cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.44220.v1/t1
title: "Table 1" of "Measurement of the proton spin structure function g1(p) with a pure hydrogen target."

description: The second systematic errors listed for G1/F1 (G1) are the uncertainties concerning R (R and F2).
description: DESY-HERA. HERMES Collaboration. Measurement of the proton spin structure function, G1, in deep inelastic scattering using a 27.6 GeV longitudinally polarised positron beam on a longitudinally polarised pure hydrogen gas internal target. Data cover the kinematical region in x from 0.021 to 0.85, and in Q**2 from 0.8 to 20 GeV**2.
DOI: 10.17182/hepdata.44220.v1/t2
title: "Table 2" of "Measurement of the proton spin structure function g1(p) with a pure hydrogen target."

description: G1 evolved at Q2 = 2.5 GeV**2, assuming G1/F1 to be independent of Q2. The second systematic errors listed for are the uncertainties concerning R and F2.
description: DESY-HERA. HERMES Collaboration. Measurement of the proton spin structure function, G1, in deep inelastic scattering using a 27.6 GeV longitudinally polarised positron beam on a longitudinally polarised pure hydrogen gas internal target. Data cover the kinematical region in x from 0.021 to 0.85, and in Q**2 from 0.8 to 20 GeV**2.
DOI: 10.17182/hepdata.44224.v1/t1
title: "Table 1" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t2
title: "Table 2" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t3
title: "Table 3" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffracitve scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t4
title: "Table 4" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t5
title: "Table 5" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t6
title: "Table 6" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t10
title: "Table 10" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t11
title: "Table 11" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t7
title: "Table 7" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t8
title: "Table 8" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t9
title: "Table 9" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t12
title: "Table 12" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Cross section for diffractive scattering.
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t13
title: "Table 13" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t14
title: "Table 14" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t15
title: "Table 15" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t16
title: "Table 16" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t17
title: "Table 17" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t18
title: "Table 18" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t19
title: "Table 19" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t20
title: "Table 20" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t21
title: "Table 21" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t22
title: "Table 22" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t23
title: "Table 23" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44224.v1/t24
title: "Table 24" of "Measurement of the diffractive cross-section in deep inelastic scattering using ZEUS 1994 data"

description: Diffractive structure function F2(D3).
description: DESY-HERA. Measurement of DIS diffractive cross section using 1994 data anddetermination of the diffractive structure function F2(*D3).The variable X(NAME =POMERON) = (MX**2 + Q2)/(W**2 + Q2) is the momentum fraction of the proton carried by the pomeron, Q2/(Q2+M_x**2) is the momentum fraction of the struck quark within the pomeron. & apos;The new results supersede those presented at in ZP C70, 391 which were affected by a technical error simulating the QED radiative corrections in the Monte-Carlo generation used for unfolding.& apos;.
DOI: 10.17182/hepdata.44248.v1/t1
title: "Table 1" of "The flavor asymmetry of the light quark sea from semi-inclusive deep inelastic scattering."

description: The ratio of parton distribution functions (PDF) is determined from the ratio of the differencies between charged pion yields for proton and neutron targets: (N_p(pi-)-N_n(pi-))/(N_p(pi+)-N_n(pi+)).
description: HERMES Collaboration. Measurement of the flavour asymmetry of the light quark sea in the kinematical ranges 0.02 & lt; x & lt; 0.3 and 1 & lt; Q2 & lt; 10 GeV**2.
DOI: 10.17182/hepdata.44249.v1/t1
title: "Table 1" of "Differential (2+1) jet event rates and determination of alpha(s) in deep inelastic scattering at HERA."

description: Y2 distribution corrected for detector effects.
description: DESY-HERA. Differential (2+1) jet event rates and determination of the str ong coupling constant in deep inelastic scattering. The +1 refers to the proton remnant jet. The JADE alogrithm (plus variants E, E0 and P) is used to define the jets, and the variable Y2 is defined as the smallest scaled jet mass (M2Jet**2/W**2) given by the combination of (2+1) jets. The 2-jet mass is the minimal one from possible 2-jet combinations when exactly 2+1 jet remains after applying of the jet-finding algorithm (see article).
DOI: 10.17182/hepdata.44249.v1/t2
title: "Table 2" of "Differential (2+1) jet event rates and determination of alpha(s) in deep inelastic scattering at HERA."

description: Y2 distribution corrected for both detector and hadronization effects.
description: DESY-HERA. Differential (2+1) jet event rates and determination of the str ong coupling constant in deep inelastic scattering. The +1 refers to the proton remnant jet. The JADE alogrithm (plus variants E, E0 and P) is used to define the jets, and the variable Y2 is defined as the smallest scaled jet mass (M2Jet**2/W**2) given by the combination of (2+1) jets. The 2-jet mass is the minimal one from possible 2-jet combinations when exactly 2+1 jet remains after applying of the jet-finding algorithm (see article).
DOI: 10.17182/hepdata.44249.v1/t3
title: "Table 3" of "Differential (2+1) jet event rates and determination of alpha(s) in deep inelastic scattering at HERA."

description: Y2 distribution using the E, E0 and P variants of the JADE alogrithm, corrected for both detector and hadronization effects. Statistical errors only.
description: DESY-HERA. Differential (2+1) jet event rates and determination of the str ong coupling constant in deep inelastic scattering. The +1 refers to the proton remnant jet. The JADE alogrithm (plus variants E, E0 and P) is used to define the jets, and the variable Y2 is defined as the smallest scaled jet mass (M2Jet**2/W**2) given by the combination of (2+1) jets. The 2-jet mass is the minimal one from possible 2-jet combinations when exactly 2+1 jet remains after applying of the jet-finding algorithm (see article).
DOI: 10.17182/hepdata.44249.v1/t4
title: "Table 4" of "Differential (2+1) jet event rates and determination of alpha(s) in deep inelastic scattering at HERA."

description: The value of alpha/s at extrapolated to the Z0 mass.. The first systematic (DSYS) errors is due to the experimental procedures, the second is from the theoretical assumptions made in the determination.
description: DESY-HERA. Differential (2+1) jet event rates and determination of the str ong coupling constant in deep inelastic scattering. The +1 refers to the proton remnant jet. The JADE alogrithm (plus variants E, E0 and P) is used to define the jets, and the variable Y2 is defined as the smallest scaled jet mass (M2Jet**2/W**2) given by the combination of (2+1) jets. The 2-jet mass is the minimal one from possible 2-jet combinations when exactly 2+1 jet remains after applying of the jet-finding algorithm (see article).
DOI: 10.17182/hepdata.44288.v1/t1
title: "Table 1" of "Forward jet production in deep inelastic scattering at HERA"

description: The second systematic (DSYS) error is the correlated systematic error due to the scale uncertainty of the calorimeter.
description: DESY-HERA. Measurement of the inclusive Forward Jet Production DifferentialCross Section in the Low x Region (0.00045 to 0.045).
DOI: 10.7910/dvn/ckez43
title: Data AHA EIA

description: Set of Data generated from the AHA EIA
DOI: 10.17182/hepdata.44302.v1/t1
title: "Table 1" of "Diffractive dijet cross-sections in photoproduction at HERA"

description: Differential cross section as a function of rapidity of the two highest Et jets in event.
description: DESY-HERA. Measurement of diffractive dijet differential cross sections in photoproduction events in which the hadronic final state containing the jets is separated with respect to the outgoing proton direction by a large rapidity gap. Jets are reconstructed using an iterative cone alogrithm in the eta-phi plane with a cone radius of 1.