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在旋磁光子晶体中实现四极拓扑绝缘体相

Realization of a quadrupole topological insulator phase in a gyromagnetic photonic crystal.

作者信息

Zhou Peiheng, Liu Gui-Geng, Wang Zihao, Li Shuwei, Xie Qindong, Zhang Yunpeng, Mandal Subhaskar, Xi Xiang, Gao Zhen, Deng Longjiang, Zhang Baile

机构信息

National Engineering Research Center of Electromagnetic Radiation Control Materials, Key Laboratory of Multi-spectral Absorbing Materials and Structures of Ministry of Education, University of Electronic Science and Technology of China, Chengdu 611731, China.

Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore 637371, Singapore.

出版信息

Natl Sci Rev. 2024 Apr 1;11(11):nwae121. doi: 10.1093/nsr/nwae121. eCollection 2024 Nov.

Abstract

The field of topological photonics was initiated with the realization of a Chern insulator phase in a gyromagnetic photonic crystal (PhC) with broken time-reversal symmetry (), hosting chiral edge states that are topologically protected propagating modes. Along a separate line of research, a quadrupole topological insulator was the first higher-order topological phase supporting localized corner states, but has been so far limited to -invariant systems, as is a key ingredient in early models. Here we report the realization of a quadrupole topological insulator phase in a gyromagnetic PhC, as a consequence of topological phase transition from the previously demonstrated Chern insulator phase. The phase transition has been demonstrated with microwave measurements, which characterize the evolution from propagating chiral edge states to localized corner states. We also demonstrate the migration of topological boundary states into the continuum, when the gyromagnetic PhC is magnetically tuned. These results extend the quadrupole topological insulator phase into -broken systems, and integrate topologically protected propagating and localized modes in a magnetically tunable photonic crystal platform.

摘要

拓扑光子学领域始于在具有破时间反演对称性的旋磁光子晶体(PhC)中实现陈绝缘体相,该晶体拥有作为拓扑保护传播模式的手性边缘态。沿着另一条研究路线,四极拓扑绝缘体是首个支持局域角态的高阶拓扑相,但迄今为止仅限于具有Z2不变性的系统,因为Z2是早期模型中的关键要素。在此,我们报告在旋磁光子晶体中实现了四极拓扑绝缘体相,这是从先前证明的陈绝缘体相进行拓扑相变的结果。该相变已通过微波测量得到证明,这些测量表征了从传播的手性边缘态到局域角态的演化。当对旋磁光子晶体进行磁调谐时,我们还展示了拓扑边界态向连续态的迁移。这些结果将四极拓扑绝缘体相扩展到具有破Z2对称性的系统中,并在一个磁可调谐光子晶体平台中整合了拓扑保护的传播模式和局域模式。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ec60/11493087/3821c4240840/nwae121fig1.jpg

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