cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.46761.v1/t14
title: "Table 14" of "Dijet photoproduction at HERA and the structure of the photon."

description: Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) &gt; 0.75 for:. -1 &lt; ETARAP(JET1) &lt; 0.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46761.v1/t15
title: "Table 15" of "Dijet photoproduction at HERA and the structure of the photon."

description: Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) &gt; 0.75 for:. 0 &lt; ETARAP(JET1) &lt; 1.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46761.v1/t16
title: "Table 16" of "Dijet photoproduction at HERA and the structure of the photon."

description: Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) &gt; 0.75 for:. 1 &lt; ETARAP(JET1) &lt; 2.4.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46761.v1/t17
title: "Table 17" of "Dijet photoproduction at HERA and the structure of the photon."

description: Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) &lt; 0.75 for:. -1 &lt; ETARAP(JET1) &lt; 0.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46761.v1/t18
title: "Table 18" of "Dijet photoproduction at HERA and the structure of the photon."

description: Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) &lt; 0.75 for:. 0 &lt; ETARAP(JET1) &lt; 1.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46761.v1/t19
title: "Table 19" of "Dijet photoproduction at HERA and the structure of the photon."

description: Measured cross section as a function of ETARAP(JET2) for X(C=GAMMA) &lt; 0.75 for:. 1 &lt; ETARAP(JET1) &lt; 2.4.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46761.v1/t20
title: "Table 20" of "Dijet photoproduction at HERA and the structure of the photon."

description: Measured cross section as a function of X(C=GAMMA) for:. 14 &lt; ET(JET1) &lt; 17 GEV.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46761.v1/t21
title: "Table 21" of "Dijet photoproduction at HERA and the structure of the photon."

description: Measured cross section as a function of X(C=GAMMA) for:. 17 &lt; ET(JET1) &lt; 25 GEV.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46761.v1/t22
title: "Table 22" of "Dijet photoproduction at HERA and the structure of the photon."

description: No description provided.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46761.v1/t23
title: "Table 23" of "Dijet photoproduction at HERA and the structure of the photon."

description: Measured cross section as a function of X(C=GAMMA) for:. 25 &lt; ET(JET1) &lt; 35 GEV.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46761.v1/t24
title: "Table 24" of "Dijet photoproduction at HERA and the structure of the photon."

description: Measured cross section as a function of X(C=GAMMA) for:. 35 &lt; ET(JET1) &lt; 90 GEV.
description: DESY-HERA. Measurement of the di-jet cross section in photoproduction data from collisions of 27.5 GeV positrons with 820 GeV protons. The data were taken during a dedicated run in 1996 and 1997 and have an integrated luminosity of 38.6 +- 0.6 pb-1. The variable X(C=GAMMA), is defined as:& lt;p& gt; X(C=GAMMA)=(ET(JET1)*EXP(-ETARAP(JET1)+ET(JET2)*EXP(-ETARAP(JET2))/2*Y*E_e where Y is the energy fraction of the radiated photon in the proton rest frame and E_e is the positron beamenergy. X(C=GAMMA) is the fractional momentum of the photon carried by the inte racting parton. The jets are defined so that ET(JET1) & gt; ET(JET2). In all the distributions, unless otherwise stated the following kinematical ranges apply:& lt;p& gt; 134 & lt; W_GAMMA-P & lt; 277 GeV& lt;br& gt; ET(JET1) & gt; 14 GeV& lt;br& gt; ET(JET2) & gt; 11 GeV& lt;br& gt; -1 & lt; ETRAP(JET1 and JET2) & lt; 2.4.
DOI: 10.17182/hepdata.46764.v1/t1
title: "Table 1" of "Measurement of dijet cross-sections in photoproduction at HERA"

description: Differential ep cross section for dijet production as a function of the invariant mass of the two jets.
description: DESY-HERA. Measurement of various jet observable cross sections in di-jet photopoduction events from collisions of 27.5 GeV positrons with 820 GeV protons at a centre-of-mass energy of 300 GeV. The data were collected during the 1995-97 HERA running period and have an integrated luminosity of 34.0 pb-1. Jets were selected using the inclusive minimunm kT algorithm with a minimum transverse energy of 25 GeV for the leading jet. The data cover the longitudinal proton momentum fraction (XP) range 0.05 to 0.6, and the photon longitudinal fraction (X(C=GAMMA)) range 0.1 to 1.
DOI: 10.17182/hepdata.46764.v1/t2
title: "Table 2" of "Measurement of dijet cross-sections in photoproduction at HERA"

description: Differential ep cross section for dijet production as a function of the average transverse energy the two jets.
description: DESY-HERA. Measurement of various jet observable cross sections in di-jet photopoduction events from collisions of 27.5 GeV positrons with 820 GeV protons at a centre-of-mass energy of 300 GeV. The data were collected during the 1995-97 HERA running period and have an integrated luminosity of 34.0 pb-1. Jets were selected using the inclusive minimunm kT algorithm with a minimum transverse energy of 25 GeV for the leading jet. The data cover the longitudinal proton momentum fraction (XP) range 0.05 to 0.6, and the photon longitudinal fraction (X(C=GAMMA)) range 0.1 to 1.
DOI: 10.17182/hepdata.46764.v1/t3
title: "Table 3" of "Measurement of dijet cross-sections in photoproduction at HERA"

