He Gao, Guoqiang Xu, Xue Zhou, Shuihua Yang, Zhongqing Su, Cheng-Wei Qiu
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引用次数: 0
Abstract
Topological Anderson phases (TAPs) offer intriguing transitions from ordered to disordered systems in photonics and acoustics. However, achieving these transitions often involves cumbersome structural modifications to introduce disorders in parameters, leading to limitations in flexible tuning of topological properties and real-space control of TAPs. Here, we exploit disordered convective perturbations in a fixed heat transport system. Continuously tunable disorder-topology interactions are enabled in thermal dissipation through irregular convective lattices. In the presence of a weak convective disorder, the trivial diffusive system undergos TAP transition, characterized by the emergence of topologically protected corner modes. Further increasing the strength of convective perturbations, a second phase transition occurs converting from TAP to Anderson phase. Our work elucidates the pivotal role of disorders in topological heat transport and provides a novel recipe for manipulating thermal behaviors in diverse topological platforms.
拓扑安德森相(TAPs)在光子学和声学领域提供了从有序系统到无序系统的有趣转变。然而,实现这些转变往往需要对结构进行繁琐的修改,以引入参数紊乱,从而限制了拓扑特性的灵活调整和 TAP 的真实空间控制。在这里,我们利用固定热传输系统中的无序对流扰动。通过不规则对流晶格,在热耗散过程中实现了连续可调的无序拓扑相互作用。在存在微弱对流无序的情况下,琐碎的扩散系统会发生拓扑安德森相变,其特征是出现拓扑保护角模式。进一步增加对流扰动的强度,就会发生从 TAP 相到安德森相的第二次相变。我们的工作阐明了紊乱在拓扑热传输中的关键作用,并为在各种拓扑平台中操纵热行为提供了新的方法。