{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.110656.v1/t25","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1897294"}},{"@id":"https://doi.org/10.1016/j.physletb.2022.137003","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2022","description":"Collision energy dependence of (top panel) directed flow slope $dv_1/dy|_{y=0}$ for p, $\\Lambda, \\pi$(combined from $\\pi^{\\pm}$), K(combined from $K^{\\pm}$ and...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1293447/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1293447/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1293447/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1293447/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1293447/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1897294?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/110656"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.110656.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1897294?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.110656.v1","@type":"Dataset","description":"We report on the measurements of directed flow $v_1$ and elliptic flow $v_2$ for hadrons $(\\pi^{\\pm}, K^{\\pm}, K_S^0, p, \\phi, \\Lambda$ and $\\Xi^-)$ from Au+Au collisions at $\\sqrt{s_{NN}} $ = 3GeV and $v_2$ for $(\\pi^{\\pm}, K^{\\pm}$, $p$ and $\\bar{p})$ at 27 and 54.4 GeV with the STAR experiment. While at the two higher energy midcentral collisions the number-of-constituent-quark (NCQ) scaling holds, at 3 GeV the $v_{2}$ at midrapidity is negative for all hadrons and the NCQ scaling is absent. In addition, the $v_1$ slopes at midrapidity for almost all observed hadrons are found to be positive, implying dominant repulsive baryonic interactions. The features of negative $v_2$ and positive $v_1$ slope at 3 GeV can be reproduced with a baryonic mean-field in transport model calculations. These results imply that the medium in such collisions is likely characterized by baryonic interactions.","name":"Disappearance of partonic collectivity in $\\sqrt{s_{NN}}$ = 3 GeV Au+Au collisions at RHIC","url":"https://www.hepdata.net/record/ins1897294?version=1"},"keywords":"AuAu, 3.0, directed flow","name":"fig5_a $p$","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/128057","version":1}