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Non-unified sparticle and particle masses in unified theories

We give examples of minimal extensions of the simplest SU(5) SUSY-GUT in which all squarks and sleptons of a family have different tree level masses at the unification scale. This phenomenon is general; it occurs when the quarks and leptons are the light remnants of a theory which contains extra hea...

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Detalles Bibliográficos
Autores principales: Dimopoulos, Savas, Pomarol, Alex
Lenguaje:eng
Publicado: 1995
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(95)00570-B
http://cds.cern.ch/record/277639
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author Dimopoulos, Savas
Pomarol, Alex
author_facet Dimopoulos, Savas
Pomarol, Alex
author_sort Dimopoulos, Savas
collection CERN
description We give examples of minimal extensions of the simplest SU(5) SUSY-GUT in which all squarks and sleptons of a family have different tree level masses at the unification scale. This phenomenon is general; it occurs when the quarks and leptons are the light remnants of a theory which contains extra heavy families at the unification scale. The examples have interesting relations between Yukawa couplings: In one model the ratio of the top to bottom Yukawas is as large as \simeq 3, partly accounting for the large m_t /m_b. Another gives m_b/m_\tau between 2/3 and 1; this relaxes the strict bounds on the top mass and neutrino properties that come from b--\tau unification. Still another allows m_s/m_\mu to be between 1/6 and 1 and evades the potentially problematic GUT relation of m_s=m_\mu. The final example has horizontal sparticle splittings in spite of the existence of horizontal symmetries.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-2776392020-07-23T02:50:07Zdoi:10.1016/0370-2693(95)00570-Bhttp://cds.cern.ch/record/277639engDimopoulos, SavasPomarol, AlexNon-unified sparticle and particle masses in unified theoriesParticle Physics - PhenomenologyWe give examples of minimal extensions of the simplest SU(5) SUSY-GUT in which all squarks and sleptons of a family have different tree level masses at the unification scale. This phenomenon is general; it occurs when the quarks and leptons are the light remnants of a theory which contains extra heavy families at the unification scale. The examples have interesting relations between Yukawa couplings: In one model the ratio of the top to bottom Yukawas is as large as \simeq 3, partly accounting for the large m_t /m_b. Another gives m_b/m_\tau between 2/3 and 1; this relaxes the strict bounds on the top mass and neutrino properties that come from b--\tau unification. Still another allows m_s/m_\mu to be between 1/6 and 1 and evades the potentially problematic GUT relation of m_s=m_\mu. The final example has horizontal sparticle splittings in spite of the existence of horizontal symmetries.We give examples of minimal extensions of the simplest SU(5) SUSY-GUT in which all squarks and sleptons of a family have different tree level masses at the unification scale. This phenomenon is general; it occurs when the quarks and leptons are the light remnants of a theory which contains extra heavy families at the unification scale. The examples have interesting relations between Yukawa couplings: In one model the ratio of the top to bottom Yukawas is as large as $\simeq 3$, partly accounting for the large $m_t /m_b$. Another gives $m_b/m_\tau$ between 2/3 and 1; this relaxes the strict bounds on the top mass and neutrino properties that come from $b$--$\tau$ unification. Still another allows $ m_s/m_\mu$ to be between 1/6 and 1 and evades the potentially problematic GUT relation of $m_s=m_\mu$. The final example has horizontal sparticle splittings in spite of the existence of horizontal symmetries.We give examples of minimal extensions of the simplest SU(5) SUSY-GUT in which all squarks and sleptons of a family have different tree level masses at the unification scale. This phenomenon is general; it occurs when the quarks and leptons are the light remnants of a theory which contains extra heavy families at the unification scale. The examples have interesting relations between Yukawa couplings: In one model the ratio of the top to bottom Yukawas is as large as ∼- 3, partly accounting for the large m t m b . Another gives m b m τ between 2 3 and 1; this relaxes the strict bounds on the top mass and neutrino properties that come from b − τ unification. Still another allows m s m μ to be between 1 6 and 1 and evades the potentially problematic GUT relation of m s = m μ . The final example has horizontal sparticle splittings in spite of the existence of horizontal symmetries.CERN-TH-95-44CERN-TH-95-044hep-ph/9502397CERN-TH-95-44oai:cds.cern.ch:2776391995-02-27
spellingShingle Particle Physics - Phenomenology
Dimopoulos, Savas
Pomarol, Alex
Non-unified sparticle and particle masses in unified theories
title Non-unified sparticle and particle masses in unified theories
title_full Non-unified sparticle and particle masses in unified theories
title_fullStr Non-unified sparticle and particle masses in unified theories
title_full_unstemmed Non-unified sparticle and particle masses in unified theories
title_short Non-unified sparticle and particle masses in unified theories
title_sort non-unified sparticle and particle masses in unified theories
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0370-2693(95)00570-B
http://cds.cern.ch/record/277639
work_keys_str_mv AT dimopoulossavas nonunifiedsparticleandparticlemassesinunifiedtheories
AT pomarolalex nonunifiedsparticleandparticlemassesinunifiedtheories