2.4.2.3 Analytical Band Structures of Si and Ge

For Si the lowest extrema of the conduction band are located along the $ \Delta$ axes near the $ X$ points of the first Brillouin zone and are called $ X$ valleys. In the case of Ge they are located exactly at the $ L$ points of the first Brillouin zone and called $ L$ valleys. Thus the surface of constant energy2.24 for Si, equation (2.76), represents six full ellipsoids while for Ge it represents eight half-ellipsoids. This is also shown in Fig. 2.6.
Figure 2.6: The surfaces of constant energy for Si and Ge.
\includegraphics[width=.8\linewidth]{figures/figure_6}
Two of the three effective masses are equal to each other and called transverse effective masses. The third mass is called the longitudinal effective mass. They are denoted by $ m_{t}$ and $ m_{l}$, respectively2.25. The numerical values [20] for the parameters of the analytical expression for the conduction band of Si and Ge are given in Table 2.1.

Table 2.1: Analytical conduction band structure parameters for Si and Ge.
  $ m_{t}^{X}$ $ m_{l}^{X}$ $ m_{t}^{L}$ $ m_{l}^{L}$ $ \alpha_{X}$ $ \alpha_{L}$
Silicon 0.191 0.903 0.126 1.634 0.5 $ eV^{-1}$ 0.3 $ eV^{-1}$
Germanium 0.204 1.791 0.101 1.387 0.5 $ eV^{-1}$ 0.3 $ eV^{-1}$


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