cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.44430.v1/t10
title: "Table 10" of "Measurement of jet shapes in photoproduction at HERA"

description: Dijet production. Data in different pseudorapidity range.
description: DESY-HERA. Study of Jet Shapes produced in quasi-real photon-proton collisions at centre-of-mass energies in the range 134 to 227 GeV. Jets are identified using a cone alogrithm in the eta-phi plane with a cone radius of one unit. The jet shape parameter PSI(R) is defined as the average fraction of the jet& apos;s transverse energy (ET) that is within an inner cone of radius R concentric with the jet defining cone (R=1). Data are given for both inclusive jet production and dijet production with jets having ET & gt; 14 GeV. All data are corrected to the hadron level. Numerical values supplied by Claudia Glasman.
DOI: 10.17182/hepdata.44430.v1/t11
title: "Table 11" of "Measurement of jet shapes in photoproduction at HERA"

description: Dijet production. Data in different pseudorapidity range.
description: DESY-HERA. Study of Jet Shapes produced in quasi-real photon-proton collisions at centre-of-mass energies in the range 134 to 227 GeV. Jets are identified using a cone alogrithm in the eta-phi plane with a cone radius of one unit. The jet shape parameter PSI(R) is defined as the average fraction of the jet& apos;s transverse energy (ET) that is within an inner cone of radius R concentric with the jet defining cone (R=1). Data are given for both inclusive jet production and dijet production with jets having ET & gt; 14 GeV. All data are corrected to the hadron level. Numerical values supplied by Claudia Glasman.
DOI: 10.17182/hepdata.44430.v1/t5
title: "Table 5" of "Measurement of jet shapes in photoproduction at HERA"

description: Inclusive jet productions. Data in different pseudorapidity ranges.
description: DESY-HERA. Study of Jet Shapes produced in quasi-real photon-proton collisions at centre-of-mass energies in the range 134 to 227 GeV. Jets are identified using a cone alogrithm in the eta-phi plane with a cone radius of one unit. The jet shape parameter PSI(R) is defined as the average fraction of the jet& apos;s transverse energy (ET) that is within an inner cone of radius R concentric with the jet defining cone (R=1). Data are given for both inclusive jet production and dijet production with jets having ET & gt; 14 GeV. All data are corrected to the hadron level. Numerical values supplied by Claudia Glasman.
DOI: 10.17182/hepdata.44430.v1/t6
title: "Table 6" of "Measurement of jet shapes in photoproduction at HERA"

description: Inclusive jet productions. Data in different pseudorapidity ranges.
description: DESY-HERA. Study of Jet Shapes produced in quasi-real photon-proton collisions at centre-of-mass energies in the range 134 to 227 GeV. Jets are identified using a cone alogrithm in the eta-phi plane with a cone radius of one unit. The jet shape parameter PSI(R) is defined as the average fraction of the jet& apos;s transverse energy (ET) that is within an inner cone of radius R concentric with the jet defining cone (R=1). Data are given for both inclusive jet production and dijet production with jets having ET & gt; 14 GeV. All data are corrected to the hadron level. Numerical values supplied by Claudia Glasman.
DOI: 10.17182/hepdata.44430.v1/t7
title: "Table 7" of "Measurement of jet shapes in photoproduction at HERA"

description: Inclusive jet productions. Data in different pseudorapidity ranges.
description: DESY-HERA. Study of Jet Shapes produced in quasi-real photon-proton collisions at centre-of-mass energies in the range 134 to 227 GeV. Jets are identified using a cone alogrithm in the eta-phi plane with a cone radius of one unit. The jet shape parameter PSI(R) is defined as the average fraction of the jet& apos;s transverse energy (ET) that is within an inner cone of radius R concentric with the jet defining cone (R=1). Data are given for both inclusive jet production and dijet production with jets having ET & gt; 14 GeV. All data are corrected to the hadron level. Numerical values supplied by Claudia Glasman.
DOI: 10.17182/hepdata.44430.v1/t8
title: "Table 8" of "Measurement of jet shapes in photoproduction at HERA"

