cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.89171.v1/t10
title: "13 TeV $\Delta\eta_{jj}$ normalized" of "Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV"

description: Data from Fig. 6 right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the invariant of pseudorapidity separation of the two $p$_T$ leading jets with $|\eta_{j}| &lt; 4.7$.
description: CERN-LHC. The measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at 13 TeV an 8 TeV are reported. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb-1 at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes $\textrm{p} \textrm{p} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$, where where $\ell,\ell^{\prime} = e, \mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_T$, and pseudorapidity of the $p_T$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_T$-leading jets and their pseudorapidity separation, are reported. The fiducial region for the 13 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, lepton $p_T$ &gt; 5 GeV, psudorapidity of electrons and muons |eta| &lt; 2.5, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The fiducial region for the 8 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, muon $p_T$ &gt; 5 GeV, electron $p_T$ &gt; 7 GeV, psudorapidity of electrons |eta| &lt; 2.5, psudorapidity of muons |eta| &lt; 2.4, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The generator-level lepton momenta are corrected by adding the momenta of generator-level photons within $\Delta \textrm{R} \left(\ell,\gamma\right) &lt; 0.1$
DOI: 10.17182/hepdata.89171.v1/t12
title: "8 TeV nJets normalized" of "Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV"

description: Data from Fig. 3 upper left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| &lt; 4.7$.
description: CERN-LHC. The measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at 13 TeV an 8 TeV are reported. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb-1 at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes $\textrm{p} \textrm{p} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$, where where $\ell,\ell^{\prime} = e, \mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_T$, and pseudorapidity of the $p_T$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_T$-leading jets and their pseudorapidity separation, are reported. The fiducial region for the 13 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, lepton $p_T$ &gt; 5 GeV, psudorapidity of electrons and muons |eta| &lt; 2.5, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The fiducial region for the 8 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, muon $p_T$ &gt; 5 GeV, electron $p_T$ &gt; 7 GeV, psudorapidity of electrons |eta| &lt; 2.5, psudorapidity of muons |eta| &lt; 2.4, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The generator-level lepton momenta are corrected by adding the momenta of generator-level photons within $\Delta \textrm{R} \left(\ell,\gamma\right) &lt; 0.1$
DOI: 10.17182/hepdata.89171.v1/t7
title: "13 TeV p$_T$-leading jet $\eta$ normalized" of "Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV"

description: Data from Fig. 4 lower right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the p$_T$-leading jet $|\eta_{j}|$ with $|\eta_{j}| &lt; 4.7$.
description: CERN-LHC. The measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at 13 TeV an 8 TeV are reported. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb-1 at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes $\textrm{p} \textrm{p} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$, where where $\ell,\ell^{\prime} = e, \mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_T$, and pseudorapidity of the $p_T$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_T$-leading jets and their pseudorapidity separation, are reported. The fiducial region for the 13 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, lepton $p_T$ &gt; 5 GeV, psudorapidity of electrons and muons |eta| &lt; 2.5, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The fiducial region for the 8 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, muon $p_T$ &gt; 5 GeV, electron $p_T$ &gt; 7 GeV, psudorapidity of electrons |eta| &lt; 2.5, psudorapidity of muons |eta| &lt; 2.4, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The generator-level lepton momenta are corrected by adding the momenta of generator-level photons within $\Delta \textrm{R} \left(\ell,\gamma\right) &lt; 0.1$
DOI: 10.17182/hepdata.89171.v1/t8
title: "13 TeV p$_T$-subleading jet $\eta$ normalized" of "Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV"

description: Data from Fig. 5 right panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the p$_T$-subleading jet $|\eta_{j}|$ with $|\eta_{j}| &lt; 4.7$.
description: CERN-LHC. The measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at 13 TeV an 8 TeV are reported. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb-1 at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes $\textrm{p} \textrm{p} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$, where where $\ell,\ell^{\prime} = e, \mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_T$, and pseudorapidity of the $p_T$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_T$-leading jets and their pseudorapidity separation, are reported. The fiducial region for the 13 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, lepton $p_T$ &gt; 5 GeV, psudorapidity of electrons and muons |eta| &lt; 2.5, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The fiducial region for the 8 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, muon $p_T$ &gt; 5 GeV, electron $p_T$ &gt; 7 GeV, psudorapidity of electrons |eta| &lt; 2.5, psudorapidity of muons |eta| &lt; 2.4, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The generator-level lepton momenta are corrected by adding the momenta of generator-level photons within $\Delta \textrm{R} \left(\ell,\gamma\right) &lt; 0.1$
DOI: 10.17182/hepdata.89171.v1/t9
title: "13 TeV $M_{jj}$ normalized" of "Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV"

