Flaviu Cipcigan edited magnetoresistance.tex  over 10 years ago

Commit id: ab8d2b8ac2ceb9020026b8449424a603c2c33ff4

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\end{equation}  Substituting the components of $\mathbf{B}$, $\mathbf{E}$ and $\mathbf{j} = n q \mathbf{p} / m^*$ into the equation of motion for the charge carrier in the presence of a magnetic field \eqref{eq:eom-B} gives:  \begin{equation}  \tau \frac{d\mathbf{j}}{dt} = - \mathbf{j} + \sigma_0 \mathbf{E} + (\omega_\textrm{c} \tau) \mathbf{j} \cross \times  \left(\frac{\mathbf{B}}{B} \right) \end{equation}  where  \begin{equation}