cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.44498.v1/t7
title: "Table 7" 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/t8
title: "Table 8" 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/t9
title: "Table 9" 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/t13
title: "Table 13" 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/t14
title: "Table 14" 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/t15
title: "Table 15" 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/t16
title: "Table 16" 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/t17
title: "Table 17" 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/t18
title: "Table 18" 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/t19
title: "Table 19" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The inclusive virtual photon-proton jet cross section.
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/t20
title: "Table 20" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The inclusive virtual photon-proton jet cross section.
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/t21
title: "Table 21" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The inclusive virtual photon-proton jet cross section.
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/t22
title: "Table 22" of "Low Q**2 jet production at HERA and virtual photon structure."

description: The inclusive virtual photon-proton jet cross section.
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.44502.v1/t1
title: "Table 1" of "Inclusive measurement of diffractive deep inelastic ep scattering"

description: No description provided.
description: DESY-HERA. Measurement of the structure function F2(NAME=D3) in the deep inelastic scattering process e p --& gt; e X Y where X and Y are final hadronic statesseparated by the largest rapidity gap interval. The system Y is that which has rapidity closest to that of the incident proton and is selected to have mass & lt; 1.6 GeV. It is coded here as P. The variable X(NAME=POMERON) is defined as q.(P-PY)/q.P where q, P and PY are the 4-momenta respectively of the exchanged virtual boson, the incident proton and the subsystem Y. BETA is defined as X/X(NAME=POMERON). The data come from the 1994 running period corresponding to 1.96 pb-1 integrated luminosity.
DOI: 10.17182/hepdata.44502.v1/t2
title: "Table 2" of "Inclusive measurement of diffractive deep inelastic ep scattering"

description: No description provided.
description: DESY-HERA. Measurement of the structure function F2(NAME=D3) in the deep inelastic scattering process e p --& gt; e X Y where X and Y are final hadronic statesseparated by the largest rapidity gap interval. The system Y is that which has rapidity closest to that of the incident proton and is selected to have mass & lt; 1.6 GeV. It is coded here as P. The variable X(NAME=POMERON) is defined as q.(P-PY)/q.P where q, P and PY are the 4-momenta respectively of the exchanged virtual boson, the incident proton and the subsystem Y. BETA is defined as X/X(NAME=POMERON). The data come from the 1994 running period corresponding to 1.96 pb-1 integrated luminosity.
DOI: 10.17182/hepdata.44502.v1/t3
title: "Table 3" of "Inclusive measurement of diffractive deep inelastic ep scattering"

description: No description provided.
description: DESY-HERA. Measurement of the structure function F2(NAME=D3) in the deep inelastic scattering process e p --& gt; e X Y where X and Y are final hadronic statesseparated by the largest rapidity gap interval. The system Y is that which has rapidity closest to that of the incident proton and is selected to have mass & lt; 1.6 GeV. It is coded here as P. The variable X(NAME=POMERON) is defined as q.(P-PY)/q.P where q, P and PY are the 4-momenta respectively of the exchanged virtual boson, the incident proton and the subsystem Y. BETA is defined as X/X(NAME=POMERON). The data come from the 1994 running period corresponding to 1.96 pb-1 integrated luminosity.
DOI: 10.17182/hepdata.44502.v1/t4
title: "Table 4" of "Inclusive measurement of diffractive deep inelastic ep scattering"

description: No description provided.
description: DESY-HERA. Measurement of the structure function F2(NAME=D3) in the deep inelastic scattering process e p --& gt; e X Y where X and Y are final hadronic statesseparated by the largest rapidity gap interval. The system Y is that which has rapidity closest to that of the incident proton and is selected to have mass & lt; 1.6 GeV. It is coded here as P. The variable X(NAME=POMERON) is defined as q.(P-PY)/q.P where q, P and PY are the 4-momenta respectively of the exchanged virtual boson, the incident proton and the subsystem Y. BETA is defined as X/X(NAME=POMERON). The data come from the 1994 running period corresponding to 1.96 pb-1 integrated luminosity.
DOI: 10.17182/hepdata.44502.v1/t5
title: "Table 5" of "Inclusive measurement of diffractive deep inelastic ep scattering"

description: No description provided.
description: DESY-HERA. Measurement of the structure function F2(NAME=D3) in the deep inelastic scattering process e p --& gt; e X Y where X and Y are final hadronic statesseparated by the largest rapidity gap interval. The system Y is that which has rapidity closest to that of the incident proton and is selected to have mass & lt; 1.6 GeV. It is coded here as P. The variable X(NAME=POMERON) is defined as q.(P-PY)/q.P where q, P and PY are the 4-momenta respectively of the exchanged virtual boson, the incident proton and the subsystem Y. BETA is defined as X/X(NAME=POMERON). The data come from the 1994 running period corresponding to 1.96 pb-1 integrated luminosity.
DOI: 10.17182/hepdata.44502.v1/t6
title: "Table 6" of "Inclusive measurement of diffractive deep inelastic ep scattering"

description: No description provided.
description: DESY-HERA. Measurement of the structure function F2(NAME=D3) in the deep inelastic scattering process e p --& gt; e X Y where X and Y are final hadronic statesseparated by the largest rapidity gap interval. The system Y is that which has rapidity closest to that of the incident proton and is selected to have mass & lt; 1.6 GeV. It is coded here as P. The variable X(NAME=POMERON) is defined as q.(P-PY)/q.P where q, P and PY are the 4-momenta respectively of the exchanged virtual boson, the incident proton and the subsystem Y. BETA is defined as X/X(NAME=POMERON). The data come from the 1994 running period corresponding to 1.96 pb-1 integrated luminosity.
DOI: 10.17182/hepdata.44502.v1/t7
title: "Table 7" of "Inclusive measurement of diffractive deep inelastic ep scattering"

description: No description provided.
description: DESY-HERA. Measurement of the structure function F2(NAME=D3) in the deep inelastic scattering process e p --& gt; e X Y where X and Y are final hadronic statesseparated by the largest rapidity gap interval. The system Y is that which has rapidity closest to that of the incident proton and is selected to have mass & lt; 1.6 GeV. It is coded here as P. The variable X(NAME=POMERON) is defined as q.(P-PY)/q.P where q, P and PY are the 4-momenta respectively of the exchanged virtual boson, the incident proton and the subsystem Y. BETA is defined as X/X(NAME=POMERON). The data come from the 1994 running period corresponding to 1.96 pb-1 integrated luminosity.
DOI: 10.17182/hepdata.44502.v1/t8
title: "Table 8" of "Inclusive measurement of diffractive deep inelastic ep scattering"

description: No description provided.
description: DESY-HERA. Measurement of the structure function F2(NAME=D3) in the deep inelastic scattering process e p --& gt; e X Y where X and Y are final hadronic statesseparated by the largest rapidity gap interval. The system Y is that which has rapidity closest to that of the incident proton and is selected to have mass & lt; 1.6 GeV. It is coded here as P. The variable X(NAME=POMERON) is defined as q.(P-PY)/q.P where q, P and PY are the 4-momenta respectively of the exchanged virtual boson, the incident proton and the subsystem Y. BETA is defined as X/X(NAME=POMERON). The data come from the 1994 running period corresponding to 1.96 pb-1 integrated luminosity.
DOI: 10.17182/hepdata.44511.v1/t1
title: "Table 1" of "Measurement of the inclusive di-jet cross section in photoproduction and determination of an effective parton distribution in the photon."

description: No description provided.
description: DESY-HERA. Measurement of the inclusive 2-JET cross section in photoproduction and determination of an Effective Parton Distribution in the photon. Integrated luminocity used for this analysis is 2.9 1/pb. Data were taken in 1994. & apos;The photoproduction events were selected by requiring that the scattered electron remains in the beam pipe (untagged events), therefore photon virtuality Q2& lt;4 GeV2, where 80 PCT of the events have Q2& lt;0.1 GeV2& apos;. X(C=GAMMA) = (E(jet1)*EXP(-ETARAP(jet1))+E(jet2)*EXP(-ETARAP(jet2) ))/ (2*Y*E_e) is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: Y = E_gamma/E_e. ET is in GeV.
DOI: 10.17182/hepdata.44511.v1/t2
title: "Table 2" of "Measurement of the inclusive di-jet cross section in photoproduction and determination of an effective parton distribution in the photon."

description: No description provided.
description: DESY-HERA. Measurement of the inclusive 2-JET cross section in photoproduction and determination of an Effective Parton Distribution in the photon. Integrated luminocity used for this analysis is 2.9 1/pb. Data were taken in 1994. & apos;The photoproduction events were selected by requiring that the scattered electron remains in the beam pipe (untagged events), therefore photon virtuality Q2& lt;4 GeV2, where 80 PCT of the events have Q2& lt;0.1 GeV2& apos;. X(C=GAMMA) = (E(jet1)*EXP(-ETARAP(jet1))+E(jet2)*EXP(-ETARAP(jet2) ))/ (2*Y*E_e) is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: Y = E_gamma/E_e. ET is in GeV.
DOI: 10.17182/hepdata.44511.v1/t3
title: "Table 3" of "Measurement of the inclusive di-jet cross section in photoproduction and determination of an effective parton distribution in the photon."

description: No description provided.
description: DESY-HERA. Measurement of the inclusive 2-JET cross section in photoproduction and determination of an Effective Parton Distribution in the photon. Integrated luminocity used for this analysis is 2.9 1/pb. Data were taken in 1994. & apos;The photoproduction events were selected by requiring that the scattered electron remains in the beam pipe (untagged events), therefore photon virtuality Q2& lt;4 GeV2, where 80 PCT of the events have Q2& lt;0.1 GeV2& apos;. X(C=GAMMA) = (E(jet1)*EXP(-ETARAP(jet1))+E(jet2)*EXP(-ETARAP(jet2) ))/ (2*Y*E_e) is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: Y = E_gamma/E_e. ET is in GeV.
DOI: 10.17182/hepdata.44511.v1/t4
title: "Table 4" of "Measurement of the inclusive di-jet cross section in photoproduction and determination of an effective parton distribution in the photon."

