cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79484.v1/t10
title: "Table 10" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $y(J/\psi J/\psi)$ for $p_{T}(J/\psi J/\psi)&gt;1$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t11
title: "Table 11" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $y(J/\psi)$ for $p_{T}(J/\psi J/\psi)&gt;1$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t12
title: "Table 12" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $|\Delta y|$ for $p_{T}(J/\psi J/\psi)&gt;1$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t13
title: "Table 13" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $|\Delta \phi|$ for $p_{T}(J/\psi J/\psi)&gt;1$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t7
title: "Table 7" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $\mathcal{A}_{\mathrm{T}}$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t8
title: "Table 8" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $M(J/\psi J/\psi)$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t9
title: "Table 9" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $p_{T}(J/\psi)$ for $p_{T}(J/\psi J/\psi)&gt;1$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t14
title: "Table 14" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $\mathcal{A}_{\mathrm{T}}$ for $p_{T}(J/\psi J/\psi)&gt;1$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t15
title: "Table 15" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $M(J/\psi J/\psi)$ for $p_{T}(J/\psi J/\psi)&gt;1$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t16
title: "Table 16" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $p_{T}(J/\psi)$ for $p_{T}(J/\psi J/\psi)&gt;3$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t17
title: "Table 17" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $y(J/\psi J/\psi)$ for $p_{T}(J/\psi J/\psi)&gt;3$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t18
title: "Table 18" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $y(J/\psi)$ for $p_{T}(J/\psi J/\psi)&gt;3$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t19
title: "Table 19" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $|\Delta y|$ for $p_{T}(J/\psi J/\psi)&gt;3$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t20
title: "Table 20" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $|\Delta \phi|$ for $p_{T}(J/\psi J/\psi)&gt;3$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t21
title: "Table 21" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $\mathcal{A}_{\mathrm{T}}$ for $p_{T}(J/\psi J/\psi)&gt;3$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79484.v1/t22
title: "Table 22" of "Measurement of the $J/\psi$ pair production cross-section in $pp$ collisions at $\sqrt{s} = 13 \,{\mathrm{TeV}}$"

description: Differential cross-section of $J/\psi$ pair as a function of $M(J/\psi J/\psi)$ for $p_{T}(J/\psi J/\psi)&gt;3$ GeV$/c$.
description: CERN-LHC. The production cross-section of $J/\psi$ pairs is measured using a data sample of $pp$ collisions collected by the LHCb experiment at a centre-of-mass energy of $\sqrt{s} = 13$ TeV, corresponding to an integrated luminosity of $279 \pm 11 {\mathrm{pb^{-1}}}$. 
The measurement is performed for $J/\psi$ mesons with a transverse momentum of less than 10 GeV$/c$ in the rapidity range $2.0
DOI: 10.17182/hepdata.79497.v1/t1
title: "Table 1" of "Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Measured differential fiducial cross sections in Higgs transverse momentum (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.
description: CERN-LHC. Measurements of fiducial and differential cross sections of Higgs boson production in the H-&gt;ZZ*-&gt;4l channel in proton-proton collisions at a centre-of-mass energy of 13 TeV with 36.1 fb^-1 of data collected in 2015 and 2016. The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons.


The 4l channel fiducial region is defined as:
- 4e, 4mu or 2e2mu
- ptElectron &gt; 7 GeV, ptMuon &gt; 5 GeV
- |etaElectron| &lt; 2.47, |etaMuon| &lt; 2.7
- ptJets &gt; 30 GeV, |etaJets| &lt; 4.4
- jets removed if overlap with lepton: deltaR(e,jet) &gt; 0.2, deltaR(m,jet) &gt; 0.1 
- Ambiguities in pairing are resolved by picking the same flavor opposite sign pair with the smallest |mZ - mll| as the leading pair, and the remaining pair with the smallest |mZ - mll| as the subleading pair
- at least one lepton with each 20, 15, 10 GeV
- mass requirements 50 GeV &lt; m12 &lt; 106 GeV, 12 GeV &lt; m34 &lt; 115 GeV
- min(DeltaR(l,l)) &gt; 0.1 (0.2) for same flavor (opposite flavor) lepton pairs
- Jpsi veto: mll &gt; 5 GeV for all same flavor opposite sign pairs
- m4l requirement: 115 GeV &lt; m4l &lt; 130 GeV
DOI: 10.17182/hepdata.79497.v1/t2
title: "Table 2" of "Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Measured differential fiducial cross sections in Higgs rapidity (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.
description: CERN-LHC. Measurements of fiducial and differential cross sections of Higgs boson production in the H-&gt;ZZ*-&gt;4l channel in proton-proton collisions at a centre-of-mass energy of 13 TeV with 36.1 fb^-1 of data collected in 2015 and 2016. The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons.


