散斑/湍流的非包裹相位分布模型

D. Draper, J. Holmes, J. Peacock
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引用次数: 1

摘要

对于由相干光束和漫射物体产生的散斑场,以及通过随机介质(如晴空湍流)传播的相干光束,已经提出了几种相位概率密度函数(p.d.f)模型。由于这些模型是基于从代表辐射的复杂场振幅中提取相位信息,因此给出了散斑的p.d.f.模型和许多湍流的p.d.f.模型。包裹相位指的是限定在主值(0-2π弧度)内的相位角。相位波动实际上代表了光程长度的变化,当以相位变化表示时,光程长度的变化可以大大超过2π。路径长度变化与未包裹的相位变化线性相关,其中ϕ = 2πΔL/λ其中ΔL表示路径长度变化。因此,在现实情况下,阶段并不局限于主要价值。此外,包装的p.d.f.表达式在数学上是复杂的,很难将它们扩展到散斑场和湍流场组合的情况下(即。其中散斑场通过湍流传播)。因此,我们提出了单独散斑和单独湍流的简单高斯解包裹相p.d.f.模型,以及湍流中使用更简单解包裹模型的组合散斑场模型。我们将用一种标准的技术从一个未包裹的p.d.f5计算包裹的p.d.f,从未包裹的高斯模型得到的包裹的p.d.f近似等价于已知的散斑相位的包裹p.d.f。从我们的实验工作中也可以看出,测量的解包裹相位近似为高斯相位。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
An Unwrapped Phase Distribution Model for Speckle/Turbulence
Several models have been proposed for the probability density function (p.d.f.) of phase for a speckle field created by a coherent beam and a diffuse object1-5 and also for a coherent beam propagating through a random medium such as clear air turbulence6-7. The p.d.f. models for speckle as well as many of the p.d.f. models for turbulence are given for the wrapped phase since the models are based on extracting phase information from the complex field amplitudes representing the radiation. Wrapped phase refers to phase angles that are limited to principal values (0-2π radians). The phase fluctuations really represent the optical path length variations which can greatly exceed 2π when represented as phase changes. Path length variations are linearly related to unwrapped phase variations by the relationship ϕ = 2πΔL/λ where ΔL represents path length variations. Consequently in a realistic situation phase is not limited to principal values. In addition the wrapped p.d.f. expressions are mathematically complicated and it would be difficult to extend them to the case where a speckle field and a turbulence field are combined (ie. where a speckle field is propagating through turbulence). Consequently simple Gaussian unwrapped phase p.d.f. models for both speckle alone and turbulence alone and a model for the combined speckle field in turbulence using the simpler unwrapped models are proposed. It will be shown using a standard technique for calculating a wrapped p.d.f. from an unwrapped p.d.f5 that the wrapped p.d.f.’s obtained from unwrapped Gaussian models are approximately equivalent to the known wrapped p.d.f.’s for speckle phase. It will also be shown from our experimental work that the measured unwrapped phase is approximately Gaussian.
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