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

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38<br />

Fourier transform to E /2 (r, w) as<br />

( ? _.;:Kl --)<br />

vVhen k/ is used as a coefficient, (2.51) is the appropriate equation. .-\ first-order<br />

expansion,<br />

(2.56)<br />

, is required for any k / which appears in a phase. The second term in equation (2.56)<br />

contains an expression for the free wave group velocity in the quartz crystaL<br />

8kl<br />

8w 2w o<br />

1<br />

(?_.;) --) I<br />

The functional form <strong>of</strong> (bl (w) is determined by the calculations in section 2..!..! as<br />

(2.58)<br />

with Po is defined by equation (2.34). Csing equations (2.27), (2.50), (2.54), (2.55).<br />

(2.56), <strong>and</strong> (2.58), the a part <strong>of</strong> the frequency space representation <strong>of</strong> the transmitted<br />

nonlinear field can be Fourier transformed to the time domain in the following steps.<br />

The a integral can be expressed as<br />

(2.59)<br />

Integration <strong>of</strong> equation (2.59) with respect to w yields<br />

(2.60)<br />

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

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