cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.13245.v1/t12
title: "Table 12" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Wide Jet Broadening BMAX.
description: CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the final ALPHA-S values together with the event shape distributions integrated over all THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the Energy Energy Correlation and it Asymmetry and the JetCone Enegy Fraction in 8 ranges of THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the normalized event shape distributions in 8 THETA ranges.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the differential two jet rates in a variety of different jet schemes, as a function of the jet separation parameter YCUT, in 8 THETA ranges.
DOI: 10.17182/hepdata.13245.v1/t13
title: "Table 13" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Total Jet Broadening BSUM.
description: CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the final ALPHA-S values together with the event shape distributions integrated over all THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the Energy Energy Correlation and it Asymmetry and the JetCone Enegy Fraction in 8 ranges of THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the normalized event shape distributions in 8 THETA ranges.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the differential two jet rates in a variety of different jet schemes, as a function of the jet separation parameter YCUT, in 8 THETA ranges.
DOI: 10.17182/hepdata.13245.v1/t14
title: "Table 14" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Differential 2-Jet Rate E0 Scheme D2(E0).
description: CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the final ALPHA-S values together with the event shape distributions integrated over all THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the Energy Energy Correlation and it Asymmetry and the JetCone Enegy Fraction in 8 ranges of THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the normalized event shape distributions in 8 THETA ranges.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the differential two jet rates in a variety of different jet schemes, as a function of the jet separation parameter YCUT, in 8 THETA ranges.
DOI: 10.17182/hepdata.13245.v1/t7
title: "Table 7" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Oblateness O.
description: CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the final ALPHA-S values together with the event shape distributions integrated over all THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the Energy Energy Correlation and it Asymmetry and the JetCone Enegy Fraction in 8 ranges of THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the normalized event shape distributions in 8 THETA ranges.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the differential two jet rates in a variety of different jet schemes, as a function of the jet separation parameter YCUT, in 8 THETA ranges.
DOI: 10.17182/hepdata.13245.v1/t8
title: "Table 8" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: C-Parameter C.
description: CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the final ALPHA-S values together with the event shape distributions integrated over all THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the Energy Energy Correlation and it Asymmetry and the JetCone Enegy Fraction in 8 ranges of THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the normalized event shape distributions in 8 THETA ranges.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the differential two jet rates in a variety of different jet schemes, as a function of the jet separation parameter YCUT, in 8 THETA ranges.
DOI: 10.17182/hepdata.13245.v1/t9
title: "Table 9" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Heavy Jet Mass.
description: CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the final ALPHA-S values together with the event shape distributions integrated over all THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the Energy Energy Correlation and it Asymmetry and the JetCone Enegy Fraction in 8 ranges of THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the normalized event shape distributions in 8 THETA ranges.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the differential two jet rates in a variety of different jet schemes, as a function of the jet separation parameter YCUT, in 8 THETA ranges.
DOI: 10.17182/hepdata.13245.v1/t15
title: "Table 15" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Differential 2-Jet Rate P0 Scheme D2(P0).
description: CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the final ALPHA-S values together with the event shape distributions integrated over all THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the Energy Energy Correlation and it Asymmetry and the JetCone Enegy Fraction in 8 ranges of THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the normalized event shape distributions in 8 THETA ranges.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the differential two jet rates in a variety of different jet schemes, as a function of the jet separation parameter YCUT, in 8 THETA ranges.
DOI: 10.17182/hepdata.13245.v1/t16
title: "Table 16" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Differential 2-Jet Rate P Scheme D2(P).
description: CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the final ALPHA-S values together with the event shape distributions integrated over all THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the Energy Energy Correlation and it Asymmetry and the JetCone Enegy Fraction in 8 ranges of THETA.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the normalized event shape distributions in 8 THETA ranges.
CERN-LEP. Determination of ALPHA-S from the measurment of 18 collinear- andinfrared- safe shape distributions as a function of the polar ange (THETA) of t he THRUST axis w.r.t. the E+ E- beam direction. The jet cone energy fraction (JCEF), defined by the integral of the energy within a conical shell of opening angle CHI about the thrust axis, gives the smallest theoretical and experimental uncertainty, and is used separately to determine ALPHA-S. The numerical values of the distributions are taken from the DELPHI report(PHYS-0827). This part gives the distributions of the differential two jet rates in a variety of different jet schemes, as a function of the jet separation parameter YCUT, in 8 THETA ranges.