I am having a hard time understanding what should be a simple concept. I have constructed a vector in MATLAB that is real and symmetric. When I take the FFT in MATLAB, the result has a significant imaginary component, even though the symmetry rules of the Fourier transform say that the FT of a real symmetric function should also be real and symmetric. My example code:
N = 1 + 2^8;
k = linspace(-1,1,N);
V = exp(-abs(k));
Vf1 = fft(fftshift(V));
Vf2 = fft(ifftshift(V));
Vf3 = ifft(fftshift(V));
Vf4 = ifft(ifftshift(V));
Vf5 = fft(V);
Vf6 = ifft(V);
disp([isreal(Vf1) isreal(Vf2) isreal(Vf3) isreal(Vf4) isreal(Vf5) isreal(Vf6)])
Result:
0 0 0 0 0 0
No combinations of (i)fft or (i)fftshift result in a real symmetric vector. I've tried with both even and odd N (N = 2^8 vs. N = 1+2^8).
I did try looking at k+flip(k) and there are some residuals on the order of eps(1), but the residuals are also symmetric and the imaginary part of the FFT is not coming out as fuzz on the order of eps(1), but rather with magnitude comparable to the real part.
What blindingly obvious thing am I missing?
Blindingly obvious thing I was missing:
The FFT is not an integral over all space, so it assumes a periodic signal. Above, I am duplicating the last point in the period when I choose an even N, and so there is no way to shift it around to put the zero frequency at the beginning without fractional indexing, which does not exist.
A word about my choice of k. It is not arbitrary. The actual problem I am trying to solve is to generate a model FTIR interferogram which I will then FFT to get a spectrum. k is the distance that the interferometer travels which gets transformed to frequency in wavenumbers. In the real problem there will be various scaling factors so that the generating function V will yield physically meaningful numbers.
