cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.11718.v1/t110
title: "Table 110" of "Measurement of neutral current cross sections at high Bjorken-x with the ZEUS detector at HERA."

description: Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
description: DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This part is from the 96-97, E+ P, CM energy 300 GeV, 38.6 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This record is from the 98-99, E- P, CM energy 318 GeV, 16.7 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This record is from the 99-00, E+ P, CM energy 318 GeV, 65.1 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DOI: 10.17182/hepdata.11718.v1/t111
title: "Table 111" of "Measurement of neutral current cross sections at high Bjorken-x with the ZEUS detector at HERA."

description: Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
description: DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This part is from the 96-97, E+ P, CM energy 300 GeV, 38.6 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This record is from the 98-99, E- P, CM energy 318 GeV, 16.7 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This record is from the 99-00, E+ P, CM energy 318 GeV, 65.1 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DOI: 10.17182/hepdata.11718.v1/t112
title: "Table 112" of "Measurement of neutral current cross sections at high Bjorken-x with the ZEUS detector at HERA."

description: Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
description: DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This part is from the 96-97, E+ P, CM energy 300 GeV, 38.6 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This record is from the 98-99, E- P, CM energy 318 GeV, 16.7 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This record is from the 99-00, E+ P, CM energy 318 GeV, 65.1 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DOI: 10.17182/hepdata.11718.v1/t113
title: "Table 113" of "Measurement of neutral current cross sections at high Bjorken-x with the ZEUS detector at HERA."

description: Breakdown of the uncorrelated and correlated systematic errors for the 99-00 E+ P NC scattering data.
description: DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This part is from the 96-97, E+ P, CM energy 300 GeV, 38.6 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This record is from the 98-99, E- P, CM energy 318 GeV, 16.7 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This record is from the 99-00, E+ P, CM energy 318 GeV, 65.1 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DOI: 10.17182/hepdata.11718.v1/t114
title: "Table 114" of "Measurement of neutral current cross sections at high Bjorken-x with the ZEUS detector at HERA."

description: Breakdown of the uncorrelated and correlated systematic errors for the integrated 99-00 E+ P NC scattering data.
description: DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This part is from the 96-97, E+ P, CM energy 300 GeV, 38.6 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This record is from the 98-99, E- P, CM energy 318 GeV, 16.7 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DESY-HERA. Measurement of the neutral current cross sections in E- P scattering at high X. A new method is used to reanalyse data already published in PR D70,052001 (2003), EPJ C21,443 (2001) and EPJ C28,175 (2003). The data are from 3 data sets. This record is from the 99-00, E+ P, CM energy 318 GeV, 65.1 pb-1 set.. A detailed breakdown of the systematic errors is also given where:. SYS-UNCOR is the uncorrelated systematic errors.. DEL1 is from the electron energy scale.. DEL2 is from the jet energy scale.. DEL3 is from the FCAL energy scale.. DEL4 is from the PDF uncertainty.. DEL5 is from the hadronic final state and simulation uncertainty.. DEL6 is from uncertainties in higher order radiative corrections.
DOI: 10.17182/hepdata.11760.v1/t1
title: "Table 1" of "Measurement of the forward $W$ boson cross-section in $pp$ collisions at $\sqrt{s} = 7 {\rm \, TeV}$"

