{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.57513.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/688457"}},{"@id":"https://doi.org/10.1103/PhysRevLett.96.012304","@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 in d+Au and p+p collisions at center-of-mass energy of 200GeV. The cross-sections and nuclear dependence of J/PSI production versus rapidity,transverse momentum and centrality are presented     In this paper, the value XF is the momentum fraction of the gluon in the deuteron, minus it's momentum fraction in Au.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t1","@type":"Dataset","description":"J/PSI differential cross section in P+P reactions( times di-lepton branching ratio B=5.9%) as a function of rapidity.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t2","@type":"Dataset","description":"J/PSI nuclear modification factor RDA,as a function of rapidity.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t3","@type":"Dataset","description":"Total cross-section for J/PSI production in P P reactions. The total cross section is estimated using a pythia calculation, normalized...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t4","@type":"Dataset","description":"Mean PT^2 values at negative, null and positive XF for D+AU reaction The mean PT is obtained with a phenomenological...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t5","@type":"Dataset","description":"Mean PT^2 values at negative,null and positive XF for P+P reaction The mean PT is obtained with a phenomenological fit...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t6","@type":"Dataset","description":"PT dependence of the Alpha power for Xf ~ -0.08.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t7","@type":"Dataset","description":"PT dependance of the Alpha power for Xf ~ 0.","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t8","@type":"Dataset","description":"PT dependance of the Alpha power for Xf ~ 0.09.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t9","@type":"Dataset","description":"Centrality dependance of the Nuclear modification factor for rapidity : y=-1.7. Centrality is represented by the number of collisions.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t10","@type":"Dataset","description":"Centrality dependance of the Nuclear modification factor for rapidity y=0.Centrality is represented by the number of collisions.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.57513.v1/t11","@type":"Dataset","description":"Centrality dependance of the Nuclear modification factor for rapidity y=1.8.Centrality is represented by the number of collisions.","name":"Table 11"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins688457?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/57513"}],"inLanguage":"en","name":"J/psi production and nuclear effects for d + Au and p + p collisions at s(NN)**(1/2) = 200-GeV.","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins688457?version=1","version":1}