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Diffraction field computation from arbitrarily distributed data points in space

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Fig. 1. The vectors k 1 and k 2 are the wave vectors of the plane waves.
Fig. 4 shows how convergence to the intersection is achieved by iterative projections onto the individual convex sets
Fig. 5. Initial diffraction field over the entire 2D space; N ¼ 256 samples per line (a) and reconstructed diffraction fields from s known data points (b)–(e); (b) matrix inversion method with s ¼ 230; (c) matrix inversion method with s ¼ 282; (d) POCS algor
Fig. 6. Normalized errors for different numbers of known samples at 200 iterations. 150135120105907560453015 0 0 1 2 3 4 5 6 7 8 s / Nnit 9 10 11 12 13 14 15 16

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