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Nonanomalous Discrete R-Symmetry and Light Gravitino

We discuss nonanomalous R-symmetry in the supersymmetric grand unified theories. In particular, we explore anomaly-free solutions predicting the gravitino mass in the range of $10^{-3} eV \lsim m_{3/2} \lsim 1 TeV$ when the $\mu$-parameter is fixed to be $\mu \simeq 1 TeV$. In the minimal SU(5) GUT,...

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Detalles Bibliográficos
Autores principales: Hamaguchi, K, Maru, N
Lenguaje:eng
Publicado: 2003
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.67.115003
http://cds.cern.ch/record/606006
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author Hamaguchi, K
Maru, N
author_facet Hamaguchi, K
Maru, N
author_sort Hamaguchi, K
collection CERN
description We discuss nonanomalous R-symmetry in the supersymmetric grand unified theories. In particular, we explore anomaly-free solutions predicting the gravitino mass in the range of $10^{-3} eV \lsim m_{3/2} \lsim 1 TeV$ when the $\mu$-parameter is fixed to be $\mu \simeq 1 TeV$. In the minimal SU(5) GUT, we have shown that $\mu \simeq 1 TeV$ is obtained only if the gravitino is ultralight with mass $m_{3/2} \sim 10^{-3} eV$. If extra fields ${\bf 5}\oplus{\bf 5^*}$ or ${\bf 10}\oplus{\bf 10^*}$ are introduced, many solutions predicting $m_{3/2} \gsim 10^{-3} eV$ are found. The R-parity is violated due to the vacuum expectation value of the superpotential, but it is controlled by the discrete R-symmetry. We find that the R-parity violating couplings are naturally suppressed much below the experimental bounds for some charge assignments. These charge assignments predict light gravitino with masses of order ${\cal O}(10^{-3} eV)$--${\cal O}(1 MeV)$. These discrete R-symmetries can be considered as solutions to the $\mu$-problem in low energy supersymmetry breaking models such as the gauge mediation.
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spelling cern-6060062019-09-30T06:29:59Zdoi:10.1103/PhysRevD.67.115003http://cds.cern.ch/record/606006engHamaguchi, KMaru, NNonanomalous Discrete R-Symmetry and Light GravitinoParticle Physics - PhenomenologyWe discuss nonanomalous R-symmetry in the supersymmetric grand unified theories. In particular, we explore anomaly-free solutions predicting the gravitino mass in the range of $10^{-3} eV \lsim m_{3/2} \lsim 1 TeV$ when the $\mu$-parameter is fixed to be $\mu \simeq 1 TeV$. In the minimal SU(5) GUT, we have shown that $\mu \simeq 1 TeV$ is obtained only if the gravitino is ultralight with mass $m_{3/2} \sim 10^{-3} eV$. If extra fields ${\bf 5}\oplus{\bf 5^*}$ or ${\bf 10}\oplus{\bf 10^*}$ are introduced, many solutions predicting $m_{3/2} \gsim 10^{-3} eV$ are found. The R-parity is violated due to the vacuum expectation value of the superpotential, but it is controlled by the discrete R-symmetry. We find that the R-parity violating couplings are naturally suppressed much below the experimental bounds for some charge assignments. These charge assignments predict light gravitino with masses of order ${\cal O}(10^{-3} eV)$--${\cal O}(1 MeV)$. These discrete R-symmetries can be considered as solutions to the $\mu$-problem in low energy supersymmetry breaking models such as the gauge mediation.hep-ph/0302163DESY-03-018DESY-2003-018UT-2003-06oai:cds.cern.ch:6060062003-02-18
spellingShingle Particle Physics - Phenomenology
Hamaguchi, K
Maru, N
Nonanomalous Discrete R-Symmetry and Light Gravitino
title Nonanomalous Discrete R-Symmetry and Light Gravitino
title_full Nonanomalous Discrete R-Symmetry and Light Gravitino
title_fullStr Nonanomalous Discrete R-Symmetry and Light Gravitino
title_full_unstemmed Nonanomalous Discrete R-Symmetry and Light Gravitino
title_short Nonanomalous Discrete R-Symmetry and Light Gravitino
title_sort nonanomalous discrete r-symmetry and light gravitino
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.67.115003
http://cds.cern.ch/record/606006
work_keys_str_mv AT hamaguchik nonanomalousdiscretersymmetryandlightgravitino
AT marun nonanomalousdiscretersymmetryandlightgravitino