cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.63860.v1/t6
title: "Table 6" of "Forward Neutron Production at the Fermilab Main Injector"

description: Lorentz-invariant cross section as a function of xF for pp collisions at 58 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t7
title: "Table 7" of "Forward Neutron Production at the Fermilab Main Injector"

description: Lorentz-invariant cross section as a function of xF for pC collisions at 58 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t8
title: "Table 8" of "Forward Neutron Production at the Fermilab Main Injector"

description: Lorentz-invariant cross section as a function of xF for pBi collisions at 58 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t9
title: "Table 9" of "Forward Neutron Production at the Fermilab Main Injector"

description: Lorentz-invariant cross section as a function of xF for pU collisions at 58 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t11
title: "Table 11" of "Forward Neutron Production at the Fermilab Main Injector"

description: Lorentz-invariant cross section as a function of xF for pBe collisions at 120 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t12
title: "Table 12" of "Forward Neutron Production at the Fermilab Main Injector"

description: Lorentz-invariant cross section as a function of xF for pC collisions at 120 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t13
title: "Table 13" of "Forward Neutron Production at the Fermilab Main Injector"

description: Lorentz-invariant cross section as a function of xF for pBi collisions at 120 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t14
title: "Table 14" of "Forward Neutron Production at the Fermilab Main Injector"

description: dsig/dxF as a function of xF for pp collisions at 58 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t15
title: "Table 15" of "Forward Neutron Production at the Fermilab Main Injector"

description: dsig/dxF as a function of xF for pC collisions at 58 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t16
title: "Table 16" of "Forward Neutron Production at the Fermilab Main Injector"

description: dsig/dxF as a function of xF for pBi collisions at 58 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t17
title: "Table 17" of "Forward Neutron Production at the Fermilab Main Injector"

description: dsig/dxF as a function of xF for pU collisions at 58 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t18
title: "Table 18" of "Forward Neutron Production at the Fermilab Main Injector"

description: dsig/dxF as a function of xF for pp collisions at 84 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t19
title: "Table 19" of "Forward Neutron Production at the Fermilab Main Injector"

description: dsig/dxF as a function of xF for pBe collisions at 120 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t20
title: "Table 20" of "Forward Neutron Production at the Fermilab Main Injector"

description: dsig/dxF as a function of xF for pC collisions at 120 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63860.v1/t21
title: "Table 21" of "Forward Neutron Production at the Fermilab Main Injector"

description: dsig/dxF as a function of xF for pBi collisions at 120 GeV.
description: Fermilab. Measurement of the cross sections for forward neutron production from a variety of targets (P, BE, BI, C and U) using proton beams of momenta 58, 84 and 120 GeV/c from the Fermilab Main Injector. Numerical values supplied by M. Longo.
DOI: 10.17182/hepdata.63866.v1/t1
title: "Table 1" of "Measurement of prompt D-meson production in p-Pb collisions at sqrt(sNN) = 5.02 TeV"

description: pT-differential cross section of prompt D0 mesons measured in p-Pb collisions in the rapidity interval -0.96
description: CERN-LHC. The pT-differential production cross sections of the prompt charmed mesons D0, D+, D*+ and Ds+ and their charge conjugate in the rapidity interval -0.96 &lt; y_{cms} &lt; 0.04 were measured in p-Pb collisions at a centre-of-mass energy sqrt(sNN) = 5.02 TeV with the ALICE detector at the LHC. The nuclear modification factor R(pPb), quantifying the D-meson yield in p-Pb collisions relative to the yield in pp collisions scaled by the number of binary nucleon-nucleon collisions, is compatible within the 15-20% uncertainties with unity in the transverse momentum interval 1 &lt; pT &lt; 24 GeV. No significant difference among the R(pPb) of the four D-meson species is observed. The results are described within uncertainties by theoretical calculations that include initial-state effects. The measurement adds experimental evidence that the modification of the momentum spectrum of D mesons observed in Pb-Pb collisions with respect to pp collisions is due to strong final-state effects induced by hot partonic matter. UPDATE (03 JUL 2015): swapped upper/lower systematic uncertainties and enlarged global normalisation uncertainty due to variation of the uncertainty of the luminosity determination.
DOI: 10.17182/hepdata.63866.v1/t2
title: "Table 2" of "Measurement of prompt D-meson production in p-Pb collisions at sqrt(sNN) = 5.02 TeV"

