STABILITY OF THE NON-HERMITIAN SKIN EFFECT IN ONE DIMENSION

被引:0
|
作者
Ammari, Habib [1 ]
Barandun, Silvio [1 ]
Davies, Bryn [2 ]
Hiltunen, Erik Orvehed [3 ]
Liu, Ping [4 ]
机构
[1] Swiss Fed Inst Technol, Dept Math, Ramistr 101, CH-8092 Zurich, Switzerland
[2] Imperial Coll London, Dept Math, 180 Queens Gate, London SW7 2AZ, England
[3] Univ Oslo, Dept Math, Postboks 1053, N-0316 Oslo, Norway
[4] Zhejiang Univ, Sch Math Sci, Hangzhou 310058, Zhejiang, Peoples R China
基金
瑞士国家科学基金会; 英国工程与自然科学研究理事会;
关键词
non-Hermitian systems; non-Hermitian skin effect; subwavelength resonators; imaginary gauge potential; Toeplitz matrix; eigenvector condensation; Anderson localization; stability analysis; disorder-induced phase transition; EIGENVALUES; MATRICES;
D O I
10.1137/23M1610537
中图分类号
O29 [应用数学];
学科分类号
070104 ;
摘要
This paper shows both analytically and numerically that the skin effect in systems of non-Hermitian subwavelength resonators is robust with respect to random imperfections in the system. The subwavelength resonators are highly contrasting material inclusions that resonate in a low-frequency regime. The non-Hermiticity is due to the introduction of a directional damping term (motivated by an imaginary gauge potential), which leads to a skin effect that is manifested by the system's eigenmo des accumulating at one edge of the structure. We elucidate the topological protection of the associated (real) eigenfrequencies and illustrate numerically the competition between the two different localization effects present when the system is randomly perturbed: the non-Hermitian skin effect and the disorder-induced Anderson localization. We show numerically that, as the strength of the disorder increases, more and more eigenmo des become localized in the bulk. Our results are based on an asymptotic matrix model for subwavelength physics and can be generalized also to tight-binding models in condensed matter theory.
引用
收藏
页码:1697 / 1717
页数:21
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