description: Inclusive jet productions. Data in different pseudorapidity ranges.
description: DESY-HERA. Study of Jet Shapes produced in quasi-real photon-proton collisions at centre-of-mass energies in the range 134 to 227 GeV. Jets are identified using a cone alogrithm in the eta-phi plane with a cone radius of one unit. The jet shape parameter PSI(R) is defined as the average fraction of the jet& apos;s transverse energy (ET) that is within an inner cone of radius R concentric with the jet defining cone (R=1). Data are given for both inclusive jet production and dijet production with jets having ET & gt; 14 GeV. All data are corrected to the hadron level. Numerical values supplied by Claudia Glasman.
DOI: 10.17182/hepdata.44430.v1/t9
title: "Table 9" of "Measurement of jet shapes in photoproduction at HERA"

description: Dijet production. Data in different pseudorapidity range.
description: DESY-HERA. Study of Jet Shapes produced in quasi-real photon-proton collisions at centre-of-mass energies in the range 134 to 227 GeV. Jets are identified using a cone alogrithm in the eta-phi plane with a cone radius of one unit. The jet shape parameter PSI(R) is defined as the average fraction of the jet& apos;s transverse energy (ET) that is within an inner cone of radius R concentric with the jet defining cone (R=1). Data are given for both inclusive jet production and dijet production with jets having ET & gt; 14 GeV. All data are corrected to the hadron level. Numerical values supplied by Claudia Glasman.
DOI: 10.17182/hepdata.44430.v1/t12
title: "Table 12" of "Measurement of jet shapes in photoproduction at HERA"

description: Dijet production. Data in different pseudorapidity range.
description: DESY-HERA. Study of Jet Shapes produced in quasi-real photon-proton collisions at centre-of-mass energies in the range 134 to 227 GeV. Jets are identified using a cone alogrithm in the eta-phi plane with a cone radius of one unit. The jet shape parameter PSI(R) is defined as the average fraction of the jet& apos;s transverse energy (ET) that is within an inner cone of radius R concentric with the jet defining cone (R=1). Data are given for both inclusive jet production and dijet production with jets having ET & gt; 14 GeV. All data are corrected to the hadron level. Numerical values supplied by Claudia Glasman.
DOI: 10.17182/hepdata.44430.v1/t13
title: "Table 13" of "Measurement of jet shapes in photoproduction at HERA"

description: Dijet production. Data seperated into two XOBS regions where XOBS represents the fraction of the photons momentum participating in the production of the two highest ET jets. Direct processes are concentrated at high XOBS and resolved at low XOBS.
description: DESY-HERA. Study of Jet Shapes produced in quasi-real photon-proton collisions at centre-of-mass energies in the range 134 to 227 GeV. Jets are identified using a cone alogrithm in the eta-phi plane with a cone radius of one unit. The jet shape parameter PSI(R) is defined as the average fraction of the jet& apos;s transverse energy (ET) that is within an inner cone of radius R concentric with the jet defining cone (R=1). Data are given for both inclusive jet production and dijet production with jets having ET & gt; 14 GeV. All data are corrected to the hadron level. Numerical values supplied by Claudia Glasman.
DOI: 10.17182/hepdata.44430.v1/t14
title: "Table 14" of "Measurement of jet shapes in photoproduction at HERA"

description: Dijet production. Data seperated into two XOBS regions where XOBS represents the fraction of the photons momentum participating in the production of the two highest ET jets. Direct processes are concentrated at high XOBS and resolved at low XOBS.
description: DESY-HERA. Study of Jet Shapes produced in quasi-real photon-proton collisions at centre-of-mass energies in the range 134 to 227 GeV. Jets are identified using a cone alogrithm in the eta-phi plane with a cone radius of one unit. The jet shape parameter PSI(R) is defined as the average fraction of the jet& apos;s transverse energy (ET) that is within an inner cone of radius R concentric with the jet defining cone (R=1). Data are given for both inclusive jet production and dijet production with jets having ET & gt; 14 GeV. All data are corrected to the hadron level. Numerical values supplied by Claudia Glasman.
DOI: 10.17182/hepdata.44431.v1/t1
title: "Table 1" of "Measurement of the diffractive structure function F2(D(4) ) at HERA"

