cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.49741.v1/t7
title: "Table 7" of "Determination of alpha(s) from hadronic event shapes in e+ e- annihilation at 192-GeV &lt;= s**(1/2) &lt;= 208-GeV"

description: The corrected distributions for the total jet broadening, BT.
description: CERN-LEP. Determination of the strong coupling constant ALPHA_S from the measured distributions of five event shape variables, THRUST, Heavy Jet Mass RHO, Total Jet Broadening BT, Wide Jet Broadening BW, and C-Parameter C-PARAM. The analysis is based on 436.8 PB-1 of E+ E- collision data at centre-of-mass energiesbetween 192 and 208 GeV. Previous published L3 data at lower energies is reanal ysed using the same analysis methods as in this paper and the results from theseare also presented. Numerical values of the event shape distributions have been supplied by S Bannerjee.
DOI: 10.17182/hepdata.49741.v1/t8
title: "Table 8" of "Determination of alpha(s) from hadronic event shapes in e+ e- annihilation at 192-GeV &lt;= s**(1/2) &lt;= 208-GeV"

description: The corrected distributions for the wide jet broadening, BW.
description: CERN-LEP. Determination of the strong coupling constant ALPHA_S from the measured distributions of five event shape variables, THRUST, Heavy Jet Mass RHO, Total Jet Broadening BT, Wide Jet Broadening BW, and C-Parameter C-PARAM. The analysis is based on 436.8 PB-1 of E+ E- collision data at centre-of-mass energiesbetween 192 and 208 GeV. Previous published L3 data at lower energies is reanal ysed using the same analysis methods as in this paper and the results from theseare also presented. Numerical values of the event shape distributions have been supplied by S Bannerjee.
DOI: 10.17182/hepdata.49741.v1/t9
title: "Table 9" of "Determination of alpha(s) from hadronic event shapes in e+ e- annihilation at 192-GeV &lt;= s**(1/2) &lt;= 208-GeV"

description: The corrected distributions for the C-parameter, C-PARAM.
description: CERN-LEP. Determination of the strong coupling constant ALPHA_S from the measured distributions of five event shape variables, THRUST, Heavy Jet Mass RHO, Total Jet Broadening BT, Wide Jet Broadening BW, and C-Parameter C-PARAM. The analysis is based on 436.8 PB-1 of E+ E- collision data at centre-of-mass energiesbetween 192 and 208 GeV. Previous published L3 data at lower energies is reanal ysed using the same analysis methods as in this paper and the results from theseare also presented. Numerical values of the event shape distributions have been supplied by S Bannerjee.
DOI: 10.17182/hepdata.49742.v1/t1
title: "Table 1" of "Particle multiplicity of unbiased gluon jets from e+ e- three jet events"

description: Measurements of the mean charged particle multiplicity of biased two-jet uds flavour events from Z0 decays as a function of the transverse momentum cutoff PT(C=LU) used to separate two- and three-jet events.
description: CERN-LEP. Measurement of the charged particle multiplicities of two- and three-jet events in hadron production from E+ E- interactions at energies around the Z0 mass. Jets are defined using the Durham jet finder but checked using the Cambridge and Luclus jet finders.
DOI: 10.17182/hepdata.49742.v1/t2
title: "Table 2" of "Particle multiplicity of unbiased gluon jets from e+ e- three jet events"

description: Measurements of the mean charged particle multiplicity of three-jet uds flavour 'Y events' from Z0 decays, as a function of the angle THETA1 between the lowest two energy jets. The results for the quark jet scale SQRT(S(C=QQBAR)) and the gluon jet scales PT(C=LU) and PT(C=LE) are also given.
description: CERN-LEP. Measurement of the charged particle multiplicities of two- and three-jet events in hadron production from E+ E- interactions at energies around the Z0 mass. Jets are defined using the Durham jet finder but checked using the Cambridge and Luclus jet finders.
DOI: 10.17182/hepdata.49742.v1/t3
title: "Table 3" of "Particle multiplicity of unbiased gluon jets from e+ e- three jet events"

description: Measurements of the unbiased gluon multiplicity as a function of the energy scale Q=PT(C=LU). The corresponding bins of THETA1 in 'Y events' are also indicated.
description: CERN-LEP. Measurement of the charged particle multiplicities of two- and three-jet events in hadron production from E+ E- interactions at energies around the Z0 mass. Jets are defined using the Durham jet finder but checked using the Cambridge and Luclus jet finders.
DOI: 10.17182/hepdata.49742.v1/t4
title: "Table 4" of "Particle multiplicity of unbiased gluon jets from e+ e- three jet events"

description: Measurements of unbiased gluon jet multiplicity as a function of the energy scale Q=PT(C=LE).
description: CERN-LEP. Measurement of the charged particle multiplicities of two- and three-jet events in hadron production from E+ E- interactions at energies around the Z0 mass. Jets are defined using the Durham jet finder but checked using the Cambridge and Luclus jet finders.
DOI: 10.17182/hepdata.49743.v1/t1
title: "Table 1" of "Measurement of the branching ratio for the process b --&gt; tau- anti-nu/tau X."

