cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.46198.v1/t4
title: "Table 4" of "Forward jet production in deep inelastic e p scattering and low-x parton dynamics at HERA."

description: Inclusive jet cross section DSIG/DX for jets of hadrons in the global phase space.
description: DESY-HERA. Measurement of inclusive jet cross sections in neutral current DIS of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-97 running period with an integrated luminosity of 38.7 pb-1. Jets are identified using the KT cluster algorithm in the longitudinally invariant inclusive mode in the laboratory frame, selected with jet transverse energy above 6 GeV and jet pseudorapidity between -1 and 3. Measurements in three phase space regions are given, global, BFKL and forward-BFKL to study parton dynamics. Gamma(P=4) is the polar angle of the jet.. In the tables the second systematic (DSYS) error is the uncertainty in the jet-energy-scale which is shown seperately from the other systematic errors.
DOI: 10.17182/hepdata.46198.v1/t5
title: "Table 5" of "Forward jet production in deep inelastic e p scattering and low-x parton dynamics at HERA."

description: Inclusive jet cross section DSIG/DETARAP for jets of hadrons in the BFKL phase space region.
description: DESY-HERA. Measurement of inclusive jet cross sections in neutral current DIS of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-97 running period with an integrated luminosity of 38.7 pb-1. Jets are identified using the KT cluster algorithm in the longitudinally invariant inclusive mode in the laboratory frame, selected with jet transverse energy above 6 GeV and jet pseudorapidity between -1 and 3. Measurements in three phase space regions are given, global, BFKL and forward-BFKL to study parton dynamics. Gamma(P=4) is the polar angle of the jet.. In the tables the second systematic (DSYS) error is the uncertainty in the jet-energy-scale which is shown seperately from the other systematic errors.
DOI: 10.17182/hepdata.46198.v1/t6
title: "Table 6" of "Forward jet production in deep inelastic e p scattering and low-x parton dynamics at HERA."

description: Inclusive jet cross section DSIG/DET for jets of hadrons in the BFKL phase space region.
description: DESY-HERA. Measurement of inclusive jet cross sections in neutral current DIS of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-97 running period with an integrated luminosity of 38.7 pb-1. Jets are identified using the KT cluster algorithm in the longitudinally invariant inclusive mode in the laboratory frame, selected with jet transverse energy above 6 GeV and jet pseudorapidity between -1 and 3. Measurements in three phase space regions are given, global, BFKL and forward-BFKL to study parton dynamics. Gamma(P=4) is the polar angle of the jet.. In the tables the second systematic (DSYS) error is the uncertainty in the jet-energy-scale which is shown seperately from the other systematic errors.
DOI: 10.17182/hepdata.46198.v1/t10
title: "Table 10" of "Forward jet production in deep inelastic e p scattering and low-x parton dynamics at HERA."

description: Inclusive jet cross section DSIG/DQ**2 for jets of hadrons in the forward-BFKL phase space region.
description: DESY-HERA. Measurement of inclusive jet cross sections in neutral current DIS of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-97 running period with an integrated luminosity of 38.7 pb-1. Jets are identified using the KT cluster algorithm in the longitudinally invariant inclusive mode in the laboratory frame, selected with jet transverse energy above 6 GeV and jet pseudorapidity between -1 and 3. Measurements in three phase space regions are given, global, BFKL and forward-BFKL to study parton dynamics. Gamma(P=4) is the polar angle of the jet.. In the tables the second systematic (DSYS) error is the uncertainty in the jet-energy-scale which is shown seperately from the other systematic errors.
DOI: 10.17182/hepdata.46198.v1/t11
title: "Table 11" of "Forward jet production in deep inelastic e p scattering and low-x parton dynamics at HERA."

