{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.114190.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1829413"}},{"@id":"https://doi.org/10.1016/j.physletb.2021.136579","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"ALICE Collaboration"},"creator":{"@type":"Organization","name":"ALICE Collaboration"},"datePublished":"2021","description":"CERN-LHC. The production of $\\Upsilon$ mesons in Pb\u2013Pb collisions at a centre-of-mass energy per nucleon pair $\\sqrt{s_{\\mathrm{NN}}}$ = 5.02 TeV is measured with the muon spectrometer of ALICE at the LHC. The yields as well as the nuclear modification factors are determined in the forward rapidity region 2.5 $<y<$ 4.0, as a function of rapidity, transverse momentum and collision centrality.\n\nThe cross sections in proton\u2013proton collisions at $\\sqrt{s}$ = 5.02 TeV used for the determination of the nuclear modification factors are also reported.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t1","@type":"Dataset","description":"Rapidity-differential yield of $\\Upsilon(1\\mathrm{S}) \\rightarrow \\mu^{+}\\mu^{-}$ divided by the average nuclear overlap function $\\langle T_{\\mathrm{AA}} \\rangle$ for the 0\u201390% centrality...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t2","@type":"Dataset","description":"Rapidity-differential yield of $\\Upsilon(2\\mathrm{S}) \\rightarrow \\mu^{+}\\mu^{-}$ divided by the average nuclear overlap function $\\langle T_{\\mathrm{AA}} \\rangle$ for the 0\u201390% centrality...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t3","@type":"Dataset","description":"$p_{\\mathrm{T}}$-differential yield of $\\Upsilon(1\\mathrm{S}) \\rightarrow \\mu^{+}\\mu^{-}$ divided by the average nuclear overlap function $\\langle T_{\\mathrm{AA}} \\rangle$ for the 0\u201390% centrality...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t4","@type":"Dataset","description":"Nuclear modification factor of $\\Upsilon(1\\mathrm{S})$ as a function of the average number of participants $\\langle N_{\\mathrm{part}} \\rangle$ or as a...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t5","@type":"Dataset","description":"Nuclear modification factor of $\\Upsilon(2\\mathrm{S})$ as a function of the average number of participants $\\langle N_{\\mathrm{part}} \\rangle$ or as a...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t6","@type":"Dataset","description":"Ratio of $\\Upsilon(2\\mathrm{S})$ and $\\Upsilon(1\\mathrm{S})$ yields (cf. equation 2 in the article for the definition) as a function of the...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t7","@type":"Dataset","description":"Relative nuclear modification factor or double yield ratio between $\\Upsilon(2\\mathrm{S})$ and $\\Upsilon(1\\mathrm{S})$ as a function of the average number of...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t8","@type":"Dataset","description":"Nuclear modification factor of $\\Upsilon(1\\mathrm{S})$ as a function of transverse momentum for the 0\u201390% centrality interval.","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t9","@type":"Dataset","description":"Nuclear modification factor of $\\Upsilon(1\\mathrm{S})$ as a function of rapidity for the 0\u201390% centrality interval.","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t10","@type":"Dataset","description":"Nuclear modification factor of $\\Upsilon(2\\mathrm{S})$ as a function of rapidity for the 0\u201390% centrality interval.","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t11","@type":"Dataset","description":"Interpolated production cross sections and cross-section ratio for $\\Upsilon(1\\mathrm{S}) \\rightarrow \\mu^{+}\\mu^{-}$ and $\\Upsilon(2\\mathrm{S}) \\rightarrow \\mu^{+}\\mu^{-}$ in proton\u2013proton collisions, integrated over...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t12","@type":"Dataset","description":"Interpolated $p_{\\mathrm{T}}$-differential cross section for $\\Upsilon(1\\mathrm{S}) \\rightarrow \\mu^{+}\\mu^{-}$ in proton\u2013proton collisions. Results used for the determination of the nuclear modification...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t13","@type":"Dataset","description":"Interpolated rapidity-differential cross section for $\\Upsilon(1\\mathrm{S}) \\rightarrow \\mu^{+}\\mu^{-}$ in proton\u2013proton collisions. Results used for the determination of the nuclear modification...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.114190.v1/t14","@type":"Dataset","description":"Interpolated rapidity-differential cross section for $\\Upsilon(2\\mathrm{S}) \\rightarrow \\mu^{+}\\mu^{-}$ in proton\u2013proton collisions. Results used for the determination of the nuclear modification...","name":"Table 14"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1829413?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/114190"}],"inLanguage":"en","name":"$\\Upsilon$ production and nuclear modification at forward rapidity in Pb-Pb collisions at $\\mathbf{\\sqrt{\\textit{s}_{\\textbf{NN}}}=5.02}$ TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1829413?version=1","version":1}