cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.114865.v1/t58
title: "Table 58" of "Cross-section measurements for the production of a $Z$ boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Measured fiducial differential cross sections for the $r_{Z,j}$ in the high-p$_{\mathrm{T}}$ region in Z($\to \ell^{+} \ell^{-}$) + high p$_{\mathrm{T}}$ jets events, where the EW Zjj contribution is treated as signal and not subtracted as background. The statistical, systematic, and luminosity uncertainties are given.
description: CERN-LHC. Cross-section measurements for the production of a Z boson decaying to a charged lepton pair in association with at least one high-transverse-momentum jet using the e+e- and mu+mu- decay channels in proton-proton collisions at a centre-of-mass energy of 13 TeV with 139 fb$^{-1}$ of data collected with the ATLAS detector. The cross-section measurements correspond to the Z boson decaying to a single charged lepton pair, or $Z\to\ell^+\ell^-$. The final states used are 2 electrons or 2 muons, and jets with transverse momentum greater than 100 GeV.
The fiducial region is defined as:
- 2 opposite signed leptons with $71 &lt; m_{ll} &lt; 111$ GeV where $m_{ll}$ is the mass of the dilepton system
- ptLepton &gt; 25 GeV
- |etaLepton| &lt; 2.5
- ptJet &gt; 100 GeV
- |yJet| &lt; 2.5
- Overlap Removal: Remove jets within $\Delta R(j,l)$ &lt; 0.2, followed by removal of leptons within $\Delta R(j,l)$ &lt; 0.4 of remaining jets. Jets used in this overlap procedure have p$_{\mathrm{T}}$ greater than 30 GeV instead of the fiducial selection of p$_{\mathrm{T}}$ greater than 100 GeV.
The High-p$_{\mathrm{T}}$ region is defined as having the leading jet p$_{\mathrm{T}}$ greater than 500 GeV.
The Collinear region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &lt; 1.4.
The Back-to-back region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &gt; 2.0.
The High-S$_{\mathrm{T}}$ region is defined as S$_{\mathrm{T}}$ &gt; 600 GeV.
Correction scale factors are given to translate the cross sections from Born-level leptons to dressed-level leptons used in this analysis.
Correction scale factors are also given to translate the cross sections obtained with an overlap removal procedure done only with jets of p$_{\mathrm{T}}$ greater than 100 GeV to the overlap removal used in this analysis.
Non-pertubative corrections are found to be consistent with zero when the leading jet p$_{\mathrm{T}}$ exceeds 100 GeV and are not needed to match the fiducial selection of these measurements.
Differential cross sections and their uncertainties are also given in the case where the EW Zjj processes are treated as signal and not subtracted as background.
DOI: 10.17182/hepdata.114865.v1/t59
title: "Table 59" of "Cross-section measurements for the production of a $Z$ boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Measured fiducial differential cross sections for the $r_{Z,j}$ in the collinear region in Z($\to \ell^{+} \ell^{-}$) + high p$_{\mathrm{T}}$ jets events, where the EW Zjj contribution is treated as signal and not subtracted as background. The statistical, systematic, and luminosity uncertainties are given.
description: CERN-LHC. Cross-section measurements for the production of a Z boson decaying to a charged lepton pair in association with at least one high-transverse-momentum jet using the e+e- and mu+mu- decay channels in proton-proton collisions at a centre-of-mass energy of 13 TeV with 139 fb$^{-1}$ of data collected with the ATLAS detector. The cross-section measurements correspond to the Z boson decaying to a single charged lepton pair, or $Z\to\ell^+\ell^-$. The final states used are 2 electrons or 2 muons, and jets with transverse momentum greater than 100 GeV.
The fiducial region is defined as:
- 2 opposite signed leptons with $71 &lt; m_{ll} &lt; 111$ GeV where $m_{ll}$ is the mass of the dilepton system
- ptLepton &gt; 25 GeV
- |etaLepton| &lt; 2.5
- ptJet &gt; 100 GeV
- |yJet| &lt; 2.5
- Overlap Removal: Remove jets within $\Delta R(j,l)$ &lt; 0.2, followed by removal of leptons within $\Delta R(j,l)$ &lt; 0.4 of remaining jets. Jets used in this overlap procedure have p$_{\mathrm{T}}$ greater than 30 GeV instead of the fiducial selection of p$_{\mathrm{T}}$ greater than 100 GeV.
