses/pluginNovosibirsk/CMD2_2004_I648023.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2004_I648023.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /CMD2_2004_I648023/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2004_I648023.yoda b/analyses/pluginNovosibirsk/CMD2_2004_I648023.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2004_I648023.yoda @@ -0,0 +1,44 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2004_I648023/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2004_I648023/d01-x01-y01 +Title: doi:10.17182/hepdata.41915.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.800000e+02 0.000000e+00 0.000000e+00 6.500000e-01 2.200000e-01 2.200000e-01 +1.040000e+03 0.000000e+00 0.000000e+00 2.010000e+00 3.300000e-01 3.300000e-01 +1.050000e+03 0.000000e+00 0.000000e+00 2.020000e+00 2.300000e-01 2.300000e-01 +1.060000e+03 0.000000e+00 0.000000e+00 2.520000e+00 3.200000e-01 3.200000e-01 +1.070000e+03 0.000000e+00 0.000000e+00 2.480000e+00 3.000000e-01 3.000000e-01 +1.080000e+03 0.000000e+00 0.000000e+00 2.960000e+00 4.000000e-01 4.000000e-01 +1.090000e+03 0.000000e+00 0.000000e+00 3.550000e+00 3.500000e-01 3.500000e-01 +1.100000e+03 0.000000e+00 0.000000e+00 4.070000e+00 4.500000e-01 4.500000e-01 +1.110000e+03 0.000000e+00 0.000000e+00 3.920000e+00 3.700000e-01 3.700000e-01 +1.120000e+03 0.000000e+00 0.000000e+00 3.850000e+00 4.800000e-01 4.800000e-01 +1.130000e+03 0.000000e+00 0.000000e+00 4.860000e+00 3.700000e-01 3.700000e-01 +1.140000e+03 0.000000e+00 0.000000e+00 6.050000e+00 4.100000e-01 4.100000e-01 +1.150000e+03 0.000000e+00 0.000000e+00 5.510000e+00 5.400000e-01 5.400000e-01 +1.160000e+03 0.000000e+00 0.000000e+00 6.300000e+00 3.800000e-01 3.800000e-01 +1.170000e+03 0.000000e+00 0.000000e+00 7.050000e+00 5.700000e-01 5.700000e-01 +1.180000e+03 0.000000e+00 0.000000e+00 8.040000e+00 4.300000e-01 4.300000e-01 +1.190000e+03 0.000000e+00 0.000000e+00 9.270000e+00 4.500000e-01 4.500000e-01 +1.200000e+03 0.000000e+00 0.000000e+00 9.730000e+00 3.700000e-01 3.700000e-01 +1.210000e+03 0.000000e+00 0.000000e+00 9.920000e+00 4.600000e-01 4.600000e-01 +1.220000e+03 0.000000e+00 0.000000e+00 1.165000e+01 5.200000e-01 5.200000e-01 +1.230000e+03 0.000000e+00 0.000000e+00 1.254000e+01 4.700000e-01 4.700000e-01 +1.240000e+03 0.000000e+00 0.000000e+00 1.273000e+01 4.800000e-01 4.800000e-01 +1.250000e+03 0.000000e+00 0.000000e+00 1.341000e+01 4.500000e-01 4.500000e-01 +1.260000e+03 0.000000e+00 0.000000e+00 1.526000e+01 4.600000e-01 4.600000e-01 +1.270000e+03 0.000000e+00 0.000000e+00 1.575000e+01 4.000000e-01 4.000000e-01 +1.280000e+03 0.000000e+00 0.000000e+00 1.614000e+01 4.300000e-01 4.300000e-01 +1.290000e+03 0.000000e+00 0.000000e+00 1.664000e+01 4.200000e-01 4.200000e-01 +1.300000e+03 0.000000e+00 0.000000e+00 1.799000e+01 4.000000e-01 4.000000e-01 +1.310000e+03 0.000000e+00 0.000000e+00 1.850000e+01 4.400000e-01 4.400000e-01 +1.320000e+03 0.000000e+00 0.000000e+00 1.972000e+01 5.000000e-01 5.000000e-01 +1.330000e+03 0.000000e+00 0.000000e+00 1.907000e+01 4.000000e-01 4.000000e-01 +1.340000e+03 0.000000e+00 0.000000e+00 2.112000e+01 5.000000e-01 5.000000e-01 +1.350000e+03 0.000000e+00 0.000000e+00 2.137000e+01 5.200000e-01 5.200000e-01 +1.360000e+03 0.000000e+00 0.000000e+00 2.216000e+01 4.300000e-01 4.300000e-01 +1.370000e+03 0.000000e+00 0.000000e+00 2.335000e+01 5.800000e-01 5.800000e-01 +1.380000e+03 0.000000e+00 0.000000e+00 2.386000e+01 3.500000e-01 3.500000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2005_I658856.cc b/analyses/pluginNovosibirsk/CMD2_2005_I658856.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2005_I658856.cc @@ -0,0 +1,136 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2005_I658856 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2005_I658856); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaGamma = bookCounter("TMP/EtaGamma"); + _numPi0Gamma = bookCounter("TMP/Pi0Gamma"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && nCount[22]==1 && nCount[111]==1) + _numPi0Gamma->fill(event.weight()); + + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(val.first==22) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaGamma->fill(event.weight()); + } + } + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + double sigma,error; + if(ix==1) { + sigma = _numEtaGamma->val(); + error = _numEtaGamma->err(); + } + else { + sigma = _numPi0Gamma->val(); + error = _numPi0Gamma->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numEtaGamma,_numPi0Gamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2005_I658856); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2005_I658856.info b/analyses/pluginNovosibirsk/CMD2_2005_I658856.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2005_I658856.info @@ -0,0 +1,35 @@ +Name: CMD2_2005_I658856 +Year: 2005 +Summary: Cross section for $e^+e^-\to\pi\gamma$ and $\eta\gamma$ for energies between 600 MeV and 1380 MeV +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 658856 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B605 (2005) 26-36 +RunInfo: e+ e- to hadrons below 0.6 and 1.38 GeV +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\pi\gamma$ and $\eta\gamma$ for energies between 600 MeV and 1380 MeV' +Keywords: +BibKey: Akhmetshin:2004gw +BibTeX: '@article{Akhmetshin:2004gw, + author = "Akhmetshin, R. R. and others", + title = "{Study of the processes e+ e- ---> eta gamma, pi0 gamma + ---> 3 gamma in the c.m. energy range 600-MeV to 1380-MeV + at CMD-2}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B605", + year = "2005", + pages = "26-36", + doi = "10.1016/j.physletb.2004.11.020", + eprint = "hep-ex/0409030", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "BUDKER-INP-2004-51", + SLACcitation = "%%CITATION = HEP-EX/0409030;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2005_I658856.plot b/analyses/pluginNovosibirsk/CMD2_2005_I658856.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2005_I658856.plot @@ -0,0 +1,16 @@ +BEGIN PLOT /CMD2_2005_I658856/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\gamma)$/nb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_2005_I658856/d02-x01-y01 +Title=$\sigma(e^+e^-\to \pi^0\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^0\gamma)$/nb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2005_I658856.yoda b/analyses/pluginNovosibirsk/CMD2_2005_I658856.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2005_I658856.yoda @@ -0,0 +1,104 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2005_I658856/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2005_I658856/d01-x01-y01 +Title: doi:10.17182/hepdata.41864.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.598600e+02 0.000000e+00 0.000000e+00 7.500000e-01 6.316051e-01 6.316051e-01 +7.598600e+02 0.000000e+00 0.000000e+00 7.300000e-01 5.118774e-01 5.118774e-01 +7.638600e+02 0.000000e+00 0.000000e+00 1.000000e+00 6.129437e-01 6.129437e-01 +7.738600e+02 0.000000e+00 0.000000e+00 1.100000e-01 2.600838e-01 2.600838e-01 +7.778600e+02 0.000000e+00 0.000000e+00 2.200000e-01 2.703225e-01 2.703225e-01 +7.798600e+02 0.000000e+00 0.000000e+00 1.500000e+00 4.687217e-01 4.687217e-01 +7.808600e+02 0.000000e+00 0.000000e+00 5.700000e-01 1.140513e+00 1.140513e+00 +7.818600e+02 0.000000e+00 0.000000e+00 9.400000e-01 1.886292e-01 1.886292e-01 +7.828600e+02 0.000000e+00 0.000000e+00 1.030000e+00 3.751256e-01 3.751256e-01 +7.838600e+02 0.000000e+00 0.000000e+00 2.200000e-01 2.903003e-01 2.903003e-01 +7.858600e+02 0.000000e+00 0.000000e+00 8.700000e-01 3.637648e-01 3.637648e-01 +7.898600e+02 0.000000e+00 0.000000e+00 3.600000e-01 4.804858e-01 4.804858e-01 +7.938600e+02 0.000000e+00 0.000000e+00 2.300000e-01 3.103070e-01 3.103070e-01 +7.998600e+02 0.000000e+00 0.000000e+00 1.000000e-01 2.300782e-01 2.300782e-01 +8.098600e+02 0.000000e+00 0.000000e+00 4.100000e-01 2.910415e-01 2.910415e-01 +8.198600e+02 0.000000e+00 0.000000e+00 4.700000e-01 2.416511e-01 2.416511e-01 +8.398600e+02 0.000000e+00 0.000000e+00 4.300000e-01 2.314425e-01 2.314425e-01 +8.798600e+02 0.000000e+00 0.000000e+00 8.000000e-02 1.500768e-01 1.500768e-01 +9.198600e+02 0.000000e+00 0.000000e+00 1.400000e-01 1.302711e-01 1.302711e-01 +9.398600e+02 0.000000e+00 0.000000e+00 6.000000e-02 1.800360e-01 1.800360e-01 +9.498600e+02 0.000000e+00 0.000000e+00 3.800000e-01 1.517229e-01 1.517229e-01 +9.578600e+02 0.000000e+00 0.000000e+00 1.700000e-01 1.204327e-01 1.204327e-01 +9.698600e+02 0.000000e+00 0.000000e+00 1.200000e-01 1.202158e-01 1.202158e-01 +9.839300e+02 0.000000e+00 0.000000e+00 7.000000e-02 1.300678e-01 1.300678e-01 +1.003910e+03 0.000000e+00 0.000000e+00 6.700000e-01 1.552934e-01 1.552934e-01 +1.010530e+03 0.000000e+00 0.000000e+00 1.480000e+00 1.829903e-01 1.829903e-01 +1.015770e+03 0.000000e+00 0.000000e+00 6.800000e+00 5.064227e-01 5.064227e-01 +1.016770e+03 0.000000e+00 0.000000e+00 1.000000e+01 6.579514e-01 6.579514e-01 +1.016910e+03 0.000000e+00 0.000000e+00 1.090000e+01 8.172001e-01 8.172001e-01 +1.017610e+03 0.000000e+00 0.000000e+00 1.377000e+01 8.860059e-01 8.860059e-01 +1.017770e+03 0.000000e+00 0.000000e+00 1.480000e+01 9.910318e-01 9.910318e-01 +1.018580e+03 0.000000e+00 0.000000e+00 2.131000e+01 1.404001e+00 1.404001e+00 +1.018830e+03 0.000000e+00 0.000000e+00 2.113000e+01 1.302811e+00 1.302811e+00 +1.019500e+03 0.000000e+00 0.000000e+00 2.150000e+01 1.359779e+00 1.359779e+00 +1.019840e+03 0.000000e+00 0.000000e+00 2.154000e+01 1.484317e+00 1.484317e+00 +1.020620e+03 0.000000e+00 0.000000e+00 1.552000e+01 9.783320e-01 9.783320e-01 +1.021540e+03 0.000000e+00 0.000000e+00 9.820000e+00 6.904757e-01 6.904757e-01 +1.022790e+03 0.000000e+00 0.000000e+00 5.380000e+00 4.144874e-01 4.144874e-01 +1.027670e+03 0.000000e+00 0.000000e+00 1.080000e+00 1.633984e-01 1.633984e-01 +1.033670e+03 0.000000e+00 0.000000e+00 3.800000e-01 1.418444e-01 1.418444e-01 +1.039590e+03 0.000000e+00 0.000000e+00 1.800000e-01 1.304478e-01 1.304478e-01 +1.049800e+03 0.000000e+00 0.000000e+00 5.000000e-02 1.300346e-01 1.300346e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2005_I658856/d02-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2005_I658856/d02-x01-y01 +Title: doi:10.17182/hepdata.41864.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.998600e+02 0.000000e+00 0.000000e+00 1.230000e+00 8.631607e-01 8.631607e-01 +6.298600e+02 0.000000e+00 0.000000e+00 1.780000e+00 7.476672e-01 7.476672e-01 +6.598600e+02 0.000000e+00 0.000000e+00 1.920000e+00 8.974247e-01 8.974247e-01 +7.198600e+02 0.000000e+00 0.000000e+00 2.000000e+00 6.609841e-01 6.609841e-01 +7.498600e+02 0.000000e+00 0.000000e+00 5.080000e+00 1.016761e+00 1.016761e+00 +7.598600e+02 0.000000e+00 0.000000e+00 8.310000e+00 1.486137e+00 1.486137e+00 +7.638600e+02 0.000000e+00 0.000000e+00 1.297000e+01 1.707629e+00 1.707629e+00 +7.698600e+02 0.000000e+00 0.000000e+00 1.764000e+01 2.062307e+00 2.062307e+00 +7.738600e+02 0.000000e+00 0.000000e+00 3.433000e+01 2.748668e+00 2.748668e+00 +7.778600e+02 0.000000e+00 0.000000e+00 7.665000e+01 5.302867e+00 5.302867e+00 +7.798600e+02 0.000000e+00 0.000000e+00 1.258100e+02 9.010425e+00 9.010425e+00 +7.808600e+02 0.000000e+00 0.000000e+00 1.849800e+02 1.561933e+01 1.561933e+01 +7.818600e+02 0.000000e+00 0.000000e+00 1.722600e+02 1.062664e+01 1.062664e+01 +7.828600e+02 0.000000e+00 0.000000e+00 1.833700e+02 1.200368e+01 1.200368e+01 +7.838600e+02 0.000000e+00 0.000000e+00 1.620000e+02 1.080541e+01 1.080541e+01 +7.858600e+02 0.000000e+00 0.000000e+00 1.184400e+02 8.234472e+00 8.234472e+00 +7.898600e+02 0.000000e+00 0.000000e+00 4.280000e+01 4.586352e+00 4.586352e+00 +7.938600e+02 0.000000e+00 0.000000e+00 1.993000e+01 2.381919e+00 2.381919e+00 +7.998600e+02 0.000000e+00 0.000000e+00 1.118000e+01 1.661437e+00 1.661437e+00 +8.098600e+02 0.000000e+00 0.000000e+00 5.220000e+00 1.134105e+00 1.134105e+00 +8.198600e+02 0.000000e+00 0.000000e+00 2.740000e+00 6.414260e-01 6.414260e-01 +8.398600e+02 0.000000e+00 0.000000e+00 1.580000e+00 4.598772e-01 4.598772e-01 +8.798600e+02 0.000000e+00 0.000000e+00 4.400000e-01 2.116529e-01 2.116529e-01 +9.198600e+02 0.000000e+00 0.000000e+00 4.100000e-01 1.323071e-01 1.323071e-01 +9.398600e+02 0.000000e+00 0.000000e+00 7.400000e-01 2.244356e-01 2.244356e-01 +9.498600e+02 0.000000e+00 0.000000e+00 5.000000e-01 1.529706e-01 1.529706e-01 +9.578600e+02 0.000000e+00 0.000000e+00 3.500000e-01 1.316852e-01 1.316852e-01 +9.698600e+02 0.000000e+00 0.000000e+00 2.600000e-01 1.210098e-01 1.210098e-01 +9.839300e+02 0.000000e+00 0.000000e+00 1.600000e-01 1.104181e-01 1.104181e-01 +1.003910e+03 0.000000e+00 0.000000e+00 4.400000e-01 1.228697e-01 1.228697e-01 +1.010530e+03 0.000000e+00 0.000000e+00 6.100000e-01 1.064874e-01 1.064874e-01 +1.015770e+03 0.000000e+00 0.000000e+00 1.950000e+00 2.063710e-01 2.063710e-01 +1.016770e+03 0.000000e+00 0.000000e+00 2.950000e+00 2.385980e-01 2.385980e-01 +1.016910e+03 0.000000e+00 0.000000e+00 3.590000e+00 3.693199e-01 3.693199e-01 +1.017610e+03 0.000000e+00 0.000000e+00 3.970000e+00 2.985620e-01 2.985620e-01 +1.017770e+03 0.000000e+00 0.000000e+00 4.290000e+00 3.519300e-01 3.519300e-01 +1.018580e+03 0.000000e+00 0.000000e+00 5.720000e+00 4.692401e-01 4.692401e-01 +1.018830e+03 0.000000e+00 0.000000e+00 5.460000e+00 3.690823e-01 3.690823e-01 +1.019500e+03 0.000000e+00 0.000000e+00 4.770000e+00 3.735110e-01 3.735110e-01 +1.019840e+03 0.000000e+00 0.000000e+00 4.540000e+00 5.870279e-01 5.870279e-01 +1.020620e+03 0.000000e+00 0.000000e+00 2.850000e+00 2.274665e-01 2.274665e-01 +1.021540e+03 0.000000e+00 0.000000e+00 1.520000e+00 1.929182e-01 1.929182e-01 +1.022790e+03 0.000000e+00 0.000000e+00 7.800000e-01 1.381674e-01 1.381674e-01 +1.027670e+03 0.000000e+00 0.000000e+00 8.000000e-02 8.014387e-02 8.014387e-02 +1.163400e+03 0.000000e+00 0.000000e+00 8.000000e-02 4.028697e-02 4.028697e-02 +1.310000e+03 0.000000e+00 0.000000e+00 5.000000e-02 2.022375e-02 2.022375e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2006_I728191.cc b/analyses/pluginNovosibirsk/CMD2_2006_I728191.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2006_I728191.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2006_I728191 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2006_I728191); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter2D temphisto(refData(3, 1, 1)); + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2DPtr mult = bookScatter2D(3, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2006_I728191); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2006_I728191.info b/analyses/pluginNovosibirsk/CMD2_2006_I728191.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2006_I728191.info @@ -0,0 +1,34 @@ +Name: CMD2_2006_I728191 +Year: 2006 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ between 370 and 520 MeV +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 728191 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- JETP Lett. 84 (2006) 413-417, 2006 +RunInfo: e+ e- to hadrons below 0.6 and 0.9 GeV +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies between 370 and 520 MeV. Useful for comparing models of the pion form factor.' +Keywords: +BibKey: Akhmetshin:2006wh +BibTeX: '@article{Akhmetshin:2006wh, + author = "Akhmetshin, R. R. and others", + title = "{Measurement of the e+ e- ---> pi+ pi- cross section with + the CMD2 detector in the 370 - 520-MeV c.m. energy + range}", + journal = "JETP Lett.", + volume = "84", + year = "2006", + pages = "413-417", + doi = "10.1134/S0021364006200021", + note = "[Pisma Zh. Eksp. Teor. Fiz.84,491(2006)]", + eprint = "hep-ex/0610016", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0610016;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2006_I728191.plot b/analyses/pluginNovosibirsk/CMD2_2006_I728191.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2006_I728191.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /CMD2_2006_I728191/d03-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +LogY=0 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2006_I728191.yoda b/analyses/pluginNovosibirsk/CMD2_2006_I728191.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2006_I728191.yoda @@ -0,0 +1,54 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2006_I728191/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2006_I728191/d01-x01-y01 +Title: doi:10.17182/hepdata.41786.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.700000e+02 0.000000e+00 0.000000e+00 6.050000e+02 1.655099e+01 1.655099e+01 +3.900000e+02 0.000000e+00 0.000000e+00 5.230000e+02 1.738974e+01 1.738974e+01 +4.100000e+02 0.000000e+00 0.000000e+00 4.760000e+02 1.928995e+01 1.928995e+01 +4.300000e+02 0.000000e+00 0.000000e+00 4.680000e+02 1.437818e+01 1.437818e+01 +4.500000e+02 0.000000e+00 0.000000e+00 4.120000e+02 1.724290e+01 1.724290e+01 +4.700000e+02 0.000000e+00 0.000000e+00 3.730000e+02 1.621164e+01 1.621164e+01 +4.800000e+02 0.000000e+00 0.000000e+00 3.290000e+02 2.112590e+01 2.112590e+01 +5.000000e+02 0.000000e+00 0.000000e+00 3.430000e+02 2.511503e+01 2.511503e+01 +5.100000e+02 0.000000e+00 0.000000e+00 3.360000e+02 2.610617e+01 2.610617e+01 +5.200000e+02 0.000000e+00 0.000000e+00 3.270000e+02 2.510457e+01 2.510457e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2006_I728191/d02-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2006_I728191/d02-x01-y01 +Title: doi:10.17182/hepdata.41786.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.700000e+02 0.000000e+00 0.000000e+00 2.050000e+00 1.208550e-01 1.208550e-01 +3.900000e+02 0.000000e+00 0.000000e+00 1.830000e+00 1.206818e-01 1.206818e-01 +4.100000e+02 0.000000e+00 0.000000e+00 1.980000e+00 1.406844e-01 1.406844e-01 +4.300000e+02 0.000000e+00 0.000000e+00 2.520000e+00 1.114054e-01 1.114054e-01 +4.500000e+02 0.000000e+00 0.000000e+00 2.690000e+00 1.511773e-01 1.511773e-01 +4.700000e+02 0.000000e+00 0.000000e+00 2.830000e+00 1.413946e-01 1.413946e-01 +4.800000e+02 0.000000e+00 0.000000e+00 3.020000e+00 2.011141e-01 2.011141e-01 +5.000000e+02 0.000000e+00 0.000000e+00 3.240000e+00 2.410692e-01 2.410692e-01 +5.100000e+02 0.000000e+00 0.000000e+00 3.830000e+00 2.514334e-01 2.514334e-01 +5.200000e+02 0.000000e+00 0.000000e+00 3.520000e+00 2.114406e-01 2.114406e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2006_I728191/d03-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2006_I728191/d03-x01-y01 +Title: doi:10.17182/hepdata.41786.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.700000e+02 0.000000e+00 0.000000e+00 9.180000e+01 5.636749e+00 5.636749e+00 +3.900000e+02 0.000000e+00 0.000000e+00 8.900000e+01 5.932801e+00 5.932801e+00 +4.100000e+02 0.000000e+00 0.000000e+00 1.000000e+02 7.034913e+00 7.034913e+00 +4.300000e+02 0.000000e+00 0.000000e+00 1.297000e+02 5.969446e+00 5.969446e+00 +4.500000e+02 0.000000e+00 0.000000e+00 1.385000e+02 7.562402e+00 7.562402e+00 +4.700000e+02 0.000000e+00 0.000000e+00 1.442000e+02 7.369456e+00 7.369456e+00 +4.800000e+02 0.000000e+00 0.000000e+00 1.524000e+02 1.035510e+01 1.035510e+01 +5.000000e+02 0.000000e+00 0.000000e+00 1.602000e+02 1.175362e+01 1.175362e+01 +5.100000e+02 0.000000e+00 0.000000e+00 1.866000e+02 1.246861e+01 1.246861e+01 +5.200000e+02 0.000000e+00 0.000000e+00 1.692000e+02 1.036787e+01 1.036787e+01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2007_I728302.cc b/analyses/pluginNovosibirsk/CMD2_2007_I728302.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2007_I728302.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2007_I728302 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2007_I728302); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2DPtr mult = bookScatter2D(2, 1, 1); + Scatter2D temphisto(refData(2, 1, 1)); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2007_I728302); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2007_I728302.info b/analyses/pluginNovosibirsk/CMD2_2007_I728302.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2007_I728302.info @@ -0,0 +1,33 @@ +Name: CMD2_2007_I728302 +Year: 2007 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ between 600 and 970 MeV +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 728302 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Lett. B648 (2007) 28-38, 2007 +RunInfo: e+ e- to hadrons below 0.6 and 0.9 GeV +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies between 600 and 970 MeV. Useful for comparing models of the pion form factor.' +Keywords: +BibKey: Akhmetshin:2006bx +BibTeX: '@article{Akhmetshin:2006bx, + author = "Akhmetshin, R. R. and others", + title = "{High-statistics measurement of the pion form factor in + the rho-meson energy range with the CMD2 detector}", + collaboration = "CMD2", + journal = "Phys. Lett.", + volume = "B648", + year = "2007", + pages = "28-38", + doi = "10.1016/j.physletb.2007.01.073", + eprint = "hep-ex/0610021", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0610021;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2007_I728302.plot b/analyses/pluginNovosibirsk/CMD2_2007_I728302.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2007_I728302.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /CMD2_2007_I728302/d02-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +LogY=0 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2007_I728302.yoda b/analyses/pluginNovosibirsk/CMD2_2007_I728302.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2007_I728302.yoda @@ -0,0 +1,74 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2007_I728302/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2007_I728302/d01-x01-y01 +Title: doi:10.17182/hepdata.41782.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.000000e+02 0.000000e+00 0.000000e+00 7.890000e+00 3.359823e-01 3.359823e-01 +6.300000e+02 0.000000e+00 0.000000e+00 1.053000e+01 3.019874e-01 3.019874e-01 +6.600000e+02 0.000000e+00 0.000000e+00 1.421000e+01 3.585012e-01 3.585012e-01 +6.900000e+02 0.000000e+00 0.000000e+00 2.127000e+01 4.531605e-01 4.531605e-01 +7.200000e+02 0.000000e+00 0.000000e+00 3.196000e+01 4.831897e-01 4.831897e-01 +7.500000e+02 0.000000e+00 0.000000e+00 4.213000e+01 7.056883e-01 7.056883e-01 +7.600000e+02 0.000000e+00 0.000000e+00 4.362000e+01 9.003739e-01 9.003739e-01 +7.640000e+02 0.000000e+00 0.000000e+00 4.448000e+01 8.121097e-01 8.121097e-01 +7.700000e+02 0.000000e+00 0.000000e+00 4.417000e+01 8.200386e-01 8.200386e-01 +7.740000e+02 0.000000e+00 0.000000e+00 4.546000e+01 6.427777e-01 6.427777e-01 +7.780000e+02 0.000000e+00 0.000000e+00 4.452000e+01 5.506813e-01 5.506813e-01 +7.800000e+02 0.000000e+00 0.000000e+00 4.300000e+01 6.572184e-01 6.572184e-01 +7.810000e+02 0.000000e+00 0.000000e+00 4.140000e+01 6.249748e-01 6.249748e-01 +7.820000e+02 0.000000e+00 0.000000e+00 3.964000e+01 3.749201e-01 3.749201e-01 +7.830000e+02 0.000000e+00 0.000000e+00 3.646000e+01 5.113484e-01 5.113484e-01 +7.840000e+02 0.000000e+00 0.000000e+00 3.380000e+01 4.582752e-01 4.582752e-01 +7.860000e+02 0.000000e+00 0.000000e+00 3.125000e+01 4.548626e-01 4.548626e-01 +7.900000e+02 0.000000e+00 0.000000e+00 3.105000e+01 6.586369e-01 6.586369e-01 +7.940000e+02 0.000000e+00 0.000000e+00 3.061000e+01 5.388564e-01 5.388564e-01 +8.000000e+02 0.000000e+00 0.000000e+00 2.982000e+01 4.571771e-01 4.571771e-01 +8.100000e+02 0.000000e+00 0.000000e+00 2.678000e+01 4.362325e-01 4.362325e-01 +8.200000e+02 0.000000e+00 0.000000e+00 2.344000e+01 3.205679e-01 3.205679e-01 +8.400000e+02 0.000000e+00 0.000000e+00 1.789000e+01 2.459336e-01 2.459336e-01 +8.800000e+02 0.000000e+00 0.000000e+00 1.037000e+01 1.714128e-01 1.714128e-01 +9.200000e+02 0.000000e+00 0.000000e+00 6.760000e+00 1.049983e-01 1.049983e-01 +9.400000e+02 0.000000e+00 0.000000e+00 5.200000e+00 1.270061e-01 1.270061e-01 +9.500000e+02 0.000000e+00 0.000000e+00 4.750000e+00 1.069766e-01 1.069766e-01 +9.580000e+02 0.000000e+00 0.000000e+00 4.260000e+00 9.623641e-02 9.623641e-02 +9.700000e+02 0.000000e+00 0.000000e+00 3.940000e+00 9.535990e-02 9.535990e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2007_I728302/d02-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2007_I728302/d02-x01-y01 +Title: doi:10.17182/hepdata.41782.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.000000e+02 0.000000e+00 0.000000e+00 3.301000e+02 1.395220e+01 1.395220e+01 +6.300000e+02 0.000000e+00 0.000000e+00 4.156000e+02 1.197098e+01 1.197098e+01 +6.600000e+02 0.000000e+00 0.000000e+00 5.291000e+02 1.338681e+01 1.338681e+01 +6.900000e+02 0.000000e+00 0.000000e+00 7.464000e+02 1.586648e+01 1.586648e+01 +7.200000e+02 0.000000e+00 0.000000e+00 1.053600e+03 1.591523e+01 1.591523e+01 +7.500000e+02 0.000000e+00 0.000000e+00 1.296600e+03 2.164705e+01 2.164705e+01 +7.600000e+02 0.000000e+00 0.000000e+00 1.311400e+03 2.711209e+01 2.711209e+01 +7.640000e+02 0.000000e+00 0.000000e+00 1.325800e+03 2.415338e+01 2.415338e+01 +7.700000e+02 0.000000e+00 0.000000e+00 1.302000e+03 2.407038e+01 2.407038e+01 +7.740000e+02 0.000000e+00 0.000000e+00 1.332200e+03 1.872817e+01 1.872817e+01 +7.780000e+02 0.000000e+00 0.000000e+00 1.296000e+03 1.601048e+01 1.601048e+01 +7.800000e+02 0.000000e+00 0.000000e+00 1.237500e+03 1.881515e+01 1.881515e+01 +7.810000e+02 0.000000e+00 0.000000e+00 1.178300e+03 1.788567e+01 1.788567e+01 +7.820000e+02 0.000000e+00 0.000000e+00 1.111700e+03 1.050981e+01 1.050981e+01 +7.830000e+02 0.000000e+00 0.000000e+00 1.007000e+03 1.420525e+01 1.420525e+01 +7.840000e+02 0.000000e+00 0.000000e+00 9.224000e+02 1.250850e+01 1.250850e+01 +7.860000e+02 0.000000e+00 0.000000e+00 8.441000e+02 1.223276e+01 1.223276e+01 +7.900000e+02 0.000000e+00 0.000000e+00 8.366000e+02 1.771309e+01 1.771309e+01 +7.940000e+02 0.000000e+00 0.000000e+00 8.225000e+02 1.439223e+01 1.439223e+01 +8.000000e+02 0.000000e+00 0.000000e+00 7.948000e+02 1.218972e+01 1.218972e+01 +8.100000e+02 0.000000e+00 0.000000e+00 7.016000e+02 1.138040e+01 1.138040e+01 +8.200000e+02 0.000000e+00 0.000000e+00 6.029000e+02 8.174549e+00 8.174549e+00 +8.400000e+02 0.000000e+00 0.000000e+00 4.433000e+02 6.211840e+00 6.211840e+00 +8.800000e+02 0.000000e+00 0.000000e+00 2.390000e+02 3.900736e+00 3.900736e+00 +9.200000e+02 0.000000e+00 0.000000e+00 1.454000e+02 2.313663e+00 2.313663e+00 +9.400000e+02 0.000000e+00 0.000000e+00 1.080000e+02 2.645089e+00 2.645089e+00 +9.500000e+02 0.000000e+00 0.000000e+00 9.720000e+01 2.239344e+00 2.239344e+00 +9.580000e+02 0.000000e+00 0.000000e+00 8.600000e+01 1.927004e+00 1.927004e+00 +9.700000e+02 0.000000e+00 0.000000e+00 7.800000e+01 1.905092e+00 1.905092e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD2_2008_I782516.cc b/analyses/pluginNovosibirsk/CMD2_2008_I782516.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2008_I782516.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD2_2008_I782516 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD2_2008_I782516); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nkaon = bookCounter("TMP/kaon"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::KPLUS) vetoEvent; + } + _nkaon->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nkaon->val(); + double error = _nkaon->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nkaon; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD2_2008_I782516); + + +} diff --git a/analyses/pluginNovosibirsk/CMD2_2008_I782516.info b/analyses/pluginNovosibirsk/CMD2_2008_I782516.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2008_I782516.info @@ -0,0 +1,34 @@ +Name: CMD2_2008_I782516 +Year: 2008 +Summary: Cross section for $e^+e^-\to K^+K^-$ near the $\phi$ mass +Experiment: CMD2 +Collider: VEPP-2M +InspireID: 782516 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Lett. B669 (2008) 217-222, 2008 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-$ at near the $\phi$ mass.' +Keywords: +BibKey: Akhmetshin:2008gz +BibTeX: '@article{Akhmetshin:2008gz, + author = "Akhmetshin, R. R. and others", + title = "{Measurement of $e^+e^- \to \phi \to K^+K^-$ cross + section with the CMD-2 detector at VEPP-2M Collider}", + collaboration = "CMD-2", + journal = "Phys. Lett.", + volume = "B669", + year = "2008", + pages = "217-222", + doi = "10.1016/j.physletb.2008.09.053", + eprint = "0804.0178", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + reportNumber = "0804.0146", + SLACcitation = "%%CITATION = ARXIV:0804.0178;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD2_2008_I782516.plot b/analyses/pluginNovosibirsk/CMD2_2008_I782516.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2008_I782516.plot @@ -0,0 +1,12 @@ +BEGIN PLOT /CMD2_2008_I782516/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD2_2008_I782516/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD2_2008_I782516.yoda b/analyses/pluginNovosibirsk/CMD2_2008_I782516.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD2_2008_I782516.yoda @@ -0,0 +1,37 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2008_I782516/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2008_I782516/d01-x01-y01 +Title: doi:10.17182/hepdata.50887.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.011570e+03 2.600000e-01 2.600000e-01 8.357000e+01 6.170278e+00 6.170278e+00 +1.016120e+03 3.000000e-02 3.000000e-02 5.492000e+02 1.420511e+01 1.420511e+01 +1.017020e+03 2.000000e-02 2.000000e-02 8.534500e+02 2.142996e+01 2.142996e+01 +1.017970e+03 2.000000e-02 2.000000e-02 1.389780e+03 3.308489e+01 3.308489e+01 +1.019200e+03 2.000000e-02 2.000000e-02 2.020040e+03 4.601690e+01 4.601690e+01 +1.020100e+03 2.000000e-02 2.000000e-02 1.825510e+03 4.247579e+01 4.247579e+01 +1.020970e+03 2.000000e-02 2.000000e-02 1.333870e+03 3.214454e+01 3.214454e+01 +1.021810e+03 3.000000e-02 3.000000e-02 9.175700e+02 2.372231e+01 2.372231e+01 +1.022750e+03 5.000000e-02 5.000000e-02 6.261600e+02 2.044693e+01 2.044693e+01 +1.028330e+03 2.600000e-01 2.600000e-01 1.438000e+02 1.087053e+01 1.087053e+01 +1.034060e+03 2.600000e-01 2.600000e-01 7.050000e+01 7.697870e+00 7.697870e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD2_2008_I782516/d02-x01-y01 +IsRef: 1 +Path: /REF/CMD2_2008_I782516/d02-x01-y01 +Title: doi:10.17182/hepdata.50887.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.011360e+03 2.600000e-01 2.600000e-01 7.572000e+01 6.053711e+00 6.053711e+00 +1.016020e+03 3.000000e-02 3.000000e-02 5.037600e+02 1.545379e+01 1.545379e+01 +1.017090e+03 2.000000e-02 2.000000e-02 8.890800e+02 2.230957e+01 2.230957e+01 +1.018020e+03 5.000000e-02 5.000000e-02 1.423230e+03 4.039372e+01 4.039372e+01 +1.018890e+03 2.000000e-02 2.000000e-02 1.951230e+03 4.966621e+01 4.966621e+01 +1.019680e+03 2.000000e-02 2.000000e-02 1.971870e+03 4.514890e+01 4.514890e+01 +1.020720e+03 3.000000e-02 3.000000e-02 1.435030e+03 3.642603e+01 3.642603e+01 +1.021740e+03 3.000000e-02 3.000000e-02 9.336900e+02 2.510309e+01 2.510309e+01 +1.022670e+03 4.000000e-02 4.000000e-02 6.065500e+02 2.160382e+01 2.160382e+01 +1.028580e+03 3.000000e-02 3.000000e-02 1.581000e+02 1.264767e+01 1.264767e+01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1385598.cc b/analyses/pluginNovosibirsk/CMD3_2016_I1385598.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1385598.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD3_2016_I1385598 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD3_2016_I1385598); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nproton = bookCounter("TMP/proton"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PROTON) vetoEvent; + } + _nproton->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nproton->val(); + double error = _nproton->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 6)); + Scatter2DPtr mult = bookScatter2D(1, 1, 6); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nproton; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD3_2016_I1385598); + + +} diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1385598.info b/analyses/pluginNovosibirsk/CMD3_2016_I1385598.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1385598.info @@ -0,0 +1,36 @@ +Name: CMD3_2016_I1385598 +Year: 2016 +Summary: Cross section for $e^+e^-\to p\bar{p}$ between the threshold and 2 GeV +Experiment: CMD3 +Collider: VEPP-2M +InspireID: 1385598 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B759 (2016) 634-640, 2016 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ between the threshold and 2 GeV.' +Keywords: [] +BibKey: Akhmetshin:2015ifg +BibTeX: '@article{Akhmetshin:2015ifg, + author = "Akhmetshin, R. R. and others", + title = "{Study of the process $e^+e^-\to p\bar{p}$ in the c.m. + energy range from threshold to 2 GeV with the CMD-3 + detector}", + collaboration = "CMD-3", + journal = "Phys. Lett.", + volume = "B759", + year = "2016", + pages = "634-640", + doi = "10.1016/j.physletb.2016.04.048", + eprint = "1507.08013", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1507.08013;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1385598.plot b/analyses/pluginNovosibirsk/CMD3_2016_I1385598.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1385598.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /CMD3_2016_I1385598/d01-x01-y06 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1385598.yoda b/analyses/pluginNovosibirsk/CMD3_2016_I1385598.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1385598.yoda @@ -0,0 +1,17 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1385598/d01-x01-y06 +IsRef: 1 +Path: /REF/CMD3_2016_I1385598/d01-x01-y06 +Title: doi:10.17182/hepdata.73805.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.900000e+03 1.000000e+01 1.000000e+01 1.200000e+00 2.952965e-01 2.952965e-01 +1.920000e+03 1.000000e+01 2.500000e+00 8.700000e-01 7.071068e-02 7.071068e-02 +1.925000e+03 2.500000e+00 7.500000e+00 9.000000e-01 7.071068e-02 7.071068e-02 +1.940000e+03 7.500000e+00 5.000000e+00 8.700000e-01 7.071068e-02 7.071068e-02 +1.950000e+03 5.000000e+00 5.000000e+00 8.900000e-01 7.810250e-02 7.810250e-02 +1.960000e+03 5.000000e+00 7.500000e+00 9.600000e-01 8.485281e-02 8.485281e-02 +1.975000e+03 7.500000e+00 2.500000e+00 9.000000e-01 7.071068e-02 7.071068e-02 +1.980000e+03 2.500000e+00 1.000000e+01 9.800000e-01 7.810250e-02 7.810250e-02 +2.000000e+03 1.000000e+01 1.000000e+01 9.500000e-01 8.485281e-02 8.485281e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1395968.cc b/analyses/pluginNovosibirsk/CMD3_2016_I1395968.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1395968.cc @@ -0,0 +1,85 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD3_2016_I1395968 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD3_2016_I1395968); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + _cKpKmpippim = bookCounter("TMP/KpKmpippim"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + if(ntotal!=4) vetoEvent; + if(nCount[321]==1 && nCount[-321]==1 && nCount[211]==1 && nCount[-211]==1) + _cKpKmpippim->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _cKpKmpippim->val(); + double error = _cKpKmpippim->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 6)); + Scatter2DPtr mult = bookScatter2D(1, 1, 6); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _cKpKmpippim; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD3_2016_I1395968); + + +} diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1395968.info b/analyses/pluginNovosibirsk/CMD3_2016_I1395968.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1395968.info @@ -0,0 +1,35 @@ +Name: CMD3_2016_I1395968 +Year: 2016 +Summary: Cross section for $e^+e^-\to K^+K^-\pi^+\pi^-$ between 1.44 and 2.01 GeV +Experiment: CMD3 +Collider: VEPP-2M +InspireID: 1395968 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B759 (2016) 634-640, 2016 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-\pi^+\pi^-$ between 1.44 and 2.01 GeV.' +Keywords: [] +BibKey: Shemyakin:2015cba +BibTeX: '@article{Shemyakin:2015cba, + author = "Shemyakin, D. N. and others", + title = "{Measurement of the $e^+e^- \to K^+K^-\pi^+\pi^-$ cross + section with the CMD-3 detector at the VEPP-2000 + collider}", + journal = "Phys. Lett.", + volume = "B756", + year = "2016", + pages = "153-160", + doi = "10.1016/j.physletb.2016.02.072", + eprint = "1510.00654", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1510.00654;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1395968.plot b/analyses/pluginNovosibirsk/CMD3_2016_I1395968.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1395968.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /CMD3_2016_I1395968/d01-x01-y06 +Title=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1395968.yoda b/analyses/pluginNovosibirsk/CMD3_2016_I1395968.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1395968.yoda @@ -0,0 +1,258 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1395968/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD3_2016_I1395968/d01-x01-y01 +Title: doi:10.17182/hepdata.76553.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.434900e+03 6.000000e+00 6.000000e+00 9.273000e+02 0.000000e+00 0.000000e+00 +1.494100e+03 6.000000e+00 6.000000e+00 5.568000e+02 0.000000e+00 0.000000e+00 +1.514600e+03 2.000000e+00 2.000000e+00 8.474000e+02 0.000000e+00 0.000000e+00 +1.522400e+03 6.000000e+00 6.000000e+00 5.395000e+02 0.000000e+00 0.000000e+00 +1.543200e+03 6.000000e+00 6.000000e+00 5.120000e+02 0.000000e+00 0.000000e+00 +1.571900e+03 6.000000e+00 6.000000e+00 5.220000e+02 0.000000e+00 0.000000e+00 +1.593800e+03 6.000000e+00 6.000000e+00 4.498000e+02 0.000000e+00 0.000000e+00 +1.595000e+03 2.000000e+00 2.000000e+00 8.327000e+02 0.000000e+00 0.000000e+00 +1.622900e+03 6.000000e+00 6.000000e+00 5.178000e+02 0.000000e+00 0.000000e+00 +1.643000e+03 6.000000e+00 6.000000e+00 4.627000e+02 0.000000e+00 0.000000e+00 +1.669400e+03 6.000000e+00 6.000000e+00 5.722000e+02 0.000000e+00 0.000000e+00 +1.674100e+03 2.000000e+00 2.000000e+00 8.947000e+02 0.000000e+00 0.000000e+00 +1.692800e+03 6.000000e+00 6.000000e+00 4.942000e+02 0.000000e+00 0.000000e+00 +1.715800e+03 2.000000e+00 2.000000e+00 8.121000e+02 0.000000e+00 0.000000e+00 +1.723100e+03 6.000000e+00 6.000000e+00 5.307000e+02 0.000000e+00 0.000000e+00 +1.741600e+03 6.000000e+00 6.000000e+00 5.423000e+02 0.000000e+00 0.000000e+00 +1.757700e+03 2.000000e+00 2.000000e+00 9.719000e+02 0.000000e+00 0.000000e+00 +1.773700e+03 6.000000e+00 6.000000e+00 5.606000e+02 0.000000e+00 0.000000e+00 +1.792900e+03 6.000000e+00 6.000000e+00 4.491000e+02 0.000000e+00 0.000000e+00 +1.798000e+03 2.000000e+00 2.000000e+00 9.984000e+02 0.000000e+00 0.000000e+00 +1.826400e+03 6.000000e+00 6.000000e+00 5.138000e+02 0.000000e+00 0.000000e+00 +1.840000e+03 2.000000e+00 2.000000e+00 9.660000e+02 0.000000e+00 0.000000e+00 +1.848600e+03 6.000000e+00 6.000000e+00 4.354000e+02 0.000000e+00 0.000000e+00 +1.871100e+03 6.000000e+00 6.000000e+00 6.710000e+02 0.000000e+00 0.000000e+00 +1.874200e+03 2.000000e+00 2.000000e+00 8.556000e+02 0.000000e+00 0.000000e+00 +1.893400e+03 6.000000e+00 6.000000e+00 5.271000e+02 0.000000e+00 0.000000e+00 +1.901200e+03 6.000000e+00 6.000000e+00 4.986000e+02 0.000000e+00 0.000000e+00 +1.903200e+03 2.000000e+00 2.000000e+00 9.004000e+02 0.000000e+00 0.000000e+00 +1.926000e+03 6.000000e+00 6.000000e+00 5.669000e+02 0.000000e+00 0.000000e+00 +1.927000e+03 6.000000e+00 6.000000e+00 5.908000e+02 0.000000e+00 0.000000e+00 +1.944800e+03 2.000000e+00 2.000000e+00 9.938000e+02 0.000000e+00 0.000000e+00 +1.952600e+03 6.000000e+00 6.000000e+00 4.510000e+02 0.000000e+00 0.000000e+00 +1.966900e+03 2.000000e+00 2.000000e+00 6.922000e+02 0.000000e+00 0.000000e+00 +1.978400e+03 6.000000e+00 6.000000e+00 5.066000e+02 0.000000e+00 0.000000e+00 +1.988600e+03 2.000000e+00 2.000000e+00 6.006000e+02 0.000000e+00 0.000000e+00 +2.004600e+03 6.000000e+00 6.000000e+00 4.781000e+02 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1395968/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD3_2016_I1395968/d01-x01-y02 +Title: doi:10.17182/hepdata.76553.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.434900e+03 6.000000e+00 6.000000e+00 2.000000e+00 0.000000e+00 0.000000e+00 +1.494100e+03 6.000000e+00 6.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +1.514600e+03 2.000000e+00 2.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 +1.522400e+03 6.000000e+00 6.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 +1.543200e+03 6.000000e+00 6.000000e+00 3.000000e+00 0.000000e+00 0.000000e+00 +1.571900e+03 6.000000e+00 6.000000e+00 7.000000e+00 0.000000e+00 0.000000e+00 +1.593800e+03 6.000000e+00 6.000000e+00 1.600000e+01 0.000000e+00 0.000000e+00 +1.595000e+03 2.000000e+00 2.000000e+00 3.900000e+01 0.000000e+00 0.000000e+00 +1.622900e+03 6.000000e+00 6.000000e+00 3.100000e+01 0.000000e+00 0.000000e+00 +1.643000e+03 6.000000e+00 6.000000e+00 7.200000e+01 0.000000e+00 0.000000e+00 +1.669400e+03 6.000000e+00 6.000000e+00 1.110000e+02 0.000000e+00 0.000000e+00 +1.674100e+03 2.000000e+00 2.000000e+00 2.200000e+02 0.000000e+00 0.000000e+00 +1.692800e+03 6.000000e+00 6.000000e+00 1.320000e+02 0.000000e+00 0.000000e+00 +1.715800e+03 2.000000e+00 2.000000e+00 2.570000e+02 0.000000e+00 0.000000e+00 +1.723100e+03 6.000000e+00 6.000000e+00 1.850000e+02 0.000000e+00 0.000000e+00 +1.741600e+03 6.000000e+00 6.000000e+00 2.080000e+02 0.000000e+00 0.000000e+00 +1.757700e+03 2.000000e+00 2.000000e+00 4.590000e+02 0.000000e+00 0.000000e+00 +1.773700e+03 6.000000e+00 6.000000e+00 2.970000e+02 0.000000e+00 0.000000e+00 +1.792900e+03 6.000000e+00 6.000000e+00 2.890000e+02 0.000000e+00 0.000000e+00 +1.798000e+03 2.000000e+00 2.000000e+00 6.840000e+02 0.000000e+00 0.000000e+00 +1.826400e+03 6.000000e+00 6.000000e+00 3.830000e+02 0.000000e+00 0.000000e+00 +1.840000e+03 2.000000e+00 2.000000e+00 7.210000e+02 0.000000e+00 0.000000e+00 +1.848600e+03 6.000000e+00 6.000000e+00 3.110000e+02 0.000000e+00 0.000000e+00 +1.871100e+03 6.000000e+00 6.000000e+00 4.970000e+02 0.000000e+00 0.000000e+00 +1.874200e+03 2.000000e+00 2.000000e+00 6.590000e+02 0.000000e+00 0.000000e+00 +1.893400e+03 6.000000e+00 6.000000e+00 3.810000e+02 0.000000e+00 0.000000e+00 +1.901200e+03 6.000000e+00 6.000000e+00 3.510000e+02 0.000000e+00 0.000000e+00 +1.903200e+03 2.000000e+00 2.000000e+00 6.820000e+02 0.000000e+00 0.000000e+00 +1.926000e+03 6.000000e+00 6.000000e+00 4.200000e+02 0.000000e+00 0.000000e+00 +1.927000e+03 6.000000e+00 6.000000e+00 4.410000e+02 0.000000e+00 0.000000e+00 +1.944800e+03 2.000000e+00 2.000000e+00 7.350000e+02 0.000000e+00 0.000000e+00 +1.952600e+03 6.000000e+00 6.000000e+00 3.260000e+02 0.000000e+00 0.000000e+00 +1.966900e+03 2.000000e+00 2.000000e+00 5.100000e+02 0.000000e+00 0.000000e+00 +1.978400e+03 6.000000e+00 6.000000e+00 3.530000e+02 0.000000e+00 0.000000e+00 +1.988600e+03 2.000000e+00 2.000000e+00 4.450000e+02 0.000000e+00 0.000000e+00 +2.004600e+03 6.000000e+00 6.000000e+00 3.130000e+02 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1395968/d01-x01-y03 +IsRef: 1 +Path: /REF/CMD3_2016_I1395968/d01-x01-y03 +Title: doi:10.17182/hepdata.76553.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.593800e+03 6.000000e+00 6.000000e+00 3.520000e+01 0.000000e+00 0.000000e+00 +1.595000e+03 2.000000e+00 2.000000e+00 3.580000e+01 0.000000e+00 0.000000e+00 +1.622900e+03 6.000000e+00 6.000000e+00 5.260000e+01 0.000000e+00 0.000000e+00 +1.643000e+03 6.000000e+00 6.000000e+00 6.290000e+01 0.000000e+00 0.000000e+00 +1.669400e+03 6.000000e+00 6.000000e+00 1.681000e+02 0.000000e+00 0.000000e+00 +1.674100e+03 2.000000e+00 2.000000e+00 2.735000e+02 0.000000e+00 0.000000e+00 +1.692800e+03 6.000000e+00 6.000000e+00 1.666000e+02 0.000000e+00 0.000000e+00 +1.715800e+03 2.000000e+00 2.000000e+00 3.988000e+02 0.000000e+00 0.000000e+00 +1.723100e+03 6.000000e+00 6.000000e+00 2.350000e+02 0.000000e+00 0.000000e+00 +1.741600e+03 6.000000e+00 6.000000e+00 2.699000e+02 0.000000e+00 0.000000e+00 +1.757700e+03 2.000000e+00 2.000000e+00 6.355000e+02 0.000000e+00 0.000000e+00 +1.773700e+03 6.000000e+00 6.000000e+00 3.969000e+02 0.000000e+00 0.000000e+00 +1.792900e+03 6.000000e+00 6.000000e+00 3.886000e+02 0.000000e+00 0.000000e+00 +1.798000e+03 2.000000e+00 2.000000e+00 8.654000e+02 0.000000e+00 0.000000e+00 +1.826400e+03 6.000000e+00 6.000000e+00 4.630000e+02 0.000000e+00 0.000000e+00 +1.840000e+03 2.000000e+00 2.000000e+00 1.007600e+03 0.000000e+00 0.000000e+00 +1.848600e+03 6.000000e+00 6.000000e+00 3.958000e+02 0.000000e+00 0.000000e+00 +1.871100e+03 6.000000e+00 6.000000e+00 6.583000e+02 0.000000e+00 0.000000e+00 +1.874200e+03 2.000000e+00 2.000000e+00 7.230000e+02 0.000000e+00 0.000000e+00 +1.893400e+03 6.000000e+00 6.000000e+00 4.591000e+02 0.000000e+00 0.000000e+00 +1.901200e+03 6.000000e+00 6.000000e+00 4.710000e+02 0.000000e+00 0.000000e+00 +1.903200e+03 2.000000e+00 2.000000e+00 8.410000e+02 0.000000e+00 0.000000e+00 +1.926000e+03 6.000000e+00 6.000000e+00 5.691000e+02 0.000000e+00 0.000000e+00 +1.927000e+03 6.000000e+00 6.000000e+00 5.322000e+02 0.000000e+00 0.000000e+00 +1.944800e+03 2.000000e+00 2.000000e+00 8.989000e+02 0.000000e+00 0.000000e+00 +1.952600e+03 6.000000e+00 6.000000e+00 3.900000e+02 0.000000e+00 0.000000e+00 +1.966900e+03 2.000000e+00 2.000000e+00 6.506000e+02 0.000000e+00 0.000000e+00 +1.978400e+03 6.000000e+00 6.000000e+00 4.120000e+02 0.000000e+00 0.000000e+00 +1.988600e+03 2.000000e+00 2.000000e+00 5.077000e+02 0.000000e+00 0.000000e+00 +2.004600e+03 6.000000e+00 6.000000e+00 3.805000e+02 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1395968/d01-x01-y04 +IsRef: 1 +Path: /REF/CMD3_2016_I1395968/d01-x01-y04 +Title: doi:10.17182/hepdata.76553.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.434900e+03 6.000000e+00 6.000000e+00 1.200000e-01 0.000000e+00 0.000000e+00 +1.494100e+03 6.000000e+00 6.000000e+00 1.200000e-01 0.000000e+00 0.000000e+00 +1.514600e+03 2.000000e+00 2.000000e+00 1.210000e-01 0.000000e+00 0.000000e+00 +1.522400e+03 6.000000e+00 6.000000e+00 1.210000e-01 0.000000e+00 0.000000e+00 +1.543200e+03 6.000000e+00 6.000000e+00 1.280000e-01 0.000000e+00 0.000000e+00 +1.571900e+03 6.000000e+00 6.000000e+00 1.360000e-01 0.000000e+00 0.000000e+00 +1.593800e+03 6.000000e+00 6.000000e+00 3.540000e-01 0.000000e+00 0.000000e+00 +1.595000e+03 2.000000e+00 2.000000e+00 3.560000e-01 0.000000e+00 0.000000e+00 +1.622900e+03 6.000000e+00 6.000000e+00 3.780000e-01 0.000000e+00 0.000000e+00 +1.643000e+03 6.000000e+00 6.000000e+00 3.930000e-01 0.000000e+00 0.000000e+00 +1.669400e+03 6.000000e+00 6.000000e+00 4.090000e-01 0.000000e+00 0.000000e+00 +1.674100e+03 2.000000e+00 2.000000e+00 4.150000e-01 0.000000e+00 0.000000e+00 +1.692800e+03 6.000000e+00 6.000000e+00 4.210000e-01 0.000000e+00 0.000000e+00 +1.715800e+03 2.000000e+00 2.000000e+00 4.280000e-01 0.000000e+00 0.000000e+00 +1.723100e+03 6.000000e+00 6.000000e+00 4.230000e-01 0.000000e+00 0.000000e+00 +1.741600e+03 6.000000e+00 6.000000e+00 4.220000e-01 0.000000e+00 0.000000e+00 +1.757700e+03 2.000000e+00 2.000000e+00 4.310000e-01 0.000000e+00 0.000000e+00 +1.773700e+03 6.000000e+00 6.000000e+00 4.250000e-01 0.000000e+00 0.000000e+00 +1.792900e+03 6.000000e+00 6.000000e+00 4.280000e-01 0.000000e+00 0.000000e+00 +1.798000e+03 2.000000e+00 2.000000e+00 4.360000e-01 0.000000e+00 0.000000e+00 +1.826400e+03 6.000000e+00 6.000000e+00 4.290000e-01 0.000000e+00 0.000000e+00 +1.840000e+03 2.000000e+00 2.000000e+00 4.380000e-01 0.000000e+00 0.000000e+00 +1.848600e+03 6.000000e+00 6.000000e+00 4.290000e-01 0.000000e+00 0.000000e+00 +1.871100e+03 6.000000e+00 6.000000e+00 4.240000e-01 0.000000e+00 0.000000e+00 +1.874200e+03 2.000000e+00 2.000000e+00 4.360000e-01 0.000000e+00 0.000000e+00 +1.893400e+03 6.000000e+00 6.000000e+00 4.200000e-01 0.000000e+00 0.000000e+00 +1.901200e+03 6.000000e+00 6.000000e+00 4.180000e-01 0.000000e+00 0.000000e+00 +1.903200e+03 2.000000e+00 2.000000e+00 4.310000e-01 0.000000e+00 0.000000e+00 +1.926000e+03 6.000000e+00 6.000000e+00 4.260000e-01 0.000000e+00 0.000000e+00 +1.927000e+03 6.000000e+00 6.000000e+00 4.130000e-01 0.000000e+00 0.000000e+00 +1.944800e+03 2.000000e+00 2.000000e+00 4.220000e-01 0.000000e+00 0.000000e+00 +1.952600e+03 6.000000e+00 6.000000e+00 4.070000e-01 0.000000e+00 0.000000e+00 +1.966900e+03 2.000000e+00 2.000000e+00 4.160000e-01 0.000000e+00 0.000000e+00 +1.978400e+03 6.000000e+00 6.000000e+00 3.980000e-01 0.000000e+00 0.000000e+00 +1.988600e+03 2.000000e+00 2.000000e+00 4.100000e-01 0.000000e+00 0.000000e+00 +2.004600e+03 6.000000e+00 6.000000e+00 3.900000e-01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1395968/d01-x01-y05 +IsRef: 1 +Path: /REF/CMD3_2016_I1395968/d01-x01-y05 +Title: doi:10.17182/hepdata.76553.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.434900e+03 6.000000e+00 6.000000e+00 8.150000e-01 0.000000e+00 0.000000e+00 +1.494100e+03 6.000000e+00 6.000000e+00 8.190000e-01 0.000000e+00 0.000000e+00 +1.514600e+03 2.000000e+00 2.000000e+00 8.210000e-01 0.000000e+00 0.000000e+00 +1.522400e+03 6.000000e+00 6.000000e+00 8.210000e-01 0.000000e+00 0.000000e+00 +1.543200e+03 6.000000e+00 6.000000e+00 8.230000e-01 0.000000e+00 0.000000e+00 +1.571900e+03 6.000000e+00 6.000000e+00 8.250000e-01 0.000000e+00 0.000000e+00 +1.593800e+03 6.000000e+00 6.000000e+00 8.270000e-01 0.000000e+00 0.000000e+00 +1.595000e+03 2.000000e+00 2.000000e+00 8.270000e-01 0.000000e+00 0.000000e+00 +1.622900e+03 6.000000e+00 6.000000e+00 8.240000e-01 0.000000e+00 0.000000e+00 +1.643000e+03 6.000000e+00 6.000000e+00 8.210000e-01 0.000000e+00 0.000000e+00 +1.669400e+03 6.000000e+00 6.000000e+00 8.320000e-01 0.000000e+00 0.000000e+00 +1.674100e+03 2.000000e+00 2.000000e+00 8.350000e-01 0.000000e+00 0.000000e+00 +1.692800e+03 6.000000e+00 6.000000e+00 8.500000e-01 0.000000e+00 0.000000e+00 +1.715800e+03 2.000000e+00 2.000000e+00 8.620000e-01 0.000000e+00 0.000000e+00 +1.723100e+03 6.000000e+00 6.000000e+00 8.630000e-01 0.000000e+00 0.000000e+00 +1.741600e+03 6.000000e+00 6.000000e+00 8.630000e-01 0.000000e+00 0.000000e+00 +1.757700e+03 2.000000e+00 2.000000e+00 8.640000e-01 0.000000e+00 0.000000e+00 +1.773700e+03 6.000000e+00 6.000000e+00 8.670000e-01 0.000000e+00 0.000000e+00 +1.792900e+03 6.000000e+00 6.000000e+00 8.730000e-01 0.000000e+00 0.000000e+00 +1.798000e+03 2.000000e+00 2.000000e+00 8.750000e-01 0.000000e+00 0.000000e+00 +1.826400e+03 6.000000e+00 6.000000e+00 8.890000e-01 0.000000e+00 0.000000e+00 +1.840000e+03 2.000000e+00 2.000000e+00 8.970000e-01 0.000000e+00 0.000000e+00 +1.848600e+03 6.000000e+00 6.000000e+00 9.030000e-01 0.000000e+00 0.000000e+00 +1.871100e+03 6.000000e+00 6.000000e+00 9.170000e-01 0.000000e+00 0.000000e+00 +1.874200e+03 2.000000e+00 2.000000e+00 9.190000e-01 0.000000e+00 0.000000e+00 +1.893400e+03 6.000000e+00 6.000000e+00 9.280000e-01 0.000000e+00 0.000000e+00 +1.901200e+03 6.000000e+00 6.000000e+00 9.300000e-01 0.000000e+00 0.000000e+00 +1.903200e+03 2.000000e+00 2.000000e+00 9.300000e-01 0.000000e+00 0.000000e+00 +1.926000e+03 6.000000e+00 6.000000e+00 9.330000e-01 0.000000e+00 0.000000e+00 +1.927000e+03 6.000000e+00 6.000000e+00 9.330000e-01 0.000000e+00 0.000000e+00 +1.944800e+03 2.000000e+00 2.000000e+00 9.350000e-01 0.000000e+00 0.000000e+00 +1.952600e+03 6.000000e+00 6.000000e+00 9.370000e-01 0.000000e+00 0.000000e+00 +1.966900e+03 2.000000e+00 2.000000e+00 9.420000e-01 0.000000e+00 0.000000e+00 +1.978400e+03 6.000000e+00 6.000000e+00 9.490000e-01 0.000000e+00 0.000000e+00 +1.988600e+03 2.000000e+00 2.000000e+00 9.560000e-01 0.000000e+00 0.000000e+00 +2.004600e+03 6.000000e+00 6.000000e+00 9.720000e-01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1395968/d01-x01-y06 +IsRef: 1 +Path: /REF/CMD3_2016_I1395968/d01-x01-y06 +Title: doi:10.17182/hepdata.76553.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.434900e+03 6.000000e+00 6.000000e+00 2.200000e-02 1.600000e-02 1.600000e-02 +1.494100e+03 6.000000e+00 6.000000e+00 1.800000e-02 1.800000e-02 1.800000e-02 +1.514600e+03 2.000000e+00 2.000000e+00 3.600000e-02 2.000000e-02 2.000000e-02 +1.522400e+03 6.000000e+00 6.000000e+00 1.900000e-02 1.900000e-02 1.900000e-02 +1.543200e+03 6.000000e+00 6.000000e+00 5.600000e-02 3.200000e-02 3.200000e-02 +1.571900e+03 6.000000e+00 6.000000e+00 1.190000e-01 4.500000e-02 4.500000e-02 +1.593800e+03 6.000000e+00 6.000000e+00 3.900000e-01 6.000000e-02 6.000000e-02 +1.595000e+03 2.000000e+00 2.000000e+00 2.900000e-01 3.000000e-02 3.000000e-02 +1.622900e+03 6.000000e+00 6.000000e+00 5.200000e-01 6.000000e-02 6.000000e-02 +1.643000e+03 6.000000e+00 6.000000e+00 8.700000e-01 8.000000e-02 8.000000e-02 +1.669400e+03 6.000000e+00 6.000000e+00 1.450000e+00 9.000000e-02 9.000000e-02 +1.674100e+03 2.000000e+00 2.000000e+00 1.640000e+00 7.000000e-02 7.000000e-02 +1.692800e+03 6.000000e+00 6.000000e+00 1.730000e+00 1.000000e-01 1.000000e-01 +1.715800e+03 2.000000e+00 2.000000e+00 2.240000e+00 9.000000e-02 9.000000e-02 +1.723100e+03 6.000000e+00 6.000000e+00 2.200000e+00 1.100000e-01 1.100000e-01 +1.741600e+03 6.000000e+00 6.000000e+00 2.470000e+00 1.100000e-01 1.100000e-01 +1.757700e+03 2.000000e+00 2.000000e+00 3.080000e+00 9.000000e-02 9.000000e-02 +1.773700e+03 6.000000e+00 6.000000e+00 3.430000e+00 1.300000e-01 1.300000e-01 +1.792900e+03 6.000000e+00 6.000000e+00 4.110000e+00 1.600000e-01 1.600000e-01 +1.798000e+03 2.000000e+00 2.000000e+00 4.140000e+00 1.100000e-01 1.100000e-01 +1.826400e+03 6.000000e+00 6.000000e+00 4.380000e+00 1.500000e-01 1.500000e-01 +1.840000e+03 2.000000e+00 2.000000e+00 4.630000e+00 1.100000e-01 1.100000e-01 +1.848600e+03 6.000000e+00 6.000000e+00 4.270000e+00 1.600000e-01 1.600000e-01 +1.871100e+03 6.000000e+00 6.000000e+00 4.500000e+00 1.300000e-01 1.300000e-01 +1.874200e+03 2.000000e+00 2.000000e+00 4.090000e+00 1.100000e-01 1.100000e-01 +1.893400e+03 6.000000e+00 6.000000e+00 4.170000e+00 1.400000e-01 1.400000e-01 +1.901200e+03 6.000000e+00 6.000000e+00 4.330000e+00 1.500000e-01 1.500000e-01 +1.903200e+03 2.000000e+00 2.000000e+00 4.310000e+00 1.100000e-01 1.100000e-01 +1.926000e+03 6.000000e+00 6.000000e+00 4.470000e+00 1.400000e-01 1.400000e-01 +1.927000e+03 6.000000e+00 6.000000e+00 4.350000e+00 1.400000e-01 1.400000e-01 +1.944800e+03 2.000000e+00 2.000000e+00 4.230000e+00 1.000000e-01 1.000000e-01 +1.952600e+03 6.000000e+00 6.000000e+00 4.230000e+00 1.600000e-01 1.600000e-01 +1.966900e+03 2.000000e+00 2.000000e+00 4.350000e+00 1.300000e-01 1.300000e-01 +1.978400e+03 6.000000e+00 6.000000e+00 4.050000e+00 1.500000e-01 1.500000e-01 +1.988600e+03 2.000000e+00 2.000000e+00 4.100000e+00 1.300000e-01 1.300000e-01 +2.004600e+03 6.000000e+00 6.000000e+00 3.880000e+00 1.500000e-01 1.500000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1444990.cc b/analyses/pluginNovosibirsk/CMD3_2016_I1444990.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1444990.cc @@ -0,0 +1,85 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD3_2016_I1444990 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD3_2016_I1444990); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + declare(FinalState(), "FS"); + _nK0K0 = bookCounter("TMP/K0K0"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && + nCount[130]==1 && nCount[310]==1) + _nK0K0->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nK0K0->val(); + double error = _nK0K0->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 6)); + Scatter2DPtr mult = bookScatter2D(1, 1, 6); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nK0K0; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD3_2016_I1444990); + + +} diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1444990.info b/analyses/pluginNovosibirsk/CMD3_2016_I1444990.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1444990.info @@ -0,0 +1,36 @@ +Name: CMD3_2016_I1444990 +Year: 2016 +Summary: Cross section for $e^+e^-\to K^0_SK^0_L$ at energies between 1.004 and 1.06 GeV +Experiment: CMD3 +Collider: VEPP-2M +InspireID: 1444990 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B760 (2016) 314-319, 2016 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to K^0_SK^0_L$ at energies between 1.004 and 1.06 GeV.' +Keywords: [] +BibKey: Kozyrev:2016raz +BibTeX: '@article{Kozyrev:2016raz, + author = "Kozyrev, E. A. and others", + title = "{Study of the process $e^+ e^- \to K^0_{S}K^0_{L}$ in the + center-of-mass energy range 1004--1060 MeV with the CMD-3 + detector at the VEPP-2000 $e^+ e^-$ collider}", + collaboration = "CMD-3", + journal = "Phys. Lett.", + volume = "B760", + year = "2016", + pages = "314-319", + doi = "10.1016/j.physletb.2016.07.003", + eprint = "1604.02981", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1604.02981;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1444990.plot b/analyses/pluginNovosibirsk/CMD3_2016_I1444990.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1444990.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /CMD3_2016_I1444990/d01-x01-y06 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD3_2016_I1444990.yoda b/analyses/pluginNovosibirsk/CMD3_2016_I1444990.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD3_2016_I1444990.yoda @@ -0,0 +1,198 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1444990/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD3_2016_I1444990/d01-x01-y01 +Title: doi:10.17182/hepdata.78538.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004066e+03 8.000000e-03 8.000000e-03 3.150000e+02 1.900000e+01 1.900000e+01 +1.010466e+03 1.000000e-02 1.000000e-02 9.083000e+03 1.000000e+02 1.000000e+02 +1.012955e+03 7.000000e-03 7.000000e-03 1.063900e+04 1.080000e+02 1.080000e+02 +1.015068e+03 1.200000e-02 1.200000e-02 2.347000e+03 5.000000e+01 5.000000e+01 +1.016105e+03 1.000000e-02 1.000000e-02 1.557400e+04 1.300000e+02 1.300000e+02 +1.017155e+03 1.200000e-02 1.200000e-02 6.561200e+04 2.640000e+02 2.640000e+02 +1.017156e+03 1.300000e-02 1.300000e-02 5.525000e+03 7.700000e+01 7.700000e+01 +1.018046e+03 2.100000e-02 2.100000e-02 1.022330e+05 3.340000e+02 3.340000e+02 +1.019118e+03 1.600000e-02 1.600000e-02 9.801400e+04 3.260000e+02 3.260000e+02 +1.019214e+03 1.900000e-02 1.900000e-02 1.605900e+04 1.320000e+02 1.320000e+02 +1.019421e+03 2.800000e-02 2.800000e-02 1.106600e+04 1.100000e+02 1.100000e+02 +1.019902e+03 1.200000e-02 1.200000e-02 1.407580e+05 3.860000e+02 3.860000e+02 +1.021222e+03 2.100000e-02 2.100000e-02 4.755200e+04 2.250000e+02 2.250000e+02 +1.021309e+03 9.000000e-03 9.000000e-03 9.545000e+03 1.020000e+02 1.020000e+02 +1.022078e+03 2.100000e-02 2.100000e-02 3.132300e+04 1.830000e+02 1.830000e+02 +1.022744e+03 1.900000e-02 1.900000e-02 1.451700e+04 1.260000e+02 1.260000e+02 +1.023264e+03 2.500000e-02 2.500000e-02 6.876000e+03 8.600000e+01 8.600000e+01 +1.025320e+03 3.100000e-02 3.100000e-02 2.319000e+03 5.100000e+01 5.100000e+01 +1.027956e+03 1.500000e-02 1.500000e-02 8.150000e+03 9.400000e+01 9.400000e+01 +1.029090e+03 1.400000e-02 1.400000e-02 1.911000e+03 4.500000e+01 4.500000e+01 +1.033907e+03 1.100000e-02 1.100000e-02 3.704000e+03 6.400000e+01 6.400000e+01 +1.040028e+03 3.500000e-02 3.500000e-02 2.839000e+03 5.600000e+01 5.600000e+01 +1.049864e+03 1.100000e-02 1.100000e-02 4.291000e+03 7.000000e+01 7.000000e+01 +1.050862e+03 3.100000e-02 3.100000e-02 1.310000e+03 3.900000e+01 3.900000e+01 +1.059947e+03 1.500000e-02 1.500000e-02 1.271000e+03 3.800000e+01 3.800000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1444990/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD3_2016_I1444990/d01-x01-y02 +Title: doi:10.17182/hepdata.78538.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004066e+03 8.000000e-03 8.000000e-03 3.210000e-01 0.000000e+00 0.000000e+00 +1.010466e+03 1.000000e-02 1.000000e-02 3.120000e-01 0.000000e+00 0.000000e+00 +1.012955e+03 7.000000e-03 7.000000e-03 3.080000e-01 0.000000e+00 0.000000e+00 +1.015068e+03 1.200000e-02 1.200000e-02 3.070000e-01 0.000000e+00 0.000000e+00 +1.016105e+03 1.000000e-02 1.000000e-02 3.040000e-01 0.000000e+00 0.000000e+00 +1.017155e+03 1.200000e-02 1.200000e-02 3.030000e-01 0.000000e+00 0.000000e+00 +1.017156e+03 1.300000e-02 1.300000e-02 3.020000e-01 0.000000e+00 0.000000e+00 +1.018046e+03 2.100000e-02 2.100000e-02 3.010000e-01 0.000000e+00 0.000000e+00 +1.019118e+03 1.600000e-02 1.600000e-02 3.000000e-01 0.000000e+00 0.000000e+00 +1.019214e+03 1.900000e-02 1.900000e-02 2.990000e-01 0.000000e+00 0.000000e+00 +1.019421e+03 2.800000e-02 2.800000e-02 2.990000e-01 0.000000e+00 0.000000e+00 +1.019902e+03 1.200000e-02 1.200000e-02 2.990000e-01 0.000000e+00 0.000000e+00 +1.021222e+03 2.100000e-02 2.100000e-02 2.990000e-01 0.000000e+00 0.000000e+00 +1.021309e+03 9.000000e-03 9.000000e-03 2.990000e-01 0.000000e+00 0.000000e+00 +1.022078e+03 2.100000e-02 2.100000e-02 2.970000e-01 0.000000e+00 0.000000e+00 +1.022744e+03 1.900000e-02 1.900000e-02 2.970000e-01 0.000000e+00 0.000000e+00 +1.023264e+03 2.500000e-02 2.500000e-02 2.970000e-01 0.000000e+00 0.000000e+00 +1.025320e+03 3.100000e-02 3.100000e-02 2.940000e-01 0.000000e+00 0.000000e+00 +1.027956e+03 1.500000e-02 1.500000e-02 2.940000e-01 0.000000e+00 0.000000e+00 +1.029090e+03 1.400000e-02 1.400000e-02 2.930000e-01 0.000000e+00 0.000000e+00 +1.033907e+03 1.100000e-02 1.100000e-02 2.920000e-01 0.000000e+00 0.000000e+00 +1.040028e+03 3.500000e-02 3.500000e-02 2.890000e-01 0.000000e+00 0.000000e+00 +1.049864e+03 1.100000e-02 1.100000e-02 2.840000e-01 0.000000e+00 0.000000e+00 +1.050862e+03 3.100000e-02 3.100000e-02 2.850000e-01 0.000000e+00 0.000000e+00 +1.059947e+03 1.500000e-02 1.500000e-02 2.760000e-01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1444990/d01-x01-y03 +IsRef: 1 +Path: /REF/CMD3_2016_I1444990/d01-x01-y03 +Title: doi:10.17182/hepdata.78538.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004066e+03 8.000000e-03 8.000000e-03 7.200000e-01 0.000000e+00 0.000000e+00 +1.010466e+03 1.000000e-02 1.000000e-02 7.300000e-01 0.000000e+00 0.000000e+00 +1.012955e+03 7.000000e-03 7.000000e-03 7.200000e-01 0.000000e+00 0.000000e+00 +1.015068e+03 1.200000e-02 1.200000e-02 7.100000e-01 0.000000e+00 0.000000e+00 +1.016105e+03 1.000000e-02 1.000000e-02 7.100000e-01 0.000000e+00 0.000000e+00 +1.017155e+03 1.200000e-02 1.200000e-02 7.000000e-01 0.000000e+00 0.000000e+00 +1.017156e+03 1.300000e-02 1.300000e-02 7.000000e-01 0.000000e+00 0.000000e+00 +1.018046e+03 2.100000e-02 2.100000e-02 7.000000e-01 0.000000e+00 0.000000e+00 +1.019118e+03 1.600000e-02 1.600000e-02 7.200000e-01 0.000000e+00 0.000000e+00 +1.019214e+03 1.900000e-02 1.900000e-02 7.200000e-01 0.000000e+00 0.000000e+00 +1.019421e+03 2.800000e-02 2.800000e-02 7.300000e-01 0.000000e+00 0.000000e+00 +1.019902e+03 1.200000e-02 1.200000e-02 7.500000e-01 0.000000e+00 0.000000e+00 +1.021222e+03 2.100000e-02 2.100000e-02 8.300000e-01 0.000000e+00 0.000000e+00 +1.021309e+03 9.000000e-03 9.000000e-03 8.300000e-01 0.000000e+00 0.000000e+00 +1.022078e+03 2.100000e-02 2.100000e-02 8.800000e-01 0.000000e+00 0.000000e+00 +1.022744e+03 1.900000e-02 1.900000e-02 9.300000e-01 0.000000e+00 0.000000e+00 +1.023264e+03 2.500000e-02 2.500000e-02 9.600000e-01 0.000000e+00 0.000000e+00 +1.025320e+03 3.100000e-02 3.100000e-02 1.080000e+00 0.000000e+00 0.000000e+00 +1.027956e+03 1.500000e-02 1.500000e-02 1.210000e+00 0.000000e+00 0.000000e+00 +1.029090e+03 1.400000e-02 1.400000e-02 1.260000e+00 0.000000e+00 0.000000e+00 +1.033907e+03 1.100000e-02 1.100000e-02 1.430000e+00 0.000000e+00 0.000000e+00 +1.040028e+03 3.500000e-02 3.500000e-02 1.600000e+00 0.000000e+00 0.000000e+00 +1.049864e+03 1.100000e-02 1.100000e-02 1.780000e+00 0.000000e+00 0.000000e+00 +1.050862e+03 3.100000e-02 3.100000e-02 1.790000e+00 0.000000e+00 0.000000e+00 +1.059947e+03 1.500000e-02 1.500000e-02 1.910000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1444990/d01-x01-y04 +IsRef: 1 +Path: /REF/CMD3_2016_I1444990/d01-x01-y04 +Title: doi:10.17182/hepdata.78538.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004066e+03 8.000000e-03 8.000000e-03 9.940000e-01 0.000000e+00 0.000000e+00 +1.010466e+03 1.000000e-02 1.000000e-02 9.920000e-01 0.000000e+00 0.000000e+00 +1.012955e+03 7.000000e-03 7.000000e-03 9.880000e-01 0.000000e+00 0.000000e+00 +1.015068e+03 1.200000e-02 1.200000e-02 9.870000e-01 0.000000e+00 0.000000e+00 +1.016105e+03 1.000000e-02 1.000000e-02 9.780000e-01 0.000000e+00 0.000000e+00 +1.017155e+03 1.200000e-02 1.200000e-02 9.830000e-01 0.000000e+00 0.000000e+00 +1.017156e+03 1.300000e-02 1.300000e-02 9.850000e-01 0.000000e+00 0.000000e+00 +1.018046e+03 2.100000e-02 2.100000e-02 9.920000e-01 0.000000e+00 0.000000e+00 +1.019118e+03 1.600000e-02 1.600000e-02 1.028000e+00 0.000000e+00 0.000000e+00 +1.019214e+03 1.900000e-02 1.900000e-02 1.022000e+00 0.000000e+00 0.000000e+00 +1.019421e+03 2.800000e-02 2.800000e-02 1.024000e+00 0.000000e+00 0.000000e+00 +1.019902e+03 1.200000e-02 1.200000e-02 1.016000e+00 0.000000e+00 0.000000e+00 +1.021222e+03 2.100000e-02 2.100000e-02 9.940000e-01 0.000000e+00 0.000000e+00 +1.021309e+03 9.000000e-03 9.000000e-03 9.940000e-01 0.000000e+00 0.000000e+00 +1.022078e+03 2.100000e-02 2.100000e-02 9.890000e-01 0.000000e+00 0.000000e+00 +1.022744e+03 1.900000e-02 1.900000e-02 9.890000e-01 0.000000e+00 0.000000e+00 +1.023264e+03 2.500000e-02 2.500000e-02 9.920000e-01 0.000000e+00 0.000000e+00 +1.025320e+03 3.100000e-02 3.100000e-02 9.960000e-01 0.000000e+00 0.000000e+00 +1.027956e+03 1.500000e-02 1.500000e-02 9.970000e-01 0.000000e+00 0.000000e+00 +1.029090e+03 1.400000e-02 1.400000e-02 9.980000e-01 0.000000e+00 0.000000e+00 +1.033907e+03 1.100000e-02 1.100000e-02 9.990000e-01 0.000000e+00 0.000000e+00 +1.040028e+03 3.500000e-02 3.500000e-02 1.000000e+00 0.000000e+00 0.000000e+00 +1.049864e+03 1.100000e-02 1.100000e-02 1.000000e+00 0.000000e+00 0.000000e+00 +1.050862e+03 3.100000e-02 3.100000e-02 1.000000e+00 0.000000e+00 0.000000e+00 +1.059947e+03 1.500000e-02 1.500000e-02 1.000000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1444990/d01-x01-y05 +IsRef: 1 +Path: /REF/CMD3_2016_I1444990/d01-x01-y05 +Title: doi:10.17182/hepdata.78538.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004066e+03 8.000000e-03 8.000000e-03 1.953500e+02 6.700000e-01 6.700000e-01 +1.010466e+03 1.000000e-02 1.000000e-02 9.360500e+02 1.440000e+00 1.440000e+00 +1.012955e+03 7.000000e-03 7.000000e-03 4.853500e+02 1.040000e+00 1.040000e+00 +1.015068e+03 1.200000e-02 1.200000e-02 4.791000e+01 3.300000e-01 3.300000e-01 +1.016105e+03 1.000000e-02 1.000000e-02 1.921100e+02 6.600000e-01 6.600000e-01 +1.017155e+03 1.200000e-02 1.200000e-02 4.789900e+02 1.040000e+00 1.040000e+00 +1.017156e+03 1.300000e-02 1.300000e-02 4.076000e+01 3.000000e-01 3.000000e-01 +1.018046e+03 2.100000e-02 2.100000e-02 4.783400e+02 1.040000e+00 1.040000e+00 +1.019118e+03 1.600000e-02 1.600000e-02 3.286200e+02 8.600000e-01 8.600000e-01 +1.019214e+03 1.900000e-02 1.900000e-02 5.275000e+01 3.400000e-01 3.400000e-01 +1.019421e+03 2.800000e-02 2.800000e-02 3.604000e+01 2.800000e-01 2.800000e-01 +1.019902e+03 1.200000e-02 1.200000e-02 4.723400e+02 1.040000e+00 1.040000e+00 +1.021222e+03 2.100000e-02 2.100000e-02 2.283400e+02 7.200000e-01 7.200000e-01 +1.021309e+03 9.000000e-03 9.000000e-03 4.685000e+01 3.300000e-01 3.300000e-01 +1.022078e+03 2.100000e-02 2.100000e-02 2.016100e+02 6.800000e-01 6.800000e-01 +1.022744e+03 1.900000e-02 1.900000e-02 1.167100e+02 5.200000e-01 5.200000e-01 +1.023264e+03 2.500000e-02 2.500000e-02 6.291000e+01 3.800000e-01 3.800000e-01 +1.025320e+03 3.100000e-02 3.100000e-02 3.632000e+01 2.800000e-01 2.800000e-01 +1.027956e+03 1.500000e-02 1.500000e-02 1.958300e+02 6.700000e-01 6.700000e-01 +1.029090e+03 1.400000e-02 1.400000e-02 5.294000e+01 3.500000e-01 3.500000e-01 +1.033907e+03 1.100000e-02 1.100000e-02 1.755500e+02 6.400000e-01 6.400000e-01 +1.040028e+03 3.500000e-02 3.500000e-02 1.959100e+02 6.800000e-01 6.800000e-01 +1.049864e+03 1.100000e-02 1.100000e-02 4.995900e+02 1.090000e+00 1.090000e+00 +1.050862e+03 3.100000e-02 3.100000e-02 1.463100e+02 5.900000e-01 5.900000e-01 +1.059947e+03 1.500000e-02 1.500000e-02 1.988600e+02 6.900000e-01 6.900000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD3_2016_I1444990/d01-x01-y06 +IsRef: 1 +Path: /REF/CMD3_2016_I1444990/d01-x01-y06 +Title: doi:10.17182/hepdata.78538.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.004066e+03 8.000000e-03 8.000000e-03 6.870000e+00 4.200000e-01 4.200000e-01 +1.010466e+03 1.000000e-02 1.000000e-02 4.216000e+01 4.700000e-01 4.700000e-01 +1.012955e+03 7.000000e-03 7.000000e-03 9.674000e+01 1.000000e+00 1.000000e+00 +1.015068e+03 1.200000e-02 1.200000e-02 2.195300e+02 5.020000e+00 5.020000e+00 +1.016105e+03 1.000000e-02 1.000000e-02 3.663300e+02 3.330000e+00 3.330000e+00 +1.017155e+03 1.200000e-02 1.200000e-02 6.281500e+02 2.950000e+00 2.950000e+00 +1.017156e+03 1.300000e-02 1.300000e-02 6.247600e+02 9.890000e+00 9.890000e+00 +1.018046e+03 2.100000e-02 2.100000e-02 9.966200e+02 4.280000e+00 4.280000e+00 +1.019118e+03 1.600000e-02 1.600000e-02 1.413650e+03 6.020000e+00 6.020000e+00 +1.019214e+03 1.900000e-02 1.900000e-02 1.433050e+03 1.503000e+01 1.503000e+01 +1.019421e+03 2.800000e-02 2.800000e-02 1.434840e+03 1.840000e+01 1.840000e+01 +1.019902e+03 1.200000e-02 1.200000e-02 1.341910e+03 4.740000e+00 4.740000e+00 +1.021222e+03 2.100000e-02 2.100000e-02 8.332000e+02 4.890000e+00 4.890000e+00 +1.021309e+03 9.000000e-03 9.000000e-03 8.075400e+02 1.036000e+01 1.036000e+01 +1.022078e+03 2.100000e-02 2.100000e-02 5.829300e+02 4.030000e+00 4.030000e+00 +1.022744e+03 1.900000e-02 1.900000e-02 4.437100e+02 4.380000e+00 4.380000e+00 +1.023264e+03 2.500000e-02 2.500000e-02 3.777700e+02 5.310000e+00 5.310000e+00 +1.025320e+03 3.100000e-02 3.100000e-02 1.992600e+02 4.970000e+00 4.970000e+00 +1.027956e+03 1.500000e-02 1.500000e-02 1.159300e+02 1.700000e+00 1.700000e+00 +1.029090e+03 1.400000e-02 1.400000e-02 9.696000e+01 3.000000e+00 3.000000e+00 +1.033907e+03 1.100000e-02 1.100000e-02 5.012000e+01 1.260000e+00 1.260000e+00 +1.040028e+03 3.500000e-02 3.500000e-02 3.127000e+01 1.010000e+00 1.010000e+00 +1.049864e+03 1.100000e-02 1.100000e-02 1.693000e+01 5.000000e-01 5.000000e-01 +1.050862e+03 3.100000e-02 3.100000e-02 1.747000e+01 9.400000e-01 9.400000e-01 +1.059947e+03 1.500000e-02 1.500000e-02 1.209000e+01 7.100000e-01 7.100000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/CMD_1985_I221309.cc b/analyses/pluginNovosibirsk/CMD_1985_I221309.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD_1985_I221309.cc @@ -0,0 +1,83 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CMD_1985_I221309 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CMD_1985_I221309); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CMD_1985_I221309); + + +} diff --git a/analyses/pluginNovosibirsk/CMD_1985_I221309.info b/analyses/pluginNovosibirsk/CMD_1985_I221309.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD_1985_I221309.info @@ -0,0 +1,31 @@ +Name: CMD_1985_I221309 +Year: 1985 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ for energies below 1.4 GeV +Experiment: CMD +Collider: VEPP-2M +InspireID: 221309 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Nucl.Phys. B256 (1985) 365-384, 1985 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies below 1.4 GeV.' +Keywords: [] +BibKey: Barkov:1985ac +BibTeX: '@article{Barkov:1985ac, + author = "Barkov, L. M. and others", + title = "{Electromagnetic Pion Form-Factor in the Timelike + Region}", + journal = "Nucl. Phys.", + volume = "B256", + year = "1985", + pages = "365-384", + doi = "10.1016/0550-3213(85)90399-2", + SLACcitation = "%%CITATION = NUPHA,B256,365;%%" +}' diff --git a/analyses/pluginNovosibirsk/CMD_1985_I221309.plot b/analyses/pluginNovosibirsk/CMD_1985_I221309.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD_1985_I221309.plot @@ -0,0 +1,12 @@ +BEGIN PLOT /CMD_1985_I221309/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /CMD_1985_I221309/d02-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/CMD_1985_I221309.yoda b/analyses/pluginNovosibirsk/CMD_1985_I221309.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/CMD_1985_I221309.yoda @@ -0,0 +1,238 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CMD_1985_I221309/d01-x01-y01 +IsRef: 1 +Path: /REF/CMD_1985_I221309/d01-x01-y01 +Title: doi:10.17182/hepdata.6886.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.000000e+02 0.000000e+00 0.000000e+00 1.020000e+02 1.200000e+01 1.200000e+01 +4.400000e+02 0.000000e+00 0.000000e+00 2.010000e+02 5.000000e+01 5.000000e+01 +6.426000e+02 0.000000e+00 0.000000e+00 4.730000e+02 4.800000e+01 4.800000e+01 +6.626000e+02 0.000000e+00 0.000000e+00 5.550000e+02 7.000000e+01 7.000000e+01 +6.776000e+02 0.000000e+00 0.000000e+00 6.370000e+02 3.200000e+01 3.200000e+01 +6.876000e+02 0.000000e+00 0.000000e+00 7.620000e+02 5.500000e+01 5.500000e+01 +6.976000e+02 0.000000e+00 0.000000e+00 8.270000e+02 3.600000e+01 3.600000e+01 +7.076000e+02 0.000000e+00 0.000000e+00 8.800000e+02 2.700000e+01 2.700000e+01 +7.176000e+02 0.000000e+00 0.000000e+00 9.730000e+02 3.100000e+01 3.100000e+01 +7.276000e+02 0.000000e+00 0.000000e+00 1.092000e+03 5.900000e+01 5.900000e+01 +7.376000e+02 0.000000e+00 0.000000e+00 1.205000e+03 4.500000e+01 4.500000e+01 +7.476000e+02 0.000000e+00 0.000000e+00 1.274000e+03 3.200000e+01 3.200000e+01 +7.576000e+02 0.000000e+00 0.000000e+00 1.298000e+03 2.900000e+01 2.900000e+01 +7.676000e+02 0.000000e+00 0.000000e+00 1.308000e+03 4.200000e+01 4.200000e+01 +7.736000e+02 0.000000e+00 0.000000e+00 1.317000e+03 7.600000e+01 7.600000e+01 +7.756000e+02 0.000000e+00 0.000000e+00 1.311000e+03 5.900000e+01 5.900000e+01 +7.776000e+02 0.000000e+00 0.000000e+00 1.264000e+03 5.500000e+01 5.500000e+01 +7.796000e+02 0.000000e+00 0.000000e+00 1.186000e+03 5.900000e+01 5.900000e+01 +7.816000e+02 0.000000e+00 0.000000e+00 1.125000e+03 4.600000e+01 4.600000e+01 +7.836000e+02 0.000000e+00 0.000000e+00 9.530000e+02 5.100000e+01 5.100000e+01 +7.856000e+02 0.000000e+00 0.000000e+00 8.490000e+02 4.500000e+01 4.500000e+01 +7.876000e+02 0.000000e+00 0.000000e+00 8.660000e+02 5.000000e+01 5.000000e+01 +7.896000e+02 0.000000e+00 0.000000e+00 8.230000e+02 4.400000e+01 4.400000e+01 +7.916000e+02 0.000000e+00 0.000000e+00 8.750000e+02 4.900000e+01 4.900000e+01 +7.976000e+02 0.000000e+00 0.000000e+00 7.870000e+02 2.900000e+01 2.900000e+01 +8.076000e+02 0.000000e+00 0.000000e+00 7.220000e+02 2.500000e+01 2.500000e+01 +8.176000e+02 0.000000e+00 0.000000e+00 6.210000e+02 1.800000e+01 1.800000e+01 +8.276000e+02 0.000000e+00 0.000000e+00 5.340000e+02 2.000000e+01 2.000000e+01 +8.376000e+02 0.000000e+00 0.000000e+00 4.620000e+02 1.300000e+01 1.300000e+01 +8.476000e+02 0.000000e+00 0.000000e+00 3.880000e+02 2.100000e+01 2.100000e+01 +8.576000e+02 0.000000e+00 0.000000e+00 3.370000e+02 1.400000e+01 1.400000e+01 +8.676000e+02 0.000000e+00 0.000000e+00 2.930000e+02 1.100000e+01 1.100000e+01 +8.776000e+02 0.000000e+00 0.000000e+00 2.480000e+02 8.000000e+00 8.000000e+00 +8.876000e+02 0.000000e+00 0.000000e+00 2.110000e+02 1.100000e+01 1.100000e+01 +8.976000e+02 0.000000e+00 0.000000e+00 1.825000e+02 6.400000e+00 6.400000e+00 +9.076000e+02 0.000000e+00 0.000000e+00 1.688000e+02 6.000000e+00 6.000000e+00 +9.176000e+02 0.000000e+00 0.000000e+00 1.427000e+02 7.400000e+00 7.400000e+00 +9.276000e+02 0.000000e+00 0.000000e+00 1.242000e+02 8.300000e+00 8.300000e+00 +9.376000e+02 0.000000e+00 0.000000e+00 1.067000e+02 5.700000e+00 5.700000e+00 +9.476000e+02 0.000000e+00 0.000000e+00 9.370000e+01 5.400000e+00 5.400000e+00 +9.576000e+02 0.000000e+00 0.000000e+00 9.390000e+01 4.800000e+00 4.800000e+00 +9.676000e+02 0.000000e+00 0.000000e+00 7.850000e+01 4.800000e+00 4.800000e+00 +9.776000e+02 0.000000e+00 0.000000e+00 7.630000e+01 4.100000e+00 4.100000e+00 +9.876000e+02 0.000000e+00 0.000000e+00 6.300000e+01 4.100000e+00 4.100000e+00 +9.976000e+02 0.000000e+00 0.000000e+00 6.500000e+01 3.300000e+00 3.300000e+00 +1.006600e+03 0.000000e+00 0.000000e+00 6.030000e+01 3.200000e+00 3.200000e+00 +1.067000e+03 0.000000e+00 0.000000e+00 3.830000e+01 3.000000e+00 3.000000e+00 +1.077000e+03 0.000000e+00 0.000000e+00 3.600000e+01 4.000000e+00 4.000000e+00 +1.087000e+03 0.000000e+00 0.000000e+00 3.360000e+01 2.800000e+00 2.800000e+00 +1.097000e+03 0.000000e+00 0.000000e+00 2.980000e+01 2.800000e+00 2.800000e+00 +1.107000e+03 0.000000e+00 0.000000e+00 3.240000e+01 2.900000e+00 2.900000e+00 +1.117000e+03 0.000000e+00 0.000000e+00 2.460000e+01 2.600000e+00 2.600000e+00 +1.127000e+03 0.000000e+00 0.000000e+00 2.320000e+01 2.500000e+00 2.500000e+00 +1.137000e+03 0.000000e+00 0.000000e+00 2.420000e+01 2.700000e+00 2.700000e+00 +1.152000e+03 0.000000e+00 0.000000e+00 2.207000e+01 2.700000e+00 2.700000e+00 +1.167000e+03 0.000000e+00 0.000000e+00 1.630000e+01 2.300000e+00 2.300000e+00 +1.177000e+03 0.000000e+00 0.000000e+00 1.920000e+01 2.600000e+00 2.600000e+00 +1.187000e+03 0.000000e+00 0.000000e+00 1.960000e+01 3.100000e+00 3.100000e+00 +1.197000e+03 0.000000e+00 0.000000e+00 1.610000e+01 2.300000e+00 2.300000e+00 +1.207000e+03 0.000000e+00 0.000000e+00 1.850000e+01 3.000000e+00 3.000000e+00 +1.217000e+03 0.000000e+00 0.000000e+00 1.030000e+01 1.900000e+00 1.900000e+00 +1.227000e+03 0.000000e+00 0.000000e+00 1.150000e+01 2.400000e+00 2.400000e+00 +1.237000e+03 0.000000e+00 0.000000e+00 1.660000e+01 2.600000e+00 2.600000e+00 +1.247000e+03 0.000000e+00 0.000000e+00 1.100000e+01 2.000000e+00 2.000000e+00 +1.257000e+03 0.000000e+00 0.000000e+00 1.110000e+01 1.800000e+00 1.800000e+00 +1.267000e+03 0.000000e+00 0.000000e+00 8.400000e+00 1.700000e+00 1.700000e+00 +1.277000e+03 0.000000e+00 0.000000e+00 5.500000e+00 1.200000e+00 1.200000e+00 +1.287000e+03 0.000000e+00 0.000000e+00 7.500000e+00 1.400000e+00 1.400000e+00 +1.297000e+03 0.000000e+00 0.000000e+00 8.100000e+00 1.800000e+00 1.800000e+00 +1.307000e+03 0.000000e+00 0.000000e+00 8.000000e+00 1.500000e+00 1.500000e+00 +1.317000e+03 0.000000e+00 0.000000e+00 8.100000e+00 1.600000e+00 1.600000e+00 +1.327000e+03 0.000000e+00 0.000000e+00 5.200000e+00 1.600000e+00 1.600000e+00 +1.337000e+03 0.000000e+00 0.000000e+00 7.700000e+00 1.700000e+00 1.700000e+00 +1.347000e+03 0.000000e+00 0.000000e+00 3.800000e+00 1.000000e+00 1.000000e+00 +1.357000e+03 0.000000e+00 0.000000e+00 4.600000e+00 1.100000e+00 1.100000e+00 +1.367000e+03 0.000000e+00 0.000000e+00 2.900000e+00 8.000000e-01 8.000000e-01 +1.377000e+03 0.000000e+00 0.000000e+00 3.200000e+00 1.000000e+00 1.000000e+00 +1.387000e+03 0.000000e+00 0.000000e+00 4.100000e+00 1.000000e+00 1.000000e+00 +1.397000e+03 0.000000e+00 0.000000e+00 2.100000e+00 7.000000e-01 7.000000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD_1985_I221309/d01-x01-y02 +IsRef: 1 +Path: /REF/CMD_1985_I221309/d01-x01-y02 +Title: doi:10.17182/hepdata.6886.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.000000e+02 0.000000e+00 0.000000e+00 2.040000e+00 2.500000e-01 2.500000e-01 +4.400000e+02 0.000000e+00 0.000000e+00 3.870000e+00 9.700000e-01 9.700000e-01 +6.426000e+02 0.000000e+00 0.000000e+00 1.224000e+01 1.240000e+00 1.240000e+00 +6.626000e+02 0.000000e+00 0.000000e+00 1.496000e+01 1.870000e+00 1.870000e+00 +6.776000e+02 0.000000e+00 0.000000e+00 1.771000e+01 9.000000e-01 9.000000e-01 +6.876000e+02 0.000000e+00 0.000000e+00 2.164000e+01 1.560000e+00 1.560000e+00 +6.976000e+02 0.000000e+00 0.000000e+00 2.396000e+01 1.050000e+00 1.050000e+00 +7.076000e+02 0.000000e+00 0.000000e+00 2.600000e+01 8.200000e-01 8.200000e-01 +7.176000e+02 0.000000e+00 0.000000e+00 2.935000e+01 9.400000e-01 9.400000e-01 +7.276000e+02 0.000000e+00 0.000000e+00 3.362000e+01 1.810000e+00 1.810000e+00 +7.376000e+02 0.000000e+00 0.000000e+00 3.788000e+01 1.400000e+00 1.400000e+00 +7.476000e+02 0.000000e+00 0.000000e+00 4.102000e+01 1.000000e+00 1.000000e+00 +7.576000e+02 0.000000e+00 0.000000e+00 4.248000e+01 9.600000e-01 9.600000e-01 +7.676000e+02 0.000000e+00 0.000000e+00 4.368000e+01 1.400000e+00 1.400000e+00 +7.736000e+02 0.000000e+00 0.000000e+00 4.452000e+01 2.590000e+00 2.590000e+00 +7.756000e+02 0.000000e+00 0.000000e+00 4.451000e+01 1.990000e+00 1.990000e+00 +7.776000e+02 0.000000e+00 0.000000e+00 4.305000e+01 1.880000e+00 1.880000e+00 +7.796000e+02 0.000000e+00 0.000000e+00 4.058000e+01 2.020000e+00 2.020000e+00 +7.816000e+02 0.000000e+00 0.000000e+00 3.862000e+01 1.580000e+00 1.580000e+00 +7.836000e+02 0.000000e+00 0.000000e+00 3.286000e+01 1.780000e+00 1.780000e+00 +7.856000e+02 0.000000e+00 0.000000e+00 2.941000e+01 1.550000e+00 1.550000e+00 +7.876000e+02 0.000000e+00 0.000000e+00 3.010000e+01 1.730000e+00 1.730000e+00 +7.896000e+02 0.000000e+00 0.000000e+00 2.873000e+01 1.520000e+00 1.520000e+00 +7.916000e+02 0.000000e+00 0.000000e+00 3.065000e+01 1.720000e+00 1.720000e+00 +7.976000e+02 0.000000e+00 0.000000e+00 2.790000e+01 1.010000e+00 1.010000e+00 +8.076000e+02 0.000000e+00 0.000000e+00 2.610000e+01 9.100000e-01 9.100000e-01 +8.176000e+02 0.000000e+00 0.000000e+00 2.290000e+01 6.500000e-01 6.500000e-01 +8.276000e+02 0.000000e+00 0.000000e+00 2.010000e+01 7.400000e-01 7.400000e-01 +8.376000e+02 0.000000e+00 0.000000e+00 1.771000e+01 5.000000e-01 5.000000e-01 +8.476000e+02 0.000000e+00 0.000000e+00 1.516000e+01 8.200000e-01 8.200000e-01 +8.576000e+02 0.000000e+00 0.000000e+00 1.344000e+01 5.800000e-01 5.800000e-01 +8.676000e+02 0.000000e+00 0.000000e+00 1.192000e+01 4.600000e-01 4.600000e-01 +8.776000e+02 0.000000e+00 0.000000e+00 1.028000e+01 3.300000e-01 3.300000e-01 +8.876000e+02 0.000000e+00 0.000000e+00 8.920000e+00 4.500000e-01 4.500000e-01 +8.976000e+02 0.000000e+00 0.000000e+00 7.850000e+00 2.800000e-01 2.800000e-01 +9.076000e+02 0.000000e+00 0.000000e+00 7.400000e+00 2.600000e-01 2.600000e-01 +9.176000e+02 0.000000e+00 0.000000e+00 6.370000e+00 3.300000e-01 3.300000e-01 +9.276000e+02 0.000000e+00 0.000000e+00 5.650000e+00 3.800000e-01 3.800000e-01 +9.376000e+02 0.000000e+00 0.000000e+00 4.940000e+00 2.700000e-01 2.700000e-01 +9.476000e+02 0.000000e+00 0.000000e+00 4.420000e+00 2.600000e-01 2.600000e-01 +9.576000e+02 0.000000e+00 0.000000e+00 4.510000e+00 2.300000e-01 2.300000e-01 +9.676000e+02 0.000000e+00 0.000000e+00 3.840000e+00 2.400000e-01 2.400000e-01 +9.776000e+02 0.000000e+00 0.000000e+00 3.800000e+00 2.000000e-01 2.000000e-01 +9.876000e+02 0.000000e+00 0.000000e+00 3.190000e+00 2.100000e-01 2.100000e-01 +9.976000e+02 0.000000e+00 0.000000e+00 3.350000e+00 1.700000e-01 1.700000e-01 +1.006600e+03 0.000000e+00 0.000000e+00 3.160000e+00 1.700000e-01 1.700000e-01 +1.067000e+03 0.000000e+00 0.000000e+00 2.250000e+00 1.800000e-01 1.800000e-01 +1.077000e+03 0.000000e+00 0.000000e+00 2.130000e+00 2.400000e-01 2.400000e-01 +1.087000e+03 0.000000e+00 0.000000e+00 2.020000e+00 1.700000e-01 1.700000e-01 +1.097000e+03 0.000000e+00 0.000000e+00 1.820000e+00 1.700000e-01 1.700000e-01 +1.107000e+03 0.000000e+00 0.000000e+00 2.010000e+00 1.800000e-01 1.800000e-01 +1.117000e+03 0.000000e+00 0.000000e+00 1.570000e+00 1.700000e-01 1.700000e-01 +1.127000e+03 0.000000e+00 0.000000e+00 1.500000e+00 1.600000e-01 1.600000e-01 +1.137000e+03 0.000000e+00 0.000000e+00 1.580000e+00 1.800000e-01 1.800000e-01 +1.152000e+03 0.000000e+00 0.000000e+00 1.470000e+00 1.800000e-01 1.800000e-01 +1.167000e+03 0.000000e+00 0.000000e+00 1.110000e+00 1.600000e-01 1.600000e-01 +1.177000e+03 0.000000e+00 0.000000e+00 1.330000e+00 1.800000e-01 1.800000e-01 +1.187000e+03 0.000000e+00 0.000000e+00 1.380000e+00 2.200000e-01 2.200000e-01 +1.197000e+03 0.000000e+00 0.000000e+00 1.150000e+00 1.600000e-01 1.600000e-01 +1.207000e+03 0.000000e+00 0.000000e+00 1.340000e+00 2.200000e-01 2.200000e-01 +1.217000e+03 0.000000e+00 0.000000e+00 7.600000e-01 1.400000e-01 1.400000e-01 +1.227000e+03 0.000000e+00 0.000000e+00 8.600000e-01 1.800000e-01 1.800000e-01 +1.237000e+03 0.000000e+00 0.000000e+00 1.260000e+00 2.000000e-01 2.000000e-01 +1.247000e+03 0.000000e+00 0.000000e+00 8.500000e-01 1.500000e-01 1.500000e-01 +1.257000e+03 0.000000e+00 0.000000e+00 8.700000e-01 1.400000e-01 1.400000e-01 +1.267000e+03 0.000000e+00 0.000000e+00 6.700000e-01 1.300000e-01 1.300000e-01 +1.277000e+03 0.000000e+00 0.000000e+00 4.400000e-01 1.000000e-01 1.000000e-01 +1.287000e+03 0.000000e+00 0.000000e+00 6.100000e-01 1.100000e-01 1.100000e-01 +1.297000e+03 0.000000e+00 0.000000e+00 6.700000e-01 1.500000e-01 1.500000e-01 +1.307000e+03 0.000000e+00 0.000000e+00 6.700000e-01 1.300000e-01 1.300000e-01 +1.317000e+03 0.000000e+00 0.000000e+00 6.900000e-01 1.600000e+00 1.600000e+00 +1.327000e+03 0.000000e+00 0.000000e+00 4.500000e-01 1.300000e-01 1.300000e-01 +1.337000e+03 0.000000e+00 0.000000e+00 6.800000e-01 1.400000e-01 1.400000e-01 +1.347000e+03 0.000000e+00 0.000000e+00 3.400000e-01 8.000000e-02 8.000000e-02 +1.357000e+03 0.000000e+00 0.000000e+00 4.100000e-01 1.000000e-01 1.000000e-01 +1.367000e+03 0.000000e+00 0.000000e+00 2.600000e-01 7.000000e-02 7.000000e-02 +1.377000e+03 0.000000e+00 0.000000e+00 3.000000e-01 9.000000e-02 9.000000e-02 +1.387000e+03 0.000000e+00 0.000000e+00 3.900000e-01 9.000000e-02 9.000000e-02 +1.397000e+03 0.000000e+00 0.000000e+00 2.000000e-01 7.000000e-02 7.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD_1985_I221309/d02-x01-y01 +IsRef: 1 +Path: /REF/CMD_1985_I221309/d02-x01-y01 +Title: doi:10.17182/hepdata.6886.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.600000e+02 0.000000e+00 0.000000e+00 7.890000e+01 6.800000e+00 6.800000e+00 +3.800000e+02 0.000000e+00 0.000000e+00 1.000000e+02 9.400000e+00 9.400000e+00 +4.100000e+02 0.000000e+00 0.000000e+00 1.201000e+02 8.100000e+00 8.100000e+00 +4.300000e+02 0.000000e+00 0.000000e+00 1.263000e+02 1.240000e+01 1.240000e+01 +4.380000e+02 0.000000e+00 0.000000e+00 1.433000e+02 1.190000e+01 1.190000e+01 +4.700000e+02 0.000000e+00 0.000000e+00 1.424000e+02 9.200000e+00 9.200000e+00 +5.400000e+02 0.000000e+00 0.000000e+00 2.081000e+02 1.400000e+01 1.400000e+01 +5.800000e+02 0.000000e+00 0.000000e+00 2.451000e+02 1.650000e+01 1.650000e+01 +6.200000e+02 0.000000e+00 0.000000e+00 3.474000e+02 2.010000e+01 2.010000e+01 +6.400000e+02 0.000000e+00 0.000000e+00 3.813000e+02 2.120000e+01 2.120000e+01 +6.600000e+02 0.000000e+00 0.000000e+00 4.672000e+02 3.300000e+01 3.300000e+01 +7.000000e+02 0.000000e+00 0.000000e+00 8.671000e+02 9.360000e+01 9.360000e+01 +7.400000e+02 0.000000e+00 0.000000e+00 1.432000e+03 1.290000e+02 1.290000e+02 +7.600000e+02 0.000000e+00 0.000000e+00 1.237000e+03 8.400000e+01 8.400000e+01 +7.700000e+02 0.000000e+00 0.000000e+00 1.303000e+03 5.300000e+01 5.300000e+01 +7.740000e+02 0.000000e+00 0.000000e+00 1.277000e+03 5.900000e+01 5.900000e+01 +7.780000e+02 0.000000e+00 0.000000e+00 1.371000e+03 5.800000e+01 5.800000e+01 +7.800000e+02 0.000000e+00 0.000000e+00 1.308000e+03 9.600000e+01 9.600000e+01 +7.820000e+02 0.000000e+00 0.000000e+00 9.500000e+02 5.300000e+01 5.300000e+01 +7.860000e+02 0.000000e+00 0.000000e+00 8.010000e+02 4.800000e+01 4.800000e+01 +7.900000e+02 0.000000e+00 0.000000e+00 8.700000e+02 4.800000e+01 4.800000e+01 +7.940000e+02 0.000000e+00 0.000000e+00 8.140000e+02 4.600000e+01 4.600000e+01 +8.000000e+02 0.000000e+00 0.000000e+00 7.550000e+02 7.100000e+01 7.100000e+01 +8.200000e+02 0.000000e+00 0.000000e+00 5.210000e+02 4.100000e+01 4.100000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CMD_1985_I221309/d02-x01-y02 +IsRef: 1 +Path: /REF/CMD_1985_I221309/d02-x01-y02 +Title: doi:10.17182/hepdata.6886.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.600000e+02 0.000000e+00 0.000000e+00 1.870000e+00 1.600000e-01 1.600000e-01 +3.800000e+02 0.000000e+00 0.000000e+00 2.130000e+00 2.000000e-01 2.000000e-01 +4.100000e+02 0.000000e+00 0.000000e+00 2.370000e+00 1.600000e-01 1.600000e-01 +4.300000e+02 0.000000e+00 0.000000e+00 2.440000e+00 2.400000e-01 2.400000e-01 +4.380000e+02 0.000000e+00 0.000000e+00 2.770000e+00 2.300000e-01 2.300000e-01 +4.700000e+02 0.000000e+00 0.000000e+00 2.770000e+00 1.800000e-01 1.800000e-01 +5.400000e+02 0.000000e+00 0.000000e+00 4.450000e+00 3.000000e-01 3.000000e-01 +5.800000e+02 0.000000e+00 0.000000e+00 5.630000e+00 3.800000e-01 3.800000e-01 +6.200000e+02 0.000000e+00 0.000000e+00 8.620000e+00 5.000000e-01 5.000000e-01 +6.400000e+02 0.000000e+00 0.000000e+00 9.870000e+00 5.500000e-01 5.500000e-01 +6.600000e+02 0.000000e+00 0.000000e+00 1.260000e+01 8.900000e-01 8.900000e-01 +7.000000e+02 0.000000e+00 0.000000e+00 2.537000e+01 2.740000e+00 2.740000e+00 +7.400000e+02 0.000000e+00 0.000000e+00 4.545000e+01 4.090000e+00 4.090000e+00 +7.600000e+02 0.000000e+00 0.000000e+00 4.090000e+01 2.790000e+00 2.790000e+00 +7.700000e+02 0.000000e+00 0.000000e+00 4.395000e+01 1.780000e+00 1.780000e+00 +7.740000e+02 0.000000e+00 0.000000e+00 4.342000e+01 2.010000e+00 2.010000e+00 +7.780000e+02 0.000000e+00 0.000000e+00 4.698000e+01 1.910000e+00 1.910000e+00 +7.800000e+02 0.000000e+00 0.000000e+00 4.501000e+01 3.290000e+00 3.290000e+00 +7.820000e+02 0.000000e+00 0.000000e+00 3.284000e+01 1.840000e+00 1.840000e+00 +7.860000e+02 0.000000e+00 0.000000e+00 2.791000e+01 1.660000e+00 1.660000e+00 +7.900000e+02 0.000000e+00 0.000000e+00 3.054000e+01 1.680000e+00 1.680000e+00 +7.940000e+02 0.000000e+00 0.000000e+00 2.882000e+01 1.640000e+00 1.640000e+00 +8.000000e+02 0.000000e+00 0.000000e+00 2.704000e+01 2.500000e+00 2.500000e+00 +8.200000e+02 0.000000e+00 0.000000e+00 1.939000e+01 1.510000e+00 1.510000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/MD1_1986_I364141.cc b/analyses/pluginNovosibirsk/MD1_1986_I364141.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/MD1_1986_I364141.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MD1_1986_I364141 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MD1_1986_I364141); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MD1_1986_I364141); + + +} diff --git a/analyses/pluginNovosibirsk/MD1_1986_I364141.info b/analyses/pluginNovosibirsk/MD1_1986_I364141.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/MD1_1986_I364141.info @@ -0,0 +1,32 @@ +Name: MD1_1986_I364141 +Year: 1986 +Summary: Measurement of $R$ for energies between 7.2 and 10.34 GeV +Experiment: MD1 +Collider: VEPP-4 +InspireID: 364141 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C70 (1996) 31-38, 1996 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by MD1 for energies between 7.2 and 10.34 GeV . + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Blinov:1993fw +BibTeX: '@article{Blinov:1993fw, + author = "Blinov, A. E. and others", + title = "{The Measurement of R in e+ e- annihilation at + center-of-mass energies between 7.2-GeV and 10.34-GeV}", + journal = "Z. Phys.", + volume = "C70", + year = "1996", + pages = "31-38", + doi = "10.1007/s002880050077", + reportNumber = "BUDKER-INP-1993-54", + SLACcitation = "%%CITATION = ZEPYA,C70,31;%%" +}' diff --git a/analyses/pluginNovosibirsk/MD1_1986_I364141.plot b/analyses/pluginNovosibirsk/MD1_1986_I364141.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/MD1_1986_I364141.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /MD1_1986_I364141/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MD1_1986_I364141/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MD1_1986_I364141/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/MD1_1986_I364141.yoda b/analyses/pluginNovosibirsk/MD1_1986_I364141.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/MD1_1986_I364141.yoda @@ -0,0 +1,48 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MD1_1986_I364141/d01-x01-y01 +IsRef: 1 +Path: /REF/MD1_1986_I364141/d01-x01-y01 +Title: doi:10.17182/hepdata.14321.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.300000e+00 5.000000e-02 5.000000e-02 3.570000e+00 2.321302e-01 2.321302e-01 +7.400000e+00 5.000000e-02 5.000000e-02 3.860000e+00 2.426433e-01 2.426433e-01 +7.500000e+00 5.000000e-02 5.000000e-02 3.890000e+00 2.457175e-01 2.457175e-01 +7.600000e+00 5.000000e-02 5.000000e-02 3.570000e+00 2.389884e-01 2.389884e-01 +7.700000e+00 5.000000e-02 5.000000e-02 3.940000e+00 2.515941e-01 2.515941e-01 +7.800000e+00 5.000000e-02 5.000000e-02 3.590000e+00 2.433963e-01 2.433963e-01 +7.900000e+00 5.000000e-02 5.000000e-02 3.660000e+00 2.476105e-01 2.476105e-01 +8.000000e+00 5.000000e-02 5.000000e-02 3.670000e+00 2.502114e-01 2.502114e-01 +8.100000e+00 5.000000e-02 5.000000e-02 3.730000e+00 2.243993e-01 2.243993e-01 +8.200000e+00 5.000000e-02 5.000000e-02 3.640000e+00 2.238337e-01 2.238337e-01 +8.300000e+00 5.000000e-02 5.000000e-02 3.400000e+00 2.183254e-01 2.183254e-01 +8.400000e+00 5.000000e-02 5.000000e-02 3.630000e+00 2.264351e-01 2.264351e-01 +8.500000e+00 5.000000e-02 5.000000e-02 3.540000e+00 2.260402e-01 2.260402e-01 +8.600000e+00 5.000000e-02 5.000000e-02 3.660000e+00 2.309696e-01 2.309696e-01 +8.700000e+00 5.000000e-02 5.000000e-02 3.440000e+00 1.668452e-01 1.668452e-01 +8.800000e+00 5.000000e-02 5.000000e-02 3.530000e+00 1.707078e-01 1.707078e-01 +8.900000e+00 5.000000e-02 5.000000e-02 3.710000e+00 1.779901e-01 1.779901e-01 +9.000000e+00 5.000000e-02 5.000000e-02 3.670000e+00 1.909496e-01 1.909496e-01 +9.100000e+00 5.000000e-02 5.000000e-02 3.630000e+00 1.901259e-01 1.901259e-01 +9.200000e+00 5.000000e-02 5.000000e-02 3.570000e+00 1.892180e-01 1.892180e-01 +9.300000e+00 5.000000e-02 5.000000e-02 3.600000e+00 1.908429e-01 1.908429e-01 +9.400000e+00 5.000000e-02 5.000000e-02 3.410000e+00 1.657175e-01 1.657175e-01 +9.500000e+00 5.000000e-02 5.000000e-02 3.630000e+00 1.744931e-01 1.744931e-01 +9.600000e+00 5.000000e-02 5.000000e-02 3.550000e+00 1.773797e-01 1.773797e-01 +9.700000e+00 5.000000e-02 5.000000e-02 3.520000e+00 1.768092e-01 1.768092e-01 +9.800000e+00 5.000000e-02 5.000000e-02 3.580000e+00 1.795158e-01 1.795158e-01 +9.900000e+00 5.000000e-02 5.000000e-02 3.490000e+00 1.767871e-01 1.767871e-01 +1.000000e+01 5.000000e-02 5.000000e-02 3.680000e+00 2.039973e-01 2.039973e-01 +1.010000e+01 5.000000e-02 5.000000e-02 3.560000e+00 2.007245e-01 2.007245e-01 +1.020000e+01 5.000000e-02 5.000000e-02 3.490000e+00 1.997941e-01 1.997941e-01 +1.029500e+01 4.500000e-02 4.500000e-02 3.480000e+00 2.814649e-01 2.814649e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MD1_1986_I364141/d02-x01-y01 +IsRef: 1 +Path: /REF/MD1_1986_I364141/d02-x01-y01 +Title: doi:10.17182/hepdata.14321.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +8.795000e+00 1.545000e+00 1.545000e+00 3.578000e+00 2.083382e-01 2.083382e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/ND_1991_I321108.cc b/analyses/pluginNovosibirsk/ND_1991_I321108.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/ND_1991_I321108.cc @@ -0,0 +1,241 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class ND_1991_I321108 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(ND_1991_I321108); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + _nOmegaPi = bookCounter("TMP/OmegaPi"); + _n2Pi = bookCounter("TMP/2Pi"); + _n3Pi = bookCounter("TMP/3Pi"); + _n4PiC = bookCounter("TMP/4PiC"); + _n4PiN = bookCounter("TMP/4PiN"); + _nEtaPiPi = bookCounter("TMP/EtaPiPi"); + _nKC = bookCounter("TMP/KC"); + _nKN = bookCounter("TMP/KN"); + _n5Pi = bookCounter("TMP/5Pi"); + } + + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2) { + if(nCount[211]==1&&nCount[-211]==1) + _n2Pi->fill(event.weight()); + if(nCount[321]==1&&nCount[-321]==1) + _nKC->fill(event.weight()); + if(nCount[310]==1&&nCount[130]==1) + _nKN->fill(event.weight()); + } + else if(ntotal==3) { + if(nCount[211]==1&&nCount[-211]==1&&nCount[111]==1) + _n3Pi->fill(event.weight()); + } + else if(ntotal==4) { + if(nCount[211]==2&&nCount[-211]==2) + _n4PiC->fill(event.weight()); + else if(nCount[211]==1&&nCount[-211]==1&&nCount[111]==2) + _n4PiN->fill(event.weight()); + } + else if(ntotal==5) { + if(nCount[211]==2&&nCount[-211]==2&&nCount[111]==1) + _n5Pi->fill(event.weight()); + } + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the eta + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nEtaPiPi->fill(event.weight()); + } + else if(p.pdgId()==223) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==111) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nOmegaPi->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<15;++ix) { + unsigned int ymax=2; + double sigma(0.),error(0.); + if(ix<=4) { + sigma = _nOmegaPi->val(); + error = _nOmegaPi->err(); + } + else if(ix==5) { + sigma = _n3Pi->val(); + error = _n3Pi->err(); + } + else if(ix==6) { + sigma = _nEtaPiPi->val(); + error = _nEtaPiPi->err(); + } + else if(ix==7) { + sigma = _n4PiC->val(); + error = _n4PiC->err(); + } + else if(ix==8) { + sigma = _n4PiN->val(); + error = _n4PiN->err(); + } + else if(ix==9) { + continue; + } + else if(ix==10) { + ymax=5; + } + else if(ix==11) { + sigma = _n2Pi->val(); + error = _n2Pi->err(); + } + else if(ix==12) { + sigma = _nKC->val(); + error = _nKC->err(); + } + else if(ix==13) { + sigma = _nKN->val(); + error = _nKN->err(); + } + else if(ix==14) { + sigma = _n5Pi->val(); + error = _n5Pi->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + for(unsigned int iy=1;iyval(); + error = _n4PiC->err(); + } + else if(iy==2) { + sigma = _n4PiN->val(); + error = _n4PiN->err(); + } + else if(iy==3) { + sigma = _nOmegaPi->val(); + error = _nOmegaPi->err(); + } + else { + sigma = _n3Pi->val(); + error = _n3Pi->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + } + Scatter2D temphisto(refData(ix, 1, iy)); + Scatter2DPtr mult = bookScatter2D(ix, 1, iy); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nOmegaPi,_n2Pi,_n3Pi,_n4PiC,_n4PiN,_nEtaPiPi,_nKC,_nKN,_n5Pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(ND_1991_I321108); + + +} diff --git a/analyses/pluginNovosibirsk/ND_1991_I321108.info b/analyses/pluginNovosibirsk/ND_1991_I321108.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/ND_1991_I321108.info @@ -0,0 +1,31 @@ +Name: ND_1991_I321108 +Year: 1991 +Summary: Cross sections for $e^+e^-\to$ exclusive hadronic states between 0.5 and 1.4 GeV. +Experiment: ND +Collider: VEPP-2M +InspireID: 321108 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - PRep 202,99 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$, $K^+K^-$, $K^0_SK^0_L$, $\pi^+\pi^-\pi^0$, + $2\pi^+2\pi^-$, $\pi^+\pi^-2\pi^0$, $\omega\pi^0$, $\eta\pi^+\pi^-$ and $2\pi^+2\pi^-\pi^0$ by ND for energies between 0.5 and 1.4 GeV.' +Keywords: +Keywords: [] +BibKey: Dolinsky:1991vq +BibTeX: '@article{Dolinsky:1991vq, + author = "Dolinsky, S. I. and others", + title = "{Summary of experiments with the neutral detector at the + e+ e- storage ring VEPP-2M}", + journal = "Phys. Rept.", + volume = "202", + year = "1991", + pages = "99-170", + doi = "10.1016/0370-1573(91)90127-8", + SLACcitation = "%%CITATION = PRPLC,202,99;%%" +}' diff --git a/analyses/pluginNovosibirsk/ND_1991_I321108.plot b/analyses/pluginNovosibirsk/ND_1991_I321108.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/ND_1991_I321108.plot @@ -0,0 +1,96 @@ +BEGIN PLOT /ND_1991_I321108/d01-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d02-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d03-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d04-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d10-x01-y03 +Title=$\sigma(e^+e^-\to \omega\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d05-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d10-x01-y04 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d06-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\eta)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\eta)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d07-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d10-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d08-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d10-x01-y02 +Title=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d11-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d12-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d13-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /ND_1991_I321108/d14-x01-y02 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/ND_1991_I321108.yoda b/analyses/pluginNovosibirsk/ND_1991_I321108.