description: Differential ep cross section for dijet production as a function of the maximum transverse energy the leading jet.
description: DESY-HERA. Measurement of various jet observable cross sections in di-jet photopoduction events from collisions of 27.5 GeV positrons with 820 GeV protons at a centre-of-mass energy of 300 GeV. The data were collected during the 1995-97 HERA running period and have an integrated luminosity of 34.0 pb-1. Jets were selected using the inclusive minimunm kT algorithm with a minimum transverse energy of 25 GeV for the leading jet. The data cover the longitudinal proton momentum fraction (XP) range 0.05 to 0.6, and the photon longitudinal fraction (X(C=GAMMA)) range 0.1 to 1.
DOI: 10.17182/hepdata.46764.v1/t4
title: "Table 4" of "Measurement of dijet cross-sections in photoproduction at HERA"

description: Differential ep cross section for dijet production as a function of the average pseudorapidity the two jets in two transverse energy regions and in the Y region 0.1 to 0.5.
description: DESY-HERA. Measurement of various jet observable cross sections in di-jet photopoduction events from collisions of 27.5 GeV positrons with 820 GeV protons at a centre-of-mass energy of 300 GeV. The data were collected during the 1995-97 HERA running period and have an integrated luminosity of 34.0 pb-1. Jets were selected using the inclusive minimunm kT algorithm with a minimum transverse energy of 25 GeV for the leading jet. The data cover the longitudinal proton momentum fraction (XP) range 0.05 to 0.6, and the photon longitudinal fraction (X(C=GAMMA)) range 0.1 to 1.
DOI: 10.17182/hepdata.46764.v1/t5
title: "Table 5" of "Measurement of dijet cross-sections in photoproduction at HERA"

description: Differential ep cross section for dijet production as a function of the average pseudorapidity the two jets in two transverse energy regions and in the Y region 0.5 to 0.9.
description: DESY-HERA. Measurement of various jet observable cross sections in di-jet photopoduction events from collisions of 27.5 GeV positrons with 820 GeV protons at a centre-of-mass energy of 300 GeV. The data were collected during the 1995-97 HERA running period and have an integrated luminosity of 34.0 pb-1. Jets were selected using the inclusive minimunm kT algorithm with a minimum transverse energy of 25 GeV for the leading jet. The data cover the longitudinal proton momentum fraction (XP) range 0.05 to 0.6, and the photon longitudinal fraction (X(C=GAMMA)) range 0.1 to 1.
DOI: 10.17182/hepdata.46764.v1/t6
title: "Table 6" of "Measurement of dijet cross-sections in photoproduction at HERA"

description: Differential ep cross section for dijet production as a function of the photon momentum fraction X(C=GAMMA) in two regions of proton fractional momentum XP.
description: DESY-HERA. Measurement of various jet observable cross sections in di-jet photopoduction events from collisions of 27.5 GeV positrons with 820 GeV protons at a centre-of-mass energy of 300 GeV. The data were collected during the 1995-97 HERA running period and have an integrated luminosity of 34.0 pb-1. Jets were selected using the inclusive minimunm kT algorithm with a minimum transverse energy of 25 GeV for the leading jet. The data cover the longitudinal proton momentum fraction (XP) range 0.05 to 0.6, and the photon longitudinal fraction (X(C=GAMMA)) range 0.1 to 1.
DOI: 10.17182/hepdata.46764.v1/t10
title: "Table 10" of "Measurement of dijet cross-sections in photoproduction at HERA"

description: Differential ep cross section for dijet production as a function of COS(THETA*) for dijet masses &gt; 65 GeV in two regions of fractional photon momentum fraction X(C=GAMMA).
description: DESY-HERA. Measurement of various jet observable cross sections in di-jet photopoduction events from collisions of 27.5 GeV positrons with 820 GeV protons at a centre-of-mass energy of 300 GeV. The data were collected during the 1995-97 HERA running period and have an integrated luminosity of 34.0 pb-1. Jets were selected using the inclusive minimunm kT algorithm with a minimum transverse energy of 25 GeV for the leading jet. The data cover the longitudinal proton momentum fraction (XP) range 0.05 to 0.6, and the photon longitudinal fraction (X(C=GAMMA)) range 0.1 to 1.
DOI: 10.17182/hepdata.46764.v1/t7
title: "Table 7" of "Measurement of dijet cross-sections in photoproduction at HERA"

