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Non-Interferometric Phase Imaging Method Based on Synthetic Phase Transfer Function

A transfer function and synthetic phase technology, applied in the field of optical imaging, can solve problems that are difficult to predict, and achieve the effect of reducing the required time and quantity

Active Publication Date: 2019-05-07
NANJING UNIV OF SCI & TECH
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  • Abstract
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Problems solved by technology

Since then, Falaggis et al. proposed the optimal sampling interval selection method to select these non-equally spaced sampling plane positions (literature [4] K.Falaggis, T.Kozacki, and M.Kujawinska, "Optimum plane selection criteria for single-beamphase retrieval techniques based on the contrast transfer function."Opt.Lett.39,30–33(2014).), but this method must accurately select the optimal sampling under the premise of knowing the signal-to-noise ratio of the collected light intensity image interval, which is difficult to predict in practice

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  • Non-Interferometric Phase Imaging Method Based on Synthetic Phase Transfer Function
  • Non-Interferometric Phase Imaging Method Based on Synthetic Phase Transfer Function
  • Non-Interferometric Phase Imaging Method Based on Synthetic Phase Transfer Function

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Embodiment Construction

[0011] combine figure 1 , the present invention first uses the camera to take a group of light intensity images at different depths of objects distributed exponentially along the optical axis, and then assumes that the objects are weak absorption and weak phase, and solves the initial phase map according to the synthetic phase transfer function, and finally The initial phase map is substituted into the composite phase transfer function iterative compensation algorithm, and finally an accurate phase map is solved. The specific implementation steps are as follows:

[0012] Step 1: Use a camera to take a group of light intensity images at different depths that are exponentially spaced along the optical axis. The positions of these images in the direction of the optical axis are (0,±z 1 ,±z 2 ,±z 3 ,...,±z N ), where 0 represents the position of the focal plane, and the rest of the positions are calculated according to the following formula:

[0013]

[0014]

[0015] z...

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Abstract

The invention discloses a non-interferometric phase imaging method based on a blending phase transfer function. The method comprises the following steps: firstly shooting a group of light intensity images of an object at an optical axis direction of different depths with exponent interval distribution by a camera, then assuming that the object has a weak absorption and a weak phase, solving an initial phase diagram according to the blending phase transfer function, and finally substituting the initial phase diagram into a blending phase transfer function iterative compensation algorithm to solve an accurate phase diagram. The method is advantageous in that quantity of light intensity images needed for recovering phase is reduced, data acquisition time is reduced, the phase distribution of the object can be accurately recovered, and phase information of objects with weak absorption and weak phases as well as objects with strong absorption and large phases can be accurately established.

Description

technical field [0001] The invention belongs to optical imaging technology, in particular to a non-interference phase imaging method based on synthetic phase transfer function. Background technique [0002] For nearly transparent objects such as biological cells, phase information is very important. However, the phase information of an object cannot be directly captured by a camera. Therefore, in recent years, quantitative phase measurement has become a hot spot for researchers at home and abroad in the fields of surface detection, optical components, and biological cell microscopic imaging. At present, many methods of phase recovery have been developed, such as digital holography, phase shift interferometry, light intensity iterative method, light intensity transmission equation method, synthetic aperture scanning method and so on. Among these quantitative phase imaging methods, the light intensity transfer equation method has gained widespread attention due to its advanta...

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Application Information

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Patent Type & Authority Patents(China)
IPC IPC(8): G01N21/00
CPCG01N21/00
Inventor 陈钱孙佳嵩左超冯世杰顾国华张玉珍胡岩张良陶天阳李加基张佳琳孔富城林飞张敏亮范瑶
Owner NANJING UNIV OF SCI & TECH