{"paper":{"title":"Majorana Neutrino and $W_{R}$ at TeV scale $ep$ Colliders","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":["hep-ex","physics.acc-ph"],"primary_cat":"hep-ph","authors_text":"Ankara, Ankara Turkey & National Academy of Sciences, Azerbaijan), Baku, Institute of Physics, M. Sahin (Usak University, S. Sultansoy (TOBB ETU, Turkey), U. Kaya (Ankara University, Usak","submitted_at":"2015-02-13T20:56:27Z","abstract_excerpt":"Production of heavy Majorana neutrino $N_{e}$ predicted by left-right symmetric extension of the Standard Model at future {\\normalsize TeV} scale $ep$ colliders have been considered. In order to estimate potential of $ep$ colliders for $N_{e}$ search we consider back-groundless process $e^{-}p\\rightarrow e^{+}X$ which is consequence of Majorana nature of $N_{e}$. It is shown that {\\normalsize linac-LHC} and {\\normalsize linac-FCC} based $ep$ colliders will cover much wider regions of $N_{e}$ and $W_{R}$ masses than corresponding linear electron-positron colliders."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.04115","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}