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dc.contributor.authorKanemura, Sen_US
dc.contributor.authorKasai, Ten_US
dc.contributor.authorLin, GLen_US
dc.contributor.authorOkada, Yen_US
dc.contributor.authorTseng, JJen_US
dc.contributor.authorYuan, CPen_US
dc.date.accessioned2019-04-03T06:39:25Z-
dc.date.available2019-04-03T06:39:25Z-
dc.date.issued2001-09-01en_US
dc.identifier.issn0556-2821en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevD.64.053007en_US
dc.identifier.urihttp://hdl.handle.net/11536/29406-
dc.description.abstractTo generate small neutrino masses radiatively, the Zee model introduces two Higgs doublets and one weak-singlet charged Higgs boson to its Higgs sector. From analyzing the renormalization group equations, we determine the possible range of the lightest CP-even Higgs boson (h) mass and the Higgs boson self-couplings as a function of the cutoff scale beyond which either some of the coupling constants are strong enough to invalidate the perturbative analysis or the stability of the electroweak vacuum is no longer guaranteed. Using the results obtained from the above analysis, we find that the singlet charged Higgs boson can significantly modify the partial decay width of h --> gamma gamma via radiative corrections, and its collider phenomenology can also be drastically different from that of the charged Higgs bosons in the usual two-Higgs-doublet models.en_US
dc.language.isoen_USen_US
dc.titlePhenomenology of Higgs bosons in the Zee modelen_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevD.64.053007en_US
dc.identifier.journalPHYSICAL REVIEW Den_US
dc.citation.volume64en_US
dc.citation.issue5en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department交大名義發表zh_TW
dc.contributor.departmentNational Chiao Tung Universityen_US
dc.identifier.wosnumberWOS:000170726200010en_US
dc.citation.woscount37en_US
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