Hall coefficient and magnetoresistance of 2D spin-polarized electron systems
arXiv:cond-mat/0601232 · doi:10.1103/PhysRevB.73.121309
Abstract
Recent measurements of the 2D Hall resistance show that the Hall coefficient is independent of the applied in-plane magnetic field, i.e., the spin-polarization of the system. We calculate the weak-field Hall coefficient and the magnetoresistance of a spin polarized 2D system using the semi-classical transport approach based on the screening theory. We solve the coupled kinetic equations of the two carrier system including electron-electron interaction. We find that the in-plane magnetic field dependence of the Hall coefficient is suppressed by the weakening of screening and the electron-electron interaction. However, the in-plane magnetoresistance is mostly determined by the change of the screening of the system, and can therefore be strongly field dependent.
5 pages with 6 figures
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Cited by in corpus (3)
- Orbital Landau level dependence of the fractional quantum Hall effect in quasi-two dimensional electron layers: finite-thickness effects
- Temperature-dependent transport in a sixfold degenerate two-dimensional electron system on a H-Si(111) surface
- High magnetic field induced charge density waves and sign reversal of the Hall coefficient in graphite