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Introduction to Nanotechnology

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A X '<br />

Wavevec<strong>to</strong>r A<br />

Si<br />

c z<br />

2.2. ENERGY BANDS 27<br />

Figure 2.18. Band structure plots of the energy bands of the indirect-gap semiconduc<strong>to</strong>rs Si and<br />

Ge. The bandgap (absence of bands) lies slightly above the Fermi energy E = 0 on both figures,<br />

with the conduction band above and the valence band below the gap. The figure shows that the<br />

lowest point or bot<strong>to</strong>m of the conduction band of Ge is at the energy E = 0.6 at the symmetry<br />

point L (labeled by b+), and for Si it is 85% of the way along the direction A, from r,5 <strong>to</strong> X,. It is<br />

clear from Fig. 2.15 that the bot<strong>to</strong>m of the conduction band of the direct-gap semiconduc<strong>to</strong>r<br />

GaAs is at the symmetry point r,. The <strong>to</strong>p of the valence band is at the center point r of the<br />

Brillouin zone for both materials.

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