# NonlinearSusceptibility

Model for an instantaneous nonlinear chi3 susceptibility. The expression for the instantaneous nonlinear polarization is given below.

PNL=ε0χ3E2EP_{NL} = \varepsilon_0 \chi_3 |E|^2 E

# Nonlinear Susceptibility

chi3: Chi3 nonlinear susceptibility.

Type: floating-point number

  • Unit: μm²/V²
  • Default: 0

# Notes

  • This model uses real time-domain fields, so χ3\chi_3 must be real. For complex fields (e.g. when using Bloch boundary conditions), the nonlinearity is applied separately to the real and imaginary parts, so that the above equation holds when both EE and PNLP_{NL} are replaced by their real or imaginary parts. The nonlinearity is applied to the real and imaginary components separately since each of those represents a physical field.
  • Different field components do not interact nonlinearly. For example, when calculating PNL,xP_{NL,x}, we approximate E2Ex2|E|^{2}\approx|E_x|^{2}. This approximation is valid when the EE field is predominantly polarized along one of the x, y, or z axes.