description: pT-differential cross section of prompt D+ mesons measured in p-Pb collisions in the rapidity interval -0.96
description: CERN-LHC. The pT-differential production cross sections of the prompt charmed mesons D0, D+, D*+ and Ds+ and their charge conjugate in the rapidity interval -0.96 &lt; y_{cms} &lt; 0.04 were measured in p-Pb collisions at a centre-of-mass energy sqrt(sNN) = 5.02 TeV with the ALICE detector at the LHC. The nuclear modification factor R(pPb), quantifying the D-meson yield in p-Pb collisions relative to the yield in pp collisions scaled by the number of binary nucleon-nucleon collisions, is compatible within the 15-20% uncertainties with unity in the transverse momentum interval 1 &lt; pT &lt; 24 GeV. No significant difference among the R(pPb) of the four D-meson species is observed. The results are described within uncertainties by theoretical calculations that include initial-state effects. The measurement adds experimental evidence that the modification of the momentum spectrum of D mesons observed in Pb-Pb collisions with respect to pp collisions is due to strong final-state effects induced by hot partonic matter. UPDATE (03 JUL 2015): swapped upper/lower systematic uncertainties and enlarged global normalisation uncertainty due to variation of the uncertainty of the luminosity determination.
DOI: 10.17182/hepdata.63866.v1/t4
title: "Table 4" of "Measurement of prompt D-meson production in p-Pb collisions at sqrt(sNN) = 5.02 TeV"

description: pT-differential cross section of prompt Ds+ mesons measured in p-Pb collisions in the rapidity interval -0.96
description: CERN-LHC. The pT-differential production cross sections of the prompt charmed mesons D0, D+, D*+ and Ds+ and their charge conjugate in the rapidity interval -0.96 &lt; y_{cms} &lt; 0.04 were measured in p-Pb collisions at a centre-of-mass energy sqrt(sNN) = 5.02 TeV with the ALICE detector at the LHC. The nuclear modification factor R(pPb), quantifying the D-meson yield in p-Pb collisions relative to the yield in pp collisions scaled by the number of binary nucleon-nucleon collisions, is compatible within the 15-20% uncertainties with unity in the transverse momentum interval 1 &lt; pT &lt; 24 GeV. No significant difference among the R(pPb) of the four D-meson species is observed. The results are described within uncertainties by theoretical calculations that include initial-state effects. The measurement adds experimental evidence that the modification of the momentum spectrum of D mesons observed in Pb-Pb collisions with respect to pp collisions is due to strong final-state effects induced by hot partonic matter. UPDATE (03 JUL 2015): swapped upper/lower systematic uncertainties and enlarged global normalisation uncertainty due to variation of the uncertainty of the luminosity determination.
DOI: 10.17182/hepdata.63866.v1/t3
title: "Table 3" of "Measurement of prompt D-meson production in p-Pb collisions at sqrt(sNN) = 5.02 TeV"

description: pT-differential cross section of prompt D*+ mesons measured in p-Pb collisions in the rapidity interval -0.96
description: CERN-LHC. The pT-differential production cross sections of the prompt charmed mesons D0, D+, D*+ and Ds+ and their charge conjugate in the rapidity interval -0.96 &lt; y_{cms} &lt; 0.04 were measured in p-Pb collisions at a centre-of-mass energy sqrt(sNN) = 5.02 TeV with the ALICE detector at the LHC. The nuclear modification factor R(pPb), quantifying the D-meson yield in p-Pb collisions relative to the yield in pp collisions scaled by the number of binary nucleon-nucleon collisions, is compatible within the 15-20% uncertainties with unity in the transverse momentum interval 1 &lt; pT &lt; 24 GeV. No significant difference among the R(pPb) of the four D-meson species is observed. The results are described within uncertainties by theoretical calculations that include initial-state effects. The measurement adds experimental evidence that the modification of the momentum spectrum of D mesons observed in Pb-Pb collisions with respect to pp collisions is due to strong final-state effects induced by hot partonic matter. UPDATE (03 JUL 2015): swapped upper/lower systematic uncertainties and enlarged global normalisation uncertainty due to variation of the uncertainty of the luminosity determination.
DOI: 10.17182/hepdata.63866.v1/t5
title: "Table 5" of "Measurement of prompt D-meson production in p-Pb collisions at sqrt(sNN) = 5.02 TeV"

