diffractive optical element
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2021 ◽  
Author(s):  
Elias Scharf ◽  
Mariana Medina-Sanchez ◽  
Robert Kuschmierz ◽  
Oliver G. Schmidt ◽  
Jürgen W. Czarske

2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Mei-Li Hsieh ◽  
Thomas D. Ditto ◽  
Yi-Wen Lee ◽  
Shiuan-Huei Lin ◽  
Heidi J. Newberg ◽  
...  

AbstractA highly dispersive, diffractive optical element is designed and realized for an extremely high spectral resolution spectroscopy for exoplanet telescope application. Our design uses an annular Fresnel hologram to transform incident starlight directly into a spectrogram. The recording of the hologram is accomplished using two spherical waves of different radius of curvature. The resultant hologram consists of an annular grating structure with a gradually shrinking period as a function of increasing radius. The variable period not only could bring the incoming star-light into focus, but also exhibits a large on-axis chromatic behavior. We demonstrate a dispersion of wavelength 430–700 nm over 190 mm on-axis distance, leading to a super fine spectral resolution 0.0266 nm at wavelength 515 nm for a detector size of 20 µm.


2021 ◽  
pp. 127340
Author(s):  
Bo Zhang ◽  
Keyan Dong ◽  
Mingxu Piao ◽  
Jianing Wang ◽  
Ru Jia ◽  
...  

Laser Physics ◽  
2021 ◽  
Vol 31 (8) ◽  
pp. 086001
Author(s):  
Yunfei Zhang ◽  
Wenzhi Qin ◽  
Liang Wang ◽  
Feiliang Chen ◽  
Xin Huang ◽  
...  

Photonics ◽  
2021 ◽  
Vol 8 (6) ◽  
pp. 204
Author(s):  
Di Wang ◽  
Yi-Wei Zheng ◽  
Nan-Nan Li ◽  
Qiong-Hua Wang

In this paper, a holographic system to suppress the speckle noise is proposed. Two spatial light modulators (SLMs) are used in the system, one of which is used for beam shaping, and the other is used for reproducing the image. By calculating the effective viewing angle of the reconstructed image, the effective hologram and the effective region of the SLM are calculated accordingly. Then, the size of the diffractive optical element (DOE) is calculated accordingly. The dynamic DOEs and effective hologram are loaded on the effective regions of the two SLMs, respectively, while the wasted areas of the two SLMs are performed with zero-padded operations. When the laser passes through the first SLM, the light can be modulated by the effective DOEs. When the modulated beam illuminates the second SLM which is loaded with the effective hologram, the image is reconstructed with better quality and lower speckle noise. Moreover, the calculation time of the hologram is reduced. Experiments indicate the validity of the proposed system.


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