# Nonequilibrium dynamics of the $\sigma$-model modes on the de Sitter space

## TL;DR

This paper investigates the nonequilibrium dynamics of sigma-model modes on de Sitter space, focusing on untangling modes via Bogoliubov transformations and analyzing their evolution using Thermo Field Dynamics.

## Contribution

It introduces a method to obtain untangled oscillators from entangled modes and applies non-equilibrium Thermo Field Dynamics to study their evolution in de Sitter space.

## Key findings

- Untangled oscillators can be derived from entangled modes using Bogoliubov transformations.
- The nonequilibrium dynamics are described by partial evolution equations in Thermo Field Dynamics.
- A local partial evolution functional for thermal doublet fields is constructed.

## Abstract

The two-dimensional $\sigma$-model with the de Sitter target space has a local canonical description in the north pole diamond of the Penrose diagram in the cosmological gauge. The left and right moving modes on the embedded base space with the topology of a cylinder are entangled among themselves and interact with the time-dependent components of the metric of the de Sitter space. Firstly we address the issue of the existence of the untangled oscillator representation and the description of the nonequilibrium dynamics of the untangled modes. We show that the untangled oscillators can be obtained from the entangled operators by applying a set of Bogoliubov transformations that satisfy a set of constraints that result from the requirement that the partial evolution generator be diagonal. Secondly, we determine the nonequilibrium dynamics of the untangled modes in the Non-Equilibrium Thermo Field Dynamics formalism. In this setting, the thermal modes are represented as thermal doublet oscillators that satisfy partial evolution equations of Heisenberg-type. We use these equations to compute the local free one-body propagator of an arbitrary mode between two times. Thirdly, we discuss the field representation of the thermal modes. We show that there is a set of thermal doublet fields that satisfy the equal time canonical commutation relations, are solutions to the $\sigma$-model equations of motion and can be decomposed in terms of thermal doublet oscillators. Finally, we construct a local partial evolution functional of Hamilton-like form for the thermal doublet fields.