The 4l channel fiducial region is defined as:
- 4e, 4mu or 2e2mu
- ptElectron &gt; 7 GeV, ptMuon &gt; 5 GeV
- |etaElectron| &lt; 2.47, |etaMuon| &lt; 2.7
- ptJets &gt; 30 GeV, |etaJets| &lt; 4.4
- jets removed if overlap with lepton: deltaR(e,jet) &gt; 0.2, deltaR(m,jet) &gt; 0.1 
- Ambiguities in pairing are resolved by picking the same flavor opposite sign pair with the smallest |mZ - mll| as the leading pair, and the remaining pair with the smallest |mZ - mll| as the subleading pair
- at least one lepton with each 20, 15, 10 GeV
- mass requirements 50 GeV &lt; m12 &lt; 106 GeV, 12 GeV &lt; m34 &lt; 115 GeV
- min(DeltaR(l,l)) &gt; 0.1 (0.2) for same flavor (opposite flavor) lepton pairs
- Jpsi veto: mll &gt; 5 GeV for all same flavor opposite sign pairs
- m4l requirement: 115 GeV &lt; m4l &lt; 130 GeV
DOI: 10.17182/hepdata.79497.v1/t3
title: "Table 3" of "Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Measured differential fiducial cross sections in invariant mass of the subleading lepton pair (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.
description: CERN-LHC. Measurements of fiducial and differential cross sections of Higgs boson production in the H-&gt;ZZ*-&gt;4l channel in proton-proton collisions at a centre-of-mass energy of 13 TeV with 36.1 fb^-1 of data collected in 2015 and 2016. The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons.


The 4l channel fiducial region is defined as:
- 4e, 4mu or 2e2mu
- ptElectron &gt; 7 GeV, ptMuon &gt; 5 GeV
- |etaElectron| &lt; 2.47, |etaMuon| &lt; 2.7
- ptJets &gt; 30 GeV, |etaJets| &lt; 4.4
- jets removed if overlap with lepton: deltaR(e,jet) &gt; 0.2, deltaR(m,jet) &gt; 0.1 
- Ambiguities in pairing are resolved by picking the same flavor opposite sign pair with the smallest |mZ - mll| as the leading pair, and the remaining pair with the smallest |mZ - mll| as the subleading pair
- at least one lepton with each 20, 15, 10 GeV
- mass requirements 50 GeV &lt; m12 &lt; 106 GeV, 12 GeV &lt; m34 &lt; 115 GeV
- min(DeltaR(l,l)) &gt; 0.1 (0.2) for same flavor (opposite flavor) lepton pairs
- Jpsi veto: mll &gt; 5 GeV for all same flavor opposite sign pairs
- m4l requirement: 115 GeV &lt; m4l &lt; 130 GeV
DOI: 10.17182/hepdata.79497.v1/t4
title: "Table 4" of "Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Measured differential fiducial cross sections in cos(theta*) (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.
description: CERN-LHC. Measurements of fiducial and differential cross sections of Higgs boson production in the H-&gt;ZZ*-&gt;4l channel in proton-proton collisions at a centre-of-mass energy of 13 TeV with 36.1 fb^-1 of data collected in 2015 and 2016. The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons.


