cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.45255.v1/t1
title: "Table 1" of "Measurement of inclusive photoproduction at 3.2 gev and comparison with electroproduction"

description: No description provided.
description: DESY accelerator.
DOI: 10.17182/hepdata.45255.v1/t2
title: "Table 2" of "Measurement of inclusive photoproduction at 3.2 gev and comparison with electroproduction"

description: No description provided.
description: DESY accelerator.
DOI: 10.17182/hepdata.45255.v1/t3
title: "Table 3" of "Measurement of inclusive photoproduction at 3.2 gev and comparison with electroproduction"

description: No description provided.
description: DESY accelerator.
DOI: 10.17182/hepdata.45260.v1/t1
title: "Table 1" of "Evidence of $W\gamma\gamma$ production in $pp$ collisions at $\sqrt{s}=8$ TeV and limits on anomalous quartic gauge couplings with the ATLAS detector"

description: The measured inclusive ($N_{jet}\geq$ 0) fiducial cross section in the e$\nu\gamma\gamma$, $\mu\nu\gamma\gamma$ channels together with the combined $\ell\nu\gamma\gamma$ cross section. The first uncertainty shown is the statistical uncertainty on the measurement, the second one is the total systematic uncertainty (excluding the term coming from the luminosity), the third one is the systematic uncertainty coming from the luminosity. A parton to particle correction factors of 0.99 is applied to the MCFM prediction.
description: CERN-LHC. Measurements of the cross section for W$\gamma\gamma$ production using the $\ell\nu\gamma\gamma$ decay channels in proton-proton collisions at a center-of-mass energy of 8 TeV with 20.3 fb$^{-1}$ of data collected in 2012. The final states used are a muon or an electron and two photons and missing transverse momentum (MET). In each final state, the inclusive and exclusive cross sections are measured. The inclusive measurement selection does not include any requirement on the number of jets, while the exclusive measurement requires that no jet is found in the event. 

The fiducial region is defined as (Table 2 of the preprint):
- p$_T^{\ell}$ &gt; 20 GeV;
- p$_T^{\nu}$ &gt; 25 GeV;
- |$\eta^{\ell}$| &lt; 2.5;
- m$_T^{W}$ &gt; 40 GeV;
- p$_T^{\gamma}$ &gt; 20 GeV (applied to both photons);
- |$\eta^{\gamma}$| &lt; 2.37 (applied to both photons);
- Photons isolation fraction, $\epsilon^p_h$ &lt; 0.5;
- Exclusive: no anti-k$_t$ jets with p$_T^{jet}$ &gt; 30 GeV and |$\eta^{jet}$| &lt; 4.4;
- $\Delta R$($\ell$,$\gamma$) &gt; 0.7, $\Delta R$($\gamma$,$\gamma$) &gt; 0.4 and $\Delta R$($\ell$ or $\gamma$, jet) &gt; 0.3.
DOI: 10.17182/hepdata.45260.v1/t2
title: "Table 2" of "Evidence of $W\gamma\gamma$ production in $pp$ collisions at $\sqrt{s}=8$ TeV and limits on anomalous quartic gauge couplings with the ATLAS detector"

description: The measured exclusive ($N_{jet}$ = 0) fiducial cross section in the e$\nu\gamma\gamma$, $\mu\nu\gamma\gamma$ channels together with the combined $\ell\nu\gamma\gamma$ cross section. The first uncertainty shown is the statistical uncertainty on the measurement, the second one is the total systematic uncertainty (excluding the term coming from the luminosity), the third one is the systematic uncertainty coming from the luminosity. A parton to particle correction factor of 0.87 is applied to the MCFM prediction.
description: CERN-LHC. Measurements of the cross section for W$\gamma\gamma$ production using the $\ell\nu\gamma\gamma$ decay channels in proton-proton collisions at a center-of-mass energy of 8 TeV with 20.3 fb$^{-1}$ of data collected in 2012. The final states used are a muon or an electron and two photons and missing transverse momentum (MET). In each final state, the inclusive and exclusive cross sections are measured. The inclusive measurement selection does not include any requirement on the number of jets, while the exclusive measurement requires that no jet is found in the event. 