description: Inclusive jet cross section DSIG/DX for jets of hadrons in the forward-BFKL phase space region.
description: DESY-HERA. Measurement of inclusive jet cross sections in neutral current DIS of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-97 running period with an integrated luminosity of 38.7 pb-1. Jets are identified using the KT cluster algorithm in the longitudinally invariant inclusive mode in the laboratory frame, selected with jet transverse energy above 6 GeV and jet pseudorapidity between -1 and 3. Measurements in three phase space regions are given, global, BFKL and forward-BFKL to study parton dynamics. Gamma(P=4) is the polar angle of the jet.. In the tables the second systematic (DSYS) error is the uncertainty in the jet-energy-scale which is shown seperately from the other systematic errors.
DOI: 10.17182/hepdata.46198.v1/t7
title: "Table 7" of "Forward jet production in deep inelastic e p scattering and low-x parton dynamics at HERA."

description: Inclusive jet cross section DSIG/DQ**2 for jets of hadrons in the BFKL phase space region.
description: DESY-HERA. Measurement of inclusive jet cross sections in neutral current DIS of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-97 running period with an integrated luminosity of 38.7 pb-1. Jets are identified using the KT cluster algorithm in the longitudinally invariant inclusive mode in the laboratory frame, selected with jet transverse energy above 6 GeV and jet pseudorapidity between -1 and 3. Measurements in three phase space regions are given, global, BFKL and forward-BFKL to study parton dynamics. Gamma(P=4) is the polar angle of the jet.. In the tables the second systematic (DSYS) error is the uncertainty in the jet-energy-scale which is shown seperately from the other systematic errors.
DOI: 10.17182/hepdata.46198.v1/t8
title: "Table 8" of "Forward jet production in deep inelastic e p scattering and low-x parton dynamics at HERA."

description: Inclusive jet cross section DSIG/DX for jets of hadrons in the BFKL phase space region.
description: DESY-HERA. Measurement of inclusive jet cross sections in neutral current DIS of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-97 running period with an integrated luminosity of 38.7 pb-1. Jets are identified using the KT cluster algorithm in the longitudinally invariant inclusive mode in the laboratory frame, selected with jet transverse energy above 6 GeV and jet pseudorapidity between -1 and 3. Measurements in three phase space regions are given, global, BFKL and forward-BFKL to study parton dynamics. Gamma(P=4) is the polar angle of the jet.. In the tables the second systematic (DSYS) error is the uncertainty in the jet-energy-scale which is shown seperately from the other systematic errors.
DOI: 10.17182/hepdata.46198.v1/t9
title: "Table 9" of "Forward jet production in deep inelastic e p scattering and low-x parton dynamics at HERA."

description: Inclusive jet cross section DSIG/DET for jets of hadrons in the forward-BFKL phase space region.
description: DESY-HERA. Measurement of inclusive jet cross sections in neutral current DIS of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-97 running period with an integrated luminosity of 38.7 pb-1. Jets are identified using the KT cluster algorithm in the longitudinally invariant inclusive mode in the laboratory frame, selected with jet transverse energy above 6 GeV and jet pseudorapidity between -1 and 3. Measurements in three phase space regions are given, global, BFKL and forward-BFKL to study parton dynamics. Gamma(P=4) is the polar angle of the jet.. In the tables the second systematic (DSYS) error is the uncertainty in the jet-energy-scale which is shown seperately from the other systematic errors.
DOI: 10.17182/hepdata.46199.v1/t1
title: "Table 1" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Differential e p photoproduction cross section as a function of the jet transverse energy.
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t2
title: "Table 2" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Differential e p photoproduction cross section as a function of JET pseudorapidity.
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t3
title: "Table 3" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Differential e p photoproduction cross section as a function of JET X(C=GAMMA).
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t4
title: "Table 4" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Differential e p photoproduction cross section as a function of JET X(C=PI).
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t5
title: "Table 5" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Differential e p DIS cross section as a function of the jet transverse energy.
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t6
title: "Table 6" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Differential e p DIS cross section as a function of the Jet pseudorapidity.
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t7
title: "Table 7" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Differential e p DIS cross section as a function of the Jet X(C=GAMMA).
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t10
title: "Table 10" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Ratio of cross section for dijet production with a leading neutron to that for inclusive dijet production as a function of the jet transverse energy.
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t11
title: "Table 11" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Ratio of cross section for dijet production with a leading neutron to that for inclusive dijet production as a function of the jet pseudorapidity.
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t8
title: "Table 8" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Differential e p DIS cross section as a function of the Jet X(C=PI).
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t9
title: "Table 9" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Differential e p DIS cross section as a function of the Q**2.
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t12
title: "Table 12" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Ratio of cross section for dijet production with a leading neutron to that for inclusive dijet production as a function of the jet X(C=GAMMA).
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t13
title: "Table 13" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Ratio of cross section for dijet production with a leading neutron to that for inclusive dijet production as a function of the jet X(C=PI).
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46199.v1/t14
title: "Table 14" of "Measurement of dijet cross sections in e p interactions with a leading neutron at HERA."

