cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.58651.v1/t10
title: "Table 10" of "Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV"

description: Double differential cross section for UPSI(2S) production times the dimuon branching fraction as a function of PT for the rapidity region 3.5-4.0. The second systematic (sys) error is due to the unknown polarisation of the UPSI(2S).
description: CERN-LHC. Measurement of the production cross sections for Upsilon(1S), Upsilon(2s) and Upsilon(3) mesons, times their branching fractions to dimuons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample, with total integrated luminosity of 25 pb-1, covers the upsilon transverse momentum range up to 15 GeV/c and the rapidity range 2.0-4.5. Integrated and differential cross sections are tabulated together with cross section ratios as a function of PT.
DOI: 10.17182/hepdata.58651.v1/t11
title: "Table 11" of "Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV"

description: Double differential cross section for UPSI(2S) production times the dimuon branching fraction as a function of PT for the rapidity region 4.0-4.5. The second systematic (sys) error is due to the unknown polarisation of the UPSI(2S).
description: CERN-LHC. Measurement of the production cross sections for Upsilon(1S), Upsilon(2s) and Upsilon(3) mesons, times their branching fractions to dimuons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample, with total integrated luminosity of 25 pb-1, covers the upsilon transverse momentum range up to 15 GeV/c and the rapidity range 2.0-4.5. Integrated and differential cross sections are tabulated together with cross section ratios as a function of PT.
DOI: 10.17182/hepdata.58651.v1/t12
title: "Table 12" of "Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV"

description: Double differential cross section for UPSI(3S) production times the dimuon branching fraction as a function of PT for the rapidity region 2.0-2.5. The second systematic (sys) error is due to the unknown polarisation of the UPSI(3S).
description: CERN-LHC. Measurement of the production cross sections for Upsilon(1S), Upsilon(2s) and Upsilon(3) mesons, times their branching fractions to dimuons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample, with total integrated luminosity of 25 pb-1, covers the upsilon transverse momentum range up to 15 GeV/c and the rapidity range 2.0-4.5. Integrated and differential cross sections are tabulated together with cross section ratios as a function of PT.
DOI: 10.17182/hepdata.58651.v1/t13
title: "Table 13" of "Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV"

description: Double differential cross section for UPSI(3S) production times the dimuon branching fraction as a function of PT for the rapidity region 2.5-3.0. The second systematic (sys) error is due to the unknown polarisation of the UPSI(3S).
description: CERN-LHC. Measurement of the production cross sections for Upsilon(1S), Upsilon(2s) and Upsilon(3) mesons, times their branching fractions to dimuons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample, with total integrated luminosity of 25 pb-1, covers the upsilon transverse momentum range up to 15 GeV/c and the rapidity range 2.0-4.5. Integrated and differential cross sections are tabulated together with cross section ratios as a function of PT.
DOI: 10.17182/hepdata.58651.v1/t8
title: "Table 8" of "Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV"

description: Double differential cross section for UPSI(2S) production times the dimuon branching fraction as a function of PT for the rapidity region 2.5-3.0. The second systematic (sys) error is due to the unknown polarisation of the UPSI(2S).
description: CERN-LHC. Measurement of the production cross sections for Upsilon(1S), Upsilon(2s) and Upsilon(3) mesons, times their branching fractions to dimuons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample, with total integrated luminosity of 25 pb-1, covers the upsilon transverse momentum range up to 15 GeV/c and the rapidity range 2.0-4.5. Integrated and differential cross sections are tabulated together with cross section ratios as a function of PT.
DOI: 10.17182/hepdata.58651.v1/t9
title: "Table 9" of "Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV"

description: Double differential cross section for UPSI(2S) production times the dimuon branching fraction as a function of PT for the rapidity region 3.0-3.5. The second systematic (sys) error is due to the unknown polarisation of the UPSI(2S).
description: CERN-LHC. Measurement of the production cross sections for Upsilon(1S), Upsilon(2s) and Upsilon(3) mesons, times their branching fractions to dimuons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample, with total integrated luminosity of 25 pb-1, covers the upsilon transverse momentum range up to 15 GeV/c and the rapidity range 2.0-4.5. Integrated and differential cross sections are tabulated together with cross section ratios as a function of PT.
DOI: 10.17182/hepdata.58651.v1/t14
title: "Table 14" of "Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV"

