{ "id": "cond-mat/0311221", "version": "v3", "published": "2003-11-10T22:48:23.000Z", "updated": "2004-07-01T14:39:47.000Z", "title": "Drift-diffusion model for spin-polarized transport in a non-degenerate 2DEG controlled by a spin-orbit interaction", "authors": [ "Semion Saikin" ], "comment": "16 pages, 3 figures", "journal": "J. Phys.: Condens. Matter 16, 5071-5081 (2004)", "doi": "10.1088/0953-8984/16/28/025", "categories": [ "cond-mat.mes-hall" ], "abstract": "We apply the Wigner function formalism to derive drift-diffusion transport equations for spin-polarized electrons in a III-V semiconductor single quantum well. Electron spin dynamics is controlled by the linear in momentum spin-orbit interaction. In a studied transport regime an electron momentum scattering rate is appreciably faster than spin dynamics. A set of transport equations is defined in terms of a particle density, spin density, and respective fluxes. The developed model allows studying of coherent dynamics of a non-equilibrium spin polarization. As an example, we consider a stationary transport regime for a heterostructure grown along the (0, 0, 1) crystallographic direction. Due to the interplay of the Rashba and Dresselhaus spin-orbit terms spin dynamics strongly depends on a transport direction. The model is consistent with results of pulse-probe measurement of spin coherence in strained semiconductor layers. It can be useful for studying properties of spin-polarized transport and modeling of spintronic devices operating in the diffusive transport regime.", "revisions": [ { "version": "v3", "updated": "2004-07-01T14:39:47.000Z" } ], "analyses": { "keywords": [ "spin-orbit interaction", "non-degenerate 2deg", "spin-polarized transport", "drift-diffusion model", "spin dynamics strongly depends" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 16, "language": "en", "license": "arXiv", "status": "editable" } } }