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

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148<br />

L x<br />

i<br />

d<br />

1<br />

E( 00)<br />

air<br />

GaN<br />

sapphire<br />

(pi! rplO E frl<br />

Figure 6.4: Geometry <strong>of</strong> nonlinear waves in GaN/AI 2 0 3 . Notation is summarized in<br />

Table 6.3.<br />

nonzero nonlinear waves in air, GaN, <strong>and</strong> sapphire, <strong>and</strong> defines phase relationships<br />

between the waves.<br />

Our model includes all factors that affect the calculated second-harmonic signal<br />

by at least 10%. Thus, the model does not include the effect <strong>of</strong> bound wave reflection<br />

from the GaN / Al 2 0 3 interface because the reflection coefficient is small. i.e.<br />

ITs12(w)12 :::::: 0.03 <strong>and</strong> IT p 12(W)1 2 :::::: 0.015, where Tsdw) is the Fresnel reflection coefficient<br />

for s-polarized light with 1 (GaN) as the incident medium <strong>and</strong> 2 (sapphire)<br />

as the substrate medium. T p 12(W) is the Fresnel reflection coefficient for p-polarized<br />

light at the same interface. However, we include E,rl in our analysis, which is the<br />

nonlinear wave that is reflected from the GaN / Ah03 interface <strong>and</strong> undergoes one<br />

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

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