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Topological Correspondence between Hermitian and Non-Hermitian Systems: Anomalous Dynamics

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arxiv 1906.08782 v1 pith:KVXQRJOL submitted 2019-06-20 cond-mat.mes-hall math-phmath.MPphysics.opticsquant-ph

classification cond-mat.mes-hallmath-phmath.MPphysics.opticsquant-ph
keywords anomalousnon-hermitiantopologicalboundaryhermitiansystemscorrespondencecorresponding
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abstract

The hallmark of symmetry-protected topological (SPT) phases is the existence of anomalous boundary states, which can only be realized with the corresponding bulk system. In this work, we show that for every Hermitian anomalous boundary mode of the ten Altland-Zirnbauer classes, a non-Hermitian counterpart can be constructed, whose long time dynamics provides a realization of the anomalous boundary state. We prove that the non-Hermitian counterpart is characterized by a point-gap topological invariant, and furthermore, that the invariant exactly matches that of the corresponding Hermitian anomalous boundary mode. We thus establish a correspondence between the topological classifications of $(d+1)$-dimensional gapped Hermitian systems and $d$-dimensional point-gapped non-Hermitian systems. We illustrate this general result with a number of examples in different dimensions. This work provides a new perspective on point-gap topological invariants in non-Hermitian systems.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Non-Hermitian Boundary State Engineering in Anomalous Floquet Topological Insulators

    cond-mat.mes-hall 2019-08 conditional novelty 7.0 of 10

    Non-Hermitian losses in anomalous Floquet insulators let boundary states detach from bulk bands and be engineered independently, enabling new chiral and directional edge transport.

  2. Hidden Chern number in one-dimensional non-Hermitian chiral-symmetric systems

    cond-mat.str-el 2019-08 conditional novelty 6.0 of 10

    The topology of certain one-dimensional non-Hermitian chains is captured by a Chern number of an effective two-dimensional Hermitian Hamiltonian, and this hidden Chern number predicts zero-real-energy end states.

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