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Вестник Российского университета дружбы народов. Серия: Математика, информатика, физика  / №4 2013

The Derivation of the Dispersion Equations of Adiabatic Waveguide Modes in the Thin-Film Waveguide Luneburg Lens in the Form of Non-Linear Partial Differential Equation of the First Order (80,00 руб.)

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Первый авторZuev
АвторыAyryan E.A., Busa J., Ivanov V.V., Sevastianov L.A., Streltsova O.I.
Страниц10
ID404376
АннотацияThis paper presents a derivation of the dispersion equation for a three-layer integratedoptical Luneburg lens based on the method of adiabatic waveguide modes. From this equation there follows the relationship between the coefifcient of phase deceleration and function, which determines the thickness of the irregular waveguide layer. The dispersion equation is represented in the form of non-linear partial differential equation of the first order with coefifcients, depending on parameters. Among these parameters are regular waveguide layer thickness and optical parameters of the pending Luneburg lens. To represent the dispersion equation in the form of differential equations in partial derivatives, it is necessary to calculate a symbolic form the determinant of a matrix of 12th order, which determines the solubility of the system of linear algebraic equations, resulting from the boundary conditions. To calculate this determinant in analytical form a procedure of reduction of the system of linear algebraic equations with the use of the computer algebra system Maple is proposed.
УДК517:519.6, 535+537.8:621.37
The Derivation of the Dispersion Equations of Adiabatic Waveguide Modes in the Thin-Film Waveguide Luneburg Lens in the Form of Non-Linear Partial Differential Equation of the First Order / M.I. Zuev [и др.] // Вестник Российского университета дружбы народов. Серия: Математика, информатика, физика .— 2013 .— №4 .— С. 124-133 .— URL: https://rucont.ru/efd/404376 (дата обращения: 15.05.2024)

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UDC 517:519.6, 535+537.8:621.37 The Derivation of the Dispersion Equations of Adiabatic M. I. Zuev∗, E. A. Ayryan∗, J. Buˇ sa†, V. V. Ivanov∗, L. A. Sevastianov‡, O. I. Streltsova∗ ∗ Laboratory of Information Technologies Joint Institute for Nuclear Research Joliot-Curie 6, 141980 Dubna, Moscow region, Russia † Technical University in Koˇ sice Letn´ a 9, 04001, Koˇ sice, Slovak Republic ‡ Telecommunication System Department Peoples’ Friendship University of Russia Miklukho-Maklaya str. 6, 117198 Moscow, Russia This paper presents a derivation of the dispersion equation for a three-layer integratedoptical Luneburg lens based on the method of adiabatic waveguide modes. <...> From this equation there follows the relationship between the coefficient of phase deceleration and function, which determines the thickness of the irregular waveguide layer. <...> The dispersion equation is represented in the form of non-linear partial differential equation of the first order with coefficients, depending on parameters. <...> Among these parameters are regular waveguide layer thickness and optical parameters of the pending Luneburg lens. <...> To represent the dispersion equation in the form of differential equations in partial derivatives, it is necessary to calculate a symbolic form the determinant of a matrix of 12th order, which determines the solubility of the system of linear algebraic equations, resulting from the boundary conditions. <...> To calculate this determinant in analytical form a procedure of reduction of the system of linear algebraic equations with the use of the computer algebra system Maple is proposed. <...> Key words and phrases: irregular integrated optical wave guide, method of adiabatic modes, computer algebra system. 1. <...> One of the most promising methods used in the modeling of the waveguide propagation of radiation with the exact tangential boundary conditions, is the method of adiabatic waveguide modes. <...> The overall objective of modeling smoothly irregular longitudinally integrated opThe waveguide Luneburg lens is an important functional element of integrated Waveguide Modes in the Thin-Film Waveguide Luneburg Lens in the Form of Non-Linear Partial Differential Equation of the First Order tical waveguides includes the task of finding the irregular surface of the waveguide layer by solving the dispersion equation. <...> In the papers [3–7] computational scheme for solving this problem has been proposed. <...> However, to develop a software module that allows to increase significantly <...>