The High-p$_{\mathrm{T}}$ region is defined as having the leading jet p$_{\mathrm{T}}$ greater than 500 GeV.
The Collinear region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &lt; 1.4.
The Back-to-back region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &gt; 2.0.
The High-S$_{\mathrm{T}}$ region is defined as S$_{\mathrm{T}}$ &gt; 600 GeV.
Correction scale factors are given to translate the cross sections from Born-level leptons to dressed-level leptons used in this analysis.
Correction scale factors are also given to translate the cross sections obtained with an overlap removal procedure done only with jets of p$_{\mathrm{T}}$ greater than 100 GeV to the overlap removal used in this analysis.
Non-pertubative corrections are found to be consistent with zero when the leading jet p$_{\mathrm{T}}$ exceeds 100 GeV and are not needed to match the fiducial selection of these measurements.
Differential cross sections and their uncertainties are also given in the case where the EW Zjj processes are treated as signal and not subtracted as background.
DOI: 10.17182/hepdata.114865.v1/t60
title: "Table 60" of "Cross-section measurements for the production of a $Z$ boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Measured fiducial differential cross sections for the $r_{Z,j}$ in the back-to-back region in Z($\to \ell^{+} \ell^{-}$) + high p$_{\mathrm{T}}$ jets events, where the EW Zjj contribution is treated as signal and not subtracted as background. The statistical, systematic, and luminosity uncertainties are given.
description: CERN-LHC. Cross-section measurements for the production of a Z boson decaying to a charged lepton pair in association with at least one high-transverse-momentum jet using the e+e- and mu+mu- decay channels in proton-proton collisions at a centre-of-mass energy of 13 TeV with 139 fb$^{-1}$ of data collected with the ATLAS detector. The cross-section measurements correspond to the Z boson decaying to a single charged lepton pair, or $Z\to\ell^+\ell^-$. The final states used are 2 electrons or 2 muons, and jets with transverse momentum greater than 100 GeV.
The fiducial region is defined as:
- 2 opposite signed leptons with $71 &lt; m_{ll} &lt; 111$ GeV where $m_{ll}$ is the mass of the dilepton system
- ptLepton &gt; 25 GeV
- |etaLepton| &lt; 2.5
- ptJet &gt; 100 GeV
- |yJet| &lt; 2.5
- Overlap Removal: Remove jets within $\Delta R(j,l)$ &lt; 0.2, followed by removal of leptons within $\Delta R(j,l)$ &lt; 0.4 of remaining jets. Jets used in this overlap procedure have p$_{\mathrm{T}}$ greater than 30 GeV instead of the fiducial selection of p$_{\mathrm{T}}$ greater than 100 GeV.
The High-p$_{\mathrm{T}}$ region is defined as having the leading jet p$_{\mathrm{T}}$ greater than 500 GeV.
The Collinear region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &lt; 1.4.
The Back-to-back region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &gt; 2.0.
The High-S$_{\mathrm{T}}$ region is defined as S$_{\mathrm{T}}$ &gt; 600 GeV.
Correction scale factors are given to translate the cross sections from Born-level leptons to dressed-level leptons used in this analysis.
Correction scale factors are also given to translate the cross sections obtained with an overlap removal procedure done only with jets of p$_{\mathrm{T}}$ greater than 100 GeV to the overlap removal used in this analysis.
Non-pertubative corrections are found to be consistent with zero when the leading jet p$_{\mathrm{T}}$ exceeds 100 GeV and are not needed to match the fiducial selection of these measurements.
Differential cross sections and their uncertainties are also given in the case where the EW Zjj processes are treated as signal and not subtracted as background.
DOI: 10.17182/hepdata.114865.v1/t61
title: "Table 61" of "Cross-section measurements for the production of a $Z$ boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Measured fiducial differential cross sections for the jet multiplicity in the collinear region in Z($\to \ell^{+} \ell^{-}$) + high p$_{\mathrm{T}}$ jets events, where the EW Zjj contribution is treated as signal and not subtracted as background. The statistical, systematic, and luminosity uncertainties are given.
description: CERN-LHC. Cross-section measurements for the production of a Z boson decaying to a charged lepton pair in association with at least one high-transverse-momentum jet using the e+e- and mu+mu- decay channels in proton-proton collisions at a centre-of-mass energy of 13 TeV with 139 fb$^{-1}$ of data collected with the ATLAS detector. The cross-section measurements correspond to the Z boson decaying to a single charged lepton pair, or $Z\to\ell^+\ell^-$. The final states used are 2 electrons or 2 muons, and jets with transverse momentum greater than 100 GeV.
