The general principle of a Fresnel lens is as follows.
- Imagine a flat pane of glass centred on an optical axis and another point P, also located on the optical axis.
- The distance between any point on the glass pane (call it X) and the point P will depend on the axial height of X (i.e. the distance from X to the optical axis).
- This path difference corresponds to a phase difference.
- The phase will alternate between being positive and negative as X moves outward from the optical axis.
- We can thus define zones of positive and negative phase contributions to the glass pane. This is the origin of Fresnel zones.
- Now, we can make a lens by preventing light from going through every second Fresnel zone. This ensures that the phase contribution at point P will only be positive (or negative), resulting in a focusing effect being obtained when a plane wave is passed through the glass pane.
- There are alternate ways to achieve this effect, for example adjusting the thickness of the glass pane in different Fresnel zones will achieve a similar effect.
- The distance between the glass pane and the point P is determined by the width of the Fresnel zones. This is in contrast to ordinary lens where the focal length depends on the curvature of the lens surface.
Re: the "theoretically limitless" part on the wikipedia articles, I think, given the context, it is saying that there are an unlimited number of Fresnel zones. A real lens, however will only span a finite number of these zones.
Claude.