Spin relaxation in narrow wires of a two-dimensional electron gas
arXiv:cond-mat/0606209 · doi:10.1103/PhysRevB.74.155316
Abstract
How does an initially homogeneous spin-polarization in a confined two-dimensional electron gas with Rashba spin-orbit coupling evolve in time? How does the relaxation time depend on system size? We study these questions for systems of a size that is much larger than the Fermi wavelength, but comparable and even shorter than the spin relaxation length. Depending on the confinement spin-relaxation may become faster or slower than in the bulk. An initially homogeneously polarized spin system evolves into a spiral pattern.
5 pages, 4 figures
References in corpus (6)
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- Suppression of Spin Relaxation in Submicron InGaAs Wires
- Spin-Hall transport of heavy holes in III-V semiconductor quantum wells
- Quasiclassical approach to the spin-Hall effect in the two-dimensional electron gas
- Long-Lived Spin Coherence States
- Quasiclassical theory of charge transport in disordered interacting electron systems
Cited by in corpus (13)
- Spontaneous Edge Accumulation of Spin Currents in Finite-Size Two-Dimensional Diffusive Spin-Orbit Coupled SFS Heterostructures
- Spin polarization decay in spin-1/2 and spin-3/2 systems
- Spontaneous Emergence of Persistent Spin Helix from Homogeneous Spin Polarization
- Enhanced longevity of the spin helix in low-symmetry quantum wells
- Semiclassical path integral approach on spin relaxations in narrow wires
- Hole spin relaxation in -type GaAs quantum wires
- Radial Spin Helix in Two-Dimensional Electron Systems with Rashba Spin-Orbit Coupling
- Current-induced spin polarization and the spin Hall effect: a quasiclassical approach
- Electron spin relaxation in n-type InAs quantum wires
- Spin drift-diffusion for two-subband quantum wells
- Effects of interaction on field-induced resonances in confined Fermi liquid
- Driving spin and charge in quantum wells by surface acoustic waves
- Reliable modeling of weak antilocalization for accurate spin-lifetime extraction