description: TAN(BETA) is the two-Higgs-doublet model parameter, while M_H is the mass of charged Higgs.
description: CERN-LEP.
DOI: 10.17182/hepdata.49744.v1/t1
title: "Table 1" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: F2 and DSIG/DX for the EE sample in the high Q**2 region as a function of X.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t2
title: "Table 2" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: Statistical correlations between the bins in the preceding table.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t3
title: "Table 3" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: The measured value of F2 and DSIG/DX for the SW data sample in the Q**2 range 9 to 15 GeV**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t4
title: "Table 4" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: The measured value of F2 and DSIG/DX for the SW data sample in the Q**2 range 15 to 30 GeV**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t5
title: "Table 5" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: The measured value of F2 and DSIG/DX for the FD data sample in the Q**2 range 30 to 50 GeV**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t6
title: "Table 6" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: The measured value of F2 and DSIG/DX for the FD data sample in the Q**2 range 50 to 150 GeV**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t7
title: "Table 7" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: The measured value of F2 and DSIG/DX for the EE data sample in the Q**2 range 400 to 2350 GeV**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t8
title: "Table 8" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: Statistical correlation between the bins for mean Q**2 value 12.1 GeV**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t9
title: "Table 9" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: Statistical correlation between the bins for mean Q**2 value 19.9 GeV**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t10
title: "Table 10" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: Statistical correlation between the bins for mean Q**2 value 39.7 GeV**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t11
title: "Table 11" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: Statistical correlation between the bins for mean Q**2 value 76.4 GeV**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t12
title: "Table 12" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: Statistical correlation between the bins for mean Q**2 value 780 GeV**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49744.v1/t13
title: "Table 13" of "Measurement of the hadronic photon structure function F2(gamma) at LEP2."

description: F2 and DSIG/DX over the full X range 0.10 to 0.60 as a function of Q**2.
description: CERN-LEP. Measurement of the hadronic structure function F2(C=GAMMA) as a function of Bjorken X and photon virtuality Q**2 using DIS data taken for E+ E- collisions at c.m. energy 183 to 209 GeV (mean=197.1) using the EE (endcap calorimeter), FD (forward calorimeter) and SW (silicon tungsten detector) data. The evolution of F2 is studied in Q**2 from 12.1 to 780 GeV**2 for the central X region 0.10 to 0.60. The data come from the 1997 - 2000 LEP running period with an integrated luminosity of 632 pb-1.. In the following tables RAD-CORR is the difference of the radiative and non-radiative corrections as a percentage of the non-radiative correction. BIN-CORR is the bin-centre correction used as a percentage of the non-corrected F2.
DOI: 10.17182/hepdata.49750.v1/t1
title: "Table 1" of "Measurement of Z / gamma* production in Compton scattering of quasi-real photons."

description: Measured values of the cross section times the branching ratio for the (Z0/GAMMA*) decay into hadrons within the restricted kinematic limits.
description: CERN-LEP. Measurment of the cross sections, times the branching ratio of (Z0/GAMMA*)into hadrons, for the quasi-real photon Compton scattering process in the react ion E+ E- --& gt; E+ E- Z0/GAMMA*. The differential cross sections of the Mandelstamvariables S-HAT, T-HAT and U-HAT are presented as well as the total cross secti on within Lorentz invariant kinematic limits. Correlation matrices between the measured and generated distributions for each variable are determined and also presented here.. The numerical values were supplied by Ivor Fleck.
DOI: 10.17182/hepdata.49750.v1/t2
title: "Table 2" of "Measurement of Z / gamma* production in Compton scattering of quasi-real photons."

description: Differential cross-section dsig_ee/dm_qq.
description: CERN-LEP. Measurment of the cross sections, times the branching ratio of (Z0/GAMMA*)into hadrons, for the quasi-real photon Compton scattering process in the react ion E+ E- --& gt; E+ E- Z0/GAMMA*. The differential cross sections of the Mandelstamvariables S-HAT, T-HAT and U-HAT are presented as well as the total cross secti on within Lorentz invariant kinematic limits. Correlation matrices between the measured and generated distributions for each variable are determined and also presented here.. The numerical values were supplied by Ivor Fleck.
DOI: 10.17182/hepdata.49750.v1/t3
title: "Table 3" of "Measurement of Z / gamma* production in Compton scattering of quasi-real photons."

