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The Utility of an Impedance Boundary Condition in the Scattering of Light from One-Dimensional Randomly Rough Dielectric Surfaces

机译:阻抗边界条件在一维随机粗糙电介质表面光散射中的效用

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摘要

Local and nonlocal impedance boundary conditions have recently been obtained for p- and s-polarized electromagnetic fields at a one-dimensional, rough vacuum–metal interface defined by the equation x3 = (x1), when the plane of incidence is the x1x3-plane. The surface impedance appearing in these boundary conditions was obtained as an expansion in powers of the ratio of the optical skin depth of the metal at the frequency of the electromagnetic field to the local radius of curvature of the surface. In this paper, we apply these boundary conditions to computer simulation studies of the scattering of p- and s-polarized light from one-dimensional, randomly rough dielectric surfaces. These surfaces are characterized by dielectric constants that are real and positive rather than by complex dielectric constants with real parts that are negative and large in magnitude, as in the case of metal surfaces. Despite this difference, which leads to an “optical skin depth” that is now purely imaginary, comparisons of the results obtained by the use of these impedance boundary conditions with those obtained by formally exact computer simulation calculations show that the former are in very good quantitative agreement with the latter. Moreover, the computation time for such scattering calculations is reduced significantly by the use of an impedance boundary condition.
机译:最近,当入射平面为x1x3平面时,在方程式x3 =(x1)定义的一维粗糙真空-金属界面上获得了p和s极化电磁场的局部和非局部阻抗边界条件。 。在这些边界条件下出现的表面阻抗是通过金属在电磁场频率下的光学趋肤深度与表面局部曲率半径之比的幂扩展而获得的。在本文中,我们将这些边界条件应用于一维,随机粗糙电介质表面对p和s偏振光的散射的计算机模拟研究。这些表面的特征在于,介电常数为实数和正数,而不是像金属表面一样,其实数部分为负且幅值较大的复数介电常数。尽管存在这种差异,但现在导致的“光学趋肤深度”纯粹是虚构的,但将这些阻抗边界条件与通过正式精确的计算机模拟计算得出的结果进行比较后,发现前者的定量非常好与后者达成协议。此外,通过使用阻抗边界条件,大大减少了用于这种散射计算的计算时间。

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