{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.14860.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/324035"}},{"@id":"https://doi.org/10.1007/BF01560444","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"DELPHI Collaboration"},"creator":{"@type":"Organization","name":"DELPHI Collaboration"},"datePublished":"1992","description":"CERN-LEP. Measurement of charged particle multiplicities in restricted rapidity intervals in Z0 hadronic decays by the Delphi Collaboration.. The data reveal the presence of a shoulder structure which is further studied by examining multiplicity distributions for 2-, 3-, and 4-jet events. Structure is found to be due to important contributions from 3- and 4-jet events with a hard gluon jet.. Rapidity is calculated with respect to the thrust axis assuming a pion mass for all particles. Data are given for particles emitted in the central rapidity intervals as well as the subset of particles emitted in a single hemisphere defined by the plane perpendicular to the thrust axis.. Errors in nearby bins are strongly correlated.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t1","@type":"Dataset","description":"Data for both hemispheres.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t2","@type":"Dataset","description":"Data for both hemispheres.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t3","@type":"Dataset","description":"Data for both hemispheres.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t4","@type":"Dataset","description":"Data for both hemispheres.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t5","@type":"Dataset","description":"Data for both hemispheres. All rapidity regions.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t6","@type":"Dataset","description":"Data for single hemisphere.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t7","@type":"Dataset","description":"Data for single hemisphere.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t8","@type":"Dataset","description":"Data for single hemisphere.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t9","@type":"Dataset","description":"Data for single hemisphere.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t10","@type":"Dataset","description":"Data for single hemisphere.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t11","@type":"Dataset","description":"Data for single hemisphere.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t12","@type":"Dataset","description":"Data for single hemisphere.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t13","@type":"Dataset","description":"Data for single hemisphere. All rapidity regions.","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t14","@type":"Dataset","description":"Multiplicity moments in central rapidity intervals.. CQ is defined as MEAN(MULT**Q)/MEAN(MULT)**Q.","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.14860.v1/t15","@type":"Dataset","description":"Multiplicity moments in a single hemisphere.. CQ is defined as MEAN(MULT**Q)/MEAN(MULT)**Q.","name":"Table 15"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins324035?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/14860"}],"inLanguage":"en","name":"Charged particle multiplicity distributions in restricted rapidity intervals in Z0 hadronic decays.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins324035?version=1","version":1}