Chinese Optics Letters, Volume. 23, Issue 10, 103601(2025)

Generation and control of high-reflection-efficiency perfect vortex beams based on all-dielectric metasurfaces

Xiaojie Sun1,2, Jiajing He1,2、*, Zhouyuan Yan1,2, Yan Wang1,2, Haixu Tao1,2, Xuan Yang1,2,3, and Jun Wang1,2
Author Affiliations
  • 1Aerospace Laser Technology and System Department, Wangzhijiang Innovation Center for Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3ShanghaiTech University, Shanghai 201210, China
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    Figures & Tables(7)
    Schematic diagram of a reflective metasurface generating a perfect vortex beam.
    Generation of perfect vortex beam phase profile. (a) The phase profile generation method of the perfect vortex beam based on BBK when r0 = 0.1 and l = 3. (b) The phase profile generation method of 2 × 2 perfect vortex beam arrays based on Dammann grating when r0 = 0.04, l = 1, and p = 9.5 µm.
    Simulation results of perfect vortex beams with different topological charges. (a)–(f) x–y plane electric field strength distributions at z = 300 µm for topological charges of l = −3, −2, −1, 1, 2, 3, respectively. (g)–(l) x–z plane electric field strength distributions for topological charges of l = −3, −2, −1, 1, 2, 3, respectively. (m)–(r) Interference results of a perfect vortex beam with a spherical wave for topological charges l = −3, −2, −1, 1, 2, 3, respectively.
    Simulation results of perfect vortex beam control with different parameters r0. (a)–(d) Electric field intensity distributions in x–y plane when r0 = 0.04, 0.06, 0.08, 0.1. (e)–(h) Electric field intensity distributions in x–z plane when r0 = 0.04, 0.06, 0.08, 0.1.
    Simulation results of perfect vortex beams for 2 × 2 arrays generated by Dammann gratings with different periods. (a)–(d) Phase profile distributions for l = −1, p = 9.5 µm, l = 1, p = 9.5 µm, l = −1, p = 19.5 µm, l = 1, p = 19.5 µm. (e)–(h) Distributions of electric field strengths in the x–y plane for l = −1, p = 9.5 µm, l = 1, p = 9.5 µm, l = −1, p = 19.5 µm, l = 1, p = 19.5 µm.
    Experimental test results of a perfect vortex beam and SEM image of the prepared metasurface sample. (a) Experimental setup diagram. (b)–(g) Experimental results with topological charges of 1, −1, 2, −2, 3, and −3, respectively. (h), (i) Experimental results of a perfect vortex beam array. (j) SEM image of the prepared metasurface sample. (k) Local SEM magnification image. (l) Comparison of experimental and simulated diameter data. (m) Comparison of the perfect vortex beam ring width results between experiments and simulations. (n)–(q) The perfect interference results of vortex beams and spherical waves.
    • Table 1. Comparison of Parameters and Methods

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      Table 1. Comparison of Parameters and Methods

      MethodWavelengthEfficiencyBeam qualityRef.
      AxiconNear-infrared55%[27]
      Axicon300 nm86.6%[28]
      AxiconVisible light55%Uniformity: 86.5%[29]
      Electric tuningMicrowave85%[32]
      AxiconMicrowave80%Uneven[33]
      BBK1550 nm89.81%Narrower rings, higher power densityThis work
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    Xiaojie Sun, Jiajing He, Zhouyuan Yan, Yan Wang, Haixu Tao, Xuan Yang, Jun Wang, "Generation and control of high-reflection-efficiency perfect vortex beams based on all-dielectric metasurfaces," Chin. Opt. Lett. 23, 103601 (2025)

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    Paper Information

    Category: Nanophotonics, Metamaterials, and Plasmonics

    Received: Mar. 25, 2025

    Accepted: May. 27, 2025

    Published Online: Sep. 8, 2025

    The Author Email: Jiajing He (jiajinghe@siom.ac.cn)

    DOI:10.3788/COL202523.103601

    CSTR:32184.14.COL202523.103601

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