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General Focus Point in the MSSM
The minimal supersymmetric extension of the Standard Model (SM) is a well motivated scenario for physics beyond the SM, which allows a perturbative description of the theory up to scales of the order of the Grand Unification scale, where gauge couplings unify. The Higgs mass parameter is insensitive...
Autores principales: | , , |
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Lenguaje: | eng |
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2014
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP04(2014)093 http://cds.cern.ch/record/1647285 |
_version_ | 1780935139328524288 |
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author | Delgado, Antonio Quiros, Mariano Wagner, Carlos |
author_facet | Delgado, Antonio Quiros, Mariano Wagner, Carlos |
author_sort | Delgado, Antonio |
collection | CERN |
description | The minimal supersymmetric extension of the Standard Model (SM) is a well motivated scenario for physics beyond the SM, which allows a perturbative description of the theory up to scales of the order of the Grand Unification scale, where gauge couplings unify. The Higgs mass parameter is insensitive to the ultraviolet physics and is only sensitive to the scale of soft supersymmetry breaking parameters. Present collider bounds suggest that the characteristic values of these parameters may be significantly larger than the weak scale. Large values of the soft breaking parameters, however, induce large radiative corrections to the Higgs mass parameter and therefore the proper electroweak scale may only be obtained by a fine tuned cancellation between the square of the holomorphic \mu-parameter and the Higgs supersymmetry breaking square mass parameter. This can only be avoided if there is a correlation between the scalar and gaugino mass parameters, such that the Higgs supersymmetry breaking parameter remains of the order of the weak scale. The scale at which this happens is dubbed as focus point. In this article, we define the general conditions required for this to happen, for different values of the messenger scale at which supersymmetry breaking is transmitted to the observable sector, and for arbitrary boundary conditions of the sfermion, gaugino, and Higgs mass parameters. Specific supersymmetry breaking scenarios in which these correlations may occur are also discussed. |
id | cern-1647285 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2014 |
record_format | invenio |
spelling | cern-16472852023-03-14T18:25:55Zdoi:10.1007/JHEP04(2014)093http://cds.cern.ch/record/1647285engDelgado, AntonioQuiros, MarianoWagner, CarlosGeneral Focus Point in the MSSMParticle Physics - PhenomenologyThe minimal supersymmetric extension of the Standard Model (SM) is a well motivated scenario for physics beyond the SM, which allows a perturbative description of the theory up to scales of the order of the Grand Unification scale, where gauge couplings unify. The Higgs mass parameter is insensitive to the ultraviolet physics and is only sensitive to the scale of soft supersymmetry breaking parameters. Present collider bounds suggest that the characteristic values of these parameters may be significantly larger than the weak scale. Large values of the soft breaking parameters, however, induce large radiative corrections to the Higgs mass parameter and therefore the proper electroweak scale may only be obtained by a fine tuned cancellation between the square of the holomorphic \mu-parameter and the Higgs supersymmetry breaking square mass parameter. This can only be avoided if there is a correlation between the scalar and gaugino mass parameters, such that the Higgs supersymmetry breaking parameter remains of the order of the weak scale. The scale at which this happens is dubbed as focus point. In this article, we define the general conditions required for this to happen, for different values of the messenger scale at which supersymmetry breaking is transmitted to the observable sector, and for arbitrary boundary conditions of the sfermion, gaugino, and Higgs mass parameters. Specific supersymmetry breaking scenarios in which these correlations may occur are also discussed.The minimal supersymmetric extension of the Standard Model (SM) is a well motivated scenario for physics beyond the SM, which allows a perturbative description of the theory up to scales of the order of the Grand Unification scale, where gauge couplings unify. The Higgs mass parameter is insensitive to the ultraviolet physics and is only sensitive to the scale of soft supersymmetry breaking parameters. Present collider bounds suggest that the characteristic values of these parameters may be significantly larger than the weak scale. Large values of the soft breaking parameters, however, induce large radiative corrections to the Higgs mass parameter and therefore the proper electroweak scale may only be obtained by a fine tuned cancellation between the square of the holomorphic \mu-parameter and the Higgs supersymmetry breaking square mass parameter. This can only be avoided if there is a correlation between the scalar and gaugino mass parameters, such that the Higgs supersymmetry breaking parameter remains of the order of the weak scale. The scale at which this happens is dubbed as focus point. In this article, we define the general conditions required for this to happen, for different values of the messenger scale at which supersymmetry breaking is transmitted to the observable sector, and for arbitrary boundary conditions of the sfermion, gaugino, and Higgs mass parameters. Specific supersymmetry breaking scenarios in which these correlations may occur are also discussed.arXiv:1402.1735CERN-PH-TH-2014-022CERN-PH-TH-2014-022oai:cds.cern.ch:16472852014-02-07 |
spellingShingle | Particle Physics - Phenomenology Delgado, Antonio Quiros, Mariano Wagner, Carlos General Focus Point in the MSSM |
title | General Focus Point in the MSSM |
title_full | General Focus Point in the MSSM |
title_fullStr | General Focus Point in the MSSM |
title_full_unstemmed | General Focus Point in the MSSM |
title_short | General Focus Point in the MSSM |
title_sort | general focus point in the mssm |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/JHEP04(2014)093 http://cds.cern.ch/record/1647285 |
work_keys_str_mv | AT delgadoantonio generalfocuspointinthemssm AT quirosmariano generalfocuspointinthemssm AT wagnercarlos generalfocuspointinthemssm |