Delocalization and higher-order topology in a nonlinear elastic lattice

Jianlin Yi, Changqing Chen
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Abstract

Topological elastic waves provide novel and robust ways for manipulating mechanical energy transfer and information transmission, with potential applications in vibration control, analog computation, and more. Recently discovered higher-order topological insulators (HOTIs) with multidimensional and hierarchical edge states can further expand the capabilities of topological elastic waves. However, the effects of nonlinearity on elastic HOTIs remain elusive. In this paper, we propose a nonlinear elastic higher-order topological Kagome lattice. After briefly reviewing its linear properties, we explore the effects of nonlinearity on the higher-order band topology and topological states. To do this, we have developed a method to calculate approximate nonlinear modes in order to identify the bulk polarization and probe the higher-order topological phase in the nonlinear lattice. We find that nonlinearity induces unusual delocalization of topological corner states, band crossing, and higher-order topological phase transition. The delocalization reveals that intracell hardening nonlinearity leads to direct delocalization of topological corner states while intracell softening nonlinearity first enhances and then reduces localization. The nonlinear higher-order topological phase is amplitude dependent, and we demonstrate a transition from a trivial to a non-trivial phase, enabling amplitude induced topological corner and edge states. Additionally, this phase transition corresponds to the closing and reopening of the bandgap, accompanied by an unusual band crossing. By examining the band topology before and after the band crossing, we find that the bulk polarization becomes quantized with respect to amplitude and can predict higher-order topological phases in nonlinear lattices. The obtained results are expected to be beneficial for the development of tunable and robust elastic wave devices.
非线性弹性晶格中的去焦化和高阶拓扑结构
拓扑弹性波为操纵机械能传递和信息传输提供了新颖而稳健的方法,有望应用于振动控制、模拟计算等领域。最近发现的具有多维和分层边缘状态的高阶拓扑绝缘体(HOTIs)可以进一步扩展拓扑弹性波的功能。然而,非线性对弹性 HOTIs 的影响仍然难以捉摸。在本文中,我们提出了一种非线性弹性高阶拓扑卡戈米晶格。在简要回顾其线性特性后,我们探讨了非线性对高阶带拓扑和拓扑状态的影响。为此,我们开发了一种计算近似非线性模式的方法,以识别体极化并探测非线性晶格中的高阶拓扑相。我们发现,非线性会诱发拓扑角态的异常脱ocalization、带交叉和高阶拓扑相变。去局域化表明,晶胞内硬化非线性导致拓扑角态直接去局域化,而晶胞内软化非线性则先增强后减弱局域化。非线性高阶拓扑相位与振幅有关,我们证明了从三阶相位到非三阶相位的过渡,从而实现了振幅诱导的拓扑角态和边态。此外,这种相位转换与带隙的关闭和重新打开相对应,并伴随着不寻常的带交叉。通过研究带越前后的带拓扑结构,我们发现体极化相对于振幅变得量子化,并能预测非线性晶格中的高阶拓扑相位。所获得的结果有望对开发可调谐且坚固耐用的弹性波器件大有裨益。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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