2016
DOI: 10.1049/iet-map.2015.0158
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Surface and leaky waves of a planar dielectric waveguide with a diffraction grating

Abstract: The eigenwave propagation problem is solved for a periodic waveguide composed of a planar dielectric waveguide and a reflecting diffraction grating. The technique the authors used is the spectral theory of open waveguide structures. The numerical data for the dependences of the propagation constants of surface and complex (leaky) eigenwaves are presented versus frequency and geometrical parameters of the periodic waveguide. In the frequency range of leaky eigenwaves, the angular‐frequency characteristics of th… Show more

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Cited by 8 publications
(6 citation statements)
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References 18 publications
(22 reference statements)
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“…The chosen option for constructing a power divider makes it possible to perform simulation without taking into account the final level of radiator matching [39] since the main part of the power reflected from the radiators is dissipated in the balanced loads of the directional coupler. The simulation was performed taking into account the following initial data: operating frequency range of the antenna: from 2,7 GHz to 2,85 GHz (5,4%); number of power divider outputs: N = 54; analyzed frequency range: fl = 2,68 GHz, fh = 2,87 GHz, M = 1901; normal frequency: fn = 2,77 GHz; type of delay line waveguide: rectangular (section a×b=62,4×17 mm); linear losses in delay lines: α = 0,07 dB/m; the number of wavelengths at the frequency of the normal forming the period of the delay line: nλ = 2,5; coefficients that determine the shape of the antenna array: p = 0,19, g = 1,65; efficiency of the power divider: η = 79%; standing wave coefficient for the voltage of the bends of the delay line (Rbn): distributed according to a random uniform law in the range from 1,02 to 1,04; standing wave ratio for the voltage of the directional coupler (Rcn): distributed according to a random uniform law in the range from 1,05 to 1,07; the initial phase of the reflection coefficient : distributed according to a random uniform law in the range from 170° to 190°.…”
Section: Simulation Resultsmentioning
confidence: 99%
“…The chosen option for constructing a power divider makes it possible to perform simulation without taking into account the final level of radiator matching [39] since the main part of the power reflected from the radiators is dissipated in the balanced loads of the directional coupler. The simulation was performed taking into account the following initial data: operating frequency range of the antenna: from 2,7 GHz to 2,85 GHz (5,4%); number of power divider outputs: N = 54; analyzed frequency range: fl = 2,68 GHz, fh = 2,87 GHz, M = 1901; normal frequency: fn = 2,77 GHz; type of delay line waveguide: rectangular (section a×b=62,4×17 mm); linear losses in delay lines: α = 0,07 dB/m; the number of wavelengths at the frequency of the normal forming the period of the delay line: nλ = 2,5; coefficients that determine the shape of the antenna array: p = 0,19, g = 1,65; efficiency of the power divider: η = 79%; standing wave coefficient for the voltage of the bends of the delay line (Rbn): distributed according to a random uniform law in the range from 1,02 to 1,04; standing wave ratio for the voltage of the directional coupler (Rcn): distributed according to a random uniform law in the range from 1,05 to 1,07; the initial phase of the reflection coefficient : distributed according to a random uniform law in the range from 170° to 190°.…”
Section: Simulation Resultsmentioning
confidence: 99%
“…Note that the matrix T does not depend on β, therefore, when solving the dispersion equation (7), it is calculated only once, which significantly reduces the search time for the roots of the dispersion equation. Note that, when deriving equations ( 6) and (7), no restrictions were imposed on the form of dependence ε(r), i.e.…”
Section: Symmetrical H-wavesmentioning
confidence: 99%
“…Note that the matrix T does not depend on β, therefore, when solving the dispersion equation (7), it is calculated only once, which significantly reduces the search time for the roots of the dispersion equation. Note that, when deriving equations ( 6) and (7), no restrictions were imposed on the form of dependence ε(r), i.e. this method allows one to calculate symmetric H-waves with a completely arbitrary nature of the change in the dielectric constant along the transverse coordinate, while ε can also be a complex quantity, which allows, for example, calculating waveguides with a complex absorption distribution in the crosssection, that is, to solve non-self-adjoint boundary value problems, in which the identity of the differential operators of the direct and adjoint boundary value problems is satisfied.…”
Section: Symmetrical H-wavesmentioning
confidence: 99%
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