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),

D( k,k )=λ( k )= i=0 M1 h e ( i )exp( j 2π M ki )=MH( k )k=0,1,...,M1( 4.33 )

where H(k) is the Fourier transforms of the extended sequences he(x).

Combining eq. (4.31) to eq. (4.33) yields

G( k )=M×H( k )F( k )k=0,1,...,M1( 4.34 )

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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