cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.45525.v1/t8
title: "Table 8" of "Charged Particle Production in High Q2 Deep-Inelastic Scattering at HERA"

description: Normalised distribution of the scaled momentum as a function of Q**2 in the X range 0.3 to 0.4.
description: DESY-HERA. Measurement of the average charged hadron multiplicity and the normalised scaled momentum in DIS collisions of 27.5 GeV positrons with 920 GeV protons at a centre of mass energy of 318 GeV. The data, with a total integrated luminosity of 44 pb-1, were taken during the 2000 running period and are analysed in the Breit frame of reference. The DSYS error shown in the tables is the correlated error coming from the electron scale uncertainty and is not included in the total error.
DOI: 10.17182/hepdata.45525.v1/t9
title: "Table 9" of "Charged Particle Production in High Q2 Deep-Inelastic Scattering at HERA"

description: Normalised distribution of the scaled momentum as a function of Q**2 in the X range 0.4 to 0.5.
description: DESY-HERA. Measurement of the average charged hadron multiplicity and the normalised scaled momentum in DIS collisions of 27.5 GeV positrons with 920 GeV protons at a centre of mass energy of 318 GeV. The data, with a total integrated luminosity of 44 pb-1, were taken during the 2000 running period and are analysed in the Breit frame of reference. The DSYS error shown in the tables is the correlated error coming from the electron scale uncertainty and is not included in the total error.
DOI: 10.17182/hepdata.45526.v1/t1
title: "Table 1" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/M(P=4_5_6) as a function of M(P=4_5_6) .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t2
title: "Table 2" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/M(P=4_5_6_7) as a function of M(P=4_5_6_7) .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t3
title: "Table 3" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/X(C=GAMMA,OBS) as a function of X(C=GAMMA,OBS) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t4
title: "Table 4" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/X(C=GAMMA,OBS) as a function of X(C=GAMMA,OBS) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t5
title: "Table 5" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/Y as a function of Y in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t6
title: "Table 6" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/Y as a function of Y in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t10
title: "Table 10" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ET(P=4) as a function of ET(P=4) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t11
title: "Table 11" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ET(P=5) as a function of ET(P=5) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t12
title: "Table 12" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ET(P=6) as a function of ET(P=6) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t13
title: "Table 13" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ET(P=7) as a function of ET(P=7) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t14
title: "Table 14" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ETARAP(P=4) as a function of ETARAP(P=4) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t15
title: "Table 15" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ETARAP(P=5) as a function of ETARAP(P=5) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t7
title: "Table 7" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ET(P=4) as a function of ET(P=4) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t8
title: "Table 8" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ET(P=5) as a function of ET(P=5) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t9
title: "Table 9" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ET(P=6) as a function of ET(P=6) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t16
title: "Table 16" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ETARAP(P=6) as a function of ETARAP(P=6) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t17
title: "Table 17" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ETARAP(P=4) as a function of ETARAP(P=4) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t18
title: "Table 18" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ETARAP(P=5) as a function of ETARAP(P=5) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t19
title: "Table 19" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ETARAP(P=6) as a function of ETARAP(P=6) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t20
title: "Table 20" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/ETARAP(P=7) as a function of ETARAP(P=7) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45526.v1/t21
title: "Table 21" of "Three- and four-jet final states in photoproduction at HERA"

