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[mu]-e conversion in nuclei and Z' physics

dc.contributor.authorBernabeu, J.en_US
dc.contributor.authorNardi, Enricoen_US
dc.contributor.authorTommasini, Danieleen_US
dc.date.accessioned2006-04-10T15:30:24Z
dc.date.available2006-04-10T15:30:24Z
dc.date.issued1993-11-22en_US
dc.identifier.citationBernabeu, J., Nardi, E., Tommasini, D. (1993/11/22)."[mu]-e conversion in nuclei and Z' physics." Nuclear Physics B 409(1): 69-86. <http://hdl.handle.net/2027.42/30445>en_US
dc.identifier.urihttp://www.sciencedirect.com/science/article/B6TVC-4719VT3-2P1/2/9966d03cfd3e8dade1d48b51f63ba2cben_US
dc.identifier.urihttps://hdl.handle.net/2027.42/30445
dc.description.abstractTogether with the existence of new neutral gauge bosons, models based on extended gauge groups (rank &gt; 4) often predict also new charged fermions. A mixing of the known fermions with new states with exotic weak-isospin assignments (left-handed singlets and right-handed doublets) will induce tree level flavour changing neutral interactions mediated by Z exchange, while if the mixing is only with new states with ordinary weak-isospin assignments, the flavour changing neutral currents are mainly due to the exchange of the lightest new neutral gauge boson Z'. We show that the present experimental limits on [mu]-e conversion in nuclei give a nuclear-model-independent bound on the Z-e-[mu] vertex which is twice as strong as that obtained from [mu] --&gt; eee. In the case of E6 models these limits provide quite stringent constraints on the Z' mass and on the Z---Z' mixing angle. We point out that the proposed experiments to search for [mu]-e conversion in nuclei have good chances to find evidence of lepton flavour violation, either in the case that new exotic fermions are present at the electroweak scale, or if a new neutral gauge boson Z' of E6 origin lighter than a few TeV exists.en_US
dc.format.extent1148719 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherElsevieren_US
dc.title[mu]-e conversion in nuclei and Z' physicsen_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.affiliationumRandall Laboratory of Physics, University of Michigan, Ann Arbor, MI 48109-1120, USAen_US
dc.contributor.affiliationotherInstituto de Física Corpuscular - CSIC and Departament de Física Teòrica, Universitat de València, E-46100 Burjassot, València, Spainen_US
dc.contributor.affiliationotherInstituto de Física Corpuscular - CSIC and Departament de Física Teòrica, Universitat de València, E-46100 Burjassot, València, Spainen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/30445/1/0000068.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1016/0550-3213(93)90446-Ven_US
dc.identifier.sourceNuclear Physics Ben_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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