• Laser & Optoelectronics Progress
  • Vol. 60, Issue 15, 1519001 (2023)
Zhengchun Zhao, Bing Wen, Yangbao Deng*, and Bing Yang
Author Affiliations
  • College of Information and Electronic Engineering, Hunan City University, Yiyang 413000, Hunan, China
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    DOI: 10.3788/LOP221708 Cite this Article Set citation alerts
    Zhengchun Zhao, Bing Wen, Yangbao Deng, Bing Yang. Propagation and Control of Airy-Gaussian Beams in Gaussian Parity-Time Symmetric Media[J]. Laser & Optoelectronics Progress, 2023, 60(15): 1519001 Copy Citation Text show less
    Intensity distribution of Airy-Gaussian beams and complex refractive index distribution of PT-symmetric media. (a) Waveforms of Airy-Gaussian beams with different distribution factors; (b) curves of refractive index distribution function and gain/loss distribution function with different modulation factors
    Fig. 1. Intensity distribution of Airy-Gaussian beams and complex refractive index distribution of PT-symmetric media. (a) Waveforms of Airy-Gaussian beams with different distribution factors; (b) curves of refractive index distribution function and gain/loss distribution function with different modulation factors
    Spatial evolution of Airy-Gaussian beams in PT symmetric media at different modulation depths. (a) P=0; (b) P=0.5;(c) P=1.5; (d) relation diagram of light field intensity with transmission distance and modulation depth
    Fig. 2. Spatial evolution of Airy-Gaussian beams in PT symmetric media at different modulation depths. (a) P=0; (b) P=0.5;(c) P=1.5; (d) relation diagram of light field intensity with transmission distance and modulation depth
    Spatial evolution of Airy-Gaussian beams in PT symmetric media with different modulation factors. (a) W0=0.4; (b) W0=0.7; (c) W0=1.0; (d) relation diagram of light field intensity with transmission distance and modulation factor
    Fig. 3. Spatial evolution of Airy-Gaussian beams in PT symmetric media with different modulation factors. (a) W0=0.4; (b) W0=0.7; (c) W0=1.0; (d) relation diagram of light field intensity with transmission distance and modulation factor
    Spatial evolution of Airy-Gaussian beams in PT symmetric media with different gain/loss coefficients. (a) W0=0.1; (b) W0=0.4; (c) W0=0.8; (d) relation diagram of light field intensity with transmission distance and gain/loss coefficient
    Fig. 4. Spatial evolution of Airy-Gaussian beams in PT symmetric media with different gain/loss coefficients. (a) W0=0.1; (b) W0=0.4; (c) W0=0.8; (d) relation diagram of light field intensity with transmission distance and gain/loss coefficient
    Relationship between the oscillation period of shedding soliton, z0,and the parameters of PT symmetric media. (a) Modulation depth; (b) modulation factor; (c) gain/loss coefficient
    Fig. 5. Relationship between the oscillation period of shedding soliton, z0,and the parameters of PT symmetric media. (a) Modulation depth; (b) modulation factor; (c) gain/loss coefficient
    Spatial evolution of Airy-Gaussian beams with different truncation coefficients in PT symmetric media. (a) a=0.01; (b) a=0.20; (c) a=0.50; (d) relation diagram of light field intensity with truncation coefficient and transmission distance
    Fig. 6. Spatial evolution of Airy-Gaussian beams with different truncation coefficients in PT symmetric media. (a) a=0.01; (b) a=0.20; (c) a=0.50; (d) relation diagram of light field intensity with truncation coefficient and transmission distance
    Spatial evolution of Airy-Gaussian beams with different distribution factors in PT symmetric media. (a) χ0=0.01; (b) χ0=0.70; (c) χ0=1.00; (d) relation diagram of light field intensity with distribution factor and transmission distance
    Fig. 7. Spatial evolution of Airy-Gaussian beams with different distribution factors in PT symmetric media. (a) χ0=0.01; (b) χ0=0.70; (c) χ0=1.00; (d) relation diagram of light field intensity with distribution factor and transmission distance
    Relationship between the maximum intensity of the shedding soliton from Airy-Gaussian beams and the parameters of PT symmetric media when distribution factors are different. (a) W0=0.5,ω=0.7; (b) P=1.0,W0=0.5; (c) P=1.0,ω=0.7
    Fig. 8. Relationship between the maximum intensity of the shedding soliton from Airy-Gaussian beams and the parameters of PT symmetric media when distribution factors are different. (a) W0=0.5,ω=0.7; (b) P=1.0,W0=0.5; (c) P=1.0,ω=0.7
    Zhengchun Zhao, Bing Wen, Yangbao Deng, Bing Yang. Propagation and Control of Airy-Gaussian Beams in Gaussian Parity-Time Symmetric Media[J]. Laser & Optoelectronics Progress, 2023, 60(15): 1519001
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