Abstract

Scalar fields appear in many theories beyond the Standard Model of particle physics. In the early universe, they are exposed to extreme conditions, including high temperature and rapid cosmic expansion. Understanding their behavior in this environment is crucial to understand the implications for cosmology. We calculate the finite temperature effective action for the field expectation value in two particularly important cases, for damped oscillations near the ground state and for scalar fields with a flat potential. We find that the behavior in both cases can in good approximation be described by a complex valued effective potential that yields Markovian equations of motion. Near the potential minimum, we recover the solution to the well-known Langevin equation. For large field values we find a very different behavior, and our result for the damping coefficient differs from the expressions frequently used in the literature. We illustrate our results in a simple scalar model, for which we give analytic approximations for the effective potential and damping coefficient. We also provide various expressions for loop integrals at finite temperature that are useful for future calculations in other models.

Highlights

  • 1.1 Scalar fields and the early universeScalar fields play important roles in particle physics and cosmology

  • In cosmology involving scalar fields, it is crucial to understand their time evolution in the early universe, where they are exposed to extreme conditions including high temperature, large energy density and rapid cosmic expansion

  • The contribution (4.27) is not physical and we artificially introduced by the approximation (4.22), which is only valid in the region Ω2χ fB (Ωχ) Γ2χ/ω

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Summary

Introduction

1.1 Scalar fields and the early universeScalar fields play important roles in particle physics and cosmology. In cosmology involving scalar fields, it is crucial to understand their time evolution in the early universe, where they are exposed to extreme conditions including high temperature, large energy density and rapid cosmic expansion. Their evolution in a time-dependent background provided by the primordial plasma and the cosmic expansion is a nonequilibrium process. There are numerous examples for scalar fields with a flat potential that evolve slowly compared to the time scale related to the propagation and interactions of individual particles, including the moduli, inflaton and axions. With the present work, focusing on the finite-temperature effects in a thermal bath, we aim to make progress towards a quantitative understanding of the nonequilibrium dynamics of scalar fields in the nontrivial backgrounds of the early universe

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