Collection of abstracts 14th
GAMM-Seminar Kiel on
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Multiscale methods and wavelets offer some promising features
for the
numerical solution of certain operator equations such as integral
equations and elliptic partial differential equations.
For a long time, these applications were restricted to simple domains
(such as the torus)
since there was no construction of wavelet bases on general domains
that could efficiently be used in implementations.
Quite recently, several papers appeared using a domain decomposition
technique by splitting the domain of interest into subdomains that are
images of a single reference square or cube under certain parametric
mappings, [CTU1,CTU2,DS1,DS2].
On the reference domain, one uses tensor products of wavelet
bases on the interval as in [DKU]
with appropriate boundary conditions.
Hence, the usefulness of such methods strongly depends on efficient
software for dealing with wavelet systems on the interval.
Since the realization of wavelet methods essentially differs
from using finite element meshes, it is neccessary to develop new
concepts for their implementation.
In this talk, we describe the main ingredients of our software and
present an example of its usage.
[CTU1] C. Canuto, A. Tabacco, and K. Urban}, The Wavelet Element Method, Part I: Construction and analysis, Istituto di Analisi Numerica del CNR, Pavia, Preprint No. 1038, 1997. [CTU2] C. Canuto, A. Tabacco, and K. Urban, he Wavelet Element Method, Part II: Realization and additional features in 2D and 3D, Istituto di Analisi Numerica del CNR, Pavia, Preprint No. 1052, 1997. [DKU] W. Dahmen, A. Kunoth, and K. Urban, Biorthogonal spline--wavelets on the interval --- Stability and moment conditions, RWTH Aachen, IGPM Preprint No. 129, 1996, Appl. Comp. Harm. Anal., to appear. [DS1] W. Dahmen and R. Schneider, Composite wavelet bases for operator equations, RWTH Aachen, IGPM Preprint No. 133, 1996. [DS2] W. Dahmen and R. Schneider, Multiscale methods for boundary integral equations I: Biorthogonal wavelets on 2D--manifolds in $\er^3$, in preparation.
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