cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.46686.v1/t5
title: "Table 5" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The dijet cross sections as a function of the rapidity gap with the requirement that ET(C=GAP) is less than ET(C=CUT).
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t6
title: "Table 6" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The dijet cross sections as a function of the rapidity gap with the requirement that ET(C=GAP) is less than ET(C=CUT).
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t7
title: "Table 7" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The gap fraction defined as the fraction of all dijet events with ET(C= GAP)
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t8
title: "Table 8" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The gap fraction defined as the fraction of all dijet events with ET(C= GAP)
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t9
title: "Table 9" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The dijet cross sections as a function of X(C=GAMMA) with the requirement that ET(C=GAP) is less than ET(C=CUT).
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t10
title: "Table 10" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The dijet cross sections as a function of X(C=GAMMA) with the requirement that ET(C=GAP) is less than ET(C=CUT).
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t11
title: "Table 11" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The gap fraction defined as the fraction of all dijet events with ET(C= GAP)
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t12
title: "Table 12" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The gap fraction defined as the fraction of all dijet events with ET(C= GAP)
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t13
title: "Table 13" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The dijet cross sections as a function of XP with the requirement that ET(C=GAP) is less than ET(C=CUT).
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t15
title: "Table 15" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The gap fraction defined as the fraction of all dijet events with ET(C= GAP)
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t14
title: "Table 14" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The dijet cross sections as a function of XP with the requirement that ET(C=GAP) is less than ET(C=CUT).
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46686.v1/t16
title: "Table 16" of "Energy flow and rapidity gaps between jets in photoproduction at HERA"

description: The gap fraction defined as the fraction of all dijet events with ET(C= GAP)
description: DESY-HERA. Measurment of the inclusive di-jet cross sections as functions of the longitudinal momentum fractions of the proton and photon which participate in the production of the jets, XP and X(C=GAMMA), and of the pseudorapidity separation between the two highest ET jets, and ET(GAP), the total summed energy between the jets. The data for this analysis were collected during the 1996 running period with 27.6 GeV positrons colliding with 820 GeV protons and have an integrated luminosity of 6.6pb-1. The Q**2 of the photon is restricted to & lt; 0.01 GeV**2 and the photon-proton centre of mass energy W is between 165 and 233 GeV.
DOI: 10.17182/hepdata.46710.v1/t1
title: "Table 1" of "Dijet production in neutral current deep inelastic scattering at HERA."

description: Dijet cross section as a function of LOG10(Q**2).
description: DESY-HERA. Measurement of the Dijet cross sections in neutral current deep inelastic scattering of 27.5 GeV postirons on 820 GeV protons. The cross sections are measured in the Breit Frame using the kT jet alogrithm. The data were collected during the 1996 and 1997 HERA runnning periods and have an integrated luminsoity of 38.4 +- 0.6 pb.-1. The following conditions hold for all the tables:. E(P=1) = 27.5 GeV. E(P=2) = 820 GeV. Y & gt; 0.04. ET(P=4,RF=BREIT) & gt; 8 GeV. ET(P=5,RF=BREIT) & gt; 5 GeV. ET(P=4,RF=LAB) & gt; 5 GeV. ET(P=5,RF=LAB) & gt; 5 GeV. ABS(ETARAP(P=3,4,RF=LAB)) & lt; 2. E(P=3) & gt; 10 GeV. The variable XI is defined as X*(1+M(P_4_5)**2/Q**2 and MEAN(ET) is the average transverse energy of the two jets with highest transverse energy in the event.. In the tables the column headed ISR/FSR is the multiplicative correction which has been applied to account for effects if initial and final-state QED radiation. The second DSYS (systematic) error in the tables is the uncertainty in the jet-energy-scale.
DOI: 10.17182/hepdata.46710.v1/t2
title: "Table 2" of "Dijet production in neutral current deep inelastic scattering at HERA."

