{ "id": "1106.3427", "version": "v2", "published": "2011-06-17T09:51:26.000Z", "updated": "2011-08-26T10:23:46.000Z", "title": "Production of doubly charged scalars from the decay of a heavy SM-like Higgs boson in the Higgs Triplet Model", "authors": [ "A. G. Akeroyd", "S. Moretti" ], "comment": "21 pages, 30 figures; in v2 all figures modified slightly to account for plotting error, discussion of impact of recent Higgs searches added, to appear in Physical Review D", "doi": "10.1103/PhysRevD.84.035028", "categories": [ "hep-ph" ], "abstract": "The Higgs Triplet Model (HTM) of neutrino mass generation predicts the existence of doubly charged Higgs bosons (H^{\\pm\\pm}). In the HTM a scalar eigenstate (H_2) is dominantly composed of the scalar field from the isospin doublet, and could be significantly heavier than H^{\\pm\\pm}. Such a scenario would allow the possibility of a large branching ratio for the decay H_2-> H^{++}H^{--}. From the production mechanism of gluon-gluon fusion, gg-> H_2, the above decay mode would give rise to pair production of doubly charged Higgs bosons (H^{++}H^{--}) with a cross section which could be significantly larger than the cross sections for the standard production mechanisms qqbar -> \\gamma,Z-> H^{++}H^{--} and q'qbar -> W -> H^{\\pm\\pm}H^{\\mp}. We discuss the phenomenological consequences for the ongoing searches for H^{\\pm\\pm} at the Tevatron and at the LHC.", "revisions": [ { "version": "v2", "updated": "2011-08-26T10:23:46.000Z" } ], "analyses": { "subjects": [ "12.60.Fr", "14.80.Fd" ], "keywords": [ "higgs triplet model", "heavy sm-like higgs boson", "doubly charged scalars", "doubly charged higgs bosons", "neutrino mass generation predicts" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physical Review D", "year": 2011, "month": "Aug", "volume": 84, "number": 3, "pages": "035028" }, "note": { "typesetting": "TeX", "pages": 21, "language": "en", "license": "arXiv", "status": "editable", "inspire": 914148, "adsabs": "2011PhRvD..84c5028A" } } }