{"@context":"http://schema.org","@id":"https://doi.org/10.17182/hepdata.141277.v1","@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":"Collection","author":{"@type":"Organization","name":"ATLAS Collaboration"},"creator":{"@type":"Organization","name":"ATLAS Collaboration"},"datePublished":"2023","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.","hasPart":[{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t1","@type":"Dataset","description":"Observed 95% CL exclusion contours in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel for boosted.","name":"Table 1"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t2","@type":"Dataset","description":"Expected 95% CL exclusion contours in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel for boosted.","name":"Table 2"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t3","@type":"Dataset","description":"Observed 95% CL exclusion contours in the $(m(W_{R}), m(N_{R}))$ plane in the muon channel for boosted.","name":"Table 3"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t4","@type":"Dataset","description":"Expected 95% CL exclusion contours in the $(m(W_{R}), m(N_{R}))$ plane in the muon channel for boosted.","name":"Table 4"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t5","@type":"Dataset","description":"Observed 95% CL exclusion contours for the assumption of Dirac type in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel...","name":"Table 5"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t6","@type":"Dataset","description":"Expected 95% CL exclusion contours for the assumption of Dirac type in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel...","name":"Table 6"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t7","@type":"Dataset","description":"Observed 95% CL exclusion contours for the assumpition of Dirac type in the $(m(W_{R}), m(N_{R}))$ plane in the muon channel...","name":"Table 7"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t8","@type":"Dataset","description":"Expected 95% CL exclusion contours for the assumption of Dirac type in the $(m(W_{R}), m(N_{R}))$ plane in the muon channel...","name":"Table 8"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t9","@type":"Dataset","description":"Observed 95% CL exclusion contours for the assumption of Majorana type in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel...","name":"Table 9"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t10","@type":"Dataset","description":"Expected 95% CL exclusion contours for the assumption of Majorana type in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel...","name":"Table 10"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t11","@type":"Dataset","description":"Observed 95% CL exclusion contours for the assumption of Majorana type in the $(m(W_{R}), m(N_{R}))$ plane in the muon channel...","name":"Table 11"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t12","@type":"Dataset","description":"Expected 95% CL exclusion contours for the assumption of Majorana type in the $(m(W_{R}), m(N_{R}))$ plane in the muon channel...","name":"Table 12"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t13","@type":"Dataset","description":"Observed 95% CL exclusion contours for the assumption of Dirac type in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel...","name":"Table 13"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t14","@type":"Dataset","description":"Expected 95% CL exclusion contours for the assumption of Dirac type in the $(m(W_{R}), m(N_{R}))$ plane in the electron channel...","name":"Table 14"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t15","@type":"Dataset","description":"Observed 95% CL exclusion contours for the assumption of Dirac type in the $(m(W_{R}), m(N_{R}))$ plane in the muon channel...","name":"Table 15"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t16","@type":"Dataset","description":"Expected 95% CL exclusion contours for the assumption of Dirac type in the $(m(W_{R}), m(N_{R}))$ plane in the muon channel...","name":"Table 16"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t17","@type":"Dataset","description":"The $m_{eJ}$ distribution in the boosted one electron channel.","name":"Table 17"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t18","@type":"Dataset","description":"The $m_{eeJ}$ distribution in the boosted two electron channel.","name":"Table 18"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t19","@type":"Dataset","description":"The $m_{\\mu\\mu J}$ distribution in the boosted two muon channel.","name":"Table 19"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t20","@type":"Dataset","description":"The $m_{jj}$ distribution in the resolved electron channel.","name":"Table 20"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t21","@type":"Dataset","description":"The $m_{jj}$ distribution in the resolved muon channel.","name":"Table 21"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t22","@type":"Dataset","description":"The $m_{eejj}$ distribution in the resolved electron channel.","name":"Table 22"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t23","@type":"Dataset","description":"The $m_{\\mu\\mu jj}$ distribution in the resolved muon channel.","name":"Table 23"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t24","@type":"Dataset","description":"The $h_{T}$ distribution in the resolved electron channel.","name":"Table 24"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t25","@type":"Dataset","description":"The $h_{T}$ distribution in the resolved muon channel.","name":"Table 25"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t26","@type":"Dataset","description":"Acceptance $\\times$ efficiency for bSR1e.","name":"Table 26"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t27","@type":"Dataset","description":"Acceptance $\\times$ efficiency for bSR2e.","name":"Table 27"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t28","@type":"Dataset","description":"Acceptance $\\times$ efficiency for bSR2mu.","name":"Table 28"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t29","@type":"Dataset","description":"Acceptance $\\times$ efficiency for rSROS2e.","name":"Table 29"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t30","@type":"Dataset","description":"Acceptance $\\times$ efficiency for rSROS2mu.","name":"Table 30"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t31","@type":"Dataset","description":"Acceptance $\\times$ efficiency for rSRSS2e.","name":"Table 31"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t32","@type":"Dataset","description":"Acceptance $\\times$ efficiency for rSRSS2mu.","name":"Table 32"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t33","@type":"Dataset","description":"Expected and observed 95% CL upper limits for $\\sigma(pp\\to W_{R})\\times B(W_{R}\\to eeqq)$ as a function of $m(W_{R})$ for the special...","name":"Table 33"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t34","@type":"Dataset","description":"Expected and observed 95% CL upper limits for $\\sigma(pp\\to W_{R})\\times B(W_{R} \\to \\mu\\mu qq)$ as a function of $m(W_{R})$ for...","name":"Table 34"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t35","@type":"Dataset","description":"Expected and observed 95% CL upper limits for $\\sigma(pp\\to W_{R})\\times B(W_{R} \\to eeqq)$ as a function of $m(W_{R})$ for the...","name":"Table 35"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t36","@type":"Dataset","description":"Expected and observed 95% CL upper limits for $\\sigma(pp\\to W_{R})\\times B(W_{R} \\to \\mu \\mu qq)$ as a function of $m(W_{R})$...","name":"Table 36"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t37","@type":"Dataset","description":"Expected and observed 95% CL upper limits for $\\sigma(pp \\to W_{R}) \\times B(W_{R} \\to eeqq)$ as a function of $m(W_{R})$...","name":"Table 37"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t38","@type":"Dataset","description":"Expected and observed 95% CL upper limits for $\\sigma(pp \\to W_{R}) \\times B(W_{R} \\to \\mu\\mu qq)$ as a function of...","name":"Table 38"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t39","@type":"Dataset","description":"Expected and observed 95% CL upper limits for $\\sigma(pp \\to W_{R}) \\times B(W_{R} \\to eeqq)$ as a function of $m(W_{R})$...","name":"Table 39"},{"@id":"https://doi.org/10.17182/hepdata.141277.v1/t40","@type":"Dataset","description":"Expected and observed 95% CL upper limits for $\\sigma(pp \\to W_{R}) \\times B(W_{R} \\to \\mu \\mu qq)$ as a function...","name":"Table 40"}],"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","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","provider":{"@type":"Organization","name":"HEPData"},"publisher":{"@type":"Organization","name":"HEPData"},"url":"https://www.hepdata.net/record/ins2652625?version=1","version":1}