Measure the phase relative to propagation through the same geometrical thickness of air. If the lens's central thickness is , its spherical surface gives
The optical-path excess is , so the phase imparted by the lens is
The constant part is a spatially uniform phase. The physically important lens transmission is therefore with
One way to identify the focus is to append propagation to the on-axis point a distance away. Its path phase has the paraxial contribution , which cancels the lens phase. Thus all incident portions of a plane wave add with the same phase at that point. The diagram below shows the thickness change and both Fourier-transform arrangements.
Figure 1.
Quadratic thin-lens phase and two optical implementations of a scaled Fourier transform
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