2008
DOI: 10.1364/josaa.25.000742
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Lensless coherent imaging by a deterministic phase retrieval method with an aperture-array filter

Abstract: Recently we have proposed a noniterative and analytic phase retrieval method using the filter of an aperture array to reconstruct a complex-valued object from a diffraction intensity pattern [Phys. Rev. Lett.98, 223901 (2007)], but this method suffers from the restriction of the far-field condition of two distances between the object and the filter and between the filter and the detector for the intensity measurement. An improved method, which extends the adaptable condition of those distances to the region of… Show more

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Cited by 15 publications
(24 citation statements)
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“…As described in the previous paper [13], the diffraction pattern of each aperture in the detector plane is isolated approximately from those of the adjoining square if the parameters of the measurement system (i.e., z, l, w and d) satisfy a condition d1 l∕z > ε2λl∕w lσ j ∕z, (j u, v), where d1 l∕z denotes the array's period in the detector plane given from the geometrical optics prediction for the wave propagation from the small object, 2λl∕w lσ j ∕z(in which σ j is the extent of the object function in the direction of u or v) represents the main width of the diffraction pattern of each square aperture in the case of the far-field diffraction, and ε indicates a safety factor larger than unity for increase of the main width due to the phase variation of the wavefront inside each aperture. Note that this is not a necessary condition but a sufficient one.…”
Section: Outline Of the Reconstruction Methodsmentioning
confidence: 95%
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“…As described in the previous paper [13], the diffraction pattern of each aperture in the detector plane is isolated approximately from those of the adjoining square if the parameters of the measurement system (i.e., z, l, w and d) satisfy a condition d1 l∕z > ε2λl∕w lσ j ∕z, (j u, v), where d1 l∕z denotes the array's period in the detector plane given from the geometrical optics prediction for the wave propagation from the small object, 2λl∕w lσ j ∕z(in which σ j is the extent of the object function in the direction of u or v) represents the main width of the diffraction pattern of each square aperture in the case of the far-field diffraction, and ε indicates a safety factor larger than unity for increase of the main width due to the phase variation of the wavefront inside each aperture. Note that this is not a necessary condition but a sufficient one.…”
Section: Outline Of the Reconstruction Methodsmentioning
confidence: 95%
“…In this section, a summary of the object reconstruction method by use of the array filter [12,13] is described for the sake of readability. Figure 1 shows a schematic diagram of the optical system used in the experiment as described in the following section.…”
Section: Outline Of the Reconstruction Methodsmentioning
confidence: 99%
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