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The electroweak phase transition in minimal supergravity models
We have explored the electroweak phase transition in minimal supergravity models by extending previous analysis of the one-loop Higgs potential to include finite temperature effects. Minimal supergravity is characterized by two higgs doublets at the electroweak scale, gauge coupling unification, and...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
1994
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Acceso en línea: | https://dx.doi.org/10.1016/0370-2693(94)90324-7 http://cds.cern.ch/record/245569 |
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author | Nanopoulos, Dimitri V. Pois, H. |
author_facet | Nanopoulos, Dimitri V. Pois, H. |
author_sort | Nanopoulos, Dimitri V. |
collection | CERN |
description | We have explored the electroweak phase transition in minimal supergravity models by extending previous analysis of the one-loop Higgs potential to include finite temperature effects. Minimal supergravity is characterized by two higgs doublets at the electroweak scale, gauge coupling unification, and universal soft-SUSY breaking at the unification scale. We have searched for the allowed parameter space that avoids washout of baryon number via unsuppressed anomalous Electroweak sphaleron processes after the phase transition. This requirement imposes strong constraints on the Higgs sector. With respect to weak scale baryogenesis, we find that the generic MSSM is {\it not} phenomenologically acceptable, and show that the additional experimental and consistency constraints of minimal supergravity restricts the mass of the lightest CP-even Higgs even further to $m_h\lsim 32\GeV$ (at one loop), also in conflict with experiment. Thus, if supergravity is to allow for baryogenesis via any other mechanism above the weak scale, it {\it must} also provide for B-L production (or some other `accidentally' conserved quantity) above the electroweak scale. Finally, we suggest that the no-scale flipped $SU(5)$ supergravity model can naturally and economically provide a source of B-L violation and realistically account for the observed ratio $n_B/n_\gamma\sim 10^{-10}$. |
id | cern-245569 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1994 |
record_format | invenio |
spelling | cern-2455692023-03-14T19:27:50Zdoi:10.1016/0370-2693(94)90324-7http://cds.cern.ch/record/245569engNanopoulos, Dimitri V.Pois, H.The electroweak phase transition in minimal supergravity modelsParticle Physics - PhenomenologyParticle Physics - TheoryWe have explored the electroweak phase transition in minimal supergravity models by extending previous analysis of the one-loop Higgs potential to include finite temperature effects. Minimal supergravity is characterized by two higgs doublets at the electroweak scale, gauge coupling unification, and universal soft-SUSY breaking at the unification scale. We have searched for the allowed parameter space that avoids washout of baryon number via unsuppressed anomalous Electroweak sphaleron processes after the phase transition. This requirement imposes strong constraints on the Higgs sector. With respect to weak scale baryogenesis, we find that the generic MSSM is {\it not} phenomenologically acceptable, and show that the additional experimental and consistency constraints of minimal supergravity restricts the mass of the lightest CP-even Higgs even further to $m_h\lsim 32\GeV$ (at one loop), also in conflict with experiment. Thus, if supergravity is to allow for baryogenesis via any other mechanism above the weak scale, it {\it must} also provide for B-L production (or some other `accidentally' conserved quantity) above the electroweak scale. Finally, we suggest that the no-scale flipped $SU(5)$ supergravity model can naturally and economically provide a source of B-L violation and realistically account for the observed ratio $n_B/n_\gamma\sim 10^{-10}$.We have explored the electroweak phase transition in minimal supergravity models by extending previous analysis of the one-loop Higgs potential to include finite temperature effects. Minimal supergravity is characterized by two higgs doublets at the electroweak scale, gauge coupling unification, and universal soft-SUSY breaking at the unification scale. We have searched for the allowed parameter space that avoids washout of baryon number via unsuppressed anomalous Electroweak sphaleron processes after the phase transition. This requirement imposes strong constraints on the Higgs sector. With respect to weak scale baryogenesis, we find that the generic MSSM is {\it not} phenomenologically acceptable, and show that the additional experimental and consistency constraints of minimal supergravity restricts the mass of the lightest CP-even Higgs even further to $m_h\lsim 32\GeV$ (at one loop), also in conflict with experiment. Thus, if supergravity is to allow for baryogenesis via any other mechanism above the weak scale, it {\it must} also provide for B-L production (or some other `accidentally' conserved quantity) above the electroweak scale. Finally, we suggest that the no-scale flipped $SU(5)$ supergravity model can naturally and economically provide a source of B-L violation and realistically account for the observed ratio $n_B/n_\gamma\sim 10~{-10}$.We have explored the electroweak phase transition in minimal supergravity models by extending previous analysis of the one-loop Higgs potential to include finite temperature effects. Minimal supergravity is characterized by two higgs doublets at the electroweak scale, gauge coupling unification, and universal soft-SUSY breaking at the unification scale. We have searched for the allowed parameter space that avoids washout of baryon number via unsuppressed anomalous Electroweak sphaleron processes after the phase transition. This requirement imposes strong constraints on the Higgs sector. With respect to weak scale baryogenesis, we find that the generic MSSM is {\it not} phenomenologically acceptable, and show that the additional experimental and consistency constraints of minimal supergravity restricts the mass of the lightest CP-even Higgs even further to $m_h\lsim 32\GeV$ (at one loop), also in conflict with experiment. Thus, if supergravity is to allow for baryogenesis via any other mechanism above the weak scale, it {\it must} also provide for B-L production (or some other `accidentally' conserved quantity) above the electroweak scale. Finally, we suggest that the no-scale flipped $SU(5)$ supergravity model can naturally and economically provide a source of B-L violation and realistically account for the observed ratio $n_B/n_\gamma\sim 10~{-10}$.We explore the electroweak phase transition in minimal supergravity models by extending our previous analysis of the one-loop Higgs potential to include finite temperature effects. Minimal supergravity is characterized by two Higgs doublets at the electroweak scale, gauge coupling unification, and universal soft-SUSY breaking at the unification scale. We have searched for the allowed parameter space where the phase transition is sufficiently first order to avoid washout of baryon number after the phase transition via unsuppressed anomalous electroweak sphaleron processes. This requirement imposes strong constraints on the Higgs sector; we find m h ≲ 60 GeV (at one loop) and tan ß ≲ 2. We argue that present Higgs searches rule out this remaining parameter space. Thus, if supergravity (with two light Higgs doublets) is to allow for baryogenesis, it must also provide for B − L production at or above the weak scale. Our results therefore indicate that the field/coupling content of minimal supergravity is insufficient to account for the baryon asymmetry of the universe (BAU). We suggest that the no-scale flipped SU (5) supergravity model naturally and economically provides a source of B − L violation and can account for the observed ratio n B n γ ∼10 −10 .hep-ph/9302205CERN-TH-6763-92CTP-TAMU-87-92ACT-16-92AACT-1992-16CERN-TH-6763-92CTP-TAMU-87-92oai:cds.cern.ch:2455691994 |
spellingShingle | Particle Physics - Phenomenology Particle Physics - Theory Nanopoulos, Dimitri V. Pois, H. The electroweak phase transition in minimal supergravity models |
title | The electroweak phase transition in minimal supergravity models |
title_full | The electroweak phase transition in minimal supergravity models |
title_fullStr | The electroweak phase transition in minimal supergravity models |
title_full_unstemmed | The electroweak phase transition in minimal supergravity models |
title_short | The electroweak phase transition in minimal supergravity models |
title_sort | electroweak phase transition in minimal supergravity models |
topic | Particle Physics - Phenomenology Particle Physics - Theory |
url | https://dx.doi.org/10.1016/0370-2693(94)90324-7 http://cds.cern.ch/record/245569 |
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