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C. Bulutay Semiconductor Electronic Structure & Optical Processes <strong>Lecture</strong> 6<br />
The Journey of the Eigenfunctions<br />
For the unperturbed H, eigenfn’s at the band edge we anticipated them to be of s and p<br />
type orbital symmetry: S, ↑ , S, ↓ , X, ↑ , X, ↓ , Y, ↑ , Y, ↓ , Z, ↑ , Z,<br />
↓<br />
u = iS ↓<br />
1<br />
u2<br />
=<br />
X − iY<br />
↑ = Y<br />
2<br />
u = Z ↓ = Y ↓<br />
3<br />
5<br />
7<br />
1 0<br />
1 0<br />
X − iY<br />
u = ↓ = Y<br />
2<br />
1 −1<br />
X + iY<br />
u4<br />
=− ↑ = Y<br />
2<br />
u = iS ↑<br />
u6<br />
X + iY<br />
=− ↓ = Y<br />
2<br />
u = Z ↑ = Y ↑<br />
1 1<br />
1 1<br />
8 1 −1<br />
↑<br />
↓<br />
↑<br />
↓<br />
Perturbation:<br />
SO+k.P<br />
Kane’s band edge eigenfn’s