• Chinese Optics Letters
  • Vol. 17, Issue 9, 091901 (2019)
Li Zhang1、2, Fei Lin2, Xiaodong Qiu2, and Lixiang Chen2、*
Author Affiliations
  • 1School of Physics and Optoelectronic Engineering, Foshan University, Foshan 528000, China
  • 2Department of Physics, Collaborative Innovation Center for Optoelectronic Semiconductors and Efficient Devices, and Jiujiang Research Institute, Xiamen University, Xiamen 361005, China
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    DOI: 10.3788/COL201917.091901 Cite this Article Set citation alerts
    Li Zhang, Fei Lin, Xiaodong Qiu, Lixiang Chen. Full vectorial feature of second-harmonic generation with full Poincaré beams[J]. Chinese Optics Letters, 2019, 17(9): 091901 Copy Citation Text show less
    Experimental setup for SHG of FP beams in BBO crystals.
    Fig. 1. Experimental setup for SHG of FP beams in BBO crystals.
    Polarization and Stokes components for an output SHG light field with α=15°. The first and second rows show the experimental and theoretical results for the six polarization components, respectively. The third and fourth rows show the experimental and theoretical Stokes components, respectively.
    Fig. 2. Polarization and Stokes components for an output SHG light field with α=15°. The first and second rows show the experimental and theoretical results for the six polarization components, respectively. The third and fourth rows show the experimental and theoretical Stokes components, respectively.
    Polarization and Stokes components for an output SHG light field with α=30°. The first and second rows show the experimental and theoretical results for the six polarization components, respectively. The third and fourth rows show the experimental and theoretical Stokes components, respectively.
    Fig. 3. Polarization and Stokes components for an output SHG light field with α=30°. The first and second rows show the experimental and theoretical results for the six polarization components, respectively. The third and fourth rows show the experimental and theoretical Stokes components, respectively.
    Polarization distribution of SHG beams with 532 nm at α=0°, 15°, 30°, 45°, 60°, 75°, 90°. Top panel, numerical simulations of the polarization distribution of fundamental beams; middle panel, numerical simulations of the polarization distribution of SHG beams; bottom panel, experimental results of the polarization distribution of SHG beams.
    Fig. 4. Polarization distribution of SHG beams with 532 nm at α=0°, 15°, 30°, 45°, 60°, 75°, 90°. Top panel, numerical simulations of the polarization distribution of fundamental beams; middle panel, numerical simulations of the polarization distribution of SHG beams; bottom panel, experimental results of the polarization distribution of SHG beams.
    Streamlines around C points at α=30°. (a) Numerical result for fundamental FP beam; (b) and (c) numerical and experimental results of the SHG FP beam, respectively. Blue lines and red points denote the L lines and C points, respectively.
    Fig. 5. Streamlines around C points at α=30°. (a) Numerical result for fundamental FP beam; (b) and (c) numerical and experimental results of the SHG FP beam, respectively. Blue lines and red points denote the L lines and C points, respectively.
     States
    ElementsHVADRL
    HWP222.5°22.5°
    QWP445°45°
    Polarizer90°90°90°
    Table 1. Settings of the Optical Elements in the Setup to Detect the States of Polarization
    Li Zhang, Fei Lin, Xiaodong Qiu, Lixiang Chen. Full vectorial feature of second-harmonic generation with full Poincaré beams[J]. Chinese Optics Letters, 2019, 17(9): 091901
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