Abstract

Driven-dissipative quantum many-body systems have attracted increasing interest in recent years as they lead to novel classes of quantum many-body phenomena. In particular, mean-field calculations predict limit cycle phases, slow oscillations instead of stationary states, in the long-time limit for a number of driven-dissipative quantum many-body systems. Using a cluster mean-field and a self-consistent Mori projector approach, we explore the persistence of such limit cycles as short range quantum correlations are taken into account in a driven-dissipative Heisenberg model.

Highlights

  • Understanding the phases of quantum many-body systems is one of the central goals of modern physics

  • We explore the existence of limit cycle phases for the model specified in equation (3) via two methods, selfconsistent Mori projectors and cluster mean field

  • We timeintegrate the equations of motion of the respective reduced density matrices using both the self-consistent Mori projector method and cluster mean-field theory until t ? γ−1, where the transient behaviour due to the product state initialisation has decayed and the system has either entered into a limit cycle or has reached a timeindependent steady state

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Summary

Introduction

Understanding the phases of quantum many-body systems is one of the central goals of modern physics. Recent advances have provided the opportunity to extend this field into the exploration of the phase diagrams of non-equilibrium quantum systems where excitations which dissipate from the system are replenished using an external driving field [3,4,5]. Experimental platforms, such as cavity arrays, superconducting circuits and polariton waveguides, have introduced a new class of systems where the interplay between coherent driving and incoherent dissipation has led to the discovery of novel phenomena. Realising limit cycles would be the discovery of a new class of phases in driven dissipative quantum many-body systems but could have important technological applications, for example in synchronising quantum many-body devices [10, 17]

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