Valley degree of freedom in topological metamaterials: from microwaves in meta-waveguides to nanoscale surface graphene plasmons (Conference Presentation)

G. Shvets
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Abstract

Topological photonics enable us to design novel devices that exploit counter-intuitive propagation of electromagnetic waves. The key ingredient of topological photonics is a photonic topological insulator (PTI): a periodic structure that, in its bulk form, exhibits a propagation bandgap for a range of frequencies, yet supports localized edge states when interfaced with a different photonic structure exhibiting a bandgap for the same frequency range. Several types of PTIs emulating their respective condensed matter counterparts have already been proposed and experimentally demonstrated. One of the simplest PTIs exploits the valley degree of freedom in photonic crystals with a C_3 spatial symmetry. I will describe two examples of such structures: one designed and experimentally demonstrated at microwave frequencies and another designed for the mid-IR spectral range. We show that the microwave PTI structure, which is based on a metallic waveguide with an embedded array of specially designed metal rods, exhibits the previously unknown phenomenon of valley-protected “perfect” refraction: when interfaced with another waveguide, the edge states refract from the PTI metamaterial into the waveguide without any reflection. For the nanoscale topological metamaterial, we utilize graphene surface plasmons (GSPs) that propagate through a sheet of graphene with nano-patterned landscape of chemical potential. The chemical potential landscaping is achieved using an electrically biased metagate placed in close proximity of the graphene sheet. The advantage of this scheme is that the topological properties of the GSPs can be rapidly turned on and off, thus heralding the new era of active topological photonics on a nanoscale
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拓扑超材料中的谷自由度:从元波导中的微波到纳米级表面石墨烯等离子体(会议报告)
拓扑光子学使我们能够设计利用电磁波反直觉传播的新装置。拓扑光子学的关键成分是光子拓扑绝缘体(PTI):一种周期性结构,其本体形式在一定频率范围内表现出传播带隙,但当与具有相同频率范围带隙的不同光子结构界面时,支持局部边缘状态。几种类型的pti模拟各自的凝聚态对应物已经被提出和实验证明。其中最简单的pti利用了具有C_3空间对称性的光子晶体中的谷自由度。我将描述这种结构的两个例子:一个是在微波频率下设计和实验证明的,另一个是在中红外光谱范围内设计的。我们展示了微波PTI结构,该结构基于金属波导,嵌入了特殊设计的金属棒阵列,表现出以前未知的谷保护“完美”折射现象:当与另一个波导接口时,边缘状态从PTI超材料折射到波导中而没有任何反射。对于纳米级拓扑超材料,我们利用石墨烯表面等离子体(GSPs),其通过具有纳米化学势的石墨烯片传播。化学势美化是通过放置在石墨烯片附近的电偏置元栅来实现的。该方案的优点是gsp的拓扑特性可以快速打开和关闭,从而预示着纳米尺度上主动拓扑光子学的新时代
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