• Acta Physica Sinica
  • Vol. 69, Issue 17, 174201-1 (2020)
Bao-Jing Hu1、2, Ming Huang1、*, Peng Li1, and Jing-Jing Yang1
Author Affiliations
  • 1School of Information Science and Engineering, Yunnan University, Kunming 650091, China
  • 2College of Science, Yunnan Agricultural University, Kunming 650201, China
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    DOI: 10.7498/aps.69.20200200 Cite this Article
    Bao-Jing Hu, Ming Huang, Peng Li, Jing-Jing Yang. Multiband plasmon-induced transparency based on nanometals-graphene hybrid model[J]. Acta Physica Sinica, 2020, 69(17): 174201-1 Copy Citation Text show less
    Schematic diagrams of single-band PIT model: (a) Three-dimensional space schematic; (b) two-dimensional plane schematic.
    Fig. 1. Schematic diagrams of single-band PIT model: (a) Three-dimensional space schematic; (b) two-dimensional plane schematic.
    Transmission spectra of the sole disks array, the sole rods array, and the single-band PIT model.
    Fig. 2. Transmission spectra of the sole disks array, the sole rods array, and the single-band PIT model.
    Distributions of electric field of single-band PIT model at (a) dip A, (b) dip B, and (c) peak.
    Fig. 3. Distributions of electric field of single-band PIT model at (a) dip A, (b) dip B, and (c) peak.
    Variations of resonant frequency and amplitude in transmission with frequency under different chemical potential of graphene in single-band PIT model.
    Fig. 4. Variations of resonant frequency and amplitude in transmission with frequency under different chemical potential of graphene in single-band PIT model.
    Comparisons of the PIT calculated by FDTD method and fitted by RTO model when chemical potential is 0 and 0.3 eV.
    Fig. 5. Comparisons of the PIT calculated by FDTD method and fitted by RTO model when chemical potential is 0 and 0.3 eV.
    Comparison of the PIT calculated by FDTD method and fitted by RTO model when chemical potential is 0.1 and 0.5 eV.
    Fig. 6. Comparison of the PIT calculated by FDTD method and fitted by RTO model when chemical potential is 0.1 and 0.5 eV.
    (a) The fitting values of parameters in RTO model with the chemical potential of graphene varying from 0 to 0.5 eV; (b) new fitting result after introducing correction factor.
    Fig. 7. (a) The fitting values of parameters in RTO model with the chemical potential of graphene varying from 0 to 0.5 eV; (b) new fitting result after introducing correction factor.
    Variations of transmission windows with different background materials in single-band PIT model.
    Fig. 8. Variations of transmission windows with different background materials in single-band PIT model.
    Variations of dip A, dip B, and peak with the different background materials in single-band PIT model.
    Fig. 9. Variations of dip A, dip B, and peak with the different background materials in single-band PIT model.
    Two-dimensional plane schematic of dual-band PIT model.
    Fig. 10. Two-dimensional plane schematic of dual-band PIT model.
    Transmission spectra of dual-band PIT model.
    Fig. 11. Transmission spectra of dual-band PIT model.
    Distributions of electric field of dual-band PIT model at (a) dip A, (b) dip B, (c) dip C, (d) peak I and (e) peak II.
    Fig. 12. Distributions of electric field of dual-band PIT model at (a) dip A, (b) dip B, (c) dip C, (d) peak I and (e) peak II.
    Variations of resonant frequency and amplitude in transmission with frequency under different chemical potential of graphene in dual-band PIT model.
    Fig. 13. Variations of resonant frequency and amplitude in transmission with frequency under different chemical potential of graphene in dual-band PIT model.
    Two-dimensional plane schematic diagram of triple-band PIT model.
    Fig. 14. Two-dimensional plane schematic diagram of triple-band PIT model.
    Transmission spectra of triple-band PIT model.
    Fig. 15. Transmission spectra of triple-band PIT model.
    Distribution of electric field of triple-band PIT model at (a) dip A, (b) dip B, (c) dip C, (d) dip D, (e) peak I, (f) peak II and (g) peak III.
    Fig. 16. Distribution of electric field of triple-band PIT model at (a) dip A, (b) dip B, (c) dip C, (d) dip D, (e) peak I, (f) peak II and (g) peak III.
    Variations of resonant frequency and amplitude in transmission with frequency under different chemical potential of graphene in triple-band PIT model.
    Fig. 17. Variations of resonant frequency and amplitude in transmission with frequency under different chemical potential of graphene in triple-band PIT model.
    Bao-Jing Hu, Ming Huang, Peng Li, Jing-Jing Yang. Multiband plasmon-induced transparency based on nanometals-graphene hybrid model[J]. Acta Physica Sinica, 2020, 69(17): 174201-1
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