diff --git a/analyses/pluginATLAS/ATLAS_2017_I1514251.cc b/analyses/pluginATLAS/ATLAS_2017_I1514251.cc --- a/analyses/pluginATLAS/ATLAS_2017_I1514251.cc +++ b/analyses/pluginATLAS/ATLAS_2017_I1514251.cc @@ -1,193 +1,178 @@ // -*- C++ -*- #include "Rivet/Analysis.hh" #include "Rivet/Projections/ZFinder.hh" #include "Rivet/Projections/FastJets.hh" #include "Rivet/Projections/VetoedFinalState.hh" namespace Rivet { /// Z + jets in pp at 13 TeV /// @note This base class contains a "mode" variable for combined, e, and mu channel derived classes class ATLAS_2017_I1514251 : public Analysis { public: /// Constructor - ATLAS_2017_I1514251(const string name="ATLAS_2017_I1514251", size_t channel = 0, - const string ref_data="ATLAS_2017_I1514251") : Analysis(name) { - // This class uses the combined e+mu mode - _mode = channel; - setRefDataName(ref_data); - } + DEFAULT_RIVET_ANALYSIS_CTOR(ATLAS_2017_I1514251); /// Book histograms and initialise projections before the run void init() { + + // Get options from the new option system + _mode = 0; + if ( getOption("LMODE") == "EL" ) _mode = 0; + if ( getOption("LMODE") == "MU" ) _mode = 1; + const FinalState fs; Cut cuts = (Cuts::pT > 25*GeV) && (Cuts::abseta < 2.5); ZFinder zeefinder(fs, cuts, PID::ELECTRON, 71*GeV, 111*GeV); ZFinder zmumufinder(fs, cuts, PID::MUON, 71*GeV, 111*GeV); declare(zeefinder, "zeefinder"); declare(zmumufinder, "zmumufinder"); // Define veto FS in order to prevent Z-decay products entering the jet algorithm VetoedFinalState had_fs; had_fs.addVetoOnThisFinalState(zeefinder); had_fs.addVetoOnThisFinalState(zmumufinder); FastJets jets(had_fs, FastJets::ANTIKT, 0.4); jets.useInvisibles(true); declare(jets, "jets"); // individual channels _h_Njets_excl = bookHisto1D( _mode + 1, 1, 1); _h_Njets = bookHisto1D( _mode + 4, 1, 1); _h_Njets_Ratio = bookScatter2D(_mode + 7, 1, 1, true); _h_leading_jet_pT_eq1jet = bookHisto1D(_mode + 10, 1, 1); _h_leading_jet_pT = bookHisto1D(_mode + 13, 1, 1); _h_leading_jet_pT_2jet = bookHisto1D(_mode + 16, 1, 1); _h_leading_jet_pT_3jet = bookHisto1D(_mode + 19, 1, 1); _h_leading_jet_pT_4jet = bookHisto1D(_mode + 22, 1, 1); _h_leading_jet_rap = bookHisto1D(_mode + 25, 1, 1); _h_HT = bookHisto1D(_mode + 28, 1, 1); _h_jet_dphi = bookHisto1D(_mode + 31, 1, 1); _h_jet_mass = bookHisto1D(_mode + 34, 1, 1); } /// Perform the per-event analysis void analyze(const Event& event) { const double weight = event.weight(); const ZFinder& zeefinder = apply(event, "zeefinder"); const ZFinder& zmumufinder = apply(event, "zmumufinder"); const Particles& zees = zeefinder.bosons(); const Particles& zmumus = zmumufinder.bosons(); //Veto Z->mumu in electron mode, and vice versa: if (_mode==1 && (zees.size()!=1 || zmumus.size() ) ) vetoEvent; else if (_mode==2 && (zees.size() || zmumus.size()!=1 ) ) vetoEvent; else if (zees.size() + zmumus.size() != 1) { // Running in combined mode, we did not find exactly one Z. Not good. MSG_DEBUG("Did not find exactly one good Z candidate"); vetoEvent; } // Find the (dressed!) leptons const Particles& leptons = zees.size() ? zeefinder.constituents() : zmumufinder.constituents(); if (leptons.size() != 2) vetoEvent; Jets jets = apply(event, "jets").jetsByPt(Cuts::pT > 30*GeV && Cuts::absrap < 2.5); bool veto = false; foreach(const Jet& j, jets) { foreach(const Particle& l, leptons) { veto |= deltaR(j, l) < 0.4; } } if (veto) vetoEvent; double HT=0; foreach(const Particle& l, leptons) { HT += l.pT(); } const size_t Njets = jets.size(); _h_Njets_excl->fill(Njets, weight); for(size_t i = 0; i <= Njets; ++i) { _h_Njets->fill(i, weight); } if (Njets < 1) vetoEvent; for(size_t i = 0; i < Njets; ++i) { HT += jets[i].pT(); } const double pT = jets[0].pT(); const double rap = jets[0].rapidity(); _h_HT->fill(HT, weight); _h_leading_jet_rap->fill(fabs(rap), weight); _h_leading_jet_pT->fill(pT, weight); if (Njets == 1) _h_leading_jet_pT_eq1jet->fill(pT, weight); if (Njets > 1) { _h_leading_jet_pT_2jet->fill(pT, weight); _h_jet_dphi->fill( deltaPhi(jets[0], jets[1]), weight ); _h_jet_mass->fill( (jets[0].momentum()+jets[1].momentum()).mass() , weight ); } if (Njets > 2) _h_leading_jet_pT_3jet->fill(pT, weight); if (Njets > 3) _h_leading_jet_pT_4jet->fill(pT, weight); } void finalize() { for (size_t i = 0; i < _h_Njets->numBins()-2; ++i) { double n = _h_Njets->bin(i + 1).sumW(); double dN = _h_Njets->bin(i + 1).sumW2(); double d = _h_Njets->bin(i).sumW(); double dD = _h_Njets->bin(i).sumW2(); double r = safediv(n, d); double e = sqrt( safediv(r * (1 - r), d) ); if ( _h_Njets->effNumEntries() != _h_Njets->numEntries() ) { // use F. James's approximation for weighted events: e = sqrt( safediv((1 - 2 * r) * dN + r * r * dD, d * d) ); } _h_Njets_Ratio->point(i).setY(r, e); } scale(_h_Njets, crossSectionPerEvent() ); scale(_h_Njets_excl, crossSectionPerEvent() ); scale(_h_HT, crossSectionPerEvent() ); scale(_h_leading_jet_rap, crossSectionPerEvent() ); scale(_h_leading_jet_pT, crossSectionPerEvent() ); scale(_h_leading_jet_pT_eq1jet, crossSectionPerEvent() ); scale(_h_leading_jet_pT_2jet, crossSectionPerEvent() ); scale(_h_leading_jet_pT_3jet, crossSectionPerEvent() ); scale(_h_leading_jet_pT_4jet, crossSectionPerEvent() ); scale(_h_jet_dphi, crossSectionPerEvent() ); scale(_h_jet_mass, crossSectionPerEvent() ); } //@} protected: size_t _mode; private: Scatter2DPtr _h_Njets_Ratio; Histo1DPtr _h_Njets; Scatter2DPtr _h_Njets_excl_Ratio; Histo1DPtr _h_Njets_excl; Histo1DPtr _h_HT; Histo1DPtr _h_leading_jet_rap; Histo1DPtr _h_leading_jet_pT; Histo1DPtr _h_leading_jet_pT_eq1jet; Histo1DPtr _h_leading_jet_pT_2jet; Histo1DPtr _h_leading_jet_pT_3jet; Histo1DPtr _h_leading_jet_pT_4jet; Histo1DPtr _h_jet_dphi; Histo1DPtr _h_jet_mass; }; + DECLARE_RIVET_PLUGIN(ATLAS_2017_I1514251); - - class ATLAS_2017_I1514251_EL : public ATLAS_2017_I1514251 { - public: - ATLAS_2017_I1514251_EL() : ATLAS_2017_I1514251("ATLAS_2017_I1514251_EL", 1) { } - }; - - - - class ATLAS_2017_I1514251_MU : public ATLAS_2017_I1514251 { - public: - ATLAS_2017_I1514251_MU() : ATLAS_2017_I1514251("ATLAS_2017_I1514251_MU", 2) { } - }; - - - DECLARE_RIVET_PLUGIN(ATLAS_2017_I1514251); - DECLARE_RIVET_PLUGIN(ATLAS_2017_I1514251_EL); - DECLARE_RIVET_PLUGIN(ATLAS_2017_I1514251_MU); } diff --git a/analyses/pluginATLAS/ATLAS_2017_I1514251.info b/analyses/pluginATLAS/ATLAS_2017_I1514251.info --- a/analyses/pluginATLAS/ATLAS_2017_I1514251.info +++ b/analyses/pluginATLAS/ATLAS_2017_I1514251.info @@ -1,45 +1,47 @@ Name: ATLAS_2017_I1514251 Year: 2017 Summary: Z plus jets at 13 TeV Experiment: ATLAS Collider: LHC InspireID: 1514251 Status: VALIDATED Authors: - Gavin Hesketh References: - arXiv:1702.05725 [hep-ex] - submitted to EPJC Keywords: - zboson - jets RunInfo: pp -> Z(->ll) + jets at 13 TeV Luminosity_fb: 3.16 Beams: [p+, p+] Energies: [13000] PtCuts: [25, 25] +Options: + - LMODE=EL,MU Description: 'Measurements of the production cross section of a $Z$ boson in association with jets in proton-proton collisions at i $\sqrt{s}=13$ TeV are presented, using data corresponding to an integrated luminosity of 3.16 fb${}^{-1}$ collected by the ATLAS experiment at the CERN Large Hadron Collider in 2015. Inclusive and differential cross sections are measured for events containing a $Z$ boson decaying to electrons or muons and produced in association with up to seven jets with $p_\text{T}>30$ GeV and $|y|<2.5$. Predictions from different Monte Carlo generators based on leading-order and next-to-leading-order matrix elements for up to two additional partons interfaced with parton shower and fixed-order predictions at next-to-leading order and next-to-next-to-leading order are compared with the measured cross sections. Good agreement within the uncertainties is observed for most of the modelled quantities, in particular with the generators which use next-to-leading-order matrix elements and the more recent next-to-next-to-leading-order fixed-order predictions.' BibKey: Aaboud:2017hbk BibTeX: '@article{Aaboud:2017hbk, author = "Aaboud, Morad and others", title = "{Measurements of the production cross section of a $Z$ boson in association with jets in pp collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector}", collaboration = "ATLAS", year = "2017", eprint = "1702.05725", archivePrefix = "arXiv", primaryClass = "hep-ex", reportNumber = "CERN-EP-2016-297", SLACcitation = "%%CITATION = ARXIV:1702.05725;%%" }' diff --git a/analyses/pluginATLAS/ATLAS_2017_I1514251.plot b/analyses/pluginATLAS/ATLAS_2017_I1514251.plot --- a/analyses/pluginATLAS/ATLAS_2017_I1514251.plot +++ b/analyses/pluginATLAS/ATLAS_2017_I1514251.plot @@ -1,97 +1,99 @@ # BEGIN PLOT /ATLAS_2017_I1514251/d.. XTwosidedTicks=1 YTwosidedTicks=1 LeftMargin=1.5 XMinorTickMarks=0 LogY=1 LegendAlign=r Title=$Z \rightarrow \ell^+ \ell^-$, dressed level # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d0[4-6] XLabel=$N_\text{jets}$ XCustomMajorTicks=0 $\ge0$ 1 $\ge1$ 2 $\ge2$ 3 $\ge3$ 4 $\ge4$ 5 $\ge5$ 6 $\ge6$ 7 $\ge7$ YLabel=$\sigma(Z + \geq N_\text{jets})$ [pb] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d0[7-9] LogY=0 XLabel=$N_\text{jets}$ XCustomMajorTicks=0 $\ge$1/$\ge$0 1 $\ge$2/$\ge$1 2 $\ge$3/$\ge$2 3 $\ge$4/$\ge$3 4 $\ge$5/$\ge$4 5 $\ge$6/$\ge$5 6 $\ge$7/$\ge$6 LegendYPos=0.3 YLabel=$\sigma(Z + \geq N_\text{jets}+1) / \sigma(Z + \geq N_\text{jets})$ # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d0[1-3] XLabel=$N_\text{jets}$ YLabel=$\sigma(Z + N_\text{jets})$ [pb] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d28 YLabel=d$\sigma/$d$H_\text{T}$ [pb/GeV] XLabel=$H_\text{T}$ [GeV] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d29 YLabel=d$\sigma/$d$H_\text{T}$ [pb/GeV] XLabel=$H_\text{T}$ [GeV] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d30 YLabel=d$\sigma/$d$H_\text{T}$ [pb/GeV] XLabel=$H_\text{T}$ [GeV] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d2[5-7] YLabel=d$\sigma/$d$y^\text{jet}$ [pb] XLabel=$y^\text{jet}$ (leading jet) # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d1[0-2] YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] XLabel=$p_\text{T}^\text{jet}$ (== 1 jet) [GeV] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d1[3-5] YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 1 jet) [GeV] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d1[6-8] YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 2 jet) [GeV] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d19 YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 3 jet) [GeV] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d20 YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 3 jet) [GeV] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d21 YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 3 jet) [GeV] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d2[2-4] YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 4 jet) [GeV] # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d3[1-3] YLabel=d$\sigma/$d$\Delta\phi$ [pb] XLabel=$\Delta\phi$(leading, second jet) LegendAlign=l LegendXPos=0.05 # END PLOT # BEGIN PLOT /ATLAS_2017_I1514251/d3[4-6] YLabel=d$\sigma/$d$M$ [pb/GeV] XLabel=$M$(leading, second jet) [GeV] # END PLOT + + diff --git a/analyses/pluginATLAS/ATLAS_2017_I1514251_EL.info b/analyses/pluginATLAS/ATLAS_2017_I1514251_EL.info deleted file mode 100644 --- a/analyses/pluginATLAS/ATLAS_2017_I1514251_EL.info +++ /dev/null @@ -1,45 +0,0 @@ -Name: ATLAS_2017_I1514251_EL -Year: 2017 -Summary: Z plus jets at 13 TeV, electron channel -Experiment: ATLAS -Collider: LHC -InspireID: 1514251 -Status: VALIDATED -Authors: - - Gavin Hesketh -References: - - arXiv:1702.05725 [hep-ex] - - submitted to EPJC -Keywords: - - zboson - - jets -RunInfo: - pp -> Z(->ee) + jets at 13 TeV -Luminosity_fb: 3.16 -Beams: [p+, p+] -Energies: [13000] -PtCuts: [25, 25] -Description: - 'Measurements of the production cross section of a $Z$ boson in association with jets in proton-proton collisions at i - $\sqrt{s}=13$ TeV are presented, using data corresponding to an integrated luminosity of 3.16 fb${}^{-1}$ collected by - the ATLAS experiment at the CERN Large Hadron Collider in 2015. Inclusive and differential cross sections are measured - for events containing a $Z$ boson decaying to electrons or muons and produced in association with up to seven jets with - $p_\text{T}>30$ GeV and $|y|<2.5$. Predictions from different Monte Carlo generators based on leading-order and - next-to-leading-order matrix elements for up to two additional partons interfaced with parton shower and fixed-order - predictions at next-to-leading order and next-to-next-to-leading order are compared with the measured cross sections. - Good agreement within the uncertainties is observed for most of the modelled quantities, in particular with the generators - which use next-to-leading-order matrix elements and the more recent next-to-next-to-leading-order fixed-order predictions.' -BibKey: Aaboud:2017hbk -BibTeX: '@article{Aaboud:2017hbk, - author = "Aaboud, Morad and others", - title = "{Measurements of the production cross section of a $Z$ - boson in association with jets in pp collisions at - $\sqrt{s} = 13$ TeV with the ATLAS detector}", - collaboration = "ATLAS", - year = "2017", - eprint = "1702.05725", - archivePrefix = "arXiv", - primaryClass = "hep-ex", - reportNumber = "CERN-EP-2016-297", - SLACcitation = "%%CITATION = ARXIV:1702.05725;%%" -}' diff --git a/analyses/pluginATLAS/ATLAS_2017_I1514251_EL.plot b/analyses/pluginATLAS/ATLAS_2017_I1514251_EL.plot deleted file mode 100644 --- a/analyses/pluginATLAS/ATLAS_2017_I1514251_EL.plot +++ /dev/null @@ -1,97 +0,0 @@ -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d.. -XTwosidedTicks=1 -YTwosidedTicks=1 -LeftMargin=1.5 -XMinorTickMarks=0 -LogY=1 -LegendAlign=r -Title=$Z \rightarrow \ell^+ \ell^-$, dressed level -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d0[4-6] -XLabel=$N_\text{jets}$ -XCustomMajorTicks=0 $\ge0$ 1 $\ge1$ 2 $\ge2$ 3 $\ge3$ 4 $\ge4$ 5 $\ge5$ 6 $\ge6$ 7 $\ge7$ -YLabel=$\sigma(Z + \geq N_\text{jets})$ [pb] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d0[7-9] -LogY=0 -XLabel=$N_\text{jets}$ -XCustomMajorTicks=0 $\ge$1/$\ge$0 1 $\ge$2/$\ge$1 2 $\ge$3/$\ge$2 3 $\ge$4/$\ge$3 4 $\ge$5/$\ge$4 5 $\ge$6/$\ge$5 6 $\ge$7/$\ge$6 -LegendYPos=0.3 -YLabel=$\sigma(Z + \geq N_\text{jets}+1) / \sigma(Z + \geq N_\text{jets})$ -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d0[1-3] -XLabel=$N_\text{jets}$ -YLabel=$\sigma(Z + N_\text{jets})$ [pb] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d28 -YLabel=d$\sigma/$d$H_\text{T}$ [pb/GeV] -XLabel=$H_\text{T}$ [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d29 -YLabel=d$\sigma/$d$H_\text{T}$ [pb/GeV] -XLabel=$H_\text{T}$ [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d30 -YLabel=d$\sigma/$d$H_\text{T}$ [pb/GeV] -XLabel=$H_\text{T}$ [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d2[5-7] -YLabel=d$\sigma/$d$y^\text{jet}$ [pb] -XLabel=$y^\text{jet}$ (leading jet) -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d1[0-2] -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (== 1 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d1[3-5] -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 1 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d1[6-8] -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 2 jet) [GeV] -# END PLOT - - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d19 -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 3 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d20 -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 3 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d21 -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 3 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d2[2-4] -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 4 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d3[1-3] -YLabel=d$\sigma/$d$\Delta\phi$ [pb] -XLabel=$\Delta\phi$(leading, second jet) -LegendAlign=l -LegendXPos=0.05 -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_EL/d3[4-6] -YLabel=d$\sigma/$d$M$ [pb/GeV] -XLabel=$M$(leading, second jet) [GeV] -# END PLOT - diff --git a/analyses/pluginATLAS/ATLAS_2017_I1514251_MU.info b/analyses/pluginATLAS/ATLAS_2017_I1514251_MU.info deleted file mode 100644 --- a/analyses/pluginATLAS/ATLAS_2017_I1514251_MU.info +++ /dev/null @@ -1,45 +0,0 @@ -Name: ATLAS_2017_I1514251_MU -Year: 2017 -Summary: Z plus jets at 13 TeV, muon channel -Experiment: ATLAS -Collider: LHC -InspireID: 1514251 -Status: VALIDATED -Authors: - - Gavin Hesketh -References: - - arXiv:1702.05725 [hep-ex] - - submitted to EPJC -Keywords: - - zboson - - jets -RunInfo: - pp -> Z(->mumu) + jets at 13 TeV -Luminosity_fb: 3.16 -Beams: [p+, p+] -Energies: [13000] -PtCuts: [25, 25] -Description: - 'Measurements of the production cross section of a $Z$ boson in association with jets in proton-proton collisions at i - $\sqrt{s}=13$ TeV are presented, using data corresponding to an integrated luminosity of 3.16 fb${}^{-1}$ collected by - the ATLAS experiment at the CERN Large Hadron Collider in 2015. Inclusive and differential cross sections are measured - for events containing a $Z$ boson decaying to electrons or muons and produced in association with up to seven jets with - $p_\text{T}>30$ GeV and $|y|<2.5$. Predictions from different Monte Carlo generators based on leading-order and - next-to-leading-order matrix elements for up to two additional partons interfaced with parton shower and fixed-order - predictions at next-to-leading order and next-to-next-to-leading order are compared with the measured cross sections. - Good agreement