{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.96601.v1/t17","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1394433"}},{"@id":"https://doi.org/10.1103/PhysRevC.93.024901","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"PHENIX Collaboration"},"creator":{"@type":"Organization","name":"PHENIX Collaboration"},"datePublished":"2020","description":"Transverse energy in Cu+Cu collisions at $\\sqrt{s_{NN}}$ = 200 GeV","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/675308/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/675308/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/675308/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/675308/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/675308/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1394433?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/96601"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.96601.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1394433?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.96601.v1","@type":"Dataset","description":"BNL-RHIC.  Measurements of midrapidity charged particle multiplicity distributions, $dN_{ch}/d\\eta$, and midrapidity transverse-energy distributions, $dE_T/d\\eta$, are presented for a variety of collision systems and energies. Included are distributions for Au+Au collisions at $\\sqrt{s_{NN}}$ = 200, 130, 62.4, 39, 27,19.6, 14.5, and 7.7 GeV, Cu+Cu collisions at $\\sqrt{s_{NN}}$ = 200 and 62.4 GeV, Cu+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV, U+U collisions at $\\sqrt{s_{NN}}$ = 193 GeV, d+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV, $^3$He+Au collisions at $\\sqrt{s_{NN}}$ 200 GeV, and p+p collisions at $\\sqrt{s_{NN}}$ = 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, $N_{qp}$. For all A+A collisions down to $\\sqrt{s_{NN}}$ = 7.7 GeV, it is observed that the midrapidity data are better described by scaling with $N_{qp}$ than scaling with $N_{part}$. Also presented are estimates of the Bjorken energy density, $\\epsilon_{BJ}$, and the ratio of $dET/d\\eta$ to $dNch/d\\eta$, the latter of which is seen to be constant as a function of centrality for all systems.","name":"Transverse energy production and charged-particle multiplicity at midrapidity in various systems from $\\sqrt{s_{NN}}=7.7$ to 200 GeV","url":"https://www.hepdata.net/record/ins1394433?version=1"},"keywords":"CU CU --> NEUTRAL X, 200","name":"Table 23","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/96620","version":1}