description: Cross section D(SIG)/COS(PSI(3)) as a function of COS(PSI(3)) in two jet invariant mass regions, 25 to 50 and &gt; 50 GeV . PSI(3) is the angle in the 3-jet CM frame between the plane containing the highest energy jet (P=4) and the beam, and the plane containing the three jets .
description: DESY-HERA. Measurement of the cross sections for 3- and 4-jet photoproduction from the collisions of 27.5 GeV electrons and positrons with 820 and 920 GeV protons having photon virtuality Q**2 & lt; 1 GeV**2. The data, which are a composite of centre-of-mass energies 300 and 318 GeV and have an integrated luminosity of 121 +- 2, come from the 1996 to 200 running periods Data are presented for a variety of variables and in two different jet invariant mass intervals. The ordering of the jets (P=4,P=5,P=6 and P=7) is in order of decreasing energy.
DOI: 10.17182/hepdata.45527.v1/t1
title: "Table 1" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Double differential cross section as a function of ET integrated over the ET bin range and the Q**2 range 150 to 200 GeV**2.
description: DESY-HERA.Measurement of inclusive jet production in neutral current DIS of 27.5 GeV positrons with 920 GeV protons equivalent to a centre of mass energy of 319 GeV. The data with an integrated luminosity of 65.4 pb-1 were analysed using the inclusive Kt jet finding algorithm in the Breit frame of reference, with single and double differential distributions being presented as functions of Q**2 (& gt; 150 Gev**2) and ET. The authors use the data to extract a precise value for the strong coupling constant ALPHAS as 0.1193 +- 0.0014(exp) +0.0047,-0.0030(th) +- 0.0016(pdf).. Details of the sources of systematic uncertainty, which make up the total systematic error, DSYS, shown in the tables (in percent) are defined as:. DUNC:Total ncorrelated uncertainty. DCORR: Total correlated uncertainty. DMOD: Uncertainty in the model dependence correction. DES: Uncertainty in the positron energy scale. DANG: Uncertainty in the positron polar angle. DHFS: Uncertainty in the HFS hadron energy scale. Also shown in the final column is the Hadronisations Correction factor, HCF.. Note that the cross sections here are integrated over the relevant bins, whereas in the plots in the papers they are given as differential cross sections.
DOI: 10.17182/hepdata.45527.v1/t2
title: "Table 2" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Double differential cross section as a function of ET integrated over the ET bin range and the Q**2 range 200 to 270 GeV**2.
description: DESY-HERA.Measurement of inclusive jet production in neutral current DIS of 27.5 GeV positrons with 920 GeV protons equivalent to a centre of mass energy of 319 GeV. The data with an integrated luminosity of 65.4 pb-1 were analysed using the inclusive Kt jet finding algorithm in the Breit frame of reference, with single and double differential distributions being presented as functions of Q**2 (& gt; 150 Gev**2) and ET. The authors use the data to extract a precise value for the strong coupling constant ALPHAS as 0.1193 +- 0.0014(exp) +0.0047,-0.0030(th) +- 0.0016(pdf).. Details of the sources of systematic uncertainty, which make up the total systematic error, DSYS, shown in the tables (in percent) are defined as:. DUNC:Total ncorrelated uncertainty. DCORR: Total correlated uncertainty. DMOD: Uncertainty in the model dependence correction. DES: Uncertainty in the positron energy scale. DANG: Uncertainty in the positron polar angle. DHFS: Uncertainty in the HFS hadron energy scale. Also shown in the final column is the Hadronisations Correction factor, HCF.. Note that the cross sections here are integrated over the relevant bins, whereas in the plots in the papers they are given as differential cross sections.
DOI: 10.17182/hepdata.45527.v1/t3
title: "Table 3" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Double differential cross section as a function of ET integrated over the ET bin range and the Q**2 range 270 to 400 GeV**2.
description: DESY-HERA.Measurement of inclusive jet production in neutral current DIS of 27.5 GeV positrons with 920 GeV protons equivalent to a centre of mass energy of 319 GeV. The data with an integrated luminosity of 65.4 pb-1 were analysed using the inclusive Kt jet finding algorithm in the Breit frame of reference, with single and double differential distributions being presented as functions of Q**2 (& gt; 150 Gev**2) and ET. The authors use the data to extract a precise value for the strong coupling constant ALPHAS as 0.1193 +- 0.0014(exp) +0.0047,-0.0030(th) +- 0.0016(pdf).. Details of the sources of systematic uncertainty, which make up the total systematic error, DSYS, shown in the tables (in percent) are defined as:. DUNC:Total ncorrelated uncertainty. DCORR: Total correlated uncertainty. DMOD: Uncertainty in the model dependence correction. DES: Uncertainty in the positron energy scale. DANG: Uncertainty in the positron polar angle. DHFS: Uncertainty in the HFS hadron energy scale. Also shown in the final column is the Hadronisations Correction factor, HCF.. Note that the cross sections here are integrated over the relevant bins, whereas in the plots in the papers they are given as differential cross sections.