1965
DOI: 10.1109/tap.1965.1138427
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Scattering by a dielectric cylinder of arbitrary cross section shape

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Cited by 937 publications
(357 citation statements)
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“…This problem is solved in [25] by the Integral Equation Method and in [26] by the Eigenfunction Expansion Method. The RCS (σ/λ) of this structure obtained by the proposed method of addition theorems and those computed by the methods in [25] and [26] agree very well as depicted in Fig. 2 for the angle of observation from 'ϕ = 0 to ϕ = π' for both TE and TM polarizations.…”
Section: Example 1: Rcs Of a Dielectric Cylinder With A Dielectric Cymentioning
confidence: 99%
“…This problem is solved in [25] by the Integral Equation Method and in [26] by the Eigenfunction Expansion Method. The RCS (σ/λ) of this structure obtained by the proposed method of addition theorems and those computed by the methods in [25] and [26] agree very well as depicted in Fig. 2 for the angle of observation from 'ϕ = 0 to ϕ = π' for both TE and TM polarizations.…”
Section: Example 1: Rcs Of a Dielectric Cylinder With A Dielectric Cymentioning
confidence: 99%
“…A given approach is assumed to be convergent if {k} → 0 , as k → ∞ . In order to apply the distorted-wave Born approximation, at the first iteration step, the field Ψ L (r ) is numerically computed by the Richmond formulation [12], which has been proved to be accurate for forward-scattering by dielectric cylinders, if a TM illumination is used. The cross-section S is partitioned into P subdomains, p = 1, .…”
Section: Description Of the Methodsmentioning
confidence: 99%
“…Moreover, the investigation domain Γ inv has been partitioned for the inversion in a grid of N inv = 32 × 32 cells [65].…”
Section: Numerical Assessment and Validationmentioning
confidence: 99%