The fiducial region is defined as (Table 2 of the preprint):
- p$_T^{\ell}$ &gt; 20 GeV;
- p$_T^{\nu}$ &gt; 25 GeV;
- |$\eta^{\ell}$| &lt; 2.5;
- m$_T^{W}$ &gt; 40 GeV;
- p$_T^{\gamma}$ &gt; 20 GeV (applied to both photons);
- |$\eta^{\gamma}$| &lt; 2.37 (applied to both photons);
- Photons isolation fraction, $\epsilon^p_h$ &lt; 0.5;
- Exclusive: no anti-k$_t$ jets with p$_T^{jet}$ &gt; 30 GeV and |$\eta^{jet}$| &lt; 4.4;
- $\Delta R$($\ell$,$\gamma$) &gt; 0.7, $\Delta R$($\gamma$,$\gamma$) &gt; 0.4 and $\Delta R$($\ell$ or $\gamma$, jet) &gt; 0.3.
DOI: 10.17182/hepdata.45260.v1/t3
title: "Table 3" of "Evidence of $W\gamma\gamma$ production in $pp$ collisions at $\sqrt{s}=8$ TeV and limits on anomalous quartic gauge couplings with the ATLAS detector"

description: Observed and expected 95\% CL limits obtained for the $f_{\mathrm{T0}}/\Lambda^4$, $f_{\mathrm{M2}}/\Lambda^4$ and $f_{\mathrm{M3}}/\Lambda^4$ aQGC parameters for the combination of the two channels. The values of $n = 0,\,1,\,2$ are the exponential choices of the form factor, $\Lambda_{\rm{FF}}$ is fixed to $600$ GeV for $f_{\mathrm{T0}}/\Lambda^4$ and to $500$ GeV for the other parameters. The $n=0$ choice produces the limits without the form factor applied.
description: CERN-LHC. Measurements of the cross section for W$\gamma\gamma$ production using the $\ell\nu\gamma\gamma$ decay channels in proton-proton collisions at a center-of-mass energy of 8 TeV with 20.3 fb$^{-1}$ of data collected in 2012. The final states used are a muon or an electron and two photons and missing transverse momentum (MET). In each final state, the inclusive and exclusive cross sections are measured. The inclusive measurement selection does not include any requirement on the number of jets, while the exclusive measurement requires that no jet is found in the event. 

The fiducial region is defined as (Table 2 of the preprint):
- p$_T^{\ell}$ &gt; 20 GeV;
- p$_T^{\nu}$ &gt; 25 GeV;
- |$\eta^{\ell}$| &lt; 2.5;
- m$_T^{W}$ &gt; 40 GeV;
- p$_T^{\gamma}$ &gt; 20 GeV (applied to both photons);
- |$\eta^{\gamma}$| &lt; 2.37 (applied to both photons);
- Photons isolation fraction, $\epsilon^p_h$ &lt; 0.5;
- Exclusive: no anti-k$_t$ jets with p$_T^{jet}$ &gt; 30 GeV and |$\eta^{jet}$| &lt; 4.4;
- $\Delta R$($\ell$,$\gamma$) &gt; 0.7, $\Delta R$($\gamma$,$\gamma$) &gt; 0.4 and $\Delta R$($\ell$ or $\gamma$, jet) &gt; 0.3.
DOI: 10.17182/hepdata.45279.v1/t1
title: "Table 1" of "Electroproduction of pions near the $\Delta(1236)$ isobar and the form-factor $G^*_M(q^2)$ of the $({\gamma} N\Delta)$ vertex"

description: Axis error includes +- 0.0/0.0 contribution.
description: DESY. Electroproduction of pions near the DELTA(1236P3) isobar and the fromfactor GM(q^2) of the (GAMMA NUCLEON DELTA ) vertex.
DOI: 10.17182/hepdata.45281.v1/t2
title: "Table 2" of "Inelastic electron - proton scattering at fixed four momentum transfer of 0.773-GeV/c**2 and 1.935-GeV/c**2"

description: No description provided.
description: No description provided.
DOI: 10.17182/hepdata.45281.v1/t3
title: "Table 3" of "Inelastic electron - proton scattering at fixed four momentum transfer of 0.773-GeV/c**2 and 1.935-GeV/c**2"

description: No description provided.
description: No description provided.
DOI: 10.17182/hepdata.45282.v1/t1
title: "Table 1" of "Neutron form-factors from quasielastic e d scattering"

description: Axis error includes +- 0.0/0.0 contribution (Due to the different effective solid angles for neutron and proton detection in the counters).
description: DESY. Neutron form factors from quasi-elastic E- DEUT scattering.
DOI: 10.17182/hepdata.45282.v1/t2
title: "Table 2" of "Neutron form-factors from quasielastic e d scattering"

