Mandal Subhaskar, Wang Ziyao, Banerjee Rimi, Teo Hau Tian, Wei Minggui, Zhou Peiheng, Xi Xiang, Gao Zhen, Liu Gui-Geng, Zhang Baile
Department of Physics, Indian Institute of Technology Bombay, Mumbai 400076, India.
Nanyang Technological University, Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Singapore 637371, Singapore.
Phys Rev Lett. 2025 Jul 2;135(1):016903. doi: 10.1103/33mm-mx88.
Photonic Chern insulators can be implemented in gyromagnetic photonic crystals with broken time-reversal (TR) symmetry. They exhibit gapless chiral edge states (CESs), enabling unidirectional propagation and demonstrating exceptional resilience to localization even in the presence of defects or disorders. However, when two Chern insulators with opposite Chern numbers are stacked together, this one-way nature can be nullified, causing the originally gapless CESs to become gapped. Recent theoretical works have proposed achieving such a topological phase transition in condensed matter systems using antiferromagnetic thin films such as MnBi_{2}Te_{4} or by coupling two quantum spin/anomalous Hall insulators, but these approaches have yet to be realized experimentally. In a bilayer gyromagnetic photonic crystal arranged in an antiferromagnetic layer configuration, our experimental observations reveal that interlayer coupling initiates a transition from a Chern insulating phase to a higher-order topological phase. This transition results in the gapping of CESs and triggers the emergence of corner states within the band gap. The corner mode energy within this gap originates from CES interactions, forming a Jackiw-Rebbi-type topological domain wall mode at the corner, which is expected to remain within the bulk band gap without relying on local symmetries such as chiral or particle-hole symmetry. These states exhibit heightened resilience against defects, distinguishing them from their TR-symmetric counterparts.
光子陈绝缘体可以在具有破时间反演(TR)对称性的旋磁光子晶体中实现。它们表现出无隙手性边缘态(CESs),实现单向传播,并且即使在存在缺陷或无序的情况下也表现出对局域化的非凡抗性。然而,当两个具有相反陈数的陈绝缘体堆叠在一起时,这种单向性质可能会消失,导致原本无隙的CESs出现能隙。最近的理论工作提出在凝聚态系统中使用诸如MnBi₂Te₄之类的反铁磁薄膜或通过耦合两个量子自旋/反常霍尔绝缘体来实现这种拓扑相变,但这些方法尚未通过实验实现。在以反铁磁层配置排列的双层旋磁光子晶体中,我们的实验观察表明,层间耦合引发了从陈绝缘相到高阶拓扑相的转变。这种转变导致CESs出现能隙,并在带隙内触发角态的出现。该能隙内的角模式能量源自CES相互作用,在角处形成一种杰克维-雷比(Jackiw-Rebbi)型拓扑畴壁模式,预计该模式将保留在体能隙内,而不依赖于诸如手性或粒子-空穴对称性等局部对称性。这些态对缺陷表现出更高的抗性,这使它们与TR对称的对应物有所区别。