{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.79407.v1/t18","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1628411"}},{"@id":"https://doi.org/10.1140/epjc/s10052-017-5491-4","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2018","description":"Figure 12, bottom, subfigure c, Upper limits at 95% CL on the resonance production cross section times branching fraction for...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/181379/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/181379/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/181379/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/181379/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/181379/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1628411?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/79407"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.79407.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1628411?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.79407.v1","@type":"Dataset","description":"A search for neutral heavy resonances is performed in the $WW\\to e\\nu\\mu\\nu$ decay channel using $pp$ collision data corresponding to an integrated luminosity of 36.1 fb$^{-1}$, collected at a centre-of-mass energy of 13 TeV by the ATLAS detector at the Large Hadron Collider. No evidence of such heavy resonances is found. In the search for production via the quark--antiquark annihilation or gluon--gluon fusion process, upper limits on $\\sigma_X \\times B(X \\to WW)$ as a function of the resonance mass are obtained in the mass range between 200 GeV and up to 5 TeV for various benchmark models: a Higgs-like scalar in different width scenarios, a two-Higgs-doublet model, a heavy vector triplet model, and a warped extra dimensions model. In the vector-boson fusion process, constraints are also obtained on these resonances, as well as on a Higgs boson in the Georgi--Machacek model and a heavy tensor particle coupling only to gauge bosons.","name":"Search for heavy resonances decaying into $WW$ in the $e\\nu\\mu\\nu$ final state in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","url":"https://www.hepdata.net/record/ins1628411?version=1"},"keywords":"PP-->X-->WW-->evmuv, SIG, 13000","name":"Table 18","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/81447","version":1}