How Does an Electron Move in Real Space on an Open Orbit in a Magnetic Field?

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SUMMARY

The discussion focuses on the motion of electrons in real space on an open orbit within a monovalent tetragonal metal subjected to a magnetic field. It emphasizes the transition from k-space to real space, highlighting the importance of the semi-classical regime where particles are localized with minimal uncertainties in position and momentum. The group velocity, defined as the gradient of the dispersion relation, leads to oscillations in one direction while maintaining a consistent flow in the opposite direction, resulting in a macroscopic current across the sample.

PREREQUISITES
  • Understanding of open orbits in solid-state physics
  • Familiarity with Brillouin zones and k-space concepts
  • Knowledge of semi-classical electron dynamics
  • Comprehension of group velocity and dispersion relations
NEXT STEPS
  • Study the effects of magnetic fields on electron motion in solids
  • Explore the concept of Brillouin zones in more depth
  • Learn about the mathematical formulation of group velocity in solid-state physics
  • Investigate the implications of macroscopic currents in conductive materials
USEFUL FOR

Physicists, materials scientists, and students studying solid-state physics, particularly those interested in electron dynamics and the effects of magnetic fields on electronic properties.

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Homework Statement


An open orbit in a monovalent tetragonal metal connects opposite faces of a Brillioun zone. A magnetic field is normal to the plane of the open orbit. Describe in real space the motion of the electron on this orbit in the presence of the magnetic field.


Homework Equations





The Attempt at a Solution


I am having loads of difficulty translating what goes on in k-space to what goes on in real space. The picture in k-space is very clear, but I am just really confused about what it means. It is not even clear to me what how the velocity vector is changing!
 
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I don't know if the text says so, but all this is predicated on working in a semi-classical regime. So the particles can be localised with small uncertainties in space and momentum. In that case, remember that the group velocity is the gradient of the dispersion relation. So for an open orbit, you would get oscillations about zero in the group velocity in some direction, but in the other direction it would always be +ve or -ve. So you would get a macroscopic current that flows across the entire sample (or you would, if it wasn't for the fact there's an identical current flowing the other way...)
 

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