{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79799.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1606329"}},{"@id":"https://doi.org/10.1016/j.physletb.2017.09.058","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"LHCb Collaboration"},"creator":{"@type":"Organization","name":"LHCb Collaboration"},"datePublished":"2017","description":"CERN-LHC. Measurements of the cross sections, the nuclear modification factors and the forward-backward ratios for prompt and nonprompt $J/\\psi$ meson production via their dimuon decay modes in proton-lead collisions at a centre-of-mass energy of 8.16 TeV. The used data, that was taken in November and December 2016, has an integrated luminosity of 13.6 nb$^{-1}$ for the proton-lead beam configuration and 20.8 nb$^{-1}$ for the backward beam configuration. The data cover the rapidity range 1.5-4.0 (- 2.5 - - 5.0) in the nucleon-nucleon centre-of-mass system and transverse momentum range 0-14 GeV/$c$ for the proton-lead (lead-proton) beam configuration. When applicable, the first systematic uncertainty indicates the bin-by-bin correlated systematic uncertainty and the second systematic uncertainty the bin-by-bin uncorrelated systematic uncertainty.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t1","@type":"Dataset","description":"The total integrated cross sections for prompt $J/\\psi$ production, assuming no polarisation, and $J/\\psi$ production from $b$-hadron decays in the...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t2","@type":"Dataset","description":"The total integrated cross sections for prompt $J/\\psi$ production, assuming no polarisation, and $J/\\psi$ production from $b$-hadron decays in the...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t3","@type":"Dataset","description":"The double-differential cross sections for prompt $J/\\psi$ production, assuming no polarisation, as a function of transverse momentum for the rapidity...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t4","@type":"Dataset","description":"The double-differential cross sections for $J/\\psi$ production from $b$-decays as a function of transverse momentum for the rapidity range $1.5...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t5","@type":"Dataset","description":"The double-differential cross sections for prompt $J/\\psi$ production, assuming no polarisation, as a function of transverse momentum for the rapidity...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t6","@type":"Dataset","description":"The double-differential cross sections for $J/\\psi$ production from $b$-hadron decays as a function of transverse momentum for the rapidity range...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t7","@type":"Dataset","description":"Fraction of $J/\\psi$ from $b$-hadron decay in bins of transverse momentum and rapidity in the nucleon-nucleon rest frame, assuming no...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t8","@type":"Dataset","description":"Fraction of $J/\\psi$ from $b$-hadron decay in bins of transverse momentum and rapidity, assuming no polarisation, in the proton-lead beam...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t9","@type":"Dataset","description":"The nuclear modification factor $R_{p \\mathrm{Pb}}$ of prompt $J/\\psi$ for transverse momentum smaller than 14 GeV/c as a function of...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t10","@type":"Dataset","description":"The nuclear modification factor $R_{p\\mathrm{Pb}}$ of prompt $J/\\psi$ integrated over transverse momentum smaller than 14 GeV/$c$ as a function of...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t11","@type":"Dataset","description":"The nuclear modification factor $R_{p\\mathrm{Pb}}$ of $J/psi$ from the decay of $b$-hadrons for transverse momentum smaller than 14 GeV/$c$ as...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t12","@type":"Dataset","description":"The nuclear modification factor $R_{p\\mathrm{Pb}}$ of $J/\\psi$ from decay of $b$-hadrons integrated over transverse momentum smaller than 14 GeV/$c$ as...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t13","@type":"Dataset","description":"The FORWARD/BACKWARD production ratio $R_{\\mathrm{FB}}$ of prompt $J/\\psi$ as a function of transverse momentum integrated over $|y^*|$ in the range...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t14","@type":"Dataset","description":"The FORWARD/BACKWARD production ratio $R_{\\mathrm{FB}}$ of prompt $J/\\psi$ as a function of rapidity $y^*$ in the nucleon-nucleon centre-of-mass frame integrated...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t15","@type":"Dataset","description":"The FORWARD/BACKWARD production ratio $R_{\\mathrm{FB}}$ of $J/\\psi$ from $b$-hadron decays as a function of transverse momentum integrated over $|y^*|$ in...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.79799.v1/t16","@type":"Dataset","description":"The FORWARD/BACKWARD production ratio $R_{\\mathrm{FB}}$ of $J/\\psi$ from $b$-hadron decays as a function of rapidity $y^*$ in the nucleon-nucleon centre-of-mass...","name":"Table 16"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1606329?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79799"}],"inLanguage":"en","name":"Prompt and nonprompt J/$\\psi$ production and nuclear modification in $p$Pb collisions at $\\sqrt{s_{\\text{NN}}}= 8.16$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1606329?version=1","version":1}