description: Dijet cross section as a function of LOG10(MEAN(ET)**2/Q**2).
description: DESY-HERA. Measurement of the Dijet cross sections in neutral current deep inelastic scattering of 27.5 GeV postirons on 820 GeV protons. The cross sections are measured in the Breit Frame using the kT jet alogrithm. The data were collected during the 1996 and 1997 HERA runnning periods and have an integrated luminsoity of 38.4 +- 0.6 pb.-1. The following conditions hold for all the tables:. E(P=1) = 27.5 GeV. E(P=2) = 820 GeV. Y & gt; 0.04. ET(P=4,RF=BREIT) & gt; 8 GeV. ET(P=5,RF=BREIT) & gt; 5 GeV. ET(P=4,RF=LAB) & gt; 5 GeV. ET(P=5,RF=LAB) & gt; 5 GeV. ABS(ETARAP(P=3,4,RF=LAB)) & lt; 2. E(P=3) & gt; 10 GeV. The variable XI is defined as X*(1+M(P_4_5)**2/Q**2 and MEAN(ET) is the average transverse energy of the two jets with highest transverse energy in the event.. In the tables the column headed ISR/FSR is the multiplicative correction which has been applied to account for effects if initial and final-state QED radiation. The second DSYS (systematic) error in the tables is the uncertainty in the jet-energy-scale.
DOI: 10.17182/hepdata.46710.v1/t3
title: "Table 3" of "Dijet production in neutral current deep inelastic scattering at HERA."

description: Dijet cross section as a function of LOG10(XI) for the ful Q**2 range.
description: DESY-HERA. Measurement of the Dijet cross sections in neutral current deep inelastic scattering of 27.5 GeV postirons on 820 GeV protons. The cross sections are measured in the Breit Frame using the kT jet alogrithm. The data were collected during the 1996 and 1997 HERA runnning periods and have an integrated luminsoity of 38.4 +- 0.6 pb.-1. The following conditions hold for all the tables:. E(P=1) = 27.5 GeV. E(P=2) = 820 GeV. Y & gt; 0.04. ET(P=4,RF=BREIT) & gt; 8 GeV. ET(P=5,RF=BREIT) & gt; 5 GeV. ET(P=4,RF=LAB) & gt; 5 GeV. ET(P=5,RF=LAB) & gt; 5 GeV. ABS(ETARAP(P=3,4,RF=LAB)) & lt; 2. E(P=3) & gt; 10 GeV. The variable XI is defined as X*(1+M(P_4_5)**2/Q**2 and MEAN(ET) is the average transverse energy of the two jets with highest transverse energy in the event.. In the tables the column headed ISR/FSR is the multiplicative correction which has been applied to account for effects if initial and final-state QED radiation. The second DSYS (systematic) error in the tables is the uncertainty in the jet-energy-scale.
DOI: 10.17182/hepdata.46710.v1/t4
title: "Table 4" of "Dijet production in neutral current deep inelastic scattering at HERA."

description: Dijet cross section as a function of LOG10(XI), in the Q**2 range 10 to 15.8 GeV**2.
description: DESY-HERA. Measurement of the Dijet cross sections in neutral current deep inelastic scattering of 27.5 GeV postirons on 820 GeV protons. The cross sections are measured in the Breit Frame using the kT jet alogrithm. The data were collected during the 1996 and 1997 HERA runnning periods and have an integrated luminsoity of 38.4 +- 0.6 pb.-1. The following conditions hold for all the tables:. E(P=1) = 27.5 GeV. E(P=2) = 820 GeV. Y & gt; 0.04. ET(P=4,RF=BREIT) & gt; 8 GeV. ET(P=5,RF=BREIT) & gt; 5 GeV. ET(P=4,RF=LAB) & gt; 5 GeV. ET(P=5,RF=LAB) & gt; 5 GeV. ABS(ETARAP(P=3,4,RF=LAB)) & lt; 2. E(P=3) & gt; 10 GeV. The variable XI is defined as X*(1+M(P_4_5)**2/Q**2 and MEAN(ET) is the average transverse energy of the two jets with highest transverse energy in the event.. In the tables the column headed ISR/FSR is the multiplicative correction which has been applied to account for effects if initial and final-state QED radiation. The second DSYS (systematic) error in the tables is the uncertainty in the jet-energy-scale.
DOI: 10.17182/hepdata.46710.v1/t5
title: "Table 5" of "Dijet production in neutral current deep inelastic scattering at HERA."

