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The fermion mass scale and possible effects of Higgs bosons on experimental observables

dc.contributor.authorHaber, Harry E.en_US
dc.contributor.authorKane, Gordon L.en_US
dc.contributor.authorSterling, T.en_US
dc.date.accessioned2006-04-07T17:30:57Z
dc.date.available2006-04-07T17:30:57Z
dc.date.issued2006-04-07T17:30:57Z
dc.identifier.citationHaber, H. E., Kane, G. L., Sterling, T. ()."The fermion mass scale and possible effects of Higgs bosons on experimental observables." Nuclear Physics B 161(2-3): 493-532. <http://hdl.handle.net/2027.42/23439>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B6TVC-473DNS7-13S/2/76f720181327dbe3410e4f230898aedaen_US
dc.identifier.urihttps://hdl.handle.net/2027.42/23439
dc.description.abstractWe consider a conventional SU(2) [circle times operator] U(1) gauge theory with two (or more) Higgs doublets, but with the fermion mass scale determined by the vacuum expectation values of the Higgs particles rather than determined only by widely differing Higgs couplings. Such an alternative to the standard theory cannot be excluded by current data; the Higgs-fermion coupling is allowed to be at least 70 times that of the standard Weinberg-Salam theory. In such a model, one has the possibility of observing large and interesting effects due to the Higgs particles in the theory. These include decays of heavy quarkonium states and Drell-Yan production of l+l-(l = e, [mu], [tau]). Restrictions due to charged Higgs scalar currents (in [pi], [mu] and [beta] decay and in neutrino production) take unexpected forms and are not too stringent. The best place to search for a Higgs is in K+N--&gt;[mu]+[mu]-X (subsect. 3.5).en_US
dc.format.extent2400277 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.titleThe fermion mass scale and possible effects of Higgs bosons on experimental observablesen_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbsecondlevelNuclear Engineering and Radiological Sciencesen_US
dc.subject.hlbtoplevelScienceen_US
dc.subject.hlbtoplevelEngineeringen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumPhysics Department, University of Michigan, Ann Arbor, Michigan 48109, USAen_US
dc.contributor.affiliationumPhysics Department, University of Michigan, Ann Arbor, Michigan 48109, USAen_US
dc.contributor.affiliationumPhysics Department, University of Michigan, Ann Arbor, Michigan 48109, USAen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/23439/1/0000388.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0550-3213(79)90225-6en_US
dc.identifier.sourceNuclear Physics Ben_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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