cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.62685.v1/t10
title: "Table 10" of "Measurement of jet shapes in top pair events at sqrt(s) = 7 TeV using the ATLAS detector"

description: Integrated jet shape as a function of the radius r for the PT range 100-150 GeV.
description: CERN-LHC. Measurement of the jet shapes in top-quark pair events from proton-proton collisions at a centre-of-mass energy of 7 TeV. The analysis uses a data sample of integrated luminosity 1.8 fb-1. Jets are reconstructed using the anti-kT algorithm with jet radius R=0.4. Jet shapes are presented as differential and integrated defined as: 
Differential (RHO) - scalar sum of jet PT in an annulus of thickness deltaR around radius r / scalar sum of jet PT in the cone of radius R. 
Integrated (PSI) - scalar sum of jet PT in cone radius r / scalar sum of jet PT in cone radius R. 
Data are shown separated into b-jets and light-jet events. 

UPDATE (22 JUL 2014): Information on the different sources of systematic uncertainty is given in the following four links, containing tables with the relative values of the uncertainty (in %) for both the differential (Diff) and integrated (Int) versions of the jet shapes for both light- (lJets) and b-jets (bJets). The uncertainties indicated with (Up) and (Down) are asymmetric, while the rest are symmetric on each bin.
DOI: 10.17182/hepdata.62685.v1/t6
title: "Table 6" of "Measurement of jet shapes in top pair events at sqrt(s) = 7 TeV using the ATLAS detector"

description: Integrated jet shape as a function of the radius r for the PT range 50-70 GeV.
description: CERN-LHC. Measurement of the jet shapes in top-quark pair events from proton-proton collisions at a centre-of-mass energy of 7 TeV. The analysis uses a data sample of integrated luminosity 1.8 fb-1. Jets are reconstructed using the anti-kT algorithm with jet radius R=0.4. Jet shapes are presented as differential and integrated defined as: 
Differential (RHO) - scalar sum of jet PT in an annulus of thickness deltaR around radius r / scalar sum of jet PT in the cone of radius R. 
Integrated (PSI) - scalar sum of jet PT in cone radius r / scalar sum of jet PT in cone radius R. 
Data are shown separated into b-jets and light-jet events. 

UPDATE (22 JUL 2014): Information on the different sources of systematic uncertainty is given in the following four links, containing tables with the relative values of the uncertainty (in %) for both the differential (Diff) and integrated (Int) versions of the jet shapes for both light- (lJets) and b-jets (bJets). The uncertainties indicated with (Up) and (Down) are asymmetric, while the rest are symmetric on each bin.
DOI: 10.17182/hepdata.62685.v1/t7
title: "Table 7" of "Measurement of jet shapes in top pair events at sqrt(s) = 7 TeV using the ATLAS detector"

description: Differential jet shape as a function of the radius r for the PT range 70-100 GeV.
description: CERN-LHC. Measurement of the jet shapes in top-quark pair events from proton-proton collisions at a centre-of-mass energy of 7 TeV. The analysis uses a data sample of integrated luminosity 1.8 fb-1. Jets are reconstructed using the anti-kT algorithm with jet radius R=0.4. Jet shapes are presented as differential and integrated defined as: 
Differential (RHO) - scalar sum of jet PT in an annulus of thickness deltaR around radius r / scalar sum of jet PT in the cone of radius R. 
Integrated (PSI) - scalar sum of jet PT in cone radius r / scalar sum of jet PT in cone radius R. 
Data are shown separated into b-jets and light-jet events. 

UPDATE (22 JUL 2014): Information on the different sources of systematic uncertainty is given in the following four links, containing tables with the relative values of the uncertainty (in %) for both the differential (Diff) and integrated (Int) versions of the jet shapes for both light- (lJets) and b-jets (bJets). The uncertainties indicated with (Up) and (Down) are asymmetric, while the rest are symmetric on each bin.
DOI: 10.17182/hepdata.62685.v1/t8
title: "Table 8" of "Measurement of jet shapes in top pair events at sqrt(s) = 7 TeV using the ATLAS detector"

description: Integrated jet shape as a function of the radius r for the PT range 70-100 GeV.
description: CERN-LHC. Measurement of the jet shapes in top-quark pair events from proton-proton collisions at a centre-of-mass energy of 7 TeV. The analysis uses a data sample of integrated luminosity 1.8 fb-1. Jets are reconstructed using the anti-kT algorithm with jet radius R=0.4. Jet shapes are presented as differential and integrated defined as: 
Differential (RHO) - scalar sum of jet PT in an annulus of thickness deltaR around radius r / scalar sum of jet PT in the cone of radius R. 
Integrated (PSI) - scalar sum of jet PT in cone radius r / scalar sum of jet PT in cone radius R. 
Data are shown separated into b-jets and light-jet events. 

