By Rudolf Kingslake
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Extra resources for Applied optics and optical engineering,Vol.IV
4 Approximate Solutions to Light Scattering Our objective now is to gain an insight into how the scattering parameters introduced above relate to the refractive index variations in tissue. For this, we have to return to the deﬁnition of the scattering amplitude. 14) V where k is the wave number and n = n/n0 is the relative refractive index within the scattering volume V. ) The problem, of course, is that this integration requires knowledge of the ﬁeld inside the scattering volume, and in order to calculate this ﬁeld one would need to solve Maxwell’s equations.
Html with variations of calculation precision (extended and double) and scattering geometries. Another resource for T-matrix calculations can be found on the SCATTLIB Web site where Fortran codes for speciﬁc scattering geometries are given, including oriented spheroids and 2D and 3D random orientations. These routines are based on codes given in the book, Light Scattering by Particles: Computational Methods, by P. W. Barber and S. C. Hill from the Advanced Series in Applied Physics Vol. 2 (World Scientiﬁc Pub.
6) where ks = |k s | = 2k sin(/2). Substituting this equation in Eq. 7) in which the identity sin2 = 1 − sin2 () cos2 () is used, where and are deﬁned as shown in Fig. 1. The term sin2 represents the effect of the polarization orientation of the incident light and is referred to as the dipole factor. 3 An example mean differential scattering cross section per unit volume plotted in spherical coordinates. The incident wave is oriented to propagate from left to right and the polarization is such that electric ﬁeld is in the vertical plane.
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