{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.90452.v1/t7","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/1738845"}},{"@id":"https://doi.org/10.1140/epjc/s10052-019-7295-1","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2019","description":"Lower limits on $\\Lambda$ as a function of $m_{e^*}$ combined for the $eejj$ and the $e\\nu J$ channels. The $\\pm\\...","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/431763/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/431763/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/431763/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/431763/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/431763/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins1738845?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/90452"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.90452.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins1738845?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.90452.v1","@type":"Dataset","description":"A search for excited electrons produced in $pp$ collisions at $\\sqrt{s} = 13$ TeV via a contact interaction $q\\bar{q} \\to ee^*$ is presented. The search uses 36.1 fb$^{-1}$ of data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron via a contact interaction into an electron and a pair of quarks ($eq\\bar{q}$) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a $W$ boson ($\\nu W$) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying $W$ boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the $pp \\to ee^* \\to eeq\\bar{q}$ and $pp \\to ee^* \\to e\\nu W$ production cross sections as a function of the excited electron mass $m_{e^*}$ at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter $\\Lambda$ of the model as a function of $m_{e^*}$. For $m_{e^*} < 0.5$ TeV, the lower bound for $\\Lambda$ is 11 TeV. In the special case of $m_{e^*} = \\Lambda$, the values of $m_{e^*} < 4.8$ TeV are excluded. The presented limits on $\\Lambda$ are more stringent than those obtained in previous searches.","name":"Search for excited electrons singly produced in proton-proton collisions at $\\sqrt{s} = 13$ TeV with the ATLAS experiment at the LHC","url":"https://www.hepdata.net/record/ins1738845?version=1"},"keywords":"P P --> e e* --> e e q q, P P --> e e* --> e nu W, $\\Lambda$, 13000, Proton-Proton scattering, Exotics, Excited lepton, Excited electron","name":"Table 7","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/90582","version":1}