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非厄米趋肤效应的数学基础

Mathematical Foundations of the Non-Hermitian Skin Effect.

作者信息

Ammari Habib, Barandun Silvio, Cao Jinghao, Davies Bryn, Hiltunen Erik Orvehed

机构信息

Department of Mathematics, ETH Zürich, Rämistrasse 101, 8092 Zürich, Switzerland.

Department of Mathematics, Imperial College London, 180 Queen's Gate, London, SW7 2AZ UK.

出版信息

Arch Ration Mech Anal. 2024;248(3):33. doi: 10.1007/s00205-024-01976-y. Epub 2024 Apr 6.

DOI:10.1007/s00205-024-01976-y
PMID:38989293
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11233337/
Abstract

We study the skin effect in a one-dimensional system of finitely many subwavelength resonators with a non-Hermitian imaginary gauge potential. Using Toeplitz matrix theory, we prove the condensation of bulk eigenmodes at one of the edges of the system. By introducing a generalised (complex) Brillouin zone, we can compute spectral bands of the associated infinitely periodic structure and prove that this is the limit of the spectra of the finite structures with arbitrarily large size. Finally, we contrast the non-Hermitian systems with imaginary gauge potentials considered here with systems where the non-Hermiticity arises due to complex material parameters, showing that the two systems are fundamentally distinct.

摘要

我们研究了具有非厄米虚规范势的有限多个亚波长谐振器的一维系统中的趋肤效应。利用托普利兹矩阵理论,我们证明了体态本征模在系统的一条边缘处发生凝聚。通过引入广义(复)布里渊区,我们可以计算相关无限周期结构的能带,并证明这是任意大尺寸有限结构光谱的极限。最后,我们将这里考虑的具有虚规范势的非厄米系统与由于复材料参数而产生非厄米性的系统进行对比,表明这两个系统在本质上是不同的。

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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/84c6/11233337/7f6cbb1c583d/205_2024_1976_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/84c6/11233337/0e542039ba0e/205_2024_1976_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/84c6/11233337/a5d2cb87c44f/205_2024_1976_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/84c6/11233337/d926d55fbe3c/205_2024_1976_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/84c6/11233337/726366d30210/205_2024_1976_Fig9_HTML.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/84c6/11233337/85fb9f9ca2c6/205_2024_1976_Fig11_HTML.jpg

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本文引用的文献

1
Imaginary Gauge Transformation in Momentum Space and Dirac Exceptional Point.动量空间中的虚规范变换与狄拉克例外点
Phys Rev Lett. 2022 Dec 9;129(24):243901. doi: 10.1103/PhysRevLett.129.243901.
2
Non-Hermitian Physics without Gain or Loss: The Skin Effect of Reflected Waves.无增益或损耗的非厄米物理:反射波的趋肤效应。
Phys Rev Lett. 2022 Aug 19;129(8):086601. doi: 10.1103/PhysRevLett.129.086601.
3
Non-Hermitian morphing of topological modes.非厄米拓扑模的变形。
Nature. 2022 Aug;608(7921):50-55. doi: 10.1038/s41586-022-04929-1. Epub 2022 Aug 3.
4
Observation of non-Hermitian topology and its bulk-edge correspondence in an active mechanical metamaterial.活性机械超材料中非厄米拓扑及其体边对应关系的观测
Proc Natl Acad Sci U S A. 2020 Nov 24;117(47):29561-29568. doi: 10.1073/pnas.2010580117. Epub 2020 Nov 9.
5
Topological Origin of Non-Hermitian Skin Effects.非厄米趋肤效应的拓扑起源
Phys Rev Lett. 2020 Feb 28;124(8):086801. doi: 10.1103/PhysRevLett.124.086801.
6
Non-Hermitian Boundary Modes and Topology.非厄米边界模式与拓扑结构。
Phys Rev Lett. 2020 Feb 7;124(5):056802. doi: 10.1103/PhysRevLett.124.056802.
7
Parity-time symmetry and exceptional points in photonics.光子学中的宇称-时间对称性与奇异点
Nat Mater. 2019 Aug;18(8):783-798. doi: 10.1038/s41563-019-0304-9. Epub 2019 Apr 8.
8
Edge Modes, Degeneracies, and Topological Numbers in Non-Hermitian Systems.非厄米系统中的边缘模式、简并度和拓扑数
Phys Rev Lett. 2017 Jan 27;118(4):040401. doi: 10.1103/PhysRevLett.118.040401. Epub 2017 Jan 23.
9
Robust light transport in non-Hermitian photonic lattices.非厄米光子晶格中的稳健光传输。
Sci Rep. 2015 Aug 28;5:13376. doi: 10.1038/srep13376.
10
Localization Transitions in Non-Hermitian Quantum Mechanics.非厄米量子力学中的局域化转变
Phys Rev Lett. 1996 Jul 15;77(3):570-573. doi: 10.1103/PhysRevLett.77.570.