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dc.contributor.authorPHENIX Collaboration
dc.date.accessioned2016-06-03T10:01:13Z
dc.date.available2016-06-03T10:01:13Z
dc.date.issued2016
dc.identifier.citationPHENIX Collaboration. (2016). Transverse energy production and charged-particle multiplicity at midrapidity in various systems from √sNN = 7.7 to 200 GeV. <i>Physical Review C</i>, <i>93</i>(2), Article 024901. <a href="https://doi.org/10.1103/PhysRevC.93.024901" target="_blank">https://doi.org/10.1103/PhysRevC.93.024901</a>
dc.identifier.otherCONVID_25569233
dc.identifier.otherTUTKAID_69299
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/50078
dc.description.abstractMeasurements of midrapidity charged-particle multiplicity distributions, dNch/dη, and midrapidity transverseenergy distributions, dET /dη, are presented for a variety of collision systems and energies. Included are distributions for Au + Au collisions at √sNN = 200, 130, 62.4, 39, 27, 19.6, 14.5, and 7.7 GeV, Cu + Cu collisions at √sNN = 200 and 62.4 GeV, Cu + Au collisions at √sNN = 200 GeV, U + U collisions at √sNN = 193 GeV, d + Au collisions at √sNN = 200 GeV, 3 He + Au collisions at √sNN = 200 GeV, and p + p collisions at √sNN = 200 GeV. Centrality-dependent distributions at midrapidity are presented in terms of the number of nucleon participants, Npart, and the number of constituent quark participants, Nqp. For all A + A collisions down to √sNN = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with Nqp than scaling with Npart. Also presented are estimates of the Bjorken energy density, εBJ, and the ratio of dET /dη to dNch/dη, the latter of which is seen to be constant as a function of centrality for all systems.
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review C
dc.subject.othercharged-particle multiplicity distributions
dc.subject.othertransverse-energy distributions
dc.titleTransverse energy production and charged-particle multiplicity at midrapidity in various systems from √sNN = 7.7 to 200 GeV
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-201606032842
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.date.updated2016-06-03T09:15:09Z
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn2469-9985
dc.relation.numberinseries2
dc.relation.volume93
dc.type.versionpublishedVersion
dc.rights.copyright© 2016 American Physical Society. Published in this repository with the kind permission of the publisher.
dc.rights.accesslevelopenAccessfi
dc.relation.doi10.1103/PhysRevC.93.024901
dc.type.okmA1


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