Ramakrishna S A, Kumar N
Raman Research Institute, Sadashivanagar, Bangalore 560 080, India.
Phys Rev E Stat Phys Plasmas Fluids Relat Interdiscip Topics. 1999 Aug;60(2 Pt A):1381-9. doi: 10.1103/physreve.60.1381.
The propagation of light in a scattering medium is described as the motion of a special kind of a Brownian particle on which the fluctuating forces act only perpendicular to its velocity. This enforces strictly and dynamically the constraint of constant speed of the photon in the medium. A Fokker-Planck equation is derived for the probability distribution in the phase space assuming the transverse fluctuating force to be a white noise. Analytic expressions for the moments of the displacement <x(n)> along with an approximate expression for the marginal probability distribution function P(x,t) are obtained. Exact numerical solutions for the phase space probability distribution for various geometries are presented. The results show that the velocity distribution randomizes in a time of about eight times the mean free time (8t*) only after which the diffusion approximation becomes valid. This factor of 8 is a well-known experimental fact. A persistence exponent of 0.435+/-0.005 is calculated for this process in two dimensions by studying the survival probability of the particle in a semi-infinite medium. The case of a stochastic amplifying medium is also discussed.
光在散射介质中的传播被描述为一种特殊布朗粒子的运动,作用在该粒子上的涨落力仅垂直于其速度。这严格且动态地强制了光子在介质中速度恒定的约束条件。假设横向涨落力为白噪声,推导了相空间中概率分布的福克 - 普朗克方程。得到了位移<x(n)>的矩的解析表达式以及边际概率分布函数P(x,t)的近似表达式。给出了各种几何形状下相空间概率分布的精确数值解。结果表明,速度分布仅在约为平均自由时间八倍(8t*)的时间后才随机化,此后扩散近似才有效。这个8的因子是一个众所周知的实验事实。通过研究粒子在半无限介质中的存活概率,计算出二维情况下此过程的持续指数为0.435±0.005。还讨论了随机放大介质的情况。