Skip to content
aiqbench takeQuantum Computing

aiqbench analysis

This study experimentally demonstrates a non-Hermitian skin effect within flat bands, revealing that the phenomenon relies on the spectral topology of surrounding dispersive bands rather than the flat band's own topology. Unlike conventional effects, this flat-band skin effect emerges only within a finite range of non-Hermitian parameters and vanishes at high non-Hermiticity, exhibiting singular discontinuities at exceptional points. The findings advance the theoretical understanding of quantum geometry and localization control in non-Hermitian systems.
Source coveringarXiv
What this isA model's reading of the article and related coverage, written for aiqbench. Not the publisher's words.

Observation of flat-band skin effect

arXiv2 min read

arXiv:2512.19745v2 Announce Type: replace Abstract: Symmetry-protected ideal flat bands in one-dimensional (1D) Hermitian lattices are populated by compact localized states (CLS) - a special class of localization with wavefunctions confined within a small region. In this work, we discover that the non-Hermitian skin effect (NHSE) can appear in a flat band. Unlike conventional NHSEs for dispersive bands that are protected by nontrivial point-gap topology, the flat band remains a point on the complex-energy plane and is therefore always topologically trivial. We found that, intriguingly, the flat-band skin effect (FBSE) is associated with the non-trivial spectral topology of the dispersive bands enclosing the flat band on the complex-energy plane, so it only emerges within a finite range of non-Hermitian parameters and can counterintuitively disappear at large non-Hermiticity. Moreover, the gaps between the flat and the dispersive bands can close at higher-order exceptional points under both periodic and open boundary conditions. The flat-band wavefunctions are discontinuous in quantum distance across these exceptional points, signifying that the gap-closing is singular. The FBSE was experimentally observed in a non-Hermitian mechanical lattice. Our work reveals flat-band phenomena unique to non-Hermitian systems and highlights new possibilities in quantum geometry and localization control.

Abstract:Symmetry-protected ideal flat bands in one-dimensional (1D) Hermitian lattices are populated by compact localized states (CLS) - a special class of localization with wavefunctions confined within a small region. In this work, we discover that the non-Hermitian skin effect (NHSE) can appear in a flat band. Unlike conventional NHSEs for dispersive bands that are protected by nontrivial point-gap topology, the flat band remains a point on the complex-energy plane and is therefore always topologically trivial. We found that, intriguingly, the flat-band skin effect (FBSE) is associated with the non-trivial spectral topology of the dispersive bands enclosing the flat band on the complex-energy plane, so it only emerges within a finite range of non-Hermitian parameters and can counterintuitively disappear at large non-Hermiticity. Moreover, the gaps between the flat and the dispersive bands can close at higher-order exceptional points under both periodic and open boundary conditions. The flat-band wavefunctions are discontinuous in quantum distance across these exceptional points, signifying that the gap-closing is singular. The FBSE was experimentally observed in a non-Hermitian mechanical lattice. Our work reveals flat-band phenomena unique to non-Hermitian systems and highlights new possibilities in quantum geometry and localization control.

This paper supercedes arXiv:2412.19034, which contains erraneous analyses and was posted prematurely. We apologize for any confusion and inconvenience

Quantum Physics (quant-ph); Other Condensed Matter (cond-mat.other); Classical Physics (physics.class-ph)

arXiv:2512.19745 [quant-ph]

(or arXiv:2512.19745v2 [quant-ph] for this version)

Full text under the publisher's open licence · 228 words

Related coverage