Author Affiliations
1 College of Physics and Electronic Engineering, Shanxi University, Taiyuan, Shanxi 0 30006, China2 State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Laser Spectroscopy, Shanxi University, Taiyuan, Shanxi 0 30006, Chinashow less
Fig. 1. Cross-section diagram of graphene-coated parallel dielectric nanowires
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
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
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
Fig. 5. Distribution of the longitudinal electric field of mode 1 with the operating frequency of (a) 35 THz and (b) 55 THz
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
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
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
Fig. 9. Distribution of the longitudinal electric field of mode 1 when ρ=(a) 30 nm and (b) 80 nm, respectively
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
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 order | Name | Property |
---|
0th | Mode 1 | Ez-cos mode | Mode 2 | Ez-cos mode | 1th | Mode 3 | Ez-cos mode | Mode 4 | Ez-sin mode | Mode 5 | Ez-sin mode | Mode 6 | Ez-cos mode |
|
Table 1. Lowest order modes