cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.45527.v1/t4
title: "Table 4" 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 400 to 700 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/t5
title: "Table 5" 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 700 to 5000 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/t6
title: "Table 6" 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 5000 to 15000 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/t7
title: "Table 7" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Single differential cross section as a function of ET integrated over the ET bin range.
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/t10
title: "Table 10" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Normalised inclusive jet cross section as a function of ET in 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/t11
title: "Table 11" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Normalised inclusive jet cross section as a function of ET in 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.
DOI: 10.17182/hepdata.45527.v1/t12
title: "Table 12" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Normalised inclusive jet cross section as a function of ET in the Q**2 range 400 to 700 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/t13
title: "Table 13" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Normalised inclusive jet cross section as a function of ET in the Q**2 range 700 to 5000 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/t14
title: "Table 14" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Normalised inclusive jet cross section as a function of ET in the Q**2 range 5000 to 15000 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/t8
title: "Table 8" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Single differential cross section as a function of Q**2 integrated over the Q**2 bin range.
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/t9
title: "Table 9" of "Measurement of Inclusive Jet Production in Deep-Inelastic Scattering at High Q^2 and Determination of the Strong Coupling"

description: Normalised inclusive jet cross section as a function of ET in 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.45528.v1/t1
title: "Table 1" of "Multijet production at low x(Bj) in deep inelastic scattering at HERA."

description: Two jet cross section D(SIG)/DQ**2 as a function of Q**2.
description: DESY-HERA. Measurement of the cross sections for inclusive dijet and trijet production in DIS collisions of 27.5 GeV electrons and positrons with 920 GeV protons at a centre-of-mass energy of 318 GeV. The data, which correspond to an integrated luminosity of 82 pb-1, were collected during the 1998-2000 running period and cover the Q**2 region from 10 to 100 GeV and low Bjorken-X region from 0.0001 to 0.01. Jets were identified in the hadronic centre-of-mass frame using the KT cluster algorithm in the longitudinally invariant inclusive mode. The second systematic (DSYS) error in the tables is from the uncertainty in the jet energy scale. In the nomenclature used here the jets are ordered in ET, namely P=4 is the jet of highest ET.. Numerical values supplied by T Daniels.
DOI: 10.17182/hepdata.45528.v1/t2
title: "Table 2" of "Multijet production at low x(Bj) in deep inelastic scattering at HERA."

description: Two jet cross section D(SIG)/DX as a function of X.
description: DESY-HERA. Measurement of the cross sections for inclusive dijet and trijet production in DIS collisions of 27.5 GeV electrons and positrons with 920 GeV protons at a centre-of-mass energy of 318 GeV. The data, which correspond to an integrated luminosity of 82 pb-1, were collected during the 1998-2000 running period and cover the Q**2 region from 10 to 100 GeV and low Bjorken-X region from 0.0001 to 0.01. Jets were identified in the hadronic centre-of-mass frame using the KT cluster algorithm in the longitudinally invariant inclusive mode. The second systematic (DSYS) error in the tables is from the uncertainty in the jet energy scale. In the nomenclature used here the jets are ordered in ET, namely P=4 is the jet of highest ET.. Numerical values supplied by T Daniels.
DOI: 10.17182/hepdata.45528.v1/t3
title: "Table 3" of "Multijet production at low x(Bj) in deep inelastic scattering at HERA."

description: Two jet cross section D(SIG)/DET(P=4,RF=CM) as a function of ET(P=4,RF=CM).
description: DESY-HERA. Measurement of the cross sections for inclusive dijet and trijet production in DIS collisions of 27.5 GeV electrons and positrons with 920 GeV protons at a centre-of-mass energy of 318 GeV. The data, which correspond to an integrated luminosity of 82 pb-1, were collected during the 1998-2000 running period and cover the Q**2 region from 10 to 100 GeV and low Bjorken-X region from 0.0001 to 0.01. Jets were identified in the hadronic centre-of-mass frame using the KT cluster algorithm in the longitudinally invariant inclusive mode. The second systematic (DSYS) error in the tables is from the uncertainty in the jet energy scale. In the nomenclature used here the jets are ordered in ET, namely P=4 is the jet of highest ET.. Numerical values supplied by T Daniels.
DOI: 10.17182/hepdata.45528.v1/t4
title: "Table 4" of "Multijet production at low x(Bj) in deep inelastic scattering at HERA."