description: Correction for final state radiation for $W^+ \rightarrow \mu^+\nu$ and $W^- \rightarrow \mu^-\bar{\nu}$ in bins of muon pseudorapidity. No loss due FSR is observed for $W^-$ in the last pseudorapidity bin because of lack of statistics.
description: CERN-LHC. A measurement of the inclusive $W \to \mu\nu$ production cross-section using data from $pp$ collisions at a centre-of-mass energy of $\sqrt{s} = 7 {\rm \, TeV}$ is presented. The analysis is based on an integrated luminosity of about $1.0 {\rm \, fb}^{-1}$ recorded with the LHCb detector. Results are reported for muons with a transverse momentum greater than $20 {\rm \, Ge\kern -0.1em V\!/}c$ and pseudorapidity between 2.0 and 4.5. The $W^{+}$ and $W^{-}$ production cross-sections are measured to be
\[
 \sigma_{W^{+} \to \mu^{+}\nu} = 861.0 \pm 2.0 \pm 11.2 \pm 14.7 {\rm \, pb},\\
 \sigma_{W^{-} \to \mu^{-}\overline{\nu}} = 675.8 \pm 1.9 \pm 8.8 \pm 11.6 {\rm \, pb},
\]
where the first uncertainty is statistical, the second is systematic and the third is due to the luminosity determination. Cross-section ratios and differential distributions as functions of the muon pseudorapidity are also presented. The ratio of $W^{+}$ to $W^{-}$ cross-sections in the same fiducial kinematic region is determined to be
\[
\frac{\sigma_{W^{+} \to \mu^{+}\nu}}{\sigma_{W^{-} \to \mu^{-}\overline{\nu}}} = 1.274 \pm 0.005 \pm 0.009,
\]
where the uncertainties are statistical and systematic, respectively. Results are in good agreement with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics.
DOI: 10.17182/hepdata.11760.v1/t2
title: "Table 2" of "Measurement of the forward $W$ boson cross-section in $pp$ collisions at $\sqrt{s} = 7 {\rm \, TeV}$"

description: Inclusive cross-section for $W^+$ and $W^-$ boson production in bins of muon pseudorapidity. The uncertainties are statistical, systematic and luminosity.
description: CERN-LHC. A measurement of the inclusive $W \to \mu\nu$ production cross-section using data from $pp$ collisions at a centre-of-mass energy of $\sqrt{s} = 7 {\rm \, TeV}$ is presented. The analysis is based on an integrated luminosity of about $1.0 {\rm \, fb}^{-1}$ recorded with the LHCb detector. Results are reported for muons with a transverse momentum greater than $20 {\rm \, Ge\kern -0.1em V\!/}c$ and pseudorapidity between 2.0 and 4.5. The $W^{+}$ and $W^{-}$ production cross-sections are measured to be
\[
 \sigma_{W^{+} \to \mu^{+}\nu} = 861.0 \pm 2.0 \pm 11.2 \pm 14.7 {\rm \, pb},\\
 \sigma_{W^{-} \to \mu^{-}\overline{\nu}} = 675.8 \pm 1.9 \pm 8.8 \pm 11.6 {\rm \, pb},
\]
where the first uncertainty is statistical, the second is systematic and the third is due to the luminosity determination. Cross-section ratios and differential distributions as functions of the muon pseudorapidity are also presented. The ratio of $W^{+}$ to $W^{-}$ cross-sections in the same fiducial kinematic region is determined to be
\[
\frac{\sigma_{W^{+} \to \mu^{+}\nu}}{\sigma_{W^{-} \to \mu^{-}\overline{\nu}}} = 1.274 \pm 0.005 \pm 0.009,
\]
where the uncertainties are statistical and systematic, respectively. Results are in good agreement with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics.
DOI: 10.17182/hepdata.11760.v1/t3
title: "Table 3" of "Measurement of the forward $W$ boson cross-section in $pp$ collisions at $\sqrt{s} = 7 {\rm \, TeV}$"

