cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.13245.v1/t27
title: "Table 27" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Asymmetry of the Energy Energy Correlation AEEC.
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/t28
title: "Table 28" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Asymmetry of the Energy Energy Correlation AEEC.
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/t29
title: "Table 29" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Jet Cone Energy Fraction.
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/t30
title: "Table 30" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Jet Cone Energy Fraction.
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/t31
title: "Table 31" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Jet Cone Energy Fraction.
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/t32
title: "Table 32" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: Jet Cone Energy Fraction.
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/t33
title: "Table 33" of "Consistent measurements of alpha(s) from precise oriented event shape distributions."

description: 1 - Thrust (1-T).
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.13342.v1/t1
title: "Table 1" of "Precise Tests of Triple Regge Theory From $\pi^0$ and $\eta$ Inclusive Production in 100-{GeV}/$c \pi^\pm p$ Collisions"

description: No description provided.
description: PLAB=99.2 GEV DATA FROM FERMILAB AT HIGH X. DATA PRESENTED HERE IS A COMPLETE COLLECTION OF THAT IN THE REFERENCE WITH REFINEMENTS THROUGH 13 OCT 1979. DATA IS A COMBINATION OF TWO BEAM ENERGIES. ONE VALUE IS 99.2 GEV, AND THE OTHER IS ABOUT TWO PERCENT LOWER AND HAS BEEN SCALED ACCORDINGLY. FOR DETAILS SEE REFERENCE KENNETT 79 CITED ABOVE.. DATA IS TRIGGER B=TRIGGER FOR -T & gt; 1 GEV2.
DOI: 10.17182/hepdata.13342.v1/t3
title: "Table 3" of "Precise Tests of Triple Regge Theory From $\pi^0$ and $\eta$ Inclusive Production in 100-{GeV}/$c \pi^\pm p$ Collisions"

description: No description provided.
description: PLAB=99.2 GEV DATA FROM FERMILAB AT HIGH X. DATA PRESENTED HERE IS A COMPLETE COLLECTION OF THAT IN THE REFERENCE WITH REFINEMENTS THROUGH 13 OCT 1979. DATA IS A COMBINATION OF TWO BEAM ENERGIES. ONE VALUE IS 99.2 GEV, AND THE OTHER IS ABOUT TWO PERCENT LOWER AND HAS BEEN SCALED ACCORDINGLY. FOR DETAILS SEE REFERENCE KENNETT 79 CITED ABOVE.. DATA IS TRIGGER B=TRIGGER FOR -T & gt; 1 GEV2.
DOI: 10.17182/hepdata.13342.v1/t2
title: "Table 2" of "Precise Tests of Triple Regge Theory From $\pi^0$ and $\eta$ Inclusive Production in 100-{GeV}/$c \pi^\pm p$ Collisions"

description: No description provided.
description: PLAB=99.2 GEV DATA FROM FERMILAB AT HIGH X. DATA PRESENTED HERE IS A COMPLETE COLLECTION OF THAT IN THE REFERENCE WITH REFINEMENTS THROUGH 13 OCT 1979. DATA IS A COMBINATION OF TWO BEAM ENERGIES. ONE VALUE IS 99.2 GEV, AND THE OTHER IS ABOUT TWO PERCENT LOWER AND HAS BEEN SCALED ACCORDINGLY. FOR DETAILS SEE REFERENCE KENNETT 79 CITED ABOVE.. DATA IS TRIGGER B=TRIGGER FOR -T & gt; 1 GEV2.
DOI: 10.17182/hepdata.13342.v1/t4
title: "Table 4" of "Precise Tests of Triple Regge Theory From $\pi^0$ and $\eta$ Inclusive Production in 100-{GeV}/$c \pi^\pm p$ Collisions"

description: No description provided.
description: PLAB=99.2 GEV DATA FROM FERMILAB AT HIGH X. DATA PRESENTED HERE IS A COMPLETE COLLECTION OF THAT IN THE REFERENCE WITH REFINEMENTS THROUGH 13 OCT 1979. DATA IS A COMBINATION OF TWO BEAM ENERGIES. ONE VALUE IS 99.2 GEV, AND THE OTHER IS ABOUT TWO PERCENT LOWER AND HAS BEEN SCALED ACCORDINGLY. FOR DETAILS SEE REFERENCE KENNETT 79 CITED ABOVE.. DATA IS TRIGGER B=TRIGGER FOR -T & gt; 1 GEV2.
DOI: 10.17182/hepdata.13342.v1/t5
title: "Table 5" of "Precise Tests of Triple Regge Theory From $\pi^0$ and $\eta$ Inclusive Production in 100-{GeV}/$c \pi^\pm p$ Collisions"

description: No description provided.
description: PLAB=99.2 GEV DATA FROM FERMILAB AT HIGH X. DATA PRESENTED HERE IS A COMPLETE COLLECTION OF THAT IN THE REFERENCE WITH REFINEMENTS THROUGH 13 OCT 1979. DATA IS A COMBINATION OF TWO BEAM ENERGIES. ONE VALUE IS 99.2 GEV, AND THE OTHER IS ABOUT TWO PERCENT LOWER AND HAS BEEN SCALED ACCORDINGLY. FOR DETAILS SEE REFERENCE KENNETT 79 CITED ABOVE.. DATA IS TRIGGER B=TRIGGER FOR -T & gt; 1 GEV2.
DOI: 10.17182/hepdata.13342.v1/t6
title: "Table 6" of "Precise Tests of Triple Regge Theory From $\pi^0$ and $\eta$ Inclusive Production in 100-{GeV}/$c \pi^\pm p$ Collisions"

description: No description provided.
description: PLAB=99.2 GEV DATA FROM FERMILAB AT HIGH X. DATA PRESENTED HERE IS A COMPLETE COLLECTION OF THAT IN THE REFERENCE WITH REFINEMENTS THROUGH 13 OCT 1979. DATA IS A COMBINATION OF TWO BEAM ENERGIES. ONE VALUE IS 99.2 GEV, AND THE OTHER IS ABOUT TWO PERCENT LOWER AND HAS BEEN SCALED ACCORDINGLY. FOR DETAILS SEE REFERENCE KENNETT 79 CITED ABOVE.. DATA IS TRIGGER B=TRIGGER FOR -T & gt; 1 GEV2.
DOI: 10.17182/hepdata.13342.v1/t7
title: "Table 7" of "Precise Tests of Triple Regge Theory From $\pi^0$ and $\eta$ Inclusive Production in 100-{GeV}/$c \pi^\pm p$ Collisions"

description: No description provided.
description: PLAB=99.2 GEV DATA FROM FERMILAB AT HIGH X. DATA PRESENTED HERE IS A COMPLETE COLLECTION OF THAT IN THE REFERENCE WITH REFINEMENTS THROUGH 13 OCT 1979. DATA IS A COMBINATION OF TWO BEAM ENERGIES. ONE VALUE IS 99.2 GEV, AND THE OTHER IS ABOUT TWO PERCENT LOWER AND HAS BEEN SCALED ACCORDINGLY. FOR DETAILS SEE REFERENCE KENNETT 79 CITED ABOVE.. DATA IS TRIGGER B=TRIGGER FOR -T & gt; 1 GEV2.