cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.57742.v1/t3
title: "Table 3" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Distribution of the effective mass for data and the SM expectation in the one-lepton plus 2 jet channel.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t4
title: "Table 4" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Distribution of the missing ET for data and the SM expectation in the one-lepton plus 2 jet channel.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t5
title: "Table 5" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Observed 95 PCT exclusion limit in the M(gluino), M(sbottom) plane obtained with the zero-lepton channel data.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t6
title: "Table 6" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Expected 95 PCT exclusion limit in the M(gluino), M(sbottom) plane obtained with the zero-lepton channel data.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t10
title: "Table 10" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Expected 95 PCT CL exclusion limits from the zero-lepton analysis on the MSUGRA/CMSSM scenario with tan(beta) = 40, A0 = 0 and MU &gt; 0.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t11
title: "Table 11" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Observed 95 PCT CL exclusion limits from the one-lepton analysis on the MSUGRA/CMSSM scenario with tan(beta) = 40, A0 = 0 and MU &gt; 0.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t7
title: "Table 7" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Observed and expected 95 PCT CL upper limits on the gluino-mediated and stop pair production cross section as a function of the gluino mass for a stop mass od 180 GeV, for the one-lepton analysis.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t8
title: "Table 8" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Observed and expected 95 PCT CL upper limits on the gluino-mediated and stop pair production cross section as a function of the gluino mass for a stop mass od 210 GeV, for the one-lepton analysis.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t9
title: "Table 9" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Observed 95 PCT CL exclusion limits from the zero-lepton analysis on the MSUGRA/CMSSM scenario with tan(beta) = 40, A0 = 0 and MU &gt; 0.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t12
title: "Table 12" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Expected 95 PCT CL exclusion limits from the one-lepton analysis on the MSUGRA/CMSSM scenario with tan(beta) = 40, A0 = 0 and MU &gt; 0.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t13
title: "Table 13" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Observed 95 PCT CL exclusion limits from the combined zero and one-lepton analyses on the MSUGRA/CMSSM scenario with tan(beta) = 40, A0 = 0 and MU &gt; 0.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57742.v1/t14
title: "Table 14" of "Search for supersymmetry in pp collisions at sqrt{s} = 7TeV in final states with missing transverse momentum and b-jets"

description: Expected 95 PCT CL exclusion limits from the combined zero and one-lepton analyses on the MSUGRA/CMSSM scenario with tan(beta) = 40, A0 = 0 and MU &gt; 0.
description: CERN-LHC. A search for SUSY particles in 7 TeV proton-proton collisions in events with large missing transverse momentum and at least one heavy flavour jet. The data, with a total integrated luminosity of 35 pb-1, are analysed in the zero-lepton plus 3 jets and one-lepton plus 2 jet channels with at least one of the jets being a heavy flavour candidate. Jets are defined with the anti-Kt algorithm with R=0.4. In the zero-lepton data the effective mass (M(C=EFFECTIVE)) is defined as the scalar sum of the missing transverse energy and the transverse momenta of the highest PT jets. In the one-lepton data the transverse mas (MT) is constructed from the highest PT lepton and the missing ET.
DOI: 10.17182/hepdata.57743.v1/t1
title: "Table 1" of "Properties of jets measured from tracks in proton-proton collisions at center-of-mass energy sqrt(s) = 7 TeV with the ATLAS detector"

description: Double differential cross sections for charged particle jets as a function of the jet PT in the |rapidity| range 0.0-0.5, shown separately for the two R values. The first (sys) errors is the correlated efficiency uncertainty and the second (sys) error is the correlated vetex splitting uncertainty. The third (sys) error is the quadratic sum of all the uncorrelated systematic uncertainties.
description: CERN-LHC. Measurement of the properties of charged particle jets produced in proton-proton collisions at a centre-of-mass energy of 7 TeV using a minimum-bias trigger. The data were taken during 2010 and have an integrated luminosity of 779 mub^{-1}. Jets are reconstructed using the anti-kT algorithm with radius parameters 0.4 and 0.6 applied to charged particles with PT &gt; 300 MeV. The measured track-based jets are corrected back to truth-level charged particle jets, which are defined to be the jets obtained when the same algoerithm is applied to all primary charged particles with the same PT cut. Measurements of the PT cross sections, multiplicities per jet, fragmentation Z distributions, transverse momentum and charged particle radial densities relative to the jet axes are presented in slices of rapidity and transverse momentum. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-4 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details.
DOI: 10.17182/hepdata.57743.v1/t2
title: "Table 2" of "Properties of jets measured from tracks in proton-proton collisions at center-of-mass energy sqrt(s) = 7 TeV with the ATLAS detector"

description: Double differential cross sections for charged particle jets as a function of the jet PT in the |rapidity| range 0.5-1.0, shown separately for the two R values. The first (sys) errors is the correlated efficiency uncertainty and the second (sys) error is the correlated vetex splitting uncertainty. The third (sys) error is the quadratic sum of all the uncorrelated systematic uncertainties.
description: CERN-LHC. Measurement of the properties of charged particle jets produced in proton-proton collisions at a centre-of-mass energy of 7 TeV using a minimum-bias trigger. The data were taken during 2010 and have an integrated luminosity of 779 mub^{-1}. Jets are reconstructed using the anti-kT algorithm with radius parameters 0.4 and 0.6 applied to charged particles with PT &gt; 300 MeV. The measured track-based jets are corrected back to truth-level charged particle jets, which are defined to be the jets obtained when the same algoerithm is applied to all primary charged particles with the same PT cut. Measurements of the PT cross sections, multiplicities per jet, fragmentation Z distributions, transverse momentum and charged particle radial densities relative to the jet axes are presented in slices of rapidity and transverse momentum. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-4 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details.
DOI: 10.17182/hepdata.57743.v1/t3
title: "Table 3" of "Properties of jets measured from tracks in proton-proton collisions at center-of-mass energy sqrt(s) = 7 TeV with the ATLAS detector"

