Random walk approach to spin dynamics in a two-dimensional electron gas with spin-orbit coupling
arXiv:1008.0132 · doi:10.1103/PhysRevB.82.155324
Abstract
We introduce and solve a semi-classical random walk (RW) model that describes the dynamics of spin polarization waves in zinc-blende semiconductor quantum wells. We derive the dispersion relations for these waves, including the Rashba, linear and cubic Dresselhaus spin-orbit interactions, as well as the effects of an electric field applied parallel to the spin polarization wavevector. In agreement with fully quantum mechanical calculations [Kleinert and Bryksin, Phys. Rev. B \textbf{76}, 205326 (2007)], the RW approach predicts that spin waves acquire a phase velocity in the presence of the field that crosses zero at a nonzero wavevector, . In addition, we show that the spin-wave decay rate is independent of field at but increases as for . These predictions can be tested experimentally by suitable transient spin grating experiments.
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- Current-controlled Spin Precession of Quasi-Stationary Electrons in a Cubic Spin-Orbit Field
- Relaxation mechanisms of the persistent spin helix
- Spin dynamics in the strong spin-orbit coupling regime
- Macroscopic transverse drift of long current-induced spin coherence in two-dimensional electron gases
- Gate control of the spin mobility through the modification of the spin-orbit interaction in two-dimensional systems
- Ambipolar spin transport in (111) GaAs quantum wells