部分石墨烯覆盖的圆形介电丝在e偏振平面波散射和吸收中的非等离子体共振

Iryna O. Mikhailikova, Sergii V. Dukhopelnykov, R. Sauleau
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引用次数: 0

摘要

我们分析了在e偏振平面波照射下,圆形介质杆的总散射截面(TSCS)和吸收截面(ACS)是如何被任意角宽和化学势的共形石墨烯条所改变的。在我们处理的核心,有一个对偶级数方程其中未知的是场角傅里叶谐波。我们对这个方程进行离散傅里叶反变换(IDFT),得到一个Fredholm第二类矩阵方程。该方法保证了所得数值结果的收敛性。我们给出了归一化的TSCS和ACS与石墨烯条的角宽度和从静态到1thz范围内的频率的关系。这些图令人信服地表明,由于石墨烯的导电性的可调性,所考虑的散射体的最低非等离子体自然模式上的共振仍然是可调谐的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Non-Plasmon Resonances in the E-polarized Plane Wave Scattering and Absorption by a Circular Dielectric Wire with Partial Graphene Cover
We analyze how the total scattering cross-section (TSCS) and absorption cross-section (ACS) of a circular dielectric rod, illuminated with the E-polarized plane wave, is modified by a conformal graphene strip of arbitrary angular width and chemical potential. In the core of our treatment, there is a dual series equation where the unknown are the field angular Fourier harmonics. We subject this equation to the Inverse Discrete Fourier Transform (IDFT) that yields a Fredholm second kind matrix equation. Such a procedure guarantees the convergence of the obtained numerical results. We present the normalized TSCS and ACS versus the angular width of graphene strip and the frequency in the range from the statics to 1 THz. These plots convincingly demonstrate that the resonances on the lowest non-plasmon natural modes of the considered scatterer are still tunable due to the tunability of graphene's conductivity.
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