Chen Xiao-Dong, Gao Zi-Xuan, Cui Xiaohan, Mo Hao-Chang, Chen Wen-Jie, Zhang Ruo-Yang, Chan C T, Dong Jian-Wen
School of Physics & State Key Laboratory of Optoelectronic Materials and Technologies, <a href="https://ror.org/0064kty71">Sun Yat-sen University</a>, Guangzhou 510275, China.
Department of Physics, <a href="https://ror.org/00q4vv597">The Hong Kong University of Science and Technology</a>, Hong Kong, China.
Phys Rev Lett. 2024 Sep 27;133(13):133802. doi: 10.1103/PhysRevLett.133.133802.
Disorder, which is ubiquitous in nature, has been extensively explored in photonics for understanding the fundamental principles of light diffusion and localization, as well as for applications in functional resonators and random lasers. Recently, the investigation of disorder in topological photonics has led to the realization of topological Anderson insulators characterized by an unexpected disorder-induced phase transition. However, the observed photonic topological Anderson insulators so far are limited to the time-reversal symmetry breaking systems. Here, we propose and realize a photonic quantum spin Hall topological Anderson insulator without breaking time-reversal symmetry. The disorder-induced topological phase transition is comprehensively confirmed through the theoretical effective Dirac Hamiltonian, numerical analysis of bulk transmission, and experimental examination of bulk and edge transmissions. We present convincing evidence for the unidirectional propagation and robust transport of helical edge modes, which are the key features of nontrivial time-reversal invariant topological Anderson insulators. Furthermore, we demonstrate disorder-induced beam steering, highlighting the potential of disorder as a new degree of freedom to manipulate light propagation in magnetic-free systems. Our work not only paves the way for observing unique topological photonic phases but also suggests potential device applications through the utilization of disorder.
无序在自然界中无处不在,在光子学领域已得到广泛研究,用于理解光扩散和局域化的基本原理,以及在功能谐振器和随机激光器中的应用。最近,对拓扑光子学中无序的研究导致了拓扑安德森绝缘体的实现,其特征是由意外的无序诱导相变。然而,迄今为止观察到的光子拓扑安德森绝缘体仅限于时间反演对称性破缺系统。在此,我们提出并实现了一种不破时间反演对称性的光子量子自旋霍尔拓扑安德森绝缘体。通过理论有效的狄拉克哈密顿量、体传输的数值分析以及体传输和边缘传输的实验检验,全面证实了无序诱导的拓扑相变。我们提供了令人信服的证据,证明了螺旋边缘模式的单向传播和稳健传输,这是非平凡时间反演不变拓扑安德森绝缘体的关键特征。此外,我们展示了无序诱导的光束转向,突出了无序作为在无磁系统中操纵光传播的新自由度的潜力。我们的工作不仅为观察独特的拓扑光子相铺平了道路,还通过利用无序暗示了潜在的器件应用。