- 5,197
- 38
Homework Statement
Cyclotron resonance for a spheroidal energy surface. Consider the energy surface
[tex]\epsilon(\mathbf{k}) = \hbar^2 \left( \frac{k_x^2 + k_y^2}{2m_t} + \frac{k_z^2}{2m_l} \right)[/tex]
where mt is the transverse mass parameter and ml is the longitudinal mass parameter. A surface on which [itex]\epsilon(\mathbf{k})[/itex] is constant will be a spheroid. Use the equation of motion with [itex]\mathbf{v} = \hbar^{-1} \nabla_{\mathbf{k}} \epsilon[/itex] to show that [itex]\omega_c = eB/(m_l m_t)^{1/2}c[/itex] when the static magnetic field B lies in the xy plane.
Homework Equations
Dynamics of Bloch Electrons
The equation of motion for an electron subject to the periodic potential of a crystal lattice is
[tex]\hbar \frac{d\mathbf{k}}{dt} = -\frac{e}{c}\mathbf{v} \times \mathbf{B} \ \ \ \textrm{cgs}[/tex][tex]\hbar \frac{d\mathbf{k}}{dt} = -e\mathbf{v} \times \mathbf{B} \ \ \ \textrm{SI}[/tex]
The Attempt at a Solution
[tex]\mathbf{v} = \hbar^{-1} \nabla_{\mathbf{k}} \epsilon(\mathbf{k}) = \hbar^{-1} \left( \hat{k}_x \frac{\partial}{\partial k_x} + \hat{k}_y \frac{\partial}{\partial k_y} + \hat{k}_z \frac{\partial}{\partial k_z} \right) \hbar^2 \left( \frac{k_x^2 + k_y^2}{2m_t} + \frac{k_z^2}{2m_l} \right)[/tex]
[tex]= \hbar \left( \hat{k}_x \frac{k_x}{m_t} + \hat{k}_y \frac{k_y}{m_t} + \hat{k}_z \frac{k_z}{m_l} \right)[/tex]
Apply the equation of motion with
[tex]\mathbf{B} = B_x \hat{x} + B_y \hat{y}[/tex]
[tex]\frac{d\mathbf{k}}{dt} = -\frac{e}{c}\left( \hat{k}_x \frac{k_x}{m_t} + \hat{k}_y \frac{k_y}{m_t} + \hat{k}_z \frac{k_z}{m_l} \right) \times (B_x \hat{x} + B_y \hat{y})[/tex]
[tex]\frac{d\mathbf{k}}{dt} = -\frac{e}{c}\left( \hat{k}_x \frac{k_x}{m_t} + \hat{k}_y \frac{k_y}{m_t} + \hat{k}_z \frac{k_z}{m_l} \right) \times (B_x \hat{x} + B_y \hat{y})[/tex]
Right so, um how am I supposed to proceed to compute such a cross product?
Last edited: