The field distribution in a finite number of nanostructured metal waveguide arrays

X. Shi, Wu Yang, H. Xing, Xiaoshuang Chen
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Abstract

We investigative the field distribution in nanostructured metal waveguide arrays. Firstly, we analyze a simple discrete system containing two adjacent metallic waveguides (N=2). The propagation constants β1 and β2 can be calculated by a rigorous field analysis approach. According to the supermode theory of conventional dielectric waveguide arrays, we can also obtain the expressions of propagation constants. So we can obtain the coupling constant and the perturbation constant of the expressions in the supermode theory. Next, we consider a system that contains five adjacent metal waveguides (N=5). The propagation constants and the wavefunctions of the supermodes can be obtained according to the coupling constant, the perturbation constant, and the supermode theory. The incident light is located at the input of the 4st waveguide. The initial excited field can be expressed as a sum of supermodes. The total field is formed by the superposition of supermodes. The variation of field amplitude with propagation distance is obtained and can predict the precise positions of the field distribution. To demonstrate the analytical results, we numerically simulate the field distribution in the waveguides (N=5) constructed with silver by the finite-difference time-domain method. The numerical simulation results show a good agreement with theoretical expectations.
有限数量纳米结构金属波导阵列中的场分布
研究了纳米结构金属波导阵列中的场分布。首先,我们分析了一个包含两个相邻金属波导(N=2)的简单离散系统。通过严格的场分析方法可以计算出传输常数β1和β2。根据传统介质波导阵列的超模理论,我们也可以得到其传播常数的表达式。从而得到了超模理论表达式的耦合常数和摄动常数。接下来,我们考虑一个包含五个相邻金属波导(N=5)的系统。根据耦合常数、微扰常数和超模理论,可以得到超模的传播常数和波函数。入射光位于第4个波导的输入端。初始激发场可以表示为超模的和。总场是由超模的叠加形成的。得到了场振幅随传播距离的变化规律,可以预测场分布的精确位置。为了证明分析结果,我们用时域有限差分法数值模拟了银构成的波导(N=5)中的场分布。数值模拟结果与理论预期吻合较好。
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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