1990
DOI: 10.1109/8.52240
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Electromagnetic scattering and radiation by surfaces of arbitrary shape in layered media. I. Theory

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Cited by 702 publications
(389 citation statements)
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“…ε i = ε i − jσ i /ω, µ i , and k i represent (in general complex) the permittivity, permeability, and wavenumber of the medium in which the target resides, and ω is the angular frequency (with a time dependence exp jωt assumed and suppressed). Details on the Green's function dyadicsḠ Aii andK Aii , as well as the scalar Green's function K ii φe have been given by Michalski and Zheng in [1], where we use their formulation C. The CFIE in (1) is valid for a more general layered medium [1], but here we only consider the half-space problem for simplicity.…”
Section: Integral Equation and Half-space Mom Formulationmentioning
confidence: 99%
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“…ε i = ε i − jσ i /ω, µ i , and k i represent (in general complex) the permittivity, permeability, and wavenumber of the medium in which the target resides, and ω is the angular frequency (with a time dependence exp jωt assumed and suppressed). Details on the Green's function dyadicsḠ Aii andK Aii , as well as the scalar Green's function K ii φe have been given by Michalski and Zheng in [1], where we use their formulation C. The CFIE in (1) is valid for a more general layered medium [1], but here we only consider the half-space problem for simplicity.…”
Section: Integral Equation and Half-space Mom Formulationmentioning
confidence: 99%
“…The dyadic half-space Green's function is evaluated rigorously using the method of discrete complex images [23], thereby avoiding direct numerical evaluation of Sommerfeld integrals [1]. Impedance matrix elements representing these near interactions are stored in a sparse matrix called [Z near ].…”
Section: Integral Equation and Half-space Mom Formulationmentioning
confidence: 99%
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