description: No description provided.
description: DESY-HERA. Measurement of the inclusive 2-JET cross section in photoproduction and determination of an Effective Parton Distribution in the photon. Integrated luminocity used for this analysis is 2.9 1/pb. Data were taken in 1994. & apos;The photoproduction events were selected by requiring that the scattered electron remains in the beam pipe (untagged events), therefore photon virtuality Q2& lt;4 GeV2, where 80 PCT of the events have Q2& lt;0.1 GeV2& apos;. X(C=GAMMA) = (E(jet1)*EXP(-ETARAP(jet1))+E(jet2)*EXP(-ETARAP(jet2) ))/ (2*Y*E_e) is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: Y = E_gamma/E_e. ET is in GeV.
DOI: 10.17182/hepdata.44511.v1/t5
title: "Table 5" of "Measurement of the inclusive di-jet cross section in photoproduction and determination of an effective parton distribution in the photon."

description: No description provided.
description: DESY-HERA. Measurement of the inclusive 2-JET cross section in photoproduction and determination of an Effective Parton Distribution in the photon. Integrated luminocity used for this analysis is 2.9 1/pb. Data were taken in 1994. & apos;The photoproduction events were selected by requiring that the scattered electron remains in the beam pipe (untagged events), therefore photon virtuality Q2& lt;4 GeV2, where 80 PCT of the events have Q2& lt;0.1 GeV2& apos;. X(C=GAMMA) = (E(jet1)*EXP(-ETARAP(jet1))+E(jet2)*EXP(-ETARAP(jet2) ))/ (2*Y*E_e) is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: Y = E_gamma/E_e. ET is in GeV.
DOI: 10.17182/hepdata.44511.v1/t6
title: "Table 6" of "Measurement of the inclusive di-jet cross section in photoproduction and determination of an effective parton distribution in the photon."

description: No description provided.
description: DESY-HERA. Measurement of the inclusive 2-JET cross section in photoproduction and determination of an Effective Parton Distribution in the photon. Integrated luminocity used for this analysis is 2.9 1/pb. Data were taken in 1994. & apos;The photoproduction events were selected by requiring that the scattered electron remains in the beam pipe (untagged events), therefore photon virtuality Q2& lt;4 GeV2, where 80 PCT of the events have Q2& lt;0.1 GeV2& apos;. X(C=GAMMA) = (E(jet1)*EXP(-ETARAP(jet1))+E(jet2)*EXP(-ETARAP(jet2) ))/ (2*Y*E_e) is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: Y = E_gamma/E_e. ET is in GeV.
DOI: 10.17182/hepdata.44511.v1/t7
title: "Table 7" of "Measurement of the inclusive di-jet cross section in photoproduction and determination of an effective parton distribution in the photon."

description: No description provided.
description: DESY-HERA. Measurement of the inclusive 2-JET cross section in photoproduction and determination of an Effective Parton Distribution in the photon. Integrated luminocity used for this analysis is 2.9 1/pb. Data were taken in 1994. & apos;The photoproduction events were selected by requiring that the scattered electron remains in the beam pipe (untagged events), therefore photon virtuality Q2& lt;4 GeV2, where 80 PCT of the events have Q2& lt;0.1 GeV2& apos;. X(C=GAMMA) = (E(jet1)*EXP(-ETARAP(jet1))+E(jet2)*EXP(-ETARAP(jet2) ))/ (2*Y*E_e) is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: Y = E_gamma/E_e. ET is in GeV.
DOI: 10.17182/hepdata.44511.v1/t8
title: "Table 8" of "Measurement of the inclusive di-jet cross section in photoproduction and determination of an effective parton distribution in the photon."

description: Effective photon parton distribution in the form X(C=GAMMA)*PDF(X,PT**2). The second systematic error is due to the uncertainty in the extraction ofthe PDF resulting from multiple parton scattering effects which was determined using the two event generators PYTHIA and PHOJET.
description: DESY-HERA. Measurement of the inclusive 2-JET cross section in photoproduction and determination of an Effective Parton Distribution in the photon. Integrated luminocity used for this analysis is 2.9 1/pb. Data were taken in 1994. & apos;The photoproduction events were selected by requiring that the scattered electron remains in the beam pipe (untagged events), therefore photon virtuality Q2& lt;4 GeV2, where 80 PCT of the events have Q2& lt;0.1 GeV2& apos;. X(C=GAMMA) = (E(jet1)*EXP(-ETARAP(jet1))+E(jet2)*EXP(-ETARAP(jet2) ))/ (2*Y*E_e) is the fraction of quasi-real photon momentum carried by its parton, where Y is the fraction of the lepton beam energy carried by quasi-real photon: Y = E_gamma/E_e. ET is in GeV.