{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.80816.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1644903"}},{"@id":"https://doi.org/10.1140/epjc/s10052-018-5950-6","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"CERN-LHC. The nuclear modification factors of J/psi and psi(2S) mesons are measured in PbPb collisions at a centre-of-mass energy per nucleon pair of 5.02 TeV. The analysis is based on PbPb and pp data samples collected by CMS at the LHC in 2015, corresponding to integrated luminosities of 464 inverse microbarns and 28 inverse picobarns, respectively. The measurements are performed in the dimuon rapidity range of abs(y)< 2.4 as a function of centrality, rapidity, and transverse momentum (pT) from pT= 3 GeV/c in the most forward region and up to 50 GeV/c. Both prompt and nonprompt (coming from b hadron decays) J/psi mesons are observed to be increasingly suppressed with centrality, with a magnitude similar to the one observed at 2.76 TeV for the two J/psi meson components. No dependence on rapidity is observed for either prompt or nonprompt J/psi mesons. An indication of a lower prompt J/psi meson suppression at pT > 25 GeV/c is seen with respect to that observed at intermediate pT. The prompt psi(2S) meson yield is found to be more suppressed than that of the prompt J/psi mesons in the entire pT range.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t1","@type":"Dataset","description":"Fraction of J/psi mesons coming from the decay of b hadrons, i.e. nonprompt J/psi meson fraction, as a function of...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t2","@type":"Dataset","description":"Fraction of J/psi mesons coming from the decay of b hadrons, i.e. nonprompt J/psi meson fraction, as a function of...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t3","@type":"Dataset","description":"Differential cross section of prompt J/psi mesons as a function of dimuon pT in pp and PbPb collisions. The PbPb...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t4","@type":"Dataset","description":"Differential cross section of J/psi mesons from b hadrons as a function of dimuon pT in pp and PbPb collisions....","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t5","@type":"Dataset","description":"Differential cross section of prompt J/psi mesons as a function of dimuon rapidty in pp and PbPb collisions. The PbPb...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t6","@type":"Dataset","description":"Differential cross section of J/psi mesons from b hadrons as a function of dimuon rapidty in pp and PbPb collisions....","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t7","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of dimuon rapidity. Global uncertainties arise from the integrated luminosity...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t8","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of collision centrality. Global uncertainties arise from the full pp...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t9","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT. Global uncertainties arise from the integrated luminosity...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t10","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the mid-rapidity interval. Global uncertainties arise...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t11","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the most forward rapidity interval. Global...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t12","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the mid- and most forward rapidity...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t13","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of pT in three centrality bins. Global uncertainties arise from...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t14","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the most forward rapidity range at...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t15","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t16","@type":"Dataset","description":"Nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the mid-rapidity range. Global uncertainties arise...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t17","@type":"Dataset","description":"95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t18","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi and psi(2S) mesons as a function of dimuon pT in the mid-rapidity range. Global...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t19","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of collision centrality in the forward rapidity range. Global uncertainties...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t20","@type":"Dataset","description":"Nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the forward rapidity range. Global uncertainties...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t21","@type":"Dataset","description":"95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of collision centrality in the...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t22","@type":"Dataset","description":"Nuclear modification factor of prompt J/psi mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t23","@type":"Dataset","description":"Nuclear modification factor of prompt psi(2S) mesons as a function of dimuon pT in the forward rapidity range. Global uncertainties...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t24","@type":"Dataset","description":"95% CL intervals on the nuclear modification factor of prompt psi(2S) mesons as a function of dimuon pT in the...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t25","@type":"Dataset","description":"Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon rapidity. Global uncertainties arise from the integrated luminosity...","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t26","@type":"Dataset","description":"Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality. Global uncertainties arise from the full pp...","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t27","@type":"Dataset","description":"Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT. Global uncertainties arise from the integrated luminosity...","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t28","@type":"Dataset","description":"Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT in the mid-rapidity interval. Global uncertainties arise...","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t29","@type":"Dataset","description":"Nuclear modification factor of nonprompt J/psi mesons as a function of dimuon pT in the most forward rapidity interval. Global...","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t30","@type":"Dataset","description":"Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality in the mid- and most forward rapidity...","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t31","@type":"Dataset","description":"Nuclear modification factor of nonprompt J/psi mesons as a function of pT in three centrality bins. Global uncertainties arise from...","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.80816.v1/t32","@type":"Dataset","description":"Nuclear modification factor of nonprompt J/psi mesons as a function of collision centrality in the most forward rapidity range at...","name":"Table 32"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1644903?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/80816"}],"inLanguage":"en","name":"Measurement of prompt and nonprompt charmonium suppression in PbPb collisions at 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1644903?version=1","version":1}