description: The measured distribution of T, the squared momentum transfer to the virtual pluton.
description: DESY-HERA. Measurement of diffractive photon dissociation in Deep Inelastic positron-proton scattering in which the proton in the final state is detected and it& apos;s momentum measured, and is required to by & gt;97% of the incoming proton momentum. The data come from the interaction of 27.5 GeV positrons on 820 GeV protons taken during the 1994 running period and have an integrated luminosity of 900 +- 14 nb-1. The variable X(NAME=POMERON) is defined as (P-PRIME).q/P.q where P and PRIME are the 4 momenta of the incident and scattered position respectively and q is the negative 4 momentum transfer carried by the virtual photon. Numerical values of figure 7 supplied by Elisabetta Gallo.
DOI: 10.17182/hepdata.44431.v1/t2
title: "Table 2" of "Measurement of the diffractive structure function F2(D(4) ) at HERA"

description: Slope of the T distribution.
description: DESY-HERA. Measurement of diffractive photon dissociation in Deep Inelastic positron-proton scattering in which the proton in the final state is detected and it& apos;s momentum measured, and is required to by & gt;97% of the incoming proton momentum. The data come from the interaction of 27.5 GeV positrons on 820 GeV protons taken during the 1994 running period and have an integrated luminosity of 900 +- 14 nb-1. The variable X(NAME=POMERON) is defined as (P-PRIME).q/P.q where P and PRIME are the 4 momenta of the incident and scattered position respectively and q is the negative 4 momentum transfer carried by the virtual photon. Numerical values of figure 7 supplied by Elisabetta Gallo.
DOI: 10.17182/hepdata.44431.v1/t3
title: "Table 3" of "Measurement of the diffractive structure function F2(D(4) ) at HERA"

description: The structure function F2(NAME=D4).
description: DESY-HERA. Measurement of diffractive photon dissociation in Deep Inelastic positron-proton scattering in which the proton in the final state is detected and it& apos;s momentum measured, and is required to by & gt;97% of the incoming proton momentum. The data come from the interaction of 27.5 GeV positrons on 820 GeV protons taken during the 1994 running period and have an integrated luminosity of 900 +- 14 nb-1. The variable X(NAME=POMERON) is defined as (P-PRIME).q/P.q where P and PRIME are the 4 momenta of the incident and scattered position respectively and q is the negative 4 momentum transfer carried by the virtual photon. Numerical values of figure 7 supplied by Elisabetta Gallo.
DOI: 10.17182/hepdata.44431.v1/t4
title: "Table 4" of "Measurement of the diffractive structure function F2(D(4) ) at HERA"

description: The structure function F2(NAME=D3).
description: DESY-HERA. Measurement of diffractive photon dissociation in Deep Inelastic positron-proton scattering in which the proton in the final state is detected and it& apos;s momentum measured, and is required to by & gt;97% of the incoming proton momentum. The data come from the interaction of 27.5 GeV positrons on 820 GeV protons taken during the 1994 running period and have an integrated luminosity of 900 +- 14 nb-1. The variable X(NAME=POMERON) is defined as (P-PRIME).q/P.q where P and PRIME are the 4 momenta of the incident and scattered position respectively and q is the negative 4 momentum transfer carried by the virtual photon. Numerical values of figure 7 supplied by Elisabetta Gallo.
DOI: 10.17182/hepdata.44434.v1/t1
title: "Table 1" of "Photo-production of psi(2S) mesons at HERA."