description: Double differential cross section for UPSI(3S) production times the dimuon branching fraction as a function of PT for the rapidity region 3.0-3.5. The second systematic (sys) error is due to the unknown polarisation of the UPSI(3S).
description: CERN-LHC. Measurement of the production cross sections for Upsilon(1S), Upsilon(2s) and Upsilon(3) mesons, times their branching fractions to dimuons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample, with total integrated luminosity of 25 pb-1, covers the upsilon transverse momentum range up to 15 GeV/c and the rapidity range 2.0-4.5. Integrated and differential cross sections are tabulated together with cross section ratios as a function of PT.
DOI: 10.17182/hepdata.58651.v1/t15
title: "Table 15" of "Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV"

description: Double differential cross section for UPSI(3S) production times the dimuon branching fraction as a function of PT for the rapidity region 3.5-4.0. The second systematic (sys) error is due to the unknown polarisation of the UPSI(3S).
description: CERN-LHC. Measurement of the production cross sections for Upsilon(1S), Upsilon(2s) and Upsilon(3) mesons, times their branching fractions to dimuons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample, with total integrated luminosity of 25 pb-1, covers the upsilon transverse momentum range up to 15 GeV/c and the rapidity range 2.0-4.5. Integrated and differential cross sections are tabulated together with cross section ratios as a function of PT.
DOI: 10.17182/hepdata.58651.v1/t16
title: "Table 16" of "Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV"

description: Double differential cross section for UPSI(3S) production times the dimuon branching fraction as a function of PT for the rapidity region 4.0-4.5. The second systematic (sys) error is due to the unknown polarisation of the UPSI(3S).
description: CERN-LHC. Measurement of the production cross sections for Upsilon(1S), Upsilon(2s) and Upsilon(3) mesons, times their branching fractions to dimuons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample, with total integrated luminosity of 25 pb-1, covers the upsilon transverse momentum range up to 15 GeV/c and the rapidity range 2.0-4.5. Integrated and differential cross sections are tabulated together with cross section ratios as a function of PT.
DOI: 10.17182/hepdata.58651.v1/t17
title: "Table 17" of "Measurement of Upsilon production in pp collisions at {\surd}s = 7 TeV"

description: Ratios of cross section with respect to the UPSI(1S) cross section as a function of PT in the rapidity range 2.0-4.4. The second systematic (sys) error is due to the unknown polarisation of the three states.
description: CERN-LHC. Measurement of the production cross sections for Upsilon(1S), Upsilon(2s) and Upsilon(3) mesons, times their branching fractions to dimuons, in proton-proton collisions at a centre-of-mass energy of 7 TeV. The data sample, with total integrated luminosity of 25 pb-1, covers the upsilon transverse momentum range up to 15 GeV/c and the rapidity range 2.0-4.5. Integrated and differential cross sections are tabulated together with cross section ratios as a function of PT.
DOI: 10.17182/hepdata.58652.v1/t1
title: "Table 1" of "Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector"

