{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.64486.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1342266"}},{"@id":"https://doi.org/10.1016/j.physletb.2015.07.037","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2015","description":"CERN-LHC.  Differential cross sections as a function of transverse momentum $p_\\mathrm{T}$ are presented for the production of $\\Upsilon(n\\mathrm{S})$ ($n$ = 1, 2, 3) states decaying into a pair of muons. Data corresponding to an integrated luminosity of 4.9 fb$^{-1}$ in pp collisions at $\\sqrt{s}$ = 7 TeV were collected with the CMS detector at the LHC. The analysis selects events with dimuon absolute rapidity $y$ lower than 1.2 and dimuon transverse momentum in the range of $p_\\mathrm{T} $ between 10 and 100 GeV. The measurements show a transition from an exponential to a power-law behavior at $p_\\mathrm{T} \\approx 20$ GeV for the three $\\Upsilon$ states. Above that transition, the $\\Upsilon(3\\mathrm{S})$ spectrum is significantly harder than that of the $\\Upsilon(1\\mathrm{S})$ and $\\Upsilon(2\\mathrm{S})$. The ratios of the $\\Upsilon(3\\mathrm{S})$ and $\\Upsilon(2\\mathrm{S})$ differential cross sections to the $\\Upsilon(1\\mathrm{S})$ cross section show a rise as $p_\\mathrm{T}$ increases at low $p_\\mathrm{T}$, then become flatter at higher $p_\\mathrm{T}$\n\nThe tables below list the results of $\\Upsilon$(1S), $\\Upsilon$(2S) and $\\Upsilon$(3S) differential cross sections (SIG) times dimuon branching fraction (B) in three rapidity bins, and ratios thereof. The $\\Upsilon$(nS) polarizations measured by CMS are taken as input. The cross sections for different polarization scenarios may be obtained using the corresponding acceptance tables that are also provided below.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t1","@type":"Dataset","description":"The $p_{\\rm T}$ bin width, the weighted mean $p_{\\rm T}$ within a bin, and the differential cross section times the...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t2","@type":"Dataset","description":"The $p_{\\rm T}$ bin width, the weighted mean $p_{\\rm T}$ within a bin, and the differential cross section times the...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t3","@type":"Dataset","description":"The $p_{\\rm T}$ bin width, the weighted mean $p_{\\rm T}$ within a bin, and the differential cross section times the...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t4","@type":"Dataset","description":"The $p_{\\rm T}$ bin width and corrected yield ratios R21 and R31 for $|y| < 0.6$. The statistical and systematic...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t5","@type":"Dataset","description":"The $p_{\\rm T}$ bin width and corrected yield ratios R21 and R31 for $0.6 < |y| < 1.2$. The statistical...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t6","@type":"Dataset","description":"The $p_{\\rm T}$ bin width and corrected yield ratios R21 and R31 for $|y| < 1.2$. The statistical and systematic...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t7","@type":"Dataset","description":"The dimuon acceptance $\\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\\mathcal{A}(\\sigma^{\\pm})$, and the values...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t8","@type":"Dataset","description":"The dimuon acceptance $\\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\\mathcal{A}(\\sigma^{\\pm})$, and the values...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t9","@type":"Dataset","description":"The dimuon acceptance $\\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\\mathcal{A}(\\sigma^{\\pm})$, and the values...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t10","@type":"Dataset","description":"The dimuon acceptance $\\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\\mathcal{A}(\\sigma^{\\pm})$, and the values...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t11","@type":"Dataset","description":"The dimuon acceptance $\\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\\mathcal{A}(\\sigma^{\\pm})$, and the values...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t12","@type":"Dataset","description":"The dimuon acceptance $\\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\\mathcal{A}(\\sigma^{\\pm})$, and the values...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t13","@type":"Dataset","description":"The dimuon acceptance $\\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\\mathcal{A}(\\sigma^{\\pm})$, and the values...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t14","@type":"Dataset","description":"The dimuon acceptance $\\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\\mathcal{A}(\\sigma^{\\pm})$, and the values...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.64486.v1/t15","@type":"Dataset","description":"The dimuon acceptance $\\mathcal{A}$ calculated using the CMS measured polarization and its positive and negative uncertainties $\\mathcal{A}(\\sigma^{\\pm})$, and the values...","name":"Table 15"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1342266?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/64486"}],"inLanguage":"en","name":"Measurements of the Upsilon(1S), Upsilon(2S), and Upsilon(3S) differential cross sections in pp collisions at sqrt(s) = 7 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1342266?version=1","version":1}