• Chinese Optics Letters
  • Vol. 18, Issue 1, 012201 (2020)
Zhenhua Li1、*, Chuanfu Cheng2、**, Hanping Liu1, Dawei Li3, Shicai Xu4, Huilan Liu1, Junye Zhang1, and Suzhen Zhang1
Author Affiliations
  • 1College of Physics and Electronic Information, Dezhou University, Dezhou 253023, China
  • 2College of Physics and Electronics, Shandong Normal University, Jinan 250014, China
  • 3Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 4Shandong Key Laboratory of Biophysics, Dezhou University, Dezhou 253023, China
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    DOI: 10.3788/COL202018.012201 Cite this Article Set citation alerts
    Zhenhua Li, Chuanfu Cheng, Hanping Liu, Dawei Li, Shicai Xu, Huilan Liu, Junye Zhang, Suzhen Zhang. Experimental generation of Kagome lattices using metasurface of integrated convex lens[J]. Chinese Optics Letters, 2020, 18(1): 012201 Copy Citation Text show less
    Schematic diagram for generating novel Kagome lattices. (a) Conventional setup may be composed by six pinholes, six transparent discs, and a lens with focal length f. The functional effect of their combination can be integrated into a single plane (b) with both amplitude modulation and phase modulation.
    Fig. 1. Schematic diagram for generating novel Kagome lattices. (a) Conventional setup may be composed by six pinholes, six transparent discs, and a lens with focal length f. The functional effect of their combination can be integrated into a single plane (b) with both amplitude modulation and phase modulation.
    (a) Schematic of the phase modulation using the metasurface of nano-apertures. The thickness of the gold film on the quartz substrate is 200 nm. For each nano-aperture, the length of each is L=150 μm, the width is w=70 μm, and the distance between neighboring apertures is 220 μm in both the x and y directions. Tuning the oriented angle difference α between two apertures, we can realize a certain phase shift of 2α in their transmitted waves. (b) Full image of the designed metasurface corresponding to Fig. 1(b). (c) SEM image of the fabricated metasurface.
    Fig. 2. (a) Schematic of the phase modulation using the metasurface of nano-apertures. The thickness of the gold film on the quartz substrate is 200 nm. For each nano-aperture, the length of each is L=150μm, the width is w=70μm, and the distance between neighboring apertures is 220 μm in both the x and y directions. Tuning the oriented angle difference α between two apertures, we can realize a certain phase shift of 2α in their transmitted waves. (b) Full image of the designed metasurface corresponding to Fig. 1(b). (c) SEM image of the fabricated metasurface.
    (a) Intensity distribution recorded by the CMOS. The intensity pattern is a periodic patchwork of hexagonal spot unit arrays and hourglass arrays consisting of five intensity maximums, as marked by red lines. (b) Interferogram of (a) and the reference wave. An interference fringe splits into two within the hourglass, but no splitting is seen within the hexagon.
    Fig. 3. (a) Intensity distribution recorded by the CMOS. The intensity pattern is a periodic patchwork of hexagonal spot unit arrays and hourglass arrays consisting of five intensity maximums, as marked by red lines. (b) Interferogram of (a) and the reference wave. An interference fringe splits into two within the hourglass, but no splitting is seen within the hexagon.
    (a) Kagome lattice generated after a six-pinhole interferometer. (b) Interferogram of (a) with a tilted plane wave.
    Fig. 4. (a) Kagome lattice generated after a six-pinhole interferometer. (b) Interferogram of (a) with a tilted plane wave.
    Zhenhua Li, Chuanfu Cheng, Hanping Liu, Dawei Li, Shicai Xu, Huilan Liu, Junye Zhang, Suzhen Zhang. Experimental generation of Kagome lattices using metasurface of integrated convex lens[J]. Chinese Optics Letters, 2020, 18(1): 012201
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