{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.98969.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/746872"}},{"@id":"https://doi.org/10.1103/PhysRevLett.99.112301","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2021","description":"We present first measurements of the $\\phi$-meson elliptic flow ($v_{2}$($p_{T}$)) and high statistics $p_{T}$ distributions for different centralities from $\\sqrt{s_{NN}}$= 200 GeV Au+Au collisions at RHIC. In minimum bias collisions the $v_{2}$ of the $\\phi$ meson is consistent with the trend observed for mesons. The ratio of the yields of the $\\Omega$ to those of the $\\phi$ as a function of transverse momentum is consistent with a model based on the recombination of thermal $s$ quarks up to $p_{T}$\u223c4 GeV/c, but disagrees at higher momenta. The nuclear modification factor ($R_{CP}$) of $\\phi$ follows the trend observed in the $K^{0}_{S}$ mesons rather than in $\\Lambda$ baryons, supporting baryon-meson scaling. Since $\\phi$-mesons are made via coalescence of seemingly thermalized s quarks in central Au+Au collisions, the observations imply hot and dense matter with partonic collectivity has been formed at RHIC.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.98969.v1/t1","@type":"Dataset","description":"The elliptic flow, $v_{2}$($p_{T}$), for the $\\phi$-meson as a function of centrality. The vertical error bars represent the statistical errors...","name":"Figure 1 top"},{"@id":"https://doi.org/10.17182/hepdata.98969.v1/t2","@type":"Dataset","description":"(color online) Transverse momentum distributions of $\\phi$-mesons from Au+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV. For clarity, distributions for different...","name":"Figure 2"},{"@id":"https://doi.org/10.17182/hepdata.98969.v1/t3","@type":"Dataset","description":"(color online) The $N(\\Omega)/N(\\phi)$ ratio vs. $p_{T}$ for three centrality bins in $\\sqrt{s_{NN}}$ = 200 GeV Au+Au collisions. The solid...","name":"Figure 3"},{"@id":"https://doi.org/10.17182/hepdata.98969.v1/t4","@type":"Dataset","description":"(color online) The $R_{CP}$ of mid-rapidity $\\phi$-mesons produced in $\\sqrt{s_{NN}}$ = 200 GeV Au+Au collisions: (top) 0-5% vs. 40-60% and...","name":"Figure 4 top"},{"@id":"https://doi.org/10.17182/hepdata.98969.v1/t5","@type":"Dataset","description":"(color online) The $R_{CP}$ of mid-rapidity $\\phi$-mesons produced in $\\sqrt{s_{NN}}$ = 200 GeV Au+Au collisions: (top) 0-5% vs. 40-60% and...","name":"Figure 4 bottom"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins746872?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/98969"}],"inLanguage":"en","name":"Partonic flow and Phi-meson production in Au + Au collisions at s(NN)**(1/2) = 200-GeV.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins746872?version=1","version":1}