{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.91135.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1737650"}},{"@id":"https://doi.org/10.1016/j.physletb.2019.134917","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2020","description":"J/PSI(1S) suppression has long been considered a sensitive signature of the formation of the Quark-Gluon Plasma (QGP) in relativistic heavy-ion collisions. In this letter, we present the first measurement of inclusive J/PSI(1S) production at mid-rapidity through the dimuon decay channel in Au+Au collisions at \\sqrtsNN\\ = 200 GeV with the STAR experiment. These measurements became possible after the installation of the Muon Telescope Detector was completed in 2014. The J/PSI(1S) yields are measured in a wide transverse momentum (pT) range of 0.15 GeV/c to 12 GeV/c from central to peripheral collisions. They extend the kinematic reach of previous measurements at RHIC with improved precision. In the 0-10% most central collisions, the J/PSI(1S) yield is suppressed by a factor of approximately 3 for pT > 5 GeV/c relative to that in p+p collisions scaled by the number of binary nucleon-nucleon collisions. The J/PSI(1S) nuclear modification factor displays little dependence on pT in all centrality bins. Model calculations can qualitatively describe the data, providing further evidence for the color-screening effect experienced by J/PSI(1S) mesons in the QGP.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.91135.v1/t1","@type":"Dataset","description":"Invariant yield of inclusive J/PSI(1S) times branching ratio to the dimuon decay in 0-80% Au+Au collisions at 200 GeV","name":"Figure 3.0.0"},{"@id":"https://doi.org/10.17182/hepdata.91135.v1/t2","@type":"Dataset","description":"Invariant yield of inclusive J/PSI(1S) times branching ratio to the dimuon decay in 0-20% Au+Au collisions at 200 GeV","name":"Figure 3.0.1"},{"@id":"https://doi.org/10.17182/hepdata.91135.v1/t3","@type":"Dataset","description":"Invariant yield of inclusive J/PSI(1S) times branching ratio to the dimuon decay in 20-40% Au+Au collisions at 200 GeV","name":"Figure 3.0.2"},{"@id":"https://doi.org/10.17182/hepdata.91135.v1/t4","@type":"Dataset","description":"Invariant yield of inclusive J/PSI(1S) times branching ratio to the dimuon decay in 40-60% Au+Au collisions at 200 GeV","name":"Figure 3.0.3"},{"@id":"https://doi.org/10.17182/hepdata.91135.v1/t5","@type":"Dataset","description":"Invariant yield of inclusive J/PSI(1S) times branching ratio to the dimuon decay in 60-80% Au+Au collisions at 200 GeV","name":"Figure 3.0.4"},{"@id":"https://doi.org/10.17182/hepdata.91135.v1/t6","@type":"Dataset","description":"Invariant yield of inclusive J/PSI(1S) times branching ratio to the dielectron decay in 0-60% Au+Au collisions at 200 GeV","name":"Figure 3.1.0"},{"@id":"https://doi.org/10.17182/hepdata.91135.v1/t7","@type":"Dataset","description":"Invariant yield of inclusive J/PSI(1S) times branching ratio to the dielectron decay in 0-20% Au+Au collisions at 200 GeV","name":"Figure 3.1.1"},{"@id":"https://doi.org/10.17182/hepdata.91135.v1/t8","@type":"Dataset","description":"Invariant yield of inclusive J/PSI(1S) times branching ratio to the dielectron decay in 20-40% Au+Au collisions at 200 GeV","name":"Figure 3.1.2"},{"@id":"https://doi.org/10.17182/hepdata.91135.v1/t9","@type":"Dataset","description":"Invariant yield of inclusive J/PSI(1S) times branching ratio to the dielectron decay in 40-60% Au+Au collisions at 200 GeV","name":"Figure 3.1.3"},{"@id":"https://doi.org/10.17182/hepdata.91135.v1/t10","@type":"Dataset","description":"Invariant yield of inclusive J/PSI(1S) times branching ratio in p+p collisions at 200 GeV. 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