{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.129080.v1/t6","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1899703"}},{"@id":"https://doi.org/10.1007/JHEP03(2022)190","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2022","description":"Prompt J/$\\psi$ cross section as a function of transverse momentum in pp at 5.02 TeV","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1313599/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1313599/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1313599/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1313599/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1899703?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/129080"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.129080.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1899703?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.129080.v1","@type":"Dataset","description":"The production of J/$\\psi$ is measured at midrapidity ($|y|<0.9$) in proton\\textendash proton collisions at $\\sqrt{s}$ = 5.02 and 13 TeV, through the dielectron decay channel, using the ALICE detector at the Large Hadron Collider. The data sets used for the analyses correspond to integrated luminosities of  $\\mathcal{L}_{\\rm int}$ = 19.4 $\\pm$ 0.4 nb$^{-1}$ and $\\mathcal{L}_{\\rm int}$ = 32.2 $\\pm$ 0.5 nb$^{-1}$ at $\\sqrt{s}$ = 5.02 and 13 TeV, respectively. The fraction of non-prompt J/$\\psi$ mesons, i.e.\\ those originating from the decay of beauty hadrons, is measured down to a transverse momentum $p_{T}$ = 2 GeV/$c$ (1 GeV/$c$) at  $\\sqrt{s}$ = 5.02 TeV (13 TeV). The $p_{T}$ and rapidity ($y$) differential cross sections, as well as the corresponding values integrated over $p_{T}$ and $y$, are carried out separately for prompt and non-prompt J/$\\psi$ mesons. The results are compared with measurements from other experiments and theoretical calculations based on quantum chromodynamics (QCD). The shape of the $p_{T}$ and $y$ distributions of beauty quarks predicted by state-of-the-art perturbative QCD models are used to extrapolate the \\bbbar pair cross section at midrapidity and in the total phase space. The total $b\\overline{b}$ cross sections are found to be $\\sigma_{\\rm b \\overline{\\rm b}} = 541 \\pm 45 (\\rm stat.) \\pm 69 (\\rm syst.)_{-12}^{+10} (\\rm extr.)~{\\rm \\mu b}$  and $\\sigma_{\\rm b \\overline{\\rm b}}~=~218 \\pm 37 (\\rm stat.) \\pm 32 (\\rm syst.)_{-9.1}^{+8.2} (\\rm extr.)~{\\rm \\mu b}$ at \\s = 13 and 5.02 TeV, respectively. The value obtained from the combination of ALICE and LHCb measurements in pp collisions at \\s = 13 TeV is also provided.","name":"Prompt and non-prompt J/$\\psi$ production cross sections at midrapidity in proton-proton collisions at $\\sqrt{s}$ = 5.02 and 13 TeV","url":"https://www.hepdata.net/record/ins1899703?version=1"},"keywords":"P P --> J/$\\psi$+X, Prompt J/$\\psi$ cross section, 5020.0, Beauty, Non-prompt J/$\\psi$, Proton-Proton Collisions","name":"Table 4b","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/129086","version":1}