description: Dijet cross section as a function of LOG10(XI), in the Q**2 range 15.8 to 25.1 GeV**2.
description: DESY-HERA. Measurement of the Dijet cross sections in neutral current deep inelastic scattering of 27.5 GeV postirons on 820 GeV protons. The cross sections are measured in the Breit Frame using the kT jet alogrithm. The data were collected during the 1996 and 1997 HERA runnning periods and have an integrated luminsoity of 38.4 +- 0.6 pb.-1. The following conditions hold for all the tables:. E(P=1) = 27.5 GeV. E(P=2) = 820 GeV. Y & gt; 0.04. ET(P=4,RF=BREIT) & gt; 8 GeV. ET(P=5,RF=BREIT) & gt; 5 GeV. ET(P=4,RF=LAB) & gt; 5 GeV. ET(P=5,RF=LAB) & gt; 5 GeV. ABS(ETARAP(P=3,4,RF=LAB)) & lt; 2. E(P=3) & gt; 10 GeV. The variable XI is defined as X*(1+M(P_4_5)**2/Q**2 and MEAN(ET) is the average transverse energy of the two jets with highest transverse energy in the event.. In the tables the column headed ISR/FSR is the multiplicative correction which has been applied to account for effects if initial and final-state QED radiation. The second DSYS (systematic) error in the tables is the uncertainty in the jet-energy-scale.
DOI: 10.17182/hepdata.46710.v1/t6
title: "Table 6" of "Dijet production in neutral current deep inelastic scattering at HERA."

description: Dijet cross section as a function of LOG10(XI), in the Q**2 range 25.1 to 39.8 GeV**2.
description: DESY-HERA. Measurement of the Dijet cross sections in neutral current deep inelastic scattering of 27.5 GeV postirons on 820 GeV protons. The cross sections are measured in the Breit Frame using the kT jet alogrithm. The data were collected during the 1996 and 1997 HERA runnning periods and have an integrated luminsoity of 38.4 +- 0.6 pb.-1. The following conditions hold for all the tables:. E(P=1) = 27.5 GeV. E(P=2) = 820 GeV. Y & gt; 0.04. ET(P=4,RF=BREIT) & gt; 8 GeV. ET(P=5,RF=BREIT) & gt; 5 GeV. ET(P=4,RF=LAB) & gt; 5 GeV. ET(P=5,RF=LAB) & gt; 5 GeV. ABS(ETARAP(P=3,4,RF=LAB)) & lt; 2. E(P=3) & gt; 10 GeV. The variable XI is defined as X*(1+M(P_4_5)**2/Q**2 and MEAN(ET) is the average transverse energy of the two jets with highest transverse energy in the event.. In the tables the column headed ISR/FSR is the multiplicative correction which has been applied to account for effects if initial and final-state QED radiation. The second DSYS (systematic) error in the tables is the uncertainty in the jet-energy-scale.
DOI: 10.17182/hepdata.46710.v1/t7
title: "Table 7" of "Dijet production in neutral current deep inelastic scattering at HERA."

description: Dijet cross section as a function of LOG10(XI), in the Q**2 range 39.8 to 63.1 GeV**2.
description: DESY-HERA. Measurement of the Dijet cross sections in neutral current deep inelastic scattering of 27.5 GeV postirons on 820 GeV protons. The cross sections are measured in the Breit Frame using the kT jet alogrithm. The data were collected during the 1996 and 1997 HERA runnning periods and have an integrated luminsoity of 38.4 +- 0.6 pb.-1. The following conditions hold for all the tables:. E(P=1) = 27.5 GeV. E(P=2) = 820 GeV. Y & gt; 0.04. ET(P=4,RF=BREIT) & gt; 8 GeV. ET(P=5,RF=BREIT) & gt; 5 GeV. ET(P=4,RF=LAB) & gt; 5 GeV. ET(P=5,RF=LAB) & gt; 5 GeV. ABS(ETARAP(P=3,4,RF=LAB)) & lt; 2. E(P=3) & gt; 10 GeV. The variable XI is defined as X*(1+M(P_4_5)**2/Q**2 and MEAN(ET) is the average transverse energy of the two jets with highest transverse energy in the event.. In the tables the column headed ISR/FSR is the multiplicative correction which has been applied to account for effects if initial and final-state QED radiation. The second DSYS (systematic) error in the tables is the uncertainty in the jet-energy-scale.
DOI: 10.17182/hepdata.46710.v1/t8
title: "Table 8" of "Dijet production in neutral current deep inelastic scattering at HERA."

