4.7 Article

Symmetry Classes of Open Fermionic Quantum Matter

期刊

PHYSICAL REVIEW X
卷 11, 期 2, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevX.11.021037

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资金

  1. Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) under Germany's Excellence Strategy Cluster of Excellence Matter and Light for Quantum Computing (ML4Q) [EXC 2004/1 390534769]
  2. DFG Collaborative Research Center (CRC) 183 Project [277101999]
  3. European Research Council (ERC) under the Horizon 2020 research and innovation program [647434]
  4. National Science Foundation [NSF PHY-1748958]
  5. DFG Collaborative Research Center (CRC) 185 Project [277625399]

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This study presents a complete symmetry classification of fermion matter in and out of thermal equilibrium, starting from the state transformations in fermionic Fock spaces and the invariance properties of the density matrix dynamical equation. The classification of generators of reversible dynamics, dissipation, and fluctuations in irreversible and interacting dynamical equations leads to a distinction between equilibrium and out-of-equilibrium symmetries, highlighting the role of time in each case. In the context of nonequilibrium quantum dynamics, a novel realization of antilinear symmetries is observed, fundamentally different from the rules of thermal equilibrium.
We present a full symmetry classification of fermion matter in and out of thermal equilibrium. Our approach starts from first principles, the ten different classes of linear and antilinear state transformations in fermionic Fock spaces, and symmetries defined via invariance properties of the dynamical equation for the density matrix. The object of classification is then the generators of reversible dynamics, dissipation and fluctuations, featuring' in the generally irreversible and interacting dynamical equations. A sharp distinction between the symmetries of equilibrium and out-of-equilibrium dynamics, respectively, arises from the different role played by time in these two cases: In unitary quantum mechanics as well as in microreversible thermal equilibrium, antilinear transformations combined with an inversion of time define time-reversal symmetry. However, out of equilibrium an inversion of time becomes meaningless, while antilinear transformations in Fock space remain physically significant, and hence must be considered in autonomy. The practical consequence of this dichotomy is a novel realization of antilinear symmetries (six out of the ten fundamental classes) in nonequilibrium quantum dynamics that is fundamentally different from the established rules of thermal equilibrium. At large times, the dynamical generators thus symmetry classified determine the steady-state nonequilibrium distributions for arbitrary interacting systems. To illustrate this principle, we consider the fixation of a symmetry protected topological phase in a system of interacting lattice fermions. More generally, we consider the practically important class of mean field interacting systems, represented by Gaussian states. This class is naturally described in the language of non-Hermitian matrices, which allows us to compare to previous classification schemes in the literature.

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