The weak electroweak phase transition
arXiv:hep-ph/9303251 · doi:10.1006/aphy.1994.1082
Abstract
We present a detailed analysis of the phase transition in the standard model at finite temperature. Using an improved perturbation theory, where plasma masses are determined from a set of one-loop gap equations, we evaluate the effective potential in next-to-leading order, i.e., including terms cubic in the gauge coupling , the scalar self-coupling and the top-quark Yukawa coupling . The gap equations yield a non-vanishing magnetic plasma mass for the gauge bosons, originating from the non-abelian self-interactions. We discuss in detail size and origin of higher order effects and conclude that the phase transition is weakly first-order up to Higgs masses of about , above which our calculation is no longer self-consistent. For larger Higgs masses even an approximation containing all contributions to is not sufficient, at least a full calculation to order is needed. These results turn out to be rather insensitive to the top-quark mass in the range . Using Langer's theory of metastability we calculate the nucleation rate of critical droplets and discuss some aspects of the cosmological electroweak phase transition.
LaTeX, 45 pages, 13 figures [not included, can be sent upon request],DESY 93-021
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