description: The measured cross section as a function of the photon transverse energy, ET, for pT(jet)&gt;20 GeV, |eta(gamma)|&lt;1.37, |y(jet)|&lt;1.2, eta(gamma)*y(jet)&gt;=0.
description: CERN-LHC. A measurement of the cross section for the production of an isolated photon in association with jets in proton-proton collisions at a center-of-mass energy sqrt(s) = 7 TeV is presented. Photons are reconstructed in the pseudorapidity range |eta(gamma)| &lt; 1.37 and with a transverse energy E_T(gamma) &gt; 25 GeV. Jets are reconstructed in the rapidity range |y(jet)| &lt; 4.4 and with a transverse momentum p_T(jet) &gt; 20 GeV. The differential cross section dsigma/dE_T(gamma) is measured, as a function of the photon transverse energy, for three different rapidity ranges of the leading-p_T jet: |y(jet)| &lt; 1.2, 1.2 &lt;= |y(jet)| &lt; 2.8 and 2.8 &lt;= |y(jet)| &lt; 4.4. For each rapidity configuration the same-sign (eta(gamma)y(jet) &gt;= 0) and opposite-sign (eta(gamma)y(jet) &lt; 0) cases are studied separately. The results are based on an integrated luminosity of 37 pb-1, collected with the ATLAS detector at the LHC. Next-to-leading order perturbative QCD calculations are found to be in fair agreement with the data, except for E_T(gamma) &lt;~ 45 GeV, where the theoretical predictions overestimate the measured cross sections. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-6 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. Note that the Lumi uncertainty is added in the total systematic uncertainties, which are given in absolute value.
DOI: 10.17182/hepdata.58652.v1/t2
title: "Table 2" of "Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector"

description: The measured cross section as a function of the photon transverse energy, ET, for pT(jet)&gt;20 GeV, |eta(gamma)|&lt;1.37, 1.2&lt;=|y(jet)|&lt;2.8, eta(gamma)*y(jet)&gt;=0.
description: CERN-LHC. A measurement of the cross section for the production of an isolated photon in association with jets in proton-proton collisions at a center-of-mass energy sqrt(s) = 7 TeV is presented. Photons are reconstructed in the pseudorapidity range |eta(gamma)| &lt; 1.37 and with a transverse energy E_T(gamma) &gt; 25 GeV. Jets are reconstructed in the rapidity range |y(jet)| &lt; 4.4 and with a transverse momentum p_T(jet) &gt; 20 GeV. The differential cross section dsigma/dE_T(gamma) is measured, as a function of the photon transverse energy, for three different rapidity ranges of the leading-p_T jet: |y(jet)| &lt; 1.2, 1.2 &lt;= |y(jet)| &lt; 2.8 and 2.8 &lt;= |y(jet)| &lt; 4.4. For each rapidity configuration the same-sign (eta(gamma)y(jet) &gt;= 0) and opposite-sign (eta(gamma)y(jet) &lt; 0) cases are studied separately. The results are based on an integrated luminosity of 37 pb-1, collected with the ATLAS detector at the LHC. Next-to-leading order perturbative QCD calculations are found to be in fair agreement with the data, except for E_T(gamma) &lt;~ 45 GeV, where the theoretical predictions overestimate the measured cross sections. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-6 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. Note that the Lumi uncertainty is added in the total systematic uncertainties, which are given in absolute value.
DOI: 10.17182/hepdata.58652.v1/t3
title: "Table 3" of "Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector"

description: The measured cross section as a function of the photon transverse energy, ET, for pT(jet)&gt;20 GeV, |eta(gamma)|&lt;1.37, 2.8&lt;=|y(jet)|&lt;4.4, eta(gamma)*y(jet)&gt;=0.
description: CERN-LHC. A measurement of the cross section for the production of an isolated photon in association with jets in proton-proton collisions at a center-of-mass energy sqrt(s) = 7 TeV is presented. Photons are reconstructed in the pseudorapidity range |eta(gamma)| &lt; 1.37 and with a transverse energy E_T(gamma) &gt; 25 GeV. Jets are reconstructed in the rapidity range |y(jet)| &lt; 4.4 and with a transverse momentum p_T(jet) &gt; 20 GeV. The differential cross section dsigma/dE_T(gamma) is measured, as a function of the photon transverse energy, for three different rapidity ranges of the leading-p_T jet: |y(jet)| &lt; 1.2, 1.2 &lt;= |y(jet)| &lt; 2.8 and 2.8 &lt;= |y(jet)| &lt; 4.4. For each rapidity configuration the same-sign (eta(gamma)y(jet) &gt;= 0) and opposite-sign (eta(gamma)y(jet) &lt; 0) cases are studied separately. The results are based on an integrated luminosity of 37 pb-1, collected with the ATLAS detector at the LHC. Next-to-leading order perturbative QCD calculations are found to be in fair agreement with the data, except for E_T(gamma) &lt;~ 45 GeV, where the theoretical predictions overestimate the measured cross sections. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-6 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. Note that the Lumi uncertainty is added in the total systematic uncertainties, which are given in absolute value.
DOI: 10.17182/hepdata.58652.v1/t4
title: "Table 4" of "Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector"

