Non-perturbative determination of the sphaleron rate for first-order phase transitions

TL;DR

This paper non-perturbatively calculates the sphaleron rate during electroweak phase transitions using lattice simulations, establishing conditions for baryon asymmetry preservation in extensions of the Standard Model.

Contribution

It provides a comprehensive non-perturbative determination of sphaleron rates across the parameter space, refining the criteria for electroweak baryogenesis viability.

Findings

Sphaleron rate determined for the entire Higgs phase region.

A new condition on the phase transition strength for baryon asymmetry preservation.

A general framework for analyzing beyond Standard Model theories at high temperature.

Abstract

In many extensions of the Standard Model electroweak phase transitions at high temperatures can be described in a minimal dimensionally reduced effective theory with SU(2) gauge field and fundamental Higgs scalar. In this effective theory, all thermodynamic information is governed by two dimensionless ratios $x \equiv \lambda_3/g^2_3$ and $y\equiv m^2_3/g^4_3$, where $\lambda_3$, $m^2_3$ and $g_3$ are the effective thermal scalar self-interaction coupling, the thermal mass and the effective gauge-coupling, respectively. By using non-perturbative lattice simulations to determine the rate of sphaleron transitions in the entire $(x,y)$-plane corresponding to the Higgs phase, and by applying previous lattice results for the bubble nucleation, we find a condition $x(T_c) \lesssim 0.025$ to guarantee preservation of the baryon asymmetry, which translates to $v/T_c \equiv \sqrt{2 \Delta \langle \phi^\dagger \phi \rangle}/T_c \gtrsim 1.33$ for the (gauge-invariant) discontinuity in Higgs condensate. This indicates that viability of the electroweak baryogenesis requires the phase transition to be slightly stronger than previously anticipated. Finally, we present a general template for analysing such viability in a wide class of beyond the Standard Model theories, in which new fields are heavy enough to be integrated out at high temperature.