{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.146723.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2692201"}},{"@id":"https://doi.org/10.1007/JHEP02(2024)066","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2024","description":"The transverse momentum ($p_T$) and centrality dependence of the nuclear modification factor $R_{AA}$ of prompt and non-prompt J/$\\psi$, the latter originating from the weak decays of beauty hadrons, have been measured by the ALICE collaboration in Pb--Pb collisions at 5.02 TeV. The measurements are carried out through the e^+e^- decay channel at midrapidity ($|y| < 0.9$) in the transverse momentum region $1.5 < $p_T$ < 10$~\\GeVc. Both prompt and non-prompt J/$\\psi$ measurements indicate a significant suppression for $p_T$ $>$ 5~\\GeVc, which becomes stronger with increasing collision centrality. The results are consistent with similar LHC measurements in the overlapping $p_T$ intervals, and cover the kinematic region down to $p_T$ = 1.5 \\GeVc at midrapidity, not accessible by other LHC experiments. The suppression of prompt J/$\\psi$ in central and semicentral collisions exhibits a decreasing trend towards lower transverse momentum, described within uncertainties by models implementing J/$\\psi$ production from recombination of c and $\\overline{\\rm c}$ quarks produced independently in different partonic scatterings. At high transverse momentum, transport models including quarkonium dissociation are able to describe the suppression for prompt J/$\\psi$. For non-prompt J/$\\psi$, the suppression predicted by models including both collisional and radiative processes for the computation of the beauty-quark energy loss inside the quark--gluon plasma is consistent with measurements within uncertainties.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t1","@type":"Dataset","description":"Non-prompt J/$\\psi$ fraction as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t2","@type":"Dataset","description":"Non-prompt J/$\\psi$ fraction as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 10-30%","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t3","@type":"Dataset","description":"Non-prompt J/$\\psi$ fraction as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t4","@type":"Dataset","description":"Non-prompt J/$\\psi$ fraction as a function of average number of participants in Pb-Pb at 5.02 TeV","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t5","@type":"Dataset","description":"Non-prompt J/$\\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t6","@type":"Dataset","description":"Prompt J/$\\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t7","@type":"Dataset","description":"Prompt J/$\\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%. Global uncertainty...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t8","@type":"Dataset","description":"Prompt J/$\\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 10-30%. Global uncertainty...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t9","@type":"Dataset","description":"Prompt J/$\\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%. Global uncertainty...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t10","@type":"Dataset","description":"Prompt J/$\\psi$ nuclear modification factor as a function of average number of participants in Pb-Pb at 5.02 TeV. Global uncertainty...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t11","@type":"Dataset","description":"Non-prompt J/$\\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 0-10%. Global uncertainty...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t12","@type":"Dataset","description":"Non-prompt J/$\\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV,, centrality 10-30%. Global uncertainty...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t13","@type":"Dataset","description":"Non-prompt J/$\\psi$ nuclear modification factor as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%. Global uncertainty...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t14","@type":"Dataset","description":"Non-prompt J/$\\psi$ nuclear modification factor as a function of average number of participants in Pb-Pb at 5.02 TeV. Global uncertainty...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t15","@type":"Dataset","description":"Prompt J/$\\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.146723.v1/t16","@type":"Dataset","description":"Non-prompt J/$\\psi$ yields as a function of transverse momentum in Pb-Pb at 5.02 TeV, centrality 30-50%","name":"Table 16"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2692201?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/146723"}],"inLanguage":"en","name":"Prompt and non-prompt J$/\\psi$ production at midrapidity in Pb$-$Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2692201?version=1","version":1}