Llamas R G, Regalado L E
Appl Opt. 1996 Oct 1;35(28):5595-9. doi: 10.1364/AO.35.005595.
The transmitted scattered energy of plane electromagnetic waves from a thin metallic film with shallow rough interfaces bounded by two semi-infinite media is calculated. Both interfaces are modeled as independent stationary random processes with a Gaussian roughness spectrum. Scattering of light is calculated for both TM (p) or TE (s) polarizations for normal and oblique angles of incidence. An integral equation is obtained for the transmitted field based on the Rayleigh method and their solution involves Fourier coefficients, depending on the roughness profiles. We present some results for the case of a single thin metallic film in the attenuated total reflection configuration for s and p polarization around the angle of the excitation of surface-plasma waves θ(sp). The transmitted scattered intensity shows a maximum at the resonant angle θ(sp) in the case of p polarization.
计算了平面电磁波从具有浅粗糙界面的薄金属膜传输的散射能量,该薄金属膜由两种半无限介质界定。两个界面均被建模为具有高斯粗糙度谱的独立平稳随机过程。针对TM(p)或TE(s)偏振,计算了正入射和斜入射情况下的光散射。基于瑞利方法得到了透射场的积分方程,其解涉及取决于粗糙度轮廓的傅里叶系数。我们给出了在衰减全反射配置下,围绕表面等离子体波激发角θ(sp)的s和p偏振单薄金属膜情况的一些结果。在p偏振情况下,透射散射强度在共振角θ(sp)处出现最大值。