description: Dijet cross section as a function of LOG10(XI), in the Q**2 range 63.1 to 100 GeV**2.
description: DESY-HERA. Measurement of the Dijet cross sections in neutral current deep inelastic scattering of 27.5 GeV postirons on 820 GeV protons. The cross sections are measured in the Breit Frame using the kT jet alogrithm. The data were collected during the 1996 and 1997 HERA runnning periods and have an integrated luminsoity of 38.4 +- 0.6 pb.-1. The following conditions hold for all the tables:. E(P=1) = 27.5 GeV. E(P=2) = 820 GeV. Y & gt; 0.04. ET(P=4,RF=BREIT) & gt; 8 GeV. ET(P=5,RF=BREIT) & gt; 5 GeV. ET(P=4,RF=LAB) & gt; 5 GeV. ET(P=5,RF=LAB) & gt; 5 GeV. ABS(ETARAP(P=3,4,RF=LAB)) & lt; 2. E(P=3) & gt; 10 GeV. The variable XI is defined as X*(1+M(P_4_5)**2/Q**2 and MEAN(ET) is the average transverse energy of the two jets with highest transverse energy in the event.. In the tables the column headed ISR/FSR is the multiplicative correction which has been applied to account for effects if initial and final-state QED radiation. The second DSYS (systematic) error in the tables is the uncertainty in the jet-energy-scale.
DOI: 10.17182/hepdata.46710.v1/t9
title: "Table 9" of "Dijet production in neutral current deep inelastic scattering at HERA."

description: Dijet cross section as a function of LOG10(XI), in the Q**2 range 100 to 214 GeV**2.. XI = X*(1+M(P_4_5)**2/Q**2.
description: DESY-HERA. Measurement of the Dijet cross sections in neutral current deep inelastic scattering of 27.5 GeV postirons on 820 GeV protons. The cross sections are measured in the Breit Frame using the kT jet alogrithm. The data were collected during the 1996 and 1997 HERA runnning periods and have an integrated luminsoity of 38.4 +- 0.6 pb.-1. The following conditions hold for all the tables:. E(P=1) = 27.5 GeV. E(P=2) = 820 GeV. Y & gt; 0.04. ET(P=4,RF=BREIT) & gt; 8 GeV. ET(P=5,RF=BREIT) & gt; 5 GeV. ET(P=4,RF=LAB) & gt; 5 GeV. ET(P=5,RF=LAB) & gt; 5 GeV. ABS(ETARAP(P=3,4,RF=LAB)) & lt; 2. E(P=3) & gt; 10 GeV. The variable XI is defined as X*(1+M(P_4_5)**2/Q**2 and MEAN(ET) is the average transverse energy of the two jets with highest transverse energy in the event.. In the tables the column headed ISR/FSR is the multiplicative correction which has been applied to account for effects if initial and final-state QED radiation. The second DSYS (systematic) error in the tables is the uncertainty in the jet-energy-scale.
DOI: 10.17182/hepdata.46710.v1/t10
title: "Table 10" of "Dijet production in neutral current deep inelastic scattering at HERA."

description: Dijet cross section as a function of LOG10(XI), in the Q**2 range 214 to 468 GeV**2.
description: DESY-HERA. Measurement of the Dijet cross sections in neutral current deep inelastic scattering of 27.5 GeV postirons on 820 GeV protons. The cross sections are measured in the Breit Frame using the kT jet alogrithm. The data were collected during the 1996 and 1997 HERA runnning periods and have an integrated luminsoity of 38.4 +- 0.6 pb.-1. The following conditions hold for all the tables:. E(P=1) = 27.5 GeV. E(P=2) = 820 GeV. Y & gt; 0.04. ET(P=4,RF=BREIT) & gt; 8 GeV. ET(P=5,RF=BREIT) & gt; 5 GeV. ET(P=4,RF=LAB) & gt; 5 GeV. ET(P=5,RF=LAB) & gt; 5 GeV. ABS(ETARAP(P=3,4,RF=LAB)) & lt; 2. E(P=3) & gt; 10 GeV. The variable XI is defined as X*(1+M(P_4_5)**2/Q**2 and MEAN(ET) is the average transverse energy of the two jets with highest transverse energy in the event.. In the tables the column headed ISR/FSR is the multiplicative correction which has been applied to account for effects if initial and final-state QED radiation. The second DSYS (systematic) error in the tables is the uncertainty in the jet-energy-scale.