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首页> 外文期刊>Optics Communications: A Journal Devoted to the Rapid Publication of Short Contributions in the Field of Optics and Interaction of Light with Matter >SCATTERING OF LIGHT FROM A THIN METALLIC FILM WITH A SHALLOW RANDOM ROUGH SURFACE BETWEEN DISSIMILAR MEDIA .1. THEORY
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SCATTERING OF LIGHT FROM A THIN METALLIC FILM WITH A SHALLOW RANDOM ROUGH SURFACE BETWEEN DISSIMILAR MEDIA .1. THEORY

机译:异质介质之间具有浅随机粗糙表面的薄金属膜发出的光的散射1。理论

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The reflected field scattered from a thin metallic film with a shallow rough random surface bounded by two semi-infinite dissimilar optical media is calculated. The model assumes that all media are homogeneous, isotropic, non-magnetic, linear and may be characterized by a frequency dependent complex dielectric function. The Rayleigh hypothesis is used to obtain an independent integral equation relating the amplitudes of the reflected fields to the incident wave. This treatment is valid for both TM(p) or TE(s) polarizations. Numerical results are obtained by assuming a Gaussian roughness spectrum for the random rough surface and the formalism is applied to simulate the scattering in the ATR-Kretschmann configuration, allowing the excitation of surface plasmons (SP), prism-metal-air. The angular dependence of the incoherent scattering shows two enhancement peaks, in addition to the well known backscattering effect. The angular positions of these two peaks are about the angle of excitation of SP (+/- theta(sp)) and are independent of the angle of incidence theta(i). They appear only for p-polarized light and are due to single-scattering effects. When theta(i) is tuned at exactly -theta(sp) the enhanced backscattering peak is screened by the peak located at this angle and the background incoherent scattering is two orders of magnitude higher for the same response computed for all other angles of incidence theta(i). (C) 1997 Elsevier Science B.V. [References: 20]
机译:计算从薄金属薄膜散射的反射场,该薄膜具有由两个半无限不同光学介质界定的浅粗糙随机表面。该模型假定所有介质都是均匀的,各向同性的,非磁性的,线性的,并且可以通过频率相关的复介电函数来表征。瑞利假设用于获得一个独立的积分方程,该方程将反射场的振幅与入射波相关联。此处理对TM(p)或TE(s)极化均有效。数值结果是通过假设随机粗糙表面的高斯粗糙度谱获得的,并且形式化用于模拟ATR-Kretschmann配置中的散射,从而允许激发表面等离激元(SP),棱镜-金属-空气。除众所周知的反向散射效应外,非相干散射的角度依赖性还显示出两个增强峰。这两个峰的角位置大约是SP的激发角(+/- theta(sp)),与入射角theta(i)无关。它们仅对于p偏振光出现,并且是由于单散射效应。当theta(i)精确调整为-theta(sp)时,增强的反向散射峰将被位于该角度的峰屏蔽,并且对于所有其他入射角theta计算出的相同响应,背景非相干散射要高两个数量级。 (一世)。 (C)1997 Elsevier Science B.V. [参考:20]

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