Off-axis Fresnel numbers in laser systems

被引:3
|
作者
Yao, Yudong [1 ]
Zhang, Junyong [1 ]
Zhang, Yanli [1 ]
Bi, Qunyu [1 ]
Zhu, Jianqiang [1 ]
机构
[1] Chinese Acad Sci, Shanghai Inst Opt & Fine Mech, 390 Qinghe Rd, Shanghai 201800, Peoples R China
基金
中国国家自然科学基金;
关键词
correction factor; off-axis Fresnel number; off-axis optical system; Rayleigh-Sommerfeld diffraction integral;
D O I
10.1017/hpl.2014.22
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
The physical meaning and essence of Fresnel numbers are discussed, and two definitions of these numbers for off-axis optical systems are proposed. The universal Fresnel number is found to be N = (alpha(2) /lambda z) * C-1 + C-2. The Rayleigh-Sommerfeld nonparaxial diffraction formula states that a simple analytical formula for the nonparaxial intensity distribution after a circular aperture can be obtained. Theoretical derivations and numerical calculations reveal that the first correction factor C-1 is equal to cos theta and the second factor C-2 is a function of the incident wavefront and the shape of the diffractive aperture. Finally, some diffraction phenomena in off-axis optical systems are explained by the off-axis Fresnel number.
引用
收藏
页数:6
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