{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.103082.v1/t5","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1672469"}},{"@id":"https://doi.org/10.1140/epjc/s10052-018-6219-9","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2021","description":"The nuclear modification factor as a function of pT for the prompt jpsi for |y|&lt;2, in 0--80% centrality bin.","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1031957/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1031957/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1031957/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1031957/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1031957/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1672469?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/103082"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.103082.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1672469?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.103082.v1","@type":"Dataset","description":"A measurement of $J/\\psi$ and $\\psi(2\\mathrm{S})$ production is presented. It is based on a data sample from Pb+Pb collisions at $\\sqrt{s_{\\mathrm{NN}}}$ = 5.02 TeV and $pp$ collisions at $\\sqrt{s}$ = 5.02 TeV recorded by the ATLAS detector at the LHC in 2015, corresponding to an integrated luminosity of $0.42\\mathrm{nb}^{-1}$ and $25\\mathrm{pb}^{-1}$ in Pb+Pb and $pp$, respectively. The measurements of per-event yields, nuclear modification factors, and non-prompt fractions are performed in the dimuon decay channel for $9 < p_{T}^{\\mu\\mu} < 40$ GeV in dimuon transverse momentum, and $-2.0 < y_{\\mu\\mu} < 2.0$ in rapidity. Strong suppression is found in Pb+Pb collisions for both prompt and non-prompt $J/\\psi$, as well as for prompt and non-prompt $\\psi(2\\mathrm{S})$, increasing with event centrality. The suppression of prompt $\\psi(2\\mathrm{S})$ is observed to be stronger than that of $J/\\psi$, while the suppression of non-prompt $\\psi(2\\mathrm{S})$ is equal to that of the non-prompt $J/\\psi$ within uncertainties, consistent with the expectation that both arise from \\textit{b}-quarks propagating through the medium. Despite prompt and non-prompt $J/\\psi$ arising from different mechanisms, the dependence of their nuclear modification factors on centrality is found to be quite similar.","name":"Prompt and non-prompt $J/\\psi$ and $\\psi(2\\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment","url":"https://www.hepdata.net/record/ins1672469?version=1"},"keywords":"PB PB --> J/PSI < MU+ MU- > X, RAA PROMPT, 5020.0","name":"Table 5","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/106264","version":1}