The fiducial region is defined as:
- 2 opposite signed leptons with $71 &lt; m_{ll} &lt; 111$ GeV where $m_{ll}$ is the mass of the dilepton system
- ptLepton &gt; 25 GeV
- |etaLepton| &lt; 2.5
- ptJet &gt; 100 GeV
- |yJet| &lt; 2.5
- Overlap Removal: Remove jets within $\Delta R(j,l)$ &lt; 0.2, followed by removal of leptons within $\Delta R(j,l)$ &lt; 0.4 of remaining jets. Jets used in this overlap procedure have p$_{\mathrm{T}}$ greater than 30 GeV instead of the fiducial selection of p$_{\mathrm{T}}$ greater than 100 GeV.
The High-p$_{\mathrm{T}}$ region is defined as having the leading jet p$_{\mathrm{T}}$ greater than 500 GeV.
The Collinear region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &lt; 1.4.
The Back-to-back region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &gt; 2.0.
The High-S$_{\mathrm{T}}$ region is defined as S$_{\mathrm{T}}$ &gt; 600 GeV.
Correction scale factors are given to translate the cross sections from Born-level leptons to dressed-level leptons used in this analysis.
Correction scale factors are also given to translate the cross sections obtained with an overlap removal procedure done only with jets of p$_{\mathrm{T}}$ greater than 100 GeV to the overlap removal used in this analysis.
Non-pertubative corrections are found to be consistent with zero when the leading jet p$_{\mathrm{T}}$ exceeds 100 GeV and are not needed to match the fiducial selection of these measurements.
Differential cross sections and their uncertainties are also given in the case where the EW Zjj processes are treated as signal and not subtracted as background.
DOI: 10.17182/hepdata.114865.v1/t63
title: "Table 63" of "Cross-section measurements for the production of a $Z$ boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Measured fiducial differential cross sections for the H$_{\mathrm{T}}$ in Z($\to \ell^{+} \ell^{-}$) + high p$_{\mathrm{T}}$ jets events, where the EW Zjj contribution is treated as signal and not subtracted as background. The statistical, systematic, and luminosity uncertainties are given.
description: CERN-LHC. Cross-section measurements for the production of a Z boson decaying to a charged lepton pair in association with at least one high-transverse-momentum jet using the e+e- and mu+mu- decay channels in proton-proton collisions at a centre-of-mass energy of 13 TeV with 139 fb$^{-1}$ of data collected with the ATLAS detector. The cross-section measurements correspond to the Z boson decaying to a single charged lepton pair, or $Z\to\ell^+\ell^-$. The final states used are 2 electrons or 2 muons, and jets with transverse momentum greater than 100 GeV.
The fiducial region is defined as:
- 2 opposite signed leptons with $71 &lt; m_{ll} &lt; 111$ GeV where $m_{ll}$ is the mass of the dilepton system
- ptLepton &gt; 25 GeV
- |etaLepton| &lt; 2.5
- ptJet &gt; 100 GeV
- |yJet| &lt; 2.5
- Overlap Removal: Remove jets within $\Delta R(j,l)$ &lt; 0.2, followed by removal of leptons within $\Delta R(j,l)$ &lt; 0.4 of remaining jets. Jets used in this overlap procedure have p$_{\mathrm{T}}$ greater than 30 GeV instead of the fiducial selection of p$_{\mathrm{T}}$ greater than 100 GeV.
The High-p$_{\mathrm{T}}$ region is defined as having the leading jet p$_{\mathrm{T}}$ greater than 500 GeV.
The Collinear region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &lt; 1.4.
The Back-to-back region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &gt; 2.0.
The High-S$_{\mathrm{T}}$ region is defined as S$_{\mathrm{T}}$ &gt; 600 GeV.
Correction scale factors are given to translate the cross sections from Born-level leptons to dressed-level leptons used in this analysis.
Correction scale factors are also given to translate the cross sections obtained with an overlap removal procedure done only with jets of p$_{\mathrm{T}}$ greater than 100 GeV to the overlap removal used in this analysis.
Non-pertubative corrections are found to be consistent with zero when the leading jet p$_{\mathrm{T}}$ exceeds 100 GeV and are not needed to match the fiducial selection of these measurements.
