• Laser & Optoelectronics Progress
  • Vol. 56, Issue 23, 230003 (2019)
Shuhe Zhang, Meng Shao, Yi Wang, Yuping Duan, and Jinhua Zhou*
Author Affiliations
  • School of Biomedical Engineering, Anhui Medical University, Hefei, Anhui 230032, China
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    DOI: 10.3788/LOP56.230003 Cite this Article Set citation alerts
    Shuhe Zhang, Meng Shao, Yi Wang, Yuping Duan, Jinhua Zhou. Ray Characterization of Optical Waves[J]. Laser & Optoelectronics Progress, 2019, 56(23): 230003 Copy Citation Text show less
    Differential geometry of ray[11]
    Fig. 1. Differential geometry of ray[11]
    Ray tube model
    Fig. 2. Ray tube model
    Univalent hyperboloid ray model of Gaussian beam. (a) Two rays launching from same point Q at beam waist; (b) relationship between wavefront and rays with equal length[55]
    Fig. 3. Univalent hyperboloid ray model of Gaussian beam. (a) Two rays launching from same point Q at beam waist; (b) relationship between wavefront and rays with equal length[55]
    Two rays passing through arbitrary point S out of beam waist[55]
    Fig. 4. Two rays passing through arbitrary point S out of beam waist[55]
    Distributions of Gaussian windowed Fourier transforms of optical wave field. (a1)-(c1) Correspond to Eq. (41); (a2)-(c2) correspond to Eq. (42); (a3)-(c3) correspond to Eq. (43)
    Fig. 5. Distributions of Gaussian windowed Fourier transforms of optical wave field. (a1)-(c1) Correspond to Eq. (41); (a2)-(c2) correspond to Eq. (42); (a3)-(c3) correspond to Eq. (43)
    Ray distributions of two different beams. (a) Airy beam; (b) Hermit-Gaussian beam
    Fig. 6. Ray distributions of two different beams. (a) Airy beam; (b) Hermit-Gaussian beam
    Physical insight of single ray in SAFE mothed
    Fig. 7. Physical insight of single ray in SAFE mothed
    Axicon-based generation of nondiffracting beam. (a) “X”-like rays which can be generated by refracting parallel rays through axicon lens; (b) ray presentation of self-repairing property of beam
    Fig. 8. Axicon-based generation of nondiffracting beam. (a) “X”-like rays which can be generated by refracting parallel rays through axicon lens; (b) ray presentation of self-repairing property of beam
    Intensity distributions. (a) Intensity distribution calculated by SAFE; (b) intensity distribution calculated by angular spectrum diffraction method; (c)(d) self-repairing situation of beam blocked at different regions, calculated by angular spectrum diffraction method
    Fig. 9. Intensity distributions. (a) Intensity distribution calculated by SAFE; (b) intensity distribution calculated by angular spectrum diffraction method; (c)(d) self-repairing situation of beam blocked at different regions, calculated by angular spectrum diffraction method
    Ray presentation of Airy beam. (a) Ray model of Airy beam built by choosing arbitrary point at parabolic caustic as reference point; (b) schematic of ray model
    Fig. 10. Ray presentation of Airy beam. (a) Ray model of Airy beam built by choosing arbitrary point at parabolic caustic as reference point; (b) schematic of ray model
    Airy beam reconstructed by SAFE method. (a) Normalized intensity distribution of xoz plane; (b) comparison of normalized intensity distribution of z = 0 plane with Airy beam
    Fig. 11. Airy beam reconstructed by SAFE method. (a) Normalized intensity distribution of xoz plane; (b) comparison of normalized intensity distribution of z = 0 plane with Airy beam
    Schematic of self-repairing property of Airy beam. (a) Ray model of Airy beam; (b) (c) optical-wave-field distributions of Airy beam blocked at different regions
    Fig. 12. Schematic of self-repairing property of Airy beam. (a) Ray model of Airy beam; (b) (c) optical-wave-field distributions of Airy beam blocked at different regions
    Beam having spiral wavefront composed by uniform skew rays. (a) Schematic of skew rays; (b) specific analyse of single ray
    Fig. 13. Beam having spiral wavefront composed by uniform skew rays. (a) Schematic of skew rays; (b) specific analyse of single ray
    Phase distributions of optical wave field with different values of m. (a) m=0; (b) m=1; (c) m=3
    Fig. 14. Phase distributions of optical wave field with different values of m. (a) m=0; (b) m=1; (c) m=3
    Corresponding relationship between point on Poincaré sphere and ellipse in real space[78]. (a) Location of point on Poincaré sphere determined by longitude angle φ and latitude angle θ; (b) parameters of ellipse in real space determined by point on Poincaré sphere
    Fig. 15. Corresponding relationship between point on Poincaré sphere and ellipse in real space[78]. (a) Location of point on Poincaré sphere determined by longitude angle φ and latitude angle θ; (b) parameters of ellipse in real space determined by point on Poincaré sphere
    Corresponding relationship between circular curve on Poincaré sphere and different kinds of Hermit-Laguerre Gaussian beams. (a1)-(c1) Circular curves on Poincaré sphere with normals toward different latitude angles θ; (a2)-(c2) ellipse distributions of normalized sizes on beam-waist plane; (a3)-(c3) corresponding ray models
    Fig. 16. Corresponding relationship between circular curve on Poincaré sphere and different kinds of Hermit-Laguerre Gaussian beams. (a1)-(c1) Circular curves on Poincaré sphere with normals toward different latitude angles θ; (a2)-(c2) ellipse distributions of normalized sizes on beam-waist plane; (a3)-(c3) corresponding ray models
    Structured Gaussian beam with decagram inner caustic[100]. (a) Curve on surface of Poincaré sphere; (b) ellipses and their outer and inner caustics; (c) normalized intensity distribution on beam-waist plane; (d) phase distribution on beam-waist plane
    Fig. 17. Structured Gaussian beam with decagram inner caustic[100]. (a) Curve on surface of Poincaré sphere; (b) ellipses and their outer and inner caustics; (c) normalized intensity distribution on beam-waist plane; (d) phase distribution on beam-waist plane
    Shuhe Zhang, Meng Shao, Yi Wang, Yuping Duan, Jinhua Zhou. Ray Characterization of Optical Waves[J]. Laser & Optoelectronics Progress, 2019, 56(23): 230003
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