description: Two jet cross section D(SIG)/DET(P=5,RF=CM) as a function of ET(P=5,RF=CM).
description: DESY-HERA. Measurement of the cross sections for inclusive dijet and trijet production in DIS collisions of 27.5 GeV electrons and positrons with 920 GeV protons at a centre-of-mass energy of 318 GeV. The data, which correspond to an integrated luminosity of 82 pb-1, were collected during the 1998-2000 running period and cover the Q**2 region from 10 to 100 GeV and low Bjorken-X region from 0.0001 to 0.01. Jets were identified in the hadronic centre-of-mass frame using the KT cluster algorithm in the longitudinally invariant inclusive mode. The second systematic (DSYS) error in the tables is from the uncertainty in the jet energy scale. In the nomenclature used here the jets are ordered in ET, namely P=4 is the jet of highest ET.. Numerical values supplied by T Daniels.
DOI: 10.17182/hepdata.45528.v1/t5
title: "Table 5" of "Multijet production at low x(Bj) in deep inelastic scattering at HERA."

description: Two jet cross section D(SIG)/DETARAP(P=4,RF=LAB) as a function of ETARAP(P=4,RF=LAB).
description: DESY-HERA. Measurement of the cross sections for inclusive dijet and trijet production in DIS collisions of 27.5 GeV electrons and positrons with 920 GeV protons at a centre-of-mass energy of 318 GeV. The data, which correspond to an integrated luminosity of 82 pb-1, were collected during the 1998-2000 running period and cover the Q**2 region from 10 to 100 GeV and low Bjorken-X region from 0.0001 to 0.01. Jets were identified in the hadronic centre-of-mass frame using the KT cluster algorithm in the longitudinally invariant inclusive mode. The second systematic (DSYS) error in the tables is from the uncertainty in the jet energy scale. In the nomenclature used here the jets are ordered in ET, namely P=4 is the jet of highest ET.. Numerical values supplied by T Daniels.
DOI: 10.17182/hepdata.45528.v1/t10
title: "Table 10" of "Multijet production at low x(Bj) in deep inelastic scattering at HERA."

description: Two jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).
description: DESY-HERA. Measurement of the cross sections for inclusive dijet and trijet production in DIS collisions of 27.5 GeV electrons and positrons with 920 GeV protons at a centre-of-mass energy of 318 GeV. The data, which correspond to an integrated luminosity of 82 pb-1, were collected during the 1998-2000 running period and cover the Q**2 region from 10 to 100 GeV and low Bjorken-X region from 0.0001 to 0.01. Jets were identified in the hadronic centre-of-mass frame using the KT cluster algorithm in the longitudinally invariant inclusive mode. The second systematic (DSYS) error in the tables is from the uncertainty in the jet energy scale. In the nomenclature used here the jets are ordered in ET, namely P=4 is the jet of highest ET.. Numerical values supplied by T Daniels.
DOI: 10.17182/hepdata.45528.v1/t11
title: "Table 11" of "Multijet production at low x(Bj) in deep inelastic scattering at HERA."

description: Two jet cross section D2(SIG)/D(ET(P=4,RF=CM)-ET(P=5,RF=CM))/DX as a function of ET(P=4,RF=CM)-ET(P=5,RF=CM).
description: DESY-HERA. Measurement of the cross sections for inclusive dijet and trijet production in DIS collisions of 27.5 GeV electrons and positrons with 920 GeV protons at a centre-of-mass energy of 318 GeV. The data, which correspond to an integrated luminosity of 82 pb-1, were collected during the 1998-2000 running period and cover the Q**2 region from 10 to 100 GeV and low Bjorken-X region from 0.0001 to 0.01. Jets were identified in the hadronic centre-of-mass frame using the KT cluster algorithm in the longitudinally invariant inclusive mode. The second systematic (DSYS) error in the tables is from the uncertainty in the jet energy scale. In the nomenclature used here the jets are ordered in ET, namely P=4 is the jet of highest ET.. Numerical values supplied by T Daniels.