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/ND_1991_I321108.yoda @@ -0,0 +1,577 @@ +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d01-x01-y01 +Path=/REF/ND_1991_I321108/d01-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +1.02 0.0 0.0 8.7 1.0 1.0 +1.05 0.0 0.0 9.1 2.1 2.1 +1.07 0.0 0.0 12.6 2.6 2.6 +1.09 0.0 0.0 12.8 2.6 2.6 + +1.11 0.0 0.0 20.9 6.2 6.2 +1.13 0.0 0.0 10.8 4.9 4.9 +1.15 0.0 0.0 14.4 5.0 5.0 +1.17 0.0 0.0 9.4 4.3 4.3 +1.19 0.0 0.0 8.1 4.0 4.0 + +1.21 0.0 0.0 18.1 3.7 3.7 +1.23 0.0 0.0 15.0 4.9 4.9 +1.25 0.0 0.0 20.3 6.4 6.4 +1.27 0.0 0.0 15.5 5.4 5.4 +1.29 0.0 0.0 14.8 3.0 3.0 + +1.31 0.0 0.0 15.0 3.3 3.3 +1.33 0.0 0.0 14.7 3.8 3.8 +1.35 0.0 0.0 14.6 3.4 3.4 +1.37 0.0 0.0 21.9 3.9 3.9 +1.39 0.0 0.0 19.1 4.0 4.0 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d02-x01-y01 +Path=/REF/ND_1991_I321108/d02-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +0.93 0.0 0.0 6.6 4.5 4.5 +0.95 0.0 0.0 4.4 1.2 1.2 +0.97 0.0 0.0 6.1 2.5 2.5 +0.99 0.0 0.0 9.7 2.7 2.7 + + + + +1.09 0.0 0.0 12.5 3.8 3.8 + +1.11 0.0 0.0 14.5 3.5 3.5 +1.13 0.0 0.0 8.5 2.3 2.3 +1.15 0.0 0.0 11.5 3.2 3.2 +1.17 0.0 0.0 13.5 3.4 3.4 +1.19 0.0 0.0 7.6 2.5 2.5 + +1.21 0.0 0.0 12.6 3.4 3.4 +1.23 0.0 0.0 22.2 4.4 4.4 +1.25 0.0 0.0 14.9 3.7 3.7 +1.27 0.0 0.0 10.0 3.3 3.3 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d03-x01-y01 +Path=/REF/ND_1991_I321108/d03-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +0.93 0.0 0.0 6.6 4.5 4.5 +0.95 0.0 0.0 4.4 1.2 1.2 +0.97 0.0 0.0 6.1 2.5 2.5 +0.99 0.0 0.0 9.7 2.7 2.7 + +1.02 0.0 0.0 8.7 1.0 1.0 +1.05 0.0 0.0 9.1 2.1 2.1 +1.07 0.0 0.0 12.6 2.6 2.6 +1.09 0.0 0.0 12.8 2.1 2.1 + +1.11 0.0 0.0 17.2 3.2 3.2 +1.13 0.0 0.0 9.3 2.2 2.2 +1.15 0.0 0.0 12.8 2.8 2.8 +1.17 0.0 0.0 11.9 2.7 2.7 +1.19 0.0 0.0 7.8 2.2 2.2 + +1.21 0.0 0.0 15.9 2.5 2.5 +1.23 0.0 0.0 19.1 3.2 3.2 +1.25 0.0 0.0 17.1 3.3 3.3 +1.27 0.0 0.0 12.5 2.9 2.9 +1.29 0.0 0.0 14.8 3.0 3.0 + +1.31 0.0 0.0 15.0 3.3 3.3 +1.33 0.0 0.0 14.7 3.8 3.8 +1.35 0.0 0.0 14.6 3.4 3.4 +1.37 0.0 0.0 21.9 3.9 3.9 +1.39 0.0 0.0 19.1 4.0 4.0 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d04-x01-y01 +Path=/REF/ND_1991_I321108/d04-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +1.0 0.0 0.0 7.8 3.1 3.1 +1.1 0.0 0.0 11.6 3.2 3.2 +1.2 0.0 0.0 8.1 3.8 3.8 +1.3 0.0 0.0 14.7 3.2 3.2 +1.4 0.0 0.0 12.1 2.8 2.8 +1.5 0.0 0.0 9.7 2.9 2.9 +1.6 0.0 0.0 3.3 3.0 3.0 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d05-x01-y01 +Path=/REF/ND_1991_I321108/d05-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +0.661 0.0 0.0 0.0 0.0 2.4 +0.671 0.0 0.0 0.0 0.0 2.4 +0.681 0.0 0.0 1.5 1.5 4.1 +0.691 0.0 0.0 1.4 1.4 4.1 +0.701 0.0 0.0 1.6 1.3 2.7 +0.711 0.0 0.0 1.1 1.3 3.6 +0.725 0.0 0.0 4.3 1.1 1.8 +0.735 0.0 0.0 6.7 1.3 2.0 +0.745 0.0 0.0 14.1 1.7 1.7 +0.755 0.0 0.0 23.4 2.9 2.9 +0.765 0.0 0.0 63.9 4.8 4.8 +0.805 0.0 0.0 74.9 3.5 3.5 +0.815 0.0 0.0 41.7 2.0 2.0 +0.825 0.0 0.0 28.2 1.6 1.6 +0.831 0.0 0.0 24.8 3.3 3.3 +0.841 0.0 0.0 18.9 2.7 2.7 +0.851 0.0 0.0 13.5 2.4 2.4 +0.861 0.0 0.0 9.8 2.0 2.0 +0.871 0.0 0.0 12.0 2.2 2.2 +0.881 0.0 0.0 11.9 2.2 2.2 +0.891 0.0 0.0 8.8 2.0 2.0 +0.901 0.0 0.0 6.6 1.7 1.7 +0.911 0.0 0.0 9.2 2.1 2.1 +0.921 0.0 0.0 11.6 2.2 2.2 +0.943 0.0 0.0 4.2 1.6 1.6 +0.956 0.0 0.0 8.1 0.8 0.8 +0.963 0.0 0.0 7.7 2.1 2.1 +0.973 0.0 0.0 11.3 3.2 3.2 +0.983 0.0 0.0 10.1 2.5 2.5 +0.993 0.0 0.0 13.8 4.7 4.7 +1.003 0.0 0.0 25.6 3.5 3.5 +1.036 0.0 0.0 5.0 3.3 3.3 +1.059 0.0 0.0 1.4 1.1 1.1 +1.099 0.0 0.0 3.2 1.0 1.0 +1.139 0.0 0.0 2.2 0.9 0.9 +1.179 0.0 0.0 2.3 0.9 0.9 +1.219 0.0 0.0 3.4 0.8 0.8 +1.259 0.0 0.0 2.2 1.0 1.0 +1.299 0.0 0.0 3.3 0.9 0.9 +1.339 0.0 0.0 4.3 1.1 1.1 +1.379 0.0 0.0 3.8 0.9 0.9 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d06-x01-y01 +Path=/REF/ND_1991_I321108/d06-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +1.075 0.0 0.0 0.0 0.5 0.5 +1.15 0.0 0.0 0.0 0.5 0.5 +1.25 0.0 0.0 0.2 0.4 0.4 +1.325 0.0 0.0 0.3 0.5 0.5 +1.375 0.0 0.0 1.2 0.6 0.6 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d07-x01-y01 +Path=/REF/ND_1991_I321108/d07-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +1.005 0.0 0.0 1.9 0.3 0.3 +1.04 0.0 0.0 2.2 0.2 0.2 +1.06 0.0 0.0 2.4 0.5 0.5 +1.08 0.0 0.0 2.2 0.5 0.5 +1.1 0.0 0.0 4.2 0.7 0.7 +1.12 0.0 0.0 4.4 0.7 0.7 +1.14 0.0 0.0 4.1 0.6 0.6 +1.16 0.0 0.0 6.7 0.7 0.7 +1.18 0.0 0.0 7.8 0.8 0.8 +1.2 0.0 0.0 9.0 0.6 0.6 +1.22 0.0 0.0 12.4 0.7 0.7 +1.24 0.0 0.0 15.5 0.7 0.7 +1.26 0.0 0.0 16.1 1.1 1.1 +1.28 0.0 0.0 17.1 0.7 0.7 +1.3 0.0 0.0 17.2 0.6 0.6 +1.32 0.0 0.0 20.2 0.7 0.7 +1.34 0.0 0.0 22.5 0.8 0.8 +1.36 0.0 0.0 23.3 0.7 0.7 +1.38 0.0 0.0 25.4 0.8 0.8 +1.395 0.0 0.0 25.5 1.2 1.2 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d08-x01-y01 +Path=/REF/ND_1991_I321108/d08-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +0.91 0.0 0.0 0.46 0.12 0.12 +0.955 0.0 0.0 3.5 0.3 0.3 +0.98 0.0 0.0 5.0 0.7 0.7 +1.0 0.0 0.0 9.3 1.1 1.1 +1.005 0.0 0.0 9.0 1.1 1.1 +1.04 0.0 0.0 11.4 1.0 1.0 +1.06 0.0 0.0 11.9 1.8 1.8 +1.08 0.0 0.0 16.8 2.2 2.2 +1.1 0.0 0.0 22.3 2.8 2.8 +1.12 0.0 0.0 21.6 2.9 2.9 +1.14 0.0 0.0 21.5 2.6 2.6 +1.16 0.0 0.0 28.4 2.8 2.8 +1.18 0.0 0.0 27.4 3.0 3.0 +1.2 0.0 0.0 25.5 2.1 2.1 +1.22 0.0 0.0 30.8 2.2 2.2 +1.24 0.0 0.0 33.9 3.1 3.1 +1.26 0.0 0.0 28.5 2.8 2.8 +1.28 0.0 0.0 36.0 2.3 2.3 +1.3 0.0 0.0 37.2 1.9 1.9 +1.32 0.0 0.0 40.3 2.2 2.2 +1.34 0.0 0.0 41.4 2.3 2.3 +1.36 0.0 0.0 41.1 1.9 1.9 +1.38 0.0 0.0 42.3 2.1 2.1 +1.395 0.0 0.0 44.9 3.2 3.2 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d09-x01-y01 +Path=/REF/ND_1991_I321108/d09-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +1.005 0.0 0.0 0.86 0.48 0.48 +1.04 0.0 0.0 0.88 0.41 0.41 +1.06 0.0 0.0 1.14 0.87 0.87 +1.08 0.0 0.0 0.35 0.14 0.14 +1.1 0.0 0.0 0.38 0.11 0.11 +1.12 0.0 0.0 0.45 0.15 0.15 +1.14 0.0 0.0 0.44 0.14 0.14 +1.16 0.0 0.0 0.43 0.09 0.09 +1.18 0.0 0.0 0.54 0.13 0.13 +1.2 0.0 0.0 0.74 0.14 0.14 +1.22 0.0 0.0 0.72 0.1 0.1 +1.24 0.0 0.0 0.78 0.13 0.13 +1.26 0.0 0.0 1.12 0.24 0.24 +1.28 0.0 0.0 0.8 0.09 0.09 +1.3 0.0 0.0 0.77 0.07 0.07 +1.32 0.0 0.0 0.8 0.05 0.05 +1.34 0.0 0.0 0.86 0.08 0.08 +1.36 0.0 0.0 0.91 0.07 0.07 +1.38 0.0 0.0 0.96 0.08 0.08 +1.395 0.0 0.0 0.89 0.11 0.11 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d10-x01-y01 +Path=/REF/ND_1991_I321108/d10-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ + + + + + + + + + + +1.05 0.0 0.0 2.0 0.2 0.2 +1.07 0.0 0.0 2.3 0.5 0.5 +1.09 0.0 0.0 2.4 0.5 0.5 +1.11 0.0 0.0 4.8 0.7 0.7 +1.13 0.0 0.0 5.1 0.8 0.8 +1.15 0.0 0.0 4.7 0.6 0.6 +1.17 0.0 0.0 7.6 0.7 0.7 +1.19 0.0 0.0 8.8 0.8 0.8 +1.21 0.0 0.0 10.0 0.6 0.6 +1.23 0.0 0.0 13.5 0.7 0.7 +1.25 0.0 0.0 16.7 0.7 0.7 +1.27 0.0 0.0 17.2 1.1 1.1 +1.29 0.0 0.0 18.0 0.7 0.7 +1.31 0.0 0.0 17.9 0.6 0.6 +1.33 0.0 0.0 20.8 0.7 0.7 +1.35 0.0 0.0 23.0 0.8 0.8 +1.37 0.0 0.0 23.5 0.7 0.7 +1.39 0.0 0.0 25.4 0.7 0.7 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d10-x01-y02 +Path=/REF/ND_1991_I321108/d10-x01-y02 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ + + +0.85 0.0 0.0 0.3 0.8 0.8 +0.87 0.0 0.0 0.8 0.6 0.6 +0.89 0.0 0.0 0.8 0.7 0.7 +0.91 0.0 0.0 0.2 0.4 0.4 +0.93 0.0 0.0 2.1 1.5 1.5 +0.95 0.0 0.0 4.2 0.6 0.6 +0.97 0.0 0.0 6.4 0.7 0.7 +0.99 0.0 0.0 8.8 1.5 1.5 +1.05 0.0 0.0 13.2 0.9 0.9 +1.07 0.0 0.0 12.9 1.4 1.4 +1.09 0.0 0.0 18.0 2.3 2.3 +1.11 0.0 0.0 23.6 2.9 2.9 +1.13 0.0 0.0 22.7 3.0 3.0 +1.15 0.0 0.0 22.5 2.7 2.7 +1.17 0.0 0.0 29.5 2.9 2.9 +1.19 0.0 0.0 28.4 3.1 3.1 +1.21 0.0 0.0 26.3 2.1 2.1 +1.23 0.0 0.0 31.7 2.2 2.2 +1.25 0.0 0.0 34.8 3.1 3.1 +1.27 0.0 0.0 29.2 2.8 2.8 +1.29 0.0 0.0 36.8 2.3 2.3 +1.31 0.0 0.0 38.0 1.9 1.9 +1.33 0.0 0.0 41.1 2.2 2.2 +1.35 0.0 0.0 42.2 2.3 2.3 +1.37 0.0 0.0 41.9 1.9 1.9 +1.39 0.0 0.0 43.5 1.8 1.8 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d10-x01-y03 +Path=/REF/ND_1991_I321108/d10-x01-y03 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ + + + + + + +0.93 0.0 0.0 6.6 4.5 4.5 +0.95 0.0 0.0 4.4 1.2 1.2 +0.97 0.0 0.0 6.1 2.5 2.5 +0.99 0.0 0.0 9.7 2.7 2.7 +1.05 0.0 0.0 9.1 2.1 2.1 +1.07 0.0 0.0 12.6 2.6 2.6 +1.09 0.0 0.0 12.8 2.1 2.1 +1.11 0.0 0.0 17.2 3.2 3.2 +1.13 0.0 0.0 9.3 2.2 2.2 +1.15 0.0 0.0 12.8 2.8 2.8 +1.17 0.0 0.0 11.9 2.7 2.7 +1.19 0.0 0.0 7.8 2.2 2.2 +1.21 0.0 0.0 15.9 2.5 2.5 +1.23 0.0 0.0 19.1 3.2 3.2 +1.25 0.0 0.0 17.1 3.3 3.3 +1.27 0.0 0.0 12.5 2.9 2.9 +1.29 0.0 0.0 14.8 3.0 3.0 +1.31 0.0 0.0 15.0 3.3 3.3 +1.33 0.0 0.0 14.7 3.8 3.8 +1.35 0.0 0.0 14.6 3.4 3.4 +1.37 0.0 0.0 21.9 3.9 3.9 +1.39 0.0 0.0 19.1 4.0 4.0 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d10-x01-y04 +Path=/REF/ND_1991_I321108/d10-x01-y04 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +0.81 0.0 0.0 50.9 1.8 1.8 +0.83 0.0 0.0 24.7 1.4 1.4 +0.85 0.0 0.0 14.1 1.8 1.8 +0.87 0.0 0.0 9.3 1.5 1.5 +0.89 0.0 0.0 9.3 1.5 1.5 +0.91 0.0 0.0 7.4 1.4 1.4 +0.93 0.0 0.0 13.2 2.5 2.5 +0.95 0.0 0.0 7.2 0.7 0.7 +0.97 0.0 0.0 9.0 1.9 1.9 +0.99 0.0 0.0 10.4 2.3 2.3 +1.05 0.0 0.0 0.9 1.7 1.7 +1.07 0.0 0.0 1.7 1.4 1.4 +1.09 0.0 0.0 3.1 1.2 1.2 +1.11 0.0 0.0 3.6 1.8 1.8 +1.13 0.0 0.0 1.9 1.3 1.3 +1.15 0.0 0.0 2.6 1.5 1.5 +1.17 0.0 0.0 1.4 1.4 1.4 +1.19 0.0 0.0 3.5 1.5 1.5 +1.21 0.0 0.0 3.2 1.1 1.1 +1.23 0.0 0.0 3.8 1.4 1.4 +1.25 0.0 0.0 1.4 1.3 1.3 +1.27 0.0 0.0 4.9 2.4 2.4 +1.29 0.0 0.0 4.1 1.4 1.4 +1.31 0.0 0.0 2.6 1.3 1.3 +1.33 0.0 0.0 3.1 1.6 1.6 +1.35 0.0 0.0 5.6 1.6 1.6 +1.37 0.0 0.0 4.4 1.4 1.4 +1.39 0.0 0.0 3.4 1.4 1.4 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d11-x01-y01 +Path=/REF/ND_1991_I321108/d11-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +0.81 0.0 0.0 684.0 15.0 15.0 +0.83 0.0 0.0 506.0 11.0 11.0 +0.85 0.0 0.0 373.0 12.0 12.0 +0.87 0.0 0.0 279.0 7.0 7.0 +0.89 0.0 0.0 205.0 6.0 6.0 +0.91 0.0 0.0 162.0 5.0 5.0 +0.93 0.0 0.0 120.0 5.0 5.0 +0.95 0.0 0.0 97.3 3.7 3.7 +0.97 0.0 0.0 78.0 3.1 3.1 +0.99 0.0 0.0 62.4 2.5 2.5 +1.05 0.0 0.0 44.5 3.0 3.0 +1.07 0.0 0.0 37.6 2.4 2.4 +1.09 0.0 0.0 32.1 2.0 2.0 +1.11 0.0 0.0 28.5 2.0 2.0 +1.13 0.0 0.0 23.9 1.8 1.8 +1.15 0.0 0.0 22.3 2.7 2.7 +1.17 0.0 0.0 17.7 1.7 1.7 +1.19 0.0 0.0 17.8 1.9 1.9 +1.21 0.0 0.0 13.0 1.6 1.6 +1.23 0.0 0.0 14.0 1.8 1.8 +1.25 0.0 0.0 11.3 1.4 1.4 +1.27 0.0 0.0 6.7 1.0 1.0 +1.29 0.0 0.0 7.8 1.1 1.1 +1.31 0.0 0.0 8.2 1.1 1.1 +1.33 0.0 0.0 6.5 1.2 1.2 +1.35 0.0 0.0 4.2 0.7 0.7 +1.37 0.0 0.0 3.0 0.6 0.6 +1.39 0.0 0.0 2.8 0.5 0.5 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d12-x01-y01 +Path=/REF/ND_1991_I321108/d12-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +1.05 0.0 0.0 52.0 10.2 10.2 +1.07 0.0 0.0 34.6 7.8 7.8 +1.09 0.0 0.0 21.0 3.9 3.9 +1.11 0.0 0.0 8.2 6.0 6.0 +1.13 0.0 0.0 10.0 2.6 2.6 +1.15 0.0 0.0 8.6 1.3 1.3 +1.17 0.0 0.0 8.0 1.1 1.1 +1.19 0.0 0.0 8.1 0.9 0.9 +1.21 0.0 0.0 5.2 0.7 0.7 +1.23 0.0 0.0 6.4 0.8 0.8 +1.25 0.0 0.0 5.9 0.7 0.7 +1.27 0.0 0.0 6.9 0.7 0.7 +1.29 0.0 0.0 5.8 0.7 0.7 +1.31 0.0 0.0 6.6 1.1 1.1 +1.33 0.0 0.0 5.8 0.8 0.8 +1.35 0.0 0.0 6.1 0.6 0.6 +1.37 0.0 0.0 6.0 0.6 0.6 +1.39 0.0 0.0 5.5 0.6 0.6 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d13-x01-y01 +Path=/REF/ND_1991_I321108/d13-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +1.09 0.0 0.0 4.2 1.4 1.4 +1.17 0.0 0.0 3.6 3.4 3.4 +1.21 0.0 0.0 1.2 0.9 0.9 +1.31 0.0 0.0 0.0 0.3 0.3 +1.35 0.0 0.0 1.2 1.7 1.7 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d14-x01-y01 +Path=/REF/ND_1991_I321108/d14-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +1.09 0.0 0.0 0.0 2.5 2.5 +1.21 0.0 0.0 0.3 0.4 0.4 +1.27 0.0 0.0 0.6 0.5 0.5 +1.35 0.0 0.0 1.0 0.5 0.5 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d15-x01-y01 +Path=/REF/ND_1991_I321108/d15-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +0.81 0.0 0.0 5.545 0.111 0.111 +0.83 0.0 0.0 4.204 0.086 0.086 +0.85 0.0 0.0 3.219 0.101 0.101 +0.87 0.0 0.0 2.516 0.06 0.06 +0.89 0.0 0.0 1.958 0.054 0.054 +0.91 0.0 0.0 1.617 0.047 0.047 +0.93 0.0 0.0 1.355 0.057 0.057 +0.95 0.0 0.0 1.134 0.039 0.039 +0.97 0.0 0.0 1.018 0.041 0.041 +0.99 0.0 0.0 0.93 0.043 0.043 +1.05 0.0 0.0 1.492 0.142 0.142 +1.07 0.0 0.0 1.245 0.117 0.117 +1.09 0.0 0.0 1.118 0.081 0.081 +1.11 0.0 0.0 1.056 0.11 0.11 +1.13 0.0 0.0 0.998 0.092 0.092 +1.15 0.0 0.0 0.995 0.092 0.092 +1.17 0.0 0.0 1.09 0.081 0.081 +1.19 0.0 0.0 1.14 0.078 0.078 +1.21 0.0 0.0 1.021 0.054 0.054 +1.23 0.0 0.0 1.264 0.062 0.062 +1.25 0.0 0.0 1.32 0.071 0.071 +1.27 0.0 0.0 1.257 0.078 0.078 +1.29 0.0 0.0 1.424 0.061 0.061 +1.31 0.0 0.0 1.486 0.058 0.058 +1.33 0.0 0.0 1.622 0.066 0.066 +1.35 0.0 0.0 1.774 0.075 0.075 +1.37 0.0 0.0 1.789 0.068 0.068 +1.39 0.0 0.0 1.877 0.068 0.068 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d16-x01-y01 +Path=/REF/ND_1991_I321108/d16-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +0.81 0.0 0.0 0.385 0.014 0.014 +0.83 0.0 0.0 0.196 0.011 0.011 +0.85 0.0 0.0 0.117 0.015 0.015 +0.87 0.0 0.0 0.081 0.013 0.013 +0.89 0.0 0.0 0.085 0.013 0.013 +0.91 0.0 0.0 0.071 0.013 0.013 +0.93 0.0 0.0 0.131 0.025 0.025 +0.95 0.0 0.0 0.075 0.008 0.008 +0.97 0.0 0.0 0.098 0.021 0.021 +0.99 0.0 0.0 0.118 0.027 0.027 +1.05 0.0 0.0 0.526 0.136 0.136 +1.07 0.0 0.0 0.358 0.111 0.111 +1.09 0.0 0.0 0.228 0.069 0.069 +1.11 0.0 0.0 0.079 0.098 0.098 +1.13 0.0 0.0 0.096 0.076 0.076 +1.15 0.0 0.0 0.097 0.073 0.073 +1.17 0.0 0.0 0.103 0.062 0.062 +1.19 0.0 0.0 0.123 0.05 0.05 +1.21 0.0 0.0 0.082 0.03 0.03 +1.23 0.0 0.0 0.109 0.036 0.036 +1.25 0.0 0.0 0.084 0.034 0.034 +1.27 0.0 0.0 0.204 0.051 0.051 +1.29 0.0 0.0 0.141 0.033 0.033 +1.31 0.0 0.0 0.129 0.037 0.037 +1.33 0.0 0.0 0.149 0.04 0.04 +1.35 0.0 0.0 0.255 0.052 0.052 +1.37 0.0 0.0 0.243 0.05 0.05 +1.39 0.0 0.0 0.219 0.051 0.051 +# END YODA_SCATTER2D + + +# BEGIN YODA_SCATTER2D /REF/ND_1991_I321108/d17-x01-y01 +Path=/REF/ND_1991_I321108/d17-x01-y01 +Type=Scatter2D +# xval xerr- xerr+ yval yerr- yerr+ +0.81 0.0 0.0 5.161 0.11 0.11 +0.83 0.0 0.0 4.009 0.085 0.085 +0.85 0.0 0.0 3.102 0.1 0.1 +0.87 0.0 0.0 2.435 0.058 0.058 +0.89 0.0 0.0 1.873 0.053 0.053 +0.91 0.0 0.0 1.547 0.045 0.045 +0.93 0.0 0.0 1.224 0.051 0.051 +0.95 0.0 0.0 1.059 0.038 0.038 +0.97 0.0 0.0 0.92 0.035 0.035 +0.99 0.0 0.0 0.812 0.034 0.034 +1.05 0.0 0.0 0.965 0.042 0.042 +1.07 0.0 0.0 0.887 0.039 0.039 +1.09 0.0 0.0 0.89 0.043 0.043 +1.11 0.0 0.0 0.977 0.052 0.052 +1.13 0.0 0.0 0.902 0.054 0.054 +1.15 0.0 0.0 0.898 0.061 0.061 +1.17 0.0 0.0 0.987 0.055 0.055 +1.19 0.0 0.0 1.017 0.061 0.061 +1.21 0.0 0.0 0.939 0.048 0.048 +1.23 0.0 0.0 1.156 0.053 0.053 +1.25 0.0 0.0 1.236 0.064 0.064 +1.27 0.0 0.0 1.054 0.06 0.06 +1.29 0.0 0.0 1.283 0.052 0.052 +1.31 0.0 0.0 1.357 0.047 0.047 +1.33 0.0 0.0 1.473 0.055 0.055 +1.35 0.0 0.0 1.518 0.055 0.055 +1.37 0.0 0.0 1.546 0.047 0.047 +1.39 0.0 0.0 1.658 0.045 0.045 +# END YODA_SCATTER2D + + diff --git a/analyses/pluginNovosibirsk/OLYA_1981_I173076.cc b/analyses/pluginNovosibirsk/OLYA_1981_I173076.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/OLYA_1981_I173076.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/FastJets.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class OLYA_1981_I173076 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(OLYA_1981_I173076); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nkaon = bookCounter("TMP/kaon"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::KPLUS) vetoEvent; + } + _nkaon->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nkaon->val(); + double error = _nkaon->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nkaon; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(OLYA_1981_I173076); + + +} diff --git a/analyses/pluginNovosibirsk/OLYA_1981_I173076.info b/analyses/pluginNovosibirsk/OLYA_1981_I173076.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/OLYA_1981_I173076.info @@ -0,0 +1,32 @@ +Name: OLYA_1981_I173076 +Year: 1981 +Summary: Cross section for $e^+e^-\to K^+K^-$ at energies between 1. and 1.4 GeV +Experiment: OLYA +Collider: VEPP-2M +InspireID: 173076 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D76 (2007) 072012, 2007 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-$ at energies between 1. and 1.4 GeV' +Keywords: +BibKey: Ivanov:1981wf +BibTeX: '@article{Ivanov:1981wf, + author = "Ivanov, P. M. and Kurdadze, L. M. and Lelchuk, M. {\relax + Yu}. and Sidorov, V. A. and Skrinsky, A. N. and + Chilingarov, A. G. and Shatunov, {\relax Yu}. M. and + Shvarts, B. A. and Eidelman, S. I.", + title = "{Measurement of the Charged Kaon Form-factor in the + Energy Range 1.0-{GeV} to 1.4-{GeV}}", + journal = "Phys. Lett.", + volume = "107B", + year = "1981", + pages = "297-300", + doi = "10.1016/0370-2693(81)90834-0", + SLACcitation = "%%CITATION = PHLTA,107B,297;%%" +}' diff --git a/analyses/pluginNovosibirsk/OLYA_1981_I173076.plot b/analyses/pluginNovosibirsk/OLYA_1981_I173076.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/OLYA_1981_I173076.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /OLYA_1981_I173076/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/OLYA_1981_I173076.yoda b/analyses/pluginNovosibirsk/OLYA_1981_I173076.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/OLYA_1981_I173076.yoda @@ -0,0 +1,76 @@ +BEGIN YODA_SCATTER2D_V2 /REF/OLYA_1981_I173076/d01-x01-y01 +IsRef: 1 +Path: /REF/OLYA_1981_I173076/d01-x01-y01 +Title: doi:10.17182/hepdata.31025.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.017000e+00 0.000000e+00 0.000000e+00 9.090000e+02 2.050000e+02 2.050000e+02 +1.018000e+00 0.000000e+00 0.000000e+00 1.121000e+03 2.000000e+02 2.000000e+02 +1.019000e+00 0.000000e+00 0.000000e+00 1.910000e+03 3.030000e+02 3.030000e+02 +1.020000e+00 0.000000e+00 0.000000e+00 1.987000e+03 2.530000e+02 2.530000e+02 +1.021000e+00 0.000000e+00 0.000000e+00 1.536000e+03 2.270000e+02 2.270000e+02 +1.022000e+00 0.000000e+00 0.000000e+00 8.010000e+02 2.430000e+02 2.430000e+02 +1.023000e+00 0.000000e+00 0.000000e+00 8.000000e+02 1.460000e+02 1.460000e+02 +1.024000e+00 0.000000e+00 0.000000e+00 3.600000e+02 7.800000e+01 7.800000e+01 +1.029000e+00 0.000000e+00 0.000000e+00 1.540000e+02 3.200000e+01 3.200000e+01 +1.032000e+00 0.000000e+00 0.000000e+00 5.000000e+01 1.700000e+01 1.700000e+01 +1.036000e+00 0.000000e+00 0.000000e+00 9.500000e+01 1.900000e+01 1.900000e+01 +1.040000e+00 0.000000e+00 0.000000e+00 4.800000e+01 1.700000e+01 1.700000e+01 +1.050000e+00 0.000000e+00 0.000000e+00 5.700000e+01 1.300000e+01 1.300000e+01 +1.060000e+00 0.000000e+00 0.000000e+00 3.770000e+01 8.100000e+00 8.100000e+00 +1.080000e+00 0.000000e+00 0.000000e+00 2.290000e+01 4.100000e+00 4.100000e+00 +1.099000e+00 0.000000e+00 0.000000e+00 8.900000e+00 6.200000e+00 6.200000e+00 +1.130000e+00 1.000000e-02 1.000000e-02 9.950000e+00 2.550000e+00 2.550000e+00 +1.150000e+00 1.000000e-02 1.000000e-02 8.560000e+00 1.340000e+00 1.340000e+00 +1.170000e+00 1.000000e-02 1.000000e-02 7.980000e+00 1.080000e+00 1.080000e+00 +1.190000e+00 1.000000e-02 1.000000e-02 8.140000e+00 9.000000e-01 9.000000e-01 +1.210000e+00 1.000000e-02 1.000000e-02 5.160000e+00 7.000000e-01 7.000000e-01 +1.230000e+00 1.000000e-02 1.000000e-02 6.390000e+00 7.900000e-01 7.900000e-01 +1.250000e+00 1.000000e-02 1.000000e-02 5.940000e+00 7.300000e-01 7.300000e-01 +1.270000e+00 1.000000e-02 1.000000e-02 6.940000e+00 7.300000e-01 7.300000e-01 +1.290000e+00 1.000000e-02 1.000000e-02 5.770000e+00 7.100000e-01 7.100000e-01 +1.310000e+00 1.000000e-02 1.000000e-02 6.580000e+00 1.130000e+00 1.130000e+00 +1.330000e+00 1.000000e-02 1.000000e-02 5.800000e+00 8.300000e-01 8.300000e-01 +1.350000e+00 1.000000e-02 1.000000e-02 6.120000e+00 6.200000e-01 6.200000e-01 +1.370000e+00 1.000000e-02 1.000000e-02 5.980000e+00 6.300000e-01 6.300000e-01 +1.390000e+00 1.000000e-02 1.000000e-02 5.500000e+00 6.000000e-01 6.000000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/OLYA_1981_I173076/d01-x01-y02 +IsRef: 1 +Path: /REF/OLYA_1981_I173076/d01-x01-y02 +Title: doi:10.17182/hepdata.31025.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.017000e+00 0.000000e+00 0.000000e+00 3.148000e+03 7.100000e+02 7.100000e+02 +1.018000e+00 0.000000e+00 0.000000e+00 3.697000e+03 6.590000e+02 6.590000e+02 +1.019000e+00 0.000000e+00 0.000000e+00 6.021000e+03 9.550000e+02 9.550000e+02 +1.020000e+00 0.000000e+00 0.000000e+00 6.005000e+03 7.640000e+02 7.640000e+02 +1.021000e+00 0.000000e+00 0.000000e+00 4.459000e+03 6.600000e+02 6.600000e+02 +1.022000e+00 0.000000e+00 0.000000e+00 2.238000e+03 6.780000e+02 6.780000e+02 +1.023000e+00 0.000000e+00 0.000000e+00 2.178000e+03 3.980000e+02 3.980000e+02 +1.024000e+00 0.000000e+00 0.000000e+00 9.110000e+02 1.980000e+02 1.980000e+02 +1.029000e+00 0.000000e+00 0.000000e+00 3.410000e+02 7.000000e+01 7.000000e+01 +1.032000e+00 0.000000e+00 0.000000e+00 9.900000e+01 3.300000e+01 3.300000e+01 +1.036000e+00 0.000000e+00 0.000000e+00 1.670000e+02 3.300000e+01 3.300000e+01 +1.040000e+00 0.000000e+00 0.000000e+00 7.700000e+01 2.600000e+01 2.600000e+01 +1.050000e+00 0.000000e+00 0.000000e+00 7.300000e+01 1.600000e+01 1.600000e+01 +1.060000e+00 0.000000e+00 0.000000e+00 4.060000e+01 8.700000e+00 8.700000e+00 +1.080000e+00 0.000000e+00 0.000000e+00 1.860000e+01 3.300000e+00 3.300000e+00 +1.099000e+00 0.000000e+00 0.000000e+00 5.800000e+00 4.100000e+00 4.100000e+00 +1.130000e+00 1.000000e-02 1.000000e-02 5.090000e+00 1.310000e+00 1.310000e+00 +1.150000e+00 1.000000e-02 1.000000e-02 3.870000e+00 6.100000e-01 6.100000e-01 +1.170000e+00 1.000000e-02 1.000000e-02 3.260000e+00 4.400000e-01 4.400000e-01 +1.190000e+00 1.000000e-02 1.000000e-02 3.050000e+00 3.400000e-01 3.400000e-01 +1.210000e+00 1.000000e-02 1.000000e-02 1.800000e+00 2.400000e-01 2.400000e-01 +1.230000e+00 1.000000e-02 1.000000e-02 2.100000e+00 2.600000e-01 2.600000e-01 +1.250000e+00 1.000000e-02 1.000000e-02 1.850000e+00 2.300000e-01 2.300000e-01 +1.270000e+00 1.000000e-02 1.000000e-02 2.070000e+00 2.200000e-01 2.200000e-01 +1.290000e+00 1.000000e-02 1.000000e-02 1.660000e+00 2.100000e-01 2.100000e-01 +1.310000e+00 1.000000e-02 1.000000e-02 1.830000e+00 3.200000e-01 3.200000e-01 +1.330000e+00 1.000000e-02 1.000000e-02 1.570000e+00 2.300000e-01 2.300000e-01 +1.350000e+00 1.000000e-02 1.000000e-02 1.620000e+00 1.600000e-01 1.600000e-01 +1.370000e+00 1.000000e-02 1.000000e-02 1.550000e+00 1.600000e-01 1.600000e-01 +1.390000e+00 1.000000e-02 1.000000e-02 1.400000e+00 1.500000e-01 1.500000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/OLYA_1984_I208231.cc b/analyses/pluginNovosibirsk/OLYA_1984_I208231.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/OLYA_1984_I208231.cc @@ -0,0 +1,79 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class OLYA_1984_I208231 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(OLYA_1984_I208231); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(OLYA_1984_I208231); + + +} diff --git a/analyses/pluginNovosibirsk/OLYA_1984_I208231.info b/analyses/pluginNovosibirsk/OLYA_1984_I208231.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/OLYA_1984_I208231.info @@ -0,0 +1,32 @@ +Name: OLYA_1984_I208231 +Year: 1984 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ for energies between 640 and 1400 MeV +Experiment: OLYA +Collider: VEPP-2M +InspireID: 208231 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Sov.J.Nucl.Phys. 40 (1984) 286-295, 1984 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies between 640 and 1400 MeV.' +Keywords: [] +BibKey: Kurdadze:1984dz +BibTeX: '@article{Kurdadze:1984dz, + author = "Kurdadze, L. M. and Lelchuk, M. {\relax Yu}. and + Pakhtusova, E. V. and Sidorov, V. A. and Skrinsky, A. N. + and Chilingarov, A. G. and Shatunov, {\relax Yu}. M. and + Shvarts, B. A. and Eidelman, S. I.", + title = "{STUDY OF THE REACTION E+ E- ---> PI+ PI- IN THE ENERGY + RANGE FROM 640-MEV - 1400-MEV}", + journal = "Sov. J. Nucl. Phys.", + volume = "40", + year = "1984", + pages = "286-295", + note = "[Yad. Fiz.40,451(1984)]", + SLACcitation = "%%CITATION = SJNCA,40,286;%%" +}' diff --git a/analyses/pluginNovosibirsk/OLYA_1984_I208231.plot b/analyses/pluginNovosibirsk/OLYA_1984_I208231.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/OLYA_1984_I208231.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /OLYA_1984_I208231/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/OLYA_1984_I208231.yoda b/analyses/pluginNovosibirsk/OLYA_1984_I208231.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/OLYA_1984_I208231.yoda @@ -0,0 +1,85 @@ +BEGIN YODA_SCATTER2D_V2 /REF/OLYA_1984_I208231/d01-x01-y01 +IsRef: 1 +Path: /REF/OLYA_1984_I208231/d01-x01-y01 +Title: doi:10.17182/hepdata.17648.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.426000e+02 0.000000e+00 0.000000e+00 4.370000e+02 4.800000e+01 4.800000e+01 +6.626000e+02 0.000000e+00 0.000000e+00 5.550000e+02 7.000000e+01 7.000000e+01 +6.776000e+02 0.000000e+00 0.000000e+00 6.370000e+02 3.200000e+01 3.200000e+01 +6.876000e+02 0.000000e+00 0.000000e+00 7.620000e+02 5.500000e+01 5.500000e+01 +6.976000e+02 0.000000e+00 0.000000e+00 8.270000e+02 3.600000e+01 3.600000e+01 +7.076000e+02 0.000000e+00 0.000000e+00 8.800000e+02 2.700000e+01 2.700000e+01 +7.176000e+02 0.000000e+00 0.000000e+00 9.730000e+02 3.100000e+01 3.100000e+01 +7.276000e+02 0.000000e+00 0.000000e+00 1.092000e+03 5.900000e+01 5.900000e+01 +7.376000e+02 0.000000e+00 0.000000e+00 1.205000e+03 4.500000e+01 4.500000e+01 +7.476000e+02 0.000000e+00 0.000000e+00 1.274000e+03 3.200000e+01 3.200000e+01 +7.576000e+02 0.000000e+00 0.000000e+00 1.298000e+03 2.900000e+01 2.900000e+01 +7.676000e+02 0.000000e+00 0.000000e+00 1.308000e+03 4.200000e+01 4.200000e+01 +7.736000e+02 0.000000e+00 0.000000e+00 1.317000e+03 7.600000e+01 7.600000e+01 +7.756000e+02 0.000000e+00 0.000000e+00 1.311000e+03 5.900000e+01 5.900000e+01 +7.776000e+02 0.000000e+00 0.000000e+00 1.264000e+03 5.500000e+01 5.500000e+01 +7.796000e+02 0.000000e+00 0.000000e+00 1.186000e+03 5.900000e+01 5.900000e+01 +7.816000e+02 0.000000e+00 0.000000e+00 1.125000e+03 4.600000e+01 4.600000e+01 +7.836000e+02 0.000000e+00 0.000000e+00 9.530000e+02 5.100000e+01 5.100000e+01 +7.856000e+02 0.000000e+00 0.000000e+00 8.490000e+02 4.500000e+01 4.500000e+01 +7.876000e+02 0.000000e+00 0.000000e+00 8.660000e+02 5.000000e+01 5.000000e+01 +7.896000e+02 0.000000e+00 0.000000e+00 8.230000e+02 4.400000e+01 4.400000e+01 +7.916000e+02 0.000000e+00 0.000000e+00 8.750000e+02 4.900000e+01 4.900000e+01 +7.976000e+02 0.000000e+00 0.000000e+00 7.870000e+02 2.900000e+01 2.900000e+01 +8.076000e+02 0.000000e+00 0.000000e+00 7.220000e+02 2.500000e+01 2.500000e+01 +8.176000e+02 0.000000e+00 0.000000e+00 6.210000e+02 1.800000e+01 1.800000e+01 +8.276000e+02 0.000000e+00 0.000000e+00 5.340000e+02 2.000000e+01 2.000000e+01 +8.376000e+02 0.000000e+00 0.000000e+00 4.620000e+02 1.300000e+01 1.300000e+01 +8.476000e+02 0.000000e+00 0.000000e+00 3.880000e+02 2.100000e+01 2.100000e+01 +8.576000e+02 0.000000e+00 0.000000e+00 3.370000e+02 1.400000e+01 1.400000e+01 +8.676000e+02 0.000000e+00 0.000000e+00 2.930000e+02 1.100000e+01 1.100000e+01 +8.776000e+02 0.000000e+00 0.000000e+00 2.480000e+02 8.000000e+00 8.000000e+00 +8.876000e+02 0.000000e+00 0.000000e+00 2.110000e+02 1.100000e+01 1.100000e+01 +8.976000e+02 0.000000e+00 0.000000e+00 1.825000e+02 6.400000e+00 6.400000e+00 +9.076000e+02 0.000000e+00 0.000000e+00 1.688000e+02 6.000000e+00 6.000000e+00 +9.176000e+02 0.000000e+00 0.000000e+00 1.427000e+02 7.400000e+00 7.400000e+00 +9.276000e+02 0.000000e+00 0.000000e+00 1.242000e+02 8.300000e+00 8.300000e+00 +9.376000e+02 0.000000e+00 0.000000e+00 1.067000e+02 5.700000e+00 5.700000e+00 +9.476000e+02 0.000000e+00 0.000000e+00 9.370000e+01 5.400000e+00 5.400000e+00 +9.576000e+02 0.000000e+00 0.000000e+00 9.390000e+01 4.800000e+00 4.800000e+00 +9.676000e+02 0.000000e+00 0.000000e+00 7.850000e+01 4.800000e+00 4.800000e+00 +9.776000e+02 0.000000e+00 0.000000e+00 7.630000e+01 4.100000e+00 4.100000e+00 +9.876000e+02 0.000000e+00 0.000000e+00 6.300000e+01 4.100000e+00 4.100000e+00 +9.976000e+02 0.000000e+00 0.000000e+00 6.500000e+01 3.300000e+00 3.300000e+00 +1.006600e+03 0.000000e+00 0.000000e+00 6.030000e+01 3.200000e+00 3.200000e+00 +1.067000e+03 0.000000e+00 0.000000e+00 3.830000e+01 3.000000e+00 3.000000e+00 +1.077000e+03 0.000000e+00 0.000000e+00 3.600000e+01 4.000000e+00 4.000000e+00 +1.087000e+03 0.000000e+00 0.000000e+00 3.360000e+01 2.800000e+00 2.800000e+00 +1.097000e+03 0.000000e+00 0.000000e+00 2.980000e+01 2.800000e+00 2.800000e+00 +1.107000e+03 0.000000e+00 0.000000e+00 3.240000e+01 2.900000e+00 2.900000e+00 +1.117000e+03 0.000000e+00 0.000000e+00 2.460000e+01 2.600000e+00 2.600000e+00 +1.127000e+03 0.000000e+00 0.000000e+00 2.320000e+01 2.500000e+00 2.500000e+00 +1.137000e+03 0.000000e+00 0.000000e+00 2.420000e+01 2.700000e+00 2.700000e+00 +1.152000e+03 0.000000e+00 0.000000e+00 2.200000e+01 2.700000e+00 2.700000e+00 +1.167000e+03 0.000000e+00 0.000000e+00 1.630000e+01 2.300000e+00 2.300000e+00 +1.177000e+03 0.000000e+00 0.000000e+00 1.920000e+01 2.600000e+00 2.600000e+00 +1.187000e+03 0.000000e+00 0.000000e+00 1.960000e+01 3.100000e+00 3.100000e+00 +1.197000e+03 0.000000e+00 0.000000e+00 1.610000e+01 2.300000e+00 2.300000e+00 +1.207000e+03 0.000000e+00 0.000000e+00 1.850000e+01 3.000000e+00 3.000000e+00 +1.217000e+03 0.000000e+00 0.000000e+00 1.030000e+01 1.900000e+00 1.900000e+00 +1.227000e+03 0.000000e+00 0.000000e+00 1.150000e+01 2.400000e+00 2.400000e+00 +1.237000e+03 0.000000e+00 0.000000e+00 1.660000e+01 2.600000e+00 2.600000e+00 +1.247000e+03 0.000000e+00 0.000000e+00 1.100000e+01 2.000000e+00 2.000000e+00 +1.257000e+03 0.000000e+00 0.000000e+00 1.110000e+01 1.800000e+00 1.800000e+00 +1.267000e+03 0.000000e+00 0.000000e+00 8.400000e+00 1.700000e+00 1.700000e+00 +1.277000e+03 0.000000e+00 0.000000e+00 5.500000e+00 1.200000e+00 1.200000e+00 +1.287000e+03 0.000000e+00 0.000000e+00 7.500000e+00 1.400000e+00 1.400000e+00 +1.297000e+03 0.000000e+00 0.000000e+00 8.100000e+00 1.800000e+00 1.800000e+00 +1.307000e+03 0.000000e+00 0.000000e+00 8.000000e+00 1.500000e+00 1.500000e+00 +1.317000e+03 0.000000e+00 0.000000e+00 8.100000e+00 1.600000e+00 1.600000e+00 +1.327000e+03 0.000000e+00 0.000000e+00 5.200000e+00 1.600000e+00 1.600000e+00 +1.337000e+03 0.000000e+00 0.000000e+00 7.700000e+00 1.700000e+00 1.700000e+00 +1.347000e+03 0.000000e+00 0.000000e+00 3.800000e+00 1.000000e+00 1.000000e+00 +1.357000e+03 0.000000e+00 0.000000e+00 4.600000e+00 1.100000e+00 1.100000e+00 +1.367000e+03 0.000000e+00 0.000000e+00 2.900000e+00 8.000000e-01 8.000000e-01 +1.377000e+03 0.000000e+00 0.000000e+00 3.200000e+00 1.000000e+00 1.000000e+00 +1.387000e+03 0.000000e+00 0.000000e+00 4.100000e+00 1.000000e+00 1.000000e+00 +1.397000e+03 0.000000e+00 0.000000e+00 2.100000e+00 7.000000e-01 7.000000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_1999_I508003.cc b/analyses/pluginNovosibirsk/SND_1999_I508003.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_1999_I508003.cc @@ -0,0 +1,88 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_1999_I508003 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_1999_I508003); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + _num3pi = bookCounter("TMP/num3"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=3) vetoEvent; + if(nCount[-211]==1&&nCount[211]==1&&nCount[111]==1) + _num3pi->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _num3pi->val(); + double error = _num3pi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _num3pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_1999_I508003); + + +} diff --git a/analyses/pluginNovosibirsk/SND_1999_I508003.info b/analyses/pluginNovosibirsk/SND_1999_I508003.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_1999_I508003.info @@ -0,0 +1,32 @@ +Name: SND_1999_I508003 +Year: 1999 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ between 1.04 and 1.38 GeV. +Experiment: SND +Collider: VEPP-2M +InspireID: 508003 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Lett. B462 (1999) 365-370, 1999 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ by SND for energies between 1.04 and 1.38 GeV.' +Keywords: +BibKey: Achasov:1999gw +BibTeX: '@article{Achasov:1999gw, + author = "Achasov, M. N. and others", + title = "{The Process e+ e- to pi+ pi- pi0 in the energy range + 2E(0) = 1.04-GeV - 1.38-GeV}", + journal = "Phys. Lett.", + volume = "B462", + year = "1999", + pages = "365-370", + doi = "10.1016/S0370-2693(99)00907-7", + eprint = "hep-ex/9910001", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/9910001;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_1999_I508003.plot b/analyses/pluginNovosibirsk/SND_1999_I508003.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_1999_I508003.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /SND_1999_I508003/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_1999_I508003.yoda b/analyses/pluginNovosibirsk/SND_1999_I508003.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_1999_I508003.yoda @@ -0,0 +1,42 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_1999_I508003/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_1999_I508003/d01-x01-y01 +Title: doi:10.17182/hepdata.28071.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.040000e+03 0.000000e+00 0.000000e+00 2.000000e-01 1.300000e+00 1.300000e+00 +1.050000e+03 0.000000e+00 0.000000e+00 4.000000e-01 1.300000e+00 1.300000e+00 +1.060000e+03 0.000000e+00 0.000000e+00 1.200000e+00 1.500000e+00 1.500000e+00 +1.070000e+03 0.000000e+00 0.000000e+00 1.800000e+00 8.000000e-01 8.000000e-01 +1.080000e+03 0.000000e+00 0.000000e+00 2.500000e+00 7.000000e-01 7.000000e-01 +1.090000e+03 0.000000e+00 0.000000e+00 2.600000e+00 6.000000e-01 6.000000e-01 +1.100000e+03 0.000000e+00 0.000000e+00 2.500000e+00 3.000000e-01 3.000000e-01 +1.110000e+03 0.000000e+00 0.000000e+00 2.600000e+00 4.000000e-01 4.000000e-01 +1.120000e+03 0.000000e+00 0.000000e+00 3.100000e+00 5.000000e-01 5.000000e-01 +1.130000e+03 0.000000e+00 0.000000e+00 2.800000e+00 4.000000e-01 4.000000e-01 +1.140000e+03 0.000000e+00 0.000000e+00 2.900000e+00 5.000000e-01 5.000000e-01 +1.150000e+03 0.000000e+00 0.000000e+00 3.800000e+00 6.000000e-01 6.000000e-01 +1.160000e+03 0.000000e+00 0.000000e+00 3.200000e+00 4.000000e-01 4.000000e-01 +1.180000e+03 0.000000e+00 0.000000e+00 4.200000e+00 5.000000e-01 5.000000e-01 +1.190000e+03 0.000000e+00 0.000000e+00 3.700000e+00 4.000000e-01 4.000000e-01 +1.200000e+03 0.000000e+00 0.000000e+00 4.000000e+00 3.000000e-01 3.000000e-01 +1.210000e+03 0.000000e+00 0.000000e+00 4.500000e+00 4.000000e-01 4.000000e-01 +1.220000e+03 0.000000e+00 0.000000e+00 4.700000e+00 5.000000e-01 5.000000e-01 +1.230000e+03 0.000000e+00 0.000000e+00 4.500000e+00 5.000000e-01 5.000000e-01 +1.240000e+03 0.000000e+00 0.000000e+00 4.100000e+00 4.000000e-01 4.000000e-01 +1.250000e+03 0.000000e+00 0.000000e+00 4.000000e+00 4.000000e-01 4.000000e-01 +1.260000e+03 0.000000e+00 0.000000e+00 4.500000e+00 4.000000e-01 4.000000e-01 +1.270000e+03 0.000000e+00 0.000000e+00 3.300000e+00 3.000000e-01 3.000000e-01 +1.280000e+03 0.000000e+00 0.000000e+00 4.100000e+00 3.000000e-01 3.000000e-01 +1.290000e+03 0.000000e+00 0.000000e+00 4.000000e+00 3.000000e-01 3.000000e-01 +1.300000e+03 0.000000e+00 0.000000e+00 3.400000e+00 3.000000e-01 3.000000e-01 +1.310000e+03 0.000000e+00 0.000000e+00 3.500000e+00 3.000000e-01 3.000000e-01 +1.320000e+03 0.000000e+00 0.000000e+00 3.800000e+00 4.000000e-01 4.000000e-01 +1.330000e+03 0.000000e+00 0.000000e+00 3.600000e+00 3.000000e-01 3.000000e-01 +1.340000e+03 0.000000e+00 0.000000e+00 3.700000e+00 3.000000e-01 3.000000e-01 +1.350000e+03 0.000000e+00 0.000000e+00 3.200000e+00 3.000000e-01 3.000000e-01 +1.360000e+03 0.000000e+00 0.000000e+00 3.200000e+00 3.000000e-01 3.000000e-01 +1.370000e+03 0.000000e+00 0.000000e+00 3.500000e+00 4.000000e-01 4.000000e-01 +1.380000e+03 0.000000e+00 0.000000e+00 3.300000e+00 2.000000e-01 2.000000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2000_I503946.cc b/analyses/pluginNovosibirsk/SND_2000_I503946.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I503946.cc @@ -0,0 +1,112 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2000_I503946 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2000_I503946); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numOmegaPi = bookCounter("TMP/OmegaPi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]+=1; + ++ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // three particles (pi0 pi0 gamma) + if(ntotal!=3) vetoEvent; + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==223) { + map nRes; + int ncount(0); + findChildren(p,nRes,ncount); + // only omega to pi0 gamma mode + if(ncount!=2) continue; + if(nRes[111]!=1 || nRes[22]!=1) continue; + // omega pi0 + if(nCount[111]-nRes[111]==1) + _numOmegaPi->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _numOmegaPi->val(); + double error = _numOmegaPi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numOmegaPi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2000_I503946); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2000_I503946.info b/analyses/pluginNovosibirsk/SND_2000_I503946.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I503946.info @@ -0,0 +1,34 @@ +Name: SND_2000_I503946 +Year: 2000 +Summary: Cross section for $e^+e^-\to\omega\pi^0\to\pi^0\pi^0\gamma$ at energies near the $\phi$ mass.' +Experiment: SND +Collider: VEPP-2M +InspireID: 503946 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Nucl. Phys (2000) B569, 158-182 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to\omega\pi^0\to\pi^0\pi^0\gamma$ at energies near the $\phi$ mass.' +Keywords: [] +BibKey: Achasov:1999wr +BibTeX: '@article{Achasov:1999wr, + author = "Achasov, M. N. and others", + title = "{Investigation of the e+ e- ---> omega pi0 ---> pi0 pi0 + gamma reaction in the energy domain near the phi meson}", + journal = "Nucl. Phys.", + volume = "B569", + year = "2000", + pages = "158-182", + doi = "10.1016/S0550-3213(99)00482-4", + eprint = "hep-ex/9907026", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/9907026;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2000_I503946.plot b/analyses/pluginNovosibirsk/SND_2000_I503946.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I503946.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2000_I503946/d01-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^0\to \pi^0\pi^0\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0\to \pi^0\pi^0\gamma)$/nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2000_I503946.yoda b/analyses/pluginNovosibirsk/SND_2000_I503946.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I503946.yoda @@ -0,0 +1,32 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2000_I503946/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2000_I503946/d01-x01-y01 +Title: doi:10.17182/hepdata.41517.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.841000e+02 0.000000e+00 0.000000e+00 5.700000e-01 1.136321e-01 1.136321e-01 +1.005000e+03 0.000000e+00 0.000000e+00 5.600000e-01 1.427725e-01 1.427725e-01 +1.010700e+03 0.000000e+00 0.000000e+00 4.700000e-01 1.027241e-01 1.027241e-01 +1.016200e+03 0.000000e+00 0.000000e+00 5.500000e-01 1.037123e-01 1.037123e-01 +1.017100e+03 0.000000e+00 0.000000e+00 4.800000e-01 1.028397e-01 1.028397e-01 +1.018100e+03 0.000000e+00 0.000000e+00 5.600000e-01 8.475848e-02 8.475848e-02 +1.019100e+03 0.000000e+00 0.000000e+00 5.900000e-01 5.805385e-02 5.805385e-02 +1.020000e+03 0.000000e+00 0.000000e+00 5.100000e-01 7.450000e-02 7.450000e-02 +1.021000e+03 0.000000e+00 0.000000e+00 7.400000e-01 1.160560e-01 1.160560e-01 +1.021900e+03 0.000000e+00 0.000000e+00 8.100000e-01 1.457404e-01 1.457404e-01 +1.022700e+03 0.000000e+00 0.000000e+00 5.500000e-01 2.117929e-01 2.117929e-01 +1.028000e+03 0.000000e+00 0.000000e+00 5.300000e-01 1.228912e-01 1.228912e-01 +1.033700e+03 0.000000e+00 0.000000e+00 9.700000e-01 1.960925e-01 1.960925e-01 +1.039800e+03 0.000000e+00 0.000000e+00 9.600000e-01 2.545663e-01 2.545663e-01 +1.060000e+03 0.000000e+00 0.000000e+00 1.080000e+00 3.146681e-01 3.146681e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2000_I503946/d02-x01-y01 +IsRef: 1 +Path: /REF/SND_2000_I503946/d02-x01-y01 +Title: doi:10.17182/hepdata.41517.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.019400e+03 0.000000e+00 0.000000e+00 7.500000e+00 9.750000e-01 9.750000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2000_I524221.cc b/analyses/pluginNovosibirsk/SND_2000_I524221.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I524221.cc @@ -0,0 +1,135 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2000_I524221 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2000_I524221); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaGamma = bookCounter("TMP/EtaGamma"); + _numPi0Gamma = bookCounter("TMP/Pi0Gamma"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && nCount[22]==1 && nCount[111]==1) + _numPi0Gamma->fill(event.weight()); + + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the eta + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(val.first==22) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaGamma->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma,error; + if(ix==1) { + sigma = _numEtaGamma->val(); + error = _numEtaGamma->err(); + } + else { + sigma = _numPi0Gamma->val(); + error = _numPi0Gamma->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, ix)); + Scatter2DPtr mult = bookScatter2D(1, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numEtaGamma,_numPi0Gamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2000_I524221); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2000_I524221.info b/analyses/pluginNovosibirsk/SND_2000_I524221.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I524221.info @@ -0,0 +1,30 @@ +Name: SND_2000_I524221 +Year: 2000 +Summary: $e^+e^-\to\pi\gamma$ and $\eta\gamma$ for energies near the $\phi$ mass +Experiment: SND +Collider: VEPP-2M +InspireID: 524221 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Eur. Phys. J. C12, 2000, 25-33 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\pi\gamma$ and $\eta\gamma$ for energies near the $\phi$ mass' +Keywords: [] +BibKey: Achasov:2000zd +BibTeX: '@article{Achasov:2000zd, + author = "Achasov, M. N. and others", + title = "{Experimental study of the processes e+ e- --> phi --> + eta gamma, pi0 gamma at VEPP-2M}", + journal = "Eur. Phys. J.", + volume = "C12", + year = "2000", + pages = "25-33", + doi = "10.1007/s100529900222", + reportNumber = "BUDKER-INP-1999-39", + SLACcitation = "%%CITATION = EPHJA,C12,25;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2000_I524221.plot b/analyses/pluginNovosibirsk/SND_2000_I524221.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I524221.plot @@ -0,0 +1,17 @@ +BEGIN PLOT /SND_2000_I524221/d01-x01-y02 +Title=$\sigma(e^+e^-\to \pi^0\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^0\gamma)$/nb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /SND_2000_I524221/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\gamma)$/nb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2000_I524221.yoda b/analyses/pluginNovosibirsk/SND_2000_I524221.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I524221.yoda @@ -0,0 +1,62 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2000_I524221/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2000_I524221/d01-x01-y01 +Title: doi:10.17182/hepdata.43394.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.855850e+02 4.550000e-01 4.550000e-01 1.900000e-01 5.000000e-01 5.000000e-01 +1.004960e+03 4.500000e-01 4.500000e-01 1.550000e+00 5.500000e-01 5.500000e-01 +1.010765e+03 4.250000e-01 4.250000e-01 3.270000e+00 5.600000e-01 5.600000e-01 +1.016070e+03 4.500000e-01 4.500000e-01 2.066000e+01 8.900000e-01 8.900000e-01 +1.017160e+03 1.800000e-01 1.800000e-01 3.243000e+01 1.180000e+00 1.180000e+00 +1.018210e+03 2.700000e-01 2.700000e-01 4.479000e+01 1.080000e+00 1.080000e+00 +1.019135e+03 2.950000e-01 2.950000e-01 5.559000e+01 7.000000e-01 7.000000e-01 +1.020065e+03 3.250000e-01 3.250000e-01 4.865000e+01 9.700000e-01 9.700000e-01 +1.021025e+03 3.050000e-01 3.050000e-01 3.055000e+01 9.100000e-01 9.100000e-01 +1.021820e+03 1.300000e-01 1.300000e-01 2.172000e+01 9.900000e-01 9.900000e-01 +1.022465e+03 3.250000e-01 3.250000e-01 1.547000e+01 9.100000e-01 9.100000e-01 +1.028115e+03 4.750000e-01 4.750000e-01 2.370000e+00 3.200000e-01 3.200000e-01 +1.033865e+03 4.850000e-01 4.850000e-01 7.900000e-01 2.100000e-01 2.100000e-01 +1.039155e+03 1.450000e-01 1.450000e-01 3.500000e-01 3.500000e-01 3.500000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2000_I524221/d01-x01-y02 +IsRef: 1 +Path: /REF/SND_2000_I524221/d01-x01-y02 +Title: doi:10.17182/hepdata.43394.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.855850e+02 4.550000e-01 4.550000e-01 2.600000e-01 2.800000e-01 2.800000e-01 +1.004960e+03 4.500000e-01 4.500000e-01 3.700000e-01 3.000000e-01 3.000000e-01 +1.010765e+03 4.250000e-01 4.250000e-01 1.150000e+00 3.200000e-01 3.200000e-01 +1.016070e+03 4.500000e-01 4.500000e-01 2.970000e+00 4.000000e-01 4.000000e-01 +1.017160e+03 1.800000e-01 1.800000e-01 2.680000e+00 6.400000e-01 6.400000e-01 +1.018210e+03 2.700000e-01 2.700000e-01 5.160000e+00 4.200000e-01 4.200000e-01 +1.019135e+03 2.950000e-01 2.950000e-01 5.400000e+00 2.500000e-01 2.500000e-01 +1.020065e+03 3.250000e-01 3.250000e-01 4.810000e+00 3.500000e-01 3.500000e-01 +1.021025e+03 3.050000e-01 3.050000e-01 2.070000e+00 2.900000e-01 2.900000e-01 +1.021820e+03 1.300000e-01 1.300000e-01 1.540000e+00 3.300000e-01 3.300000e-01 +1.022465e+03 3.250000e-01 3.250000e-01 1.070000e+00 2.900000e-01 2.900000e-01 +1.028115e+03 4.750000e-01 4.750000e-01 3.000000e-02 3.000000e-02 3.000000e-02 +1.033865e+03 4.850000e-01 4.850000e-01 0.000000e+00 1.000000e-02 1.000000e-02 +1.039155e+03 1.450000e-01 1.450000e-01 -4.000000e-02 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2000_I524221/d02-x01-y01 +IsRef: 1 +Path: /REF/SND_2000_I524221/d02-x01-y01 +Title: doi:10.17182/hepdata.43394.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.019400e+03 0.000000e+00 0.000000e+00 2.216000e+01 6.229767e-01 6.229767e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2000_I524221/d02-x01-y02 +IsRef: 1 +Path: /REF/SND_2000_I524221/d02-x01-y02 +Title: doi:10.17182/hepdata.43394.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.019400e+03 0.000000e+00 0.000000e+00 5.120000e+00 3.807887e-01 4.085340e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2000_I527752.cc b/analyses/pluginNovosibirsk/SND_2000_I527752.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I527752.cc @@ -0,0 +1,111 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2000_I527752 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2000_I527752); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numOmegaPi = bookCounter("TMP/OmegaPi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]+=1; + ++ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // three particles (pi0 pi0 gamma) + if(ntotal!=3) vetoEvent; + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==223) { + map nRes; + int ncount(0); + findChildren(p,nRes,ncount); + // only omega to pi0 gamma mode + if(ncount!=2) continue; + if(nRes[111]!=1 || nRes[22]!=1) continue; + // omega pi0 + if(nCount[111]-nRes[111]==1) + _numOmegaPi->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _numOmegaPi->val(); + double error = _numOmegaPi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + /// @name Histograms + //@{ + CounterPtr _numOmegaPi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2000_I527752); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2000_I527752.info b/analyses/pluginNovosibirsk/SND_2000_I527752.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I527752.info @@ -0,0 +1,35 @@ +Name: SND_2000_I527752 +Year: 2000 +Summary: Cross section for $e^+e^-\to\omega\pi^0\to\pi^0\pi^0\gamma$ for energies below 1.4 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 527752 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B486 (2000) 29-34, 2000 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to\omega\pi^0\to\pi^0\pi^0\gamma$ for energies below 1.4 GeV.' +Keywords: +Keywords: +BibKey: Achasov:2000wy +BibTeX: '@article{Achasov:2000wy, + author = "Achasov, M. N. and others", + title = "{The Process e+ e- ---> omega pi0 ---> pi0 pi0 gamma up + to 1.4-GeV}", + journal = "Phys. Lett.", + volume = "B486", + year = "2000", + pages = "29-34", + doi = "10.1016/S0370-2693(00)00706-1", + eprint = "hep-ex/0005032", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0005032;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2000_I527752.plot b/analyses/pluginNovosibirsk/SND_2000_I527752.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I527752.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2000_I527752/d01-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^0\to \pi^0\pi^0\gamma)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0\to \pi^0\pi^0\gamma)$/nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2000_I527752.yoda b/analyses/pluginNovosibirsk/SND_2000_I527752.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2000_I527752.yoda @@ -0,0 +1,31 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2000_I527752/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2000_I527752/d01-x01-y01 +Title: doi:10.17182/hepdata.41747.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.200000e+02 2.000000e-01 2.000000e-01 6.000000e-02 4.012692e-02 4.012692e-02 +9.400000e+02 2.000000e-01 2.000000e-01 2.000000e-01 5.111751e-02 5.111751e-02 +9.540000e+02 2.000000e+00 2.000000e+00 2.800000e-01 5.216781e-02 5.216781e-02 +9.730000e+02 4.300000e+00 4.300000e+00 6.000000e-01 7.692204e-02 7.692204e-02 +1.020000e+03 0.000000e+00 0.000000e+00 7.400000e-01 4.412448e-02 4.412448e-02 +1.045000e+03 5.000000e+00 5.000000e+00 9.600000e-01 1.396550e-01 1.396550e-01 +1.063000e+03 4.400000e+00 4.400000e+00 9.500000e-01 1.031967e-01 1.031967e-01 +1.081000e+03 3.500000e+00 3.500000e+00 1.070000e+00 9.019059e-02 9.019059e-02 +1.102000e+03 3.800000e+00 3.800000e+00 9.600000e-01 8.662286e-02 8.662286e-02 +1.123000e+03 4.400000e+00 4.400000e+00 1.130000e+00 1.082000e-01 1.082000e-01 +1.142000e+03 4.000000e+00 4.000000e+00 1.090000e+00 1.070345e-01 1.070345e-01 +1.160000e+03 4.000000e-01 4.000000e-01 1.370000e+00 1.319176e-01 1.319176e-01 +1.183000e+03 4.600000e+00 4.600000e+00 1.300000e+00 1.057083e-01 1.057083e-01 +1.203000e+03 4.400000e+00 4.400000e+00 1.360000e+00 1.078198e-01 1.078198e-01 +1.223000e+03 4.600000e+00 4.600000e+00 1.350000e+00 1.151024e-01 1.151024e-01 +1.243000e+03 4.800000e+00 4.800000e+00 1.480000e+00 1.121957e-01 1.121957e-01 +1.266000e+03 5.100000e+00 5.100000e+00 1.630000e+00 1.400205e-01 1.400205e-01 +1.285000e+03 5.200000e+00 5.200000e+00 1.460000e+00 1.188351e-01 1.188351e-01 +1.304000e+03 5.000000e+00 5.000000e+00 1.450000e+00 1.184887e-01 1.184887e-01 +1.325000e+03 5.000000e+00 5.000000e+00 1.550000e+00 9.158091e-02 9.158091e-02 +1.344000e+03 5.800000e+00 5.800000e+00 1.520000e+00 1.136964e-01 1.136964e-01 +1.363000e+03 4.600000e+00 4.600000e+00 1.540000e+00 1.077022e-01 1.077022e-01 +1.380000e+03 5.000000e-01 5.000000e-01 1.320000e+00 1.141152e-01 1.141152e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2001_I533574.cc b/analyses/pluginNovosibirsk/SND_2001_I533574.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2001_I533574.cc @@ -0,0 +1,111 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2001_I533574 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2001_I533574); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + _nKpKm = bookCounter("TMP/KpKm"); + _nK0K0 = bookCounter("TMP/K0K0"); + _n3pi = bookCounter("TMP/3pi"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2) { + if(nCount[321]==1 && nCount[-321]==1) + _nKpKm->fill(event.weight()); + else if(nCount[130]==1 && nCount[310]==1) + _nK0K0->fill(event.weight()); + } + else if(ntotal==3 && nCount[211] == 1 && nCount[-211] == 1 && nCount[111] == 1) + _n3pi->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int iy=1;iy<3;++iy) { + for(unsigned int ix=1;ix<5;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _nKpKm->val(); + error = _nKpKm->err(); + } + else if(ix==2) { + sigma = _nK0K0->val(); + error = _nK0K0->err(); + } + else if(ix==3) { + sigma = _nK0K0->val(); + error = _nK0K0->err(); + } + else if(ix==4) { + sigma = _n3pi->val(); + error = _n3pi->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(iy, 1, ix)); + Scatter2DPtr mult = bookScatter2D(iy, 1, ix); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nKpKm,_nK0K0,_n3pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2001_I533574); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2001_I533574.info b/analyses/pluginNovosibirsk/SND_2001_I533574.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2001_I533574.info @@ -0,0 +1,35 @@ +Name: SND_2001_I533574 +Year: 2001 +Summary: Cross section for $e^+e^-\to$ $K^+K^-$, $K_S^0K_L^0$ and $\pi^+\pi^-\pi^0$ near the $\phi$ resonance +Experiment: SND +Collider: VEPP-2M +InspireID: 533574 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D63 (2001) 072002 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to$ $K^+K^-$, $K_S^0K_L^0$ and $\pi^+\pi^-\pi^0$ near the $\phi$ resonance' +Keywords: +BibKey: Achasov:2000am +BibTeX: '@article{Achasov:2000am, + author = "Achasov, M. N. and others", + title = "{Measurements of the parameters of the $\phi(1020)$ + resonance through studies of the processes $e^+ e^- \to + K^+ K^-$, $K_SK_L$, and $\pi^+ \pi^- \pi^0$}", + journal = "Phys. Rev.", + volume = "D63", + year = "2001", + pages = "072002", + doi = "10.1103/PhysRevD.63.072002", + eprint = "hep-ex/0009036", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0009036;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2001_I533574.plot b/analyses/pluginNovosibirsk/SND_2001_I533574.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2001_I533574.plot @@ -0,0 +1,53 @@ +BEGIN PLOT /SND_2001_I533574/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /SND_2001_I533574/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /SND_2001_I533574/d01-x01-y02 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ (charged mode) +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /SND_2001_I533574/d02-x01-y02 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ (charged mode) +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /SND_2001_I533574/d01-x01-y03 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ (neutral mode) +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /SND_2001_I533574/d02-x01-y03 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ (neutral mode) +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /SND_2001_I533574/d01-x01-y04 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /SND_2001_I533574/d02-x01-y04 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2001_I533574.yoda b/analyses/pluginNovosibirsk/SND_2001_I533574.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2001_I533574.yoda @@ -0,0 +1,184 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2001_I533574/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2001_I533574/d01-x01-y01 +Title: doi:10.17182/hepdata.41706.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.010170e+03 0.000000e+00 0.000000e+00 4.810000e+01 1.394048e+01 1.394048e+01 +1.015750e+03 0.000000e+00 0.000000e+00 4.090000e+02 4.090912e+01 4.090912e+01 +1.016680e+03 0.000000e+00 0.000000e+00 7.171000e+02 7.015067e+01 7.015067e+01 +1.017590e+03 0.000000e+00 0.000000e+00 1.112000e+03 1.095811e+02 1.095811e+02 +1.018780e+03 0.000000e+00 0.000000e+00 1.794100e+03 1.687364e+02 1.687364e+02 +1.019790e+03 0.000000e+00 0.000000e+00 1.898100e+03 1.743737e+02 1.743737e+02 +1.020650e+03 0.000000e+00 0.000000e+00 1.471900e+03 1.389523e+02 1.389523e+02 +1.021680e+03 0.000000e+00 0.000000e+00 9.284000e+02 8.900044e+01 8.900044e+01 +1.023270e+03 0.000000e+00 0.000000e+00 5.144000e+02 4.894287e+01 4.894287e+01 +1.028230e+03 0.000000e+00 0.000000e+00 1.611000e+02 1.522213e+01 1.522213e+01 +1.033840e+03 0.000000e+00 0.000000e+00 7.290000e+01 6.963186e+00 6.963186e+00 +1.039590e+03 0.000000e+00 0.000000e+00 4.740000e+01 4.576332e+00 4.576332e+00 +1.049810e+03 0.000000e+00 0.000000e+00 2.900000e+01 2.931208e+00 2.931208e+00 +1.059660e+03 0.000000e+00 0.000000e+00 1.860000e+01 2.012184e+00 2.012184e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2001_I533574/d01-x01-y02 +IsRef: 1 +Path: /REF/SND_2001_I533574/d01-x01-y02 +Title: doi:10.17182/hepdata.41706.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.003910e+03 0.000000e+00 0.000000e+00 7.700000e+00 3.073614e+00 3.073614e+00 +1.010170e+03 0.000000e+00 0.000000e+00 4.520000e+01 7.253728e+00 7.253728e+00 +1.015750e+03 0.000000e+00 0.000000e+00 3.155000e+02 3.403929e+01 3.403929e+01 +1.016680e+03 0.000000e+00 0.000000e+00 5.255000e+02 5.237308e+01 5.237308e+01 +1.017590e+03 0.000000e+00 0.000000e+00 8.363000e+02 8.177969e+01 8.177969e+01 +1.018780e+03 0.000000e+00 0.000000e+00 1.324700e+03 1.219235e+02 1.219235e+02 +1.019790e+03 0.000000e+00 0.000000e+00 1.388400e+03 1.258844e+02 1.258844e+02 +1.020650e+03 0.000000e+00 0.000000e+00 1.053000e+03 9.812690e+01 9.812690e+01 +1.021680e+03 0.000000e+00 0.000000e+00 6.480000e+02 6.330479e+01 6.330479e+01 +1.023270e+03 0.000000e+00 0.000000e+00 3.520000e+02 3.483174e+01 3.483174e+01 +1.028230e+03 0.000000e+00 0.000000e+00 1.030000e+02 1.135793e+01 1.135793e+01 +1.033840e+03 0.000000e+00 0.000000e+00 4.510000e+01 5.598077e+00 5.598077e+00 +1.039590e+03 0.000000e+00 0.000000e+00 2.830000e+01 3.957210e+00 3.957210e+00 +1.049810e+03 0.000000e+00 0.000000e+00 1.330000e+01 2.470613e+00 2.470613e+00 +1.059660e+03 0.000000e+00 0.000000e+00 1.700000e+01 3.712055e+00 3.712055e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2001_I533574/d01-x01-y03 +IsRef: 1 +Path: /REF/SND_2001_I533574/d01-x01-y03 +Title: doi:10.17182/hepdata.41706.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.003910e+03 0.000000e+00 0.000000e+00 7.700000e+00 1.202957e+00 1.202957e+00 +1.010170e+03 0.000000e+00 0.000000e+00 3.400000e+01 4.069078e+00 4.069078e+00 +1.015750e+03 0.000000e+00 0.000000e+00 2.945000e+02 2.882573e+01 2.882573e+01 +1.016680e+03 0.000000e+00 0.000000e+00 5.131000e+02 4.908861e+01 4.908861e+01 +1.017590e+03 0.000000e+00 0.000000e+00 8.091000e+02 7.741390e+01 7.741390e+01 +1.018780e+03 0.000000e+00 0.000000e+00 1.295000e+03 1.173973e+02 1.173973e+02 +1.019790e+03 0.000000e+00 0.000000e+00 1.372400e+03 1.215506e+02 1.215506e+02 +1.020650e+03 0.000000e+00 0.000000e+00 1.051900e+03 9.624011e+01 9.624011e+01 +1.021680e+03 0.000000e+00 0.000000e+00 6.672000e+02 6.208229e+01 6.208229e+01 +1.023270e+03 0.000000e+00 0.000000e+00 3.595000e+02 3.333903e+01 3.333903e+01 +1.028230e+03 0.000000e+00 0.000000e+00 1.081000e+02 1.020398e+01 1.020398e+01 +1.033840e+03 0.000000e+00 0.000000e+00 5.200000e+01 4.980047e+00 4.980047e+00 +1.039590e+03 0.000000e+00 0.000000e+00 3.100000e+01 3.107555e+00 3.107555e+00 +1.049810e+03 0.000000e+00 0.000000e+00 1.640000e+01 1.757335e+00 1.757335e+00 +1.059660e+03 0.000000e+00 0.000000e+00 1.100000e+01 1.285481e+00 1.285481e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2001_I533574/d01-x01-y04 +IsRef: 1 +Path: /REF/SND_2001_I533574/d01-x01-y04 +Title: doi:10.17182/hepdata.41706.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.842100e+02 0.000000e+00 0.000000e+00 1.810000e+01 1.811217e+00 1.811217e+00 +1.003910e+03 0.000000e+00 0.000000e+00 3.620000e+01 3.401768e+00 3.401768e+00 +1.010170e+03 0.000000e+00 0.000000e+00 6.850000e+01 6.414379e+00 6.414379e+00 +1.015750e+03 0.000000e+00 0.000000e+00 2.431000e+02 2.240324e+01 2.240324e+01 +1.016680e+03 0.000000e+00 0.000000e+00 3.589000e+02 3.291975e+01 3.291975e+01 +1.017590e+03 0.000000e+00 0.000000e+00 4.936000e+02 4.537958e+01 4.537958e+01 +1.018780e+03 0.000000e+00 0.000000e+00 6.586000e+02 5.835665e+01 5.835665e+01 +1.019790e+03 0.000000e+00 0.000000e+00 5.955000e+02 5.360039e+01 5.360039e+01 +1.020650e+03 0.000000e+00 0.000000e+00 3.998000e+02 3.762451e+01 3.762451e+01 +1.021680e+03 0.000000e+00 0.000000e+00 2.174000e+02 2.070407e+01 2.070407e+01 +1.023270e+03 0.000000e+00 0.000000e+00 9.220000e+01 8.698554e+00 8.698554e+00 +1.028230e+03 0.000000e+00 0.000000e+00 1.120000e+01 1.170359e+00 1.170359e+00 +1.033840e+03 0.000000e+00 0.000000e+00 1.400000e+00 1.764918e-01 1.937766e-01 +1.039590e+03 0.000000e+00 0.000000e+00 9.600000e-02 5.166718e-02 9.093678e-02 +1.049810e+03 0.000000e+00 0.000000e+00 6.130000e-01 1.048555e-01 1.256769e-01 +1.059660e+03 0.000000e+00 0.000000e+00 1.304000e+00 2.281641e-01 2.352846e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2001_I533574/d02-x01-y01 +IsRef: 1 +Path: /REF/SND_2001_I533574/d02-x01-y01 +Title: doi:10.17182/hepdata.41706.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.010340e+03 0.000000e+00 0.000000e+00 3.870000e+01 1.323382e+01 1.323382e+01 +1.015430e+03 0.000000e+00 0.000000e+00 3.542000e+02 3.524083e+01 3.524083e+01 +1.016780e+03 0.000000e+00 0.000000e+00 7.347000e+02 7.238889e+01 7.238889e+01 +1.017720e+03 0.000000e+00 0.000000e+00 1.181800e+03 1.162938e+02 1.162938e+02 +1.018620e+03 0.000000e+00 0.000000e+00 1.726700e+03 1.637470e+02 1.637470e+02 +1.019510e+03 0.000000e+00 0.000000e+00 1.946200e+03 1.782636e+02 1.782636e+02 +1.020430e+03 0.000000e+00 0.000000e+00 1.639600e+03 1.532926e+02 1.532926e+02 +1.021410e+03 0.000000e+00 0.000000e+00 1.087200e+03 1.034134e+02 1.034134e+02 +1.022320e+03 0.000000e+00 0.000000e+00 6.729000e+02 6.559392e+01 6.559392e+01 +1.027520e+03 0.000000e+00 0.000000e+00 1.796000e+02 1.705443e+01 1.705443e+01 +1.033580e+03 0.000000e+00 0.000000e+00 7.990000e+01 7.520094e+00 7.520094e+00 +1.039640e+03 0.000000e+00 0.000000e+00 4.870000e+01 4.636261e+00 4.636261e+00 +1.049600e+03 0.000000e+00 0.000000e+00 3.120000e+01 3.096887e+00 3.096887e+00 +1.059520e+03 0.000000e+00 0.000000e+00 2.090000e+01 2.175772e+00 2.175772e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2001_I533574/d02-x01-y02 +IsRef: 1 +Path: /REF/SND_2001_I533574/d02-x01-y02 +Title: doi:10.17182/hepdata.41706.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.003710e+03 0.000000e+00 0.000000e+00 7.400000e+00 2.970344e+00 2.970344e+00 +1.010340e+03 0.000000e+00 0.000000e+00 4.000000e+01 7.194137e+00 7.194137e+00 +1.015430e+03 0.000000e+00 0.000000e+00 2.883000e+02 3.037473e+01 3.037473e+01 +1.016780e+03 0.000000e+00 0.000000e+00 5.640000e+02 5.597474e+01 5.597474e+01 +1.017720e+03 0.000000e+00 0.000000e+00 9.231000e+02 8.936464e+01 8.936464e+01 +1.018620e+03 0.000000e+00 0.000000e+00 1.337100e+03 1.237149e+02 1.237149e+02 +1.019510e+03 0.000000e+00 0.000000e+00 1.473800e+03 1.326039e+02 1.326039e+02 +1.020430e+03 0.000000e+00 0.000000e+00 1.193100e+03 1.100834e+02 1.100834e+02 +1.021410e+03 0.000000e+00 0.000000e+00 7.575000e+02 7.337113e+01 7.337113e+01 +1.022320e+03 0.000000e+00 0.000000e+00 4.659000e+02 4.729821e+01 4.729821e+01 +1.027520e+03 0.000000e+00 0.000000e+00 1.238000e+02 1.328219e+01 1.328219e+01 +1.033580e+03 0.000000e+00 0.000000e+00 5.540000e+01 6.386277e+00 6.386277e+00 +1.039640e+03 0.000000e+00 0.000000e+00 2.730000e+01 3.824949e+00 3.824949e+00 +1.049600e+03 0.000000e+00 0.000000e+00 1.500000e+01 2.568409e+00 2.568409e+00 +1.059520e+03 0.000000e+00 0.000000e+00 1.400000e+01 3.311803e+00 3.311803e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2001_I533574/d02-x01-y03 +IsRef: 1 +Path: /REF/SND_2001_I533574/d02-x01-y03 +Title: doi:10.17182/hepdata.41706.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.003710e+03 0.000000e+00 0.000000e+00 6.700000e+00 1.156942e+00 1.156942e+00 +1.010340e+03 0.000000e+00 0.000000e+00 3.370000e+01 3.981738e+00 3.981738e+00 +1.015430e+03 0.000000e+00 0.000000e+00 2.659000e+02 2.566340e+01 2.566340e+01 +1.016780e+03 0.000000e+00 0.000000e+00 5.326000e+02 5.108807e+01 5.108807e+01 +1.017720e+03 0.000000e+00 0.000000e+00 8.751000e+02 8.329290e+01 8.329290e+01 +1.018620e+03 0.000000e+00 0.000000e+00 1.268500e+03 1.159821e+02 1.159821e+02 +1.019510e+03 0.000000e+00 0.000000e+00 1.426300e+03 1.257277e+02 1.257277e+02 +1.020430e+03 0.000000e+00 0.000000e+00 1.165200e+03 1.057105e+02 1.057105e+02 +1.021410e+03 0.000000e+00 0.000000e+00 7.670000e+02 7.103786e+01 7.103786e+01 +1.022320e+03 0.000000e+00 0.000000e+00 4.754000e+02 4.491765e+01 4.491765e+01 +1.027520e+03 0.000000e+00 0.000000e+00 1.253000e+02 1.166338e+01 1.166338e+01 +1.033580e+03 0.000000e+00 0.000000e+00 5.480000e+01 5.161969e+00 5.161969e+00 +1.039640e+03 0.000000e+00 0.000000e+00 2.960000e+01 2.954170e+00 2.954170e+00 +1.049600e+03 0.000000e+00 0.000000e+00 1.750000e+01 1.835601e+00 1.835601e+00 +1.059520e+03 0.000000e+00 0.000000e+00 1.170000e+01 1.331273e+00 1.331273e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2001_I533574/d02-x01-y04 +IsRef: 1 +Path: /REF/SND_2001_I533574/d02-x01-y04 +Title: doi:10.17182/hepdata.41706.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.840200e+02 0.000000e+00 0.000000e+00 1.730000e+01 1.702042e+00 1.702042e+00 +1.003710e+03 0.000000e+00 0.000000e+00 3.760000e+01 3.552628e+00 3.552628e+00 +1.010340e+03 0.000000e+00 0.000000e+00 6.950000e+01 6.532604e+00 6.532604e+00 +1.015430e+03 0.000000e+00 0.000000e+00 2.200000e+02 2.018005e+01 2.018005e+01 +1.016780e+03 0.000000e+00 0.000000e+00 3.536000e+02 3.265093e+01 3.265093e+01 +1.017720e+03 0.000000e+00 0.000000e+00 5.150000e+02 4.726681e+01 4.726681e+01 +1.018620e+03 0.000000e+00 0.000000e+00 6.642000e+02 5.914736e+01 5.914736e+01 +1.019510e+03 0.000000e+00 0.000000e+00 6.670000e+02 5.911132e+01 5.911132e+01 +1.020430e+03 0.000000e+00 0.000000e+00 4.712000e+02 4.375585e+01 4.375585e+01 +1.021410e+03 0.000000e+00 0.000000e+00 2.701000e+02 2.545891e+01 2.545891e+01 +1.022320e+03 0.000000e+00 0.000000e+00 1.429000e+02 1.382752e+01 1.382752e+01 +1.027520e+03 0.000000e+00 0.000000e+00 1.580300e+01 1.565287e+00 1.565287e+00 +1.033580e+03 0.000000e+00 0.000000e+00 1.737000e+00 2.010509e-01 2.133576e-01 +1.039640e+03 0.000000e+00 0.000000e+00 9.400000e-02 6.121791e-02 8.091744e-02 +1.049600e+03 0.000000e+00 0.000000e+00 5.950000e-01 9.007609e-02 1.136385e-01 +1.059520e+03 0.000000e+00 0.000000e+00 1.238000e+00 1.896277e-01 1.948298e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2001_I579319.cc b/analyses/pluginNovosibirsk/SND_2001_I579319.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2001_I579319.cc @@ -0,0 +1,97 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2001_I579319 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2001_I579319); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion1 = bookCounter("TMP/pion1"); + _npion2 = bookCounter("TMP/pion2"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=4) vetoEvent; + if(nCount[-211]==2&&nCount[211]==2) + _npion1->fill(event.weight()); + else if(nCount[-211]==1&&nCount[211]==1&&nCount[111]==2) + _npion2->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma,error; + if(ix==1) { + sigma = _npion1->val(); + error = _npion1->err(); + } + else { + sigma = _npion2->val(); + error = _npion2->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion1,_npion2; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2001_I579319); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2001_I579319.info b/analyses/pluginNovosibirsk/SND_2001_I579319.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2001_I579319.info @@ -0,0 +1,27 @@ +Name: SND_2001_I579319 +Year: 2001 +Summary: Cross section for $e^+e^-2\pi^+2\pi^-$ and $\pi^+\pi^-2\pi^0$ between 1 and 1.4 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 579319 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - INP-2001-34 (2001) +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+2\pi^-$ and $\pi^+\pi^-2\pi^0$ between 1 and 1.4 GeV' +BibKey: Achasov:2001gp +BibTeX: '@article{Achasov:2001gp, + author = "Achasov, M. N. and others", + title = "{e+ e- --> 4pi processes investigation in the energy + range 0.98-GeV to 1.38-GeV with SND detector}", + collaboration = "SND", + year = "2001", + reportNumber = "BUDKER-INP-2001-34", + SLACcitation = "%%CITATION = BUDKER-INP-2001-34;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2001_I579319.plot b/analyses/pluginNovosibirsk/SND_2001_I579319.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2001_I579319.plot @@ -0,0 +1,16 @@ +BEGIN PLOT /SND_2001_I579319/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT +BEGIN PLOT /SND_2001_I579319/d02-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-2\pi^0)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2001_I579319.yoda b/analyses/pluginNovosibirsk/SND_2001_I579319.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2001_I579319.yoda @@ -0,0 +1,99 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2001_I579319/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2001_I579319/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.98000 0.00000 0.00000 1.07000e+00 2.10000e-01 2.10000e-01 +0.98410 0.00000 0.00000 1.21000e+00 9.00000e-02 9.00000e-02 +1.00380 0.00000 0.00000 1.26000e+00 1.20000e-01 1.20000e-01 +1.00968 0.00000 0.00000 1.43000e+00 1.50000e-01 1.50000e-01 +1.01566 0.00000 0.00000 1.68000e+00 1.60000e-01 1.60000e-01 +1.01668 0.00000 0.00000 1.60000e+00 1.20000e-01 1.20000e-01 +1.01766 0.00000 0.00000 1.78000e+00 1.20000e-01 1.20000e-01 +1.01864 0.00000 0.00000 1.72000e+00 1.10000e-01 1.10000e-01 +1.01962 0.00000 0.00000 1.96000e+00 1.00000e-01 1.00000e-01 +1.02058 0.00000 0.00000 1.76000e+00 1.20000e-01 1.20000e-01 +1.02164 0.00000 0.00000 1.92000e+00 1.70000e-01 1.70000e-01 +1.02276 0.00000 0.00000 1.72000e+00 1.50000e-01 1.50000e-01 +1.02774 0.00000 0.00000 1.91000e+00 1.50000e-01 1.50000e-01 +1.03372 0.00000 0.00000 1.88000e+00 1.70000e-01 1.70000e-01 +1.04000 0.00000 0.00000 2.09000e+00 1.50000e-01 1.50000e-01 +1.05000 0.00000 0.00000 2.37000e+00 1.50000e-01 1.50000e-01 +1.06000 0.00000 0.00000 2.52000e+00 1.30000e-01 1.30000e-01 +1.07000 0.00000 0.00000 3.11000e+00 3.50000e-01 3.50000e-01 +1.08000 0.00000 0.00000 4.67000e+00 1.80000e-01 1.80000e-01 +1.09000 0.00000 0.00000 3.52000e+00 3.80000e-01 3.80000e-01 +1.10000 0.00000 0.00000 3.92000e+00 1.90000e-01 1.90000e-01 +1.11000 0.00000 0.00000 4.48000e+00 4.30000e-01 4.30000e-01 +1.12000 0.00000 0.00000 4.93000e+00 2.50000e-01 2.50000e-01 +1.13000 0.00000 0.00000 5.45000e+00 4.30000e-01 4.30000e-01 +1.14000 0.00000 0.00000 6.00000e+00 2.80000e-01 2.80000e-01 +1.15000 0.00000 0.00000 7.32000e+00 6.20000e-01 6.20000e-01 +1.16000 0.00000 0.00000 7.33000e+00 3.00000e-01 3.00000e-01 +1.18000 0.00000 0.00000 8.60000e+00 2.80000e-01 2.80000e-01 +1.19000 0.00000 0.00000 8.68000e+00 4.20000e-01 4.20000e-01 +1.20000 0.00000 0.00000 1.15700e+01 3.20000e-01 3.20000e-01 +1.21000 0.00000 0.00000 1.05800e+01 5.10000e-01 5.10000e-01 +1.22000 0.00000 0.00000 1.16600e+01 3.60000e-01 3.60000e-01 +1.23000 0.00000 0.00000 1.08400e+01 5.20000e-01 5.20000e-01 +1.24000 0.00000 0.00000 1.33600e+01 3.60000e-01 3.60000e-01 +1.25000 0.00000 0.00000 1.50300e+01 5.00000e-01 5.00000e-01 +1.26000 0.00000 0.00000 1.36900e+01 5.40000e-01 5.40000e-01 +1.27000 0.00000 0.00000 1.67400e+01 4.90000e-01 4.90000e-01 +1.28000 0.00000 0.00000 1.66600e+01 5.00000e-01 5.00000e-01 +1.29000 0.00000 0.00000 1.62100e+01 4.50000e-01 4.50000e-01 +1.30000 0.00000 0.00000 1.83200e+01 5.00000e-01 5.00000e-01 +1.31000 0.00000 0.00000 1.73800e+01 5.30000e-01 5.30000e-01 +1.32000 0.00000 0.00000 1.72800e+01 4.90000e-01 4.90000e-01 +1.33000 0.00000 0.00000 1.85500e+01 4.50000e-01 4.50000e-01 +1.34000 0.00000 0.00000 2.21900e+01 4.60000e-01 4.60000e-01 +1.35000 0.00000 0.00000 2.16600e+01 5.30000e-01 5.30000e-01 +1.36000 0.00000 0.00000 2.39900e+01 3.60000e-01 3.60000e-01 +1.37000 0.00000 0.00000 2.38600e+01 5.50000e-01 5.50000e-01 +1.38000 0.00000 0.00000 2.40900e+01 4.00000e-01 4.00000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2001_I579319/d02-x01-y01 +IsRef: 1 +Path: /REF/SND_2001_I579319/d02-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.98000 0.00000 0.00000 5.56000e+00 1.58000e+00 1.58000e+00 +1.01900 0.00000 0.00000 8.07000e+00 1.65000e+00 1.65000e+00 +1.04000 0.00000 0.00000 9.17000e+00 1.47000e+00 1.47000e+00 +1.05000 0.00000 0.00000 1.06600e+01 1.35000e+00 1.35000e+00 +1.06000 0.00000 0.00000 1.14500e+01 7.50000e-01 7.50000e-01 +1.07000 0.00000 0.00000 1.02600e+01 1.25000e+00 1.25000e+00 +1.08000 0.00000 0.00000 1.36700e+01 6.30000e-01 6.30000e-01 +1.09000 0.00000 0.00000 1.30100e+01 1.37000e+00 1.37000e+00 +1.10000 0.00000 0.00000 1.44100e+01 4.20000e-01 4.20000e-01 +1.11000 0.00000 0.00000 1.20200e+01 8.60000e-01 8.60000e-01 +1.12000 0.00000 0.00000 1.56700e+01 5.40000e-01 5.40000e-01 +1.13000 0.00000 0.00000 1.54100e+01 8.80000e-01 8.80000e-01 +1.14000 0.00000 0.00000 1.65000e+01 5.80000e-01 5.80000e-01 +1.15000 0.00000 0.00000 1.57800e+01 1.16000e+00 1.16000e+00 +1.16000 0.00000 0.00000 1.73400e+01 5.80000e-01 5.80000e-01 +1.18000 0.00000 0.00000 1.91400e+01 5.40000e-01 5.40000e-01 +1.20000 0.00000 0.00000 1.95400e+01 5.50000e-01 5.50000e-01 +1.21000 0.00000 0.00000 1.93600e+01 9.20000e-01 9.20000e-01 +1.22000 0.00000 0.00000 2.01000e+01 6.40000e-01 6.40000e-01 +1.23000 0.00000 0.00000 2.03400e+01 1.00000e+00 1.00000e+00 +1.24000 0.00000 0.00000 2.20300e+01 6.30000e-01 6.30000e-01 +1.25000 0.00000 0.00000 2.23500e+01 8.50000e-01 8.50000e-01 +1.26000 0.00000 0.00000 2.23300e+01 9.40000e-01 9.40000e-01 +1.27000 0.00000 0.00000 2.46900e+01 8.20000e-01 8.20000e-01 +1.28000 0.00000 0.00000 2.40300e+01 8.30000e-01 8.30000e-01 +1.29000 0.00000 0.00000 2.44600e+01 7.60000e-01 7.60000e-01 +1.30000 0.00000 0.00000 2.65700e+01 8.30000e-01 8.30000e-01 +1.31000 0.00000 0.00000 2.42900e+01 8.70000e-01 8.70000e-01 +1.32000 0.00000 0.00000 2.59200e+01 8.40000e-01 8.40000e-01 +1.33000 0.00000 0.00000 2.63100e+01 7.50000e-01 7.50000e-01 +1.34000 0.00000 0.00000 2.71900e+01 6.30000e-01 6.30000e-01 +1.35000 0.00000 0.00000 2.88100e+01 8.30000e-01 8.30000e-01 +1.36000 0.00000 0.00000 2.83500e+01 5.40000e-01 5.40000e-01 +1.37000 0.00000 0.00000 2.89900e+01 8.10000e-01 8.10000e-01 +1.38000 0.00000 0.00000 2.88000e+01 5.80000e-01 5.80000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2002_I582183.cc b/analyses/pluginNovosibirsk/SND_2002_I582183.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2002_I582183.cc @@ -0,0 +1,88 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2002_I582183 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2002_I582183); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + _num3pi = bookCounter("TMP/num3"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=3) vetoEvent; + if(nCount[-211]==1&&nCount[211]==1&&nCount[111]==1) + _num3pi->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _num3pi->val(); + double error = _num3pi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _num3pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2002_I582183); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2002_I582183.info b/analyses/pluginNovosibirsk/SND_2002_I582183.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2002_I582183.info @@ -0,0 +1,32 @@ +Name: SND_2002_I582183 +Year: 2002 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ between 0.98 and 1.38 GeV. +Experiment: SND +Collider: VEPP-2M +InspireID: 582183 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys. Rev. D66 (2002) 032001 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ by SND for energies between 0.98 and 1.38 GeV.' +Keywords: +BibKey: Achasov:2002ud +BibTeX: '@article{Achasov:2002ud, + author = "Achasov, M. N. and others", + title = "{Study of the process e+ e- ---> pi+ pi- pi0 in the + energy region s**(1/2) from 0.98-GeV to 1.38-GeV}", + journal = "Phys. Rev.", + volume = "D66", + year = "2002", + pages = "032001", + doi = "10.1103/PhysRevD.66.032001", + eprint = "hep-ex/0201040", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0201040;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2002_I582183.plot b/analyses/pluginNovosibirsk/SND_2002_I582183.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2002_I582183.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /SND_2002_I582183/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/pb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2002_I582183.yoda b/analyses/pluginNovosibirsk/SND_2002_I582183.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2002_I582183.yoda @@ -0,0 +1,75 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2002_I582183/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2002_I582183/d01-x01-y01 +Title: doi:10.17182/hepdata.41974.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.800000e+02 0.000000e+00 0.000000e+00 1.558000e+01 1.360331e+00 1.360331e+00 +9.840200e+02 0.000000e+00 0.000000e+00 1.730000e+01 1.174564e+00 1.174564e+00 +9.842100e+02 0.000000e+00 0.000000e+00 1.810000e+01 1.279883e+00 1.279883e+00 +1.003710e+03 0.000000e+00 0.000000e+00 3.760000e+01 2.344014e+00 2.344014e+00 +1.003910e+03 0.000000e+00 0.000000e+00 3.620000e+01 2.228475e+00 2.228475e+00 +1.010170e+03 0.000000e+00 0.000000e+00 6.850000e+01 4.178086e+00 4.178086e+00 +1.010340e+03 0.000000e+00 0.000000e+00 6.950000e+01 4.284904e+00 4.284904e+00 +1.015430e+03 0.000000e+00 0.000000e+00 2.200000e+02 1.277693e+01 1.277693e+01 +1.015750e+03 0.000000e+00 0.000000e+00 2.431000e+02 1.428690e+01 1.428690e+01 +1.016680e+03 0.000000e+00 0.000000e+00 3.589000e+02 2.083755e+01 2.083755e+01 +1.016780e+03 0.000000e+00 0.000000e+00 3.536000e+02 2.087564e+01 2.087564e+01 +1.017590e+03 0.000000e+00 0.000000e+00 4.936000e+02 2.882902e+01 2.882902e+01 +1.017720e+03 0.000000e+00 0.000000e+00 5.150000e+02 2.995250e+01 2.995250e+01 +1.018620e+03 0.000000e+00 0.000000e+00 6.642000e+02 3.570034e+01 3.570034e+01 +1.018780e+03 0.000000e+00 0.000000e+00 6.586000e+02 3.491339e+01 3.491339e+01 +1.019510e+03 0.000000e+00 0.000000e+00 6.670000e+02 3.537602e+01 3.537602e+01 +1.019790e+03 0.000000e+00 0.000000e+00 5.955000e+02 3.294029e+01 3.294029e+01 +1.020430e+03 0.000000e+00 0.000000e+00 4.712000e+02 2.820148e+01 2.820148e+01 +1.020650e+03 0.000000e+00 0.000000e+00 3.998000e+02 2.469514e+01 2.469514e+01 +1.021410e+03 0.000000e+00 0.000000e+00 2.701000e+02 1.674903e+01 1.674903e+01 +1.021680e+03 0.000000e+00 0.000000e+00 2.174000e+02 1.379880e+01 1.379880e+01 +1.022320e+03 0.000000e+00 0.000000e+00 1.429000e+02 9.390932e+00 9.390932e+00 +1.023270e+03 0.000000e+00 0.000000e+00 9.220000e+01 5.728185e+00 5.728185e+00 +1.027520e+03 0.000000e+00 0.000000e+00 1.533000e+01 1.206027e+00 1.206027e+00 +1.028230e+03 0.000000e+00 0.000000e+00 1.081000e+01 9.730879e-01 9.730879e-01 +1.033580e+03 0.000000e+00 0.000000e+00 1.750000e+00 4.924429e-01 4.924429e-01 +1.033840e+03 0.000000e+00 0.000000e+00 1.430000e+00 4.368066e-01 4.368066e-01 +1.039590e+03 0.000000e+00 0.000000e+00 3.700000e-01 3.125700e-01 3.125700e-01 +1.039640e+03 0.000000e+00 0.000000e+00 3.700000e-01 3.114482e-01 3.114482e-01 +1.040000e+03 0.000000e+00 0.000000e+00 4.000000e-01 3.324154e-01 3.324154e-01 +1.049600e+03 0.000000e+00 0.000000e+00 1.120000e+00 2.418677e-01 2.418677e-01 +1.049810e+03 0.000000e+00 0.000000e+00 1.140000e+00 2.580698e-01 2.580698e-01 +1.050000e+03 0.000000e+00 0.000000e+00 1.370000e+00 3.000000e-01 3.000000e-01 +1.059520e+03 0.000000e+00 0.000000e+00 1.750000e+00 2.469818e-01 2.469818e-01 +1.059660e+03 0.000000e+00 0.000000e+00 1.840000e+00 3.087070e-01 3.087070e-01 +1.060000e+03 0.000000e+00 0.000000e+00 2.460000e+00 2.758623e-01 2.758623e-01 +1.070000e+03 0.000000e+00 0.000000e+00 3.210000e+00 5.069517e-01 5.069517e-01 +1.080000e+03 0.000000e+00 0.000000e+00 3.460000e+00 3.255764e-01 3.255764e-01 +1.090000e+03 0.000000e+00 0.000000e+00 3.840000e+00 6.109828e-01 6.109828e-01 +1.100000e+03 0.000000e+00 0.000000e+00 4.070000e+00 3.764306e-01 3.764306e-01 +1.110000e+03 0.000000e+00 0.000000e+00 5.660000e+00 9.424436e-01 9.424436e-01 +1.120000e+03 0.000000e+00 0.000000e+00 5.190000e+00 5.161395e-01 5.161395e-01 +1.130000e+03 0.000000e+00 0.000000e+00 5.040000e+00 7.300685e-01 7.300685e-01 +1.140000e+03 0.000000e+00 0.000000e+00 4.500000e+00 4.770744e-01 4.770744e-01 +1.150000e+03 0.000000e+00 0.000000e+00 6.400000e+00 1.044031e+00 1.044031e+00 +1.160000e+03 0.000000e+00 0.000000e+00 5.120000e+00 4.860041e-01 4.860041e-01 +1.180000e+03 0.000000e+00 0.000000e+00 5.300000e+00 4.763402e-01 4.763402e-01 +1.190000e+03 0.000000e+00 0.000000e+00 5.440000e+00 6.090156e-01 6.090156e-01 +1.200000e+03 0.000000e+00 0.000000e+00 4.890000e+00 4.252058e-01 4.252058e-01 +1.210000e+03 0.000000e+00 0.000000e+00 6.390000e+00 6.946222e-01 6.946222e-01 +1.220000e+03 0.000000e+00 0.000000e+00 5.680000e+00 5.200961e-01 5.200961e-01 +1.230000e+03 0.000000e+00 0.000000e+00 5.480000e+00 6.664833e-01 6.664833e-01 +1.240000e+03 0.000000e+00 0.000000e+00 4.960000e+00 4.341659e-01 4.341659e-01 +1.250000e+03 0.000000e+00 0.000000e+00 5.910000e+00 6.074537e-01 6.074537e-01 +1.260000e+03 0.000000e+00 0.000000e+00 5.920000e+00 6.847627e-01 6.847627e-01 +1.270000e+03 0.000000e+00 0.000000e+00 5.410000e+00 5.630275e-01 5.630275e-01 +1.280000e+03 0.000000e+00 0.000000e+00 5.500000e+00 5.300943e-01 5.300943e-01 +1.290000e+03 0.000000e+00 0.000000e+00 5.460000e+00 5.220153e-01 5.220153e-01 +1.300000e+03 0.000000e+00 0.000000e+00 5.130000e+00 4.940648e-01 4.940648e-01 +1.310000e+03 0.000000e+00 0.000000e+00 5.590000e+00 6.053924e-01 6.053924e-01 +1.320000e+03 0.000000e+00 0.000000e+00 5.440000e+00 5.382379e-01 5.382379e-01 +1.330000e+03 0.000000e+00 0.000000e+00 5.170000e+00 4.780167e-01 4.780167e-01 +1.340000e+03 0.000000e+00 0.000000e+00 4.700000e+00 4.341659e-01 4.341659e-01 +1.350000e+03 0.000000e+00 0.000000e+00 4.820000e+00 4.909175e-01 4.909175e-01 +1.360000e+03 0.000000e+00 0.000000e+00 4.680000e+00 3.818377e-01 3.818377e-01 +1.370000e+03 0.000000e+00 0.000000e+00 5.090000e+00 5.186521e-01 5.186521e-01 +1.380000e+03 0.000000e+00 0.000000e+00 4.210000e+00 3.753665e-01 3.753665e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2002_I587084.cc b/analyses/pluginNovosibirsk/SND_2002_I587084.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2002_I587084.cc @@ -0,0 +1,88 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2002_I587084 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2002_I587084); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + _numPiPiGamma = bookCounter("TMP/PiPiGamma"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // three particles (pi0 pi0 gamma) + if(ntotal!=3) vetoEvent; + if(nCount[111]==2 && nCount[22]==1) + _numPiPiGamma->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _numPiPiGamma->val(); + double error = _numPiPiGamma->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numPiPiGamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2002_I587084); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2002_I587084.info b/analyses/pluginNovosibirsk/SND_2002_I587084.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2002_I587084.info @@ -0,0 +1,34 @@ +Name: SND_2002_I587084 +Year: 2002 +Summary: Cross section for $e^+e^-\to\pi^0\pi^0\gamma$ at energies between 0.6 and 0.97 GeV. +Experiment: SND +Collider: VEPP-2M +InspireID: 587084 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D94 (2016) no.11, 112001 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^0\pi^0\gamma$ at energies between 0.6 and 0.97 GeV.' +Keywords: [] +BibKey: Achasov:2002jv +BibTeX: '@article{Achasov:2002jv, + author = "Achasov, M. N. and others", + title = "{Experimental study of rho ---> pi0 pi0 gamma and omega + ---> pi0 pi0 gamma decays}", + journal = "Phys. Lett.", + volume = "B537", + year = "2002", + pages = "201-210", + doi = "10.1016/S0370-2693(02)01825-7", + eprint = "hep-ex/0205068", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0205068;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2002_I587084.plot b/analyses/pluginNovosibirsk/SND_2002_I587084.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2002_I587084.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2002_I587084/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^0\pi^0\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^0\pi^0\gamma)$/nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2002_I587084.yoda b/analyses/pluginNovosibirsk/SND_2002_I587084.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2002_I587084.yoda @@ -0,0 +1,38 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2002_I587084/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2002_I587084/d01-x01-y01 +Title: doi:10.17182/hepdata.41973.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.001000e+02 2.900000e-01 2.900000e-01 -5.000000e-03 2.030394e-03 5.200118e-02 +6.301000e+02 3.000000e-01 3.000000e-01 -4.000000e-03 2.019505e-03 4.100096e-02 +6.602000e+02 2.500000e-01 2.500000e-01 2.500000e-02 1.908042e-02 4.003826e-02 +6.902000e+02 2.900000e-01 2.900000e-01 4.600000e-02 3.315672e-02 6.707733e-02 +7.203000e+02 2.600000e-01 2.600000e-01 2.000000e-03 7.001400e-03 1.800054e-02 +7.502000e+02 3.200000e-01 3.200000e-01 5.700000e-02 3.224779e-02 5.713948e-02 +7.602000e+02 3.100000e-01 3.100000e-01 3.200000e-02 2.410431e-02 4.905117e-02 +7.642000e+02 3.200000e-01 3.200000e-01 8.500000e-02 3.846300e-02 6.029430e-02 +7.702000e+02 3.100000e-01 3.100000e-01 1.220000e-01 4.482111e-02 6.357619e-02 +7.742000e+02 3.400000e-01 3.400000e-01 1.450000e-01 5.592873e-02 8.163346e-02 +7.781000e+02 3.400000e-01 3.400000e-01 1.040000e-01 4.558507e-02 6.838858e-02 +7.802000e+02 3.500000e-01 3.500000e-01 2.180000e-01 6.094151e-02 7.653671e-02 +7.811000e+02 3.300000e-01 3.300000e-01 2.570000e-01 6.359749e-02 7.810019e-02 +7.821000e+02 3.100000e-01 3.100000e-01 2.400000e-01 4.523538e-02 5.274694e-02 +7.832000e+02 3.000000e-01 3.000000e-01 2.800000e-01 5.838801e-02 6.884882e-02 +7.842000e+02 3.200000e-01 3.200000e-01 3.010000e-01 6.643000e-02 7.983073e-02 +7.853000e+02 2.400000e-01 2.400000e-01 2.380000e-01 7.195523e-02 9.546494e-02 +7.861000e+02 3.300000e-01 3.300000e-01 1.700000e-01 5.334426e-02 7.199035e-02 +7.901000e+02 3.400000e-01 3.400000e-01 7.400000e-02 3.934250e-02 6.420929e-02 +7.942000e+02 3.400000e-01 3.400000e-01 1.400000e-02 1.503198e-02 4.201143e-02 +8.002000e+02 3.200000e-01 3.200000e-01 1.300000e-01 4.297453e-02 5.772183e-02 +8.102000e+02 3.400000e-01 3.400000e-01 3.700000e-02 2.413935e-02 3.011159e-02 +8.201000e+02 3.600000e-01 3.600000e-01 2.100000e-02 1.606739e-02 3.303272e-02 +8.402000e+02 3.500000e-01 3.500000e-01 4.200000e-02 1.626787e-02 2.318714e-02 +8.800000e+02 4.100000e-01 4.100000e-01 7.800000e-02 3.147716e-02 4.533003e-02 +9.199000e+02 4.400000e-01 4.400000e-01 6.900000e-02 2.546230e-02 3.533170e-02 +9.399000e+02 4.300000e-01 4.300000e-01 2.140000e-01 4.932951e-02 5.990326e-02 +9.497000e+02 3.200000e-01 3.200000e-01 3.380000e-01 7.959771e-02 9.790197e-02 +9.577000e+02 3.200000e-01 3.200000e-01 2.420000e-01 6.910835e-02 9.059781e-02 +9.697000e+02 3.400000e-01 3.400000e-01 5.240000e-01 1.055766e-01 1.245248e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2003_I612867.cc b/analyses/pluginNovosibirsk/SND_2003_I612867.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2003_I612867.cc @@ -0,0 +1,84 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2003_I612867 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2003_I612867); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + _numPi0Gamma = bookCounter("TMP/Pi0Gamma"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && nCount[22]==1 && nCount[111]==1) + _numPi0Gamma->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _numPi0Gamma->val(); + double error = _numPi0Gamma->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numPi0Gamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2003_I612867); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2003_I612867.info b/analyses/pluginNovosibirsk/SND_2003_I612867.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2003_I612867.info @@ -0,0 +1,31 @@ +Name: SND_2003_I612867 +Year: 2003 +Summary: Cross section for $e^+e^-\to\pi\gamma$ for energies between 600 MeV and 970 MeV +Experiment: SND +Collider: VEPP-2M +InspireID: 612867 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys. Lett. B559, 171 (2003) +RunInfo: e+ e- to hadrons below 0.6 and 1.38 GeV +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\pi\gamma$ for energies between 600 MeV and 970 MeV' +BibKey: Achasov:2003ed +BibTeX: '@article{Achasov:2003ed, + author = "Achasov, M. N. and others", + title = "{Experimental study of the e+ e- ---> pi0 gamma process + in the energy region s**1/2 = 0.60-GeV - 0.97-GeV}", + journal = "Phys. Lett.", + volume = "B559", + year = "2003", + pages = "171-178", + doi = "10.1016/S0370-2693(03)00336-8", + eprint = "hep-ex/0302004", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0302004;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2003_I612867.plot b/analyses/pluginNovosibirsk/SND_2003_I612867.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2003_I612867.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2003_I612867/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^0\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^0\gamma)$/nb +LogY=1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2003_I612867.yoda b/analyses/pluginNovosibirsk/SND_2003_I612867.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2003_I612867.yoda @@ -0,0 +1,56 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2003_I612867/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2003_I612867/d01-x01-y01 +Title: doi:10.17182/hepdata.41964.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.995200e+02 1.400000e-01 1.400000e-01 1.230000e+00 7.930952e-01 7.930952e-01 +6.295100e+02 1.500000e-01 1.500000e-01 1.310000e+00 8.045496e-01 8.045496e-01 +6.595200e+02 1.600000e-01 1.600000e-01 4.500000e-01 6.525335e-01 6.525335e-01 +6.895600e+02 1.900000e-01 1.900000e-01 1.100000e+00 6.618912e-01 6.618912e-01 +7.195100e+02 1.800000e-01 1.800000e-01 1.970000e+00 5.882176e-01 5.882176e-01 +7.495000e+02 2.000000e-01 2.000000e-01 4.090000e+00 7.818568e-01 7.818568e-01 +7.595000e+02 2.000000e-01 2.000000e-01 7.710000e+00 1.103087e+00 1.103087e+00 +7.635000e+02 2.100000e-01 2.100000e-01 1.027000e+01 1.279453e+00 1.279453e+00 +7.695000e+02 2.100000e-01 2.100000e-01 1.895000e+01 1.808010e+00 1.808010e+00 +7.735000e+02 2.100000e-01 2.100000e-01 3.162000e+01 2.093466e+00 2.093466e+00 +7.775000e+02 2.100000e-01 2.100000e-01 7.960000e+01 3.026450e+00 3.026450e+00 +7.787100e+02 2.200000e-01 2.200000e-01 9.389000e+01 8.982722e+00 8.982722e+00 +7.794800e+02 2.400000e-01 2.400000e-01 1.184900e+02 4.540396e+00 4.540396e+00 +7.805900e+02 2.300000e-01 2.300000e-01 1.513600e+02 4.919350e+00 4.919350e+00 +7.816300e+02 2.400000e-01 2.400000e-01 1.728200e+02 5.344848e+00 5.344848e+00 +7.825200e+02 2.100000e-01 2.100000e-01 1.698300e+02 5.594748e+00 5.594748e+00 +7.835100e+02 2.100000e-01 2.100000e-01 1.595300e+02 6.196491e+00 6.196491e+00 +7.855100e+02 2.200000e-01 2.200000e-01 1.131500e+02 3.978002e+00 3.978002e+00 +7.895000e+02 2.200000e-01 2.200000e-01 4.761000e+01 2.191004e+00 2.191004e+00 +7.934900e+02 2.300000e-01 2.300000e-01 2.126000e+01 1.360147e+00 1.360147e+00 +7.994900e+02 2.300000e-01 2.300000e-01 1.127000e+01 8.300602e-01 8.300602e-01 +8.094900e+02 2.500000e-01 2.500000e-01 4.700000e+00 4.492215e-01 4.492215e-01 +8.194900e+02 2.400000e-01 2.400000e-01 2.900000e+00 3.140064e-01 3.140064e-01 +8.394700e+02 2.500000e-01 2.500000e-01 1.590000e+00 1.931321e-01 1.931321e-01 +8.794500e+02 2.700000e-01 2.700000e-01 7.200000e-01 2.334524e-01 2.334524e-01 +9.194300e+02 3.200000e-01 3.200000e-01 5.400000e-01 1.264911e-01 1.264911e-01 +9.394500e+02 3.000000e-01 3.000000e-01 3.900000e-01 1.500000e-01 1.500000e-01 +9.494500e+02 2.900000e-01 2.900000e-01 3.900000e-01 1.431782e-01 1.431782e-01 +9.574500e+02 2.900000e-01 2.900000e-01 4.000000e-01 1.431782e-01 1.431782e-01 +9.694600e+02 3.000000e-01 3.000000e-01 4.800000e-01 1.640122e-01 1.640122e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2003_I612867/d02-x01-y01 +IsRef: 1 +Path: /REF/SND_2003_I612867/d02-x01-y01 +Title: doi:10.17182/hepdata.41964.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.850000e-01 1.850000e-01 1.850000e-01 1.558000e+02 5.507268e+00 5.507268e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2003_I612867/d02-x01-y02 +IsRef: 1 +Path: /REF/SND_2003_I612867/d02-x01-y02 +Title: doi:10.17182/hepdata.41964.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.850000e-01 1.850000e-01 1.850000e-01 5.800000e-01 1.526434e-01 1.526434e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2003_I619011.cc b/analyses/pluginNovosibirsk/SND_2003_I619011.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2003_I619011.cc @@ -0,0 +1,88 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2003_I619011 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2003_I619011); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + _num3pi = bookCounter("TMP/num3"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=3) vetoEvent; + if(nCount[-211]==1&&nCount[211]==1&&nCount[111]==1) + _num3pi->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _num3pi->val(); + double error = _num3pi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _num3pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2003_I619011); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2003_I619011.info b/analyses/pluginNovosibirsk/SND_2003_I619011.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2003_I619011.info @@ -0,0 +1,32 @@ +Name: SND_2003_I619011 +Year: 2003 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ between 0.44 and 0.97 GeV. +Experiment: SND +Collider: VEPP-2M +InspireID: 619011 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D68 (2003) 052006, 2003 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ by SND for energies between 0.44 and 0.97 GeV.' +Keywords: +BibKey: Achasov:2003ir +BibTeX: '@article{Achasov:2003ir, + author = "Achasov, M. N. and others", + title = "{Study of the process e+ e- ---> pi+ pi- pi0 in the + energy region s**(1/2) below 0.98-GeV}", + journal = "Phys. Rev.", + volume = "D68", + year = "2003", + pages = "052006", + doi = "10.1103/PhysRevD.68.052006", + eprint = "hep-ex/0305049", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0305049;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2003_I619011.plot b/analyses/pluginNovosibirsk/SND_2003_I619011.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2003_I619011.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2003_I619011/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +LegendXPos=0.1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2003_I619011.yoda b/analyses/pluginNovosibirsk/SND_2003_I619011.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2003_I619011.yoda @@ -0,0 +1,57 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2003_I619011/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2003_I619011/d01-x01-y01 +Title: doi:10.17182/hepdata.41957.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.600000e+02 0.000000e+00 0.000000e+00 4.600000e-01 2.385372e-01 2.385372e-01 +6.900000e+02 0.000000e+00 0.000000e+00 1.100000e+00 3.189044e-01 3.189044e-01 +7.200000e+02 0.000000e+00 0.000000e+00 3.690000e+00 3.061046e-01 3.061046e-01 +7.497900e+02 0.000000e+00 0.000000e+00 1.640000e+01 1.448033e+00 1.448033e+00 +7.504000e+02 0.000000e+00 0.000000e+00 2.012000e+01 1.089036e+00 1.089036e+00 +7.597900e+02 0.000000e+00 0.000000e+00 4.614000e+01 2.840370e+00 2.840370e+00 +7.604000e+02 0.000000e+00 0.000000e+00 4.538000e+01 1.956016e+00 1.956016e+00 +7.637900e+02 0.000000e+00 0.000000e+00 6.343000e+01 3.598027e+00 3.598027e+00 +7.644000e+02 0.000000e+00 0.000000e+00 6.848000e+01 2.840070e+00 2.840070e+00 +7.697900e+02 0.000000e+00 0.000000e+00 1.297400e+02 6.357366e+00 6.357366e+00 +7.704000e+02 0.000000e+00 0.000000e+00 1.585800e+02 6.368493e+00 6.368493e+00 +7.737900e+02 0.000000e+00 0.000000e+00 2.787200e+02 1.232101e+01 1.232101e+01 +7.744000e+02 0.000000e+00 0.000000e+00 3.259000e+02 1.360925e+01 1.360925e+01 +7.777900e+02 0.000000e+00 0.000000e+00 6.930800e+02 3.050171e+01 3.050171e+01 +7.781100e+02 0.000000e+00 0.000000e+00 7.654100e+02 3.284025e+01 3.284025e+01 +7.784000e+02 0.000000e+00 0.000000e+00 8.228100e+02 3.528772e+01 3.528772e+01 +7.797900e+02 0.000000e+00 0.000000e+00 1.098850e+03 4.827946e+01 4.827946e+01 +7.799000e+02 0.000000e+00 0.000000e+00 1.146890e+03 4.847540e+01 4.847540e+01 +7.804000e+02 0.000000e+00 0.000000e+00 1.261060e+03 5.167323e+01 5.167323e+01 +7.807900e+02 0.000000e+00 0.000000e+00 1.369110e+03 5.473159e+01 5.473159e+01 +7.814000e+02 0.000000e+00 0.000000e+00 1.470940e+03 5.620744e+01 5.620744e+01 +7.817900e+02 0.000000e+00 0.000000e+00 1.550800e+03 5.708546e+01 5.708546e+01 +7.821300e+02 0.000000e+00 0.000000e+00 1.552850e+03 6.665360e+01 6.665360e+01 +7.824000e+02 0.000000e+00 0.000000e+00 1.584210e+03 5.673854e+01 5.673854e+01 +7.827900e+02 0.000000e+00 0.000000e+00 1.624770e+03 5.890626e+01 5.890626e+01 +7.829000e+02 0.000000e+00 0.000000e+00 1.627560e+03 5.847196e+01 5.847196e+01 +7.834000e+02 0.000000e+00 0.000000e+00 1.542580e+03 5.527381e+01 5.527381e+01 +7.837900e+02 0.000000e+00 0.000000e+00 1.514970e+03 5.640763e+01 5.640763e+01 +7.844000e+02 0.000000e+00 0.000000e+00 1.382690e+03 5.188224e+01 5.188224e+01 +7.854000e+02 0.000000e+00 0.000000e+00 1.154290e+03 4.525159e+01 4.525159e+01 +7.857900e+02 0.000000e+00 0.000000e+00 1.068390e+03 4.320052e+01 4.320052e+01 +7.861800e+02 0.000000e+00 0.000000e+00 9.989200e+02 4.211853e+01 4.211853e+01 +7.864000e+02 0.000000e+00 0.000000e+00 9.436300e+02 3.773765e+01 3.773765e+01 +7.897900e+02 0.000000e+00 0.000000e+00 4.379100e+02 1.824869e+01 1.824869e+01 +7.904000e+02 0.000000e+00 0.000000e+00 4.193100e+02 1.647818e+01 1.647818e+01 +7.937900e+02 0.000000e+00 0.000000e+00 2.335400e+02 9.655719e+00 9.655719e+00 +7.944000e+02 0.000000e+00 0.000000e+00 2.152500e+02 8.307647e+00 8.307647e+00 +7.997900e+02 0.000000e+00 0.000000e+00 1.110900e+02 4.829120e+00 4.829120e+00 +8.004000e+02 0.000000e+00 0.000000e+00 1.104200e+02 4.195331e+00 4.195331e+00 +8.097900e+02 0.000000e+00 0.000000e+00 5.581000e+01 2.522400e+00 2.522400e+00 +8.104000e+02 0.000000e+00 0.000000e+00 5.384000e+01 2.134127e+00 2.134127e+00 +8.200000e+02 0.000000e+00 0.000000e+00 3.293000e+01 1.332817e+00 1.332817e+00 +8.400000e+02 0.000000e+00 0.000000e+00 1.877000e+01 7.738863e-01 7.738863e-01 +8.800000e+02 0.000000e+00 0.000000e+00 1.122000e+01 5.841233e-01 5.841233e-01 +9.200000e+02 0.000000e+00 0.000000e+00 9.820000e+00 6.341136e-01 6.341136e-01 +9.400000e+02 0.000000e+00 0.000000e+00 9.830000e+00 6.621933e-01 6.621933e-01 +9.500000e+02 0.000000e+00 0.000000e+00 1.117000e+01 8.489994e-01 8.489994e-01 +9.580000e+02 0.000000e+00 0.000000e+00 1.133000e+01 8.637129e-01 8.637129e-01 +9.700000e+02 0.000000e+00 0.000000e+00 1.282000e+01 9.620811e-01 9.620811e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2005_I686349.cc b/analyses/pluginNovosibirsk/SND_2005_I686349.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2005_I686349.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2005_I686349 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2005_I686349); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2005_I686349); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2005_I686349.info b/analyses/pluginNovosibirsk/SND_2005_I686349.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2005_I686349.info @@ -0,0 +1,36 @@ +Name: SND_2005_I686349 +Year: 2005 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ at energies between 0.4 and 1 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 686349 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- J. Exp. Theor. Phys. 101, 1053 (2005) +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies between 0.4 and 1 GeV' +Keywords: [] +BibKey: Achasov:2005rg +BibTeX: '@article{Achasov:2005rg, + author = "Achasov, M. N. and others", + title = "{Study of the process e+ e- ---> pi+ pi- in the energy + region 400 < s**(1/2) < 1000-MeV}", + journal = "J. Exp. Theor. Phys.", + volume = "101", + year = "2005", + number = "6", + pages = "1053-1070", + doi = "10.1134/1.2163921", + note = "[Zh. Eksp. Teor. Fiz.128,no.6,1201(2005)]", + eprint = "hep-ex/0506076", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0506076;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2005_I686349.plot b/analyses/pluginNovosibirsk/SND_2005_I686349.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2005_I686349.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /SND_2005_I686349/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2005_I686349.yoda b/analyses/pluginNovosibirsk/SND_2005_I686349.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2005_I686349.yoda @@ -0,0 +1,159 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2005_I686349/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2005_I686349/d01-x01-y01 +Title: doi:10.17182/hepdata.41873.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.900000e+02 0.000000e+00 0.000000e+00 1.163700e+02 2.178000e+01 2.178000e+01 +4.100000e+02 0.000000e+00 0.000000e+00 1.250600e+02 1.892000e+01 1.892000e+01 +4.300000e+02 0.000000e+00 0.000000e+00 1.092500e+02 1.254000e+01 1.254000e+01 +4.400000e+02 0.000000e+00 0.000000e+00 1.147500e+02 1.551000e+01 1.551000e+01 +4.500000e+02 0.000000e+00 0.000000e+00 1.404700e+02 1.424000e+01 1.424000e+01 +4.700000e+02 0.000000e+00 0.000000e+00 1.436100e+02 1.328000e+01 1.328000e+01 +4.800000e+02 0.000000e+00 0.000000e+00 1.656000e+02 9.720000e+00 9.720000e+00 +5.000000e+02 0.000000e+00 0.000000e+00 1.763200e+02 1.093000e+01 1.093000e+01 +5.100000e+02 0.000000e+00 0.000000e+00 1.753700e+02 1.681000e+01 1.681000e+01 +5.200000e+02 0.000000e+00 0.000000e+00 1.795500e+02 1.042000e+01 1.042000e+01 +5.300000e+02 0.000000e+00 0.000000e+00 2.023200e+02 2.304000e+01 2.304000e+01 +5.400000e+02 0.000000e+00 0.000000e+00 2.156100e+02 1.379000e+01 1.379000e+01 +5.500000e+02 0.000000e+00 0.000000e+00 2.210000e+02 1.783000e+01 1.783000e+01 +5.600000e+02 0.000000e+00 0.000000e+00 2.309100e+02 1.269000e+01 1.269000e+01 +5.800000e+02 0.000000e+00 0.000000e+00 2.614900e+02 1.478000e+01 1.478000e+01 +6.000000e+02 0.000000e+00 0.000000e+00 2.960600e+02 1.092000e+01 1.092000e+01 +6.300000e+02 0.000000e+00 0.000000e+00 3.986100e+02 8.730000e+00 8.730000e+00 +6.600000e+02 0.000000e+00 0.000000e+00 5.437500e+02 6.240000e+00 6.240000e+00 +6.900000e+02 0.000000e+00 0.000000e+00 7.645300e+02 8.310000e+00 8.310000e+00 +7.200000e+02 0.000000e+00 0.000000e+00 1.060140e+03 7.110000e+00 7.110000e+00 +7.500000e+02 0.000000e+00 0.000000e+00 1.291960e+03 2.280000e+01 2.280000e+01 +7.600000e+02 0.000000e+00 0.000000e+00 1.308400e+03 1.008000e+01 1.008000e+01 +7.640000e+02 0.000000e+00 0.000000e+00 1.304400e+03 9.800000e+00 9.800000e+00 +7.700000e+02 0.000000e+00 0.000000e+00 1.302160e+03 9.670000e+00 9.670000e+00 +7.740000e+02 0.000000e+00 0.000000e+00 1.331590e+03 9.870000e+00 9.870000e+00 +7.780000e+02 0.000000e+00 0.000000e+00 1.314330e+03 9.780000e+00 9.780000e+00 +7.800000e+02 0.000000e+00 0.000000e+00 1.233580e+03 1.017000e+01 1.017000e+01 +7.810000e+02 0.000000e+00 0.000000e+00 1.161620e+03 1.084000e+01 1.084000e+01 +7.820000e+02 0.000000e+00 0.000000e+00 1.106690e+03 2.644000e+01 2.644000e+01 +7.830000e+02 0.000000e+00 0.000000e+00 1.022450e+03 1.099000e+01 1.099000e+01 +7.840000e+02 0.000000e+00 0.000000e+00 9.404200e+02 1.912000e+01 1.912000e+01 +7.850000e+02 0.000000e+00 0.000000e+00 8.876800e+02 8.810000e+00 8.810000e+00 +7.860000e+02 0.000000e+00 0.000000e+00 8.742300e+02 7.420000e+00 7.420000e+00 +7.900000e+02 0.000000e+00 0.000000e+00 8.555500e+02 1.698000e+01 1.698000e+01 +7.940000e+02 0.000000e+00 0.000000e+00 8.593500e+02 7.190000e+00 7.190000e+00 +8.000000e+02 0.000000e+00 0.000000e+00 8.226600e+02 7.050000e+00 7.050000e+00 +8.100000e+02 0.000000e+00 0.000000e+00 7.159400e+02 6.210000e+00 6.210000e+00 +8.200000e+02 0.000000e+00 0.000000e+00 6.225400e+02 5.540000e+00 5.540000e+00 +8.400000e+02 0.000000e+00 0.000000e+00 4.507000e+02 4.190000e+00 4.190000e+00 +8.800000e+02 0.000000e+00 0.000000e+00 2.463800e+02 2.800000e+00 2.800000e+00 +9.200000e+02 0.000000e+00 0.000000e+00 1.477800e+02 5.150000e+00 5.150000e+00 +9.400000e+02 0.000000e+00 0.000000e+00 1.151400e+02 1.570000e+00 1.570000e+00 +9.500000e+02 0.000000e+00 0.000000e+00 1.015200e+02 1.930000e+00 1.930000e+00 +9.580000e+02 0.000000e+00 0.000000e+00 9.133000e+01 1.960000e+00 1.960000e+00 +9.700000e+02 0.000000e+00 0.000000e+00 7.668000e+01 1.790000e+00 1.790000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2005_I686349/d02-x01-y01 +IsRef: 1 +Path: /REF/SND_2005_I686349/d02-x01-y01 +Title: doi:10.17182/hepdata.41873.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.900000e+02 0.000000e+00 0.000000e+00 2.390000e+00 4.500000e-01 4.500000e-01 +4.100000e+02 0.000000e+00 0.000000e+00 2.460000e+00 3.700000e-01 3.700000e-01 +4.300000e+02 0.000000e+00 0.000000e+00 2.110000e+00 2.400000e-01 2.400000e-01 +4.400000e+02 0.000000e+00 0.000000e+00 2.220000e+00 3.000000e-01 3.000000e-01 +4.500000e+02 0.000000e+00 0.000000e+00 2.710000e+00 2.800000e-01 2.800000e-01 +4.700000e+02 0.000000e+00 0.000000e+00 2.810000e+00 2.600000e-01 2.600000e-01 +4.800000e+02 0.000000e+00 0.000000e+00 3.260000e+00 1.900000e-01 1.900000e-01 +5.000000e+02 0.000000e+00 0.000000e+00 3.550000e+00 2.200000e-01 2.200000e-01 +5.100000e+02 0.000000e+00 0.000000e+00 3.580000e+00 3.400000e-01 3.400000e-01 +5.200000e+02 0.000000e+00 0.000000e+00 3.720000e+00 2.200000e-01 2.200000e-01 +5.300000e+02 0.000000e+00 0.000000e+00 4.260000e+00 4.900000e-01 4.900000e-01 +5.400000e+02 0.000000e+00 0.000000e+00 4.620000e+00 3.000000e-01 3.000000e-01 +5.500000e+02 0.000000e+00 0.000000e+00 4.810000e+00 3.900000e-01 3.900000e-01 +5.600000e+02 0.000000e+00 0.000000e+00 5.120000e+00 2.800000e-01 2.800000e-01 +5.800000e+02 0.000000e+00 0.000000e+00 6.010000e+00 3.400000e-01 3.400000e-01 +6.000000e+02 0.000000e+00 0.000000e+00 7.080000e+00 2.600000e-01 2.600000e-01 +6.300000e+02 0.000000e+00 0.000000e+00 1.011000e+01 2.200000e-01 2.200000e-01 +6.600000e+02 0.000000e+00 0.000000e+00 1.466000e+01 1.700000e-01 1.700000e-01 +6.900000e+02 0.000000e+00 0.000000e+00 2.192000e+01 2.400000e-01 2.400000e-01 +7.200000e+02 0.000000e+00 0.000000e+00 3.231000e+01 2.200000e-01 2.200000e-01 +7.500000e+02 0.000000e+00 0.000000e+00 4.186000e+01 7.400000e-01 7.400000e-01 +7.600000e+02 0.000000e+00 0.000000e+00 4.326000e+01 3.300000e-01 3.300000e-01 +7.640000e+02 0.000000e+00 0.000000e+00 4.347000e+01 3.300000e-01 3.300000e-01 +7.700000e+02 0.000000e+00 0.000000e+00 4.392000e+01 3.300000e-01 3.300000e-01 +7.740000e+02 0.000000e+00 0.000000e+00 4.528000e+01 3.400000e-01 3.400000e-01 +7.780000e+02 0.000000e+00 0.000000e+00 4.505000e+01 3.400000e-01 3.400000e-01 +7.800000e+02 0.000000e+00 0.000000e+00 4.245000e+01 3.500000e-01 3.500000e-01 +7.810000e+02 0.000000e+00 0.000000e+00 4.006000e+01 3.700000e-01 3.700000e-01 +7.820000e+02 0.000000e+00 0.000000e+00 3.824000e+01 9.100000e-01 9.100000e-01 +7.830000e+02 0.000000e+00 0.000000e+00 3.540000e+01 3.800000e-01 3.800000e-01 +7.840000e+02 0.000000e+00 0.000000e+00 3.262000e+01 6.600000e-01 6.600000e-01 +7.850000e+02 0.000000e+00 0.000000e+00 3.086000e+01 3.100000e-01 3.100000e-01 +7.860000e+02 0.000000e+00 0.000000e+00 3.045000e+01 2.600000e-01 2.600000e-01 +7.900000e+02 0.000000e+00 0.000000e+00 3.004000e+01 6.000000e-01 6.000000e-01 +7.940000e+02 0.000000e+00 0.000000e+00 3.041000e+01 2.500000e-01 2.500000e-01 +8.000000e+02 0.000000e+00 0.000000e+00 2.946000e+01 2.500000e-01 2.500000e-01 +8.100000e+02 0.000000e+00 0.000000e+00 2.615000e+01 2.300000e-01 2.300000e-01 +8.200000e+02 0.000000e+00 0.000000e+00 2.319000e+01 2.100000e-01 2.100000e-01 +8.400000e+02 0.000000e+00 0.000000e+00 1.746000e+01 1.600000e-01 1.600000e-01 +8.800000e+02 0.000000e+00 0.000000e+00 1.030000e+01 1.200000e-01 1.200000e-01 +9.200000e+02 0.000000e+00 0.000000e+00 6.660000e+00 2.300000e-01 2.300000e-01 +9.400000e+02 0.000000e+00 0.000000e+00 5.380000e+00 7.000000e-02 7.000000e-02 +9.500000e+02 0.000000e+00 0.000000e+00 4.830000e+00 9.000000e-02 9.000000e-02 +9.580000e+02 0.000000e+00 0.000000e+00 4.410000e+00 9.000000e-02 9.000000e-02 +9.700000e+02 0.000000e+00 0.000000e+00 3.780000e+00 9.000000e-02 9.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2005_I686349/d03-x01-y01 +IsRef: 1 +Path: /REF/SND_2005_I686349/d03-x01-y01 +Title: doi:10.17182/hepdata.41873.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.900000e+02 0.000000e+00 0.000000e+00 1.161700e+02 2.174000e+01 2.174000e+01 +4.100000e+02 0.000000e+00 0.000000e+00 1.247000e+02 1.887000e+01 1.887000e+01 +4.300000e+02 0.000000e+00 0.000000e+00 1.088300e+02 1.249000e+01 1.249000e+01 +4.400000e+02 0.000000e+00 0.000000e+00 1.142600e+02 1.544000e+01 1.544000e+01 +4.500000e+02 0.000000e+00 0.000000e+00 1.398200e+02 1.417000e+01 1.417000e+01 +4.700000e+02 0.000000e+00 0.000000e+00 1.431400e+02 1.324000e+01 1.324000e+01 +4.800000e+02 0.000000e+00 0.000000e+00 1.650100e+02 9.690000e+00 9.690000e+00 +5.000000e+02 0.000000e+00 0.000000e+00 1.756000e+02 1.089000e+01 1.089000e+01 +5.100000e+02 0.000000e+00 0.000000e+00 1.746200e+02 1.674000e+01 1.674000e+01 +5.200000e+02 0.000000e+00 0.000000e+00 1.791000e+02 1.039000e+01 1.039000e+01 +5.300000e+02 0.000000e+00 0.000000e+00 2.017700e+02 2.298000e+01 2.298000e+01 +5.400000e+02 0.000000e+00 0.000000e+00 2.149900e+02 1.375000e+01 1.375000e+01 +5.500000e+02 0.000000e+00 0.000000e+00 2.203300e+02 1.778000e+01 1.778000e+01 +5.600000e+02 0.000000e+00 0.000000e+00 2.305400e+02 1.267000e+01 1.267000e+01 +5.800000e+02 0.000000e+00 0.000000e+00 2.611100e+02 1.476000e+01 1.476000e+01 +6.000000e+02 0.000000e+00 0.000000e+00 2.961700e+02 1.092000e+01 1.092000e+01 +6.300000e+02 0.000000e+00 0.000000e+00 3.994900e+02 8.750000e+00 8.750000e+00 +6.600000e+02 0.000000e+00 0.000000e+00 5.460500e+02 6.270000e+00 6.270000e+00 +6.900000e+02 0.000000e+00 0.000000e+00 7.695600e+02 8.360000e+00 8.360000e+00 +7.200000e+02 0.000000e+00 0.000000e+00 1.064320e+03 7.140000e+00 7.140000e+00 +7.500000e+02 0.000000e+00 0.000000e+00 1.288310e+03 2.274000e+01 2.274000e+01 +7.600000e+02 0.000000e+00 0.000000e+00 1.301280e+03 1.003000e+01 1.003000e+01 +7.640000e+02 0.000000e+00 0.000000e+00 1.297320e+03 9.750000e+00 9.750000e+00 +7.700000e+02 0.000000e+00 0.000000e+00 1.296230e+03 9.630000e+00 9.630000e+00 +7.740000e+02 0.000000e+00 0.000000e+00 1.326860e+03 9.830000e+00 9.830000e+00 +7.780000e+02 0.000000e+00 0.000000e+00 1.309000e+03 9.740000e+00 9.740000e+00 +7.800000e+02 0.000000e+00 0.000000e+00 1.220000e+03 1.006000e+01 1.006000e+01 +7.810000e+02 0.000000e+00 0.000000e+00 1.138880e+03 1.063000e+01 1.063000e+01 +7.820000e+02 0.000000e+00 0.000000e+00 1.073850e+03 2.566000e+01 2.566000e+01 +7.830000e+02 0.000000e+00 0.000000e+00 9.795200e+02 1.053000e+01 1.053000e+01 +7.840000e+02 0.000000e+00 0.000000e+00 8.909400e+02 1.811000e+01 1.811000e+01 +7.850000e+02 0.000000e+00 0.000000e+00 8.352500e+02 8.290000e+00 8.290000e+00 +7.860000e+02 0.000000e+00 0.000000e+00 8.204400e+02 6.960000e+00 6.960000e+00 +7.900000e+02 0.000000e+00 0.000000e+00 8.069600e+02 1.602000e+01 1.602000e+01 +7.940000e+02 0.000000e+00 0.000000e+00 8.158400e+02 6.830000e+00 6.830000e+00 +8.000000e+02 0.000000e+00 0.000000e+00 7.854200e+02 6.730000e+00 6.730000e+00 +8.100000e+02 0.000000e+00 0.000000e+00 6.852600e+02 5.940000e+00 5.940000e+00 +8.200000e+02 0.000000e+00 0.000000e+00 5.972400e+02 5.310000e+00 5.310000e+00 +8.400000e+02 0.000000e+00 0.000000e+00 4.333900e+02 4.030000e+00 4.030000e+00 +8.800000e+02 0.000000e+00 0.000000e+00 2.379300e+02 2.700000e+00 2.700000e+00 +9.200000e+02 0.000000e+00 0.000000e+00 1.435700e+02 5.000000e+00 5.000000e+00 +9.400000e+02 0.000000e+00 0.000000e+00 1.122500e+02 1.530000e+00 1.530000e+00 +9.500000e+02 0.000000e+00 0.000000e+00 9.907000e+01 1.880000e+00 1.880000e+00 +9.580000e+02 0.000000e+00 0.000000e+00 8.922000e+01 1.910000e+00 1.910000e+00 +9.700000e+02 0.000000e+00 0.000000e+00 7.506000e+01 1.750000e+00 1.750000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2006_I717778.cc b/analyses/pluginNovosibirsk/SND_2006_I717778.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2006_I717778.cc @@ -0,0 +1,122 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2006_I717778 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2006_I717778); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaGamma = bookCounter("TMP/EtaGamma"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(val.first==22) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaGamma->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _numEtaGamma->val(); + double error = _numEtaGamma->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + /// @name Histograms + //@{ + CounterPtr _numEtaGamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2006_I717778); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2006_I717778.info b/analyses/pluginNovosibirsk/SND_2006_I717778.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2006_I717778.info @@ -0,0 +1,32 @@ +Name: SND_2006_I717778 +Year: 2006 +Summary: Cross section for $e^+e^-\to\eta\gamma$ for energies between 600 MeV and 1380 MeV +Experiment: SND +Collider: VEPP-2M +InspireID: 717778 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D74 (2006) 014016 +RunInfo: e+ e- to hadrons below 0.6 and 1.38 GeV +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\eta\gamma$ for energies between 600 MeV and 1380 MeV ' +Keywords: [] +BibKey: Achasov:2006dv +BibTeX: '@article{Achasov:2006dv, + author = "Achasov, M. N. and others", + title = "{Study of the e+ e- ---> eta gamma process with SND + detector at the VEPP-2M e+ e- collider}", + journal = "Phys. Rev.", + volume = "D74", + year = "2006", + pages = "014016", + doi = "10.1103/PhysRevD.74.014016", + eprint = "hep-ex/0605109", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0605109;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2006_I717778.plot b/analyses/pluginNovosibirsk/SND_2006_I717778.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2006_I717778.plot @@ -0,0 +1,16 @@ +BEGIN PLOT /SND_2006_I717778/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\gamma)$/nb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /SND_2006_I717778/d02-x01-y01 +Title=$\sigma(e^+e^-\to \eta\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\gamma)$/nb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2006_I717778.yoda b/analyses/pluginNovosibirsk/SND_2006_I717778.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2006_I717778.yoda @@ -0,0 +1,94 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2006_I717778/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2006_I717778/d01-x01-y01 +Title: doi:10.17182/hepdata.41804.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.600000e+02 1.800000e-01 1.800000e-01 5.900000e-02 3.800000e-02 7.800000e-02 +7.200000e+02 2.100000e-01 2.100000e-01 2.200000e-01 5.000000e-02 7.000000e-02 +7.499800e+02 2.300000e-01 2.300000e-01 3.300000e-01 1.000000e-01 1.400000e-01 +7.600000e+02 2.400000e-01 2.400000e-01 3.600000e-01 1.000000e-01 1.400000e-01 +7.640000e+02 2.600000e-01 2.600000e-01 3.200000e-01 9.000000e-02 1.300000e-01 +7.700000e+02 2.500000e-01 2.500000e-01 5.400000e-01 1.200000e-01 1.500000e-01 +7.739800e+02 2.500000e-01 2.500000e-01 7.800000e-01 1.700000e-01 2.000000e-01 +7.780000e+02 3.000000e-01 3.000000e-01 1.500000e+00 2.200000e-01 2.200000e-01 +7.800000e+02 2.500000e-01 2.500000e-01 1.580000e+00 2.100000e-01 2.100000e-01 +7.809800e+02 2.400000e-01 2.400000e-01 2.180000e+00 2.300000e-01 2.300000e-01 +7.820000e+02 2.400000e-01 2.400000e-01 2.130000e+00 1.700000e-01 1.700000e-01 +7.830000e+02 2.400000e-01 2.400000e-01 2.000000e+00 1.900000e-01 1.900000e-01 +7.839800e+02 2.400000e-01 2.400000e-01 1.840000e+00 2.100000e-01 2.100000e-01 +7.850200e+02 2.400000e-01 2.400000e-01 1.520000e+00 2.300000e-01 2.300000e-01 +7.859800e+02 2.400000e-01 2.400000e-01 1.320000e+00 1.900000e-01 1.900000e-01 +7.899600e+02 2.500000e-01 2.500000e-01 8.500000e-01 1.700000e-01 2.100000e-01 +7.939600e+02 2.500000e-01 2.500000e-01 5.900000e-01 1.300000e-01 1.700000e-01 +8.000000e+02 2.500000e-01 2.500000e-01 5.700000e-01 1.100000e-01 1.400000e-01 +8.099800e+02 2.600000e-01 2.600000e-01 2.900000e-01 8.000000e-02 1.100000e-01 +8.199400e+02 2.600000e-01 2.600000e-01 4.600000e-01 9.000000e-02 1.200000e-01 +8.400000e+02 2.800000e-01 2.800000e-01 2.500000e-01 5.000000e-02 6.000000e-02 +8.799200e+02 3.100000e-01 3.100000e-01 1.900000e-01 6.000000e-02 8.000000e-02 +9.198600e+02 3.500000e-01 3.500000e-01 2.700000e-01 6.000000e-02 8.000000e-02 +9.398800e+02 3.400000e-01 3.400000e-01 2.700000e-01 6.000000e-02 8.000000e-02 +9.497800e+02 3.200000e-01 3.200000e-01 1.600000e-01 6.000000e-02 1.000000e-01 +9.578000e+02 3.200000e-01 3.200000e-01 3.900000e-01 1.100000e-01 1.400000e-01 +9.698000e+02 3.400000e-01 3.400000e-01 2.300000e-01 8.000000e-02 1.100000e-01 +9.800000e+02 2.100000e-01 2.100000e-01 2.400000e-01 1.200000e-01 1.900000e-01 +9.841000e+02 3.700000e-01 3.700000e-01 4.200000e-01 9.000000e-02 1.200000e-01 +1.003820e+03 3.800000e-01 3.800000e-01 1.600000e+00 1.900000e-01 1.900000e-01 +1.009680e+03 3.900000e-01 3.900000e-01 3.180000e+00 3.100000e-01 3.100000e-01 +1.015640e+03 3.900000e-01 3.900000e-01 1.510000e+01 8.900000e-01 8.900000e-01 +1.016700e+03 3.800000e-01 3.800000e-01 2.499000e+01 1.260000e+00 1.260000e+00 +1.017660e+03 3.800000e-01 3.800000e-01 3.544000e+01 1.790000e+00 1.790000e+00 +1.018640e+03 3.900000e-01 3.900000e-01 5.353000e+01 1.730000e+00 1.730000e+00 +1.019620e+03 4.200000e-01 4.200000e-01 5.402000e+01 1.290000e+00 1.290000e+00 +1.020580e+03 4.000000e-01 4.000000e-01 4.131000e+01 1.700000e+00 1.700000e+00 +1.021640e+03 4.100000e-01 4.100000e-01 2.332000e+01 1.220000e+00 1.220000e+00 +1.022780e+03 3.900000e-01 3.900000e-01 1.224000e+01 7.000000e-01 7.000000e-01 +1.027760e+03 4.000000e-01 4.000000e-01 2.760000e+00 1.900000e-01 1.900000e-01 +1.033700e+03 3.900000e-01 3.900000e-01 8.000000e-01 8.000000e-02 8.000000e-02 +1.039680e+03 3.900000e-01 3.900000e-01 3.000000e-01 4.000000e-02 4.000000e-02 +1.049760e+03 3.900000e-01 3.900000e-01 8.900000e-02 1.400000e-02 1.400000e-02 +1.059760e+03 4.400000e-01 4.400000e-01 4.600000e-02 7.000000e-03 7.000000e-03 +1.078540e+03 3.550000e+00 3.550000e+00 1.400000e-02 3.000000e-03 4.000000e-03 +1.099920e+03 5.450000e+00 5.450000e+00 5.000000e-03 2.000000e-03 2.000000e-03 +1.131580e+03 1.049000e+01 1.049000e+01 1.000000e-02 3.000000e-03 4.000000e-03 +1.182960e+03 1.508000e+01 1.508000e+01 1.500000e-02 7.000000e-03 1.200000e-02 +1.227340e+03 1.114000e+01 1.114000e+01 1.300000e-02 1.000000e-02 2.900000e-02 +1.271680e+03 1.433000e+01 1.433000e+01 4.600000e-02 2.500000e-02 4.500000e-02 +1.315440e+03 1.172000e+01 1.172000e+01 1.900000e-02 1.600000e-02 4.500000e-02 +1.360440e+03 1.439000e+01 1.439000e+01 2.100000e-02 1.300000e-02 2.700000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2006_I717778/d02-x01-y01 +IsRef: 1 +Path: /REF/SND_2006_I717778/d02-x01-y01 +Title: doi:10.17182/hepdata.41804.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.552600e+02 5.000000e+00 5.000000e+00 1.900000e-01 1.300000e-01 1.300000e-01 +7.691200e+02 3.980000e+00 3.980000e+00 4.000000e-01 1.700000e-01 1.700000e-01 +7.779600e+02 2.400000e-01 2.400000e-01 1.120000e+00 5.200000e-01 5.200000e-01 +7.799800e+02 2.800000e-01 2.800000e-01 1.280000e+00 5.300000e-01 5.300000e-01 +7.809800e+02 2.400000e-01 2.400000e-01 1.380000e+00 5.100000e-01 5.100000e-01 +7.820000e+02 2.400000e-01 2.400000e-01 1.710000e+00 4.600000e-01 4.600000e-01 +7.830000e+02 2.400000e-01 2.400000e-01 2.230000e+00 5.400000e-01 5.400000e-01 +7.839800e+02 2.400000e-01 2.400000e-01 1.980000e+00 5.500000e-01 5.500000e-01 +7.850200e+02 2.400000e-01 2.400000e-01 1.920000e+00 7.000000e-01 7.000000e-01 +7.859800e+02 2.400000e-01 2.400000e-01 1.400000e+00 5.400000e-01 5.400000e-01 +7.920600e+02 2.020000e+00 2.020000e+00 8.100000e-01 2.600000e-01 2.600000e-01 +8.233600e+02 1.590000e+01 1.590000e+01 3.000000e-01 1.400000e-01 1.400000e-01 +9.315200e+02 2.870000e+01 2.870000e+01 2.500000e-01 1.000000e-01 1.000000e-01 +9.921400e+02 1.040000e+01 1.040000e+01 5.400000e-01 2.300000e-01 2.300000e-01 +1.009680e+03 3.900000e-01 3.900000e-01 3.300000e+00 1.040000e+00 1.040000e+00 +1.015640e+03 3.900000e-01 3.900000e-01 1.507000e+01 1.740000e+00 1.740000e+00 +1.016700e+03 3.800000e-01 3.800000e-01 2.270000e+01 1.950000e+00 1.950000e+00 +1.017660e+03 3.800000e-01 3.800000e-01 3.714000e+01 2.420000e+00 2.420000e+00 +1.018640e+03 3.900000e-01 3.900000e-01 5.183000e+01 2.680000e+00 2.680000e+00 +1.019620e+03 4.200000e-01 4.200000e-01 5.563000e+01 2.460000e+00 2.460000e+00 +1.020580e+03 4.000000e-01 4.000000e-01 4.087000e+01 2.540000e+00 2.540000e+00 +1.021640e+03 4.100000e-01 4.100000e-01 2.497000e+01 2.130000e+00 2.130000e+00 +1.022780e+03 3.900000e-01 3.900000e-01 1.201000e+01 1.370000e+00 1.370000e+00 +1.027760e+03 4.000000e-01 4.000000e-01 2.790000e+00 4.700000e-01 4.700000e-01 +1.036960e+03 3.000000e+00 3.000000e+00 4.100000e-01 1.000000e-01 1.000000e-01 +1.055640e+03 4.940000e+00 4.940000e+00 6.400000e-02 2.700000e-02 2.700000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2006_I720035.cc b/analyses/pluginNovosibirsk/SND_2006_I720035.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2006_I720035.cc @@ -0,0 +1,86 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2006_I720035 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2006_I720035); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + declare(FinalState(), "FS"); + _nK0K0 = bookCounter("TMP/K0K0"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && + nCount[130]==1 && nCount[310]==1) + _nK0K0->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _nK0K0->val(); + double error = _nK0K0->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nK0K0; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2006_I720035); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2006_I720035.info b/analyses/pluginNovosibirsk/SND_2006_I720035.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2006_I720035.info @@ -0,0 +1,37 @@ +Name: SND_2006_I720035 +Year: 2006 +Summary: Measurement of the cross section for $e^+e^-\to K_S^0K_L^0$ at energies between 1.04 and 1.38 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 720035 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- J. Exp. Theor. Phys. 103, 720 (2006) +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to K_S^0K_L^0$ at energies between 1.04 and 1.38 GeV' +Keywords: [] +BibKey: Achasov:2006bv +BibTeX: '@article{Achasov:2006bv, + author = "Achasov, M. N. and others", + title = "{Experimental study of the reaction e+ d- ---> K(S)K(L) + in the energy range s**(1/2) = 1.04-GeV divided by + 1.38-GeV}", + journal = "J. Exp. Theor. Phys.", + volume = "103", + year = "2006", + number = "5", + pages = "720-727", + doi = "10.1134/S1063776106110070", + note = "[Zh. Eksp. Teor. Fiz.130,no.5,831(2006)]", + eprint = "hep-ex/0606057", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = HEP-EX/0606057;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2006_I720035.plot b/analyses/pluginNovosibirsk/SND_2006_I720035.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2006_I720035.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /SND_2006_I720035/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2006_I720035.yoda b/analyses/pluginNovosibirsk/SND_2006_I720035.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2006_I720035.yoda @@ -0,0 +1,30 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2006_I720035/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2006_I720035/d01-x01-y01 +Title: doi:10.17182/hepdata.41792.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.040000e+00 0.000000e+00 0.000000e+00 2.730000e+01 1.969772e+00 1.969772e+00 +1.050000e+00 0.000000e+00 0.000000e+00 1.550000e+01 1.300000e+00 1.300000e+00 +1.060000e+00 0.000000e+00 0.000000e+00 1.030000e+01 5.830952e-01 5.830952e-01 +1.070000e+00 0.000000e+00 0.000000e+00 7.200000e+00 8.246211e-01 8.246211e-01 +1.080000e+00 0.000000e+00 0.000000e+00 6.400000e+00 3.605551e-01 3.605551e-01 +1.090000e+00 0.000000e+00 0.000000e+00 5.200000e+00 8.246211e-01 8.246211e-01 +1.100000e+00 0.000000e+00 0.000000e+00 4.000000e+00 3.162278e-01 3.162278e-01 +1.110000e+00 0.000000e+00 0.000000e+00 2.750000e+00 6.549046e-01 6.549046e-01 +1.125000e+00 5.000000e-03 5.000000e-03 2.810000e+00 3.132092e-01 3.132092e-01 +1.145000e+00 5.000000e-03 5.000000e-03 2.220000e+00 3.080584e-01 3.080584e-01 +1.160000e+00 0.000000e+00 0.000000e+00 1.740000e+00 2.942788e-01 2.942788e-01 +1.185000e+00 5.000000e-03 5.000000e-03 1.040000e+00 1.824829e-01 1.824829e-01 +1.205000e+00 5.000000e-03 5.000000e-03 8.000000e-01 1.627882e-01 1.627882e-01 +1.225000e+00 5.000000e-03 5.000000e-03 7.700000e-01 1.811077e-01 1.811077e-01 +1.245000e+00 5.000000e-03 5.000000e-03 6.200000e-01 1.513275e-01 1.513275e-01 +1.265000e+00 5.000000e-03 5.000000e-03 6.600000e-01 1.811077e-01 2.408319e-01 +1.285000e+00 5.000000e-03 5.000000e-03 6.800000e-01 1.711724e-01 2.209072e-01 +1.305000e+00 5.000000e-03 5.000000e-03 4.300000e-01 1.403567e-01 1.902630e-01 +1.325000e+00 5.000000e-03 5.000000e-03 4.000000e-02 7.071068e-02 1.204159e-01 +1.345000e+00 5.000000e-03 5.000000e-03 3.300000e-01 1.104536e-01 1.503330e-01 +1.360000e+00 0.000000e+00 0.000000e+00 2.900000e-01 1.204159e-01 1.603122e-01 +1.375000e+00 5.000000e-03 5.000000e-03 2.800000e-01 1.104536e-01 1.403567e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2007_I755881.cc b/analyses/pluginNovosibirsk/SND_2007_I755881.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2007_I755881.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2007_I755881 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2007_I755881); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nkaon = bookCounter("TMP/kaon"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::KPLUS) vetoEvent; + } + _nkaon->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nkaon->val(); + double error = _nkaon->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nkaon; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2007_I755881); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2007_I755881.info b/analyses/pluginNovosibirsk/SND_2007_I755881.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2007_I755881.info @@ -0,0 +1,33 @@ +Name: SND_2007_I755881 +Year: 2007 +Summary: Cross section for $e^+e^-\to K^+K^-$ between 1.04 and 1.38 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 755881 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D76 (2007) 072012, 2007 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-$ at energies between 1.04 and 1.38 GeV' +Keywords: +BibKey: Achasov:2007kg +BibTeX: '@article{Achasov:2007kg, + author = "Achasov, M. N. and others", + title = "{Measurement of the e+e- -> K+K- process cross-section in + the energy range s**(1/2) = 1.04 - 1.38 GeV with the SND + detector in the experiment at VEPP-2M e+e- collider}", + journal = "Phys. Rev.", + volume = "D76", + year = "2007", + pages = "072012", + doi = "10.1103/PhysRevD.76.072012", + eprint = "0707.2279", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:0707.2279;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2007_I755881.plot b/analyses/pluginNovosibirsk/SND_2007_I755881.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2007_I755881.plot @@ -0,0 +1,5 @@ +BEGIN PLOT /SND_2007_I755881/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2007_I755881.yoda b/analyses/pluginNovosibirsk/SND_2007_I755881.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2007_I755881.yoda @@ -0,0 +1,84 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2007_I755881/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2007_I755881/d01-x01-y01 +Title: doi:10.17182/hepdata.51605.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.040000e+00 5.000000e-03 5.000000e-03 4.430000e+01 2.507987e+00 2.507987e+00 +1.050000e+00 5.000000e-03 5.000000e-03 2.712000e+01 1.678005e+00 1.678005e+00 +1.060000e+00 5.000000e-03 5.000000e-03 2.090000e+01 8.321658e-01 8.321658e-01 +1.070000e+00 5.000000e-03 5.000000e-03 1.596000e+01 1.153776e+00 1.153776e+00 +1.080000e+00 5.000000e-03 5.000000e-03 1.494000e+01 6.350591e-01 6.350591e-01 +1.090000e+00 5.000000e-03 5.000000e-03 1.297000e+01 8.556284e-01 8.556284e-01 +1.100000e+00 5.000000e-03 5.000000e-03 1.228000e+01 4.580393e-01 4.580393e-01 +1.110000e+00 5.000000e-03 5.000000e-03 9.910000e+00 6.935416e-01 6.935416e-01 +1.120000e+00 5.000000e-03 5.000000e-03 1.049000e+01 5.521775e-01 5.521775e-01 +1.130000e+00 5.000000e-03 5.000000e-03 9.870000e+00 6.435060e-01 6.435060e-01 +1.140000e+00 5.000000e-03 5.000000e-03 1.016000e+01 5.920304e-01 5.920304e-01 +1.150000e+00 5.000000e-03 5.000000e-03 9.620000e+00 7.451845e-01 7.451845e-01 +1.160000e+00 5.000000e-03 5.000000e-03 1.025000e+01 5.560576e-01 5.560576e-01 +1.180000e+00 5.000000e-03 5.000000e-03 9.880000e+00 4.661545e-01 4.661545e-01 +1.190000e+00 5.000000e-03 5.000000e-03 8.050000e+00 5.640035e-01 5.640035e-01 +1.200000e+00 5.000000e-03 5.000000e-03 9.090000e+00 3.182766e-01 3.182766e-01 +1.210000e+00 5.000000e-03 5.000000e-03 9.500000e+00 5.966574e-01 5.966574e-01 +1.220000e+00 5.000000e-03 5.000000e-03 8.070000e+00 3.940812e-01 3.940812e-01 +1.230000e+00 5.000000e-03 5.000000e-03 9.430000e+00 6.389053e-01 6.389053e-01 +1.240000e+00 5.000000e-03 5.000000e-03 8.060000e+00 3.720215e-01 3.720215e-01 +1.250000e+00 5.000000e-03 5.000000e-03 8.640000e+00 5.341348e-01 5.341348e-01 +1.260000e+00 5.000000e-03 5.000000e-03 8.030000e+00 5.263079e-01 5.263079e-01 +1.270000e+00 5.000000e-03 5.000000e-03 8.140000e+00 4.622770e-01 4.622770e-01 +1.280000e+00 5.000000e-03 5.000000e-03 7.220000e+00 4.743416e-01 4.743416e-01 +1.290000e+00 5.000000e-03 5.000000e-03 6.850000e+00 4.716991e-01 4.716991e-01 +1.300000e+00 5.000000e-03 5.000000e-03 7.120000e+00 4.140048e-01 4.140048e-01 +1.310000e+00 5.000000e-03 5.000000e-03 7.300000e+00 5.000000e-01 5.000000e-01 +1.320000e+00 5.000000e-03 5.000000e-03 7.260000e+00 4.701064e-01 4.701064e-01 +1.330000e+00 5.000000e-03 5.000000e-03 6.790000e+00 4.548626e-01 4.548626e-01 +1.340000e+00 5.000000e-03 5.000000e-03 6.130000e+00 3.328663e-01 3.328663e-01 +1.350000e+00 5.000000e-03 5.000000e-03 6.820000e+00 4.687217e-01 4.687217e-01 +1.360000e+00 5.000000e-03 5.000000e-03 6.150000e+00 3.138471e-01 3.138471e-01 +1.370000e+00 5.000000e-03 5.000000e-03 5.970000e+00 4.579301e-01 4.579301e-01 +1.380000e+00 5.000000e-03 5.000000e-03 6.050000e+00 3.584690e-01 3.584690e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2007_I755881/d01-x01-y02 +IsRef: 1 +Path: /REF/SND_2007_I755881/d01-x01-y02 +Title: doi:10.17182/hepdata.51605.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.040000e+00 5.000000e-03 5.000000e-03 7.122000e+01 4.080000e+00 4.080000e+00 +1.050000e+00 5.000000e-03 5.000000e-03 3.496000e+01 2.160000e+00 2.160000e+00 +1.060000e+00 5.000000e-03 5.000000e-03 2.246000e+01 9.100000e-01 9.100000e-01 +1.070000e+00 5.000000e-03 5.000000e-03 1.470000e+01 1.070000e+00 1.070000e+00 +1.080000e+00 5.000000e-03 5.000000e-03 1.206000e+01 5.300000e-01 5.300000e-01 +1.090000e+00 5.000000e-03 5.000000e-03 9.340000e+00 6.200000e-01 6.200000e-01 +1.100000e+00 5.000000e-03 5.000000e-03 7.990000e+00 3.000000e-01 3.000000e-01 +1.110000e+00 5.000000e-03 5.000000e-03 5.890000e+00 4.100000e-01 4.100000e-01 +1.120000e+00 5.000000e-03 5.000000e-03 5.760000e+00 3.000000e-01 3.000000e-01 +1.130000e+00 5.000000e-03 5.000000e-03 5.050000e+00 3.300000e-01 3.300000e-01 +1.140000e+00 5.000000e-03 5.000000e-03 4.870000e+00 2.800000e-01 2.800000e-01 +1.150000e+00 5.000000e-03 5.000000e-03 4.350000e+00 3.400000e-01 3.400000e-01 +1.160000e+00 5.000000e-03 5.000000e-03 4.390000e+00 2.400000e-01 2.400000e-01 +1.180000e+00 5.000000e-03 5.000000e-03 3.860000e+00 1.800000e-01 1.800000e-01 +1.190000e+00 5.000000e-03 5.000000e-03 3.020000e+00 2.100000e-01 2.100000e-01 +1.200000e+00 5.000000e-03 5.000000e-03 3.280000e+00 1.200000e-01 1.200000e-01 +1.210000e+00 5.000000e-03 5.000000e-03 3.320000e+00 2.100000e-01 2.100000e-01 +1.220000e+00 5.000000e-03 5.000000e-03 2.730000e+00 1.400000e-01 1.400000e-01 +1.230000e+00 5.000000e-03 5.000000e-03 3.100000e+00 2.100000e-01 2.100000e-01 +1.240000e+00 5.000000e-03 5.000000e-03 2.580000e+00 1.200000e-01 1.200000e-01 +1.250000e+00 5.000000e-03 5.000000e-03 2.690000e+00 1.700000e-01 1.700000e-01 +1.260000e+00 5.000000e-03 5.000000e-03 2.450000e+00 1.600000e-01 1.600000e-01 +1.270000e+00 5.000000e-03 5.000000e-03 2.430000e+00 1.400000e-01 1.400000e-01 +1.280000e+00 5.000000e-03 5.000000e-03 2.110000e+00 1.400000e-01 1.400000e-01 +1.290000e+00 5.000000e-03 5.000000e-03 1.970000e+00 1.400000e-01 1.400000e-01 +1.300000e+00 5.000000e-03 5.000000e-03 2.010000e+00 1.200000e-01 1.200000e-01 +1.310000e+00 5.000000e-03 5.000000e-03 2.030000e+00 1.400000e-01 1.400000e-01 +1.320000e+00 5.000000e-03 5.000000e-03 1.990000e+00 1.300000e-01 1.300000e-01 +1.330000e+00 5.000000e-03 5.000000e-03 1.840000e+00 1.200000e-01 1.200000e-01 +1.340000e+00 5.000000e-03 5.000000e-03 1.640000e+00 9.000000e-02 9.000000e-02 +1.350000e+00 5.000000e-03 5.000000e-03 1.800000e+00 1.200000e-01 1.200000e-01 +1.360000e+00 5.000000e-03 5.000000e-03 1.610000e+00 8.000000e-02 8.000000e-02 +1.370000e+00 5.000000e-03 5.000000e-03 1.550000e+00 1.200000e-01 1.200000e-01 +1.380000e+00 5.000000e-03 5.000000e-03 1.560000e+00 9.000000e-02 9.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2014_I1275333.cc b/analyses/pluginNovosibirsk/SND_2014_I1275333.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2014_I1275333.cc @@ -0,0 +1,121 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2014_I1275333 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2014_I1275333); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaGamma = bookCounter("TMP/EtaGamma"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=1) continue; + bool matched = true; + for(auto const & val : nRes) { + if(val.first==22) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaGamma->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _numEtaGamma->val(); + double error = _numEtaGamma->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numEtaGamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2014_I1275333); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2014_I1275333.info b/analyses/pluginNovosibirsk/SND_2014_I1275333.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2014_I1275333.info @@ -0,0 +1,33 @@ +Name: SND_2014_I1275333 +Year: 2014 +Summary: Cross section for $e^+e^-\to\eta\gamma$ for energies between 1.07 and 2 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 1275333 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D90 (2014) 032002 +RunInfo: e+ e- to hadrons below 0.6 and 1.38 GeV +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\eta\gamma$ for energies between 1.07 and 2 GeV.' +Keywords: [] +BibKey: Achasov:2013eli +BibTeX: '@article{Achasov:2013eli, + author = "Achasov, M. N. and others", + title = "{Study of the process $e^+e^-\to\eta\gamma$ in the + center-of-mass energy range 1.07--2.00 GeV}", + journal = "Phys. Rev.", + volume = "D90", + year = "2014", + number = "3", + pages = "032002", + doi = "10.1103/PhysRevD.90.032002", + eprint = "1312.7078", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1312.7078;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2014_I1275333.plot b/analyses/pluginNovosibirsk/SND_2014_I1275333.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2014_I1275333.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /SND_2014_I1275333/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\gamma)$/pb +LogY=1 +LegendXPos=0.1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2014_I1275333.yoda b/analyses/pluginNovosibirsk/SND_2014_I1275333.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2014_I1275333.yoda @@ -0,0 +1,26 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2014_I1275333/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2014_I1275333/d01-x01-y01 +Title: doi:10.17182/hepdata.62279.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.100000e+03 2.500000e+01 2.500000e+01 4.000000e+00 2.039608e+01 4.561798e+01 +1.175000e+03 2.500000e+01 2.500000e+01 2.100000e+01 1.315295e+01 2.209072e+01 +1.262500e+03 3.750000e+01 3.750000e+01 1.800000e+01 8.246211e+00 1.414214e+01 +1.362500e+03 3.750000e+01 3.750000e+01 2.400000e+01 1.019804e+01 1.513275e+01 +1.462500e+03 3.750000e+01 3.750000e+01 3.700000e+01 1.216553e+01 1.811077e+01 +1.560000e+03 4.000000e+01 4.000000e+01 4.400000e+01 1.414214e+01 1.910497e+01 +1.662500e+03 3.750000e+01 3.750000e+01 1.800000e+01 1.019804e+01 1.910497e+01 +1.760000e+03 4.000000e+01 4.000000e+01 3.000000e+00 3.162278e+00 1.104536e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2014_I1275333/d02-x01-y01 +IsRef: 1 +Path: /REF/SND_2014_I1275333/d02-x01-y01 +Title: doi:10.17182/hepdata.62279.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000000e+00 5.000000e-01 5.000000e-01 5.700000e+01 1.220656e+01 1.220656e+01 +2.000000e+00 5.000000e-01 5.000000e-01 5.200000e+01 2.267157e+01 2.267157e+01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2014_I1321689.cc b/analyses/pluginNovosibirsk/SND_2014_I1321689.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2014_I1321689.cc @@ -0,0 +1,86 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2014_I1321689 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2014_I1321689); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nneutron = bookCounter("TMP/neutron"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::NEUTRON) vetoEvent; + } + _nneutron->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _nneutron->val(); + double error = _nneutron->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nneutron; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2014_I1321689); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2014_I1321689.info b/analyses/pluginNovosibirsk/SND_2014_I1321689.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2014_I1321689.info @@ -0,0 +1,35 @@ +Name: SND_2014_I1321689 +Year: 2014 +Summary: Cross section for $e^+e^-\to n\bar{n}$ between threshold and 2 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 1321689 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D90 (2014) 112007, 2014 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to n\bar{n}$ at energies between threshold and 2 GeV.' +Keywords: +BibKey: Achasov:2014ncd +BibTeX: '@article{Achasov:2014ncd, + author = "Achasov, M. N. and others", + title = "{Study of the process $e^+e^-\to n\bar{n}$ at the + VEPP-2000 $e^+e^-$ collider with the SND detector}", + journal = "Phys. Rev.", + volume = "D90", + year = "2014", + number = "11", + pages = "112007", + doi = "10.1103/PhysRevD.90.112007", + eprint = "1410.3188", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1410.3188;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2014_I1321689.plot b/analyses/pluginNovosibirsk/SND_2014_I1321689.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2014_I1321689.plot @@ -0,0 +1,14 @@ +BEGIN PLOT /SND_2014_I1321689/d01-x01-y01 +Title=$\sigma(e^+e^-\to n\bar{n})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to n\bar{n})$/nb +ConnectGaps=1 +LogY=0 +END PLOT +BEGIN PLOT /SND_2014_I1321689/d02-x01-y01 +Title=$\sigma(e^+e^-\to n\bar{n})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to n\bar{n})$/nb +ConnectGaps=1 +LogY=0 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2014_I1321689.yoda b/analyses/pluginNovosibirsk/SND_2014_I1321689.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2014_I1321689.yoda @@ -0,0 +1,54 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2014_I1321689/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2014_I1321689/d01-x01-y01 +Title: doi:10.17182/hepdata.71416.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.890000e+03 0.000000e+00 0.000000e+00 8.300000e-01 2.700000e-01 2.700000e-01 +1.900000e+03 0.000000e+00 0.000000e+00 1.560000e+00 2.900000e-01 2.900000e-01 +1.925000e+03 0.000000e+00 0.000000e+00 7.800000e-01 1.800000e-01 1.800000e-01 +1.950000e+03 0.000000e+00 0.000000e+00 1.300000e+00 2.600000e-01 2.600000e-01 +1.975000e+03 0.000000e+00 0.000000e+00 8.700000e-01 2.200000e-01 2.200000e-01 +2.000000e+03 0.000000e+00 0.000000e+00 8.700000e-01 2.200000e-01 2.200000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2014_I1321689/d01-x01-y02 +IsRef: 1 +Path: /REF/SND_2014_I1321689/d01-x01-y02 +Title: doi:10.17182/hepdata.71416.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.890000e+03 0.000000e+00 0.000000e+00 4.500000e-01 9.000000e-02 9.000000e-02 +1.900000e+03 0.000000e+00 0.000000e+00 5.300000e-01 6.000000e-02 6.000000e-02 +1.925000e+03 0.000000e+00 0.000000e+00 3.200000e-01 4.000000e-02 4.000000e-02 +1.950000e+03 0.000000e+00 0.000000e+00 3.800000e-01 4.000000e-02 4.000000e-02 +1.975000e+03 0.000000e+00 0.000000e+00 2.900000e-01 4.000000e-02 4.000000e-02 +2.000000e+03 0.000000e+00 0.000000e+00 2.800000e-01 4.000000e-02 4.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2014_I1321689/d02-x01-y01 +IsRef: 1 +Path: /REF/SND_2014_I1321689/d02-x01-y01 +Title: doi:10.17182/hepdata.71416.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.900000e+03 0.000000e+00 0.000000e+00 7.300000e-01 1.600000e-01 1.600000e-01 +1.920000e+03 0.000000e+00 0.000000e+00 4.900000e-01 1.500000e-01 1.500000e-01 +1.940000e+03 0.000000e+00 0.000000e+00 6.400000e-01 1.300000e-01 1.300000e-01 +1.960000e+03 0.000000e+00 0.000000e+00 7.200000e-01 1.800000e-01 1.800000e-01 +1.980000e+03 0.000000e+00 0.000000e+00 8.200000e-01 1.800000e-01 1.800000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2014_I1321689/d02-x01-y02 +IsRef: 1 +Path: /REF/SND_2014_I1321689/d02-x01-y02 +Title: doi:10.17182/hepdata.71416.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.900000e+03 0.000000e+00 0.000000e+00 3.700000e-01 6.000000e-02 6.000000e-02 +1.920000e+03 0.000000e+00 0.000000e+00 2.700000e-01 6.000000e-02 6.000000e-02 +1.940000e+03 0.000000e+00 0.000000e+00 2.800000e-01 4.000000e-02 4.000000e-02 +1.960000e+03 0.000000e+00 0.000000e+00 2.800000e-01 5.000000e-02 5.000000e-02 +1.980000e+03 0.000000e+00 0.000000e+00 2.900000e-01 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2015_I1332929.cc b/analyses/pluginNovosibirsk/SND_2015_I1332929.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2015_I1332929.cc @@ -0,0 +1,120 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2015_I1332929 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2015_I1332929); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaPiPi = bookCounter("TMP/EtaPiPi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaPiPi->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _numEtaPiPi->val(); + double error = _numEtaPiPi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numEtaPiPi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2015_I1332929); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2015_I1332929.info b/analyses/pluginNovosibirsk/SND_2015_I1332929.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2015_I1332929.info @@ -0,0 +1,37 @@ +Name: SND_2015_I1332929 +Year: 2015 +Summary: Cross section for $e^+e^-\to\eta\pi^+\pi^-$ between 1.22 and 2 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 1332929 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Rev. D91 (2015) 052013, 2015 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to\eta\pi^+\pi^-$ at energies between 1.22 and 2 GeV.' +Keywords: +BibKey: Aulchenko:2014vkn +BibTeX: '@article{Aulchenko:2014vkn, + author = "Aulchenko, V. M. and others", + title = "{Measurement of the $e^+e^- \to \eta\pi^+\pi^-$ cross + section in the center-of-mass energy range 1.22-2.00 GeV + with the SND detector at the VEPP-2000 collider}", + collaboration = "SND", + journal = "Phys. Rev.", + volume = "D91", + year = "2015", + number = "5", + pages = "052013", + doi = "10.1103/PhysRevD.91.052013", + eprint = "1412.1971", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1412.1971;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2015_I1332929.plot b/analyses/pluginNovosibirsk/SND_2015_I1332929.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2015_I1332929.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /SND_2015_I1332929/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$/nb +LogY=0 +LegendXPos=0.7 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2015_I1332929.yoda b/analyses/pluginNovosibirsk/SND_2015_I1332929.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2015_I1332929.yoda @@ -0,0 +1,205 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2015_I1332929/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2015_I1332929/d01-x01-y01 +Title: doi:10.17182/hepdata.73176.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.225000e+00 0.000000e+00 0.000000e+00 3.500000e-01 1.500000e-01 1.500000e-01 +1.250000e+00 0.000000e+00 0.000000e+00 1.700000e-01 1.500000e-01 1.500000e-01 +1.278000e+00 0.000000e+00 0.000000e+00 4.900000e-01 1.300000e-01 1.300000e-01 +1.300000e+00 0.000000e+00 0.000000e+00 5.000000e-01 1.900000e-01 1.900000e-01 +1.325000e+00 0.000000e+00 0.000000e+00 7.400000e-01 1.900000e-01 1.900000e-01 +1.356000e+00 0.000000e+00 0.000000e+00 1.070000e+00 1.500000e-01 1.500000e-01 +1.375000e+00 0.000000e+00 0.000000e+00 1.250000e+00 2.200000e-01 2.200000e-01 +1.400000e+00 0.000000e+00 0.000000e+00 1.690000e+00 2.400000e-01 2.400000e-01 +1.425000e+00 0.000000e+00 0.000000e+00 2.230000e+00 2.500000e-01 2.500000e-01 +1.443000e+00 0.000000e+00 0.000000e+00 2.760000e+00 1.900000e-01 1.900000e-01 +1.475000e+00 0.000000e+00 0.000000e+00 3.310000e+00 2.900000e-01 2.900000e-01 +1.500000e+00 0.000000e+00 0.000000e+00 3.630000e+00 2.900000e-01 2.900000e-01 +1.522000e+00 0.000000e+00 0.000000e+00 4.470000e+00 2.300000e-01 2.300000e-01 +1.550000e+00 0.000000e+00 0.000000e+00 4.280000e+00 3.300000e-01 3.300000e-01 +1.575000e+00 0.000000e+00 0.000000e+00 3.610000e+00 3.600000e-01 3.600000e-01 +1.600000e+00 0.000000e+00 0.000000e+00 3.300000e+00 3.400000e-01 3.400000e-01 +1.625000e+00 0.000000e+00 0.000000e+00 3.760000e+00 3.400000e-01 3.400000e-01 +1.650000e+00 0.000000e+00 0.000000e+00 2.530000e+00 3.200000e-01 3.200000e-01 +1.678000e+00 0.000000e+00 0.000000e+00 2.410000e+00 1.900000e-01 1.900000e-01 +1.700000e+00 0.000000e+00 0.000000e+00 2.790000e+00 3.100000e-01 3.100000e-01 +1.723000e+00 0.000000e+00 0.000000e+00 2.050000e+00 2.000000e-01 2.000000e-01 +1.756000e+00 0.000000e+00 0.000000e+00 2.260000e+00 1.900000e-01 1.900000e-01 +1.775000e+00 0.000000e+00 0.000000e+00 1.970000e+00 2.800000e-01 2.800000e-01 +1.800000e+00 0.000000e+00 0.000000e+00 2.090000e+00 1.700000e-01 1.700000e-01 +1.825000e+00 0.000000e+00 0.000000e+00 1.470000e+00 2.400000e-01 2.400000e-01 +1.843000e+00 0.000000e+00 0.000000e+00 1.360000e+00 1.500000e-01 1.500000e-01 +1.871000e+00 0.000000e+00 0.000000e+00 9.400000e-01 1.300000e-01 1.300000e-01 +1.897000e+00 0.000000e+00 0.000000e+00 8.900000e-01 1.100000e-01 1.100000e-01 +1.922000e+00 0.000000e+00 0.000000e+00 8.100000e-01 1.300000e-01 1.300000e-01 +1.943000e+00 0.000000e+00 0.000000e+00 7.500000e-01 1.200000e-01 1.200000e-01 +1.960000e+00 0.000000e+00 0.000000e+00 7.600000e-01 1.700000e-01 1.700000e-01 +1.978000e+00 0.000000e+00 0.000000e+00 8.100000e-01 1.500000e-01 1.500000e-01 +2.000000e+00 0.000000e+00 0.000000e+00 8.400000e-01 2.100000e-01 2.100000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2015_I1332929/d01-x01-y02 +IsRef: 1 +Path: /REF/SND_2015_I1332929/d01-x01-y02 +Title: doi:10.17182/hepdata.73176.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.225000e+00 0.000000e+00 0.000000e+00 2.000000e+01 9.000000e+00 9.000000e+00 +1.250000e+00 0.000000e+00 0.000000e+00 8.000000e+00 7.000000e+00 7.000000e+00 +1.278000e+00 0.000000e+00 0.000000e+00 5.600000e+01 1.600000e+01 1.600000e+01 +1.300000e+00 0.000000e+00 0.000000e+00 2.300000e+01 1.000000e+01 1.000000e+01 +1.325000e+00 0.000000e+00 0.000000e+00 3.800000e+01 1.000000e+01 1.000000e+01 +1.356000e+00 0.000000e+00 0.000000e+00 1.370000e+02 2.100000e+01 2.100000e+01 +1.375000e+00 0.000000e+00 0.000000e+00 7.000000e+01 1.300000e+01 1.300000e+01 +1.400000e+00 0.000000e+00 0.000000e+00 1.000000e+02 1.500000e+01 1.500000e+01 +1.425000e+00 0.000000e+00 0.000000e+00 1.250000e+02 1.500000e+01 1.500000e+01 +1.443000e+00 0.000000e+00 0.000000e+00 3.550000e+02 2.600000e+01 2.600000e+01 +1.475000e+00 0.000000e+00 0.000000e+00 1.910000e+02 1.800000e+01 1.800000e+01 +1.500000e+00 0.000000e+00 0.000000e+00 2.440000e+02 2.000000e+01 2.000000e+01 +1.522000e+00 0.000000e+00 0.000000e+00 5.680000e+02 3.000000e+01 3.000000e+01 +1.550000e+00 0.000000e+00 0.000000e+00 2.250000e+02 1.800000e+01 1.800000e+01 +1.575000e+00 0.000000e+00 0.000000e+00 1.540000e+02 1.600000e+01 1.600000e+01 +1.600000e+00 0.000000e+00 0.000000e+00 1.390000e+02 1.500000e+01 1.500000e+01 +1.625000e+00 0.000000e+00 0.000000e+00 1.890000e+02 1.700000e+01 1.700000e+01 +1.650000e+00 0.000000e+00 0.000000e+00 1.160000e+02 1.500000e+01 1.500000e+01 +1.678000e+00 0.000000e+00 0.000000e+00 2.900000e+02 2.300000e+01 2.300000e+01 +1.700000e+00 0.000000e+00 0.000000e+00 1.260000e+02 1.400000e+01 1.400000e+01 +1.723000e+00 0.000000e+00 0.000000e+00 1.930000e+02 1.900000e+01 1.900000e+01 +1.756000e+00 0.000000e+00 0.000000e+00 2.490000e+02 2.000000e+01 2.000000e+01 +1.775000e+00 0.000000e+00 0.000000e+00 9.100000e+01 1.300000e+01 1.300000e+01 +1.800000e+00 0.000000e+00 0.000000e+00 2.740000e+02 2.200000e+01 2.200000e+01 +1.825000e+00 0.000000e+00 0.000000e+00 7.400000e+01 1.200000e+01 1.200000e+01 +1.843000e+00 0.000000e+00 0.000000e+00 1.730000e+02 1.800000e+01 1.800000e+01 +1.871000e+00 0.000000e+00 0.000000e+00 1.370000e+02 1.800000e+01 1.800000e+01 +1.897000e+00 0.000000e+00 0.000000e+00 1.710000e+02 2.000000e+01 2.000000e+01 +1.922000e+00 0.000000e+00 0.000000e+00 1.000000e+02 1.500000e+01 1.500000e+01 +1.943000e+00 0.000000e+00 0.000000e+00 1.020000e+02 1.500000e+01 1.500000e+01 +1.960000e+00 0.000000e+00 0.000000e+00 5.200000e+01 1.100000e+01 1.100000e+01 +1.978000e+00 0.000000e+00 0.000000e+00 8.600000e+01 1.400000e+01 1.400000e+01 +2.000000e+00 0.000000e+00 0.000000e+00 4.700000e+01 1.000000e+01 1.000000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2015_I1332929/d01-x01-y03 +IsRef: 1 +Path: /REF/SND_2015_I1332929/d01-x01-y03 +Title: doi:10.17182/hepdata.73176.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.225000e+00 0.000000e+00 0.000000e+00 1.050000e-01 0.000000e+00 0.000000e+00 +1.250000e+00 0.000000e+00 0.000000e+00 1.020000e-01 0.000000e+00 0.000000e+00 +1.278000e+00 0.000000e+00 0.000000e+00 9.700000e-02 0.000000e+00 0.000000e+00 +1.300000e+00 0.000000e+00 0.000000e+00 9.900000e-02 0.000000e+00 0.000000e+00 +1.325000e+00 0.000000e+00 0.000000e+00 9.900000e-02 0.000000e+00 0.000000e+00 +1.356000e+00 0.000000e+00 0.000000e+00 9.600000e-02 0.000000e+00 0.000000e+00 +1.375000e+00 0.000000e+00 0.000000e+00 9.700000e-02 0.000000e+00 0.000000e+00 +1.400000e+00 0.000000e+00 0.000000e+00 9.500000e-02 0.000000e+00 0.000000e+00 +1.425000e+00 0.000000e+00 0.000000e+00 9.700000e-02 0.000000e+00 0.000000e+00 +1.443000e+00 0.000000e+00 0.000000e+00 9.100000e-02 0.000000e+00 0.000000e+00 +1.475000e+00 0.000000e+00 0.000000e+00 9.600000e-02 0.000000e+00 0.000000e+00 +1.500000e+00 0.000000e+00 0.000000e+00 9.200000e-02 0.000000e+00 0.000000e+00 +1.522000e+00 0.000000e+00 0.000000e+00 9.000000e-02 0.000000e+00 0.000000e+00 +1.550000e+00 0.000000e+00 0.000000e+00 9.000000e-02 0.000000e+00 0.000000e+00 +1.575000e+00 0.000000e+00 0.000000e+00 9.300000e-02 0.000000e+00 0.000000e+00 +1.600000e+00 0.000000e+00 0.000000e+00 8.900000e-02 0.000000e+00 0.000000e+00 +1.625000e+00 0.000000e+00 0.000000e+00 8.700000e-02 0.000000e+00 0.000000e+00 +1.650000e+00 0.000000e+00 0.000000e+00 8.500000e-02 0.000000e+00 0.000000e+00 +1.678000e+00 0.000000e+00 0.000000e+00 8.200000e-02 0.000000e+00 0.000000e+00 +1.700000e+00 0.000000e+00 0.000000e+00 8.500000e-02 0.000000e+00 0.000000e+00 +1.723000e+00 0.000000e+00 0.000000e+00 8.200000e-02 0.000000e+00 0.000000e+00 +1.756000e+00 0.000000e+00 0.000000e+00 8.100000e-02 0.000000e+00 0.000000e+00 +1.775000e+00 0.000000e+00 0.000000e+00 8.500000e-02 0.000000e+00 0.000000e+00 +1.800000e+00 0.000000e+00 0.000000e+00 8.000000e-02 0.000000e+00 0.000000e+00 +1.825000e+00 0.000000e+00 0.000000e+00 8.100000e-02 0.000000e+00 0.000000e+00 +1.843000e+00 0.000000e+00 0.000000e+00 7.500000e-02 0.000000e+00 0.000000e+00 +1.871000e+00 0.000000e+00 0.000000e+00 7.400000e-02 0.000000e+00 0.000000e+00 +1.897000e+00 0.000000e+00 0.000000e+00 7.300000e-02 0.000000e+00 0.000000e+00 +1.922000e+00 0.000000e+00 0.000000e+00 7.300000e-02 0.000000e+00 0.000000e+00 +1.943000e+00 0.000000e+00 0.000000e+00 7.600000e-02 0.000000e+00 0.000000e+00 +1.960000e+00 0.000000e+00 0.000000e+00 6.900000e-02 0.000000e+00 0.000000e+00 +1.978000e+00 0.000000e+00 0.000000e+00 6.800000e-02 0.000000e+00 0.000000e+00 +2.000000e+00 0.000000e+00 0.000000e+00 6.800000e-02 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2015_I1332929/d01-x01-y04 +IsRef: 1 +Path: /REF/SND_2015_I1332929/d01-x01-y04 +Title: doi:10.17182/hepdata.73176.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.225000e+00 0.000000e+00 0.000000e+00 5.530000e+02 0.000000e+00 0.000000e+00 +1.250000e+00 0.000000e+00 0.000000e+00 4.660000e+02 0.000000e+00 0.000000e+00 +1.278000e+00 0.000000e+00 0.000000e+00 1.225000e+03 0.000000e+00 0.000000e+00 +1.300000e+00 0.000000e+00 0.000000e+00 4.840000e+02 0.000000e+00 0.000000e+00 +1.325000e+00 0.000000e+00 0.000000e+00 5.420000e+02 0.000000e+00 0.000000e+00 +1.356000e+00 0.000000e+00 0.000000e+00 1.398000e+03 0.000000e+00 0.000000e+00 +1.375000e+00 0.000000e+00 0.000000e+00 5.990000e+02 0.000000e+00 0.000000e+00 +1.400000e+00 0.000000e+00 0.000000e+00 6.430000e+02 0.000000e+00 0.000000e+00 +1.425000e+00 0.000000e+00 0.000000e+00 5.910000e+02 0.000000e+00 0.000000e+00 +1.443000e+00 0.000000e+00 0.000000e+00 1.442000e+03 0.000000e+00 0.000000e+00 +1.475000e+00 0.000000e+00 0.000000e+00 6.080000e+02 0.000000e+00 0.000000e+00 +1.500000e+00 0.000000e+00 0.000000e+00 7.310000e+02 0.000000e+00 0.000000e+00 +1.522000e+00 0.000000e+00 0.000000e+00 1.395000e+03 0.000000e+00 0.000000e+00 +1.550000e+00 0.000000e+00 0.000000e+00 5.660000e+02 0.000000e+00 0.000000e+00 +1.575000e+00 0.000000e+00 0.000000e+00 4.360000e+02 0.000000e+00 0.000000e+00 +1.600000e+00 0.000000e+00 0.000000e+00 4.460000e+02 0.000000e+00 0.000000e+00 +1.625000e+00 0.000000e+00 0.000000e+00 5.300000e+02 0.000000e+00 0.000000e+00 +1.650000e+00 0.000000e+00 0.000000e+00 4.900000e+02 0.000000e+00 0.000000e+00 +1.678000e+00 0.000000e+00 0.000000e+00 1.314000e+03 0.000000e+00 0.000000e+00 +1.700000e+00 0.000000e+00 0.000000e+00 4.720000e+02 0.000000e+00 0.000000e+00 +1.723000e+00 0.000000e+00 0.000000e+00 1.022000e+03 0.000000e+00 0.000000e+00 +1.756000e+00 0.000000e+00 0.000000e+00 1.198000e+03 0.000000e+00 0.000000e+00 +1.775000e+00 0.000000e+00 0.000000e+00 4.730000e+02 0.000000e+00 0.000000e+00 +1.800000e+00 0.000000e+00 0.000000e+00 1.391000e+03 0.000000e+00 0.000000e+00 +1.825000e+00 0.000000e+00 0.000000e+00 5.130000e+02 0.000000e+00 0.000000e+00 +1.843000e+00 0.000000e+00 0.000000e+00 1.369000e+03 0.000000e+00 0.000000e+00 +1.871000e+00 0.000000e+00 0.000000e+00 1.555000e+03 0.000000e+00 0.000000e+00 +1.897000e+00 0.000000e+00 0.000000e+00 2.033000e+03 0.000000e+00 0.000000e+00 +1.922000e+00 0.000000e+00 0.000000e+00 1.256000e+03 0.000000e+00 0.000000e+00 +1.943000e+00 0.000000e+00 0.000000e+00 1.312000e+03 0.000000e+00 0.000000e+00 +1.960000e+00 0.000000e+00 0.000000e+00 7.240000e+02 0.000000e+00 0.000000e+00 +1.978000e+00 0.000000e+00 0.000000e+00 1.125000e+03 0.000000e+00 0.000000e+00 +2.000000e+00 0.000000e+00 0.000000e+00 5.760000e+02 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2015_I1332929/d01-x01-y05 +IsRef: 1 +Path: /REF/SND_2015_I1332929/d01-x01-y05 +Title: doi:10.17182/hepdata.73176.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.225000e+00 0.000000e+00 0.000000e+00 8.700000e-01 0.000000e+00 0.000000e+00 +1.250000e+00 0.000000e+00 0.000000e+00 8.700000e-01 0.000000e+00 0.000000e+00 +1.278000e+00 0.000000e+00 0.000000e+00 8.700000e-01 0.000000e+00 0.000000e+00 +1.300000e+00 0.000000e+00 0.000000e+00 8.700000e-01 0.000000e+00 0.000000e+00 +1.325000e+00 0.000000e+00 0.000000e+00 8.600000e-01 0.000000e+00 0.000000e+00 +1.356000e+00 0.000000e+00 0.000000e+00 8.600000e-01 0.000000e+00 0.000000e+00 +1.375000e+00 0.000000e+00 0.000000e+00 8.600000e-01 0.000000e+00 0.000000e+00 +1.400000e+00 0.000000e+00 0.000000e+00 8.700000e-01 0.000000e+00 0.000000e+00 +1.425000e+00 0.000000e+00 0.000000e+00 8.700000e-01 0.000000e+00 0.000000e+00 +1.443000e+00 0.000000e+00 0.000000e+00 8.800000e-01 0.000000e+00 0.000000e+00 +1.475000e+00 0.000000e+00 0.000000e+00 8.900000e-01 0.000000e+00 0.000000e+00 +1.500000e+00 0.000000e+00 0.000000e+00 9.000000e-01 0.000000e+00 0.000000e+00 +1.522000e+00 0.000000e+00 0.000000e+00 9.100000e-01 0.000000e+00 0.000000e+00 +1.550000e+00 0.000000e+00 0.000000e+00 9.300000e-01 0.000000e+00 0.000000e+00 +1.575000e+00 0.000000e+00 0.000000e+00 9.400000e-01 0.000000e+00 0.000000e+00 +1.600000e+00 0.000000e+00 0.000000e+00 9.600000e-01 0.000000e+00 0.000000e+00 +1.625000e+00 0.000000e+00 0.000000e+00 9.800000e-01 0.000000e+00 0.000000e+00 +1.650000e+00 0.000000e+00 0.000000e+00 9.900000e-01 0.000000e+00 0.000000e+00 +1.678000e+00 0.000000e+00 0.000000e+00 1.010000e+00 0.000000e+00 0.000000e+00 +1.700000e+00 0.000000e+00 0.000000e+00 1.010000e+00 0.000000e+00 0.000000e+00 +1.723000e+00 0.000000e+00 0.000000e+00 1.010000e+00 0.000000e+00 0.000000e+00 +1.756000e+00 0.000000e+00 0.000000e+00 1.020000e+00 0.000000e+00 0.000000e+00 +1.775000e+00 0.000000e+00 0.000000e+00 1.030000e+00 0.000000e+00 0.000000e+00 +1.800000e+00 0.000000e+00 0.000000e+00 1.060000e+00 0.000000e+00 0.000000e+00 +1.825000e+00 0.000000e+00 0.000000e+00 1.090000e+00 0.000000e+00 0.000000e+00 +1.843000e+00 0.000000e+00 0.000000e+00 1.110000e+00 0.000000e+00 0.000000e+00 +1.871000e+00 0.000000e+00 0.000000e+00 1.140000e+00 0.000000e+00 0.000000e+00 +1.897000e+00 0.000000e+00 0.000000e+00 1.170000e+00 0.000000e+00 0.000000e+00 +1.922000e+00 0.000000e+00 0.000000e+00 1.200000e+00 0.000000e+00 0.000000e+00 +1.943000e+00 0.000000e+00 0.000000e+00 1.220000e+00 0.000000e+00 0.000000e+00 +1.960000e+00 0.000000e+00 0.000000e+00 1.240000e+00 0.000000e+00 0.000000e+00 +1.978000e+00 0.000000e+00 0.000000e+00 1.250000e+00 0.000000e+00 0.000000e+00 +2.000000e+00 0.000000e+00 0.000000e+00 1.280000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2015_I1389908.cc b/analyses/pluginNovosibirsk/SND_2015_I1389908.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2015_I1389908.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2015_I1389908 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2015_I1389908); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + _num3pi = bookCounter("TMP/num3"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=3) vetoEvent; + if(nCount[-211]==1&&nCount[211]==1&&nCount[111]==1) + _num3pi->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _num3pi->val(); + double error = _num3pi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _num3pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2015_I1389908); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2015_I1389908.info b/analyses/pluginNovosibirsk/SND_2015_I1389908.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2015_I1389908.info @@ -0,0 +1,37 @@ +Name: SND_2015_I1389908 +Year: 2015 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ between 1.05 and 2 GeV. +Experiment: SND +Collider: VEPP-2M +InspireID: 1389908 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - J.Exp.Theor.Phys. 121 (2015) no.1, 27-34 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-\pi^0$ by SND for energies between 1.05 and 2 GeV.' +BibKey: Aulchenko:2015mwt +BibTeX: '%%% contains utf-8, see: http://inspirehep.net/info/faq/general#utf8 +%%% add \usepackage[utf8]{inputenc} to your latex preamble + +@article{Aulchenko:2015mwt, + author = "Aulchenko, V. M. and others", + title = "{Study of the e$^{+}$ e$^{–}$ → + $\pi^+\pi^-\pi^0$ process in the energy range + 1.05–2.00 GeV}", + journal = "J. Exp. Theor. Phys.", + volume = "121", + year = "2015", + number = "1", + pages = "27-34", + doi = "10.1134/S1063776115060023", + note = "[Zh. Eksp. Teor. Fiz.148,no.1,34(2015)]", + SLACcitation = "%%CITATION = JTPHE,121,27;%%" +}' +ToDo: + - Implement the analysis, test it, remove this ToDo, and mark as VALIDATED :-) + diff --git a/analyses/pluginNovosibirsk/SND_2015_I1389908.plot b/analyses/pluginNovosibirsk/SND_2015_I1389908.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2015_I1389908.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2015_I1389908/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +LegendXPos=0.1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2015_I1389908.yoda b/analyses/pluginNovosibirsk/SND_2015_I1389908.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2015_I1389908.yoda @@ -0,0 +1,48 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2015_I1389908/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2015_I1389908/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.05000 0.00000 0.00000 9.80000e-01 5.88218e-01 5.88218e-01 +1.07500 0.00000 0.00000 3.07000e+00 7.22357e-01 7.22357e-01 +1.10000 0.00000 0.00000 3.96000e+00 6.57647e-01 6.57647e-01 +1.12500 0.00000 0.00000 4.52000e+00 3.75366e-01 3.75366e-01 +1.15000 0.00000 0.00000 5.13000e+00 3.82099e-01 3.82099e-01 +1.17500 0.00000 0.00000 5.29000e+00 3.54683e-01 3.54683e-01 +1.20000 0.00000 0.00000 5.07000e+00 3.48281e-01 3.48281e-01 +1.22500 0.00000 0.00000 5.72000e+00 3.67967e-01 3.67967e-01 +1.25000 0.00000 0.00000 5.93000e+00 3.67967e-01 3.67967e-01 +1.27500 0.00000 0.00000 5.50000e+00 3.76431e-01 3.76431e-01 +1.30000 0.00000 0.00000 4.87000e+00 3.34215e-01 3.34215e-01 +1.32500 0.00000 0.00000 4.86000e+00 3.04138e-01 3.04138e-01 +1.35000 0.00000 0.00000 4.97000e+00 3.18904e-01 3.18904e-01 +1.37500 0.00000 0.00000 4.75000e+00 2.97321e-01 2.97321e-01 +1.40000 0.00000 0.00000 4.12000e+00 3.00000e-01 3.00000e-01 +1.42500 0.00000 0.00000 3.99000e+00 2.86007e-01 2.86007e-01 +1.45000 0.00000 0.00000 4.04000e+00 2.94109e-01 2.94109e-01 +1.47500 0.00000 0.00000 4.25000e+00 2.76586e-01 2.76586e-01 +1.50000 0.00000 0.00000 4.39000e+00 2.68701e-01 2.68701e-01 +1.52500 0.00000 0.00000 4.47000e+00 3.06105e-01 3.06105e-01 +1.55000 0.00000 0.00000 4.58000e+00 3.12410e-01 3.12410e-01 +1.57500 0.00000 0.00000 4.66000e+00 3.12410e-01 3.12410e-01 +1.60000 0.00000 0.00000 5.73000e+00 3.67967e-01 3.67967e-01 +1.62500 0.00000 0.00000 5.03000e+00 3.56090e-01 3.56090e-01 +1.65000 0.00000 0.00000 4.64000e+00 3.20156e-01 3.20156e-01 +1.67500 0.00000 0.00000 3.45000e+00 2.66271e-01 2.66271e-01 +1.70000 0.00000 0.00000 2.65000e+00 2.54951e-01 2.54951e-01 +1.72500 0.00000 0.00000 2.18000e+00 2.10238e-01 2.10238e-01 +1.75000 0.00000 0.00000 1.85000e+00 1.96977e-01 1.96977e-01 +1.77500 0.00000 0.00000 1.66000e+00 1.74642e-01 1.74642e-01 +1.80000 0.00000 0.00000 1.08000e+00 1.86815e-01 1.86815e-01 +1.82500 0.00000 0.00000 1.31000e+00 1.52315e-01 1.52315e-01 +1.85000 0.00000 0.00000 1.30000e+00 1.80278e-01 1.80278e-01 +1.87000 0.00000 0.00000 9.30000e-01 1.36015e-01 1.36015e-01 +1.89000 0.00000 0.00000 6.80000e-01 1.23693e-01 1.23693e-01 +1.90000 0.00000 0.00000 1.03000e+00 1.45602e-01 1.45602e-01 +1.92500 0.00000 0.00000 6.50000e-01 1.04403e-01 1.04403e-01 +1.95000 0.00000 0.00000 4.90000e-01 1.21655e-01 1.21655e-01 +1.97500 0.00000 0.00000 6.60000e-01 1.33417e-01 1.33417e-01 +2.00000 0.00000 0.00000 8.10000e-01 1.52971e-01 1.52971e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2016_I1418483.cc b/analyses/pluginNovosibirsk/SND_2016_I1418483.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1418483.cc @@ -0,0 +1,83 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2016_I1418483 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2016_I1418483); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + _numPi0Gamma = bookCounter("TMP/Pi0Gamma"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && nCount[22]==1 && nCount[111]==1) + _numPi0Gamma->fill(event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _numPi0Gamma->val(); + double error = _numPi0Gamma->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 5)); + Scatter2DPtr mult = bookScatter2D(1, 1, 5); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numPi0Gamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2016_I1418483); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2016_I1418483.info b/analyses/pluginNovosibirsk/SND_2016_I1418483.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1418483.info @@ -0,0 +1,34 @@ +Name: SND_2016_I1418483 +Year: 2016 +Summary: Cross section for $e^+e^-\to\pi\gamma$ for energies between 600 MeV and 1380 MeV +Experiment: SND +Collider: VEPP-2M +InspireID: 1418483 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D93 (2016) no.9, 092001 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\pi\gamma$ for energies between 600 MeV and 1380 MeV' +Keywords: [] +BibKey: Achasov:2016bfr +BibTeX: '@article{Achasov:2016bfr, + author = "Achasov, M. N. and others", + title = "{Study of the reaction $e^+e^- \to \pi^0\gamma$ with the + SND detector at the VEPP-2M collider}", + collaboration = "SND", + journal = "Phys. Rev.", + volume = "D93", + year = "2016", + number = "9", + pages = "092001", + doi = "10.1103/PhysRevD.93.092001", + eprint = "1601.08061", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1601.08061;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2016_I1418483.plot b/analyses/pluginNovosibirsk/SND_2016_I1418483.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1418483.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2016_I1418483/d01-x01-y05 +Title=$\sigma(e^+e^-\to \pi^0\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^0\gamma)$/nb +LogY=1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2016_I1418483.yoda b/analyses/pluginNovosibirsk/SND_2016_I1418483.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1418483.yoda @@ -0,0 +1,345 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1418483/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2016_I1418483/d01-x01-y01 +Title: doi:10.17182/hepdata.77047.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.000000e+02 0.000000e+00 0.000000e+00 8.700000e+01 0.000000e+00 0.000000e+00 +6.300000e+02 0.000000e+00 0.000000e+00 1.180000e+02 0.000000e+00 0.000000e+00 +6.600000e+02 0.000000e+00 0.000000e+00 2.740000e+02 0.000000e+00 0.000000e+00 +6.900000e+02 0.000000e+00 0.000000e+00 1.720000e+02 0.000000e+00 0.000000e+00 +7.200000e+02 0.000000e+00 0.000000e+00 5.700000e+02 0.000000e+00 0.000000e+00 +7.502600e+02 0.000000e+00 0.000000e+00 2.210000e+02 0.000000e+00 0.000000e+00 +7.602900e+02 0.000000e+00 0.000000e+00 2.420000e+02 0.000000e+00 0.000000e+00 +7.643100e+02 0.000000e+00 0.000000e+00 2.530000e+02 0.000000e+00 0.000000e+00 +7.697900e+02 0.000000e+00 0.000000e+00 4.500000e+01 0.000000e+00 0.000000e+00 +7.704000e+02 0.000000e+00 0.000000e+00 2.430000e+02 0.000000e+00 0.000000e+00 +7.737900e+02 0.000000e+00 0.000000e+00 6.400000e+01 0.000000e+00 0.000000e+00 +7.744000e+02 0.000000e+00 0.000000e+00 1.550000e+02 0.000000e+00 0.000000e+00 +7.778600e+02 0.000000e+00 0.000000e+00 9.800000e+01 0.000000e+00 0.000000e+00 +7.784000e+02 0.000000e+00 0.000000e+00 1.520000e+02 0.000000e+00 0.000000e+00 +7.797900e+02 0.000000e+00 0.000000e+00 4.200000e+01 0.000000e+00 0.000000e+00 +7.802000e+02 0.000000e+00 0.000000e+00 2.700000e+02 0.000000e+00 0.000000e+00 +7.807900e+02 0.000000e+00 0.000000e+00 1.340000e+02 0.000000e+00 0.000000e+00 +7.814000e+02 0.000000e+00 0.000000e+00 2.080000e+02 0.000000e+00 0.000000e+00 +7.818000e+02 0.000000e+00 0.000000e+00 3.770000e+02 0.000000e+00 0.000000e+00 +7.824000e+02 0.000000e+00 0.000000e+00 2.870000e+02 0.000000e+00 0.000000e+00 +7.827900e+02 0.000000e+00 0.000000e+00 8.300000e+01 0.000000e+00 0.000000e+00 +7.832500e+02 0.000000e+00 0.000000e+00 3.970000e+02 0.000000e+00 0.000000e+00 +7.837900e+02 0.000000e+00 0.000000e+00 7.700000e+01 0.000000e+00 0.000000e+00 +7.844000e+02 0.000000e+00 0.000000e+00 2.760000e+02 0.000000e+00 0.000000e+00 +7.854000e+02 0.000000e+00 0.000000e+00 2.170000e+02 0.000000e+00 0.000000e+00 +7.858700e+02 0.000000e+00 0.000000e+00 9.500000e+01 0.000000e+00 0.000000e+00 +7.864000e+02 0.000000e+00 0.000000e+00 1.720000e+02 0.000000e+00 0.000000e+00 +7.897900e+02 0.000000e+00 0.000000e+00 5.800000e+01 0.000000e+00 0.000000e+00 +7.904000e+02 0.000000e+00 0.000000e+00 1.330000e+02 0.000000e+00 0.000000e+00 +7.937900e+02 0.000000e+00 0.000000e+00 5.400000e+01 0.000000e+00 0.000000e+00 +7.944000e+02 0.000000e+00 0.000000e+00 1.550000e+02 0.000000e+00 0.000000e+00 +8.002800e+02 0.000000e+00 0.000000e+00 2.800000e+02 0.000000e+00 0.000000e+00 +8.102500e+02 0.000000e+00 0.000000e+00 2.840000e+02 0.000000e+00 0.000000e+00 +8.200000e+02 0.000000e+00 0.000000e+00 3.200000e+02 0.000000e+00 0.000000e+00 +8.400000e+02 0.000000e+00 0.000000e+00 6.870000e+02 0.000000e+00 0.000000e+00 +8.800000e+02 0.000000e+00 0.000000e+00 3.830000e+02 0.000000e+00 0.000000e+00 +9.200000e+02 0.000000e+00 0.000000e+00 4.890000e+02 0.000000e+00 0.000000e+00 +9.400000e+02 0.000000e+00 0.000000e+00 4.800000e+02 0.000000e+00 0.000000e+00 +9.500000e+02 0.000000e+00 0.000000e+00 2.680000e+02 0.000000e+00 0.000000e+00 +9.580000e+02 0.000000e+00 0.000000e+00 2.410000e+02 0.000000e+00 0.000000e+00 +9.700000e+02 0.000000e+00 0.000000e+00 2.580000e+02 0.000000e+00 0.000000e+00 +9.841100e+02 0.000000e+00 0.000000e+00 3.530000e+02 0.000000e+00 0.000000e+00 +1.003820e+03 0.000000e+00 0.000000e+00 3.720000e+02 0.000000e+00 0.000000e+00 +1.010260e+03 0.000000e+00 0.000000e+00 3.010000e+02 0.000000e+00 0.000000e+00 +1.015580e+03 0.000000e+00 0.000000e+00 3.470000e+02 0.000000e+00 0.000000e+00 +1.016730e+03 0.000000e+00 0.000000e+00 5.950000e+02 0.000000e+00 0.000000e+00 +1.017660e+03 0.000000e+00 0.000000e+00 9.420000e+02 0.000000e+00 0.000000e+00 +1.018700e+03 0.000000e+00 0.000000e+00 9.860000e+02 0.000000e+00 0.000000e+00 +1.019660e+03 0.000000e+00 0.000000e+00 1.001000e+03 0.000000e+00 0.000000e+00 +1.020530e+03 0.000000e+00 0.000000e+00 6.380000e+02 0.000000e+00 0.000000e+00 +1.021540e+03 0.000000e+00 0.000000e+00 3.280000e+02 0.000000e+00 0.000000e+00 +1.022820e+03 0.000000e+00 0.000000e+00 3.620000e+02 0.000000e+00 0.000000e+00 +1.027810e+03 0.000000e+00 0.000000e+00 3.690000e+02 0.000000e+00 0.000000e+00 +1.033700e+03 0.000000e+00 0.000000e+00 3.270000e+02 0.000000e+00 0.000000e+00 +1.039620e+03 0.000000e+00 0.000000e+00 3.280000e+02 0.000000e+00 0.000000e+00 +1.049710e+03 0.000000e+00 0.000000e+00 3.650000e+02 0.000000e+00 0.000000e+00 +1.059580e+03 0.000000e+00 0.000000e+00 3.730000e+02 0.000000e+00 0.000000e+00 +1.080000e+03 1.000000e+01 1.000000e+01 7.800000e+02 0.000000e+00 0.000000e+00 +1.127000e+03 2.700000e+01 3.300000e+01 1.654000e+03 0.000000e+00 0.000000e+00 +1.201000e+03 2.100000e+01 2.900000e+01 1.659000e+03 0.000000e+00 0.000000e+00 +1.269000e+03 2.900000e+01 3.100000e+01 1.762000e+03 0.000000e+00 0.000000e+00 +1.350000e+03 4.000000e+01 3.000000e+01 2.781000e+03 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1418483/d01-x01-y02 +IsRef: 1 +Path: /REF/SND_2016_I1418483/d01-x01-y02 +Title: doi:10.17182/hepdata.77047.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.000000e+02 0.000000e+00 0.000000e+00 3.530000e+01 0.000000e+00 0.000000e+00 +6.300000e+02 0.000000e+00 0.000000e+00 3.660000e+01 0.000000e+00 0.000000e+00 +6.600000e+02 0.000000e+00 0.000000e+00 3.740000e+01 0.000000e+00 0.000000e+00 +6.900000e+02 0.000000e+00 0.000000e+00 3.770000e+01 0.000000e+00 0.000000e+00 +7.200000e+02 0.000000e+00 0.000000e+00 3.890000e+01 0.000000e+00 0.000000e+00 +7.502600e+02 0.000000e+00 0.000000e+00 3.950000e+01 0.000000e+00 0.000000e+00 +7.602900e+02 0.000000e+00 0.000000e+00 3.980000e+01 0.000000e+00 0.000000e+00 +7.643100e+02 0.000000e+00 0.000000e+00 4.000000e+01 0.000000e+00 0.000000e+00 +7.697900e+02 0.000000e+00 0.000000e+00 4.010000e+01 0.000000e+00 0.000000e+00 +7.704000e+02 0.000000e+00 0.000000e+00 4.010000e+01 0.000000e+00 0.000000e+00 +7.737900e+02 0.000000e+00 0.000000e+00 4.020000e+01 0.000000e+00 0.000000e+00 +7.744000e+02 0.000000e+00 0.000000e+00 4.030000e+01 0.000000e+00 0.000000e+00 +7.778600e+02 0.000000e+00 0.000000e+00 4.020000e+01 0.000000e+00 0.000000e+00 +7.784000e+02 0.000000e+00 0.000000e+00 4.030000e+01 0.000000e+00 0.000000e+00 +7.797900e+02 0.000000e+00 0.000000e+00 4.070000e+01 0.000000e+00 0.000000e+00 +7.802000e+02 0.000000e+00 0.000000e+00 4.030000e+01 0.000000e+00 0.000000e+00 +7.807900e+02 0.000000e+00 0.000000e+00 4.050000e+01 0.000000e+00 0.000000e+00 +7.814000e+02 0.000000e+00 0.000000e+00 4.020000e+01 0.000000e+00 0.000000e+00 +7.818000e+02 0.000000e+00 0.000000e+00 4.040000e+01 0.000000e+00 0.000000e+00 +7.824000e+02 0.000000e+00 0.000000e+00 4.020000e+01 0.000000e+00 0.000000e+00 +7.827900e+02 0.000000e+00 0.000000e+00 4.080000e+01 0.000000e+00 0.000000e+00 +7.832500e+02 0.000000e+00 0.000000e+00 4.020000e+01 0.000000e+00 0.000000e+00 +7.837900e+02 0.000000e+00 0.000000e+00 4.080000e+01 0.000000e+00 0.000000e+00 +7.844000e+02 0.000000e+00 0.000000e+00 4.040000e+01 0.000000e+00 0.000000e+00 +7.854000e+02 0.000000e+00 0.000000e+00 4.030000e+01 0.000000e+00 0.000000e+00 +7.858700e+02 0.000000e+00 0.000000e+00 4.060000e+01 0.000000e+00 0.000000e+00 +7.864000e+02 0.000000e+00 0.000000e+00 4.040000e+01 0.000000e+00 0.000000e+00 +7.897900e+02 0.000000e+00 0.000000e+00 4.080000e+01 0.000000e+00 0.000000e+00 +7.904000e+02 0.000000e+00 0.000000e+00 4.040000e+01 0.000000e+00 0.000000e+00 +7.937900e+02 0.000000e+00 0.000000e+00 4.090000e+01 0.000000e+00 0.000000e+00 +7.944000e+02 0.000000e+00 0.000000e+00 4.060000e+01 0.000000e+00 0.000000e+00 +8.002800e+02 0.000000e+00 0.000000e+00 4.060000e+01 0.000000e+00 0.000000e+00 +8.102500e+02 0.000000e+00 0.000000e+00 4.090000e+01 0.000000e+00 0.000000e+00 +8.200000e+02 0.000000e+00 0.000000e+00 4.120000e+01 0.000000e+00 0.000000e+00 +8.400000e+02 0.000000e+00 0.000000e+00 4.090000e+01 0.000000e+00 0.000000e+00 +8.800000e+02 0.000000e+00 0.000000e+00 4.140000e+01 0.000000e+00 0.000000e+00 +9.200000e+02 0.000000e+00 0.000000e+00 4.150000e+01 0.000000e+00 0.000000e+00 +9.400000e+02 0.000000e+00 0.000000e+00 4.230000e+01 0.000000e+00 0.000000e+00 +9.500000e+02 0.000000e+00 0.000000e+00 4.240000e+01 0.000000e+00 0.000000e+00 +9.580000e+02 0.000000e+00 0.000000e+00 4.310000e+01 0.000000e+00 0.000000e+00 +9.700000e+02 0.000000e+00 0.000000e+00 4.380000e+01 0.000000e+00 0.000000e+00 +9.841100e+02 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.003820e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.010260e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.015580e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.016730e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.017660e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.018700e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.019660e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.020530e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.021540e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.022820e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.027810e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.033700e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.039620e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.049710e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.059580e+03 0.000000e+00 0.000000e+00 4.300000e+01 0.000000e+00 0.000000e+00 +1.080000e+03 1.000000e+01 1.000000e+01 2.530000e+01 0.000000e+00 0.000000e+00 +1.127000e+03 2.700000e+01 3.300000e+01 2.520000e+01 0.000000e+00 0.000000e+00 +1.201000e+03 2.100000e+01 2.900000e+01 2.450000e+01 0.000000e+00 0.000000e+00 +1.269000e+03 2.900000e+01 3.100000e+01 2.370000e+01 0.000000e+00 0.000000e+00 +1.350000e+03 4.000000e+01 3.000000e+01 2.230000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1418483/d01-x01-y03 +IsRef: 1 +Path: /REF/SND_2016_I1418483/d01-x01-y03 +Title: doi:10.17182/hepdata.77047.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.000000e+02 0.000000e+00 0.000000e+00 0.000000e+00 1.100000e+01 1.100000e+01 +6.300000e+02 0.000000e+00 0.000000e+00 2.400000e+01 1.300000e+01 1.300000e+01 +6.600000e+02 0.000000e+00 0.000000e+00 6.500000e+01 1.900000e+01 1.900000e+01 +6.900000e+02 0.000000e+00 0.000000e+00 7.800000e+01 1.600000e+01 1.600000e+01 +7.200000e+02 0.000000e+00 0.000000e+00 4.000000e+02 3.200000e+01 3.200000e+01 +7.502600e+02 0.000000e+00 0.000000e+00 3.370000e+02 2.400000e+01 2.400000e+01 +7.602900e+02 0.000000e+00 0.000000e+00 6.350000e+02 3.000000e+01 3.000000e+01 +7.643100e+02 0.000000e+00 0.000000e+00 8.870000e+02 3.500000e+01 3.500000e+01 +7.697900e+02 0.000000e+00 0.000000e+00 2.600000e+02 1.800000e+01 1.800000e+01 +7.704000e+02 0.000000e+00 0.000000e+00 1.660000e+03 4.500000e+01 4.500000e+01 +7.737900e+02 0.000000e+00 0.000000e+00 6.670000e+02 2.800000e+01 2.800000e+01 +7.744000e+02 0.000000e+00 0.000000e+00 1.926000e+03 4.700000e+01 4.700000e+01 +7.778600e+02 0.000000e+00 0.000000e+00 2.461000e+03 5.100000e+01 5.100000e+01 +7.784000e+02 0.000000e+00 0.000000e+00 4.210000e+03 6.700000e+01 6.700000e+01 +7.797900e+02 0.000000e+00 0.000000e+00 1.512000e+03 4.000000e+01 4.000000e+01 +7.802000e+02 0.000000e+00 0.000000e+00 1.106300e+04 1.080000e+02 1.080000e+02 +7.807900e+02 0.000000e+00 0.000000e+00 6.202000e+03 8.100000e+01 8.100000e+01 +7.814000e+02 0.000000e+00 0.000000e+00 1.037800e+04 1.050000e+02 1.050000e+02 +7.818000e+02 0.000000e+00 0.000000e+00 1.983100e+04 1.440000e+02 1.440000e+02 +7.824000e+02 0.000000e+00 0.000000e+00 1.538100e+04 1.270000e+02 1.270000e+02 +7.827900e+02 0.000000e+00 0.000000e+00 4.473000e+03 6.900000e+01 6.900000e+01 +7.832500e+02 0.000000e+00 0.000000e+00 2.105300e+04 1.490000e+02 1.490000e+02 +7.837900e+02 0.000000e+00 0.000000e+00 3.980000e+03 6.400000e+01 6.400000e+01 +7.844000e+02 0.000000e+00 0.000000e+00 1.344700e+04 1.190000e+02 1.190000e+02 +7.854000e+02 0.000000e+00 0.000000e+00 9.003000e+03 9.800000e+01 9.800000e+01 +7.858700e+02 0.000000e+00 0.000000e+00 3.599000e+03 6.200000e+01 6.200000e+01 +7.864000e+02 0.000000e+00 0.000000e+00 5.982000e+03 8.800000e+01 8.800000e+01 +7.897900e+02 0.000000e+00 0.000000e+00 1.131000e+03 3.500000e+01 3.500000e+01 +7.904000e+02 0.000000e+00 0.000000e+00 2.311000e+03 5.100000e+01 5.100000e+01 +7.937900e+02 0.000000e+00 0.000000e+00 5.800000e+02 2.600000e+01 2.600000e+01 +7.944000e+02 0.000000e+00 0.000000e+00 1.600000e+03 4.300000e+01 4.300000e+01 +8.002800e+02 0.000000e+00 0.000000e+00 1.719000e+03 4.600000e+01 4.600000e+01 +8.102500e+02 0.000000e+00 0.000000e+00 9.290000e+02 3.600000e+01 3.600000e+01 +8.200000e+02 0.000000e+00 0.000000e+00 7.390000e+02 3.400000e+01 3.400000e+01 +8.400000e+02 0.000000e+00 0.000000e+00 8.510000e+02 4.200000e+01 4.200000e+01 +8.800000e+02 0.000000e+00 0.000000e+00 2.390000e+02 2.600000e+01 2.600000e+01 +9.200000e+02 0.000000e+00 0.000000e+00 1.420000e+02 2.600000e+01 2.600000e+01 +9.400000e+02 0.000000e+00 0.000000e+00 9.300000e+01 2.300000e+01 2.300000e+01 +9.500000e+02 0.000000e+00 0.000000e+00 4.300000e+01 1.500000e+01 1.500000e+01 +9.580000e+02 0.000000e+00 0.000000e+00 4.800000e+01 1.500000e+01 1.500000e+01 +9.700000e+02 0.000000e+00 0.000000e+00 4.500000e+01 1.500000e+01 1.500000e+01 +9.841100e+02 0.000000e+00 0.000000e+00 5.200000e+01 1.600000e+01 1.600000e+01 +1.003820e+03 0.000000e+00 0.000000e+00 6.700000e+01 1.800000e+01 1.800000e+01 +1.010260e+03 0.000000e+00 0.000000e+00 7.300000e+01 1.600000e+01 1.600000e+01 +1.015580e+03 0.000000e+00 0.000000e+00 2.410000e+02 2.300000e+01 2.300000e+01 +1.016730e+03 0.000000e+00 0.000000e+00 7.220000e+02 3.600000e+01 3.600000e+01 +1.017660e+03 0.000000e+00 0.000000e+00 1.338000e+03 4.900000e+01 4.900000e+01 +1.018700e+03 0.000000e+00 0.000000e+00 1.747000e+03 5.500000e+01 5.500000e+01 +1.019660e+03 0.000000e+00 0.000000e+00 1.642000e+03 5.400000e+01 5.400000e+01 +1.020530e+03 0.000000e+00 0.000000e+00 8.930000e+02 4.000000e+01 4.000000e+01 +1.021540e+03 0.000000e+00 0.000000e+00 2.230000e+02 2.300000e+01 2.300000e+01 +1.022820e+03 0.000000e+00 0.000000e+00 1.480000e+02 2.100000e+01 2.100000e+01 +1.027810e+03 0.000000e+00 0.000000e+00 5.100000e+01 1.800000e+01 1.800000e+01 +1.033700e+03 0.000000e+00 0.000000e+00 1.500000e+01 1.500000e+01 1.500000e+01 +1.039620e+03 0.000000e+00 0.000000e+00 1.000000e+01 1.500000e+01 1.500000e+01 +1.049710e+03 0.000000e+00 0.000000e+00 2.200000e+01 1.600000e+01 1.600000e+01 +1.059580e+03 0.000000e+00 0.000000e+00 1.700000e+01 1.700000e+01 1.700000e+01 +1.080000e+03 1.000000e+01 1.000000e+01 2.400000e+01 1.000000e+01 1.000000e+01 +1.127000e+03 2.700000e+01 3.300000e+01 1.500000e+01 1.200000e+01 1.200000e+01 +1.201000e+03 2.100000e+01 2.900000e+01 1.700000e+01 1.100000e+01 1.100000e+01 +1.269000e+03 2.900000e+01 3.100000e+01 2.700000e+01 1.000000e+01 1.000000e+01 +1.350000e+03 4.000000e+01 3.000000e+01 1.500000e+01 1.100000e+01 1.100000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1418483/d01-x01-y04 +IsRef: 1 +Path: /REF/SND_2016_I1418483/d01-x01-y04 +Title: doi:10.17182/hepdata.77047.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.000000e+02 0.000000e+00 0.000000e+00 9.190000e-01 1.000000e-03 1.000000e-03 +6.300000e+02 0.000000e+00 0.000000e+00 9.130000e-01 1.000000e-03 1.000000e-03 +6.600000e+02 0.000000e+00 0.000000e+00 9.060000e-01 1.000000e-03 1.000000e-03 +6.900000e+02 0.000000e+00 0.000000e+00 8.990000e-01 1.000000e-03 1.000000e-03 +7.200000e+02 0.000000e+00 0.000000e+00 8.900000e-01 1.000000e-03 1.000000e-03 +7.502600e+02 0.000000e+00 0.000000e+00 8.650000e-01 1.000000e-03 1.000000e-03 +7.602900e+02 0.000000e+00 0.000000e+00 8.440000e-01 1.000000e-03 1.000000e-03 +7.643100e+02 0.000000e+00 0.000000e+00 8.320000e-01 1.000000e-03 1.000000e-03 +7.697900e+02 0.000000e+00 0.000000e+00 8.120000e-01 1.000000e-03 1.000000e-03 +7.704000e+02 0.000000e+00 0.000000e+00 8.090000e-01 1.000000e-03 1.000000e-03 +7.737900e+02 0.000000e+00 0.000000e+00 7.940000e-01 1.000000e-03 1.000000e-03 +7.744000e+02 0.000000e+00 0.000000e+00 7.910000e-01 1.000000e-03 1.000000e-03 +7.778600e+02 0.000000e+00 0.000000e+00 7.750000e-01 1.000000e-03 1.000000e-03 +7.784000e+02 0.000000e+00 0.000000e+00 7.740000e-01 1.000000e-03 1.000000e-03 +7.797900e+02 0.000000e+00 0.000000e+00 7.710000e-01 1.000000e-03 1.000000e-03 +7.802000e+02 0.000000e+00 0.000000e+00 7.720000e-01 1.000000e-03 1.000000e-03 +7.807900e+02 0.000000e+00 0.000000e+00 7.740000e-01 1.000000e-03 1.000000e-03 +7.814000e+02 0.000000e+00 0.000000e+00 7.780000e-01 1.000000e-03 1.000000e-03 +7.818000e+02 0.000000e+00 0.000000e+00 7.820000e-01 1.000000e-03 1.000000e-03 +7.824000e+02 0.000000e+00 0.000000e+00 7.900000e-01 1.000000e-03 1.000000e-03 +7.827900e+02 0.000000e+00 0.000000e+00 7.970000e-01 1.000000e-03 1.000000e-03 +7.832500e+02 0.000000e+00 0.000000e+00 8.060000e-01 1.000000e-03 1.000000e-03 +7.837900e+02 0.000000e+00 0.000000e+00 8.190000e-01 1.000000e-03 1.000000e-03 +7.844000e+02 0.000000e+00 0.000000e+00 8.360000e-01 1.000000e-03 1.000000e-03 +7.854000e+02 0.000000e+00 0.000000e+00 8.690000e-01 1.000000e-03 1.000000e-03 +7.858700e+02 0.000000e+00 0.000000e+00 8.860000e-01 1.000000e-03 1.000000e-03 +7.864000e+02 0.000000e+00 0.000000e+00 9.060000e-01 1.000000e-03 1.000000e-03 +7.897900e+02 0.000000e+00 0.000000e+00 1.040000e+00 1.000000e-03 1.000000e-03 +7.904000e+02 0.000000e+00 0.000000e+00 1.064000e+00 1.000000e-03 1.000000e-03 +7.937900e+02 0.000000e+00 0.000000e+00 1.197000e+00 1.000000e-03 1.000000e-03 +7.944000e+02 0.000000e+00 0.000000e+00 1.220000e+00 1.000000e-03 1.000000e-03 +8.002800e+02 0.000000e+00 0.000000e+00 1.422000e+00 1.000000e-03 1.000000e-03 +8.102500e+02 0.000000e+00 0.000000e+00 1.682000e+00 2.000000e-03 2.000000e-03 +8.200000e+02 0.000000e+00 0.000000e+00 1.848000e+00 3.000000e-03 3.000000e-03 +8.400000e+02 0.000000e+00 0.000000e+00 2.016000e+00 3.000000e-03 3.000000e-03 +8.800000e+02 0.000000e+00 0.000000e+00 1.861000e+00 3.000000e-03 3.000000e-03 +9.200000e+02 0.000000e+00 0.000000e+00 1.353000e+00 1.000000e-03 1.000000e-03 +9.400000e+02 0.000000e+00 0.000000e+00 1.183000e+00 1.000000e-03 1.000000e-03 +9.500000e+02 0.000000e+00 0.000000e+00 1.125000e+00 1.000000e-03 1.000000e-03 +9.580000e+02 0.000000e+00 0.000000e+00 1.088000e+00 1.000000e-03 1.000000e-03 +9.700000e+02 0.000000e+00 0.000000e+00 1.044000e+00 1.000000e-03 1.000000e-03 +9.841100e+02 0.000000e+00 0.000000e+00 1.002000e+00 1.000000e-03 1.000000e-03 +1.003820e+03 0.000000e+00 0.000000e+00 9.050000e-01 3.000000e-03 3.000000e-03 +1.010260e+03 0.000000e+00 0.000000e+00 8.440000e-01 2.000000e-03 2.000000e-03 +1.015580e+03 0.000000e+00 0.000000e+00 7.690000e-01 1.000000e-03 1.000000e-03 +1.016730e+03 0.000000e+00 0.000000e+00 7.520000e-01 1.000000e-03 1.000000e-03 +1.017660e+03 0.000000e+00 0.000000e+00 7.430000e-01 1.000000e-03 1.000000e-03 +1.018700e+03 0.000000e+00 0.000000e+00 7.490000e-01 2.000000e-03 2.000000e-03 +1.019660e+03 0.000000e+00 0.000000e+00 7.910000e-01 3.000000e-03 3.000000e-03 +1.020530e+03 0.000000e+00 0.000000e+00 8.710000e-01 6.000000e-03 6.000000e-03 +1.021540e+03 0.000000e+00 0.000000e+00 1.020000e+00 2.000000e-03 2.000000e-03 +1.022820e+03 0.000000e+00 0.000000e+00 1.300000e+00 5.000000e-03 5.000000e-03 +1.080000e+03 1.000000e+01 1.000000e+01 1.640000e+00 2.000000e-03 2.000000e-03 +1.127000e+03 2.700000e+01 3.300000e+01 1.170000e+00 6.000000e-03 6.000000e-03 +1.201000e+03 2.100000e+01 2.900000e+01 1.020000e+00 3.000000e-03 3.000000e-03 +1.269000e+03 2.900000e+01 3.100000e+01 9.800000e-01 3.000000e-03 3.000000e-03 +1.350000e+03 4.000000e+01 3.000000e+01 9.100000e-01 8.000000e-03 8.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1418483/d01-x01-y05 +IsRef: 1 +Path: /REF/SND_2016_I1418483/d01-x01-y05 +Title: doi:10.17182/hepdata.77047.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.000000e+02 0.000000e+00 0.000000e+00 0.000000e+00 4.001250e-01 4.001250e-01 +6.300000e+02 0.000000e+00 0.000000e+00 6.100000e-01 3.301515e-01 3.301515e-01 +6.600000e+02 0.000000e+00 0.000000e+00 7.000000e-01 2.002498e-01 2.002498e-01 +6.900000e+02 0.000000e+00 0.000000e+00 1.330000e+00 2.807134e-01 2.807134e-01 +7.200000e+02 0.000000e+00 0.000000e+00 2.030000e+00 1.627882e-01 1.627882e-01 +7.502600e+02 0.000000e+00 0.000000e+00 4.450000e+00 3.255764e-01 3.255764e-01 +7.602900e+02 0.000000e+00 0.000000e+00 7.810000e+00 3.956008e-01 3.956008e-01 +7.643100e+02 0.000000e+00 0.000000e+00 1.052000e+01 4.459821e-01 4.459821e-01 +7.697900e+02 0.000000e+00 0.000000e+00 1.788000e+01 1.280976e+00 1.280976e+00 +7.704000e+02 0.000000e+00 0.000000e+00 2.102000e+01 6.576473e-01 6.576473e-01 +7.737900e+02 0.000000e+00 0.000000e+00 3.250000e+01 1.486607e+00 1.486607e+00 +7.744000e+02 0.000000e+00 0.000000e+00 3.910000e+01 1.166190e+00 1.166190e+00 +7.778600e+02 0.000000e+00 0.000000e+00 8.050000e+01 2.280351e+00 2.280351e+00 +7.784000e+02 0.000000e+00 0.000000e+00 8.900000e+01 2.193171e+00 2.193171e+00 +7.797900e+02 0.000000e+00 0.000000e+00 1.139000e+02 3.858756e+00 3.858756e+00 +7.802000e+02 0.000000e+00 0.000000e+00 1.320000e+02 2.662705e+00 2.662705e+00 +7.807900e+02 0.000000e+00 0.000000e+00 1.474000e+02 3.182766e+00 3.182766e+00 +7.814000e+02 0.000000e+00 0.000000e+00 1.598000e+02 3.061046e+00 3.061046e+00 +7.818000e+02 0.000000e+00 0.000000e+00 1.669000e+02 2.830194e+00 2.830194e+00 +7.824000e+02 0.000000e+00 0.000000e+00 1.692000e+02 2.860070e+00 2.860070e+00 +7.827900e+02 0.000000e+00 0.000000e+00 1.664000e+02 3.701351e+00 3.701351e+00 +7.832500e+02 0.000000e+00 0.000000e+00 1.639000e+02 2.662705e+00 2.662705e+00 +7.837900e+02 0.000000e+00 0.000000e+00 1.558000e+02 3.640055e+00 3.640055e+00 +7.844000e+02 0.000000e+00 0.000000e+00 1.444000e+02 2.662705e+00 2.662705e+00 +7.854000e+02 0.000000e+00 0.000000e+00 1.182000e+02 2.420744e+00 2.420744e+00 +7.858700e+02 0.000000e+00 0.000000e+00 1.055000e+02 2.624881e+00 2.624881e+00 +7.864000e+02 0.000000e+00 0.000000e+00 9.480000e+01 2.193171e+00 2.193171e+00 +7.897900e+02 0.000000e+00 0.000000e+00 4.610000e+01 1.746425e+00 1.746425e+00 +7.904000e+02 0.000000e+00 0.000000e+00 4.040000e+01 1.166190e+00 1.166190e+00 +7.937900e+02 0.000000e+00 0.000000e+00 2.200000e+01 1.236932e+00 1.236932e+00 +7.944000e+02 0.000000e+00 0.000000e+00 2.080000e+01 7.615773e-01 7.615773e-01 +8.002800e+02 0.000000e+00 0.000000e+00 1.060000e+01 4.123106e-01 4.123106e-01 +8.102500e+02 0.000000e+00 0.000000e+00 4.760000e+00 3.275668e-01 3.275668e-01 +8.200000e+02 0.000000e+00 0.000000e+00 3.030000e+00 2.630589e-01 2.630589e-01 +8.400000e+02 0.000000e+00 0.000000e+00 1.500000e+00 1.513275e-01 1.513275e-01 +8.800000e+02 0.000000e+00 0.000000e+00 8.100000e-01 1.603122e-01 1.603122e-01 +9.200000e+02 0.000000e+00 0.000000e+00 5.200000e-01 1.303840e-01 1.303840e-01 +9.400000e+02 0.000000e+00 0.000000e+00 3.900000e-01 1.104536e-01 1.104536e-01 +9.500000e+02 0.000000e+00 0.000000e+00 3.300000e-01 1.403567e-01 1.403567e-01 +9.580000e+02 0.000000e+00 0.000000e+00 4.200000e-01 1.403567e-01 1.403567e-01 +9.700000e+02 0.000000e+00 0.000000e+00 3.800000e-01 1.403567e-01 1.403567e-01 +9.841100e+02 0.000000e+00 0.000000e+00 3.400000e-01 1.104536e-01 1.104536e-01 +1.003820e+03 0.000000e+00 0.000000e+00 4.600000e-01 1.204159e-01 1.204159e-01 +1.010260e+03 0.000000e+00 0.000000e+00 6.700000e-01 1.503330e-01 1.503330e-01 +1.015580e+03 0.000000e+00 0.000000e+00 2.080000e+00 2.137756e-01 2.137756e-01 +1.016730e+03 0.000000e+00 0.000000e+00 3.720000e+00 2.024846e-01 2.024846e-01 +1.017660e+03 0.000000e+00 0.000000e+00 4.440000e+00 1.835756e-01 1.835756e-01 +1.018700e+03 0.000000e+00 0.000000e+00 5.630000e+00 1.969772e-01 1.969772e-01 +1.019660e+03 0.000000e+00 0.000000e+00 4.930000e+00 1.886796e-01 1.886796e-01 +1.020530e+03 0.000000e+00 0.000000e+00 3.710000e+00 1.923538e-01 1.923538e-01 +1.021540e+03 0.000000e+00 0.000000e+00 1.530000e+00 1.676305e-01 1.676305e-01 +1.022820e+03 0.000000e+00 0.000000e+00 7.100000e-01 1.431782e-01 1.431782e-01 +1.027810e+03 0.000000e+00 0.000000e+00 5.000000e-02 1.140175e-01 1.140175e-01 +1.033700e+03 0.000000e+00 0.000000e+00 0.000000e+00 1.104536e-01 1.104536e-01 +1.039620e+03 0.000000e+00 0.000000e+00 1.000000e-02 1.104536e-01 1.104536e-01 +1.049710e+03 0.000000e+00 0.000000e+00 4.000000e-02 1.004988e-01 1.004988e-01 +1.059580e+03 0.000000e+00 0.000000e+00 4.000000e-02 1.104536e-01 1.104536e-01 +1.080000e+03 1.000000e+01 1.000000e+01 7.500000e-02 4.964877e-02 4.964877e-02 +1.127000e+03 2.700000e+01 3.300000e+01 3.000000e-02 2.807134e-02 2.807134e-02 +1.201000e+03 2.100000e+01 2.900000e+01 4.000000e-02 2.701851e-02 2.701851e-02 +1.269000e+03 2.900000e+01 3.100000e+01 6.500000e-02 2.517936e-02 2.517936e-02 +1.350000e+03 4.000000e+01 3.000000e+01 2.700000e-02 1.910497e-02 1.910497e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2016_I1471515.cc b/analyses/pluginNovosibirsk/SND_2016_I1471515.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1471515.cc @@ -0,0 +1,122 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2016_I1471515 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2016_I1471515); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nOmegaEtaPi= bookCounter("/TMP/nOmegaEtaPi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=223) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + foreach (const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=221) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=1) continue; + bool matched2 = true; + for(auto const & val : nResB) { + if(val.first==111) { + if(val.second!=1) { + matched2 = false; + break; + } + } + else if(val.second!=0) { + matched2 = false; + break; + } + } + if(matched2) { + _nOmegaEtaPi->fill(event.weight()); + break; + } + } + } + } + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nOmegaEtaPi->val(); + double error = _nOmegaEtaPi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 6)); + Scatter2DPtr mult = bookScatter2D(1, 1, 6); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nOmegaEtaPi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2016_I1471515); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2016_I1471515.info b/analyses/pluginNovosibirsk/SND_2016_I1471515.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1471515.info @@ -0,0 +1,32 @@ +Name: SND_2016_I1471515 +Year: 2016 +Summary: Cross section for $e^+e^-\to\eta\omega\pi^0$ for energies below 2 GeV +Experiment: SND +Collider: +InspireID: 1471515 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D94 (2016) no.9, 092002 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\eta\omega\pi^0$ for energies below 2 GeV' +BibKey: Achasov:2016eyg +BibTeX: '@article{Achasov:2016eyg, + author = "Achasov, M. N. and others", + title = "{Study of the process $e^+e^-\to\omega\eta\pi^0$ in the + energy range $\sqrt{s} <2$ GeV with the SND detector}", + journal = "Phys. Rev.", + volume = "D94", + year = "2016", + number = "3", + pages = "032010", + doi = "10.1103/PhysRevD.94.032010", + eprint = "1606.06481", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1606.06481;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2016_I1471515.plot b/analyses/pluginNovosibirsk/SND_2016_I1471515.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1471515.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /SND_2016_I1471515/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\omega\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\omega\pi^0)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2016_I1471515.yoda b/analyses/pluginNovosibirsk/SND_2016_I1471515.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1471515.yoda @@ -0,0 +1,136 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1471515/d01-x01-y01 +Variations: [""] +ErrorBreakdown: {0: {}, 1: {}, 2: {}, 3: {}, 4: {}, 5: {}, 6: {}, 7: {}, 8: {}, 9: {}, 10: {}, 11: {}} + +IsRef: 1 +Path: /REF/SND_2016_I1471515/d01-x01-y01 +Title: doi:10.17182/hepdata.82577.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.550000e+03 5.000000e+01 5.000000e+01 5.888000e+03 0.000000e+00 0.000000e+00 +1.650000e+03 5.000000e+01 5.000000e+01 5.004000e+03 0.000000e+00 0.000000e+00 +1.725000e+03 2.500000e+01 2.500000e+01 2.261000e+03 0.000000e+00 0.000000e+00 +1.775000e+03 2.500000e+01 2.500000e+01 2.392000e+03 0.000000e+00 0.000000e+00 +1.812500e+03 1.250000e+01 1.250000e+01 2.373000e+03 0.000000e+00 0.000000e+00 +1.837500e+03 1.250000e+01 1.250000e+01 1.897000e+03 0.000000e+00 0.000000e+00 +1.862500e+03 1.250000e+01 1.250000e+01 2.527000e+03 0.000000e+00 0.000000e+00 +1.887500e+03 1.250000e+01 1.250000e+01 6.620000e+02 0.000000e+00 0.000000e+00 +1.912500e+03 1.250000e+01 1.250000e+01 3.459000e+03 0.000000e+00 0.000000e+00 +1.937500e+03 1.250000e+01 1.250000e+01 2.361000e+03 0.000000e+00 0.000000e+00 +1.962500e+03 1.250000e+01 1.250000e+01 2.077000e+03 0.000000e+00 0.000000e+00 +1.987500e+03 1.250000e+01 1.250000e+01 2.682000e+03 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1471515/d01-x01-y02 +Variations: [""] +ErrorBreakdown: {0: {}, 1: {}, 2: {}, 3: {}, 4: {}, 5: {}, 6: {}, 7: {}, 8: {}, 9: {}, 10: {}, 11: {}} + +IsRef: 1 +Path: /REF/SND_2016_I1471515/d01-x01-y02 +Title: doi:10.17182/hepdata.82577.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.550000e+03 5.000000e+01 5.000000e+01 0.000000e+00 0.000000e+00 0.000000e+00 +1.650000e+03 5.000000e+01 5.000000e+01 0.000000e+00 0.000000e+00 0.000000e+00 +1.725000e+03 2.500000e+01 2.500000e+01 1.000000e+00 0.000000e+00 0.000000e+00 +1.775000e+03 2.500000e+01 2.500000e+01 3.000000e+00 0.000000e+00 0.000000e+00 +1.812500e+03 1.250000e+01 1.250000e+01 6.000000e+00 0.000000e+00 0.000000e+00 +1.837500e+03 1.250000e+01 1.250000e+01 7.000000e+00 0.000000e+00 0.000000e+00 +1.862500e+03 1.250000e+01 1.250000e+01 8.000000e+00 0.000000e+00 0.000000e+00 +1.887500e+03 1.250000e+01 1.250000e+01 3.000000e+00 0.000000e+00 0.000000e+00 +1.912500e+03 1.250000e+01 1.250000e+01 9.000000e+00 0.000000e+00 0.000000e+00 +1.937500e+03 1.250000e+01 1.250000e+01 1.100000e+01 0.000000e+00 0.000000e+00 +1.962500e+03 1.250000e+01 1.250000e+01 5.000000e+00 0.000000e+00 0.000000e+00 +1.987500e+03 1.250000e+01 1.250000e+01 9.000000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1471515/d01-x01-y03 +Variations: [""] +ErrorBreakdown: {0: {}, 1: {}, 2: {}, 3: {}, 4: {}, 5: {}, 6: {}, 7: {}, 8: {}, 9: {}, 10: {}, 11: {}} + +IsRef: 1 +Path: /REF/SND_2016_I1471515/d01-x01-y03 +Title: doi:10.17182/hepdata.82577.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.550000e+03 5.000000e+01 5.000000e+01 2.000000e-02 0.000000e+00 0.000000e+00 +1.650000e+03 5.000000e+01 5.000000e+01 2.100000e-01 0.000000e+00 0.000000e+00 +1.725000e+03 2.500000e+01 2.500000e+01 1.300000e-01 0.000000e+00 0.000000e+00 +1.775000e+03 2.500000e+01 2.500000e+01 9.000000e-02 0.000000e+00 0.000000e+00 +1.812500e+03 1.250000e+01 1.250000e+01 9.000000e-02 0.000000e+00 0.000000e+00 +1.837500e+03 1.250000e+01 1.250000e+01 5.000000e-02 0.000000e+00 0.000000e+00 +1.862500e+03 1.250000e+01 1.250000e+01 6.000000e-02 0.000000e+00 0.000000e+00 +1.887500e+03 1.250000e+01 1.250000e+01 2.000000e-02 0.000000e+00 0.000000e+00 +1.912500e+03 1.250000e+01 1.250000e+01 7.000000e-02 0.000000e+00 0.000000e+00 +1.937500e+03 1.250000e+01 1.250000e+01 5.000000e-02 0.000000e+00 0.000000e+00 +1.962500e+03 1.250000e+01 1.250000e+01 6.000000e-02 0.000000e+00 0.000000e+00 +1.987500e+03 1.250000e+01 1.250000e+01 6.000000e-02 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1471515/d01-x01-y04 +Variations: [""] +ErrorBreakdown: {0: {}, 1: {}, 2: {}, 3: {}, 4: {}, 5: {}, 6: {}, 7: {}, 8: {}, 9: {}, 10: {}, 11: {}} + +IsRef: 1 +Path: /REF/SND_2016_I1471515/d01-x01-y04 +Title: doi:10.17182/hepdata.82577.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.550000e+03 5.000000e+01 5.000000e+01 2.850000e+00 0.000000e+00 0.000000e+00 +1.650000e+03 5.000000e+01 5.000000e+01 4.030000e+00 0.000000e+00 0.000000e+00 +1.725000e+03 2.500000e+01 2.500000e+01 4.250000e+00 0.000000e+00 0.000000e+00 +1.775000e+03 2.500000e+01 2.500000e+01 4.290000e+00 0.000000e+00 0.000000e+00 +1.812500e+03 1.250000e+01 1.250000e+01 4.610000e+00 0.000000e+00 0.000000e+00 +1.837500e+03 1.250000e+01 1.250000e+01 5.020000e+00 0.000000e+00 0.000000e+00 +1.862500e+03 1.250000e+01 1.250000e+01 5.340000e+00 0.000000e+00 0.000000e+00 +1.887500e+03 1.250000e+01 1.250000e+01 5.580000e+00 0.000000e+00 0.000000e+00 +1.912500e+03 1.250000e+01 1.250000e+01 5.120000e+00 0.000000e+00 0.000000e+00 +1.937500e+03 1.250000e+01 1.250000e+01 5.980000e+00 0.000000e+00 0.000000e+00 +1.962500e+03 1.250000e+01 1.250000e+01 5.640000e+00 0.000000e+00 0.000000e+00 +1.987500e+03 1.250000e+01 1.250000e+01 6.140000e+00 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1471515/d01-x01-y05 +Variations: [""] +ErrorBreakdown: {0: {}, 1: {}, 2: {}, 3: {}, 4: {}, 5: {}, 6: {}, 7: {}, 8: {}, 9: {}, 10: {}, 11: {}} + +IsRef: 1 +Path: /REF/SND_2016_I1471515/d01-x01-y05 +Title: doi:10.17182/hepdata.82577.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.550000e+03 5.000000e+01 5.000000e+01 7.790000e-01 0.000000e+00 0.000000e+00 +1.650000e+03 5.000000e+01 5.000000e+01 8.150000e-01 0.000000e+00 0.000000e+00 +1.725000e+03 2.500000e+01 2.500000e+01 8.130000e-01 0.000000e+00 0.000000e+00 +1.775000e+03 2.500000e+01 2.500000e+01 8.100000e-01 0.000000e+00 0.000000e+00 +1.812500e+03 1.250000e+01 1.250000e+01 8.230000e-01 0.000000e+00 0.000000e+00 +1.837500e+03 1.250000e+01 1.250000e+01 8.410000e-01 0.000000e+00 0.000000e+00 +1.862500e+03 1.250000e+01 1.250000e+01 8.550000e-01 0.000000e+00 0.000000e+00 +1.887500e+03 1.250000e+01 1.250000e+01 8.650000e-01 0.000000e+00 0.000000e+00 +1.912500e+03 1.250000e+01 1.250000e+01 8.710000e-01 0.000000e+00 0.000000e+00 +1.937500e+03 1.250000e+01 1.250000e+01 8.800000e-01 0.000000e+00 0.000000e+00 +1.962500e+03 1.250000e+01 1.250000e+01 8.870000e-01 0.000000e+00 0.000000e+00 +1.987500e+03 1.250000e+01 1.250000e+01 8.930000e-01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1471515/d01-x01-y06 +Variations: [""] +ErrorBreakdown: {2: {error: {dn: -0.3, up: 0.9}}, 3: {error: {dn: -0.6, up: 1.1}}, 4: {error: {dn: -0.8, up: 1.3}}, 5: {error: {dn: -1.0, up: 1.5}}, 6: {error: {dn: -0.8, up: 1.1}}, 7: {error: {dn: -1.6, up: 2.9}}, 8: {error: {dn: -0.6, up: 0.9}}, 9: {error: {dn: -0.8, up: 1.1}}, 10: {error: {dn: -0.7, up: 1.0}}, 11: {error: {dn: -0.6, up: 0.9}}} + +IsRef: 1 +Path: /REF/SND_2016_I1471515/d01-x01-y06 +Title: doi:10.17182/hepdata.82577.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.725000e+03 2.500000e+01 2.500000e+01 4.000000e-01 3.000000e-01 9.000000e-01 +1.775000e+03 2.500000e+01 2.500000e+01 1.100000e+00 6.000000e-01 1.100000e+00 +1.812500e+03 1.250000e+01 1.250000e+01 2.100000e+00 8.000000e-01 1.300000e+00 +1.837500e+03 1.250000e+01 1.250000e+01 2.800000e+00 1.000000e+00 1.500000e+00 +1.862500e+03 1.250000e+01 1.250000e+01 2.200000e+00 8.000000e-01 1.100000e+00 +1.887500e+03 1.250000e+01 1.250000e+01 3.000000e+00 1.600000e+00 2.900000e+00 +1.912500e+03 1.250000e+01 1.250000e+01 1.900000e+00 6.000000e-01 9.000000e-01 +1.937500e+03 1.250000e+01 1.250000e+01 2.800000e+00 8.000000e-01 1.100000e+00 +1.962500e+03 1.250000e+01 1.250000e+01 1.500000e+00 7.000000e-01 1.000000e+00 +1.987500e+03 1.250000e+01 1.250000e+01 1.900000e+00 6.000000e-01 9.000000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2016_I1473343.cc b/analyses/pluginNovosibirsk/SND_2016_I1473343.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1473343.cc @@ -0,0 +1,115 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2016_I1473343 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2016_I1473343); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nOmegaEta= bookCounter("/TMP/nOmegaEta"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=223) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + foreach (const Particle& p2, ufs.particles()) { + if(p2.pdgId()!=221) continue; + map nResB = nRes; + int ncountB = ncount; + findChildren(p2,nResB,ncountB); + if(ncountB!=0) continue; + bool matched2 = true; + for(auto const & val : nResB) { + if(val.second!=0) { + matched2 = false; + break; + } + } + if(matched2) { + _nOmegaEta->fill(event.weight()); + break; + } + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nOmegaEta->val(); + double error = _nOmegaEta->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + //@} + + + /// @name Histograms + //@{ + CounterPtr _nOmegaEta; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2016_I1473343); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2016_I1473343.info b/analyses/pluginNovosibirsk/SND_2016_I1473343.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1473343.info @@ -0,0 +1,33 @@ +Name: SND_2016_I1473343 +Year: 2016 +Summary: Cross section for $e^+e^-\to\eta\omega$ for energies below 2 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 1473343 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D94 (2016) no.9, 092002 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\eta\omega$ for energies below 2 GeV' +Keywords: [] +BibKey: Achasov:2016qvd +BibTeX: '@article{Achasov:2016qvd, + author = "Achasov, M. N. and others", + title = "{Measurement of the $e^+e^- \to \omega\eta$ cross section + below $\sqrt{s}=2$ GeV}", + journal = "Phys. Rev.", + volume = "D94", + year = "2016", + number = "9", + pages = "092002", + doi = "10.1103/PhysRevD.94.092002", + eprint = "1607.00371", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1607.00371;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2016_I1473343.plot b/analyses/pluginNovosibirsk/SND_2016_I1473343.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1473343.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2016_I1473343/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\omega)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta\omega)$/nb +ConnectGaps=1 +LogY=0 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2016_I1473343.yoda b/analyses/pluginNovosibirsk/SND_2016_I1473343.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1473343.yoda @@ -0,0 +1,21 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1473343/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2016_I1473343/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.36700 0.02700 0.02700 -7.00000e-02 5.00000e-02 5.00000e-02 +1.41900 0.02500 0.02500 1.90000e-01 6.00000e-02 6.00000e-02 +1.46900 0.02500 0.02500 3.50000e-01 1.00000e-01 1.00000e-01 +1.51900 0.02500 0.02500 1.50000e-01 2.14709e-01 1.00000e-01 +1.56900 0.02500 0.02500 8.70000e-01 1.10454e-01 1.10454e-01 +1.61900 0.02500 0.02500 1.26000e+00 2.15870e-01 2.10238e-01 +1.66900 0.02500 0.02500 2.01000e+00 2.23607e-01 2.02237e-01 +1.71900 0.02500 0.02500 8.70000e-01 2.34307e-01 1.81108e-01 +1.76900 0.02500 0.02500 4.40000e-01 1.74642e-01 1.72627e-01 +1.81900 0.02500 0.02500 1.70000e-01 1.43178e-01 1.41421e-01 +1.86900 0.02500 0.02500 -3.00000e-02 1.51327e-01 1.50000e-01 +1.91900 0.02500 0.02500 -6.00000e-02 1.43178e-01 1.40357e-01 +1.97200 0.02800 0.02800 -6.00000e-02 1.72627e-01 1.70294e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2016_I1484677.cc b/analyses/pluginNovosibirsk/SND_2016_I1484677.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1484677.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2016_I1484677 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2016_I1484677); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nkaon = bookCounter("TMP/kaon"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::KPLUS) vetoEvent; + } + _nkaon->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nkaon->val(); + double error = _nkaon->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nkaon; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2016_I1484677); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2016_I1484677.info b/analyses/pluginNovosibirsk/SND_2016_I1484677.