Abstract

Master equations are a vital tool to model heat flow through nanoscale thermodynamic systems. Most practical devices are made up of interacting sub-system, and are often modelled using either local master equations (LMEs) or global master equations (GMEs). While the limiting cases in which either the LME or the GME breaks down are well understood, there exists a 'grey area' in which both equations capture steady-state heat currents reliably, but predict very different transient heat flows. In such cases, which one should we trust? Here, we show that, when it comes to dynamics, the local approach can be more reliable than the global one for weakly interacting open quantum systems. This is due to the fact that the secular approximation, which underpins the GME, can destroy key dynamical features. To illustrate this, we consider a minimal transport setup and show that its LME displays exceptional points (EPs). These singularities have been observed in a superconducting-circuit realisation of the model \cite{partanen2019exceptional}. However, in stark contrast to experimental evidence, no EPs appear within the global approach. We then show that the EPs are a feature built into the Redfield equation, which is more accurate than the LME and the GME. Finally, we show that the local approach emerges as the weak-interaction limit of the Redfield equation, and that it entirely avoids the secular approximation.

Highlights

  • Master equations and quantum thermodynamics go hand in hand

  • We find that the local master equations (LMEs) exhibits a family of exceptional points [51] (EPs) in its dynamics, while the corresponding global master equations (GMEs) does not

  • We work in the regime of resonant oscillators, i.e. ωh = ωc = ω, which is a necessary condition for the appearance of the exceptional points in the example model considered, as shown in Appendix C

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Summary

Introduction

Master equations and quantum thermodynamics go hand in hand. The Gorini–Kossakowski–Sudarshan–Lindblad (GKSL) quantum master equation [15, 16] makes it easy to draw parallels between the dissipative dynamics of a single open quantum system and the thermodynamics of macroscopic devices [17,18,19]. These equations can be derived from first principles in the limit of weak system– environment coupling, and may lead to thermal equilibrium [20]. The underlying assumptions of the global master equation require a clean timescale separation [21], which may break down for, e.g., small multipartite quantum-thermodynamic devices that interact weakly among them (see, e.g.,[22, 23]) and large many-body open quantum systems [24]

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