UPDATE (22 JUL 2014): Information on the different sources of systematic uncertainty is given in the following four links, containing tables with the relative values of the uncertainty (in %) for both the differential (Diff) and integrated (Int) versions of the jet shapes for both light- (lJets) and b-jets (bJets). The uncertainties indicated with (Up) and (Down) are asymmetric, while the rest are symmetric on each bin.
DOI: 10.17182/hepdata.62685.v1/t9
title: "Table 9" of "Measurement of jet shapes in top pair events at sqrt(s) = 7 TeV using the ATLAS detector"

description: Differential jet shape as a function of the radius r for the PT range 100-150 GeV.
description: CERN-LHC. Measurement of the jet shapes in top-quark pair events from proton-proton collisions at a centre-of-mass energy of 7 TeV. The analysis uses a data sample of integrated luminosity 1.8 fb-1. Jets are reconstructed using the anti-kT algorithm with jet radius R=0.4. Jet shapes are presented as differential and integrated defined as: 
Differential (RHO) - scalar sum of jet PT in an annulus of thickness deltaR around radius r / scalar sum of jet PT in the cone of radius R. 
Integrated (PSI) - scalar sum of jet PT in cone radius r / scalar sum of jet PT in cone radius R. 
Data are shown separated into b-jets and light-jet events. 

UPDATE (22 JUL 2014): Information on the different sources of systematic uncertainty is given in the following four links, containing tables with the relative values of the uncertainty (in %) for both the differential (Diff) and integrated (Int) versions of the jet shapes for both light- (lJets) and b-jets (bJets). The uncertainties indicated with (Up) and (Down) are asymmetric, while the rest are symmetric on each bin.
DOI: 10.17182/hepdata.62686.v1/t1
title: "Table 1" of "Measurement of the ZZ production cross section and search for anomalous couplings in 2l2l' final states in pp collisions at sqrt(s)=7 TeV"

description: The measured total ZZ cross section. The (sys) error is the total systematic error, luminosity uncertainty is separated.
description: CERN-LHC. A measurement is presented of the ZZ production cross section in the ZZ -&gt; 2l2l' decay mode with l = e, mu and l' = e, mu, tau in proton-proton collisions at sqrt(s) = 7 TeV with the CMS experiment at the LHC. Results are based on data corresponding to an integrated luminosity of 5.0 fb-1. The measured cross section sigma (pp -&gt; ZZ) = 6.24 +0.86/-0.80 (stat.) +0.41/-0.32 (syst.) +- 0.14 (lumi.) pb is consistent with the standard model predictions. The following limits on ZZZ and ZZgamma anomalous trilinear gauge couplings are set at 95% confidence level: -0.011 &lt; f4Z &lt; 0.012, -0.012 &lt; f5Z &lt; 0.012, -0.013 &lt; f4gamma &lt; 0.015, and -0.014 &lt; f5gamma &lt; 0.014.
DOI: 10.17182/hepdata.62698.v1/t1
title: "Table 1" of "Measurement of Inclusive W and Z Boson Production Cross Sections in pp Collisions at $\sqrt{s}$ = 8 TeV"

