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

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115<br />

5.2.1 B<strong>and</strong> Gap <strong>Physics</strong><br />

GaN is a direct b<strong>and</strong> gap semiconductor with a b<strong>and</strong> gap <strong>of</strong> 3.4 e V. Because a<br />

medium's response to an incident light field is enhanced when the photon has an<br />

energy nearly equal to an energy state <strong>of</strong> the system, the properties <strong>of</strong> the conduction<br />

b<strong>and</strong> minimum <strong>and</strong> valence b<strong>and</strong> maximum strongly influence the optical characteristics<br />

<strong>of</strong> GaN in the near b<strong>and</strong> gap region. Therefore. in this section we focus<br />

mainly on the characteristics <strong>of</strong> the valence b<strong>and</strong> maximum <strong>and</strong> the conduction b<strong>and</strong><br />

minimum. This section includes some discussion <strong>of</strong> group theory, which will be more<br />

thoroughly explained in section 5.4. Fig. 5.2 displays the calculated b<strong>and</strong> structure<br />

<strong>of</strong> GaN. The b<strong>and</strong> gap sits at the r point <strong>of</strong> the Brillouin zone (see Fig. 5.3).<br />

The<br />

valence b<strong>and</strong> maximum is built (principally) <strong>of</strong> the N 2p states. In the absence <strong>of</strong><br />

spin orbit splitting, the valence b<strong>and</strong> maximum consists <strong>of</strong> r 6 <strong>and</strong> r l b<strong>and</strong>s that are<br />

split by the hexagonal crystal field by ~cr<br />

= 22 meV [78]. \Vhen spin is included.<br />

the r 6 b<strong>and</strong> splits into r 9 <strong>and</strong> r 7 b<strong>and</strong>s, separated by the spin-orbit energy <strong>of</strong> ~so =<br />

11 meV [78]. Inclusion <strong>of</strong> spin also transforms the r l b<strong>and</strong> to r 7 . Because spin orbit<br />

splitting is so small, matrix elements may be calculated from the representation <strong>of</strong><br />

the point group without spin.<br />

The conduction b<strong>and</strong> minimum is built (principally) <strong>of</strong> the Ga <strong>and</strong> ~ s-states.<br />

Without spin, the state is labeled as r l , <strong>and</strong> with the inclusion <strong>of</strong> spin, the b<strong>and</strong><br />

transforms as r 7. The valence <strong>and</strong> conduction b<strong>and</strong>s are separated by 3.4 eV at room<br />

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

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