Spin Polarization of Quasi Two-Dimensional Hole Systems
arXiv:cond-mat/0401067 · doi:10.1103/PhysRevB.71.113307
Abstract
In quasi two-dimensional (2D) hole systems with an effective spin j=3/2, heavy hole-light hole splitting results in a quantization of angular momentum perpendicular to the 2D plane. The spin polarization of quasi 2D hole systems due to an in-plane magnetic field B thus competes with the heavy hole-light hole splitting. As a result, the spin polarization of hole systems is very different from the spin polarization of j=1/2 electron systems. In particular, it is shown that the spin polarization of quasi 2D heavy hole systems can change its sign at a finite value of B.
4 pages, 2 figures
References in corpus (4)
- Metal-insulator transition in two-dimensional electron systems
- Spin Susceptibility of an Ultra-Low Density Two Dimensional Electron System
- Spin Orientation and Spin Precession in Inversion-Asymmetric Quasi Two-Dimensional Electron Systems
- Role of finite layer thickness in spin-polarization of GaAs 2D electrons in strong parallel magnetic fields
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- Spin states in InAs/AlSb/GaSb semiconductor quantum wells
- Current-induced Spin Polarization in Two-Dimensional Hole Gas
- Spin-subband populations and spin polarization of quasi two-dimensional carriers under in-plane magnetic field
- Spin Hall Conductance of the Two Dimensional Hole Gas in a Perpendicular Magnetic Field
- Carrier-density-controlled anisotropic spin susceptibility of two-dimensional hole systems
- Electrical and thermoelectric transport properties of two-dimensional fermionic systems with -cubic spin-orbit coupling
- Magnetotransport properties of two-dimensional fermions with -cubic Rashba spin-orbit interaction
- Non-adiabatic Berry phase for semiconductor heavy holes under the coexistence of Rashba and Dresselhaus spin-orbit interactions
- Coulomb-exchange effects in nanowires with spin splitting due to a radial electric field