Entropy production dynamics in quench protocols of a driven-dissipative critical system

TL;DR

This paper investigates how entropy production evolves during sudden changes in a driven-dissipative quantum system, revealing insights into non-adiabaticity and quantum fluctuations using a Husimi Q-function approach.

Contribution

It introduces a formalism to analyze entropy production dynamics in a driven-dissipative system, distinguishing classical and quantum contributions during quenches.

Findings

Entropy production rate splits into classical and quantum parts.

Quantum fluctuations dominate during non-adiabatic quenches.

The framework captures non-Gaussian and out-of-equilibrium effects.

Abstract

Driven-dissipative phase transitions are currently a topic of intense research due to the prospect of experimental realizations in quantum optical setups. The most paradigmatic model presenting such a transition is the Kerr model, which predicts the phenomenon of optical bistability, where the system may relax to two different steady-states for the same driving condition. These states, however, are inherently out-of-equilibrium and are thus characterized by the continuous production of irreversible entropy, a key quantifier in thermodynamics. In this paper we study the dynamics of the entropy production rate in a quench scenario of the Kerr model, where the external pump is abruptly changed. This is accomplished using a recently developed formalism, based on the Husimi $Q$-function, which is particularly tailored for driven-dissipative and non-Gaussian bosonic systems [Phys. Rev. Res. 2, 013136 (2020)]. Within this framework the entropy production can be split into two contributions, one being extensive with the drive and describing classical irreversibility, and the other being intensive and directly related to quantum fluctuations. The latter, in particular, is found to reveal the high degree of non-adiabaticity, for quenches between different metastable states.