Stochastic entropy production associated with quantum measurement in a framework of Markovian quantum state diffusion

TL;DR

This paper explores the stochastic entropy production in a two-level open quantum system under continuous measurement, revealing how measurement influences the system's unpredictability and thermodynamics.

Contribution

It introduces a framework analyzing stochastic entropy production during quantum measurement, highlighting differences from von Neumann entropy and effects of simultaneous non-commuting measurements.

Findings

Entropy production increases as the system approaches an eigenstate.

Simultaneous measurement of non-commuting observables leads to stationary states.

Transitions between stationary states produce finite positive entropy production.

Abstract

The reduced density matrix that characterises the state of an open quantum system is a projection from the full density matrix of the quantum system and its environment, and there are many full density matrices consistent with a given reduced version. Without a specification of relevant details of the environment, the evolution of a reduced density matrix is therefore typically unpredictable, even if the dynamics are deterministic. With this in mind, we investigate a two level open quantum system using a framework of quantum state diffusion. We consider the pseudorandom evolution of its reduced density matrix when subjected to an environment-driven process of continuous quantum measurement of a system observable, using dynamics that asymptotically send the system to an eigenstate. The unpredictability is characterised by a stochastic entropy production, the average of which corresponds to an increase in the subjective uncertainty of the quantum state adopted by the system and environment, given the underspecified dynamics. This differs from a change in von Neumann entropy, and can continue indefinitely as the system is guided towards an eigenstate. As one would expect, the simultaneous measurement of two non-commuting observables within the same framework does not send the system to an eigenstate. Instead, the probability density function describing the reduced density matrix of the system becomes stationary over a continuum of pure states, a situation characterised by zero further stochastic entropy production. Transitions between such stationary states, brought about by changes in the relative strengths of the two measurement processes, give rise to finite positive mean stochastic entropy production. The framework investigated can offer useful perspectives on both the dynamics and irreversible thermodynamics of measurement in quantum systems.