{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.141741.v1/t8","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/664944"}},{"@id":"https://doi.org/10.1103/PhysRevLett.94.232302","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"PHENIX Collaboration"},"creator":{"@type":"Organization","name":"PHENIX Collaboration"},"datePublished":"2023","description":"Differential anisotropy $v_2$($p_T$) for centrality selection 13 - 26%.","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1523976/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1523976/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1523976/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1523976/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1523976/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins664944?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/141741"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.141741.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins664944?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.141741.v1","@type":"Dataset","description":"New measurements are presented for charged hadron azimuthal correlations at mid-rapidity in Au+Au collissions at $\\sqrt{s_{NN}}$ = 62.4 and 200 GeV. They are compared to earlier measurements obtained at $\\sqrt{s_{NN}}$ = 130 GeV and in Pb+Pb collisions at $\\sqrt{s_{NN}}$ = 17.2 GeV. Sizeable anisotropies are observed with centrality and transverse momentum ($p_T$) dependence characteristic of elliptic flow ($v_2$). For a broad range of centralities, the observed magnitudes and trends of the differential anisotropy, $v_2$($p_T$), change very little over the collision energy range $\\sqrt{s_{NN}}$ = 62-200 GeV, indicating saturation of the excitation function for $v_2$ at these energies. Sucha a saturation may be indicative of the dominance of a very soft equation of state for $\\sqrt{s_{NN}}$ ~ 60-200 GeV.","name":"Saturation of azimuthal anisotropy in Au + Au collisions at s(NN)**(1/2) = 62-GeV - 200-GeV.","url":"https://www.hepdata.net/record/ins664944?version=1"},"keywords":"AU + AU --> CHARGED X0, 200.0, ppg047","name":"Figure 3d","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/141822","version":1}