Monolithic intensity correction type lattice structure optical DOE device and design method thereof
A technology of lattice structure and design method, applied in optical components, optics, instruments, etc., can solve the problems of reducing the utilization rate of light energy, improving the difficulty of assembly alignment, etc., and achieves a simple structure, improved test accuracy, and uniform light intensity. Effect
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Embodiment 1
[0017] Example 1: The system uses a LD laser with a wavelength of 650 nm as the light source, and requires a structured light with a divergence angle of 35°×35°, a number of 900 points, and a regular arrangement of 30×30, and a working distance of 1m. First draw a dot matrix target map, with equal intensity distribution at each point. Adjust the light intensity and coordinates of each point based on the Rayleigh-Somurphy integration. The coordinate adjustment formula is as follows: x 2 =ax 1 ,y 2 =ay 1 ( z is 1m, ), the intensity adjustment formula is as follows: u(x 2 ,y 2 )=u(x 1 ,y 1 )k, The value changes continuously as the position changes. The target map after the coordinate and intensity correction is obtained, and the phase distribution of the diffraction element is obtained through iterative design. After the device is processed, the device is placed in the system for actual testing, and then the light intensity and position are optimized according to the test data...
Embodiment 2
[0018] Embodiment 2: The system uses an LD laser with a wavelength of 830 nm as the light source, and requires a divergence angle of 60°×40°, a number of 35,000 points, and a structured light that is completely randomly arranged, and the use distance is 5m. First draw a dot-matrix target map with equal intensity distribution at each point, such as figure 2 (a) Shown. Adjust the light intensity and coordinates of each point based on the Rayleigh-Somurphy integration. The coordinate adjustment formula is as follows x 2 =ax 1 ,y 2 =ay 1 ( z is 5m, ), the intensity adjustment formula is as follows: u(x 2 ,y 2 )=u(x 1 ,y 1 )k, k changes in stages with position changes: Then get the coordinate and intensity corrected target map, such as figure 2 (b) Shown. The phase distribution of the diffraction element is obtained by iterative design. After the device is processed, the device is placed in the system for actual testing, and then the light intensity and position are optimiz...
Embodiment 3
[0019] Embodiment 3: The system uses a Vcsel laser with a wavelength of 940 nm as the light source, and requires a divergence angle of 60°×60°, a number of points of 8,500, and a structured light that is completely randomly arranged, and the use distance is 2m. First draw a dot matrix target map, with equal intensity distribution at each point. Adjust the coordinates of each point in the dot matrix target map based on the Rayleigh-Somurphy integral, the formula is as follows: 2 =ax 1 ,y 2 =ay 1 ( z is 2m, ), the intensity will not be adjusted first. The phase distribution of the diffraction element is obtained by iterative design. The processed device is placed in the system for actual testing, and then the light intensity and position parameters are adjusted according to the test data to optimize the structure. Through 3 to 5 optimizations and feedback, the inconsistency of the center and edge responses of the receiver camera is overcome to obtain a lattice The structured l...
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