基板上石墨烯带状光栅的h偏振太赫兹波散射:电磁感应透明

Fedir O. Yevtushenko
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引用次数: 0

摘要

本文用数值方法分析了有限厚度介质衬底上的石墨烯无限光栅对h偏振平面波的散射和吸收。全波处理是基于解析半反演,借助黎曼-希尔伯特问题的显式解进行的。所得结果为Floquet谐波幅值的Fredholm第二类无限矩阵方程。因此,相应的代码是无网格的,具有保证的收敛性。数值结果表明,当带材宽度和周期为微尺度时,这种超表面表现出复杂的频率选择行为。也就是说,存在三种具有不同q因子的自然模式类型:衬底模式、等离子体带模式和晶格模式。如果衬底不存在,则后一种模式不存在,并且可以具有超高的q因子。由于石墨烯的导电性取决于其化学势,因此这种超表面的透明度和反射率可以在很宽的范围内调节。然而,在晶格模式共振中,可调性被破坏。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
H-Polarized Terahertz Wave Scattering from On-Substrate Graphene Strip Grating: Electromagnetically Induced Transparency
We analyze numerically the H-polarized plane wave scattering and absorption by an infinite grating of flat graphene strips lying on a dielectric substrate of finite thickness. The full-wave treatment is based on the analytical semi-inversion, performed with the aid of explicit solution of the Riemann-Hilbert Problem. The result of this procedure is a Fredholm second-kind infinite matrix equation for the Floquet harmonic amplitudes. Thus, the corresponding code is meshless and has a guaranteed convergence. Numerical results show that if the strip width and periodicity have microsize dimensions such a metasurface demonstrates complicated frequency-selective behavior. Namely, three natural mode types with different Q-factors are present: substrate modes, plasmon strip modes, and lattice modes. The latter modes do not exist if the substrate is absent and can have ultra-high Q-factors. As graphene’s conductivity depends on its chemical potential, the transparency and reflectivity of such a metasurface can be tuned in wide range. However, the tunability is spoiled at the lattice-mode resonances.
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