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  • Letter

Random matrix theory for quantum and classical metastability in local Liouvillians

Jimin L. Li1, Dominic C. Rose2,3,4, Juan P. Garrahan2,3, and David J. Luitz5

  • 1Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, United Kingdom
  • 2School of Physics and Astronomy, University of Nottingham, Nottingham NG7 2RD, United Kingdom
  • 3Centre for the Mathematics and Theoretical Physics of Quantum Non-Equilibrium Systems, University of Nottingham, Nottingham NG7 2RD, United Kingdom
  • 4Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, United Kingdom
  • 5Max Planck Institute for the Physics of Complex Systems, Noethnitzer Straße 38, 01187 Dresden, Germany

Phys. Rev. B 105, L180201 – Published 6 May, 2022

DOI: https://doi.org/10.1103/PhysRevB.105.L180201

Abstract

We consider the effects of strong dissipation in quantum systems with a notion of locality, which induces a hierarchy of many-body relaxation timescales as shown by K. Wang, F. Piazza, and D. J. Luitz [Phys. Rev. Lett. 124, 100604 (2020)]. If the strength of the dissipation varies strongly in the system, additional separations of timescales can emerge, inducing a manifold of metastable states, to which observables relax first, before relaxing to the steady state. Our simple model, involving one or two “good” qubits with dissipation reduced by a factor α<1 compared to the other “bad” qubits, confirms this picture and admits a perturbative treatment.

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