{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.13245.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/522656"}},{"@id":"https://doi.org/10.1007/s100520000354","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"DELPHI Collaboration"},"creator":{"@type":"Organization","name":"DELPHI Collaboration"},"datePublished":"2000","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.\nCERN-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.\nCERN-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.\nCERN-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.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t1","@type":"Dataset","description":"The weighted value of ALPHA-S from all the measured observables using experimentally optimized renormalization scale values and corrected for the...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t2","@type":"Dataset","description":"The value of ALPHA-S derived from the JCEF and corrected for heavy quark mass effects. The quoted errors are respectively...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t3","@type":"Dataset","description":"Energy Energy Correlation EEC.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t4","@type":"Dataset","description":"Asymmetry of the Energy Energy Correlation AEEC.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t5","@type":"Dataset","description":"Jet Cone Energy Fraction.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t6","@type":"Dataset","description":"1 - Thrust (1-T).","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t7","@type":"Dataset","description":"Oblateness O.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t8","@type":"Dataset","description":"C-Parameter C.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t9","@type":"Dataset","description":"Heavy Jet Mass.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t10","@type":"Dataset","description":"Sum of the Jet Masses.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t11","@type":"Dataset","description":"Difference of the Jet Masses.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t12","@type":"Dataset","description":"Wide Jet Broadening BMAX.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t13","@type":"Dataset","description":"Total Jet Broadening BSUM.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t14","@type":"Dataset","description":"Differential 2-Jet Rate E0 Scheme D2(E0).","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t15","@type":"Dataset","description":"Differential 2-Jet Rate P0 Scheme D2(P0).","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t16","@type":"Dataset","description":"Differential 2-Jet Rate P Scheme D2(P).","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t17","@type":"Dataset","description":"Differential 2-Jet Rate Jade Alogrithm D2(Jad).","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t18","@type":"Dataset","description":"Differential 2-Jet Rate Durham Alogrithm D2(Dur).","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t19","@type":"Dataset","description":"Differential 2-Jet Rate Geneva Alogrithm D2(Gen).","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t20","@type":"Dataset","description":"Differential 2-Jet Rate Cambridge Alogrithm D2(Cam).","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t21","@type":"Dataset","description":"Energy Energy Correlation EEC.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t22","@type":"Dataset","description":"Energy Energy Correlation EEC.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t23","@type":"Dataset","description":"Energy Energy Correlation EEC.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t24","@type":"Dataset","description":"Energy Energy Correlation EEC.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t25","@type":"Dataset","description":"Asymmetry of the Energy Energy Correlation AEEC.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t26","@type":"Dataset","description":"Asymmetry of the Energy Energy Correlation AEEC.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t27","@type":"Dataset","description":"Asymmetry of the Energy Energy Correlation AEEC.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t28","@type":"Dataset","description":"Asymmetry of the Energy Energy Correlation AEEC.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t29","@type":"Dataset","description":"Jet Cone Energy Fraction.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t30","@type":"Dataset","description":"Jet Cone Energy Fraction.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t31","@type":"Dataset","description":"Jet Cone Energy Fraction.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t32","@type":"Dataset","description":"Jet Cone Energy Fraction.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.13245.v1/t33","@type":"Dataset","description":"1 - Thrust (1-T).","name":"Table 33"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins522656?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/13245"}],"inLanguage":"en","name":"Consistent measurements of alpha(s) from precise oriented event shape distributions.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins522656?version=1","version":1}