TY - JOUR
T1 - Electroweak baryogenesis in the adiabatic limit
AU - Dine, Michael
AU - Thomas, Scott
N1 - Funding Information:
The electroweak transition, if first order, proceeds by formation of bubbles. The baryon asymmetry is produced in or near the bubble walls, which are the sites of the most significant departures from equilib- * Supported in part by the U.S. Department of Energy and the Texas National Research Laboratory Commission under grant numbers RGFY 93-263 and RGFY 93-330.
PY - 1994/5/26
Y1 - 1994/5/26
N2 - Electroweak baryogenesis can occur in the "adiabatic limit", in which expanding bubbles of true vacuum are assumed to have rather thick walls and be slowly moving. Here the problem of calculating the baryon asymmetry in this limit is reconsidered. A simple prescription for obtaining the relevant kinetic equations is given. An additional suppression beyond that usually assumed is found. This arises because the generation of an asymmetry requires violation of approximately conserved currents by Higgs expectation values, which are small near the front of the walls. As applications, the asymmetries in multi-Higgs models and the minimal supersymmetric standard model are estimated to be proportional to α8w and α6w respectively. Also, in this limit the baryon asymmetry in the minimal standard model is extraordinary small.
AB - Electroweak baryogenesis can occur in the "adiabatic limit", in which expanding bubbles of true vacuum are assumed to have rather thick walls and be slowly moving. Here the problem of calculating the baryon asymmetry in this limit is reconsidered. A simple prescription for obtaining the relevant kinetic equations is given. An additional suppression beyond that usually assumed is found. This arises because the generation of an asymmetry requires violation of approximately conserved currents by Higgs expectation values, which are small near the front of the walls. As applications, the asymmetries in multi-Higgs models and the minimal supersymmetric standard model are estimated to be proportional to α8w and α6w respectively. Also, in this limit the baryon asymmetry in the minimal standard model is extraordinary small.
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U2 - 10.1016/0370-2693(94)90430-8
DO - 10.1016/0370-2693(94)90430-8
M3 - Article
AN - SCOPUS:0003164385
SN - 0370-2693
VL - 328
SP - 73
EP - 78
JO - Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
JF - Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
IS - 1-2
ER -