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The MSSM Parameter Space with Non-Universal Higgs Masses

Without assuming that Higgs masses have the same values as other scalar masses at the input GUT scale, we combine constraints on the minimal supersymmetric extension of the Standard Model (MSSM) coming from the cold dark matter density with the limits from direct searches at accelerators such as LEP...

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Detalles Bibliográficos
Autores principales: Ellis, John R., Olive, Keith A., Santoso, Yudi
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(02)02071-3
http://cds.cern.ch/record/547374
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author Ellis, John R.
Olive, Keith A.
Santoso, Yudi
author_facet Ellis, John R.
Olive, Keith A.
Santoso, Yudi
author_sort Ellis, John R.
collection CERN
description Without assuming that Higgs masses have the same values as other scalar masses at the input GUT scale, we combine constraints on the minimal supersymmetric extension of the Standard Model (MSSM) coming from the cold dark matter density with the limits from direct searches at accelerators such as LEP, indirect measurements such as b to s gamma decay and the anomalous magnetic moment of the muon. The requirement that Higgs masses-squared be positive at the GUT scale imposes important restrictions on the MSSM parameter space, as does the requirement that the LSP be neutral. We analyze the interplay of these constraints in the (mu, m_A), (mu, m_{1/2}), (m_{1/2}, m_0) and (m_A, tan beta) planes. These exhibit new features not seen in the corresponding planes in the constrained MSSM in which universality is extended to Higgs masses.
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spelling cern-5473742023-03-14T18:03:02Zdoi:10.1016/S0370-2693(02)02071-3http://cds.cern.ch/record/547374engEllis, John R.Olive, Keith A.Santoso, YudiThe MSSM Parameter Space with Non-Universal Higgs MassesParticle Physics - PhenomenologyWithout assuming that Higgs masses have the same values as other scalar masses at the input GUT scale, we combine constraints on the minimal supersymmetric extension of the Standard Model (MSSM) coming from the cold dark matter density with the limits from direct searches at accelerators such as LEP, indirect measurements such as b to s gamma decay and the anomalous magnetic moment of the muon. The requirement that Higgs masses-squared be positive at the GUT scale imposes important restrictions on the MSSM parameter space, as does the requirement that the LSP be neutral. We analyze the interplay of these constraints in the (mu, m_A), (mu, m_{1/2}), (m_{1/2}, m_0) and (m_A, tan beta) planes. These exhibit new features not seen in the corresponding planes in the constrained MSSM in which universality is extended to Higgs masses.Without assuming that Higgs masses have the same values as other scalar masses at the input GUT scale, we combine constraints on the minimal supersymmetric extension of the Standard Model (MSSM) coming from the cold dark matter density with the limits from direct searches at accelerators such as LEP, indirect measurements such as b → sγ decay and the anomalous magnetic moment of the muon. The requirement that Higgs masses-squared be positive at the GUT scale imposes important restrictions on the MSSM parameter space, as does the requirement that the LSP be neutral. We analyze the interplay of these constraints in the ( μ , m A ), ( μ , m 1/2 ), ( m 1/2 , m 0 ) and ( m A ,tan β ) planes. These exhibit new features not seen in the corresponding planes in the constrained MSSM in which universality is extended to Higgs masses.Without assuming that Higgs masses have the same values as other scalar masses at the input GUT scale, we combine constraints on the minimal supersymmetric extension of the Standard Model (MSSM) coming from the cold dark matter density with the limits from direct searches at accelerators such as LEP, indirect measurements such as b to s gamma decay and the anomalous magnetic moment of the muon. The requirement that Higgs masses-squared be positive at the GUT scale imposes important restrictions on the MSSM parameter space, as does the requirement that the LSP be neutral. We analyze the interplay of these constraints in the (mu, m_A), (mu, m_{1/2}), (m_{1/2}, m_0) and (m_A, tan beta) planes. These exhibit new features not seen in the corresponding planes in the constrained MSSM in which universality is extended to Higgs masses.hep-ph/0204192CERN-TH-2002-081UMN-TH-2049-02TPI-MINN-02-09CERN-TH-2002-081UMN-TH-2049TPI-MINN-2002-09oai:cds.cern.ch:5473742002-04-16
spellingShingle Particle Physics - Phenomenology
Ellis, John R.
Olive, Keith A.
Santoso, Yudi
The MSSM Parameter Space with Non-Universal Higgs Masses
title The MSSM Parameter Space with Non-Universal Higgs Masses
title_full The MSSM Parameter Space with Non-Universal Higgs Masses
title_fullStr The MSSM Parameter Space with Non-Universal Higgs Masses
title_full_unstemmed The MSSM Parameter Space with Non-Universal Higgs Masses
title_short The MSSM Parameter Space with Non-Universal Higgs Masses
title_sort mssm parameter space with non-universal higgs masses
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0370-2693(02)02071-3
http://cds.cern.ch/record/547374
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