description: Double differential cross sections for charged particle jets as a function of the jet PT in the |rapidity| range 1.0-1.5, shown separately for the two R values. The first (sys) errors is the correlated efficiency uncertainty and the second (sys) error is the correlated vetex splitting uncertainty. The third (sys) error is the quadratic sum of all the uncorrelated systematic uncertainties.
description: CERN-LHC. Measurement of the properties of charged particle jets produced in proton-proton collisions at a centre-of-mass energy of 7 TeV using a minimum-bias trigger. The data were taken during 2010 and have an integrated luminosity of 779 mub^{-1}. Jets are reconstructed using the anti-kT algorithm with radius parameters 0.4 and 0.6 applied to charged particles with PT &gt; 300 MeV. The measured track-based jets are corrected back to truth-level charged particle jets, which are defined to be the jets obtained when the same algoerithm is applied to all primary charged particles with the same PT cut. Measurements of the PT cross sections, multiplicities per jet, fragmentation Z distributions, transverse momentum and charged particle radial densities relative to the jet axes are presented in slices of rapidity and transverse momentum. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-4 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details.
DOI: 10.17182/hepdata.57743.v1/t4
title: "Table 4" of "Properties of jets measured from tracks in proton-proton collisions at center-of-mass energy sqrt(s) = 7 TeV with the ATLAS detector"

description: Double differential cross sections for charged particle jets as a function of the jet PT in the |rapidity| range 1.5-1.9, shown separately for the two R values. The first (sys) errors is the correlated efficiency uncertainty and the second (sys) error is the correlated vetex splitting uncertainty. The third (sys) error is the quadratic sum of all the uncorrelated systematic uncertainties.
description: CERN-LHC. Measurement of the properties of charged particle jets produced in proton-proton collisions at a centre-of-mass energy of 7 TeV using a minimum-bias trigger. The data were taken during 2010 and have an integrated luminosity of 779 mub^{-1}. Jets are reconstructed using the anti-kT algorithm with radius parameters 0.4 and 0.6 applied to charged particles with PT &gt; 300 MeV. The measured track-based jets are corrected back to truth-level charged particle jets, which are defined to be the jets obtained when the same algoerithm is applied to all primary charged particles with the same PT cut. Measurements of the PT cross sections, multiplicities per jet, fragmentation Z distributions, transverse momentum and charged particle radial densities relative to the jet axes are presented in slices of rapidity and transverse momentum. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-4 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details.
DOI: 10.17182/hepdata.57743.v1/t5
title: "Table 5" of "Properties of jets measured from tracks in proton-proton collisions at center-of-mass energy sqrt(s) = 7 TeV with the ATLAS detector"

description: Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 4-6 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.
description: CERN-LHC. Measurement of the properties of charged particle jets produced in proton-proton collisions at a centre-of-mass energy of 7 TeV using a minimum-bias trigger. The data were taken during 2010 and have an integrated luminosity of 779 mub^{-1}. Jets are reconstructed using the anti-kT algorithm with radius parameters 0.4 and 0.6 applied to charged particles with PT &gt; 300 MeV. The measured track-based jets are corrected back to truth-level charged particle jets, which are defined to be the jets obtained when the same algoerithm is applied to all primary charged particles with the same PT cut. Measurements of the PT cross sections, multiplicities per jet, fragmentation Z distributions, transverse momentum and charged particle radial densities relative to the jet axes are presented in slices of rapidity and transverse momentum. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-4 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details.
DOI: 10.17182/hepdata.57743.v1/t6
title: "Table 6" of "Properties of jets measured from tracks in proton-proton collisions at center-of-mass energy sqrt(s) = 7 TeV with the ATLAS detector"

description: Multiplicity of charged particles per jet in the |rapidity| range 0.0-1.9 and transverse momentum 6-10 GeV shown separately for the two different jet radius parameter (R) values of 0.4 and 0.6.
description: CERN-LHC. Measurement of the properties of charged particle jets produced in proton-proton collisions at a centre-of-mass energy of 7 TeV using a minimum-bias trigger. The data were taken during 2010 and have an integrated luminosity of 779 mub^{-1}. Jets are reconstructed using the anti-kT algorithm with radius parameters 0.4 and 0.6 applied to charged particles with PT &gt; 300 MeV. The measured track-based jets are corrected back to truth-level charged particle jets, which are defined to be the jets obtained when the same algoerithm is applied to all primary charged particles with the same PT cut. Measurements of the PT cross sections, multiplicities per jet, fragmentation Z distributions, transverse momentum and charged particle radial densities relative to the jet axes are presented in slices of rapidity and transverse momentum. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-4 below should be multiplied by a factor of 1.0187 to take into account the updated value of the integrated luminosity for the ATLAS 2010 data taking period. The uncertainty on the global normalisation ("Lumi") increases slightly from 3.4% to 3.5%. See Eur.Phys.J. C73 (2013) 2518 for more details.