DocumentCode
1358377
Title
Diagonal preconditioners for the EFIE using a wavelet basis
Author
Canning, Francis X. ; Scholl, James F.
Author_Institution
Rockwell Inst. Sci. Center, Thousand Oaks, CA, USA
Volume
44
Issue
9
fYear
1996
fDate
9/1/1996 12:00:00 AM
Firstpage
1239
Lastpage
1246
Abstract
The electric field integral equation (EFIE) has found widespread use and in practice has been accepted as a stable method. However, mathematically, the solution of the EFIE is an “ill-posed” problem. In practical terms, as one uses more and more expansion and testing functions per wavelength, the condition number of the resulting moment-method matrix increases (without bound). This means that for high-sampling densities, iterative methods such as conjugate gradients converge more slowly. However, there is a way to change all this. The EFIE is considered using a wavelet basis for expansion and for testing functions. Then, the resulting matrix is multiplied on both sides by a diagonal matrix. This results in a well-conditioned matrix which behaves much like the matrix for the magnetic field integral equation (MFIE). Consequences for the stability and convergence rate of iterative methods are described
Keywords
convergence of numerical methods; electric fields; integral equations; iterative methods; matrix algebra; method of moments; numerical stability; wavelet transforms; EFIE; MFIE; condition number; convergence rate; diagonal matrix; diagonal preconditioners; electric field integral equation; expansion functions; high-sampling densities; ill-posed problem; iterative methods; magnetic field integral equation; moment-method matrix; stability; stable method; testing functions; wavelength; wavelet basis; well-conditioned matrix; Canning; Convergence; Integral equations; Iterative methods; Magnetic fields; Moment methods; Sampling methods; Senior members; Stability; Testing;
fLanguage
English
Journal_Title
Antennas and Propagation, IEEE Transactions on
Publisher
ieee
ISSN
0018-926X
Type
jour
DOI
10.1109/8.535382
Filename
535382
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