{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.77015.v2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1489189"}},{"@id":"https://doi.org/10.1140/epjc/s10052-017-4781-1","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2017","description":"CERN-LHC. The nuclear modification factor $R_{AA}$ and the azimuthal anisotropy coefficient $v_{2}$ of prompt and nonprompt (i.e. those from decays of b hadrons) J/$\\psi$ mesons, measured from PbPb and pp collisions at $\\sqrt{\\mathrm{s_{NN}}}$=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta $p_{T}>$6.5 GeV/c and rapidity $|y|<$2.4, extending down to $p_{T}$=3 GeV/c in the 1.6$<|y|<$2.4 range. The $v_{2}$ of prompt J/$\\psi$ is found to be nonzero and constant over the full kinematic range studied, while the measured $v_{2}$ of nonprompt J/$\\psi$ is consistent with zero. The $R_{AA}$ of prompt J/$\\psi$ exhibits a suppression that increases with centrality but does not vary as a function of either y or $p_{T}$ in the fiducial range. The nonprompt J/$\\psi$ $R_{AA}$ shows a suppression which becomes stronger as rapidity or $p_{T}$ increase. The $v_{2}$ and nuclear suppression of open and hidden charm, and of open charm and beauty, are compared. \n\nSee arXiv:1610.00613 for more details.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t1","@type":"Dataset","description":"Prompt J/$\\psi$ $v_{2}$ as a function of centrality. The average ${N}_{\\rm part}$ values correspond to events flatly distributed across centrality.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t2","@type":"Dataset","description":"Prompt J/$\\psi$ $v_{2}$ as a function of rapidity.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t3","@type":"Dataset","description":"Prompt J/$\\psi$ $v_{2}$ as a function of $p_{T}$.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t4","@type":"Dataset","description":"Prompt J/$\\psi$ $R_{\\rm AA}$ as a function of centrality. The average ${N}_{\\rm part}$ values correspond to events flatly distributed across...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t5","@type":"Dataset","description":"Prompt J/$\\psi$ $R_{\\rm AA}$ as a function of rapidity.","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t6","@type":"Dataset","description":"Prompt J/$\\psi$ $R_{\\rm AA}$ as a function of $p_{\\rm T}$.","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t7","@type":"Dataset","description":"Prompt J/$\\psi$ $R_{\\rm AA}$ as a function of centrality at high $p_{\\rm T}$, 6.5$<p_{\\rm T}<$30 GeV/c, in three different $|y|$...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t8","@type":"Dataset","description":"Prompt J/$\\psi$ $R_{\\rm AA}$ as a function of centrality, at forward rapidity, 1.6$<|y|<$2.4, for two different $p_{\\rm T}$ regions.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t9","@type":"Dataset","description":"Nonprompt J/$\\psi$ $v_{2}$ as a function of $p_{\\rm T}$.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t10","@type":"Dataset","description":"Nonprompt J/$\\psi$ $R_{\\rm AA}$ as a function of centrality. The average ${N}_{\\rm part}$ values correspond to events flatly distributed across...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t11","@type":"Dataset","description":"Nonprompt J/$\\psi$ $R_{\\rm AA}$ as a function of rapidity.","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t12","@type":"Dataset","description":"Nonprompt J/$\\psi$ $R_{\\rm AA}$ as a function of $p_{\\rm T}$.","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t13","@type":"Dataset","description":"Nonprompt J/$\\psi$ $R_{\\rm AA}$ as a function of centrality. The average ${N}_{\\rm part}$ values correspond to events flatly distributed across...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.77015.v2/t14","@type":"Dataset","description":"Nonprompt J/$\\psi$ $R_{\\rm AA}$ as a function of centrality. The average ${N}_{\\rm part}$ values correspond to events flatly distributed across...","name":"Table 14"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1489189?version=2"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/77015"}],"inLanguage":"en","name":"Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at sqrt(s[NN]) = 2.76 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1489189?version=2","version":2}