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Electroweak Baryogenesis and Higgs and Stop Searches at LEP and the Tevatron

It has been recently shown that the observed baryon number may originate at the electroweak phase transition, provided that the Higgs boson and the lightest stop are sufficiently light. In this work, we perform a detailed analysis, including all dominant two-loop finite temperature corrections to th...

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Detalles Bibliográficos
Autores principales: Carena, Marcela, Quiros, M., Wagner, C.E.M.
Lenguaje:eng
Publicado: 1997
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0550-3213(98)00187-4
http://cds.cern.ch/record/336566
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author Carena, Marcela
Quiros, M.
Wagner, C.E.M.
author_facet Carena, Marcela
Quiros, M.
Wagner, C.E.M.
author_sort Carena, Marcela
collection CERN
description It has been recently shown that the observed baryon number may originate at the electroweak phase transition, provided that the Higgs boson and the lightest stop are sufficiently light. In this work, we perform a detailed analysis, including all dominant two-loop finite temperature corrections to the Higgs effective potential, as well as the non-trivial effects proceeding from the mixing in the stop sector, to define the region of parameter space for which electroweak baryogenesis can happen. The limits on the stop and Higgs masses are obtained by taking into account the experimental bounds on these quantities, as well as those coming from the requirement of avoiding dangerous color breaking minima. We find for the Higgs mass $m_h \simlt 105$ GeV, while the stop mass may be close to the present experimental bound and must be smaller than, or of order of, the top quark mass. These results provide a very strong motivation for further non-perturbative analysis of the electroweak phase transition, as well as for the search for Higgs and stop particles at the LEP and Tevatron colliders.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1997
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spelling cern-3365662023-01-31T09:14:49Zdoi:10.1016/S0550-3213(98)00187-4http://cds.cern.ch/record/336566engCarena, MarcelaQuiros, M.Wagner, C.E.M.Electroweak Baryogenesis and Higgs and Stop Searches at LEP and the TevatronParticle Physics - PhenomenologyIt has been recently shown that the observed baryon number may originate at the electroweak phase transition, provided that the Higgs boson and the lightest stop are sufficiently light. In this work, we perform a detailed analysis, including all dominant two-loop finite temperature corrections to the Higgs effective potential, as well as the non-trivial effects proceeding from the mixing in the stop sector, to define the region of parameter space for which electroweak baryogenesis can happen. The limits on the stop and Higgs masses are obtained by taking into account the experimental bounds on these quantities, as well as those coming from the requirement of avoiding dangerous color breaking minima. We find for the Higgs mass $m_h \simlt 105$ GeV, while the stop mass may be close to the present experimental bound and must be smaller than, or of order of, the top quark mass. These results provide a very strong motivation for further non-perturbative analysis of the electroweak phase transition, as well as for the search for Higgs and stop particles at the LEP and Tevatron colliders.It has been recently shown that the observed baryon number may originate at the electroweak phase transition, provided that the Higgs boson and the lightest stop are sufficiently light. In this work, we perform a detailed analysis, including all dominant two-loop finite temperature corrections to the Higgs effective potential, as well as the non-trivial effects proceeding from the mixing in the stop sector, to define the region of parameter space for which electroweak baryogenesis can happen. The limits on the stop and Higgs masses are obtained by taking into account the experimental bounds on these quantities, as well as those coming from the requirement of avoiding dangerous color breaking minima. We find for the Higgs mass $m_h \simlt 105$ GeV, while the stop mass may be close to the present experimental bound and must be smaller than, or of order of, the top quark mass. These results provide a very strong motivation for further non-perturbative analysis of the electroweak phase transition, as well as for the search for Higgs and stop particles at the LEP and Tevatron colliders.It has been recently shown that the observed baryon number may originate at the electroweak phase transition, provided that the Higgs boson and the lightest stop are sufficiently light. In this work, we perform a detailed analysis, including all dominant two-loop finite temperature corrections to the Higgs effective potential, as well as the non-trivial effects proceeding from the mixing in the stop sector, to define the region of parameter space for which electroweak baryogenesis can happen. The limits on the stop and Higgs masses are obtained by taking into account the experimental bounds on these quantities, as well as those coming from the requirement of avoiding dangerous color breaking minima. We find for the Higgs mass $m_h \simlt 105$ GeV, while the stop mass may be close to the present experimental bound and must be smaller than, or of order of, the top quark mass. These results provide a very strong motivation for further non-perturbative analysis of the electroweak phase transition, as well as for the search for Higgs and stop particles at the LEP and Tevatron colliders.It has been recently shown that the observed baryon number may originate at the electroweak phase transition, provided that the Higgs boson and the lightest stop are sufficiently light. In this work, we perform a detailed analysis, including all dominant two-loop finite temperature corrections to the Higgs effective potential, as well as the non-trivial effects proceeding from the mixing in the stop sector, to define the region of parameter space for which electroweak baryogenesis can happen. The limits on the stop and Higgs masses are obtained by taking into account the experimental bounds on these quantities, as well as those coming from the requirement of avoiding dangerous color breaking minima. We find for the Higgs mass $m_h \simlt 105$ GeV, while the stop mass may be close to the present experimental bound and must be smaller than, or of order of, the top quark mass. These results provide a very strong motivation for further non-perturbative analysis of the electroweak phase transition, as well as for the search for Higgs and stop particles at the LEP and Tevatron colliders.It has been recently shown that the observed baryon number may originate at the electroweak phase transition, provided that the Higgs boson and the lightest stop are sufficiently light. In this work, we perform a detailed analysis, including all dominant two-loop finite-temperature corrections to the Higgs effective potential, as well as the non-trivial effects proceeding from the mixing in the stop sector, to define the region of parameter space for which electroweak baryogenesis can happen. The limits on the stop and Higgs masses are obtained by taking into account the experimental bounds on these quantities, as well as those coming from the requirement of avoiding dangerous color breaking minima. We find for the Higgs mass m h ⪷ 105 GeV , while the stop mass may be close to the present experimental bound and must be smaller than, or of the order of, the top quark mass. These results provide a very strong motivation for further non-perturbative analysis of the electroweak phase transition, as well as for the search for Higgs and stop particles at the LEP and Tevatron colliders.hep-ph/9710401FERMILAB-PUB-97-327-TCERN-TH-97-190IEM-FT-165-97CERN-TH-97-190FERMILAB-PUB-97-327-TIEM-FT-165oai:cds.cern.ch:3365661997-10-21
spellingShingle Particle Physics - Phenomenology
Carena, Marcela
Quiros, M.
Wagner, C.E.M.
Electroweak Baryogenesis and Higgs and Stop Searches at LEP and the Tevatron
title Electroweak Baryogenesis and Higgs and Stop Searches at LEP and the Tevatron
title_full Electroweak Baryogenesis and Higgs and Stop Searches at LEP and the Tevatron
title_fullStr Electroweak Baryogenesis and Higgs and Stop Searches at LEP and the Tevatron
title_full_unstemmed Electroweak Baryogenesis and Higgs and Stop Searches at LEP and the Tevatron
title_short Electroweak Baryogenesis and Higgs and Stop Searches at LEP and the Tevatron
title_sort electroweak baryogenesis and higgs and stop searches at lep and the tevatron
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/S0550-3213(98)00187-4
http://cds.cern.ch/record/336566
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AT quirosm electroweakbaryogenesisandhiggsandstopsearchesatlepandthetevatron
AT wagnercem electroweakbaryogenesisandhiggsandstopsearchesatlepandthetevatron