description: Overall value for photoproduction cross section combining the different decay modes and data sample.. 1994 and 1995 data.. The second systematic error is from the branching ratio uncertainties.
description: H1 Collaboration. Study of Quasi-Elastic Photoproduction of PSI(2S) mesons at the photon-proton centre-of-mass energies 40 to 160 GeV. Quasi-elastic is defined as the kinematical region z& gt;0.95, where z=E(psi(2s))/E(gamma) in the rest frame of the proton. Uncertainties due to the imprecisely known branching ratios of the PSI(2S)decays are not included.
DOI: 10.17182/hepdata.44434.v1/t2
title: "Table 2" of "Photo-production of psi(2S) mesons at HERA."

description: Combined cross section from PSI(3685) --&gt; J/PSI(1S) &lt; E+ E- &gt; PI+ PI- and PSI(3685) --&gt; J/PSI(1S) &lt; MU+ MU- &gt; PI+ PI- modes using both the 1994 and 1995 data.. The second systematic error is from the branching ratio uncertainties.
description: H1 Collaboration. Study of Quasi-Elastic Photoproduction of PSI(2S) mesons at the photon-proton centre-of-mass energies 40 to 160 GeV. Quasi-elastic is defined as the kinematical region z& gt;0.95, where z=E(psi(2s))/E(gamma) in the rest frame of the proton. Uncertainties due to the imprecisely known branching ratios of the PSI(2S)decays are not included.
DOI: 10.17182/hepdata.44434.v1/t3
title: "Table 3" of "Photo-production of psi(2S) mesons at HERA."

description: Cross section from PSI(3685) --&gt; J/PSI(1S) &lt; E+ E- &gt; PI+ PI- mode.
description: H1 Collaboration. Study of Quasi-Elastic Photoproduction of PSI(2S) mesons at the photon-proton centre-of-mass energies 40 to 160 GeV. Quasi-elastic is defined as the kinematical region z& gt;0.95, where z=E(psi(2s))/E(gamma) in the rest frame of the proton. Uncertainties due to the imprecisely known branching ratios of the PSI(2S)decays are not included.
DOI: 10.17182/hepdata.44434.v1/t4
title: "Table 4" of "Photo-production of psi(2S) mesons at HERA."

description: Cross section from PSI(3685) --&gt; J/PSI(1S) &lt; MU+ MU- &gt; PI+ PI- mode.
description: H1 Collaboration. Study of Quasi-Elastic Photoproduction of PSI(2S) mesons at the photon-proton centre-of-mass energies 40 to 160 GeV. Quasi-elastic is defined as the kinematical region z& gt;0.95, where z=E(psi(2s))/E(gamma) in the rest frame of the proton. Uncertainties due to the imprecisely known branching ratios of the PSI(2S)decays are not included.
DOI: 10.17182/hepdata.44434.v1/t5
title: "Table 5" of "Photo-production of psi(2S) mesons at HERA."

description: Cross section from PSI(3685) --&gt; E+ E- + MU+ MU- mode.
description: H1 Collaboration. Study of Quasi-Elastic Photoproduction of PSI(2S) mesons at the photon-proton centre-of-mass energies 40 to 160 GeV. Quasi-elastic is defined as the kinematical region z& gt;0.95, where z=E(psi(2s))/E(gamma) in the rest frame of the proton. Uncertainties due to the imprecisely known branching ratios of the PSI(2S)decays are not included.
DOI: 10.17182/hepdata.44434.v1/t6
title: "Table 6" of "Photo-production of psi(2S) mesons at HERA."

description: Cross section from PSI(3685) --&gt; J/PSI(1S) &lt; E+ E- &gt; PI+ PI- mode.
description: H1 Collaboration. Study of Quasi-Elastic Photoproduction of PSI(2S) mesons at the photon-proton centre-of-mass energies 40 to 160 GeV. Quasi-elastic is defined as the kinematical region z& gt;0.95, where z=E(psi(2s))/E(gamma) in the rest frame of the proton. Uncertainties due to the imprecisely known branching ratios of the PSI(2S)decays are not included.
DOI: 10.17182/hepdata.44434.v1/t7
title: "Table 7" of "Photo-production of psi(2S) mesons at HERA."

