1963
DOI: 10.1109/tap.1963.1138053
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Scattering from a gyrotropic cylinder

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Cited by 15 publications
(15 citation statements)
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“…The validity of our calculations is confirmed by comparison with HFSS commercial software. The blue dots depict results for Q sc /(πR 2 2 ) obtained via HFSS simulations, thus establishing a good agreement with the VIE. It should be mentioned that an excellent agreement can be met, especially for the localized surface plasmon (LSP) appearing at λ b /R 2 9.92, but it would require a tremendous amount of CPU time for HFSS to extract the spectrum using its finite element solver.…”
Section: Engineering Functional Spherical Terahertz Antennas For Diresupporting
confidence: 70%
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“…The validity of our calculations is confirmed by comparison with HFSS commercial software. The blue dots depict results for Q sc /(πR 2 2 ) obtained via HFSS simulations, thus establishing a good agreement with the VIE. It should be mentioned that an excellent agreement can be met, especially for the localized surface plasmon (LSP) appearing at λ b /R 2 9.92, but it would require a tremendous amount of CPU time for HFSS to extract the spectrum using its finite element solver.…”
Section: Engineering Functional Spherical Terahertz Antennas For Diresupporting
confidence: 70%
“…In the analysis that follows, we demonstrate a state which corresponds to forward-scattering in the absence of magnetic field, and to back-scattering with non-zero external magnetic bias. Figure 2A depicts the normalized scattering cross section Q sc /(πR 2 2 ) versus the normalized wavelength λ b /R 2 , under null magnetic field, for outer radius value R 2 10 μm, and R 1 /R 2 0.9. In addition to the full-wave contribution to Q sc -i.e., all spherical harmonics and angular momentum terms, required for convergence, contribute in Eq.…”
Section: Engineering Functional Spherical Terahertz Antennas For Dirementioning
confidence: 99%
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“…However, for the well-known practical G-type materials [7], having permittivity and permeability tensors defined in a Cartesian coordinate system denoted by ζ = ζ 0 ζ r for ζ = ε, μ with tensor elements ζ xx = ζ yy , ζ yx = −ζ xy , and all the other tensor elements except ζ zz being zero and of which gyrotropic [1], [2], [35], [36] is a special case when ζ xy is purely imaginary, one can still obtain expressions for the electric and magnetic fields within the elliptic cylinder in the form of infinite series involving Mathieu functions as shown in Appendix B, and thereby a formal series solution to the associated scattering problem. This is as a result of the tensor elements ζ τσ in the Cartesian coordinate system for τ = x, y, z and σ = x, y, z as in (A18), transforming into the corresponding elements ζ τσ in the elliptic coordinate system for τ = u, v, z and σ = u, v, z as in (A19).…”
Section: Fields Within the Coatingmentioning
confidence: 99%
“…Consequently, a series solution to the problem of scattering of a transverse magnetically polarized incident plane wave by an anisotropic elliptic cylinder composed of a G-type material can also be obtained, which includes gyrotropic [1], [2], [35], [36] as well as gyromagnetic [41]- [44] materials, as special cases.…”
Section: Appendix Bmentioning
confidence: 99%