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

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150<br />

wavevector components. The free wavevectors are defined as<br />

k fi -<br />

7rnfiW<br />

c<br />

(6.5 )<br />

k fiz - - cos 8 fi k fi (6.6)<br />

k fix - sin 8 fi k fi, (6.7)<br />

where i is equal to 0, 1, 2 <strong>and</strong> denotes the air, GaN, <strong>and</strong> sapphire regions, respectively,<br />

<strong>and</strong> W is the angular frequency <strong>of</strong> the second-harmonic fields. The bound wavevectors<br />

are defined similarly with nbL substituted for nfi. The free (bound) wave angle <strong>of</strong><br />

incidence in region i is 8 fi (8bi) <strong>and</strong> is determined from 8 0 <strong>and</strong> nfi (nbi) by Snell's law.<br />

'-IVe now determine the nonlinear polarization induced in Ga0.' by the applied<br />

fundamental field.<br />

The p-polarized fundamental light field generates a nonlinear<br />

polarization <strong>of</strong> the form<br />

P<br />

(2) _ 2 2 ( ) (2) E E<br />

x - tpOL Wo Xxzx x z (6.8)<br />

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

P (2) - t2 ( ) ( (2) E E (2) E E )<br />

z - pOL Wo Xzxx x x + X;;zz ;; z . (6.9)<br />

Note that E is the incident fundamental field <strong>and</strong> tpoL(wo)E is the fundamental field<br />

transmitted into the GaN film. The nonlinear polarization generated by an s-polarized<br />

fundamental field is<br />

P<br />

(2) _ 2 ( ) (2) E E<br />

z - tsOL Wo Xzyy Y y. (6.10)<br />

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

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