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共振光子晶体衍射中拓扑极化缺陷的起源与守恒

Origins and conservation of topological polarization defects in resonant photonic-crystal diffraction.

作者信息

Yin Xuefan, Inoue Takuya, Peng Chao, Noda Susumu

机构信息

Department of Electronic Science and Engineering, Kyoto University, Kyoto-Daigaku-Katsura, Nishikyo-ku, Kyoto, 615-8510, Japan.

State Key Laboratory of Advanced Optical Communication Systems and Networks, School of Electronics, & Frontiers Science Center for Nano-optoelectronics, Peking University, Beijing, 100871, China.

出版信息

Nanophotonics. 2025 Jan 3;14(1):95-105. doi: 10.1515/nanoph-2024-0514. eCollection 2025 Jan.

Abstract

We present a continuative definition of topological charge to depict the polarization defects on any resonant diffraction orders in photonic crystal slab regardless they are radiative or evanescent. By using such a generalized definition, we investigate the origins and conservation of polarization defects across the whole Brillouin zone. We found that the mode crossings due to Brillouin zone folding contribute to the emergence of polarization defects in the entire Brillouin zone. These polarization defects eventually originate from the spontaneous symmetry breaking of line degeneracies fixed at Brillouin zone center or edges, or inter-band coupling caused by accidental Bloch band crossings. Unlike Bloch states, the polarization defects live and evolve in an unbound momentum space, obeying a local conservation law as a direct consequence of Stokes' theorem, but the total charge number is countless.

摘要

我们提出了拓扑电荷的连续定义,以描述光子晶体平板中任何共振衍射级次上的极化缺陷,无论它们是辐射的还是倏逝的。通过使用这种广义定义,我们研究了整个布里渊区极化缺陷的起源和守恒。我们发现,由于布里渊区折叠导致的模式交叉促成了整个布里渊区极化缺陷的出现。这些极化缺陷最终源于固定在布里渊区中心或边缘的线简并的自发对称性破缺,或由偶然的布洛赫能带交叉引起的带间耦合。与布洛赫态不同,极化缺陷在无界动量空间中存在和演化,作为斯托克斯定理的直接结果,它们服从局部守恒定律,但总电荷数是无穷的。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/6a2b/11744457/a1b8c2b3857c/j_nanoph-2024-0514_fig_001.jpg

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