The 4l channel fiducial region is defined as:
- 4e, 4mu or 2e2mu
- ptElectron &gt; 7 GeV, ptMuon &gt; 5 GeV
- |etaElectron| &lt; 2.47, |etaMuon| &lt; 2.7
- ptJets &gt; 30 GeV, |etaJets| &lt; 4.4
- jets removed if overlap with lepton: deltaR(e,jet) &gt; 0.2, deltaR(m,jet) &gt; 0.1 
- Ambiguities in pairing are resolved by picking the same flavor opposite sign pair with the smallest |mZ - mll| as the leading pair, and the remaining pair with the smallest |mZ - mll| as the subleading pair
- at least one lepton with each 20, 15, 10 GeV
- mass requirements 50 GeV &lt; m12 &lt; 106 GeV, 12 GeV &lt; m34 &lt; 115 GeV
- min(DeltaR(l,l)) &gt; 0.1 (0.2) for same flavor (opposite flavor) lepton pairs
- Jpsi veto: mll &gt; 5 GeV for all same flavor opposite sign pairs
- m4l requirement: 115 GeV &lt; m4l &lt; 130 GeV
DOI: 10.17182/hepdata.79497.v1/t10
title: "Table 10" of "Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Measured differential fiducial cross sections in Higgs transverse momentum for 0 jet events (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.
description: CERN-LHC. Measurements of fiducial and differential cross sections of Higgs boson production in the H-&gt;ZZ*-&gt;4l channel in proton-proton collisions at a centre-of-mass energy of 13 TeV with 36.1 fb^-1 of data collected in 2015 and 2016. The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons.


The 4l channel fiducial region is defined as:
- 4e, 4mu or 2e2mu
- ptElectron &gt; 7 GeV, ptMuon &gt; 5 GeV
- |etaElectron| &lt; 2.47, |etaMuon| &lt; 2.7
- ptJets &gt; 30 GeV, |etaJets| &lt; 4.4
- jets removed if overlap with lepton: deltaR(e,jet) &gt; 0.2, deltaR(m,jet) &gt; 0.1 
- Ambiguities in pairing are resolved by picking the same flavor opposite sign pair with the smallest |mZ - mll| as the leading pair, and the remaining pair with the smallest |mZ - mll| as the subleading pair
- at least one lepton with each 20, 15, 10 GeV
- mass requirements 50 GeV &lt; m12 &lt; 106 GeV, 12 GeV &lt; m34 &lt; 115 GeV
- min(DeltaR(l,l)) &gt; 0.1 (0.2) for same flavor (opposite flavor) lepton pairs
- Jpsi veto: mll &gt; 5 GeV for all same flavor opposite sign pairs
- m4l requirement: 115 GeV &lt; m4l &lt; 130 GeV
DOI: 10.17182/hepdata.79497.v1/t11
title: "Table 11" of "Measurement of inclusive and differential cross sections in the $H \rightarrow ZZ^* \rightarrow 4\ell$ decay channel in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Measured differential fiducial cross sections in Higgs transverse momentum for 1-jet events (second column). The given uncertainty is split into statistical (first) and systematic components (second). Values without uncertainties are 95% CL limits in the absence of signal events. The third column gives the theoretical prediction of Higgs production in the fiducial volume using Powheg NNLOPS for the ggF process, Powheg for the VBF and the VH processes, and Madgraph5_aMC@NLO for the ttH and bbH processes. The uncertainty includes PDF, scale, and branching fraction uncertainty. All predictions were normalized to the best available inclusive Higgs production cross sections at the time of the publication.
description: CERN-LHC. Measurements of fiducial and differential cross sections of Higgs boson production in the H-&gt;ZZ*-&gt;4l channel in proton-proton collisions at a centre-of-mass energy of 13 TeV with 36.1 fb^-1 of data collected in 2015 and 2016. The final states used are 4 electrons, 4 muons, 2 electrons and 2 muons.


The 4l channel fiducial region is defined as:
- 4e, 4mu or 2e2mu
- ptElectron &gt; 7 GeV, ptMuon &gt; 5 GeV
- |etaElectron| &lt; 2.47, |etaMuon| &lt; 2.7
- ptJets &gt; 30 GeV, |etaJets| &lt; 4.4
- jets removed if overlap with lepton: deltaR(e,jet) &gt; 0.2, deltaR(m,jet) &gt; 0.1 
- Ambiguities in pairing are resolved by picking the same flavor opposite sign pair with the smallest |mZ - mll| as the leading pair, and the remaining pair with the smallest |mZ - mll| as the subleading pair
- at least one lepton with each 20, 15, 10 GeV
- mass requirements 50 GeV &lt; m12 &lt; 106 GeV, 12 GeV &lt; m34 &lt; 115 GeV
- min(DeltaR(l,l)) &gt; 0.1 (0.2) for same flavor (opposite flavor) lepton pairs
- Jpsi veto: mll &gt; 5 GeV for all same flavor opposite sign pairs
- m4l requirement: 115 GeV &lt; m4l &lt; 130 GeV