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William Angerer - Department of Physics and Astronomy - University ...

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33<br />

2.4.4 Calculation <strong>of</strong> the Bound Wave From the Nonlinear Wave Equation<br />

Once the nonlinear polarization is determined from the fundamental fields, the nonlinear<br />

waves may calculated from the nonlinear wave equation <strong>and</strong> boundary conditions.<br />

This section outlines the calculation <strong>of</strong> the nonlinear bound wave from the<br />

wave equation <strong>and</strong> the nonlinear polarization.<br />

The nonlinear wave equation in frequency space is [461<br />

(2.36)<br />

The particular solution to the nonlinear wave equation must oscillate with the same<br />

phase as the nonlinear polarization (equation (2.33)), i.e. eikb(w)y.<br />

Since, kb is the<br />

bound wavevector, we subscript the particular solution <strong>of</strong> the wave equation with<br />

·'b" to denote it is the bound wave field. This solution has the form<br />

(2.37)<br />

Thus, the wave equation for Ebx is<br />

(2.38)<br />

vVe further simplify this expression by making a zeroth-order approximation for the<br />

coefficients in equation (2.38). We assume that w = 2w o • In other words. we assume<br />

that the angular frequency is identically equal to the center frequency <strong>of</strong> the Gaussian<br />

for the coefficients in equation (2.38). This approximation leads to the following<br />

Reproduced with permission <strong>of</strong> the copyright owner. Further reproduction prohibited without permission.

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