{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.93070.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1699106"}},{"@id":"https://doi.org/10.1007/JHEP11(2018)194","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"LHCb Collaboration"},"creator":{"@type":"Organization","name":"LHCb Collaboration"},"datePublished":"2020","description":"CERN-LHC. The production of $\\Upsilon(nS)$ mesons ($n=1,2,3$) in $p$Pb and Pb$p$ collisions at a centre-of-mass energy per nucleon pair $\\sqrt{s_{NN}}=8.16$ TeV is measured by the LHCb experiment, using a data sample corresponding to an integrated luminosity of 31.8 $nb^{-1}$. The $\\Upsilon(nS)$ mesons are reconstructed through their decays into two opposite-sign muons. The measurements comprise the differential production cross-sections of the $\\Upsilon(1S)$ and $\\Upsilon(2S)$ states, their forward-to-backward ratios and nuclear modification factors, performed as a function of the transverse momentum p_{T} and rapidity in the nucleon-nucleon centre-of-mass frame $y^*$ of the $\\Upsilon(nS)$ states, in the kinematic range $p_{T}<25$ GeV$/c$ and $1.5<y^*<4.0$ ($-5.0<y^*<-2.5$) for $p$Pb (Pb$p$) collisions. In addition, production cross-sections for $\\Upsilon(3S)$ are measured integrated over phase space and the production ratios between all three $\\Upsilon(nS)$ states are determined.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t1","@type":"Dataset","description":"$\\Upsilon(1S)$ production cross-section in $p$Pb, as a function of $p_{T}$ and $y*$. The uncertainty is the sum in quadrature of...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t2","@type":"Dataset","description":"$\\Upsilon(1S)$ production cross-section in Pb$p$, as a function of $p_{T}$ and $y^*$. The uncertainty is the sum in quadrature of...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t3","@type":"Dataset","description":"$\\Upsilon(1S)$ production cross-section in $p$Pb and Pb$p$, as a function of $p_{T}$. The uncertainty is the sum in quadrature of...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t4","@type":"Dataset","description":"$\\Upsilon(1S)$ production cross-section in $p$Pb and Pb$p$, as a function of $y^*$. The uncertainty is the sum in quadrature of...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t5","@type":"Dataset","description":"$\\Upsilon(2S)$ production cross-section in $p$Pb and Pb$p$, as a function of $p_{T}$. The uncertainty is the sum in quadrature of...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t6","@type":"Dataset","description":"$\\Upsilon(2S)$ production cross-section in $p$Pb and Pb$p$, as a function of $y^*$. The uncertainty is the sum in quadrature of...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t7","@type":"Dataset","description":"Scaled $pp$ differential cross-section in $p_{T}$ at $\\sqrt{s_{NN}}=8.16$ TeV. The first uncertainty is statistical, the second is systematic, which includes...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t8","@type":"Dataset","description":"Scaled $pp$ differential cross-section in $y$ at $\\sqrt{s_{NN}}=8.16$ TeV. The first uncertainty is statistical, the second is systematic, which includes...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t9","@type":"Dataset","description":"$\\Upsilon(1S)$ nuclear modification factor, $R_{p{\\rm Pb}}^{\\Upsilon(1S)}$, in $p$Pb and Pb$p$ as a function of $p_{T}$ integrated over $y^*$ in the...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t10","@type":"Dataset","description":"$\\Upsilon(1S)$ nuclear modification factor, $R_{p{\\rm Pb}}^{\\Upsilon(1S)}$, in $p$Pb and Pb$p$ as a function of $y^*$ integrated over $p_{T}$ in the...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t11","@type":"Dataset","description":"$\\Upsilon(2S)$ nuclear modification factor, $R_{p{\\rm Pb}}^{\\Upsilon(2S)}$, in $p$Pb and Pb$p$ as a function of $p_{T}$ integrated over $y^*$ in the...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t12","@type":"Dataset","description":"$\\Upsilon(2S)$ nuclear modification factor, $R_{p{\\rm Pb}}^{\\Upsilon(2S)}$, in $p$Pb and Pb$p$ as a function of $y^*$ integrated over $p_{T}$ in the...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t13","@type":"Dataset","description":"$\\Upsilon(1S)$ forward-to-backward ratio, $R_{{\\rm FB}}^{\\Upsilon(1S)}$, as a function of $p_{T}$ integrated over $\\vert y^* \\vert$ in the range $2.5 <...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t14","@type":"Dataset","description":"$\\Upsilon(1S)$ forward-to-backward ratio, $R_{{\\rm FB}}^{\\Upsilon(1S)}$, as a function of $\\vert y^* \\vert$ integrated over $p_{T}$ in the range $0 <...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t15","@type":"Dataset","description":"$\\Upsilon(2S)$ to $\\Upsilon(1S)$ ratio, in $p$Pb and Pb$p$ as a function of $p_{T}$ integrated over $y^*$ in the range $1.5...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t16","@type":"Dataset","description":"$\\Upsilon(2S)$ to $\\Upsilon(1S)$ ratio, in $p$Pb and Pb$p$ as a function of $y^*$ integrated over $p_{T}$ in the range $0...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.93070.v1/t17","@type":"Dataset","description":"$\\Upsilon(1S)$ to non-prompt $J/\\psi$, in $p$Pb and Pb$p$ as a function of $y^*$ integrated over $p_{T}$ in the range $0...","name":"Table 17"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1699106?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/93070"}],"inLanguage":"en","name":"Study of $\\Upsilon$ production in $p$Pb collisions at $\\sqrt{s_{NN}}=8.16$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1699106?version=1","version":1}