Two methods to deconvolve: L1-method using simplex algorithm and L2-method using least squares and parameter
If r(t) is the linear scattering response of an object to an excitation waveform e(t) , then r(t) = (e \ast h) (t) . One would like to deconvolve and solve for h(t) , the impulse response. It is well-known that this is often an ill-conditioned problem. Two methods are discussed. The first method rep...
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| Published in: | IEEE transactions on antennas and propagation Vol. 32; no. 3; pp. 219 - 225 |
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| Main Author: | |
| Format: | Journal Article |
| Language: | English |
| Published: |
New York, NY
IEEE
01.03.1984
Institute of Electrical and Electronics Engineers |
| Subjects: | |
| ISSN: | 0018-926X, 1558-2221 |
| Online Access: | Get full text |
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| Summary: | If r(t) is the linear scattering response of an object to an excitation waveform e(t) , then r(t) = (e \ast h) (t) . One would like to deconvolve and solve for h(t) , the impulse response. It is well-known that this is often an ill-conditioned problem. Two methods are discussed. The first method replaces the discretized matrix form E \cdot H = R by the following problem. Minimize \|h_{1}\|+ \ldots + \|h_{n}\| subject to R - \lambda \leq E \cdot H \leq R + \lambda where \lambda is a column vector chosen sufficiently small to yield acceptable residuals, yet large enough to make the problem well-conditioned. This problem is converted to a linear programming problem so that the simplex algorithm can be used. The second method is to minimize \parallel E \cdot H - R \parallel^{2} +\lambda \parallel H \parallel^{2} where again \lambda is chosen small enough to yield acceptable residuals and large enough to make the problem well-conditioned. The method will be demonstrated with a Hilbert matrix inversion problem, and also by the deconvolution of the impulse response of a simple target from measured data. |
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| ISSN: | 0018-926X 1558-2221 |
| DOI: | 10.1109/TAP.1984.1143312 |