Hidden Zero Modes and Topology of Multiband Non-Hermitian Systems

In a finite one-dimensional non-Hermitian system, the number of zero modes does not necessarily reflect the topology of the system. This is known as the breakdown of the bulk-boundary correspondence and has led to misconceptions about the topological protection of edge modes in such systems. Here we show why this breakdown does occur and that it typically results in hidden zero modes, extremely long-lived zero energy excitations, which are only revealed when considering the singular value instead of the eigenvalue spectrum. We point out, furthermore, that in a finite multiband non-Hermitian system with Hamiltonian H, one needs to consider also the reflected Hamiltonian H[over ˜], which is in general distinct from the adjoint H^{†}, to properly relate the number of protected zeros to the winding number of H.

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Publication Details

Journal
Physical Review Letters
Published
2025-02-05
DOI
https://doi.org/10.1103/physrevlett.134.056601
Citations
7
Primary Topic
Quantum Mechanics and Non-Hermitian Physics
Type
article
Field-Weighted Citation Impact
8.73

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article

Hidden Zero Modes and Topology of Multiband Non-Hermitian Systems

Jesko Sirker, Kyle Monkman
7 citations
Physical Review Letters
Quantum Mechanics and Non-Hermitian Physics
8.73
article

Hidden Zero Modes and Topology of Multiband Non-Hermitian Systems

Jesko Sirker, Kyle Monkman
article en
7 citations

Abstract

In a finite one-dimensional non-Hermitian system, the number of zero modes does not necessarily reflect the topology of the system. This is known as the breakdown of the bulk-boundary correspondence and has led to misconceptions about the topological protection of edge modes in such systems. Here we show why this breakdown does occur and that it typically results in hidden zero modes, extremely long-lived zero energy excitations, which are only revealed when considering the singular value instead of the eigenvalue spectrum. We point out, furthermore, that in a finite multiband non-Hermitian system with Hamiltonian H, one needs to consider also the reflected Hamiltonian H[over ˜], which is in general distinct from the adjoint H^{†}, to properly relate the number of protected zeros to the winding number of H.

Physical Review LettersVol. 134(5)
University of British Columbia (CA), University of Manitoba (CA)
Deutsche Forschungsgemeinschaft, Natural Sciences and Engineering Research Council of Canada
Openalex Percentile: Top 2%
Quantum Mechanics and Non-Hermitian Physics
8.73
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