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METHOD FOR IMAGING TARGET OBJECT WITHIN MEDIA WHICH BRING ABOUT SIMULTANEOUSLY SCATTERING AND ABERRATION
METHOD FOR IMAGING TARGET OBJECT WITHIN MEDIA WHICH BRING ABOUT SIMULTANEOUSLY SCATTERING AND ABERRATION
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机译：在同时散射和像差的媒体中对目标对象成像的方法
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摘要
The present invention relates to a method of imaging a target object in a medium that causes both scattering and aberration, comprising the steps of: (a) obtaining a plurality of outgoing beams emitted from the target object while varying the incident angle of the incident beam; (b) constructing a time-division output matrix composed of an incident wave vector of the incident beam and an output wave vector of the output beam; (c) reconstructing the time-divisional output matrix into an incident path aberration correction matrix composed of the difference between the exit wave vector and the incident wave vector and the incident wave vector; (d) calculating an optimum incident path aberration correction set in which the incident path aberration correction set is reflected in the incident path aberration correction matrix and a complex sum total intensity of a difference spectrum between the outgoing beam and the incident beam is maximum; (e) correcting the time-division output matrix using the optimal incident path aberration correction set; (f) reconstructing the time-divisional emission matrix corrected in step (e) into an emission-path aberration correction matrix composed of the difference between the emission-wave vector, the incident-wave vector and the emission-wave vector; (g) an output path aberration correction set is reflected in the emission path aberration correction matrix, and an optimum sum of the sum of the sum of the spectra of the difference between the incident beam and the output beam in the opposite phase corresponding to the emission path aberration correction matrix An emission path aberration correction set is calculated; (h) correcting the time-division output matrix corrected in the step (e) using the optimal output path aberration correction set; (i) an image is obtained by accumulation of the same outgoing beam components in the time-division output matrix corrected in the step (h).
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