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

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10<br />

the electric fields as<br />

In this thesis, we are concerned principally with second-harmonic generation<br />

(SHG), which is mediated by the second term in equation (2.3) with w = 2w o • i.e.<br />

(2.-1)<br />

Since dipole allowed nonlinearities occur in GaN, the local field approximation is<br />

valid.<br />

Once the second-order nonlinear polarization is determined from the second-order<br />

susceptibility <strong>and</strong> the incident fields, the nonlinear fields generated within the medium<br />

are determined from boundary conditions <strong>and</strong> the nonlinear wave equation<br />

€(w) 8 2 47r 8 2 2<br />

'V x 'V x E(w} + --E(w} = ----p( }(w).<br />

Solutions to equation (2.5) must also satisfy<br />

c2 8t 2 c 2 8t 2 (<br />

.) -) _ .. J<br />

'V. D(w) = 0 (2.6)<br />

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

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