Fourier says that any (non-pathological) waveform can be decomposed into a bunch of sinewaves. The FFT does that for reasonable samples of a given waveform.
So your FFT results are the coefficients of each sinewave sub-component: the first for 0 Hz (or DC, or sum), the 2nd for a sinewave of 1 period per aperture, the next: 2 cycles per aperture, and etc. You can consider each coefficient pair x+iy, as either a vector in the complex plane for a sinewave's magnitude and phase, or as multipliers for a cosine and a sine that sum up to another sinewave of a specified phase.