Time-dependent Debye-Mie Series Solutions for Electromagnetic Scattering

TL;DR

This paper introduces a stable, rapidly convergent quasi-analytical method for transient electromagnetic scattering from spheres, overcoming oscillatory convolution issues in traditional frequency domain Mie solutions.

Contribution

It develops a novel approach using vector tesseral harmonics and a new Green's function addition theorem to compute time-dependent Mie scattering efficiently.

Findings

Method is stable and converges rapidly.

Numerical examples demonstrate high accuracy.

System is orthogonal, meshfree, and free of singularities.

Abstract

Frequency domain Mie solutions to scattering from spheres have been used for a long time. However, deriving their transient analogue is a challenge as it involves an inverse Fourier transform of the spherical Hankel functions (and their derivatives) that are convolved with inverse Fourier transforms of spherical Bessel functions (and their derivatives). Series expansion of these convolutions are highly oscillatory (therefore, poorly convergent) and unstable. Indeed, the literature on numerical computation of this convolution is very sparse. In this paper, we present a novel quasi-analytical approach to computing transient Mie scattering that is both stable and rapidly convergent. The approach espoused here is to use vector tesseral harmonics as basis function for the currents in time domain integral equations together with a novel addition theorem for the Green's functions that renders these expansions stable. This procedure results in an orthogonal, spatially-meshfree and singularity-free system, giving us a set of one dimensional Volterra Integral equations. Time-dependent multipole coefficients for each mode are obtained via a time marching procedure. Finally, several numerical examples are presented to show the accuracy and stability the proposed method.