Contributed Article
Microscopic theory of spin-filtering in non-magnetic semiconductor nanostructures
Article first published online: 29 NOV 2007
DOI: 10.1002/pssc.200776593
Copyright © 2008 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim
Issue

physica status solidi (c)
Special Issue: 15th International Conference on Nonequilibrium Carrier Dynamics in Semiconductors (HCTS-15)
Volume 5, Issue 1, pages 290–293, January 2008
Additional Information
How to Cite
Kubis, T. and Vogl, P. (2008), Microscopic theory of spin-filtering in non-magnetic semiconductor nanostructures. Phys. Status Solidi C, 5: 290–293. doi: 10.1002/pssc.200776593
Publication History
- Issue published online: 7 JAN 2008
- Article first published online: 29 NOV 2007
- Manuscript Accepted: 28 AUG 2007
- Manuscript Revised: 22 AUG 2007
- Manuscript Received: 20 JUL 2007
Funded by
- Deutsche Forschungsgemeinschaft (SFB 631, SPP 1285)
- Österreichische Fonds zur Förderung der Wissenschaft (SFB IRON)
- Nano Initiative Munich
- Abstract
- References
- Cited By
Keywords:
- 72.25.Mk
Abstract
In this paper, we investigate the intrinsic spin-Hall effect in mesoscopic systems, i.e. spin-orbit induced spin-polarizations with and without external magnetic fields in confined two-dimensional systems at low temperatures. We employ a non-equilibrium Green's function approach that takes into account the coupling of non-equilibrium spin occupancies and spin-resolved electronic scattering states in open nanometer quantum systems. Importantly, our calculations go beyond the widely used continuum approximation of the spin-orbit interaction in the envelope function approximation and are based on a microscopic relativistic tight-binding approach that ensures the spin-orbit effects to be properly taken into account for any degree of charge confinement and localization and to all orders in the electron wave vector. We show that the qualitative trends and results in spin polarizations, their dependency on charge density, spin-orbit interaction strength, and confinement, as obtained within the envelope function approximation, agree with the results of atomistic calculations. The quantitative results, on the other hand, can differ significantly. (© 2008 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim)

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