Startseite Mathematik 10. Time-harmonic electro-magnetic scattering in exterior weak Lipschitz domains with mixed boundary conditions
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10. Time-harmonic electro-magnetic scattering in exterior weak Lipschitz domains with mixed boundary conditions

  • Frank Osterbrink und Dirk Pauly
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Maxwell’s Equations
Ein Kapitel aus dem Buch Maxwell’s Equations

Abstract

This paper treats the time-harmonic electro-magnetic scattering or radiation problem governed by Maxwell’s equations, i. e., − rot H + iωεE = F in Ω, E × ν = 0 on Γ1, rot E + iωμH = G in Ω, H × ν = 0 on Γ2, where ω ∈ ℂ \ (0) and Ω ⊂ ℝ3 is an exterior weak Lipschitz domain with boundary Γ divided into two disjoint parts Γ1 and Γ2. We will present a solution theory using the framework of polynomially weighted Sobolev spaces for the rotation and divergence. For the physically interesting case ω ∈ ℝ \ (0), we will show a Fredholm alternative type result to hold using the principle of limiting absorption introduced by Eidus in the 1960s. The necessary a priori estimate and polynomial decay of eigenfunctions for the Maxwell equations will be obtained by transferring well-known results for the Helmholtz equation using a suitable decomposition of the fields E and H. The crucial point for existence is a local version of Weck’s selection theorem, also called Maxwell compactness property.

Abstract

This paper treats the time-harmonic electro-magnetic scattering or radiation problem governed by Maxwell’s equations, i. e., − rot H + iωεE = F in Ω, E × ν = 0 on Γ1, rot E + iωμH = G in Ω, H × ν = 0 on Γ2, where ω ∈ ℂ \ (0) and Ω ⊂ ℝ3 is an exterior weak Lipschitz domain with boundary Γ divided into two disjoint parts Γ1 and Γ2. We will present a solution theory using the framework of polynomially weighted Sobolev spaces for the rotation and divergence. For the physically interesting case ω ∈ ℝ \ (0), we will show a Fredholm alternative type result to hold using the principle of limiting absorption introduced by Eidus in the 1960s. The necessary a priori estimate and polynomial decay of eigenfunctions for the Maxwell equations will be obtained by transferring well-known results for the Helmholtz equation using a suitable decomposition of the fields E and H. The crucial point for existence is a local version of Weck’s selection theorem, also called Maxwell compactness property.

Heruntergeladen am 30.9.2025 von https://www.degruyterbrill.com/document/doi/10.1515/9783110543612-010/html
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