Fig. 3. (a) Output response of add-drop-channel micro-ring resonators versus chemical potential of graphene when coupling gap is 2-6 nm and frequency is 30 THz. (a) Through-port; (b) drop-port
Fig. 5. Magnetic field intensity distributions of add-drop-channel micro-ring resonators at frequency of 30 THz under different chemical potentials of graphene. (a) 0.677 eV; (b) 0.95 eV
Fig. 6. Field intensity distributions of graphene-based plasmonic waveguide at frequency of 30 THz when chemical potential of graphene is 0.677 eV and 0.95 eV, respectively. (a) (c) Electric field; (b) (d) magnetic field
Fig. 7. Magnetic field intensity distributions of XNOR/XOR logic gates of graphene-based plasmonic waveguide at frequency of 30 THz under different input logic states of MRR 1 and MRR 2. (a) 00; (b) 01; (c) 10; (d) 11
Fig. 8. Transmission spectra of XNOR/XOR logic gates of graphene-based plasmonic waveguide under different input logic states of MRR 1 and MRR 2. (a) 00; (b) 01; (c) 10; (d) 11