{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.141277.v1/t18","@reverse":{"isBasedOn":[{"@type":"ScholarlyArticle","identifier":{"@type":"PropertyValue","propertyID":"URL","value":"https://inspirehep.net/literature/2652625"}},{"@id":"https://doi.org/10.1140/epjc/s10052-023-12021-9","@type":"JournalArticle"}]},"@type":"Dataset","additionalType":"Dataset","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","description":"The $m_{eeJ}$ distribution in the boosted two electron channel.","distribution":[{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1558317/root","description":"ROOT file","encodingFormat":"https://root.cern"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1558317/yaml","description":"YAML file","encodingFormat":"https://yaml.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1558317/csv","description":"CSV file","encodingFormat":"text/csv"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1558317/yoda","description":"YODA file","encodingFormat":"https://yoda.hepforge.org"},{"@type":"DataDownload","contentUrl":"https://www.hepdata.net/download/table/1558317/yoda.h5","description":"YODA.H5 file","encodingFormat":"https://yoda.hepforge.org"}],"identifier":[{"@type":"PropertyValue","propertyID":"HEPDataRecord","value":"https://www.hepdata.net/record/ins2652625?version=1"},{"@type":"PropertyValue","propertyID":"HEPDataRecordAlt","value":"https://www.hepdata.net/record/141277"}],"inLanguage":"en","includedInDataCatalog":{"@id":"https://doi.org/10.17182/hepdata.141277.v1","@type":"DataCatalog","url":"https://www.hepdata.net/record/ins2652625?version=1"},"isPartOf":{"@id":"https://doi.org/10.17182/hepdata.141277.v1","@type":"Dataset","description":"A search for heavy right-handed Majorana or Dirac neutrinos $N_{\\mathrm{R}}$ and heavy right-handed gauge bosons $W_{\\mathrm{R}}$ is performed in events with energetic electrons or muons, with the same or opposite electric charge, and energetic jets. The search is carried out separately for topologies of clearly separated final-state products (``resolved channel) and topologies with boosted final states with hadronic products partially overlapping and reconstructed as a large-radius jet, caused by a large mass difference between $W_{\\mathrm{R}}$ and $N_{\\mathrm{R}}$ (``boosted channel). The events are selected from $pp$ collision data at the LHC with an integrated luminosity of 139 fb$^{-1}$ collected by the ATLAS detector at $\\sqrt{s}$ = 13 TeV. No significant deviations from the Standard Model predictions are observed. The results are interpreted within the theoretical framework of a left-right symmetric model, and lower limits at 95% confidence level are set on masses in the heavy right-handed $W_{\\mathrm{R}}$ boson and $N_{\\mathrm{R}}$ plane. The excluded region extends to about $m(W_{\\mathrm{R}}) = 6.4$ TeV for both Majorana and Dirac $N_{\\mathrm{R}}$ neutrinos at $m(N_{\\mathrm{R}})<1$ TeV. $N_{\\mathrm{R}}$ with masses of less than 3.5 (3.6) TeV are excluded in the electron (muon) channel at $m(W_{\\mathrm{R}})=4.8$ TeV for the Majorana neutrinos, and limits of $m(N_{\\mathrm{R}})$ up to  3.6 TeV for $m(W_{\\mathrm{R}}) = 5.2$ (5.0) TeV in the electron (muon) channel are set for the Dirac neutrinos.","name":"Search for heavy Majorana or Dirac neutrinos and right-handed $W$ gauge bosons in final states with charged leptons and jets in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","url":"https://www.hepdata.net/record/ins2652625?version=1"},"keywords":"P P --> WR, WR --> NR l, Right-handed, Heavy neutrino, Gauge boson, Left-Right Symmetric Model, 13000.0","name":"Table 18","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/144457","version":1}