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1484677.info @@ -0,0 +1,34 @@ +Name: SND_2016_I1484677 +Year: 2016 +Summary: Cross section for $e^+e^-\to K^+K^-$ between 1.05 and 2 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 1484677 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D94 (2016) no.11, 112006 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-$ at energies between 1.05 and 2 GeV' +Keywords: +BibKey: Achasov:2016lbc +BibTeX: '@article{Achasov:2016lbc, + author = "Achasov, M. N. and others", + title = "{Measurement of the $\mathbf{e^+e^-\to K^+K^-}$ cross + section in the energy range $\mathbf{\sqrt{s}=1.05-2.0}$ + GeV}", + journal = "Phys. Rev.", + volume = "D94", + year = "2016", + number = "11", + pages = "112006", + doi = "10.1103/PhysRevD.94.112006", + eprint = "1608.08757", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1608.08757;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2016_I1484677.plot b/analyses/pluginNovosibirsk/SND_2016_I1484677.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1484677.plot @@ -0,0 +1,12 @@ +BEGIN PLOT /SND_2016_I1484677/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /SND_2016_I1484677/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2016_I1484677.yoda b/analyses/pluginNovosibirsk/SND_2016_I1484677.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1484677.yoda @@ -0,0 +1,72 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1484677/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2016_I1484677/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.04700 0.00000 0.00000 3.62430e+01 7.56508e-01 7.56508e-01 +1.07500 0.00000 0.00000 1.84830e+01 3.88104e-01 3.88104e-01 +1.09700 0.00000 0.00000 1.41840e+01 3.05601e-01 3.05601e-01 +1.12400 0.00000 0.00000 1.13070e+01 2.47407e-01 2.47407e-01 +1.15100 0.00000 0.00000 9.41500e+00 2.27482e-01 2.27482e-01 +1.17400 0.00000 0.00000 9.14800e+00 2.08331e-01 2.08331e-01 +1.19600 0.00000 0.00000 7.73700e+00 1.83330e-01 1.83330e-01 +1.22300 0.00000 0.00000 7.26900e+00 2.03571e-01 2.03571e-01 +1.24500 0.00000 0.00000 6.62400e+00 2.08406e-01 2.08406e-01 +1.27300 0.00000 0.00000 6.51800e+00 1.91888e-01 1.91888e-01 +1.29500 0.00000 0.00000 5.96400e+00 2.01040e-01 2.01040e-01 +1.32300 0.00000 0.00000 5.71800e+00 1.72177e-01 1.72177e-01 +1.34400 0.00000 0.00000 5.16000e+00 1.63294e-01 1.63294e-01 +1.37400 0.00000 0.00000 5.30800e+00 1.50360e-01 1.50360e-01 +1.39400 0.00000 0.00000 5.00100e+00 1.47139e-01 1.47139e-01 +1.42300 0.00000 0.00000 4.57900e+00 1.36418e-01 1.36418e-01 +1.44300 0.00000 0.00000 4.25400e+00 1.48385e-01 1.48385e-01 +1.47100 0.00000 0.00000 4.09300e+00 1.24326e-01 1.24326e-01 +1.49400 0.00000 0.00000 3.64600e+00 1.20420e-01 1.20420e-01 +1.52200 0.00000 0.00000 3.67900e+00 1.33701e-01 1.33701e-01 +1.54300 0.00000 0.00000 3.38200e+00 1.30035e-01 1.30035e-01 +1.57200 0.00000 0.00000 3.51800e+00 1.30173e-01 1.30173e-01 +1.59400 0.00000 0.00000 3.50700e+00 1.59101e-01 1.59101e-01 +1.62300 0.00000 0.00000 3.02200e+00 1.10693e-01 1.10693e-01 +1.64300 0.00000 0.00000 2.81500e+00 1.12947e-01 1.12947e-01 +1.66900 0.00000 0.00000 2.15500e+00 9.61353e-02 9.61353e-02 +1.69300 0.00000 0.00000 1.57000e+00 8.42021e-02 8.42021e-02 +1.72300 0.00000 0.00000 9.68000e-01 7.18401e-02 7.18401e-02 +1.74200 0.00000 0.00000 6.33000e-01 5.26308e-02 5.26308e-02 +1.77400 0.00000 0.00000 3.10000e-01 3.71080e-02 3.71080e-02 +1.79300 0.00000 0.00000 1.70000e-01 3.59026e-02 3.59026e-02 +1.82600 0.00000 0.00000 2.15000e-01 3.60555e-02 3.60555e-02 +1.84900 0.00000 0.00000 1.71000e-01 4.29418e-02 4.29418e-02 +1.87100 0.00000 0.00000 2.91000e-01 3.98121e-02 3.98121e-02 +1.89300 0.00000 0.00000 3.45000e-01 4.30813e-02 4.30813e-02 +1.90100 0.00000 0.00000 3.43000e-01 5.06952e-02 5.06952e-02 +1.92700 0.00000 0.00000 3.16000e-01 4.42719e-02 4.42719e-02 +1.95300 0.00000 0.00000 3.57000e-01 6.28172e-02 6.28172e-02 +1.97800 0.00000 0.00000 3.32000e-01 5.75674e-02 5.75674e-02 +2.00500 0.00000 0.00000 3.67000e-01 5.05964e-02 5.05964e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1484677/d02-x01-y01 +IsRef: 1 +Path: /REF/SND_2016_I1484677/d02-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.27700 0.00000 0.00000 6.35800e+00 1.76604e-01 1.76604e-01 +1.35700 0.00000 0.00000 5.33900e+00 1.51013e-01 1.51013e-01 +1.43500 0.00000 0.00000 4.11400e+00 1.20673e-01 1.20673e-01 +1.51500 0.00000 0.00000 3.57400e+00 1.11517e-01 1.11517e-01 +1.59500 0.00000 0.00000 3.30200e+00 1.05475e-01 1.05475e-01 +1.67400 0.00000 0.00000 1.77000e+00 6.93181e-02 6.93181e-02 +1.71600 0.00000 0.00000 1.11500e+00 7.90569e-02 7.90569e-02 +1.75800 0.00000 0.00000 5.03000e-01 4.04969e-02 4.04969e-02 +1.79800 0.00000 0.00000 1.87000e-01 2.96816e-02 2.96816e-02 +1.84000 0.00000 0.00000 2.93000e-01 4.33244e-02 4.33244e-02 +1.87400 0.00000 0.00000 2.76000e-01 3.66742e-02 3.66742e-02 +1.90300 0.00000 0.00000 2.87000e-01 3.71214e-02 3.71214e-02 +1.92600 0.00000 0.00000 3.67000e-01 4.68188e-02 4.68188e-02 +1.94500 0.00000 0.00000 2.63000e-01 3.71618e-02 3.71618e-02 +1.96700 0.00000 0.00000 3.31000e-01 4.36578e-02 4.36578e-02 +1.98900 0.00000 0.00000 3.46000e-01 4.83839e-02 4.83839e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2016_I1489182.cc b/analyses/pluginNovosibirsk/SND_2016_I1489182.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1489182.cc @@ -0,0 +1,111 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2016_I1489182 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2016_I1489182); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numOmegaPi = bookCounter("TMP/OmegaPi"); + } + + + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]+=1; + ++ncount; + } + else + findChildren(child,nRes,ncount); + } + } + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // three particles (pi0 pi0 gamma) + if(ntotal!=3) vetoEvent; + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==223) { + map nRes; + int ncount(0); + findChildren(p,nRes,ncount); + // only omega to pi0 gamma mode + if(ncount!=2) continue; + if(nRes[111]!=1 || nRes[22]!=1) continue; + // omega pi0 + if(nCount[111]-nRes[111]==1) + _numOmegaPi->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + double sigma = _numOmegaPi->val(); + double error = _numOmegaPi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + /// @name Histograms + //@{ + CounterPtr _numOmegaPi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2016_I1489182); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2016_I1489182.info b/analyses/pluginNovosibirsk/SND_2016_I1489182.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1489182.info @@ -0,0 +1,35 @@ +Name: SND_2016_I1489182 +Year: 2016 +Summary: Cross section for $e^+e^-\to\omega\pi^0\to\pi^0\pi^0\gamma$ between 1.05 and 2 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 1489182 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D94 (2016) no.11, 112001 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to\omega\pi^0\to\pi^0\pi^0\gamma$ at energies between 1.05 and 2 GeV.' +Keywords: +BibKey: Achasov:2016zvn +BibTeX: '@article{Achasov:2016zvn, + author = "Achasov, M. N. and others", + title = "{Updated measurement of the $e^+e^- \to \omega \pi^0 \to + \pi^0\pi^0\gamma$ cross section with the SND detector}", + journal = "Phys. Rev.", + volume = "D94", + year = "2016", + number = "11", + pages = "112001", + doi = "10.1103/PhysRevD.94.112001", + eprint = "1610.00235", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1610.00235;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2016_I1489182.plot b/analyses/pluginNovosibirsk/SND_2016_I1489182.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1489182.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2016_I1489182/d01-x01-y01 +Title=$\sigma(e^+e^-\to \omega\pi^0\to \pi^0\pi^0\gamma)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \omega\pi^0\to \pi^0\pi^0\gamma)$/nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2016_I1489182.yoda b/analyses/pluginNovosibirsk/SND_2016_I1489182.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2016_I1489182.yoda @@ -0,0 +1,64 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2016_I1489182/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2016_I1489182/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1047.00000 6.00000 6.00000 0.95000 0.11000 0.11000 +1075.00000 6.00000 6.00000 1.04000 0.09000 0.09000 +1097.00000 6.00000 6.00000 1.08000 0.07000 0.07000 +1124.00000 6.00000 6.00000 1.26000 0.11000 0.11000 +1151.00000 6.00000 6.00000 1.30000 0.10000 0.10000 +1174.00000 6.00000 6.00000 1.29000 0.12000 0.12000 +1196.00000 6.00000 6.00000 1.39000 0.07000 0.07000 +1223.00000 6.00000 6.00000 1.33000 0.11000 0.11000 +1245.00000 6.00000 6.00000 1.25000 0.12000 0.12000 +1273.00000 6.00000 2.00000 1.53000 0.13000 0.13000 +1277.00000 2.00000 2.00000 1.38000 0.09000 0.09000 +1295.00000 6.00000 6.00000 1.56000 0.07000 0.07000 +1323.00000 6.00000 6.00000 1.54000 0.12000 0.12000 +1344.00000 6.00000 6.00000 1.50000 0.13000 0.13000 +1357.00000 2.00000 2.00000 1.60000 0.11000 0.11000 +1374.00000 6.00000 6.00000 1.55000 0.12000 0.12000 +1394.00000 6.00000 6.00000 1.61000 0.09000 0.09000 +1423.00000 6.00000 6.00000 1.78000 0.10000 0.10000 +1435.00000 2.00000 2.00000 1.67000 0.09000 0.09000 +1443.00000 6.00000 6.00000 1.47000 0.12000 0.12000 +1471.00000 6.00000 6.00000 1.37000 0.10000 0.10000 +1494.00000 6.00000 6.00000 1.42000 0.06000 0.06000 +1515.00000 2.00000 2.00000 1.21000 0.08000 0.08000 +1522.00000 5.00000 6.00000 1.48000 0.10000 0.10000 +1543.00000 6.00000 6.00000 1.13000 0.08000 0.08000 +1572.00000 6.00000 6.00000 0.93000 0.08000 0.08000 +1594.00000 6.00000 0.50000 0.80000 0.06000 0.06000 +1595.00000 0.50000 2.00000 0.77000 0.07000 0.07000 +1623.00000 6.00000 6.00000 0.70000 0.08000 0.08000 +1643.00000 6.00000 6.00000 0.54000 0.07000 0.07000 +1669.00000 6.00000 3.00000 0.45000 0.07000 0.07000 +1674.00000 2.00000 2.00000 0.41000 0.04000 0.04000 +1693.00000 6.00000 6.00000 0.35000 0.04000 0.04000 +1716.00000 2.00000 2.00000 0.30000 0.05000 0.05000 +1723.00000 5.00000 6.00000 0.17000 0.04000 0.04000 +1742.00000 6.00000 6.00000 0.17000 0.04000 0.04000 +1758.00000 2.00000 2.00000 0.17000 0.04000 0.04000 +1774.00000 6.00000 6.00000 0.20000 0.04000 0.04000 +1793.00000 6.00000 3.00000 0.19000 0.03000 0.03000 +1798.00000 2.00000 2.00000 0.14000 0.03000 0.03000 +1826.00000 6.00000 6.00000 0.09000 0.03000 0.03000 +1840.00000 2.00000 2.00000 0.12000 0.03000 0.03000 +1849.00000 6.00000 6.00000 0.07000 0.04000 0.04000 +1871.00000 6.00000 1.50000 0.10000 0.03000 0.03000 +1874.00000 1.50000 2.00000 0.12000 0.02000 0.02000 +1893.00000 6.00000 4.00000 0.13000 0.03000 0.03000 +1901.00000 4.00000 1.00000 0.06000 0.02000 0.02000 +1903.00000 1.00000 2.00000 0.08000 0.03000 0.03000 +1926.00000 2.00000 0.50000 0.08000 0.03000 0.03000 +1927.00000 0.50000 6.00000 0.10000 0.03000 0.03000 +1945.00000 2.00000 2.00000 0.06000 0.02000 0.02000 +1953.00000 6.00000 6.00000 0.03000 0.03000 0.03000 +1967.00000 2.00000 2.00000 0.06000 0.03000 0.03000 +1978.00000 6.00000 6.00000 0.05000 0.05000 0.02000 +1989.00000 2.00000 2.00000 0.06000 0.02000 0.02000 +2005.00000 6.00000 6.00000 0.07000 0.03000 0.03000 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2018_I1637194.cc b/analyses/pluginNovosibirsk/SND_2018_I1637194.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1637194.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2018_I1637194 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2018_I1637194); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + _nKKpi= bookCounter( "/TMP/nKKpi" ); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + if(ntotal==3 && nCount[130]==1 && nCount[310]==1 && nCount[111] ==1) + _nKKpi->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nKKpi->val(); + double error = _nKKpi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nKKpi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2018_I1637194); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2018_I1637194.info b/analyses/pluginNovosibirsk/SND_2018_I1637194.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1637194.info @@ -0,0 +1,35 @@ +Name: SND_2018_I1637194 +Year: 2018 +Summary: Cross section for $e^+e^-\to$ $K^0_SK^0_L\pi^0$ for energies between 1.3 and 2.0 +Experiment: SND +Collider: VEPP-2M +InspireID: 1637194 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D97 (2018) no.3, 032011 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to$ $K^0_SK^0_L\pi^0$ for energies from 1.3 to 2.0 GeV.' +Keywords: +BibKey: Achasov:2017vaq +BibTeX: '@article{Achasov:2017vaq, + author = "Achasov, M. N. and others", + title = "{Measurement of the $\mathbf{e^+e^- \rightarrow K_S K_L + \pi^0}$ cross section in the energy range + $\mathbf{\sqrt{s}=1.3-2.0}$ GeV}", + journal = "Phys. Rev.", + volume = "D97", + year = "2018", + number = "3", + pages = "032011", + doi = "10.1103/PhysRevD.97.032011", + eprint = "1711.07143", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1711.07143;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2018_I1637194.plot b/analyses/pluginNovosibirsk/SND_2018_I1637194.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1637194.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /SND_2018_I1637194/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^0_L \pi^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^0_SK^0_L \pi^0)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2018_I1637194.yoda b/analyses/pluginNovosibirsk/SND_2018_I1637194.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1637194.yoda @@ -0,0 +1,23 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2018_I1637194/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2018_I1637194/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.32500 0.02500 0.02500 1.40000e-01 5.00000e-02 5.00000e-02 +1.36750 0.00750 0.00750 1.40000e-01 6.00000e-02 6.00000e-02 +1.42000 0.02000 0.02000 5.20000e-01 8.00000e-02 8.00000e-02 +1.46250 0.01250 0.01250 9.00000e-01 1.60000e-01 1.60000e-01 +1.50000 0.00000 0.00000 1.35000e+00 1.30000e-01 1.30000e-01 +1.52250 0.00250 0.00250 1.49000e+00 1.80000e-01 1.80000e-01 +1.56250 0.01250 0.01250 2.48000e+00 2.40000e-01 2.40000e-01 +1.62500 0.02500 0.02500 2.80000e+00 1.90000e-01 1.90000e-01 +1.68750 0.01250 0.01250 2.85000e+00 2.00000e-01 2.00000e-01 +1.73500 0.01500 0.01500 2.30000e+00 2.10000e-01 2.10000e-01 +1.78000 0.02000 0.02000 1.81000e+00 1.50000e-01 1.50000e-01 +1.83750 0.01250 0.01250 1.00000e+00 2.30000e-01 2.30000e-01 +1.88500 0.01500 0.01500 5.50000e-01 9.00000e-02 9.00000e-02 +1.93500 0.01500 0.01500 3.90000e-01 1.20000e-01 1.20000e-01 +1.98000 0.02000 0.02000 4.10000e-01 1.50000e-01 1.50000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2018_I1638368.cc b/analyses/pluginNovosibirsk/SND_2018_I1638368.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1638368.cc @@ -0,0 +1,120 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2018_I1638368 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2018_I1638368); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaPiPi = bookCounter("TMP/EtaPiPi"); + } + + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaPiPi->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _numEtaPiPi->val(); + double error = _numEtaPiPi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numEtaPiPi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2018_I1638368); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2018_I1638368.info b/analyses/pluginNovosibirsk/SND_2018_I1638368.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1638368.info @@ -0,0 +1,35 @@ +Name: SND_2018_I1638368 +Year: 2018 +Summary: Cross section for $e^+e^-\to\eta\pi^+\pi^-$ between 1.08 and 2 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 1638368 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D97 (2018) no.1, 012008 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to\eta\pi^+\pi^-$ at energies between 1.08 and 2 GeV.' +Keywords: +BibKey: Achasov:2017kqm +BibTeX: '@article{Achasov:2017kqm, + author = "Achasov, M. N. and others", + title = "{Measurement of the $e^+e^- \to \eta\pi^+\pi^-$ cross + section with the SND detector at the VEPP-2000 collider}", + journal = "Phys. Rev.", + volume = "D97", + year = "2018", + number = "1", + pages = "012008", + doi = "10.1103/PhysRevD.97.012008", + eprint = "1711.08862", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1711.08862;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2018_I1638368.plot b/analyses/pluginNovosibirsk/SND_2018_I1638368.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1638368.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /SND_2018_I1638368/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$/nb +LogY=0 +LegendXPos=0.7 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2018_I1638368.yoda b/analyses/pluginNovosibirsk/SND_2018_I1638368.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1638368.yoda @@ -0,0 +1,47 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2018_I1638368/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2018_I1638368/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.07500 0.00000 0.00000 3.70000e-01 2.50000e-01 2.50000e-01 +1.09700 0.00000 0.00000 9.00000e-02 1.50000e-01 1.50000e-01 +1.12400 0.00000 0.00000 1.30000e-01 2.00000e-01 2.00000e-01 +1.15100 0.00000 0.00000 1.70000e-01 1.60000e-01 1.60000e-01 +1.17400 0.00000 0.00000 8.00000e-02 1.90000e-01 1.90000e-01 +1.19600 0.00000 0.00000 2.10000e-01 1.60000e-01 1.60000e-01 +1.22300 0.00000 0.00000 3.30000e-01 1.30000e-01 1.30000e-01 +1.24500 0.00000 0.00000 1.50000e-01 1.20000e-01 1.20000e-01 +1.27500 0.00000 0.00000 3.30000e-01 9.00000e-02 9.00000e-02 +1.29500 0.00000 0.00000 5.10000e-01 1.50000e-01 1.50000e-01 +1.32300 0.00000 0.00000 7.10000e-01 1.60000e-01 1.60000e-01 +1.35100 0.00000 0.00000 1.02000e+00 1.20000e-01 1.20000e-01 +1.37400 0.00000 0.00000 1.22000e+00 1.90000e-01 1.90000e-01 +1.39400 0.00000 0.00000 1.86000e+00 2.00000e-01 2.00000e-01 +1.42300 0.00000 0.00000 2.06000e+00 2.10000e-01 2.10000e-01 +1.43800 0.00000 0.00000 3.03000e+00 1.60000e-01 1.60000e-01 +1.47100 0.00000 0.00000 3.29000e+00 2.50000e-01 2.50000e-01 +1.49400 0.00000 0.00000 3.82000e+00 2.40000e-01 2.40000e-01 +1.51700 0.00000 0.00000 4.44000e+00 1.90000e-01 1.90000e-01 +1.54300 0.00000 0.00000 4.55000e+00 2.80000e-01 2.80000e-01 +1.57200 0.00000 0.00000 3.94000e+00 3.00000e-01 3.00000e-01 +1.59400 0.00000 0.00000 3.34000e+00 3.10000e-01 3.10000e-01 +1.62300 0.00000 0.00000 3.12000e+00 2.80000e-01 2.80000e-01 +1.64300 0.00000 0.00000 2.45000e+00 2.80000e-01 2.80000e-01 +1.67200 0.00000 0.00000 2.30000e+00 1.60000e-01 1.60000e-01 +1.69300 0.00000 0.00000 2.67000e+00 2.70000e-01 2.70000e-01 +1.72000 0.00000 0.00000 2.23000e+00 1.70000e-01 1.70000e-01 +1.75100 0.00000 0.00000 2.36000e+00 1.70000e-01 1.70000e-01 +1.77400 0.00000 0.00000 1.96000e+00 2.50000e-01 2.50000e-01 +1.79700 0.00000 0.00000 2.00000e+00 1.60000e-01 1.60000e-01 +1.82600 0.00000 0.00000 1.44000e+00 2.20000e-01 2.20000e-01 +1.84300 0.00000 0.00000 1.31000e+00 1.40000e-01 1.40000e-01 +1.87300 0.00000 0.00000 9.70000e-01 1.30000e-01 1.30000e-01 +1.90000 0.00000 0.00000 7.90000e-01 1.00000e-01 1.00000e-01 +1.92700 0.00000 0.00000 7.60000e-01 1.30000e-01 1.30000e-01 +1.94700 0.00000 0.00000 7.10000e-01 1.20000e-01 1.20000e-01 +1.96700 0.00000 0.00000 7.40000e-01 1.80000e-01 1.80000e-01 +1.98400 0.00000 0.00000 7.40000e-01 1.50000e-01 1.50000e-01 +2.00500 0.00000 0.00000 7.80000e-01 2.20000e-01 2.20000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2018_I1693737.cc b/analyses/pluginNovosibirsk/SND_2018_I1693737.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1693737.cc @@ -0,0 +1,115 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2018_I1693737 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2018_I1693737); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nKKEta= bookCounter("/TMP/nKKEta"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + if(p.pdgId()!=221) continue; + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==321) { + if(val.second!=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nKKEta->fill(event.weight()); + break; + } + } + } + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nKKEta->val(); + double error = _nKKEta->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nKKEta; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2018_I1693737); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2018_I1693737.info b/analyses/pluginNovosibirsk/SND_2018_I1693737.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1693737.info @@ -0,0 +1,34 @@ +Name: SND_2018_I1693737 +Year: 2018 +Summary: Cross section for $e^+e^-\to\eta K^+K^-$ for energies below 2 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 1693737 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Atom.Nucl. 81 (2018) no.2, 205-213 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\eta K^+K^-$ for energies below 2 GeV' +Keywords: [] +BibKey: Achasov:2018ygm +BibTeX: '%%% contains utf-8, see: http://inspirehep.net/info/faq/general#utf8 +%%% add \usepackage[utf8]{inputenc} to your latex preamble + +@article{Achasov:2018ygm, + author = "Achasov, M. N. and others", + title = "{Measurement of the $e^+e^−\to\eta K^+K^−$ Cross + Section by Means of the SND Detector}", + journal = "Phys. Atom. Nucl.", + volume = "81", + year = "2018", + number = "2", + pages = "205-213", + doi = "10.1134/S1063778818020023", + note = "[Yad. Fiz.81,no.2,195(2018)]", + SLACcitation = "%%CITATION = PANUE,81,205;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2018_I1693737.plot b/analyses/pluginNovosibirsk/SND_2018_I1693737.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1693737.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2018_I1693737/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \eta K^+K^-)$/nb +ConnectGaps=1 +LogY=0 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2018_I1693737.yoda b/analyses/pluginNovosibirsk/SND_2018_I1693737.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1693737.yoda @@ -0,0 +1,20 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2018_I1693737/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2018_I1693737/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.59000 0.03000 0.03000 0.00000e+00 7.07107e-02 9.05539e-02 +1.64000 0.02000 0.02000 4.10000e-01 1.31529e-01 1.31529e-01 +1.68000 0.02000 0.02000 1.09000e+00 1.70880e-01 1.70880e-01 +1.72000 0.02000 0.02000 9.30000e-01 1.58114e-01 1.58114e-01 +1.75500 0.01500 0.01500 9.40000e-01 2.06155e-01 2.06155e-01 +1.79500 0.02500 0.02500 5.80000e-01 1.20830e-01 1.20830e-01 +1.83500 0.01500 0.01500 4.50000e-01 1.26491e-01 1.26491e-01 +1.87000 0.02000 0.02000 3.10000e-01 9.48683e-02 9.48683e-02 +1.89500 0.00500 0.00500 3.30000e-01 1.33417e-01 1.33417e-01 +1.92500 0.02500 0.02500 3.70000e-01 1.04403e-01 1.04403e-01 +1.96000 0.01000 0.01000 7.00000e-02 7.07107e-02 5.09902e-02 +1.98500 0.01500 0.01500 2.30000e-01 1.01119e-01 1.01119e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginNovosibirsk/SND_2018_I1694988.cc b/analyses/pluginNovosibirsk/SND_2018_I1694988.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1694988.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class SND_2018_I1694988 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(SND_2018_I1694988); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + _numPi0Gamma = bookCounter("TMP/Pi0Gamma"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && nCount[22]==1 && nCount[111]==1) + _numPi0Gamma->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _numPi0Gamma->val(); + double error = _numPi0Gamma->err(); + sigma *= crossSection()/ sumOfWeights() /picobarn; + error *= crossSection()/ sumOfWeights() /picobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numPi0Gamma; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(SND_2018_I1694988); + + +} diff --git a/analyses/pluginNovosibirsk/SND_2018_I1694988.info b/analyses/pluginNovosibirsk/SND_2018_I1694988.info new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1694988.info @@ -0,0 +1,28 @@ +Name: SND_2018_I1694988 +Year: 2018 +Summary: Cross section for $e^+e^-\to\pi\gamma$ for energies between 1.075 GeV and 2 GeV +Experiment: SND +Collider: VEPP-2M +InspireID: 1694988 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - arXiv:1809.07631 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Cross section for $e^+e^-\to\pi\gamma$ for energies between 1.075 GeV and 2 GeV ' +Keywords: [] +BibKey: Achasov:2018ujw +BibTeX: '@article{Achasov:2018ujw, + author = "Achasov, M. N. and others", + title = "{Measurement of the $e^+e^- \to \pi^0\gamma$ cross + section in the energy range 1.075--2 GeV at SND}", + year = "2018", + eprint = "1809.07631", + archivePrefix = "arXiv", + primaryClass = "hep-ex", + SLACcitation = "%%CITATION = ARXIV:1809.07631;%%" +}' diff --git a/analyses/pluginNovosibirsk/SND_2018_I1694988.plot b/analyses/pluginNovosibirsk/SND_2018_I1694988.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1694988.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /SND_2018_I1694988/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^0\gamma)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^0\gamma)$/pb +LogY=1 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginNovosibirsk/SND_2018_I1694988.yoda b/analyses/pluginNovosibirsk/SND_2018_I1694988.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginNovosibirsk/SND_2018_I1694988.yoda @@ -0,0 +1,19 @@ +BEGIN YODA_SCATTER2D_V2 /REF/SND_2018_I1694988/d01-x01-y01 +IsRef: 1 +Path: /REF/SND_2018_I1694988/d01-x01-y01 +Title: +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1075.00000 0.00000 0.00000 9.30000e+01 4.51774e+01 4.51774e+01 +1119.00000 0.00000 0.00000 4.80000e+01 2.91548e+01 2.91548e+01 +1200.00000 0.00000 0.00000 6.00000e+01 2.60768e+01 2.60768e+01 +1284.00000 0.00000 0.00000 5.00000e+01 2.10950e+01 2.10950e+01 +1353.00000 0.00000 0.00000 2.30000e+01 1.90263e+01 1.90263e+01 +1425.00000 0.00000 0.00000 -1.30000e+01 1.50333e+01 1.50333e+01 +1509.00000 0.00000 0.00000 -1.10000e+01 1.30384e+01 1.30384e+01 +1607.00000 0.00000 0.00000 1.20000e+01 1.61245e+01 1.61245e+01 +1705.00000 0.00000 0.00000 -1.00000e+00 1.31529e+01 1.31529e+01 +1804.00000 0.00000 0.00000 4.00000e+00 1.50333e+01 1.50333e+01 +1926.00000 0.00000 0.00000 -8.00000e+00 1.30384e+01 1.30384e+01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1978_I134061.cc b/analyses/pluginOrsay/DM1_1978_I134061.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1978_I134061.cc @@ -0,0 +1,79 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1978_I134061 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1978_I134061); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1978_I134061); + + +} diff --git a/analyses/pluginOrsay/DM1_1978_I134061.info b/analyses/pluginOrsay/DM1_1978_I134061.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1978_I134061.info @@ -0,0 +1,28 @@ +Name: DM1_1978_I134061 +Year: 1978 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ between 0.483 and 1.096 GeV +Experiment: DM1 +Collider: ACO +InspireID: 134061 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B76 (1978) 512-516, 1978 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies between 0.483 and 1.096 GeV. Useful for comparing models of the pion form factor.' +Keywords: +BibKey: Quenzer:1978qt +BibTeX: '@article{Quenzer:1978qt, + author = "Quenzer, A. and others", + title = "{Pion Form-Factor from 480-MeV to 1100-MeV}", + journal = "Phys. Lett.", + volume = "76B", + year = "1978", + pages = "512-516", + doi = "10.1016/0370-2693(78)90918-8", + SLACcitation = "%%CITATION = PHLTA,76B,512;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1978_I134061.plot b/analyses/pluginOrsay/DM1_1978_I134061.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1978_I134061.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /DM1_1978_I134061/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +LogY=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1978_I134061.yoda b/analyses/pluginOrsay/DM1_1978_I134061.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1978_I134061.yoda @@ -0,0 +1,48 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1978_I134061/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1978_I134061/d01-x01-y01 +Title: doi:10.17182/hepdata.27443.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.830000e+02 0.000000e+00 0.000000e+00 1.570000e+02 2.325790e+01 2.325790e+01 +6.024000e+02 0.000000e+00 0.000000e+00 3.410000e+02 3.189483e+01 3.189483e+01 +7.000000e+02 0.000000e+00 0.000000e+00 8.150000e+02 6.742763e+01 6.742763e+01 +7.502000e+02 0.000000e+00 0.000000e+00 1.114000e+03 7.795282e+01 7.795282e+01 +7.732000e+02 0.000000e+00 0.000000e+00 1.300000e+03 9.538847e+01 9.538847e+01 +7.782000e+02 0.000000e+00 0.000000e+00 1.295000e+03 9.535555e+01 9.535555e+01 +7.832000e+02 0.000000e+00 0.000000e+00 9.340000e+02 6.817052e+01 6.817052e+01 +7.882000e+02 0.000000e+00 0.000000e+00 8.390000e+02 6.564829e+01 6.564829e+01 +7.932000e+02 0.000000e+00 0.000000e+00 7.080000e+02 5.908986e+01 5.908986e+01 +8.432000e+02 0.000000e+00 0.000000e+00 3.990000e+02 3.705473e+01 3.705473e+01 +8.932000e+02 0.000000e+00 0.000000e+00 2.060000e+02 2.050705e+01 2.050705e+01 +9.630000e+02 0.000000e+00 0.000000e+00 6.900000e+01 1.011456e+01 1.011456e+01 +9.850000e+02 0.000000e+00 0.000000e+00 5.440000e+01 1.056799e+01 1.056799e+01 +1.003000e+03 0.000000e+00 0.000000e+00 6.470000e+01 9.902831e+00 9.902831e+00 +1.053000e+03 0.000000e+00 0.000000e+00 3.400000e+01 1.002794e+01 1.002794e+01 +1.096000e+03 0.000000e+00 0.000000e+00 2.750000e+01 1.111648e+01 1.111648e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1978_I134061/d01-x01-y02 +IsRef: 1 +Path: /REF/DM1_1978_I134061/d01-x01-y02 +Title: doi:10.17182/hepdata.27443.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.830000e+02 0.000000e+00 0.000000e+00 3.040000e+00 4.549428e-01 4.549428e-01 +6.024000e+02 0.000000e+00 0.000000e+00 8.070000e+00 7.707272e-01 7.707272e-01 +7.000000e+02 0.000000e+00 0.000000e+00 2.380000e+01 1.970826e+00 1.970826e+00 +7.502000e+02 0.000000e+00 0.000000e+00 3.610000e+01 2.527994e+00 2.527994e+00 +7.732000e+02 0.000000e+00 0.000000e+00 4.400000e+01 3.152305e+00 3.152305e+00 +7.782000e+02 0.000000e+00 0.000000e+00 4.440000e+01 3.250252e+00 3.250252e+00 +7.832000e+02 0.000000e+00 0.000000e+00 3.230000e+01 2.311915e+00 2.311915e+00 +7.882000e+02 0.000000e+00 0.000000e+00 2.930000e+01 2.388621e+00 2.388621e+00 +7.932000e+02 0.000000e+00 0.000000e+00 2.500000e+01 2.170829e+00 2.170829e+00 +8.432000e+02 0.000000e+00 0.000000e+00 1.560000e+01 1.538761e+00 1.538761e+00 +8.932000e+02 0.000000e+00 0.000000e+00 8.800000e+00 8.912805e-01 8.912805e-01 +9.630000e+02 0.000000e+00 0.000000e+00 3.360000e+00 4.757774e-01 4.757774e-01 +9.850000e+02 0.000000e+00 0.000000e+00 2.760000e+00 5.334669e-01 5.334669e-01 +1.003000e+03 0.000000e+00 0.000000e+00 3.380000e+00 5.153925e-01 5.153925e-01 +1.053000e+03 0.000000e+00 0.000000e+00 1.930000e+00 5.217306e-01 5.217306e-01 +1.096000e+03 0.000000e+00 0.000000e+00 1.680000e+00 6.710187e-01 6.710187e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1979_I132828.cc b/analyses/pluginOrsay/DM1_1979_I132828.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1979_I132828.cc @@ -0,0 +1,79 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1979_I132828 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1979_I132828); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // Book histograms + _npion = bookCounter("TMP/pion"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=4) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1979_I132828); + + +} diff --git a/analyses/pluginOrsay/DM1_1979_I132828.info b/analyses/pluginOrsay/DM1_1979_I132828.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1979_I132828.info @@ -0,0 +1,32 @@ +Name: DM1_1979_I132828 +Year: 1979 +Summary: Cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ between 0.89 and 1.1 GeV +Experiment: DM1 +Collider: ACO +InspireID: 132828 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B81 (1979) 389-392, 1979 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ between 0.89 and 1.1 GeV' +Keywords: +BibKey: Cordier:1978yp +BibTeX: '@article{Cordier:1978yp, + author = "Cordier, A. and others", + title = "{Cross-section of the Reaction $e^+ e^- \to \pi^+ \pi^- + \pi^+ \pi^-$ for Center-of-mass Energies From 890-{MeV} to + 1100-{MeV}}", + journal = "Phys. Lett.", + volume = "81B", + year = "1979", + pages = "389-392", + doi = "10.1016/0370-2693(79)90360-5", + reportNumber = "LAL-78/31", + SLACcitation = "%%CITATION = PHLTA,81B,389;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1979_I132828.plot b/analyses/pluginOrsay/DM1_1979_I132828.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1979_I132828.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /DM1_1979_I132828/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1979_I132828.yoda b/analyses/pluginOrsay/DM1_1979_I132828.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1979_I132828.yoda @@ -0,0 +1,12 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1979_I132828/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1979_I132828/d01-x01-y01 +Title: doi:10.17182/hepdata.27360.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.825000e+02 1.950000e+01 1.950000e+01 1.000000e+00 6.000000e-01 6.000000e-01 +1.101550e+03 7.500000e+00 7.500000e+00 2.400000e+00 9.000000e-01 9.000000e-01 +1.056000e+03 0.000000e+00 0.000000e+00 4.400000e+00 1.600000e+00 1.600000e+00 +1.098500e+03 0.000000e+00 0.000000e+00 3.900000e+00 9.000000e-01 9.000000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1979_I141565.cc b/analyses/pluginOrsay/DM1_1979_I141565.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1979_I141565.cc @@ -0,0 +1,80 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1979_I141565 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1979_I141565); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + _nProton= bookCounter( "/TMP/nProton" ); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + // total hadronic and muonic cross sections + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && nCount[2212]==1 && nCount[-2212]==1) + _nProton->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sigma = _nProton->val()*fact; + double error = _nProton->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nProton; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1979_I141565); + + +} diff --git a/analyses/pluginOrsay/DM1_1979_I141565.info b/analyses/pluginOrsay/DM1_1979_I141565.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1979_I141565.info @@ -0,0 +1,30 @@ +Name: DM1_1979_I141565 +Year: 1979 +Summary: Cross section for $e^+e^-\to p\bar{p}$ between 1.925 and 2.18 GeV +Experiment: DM1 +Collider: DCI +InspireID: 141565 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B86 (1979) 395-398, 1979 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ between 1.925 and 2.18 GeV.' +Keywords: +BibKey: Delcourt:1979ed +BibTeX: '@article{Delcourt:1979ed, + author = "Delcourt, B. and others", + title = "{Study of the Reaction $e^+ e^- \to p \bar{p}$ in the + Total Energy Range 1925-{MeV} - 2180-{MeV}}", + journal = "Phys. Lett.", + volume = "86B", + year = "1979", + pages = "395-398", + doi = "10.1016/0370-2693(79)90864-5", + reportNumber = "LAL-79/12", + SLACcitation = "%%CITATION = PHLTA,86B,395;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1979_I141565.plot b/analyses/pluginOrsay/DM1_1979_I141565.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1979_I141565.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /DM1_1979_I141565/d01-x01-y01 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1979_I141565.yoda b/analyses/pluginOrsay/DM1_1979_I141565.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1979_I141565.yoda @@ -0,0 +1,24 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1979_I141565/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1979_I141565/d01-x01-y01 +Title: doi:10.17182/hepdata.27308.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.937000e+00 1.200000e-02 1.800000e-02 1.310000e+00 4.000000e-01 4.000000e-01 +1.973000e+00 1.700000e-02 2.000000e-02 6.200000e-01 4.000000e-01 4.000000e-01 +2.025000e+00 2.300000e-02 3.500000e-02 8.000000e-01 2.000000e-01 2.000000e-01 +2.135000e+00 2.500000e-02 4.500000e-02 5.500000e-01 1.900000e-01 1.900000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1979_I141565/d01-x01-y02 +IsRef: 1 +Path: /REF/DM1_1979_I141565/d01-x01-y02 +Title: doi:10.17182/hepdata.27308.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.937000e+00 1.200000e-02 1.800000e-02 1.550000e-01 4.700000e-02 4.700000e-02 +1.973000e+00 1.700000e-02 2.000000e-02 6.200000e-02 4.000000e-02 4.000000e-02 +2.025000e+00 2.300000e-02 3.500000e-02 7.000000e-02 1.800000e-02 1.800000e-02 +2.135000e+00 2.500000e-02 4.500000e-02 4.300000e-02 1.500000e-02 1.500000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1980_I140174.cc b/analyses/pluginOrsay/DM1_1980_I140174.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1980_I140174.cc @@ -0,0 +1,83 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1980_I140174 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1980_I140174); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _n3pi = bookCounter("TMP/3pi"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==3 && nCount[211] == 1 && nCount[-211] == 1 && nCount[111] == 1) + _n3pi->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _n3pi->val(); + double error = _n3pi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _n3pi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1980_I140174); + + +} diff --git a/analyses/pluginOrsay/DM1_1980_I140174.info b/analyses/pluginOrsay/DM1_1980_I140174.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1980_I140174.info @@ -0,0 +1,32 @@ +Name: DM1_1980_I140174 +Year: 1980 +Summary: Cross section for $e^+e^-\to\pi^+\pi^-\pi^0$ at energies between 0.75 and 1.1 GeV. +Experiment: DM1 +Collider: ACO +InspireID: 140174 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Nucl.Phys. B172 (1980) 13-24, 1980 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^-\pi^0$ at energies between 0.75 and 1.1 GeV.' +Keywords: [] +BibKey: Cordier:1979qg +BibTeX: '@article{Cordier:1979qg, + author = "Cordier, A. and others", + title = "{Cross-section of the Reaction $e^+ e^- \to \pi^+ \pi^- + \pi^0$ for Center-of-mass Energies From 750-{MeV} to + 1100-{MeV}}", + journal = "Nucl. Phys.", + volume = "B172", + year = "1980", + pages = "13-24", + doi = "10.1016/0550-3213(80)90157-1", + reportNumber = "LAL-79/1", + SLACcitation = "%%CITATION = NUPHA,B172,13;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1980_I140174.plot b/analyses/pluginOrsay/DM1_1980_I140174.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1980_I140174.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /DM1_1980_I140174/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1980_I140174.yoda b/analyses/pluginOrsay/DM1_1980_I140174.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1980_I140174.yoda @@ -0,0 +1,34 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1980_I140174/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1980_I140174/d01-x01-y01 +Title: doi:10.17182/hepdata.34511.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +7.502000e+02 0.000000e+00 0.000000e+00 1.500000e+01 1.101047e+01 1.101047e+01 +7.732000e+02 0.000000e+00 0.000000e+00 2.470000e+02 4.765997e+01 4.765997e+01 +7.782000e+02 0.000000e+00 0.000000e+00 7.760000e+02 1.059511e+02 1.059511e+02 +7.832000e+02 0.000000e+00 0.000000e+00 1.392000e+03 1.383661e+02 1.383661e+02 +7.892000e+02 0.000000e+00 0.000000e+00 7.390000e+02 9.208815e+01 9.208815e+01 +7.932000e+02 0.000000e+00 0.000000e+00 3.170000e+02 5.298019e+01 5.298019e+01 +8.432000e+02 0.000000e+00 0.000000e+00 2.360000e+01 1.062687e+01 1.062687e+01 +8.932000e+02 0.000000e+00 0.000000e+00 9.500000e+00 4.809617e+00 4.809617e+00 +9.630000e+02 0.000000e+00 0.000000e+00 1.850000e+01 7.024989e+00 7.024989e+00 +9.850000e+02 0.000000e+00 0.000000e+00 1.450000e+01 7.414533e+00 7.414533e+00 +1.002000e+03 0.000000e+00 0.000000e+00 3.180000e+01 8.064460e+00 8.064460e+00 +1.011000e+03 0.000000e+00 0.000000e+00 8.600000e+01 5.107420e+01 5.107420e+01 +1.015000e+03 0.000000e+00 0.000000e+00 1.770000e+02 6.624259e+01 6.624259e+01 +1.017000e+03 0.000000e+00 0.000000e+00 3.350000e+02 7.279367e+01 7.279367e+01 +1.018000e+03 0.000000e+00 0.000000e+00 3.930000e+02 6.326259e+01 6.326259e+01 +1.018280e+03 0.000000e+00 0.000000e+00 4.670000e+02 1.239045e+02 1.239045e+02 +1.018480e+03 0.000000e+00 0.000000e+00 4.570000e+02 1.785997e+02 1.785997e+02 +1.019000e+03 0.000000e+00 0.000000e+00 6.040000e+02 5.829727e+01 5.829727e+01 +1.019140e+03 0.000000e+00 0.000000e+00 6.960000e+02 1.467005e+02 1.467005e+02 +1.019440e+03 0.000000e+00 0.000000e+00 6.030000e+02 8.132242e+01 8.132242e+01 +1.020000e+03 0.000000e+00 0.000000e+00 5.700000e+02 5.889565e+01 5.889565e+01 +1.020600e+03 0.000000e+00 0.000000e+00 5.680000e+02 8.985748e+01 8.985748e+01 +1.021000e+03 0.000000e+00 0.000000e+00 4.100000e+02 6.044116e+01 6.044116e+01 +1.023000e+03 0.000000e+00 0.000000e+00 8.800000e+01 3.212367e+01 3.212367e+01 +1.058000e+03 0.000000e+00 0.000000e+00 9.800000e+00 4.111976e+00 4.111976e+00 +1.098000e+03 0.000000e+00 0.000000e+00 1.130000e+01 4.315177e+00 4.315177e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1981_I156053.cc b/analyses/pluginOrsay/DM1_1981_I156053.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I156053.cc @@ -0,0 +1,85 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1981_I156053 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1981_I156053); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nKSKL = bookCounter("TMP/nKSKL"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + if(ntotal==2 && nCount[130]==1 && nCount[310]==1) + _nKSKL->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nKSKL->val(); + double error = _nKSKL->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nKSKL; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1981_I156053); + + +} diff --git a/analyses/pluginOrsay/DM1_1981_I156053.info b/analyses/pluginOrsay/DM1_1981_I156053.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I156053.info @@ -0,0 +1,32 @@ +Name: DM1_1981_I156053 +Year: 1981 +Summary: Cross section for $e^+e^-\to K^0_SK^0_L$ between 1.4 and 2.18 GeV +Experiment: DM1 +Collider: DCI +InspireID: 156053 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B99 (1981) 261-264, 1981 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-$ at energies between 1.35 and 2.4 GeV' +Keywords: +BibKey: Mane:1980ep +BibTeX: '@article{Mane:1980ep, + author = "Mane, F. and Bisello, D. and Bizot, J. C. and Buon, J. + and Cordier, A. and Delcourt, B.", + title = "{Study of the Reaction $e^+ e^- \to K^0_S K^0_L$ in the + Total Energy Range 1.4-{GeV} to 2.18-{GeV} and + Interpretation of the $K^+$ and $K^0$ Form-factors}", + journal = "Phys. Lett.", + volume = "99B", + year = "1981", + pages = "261-264", + doi = "10.1016/0370-2693(81)91122-9", + reportNumber = "LAL/80-37", + SLACcitation = "%%CITATION = PHLTA,99B,261;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1981_I156053.plot b/analyses/pluginOrsay/DM1_1981_I156053.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I156053.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /DM1_1981_I156053/d01-x01-y01 +Title=$\sigma(e^+e^-\to K_S^0K_L^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K_S^0K_L^0)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1981_I156053.yoda b/analyses/pluginOrsay/DM1_1981_I156053.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I156053.yoda @@ -0,0 +1,36 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1981_I156053/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1981_I156053/d01-x01-y01 +Title: doi:10.17182/hepdata.38245.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.441500e+00 4.150000e-02 4.150000e-02 2.400000e-01 1.900000e-01 1.900000e-01 +1.524500e+00 2.450000e-02 2.450000e-02 3.800000e-01 3.000000e-02 3.000000e-02 +1.574500e+00 2.450000e-02 2.450000e-02 6.100000e-01 2.500000e-01 2.500000e-01 +1.612000e+00 1.200000e-02 1.200000e-02 7.000000e-01 2.900000e-01 2.900000e-01 +1.637000e+00 1.200000e-02 1.200000e-02 7.400000e-01 1.500000e-01 1.500000e-01 +1.674500e+00 2.450000e-02 2.450000e-02 3.200000e-01 1.200000e-01 1.200000e-01 +1.749500e+00 4.950000e-02 4.950000e-02 1.800000e-01 1.200000e-01 1.200000e-01 +1.877500e+00 7.750000e-02 7.750000e-02 1.000000e-02 5.000000e-02 5.000000e-02 +2.008500e+00 5.350000e-02 5.350000e-02 1.900000e-01 1.000000e-01 1.000000e-01 +2.140000e+00 3.500000e-02 3.500000e-02 7.000000e-02 7.000000e-02 7.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1981_I156053/d01-x01-y02 +IsRef: 1 +Path: /REF/DM1_1981_I156053/d01-x01-y02 +Title: doi:10.17182/hepdata.38245.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.441500e+00 4.150000e-02 4.150000e-02 6.100000e-02 4.900000e-02 4.900000e-02 +1.524500e+00 2.450000e-02 2.450000e-02 9.400000e-02 7.500000e-02 7.500000e-02 +1.574500e+00 2.450000e-02 2.450000e-02 1.490000e-01 6.100000e-02 6.100000e-02 +1.612000e+00 1.200000e-02 1.200000e-02 1.720000e-01 7.000000e-02 7.000000e-02 +1.637000e+00 1.200000e-02 1.200000e-02 1.830000e-01 3.700000e-02 3.700000e-02 +1.674500e+00 2.450000e-02 2.450000e-02 8.100000e-02 3.000000e-02 3.000000e-02 +1.749500e+00 4.950000e-02 4.950000e-02 4.700000e-02 3.100000e-02 3.100000e-02 +1.877500e+00 7.750000e-02 7.750000e-02 4.000000e-03 1.300000e-02 1.300000e-02 +2.008500e+00 5.350000e-02 5.350000e-02 5.500000e-02 3.000000e-02 3.000000e-02 +2.140000e+00 3.500000e-02 3.500000e-02 2.200000e-02 2.200000e-02 2.200000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1981_I156054.cc b/analyses/pluginOrsay/DM1_1981_I156054.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I156054.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1981_I156054 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1981_I156054); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nkaon = bookCounter("TMP/kaon"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::KPLUS) vetoEvent; + } + _nkaon->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nkaon->val(); + double error = _nkaon->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nkaon; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1981_I156054); + + +} diff --git a/analyses/pluginOrsay/DM1_1981_I156054.info b/analyses/pluginOrsay/DM1_1981_I156054.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I156054.info @@ -0,0 +1,31 @@ +Name: DM1_1981_I156054 +Year: 1981 +Summary: Cross section for $e^+e^-\to K^+K^-$ between 1.4 and 2.6 GeV +Experiment: DM1 +Collider: DCI +InspireID: 156054 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B99 (1981) 257-260, 1981 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-$ at energies between 1.4 and 2.6 GeV' +Keywords: +BibKey: Delcourt:1980eq +BibTeX: '@article{Delcourt:1980eq, + author = "Delcourt, B. and Bisello, D. and Bizot, J. C. and Buon, + J. and Cordier, A. and Mane, F.", + title = "{Study of the Reaction $e^+ e^- \to K^+ K^-$ in the Total + Energy Range 1400-{MeV} to 2060-{MeV}}", + journal = "Phys. Lett.", + volume = "99B", + year = "1981", + pages = "257-260", + doi = "10.1016/0370-2693(81)91121-7", + reportNumber = "LAL/80-36", + SLACcitation = "%%CITATION = PHLTA,99B,257;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1981_I156054.plot b/analyses/pluginOrsay/DM1_1981_I156054.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I156054.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /DM1_1981_I156054/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1981_I156054.yoda b/analyses/pluginOrsay/DM1_1981_I156054.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I156054.yoda @@ -0,0 +1,48 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1981_I156054/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1981_I156054/d01-x01-y01 +Title: doi:10.17182/hepdata.38243.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.424500e+00 2.450000e-02 2.450000e-02 5.300000e+00 9.000000e-01 9.000000e-01 +1.467500e+00 1.750000e-02 1.750000e-02 3.600000e+00 9.000000e-01 9.000000e-01 +1.524500e+00 2.450000e-02 2.450000e-02 3.200000e+00 6.500000e-01 6.500000e-01 +1.574500e+00 2.450000e-02 2.450000e-02 2.070000e+00 4.000000e-01 4.000000e-01 +1.609500e+00 9.500000e-03 9.500000e-03 3.100000e+00 6.000000e-01 6.000000e-01 +1.629500e+00 9.500000e-03 9.500000e-03 2.680000e+00 3.000000e-01 3.000000e-01 +1.649500e+00 9.500000e-03 9.500000e-03 2.040000e+00 3.500000e-01 3.500000e-01 +1.669500e+00 9.500000e-03 9.500000e-03 2.470000e+00 4.000000e-01 4.000000e-01 +1.689500e+00 9.500000e-03 9.500000e-03 1.430000e+00 4.000000e-01 4.000000e-01 +1.714500e+00 1.450000e-02 1.450000e-02 2.500000e-01 6.000000e-01 6.000000e-01 +1.744500e+00 1.450000e-02 1.450000e-02 5.700000e-01 3.000000e-01 3.000000e-01 +1.779500e+00 1.950000e-02 1.950000e-02 -2.000000e-01 3.000000e-01 3.000000e-01 +1.824500e+00 2.450000e-02 2.450000e-02 -3.000000e-01 4.000000e-01 4.000000e-01 +1.889500e+00 3.950000e-02 3.950000e-02 9.600000e-01 2.800000e-01 2.800000e-01 +1.961250e+00 3.125000e-02 3.125000e-02 3.300000e-01 2.500000e-01 2.500000e-01 +2.030000e+00 3.000000e-02 3.000000e-02 4.000000e-01 3.000000e-01 3.000000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1981_I156054/d01-x01-y02 +IsRef: 1 +Path: /REF/DM1_1981_I156054/d01-x01-y02 +Title: doi:10.17182/hepdata.38243.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.424500e+00 2.450000e-02 2.450000e-02 1.330000e+00 2.340257e-01 2.340257e-01 +1.467500e+00 1.750000e-02 1.750000e-02 8.800000e-01 2.457394e-01 2.457394e-01 +1.524500e+00 2.450000e-02 2.450000e-02 7.700000e-01 1.665366e-01 1.665366e-01 +1.574500e+00 2.450000e-02 2.450000e-02 5.000000e-01 9.486833e-02 9.486833e-02 +1.609500e+00 9.500000e-03 9.500000e-03 7.500000e-01 1.566046e-01 1.566046e-01 +1.629500e+00 9.500000e-03 9.500000e-03 6.500000e-01 8.013114e-02 8.013114e-02 +1.649500e+00 9.500000e-03 9.500000e-03 5.000000e-01 7.615773e-02 7.615773e-02 +1.669500e+00 9.500000e-03 9.500000e-03 6.000000e-01 1.062826e-01 1.062826e-01 +1.689500e+00 9.500000e-03 9.500000e-03 3.500000e-01 1.021812e-01 1.021812e-01 +1.714500e+00 1.450000e-02 1.450000e-02 6.000000e-02 1.500432e-01 1.500432e-01 +1.744500e+00 1.450000e-02 1.450000e-02 1.400000e-01 7.050220e-02 7.050220e-02 +1.779500e+00 1.950000e-02 1.950000e-02 -5.000000e-02 7.006426e-02 7.006426e-02 +1.824500e+00 2.450000e-02 2.450000e-02 -7.000000e-02 9.009795e-02 9.009795e-02 +1.889500e+00 3.950000e-02 3.950000e-02 2.500000e-01 7.158911e-02 7.158911e-02 +1.961250e+00 3.125000e-02 3.125000e-02 9.000000e-02 7.020798e-02 7.020798e-02 +2.030000e+00 3.000000e-02 3.000000e-02 1.100000e-01 9.024168e-02 9.024168e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1981_I166353.cc b/analyses/pluginOrsay/DM1_1981_I166353.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I166353.cc @@ -0,0 +1,75 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1981_I166353 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1981_I166353); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + _num3pip3pim = bookCounter("TMP/num3pip3pim"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=211) vetoEvent; + ++ntotal; + } + if(ntotal!=6) vetoEvent; + _num3pip3pim->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sigma = _num3pip3pim->val()*fact; + double error = _num3pip3pim->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + //@} + + /// @name Histograms + //@{ + CounterPtr _num3pip3pim; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1981_I166353); + + +} diff --git a/analyses/pluginOrsay/DM1_1981_I166353.info b/analyses/pluginOrsay/DM1_1981_I166353.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I166353.info @@ -0,0 +1,33 @@ +Name: DM1_1981_I166353 +Year: 1981 +Summary: Cross section for $e^+e^-\to 3\pi^+3\pi^-$ between 1.4 and 2.11 GeV +Experiment: DM1 +Collider: DCI +InspireID: 166353 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D73.052003 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Luminosity_fb: 1 +Description: + 'Cross section for $e^+e^-\to3\pi^+3\pi^-$ between 1.4 and 2.18 GeV' +Keywords: +Keywords: [] +BibKey: Bisello:1981sh +BibTeX: '@article{Bisello:1981sh, + author = "Bisello, D. and Bizot, J. C. and Buon, J. and Cordier, A. + and Delcourt, B. and Mane, F.", + title = "{Study of the Reaction $e^+ e^- \to 3 \pi^+ 3 \pi^-$ in + the Total Energy Range 1400-{MeV} to 2180-{MeV}}", + journal = "Phys. Lett.", + volume = "107B", + year = "1981", + pages = "145-147", + doi = "10.1016/0370-2693(81)91169-2", + reportNumber = "LAL 81/19", + SLACcitation = "%%CITATION = PHLTA,107B,145;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1981_I166353.plot b/analyses/pluginOrsay/DM1_1981_I166353.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I166353.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /DM1_1981_I166353/d01-x01-y01 +Title=$\sigma(e^+e^-\to 3\pi^+3\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 3\pi^+3\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1981_I166353.yoda b/analyses/pluginOrsay/DM1_1981_I166353.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I166353.yoda @@ -0,0 +1,14 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1981_I166353/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1981_I166353/d01-x01-y01 +Title: doi:10.17182/hepdata.31033.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.650000e+00 5.000000e-02 5.000000e-02 5.200000e-01 1.100000e-01 1.824811e-01 +1.750000e+00 5.000000e-02 5.000000e-02 1.400000e+00 3.100000e-01 4.997639e-01 +1.850000e+00 5.000000e-02 5.000000e-02 1.160000e+00 2.800000e-01 4.288298e-01 +1.950000e+00 5.000000e-02 5.000000e-02 1.280000e+00 2.900000e-01 4.610321e-01 +2.030000e+00 3.000000e-02 3.000000e-02 1.880000e+00 3.100000e-01 6.108985e-01 +2.145000e+00 3.500000e-02 3.500000e-02 2.330000e+00 3.600000e-01 7.451347e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1981_I166964.cc b/analyses/pluginOrsay/DM1_1981_I166964.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I166964.cc @@ -0,0 +1,117 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1981_I166964 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1981_I166964); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nomega = bookCounter("TMP/omega"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==223) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // omega pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nomega->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sigma = _nomega->val()*fact; + double error = _nomega->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nomega; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1981_I166964); + + +} diff --git a/analyses/pluginOrsay/DM1_1981_I166964.info b/analyses/pluginOrsay/DM1_1981_I166964.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I166964.info @@ -0,0 +1,31 @@ +Name: DM1_1981_I166964 +Year: 1981 +Summary: Cross section for $e^+e^-\to\omega\pi^+\pi^-$ at energies between 1.4 and 2.2 GeV +Experiment: DM1 +Collider: DCI +InspireID: 166964 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B106 (1981) 155-158, 1981 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\omega\pi^+\pi^-$ at energies between 1.4 and 2.2 GeV.' +BibKey: Cordier:1981zs +BibTeX: '@article{Cordier:1981zs, + author = "Cordier, A. and Bisello, D. and Bizot, J. C. and Buon, J. + and Delcourt, B. and Mane, F.", + title = "{Observation of a New Isoscalar Vector Meson in $e^+ e^- + \to \omega \pi^+ \pi^-$ Annihilation at 1.65-{GeV}}", + journal = "Phys. Lett.", + volume = "106B", + year = "1981", + pages = "155-158", + doi = "10.1016/0370-2693(81)91101-1", + reportNumber = "LAL 81/20", + SLACcitation = "%%CITATION = PHLTA,106B,155;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1981_I166964.plot b/analyses/pluginOrsay/DM1_1981_I166964.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I166964.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /DM1_1981_I166964/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\omega)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\omega)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1981_I166964.yoda b/analyses/pluginOrsay/DM1_1981_I166964.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1981_I166964.yoda @@ -0,0 +1,23 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1981_I166964/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1981_I166964/d01-x01-y01 +Title: doi:10.17182/hepdata.31042.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.442500e+03 4.250000e+01 4.250000e+01 5.200000e-01 1.028394e+00 1.028394e+00 +1.530000e+03 3.000000e+01 3.000000e+01 4.900000e-01 9.054598e-01 9.054598e-01 +1.575000e+03 1.500000e+01 1.500000e+01 2.300000e+00 1.113138e+00 1.113138e+00 +1.606500e+03 1.650000e+01 1.650000e+01 2.010000e+00 1.058762e+00 1.058762e+00 +1.633000e+03 1.000000e+01 1.000000e+01 4.050000e+00 9.079626e-01 9.079626e-01 +1.653000e+03 1.000000e+01 1.000000e+01 3.410000e+00 9.382668e-01 9.382668e-01 +1.673000e+03 1.000000e+01 1.000000e+01 3.960000e+00 1.233051e+00 1.233051e+00 +1.704000e+03 2.100000e+01 2.100000e+01 2.950000e+00 1.113156e+00 1.113156e+00 +1.748500e+03 2.350000e+01 2.350000e+01 9.100000e-01 7.647383e-01 7.647383e-01 +1.792000e+03 2.000000e+01 2.000000e+01 1.430000e+00 8.282189e-01 8.282189e-01 +1.846500e+03 3.450000e+01 3.450000e+01 2.080000e+00 8.907863e-01 8.907863e-01 +1.908500e+03 2.750000e+01 2.750000e+01 8.700000e-01 7.020679e-01 7.020679e-01 +1.964500e+03 2.850000e+01 2.850000e+01 5.800000e-01 6.081481e-01 6.081481e-01 +2.031000e+03 2.900000e+01 2.900000e+01 -9.000000e-02 3.232903e-01 3.232903e-01 +2.145000e+03 3.500000e+01 3.500000e+01 7.900000e-01 7.134333e-01 7.134333e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1982_I168552.cc b/analyses/pluginOrsay/DM1_1982_I168552.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I168552.cc @@ -0,0 +1,78 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1982_I168552 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1982_I168552); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=4) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1982_I168552); + + +} diff --git a/analyses/pluginOrsay/DM1_1982_I168552.info b/analyses/pluginOrsay/DM1_1982_I168552.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I168552.info @@ -0,0 +1,32 @@ +Name: DM1_1982_I168552 +Year: 1982 +Summary: Cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ between 1.4 and 2.18 GeV +Experiment: DM1 +Collider: DCI +InspireID: 168552 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B109 (1982) 129-132, 1982 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^+\pi^-\pi^+$ between 1.4 and 2.18 GeV' +Keywords: +BibKey: Cordier:1981zn +BibTeX: '@article{Cordier:1981zn, + author = "Cordier, A. and Bisello, D. and Bizot, J. C. and Buon, J. + and Delcourt, B. and Fayard, L. and Mane, F.", + title = "{Study of the $e^+ e^- \to \pi^+ \pi^- \pi^+ \pi^-$ + Reaction in the 1.4-{GeV} to 2.18-{GeV} Energy Range}", + journal = "Phys. Lett.", + volume = "109B", + year = "1982", + pages = "129-132", + doi = "10.1016/0370-2693(82)90478-6", + reportNumber = "LAL 81/33", + SLACcitation = "%%CITATION = PHLTA,109B,129;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1982_I168552.plot b/analyses/pluginOrsay/DM1_1982_I168552.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I168552.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /DM1_1982_I168552/d01-x01-y01 +Title=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to 2\pi^+2\pi^-)$/nb +LogY=0 +LegendXPos=0.8 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1982_I168552.yoda b/analyses/pluginOrsay/DM1_1982_I168552.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I168552.yoda @@ -0,0 +1,45 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1982_I168552/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1982_I168552/d01-x01-y01 +Title: doi:10.17182/hepdata.30995.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.410000e+00 0.000000e+00 0.000000e+00 3.020000e+01 3.857512e+00 3.857512e+00 +1.430000e+00 0.000000e+00 0.000000e+00 3.330000e+01 4.287062e+00 4.287062e+00 +1.450000e+00 0.000000e+00 0.000000e+00 3.320000e+01 4.216918e+00 4.216918e+00 +1.470000e+00 0.000000e+00 0.000000e+00 3.240000e+01 4.154227e+00 4.154227e+00 +1.482000e+00 0.000000e+00 0.000000e+00 3.420000e+01 5.262737e+00 5.262737e+00 +1.510000e+00 0.000000e+00 0.000000e+00 3.330000e+01 4.164000e+00 4.164000e+00 +1.530000e+00 0.000000e+00 0.000000e+00 3.300000e+01 4.140048e+00 4.140048e+00 +1.550000e+00 0.000000e+00 0.000000e+00 3.390000e+01 4.096596e+00 4.096596e+00 +1.570000e+00 0.000000e+00 0.000000e+00 3.100000e+01 3.689173e+00 3.689173e+00 +1.588000e+00 0.000000e+00 0.000000e+00 2.890000e+01 3.458627e+00 3.458627e+00 +1.610000e+00 0.000000e+00 0.000000e+00 2.730000e+01 3.270000e+00 3.270000e+00 +1.630000e+00 0.000000e+00 0.000000e+00 2.520000e+01 2.882776e+00 2.882776e+00 +1.650000e+00 0.000000e+00 0.000000e+00 2.360000e+01 2.694364e+00 2.694364e+00 +1.670000e+00 0.000000e+00 0.000000e+00 2.250000e+01 2.598557e+00 2.598557e+00 +1.690000e+00 0.000000e+00 0.000000e+00 2.060000e+01 2.490703e+00 2.490703e+00 +1.708000e+00 0.000000e+00 0.000000e+00 1.930000e+01 2.571945e+00 2.571945e+00 +1.730000e+00 0.000000e+00 0.000000e+00 1.760000e+01 2.517459e+00 2.517459e+00 +1.750000e+00 0.000000e+00 0.000000e+00 1.660000e+01 2.171543e+00 2.171543e+00 +1.770000e+00 0.000000e+00 0.000000e+00 1.460000e+01 1.828004e+00 1.828004e+00 +1.788000e+00 0.000000e+00 0.000000e+00 1.290000e+01 1.695317e+00 1.695317e+00 +1.810000e+00 0.000000e+00 0.000000e+00 1.180000e+01 1.682974e+00 1.682974e+00 +1.830000e+00 0.000000e+00 0.000000e+00 9.000000e+00 1.345362e+00 1.345362e+00 +1.850000e+00 0.000000e+00 0.000000e+00 8.300000e+00 1.378006e+00 1.378006e+00 +1.870000e+00 0.000000e+00 0.000000e+00 9.200000e+00 1.512085e+00 1.512085e+00 +1.890000e+00 0.000000e+00 0.000000e+00 7.000000e+00 1.220656e+00 1.220656e+00 +1.910000e+00 0.000000e+00 0.000000e+00 8.000000e+00 1.360147e+00 1.360147e+00 +1.932000e+00 0.000000e+00 0.000000e+00 7.100000e+00 9.970456e-01 9.970456e-01 +1.948000e+00 0.000000e+00 0.000000e+00 6.300000e+00 1.018283e+00 1.018283e+00 +1.970000e+00 0.000000e+00 0.000000e+00 7.000000e+00 1.140175e+00 1.140175e+00 +1.986000e+00 0.000000e+00 0.000000e+00 7.100000e+00 1.309236e+00 1.309236e+00 +2.010000e+00 0.000000e+00 0.000000e+00 8.400000e+00 1.160000e+00 1.160000e+00 +2.030000e+00 0.000000e+00 0.000000e+00 7.500000e+00 1.025914e+00 1.025914e+00 +2.047000e+00 0.000000e+00 0.000000e+00 6.900000e+00 1.056456e+00 1.056456e+00 +2.112000e+00 0.000000e+00 0.000000e+00 6.900000e+00 1.742441e+00 1.742441e+00 +2.130000e+00 0.000000e+00 0.000000e+00 5.700000e+00 9.027181e-01 9.027181e-01 +2.147000e+00 0.000000e+00 0.000000e+00 5.900000e+00 8.414868e-01 8.414868e-01 +2.166000e+00 0.000000e+00 0.000000e+00 7.000000e+00 1.838478e+00 1.838478e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1982_I169382.cc b/analyses/pluginOrsay/DM1_1982_I169382.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I169382.cc @@ -0,0 +1,83 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1982_I169382 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1982_I169382); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + _cKpKmpippim = bookCounter("TMP/KpKmpippim"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + + if(ntotal!=4) vetoEvent; + if(nCount[321]==1 && nCount[-321]==1 && nCount[211]==1 && nCount[-211]==1) + _cKpKmpippim->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _cKpKmpippim->val(); + double error = _cKpKmpippim->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _cKpKmpippim; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1982_I169382); + + +} diff --git a/analyses/pluginOrsay/DM1_1982_I169382.info b/analyses/pluginOrsay/DM1_1982_I169382.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I169382.info @@ -0,0 +1,33 @@ +Name: DM1_1982_I169382 +Year: 1982 +Summary: Cross section for $e^+e^-\to K^+K^-\pi^+\pi^-$ between 1.3 and 2.2 GeV +Experiment: DM1 +Collider: DCI +InspireID: 169382 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B110 (1982) 335-338, 1982 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-\pi^+\pi^-$ between 1.4 and 2.2 GeV.' +Keywords: [] +BibKey: Cordier:1981en +BibTeX: '@article{Cordier:1981en, + author = "Cordier, A. and Bisello, D. and Bizot, J. C. and Buon, J. + and Delcourt, B. and Fayard, L. and Mane, F.", + title = "{Study of the $e^+ e^- \to \pi^+ \pi^- K^+ K^-$ Reaction + From 1.4-{GeV} to 2.18-{GeV}}", + journal = "Phys. Lett.", + volume = "110B", + year = "1982", + pages = "335-338", + doi = "10.1016/0370-2693(82)91267-9", + reportNumber = "LAL-81/35", + SLACcitation = "%%CITATION = PHLTA,110B,335;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1982_I169382.plot b/analyses/pluginOrsay/DM1_1982_I169382.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I169382.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /DM1_1982_I169382/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^+\pi^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1982_I169382.yoda b/analyses/pluginOrsay/DM1_1982_I169382.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I169382.yoda @@ -0,0 +1,45 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1982_I169382/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1982_I169382/d01-x01-y01 +Title: doi:10.17182/hepdata.30957.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.625000e+00 2.500000e-02 2.500000e-02 9.900000e-01 2.463000e-01 2.463000e-01 +1.675000e+00 2.500000e-02 2.500000e-02 1.730000e+00 4.160289e-01 4.160289e-01 +1.725000e+00 2.500000e-02 2.500000e-02 2.800000e+00 8.607532e-01 8.607532e-01 +1.775000e+00 2.500000e-02 2.500000e-02 3.310000e+00 6.826845e-01 6.826845e-01 +1.825000e+00 2.500000e-02 2.500000e-02 4.480000e+00 1.005778e+00 1.005778e+00 +1.875000e+00 2.500000e-02 2.500000e-02 5.920000e+00 1.269797e+00 1.269797e+00 +1.950000e+00 5.000000e-02 5.000000e-02 4.860000e+00 8.376582e-01 8.376582e-01 +2.030000e+00 3.000000e-02 3.000000e-02 5.330000e+00 8.846527e-01 8.846527e-01 +2.140000e+00 4.000000e-02 4.000000e-02 4.160000e+00 7.433469e-01 7.433469e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1982_I169382/d02-x01-y01 +IsRef: 1 +Path: /REF/DM1_1982_I169382/d02-x01-y01 +Title: doi:10.17182/hepdata.30957.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.650000e+00 5.000000e-02 5.000000e-02 4.600000e-01 5.980000e-02 5.980000e-02 +1.750000e+00 5.000000e-02 5.000000e-02 8.000000e-01 1.040000e-01 1.040000e-01 +1.850000e+00 5.000000e-02 5.000000e-02 5.200000e-01 6.760000e-02 6.760000e-02 +1.950000e+00 5.000000e-02 5.000000e-02 1.060000e+00 1.378000e-01 1.378000e-01 +2.030000e+00 3.000000e-02 3.000000e-02 2.600000e-01 3.380000e-02 3.380000e-02 +2.140000e+00 4.000000e-02 4.000000e-02 2.200000e-01 2.860000e-02 2.860000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1982_I169382/d02-x01-y02 +IsRef: 1 +Path: /REF/DM1_1982_I169382/d02-x01-y02 +Title: doi:10.17182/hepdata.30957.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.650000e+00 5.000000e-02 5.000000e-02 3.800000e-01 4.940000e-02 4.940000e-02 +1.750000e+00 5.000000e-02 5.000000e-02 2.600000e-01 3.380000e-02 3.380000e-02 +1.850000e+00 5.000000e-02 5.000000e-02 1.000000e-01 1.300000e-02 1.300000e-02 +1.950000e+00 5.000000e-02 5.000000e-02 2.200000e-01 2.860000e-02 2.860000e-02 +2.030000e+00 3.000000e-02 3.000000e-02 5.000000e-02 6.500000e-03 6.500000e-03 +2.140000e+00 4.000000e-02 4.000000e-02 5.000000e-02 6.500000e-03 6.500000e-03 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM1_1982_I176801.cc b/analyses/pluginOrsay/DM1_1982_I176801.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I176801.cc @@ -0,0 +1,85 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM1_1982_I176801 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM1_1982_I176801); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + _nKKpi= bookCounter("/TMP/nKKpi"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=3) vetoEvent; + if(nCount[310]==1 && + ((nCount[ 211]==1&&nCount[-321]==1)|| + (nCount[-211]==1&&nCount[ 321]==1))) + _nKKpi->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nKKpi->val(); + double error = _nKKpi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nKKpi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM1_1982_I176801); + + +} diff --git a/analyses/pluginOrsay/DM1_1982_I176801.info b/analyses/pluginOrsay/DM1_1982_I176801.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I176801.info @@ -0,0 +1,34 @@ +Name: DM1_1982_I176801 +Year: 1982 +Summary: Cross section for $e^+e^-\to K^0_SK^\pm\pi^\mp$ for energies from 1.4 to 2.1 GeV +Experiment: DM1 +Collider: DCI +InspireID: 176801 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C52 (1991) 227-230, 1991 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to$ ^0_SK^\pm\pi^\mp$ + for energies from 1.4 to 2.`x GeV.' +Keywords: +BibKey: Mane:1982si +BibTeX: '@article{Mane:1982si, + author = "Mane, F. and Bisello, D. and Bizot, J. C. and Buon, J. + and Cordier, A. and Delcourt, B.", + title = "{Study of $e^+ e^- \to K^0_S K^\pm \pi^\mp$ in the + 1.4-{GeV} to 2.18-{GeV} Energy Range: A New Observation of + an Isoscalar Vector Meson $\phi^\prime$ (1.65-{GeV})}", + journal = "Phys. Lett.", + volume = "112B", + year = "1982", + pages = "178-182", + doi = "10.1016/0370-2693(82)90324-0", + reportNumber = "LAL-82/02", + SLACcitation = "%%CITATION = PHLTA,112B,178;%%" +}' diff --git a/analyses/pluginOrsay/DM1_1982_I176801.plot b/analyses/pluginOrsay/DM1_1982_I176801.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I176801.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /DM1_1982_I176801/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^\pm \pi^\mp)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^\pm \pi^\mp)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM1_1982_I176801.yoda b/analyses/pluginOrsay/DM1_1982_I176801.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM1_1982_I176801.yoda @@ -0,0 +1,23 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM1_1982_I176801/d01-x01-y01 +IsRef: 1 +Path: /REF/DM1_1982_I176801/d01-x01-y01 +Title: doi:10.17182/hepdata.30954.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.441500e+03 4.150000e+01 4.150000e+01 1.270000e+00 5.200000e-01 5.200000e-01 +1.524500e+03 2.450000e+01 2.450000e+01 2.210000e+00 8.400000e-01 8.400000e-01 +1.574500e+03 2.450000e+01 2.450000e+01 3.610000e+00 7.400000e-01 7.400000e-01 +1.612000e+03 1.200000e+01 1.200000e+01 3.860000e+00 9.400000e-01 9.400000e-01 +1.629500e+03 4.500000e+00 4.500000e+00 4.770000e+00 9.000000e-01 9.000000e-01 +1.642000e+03 7.000000e+00 7.000000e+00 4.190000e+00 6.200000e-01 6.200000e-01 +1.662000e+03 1.200000e+01 1.200000e+01 4.690000e+00 7.800000e-01 7.800000e-01 +1.687000e+03 1.200000e+01 1.200000e+01 5.870000e+00 1.070000e+00 1.070000e+00 +1.724500e+03 2.450000e+01 2.450000e+01 1.340000e+00 6.700000e-01 6.700000e-01 +1.774500e+03 2.450000e+01 2.450000e+01 1.810000e+00 5.000000e-01 5.000000e-01 +1.819500e+03 1.950000e+01 1.950000e+01 1.970000e+00 7.400000e-01 7.400000e-01 +1.882000e+03 4.200000e+01 4.200000e+01 1.080000e+00 4.400000e-01 4.400000e-01 +1.961500e+03 3.650000e+01 3.650000e+01 4.000000e-01 2.300000e-01 2.300000e-01 +2.031000e+03 2.900000e+01 2.900000e+01 1.010000e+00 3.200000e-01 3.200000e-01 +2.140000e+03 3.500000e+01 3.500000e+01 7.600000e-01 2.900000e-01 2.900000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM2_1983_I190558.cc b/analyses/pluginOrsay/DM2_1983_I190558.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1983_I190558.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/FastJets.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM2_1983_I190558 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM2_1983_I190558); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nproton = bookCounter("TMP/proton"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PROTON) vetoEvent; + } + _nproton->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nproton->val(); + double error = _nproton->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nproton; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM2_1983_I190558); + + +} diff --git a/analyses/pluginOrsay/DM2_1983_I190558.info b/analyses/pluginOrsay/DM2_1983_I190558.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1983_I190558.info @@ -0,0 +1,31 @@ +Name: DM2_1983_I190558 +Year: 1983 +Summary: Cross section for $e^+e^-\to p\bar{p}$ between 1.975 and 2.250 GeV +Experiment: DM2 +Collider: DCI +InspireID: 190558 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Nucl.Phys. B224 (1983) 379, 1983 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ between 1.975 and 2.250 GeV ' +BibKey: Bisello:1983at +BibTeX: '@article{Bisello:1983at, + author = "Bisello, D. and others", + title = "{>A Measurement of $e^+ e^- \to \bar{p} p$ for 1975-{MeV} + $\le \sqrt{s} \le$ 2250-{MeV}}", + journal = "Nucl. Phys.", + volume = "B224", + year = "1983", + pages = "379", + doi = "10.1016/0550-3213(83)90381-4", + reportNumber = "LAL 83/15", + SLACcitation = "%%CITATION = NUPHA,B224,379;%%" +}' diff --git a/analyses/pluginOrsay/DM2_1983_I190558.plot b/analyses/pluginOrsay/DM2_1983_I190558.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1983_I190558.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /DM2_1983_I190558/d01-x01-y01 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM2_1983_I190558.yoda b/analyses/pluginOrsay/DM2_1983_I190558.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1983_I190558.yoda @@ -0,0 +1,43 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1983_I190558/d01-x01-y01 +IsRef: 1 +Path: /REF/DM2_1983_I190558/d01-x01-y01 +Title: doi:10.17182/hepdata.33935.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.000000e+03 2.500000e+01 2.500000e+01 7.600000e-01 1.600000e-01 1.600000e-01 +2.050000e+03 2.500000e+01 2.500000e+01 5.600000e-01 1.100000e-01 1.100000e-01 +2.100000e+03 2.500000e+01 2.500000e+01 4.400000e-01 1.000000e-01 1.000000e-01 +2.150000e+03 2.500000e+01 2.500000e+01 3.500000e-01 9.000000e-02 9.000000e-02 +2.200000e+03 2.500000e+01 2.500000e+01 4.500000e-01 1.000000e-01 1.000000e-01 +2.237500e+03 1.250000e+01 1.250000e+01 2.400000e-01 1.400000e-01 1.400000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1983_I190558/d02-x01-y01 +IsRef: 1 +Path: /REF/DM2_1983_I190558/d02-x01-y01 +Title: doi:10.17182/hepdata.33935.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.000000e+00 0.000000e+00 0.000000e+00 2.600000e-01 3.000000e-02 3.000000e-02 +4.200000e+00 0.000000e+00 0.000000e+00 2.200000e-01 2.000000e-02 2.000000e-02 +4.400000e+00 0.000000e+00 0.000000e+00 1.900000e-01 2.000000e-02 2.000000e-02 +4.600000e+00 0.000000e+00 0.000000e+00 1.700000e-01 2.000000e-02 2.000000e-02 +4.800000e+00 0.000000e+00 0.000000e+00 1.900000e-01 2.000000e-02 2.000000e-02 +5.000000e+00 0.000000e+00 0.000000e+00 1.400000e-01 4.000000e-02 4.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1983_I190558/d03-x01-y01 +IsRef: 1 +Path: /REF/DM2_1983_I190558/d03-x01-y01 +Title: doi:10.17182/hepdata.33935.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-02 5.000000e-02 5.000000e-02 5.800000e-01 1.300000e-01 1.300000e-01 +1.500000e-01 5.000000e-02 5.000000e-02 4.000000e-01 1.100000e-01 1.100000e-01 +2.500000e-01 5.000000e-02 5.000000e-02 6.000000e-01 1.300000e-01 1.300000e-01 +3.500000e-01 5.000000e-02 5.000000e-02 4.000000e-01 1.100000e-01 1.100000e-01 +4.500000e-01 5.000000e-02 5.000000e-02 5.000000e-01 1.200000e-01 1.200000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 3.600000e-01 1.000000e-01 1.000000e-01 +6.500000e-01 5.000000e-02 5.000000e-02 3.800000e-01 1.500000e-01 1.500000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM2_1988_I262690.cc b/analyses/pluginOrsay/DM2_1988_I262690.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1988_I262690.cc @@ -0,0 +1,82 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM2_1988_I262690 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM2_1988_I262690); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _nkaon = bookCounter("TMP/kaon"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::KPLUS) vetoEvent; + } + _nkaon->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nkaon->val(); + double error = _nkaon->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nkaon; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM2_1988_I262690); + + +} diff --git a/analyses/pluginOrsay/DM2_1988_I262690.info b/analyses/pluginOrsay/DM2_1988_I262690.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1988_I262690.info @@ -0,0 +1,33 @@ +Name: DM2_1988_I262690 +Year: 1988 +Summary: Cross section for $e^+e^-\to K^+K^-$ between 1.35 and 2.4 GeV +Experiment: DM2 +Collider: DCI +InspireID: 262690 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Z.Phys. C39 (1988) 13 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to K^+K^-$ at energies between 1.35 and 2.4 GeV' +Keywords: +BibKey: Bisello:1988ez +BibTeX: '@article{Bisello:1988ez, + author = "Bisello, D. and others", + title = "{Study of the Reaction $e^+ e^- \to K^+ K^-$ in the + Energy Range 1350 $\le \sqrt{s} \le$ 2400-{MeV}}", + booktitle = "{Z. PHYS. C39 (1988) 13-19 AND ORSAY LAB. ACCEL. LIN. - + L.A.L. 88-01 (88,REC.JUL.) 16p}", + collaboration = "DM2", + journal = "Z. Phys.", + volume = "C39", + year = "1988", + pages = "13", + doi = "10.1007/BF01560386", + reportNumber = "LAL-88-01", + SLACcitation = "%%CITATION = ZEPYA,C39,13;%%" +}' diff --git a/analyses/pluginOrsay/DM2_1988_I262690.plot b/analyses/pluginOrsay/DM2_1988_I262690.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1988_I262690.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /DM2_1988_I262690/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^+K^-)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM2_1988_I262690.yoda b/analyses/pluginOrsay/DM2_1988_I262690.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1988_I262690.yoda @@ -0,0 +1,58 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1988_I262690/d01-x01-y01 +IsRef: 1 +Path: /REF/DM2_1988_I262690/d01-x01-y01 +Title: doi:10.17182/hepdata.15622.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.349500e+03 1.950000e+01 1.950000e+01 4.360000e+00 5.100000e-01 5.100000e-01 +1.399500e+03 9.500000e+00 9.500000e+00 4.010000e+00 8.100000e-01 8.100000e-01 +1.444500e+03 3.450000e+01 3.450000e+01 3.140000e+00 2.800000e-01 2.800000e-01 +1.499500e+03 1.950000e+01 1.950000e+01 2.270000e+00 4.300000e-01 4.300000e-01 +1.559500e+03 1.950000e+01 1.950000e+01 2.160000e+00 4.300000e-01 4.300000e-01 +1.589500e+03 9.500000e+00 9.500000e+00 2.230000e+00 4.700000e-01 4.700000e-01 +1.609500e+03 9.500000e+00 9.500000e+00 2.180000e+00 3.500000e-01 3.500000e-01 +1.629500e+03 9.500000e+00 9.500000e+00 1.870000e+00 3.200000e-01 3.200000e-01 +1.649500e+03 9.500000e+00 9.500000e+00 1.640000e+00 2.000000e-01 2.000000e-01 +1.674500e+03 1.450000e+01 1.450000e+01 1.020000e+00 1.700000e-01 1.700000e-01 +1.714500e+03 1.450000e+01 1.450000e+01 8.100000e-01 1.800000e-01 1.800000e-01 +1.754500e+03 2.450000e+01 2.450000e+01 6.400000e-01 1.200000e-01 1.200000e-01 +1.804500e+03 2.450000e+01 2.450000e+01 1.000000e-01 7.000000e-02 7.000000e-02 +1.849500e+03 1.950000e+01 1.950000e+01 1.600000e-01 1.400000e-01 1.400000e-01 +1.894500e+03 2.450000e+01 2.450000e+01 1.700000e-01 1.500000e-01 1.500000e-01 +1.934500e+03 1.450000e+01 1.450000e+01 2.300000e-01 1.900000e-01 1.900000e-01 +1.959500e+03 9.500000e+00 9.500000e+00 2.000000e-01 2.800000e-01 2.800000e-01 +1.989500e+03 1.950000e+01 1.950000e+01 1.500000e-01 1.600000e-01 1.600000e-01 +2.024500e+03 1.450000e+01 1.450000e+01 2.000000e-01 1.300000e-01 1.300000e-01 +2.054500e+03 1.450000e+01 1.450000e+01 3.200000e-01 1.600000e-01 1.600000e-01 +2.084500e+03 1.450000e+01 1.450000e+01 1.700000e-01 1.200000e-01 1.200000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1988_I262690/d02-x01-y01 +IsRef: 1 +Path: /REF/DM2_1988_I262690/d02-x01-y01 +Title: doi:10.17182/hepdata.15622.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.349500e+03 1.950000e+01 1.950000e+01 1.170000e+00 1.400000e-01 1.400000e-01 +1.399500e+03 9.500000e+00 9.500000e+00 1.010000e+00 2.100000e-01 2.100000e-01 +1.444500e+03 3.450000e+01 3.450000e+01 7.700000e-01 1.000000e-01 1.000000e-01 +1.499500e+03 1.950000e+01 1.950000e+01 5.500000e-01 1.100000e-01 1.100000e-01 +1.559500e+03 1.950000e+01 1.950000e+01 5.200000e-01 1.100000e-01 1.100000e-01 +1.589500e+03 9.500000e+00 9.500000e+00 5.400000e-01 1.100000e-01 1.100000e-01 +1.609500e+03 9.500000e+00 9.500000e+00 5.300000e-01 8.000000e-02 8.000000e-02 +1.629500e+03 9.500000e+00 9.500000e+00 4.500000e-01 8.000000e-02 8.000000e-02 +1.649500e+03 9.500000e+00 9.500000e+00 4.000000e-01 5.000000e-02 5.000000e-02 +1.674500e+03 1.450000e+01 1.450000e+01 2.500000e-01 4.000000e-02 4.000000e-02 +1.714500e+03 1.450000e+01 1.450000e+01 2.000000e-01 4.000000e-02 4.000000e-02 +1.754500e+03 2.450000e+01 2.450000e+01 1.600000e-01 3.000000e-02 3.000000e-02 +1.804500e+03 2.450000e+01 2.450000e+01 3.000000e-02 2.000000e-02 2.000000e-02 +1.849500e+03 1.950000e+01 1.950000e+01 4.000000e-02 4.000000e-02 4.000000e-02 +1.894500e+03 2.450000e+01 2.450000e+01 5.000000e-02 4.000000e-02 4.000000e-02 +1.934500e+03 1.450000e+01 1.450000e+01 6.000000e-02 5.000000e-02 5.000000e-02 +1.959500e+03 9.500000e+00 9.500000e+00 5.000000e-02 8.000000e-02 8.000000e-02 +1.989500e+03 1.950000e+01 1.950000e+01 4.000000e-02 4.000000e-02 4.000000e-02 +2.024500e+03 1.450000e+01 1.450000e+01 6.000000e-02 4.000000e-02 4.000000e-02 +2.054500e+03 1.450000e+01 1.450000e+01 1.000000e-01 5.000000e-02 5.000000e-02 +2.084500e+03 1.450000e+01 1.450000e+01 5.000000e-02 3.000000e-02 3.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM2_1988_I264144.cc b/analyses/pluginOrsay/DM2_1988_I264144.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1988_I264144.cc @@ -0,0 +1,119 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM2_1988_I264144 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM2_1988_I264144); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _numEtaPiPi = bookCounter("TMP/EtaPiPi"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==221) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // eta pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _numEtaPiPi->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _numEtaPiPi->val(); + double error = _numEtaPiPi->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _numEtaPiPi; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM2_1988_I264144); + + +} diff --git a/analyses/pluginOrsay/DM2_1988_I264144.info b/analyses/pluginOrsay/DM2_1988_I264144.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1988_I264144.info @@ -0,0 +1,34 @@ +Name: DM2_1988_I264144 +Year: 1988 +Summary: Cross section for $e^+e^-\to\eta\pi^+\pi^-$ at energies between 1.35 and 2.4 GeV +Experiment: DM2 +Collider: DCI +InspireID: 264144 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B212 (1988) 133-138, 1988 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: +Description: + 'Measurement of the cross section for $e^+e^-\to\eta\pi^+\pi^-$ at energies between 1.35 and 2.4 GeV.' +Keywords: +BibKey: Antonelli:1988fw +BibTeX: '@article{Antonelli:1988fw, + author = "Antonelli, A. and others", + title = "{Measurement of the Reaction $e^+ e^- \to \eta \pi^+ + \pi^-$ in the Center-of-mass Energy Interval 1350-{MeV} to + 2400-{MeV}}", + collaboration = "DM2", + journal = "Phys. Lett.", + volume = "B212", + year = "1988", + pages = "133-138", + doi = "10.1016/0370-2693(88)91250-6", + reportNumber = "LAL-88-11", + SLACcitation = "%%CITATION = PHLTA,B212,133;%%" +}' diff --git a/analyses/pluginOrsay/DM2_1988_I264144.plot b/analyses/pluginOrsay/DM2_1988_I264144.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1988_I264144.plot @@ -0,0 +1,8 @@ +BEGIN PLOT /DM2_1988_I264144/d01-x01-y01 +Title=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \eta\pi^+\pi^-)$/nb +LogY=0 +LegendXPos=0.7 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM2_1988_I264144.yoda b/analyses/pluginOrsay/DM2_1988_I264144.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1988_I264144.yoda @@ -0,0 +1,27 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1988_I264144/d01-x01-y01 +IsRef: 1 +Path: /REF/DM2_1988_I264144/d01-x01-y01 +Title: doi:10.17182/hepdata.29912.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.350000e+03 0.000000e+00 0.000000e+00 1.940000e+00 7.700000e-01 7.700000e-01 +1.375000e+03 2.500000e+01 2.500000e+01 1.210000e+00 8.500000e-01 8.500000e-01 +1.425000e+03 2.500000e+01 2.500000e+01 1.070000e+00 6.000000e-01 6.000000e-01 +1.475000e+03 2.500000e+01 2.500000e+01 3.830000e+00 8.400000e-01 8.400000e-01 +1.525000e+03 2.500000e+01 2.500000e+01 3.770000e+00 8.600000e-01 8.600000e-01 +1.575000e+03 2.500000e+01 2.500000e+01 3.190000e+00 7.200000e-01 7.200000e-01 +1.625000e+03 2.500000e+01 2.500000e+01 1.340000e+00 3.400000e-01 3.400000e-01 +1.675000e+03 2.500000e+01 2.500000e+01 1.670000e+00 4.400000e-01 4.400000e-01 +1.725000e+03 2.500000e+01 2.500000e+01 1.270000e+00 3.900000e-01 3.900000e-01 +1.775000e+03 2.500000e+01 2.500000e+01 2.770000e+00 6.800000e-01 6.800000e-01 +1.825000e+03 2.500000e+01 2.500000e+01 9.000000e-01 3.200000e-01 3.200000e-01 +1.875000e+03 2.500000e+01 2.500000e+01 1.570000e+00 4.700000e-01 4.700000e-01 +1.925000e+03 2.500000e+01 2.500000e+01 2.100000e-01 2.800000e-01 2.800000e-01 +1.975000e+03 2.500000e+01 2.500000e+01 3.100000e-01 3.400000e-01 3.400000e-01 +2.025000e+03 2.500000e+01 2.500000e+01 3.800000e-01 2.500000e-01 2.500000e-01 +2.075000e+03 2.500000e+01 2.500000e+01 2.800000e-01 2.000000e-01 2.000000e-01 +2.125000e+03 2.500000e+01 2.500000e+01 1.600000e-01 1.800000e-01 1.800000e-01 +2.175000e+03 2.500000e+01 2.500000e+01 8.000000e-02 1.400000e-01 1.400000e-01 +2.400000e+03 0.000000e+00 0.000000e+00 2.200000e-01 1.100000e-01 1.100000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM2_1989_I267118.cc b/analyses/pluginOrsay/DM2_1989_I267118.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1989_I267118.cc @@ -0,0 +1,81 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM2_1989_I267118 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM2_1989_I267118); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _npion = bookCounter("TMP/pion"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + if(fs.particles().size()!=2) vetoEvent; + foreach (const Particle& p, fs.particles()) { + if(abs(p.pdgId())!=PID::PIPLUS) vetoEvent; + } + _npion->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _npion->val(); + double error = _npion->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _npion; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM2_1989_I267118); + + +} diff --git a/analyses/pluginOrsay/DM2_1989_I267118.info b/analyses/pluginOrsay/DM2_1989_I267118.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1989_I267118.info @@ -0,0 +1,31 @@ +Name: DM2_1989_I267118 +Year: 1989 +Summary: Cross section for $e^+e^-\to \pi^+\pi^-$ between 1.35 and 2.4 GeV +Experiment: DM2 +Collider: DCI +InspireID: 267118 +Status: VALIDATED +Authors: + - Peter Richardson +References: +- Phys.Lett. B220 (1989) 321-327, 1989 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e+, e-] +Description: + 'Measurement of the cross section for $e^+e^-\to \pi^+\pi^-$ at energies between 1.35 and 2.4 GeV. Useful for comparing models of the pion form factor.' +Keywords: +BibKey: Bisello:1988hq +BibTeX: '@article{Bisello:1988hq, + author = "Bisello, D. and others", + title = "{The Pion Electromagnetic Form-factor in the Timelike + Energy Range 1.35-{GeV} $\le \sqrt{s} \le$ 2.4-{GeV}}", + collaboration = "DM2", + journal = "Phys. Lett.", + volume = "B220", + year = "1989", + pages = "321-327", + doi = "10.1016/0370-2693(89)90060-9", + reportNumber = "LAL-88-47", + SLACcitation = "%%CITATION = PHLTA,B220,321;%%" +}' diff --git a/analyses/pluginOrsay/DM2_1989_I267118.plot b/analyses/pluginOrsay/DM2_1989_I267118.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1989_I267118.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /DM2_1989_I267118/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-)$/nb +ConnectGaps=1 +LogY=1 +END PLOT diff --git a/analyses/pluginOrsay/DM2_1989_I267118.yoda b/analyses/pluginOrsay/DM2_1989_I267118.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1989_I267118.yoda @@ -0,0 +1,50 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1989_I267118/d01-x01-y01 +IsRef: 1 +Path: /REF/DM2_1989_I267118/d01-x01-y01 +Title: doi:10.17182/hepdata.29829.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.350000e+00 0.000000e+00 0.000000e+00 5.880000e+00 1.066711e+00 1.066711e+00 +1.395000e+00 0.000000e+00 0.000000e+00 5.650000e+00 1.404487e+00 1.404487e+00 +1.425000e+00 0.000000e+00 0.000000e+00 2.130000e+00 5.350059e-01 5.350059e-01 +1.475000e+00 0.000000e+00 0.000000e+00 1.400000e+00 4.246457e-01 4.246457e-01 +1.525000e+00 0.000000e+00 0.000000e+00 6.900000e-01 4.084799e-01 4.084799e-01 +1.575000e+00 0.000000e+00 0.000000e+00 5.400000e-01 3.167002e-01 3.167002e-01 +1.625000e+00 0.000000e+00 0.000000e+00 6.000000e-01 1.846185e-01 1.846185e-01 +1.675000e+00 0.000000e+00 0.000000e+00 8.700000e-01 2.525854e-01 2.525854e-01 +1.725000e+00 0.000000e+00 0.000000e+00 2.330000e+00 4.962622e-01 4.962622e-01 +1.775000e+00 0.000000e+00 0.000000e+00 1.460000e+00 3.736242e-01 3.736242e-01 +1.825000e+00 0.000000e+00 0.000000e+00 1.950000e+00 4.895467e-01 4.895467e-01 +1.875000e+00 0.000000e+00 0.000000e+00 1.660000e+00 5.012790e-01 5.012790e-01 +1.925000e+00 0.000000e+00 0.000000e+00 1.180000e+00 3.683077e-01 3.683077e-01 +1.975000e+00 0.000000e+00 0.000000e+00 1.500000e-01 1.510761e-01 1.510761e-01 +2.025000e+00 0.000000e+00 0.000000e+00 5.500000e-01 2.201272e-01 2.201272e-01 +2.075000e+00 0.000000e+00 0.000000e+00 3.800000e-01 1.760095e-01 1.760095e-01 +2.125000e+00 0.000000e+00 0.000000e+00 3.200000e-01 1.645435e-01 1.645435e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1989_I267118/d01-x01-y02 +IsRef: 1 +Path: /REF/DM2_1989_I267118/d01-x01-y02 +Title: doi:10.17182/hepdata.29829.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.350000e+00 0.000000e+00 0.000000e+00 5.300000e-01 9.457780e-02 9.457780e-02 +1.395000e+00 0.000000e+00 0.000000e+00 5.400000e-01 1.363783e-01 1.363783e-01 +1.425000e+00 0.000000e+00 0.000000e+00 2.100000e-01 5.599143e-02 5.599143e-02 +1.475000e+00 0.000000e+00 0.000000e+00 1.500000e-01 4.386342e-02 4.386342e-02 +1.525000e+00 0.000000e+00 0.000000e+00 8.000000e-02 5.091326e-02 5.091326e-02 +1.575000e+00 0.000000e+00 0.000000e+00 6.000000e-02 4.064283e-02 4.064283e-02 +1.625000e+00 0.000000e+00 0.000000e+00 8.000000e-02 2.218468e-02 2.218468e-02 +1.675000e+00 0.000000e+00 0.000000e+00 1.200000e-01 3.327702e-02 3.327702e-02 +1.725000e+00 0.000000e+00 0.000000e+00 3.300000e-01 7.188992e-02 7.188992e-02 +1.775000e+00 0.000000e+00 0.000000e+00 2.200000e-01 5.654167e-02 5.654167e-02 +1.825000e+00 0.000000e+00 0.000000e+00 3.100000e-01 7.927068e-02 7.927068e-02 +1.875000e+00 0.000000e+00 0.000000e+00 2.800000e-01 8.676958e-02 8.676958e-02 +1.925000e+00 0.000000e+00 0.000000e+00 2.100000e-01 6.507718e-02 6.507718e-02 +1.975000e+00 0.000000e+00 0.000000e+00 3.000000e-02 3.021523e-02 3.021523e-02 +2.025000e+00 0.000000e+00 0.000000e+00 1.100000e-01 4.212173e-02 4.212173e-02 +2.075000e+00 0.000000e+00 0.000000e+00 8.000000e-02 3.149857e-02 3.149857e-02 +2.125000e+00 0.000000e+00 0.000000e+00 7.000000e-02 3.115381e-02 3.115381e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM2_1990_I297706.cc b/analyses/pluginOrsay/DM2_1990_I297706.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1990_I297706.cc @@ -0,0 +1,149 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM2_1990_I297706 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM2_1990_I297706); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _nProton= bookCounter( "/TMP/nProton" ); + _nLambda= bookCounter( "/TMP/nLambda" ); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + // total hadronic and muonic cross sections + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==2 && nCount[2212]==1 && nCount[-2212]==1) + _nProton->fill(event.weight()); + + // find the Lambdas + const FinalState& ufs = apply(event, "UFS"); + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + for(unsigned int iy=ix+1;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _nLambda->fill(event.weight()); + break; + } + } + if(matched) break; + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /picobarn; + for(unsigned int ix=1;ix<3;++ix) { + double sigma,error; + if(ix==1) { + sigma = _nProton->val()*fact; + error = _nProton->err()*fact; + } + else { + sigma = _nLambda->val()*fact; + error = _nLambda->err()*fact; + } + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + //@} + + /// @name Histograms + //@{ + CounterPtr _nProton,_nLambda; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM2_1990_I297706); + + +} diff --git a/analyses/pluginOrsay/DM2_1990_I297706.info b/analyses/pluginOrsay/DM2_1990_I297706.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1990_I297706.info @@ -0,0 +1,31 @@ +Name: DM2_1990_I297706 +Year: 1990 +Summary: Cross section for $e^+e^-\to p\bar{p}$ and $\Lambda\bar{\Lambda}$ at 2.4 GeV +Experiment: DM2 +Collider: DCI +InspireID: 297706 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C48 (1990) 23-28, 1990 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Description: + 'Measurement of the cross section for $e^+e^-\to p\bar{p}$ and $\Lambda\bar{\Lambda}$ at 2.4 GeV.' +Keywords: +BibKey: Bisello:1990rf +BibTeX: '@article{Bisello:1990rf, + author = "Bisello, D. and others", + title = "{Baryon pair production in e+ e- annihilation at S**(1/2) + = 2.4-GeV}", + collaboration = "DM2", + journal = "Z. Phys.", + volume = "C48", + year = "1990", + pages = "23-28", + doi = "10.1007/BF01565602", + reportNumber = "LAL-90-13", + SLACcitation = "%%CITATION = ZEPYA,C48,23;%%" +}' diff --git a/analyses/pluginOrsay/DM2_1990_I297706.plot b/analyses/pluginOrsay/DM2_1990_I297706.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1990_I297706.plot @@ -0,0 +1,16 @@ +BEGIN PLOT /DM2_1990_I297706/d01-x01-y01 +Title=$\sigma(e^+e^-\to p\bar{p})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to p\bar{p})$/pb +ConnectGaps=1 +XMin=2. +XMax=3. +END PLOT +BEGIN PLOT /DM2_1990_I297706/d02-x01-y01 +Title=$\sigma(e^+e^-\to \Lambda\bar{\Lambda})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \Lambda\bar{\Lambda})$/pb +ConnectGaps=1 +XMin=2. +XMax=3. +END PLOT \ No newline at end of file diff --git a/analyses/pluginOrsay/DM2_1990_I297706.yoda b/analyses/pluginOrsay/DM2_1990_I297706.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1990_I297706.yoda @@ -0,0 +1,42 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1990_I297706/d01-x01-y01 +IsRef: 1 +Path: /REF/DM2_1990_I297706/d01-x01-y01 +Title: doi:10.17182/hepdata.15128.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.386000e+00 0.000000e+00 0.000000e+00 8.600000e+01 2.700000e+01 3.600000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1990_I297706/d02-x01-y01 +IsRef: 1 +Path: /REF/DM2_1990_I297706/d02-x01-y01 +Title: doi:10.17182/hepdata.15128.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.386000e+00 0.000000e+00 0.000000e+00 1.000000e+02 3.500000e+01 6.500000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1990_I297706/d03-x01-y01 +IsRef: 1 +Path: /REF/DM2_1990_I297706/d03-x01-y01 +Title: doi:10.17182/hepdata.15128.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1990_I297706/d04-x01-y01 +IsRef: 1 +Path: /REF/DM2_1990_I297706/d04-x01-y01 +Title: doi:10.17182/hepdata.15128.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1990_I297706/d05-x01-y01 +IsRef: 1 +Path: /REF/DM2_1990_I297706/d05-x01-y01 +Title: doi:10.17182/hepdata.15128.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM2_1991_I318558.cc b/analyses/pluginOrsay/DM2_1991_I318558.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1991_I318558.cc @@ -0,0 +1,95 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM2_1991_I318558 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM2_1991_I318558); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + // Book histograms + for(unsigned int ix=1;ix<3;++ix) { + stringstream ss; + ss << "TMP/n" << ix; + _nMeson[ix]= bookCounter(ss.str()); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal!=3) vetoEvent; + if(nCount[310]==1 && + ((nCount[ 211]==1&&nCount[-321]==1)|| + (nCount[-211]==1&&nCount[ 321]==1))) + _nMeson[1]->fill(event.weight()); + else if(nCount[321]==1 && + nCount[-321]==1 && nCount[111]==1) + _nMeson[2]->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma = _nMeson[ix]->val(); + double error = _nMeson[ix]->err(); + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nMeson[3]; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM2_1991_I318558); + + +} diff --git a/analyses/pluginOrsay/DM2_1991_I318558.info b/analyses/pluginOrsay/DM2_1991_I318558.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1991_I318558.info @@ -0,0 +1,33 @@ +Name: DM2_1991_I318558 +Year: 1991 +Summary: Cross section for $e^+e^-\to$ $K^+K^-\pi^0$ and $K^0_SK^\pm\pi^\mp$ for energies from 1.3 to 2.2 GeV +Experiment: DM2 +Collider: DCI +InspireID: 318558 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C52 (1991) 227-230, 1991 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to$ $K^+K^-\pi^0$ and $K^0_SK^\pm\pi^\mp$ + for energies from 1.3 to 2.2 GeV.' +Keywords: +BibKey: Bisello:1991kd +BibTeX: '@article{Bisello:1991kd, + author = "Bisello, D. and others", + title = "{Observation of an isoscalar vector meson at + approximately = 1650-MeV/c**2 in the e+ e- ---> K anti-K + pi reaction}", + journal = "Z. Phys.", + volume = "C52", + year = "1991", + pages = "227-230", + doi = "10.1007/BF01560440", + reportNumber = "LAL-91-24", + SLACcitation = "%%CITATION = ZEPYA,C52,227;%%" +}' diff --git a/analyses/pluginOrsay/DM2_1991_I318558.plot b/analyses/pluginOrsay/DM2_1991_I318558.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1991_I318558.plot @@ -0,0 +1,13 @@ +BEGIN PLOT /DM2_1991_I318558/d01-x01-y01 +Title=$\sigma(e^+e^-\to K^0_SK^\pm \pi^\mp)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^0_SK^\pm \pi^\mp)$/nb +ConnectGaps=1 +END PLOT + +BEGIN PLOT /DM2_1991_I318558/d02-x01-y01 +Title=$\sigma(e^+e^-\to K^+K^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to K^+K^-\pi^0)$/nb +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginOrsay/DM2_1991_I318558.yoda b/analyses/pluginOrsay/DM2_1991_I318558.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1991_I318558.yoda @@ -0,0 +1,47 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1991_I318558/d01-x01-y01 +IsRef: 1 +Path: /REF/DM2_1991_I318558/d01-x01-y01 +Title: doi:10.17182/hepdata.14928.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.340000e+03 0.000000e+00 0.000000e+00 2.500000e-01 2.500000e-01 2.500000e-01 +1.420000e+03 0.000000e+00 0.000000e+00 5.400000e-01 3.000000e-01 3.000000e-01 +1.460000e+03 0.000000e+00 0.000000e+00 1.880000e+00 7.800000e-01 7.800000e-01 +1.500000e+03 0.000000e+00 0.000000e+00 1.010000e+00 4.200000e-01 4.200000e-01 +1.540000e+03 0.000000e+00 0.000000e+00 2.350000e+00 7.900000e-01 7.900000e-01 +1.580000e+03 0.000000e+00 0.000000e+00 2.500000e+00 7.000000e-01 7.000000e-01 +1.620000e+03 0.000000e+00 0.000000e+00 4.300000e+00 8.000000e-01 8.000000e-01 +1.660000e+03 0.000000e+00 0.000000e+00 3.770000e+00 6.500000e-01 6.500000e-01 +1.700000e+03 0.000000e+00 0.000000e+00 3.250000e+00 6.500000e-01 6.500000e-01 +1.740000e+03 0.000000e+00 0.000000e+00 2.560000e+00 6.100000e-01 6.100000e-01 +1.780000e+03 0.000000e+00 0.000000e+00 2.210000e+00 6.900000e-01 6.900000e-01 +1.820000e+03 0.000000e+00 0.000000e+00 1.190000e+00 3.900000e-01 3.900000e-01 +1.860000e+03 0.000000e+00 0.000000e+00 8.100000e-01 3.700000e-01 3.700000e-01 +1.900000e+03 0.000000e+00 0.000000e+00 1.330000e+00 5.300000e-01 5.300000e-01 +1.940000e+03 0.000000e+00 0.000000e+00 5.500000e-01 3.500000e-01 3.500000e-01 +1.980000e+03 0.000000e+00 0.000000e+00 1.220000e+00 5.600000e-01 5.600000e-01 +2.020000e+03 0.000000e+00 0.000000e+00 8.000000e-01 3.400000e-01 3.400000e-01 +2.040000e+03 0.000000e+00 0.000000e+00 1.120000e+00 4.000000e-01 4.000000e-01 +2.100000e+03 0.000000e+00 0.000000e+00 5.300000e-01 3.000000e-01 3.000000e-01 +2.140000e+03 0.000000e+00 0.000000e+00 1.220000e+00 4.200000e-01 4.200000e-01 +2.180000e+03 0.000000e+00 0.000000e+00 1.050000e+00 3.700000e-01 3.700000e-01 +2.220000e+03 0.000000e+00 0.000000e+00 1.050000e+00 4.700000e-01 4.700000e-01 +2.260000e+03 0.000000e+00 0.000000e+00 1.120000e+00 1.120000e+00 1.120000e+00 +2.380000e+03 0.000000e+00 0.000000e+00 7.700000e-01 2.300000e-01 2.300000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1991_I318558/d02-x01-y01 +IsRef: 1 +Path: /REF/DM2_1991_I318558/d02-x01-y01 +Title: doi:10.17182/hepdata.14928.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.480000e+03 0.000000e+00 0.000000e+00 3.600000e-01 2.400000e-01 7.200000e-01 +1.550000e+03 0.000000e+00 0.000000e+00 7.300000e-01 5.300000e-01 1.490000e+00 +1.610000e+03 0.000000e+00 0.000000e+00 1.080000e+00 4.600000e-01 5.400000e-01 +1.670000e+03 0.000000e+00 0.000000e+00 4.300000e-01 2.200000e-01 2.700000e-01 +1.730000e+03 0.000000e+00 0.000000e+00 3.200000e-01 2.200000e-01 4.000000e-01 +1.790000e+03 0.000000e+00 0.000000e+00 1.500000e-01 1.500000e-01 3.400000e-01 +1.860000e+03 0.000000e+00 0.000000e+00 6.100000e-01 2.500000e-01 3.300000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginOrsay/DM2_1992_I339265.cc b/analyses/pluginOrsay/DM2_1992_I339265.