• Chinese Journal of Lasers
  • Vol. 48, Issue 23, 2314002 (2021)
Yuling Lü, Fengping Yan*, Xuemei Du, and Wei Wang
Author Affiliations
  • Key Laboratory of All Optical Network and Advanced Telecommunication Network, Ministry of Education, Institute of Lightwave Technology, Beijing Jiaotong University, Beijing 100044, China
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    DOI: 10.3788/CJL202148.2314002 Cite this Article Set citation alerts
    Yuling Lü, Fengping Yan, Xuemei Du, Wei Wang. Polarization- and Angle-Insensitive Electromagnetically Induced Transparency-Like Metamaterial[J]. Chinese Journal of Lasers, 2021, 48(23): 2314002 Copy Citation Text show less
    Schematic of structure of EIT-like metamaterial. (a) Three-dimensional diagram; (b) front view
    Fig. 1. Schematic of structure of EIT-like metamaterial. (a) Three-dimensional diagram; (b) front view
    Transmission spectra of cross structure, 4L structure and complete structure
    Fig. 2. Transmission spectra of cross structure, 4L structure and complete structure
    Electric field intensity and surface current distribution of EIT-like metamaterials at resonant frequencies. (a) Electric field intensity distribution at 1.75 THz; (b) electric field intensity distribution at 1.94 THz; (c) electric field intensity distribution at 2.18 THz; (d) surface current distribution at 1.75 THz; (e) surface current distribution at 1.94 THz; (f) surface current distribution at 2.18 THz
    Fig. 3. Electric field intensity and surface current distribution of EIT-like metamaterials at resonant frequencies. (a) Electric field intensity distribution at 1.75 THz; (b) electric field intensity distribution at 1.94 THz; (c) electric field intensity distribution at 2.18 THz; (d) surface current distribution at 1.75 THz; (e) surface current distribution at 1.94 THz; (f) surface current distribution at 2.18 THz
    Transmission spectra of 4L resonant element and complete metamaterial structure at different l values. (a) Transmission spectra of 4L resonant element; (b) transmission spectra of complete metamaterial structure
    Fig. 4. Transmission spectra of 4L resonant element and complete metamaterial structure at different l values. (a) Transmission spectra of 4L resonant element; (b) transmission spectra of complete metamaterial structure
    Transmission spectra of cross resonant element and complete metamaterial structure at different L values. (a) Transmission spectra of cross resonant element; (b) transmission spectra of complete metamaterial structure
    Fig. 5. Transmission spectra of cross resonant element and complete metamaterial structure at different L values. (a) Transmission spectra of cross resonant element; (b) transmission spectra of complete metamaterial structure
    Transmission spectra at different distances and electric field intensity distribution at transmission peak. (a) Transmission spectra; (b) electric field intensity distribution at transmission peak
    Fig. 6. Transmission spectra at different distances and electric field intensity distribution at transmission peak. (a) Transmission spectra; (b) electric field intensity distribution at transmission peak
    Transmission spectra of EIT-like metamaterial structure at different Fermi levels
    Fig. 7. Transmission spectra of EIT-like metamaterial structure at different Fermi levels
    Transmission spectra of EIT-like metamaterial structures with TE polarization and TM polarization
    Fig. 8. Transmission spectra of EIT-like metamaterial structures with TE polarization and TM polarization
    Transmission spectra at different incidence angles. (a) TE polarization; (b) TM polarization
    Fig. 9. Transmission spectra at different incidence angles. (a) TE polarization; (b) TM polarization
    Phase change and group delay of different Fermi levels. (a) Phase change; (b) group delay
    Fig. 10. Phase change and group delay of different Fermi levels. (a) Phase change; (b) group delay
    Transmission spectra and refractive index sensitivity of EIT-like metamaterial under different refractive indexes. (a) Transmission spectra under different refractive indices; (b) refractive index sensitivity at different Fermi levels
    Fig. 11. Transmission spectra and refractive index sensitivity of EIT-like metamaterial under different refractive indexes. (a) Transmission spectra under different refractive indices; (b) refractive index sensitivity at different Fermi levels
    StructureRef. [32]This work
    EIT-likemetamaterials typeDirac semimetal filmsGraphene
    Symmetry typeFourfold symmetryx-y symmetry
    Polarizationangle /(°)0--450--90
    Table 1. Polarization insensitivity of different metamaterial structures
    StructureEIT-like
    metamaterial type
    Refractive index sensitivity /
    (GHz·RIU-1)
    Ref. [38]Copper51.18
    Ref. [39]Silver60.69
    Ref. [40]Gold61.00
    Ref. [41]Silicon231.00
    This workGraphene395.00
    Table 2. Comparison of sensitivity of other EIT-like metamaterials and EIT-like metamaterials studied in this paper
    Yuling Lü, Fengping Yan, Xuemei Du, Wei Wang. Polarization- and Angle-Insensitive Electromagnetically Induced Transparency-Like Metamaterial[J]. Chinese Journal of Lasers, 2021, 48(23): 2314002
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