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Shubnikov–de Haas effect (Read 2554 times)
Gerrit-Jan Linker
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Shubnikov–de Haas effect
12.10.12 at 08:32:52
Shubnikov–de Haas effect
The Shubnikov–de Haas effect (ShdH) is a macroscopic manifestation of the inherent quantum mechanical nature of matter.
The effect concerns an oscillation in the conductivity of a material that occurs at low temperatures in the presence of very intense magnetic fields.  
It is often used to determine the effective mass of charge carriers (electrons and electron holes), allowing investigators to distinguish among majority and minority carrier populations.
At sufficiently low temperatures and high magnetic fields, the free electrons in the conduction band of a metal, semimetal, or narrow band gap semiconductor will behave like simple harmonic oscillators. When the magnetic field strength is changed, the oscillation period of the simple harmonic oscillators changes proportionally. The resulting energy spectrum is made up of Landau levels separated by the cyclotron energy. These Landau levels are further split by the Zeeman energy. In each Landau level the cyclotron and Zeeman energies and the number of electron states (eB/h) all increase linearly with increasing magnetic field. Thus, as the magnetic field increases, the spin-split Landau levels move to higher energy. As each energy level passes through the Fermi energy, it depopulates as the electrons become free to flow as current. This causes the material's transport and thermodynamic properties to oscillate periodically, producing a measurable oscillation in the material's conductivity. Since the transition across the Fermi 'edge' spans a small range of energies, the waveform is square rather than sinusoidal, with the shape becoming ever more square as the temperature is lowered.
(ET)2I3 is a textbook example of the ShdH effect in a 2D conductor.
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« Last Edit: 12.10.12 at 08:35:23 by Gerrit-Jan Linker »  

Gerrit-Jan Linker
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