description: No description provided.
description: DESY. Neutron form factors from quasi-elastic E- DEUT scattering.
DOI: 10.15468/dl.mphf68
title: Occurrence Download

description: A dataset containing 4361727 species occurrences available in GBIF matching the query:
{
 "and" : [
 "TaxonKey is one of (Acanella arbuscula, Antipathella subpinnata, Antipathes dichotoma, Callogorgia verticillata, Corallium johnsoni, Corallium rubrum, Dendrophyllia cornigera, Dendrophyllia ramea, Desmophyllum dianthus, Desmophyllum pertusum, Enallopsammia rostrata, Isidella elongata, Keratoisis, Leiopathes glaberrima, Madrepora oculata, Paragorgia arborea, Paramuricea placomus, Primnoa resedaeformis, Solenosmilia variabilis, Stichopathes, Viminella flagellum)",
 "HasCoordinate is true",
 "Geometry POLYGON((-40 36, 15 36, 15 72, -40 72, -40 36))"
 ]
}

 The dataset includes 4361727 records from 92 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015106-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.45283.v1/t1
title: "Table 1" of "Angular correlations in three-jet events in ep collisions at HERA"

description: Integrated 3-jet photoproduction cross section.
description: DESY-HERA. Measurement of the cross sections and angular correlations in 3-jet production in photoproduction and NC DIS events at centre of mass energies 300 and 318 GeV. The data were collected during the 1995 to 2000 HERA running period with a total integrated luminosity of 127 pb-1 with both E+P and E- P collisions.. The definition of the angular correlation variables are:-. THETA(C=H), the angle between the plane determined by the highest ET jet and the beam and the plane determined by the two jets with lowest ET.. ALPHA(C=23), the angle between the lowest ET jets.. BETA(C=KSW), based on the Korner-Schierholz-Willrodt angle in 4 jets (see text of article).. GAMMA(C=H), angle of the scattered quark in the quark parton model.
DOI: 10.17182/hepdata.45281.v1/t1
title: "Table 1" of "Inelastic electron - proton scattering at fixed four momentum transfer of 0.773-GeV/c**2 and 1.935-GeV/c**2"

description: No description provided.
description: No description provided.
DOI: 10.17182/hepdata.45281.v1/t4
title: "Table 4" of "Inelastic electron - proton scattering at fixed four momentum transfer of 0.773-GeV/c**2 and 1.935-GeV/c**2"

description: No description provided.
description: No description provided.
DOI: 10.17182/hepdata.45283.v1/t2
title: "Table 2" of "Angular correlations in three-jet events in ep collisions at HERA"

description: Integrated 3-jet cross sections in NC DIS.
description: DESY-HERA. Measurement of the cross sections and angular correlations in 3-jet production in photoproduction and NC DIS events at centre of mass energies 300 and 318 GeV. The data were collected during the 1995 to 2000 HERA running period with a total integrated luminosity of 127 pb-1 with both E+P and E- P collisions.. The definition of the angular correlation variables are:-. THETA(C=H), the angle between the plane determined by the highest ET jet and the beam and the plane determined by the two jets with lowest ET.. ALPHA(C=23), the angle between the lowest ET jets.. BETA(C=KSW), based on the Korner-Schierholz-Willrodt angle in 4 jets (see text of article).. GAMMA(C=H), angle of the scattered quark in the quark parton model.
DOI: 10.17182/hepdata.45283.v1/t3
title: "Table 3" of "Angular correlations in three-jet events in ep collisions at HERA"

description: Normalized differential 3-jet photoproduction cross section as a function of THETA(H).
description: DESY-HERA. Measurement of the cross sections and angular correlations in 3-jet production in photoproduction and NC DIS events at centre of mass energies 300 and 318 GeV. The data were collected during the 1995 to 2000 HERA running period with a total integrated luminosity of 127 pb-1 with both E+P and E- P collisions.. The definition of the angular correlation variables are:-. THETA(C=H), the angle between the plane determined by the highest ET jet and the beam and the plane determined by the two jets with lowest ET.. ALPHA(C=23), the angle between the lowest ET jets.. BETA(C=KSW), based on the Korner-Schierholz-Willrodt angle in 4 jets (see text of article).. GAMMA(C=H), angle of the scattered quark in the quark parton model.
DOI: 10.17182/hepdata.45283.v1/t4
title: "Table 4" of "Angular correlations in three-jet events in ep collisions at HERA"

