Guiding electromagnetic waves around sharp corners: topologically protected photonic transport in meta-waveguides (Presentation Recording)

G. Shvets, A. Khanikaev, Tzuhsuan Ma, K. Lai
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Abstract

Science thrives on analogies, and a considerable number of inventions and discoveries have been made by pursuing an unexpected connection to a very different field of inquiry. For example, photonic crystals have been referred to as “semiconductors of light” because of the far-reaching analogies between electron propagation in a crystal lattice and light propagation in a periodically modulated photonic environment. However, two aspects of electron behavior, its spin and helicity, escaped emulation by photonic systems until recent invention of photonic topological insulators (PTIs). The impetus for these developments in photonics came from the discovery of topologically nontrivial phases in condensed matter physics enabling edge states immune to scattering. The realization of topologically protected transport in photonics would circumvent a fundamental limitation imposed by the wave equation: inability of reflections-free light propagation along sharply bent pathway. Topologically protected electromagnetic states could be used for transporting photons without any scattering, potentially underpinning new revolutionary concepts in applied science and engineering. I will demonstrate that a PTI can be constructed by applying three types of perturbations: (a) finite bianisotropy, (b) gyromagnetic inclusion breaking the time-reversal (T) symmetry, and (c) asymmetric rods breaking the parity (P) symmetry. We will experimentally demonstrate (i) the existence of the full topological bandgap in a bianisotropic, and (ii) the reflectionless nature of wave propagation along the interface between two PTIs with opposite signs of the bianisotropy.
在尖角处引导电磁波:元波导中受拓扑保护的光子输运(演讲记录)
科学在类比中蓬勃发展,相当多的发明和发现是通过追求与一个非常不同的研究领域的意想不到的联系而取得的。例如,光子晶体被称为“光的半导体”,因为电子在晶格中的传播和光在周期性调制光子环境中的传播有着深远的相似之处。然而,电子行为的两个方面,它的自旋和螺旋度,一直没有被光子系统模拟,直到最近光子拓扑绝缘体(pti)的发明。这些光子学发展的动力来自于凝聚态物理中拓扑非平凡相的发现,这使得边缘态不受散射的影响。光子学中拓扑保护输运的实现将绕过波动方程所施加的一个基本限制:无反射光不能沿着急剧弯曲的路径传播。拓扑保护的电磁态可以用于传输光子而不产生任何散射,潜在地支持应用科学和工程中新的革命性概念。我将证明PTI可以通过应用三种类型的扰动来构建:(a)有限双各向异性,(b)陀螺磁包体破坏时间反转(T)对称性,以及(c)不对称棒破坏奇偶性(P)对称性。我们将通过实验证明(i)在双各向异性中存在完整的拓扑带隙,以及(ii)波沿着具有相反双各向异性符号的两个pti之间的界面传播的无反射性质。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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