{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79055.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1605750"}},{"@id":"https://doi.org/10.1103/PhysRevLett.120.142301","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2018","description":"CERN-LHC. The relative yields of \u03a5 mesons produced in pp and PbPb collisions at 5.02TeV and reconstructed via the dimuon decay channel are measured using data collected by the CMS experiment. Double ratios are formed by comparing the yields of the excited states, \u03a5(2S) and \u03a5(3S), to the ground state, \u03a5(1S), in both PbPb and pp collisions at the same center-of-mass energy, in data collected in 2015. The double ratios are studied as a function of collision centrality, as well as \u03a5 transverse momentum and rapidity.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79055.v1/t1","@type":"Dataset","description":"Double ratio of measured yields, $(N_{\\varUpsilon(2S)} / N_{\\varUpsilon(1S)})_{\\mathrm{PbPb}} / (N_{\\varUpsilon(2S)} / N_{\\varUpsilon(1S)})_{pp}$, as a function of centrality, for upsilon $|y|<2.4$...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.79055.v1/t2","@type":"Dataset","description":"Double ratio of measured yields, $(N_{\\varUpsilon(2S)} / N_{\\varUpsilon(1S)})_{\\mathrm{PbPb}} / (N_{\\varUpsilon(2S)} / N_{\\varUpsilon(1S)})_{pp}$, as a function of pT, for upsilon $|y|<2.4$,...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.79055.v1/t3","@type":"Dataset","description":"Double ratio of measured yields, $(N_{\\varUpsilon(2S)} / N_{\\varUpsilon(1S)})_{\\mathrm{PbPb}} / (N_{\\varUpsilon(2S)} / N_{\\varUpsilon(1S)})_{pp}$, as a function of rapidity, for upsilon $pT<30$GeV,...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.79055.v1/t4","@type":"Dataset","description":"95% CL intervals on the double ratio of measured yields, $(N_{\\varUpsilon(3S)} / N_{\\varUpsilon(1S)})_{\\mathrm{PbPb}} / (N_{\\varUpsilon(3S)} / N_{\\varUpsilon(1S)})_{pp}$, as a function...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.79055.v1/t5","@type":"Dataset","description":"68% CL intervals on the double ratio of measured yields, $(N_{\\varUpsilon(3S)} / N_{\\varUpsilon(1S)})_{\\mathrm{PbPb}} / (N_{\\varUpsilon(3S)} / N_{\\varUpsilon(1S)})_{pp}$, as a function...","name":"Table 5"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1605750?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79055"}],"inLanguage":"en","name":"Suppression of excited Upsilon states relative to the ground state in PbPb collisions at sqrt(sNN) = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1605750?version=1","version":1}