• Chinese Optics Letters
  • Vol. 19, Issue 2, 022602 (2021)
Guanxue Wang, Yu Miao, Yang Li, Xinzhi Shan, and Xiumin Gao*
Author Affiliations
  • School of Optical-Electrical and Computer Engineering, University of Shanghai for Science and Technology, Shanghai 200093, China
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    DOI: 10.3788/COL202119.022602 Cite this Article Set citation alerts
    Guanxue Wang, Yu Miao, Yang Li, Xinzhi Shan, Xiumin Gao. Experimental and theoretical study of linearly polarized Lorentz–Gauss beams with heterogeneous distribution[J]. Chinese Optics Letters, 2021, 19(2): 022602 Copy Citation Text show less
    Transition mechanism diagram of FTM.
    Fig. 1. Transition mechanism diagram of FTM.
    Experiment setup. λ/2, half-wave plate; M, mirror; L1, lens with focal length of 100 mm; L2, lens with focal length of 300 mm; SLM, spatial light modulator; CCD, charge coupled device. The inset depicts the hologram of LGB-HA.
    Fig. 2. Experiment setup. λ/2, half-wave plate; M, mirror; L1, lens with focal length of 100 mm; L2, lens with focal length of 300 mm; SLM, spatial light modulator; CCD, charge coupled device. The inset depicts the hologram of LGB-HA.
    Two methods for the generation of LGB-HA corresponding to numerical simulation under NA = 0.09, B = 4, m = 3, ωx = 0.3, γp = 0.3 with various phase factor n. (a1)–(a3) Numerical simulation results for n = 3, 4, and 6, respectively; (b1)–(b3) experimental results of FTM with phase parameter n = 3, 4, and 6; (c1)–(c3) phase patterns consist of the upper left corner mapping to FTM and the lower right corner mapping to CAM. (d1)–(d3) Experimental results of CAM with phase parameter n=3, 4, and 6.
    Fig. 3. Two methods for the generation of LGB-HA corresponding to numerical simulation under NA = 0.09, B = 4, m = 3, ωx = 0.3, γp = 0.3 with various phase factor n. (a1)–(a3) Numerical simulation results for n = 3, 4, and 6, respectively; (b1)–(b3) experimental results of FTM with phase parameter n = 3, 4, and 6; (c1)–(c3) phase patterns consist of the upper left corner mapping to FTM and the lower right corner mapping to CAM. (d1)–(d3) Experimental results of CAM with phase parameter n=3, 4, and 6.
    Intensity distributions of LGB-HA corresponding to numerical simulation under NA = 0.09, B = 4, m = 3, ωx = 0.3, γp = 0.3 with different phase factor n. The upper layer is simulation results, the bottom layer is experiment results, and the middle layer is the complex amplitude hologram. Internal details emerge corresponding to the regions marked by the overlaid white circles.
    Fig. 4. Intensity distributions of LGB-HA corresponding to numerical simulation under NA = 0.09, B = 4, m = 3, ωx = 0.3, γp = 0.3 with different phase factor n. The upper layer is simulation results, the bottom layer is experiment results, and the middle layer is the complex amplitude hologram. Internal details emerge corresponding to the regions marked by the overlaid white circles.
    Normalized axis-directed energy distribution profiles in the focal plane of the simulation results, FTM and CAM under m = 3, B = 4, n = 6. (a) Theoretical simulation results. (b) Experimental result of FTM. (c) Experimental result of CAM.
    Fig. 5. Normalized axis-directed energy distribution profiles in the focal plane of the simulation results, FTM and CAM under m = 3, B = 4, n = 6. (a) Theoretical simulation results. (b) Experimental result of FTM. (c) Experimental result of CAM.
    Guanxue Wang, Yu Miao, Yang Li, Xinzhi Shan, Xiumin Gao. Experimental and theoretical study of linearly polarized Lorentz–Gauss beams with heterogeneous distribution[J]. Chinese Optics Letters, 2021, 19(2): 022602
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