description: Nuclear modification factor R(pPb) of prompt D0 mesons vs. pT measured in p-Pb collisions in the rapidity interval -0.96
description: CERN-LHC. The pT-differential production cross sections of the prompt charmed mesons D0, D+, D*+ and Ds+ and their charge conjugate in the rapidity interval -0.96 &lt; y_{cms} &lt; 0.04 were measured in p-Pb collisions at a centre-of-mass energy sqrt(sNN) = 5.02 TeV with the ALICE detector at the LHC. The nuclear modification factor R(pPb), quantifying the D-meson yield in p-Pb collisions relative to the yield in pp collisions scaled by the number of binary nucleon-nucleon collisions, is compatible within the 15-20% uncertainties with unity in the transverse momentum interval 1 &lt; pT &lt; 24 GeV. No significant difference among the R(pPb) of the four D-meson species is observed. The results are described within uncertainties by theoretical calculations that include initial-state effects. The measurement adds experimental evidence that the modification of the momentum spectrum of D mesons observed in Pb-Pb collisions with respect to pp collisions is due to strong final-state effects induced by hot partonic matter. UPDATE (03 JUL 2015): swapped upper/lower systematic uncertainties and enlarged global normalisation uncertainty due to variation of the uncertainty of the luminosity determination.
DOI: 10.17182/hepdata.63866.v1/t6
title: "Table 6" of "Measurement of prompt D-meson production in p-Pb collisions at sqrt(sNN) = 5.02 TeV"

description: Nuclear modification factor R(pPb) of D+ mesons vs. pT measured in p-Pb collisions in the rapidity interval -0.96
description: CERN-LHC. The pT-differential production cross sections of the prompt charmed mesons D0, D+, D*+ and Ds+ and their charge conjugate in the rapidity interval -0.96 &lt; y_{cms} &lt; 0.04 were measured in p-Pb collisions at a centre-of-mass energy sqrt(sNN) = 5.02 TeV with the ALICE detector at the LHC. The nuclear modification factor R(pPb), quantifying the D-meson yield in p-Pb collisions relative to the yield in pp collisions scaled by the number of binary nucleon-nucleon collisions, is compatible within the 15-20% uncertainties with unity in the transverse momentum interval 1 &lt; pT &lt; 24 GeV. No significant difference among the R(pPb) of the four D-meson species is observed. The results are described within uncertainties by theoretical calculations that include initial-state effects. The measurement adds experimental evidence that the modification of the momentum spectrum of D mesons observed in Pb-Pb collisions with respect to pp collisions is due to strong final-state effects induced by hot partonic matter. UPDATE (03 JUL 2015): swapped upper/lower systematic uncertainties and enlarged global normalisation uncertainty due to variation of the uncertainty of the luminosity determination.
DOI: 10.17182/hepdata.63866.v1/t7
title: "Table 7" of "Measurement of prompt D-meson production in p-Pb collisions at sqrt(sNN) = 5.02 TeV"

description: Nuclear modification factor R(pPb) of D*+ mesons vs. pT measured in p-Pb collisions in the rapidity interval -0.96
description: CERN-LHC. The pT-differential production cross sections of the prompt charmed mesons D0, D+, D*+ and Ds+ and their charge conjugate in the rapidity interval -0.96 &lt; y_{cms} &lt; 0.04 were measured in p-Pb collisions at a centre-of-mass energy sqrt(sNN) = 5.02 TeV with the ALICE detector at the LHC. The nuclear modification factor R(pPb), quantifying the D-meson yield in p-Pb collisions relative to the yield in pp collisions scaled by the number of binary nucleon-nucleon collisions, is compatible within the 15-20% uncertainties with unity in the transverse momentum interval 1 &lt; pT &lt; 24 GeV. No significant difference among the R(pPb) of the four D-meson species is observed. The results are described within uncertainties by theoretical calculations that include initial-state effects. The measurement adds experimental evidence that the modification of the momentum spectrum of D mesons observed in Pb-Pb collisions with respect to pp collisions is due to strong final-state effects induced by hot partonic matter. UPDATE (03 JUL 2015): swapped upper/lower systematic uncertainties and enlarged global normalisation uncertainty due to variation of the uncertainty of the luminosity determination.
DOI: 10.17182/hepdata.63866.v1/t8
title: "Table 8" of "Measurement of prompt D-meson production in p-Pb collisions at sqrt(sNN) = 5.02 TeV"

description: Nuclear modification factor R(pPb) of Ds+ mesons vs. pT measured in p-Pb collisions in the rapidity interval -0.96
description: CERN-LHC. The pT-differential production cross sections of the prompt charmed mesons D0, D+, D*+ and Ds+ and their charge conjugate in the rapidity interval -0.96 &lt; y_{cms} &lt; 0.04 were measured in p-Pb collisions at a centre-of-mass energy sqrt(sNN) = 5.02 TeV with the ALICE detector at the LHC. The nuclear modification factor R(pPb), quantifying the D-meson yield in p-Pb collisions relative to the yield in pp collisions scaled by the number of binary nucleon-nucleon collisions, is compatible within the 15-20% uncertainties with unity in the transverse momentum interval 1 &lt; pT &lt; 24 GeV. No significant difference among the R(pPb) of the four D-meson species is observed. The results are described within uncertainties by theoretical calculations that include initial-state effects. The measurement adds experimental evidence that the modification of the momentum spectrum of D mesons observed in Pb-Pb collisions with respect to pp collisions is due to strong final-state effects induced by hot partonic matter. UPDATE (03 JUL 2015): swapped upper/lower systematic uncertainties and enlarged global normalisation uncertainty due to variation of the uncertainty of the luminosity determination.
DOI: 10.17182/hepdata.63866.v1/t9
title: "Table 9" of "Measurement of prompt D-meson production in p-Pb collisions at sqrt(sNN) = 5.02 TeV"

