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Towards the Theory of Cosmological Phase Transitions

M. Dine, R. Leigh, P. Huet, A. Linde, D. Linde

TL;DR

The paper analyzes the electroweak phase transition at finite temperature, deriving and examining the finite-temperature potential $V(\phi,T)$ and the bubble nucleation dynamics through the action $S_3$ and rate $S_3/T$. It shows that no dangerous linear terms arise in the effective potential after careful higher-order accounting, but the cubic term is reduced by a factor of $2/3$ due to infrared screening, weakening the transition in the minimal Standard Model and challenging baryogenesis scenarios. Bubble formation is dominated by critical bubbles with $S_3/T\sim130$–$140$ for a strongly first-order transition, while subcritical bubbles are only relevant for extremely weak transitions. The bubble wall propagation through the hot plasma is generally non-relativistic and thick across several parameter regimes, with density enhancements and damping slowing the wall further; the results motivate exploring extensions of the Standard Model to realize a sufficiently strong first-order transition for successful baryogenesis.

Abstract

We discuss recent progress (and controversies) in the theory of finite temperature phase transitions. This includes the structure of the effective potential at a finite temperature, the infrared problem in quantum statistics of gauge fields, the theory of formation of critical and subcritical bubbles and the theory of bubble wall propagation.

Towards the Theory of Cosmological Phase Transitions

TL;DR

The paper analyzes the electroweak phase transition at finite temperature, deriving and examining the finite-temperature potential and the bubble nucleation dynamics through the action and rate . It shows that no dangerous linear terms arise in the effective potential after careful higher-order accounting, but the cubic term is reduced by a factor of due to infrared screening, weakening the transition in the minimal Standard Model and challenging baryogenesis scenarios. Bubble formation is dominated by critical bubbles with for a strongly first-order transition, while subcritical bubbles are only relevant for extremely weak transitions. The bubble wall propagation through the hot plasma is generally non-relativistic and thick across several parameter regimes, with density enhancements and damping slowing the wall further; the results motivate exploring extensions of the Standard Model to realize a sufficiently strong first-order transition for successful baryogenesis.

Abstract

We discuss recent progress (and controversies) in the theory of finite temperature phase transitions. This includes the structure of the effective potential at a finite temperature, the infrared problem in quantum statistics of gauge fields, the theory of formation of critical and subcritical bubbles and the theory of bubble wall propagation.

Paper Structure

This paper contains 12 sections, 95 equations.