Hall effect - semiclassical approach

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SUMMARY

The discussion centers on the semiclassical treatment of the Hall effect as presented in the Aschroft and Mermin textbook. The introduction of the drift velocity vector is essential for understanding the motion of charged particles in crossed electric (E) and magnetic (B) fields. This drift velocity takes the form of the cross product of the electric and magnetic fields (E x B), which describes the cycloidal trajectory of a free charged particle. The transformation to a frame where the electric field is zero (E' = 0) is a critical step in deriving this behavior.

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  • Understanding of the Hall effect and its implications in physics.
  • Familiarity with the concepts of electric (E) and magnetic (B) fields.
  • Knowledge of semiclassical physics and particle dynamics.
  • Experience with frame transformations in special relativity.
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  • Study the derivation of the Hall effect in the context of semiclassical physics.
  • Explore the mathematical formulation of drift velocity in electromagnetic fields.
  • Learn about cycloidal motion of charged particles in crossed fields.
  • Investigate frame transformations and their applications in classical and relativistic physics.
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Physics students, educators, and researchers interested in advanced topics in electromagnetism and the semiclassical approach to particle dynamics.

armandowww
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I'm perplexed by semiclassical treatment of Hall effect.
I'm referring to Aschroft Mermin text. At page 233 is my doubt:
why is it necessary the introduction of w drift velocity vector and why does it take that form? :rolleyes:
 
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Recall the trajectory of a free charged particle in crossed E and B fields (from Jackson, or some SR course) - it is a cycloid with a drift velocity along E X B.

You can derive this by transforming to the frame where E' = 0.
 
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