• Acta Optica Sinica
  • Vol. 38, Issue 2, 0223002 (2018)
Yanling Peng1, Wenrui Xue1、*, Zhuangzhi Wei1, and Changyong Li2
Author Affiliations
  • 1 College of Physics and Electronic Engineering, Shanxi University, Taiyuan, Shanxi 0 30006, China
  • 2 State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Laser Spectroscopy, Shanxi University, Taiyuan, Shanxi 0 30006, China
  • show less
    DOI: 10.3788/AOS201838.0223002 Cite this Article Set citation alerts
    Yanling Peng, Wenrui Xue, Zhuangzhi Wei, Changyong Li. Analysis of Modes in Graphene-Coated Parallel Dielectric Nanowires[J]. Acta Optica Sinica, 2018, 38(2): 0223002 Copy Citation Text show less
    Cross-section diagram of graphene-coated parallel dielectric nanowires
    Fig. 1. Cross-section diagram of graphene-coated parallel dielectric nanowires
    (a) Real part and (b) imaginary part of the conductivity of graphene as functions of the operating frequency while the Fermi energies are 0.4, 0.5, 0.6 eV, respectively
    Fig. 2. (a) Real part and (b) imaginary part of the conductivity of graphene as functions of the operating frequency while the Fermi energies are 0.4, 0.5, 0.6 eV, respectively
    Field distributions of the six lowest order modes when f=51.579 THz, ρ=100 nm, d=50 nm, EF=0.5 eV. (a)~(f) are the longitudinal electric field distributions; (g)~(l) are the electric field intensity distributions
    Fig. 3. Field distributions of the six lowest order modes when f=51.579 THz, ρ=100 nm, d=50 nm, EF=0.5 eV. (a)~(f) are the longitudinal electric field distributions; (g)~(l) are the electric field intensity distributions
    Dependence of (a) effective refractive index and (b) propagation length on the operating frequency when ρ=100 nm, d= 50 nm, EF= 0.5 eV
    Fig. 4. Dependence of (a) effective refractive index and (b) propagation length on the operating frequency when ρ=100 nm, d= 50 nm, EF= 0.5 eV
    Distribution of the longitudinal electric field of mode 1 with the operating frequency of (a) 35 THz and (b) 55 THz
    Fig. 5. Distribution of the longitudinal electric field of mode 1 with the operating frequency of (a) 35 THz and (b) 55 THz
    Dependence of (a) effective refractive index and (b) propagation length on the spacing d when f= 51.579 THz, ρ=100 nm, EF=0.5 eV
    Fig. 6. Dependence of (a) effective refractive index and (b) propagation length on the spacing d when f= 51.579 THz, ρ=100 nm, EF=0.5 eV
    Distribution of the longitudinal electric field of mode 1 with the spacing d of (a) 10 nm, (b) 20 nm and (c) 75 nm
    Fig. 7. Distribution of the longitudinal electric field of mode 1 with the spacing d of (a) 10 nm, (b) 20 nm and (c) 75 nm
    Dependence of (a) effective refractive index and (b) propagation length on radius ρ when d=50 nm, f=51.579 THz, EF=0.5 eV
    Fig. 8. Dependence of (a) effective refractive index and (b) propagation length on radius ρ when d=50 nm, f=51.579 THz, EF=0.5 eV
    Distribution of the longitudinal electric field of mode 1 when ρ=(a) 30 nm and (b) 80 nm, respectively
    Fig. 9. Distribution of the longitudinal electric field of mode 1 when ρ=(a) 30 nm and (b) 80 nm, respectively
    Dependence of (a) effective refractive index and (b) propagation length on the Fermi energy EF when ρ=100 nm, d=50 nm, f=51.579 THz
    Fig. 10. Dependence of (a) effective refractive index and (b) propagation length on the Fermi energy EF when ρ=100 nm, d=50 nm, f=51.579 THz
    Distributions of the longitudinal electric field of mode 1 with the Fermi energy EF of (a) 0.4 eV and (b) 0.6 eV
    Fig. 11. Distributions of the longitudinal electric field of mode 1 with the Fermi energy EF of (a) 0.4 eV and (b) 0.6 eV
    Mode orderNameProperty
    0thMode 1Ez-cos mode
    Mode 2Ez-cos mode
    1thMode 3Ez-cos mode
    Mode 4Ez-sin mode
    Mode 5Ez-sin mode
    Mode 6Ez-cos mode
    Table 1. Lowest order modes
    Yanling Peng, Wenrui Xue, Zhuangzhi Wei, Changyong Li. Analysis of Modes in Graphene-Coated Parallel Dielectric Nanowires[J]. Acta Optica Sinica, 2018, 38(2): 0223002
    Download Citation