Journal
JOURNAL OF QUANTITATIVE SPECTROSCOPY & RADIATIVE TRANSFER
Volume 242, Issue -, Pages -Publisher
PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.jqsrt.2019.106779
Keywords
Generalized Lorenz-Mie theory; Extended boundary condition method; T-Matrix; Beam shape coefficients; Vector spherical wave functions
Categories
Funding
- FAPESP (Sao Paulo Research Foundation) [2017/10445-0]
- CNPq (National Council for Scientific and Technological Development) [426990/2018-8, 307898/2018-0]
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When dealing with light scattering theories such as the T-matrix methods for structured laser beams, e.g. Generalized Lorenz-Mie Theory (GLMT) or the Extended Boundary Condition Method (EBCM), EM fields are expanded over a set of Vector Spherical Wave Functions (VSWFs) involving spherical Bessel functions, with expansion coefficients expressed in terms of Beam Shape Coefficients (BSCs). Although spherical Bessel functions are orthogonal over the range (-infinity, +infinity), the GLMT may be expressed using a non-orthogonal set of spherical Bessel functions defined over (0, +infinity), allowing one to generate an infinite number of quadratures for evaluating the BSCs. This paper points out the difference between orthogonal and non-orthogonal spherical Bessel functions, establishes the infinite number of quadratures and discusses its properties. (C) 2019 Elsevier Ltd. All rights reserved.
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