1996
DOI: 10.1137/s0036141094271259
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On the Solution of Time-Harmonic Scattering Problems for Maxwell’s Equations

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Cited by 137 publications
(168 citation statements)
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“…We seek solutions E, H ∈ H loc (curl; R 3 ) to (1.8); see [19,22,23,31] for the well-posedness of the scattering system (1.8). Here and also in what follows, we shall often use the spaces H loc (curl; X) = {U | B ∈ H(curl; B); B is any bounded subdomain of X} and…”
Section: Mathematical Formulationmentioning
confidence: 99%
“…We seek solutions E, H ∈ H loc (curl; R 3 ) to (1.8); see [19,22,23,31] for the well-posedness of the scattering system (1.8). Here and also in what follows, we shall often use the spaces H loc (curl; X) = {U | B ∈ H(curl; B); B is any bounded subdomain of X} and…”
Section: Mathematical Formulationmentioning
confidence: 99%
“…Consequently the nonzero eigenvalues of interest can be captured by choosing the parameter s large enough (or by taking different values of s). In that respect, our method is similar to the discrete regularization method for standard edge elements [3,18] and can be compared with the so-called grad-div regularizated method for the continuous Maxwell's problem where the term s Ω div u div v is added to the standard bilinear form of the curl [13,16].…”
Section: Some Numerical Testsmentioning
confidence: 99%
“…The scattered fields have to satisfy the Silver-Müller radiation conditions (5). As a consequence of Rellich's lemma and the unique continuation principle, the transmission problem (2)-(5) has a unique solution [10,20].…”
Section: Mathematical Modelmentioning
confidence: 99%