Spectral topology and delocalization in disordered Hatano–Nelson chains

Abstract The unidirectional Hatano–Nelson chain serves as the fundamental non-Hermitian building block of the Su–Schrieffer–Heeger (SSH) model. We investigate its Anderson localization properties under diagonal binary disorder. For weak disorder, the complex eigenvalue spectrum forms a single closed loop, which bifurcates into two distinct loops at a critical disorder threshold. Correspondingly, the spectral winding number ν undergoes a transition from ν = 1 in the weak-disorder regime, through ν = 1/2 at the critical point, to ν = 0 in the strong-disorder limit. We show that the eigenstates are subexponentially localized, with a localization length that varies analytically as a function of the momentum-like quantum number q . Notably, at weak and critical disorder, the spectrum hosts two completely delocalized states with diverging localization lengths. This divergence is directly correlated with the non-trivial spectral winding number. These findings remain robust under various boundary conditions, with the exception of strictly open boundaries.

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Publication Details

Journal
Zeitschrift für Naturforschung A
Published
2026-04-22
DOI
https://doi.org/10.1515/zna-2026-0013
Primary Topic
Quantum Mechanics and Non-Hermitian Physics
Type
article
Field-Weighted Citation Impact
0.00
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article

Spectral topology and delocalization in disordered Hatano–Nelson chains

Sergej Flach, Supriyo Ghosh
Zeitschrift für Naturforschung A
Quantum Mechanics and Non-Hermitian Physics
article

Spectral topology and delocalization in disordered Hatano–Nelson chains

Sergej Flach, Supriyo Ghosh
article en

Abstract

Abstract The unidirectional Hatano–Nelson chain serves as the fundamental non-Hermitian building block of the Su–Schrieffer–Heeger (SSH) model. We investigate its Anderson localization properties under diagonal binary disorder. For weak disorder, the complex eigenvalue spectrum forms a single closed loop, which bifurcates into two distinct loops at a critical disorder threshold. Correspondingly, the spectral winding number ν undergoes a transition from ν = 1 in the weak-disorder regime, through ν = 1/2 at the critical point, to ν = 0 in the strong-disorder limit. We show that the eigenstates are subexponentially localized, with a localization length that varies analytically as a function of the momentum-like quantum number q . Notably, at weak and critical disorder, the spectrum hosts two completely delocalized states with diverging localization lengths. This divergence is directly correlated with the non-trivial spectral winding number. These findings remain robust under various boundary conditions, with the exception of strictly open boundaries.

Zeitschrift für Naturforschung AVol. 81(5)
Visva-Bharati University (IN), Institute for Basic Science (KR), Massey University (NZ), Korea University of Science and Technology (KR)
Openalex Percentile: Top 13%
Quantum Mechanics and Non-Hermitian Physics
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