{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.47582.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/428072"}},{"@id":"https://doi.org/10.1016/S0370-1573(97)00045-8","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALEPH Collaboration"},"creator":{"@type":"Organization","name":"ALEPH Collaboration"},"datePublished":"1997","description":"CERN-LEP. Review of all data from ALEPH on QCD including multiplicities, jet rates and identified particle distributions. Some of the data is new and previously unpublished, and some has been published before. All is coded here for completeness. To appear in Physics Reports.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t1","@type":"Dataset","description":"Charged particle sphericity distribution.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t2","@type":"Dataset","description":"Charged particle aplanarity distribution.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t3","@type":"Dataset","description":"Charged particle Thrust distribution.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t4","@type":"Dataset","description":"Charged particle Thrust(minor) distribution.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t5","@type":"Dataset","description":"Charged particle Two-jet resolution variable, Y3 distribution.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t6","@type":"Dataset","description":"Charged particle Heavy Jet Mass distribution.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t7","@type":"Dataset","description":"Charged particle C-Parameter distribution.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t8","@type":"Dataset","description":"Charged particle Oblateness distribution.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t9","@type":"Dataset","description":"Charged particle XP distribution.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t10","@type":"Dataset","description":"Charged particle rapidity distribution.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t11","@type":"Dataset","description":"Charged particle PTIN distribution.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t12","@type":"Dataset","description":"Charged particle PTOUT distribution.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t13","@type":"Dataset","description":"Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t14","@type":"Dataset","description":"Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t15","@type":"Dataset","description":"Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t16","@type":"Dataset","description":"Measure n-jet rates using the Durham cluster algorithm as a function of thejet-resolution parameter YCUT.","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t17","@type":"Dataset","description":"Charged particle inclusive distribution of -LN(1/X).","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t18","@type":"Dataset","description":"Unfolded charged particle multiplicity distribution giving the probability to have a hadronic Z0 decay with N charged particles.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t19","@type":"Dataset","description":"Values of the mean values of the leading moments of the charged particle multiplicity distribution. R2 is the second binomial...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t20","@type":"Dataset","description":"Unfolded values of the the mean multiplicity and dispersion of the multiplicity distributions integaretd over the rapidity region -0.5 to...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t21","@type":"Dataset","description":"Unfolded values of the the mean multiplicity and dispersion of the multiplicity distributions integrated over the rapidity region -1.0 to...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t22","@type":"Dataset","description":"Unfolded values of the the mean multiplicity and dispersion of the multiplicity distributions integrated over the rapidity region -1.5 to...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t23","@type":"Dataset","description":"Unfolded values of the the mean multiplicity and dispersion of the multiplicity distributions integrated over the rapidity region -2.0 to...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t24","@type":"Dataset","description":"Unfolded values of the the mean multiplicity and dispersion of the multiplicity distribution integrated over the full rapidity region.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t25","@type":"Dataset","description":"Differential cross sections for the inclusive production of PI+-. Additional 3pct systematic uncertainty.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t26","@type":"Dataset","description":"Differential cross sections for the inclusive production of K+-. Additionalsystematic uncertainty 3% above and 5% below X = 0.010.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t27","@type":"Dataset","description":"Differential cross sections for the inclusive production of P PBAR. Additional systematic uncertainty 3% above and 5% below X =...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t28","@type":"Dataset","description":"Measured inclusive photon cross section. Errors contain both statistical and systematic uncertainties.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t29","@type":"Dataset","description":"Measured differential cross section for PI0 production.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t30","@type":"Dataset","description":"Measured fragmentation function at the ETA meson. Additional 6pct systematic error.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t31","@type":"Dataset","description":"Measured fragmentation function at the ETAPRIME meson. Additional 8pct systematic error.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t32","@type":"Dataset","description":"Inclusive K0 spectrum. Additional 2pct normalization error.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t33","@type":"Dataset","description":"Inclusive LAMBDA spectrum. Additional 4pct normalization error.","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t34","@type":"Dataset","description":"Fragmentation distribution for XI production.","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t35","@type":"Dataset","description":"Fragmentation distribution for SIGMA(1385) production.","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t36","@type":"Dataset","description":"Fragmentation distribution for XI(1530) production.","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t37","@type":"Dataset","description":"Differential cross section for RHO0 production.","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t38","@type":"Dataset","description":"Differential cross section for OMEGA production.","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t39","@type":"Dataset","description":"Differential cross section for K*0 production.","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t40","@type":"Dataset","description":"Differential cross section for PHI production.","name":"Table 40"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t41","@type":"Dataset","description":"Differential cross section for K*0 production as a function of the transverse momentum with respect to the Thrust axis.","name":"Table 41"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t42","@type":"Dataset","description":"Differential cross section for PHI production as a function of the transverse momentum with respect to the Thrust axis.","name":"Table 42"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t43","@type":"Dataset","description":"Fragmentation distribution for K*+- production.","name":"Table 43"},{"@id":"https://doi.org/10.17182/hepdata.47582.v1/t44","@type":"Dataset","description":"Mean Multiplicities. Where a second systematic error is given, this is due to the uncertainty in the extrapolation to X...","name":"Table 44"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins428072?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/47582"}],"inLanguage":"en","name":"Studies of quantum chromodynamics with the ALEPH detector","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins428072?version=1","version":1}