Differential cross sections and their uncertainties are also given in the case where the EW Zjj processes are treated as signal and not subtracted as background.
DOI: 10.17182/hepdata.114865.v1/t64
title: "Table 64" of "Cross-section measurements for the production of a $Z$ boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Measured fiducial differential cross sections for the $\Delta R_{Z,j}^{min}$ in the high-S$_{\mathrm{T}}$ region in Z($\to \ell^{+} \ell^{-}$) + high p$_{\mathrm{T}}$ jets events, where the EW Zjj contribution is treated as signal and not subtracted as background. The statistical, systematic, and luminosity uncertainties are given.
description: CERN-LHC. Cross-section measurements for the production of a Z boson decaying to a charged lepton pair in association with at least one high-transverse-momentum jet using the e+e- and mu+mu- decay channels in proton-proton collisions at a centre-of-mass energy of 13 TeV with 139 fb$^{-1}$ of data collected with the ATLAS detector. The cross-section measurements correspond to the Z boson decaying to a single charged lepton pair, or $Z\to\ell^+\ell^-$. The final states used are 2 electrons or 2 muons, and jets with transverse momentum greater than 100 GeV.
The fiducial region is defined as:
- 2 opposite signed leptons with $71 &lt; m_{ll} &lt; 111$ GeV where $m_{ll}$ is the mass of the dilepton system
- ptLepton &gt; 25 GeV
- |etaLepton| &lt; 2.5
- ptJet &gt; 100 GeV
- |yJet| &lt; 2.5
- Overlap Removal: Remove jets within $\Delta R(j,l)$ &lt; 0.2, followed by removal of leptons within $\Delta R(j,l)$ &lt; 0.4 of remaining jets. Jets used in this overlap procedure have p$_{\mathrm{T}}$ greater than 30 GeV instead of the fiducial selection of p$_{\mathrm{T}}$ greater than 100 GeV.
The High-p$_{\mathrm{T}}$ region is defined as having the leading jet p$_{\mathrm{T}}$ greater than 500 GeV.
The Collinear region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &lt; 1.4.
The Back-to-back region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &gt; 2.0.
The High-S$_{\mathrm{T}}$ region is defined as S$_{\mathrm{T}}$ &gt; 600 GeV.
Correction scale factors are given to translate the cross sections from Born-level leptons to dressed-level leptons used in this analysis.
Correction scale factors are also given to translate the cross sections obtained with an overlap removal procedure done only with jets of p$_{\mathrm{T}}$ greater than 100 GeV to the overlap removal used in this analysis.
Non-pertubative corrections are found to be consistent with zero when the leading jet p$_{\mathrm{T}}$ exceeds 100 GeV and are not needed to match the fiducial selection of these measurements.
Differential cross sections and their uncertainties are also given in the case where the EW Zjj processes are treated as signal and not subtracted as background.
DOI: 10.25549/vercoutere-ouc110610461
title: 2 nude women and 2 black cats plus word salad

description: Two orange nude females with brown hair (one standing with one arm raised to her head and the other hand on her hips; one sitting on the ground reading a book with one hand in her lap); two black cats at their feet; one green plant; area under the figures is turquoise and green; remainder ot the page is a word salad printed in turquoise on an unpainted background. See description of 347 for OT notes.
DOI: 10.17182/hepdata.114865.v1/t62
title: "Table 62" of "Cross-section measurements for the production of a $Z$ boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Measured fiducial differential cross sections for the jet multiplicity in the back-to-back region in Z($\to \ell^{+} \ell^{-}$) + high p$_{\mathrm{T}}$ jets events, where the EW Zjj contribution is treated as signal and not subtracted as background. The statistical, systematic, and luminosity uncertainties are given.
description: CERN-LHC. Cross-section measurements for the production of a Z boson decaying to a charged lepton pair in association with at least one high-transverse-momentum jet using the e+e- and mu+mu- decay channels in proton-proton collisions at a centre-of-mass energy of 13 TeV with 139 fb$^{-1}$ of data collected with the ATLAS detector. The cross-section measurements correspond to the Z boson decaying to a single charged lepton pair, or $Z\to\ell^+\ell^-$. The final states used are 2 electrons or 2 muons, and jets with transverse momentum greater than 100 GeV.
