• Laser & Optoelectronics Progress
  • Vol. 57, Issue 23, 232601 (2020)
Lingyi Wang1, Kaikai Huang1、*, Xian Zhang2, and Xuanhui Lu1
Author Affiliations
  • 1Physics Department, Zhejiang University, Hangzhou, Zhejiang 310027, China
  • 2Institute of Advanced Technology, Zhejiang University, Hangzhou, Zhejiang 310027, China
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    DOI: 10.3788/LOP57.232601 Cite this Article Set citation alerts
    Lingyi Wang, Kaikai Huang, Xian Zhang, Xuanhui Lu. Manipulation of Abruptly Autofocusing Property of Circular Airy Beam Carrying Hard-Edge Annular Aperture[J]. Laser & Optoelectronics Progress, 2020, 57(23): 232601 Copy Citation Text show less
    Schematic of Airy beam carring hard-edge aperture
    Fig. 1. Schematic of Airy beam carring hard-edge aperture
    Propagation of Airy beam with hard-edge aperture. (a) Initial intensity distribution; (b) Airy beam main lobe intensity distribution; (c) Airy beam propagation diagram
    Fig. 2. Propagation of Airy beam with hard-edge aperture. (a) Initial intensity distribution; (b) Airy beam main lobe intensity distribution; (c) Airy beam propagation diagram
    Intensity distributions. (a) Light intensity distribution of the z-axis after the plane wave passes through the aperture;(b)(c) light intensity distribution of the main lobe after the ideal and attenuated Airy beam enters the aperture
    Fig. 3. Intensity distributions. (a) Light intensity distribution of the z-axis after the plane wave passes through the aperture;(b)(c) light intensity distribution of the main lobe after the ideal and attenuated Airy beam enters the aperture
    Schematic of optical principle of annular aperture annular aperture CAB
    Fig. 4. Schematic of optical principle of annular aperture annular aperture CAB
    Light intensity distribution of CAB incident plane under annual aperture. (a) Radial intensity distribution; (b) two-dimensional distribution
    Fig. 5. Light intensity distribution of CAB incident plane under annual aperture. (a) Radial intensity distribution; (b) two-dimensional distribution
    Numerical simulation results. (a) Light intensity change of self-focusing peak at zf with changing rt; (b) intensity distribution of CAB on z axis with A aperture and no aperture
    Fig. 6. Numerical simulation results. (a) Light intensity change of self-focusing peak at zf with changing rt; (b) intensity distribution of CAB on z axis with A aperture and no aperture
    Main lobe intensity distribution of one-dimensional ideal Airy beam with correspond aperture
    Fig. 7. Main lobe intensity distribution of one-dimensional ideal Airy beam with correspond aperture
    Numerical simulation results. (a) Light intensity change of self-focusing peak at zf with changing rblock; (b) intensity distribution of CAB on z axis with strip aperture, B aperture, and no aperture
    Fig. 8. Numerical simulation results. (a) Light intensity change of self-focusing peak at zf with changing rblock; (b) intensity distribution of CAB on z axis with strip aperture, B aperture, and no aperture
    Self-focusing peak light intensity enhancement of CAB at zf with three type apertures under different decay factors
    Fig. 9. Self-focusing peak light intensity enhancement of CAB at zf with three type apertures under different decay factors
    Initial CAB radial light intensity distribution. (a) α=0.01; (b) α=0.05
    Fig. 10. Initial CAB radial light intensity distribution. (a) α=0.01; (b) α=0.05
    Lingyi Wang, Kaikai Huang, Xian Zhang, Xuanhui Lu. Manipulation of Abruptly Autofocusing Property of Circular Airy Beam Carrying Hard-Edge Annular Aperture[J]. Laser & Optoelectronics Progress, 2020, 57(23): 232601
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