1959
DOI: 10.1109/tap.1959.1144754
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On the discontinuity problem at the input to an anisotropic waveguide

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Cited by 14 publications
(4 citation statements)
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“…We now demonstrate some general properties for the solutions of the eigenproblem (6). It has already been said that a lossless material is characterized by a hermitian symmetric material matrix, M = M H .…”
Section: Bianisotropic Materialsmentioning
confidence: 89%
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“…We now demonstrate some general properties for the solutions of the eigenproblem (6). It has already been said that a lossless material is characterized by a hermitian symmetric material matrix, M = M H .…”
Section: Bianisotropic Materialsmentioning
confidence: 89%
“…A general formalism for anisotropic waveguides was presented in a series of papers in the late fifties [5][6][7][8], but they have had surprisingly few followers. The bianisotropic case is treated by [21] and [4].…”
Section: Introductionmentioning
confidence: 99%
“…This condition can be phrased as an integral equa-tion for the field in the plane of the bed boundary. We extracted useful information from this equation by variational techniques (Angulo, 1957;Angulo and Chang, 1959;Bresler, 1959;Reinhart et al, 1971;Hockham and Sharpe, 1972;Ikegami, 1972;Rozzi, 1978;Rozzi and Veld, 1980) Wiener-Hopf methods (Angulo and Chang, 1953;Angulo and Chang, 1959;Kay, 1959;Aoki and Miyazaki, 1982) expansion in Neuman series (Gelin et al, 1979;Gelin et al, 1981), and mode matching (Clarricoats et al, 1972;Hockham and Sharpe, 1972;Brooke and Kharadly, 1982;Mahmoud and Beal, 1975;Morishita et al, 1979). The most significant technical complication of junction problems in an open waveguide is the treatment of the continuous spectrum.…”
Section: Introductionmentioning
confidence: 99%
“…Analytical solutions were obtained by several researchers for some simple structures [6] in which the ferrite slabs were transversely magnetized, while other structures or biasing in an arbitrary direction were solved using numerical methods, such as the finite-element method (FEM) [7,8]. Bresler [9] formulated the integral equation for discontinuity at the transverse plane by separating two regions in a waveguide -one isotropic and the other anisotropic -and then used the variational expression based on the integral equation to obtain numerical results for the scattering parameters. An analytical solution and experimental results for an E-plane ferrite-slab-filled rectangular waveguide were presented by O'Brien [10,11].…”
Section: Introductionmentioning
confidence: 99%