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Charged-Lepton-Flavour Violation in the CMSSM in View of the Muon Anomalous Magnetic Moment

We use the BNL E821 measurement of g - 2, the anomalous magnetic moment of the muon, to normalize, within a supersymmetric GUT framework, constrained MSSM (CMSSM) predictions for processes that violate charged-lepton flavour conservation, including mu to e gamma, mu to e conversion and K^0_L to mu e...

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Detalles Bibliográficos
Autores principales: Carvalho, D.F., Ellis, John R., Gomez, M.E., Lola, S.
Lenguaje:eng
Publicado: 2001
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(01)00835-8
http://cds.cern.ch/record/492552
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author Carvalho, D.F.
Ellis, John R.
Gomez, M.E.
Lola, S.
author_facet Carvalho, D.F.
Ellis, John R.
Gomez, M.E.
Lola, S.
author_sort Carvalho, D.F.
collection CERN
description We use the BNL E821 measurement of g - 2, the anomalous magnetic moment of the muon, to normalize, within a supersymmetric GUT framework, constrained MSSM (CMSSM) predictions for processes that violate charged-lepton flavour conservation, including mu to e gamma, mu to e conversion and K^0_L to mu e. We illustrate our analysis with two examples of lepton mass matrix textures motivated by data on neutrino oscillations. We find that mu to e gamma may well occur at a rate within one or two (two or three) orders of magnitude of the present experimental upper limit if g - 2 is within the one- (two-)standard deviation range indicated by E821. We also find that mu to e conversion is likely to occur at rate measurable by MECO, and there is a chance that K^0_L to mu e may be observable in an experiment using an intense proton source.
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spelling cern-4925522023-03-14T18:09:49Zdoi:10.1016/S0370-2693(01)00835-8http://cds.cern.ch/record/492552engCarvalho, D.F.Ellis, John R.Gomez, M.E.Lola, S.Charged-Lepton-Flavour Violation in the CMSSM in View of the Muon Anomalous Magnetic MomentParticle Physics - PhenomenologyWe use the BNL E821 measurement of g - 2, the anomalous magnetic moment of the muon, to normalize, within a supersymmetric GUT framework, constrained MSSM (CMSSM) predictions for processes that violate charged-lepton flavour conservation, including mu to e gamma, mu to e conversion and K^0_L to mu e. We illustrate our analysis with two examples of lepton mass matrix textures motivated by data on neutrino oscillations. We find that mu to e gamma may well occur at a rate within one or two (two or three) orders of magnitude of the present experimental upper limit if g - 2 is within the one- (two-)standard deviation range indicated by E821. We also find that mu to e conversion is likely to occur at rate measurable by MECO, and there is a chance that K^0_L to mu e may be observable in an experiment using an intense proton source.We use the BNL E821 measurement of g - 2, the anomalous magnetic moment of the muon, to normalize, within a supersymmetric GUT framework, constrained MSSM (CMSSM) predictions for processes that violate charged-lepton flavour conservation, including mu to e gamma, mu to e conversion and K^0_L to mu e. We illustrate our analysis with two examples of lepton mass matrix textures motivated by data on neutrino oscillations. We find that mu to e gamma may well occur at a rate within one or two (two or three) orders of magnitude of the present experimental upper limit if g - 2 is within the one- (two-)standard deviation range indicated by E821. We also find that mu to e conversion is likely to occur at rate measurable by MECO, and there is a chance that K^0_L to mu e may be observable in an experiment using an intense proton source.We use the BNL E821 measurement of g μ −2, the anomalous magnetic moment of the muon, to normalize, within a supersymmetric GUT framework, constrained MSSM (CMSSM) predictions for processes that violate charged-lepton flavour conservation, including μ → eγ , μ → e conversion and K 0 L → μ ± e ∓ . We illustrate our analysis with two examples of lepton mass matrix textures motivated by data on neutrino oscillations. We find that μ → eγ may well occur at a rate within one or two (two or three) orders of magnitude of the present experimental upper limit if g μ −2 is within the one- (two-)standard deviation range indicated by E821. We also find that μ → e conversion is likely to occur at rate measurable by MECO, and there is a chance that K 0 L → μ ± e ∓ may be observable in an experiment using an intense proton source.hep-ph/0103256CERN-TH-2001-085FISIST-06-2001-CFIFCERN-TH-2001-085FISIST-2001-06-CFIFoai:cds.cern.ch:4925522001-03-23
spellingShingle Particle Physics - Phenomenology
Carvalho, D.F.
Ellis, John R.
Gomez, M.E.
Lola, S.
Charged-Lepton-Flavour Violation in the CMSSM in View of the Muon Anomalous Magnetic Moment
title Charged-Lepton-Flavour Violation in the CMSSM in View of the Muon Anomalous Magnetic Moment
title_full Charged-Lepton-Flavour Violation in the CMSSM in View of the Muon Anomalous Magnetic Moment
title_fullStr Charged-Lepton-Flavour Violation in the CMSSM in View of the Muon Anomalous Magnetic Moment
title_full_unstemmed Charged-Lepton-Flavour Violation in the CMSSM in View of the Muon Anomalous Magnetic Moment
title_short Charged-Lepton-Flavour Violation in the CMSSM in View of the Muon Anomalous Magnetic Moment
title_sort charged-lepton-flavour violation in the cmssm in view of the muon anomalous magnetic moment
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0370-2693(01)00835-8
http://cds.cern.ch/record/492552
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