cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.43992.v1/t5
title: "Table 5" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the full x(gamma) range as a function of the ET of the leading jet.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t6
title: "Table 6" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the full x(gamma) range as a function of the ET of the leading jet.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t10
title: "Table 10" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the ET of the leading jet.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t7
title: "Table 7" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the ET of the leading jet.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t8
title: "Table 8" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the ET of the leading jet.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t9
title: "Table 9" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the ET of the leading jet.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.5281/zenodo.17523554
title: Empirical Test — Law of Existence (Triadic Balance MNIST) v1.0 — Result: balance confirmed within empirical benchmark (dB + dC + dR ≈ 0)

description: We report an empirical test of the Law of Existence: during active learning, normalized changes in Persistence (dB), Coherence (dC), and Responsiveness (dR) sum to near zero.

Using the MNIST benchmark under fixed architecture and optimizer, windowed bootstrap analysis shows dB + dC + dR ≈ 0 within ±0.05 CI in dynamic segments, while equilibrium and shuffled controls deviate significantly.

This confirms the triadic balance predicted by the Grammar of Existence, linking structural, relational, and response dynamics into a conserved transformation capacity.
DOI: 10.5281/zenodo.17523555
title: Empirical Test — Law of Existence (Triadic Balance MNIST) v1.0 — Result: balance confirmed within empirical benchmark (dB + dC + dR ≈ 0)

description: We report an empirical test of the Law of Existence: during active learning, normalized changes in Persistence (dB), Coherence (dC), and Responsiveness (dR) sum to near zero.

Using the MNIST benchmark under fixed architecture and optimizer, windowed bootstrap analysis shows dB + dC + dR ≈ 0 within ±0.05 CI in dynamic segments, while equilibrium and shuffled controls deviate significantly.

This confirms the triadic balance predicted by the Grammar of Existence, linking structural, relational, and response dynamics into a conserved transformation capacity.
DOI: 10.17182/hepdata.43992.v1/t11
title: "Table 11" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the ET of the leading jet.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t12
title: "Table 12" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the ET of the leading jet.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t13
title: "Table 13" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t14
title: "Table 14" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t15
title: "Table 15" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t17
title: "Table 17" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the pseudorapidity of the jet with the other jet fixed.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t18
title: "Table 18" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the pseudorapidity of the jet with the other jet fixed.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t16
title: "Table 16" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the pseudorapidity of the jet with the other jet fixed.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t19
title: "Table 19" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t21
title: "Table 21" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t22
title: "Table 22" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t24
title: "Table 24" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.44039.v1/t1
title: "Table 1" of "Charmonium production in deep inelastic scattering at HERA"

description: Cross section for elastic J/PSI photoproduction in W bins.
description: DESY-HERA. Measurement of charmonium production (J/PSI and PSI(2s)) in elastic, quasi-elastic and inclusive reactions at Q**2 for 2 to 80 GeV**2 and photon-proton CM energy (W) 25 to 180 GeV. The data come from the 1995 to 1997 runningperiods with a total integrated luminosity of 27.3 +- 0.4 PB-1, with 27.5 GeV p ositrons interacting with 820 GeV protons.
DOI: 10.17182/hepdata.43992.v1/t2
title: "Table 2" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the full x(gamma) range as a function of the ET of the leading jet.
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t20
title: "Table 20" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the full x(gamma) range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.
DOI: 10.17182/hepdata.43992.v1/t23
title: "Table 23" of "Measurement of Dijet photoproduction at high transverse energies at HERA"

description: The dijet cross section for the x(gamma)&gt;0.75 range as a function of the pseudorapidity of the jet with the other jet fixed. This data is for a restricted range of y, (W = 212 to 277 GeV).
description: DESY-HERA. Measurement of the cross sections for the photoproduction of dijets at high transverse energies produced in the collisions of 27.5 GeV positrons on 820 GeV protons. The data come from a sample with integrated luminosity 6.3 pb-1. Jets are defined by applying a KT-clustering algorithm to the final state hadrons. The variable X(C=GAMMA) is the fractional longitudinal momentum of the photon participating in the production of the two highest ET jets. The cross section is measured as a function of three variables ET(Leading Jet), ET(Jet1) and ET(Jet2). Every event counts twice to the cross section corresponding to each respectively being the leading jet. In the following table the second systematic (DSYS) error is due to the uncertainty in the energy scale.