description: Cross section from PSI(3685) --&gt; J/PSI(1S) &lt; MU+ MU- &gt; PI+ PI- mode.
description: H1 Collaboration. Study of Quasi-Elastic Photoproduction of PSI(2S) mesons at the photon-proton centre-of-mass energies 40 to 160 GeV. Quasi-elastic is defined as the kinematical region z& gt;0.95, where z=E(psi(2s))/E(gamma) in the rest frame of the proton. Uncertainties due to the imprecisely known branching ratios of the PSI(2S)decays are not included.
DOI: 10.17182/hepdata.44434.v1/t8
title: "Table 8" of "Photo-production of psi(2S) mesons at HERA."

description: Cross section from PSI(3685) --&gt; E+ E- + MU+ MU- mode.
description: H1 Collaboration. Study of Quasi-Elastic Photoproduction of PSI(2S) mesons at the photon-proton centre-of-mass energies 40 to 160 GeV. Quasi-elastic is defined as the kinematical region z& gt;0.95, where z=E(psi(2s))/E(gamma) in the rest frame of the proton. Uncertainties due to the imprecisely known branching ratios of the PSI(2S)decays are not included.
DOI: 10.17182/hepdata.44434.v1/t9
title: "Table 9" of "Photo-production of psi(2S) mesons at HERA."

