{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.29273.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/319520"}},{"@id":"https://doi.org/10.1016/0370-2693(91)90575-B","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALEPH Collaboration"},"creator":{"@type":"Organization","name":"ALEPH Collaboration"},"datePublished":"1991","description":"CERN-LEP. ALEPH Collaboration. Measurement of the charged particle multiplicity distribution in hadronic Z decays produced in e+ e- annihilation.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.29273.v1/t1","@type":"Dataset","description":"Unfolded charged particle multiplicity distribution. The entry for N=2 is from the LUND 7.2 parton shower model.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.29273.v1/t2","@type":"Dataset","description":"Leading moments of the charged particle multiplicity. R2 is the second binomial moment given by MEAN(MULT(MULT-1))/(MEAN(MULT))**2.","name":"Table 2"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins319520?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/29273"}],"inLanguage":"en","name":"Measurement of the charged particle multiplicity distribution in hadronic Z decays","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins319520?version=1","version":1}