cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.44302.v1/t2
title: "Table 2" of "Diffractive dijet cross-sections in photoproduction at HERA"

description: Differential cross section as a function of transverse energy Et of the tw o highest Et jets in event.
description: DESY-HERA. Measurement of diffractive dijet differential cross sections in photoproduction events in which the hadronic final state containing the jets is separated with respect to the outgoing proton direction by a large rapidity gap. Jets are reconstructed using an iterative cone alogrithm in the eta-phi plane with a cone radius of 1.
DOI: 10.17182/hepdata.44302.v1/t3
title: "Table 3" of "Diffractive dijet cross-sections in photoproduction at HERA"

description: Differential cross section as a function of invariant mass of the GAMMA P system.
description: DESY-HERA. Measurement of diffractive dijet differential cross sections in photoproduction events in which the hadronic final state containing the jets is separated with respect to the outgoing proton direction by a large rapidity gap. Jets are reconstructed using an iterative cone alogrithm in the eta-phi plane with a cone radius of 1.
DOI: 10.17182/hepdata.44302.v1/t4
title: "Table 4" of "Diffractive dijet cross-sections in photoproduction at HERA"

description: Differential cross section as a function of X_gamma=(ET(JET1)*EXP(-ETARAP( JET1)) + ET(JET2)*EXP(-ETARAP(JET2)))/ (2*Y*E), the fraction of the photon momentum carried by the highest E_t jets. E is the incident positron energy.
description: DESY-HERA. Measurement of diffractive dijet differential cross sections in photoproduction events in which the hadronic final state containing the jets is separated with respect to the outgoing proton direction by a large rapidity gap. Jets are reconstructed using an iterative cone alogrithm in the eta-phi plane with a cone radius of 1.
DOI: 10.17182/hepdata.44302.v1/t5
title: "Table 5" of "Diffractive dijet cross-sections in photoproduction at HERA"

description: Differential cross section as a function of BETA = (ET(JET1)*EXP(-ETARAP(J ET1)) + ET(JET2)*EXP(-ETARAP(JET2)))/ (2*XPOMERON*E_p), the fraction of the photon momentum carried by the highest E_t jets. E_p is the incident proton energy.
description: DESY-HERA. Measurement of diffractive dijet differential cross sections in photoproduction events in which the hadronic final state containing the jets is separated with respect to the outgoing proton direction by a large rapidity gap. Jets are reconstructed using an iterative cone alogrithm in the eta-phi plane with a cone radius of 1.
DOI: 10.17182/hepdata.44312.v1/t1
title: "Table 1" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in neutral-current DIS for jets with ET greater than 14 GeV in different etarap regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t2
title: "Table 2" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in neutral-current DIS for jets with ET greater than 14 GeV in different etarap regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t3
title: "Table 3" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in neutral-current DIS for jets with ET greater than 14 GeV in different etarap regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t4
title: "Table 4" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in neutral-current DIS for jets with ET greater than 14 GeV in different etarap regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t5
title: "Table 5" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in neutral-current DIS for jets in the etarap range -1 to 2 in different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t6
title: "Table 6" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in neutral-current DIS for jets in the etarap range -1 to 2 in different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t7
title: "Table 7" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in neutral-current DIS for jets in the etarap range -1 to 2 in different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t10
title: "Table 10" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: The measured integrated jet shape, corrected to the hadron level, in neutral-current DIS at a fixed value of R=0.5 as a function of the jet ET.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t11
title: "Table 11" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in charged-current DIS for jets in the etarap range -1 to 2 in different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t12
title: "Table 12" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in charged-current DIS for jets in the etarap range -1 to 2 in different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t8
title: "Table 8" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in neutral-current DIS for jets in the etarap range -1 to 2 in different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t9
title: "Table 9" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: The measured integrated jet shape, corrected to the hadron level, in neutral-current DIS at a fixed value of R=0.5 as a function of the jet rapidity.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t13
title: "Table 13" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in charged-current DIS for jets in the etarap range -1 to 2 in different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t14
title: "Table 14" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured differential jet shapes, corrected to the hadron level, in charged-current DIS for jets in the etarap range -1 to 2 in different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t15
title: "Table 15" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: The measured integrated jet shape, corrected to the hadron level, in charged-current DIS at a fixed value of R=0.5 as a function of the jet rapidity.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t16
title: "Table 16" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: The measured integrated jet shape, corrected to the hadron level, in charged-current DIS at a fixed value of R=0.5 as a function of the jet ET.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t17
title: "Table 17" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Comparison of the charged-current and neutral-current differential jet shapes for different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t18
title: "Table 18" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Comparison of the charged-current and neutral-current differential jet shapes for different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t19
title: "Table 19" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Comparison of the charged-current and neutral-current differential jet shapes for different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t20
title: "Table 20" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Comparison of the charged-current and neutral-current differential jet shapes for different ET regions.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t21
title: "Table 21" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: The measured integrated jet shape, corrected to the hadron level, in neutral-current DIS as a function of R.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t22
title: "Table 22" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Comparison of the differential jet shape with those from E+E- interactions obtained in a comparable data from OPAL (Alees et al. ZP C63 (94) 197).
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.
DOI: 10.17182/hepdata.44312.v1/t23
title: "Table 23" of "Measurement of jet shapes in high Q**2 deep inelastic scattering at HERA"

description: Measured integrated jet shapes, corrected to the hadron level, in neutral-current DIS as a function of R.
description: DESY-HERA. Measurement of the differential and integral high ET jet shapes in both neutral-current and charged-current DIS of positrons on protons at Q**2 & gt; 100 GeV. Jets are defined using an iterative cone algorithm in the etarap-phi planewith a cone radius R of 1. The differential jet shape, RHO(R) is defined as the average fraction of the jet& apos;s ET that lies inside an annulus in the etarap-phi plane of width DeltaR at radius R. In this analysis DeltaR = 0.1. The integrated jet shape PSI(R) is the average fraction of the jet& apos;s ET which lies inside a radius R. Numerical values supplied by M. Martinez.