• Chinese Physics B
  • Vol. 29, Issue 10, (2020)
Pengdi Wang1 and Xianghua Zeng1、2、†
Author Affiliations
  • 1College of Physics Science and Technology & Institute of Optoelectronic Technology, Yangzhou University, Yangzhou 225002, China
  • 2College of Electrical, Energy and Power Engineering, Yangzhou University, Yangzhou 517, China
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    DOI: 10.1088/1674-1056/abab70 Cite this Article
    Pengdi Wang, Xianghua Zeng. High efficient Al: ZnO based bifocus metalens in visible spectrum[J]. Chinese Physics B, 2020, 29(10): Copy Citation Text show less
    (a) Structure of the AZO unit cell. (b) The longitudinal cross-section of the AZO unit cell with a height of H. (c) The transverse section of the AZO unit cell, where L and W represent the length and width of AZO nanorod, and Ix, Iy represent the length and width of ITO substrate. (d) Crystal axes (fast axis and low axis) coincide with Ex and Ey of the incident wave. (e) The AZO nanorod rotated by θ. (f) AZO refractive index n, k diagram.
    Fig. 1. (a) Structure of the AZO unit cell. (b) The longitudinal cross-section of the AZO unit cell with a height of H. (c) The transverse section of the AZO unit cell, where L and W represent the length and width of AZO nanorod, and Ix, Iy represent the length and width of ITO substrate. (d) Crystal axes (fast axis and low axis) coincide with Ex and Ey of the incident wave. (e) The AZO nanorod rotated by θ. (f) AZO refractive index n, k diagram.
    Polarization efficiency of the three structures, the incident light with left/right circled polarization and the transmission light with right/light circled polarization.
    Fig. 2. Polarization efficiency of the three structures, the incident light with left/right circled polarization and the transmission light with right/light circled polarization.
    Polarization conversion efficiency versus wavelength for different AZO plates: (a) AZO plates with different width W; (b) AZO plates with different length L; (c), (d) substrates with different length Ix and width Iy, respectively.
    Fig. 3. Polarization conversion efficiency versus wavelength for different AZO plates: (a) AZO plates with different width W; (b) AZO plates with different length L; (c), (d) substrates with different length Ix and width Iy, respectively.
    (a) Schematic of polarity flip. (b)–(d) The relationship between the additional phase φ of the transmission field and the θ angle for samples S1 (450 nm), S2 (530 nm), and S3 (650 nm), respectively.
    Fig. 4. (a) Schematic of polarity flip. (b)–(d) The relationship between the additional phase φ of the transmission field and the θ angle for samples S1 (450 nm), S2 (530 nm), and S3 (650 nm), respectively.
    Schematic of metalens designed according to PB phase method: (a) 1-D metalens, (b), (c) 2-D metalens.
    Fig. 5. Schematic of metalens designed according to PB phase method: (a) 1-D metalens, (b), (c) 2-D metalens.
    The phase profiles of Ex and Ey for the three structures: (a) S1 (450 nm), (b) S2 (530 nm), (c) S3 (650 nm), where the left picture in (a)–(c) is corresponding to the one without AZO. At z = 4 μm, the retardation phase curves of Ex, Ey and their differences for (d) S1 (450 nm), (e) S2 (530 nm), (f) S3 (650 nm).
    Fig. 6. The phase profiles of Ex and Ey for the three structures: (a) S1 (450 nm), (b) S2 (530 nm), (c) S3 (650 nm), where the left picture in (a)–(c) is corresponding to the one without AZO. At z = 4 μm, the retardation phase curves of Ex, Ey and their differences for (d) S1 (450 nm), (e) S2 (530 nm), (f) S3 (650 nm).
    The 1-D AZO metalens designed based on Fig. 3(a) with a total transverse length of 20 μm, with a circularly polarized incident light. (a)–(c) The diagram of power distribution in the x–z plane for the S1 (450 nm), S2 (530 nm), and S3 (650 nm), respectively. (d)–(f) Normalized intensity diagrams based on the three images at z = 10 μm. (g)–(i) x–z plane phase profile diagram at y = 0 μm in the x–z plane.
    Fig. 7. The 1-D AZO metalens designed based on Fig. 3(a) with a total transverse length of 20 μm, with a circularly polarized incident light. (a)–(c) The diagram of power distribution in the xz plane for the S1 (450 nm), S2 (530 nm), and S3 (650 nm), respectively. (d)–(f) Normalized intensity diagrams based on the three images at z = 10 μm. (g)–(i) xz plane phase profile diagram at y = 0 μm in the xz plane.
    The intensity distribution on x–z plane of 2-D metalens: (a) S1 (450 nm), (b) S2 (530 nm), (c) S3 (650 nm), the z coordinates of two focal points are marked on the graph. (d)–(i) The x–y section of intensity distribution diagram at corresponding z values (marked in the upper right corner).
    Fig. 8. The intensity distribution on xz plane of 2-D metalens: (a) S1 (450 nm), (b) S2 (530 nm), (c) S3 (650 nm), the z coordinates of two focal points are marked on the graph. (d)–(i) The xy section of intensity distribution diagram at corresponding z values (marked in the upper right corner).
    (a)–(f) The normalized intensity diagram on the x-y plane at different z values corresponding to the six focal points in Figs. 8(d)–8(i).
    Fig. 9. (a)–(f) The normalized intensity diagram on the x-y plane at different z values corresponding to the six focal points in Figs. 8(d)8(i).
    The x–z cross-section intensity distribution of 2D-metalens with the S3 structure of AZO nanorods by the PB phase method: (a) 60 × 60 AZO nanorods, (b) 40 × 40 AZO nanorods.
    Fig. 10. The xz cross-section intensity distribution of 2D-metalens with the S3 structure of AZO nanorods by the PB phase method: (a) 60 × 60 AZO nanorods, (b) 40 × 40 AZO nanorods.
    StructureS1S2S3
    Length (L)/nm454545
    Width (W)/nm909090
    Height (H)/nm140018502600
    Ix/nm100100100
    Iy/nm100100100
    Table 1. Structure parameters of S1, S2, and S3.
    Wavelength450530650
    Ex (with structure)/π20.32117.60114.939
    Ex and Ey (without structure)/π17.76915.05312.304
    Ey (with structure)/π19.12516.44613.802
    Phase shift of Ex/π2.5522.5482.635
    Phase shift of Ey/π1.3561.3931.498
    Phase difference/π1.1961.1551.137
    Table 2. Phase shift of Ex and Ey for linearly polarized incident light at 450 nm, 530 nm, and 650 nm with respect to Figs. 6(d)6(f).
    StructureFE of point 1FE of point 2NA of point 1NA of point 2
    S10.5360.2380.4100.707
    S20.6060.2730.4300.725
    S30.6450.3370.4470.721
    Table 3. Focusing efficiency (FE) and NA of 2D-metalen with structures (S1, S2, S3) designed by PB phase method.
    Pengdi Wang, Xianghua Zeng. High efficient Al: ZnO based bifocus metalens in visible spectrum[J]. Chinese Physics B, 2020, 29(10):
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