Abstract

Steady-state observables, such as occupation numbers and currents, are crucial experimental signatures in open quantum systems. The time-convolutionless (TCL) master equation, which is both exact and time-local, is an ideal candidate for the perturbative computation of such observables. We develop a diagrammatic approach to evaluate the steady-state TCL generator based on operators rather than superoperators. We obtain the steady-state occupation numbers, extend our formulation to the calculation of currents, and provide a simple physical interpretation of the diagrams. We further benchmark our method on a single non-interacting level coupled to Fermi reservoirs, where we recover the exact expansion to next-to-leading order. The low number of diagrams appearing in our formulation makes the extension to higher orders accessible. Combined, these properties make the steady-state time-convolutionless master equation an effective tool for the calculation of steady-state properties in open quantum systems.

Highlights

  • Open quantum systems constitute a wide research area that permeates both fundamental and applied physics [1,2]

  • The presence of the environment can fundamentally change the dynamics of the system [18,19,20], while leaving it sufficiently coherent for quantum effects to be crucial in explaining its behavior

  • We focus on the STCL master equation approach and demonstrate that it serves as a practical tool to compute the steady state of open quantum systems

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Summary

Introduction

Open quantum systems constitute a wide research area that permeates both fundamental and applied physics [1,2]. Given the recent developments in quantum technologies, such systems promise great advances in computing [12,13], simulation [14], and sensing [15,16,17]. Regardless of the specific realization, open systems can all be broadly described as containing a small system of central interest that is coupled to a large environment. We consider a setup composed of a system and an environment as shown, and compute its steady-state properties. To this end, we focus on the time evolution of the system after a slow switch-on using a master equation.

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