Cyclotron Resonance (Solid State Physics)

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SUMMARY

The discussion focuses on cyclotron resonance in solid state physics, specifically analyzing the energy surface described by the equation ε(𝑘) = ℏ²((𝑘ₓ² + 𝑘ᵧ²)/(2𝑚ₜ) + 𝑘𝓏²/(2𝑚ₗ)). Participants explore the derivation of the cyclotron frequency ωₕ = eB/(mₗmₜ)¹/²c, under the condition that the static magnetic field B is oriented in the xy-plane. The conversation highlights the dynamics of Bloch electrons and the application of the equation of motion in momentum space, emphasizing the importance of understanding the cross product of vectors in this context.

PREREQUISITES
  • Understanding of solid state physics concepts, particularly cyclotron resonance.
  • Familiarity with Bloch's theorem and the dynamics of Bloch electrons.
  • Knowledge of vector calculus, specifically cross products in three-dimensional space.
  • Proficiency in using the Schrödinger equation in momentum space representation.
NEXT STEPS
  • Study the derivation of cyclotron resonance in different geometries, such as spherical and ellipsoidal energy surfaces.
  • Learn about the implications of transverse and longitudinal mass parameters in solid state systems.
  • Explore the application of the equation of motion for charged particles in electromagnetic fields.
  • Investigate the momentum space representation of quantum operators and their physical interpretations.
USEFUL FOR

Students and researchers in solid state physics, particularly those focusing on quantum mechanics and the behavior of electrons in magnetic fields. This discussion is beneficial for anyone looking to deepen their understanding of cyclotron resonance and its mathematical foundations.

cepheid
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Homework Statement



Cyclotron resonance for a spheroidal energy surface. Consider the energy surface

\epsilon(\mathbf{k}) = \hbar^2 \left( \frac{k_x^2 + k_y^2}{2m_t} + \frac{k_z^2}{2m_l} \right)​

where mt is the transverse mass parameter and ml is the longitudinal mass parameter. A surface on which \epsilon(\mathbf{k}) is constant will be a spheroid. Use the equation of motion with \mathbf{v} = \hbar^{-1} \nabla_{\mathbf{k}} \epsilon to show that \omega_c = eB/(m_l m_t)^{1/2}c 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

\hbar \frac{d\mathbf{k}}{dt} = -\frac{e}{c}\mathbf{v} \times \mathbf{B} \ \ \ \textrm{cgs}\hbar \frac{d\mathbf{k}}{dt} = -e\mathbf{v} \times \mathbf{B} \ \ \ \textrm{SI}

The Attempt at a Solution



\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)​

= \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)​

Apply the equation of motion with

\mathbf{B} = B_x \hat{x} + B_y \hat{y}

\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})

Right so, um how am I supposed to proceed to compute such a cross product? :rolleyes:
 
Last edited:
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so, you have problem with mixing coordinate space vectors with momentum space vectors. you can still do this as long as you know what is
\hat k_i \times \hat x_j
at the moment I can't recall what this is... but i think \hat k_i \perp \hat x_i
should try the momentum space representation of the position operator as a guide to convert them, perhaps?
 
Did you ever figure this out?
 
Last edited:
I just had this on a test, but didn't get it done so as you can imagine i was curious about it. Also, just realized you put this on here a year ago so nevermind.
 

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