{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.63971.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1280929"}},{"@id":"https://doi.org/10.1140/epjc/s10052-014-2835-1","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"LHCb Collaboration"},"creator":{"@type":"Organization","name":"LHCb Collaboration"},"datePublished":"2014","description":"CERN-LHC. The production of Upsilon(1S), Upsilon(2S) and Upsilon(3S) mesons decaying into the dimuon final state is studied with the LHCb detector using a data sample corresponding to an integrated luminosity of 3.3 pb^{-1} collected in proton-proton collisions at a centre-of-mass energy of sqrt(s) = 2.76 TeV. The differential production cross-sections times dimuon branching fractions are measured as functions of the Upsilon transverse momentum and rapidity, over the ranges pT < 15 GeV and 2.0 < y < 4.5.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.63971.v1/t1","@type":"Dataset","description":"Integrated cross-sections times dimuon branching fractions in the PT range < 15 GeV and rapidity in the range 2.0-4.5. The...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.63971.v1/t2","@type":"Dataset","description":"Integrated cross-sections times dimuon branching fractions in the PT range < 15 GeV and rapidity in the range 2.5-4.0. The...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.63971.v1/t3","@type":"Dataset","description":"Single differential cross-section for UPSI(1S) times the dimuon branching fraction as a function of PT for the rapidity region 2.0-4.5...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.63971.v1/t4","@type":"Dataset","description":"Single differential cross-section for UPSI(2S) times the dimuon branching fraction as a function of PT for the rapidity region 2.0-4.5...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.63971.v1/t5","@type":"Dataset","description":"Single differential cross-section for UPSI(3S) times the dimuon branching fraction as a function of PT for the rapidity region 2.0-4.5...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.63971.v1/t6","@type":"Dataset","description":"Single differential cross-section for UPSI(1S) times the dimuon branching fraction as a function of rapidity for PT < 15 GeV...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.63971.v1/t7","@type":"Dataset","description":"Single differential cross-section for UPSI(2S) times the dimuon branching fraction as a function of rapidity for PT < 15 GeV...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.63971.v1/t8","@type":"Dataset","description":"Single differential cross-section for UPSI(3S) times the dimuon branching fraction as a function of rapidity for PT < 15 GeV...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.63971.v1/t9","@type":"Dataset","description":"Ratios of UPSI(2S) to UPSI(1S) and UPSI(3S) to UPSI(1S) cross-sections times the dimuon branching fractions as a function of PT...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.63971.v1/t10","@type":"Dataset","description":"Ratios of UPSI(2S) to UPSI(1S) and UPSI(3S) to UPSI(1S) cross-sections times the dimuon branching fractions as a function of rapidity...","name":"Table 10"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1280929?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/63971"}],"inLanguage":"en","name":"Measurement of Upsilon production in pp collisions at sqrt{s}=2.76 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1280929?version=1","version":1}