description: W+ total and fiducial production cross sections times branching fractions.
description: CERN-LHC. Measurement of total and fiducial inclusive W and Z boson production cross sections in pp collisions at sqrt(s) = 8 TeV. Electron and muon final states are analyzed in a data sample collected in 2012 with the CMS detector corresponding to an integrated luminosity of 18.2 +- 0.5 inverse picobarns. The measured total inclusive cross sections times branching fractions are SIG(P P --&gt; W X) * BR(W --&gt; LEPTON NU) = 12.21 +- 0.03 (stat.) +- 0.24 (syst.) +- 0.32 (lum.) nb and SIG(P P --&gt; Z0 X) * BR(Z0 --&gt; LEPTON+ LEPTON-) = 1.15 +- 0.01 (stat.) +- 0.02 (syst.) +- 0.03 (lum.) nb for the dilepton mass in the range of 60 to 120 GeV. Ratios of cross sections are reported with a precision of 2%.
DOI: 10.17182/hepdata.62698.v1/t2
title: "Table 2" of "Measurement of Inclusive W and Z Boson Production Cross Sections in pp Collisions at $\sqrt{s}$ = 8 TeV"

description: W- total and fiducial production cross sections times branching fractions.
description: CERN-LHC. Measurement of total and fiducial inclusive W and Z boson production cross sections in pp collisions at sqrt(s) = 8 TeV. Electron and muon final states are analyzed in a data sample collected in 2012 with the CMS detector corresponding to an integrated luminosity of 18.2 +- 0.5 inverse picobarns. The measured total inclusive cross sections times branching fractions are SIG(P P --&gt; W X) * BR(W --&gt; LEPTON NU) = 12.21 +- 0.03 (stat.) +- 0.24 (syst.) +- 0.32 (lum.) nb and SIG(P P --&gt; Z0 X) * BR(Z0 --&gt; LEPTON+ LEPTON-) = 1.15 +- 0.01 (stat.) +- 0.02 (syst.) +- 0.03 (lum.) nb for the dilepton mass in the range of 60 to 120 GeV. Ratios of cross sections are reported with a precision of 2%.
DOI: 10.17182/hepdata.62698.v1/t3
title: "Table 3" of "Measurement of Inclusive W and Z Boson Production Cross Sections in pp Collisions at $\sqrt{s}$ = 8 TeV"

description: (W+ + W-) total and fiducial production cross sections times branching fractions.
description: CERN-LHC. Measurement of total and fiducial inclusive W and Z boson production cross sections in pp collisions at sqrt(s) = 8 TeV. Electron and muon final states are analyzed in a data sample collected in 2012 with the CMS detector corresponding to an integrated luminosity of 18.2 +- 0.5 inverse picobarns. The measured total inclusive cross sections times branching fractions are SIG(P P --&gt; W X) * BR(W --&gt; LEPTON NU) = 12.21 +- 0.03 (stat.) +- 0.24 (syst.) +- 0.32 (lum.) nb and SIG(P P --&gt; Z0 X) * BR(Z0 --&gt; LEPTON+ LEPTON-) = 1.15 +- 0.01 (stat.) +- 0.02 (syst.) +- 0.03 (lum.) nb for the dilepton mass in the range of 60 to 120 GeV. Ratios of cross sections are reported with a precision of 2%.
DOI: 10.17182/hepdata.62698.v1/t4
title: "Table 4" of "Measurement of Inclusive W and Z Boson Production Cross Sections in pp Collisions at $\sqrt{s}$ = 8 TeV"

description: Z0 total and fiducial production cross sections times branching fractions.
description: CERN-LHC. Measurement of total and fiducial inclusive W and Z boson production cross sections in pp collisions at sqrt(s) = 8 TeV. Electron and muon final states are analyzed in a data sample collected in 2012 with the CMS detector corresponding to an integrated luminosity of 18.2 +- 0.5 inverse picobarns. The measured total inclusive cross sections times branching fractions are SIG(P P --&gt; W X) * BR(W --&gt; LEPTON NU) = 12.21 +- 0.03 (stat.) +- 0.24 (syst.) +- 0.32 (lum.) nb and SIG(P P --&gt; Z0 X) * BR(Z0 --&gt; LEPTON+ LEPTON-) = 1.15 +- 0.01 (stat.) +- 0.02 (syst.) +- 0.03 (lum.) nb for the dilepton mass in the range of 60 to 120 GeV. Ratios of cross sections are reported with a precision of 2%.
DOI: 10.17182/hepdata.62698.v1/t5
title: "Table 5" of "Measurement of Inclusive W and Z Boson Production Cross Sections in pp Collisions at $\sqrt{s}$ = 8 TeV"

