arXiv · cond-mat/0411488
Zitterbewegung and its effects on electrons in semiconductors
Abstract
An analogy between the band structure of narrow gap semiconductors and the Dirac equation for relativistic electrons in vacuum is used to demonstrate that semiconductor electrons experience a Zitterbewegung (trembling motion). Its frequency is $ω_Z \approx {\cal E}_g/\hbar$ and its amplitude is $λ_Z$, where $λ_Z = \hbar/m^*_0 u$ corresponds to the Compton wavelength in vacuum (${\cal E}_g$ is the energy gap, $m^*_0$ is the effective mass and $u \approx 1.3\times10^8$ cm/sec). Once the electrons are described by a two-component spinor for a specific energy band there is no Zitterbewegung but the electrons should be treated as extended objects of size $λ_Z$. Possible consequences of the above predictions are indicated.
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Wlodek Zawadzki. 2004-11-18. Zitterbewegung and its effects on electrons in semiconductors. https://doi.org/10.1103/physrevb.72.085217
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