학술논문

Static Surface Mode Expansion for the Electromagnetic Scattering From Penetrable Objects
Document Type
Periodical
Source
IEEE Transactions on Antennas and Propagation IEEE Trans. Antennas Propagat. Antennas and Propagation, IEEE Transactions on. 71(8):6779-6793 Aug, 2023
Subject
Fields, Waves and Electromagnetics
Aerospace
Transportation
Components, Circuits, Devices and Systems
Eigenvalues and eigenfunctions
Electromagnetic scattering
Stars
Shape
Manganese
Integral equations
Electromagnetics
Computational electromagnetics
dielectric resonators
eigenvalues and eigenfunctions
electromagnetic scattering
integral equations
plasmonics
resonance
resonators
Language
ISSN
0018-926X
1558-2221
Abstract
We introduce longitudinal and transverse static surface modes and use them to solve the scattering problem from penetrable objects with arbitrary shapes. The longitudinal static modes are the eigenmodes, with zero surface-curl, of the electrostatic integral operator that determines the tangential component of the electric field, as a function of the surface charge density. The transverse static modes are the eigenmodes, with zero surface-divergence, of the magnetostatic integral operator that determines the tangential component of the vector potential, as a function of the surface current density. These static modes are solely determined by the object’s shape, thus, the same static basis can be used regardless of the operating frequency or material properties. We expand the unknown surface currents of the Poggio-Miller-Chang-Harrington-Wu–Tsai (PMCHWT) equation in terms of the static modes and solve it using Galerkin-projections. The static modes expansion allows for the regularization of the integral operators and also leads to a significant reduction in the number of unknowns compared to a discretization based on sub-domain basis functions. As a consequence, the CPU-time required for the numerical solution of the scattering problem from arrays of identical particles is significantly reduced by employing an expansion in terms of static modes of the isolated particle.