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The $\mu$-problem in theories with gauge-mediated supersymmetry breaking

We point out that the \mu-problem in theories in which supersymmetry breaking is communicated to the observable sector by gauge interactions is more severe than the one encountered in the conventional gravity-mediated scenarios. The difficulty is that once \mu is generated by a one-loop diagram, the...

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Detalles Bibliográficos
Autores principales: Dvali, G.R., Giudice, G.F., Pomarol, A.
Lenguaje:eng
Publicado: 1996
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0550-3213(96)00404-X
http://cds.cern.ch/record/299468
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author Dvali, G.R.
Giudice, G.F.
Pomarol, A.
author_facet Dvali, G.R.
Giudice, G.F.
Pomarol, A.
author_sort Dvali, G.R.
collection CERN
description We point out that the \mu-problem in theories in which supersymmetry breaking is communicated to the observable sector by gauge interactions is more severe than the one encountered in the conventional gravity-mediated scenarios. The difficulty is that once \mu is generated by a one-loop diagram, then usually \bmu is also generated at the same loop order. This leads to the problematic relation \bmu \sim \mu \Lambda, where \Lambda \sim 10--100 TeV is the effective supersymmetry-breaking scale. We present a class of theories for which this problem is naturally solved. Here, without any fine tuning among parameters, \mu is generated at one loop, while \bmu arises only at the two-loop level. This mechanism can naturally lead to an interpretation of the Higgs doublets as pseudo-Goldstone bosons of an approximate global symmetry.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1996
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spelling cern-2994682023-03-14T17:17:59Zdoi:10.1016/0550-3213(96)00404-Xhttp://cds.cern.ch/record/299468engDvali, G.R.Giudice, G.F.Pomarol, A.The $\mu$-problem in theories with gauge-mediated supersymmetry breakingParticle Physics - PhenomenologyWe point out that the \mu-problem in theories in which supersymmetry breaking is communicated to the observable sector by gauge interactions is more severe than the one encountered in the conventional gravity-mediated scenarios. The difficulty is that once \mu is generated by a one-loop diagram, then usually \bmu is also generated at the same loop order. This leads to the problematic relation \bmu \sim \mu \Lambda, where \Lambda \sim 10--100 TeV is the effective supersymmetry-breaking scale. We present a class of theories for which this problem is naturally solved. Here, without any fine tuning among parameters, \mu is generated at one loop, while \bmu arises only at the two-loop level. This mechanism can naturally lead to an interpretation of the Higgs doublets as pseudo-Goldstone bosons of an approximate global symmetry.We point out that the $\mu$-problem in theories in which supersymmetry breaking is communicated to the observable sector by gauge interactions is more severe than the one encountered in the conventional gravity-mediated scenarios. The difficulty is that once $\mu$ is generated by a one-loop diagram, then usually $\bmu$ is also generated at the same loop order. This leads to the problematic relation $\bmu \sim \mu \Lambda$, where $\Lambda \sim$ 10--100 TeV is the effective supersymmetry-breaking scale. We present a class of theories for which this problem is naturally solved. Here, without any fine tuning among parameters, $\mu$ is generated at one loop, while $\bmu$ arises only at the two-loop level. This mechanism can naturally lead to an interpretation of the Higgs doublets as pseudo-Goldstone bosons of an approximate global symmetry.We point out that the μ-problem in theories in which supersymmetry breaking is communicated to the observable sector by gauge interactions is more severe than the one encountered in the conventional gravity-mediated scenarios. The difficulty is that once μ is generated by a one-loop diagram, then usually B μ is also generated at the same loop order. This leads to the problematic relation B μ t μ where t 10–100 TeV is the effective supersymmetry-breaking scale. We 0 present a class of theories for which this problem is naturally solved. Here, without any fine tuning among parameters, μ is generated at one loop, while B μ arises only at the two-loop level. This mechanism can naturally lead to an interpretation of the Higgs doublets as pseudo-Goldstone bosons of an approximate global symmetry.hep-ph/9603238CERN-TH-96-61CERN-TH-96-061oai:cds.cern.ch:2994681996-03-06
spellingShingle Particle Physics - Phenomenology
Dvali, G.R.
Giudice, G.F.
Pomarol, A.
The $\mu$-problem in theories with gauge-mediated supersymmetry breaking
title The $\mu$-problem in theories with gauge-mediated supersymmetry breaking
title_full The $\mu$-problem in theories with gauge-mediated supersymmetry breaking
title_fullStr The $\mu$-problem in theories with gauge-mediated supersymmetry breaking
title_full_unstemmed The $\mu$-problem in theories with gauge-mediated supersymmetry breaking
title_short The $\mu$-problem in theories with gauge-mediated supersymmetry breaking
title_sort $\mu$-problem in theories with gauge-mediated supersymmetry breaking
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0550-3213(96)00404-X
http://cds.cern.ch/record/299468
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