Fig. 1. The third-order nonlinear, linear, as well as total OAC based on incident photon energy at the parameters of R = 10.0 nm, L = 10.0 nm, V0 = 100 meV, F = 100 kV/cm, I = 5.0 MW/cm2.
Fig. 2. The total OAC based on the incident photon energy at R = 10.0 nm, L = 10.0 nm, V0 = 100 meV, I = 5.0 MW/cm2 and four different values of F.
Fig. 3. The total OAC based on the incident photon energy at R = 10.0 nm, V0 = 100 meV, F = 100 kV/cm, I = 5.0 MW/cm2 and four different values of L.
Fig. 4. The total OAC based on the incident photon energy at L = 10.0 nm, V0 = 100 meV, F = 100 kV/cm, I = 5.0 MW/cm2 and three different values of R.
Fig. 5. The total OAC based on the incident photon energy at R = 10.0 nm, L = 10.0 nm, F = 100 kV/cm, I = 5.0 MW/cm2 and three distinct values of V0.
Fig. 6. The total OAC based on the incident photon energy at R = 10.0 nm, L = 10.0 nm, V0 = 100 meV, F = 100 kV/cm and three distinct values of I.