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中文摘要: 当电磁波在周期性介质中传播时,会因布拉格散射形成电磁波禁带,导致电磁波在一定的频率范围内不能传播。为解决上述问题,在空气背景下以氧化铝材料构建了两种不同类型的正方晶格,利用有限元法求解了三种不同光子晶体的能带,其中两种是由第一种滑移操作得来的;然后通过对两种不同类型的晶格进行拼接,构建超元胞,最终实现了拓扑边缘态;通过分析单晶格元胞能带,总结出拓扑边缘态形成的位置原因,提出的该方法形成的拓扑边缘态能对电磁波通过的频率进行相应的调控,为可调微波器件提供了新颖的设计思路。
Abstract:When electromagnetic waves propagate in periodic media, they cannot propagate in a certain frequency range due to the bandgap of electromagnetic waves formed by Bragg scattering. In order to solve the above problem, two different types of square lattice are constructed with alumina material under the background of air, and the energy bands of three different photonic crystals are solved by the finite element method. Two of them are derived from the first sliding operation; Then, by splicing two different types of lattices, the supercell is constructed, and the topological edge state is finally realized. By analyzing the single lattice cell energy band, the position reason for topological edge state formation is summarized, and the topological edge state formed by the proposed method can regulate the passing frequency of electromagnetic wave accordingly, which provides a novel design idea for tunable microwave devices.
keywords: photonic crystal band structure edge state electromagnetic wave regulation tetragonal lattice
文章编号:20250405 中图分类号:O539; TP61+2.4 文献标志码:A
基金项目:国家重点基础研究发展计划(2022YFE0204100)
引用文本:
刘子逸,李健飞,陈晨,姚静锋,袁承勋.滑移晶格引导的拓扑边缘态[J].飞控与探测,2025,8(4):37-42.
刘子逸,李健飞,陈晨,姚静锋,袁承勋.滑移晶格引导的拓扑边缘态[J].飞控与探测,2025,8(4):37-42.