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1992_I339265.cc @@ -0,0 +1,133 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class DM2_1992_I339265 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(DM2_1992_I339265); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _n3pi = bookCounter("TMP/3pi"); + _nomega = bookCounter("TMP/omega"); + } + + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + --nRes[child.pdgId()]; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + if(ntotal==3 && nCount[211] == 1 && nCount[-211] == 1 && nCount[111] == 1) + _n3pi->fill(event.weight()); + + const FinalState& ufs = apply(event, "UFS"); + foreach (const Particle& p, ufs.particles()) { + if(p.children().empty()) continue; + // find the omega + if(p.pdgId()==223) { + map nRes = nCount; + int ncount = ntotal; + findChildren(p,nRes,ncount); + // omega pi+pi- + if(ncount!=2) continue; + bool matched = true; + for(auto const & val : nRes) { + if(abs(val.first)==211) { + if(val.second !=1) { + matched = false; + break; + } + } + else if(val.second!=0) { + matched = false; + break; + } + } + if(matched) + _nomega->fill(event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma = 0., error = 0.; + if(ix==1) { + sigma = _n3pi->val(); + error = _n3pi->err(); + } + else if(ix==2) { + sigma = _nomega->val(); + error = _nomega->err(); + } + sigma *= crossSection()/ sumOfWeights() /nanobarn; + error *= crossSection()/ sumOfWeights() /nanobarn; + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/MeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _n3pi,_nomega; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(DM2_1992_I339265); + + +} diff --git a/analyses/pluginOrsay/DM2_1992_I339265.info b/analyses/pluginOrsay/DM2_1992_I339265.info new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1992_I339265.info @@ -0,0 +1,32 @@ +Name: DM2_1992_I339265 +Year: 1992 +Summary: Cross section for $e^+e^-\to\pi^+\pi^-\pi^0$ and $\omega\pi^+\pi^-$ at energies between 1.35 and 2.4 GeV +Experiment: DM2 +Collider: DCI +InspireID: 339265 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C56 (1992) 15-20, 1992 +RunInfo: e+e- to hadrons +NeedCrossSection: yes +Beams: [e+,e-] +Luminosity_fb: +Description: + 'Measurement of the cross section for $e^+e^-\to\pi^+\pi^-\pi^0$ and $\omega\pi^+\pi^-$ at energies between 1.35 and 2.4 GeV.' +BibKey: Antonelli:1992jx +BibTeX: '@article{Antonelli:1992jx, + author = "Antonelli, A. and others", + title = "{Measurement of the e+ e- ---> pi+ pi- pi0 and e+ e- ---> + omega pi+ pi- reactions in the energy interval 1350-MeV - + 2400-MeV}", + collaboration = "DM2", + journal = "Z. Phys.", + volume = "C56", + year = "1992", + pages = "15-20", + doi = "10.1007/BF01589702", + reportNumber = "LAL-92-08", + SLACcitation = "%%CITATION = ZEPYA,C56,15;%%" +}' diff --git a/analyses/pluginOrsay/DM2_1992_I339265.plot b/analyses/pluginOrsay/DM2_1992_I339265.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1992_I339265.plot @@ -0,0 +1,12 @@ +BEGIN PLOT /DM2_1992_I339265/d01-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\pi^0)$/nb +ConnectGaps=1 +END PLOT +BEGIN PLOT /DM2_1992_I339265/d02-x01-y01 +Title=$\sigma(e^+e^-\to \pi^+\pi^-\omega)$ +XLabel=$\sqrt{s}$/MeV +YLabel=$\sigma(e^+e^-\to \pi^+\pi^-\omega)$/nb +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginOrsay/DM2_1992_I339265.yoda b/analyses/pluginOrsay/DM2_1992_I339265.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginOrsay/DM2_1992_I339265.yoda @@ -0,0 +1,56 @@ +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1992_I339265/d01-x01-y01 +IsRef: 1 +Path: /REF/DM2_1992_I339265/d01-x01-y01 +Title: doi:10.17182/hepdata.14555.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.340000e+03 0.000000e+00 0.000000e+00 3.360000e+00 7.900000e-01 7.900000e-01 +1.395000e+03 5.000000e+00 5.000000e+00 1.620000e+00 7.400000e-01 7.400000e-01 +1.425000e+03 2.500000e+01 2.500000e+01 2.590000e+00 5.700000e-01 5.700000e-01 +1.475000e+03 2.500000e+01 2.500000e+01 2.190000e+00 5.100000e-01 5.100000e-01 +1.525000e+03 2.500000e+01 2.500000e+01 1.260000e+00 4.700000e-01 4.700000e-01 +1.575000e+03 2.500000e+01 2.500000e+01 1.940000e+00 4.300000e-01 4.300000e-01 +1.625000e+03 2.500000e+01 2.500000e+01 2.240000e+00 3.000000e-01 3.000000e-01 +1.675000e+03 2.500000e+01 2.500000e+01 1.260000e+00 2.600000e-01 2.600000e-01 +1.725000e+03 2.500000e+01 2.500000e+01 6.400000e-01 2.100000e-01 2.100000e-01 +1.775000e+03 2.500000e+01 2.500000e+01 7.100000e-01 3.000000e-01 3.000000e-01 +1.825000e+03 2.500000e+01 2.500000e+01 3.800000e-01 1.700000e-01 1.700000e-01 +1.875000e+03 2.500000e+01 2.500000e+01 5.000000e-01 2.100000e-01 2.100000e-01 +1.925000e+03 2.500000e+01 2.500000e+01 3.900000e-01 2.000000e-01 2.000000e-01 +1.975000e+03 2.500000e+01 2.500000e+01 5.400000e-01 3.000000e-01 3.000000e-01 +2.025000e+03 2.500000e+01 2.500000e+01 1.600000e-01 1.100000e-01 1.100000e-01 +2.075000e+03 2.500000e+01 2.500000e+01 2.800000e-01 1.500000e-01 1.500000e-01 +2.125000e+03 2.500000e+01 2.500000e+01 3.000000e-01 1.400000e-01 1.400000e-01 +2.175000e+03 2.500000e+01 2.500000e+01 2.300000e-01 1.600000e-01 1.600000e-01 +2.222500e+03 2.250000e+01 2.250000e+01 0.000000e+00 1.000000e-01 1.000000e-01 +2.400000e+03 0.000000e+00 0.000000e+00 2.500000e-01 9.000000e-02 9.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/DM2_1992_I339265/d02-x01-y01 +IsRef: 1 +Path: /REF/DM2_1992_I339265/d02-x01-y01 +Title: doi:10.17182/hepdata.14555.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.340000e+03 0.000000e+00 0.000000e+00 6.000000e-02 1.700000e-01 1.700000e-01 +1.395000e+03 5.000000e+00 5.000000e+00 2.100000e-01 2.700000e-01 2.700000e-01 +1.425000e+03 2.500000e+01 2.500000e+01 5.100000e-01 2.300000e-01 2.300000e-01 +1.475000e+03 2.500000e+01 2.500000e+01 6.700000e-01 2.400000e-01 2.400000e-01 +1.525000e+03 2.500000e+01 2.500000e+01 1.160000e+00 3.200000e-01 3.200000e-01 +1.575000e+03 2.500000e+01 2.500000e+01 1.310000e+00 3.000000e-01 3.000000e-01 +1.625000e+03 2.500000e+01 2.500000e+01 2.220000e+00 2.700000e-01 2.700000e-01 +1.675000e+03 2.500000e+01 2.500000e+01 2.080000e+00 2.700000e-01 2.700000e-01 +1.725000e+03 2.500000e+01 2.500000e+01 1.460000e+00 2.400000e-01 2.400000e-01 +1.775000e+03 2.500000e+01 2.500000e+01 1.790000e+00 4.000000e-01 4.000000e-01 +1.825000e+03 2.500000e+01 2.500000e+01 1.060000e+00 2.300000e-01 2.300000e-01 +1.875000e+03 2.500000e+01 2.500000e+01 8.400000e-01 2.500000e-01 2.500000e-01 +1.925000e+03 2.500000e+01 2.500000e+01 6.100000e-01 2.100000e-01 2.100000e-01 +1.975000e+03 2.500000e+01 2.500000e+01 5.900000e-01 2.500000e-01 2.500000e-01 +2.025000e+03 2.500000e+01 2.500000e+01 3.900000e-01 1.500000e-01 1.500000e-01 +2.075000e+03 2.500000e+01 2.500000e+01 3.300000e-01 1.300000e-01 1.300000e-01 +2.125000e+03 2.500000e+01 2.500000e+01 2.100000e-01 1.100000e-01 1.100000e-01 +2.175000e+03 2.500000e+01 2.500000e+01 3.300000e-01 1.500000e-01 1.500000e-01 +2.222500e+03 2.250000e+01 2.250000e+01 1.100000e-01 1.400000e-01 1.400000e-01 +2.400000e+03 0.000000e+00 0.000000e+00 2.400000e-01 1.900000e-01 1.900000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/CELLO_1981_I166365.cc b/analyses/pluginPetra/CELLO_1981_I166365.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1981_I166365.cc @@ -0,0 +1,102 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CELLO_1981_I166365 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CELLO_1981_I166365); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else { + _c_hadrons->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CELLO_1981_I166365); + + +} diff --git a/analyses/pluginPetra/CELLO_1981_I166365.info b/analyses/pluginPetra/CELLO_1981_I166365.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1981_I166365.info @@ -0,0 +1,29 @@ +Name: CELLO_1981_I166365 +Year: 1981 +Summary: Measurement of $R$ for energies between 33 and 36.7 GeV +Experiment: CELLO +Collider: PETRA +InspireID: 166365 +Status: VALIDATED +Authors: + - Peter Richardson +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 14 and 46.6 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Behrend:1981sy +BibTeX: '@article{Behrend:1981sy, + author = "Behrend, H. J. and others", + title = "{SEARCH FOR NARROW QUARKONIUM STATES AND PAIR PRODUCTION + OF NEW HEAVY QUARKS AT c.m. ENERGIES FROM 33-GeV TO + 36.7-GeV}", + collaboration = "CELLO", + journal = "Submitted to: Phys. Lett. B", + year = "1981", + reportNumber = "DESY-81-029", + SLACcitation = "%%CITATION = DESY-81-029;%%" +}' diff --git a/analyses/pluginPetra/CELLO_1981_I166365.plot b/analyses/pluginPetra/CELLO_1981_I166365.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1981_I166365.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /CELLO_1981_I166365/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CELLO_1981_I166365/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CELLO_1981_I166365/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/CELLO_1981_I166365.yoda b/analyses/pluginPetra/CELLO_1981_I166365.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1981_I166365.yoda @@ -0,0 +1,9 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CELLO_1981_I166365/d01-x01-y01 +IsRef: 1 +Path: /REF/CELLO_1981_I166365/d01-x01-y01 +Title: doi:10.17182/hepdata.45222.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.486000e+01 1.860000e+00 1.860000e+00 3.850000e+00 3.324154e-01 3.324154e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/CELLO_1984_I202783.cc b/analyses/pluginPetra/CELLO_1984_I202783.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1984_I202783.cc @@ -0,0 +1,102 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CELLO_1984_I202783 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CELLO_1984_I202783); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else { + _c_hadrons->fill(event.weight()); + } + + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(2, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(2, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CELLO_1984_I202783); + + +} diff --git a/analyses/pluginPetra/CELLO_1984_I202783.info b/analyses/pluginPetra/CELLO_1984_I202783.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1984_I202783.info @@ -0,0 +1,33 @@ +Name: CELLO_1984_I202783 +Year: 1984 +Summary: Measurement of $R$ for energies between 33 and 47 GeV +Experiment: CELLO +Collider: PETRA +InspireID: 202783 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B144 (1984) 297-301, 1984 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 33 and 47 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Behrend:1984ub +BibTeX: '@article{Behrend:1984ub, + author = "Behrend, H. J. and others", + title = "{Search for New Heavy Quarks in $e^+ e^-$ Collisions Up + to 46.78-{GeV} Center-of-mass Energy}", + collaboration = "CELLO", + journal = "Phys. Lett.", + volume = "144B", + year = "1984", + pages = "297-301", + doi = "10.1016/0370-2693(84)91824-0", + reportNumber = "DESY-84-051", + SLACcitation = "%%CITATION = PHLTA,144B,297;%%" +}' diff --git a/analyses/pluginPetra/CELLO_1984_I202783.plot b/analyses/pluginPetra/CELLO_1984_I202783.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1984_I202783.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /CELLO_1984_I202783/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CELLO_1984_I202783/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CELLO_1984_I202783/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/CELLO_1984_I202783.yoda b/analyses/pluginPetra/CELLO_1984_I202783.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1984_I202783.yoda @@ -0,0 +1,18 @@ +BEGIN YODA_SCATTER1D_V2 /REF/CELLO_1984_I202783/d01-x01-y01 +IsRef: 1 +Path: /REF/CELLO_1984_I202783/d01-x01-y01 +Title: doi:10.17182/hepdata.30514.v1/t1 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CELLO_1984_I202783/d02-x01-y01 +IsRef: 1 +Path: /REF/CELLO_1984_I202783/d02-x01-y01 +Title: doi:10.17182/hepdata.30514.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.486000e+01 1.860000e+00 1.860000e+00 3.850000e+00 3.324154e-01 3.324154e-01 +4.272000e+01 4.060000e+00 4.060000e+00 4.040000e+00 3.257299e-01 3.257299e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/CELLO_1987_I236981.cc b/analyses/pluginPetra/CELLO_1987_I236981.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1987_I236981.cc @@ -0,0 +1,102 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CELLO_1987_I236981 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CELLO_1987_I236981); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(FinalState(), "FS"); + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else { + _c_hadrons->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CELLO_1987_I236981); + + +} diff --git a/analyses/pluginPetra/CELLO_1987_I236981.info b/analyses/pluginPetra/CELLO_1987_I236981.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1987_I236981.info @@ -0,0 +1,34 @@ +Name: CELLO_1987_I236981 +Year: 1987 +Summary: Measurement of $R$ for energies between 14 and 46.6 GeV +Experiment: CELLO +Collider: PETRA +InspireID: 236981 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B183 (1987) 400-411, 1987 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 14 and 46.6 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Behrend:1986md +BibTeX: '@article{Behrend:1986md, + author = "Behrend, H. J. and others", + title = "{Determination of alpha-s and sin**2theta(w) from + Measurements of the Total Hadronic Cross-Section in e+ e- + Annihilation}", + collaboration = "CELLO", + journal = "Phys. Lett.", + volume = "B183", + year = "1987", + pages = "400-411", + doi = "10.1016/0370-2693(87)90986-5", + reportNumber = "DESY-86-133", + SLACcitation = "%%CITATION = PHLTA,B183,400;%%" +}' diff --git a/analyses/pluginPetra/CELLO_1987_I236981.plot b/analyses/pluginPetra/CELLO_1987_I236981.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1987_I236981.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /CELLO_1987_I236981/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CELLO_1987_I236981/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CELLO_1987_I236981/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/CELLO_1987_I236981.yoda b/analyses/pluginPetra/CELLO_1987_I236981.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/CELLO_1987_I236981.yoda @@ -0,0 +1,53 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CELLO_1987_I236981/d01-x01-y01 +IsRef: 1 +Path: /REF/CELLO_1987_I236981/d01-x01-y01 +Title: doi:10.17182/hepdata.30231.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.400000e+01 0.000000e+00 0.000000e+00 4.100000e+00 1.555635e-01 1.555635e-01 +2.200000e+01 0.000000e+00 0.000000e+00 3.860000e+00 1.562050e-01 1.562050e-01 +3.380000e+01 0.000000e+00 0.000000e+00 3.740000e+00 1.414214e-01 1.414214e-01 +3.830000e+01 0.000000e+00 0.000000e+00 3.890000e+00 1.345362e-01 1.345362e-01 +4.150000e+01 0.000000e+00 0.000000e+00 4.030000e+00 1.972308e-01 1.972308e-01 +4.350000e+01 0.000000e+00 0.000000e+00 3.970000e+00 1.204159e-01 1.204159e-01 +4.420000e+01 0.000000e+00 0.000000e+00 4.010000e+00 1.280625e-01 1.280625e-01 +4.600000e+01 0.000000e+00 0.000000e+00 4.090000e+00 2.325941e-01 2.325941e-01 +4.660000e+01 0.000000e+00 0.000000e+00 4.200000e+00 3.736308e-01 3.736308e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CELLO_1987_I236981/d02-x01-y01 +IsRef: 1 +Path: /REF/CELLO_1987_I236981/d02-x01-y01 +Title: doi:10.17182/hepdata.30231.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.400000e+01 0.000000e+00 0.000000e+00 1.900000e-01 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CELLO_1987_I236981/d02-x01-y02 +IsRef: 1 +Path: /REF/CELLO_1987_I236981/d02-x01-y02 +Title: doi:10.17182/hepdata.30231.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.400000e+01 0.000000e+00 0.000000e+00 2.000000e-01 3.000000e-02 3.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CELLO_1987_I236981/d02-x01-y03 +IsRef: 1 +Path: /REF/CELLO_1987_I236981/d02-x01-y03 +Title: doi:10.17182/hepdata.30231.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.400000e+01 0.000000e+00 0.000000e+00 1.650000e-01 3.000000e-02 3.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CELLO_1987_I236981/d02-x01-y04 +IsRef: 1 +Path: /REF/CELLO_1987_I236981/d02-x01-y04 +Title: doi:10.17182/hepdata.30231.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.400000e+01 0.000000e+00 0.000000e+00 2.360000e-01 2.000000e-02 2.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/JADE_1979_I142874.cc b/analyses/pluginPetra/JADE_1979_I142874.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/JADE_1979_I142874.cc @@ -0,0 +1,75 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/ChargedFinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class JADE_1979_I142874 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(JADE_1979_I142874); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(ChargedFinalState(), "FS"); + + // Book histograms + _nHadrons= bookCounter("TMP/hadrons"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const ChargedFinalState& fs = apply(event, "FS"); + _nHadrons->fill(fs.particles().size()*event.weight()); + + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nHadrons->val()/sumOfWeights(); + double error = _nHadrons->err()/sumOfWeights(); + Scatter2D temphisto(refData(2, 1, 1)); + Scatter2DPtr mult = bookScatter2D(2, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + //@} + + + /// @name Histograms + //@{ + CounterPtr _nHadrons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(JADE_1979_I142874); + + +} diff --git a/analyses/pluginPetra/JADE_1979_I142874.info b/analyses/pluginPetra/JADE_1979_I142874.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/JADE_1979_I142874.info @@ -0,0 +1,32 @@ +Name: JADE_1979_I142874 +Year: 1979 +Summary: Charged hadron multiplicity +Experiment: JADE +Collider: PETRA +InspireID: 142874 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B88 (1979) 171-176, 1979 +RunInfo: e+e- to hadrons +NeedCrossSection: no +Beams: [e-, e+] +Energies: [22,27.7,30,31.6] +Description: + 'Charged hadrom multiplcity at a range of energies, use with care as its not clear if $K_S^0$ decays are included of not, within the systematic error of 1.5' +Keywords: [] +BibKey: Bartel:1979zn +BibTeX: '@article{Bartel:1979zn, + author = "Bartel, W. and others", + title = "{Total Cross-Section for Hadron Production by e+ e- + Annihilation at PETRA Energies}", + collaboration = "JADE", + journal = "Phys. Lett.", + volume = "88B", + year = "1979", + pages = "171-176", + doi = "10.1016/0370-2693(79)90139-4", + reportNumber = "DESY-79-64", + SLACcitation = "%%CITATION = PHLTA,88B,171;%%" +}' diff --git a/analyses/pluginPetra/JADE_1979_I142874.plot b/analyses/pluginPetra/JADE_1979_I142874.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/JADE_1979_I142874.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /JADE_1979_I142874/d02-x01-y01 +Title=Charged hadron multiplicity +XLabel=$\sqrt{s}$/GeV +YLabel="$N_{\text{charged}}$ +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/JADE_1979_I142874.yoda b/analyses/pluginPetra/JADE_1979_I142874.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/JADE_1979_I142874.yoda @@ -0,0 +1,24 @@ +BEGIN YODA_SCATTER2D_V2 /REF/JADE_1979_I142874/d01-x01-y01 +IsRef: 1 +Path: /REF/JADE_1979_I142874/d01-x01-y01 +Title: doi:10.17182/hepdata.27277.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.200000e+01 0.000000e+00 0.000000e+00 2.900000e+00 7.000000e-01 7.000000e-01 +2.770000e+01 0.000000e+00 0.000000e+00 4.000000e+00 5.000000e-01 5.000000e-01 +3.000000e+01 0.000000e+00 0.000000e+00 4.600000e+00 4.000000e-01 4.000000e-01 +3.160000e+01 0.000000e+00 0.000000e+00 4.200000e+00 6.000000e-01 6.000000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/JADE_1979_I142874/d02-x01-y01 +IsRef: 1 +Path: /REF/JADE_1979_I142874/d02-x01-y01 +Title: doi:10.17182/hepdata.27277.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.200000e+01 0.000000e+00 0.000000e+00 1.010000e+01 7.000000e-01 7.000000e-01 +2.770000e+01 0.000000e+00 0.000000e+00 1.160000e+01 5.000000e-01 5.000000e-01 +3.000000e+01 0.000000e+00 0.000000e+00 1.170000e+01 5.000000e-01 5.000000e-01 +3.160000e+01 0.000000e+00 0.000000e+00 1.090000e+01 6.000000e-01 6.000000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/JADE_1987_I234905.cc b/analyses/pluginPetra/JADE_1987_I234905.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/JADE_1987_I234905.cc @@ -0,0 +1,101 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class JADE_1987_I234905 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(JADE_1987_I234905); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else { + _c_hadrons->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(JADE_1987_I234905); + + +} diff --git a/analyses/pluginPetra/JADE_1987_I234905.info b/analyses/pluginPetra/JADE_1987_I234905.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/JADE_1987_I234905.info @@ -0,0 +1,31 @@ +Name: JADE_1987_I234905 +Year: 1987 +Summary: Measurement of $R$ for energies between 12 and 46.47 GeV +Experiment: JADE +Collider: PETRA +InspireID: 234905 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rept. 148 (1987) 67, 1987 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 12 and 46.47 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Naroska:1986si +BibTeX: '@article{Naroska:1986si, + author = "Naroska, B.", + title = "{E+ e- Physics with the JADE Detector at PETRA}", + journal = "Phys. Rept.", + volume = "148", + year = "1987", + pages = "67", + doi = "10.1016/0370-1573(87)90031-7", + reportNumber = "DESY-86-113", + SLACcitation = "%%CITATION = PRPLC,148,67;%%" +}' diff --git a/analyses/pluginPetra/JADE_1987_I234905.plot b/analyses/pluginPetra/JADE_1987_I234905.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/JADE_1987_I234905.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /JADE_1987_I234905/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /JADE_1987_I234905/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /JADE_1987_I234905/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/JADE_1987_I234905.yoda b/analyses/pluginPetra/JADE_1987_I234905.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/JADE_1987_I234905.yoda @@ -0,0 +1,28 @@ +BEGIN YODA_SCATTER2D_V2 /REF/JADE_1987_I234905/d01-x01-y01 +IsRef: 1 +Path: /REF/JADE_1987_I234905/d01-x01-y01 +Title: doi:10.17182/hepdata.45203.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 3.450000e+00 2.824108e-01 2.824108e-01 +1.404000e+01 0.000000e+00 0.000000e+00 3.940000e+00 1.689426e-01 1.689426e-01 +2.200000e+01 0.000000e+00 0.000000e+00 4.110000e+00 1.631865e-01 1.631865e-01 +2.501000e+01 0.000000e+00 0.000000e+00 4.240000e+00 3.073355e-01 3.073355e-01 +2.766000e+01 0.000000e+00 0.000000e+00 3.850000e+00 4.888126e-01 4.888126e-01 +2.993000e+01 0.000000e+00 0.000000e+00 3.550000e+00 4.089732e-01 4.089732e-01 +3.038000e+01 0.000000e+00 0.000000e+00 3.850000e+00 2.112765e-01 2.112765e-01 +3.129000e+01 0.000000e+00 0.000000e+00 3.830000e+00 2.947020e-01 2.947020e-01 +3.389000e+01 0.000000e+00 0.000000e+00 4.160000e+00 1.413083e-01 1.413083e-01 +3.450000e+01 0.000000e+00 0.000000e+00 3.930000e+00 2.211250e-01 2.211250e-01 +3.501000e+01 0.000000e+00 0.000000e+00 3.930000e+00 1.374637e-01 1.374637e-01 +3.545000e+01 0.000000e+00 0.000000e+00 3.930000e+00 2.032148e-01 2.032148e-01 +3.638000e+01 0.000000e+00 0.000000e+00 3.710000e+00 2.280967e-01 2.280967e-01 +4.032000e+01 0.000000e+00 0.000000e+00 4.050000e+00 2.172282e-01 2.172282e-01 +4.118000e+01 0.000000e+00 0.000000e+00 4.210000e+00 2.457265e-01 2.457265e-01 +4.255000e+01 0.000000e+00 0.000000e+00 4.200000e+00 2.456107e-01 2.456107e-01 +4.353000e+01 0.000000e+00 0.000000e+00 4.000000e+00 2.254240e-01 2.254240e-01 +4.441000e+01 0.000000e+00 0.000000e+00 3.980000e+00 2.251846e-01 2.251846e-01 +4.559000e+01 0.000000e+00 0.000000e+00 4.400000e+00 2.479664e-01 2.479664e-01 +4.647000e+01 0.000000e+00 0.000000e+00 4.040000e+00 2.619798e-01 2.619798e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/MARKJ_1979_I141976.cc b/analyses/pluginPetra/MARKJ_1979_I141976.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1979_I141976.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKJ_1979_I141976 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKJ_1979_I141976); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKJ_1979_I141976); + + +} diff --git a/analyses/pluginPetra/MARKJ_1979_I141976.info b/analyses/pluginPetra/MARKJ_1979_I141976.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1979_I141976.info @@ -0,0 +1,32 @@ +Name: MARKJ_1979_I141976 +Year: 1979 +Summary: Measurement of $R$ at 31.57 GeV +Experiment: MARKJ +Collider: PETRA +InspireID: 141976 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B85 (1979) 463-466, 1979 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by MARKJ for 31.57 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Barber:1979ru +BibTeX: '@article{Barber:1979ru, + author = "Barber, D. P. and others", + title = "{Study of Electron - Positron Collisions at the Highest + {PETRA} Energy}", + collaboration = "Aachen-DESY-Annecy(LAPP)-MIT-NIKHEF-Beijing", + journal = "Phys. Lett.", + volume = "85B", + year = "1979", + pages = "463-466", + doi = "10.1016/0370-2693(79)91296-6", + reportNumber = "MIT-LNS-104", + SLACcitation = "%%CITATION = PHLTA,85B,463;%%" +}' diff --git a/analyses/pluginPetra/MARKJ_1979_I141976.plot b/analyses/pluginPetra/MARKJ_1979_I141976.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1979_I141976.plot @@ -0,0 +1,27 @@ +BEGIN PLOT /MARKJ_1979_I141976/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +XMin=31 +XMax=32 +END PLOT +BEGIN PLOT /MARKJ_1979_I141976/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=31 +XMax=32 +END PLOT +BEGIN PLOT /MARKJ_1979_I141976/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +XMin=31 +XMax=32 +END PLOT \ No newline at end of file diff --git a/analyses/pluginPetra/MARKJ_1979_I141976.yoda b/analyses/pluginPetra/MARKJ_1979_I141976.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1979_I141976.yoda @@ -0,0 +1,17 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKJ_1979_I141976/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1979_I141976/d01-x01-y01 +Title: doi:10.17182/hepdata.27332.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.157000e+01 0.000000e+00 0.000000e+00 4.000000e+00 7.810250e-01 7.810250e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1979_I141976/d02-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1979_I141976/d02-x01-y01 +Title: doi:10.17182/hepdata.27332.v1/t2 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 diff --git a/analyses/pluginPetra/MARKJ_1980_I158857.cc b/analyses/pluginPetra/MARKJ_1980_I158857.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1980_I158857.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKJ_1980_I158857 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKJ_1980_I158857); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKJ_1980_I158857); + + +} diff --git a/analyses/pluginPetra/MARKJ_1980_I158857.info b/analyses/pluginPetra/MARKJ_1980_I158857.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1980_I158857.info @@ -0,0 +1,31 @@ +Name: MARKJ_1980_I158857 +Year: 1980 +Summary: Measurement of $R$ between 12 and 35.8 GeV +Experiment: MARKJ +Collider: PETRA +InspireID: 158857 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rept. 63 (1980) 337-391, 1980 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by MARKJ between 12 and 35.8 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Barber:1980uq +BibTeX: '@article{Barber:1980uq, + author = "Barber, D. P. and others", + title = "{PHYSICS WITH HIGH-ENERGY ELECTRON POSITRON COLLIDING + BEAMS WITH THE MARK-J DETECTOR}", + collaboration = "MARK-J, AACHEN-DESY-MIT-NIKHEF-BEIJING", + journal = "Phys. Rept.", + volume = "63", + year = "1980", + pages = "337-391", + doi = "10.1016/0370-1573(80)90169-6", + SLACcitation = "%%CITATION = PRPLC,63,337;%%" +}' diff --git a/analyses/pluginPetra/MARKJ_1980_I158857.plot b/analyses/pluginPetra/MARKJ_1980_I158857.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1980_I158857.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /MARKJ_1980_I158857/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKJ_1980_I158857/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKJ_1980_I158857/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginPetra/MARKJ_1980_I158857.yoda b/analyses/pluginPetra/MARKJ_1980_I158857.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1980_I158857.yoda @@ -0,0 +1,44 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKJ_1980_I158857/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1980_I158857/d01-x01-y01 +Title: doi:10.17182/hepdata.27618.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 4.030000e+00 4.907229e-01 4.907229e-01 +1.300000e+01 0.000000e+00 0.000000e+00 4.100000e+00 6.466065e-01 6.466065e-01 +1.700000e+01 0.000000e+00 0.000000e+00 4.400000e+00 7.440430e-01 7.440430e-01 +2.200000e+01 0.000000e+00 0.000000e+00 4.700000e+00 8.431489e-01 8.431489e-01 +2.757000e+01 0.000000e+00 0.000000e+00 3.800000e+00 4.841487e-01 4.841487e-01 +3.000000e+01 0.000000e+00 0.000000e+00 4.200000e+00 5.161395e-01 5.161395e-01 +3.068000e+01 7.800000e-01 7.800000e-01 4.400000e+00 4.681880e-01 4.681880e-01 +3.160000e+01 0.000000e+00 0.000000e+00 4.000000e+00 6.403124e-01 6.403124e-01 +3.300000e+01 0.000000e+00 0.000000e+00 3.300000e+00 6.847627e-01 6.847627e-01 +3.400000e+01 0.000000e+00 0.000000e+00 1.800000e+00 6.264184e-01 1.312402e+00 +3.528000e+01 2.800000e-01 2.800000e-01 4.000000e+00 4.517743e-01 4.517743e-01 +3.580000e+01 0.000000e+00 0.000000e+00 4.700000e+00 8.431489e-01 8.431489e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1980_I158857/d02-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1980_I158857/d02-x01-y01 +Title: doi:10.17182/hepdata.27618.v1/t2 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1980_I158857/d03-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1980_I158857/d03-x01-y01 +Title: doi:10.17182/hepdata.27618.v1/t3 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1980_I158857/d04-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1980_I158857/d04-x01-y01 +Title: doi:10.17182/hepdata.27618.v1/t4 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 diff --git a/analyses/pluginPetra/MARKJ_1982_I166369.cc b/analyses/pluginPetra/MARKJ_1982_I166369.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1982_I166369.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKJ_1982_I166369 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKJ_1982_I166369); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKJ_1982_I166369); + + +} diff --git a/analyses/pluginPetra/MARKJ_1982_I166369.info b/analyses/pluginPetra/MARKJ_1982_I166369.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1982_I166369.info @@ -0,0 +1,31 @@ +Name: MARKJ_1982_I166369 +Year: 1982 +Summary: Measurement of $R$ between 33 and 36.7 GeV +Experiment: MARKJ +Collider: PETRA +InspireID: 166369 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B108 (1982) 63-66, 1982 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by MARKJ between 33 and 36.7 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Barber:1981tc +BibTeX: '@article{Barber:1981tc, + author = "Barber, D. P. and others", + title = "{Measurement of Hadron Production and Three Jet Event + Properties at {PETRA} {MIT}}", + journal = "Phys. Lett.", + volume = "108B", + year = "1982", + pages = "63-66", + doi = "10.1016/0370-2693(82)91143-1", + reportNumber = "MIT-LNS-115", + SLACcitation = "%%CITATION = PHLTA,108B,63;%%" +}' diff --git a/analyses/pluginPetra/MARKJ_1982_I166369.plot b/analyses/pluginPetra/MARKJ_1982_I166369.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1982_I166369.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /MARKJ_1982_I166369/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKJ_1982_I166369/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKJ_1982_I166369/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/MARKJ_1982_I166369.yoda b/analyses/pluginPetra/MARKJ_1982_I166369.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1982_I166369.yoda @@ -0,0 +1,9 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKJ_1982_I166369/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1982_I166369/d01-x01-y01 +Title: doi:10.17182/hepdata.31009.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.485000e+01 1.850000e+00 1.850000e+00 3.750000e+00 3.783186e-01 3.783186e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/MARKJ_1983_I182337.cc b/analyses/pluginPetra/MARKJ_1983_I182337.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1983_I182337.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKJ_1983_I182337 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKJ_1983_I182337); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(4, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(4, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKJ_1983_I182337); + + +} diff --git a/analyses/pluginPetra/MARKJ_1983_I182337.info b/analyses/pluginPetra/MARKJ_1983_I182337.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1983_I182337.info @@ -0,0 +1,31 @@ +Name: MARKJ_1983_I182337 +Year: 1983 +Summary: Measurement of $R$ between 29.9 and 38.54 GeV +Experiment: MARKJ +Collider: PETRA +InspireID: 182337 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 50 (1983) 799, 1983 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by MARKJ between 29.9 and 38.54 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Adeva:1982bs +BibTeX: '@article{Adeva:1982bs, + author = "Adeva, B. and others", + title = "{Search for Top Quark and a Test of Models Without Top + Quark at the Highest {PETRA} Energies}", + journal = "Phys. Rev. Lett.", + volume = "50", + year = "1983", + pages = "799", + doi = "10.1103/PhysRevLett.50.799", + reportNumber = "MIT-LNS-128", + SLACcitation = "%%CITATION = PRLTA,50,799;%%" +}' diff --git a/analyses/pluginPetra/MARKJ_1983_I182337.plot b/analyses/pluginPetra/MARKJ_1983_I182337.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1983_I182337.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /MARKJ_1983_I182337/d04-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKJ_1983_I182337/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKJ_1983_I182337/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginPetra/MARKJ_1983_I182337.yoda b/analyses/pluginPetra/MARKJ_1983_I182337.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1983_I182337.yoda @@ -0,0 +1,35 @@ +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1983_I182337/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1983_I182337/d01-x01-y01 +Title: doi:10.17182/hepdata.20549.v1/t1 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1983_I182337/d02-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1983_I182337/d02-x01-y01 +Title: doi:10.17182/hepdata.20549.v1/t2 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1983_I182337/d03-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1983_I182337/d03-x01-y01 +Title: doi:10.17182/hepdata.20549.v1/t3 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKJ_1983_I182337/d04-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1983_I182337/d04-x01-y01 +Title: doi:10.17182/hepdata.20549.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.331000e+01 3.410000e+00 3.410000e+00 3.760000e+00 2.310744e-01 2.310744e-01 +3.828500e+01 3.450000e-01 3.450000e-01 3.910000e+00 3.018893e-01 3.018893e-01 +3.858500e+01 4.500000e-02 4.500000e-02 3.750000e+00 5.574271e-01 5.574271e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/MARKJ_1984_I196567.cc b/analyses/pluginPetra/MARKJ_1984_I196567.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1984_I196567.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKJ_1984_I196567 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKJ_1984_I196567); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKJ_1984_I196567); + + +} diff --git a/analyses/pluginPetra/MARKJ_1984_I196567.info b/analyses/pluginPetra/MARKJ_1984_I196567.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1984_I196567.info @@ -0,0 +1,32 @@ +Name: MARKJ_1984_I196567 +Year: 1984 +Summary: Measurement of $R$ between 12 and 42.63 GeV +Experiment: MARKJ +Collider: PETRA +InspireID: 196567 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rept. 109 (1984) 131, 1984 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by MARKJ between 42.63 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Adeva:1983iu +BibTeX: '@article{Adeva:1983iu, + author = "Adeva, B. and others", + title = "{A Summary of Recent Experimental Results From Mark-$J$: + High-energy $e^+ e^-$ Collisions at {PETRA}}", + collaboration = "Mark-J", + journal = "Phys. Rept.", + volume = "109", + year = "1984", + pages = "131", + doi = "10.1016/0370-1573(84)90124-8", + reportNumber = "MIT-LNS-131", + SLACcitation = "%%CITATION = PRPLC,109,131;%%" +}' diff --git a/analyses/pluginPetra/MARKJ_1984_I196567.plot b/analyses/pluginPetra/MARKJ_1984_I196567.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1984_I196567.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /MARKJ_1984_I196567/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKJ_1984_I196567/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKJ_1984_I196567/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginPetra/MARKJ_1984_I196567.yoda b/analyses/pluginPetra/MARKJ_1984_I196567.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1984_I196567.yoda @@ -0,0 +1,75 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKJ_1984_I196567/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1984_I196567/d01-x01-y01 +Title: doi:10.17182/hepdata.30997.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 3.600000e+00 2.700000e-01 2.700000e-01 +1.403200e+01 0.000000e+00 0.000000e+00 3.730000e+00 1.300000e-01 1.300000e-01 +2.199200e+01 0.000000e+00 0.000000e+00 3.580000e+00 1.300000e-01 1.300000e-01 +2.500400e+01 0.000000e+00 0.000000e+00 4.150000e+00 2.500000e-01 2.500000e-01 +3.060400e+01 0.000000e+00 0.000000e+00 4.070000e+00 1.900000e-01 1.900000e-01 +3.297800e+01 0.000000e+00 0.000000e+00 4.060000e+00 2.700000e-01 2.700000e-01 +3.388400e+01 0.000000e+00 0.000000e+00 3.810000e+00 1.300000e-01 1.300000e-01 +3.463400e+01 0.000000e+00 0.000000e+00 3.850000e+00 1.200000e-01 1.200000e-01 +3.508600e+01 0.000000e+00 0.000000e+00 4.100000e+00 1.400000e-01 1.400000e-01 +3.642400e+01 0.000000e+00 0.000000e+00 3.930000e+00 1.800000e-01 1.800000e-01 +3.823200e+01 0.000000e+00 0.000000e+00 3.950000e+00 2.200000e-01 2.200000e-01 +4.036000e+01 0.000000e+00 0.000000e+00 3.800000e+00 1.900000e-01 1.900000e-01 +4.150300e+01 0.000000e+00 0.000000e+00 4.370000e+00 2.400000e-01 2.400000e-01 +4.262700e+01 0.000000e+00 0.000000e+00 3.860000e+00 2.100000e-01 2.100000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1984_I196567/d02-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1984_I196567/d02-x01-y01 +Title: doi:10.17182/hepdata.30997.v1/t2 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1984_I196567/d03-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1984_I196567/d03-x01-y01 +Title: doi:10.17182/hepdata.30997.v1/t3 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKJ_1984_I196567/d04-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1984_I196567/d04-x01-y01 +Title: doi:10.17182/hepdata.30997.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +-7.000000e-01 0.000000e+00 0.000000e+00 8.400000e-01 8.300000e-02 8.300000e-02 +-5.000000e-01 0.000000e+00 0.000000e+00 7.820000e-01 7.000000e-02 7.000000e-02 +-3.000000e-01 0.000000e+00 0.000000e+00 4.970000e-01 5.300000e-02 5.300000e-02 +-1.000000e-01 0.000000e+00 0.000000e+00 5.400000e-01 5.800000e-02 5.800000e-02 +1.000000e-01 0.000000e+00 0.000000e+00 5.100000e-01 5.300000e-02 5.300000e-02 +3.000000e-01 0.000000e+00 0.000000e+00 5.030000e-01 5.400000e-02 5.400000e-02 +5.000000e-01 0.000000e+00 0.000000e+00 6.650000e-01 6.400000e-02 6.400000e-02 +7.000000e-01 0.000000e+00 0.000000e+00 6.500000e-01 7.600000e-02 7.600000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKJ_1984_I196567/d05-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1984_I196567/d05-x01-y01 +Title: doi:10.17182/hepdata.30997.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.430000e+01 0.000000e+00 0.000000e+00 1.210000e+00 2.000000e-01 2.000000e-01 +2.250000e+01 0.000000e+00 0.000000e+00 1.080000e+00 1.600000e-01 1.600000e-01 +3.500000e+01 0.000000e+00 0.000000e+00 1.030000e+00 9.000000e-02 9.000000e-02 +4.040000e+01 0.000000e+00 0.000000e+00 1.120000e+00 1.200000e-01 1.200000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKJ_1984_I196567/d06-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1984_I196567/d06-x01-y01 +Title: doi:10.17182/hepdata.30997.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.460000e+01 0.000000e+00 0.000000e+00 -7.500000e+00 3.150000e-01 3.150000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/MARKJ_1986_I230297.cc b/analyses/pluginPetra/MARKJ_1986_I230297.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1986_I230297.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKJ_1986_I230297 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKJ_1986_I230297); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKJ_1986_I230297); + + +} diff --git a/analyses/pluginPetra/MARKJ_1986_I230297.info b/analyses/pluginPetra/MARKJ_1986_I230297.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1986_I230297.info @@ -0,0 +1,33 @@ +Name: MARKJ_1986_I230297 +Year: 1986 +Summary: Measurement of $R$ between 12 and 46.78 GeV +Experiment: MARKJ +Collider: PETRA +InspireID: 230297 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D34 (1986) 681-691, 1986 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by MARKJ between 12 and 46.78 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Adeva:1986nt +BibTeX: '@article{Adeva:1986nt, + author = "Adeva, B. and others", + title = "{Study of Hadron and Inclusive Muon Production From + Electron Positron Annihilation at 39.79-{GeV} $\le + \sqrt{s} \le$ 46.78-{GeV}}", + collaboration = "Mark-J", + journal = "Phys. Rev.", + volume = "D34", + year = "1986", + pages = "681-691", + doi = "10.1103/PhysRevD.34.681", + reportNumber = "MIT-LNS-146", + SLACcitation = "%%CITATION = PHRVA,D34,681;%%" +}' diff --git a/analyses/pluginPetra/MARKJ_1986_I230297.plot b/analyses/pluginPetra/MARKJ_1986_I230297.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1986_I230297.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /MARKJ_1986_I230297/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKJ_1986_I230297/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKJ_1986_I230297/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginPetra/MARKJ_1986_I230297.yoda b/analyses/pluginPetra/MARKJ_1986_I230297.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/MARKJ_1986_I230297.yoda @@ -0,0 +1,42 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKJ_1986_I230297/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1986_I230297/d01-x01-y01 +Title: doi:10.17182/hepdata.23423.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 3.470000e+00 3.043062e-01 3.043062e-01 +1.403000e+01 0.000000e+00 0.000000e+00 3.710000e+00 1.982681e-01 1.982681e-01 +2.199000e+01 0.000000e+00 0.000000e+00 3.550000e+00 1.946953e-01 1.946953e-01 +2.500000e+01 0.000000e+00 0.000000e+00 4.030000e+00 2.910365e-01 2.910365e-01 +3.061000e+01 0.000000e+00 0.000000e+00 4.150000e+00 2.560395e-01 2.560395e-01 +3.379000e+01 0.000000e+00 0.000000e+00 3.860000e+00 2.053022e-01 2.053022e-01 +3.461000e+01 0.000000e+00 0.000000e+00 3.780000e+00 1.913661e-01 1.913661e-01 +3.510000e+01 0.000000e+00 0.000000e+00 3.940000e+00 2.059345e-01 2.059345e-01 +3.631000e+01 0.000000e+00 0.000000e+00 3.880000e+00 2.514677e-01 2.514677e-01 +3.740000e+01 0.000000e+00 0.000000e+00 3.590000e+00 3.669063e-01 3.669063e-01 +3.838000e+01 0.000000e+00 0.000000e+00 4.030000e+00 2.769517e-01 2.769517e-01 +4.034000e+01 0.000000e+00 0.000000e+00 3.870000e+00 2.510822e-01 2.510822e-01 +4.150000e+01 0.000000e+00 0.000000e+00 4.440000e+00 3.055880e-01 3.055880e-01 +4.250000e+01 0.000000e+00 0.000000e+00 3.890000e+00 2.789807e-01 2.789807e-01 +4.346000e+01 0.000000e+00 0.000000e+00 3.750000e+00 2.530934e-01 2.530934e-01 +4.423000e+01 0.000000e+00 0.000000e+00 4.150000e+00 2.223876e-01 2.223876e-01 +4.548000e+01 0.000000e+00 0.000000e+00 4.170000e+00 2.820855e-01 2.820855e-01 +4.647000e+01 0.000000e+00 0.000000e+00 4.420000e+00 2.788207e-01 2.788207e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1986_I230297/d02-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1986_I230297/d02-x01-y01 +Title: doi:10.17182/hepdata.23423.v1/t2 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKJ_1986_I230297/d03-x01-y01 +IsRef: 1 +Path: /REF/MARKJ_1986_I230297/d03-x01-y01 +Title: doi:10.17182/hepdata.23423.v1/t3 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 diff --git a/analyses/pluginPetra/PLUTO_1979_I140294.cc b/analyses/pluginPetra/PLUTO_1979_I140294.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I140294.cc @@ -0,0 +1,103 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class PLUTO_1979_I140294 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(PLUTO_1979_I140294); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + ostringstream title; + title << "d0" << ix << "_sigma"; + Scatter2DPtr hadrons = bookScatter2D(title.str() + "_hadrons"); + Scatter2DPtr muons = bookScatter2D(title.str() + "_muons" ); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(PLUTO_1979_I140294); + + +} diff --git a/analyses/pluginPetra/PLUTO_1979_I140294.info b/analyses/pluginPetra/PLUTO_1979_I140294.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I140294.info @@ -0,0 +1,34 @@ +Name: PLUTO_1979_I140294 +Year: 1979 +Summary: Measurement of $R$ between 3 and 17 GeV +Experiment: PLUTO +Collider: PETRA +InspireID: 140294 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B81 (1979) 410-415, 1979 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by PLUTO for energies between 3 and 17 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Berger:1979bp +BibTeX: '@article{Berger:1979bp, + author = "Berger, Christoph and others", + title = "{Cross-Sections and Event Topologies in e+ e- + Annihilation at 13-GeV and 17-GeV Observed with the PLUTO + Detector}", + collaboration = "PLUTO", + journal = "Phys. Lett.", + volume = "81B", + year = "1979", + pages = "410-415", + doi = "10.1016/0370-2693(79)90365-4", + reportNumber = "DESY-79-11", + SLACcitation = "%%CITATION = PHLTA,81B,410;%%" +}' diff --git a/analyses/pluginPetra/PLUTO_1979_I140294.plot b/analyses/pluginPetra/PLUTO_1979_I140294.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I140294.plot @@ -0,0 +1,42 @@ +BEGIN PLOT /PLUTO_1979_I140294/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1979_I140294/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1979_I140294/d01_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1979_I140294/d01_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1979_I140294/d02_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1979_I140294/d02_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/PLUTO_1979_I140294.yoda b/analyses/pluginPetra/PLUTO_1979_I140294.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I140294.yoda @@ -0,0 +1,25 @@ +BEGIN YODA_SCATTER2D_V2 /REF/PLUTO_1979_I140294/d01-x01-y01 +IsRef: 1 +Path: /REF/PLUTO_1979_I140294/d01-x01-y01 +Title: doi:10.17182/hepdata.45239.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.600000e+00 0.000000e+00 0.000000e+00 2.080000e+00 3.000000e-02 3.000000e-02 +4.030000e+00 0.000000e+00 0.000000e+00 4.490000e+00 9.000000e-02 9.000000e-02 +5.000000e+00 0.000000e+00 0.000000e+00 3.820000e+00 4.000000e-02 4.000000e-02 +7.700000e+00 0.000000e+00 0.000000e+00 3.920000e+00 2.600000e-01 2.600000e-01 +9.400000e+00 0.000000e+00 0.000000e+00 3.700000e+00 3.000000e-01 3.000000e-01 +1.300000e+01 0.000000e+00 0.000000e+00 5.000000e+00 5.000000e-01 5.000000e-01 +1.700000e+01 0.000000e+00 0.000000e+00 4.300000e+00 5.000000e-01 5.000000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PLUTO_1979_I140294/d02-x01-y01 +IsRef: 1 +Path: /REF/PLUTO_1979_I140294/d02-x01-y01 +Title: doi:10.17182/hepdata.45239.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.300000e+01 0.000000e+00 0.000000e+00 5.700000e+00 2.046851e+00 2.046851e+00 +1.700000e+01 0.000000e+00 0.000000e+00 4.200000e+00 1.305986e+00 1.305986e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/PLUTO_1979_I140818.cc b/analyses/pluginPetra/PLUTO_1979_I140818.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I140818.cc @@ -0,0 +1,90 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class PLUTO_1979_I140818 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(PLUTO_1979_I140818); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + vetoEvent; + // everything else + else { + _c_hadrons->fill(event.weight()); + } + + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + Scatter2D temphisto(refData(2, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(2, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + } + else { + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(PLUTO_1979_I140818); + + +} diff --git a/analyses/pluginPetra/PLUTO_1979_I140818.info b/analyses/pluginPetra/PLUTO_1979_I140818.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I140818.info @@ -0,0 +1,31 @@ +Name: PLUTO_1979_I140818 +Year: 1979 +Summary: Hadronic cross section in $e^+e^-$ collisions for energies between 9.4 to 9.48 +Experiment: PLUTO +Collider: PETRA +InspireID: 140818 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C1 (1979) 343, 1979 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of the hadronic cross section in $e^+e^-$ collisions for energies between 9.4 to 9.48 GeV.' +Keywords: [] +BibKey: Berger:1979uv +BibTeX: '@article{Berger:1979uv, + author = "Berger, Christoph and others", + title = "{Measurement of Leptonic Branching Ratios of the + $\Upsilon$ (9.46)}", + collaboration = "PLUTO", + journal = "Z. Phys.", + volume = "C1", + year = "1979", + pages = "343", + doi = "10.1007/BF01546972", + reportNumber = "DESY-79-19", + SLACcitation = "%%CITATION = ZEPYA,C1,343;%%" +}' diff --git a/analyses/pluginPetra/PLUTO_1979_I140818.plot b/analyses/pluginPetra/PLUTO_1979_I140818.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I140818.plot @@ -0,0 +1,6 @@ +BEGIN PLOT /PLUTO_1979_I140818/d02-x01-y01 +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/PLUTO_1979_I140818.yoda b/analyses/pluginPetra/PLUTO_1979_I140818.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I140818.yoda @@ -0,0 +1,22 @@ +BEGIN YODA_SCATTER2D_V2 /REF/PLUTO_1979_I140818/d02-x01-y01 +IsRef: 1 +Path: /REF/PLUTO_1979_I140818/d02-x01-y01 +Title: doi:10.17182/hepdata.16475.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.400000e+00 0.000000e+00 0.000000e+00 3.130000e+00 5.700000e-01 5.700000e-01 +9.410000e+00 0.000000e+00 0.000000e+00 4.550000e+00 8.500000e-01 8.500000e-01 +9.420000e+00 0.000000e+00 0.000000e+00 3.700000e+00 6.000000e-01 6.000000e-01 +9.430000e+00 0.000000e+00 0.000000e+00 3.950000e+00 7.000000e-01 7.000000e-01 +9.436000e+00 0.000000e+00 0.000000e+00 5.200000e+00 8.700000e-01 8.700000e-01 +9.440000e+00 0.000000e+00 0.000000e+00 2.070000e+00 1.000000e+00 1.000000e+00 +9.445000e+00 0.000000e+00 0.000000e+00 7.400000e+00 1.200000e+00 1.200000e+00 +9.450000e+00 0.000000e+00 0.000000e+00 1.190000e+01 1.400000e+00 1.400000e+00 +9.456000e+00 0.000000e+00 0.000000e+00 1.555000e+01 5.000000e-01 5.000000e-01 +9.460000e+00 0.000000e+00 0.000000e+00 1.477000e+01 6.700000e-01 6.700000e-01 +9.465000e+00 0.000000e+00 0.000000e+00 1.067000e+01 9.200000e-01 9.200000e-01 +9.470000e+00 0.000000e+00 0.000000e+00 7.120000e+00 1.190000e+00 1.190000e+00 +9.475000e+00 0.000000e+00 0.000000e+00 3.130000e+00 7.100000e-01 7.100000e-01 +9.480000e+00 0.000000e+00 0.000000e+00 4.330000e+00 7.300000e-01 7.300000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/PLUTO_1979_I142517.cc b/analyses/pluginPetra/PLUTO_1979_I142517.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I142517.cc @@ -0,0 +1,101 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class PLUTO_1979_I142517 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(PLUTO_1979_I142517); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else { + _c_hadrons->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(PLUTO_1979_I142517); + + +} diff --git a/analyses/pluginPetra/PLUTO_1979_I142517.info b/analyses/pluginPetra/PLUTO_1979_I142517.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I142517.info @@ -0,0 +1,34 @@ +Name: PLUTO_1979_I142517 +Year: 1979 +Summary: Measurement of $R$ between 22 and 31.6 GeV +Experiment: PLUTO +Collider: PETRA +InspireID: 142517 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B86 (1979) 413-417, 1979 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 22 and 31.6 GeV. + The hadronic cross section is also measured in the $\Upsilon$ region, 9.3 to 9.48 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Berger:1979wn +BibTeX: '@article{Berger:1979wn, + author = "Berger, Christoph and others", + title = "{Search for a Top Threshold in Hadronic $e^+ e^-$ + Annihilation at Energies Between 22-{GeV} and 31.6-{GeV}}", + collaboration = "PLUTO", + journal = "Phys. Lett.", + volume = "86B", + year = "1979", + pages = "413-417", + doi = "10.1016/0370-2693(79)90868-2", + reportNumber = "DESY-79-56", + SLACcitation = "%%CITATION = PHLTA,86B,413;%%" +}' diff --git a/analyses/pluginPetra/PLUTO_1979_I142517.plot b/analyses/pluginPetra/PLUTO_1979_I142517.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I142517.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /PLUTO_1979_I142517/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1979_I142517/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1979_I142517/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginPetra/PLUTO_1979_I142517.yoda b/analyses/pluginPetra/PLUTO_1979_I142517.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1979_I142517.yoda @@ -0,0 +1,12 @@ +BEGIN YODA_SCATTER2D_V2 /REF/PLUTO_1979_I142517/d01-x01-y01 +IsRef: 1 +Path: /REF/PLUTO_1979_I142517/d01-x01-y01 +Title: doi:10.17182/hepdata.27295.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +22.00e+00 0.000000e+00 0.000000e+00 3.410000e+00 8.057177e-01 8.057177e-01 +27.60e+00 0.000000e+00 0.000000e+00 3.640000e+00 4.781171e-01 4.781171e-01 +30.00e+00 0.000000e+00 0.000000e+00 4.380000e+00 5.733620e-01 5.733620e-01 +31.60e+00 0.000000e+00 0.000000e+00 3.590000e+00 6.318869e-01 6.318869e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/PLUTO_1980_I152291.cc b/analyses/pluginPetra/PLUTO_1980_I152291.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1980_I152291.cc @@ -0,0 +1,103 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class PLUTO_1980_I152291 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(PLUTO_1980_I152291); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + ostringstream title; + title << "d0" << ix << "_sigma"; + Scatter2DPtr hadrons = bookScatter2D(title.str() + "_hadrons"); + Scatter2DPtr muons = bookScatter2D(title.str() + "_muons" ); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(PLUTO_1980_I152291); + + +} diff --git a/analyses/pluginPetra/PLUTO_1980_I152291.info b/analyses/pluginPetra/PLUTO_1980_I152291.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1980_I152291.info @@ -0,0 +1,33 @@ +Name: PLUTO_1980_I152291 +Year: 1980 +Summary: Measurement of $R$ between 30 and 31 GeV +Experiment: PLUTO +Collider: PETRA +InspireID: 152291 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B91 (1980) 148-151, 1980 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by PLUTO for energies between 30 and 31 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Berger:1980rt +BibTeX: '@article{Berger:1980rt, + author = "Berger, Christoph and others", + title = "{Search for Narrow Resonances in $e^+ e^-$ Annihilation + at {PETRA}}", + collaboration = "PLUTO", + journal = "Phys. Lett.", + volume = "91B", + year = "1980", + pages = "148-151", + doi = "10.1016/0370-2693(80)90681-4", + reportNumber = "DESY-80-02", + SLACcitation = "%%CITATION = PHLTA,91B,148;%%" +}' diff --git a/analyses/pluginPetra/PLUTO_1980_I152291.plot b/analyses/pluginPetra/PLUTO_1980_I152291.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1980_I152291.plot @@ -0,0 +1,42 @@ +BEGIN PLOT /PLUTO_1980_I152291/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1980_I152291/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1980_I152291/d01_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1980_I152291/d01_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1980_I152291/d02_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1980_I152291/d02_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/PLUTO_1980_I152291.yoda b/analyses/pluginPetra/PLUTO_1980_I152291.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1980_I152291.yoda @@ -0,0 +1,18 @@ +BEGIN YODA_SCATTER2D_V2 /REF/PLUTO_1980_I152291/d01-x01-y01 +IsRef: 1 +Path: /REF/PLUTO_1980_I152291/d01-x01-y01 +Title: doi:10.17182/hepdata.27236.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.068000e+01 7.800000e-01 7.800000e-01 3.800000e+00 6.040695e-01 6.040695e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PLUTO_1980_I152291/d02-x01-y01 +IsRef: 1 +Path: /REF/PLUTO_1980_I152291/d02-x01-y01 +Title: doi:10.17182/hepdata.27236.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.080000e+01 8.000000e-01 8.000000e-01 3.900000e+00 7.951258e-01 7.951258e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/PLUTO_1982_I166799.cc b/analyses/pluginPetra/PLUTO_1982_I166799.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1982_I166799.cc @@ -0,0 +1,117 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class PLUTO_1982_I166799 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(PLUTO_1982_I166799); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else { + _c_hadrons->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + // cross section + Scatter2D temphisto2(refData(2, 1, 1)); + hadrons = bookScatter2D(2, 1, 1); + for (size_t b = 0; b < temphisto2.numPoints(); b++) { + const double x = temphisto2.point(b).x(); + pair ex = temphisto2.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + } + else { + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(PLUTO_1982_I166799); + + +} diff --git a/analyses/pluginPetra/PLUTO_1982_I166799.info b/analyses/pluginPetra/PLUTO_1982_I166799.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1982_I166799.info @@ -0,0 +1,33 @@ +Name: PLUTO_1982_I166799 +Year: 1982 +Summary: Measurement of $R$ between 3.6 and 30 GeV and hadronic cross section from 9.3 to 9.48 GeV +Experiment: PLUTO +Collider: PETRA +InspireID: 166799 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rept. 83 (1982) 151-280, 1982 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 3.6 and 30 GeV. + The hadronic cross section is also measured in the $\Upsilon$ region, 9.3 to 9.48 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Criegee:1981qx +BibTeX: '@article{Criegee:1981qx, + author = "Criegee, Lutz and Knies, Gerhard", + title = "{Review of $e^+ e^-$ Experiments With Pluto From 3-{GeV} + to 31-{GeV}}", + journal = "Phys. Rept.", + volume = "83", + year = "1982", + pages = "151-280", + doi = "10.1016/0370-1573(82)90012-6", + reportNumber = "DESY-81-044", + SLACcitation = "%%CITATION = PRPLC,83,151;%%" +}' diff --git a/analyses/pluginPetra/PLUTO_1982_I166799.plot b/analyses/pluginPetra/PLUTO_1982_I166799.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1982_I166799.plot @@ -0,0 +1,27 @@ +BEGIN PLOT /PLUTO_1982_I166799/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1982_I166799/d02-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1982_I166799/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /PLUTO_1982_I166799/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 diff --git a/analyses/pluginPetra/PLUTO_1982_I166799.yoda b/analyses/pluginPetra/PLUTO_1982_I166799.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/PLUTO_1982_I166799.yoda @@ -0,0 +1,85 @@ +BEGIN YODA_SCATTER2D_V2 /REF/PLUTO_1982_I166799/d01-x01-y01 +IsRef: 1 +Path: /REF/PLUTO_1982_I166799/d01-x01-y01 +Title: doi:10.17182/hepdata.19326.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.600000e+00 0.000000e+00 0.000000e+00 2.290000e+00 3.000000e-02 3.000000e-02 +3.630000e+00 0.000000e+00 0.000000e+00 2.070000e+00 8.000000e-02 8.000000e-02 +3.660000e+00 0.000000e+00 0.000000e+00 2.130000e+00 9.000000e-02 9.000000e-02 +4.000000e+00 0.000000e+00 0.000000e+00 3.380000e+00 8.000000e-02 8.000000e-02 +4.020000e+00 0.000000e+00 0.000000e+00 4.520000e+00 5.000000e-02 5.000000e-02 +4.030000e+00 0.000000e+00 0.000000e+00 4.540000e+00 9.000000e-02 9.000000e-02 +4.050000e+00 0.000000e+00 0.000000e+00 3.880000e+00 1.100000e-01 1.100000e-01 +4.070000e+00 0.000000e+00 0.000000e+00 3.420000e+00 1.100000e-01 1.100000e-01 +4.090000e+00 0.000000e+00 0.000000e+00 3.830000e+00 1.100000e-01 1.100000e-01 +4.110000e+00 0.000000e+00 0.000000e+00 3.500000e+00 1.300000e-01 1.300000e-01 +4.130000e+00 0.000000e+00 0.000000e+00 4.400000e+00 1.500000e-01 1.500000e-01 +4.150000e+00 0.000000e+00 0.000000e+00 4.190000e+00 1.700000e-01 1.700000e-01 +4.180000e+00 0.000000e+00 0.000000e+00 3.570000e+00 2.000000e-01 2.000000e-01 +4.190000e+00 0.000000e+00 0.000000e+00 3.220000e+00 2.300000e-01 2.300000e-01 +4.220000e+00 0.000000e+00 0.000000e+00 3.120000e+00 1.600000e-01 1.600000e-01 +4.240000e+00 0.000000e+00 0.000000e+00 2.920000e+00 1.800000e-01 1.800000e-01 +4.250000e+00 0.000000e+00 0.000000e+00 2.320000e+00 1.700000e-01 1.700000e-01 +4.280000e+00 0.000000e+00 0.000000e+00 3.210000e+00 2.900000e-01 2.900000e-01 +4.300000e+00 0.000000e+00 0.000000e+00 3.150000e+00 2.800000e-01 2.800000e-01 +4.310000e+00 0.000000e+00 0.000000e+00 3.340000e+00 1.500000e-01 1.500000e-01 +4.330000e+00 0.000000e+00 0.000000e+00 3.660000e+00 1.600000e-01 1.600000e-01 +4.350000e+00 0.000000e+00 0.000000e+00 3.350000e+00 1.300000e-01 1.300000e-01 +4.380000e+00 0.000000e+00 0.000000e+00 4.190000e+00 2.100000e-01 2.100000e-01 +4.390000e+00 0.000000e+00 0.000000e+00 4.430000e+00 1.400000e-01 1.400000e-01 +4.410000e+00 0.000000e+00 0.000000e+00 4.100000e+00 6.000000e-02 6.000000e-02 +4.440000e+00 0.000000e+00 0.000000e+00 3.970000e+00 1.700000e-01 1.700000e-01 +4.460000e+00 0.000000e+00 0.000000e+00 3.540000e+00 1.600000e-01 1.600000e-01 +4.500000e+00 0.000000e+00 0.000000e+00 3.720000e+00 7.000000e-02 7.000000e-02 +4.540000e+00 0.000000e+00 0.000000e+00 3.900000e+00 1.500000e-01 1.500000e-01 +4.570000e+00 0.000000e+00 0.000000e+00 3.660000e+00 1.300000e-01 1.300000e-01 +4.620000e+00 0.000000e+00 0.000000e+00 3.550000e+00 1.100000e-01 1.100000e-01 +4.660000e+00 0.000000e+00 0.000000e+00 3.910000e+00 1.400000e-01 1.400000e-01 +4.710000e+00 0.000000e+00 0.000000e+00 3.730000e+00 1.600000e-01 1.600000e-01 +4.980000e+00 0.000000e+00 0.000000e+00 3.850000e+00 4.000000e-02 4.000000e-02 +7.700000e+00 0.000000e+00 0.000000e+00 3.920000e+00 2.600000e-01 2.600000e-01 +9.300000e+00 0.000000e+00 0.000000e+00 3.450000e+00 6.200000e-01 6.200000e-01 +9.350000e+00 0.000000e+00 0.000000e+00 3.820000e+00 7.500000e-01 7.500000e-01 +9.370000e+00 0.000000e+00 0.000000e+00 4.680000e+00 8.200000e-01 8.200000e-01 +9.380000e+00 0.000000e+00 0.000000e+00 5.040000e+00 8.900000e-01 8.900000e-01 +9.390000e+00 0.000000e+00 0.000000e+00 3.880000e+00 4.700000e-01 4.700000e-01 +9.400000e+00 0.000000e+00 0.000000e+00 3.160000e+00 6.300000e-01 6.300000e-01 +9.410000e+00 0.000000e+00 0.000000e+00 3.580000e+00 7.000000e-01 7.000000e-01 +9.420000e+00 0.000000e+00 0.000000e+00 3.930000e+00 6.400000e-01 6.400000e-01 +9.430000e+00 0.000000e+00 0.000000e+00 4.050000e+00 6.400000e-01 6.400000e-01 +9.440000e+00 0.000000e+00 0.000000e+00 2.920000e+00 8.200000e-01 8.200000e-01 +1.200000e+01 0.000000e+00 0.000000e+00 4.290000e+00 2.900000e-01 2.900000e-01 +1.300000e+01 0.000000e+00 0.000000e+00 4.100000e+00 4.500000e-01 4.500000e-01 +1.700000e+01 0.000000e+00 0.000000e+00 3.600000e+00 3.700000e-01 3.700000e-01 +2.200000e+01 0.000000e+00 0.000000e+00 3.470000e+00 6.000000e-01 6.000000e-01 +2.760000e+01 0.000000e+00 0.000000e+00 4.070000e+00 2.900000e-01 2.900000e-01 +3.080000e+01 8.000000e-01 8.000000e-01 4.100000e+00 1.300000e-01 1.300000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/PLUTO_1982_I166799/d02-x01-y01 +IsRef: 1 +Path: /REF/PLUTO_1982_I166799/d02-x01-y01 +Title: doi:10.17182/hepdata.19326.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +9.300000e+00 0.000000e+00 0.000000e+00 3.900000e+00 7.380759e-01 7.380759e-01 +9.350000e+00 0.000000e+00 0.000000e+00 4.300000e+00 9.362500e-01 9.362500e-01 +9.370000e+00 0.000000e+00 0.000000e+00 5.100000e+00 9.505977e-01 9.505977e-01 +9.380000e+00 0.000000e+00 0.000000e+00 5.500000e+00 1.148434e+00 1.148434e+00 +9.390000e+00 0.000000e+00 0.000000e+00 4.200000e+00 5.599143e-01 5.599143e-01 +9.400000e+00 0.000000e+00 0.000000e+00 3.500000e+00 7.308215e-01 7.308215e-01 +9.410000e+00 0.000000e+00 0.000000e+00 4.000000e+00 8.352245e-01 8.352245e-01 +9.420000e+00 0.000000e+00 0.000000e+00 4.300000e+00 7.460322e-01 7.460322e-01 +9.433000e+00 0.000000e+00 0.000000e+00 4.400000e+00 7.481283e-01 7.481283e-01 +9.440000e+00 0.000000e+00 0.000000e+00 3.100000e+00 9.190190e-01 9.190190e-01 +9.445000e+00 0.000000e+00 0.000000e+00 7.700000e+00 1.193082e+00 1.193082e+00 +9.450000e+00 0.000000e+00 0.000000e+00 1.080000e+01 1.542694e+00 1.542694e+00 +9.455000e+00 0.000000e+00 0.000000e+00 1.480000e+01 1.264335e+00 1.264335e+00 +9.460000e+00 0.000000e+00 0.000000e+00 1.380000e+01 1.376802e+00 1.376802e+00 +9.465000e+00 0.000000e+00 0.000000e+00 1.050000e+01 1.267636e+00 1.267636e+00 +9.470000e+00 0.000000e+00 0.000000e+00 8.000000e+00 1.480000e+00 1.480000e+00 +9.475000e+00 0.000000e+00 0.000000e+00 3.000000e+00 7.227724e-01 7.227724e-01 +9.480000e+00 0.000000e+00 0.000000e+00 5.000000e+00 8.544004e-01 8.544004e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/TASSO_1979_I140303.cc b/analyses/pluginPetra/TASSO_1979_I140303.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1979_I140303.cc @@ -0,0 +1,101 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class TASSO_1979_I140303 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(TASSO_1979_I140303); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else { + _c_hadrons->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(TASSO_1979_I140303); + + +} diff --git a/analyses/pluginPetra/TASSO_1979_I140303.info b/analyses/pluginPetra/TASSO_1979_I140303.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1979_I140303.info @@ -0,0 +1,33 @@ +Name: TASSO_1979_I140303 +Year: 1979 +Summary: Measurement of $R$ for energies between 13 and 17 GeV +Experiment: TASSO +Collider: PETRA +InspireID: 140303 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B83 (1979) 261-266, 1979 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 13 and 17 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Brandelik:1979cj +BibTeX: '@article{Brandelik:1979cj, + author = "Brandelik, R. and others", + title = "{Properties of Hadron Final States in e+ e- Annihilation + at 13-GeV and 17-GeV Center-Of-Mass Energies}", + collaboration = "TASSO", + journal = "Phys. Lett.", + volume = "83B", + year = "1979", + pages = "261-266", + doi = "10.1016/0370-2693(79)90699-3", + reportNumber = "DESY-79-14", + SLACcitation = "%%CITATION = PHLTA,83B,261;%%" +}' diff --git a/analyses/pluginPetra/TASSO_1979_I140303.plot b/analyses/pluginPetra/TASSO_1979_I140303.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1979_I140303.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /TASSO_1979_I140303/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1979_I140303/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1979_I140303/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/TASSO_1979_I140303.yoda b/analyses/pluginPetra/TASSO_1979_I140303.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1979_I140303.yoda @@ -0,0 +1,18 @@ +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1979_I140303/d01-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1979_I140303/d01-x01-y01 +Title: doi:10.17182/hepdata.27352.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.300000e+01 0.000000e+00 0.000000e+00 5.600000e+00 1.320757e+00 1.320757e+00 +1.700000e+01 0.000000e+00 0.000000e+00 4.000000e+00 1.063015e+00 1.063015e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/TASSO_1979_I140303/d02-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1979_I140303/d02-x01-y01 +Title: doi:10.17182/hepdata.27352.v1/t2 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 diff --git a/analyses/pluginPetra/TASSO_1980_I143690.cc b/analyses/pluginPetra/TASSO_1980_I143690.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1980_I143690.cc @@ -0,0 +1,101 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class TASSO_1980_I143690 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(TASSO_1980_I143690); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else { + _c_hadrons->fill(event.weight()); + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(TASSO_1980_I143690); + + +} diff --git a/analyses/pluginPetra/TASSO_1980_I143690.info b/analyses/pluginPetra/TASSO_1980_I143690.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1980_I143690.info @@ -0,0 +1,33 @@ +Name: TASSO_1980_I143690 +Year: 1980 +Summary: Measurement of $R$ for energies between 12 and 39 GeV +Experiment: TASSO +Collider: PETRA +InspireID: 143690 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C4 (1980) 87, 1980 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 12 and 39 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Brandelik:1979bv +BibTeX: '@article{Brandelik:1979bv, + author = "Brandelik, R. and others", + title = "{E+ e- Annihilation at High-Energies and Search for the + t-Quark Continuum Contribution}", + collaboration = "TASSO", + journal = "Z. Phys.", + volume = "C4", + year = "1980", + pages = "87", + doi = "10.1007/BF01554391", + reportNumber = "DESY-79/74", + SLACcitation = "%%CITATION = ZEPYA,C4,87;%%" +}' diff --git a/analyses/pluginPetra/TASSO_1980_I143690.plot b/analyses/pluginPetra/TASSO_1980_I143690.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1980_I143690.plot @@ -0,0 +1,22 @@ +BEGIN PLOT /TASSO_1980_I143690/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1980_I143690/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1980_I143690/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT + diff --git a/analyses/pluginPetra/TASSO_1980_I143690.yoda b/analyses/pluginPetra/TASSO_1980_I143690.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1980_I143690.yoda @@ -0,0 +1,15 @@ +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1980_I143690/d01-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1980_I143690/d01-x01-y01 +Title: doi:10.17182/hepdata.15599.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 4.000000e+00 5.656854e-01 5.656854e-01 +1.300000e+01 0.000000e+00 0.000000e+00 5.400000e+00 9.651943e-01 9.651943e-01 +1.700000e+01 0.000000e+00 0.000000e+00 3.100000e+00 6.753518e-01 6.753518e-01 +2.200000e+01 0.000000e+00 0.000000e+00 3.200000e+00 8.616264e-01 8.616264e-01 +2.755000e+01 1.500000e-01 1.500000e-01 3.900000e+00 5.586591e-01 5.586591e-01 +3.040000e+01 5.000000e-01 5.000000e-01 4.000000e+00 4.472136e-01 4.472136e-01 +3.125000e+01 3.500000e-01 3.500000e-01 3.700000e+00 4.763402e-01 4.763402e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/TASSO_1982_I176887.cc b/analyses/pluginPetra/TASSO_1982_I176887.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1982_I176887.cc @@ -0,0 +1,102 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class TASSO_1982_I176887 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(TASSO_1982_I176887); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + for(unsigned int ix=1;ix<4;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + ostringstream title; + title << "d0" << ix << "_sigma"; + Scatter2DPtr hadrons = bookScatter2D(title.str() + "_hadrons"); + Scatter2DPtr muons = bookScatter2D(title.str() + "_muons" ); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(TASSO_1982_I176887); + + +} diff --git a/analyses/pluginPetra/TASSO_1982_I176887.info b/analyses/pluginPetra/TASSO_1982_I176887.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1982_I176887.info @@ -0,0 +1,33 @@ +Name: TASSO_1982_I176887 +Year: 1982 +Summary: Measurement of $R$ between 12 and 36.7 GeV +Experiment: TASSO +Collider: PETRA +InspireID: 176887 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B113 (1982) 499-508, 1982 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by TASSO for energies between 12 and 36.7 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Brandelik:1982zi +BibTeX: '@article{Brandelik:1982zi, + author = "Brandelik, R. and others", + title = "{A Measurement of Sigma(tot) (e+ e- ---> Hadrons) for CM + Energies Between 12.0-GeV and 36.7-GeV}", + collaboration = "TASSO", + journal = "Phys. Lett.", + volume = "113B", + year = "1982", + pages = "499-508", + doi = "10.1016/0370-2693(82)90794-8", + reportNumber = "DESY-82-010", + SLACcitation = "%%CITATION = PHLTA,113B,499;%%" +}' diff --git a/analyses/pluginPetra/TASSO_1982_I176887.plot b/analyses/pluginPetra/TASSO_1982_I176887.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1982_I176887.plot @@ -0,0 +1,63 @@ +BEGIN PLOT /TASSO_1982_I176887/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1982_I176887/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1982_I176887/d03-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1982_I176887/d01_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1982_I176887/d01_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1982_I176887/d02_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1982_I176887/d02_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1982_I176887/d03_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1982_I176887/d03_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/TASSO_1982_I176887.yoda b/analyses/pluginPetra/TASSO_1982_I176887.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1982_I176887.yoda @@ -0,0 +1,232 @@ +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1982_I176887/d01-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1982_I176887/d01-x01-y01 +Title: doi:10.17182/hepdata.6666.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 3.800000e+00 2.800000e-01 2.800000e-01 +2.755000e+01 1.500000e-01 1.500000e-01 3.910000e+00 3.200000e-01 3.200000e-01 +3.020000e+01 3.000000e-01 3.000000e-01 3.940000e+00 1.800000e-01 1.800000e-01 +3.100000e+01 5.000000e-01 5.000000e-01 3.660000e+00 1.800000e-01 1.800000e-01 +3.300000e+01 5.000000e-01 5.000000e-01 4.480000e+00 2.800000e-01 2.800000e-01 +3.400000e+01 5.000000e-01 5.000000e-01 4.090000e+00 2.000000e-01 2.000000e-01 +3.500000e+01 5.000000e-01 5.000000e-01 4.030000e+00 1.700000e-01 1.700000e-01 +3.610000e+01 6.000000e-01 6.000000e-01 3.930000e+00 1.700000e-01 1.700000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1982_I176887/d02-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1982_I176887/d02-x01-y01 +Title: doi:10.17182/hepdata.6666.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.400000e+01 0.000000e+00 0.000000e+00 4.140000e+00 3.000000e-01 3.000000e-01 +2.200000e+01 0.000000e+00 0.000000e+00 3.890000e+00 1.700000e-01 1.700000e-01 +2.500000e+01 0.000000e+00 0.000000e+00 3.720000e+00 3.800000e-01 3.800000e-01 +3.300000e+01 0.000000e+00 0.000000e+00 3.730000e+00 2.700000e-01 2.700000e-01 +3.400000e+01 0.000000e+00 0.000000e+00 4.130000e+00 1.300000e-01 1.300000e-01 +3.500000e+01 0.000000e+00 0.000000e+00 4.220000e+00 9.000000e-02 9.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1982_I176887/d03-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1982_I176887/d03-x01-y01 +Title: doi:10.17182/hepdata.6666.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.300000e+01 0.000000e+00 0.000000e+00 3.190000e+00 6.300000e-01 6.300000e-01 +3.306000e+01 0.000000e+00 0.000000e+00 3.750000e+00 7.200000e-01 7.200000e-01 +3.308000e+01 0.000000e+00 0.000000e+00 3.280000e+00 1.070000e+00 1.070000e+00 +3.310000e+01 0.000000e+00 0.000000e+00 2.710000e+00 1.060000e+00 1.060000e+00 +3.312000e+01 0.000000e+00 0.000000e+00 5.190000e+00 1.470000e+00 1.470000e+00 +3.314000e+01 0.000000e+00 0.000000e+00 4.040000e+00 1.250000e+00 1.250000e+00 +3.316000e+01 0.000000e+00 0.000000e+00 6.600000e+00 1.580000e+00 1.580000e+00 +3.318000e+01 0.000000e+00 0.000000e+00 2.820000e+00 1.100000e+00 1.100000e+00 +3.320000e+01 0.000000e+00 0.000000e+00 5.520000e+00 1.780000e+00 1.780000e+00 +3.328000e+01 0.000000e+00 0.000000e+00 4.780000e+00 1.410000e+00 1.410000e+00 +3.330000e+01 0.000000e+00 0.000000e+00 4.570000e+00 1.410000e+00 1.410000e+00 +3.332000e+01 0.000000e+00 0.000000e+00 5.850000e+00 1.650000e+00 1.650000e+00 +3.334000e+01 0.000000e+00 0.000000e+00 6.150000e+00 1.730000e+00 1.730000e+00 +3.336000e+01 0.000000e+00 0.000000e+00 3.120000e+00 1.440000e+00 1.440000e+00 +3.338000e+01 0.000000e+00 0.000000e+00 5.680000e+00 1.830000e+00 1.830000e+00 +3.340000e+01 0.000000e+00 0.000000e+00 5.300000e+00 1.500000e+00 1.500000e+00 +3.342000e+01 0.000000e+00 0.000000e+00 2.310000e+00 1.080000e+00 1.080000e+00 +3.344000e+01 0.000000e+00 0.000000e+00 4.500000e+00 1.390000e+00 1.390000e+00 +3.346000e+01 0.000000e+00 0.000000e+00 5.310000e+00 1.500000e+00 1.500000e+00 +3.348000e+01 0.000000e+00 0.000000e+00 4.060000e+00 1.390000e+00 1.390000e+00 +3.350000e+01 0.000000e+00 0.000000e+00 6.540000e+00 1.780000e+00 1.780000e+00 +3.352000e+01 0.000000e+00 0.000000e+00 3.590000e+00 1.230000e+00 1.230000e+00 +3.354000e+01 0.000000e+00 0.000000e+00 3.680000e+00 1.340000e+00 1.340000e+00 +3.356000e+01 0.000000e+00 0.000000e+00 3.330000e+00 1.300000e+00 1.300000e+00 +3.358000e+01 0.000000e+00 0.000000e+00 5.830000e+00 1.640000e+00 1.640000e+00 +3.360000e+01 0.000000e+00 0.000000e+00 3.470000e+00 1.260000e+00 1.260000e+00 +3.362000e+01 0.000000e+00 0.000000e+00 3.180000e+00 1.640000e+00 1.640000e+00 +3.364000e+01 0.000000e+00 0.000000e+00 4.210000e+00 1.440000e+00 1.440000e+00 +3.366000e+01 0.000000e+00 0.000000e+00 8.360000e+00 1.940000e+00 1.940000e+00 +3.368000e+01 0.000000e+00 0.000000e+00 1.400000e+00 8.600000e-01 8.600000e-01 +3.370000e+01 0.000000e+00 0.000000e+00 3.630000e+00 1.320000e+00 1.320000e+00 +3.372000e+01 0.000000e+00 0.000000e+00 3.240000e+00 1.260000e+00 1.260000e+00 +3.374000e+01 0.000000e+00 0.000000e+00 3.160000e+00 1.230000e+00 1.230000e+00 +3.376000e+01 0.000000e+00 0.000000e+00 4.790000e+00 1.480000e+00 1.480000e+00 +3.378000e+01 0.000000e+00 0.000000e+00 5.330000e+00 1.040000e+00 1.040000e+00 +3.380000e+01 0.000000e+00 0.000000e+00 3.650000e+00 7.000000e-01 7.000000e-01 +3.382000e+01 0.000000e+00 0.000000e+00 4.740000e+00 8.700000e-01 8.700000e-01 +3.384000e+01 0.000000e+00 0.000000e+00 4.580000e+00 9.800000e-01 9.800000e-01 +3.386000e+01 0.000000e+00 0.000000e+00 2.740000e+00 8.200000e-01 8.200000e-01 +3.388000e+01 0.000000e+00 0.000000e+00 5.250000e+00 7.200000e-01 7.200000e-01 +3.390000e+01 0.000000e+00 0.000000e+00 4.540000e+00 1.010000e+00 1.010000e+00 +3.392000e+01 0.000000e+00 0.000000e+00 5.180000e+00 1.100000e+00 1.100000e+00 +3.394000e+01 0.000000e+00 0.000000e+00 2.790000e+00 9.100000e-01 9.100000e-01 +3.396000e+01 0.000000e+00 0.000000e+00 5.820000e+00 1.970000e+00 1.970000e+00 +3.400000e+01 0.000000e+00 0.000000e+00 3.770000e+00 8.900000e-01 8.900000e-01 +3.402000e+01 0.000000e+00 0.000000e+00 4.110000e+00 1.400000e+00 1.400000e+00 +3.404000e+01 0.000000e+00 0.000000e+00 3.920000e+00 1.340000e+00 1.340000e+00 +3.406000e+01 0.000000e+00 0.000000e+00 4.080000e+00 1.210000e+00 1.210000e+00 +3.408000e+01 0.000000e+00 0.000000e+00 2.560000e+00 1.010000e+00 1.010000e+00 +3.410000e+01 0.000000e+00 0.000000e+00 4.280000e+00 1.260000e+00 1.260000e+00 +3.412000e+01 0.000000e+00 0.000000e+00 3.280000e+00 1.130000e+00 1.130000e+00 +3.414000e+01 0.000000e+00 0.000000e+00 3.570000e+00 1.300000e+00 1.300000e+00 +3.416000e+01 0.000000e+00 0.000000e+00 6.900000e+00 2.020000e+00 2.020000e+00 +3.418000e+01 0.000000e+00 0.000000e+00 3.820000e+00 1.310000e+00 1.310000e+00 +3.420000e+01 0.000000e+00 0.000000e+00 5.140000e+00 1.230000e+00 1.230000e+00 +3.422000e+01 0.000000e+00 0.000000e+00 2.780000e+00 1.180000e+00 1.180000e+00 +3.424000e+01 0.000000e+00 0.000000e+00 2.140000e+00 1.120000e+00 1.120000e+00 +3.426000e+01 0.000000e+00 0.000000e+00 4.340000e+00 1.340000e+00 1.340000e+00 +3.428000e+01 0.000000e+00 0.000000e+00 1.760000e+00 9.300000e-01 9.300000e-01 +3.430000e+01 0.000000e+00 0.000000e+00 5.860000e+00 1.540000e+00 1.540000e+00 +3.432000e+01 0.000000e+00 0.000000e+00 4.020000e+00 1.300000e+00 1.300000e+00 +3.434000e+01 0.000000e+00 0.000000e+00 5.950000e+00 1.680000e+00 1.680000e+00 +3.436000e+01 0.000000e+00 0.000000e+00 3.650000e+00 1.330000e+00 1.330000e+00 +3.438000e+01 0.000000e+00 0.000000e+00 3.110000e+00 1.070000e+00 1.070000e+00 +3.440000e+01 0.000000e+00 0.000000e+00 3.860000e+00 1.250000e+00 1.250000e+00 +3.442000e+01 0.000000e+00 0.000000e+00 3.460000e+00 1.070000e+00 1.070000e+00 +3.444000e+01 0.000000e+00 0.000000e+00 6.390000e+00 1.620000e+00 1.620000e+00 +3.446000e+01 0.000000e+00 0.000000e+00 5.950000e+00 1.820000e+00 1.820000e+00 +3.448000e+01 0.000000e+00 0.000000e+00 3.100000e+00 1.210000e+00 1.210000e+00 +3.450000e+01 0.000000e+00 0.000000e+00 2.930000e+00 1.240000e+00 1.240000e+00 +3.452000e+01 0.000000e+00 0.000000e+00 3.420000e+00 1.170000e+00 1.170000e+00 +3.454000e+01 0.000000e+00 0.000000e+00 4.000000e+00 1.180000e+00 1.180000e+00 +3.456000e+01 0.000000e+00 0.000000e+00 1.600000e+00 7.600000e-01 7.600000e-01 +3.458000e+01 0.000000e+00 0.000000e+00 3.070000e+00 8.500000e-01 8.500000e-01 +3.460000e+01 0.000000e+00 0.000000e+00 3.950000e+00 1.170000e+00 1.170000e+00 +3.462000e+01 0.000000e+00 0.000000e+00 3.920000e+00 1.270000e+00 1.270000e+00 +3.464000e+01 0.000000e+00 0.000000e+00 4.440000e+00 1.260000e+00 1.260000e+00 +3.466000e+01 0.000000e+00 0.000000e+00 3.830000e+00 1.480000e+00 1.480000e+00 +3.468000e+01 0.000000e+00 0.000000e+00 5.760000e+00 2.070000e+00 2.070000e+00 +3.470000e+01 0.000000e+00 0.000000e+00 5.470000e+00 1.540000e+00 1.540000e+00 +3.472000e+01 0.000000e+00 0.000000e+00 3.910000e+00 1.340000e+00 1.340000e+00 +3.474000e+01 0.000000e+00 0.000000e+00 6.600000e+00 1.670000e+00 1.670000e+00 +3.476000e+01 0.000000e+00 0.000000e+00 3.390000e+00 1.230000e+00 1.230000e+00 +3.478000e+01 0.000000e+00 0.000000e+00 4.270000e+00 1.380000e+00 1.380000e+00 +3.480000e+01 0.000000e+00 0.000000e+00 3.900000e+00 1.150000e+00 1.150000e+00 +3.482000e+01 0.000000e+00 0.000000e+00 2.290000e+00 9.000000e-01 9.000000e-01 +3.484000e+01 0.000000e+00 0.000000e+00 2.080000e+00 8.900000e-01 8.900000e-01 +3.486000e+01 0.000000e+00 0.000000e+00 4.670000e+00 1.440000e+00 1.440000e+00 +3.488000e+01 0.000000e+00 0.000000e+00 3.220000e+00 1.250000e+00 1.250000e+00 +3.490000e+01 0.000000e+00 0.000000e+00 4.870000e+00 1.570000e+00 1.570000e+00 +3.492000e+01 0.000000e+00 0.000000e+00 3.900000e+00 1.790000e+00 1.790000e+00 +3.494000e+01 0.000000e+00 0.000000e+00 5.290000e+00 1.440000e+00 1.440000e+00 +3.496000e+01 0.000000e+00 0.000000e+00 3.930000e+00 1.340000e+00 1.340000e+00 +3.498000e+01 0.000000e+00 0.000000e+00 1.760000e+00 9.300000e-01 9.300000e-01 +3.500000e+01 0.000000e+00 0.000000e+00 4.120000e+00 4.600000e-01 4.600000e-01 +3.502000e+01 0.000000e+00 0.000000e+00 4.040000e+00 1.070000e+00 1.070000e+00 +3.504000e+01 0.000000e+00 0.000000e+00 4.850000e+00 1.110000e+00 1.110000e+00 +3.506000e+01 0.000000e+00 0.000000e+00 1.580000e+00 9.700000e-01 9.700000e-01 +3.508000e+01 0.000000e+00 0.000000e+00 3.310000e+00 1.290000e+00 1.290000e+00 +3.510000e+01 0.000000e+00 0.000000e+00 4.640000e+00 1.680000e+00 1.680000e+00 +3.512000e+01 0.000000e+00 0.000000e+00 2.380000e+00 1.110000e+00 1.110000e+00 +3.514000e+01 0.000000e+00 0.000000e+00 1.550000e+00 9.500000e-01 9.500000e-01 +3.516000e+01 0.000000e+00 0.000000e+00 2.240000e+00 1.050000e+00 1.050000e+00 +3.518000e+01 0.000000e+00 0.000000e+00 4.520000e+00 1.540000e+00 1.540000e+00 +3.520000e+01 0.000000e+00 0.000000e+00 8.470000e+00 2.290000e+00 2.290000e+00 +3.522000e+01 0.000000e+00 0.000000e+00 5.680000e+00 1.830000e+00 1.830000e+00 +3.524000e+01 0.000000e+00 0.000000e+00 4.680000e+00 1.020000e+00 1.020000e+00 +3.526000e+01 0.000000e+00 0.000000e+00 4.360000e+00 1.120000e+00 1.120000e+00 +3.528000e+01 0.000000e+00 0.000000e+00 3.290000e+00 1.200000e+00 1.200000e+00 +3.530000e+01 0.000000e+00 0.000000e+00 3.030000e+00 1.110000e+00 1.110000e+00 +3.532000e+01 0.000000e+00 0.000000e+00 3.470000e+00 1.190000e+00 1.190000e+00 +3.534000e+01 0.000000e+00 0.000000e+00 3.660000e+00 1.250000e+00 1.250000e+00 +3.536000e+01 0.000000e+00 0.000000e+00 5.440000e+00 1.600000e+00 1.600000e+00 +3.538000e+01 0.000000e+00 0.000000e+00 6.470000e+00 1.700000e+00 1.700000e+00 +3.540000e+01 0.000000e+00 0.000000e+00 4.160000e+00 1.280000e+00 1.280000e+00 +3.542000e+01 0.000000e+00 0.000000e+00 3.580000e+00 1.160000e+00 1.160000e+00 +3.544000e+01 0.000000e+00 0.000000e+00 5.300000e+00 1.500000e+00 1.500000e+00 +3.546000e+01 0.000000e+00 0.000000e+00 3.250000e+00 1.370000e+00 1.370000e+00 +3.550000e+01 0.000000e+00 0.000000e+00 2.610000e+00 1.210000e+00 1.210000e+00 +3.552000e+01 0.000000e+00 0.000000e+00 5.070000e+00 1.560000e+00 1.560000e+00 +3.554000e+01 0.000000e+00 0.000000e+00 3.490000e+00 1.200000e+00 1.200000e+00 +3.556000e+01 0.000000e+00 0.000000e+00 4.240000e+00 1.020000e+00 1.020000e+00 +3.558000e+01 0.000000e+00 0.000000e+00 5.580000e+00 1.140000e+00 1.140000e+00 +3.560000e+01 0.000000e+00 0.000000e+00 2.800000e+00 9.200000e-01 9.200000e-01 +3.562000e+01 0.000000e+00 0.000000e+00 4.020000e+00 1.100000e+00 1.100000e+00 +3.568000e+01 0.000000e+00 0.000000e+00 5.000000e+00 1.610000e+00 1.610000e+00 +3.570000e+01 0.000000e+00 0.000000e+00 8.800000e-01 6.900000e-01 6.900000e-01 +3.572000e+01 0.000000e+00 0.000000e+00 2.350000e+00 7.100000e-01 7.100000e-01 +3.574000e+01 0.000000e+00 0.000000e+00 3.470000e+00 8.700000e-01 8.700000e-01 +3.576000e+01 0.000000e+00 0.000000e+00 5.640000e+00 1.220000e+00 1.220000e+00 +3.578000e+01 0.000000e+00 0.000000e+00 9.900000e-01 7.700000e-01 7.700000e-01 +3.580000e+01 0.000000e+00 0.000000e+00 4.500000e+00 7.500000e-01 7.500000e-01 +3.582000e+01 0.000000e+00 0.000000e+00 2.370000e+00 1.230000e+00 1.230000e+00 +3.584000e+01 0.000000e+00 0.000000e+00 5.230000e+00 1.890000e+00 1.890000e+00 +3.586000e+01 0.000000e+00 0.000000e+00 4.520000e+00 1.540000e+00 1.540000e+00 +3.588000e+01 0.000000e+00 0.000000e+00 2.110000e+00 9.900000e-01 9.900000e-01 +3.590000e+01 0.000000e+00 0.000000e+00 3.390000e+00 1.740000e+00 1.740000e+00 +3.592000e+01 0.000000e+00 0.000000e+00 3.780000e+00 1.580000e+00 1.580000e+00 +3.594000e+01 0.000000e+00 0.000000e+00 3.680000e+00 1.540000e+00 1.540000e+00 +3.596000e+01 0.000000e+00 0.000000e+00 2.400000e+00 1.020000e+00 1.020000e+00 +3.598000e+01 0.000000e+00 0.000000e+00 3.190000e+00 1.650000e+00 1.650000e+00 +3.600000e+01 0.000000e+00 0.000000e+00 5.500000e+00 1.870000e+00 1.870000e+00 +3.602000e+01 0.000000e+00 0.000000e+00 2.040000e+00 1.070000e+00 1.070000e+00 +3.604000e+01 0.000000e+00 0.000000e+00 4.770000e+00 1.400000e+00 1.400000e+00 +3.606000e+01 0.000000e+00 0.000000e+00 3.090000e+00 1.200000e+00 1.200000e+00 +3.608000e+01 0.000000e+00 0.000000e+00 2.780000e+00 1.090000e+00 1.090000e+00 +3.610000e+01 0.000000e+00 0.000000e+00 3.060000e+00 1.290000e+00 1.290000e+00 +3.612000e+01 0.000000e+00 0.000000e+00 5.370000e+00 1.650000e+00 1.650000e+00 +3.614000e+01 0.000000e+00 0.000000e+00 5.000000e+00 1.610000e+00 1.610000e+00 +3.616000e+01 0.000000e+00 0.000000e+00 4.540000e+00 1.470000e+00 1.470000e+00 +3.618000e+01 0.000000e+00 0.000000e+00 4.930000e+00 1.520000e+00 1.520000e+00 +3.620000e+01 0.000000e+00 0.000000e+00 2.900000e+00 1.230000e+00 1.230000e+00 +3.622000e+01 0.000000e+00 0.000000e+00 2.540000e+00 1.080000e+00 1.080000e+00 +3.624000e+01 0.000000e+00 0.000000e+00 2.090000e+00 1.100000e+00 1.100000e+00 +3.626000e+01 0.000000e+00 0.000000e+00 6.510000e+00 1.770000e+00 1.770000e+00 +3.628000e+01 0.000000e+00 0.000000e+00 4.460000e+00 1.520000e+00 1.520000e+00 +3.630000e+01 0.000000e+00 0.000000e+00 2.980000e+00 1.380000e+00 1.380000e+00 +3.632000e+01 0.000000e+00 0.000000e+00 3.250000e+00 1.370000e+00 1.370000e+00 +3.634000e+01 0.000000e+00 0.000000e+00 2.260000e+00 1.050000e+00 1.050000e+00 +3.636000e+01 0.000000e+00 0.000000e+00 2.590000e+00 1.350000e+00 1.350000e+00 +3.638000e+01 0.000000e+00 0.000000e+00 7.320000e+00 2.140000e+00 2.140000e+00 +3.642000e+01 0.000000e+00 0.000000e+00 4.820000e+00 1.640000e+00 1.640000e+00 +3.644000e+01 0.000000e+00 0.000000e+00 6.060000e+00 1.710000e+00 1.710000e+00 +3.646000e+01 0.000000e+00 0.000000e+00 3.700000e+00 6.300000e-01 6.300000e-01 +3.648000e+01 0.000000e+00 0.000000e+00 2.900000e+00 1.220000e+00 1.220000e+00 +3.650000e+01 0.000000e+00 0.000000e+00 4.320000e+00 1.400000e+00 1.400000e+00 +3.652000e+01 0.000000e+00 0.000000e+00 3.560000e+00 1.380000e+00 1.380000e+00 +3.654000e+01 0.000000e+00 0.000000e+00 4.720000e+00 1.520000e+00 1.520000e+00 +3.656000e+01 0.000000e+00 0.000000e+00 1.600000e+00 9.800000e-01 9.800000e-01 +3.658000e+01 0.000000e+00 0.000000e+00 3.030000e+00 1.280000e+00 1.280000e+00 +3.660000e+01 0.000000e+00 0.000000e+00 2.230000e+00 1.160000e+00 1.160000e+00 +3.662000e+01 0.000000e+00 0.000000e+00 2.170000e+00 1.130000e+00 1.130000e+00 +3.664000e+01 0.000000e+00 0.000000e+00 2.790000e+00 1.450000e+00 1.450000e+00 +3.666000e+01 0.000000e+00 0.000000e+00 3.310000e+00 6.200000e-01 6.200000e-01 +3.668000e+01 0.000000e+00 0.000000e+00 5.050000e+00 1.950000e+00 1.950000e+00 +3.670000e+01 0.000000e+00 0.000000e+00 2.360000e+00 1.230000e+00 1.230000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1982_I176887/d04-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1982_I176887/d04-x01-y01 +Title: doi:10.17182/hepdata.6666.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000000e+03 0.000000e+00 0.000000e+00 1.800000e-01 1.431782e-01 1.431782e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1982_I176887/d04-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1982_I176887/d04-x01-y02 +Title: doi:10.17182/hepdata.6666.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000000e+03 0.000000e+00 0.000000e+00 4.000000e-01 1.612452e-01 1.612452e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/TASSO_1984_I195333.cc b/analyses/pluginPetra/TASSO_1984_I195333.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1984_I195333.cc @@ -0,0 +1,248 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/Sphericity.hh" +#include "Rivet/Projections/Thrust.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class TASSO_1984_I195333 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(TASSO_1984_I195333); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + const FinalState fs; + declare(fs, "FS"); + declare(Sphericity(fs), "Sphericity"); + declare(Thrust(fs), "Thrust"); + + // counters for R + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + _h_weight = 0.; + unsigned int iloc(0); + if(fuzzyEquals(sqrtS()/GeV, 14 , 1E-3)) + iloc = 1; + else if(fuzzyEquals(sqrtS()/GeV, 22 , 1E-3)) + iloc = 2; + else if(fuzzyEquals(sqrtS()/GeV, 34 , 1E-3)) + iloc = 3; + if(iloc!=0) { + _h_mult = bookHisto1D( 3,1,iloc); + _h_p = bookHisto1D( 5,1,iloc); + _h_xp = bookHisto1D( 6,1,iloc); + _h_pl = bookHisto1D( 7,1,iloc); + _h_pt = bookHisto1D( 8,1,iloc); + _h_pt2 = bookHisto1D( 9,1,iloc); + _h_xl = bookHisto1D(10,1,iloc); + _h_xT = bookHisto1D(11,1,iloc); + _h_S = bookHisto1D(12,1,iloc); + _h_T = bookHisto1D(13,1,iloc); + _h_y = bookHisto1D(14,1,iloc); + } + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + unsigned int nCharged(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + if(PID::isCharged(p.pdgId())) ++nCharged; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) { + _c_muons->fill(event.weight()); + return; + } + // everything else + _c_hadrons->fill(event.weight()); + _h_weight +=event.weight(); + _n_charged.fill(nCharged,event.weight()); + _n_total.fill(ntotal,event.weight()); + // thrust + const Thrust& thrust = apply(event, "Thrust"); + _thrust.fill(thrust.thrust(),event.weight()); + // sphericity + const Sphericity& sphericity = apply(event, "Sphericity"); + _sphericity.fill(sphericity.sphericity(), event.weight()); + // global distributions + if(_h_mult) _h_mult->fill(nCharged,event.weight()); + if(_h_S) _h_S ->fill(sphericity.sphericity(), event.weight()); + if(_h_T) _h_T ->fill(thrust.thrust(), event.weight()); + // single particle distributions + foreach (const Particle& p, fs.particles()) { + if(!PID::isCharged(p.pdgId())) continue; + const Vector3 mom3 = p.p3(); + double pp = mom3.mod(); + _p_total.fill(pp); + if(_h_p) _h_p ->fill(pp,event.weight()); + if(_h_xp) _h_xp->fill(2.*pp/sqrtS(),event.weight()); + const double mom = dot(sphericity.sphericityAxis(), mom3); + _p_l.fill(fabs(mom),event.weight()); + if(_h_pl) _h_pl->fill(fabs(mom),event.weight()); + if(_h_xl) _h_xl->fill(2.*fabs(mom)/sqrtS(),event.weight()); + const double pTin = dot(mom3, sphericity.sphericityMajorAxis()); + _pt2_in.fill(sqr(pTin),event.weight()); + const double pTout = dot(mom3, sphericity.sphericityMinorAxis()); + _pt2_out.fill(sqr(pTout),event.weight()); + double pT = sqr(pTin) + sqr(pTout); + _pt2.fill(pT,event.weight()); + if(_h_pt2) _h_pt2->fill(pT,event.weight()); + pT=sqrt(pT); + _pt.fill(pT,event.weight()); + if(_h_pt) _h_pt->fill(pT,event.weight()); + if(_h_xT) _h_xT->fill(2.*pT/sqrtS(),event.weight()); + if(_h_y) { + const double rap = 0.5 * log((p.E() + mom) / + (p.E() - mom)); + _h_y->fill(fabs(rap),event.weight()); + } + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + // charged particle multiplicity distribution + if(_h_mult) normalize(_h_mult,2.); + for(unsigned int iy=1;iy<12;++iy) { + double value,error; + if(iy==1) { + value = _n_charged.xMean(); + error = _n_charged.xStdErr(); + } + else if(iy==2) { + double num = _n_charged.xMean(); + double den = _n_total.xMean(); + value = num/den; + error = value*sqrt(sqr(_n_charged.xStdErr()/num)+sqr(_n_total.xStdErr()/den)); + } + else if(iy==3) { + value = _n_charged.xStdDev(); + error = _n_charged.xStdErr(); + } + else if(iy==4) { + value = _sphericity.xMean(); + error = _sphericity.xStdErr(); + } + else if(iy==5) { + value = _thrust.xMean(); + error = _thrust.xStdErr(); + } + else if(iy==6) { + value = _p_total.xMean(); + error = _p_total.xStdErr(); + } + else if(iy==7) { + value = _p_l.xMean(); + error = _p_l.xStdErr(); + } + else if(iy==8) { + value = _pt.xMean(); + error = _pt.xStdErr(); + } + else if(iy==9) { + value = _pt2.xMean(); + error = _pt2.xStdErr(); + } + else if(iy==10) { + value = _pt2_in.xMean(); + error = _pt2_in.xStdErr(); + } + else if(iy==11) { + value = _pt2_out.xMean(); + error = _pt2_out.xStdErr(); + } + Scatter2D temphisto(refData(4, 1, iy)); + Scatter2DPtr mult = bookScatter2D(4, 1, iy); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, value, ex, make_pair(error,error)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + // scale the distributions + scale(_h_p ,1./_h_weight); + scale(_h_xp ,1./_h_weight); + scale(_h_pl ,1./_h_weight); + scale(_h_pt ,1./_h_weight); + scale(_h_pt2,1./_h_weight); + scale(_h_xl ,1./_h_weight); + scale(_h_xT ,1./_h_weight); + scale(_h_S ,1./_h_weight); + scale(_h_T ,1./_h_weight); + scale(_h_y ,1./_h_weight); + } + + //@} + + + /// @name Histograms + //@{ + Histo1DPtr _h_mult,_h_p,_h_xp,_h_pl,_h_pt,_h_pt2,_h_xl,_h_xT,_h_S,_h_T,_h_y; + CounterPtr _c_hadrons, _c_muons; + YODA::Dbn1D _n_charged,_n_total,_sphericity,_thrust,_p_total, + _p_l,_pt,_pt2,_pt2_in,_pt2_out; + double _h_weight; + //@} + + }; + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(TASSO_1984_I195333); + +} diff --git a/analyses/pluginPetra/TASSO_1984_I195333.info b/analyses/pluginPetra/TASSO_1984_I195333.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1984_I195333.info @@ -0,0 +1,35 @@ +Name: TASSO_1984_I195333 +Year: 1984 +Summary: Measurements of charged particle multiplicities, $R$ and event shapes between 12 and 43 GeV +Experiment: TASSO +Collider: PETRA +InspireID: 195333 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Z.Phys. C22 (1984) 307-340, 1984 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$, charged particle multiplicites and event shapes in $e^+e^-$ collisions for energies between 12 and 43 GeV. + The average charged particle multiplicity, thrust and sphericity are measured for a range of energies. The distributions + are available for 12, 22 and 34 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Althoff:1983ew +BibTeX: '@article{Althoff:1983ew, + author = "Althoff, M. and others", + title = "{Jet Production and Fragmentation in e+ e- Annihilation + at 12-GeV to 43-GeV}", + collaboration = "TASSO", + journal = "Z. Phys.", + volume = "C22", + year = "1984", + pages = "307-340", + doi = "10.1007/BF01547419", + reportNumber = "DESY-83-130", + SLACcitation = "%%CITATION = ZEPYA,C22,307;%%" +}' diff --git a/analyses/pluginPetra/TASSO_1984_I195333.plot b/analyses/pluginPetra/TASSO_1984_I195333.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1984_I195333.plot @@ -0,0 +1,340 @@ +BEGIN PLOT /TASSO_1984_I195333/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d03-x01-y01 +Title=Charged Particle Multiplicity at 14 GeV +XLabel=$N$ +YLabel=Probability +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d03-x01-y02 +Title=Charged Particle Multiplicity at 22 GeV +XLabel=$N$ +YLabel=Probability +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d03-x01-y03 +Title=Charged Particle Multiplicity at 34 GeV +XLabel=$N$ +YLabel=Probability +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y01 +Title=Averaged Charged particle Multiplicity +XLabel=$\sqrt{s}/$GeV +YLabel=$\langle N_{\text{charged}}\rangle$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y02 +Title=Charged Particle Fraction +XLabel=$\sqrt{s}/$GeV +YLabel=$f_{\text{charged}}$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y03 +Title=Charged Particle Dispersion +XLabel=$\sqrt{s}/$GeV +YLabel=$D$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y04 +Title=Average Sphericity +XLabel=$\sqrt{s}/$GeV +YLabel=$\langle S\rangle$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y05 +Title=Average Thrust +XLabel=$\sqrt{s}/$GeV +YLabel=$\langle T\rangle$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y06 +Title=Average Particle Momentum +XLabel=$\sqrt{s}/$GeV +YLabel=$\langle p\rangle$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y07 +Title=Average Particle Longitudinal Momentum +XLabel=$\sqrt{s}/$GeV +YLabel=$\langle p_l\rangle$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y08 +Title=Average Particle Transverse Momentum +XLabel=$\sqrt{s}/$GeV +YLabel=$\langle p_T\rangle$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y09 +Title=Average Particle Transverse Momentum Squared +XLabel=$\sqrt{s}/$GeV +YLabel=$\langle p^2_T\rangle$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y10 +Title=Average Particle Transverse Momentum Squared +XLabel=$\sqrt{s}/$GeV +YLabel=$\langle p^2_{T\text{in}}\rangle$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d04-x01-y11 +Title=Average Particle Transverse Momentum Squared +XLabel=$\sqrt{s}/$GeV +YLabel=$\langle p^2_{T\text{out}}\rangle$ +LogY=0 +ConnectGaps=1 +END PLOT + + +BEGIN PLOT /TASSO_1984_I195333/d05-x01-y01 +Title=Charged Particle Momentum at 14 GeV +XLabel=$p$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d05-x01-y02 +Title=Charged Particle Momentum at 22 GeV +XLabel=$p$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d05-x01-y03 +Title=Charged Particle Momentum at 34 GeV +XLabel=$p$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p}$ +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /TASSO_1984_I195333/d06-x01-y01 +Title=Charged Particle Momentum at 14 GeV +XLabel=$x_p$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}x_p}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d06-x01-y02 +Title=Charged Particle Momentum at 22 GeV +XLabel=$x_p$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}x_p}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d06-x01-y03 +Title=Charged Particle Momentum at 34 GeV +XLabel=$x_p$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}x_p}$ +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /TASSO_1984_I195333/d07-x01-y01 +Title=Charged Particle Momentum at 14 GeV +XLabel=$p_\|$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p_\|}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d07-x01-y02 +Title=Charged Particle Momentum at 22 GeV +XLabel=$p_\|$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p_\|}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d07-x01-y03 +Title=Charged Particle Momentum at 34 GeV +XLabel=$p_\|$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p_\|}$ +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /TASSO_1984_I195333/d08-x01-y01 +Title=Charged Particle Transverse Momentum at 14 GeV +XLabel=$p_\perp$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p_\perp}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d08-x01-y02 +Title=Charged Particle Transverse Momentum at 22 GeV +XLabel=$p_\perp$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p_\perp}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d08-x01-y03 +Title=Charged Particle Transverse Momentum at 34 GeV +XLabel=$p_\perp$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p_\perp}$ +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /TASSO_1984_I195333/d09-x01-y01 +Title=Charged Particle Transverse Momentum at 14 GeV +XLabel=$p^2_\perp$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p^2_\perp}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d09-x01-y02 +Title=Charged Particle Transverse Momentum at 22 GeV +XLabel=$p^2_\perp$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p^2_\perp}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d09-x01-y03 +Title=Charged Particle Transverse Momentum at 34 GeV +XLabel=$p^2_\perp$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}p^2_\perp}$ +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /TASSO_1984_I195333/d10-x01-y01 +Title=Charged Particle Momentum at 14 GeV +XLabel=$x_{p_\|}$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}x_{p_\|}}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d10-x01-y02 +Title=Charged Particle Momentum at 22 GeV +XLabel=$x_{p_\|}$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}x_{p_\|}}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d10-x01-y03 +Title=Charged Particle Momentum at 34 GeV +XLabel=$x_{p_\|}$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}x_{p_\|}}$ +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /TASSO_1984_I195333/d11-x01-y01 +Title=Charged Particle Transverse Momentum at 14 GeV +XLabel=$x_\perp$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}x_\perp}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d11-x01-y02 +Title=Charged Particle Transverse Momentum at 22 GeV +XLabel=$x_\perp$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}x_\perp}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d11-x01-y03 +Title=Charged Particle Transverse Momentum at 34 GeV +XLabel=$x_\perp$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}x_\perp}$ +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /TASSO_1984_I195333/d12-x01-y01 +Title=Sphericity at 14 GeV +XLabel=$S$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}S}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d12-x01-y02 +Title=Sphericity at 22 GeV +XLabel=$S$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}S}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d12-x01-y03 +Title=Sphericity at 34 GeV +XLabel=$S$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}S}$ +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /TASSO_1984_I195333/d13-x01-y01 +Title=Thrust at 14 GeV +XLabel=$T$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}T}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d13-x01-y02 +Title=Thrust at 22 GeV +XLabel=$T$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}T}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d13-x01-y03 +Title=Thrust at 34 GeV +XLabel=$T$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}T}$ +LogY=1 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /TASSO_1984_I195333/d14-x01-y01 +Title=Charged Particle Rapidity at 14 GeV +XLabel=$|y|$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}|y|}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d14-x01-y02 +Title=Charged Particle Rapidity at 22 GeV +XLabel=$|y|$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}|y|}$ +LogY=1 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I195333/d14-x01-y03 +Title=Charged Particle Rapidity at 34 GeV +XLabel=$|y|$ +YLabel=$\frac1{\sigma}\frac{\text{d}\sigma}{\text{d}|y|}$ +LogY=1 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginPetra/TASSO_1984_I195333.yoda b/analyses/pluginPetra/TASSO_1984_I195333.