“…If two pulses centered at the carrier frequencies and , propagate in opposite directions with wave vectors and , and group velocities and , respectively, the space representation of the field is (37) The interference pattern of the spectral components of this field (for example, considering the component at from the forward-propagating pulse and the component at of the backward-propagating pulse) is weighted by a complex coupling coefficient which depends on the material properties, the orientation of the medium, and the polarization of the waves [27], [31]. Therefore, we may write the grating as (38) where is the total optical power. Equation (38), describing the refractive index, may be used to express the nonlinear polarization as in standard coupled-mode theory [27]; the formalism presented in Section IV then dictates the polarization-driven evolution of the fields.…”