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首页> 外文期刊>Physical review, E. Statistical physics, plasmas, fluids, and related interdisciplinary topics >Diffusing-light spectroscopies beyond the diffusion limit: The role of ballistic transport and anisotropic scattering
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Diffusing-light spectroscopies beyond the diffusion limit: The role of ballistic transport and anisotropic scattering

机译:漫射光谱超出漫射极限:弹道传输和各向异性散射的作用

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摘要

Diffuse transmission and diffusing-wave spectroscopy (DWS) can be used to probe the structure and dynamics of opaque materials such as colloids, foams, and sand. A crucial step is to model photon transport as a diffusion process. This approach is acceptable for optically thick samples, far into the limit of strong multiple scattering; however, it becomes increasingly inaccurate for thinner samples for several reasons. Here, we correct for two of these defects. By modeling photon propagation by a telegrapher equation with suitable boundary conditions, we can account for the ballistic transport of photons at finite speed between successive scattering events. By introducing a discontinuity in the photon concentration at the source point, and then averaging over a range of penetration depths, we can account for the fact that photons usually scatter anisotropically into the forward direction, rather than being completely randomized at each event. The accuracy of our approach is tested by comparison both with random walk computer simulations and with experiments on specially designed suspensions of polystyrene spheres. We find that our predictions extend the utility of diffuse transmission to slabs of all thicknesses and of DWS to slabs down to about two transport mean free paths. [References: 36]
机译:漫透射和散射波谱(DWS)可用于探测不透明材料(例如胶体,泡沫和沙子)的结构和动力学。至关重要的一步是将光子传输建模为扩散过程。这种方法对于光学上较厚的样品是可以接受的,远不能达到强多次散射的极限。但是,由于以下几个原因,对于更薄的样品它变得越来越不准确。在这里,我们纠正了其中两个缺陷。通过用具有适当边界条件的电报方程式对光子的传播进行建模,我们可以解释连续散射事件之间光子在有限速度下的弹道传输。通过在源点引入光子浓度的不连续性,然后在穿透深度范围内取平均值,我们可以解释一个事实,即光子通常各向异性地向正方向散射,而不是在每次事件时都被完全随机化。通过与随机游走计算机模拟和专门设计的聚苯乙烯球体悬浮液进行比较,测试了我们方法的准确性。我们发现,我们的预测将扩散传输的效用扩展到了所有厚度的平板上,将DWS扩展到了大约两个传输平均自由程的平板上。 [参考:36]

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