{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.99158.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1258446"}},{"@id":"https://doi.org/10.1103/PhysRevC.90.024906","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"STAR Collaboration"},"creator":{"@type":"Organization","name":"STAR Collaboration"},"datePublished":"2020","description":"The $J/\\psi$ $p_T$ spectrum and nuclear modification factor ($R_{AA}$) are reported for $p_T$ &lt; 5 GeV/c and |y|&lt;1 from 0% to 60% central Au+Au and Cu+Cu collisions at $\\sqrt{s_{NN}}$ = 200 GeV at STAR. A significant suppression of $p_T$-integrated $J/\\psi$ production is observed in central Au+Au events. The Cu+Cu data are consistent with no suppression, although the precision is limited by the available statistics. $R_{AA}$ in Au+Au collisions exhibits a strong suppression at low transverse momentum and gradually increases with $p_T$. The data are compared to high-$p_T$ STAR results and previously published BNL Relativistic Heavy Ion Collider results. Comparing with model calculations, it is found that the invariant yields at low $p_T$ are significantly above hydrodynamic flow predictions but are consistent with models that include color screening and regeneration.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t1","@type":"Dataset","description":"The invariant yield versus transverse momentum for |y| &lt; 1 in 0-20% centrality in Au+Au collisions (solid circles). The results...","name":"Figure 9a"},{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t2","@type":"Dataset","description":"The invariant yield versus transverse momentum for |y| &lt; 1 in 20-40% centrality in Au+Au collisions (solid circles). The results...","name":"Figure 9b"},{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t3","@type":"Dataset","description":"The invariant yield versus transverse momentum for |y| &lt; 1 in 40-60% centrality in Au+Au collisions (solid circles). The results...","name":"Figure 9c"},{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t4","@type":"Dataset","description":"The invariant yield versus transverse momentum for |y| &lt; 1 in 0-60% centrality in Au+Au collisions (solid circles). The results...","name":"Figure 9d"},{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t5","@type":"Dataset","description":"The $J/\\psi$ nuclear modification factor versus transverse momentum for |y| &lt; 1 and $p_T$ &lt; 5 GeV/c for 0-60% centrality...","name":"Figure 12a"},{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t6","@type":"Dataset","description":"The $J/\\psi$ nuclear modification factor versus transverse momentum for |y| &lt; 1 and $p_T$ &lt; 5 GeV/c for 0-20% centrality...","name":"Figure 12b"},{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t7","@type":"Dataset","description":"The $J/\\psi$ nuclear modification factor versus transverse momentum for |y| &lt; 1 and $p_T$ &lt; 5 GeV/c for 20-40% centrality...","name":"Figure 12c"},{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t8","@type":"Dataset","description":"The $J/\\psi$ nuclear modification factor versus transverse momentum for |y| &lt; 1 and $p_T$ &lt; 5 GeV/c for 40-60% centrality...","name":"Figure 12d"},{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t9","@type":"Dataset","description":"The $J/\\psi$ invariant yield and nuclear modification factor as a function of centrality for |y| &lt; 1 in Au+Au collisions...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t10","@type":"Dataset","description":"The $J/\\psi$ invariant yield $Bd^2N/(2\\pi p_Tdydp_T) [(GeV/c)^{-2}]$ and nuclear modification factor as a function of transverse momentum for |y| &lt;...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.99158.v1/t11","@type":"Dataset","description":"The $J/\\psi$ invariant yield and nuclear modification factor for |y| &lt; 1 in Cu+Cu collisions at $\\sqrt{s_{NN}}$ = 200 GeV.","name":"Table 7"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1258446?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/99158"}],"inLanguage":"en","name":"$J/\\psi$ production at low $p_T$ in Au+Au and Cu+Cu collisions at $\\sqrt{s_{_{NN}}}$ = 200 GeV at STAR","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1258446?version=1","version":1}
