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Imaginary-Stark Skin Effect

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arxiv 2404.16774 v3 pith:7GADKOUJ submitted 2024-04-25 quant-ph cond-mat.quant-gas

classification quant-phcond-mat.quant-gas
keywords nhseskinsystemseffectissenon-hermitianboundaryeigenstates
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A unique phenomenon in non-Hermitian systems is the non-Hermitian skin effect (NHSE), namely the boundary localization of continuous-spectrum eigenstates. However, studies on the NHSE in systems without translational invariance are still limited. Here, we unveil a new class of NHSE, dubbed the imaginary-Stark skin effect (ISSE), in a one-dimensional lossy lattice with a spatially increasing loss rate. This ISSE is beyond the framework of non-Bloch band theory and exhibits intriguing properties significantly different from the conventional NHSE. Specifically, the energy spectrum of our model has a T-shaped feature, with approximately half of the eigenstates localized at the left boundary. Furthermore, each skin mode can be expressed as a single stable, exponentially-decaying wave within the bulk region. Such peculiar behaviors are analyzed via the transfer-matrix method, whose eigendecomposition quantifies the formation of the ISSE. Our work provides new insights into the NHSE in systems without translational symmetry and contributes to the understanding of 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. Fate of moir\'e flat bands for a weakly repulsive Bose-Einstein condensate in one-dimensional $\mathcal{PT}$-symmetric bichromatic optical lattices

    cond-mat.quant-gas 2026-08 conditional novelty 7.0 of 10

    In a PT-symmetric 1D moiré lattice, the parity of the denominator q controls which bands first break PT symmetry and whether the lowest flat band broadens monotonically or nonmonotonically; weak interactions shift but...

  2. Versatile Control of Nonlinear Topological States in Non-Hermitian Systems

    quant-ph 2024-11 conditional novelty 6.0 of 10

    Nonlinear hopping in both the Hermitian and non-Hermitian halves of a topological interface lattice fully delocalizes the zero mode and allows its profile to be designed arbitrarily.

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