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. 2009 Jun 15;34(12):1891-3.
doi: 10.1364/ol.34.001891.

Nonscalar elastic light scattering from continuous random media in the Born approximation

Affiliations

Nonscalar elastic light scattering from continuous random media in the Born approximation

Jeremy D Rogers et al. Opt Lett. .

Erratum in

  • Opt Lett. 2010 May 1;35(9):1367

Abstract

A three-parameter model based on the Whittle-Matérn correlation family is used to describe continuous random refractive-index fluctuations. The differential scattering cross section is derived from the index correlation function using nonscalar scattering formulas within the Born approximation. Parameters such as scattering coefficient, anisotropy factor, and spectral dependence are derived from the differential scattering cross section for this general class of functions.

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Figures

Fig. 1
Fig. 1
Index correlation functions for some values of m.
Fig. 2
Fig. 2
Above: An example differential scattering cross section plotted in spherical coordinates. The incident wave propagates from left to right and the polarization is such that electric field is in the vertical plane. The dimple is located at the origin. Below: Comparison of the rotationally averaged σup (inner) corresponding to unpolarized incidence and the scalar wave approximation σsw (outer) for klc = 0.1 (isotropic scattering) shown left, and klc = 1 (forward scattering) shown right.
Fig. 3
Fig. 3
Wavelength normalized scattering coefficient μs/k as a function of wavelength normalized index correlation length klc. Inset shows the normalized mean free path kls = ks dependence. It should be noted that although no limit is shown for μs, the value is inherently limited by the requirement that ls > lc. This weak scattering limit requires that the value of dn2(klc)2 ≪ 1.
Fig. 4
Fig. 4
Reduced scattering coefficient as a function of index correlation length (each normalized by wavelength).
Fig. 5
Fig. 5
Plots of μs vs klc with and without the dipole factor.

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