{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.110656.v1","@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":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2022","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.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.110656.v1/t1","@type":"Dataset","description":"Event plane resolution as a function of collision centrality from Au+Au collisions at $\\sqrt{s_{NN}}$=3 (a), 27 and 54.4 GeV (b)....","name":"fig2"},{"@id":"https://doi.org/10.17182/hepdata.110656.v1/t2","@type":"Dataset","description":"Rapidity($y$) dependence of $v_1$ (top panels) and $v_2$ (bottom panels) of proton and $\\Lambda$ baryons (left panels), pions (middle panels)...","name":"fig3 top"},{"@id":"https://doi.org/10.17182/hepdata.110656.v1/t3","@type":"Dataset","description":"Rapidity($y$) dependence of $v_1$ (top panels) and $v_2$ (bottom panels) of proton and $\\Lambda$ baryons (left panels), pions (middle panels)...","name":"fig3 bottom (p, $\\pi^{\\pm}$, K+)"},{"@id":"https://doi.org/10.17182/hepdata.110656.v1/t4","@type":"Dataset","description":"Rapidity($y$) 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