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

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153<br />

GaN/Ah03 interface, which propagates through the sapphire substrate. E f2 . The<br />

free nonlinear waves have the form<br />

(6.16)<br />

with j = L rl, or 2. The amplitude <strong>of</strong> the free wave components are<br />

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

kfjz<br />

E/ix = --k Efj.<br />

fj<br />

( 6.17)<br />

Matching boundary conditions at the air/CaN interface determines Ell as<br />

k 10 2 k lIz ) -1(k210<br />

)<br />

Ell = ( k k - k/l (kbl.: - -k)EblX - kblxEblz .<br />

fOz /1<br />

fOz<br />

(6.18)<br />

Similarly, matching boundary conditions at the GaN/A.l 2 0 3 interface determines E frl<br />

<strong>and</strong> Ef2 as<br />

(<br />

k2 k ) -1 ( k 2<br />

k<br />

k 12z 11<br />

11 bIz k<br />

12z<br />

blx<br />

_ 12 lIz + k (k _ -.E..)E e-i(kbl=+kfl=Jd<br />

(6.19)<br />

-k E e-i(kb1=+kfl=Jd + (k _ kJ2k/lZ)E e-i2k/l=dJ)<br />

blx bIz 11 k k 11<br />

12z 11<br />

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

(<br />

k2 k )-l( k 2<br />

12 bIz - -- blx - -<br />

k /lz kf2<br />

k/lrz<br />

11 12z + k (k Ilr)E e-i(kbl--k/2-Jd<br />

(6.20)<br />

-k E e-i(kbl=-k/ 2=)d+2k E e-i(k fl =-k/2=Jd)<br />

blx bIz 11 fl .<br />

The previous calculations determine the magnitude <strong>of</strong> the nonlinear waves. The<br />

measured SHG signal also requires inclusion <strong>of</strong> the phase relationships between the<br />

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

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