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Electroweak baryogenesis and low energy supersymmetry

Electroweak baryogenesis is an interesting theoretical scenario, which demands physics beyond the Standard Model at energy scales of the order of the weak boson masses. It has been recently emphasized that, in the presence of light stops, the electroweak phase transition can be strongly first order,...

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Detalles Bibliográficos
Autores principales: Carena, Marcela, Quiros, M., Riotto, A., Vilja, I., Wagner, C.E.M.
Lenguaje:eng
Publicado: 1997
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(97)00412-4
http://cds.cern.ch/record/321167
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author Carena, Marcela
Quiros, M.
Riotto, A.
Vilja, I.
Wagner, C.E.M.
author_facet Carena, Marcela
Quiros, M.
Riotto, A.
Vilja, I.
Wagner, C.E.M.
author_sort Carena, Marcela
collection CERN
description Electroweak baryogenesis is an interesting theoretical scenario, which demands physics beyond the Standard Model at energy scales of the order of the weak boson masses. It has been recently emphasized that, in the presence of light stops, the electroweak phase transition can be strongly first order, opening the window for electroweak baryogenesis in the MSSM. For the realization of this scenario, the Higgs boson must be light, at the reach of the LEP2 collider. In this article, we compute the baryon asymmetry assuming the presence of non-trivial CP violating phases in the parameters associated with the left-right stop mixing term and the Higgsino mass $\mu$. We conclude that a phase $|\sin \phi_{\mu}| > 0.01$ and Higgsino and gaugino mass parameters $|\mu| \simeq M_2$, and of the order of the electroweak scale, are necessary in order to generate the observed baryon asymmetry.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1997
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spelling cern-3211672023-01-31T10:08:11Zdoi:10.1016/S0550-3213(97)00412-4http://cds.cern.ch/record/321167engCarena, MarcelaQuiros, M.Riotto, A.Vilja, I.Wagner, C.E.M.Electroweak baryogenesis and low energy supersymmetryParticle Physics - PhenomenologyElectroweak baryogenesis is an interesting theoretical scenario, which demands physics beyond the Standard Model at energy scales of the order of the weak boson masses. It has been recently emphasized that, in the presence of light stops, the electroweak phase transition can be strongly first order, opening the window for electroweak baryogenesis in the MSSM. For the realization of this scenario, the Higgs boson must be light, at the reach of the LEP2 collider. In this article, we compute the baryon asymmetry assuming the presence of non-trivial CP violating phases in the parameters associated with the left-right stop mixing term and the Higgsino mass $\mu$. We conclude that a phase $|\sin \phi_{\mu}| > 0.01$ and Higgsino and gaugino mass parameters $|\mu| \simeq M_2$, and of the order of the electroweak scale, are necessary in order to generate the observed baryon asymmetry.Electroweak baryogenesis is an interesting theoretical scenario, which demands physics beyond the Standard Model at energy scales of the order of the weak boson masses. It has been recently emphasized that, in the presence of light stops, the electroweak phase transition can be strongly first order, opening the window for electroweak baryogenesis in the MSSM. For the realization of this scenario, the Higgs boson must be light, at the reach of the LEP2 collider. In this article, we compute the baryon asymmetry assuming the presence of non-trivial CP violating phases in the parameters associated with the left-right stop mixing term and the Higgsino mass $\mu$. We conclude that a phase $|\sin \phi_{\mu}| > 0.01$ and Higgsino and gaugino mass parameters $|\mu| \simeq M_2$, and of the order of the electroweak scale, are necessary in order to generate the observed baryon asymmetry.Electroweak baryogenesis is an interesting theoretical scenario, which demands physics beyond the Standard Model at energy scales of the order of the weak boson masses. It has been recently emphasized that, in the presence of light stops, the electroweak phase transition can be strongly first order, opening the window for electroweak baryogenesis in the MSSM. For the realization of this scenario, the Higgs boson must be light, at the reach of the LEP2 collider. In this article, we compute the baryon asymmetry assuming the presence of non-trivial CP violating phases in the parameters associated with the left-right stop mixing term and the Higgsino mass $\mu$. We conclude that a phase $|\sin \phi_{\mu}| > 0.01$ and Higgsino and gaugino mass parameters $|\mu| \simeq M_2$, and of the order of the electroweak scale, are necessary in order to generate the observed baryon asymmetry.Electroweak baryogenesis is an interesting theoretical scenario, which demands physics beyond the Standard Model at energy scales of the order of the weak boson masses. It has been recently emphasized that, in the presence of light stops, the electroweak phase transition can be strongly first order, opening the window for electroweak baryogenesis in the