{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.47800.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/424112"}},{"@id":"https://doi.org/10.1007/s002880050295","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"DELPHI Collaboration"},"creator":{"@type":"Organization","name":"DELPHI Collaboration"},"datePublished":"1996","description":"CERN-LEP. Measurement of event-shape and charged particle inclusive distributions in 750000 decays of the Z0 to hadrons.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t1","@type":"Dataset","description":"Transverse momentum PTIN w.r.t. the Thrust axis. For the first table Thrust axis definition is from seen charged particles corrected...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t2","@type":"Dataset","description":"Transverse momentum PTOUT w.r.t. the Thrust axis. For the first table Thrust axis definition is from seen charged particles corrected...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t3","@type":"Dataset","description":"Transverse momentum PTIN w.r.t. the Sphericity axis. For the first table Sphericity axis definition is from seen charged particles corrected...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t4","@type":"Dataset","description":"Transverse momentum PTOUT w.r.t. the Shericity axis. For the first table Sphericity axis definition is from seen charged particles corrected...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t5","@type":"Dataset","description":"Rapidity, YT, w.r.t. the Thrust axis. For the first table Thrust axis definition is from seen charged particles corrected to...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t6","@type":"Dataset","description":"Rapidity, YS, w.r.t. the Sphericity axis. For the first table Sphericity axis definition is from seen charged particles corrected to...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t7","@type":"Dataset","description":"Scaled momentum distribution, XP. Corrected to final state charged particles.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t8","@type":"Dataset","description":"LN(1/XP) distribution. Corrected to final state charged particles.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t9","@type":"Dataset","description":"Mean PTOUT V XP. Corrected to final state charged particles.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t10","@type":"Dataset","description":"Mean PT V XP. Corrected to final state charged particles.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t11","@type":"Dataset","description":"1-Thrust distribution. Corrected to final state particles.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t12","@type":"Dataset","description":"Thrust Major distribution. Corrected to final state particles.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t13","@type":"Dataset","description":"Thrust Minor distribution. Corrected to final state particles.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t14","@type":"Dataset","description":"Oblateness distribution. Corrected to final state particles.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t15","@type":"Dataset","description":"Sphericity distribution. Corrected to final state particles.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t16","@type":"Dataset","description":"Aplanarity distribution. Corrected to final state particles.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t17","@type":"Dataset","description":"Planarity distribution. Corrected to final state particles.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t18","@type":"Dataset","description":"C-Parameter distribution. Corrected to final state particles.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t19","@type":"Dataset","description":"D-Parameter distribution. Corrected to final state particles.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t20","@type":"Dataset","description":"Heavy-Hemisphere-Mass distribution. Corrected to final state particles.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t21","@type":"Dataset","description":"Light-Hemisphere-Mass distribution. Corrected to final state particles.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t22","@type":"Dataset","description":"Difference in Hemisphere Masses. Corrected to final state particles.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t23","@type":"Dataset","description":"Wide Hemisphere Broadening, BMAX. Corrected to final state particles.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t24","@type":"Dataset","description":"Narrow Hemisphere Broadening, BMIN. Corrected to final state particles.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t25","@type":"Dataset","description":"Total Hemisphere Broadening, BSUM. Corrected to final state particles.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t26","@type":"Dataset","description":"Difference of the Hemisphere Broadening, BDIFF. Corrected to final state particles.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t27","@type":"Dataset","description":"Differential 2-jet rate for the Durham Algorithm. Corrected to final state particles. YCUT is the jet finding cutt-off parameter.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t28","@type":"Dataset","description":"Differential 2-jet rate for the JADE Algorithm. Corrected to final state particles. YCUT is the jet finding cutt-off parameter.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t29","@type":"Dataset","description":"Differential 3-jet rate for the Durham Algorithm. Corrected to final state particles. YCUT is the jet finding cutt-off parameter.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t30","@type":"Dataset","description":"Differential 3-jet rate for the JADE Algorithm. Corrected to final state particles. YCUT is the jet finding cutt-off parameter.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t31","@type":"Dataset","description":"Differential 4-jet rate for the Durham Algorithm. Corrected to final state particles. YCUT is the jet finding cutt-off parameter.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t32","@type":"Dataset","description":"Differential 4-jet rate for the JADE Algorithm. Corrected to final state particles. YCUT is the jet finding cutt-off parameter.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t33","@type":"Dataset","description":"Energy-Energy Correlation EEC. Corrected to final state particles.","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t34","@type":"Dataset","description":"Asymmetry of the Energy-Energy Correlation AEEC. Corrected to final state particles.","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t35","@type":"Dataset","description":"Charged particle multiplicity compiled from current LEP I data.","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t36","@type":"Dataset","description":"Compilation of multiplicities of pseudoscalar mesons from current LEP I data.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t37","@type":"Dataset","description":"Compilation of multiplicities of scalar mesons from current LEP I data.","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t38","@type":"Dataset","description":"Compilation of multiplicities of vector mesons from current LEP I data.","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t39","@type":"Dataset","description":"Compilation of multiplicities of tensor mesons from current LEP I data.","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t40","@type":"Dataset","description":"Compilation of multiplicities of baryons from current LEP I data.","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t41","@type":"Dataset","description":"LOG(1/XP) distribution for K0 production.. Data read from plot.","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t42","@type":"Dataset","description":"LOG(1/XP) distribution for K+- production.. Data read from plot.","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t43","@type":"Dataset","description":"XP distribution for K*(892)0 production.. Data read from plot.","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t44","@type":"Dataset","description":"XP distribution for K*(892)+- production.. Data read from plot.","name":"Table 44"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t45","@type":"Dataset","description":"XE distribution for PHI production.. Data read from plot.","name":"Table 45"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t46","@type":"Dataset","description":"XP distribution for RHO0 production.. Data read from plot.","name":"Table 46"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t47","@type":"Dataset","description":"XP distribution for F0(980) production.. Data read from plot.","name":"Table 47"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t48","@type":"Dataset","description":"XP distribution for F2(1270) production.. Data read from plot.","name":"Table 48"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t49","@type":"Dataset","description":"LOG(1/XP) distribution for P production.. Data read from plot.","name":"Table 49"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t50","@type":"Dataset","description":"LOG(1/XP) distribution for LAMBDA production.. Data read from plot.","name":"Table 50"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t51","@type":"Dataset","description":"XP distribution for P production.. Data read from plot.","name":"Table 51"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t52","@type":"Dataset","description":"XP distribution for LAMBDA production.. Data read from plot.","name":"Table 52"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t53","@type":"Dataset","description":"XP distribution for XI+- production.. Data read from plot.","name":"Table 53"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t54","@type":"Dataset","description":"XP distribution for DEL++ production.. Data read from plot.","name":"Table 54"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t55","@type":"Dataset","description":"XP distribution for SIGMA(1385)+ production.. Data read from plot.","name":"Table 55"},{"@id":"https://doi.org/10.17182/hepdata.47800.v1/t56","@type":"Dataset","description":"XP distribution for XI(1530)0 production.. Data read from plot.","name":"Table 56"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins424112?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/47800"}],"inLanguage":"en","name":"Tuning and test of fragmentation models based on identified particles and precision event shape data.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins424112?version=1","version":1}