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Kinetics of Sub-Critical Bubbles and the Electroweak Transition

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abstract

We investigate the role of large amplitude sub-critical thermal fluctuations in the dynamics of first order phase transitions. In particular, we obtain a kinetic equation for the number density of sub-critical fluctuations of the broken-symmetric phase within the symmetric phase, modeled as spherical bubbles, and solve it analytically for temperatures above the critical temperature. We study the approach to equilibrium and obtain the equilibrium distribution of sub-critical bubbles of the unstable phase by examining three possible mechanisms responsible for their removal; their shrinking, their coupling to thermal noise, and by thermal fluctuations of the true vacuum inside them. We show that for sufficiently strong transitions, either the shrinking or the coupling to thermal noise dominate the dynamics. As the strength of the transition weakens we show that sub-critical fluctuations become progressively more important, as a larger fraction of the total volume is occupied by the broken-symmetric phase, until the point where our analytical approach breaks down. Our investigation suggests that pre-transitional phenomena may considerably change the dynamics of sufficiently weak first-order transitions. We apply our results to the standard electroweak transition.

fields

hep-ph 1

years

2026 1

verdicts

UNVERDICTED 1

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Subcritical bubble prehistory in weak first-order phase transition

hep-ph · 2026-05-24 · unverdicted · novelty 5.0

In weak first-order phase transitions, subcritical bubbles reach percent-level volume fractions before critical nucleation when phases are nearly degenerate at Tn, invalidating the homogeneous-background assumption for points satisfying log10 f̂_ξ(Tn) ≃ -1.95.

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  • Subcritical bubble prehistory in weak first-order phase transition hep-ph · 2026-05-24 · unverdicted · none · ref 36 · internal anchor

    In weak first-order phase transitions, subcritical bubbles reach percent-level volume fractions before critical nucleation when phases are nearly degenerate at Tn, invalidating the homogeneous-background assumption for points satisfying log10 f̂_ξ(Tn) ≃ -1.95.