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1984_I195333.yoda @@ -0,0 +1,1102 @@ +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d01-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d01-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 3.800000e+00 2.800000e-01 2.800000e-01 +1.400000e+01 0.000000e+00 0.000000e+00 4.140000e+00 3.000000e-01 3.000000e-01 +2.200000e+01 0.000000e+00 0.000000e+00 3.890000e+00 1.700000e-01 1.700000e-01 +2.500000e+01 0.000000e+00 0.000000e+00 3.720000e+00 3.800000e-01 3.800000e-01 +2.750000e+01 1.000000e-01 2.000000e-01 3.910000e+00 3.200000e-01 3.200000e-01 +3.010000e+01 2.000000e-01 0.000000e+00 3.940000e+00 1.800000e-01 1.800000e-01 +3.110000e+01 6.000000e-01 4.000000e-01 3.660000e+00 1.800000e-01 1.800000e-01 +3.320000e+01 7.000000e-01 3.000000e-01 4.090000e+00 1.900000e-01 1.900000e-01 +3.400000e+01 5.000000e-01 5.000000e-01 4.120000e+00 1.100000e-01 1.100000e-01 +3.470000e+01 2.000000e-01 8.000000e-01 4.080000e+00 9.000000e-02 9.000000e-02 +3.610000e+01 6.000000e-01 6.000000e-01 3.930000e+00 1.900000e-01 1.900000e-01 +4.140000e+01 2.700000e+00 1.700000e+00 4.060000e+00 2.900000e-01 2.900000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d02-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d02-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.855000e+01 1.455000e+01 1.455000e+01 4.040000e+00 1.910497e-01 1.910497e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d03-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d03-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.000000e+00 1.000000e+00 1.000000e+00 1.000000e-03 1.000000e-03 1.000000e-03 +2.000000e+00 1.000000e+00 1.000000e+00 1.700000e-02 8.000000e-03 8.000000e-03 +4.000000e+00 1.000000e+00 1.000000e+00 7.600000e-02 1.000000e-02 1.000000e-02 +6.000000e+00 1.000000e+00 1.000000e+00 1.720000e-01 1.100000e-02 1.100000e-02 +8.000000e+00 1.000000e+00 1.000000e+00 2.480000e-01 1.300000e-02 1.300000e-02 +1.000000e+01 1.000000e+00 1.000000e+00 2.260000e-01 1.500000e-02 1.500000e-02 +1.200000e+01 1.000000e+00 1.000000e+00 1.480000e-01 1.500000e-02 1.500000e-02 +1.400000e+01 1.000000e+00 1.000000e+00 7.200000e-02 1.200000e-02 1.200000e-02 +1.600000e+01 1.000000e+00 1.000000e+00 2.700000e-02 9.000000e-03 9.000000e-03 +1.800000e+01 1.000000e+00 1.000000e+00 9.000000e-03 5.000000e-03 5.000000e-03 +2.000000e+01 1.000000e+00 1.000000e+00 3.000000e-03 2.000000e-03 2.000000e-03 +2.200000e+01 1.000000e+00 1.000000e+00 1.000000e-03 1.000000e-03 1.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d03-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d03-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.000000e+00 1.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.000000e+00 1.000000e+00 1.000000e+00 5.000000e-03 3.000000e-03 3.000000e-03 +4.000000e+00 1.000000e+00 1.000000e+00 2.800000e-02 7.000000e-03 7.000000e-03 +6.000000e+00 1.000000e+00 1.000000e+00 8.500000e-02 1.000000e-02 1.000000e-02 +8.000000e+00 1.000000e+00 1.000000e+00 1.730000e-01 1.300000e-02 1.300000e-02 +1.000000e+01 1.000000e+00 1.000000e+00 2.080000e-01 1.400000e-02 1.400000e-02 +1.200000e+01 1.000000e+00 1.000000e+00 2.040000e-01 1.700000e-02 1.700000e-02 +1.400000e+01 1.000000e+00 1.000000e+00 1.400000e-01 1.700000e-02 1.700000e-02 +1.600000e+01 1.000000e+00 1.000000e+00 8.600000e-02 1.500000e-02 1.500000e-02 +1.800000e+01 1.000000e+00 1.000000e+00 4.100000e-02 1.500000e-02 1.500000e-02 +2.000000e+01 1.000000e+00 1.000000e+00 1.800000e-02 1.000000e-02 1.000000e-02 +2.200000e+01 1.000000e+00 1.000000e+00 7.000000e-03 4.000000e-03 4.000000e-03 +2.400000e+01 1.000000e+00 1.000000e+00 2.000000e-03 1.000000e-03 1.000000e-03 +2.600000e+01 1.000000e+00 1.000000e+00 1.000000e-03 1.000000e-03 1.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d03-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d03-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.000000e+00 1.000000e+00 1.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.000000e+00 1.000000e+00 1.000000e+00 3.000000e-03 2.000000e-03 2.000000e-03 +4.000000e+00 1.000000e+00 1.000000e+00 1.500000e-02 8.000000e-03 8.000000e-03 +6.000000e+00 1.000000e+00 1.000000e+00 4.300000e-02 2.000000e-03 2.000000e-03 +8.000000e+00 1.000000e+00 1.000000e+00 8.800000e-02 3.000000e-03 3.000000e-03 +1.000000e+01 1.000000e+00 1.000000e+00 1.460000e-01 3.000000e-03 3.000000e-03 +1.200000e+01 1.000000e+00 1.000000e+00 1.850000e-01 4.000000e-03 4.000000e-03 +1.400000e+01 1.000000e+00 1.000000e+00 1.800000e-01 5.000000e-03 5.000000e-03 +1.600000e+01 1.000000e+00 1.000000e+00 1.420000e-01 5.000000e-03 5.000000e-03 +1.800000e+01 1.000000e+00 1.000000e+00 9.200000e-02 4.000000e-03 4.000000e-03 +2.000000e+01 1.000000e+00 1.000000e+00 5.200000e-02 4.000000e-03 4.000000e-03 +2.200000e+01 1.000000e+00 1.000000e+00 2.800000e-02 3.000000e-03 3.000000e-03 +2.400000e+01 1.000000e+00 1.000000e+00 1.500000e-02 3.000000e-03 3.000000e-03 +2.600000e+01 1.000000e+00 1.000000e+00 6.000000e-03 2.000000e-03 2.000000e-03 +2.800000e+01 1.000000e+00 1.000000e+00 2.000000e-03 1.000000e-03 1.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 8.480000e+00 2.100000e-01 2.100000e-01 +1.400000e+01 0.000000e+00 0.000000e+00 9.080000e+00 5.000000e-02 5.000000e-02 +2.200000e+01 0.000000e+00 0.000000e+00 1.122000e+01 7.000000e-02 7.000000e-02 +2.500000e+01 0.000000e+00 0.000000e+00 1.169000e+01 2.400000e-01 2.400000e-01 +3.050000e+01 0.000000e+00 0.000000e+00 1.279000e+01 1.300000e-01 1.300000e-01 +3.450000e+01 0.000000e+00 0.000000e+00 1.348000e+01 3.000000e-02 3.000000e-02 +4.150000e+01 0.000000e+00 0.000000e+00 1.441000e+01 2.400000e-01 2.400000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 5.900000e-01 2.000000e-02 2.000000e-02 +1.400000e+01 0.000000e+00 0.000000e+00 5.800000e-01 1.000000e-02 1.000000e-02 +2.200000e+01 0.000000e+00 0.000000e+00 5.800000e-01 1.000000e-02 1.000000e-02 +2.500000e+01 0.000000e+00 0.000000e+00 5.800000e-01 2.000000e-02 2.000000e-02 +3.050000e+01 0.000000e+00 0.000000e+00 6.000000e-01 1.000000e-02 1.000000e-02 +3.450000e+01 0.000000e+00 0.000000e+00 5.900000e-01 2.000000e-03 2.000000e-03 +4.150000e+01 0.000000e+00 0.000000e+00 5.800000e-01 1.500000e-02 1.500000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.400000e+01 0.000000e+00 0.000000e+00 3.240000e+00 8.000000e-02 8.000000e-02 +2.200000e+01 0.000000e+00 0.000000e+00 3.810000e+00 2.500000e-01 2.500000e-01 +3.450000e+01 0.000000e+00 0.000000e+00 4.460000e+00 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y04 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y04 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 2.550000e-01 1.700000e-02 1.700000e-02 +1.400000e+01 0.000000e+00 0.000000e+00 2.130000e-01 4.000000e-03 4.000000e-03 +2.200000e+01 0.000000e+00 0.000000e+00 1.450000e-01 4.000000e-03 4.000000e-03 +2.500000e+01 0.000000e+00 0.000000e+00 1.270000e-01 9.000000e-03 9.000000e-03 +3.050000e+01 0.000000e+00 0.000000e+00 1.120000e-01 6.000000e-03 6.000000e-03 +3.450000e+01 0.000000e+00 0.000000e+00 1.080000e-01 1.000000e-03 1.000000e-03 +4.150000e+01 0.000000e+00 0.000000e+00 1.080000e-01 5.000000e-03 5.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y05 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y05 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 8.400000e-01 8.000000e-03 8.000000e-03 +1.400000e+01 0.000000e+00 0.000000e+00 8.550000e-01 2.000000e-03 2.000000e-03 +2.200000e+01 0.000000e+00 0.000000e+00 8.840000e-01 2.000000e-03 2.000000e-03 +2.500000e+01 0.000000e+00 0.000000e+00 8.980000e-01 5.000000e-03 5.000000e-03 +3.050000e+01 0.000000e+00 0.000000e+00 9.000000e-01 3.000000e-03 3.000000e-03 +3.450000e+01 0.000000e+00 0.000000e+00 9.020000e-01 1.000000e-03 1.000000e-03 +4.150000e+01 0.000000e+00 0.000000e+00 9.050000e-01 3.000000e-03 3.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y06 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y06 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 8.410000e-01 2.100000e-02 2.100000e-02 +1.400000e+01 0.000000e+00 0.000000e+00 8.950000e-01 6.000000e-03 6.000000e-03 +2.200000e+01 0.000000e+00 0.000000e+00 1.163000e+00 1.000000e-02 1.000000e-02 +2.500000e+01 0.000000e+00 0.000000e+00 1.233000e+00 3.200000e-02 3.200000e-02 +3.050000e+01 0.000000e+00 0.000000e+00 1.424000e+00 1.900000e-02 1.900000e-02 +3.450000e+01 0.000000e+00 0.000000e+00 1.512000e+00 4.000000e-03 4.000000e-03 +4.150000e+01 0.000000e+00 0.000000e+00 1.671000e+00 1.900000e-02 1.900000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y07 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y07 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 6.830000e-01 2.300000e-02 2.300000e-02 +1.400000e+01 0.000000e+00 0.000000e+00 7.560000e-01 7.000000e-03 7.000000e-03 +2.200000e+01 0.000000e+00 0.000000e+00 1.019000e+00 1.100000e-02 1.100000e-02 +2.500000e+01 0.000000e+00 0.000000e+00 1.075000e+00 3.100000e-02 3.100000e-02 +3.050000e+01 0.000000e+00 0.000000e+00 1.281000e+00 2.200000e-02 2.200000e-02 +3.450000e+01 0.000000e+00 0.000000e+00 1.350000e+00 5.000000e-03 5.000000e-03 +4.150000e+01 0.000000e+00 0.000000e+00 1.523000e+00 2.200000e-02 2.200000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y08 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y08 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 3.400000e-01 7.000000e-03 7.000000e-03 +1.400000e+01 0.000000e+00 0.000000e+00 3.340000e-01 2.000000e-03 2.000000e-03 +2.200000e+01 0.000000e+00 0.000000e+00 3.770000e-01 3.000000e-03 3.000000e-03 +2.500000e+01 0.000000e+00 0.000000e+00 3.680000e-01 7.000000e-03 7.000000e-03 +3.050000e+01 0.000000e+00 0.000000e+00 4.040000e-01 4.000000e-03 4.000000e-03 +3.450000e+01 0.000000e+00 0.000000e+00 4.220000e-01 1.000000e-03 1.000000e-03 +4.150000e+01 0.000000e+00 0.000000e+00 4.880000e-01 4.000000e-03 4.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y09 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y09 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 1.710000e-01 8.000000e-03 8.000000e-03 +1.400000e+01 0.000000e+00 0.000000e+00 1.680000e-01 2.000000e-03 2.000000e-03 +2.200000e+01 0.000000e+00 0.000000e+00 2.320000e-01 4.000000e-03 4.000000e-03 +2.500000e+01 0.000000e+00 0.000000e+00 2.130000e-01 9.000000e-03 9.000000e-03 +3.050000e+01 0.000000e+00 0.000000e+00 2.810000e-01 8.000000e-03 8.000000e-03 +3.450000e+01 0.000000e+00 0.000000e+00 3.110000e-01 2.000000e-03 2.000000e-03 +4.150000e+01 0.000000e+00 0.000000e+00 3.500000e-01 9.000000e-03 9.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y10 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y10 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 1.280000e-01 9.000000e-03 9.000000e-03 +1.400000e+01 0.000000e+00 0.000000e+00 1.310000e-01 2.000000e-03 2.000000e-03 +2.200000e+01 0.000000e+00 0.000000e+00 1.840000e-01 9.000000e-03 9.000000e-03 +2.500000e+01 0.000000e+00 0.000000e+00 1.610000e-01 1.100000e-02 1.100000e-02 +3.050000e+01 0.000000e+00 0.000000e+00 2.230000e-01 1.200000e-02 1.200000e-02 +3.450000e+01 0.000000e+00 0.000000e+00 2.510000e-01 3.000000e-03 3.000000e-03 +4.150000e+01 0.000000e+00 0.000000e+00 2.800000e-01 1.200000e-02 1.200000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d04-x01-y11 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d04-x01-y11 +Title: doi:10.17182/hepdata.16272.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.200000e+01 0.000000e+00 0.000000e+00 4.400000e-02 2.000000e-03 2.000000e-03 +1.400000e+01 0.000000e+00 0.000000e+00 4.400000e-02 1.000000e-03 1.000000e-03 +2.200000e+01 0.000000e+00 0.000000e+00 5.900000e-02 2.000000e-03 2.000000e-03 +2.500000e+01 0.000000e+00 0.000000e+00 5.500000e-02 2.000000e-03 2.000000e-03 +3.050000e+01 0.000000e+00 0.000000e+00 6.100000e-02 2.000000e-03 2.000000e-03 +3.450000e+01 0.000000e+00 0.000000e+00 6.800000e-02 1.000000e-03 1.000000e-03 +4.150000e+01 0.000000e+00 0.000000e+00 7.500000e-02 2.000000e-03 2.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d05-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d05-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.500000e-01 5.000000e-02 5.000000e-02 6.224000e+00 1.840000e-01 1.840000e-01 +2.500000e-01 5.000000e-02 5.000000e-02 1.034000e+01 2.300000e-01 2.300000e-01 +3.500000e-01 5.000000e-02 5.000000e-02 9.898000e+00 2.250000e-01 2.250000e-01 +4.500000e-01 5.000000e-02 5.000000e-02 8.592000e+00 2.050000e-01 2.050000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 7.251000e+00 1.880000e-01 1.880000e-01 +6.500000e-01 5.000000e-02 5.000000e-02 5.840000e+00 1.670000e-01 1.670000e-01 +7.500000e-01 5.000000e-02 5.000000e-02 4.957000e+00 1.540000e-01 1.540000e-01 +9.000000e-01 1.000000e-01 1.000000e-01 3.934000e+00 9.600000e-02 9.600000e-02 +1.100000e+00 1.000000e-01 1.000000e-01 2.893000e+00 8.300000e-02 8.300000e-02 +1.300000e+00 1.000000e-01 1.000000e-01 2.204000e+00 7.300000e-02 7.300000e-02 +1.500000e+00 1.000000e-01 1.000000e-01 1.778000e+00 6.600000e-02 6.600000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 1.315000e+00 5.700000e-02 5.700000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 1.077000e+00 5.200000e-02 5.200000e-02 +2.100000e+00 1.000000e-01 1.000000e-01 8.350000e-01 4.600000e-02 4.600000e-02 +2.300000e+00 1.000000e-01 1.000000e-01 7.510000e-01 4.400000e-02 4.400000e-02 +2.500000e+00 1.000000e-01 1.000000e-01 5.230000e-01 3.700000e-02 3.700000e-02 +2.700000e+00 1.000000e-01 1.000000e-01 3.840000e-01 3.200000e-02 3.200000e-02 +2.900000e+00 1.000000e-01 1.000000e-01 3.420000e-01 3.000000e-02 3.000000e-02 +3.250000e+00 2.500000e-01 2.500000e-01 2.090000e-01 1.500000e-02 1.500000e-02 +3.750000e+00 2.500000e-01 2.500000e-01 1.340000e-01 1.200000e-02 1.200000e-02 +5.000000e+00 1.000000e+00 1.000000e+00 3.600000e-02 3.000000e-03 3.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d05-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d05-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.500000e-01 5.000000e-02 5.000000e-02 6.248000e+00 2.140000e-01 2.140000e-01 +2.500000e-01 5.000000e-02 5.000000e-02 1.027000e+01 2.750000e-01 2.750000e-01 +3.500000e-01 5.000000e-02 5.000000e-02 1.011000e+01 2.720000e-01 2.720000e-01 +4.500000e-01 5.000000e-02 5.000000e-02 9.045000e+00 2.580000e-01 2.580000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 7.885000e+00 2.410000e-01 2.410000e-01 +6.500000e-01 5.000000e-02 5.000000e-02 7.236000e+00 2.310000e-01 2.310000e-01 +7.500000e-01 5.000000e-02 5.000000e-02 6.207000e+00 2.140000e-01 2.140000e-01 +9.000000e-01 1.000000e-01 1.000000e-01 5.028000e+00 1.360000e-01 1.360000e-01 +1.100000e+00 1.000000e-01 1.000000e-01 3.836000e+00 1.190000e-01 1.190000e-01 +1.300000e+00 1.000000e-01 1.000000e-01 2.883000e+00 1.030000e-01 1.030000e-01 +1.500000e+00 1.000000e-01 1.000000e-01 2.264000e+00 9.100000e-02 9.100000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 1.951000e+00 8.500000e-02 8.500000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 1.422000e+00 7.300000e-02 7.300000e-02 +2.100000e+00 1.000000e-01 1.000000e-01 1.352000e+00 7.100000e-02 7.100000e-02 +2.300000e+00 1.000000e-01 1.000000e-01 1.097000e+00 6.400000e-02 6.400000e-02 +2.500000e+00 1.000000e-01 1.000000e-01 8.160000e-01 5.500000e-02 5.500000e-02 +2.700000e+00 1.000000e-01 1.000000e-01 8.110000e-01 5.500000e-02 5.500000e-02 +2.900000e+00 1.000000e-01 1.000000e-01 6.310000e-01 4.900000e-02 4.900000e-02 +3.250000e+00 2.500000e-01 2.500000e-01 4.840000e-01 2.700000e-02 2.700000e-02 +3.750000e+00 2.500000e-01 2.500000e-01 3.070000e-01 2.100000e-02 2.100000e-02 +5.000000e+00 1.000000e+00 1.000000e+00 1.440000e-01 8.000000e-03 8.000000e-03 +7.000000e+00 1.000000e+00 1.000000e+00 3.800000e-02 4.000000e-03 4.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d05-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d05-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.500000e-01 5.000000e-02 5.000000e-02 6.298000e+00 7.600000e-02 7.600000e-02 +2.500000e-01 5.000000e-02 5.000000e-02 1.067000e+01 9.900000e-02 9.900000e-02 +3.500000e-01 5.000000e-02 5.000000e-02 1.051000e+01 9.800000e-02 9.800000e-02 +4.500000e-01 5.000000e-02 5.000000e-02 9.628000e+00 9.400000e-02 9.400000e-02 +5.500000e-01 5.000000e-02 5.000000e-02 8.546000e+00 8.800000e-02 8.800000e-02 +6.500000e-01 5.000000e-02 5.000000e-02 7.737000e+00 8.400000e-02 8.400000e-02 +7.500000e-01 5.000000e-02 5.000000e-02 6.638000e+00 7.800000e-02 7.800000e-02 +9.000000e-01 1.000000e-01 1.000000e-01 5.495000e+00 5.000000e-02 5.000000e-02 +1.100000e+00 1.000000e-01 1.000000e-01 4.294000e+00 4.400000e-02 4.400000e-02 +1.300000e+00 1.000000e-01 1.000000e-01 3.534000e+00 4.000000e-02 4.000000e-02 +1.500000e+00 1.000000e-01 1.000000e-01 2.778000e+00 3.600000e-02 3.600000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 2.465000e+00 3.400000e-02 3.400000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 2.088000e+00 3.100000e-02 3.100000e-02 +2.100000e+00 1.000000e-01 1.000000e-01 1.710000e+00 2.800000e-02 2.800000e-02 +2.300000e+00 1.000000e-01 1.000000e-01 1.510000e+00 2.600000e-02 2.600000e-02 +2.500000e+00 1.000000e-01 1.000000e-01 1.238000e+00 2.400000e-02 2.400000e-02 +2.700000e+00 1.000000e-01 1.000000e-01 1.124000e+00 2.300000e-02 2.300000e-02 +2.900000e+00 1.000000e-01 1.000000e-01 9.600000e-01 2.100000e-02 2.100000e-02 +3.250000e+00 2.500000e-01 2.500000e-01 8.020000e-01 1.200000e-02 1.200000e-02 +3.750000e+00 2.500000e-01 2.500000e-01 5.860000e-01 1.100000e-02 1.100000e-02 +5.000000e+00 1.000000e+00 1.000000e+00 2.950000e-01 4.000000e-03 4.000000e-03 +7.000000e+00 1.000000e+00 1.000000e+00 1.170000e-01 3.000000e-03 3.000000e-03 +9.000000e+00 1.000000e+00 1.000000e+00 4.600000e-02 2.000000e-03 2.000000e-03 +1.100000e+01 1.000000e+00 1.000000e+00 8.000000e-03 1.000000e-03 1.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d06-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d06-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 5.000000e-03 5.000000e-03 5.498000e+01 3.460000e+00 3.460000e+00 +3.500000e-02 5.000000e-03 5.000000e-03 6.640000e+01 4.120000e+00 4.120000e+00 +4.500000e-02 5.000000e-03 5.000000e-03 6.814000e+01 4.200000e+00 4.200000e+00 +5.500000e-02 5.000000e-03 5.000000e-03 6.142000e+01 3.840000e+00 3.840000e+00 +7.000000e-02 1.000000e-02 1.000000e-02 5.672000e+01 3.400000e+00 3.400000e+00 +9.000000e-02 1.000000e-02 1.000000e-02 4.279000e+01 2.600000e+00 2.600000e+00 +1.100000e-01 1.000000e-02 1.000000e-02 3.470000e+01 2.160000e+00 2.160000e+00 +1.300000e-01 1.000000e-02 1.000000e-02 2.811000e+01 1.770000e+00 1.770000e+00 +1.500000e-01 1.000000e-02 1.000000e-02 2.156000e+01 1.410000e+00 1.410000e+00 +1.700000e-01 1.000000e-02 1.000000e-02 1.910000e+01 1.240000e+00 1.240000e+00 +1.900000e-01 1.000000e-02 1.000000e-02 1.504000e+01 1.020000e+00 1.020000e+00 +2.250000e-01 2.500000e-02 2.500000e-02 1.158000e+01 7.200000e-01 7.200000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 7.410000e+00 5.000000e-01 5.000000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 5.250000e+00 3.600000e-01 3.600000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 3.320000e+00 2.500000e-01 2.500000e-01 +4.500000e-01 5.000000e-02 5.000000e-02 1.830000e+00 1.400000e-01 1.400000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 9.300000e-01 9.000000e-02 9.000000e-02 +6.500000e-01 5.000000e-02 5.000000e-02 4.000000e-01 5.000000e-02 5.000000e-02 +7.500000e-01 5.000000e-02 5.000000e-02 2.100000e-01 4.000000e-02 4.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d06-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d06-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 5.000000e-03 5.000000e-03 1.168000e+02 7.700000e+00 7.700000e+00 +3.500000e-02 5.000000e-03 5.000000e-03 1.105000e+02 6.600000e+00 6.600000e+00 +4.500000e-02 5.000000e-03 5.000000e-03 9.330000e+01 5.200000e+00 5.200000e+00 +5.500000e-02 5.000000e-03 5.000000e-03 8.580000e+01 4.500000e+00 4.500000e+00 +7.000000e-02 1.000000e-02 1.000000e-02 6.490000e+01 3.200000e+00 3.200000e+00 +9.000000e-02 1.000000e-02 1.000000e-02 4.950000e+01 2.400000e+00 2.400000e+00 +1.100000e-01 1.000000e-02 1.000000e-02 3.420000e+01 1.600000e+00 1.600000e+00 +1.300000e-01 1.000000e-02 1.000000e-02 2.700000e+01 1.400000e+00 1.400000e+00 +1.500000e-01 1.000000e-02 1.000000e-02 2.120000e+01 1.100000e+00 1.100000e+00 +1.700000e-01 1.000000e-02 1.000000e-02 1.672000e+01 9.600000e-01 9.600000e-01 +1.900000e-01 1.000000e-02 1.000000e-02 1.423000e+01 8.700000e-01 8.700000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.013000e+01 5.200000e-01 5.200000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 6.710000e+00 4.000000e-01 4.000000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 4.220000e+00 2.900000e-01 2.900000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 2.950000e+00 2.300000e-01 2.300000e-01 +4.500000e-01 5.000000e-02 5.000000e-02 1.550000e+00 1.100000e-01 1.100000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 7.800000e-01 8.000000e-02 8.000000e-02 +6.500000e-01 5.000000e-02 5.000000e-02 3.800000e-01 5.000000e-02 5.000000e-02 +7.500000e-01 5.000000e-02 5.000000e-02 2.100000e-01 4.000000e-02 4.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d06-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d06-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 5.000000e-03 5.000000e-03 1.626000e+02 2.150000e+01 2.150000e+01 +3.500000e-02 5.000000e-03 5.000000e-03 1.358000e+02 1.550000e+01 1.550000e+01 +4.500000e-02 5.000000e-03 5.000000e-03 1.068000e+02 9.500000e+00 9.500000e+00 +5.500000e-02 5.000000e-03 5.000000e-03 8.580000e+01 5.700000e+00 5.700000e+00 +7.000000e-02 1.000000e-02 1.000000e-02 6.270000e+01 3.500000e+00 3.500000e+00 +9.000000e-02 1.000000e-02 1.000000e-02 4.510000e+01 1.600000e+00 1.600000e+00 +1.100000e-01 1.000000e-02 1.000000e-02 3.400000e+01 9.000000e-01 9.000000e-01 +1.300000e-01 1.000000e-02 1.000000e-02 2.572000e+01 6.800000e-01 6.800000e-01 +1.500000e-01 1.000000e-02 1.000000e-02 1.950000e+01 5.300000e-01 5.300000e-01 +1.700000e-01 1.000000e-02 1.000000e-02 1.638000e+01 4.800000e-01 4.800000e-01 +1.900000e-01 1.000000e-02 1.000000e-02 1.334000e+01 3.900000e-01 3.900000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 9.230000e+00 2.500000e-01 2.500000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 5.690000e+00 1.700000e-01 1.700000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 3.660000e+00 1.100000e-01 1.100000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 2.560000e+00 1.000000e-01 1.000000e-01 +4.500000e-01 5.000000e-02 5.000000e-02 1.410000e+00 1.000000e-01 1.000000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 6.600000e-01 4.000000e-02 4.000000e-02 +6.500000e-01 5.000000e-02 5.000000e-02 3.600000e-01 3.000000e-02 3.000000e-02 +7.500000e-01 5.000000e-02 5.000000e-02 1.900000e-01 4.000000e-02 4.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d07-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d07-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t7 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 2.500000e-02 2.500000e-02 8.732000e+00 2.920000e-01 2.920000e-01 +7.500000e-02 2.500000e-02 2.500000e-02 9.431000e+00 3.040000e-01 3.040000e-01 +1.250000e-01 2.500000e-02 2.500000e-02 1.171000e+01 3.390000e-01 3.390000e-01 +1.750000e-01 2.500000e-02 2.500000e-02 1.105000e+01 3.290000e-01 3.290000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.082000e+01 3.260000e-01 3.260000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 8.866000e+00 2.960000e-01 2.960000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 8.621000e+00 2.920000e-01 2.920000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 7.690000e+00 2.760000e-01 2.760000e-01 +4.250000e-01 2.500000e-02 2.500000e-02 6.574000e+00 2.560000e-01 2.560000e-01 +4.750000e-01 2.500000e-02 2.500000e-02 6.161000e+00 2.480000e-01 2.480000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 5.250000e+00 1.620000e-01 1.620000e-01 +6.500000e-01 5.000000e-02 5.000000e-02 4.448000e+00 1.500000e-01 1.500000e-01 +7.500000e-01 5.000000e-02 5.000000e-02 3.875000e+00 1.400000e-01 1.400000e-01 +8.500000e-01 5.000000e-02 5.000000e-02 3.348000e+00 1.300000e-01 1.300000e-01 +9.500000e-01 5.000000e-02 5.000000e-02 2.850000e+00 1.200000e-01 1.200000e-01 +1.100000e+00 1.000000e-01 1.000000e-01 2.517000e+00 8.000000e-02 8.000000e-02 +1.300000e+00 1.000000e-01 1.000000e-01 1.950000e+00 7.100000e-02 7.100000e-02 +1.500000e+00 1.000000e-01 1.000000e-01 1.538000e+00 6.300000e-02 6.300000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 1.199000e+00 5.500000e-02 5.500000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 9.580000e-01 5.000000e-02 5.000000e-02 +2.500000e+00 5.000000e-01 5.000000e-01 4.830000e-01 1.500000e-02 1.500000e-02 +3.500000e+00 5.000000e-01 5.000000e-01 1.450000e-01 8.000000e-03 8.000000e-03 +4.500000e+00 5.000000e-01 5.000000e-01 4.600000e-02 5.000000e-03 5.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d07-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d07-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t7 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 2.500000e-02 2.500000e-02 7.881000e+00 3.280000e-01 3.280000e-01 +7.500000e-02 2.500000e-02 2.500000e-02 9.595000e+00 3.640000e-01 3.640000e-01 +1.250000e-01 2.500000e-02 2.500000e-02 1.106000e+01 3.920000e-01 3.920000e-01 +1.750000e-01 2.500000e-02 2.500000e-02 1.197000e+01 4.100000e-01 4.100000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.054500e+01 3.870000e-01 3.870000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 9.804000e+00 3.750000e-01 3.750000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 9.139000e+00 3.640000e-01 3.640000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 8.342000e+00 3.490000e-01 3.490000e-01 +4.250000e-01 2.500000e-02 2.500000e-02 7.526000e+00 3.330000e-01 3.330000e-01 +4.750000e-01 2.500000e-02 2.500000e-02 7.346000e+00 3.300000e-01 3.300000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 6.703000e+00 2.240000e-01 2.240000e-01 +6.500000e-01 5.000000e-02 5.000000e-02 5.393000e+00 2.020000e-01 2.020000e-01 +7.500000e-01 5.000000e-02 5.000000e-02 4.909000e+00 1.940000e-01 1.940000e-01 +8.500000e-01 5.000000e-02 5.000000e-02 4.630000e+00 1.890000e-01 1.890000e-01 +9.500000e-01 5.000000e-02 5.000000e-02 3.833000e+00 1.730000e-01 1.730000e-01 +1.100000e+00 1.000000e-01 1.000000e-01 3.269000e+00 1.130000e-01 1.130000e-01 +1.300000e+00 1.000000e-01 1.000000e-01 2.591000e+00 1.010000e-01 1.010000e-01 +1.500000e+00 1.000000e-01 1.000000e-01 2.111000e+00 9.100000e-02 9.100000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 1.661000e+00 8.100000e-02 8.100000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 1.358000e+00 7.300000e-02 7.300000e-02 +2.500000e+00 5.000000e-01 5.000000e-01 8.220000e-01 2.500000e-02 2.500000e-02 +3.500000e+00 5.000000e-01 5.000000e-01 3.560000e-01 2.500000e-02 2.500000e-02 +4.500000e+00 5.000000e-01 5.000000e-01 1.740000e-01 1.100000e-02 1.100000e-02 +5.500000e+00 5.000000e-01 5.000000e-01 8.000000e-02 8.000000e-03 8.000000e-03 +7.000000e+00 1.000000e+00 1.000000e+00 3.200000e-02 3.000000e-03 3.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d07-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d07-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t7 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 2.500000e-02 2.500000e-02 8.454000e+00 1.200000e-01 1.200000e-01 +7.500000e-02 2.500000e-02 2.500000e-02 9.394000e+00 1.270000e-01 1.270000e-01 +1.250000e-01 2.500000e-02 2.500000e-02 1.245000e+01 1.470000e-01 1.470000e-01 +1.750000e-01 2.500000e-02 2.500000e-02 1.245000e+01 1.470000e-01 1.470000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.163000e+01 1.430000e-01 1.430000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 1.052000e+01 1.370000e-01 1.370000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 9.640000e+00 1.310000e-01 1.310000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 8.849000e+00 1.260000e-01 1.260000e-01 +4.250000e-01 2.500000e-02 2.500000e-02 8.423000e+00 1.240000e-01 1.240000e-01 +4.750000e-01 2.500000e-02 2.500000e-02 7.639000e+00 1.180000e-01 1.180000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 7.037000e+00 8.000000e-02 8.000000e-02 +6.500000e-01 5.000000e-02 5.000000e-02 6.153000e+00 7.600000e-02 7.600000e-02 +7.500000e-01 5.000000e-02 5.000000e-02 5.454000e+00 7.200000e-02 7.200000e-02 +8.500000e-01 5.000000e-02 5.000000e-02 4.882000e+00 6.800000e-02 6.800000e-02 +9.500000e-01 5.000000e-02 5.000000e-02 4.392000e+00 6.500000e-02 6.500000e-02 +1.100000e+00 1.000000e-01 1.000000e-01 3.675000e+00 4.200000e-02 4.200000e-02 +1.300000e+00 1.000000e-01 1.000000e-01 3.068000e+00 3.900000e-02 3.900000e-02 +1.500000e+00 1.000000e-01 1.000000e-01 2.558000e+00 3.500000e-02 3.500000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 2.222000e+00 3.300000e-02 3.300000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 1.847000e+00 3.000000e-02 3.000000e-02 +2.500000e+00 5.000000e-01 5.000000e-01 1.181000e+00 1.100000e-02 1.100000e-02 +3.500000e+00 5.000000e-01 5.000000e-01 6.420000e-01 8.000000e-03 8.000000e-03 +4.500000e+00 5.000000e-01 5.000000e-01 3.370000e-01 6.000000e-03 6.000000e-03 +5.500000e+00 5.000000e-01 5.000000e-01 2.060000e-01 4.000000e-03 4.000000e-03 +7.000000e+00 1.000000e+00 1.000000e+00 1.070000e-01 2.000000e-03 2.000000e-03 +9.000000e+00 1.000000e+00 1.000000e+00 4.100000e-02 2.000000e-03 2.000000e-03 +1.100000e+01 1.000000e+00 1.000000e+00 1.900000e-02 1.000000e-03 1.000000e-03 +1.300000e+01 1.000000e+00 1.000000e+00 7.000000e-03 1.000000e-03 1.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d08-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d08-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t8 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 2.500000e-02 2.500000e-02 5.609000e+00 2.500000e-01 2.500000e-01 +7.500000e-02 2.500000e-02 2.500000e-02 1.296000e+01 3.800000e-01 3.800000e-01 +1.250000e-01 2.500000e-02 2.500000e-02 1.899000e+01 4.600000e-01 4.600000e-01 +1.750000e-01 2.500000e-02 2.500000e-02 2.075000e+01 4.810000e-01 4.810000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.989000e+01 4.710000e-01 4.710000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 1.879000e+01 4.580000e-01 4.580000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 1.615000e+01 4.240000e-01 4.240000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 1.351000e+01 3.880000e-01 3.880000e-01 +4.250000e-01 2.500000e-02 2.500000e-02 1.078000e+01 3.470000e-01 3.470000e-01 +4.750000e-01 2.500000e-02 2.500000e-02 8.586000e+00 3.090000e-01 3.090000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 5.926000e+00 1.820000e-01 1.820000e-01 +6.500000e-01 5.000000e-02 5.000000e-02 3.841000e+00 1.460000e-01 1.460000e-01 +7.500000e-01 5.000000e-02 5.000000e-02 2.052000e+00 1.070000e-01 1.070000e-01 +8.500000e-01 5.000000e-02 5.000000e-02 1.399000e+00 8.800000e-02 8.800000e-02 +9.500000e-01 5.000000e-02 5.000000e-02 6.750000e-01 6.100000e-02 6.100000e-02 +1.100000e+00 1.000000e-01 1.000000e-01 5.650000e-01 4.500000e-02 4.500000e-02 +1.300000e+00 1.000000e-01 1.000000e-01 1.760000e-01 2.600000e-02 2.600000e-02 +1.500000e+00 1.000000e-01 1.000000e-01 8.800000e-02 1.900000e-02 1.900000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 3.100000e-02 1.200000e-02 1.200000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 2.700000e-02 1.100000e-02 1.100000e-02 +2.250000e+00 2.500000e-01 2.500000e-01 5.000000e-03 3.000000e-03 3.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d08-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d08-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t8 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 2.500000e-02 2.500000e-02 6.432000e+00 3.280000e-01 3.280000e-01 +7.500000e-02 2.500000e-02 2.500000e-02 1.571000e+01 5.130000e-01 5.130000e-01 +1.250000e-01 2.500000e-02 2.500000e-02 2.035000e+01 5.840000e-01 5.840000e-01 +1.750000e-01 2.500000e-02 2.500000e-02 2.330000e+01 6.250000e-01 6.250000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 2.228000e+01 6.110000e-01 6.110000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 2.186000e+01 6.050000e-01 6.050000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 1.846000e+01 5.560000e-01 5.560000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 1.616000e+01 5.200000e-01 5.200000e-01 +4.250000e-01 2.500000e-02 2.500000e-02 1.316000e+01 4.700000e-01 4.700000e-01 +4.750000e-01 2.500000e-02 2.500000e-02 1.120000e+01 4.330000e-01 4.330000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 8.022000e+00 2.590000e-01 2.590000e-01 +6.500000e-01 5.000000e-02 5.000000e-02 5.619000e+00 2.170000e-01 2.170000e-01 +7.500000e-01 5.000000e-02 5.000000e-02 3.718000e+00 1.770000e-01 1.770000e-01 +8.500000e-01 5.000000e-02 5.000000e-02 2.387000e+00 1.410000e-01 1.410000e-01 +9.500000e-01 5.000000e-02 5.000000e-02 1.692000e+00 1.190000e-01 1.190000e-01 +1.100000e+00 1.000000e-01 1.000000e-01 9.610000e-01 6.500000e-02 6.500000e-02 +1.300000e+00 1.000000e-01 1.000000e-01 4.480000e-01 4.500000e-02 4.500000e-02 +1.500000e+00 1.000000e-01 1.000000e-01 2.420000e-01 3.300000e-02 3.300000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 1.770000e-01 2.900000e-02 2.900000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 1.050000e-01 2.200000e-02 2.200000e-02 +2.250000e+00 2.500000e-01 2.500000e-01 4.700000e-02 1.000000e-02 1.000000e-02 +2.750000e+00 2.500000e-01 2.500000e-01 1.500000e-02 7.000000e-03 7.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d08-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d08-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t8 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 2.500000e-02 2.500000e-02 8.030000e+00 1.120000e-01 1.120000e-01 +7.500000e-02 2.500000e-02 2.500000e-02 1.719200e+01 1.640000e-01 1.640000e-01 +1.250000e-01 2.500000e-02 2.500000e-02 2.327000e+01 1.910000e-01 1.910000e-01 +1.750000e-01 2.500000e-02 2.500000e-02 2.542000e+01 1.990000e-01 1.990000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 2.463000e+01 1.960000e-01 1.960000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 2.282000e+01 1.890000e-01 1.890000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 2.067000e+01 1.800000e-01 1.800000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 1.790000e+01 1.670000e-01 1.670000e-01 +4.250000e-01 2.500000e-02 2.500000e-02 1.543000e+01 1.550000e-01 1.550000e-01 +4.750000e-01 2.500000e-02 2.500000e-02 1.302000e+01 1.430000e-01 1.430000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 1.023000e+01 8.900000e-02 8.900000e-02 +6.500000e-01 5.000000e-02 5.000000e-02 7.326000e+00 7.500000e-02 7.500000e-02 +7.500000e-01 5.000000e-02 5.000000e-02 5.222000e+00 6.400000e-02 6.400000e-02 +8.500000e-01 5.000000e-02 5.000000e-02 3.712000e+00 5.400000e-02 5.400000e-02 +9.500000e-01 5.000000e-02 5.000000e-02 2.667000e+00 4.500000e-02 4.500000e-02 +1.100000e+00 1.000000e-01 1.000000e-01 1.712000e+00 2.600000e-02 2.600000e-02 +1.300000e+00 1.000000e-01 1.000000e-01 9.760000e-01 1.900000e-02 1.900000e-02 +1.500000e+00 1.000000e-01 1.000000e-01 5.720000e-01 1.500000e-02 1.500000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 3.680000e-01 1.200000e-02 1.200000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 2.320000e-01 9.000000e-03 9.000000e-03 +2.250000e+00 2.500000e-01 2.500000e-01 1.140000e-01 4.000000e-03 4.000000e-03 +2.750000e+00 2.500000e-01 2.500000e-01 4.300000e-02 3.000000e-03 3.000000e-03 +3.500000e+00 5.000000e-01 5.000000e-01 1.200000e-02 1.000000e-03 1.000000e-03 +5.000000e+00 1.000000e+00 1.000000e+00 1.400000e-03 0.000000e+00 0.000000e+00 +7.000000e+00 1.000000e+00 1.000000e+00 4.000000e-04 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d09-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d09-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t9 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-03 5.000000e-03 5.000000e-03 9.282000e+01 2.275000e+00 2.275000e+00 +1.500000e-02 5.000000e-03 5.000000e-03 7.587000e+01 2.057000e+00 2.057000e+00 +3.000000e-02 1.000000e-02 1.000000e-02 6.139000e+01 1.308000e+00 1.308000e+00 +5.000000e-02 1.000000e-02 1.000000e-02 4.526000e+01 1.123000e+00 1.123000e+00 +7.000000e-02 1.000000e-02 1.000000e-02 3.637000e+01 1.007000e+00 1.007000e+00 +9.000000e-02 1.000000e-02 1.000000e-02 2.904000e+01 9.000000e-01 9.000000e-01 +1.100000e-01 1.000000e-02 1.000000e-02 2.353000e+01 8.100000e-01 8.100000e-01 +1.300000e-01 1.000000e-02 1.000000e-02 1.960000e+01 7.390000e-01 7.390000e-01 +1.500000e-01 1.000000e-02 1.000000e-02 1.703000e+01 6.890000e-01 6.890000e-01 +1.700000e-01 1.000000e-02 1.000000e-02 1.363000e+01 6.170000e-01 6.170000e-01 +1.900000e-01 1.000000e-02 1.000000e-02 1.216000e+01 5.820000e-01 5.820000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 9.055000e+00 3.180000e-01 3.180000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 6.468000e+00 2.690000e-01 2.690000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 4.661000e+00 2.280000e-01 2.280000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 3.546000e+00 1.990000e-01 1.990000e-01 +5.000000e-01 1.000000e-01 1.000000e-01 2.024000e+00 7.500000e-02 7.500000e-02 +7.000000e-01 1.000000e-01 1.000000e-01 8.840000e-01 5.000000e-02 5.000000e-02 +1.000000e+00 2.000000e-01 2.000000e-01 3.140000e-01 2.100000e-02 2.100000e-02 +1.400000e+00 2.000000e-01 2.000000e-01 1.230000e-01 1.300000e-02 1.300000e-02 +1.800000e+00 2.000000e-01 2.000000e-01 3.800000e-02 7.000000e-03 7.000000e-03 +2.500000e+00 5.000000e-01 5.000000e-01 1.900000e-02 4.000000e-03 4.000000e-03 +3.500000e+00 5.000000e-01 5.000000e-01 7.700000e-03 2.700000e-03 2.700000e-03 +5.000000e+00 1.000000e+00 1.000000e+00 1.800000e-03 1.000000e-03 1.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d09-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d09-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t9 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-03 5.000000e-03 5.000000e-03 1.107020e+02 3.050000e+00 3.050000e+00 +1.500000e-02 5.000000e-03 5.000000e-03 8.232000e+01 2.620000e+00 2.620000e+00 +3.000000e-02 1.000000e-02 1.000000e-02 6.795000e+01 1.690000e+00 1.690000e+00 +5.000000e-02 1.000000e-02 1.000000e-02 4.995000e+01 1.449000e+00 1.449000e+00 +7.000000e-02 1.000000e-02 1.000000e-02 4.116000e+01 1.313000e+00 1.313000e+00 +9.000000e-02 1.000000e-02 1.000000e-02 3.572000e+01 1.223000e+00 1.223000e+00 +1.100000e-01 1.000000e-02 1.000000e-02 2.655000e+01 1.054000e+00 1.054000e+00 +1.300000e-01 1.000000e-02 1.000000e-02 2.253000e+01 9.710000e-01 9.710000e-01 +1.500000e-01 1.000000e-02 1.000000e-02 2.098000e+01 9.370000e-01 9.370000e-01 +1.700000e-01 1.000000e-02 1.000000e-02 1.688000e+01 8.410000e-01 8.410000e-01 +1.900000e-01 1.000000e-02 1.000000e-02 1.453000e+01 7.800000e-01 7.800000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.181000e+01 4.450000e-01 4.450000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 8.224000e+00 3.710000e-01 3.710000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 6.466000e+00 3.290000e-01 3.290000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 5.578000e+00 3.060000e-01 3.060000e-01 +5.000000e-01 1.000000e-01 1.000000e-01 3.204000e+00 1.160000e-01 1.160000e-01 +7.000000e-01 1.000000e-01 1.000000e-01 1.541000e+00 8.000000e-02 8.000000e-02 +1.000000e+00 2.000000e-01 2.000000e-01 7.140000e-01 3.900000e-02 3.900000e-02 +1.400000e+00 2.000000e-01 2.000000e-01 2.870000e-01 2.500000e-02 2.500000e-02 +1.800000e+00 2.000000e-01 2.000000e-01 1.300000e-01 1.600000e-02 1.600000e-02 +2.500000e+00 5.000000e-01 5.000000e-01 6.900000e-02 8.000000e-03 8.000000e-03 +3.500000e+00 5.000000e-01 5.000000e-01 3.000000e-02 5.000000e-03 5.000000e-03 +5.000000e+00 1.000000e+00 1.000000e+00 1.200000e-02 3.000000e-03 3.000000e-03 +7.000000e+00 1.000000e+00 1.000000e+00 3.000000e-03 2.000000e-03 2.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d09-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d09-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t9 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-03 5.000000e-03 5.000000e-03 1.256000e+02 9.910000e-01 9.910000e-01 +1.500000e-02 5.000000e-03 5.000000e-03 9.465000e+01 8.610000e-01 8.610000e-01 +3.000000e-02 1.000000e-02 1.000000e-02 7.378000e+01 5.380000e-01 5.380000e-01 +5.000000e-02 1.000000e-02 1.000000e-02 5.528000e+01 4.650000e-01 4.650000e-01 +7.000000e-02 1.000000e-02 1.000000e-02 4.416000e+01 4.160000e-01 4.160000e-01 +9.000000e-02 1.000000e-02 1.000000e-02 3.642000e+01 3.770000e-01 3.770000e-01 +1.100000e-01 1.000000e-02 1.000000e-02 3.082000e+01 3.470000e-01 3.470000e-01 +1.300000e-01 1.000000e-02 1.000000e-02 2.588000e+01 3.180000e-01 3.180000e-01 +1.500000e-01 1.000000e-02 1.000000e-02 2.251000e+01 2.970000e-01 2.970000e-01 +1.700000e-01 1.000000e-02 1.000000e-02 2.034000e+01 2.820000e-01 2.820000e-01 +1.900000e-01 1.000000e-02 1.000000e-02 1.643000e+01 2.530000e-01 2.530000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.381000e+01 1.470000e-01 1.470000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 1.086000e+01 1.300000e-01 1.300000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 8.262000e+00 1.140000e-01 1.140000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 6.826000e+00 1.030000e-01 1.030000e-01 +5.000000e-01 1.000000e-01 1.000000e-01 4.402000e+00 4.100000e-02 4.100000e-02 +7.000000e-01 1.000000e-01 1.000000e-01 2.320000e+00 3.000000e-02 3.000000e-02 +1.000000e+00 2.000000e-01 2.000000e-01 1.184000e+00 1.500000e-02 1.500000e-02 +1.400000e+00 2.000000e-01 2.000000e-01 5.760000e-01 1.100000e-02 1.100000e-02 +1.800000e+00 2.000000e-01 2.000000e-01 3.220000e-01 8.000000e-03 8.000000e-03 +2.500000e+00 5.000000e-01 5.000000e-01 1.570000e-01 4.000000e-03 4.000000e-03 +3.500000e+00 5.000000e-01 5.000000e-01 6.600000e-02 2.000000e-03 2.000000e-03 +5.000000e+00 1.000000e+00 1.000000e+00 2.600000e-02 1.000000e-03 1.000000e-03 +7.000000e+00 1.000000e+00 1.000000e+00 9.800000e-03 6.000000e-04 6.000000e-04 +9.000000e+00 1.000000e+00 1.000000e+00 4.900000e-03 4.000000e-04 4.000000e-04 +1.100000e+01 1.000000e+00 1.000000e+00 2.300000e-03 3.000000e-04 3.000000e-04 +1.300000e+01 1.000000e+00 1.000000e+00 1.300000e-03 3.000000e-04 3.000000e-04 +1.500000e+01 1.000000e+00 1.000000e+00 1.100000e-03 2.000000e-04 2.000000e-04 +1.700000e+01 1.000000e+00 1.000000e+00 6.500000e-04 1.800000e-04 1.800000e-04 +1.900000e+01 1.000000e+00 1.000000e+00 2.900000e-04 1.300000e-04 1.300000e-04 +2.500000e+01 5.000000e+00 5.000000e+00 2.000000e-04 9.000000e-05 9.000000e-05 +3.500000e+01 5.000000e+00 5.000000e+00 3.000000e-05 2.000000e-05 2.000000e-05 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d10-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d10-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t10 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 5.000000e-03 5.000000e-03 7.740000e+01 3.460000e+00 3.460000e+00 +3.500000e-02 5.000000e-03 5.000000e-03 7.050000e+01 4.120000e+00 4.120000e+00 +4.500000e-02 5.000000e-03 5.000000e-03 6.064000e+01 3.200000e+00 3.200000e+00 +5.500000e-02 5.000000e-03 5.000000e-03 5.100000e+01 3.140000e+00 3.140000e+00 +7.000000e-02 1.000000e-02 1.000000e-02 4.130000e+01 2.900000e+00 2.900000e+00 +9.000000e-02 1.000000e-02 1.000000e-02 3.140000e+01 2.000000e+00 2.000000e+00 +1.100000e-01 1.000000e-02 1.000000e-02 2.520000e+01 1.600000e+00 1.600000e+00 +1.300000e-01 1.000000e-02 1.000000e-02 2.170000e+01 1.530000e+00 1.530000e+00 +1.500000e-01 1.000000e-02 1.000000e-02 1.790000e+01 1.210000e+00 1.210000e+00 +1.700000e-01 1.000000e-02 1.000000e-02 1.550000e+01 1.120000e+00 1.120000e+00 +1.900000e-01 1.000000e-02 1.000000e-02 1.250000e+01 9.500000e-01 9.500000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 9.400000e+00 7.200000e-01 7.200000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 6.350000e+00 4.500000e-01 4.500000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 4.350000e+00 3.600000e-01 3.600000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 2.750000e+00 2.500000e-01 2.500000e-01 +4.500000e-01 5.000000e-02 5.000000e-02 1.580000e+00 9.000000e-02 9.000000e-02 +5.500000e-01 5.000000e-02 5.000000e-02 8.800000e-01 7.000000e-02 7.000000e-02 +7.000000e-01 1.000000e-01 1.000000e-01 2.600000e-01 4.000000e-02 4.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d10-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d10-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t10 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 5.000000e-03 5.000000e-03 1.145000e+02 7.940000e+00 7.940000e+00 +3.500000e-02 5.000000e-03 5.000000e-03 9.160000e+01 6.500000e+00 6.500000e+00 +4.500000e-02 5.000000e-03 5.000000e-03 7.950000e+01 4.500000e+00 4.500000e+00 +5.500000e-02 5.000000e-03 5.000000e-03 6.284000e+01 4.000000e+00 4.000000e+00 +7.000000e-02 1.000000e-02 1.000000e-02 4.950000e+01 1.340000e+00 1.340000e+00 +9.000000e-02 1.000000e-02 1.000000e-02 3.730000e+01 1.900000e+00 1.900000e+00 +1.100000e-01 1.000000e-02 1.000000e-02 2.910000e+01 1.300000e+00 1.300000e+00 +1.300000e-01 1.000000e-02 1.000000e-02 2.110000e+01 1.000000e+00 1.000000e+00 +1.500000e-01 1.000000e-02 1.000000e-02 1.860000e+01 9.000000e-01 9.000000e-01 +1.700000e-01 1.000000e-02 1.000000e-02 1.340000e+01 8.400000e-01 8.400000e-01 +1.900000e-01 1.000000e-02 1.000000e-02 1.220000e+01 8.000000e-01 8.000000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 8.720000e+00 5.100000e-01 5.100000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 5.800000e+00 3.900000e-01 3.900000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 3.760000e+00 2.800000e-01 2.800000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 2.800000e+00 2.300000e-01 2.300000e-01 +4.500000e-01 5.000000e-02 5.000000e-02 1.480000e+00 1.100000e-01 1.100000e-01 +5.500000e-01 5.000000e-02 5.000000e-02 7.000000e-01 7.000000e-02 7.000000e-02 +7.000000e-01 1.000000e-01 1.000000e-01 2.800000e-01 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d10-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d10-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t10 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.500000e-02 5.000000e-03 5.000000e-03 1.439000e+02 2.150000e+01 2.150000e+01 +3.500000e-02 5.000000e-03 5.000000e-03 1.123000e+02 1.450000e+01 1.450000e+01 +4.500000e-02 5.000000e-03 5.000000e-03 8.940000e+01 9.000000e+00 9.000000e+00 +5.500000e-02 5.000000e-03 5.000000e-03 7.290000e+01 5.100000e+00 5.100000e+00 +7.000000e-02 1.000000e-02 1.000000e-02 5.490000e+01 2.700000e+00 2.700000e+00 +9.000000e-02 1.000000e-02 1.000000e-02 3.980000e+01 1.400000e+00 1.400000e+00 +1.100000e-01 1.000000e-02 1.000000e-02 3.090000e+01 8.000000e-01 8.000000e-01 +1.300000e-01 1.000000e-02 1.000000e-02 2.342000e+01 6.000000e-01 6.000000e-01 +1.500000e-01 1.000000e-02 1.000000e-02 1.830000e+01 5.300000e-01 5.300000e-01 +1.700000e-01 1.000000e-02 1.000000e-02 1.470000e+01 4.000000e-01 4.000000e-01 +1.900000e-01 1.000000e-02 1.000000e-02 1.240000e+01 3.500000e-01 3.500000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 8.630000e+00 2.500000e-01 2.500000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 5.260000e+00 1.700000e-01 1.700000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 3.490000e+00 1.100000e-01 1.100000e-01 +3.750000e-01 2.500000e-02 2.500000e-02 2.370000e+00 1.000000e-01 1.000000e-01 +4.500000e-01 5.000000e-02 5.000000e-02 1.270000e+00 8.000000e-02 8.000000e-02 +5.500000e-01 5.000000e-02 5.000000e-02 6.300000e-01 2.000000e-02 2.000000e-02 +7.000000e-01 1.000000e-01 1.000000e-01 2.400000e-01 2.000000e-02 2.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d11-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d11-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t11 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-03 5.000000e-03 5.000000e-03 5.252000e+01 1.740000e+00 1.740000e+00 +1.500000e-02 5.000000e-03 5.000000e-03 1.157000e+02 2.540000e+00 2.540000e+00 +2.500000e-02 5.000000e-03 5.000000e-03 1.438000e+02 2.800000e+00 2.800000e+00 +3.500000e-02 5.000000e-03 5.000000e-03 1.328000e+02 2.670000e+00 2.670000e+00 +4.500000e-02 5.000000e-03 5.000000e-03 1.122000e+02 2.450000e+00 2.450000e+00 +5.500000e-02 5.000000e-03 5.000000e-03 8.641000e+01 2.160000e+00 2.160000e+00 +6.500000e-02 5.000000e-03 5.000000e-03 6.599000e+01 1.900000e+00 1.900000e+00 +7.500000e-02 5.000000e-03 5.000000e-03 4.615000e+01 1.610000e+00 1.610000e+00 +8.500000e-02 5.000000e-03 5.000000e-03 3.384000e+01 1.390000e+00 1.390000e+00 +9.500000e-02 5.000000e-03 5.000000e-03 2.678000e+01 1.260000e+00 1.260000e+00 +1.100000e-01 1.000000e-02 1.000000e-02 1.526000e+01 6.900000e-01 6.900000e-01 +1.300000e-01 1.000000e-02 1.000000e-02 7.490000e+00 5.000000e-01 5.000000e-01 +1.500000e-01 1.000000e-02 1.000000e-02 4.890000e+00 4.200000e-01 4.200000e-01 +1.700000e-01 1.000000e-02 1.000000e-02 2.650000e+00 3.200000e-01 3.200000e-01 +1.900000e-01 1.000000e-02 1.000000e-02 1.020000e+00 2.100000e-01 2.100000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 4.800000e-01 9.000000e-02 9.000000e-02 +2.750000e-01 2.500000e-02 2.500000e-02 2.000000e-01 6.000000e-02 6.000000e-02 +3.500000e-01 5.000000e-02 5.000000e-02 1.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d11-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d11-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t11 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-03 5.000000e-03 5.000000e-03 1.261000e+02 3.220000e+00 3.220000e+00 +1.500000e-02 5.000000e-03 5.000000e-03 2.417000e+02 4.470000e+00 4.470000e+00 +2.500000e-02 5.000000e-03 5.000000e-03 2.327000e+02 4.400000e+00 4.400000e+00 +3.500000e-02 5.000000e-03 5.000000e-03 1.694000e+02 3.760000e+00 3.760000e+00 +4.500000e-02 5.000000e-03 5.000000e-03 1.133000e+02 3.090000e+00 3.090000e+00 +5.500000e-02 5.000000e-03 5.000000e-03 7.485000e+01 2.510000e+00 2.510000e+00 +6.500000e-02 5.000000e-03 5.000000e-03 4.691000e+01 2.000000e+00 2.000000e+00 +7.500000e-02 5.000000e-03 5.000000e-03 2.978000e+01 1.590000e+00 1.590000e+00 +8.500000e-02 5.000000e-03 5.000000e-03 2.081000e+01 1.340000e+00 1.340000e+00 +9.500000e-02 5.000000e-03 5.000000e-03 1.234000e+01 1.030000e+00 1.030000e+00 +1.100000e-01 1.000000e-02 1.000000e-02 6.670000e+00 5.400000e-01 5.400000e-01 +1.300000e-01 1.000000e-02 1.000000e-02 3.560000e+00 4.000000e-01 4.000000e-01 +1.500000e-01 1.000000e-02 1.000000e-02 1.910000e+00 2.900000e-01 2.900000e-01 +1.700000e-01 1.000000e-02 1.000000e-02 1.310000e+00 2.500000e-01 2.500000e-01 +1.900000e-01 1.000000e-02 1.000000e-02 1.060000e+00 2.100000e-01 2.100000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.800000e-01 6.000000e-02 6.000000e-02 +2.750000e-01 2.500000e-02 2.500000e-02 8.000000e-02 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d11-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d11-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t11 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e-03 5.000000e-03 5.000000e-03 3.010000e+02 1.550000e+00 1.550000e+00 +1.500000e-02 5.000000e-03 5.000000e-03 4.006000e+02 1.780000e+00 1.780000e+00 +2.500000e-02 5.000000e-03 5.000000e-03 2.610000e+02 1.430000e+00 1.430000e+00 +3.500000e-02 5.000000e-03 5.000000e-03 1.483000e+02 1.070000e+00 1.070000e+00 +4.500000e-02 5.000000e-03 5.000000e-03 8.240000e+01 8.000000e-01 8.000000e-01 +5.500000e-02 5.000000e-03 5.000000e-03 4.661000e+01 6.000000e-01 6.000000e-01 +6.500000e-02 5.000000e-03 5.000000e-03 2.782000e+01 4.600000e-01 4.600000e-01 +7.500000e-02 5.000000e-03 5.000000e-03 1.713000e+01 3.700000e-01 3.700000e-01 +8.500000e-02 5.000000e-03 5.000000e-03 1.072000e+01 2.900000e-01 2.900000e-01 +9.500000e-02 5.000000e-03 5.000000e-03 7.350000e+00 2.400000e-01 2.400000e-01 +1.100000e-01 1.000000e-02 1.000000e-02 4.250000e+00 1.300000e-01 1.300000e-01 +1.300000e-01 1.000000e-02 1.000000e-02 1.980000e+00 9.000000e-02 9.000000e-02 +1.500000e-01 1.000000e-02 1.000000e-02 1.050000e+00 7.000000e-02 7.000000e-02 +1.700000e-01 1.000000e-02 1.000000e-02 5.400000e-01 5.000000e-02 5.000000e-02 +1.900000e-01 1.000000e-02 1.000000e-02 2.700000e-01 3.000000e-02 3.000000e-02 +2.250000e-01 2.500000e-02 2.500000e-02 1.200000e-01 2.000000e-02 2.000000e-02 +2.750000e-01 2.500000e-02 2.500000e-02 3.000000e-02 1.000000e-02 1.000000e-02 +3.500000e-01 5.000000e-02 5.000000e-02 8.000000e-03 2.000000e-03 2.000000e-03 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d12-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d12-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t12 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.250000e-02 1.250000e-02 1.250000e-02 1.140000e+00 1.500000e-01 1.500000e-01 +3.750000e-02 1.250000e-02 1.250000e-02 2.720000e+00 2.400000e-01 2.400000e-01 +6.250000e-02 1.250000e-02 1.250000e-02 3.870000e+00 2.900000e-01 2.900000e-01 +8.750000e-02 1.250000e-02 1.250000e-02 4.210000e+00 3.000000e-01 3.000000e-01 +1.250000e-01 2.500000e-02 2.500000e-02 3.680000e+00 2.000000e-01 2.000000e-01 +1.750000e-01 2.500000e-02 2.500000e-02 2.630000e+00 1.600000e-01 1.600000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.670000e+00 1.300000e-01 1.300000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 1.440000e+00 1.100000e-01 1.100000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 1.030000e+00 9.000000e-02 9.000000e-02 +3.750000e-01 2.500000e-02 2.500000e-02 9.900000e-01 9.000000e-02 9.000000e-02 +4.250000e-01 2.500000e-02 2.500000e-02 5.500000e-01 7.000000e-02 7.000000e-02 +4.750000e-01 2.500000e-02 2.500000e-02 5.100000e-01 6.000000e-02 6.000000e-02 +5.250000e-01 2.500000e-02 2.500000e-02 3.700000e-01 5.000000e-02 5.000000e-02 +5.750000e-01 2.500000e-02 2.500000e-02 3.900000e-01 6.000000e-02 6.000000e-02 +6.250000e-01 2.500000e-02 2.500000e-02 3.300000e-01 5.000000e-02 5.000000e-02 +6.750000e-01 2.500000e-02 2.500000e-02 2.600000e-01 5.000000e-02 5.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d12-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d12-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t12 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.250000e-02 1.250000e-02 1.250000e-02 2.220000e+00 2.300000e-01 2.300000e-01 +3.750000e-02 1.250000e-02 1.250000e-02 6.230000e+00 4.600000e-01 4.600000e-01 +6.250000e-02 1.250000e-02 1.250000e-02 6.550000e+00 4.800000e-01 4.800000e-01 +8.750000e-02 1.250000e-02 1.250000e-02 5.060000e+00 4.100000e-01 4.100000e-01 +1.250000e-01 2.500000e-02 2.500000e-02 3.010000e+00 2.100000e-01 2.100000e-01 +1.750000e-01 2.500000e-02 2.500000e-02 2.260000e+00 1.700000e-01 1.700000e-01 +2.250000e-01 2.500000e-02 2.500000e-02 1.320000e+00 1.300000e-01 1.300000e-01 +2.750000e-01 2.500000e-02 2.500000e-02 9.200000e-01 1.000000e-01 1.000000e-01 +3.250000e-01 2.500000e-02 2.500000e-02 7.200000e-01 9.000000e-02 9.000000e-02 +3.750000e-01 2.500000e-02 2.500000e-02 5.800000e-01 8.000000e-02 8.000000e-02 +4.250000e-01 2.500000e-02 2.500000e-02 3.000000e-01 5.000000e-02 5.000000e-02 +4.750000e-01 2.500000e-02 2.500000e-02 3.400000e-01 6.000000e-02 6.000000e-02 +5.250000e-01 2.500000e-02 2.500000e-02 1.700000e-01 4.000000e-02 4.000000e-02 +5.750000e-01 2.500000e-02 2.500000e-02 1.000000e-01 3.000000e-02 3.000000e-02 +6.250000e-01 2.500000e-02 2.500000e-02 1.300000e-01 3.000000e-02 3.000000e-02 +6.750000e-01 2.500000e-02 2.500000e-02 1.100000e-01 3.000000e-02 3.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d12-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d12-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t12 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.250000e-02 1.250000e-02 1.250000e-02 6.290000e+00 1.600000e-01 1.600000e-01 +3.750000e-02 1.250000e-02 1.250000e-02 8.870000e+00 2.000000e-01 2.000000e-01 +6.250000e-02 1.250000e-02 1.250000e-02 5.770000e+00 1.500000e-01 1.500000e-01 +8.750000e-02 1.250000e-02 1.250000e-02 4.120000e+00 1.200000e-01 1.200000e-01 +1.250000e-01 2.500000e-02 2.500000e-02 2.700000e+00 7.000000e-02 7.000000e-02 +1.750000e-01 2.500000e-02 2.500000e-02 1.580000e+00 5.000000e-02 5.000000e-02 +2.250000e-01 2.500000e-02 2.500000e-02 1.140000e+00 4.000000e-02 4.000000e-02 +2.750000e-01 2.500000e-02 2.500000e-02 6.800000e-01 3.000000e-02 3.000000e-02 +3.250000e-01 2.500000e-02 2.500000e-02 4.500000e-01 2.000000e-02 2.000000e-02 +3.750000e-01 2.500000e-02 2.500000e-02 2.900000e-01 2.000000e-02 2.000000e-02 +4.250000e-01 2.500000e-02 2.500000e-02 1.900000e-01 1.000000e-02 1.000000e-02 +4.750000e-01 2.500000e-02 2.500000e-02 1.300000e-01 1.000000e-02 1.000000e-02 +5.250000e-01 2.500000e-02 2.500000e-02 1.100000e-01 1.000000e-02 1.000000e-02 +5.750000e-01 2.500000e-02 2.500000e-02 1.000000e-01 1.000000e-02 1.000000e-02 +6.250000e-01 2.500000e-02 2.500000e-02 7.000000e-02 1.000000e-02 1.000000e-02 +6.750000e-01 2.500000e-02 2.500000e-02 4.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d13-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d13-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t13 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.200000e-01 2.000000e-02 2.000000e-02 3.400000e-01 7.000000e-02 7.000000e-02 +6.600000e-01 2.000000e-02 2.000000e-02 4.400000e-01 7.000000e-02 7.000000e-02 +7.000000e-01 2.000000e-02 2.000000e-02 1.170000e+00 1.100000e-01 1.100000e-01 +7.400000e-01 2.000000e-02 2.000000e-02 1.560000e+00 1.200000e-01 1.200000e-01 +7.800000e-01 2.000000e-02 2.000000e-02 2.170000e+00 1.600000e-01 1.600000e-01 +8.200000e-01 2.000000e-02 2.000000e-02 3.320000e+00 2.000000e-01 2.000000e-01 +8.600000e-01 2.000000e-02 2.000000e-02 4.080000e+00 2.200000e-01 2.200000e-01 +8.900000e-01 1.000000e-02 1.000000e-02 5.360000e+00 3.600000e-01 3.600000e-01 +9.100000e-01 1.000000e-02 1.000000e-02 5.670000e+00 3.700000e-01 3.700000e-01 +9.300000e-01 1.000000e-02 1.000000e-02 5.630000e+00 3.500000e-01 3.500000e-01 +9.500000e-01 1.000000e-02 1.000000e-02 4.040000e+00 2.900000e-01 2.900000e-01 +9.700000e-01 1.000000e-02 1.000000e-02 2.550000e+00 2.300000e-01 2.300000e-01 +9.900000e-01 1.000000e-02 1.000000e-02 5.900000e-01 1.100000e-01 1.100000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d13-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d13-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t13 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.200000e-01 2.000000e-02 2.000000e-02 5.000000e-02 3.000000e-02 3.000000e-02 +6.600000e-01 2.000000e-02 2.000000e-02 2.400000e-01 6.000000e-02 6.000000e-02 +7.000000e-01 2.000000e-02 2.000000e-02 5.000000e-01 8.000000e-02 8.000000e-02 +7.400000e-01 2.000000e-02 2.000000e-02 9.000000e-01 1.100000e-01 1.100000e-01 +7.800000e-01 2.000000e-02 2.000000e-02 1.380000e+00 1.400000e-01 1.400000e-01 +8.200000e-01 2.000000e-02 2.000000e-02 2.530000e+00 2.000000e-01 2.000000e-01 +8.600000e-01 2.000000e-02 2.000000e-02 3.840000e+00 2.500000e-01 2.500000e-01 +8.900000e-01 1.000000e-02 1.000000e-02 5.460000e+00 4.300000e-01 4.300000e-01 +9.100000e-01 1.000000e-02 1.000000e-02 6.250000e+00 4.600000e-01 4.600000e-01 +9.300000e-01 1.000000e-02 1.000000e-02 7.740000e+00 5.400000e-01 5.400000e-01 +9.500000e-01 1.000000e-02 1.000000e-02 6.800000e+00 4.600000e-01 4.600000e-01 +9.700000e-01 1.000000e-02 1.000000e-02 3.820000e+00 3.300000e-01 3.300000e-01 +9.900000e-01 1.000000e-02 1.000000e-02 9.300000e-01 1.500000e-01 1.500000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d13-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d13-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t13 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.200000e-01 2.000000e-02 2.000000e-02 2.000000e-02 1.000000e-02 1.000000e-02 +6.600000e-01 2.000000e-02 2.000000e-02 1.100000e-01 1.000000e-02 1.000000e-02 +7.000000e-01 2.000000e-02 2.000000e-02 2.600000e-01 2.000000e-02 2.000000e-02 +7.400000e-01 2.000000e-02 2.000000e-02 4.800000e-01 2.000000e-02 2.000000e-02 +7.800000e-01 2.000000e-02 2.000000e-02 9.200000e-01 4.000000e-02 4.000000e-02 +8.200000e-01 2.000000e-02 2.000000e-02 1.970000e+00 6.000000e-02 6.000000e-02 +8.600000e-01 2.000000e-02 2.000000e-02 3.020000e+00 8.000000e-02 8.000000e-02 +8.900000e-01 1.000000e-02 1.000000e-02 4.400000e+00 1.300000e-01 1.300000e-01 +9.100000e-01 1.000000e-02 1.000000e-02 5.760000e+00 1.500000e-01 1.500000e-01 +9.300000e-01 1.000000e-02 1.000000e-02 8.110000e+00 1.900000e-01 1.900000e-01 +9.500000e-01 1.000000e-02 1.000000e-02 9.700000e+00 2.100000e-01 2.100000e-01 +9.700000e-01 1.000000e-02 1.000000e-02 6.640000e+00 1.600000e-01 1.600000e-01 +9.900000e-01 1.000000e-02 1.000000e-02 1.860000e+00 8.000000e-02 8.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d14-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d14-x01-y01 +Title: doi:10.17182/hepdata.16272.v1/t14 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000000e-01 1.000000e-01 1.000000e-01 3.740000e+00 1.300000e-01 1.300000e-01 +3.000000e-01 1.000000e-01 1.000000e-01 4.050000e+00 1.100000e-01 1.100000e-01 +5.000000e-01 1.000000e-01 1.000000e-01 3.980000e+00 1.000000e-01 1.000000e-01 +7.000000e-01 1.000000e-01 1.000000e-01 4.220000e+00 1.000000e-01 1.000000e-01 +9.000000e-01 1.000000e-01 1.000000e-01 3.970000e+00 9.000000e-02 9.000000e-02 +1.100000e+00 1.000000e-01 1.000000e-01 3.890000e+00 9.000000e-02 9.000000e-02 +1.300000e+00 1.000000e-01 1.000000e-01 3.710000e+00 9.000000e-02 9.000000e-02 +1.500000e+00 1.000000e-01 1.000000e-01 3.300000e+00 8.000000e-02 8.000000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 3.100000e+00 8.000000e-02 8.000000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 2.600000e+00 7.000000e-02 7.000000e-02 +2.100000e+00 1.000000e-01 1.000000e-01 2.110000e+00 7.000000e-02 7.000000e-02 +2.300000e+00 1.000000e-01 1.000000e-01 1.680000e+00 6.000000e-02 6.000000e-02 +2.500000e+00 1.000000e-01 1.000000e-01 1.310000e+00 6.000000e-02 6.000000e-02 +2.700000e+00 1.000000e-01 1.000000e-01 9.900000e-01 5.000000e-02 5.000000e-02 +2.900000e+00 1.000000e-01 1.000000e-01 6.200000e-01 4.000000e-02 4.000000e-02 +3.100000e+00 1.000000e-01 1.000000e-01 4.300000e-01 3.000000e-02 3.000000e-02 +3.300000e+00 1.000000e-01 1.000000e-01 1.900000e-01 2.000000e-02 2.000000e-02 +3.500000e+00 1.000000e-01 1.000000e-01 1.200000e-01 2.000000e-02 2.000000e-02 +3.700000e+00 1.000000e-01 1.000000e-01 5.000000e-02 1.000000e-02 1.000000e-02 +3.900000e+00 1.000000e-01 1.000000e-01 3.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d14-x01-y02 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d14-x01-y02 +Title: doi:10.17182/hepdata.16272.v1/t14 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000000e-01 1.000000e-01 1.000000e-01 3.770000e+00 1.500000e-01 1.500000e-01 +3.000000e-01 1.000000e-01 1.000000e-01 4.000000e+00 1.300000e-01 1.300000e-01 +5.000000e-01 1.000000e-01 1.000000e-01 4.310000e+00 1.500000e-01 1.500000e-01 +7.000000e-01 1.000000e-01 1.000000e-01 4.570000e+00 1.200000e-01 1.200000e-01 +9.000000e-01 1.000000e-01 1.000000e-01 4.500000e+00 1.300000e-01 1.300000e-01 +1.100000e+00 1.000000e-01 1.000000e-01 4.540000e+00 1.300000e-01 1.300000e-01 +1.300000e+00 1.000000e-01 1.000000e-01 4.540000e+00 1.300000e-01 1.300000e-01 +1.500000e+00 1.000000e-01 1.000000e-01 4.310000e+00 1.300000e-01 1.300000e-01 +1.700000e+00 1.000000e-01 1.000000e-01 4.020000e+00 1.200000e-01 1.200000e-01 +1.900000e+00 1.000000e-01 1.000000e-01 3.610000e+00 1.300000e-01 1.300000e-01 +2.100000e+00 1.000000e-01 1.000000e-01 3.030000e+00 1.100000e-01 1.100000e-01 +2.300000e+00 1.000000e-01 1.000000e-01 2.670000e+00 1.000000e-01 1.000000e-01 +2.500000e+00 1.000000e-01 1.000000e-01 2.260000e+00 9.000000e-02 9.000000e-02 +2.700000e+00 1.000000e-01 1.000000e-01 1.650000e+00 8.000000e-02 8.000000e-02 +2.900000e+00 1.000000e-01 1.000000e-01 1.090000e+00 7.000000e-02 7.000000e-02 +3.100000e+00 1.000000e-01 1.000000e-01 6.700000e-01 5.000000e-02 5.000000e-02 +3.300000e+00 1.000000e-01 1.000000e-01 5.500000e-01 5.000000e-02 5.000000e-02 +3.500000e+00 1.000000e-01 1.000000e-01 3.400000e-01 4.000000e-02 4.000000e-02 +3.700000e+00 1.000000e-01 1.000000e-01 2.000000e-01 3.000000e-02 3.000000e-02 +3.900000e+00 1.000000e-01 1.000000e-01 8.000000e-02 2.000000e-02 2.000000e-02 +4.100000e+00 1.000000e-01 1.000000e-01 5.000000e-02 2.000000e-02 2.000000e-02 +4.300000e+00 1.000000e-01 1.000000e-01 4.000000e-02 2.000000e-02 2.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I195333/d14-x01-y03 +IsRef: 1 +Path: /REF/TASSO_1984_I195333/d14-x01-y03 +Title: doi:10.17182/hepdata.16272.v1/t14 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000000e-01 1.000000e-01 1.000000e-01 4.100000e+00 5.000000e-02 5.000000e-02 +3.000000e-01 1.000000e-01 1.000000e-01 4.500000e+00 5.000000e-02 5.000000e-02 +5.000000e-01 1.000000e-01 1.000000e-01 4.690000e+00 5.000000e-02 5.000000e-02 +7.000000e-01 1.000000e-01 1.000000e-01 4.880000e+00 5.000000e-02 5.000000e-02 +9.000000e-01 1.000000e-01 1.000000e-01 4.990000e+00 5.000000e-02 5.000000e-02 +1.100000e+00 1.000000e-01 1.000000e-01 4.990000e+00 5.000000e-02 5.000000e-02 +1.300000e+00 1.000000e-01 1.000000e-01 4.940000e+00 5.000000e-02 5.000000e-02 +1.500000e+00 1.000000e-01 1.000000e-01 4.800000e+00 5.000000e-02 5.000000e-02 +1.700000e+00 1.000000e-01 1.000000e-01 4.680000e+00 5.000000e-02 5.000000e-02 +1.900000e+00 1.000000e-01 1.000000e-01 4.430000e+00 4.000000e-02 4.000000e-02 +2.100000e+00 1.000000e-01 1.000000e-01 3.940000e+00 4.000000e-02 4.000000e-02 +2.300000e+00 1.000000e-01 1.000000e-01 3.530000e+00 4.000000e-02 4.000000e-02 +2.500000e+00 1.000000e-01 1.000000e-01 2.930000e+00 4.000000e-02 4.000000e-02 +2.700000e+00 1.000000e-01 1.000000e-01 2.490000e+00 4.000000e-02 4.000000e-02 +2.900000e+00 1.000000e-01 1.000000e-01 1.850000e+00 3.000000e-02 3.000000e-02 +3.100000e+00 1.000000e-01 1.000000e-01 1.420000e+00 3.000000e-02 3.000000e-02 +3.300000e+00 1.000000e-01 1.000000e-01 1.050000e+00 3.000000e-02 3.000000e-02 +3.500000e+00 1.000000e-01 1.000000e-01 7.100000e-01 2.000000e-02 2.000000e-02 +3.700000e+00 1.000000e-01 1.000000e-01 5.000000e-01 2.000000e-02 2.000000e-02 +3.900000e+00 1.000000e-01 1.000000e-01 3.000000e-01 1.000000e-02 1.000000e-02 +4.100000e+00 1.000000e-01 1.000000e-01 1.800000e-01 1.000000e-02 1.000000e-02 +4.300000e+00 1.000000e-01 1.000000e-01 9.000000e-02 1.000000e-02 1.000000e-02 +4.500000e+00 1.000000e-01 1.000000e-01 6.000000e-02 1.000000e-02 1.000000e-02 +4.700000e+00 1.000000e-01 1.000000e-01 3.000000e-02 1.000000e-02 1.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginPetra/TASSO_1984_I199468.cc b/analyses/pluginPetra/TASSO_1984_I199468.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1984_I199468.cc @@ -0,0 +1,101 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class TASSO_1984_I199468 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(TASSO_1984_I199468); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + + } + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + ostringstream title; + title << "d0" << ix; + Scatter2DPtr hadrons = bookScatter2D(title.str()+"_sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D(title.str()+"_sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + //@} + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(TASSO_1984_I199468); + + +} diff --git a/analyses/pluginPetra/TASSO_1984_I199468.info b/analyses/pluginPetra/TASSO_1984_I199468.info new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1984_I199468.info @@ -0,0 +1,33 @@ +Name: TASSO_1984_I199468 +Year: 1984 +Summary: Measurement of $R$ for energies between 39.8 and 45.2 GeV +Experiment: TASSO +Collider: PETRA +InspireID: 199468 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B138 (1984) 441-448, 1984 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions for energies between 39.8 and 45.2 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Althoff:1984us +BibTeX: '@article{Althoff:1984us, + author = "Althoff, M. and others", + title = "{Measurement of r and Search for the Top Quark in e+ e- + Annihilation Between 39.8-GeV and 45.2-GeV}", + collaboration = "TASSO", + journal = "Phys. Lett.", + volume = "138B", + year = "1984", + pages = "441-448", + doi = "10.1016/0370-2693(84)91936-1", + reportNumber = "DESY-84-001", + SLACcitation = "%%CITATION = PHLTA,138B,441;%%" +}' diff --git a/analyses/pluginPetra/TASSO_1984_I199468.plot b/analyses/pluginPetra/TASSO_1984_I199468.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1984_I199468.plot @@ -0,0 +1,42 @@ +BEGIN PLOT /TASSO_1984_I199468/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I199468/d01_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I199468/d01_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I199468/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I199468/d02_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TASSO_1984_I199468/d02_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginPetra/TASSO_1984_I199468.yoda b/analyses/pluginPetra/TASSO_1984_I199468.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginPetra/TASSO_1984_I199468.yoda @@ -0,0 +1,209 @@ +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I199468/d01-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I199468/d01-x01-y01 +Title: doi:10.17182/hepdata.6655.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.979000e+01 0.000000e+00 0.000000e+00 4.550000e+00 1.645177e+00 1.645177e+00 +3.982000e+01 0.000000e+00 0.000000e+00 5.930000e+00 1.410259e+00 1.410259e+00 +3.985000e+01 0.000000e+00 0.000000e+00 5.190000e+00 1.265809e+00 1.265809e+00 +3.988000e+01 0.000000e+00 0.000000e+00 3.910000e+00 1.343729e+00 1.343729e+00 +3.991000e+01 0.000000e+00 0.000000e+00 3.150000e+00 1.081075e+00 1.081075e+00 +3.994000e+01 0.000000e+00 0.000000e+00 3.410000e+00 1.063212e+00 1.063212e+00 +3.997000e+01 0.000000e+00 0.000000e+00 6.450000e+00 1.660358e+00 1.660358e+00 +4.000000e+01 0.000000e+00 0.000000e+00 3.510000e+00 9.064660e-01 9.064660e-01 +4.003000e+01 0.000000e+00 0.000000e+00 1.600000e+00 8.436507e-01 8.436507e-01 +4.006000e+01 0.000000e+00 0.000000e+00 4.180000e+00 1.296284e+00 1.296284e+00 +4.009000e+01 0.000000e+00 0.000000e+00 2.350000e+00 9.966742e-01 9.966742e-01 +4.012000e+01 0.000000e+00 0.000000e+00 6.170000e+00 1.256902e+00 1.256902e+00 +4.015000e+01 0.000000e+00 0.000000e+00 5.760000e+00 1.487030e+00 1.487030e+00 +4.018000e+01 0.000000e+00 0.000000e+00 3.640000e+00 1.252762e+00 1.252762e+00 +4.021000e+01 0.000000e+00 0.000000e+00 2.260000e+00 9.564326e-01 9.564326e-01 +4.024000e+01 0.000000e+00 0.000000e+00 4.330000e+00 1.812461e+00 1.812461e+00 +4.027000e+01 0.000000e+00 0.000000e+00 2.460000e+00 9.675381e-01 9.675381e-01 +4.030000e+01 0.000000e+00 0.000000e+00 3.060000e+00 1.050753e+00 1.050753e+00 +4.033000e+01 0.000000e+00 0.000000e+00 4.740000e+00 1.222270e+00 1.222270e+00 +4.036000e+01 0.000000e+00 0.000000e+00 2.600000e+00 1.097420e+00 1.097420e+00 +4.039000e+01 0.000000e+00 0.000000e+00 5.310000e+00 1.640762e+00 1.640762e+00 +4.042000e+01 0.000000e+00 0.000000e+00 4.100000e+00 1.335201e+00 1.335201e+00 +4.045000e+01 0.000000e+00 0.000000e+00 5.920000e+00 1.576910e+00 1.576910e+00 +4.048000e+01 0.000000e+00 0.000000e+00 3.570000e+00 1.163228e+00 1.163228e+00 +4.051000e+01 0.000000e+00 0.000000e+00 3.270000e+00 1.072042e+00 1.072042e+00 +4.054000e+01 0.000000e+00 0.000000e+00 3.120000e+00 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+4.474000e+01 0.000000e+00 0.000000e+00 4.920000e+00 1.519250e+00 1.519250e+00 +4.477000e+01 0.000000e+00 0.000000e+00 4.950000e+00 1.529356e+00 1.529356e+00 +4.480000e+01 0.000000e+00 0.000000e+00 3.990000e+00 1.235566e+00 1.235566e+00 +4.483000e+01 0.000000e+00 0.000000e+00 4.710000e+00 1.399165e+00 1.399165e+00 +4.486000e+01 0.000000e+00 0.000000e+00 4.500000e+00 1.535910e+00 1.535910e+00 +4.489000e+01 0.000000e+00 0.000000e+00 5.540000e+00 1.475192e+00 1.475192e+00 +4.492000e+01 0.000000e+00 0.000000e+00 3.450000e+00 1.182150e+00 1.182150e+00 +4.495000e+01 0.000000e+00 0.000000e+00 6.180000e+00 1.638231e+00 1.638231e+00 +4.498000e+01 0.000000e+00 0.000000e+00 4.940000e+00 1.608320e+00 1.608320e+00 +4.501000e+01 0.000000e+00 0.000000e+00 4.800000e+00 1.557857e+00 1.557857e+00 +4.504000e+01 0.000000e+00 0.000000e+00 2.690000e+00 1.048320e+00 1.048320e+00 +4.507000e+01 0.000000e+00 0.000000e+00 4.970000e+00 1.421023e+00 1.421023e+00 +4.510000e+01 0.000000e+00 0.000000e+00 4.790000e+00 1.419538e+00 1.419538e+00 +4.513000e+01 0.000000e+00 0.000000e+00 5.840000e+00 1.605705e+00 1.605705e+00 +4.516000e+01 0.000000e+00 0.000000e+00 4.970000e+00 1.539385e+00 1.539385e+00 +4.519000e+01 0.000000e+00 0.000000e+00 2.600000e+00 1.097420e+00 1.097420e+00 +4.522000e+01 0.000000e+00 0.000000e+00 5.690000e+00 2.058965e+00 2.058965e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I199468/d02-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I199468/d02-x01-y01 +Title: doi:10.17182/hepdata.6655.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.145000e+01 1.650000e+00 1.650000e+00 4.080000e+00 3.071938e-01 3.071938e-01 +4.420000e+01 1.000000e+00 1.000000e+00 4.220000e+00 3.353475e-01 3.353475e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TASSO_1984_I199468/d03-x01-y01 +IsRef: 1 +Path: /REF/TASSO_1984_I199468/d03-x01-y01 +Title: doi:10.17182/hepdata.6655.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +4.250000e+01 2.700000e+00 2.700000e+00 3.000000e-01 7.000000e-02 2.300000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.cc b/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.cc @@ -0,0 +1,141 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CRYSTAL_BALL_1986_I238081 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CRYSTAL_BALL_1986_I238081); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + _c_D_star = bookCounter("/TMP/sigma_D_star"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + + const FinalState& ufs = apply(event, "UFS"); + bool found = false; + foreach(const Particle & p, ufs.particles()) { + if(abs(p.pdgId())!=413 && abs(p.pdgId())!=423) continue; + bool fs = true; + foreach(const Particle & child, p.children()) { + if(child.pdgId()==p.pdgId()) { + fs = false; + break; + } + } + if(fs) { + found = true; + break; + } + } + if(found) + _c_D_star->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + // R + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + // D* + fact = crossSection()/ sumOfWeights() /nanobarn; + double sigma = _c_D_star->val()*fact; + double error = _c_D_star->err()*fact; + Scatter2D temphisto2(refData(2, 1, 1)); + Scatter2DPtr mult2 = bookScatter2D(2, 1, 1); + for (size_t b = 0; b < temphisto2.numPoints(); b++) { + const double x = temphisto2.point(b).x(); + pair ex = temphisto2.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult2 ->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult2 ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons,_c_D_star; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CRYSTAL_BALL_1986_I238081); + + +} diff --git a/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.info b/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.info new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.info @@ -0,0 +1,30 @@ +Name: CRYSTAL_BALL_1986_I238081 +Year: 1986 +Summary: Measurement of $R$ and $D^*$ production for energies between 3.67 and 4.5 GeV. +Experiment: CRYSTAL_BALL +Collider: Spear +InspireID: 238081 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - https://doi.org/10.17182/hepdata.18759 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by the Crystal Ball experiment for energies between 3.67 and 4.5 GeV. + The cross section for $D^*$ production is also measured. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Osterheld:1986hw +BibTeX: '@article{Osterheld:1986hw, + author = "Osterheld, A. and others", + title = "{Measurements of Total Hadronic and Inclusive $D^*$ + Cross-sections in $e^+ e^-$ Annihilations Between + 3.87-{GeV} and 4.5-{GeV}}", + journal = "Submitted to: Phys. Rev. D", + year = "1986", + reportNumber = "SLAC-PUB-4160", + SLACcitation = "%%CITATION = SLAC-PUB-4160;%%" +}' diff --git a/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.plot b/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.plot @@ -0,0 +1,28 @@ +BEGIN PLOT /CRYSTAL_BALL_1986_I238081/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CRYSTAL_BALL_1986_I238081/d02-x01-y01 +Title=$\sigma(e^+e^-\to D^*+X)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^*+X)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CRYSTAL_BALL_1986_I238081/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/nb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CRYSTAL_BALL_1986_I238081/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/nb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.yoda b/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/CRYSTAL_BALL_1986_I238081.yoda @@ -0,0 +1,128 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CRYSTAL_BALL_1986_I238081/d01-x01-y01 +IsRef: 1 +Path: /REF/CRYSTAL_BALL_1986_I238081/d01-x01-y01 +Title: doi:10.17182/hepdata.18759.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.670000e+00 0.000000e+00 0.000000e+00 2.500000e+00 2.261637e-01 2.261637e-01 +3.878000e+00 0.000000e+00 0.000000e+00 2.490000e+00 2.797870e-01 2.797870e-01 +3.884000e+00 0.000000e+00 0.000000e+00 2.650000e+00 2.904591e-01 2.904591e-01 +3.890000e+00 0.000000e+00 0.000000e+00 2.550000e+00 2.775221e-01 2.775221e-01 +3.896000e+00 0.000000e+00 0.000000e+00 2.580000e+00 2.921598e-01 2.921598e-01 +3.902000e+00 0.000000e+00 0.000000e+00 2.780000e+00 2.993162e-01 2.993162e-01 +3.908000e+00 0.000000e+00 0.000000e+00 2.610000e+00 2.941250e-01 2.941250e-01 +3.914000e+00 0.000000e+00 0.000000e+00 3.230000e+00 3.544058e-01 3.544058e-01 +3.920000e+00 0.000000e+00 0.000000e+00 2.920000e+00 3.149529e-01 3.149529e-01 +3.926000e+00 0.000000e+00 0.000000e+00 2.710000e+00 2.945273e-01 2.945273e-01 +3.932000e+00 0.000000e+00 0.000000e+00 3.070000e+00 3.312767e-01 3.312767e-01 +3.938000e+00 0.000000e+00 0.000000e+00 2.630000e+00 2.891108e-01 2.891108e-01 +3.944000e+00 0.000000e+00 0.000000e+00 3.350000e+00 3.507798e-01 3.507798e-01 +3.950000e+00 0.000000e+00 0.000000e+00 3.110000e+00 3.117267e-01 3.117267e-01 +3.956000e+00 0.000000e+00 0.000000e+00 2.800000e+00 2.891643e-01 2.891643e-01 +3.962000e+00 0.000000e+00 0.000000e+00 2.970000e+00 2.962679e-01 2.962679e-01 +3.968000e+00 0.000000e+00 0.000000e+00 3.150000e+00 3.428214e-01 3.428214e-01 +3.974000e+00 0.000000e+00 0.000000e+00 3.400000e+00 3.600611e-01 3.600611e-01 +3.980000e+00 0.000000e+00 0.000000e+00 3.450000e+00 3.635636e-01 3.635636e-01 +3.986000e+00 0.000000e+00 0.000000e+00 3.750000e+00 3.795557e-01 3.795557e-01 +3.992000e+00 0.000000e+00 0.000000e+00 3.430000e+00 3.456302e-01 3.456302e-01 +3.998000e+00 0.000000e+00 0.000000e+00 3.420000e+00 3.502190e-01 3.502190e-01 +4.004000e+00 0.000000e+00 0.000000e+00 3.380000e+00 3.586650e-01 3.586650e-01 +4.010000e+00 0.000000e+00 0.000000e+00 3.950000e+00 4.047944e-01 4.047944e-01 +4.016000e+00 0.000000e+00 0.000000e+00 3.840000e+00 3.968847e-01 3.968847e-01 +4.022000e+00 0.000000e+00 0.000000e+00 4.720000e+00 4.716568e-01 4.716568e-01 +4.028000e+00 0.000000e+00 0.000000e+00 4.680000e+00 4.148226e-01 4.148226e-01 +4.034000e+00 0.000000e+00 0.000000e+00 4.820000e+00 4.481292e-01 4.481292e-01 +4.040000e+00 0.000000e+00 0.000000e+00 4.540000e+00 4.148805e-01 4.148805e-01 +4.046000e+00 0.000000e+00 0.000000e+00 4.610000e+00 4.115404e-01 4.115404e-01 +4.052000e+00 0.000000e+00 0.000000e+00 4.430000e+00 3.915664e-01 3.915664e-01 +4.058000e+00 0.000000e+00 0.000000e+00 4.290000e+00 3.798557e-01 3.798557e-01 +4.064000e+00 0.000000e+00 0.000000e+00 4.010000e+00 3.565007e-01 3.565007e-01 +4.070000e+00 0.000000e+00 0.000000e+00 4.040000e+00 3.645269e-01 3.645269e-01 +4.076000e+00 0.000000e+00 0.000000e+00 4.060000e+00 3.661675e-01 3.661675e-01 +4.082000e+00 0.000000e+00 0.000000e+00 3.920000e+00 3.546990e-01 3.546990e-01 +4.088000e+00 0.000000e+00 0.000000e+00 4.070000e+00 3.669881e-01 3.669881e-01 +4.094000e+00 0.000000e+00 0.000000e+00 4.030000e+00 3.637068e-01 3.637068e-01 +4.100000e+00 0.000000e+00 0.000000e+00 4.140000e+00 3.727372e-01 3.727372e-01 +4.105000e+00 0.000000e+00 0.000000e+00 4.030000e+00 3.581657e-01 3.581657e-01 +4.109000e+00 0.000000e+00 0.000000e+00 4.060000e+00 3.801035e-01 3.801035e-01 +4.113000e+00 0.000000e+00 0.000000e+00 4.190000e+00 3.692088e-01 3.692088e-01 +4.118000e+00 0.000000e+00 0.000000e+00 4.060000e+00 3.582997e-01 3.582997e-01 +4.121000e+00 0.000000e+00 0.000000e+00 4.200000e+00 3.662458e-01 3.662458e-01 +4.125000e+00 0.000000e+00 0.000000e+00 4.210000e+00 3.688609e-01 3.688609e-01 +4.129000e+00 0.000000e+00 0.000000e+00 4.140000e+00 3.650110e-01 3.650110e-01 +4.133000e+00 0.000000e+00 0.000000e+00 4.080000e+00 3.678089e-01 3.678089e-01 +4.136000e+00 0.000000e+00 0.000000e+00 4.020000e+00 3.628870e-01 3.628870e-01 +4.141000e+00 0.000000e+00 0.000000e+00 4.090000e+00 3.608157e-01 3.608157e-01 +4.147000e+00 0.000000e+00 0.000000e+00 4.240000e+00 3.734089e-01 3.734089e-01 +4.153000e+00 0.000000e+00 0.000000e+00 4.280000e+00 3.747748e-01 3.747748e-01 +4.159000e+00 0.000000e+00 0.000000e+00 4.110000e+00 3.624935e-01 3.624935e-01 +4.165000e+00 0.000000e+00 0.000000e+00 4.000000e+00 3.532704e-01 3.532704e-01 +4.171000e+00 0.000000e+00 0.000000e+00 4.140000e+00 3.650110e-01 3.650110e-01 +4.177000e+00 0.000000e+00 0.000000e+00 4.060000e+00 3.582997e-01 3.582997e-01 +4.182000e+00 0.000000e+00 0.000000e+00 4.380000e+00 4.055423e-01 4.055423e-01 +4.185000e+00 0.000000e+00 0.000000e+00 4.140000e+00 3.673323e-01 3.673323e-01 +4.190000e+00 0.000000e+00 0.000000e+00 3.870000e+00 3.476047e-01 3.476047e-01 +4.195000e+00 0.000000e+00 0.000000e+00 3.910000e+00 3.457339e-01 3.457339e-01 +4.201000e+00 0.000000e+00 0.000000e+00 3.730000e+00 3.332498e-01 3.332498e-01 +4.208000e+00 0.000000e+00 0.000000e+00 3.710000e+00 3.230392e-01 3.230392e-01 +4.212000e+00 0.000000e+00 0.000000e+00 3.690000e+00 3.469281e-01 3.469281e-01 +4.214000e+00 0.000000e+00 0.000000e+00 3.550000e+00 3.213386e-01 3.213386e-01 +4.220000e+00 0.000000e+00 0.000000e+00 3.310000e+00 2.957620e-01 2.957620e-01 +4.226000e+00 0.000000e+00 0.000000e+00 2.950000e+00 2.851289e-01 2.851289e-01 +4.232000e+00 0.000000e+00 0.000000e+00 3.020000e+00 2.718289e-01 2.718289e-01 +4.238000e+00 0.000000e+00 0.000000e+00 3.060000e+00 2.935824e-01 2.935824e-01 +4.244000e+00 0.000000e+00 0.000000e+00 3.020000e+00 2.718289e-01 2.718289e-01 +4.250000e+00 0.000000e+00 0.000000e+00 3.110000e+00 2.822650e-01 2.822650e-01 +4.256000e+00 0.000000e+00 0.000000e+00 3.020000e+00 2.666289e-01 2.666289e-01 +4.262000e+00 0.000000e+00 0.000000e+00 3.090000e+00 3.004263e-01 3.004263e-01 +4.268000e+00 0.000000e+00 0.000000e+00 2.910000e+00 2.628002e-01 2.628002e-01 +4.274000e+00 0.000000e+00 0.000000e+00 2.920000e+00 2.828345e-01 2.828345e-01 +4.280000e+00 0.000000e+00 0.000000e+00 3.070000e+00 2.759425e-01 2.759425e-01 +4.292000e+00 0.000000e+00 0.000000e+00 2.980000e+00 2.685423e-01 2.685423e-01 +4.304000e+00 0.000000e+00 0.000000e+00 3.340000e+00 3.010838e-01 3.010838e-01 +4.316000e+00 0.000000e+00 0.000000e+00 3.230000e+00 2.920676e-01 2.920676e-01 +4.328000e+00 0.000000e+00 0.000000e+00 3.320000e+00 2.994424e-01 2.994424e-01 +4.340000e+00 0.000000e+00 0.000000e+00 3.430000e+00 3.084806e-01 3.084806e-01 +4.352000e+00 0.000000e+00 0.000000e+00 3.440000e+00 3.019415e-01 3.019415e-01 +4.364000e+00 0.000000e+00 0.000000e+00 3.650000e+00 3.266290e-01 3.266290e-01 +4.376000e+00 0.000000e+00 0.000000e+00 3.750000e+00 3.349067e-01 3.349067e-01 +4.382000e+00 0.000000e+00 0.000000e+00 3.860000e+00 3.685879e-01 3.685879e-01 +4.388000e+00 0.000000e+00 0.000000e+00 3.820000e+00 3.407107e-01 3.407107e-01 +4.394000e+00 0.000000e+00 0.000000e+00 3.990000e+00 4.023789e-01 4.023789e-01 +4.400000e+00 0.000000e+00 0.000000e+00 4.000000e+00 3.532704e-01 3.532704e-01 +4.406000e+00 0.000000e+00 0.000000e+00 3.790000e+00 3.878071e-01 3.878071e-01 +4.412000e+00 0.000000e+00 0.000000e+00 3.940000e+00 3.482451e-01 3.482451e-01 +4.418000e+00 0.000000e+00 0.000000e+00 4.030000e+00 3.637068e-01 3.637068e-01 +4.424000e+00 0.000000e+00 0.000000e+00 4.020000e+00 3.509800e-01 3.509800e-01 +4.430000e+00 0.000000e+00 0.000000e+00 4.090000e+00 3.686298e-01 3.686298e-01 +4.436000e+00 0.000000e+00 0.000000e+00 4.050000e+00 3.598312e-01 3.598312e-01 +4.442000e+00 0.000000e+00 0.000000e+00 3.890000e+00 3.898430e-01 3.898430e-01 +4.448000e+00 0.000000e+00 0.000000e+00 3.920000e+00 3.517263e-01 3.517263e-01 +4.460000e+00 0.000000e+00 0.000000e+00 3.850000e+00 3.868934e-01 3.868934e-01 +4.472000e+00 0.000000e+00 0.000000e+00 3.840000e+00 3.861573e-01 3.861573e-01 +4.484000e+00 0.000000e+00 0.000000e+00 3.610000e+00 3.748834e-01 3.748834e-01 +4.496000e+00 0.000000e+00 0.000000e+00 3.720000e+00 3.827586e-01 3.827586e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CRYSTAL_BALL_1986_I238081/d02-x01-y01 +IsRef: 1 +Path: /REF/CRYSTAL_BALL_1986_I238081/d02-x01-y01 +Title: doi:10.17182/hepdata.18759.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.949000e+00 7.900000e-02 6.400000e-02 3.450000e+00 9.366542e-01 9.366542e-01 +4.042000e+00 2.900000e-02 1.800000e-02 1.696000e+01 2.942610e+00 2.942610e+00 +4.080000e+00 2.000000e-02 2.200000e-02 1.510000e+01 2.701193e+00 2.701193e+00 +4.114000e+00 1.200000e-02 7.000000e-03 1.475000e+01 2.625400e+00 2.625400e+00 +4.124000e+00 3.000000e-03 5.000000e-03 1.497000e+01 2.690773e+00 2.690773e+00 +4.139000e+00 1.000000e-02 1.100000e-02 1.266000e+01 2.329748e+00 2.329748e+00 +4.161000e+00 1.100000e-02 1.300000e-02 1.316000e+01 2.448699e+00 2.448699e+00 +4.188000e+00 1.400000e-02 1.600000e-02 1.525000e+01 2.712973e+00 2.712973e+00 +4.216000e+00 1.200000e-02 2.400000e-02 8.300000e+00 1.729571e+00 1.729571e+00 +4.268000e+00 2.800000e-02 4.200000e-02 6.030000e+00 1.349261e+00 1.349261e+00 +4.339000e+00 2.900000e-02 2.100000e-02 6.650000e+00 1.652734e+00 1.652734e+00 +4.384000e+00 2.400000e-02 1.900000e-02 1.076000e+01 2.313865e+00 2.313865e+00 +4.419000e+00 1.600000e-02 9.000000e-03 9.760000e+00 2.216277e+00 2.216277e+00 +4.446000e+00 1.800000e-02 5.400000e-02 9.600000e+00 2.147465e+00 2.147465e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.cc b/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.cc @@ -0,0 +1,103 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class CRYSTAL_BALL_1990_I294419 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(CRYSTAL_BALL_1990_I294419); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + for(unsigned int ix=1;ix<3;++ix) { + Scatter2D temphisto(refData(ix, 1, 1)); + ostringstream title; + title << "d0" << ix; + Scatter2DPtr hadrons = bookScatter2D(title.str()+"sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D(title.str()+"sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(CRYSTAL_BALL_1990_I294419); + + +} diff --git a/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.info b/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.info new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.info @@ -0,0 +1,30 @@ +Name: CRYSTAL_BALL_1990_I294419 +Year: 1990 +Summary: Measurement of $R$ for energies between 5 and 7.4 GeV +Experiment: CRYSTAL_BALL +Collider: Spear +InspireID: 294419 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B234 (1990) 525-533, 1990 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by the Crystal Ball experiment + for energies between 5 and 7.4 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Edwards:1990pc +BibTeX: '@article{Edwards:1990pc, + author = "Edwards, C. and others", + title = "{Hadron Production in $e^+ e^-$ Annihilation From + $\sqrt{s}=5$-{GeV} to 7.4-{GeV}}", + journal = "Submitted to: Phys. Rev. D", + year = "1990", + reportNumber = "SLAC-PUB-5160", + SLACcitation = "%%CITATION = SLAC-PUB-5160;%%" +}' diff --git a/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.plot b/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.plot @@ -0,0 +1,42 @@ +BEGIN PLOT /CRYSTAL_BALL_1990_I294419/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CRYSTAL_BALL_1990_I294419/d01_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CRYSTAL_BALL_1990_I294419/d01_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CRYSTAL_BALL_1990_I294419/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CRYSTAL_BALL_1990_I294419/d02_sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /CRYSTAL_BALL_1990_I294419/d02_sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.yoda b/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/CRYSTAL_BALL_1990_I294419.yoda @@ -0,0 +1,49 @@ +BEGIN YODA_SCATTER2D_V2 /REF/CRYSTAL_BALL_1990_I294419/d01-x01-y01 +IsRef: 1 +Path: /REF/CRYSTAL_BALL_1990_I294419/d01-x01-y01 +Title: doi:10.17182/hepdata.18758.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.200000e+00 0.000000e+00 0.000000e+00 3.440000e+00 1.523155e-01 1.523155e-01 +6.000000e+00 0.000000e+00 0.000000e+00 3.440000e+00 1.581139e-01 1.581139e-01 +6.500000e+00 0.000000e+00 0.000000e+00 3.620000e+00 2.024846e-01 2.024846e-01 +7.000000e+00 0.000000e+00 0.000000e+00 3.710000e+00 1.923538e-01 1.923538e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CRYSTAL_BALL_1990_I294419/d02-x01-y01 +IsRef: 1 +Path: /REF/CRYSTAL_BALL_1990_I294419/d02-x01-y01 +Title: doi:10.17182/hepdata.18758.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e+00 0.000000e+00 0.000000e+00 3.420000e+00 1.697056e-01 1.697056e-01 +5.250000e+00 0.000000e+00 0.000000e+00 3.570000e+00 1.140175e-01 1.140175e-01 +5.500000e+00 0.000000e+00 0.000000e+00 3.410000e+00 1.166190e-01 1.166190e-01 +5.750000e+00 0.000000e+00 0.000000e+00 3.440000e+00 1.118034e-01 1.118034e-01 +6.000000e+00 0.000000e+00 0.000000e+00 3.500000e+00 1.280625e-01 1.280625e-01 +6.250000e+00 0.000000e+00 0.000000e+00 3.310000e+00 1.044031e-01 1.044031e-01 +6.500000e+00 0.000000e+00 0.000000e+00 3.370000e+00 1.044031e-01 1.044031e-01 +6.750000e+00 0.000000e+00 0.000000e+00 3.420000e+00 1.081665e-01 1.081665e-01 +7.000000e+00 0.000000e+00 0.000000e+00 3.350000e+00 1.077033e-01 1.077033e-01 +7.250000e+00 0.000000e+00 0.000000e+00 3.570000e+00 1.303840e-01 1.303840e-01 +7.400000e+00 0.000000e+00 0.000000e+00 3.350000e+00 1.720465e-01 1.720465e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CRYSTAL_BALL_1990_I294419/d03-x01-y01 +IsRef: 1 +Path: /REF/CRYSTAL_BALL_1990_I294419/d03-x01-y01 +Title: doi:10.17182/hepdata.18758.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.000000e+00 1.000000e+00 1.400000e+00 3.440000e+00 1.824829e-01 1.824829e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/CRYSTAL_BALL_1990_I294419/d04-x01-y01 +IsRef: 1 +Path: /REF/CRYSTAL_BALL_1990_I294419/d04-x01-y01 +Title: doi:10.17182/hepdata.18758.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.000000e+00 0.000000e+00 0.000000e+00 1.200000e-01 1.100000e-01 1.100000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/HRS_1986_I18502.cc b/analyses/pluginSLAC/HRS_1986_I18502.cc rename from analyses/pluginMisc/HRS_1986_I18502.cc rename to analyses/pluginSLAC/HRS_1986_I18502.cc diff --git a/analyses/pluginMisc/HRS_1986_I18502.info b/analyses/pluginSLAC/HRS_1986_I18502.info rename from analyses/pluginMisc/HRS_1986_I18502.info rename to analyses/pluginSLAC/HRS_1986_I18502.info diff --git a/analyses/pluginMisc/HRS_1986_I18502.plot b/analyses/pluginSLAC/HRS_1986_I18502.plot rename from analyses/pluginMisc/HRS_1986_I18502.plot rename to analyses/pluginSLAC/HRS_1986_I18502.plot diff --git a/analyses/pluginMisc/HRS_1986_I18502.yoda b/analyses/pluginSLAC/HRS_1986_I18502.yoda rename from analyses/pluginMisc/HRS_1986_I18502.yoda rename to analyses/pluginSLAC/HRS_1986_I18502.yoda diff --git a/analyses/pluginSLAC/MAC_1985_I206052.cc b/analyses/pluginSLAC/MAC_1985_I206052.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MAC_1985_I206052.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MAC_1985_I206052 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MAC_1985_I206052); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MAC_1985_I206052); + + +} diff --git a/analyses/pluginSLAC/MAC_1985_I206052.info b/analyses/pluginSLAC/MAC_1985_I206052.info new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MAC_1985_I206052.info @@ -0,0 +1,33 @@ +Name: MAC_1985_I206052 +Year: 1985 +Summary: Measurement of $R$ at 29 GeV +Experiment: MAC +Collider: PEP +InspireID: 206052 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D31 (1985) 1537, 1985 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by MAC at 29 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Fernandez:1984yw +BibTeX: '@article{Fernandez:1984yw, + author = "Fernandez, E. and others", + title = "{Precision Measurement of the Total Cross-section for + $e^+ e^- \to$ Hadrons at a Center-of-mass Energy of + 29-{GeV}}", + journal = "Phys. Rev.", + volume = "D31", + year = "1985", + pages = "1537", + doi = "10.1103/PhysRevD.31.1537", + reportNumber = "SLAC-PUB-3479", + SLACcitation = "%%CITATION = PHRVA,D31,1537;%%" +}' diff --git a/analyses/pluginSLAC/MAC_1985_I206052.plot b/analyses/pluginSLAC/MAC_1985_I206052.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MAC_1985_I206052.plot @@ -0,0 +1,27 @@ +BEGIN PLOT /MAC_1985_I206052/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +XMin=28. +XMax=30. +END PLOT +BEGIN PLOT /MAC_1985_I206052/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=28. +XMax=30. +END PLOT +BEGIN PLOT /MAC_1985_I206052/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +XMin=28. +XMax=30. +END PLOT diff --git a/analyses/pluginSLAC/MAC_1985_I206052.yoda b/analyses/pluginSLAC/MAC_1985_I206052.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MAC_1985_I206052.yoda @@ -0,0 +1,27 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MAC_1985_I206052/d01-x01-y01 +IsRef: 1 +Path: /REF/MAC_1985_I206052/d01-x01-y01 +Title: doi:10.17182/hepdata.4048.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.900000e+01 0.000000e+00 0.000000e+00 3.960000e+00 9.486833e-02 9.486833e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MAC_1985_I206052/d02-x01-y01 +IsRef: 1 +Path: /REF/MAC_1985_I206052/d02-x01-y01 +Title: doi:10.17182/hepdata.4048.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.900000e+01 0.000000e+00 0.000000e+00 2.300000e-01 6.000000e-02 6.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MAC_1985_I206052/d02-x01-y02 +IsRef: 1 +Path: /REF/MAC_1985_I206052/d02-x01-y02 +Title: doi:10.17182/hepdata.4048.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.900000e+01 0.000000e+00 0.000000e+00 8.200000e-01 5.900000e-01 9.000000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginSLAC/MARKII_1979_I143939.cc b/analyses/pluginSLAC/MARKII_1979_I143939.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKII_1979_I143939.cc @@ -0,0 +1,180 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" +#include "Rivet/Projections/UnstableParticles.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKII_1979_I143939 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKII_1979_I143939); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + declare(UnstableParticles(), "UFS"); + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + _c_DD = bookCounter("/TMP/sigma_DD"); + } + + void findChildren(const Particle & p,map & nRes, int &ncount) { + foreach(const Particle &child, p.children()) { + if(child.children().empty()) { + nRes[child.pdgId()]-=1; + --ncount; + } + else + findChildren(child,nRes,ncount); + } + } + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + // total hadronic and muonic cross sections + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + // identified final state with D mesons + const FinalState& ufs = apply(event, "UFS"); + for(unsigned int ix=0;ix nRes = nCount; + int ncount = ntotal; + findChildren(p1,nRes,ncount); + // loop over the other fs particles + for(unsigned int iy=ix+1;iy nRes2 = nRes; + int ncount2 = ncount; + findChildren(p2,nRes2,ncount2); + if(ncount2!=0) continue; + matched=true; + for(auto const & val : nRes2) { + if(val.second!=0) { + matched = false; + break; + } + } + if(matched) { + _c_DD ->fill(event.weight()); + break; + } + } + if(matched) break; + } + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(2, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(2,1,1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + double sigma = _c_DD->val()*fact; + double error = _c_DD->err()*fact; + Scatter2D temphisto2(refData(3, 1, 1)); + mult = bookScatter2D(3,1,1); + for (size_t b = 0; b < temphisto2.numPoints(); b++) { + const double x = temphisto2.point(b).x(); + pair ex = temphisto2.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons, _c_DD; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKII_1979_I143939); + + +} diff --git a/analyses/pluginSLAC/MARKII_1979_I143939.info b/analyses/pluginSLAC/MARKII_1979_I143939.info new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKII_1979_I143939.info @@ -0,0 +1,30 @@ +Name: MARKII_1979_I143939 +Year: 1979 +Summary: Measurement of $R$ and $D\bar{D}$ cross section between 3.67 and 3.872 GeV +Experiment: MARKII +Collider: SPEAR +InspireID: 143939 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Schindler, R.H. PhD Thesis, 1979 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ and the $D\bar{D}$ cross section in $e^+e^-$ collisions between 3.67 and 3.872 GeV + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Schindler:1979rj +BibTeX: '@phdthesis{Schindler:1979rj, + author = "Schindler, R. H.", + title = "{CHARMED MESON PRODUCTION AND DECAY PROPERTIES AT THE + psi-prime-prime (3770)}", + school = "SLAC", + url = "http://inspirebeta.net/record/143939/files/slac-r-219.pdf", + year = "1979", + reportNumber = "SLAC-R-0219, SLAC-R-219, SLAC-0219, SLAC-219", + SLACcitation = "%%CITATION = SLAC-R-0219;%%" +}' diff --git a/analyses/pluginSLAC/MARKII_1979_I143939.plot b/analyses/pluginSLAC/MARKII_1979_I143939.