{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.93262.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/660793"}},{"@id":"https://doi.org/10.1103/PhysRevC.72.014904","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2021","description":"The results from the STAR Collaboration on directed flow (v_1), elliptic flow (v_2), and the fourth harmonic (v_4) in the anisotropic azimuthal distribution of particles from Au+Au collisions at sqrtsNN = 200 GeV are summarized and compared with results from other experiments and theoretical models. Results for identified particles are presented and fit with a Blast Wave model. Different anisotropic flow analysis methods are compared and nonflow effects are extracted from the data. For v_2, scaling with the number of constituent quarks and parton coalescence is discussed. For v_4, scaling with v_2^2 and quark coalescence is discussed.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t1","@type":"Dataset","description":"Directed flow of charged hadrons v1{3} as a function of pseudorapidity for 10\u201370% centrality.","name":"Figure 2_1"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t2","@type":"Dataset","description":"Directed flow of charged hadrons v1 {EP1,EP2} as a function of pseudorapidity for 20\u201360% centrality.","name":"Figure 2_2"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t3","@type":"Dataset","description":"Charged hadron v2 for the centrality bins 5 to 10% and in steps of 10% starting at 10, 20, 30,...","name":"Figure 4"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t4","@type":"Dataset","description":"Charged hadron v2 for the centrality bin 0-50%.","name":"Figure 5"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t5","@type":"Dataset","description":"v2(4) vs. p_T for pions for 20 - 60% centrality","name":"Figure 6_1"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t6","@type":"Dataset","description":"v2(4) vs. p_T for kaons for 20 - 60% centrality","name":"Figure 6_2"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t7","@type":"Dataset","description":"v2(4) vs. p_T for anti-protons for 20 - 60% centrality","name":"Figure 6_3"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t8","@type":"Dataset","description":"v2(2) vs. centrality for pions","name":"Figure 7a"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t9","@type":"Dataset","description":"v2(2) vs. centrality for kaons","name":"Figure 7b"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t10","@type":"Dataset","description":"v2(2) vs. centrality for anti-protons","name":"Figure 7c"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t11","@type":"Dataset","description":"v2 vs. p_T for particles identified in the RICH (min. bias) for pions+kaons and protons/antiprotons","name":"Figure 8"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t12","@type":"Dataset","description":"v2 for Kshort for min. bias","name":"Figure 9_1"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t13","@type":"Dataset","description":"v2 for kaons from kinks for min. bias","name":"Figure 9_2"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t14","@type":"Dataset","description":"v2 for kaons from dE/dx for min. bias","name":"Figure 9_3"},{"@id":"https://doi.org/10.17182/hepdata.93262.v1/t15","@type":"Dataset","description":"v2 for Lambda+Lambdabar for min. bias [PRL/92/052302/2004]. 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