“…In the case of a given pinhole size and an aberrated phase as shown in Figure 5 From Figure 5(b) it can be deduced that, by varying α, the intensity ratio of the two interfering beams can be adjusted in order to maximize the fringe contrast, which can reach unity in the case of any an input wavefront aberration. As a result, in the proposed common path PDI, the fringe contrast can be adjusted easily -whereas this is very difficult in many previous common path PDI systems [1,4,5,9,10].…”