{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.82210.v1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1670013"}},{"@id":"https://doi.org/10.1007/JHEP07(2018)134","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Collection","author":{"@type":"Organization","name":"LHCb Collaboration"},"creator":{"@type":"Organization","name":"LHCb Collaboration"},"datePublished":"2019","description":"CERN-LHCb.The production of $\\Upsilon$ mesons in $pp$ collisions \n at $\\sqrt{s}=13$ TeV is studied with the LHCb detector using data samples corresponding \n to an integrated luminosity of 277 pb$^{-1}$. The production cross-sections \n and ratios of cross-sections are measured as functions\nof the meson transverse momentum\n $p_T$ and rapidity $y$, for $p_T < 30$ GeV/$c$\nand $2.0<y<4.5$.\n $\\Upsilon$ mesons are recontructed using $\\Upsilon \\to \\mu^+\n\\mu^-$ decay mode.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t1","@type":"Dataset","description":"Double-differential cross-sections times dimuon branching fraction in different bins of $p_T$ and $y$ for $\\Upsilon$(1S) (in pb). The first uncertainty...","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t2","@type":"Dataset","description":"Double-differential cross-sections times dimuon branching fraction in different bins of $p_T$ and $y$ for $\\Upsilon$(2S) (in pb). The first uncertainty...","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t3","@type":"Dataset","description":"Double-differential cross-sections times dimuon branching fraction in different bins of $p_T$ and $y$ for $\\Upsilon$(3S) (in pb). The first uncertainty...","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t4","@type":"Dataset","description":"Differential cross-sections multiplied by dimuon branching fractions for $\\Upsilon$(1S), $\\Upsilon$(2S) and $\\Upsilon$(3S) states versus $p_T$ integrated over $y$ between 2.0...","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t5","@type":"Dataset","description":"Differential cross-sections multiplied by dimuon branching fractions for $\\Upsilon$(1S), $\\Upsilon$(2S) and $\\Upsilon$(3S) states versus $y$ integrated over $p_T$ from 0...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t6","@type":"Dataset","description":"Ratios of double-differential cross-sections times dimuon branching fractions for $\\Upsilon$(2S) to $\\Upsilon$(1S).","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t7","@type":"Dataset","description":"Ratios of double-differential cross-sections times dimuon branching fractions for $\\Upsilon$(3S) to $\\Upsilon$(1S).","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t8","@type":"Dataset","description":"Ratios of differential cross-sections times dimuon branching fractions versus $p_T$ over $y$ for $\\Upsilon$(2S) to $\\Upsilon$(1S) and $\\Upsilon$(3S) to $\\Upsilon$(1S).","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t9","@type":"Dataset","description":"Ratios of differential cross-sections times dimuon branching fractions versus $y$ over $p_T$ for $\\Upsilon$(2S) to $\\Upsilon$(1S) and $\\Upsilon$(3S) to $\\Upsilon$(1S).","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t10","@type":"Dataset","description":"The cross-section ratios between 13 TeV and 8 TeV in different bins of $p_T$ and $y$ for $\\Upsilon$(1S).","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t11","@type":"Dataset","description":"The cross-section ratios between 13 TeV and 8 TeV in different bins of $p_T$ and $y$ for $\\Upsilon$(2S).","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t12","@type":"Dataset","description":"The cross-section ratios between 13 TeV and 8 TeV in different bins of $p_T$ and $y$ for $\\Upsilon$(3S).","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t13","@type":"Dataset","description":"Ratios of differential cross-sections between 13 TeV and 8 TeV measurements versus $p_T$ over $y$ for $\\Upsilon$(1S), $\\Upsilon$(2S) and $\\Upsilon$(3S).","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.82210.v1/t14","@type":"Dataset","description":"Ratios of differential cross-sections between 13 TeV and 8 TeV measurements versus $y$ over $p_T$ for $\\Upsilon$(1S), $\\Upsilon$(2S) and $\\Upsilon$(3S).","name":"Table 14"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1670013?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/82210"}],"inLanguage":"en","name":"Measurement of $\\Upsilon$ production in $pp$ collisions at $\\sqrt{s}$= 13 TeV","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins1670013?version=1","version":1}