2000
DOI: 10.1142/s0218202500000197
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Existence, Uniqueness and Regularity for Solutionsv of the Conical Diffraction Problem

Abstract: This paper is devoted to the analysis of two Helmholtz equations in ℝ2 coupled via quasiperiodic transmission conditions on a set of piecewise smooth interfaces. The solution of this system is quasiperiodic in one direction and satisfies outgoing wave conditions with respect to the other direction. It is shown that Maxwell's equations for the diffraction of a time-harmonic oblique incident plane wave by periodic interfaces can be reduced to problems of this kind. The analysis is based on a strongly elliptic va… Show more

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Cited by 29 publications
(43 citation statements)
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“…[2,11]) that the finite energy condition (2.2) is satisfied only if the z-components of E and B are H 1 -regular. Moreover, E z , B z determine the other components of the electric and magnetic fields and are solutions of the Helmholtz equations…”
Section: Figure 1 Cross Section Of a Multilayer Gratingmentioning
confidence: 99%
See 2 more Smart Citations
“…[2,11]) that the finite energy condition (2.2) is satisfied only if the z-components of E and B are H 1 -regular. Moreover, E z , B z determine the other components of the electric and magnetic fields and are solutions of the Helmholtz equations…”
Section: Figure 1 Cross Section Of a Multilayer Gratingmentioning
confidence: 99%
“…To prove that the Rayleigh coefficientsû ± n ,v ± n vanish for arbitrary non-trivial solutions (u, v) we proceed as in [2,11]. Choose a periodic cell Ω H , which has in the x-direction the width d, is bounded by the straight lines {y = ±H} and contains Γ j , j = k, .…”
Section: Uniquenessmentioning
confidence: 99%
See 1 more Smart Citation
“…Ammari, Bao & Wood [3], Bao & Dobson [9], Bonnet-Bendhia & Starling [10], Elschner & Schmidt [26], Elschner, Hinder, Penzel & Schmidt [27], Elschner & Yamamoto [28] and Kirsch [33]. In the case of elastic scattering by periodic surfaces, the variational approach is established by Elschner & Hu in [24,25] for the boundary value problems of the first, second, third and fourth kind as well as for transmission problems with non-smooth interfaces in R n (n = 2, 3).…”
Section: Introductionmentioning
confidence: 99%
“…In Section 4 we introduce a variational formulation to couple the PML to the interior problem. In contrast to Elschner et al [11,10] the electromagnetic field E = (E 1 , E 2 , E 3 ) is discretized with higher order Whitney elements for the (E 1 , E 2 ) component and Lagrange elements of the same order in the E 3 component. This allows for the accurate evaluation of Fourier coefficients needed for the coupling to a multi-layer stack as well for the computation of the far field coefficients.…”
Section: Introductionmentioning
confidence: 99%