Please use this identifier to cite or link to this item: https://ir.swu.ac.th/jspui/handle/123456789/13935
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dc.contributor.authorGrinstein B.
dc.contributor.authorMurphy C.W.
dc.contributor.authorPirtskhalava D.
dc.contributor.authorUttayarat P.
dc.date.accessioned2021-04-05T03:32:43Z-
dc.date.available2021-04-05T03:32:43Z-
dc.date.issued2014
dc.identifier.issn11266708
dc.identifier.other2-s2.0-84901683578
dc.identifier.urihttps://ir.swu.ac.th/jspui/handle/123456789/13935-
dc.identifier.urihttps://www.scopus.com/inward/record.uri?eid=2-s2.0-84901683578&doi=10.1007%2fJHEP05%282014%29083&partnerID=40&md5=a71bfb4c35b3db68490bd5e29d9da1e5
dc.description.abstractWe present a sum rule for Higgs fields in general representations under SU(2) L × U(1) Y that follows from the connection between the Higgs couplings and the mechanism that gives the electroweak bosons their masses, and at the same time restricts these couplings. Sum rules that follow from perturbative unitarity will require us to include singly and doubly charged Higgses in our analysis. We examine the consequences of these sum rules for Higgs phenomenology in both model independent and model specific ways. The relation between our sum rules and other works, based on dispersion relations, is also clarified. © 2014 The Author(s).
dc.titleTheoretical constraints on additional Higgs bosons in light of the 126 GeV Higgs
dc.typeArticle
dc.rights.holderScopus
dc.identifier.bibliograpycitationJournal of High Energy Physics. Vol 2014, No.5 (2014)
dc.identifier.doi10.1007/JHEP05(2014)083
Appears in Collections:Scopus 1983-2021

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