{ "id": "0901.0053", "version": "v1", "published": "2008-12-31T04:16:16.000Z", "updated": "2008-12-31T04:16:16.000Z", "title": "Spin Hall effect in the kagome lattice with Rashba spin-orbit interaction", "authors": [ "Guocai Liu", "Ping Zhang", "Zhigang Wang", "Shu-Shen Li" ], "comment": "7 pages, 3 figures. Phys. Rev. B (in press)", "doi": "10.1103/PhysRevB.79.035323", "categories": [ "cond-mat.mes-hall", "cond-mat.str-el" ], "abstract": "We study the spin Hall effect in the kagom\\'{e} lattice with Rashba spin-orbit coupling. The conserved spin Hall conductance $\\sigma_{xy}^{s}$ (see text) and its two components, i.e., the conventional term $\\sigma_{xy}^{s0}$ and the spin-torque-dipole term $\\sigma_{xy}^{s\\tau}$, are numerically calculated, which show a series of plateaus as a function of the electron Fermi energy $\\epsilon_{F}$. A consistent two-band analysis, as well as a Berry-phase interpretation, is also given. We show that these plateaus are a consequence of the various Fermi-surface topologies when tuning $\\epsilon_{F}$. In particular, we predict that compared to the case with the Fermi surface encircling the $\\mathbf{\\Gamma}$ point in the Brillouin zone, the amplitude of the spin Hall conductance with the Fermi surface encircling the $\\mathbf{K}$ points is twice enhanced, which makes it highly meaningful in the future to systematically carry out studies of the $\\mathbf{K}$-valley spintronics.", "revisions": [ { "version": "v1", "updated": "2008-12-31T04:16:16.000Z" } ], "analyses": { "subjects": [ "73.23.-b", "72.25.Dc", "72.10.Bg" ], "keywords": [ "spin hall effect", "rashba spin-orbit interaction", "kagome lattice", "fermi surface encircling", "conserved spin hall conductance" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Physics Letters A", "year": 2009, "month": "May", "volume": 373, "number": "23-24", "pages": 2091 }, "note": { "typesetting": "TeX", "pages": 7, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2009PhLA..373.2091L" } } }