description: Second systematic error is due to uncertainties in the PSI(2S) partial widths. J/PSI cross section 119.5+-11.2+-12.0 nb is from NP B472, 3. Extrapolation to Q2=0.
description: H1 Collaboration. Study of Quasi-Elastic Photoproduction of PSI(2S) mesons at the photon-proton centre-of-mass energies 40 to 160 GeV. Quasi-elastic is defined as the kinematical region z& gt;0.95, where z=E(psi(2s))/E(gamma) in the rest frame of the proton. Uncertainties due to the imprecisely known branching ratios of the PSI(2S)decays are not included.
DOI: 10.17182/hepdata.44498.v1/t1
title: "Table 1" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The ET differential jet cross section in the virtual-photon CM frame.
description: DESY-HERA. Measurement of the differential inclusive jet cross sections w.r.t the Transverse Energy (ET) and Psuedorapidity (TARAP) in the virtual photon-proton centre-of-mass frame in positron-proton collisions in the Q**2 range 0 to 49 GeV**2 and y range 0.3 to 0.6. The data come from the 1994 and 195 running periods.. The numerical values of figures 3 and 4, the gamma*-p cross sections, havebeen calculated from the data in table 2 combined with the Flux factors in the differents Q**2 ranges which are tabulated in the paper.
DOI: 10.17182/hepdata.44498.v1/t2
title: "Table 2" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The ET differential jet cross section in the virtual-photon CM frame.
description: DESY-HERA. Measurement of the differential inclusive jet cross sections w.r.t the Transverse Energy (ET) and Psuedorapidity (TARAP) in the virtual photon-proton centre-of-mass frame in positron-proton collisions in the Q**2 range 0 to 49 GeV**2 and y range 0.3 to 0.6. The data come from the 1994 and 195 running periods.. The numerical values of figures 3 and 4, the gamma*-p cross sections, havebeen calculated from the data in table 2 combined with the Flux factors in the differents Q**2 ranges which are tabulated in the paper.
DOI: 10.17182/hepdata.44498.v1/t3
title: "Table 3" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The ET differential jet cross section in the virtual-photon CM frame.
description: DESY-HERA. Measurement of the differential inclusive jet cross sections w.r.t the Transverse Energy (ET) and Psuedorapidity (TARAP) in the virtual photon-proton centre-of-mass frame in positron-proton collisions in the Q**2 range 0 to 49 GeV**2 and y range 0.3 to 0.6. The data come from the 1994 and 195 running periods.. The numerical values of figures 3 and 4, the gamma*-p cross sections, havebeen calculated from the data in table 2 combined with the Flux factors in the differents Q**2 ranges which are tabulated in the paper.
DOI: 10.17182/hepdata.44498.v1/t4
title: "Table 4" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The ET differential jet cross section in the virtual-photon CM frame.
description: DESY-HERA. Measurement of the differential inclusive jet cross sections w.r.t the Transverse Energy (ET) and Psuedorapidity (TARAP) in the virtual photon-proton centre-of-mass frame in positron-proton collisions in the Q**2 range 0 to 49 GeV**2 and y range 0.3 to 0.6. The data come from the 1994 and 195 running periods.. The numerical values of figures 3 and 4, the gamma*-p cross sections, havebeen calculated from the data in table 2 combined with the Flux factors in the differents Q**2 ranges which are tabulated in the paper.
DOI: 10.17182/hepdata.44498.v1/t5
title: "Table 5" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The ET differential jet cross section in the virtual-photon CM frame.
description: DESY-HERA. Measurement of the differential inclusive jet cross sections w.r.t the Transverse Energy (ET) and Psuedorapidity (TARAP) in the virtual photon-proton centre-of-mass frame in positron-proton collisions in the Q**2 range 0 to 49 GeV**2 and y range 0.3 to 0.6. The data come from the 1994 and 195 running periods.. The numerical values of figures 3 and 4, the gamma*-p cross sections, havebeen calculated from the data in table 2 combined with the Flux factors in the differents Q**2 ranges which are tabulated in the paper.
DOI: 10.17182/hepdata.44498.v1/t6
title: "Table 6" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The ET differential jet cross section in the virtual-photon CM frame.
description: DESY-HERA. Measurement of the differential inclusive jet cross sections w.r.t the Transverse Energy (ET) and Psuedorapidity (TARAP) in the virtual photon-proton centre-of-mass frame in positron-proton collisions in the Q**2 range 0 to 49 GeV**2 and y range 0.3 to 0.6. The data come from the 1994 and 195 running periods.. The numerical values of figures 3 and 4, the gamma*-p cross sections, havebeen calculated from the data in table 2 combined with the Flux factors in the differents Q**2 ranges which are tabulated in the paper.
DOI: 10.17182/hepdata.44498.v1/t10
title: "Table 10" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The ETARAP differential jet cross section in the virtual-photon CM frame.
description: DESY-HERA. Measurement of the differential inclusive jet cross sections w.r.t the Transverse Energy (ET) and Psuedorapidity (TARAP) in the virtual photon-proton centre-of-mass frame in positron-proton collisions in the Q**2 range 0 to 49 GeV**2 and y range 0.3 to 0.6. The data come from the 1994 and 195 running periods.. The numerical values of figures 3 and 4, the gamma*-p cross sections, havebeen calculated from the data in table 2 combined with the Flux factors in the differents Q**2 ranges which are tabulated in the paper.
DOI: 10.17182/hepdata.44498.v1/t11
title: "Table 11" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The ETARAP differential jet cross section in the virtual-photon CM frame.
description: DESY-HERA. Measurement of the differential inclusive jet cross sections w.r.t the Transverse Energy (ET) and Psuedorapidity (TARAP) in the virtual photon-proton centre-of-mass frame in positron-proton collisions in the Q**2 range 0 to 49 GeV**2 and y range 0.3 to 0.6. The data come from the 1994 and 195 running periods.. The numerical values of figures 3 and 4, the gamma*-p cross sections, havebeen calculated from the data in table 2 combined with the Flux factors in the differents Q**2 ranges which are tabulated in the paper.
DOI: 10.17182/hepdata.44498.v1/t12
title: "Table 12" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The ETARAP differential jet cross section in the virtual-photon CM frame.
description: DESY-HERA. Measurement of the differential inclusive jet cross sections w.r.t the Transverse Energy (ET) and Psuedorapidity (TARAP) in the virtual photon-proton centre-of-mass frame in positron-proton collisions in the Q**2 range 0 to 49 GeV**2 and y range 0.3 to 0.6. The data come from the 1994 and 195 running periods.. The numerical values of figures 3 and 4, the gamma*-p cross sections, havebeen calculated from the data in table 2 combined with the Flux factors in the differents Q**2 ranges which are tabulated in the paper.