{"paper":{"title":"Bounds on the mass of doubly-charged Higgs bosons in the same-sign diboson decay scenario","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Hiroshi Yokoya, Kei Yagyu, Mariko Kikuchi, Shinya Kanemura","submitted_at":"2014-07-24T12:33:37Z","abstract_excerpt":"A direct search for doubly-charged Higgs bosons $H^{\\pm\\pm}$ is one of the most important probe in the Higgs Triplet Model, which is motivated by generation mechanisms of tiny neutrino masses. There are two major decay modes of $H^{\\pm\\pm}$; i.e., the same-sign dilepton decay $H^{\\pm\\pm}\\to\\ell^\\pm\\ell^\\pm$ and the same-sign diboson decay $H^{\\pm\\pm}\\to W^{\\pm(*)}W^{\\pm(*)}$. For the case where the former decay mode is dominant, the lower limit on the mass of $H^{\\pm\\pm}$ has been set at about 400 GeV by ATLAS and CMS Collaborations. On the other hand, for the case where the latter decay mode "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.6547","kind":"arxiv","version":1},"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"}