1986
DOI: 10.1016/0041-5553(86)90126-6
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A difference scheme for the non-stationary maxwell equations in waveguide systems

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Cited by 4 publications
(12 citation statements)
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“…The solutions that satisfy the zero initial conditions and are free from any components propagating along the decreasing z j . This formula is derived through the integral Laplace transform over t or the Fourier cosine transform over z j [ Maikov et al , 1986]. Actually, on the assumption that at the initial moment of time t = 0 the excitation wave U j ( g , t ) has not yet reached the discontinuity boundary in the plane z 1 = 0, we obtain for the amplitudes { w nj ( z j , t )} a sequence of homogeneous initial boundary value problems: By using in the Fourier cosine transform over z j at the semi‐axes z j ≥ 0 (image ↔ original) we obtain the following Caushy problems for the images nj (ω, t ): Here we had taken into account that the waves U j s ( z j , t ) are free of components propagating along the decreasing z j .…”
Section: Evolutionary Basis Of the Signal And Transform Operatorsmentioning
confidence: 99%
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“…The solutions that satisfy the zero initial conditions and are free from any components propagating along the decreasing z j . This formula is derived through the integral Laplace transform over t or the Fourier cosine transform over z j [ Maikov et al , 1986]. Actually, on the assumption that at the initial moment of time t = 0 the excitation wave U j ( g , t ) has not yet reached the discontinuity boundary in the plane z 1 = 0, we obtain for the amplitudes { w nj ( z j , t )} a sequence of homogeneous initial boundary value problems: By using in the Fourier cosine transform over z j at the semi‐axes z j ≥ 0 (image ↔ original) we obtain the following Caushy problems for the images nj (ω, t ): Here we had taken into account that the waves U j s ( z j , t ) are free of components propagating along the decreasing z j .…”
Section: Evolutionary Basis Of the Signal And Transform Operatorsmentioning
confidence: 99%
“…The solutions that satisfy the zero initial conditions and are free from any components propagating along the decreasing z j . This formula is derived through the integral Laplace transform over t or the Fourier cosine transform over z j [Maikov et al, 1986]. Actually, on the assumption that at the initial moment of time t = 0 the excitation wave U j (g, t)…”
Section: Essential Definitionsmentioning
confidence: 99%
“…Exact absorbing conditions (EAC) are used in computational electrodynamics of nonsine waves for truncating the domain of computation when replacing the original open initial boundary value problem by a modified problem formulated in a bounded domain [1][2][3][4][5][6][7][8][9]. In the present work, we construct and analyze the EAC as applied to the axially symmetrical waveguide structures illuminated by symmetrical pulsed TEand TM-waves (or TE 0 -and TM 0 -waves) and prove the equivalency of the original (open) and modified (closed) initial boundary value problems.…”
Section: Introductionmentioning
confidence: 99%
“…They have already taken their proper place in electromagnetic simulation in fundamental and applied electromagnetics. In 1986, scientists from Moscow State University, Ⱥ. R. Maikov, A. G. Sveshnikov, and S. A. Yakunin, published their paper [18]. In this paper the exact non-local conditions for virtual boundaries in regular semi-infinite hollow waveguides (with constant cross section), serving as channels for signals propagating from certain resonant junctions, were formulated for the fist time.…”
mentioning
confidence: 97%
“…In this paper the exact non-local conditions for virtual boundaries in regular semi-infinite hollow waveguides (with constant cross section), serving as channels for signals propagating from certain resonant junctions, were formulated for the fist time. Later on (see for example, references [19]-[29]) the approach suggested in [18], that is based on the utilization of radiation conditions for time-spatial amplitudes of outgoing modes, has been modified for various electromagnetic problems: antenna design, analysis and synthesis problems for quasi optical open resonators with dispersive elements, electromagnetic monitoring of human environment and others. For several particular cases the problems of non-locality, the problems of large and distant sources and the problem of corner points, points of intersection of coordinate boundaries, have been resolved in a rigorous way.…”
mentioning
confidence: 99%