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Speckle correlations in the light scattered by a dielectric film with a rough surface: Guided wave effects

机译:具有粗糙表面的介电膜散射的光中的斑点相关性:导波效应

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Diagrammatic perturbation theory is used to compute the angular intensity correlation function C(q,kq',k')=[[I(qk)-[I(qk)]][I(q'k')-[I(q'k')]] for s-polarized light scattered from a dielectric film on a perfectly conducting substrate. The scattering system supports two or more guided waves. The illuminated surface of the film is a weakly rough, one-dimensional random surface, I(qk) is the squared modulus of the scattering matrix for the system, and q,q' and k,k' are the projections on the mean scattering surface of the wave vectors of the scattered and incident light, respectively. Contributions to C include (a) short-range memory effect and time-reversed memory effect terms associated with the resonant excitation of the guided waves in the film, C-(1); (b) an additional short-range term of comparable magnitude C-(10); (c) a long-range term C-(2); (d) an infinite-range term C-(3); and (e) a term C-(1.5) that, along with C-(2), displays peaks associated with the excitation of guided waves. In contrast with the results obtained in the scattering of light from the random surface of a semi-infinite medium, interesting features arise in the speckle correlators in the present system due to the existence of the guided waves, such as various satellite peaks and a large multiplicity of resonant features. Both C-(1) and C-(2) exhibit additional peaks whose positions depend on the difference between the wave numbers of two guided waves (the most interesting case of peaks arising from guided waves), whereas C-(1.5) exhibits additional peaks whose positions depend only on the wave numbers of the guided waves taken individually. [References: 29]
机译:图解扰动理论用于计算角强度相关函数C(q,k q',k')= [[I(q k)-[I(q k)]] [I(q' k ')-[I(q' k')]]用于从理想导电基板上的介电膜散射的s偏振光。散射系统支持两个或多个导波。薄膜的照射表面是弱粗糙的一维随机表面,I(q k)是系统散射矩阵的平方模,而q,q'和k,k'是在系统上的投影。散射光和入射光的波矢量的平均散射面。对C的贡献包括:(a)与胶片中导波的共振激发相关的短程记忆效应和时间反转记忆效应项C-(1); (b)可比幅度为C-(10)的另一个短期术语; (c)长期C-(2); (d)无限范围项C-(3); (e)术语C-(1.5)与C-(2)一起显示与导波激发相关的峰值。与从半无限介质的随机表面散射光获得的结果相反,在本系统中的散斑相关器中由于导波的存在而出现了有趣的特征,例如各种卫星峰值和较大的导波。共振特征的多样性。 C-(1)和C-(2)均显示其他峰,其位置取决于两个导波的波数之间的差异(最有趣的情况是由导波产生的峰),而C-(1.5)则显示附加峰峰的位置仅取决于单独获取的导波的波数。 [参考:29]

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