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKII_1979_I143939.plot @@ -0,0 +1,30 @@ +BEGIN PLOT /MARKII_1979_I143939/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /MARKII_1979_I143939/d03-x01-y01 +Title=$\sigma(e^+e^-\to D^+D^-, D^0\bar{D}^0)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to D^+D^-, D^0\bar{D}^0)$ +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /MARKII_1979_I143939/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKII_1979_I143939/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginSLAC/MARKII_1979_I143939.yoda b/analyses/pluginSLAC/MARKII_1979_I143939.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKII_1979_I143939.yoda @@ -0,0 +1,123 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKII_1979_I143939/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKII_1979_I143939/d01-x01-y01 +Title: doi:10.17182/hepdata.18893.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.670000e+00 0.000000e+00 0.000000e+00 2.410000e+00 2.838679e-01 2.838679e-01 +3.692000e+00 0.000000e+00 0.000000e+00 7.100000e+00 8.300602e-01 8.300602e-01 +3.704000e+00 0.000000e+00 0.000000e+00 4.560000e+00 5.628819e-01 5.628819e-01 +3.716000e+00 0.000000e+00 0.000000e+00 3.620000e+00 4.638362e-01 4.638362e-01 +3.728000e+00 0.000000e+00 0.000000e+00 3.690000e+00 4.693197e-01 4.693197e-01 +3.740000e+00 0.000000e+00 0.000000e+00 3.510000e+00 4.039814e-01 4.039814e-01 +3.746000e+00 0.000000e+00 0.000000e+00 3.390000e+00 3.936001e-01 3.936001e-01 +3.752000e+00 0.000000e+00 0.000000e+00 3.970000e+00 4.588126e-01 4.588126e-01 +3.758000e+00 0.000000e+00 0.000000e+00 4.130000e+00 4.727251e-01 4.727251e-01 +3.764000e+00 0.000000e+00 0.000000e+00 4.350000e+00 5.400231e-01 5.400231e-01 +3.770000e+00 0.000000e+00 0.000000e+00 4.390000e+00 5.432504e-01 5.432504e-01 +3.771000e+00 0.000000e+00 0.000000e+00 3.960000e+00 4.908319e-01 4.908319e-01 +3.772000e+00 0.000000e+00 0.000000e+00 4.260000e+00 5.268548e-01 5.268548e-01 +3.776000e+00 0.000000e+00 0.000000e+00 3.880000e+00 4.904529e-01 4.904529e-01 +3.782000e+00 0.000000e+00 0.000000e+00 3.260000e+00 4.108236e-01 4.108236e-01 +3.788000e+00 0.000000e+00 0.000000e+00 3.080000e+00 3.904664e-01 3.904664e-01 +3.794000e+00 0.000000e+00 0.000000e+00 2.990000e+00 3.897448e-01 3.897448e-01 +3.800000e+00 0.000000e+00 0.000000e+00 3.260000e+00 4.169844e-01 4.169844e-01 +3.812000e+00 0.000000e+00 0.000000e+00 2.630000e+00 3.428834e-01 3.428834e-01 +3.824000e+00 0.000000e+00 0.000000e+00 3.070000e+00 3.959154e-01 3.959154e-01 +3.836000e+00 0.000000e+00 0.000000e+00 2.650000e+00 3.508917e-01 3.508917e-01 +3.848000e+00 0.000000e+00 0.000000e+00 2.790000e+00 3.615812e-01 3.615812e-01 +3.860000e+00 0.000000e+00 0.000000e+00 2.780000e+00 3.672656e-01 3.672656e-01 +3.872000e+00 0.000000e+00 0.000000e+00 2.930000e+00 3.787466e-01 3.787466e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKII_1979_I143939/d02-x01-y01 +IsRef: 1 +Path: /REF/MARKII_1979_I143939/d02-x01-y01 +Title: doi:10.17182/hepdata.18893.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.670000e+00 0.000000e+00 0.000000e+00 2.180000e+00 2.646205e-01 2.646205e-01 +3.692000e+00 0.000000e+00 0.000000e+00 2.060000e+00 4.767977e-01 4.767977e-01 +3.704000e+00 0.000000e+00 0.000000e+00 2.280000e+00 4.011035e-01 4.011035e-01 +3.716000e+00 0.000000e+00 0.000000e+00 2.080000e+00 3.568809e-01 3.568809e-01 +3.728000e+00 0.000000e+00 0.000000e+00 2.670000e+00 3.941941e-01 3.941941e-01 +3.740000e+00 0.000000e+00 0.000000e+00 2.660000e+00 3.328002e-01 3.328002e-01 +3.746000e+00 0.000000e+00 0.000000e+00 2.600000e+00 3.280244e-01 3.280244e-01 +3.752000e+00 0.000000e+00 0.000000e+00 3.490000e+00 4.179725e-01 4.179725e-01 +3.758000e+00 0.000000e+00 0.000000e+00 3.760000e+00 4.407675e-01 4.407675e-01 +3.764000e+00 0.000000e+00 0.000000e+00 4.040000e+00 5.153795e-01 5.153795e-01 +3.770000e+00 0.000000e+00 0.000000e+00 4.130000e+00 5.224644e-01 5.224644e-01 +3.771000e+00 0.000000e+00 0.000000e+00 3.470000e+00 4.522267e-01 4.522267e-01 +3.772000e+00 0.000000e+00 0.000000e+00 3.810000e+00 4.911833e-01 4.911833e-01 +3.776000e+00 0.000000e+00 0.000000e+00 3.320000e+00 4.474640e-01 4.474640e-01 +3.782000e+00 0.000000e+00 0.000000e+00 2.640000e+00 3.635877e-01 3.635877e-01 +3.788000e+00 0.000000e+00 0.000000e+00 2.460000e+00 3.436801e-01 3.436801e-01 +3.794000e+00 0.000000e+00 0.000000e+00 2.390000e+00 3.458627e-01 3.458627e-01 +3.800000e+00 0.000000e+00 0.000000e+00 2.640000e+00 3.705347e-01 3.705347e-01 +3.812000e+00 0.000000e+00 0.000000e+00 2.130000e+00 3.062172e-01 3.062172e-01 +3.824000e+00 0.000000e+00 0.000000e+00 2.490000e+00 3.528470e-01 3.528470e-01 +3.836000e+00 0.000000e+00 0.000000e+00 2.200000e+00 3.182766e-01 3.182766e-01 +3.848000e+00 0.000000e+00 0.000000e+00 2.310000e+00 3.259770e-01 3.259770e-01 +3.860000e+00 0.000000e+00 0.000000e+00 2.320000e+00 3.338023e-01 3.338023e-01 +3.872000e+00 0.000000e+00 0.000000e+00 2.420000e+00 3.408284e-01 3.408284e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKII_1979_I143939/d03-x01-y01 +IsRef: 1 +Path: /REF/MARKII_1979_I143939/d03-x01-y01 +Title: doi:10.17182/hepdata.18893.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.670000e+00 0.000000e+00 0.000000e+00 -2.600000e-01 9.703484e-01 9.703484e-01 +3.692000e+00 0.000000e+00 0.000000e+00 -1.080000e+00 2.872031e+00 2.872031e+00 +3.704000e+00 0.000000e+00 0.000000e+00 3.300000e-01 2.090261e+00 2.090261e+00 +3.716000e+00 0.000000e+00 0.000000e+00 -9.000000e-01 1.822224e+00 1.822224e+00 +3.728000e+00 0.000000e+00 0.000000e+00 1.710000e+00 1.818060e+00 1.818060e+00 +3.740000e+00 0.000000e+00 0.000000e+00 1.880000e+00 1.254171e+00 1.254171e+00 +3.746000e+00 0.000000e+00 0.000000e+00 1.620000e+00 1.250537e+00 1.250537e+00 +3.752000e+00 0.000000e+00 0.000000e+00 5.560000e+00 1.524971e+00 1.524971e+00 +3.758000e+00 0.000000e+00 0.000000e+00 6.840000e+00 1.567149e+00 1.567149e+00 +3.764000e+00 0.000000e+00 0.000000e+00 8.460000e+00 2.134787e+00 2.134787e+00 +3.770000e+00 0.000000e+00 0.000000e+00 9.550000e+00 2.171296e+00 2.171296e+00 +3.771000e+00 0.000000e+00 0.000000e+00 6.330000e+00 1.879784e+00 1.879784e+00 +3.772000e+00 0.000000e+00 0.000000e+00 8.190000e+00 2.059821e+00 2.059821e+00 +3.776000e+00 0.000000e+00 0.000000e+00 5.970000e+00 1.924918e+00 1.924918e+00 +3.782000e+00 0.000000e+00 0.000000e+00 2.430000e+00 1.539301e+00 1.539301e+00 +3.788000e+00 0.000000e+00 0.000000e+00 1.450000e+00 1.457232e+00 1.457232e+00 +3.794000e+00 0.000000e+00 0.000000e+00 1.080000e+00 1.513857e+00 1.513857e+00 +3.800000e+00 0.000000e+00 0.000000e+00 2.850000e+00 1.585820e+00 1.585820e+00 +3.812000e+00 0.000000e+00 0.000000e+00 -7.200000e-01 1.311977e+00 1.311977e+00 +3.824000e+00 0.000000e+00 0.000000e+00 2.100000e+00 1.494824e+00 1.494824e+00 +3.836000e+00 0.000000e+00 0.000000e+00 -2.200000e-01 1.360178e+00 1.360178e+00 +3.848000e+00 0.000000e+00 0.000000e+00 7.600000e-01 1.352138e+00 1.352138e+00 +3.860000e+00 0.000000e+00 0.000000e+00 8.100000e-01 1.402341e+00 1.402341e+00 +3.872000e+00 0.000000e+00 0.000000e+00 1.800000e+00 1.401606e+00 1.401606e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKII_1979_I143939/d04-x01-y01 +IsRef: 1 +Path: /REF/MARKII_1979_I143939/d04-x01-y01 +Title: doi:10.17182/hepdata.18893.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.771000e+00 1.000000e-03 1.000000e-03 6.990000e+00 1.292401e+00 1.303189e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKII_1979_I143939/d04-x01-y02 +IsRef: 1 +Path: /REF/MARKII_1979_I143939/d04-x01-y02 +Title: doi:10.17182/hepdata.18893.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.771000e+00 1.000000e-03 1.000000e-03 8.000000e+00 1.733955e+00 1.733955e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKII_1979_I143939/d04-x01-y03 +IsRef: 1 +Path: /REF/MARKII_1979_I143939/d04-x01-y03 +Title: doi:10.17182/hepdata.18893.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.771000e+00 1.000000e-03 1.000000e-03 6.000000e+00 1.385208e+00 1.385208e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginSLAC/MARKII_1991_I295286.cc b/analyses/pluginSLAC/MARKII_1991_I295286.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKII_1991_I295286.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKII_1991_I295286 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKII_1991_I295286); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKII_1991_I295286); + + +} diff --git a/analyses/pluginSLAC/MARKII_1991_I295286.info b/analyses/pluginSLAC/MARKII_1991_I295286.info new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKII_1991_I295286.info @@ -0,0 +1,33 @@ +Name: MARKII_1991_I295286 +Year: 1991 +Summary: Measurement of $R$ at 29 GeV +Experiment: MARKII +Collider: PEP +InspireID: 295286 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D43 (1991) 34-45, 1991 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by MARKII at 29 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: VonZanthier:1990we +BibTeX: '@article{VonZanthier:1990we, + author = "Von Zanthier, Christoph and others", + title = "{Measurement of the Total Hadronic Cross-section in $e^+ + e^-$ Annihilation at $\sqrt{s}=29$-{GeV}}", + collaboration = "MARK-II", + journal = "Phys. Rev.", + volume = "D43", + year = "1991", + pages = "34-45", + doi = "10.1103/PhysRevD.43.34", + reportNumber = "SLAC-PUB-5213, LBL-28859", + SLACcitation = "%%CITATION = PHRVA,D43,34;%%" +}' diff --git a/analyses/pluginSLAC/MARKII_1991_I295286.plot b/analyses/pluginSLAC/MARKII_1991_I295286.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKII_1991_I295286.plot @@ -0,0 +1,27 @@ +BEGIN PLOT /MARKII_1991_I295286/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +XMin=28. +XMax=30. +END PLOT +BEGIN PLOT /MARKII_1991_I295286/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=28. +XMax=30. +END PLOT +BEGIN PLOT /MARKII_1991_I295286/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +XMin=28. +XMax=30. +END PLOT \ No newline at end of file diff --git a/analyses/pluginSLAC/MARKII_1991_I295286.yoda b/analyses/pluginSLAC/MARKII_1991_I295286.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKII_1991_I295286.yoda @@ -0,0 +1,9 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKII_1991_I295286/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKII_1991_I295286/d01-x01-y01 +Title: doi:10.17182/hepdata.22852.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.900000e+01 0.000000e+00 0.000000e+00 3.920000e+00 1.029563e-01 1.029563e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginSLAC/MARKI_1975_I100592.cc b/analyses/pluginSLAC/MARKI_1975_I100592.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1975_I100592.cc @@ -0,0 +1,85 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/ChargedFinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKI_1975_I100592 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKI_1975_I100592); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(ChargedFinalState(), "FS"); + + // Book histograms + _nHadrons= bookCounter("TMP/hadrons"); + _nEvent= bookCounter("TMP/event"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const ChargedFinalState& fs = apply(event, "FS"); + _nEvent->fill(event.weight()); + _nHadrons->fill(fs.particles().size()*event.weight()); + } + + /// Normalise histograms etc., after the run + void finalize() { + for(unsigned int ix=1;ix<3;++ix) { + double sigma,error; + if(ix==1) { + sigma = _nEvent->val()*crossSection()/ sumOfWeights() /nanobarn; + error = _nEvent->err()*crossSection()/ sumOfWeights() /nanobarn; + } + else { + sigma = _nHadrons->val()/sumOfWeights(); + error = _nHadrons->err()/sumOfWeights(); + } + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nHadrons,_nEvent; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKI_1975_I100592); + + +} diff --git a/analyses/pluginSLAC/MARKI_1975_I100592.info b/analyses/pluginSLAC/MARKI_1975_I100592.info new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1975_I100592.info @@ -0,0 +1,30 @@ +Name: MARKI_1975_I100592 +Year: 1975 +Summary: Cross section and charged particle multiplicity for energies between 2.6 and 5 GeV +Experiment: MARKI +Collider: SPEAR +InspireID: 100592 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 34 (1975) 764, 1975 +RunInfo: e+e- to hadrons +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Cross section and harged particle multiplicity for energies between 2.6 and 5 GeV' +BibKey: Augustin:1975yq +BibTeX: '@article{Augustin:1975yq, + author = "Augustin, J. E. and others", + title = "{Total Cross-Section for Hadron Production by + electron-Positron Annihilation Between 2.4-GeV and 5.0-GeV + Center-Of-Mass Energy}", + journal = "Phys. Rev. Lett.", + volume = "34", + year = "1975", + pages = "764", + doi = "10.1103/PhysRevLett.34.764", + reportNumber = "SLAC-PUB-1520, LBL-3621", + SLACcitation = "%%CITATION = PRLTA,34,764;%%" +}' diff --git a/analyses/pluginSLAC/MARKI_1975_I100592.plot b/analyses/pluginSLAC/MARKI_1975_I100592.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1975_I100592.plot @@ -0,0 +1,15 @@ +BEGIN PLOT /MARKI_1975_I100592/d01-x01-y01 +Title=Hadronic cross section +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to\text{hadrons})/$nb +ConnectGaps=1 +LogY=0 +END PLOT + +BEGIN PLOT /MARKI_1975_I100592/d02-x01-y01 +Title=Charged hadron multiplicity +XLabel=$\sqrt{s}$/GeV +YLabel=$N_{\text{charged}}$ +ConnectGaps=1 +LogY=0 +END PLOT diff --git a/analyses/pluginSLAC/MARKI_1975_I100592.yoda b/analyses/pluginSLAC/MARKI_1975_I100592.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1975_I100592.yoda @@ -0,0 +1,52 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1975_I100592/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1975_I100592/d01-x01-y01 +Title: doi:10.17182/hepdata.21227.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.400000e+00 0.000000e+00 0.000000e+00 3.180000e+01 4.803374e+00 4.803374e+00 +2.600000e+00 0.000000e+00 0.000000e+00 3.250000e+01 5.470146e+00 5.470146e+00 +2.800000e+00 0.000000e+00 0.000000e+00 2.940000e+01 5.045156e+00 5.045156e+00 +3.000000e+00 0.000000e+00 0.000000e+00 2.330000e+01 3.070651e+00 3.070651e+00 +3.100000e+00 0.000000e+00 0.000000e+00 2.250000e+01 4.077070e+00 4.077070e+00 +3.200000e+00 0.000000e+00 0.000000e+00 2.140000e+01 3.141592e+00 3.141592e+00 +3.300000e+00 0.000000e+00 0.000000e+00 1.890000e+01 3.214358e+00 3.214358e+00 +3.400000e+00 0.000000e+00 0.000000e+00 1.870000e+01 3.042515e+00 3.042515e+00 +3.600000e+00 0.000000e+00 0.000000e+00 1.910000e+01 2.913434e+00 2.913434e+00 +3.800000e+00 0.000000e+00 0.000000e+00 1.970000e+01 2.602095e+00 2.602095e+00 +4.000000e+00 0.000000e+00 0.000000e+00 2.450000e+01 4.110049e+00 4.110049e+00 +4.100000e+00 0.000000e+00 0.000000e+00 3.180000e+01 4.803374e+00 4.803374e+00 +4.200000e+00 0.000000e+00 0.000000e+00 2.810000e+01 3.896935e+00 3.896935e+00 +4.300000e+00 0.000000e+00 0.000000e+00 2.360000e+01 3.661912e+00 3.661912e+00 +4.400000e+00 0.000000e+00 0.000000e+00 1.960000e+01 3.176728e+00 3.176728e+00 +4.600000e+00 0.000000e+00 0.000000e+00 1.530000e+01 2.439447e+00 2.439447e+00 +4.800000e+00 0.000000e+00 0.000000e+00 1.820000e+01 2.358474e+00 2.358474e+00 +5.000000e+00 0.000000e+00 0.000000e+00 1.770000e+01 2.320108e+00 2.320108e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1975_I100592/d02-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1975_I100592/d02-x01-y01 +Title: doi:10.17182/hepdata.21227.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.400000e+00 0.000000e+00 0.000000e+00 3.310000e+00 1.200000e-01 1.200000e-01 +2.600000e+00 0.000000e+00 0.000000e+00 3.180000e+00 1.500000e-01 1.500000e-01 +2.800000e+00 0.000000e+00 0.000000e+00 3.370000e+00 1.800000e-01 1.800000e-01 +3.000000e+00 0.000000e+00 0.000000e+00 3.550000e+00 4.000000e-02 4.000000e-02 +3.100000e+00 0.000000e+00 0.000000e+00 3.510000e+00 2.100000e-01 2.100000e-01 +3.200000e+00 0.000000e+00 0.000000e+00 3.890000e+00 1.200000e-01 1.200000e-01 +3.300000e+00 0.000000e+00 0.000000e+00 3.840000e+00 1.900000e-01 1.900000e-01 +3.400000e+00 0.000000e+00 0.000000e+00 3.930000e+00 1.900000e-01 1.900000e-01 +3.600000e+00 0.000000e+00 0.000000e+00 4.000000e+00 1.700000e-01 1.700000e-01 +3.800000e+00 0.000000e+00 0.000000e+00 3.870000e+00 5.000000e-02 5.000000e-02 +4.000000e+00 0.000000e+00 0.000000e+00 3.900000e+00 2.000000e-01 2.000000e-01 +4.100000e+00 0.000000e+00 0.000000e+00 4.040000e+00 1.700000e-01 1.700000e-01 +4.200000e+00 0.000000e+00 0.000000e+00 4.000000e+00 1.000000e-01 1.000000e-01 +4.300000e+00 0.000000e+00 0.000000e+00 4.020000e+00 1.800000e-01 1.800000e-01 +4.400000e+00 0.000000e+00 0.000000e+00 4.400000e+00 2.400000e-01 2.400000e-01 +4.600000e+00 0.000000e+00 0.000000e+00 4.620000e+00 2.300000e-01 2.300000e-01 +4.800000e+00 0.000000e+00 0.000000e+00 4.310000e+00 4.000000e-02 4.000000e-02 +5.000000e+00 0.000000e+00 0.000000e+00 4.320000e+00 9.000000e-02 9.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginSLAC/MARKI_1975_I100733.cc b/analyses/pluginSLAC/MARKI_1975_I100733.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1975_I100733.cc @@ -0,0 +1,113 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKI_1975_I100733 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKI_1975_I100733); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + declare(FinalState(), "FS"); + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + // if(inRange(sqrtS()/GeV,2.999,3.001)) + // _h_charged = bookHisto1D(3, 1, 1); + // else if(inRange(sqrtS()/GeV,4.799,4.801)) + // _h_charged = bookHisto1D(3, 1, 2); + // else if(inRange(sqrtS()/GeV,7.399,7.401)) + // _h_charged = bookHisto1D(3, 1, 3); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + // if(PID::isCharged(p.pdgId())&&_h_charged&&abs(p.pdgId())!=13) { + // double x = 2.*p.p3().mod()/sqrtS(); + // _h_charged->fill(x,event.weight()); + // } + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + // if(_h_charged) { + // //scale(_h_charged, crossSection()/ sumOfWeights() /microbarn*sqr(sqrtS())); + // } + // R + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D(1,1,1); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(2,1,1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + // Histo1DPtr _h_charged; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKI_1975_I100733); + + +} diff --git a/analyses/pluginSLAC/MARKI_1975_I100733.info b/analyses/pluginSLAC/MARKI_1975_I100733.info new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1975_I100733.info @@ -0,0 +1,33 @@ +Name: MARKI_1975_I100733 +Year: 1975 +Summary: Measurement of $R$ and the hadronic cross section for energies between 2.4 and 6.9 GeV +Experiment: MARKI +Collider: Spear +InspireID: 100733 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - https://doi.org/10.17182/hepdata.18759 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ and the hadronic cross section for energies between 2.4 and 6.9 GeV. + The charged hadron spectum at 3, 4.8 and 7.4 GeV is also measured. + The muonic cross sections is also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Schwitters:1975fv +BibTeX: '@inproceedings{Schwitters:1975fv, + author = "Schwitters, R.", + title = "{Hadron Production at SPEAR}", + booktitle = "{1975 International Symposium on Lepton and Photon + Interactions at High-Energies. Proceedings. Stanford + University, August 21-27, 1975}", + url = "http://www-public.slac.stanford.edu/sciDoc/docMeta.aspx?slacPubNumber=SLAC-PUB-1666", + year = "1975", + pages = "5", + reportNumber = "SLAC-PUB-1666", + SLACcitation = "%%CITATION = SLAC-PUB-1666;%%" +}' diff --git a/analyses/pluginSLAC/MARKI_1975_I100733.plot b/analyses/pluginSLAC/MARKI_1975_I100733.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1975_I100733.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /MARKI_1975_I100733/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKI_1975_I100733/d01-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/$nb +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKI_1975_I100733/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/$nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginSLAC/MARKI_1975_I100733.yoda b/analyses/pluginSLAC/MARKI_1975_I100733.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1975_I100733.yoda @@ -0,0 +1,299 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1975_I100733/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1975_I100733/d01-x01-y01 +Title: doi:10.17182/hepdata.70356.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.400000e+00 0.000000e+00 0.000000e+00 3.180000e+01 4.803374e+00 4.803374e+00 +2.600000e+00 0.000000e+00 0.000000e+00 3.240000e+01 5.384013e+00 5.384013e+00 +2.800000e+00 0.000000e+00 0.000000e+00 2.940000e+01 5.045156e+00 5.045156e+00 +3.000000e+00 0.000000e+00 0.000000e+00 2.320000e+01 2.998733e+00 2.998733e+00 +3.100000e+00 0.000000e+00 0.000000e+00 2.240000e+01 3.988433e+00 3.988433e+00 +3.200000e+00 0.000000e+00 0.000000e+00 2.130000e+01 3.062172e+00 3.062172e+00 +3.300000e+00 0.000000e+00 0.000000e+00 1.880000e+01 3.128003e+00 3.128003e+00 +3.400000e+00 0.000000e+00 0.000000e+00 1.860000e+01 2.957972e+00 2.957972e+00 +3.600000e+00 0.000000e+00 0.000000e+00 1.900000e+01 2.831960e+00 2.831960e+00 +3.800000e+00 0.000000e+00 0.000000e+00 1.960000e+01 2.530138e+00 2.530138e+00 +3.900000e+00 0.000000e+00 0.000000e+00 1.810000e+01 2.697425e+00 2.697425e+00 +3.920000e+00 0.000000e+00 0.000000e+00 1.960000e+01 3.500229e+00 3.500229e+00 +3.930000e+00 0.000000e+00 0.000000e+00 2.530000e+01 4.482287e+00 4.482287e+00 +4.450000e+00 0.000000e+00 0.000000e+00 1.850000e+01 3.272996e+00 3.272996e+00 +4.470000e+00 0.000000e+00 0.000000e+00 2.210000e+01 3.888972e+00 3.888972e+00 +4.490000e+00 0.000000e+00 0.000000e+00 1.830000e+01 2.785480e+00 2.785480e+00 +4.540000e+00 0.000000e+00 0.000000e+00 1.810000e+01 2.772382e+00 2.772382e+00 +4.590000e+00 0.000000e+00 0.000000e+00 1.670000e+01 2.455382e+00 2.455382e+00 +4.600000e+00 0.000000e+00 0.000000e+00 1.520000e+01 2.355929e+00 2.355929e+00 +4.640000e+00 0.000000e+00 0.000000e+00 1.660000e+01 3.255088e+00 3.255088e+00 +4.690000e+00 0.000000e+00 0.000000e+00 1.770000e+01 2.596709e+00 2.596709e+00 +4.790000e+00 0.000000e+00 0.000000e+00 1.740000e+01 2.576354e+00 2.576354e+00 +4.810000e+00 0.000000e+00 0.000000e+00 1.800000e+01 2.280351e+00 2.280351e+00 +4.890000e+00 0.000000e+00 0.000000e+00 1.600000e+01 2.408319e+00 2.408319e+00 +5.000000e+00 0.000000e+00 0.000000e+00 1.760000e+01 2.248911e+00 2.248911e+00 +5.100000e+00 0.000000e+00 0.000000e+00 1.740000e+01 2.650962e+00 2.650962e+00 +5.200000e+00 0.000000e+00 0.000000e+00 1.400000e+01 2.126029e+00 2.126029e+00 +5.300000e+00 0.000000e+00 0.000000e+00 1.490000e+01 2.260553e+00 2.260553e+00 +5.400000e+00 0.000000e+00 0.000000e+00 1.520000e+01 2.355929e+00 2.355929e+00 +5.500000e+00 0.000000e+00 0.000000e+00 1.260000e+01 1.958979e+00 1.958979e+00 +5.600000e+00 0.000000e+00 0.000000e+00 1.400000e+01 2.202272e+00 2.202272e+00 +5.700000e+00 0.000000e+00 0.000000e+00 1.400000e+01 2.126029e+00 2.126029e+00 +5.800000e+00 0.000000e+00 0.000000e+00 1.400000e+01 2.126029e+00 2.126029e+00 +5.900000e+00 0.000000e+00 0.000000e+00 1.230000e+01 1.939820e+00 1.939820e+00 +6.000000e+00 0.000000e+00 0.000000e+00 1.290000e+01 1.978408e+00 1.978408e+00 +6.100000e+00 0.000000e+00 0.000000e+00 1.250000e+01 1.803469e+00 1.803469e+00 +6.200000e+00 0.000000e+00 0.000000e+00 1.160000e+01 1.669012e+00 1.669012e+00 +6.250000e+00 0.000000e+00 0.000000e+00 1.150000e+01 1.735655e+00 1.735655e+00 +6.300000e+00 0.000000e+00 0.000000e+00 1.100000e+01 1.627882e+00 1.627882e+00 +6.350000e+00 0.000000e+00 0.000000e+00 1.150000e+01 1.735655e+00 1.735655e+00 +6.400000e+00 0.000000e+00 0.000000e+00 1.160000e+01 1.669012e+00 1.669012e+00 +6.450000e+00 0.000000e+00 0.000000e+00 1.090000e+01 1.621142e+00 1.621142e+00 +6.500000e+00 0.000000e+00 0.000000e+00 1.010000e+01 1.568471e+00 1.568471e+00 +6.550000e+00 0.000000e+00 0.000000e+00 1.030000e+01 1.581423e+00 1.581423e+00 +6.600000e+00 0.000000e+00 0.000000e+00 1.090000e+01 1.621142e+00 1.621142e+00 +6.650000e+00 0.000000e+00 0.000000e+00 9.800000e+00 1.549322e+00 1.549322e+00 +6.700000e+00 0.000000e+00 0.000000e+00 9.400000e+00 1.372443e+00 1.372443e+00 +6.750000e+00 0.000000e+00 0.000000e+00 1.150000e+01 1.811767e+00 1.811767e+00 +6.800000e+00 0.000000e+00 0.000000e+00 9.800000e+00 1.473228e+00 1.473228e+00 +6.850000e+00 0.000000e+00 0.000000e+00 9.500000e+00 1.379311e+00 1.379311e+00 +6.900000e+00 0.000000e+00 0.000000e+00 9.300000e+00 1.440451e+00 1.440451e+00 +6.950000e+00 0.000000e+00 0.000000e+00 9.300000e+00 1.440451e+00 1.440451e+00 +7.000000e+00 0.000000e+00 0.000000e+00 8.500000e+00 1.390144e+00 1.390144e+00 +7.050000e+00 0.000000e+00 0.000000e+00 8.400000e+00 1.305986e+00 1.305986e+00 +7.100000e+00 0.000000e+00 0.000000e+00 9.300000e+00 1.226744e+00 1.226744e+00 +7.100000e+00 0.000000e+00 0.000000e+00 8.700000e+00 1.325481e+00 1.325481e+00 +7.150000e+00 0.000000e+00 0.000000e+00 8.100000e+00 1.210826e+00 1.210826e+00 +7.200000e+00 0.000000e+00 0.000000e+00 8.100000e+00 1.210826e+00 1.210826e+00 +7.250000e+00 0.000000e+00 0.000000e+00 9.100000e+00 1.352072e+00 1.352072e+00 +7.300000e+00 0.000000e+00 0.000000e+00 7.600000e+00 1.177964e+00 1.177964e+00 +7.350000e+00 0.000000e+00 0.000000e+00 8.100000e+00 1.138464e+00 1.138464e+00 +7.400000e+00 0.000000e+00 0.000000e+00 8.100000e+00 1.138464e+00 1.138464e+00 +7.600000e+00 0.000000e+00 0.000000e+00 8.000000e+00 1.442221e+00 1.442221e+00 +7.800000e+00 0.000000e+00 0.000000e+00 7.600000e+00 1.103449e+00 1.103449e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1975_I100733/d02-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1975_I100733/d02-x01-y01 +Title: doi:10.17182/hepdata.70356.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.400000e+00 0.000000e+00 0.000000e+00 2.090000e+00 3.182468e-01 3.182468e-01 +2.600000e+00 0.000000e+00 0.000000e+00 2.530000e+00 4.158233e-01 4.158233e-01 +2.800000e+00 0.000000e+00 0.000000e+00 2.650000e+00 4.390046e-01 4.390046e-01 +3.000000e+00 0.000000e+00 0.000000e+00 2.420000e+00 3.204122e-01 3.204122e-01 +3.100000e+00 0.000000e+00 0.000000e+00 2.500000e+00 4.465423e-01 4.465423e-01 +3.200000e+00 0.000000e+00 0.000000e+00 2.530000e+00 3.700122e-01 3.700122e-01 +3.300000e+00 0.000000e+00 0.000000e+00 2.380000e+00 3.988032e-01 3.988032e-01 +3.400000e+00 0.000000e+00 0.000000e+00 2.490000e+00 3.976192e-01 3.976192e-01 +3.600000e+00 0.000000e+00 0.000000e+00 2.870000e+00 4.449371e-01 4.449371e-01 +3.800000e+00 0.000000e+00 0.000000e+00 3.380000e+00 4.389123e-01 4.389123e-01 +3.890000e+00 0.000000e+00 0.000000e+00 3.190000e+00 3.614706e-01 3.614706e-01 +3.900000e+00 0.000000e+00 0.000000e+00 3.500000e+00 4.482187e-01 4.482187e-01 +3.910000e+00 0.000000e+00 0.000000e+00 3.500000e+00 4.301163e-01 4.301163e-01 +3.920000e+00 0.000000e+00 0.000000e+00 4.080000e+00 5.064227e-01 5.064227e-01 +3.925000e+00 0.000000e+00 0.000000e+00 4.630000e+00 6.053668e-01 6.053668e-01 +3.935000e+00 0.000000e+00 0.000000e+00 3.790000e+00 5.366945e-01 5.366945e-01 +3.940000e+00 0.000000e+00 0.000000e+00 4.610000e+00 6.655231e-01 6.655231e-01 +3.955000e+00 0.000000e+00 0.000000e+00 4.580000e+00 6.015513e-01 6.015513e-01 +3.960000e+00 0.000000e+00 0.000000e+00 4.900000e+00 6.859300e-01 6.859300e-01 +3.975000e+00 0.000000e+00 0.000000e+00 4.700000e+00 5.522681e-01 5.522681e-01 +3.980000e+00 0.000000e+00 0.000000e+00 4.500000e+00 4.924429e-01 4.924429e-01 +3.990000e+00 0.000000e+00 0.000000e+00 4.220000e+00 4.806079e-01 4.806079e-01 +4.000000e+00 0.000000e+00 0.000000e+00 4.200000e+00 6.303174e-01 6.303174e-01 +4.015000e+00 0.000000e+00 0.000000e+00 5.380000e+00 6.065014e-01 6.065014e-01 +4.020000e+00 0.000000e+00 0.000000e+00 6.510000e+00 7.588814e-01 7.588814e-01 +4.030000e+00 0.000000e+00 0.000000e+00 6.180000e+00 7.825113e-01 7.825113e-01 +4.035000e+00 0.000000e+00 0.000000e+00 5.520000e+00 6.701522e-01 6.701522e-01 +4.045000e+00 0.000000e+00 0.000000e+00 5.690000e+00 8.196713e-01 8.196713e-01 +4.060000e+00 0.000000e+00 0.000000e+00 5.290000e+00 6.131403e-01 6.131403e-01 +4.065000e+00 0.000000e+00 0.000000e+00 5.790000e+00 8.779755e-01 8.779755e-01 +4.075000e+00 0.000000e+00 0.000000e+00 5.000000e+00 7.733693e-01 7.733693e-01 +4.085000e+00 0.000000e+00 0.000000e+00 5.370000e+00 6.103024e-01 6.103024e-01 +4.105000e+00 0.000000e+00 0.000000e+00 6.190000e+00 7.772136e-01 7.772136e-01 +4.115000e+00 0.000000e+00 0.000000e+00 6.010000e+00 6.509232e-01 6.509232e-01 +4.120000e+00 0.000000e+00 0.000000e+00 5.370000e+00 7.831149e-01 7.831149e-01 +4.130000e+00 0.000000e+00 0.000000e+00 5.580000e+00 5.927596e-01 5.927596e-01 +4.145000e+00 0.000000e+00 0.000000e+00 5.580000e+00 8.048379e-01 8.048379e-01 +4.160000e+00 0.000000e+00 0.000000e+00 5.200000e+00 8.168843e-01 8.168843e-01 +4.190000e+00 0.000000e+00 0.000000e+00 4.790000e+00 5.153067e-01 5.153067e-01 +4.200000e+00 0.000000e+00 0.000000e+00 5.120000e+00 8.195999e-01 8.195999e-01 +4.215000e+00 0.000000e+00 0.000000e+00 4.790000e+00 7.599612e-01 7.599612e-01 +4.250000e+00 0.000000e+00 0.000000e+00 4.030000e+00 7.311012e-01 7.311012e-01 +4.260000e+00 0.000000e+00 0.000000e+00 5.390000e+00 7.844877e-01 7.844877e-01 +4.285000e+00 0.000000e+00 0.000000e+00 4.100000e+00 4.518849e-01 4.518849e-01 +4.305000e+00 0.000000e+00 0.000000e+00 4.260000e+00 6.492888e-01 6.492888e-01 +4.325000e+00 0.000000e+00 0.000000e+00 3.710000e+00 6.146064e-01 6.146064e-01 +4.335000e+00 0.000000e+00 0.000000e+00 4.430000e+00 7.378001e-01 7.378001e-01 +4.340000e+00 0.000000e+00 0.000000e+00 4.710000e+00 7.471553e-01 7.471553e-01 +4.350000e+00 0.000000e+00 0.000000e+00 4.820000e+00 7.618556e-01 7.618556e-01 +4.365000e+00 0.000000e+00 0.000000e+00 4.700000e+00 6.646804e-01 6.646804e-01 +4.370000e+00 0.000000e+00 0.000000e+00 4.940000e+00 6.232463e-01 6.232463e-01 +4.385000e+00 0.000000e+00 0.000000e+00 4.900000e+00 5.547071e-01 5.547071e-01 +4.390000e+00 0.000000e+00 0.000000e+00 4.200000e+00 5.103920e-01 5.103920e-01 +4.400000e+00 0.000000e+00 0.000000e+00 5.900000e+00 8.927486e-01 8.927486e-01 +4.405000e+00 0.000000e+00 0.000000e+00 5.740000e+00 6.386517e-01 6.386517e-01 +4.410000e+00 0.000000e+00 0.000000e+00 5.800000e+00 6.933974e-01 6.933974e-01 +4.415000e+00 0.000000e+00 0.000000e+00 6.180000e+00 7.704051e-01 7.704051e-01 +4.420000e+00 0.000000e+00 0.000000e+00 5.740000e+00 7.172001e-01 7.172001e-01 +4.425000e+00 0.000000e+00 0.000000e+00 5.530000e+00 7.257472e-01 7.257472e-01 +4.430000e+00 0.000000e+00 0.000000e+00 5.840000e+00 6.860437e-01 6.860437e-01 +4.440000e+00 0.000000e+00 0.000000e+00 5.130000e+00 5.892953e-01 5.892953e-01 +4.445000e+00 0.000000e+00 0.000000e+00 4.600000e+00 5.780138e-01 5.780138e-01 +4.465000e+00 0.000000e+00 0.000000e+00 5.110000e+00 7.010856e-01 7.010856e-01 +4.470000e+00 0.000000e+00 0.000000e+00 5.010000e+00 6.111473e-01 6.111473e-01 +4.485000e+00 0.000000e+00 0.000000e+00 4.340000e+00 5.164843e-01 5.164843e-01 +4.500000e+00 0.000000e+00 0.000000e+00 4.310000e+00 6.601220e-01 6.601220e-01 +4.510000e+00 0.000000e+00 0.000000e+00 4.630000e+00 5.571975e-01 5.571975e-01 +4.535000e+00 0.000000e+00 0.000000e+00 4.400000e+00 5.325411e-01 5.325411e-01 +4.550000e+00 0.000000e+00 0.000000e+00 4.390000e+00 6.805299e-01 6.805299e-01 +4.600000e+00 0.000000e+00 0.000000e+00 4.110000e+00 6.168638e-01 6.168638e-01 +4.620000e+00 0.000000e+00 0.000000e+00 3.720000e+00 5.915945e-01 5.915945e-01 +4.650000e+00 0.000000e+00 0.000000e+00 4.190000e+00 8.244156e-01 8.244156e-01 +4.700000e+00 0.000000e+00 0.000000e+00 4.560000e+00 6.916184e-01 6.916184e-01 +4.800000e+00 0.000000e+00 0.000000e+00 4.630000e+00 7.037535e-01 7.037535e-01 +4.820000e+00 0.000000e+00 0.000000e+00 4.850000e+00 6.223544e-01 6.223544e-01 +4.900000e+00 0.000000e+00 0.000000e+00 4.470000e+00 6.706780e-01 6.706780e-01 +5.000000e+00 0.000000e+00 0.000000e+00 5.130000e+00 6.630000e-01 6.630000e-01 +5.100000e+00 0.000000e+00 0.000000e+00 5.280000e+00 8.143611e-01 8.143611e-01 +5.200000e+00 0.000000e+00 0.000000e+00 4.400000e+00 6.965630e-01 6.965630e-01 +5.300000e+00 0.000000e+00 0.000000e+00 4.840000e+00 7.554178e-01 7.554178e-01 +5.400000e+00 0.000000e+00 0.000000e+00 5.140000e+00 8.053546e-01 8.053546e-01 +5.500000e+00 0.000000e+00 0.000000e+00 4.460000e+00 6.850664e-01 6.850664e-01 +5.600000e+00 0.000000e+00 0.000000e+00 5.150000e+00 8.137106e-01 8.137106e-01 +5.700000e+00 0.000000e+00 0.000000e+00 5.340000e+00 8.182640e-01 8.182640e-01 +5.800000e+00 0.000000e+00 0.000000e+00 5.470000e+00 8.649329e-01 8.649329e-01 +5.900000e+00 0.000000e+00 0.000000e+00 5.010000e+00 7.664209e-01 7.664209e-01 +6.000000e+00 0.000000e+00 0.000000e+00 5.420000e+00 8.235071e-01 8.235071e-01 +6.100000e+00 0.000000e+00 0.000000e+00 5.370000e+00 7.904233e-01 7.904233e-01 +6.200000e+00 0.000000e+00 0.000000e+00 5.270000e+00 7.403573e-01 7.403573e-01 +6.250000e+00 0.000000e+00 0.000000e+00 5.170000e+00 8.072726e-01 8.072726e-01 +6.300000e+00 0.000000e+00 0.000000e+00 5.130000e+00 7.818369e-01 7.818369e-01 +6.350000e+00 0.000000e+00 0.000000e+00 5.360000e+00 8.348030e-01 8.348030e-01 +6.400000e+00 0.000000e+00 0.000000e+00 5.540000e+00 8.240243e-01 8.240243e-01 +6.450000e+00 0.000000e+00 0.000000e+00 5.290000e+00 8.074286e-01 8.074286e-01 +6.500000e+00 0.000000e+00 0.000000e+00 4.970000e+00 7.791078e-01 7.791078e-01 +6.550000e+00 0.000000e+00 0.000000e+00 5.110000e+00 8.111849e-01 8.111849e-01 +6.600000e+00 0.000000e+00 0.000000e+00 5.550000e+00 8.547076e-01 8.547076e-01 +6.650000e+00 0.000000e+00 0.000000e+00 5.060000e+00 7.848796e-01 7.848796e-01 +6.700000e+00 0.000000e+00 0.000000e+00 4.920000e+00 7.836862e-01 7.836862e-01 +6.750000e+00 0.000000e+00 0.000000e+00 6.100000e+00 9.436631e-01 9.436631e-01 +6.800000e+00 0.000000e+00 0.000000e+00 5.280000e+00 7.917601e-01 7.917601e-01 +6.850000e+00 0.000000e+00 0.000000e+00 5.200000e+00 7.789737e-01 7.789737e-01 +6.900000e+00 0.000000e+00 0.000000e+00 5.110000e+00 7.957518e-01 7.957518e-01 +6.950000e+00 0.000000e+00 0.000000e+00 5.240000e+00 8.505739e-01 8.505739e-01 +7.000000e+00 0.000000e+00 0.000000e+00 4.840000e+00 7.477673e-01 7.477673e-01 +7.040000e+00 0.000000e+00 0.000000e+00 4.780000e+00 7.438978e-01 7.438978e-01 +7.070000e+00 0.000000e+00 0.000000e+00 5.380000e+00 7.765591e-01 7.765591e-01 +7.100000e+00 0.000000e+00 0.000000e+00 5.140000e+00 7.976816e-01 7.976816e-01 +7.150000e+00 0.000000e+00 0.000000e+00 4.820000e+00 7.388667e-01 7.388667e-01 +7.200000e+00 0.000000e+00 0.000000e+00 4.870000e+00 7.346217e-01 7.346217e-01 +7.250000e+00 0.000000e+00 0.000000e+00 5.550000e+00 8.623369e-01 8.623369e-01 +7.300000e+00 0.000000e+00 0.000000e+00 4.670000e+00 7.368779e-01 7.368779e-01 +7.350000e+00 0.000000e+00 0.000000e+00 5.050000e+00 7.466760e-01 7.466760e-01 +7.400000e+00 0.000000e+00 0.000000e+00 5.200000e+00 7.144928e-01 7.144928e-01 +7.600000e+00 0.000000e+00 0.000000e+00 5.380000e+00 8.592695e-01 8.592695e-01 +7.800000e+00 0.000000e+00 0.000000e+00 5.370000e+00 7.904233e-01 7.904233e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1975_I100733/d03-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1975_I100733/d03-x01-y01 +Title: doi:10.17182/hepdata.70356.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.000000e+00 0.000000e+00 0.000000e+00 9.000000e-01 2.247221e-01 2.247221e-01 +0.000000e+00 0.000000e+00 0.000000e+00 1.280000e+00 3.031831e-01 3.031831e-01 +1.100000e-01 0.000000e+00 0.000000e+00 1.680000e+00 3.914333e-01 3.914333e-01 +1.300000e-01 0.000000e+00 0.000000e+00 1.980000e+00 4.587156e-01 4.587156e-01 +1.500000e-01 0.000000e+00 0.000000e+00 2.140000e+00 5.186328e-01 5.186328e-01 +1.700000e-01 0.000000e+00 0.000000e+00 2.290000e+00 5.335775e-01 5.335775e-01 +1.900000e-01 0.000000e+00 0.000000e+00 2.280000e+00 5.314320e-01 5.314320e-01 +2.100000e-01 0.000000e+00 0.000000e+00 2.490000e+00 5.766325e-01 5.766325e-01 +2.300000e-01 0.000000e+00 0.000000e+00 2.100000e+00 4.929503e-01 4.929503e-01 +2.500000e-01 0.000000e+00 0.000000e+00 2.100000e+00 4.929503e-01 4.929503e-01 +2.700000e-01 0.000000e+00 0.000000e+00 1.980000e+00 4.643490e-01 4.643490e-01 +2.900000e-01 0.000000e+00 0.000000e+00 1.900000e+00 4.442972e-01 4.442972e-01 +3.100000e-01 0.000000e+00 0.000000e+00 1.840000e+00 4.346033e-01 4.346033e-01 +3.300000e-01 0.000000e+00 0.000000e+00 1.680000e+00 3.943602e-01 3.943602e-01 +3.500000e-01 0.000000e+00 0.000000e+00 1.540000e+00 3.585805e-01 3.585805e-01 +3.700000e-01 0.000000e+00 0.000000e+00 1.340000e+00 3.158797e-01 3.158797e-01 +3.900000e-01 0.000000e+00 0.000000e+00 1.160000e+00 2.779928e-01 2.779928e-01 +4.100000e-01 0.000000e+00 0.000000e+00 1.060000e+00 2.572547e-01 2.572547e-01 +4.500000e-01 0.000000e+00 0.000000e+00 7.900000e-01 2.029901e-01 2.029901e-01 +4.900000e-01 0.000000e+00 0.000000e+00 8.400000e-01 1.971801e-01 1.971801e-01 +5.300000e-01 0.000000e+00 0.000000e+00 5.600000e-01 1.348332e-01 1.348332e-01 +5.900000e-01 0.000000e+00 0.000000e+00 4.200000e-01 1.063955e-01 1.063955e-01 +6.700000e-01 0.000000e+00 0.000000e+00 3.300000e-01 7.965551e-02 7.965551e-02 +7.500000e-01 0.000000e+00 0.000000e+00 3.000000e-01 7.348469e-02 7.348469e-02 +8.400000e-01 0.000000e+00 0.000000e+00 1.900000e-01 5.200961e-02 5.200961e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1975_I100733/d03-x01-y02 +IsRef: 1 +Path: /REF/MARKI_1975_I100733/d03-x01-y02 +Title: doi:10.17182/hepdata.70356.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.000000e+00 0.000000e+00 0.000000e+00 3.800000e+00 8.497058e-01 8.497058e-01 +0.000000e+00 0.000000e+00 0.000000e+00 4.200000e+00 9.391486e-01 9.391486e-01 +0.000000e+00 0.000000e+00 0.000000e+00 5.540000e+00 1.238782e+00 1.238782e+00 +0.000000e+00 0.000000e+00 0.000000e+00 6.670000e+00 1.491457e+00 1.491457e+00 +1.100000e-01 0.000000e+00 0.000000e+00 7.380000e+00 1.650218e+00 1.650218e+00 +1.300000e-01 0.000000e+00 0.000000e+00 7.410000e+00 1.656926e+00 1.656926e+00 +1.500000e-01 0.000000e+00 0.000000e+00 7.180000e+00 1.605497e+00 1.605497e+00 +1.700000e-01 0.000000e+00 0.000000e+00 6.490000e+00 1.451208e+00 1.451208e+00 +1.900000e-01 0.000000e+00 0.000000e+00 6.080000e+00 1.359529e+00 1.359529e+00 +2.100000e-01 0.000000e+00 0.000000e+00 5.440000e+00 1.216421e+00 1.216421e+00 +2.300000e-01 0.000000e+00 0.000000e+00 4.730000e+00 1.057660e+00 1.057660e+00 +2.500000e-01 0.000000e+00 0.000000e+00 3.970000e+00 8.877190e-01 8.877190e-01 +2.700000e-01 0.000000e+00 0.000000e+00 3.840000e+00 8.586501e-01 8.586501e-01 +2.900000e-01 0.000000e+00 0.000000e+00 3.270000e+00 7.311942e-01 7.311942e-01 +3.100000e-01 0.000000e+00 0.000000e+00 2.900000e+00 6.484597e-01 6.484597e-01 +3.300000e-01 0.000000e+00 0.000000e+00 2.500000e+00 5.590170e-01 5.590170e-01 +3.500000e-01 0.000000e+00 0.000000e+00 2.330000e+00 5.210038e-01 5.210038e-01 +3.700000e-01 0.000000e+00 0.000000e+00 1.740000e+00 3.890758e-01 3.890758e-01 +3.900000e-01 0.000000e+00 0.000000e+00 1.490000e+00 3.331741e-01 3.331741e-01 +4.100000e-01 0.000000e+00 0.000000e+00 1.270000e+00 2.839806e-01 2.839806e-01 +4.500000e-01 0.000000e+00 0.000000e+00 1.030000e+00 2.303150e-01 2.303150e-01 +4.900000e-01 0.000000e+00 0.000000e+00 7.200000e-01 1.609969e-01 1.609969e-01 +5.300000e-01 0.000000e+00 0.000000e+00 5.200000e-01 1.162755e-01 1.162755e-01 +5.900000e-01 0.000000e+00 0.000000e+00 4.500000e-01 1.006231e-01 1.006231e-01 +6.700000e-01 0.000000e+00 0.000000e+00 2.700000e-01 6.037384e-02 6.037384e-02 +7.500000e-01 0.000000e+00 0.000000e+00 1.900000e-01 4.248529e-02 4.248529e-02 +8.400000e-01 0.000000e+00 0.000000e+00 1.700000e-01 3.801316e-02 3.801316e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1975_I100733/d03-x01-y03 +IsRef: 1 +Path: /REF/MARKI_1975_I100733/d03-x01-y03 +Title: doi:10.17182/hepdata.70356.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +0.000000e+00 0.000000e+00 0.000000e+00 1.310000e+01 2.929249e+00 2.929249e+00 +0.000000e+00 0.000000e+00 0.000000e+00 1.410000e+01 3.152856e+00 3.152856e+00 +0.000000e+00 0.000000e+00 0.000000e+00 1.480000e+01 3.309381e+00 3.309381e+00 +0.000000e+00 0.000000e+00 0.000000e+00 1.400000e+01 3.130495e+00 3.130495e+00 +1.100000e-01 0.000000e+00 0.000000e+00 1.300000e+01 2.906888e+00 2.906888e+00 +1.300000e-01 0.000000e+00 0.000000e+00 1.120000e+01 2.504396e+00 2.504396e+00 +1.500000e-01 0.000000e+00 0.000000e+00 1.000000e+01 2.236068e+00 2.236068e+00 +1.700000e-01 0.000000e+00 0.000000e+00 8.100000e+00 1.811215e+00 1.811215e+00 +1.900000e-01 0.000000e+00 0.000000e+00 7.000000e+00 1.565248e+00 1.565248e+00 +2.100000e-01 0.000000e+00 0.000000e+00 5.800000e+00 1.296919e+00 1.296919e+00 +2.300000e-01 0.000000e+00 0.000000e+00 4.800000e+00 1.073313e+00 1.073313e+00 +2.500000e-01 0.000000e+00 0.000000e+00 4.200000e+00 9.391486e-01 9.391486e-01 +2.700000e-01 0.000000e+00 0.000000e+00 3.300000e+00 7.379024e-01 7.379024e-01 +2.900000e-01 0.000000e+00 0.000000e+00 3.200000e+00 7.155418e-01 7.155418e-01 +3.100000e-01 0.000000e+00 0.000000e+00 2.700000e+00 6.037384e-01 6.037384e-01 +3.300000e-01 0.000000e+00 0.000000e+00 2.200000e+00 4.919350e-01 4.919350e-01 +3.500000e-01 0.000000e+00 0.000000e+00 2.000000e+00 4.472136e-01 4.472136e-01 +3.700000e-01 0.000000e+00 0.000000e+00 1.700000e+00 3.801316e-01 3.801316e-01 +3.900000e-01 0.000000e+00 0.000000e+00 1.400000e+00 3.130495e-01 3.130495e-01 +4.100000e-01 0.000000e+00 0.000000e+00 1.200000e+00 2.683282e-01 2.683282e-01 +4.500000e-01 0.000000e+00 0.000000e+00 1.030000e+00 2.407177e-01 2.407177e-01 +4.900000e-01 0.000000e+00 0.000000e+00 7.500000e-01 1.750000e-01 1.750000e-01 +5.300000e-01 0.000000e+00 0.000000e+00 6.700000e-01 1.579399e-01 1.579399e-01 +5.900000e-01 0.000000e+00 0.000000e+00 4.500000e-01 1.082820e-01 1.082820e-01 +6.700000e-01 0.000000e+00 0.000000e+00 3.100000e-01 7.553145e-02 7.553145e-02 +7.500000e-01 0.000000e+00 0.000000e+00 2.000000e-01 5.385165e-02 5.385165e-02 +8.400000e-01 0.000000e+00 0.000000e+00 1.000000e-01 3.000000e-02 3.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginSLAC/MARKI_1976_I108144.cc b/analyses/pluginSLAC/MARKI_1976_I108144.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1976_I108144.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKI_1976_I108144 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKI_1976_I108144); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKI_1976_I108144); + + +} diff --git a/analyses/pluginSLAC/MARKI_1976_I108144.info b/analyses/pluginSLAC/MARKI_1976_I108144.info new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1976_I108144.info @@ -0,0 +1,31 @@ +Name: MARKI_1976_I108144 +Year: 1976 +Summary: Measurement of $R$ between 3.888 and 4.586 GeV +Experiment: MARKI +Collider: Spear +InspireID: 108144 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 36 (1976) 700, 1976 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by MARKI for energies between 3.888 and 4.586 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Siegrist:1976br +BibTeX: '@article{Siegrist:1976br, + author = "Siegrist, J. and others", + title = "{Observation of a Resonance at 4.4-GeV and Additional + Structure Near 4.1-GeV in e+ e- Annihilation}", + journal = "Phys. Rev. Lett.", + volume = "36", + year = "1976", + pages = "700", + doi = "10.1103/PhysRevLett.36.700", + reportNumber = "SLAC-PUB-1717, LBL-4804", + SLACcitation = "%%CITATION = PRLTA,36,700;%%" +}' diff --git a/analyses/pluginSLAC/MARKI_1976_I108144.plot b/analyses/pluginSLAC/MARKI_1976_I108144.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1976_I108144.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /MARKI_1976_I108144/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKI_1976_I108144/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKI_1976_I108144/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginSLAC/MARKI_1976_I108144.yoda b/analyses/pluginSLAC/MARKI_1976_I108144.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1976_I108144.yoda @@ -0,0 +1,67 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1976_I108144/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1976_I108144/d01-x01-y01 +Title: doi:10.17182/hepdata.21093.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.888000e+00 0.000000e+00 0.000000e+00 3.180000e+00 5.063882e-01 5.063882e-01 +3.899000e+00 0.000000e+00 0.000000e+00 3.474000e+00 6.012863e-01 6.012863e-01 +3.908000e+00 0.000000e+00 0.000000e+00 3.470000e+00 6.386081e-01 6.386081e-01 +3.919000e+00 0.000000e+00 0.000000e+00 4.006000e+00 6.672187e-01 6.672187e-01 +3.926000e+00 0.000000e+00 0.000000e+00 4.560000e+00 8.299132e-01 8.299132e-01 +3.938600e+00 0.000000e+00 0.000000e+00 3.800000e+00 6.527051e-01 6.527051e-01 +3.946000e+00 0.000000e+00 0.000000e+00 4.580000e+00 8.323875e-01 8.323875e-01 +3.958600e+00 0.000000e+00 0.000000e+00 4.537000e+00 7.634555e-01 7.634555e-01 +3.966000e+00 0.000000e+00 0.000000e+00 4.850000e+00 8.884572e-01 8.884572e-01 +3.978200e+00 0.000000e+00 0.000000e+00 4.685000e+00 7.772268e-01 7.772268e-01 +3.986000e+00 0.000000e+00 0.000000e+00 4.450000e+00 6.913438e-01 6.913438e-01 +3.997400e+00 0.000000e+00 0.000000e+00 4.165000e+00 6.805972e-01 6.805972e-01 +4.006000e+00 0.000000e+00 0.000000e+00 4.140000e+00 7.669035e-01 7.669035e-01 +4.017800e+00 0.000000e+00 0.000000e+00 5.390000e+00 8.546352e-01 8.546352e-01 +4.024000e+00 0.000000e+00 0.000000e+00 6.190000e+00 1.084303e+00 1.084303e+00 +4.028600e+00 0.000000e+00 0.000000e+00 6.670000e+00 1.214793e+00 1.214793e+00 +4.037000e+00 0.000000e+00 0.000000e+00 6.160000e+00 1.020849e+00 1.020849e+00 +4.038000e+00 0.000000e+00 0.000000e+00 5.510000e+00 8.899451e-01 8.899451e-01 +4.046000e+00 0.000000e+00 0.000000e+00 5.710000e+00 1.045750e+00 1.045750e+00 +4.057000e+00 0.000000e+00 0.000000e+00 5.264000e+00 9.405260e-01 9.405260e-01 +4.066000e+00 0.000000e+00 0.000000e+00 5.810000e+00 1.093212e+00 1.093212e+00 +4.076200e+00 0.000000e+00 0.000000e+00 5.007000e+00 9.356496e-01 9.356496e-01 +4.086000e+00 0.000000e+00 0.000000e+00 5.450000e+00 8.492386e-01 8.492386e-01 +4.106000e+00 0.000000e+00 0.000000e+00 6.140000e+00 1.133067e+00 1.133067e+00 +4.112000e+00 0.000000e+00 0.000000e+00 6.000000e+00 9.585927e-01 9.585927e-01 +4.126000e+00 0.000000e+00 0.000000e+00 5.400000e+00 9.962429e-01 9.962429e-01 +4.136000e+00 0.000000e+00 0.000000e+00 5.620000e+00 8.562412e-01 8.562412e-01 +4.146000e+00 0.000000e+00 0.000000e+00 5.630000e+00 1.053603e+00 1.053603e+00 +4.164000e+00 0.000000e+00 0.000000e+00 5.190000e+00 9.828847e-01 9.828847e-01 +4.186000e+00 0.000000e+00 0.000000e+00 4.740000e+00 7.334310e-01 7.334310e-01 +4.206000e+00 0.000000e+00 0.000000e+00 5.100000e+00 9.480638e-01 9.480638e-01 +4.226000e+00 0.000000e+00 0.000000e+00 4.720000e+00 8.844004e-01 8.844004e-01 +4.244000e+00 0.000000e+00 0.000000e+00 3.940000e+00 8.073295e-01 8.073295e-01 +4.264000e+00 0.000000e+00 0.000000e+00 5.350000e+00 1.026453e+00 1.026453e+00 +4.284000e+00 0.000000e+00 0.000000e+00 4.060000e+00 6.296674e-01 6.296674e-01 +4.302000e+00 0.000000e+00 0.000000e+00 4.340000e+00 8.522329e-01 8.522329e-01 +4.326000e+00 0.000000e+00 0.000000e+00 3.630000e+00 7.063853e-01 7.063853e-01 +4.331800e+00 0.000000e+00 0.000000e+00 4.416000e+00 7.404963e-01 7.404963e-01 +4.346000e+00 0.000000e+00 0.000000e+00 4.690000e+00 8.929794e-01 8.929794e-01 +4.350800e+00 0.000000e+00 0.000000e+00 4.755000e+00 9.250117e-01 9.250117e-01 +4.366000e+00 0.000000e+00 0.000000e+00 4.690000e+00 8.573286e-01 8.573286e-01 +4.371000e+00 0.000000e+00 0.000000e+00 4.957000e+00 8.680844e-01 8.680844e-01 +4.384000e+00 0.000000e+00 0.000000e+00 4.910000e+00 7.686561e-01 7.686561e-01 +4.390400e+00 0.000000e+00 0.000000e+00 4.191000e+00 7.049552e-01 7.049552e-01 +4.404200e+00 0.000000e+00 0.000000e+00 5.681000e+00 9.204692e-01 9.204692e-01 +4.406000e+00 0.000000e+00 0.000000e+00 5.960000e+00 1.044431e+00 1.044431e+00 +4.414000e+00 0.000000e+00 0.000000e+00 5.920000e+00 9.329201e-01 9.329201e-01 +4.419600e+00 0.000000e+00 0.000000e+00 5.683000e+00 9.852446e-01 9.852446e-01 +4.426000e+00 0.000000e+00 0.000000e+00 5.520000e+00 9.724629e-01 9.724629e-01 +4.429200e+00 0.000000e+00 0.000000e+00 5.765000e+00 9.321462e-01 9.321462e-01 +4.438000e+00 0.000000e+00 0.000000e+00 5.110000e+00 8.306156e-01 8.306156e-01 +4.444000e+00 0.000000e+00 0.000000e+00 4.290000e+00 7.739459e-01 7.739459e-01 +4.449400e+00 0.000000e+00 0.000000e+00 4.739000e+00 8.622365e-01 8.622365e-01 +4.464000e+00 0.000000e+00 0.000000e+00 5.160000e+00 9.269175e-01 9.269175e-01 +4.468600e+00 0.000000e+00 0.000000e+00 5.004000e+00 8.514719e-01 8.514719e-01 +4.484000e+00 0.000000e+00 0.000000e+00 4.310000e+00 6.829072e-01 6.829072e-01 +4.512600e+00 0.000000e+00 0.000000e+00 4.586000e+00 7.492766e-01 7.492766e-01 +4.536000e+00 0.000000e+00 0.000000e+00 4.370000e+00 7.051810e-01 7.051810e-01 +4.586000e+00 0.000000e+00 0.000000e+00 4.080000e+00 6.438509e-01 6.438509e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginSLAC/MARKI_1977_I119979.cc b/analyses/pluginSLAC/MARKI_1977_I119979.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1977_I119979.cc @@ -0,0 +1,101 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKI_1977_I119979 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKI_1977_I119979); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + declare(FinalState(), "FS"); + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + // R + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /nanobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("simga_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult1 = bookScatter2D(1,1,1); + Scatter2DPtr mult2 = bookScatter2D(2,1,1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult1 ->addPoint(x, rval, ex, rerr); + mult2 ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult1 ->addPoint(x, 0., ex, make_pair(0.,.0)); + mult2 ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKI_1977_I119979); + + +} diff --git a/analyses/pluginSLAC/MARKI_1977_I119979.info b/analyses/pluginSLAC/MARKI_1977_I119979.info new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1977_I119979.info @@ -0,0 +1,33 @@ +Name: MARKI_1977_I119979 +Year: 1977 +Summary: Measurement of $R$ for energies between 3.598 and 3.886 GeV +Experiment: MARKI +Collider: Spear +InspireID: 119979 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev.Lett. 39 (1977) 526, 1977 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ and the hadronic cross section for energies between 3.598 and 3.886 GeV. + The hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Rapidis:1977cv +BibTeX: '@article{Rapidis:1977cv, + author = "Rapidis, Petros A. and others", + title = "{Observation of a Resonance in e+ e- Annihilation Just + Above Charm Threshold}", + journal = "Phys. Rev. Lett.", + volume = "39", + year = "1977", + pages = "526", + doi = "10.1103/PhysRevLett.39.526, 10.1103/PhysRevLett.39.974", + note = "[Erratum: Phys. Rev. Lett.39,974(1977)]", + reportNumber = "SLAC-PUB-1959, LBL-6484", + SLACcitation = "%%CITATION = PRLTA,39,526;%%" +}' diff --git a/analyses/pluginSLAC/MARKI_1977_I119979.plot b/analyses/pluginSLAC/MARKI_1977_I119979.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1977_I119979.plot @@ -0,0 +1,30 @@ +BEGIN PLOT /MARKI_1977_I119979/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /MARKI_1977_I119979/d02-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ including radiative cross sections +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /MARKI_1977_I119979/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/$nb +LogY=0 +ConnectGaps=1 +END PLOT + +BEGIN PLOT /MARKI_1977_I119979/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/$nb +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginSLAC/MARKI_1977_I119979.yoda b/analyses/pluginSLAC/MARKI_1977_I119979.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1977_I119979.yoda @@ -0,0 +1,58 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1977_I119979/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1977_I119979/d01-x01-y01 +Title: doi:10.17182/hepdata.20971.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.598000e+00 0.000000e+00 0.000000e+00 2.860000e+00 4.614553e-01 4.614553e-01 +3.692000e+00 0.000000e+00 0.000000e+00 8.570000e+00 1.329703e+00 1.329703e+00 +3.710000e+00 0.000000e+00 0.000000e+00 4.720000e+00 7.897873e-01 7.897873e-01 +3.730000e+00 0.000000e+00 0.000000e+00 3.920000e+00 6.179353e-01 6.179353e-01 +3.740000e+00 0.000000e+00 0.000000e+00 4.070000e+00 6.393827e-01 6.393827e-01 +3.750000e+00 0.000000e+00 0.000000e+00 4.260000e+00 6.666491e-01 6.666491e-01 +3.762000e+00 0.000000e+00 0.000000e+00 4.620000e+00 7.212829e-01 7.212829e-01 +3.766000e+00 0.000000e+00 0.000000e+00 4.950000e+00 7.744070e-01 7.744070e-01 +3.770000e+00 0.000000e+00 0.000000e+00 4.890000e+00 7.629694e-01 7.629694e-01 +3.774000e+00 0.000000e+00 0.000000e+00 5.080000e+00 7.713910e-01 7.713910e-01 +3.780000e+00 0.000000e+00 0.000000e+00 4.840000e+00 7.557619e-01 7.557619e-01 +3.786000e+00 0.000000e+00 0.000000e+00 4.170000e+00 6.566965e-01 6.566965e-01 +3.790000e+00 0.000000e+00 0.000000e+00 4.060000e+00 6.379506e-01 6.379506e-01 +3.800000e+00 0.000000e+00 0.000000e+00 3.950000e+00 6.192384e-01 6.192384e-01 +3.810000e+00 0.000000e+00 0.000000e+00 3.680000e+00 5.775846e-01 5.775846e-01 +3.821000e+00 0.000000e+00 0.000000e+00 3.570000e+00 5.618365e-01 5.618365e-01 +3.830000e+00 0.000000e+00 0.000000e+00 3.450000e+00 5.447075e-01 5.447075e-01 +3.850000e+00 0.000000e+00 0.000000e+00 3.430000e+00 5.450782e-01 5.450782e-01 +3.865000e+00 0.000000e+00 0.000000e+00 3.810000e+00 6.123824e-01 6.123824e-01 +3.870000e+00 0.000000e+00 0.000000e+00 3.530000e+00 5.592587e-01 5.592587e-01 +3.886000e+00 0.000000e+00 0.000000e+00 3.900000e+00 6.182435e-01 6.182435e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1977_I119979/d02-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1977_I119979/d02-x01-y01 +Title: doi:10.17182/hepdata.20971.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.598000e+00 0.000000e+00 0.000000e+00 2.460000e+00 4.062770e-01 4.062770e-01 +3.692000e+00 0.000000e+00 0.000000e+00 2.400000e+00 4.951767e-01 4.951767e-01 +3.710000e+00 0.000000e+00 0.000000e+00 2.350000e+00 4.967457e-01 4.967457e-01 +3.730000e+00 0.000000e+00 0.000000e+00 2.480000e+00 4.177128e-01 4.177128e-01 +3.740000e+00 0.000000e+00 0.000000e+00 2.940000e+00 4.842324e-01 4.842324e-01 +3.750000e+00 0.000000e+00 0.000000e+00 3.340000e+00 5.432320e-01 5.432320e-01 +3.762000e+00 0.000000e+00 0.000000e+00 3.920000e+00 6.278089e-01 6.278089e-01 +3.766000e+00 0.000000e+00 0.000000e+00 4.400000e+00 7.057620e-01 7.057620e-01 +3.770000e+00 0.000000e+00 0.000000e+00 4.340000e+00 6.904354e-01 6.904354e-01 +3.774000e+00 0.000000e+00 0.000000e+00 4.590000e+00 7.006656e-01 7.006656e-01 +3.780000e+00 0.000000e+00 0.000000e+00 4.230000e+00 6.749002e-01 6.749002e-01 +3.786000e+00 0.000000e+00 0.000000e+00 3.400000e+00 5.515433e-01 5.515433e-01 +3.790000e+00 0.000000e+00 0.000000e+00 3.270000e+00 5.260135e-01 5.260135e-01 +3.800000e+00 0.000000e+00 0.000000e+00 3.120000e+00 5.014220e-01 5.014220e-01 +3.810000e+00 0.000000e+00 0.000000e+00 2.850000e+00 4.600611e-01 4.600611e-01 +3.821000e+00 0.000000e+00 0.000000e+00 2.770000e+00 4.489323e-01 4.489323e-01 +3.830000e+00 0.000000e+00 0.000000e+00 2.680000e+00 4.364676e-01 4.364676e-01 +3.850000e+00 0.000000e+00 0.000000e+00 2.720000e+00 4.459417e-01 4.459417e-01 +3.865000e+00 0.000000e+00 0.000000e+00 3.210000e+00 5.293791e-01 5.293791e-01 +3.870000e+00 0.000000e+00 0.000000e+00 2.930000e+00 4.749318e-01 4.749318e-01 +3.886000e+00 0.000000e+00 0.000000e+00 3.390000e+00 5.501566e-01 5.501566e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginSLAC/MARKI_1982_I169326.cc b/analyses/pluginSLAC/MARKI_1982_I169326.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1982_I169326.cc @@ -0,0 +1,75 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/ChargedFinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class MARKI_1982_I169326 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(MARKI_1982_I169326); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + + // Initialise and register projections + declare(ChargedFinalState(), "FS"); + + // Book histograms + _nHadrons= bookCounter("TMP/hadrons"); + + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const ChargedFinalState& fs = apply(event, "FS"); + _nHadrons->fill(fs.particles().size()*event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double sigma = _nHadrons->val()/sumOfWeights(); + double error = _nHadrons->err()/sumOfWeights(); + Scatter2D temphisto(refData(6, 1, 1)); + Scatter2DPtr mult = bookScatter2D(6, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _nHadrons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(MARKI_1982_I169326); + + +} diff --git a/analyses/pluginSLAC/MARKI_1982_I169326.info b/analyses/pluginSLAC/MARKI_1982_I169326.info new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1982_I169326.info @@ -0,0 +1,32 @@ +Name: MARKI_1982_I169326 +Year: 1982 +Summary: Charged particle multiplicity for energies between 2.6 and 7.8 GeV +Experiment: MARKI +Collider: SPEAR +InspireID: 169326 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Rev. D26 (1982) 969, 1982 +RunInfo: e+e- to hadrons +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Charged particle multiplicity for energies between 2.6 and 7.8 GeV' +Keywords: [] +BibKey: Siegrist:1981zp +BibTeX: '@article{Siegrist:1981zp, + author = "Siegrist, J. and others", + title = "{Hadron Production by e+ e- Annihilation at + Center-Of-Mass Energies Between 2.6-GeV and 7.8-GeV. Part + 1. Total Cross-Section, Multiplicities and Inclusive + Momentum Distributions}", + journal = "Phys. Rev.", + volume = "D26", + year = "1982", + pages = "969", + doi = "10.1103/PhysRevD.26.969", + reportNumber = "SLAC-PUB-2831, LBL-13464", + SLACcitation = "%%CITATION = PHRVA,D26,969;%%" +}' diff --git a/analyses/pluginSLAC/MARKI_1982_I169326.plot b/analyses/pluginSLAC/MARKI_1982_I169326.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1982_I169326.plot @@ -0,0 +1,7 @@ +BEGIN PLOT /MARKI_1982_I169326/d06-x01-y01 +Title=Charged hadron multiplicity +XLabel=$\sqrt{s}$/GeV +YLabel="$N_{\text{charged}}$ +ConnectGaps=1 +LogY=0 +END PLOT diff --git a/analyses/pluginSLAC/MARKI_1982_I169326.yoda b/analyses/pluginSLAC/MARKI_1982_I169326.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginSLAC/MARKI_1982_I169326.yoda @@ -0,0 +1,293 @@ +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1982_I169326/d01-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1982_I169326/d01-x01-y01 +Title: doi:10.17182/hepdata.23889.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.600000e+00 0.000000e+00 0.000000e+00 2.850000e+00 7.400000e-01 7.400000e-01 +2.800000e+00 0.000000e+00 0.000000e+00 2.540000e+00 4.600000e-01 4.600000e-01 +3.000000e+00 0.000000e+00 0.000000e+00 2.590000e+00 1.500000e-01 1.500000e-01 +3.150000e+00 0.000000e+00 0.000000e+00 2.790000e+00 4.200000e-01 4.200000e-01 +3.200000e+00 0.000000e+00 0.000000e+00 2.800000e+00 3.200000e-01 3.200000e-01 +3.300000e+00 0.000000e+00 0.000000e+00 2.650000e+00 4.600000e-01 4.600000e-01 +3.400000e+00 0.000000e+00 0.000000e+00 2.350000e+00 2.800000e-01 2.800000e-01 +3.450000e+00 0.000000e+00 0.000000e+00 2.120000e+00 3.000000e-01 3.000000e-01 +3.500000e+00 0.000000e+00 0.000000e+00 2.630000e+00 3.500000e-01 3.500000e-01 +3.550000e+00 0.000000e+00 0.000000e+00 2.500000e+00 3.000000e-01 3.000000e-01 +3.600000e+00 0.000000e+00 0.000000e+00 2.820000e+00 2.600000e-01 2.600000e-01 +3.650000e+00 0.000000e+00 0.000000e+00 2.500000e+00 1.900000e-01 1.900000e-01 +3.750000e+00 0.000000e+00 0.000000e+00 4.080000e+00 3.600000e-01 3.600000e-01 +3.800000e+00 0.000000e+00 0.000000e+00 2.760000e+00 2.600000e-01 2.600000e-01 +3.850000e+00 0.000000e+00 0.000000e+00 2.400000e+00 2.900000e-01 2.900000e-01 +3.900000e+00 0.000000e+00 0.000000e+00 3.040000e+00 1.300000e-01 1.300000e-01 +3.950000e+00 0.000000e+00 0.000000e+00 4.070000e+00 2.000000e-01 2.000000e-01 +4.000000e+00 0.000000e+00 0.000000e+00 4.290000e+00 1.300000e-01 1.300000e-01 +4.050000e+00 0.000000e+00 0.000000e+00 5.730000e+00 9.000000e-02 9.000000e-02 +4.100000e+00 0.000000e+00 0.000000e+00 4.970000e+00 1.500000e-01 1.500000e-01 +4.150000e+00 0.000000e+00 0.000000e+00 4.780000e+00 1.300000e-01 1.300000e-01 +4.200000e+00 0.000000e+00 0.000000e+00 4.110000e+00 1.400000e-01 1.400000e-01 +4.250000e+00 0.000000e+00 0.000000e+00 3.780000e+00 1.800000e-01 1.800000e-01 +4.300000e+00 0.000000e+00 0.000000e+00 3.470000e+00 1.500000e-01 1.500000e-01 +4.350000e+00 0.000000e+00 0.000000e+00 3.910000e+00 1.900000e-01 1.900000e-01 +4.400000e+00 0.000000e+00 0.000000e+00 5.010000e+00 8.000000e-02 8.000000e-02 +4.450000e+00 0.000000e+00 0.000000e+00 4.600000e+00 1.800000e-01 1.800000e-01 +4.500000e+00 0.000000e+00 0.000000e+00 3.790000e+00 1.800000e-01 1.800000e-01 +4.550000e+00 0.000000e+00 0.000000e+00 3.550000e+00 2.500000e-01 2.500000e-01 +4.600000e+00 0.000000e+00 0.000000e+00 3.330000e+00 1.900000e-01 1.900000e-01 +4.650000e+00 0.000000e+00 0.000000e+00 3.640000e+00 5.300000e-01 5.300000e-01 +4.700000e+00 0.000000e+00 0.000000e+00 3.860000e+00 2.300000e-01 2.300000e-01 +4.800000e+00 0.000000e+00 0.000000e+00 3.970000e+00 1.900000e-01 1.900000e-01 +4.900000e+00 0.000000e+00 0.000000e+00 3.610000e+00 2.500000e-01 2.500000e-01 +5.100000e+00 0.000000e+00 0.000000e+00 4.340000e+00 2.900000e-01 2.900000e-01 +5.200000e+00 0.000000e+00 0.000000e+00 3.570000e+00 2.700000e-01 2.700000e-01 +5.300000e+00 0.000000e+00 0.000000e+00 3.680000e+00 2.700000e-01 2.700000e-01 +5.400000e+00 0.000000e+00 0.000000e+00 4.240000e+00 3.100000e-01 3.100000e-01 +5.500000e+00 0.000000e+00 0.000000e+00 3.570000e+00 2.400000e-01 2.400000e-01 +5.600000e+00 0.000000e+00 0.000000e+00 4.080000e+00 3.200000e-01 3.200000e-01 +5.700000e+00 0.000000e+00 0.000000e+00 4.090000e+00 1.600000e-01 1.600000e-01 +5.750000e+00 0.000000e+00 0.000000e+00 4.120000e+00 2.000000e-01 2.000000e-01 +5.800000e+00 0.000000e+00 0.000000e+00 4.130000e+00 1.600000e-01 1.600000e-01 +5.850000e+00 0.000000e+00 0.000000e+00 4.130000e+00 1.900000e-01 1.900000e-01 +5.900000e+00 0.000000e+00 0.000000e+00 4.090000e+00 1.400000e-01 1.400000e-01 +5.950000e+00 0.000000e+00 0.000000e+00 4.170000e+00 1.600000e-01 1.600000e-01 +6.000000e+00 0.000000e+00 0.000000e+00 4.170000e+00 9.000000e-02 9.000000e-02 +6.050000e+00 0.000000e+00 0.000000e+00 4.160000e+00 1.800000e-01 1.800000e-01 +6.100000e+00 0.000000e+00 0.000000e+00 4.040000e+00 1.500000e-01 1.500000e-01 +6.150000e+00 0.000000e+00 0.000000e+00 4.340000e+00 1.600000e-01 1.600000e-01 +6.200000e+00 0.000000e+00 0.000000e+00 4.050000e+00 8.000000e-02 8.000000e-02 +6.250000e+00 0.000000e+00 0.000000e+00 3.960000e+00 1.400000e-01 1.400000e-01 +6.300000e+00 0.000000e+00 0.000000e+00 4.270000e+00 1.400000e-01 1.400000e-01 +6.350000e+00 0.000000e+00 0.000000e+00 4.470000e+00 1.700000e-01 1.700000e-01 +6.400000e+00 0.000000e+00 0.000000e+00 4.310000e+00 1.300000e-01 1.300000e-01 +6.450000e+00 0.000000e+00 0.000000e+00 4.230000e+00 1.400000e-01 1.400000e-01 +6.500000e+00 0.000000e+00 0.000000e+00 4.400000e+00 1.500000e-01 1.500000e-01 +6.550000e+00 0.000000e+00 0.000000e+00 4.660000e+00 1.600000e-01 1.600000e-01 +6.600000e+00 0.000000e+00 0.000000e+00 4.500000e+00 1.700000e-01 1.700000e-01 +6.650000e+00 0.000000e+00 0.000000e+00 4.250000e+00 1.600000e-01 1.600000e-01 +6.700000e+00 0.000000e+00 0.000000e+00 4.630000e+00 1.500000e-01 1.500000e-01 +6.750000e+00 0.000000e+00 0.000000e+00 4.380000e+00 1.500000e-01 1.500000e-01 +6.800000e+00 0.000000e+00 0.000000e+00 4.440000e+00 1.600000e-01 1.600000e-01 +6.850000e+00 0.000000e+00 0.000000e+00 4.500000e+00 1.300000e-01 1.300000e-01 +6.900000e+00 0.000000e+00 0.000000e+00 4.410000e+00 1.500000e-01 1.500000e-01 +6.950000e+00 0.000000e+00 0.000000e+00 4.230000e+00 1.700000e-01 1.700000e-01 +7.000000e+00 0.000000e+00 0.000000e+00 4.100000e+00 1.200000e-01 1.200000e-01 +7.050000e+00 0.000000e+00 0.000000e+00 4.310000e+00 9.000000e-02 9.000000e-02 +7.100000e+00 0.000000e+00 0.000000e+00 4.320000e+00 1.400000e-01 1.400000e-01 +7.150000e+00 0.000000e+00 0.000000e+00 4.290000e+00 1.100000e-01 1.100000e-01 +7.200000e+00 0.000000e+00 0.000000e+00 4.270000e+00 1.100000e-01 1.100000e-01 +7.250000e+00 0.000000e+00 0.000000e+00 4.390000e+00 1.100000e-01 1.100000e-01 +7.300000e+00 0.000000e+00 0.000000e+00 4.290000e+00 1.100000e-01 1.100000e-01 +7.350000e+00 0.000000e+00 0.000000e+00 4.330000e+00 9.000000e-02 9.000000e-02 +7.400000e+00 0.000000e+00 0.000000e+00 4.460000e+00 8.000000e-02 8.000000e-02 +7.450000e+00 0.000000e+00 0.000000e+00 4.510000e+00 1.400000e-01 1.400000e-01 +7.500000e+00 0.000000e+00 0.000000e+00 4.180000e+00 5.900000e-01 5.900000e-01 +7.800000e+00 0.000000e+00 0.000000e+00 4.470000e+00 5.300000e-01 5.300000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1982_I169326/d02-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1982_I169326/d02-x01-y01 +Title: doi:10.17182/hepdata.23889.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000000e+00 5.000000e-01 5.000000e-01 2.700000e+00 5.000000e-01 5.000000e-01 +2.000000e+00 5.000000e-01 5.000000e-01 4.300000e+00 4.000000e-01 4.000000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1982_I169326/d03-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1982_I169326/d03-x01-y01 +Title: doi:10.17182/hepdata.23889.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.400000e+00 0.000000e+00 0.000000e+00 1.640000e+00 5.800000e-01 5.800000e-01 +3.410000e+00 0.000000e+00 0.000000e+00 3.120000e+00 8.800000e-01 8.800000e-01 +3.420000e+00 0.000000e+00 0.000000e+00 1.890000e+00 6.400000e-01 6.400000e-01 +3.430000e+00 0.000000e+00 0.000000e+00 1.240000e+00 6.500000e-01 6.500000e-01 +3.440000e+00 0.000000e+00 0.000000e+00 2.050000e+00 6.700000e-01 6.700000e-01 +3.450000e+00 0.000000e+00 0.000000e+00 2.590000e+00 6.500000e-01 6.500000e-01 +3.460000e+00 0.000000e+00 0.000000e+00 2.700000e+00 8.400000e-01 8.400000e-01 +3.470000e+00 0.000000e+00 0.000000e+00 2.010000e+00 6.000000e-01 6.000000e-01 +3.480000e+00 0.000000e+00 0.000000e+00 2.690000e+00 8.400000e-01 8.400000e-01 +3.490000e+00 0.000000e+00 0.000000e+00 4.200000e+00 1.200000e+00 1.200000e+00 +3.500000e+00 0.000000e+00 0.000000e+00 1.270000e+00 4.900000e-01 4.900000e-01 +3.510000e+00 0.000000e+00 0.000000e+00 2.690000e+00 7.400000e-01 7.400000e-01 +3.520000e+00 0.000000e+00 0.000000e+00 2.870000e+00 7.600000e-01 7.600000e-01 +3.530000e+00 0.000000e+00 0.000000e+00 1.770000e+00 5.500000e-01 5.500000e-01 +3.540000e+00 0.000000e+00 0.000000e+00 2.750000e+00 8.500000e-01 8.500000e-01 +3.550000e+00 0.000000e+00 0.000000e+00 2.800000e+00 6.400000e-01 6.400000e-01 +3.560000e+00 0.000000e+00 0.000000e+00 2.590000e+00 5.900000e-01 5.900000e-01 +3.570000e+00 0.000000e+00 0.000000e+00 2.620000e+00 8.400000e-01 8.400000e-01 +3.580000e+00 0.000000e+00 0.000000e+00 2.010000e+00 6.000000e-01 6.000000e-01 +3.590000e+00 0.000000e+00 0.000000e+00 2.870000e+00 5.900000e-01 5.900000e-01 +3.600000e+00 0.000000e+00 0.000000e+00 2.560000e+00 7.400000e-01 7.400000e-01 +3.610000e+00 0.000000e+00 0.000000e+00 3.380000e+00 8.600000e-01 8.600000e-01 +3.620000e+00 0.000000e+00 0.000000e+00 3.700000e+00 1.010000e+00 1.010000e+00 +3.630000e+00 0.000000e+00 0.000000e+00 2.600000e+00 5.200000e-01 5.200000e-01 +3.640000e+00 0.000000e+00 0.000000e+00 2.180000e+00 3.100000e-01 3.100000e-01 +3.650000e+00 0.000000e+00 0.000000e+00 2.820000e+00 4.900000e-01 4.900000e-01 +3.660000e+00 0.000000e+00 0.000000e+00 2.780000e+00 4.300000e-01 4.300000e-01 +3.670000e+00 0.000000e+00 0.000000e+00 2.370000e+00 3.900000e-01 3.900000e-01 +3.720000e+00 0.000000e+00 0.000000e+00 3.120000e+00 9.400000e-01 9.400000e-01 +3.730000e+00 0.000000e+00 0.000000e+00 2.830000e+00 8.800000e-01 8.800000e-01 +3.740000e+00 0.000000e+00 0.000000e+00 4.780000e+00 1.160000e+00 1.160000e+00 +3.750000e+00 0.000000e+00 0.000000e+00 4.800000e+00 1.370000e+00 1.370000e+00 +3.760000e+00 0.000000e+00 0.000000e+00 4.010000e+00 5.100000e-01 5.100000e-01 +3.770000e+00 0.000000e+00 0.000000e+00 4.380000e+00 8.400000e-01 8.400000e-01 +3.780000e+00 0.000000e+00 0.000000e+00 4.050000e+00 6.900000e-01 6.900000e-01 +3.790000e+00 0.000000e+00 0.000000e+00 3.520000e+00 5.500000e-01 5.500000e-01 +3.800000e+00 0.000000e+00 0.000000e+00 1.460000e+00 4.100000e-01 4.100000e-01 +3.810000e+00 0.000000e+00 0.000000e+00 2.780000e+00 8.400000e-01 8.400000e-01 +3.820000e+00 0.000000e+00 0.000000e+00 1.470000e+00 4.500000e-01 4.500000e-01 +3.830000e+00 0.000000e+00 0.000000e+00 1.890000e+00 5.700000e-01 5.700000e-01 +3.840000e+00 0.000000e+00 0.000000e+00 2.420000e+00 6.800000e-01 6.800000e-01 +3.850000e+00 0.000000e+00 0.000000e+00 2.520000e+00 6.100000e-01 6.100000e-01 +3.860000e+00 0.000000e+00 0.000000e+00 2.620000e+00 7.200000e-01 7.200000e-01 +3.870000e+00 0.000000e+00 0.000000e+00 2.660000e+00 6.400000e-01 6.400000e-01 +3.880000e+00 0.000000e+00 0.000000e+00 2.400000e+00 7.000000e-01 7.000000e-01 +3.890000e+00 0.000000e+00 0.000000e+00 2.830000e+00 1.700000e-01 1.700000e-01 +3.900000e+00 0.000000e+00 0.000000e+00 2.980000e+00 2.800000e-01 2.800000e-01 +3.910000e+00 0.000000e+00 0.000000e+00 3.210000e+00 3.400000e-01 3.400000e-01 +3.920000e+00 0.000000e+00 0.000000e+00 3.490000e+00 3.000000e-01 3.000000e-01 +3.930000e+00 0.000000e+00 0.000000e+00 4.270000e+00 4.900000e-01 4.900000e-01 +3.940000e+00 0.000000e+00 0.000000e+00 3.500000e+00 3.300000e-01 3.300000e-01 +3.950000e+00 0.000000e+00 0.000000e+00 4.040000e+00 5.100000e-01 5.100000e-01 +3.960000e+00 0.000000e+00 0.000000e+00 4.270000e+00 3.800000e-01 3.800000e-01 +3.970000e+00 0.000000e+00 0.000000e+00 4.610000e+00 5.300000e-01 5.300000e-01 +3.980000e+00 0.000000e+00 0.000000e+00 4.110000e+00 3.300000e-01 3.300000e-01 +3.990000e+00 0.000000e+00 0.000000e+00 4.040000e+00 1.900000e-01 1.900000e-01 +4.000000e+00 0.000000e+00 0.000000e+00 3.940000e+00 2.200000e-01 2.200000e-01 +4.010000e+00 0.000000e+00 0.000000e+00 4.470000e+00 3.600000e-01 3.600000e-01 +4.020000e+00 0.000000e+00 0.000000e+00 5.160000e+00 3.000000e-01 3.000000e-01 +4.030000e+00 0.000000e+00 0.000000e+00 5.770000e+00 1.000000e-01 1.000000e-01 +4.040000e+00 0.000000e+00 0.000000e+00 5.210000e+00 2.500000e-01 2.500000e-01 +4.050000e+00 0.000000e+00 0.000000e+00 4.880000e+00 5.000000e-01 5.000000e-01 +4.060000e+00 0.000000e+00 0.000000e+00 4.750000e+00 2.700000e-01 2.700000e-01 +4.070000e+00 0.000000e+00 0.000000e+00 4.730000e+00 5.900000e-01 5.900000e-01 +4.080000e+00 0.000000e+00 0.000000e+00 5.290000e+00 4.000000e-01 4.000000e-01 +4.090000e+00 0.000000e+00 0.000000e+00 4.790000e+00 2.200000e-01 2.200000e-01 +4.100000e+00 0.000000e+00 0.000000e+00 5.170000e+00 5.600000e-01 5.600000e-01 +4.110000e+00 0.000000e+00 0.000000e+00 4.970000e+00 2.100000e-01 2.100000e-01 +4.120000e+00 0.000000e+00 0.000000e+00 5.390000e+00 7.200000e-01 7.200000e-01 +4.130000e+00 0.000000e+00 0.000000e+00 4.470000e+00 4.200000e-01 4.200000e-01 +4.140000e+00 0.000000e+00 0.000000e+00 4.830000e+00 1.400000e-01 1.400000e-01 +4.150000e+00 0.000000e+00 0.000000e+00 4.720000e+00 5.900000e-01 5.900000e-01 +4.160000e+00 0.000000e+00 0.000000e+00 5.220000e+00 8.000000e-01 8.000000e-01 +4.170000e+00 0.000000e+00 0.000000e+00 4.790000e+00 5.300000e-01 5.300000e-01 +4.180000e+00 0.000000e+00 0.000000e+00 5.200000e+00 5.800000e-01 5.800000e-01 +4.190000e+00 0.000000e+00 0.000000e+00 4.080000e+00 1.700000e-01 1.700000e-01 +4.200000e+00 0.000000e+00 0.000000e+00 3.850000e+00 6.300000e-01 6.300000e-01 +4.210000e+00 0.000000e+00 0.000000e+00 3.990000e+00 3.200000e-01 3.200000e-01 +4.220000e+00 0.000000e+00 0.000000e+00 3.930000e+00 5.300000e-01 5.300000e-01 +4.230000e+00 0.000000e+00 0.000000e+00 4.160000e+00 5.700000e-01 5.700000e-01 +4.240000e+00 0.000000e+00 0.000000e+00 3.920000e+00 3.200000e-01 3.200000e-01 +4.250000e+00 0.000000e+00 0.000000e+00 2.990000e+00 4.700000e-01 4.700000e-01 +4.260000e+00 0.000000e+00 0.000000e+00 4.710000e+00 6.300000e-01 6.300000e-01 +4.270000e+00 0.000000e+00 0.000000e+00 3.520000e+00 2.700000e-01 2.700000e-01 +4.280000e+00 0.000000e+00 0.000000e+00 3.560000e+00 3.100000e-01 3.100000e-01 +4.290000e+00 0.000000e+00 0.000000e+00 3.420000e+00 1.700000e-01 1.700000e-01 +4.300000e+00 0.000000e+00 0.000000e+00 3.620000e+00 5.000000e-01 5.000000e-01 +4.330000e+00 0.000000e+00 0.000000e+00 3.450000e+00 2.600000e-01 2.600000e-01 +4.350000e+00 0.000000e+00 0.000000e+00 3.960000e+00 3.800000e-01 3.800000e-01 +4.370000e+00 0.000000e+00 0.000000e+00 4.460000e+00 3.400000e-01 3.400000e-01 +4.380000e+00 0.000000e+00 0.000000e+00 4.670000e+00 3.800000e-01 3.800000e-01 +4.390000e+00 0.000000e+00 0.000000e+00 4.190000e+00 2.100000e-01 2.100000e-01 +4.400000e+00 0.000000e+00 0.000000e+00 5.260000e+00 3.400000e-01 3.400000e-01 +4.410000e+00 0.000000e+00 0.000000e+00 5.060000e+00 1.000000e-01 1.000000e-01 +4.420000e+00 0.000000e+00 0.000000e+00 5.170000e+00 9.000000e-02 9.000000e-02 +4.430000e+00 0.000000e+00 0.000000e+00 5.080000e+00 3.000000e-01 3.000000e-01 +4.440000e+00 0.000000e+00 0.000000e+00 4.260000e+00 2.800000e-01 2.800000e-01 +4.450000e+00 0.000000e+00 0.000000e+00 4.590000e+00 4.900000e-01 4.900000e-01 +4.460000e+00 0.000000e+00 0.000000e+00 4.630000e+00 5.300000e-01 5.300000e-01 +4.470000e+00 0.000000e+00 0.000000e+00 4.580000e+00 6.200000e-01 6.200000e-01 +4.490000e+00 0.000000e+00 0.000000e+00 3.610000e+00 2.200000e-01 2.200000e-01 +4.510000e+00 0.000000e+00 0.000000e+00 4.130000e+00 3.100000e-01 3.100000e-01 +4.530000e+00 0.000000e+00 0.000000e+00 3.640000e+00 3.800000e-01 3.800000e-01 +4.540000e+00 0.000000e+00 0.000000e+00 3.470000e+00 3.400000e-01 3.400000e-01 +4.580000e+00 0.000000e+00 0.000000e+00 3.690000e+00 5.700000e-01 5.700000e-01 +4.590000e+00 0.000000e+00 0.000000e+00 3.260000e+00 2.000000e-01 2.000000e-01 +4.630000e+00 0.000000e+00 0.000000e+00 3.590000e+00 5.200000e-01 5.200000e-01 +4.680000e+00 0.000000e+00 0.000000e+00 3.930000e+00 3.600000e-01 3.600000e-01 +4.690000e+00 0.000000e+00 0.000000e+00 3.770000e+00 2.900000e-01 2.900000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1982_I169326/d04-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1982_I169326/d04-x01-y01 +Title: doi:10.17182/hepdata.23889.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +3.350000e+00 1.500000e-01 1.500000e-01 9.700000e+02 0.000000e+00 0.000000e+00 +3.590000e+00 9.000000e-02 9.000000e-02 7.800000e+02 0.000000e+00 0.000000e+00 +3.860000e+00 1.400000e-01 1.400000e-01 8.500000e+02 0.000000e+00 0.000000e+00 +4.200000e+00 2.000000e-01 2.000000e-01 6.200000e+02 0.000000e+00 0.000000e+00 +4.650000e+00 2.500000e-01 2.500000e-01 5.800000e+02 0.000000e+00 0.000000e+00 +5.275000e+00 3.750000e-01 3.750000e-01 8.000000e+02 0.000000e+00 0.000000e+00 +5.825000e+00 1.750000e-01 1.750000e-01 9.000000e+01 0.000000e+00 0.000000e+00 +6.225000e+00 2.250000e-01 2.250000e-01 1.000000e+02 0.000000e+00 0.000000e+00 +6.700000e+00 2.500000e-01 2.500000e-01 6.500000e+01 0.000000e+00 0.000000e+00 +7.200000e+00 2.500000e-01 2.500000e-01 3.500000e+01 0.000000e+00 0.000000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKI_1982_I169326/d05-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1982_I169326/d05-x01-y01 +Title: doi:10.17182/hepdata.23889.v1/t5 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/MARKI_1982_I169326/d06-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1982_I169326/d06-x01-y01 +Title: doi:10.17182/hepdata.23889.v1/t6 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +2.600000e+00 0.000000e+00 0.000000e+00 3.750000e+00 4.200000e-01 4.200000e-01 +2.800000e+00 0.000000e+00 0.000000e+00 3.790000e+00 2.400000e-01 2.400000e-01 +3.000000e+00 0.000000e+00 0.000000e+00 3.930000e+00 9.000000e-02 9.000000e-02 +3.200000e+00 0.000000e+00 0.000000e+00 4.190000e+00 1.500000e-01 1.500000e-01 +3.300000e+00 0.000000e+00 0.000000e+00 4.140000e+00 2.500000e-01 2.500000e-01 +3.400000e+00 0.000000e+00 0.000000e+00 4.100000e+00 2.200000e-01 2.200000e-01 +3.600000e+00 0.000000e+00 0.000000e+00 4.440000e+00 2.500000e-01 2.500000e-01 +3.800000e+00 0.000000e+00 0.000000e+00 4.290000e+00 6.000000e-02 6.000000e-02 +3.900000e+00 0.000000e+00 0.000000e+00 4.320000e+00 1.300000e-01 1.300000e-01 +4.000000e+00 0.000000e+00 0.000000e+00 4.370000e+00 4.000000e-02 4.000000e-02 +4.100000e+00 0.000000e+00 0.000000e+00 4.400000e+00 1.000000e-01 1.000000e-01 +4.200000e+00 0.000000e+00 0.000000e+00 4.580000e+00 1.300000e-01 1.300000e-01 +4.300000e+00 0.000000e+00 0.000000e+00 4.610000e+00 1.500000e-01 1.500000e-01 +4.400000e+00 0.000000e+00 0.000000e+00 4.560000e+00 4.000000e-02 4.000000e-02 +4.500000e+00 0.000000e+00 0.000000e+00 4.790000e+00 2.300000e-01 2.300000e-01 +4.600000e+00 0.000000e+00 0.000000e+00 4.980000e+00 3.000000e-01 3.000000e-01 +4.700000e+00 0.000000e+00 0.000000e+00 4.490000e+00 3.000000e-01 3.000000e-01 +4.800000e+00 0.000000e+00 0.000000e+00 4.850000e+00 7.000000e-02 7.000000e-02 +5.100000e+00 0.000000e+00 0.000000e+00 4.430000e+00 2.300000e-01 2.300000e-01 +5.400000e+00 0.000000e+00 0.000000e+00 5.150000e+00 2.500000e-01 2.500000e-01 +5.600000e+00 0.000000e+00 0.000000e+00 4.960000e+00 1.800000e-01 1.800000e-01 +5.800000e+00 0.000000e+00 0.000000e+00 5.280000e+00 1.300000e-01 1.300000e-01 +6.000000e+00 0.000000e+00 0.000000e+00 4.970000e+00 1.100000e-01 1.100000e-01 +6.100000e+00 0.000000e+00 0.000000e+00 5.090000e+00 1.600000e-01 1.600000e-01 +6.200000e+00 0.000000e+00 0.000000e+00 5.320000e+00 1.000000e-01 1.000000e-01 +6.300000e+00 0.000000e+00 0.000000e+00 5.330000e+00 1.600000e-01 1.600000e-01 +6.400000e+00 0.000000e+00 0.000000e+00 5.330000e+00 1.600000e-01 1.600000e-01 +6.500000e+00 0.000000e+00 0.000000e+00 5.320000e+00 1.900000e-01 1.900000e-01 +6.600000e+00 0.000000e+00 0.000000e+00 5.020000e+00 1.800000e-01 1.800000e-01 +6.700000e+00 0.000000e+00 0.000000e+00 5.200000e+00 1.700000e-01 1.700000e-01 +6.800000e+00 0.000000e+00 0.000000e+00 5.270000e+00 1.300000e-01 1.300000e-01 +6.900000e+00 0.000000e+00 0.000000e+00 5.270000e+00 1.900000e-01 1.900000e-01 +7.000000e+00 0.000000e+00 0.000000e+00 5.150000e+00 1.400000e-01 1.400000e-01 +7.100000e+00 0.000000e+00 0.000000e+00 5.280000e+00 1.500000e-01 1.500000e-01 +7.200000e+00 0.000000e+00 0.000000e+00 5.290000e+00 1.100000e-01 1.100000e-01 +7.300000e+00 0.000000e+00 0.000000e+00 5.300000e+00 1.300000e-01 1.300000e-01 +7.400000e+00 0.000000e+00 0.000000e+00 5.490000e+00 1.400000e-01 1.400000e-01 +7.800000e+00 0.000000e+00 0.000000e+00 5.750000e+00 3.300000e-01 3.300000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER1D_V2 /REF/MARKI_1982_I169326/d07-x01-y01 +IsRef: 1 +Path: /REF/MARKI_1982_I169326/d07-x01-y01 +Title: doi:10.17182/hepdata.23889.v1/t7 +Type: Scatter1D +--- +# xval xerr- xerr+ +END YODA_SCATTER1D_V2 diff --git a/analyses/pluginMisc/TPC_1987_I235694.cc b/analyses/pluginSLAC/TPC_1987_I235694.cc rename from analyses/pluginMisc/TPC_1987_I235694.cc rename to analyses/pluginSLAC/TPC_1987_I235694.cc diff --git a/analyses/pluginMisc/TPC_1987_I235694.info b/analyses/pluginSLAC/TPC_1987_I235694.info rename from analyses/pluginMisc/TPC_1987_I235694.info rename to analyses/pluginSLAC/TPC_1987_I235694.info diff --git a/analyses/pluginMisc/TPC_1987_I235694.plot b/analyses/pluginSLAC/TPC_1987_I235694.plot rename from analyses/pluginMisc/TPC_1987_I235694.plot rename to analyses/pluginSLAC/TPC_1987_I235694.plot diff --git a/analyses/pluginMisc/TPC_1987_I235694.yoda b/analyses/pluginSLAC/TPC_1987_I235694.yoda rename from analyses/pluginMisc/TPC_1987_I235694.yoda rename to analyses/pluginSLAC/TPC_1987_I235694.yoda diff --git a/analyses/pluginTristan/AMY_1990_I294525.cc b/analyses/pluginTristan/AMY_1990_I294525.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/AMY_1990_I294525.cc @@ -0,0 +1,98 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class AMY_1990_I294525 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(AMY_1990_I294525); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(AMY_1990_I294525); + + +} diff --git a/analyses/pluginTristan/AMY_1990_I294525.info b/analyses/pluginTristan/AMY_1990_I294525.info new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/AMY_1990_I294525.info @@ -0,0 +1,32 @@ +Name: AMY_1990_I294525 +Year: 1990 +Summary: Measurement of $R$ for energies between 50 and 61.4 GeV. +Experiment: AMY +Collider: Tristan +InspireID: 294525 +Authors: + - Peter Richardson +References: + - Phys.Rev. D42 (1990) 1339-1349, 1990 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by AMY for energies between 50 and 61.4 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Kumita:1990my +BibTeX: '@article{Kumita:1990my, + author = "Kumita, T. and others", + title = "{Measurements of $R$ for $e^+e^-$ annihilation at + TRISTAN}", + collaboration = "AMY", + journal = "Phys. Rev.", + volume = "D42", + year = "1990", + pages = "1339-1349", + doi = "10.1103/PhysRevD.42.1339", + reportNumber = "KEK-PREPRINT-89-188, AMY-89-21", + SLACcitation = "%%CITATION = PHRVA,D42,1339;%%" +}' diff --git a/analyses/pluginTristan/AMY_1990_I294525.plot b/analyses/pluginTristan/AMY_1990_I294525.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/AMY_1990_I294525.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /AMY_1990_I294525/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /AMY_1990_I294525/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /AMY_1990_I294525/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginTristan/AMY_1990_I294525.yoda b/analyses/pluginTristan/AMY_1990_I294525.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/AMY_1990_I294525.yoda @@ -0,0 +1,21 @@ +BEGIN YODA_SCATTER2D_V2 /REF/AMY_1990_I294525/d01-x01-y01 +IsRef: 1 +Path: /REF/AMY_1990_I294525/d01-x01-y01 +Title: doi:10.17182/hepdata.22908.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e+01 0.000000e+00 0.000000e+00 4.540000e+00 5.000000e-01 5.000000e-01 +5.200000e+01 0.000000e+00 0.000000e+00 4.330000e+00 2.200000e-01 2.200000e-01 +5.400000e+01 0.000000e+00 0.000000e+00 4.720000e+00 6.300000e-01 6.300000e-01 +5.500000e+01 0.000000e+00 0.000000e+00 4.670000e+00 2.500000e-01 2.500000e-01 +5.600000e+01 0.000000e+00 0.000000e+00 5.240000e+00 2.000000e-01 2.000000e-01 +5.650000e+01 0.000000e+00 0.000000e+00 5.370000e+00 5.000000e-01 5.000000e-01 +5.700000e+01 0.000000e+00 0.000000e+00 4.950000e+00 2.300000e-01 2.300000e-01 +5.850000e+01 0.000000e+00 0.000000e+00 5.340000e+00 5.900000e-01 5.900000e-01 +5.900000e+01 0.000000e+00 0.000000e+00 5.440000e+00 6.300000e-01 6.300000e-01 +5.905000e+01 0.000000e+00 0.000000e+00 6.610000e+00 8.300000e-01 8.300000e-01 +6.000000e+01 0.000000e+00 0.000000e+00 5.830000e+00 3.000000e-01 3.000000e-01 +6.080000e+01 0.000000e+00 0.000000e+00 5.560000e+00 3.000000e-01 3.000000e-01 +6.140000e+01 0.000000e+00 0.000000e+00 5.380000e+00 2.700000e-01 2.700000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginMisc/AMY_1990_I295160.cc b/analyses/pluginTristan/AMY_1990_I295160.cc rename from analyses/pluginMisc/AMY_1990_I295160.cc rename to analyses/pluginTristan/AMY_1990_I295160.cc diff --git a/analyses/pluginMisc/AMY_1990_I295160.info b/analyses/pluginTristan/AMY_1990_I295160.info rename from analyses/pluginMisc/AMY_1990_I295160.info rename to analyses/pluginTristan/AMY_1990_I295160.info diff --git a/analyses/pluginMisc/AMY_1990_I295160.plot b/analyses/pluginTristan/AMY_1990_I295160.plot rename from analyses/pluginMisc/AMY_1990_I295160.plot rename to analyses/pluginTristan/AMY_1990_I295160.plot diff --git a/analyses/pluginMisc/AMY_1990_I295160.yoda b/analyses/pluginTristan/AMY_1990_I295160.yoda rename from analyses/pluginMisc/AMY_1990_I295160.yoda rename to analyses/pluginTristan/AMY_1990_I295160.yoda diff --git a/analyses/pluginTristan/TOPAZ_1990_I283003.cc b/analyses/pluginTristan/TOPAZ_1990_I283003.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1990_I283003.cc @@ -0,0 +1,98 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class TOPAZ_1990_I283003 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(TOPAZ_1990_I283003); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(TOPAZ_1990_I283003); + + +} diff --git a/analyses/pluginTristan/TOPAZ_1990_I283003.info b/analyses/pluginTristan/TOPAZ_1990_I283003.info new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1990_I283003.info @@ -0,0 +1,36 @@ +Name: TOPAZ_1990_I283003 +Year: 1990 +Summary: Measurement of $R$ for energies between 50 and 61.4 GeV +Experiment: TOPAZ +Collider: Tristan +InspireID: 283003 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B234 (1990) 525-533, 1990 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by TOPAZ for energies between 50 and 61.4 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Adachi:1989yz +BibTeX: '@article{Adachi:1989yz, + author = "Adachi, I. and others", + title = "{Measurement of the Total Hadronic Cross-sections in + e$^{+} $e$^{-}$ Annihilation and Determination of the + Standard Model Parameters}", + collaboration = "TOPAZ", + journal = "Phys. Lett.", + volume = "B234", + year = "1990", + pages = "525-533", + doi = "10.1016/0370-2693(90)92052-K", + reportNumber = "KEK-PREPRINT-89-136, DPNU-89-51, INS-779, KOBE-HEP-89-10, + NWU-HEP-89-04, OCU-HEP-89-04, PU-89-636, TU-HEP-89-03, + TUAT-HEP-89-03, UT-HE-89-08", + SLACcitation = "%%CITATION = PHLTA,B234,525;%%" +}' diff --git a/analyses/pluginTristan/TOPAZ_1990_I283003.plot b/analyses/pluginTristan/TOPAZ_1990_I283003.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1990_I283003.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /TOPAZ_1990_I283003/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TOPAZ_1990_I283003/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TOPAZ_1990_I283003/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginTristan/TOPAZ_1990_I283003.yoda b/analyses/pluginTristan/TOPAZ_1990_I283003.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1990_I283003.yoda @@ -0,0 +1,38 @@ +BEGIN YODA_SCATTER2D_V2 /REF/TOPAZ_1990_I283003/d01-x01-y01 +IsRef: 1 +Path: /REF/TOPAZ_1990_I283003/d01-x01-y01 +Title: doi:10.17182/hepdata.29733.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e+01 0.000000e+00 0.000000e+00 4.530000e+00 6.488451e-01 6.488451e-01 +5.200000e+01 0.000000e+00 0.000000e+00 4.530000e+00 3.264966e-01 3.264966e-01 +5.400000e+01 0.000000e+00 0.000000e+00 4.980000e+00 6.441273e-01 6.441273e-01 +5.500000e+01 0.000000e+00 0.000000e+00 4.640000e+00 3.606938e-01 3.606938e-01 +5.600000e+01 0.000000e+00 0.000000e+00 5.070000e+00 3.560899e-01 3.560899e-01 +5.650000e+01 0.000000e+00 0.000000e+00 5.110000e+00 5.660389e-01 5.660389e-01 +5.700000e+01 0.000000e+00 0.000000e+00 5.150000e+00 3.828838e-01 3.828838e-01 +5.829000e+01 0.000000e+00 0.000000e+00 5.340000e+00 5.382379e-01 5.382379e-01 +5.906000e+01 0.000000e+00 0.000000e+00 5.740000e+00 5.420332e-01 5.420332e-01 +6.000000e+01 0.000000e+00 0.000000e+00 5.310000e+00 4.172529e-01 4.172529e-01 +6.080000e+01 0.000000e+00 0.000000e+00 5.660000e+00 4.252058e-01 4.252058e-01 +6.140000e+01 0.000000e+00 0.000000e+00 5.860000e+00 4.527693e-01 4.527693e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TOPAZ_1990_I283003/d02-x01-y01 +IsRef: 1 +Path: /REF/TOPAZ_1990_I283003/d02-x01-y01 +Title: doi:10.17182/hepdata.29733.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.570000e+01 5.700000e+00 5.700000e+00 2.330000e-01 2.500000e-02 3.500000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TOPAZ_1990_I283003/d02-x01-y02 +IsRef: 1 +Path: /REF/TOPAZ_1990_I283003/d02-x01-y02 +Title: doi:10.17182/hepdata.29733.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.570000e+01 5.700000e+00 5.700000e+00 3.270000e-01 2.060000e-01 2.750000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginTristan/TOPAZ_1993_I353845.cc b/analyses/pluginTristan/TOPAZ_1993_I353845.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1993_I353845.cc @@ -0,0 +1,97 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class TOPAZ_1993_I353845 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(TOPAZ_1993_I353845); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /picobarn; + for(unsigned int ix=2;ix<5;ix+=2) { + double sigma,error; + if(ix==2) { + sigma = _c_hadrons->val()*fact; + error = _c_hadrons->err()*fact; + } + else { + sigma = _c_muons ->val()*fact; + error = _c_muons ->err()*fact; + } + Scatter2D temphisto(refData(ix, 1, 1)); + Scatter2DPtr mult = bookScatter2D(ix, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(TOPAZ_1993_I353845); + + +} diff --git a/analyses/pluginTristan/TOPAZ_1993_I353845.info b/analyses/pluginTristan/TOPAZ_1993_I353845.info new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1993_I353845.info @@ -0,0 +1,33 @@ +Name: TOPAZ_1993_I353845 +Year: 1993 +Summary: Cross section in $e^+e^-\to$hadrons for energies between 57.37 and 59.84 GeV +Experiment: TOPAZ +Collider: Tristan +InspireID: 353845 +Authors: + - Peter Richardson +References: + - Phys.Lett. B304 (1993) 373-380, 1993 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of the hadronic cross section in $e^+e^-$ collisions by TOPAZ for energies between 57.37 and 59.84 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +BibKey: Abe:1993fy +BibTeX: '@article{Abe:1993fy, + author = "Abe, K. and others", + title = "{Search for a narrow resonance in e+ e- collisions + between E(cm) = 58-GeV and 60-GeV}", + collaboration = "TOPAZ", + journal = "Phys. Lett.", + volume = "B304", + year = "1993", + pages = "373-380", + doi = "10.1016/0370-2693(93)90311-5", + reportNumber = "KEK-PREPRINT-92-205, TUAT-HEP-93-01, NWU-HEP-9302, + DPNU-93-08, OCU-HEP-93-1, PU-93-666, INS-966, + KOBE-HEP-93-04, TIT-HPE-93-03", + SLACcitation = "%%CITATION = PHLTA,B304,373;%%" +}' diff --git a/analyses/pluginTristan/TOPAZ_1993_I353845.plot b/analyses/pluginTristan/TOPAZ_1993_I353845.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1993_I353845.plot @@ -0,0 +1,14 @@ +BEGIN PLOT /TOPAZ_1993_I353845/d02-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /TOPAZ_1993_I353845/d04-x01-y01 +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT \ No newline at end of file diff --git a/analyses/pluginTristan/TOPAZ_1993_I353845.yoda b/analyses/pluginTristan/TOPAZ_1993_I353845.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1993_I353845.yoda @@ -0,0 +1,72 @@ +BEGIN YODA_SCATTER2D_V2 /REF/TOPAZ_1993_I353845/d01-x01-y01 +IsRef: 1 +Path: /REF/TOPAZ_1993_I353845/d01-x01-y01 +Title: doi:10.17182/hepdata.28918.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.737000e+01 0.000000e+00 0.000000e+00 4.700000e+01 7.600000e+00 7.600000e+00 +5.777000e+01 0.000000e+00 0.000000e+00 5.160000e+01 1.800000e+00 1.800000e+00 +5.797000e+01 0.000000e+00 0.000000e+00 4.030000e+01 6.400000e+00 6.400000e+00 +5.822000e+01 0.000000e+00 0.000000e+00 4.190000e+01 6.300000e+00 6.300000e+00 +5.847000e+01 0.000000e+00 0.000000e+00 3.620000e+01 5.900000e+00 5.900000e+00 +5.872000e+01 0.000000e+00 0.000000e+00 4.960000e+01 5.900000e+00 5.900000e+00 +5.897000e+01 0.000000e+00 0.000000e+00 5.860000e+01 7.400000e+00 7.400000e+00 +5.922000e+01 0.000000e+00 0.000000e+00 5.130000e+01 7.600000e+00 7.600000e+00 +5.947000e+01 0.000000e+00 0.000000e+00 5.290000e+01 8.600000e+00 8.600000e+00 +5.984000e+01 0.000000e+00 0.000000e+00 4.500000e+01 4.200000e+00 4.200000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TOPAZ_1993_I353845/d02-x01-y01 +IsRef: 1 +Path: /REF/TOPAZ_1993_I353845/d02-x01-y01 +Title: doi:10.17182/hepdata.28918.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.737000e+01 0.000000e+00 0.000000e+00 1.305800e+02 1.348000e+01 1.348000e+01 +5.777000e+01 0.000000e+00 0.000000e+00 1.436400e+02 5.530000e+00 5.530000e+00 +5.797000e+01 0.000000e+00 0.000000e+00 1.395400e+02 1.285000e+01 1.285000e+01 +5.822000e+01 0.000000e+00 0.000000e+00 1.352800e+02 1.231000e+01 1.231000e+01 +5.847000e+01 0.000000e+00 0.000000e+00 1.218400e+02 1.161000e+01 1.161000e+01 +5.872000e+01 0.000000e+00 0.000000e+00 1.353500e+02 1.099000e+01 1.099000e+01 +5.897000e+01 0.000000e+00 0.000000e+00 1.558300e+02 1.335000e+01 1.335000e+01 +5.922000e+01 0.000000e+00 0.000000e+00 1.406600e+02 1.266000e+01 1.266000e+01 +5.947000e+01 0.000000e+00 0.000000e+00 1.494800e+02 1.543000e+01 1.543000e+01 +5.984000e+01 0.000000e+00 0.000000e+00 1.279300e+02 9.780000e+00 9.780000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TOPAZ_1993_I353845/d03-x01-y01 +IsRef: 1 +Path: /REF/TOPAZ_1993_I353845/d03-x01-y01 +Title: doi:10.17182/hepdata.28918.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.737000e+01 0.000000e+00 0.000000e+00 4.059000e+02 2.540000e+01 2.540000e+01 +5.777000e+01 0.000000e+00 0.000000e+00 4.061000e+02 1.040000e+01 1.040000e+01 +5.797000e+01 0.000000e+00 0.000000e+00 4.111000e+02 2.350000e+01 2.350000e+01 +5.822000e+01 0.000000e+00 0.000000e+00 4.073000e+02 2.280000e+01 2.280000e+01 +5.847000e+01 0.000000e+00 0.000000e+00 3.910000e+02 2.230000e+01 2.230000e+01 +5.872000e+01 0.000000e+00 0.000000e+00 4.166000e+02 2.070000e+01 2.070000e+01 +5.897000e+01 0.000000e+00 0.000000e+00 3.781000e+02 2.170000e+01 2.170000e+01 +5.922000e+01 0.000000e+00 0.000000e+00 3.723000e+02 2.310000e+01 2.310000e+01 +5.947000e+01 0.000000e+00 0.000000e+00 4.225000e+02 2.730000e+01 2.730000e+01 +5.984000e+01 0.000000e+00 0.000000e+00 3.640000e+02 1.440000e+01 1.440000e+01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/TOPAZ_1993_I353845/d04-x01-y01 +IsRef: 1 +Path: /REF/TOPAZ_1993_I353845/d04-x01-y01 +Title: doi:10.17182/hepdata.28918.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.737000e+01 0.000000e+00 0.000000e+00 3.120000e+01 8.200000e+00 8.200000e+00 +5.777000e+01 0.000000e+00 0.000000e+00 2.479000e+01 1.180000e+00 1.180000e+00 +5.797000e+01 0.000000e+00 0.000000e+00 2.200000e+01 6.200000e+00 6.200000e+00 +5.822000e+01 0.000000e+00 0.000000e+00 3.350000e+01 7.500000e+00 7.500000e+00 +5.847000e+01 0.000000e+00 0.000000e+00 2.080000e+01 5.900000e+00 5.900000e+00 +5.872000e+01 0.000000e+00 0.000000e+00 2.040000e+01 5.100000e+00 5.100000e+00 +5.897000e+01 0.000000e+00 0.000000e+00 1.890000e+01 5.600000e+00 5.600000e+00 +5.922000e+01 0.000000e+00 0.000000e+00 2.240000e+01 6.700000e+00 6.700000e+00 +5.947000e+01 0.000000e+00 0.000000e+00 3.280000e+01 9.000000e+00 9.000000e+00 +5.984000e+01 0.000000e+00 0.000000e+00 2.830000e+01 4.400000e+00 4.400000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginTristan/TOPAZ_1995_I381777.cc b/analyses/pluginTristan/TOPAZ_1995_I381777.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1995_I381777.cc @@ -0,0 +1,87 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class TOPAZ_1995_I381777 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(TOPAZ_1995_I381777); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + vetoEvent; + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /picobarn; + double sigma = _c_hadrons->val()*fact; + double error = _c_hadrons->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(TOPAZ_1995_I381777); + + +} diff --git a/analyses/pluginTristan/TOPAZ_1995_I381777.info b/analyses/pluginTristan/TOPAZ_1995_I381777.info new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1995_I381777.info @@ -0,0 +1,32 @@ +Name: TOPAZ_1995_I381777 +Year: 1995 +Summary: Cross section in $e^+e^-\to$hadrons for 57.77 GeV +Experiment: TOPAZ +Collider: Tristan +InspireID: 381777 +Authors: + - Peter Richardson +References: + - Phys.Lett. B347 (1995) 171-178, 1995 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of the hadronic cross section in $e^+e^-$ collisions by TOPAZ for 57.77 GeV.' +BibKey: Miyabayashi:1994ej +BibTeX: '@article{Miyabayashi:1994ej, + author = "Miyabayashi, K. and others", + title = "{Measurement of the total hadronic cross-section and + determination of gamma - Z interference in e+ e- + annihilation}", + collaboration = "TOPAZ", + journal = "Phys. Lett.", + volume = "B347", + year = "1995", + pages = "171-178", + doi = "10.1016/0370-2693(95)00038-M", + reportNumber = "DPNU-94-47, NWU-HEP-94-06, KEK-PREPRINT-94-152, + TUAT-HEP-94-05, TIT-HPE-94-11, OCU-HEP-94-09, PU-94-688, + INS-1074, KOBE-HEP-94-08", + SLACcitation = "%%CITATION = PHLTA,B347,171;%%" +}' diff --git a/analyses/pluginTristan/TOPAZ_1995_I381777.plot b/analyses/pluginTristan/TOPAZ_1995_I381777.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1995_I381777.plot @@ -0,0 +1,9 @@ +BEGIN PLOT /TOPAZ_1995_I381777/d01-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=57 +XMax=58 +END PLOT \ No newline at end of file diff --git a/analyses/pluginTristan/TOPAZ_1995_I381777.yoda b/analyses/pluginTristan/TOPAZ_1995_I381777.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/TOPAZ_1995_I381777.yoda @@ -0,0 +1,9 @@ +BEGIN YODA_SCATTER2D_V2 /REF/TOPAZ_1995_I381777/d01-x01-y01 +IsRef: 1 +Path: /REF/TOPAZ_1995_I381777/d01-x01-y01 +Title: doi:10.17182/hepdata.38368.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.777000e+01 0.000000e+00 0.000000e+00 1.436000e+02 4.743416e+00 4.743416e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginTristan/VENUS_1987_I251274.cc b/analyses/pluginTristan/VENUS_1987_I251274.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1987_I251274.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class VENUS_1987_I251274 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(VENUS_1987_I251274); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(VENUS_1987_I251274); + + +} diff --git a/analyses/pluginTristan/VENUS_1987_I251274.info b/analyses/pluginTristan/VENUS_1987_I251274.info new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1987_I251274.info @@ -0,0 +1,35 @@ +Name: VENUS_1987_I251274 +Year: 1987 +Summary: Measurement of $R$ for energies between 50 and 52 GeV +Experiment: VENUS +Collider: Tristan +InspireID: 251274 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B198 (1987) 570, 1987 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by VENUS for energies between 50 and 52 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Yoshida:1987sf +BibTeX: '@article{Yoshida:1987sf, + author = "Yoshida, H. and others", + title = "{Measurement of R and Search for New Heavy Quarks in $e^+ + e^-$ Annihilation at 50-{GeV} and 52-{GeV} Center-of-mass + Energies}", + collaboration = "Venus", + journal = "Phys. Lett.", + volume = "B198", + year = "1987", + pages = "570", + doi = "10.1016/0370-2693(87)90920-8", + reportNumber = "KEK-PREPRINT-87-81, KOBE-HEP-87-03, KUNS-893, OULNS-87-5, + TMUP-HEL-87-22", + SLACcitation = "%%CITATION = PHLTA,B198,570;%%" +}' diff --git a/analyses/pluginTristan/VENUS_1987_I251274.plot b/analyses/pluginTristan/VENUS_1987_I251274.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1987_I251274.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /VENUS_1987_I251274/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /VENUS_1987_I251274/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /VENUS_1987_I251274/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginTristan/VENUS_1987_I251274.yoda b/analyses/pluginTristan/VENUS_1987_I251274.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1987_I251274.yoda @@ -0,0 +1,10 @@ +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1987_I251274/d01-x01-y01 +IsRef: 1 +Path: /REF/VENUS_1987_I251274/d01-x01-y01 +Title: doi:10.17182/hepdata.30074.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.000000e+01 0.000000e+00 0.000000e+00 4.400000e+00 6.403124e-01 6.403124e-01 +5.200000e+01 0.000000e+00 0.000000e+00 4.700000e+00 5.830952e-01 5.830952e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginTristan/VENUS_1990_I283774.cc b/analyses/pluginTristan/VENUS_1990_I283774.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1990_I283774.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class VENUS_1990_I283774 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(VENUS_1990_I283774); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(VENUS_1990_I283774); + + +} diff --git a/analyses/pluginTristan/VENUS_1990_I283774.info b/analyses/pluginTristan/VENUS_1990_I283774.info new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1990_I283774.info @@ -0,0 +1,35 @@ +Name: VENUS_1990_I283774 +Year: 1990 +Summary: Measurement of $R$ for energies between 50 and 61.4 GeV +Experiment: VENUS +Collider: Tristan +InspireID: 283774 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B234 (1990) 382-388, 1990 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by VENUS for energies between 50 and 61.4 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Abe:1989qx +BibTeX: '@article{Abe:1989qx, + author = "Abe, K. and others", + title = "{Measurement of R and Search for New Quark Flavors + Decaying Into Multi - Jet Final States in $e^+ e^-$ + Collisions Between 54-{GeV} and 61.4-{GeV} c.m. Energies}", + collaboration = "VENUS", + journal = "Phys. Lett.", + volume = "B234", + year = "1990", + pages = "382-388", + doi = "10.1016/0370-2693(90)91946-9", + reportNumber = "KEK-PREPRINT-89-135, HUPD-8916, KOBE-HEP-89-09, KUNS-990, + OULNS-89-10, TMUP-HEL-89-31", + SLACcitation = "%%CITATION = PHLTA,B234,382;%%" +}' diff --git a/analyses/pluginTristan/VENUS_1990_I283774.plot b/analyses/pluginTristan/VENUS_1990_I283774.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1990_I283774.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /VENUS_1990_I283774/d01-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /VENUS_1990_I283774/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /VENUS_1990_I283774/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginTristan/VENUS_1990_I283774.yoda b/analyses/pluginTristan/VENUS_1990_I283774.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1990_I283774.yoda @@ -0,0 +1,19 @@ +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1990_I283774/d01-x01-y01 +IsRef: 1 +Path: /REF/VENUS_1990_I283774/d01-x01-y01 +Title: doi:10.17182/hepdata.29755.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.400000e+01 0.000000e+00 0.000000e+00 4.690000e+00 4.400000e-01 4.400000e-01 +5.500000e+01 0.000000e+00 0.000000e+00 4.320000e+00 3.000000e-01 3.000000e-01 +5.600000e+01 0.000000e+00 0.000000e+00 4.660000e+00 1.800000e-01 1.800000e-01 +5.650000e+01 0.000000e+00 0.000000e+00 3.940000e+00 4.100000e-01 4.100000e-01 +5.700000e+01 0.000000e+00 0.000000e+00 4.990000e+00 2.200000e-01 2.200000e-01 +5.850000e+01 0.000000e+00 0.000000e+00 4.920000e+00 4.300000e-01 4.300000e-01 +5.900000e+01 0.000000e+00 0.000000e+00 4.860000e+00 4.600000e-01 4.600000e-01 +5.905000e+01 0.000000e+00 0.000000e+00 6.070000e+00 6.500000e-01 6.500000e-01 +6.000000e+01 0.000000e+00 0.000000e+00 5.290000e+00 2.500000e-01 2.500000e-01 +6.080000e+01 0.000000e+00 0.000000e+00 5.700000e+00 2.400000e-01 2.400000e-01 +6.140000e+01 0.000000e+00 0.000000e+00 5.010000e+00 2.100000e-01 2.100000e-01 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginTristan/VENUS_1990_I296392.cc b/analyses/pluginTristan/VENUS_1990_I296392.