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Electroweak Baryogenesis and the Expansion Rate of the Universe

A homogeneous mode of a scalar field in a ``fast roll'' ( \dot{\phi}^2 >> V(\phi)), which has an energy density scaling as 1/a^6 in an expanding universe, could dominate the universe at the electroweak epoch. The requirement that the energy in the mode red-shift away before nucleosyn...

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Autor principal: Joyce, Michael
Lenguaje:eng
Publicado: 1996
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.55.1875
http://cds.cern.ch/record/304635
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author Joyce, Michael
author_facet Joyce, Michael
author_sort Joyce, Michael
collection CERN
description A homogeneous mode of a scalar field in a ``fast roll'' ( \dot{\phi}^2 >> V(\phi)), which has an energy density scaling as 1/a^6 in an expanding universe, could dominate the universe at the electroweak epoch. The requirement that the energy in the mode red-shift away before nucleosynthesis gives a significantly weakened sphaleron bound for the preservation of a baryon asymmetry produced at a first-order phase transition. The observed baryon asymmetry might even be produced at the electroweak scale in the case that the phase transition is second-order or cross-over. A period where the energy in the universe is dominated by such a mode, which I term {\it kination}, can occur as a scalar field rolls down an exponential potential well motivated in many extensions of standard model physics. A cosmological ``constant'' at the present epoch may also result.
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institution Organización Europea para la Investigación Nuclear
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publishDate 1996
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spelling cern-3046352023-03-14T17:18:01Zdoi:10.1103/PhysRevD.55.1875http://cds.cern.ch/record/304635engJoyce, MichaelElectroweak Baryogenesis and the Expansion Rate of the UniverseParticle Physics - PhenomenologyA homogeneous mode of a scalar field in a ``fast roll'' ( \dot{\phi}^2 >> V(\phi)), which has an energy density scaling as 1/a^6 in an expanding universe, could dominate the universe at the electroweak epoch. The requirement that the energy in the mode red-shift away before nucleosynthesis gives a significantly weakened sphaleron bound for the preservation of a baryon asymmetry produced at a first-order phase transition. The observed baryon asymmetry might even be produced at the electroweak scale in the case that the phase transition is second-order or cross-over. A period where the energy in the universe is dominated by such a mode, which I term {\it kination}, can occur as a scalar field rolls down an exponential potential well motivated in many extensions of standard model physics. A cosmological ``constant'' at the present epoch may also result.A homogeneous mode of a scalar field in a ``fast roll'' ($ \dot{\phi}~2 >> V(\phi)$), which has an energy density scaling as $1/a~6$ in an expanding universe, could dominate the universe at the electroweak epoch. The requirement that the energy in the mode red-shift away before nucleosynthesis gives a significantly weakened sphaleron bound for the preservation of a baryon asymmetry produced at a first-order phase transition. The observed baryon asymmetry might even be produced at the electroweak scale in the case that the phase transition is second-order or cross-over. A period where the energy in the universe is dominated by such a mode, which I term {\it kination}, can occur as a scalar field rolls down an exponential potential well motivated in many extensions of standard model physics. A cosmological ``constant'' at the present epoch may also result.The standard requirement for the production of baryons at the electroweak phase transition, that the phase transition be first order and the sphaleron bound be satisfied, is predicated on the assumption of a radiation dominated universe at that epoch. One simple alternative - domination by the energy in a kinetic mode of a scalar field which scales as $1/a^6$ - gives a significantly weakened sphaleron bound for the preservation of a baryon asymmetry produced at a first-order phase transition, and allows the possibility that the observed baryon asymmetry be produced when the phase transition is second-order or cross-over. Such a phase of `kination' at the electroweak scale can occur in various ways as a scalar field evolves in an exponential potential after inflation.hep-ph/9606223CERN-TH-96-098CERN-TH-96-98CERN-TH-96-098oai:cds.cern.ch:3046351996-06-04
spellingShingle Particle Physics - Phenomenology
Joyce, Michael
Electroweak Baryogenesis and the Expansion Rate of the Universe
title Electroweak Baryogenesis and the Expansion Rate of the Universe
title_full Electroweak Baryogenesis and the Expansion Rate of the Universe
title_fullStr Electroweak Baryogenesis and the Expansion Rate of the Universe
title_full_unstemmed Electroweak Baryogenesis and the Expansion Rate of the Universe
title_short Electroweak Baryogenesis and the Expansion Rate of the Universe
title_sort electroweak baryogenesis and the expansion rate of the universe
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.55.1875
http://cds.cern.ch/record/304635
work_keys_str_mv AT joycemichael electroweakbaryogenesisandtheexpansionrateoftheuniverse