Spin splitting of two dimensional states in the conduction band of asymmetric heterostructures: contribution from the atomically sharp interface
arXiv:1410.2432 · doi:10.1134/S002136401315006X
Abstract
The effect of an atomically sharp impenetrable interface on the spin splitting of the spectrum of two-dimensional electrons in heterostructures based on (001) III-V compounds has been analyzed. To this end, the single band Hamiltonian for envelope functions is supplemented by a general boundary condition taking into account the possibility of the existence of Tamm states. This boundary condition also takes into account the spin-orbit interaction, the asymmetry of a quantum well, and the lack of inversion symmetry in the crystal and contains the single phenomenological length characterizing the structure of the interface at atomic scales. The model of a quasitriangular well created by the electric field has been considered. After the unitary transformation to zero boundary conditions, in the modified Hamiltonian interfacial contribution appears, from which the two-dimensional spin Hamiltonian is obtained through averaging over the fast motion along the normal. In the absence of magnetic field , this contribution is the sum of the Dresselhaus and the Bychkov-Rashba terms with the constants renormalized owing to the interfacial contribution. In the field containing the quantizing component , the off - diagonal (in cubic axes) components of the -factor tensor are linear functions of and the number of the Landau level . The results are in qualitative agreement with the experimental data.
corrected version
References in corpus (2)
Cited by in corpus (4)
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- Interface Contributions to the Spin-Orbit Interaction Parameters of Electrons at the (001) GaAs/AlGaAs Interface
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- Electron density effect on spin-orbit interaction in [001] GaAs quantum wells