description: Normalized differential 3-jet photoproduction cross section as a function of COS(ALPHA(23)).
description: DESY-HERA. Measurement of the cross sections and angular correlations in 3-jet production in photoproduction and NC DIS events at centre of mass energies 300 and 318 GeV. The data were collected during the 1995 to 2000 HERA running period with a total integrated luminosity of 127 pb-1 with both E+P and E- P collisions.. The definition of the angular correlation variables are:-. THETA(C=H), the angle between the plane determined by the highest ET jet and the beam and the plane determined by the two jets with lowest ET.. ALPHA(C=23), the angle between the lowest ET jets.. BETA(C=KSW), based on the Korner-Schierholz-Willrodt angle in 4 jets (see text of article).. GAMMA(C=H), angle of the scattered quark in the quark parton model.
DOI: 10.17182/hepdata.45283.v1/t5
title: "Table 5" of "Angular correlations in three-jet events in ep collisions at HERA"

description: Normalized differential 3-jet photoproduction cross section as a function of COS(BETA(KSW)).
description: DESY-HERA. Measurement of the cross sections and angular correlations in 3-jet production in photoproduction and NC DIS events at centre of mass energies 300 and 318 GeV. The data were collected during the 1995 to 2000 HERA running period with a total integrated luminosity of 127 pb-1 with both E+P and E- P collisions.. The definition of the angular correlation variables are:-. THETA(C=H), the angle between the plane determined by the highest ET jet and the beam and the plane determined by the two jets with lowest ET.. ALPHA(C=23), the angle between the lowest ET jets.. BETA(C=KSW), based on the Korner-Schierholz-Willrodt angle in 4 jets (see text of article).. GAMMA(C=H), angle of the scattered quark in the quark parton model.
DOI: 10.17182/hepdata.45283.v1/t6
title: "Table 6" of "Angular correlations in three-jet events in ep collisions at HERA"

description: Normalized differential EP cross section for 3-jet production in NC DIS as a function of THETA(H).
description: DESY-HERA. Measurement of the cross sections and angular correlations in 3-jet production in photoproduction and NC DIS events at centre of mass energies 300 and 318 GeV. The data were collected during the 1995 to 2000 HERA running period with a total integrated luminosity of 127 pb-1 with both E+P and E- P collisions.. The definition of the angular correlation variables are:-. THETA(C=H), the angle between the plane determined by the highest ET jet and the beam and the plane determined by the two jets with lowest ET.. ALPHA(C=23), the angle between the lowest ET jets.. BETA(C=KSW), based on the Korner-Schierholz-Willrodt angle in 4 jets (see text of article).. GAMMA(C=H), angle of the scattered quark in the quark parton model.
DOI: 10.17182/hepdata.45283.v1/t7
title: "Table 7" of "Angular correlations in three-jet events in ep collisions at HERA"

description: Normalized differential EP cross section for 3-jet production in NC DIS as a function of COS(ALPHA(23)).
description: DESY-HERA. Measurement of the cross sections and angular correlations in 3-jet production in photoproduction and NC DIS events at centre of mass energies 300 and 318 GeV. The data were collected during the 1995 to 2000 HERA running period with a total integrated luminosity of 127 pb-1 with both E+P and E- P collisions.. The definition of the angular correlation variables are:-. THETA(C=H), the angle between the plane determined by the highest ET jet and the beam and the plane determined by the two jets with lowest ET.. ALPHA(C=23), the angle between the lowest ET jets.. BETA(C=KSW), based on the Korner-Schierholz-Willrodt angle in 4 jets (see text of article).. GAMMA(C=H), angle of the scattered quark in the quark parton model.
DOI: 10.17182/hepdata.45283.v1/t8
title: "Table 8" of "Angular correlations in three-jet events in ep collisions at HERA"

