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Approximation theory methods for solving elliptic eigenvalue problems

Identifieur interne : 001230 ( Istex/Curation ); précédent : 001229; suivant : 001231

Approximation theory methods for solving elliptic eigenvalue problems

Auteurs : G. Still [Pays-Bas]

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RBID : ISTEX:4EED5B54B8C087DCD6BCBA275CB1EBEFBBB6693D

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Abstract

Eigenvalue problems with elliptic operators L on a domain G ⊂ R2 are considered. By applying results from complex approximation theory we obtain results on the approximation properties of special classes of solutions of Lu = 0 on G . These solutions are used as trial functions in a method for solving the eigenvalue problem which is based on a‐posteriori error bounds. Singular trial functions are applied to smooth the problem at corner points of G . In special situations, this method can produce approximations of eigenvalues and eigenfunctions with extremely high accuracy by only using a low number of trial functions. Some illustrative numerical examples for the eigenvalue problem with the Laplacian are presented. We discuss two problems from plasma physics (‘relaxed plasma’, ‘MHD‐equation’).

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DOI: 10.1002/zamm.200310081

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ISTEX:4EED5B54B8C087DCD6BCBA275CB1EBEFBBB6693D

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<div type="abstract" xml:lang="en">Eigenvalue problems with elliptic operators L on a domain G ⊂ R2 are considered. By applying results from complex approximation theory we obtain results on the approximation properties of special classes of solutions of Lu = 0 on G . These solutions are used as trial functions in a method for solving the eigenvalue problem which is based on a‐posteriori error bounds. Singular trial functions are applied to smooth the problem at corner points of G . In special situations, this method can produce approximations of eigenvalues and eigenfunctions with extremely high accuracy by only using a low number of trial functions. Some illustrative numerical examples for the eigenvalue problem with the Laplacian are presented. We discuss two problems from plasma physics (‘relaxed plasma’, ‘MHD‐equation’).</div>
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