{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.89400.v1/t3","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1487288"}},{"@id":"https://doi.org/10.1140/epjc/s10052-017-4730-z","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"CMS Collaboration"},"creator":{"@type":"Organization","name":"CMS Collaboration"},"datePublished":"2019","description":"Differential cross section as function of the Z boson transverse momentum.","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/414600/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/414600/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/414600/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/414600/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/414600/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1487288?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/89400"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.89400.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1487288?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.89400.v1","@type":"Dataset","description":"CERN LHC. The WZ production cross section is measured by the CMS experiment at the CERN LHC in proton-proton collision data samples corresponding to integrated luminosities of 4.9 fb\u22121 collected at \u221as = 7 TeV, and 19.6 fb\u22121 at \u221as= 8 TeV. The measurements are performed using the fully-leptonic WZ decay modes with electrons and muons in the final state. The measured cross sections for 71 < mZ < 111 GeV are \u03c3(pp \u2192 WZ; \u221as = 7 TeV) = 20.14 \u00b1 1.32 (stat) \u00b1 0.38 (theo) \u00b1 1.06 (exp) \u00b1 0.44 (lumi) pb and \u03c3(pp \u2192 WZ; \u221as = 8 TeV) = 24.09 \u00b1 0.87 (stat) \u00b1 0.80 (theo) \u00b1 1.40 (exp) \u00b1 0.63 (lumi) pb. Differential cross sections with respect to the Z boson pT, the leading jet pT, and the number of jets are obtained using the \u221as = 8 TeV data. The results are consistent with standard model predictions and constraints on anomalous triple gauge couplings are obtained.","name":"Measurement of the WZ production cross section in pp collisions at sqrt{s} = 7 and 8 TeV and search for anomalous triple gauge couplings at sqrt{s} = 8 TeV","url":"https://www.hepdata.net/record/ins1487288?version=1"},"keywords":"P P --> W Z0 X, DSIG/DPT(Z), 8000.0, Electroweak, Differential cross section, Proton-Proton Scattering, WZ production","name":"Table 3","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/89416","version":1}