Intensity and phase distribution in deep Fresnel diffraction region generated by multi-pinhole aperture

Optik ◽  
2014 ◽  
Vol 125 (20) ◽  
pp. 6329-6334
Author(s):  
Man Liu
2014 ◽  
Vol 53 (29) ◽  
pp. 6920
Author(s):  
Qiaofeng Tan ◽  
Qixia Wang ◽  
Yue Fang ◽  
Huarong Gu ◽  
Guofan Jin

2010 ◽  
Vol 19 (12) ◽  
pp. 124202
Author(s):  
Hong-Sheng Song ◽  
Man Liu ◽  
Gui-Yuan Liu ◽  
Zhi-Wei Xu ◽  
Shu-Yun Teng ◽  
...  

2014 ◽  
Vol 63 (9) ◽  
pp. 094201
Author(s):  
Song Hong-Sheng ◽  
Zhuang Qiao ◽  
Liu Gui-Yuan ◽  
Qin Xi-Feng ◽  
Cheng Chuan-Fu

2007 ◽  
Vol 24 (6) ◽  
pp. 1656 ◽  
Author(s):  
Shuyun Teng ◽  
Xiaoyi Chen ◽  
Tongjun Zhou ◽  
Chuanfu Cheng

2015 ◽  
Vol 32 (10) ◽  
pp. 104209
Author(s):  
Shu-Na Jiang ◽  
Xing Li ◽  
Li Ma ◽  
Ya-Ru Gao ◽  
Wei-Ling Gui ◽  
...  

2013 ◽  
Vol 859 ◽  
pp. 453-456
Author(s):  
Huai Sheng Wang

Our analysis is based on the pure phase distribution equations of the Fresnel diffraction of an amplitude grating. Suppose P and M are positive integers which have no common divisor and 1/M is the opening ratio of the amplitude grating. Characteristics of the pure distributions are analysed. For instance at the fractional P/2M Talbot distance and (1-P/2M) Talbot distance, the amplitudes of the Fresnel diffraction field of the grating are the same while the phases are opposite. As an example we design two Talbot illuminators which phase distributions occur respectively at the fractional P/2M and (1-P/2M ) Talbot distance. Both phase distribution can carry out illumination behind them. Array illumination has important application in information optics


2012 ◽  
Vol 61 (7) ◽  
pp. 074201
Author(s):  
Chen Xiao-Yi ◽  
Liu Man ◽  
Li Hai-Xia ◽  
Zhang Mei-Na ◽  
Song Hong-Sheng ◽  
...  

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