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This intensity distribution is the intensity impulse response (sometimes called point spread function) of the optical system and fully characterizes that optical system.
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And when we do that, what happens is that we smear out the picture, or effectively convulve the impulses with the point spread function of the optical system.
The point spread function of the optical system was required for the FDR-deconvolution process described below.
Thus, the lens alone performs two main functions of the optical system.
Here, the use of pupil apodization, namely the manipulation of the amplitude and/or phase of the light at the pupil planes is explored as a means to narrow the point spread function (PSF) of the optical system.
A complete description of the receiver function is given as the convolution of this pinhole function with the incoherent-PSF of the optical system.
Subsequently, aberrations of the optical system could be simulated and corrected by adjusting the HOE function.
If the form of this function is known, then basic properties of the optical system (such as the directions of the emergent rays) can easily be obtained.
The multifunctional HOE maintains both the transmitting and receiving functions of the optical front end and is designed so that the alignment of the optical system is independent of small changes in the wavelength and temperature.
F, the coordinate system of the optical system.
BB contributed to the design of the optical system.
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