{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.102947.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/695404"}},{"@id":"https://doi.org/10.1103/PhysRevC.73.034903","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2021","description":"We present the directed flow ($v_1$) measured in Au+Au collisions at $\\sqrt{s_{_{NN}}}$ = 62.4 GeV in the mid-pseudorapidity region $|\\eta|<1.3$ and in the forward pseudorapidity region $2.5 < |\\eta| < 4.0$. The results are obtained using the three-particle cumulant method, the event plane method with mixed harmonics, and for the first time at the Relativistic Heavy Ion Collider (RHIC), the standard method with the event plane reconstructed from spectator neutrons. Results from all three methods are in good agreement. Over the pseudorapidity range studied, charged particle directed flow is in the direction opposite to that of fragmentation neutrons.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t1","@type":"Dataset","description":"Directed flow of charged particles as a function of pseudorapidity, for centrality 10%-70%.","name":"Table 1a"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t2","@type":"Dataset","description":"Directed flow of charged particles as a function of pseudorapidity, for centrality 10%-70%.","name":"Table 1b"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t3","@type":"Dataset","description":"Directed flow of charged particles as a function of pseudorapidity, for centrality 10%-70%.","name":"Table 1c"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t4","@type":"Dataset","description":"Directed flow of charged particles as a function of pseudorapidity, for centrality 10%-70%.","name":"Table 1d"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t5","@type":"Dataset","description":"Directed flow of charged particles as a function of pseudorapidity, for centrality 10%-70%.","name":"Table 1e"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t6","@type":"Dataset","description":"Directed flow of charged particles as a function of pseudorapidity, for centrality 10%-70%.","name":"Table 1f"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t7","@type":"Dataset","description":"$v_1$ versus rapidity for charged particles.","name":"Table 2a"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t8","@type":"Dataset","description":"$v_1$ versus rapidity for pions.","name":"Table 2b"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t9","@type":"Dataset","description":"$v_1$ versus rapidity for protons.","name":"Table 2c"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t10","@type":"Dataset","description":"Directed flow of charged particles as a function of pseudorapidity for the 60-70% and 70-80% centrality classes.","name":"Table 3per"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t11","@type":"Dataset","description":"Directed flow of charged particles as a function of pseudorapidity for the 10-20%, 20-30%, 30-40%, 40-50% and 50-60% centrality classes.","name":"Table 3semi"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t12","@type":"Dataset","description":"Directed flow of charged particles as a function of pseudorapidity for the 5-10% centrality class.","name":"Table 3510"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t13","@type":"Dataset","description":"Directed flow of charged particles as a function of pseudorapidity for the 0-5% centrality class.","name":"Table 305"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t14","@type":"Dataset","description":"$v_1${3} versus $p_t$ measured in the main TPC (|$\\eta$| &lt; 1.3), for centrality 10%-70%.","name":"Table 4upper"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t15","@type":"Dataset","description":"$v_1${3} versus $p_t$ measured in the Forward TPC (2.5 &lt; |$\\eta$| &lt; 4.0), for different centralities.","name":"Table 4lower"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t16","@type":"Dataset","description":"Directed flow of charged particles as a function of impact parameter for the mid-pseudorapidity region (|$\\eta$| &lt; 1.3) and the...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t17","@type":"Dataset","description":"Charged particle $v_1$ for Au+Au collisions (10%-70%) at 200 GeV as a function of $\\eta-y_{beam}$.","name":"Table 6a"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t18","@type":"Dataset","description":"Charged particle $v_1$ for Au+Au collisions (10%-70%) at 62.4 GeV as a function of $\\eta-y_{beam}$.","name":"Table 6b"},{"@id":"https://doi.org/10.17182/hepdata.102947.v1/t19","@type":"Dataset","description":"Charged particle $v_1$ for Pb+Pb collisions (12.5%-33.5%) at 17.2 GeV as a function of $y-y_{beam}$.","name":"Table 6c"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins695404?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/102947"}],"inLanguage":"en","name":"Directed flow in Au + Au collisions at s(NN)**(1/2) = 62-GeV.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins695404?version=1","version":1}