description: Average of D0, D+, D*+ nuclear modification factors R(pPb) vs. pT.
description: CERN-LHC. The pT-differential production cross sections of the prompt charmed mesons D0, D+, D*+ and Ds+ and their charge conjugate in the rapidity interval -0.96 &lt; y_{cms} &lt; 0.04 were measured in p-Pb collisions at a centre-of-mass energy sqrt(sNN) = 5.02 TeV with the ALICE detector at the LHC. The nuclear modification factor R(pPb), quantifying the D-meson yield in p-Pb collisions relative to the yield in pp collisions scaled by the number of binary nucleon-nucleon collisions, is compatible within the 15-20% uncertainties with unity in the transverse momentum interval 1 &lt; pT &lt; 24 GeV. No significant difference among the R(pPb) of the four D-meson species is observed. The results are described within uncertainties by theoretical calculations that include initial-state effects. The measurement adds experimental evidence that the modification of the momentum spectrum of D mesons observed in Pb-Pb collisions with respect to pp collisions is due to strong final-state effects induced by hot partonic matter. UPDATE (03 JUL 2015): swapped upper/lower systematic uncertainties and enlarged global normalisation uncertainty due to variation of the uncertainty of the luminosity determination.
DOI: 10.17182/hepdata.63897.v1/t1
title: "Table 1" of "Measurement of hard double-parton interactions in $W(\to l\nu)$+ 2 jet events at $\sqrt{s}$=7 TeV with the ATLAS detector"

description: Distribution of Delta(jets,normalised), defined in Eq. (11) of the paper as the transverse momentum of the dijet system normalised by the sum of the individual transverse momenta, in the data after unfolding to hadron level. The errors on the data represent the quadrature sum of the statistical and systematic uncertainties. Data have been normalised to unity.
description: CERN-LHC. The production of W bosons in association with two jets in proton-proton collisions at a centre-of-mass energy of sqrt(s) = 7 TeV has been analysed for the presence of double-parton interactions using data corresponding to an integrated luminosity of 36 pb^-1, collected in 2010 with the ATLAS detector at the LHC. The fraction of events arising from double-parton interactions, f_{DP}^{(D)}, has been measured through the momentum balance between the two jets and amounts to f_{DP}^{(D)} = 0.08 +- 0.01 (stat.) +- 0.02 (sys) for jets with transverse momentum pT &gt; 20 GeV and rapidity |y| &lt; 2.8. This corresponds to a measurement of the effective area parameter for hard double-parton interactions of sigma_{eff} = 15 +- 3 (stat.) +5,-3 (sys.) mb.

Data points reverse engineered from Figure 9 of paper by Evgeny Slavin.
DOI: 10.17182/hepdata.63897.v1/t2
title: "Table 2" of "Measurement of hard double-parton interactions in $W(\to l\nu)$+ 2 jet events at $\sqrt{s}$=7 TeV with the ATLAS detector"

description: Distribution of Delta(jets), defined in Eq. (10) of the paper as the transverse momentum of the dijet system, in the data after unfolding to hadron level. The errors on the data represent the quadrature sum of the statistical and systematic uncertainties. Data have been normalised to unity.
description: CERN-LHC. The production of W bosons in association with two jets in proton-proton collisions at a centre-of-mass energy of sqrt(s) = 7 TeV has been analysed for the presence of double-parton interactions using data corresponding to an integrated luminosity of 36 pb^-1, collected in 2010 with the ATLAS detector at the LHC. The fraction of events arising from double-parton interactions, f_{DP}^{(D)}, has been measured through the momentum balance between the two jets and amounts to f_{DP}^{(D)} = 0.08 +- 0.01 (stat.) +- 0.02 (sys) for jets with transverse momentum pT &gt; 20 GeV and rapidity |y| &lt; 2.8. This corresponds to a measurement of the effective area parameter for hard double-parton interactions of sigma_{eff} = 15 +- 3 (stat.) +5,-3 (sys.) mb.

Data points reverse engineered from Figure 9 of paper by Evgeny Slavin.