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Maximal sfermion flavour violation in super-GUTs

We consider supersymmetric grand unified theories with soft supersymmetry-breaking scalar masses $m_0$ specified above the GUT scale (super-GUTs) and patterns of Yukawa couplings motivated by upper limits on flavour-changing interactions beyond the Standard Model. If the scalar masses are smaller th...

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Detalles Bibliográficos
Autores principales: Ellis, John, Olive, Keith, Velasco-Sevilla, Liliana
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1140/epjc/s10052-016-4398-9
http://cds.cern.ch/record/2150939
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author Ellis, John
Olive, Keith
Velasco-Sevilla, Liliana
author_facet Ellis, John
Olive, Keith
Velasco-Sevilla, Liliana
author_sort Ellis, John
collection CERN
description We consider supersymmetric grand unified theories with soft supersymmetry-breaking scalar masses $m_0$ specified above the GUT scale (super-GUTs) and patterns of Yukawa couplings motivated by upper limits on flavour-changing interactions beyond the Standard Model. If the scalar masses are smaller than the gaugino masses $m_{1/2}$, as is expected in no-scale models, the dominant effects of renormalization between the input scale and the GUT scale are generally expected to be those due to the gauge couplings, which are proportional to $m_{1/2}$ and generation-independent. In this case, the input scalar masses $m_0$ may violate flavour maximally, a scenario we call MaxFV, and there is no supersymmetric flavour problem. We illustrate this possibility within various specific super-GUT scenarios that are deformations of no-scale gravity.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
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spelling cern-21509392022-08-10T12:46:48Zdoi:10.1140/epjc/s10052-016-4398-9http://cds.cern.ch/record/2150939engEllis, JohnOlive, KeithVelasco-Sevilla, LilianaMaximal sfermion flavour violation in super-GUTsParticle Physics - PhenomenologyWe consider supersymmetric grand unified theories with soft supersymmetry-breaking scalar masses $m_0$ specified above the GUT scale (super-GUTs) and patterns of Yukawa couplings motivated by upper limits on flavour-changing interactions beyond the Standard Model. If the scalar masses are smaller than the gaugino masses $m_{1/2}$, as is expected in no-scale models, the dominant effects of renormalization between the input scale and the GUT scale are generally expected to be those due to the gauge couplings, which are proportional to $m_{1/2}$ and generation-independent. In this case, the input scalar masses $m_0$ may violate flavour maximally, a scenario we call MaxFV, and there is no supersymmetric flavour problem. We illustrate this possibility within various specific super-GUT scenarios that are deformations of no-scale gravity.We consider supersymmetric grand unified theories with soft supersymmetry-breaking scalar masses $m_0$ specified above the GUT scale (super-GUTs) and patterns of Yukawa couplings motivated by upper limits on flavour-changing interactions beyond the Standard Model. If the scalar masses are smaller than the gaugino masses $m_{1/2}$ , as is expected in no-scale models, the dominant effects of renormalisation between the input scale and the GUT scale are generally expected to be those due to the gauge couplings, which are proportional to $m_{1/2}$ and generation independent. In this case, the input scalar masses $m_0$ may violate flavour maximally, a scenario we call MaxSFV, and there is no supersymmetric flavour problem. We illustrate this possibility within various specific super-GUT scenarios that are deformations of no-scale gravity.We consider supersymmetric grand unified theories with soft supersymmetry-breaking scalar masses $m_0$ specified above the GUT scale (super-GUTs) and patterns of Yukawa couplings motivated by upper limits on flavour-changing interactions beyond the Standard Model. If the scalar masses are smaller than the gaugino masses $m_{1/2}$, as is expected in no-scale models, the dominant effects of renormalization between the input scale and the GUT scale are generally expected to be those due to the gauge couplings, which are proportional to $m_{1/2}$ and generation-independent. In this case, the input scalar masses $m_0$ may violate flavour maximally, a scenario we call MaxSFV, and there is no supersymmetric flavour problem. We illustrate this possibility within various specific super-GUT scenarios that are deformations of no-scale gravity.arXiv:1605.01398KCL-PH-TH-2016-20LCTS-2016-13CERN-PH-TH-2016-095FTPI-MINN-16-16UMN-TH-3526-16KCL-PH-TH-2016-20LCTS-2016-13CERN-PH-TH-2016-095UMN-TH-3526-16FTPI-MINN-16-16oai:cds.cern.ch:21509392016-05-04
spellingShingle Particle Physics - Phenomenology
Ellis, John
Olive, Keith
Velasco-Sevilla, Liliana
Maximal sfermion flavour violation in super-GUTs
title Maximal sfermion flavour violation in super-GUTs
title_full Maximal sfermion flavour violation in super-GUTs
title_fullStr Maximal sfermion flavour violation in super-GUTs
title_full_unstemmed Maximal sfermion flavour violation in super-GUTs
title_short Maximal sfermion flavour violation in super-GUTs
title_sort maximal sfermion flavour violation in super-guts
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1140/epjc/s10052-016-4398-9
http://cds.cern.ch/record/2150939
work_keys_str_mv AT ellisjohn maximalsfermionflavourviolationinsuperguts
AT olivekeith maximalsfermionflavourviolationinsuperguts
AT velascosevillaliliana maximalsfermionflavourviolationinsuperguts