MSSM. For the realization of this scenario, the Higgs boson must be light, at the reach of the LEP2 collider. In this article, we compute the baryon asymmetry assuming the presence of non-trivial CP violating phases in the parameters associated with the left-right stop mixing term and the Higgsino mass $\mu$. We conclude that a phase $|\sin \phi_{\mu}| > 0.01$ and Higgsino and gaugino mass parameters $|\mu| \simeq M_2$, and of the order of the electroweak scale, are necessary in order to generate the observed baryon asymmetry.Electroweak baryogenesis is an interesting theoretical scenario, which demands physics beyond the Standard Model at energy scales of the order of the weak boson masses. It has been recently emphasized that, in the presence of light stops, the electroweak phase transition can be strongly first order, opening the window for electroweak baryogenesis in the MSSM. For the realization of this scenario, the Higgs boson must be light, at the reach of the LEP2 collider. In this article, we compute the baryon asymmetry assuming the presence of non-trivial CP violating phases in the parameters associated with the left-right stop mixing term and the Higgsino mass $\mu$. We conclude that a phase $|\sin \phi_{\mu}| > 0.01$ and Higgsino and gaugino mass parameters $|\mu| \simeq M_2$, and of the order of the electroweak scale, are necessary in order to generate the observed baryon asymmetry.Electroweak baryogenesis is an interesting theoretical scenario, which demands physics beyond the Standard Model at energy scales of the order of the weak boson masses. It has been recently emphasized that, in the presence of light stops, the electroweak phase transition can be strongly first order, opening the window for electroweak baryogenesis in the MSSM. For the realization of this scenario, the Higgs boson must be light, at the reach of the LEP2 collider. In this article, we compute the baryon asymmetry assuming the presence of non-trivial CP violating phases in the parameters associated with the left-right stop mixing term and the Higgsino mass $\mu$. We conclude that a phase $|\sin \phi_{\mu}| > 0.01$ and Higgsino and gaugino mass parameters $|\mu| \simeq M_2$, and of the order of the electroweak scale, are necessary in order to generate the observed baryon asymmetry.Electroweak baryogenesis is an interesting theoretical scenario, which demands physics beyond the Standard Model at energy scales of the order of the weak boson masses. It has been recently emphasized that, in the presence of light stops, the electroweak phase transition can be strongly first order, opening the window for electroweak baryogenesis in the MSSM. For the realization of this scenario, the Higgs boson must be light, at the reach of the LEP2 collider. In this article, we compute the baryon asymmetry assuming the presence of non-trivial CP violating phases in the parameters associated with the left-right stop mixing term and the Higgsino mass $\mu$. We conclude that a phase $|\sin \phi_{\mu}| > 0.01$ and Higgsino and gaugino mass parameters $|\mu| \simeq M_2$, and of the order of the electroweak scale, are necessary in order to generate the observed baryon asymmetry.Electroweak baryogenesis is an interesting theoretical scenario, which demands physics beyond the Standard Model at energy scales of the order of the weak boson masses. It has been recently emphasized that, in the presence of light stops, the electroweak phase transition can be strongly first order, opening the window for electroweak baryogenesis in the MSSM. For the realization of this scenario, the Higgs boson must be light, at the reach of the LEP2 collider. In this article, we compute the baryon asymmetry assuming the presence of non-trivial CP-violating phases in the parameters associated with the left-right stop mixing term and the Higgsino mass μ. We conclude that a phase |sin Φ μ | > 0.01 and Higgsino and gaugino mass parameters | μ | ≅ M 2 , and of the order of the electroweak scale, are necessary in order to generate the observed baryon asymmetry.hep-ph/9702409CERN-TH-96-242IEM-FT-140-96FERMILAB-PUB-96-271-ATURKU-FL-P23-96CERN-TH-96-242FERMILAB-PUB-96-271-AIEM-FT-140TURKU-FL-P-23oai:cds.cern.ch:3211671997-02-24
spellingShingle Particle Physics - Phenomenology
Carena, Marcela
Quiros, M.
Riotto, A.
Vilja, I.
Wagner, C.E.M.
Electroweak baryogenesis and low energy supersymmetry
title Electroweak baryogenesis and low energy supersymmetry
title_full Electroweak baryogenesis and low energy supersymmetry
title_fullStr Electroweak baryogenesis and low energy supersymmetry
title_full_unstemmed Electroweak baryogenesis and low energy supersymmetry
title_short Electroweak baryogenesis and low energy supersymmetry
title_sort electroweak baryogenesis and low energy supersymmetry
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0550-3213(97)00412-4
http://cds.cern.ch/record/321167
work_keys_str_mv AT carenamarcela electroweakbaryogenesisandlowenergysupersymmetry
AT quirosm electroweakbaryogenesisandlowenergysupersymmetry
AT riottoa electroweakbaryogenesisandlowenergysupersymmetry
AT viljai electroweakbaryogenesisandlowenergysupersymmetry
AT wagnercem electroweakbaryogenesisandlowenergysupersymmetry