• Photonics Research
  • Vol. 10, Issue 8, 1924 (2022)
Dingpeng Liao1、†, Fengliang Dong2、†, Kun Zhang1、2、†, Yi Zhou1, Gaofeng Liang1, Zhihai Zhang1, Zhongquan Wen1, Zhengguo Shang1, Gang Chen1、*, Luru Dai2、3, and Weiguo Chu2、4
Author Affiliations
  • 1Key Laboratory of Optoelectronic Technology & Systems (Chongqing University), Ministry of Education, and College of Optoelectronic Engineering, Chongqing University, Chongqing 400044, China
  • 2National Center for Nanoscience and Technology, Beijing 100190, China
  • 3e-mail: dai@nanoctr.cn
  • 4e-mail: wgchu@nanoctr.cn
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    DOI: 10.1364/PRJ.462848 Cite this Article Set citation alerts
    Dingpeng Liao, Fengliang Dong, Kun Zhang, Yi Zhou, Gaofeng Liang, Zhihai Zhang, Zhongquan Wen, Zhengguo Shang, Gang Chen, Luru Dai, Weiguo Chu. Flat-field superoscillation metalens[J]. Photonics Research, 2022, 10(8): 1924 Copy Citation Text show less
    Flat-field superoscillation metalens. (a) Schematic illustration of focusing of off-axis light by a flat-field superoscillation metalens. (b) Schematic illustration of the a-Si dielectric meta-atom for geometric-phase manipulation in the metalens.
    Fig. 1. Flat-field superoscillation metalens. (a) Schematic illustration of focusing of off-axis light by a flat-field superoscillation metalens. (b) Schematic illustration of the a-Si dielectric meta-atom for geometric-phase manipulation in the metalens.
    Results of the optimized flat-field superoscillation metalens. (a) Phase profile of the lens φ(x,y); (b) peak intensity (red solid), full width at half-maximum FWHMx (blue solid) and FWHMy (blue open) in x and y directions, and sidelobe ratio in x (green solid) and y (green open) directions at different incident angles.
    Fig. 2. Results of the optimized flat-field superoscillation metalens. (a) Phase profile of the lens φ(x,y); (b) peak intensity (red solid), full width at half-maximum FWHMx (blue solid) and FWHMy (blue open) in x and y directions, and sidelobe ratio in x (green solid) and y (green open) directions at different incident angles.
    (a) Diagram of the superoscillation focusing metalens arrangement in square lattice array, where inset gives the arrangement of the meta-atoms located at the device center. (b) SEM picture of the central part of the fabricated flat-field superoscillation metalens.
    Fig. 3. (a) Diagram of the superoscillation focusing metalens arrangement in square lattice array, where inset gives the arrangement of the meta-atoms located at the device center. (b) SEM picture of the central part of the fabricated flat-field superoscillation metalens.
    Focusing performance of the flat-field superoscillation metalens. (a), (e) Simulation results of the optical intensity profile on the designed focal plane for different incident angles of 0°, 0.5°, 1.0°, 1.5°, 2.0°, 2.5°, 3.0°, 3.5°, 4.0°, and 4.5°; (b), (f) intensity distribution curves in x direction (blue) and y direction (red), both crossing the focal spot center; (c), (g) experimental results of the optical intensity profile on the designed focal plane for the 10 incident angles; (d), (h) intensity distribution curves in x direction (blue) and y direction (red), both crossing the focal spot center; (i) focusing performance parameters obtained from the experimental results, including peak intensity (red), spot size (FWHM) in x (blue solid) and y (blue open) directions and sidelobe ratio in x (green solid) and y (green open) directions; (j) spot displacement on the focal plane for the simulation result (red) and experimental result (blue).
    Fig. 4. Focusing performance of the flat-field superoscillation metalens. (a), (e) Simulation results of the optical intensity profile on the designed focal plane for different incident angles of 0°, 0.5°, 1.0°, 1.5°, 2.0°, 2.5°, 3.0°, 3.5°, 4.0°, and 4.5°; (b), (f) intensity distribution curves in x direction (blue) and y direction (red), both crossing the focal spot center; (c), (g) experimental results of the optical intensity profile on the designed focal plane for the 10 incident angles; (d), (h) intensity distribution curves in x direction (blue) and y direction (red), both crossing the focal spot center; (i) focusing performance parameters obtained from the experimental results, including peak intensity (red), spot size (FWHM) in x (blue solid) and y (blue open) directions and sidelobe ratio in x (green solid) and y (green open) directions; (j) spot displacement on the focal plane for the simulation result (red) and experimental result (blue).
    Optical propagation properties on the incident plane (xz plane) at different incident angles. Simulation results: (a), (e) intensity distribution on xz propagation plane; (b), (f) peak intensity (red), FWHM (blue), and sidelobe ratio (green) along the propagation direction. Experimental results: (c), (g) intensity distribution on the xz propagation plane; (d), (h) peak intensity (red), FWHM (blue), and sidelobe ratio (green) along the propagation direction. The Abbe diffraction limit and superoscillation criterion are displayed by the dashed curve and dashed-dotted curve, respectively. The focal plane is denoted by the vertical dashed line.
    Fig. 5. Optical propagation properties on the incident plane (xz plane) at different incident angles. Simulation results: (a), (e) intensity distribution on xz propagation plane; (b), (f) peak intensity (red), FWHM (blue), and sidelobe ratio (green) along the propagation direction. Experimental results: (c), (g) intensity distribution on the xz propagation plane; (d), (h) peak intensity (red), FWHM (blue), and sidelobe ratio (green) along the propagation direction. The Abbe diffraction limit and superoscillation criterion are displayed by the dashed curve and dashed-dotted curve, respectively. The focal plane is denoted by the vertical dashed line.
    Poynting vector on the incident plane (xz plane) at different incident angles, where the blue arrows give the direction of energy flow.
    Fig. 6. Poynting vector on the incident plane (xz plane) at different incident angles, where the blue arrows give the direction of energy flow.
    No. of RingsPhase of Rings (pi) φi=2πpi/32
    #1–#14000C040000J500000006000006000000D00000000100000000000000000420000000400000000000000000000020002000000000000000002000000000000000N001000063302
    #141–#280000301442010C44000101104400004443100544641440054454040415474570FD4001F000C88A00910B207003005546W0CQG010QJ09H0F5XH2SG2F7PGQBE1F2P00W64CP44M32
    #281–#420APA6A7P7B4AQG4QBQ4523VZ8EHKFN7N3322Y562F73A22EG325250YQ3312175035E6C290RB40S002XB10330210R6Z0D50305V2004005Y014M171YQ03P0KAF4K60448D010A90H0
    #421–#562M0R001E4C20Q84463X20MAM20054P8A0C2E0B070B0W0HC6WJR200N00X12M0P0F0H0GD0S4M2C383K0H0K0BX8S1027Z5P2Z0Q2H2JAGS3Q060M110E063MC20072200Q3G0E00N0M0D0
    Table 1. Phase Distribution along Radial Direction
    Dingpeng Liao, Fengliang Dong, Kun Zhang, Yi Zhou, Gaofeng Liang, Zhihai Zhang, Zhongquan Wen, Zhengguo Shang, Gang Chen, Luru Dai, Weiguo Chu. Flat-field superoscillation metalens[J]. Photonics Research, 2022, 10(8): 1924
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