• Opto-Electronic Advances
  • Vol. 4, Issue 1, 200008 (2021)
Yilin Wang1, Qingbin Fan1, and Ting Xu1,2,*
Author Affiliations
  • 1National Laboratory of Solid-State Microstructures, Key Laboratory of Intelligent Optical Sensing and Integration and College of Engineering and Applied Sciences, Nanjing University, Nanjing 210093, China
  • 2Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China.
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    DOI: 10.29026/oea.2021.200008 Cite this Article
    Yilin Wang, Qingbin Fan, Ting Xu. Design of high efficiency achromatic metalens with large operation bandwidth using bilayer architecture[J]. Opto-Electronic Advances, 2021, 4(1): 200008 Copy Citation Text show less
    Schematic for bilayer broadband achromatic metalens. It has the same focal plane over a large continuous wavelength region. Inset: Oblique view of a unit cell of a bilayer Si nanopillars with different heights h1 = 850 nm, h2 = 1500 nm, in-plane cross-sectional dimensions Dx = 420 nm, Dy = 190 nm and lattice constant P = 500 nm, on a SiO2 substrate. Right: The top view of each layer.
    Fig. 1. Schematic for bilayer broadband achromatic metalens. It has the same focal plane over a large continuous wavelength region. Inset: Oblique view of a unit cell of a bilayer Si nanopillars with different heights h1 = 850 nm, h2 = 1500 nm, in-plane cross-sectional dimensions Dx = 420 nm, Dy = 190 nm and lattice constant P = 500 nm, on a SiO2 substrate. Right: The top view of each layer.
    (a) Simulated polarization conversion efficiency of the top rectangular nanopillar as a function of wavelengths from 1000 nm to 1700 nm. Each nanopillar with 500 nm periods, in-plane cross-sectional dimensions Dx = 420 nm, Dy = 190 nm. (b, c) Transmission coefficient and phase map of the bottom cylindrical nanopillar with different diameters d as a function of wavelength from 1000 nm to 1700 nm. (d) Phase spectra for cylindrical nanopillar with four different diameters as a function of frequency.
    Fig. 2. (a) Simulated polarization conversion efficiency of the top rectangular nanopillar as a function of wavelengths from 1000 nm to 1700 nm. Each nanopillar with 500 nm periods, in-plane cross-sectional dimensions Dx = 420 nm, Dy = 190 nm. (b, c) Transmission coefficient and phase map of the bottom cylindrical nanopillar with different diameters d as a function of wavelength from 1000 nm to 1700 nm. (d) Phase spectra for cylindrical nanopillar with four different diameters as a function of frequency.
    The phase profile of bilayer achromatic metalens. (a) The ideal phase profile at the λmax. (b) The bottom layer normalized phase compensation profile over a wavelength region from 1000 nm to 1700 nm, at a step of 100 nm. (c) The required phase profile of top layer.
    Fig. 3. The phase profile of bilayer achromatic metalens. (a) The ideal phase profile at the λmax. (b) The bottom layer normalized phase compensation profile over a wavelength region from 1000 nm to 1700 nm, at a step of 100 nm. (c) The required phase profile of top layer.
    Simulated verification of chromatic and achromatic metalens. (a, b) Numerical intensity profiles of broadband chromatic (a) and achromatic (b) metalens with NA = 0.15 at various incident wavelengths. The red dashed line indicates the position of the focal plane. (c, d) Normalized intensity profiles along the red dashed lines of (b). Scale bar: 6 μm.
    Fig. 4. Simulated verification of chromatic and achromatic metalens. (a, b) Numerical intensity profiles of broadband chromatic (a) and achromatic (b) metalens with NA = 0.15 at various incident wavelengths. The red dashed line indicates the position of the focal plane. (c, d) Normalized intensity profiles along the red dashed lines of (b). Scale bar: 6 μm.
    Performance of broadband achromatic metalens. (a) The focal length shift values of both chromatic and achromatic metalenses as a function of incident wavelength. (b) The FWHM of the focal spots as a function of indent wavelength. (c) The efficiency of achromatic metalens as a function of incident wavelength.
    Fig. 5. Performance of broadband achromatic metalens. (a) The focal length shift values of both chromatic and achromatic metalenses as a function of incident wavelength. (b) The FWHM of the focal spots as a function of indent wavelength. (c) The efficiency of achromatic metalens as a function of incident wavelength.
    The influence of structural deviations on the lensing quality. (a)– (d) The simulated focal intensity profiles of bilayer metalens with perfect alignment (a), misalignment of 500 nm (b), 1 μm (c) and 1.5 μm (d) between two metasurface layers at three different wavelengths.
    Fig. 6. The influence of structural deviations on the lensing quality. (a) (d) The simulated focal intensity profiles of bilayer metalens with perfect alignment (a), misalignment of 500 nm (b), 1 μm (c) and 1.5 μm (d) between two metasurface layers at three different wavelengths.
    Yilin Wang, Qingbin Fan, Ting Xu. Design of high efficiency achromatic metalens with large operation bandwidth using bilayer architecture[J]. Opto-Electronic Advances, 2021, 4(1): 200008
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