{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.88291.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2037640"}},{"@id":"https://doi.org/10.1016/j.physletb.2022.137397","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2022","description":"Production cross sections of $\\Upsilon(1S)$, $\\Upsilon(2S)$, and $\\Upsilon(3S)$ states decaying into $\\mu^{+}\\mu^{-}$ in proton-lead (pPb) collisions are reported using data collected by the CMS experiment at $\\sqrt{s_{_{\\mathrm{NN}}}} = $ 5.02 TeV. A comparison is made with corresponding cross sections obtained with pp data measured at the same collision energy and scaled by the Pb nucleus mass number. The nuclear modification factor for $\\Upsilon(1S)$ is found to be $R_{\\mathrm{pPb}}(\\Upsilon(1S)) = $ 0.806 $ \\pm\\ $ 0.024 (stat) $ \\pm\\ $ 0.059 (syst). Similar results for the excited states indicate a sequential suppression pattern, such that $R_{\\mathrm{pPb}}(\\Upsilon(1S)) > R_{\\mathrm{pPb}}(\\Upsilon(2S)) > R_{\\mathrm{pPb}}(\\Upsilon(3S))$. The suppression is much less pronounced in pPb than in PbPb collisions, and independent of transverse momentum $p^{\\Upsilon}_{T}$ and center-of-mass rapidity $y^{\\Upsilon}_{CM}$ of the individual $\\Upsilon$ state in the studied range $p^{\\Upsilon}_{T} < $ 30 GeV/c and $|y^{\\Upsilon}_{CM}| < $ 1.93. Models that incorporate sequential suppression of bottomonia in pPb collisions are in better agreement with the data than those which only assume initial-state modifications.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t1","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(1S) as a function of pT in pPb collisions. The global uncertainty...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t2","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(2S) as a function of pT in pPb collisions. The global uncertainty...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t3","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(3S) as a function of pT in pPb collisions. The global uncertainty...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t4","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(1S) as a function of $y^{Y}_{CM}$ in pPb collisions. The global uncertainty...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t5","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(2S) as a function of $y^{Y}_{CM}$ in pPb collisions. The global uncertainty...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t6","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(3S) as a function of $y^{Y}_{CM}$ in pPb collisions. The global uncertainty...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t7","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(1S) as a function of pT in pp collisions. The global uncertainty...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t8","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(2S) as a function of pT in pp collisions. The global uncertainty...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t9","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(3S) as a function of pT in pp collisions. The global uncertainty...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t10","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(1S) as a function of $|y^{Y}_{CM}|$ in pp collisions. The global uncertainty...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t11","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(2S) as a function of $|y^{Y}_{CM}|$ in pp collisions. The global uncertainty...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t12","@type":"Dataset","description":"Differential cross section times dimuon branching fraction of Y(3S) as a function of $|y^{Y}_{CM}|$ in pp collisions. The global uncertainty...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t13","@type":"Dataset","description":"Nuclear modification factor of Y(1S) as a function of pT. The global uncertainty arises from the integrated luminosity uncertainties in...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t14","@type":"Dataset","description":"Nuclear modification factor of Y(2S) as a function of pT. The global uncertainty arises from the integrated luminosity uncertainties in...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t15","@type":"Dataset","description":"Nuclear modification factor of Y(3S) as a function of pT. The global uncertainty arises from the integrated luminosity uncertainties in...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t16","@type":"Dataset","description":"Nuclear modification factor of Y(1S) as a function of $y^{Y}_{CM}$. The global uncertainty arises from the integrated luminosity uncertainties in...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t17","@type":"Dataset","description":"Nuclear modification factor of Y(2S) as a function of $y^{Y}_{CM}$. The global uncertainty arises from the integrated luminosity uncertainties in...","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t18","@type":"Dataset","description":"Nuclear modification factor of Y(3S) as a function of $y^{Y}_{CM}$. The global uncertainty arises from the integrated luminosity uncertainties in...","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t19","@type":"Dataset","description":"Nuclear modification factor of Y(1S) at forward and backward $y^{Y}_{CM}$ for pT < 6 GeV/c. The global uncertainty arises from...","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t20","@type":"Dataset","description":"Nuclear modification factor of Y(2S) at forward and backward $y^{Y}_{CM}$ for pT < 6 GeV/c. The global uncertainty arises from...","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t21","@type":"Dataset","description":"Nuclear modification factor of Y(3S) at forward and backward $y^{Y}_{CM}$ for pT < 6 GeV/c. The global uncertainty arises from...","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t22","@type":"Dataset","description":"Nuclear modification factor of Y(1S) at forward and backward $y^{Y}_{CM}$ for 6 < pT < 30 GeV/c. The global uncertainty...","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t23","@type":"Dataset","description":"Nuclear modification factor of Y(2S) at forward and backward $y^{Y}_{CM}$ for 6 < pT < 30 GeV/c. The global uncertainty...","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t24","@type":"Dataset","description":"Nuclear modification factor of Y(3S) at forward and backward $y^{Y}_{CM}$ for 6 < pT < 30 GeV/c. The global uncertainty...","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t25","@type":"Dataset","description":"RFB of Y(1S) versus $N^{|\\eta_{lab}|<2.4}_{tracks}$.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t26","@type":"Dataset","description":"RFB of Y(2S) versus $N^{|\\eta_{lab}|<2.4}_{tracks}$.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t27","@type":"Dataset","description":"RFB of Y(3S) versus $N^{|\\eta_{lab}|<2.4}_{tracks}$.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t28","@type":"Dataset","description":"RFB of Y(1S) versus $E^{|\\eta_{lab}|>4}_{T}$.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t29","@type":"Dataset","description":"RFB of Y(2S) versus $E^{|\\eta_{lab}|>4}_{T}$.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t30","@type":"Dataset","description":"RFB of Y(3S) versus $E^{|\\eta_{lab}|>4}_{T}$.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.88291.v1/t31","@type":"Dataset","description":"Nuclear modification factor of Y(1S), Y(2S), and Y(3S) integrated over pT and $y^{Y}_{CM}$. The global uncertainty arises from the integrated...","name":"Table 31"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2037640?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/88291"}],"inLanguage":"en","name":"Nuclear modification of $\\Upsilon$ states in pPb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.02 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2037640?version=1","version":1}