{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.130237.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1862791"}},{"@id":"https://doi.org/10.1007/JHEP06(2022)011","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2022","description":"The measurement of inclusive, prompt, and non-prompt J/$\\psi$ production in p$-$Pb collisions at a nucleon--nucleon centre-of-mass energy $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV is presented. The inclusive $\\rm{J}/\\psi$ mesons are reconstructed in the dielectron decay channel at midrapidity down to a transverse momentum $p_\\mathrm{T}$ = 0. Non-prompt J/$\\psi$ mesons, which originate from the decay of beauty hadrons, are separated from promptly produced J/$\\psi$ on a statistical basis for $p_\\mathrm{T}$ larger than 1.0 GeV/$c$. These results are based on the data sample collected by the ALICE detector during the 2016 LHC p\u2212Pb run, corresponding to an integrated luminosity of $\\it{L}_{int}$=292$\\pm$11$\\mathrm{\\mu b}^{-1}$.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t1","@type":"Dataset","description":"Fraction of non-prompt $\\rm{J}/\\psi$ in pp collisions at $\\sqrt{s}$ = 5.02 TeV for different $p_\\mathrm{T}$ ranges, as determined with a...","name":"Table 3 p-p"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t2","@type":"Dataset","description":"Inclusive d$^2\\sigma$/d$y$d$p_{\\rm T}$ in bins of $p_{\\mathrm{T}}^{J/\\psi}$ for prompt J/$\\psi$ in p--Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Figure 3"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t3","@type":"Dataset","description":"Fraction of non-prompt J/$\\psi$ in p--Pb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV for different $p_\\mathrm{T}$ ranges.","name":"Figure 4"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t4","@type":"Dataset","description":"d$\\sigma$/dy for prompt J/$\\psi$ in p--Pb collisions at $\\sqrt{s_NN}$=5.02 TeV. The systematic uncertainty includes also the contribution from the extrapolation...","name":"Figure 5a"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t5","@type":"Dataset","description":"d$^2\\sigma$/d$y$d$p_{\\rm T}$ in bins of $p_{\\mathrm{T}}^{J/\\psi}$ for prompt J/$\\psi$ in p--Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Figure 5b"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t6","@type":"Dataset","description":"d$\\sigma$/dy for non-prompt J/$\\psi$ in p--Pb collisions at $\\sqrt{s_NN}$=5.02 TeV. The extrapolation uncertainty related to the procedure to go from...","name":"Figure 6a"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t7","@type":"Dataset","description":"d$^2\\sigma$/d$y$d$p_{\\rm T}$ in bins of $p_{\\mathrm{T}}^{J/\\psi}$ for non-prompt J/$\\psi$ in p--Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV at midrapidity..","name":"Figure 6b"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t8","@type":"Dataset","description":"Nuclear modification factor ($R_{pPb}$) in bins of $p_{\\mathrm{T}}^{J/\\psi}$ for prompt J/$\\psi$ in p--Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV at...","name":"Figure 7a"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t9","@type":"Dataset","description":"Nuclear modification factor ($R_{pPb}$) for inclusive and prompt J/$\\psi$ in p--Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV at midrapidity.","name":"Figure 7b"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t10","@type":"Dataset","description":"Nuclear modification factor ($R_{pPb}$) in bins of $p_{\\mathrm{T}}^{J/\\psi}$ for non-prompt J/$\\psi$ in p--Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV at...","name":"Figure 8a"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t11","@type":"Dataset","description":"Nuclear modification factor ($R_{pPb}$) for non-prompt J/$\\psi$ in p--Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV at midrapidity.","name":"Figure 8b"},{"@id":"https://doi.org/10.17182/hepdata.130237.v1/t12","@type":"Dataset","description":"Beauty production cross section at midrapidity (d$sigma$/d$y$) in p--Pb collisions at $\\sqrt{s_{NN}}$ = 5.02 TeV.","name":"Text_Page15"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1862791?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/130237"}],"inLanguage":"en","name":"Inclusive, prompt and non-prompt ${\\rm J}/\\psi$ production at midrapidity in p$-$Pb collisions at $\\sqrt{s_{\\rm NN}} = 5.02$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1862791?version=1","version":1}