{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.57282.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/731670"}},{"@id":"https://doi.org/10.1103/PhysRevLett.98.232301","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"PHENIX Collaboration"},"creator":{"@type":"Organization","name":"PHENIX Collaboration"},"datePublished":"2011","description":"Measurement of J/PSI production at the PHENIX experiment, in Au+Au collisions at center-of-mass energy of 200GeV, for rapidities,-2.2<y<2.2. The J/PSI invariant yield and nuclear modification factor Raa as a function of centrality, transverse momentum and rapidity are reported.     The statistical errors are the combination of statistical error and uncorrelated point-to-point systematic error (i.e. which can move the points independently of each other),quadratically summed. The systematic error is the point-to-point correlated systematic errors (which can move the points coherently, thus not necessarly by the same amount).Global systematic are mentionned in comments, if necessary.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t1","@type":"Dataset","description":"J/PSI invariant yield versus transverse momentum for 0-20%, 20-40%, 40-60%, 60-92% centrality at mid rapidity :,-0.35<y<0.35 An up/down correction, to...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t2","@type":"Dataset","description":"J/PSI invariant yield versus transverse momentum for 0-20%, 20-40%, 40-60%, 60-92% centrality at forward rapidities : absolute value of y...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t3","@type":"Dataset","description":"Mean PT^2 values for different bins of centrality, at mid rapidities :-0.35<y<0.35,.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t4","@type":"Dataset","description":"Mean PT^2 values at forward rapidities (absolute value of y belongs to [1.2;2.2]), for different bins of centrality.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t5","@type":"Dataset","description":"J/PSI invariant yield versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality, at mid rapidity :,-0.35<y<0.35 An up/down correction, to translate...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t6","@type":"Dataset","description":"J/PSI invariant yield versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality,at forward rapidities (absolute value of y belongs to [1.2;2.2])....","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t7","@type":"Dataset","description":"Nuclear modification factor Raa versus transverse momentum for 0-20%, 20-40%, 40-60%, 60-92% centrality, at mid rapidities :-0.35<y<0.35. An additional +-...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t8","@type":"Dataset","description":"Nuclear modification factor Raa versus transverse momentum for 0-20%, 20-40%, 40-60%, 60-92% centrality, at forward rapidities : absolute value of...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t9","@type":"Dataset","description":"Nuclear modification factor Raa versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality, at mid rapidities :,-0.35<y<0.35. An additional +- 10%...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t10","@type":"Dataset","description":"Nuclear modification factor Raa versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality, at forward rapidities : absolute value of y...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t11","@type":"Dataset","description":"The number of participants Npart and the nuclear modification factor Raa versus centrality at mid rapidities :,-0.35<y<0.35. An additional +-...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t12","@type":"Dataset","description":"The number of participants Npart and the nuclear modification factor Raa versus centrality at forward rapidities : absolute value of...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.57282.v1/t13","@type":"Dataset","description":"Ratio of nuclear modification factors RAA(forward rapidity)/RAA(mid rapidity), versus centrality. For the two most central bins, mid rapidity points have...","name":"Table 13"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins731670?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/57282"}],"inLanguage":"en","name":"J/psi production vs centrality, transverse momentum, and rapidity 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/ins731670?version=1","version":1}