within the uncertainties is observed for most of the modelled quantities, in particular with the generators - which use next-to-leading-order matrix elements and the more recent next-to-next-to-leading-order fixed-order predictions.' -BibKey: Aaboud:2017hbk -BibTeX: '@article{Aaboud:2017hbk, - author = "Aaboud, Morad and others", - title = "{Measurements of the production cross section of a $Z$ - boson in association with jets in pp collisions at - $\sqrt{s} = 13$ TeV with the ATLAS detector}", - collaboration = "ATLAS", - year = "2017", - eprint = "1702.05725", - archivePrefix = "arXiv", - primaryClass = "hep-ex", - reportNumber = "CERN-EP-2016-297", - SLACcitation = "%%CITATION = ARXIV:1702.05725;%%" -}' diff --git a/analyses/pluginATLAS/ATLAS_2017_I1514251_MU.plot b/analyses/pluginATLAS/ATLAS_2017_I1514251_MU.plot deleted file mode 100644 --- a/analyses/pluginATLAS/ATLAS_2017_I1514251_MU.plot +++ /dev/null @@ -1,97 +0,0 @@ -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d.. -XTwosidedTicks=1 -YTwosidedTicks=1 -LeftMargin=1.5 -XMinorTickMarks=0 -LogY=1 -LegendAlign=r -Title=$Z \rightarrow \ell^+ \ell^-$, dressed level -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d0[4-6] -XLabel=$N_\text{jets}$ -XCustomMajorTicks=0 $\ge0$ 1 $\ge1$ 2 $\ge2$ 3 $\ge3$ 4 $\ge4$ 5 $\ge5$ 6 $\ge6$ 7 $\ge7$ -YLabel=$\sigma(Z + \geq N_\text{jets})$ [pb] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d0[7-9] -LogY=0 -XLabel=$N_\text{jets}$ -XCustomMajorTicks=0 $\ge$1/$\ge$0 1 $\ge$2/$\ge$1 2 $\ge$3/$\ge$2 3 $\ge$4/$\ge$3 4 $\ge$5/$\ge$4 5 $\ge$6/$\ge$5 6 $\ge$7/$\ge$6 -LegendYPos=0.3 -YLabel=$\sigma(Z + \geq N_\text{jets}+1) / \sigma(Z + \geq N_\text{jets})$ -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d0[1-3] -XLabel=$N_\text{jets}$ -YLabel=$\sigma(Z + N_\text{jets})$ [pb] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d28 -YLabel=d$\sigma/$d$H_\text{T}$ [pb/GeV] -XLabel=$H_\text{T}$ [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d29 -YLabel=d$\sigma/$d$H_\text{T}$ [pb/GeV] -XLabel=$H_\text{T}$ [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d30 -YLabel=d$\sigma/$d$H_\text{T}$ [pb/GeV] -XLabel=$H_\text{T}$ [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d2[5-7] -YLabel=d$\sigma/$d$y^\text{jet}$ [pb] -XLabel=$y^\text{jet}$ (leading jet) -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d1[0-2] -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (== 1 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d1[3-5] -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 1 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d1[6-8] -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 2 jet) [GeV] -# END PLOT - - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d19 -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 3 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d20 -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 3 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d21 -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 3 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d2[2-4] -YLabel=d$\sigma/$d$p_\text{T}^\text{jet}$ [pb/GeV] -XLabel=$p_\text{T}^\text{jet}$ (leading jet, $\ge$ 4 jet) [GeV] -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d3[1-3] -YLabel=d$\sigma/$d$\Delta\phi$ [pb] -XLabel=$\Delta\phi$(leading, second jet) -LegendAlign=l -LegendXPos=0.05 -# END PLOT - -# BEGIN PLOT /ATLAS_2017_I1514251_MU/d3[4-6] -YLabel=d$\sigma/$d$M$ [pb/GeV] -XLabel=$M$(leading, second jet) [GeV] -# END PLOT -