Author Affiliations
1Guangdong Provincial Key Laboratory of Optical Fiber Sensing and Communications, Institute of Photonics Technology, Jinan University, Guangzhou, Guangdong 510632, China2Institute of Microscale Optoelectronics, Shenzhen University, Shenzhen, Guangdong 518060, Chinashow less
Fig. 1. Schematic for comparison between phase-gradient metasurfaces and single unit-cell metagrating structures. (a) Reflection and (b) transmission phase-gradient metasurfaces; (c) reflection and (d) transmission single unit-cell metagrating surfaces
Fig. 2. Symmetric reflection metagrating
[29]. (a) Schematic of metallic groove metagrating; (b)
k-space diffraction order chart composed of multiple Wood anomaly lines;(c)
versus incident angle and wave number; (d) -1th and 0
th order diffraction efficiency spectra and local mode amplitude spectra; (e) magnetic field (
Hy) distribution diagram for perfect retro-reflection with incident angle of 30°
Fig. 3. Asymmetric reflection metagrating
[28]. (a) Metagrating composed of bianisotropic unit cells array with perpendicular electric resonance and magnetic resonance as well as schematic of asymmetric perfect diffraction; (b) parameter scanning image of cancellation factor under normal incidence; (c) diffraction efficiency of each diffraction order corresponding to normalized frequency denoted by red star in
Fig.3 (b); (d) distributions of incident and reflected fields at designed frequency
Fig. 4. Symmetric transmission metagrating. (a) Principle diagram of plane wave diffraction from all-dielectric metagrating
[69];(b) normalized scattering spectra of electromagnetic multipoles excited by p-polarized wave and s-polarized wave, respectively
[69];(c) experimental demonstration of realization of beam bending with all-dielectric metagrating
[71]; (d) schematic of transmission SiN
x metagrating
[72];(e) theoretical efficiency diagram of perfect transmission end diffraction
[72]; (f) -1th order diffraction efficiency diagram for large angle and wide bandwidth
[72]; (g) magnetic field pattern of perfect transmission end diffraction
[72] Fig. 5. Asymmetric transmission metagrating. (a) (Left) dielectric double-ridge waveguide with different widths and free-space radiation under certain phase difference and (right) far-field response image of double-ridge metagrating
[64]; (b) extraordinary diffraction of bianisotropic transimission metagrating
[61]; (c) transmission metagrating with fish-shaped structure
[65]; (d) broadband large-angle asymmetric diffraction kissing double-nanopillar metagrating
[74]; (e) freeform metagrating constructed using topological optimization
[66]; (f) metagrating constructed by deep learning
[77] Fig. 6. Reconfigurable metagrating. (a) Schematic of reconfigurable metagrating composed of metal-graphene-metal sandwiched structure
[79]; (b) schematic of spin-locked reflection of right-handed circularly polarized beam under varying incident angles with reconfigurable spin-locked reflection metagrating
[82] Fig. 7. Applications of metagrating lenses with large numerical aperture. (a) (Upper)SEM images of metagrating lens are displayed (scale bars indicating 10 μm, 5 μm, and 500 nm from left to right), (middle) focal field distributions of metalens in
xz plane and
xy plane, and (down) normalized intensity map along
z direction at
x=0 and normalized intensity map along
x direction at
z=45.05 μm
[83]; (b) (upper) design diagram of hybrid metalens and actual metalens (bottom left) phase distribution and structure diagram of phase-gradient metasurface, (bottom right) structure diagram of wide angle deflection metagrating, diffraction efficiencies of metagrating (dot) and diffraction efficiencies of phase-gradient metasurface (solid line) under different diffraction angles
[84] Fig. 8. Achromatic focusing of metagrating
[85]. (a) Schematics of beam deflection of coaxial small-angle achromatic metasurface and off-axis wide-angle achromatic metasurface; (b) structural diagrams of off-axis wide-angle achromatic metal groove metagrating; (c) effect diagrams of achromatic focusing
Fig. 9. Multifunctional device with angle selectivity of metagrating
[86]. (a) Flow chart of extraordinary optical transmission (EOT), total internal reflection (TIR) and extraordinary optical diffraction (EOD) of multifunctional metasurface; (b) phase profiles of EOT, TIR and EOD at different incident angles and incident wavelengths; (c) numerical simulation results of EOT, TIR and EOD focusing at different incident angles
Fig. 10. Applications of metagrating holograms with ultra-large angle tolerance. (a) Metasurface hologram device designed by sub-wavelength dielectric metagratings and detour phase
[32]; (b) metasurface hologram device with large angle tolerance designed by subwavelength metal metagratings
[46]; (c) metasurface hologram device based on perfect diffraction dielectric metagratings
[72] Fig. 11. Metagratings used for converting surface plasma polariton (SPP) into arbitrary free-space wavefront. (a) Schematic of conversion from SPP wave to free-space wave through diffraction orders of metagrating
[88]; (b) modulated metagrating for free-space Airy beam generation by SPP excitation
[88]; (c) modulated metal metagrating used for 3D plasmonic micro-projector
[89];(d) modulated metallic slit metagrating used for conversion from SPP waves with different polarization and propagation directions to different free-space holographic images
[90] Fig. 12. Circular metagratings used for mutual conversion between cylindrical SPP wave and arbitrary free-space wavefront. (a) Circular metallic groove metagrating with central hole
[91]; (b) circular metallic slit metagrating formed by interference between SPP wave and free-space vortex beam
[92]