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

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216<br />

<strong>and</strong><br />

(CA)<br />

with f.b == t(.:.vo) <strong>and</strong> f./ == f.(2wo). These simplification lead to the relationship<br />

(C.5)<br />

vVe compare this to the relationship between Eb r<br />

<strong>and</strong> PP) without the zeroth<br />

order expansion, namely<br />

(C.6)<br />

The quantity that we measure is the SHG intensity averaged over all angular frequendes.<br />

:\"ote. this is obviously identical to the SHG intensity averaged over the pulse<br />

duration ..-\s stated previously, the SHG intensity depends on both the bound wave<br />

<strong>and</strong> free wave fields. The free wave is related to the bound wave by factors that are<br />

independent <strong>of</strong> w. Therefore, it is sufficient to compare the intensities <strong>of</strong> the bound<br />

waves with <strong>and</strong> without the zeroth order phase approximation to determine if the<br />

phase approximation is valid. For GaN (quartz), the discrepancy between the zeroth<br />

order approximation <strong>and</strong> the full approximation is less than .17% (.06%) over the<br />

fundamental wavelength range <strong>of</strong> 740 nm to 1 /-lm. Thus, the zeroth order expansion<br />

<strong>of</strong> w is valid for the coefficients <strong>of</strong> the bound wave field.<br />

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

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