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1990_I296392.cc @@ -0,0 +1,99 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class VENUS_1990_I296392 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(VENUS_1990_I296392); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + _c_muons = bookCounter("/TMP/sigma_muons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + _c_muons->fill(event.weight()); + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + Scatter1D R = *_c_hadrons/ *_c_muons; + double rval = R.point(0).x(); + pair rerr = R.point(0).xErrs(); + double fact = crossSection()/ sumOfWeights() /picobarn; + double sig_h = _c_hadrons->val()*fact; + double err_h = _c_hadrons->err()*fact; + double sig_m = _c_muons ->val()*fact; + double err_m = _c_muons ->err()*fact; + Scatter2D temphisto(refData(3, 1, 1)); + Scatter2DPtr hadrons = bookScatter2D("sigma_hadrons"); + Scatter2DPtr muons = bookScatter2D("sigma_muons" ); + Scatter2DPtr mult = bookScatter2D(3, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, rval, ex, rerr); + hadrons->addPoint(x, sig_h, ex, make_pair(err_h,err_h)); + muons ->addPoint(x, sig_m, ex, make_pair(err_m,err_m)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + hadrons->addPoint(x, 0., ex, make_pair(0.,.0)); + muons ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons, _c_muons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(VENUS_1990_I296392); + + +} diff --git a/analyses/pluginTristan/VENUS_1990_I296392.info b/analyses/pluginTristan/VENUS_1990_I296392.info new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1990_I296392.info @@ -0,0 +1,34 @@ +Name: VENUS_1990_I296392 +Year: 1990 +Summary: Measurement of $R$ for energies between 50 and 64 GeV +Experiment: VENUS +Collider: Tristan +InspireID: 296392 +Status: VALIDATED +Authors: + - Peter Richardson +References: + - Phys.Lett. B246 (1990) 297-305, 1990 +RunInfo: e+ e- to hadrons and e+ e- to mu+ mu- (for normalization) +NeedCrossSection: no +Beams: [e-, e+] +Description: + 'Measurement of $R$ in $e^+e^-$ collisions by VENUS for energies between 50 and 64 GeV. + The individual hadronic and muonic cross sections are also outputted to the yoda file + so that ratio $R$ can be recalcuated if runs are combined.' +Keywords: [] +BibKey: Abe:1990rr +BibTeX: '@article{Abe:1990rr, + author = "Abe, K. and others", + title = "{Experimental limits on extra $Z$ bosons from $e^{+} + e^{-}$ annihilation data with the VENUS detector at + $\sqrt{s}$ = 50-GeV to approximately 64-GeV}", + collaboration = "VENUS", + journal = "Phys. Lett.", + volume = "B246", + year = "1990", + pages = "297-305", + doi = "10.1016/0370-2693(90)91348-F", + reportNumber = "KEK-PREPRINT-90-34", + SLACcitation = "%%CITATION = PHLTA,B246,297;%%" +}' diff --git a/analyses/pluginTristan/VENUS_1990_I296392.plot b/analyses/pluginTristan/VENUS_1990_I296392.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1990_I296392.plot @@ -0,0 +1,21 @@ +BEGIN PLOT /VENUS_1990_I296392/d03-x01-y01 +Title=$R=\sigma(e^+e^-\to \text{hadrons})/\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$R$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /VENUS_1990_I296392/sigma_hadrons +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +END PLOT +BEGIN PLOT /VENUS_1990_I296392/sigma_muons +Title=$\sigma(e^+e^-\to \mu^+\mu^-)$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \mu^+\mu^-)/pb$ +LogY=0 +ConnectGaps=1 +END PLOT diff --git a/analyses/pluginTristan/VENUS_1990_I296392.yoda b/analyses/pluginTristan/VENUS_1990_I296392.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1990_I296392.yoda @@ -0,0 +1,102 @@ +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1990_I296392/d01-x01-y01 +IsRef: 1 +Path: /REF/VENUS_1990_I296392/d01-x01-y01 +Title: doi:10.17182/hepdata.29664.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.140000e+01 0.000000e+00 0.000000e+00 1.110000e+00 1.581139e-01 1.581139e-01 +6.360000e+01 0.000000e+00 0.000000e+00 9.300000e-01 3.373426e-01 3.373426e-01 +6.400000e+01 0.000000e+00 0.000000e+00 1.290000e+00 2.789265e-01 2.789265e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1990_I296392/d01-x01-y02 +IsRef: 1 +Path: /REF/VENUS_1990_I296392/d01-x01-y02 +Title: doi:10.17182/hepdata.29664.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.140000e+01 0.000000e+00 0.000000e+00 1.210000e+00 2.061553e-01 2.061553e-01 +6.360000e+01 0.000000e+00 0.000000e+00 7.100000e-01 3.847077e-01 3.847077e-01 +6.400000e+01 0.000000e+00 0.000000e+00 1.190000e+00 3.373426e-01 3.373426e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1990_I296392/d02-x01-y01 +IsRef: 1 +Path: /REF/VENUS_1990_I296392/d02-x01-y01 +Title: doi:10.17182/hepdata.29664.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.140000e+01 0.000000e+00 0.000000e+00 -3.500000e-01 1.400000e-01 1.400000e-01 +6.360000e+01 0.000000e+00 0.000000e+00 -9.000000e-02 4.500000e-01 4.500000e-01 +6.400000e+01 0.000000e+00 0.000000e+00 1.100000e-01 2.300000e-01 2.300000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1990_I296392/d02-x01-y02 +IsRef: 1 +Path: /REF/VENUS_1990_I296392/d02-x01-y02 +Title: doi:10.17182/hepdata.29664.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.140000e+01 0.000000e+00 0.000000e+00 -6.700000e-01 1.000000e-01 1.000000e-01 +6.360000e+01 0.000000e+00 0.000000e+00 -5.000000e-02 4.600000e-01 4.900000e-01 +6.400000e+01 0.000000e+00 0.000000e+00 -9.000000e-02 3.500000e-01 3.500000e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1990_I296392/d03-x01-y01 +IsRef: 1 +Path: /REF/VENUS_1990_I296392/d03-x01-y01 +Title: doi:10.17182/hepdata.29664.v1/t3 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +6.360000e+01 0.000000e+00 0.000000e+00 6.160000e+00 7.093659e-01 7.093659e-01 +6.400000e+01 0.000000e+00 0.000000e+00 5.850000e+00 5.147815e-01 5.147815e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1990_I296392/d04-x01-y01 +IsRef: 1 +Path: /REF/VENUS_1990_I296392/d04-x01-y01 +Title: doi:10.17182/hepdata.29664.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.290000e+01 0.000000e+00 0.000000e+00 1.180000e+00 1.077033e-01 1.077033e-01 +5.640000e+01 0.000000e+00 0.000000e+00 1.050000e+00 8.544004e-02 8.544004e-02 +5.940000e+01 0.000000e+00 0.000000e+00 9.700000e-01 1.044031e-01 1.044031e-01 +6.160000e+01 0.000000e+00 0.000000e+00 1.070000e+00 9.848858e-02 9.848858e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1990_I296392/d04-x01-y02 +IsRef: 1 +Path: /REF/VENUS_1990_I296392/d04-x01-y02 +Title: doi:10.17182/hepdata.29664.v1/t4 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.290000e+01 0.000000e+00 0.000000e+00 1.130000e+00 1.456022e-01 1.456022e-01 +5.640000e+01 0.000000e+00 0.000000e+00 1.010000e+00 1.077033e-01 1.077033e-01 +5.940000e+01 0.000000e+00 0.000000e+00 9.300000e-01 1.360147e-01 1.360147e-01 +6.160000e+01 0.000000e+00 0.000000e+00 1.100000e+00 1.264911e-01 1.264911e-01 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1990_I296392/d05-x01-y01 +IsRef: 1 +Path: /REF/VENUS_1990_I296392/d05-x01-y01 +Title: doi:10.17182/hepdata.29664.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.290000e+01 0.000000e+00 0.000000e+00 -3.300000e-01 9.000000e-02 9.000000e-02 +5.640000e+01 0.000000e+00 0.000000e+00 -2.700000e-01 8.000000e-02 8.000000e-02 +5.940000e+01 0.000000e+00 0.000000e+00 -3.000000e-01 1.000000e-01 1.000000e-01 +6.160000e+01 0.000000e+00 0.000000e+00 -2.300000e-01 9.000000e-02 9.000000e-02 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1990_I296392/d05-x01-y02 +IsRef: 1 +Path: /REF/VENUS_1990_I296392/d05-x01-y02 +Title: doi:10.17182/hepdata.29664.v1/t5 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.290000e+01 0.000000e+00 0.000000e+00 -2.300000e-01 1.200000e-01 1.200000e-01 +5.640000e+01 0.000000e+00 0.000000e+00 -3.100000e-01 1.100000e-01 1.100000e-01 +5.940000e+01 0.000000e+00 0.000000e+00 -2.900000e-01 1.400000e-01 1.400000e-01 +6.160000e+01 0.000000e+00 0.000000e+00 -5.700000e-01 9.000000e-02 9.000000e-02 +END YODA_SCATTER2D_V2 diff --git a/analyses/pluginTristan/VENUS_1999_I500179.cc b/analyses/pluginTristan/VENUS_1999_I500179.cc new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1999_I500179.cc @@ -0,0 +1,87 @@ +// -*- C++ -*- +#include "Rivet/Analysis.hh" +#include "Rivet/Projections/FinalState.hh" + +namespace Rivet { + + + /// @brief Add a short analysis description here + class VENUS_1999_I500179 : public Analysis { + public: + + /// Constructor + DEFAULT_RIVET_ANALYSIS_CTOR(VENUS_1999_I500179); + + + /// @name Analysis methods + //@{ + + /// Book histograms and initialise projections before the run + void init() { + // Initialise and register projections + declare(FinalState(), "FS"); + + // Book histograms + _c_hadrons = bookCounter("/TMP/sigma_hadrons"); + } + + + /// Perform the per-event analysis + void analyze(const Event& event) { + const FinalState& fs = apply(event, "FS"); + + map nCount; + int ntotal(0); + foreach (const Particle& p, fs.particles()) { + nCount[p.pdgId()] += 1; + ++ntotal; + } + // mu+mu- + photons + if(nCount[-13]==1 and nCount[13]==1 && + ntotal==2+nCount[22]) + vetoEvent; + // everything else + else + _c_hadrons->fill(event.weight()); + } + + + /// Normalise histograms etc., after the run + void finalize() { + double fact = crossSection()/ sumOfWeights() /picobarn; + double sigma = _c_hadrons->val()*fact; + double error = _c_hadrons->err()*fact; + Scatter2D temphisto(refData(1, 1, 1)); + Scatter2DPtr mult = bookScatter2D(1, 1, 1); + for (size_t b = 0; b < temphisto.numPoints(); b++) { + const double x = temphisto.point(b).x(); + pair ex = temphisto.point(b).xErrs(); + pair ex2 = ex; + if(ex2.first ==0.) ex2. first=0.0001; + if(ex2.second==0.) ex2.second=0.0001; + if (inRange(sqrtS()/GeV, x-ex2.first, x+ex2.second)) { + mult ->addPoint(x, sigma, ex, make_pair(error,error)); + } + else { + mult ->addPoint(x, 0., ex, make_pair(0.,.0)); + } + } + } + + //@} + + + /// @name Histograms + //@{ + CounterPtr _c_hadrons; + //@} + + + }; + + + // The hook for the plugin system + DECLARE_RIVET_PLUGIN(VENUS_1999_I500179); + + +} diff --git a/analyses/pluginTristan/VENUS_1999_I500179.info b/analyses/pluginTristan/VENUS_1999_I500179.info new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1999_I500179.info @@ -0,0 +1,28 @@ +Name: VENUS_1999_I500179 +Year: 1999 +Summary: Cross section in $e^+e^-\to$hadrons for 57.77 GeV +Experiment: VENUS +Collider: Tristan +InspireID: 500179 +Authors: + - Peter Richardson +References: + - Phys.Lett. B198 (1987) 570, 1987 +RunInfo: e+ e- to hadrons +NeedCrossSection: yes +Beams: [e-, e+] +Description: + 'Measurement of the hadronic cross section in $e^+e^-$ collisions by VENUS for 57.77 GeV.' +BibKey: Yusa:1999dx +BibTeX: '@article{Yusa:1999dx, + author = "Yusa, K. and others", + title = "{Precise measurement of the total hadronic cross-section + in e+ e- annihilation at s**(1/2) = 57.77-GeV}", + collaboration = "VENUS", + journal = "Phys. Lett.", + volume = "B447", + year = "1999", + pages = "167-177", + doi = "10.1016/S0370-2693(98)01560-3", + SLACcitation = "%%CITATION = PHLTA,B447,167;%%" +}' diff --git a/analyses/pluginTristan/VENUS_1999_I500179.plot b/analyses/pluginTristan/VENUS_1999_I500179.plot new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1999_I500179.plot @@ -0,0 +1,9 @@ +BEGIN PLOT /VENUS_1999_I500179/d01-x01-y01 +Title=$\sigma(e^+e^-\to \text{hadrons})$ +XLabel=$\sqrt{s}$/GeV +YLabel=$\sigma(e^+e^-\to \text{hadrons})/pb$ +LogY=0 +ConnectGaps=1 +XMin=57 +XMax=58 +END PLOT diff --git a/analyses/pluginTristan/VENUS_1999_I500179.yoda b/analyses/pluginTristan/VENUS_1999_I500179.yoda new file mode 100644 --- /dev/null +++ b/analyses/pluginTristan/VENUS_1999_I500179.yoda @@ -0,0 +1,18 @@ +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1999_I500179/d01-x01-y01 +IsRef: 1 +Path: /REF/VENUS_1999_I500179/d01-x01-y01 +Title: doi:10.17182/hepdata.5548.v1/t1 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +5.777000e+01 0.000000e+00 0.000000e+00 1.403000e+02 1.800000e+00 1.800000e+00 +END YODA_SCATTER2D_V2 +BEGIN YODA_SCATTER2D_V2 /REF/VENUS_1999_I500179/d02-x01-y01 +IsRef: 1 +Path: /REF/VENUS_1999_I500179/d02-x01-y01 +Title: doi:10.17182/hepdata.5548.v1/t2 +Type: Scatter2D +--- +# xval xerr- xerr+ yval yerr- yerr+ +1.000000e+00 5.000000e-01 5.000000e-01 1.403000e+02 1.800000e+00 1.800000e+00 +END YODA_SCATTER2D_V2 diff --git a/analyses/valref/ALEPH_1999_S4193598.yoda b/analyses/valref/ALEPH_1999_S4193598.yoda --- a/analyses/valref/ALEPH_1999_S4193598.yoda +++ b/analyses/valref/ALEPH_1999_S4193598.yoda @@ -1,69 +1,69 @@ BEGIN YODA_HISTO1D_V2 /RAW/ALEPH_1999_S4193598/d01-x01-y01 Path: /RAW/ALEPH_1999_S4193598/d01-x01-y01 -ScaledBy: 2.82954545454545451e-05 +ScaledBy: 2.82954545454545472e-02 Title: ~ Type: Histo1D XLabel: ~ YLabel: ~ --- # Mean: 3.573089e-01 # Area: 1.760000e+02 # ID ID sumw sumw2 sumwx sumwx2 numEntries Total Total 1.760000e+02 1.760000e+02 6.288636e+01 2.793199e+01 1.760000e+02 Underflow Underflow 7.000000e+00 7.000000e+00 4.534084e-01 3.039791e-02 7.000000e+00 Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 # xlow xhigh sumw sumw2 sumwx sumwx2 numEntries 1.000000e-01 1.500000e-01 1.000000e+01 1.000000e+01 1.239129e+00 1.549535e-01 1.000000e+01 1.500000e-01 2.000000e-01 1.400000e+01 1.400000e+01 2.394899e+00 4.119541e-01 1.400000e+01 2.000000e-01 2.500000e-01 1.900000e+01 1.900000e+01 4.214117e+00 9.378261e-01 1.900000e+01 2.500000e-01 3.000000e-01 1.700000e+01 1.700000e+01 4.622516e+00 1.259254e+00 1.700000e+01 3.000000e-01 3.500000e-01 3.200000e+01 3.200000e+01 1.034310e+01 3.351269e+00 3.200000e+01 3.500000e-01 4.000000e-01 2.000000e+01 2.000000e+01 7.442032e+00 2.772880e+00 2.000000e+01 4.000000e-01 4.500000e-01 1.300000e+01 1.300000e+01 5.560047e+00 2.381113e+00 1.300000e+01 4.500000e-01 5.000000e-01 1.000000e+01 1.000000e+01 4.730159e+00 2.240036e+00 1.000000e+01 5.000000e-01 5.500000e-01 7.000000e+00 7.000000e+00 3.652235e+00 1.906559e+00 7.000000e+00 5.500000e-01 6.000000e-01 3.000000e+00 3.000000e+00 1.734239e+00 1.003272e+00 3.000000e+00 6.000000e-01 6.500000e-01 9.000000e+00 9.000000e+00 5.551161e+00 3.425534e+00 9.000000e+00 6.500000e-01 7.000000e-01 6.000000e+00 6.000000e+00 4.031682e+00 2.710226e+00 6.000000e+00 7.000000e-01 7.500000e-01 5.000000e+00 5.000000e+00 3.619059e+00 2.620297e+00 5.000000e+00 7.500000e-01 8.000000e-01 1.000000e+00 1.000000e+00 7.736032e-01 5.984619e-01 1.000000e+00 8.000000e-01 8.500000e-01 1.000000e+00 1.000000e+00 8.003207e-01 6.405132e-01 1.000000e+00 8.500000e-01 9.000000e-01 2.000000e+00 2.000000e+00 1.724655e+00 1.487447e+00 2.000000e+00 9.000000e-01 9.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 9.500000e-01 1.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 END YODA_HISTO1D_V2 BEGIN YODA_HISTO1D_V2 /ALEPH_1999_S4193598/d01-x01-y01 Path: /ALEPH_1999_S4193598/d01-x01-y01 -ScaledBy: 2.82954545454545451e-05 +ScaledBy: 2.82954545454545472e-02 Title: ~ Type: Histo1D XLabel: ~ YLabel: ~ --- # Mean: 3.573088e-01 -# Area: 4.980000e-03 +# Area: 4.980000e+00 # ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 4.980000e-03 1.409114e-07 1.779398e-03 7.903484e-04 1.760000e+02 -Underflow Underflow 1.980682e-04 5.604429e-09 1.282940e-05 8.601226e-07 7.000000e+00 +Total Total 4.980000e+00 1.409114e-01 1.779398e+00 7.903484e-01 1.760000e+02 +Underflow Underflow 1.980682e-01 5.604429e-03 1.282940e-02 8.601226e-04 7.000000e+00 Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 # xlow xhigh sumw sumw2 sumwx sumwx2 numEntries -1.000000e-01 1.500000e-01 2.829545e-04 8.006327e-09 3.506173e-05 4.384479e-06 1.000000e+01 -1.500000e-01 2.000000e-01 3.961364e-04 1.120886e-08 6.776476e-05 1.165643e-05 1.400000e+01 -2.000000e-01 2.500000e-01 5.376136e-04 1.521202e-08 1.192404e-04 2.653622e-05 1.900000e+01 -2.500000e-01 3.000000e-01 4.810227e-04 1.361076e-08 1.307962e-04 3.563117e-05 1.700000e+01 -3.000000e-01 3.500000e-01 9.054545e-04 2.562025e-08 2.926626e-04 9.482568e-05 3.200000e+01 -3.500000e-01 4.000000e-01 5.659091e-04 1.601265e-08 2.105757e-04 7.845990e-05 2.000000e+01 -4.000000e-01 4.500000e-01 3.678409e-04 1.040823e-08 1.573241e-04 6.737468e-05 1.300000e+01 -4.500000e-01 5.000000e-01 2.829545e-04 8.006327e-09 1.338420e-04 6.338283e-05 1.000000e+01 -5.000000e-01 5.500000e-01 1.980682e-04 5.604429e-09 1.033416e-04 5.394695e-05 7.000000e+00 -5.500000e-01 6.000000e-01 8.488636e-05 2.401898e-09 4.907108e-05 2.838805e-05 3.000000e+00 -6.000000e-01 6.500000e-01 2.546591e-04 7.205695e-09 1.570726e-04 9.692704e-05 9.000000e+00 -6.500000e-01 7.000000e-01 1.697727e-04 4.803796e-09 1.140783e-04 7.668708e-05 6.000000e+00 -7.000000e-01 7.500000e-01 1.414773e-04 4.003164e-09 1.024029e-04 7.414249e-05 5.000000e+00 -7.500000e-01 8.000000e-01 2.829545e-05 8.006327e-10 2.188945e-05 1.693375e-05 1.000000e+00 -8.000000e-01 8.500000e-01 2.829545e-05 8.006327e-10 2.264544e-05 1.812361e-05 1.000000e+00 -8.500000e-01 9.000000e-01 5.659091e-05 1.601265e-09 4.879990e-05 4.208797e-05 2.000000e+00 +1.000000e-01 1.500000e-01 2.829545e-01 8.006327e-03 3.506173e-02 4.384479e-03 1.000000e+01 +1.500000e-01 2.000000e-01 3.961364e-01 1.120886e-02 6.776476e-02 1.165643e-02 1.400000e+01 +2.000000e-01 2.500000e-01 5.376136e-01 1.521202e-02 1.192404e-01 2.653622e-02 1.900000e+01 +2.500000e-01 3.000000e-01 4.810227e-01 1.361076e-02 1.307962e-01 3.563117e-02 1.700000e+01 +3.000000e-01 3.500000e-01 9.054545e-01 2.562025e-02 2.926626e-01 9.482568e-02 3.200000e+01 +3.500000e-01 4.000000e-01 5.659091e-01 1.601265e-02 2.105757e-01 7.845990e-02 2.000000e+01 +4.000000e-01 4.500000e-01 3.678409e-01 1.040823e-02 1.573241e-01 6.737468e-02 1.300000e+01 +4.500000e-01 5.000000e-01 2.829545e-01 8.006327e-03 1.338420e-01 6.338283e-02 1.000000e+01 +5.000000e-01 5.500000e-01 1.980682e-01 5.604429e-03 1.033416e-01 5.394695e-02 7.000000e+00 +5.500000e-01 6.000000e-01 8.488636e-02 2.401898e-03 4.907108e-02 2.838805e-02 3.000000e+00 +6.000000e-01 6.500000e-01 2.546591e-01 7.205695e-03 1.570726e-01 9.692704e-02 9.000000e+00 +6.500000e-01 7.000000e-01 1.697727e-01 4.803796e-03 1.140783e-01 7.668708e-02 6.000000e+00 +7.000000e-01 7.500000e-01 1.414773e-01 4.003164e-03 1.024029e-01 7.414249e-02 5.000000e+00 +7.500000e-01 8.000000e-01 2.829545e-02 8.006327e-04 2.188945e-02 1.693375e-02 1.000000e+00 +8.000000e-01 8.500000e-01 2.829545e-02 8.006327e-04 2.264544e-02 1.812361e-02 1.000000e+00 +8.500000e-01 9.000000e-01 5.659091e-02 1.601265e-03 4.879990e-02 4.208797e-02 2.000000e+00 9.000000e-01 9.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 9.500000e-01 1.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 END YODA_HISTO1D_V2 diff --git a/analyses/valref/OPAL_2004_I631361-8.yoda b/analyses/valref/OPAL_2004_I631361-8.yoda new file mode 100644 --- /dev/null +++ b/analyses/valref/OPAL_2004_I631361-8.yoda @@ -0,0 +1,593 @@ +BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361:PROCESS=QQ/d03-x01-y01 +Path: /OPAL_2004_I631361:PROCESS=QQ/d03-x01-y01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361:PROCESS=QQ/d03-x01-y02 +Path: /RAW/OPAL_2004_I631361:PROCESS=QQ/d03-x01-y02 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361:PROCESS=QQ/d03-x01-y01 +Path: /RAW/OPAL_2004_I631361:PROCESS=QQ/d03-x01-y01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361:PROCESS=QQ/d01-x01-y02 +Path: /RAW/OPAL_2004_I631361:PROCESS=QQ/d01-x01-y02 +ScaledBy: 1.25000000000000000e-01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: 4.125000e+00 +# Area: 8.000000e+00 +# ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 8.000000e+00 8.000000e+00 3.300000e+01 1.750000e+02 8.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 1.000000e+00 1.000000e+00 1.000000e+00 1.000000e+00 1.000000e+00 +1.500000e+00 2.500000e+00 2.000000e+00 2.000000e+00 4.000000e+00 8.000000e+00 2.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 2.000000e+00 2.000000e+00 8.000000e+00 3.200000e+01 2.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 1.000000e+00 1.000000e+00 6.000000e+00 3.600000e+01 1.000000e+00 +6.500000e+00 7.500000e+00 2.000000e+00 2.000000e+00 1.400000e+01 9.800000e+01 2.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361:PROCESS=QQ/d05-x01-y01 +Path: /RAW/OPAL_2004_I631361:PROCESS=QQ/d05-x01-y01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +0.000000e+00 1.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.000000e-02 2.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.000000e-02 3.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.000000e-02 4.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.000000e-02 5.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-02 6.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.000000e-02 7.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.000000e-02 8.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.000000e-02 9.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.000000e-02 1.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.000000e-01 1.200000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.200000e-01 1.400000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.400000e-01 1.600000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.600000e-01 1.800000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.800000e-01 2.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.000000e-01 2.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e-01 3.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.000000e-01 4.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 6.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.000000e-01 8.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.000000e-01 1.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361:PROCESS=QQ/d03-x01-y02 +Path: /OPAL_2004_I631361:PROCESS=QQ/d03-x01-y02 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361:PROCESS=QQ/d02-x01-y01 +Path: /RAW/OPAL_2004_I631361:PROCESS=QQ/d02-x01-y01 +ScaledBy: 1.00000000000000000e+00 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: 5.000000e+00 +# Area: 1.000000e+00 +# ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 1.000000e+00 1.000000e+00 5.000000e+00 2.500000e+01 1.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.500000e+00 5.500000e+00 1.000000e+00 1.000000e+00 5.000000e+00 2.500000e+01 1.000000e+00 +5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361:PROCESS=QQ/d01-x01-y01 +Path: /OPAL_2004_I631361:PROCESS=QQ/d01-x01-y01 +ScaledBy: 2.50000000000000000e-01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: 4.500000e+00 +# Area: 1.000000e+00 +# ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 1.000000e+00 2.500000e-01 4.500000e+00 2.250000e+01 4.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e+00 3.500000e+00 2.500000e-01 6.250000e-02 7.500000e-01 2.250000e+00 1.000000e+00 +3.500000e+00 4.500000e+00 5.000000e-01 1.250000e-01 2.000000e+00 8.000000e+00 2.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.500000e+00 7.500000e+00 2.500000e-01 6.250000e-02 1.750000e+00 1.225000e+01 1.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361:PROCESS=QQ/d01-x01-y02 +Path: /OPAL_2004_I631361:PROCESS=QQ/d01-x01-y02 +ScaledBy: 1.25000000000000000e-01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: 4.125000e+00 +# Area: 1.000000e+00 +# ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 1.000000e+00 1.250000e-01 4.125000e+00 2.187500e+01 8.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 1.250000e-01 1.562500e-02 1.250000e-01 1.250000e-01 1.000000e+00 +1.500000e+00 2.500000e+00 2.500000e-01 3.125000e-02 5.000000e-01 1.000000e+00 2.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 2.500000e-01 3.125000e-02 1.000000e+00 4.000000e+00 2.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 1.250000e-01 1.562500e-02 7.500000e-01 4.500000e+00 1.000000e+00 +6.500000e+00 7.500000e+00 2.500000e-01 3.125000e-02 1.750000e+00 1.225000e+01 2.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361:PROCESS=QQ/d01-x01-y03 +Path: /OPAL_2004_I631361:PROCESS=QQ/d01-x01-y03 +ScaledBy: 3.33333333333333315e-01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: 5.000000e+00 +# Area: 1.000000e+00 +# ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 1.000000e+00 3.333333e-01 5.000000e+00 2.966667e+01 3.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 3.333333e-01 1.111111e-01 6.666667e-01 1.333333e+00 1.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 3.333333e-01 1.111111e-01 2.000000e+00 1.200000e+01 1.000000e+00 +6.500000e+00 7.500000e+00 3.333333e-01 1.111111e-01 2.333333e+00 1.633333e+01 1.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361:PROCESS=QQ/d01-x01-y01 +Path: /RAW/OPAL_2004_I631361:PROCESS=QQ/d01-x01-y01 +ScaledBy: 2.50000000000000000e-01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: 4.500000e+00 +# Area: 4.000000e+00 +# ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 4.000000e+00 4.000000e+00 1.800000e+01 9.000000e+01 4.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e+00 3.500000e+00 1.000000e+00 1.000000e+00 3.000000e+00 9.000000e+00 1.000000e+00 +3.500000e+00 4.500000e+00 2.000000e+00 2.000000e+00 8.000000e+00 3.200000e+01 2.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.500000e+00 7.500000e+00 1.000000e+00 1.000000e+00 7.000000e+00 4.900000e+01 1.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361:PROCESS=QQ/d01-x01-y03 +Path: /RAW/OPAL_2004_I631361:PROCESS=QQ/d01-x01-y03 +ScaledBy: 3.33333333333333315e-01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: 5.000000e+00 +# Area: 3.000000e+00 +# ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 3.000000e+00 3.000000e+00 1.500000e+01 8.900000e+01 3.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 1.000000e+00 1.000000e+00 2.000000e+00 4.000000e+00 1.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 1.000000e+00 1.000000e+00 6.000000e+00 3.600000e+01 1.000000e+00 +6.500000e+00 7.500000e+00 1.000000e+00 1.000000e+00 7.000000e+00 4.900000e+01 1.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361:PROCESS=QQ/d02-x01-y02 +Path: /RAW/OPAL_2004_I631361:PROCESS=QQ/d02-x01-y02 +ScaledBy: 2.50000000000000000e-01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: 6.750000e+00 +# Area: 4.000000e+00 +# ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 4.000000e+00 4.000000e+00 2.700000e+01 2.250000e+02 4.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 1.000000e+00 1.000000e+00 2.000000e+00 4.000000e+00 1.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 1.000000e+00 1.000000e+00 6.000000e+00 3.600000e+01 1.000000e+00 +6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.500000e+00 8.500000e+00 1.000000e+00 1.000000e+00 8.000000e+00 6.400000e+01 1.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 1.000000e+00 1.000000e+00 1.100000e+01 1.210000e+02 1.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.650000e+01 1.750000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.750000e+01 1.850000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361:PROCESS=QQ/d05-x01-y02 +Path: /RAW/OPAL_2004_I631361:PROCESS=QQ/d05-x01-y02 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +0.000000e+00 1.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.000000e-02 2.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.000000e-02 3.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.000000e-02 4.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.000000e-02 5.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-02 6.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.000000e-02 7.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.000000e-02 8.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.000000e-02 9.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.000000e-02 1.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.000000e-01 1.200000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.200000e-01 1.400000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.400000e-01 1.600000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.600000e-01 1.800000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.800000e-01 2.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.000000e-01 2.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e-01 3.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.000000e-01 4.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 6.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.000000e-01 8.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361:PROCESS=QQ/d05-x01-y01 +Path: /OPAL_2004_I631361:PROCESS=QQ/d05-x01-y01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +0.000000e+00 1.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.000000e-02 2.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.000000e-02 3.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.000000e-02 4.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.000000e-02 5.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-02 6.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.000000e-02 7.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.000000e-02 8.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.000000e-02 9.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.000000e-02 1.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.000000e-01 1.200000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.200000e-01 1.400000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.400000e-01 1.600000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.600000e-01 1.800000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.800000e-01 2.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.000000e-01 2.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e-01 3.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.000000e-01 4.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 6.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.000000e-01 8.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.000000e-01 1.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361:PROCESS=QQ/d05-x01-y02 +Path: /OPAL_2004_I631361:PROCESS=QQ/d05-x01-y02 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +0.000000e+00 1.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.000000e-02 2.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.000000e-02 3.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.000000e-02 4.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.000000e-02 5.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-02 6.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.000000e-02 7.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.000000e-02 8.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.000000e-02 9.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.000000e-02 1.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.000000e-01 1.200000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.200000e-01 1.400000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.400000e-01 1.600000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.600000e-01 1.800000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.800000e-01 2.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.000000e-01 2.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e-01 3.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.000000e-01 4.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 6.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.000000e-01 8.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361:PROCESS=QQ/d02-x01-y02 +Path: /OPAL_2004_I631361:PROCESS=QQ/d02-x01-y02 +ScaledBy: 2.50000000000000000e-01 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: 6.750000e+00 +# Area: 1.000000e+00 +# ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 1.000000e+00 2.500000e-01 6.750000e+00 5.625000e+01 4.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 2.500000e-01 6.250000e-02 5.000000e-01 1.000000e+00 1.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.500000e+00 6.500000e+00 2.500000e-01 6.250000e-02 1.500000e+00 9.000000e+00 1.000000e+00 +6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.500000e+00 8.500000e+00 2.500000e-01 6.250000e-02 2.000000e+00 1.600000e+01 1.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 2.500000e-01 6.250000e-02 2.750000e+00 3.025000e+01 1.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.650000e+01 1.750000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.750000e+01 1.850000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 + +BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361:PROCESS=QQ/d02-x01-y01 +Path: /OPAL_2004_I631361:PROCESS=QQ/d02-x01-y01 +ScaledBy: 1.00000000000000000e+00 +Title: ~ +Type: Histo1D +XLabel: ~ +YLabel: ~ +--- +# Mean: 5.000000e+00 +# Area: 1.000000e+00 +# ID ID sumw sumw2 sumwx sumwx2 numEntries +Total Total 1.000000e+00 1.000000e+00 5.000000e+00 2.500000e+01 1.000000e+00 +Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries +-5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +4.500000e+00 5.500000e+00 1.000000e+00 1.000000e+00 5.000000e+00 2.500000e+01 1.000000e+00 +5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 +END YODA_HISTO1D_V2 diff --git a/analyses/valref/OPAL_2004_I631361_qq.yoda b/analyses/valref/OPAL_2004_I631361_qq.yoda deleted file mode 100644 --- a/analyses/valref/OPAL_2004_I631361_qq.yoda +++ /dev/null @@ -1,593 +0,0 @@ -BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361_qq/d03-x01-y01 -Path: /OPAL_2004_I631361_qq/d03-x01-y01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361_qq/d03-x01-y02 -Path: /RAW/OPAL_2004_I631361_qq/d03-x01-y02 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361_qq/d03-x01-y01 -Path: /RAW/OPAL_2004_I631361_qq/d03-x01-y01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361_qq/d01-x01-y02 -Path: /RAW/OPAL_2004_I631361_qq/d01-x01-y02 -ScaledBy: 1.25000000000000000e-01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: 4.125000e+00 -# Area: 8.000000e+00 -# ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 8.000000e+00 8.000000e+00 3.300000e+01 1.750000e+02 8.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 1.000000e+00 1.000000e+00 1.000000e+00 1.000000e+00 1.000000e+00 -1.500000e+00 2.500000e+00 2.000000e+00 2.000000e+00 4.000000e+00 8.000000e+00 2.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 2.000000e+00 2.000000e+00 8.000000e+00 3.200000e+01 2.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 1.000000e+00 1.000000e+00 6.000000e+00 3.600000e+01 1.000000e+00 -6.500000e+00 7.500000e+00 2.000000e+00 2.000000e+00 1.400000e+01 9.800000e+01 2.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361_qq/d05-x01-y01 -Path: /RAW/OPAL_2004_I631361_qq/d05-x01-y01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries -0.000000e+00 1.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.000000e-02 2.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.000000e-02 3.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.000000e-02 4.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.000000e-02 5.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-02 6.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.000000e-02 7.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.000000e-02 8.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.000000e-02 9.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.000000e-02 1.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.000000e-01 1.200000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.200000e-01 1.400000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.400000e-01 1.600000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.600000e-01 1.800000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.800000e-01 2.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.000000e-01 2.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e-01 3.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.000000e-01 4.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 6.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.000000e-01 8.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.000000e-01 1.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361_qq/d03-x01-y02 -Path: /OPAL_2004_I631361_qq/d03-x01-y02 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361_qq/d02-x01-y01 -Path: /RAW/OPAL_2004_I631361_qq/d02-x01-y01 -ScaledBy: 1.00000000000000000e+00 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: 5.000000e+00 -# Area: 1.000000e+00 -# ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 1.000000e+00 1.000000e+00 5.000000e+00 2.500000e+01 1.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.500000e+00 5.500000e+00 1.000000e+00 1.000000e+00 5.000000e+00 2.500000e+01 1.000000e+00 -5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361_qq/d01-x01-y01 -Path: /OPAL_2004_I631361_qq/d01-x01-y01 -ScaledBy: 2.50000000000000000e-01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: 4.500000e+00 -# Area: 1.000000e+00 -# ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 1.000000e+00 2.500000e-01 4.500000e+00 2.250000e+01 4.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e+00 3.500000e+00 2.500000e-01 6.250000e-02 7.500000e-01 2.250000e+00 1.000000e+00 -3.500000e+00 4.500000e+00 5.000000e-01 1.250000e-01 2.000000e+00 8.000000e+00 2.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.500000e+00 7.500000e+00 2.500000e-01 6.250000e-02 1.750000e+00 1.225000e+01 1.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361_qq/d01-x01-y02 -Path: /OPAL_2004_I631361_qq/d01-x01-y02 -ScaledBy: 1.25000000000000000e-01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: 4.125000e+00 -# Area: 1.000000e+00 -# ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 1.000000e+00 1.250000e-01 4.125000e+00 2.187500e+01 8.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 1.250000e-01 1.562500e-02 1.250000e-01 1.250000e-01 1.000000e+00 -1.500000e+00 2.500000e+00 2.500000e-01 3.125000e-02 5.000000e-01 1.000000e+00 2.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 2.500000e-01 3.125000e-02 1.000000e+00 4.000000e+00 2.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 1.250000e-01 1.562500e-02 7.500000e-01 4.500000e+00 1.000000e+00 -6.500000e+00 7.500000e+00 2.500000e-01 3.125000e-02 1.750000e+00 1.225000e+01 2.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361_qq/d01-x01-y03 -Path: /OPAL_2004_I631361_qq/d01-x01-y03 -ScaledBy: 3.33333333333333315e-01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: 5.000000e+00 -# Area: 1.000000e+00 -# ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 1.000000e+00 3.333333e-01 5.000000e+00 2.966667e+01 3.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 3.333333e-01 1.111111e-01 6.666667e-01 1.333333e+00 1.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 3.333333e-01 1.111111e-01 2.000000e+00 1.200000e+01 1.000000e+00 -6.500000e+00 7.500000e+00 3.333333e-01 1.111111e-01 2.333333e+00 1.633333e+01 1.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361_qq/d01-x01-y01 -Path: /RAW/OPAL_2004_I631361_qq/d01-x01-y01 -ScaledBy: 2.50000000000000000e-01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: 4.500000e+00 -# Area: 4.000000e+00 -# ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 4.000000e+00 4.000000e+00 1.800000e+01 9.000000e+01 4.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e+00 3.500000e+00 1.000000e+00 1.000000e+00 3.000000e+00 9.000000e+00 1.000000e+00 -3.500000e+00 4.500000e+00 2.000000e+00 2.000000e+00 8.000000e+00 3.200000e+01 2.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.500000e+00 7.500000e+00 1.000000e+00 1.000000e+00 7.000000e+00 4.900000e+01 1.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361_qq/d01-x01-y03 -Path: /RAW/OPAL_2004_I631361_qq/d01-x01-y03 -ScaledBy: 3.33333333333333315e-01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: 5.000000e+00 -# Area: 3.000000e+00 -# ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 3.000000e+00 3.000000e+00 1.500000e+01 8.900000e+01 3.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 1.000000e+00 1.000000e+00 2.000000e+00 4.000000e+00 1.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 1.000000e+00 1.000000e+00 6.000000e+00 3.600000e+01 1.000000e+00 -6.500000e+00 7.500000e+00 1.000000e+00 1.000000e+00 7.000000e+00 4.900000e+01 1.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361_qq/d02-x01-y02 -Path: /RAW/OPAL_2004_I631361_qq/d02-x01-y02 -ScaledBy: 2.50000000000000000e-01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: 6.750000e+00 -# Area: 4.000000e+00 -# ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 4.000000e+00 4.000000e+00 2.700000e+01 2.250000e+02 4.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 1.000000e+00 1.000000e+00 2.000000e+00 4.000000e+00 1.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 1.000000e+00 1.000000e+00 6.000000e+00 3.600000e+01 1.000000e+00 -6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.500000e+00 8.500000e+00 1.000000e+00 1.000000e+00 8.000000e+00 6.400000e+01 1.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 1.000000e+00 1.000000e+00 1.100000e+01 1.210000e+02 1.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.650000e+01 1.750000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.750000e+01 1.850000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /RAW/OPAL_2004_I631361_qq/d05-x01-y02 -Path: /RAW/OPAL_2004_I631361_qq/d05-x01-y02 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries -0.000000e+00 1.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.000000e-02 2.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.000000e-02 3.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.000000e-02 4.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.000000e-02 5.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-02 6.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.000000e-02 7.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.000000e-02 8.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.000000e-02 9.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.000000e-02 1.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.000000e-01 1.200000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.200000e-01 1.400000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.400000e-01 1.600000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.600000e-01 1.800000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.800000e-01 2.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.000000e-01 2.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e-01 3.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.000000e-01 4.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 6.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.000000e-01 8.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361_qq/d05-x01-y01 -Path: /OPAL_2004_I631361_qq/d05-x01-y01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries -0.000000e+00 1.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.000000e-02 2.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.000000e-02 3.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.000000e-02 4.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.000000e-02 5.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-02 6.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.000000e-02 7.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.000000e-02 8.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.000000e-02 9.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.000000e-02 1.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.000000e-01 1.200000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.200000e-01 1.400000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.400000e-01 1.600000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.600000e-01 1.800000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.800000e-01 2.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.000000e-01 2.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e-01 3.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.000000e-01 4.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 6.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.000000e-01 8.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.000000e-01 1.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361_qq/d05-x01-y02 -Path: /OPAL_2004_I631361_qq/d05-x01-y02 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: # ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries -0.000000e+00 1.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.000000e-02 2.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.000000e-02 3.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.000000e-02 4.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.000000e-02 5.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-02 6.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.000000e-02 7.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.000000e-02 8.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.000000e-02 9.000000e-02 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.000000e-02 1.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.000000e-01 1.200000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.200000e-01 1.400000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.400000e-01 1.600000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.600000e-01 1.800000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.800000e-01 2.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.000000e-01 2.500000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e-01 3.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.000000e-01 4.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 6.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.000000e-01 8.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361_qq/d02-x01-y02 -Path: /OPAL_2004_I631361_qq/d02-x01-y02 -ScaledBy: 2.50000000000000000e-01 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: 6.750000e+00 -# Area: 1.000000e+00 -# ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 1.000000e+00 2.500000e-01 6.750000e+00 5.625000e+01 4.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 2.500000e-01 6.250000e-02 5.000000e-01 1.000000e+00 1.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.500000e+00 5.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.500000e+00 6.500000e+00 2.500000e-01 6.250000e-02 1.500000e+00 9.000000e+00 1.000000e+00 -6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.500000e+00 8.500000e+00 2.500000e-01 6.250000e-02 2.000000e+00 1.600000e+01 1.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 2.500000e-01 6.250000e-02 2.750000e+00 3.025000e+01 1.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.650000e+01 1.750000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.750000e+01 1.850000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 - -BEGIN YODA_HISTO1D_V2 /OPAL_2004_I631361_qq/d02-x01-y01 -Path: /OPAL_2004_I631361_qq/d02-x01-y01 -ScaledBy: 1.00000000000000000e+00 -Title: ~ -Type: Histo1D -XLabel: ~ -YLabel: ~ ---- -# Mean: 5.000000e+00 -# Area: 1.000000e+00 -# ID ID sumw sumw2 sumwx sumwx2 numEntries -Total Total 1.000000e+00 1.000000e+00 5.000000e+00 2.500000e+01 1.000000e+00 -Underflow Underflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -Overflow Overflow 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -# xlow xhigh sumw sumw2 sumwx sumwx2 numEntries --5.000000e-01 5.000000e-01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -5.000000e-01 1.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.500000e+00 2.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -2.500000e+00 3.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -3.500000e+00 4.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -4.500000e+00 5.500000e+00 1.000000e+00 1.000000e+00 5.000000e+00 2.500000e+01 1.000000e+00 -5.500000e+00 6.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -6.500000e+00 7.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -7.500000e+00 8.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -8.500000e+00 9.500000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -9.500000e+00 1.050000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.050000e+01 1.150000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.150000e+01 1.250000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.250000e+01 1.350000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.350000e+01 1.450000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.450000e+01 1.550000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -1.550000e+01 1.650000e+01 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 0.000000e+00 -END YODA_HISTO1D_V2 diff --git a/bin/rivet b/bin/rivet --- a/bin/rivet +++ b/bin/rivet @@ -1,674 +1,674 @@ #! /usr/bin/env python """\ Run Rivet analyses on HepMC events read from a file or Unix pipe Examples: %(prog)s [options] [ ...] or mkfifo fifo.hepmc my_generator -o fifo.hepmc & %(prog)s [options] fifo.hepmc ENVIRONMENT: * RIVET_ANALYSIS_PATH: list of paths to be searched for plugin analysis libraries at runtime * RIVET_DATA_PATH: list of paths to be searched for data files (defaults to use analysis path) * RIVET_WEIGHT_INDEX: the numerical weight-vector index to use in this run (default = 0; -1 = ignore weights) * See the documentation for more environment variables. """ from __future__ import print_function import os, sys ## Load the rivet module try: import rivet except: ## If rivet loading failed, try to bootstrap the Python path! try: # TODO: Is this a good idea? Maybe just notify the user that their PYTHONPATH is wrong? import commands modname = sys.modules[__name__].__file__ binpath = os.path.dirname(modname) rivetconfigpath = os.path.join(binpath, "rivet-config") rivetpypath = commands.getoutput(rivetconfigpath + " --pythonpath") sys.path.append(rivetpypath) import rivet except: sys.stderr.write("The rivet Python module could not be loaded: is your PYTHONPATH set correctly?\n") sys.exit(5) rivet.util.check_python_version() rivet.util.set_process_name("rivet") import time, datetime, logging, signal ## Parse command line options import argparse parser = argparse.ArgumentParser(description=__doc__) parser.add_argument("ARGS", nargs="*") parser.add_argument("--version", dest="SHOW_VERSION", action="store_true", default=False, help="show Rivet version") anagroup = parser.add_argument_group("Analysis handling") anagroup.add_argument("-a", "--analysis", "--analyses", dest="ANALYSES", action="append", default=[], metavar="ANA", help="add an analysis (or comma-separated list of analyses) to the processing list.") anagroup.add_argument("--list-analyses", "--list", dest="LIST_ANALYSES", action="store_true", default=False, help="show the list of available analyses' names. With -v, it shows the descriptions, too") anagroup.add_argument("--list-keywords", "--keywords", dest="LIST_KEYWORDS", action="store_true", default=False, help="show the list of available keywords.") anagroup.add_argument("--list-used-analyses", action="store_true", dest="LIST_USED_ANALYSES", default=False, help="list the analyses used by this command (after subtraction of inappropriate ones)") anagroup.add_argument("--show-analysis", "--show-analyses", "--show", dest="SHOW_ANALYSES", action="append", default=[], help="show the details of an analysis") anagroup.add_argument("--show-bibtex", dest="SHOW_BIBTEX", action="store_true", default=False, help="show BibTeX entries for all used analyses") anagroup.add_argument("--analysis-path", dest="ANALYSIS_PATH", metavar="PATH", default=None, help="specify the analysis search path (cf. $RIVET_ANALYSIS_PATH).") # TODO: remove/deprecate the append? anagroup.add_argument("--analysis-path-append", dest="ANALYSIS_PATH_APPEND", metavar="PATH", default=None, help="append to the analysis search path (cf. $RIVET_ANALYSIS_PATH).") anagroup.add_argument("--pwd", dest="ANALYSIS_PATH_PWD", action="store_true", default=False, help="append the current directory (pwd) to the analysis/data search paths (cf. $RIVET_ANALYSIS_PATH).") extragroup = parser.add_argument_group("Extra run settings") extragroup.add_argument("-o", "-H", "--histo-file", dest="HISTOFILE", default="Rivet.yoda", help="specify the output histo file path (default = %(default)s)") extragroup.add_argument("-p", "--preload-file", dest="PRELOADFILE", default=None, help="specify and old yoda file to initialize (default = %(default)s)") extragroup.add_argument("--no-histo-file", dest="WRITE_DATA", action="store_false", default=True, help="don't write out any histogram file at the end of the run (default = write)") extragroup.add_argument("-x", "--cross-section", dest="CROSS_SECTION", default=None, metavar="XS", help="specify the signal process cross-section in pb") extragroup.add_argument("-n", "--nevts", dest="MAXEVTNUM", type=int, default=None, metavar="NUM", help="restrict the max number of events to process") extragroup.add_argument("--nskip", dest="EVTSKIPNUM", type=int, default=0, metavar="NUM", help="skip NUM events read from input before beginning processing") extragroup.add_argument("--runname", dest="RUN_NAME", default=None, metavar="NAME", help="give an optional run name, to be prepended as a 'top level directory' in histo paths") extragroup.add_argument("--ignore-beams", dest="IGNORE_BEAMS", action="store_true", default=False, help="ignore input event beams when checking analysis compatibility. " "WARNING: analyses may not work correctly, or at all, with inappropriate beams") extragroup.add_argument("-d", "--dump", "--histo-interval", dest="DUMP_PERIOD", type=int, default=1000, metavar="NUM", help="specify the number of events between histogram file updates, " "default = %(default)s. Set to 0 to only write out at the end of the run. " "Note that intermediate histograms will be those from the analyze step " "only, except for analyses explicitly declared Reentrant for which the " "finalize function is executed first.") timinggroup = parser.add_argument_group("Timeouts and periodic operations") timinggroup.add_argument("--event-timeout", dest="EVENT_TIMEOUT", type=int, default=21600, metavar="NSECS", help="max time in whole seconds to wait for an event to be generated from the specified source (default = %(default)s)") timinggroup.add_argument("--run-timeout", dest="RUN_TIMEOUT", type=int, default=None, metavar="NSECS", help="max time in whole seconds to wait for the run to finish. This can be useful on batch systems such " "as the LCG Grid where tokens expire on a fixed wall-clock and can render long Rivet runs unable to write " "out the final histogram file (default = unlimited)") verbgroup = parser.add_argument_group("Verbosity control") parser.add_argument("-l", dest="NATIVE_LOG_STRS", action="append", default=[], help="set a log level in the Rivet library") verbgroup.add_argument("-v", "--verbose", action="store_const", const=logging.DEBUG, dest="LOGLEVEL", default=logging.INFO, help="print debug (very verbose) messages") verbgroup.add_argument("-q", "--quiet", action="store_const", const=logging.WARNING, dest="LOGLEVEL", default=logging.INFO, help="be very quiet") args = parser.parse_args() ## Print the version and exit if args.SHOW_VERSION: print("rivet v%s" % rivet.version()) sys.exit(0) ## Override/modify analysis search path if args.ANALYSIS_PATH: rivet.setAnalysisLibPaths(args.ANALYSIS_PATH.split(":")) rivet.setAnalysisDataPaths(args.ANALYSIS_PATH.split(":")) if args.ANALYSIS_PATH_APPEND: for ap in args.ANALYSIS_PATH_APPEND.split(":"): rivet.addAnalysisLibPath(ap) rivet.addAnalysisDataPath(ap) if args.ANALYSIS_PATH_PWD: rivet.addAnalysisLibPath(os.path.abspath(".")) rivet.addAnalysisDataPath(os.path.abspath(".")) ## Configure logging logging.basicConfig(level=args.LOGLEVEL, format="%(message)s") for l in args.NATIVE_LOG_STRS: name, level = None, None try: name, level = l.split("=") except: name = "Rivet" level = l ## Fix name if name != "Rivet" and not name.startswith("Rivet."): name = "Rivet." + name try: ## Get right error type level = rivet.LEVELS.get(level.upper(), None) logging.debug("Setting log level: %s %d" % (name, level)) rivet.setLogLevel(name, level) except: logging.warning("Couldn't process logging string '%s'" % l) ############################ ## Listing available analyses/keywords def getAnalysesByKeyword(alist, kstring): add, veto, ret = [], [], [] bits = [i for i in kstring.replace("^@", "@^").split("@") if len(i) > 0] for b in bits: if b.startswith("^"): veto.append(b.strip("^")) else: add.append(b) add = set(add) veto = set(veto) for a in alist: kwds = set([i.lower() for i in rivet.AnalysisLoader.getAnalysis(a).keywords()]) if kwds.intersection(veto) and len(kwds.intersection(add)) == len(list(add)): ret.append(a) return ret ## List of analyses all_analyses = rivet.AnalysisLoader.analysisNames() if args.LIST_ANALYSES: ## Treat args as case-insensitive regexes if present regexes = None if args.ARGS: import re regexes = [re.compile(arg, re.I) for arg in args.ARGS] # import tempfile, subprocess # tf, tfpath = tempfile.mkstemp(prefix="rivet-list.") names = [] msg = [] for aname in all_analyses: if not regexes: toshow = True else: toshow = False for regex in regexes: if regex.search(aname): toshow = True break if toshow: names.append(aname) msg.append('') if args.LOGLEVEL <= logging.INFO: a = rivet.AnalysisLoader.getAnalysis(aname) st = "" if a.status() == "VALIDATED" else ("[%s] " % a.status()) # detex will very likely introduce some non-ASCII chars from # greek names in analysis titles. # The u"" prefix and explicit print encoding are necessary for # py2 to handle this properly msg[-1] = u"%s%s" % (st, a.summary()) if args.LOGLEVEL < logging.INFO: if a.keywords(): msg[-1] += u" [%s]" % " ".join(a.keywords()) if a.luminosityfb(): msg[-1] += u" [ \int L = %s fb^{-1} ]" % a.luminosityfb() msg = rivet.util.detex(msg) retlist = '\n'.join([ u"%-25s %s" % (a,m) for a,m in zip(names,msg) ]) if type(u'') is not str: retlist = retlist.encode('utf-8') print(retlist) sys.exit(0) def getKeywords(alist): all_keywords = [] for a in alist: all_keywords.extend(rivet.AnalysisLoader.getAnalysis(a).keywords()) all_keywords = [i.lower() for i in all_keywords] return sorted(list(set(all_keywords))) ## List keywords if args.LIST_KEYWORDS: # a = rivet.AnalysisLoader.getAnalysis(aname) for k in getKeywords(all_analyses): print(k) sys.exit(0) ## Show analyses' details if len(args.SHOW_ANALYSES) > 0: toshow = [] for i, a in enumerate(args.SHOW_ANALYSES): a_up = a.upper() if a_up in all_analyses and a_up not in toshow: toshow.append(a_up) else: ## Treat as a case-insensitive regex import re regex = re.compile(a, re.I) for ana in all_analyses: if regex.search(ana) and a_up not in toshow: toshow.append(ana) msgs = [] for i, name in enumerate(sorted(toshow)): import textwrap ana = rivet.AnalysisLoader.getAnalysis(name) msg = "" msg += name + "\n" msg += (len(name) * "=") + "\n\n" msg += rivet.util.detex(ana.summary()) + "\n\n" msg += "Status: " + ana.status() + "\n\n" # TODO: reduce to only show Inspire in v3 if ana.inspireId(): msg += "Inspire ID: " + ana.inspireId() + "\n" msg += "Inspire URL: http://inspire-hep.net/record/" + ana.inspireId() + "\n" msg += "HepData URL: http://hepdata.net/record/ins" + ana.inspireId() + "\n" elif ana.spiresId(): msg += "Spires ID: " + ana.spiresId() + "\n" msg += "Inspire URL: http://inspire-hep.net/search?p=find+key+" + ana.spiresId() + "\n" msg += "HepData URL: http://hepdata.cedar.ac.uk/view/irn" + ana.spiresId() + "\n" if ana.year(): msg += "Year of publication: " + ana.year() + "\n" if ana.bibKey(): msg += "BibTeX key: " + ana.bibKey() + "\n" msg += "Authors:\n" for a in ana.authors(): msg += " " + a + "\n" msg += "\n" msg += "Description:\n" twrap = textwrap.TextWrapper(width=75, initial_indent=2*" ", subsequent_indent=2*" ") msg += twrap.fill(rivet.util.detex(ana.description())) + "\n\n" if ana.experiment(): msg += "Experiment: " + ana.experiment() if ana.collider(): msg += "(%s)" % ana.collider() msg += "\n" # TODO: move this formatting into Analysis or a helper function? if ana.requiredBeams(): def pid_to_str(pid): if pid == 11: return "e-" elif pid == -11: return "e+" elif pid == 2212: return "p+" elif pid == -2212: return "p-" elif pid == 10000: return "*" else: return str(pid) beamstrs = [] for bp in ana.requiredBeams(): beamstrs.append(pid_to_str(bp[0]) + " " + pid_to_str(bp[1])) msg += "Beams:" + ", ".join(beamstrs) + "\n" if ana.requiredEnergies(): msg += "Beam energies:" + "; ".join(["(%0.1f, %0.1f) GeV\n" % (epair[0], epair[1]) for epair in ana.requiredEnergies()]) else: msg += "Beam energies: ANY\n" if ana.runInfo(): msg += "Run details:\n" twrap = textwrap.TextWrapper(width=75, initial_indent=2*" ", subsequent_indent=4*" ") for l in ana.runInfo().split("\n"): msg += twrap.fill(l) + "\n" if ana.luminosityfb(): msg+= "\nIntegrated data luminosity = %s inverse fb.\n"%ana.luminosityfb() if ana.keywords(): msg += "\nAnalysis keywords:" for k in ana.keywords(): msg += " %s"%k msg+= "\n\n" if ana.references(): msg += "\n" + "References:\n" for r in ana.references(): url = None if r.startswith("arXiv:"): code = r.split()[0].replace("arXiv:", "") url = "http://arxiv.org/abs/" + code elif r.startswith("doi:"): code = r.replace("doi:", "") url = "http://dx.doi.org/" + code if url is not None: r += " - " + url msg += " " + r + "\n" ## Add to the output msgs.append(msg) ## Write the combined messages to a temporary file and page it if msgs: try: import tempfile, subprocess tffd, tfpath = tempfile.mkstemp(prefix="rivet-show.") msgsum = u"\n\n".join(msgs) - if type(u'') is str: + if type(u'') is not str: msgsum = msgsum.encode('utf-8') os.write(tffd, msgsum) if sys.stdout.isatty(): pager = subprocess.Popen(["less", "-FX", tfpath]) #, stdin=subprocess.PIPE) pager.communicate() else: f = open(tfpath) print(f.read()) f.close() finally: os.unlink(tfpath) #< always clean up sys.exit(0) ############################ ## Actual analysis runs ## We allow comma-separated lists of analysis names -- normalise the list here newanas = [] for a in args.ANALYSES: if "," in a: newanas += a.split(",") elif "@" in a: #< NB. this bans combination of ana lists and keywords in a single arg temp = getAnalysesByKeyword(all_analyses, a) for i in temp: newanas.append(i) else: newanas.append(a) args.ANALYSES = newanas ## Parse supplied cross-section if args.CROSS_SECTION is not None: xsstr = args.CROSS_SECTION try: args.CROSS_SECTION = float(xsstr) except: import re suffmatch = re.search(r"[^\d.]", xsstr) if not suffmatch: raise ValueError("Bad cross-section string: %s" % xsstr) factor = base = None suffstart = suffmatch.start() if suffstart != -1: base = xsstr[:suffstart] suffix = xsstr[suffstart:].lower() if suffix == "mb": factor = 1e+9 elif suffix == "mub": factor = 1e+6 elif suffix == "nb": factor = 1e+3 elif suffix == "pb": factor = 1 elif suffix == "fb": factor = 1e-3 elif suffix == "ab": factor = 1e-6 if factor is None or base is None: raise ValueError("Bad cross-section string: %s" % xsstr) xs = float(base) * factor args.CROSS_SECTION = xs ## Print the available CLI options! #if args.LIST_OPTIONS: # for o in parser.option_list: # print(o.get_opt_string()) # sys.exit(0) ## Set up signal handling RECVD_KILL_SIGNAL = None def handleKillSignal(signum, frame): "Declare us as having been signalled, and return to default handling behaviour" global RECVD_KILL_SIGNAL logging.critical("Signal handler called with signal " + str(signum)) RECVD_KILL_SIGNAL = signum signal.signal(signum, signal.SIG_DFL) ## Signals to handle signal.signal(signal.SIGTERM, handleKillSignal); signal.signal(signal.SIGHUP, handleKillSignal); signal.signal(signal.SIGINT, handleKillSignal); signal.signal(signal.SIGUSR1, handleKillSignal); signal.signal(signal.SIGUSR2, handleKillSignal); try: signal.signal(signal.SIGXCPU, handleKillSignal); except: pass ## Identify HepMC files/streams ## TODO: check readability, deal with stdin if len(args.ARGS) > 0: HEPMCFILES = args.ARGS else: HEPMCFILES = ["-"] ## Event number logging def logNEvt(n, starttime, maxevtnum): if n % 10000 == 0: nevtloglevel = logging.CRITICAL elif n % 1000 == 0: nevtloglevel = logging.WARNING elif n % 100 == 0: nevtloglevel = logging.INFO else: nevtloglevel = logging.DEBUG currenttime = datetime.datetime.now().replace(microsecond=0) elapsedtime = currenttime - starttime logging.log(nevtloglevel, "Event %d (%s elapsed)" % (n, str(elapsedtime))) # if maxevtnum is None: # logging.log(nevtloglevel, "Event %d (%s elapsed)" % (n, str(elapsedtime))) # else: # remainingtime = (maxevtnum-n) * elapsedtime.total_seconds() / float(n) # eta = time.strftime("%a %b %d %H:%M", datetime.localtime(currenttime + remainingtime)) # logging.log(nevtloglevel, "Event %d (%d s elapsed / %d s left) -> ETA: %s" % # (n, elapsedtime, remainingtime, eta)) ## Do some checks on output histo file, before we stat the event loop histo_parentdir = os.path.dirname(os.path.abspath(args.HISTOFILE)) if not os.path.exists(histo_parentdir): logging.error('Parent path of output histogram file does not exist: %s\nExiting.' % histo_parentdir) sys.exit(4) if not os.access(histo_parentdir,os.W_OK): logging.error('Insufficient permissions to write output histogram file to directory %s\nExiting.' % histo_parentdir) sys.exit(4) ## Set up analysis handler RUNNAME = args.RUN_NAME or "" ah = rivet.AnalysisHandler(RUNNAME) ah.setIgnoreBeams(args.IGNORE_BEAMS) for a in args.ANALYSES: ## Print warning message and exit if not a valid analysis name if not rivet.stripOptions(a) in all_analyses: logging.warning("'%s' is not a known Rivet analysis! Do you need to set RIVET_ANALYSIS_PATH or use the --pwd switch?\n" % a) # TODO: lay out more neatly, or even try for a "did you mean XXXX?" heuristic? logging.warning("There are %d currently available analyses:\n" % len(all_analyses) + ", ".join(all_analyses)) sys.exit(1) logging.debug("Adding analysis '%s'" % a) ah.addAnalysis(a) if args.PRELOADFILE is not None: ah.readData(args.PRELOADFILE) if args.DUMP_PERIOD: ah.dump(args.HISTOFILE, args.DUMP_PERIOD) if args.SHOW_BIBTEX: bibs = [] for aname in sorted(ah.analysisNames()): ana = rivet.AnalysisLoader.getAnalysis(aname) bibs.append("% " + aname + "\n" + ana.bibTeX()) if bibs: print("\nBibTeX for used Rivet analyses:\n") print("% --------------------------\n") print("\n\n".join(bibs) + "\n") print("% --------------------------\n") ## Read and process events run = rivet.Run(ah) if args.CROSS_SECTION is not None: logging.info("User-supplied cross-section = %e pb" % args.CROSS_SECTION) run.setCrossSection(args.CROSS_SECTION) if args.LIST_USED_ANALYSES is not None: run.setListAnalyses(args.LIST_USED_ANALYSES) ## Print platform type import platform starttime = datetime.datetime.now().replace(microsecond=0) logging.info("Rivet %s running on machine %s (%s) at %s" % \ (rivet.version(), platform.node(), platform.machine(), str(starttime))) def min_nonnull(a, b): "A version of min which considers None to always be greater than a real number" if a is None: return b if b is None: return a return min(a, b) ## Set up an event timeout handler class TimeoutException(Exception): pass if args.EVENT_TIMEOUT or args.RUN_TIMEOUT: def evttimeouthandler(signum, frame): logging.warn("It has taken more than %d secs to get an event! Is the input event stream working?" % min_nonnull(args.EVENT_TIMEOUT, args.RUN_TIMEOUT)) raise TimeoutException("Event timeout") signal.signal(signal.SIGALRM, evttimeouthandler) ## Init run based on one event hepmcfile = HEPMCFILES[0] ## Apply a file-level weight derived from the filename hepmcfileweight = 1.0 if ":" in hepmcfile: hepmcfile, hepmcfileweight = hepmcfile.rsplit(":", 1) hepmcfileweight = float(hepmcfileweight) try: if args.EVENT_TIMEOUT or args.RUN_TIMEOUT: signal.alarm(min_nonnull(args.EVENT_TIMEOUT, args.RUN_TIMEOUT)) init_ok = run.init(hepmcfile, hepmcfileweight) signal.alarm(0) if not init_ok: logging.error("Failed to initialise using event file '%s'... exiting" % hepmcfile) sys.exit(2) except TimeoutException as te: logging.error("Timeout in initialisation from event file '%s'... exiting" % hepmcfile) sys.exit(3) except Exception as ex: logging.warning("Could not read from '%s' (error=%s)" % (hepmcfile, str(ex))) sys.exit(3) ## Event loop evtnum = 0 for fileidx, hepmcfile in enumerate(HEPMCFILES): ## Apply a file-level weight derived from the filename hepmcfileweight = 1.0 if ":" in hepmcfile: hepmcfile, hepmcfileweight = hepmcfile.rsplit(":", 1) hepmcfileweight = float(hepmcfileweight) ## Open next HepMC file (NB. this doesn't apply to the first file: it was already used for the run init) if fileidx > 0: try: run.openFile(hepmcfile, hepmcfileweight) except Exception as ex: logging.warning("Could not read from '%s' (error=%s)" % (hepmcfile, ex)) continue if not run.readEvent(): logging.warning("Could not read events from '%s'" % hepmcfile) continue ## Announce new file msg = "Reading events from '%s'" % hepmcfile if hepmcfileweight != 1.0: msg += " (file weight = %e)" % hepmcfileweight logging.info(msg) ## The event loop while args.MAXEVTNUM is None or evtnum-args.EVTSKIPNUM < args.MAXEVTNUM: evtnum += 1 ## Optional event skipping if evtnum <= args.EVTSKIPNUM: logging.debug("Skipping event #%i" % evtnum) run.skipEvent(); continue ## Only log the event number once we're actually processing logNEvt(evtnum, starttime, args.MAXEVTNUM) ## Process this event processed_ok = run.processEvent() if not processed_ok: logging.warn("Event processing failed for evt #%i!" % evtnum) break ## Set flag to exit event loop if run timeout exceeded if args.RUN_TIMEOUT and (time.time() - starttime) > args.RUN_TIMEOUT: logging.warning("Run timeout of %d secs exceeded... exiting gracefully" % args.RUN_TIMEOUT) RECVD_KILL_SIGNAL = True ## Exit the loop if signalled if RECVD_KILL_SIGNAL is not None: break ## Read next event (with timeout handling if requested) try: if args.EVENT_TIMEOUT: signal.alarm(args.EVENT_TIMEOUT) read_ok = run.readEvent() signal.alarm(0) if not read_ok: break except TimeoutException as te: logging.error("Timeout in reading event from '%s'... exiting" % hepmcfile) sys.exit(3) ## Print end-of-loop messages loopendtime = datetime.datetime.now().replace(microsecond=0) logging.info("Finished event loop at %s" % str(loopendtime)) logging.info("Cross-section = %e pb" % ah.crossSection()) print() ## Finalize and write out data file run.finalize() if args.WRITE_DATA: ah.writeData(args.HISTOFILE) print() endtime = datetime.datetime.now().replace(microsecond=0) logging.info("Rivet run completed at %s, time elapsed = %s" % (str(endtime), str(endtime-starttime))) print() logging.info("Histograms written to %s" % os.path.abspath(args.HISTOFILE)) diff --git a/bin/rivet-mkvaldir b/bin/rivet-mkvaldir --- a/bin/rivet-mkvaldir +++ b/bin/rivet-mkvaldir @@ -1,301 +1,303 @@ #! /usr/bin/env python """ Build a directory with a Makefile for running a validation suit. """ import os, sys, shutil, commands ## Load the rivet module try: import rivet except: ## If rivet loading failed, try to bootstrap the Python path! try: # TODO: Is this a good idea? Maybe just notify the user that # their PYTHONPATH is wrong? modname = sys.modules[__name__].__file__ binpath = os.path.dirname(modname) rivetconfigpath = os.path.join(binpath, "rivet-config") rivetpypath = commands.getoutput(rivetconfigpath + " --pythonpath") sys.path.append(rivetpypath) import rivet except: sys.stderr.write("The rivet Python module could not be loaded: " + \ "is your PYTHONPATH set correctly?\n") sys.exit(5) rivet.util.check_python_version() rivet.util.set_process_name("rivet-merge") import time, datetime, logging, signal ## Parse command line options import argparse parser = argparse.ArgumentParser(description=__doc__) extragroup = parser.add_argument_group("Run settings") extragroup.add_argument("VALDIR", nargs=1, help="directory where the " + \ "Makefile for running the validation will be written") extragroup.add_argument("--hepmc-dir", dest="HEPMCDIR", default="", help="specify the HepMC files used for " + \ "the validation should be downloaded") extragroup.add_argument("--ref-dir", dest="REFDIR", default="", help="specify the directory where the reference " + \ "yodas are located.") args = parser.parse_args() #################################################### ## create and configure validation directory valdir = str(args.VALDIR[0]) hepmcdir = valdir + "/HEPMC" if not os.path.exists(valdir) and not os.path.realpath(valdir)==os.getcwd(): try: os.makedirs(valdir) except: print("Error: failed to make new directory '%s'" % valdir) sys.exit(1) if not args.HEPMCDIR : if not os.path.exists(hepmcdir): try: os.makedirs(hepmcdir) except: print("Error: failed to make new directory '%s'" % hepmcdir) sys.exit(1) else: if os.path.exists(hepmcdir) and os.path.islink(hepmcdir): out = commands.getstatusoutput("rm -f " + hepmcdir) if os.path.exists(hepmcdir): print("Error: please remove directory '" + hepmcdir + \ "' before spicifying a new location for HepMC files") sys.exit(1) if not os.path.exists(args.HEPMCDIR): try: os.makedirs(args.HEPMCDIR) except: print("Error: failed to make new directory '%s'" % args.HEPMCDIR) sys.exit(1) out = commands.getstatusoutput("ln -sf " + os.path.relpath(args.HEPMCDIR, valdir) + " " + hepmcdir) if os.path.exists(valdir + "/tmp"): shutil.rmtree(valdir + "/tmp") try: os.makedirs(valdir + "/tmp") except: print("Error: failed to make tmo directory '%s'" % valdir + "/tmp") sys.exit(1) refdir = args.REFDIR if not refdir : rivetdatapath = commands.getoutput("rivet-config --datadir") refdir = rivetdatapath + "/valref" out = commands.getstatusoutput("rm -f " + valdir + "/refyodas") out = commands.getstatusoutput("ln -s " + os.path.relpath(refdir, valdir) + " " + valdir + "/refyodas") ####################################### ## Collect information from .info files valyodas = set() valanalyses = set() valhepmcs = set() valtargets = dict() hepmctargets = dict() ## Get all analysis names all_analyses = rivet.AnalysisLoader.analysisNames() for ananame in all_analyses: ana = rivet.AnalysisLoader.getAnalysis(ananame) for line in ana.validation(): valanalyses.add(ananame) line = line.replace("$A", ananame) sublines = line.split(";"); targets = sublines[0].split(" ") targetname = targets[0] hepmcname = targets[1] valyodas.add(targetname + ".yoda") valhepmcs.add(hepmcname) if len(sublines) == 1: valtargets[targetname] = "tmp/" + hepmcname + ".yoda " + \ " ".join(targets[2:]) + "\n\t@echo extracting " + \ targetname + ".yoda\n\t@echo " + hepmcname + " > tmp/" + \ - targetname + ".log\n\t@yoda2yoda -m " + ananame + \ - " tmp/" + hepmcname + ".yoda " + targetname + ".yoda >> tmp/" + \ + targetname + ".log\n\t@yoda2yoda -m /" + ananame + \ + "/ tmp/" + hepmcname + ".yoda " + targetname + ".yoda >> tmp/" + \ targetname + ".log 2>&1\n" if not hepmctargets.has_key(hepmcname): hepmctargets[hepmcname] = ananame else: hepmctargets[hepmcname] += " " + ananame else: valtargets[targetname] = "HEPMC/" + hepmcname + ".hepmc.gz " +\ " ".join(targets[2:]) if len(sublines) > 1: valtargets[targetname] += "\n\t@echo running " + \ targetname + ".yoda\n\t@echo " + hepmcname + " > tmp/" + \ targetname + ".log\n\t@" + sublines[1].strip() +\ - " > tmp/" + targetname + ".log 2>&1\n" + " >> tmp/" + targetname + ".log 2>&1\n" for subline in sublines[2:]: - valtargets[targetname] += "\n\t" + subline.strip() + \ + valtargets[targetname] += "\t" + subline.strip() + \ " >> tmp/" + targetname + ".log 2>&1\n" if len(sublines) > 1: - valtargets[targetname] += "\n\t@echo done " + \ + valtargets[targetname] += "\t@echo done " + \ targetname + ".yoda\n" ############################# ## Write the Makefile mf = open(valdir + "/Makefile", 'w') ## Header and default and help targets. mf.write("""# # This Makefile administers the validation for Rivet. # # Usage: make check # # For more information use: make help # # This Makefile was produced by rivet-mkvaldir which scanned all # analysis .info files and parsed the "Validation:" section for # determining how to use the existing HepMC validation files to obtain # a set of reference YODA files that should be reproduced. The # direcorey where these reference files are stored is linked to # ./refyodas . The HepMC files are stored in ./HEPMC and will be # automatically downloaded if missing. In the end of running 'make # check', the newly produced YODA files will be compared with the # reference ones. If differences are found in any histogram, the # corresponing plot will be produced by rivet-mkhtml and can be # accessed from the index.html file. # # The syntax for specifying a reference YODA in the .info file looks # as follows: # # - YODA-name HEPMC-name [other dependencies] [[; commandline] ...] # # the YODA-name should be given without the .yoda suffix and typically # is constructed from the analysis name with some number appended if # there are more than one reference YODA for an analysis. Note that # the sting "$A" can be used anywher and will be expanded to the # analysis name. HEPMC-name should given without the ".hepmc.gz" # suffix. "other dependencies" can eg. include the reference YODA from # another analysis that are referenced in any of the # "commandline"s. If no commandline is given the analysis will be run # together with a bunch of other analyses and the YODA-name.yoda will -# be extracted formthe resulting yoda. +# be extracted form the resulting yoda. The command lines will be used +# as make recipes where the output YODA file can be given by $@ and the +# HepMC file by $< # # When submitting a new analysis to Rivet, the "Validation:" section # of the .info file must be present and all the corresponding YODA # reference file should be be included in the submission. If a # non-standard HepMC file is needed to reproduce the reference YODA, # this must be included as well. # all: @head -7 $(firstword $(MAKEFILE_LIST)) help: - @head -41 $(firstword $(MAKEFILE_LIST)) | grep -v "# For more information" + @head -43 $(firstword $(MAKEFILE_LIST)) | grep -v "# For more information" """) ## target for comparing the generated yodas with the reference ones mf.write(""" %.diff: %.yoda @rm -rf $@ @if [ -e refyodas/$< ]; then \\ if ! yodadiff $< refyodas/$< -t 1e-2 -q; then \\ echo $< differs from reference yoda; \\ only=""; \\ for plot in `yodadiff $< refyodas/$< -t 1e-2 -l`; do \\ only="$$only -m $$plot"; \\ done; \\ rivet-mkhtml $$only -o $@ $< refyodas/$<:Title=ref > /dev/null 2>&1; \\ else \\ echo $< is the same as reference yoda; \\ touch $@; \\ fi \\ else \\ echo $< has no reference yoda; \\ echo $< has no reference yoda > $@; \\ fi """) ## the main check target mf.write("VALYODAS =") for ana in valtargets: mf.write(" " + ana + ".yoda") mf.write("\n\nVALDIFFS =") for ana in valtargets: mf.write(" " + ana + ".diff") mf.write("""\n .PRECIOUS: $(VALYODAS) check: $(VALDIFFS) @echo "

Problematic analyses in Rivet validation

" > index.html @for dir in $^; do \\ if [ -d $$dir ]; then \\ for subdir in `ls $$dir`; do \\ if [ -f $$dir/$$subdir/index.html ]; then\\ echo -n "$${dir/.diff/} (" >> index.html; \\ echo -n `head -1 tmp/$${dir/.diff/.log}` >> index.html; \\ echo ")
" >> index.html; \\ fi \\ done \\ elif [ -s $$dir ]; then \\ echo "$${dir/.diff/}: no reference yoda
" >> index.html; \\ fi \\ done @echo "" @if grep -q href index.html; then \\ echo "Differences found, open index.html to inspect plots."; \\ else \\ echo "No differences found!"; \\ fi clean: rm -f $(VALYODAS) rm -rf tmp rm -rf $(VALDIFFS) rm index.html %.recheck: %.yoda rm -f $< hepmc=tmp/$<; rm -f tmp/`head -1 $${hepmc/.yoda/.log}`".yoda" $(MAKE) check """) ## targets for hepmc files with several analyses for hepmc in hepmctargets: mf.write("tmp/" + hepmc + ".yoda: HEPMC/" + hepmc + ".hepmc.gz\n") mf.write("\t@echo running " + hepmc + "\n") cmd = "\t@rivet HEPMC/" + hepmc + ".hepmc.gz -o tmp/" + hepmc + ".yoda" for ana in hepmctargets[hepmc].split(" "): cmd += " -a " + ana mf.write(cmd + " > tmp/" + hepmc + ".log 2>&1\n") mf.write("\t@echo done " + hepmc + "\n\n") ## targets for the .yoda files to be compared to the reference ones for ana in valtargets: mf.write(ana + ".yoda: " + valtargets[ana] + "\n") mf.write("\n") ## target for fetching the standard HepMC files fromcernbox mf.write("HEPMC/%.hepmc.gz:\n") mf.write("\twget 'https://cernbox.cern.ch/index.php/s/6QD1dvXFt1FJ7Dy/download?path=%2F&x-access-token=eyJhbGciOiJIUzI1NiIsInR5cCI6IkpXVCJ9.eyJkcm9wX29ubHkiOmZhbHNlLCJleHAiOiIyMDE5LTA1LTMxVDE0OjAwOjU3LjgzNzgzMzIwMSswMjowMCIsImV4cGlyZXMiOjAsImlkIjoiMTYzMTI1IiwiaXRlbV90eXBlIjoxLCJtdGltZSI6MTU0OTk2OTEwOCwib3duZXIiOiJhYnVja2xleSIsInBhdGgiOiJlb3Nob21lLWE6MTkwOTgzOTkiLCJwcm90ZWN0ZWQiOmZhbHNlLCJyZWFkX29ubHkiOnRydWUsInNoYXJlX25hbWUiOiJSaXZldCB2YWxpZGF0aW9uIEhlcE1DIiwidG9rZW4iOiI2UUQxZHZYRnQxRko3RHkifQ.lvLykwYq_NheD6ld2IidhogrKdQfVz43y8wOooYF6Kg&files=$(@F)' -O $@\n\n") diff --git a/docker/rivet/Dockerfile b/docker/rivet/Dockerfile --- a/docker/rivet/Dockerfile +++ b/docker/rivet/Dockerfile @@ -1,26 +1,26 @@ FROM fedora:27 LABEL maintainer="rivet@projects.hepforge.org" RUN dnf update -y \ && dnf install -y \ make gcc-c++ gcc-gfortran redhat-rpm-config \ wget tar less bzip2 findutils which nano zlib-devel \ - python python-devel file python-matplotlib gsl-devel \ + python python-devel python-requests file python-matplotlib gsl-devel \ texlive-latex-bin texlive-texconfig-bin texlive-pst-tools \ ghostscript ImageMagick texlive-dvips texlive-relsize \ texlive-cm texlive-hyphen-base texlive-collection-fontsrecommended \ && dnf clean all RUN mkdir /code && cd /code \ && wget https://phab.hepforge.org/source/rivetbootstraphg/browse/2.7.2/rivet-bootstrap?view=raw -O rivet-bootstrap \ && chmod +x rivet-bootstrap \ && INSTALL_PREFIX=/usr/local INSTALL_GSL=0 INSTALL_RIVETDEV=0 MAKE="make -j7" ./rivet-bootstrap \ && echo "source /usr/local/share/Rivet/rivet-completion" > /etc/profile.d/rivet-completion.sh \ && echo "source /usr/local/share/YODA/yoda-completion" > /etc/profile.d/yoda-completion.sh \ && texconfig rehash \ && rm -rf /code ENV LD_LIBRARY_PATH /usr/local/lib ENV PYTHONPATH /usr/local/lib64/python2.7/site-packages WORKDIR /work diff --git a/include/Rivet/Event.hh b/include/Rivet/Event.hh --- a/include/Rivet/Event.hh +++ b/include/Rivet/Event.hh @@ -1,207 +1,218 @@ // -*- C++ -*- #ifndef RIVET_Event_HH #define RIVET_Event_HH #include "Rivet/Config/RivetCommon.hh" #include "Rivet/Particle.hh" #include "Rivet/Projection.hh" namespace Rivet { /// Rivet wrapper for HepMC event and Projection references. /// /// Event is a concrete class representing an generated event in Rivet. It is /// constructed given a HepMC::GenEvent, a pointer to which is kept by the /// Event object throughout its lifetime. The user must therefore make sure /// that the corresponding HepMC::GenEvent will persist at least as long as /// the Event object. /// /// In addition to the HepMC::GenEvent object the Event also keeps track of /// all Projection objects which have been applied to the Event so far. class Event { public: /// @name Constructors and destructors. //@{ /// Constructor from a HepMC GenEvent pointer Event(const GenEvent* ge, bool strip = false) : _genevent_original(ge) { assert(ge); _genevent = *ge; if ( strip ) _strip(_genevent); _init(*ge); } /// Constructor from a HepMC GenEvent reference /// @deprecated HepMC uses pointers, so we should talk to HepMC via pointers Event(const GenEvent& ge, bool strip = false) : _genevent_original(&ge), _genevent(ge) { if ( strip ) _strip(_genevent); _init(ge); } /// Copy constructor Event(const Event& e) : _genevent_original(e._genevent_original), _genevent(e._genevent) { } //@} /// @name Major event properties //@{ /// The generated event obtained from an external event generator const GenEvent* genEvent() const { return &_genevent; } /// The generated event obtained from an external event generator const GenEvent* originalGenEvent() const { return _genevent_original; } /// @brief The generation weight associated with the event /// /// @todo This needs to be revisited when we finally add the mechanism to /// support NLO counter-events and weight vectors. double weight() const; /// Get the beam particles ParticlePair beams() const; /// Get the beam centre-of-mass energy double sqrtS() const; /// Get the beam centre-of-mass energy per nucleon double asqrtS() const; /// Get the generator centrality (impact-parameter quantile in [0,1]; or -1 if undefined (usual for non-HI generators)) //double centrality() const; // /// Get the boost to the beam centre-of-mass // Vector3 beamCMSBoost() const; // /// Get the boost to the beam centre-of-mass // LorentzTransform beamCMSTransform(); //@} /// @name Access to event particles //@{ /// All the raw GenEvent particles, wrapped in Rivet::Particle objects const Particles& allParticles() const; /// @brief All the raw GenEvent particles, wrapped in Rivet::Particle objects, but with a Cut applied /// /// @note Due to the cut, this returns by value, i.e. involves an expensive copy inline Particles allParticles(const Cut& c) const { return filter_select(allParticles(), c); } /// @brief All the raw GenEvent particles, wrapped in Rivet::Particle objects, but with a selection function applied /// /// @note Due to the cut, this returns by value, i.e. involves an expensive copy template inline Particles allParticles(const FN& f) const { return filter_select(allParticles(), f); } //@} /// @name Projection running //@{ /// @brief Add a projection @a p to this Event. /// /// If an equivalent Projection has been applied before, the /// Projection::project(const Event&) of @a p is not called and a reference /// to the previous equivalent projection is returned. If no previous /// Projection was found, the Projection::project(const Event&) of @a p is /// called and a reference to @a p is returned. + /// + /// @todo Can make this non-templated, since only cares about ptr to Projection base class + /// + /// @note Comparisons here are by direct pointer comparison, because + /// equivalence is guaranteed if pointers are equal, and inequivalence + /// guaranteed if they aren't, thanks to the ProjectionHandler registry template const PROJ& applyProjection(PROJ& p) const { Log& log = Log::getLog("Rivet.Event"); static bool docaching = getEnvParam("RIVET_CACHE_PROJECTIONS", true); if (docaching) { log << Log::TRACE << "Applying projection " << &p << " (" << p.name() << ") -> comparing to projections " << _projections << endl; // First search for this projection *or an equivalent* in the already-executed list const Projection* cpp(&p); - std::set::const_iterator old = _projections.find(cpp); + /// @note Currently using reint cast to integer type to bypass operator==(Proj*, Proj*) + // std::set::const_iterator old = _projections.find(cpp); + std::set::const_iterator old = std::begin(_projections); + std::uintptr_t recpp = reinterpret_cast(cpp); + for (; old != _projections.end(); ++old) + if (reinterpret_cast(*old) == recpp) break; if (old != _projections.end()) { log << Log::TRACE << "Equivalent projection found -> returning already-run projection " << *old << endl; const Projection& pRef = **old; return pcast(pRef); } log << Log::TRACE << "No equivalent projection in the already-run list -> projecting now" << endl; } else { log << Log::TRACE << "Applying projection " << &p << " (" << p.name() << ") WITHOUT projection caching & comparison" << endl; } // If this one hasn't been run yet on this event, run it and add to the list Projection* pp = const_cast(&p); pp->_isValid = true; pp->project(*this); if (docaching) _projections.insert(pp); return p; } /// @brief Add a projection @a p to this Event by pointer. template const PROJ& applyProjection(PROJ* pp) const { if (!pp) throw Error("Event::applyProjection(PROJ*): Projection pointer is null."); return applyProjection(*pp); } //@} private: /// @brief Actual (shared) implementation of the constructors from GenEvents void _init(const GenEvent& ge); /// @brief Remove uninteresting or unphysicsl particles in the /// GenEvent to speed up searches. void _strip(GenEvent & ge); // /// @brief Convert the GenEvent to use conventional alignment // /// // /// For example, FHerwig only produces DIS events in the unconventional // /// hadron-lepton orientation and has to be corrected for DIS analysis // /// portability. // void _geNormAlignment(); /// @brief The generated event, as obtained from an external generator. /// /// This is the original GenEvent. In practise the version seen by users /// will often/always be a modified one. /// /// @todo Provide access to this via an Event::originalGenEvent() method? If requested... const GenEvent* _genevent_original; /// @brief The GenEvent used by Rivet analysis projections etc. /// /// This version may be rotated to a "normal" alignment, have /// generator-specific particles stripped out, etc. If an analysis is /// affected by these modifications, it is probably an unphysical analysis! /// /// Stored as a non-pointer since it may get overwritten, and memory for /// copying and cleanup is neater this way. /// @todo Change needed for HepMC3? mutable GenEvent _genevent; /// All the GenEvent particles, wrapped as Rivet::Particles /// @note To be populated lazily, hence mutability mutable Particles _particles; /// The set of Projection objects applied so far mutable std::set _projections; }; } #endif diff --git a/include/Rivet/Projections/SmearedParticles.hh b/include/Rivet/Projections/SmearedParticles.hh --- a/include/Rivet/Projections/SmearedParticles.hh +++ b/include/Rivet/Projections/SmearedParticles.hh @@ -1,173 +1,178 @@ // -*- C++ -*- #ifndef RIVET_SmearedParticles_HH #define RIVET_SmearedParticles_HH #include "Rivet/Particle.hh" #include "Rivet/Projection.hh" #include "Rivet/Projections/ParticleFinder.hh" #include "Rivet/Tools/SmearingFunctions.hh" namespace Rivet { // Recursive variadic template arg decoding namespace { template vector& toEffSmearFns(vector& v, const T& t) { v.push_back(ParticleEffSmearFn(t)); return v; } template vector& toEffSmearFns(vector& v, const T& first, ARGS... args) { v.push_back(ParticleEffSmearFn(first)); toEffSmearFns(v, args...); return v; } } /// Wrapper projection for smearing {@link Jet}s with detector resolutions and efficiencies class SmearedParticles : public ParticleFinder { public: /// @name Constructors etc. //@{ /// @brief Constructor with const efficiency SmearedParticles(const ParticleFinder& pf, double eff, const Cut& c=Cuts::open()) : SmearedParticles(pf, {{eff}}, c) { } /// @brief Constructor with an efficiency function SmearedParticles(const ParticleFinder& pf, const ParticleEffFn& effFn, const Cut& c=Cuts::open()) : SmearedParticles(pf, {{effFn}}, c) { } /// @brief Constructor with const efficiency followed by a smearing function SmearedParticles(const ParticleFinder& pf, double eff, const ParticleSmearFn& smearFn, const Cut& c=Cuts::open()) : SmearedParticles(pf, {eff, smearFn}, c) { } /// @brief Constructor with a smearing function followed by const efficiency SmearedParticles(const ParticleFinder& pf, const ParticleSmearFn& smearFn, double eff, const Cut& c=Cuts::open()) : SmearedParticles(pf, {smearFn, eff}, c) { } /// @brief Constructor with an efficiency function followed by a smearing function SmearedParticles(const ParticleFinder& pf, const ParticleEffFn& effFn, const ParticleSmearFn& smearFn, const Cut& c=Cuts::open()) : SmearedParticles(pf, {effFn, smearFn}, c) { } /// @brief Constructor with a smearing function followed by an efficiency function SmearedParticles(const ParticleFinder& pf, const ParticleSmearFn& smearFn, const ParticleEffFn& effFn, const Cut& c=Cuts::open()) : SmearedParticles(pf, {smearFn, effFn}, c) { } /// @brief Constructor with an ordered list of efficiency and/or smearing functions SmearedParticles(const ParticleFinder& pf, const vector& effSmearFns, const Cut& c=Cuts::open()) : ParticleFinder(c), _detFns(effSmearFns) { setName("SmearedParticles"); addProjection(pf, "TruthParticles"); } /// @brief Constructor with an ordered list of efficiency and/or smearing functions SmearedParticles(const ParticleFinder& pf, const initializer_list& effSmearFns, const Cut& c=Cuts::open()) : SmearedParticles(pf, vector{effSmearFns}, c) { } /// @brief Constructor with a variadic ordered list of efficiency and smearing function args /// @note The Cut must be provided *before* the eff/smearing functions /// @todo Wouldn't it be nice if the Cut could also go *after* the parameter pack? template SmearedParticles(const ParticleFinder& pf, const Cut& c, ARGS... effSmearFns) : SmearedParticles(pf, toEffSmearFns(_detFns, effSmearFns...), c) { } /// Clone on the heap. DEFAULT_RIVET_PROJ_CLONE(SmearedParticles); //@} /// Compare to another SmearedParticles + /// + /// @note Comparing detector functions doesn't work for functors/lambdas, + /// hence are always treated as not equivalent int compare(const Projection& p) const { const SmearedParticles& other = dynamic_cast(p); // Compare truth particles definitions const int teq = mkPCmp(other, "TruthParticles"); if (teq != EQUIVALENT) return teq; // Compare lists of detector functions const int nfeq = cmp(_detFns.size(), other._detFns.size()); + MSG_TRACE("Numbers of detector functions = " << _detFns.size() << " VS " << other._detFns.size()); if (nfeq != EQUIVALENT) return nfeq; for (size_t i = 0; i < _detFns.size(); ++i) { const int feq = _detFns[i].cmp(other._detFns[i]); if (feq != EQUIVALENT) return feq; } // If we got this far, we're equal + MSG_DEBUG("Equivalent detected! " << p.name() << ", " << this->name()); return EQUIVALENT; } /// Perform the particle finding & smearing calculation void project(const Event& e) { // Copying and filtering const Particles& truthparticles = apply(e, "TruthParticles").particlesByPt(); _theParticles.clear(); _theParticles.reserve(truthparticles.size()); for (const Particle& p : truthparticles) { Particle pdet = p; double peff = -1; bool keep = true; for (const ParticleEffSmearFn& fn : _detFns) { tie(pdet, peff) = fn(pdet); // smear & eff MSG_DEBUG("New det particle: pid=" << pdet.pid() << ", mom=" << pdet.mom()/GeV << " GeV, " << "pT=" << pdet.pT()/GeV << ", eta=" << pdet.eta() << " : eff=" << 100*peff << "%"); if (peff <= 0) { keep = false; break; } //< no need to roll expensive dice (and we deal with -ve probabilities, just in case) if (peff < 1 && rand01() > peff) { keep = false; break; } //< roll dice (and deal with >1 probabilities, just in case) } if (keep) { pdet.addConstituent(p); //< record where the smearing was built from _theParticles.push_back(pdet); } } } /// Reset the projection. Smearing functions will be unchanged. void reset() { _theParticles.clear(); } private: /// Stored efficiency & smearing functions vector _detFns; }; } #endif diff --git a/include/Rivet/Tools/RivetSTL.hh b/include/Rivet/Tools/RivetSTL.hh --- a/include/Rivet/Tools/RivetSTL.hh +++ b/include/Rivet/Tools/RivetSTL.hh @@ -1,182 +1,182 @@ #ifndef RIVET_RivetSTL_HH #define RIVET_RivetSTL_HH #include #include #include #include #include #include #include #include #include #include #include #include #include #include #include #include #include #include #include #include #include #ifndef foreach /// @decl A foreach macro for backward compatibility with BOOST_FOREACH #define foreach(value, container) for (value : container) #endif namespace Rivet { /// We implicitly use STL entities in the Rivet namespace using namespace std; /// @name Streaming containers as string reps /// @todo Make these named toStr rather than operator<< /// @todo Make these generic to any iterable //@{ /// Convenient function for streaming out vectors of any streamable object. template inline std::ostream& operator<<(std::ostream& os, const std::vector& vec) { os << "[ "; for (size_t i=0; i inline std::ostream& operator<<(std::ostream& os, const std::list& vec) { os << "[ "; for (size_t i=0; i inline bool contains(const std::initializer_list& il, const T& x) { return find(begin(il), end(il), x) != end(il); } /// Does the vector @a v contain @a x? template inline bool contains(const std::vector& v, const T& x) { return find(begin(v), end(v), x) != end(v); } /// Does the list @a l contain @a x? template inline bool contains(const std::list& l, const T& x) { return find(begin(l), end(l), x) != end(l); } /// Does the set @a s contain @a x? template inline bool contains(const std::set& s, const T& x) { return find(begin(s), end(s), x) != end(s); } /// Does the map @a m contain the key @a key? template inline bool has_key(const std::map& m, const K& key) { return m.find(key) != end(m); } /// Does the map @a m contain the value @a val? template inline bool has_value(const std::map& m, const T& val) { for (typename std::map::const_iterator it = begin(m); it != end(m); ++it) { if (it->second == val) return true; } return false; } //@} } namespace std { /// @name Container filling and merging //@{ /// Append a single item to vector @a v template inline void operator+=(std::vector& v, const T& x) { v.push_back(x); } /// Append all the items from vector @a v2 to vector @a v1 template inline void operator+=(std::vector& v1, const std::vector& v2) { for (const auto& x : v2) v1.push_back(x); } /// Create a new vector from the concatenated items in vectors @a v1 and @a v2 template inline std::vector operator+(const std::vector& v1, const std::vector& v2) { std::vector rtn(v1); rtn += v2; return rtn; } /// Merge the contents of set @a s2 into @a s1 template inline void operator+=(std::set& s1, const std::set& s2) { for (const auto& x : s2) s1.insert(x); } /// Merge the contents of sets @a s1 and @a s2 template inline std::set operator+(const std::set& s1, const std::set& s2) { std::set rtn(s1); rtn += s2; return rtn; } //@} /// @name Function helpers //@{ /// Get a function pointer / hash integer from an std::function template - inline size_t get_address(std::function f) { + inline uintptr_t get_address(std::function f) { typedef T(fnType)(U...); fnType ** fnPointer = f.template target(); - return (fnPointer != nullptr) ? reinterpret_cast(*fnPointer) : 0; + return (fnPointer != nullptr) ? reinterpret_cast(*fnPointer) : 0; } //@} } #endif diff --git a/src/Core/Particle.cc b/src/Core/Particle.cc --- a/src/Core/Particle.cc +++ b/src/Core/Particle.cc @@ -1,333 +1,334 @@ #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() != nullptr && genParticle()->status() == 1 && genParticle()->end_vertex() == nullptr; } 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() == nullptr) return rtn; ConstGenVertexPtr gv = genParticle()->production_vertex(); if (gv == nullptr) return rtn; vector ancestors = HepMCUtils::particles(genParticle(), Relatives::ANCESTORS); for(const auto &a: ancestors){ if(physical_only && a->status() != 1 && a->status() != 2) continue; const Particle p(a); if(c != Cuts::OPEN && !c->accept(p)) continue; rtn += p; } return rtn; } Particles Particle::parents(const Cut& c) const { Particles rtn; ConstGenVertexPtr gv = genParticle()->production_vertex(); if (gv == nullptr) return rtn; for(ConstGenParticlePtr it: HepMCUtils::particles(gv, Relatives::PARENTS)){ 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; ConstGenVertexPtr gv = 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(ConstGenParticlePtr it: HepMCUtils::particles(gv, Relatives::CHILDREN)){ 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; ConstGenVertexPtr gv = 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::descendants)) for(ConstGenParticlePtr it: HepMCUtils::particles(gv, Relatives::DESCENDANTS)){ 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(ConstGenParticlePtr it2: HepMCUtils::particles(it->end_vertex(), Relatives::CHILDREN)){ // 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; ConstGenVertexPtr gv = 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::descendants)) for(ConstGenParticlePtr it: HepMCUtils::particles(gv, Relatives::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() == nullptr) return 0; if (genParticle()->production_vertex() == nullptr) return 0; const RivetHepMC::FourVector v1 = genParticle()->production_vertex()->position(); const RivetHepMC::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 { 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; } // Obtain links to parentage if (genParticle() == nullptr) { _isDirect = std::make_pair(false, true); break; } // no HepMC connection, give up! Throw UserError exception? ConstGenVertexPtr prodVtx = genParticle()->production_vertex(); if (prodVtx == nullptr) { _isDirect = std::make_pair(false, true); break; } // orphaned particle, has to be assume false std::pair thebeams = HepMCUtils::beams(prodVtx->parent_event()); for (ConstGenParticlePtr ancestor : HepMCUtils::particles(prodVtx, Relatives::ANCESTORS)) { const PdgId pid = ancestor->pdg_id(); /// @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 if (ancestor->status() != 2) continue; // no non-standard // statuses or beams to // be used in decision // making + if (ancestor == thebeams.first || ancestor == thebeams.second) continue; // ignore beam particles 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 _isDirect.first; } /////////////////////// // DISABLED UNTIL VANILLA CC7 COMPATIBILITY NOT NEEDED // /// Particles copy constructor from vector // Particles::Particles(const std::vector& 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; } }