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A natural solution to the $\mu$ problem

We propose a simple mechanism for solving the $\mu$ problem in the context of minimal low--energy supergravity models. This is based on the appearance of non--renormalizable couplings in the superpotential. In particular, if $H_1H_2$ is an allowed operator by all the symmetries of the theory, it is...

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Detalles Bibliográficos
Autores principales: Casas, J.A., Munoz, C.
Lenguaje:eng
Publicado: 1993
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(93)90081-R
http://cds.cern.ch/record/245793
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author Casas, J.A.
Munoz, C.
author_facet Casas, J.A.
Munoz, C.
author_sort Casas, J.A.
collection CERN
description We propose a simple mechanism for solving the $\mu$ problem in the context of minimal low--energy supergravity models. This is based on the appearance of non--renormalizable couplings in the superpotential. In particular, if $H_1H_2$ is an allowed operator by all the symmetries of the theory, it is natural to promote the usual renormalizable superpotential $W_o$ to $W_o+\lambda W_o H_1H_2$, yielding an effective $\mu$ parameter whose size is directly related to the gravitino mass once supersymmetry is broken (this result is maintained if $H_1H_2$ couples with different strengths to the various terms present in $W_o$). On the other hand, the $\mu$ term must be absent from $W_o$, otherwise the natural scale for $\mu$ would be $M_P$. Remarkably enough, this is entirely justified in the supergravity theories coming from superstrings, where mass terms for light fields are forbidden in the superpotential. We also analyse the $SU(2)\times U(1)$ breaking, finding that it takes place satisfactorily. Finally, we give a realistic example in which supersymmetry is broken by gaugino condensation, where the mechanism proposed for solving the $\mu$ problem can be gracefully implemented.
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spelling cern-2457932023-03-14T18:53:09Zdoi:10.1016/0370-2693(93)90081-Rhttp://cds.cern.ch/record/245793engCasas, J.A.Munoz, C.A natural solution to the $\mu$ problemGeneral Theoretical PhysicsParticle Physics - PhenomenologyWe propose a simple mechanism for solving the $\mu$ problem in the context of minimal low--energy supergravity models. This is based on the appearance of non--renormalizable couplings in the superpotential. In particular, if $H_1H_2$ is an allowed operator by all the symmetries of the theory, it is natural to promote the usual renormalizable superpotential $W_o$ to $W_o+\lambda W_o H_1H_2$, yielding an effective $\mu$ parameter whose size is directly related to the gravitino mass once supersymmetry is broken (this result is maintained if $H_1H_2$ couples with different strengths to the various terms present in $W_o$). On the other hand, the $\mu$ term must be absent from $W_o$, otherwise the natural scale for $\mu$ would be $M_P$. Remarkably enough, this is entirely justified in the supergravity theories coming from superstrings, where mass terms for light fields are forbidden in the superpotential. We also analyse the $SU(2)\times U(1)$ breaking, finding that it takes place satisfactorily. Finally, we give a realistic example in which supersymmetry is broken by gaugino condensation, where the mechanism proposed for solving the $\mu$ problem can be gracefully implemented.We propose a simple mechanism for solving the μ-problem in the context of minimal low-energy supergravity models. This is based on the appearance of non-renormalizable couplings in the superpotential. In particular, if H 1 H 2 is an allowed operator by all the symmetries of the theory, it is natural to promote the usual renormalizable superpotential W 0 to W 0 + λW 0 H 1 H 2 , yielding an effective μ parameter whose size is directly related to the gravitino mass once supersymmetry is broken (this result is maintained if H 1 H 2 couples with different strengths to the various terms present in W 0 ). On the other hand, the μ-term must be absent in W 0 , otherwise the natural scale for μ would be M > Pl . Remarkably enough, this is entirely justified in the SUGRA theories coming from superstrings, where mass terms for light fields are forbidden in the superpotential. We also analyze the SU(2)×U(1) breaking, finding that it takes place satisfactorily. Finally, we give a realistic example in which SUSY is broken by gaugino condensation where the mechanism proposed for solving the μ-problem can be gracefully implemented.We propose a simple mechanism for solving the $\mu$ problem in the context of minimal low--energy supergravity models. This is based on the appearance of non--renormalizable couplings in the superpotential. In particular, if $H_1H_2$ is an allowed operator by all the symmetries of the theory, it is natural to promote the usual renormalizable superpotential $W_o$ to $W_o+\lambda W_o H_1H_2$, yielding an effective $\mu$ parameter whose size is directly related to the gravitino mass once supersymmetry is broken (this result is maintained if $H_1H_2$ couples with different strengths to the various terms present in $W_o$). On the other hand, the $\mu$ term must be absent from $W_o$, otherwise the natural scale for $\mu$ would be $M_P$. Remarkably enough, this is entirely justified in the supergravity theories coming from superstrings, where mass terms for light fields are forbidden in the superpotential. We also analyse the $SU(2)\times U(1)$ breaking, finding that it takes place satisfactorily. Finally, we give a realistic example in which supersymmetry is broken by gaugino condensation, where the mechanism proposed for solving the $\mu$ problem can be gracefully implemented.hep-ph/9302227FTUAM-92-45CERN-TH-6764-92IEM-FT-66-92CERN-TH-6764-92FTUAM-92-45IEM-FT-66oai:cds.cern.ch:2457931993
spellingShingle General Theoretical Physics
Particle Physics - Phenomenology
Casas, J.A.
Munoz, C.
A natural solution to the $\mu$ problem
title A natural solution to the $\mu$ problem
title_full A natural solution to the $\mu$ problem
title_fullStr A natural solution to the $\mu$ problem
title_full_unstemmed A natural solution to the $\mu$ problem
title_short A natural solution to the $\mu$ problem
title_sort natural solution to the $\mu$ problem
topic General Theoretical Physics
Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0370-2693(93)90081-R
http://cds.cern.ch/record/245793
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