{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.76739.v1/t1","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1477805"}},{"@id":"https://doi.org/10.1016/j.physletb.2017.01.011","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2017","description":"The fiducial pp to WZ to lnul'l' cross section. The first systematic uncertainty is detector systematics and the second is...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/69975/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/69975/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/69975/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/69975/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/69975/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1477805?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/76739"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.76739.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1477805?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.76739.v1","@type":"Dataset","description":"CERN-LHC. The WZ production cross section in proton-proton collisions at sqrt(s) = 13 TeV is measured with the CMS experiment at the LHC using a data sample corresponding to an integrated luminosity of 2.3 inverse fb. The measurement is performed in the leptonic decay modes WZ to l nu l' l', where l, l' = e, mu. The measured cross section for the range 60 < m[l'l'] < 120 GeV is 39.9 +/- 3.2 (stat) +2.9/-3.1 (syst) +/- 0.4 (theo) +/- 1.3 (lumi) pb, consistent with the standard model prediction.\n\nFiducial region definition\n- leading Z lepton pt > 20 GeV\n- subleading Z lepton pt > 10 GeV\n- W lepton pt > 20 GeV\n- lepton |eta| < 2.5\n- Z invariant mass between 60 and 120 GeV\n- any same-flavor opposite-sign lepton pair invariant mass > 4 GeV\n\nTotal cross section region definition\n- Z invariant mass between 60 and 120 GeV\n- any same-flavor opposite-sign lepton pair invariant mass > 4 GeV","name":"Measurement of the WZ production cross section in pp collisions at sqrt(s) = 13 TeV","url":"https://www.hepdata.net/record/ins1477805?version=1"},"keywords":"P P --> W Z0 X, SIG, 13000, Inclusive, Integrated Cross Section, Cross Section, Proton-Proton Scattering, WZ Production, Diboson","name":"Fiducial cross section","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/77427","version":1}