The fiducial region is defined as:
- 2 opposite signed leptons with $71 &lt; m_{ll} &lt; 111$ GeV where $m_{ll}$ is the mass of the dilepton system
- ptLepton &gt; 25 GeV
- |etaLepton| &lt; 2.5
- ptJet &gt; 100 GeV
- |yJet| &lt; 2.5
- Overlap Removal: Remove jets within $\Delta R(j,l)$ &lt; 0.2, followed by removal of leptons within $\Delta R(j,l)$ &lt; 0.4 of remaining jets. Jets used in this overlap procedure have p$_{\mathrm{T}}$ greater than 30 GeV instead of the fiducial selection of p$_{\mathrm{T}}$ greater than 100 GeV.
The High-p$_{\mathrm{T}}$ region is defined as having the leading jet p$_{\mathrm{T}}$ greater than 500 GeV.
The Collinear region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &lt; 1.4.
The Back-to-back region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &gt; 2.0.
The High-S$_{\mathrm{T}}$ region is defined as S$_{\mathrm{T}}$ &gt; 600 GeV.
Correction scale factors are given to translate the cross sections from Born-level leptons to dressed-level leptons used in this analysis.
Correction scale factors are also given to translate the cross sections obtained with an overlap removal procedure done only with jets of p$_{\mathrm{T}}$ greater than 100 GeV to the overlap removal used in this analysis.
Non-pertubative corrections are found to be consistent with zero when the leading jet p$_{\mathrm{T}}$ exceeds 100 GeV and are not needed to match the fiducial selection of these measurements.
Differential cross sections and their uncertainties are also given in the case where the EW Zjj processes are treated as signal and not subtracted as background.
DOI: 10.17182/hepdata.114865.v1/t65
title: "Table 65" of "Cross-section measurements for the production of a $Z$ boson in association with high-transverse-momentum jets in $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Measured fiducial differential cross sections for the jet multiplicity in the high-S$_{\mathrm{T}}$ region in Z($\to \ell^{+} \ell^{-}$) + high p$_{\mathrm{T}}$ jets events, where the EW Zjj contribution is treated as signal and not subtracted as background. The statistical, systematic, and luminosity uncertainties are given.
description: CERN-LHC. Cross-section measurements for the production of a Z boson decaying to a charged lepton pair in association with at least one high-transverse-momentum jet using the e+e- and mu+mu- decay channels in proton-proton collisions at a centre-of-mass energy of 13 TeV with 139 fb$^{-1}$ of data collected with the ATLAS detector. The cross-section measurements correspond to the Z boson decaying to a single charged lepton pair, or $Z\to\ell^+\ell^-$. The final states used are 2 electrons or 2 muons, and jets with transverse momentum greater than 100 GeV.
The fiducial region is defined as:
- 2 opposite signed leptons with $71 &lt; m_{ll} &lt; 111$ GeV where $m_{ll}$ is the mass of the dilepton system
- ptLepton &gt; 25 GeV
- |etaLepton| &lt; 2.5
- ptJet &gt; 100 GeV
- |yJet| &lt; 2.5
- Overlap Removal: Remove jets within $\Delta R(j,l)$ &lt; 0.2, followed by removal of leptons within $\Delta R(j,l)$ &lt; 0.4 of remaining jets. Jets used in this overlap procedure have p$_{\mathrm{T}}$ greater than 30 GeV instead of the fiducial selection of p$_{\mathrm{T}}$ greater than 100 GeV.
The High-p$_{\mathrm{T}}$ region is defined as having the leading jet p$_{\mathrm{T}}$ greater than 500 GeV.
The Collinear region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &lt; 1.4.
The Back-to-back region is defined as a subset of the High-p$_{\mathrm{T}}$ region, where the minimum $\Delta R(Z,j)$ &gt; 2.0.
The High-S$_{\mathrm{T}}$ region is defined as S$_{\mathrm{T}}$ &gt; 600 GeV.
Correction scale factors are given to translate the cross sections from Born-level leptons to dressed-level leptons used in this analysis.
Correction scale factors are also given to translate the cross sections obtained with an overlap removal procedure done only with jets of p$_{\mathrm{T}}$ greater than 100 GeV to the overlap removal used in this analysis.
Non-pertubative corrections are found to be consistent with zero when the leading jet p$_{\mathrm{T}}$ exceeds 100 GeV and are not needed to match the fiducial selection of these measurements.
Differential cross sections and their uncertainties are also given in the case where the EW Zjj processes are treated as signal and not subtracted as background.