description: Normalized differential EP cross section for 3-jet production in NC DIS as a function of COS(BETA(KSW)).
description: DESY-HERA. Measurement of the cross sections and angular correlations in 3-jet production in photoproduction and NC DIS events at centre of mass energies 300 and 318 GeV. The data were collected during the 1995 to 2000 HERA running period with a total integrated luminosity of 127 pb-1 with both E+P and E- P collisions.. The definition of the angular correlation variables are:-. THETA(C=H), the angle between the plane determined by the highest ET jet and the beam and the plane determined by the two jets with lowest ET.. ALPHA(C=23), the angle between the lowest ET jets.. BETA(C=KSW), based on the Korner-Schierholz-Willrodt angle in 4 jets (see text of article).. GAMMA(C=H), angle of the scattered quark in the quark parton model.
DOI: 10.17182/hepdata.45283.v1/t9
title: "Table 9" of "Angular correlations in three-jet events in ep collisions at HERA"

description: Normalized differential EP cross section of 3-jet production in NC DIS as afunction of the pseudorapidity of the jet with the largest pseudorapidity.
description: DESY-HERA. Measurement of the cross sections and angular correlations in 3-jet production in photoproduction and NC DIS events at centre of mass energies 300 and 318 GeV. The data were collected during the 1995 to 2000 HERA running period with a total integrated luminosity of 127 pb-1 with both E+P and E- P collisions.. The definition of the angular correlation variables are:-. THETA(C=H), the angle between the plane determined by the highest ET jet and the beam and the plane determined by the two jets with lowest ET.. ALPHA(C=23), the angle between the lowest ET jets.. BETA(C=KSW), based on the Korner-Schierholz-Willrodt angle in 4 jets (see text of article).. GAMMA(C=H), angle of the scattered quark in the quark parton model.
DOI: 10.17182/hepdata.45284.v1/t2
title: "Table 2" of "Electromagnetic proton form-factors at squared four momentum transfers between 1-GeV/c**2 and 3-GeV/c**2"

description: CONST(NAME=MU) is the magnetic moment.
description: DESY. Electromagnetic proton form factors at squared four momentum transfers between 1 and 3 GeV**2.
DOI: 10.17182/hepdata.45284.v1/t1
title: "Table 1" of "Electromagnetic proton form-factors at squared four momentum transfers between 1-GeV/c**2 and 3-GeV/c**2"

description: Axis error includes +- 2.5/2.5 contribution (Due to counting statisticss, separation of elastic events, beam monitoring, incident energy, scattering angle, proton absorption, solid angle, target length and density).
description: DESY. Electromagnetic proton form factors at squared four momentum transfers between 1 and 3 GeV**2.
DOI: 10.17182/hepdata.45286.v1/t1
title: "Table 1" of "The Q**2-dependence of the generalised Gerasimov-Drell-Hearn integral for the deuteron, proton and neutron."

description: The value of the GDH integral, as a function of Q**2 , for the deuteron in three W**2 regions, the total ( &gt; 1 GeV**2), the nucleon resonance ( 1 to 4.2 GeV**2) and the DIS (4.2 to 45 GeV**2).
description: DESY HERA. Measurement of the Gerasimov-Drell-Hearn (GDH) integral for the deuteron, proton and neutron from collisions of 27.57 GeV longitudinally polarised positrons with a longitudinally polarised atomic Deuterium gas target internal to the HERA storage ring in 1998 and 2000, and with an internal polarised atomic Hydrogen target in 1997.. The GDH integral is defined as:. INT[sig_1/2 - sig_3/2]d(nu)/nu , nu_0 & lt; nu & lt; infinity, where sig_1/2 and sig_3/2 are photoabsorption cross sections for total helicity of the photon-nucleon system equal to 1/2 and 3/2, respectively, nu is the photon energy in the target rest frame, nu_0 is the pion production threshold. In the last three tables the generalisation used are:. Generalisation A: INT = CONST*INT(A1(~)*F1)*D(X). Generalisation B: INT = CONST*INT(A1(~)*F1/SQRT(1+Q**2/NU**2))*D(X). Generalisation B: INT = CONST*INT(A1(~)*F1/(1-X))D(X). where CONST = 8*ALPHA*PI**2/Q**2.. The range of the integrals in the tables is from X=0 to X=Q**2/(2*M*NU_0).
DOI: 10.17182/hepdata.45286.v1/t2
title: "Table 2" of "The Q**2-dependence of the generalised Gerasimov-Drell-Hearn integral for the deuteron, proton and neutron."

