• Chinese Optics Letters
  • Vol. 15, Issue 3, 030007 (2017)
Yuquan Zhang1、2, Xiujie Dou1, Yong Yang2, Chen Xie3, Jing Bu2、4、*, Changjun Min1, and Xiaocong Yuan1
Author Affiliations
  • 1Nanophotonics Research Centre, Shenzhen University & Key Laboratory of Optoelectronic Devices and Systems of Ministry of Education and Guangdong Province, College of Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, China
  • 2Key Laboratory of Optical Information Science and Technology of the Education Ministry of China, Institute of Modern Optics, Nankai University, Tianjin 300071, China
  • 3Ultrafast Laser Laboratory, Key Laboratory of Opto-electronic Information Technical Science of Ministry of Education, College of Precision Instruments and Opto-electronics Engineering, Tianjin University, Tianjin 300072, China
  • 4College of Mathematics and Statistics, Shenzhen University, Shenzhen 518060, China
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    DOI: 10.3788/COL201715.030007 Cite this Article Set citation alerts
    Yuquan Zhang, Xiujie Dou, Yong Yang, Chen Xie, Jing Bu, Changjun Min, Xiaocong Yuan. Flexible generation of femtosecond cylindrical vector beams (Invited Paper)[J]. Chinese Optics Letters, 2017, 15(3): 030007 Copy Citation Text show less
    Configuration of generation of negative first-order fs pulsed CVB. Any other orders can be generated by inserting the VR and 1/2λ plates. The blue arrows in the subgraph are the direction of the VR’s fast axis, and the black ones depict polarization of generated CVBs.
    Fig. 1. Configuration of generation of negative first-order fs pulsed CVB. Any other orders can be generated by inserting the VR and 1/2λ plates. The blue arrows in the subgraph are the direction of the VR’s fast axis, and the black ones depict polarization of generated CVBs.
    Detection of output fs pulsed CVBs. (a)–(d) polarization distribution of the first, second, third, and fourth-order fs pulsed CVBs, (e)–(h) the intensity distribution of CVBs, which are generally similar and donut-shaped but with different radius ratios, (i)–(l) petal intensity distribution of CVBs after a polarizer.
    Fig. 2. Detection of output fs pulsed CVBs. (a)–(d) polarization distribution of the first, second, third, and fourth-order fs pulsed CVBs, (e)–(h) the intensity distribution of CVBs, which are generally similar and donut-shaped but with different radius ratios, (i)–(l) petal intensity distribution of CVBs after a polarizer.
    Petal intensity distribution after the polarizer with different polarization angles (θ).
    Fig. 3. Petal intensity distribution after the polarizer with different polarization angles (θ).
    (a) Time domain comparison and (b) optical spectrum of the input beam and generated CVBs. The pulse is stretched by several fs for each optical component, and it only shows a slight difference in the spectral profile.
    Fig. 4. (a) Time domain comparison and (b) optical spectrum of the input beam and generated CVBs. The pulse is stretched by several fs for each optical component, and it only shows a slight difference in the spectral profile.
     Autocorrelation width/fsPower/mW
    Original beam52434.5
    1-order CVB58430.6
    −1-order CVB72425.9
    3-order CVB84419.7
    Table 1. Experimental Pulse Statistics of the Original and Generated Beams
    Yuquan Zhang, Xiujie Dou, Yong Yang, Chen Xie, Jing Bu, Changjun Min, Xiaocong Yuan. Flexible generation of femtosecond cylindrical vector beams (Invited Paper)[J]. Chinese Optics Letters, 2017, 15(3): 030007
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