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

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50<br />

2.6 Conclusion<br />

In this brief section we relate the theoretical results derived in this chapter to the<br />

nonlinear optical properties <strong>of</strong> GaN, which are presented in the subsequent chapters.<br />

In section 2.2, we discuss the properties <strong>of</strong> the second-order nonlinear susceptibility,<br />

x;}L(w = 2wo). vVe suggest which states lead to a resonant enhancement <strong>of</strong><br />

x~~L(w<br />

= 2wo) for both GaN bulk <strong>and</strong> defect states in sections 5.-1.1 <strong>and</strong> 6.5, respectively.<br />

The determination <strong>of</strong> the states that contribute to the nonlinear optical<br />

response follows directly from the application <strong>of</strong> group theory to equation 2.8.<br />

In section 2.3 we discuss the relationship between material symmetry <strong>and</strong> secondorder<br />

susceptibility elements. Using symmetry, we determined the unique nonzero<br />

susceptibility elements for GaN. These elements, combined with experimental geometry.<br />

influence nonlinear optical transmittance spectra <strong>of</strong> GaN (see chapter 6).<br />

Finally, the majority <strong>of</strong> this introductory nonlinear optics chapter is concerned<br />

with a detailed investigation <strong>of</strong> nonlinear optical interference, i.e. Maker fringes. vVe<br />

contrast nonlinear optical interference for monochromatic <strong>and</strong> ultrafast laser sources.<br />

\Ve demonstrated that nonlinear optical interference, which is due to wavevector<br />

mismatch, is damped by group velocity mismatch. We apply this ultrafast analysis to<br />

determine the second-order susceptibility elements from the nonlinear optical spectra<br />

<strong>of</strong> GaN in sections 6.3 <strong>and</strong> 6.4.<br />

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

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