description: The measured cross section as a function of the photon transverse energy, ET, for pT(jet)&gt;20 GeV, |eta(gamma)|&lt;1.37, |y(jet)|&lt;1.2, eta(gamma)*y(jet)&lt;0.
description: CERN-LHC. A measurement of the cross section for the production of an isolated photon in association with jets in proton-proton collisions at a center-of-mass energy sqrt(s) = 7 TeV is presented. Photons are reconstructed in the pseudorapidity range |eta(gamma)| &lt; 1.37 and with a transverse energy E_T(gamma) &gt; 25 GeV. Jets are reconstructed in the rapidity range |y(jet)| &lt; 4.4 and with a transverse momentum p_T(jet) &gt; 20 GeV. The differential cross section dsigma/dE_T(gamma) is measured, as a function of the photon transverse energy, for three different rapidity ranges of the leading-p_T jet: |y(jet)| &lt; 1.2, 1.2 &lt;= |y(jet)| &lt; 2.8 and 2.8 &lt;= |y(jet)| &lt; 4.4. For each rapidity configuration the same-sign (eta(gamma)y(jet) &gt;= 0) and opposite-sign (eta(gamma)y(jet) &lt; 0) cases are studied separately. The results are based on an integrated luminosity of 37 pb-1, collected with the ATLAS detector at the LHC. Next-to-leading order perturbative QCD calculations are found to be in fair agreement with the data, except for E_T(gamma) &lt;~ 45 GeV, where the theoretical predictions overestimate the measured cross sections. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-6 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. Note that the Lumi uncertainty is added in the total systematic uncertainties, which are given in absolute value.
DOI: 10.17182/hepdata.58652.v1/t5
title: "Table 5" of "Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector"

description: The measured cross section as a function of the photon transverse energy, ET, for pT(jet)&gt;20 GeV, |eta(gamma)|&lt;1.37, 1.2&lt;=|y(jet)|&lt;2.8, eta(gamma)*y(jet)&lt;0.
description: CERN-LHC. A measurement of the cross section for the production of an isolated photon in association with jets in proton-proton collisions at a center-of-mass energy sqrt(s) = 7 TeV is presented. Photons are reconstructed in the pseudorapidity range |eta(gamma)| &lt; 1.37 and with a transverse energy E_T(gamma) &gt; 25 GeV. Jets are reconstructed in the rapidity range |y(jet)| &lt; 4.4 and with a transverse momentum p_T(jet) &gt; 20 GeV. The differential cross section dsigma/dE_T(gamma) is measured, as a function of the photon transverse energy, for three different rapidity ranges of the leading-p_T jet: |y(jet)| &lt; 1.2, 1.2 &lt;= |y(jet)| &lt; 2.8 and 2.8 &lt;= |y(jet)| &lt; 4.4. For each rapidity configuration the same-sign (eta(gamma)y(jet) &gt;= 0) and opposite-sign (eta(gamma)y(jet) &lt; 0) cases are studied separately. The results are based on an integrated luminosity of 37 pb-1, collected with the ATLAS detector at the LHC. Next-to-leading order perturbative QCD calculations are found to be in fair agreement with the data, except for E_T(gamma) &lt;~ 45 GeV, where the theoretical predictions overestimate the measured cross sections. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-6 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. Note that the Lumi uncertainty is added in the total systematic uncertainties, which are given in absolute value.
DOI: 10.17182/hepdata.58652.v1/t6
title: "Table 6" of "Measurement of the production cross section of an isolated photon associated with jets in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector"