description: Data from Fig. 6 left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 13$ TeV as a function of the invariant mass of the two p$_T$ leading jets with $|\eta_{j}| &lt; 4.7$.
description: CERN-LHC. The measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at 13 TeV an 8 TeV are reported. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb-1 at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes $\textrm{p} \textrm{p} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$, where where $\ell,\ell^{\prime} = e, \mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_T$, and pseudorapidity of the $p_T$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_T$-leading jets and their pseudorapidity separation, are reported. The fiducial region for the 13 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, lepton $p_T$ &gt; 5 GeV, psudorapidity of electrons and muons |eta| &lt; 2.5, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The fiducial region for the 8 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, muon $p_T$ &gt; 5 GeV, electron $p_T$ &gt; 7 GeV, psudorapidity of electrons |eta| &lt; 2.5, psudorapidity of muons |eta| &lt; 2.4, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The generator-level lepton momenta are corrected by adding the momenta of generator-level photons within $\Delta \textrm{R} \left(\ell,\gamma\right) &lt; 0.1$
DOI: 10.17182/hepdata.89171.v1/t11
title: "8 TeV nJets" of "Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV"

description: Data from Fig. 2 upper left. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| &lt; 4.7$.
description: CERN-LHC. The measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at 13 TeV an 8 TeV are reported. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb-1 at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes $\textrm{p} \textrm{p} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$, where where $\ell,\ell^{\prime} = e, \mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_T$, and pseudorapidity of the $p_T$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_T$-leading jets and their pseudorapidity separation, are reported. The fiducial region for the 13 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, lepton $p_T$ &gt; 5 GeV, psudorapidity of electrons and muons |eta| &lt; 2.5, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The fiducial region for the 8 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, muon $p_T$ &gt; 5 GeV, electron $p_T$ &gt; 7 GeV, psudorapidity of electrons |eta| &lt; 2.5, psudorapidity of muons |eta| &lt; 2.4, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The generator-level lepton momenta are corrected by adding the momenta of generator-level photons within $\Delta \textrm{R} \left(\ell,\gamma\right) &lt; 0.1$
DOI: 10.17182/hepdata.89171.v1/t13
title: "8 TeV Table nJets Central" of "Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV"

description: Data from Fig. 2 lower left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| &lt; 2.4$.
description: CERN-LHC. The measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at 13 TeV an 8 TeV are reported. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb-1 at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes $\textrm{p} \textrm{p} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$, where where $\ell,\ell^{\prime} = e, \mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_T$, and pseudorapidity of the $p_T$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_T$-leading jets and their pseudorapidity separation, are reported. The fiducial region for the 13 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, lepton $p_T$ &gt; 5 GeV, psudorapidity of electrons and muons |eta| &lt; 2.5, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The fiducial region for the 8 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, muon $p_T$ &gt; 5 GeV, electron $p_T$ &gt; 7 GeV, psudorapidity of electrons |eta| &lt; 2.5, psudorapidity of muons |eta| &lt; 2.4, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The generator-level lepton momenta are corrected by adding the momenta of generator-level photons within $\Delta \textrm{R} \left(\ell,\gamma\right) &lt; 0.1$
DOI: 10.17182/hepdata.89171.v1/t14
title: "8 TeV nJets Central normalized" of "Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV"

