TL;DR: In this article, the phase reconstruction problem for wave amplitude and coherence functions was studied and a survey of specific inverse problems was presented. But the phase recovery problem was not addressed in this paper.
Abstract: 1. Introduction.- 1.1 Direct and Inverse Problems in Optical Physics.- 1.2 Role of Prior Knowledge.- 1.3 Survey of Specific Inverse Problems.- 1.4 Notati on i n Coherence Theory.- References.- 2. The Phase Reconstruction Problem for Wave Amplitudes and Coherence Functions.- 2.1 Phase Reconstruction for Wave Ampl i tudes.- 2.1.1 Relevance of the Phase Problem for Object Structure Determi nation.- 2.1.2 Derivation of the Basic Equations Governing the Phase Probl em.- 2.1.3 General Considerations on the Phase Problem.- 2.1.4 Greenaway's Proposal for Phase Recovery from a Single Intensity Distribution.- 2.1.5 The Method of Half-Plane Apertures for Semi-Weak Objects.- 2.1.6 The Logarithmic Hilbert Transform: Methods for Circumventing Complications Due to Zeros.- 2.1.7 Phase Retrieval for Strong Objects from Two Defocused Images.- 2.1.8 Phase Retrieval from the Intensity Distributions in Exit Pupil and Image Plane.- 2.1.9 Phase Retrieval from Two Defocused Images for Semi-Weak Objects.- 2.2 Phase Reconstruction for Coherence Functions.- 2.2.1 Phase Determination of Optical Coherence Functions.- 2.2.2 Determination of the Phase of the Spatial Coherence Function with an Incoherent Reference Point Source.- 2.2.3 Determination of the Phase of the Spatial Coherence Function with an Exponential Filter.- 2.2.4 Determination of the Phase of the Spatial Coherence Function from the Intensity in the Fraunhofer Plane.- References.- 3. The Uniqueness of Inverse Problems.- 3.1 Summary of Inverse Problems.- 3.1.1 Inverse Sturm-Liouville Problems.- 3.1.2 Reconstruction Problems.- 3.1.3 Three-Dimensional Reconstruction from Projections.- 3.2 Inverse Diffraction.- 3.2.1 Inverse Diffraction from Far-Field Data.- 3.2.2 Inverse Diffraction from Spherical Surface to Spherical Surface.- 3.2.3 Inverse Diffraction from Plane to Plane.- 3.2.4 Generalization to Arbitrary Surfaces.- 3.2.5 The Determination of the Shape of a Scatterer from Far-Field Data.- 3.3 Non-Radiating Sources.- 3.3.1 Early Results and Special Cases.- 3.3.2 General Theory.- 3.3.3 Integral Equations and Uniqueness by Prior Knowledge.- 3.4 The Determination of an Object from Scattering Data.- 3.4.1 Examples of Nonuniqueness.- 3.4.2 Phase Shift Analysis and the Reconstruction of a Potential.- 3.4.3 The Determination of a Potential or Index of Refraction from the Scattered Fields Generated by a Set of Monochromati c PIane Waves.- 3.4.4 The Unique Determination of an Object from Scattering Data.- 3.4.5 The Analytical Continuation of the Electromagnetic Field from the Exterior to the Interior of a Scatterer and Its Physical Implications.- References.- 4. Spatial Resolution of Subwavelength Sources from Optical Far-Zone Data.- 4.1 Approaches to Superresolution.- 4.1.1 Array of Sources with Known Radiation Pattern.- 4.1.2 Superresolution Using Evanescent Waves.- 4.1.3 x-Locali zed Sources.- 4.2 Partial Waves Associated with Complex Spatial Frequencies.- 4.3 Representations and Expansions of the EM Field.- 4.3.1 Integral Representations.- 4.3.2 Partial-Wave Representation of Exterior Field.- 4.3.3 Multipole Waves.- 4.3.4 Plane Waves.- 4.4 Band-Limiting at Variance with X-Localized Sources.- 4.5 High-Frequency Information in the Far Zone Given a X-Localized Source.- 4.6 X-Localized Sources Reconstructed from Far-Zone Data.- 4.7 Measurement of Phase and Magnitude of the Optical Radiation Pattern.- 4.8 Discussion.- References.- 5. Radiometry and Coherence.- 5.1 The Development of Radiometry.- 5.1.1 The Classical Period.- 5.1.2 The Baroque Period.- 5.1.3 The Modern Period.- 5.2 Coherence of Blackbody Radiation.- 5.2.1 Temporal Coherence.- 5.2.2 Spatial Coherence.- 5.3 First-Order Radiometry.- 5.3.1 Energy Flow in Scalar Fields.- 5.3.2 Coherence Theory and the Radiometrie Quantities.- 5.3.3 The Van Cittert-Zernike Theorem.- 5.3.4 An Example: Quasi stationary Sources.- 5.4 Radiant Intensity and Angular Coherence.- 5.4.1 Source Models.- 5.4.2 Inverse Relations.- 5.4.3 Bessel-Correlated Sources.- 5.4.4 Gauss-Correlated Sources.- 5.4.5 An Application: Coherence of Thermionic Sources.- 5.5 Radiation Efficiency.- 5.5.1 Radiance of Model Sources.- 5.5.2 Emittance and Radiation Efficiency.- 5.5.3 Exampl es.- 5.6 Second-Order Radiometry.- 5.6.1 Radiant Intensity Fluctuation and Autocorrelation.- 5.6.2 Second-Order Radiometric Quantities.- 5.6.3 An Example: Gauss-Correlated Chaotic Source.- References.- 6. Statistical Features of Phase Screens from Scattering Data.- 6.1 Basic Formulation of the Statistical Problem.- 6.1.1 Physical Models.- 6.1.2 Characteristic Functional of the Scattered Light.- 6.1.3 Correlation Functions.- 6.1.4 Gaussian Limit.- 6.2 More General Detection and Coherence Conditions.- 6.2.1 Gaussian Scattered Field.- 6.2.2 Polychromatic Speckle Patterns.- 6.3 Amplitude and Intensity Correlations.- 6.3.1 Information Contained in Amplitude Correlations.- 6.3.2 Information Contained in Intensity Correlations.- 6.3.3 Moving Diffusers.- 6.4 Number-Dependent Effects.- 6.4.1 Moments and Probability Distribution of Intensity.- 6.4.2 Examples.- 6.4.3 Applications.- 6.5 Concluding Remarks.- References.- Additional References with Titles.
TL;DR: In this paper, the phase retrieval problem in geometrical optics is shown to possess a unique solution within the framework of the diffraction theory of image formation, and a simple proof and example of the nonuniqueness of phase retrieval in this limit is presented.
Abstract: The treatment of the problem of deducing the phase of an optical wavefield from image- and diffraction-plane intensity measurements recently presented by Robinson [ J. Opt. Soc. Am68, 87– 92 ( 1968)] is shown to be valid only in the limit of geometrical optics. A simple proof and example of the nonuniqueness of the phase retrieval problem in this limit is presented. It is argued that although the phase retrieval is not unique in the geometrical optics limit it does appear to possess a unique solution within the framework of the diffraction theory of image formation.