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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

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