description: The measured cross section as a function of the photon transverse energy, ET, for pT(jet)&gt;20 GeV, |eta(gamma)|&lt;1.37, 2.8&lt;=|y(jet)|&lt;4.4, eta(gamma)*y(jet)&lt;0.
description: CERN-LHC. A measurement of the cross section for the production of an isolated photon in association with jets in proton-proton collisions at a center-of-mass energy sqrt(s) = 7 TeV is presented. Photons are reconstructed in the pseudorapidity range |eta(gamma)| &lt; 1.37 and with a transverse energy E_T(gamma) &gt; 25 GeV. Jets are reconstructed in the rapidity range |y(jet)| &lt; 4.4 and with a transverse momentum p_T(jet) &gt; 20 GeV. The differential cross section dsigma/dE_T(gamma) is measured, as a function of the photon transverse energy, for three different rapidity ranges of the leading-p_T jet: |y(jet)| &lt; 1.2, 1.2 &lt;= |y(jet)| &lt; 2.8 and 2.8 &lt;= |y(jet)| &lt; 4.4. For each rapidity configuration the same-sign (eta(gamma)y(jet) &gt;= 0) and opposite-sign (eta(gamma)y(jet) &lt; 0) cases are studied separately. The results are based on an integrated luminosity of 37 pb-1, collected with the ATLAS detector at the LHC. Next-to-leading order perturbative QCD calculations are found to be in fair agreement with the data, except for E_T(gamma) &lt;~ 45 GeV, where the theoretical predictions overestimate the measured cross sections. 

Note added (27 JUN 2014):
The cross section values reported in Tables 1-6 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. Note that the Lumi uncertainty is added in the total systematic uncertainties, which are given in absolute value.
DOI: 10.17182/hepdata.58676.v1/t1
title: "Table 1" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

description: pT-differential production cross section of muons from heavy flavour decays, in the rapidity range 2.5
description: CERN-LHV. Measurement of the production of muons from heavy flavour decays at forward rapidity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The analysis uses a data sample of total integrated luminosity of 16.5 nb-1 with transverse momentum and rapidity distributions being given in the regions 2-12 GeV/c and 2.4-4 respectively.
DOI: 10.17182/hepdata.58676.v1/t2
title: "Table 2" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

description: y-differential production cross section of muons from heavy flavour decays, in the range 2
description: CERN-LHV. Measurement of the production of muons from heavy flavour decays at forward rapidity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The analysis uses a data sample of total integrated luminosity of 16.5 nb-1 with transverse momentum and rapidity distributions being given in the regions 2-12 GeV/c and 2.4-4 respectively.
DOI: 10.17182/hepdata.58676.v1/t3
title: "Table 3" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

description: pT-differential production cross section of muons from heavy flavour decays, in the rapidity range 2.5
description: CERN-LHV. Measurement of the production of muons from heavy flavour decays at forward rapidity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The analysis uses a data sample of total integrated luminosity of 16.5 nb-1 with transverse momentum and rapidity distributions being given in the regions 2-12 GeV/c and 2.4-4 respectively.
DOI: 10.17182/hepdata.58676.v1/t4
title: "Table 4" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

description: pT-differential production cross section of muons from heavy flavour decays, in the rapidity range 2.8
description: CERN-LHV. Measurement of the production of muons from heavy flavour decays at forward rapidity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The analysis uses a data sample of total integrated luminosity of 16.5 nb-1 with transverse momentum and rapidity distributions being given in the regions 2-12 GeV/c and 2.4-4 respectively.
DOI: 10.17182/hepdata.58676.v1/t5
title: "Table 5" of "Heavy flavour decay muon production at forward rapidity in proton--proton collisions at \sqrt(s) = 7 TeV"

description: pT-differential production cross section of muons from heavy flavour decays, in the rapidity range 3.1
description: CERN-LHV. Measurement of the production of muons from heavy flavour decays at forward rapidity in proton-proton collisions at a centre-of-mass energy of 7 TeV. The analysis uses a data sample of total integrated luminosity of 16.5 nb-1 with transverse momentum and rapidity distributions being given in the regions 2-12 GeV/c and 2.4-4 respectively.