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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...
Autores principales: | , |
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Lenguaje: | eng |
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1995
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Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(95)00570-B http://cds.cern.ch/record/277639 |
_version_ | 1780887664591896576 |
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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. |
id | cern-277639 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1995 |
record_format | invenio |
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 |