{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.73583.v1/t9","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1399056"}},{"@id":"https://doi.org/10.1007/JHEP07(2016)052","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"LHCb Collaboration"},"creator":{"@type":"Organization","name":"LHCb Collaboration"},"datePublished":"2016","description":"Normalized differential cross-section $\\frac{\\pi}{\\sigma}\\frac{ \\mathrm{d}\\sigma(\\Upsilon(1S)D^0)}{\\mathrm{d} \\left| \\Delta \\phi \\right| }$ for $2<y(\\Upsilon(1S))<4.5$, $2<y(D^0)<4.5$, $p_T(D^0)>1$ GeV/$c$. Only statistical uncertainties are quoted...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/65416/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/65416/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/65416/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/65416/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1399056?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/73583"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.73583.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1399056?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.73583.v1","@type":"Dataset","description":"CERN-LHCb. Associated production of bottomonia and open charm hadrons in $pp$ collisions at $\\sqrt{s}=7$ and $8$TeV is observed\n    using data corresponding to an integrated luminosity of 3 fb$^{-1}$ accumulated with the LHCb detector.\n    The observation of five combinations, $\\Upsilon(1S)D^0$, $\\Upsilon(2S)D^0$, $\\Upsilon(1S)D^+$, $\\Upsilon(2S)D^+$\n    and $\\Upsilon(1S)D^+_s$, is reported. Production cross-sections are measured for $\\Upsilon(1S)D^0$ and $\\Upsilon(1S)D^+$pairs\n    in the forward region. The measured cross-sections and the differential distributions indicate the dominance of double parton\n    scattering as the main production mechanism. This allows a precise measurement of the effective cross-section for double\n    parton scattering. $\\Upsilon$ mesons are recontructed using $\\Upsilon \\to \\mu^+ \\mu^-$ decay mode, while for charm hadrons\n    $D^0 \\to K^- \\pi^+$, $D^+ \\to K^- \\pi^+ \\pi^+$, $D^+_s \\to K^- K^+ \\pi^+$ and $\\Lambda_c \\to K^- \\pi^+$ decay modes are used.","name":"Production of associated $\\Upsilon$ and open charm hadrons in $pp$ collisions at $\\sqrt{s}=7$ and $8$TeV via double parton scattering","url":"https://www.hepdata.net/record/ins1399056?version=1"},"keywords":"P P --> UPSILON(1S) D0, D(SIG)/DPHI, Exclusive, Upsilon, Azimuthal Angular Dependence, Proton-Proton Scattering, Strange Production, Charm Production, Muon Production, 7000.0-8000.0","name":"Table 9","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/73594","version":1}