• Chinese Journal of Lasers
  • Vol. 48, Issue 13, 1308001 (2021)
Tao Wang, Cheng Lian, Liankai Wang, Kewei Huan, Yining Mu, and Weijun Chen*
Author Affiliations
  • School of Science, Changchun University of Science and Technology, Changchun, Jilin 130022, China
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    DOI: 10.3788/CJL202148.1308001 Cite this Article Set citation alerts
    Tao Wang, Cheng Lian, Liankai Wang, Kewei Huan, Yining Mu, Weijun Chen. Interaction of Airy Beams and Soliton in Saturable Nonlinear Medium[J]. Chinese Journal of Lasers, 2021, 48(13): 1308001 Copy Citation Text show less
    Transmission evolution diagrams of light beam in different media. (a) FEAB in free space; (b) soliton in saturated nonlinear medium
    Fig. 1. Transmission evolution diagrams of light beam in different media. (a) FEAB in free space; (b) soliton in saturated nonlinear medium
    Interaction between FEAB and soliton at different phase differences. (a) Q=0; (b) Q=π
    Fig. 2. Interaction between FEAB and soliton at different phase differences. (a) Q=0; (b) Q
    Propagation of breathing soliton with different phase differences. (a) Q=-π/2; (b) Q=π/2
    Fig. 3. Propagation of breathing soliton with different phase differences. (a) Q=-π/2; (b) Q=π/2
    Variation curves of characteristic parameters of the breathing soliton. (a) Oscillation transmission diagram of the breathing soliton; (b) variation curve of the average peak intensity of the breathing soliton with R when Q=0; (c) variation curve of the average peak intensity of the breathing soliton with R when Q=π; (d) peak position of breathing soliton under different phase differences
    Fig. 4. Variation curves of characteristic parameters of the breathing soliton. (a) Oscillation transmission diagram of the breathing soliton; (b) variation curve of the average peak intensity of the breathing soliton with R when Q=0; (c) variation curve of the average peak intensity of the breathing soliton with R when Q=π; (d) peak position of breathing soliton under different phase differences
    Interaction of strong energy FEAB and soliton. (a) Intensity ratio is 50%, Q=0; (b) intensity ratio is 100%, Q=0; (c) intensity ratio is 50%, Q=π; (d) intensity ratio is 100%, Q=π
    Fig. 5. Interaction of strong energy FEAB and soliton. (a) Intensity ratio is 50%, Q=0; (b) intensity ratio is 100%, Q=0; (c) intensity ratio is 50%, Q=π; (d) intensity ratio is 100%, Q
    Interaction of FEAB and soliton with different β. (a) Q=0; (b) Q=π
    Fig. 6. Interaction of FEAB and soliton with different β. (a) Q=0; (b) Q
    Interaction of weak energy double FEABs and soliton. (a) Q=0; (b) Q=π
    Fig. 7. Interaction of weak energy double FEABs and soliton. (a) Q=0; (b) Q
    Interaction of double FEABs and soliton at different initial intervals. (a) Q=0; (b) Q=π
    Fig. 8. Interaction of double FEABs and soliton at different initial intervals. (a) Q=0; (b) Q
    Interaction of double FEABs and soliton under different initial amplitude ratios. (a) Q=0; (b) Q=π
    Fig. 9. Interaction of double FEABs and soliton under different initial amplitude ratios. (a) Q=0; (b) Q
    Tao Wang, Cheng Lian, Liankai Wang, Kewei Huan, Yining Mu, Weijun Chen. Interaction of Airy Beams and Soliton in Saturable Nonlinear Medium[J]. Chinese Journal of Lasers, 2021, 48(13): 1308001
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