Figure 13

Holograms of the USAF target with maximum path difference. The upper line shows holograms of the random multiplexing method with phase shifts of (a) θ = 0, (b) 2π/3 and (c) 4π/3, (d) phase, (e) magnitude, of the complex hologram and (f) reconstructed image of the USAF target. Holograms of the TAP- GSA method with phase shifts of (g) θ = 0, (h) 2π/3 and (i) 4π/3, (j) phase, (k) magnitude, of complex hologram, and (l) reconstructed image of the pinhole. Holograms of the polarization multiplexing method with phase shifts of (m) θ = 0, (n) 2π/3 and (o) 4π/3, (p) phase, (q) magnitude, of the complex hologram, and (r) reconstructed image of the USAF object.