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

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Appendix A<br />

Justification <strong>of</strong> First Order Expansion <strong>of</strong> the Phase<br />

In sections 2AA <strong>and</strong> 2.4.5, we truncated the expansion <strong>of</strong> k(w) to first order in<br />

(w - 2wo) for any k(w) which appeared in a phase. In this appendix, we justify this<br />

expansion by demonstrating that the second order term is negligible for the second<br />

harmonic pulse generated in quartz or GaN from a Ti:Ah03 fundamental source. The<br />

calculation follows the analysis developed by Silverstri et al [117].<br />

The first order term in the expansion <strong>of</strong> k(w) about (w - 2wo) gives rise to the<br />

group velocity mismatch which damps the interference <strong>of</strong> the bound <strong>and</strong> free waves.<br />

The second order term in the expansion accounts for the broadening <strong>of</strong> the pulse<br />

in time. This effect, known as group velocity dispersion (GVD), occurs because the<br />

frequency components <strong>of</strong> the pulse do not have the same group velocity. The pulse<br />

broadening increases as the distance through which pulse propagates increases or the<br />

dispersion is increased.<br />

In equation (2.42) we defined the general form <strong>of</strong> the nonlinear ultrafast waves<br />

209<br />

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

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