• Laser & Optoelectronics Progress
  • Vol. 56, Issue 24, 240602 (2019)
Yuhao Wang**, Yan Xiao*, Xiaoqin Bai, and Jing Zhang
Author Affiliations
  • College of Physics and Electronics Engineering, Shanxi University, Taiyuan, Shanxi 030006, China
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    DOI: 10.3788/LOP56.240602 Cite this Article Set citation alerts
    Yuhao Wang, Yan Xiao, Xiaoqin Bai, Jing Zhang. Optical Field Rotation of Finite Energy Airy-Hermite-Gaussian Beams in Medium with Potential Well[J]. Laser & Optoelectronics Progress, 2019, 56(24): 240602 Copy Citation Text show less
    Intensity distributions of FEAHG beams. (a1)-(a6) α=0; (b1)-(b6) α=0.3; (c1)-(c6) α=0.4; (d1)-(d6) α=0.5
    Fig. 1. Intensity distributions of FEAHG beams. (a1)-(a6) α=0; (b1)-(b6) α=0.3; (c1)-(c6) α=0.4; (d1)-(d6) α=0.5
    Propagation distance for optical structure rotation versus intensity of potential well
    Fig. 2. Propagation distance for optical structure rotation versus intensity of potential well
    Diagrams of incidence of FEAHG beams. (a) n=2; (b) n=3
    Fig. 3. Diagrams of incidence of FEAHG beams. (a) n=2; (b) n=3
    Intensity distributions of FEAHG beams. (a1)-(a6) n=2; (b1)-(b6) n=3
    Fig. 4. Intensity distributions of FEAHG beams. (a1)-(a6) n=2; (b1)-(b6) n=3
    Intensity distributions of FEAHG beams. (a1)-(a6) θ=0, B=0; (b1)-(b6) θ=0, B=1; (c1)-(c6) θ=0, B=2; (d1)-(d6) θ=π, B=2
    Fig. 5. Intensity distributions of FEAHG beams. (a1)-(a6) θ=0, B=0; (b1)-(b6) θ=0, B=1; (c1)-(c6) θ=0, B=2; (d1)-(d6) θ=π, B=2
    Yuhao Wang, Yan Xiao, Xiaoqin Bai, Jing Zhang. Optical Field Rotation of Finite Energy Airy-Hermite-Gaussian Beams in Medium with Potential Well[J]. Laser & Optoelectronics Progress, 2019, 56(24): 240602
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