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27 February 1984 Phase Unwrapping In Two Contexts
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Proceedings Volume 0373, Transformations in Optical Signal Processing; (1984) https://doi.org/10.1117/12.934551
Event: Transformations in Optical Signal Processing, 1981, Seattle, United States
Abstract
The ambiguity of the complex logarithm, whereby its imaginary part is only specified modulo 2r, poses a problem that often arises in diverse contexts. This article reports on the inadequacy of phase unwrapping in two separate contexts. One example occurs with image restoration that is intended to counteract the deleterious effects of at-mospheric turbulence. By tracking the positions (phases) of all the interference fringes that compose the image, the mean positions might be estimated. When only a few photons are available however, the resulting uncertainties sometimes lead to 27r slips that drastically upset the mean positions. A second example occurs in rotational synthesis, where the only available information lies on a single circle in the 2-D space-frequency complex domain. If it were possible to reliably unwrap the imaginary part of the logarithms around that circle, we could easily find the brightest point of the picture domain. The procedure attempts to trace a path as the source traverses interference fringes, without ever accidently slipping a fringe. In both examples, subsidiary contributions occasionally conspire to give the 27 slips. Smooth continuity is not quite sufficient as a basis for phase unwrapping. The problem is especially important because the character of images is more dependent on the phases of their Fourier components than on the amplitudes. Perhaps it will become possible to invoke other criteria than continuity for more reliable phase unwrapping.
© (1984) COPYRIGHT Society of Photo-Optical Instrumentation Engineers (SPIE). Downloading of the abstract is permitted for personal use only.
Lawrence Mertz "Phase Unwrapping In Two Contexts", Proc. SPIE 0373, Transformations in Optical Signal Processing, (27 February 1984); https://doi.org/10.1117/12.934551
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