Wavefront Testing of Large-Aperture Continuous Phase Plate

2010 ◽  
Vol 37 (3) ◽  
pp. 809-814
Author(s):  
柴立群 Chai Liqun ◽  
于瀛洁 Yu Yingjie ◽  
石琦凯 Shi Qikai ◽  
许乔 Xu Qiao ◽  
温圣林 Wen Shenglin ◽  
...  
2013 ◽  
Vol 25 (12) ◽  
pp. 3329-3332
Author(s):  
颜浩 Yan Hao ◽  
杨春林 Yang Chunlin ◽  
石琦凯 Shi Qikai ◽  
温圣林 Wen Shenglin ◽  
嵇保健 Ji Baojian

2018 ◽  
Vol 16 (10) ◽  
pp. 102201 ◽  
Author(s):  
Xing Su Xing Su ◽  
Longguang Xia Longguang Xia ◽  
Kan Liu Kan Liu ◽  
Peng Zhang Peng Zhang ◽  
Ping Li Ping Li ◽  
...  

Micromachines ◽  
2021 ◽  
Vol 12 (6) ◽  
pp. 683
Author(s):  
Huiliang Jin ◽  
Caixue Tang ◽  
Haibo Li ◽  
Yuanhang Zhang ◽  
Yaguo Li

The continuous phase plate (CPP) is the vital diffractive optical element involved in laser beam shaping and smoothing in high-power laser systems. The high gradients, small spatial periods, and complex features make it difficult to achieve high accuracy when manufacturing such systems. A high-accuracy and high-efficiency surface topography manufacturing method for CPP is presented in this paper. The atmospheric pressure plasma jet (APPJ) system is presented and the removal characteristics are studied to obtain the optimal processing parameters. An optimized iterative algorithm based on the dwell point matrix and a fast Fourier transform (FFT) is proposed to improve the accuracy and efficiency in the dwell time calculation process. A 120 mm × 120 mm CPP surface topography with a 1326.2 nm peak-to-valley (PV) value is fabricated with four iteration steps after approximately 1.6 h of plasma processing. The residual figure error between the prescribed surface topography and plasma-processed surface topography is 28.08 nm root mean square (RMS). The far-field distribution characteristic of the plasma-fabricated surface is analyzed, for which the energy radius deviation is 11 μm at 90% encircled energy. The experimental results demonstrates the potential of the APPJ approach for the manufacturing of complex surface topographies.


2009 ◽  
Vol 58 (5) ◽  
pp. 3130
Author(s):  
Yao Xin ◽  
Gao Fu-Hua ◽  
Zhang Yi-Xiao ◽  
Wen Sheng-Lin ◽  
Guo Yong-Kang ◽  
...  

2010 ◽  
Vol 22 (11) ◽  
pp. 2634-2638
Author(s):  
林中校 Lin Zhongxiao ◽  
张蓉竹 Zhang Rongzhu ◽  
杨春林 Yang Chunlin ◽  
许乔 Xu Qiao

2014 ◽  
Vol 26 (10) ◽  
pp. 102003
Author(s):  
肖谦裔 Xiao Qianyi ◽  
吕晨 Lü Chen ◽  
张蓉竹 Zhang Rongzhu

2013 ◽  
Vol 25 (12) ◽  
pp. 3205-3209
Author(s):  
李强 Li Qiang ◽  
徐凯源 Xu Kaiyuan ◽  
刘昂 Liu Ang ◽  
何宇航 He Yuhang ◽  
高波 Gao Bo

2012 ◽  
Vol 24 (10) ◽  
pp. 2296-2300 ◽  
Author(s):  
温圣林 Wen Shenglin ◽  
石琦凯 Shi Qikai ◽  
颜浩 Yan Hao ◽  
张远航 Zhang Yuanhang ◽  
杨春林 Yang Chunlin ◽  
...  

1979 ◽  
Vol 1 (4) ◽  
pp. 325-332
Author(s):  
Gerard A. Alphonse ◽  
David Vilkomerso

In reflective imaging, waves must be scattered by the object over a broad solid angle so that some of the reflected waves impinge upon the collecting aperture. Surfaces such as biological specimens under study in acoustic imaging are considered smooth at the wavelengths used (e.g., 1 mm) and therefore act as specular reflectors. In order to obtain reflection over a broad spatial range, large aperture, sector or compound scanning are used. In certain types of systems, diffuse insonification is sometimes used by imaging a raster of random phase points onto the surface. However interference between the waves from these point sources produces random fringes or “speckle-like” patterns overlaying the image. In optics these fringes have been reduced by rotating the diffuser. A similar approach has been taken here. This paper describes a simple random phase plate having two levels, 0° and 180 phase that can, by rotation, change the relative phases of the diffuse insonification points so as to reduce the speckle-like effect in the image. The temporal bandwidth of the random phase plate is narrow because of standing waves in it. To reduce standing waves the diffuser is intimately coupled to a wedged transducer. This combination is used to obtain diffuse insonification with broad spatial and temporal bandwidth.


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