description: The value of the GDH integral, as a function of Q**2 , for the proton in three W**2 regions, the total ( &gt; 1 GeV**2), the nucleon resonance ( 1 to 4.2 GeV**2) and the DIS (4.2 to 45 GeV**2).
description: DESY HERA. Measurement of the Gerasimov-Drell-Hearn (GDH) integral for the deuteron, proton and neutron from collisions of 27.57 GeV longitudinally polarised positrons with a longitudinally polarised atomic Deuterium gas target internal to the HERA storage ring in 1998 and 2000, and with an internal polarised atomic Hydrogen target in 1997.. The GDH integral is defined as:. INT[sig_1/2 - sig_3/2]d(nu)/nu , nu_0 & lt; nu & lt; infinity, where sig_1/2 and sig_3/2 are photoabsorption cross sections for total helicity of the photon-nucleon system equal to 1/2 and 3/2, respectively, nu is the photon energy in the target rest frame, nu_0 is the pion production threshold. In the last three tables the generalisation used are:. Generalisation A: INT = CONST*INT(A1(~)*F1)*D(X). Generalisation B: INT = CONST*INT(A1(~)*F1/SQRT(1+Q**2/NU**2))*D(X). Generalisation B: INT = CONST*INT(A1(~)*F1/(1-X))D(X). where CONST = 8*ALPHA*PI**2/Q**2.. The range of the integrals in the tables is from X=0 to X=Q**2/(2*M*NU_0).
DOI: 10.17182/hepdata.45286.v1/t3
title: "Table 3" of "The Q**2-dependence of the generalised Gerasimov-Drell-Hearn integral for the deuteron, proton and neutron."

description: The value of the GDH integral, as a function of Q**2 , for the neutron in three W**2 regions, the total ( &gt; 1 GeV**2), the nucleon resonance ( 1 to 4.2 GeV**2) and the DIS (4.2 to 45 GeV**2).
description: DESY HERA. Measurement of the Gerasimov-Drell-Hearn (GDH) integral for the deuteron, proton and neutron from collisions of 27.57 GeV longitudinally polarised positrons with a longitudinally polarised atomic Deuterium gas target internal to the HERA storage ring in 1998 and 2000, and with an internal polarised atomic Hydrogen target in 1997.. The GDH integral is defined as:. INT[sig_1/2 - sig_3/2]d(nu)/nu , nu_0 & lt; nu & lt; infinity, where sig_1/2 and sig_3/2 are photoabsorption cross sections for total helicity of the photon-nucleon system equal to 1/2 and 3/2, respectively, nu is the photon energy in the target rest frame, nu_0 is the pion production threshold. In the last three tables the generalisation used are:. Generalisation A: INT = CONST*INT(A1(~)*F1)*D(X). Generalisation B: INT = CONST*INT(A1(~)*F1/SQRT(1+Q**2/NU**2))*D(X). Generalisation B: INT = CONST*INT(A1(~)*F1/(1-X))D(X). where CONST = 8*ALPHA*PI**2/Q**2.. The range of the integrals in the tables is from X=0 to X=Q**2/(2*M*NU_0).
DOI: 10.17182/hepdata.45286.v1/t5
title: "Table 5" of "The Q**2-dependence of the generalised Gerasimov-Drell-Hearn integral for the deuteron, proton and neutron."

description: The value of the GDH integral for the proton, as a function of Q**2, for the full W**2 region for the three generalisations A, B and C.. = E+ P --&gt; E+ X.
description: DESY HERA. Measurement of the Gerasimov-Drell-Hearn (GDH) integral for the deuteron, proton and neutron from collisions of 27.57 GeV longitudinally polarised positrons with a longitudinally polarised atomic Deuterium gas target internal to the HERA storage ring in 1998 and 2000, and with an internal polarised atomic Hydrogen target in 1997.. The GDH integral is defined as:. INT[sig_1/2 - sig_3/2]d(nu)/nu , nu_0 & lt; nu & lt; infinity, where sig_1/2 and sig_3/2 are photoabsorption cross sections for total helicity of the photon-nucleon system equal to 1/2 and 3/2, respectively, nu is the photon energy in the target rest frame, nu_0 is the pion production threshold. In the last three tables the generalisation used are:. Generalisation A: INT = CONST*INT(A1(~)*F1)*D(X). Generalisation B: INT = CONST*INT(A1(~)*F1/SQRT(1+Q**2/NU**2))*D(X). Generalisation B: INT = CONST*INT(A1(~)*F1/(1-X))D(X). where CONST = 8*ALPHA*PI**2/Q**2.. The range of the integrals in the tables is from X=0 to X=Q**2/(2*M*NU_0).