F(k) and G(k) are the Fourier transforms of the extended sequences fe(x) and ge(x), respectively.
The diagonal elements of D in eq. (4.30) are the eigenvalues of H. Following eq. (4.23),
where H(k) is the Fourier transforms of the extended sequences he(x).
Combining eq. (4.31) to eq. (4.33) yields
The right side of eq. (4.34) is the convolution of fe(x) and he(x) in the frequency domain. It can be calculated with the help of FFT.
Now, consider the 2-D cases (with noise). Taking eq. (4.28) into eq. (4.20), and multiplying both sides by W
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