description: Ratio of $W^+$ to $W^-$ cross-section in bins of muon pseudorapidity. The uncertainties are statistical and systematic.
description: CERN-LHC. A measurement of the inclusive $W \to \mu\nu$ production cross-section using data from $pp$ collisions at a centre-of-mass energy of $\sqrt{s} = 7 {\rm \, TeV}$ is presented. The analysis is based on an integrated luminosity of about $1.0 {\rm \, fb}^{-1}$ recorded with the LHCb detector. Results are reported for muons with a transverse momentum greater than $20 {\rm \, Ge\kern -0.1em V\!/}c$ and pseudorapidity between 2.0 and 4.5. The $W^{+}$ and $W^{-}$ production cross-sections are measured to be
\[
 \sigma_{W^{+} \to \mu^{+}\nu} = 861.0 \pm 2.0 \pm 11.2 \pm 14.7 {\rm \, pb},\\
 \sigma_{W^{-} \to \mu^{-}\overline{\nu}} = 675.8 \pm 1.9 \pm 8.8 \pm 11.6 {\rm \, pb},
\]
where the first uncertainty is statistical, the second is systematic and the third is due to the luminosity determination. Cross-section ratios and differential distributions as functions of the muon pseudorapidity are also presented. The ratio of $W^{+}$ to $W^{-}$ cross-sections in the same fiducial kinematic region is determined to be
\[
\frac{\sigma_{W^{+} \to \mu^{+}\nu}}{\sigma_{W^{-} \to \mu^{-}\overline{\nu}}} = 1.274 \pm 0.005 \pm 0.009,
\]
where the uncertainties are statistical and systematic, respectively. Results are in good agreement with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics.
DOI: 10.17182/hepdata.11760.v1/t4
title: "Table 4" of "Measurement of the forward $W$ boson cross-section in $pp$ collisions at $\sqrt{s} = 7 {\rm \, TeV}$"

description: Lepton charge asymmetry in bins of muon pseudorapidity. The uncertainties are statistical and systematic.
description: CERN-LHC. A measurement of the inclusive $W \to \mu\nu$ production cross-section using data from $pp$ collisions at a centre-of-mass energy of $\sqrt{s} = 7 {\rm \, TeV}$ is presented. The analysis is based on an integrated luminosity of about $1.0 {\rm \, fb}^{-1}$ recorded with the LHCb detector. Results are reported for muons with a transverse momentum greater than $20 {\rm \, Ge\kern -0.1em V\!/}c$ and pseudorapidity between 2.0 and 4.5. The $W^{+}$ and $W^{-}$ production cross-sections are measured to be
\[
 \sigma_{W^{+} \to \mu^{+}\nu} = 861.0 \pm 2.0 \pm 11.2 \pm 14.7 {\rm \, pb},\\
 \sigma_{W^{-} \to \mu^{-}\overline{\nu}} = 675.8 \pm 1.9 \pm 8.8 \pm 11.6 {\rm \, pb},
\]
where the first uncertainty is statistical, the second is systematic and the third is due to the luminosity determination. Cross-section ratios and differential distributions as functions of the muon pseudorapidity are also presented. The ratio of $W^{+}$ to $W^{-}$ cross-sections in the same fiducial kinematic region is determined to be
\[
\frac{\sigma_{W^{+} \to \mu^{+}\nu}}{\sigma_{W^{-} \to \mu^{-}\overline{\nu}}} = 1.274 \pm 0.005 \pm 0.009,
\]
where the uncertainties are statistical and systematic, respectively. Results are in good agreement with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics.
DOI: 10.17182/hepdata.11816.v1/t2
title: "Table 2" of "Study of deep inelastic inclusive and diffractive scattering with the ZEUS forward plug calorimeter."

description: Measurement of the proton structure function F2 at Q**2 = 4.0 GeV**2.
description: DESY-HERA. Measurement of diffractive production cross sections and structure functions in DIS scattering of 27.5 GeV electrons with 920 GeV protons. The data come from the 1998-1999 running period and have an integrated luminosity of 4.2 pb-1. The data cover the GAMMA*P centre of mass energy W from 37 to 245 GeV and Q**2 from 2.2 to 8.0 GeV. Data are presented as cross sections and also in terms of the diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON), BETA and Q**2. X(NAME=POMERON) is the fraction of the protons momentum carried by the Pomeron and BETA is the fraction of the Pomeron momentum carried by the struck quark.
DOI: 10.17182/hepdata.11815.v1/t1
title: "Table 1" of "phi MESON PRODUCTION AT THE UPSILON RESONANCES AND THE NEARBY CONTINUUM"

