Abstract

In the study of $\mathcal{P}\mathcal{T}$-symmetric quantum systems with non-Hermitian perturbations, one of the most important questions is whether eigenvalues stay real or whether $\mathcal{P}\mathcal{T}$-symmetry is spontaneously broken when eigenvalues meet. A particularly interesting set of eigenstates is provided by the degenerate ground-state subspace of systems with topological order. In this paper, we present simple criteria that guarantee the protection of $\mathcal{P}\mathcal{T}$-symmetry and, thus, the reality of the eigenvalues in topological many-body systems. We formulate these criteria in both geometric and algebraic form, and demonstrate them using the toric code and several different fracton models as examples. Our analysis reveals that $\mathcal{P}\mathcal{T}$-symmetry is robust against a remarkably large class of non-Hermitian perturbations in these models; this is particularly striking in the case of fracton models due to the exponentially large number of degenerate states.

Highlights

  • Isolated systems are governed by Hermitian Hamiltonians, with real energy eigenvalues and unitary time evolution

  • We studied the behavior of the eigenvalues of quantum many-body Hamiltonians of the form of Eq (2), i.e., starting from a Hermitian system, H0, we turn on a non-Hermitian perturbation, V, and demand that the entire Hamiltonian be pseudo-Hermitian

  • Using pseudo-Hermiticity rather than PT symmetry is related to the fact that the former is more general than the latter [115]; we note, that all of the explicit examples considered here are both PT symmetric and pseudo-Hermitian

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Summary

INTRODUCTION

Isolated systems are governed by Hermitian Hamiltonians, with real energy eigenvalues and unitary time evolution. Non-Hermitian Hamiltonians [1,2,3,4,5], for which eigenvalues may generally be complex, are physically relevant as effective descriptions of a large variety of different systems They have been studied in the context of biological [6,7,8], mechanical [9], and photonic [10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32] systems, electrical circuits [33,34,35], cavities [36,37,38,39], optical lattices [40], superconductors [41,42], and open quantum systems [4,32,43,44,45,46,47].

PSEUDO-HERMITIAN PERTURBATIONS
Protection of reality of energies
Remarks on condition for reality
NON-HERMITIAN TORIC CODES
Pseudo-Hermitian perturbations
Starting with perturbed toric code
Exceptional points
Other metric operators
Arbitrary system sizes
NON-HERMITIAN FRACTON MODELS
X-cube model
Checkerboard model
Haah’s codes
NON-HERMITIAN QUANTUM FRACTAL LIQUIDS
Polynomial representation of operators
SUMMARY AND CONCLUSIONS
Expansion in
Expansion in energy separation
Approximate orthogonality
Full Text
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