{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.14774.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/321190"}},{"@id":"https://doi.org/10.1007/BF01559731","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"OPAL Collaboration"},"creator":{"@type":"Organization","name":"OPAL Collaboration"},"datePublished":"1992","description":"CERN-LEP. Study of charged particle multplicities in hadronic decays of the Z0 by the OPAL Collaboration. Data come from 82,941 events collected within 100 MeV of the Z0 peak, and are fully corrected for initial-state radiation, and detector acceptance and resolution.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.14774.v1/t1","@type":"Dataset","description":"Distribution for whole event. The data at multiplicites 2 and 4 come from Monte Carlo data.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.14774.v1/t2","@type":"Dataset","description":"Distribution for single hemisphere.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.14774.v1/t3","@type":"Dataset","description":"Distribution for whole event. The data at multiplicites 2 and 4 come from Monte Carlo data.. Contributions from K0S and...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.14774.v1/t4","@type":"Dataset","description":"Distribution for single hemisphere.. Contributions from K0S and LAMBDA decays have been subtracted.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.14774.v1/t5","@type":"Dataset","description":"Moments of multiplicity distributions for whole event data.. MULTQ(NAME=CQ) is defined as MEAN(MULT**Q)/MEAN(MULT**Q).","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.14774.v1/t6","@type":"Dataset","description":"Moments of multiplicity distributions for single hemisphere data.. MULTQ(NAME=CQ) is defined as MEAN(MULT**Q)/MEAN(MULT**Q).","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.14774.v1/t7","@type":"Dataset","description":"Moments of multiplicity distributions for whole event data.. MULTQ(NAME=CQ) is defined as MEAN(MULT**Q)/MEAN(MULT**Q). Contributions from K0S and LAMBDA decays have...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.14774.v1/t8","@type":"Dataset","description":"Moments of multiplicity distributions for single hemisphere data.. MULTQ(NAME=CQ) is defined as MEAN(MULT**Q)/MEAN(MULT**Q). Contributions from K0S and LAMBDA decays have...","name":"Table 8"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins321190?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/14774"}],"inLanguage":"en","name":"A Study of charged particle multiplicities in hadronic decays of the Z0","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins321190?version=1","version":1}