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A phase recovery image reproduction method for lensless imaging

A phase recovery, lensless technology, applied in image data processing, 2D image generation, optics, etc., can solve the problem of not being able to restore the target image, etc., and achieve less computing time, clear recovery targets, and simple and easy-to-operate experimental equipment Effect

Inactive Publication Date: 2019-03-15
CHANGSHA UNIVERSITY OF SCIENCE AND TECHNOLOGY
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Problems solved by technology

[0005] Aiming at the problems existing in the prior art, the present invention proposes a phase recovery image reproduction method without lens imaging, which solves the diffraction limit problem encountered in the construction of the optical system in the prior art, and also solves the stagnation of the IFT algorithm in the iterative process. The problem that a certain local minimum value cannot restore the target image has achieved the effect of simple and easy to operate experimental equipment, less computing time in the iterative process, and a clear restored target

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  • A phase recovery image reproduction method for lensless imaging
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  • A phase recovery image reproduction method for lensless imaging

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Embodiment Construction

[0021] The present invention will be described in detail below in conjunction with the accompanying drawings and specific embodiments.

[0022] The present invention is a simple optical device based on CDI to obtain a power spectrum diagram, and the experimental principle diagram is as follows figure 1 As shown, a beam of laser beam is collimated and expanded, irradiates the target, passes through a Fourier lens, and uses a camera at the focal length f to receive the spectrogram of the target. In the experiment, a laser with collimated beam expansion is used, and red light (λ=632.8nm) is used to irradiate the target object. The light source for illuminating the object is parallel light, and the object can be placed in any one between the Fourier lens and the light source. After the laser irradiates the target, it passes through the Fourier lens to obtain the spectrum of the target in the Fourier domain, and then collect it with a CCD without an imaging lens. The distance betwe...

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Abstract

The invention provides a phase recovery image reproduction method for lensless imaging, Fast power spectra were captured by the experimental device of coherent diffraction imaging, the imaging devicerequires only one collimated beam-spreading laser, A Fourier lens and a CCD detector, the detected power spectrum is reconstructed in three steps, the first step is to calculate an initial phase by using a hybrid input-output algorithm, Soft aperture scanning is then performed, instead of scanning in the target plane and the spatial spectral plane, The second step combines the Ptychography algorithm to enhance the Fourier domain constraints, and uses the phase iterative restoration algorithm to achieve the reconstruction of the target image. In the third step, in order to further reduce the normalized root mean square error, the error reduction algorithm is used to reconstruct the target image. The imaging device of the invention is simple, and the algorithm can quickly reconstruct an accurate target image from a power spectrum diagram, thereby realizing the function of image reproduction.

Description

technical field [0001] The invention relates to the field of coherent diffraction imaging, in particular to a phase recovery image reproduction method for lensless imaging. Background technique [0002] In practical situations, the image directly measured is often only the intensity distribution of the wave field, and the phase distribution of the wave field is often difficult to measure directly, or even impossible. Therefore, recovering phase information from intensity measurement data has been researched in recent years. The hotspot, phase recovery algorithm is such a method of deriving the amplitude and phase of the radiation source from the intensity measurement data. [0003] At present, there are two commonly used phase recovery methods, one is to use a phase difference sensor (specifically, a wavefront sensor can be used) to directly detect the phase difference of the optical system, and the other is to use the Gerchberg–Saxton (GS) algorithm to The optimal theoreti...

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Application Information

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Patent Type & Authority Applications(China)
IPC IPC(8): G06T11/00G02B27/00
CPCG02B27/0012G06T11/00
Inventor 王威郭艳芳唐武盛李修建李梦竹王新衣文军朱梦筠付美城王潇春聂倩雯
Owner CHANGSHA UNIVERSITY OF SCIENCE AND TECHNOLOGY
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