Abstract

When a quantum field is in contact with a thermal bath, the vacuum state of the field may be generalized to a thermal vacuum state, which takes into account the thermal noise. In thermo field dynamics, this is realized by doubling the dimensionality of the Fock space of the system. Interestingly, the representation of thermal noise by means of an augmented space is also found in a distinctly different approach based on the Wigner transform of both the field operators and density matrix, which we pursue here. Specifically, the thermal noise is introduced by augmenting the classical-like Wigner phase space by means of Nosé–Hoover chain thermostats, which can be readily simulated on a computer. In this paper, we illustrate how this may be achieved and discuss how non-equilibrium quantum thermal distributions of the field modes can be numerically simulated.

Highlights

  • According to quantum field theory, the vacuum is filled by fluctuating quantum fields

  • In thermo field dynamics [24,25,26], the vacuum state is generalized to a thermal vacuum state by doubling the dimension of the Fock space of the original vacuum

  • The simulation protocol, which involves an Nosé–Hoover chain (NHC) thermostat [44,45] coupled to each field mode, propagates the dynamics of a thermal state living in an extended Wigner space [67]

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Summary

Introduction

According to quantum field theory, the vacuum is filled by fluctuating quantum fields. We illustrate an approach to simulate the thermal distributions of bosonic fields [27,28,29,30,31,32,33,34] on a computer, which exploits the Wigner formulation of quantum field theory [35,36,37,38,39,40]. It is possible to simulate quantum thermal distributions with a different temperature for each mode and to define a time-dependent temperature. This is achieved by means of a technique called massive.

Wigner Formulation of Bosonic Field Theory
Computer Simulation of Thermal Field States
Conclusions
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