description: Ratio of the cross section for dijet production with a leading neutron to that for inclusive dijet production as a function of Q**2.
description: DESY-HERA. Measurements of photoproduction and DIS production of dijets with a leading neutron in collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during the 1996-1997 running period and have an integrated luminosity of 19.2 pb-1. In the tables the first systematic (DSYS) error is the uncorrelated systematic error and the second is correlated. The following definitions are used:. X(C=GAMMA) is the fraction of the 4-momentum of the virtual photon which participates in the hard interaction.. X(C=PI) is the fraction of the 4-momentum of the pion, in the pion exchange model, which participates in the hard interaction.. See the text of the paper of more detailed definitions.
DOI: 10.17182/hepdata.46200.v1/t1
title: "Table 1" of "Measurement of prompt photon cross sections in photoproduction at HERA."

description: Inclusive prompt photon differential cross section as a function of ET.
description: DESY-HERA. Measurement of cross sections for prompt photon production in photoproduction data. The data come from the 1996 to 2000 running period with electrons and positrons of energy 27.6 GeV colliding with protons of energies 820 and 920 GeV giving c.m. energies of 301 and 319 GeV. The total integrated luminosity is 105 pb-1 (28.8 pb-1 and 61.3 pb-1 from E+ P at 301 and 319 GeV respectively, and 14.9 GeV with E- P at 319 GeV). The data cover the GAMMA P c.m. range W from 142 to 266 GeV with cross sections measured for the PT range of the photon 5 to 10 GeV and for associated jets with ET(JET) & gt; 4.5 GeV.
DOI: 10.17182/hepdata.46200.v1/t2
title: "Table 2" of "Measurement of prompt photon cross sections in photoproduction at HERA."

description: Inclusive prompt photon differential cross section as a function of the pseudorapidity.
description: DESY-HERA. Measurement of cross sections for prompt photon production in photoproduction data. The data come from the 1996 to 2000 running period with electrons and positrons of energy 27.6 GeV colliding with protons of energies 820 and 920 GeV giving c.m. energies of 301 and 319 GeV. The total integrated luminosity is 105 pb-1 (28.8 pb-1 and 61.3 pb-1 from E+ P at 301 and 319 GeV respectively, and 14.9 GeV with E- P at 319 GeV). The data cover the GAMMA P c.m. range W from 142 to 266 GeV with cross sections measured for the PT range of the photon 5 to 10 GeV and for associated jets with ET(JET) & gt; 4.5 GeV.
DOI: 10.17182/hepdata.46200.v1/t3
title: "Table 3" of "Measurement of prompt photon cross sections in photoproduction at HERA."

description: Prompt photon cross section as a function of the photon ET with an additional jet requirement.
description: DESY-HERA. Measurement of cross sections for prompt photon production in photoproduction data. The data come from the 1996 to 2000 running period with electrons and positrons of energy 27.6 GeV colliding with protons of energies 820 and 920 GeV giving c.m. energies of 301 and 319 GeV. The total integrated luminosity is 105 pb-1 (28.8 pb-1 and 61.3 pb-1 from E+ P at 301 and 319 GeV respectively, and 14.9 GeV with E- P at 319 GeV). The data cover the GAMMA P c.m. range W from 142 to 266 GeV with cross sections measured for the PT range of the photon 5 to 10 GeV and for associated jets with ET(JET) & gt; 4.5 GeV.