{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.23443.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/18502"}},{"@id":"https://doi.org/10.1103/PhysRevD.34.3304","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":[{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Derrick, M."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Gan, K.K."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Kooijman, P."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Loos, J.S."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Musgrave, B."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Price, L.E."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Repond, J."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Schlereth, J."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Sugano, K."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Weiss, J.M."}],"creator":[{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Derrick, M."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Gan, K.K."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Kooijman, P."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Loos, J.S."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Musgrave, B."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Price, L.E."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Repond, J."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Schlereth, J."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Sugano, K."},{"@type":"Person","affiliation":{"@type":"Organization","name":"Argonne"},"name":"Weiss, J.M."}],"datePublished":"1986","description":"SLAC-PEP. HRS Collaboration. 29 Gev e+ e- annihilations. Charged particle multiplicities and single particle rapidity distributions. Inclusive data refer to the full data sample (30K events). Two Jet data has additional sphericity (0.25) and aplanarity (& lt;0.1) cuts (24 K events). Luminosity 185 pb**-1. Some results have been presented earlier in Derrick et al., PL 165B(85)449 (& lt;a href=http://durpdg.dur.ac.uk/scripts/reacsearch.csh/TESTREAC/red+1367& gt; RED = 1367 & lt;/a& gt;) and PL 168B(86)299, (& lt;a href=http://durpdg.dur.ac.uk/scripts/reacsearch.csh/TESTREAC/red+1435& gt; RED = 1435 & lt;/a& gt;).","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t1","@type":"Dataset","description":"Charged particle multiplicity distribution for the Inclusive Data Sample.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t2","@type":"Dataset","description":"Charged particle multiplicity distribution for the Two Jet Data Sample.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t3","@type":"Dataset","description":"Properties of multiplicity distributions for Inclusive Data Sample.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t4","@type":"Dataset","description":"Properties of multiplicity distributions for Two Jet Data Sample.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t5","@type":"Dataset","description":"Single jet charged particle multiplicitydistributions for the Inclusive Data Sample where the events have been divided into two back to...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t6","@type":"Dataset","description":"Single jet charged particle multiplicity distributions for the Two Jet Data Sample where the events have been divided into two...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t7","@type":"Dataset","description":"Properties of single jet multiplicity distributions for the Inclusive Data Sample.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t8","@type":"Dataset","description":"Properties of single jet multiplicity distributions for the Two Jet Data Sample.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t9","@type":"Dataset","description":"Multiplicity Moments for the Inclusive Data Sample. CQ = MEAN(N**Q)/MEAN(N)**Q.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t10","@type":"Dataset","description":"Multiplicity Moments for the Two Jet Data Sample. CQ = MEAN(N**Q)/MEAN(N)**Q.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t11","@type":"Dataset","description":"Multiplicity Moments for the Single Jet of the Inclusive Data Sample. CQ = MEAN(N**Q)/MEAN(N)**Q.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t12","@type":"Dataset","description":"Multiplicity Moments for the Single Jet of the Two Jet Data Sample. CQ = MEAN(N**Q)/MEAN(N)**Q.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.23443.v1/t13","@type":"Dataset","description":"No description provided.","name":"Table 13"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins18502?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/23443"}],"inLanguage":"en","name":"Study of Quark Fragmentation in e+ e- Annihilation at 29-GeV: Charged Particle Multiplicity and Single Particle Rapidity Distributions","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins18502?version=1","version":1}