description: Differential cross-section dsigma_ee/dsqrt(shat).
description: CERN-LEP. Measurment of the cross sections, times the branching ratio of (Z0/GAMMA*)into hadrons, for the quasi-real photon Compton scattering process in the react ion E+ E- --& gt; E+ E- Z0/GAMMA*. The differential cross sections of the Mandelstamvariables S-HAT, T-HAT and U-HAT are presented as well as the total cross secti on within Lorentz invariant kinematic limits. Correlation matrices between the measured and generated distributions for each variable are determined and also presented here.. The numerical values were supplied by Ivor Fleck.
DOI: 10.17182/hepdata.49750.v1/t4
title: "Table 4" of "Measurement of Z / gamma* production in Compton scattering of quasi-real photons."

description: Differential cross-section dsig_ee/d(that).
description: CERN-LEP. Measurment of the cross sections, times the branching ratio of (Z0/GAMMA*)into hadrons, for the quasi-real photon Compton scattering process in the react ion E+ E- --& gt; E+ E- Z0/GAMMA*. The differential cross sections of the Mandelstamvariables S-HAT, T-HAT and U-HAT are presented as well as the total cross secti on within Lorentz invariant kinematic limits. Correlation matrices between the measured and generated distributions for each variable are determined and also presented here.. The numerical values were supplied by Ivor Fleck.
DOI: 10.17182/hepdata.49750.v1/t5
title: "Table 5" of "Measurement of Z / gamma* production in Compton scattering of quasi-real photons."

description: Differential cross-section dsig_ee/d(uhat).
description: CERN-LEP. Measurment of the cross sections, times the branching ratio of (Z0/GAMMA*)into hadrons, for the quasi-real photon Compton scattering process in the react ion E+ E- --& gt; E+ E- Z0/GAMMA*. The differential cross sections of the Mandelstamvariables S-HAT, T-HAT and U-HAT are presented as well as the total cross secti on within Lorentz invariant kinematic limits. Correlation matrices between the measured and generated distributions for each variable are determined and also presented here.. The numerical values were supplied by Ivor Fleck.
DOI: 10.17182/hepdata.49750.v1/t6
title: "Table 6" of "Measurement of Z / gamma* production in Compton scattering of quasi-real photons."

description: Differential cross-section dsig_eg/dm_qq.
description: CERN-LEP. Measurment of the cross sections, times the branching ratio of (Z0/GAMMA*)into hadrons, for the quasi-real photon Compton scattering process in the react ion E+ E- --& gt; E+ E- Z0/GAMMA*. The differential cross sections of the Mandelstamvariables S-HAT, T-HAT and U-HAT are presented as well as the total cross secti on within Lorentz invariant kinematic limits. Correlation matrices between the measured and generated distributions for each variable are determined and also presented here.. The numerical values were supplied by Ivor Fleck.
DOI: 10.17182/hepdata.49750.v1/t7
title: "Table 7" of "Measurement of Z / gamma* production in Compton scattering of quasi-real photons."

description: Cross-section sigma_eg v. sqrt(shat).
description: CERN-LEP. Measurment of the cross sections, times the branching ratio of (Z0/GAMMA*)into hadrons, for the quasi-real photon Compton scattering process in the react ion E+ E- --& gt; E+ E- Z0/GAMMA*. The differential cross sections of the Mandelstamvariables S-HAT, T-HAT and U-HAT are presented as well as the total cross secti on within Lorentz invariant kinematic limits. Correlation matrices between the measured and generated distributions for each variable are determined and also presented here.. The numerical values were supplied by Ivor Fleck.
DOI: 10.17182/hepdata.49750.v1/t8
title: "Table 8" of "Measurement of Z / gamma* production in Compton scattering of quasi-real photons."

description: Differential cross-section dsig_eg/d(that).
description: CERN-LEP. Measurment of the cross sections, times the branching ratio of (Z0/GAMMA*)into hadrons, for the quasi-real photon Compton scattering process in the react ion E+ E- --& gt; E+ E- Z0/GAMMA*. The differential cross sections of the Mandelstamvariables S-HAT, T-HAT and U-HAT are presented as well as the total cross secti on within Lorentz invariant kinematic limits. Correlation matrices between the measured and generated distributions for each variable are determined and also presented here.. The numerical values were supplied by Ivor Fleck.