description: No description provided.
description: CESR-CLEO MAGNETIC DETECTOR. PHI MESON PRODUCTION AT THE UPSILON RESONANCE AND THE NEARBY CONTINUUM. PHI IDENTIFIED BY K+ K- DECAY MODE. FOR LOWEST MOMENTA BIN 1-2 GEV SIGNAL IS IMPROVED BY REQUIRING AT LEAST ONE KAON TO BE IDENTIFIED. THIS METHOD IS NOT APPLICABLE TO HIGHER MOMENTA. DATA ON MASS (K+ K-) SPECTRA FITTED WITH SMOOTH POLYNOMIAL PLUS GAUSSIAN. DIRECT UPSI(1S) DECAY DATA WERE CORRECTED FOR THE NON-RESONANT BACKGROUND, AND THE DECAYS VIA THE ONE-PHOTON INTERMEDIATE STAGE.
DOI: 10.17182/hepdata.11816.v1/t1
title: "Table 1" of "Study of deep inelastic inclusive and diffractive scattering with the ZEUS forward plug calorimeter."

description: Measurement of the proton structure function F2 at Q**2 = 2.7 GeV**2.
description: DESY-HERA. Measurement of diffractive production cross sections and structure functions in DIS scattering of 27.5 GeV electrons with 920 GeV protons. The data come from the 1998-1999 running period and have an integrated luminosity of 4.2 pb-1. The data cover the GAMMA*P centre of mass energy W from 37 to 245 GeV and Q**2 from 2.2 to 8.0 GeV. Data are presented as cross sections and also in terms of the diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON), BETA and Q**2. X(NAME=POMERON) is the fraction of the protons momentum carried by the Pomeron and BETA is the fraction of the Pomeron momentum carried by the struck quark.
DOI: 10.17182/hepdata.11816.v1/t3
title: "Table 3" of "Study of deep inelastic inclusive and diffractive scattering with the ZEUS forward plug calorimeter."

description: Measurement of the proton structure function F2 at Q**2 = 6.0 GeV**2.
description: DESY-HERA. Measurement of diffractive production cross sections and structure functions in DIS scattering of 27.5 GeV electrons with 920 GeV protons. The data come from the 1998-1999 running period and have an integrated luminosity of 4.2 pb-1. The data cover the GAMMA*P centre of mass energy W from 37 to 245 GeV and Q**2 from 2.2 to 8.0 GeV. Data are presented as cross sections and also in terms of the diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON), BETA and Q**2. X(NAME=POMERON) is the fraction of the protons momentum carried by the Pomeron and BETA is the fraction of the Pomeron momentum carried by the struck quark.
DOI: 10.17182/hepdata.11816.v1/t4
title: "Table 4" of "Study of deep inelastic inclusive and diffractive scattering with the ZEUS forward plug calorimeter."

description: Measurement of the proton structure function F2 at Q**2 = 8.0 GeV**2.
description: DESY-HERA. Measurement of diffractive production cross sections and structure functions in DIS scattering of 27.5 GeV electrons with 920 GeV protons. The data come from the 1998-1999 running period and have an integrated luminosity of 4.2 pb-1. The data cover the GAMMA*P centre of mass energy W from 37 to 245 GeV and Q**2 from 2.2 to 8.0 GeV. Data are presented as cross sections and also in terms of the diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON), BETA and Q**2. X(NAME=POMERON) is the fraction of the protons momentum carried by the Pomeron and BETA is the fraction of the Pomeron momentum carried by the struck quark.
DOI: 10.17182/hepdata.11816.v1/t5
title: "Table 5" of "Study of deep inelastic inclusive and diffractive scattering with the ZEUS forward plug calorimeter."

description: Measurement of the proton structure function F2 at Q**2 = 14.0 GeV**2.
description: DESY-HERA. Measurement of diffractive production cross sections and structure functions in DIS scattering of 27.5 GeV electrons with 920 GeV protons. The data come from the 1998-1999 running period and have an integrated luminosity of 4.2 pb-1. The data cover the GAMMA*P centre of mass energy W from 37 to 245 GeV and Q**2 from 2.2 to 8.0 GeV. Data are presented as cross sections and also in terms of the diffractive structure function F2(NAME=D3) as a function of X(NAME=POMERON), BETA and Q**2. X(NAME=POMERON) is the fraction of the protons momentum carried by the Pomeron and BETA is the fraction of the Pomeron momentum carried by the struck quark.