{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.82546.v1/t2","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1676472"}},{"@id":"https://doi.org/10.1016/j.physletb.2018.10.021","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"The signal selection acceptance times efficiency (A$\\times \\epsilon$), defined as the ratio of the number of MC signal events in...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/256380/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/256380/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/256380/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/256380/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/256380/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1676472?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/82546"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.82546.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1676472?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.82546.v1","@type":"Dataset","description":"CERN-LHC, ATLAS\nHEP data for the Search for resonant W Z Production in the fully leptonic final state in Proton-Proton Collisions at sqrt(s) = 13 TeV with the ATLAS Detector.\n\nA search is performed for a heavy resonance decaying to W Z in the fully leptonic channel. It is based on proton-proton collision data collected by the ATLAS experiment at the LHC at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 36.1 fb$^{\u22121}$. No significant excess is observed over Standard Model predictions and limits are set on the production cross section times branching ratio of a heavy vector particle produced either in quark-antiquark fusion or by vector boson fusion. Constraints are also obtained on the mass and couplings of a singly-charged Higgs, in the Georgi-Machacek model, produced by vector boson fusion.","name":"Search for resonant $WZ$ production in the fully leptonic final state in proton-proton collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","url":"https://www.hepdata.net/record/ins1676472?version=1"},"keywords":"WPRIME --> Z0 W, 13000.0, HVT, WZ, lvll, W', resonance","name":"Table 2","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/83530","version":1}