description: Differential ep cross section for dijet production as a function of the proton momentum fraction XP in two regions of photon fractional momentum X(C=GAMMA).
description: DESY-HERA. Measurement of various jet observable cross sections in di-jet photopoduction events from collisions of 27.5 GeV positrons with 820 GeV protons at a centre-of-mass energy of 300 GeV. The data were collected during the 1995-97 HERA running period and have an integrated luminosity of 34.0 pb-1. Jets were selected using the inclusive minimunm kT algorithm with a minimum transverse energy of 25 GeV for the leading jet. The data cover the longitudinal proton momentum fraction (XP) range 0.05 to 0.6, and the photon longitudinal fraction (X(C=GAMMA)) range 0.1 to 1.
DOI: 10.17182/hepdata.46764.v1/t8
title: "Table 8" of "Measurement of dijet cross-sections in photoproduction at HERA"

description: Differential ep cross section for dijet production as a function of the photon momentum fraction X(C=GAMMA) in two regions maximum jet transverseenergy.
description: DESY-HERA. Measurement of various jet observable cross sections in di-jet photopoduction events from collisions of 27.5 GeV positrons with 820 GeV protons at a centre-of-mass energy of 300 GeV. The data were collected during the 1995-97 HERA running period and have an integrated luminosity of 34.0 pb-1. Jets were selected using the inclusive minimunm kT algorithm with a minimum transverse energy of 25 GeV for the leading jet. The data cover the longitudinal proton momentum fraction (XP) range 0.05 to 0.6, and the photon longitudinal fraction (X(C=GAMMA)) range 0.1 to 1.
DOI: 10.17182/hepdata.46764.v1/t9
title: "Table 9" of "Measurement of dijet cross-sections in photoproduction at HERA"

description: Differential ep cross section for dijet production as a function of COS(THETA*) in two regions of fractional photon momentum fraction X(C=GAMMA).
description: DESY-HERA. Measurement of various jet observable cross sections in di-jet photopoduction events from collisions of 27.5 GeV positrons with 820 GeV protons at a centre-of-mass energy of 300 GeV. The data were collected during the 1995-97 HERA running period and have an integrated luminosity of 34.0 pb-1. Jets were selected using the inclusive minimunm kT algorithm with a minimum transverse energy of 25 GeV for the leading jet. The data cover the longitudinal proton momentum fraction (XP) range 0.05 to 0.6, and the photon longitudinal fraction (X(C=GAMMA)) range 0.1 to 1.
DOI: 10.17182/hepdata.46767.v1/t1
title: "Table 1" of "D*+- meson production in deep-inelastic diffractive interactions at HERA."

description: The total D*+- production cross section for the given kinematic region. Also given is the ratio to the DIS*+- production cross section in the samekinematic region.
description: DESY-HERA. Measurement of the cross section for D*+- meson production in diffractive DIS of 27.5 GeV positrons on 820 GeV protons. The process ep --& gt; eXY, where the system X contains at least one charged D* and is seperated by a large rapidity gap from the low mass proton remnant, is studied. The data were collected over the years 1996 and 1997 with an integrated luminosity of 19.1 pb-1. Numerical values were supplied by P. Schleper.
DOI: 10.17182/hepdata.46767.v1/t2
title: "Table 2" of "D*+- meson production in deep-inelastic diffractive interactions at HERA."

description: Cross section as a function of X(NAME=POMERON).
description: DESY-HERA. Measurement of the cross section for D*+- meson production in diffractive DIS of 27.5 GeV positrons on 820 GeV protons. The process ep --& gt; eXY, where the system X contains at least one charged D* and is seperated by a large rapidity gap from the low mass proton remnant, is studied. The data were collected over the years 1996 and 1997 with an integrated luminosity of 19.1 pb-1. Numerical values were supplied by P. Schleper.
DOI: 10.17182/hepdata.46767.v1/t3
title: "Table 3" of "D*+- meson production in deep-inelastic diffractive interactions at HERA."

description: Cross section as a function of LOG10(BETA). BETA = X/X(NAME=POMERON).
description: DESY-HERA. Measurement of the cross section for D*+- meson production in diffractive DIS of 27.5 GeV positrons on 820 GeV protons. The process ep --& gt; eXY, where the system X contains at least one charged D* and is seperated by a large rapidity gap from the low mass proton remnant, is studied. The data were collected over the years 1996 and 1997 with an integrated luminosity of 19.1 pb-1. Numerical values were supplied by P. Schleper.
DOI: 10.17182/hepdata.46767.v1/t4
title: "Table 4" of "D*+- meson production in deep-inelastic diffractive interactions at HERA."

description: Cross section as a function of Z(NAME=POMERON,C=OBSERVED).
description: DESY-HERA. Measurement of the cross section for D*+- meson production in diffractive DIS of 27.5 GeV positrons on 820 GeV protons. The process ep --& gt; eXY, where the system X contains at least one charged D* and is seperated by a large rapidity gap from the low mass proton remnant, is studied. The data were collected over the years 1996 and 1997 with an integrated luminosity of 19.1 pb-1. Numerical values were supplied by P. Schleper.