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
Summary
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].
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