Perfect optical vortex array with controllable diffraction order and topological charge

2016 ◽  
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pp. 1836 ◽  
Author(s):  
Shiyao Fu ◽  
Tonglu Wang ◽  
Chunqing Gao
2009 ◽  
Vol 17 (17) ◽  
pp. 14517 ◽  
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Kazuhiko Oka ◽  
Ryuji Morita

2009 ◽  
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Author(s):  
Valeria Garbin ◽  
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Michel Versluis ◽  
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2021 ◽  
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Hengfei ZHANG ◽  
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liantuan xiao ◽  
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2016 ◽  
Vol 40 (6) ◽  
pp. 781-792 ◽  
Author(s):  
V. V. Kotlyar ◽  
A. A. Kovalev ◽  
A. P. Porfirev

2019 ◽  
Vol 48 (7) ◽  
pp. 726001
Author(s):  
任斐斐 REN Fei-fei ◽  
梁言生 LIANG Yan-sheng ◽  
蔡亚楠 CAI Ya-nan ◽  
何旻儒 HE Min-ru ◽  
雷铭 LEI Ming ◽  
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2019 ◽  
Vol 9 (19) ◽  
pp. 3956
Author(s):  
Wang ◽  
Huang ◽  
Toyoda ◽  
Liu

A generalized contour-sum method has been proposed to measure the topological charge (TC) of an optical vortex (OV) beam using a Shack–Hartmann wavefront sensor (SH-WFS). Moreover, a recent study extended it to be workable for measuring an aberrated OV beam. However, when the OV beam suffers from severe distortion, the closed path for circulation calculation becomes crucial. In this paper, we evaluate the performance of five closed path determination methods, including watershed transformation, maximum average-intensity circle extraction, a combination of watershed transformation and maximum average-intensity circle extraction, and perfectly round circles assignation. In the experiments, we used a phase-only spatial light modulator to generate OV beams and aberrations, while an SH-WFS was used to measure the intensity profile and phase slopes. The results show that when determining the TC values of distorted donut-shaped OV beams, the watershed-transformed maximum average-intensity circle method performed the best, and the maximum average-intensity circle method and the watershed transformation method came second and third, while the worst was the perfect circles assignation method. The discussions that explain our experimental results are also given.


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