description: W+ to W- ratios of total and fiducial production cross sections times branching fractions.
description: CERN-LHC. Measurement of total and fiducial inclusive W and Z boson production cross sections in pp collisions at sqrt(s) = 8 TeV. Electron and muon final states are analyzed in a data sample collected in 2012 with the CMS detector corresponding to an integrated luminosity of 18.2 +- 0.5 inverse picobarns. The measured total inclusive cross sections times branching fractions are SIG(P P --&gt; W X) * BR(W --&gt; LEPTON NU) = 12.21 +- 0.03 (stat.) +- 0.24 (syst.) +- 0.32 (lum.) nb and SIG(P P --&gt; Z0 X) * BR(Z0 --&gt; LEPTON+ LEPTON-) = 1.15 +- 0.01 (stat.) +- 0.02 (syst.) +- 0.03 (lum.) nb for the dilepton mass in the range of 60 to 120 GeV. Ratios of cross sections are reported with a precision of 2%.
DOI: 10.17182/hepdata.62698.v1/t6
title: "Table 6" of "Measurement of Inclusive W and Z Boson Production Cross Sections in pp Collisions at $\sqrt{s}$ = 8 TeV"

description: (W+ + W-) to Z0 ratios of total and fiducial production cross sections times branching fractions.
description: CERN-LHC. Measurement of total and fiducial inclusive W and Z boson production cross sections in pp collisions at sqrt(s) = 8 TeV. Electron and muon final states are analyzed in a data sample collected in 2012 with the CMS detector corresponding to an integrated luminosity of 18.2 +- 0.5 inverse picobarns. The measured total inclusive cross sections times branching fractions are SIG(P P --&gt; W X) * BR(W --&gt; LEPTON NU) = 12.21 +- 0.03 (stat.) +- 0.24 (syst.) +- 0.32 (lum.) nb and SIG(P P --&gt; Z0 X) * BR(Z0 --&gt; LEPTON+ LEPTON-) = 1.15 +- 0.01 (stat.) +- 0.02 (syst.) +- 0.03 (lum.) nb for the dilepton mass in the range of 60 to 120 GeV. Ratios of cross sections are reported with a precision of 2%.
DOI: 10.17182/hepdata.62699.v1/t1
title: "Table 1" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: The pT distribution of disappearing-track candidates.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t2
title: "Table 2" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Observed CLs contour in the ( M(CHARGINO), TAU(CHARGINO) ) space for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t3
title: "Table 3" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Observed CLs contour with minus 1-sigma signal cross-section uncertainty in the ( M(CHARGINO), TAU(CHARGINO) ) space for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t4
title: "Table 4" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Observed CLs contour with plus 1-sigma signal cross-section uncertainty in the ( M(CHARGINO), TAU(CHARGINO) ) space for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t5
title: "Table 5" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Expected CLs contour in the ( M(CHARGINO), TAU(CHARGINO) ) space for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t6
title: "Table 6" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Expected CLs contour with minus 1-sigma experimental uncertainty in the ( M(CHARGINO), TAU(CHARGINO) ) space for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.
DOI: 10.17182/hepdata.62699.v1/t7
title: "Table 7" of "Search for charginos nearly mass-degenerate with the lightest neutralino based on a disappearing-track signature in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector"

description: Expected CLs contour with plus 1-sigma experimental uncertainty in the ( M(CHARGINO), TAU(CHARGINO) ) space for tan(beta) = 5 and mu &gt; 0.
description: CERN-LHC. A search is presented for direct chargino production based on a disappearing-track signature using 20.3 fb^-1 of proton-proton collisions at sqrt(s) = 8 TeV collected in 2012 with the ATLAS experiment at the LHC. In anomaly-mediated supersymmetry breaking (AMSB) models, the lightest chargino is nearly mass-degenerate with the lightest neutralino and its lifetime is long enough to be detected in the tracking detectors by identifying decays that result in tracks with no associated hits in the outer region of the tracking system. Some models with supersymmetry also predict charginos with a significant lifetime. This analysis attains sensitivity for charginos with a lifetime between 0.1 ns and 10 ns, and significantly surpasses the reach of the LEP experiments. No significant excess above the background expectation is observed for candidate tracks with large transverse momentum, and constraints on chargino properties are obtained. In the AMSB scenarios, a chargino mass below 270 GeV is excluded at 95% confidence level.