description: Data from Fig. 3 lower left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the jet multiplicity with $|\eta| &lt; 2.4$.
description: CERN-LHC. The measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at 13 TeV an 8 TeV are reported. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb-1 at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes $\textrm{p} \textrm{p} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$, where where $\ell,\ell^{\prime} = e, \mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_T$, and pseudorapidity of the $p_T$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_T$-leading jets and their pseudorapidity separation, are reported. The fiducial region for the 13 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, lepton $p_T$ &gt; 5 GeV, psudorapidity of electrons and muons |eta| &lt; 2.5, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The fiducial region for the 8 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, muon $p_T$ &gt; 5 GeV, electron $p_T$ &gt; 7 GeV, psudorapidity of electrons |eta| &lt; 2.5, psudorapidity of muons |eta| &lt; 2.4, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The generator-level lepton momenta are corrected by adding the momenta of generator-level photons within $\Delta \textrm{R} \left(\ell,\gamma\right) &lt; 0.1$
DOI: 10.17182/hepdata.89171.v1/t15
title: "8 TeV p$_T$-leading jet p$_T$ normalized" of "Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV"

description: Data from Fig. 4 upper left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the p$_T$-leading jet transverse momentum with $|\eta| &lt; 4.7$.
description: CERN-LHC. The measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at 13 TeV an 8 TeV are reported. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb-1 at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes $\textrm{p} \textrm{p} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$, where where $\ell,\ell^{\prime} = e, \mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_T$, and pseudorapidity of the $p_T$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_T$-leading jets and their pseudorapidity separation, are reported. The fiducial region for the 13 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, lepton $p_T$ &gt; 5 GeV, psudorapidity of electrons and muons |eta| &lt; 2.5, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The fiducial region for the 8 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, muon $p_T$ &gt; 5 GeV, electron $p_T$ &gt; 7 GeV, psudorapidity of electrons |eta| &lt; 2.5, psudorapidity of muons |eta| &lt; 2.4, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The generator-level lepton momenta are corrected by adding the momenta of generator-level photons within $\Delta \textrm{R} \left(\ell,\gamma\right) &lt; 0.1$
DOI: 10.17182/hepdata.89171.v1/t16
title: "8 TeV p$_T$-leading jet $|\eta|$ normalized" of "Measurement of differential cross sections for Z boson pair production in association with jets at $\sqrt{s}=$ 8 and 13 TeV"

description: Data from Fig. 4 lower left panel. The $\textrm{pp} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$ normalized differential cross section at $\sqrt{s} = 8$ TeV as a function of the p$_T$-leading jet transverse $\eta$ with $|\eta| &lt; 4.7$.
description: CERN-LHC. The measurements of differential cross sections for the production of two Z bosons in association with jets in proton-proton collisions at 13 TeV an 8 TeV are reported. The analysis is based on data samples collected at the LHC with the CMS detector, corresponding to integrated luminosities of 19.7 and 35.9 fb-1 at 8 and 13 TeV, respectively. The measurements are performed in the leptonic decay modes $\textrm{p} \textrm{p} \to \textrm{ZZ}\to \ell\ell\ell^{\prime}\ell^{\prime}$, where where $\ell,\ell^{\prime} = e, \mu$. The differential cross sections as a function of the jet multiplicity, the transverse momentum $p_T$, and pseudorapidity of the $p_T$-leading and subleading jets are presented. In addition, the differential cross sections as a function of variables sensitive to the vector boson scattering, such as the invariant mass of the two $p_T$-leading jets and their pseudorapidity separation, are reported. The fiducial region for the 13 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, lepton $p_T$ &gt; 5 GeV, psudorapidity of electrons and muons |eta| &lt; 2.5, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The fiducial region for the 8 TeV analysis is defined as: leading lepton $p_T$ &gt; 20 GeV, subleading lepton $p_T$ &gt; 10 GeV, muon $p_T$ &gt; 5 GeV, electron $p_T$ &gt; 7 GeV, psudorapidity of electrons |eta| &lt; 2.5, psudorapidity of muons |eta| &lt; 2.4, invariant mass of any opposite-sign same-flavor lepton pair $\textrm{m}_{\ell \ell} &gt; 4$ GeV, invariant mass of the Z boson $60 &lt; \textrm{m}_{\textrm{Z1}},\textrm{m}_{\textrm{Z2}} &lt; 120$ GeV. The generator-level lepton momenta are corrected by adding the momenta of generator-level photons within $\Delta \textrm{R} \left(\ell,\gamma\right) &lt; 0.1$