Comparing Eq. (5.34) with
| \begin{equation*} \vec{j}= \sigma \vec{E} \qquad , \end{equation*} | (5.35) |
we find
| \begin{equation*} \sigma = \frac{q^2 \tau n_e}{m^*} \qquad ; \end{equation*} | (5.36) |
including the mobility
| \begin{equation*} \mu_e := \frac{q \tau}{m^*} \qquad , \end{equation*} | (5.37) |
we finally get
| \begin{equation*} \sigma = q \mu_e n_e \qquad . \end{equation*} | (5.38) |
Additional information and several illustrative graphics can be found in the MaWi II script.
© J. Carstensen (Stat. Meth.)