Intrinsic Spin-Hall Effect in 2D Electron Systems
Eugene Mishchenko
Department of Physics, University of Utah
Conventional Hall effect is manifested by the
accumulation of electric charges at the edges of a conductor placed in a
magnetic field when electric current is driven through it. Spin-Hall effect
is a spin analog of the Hall effect: in the presence of electric current
spins of different directions may be driven to the opposite edges of a
conductor. This effect occurs as a result of spin-orbital interaction which
couples electron spin to its momentum. Spin-Hall effect can be extrinsic
(due to impurities) or intrinsic (due to band structure). I will present an
overview of basic theoretical concepts of Spin-Hall Effect as well as
address several existing experiments. Intrinsic Spin-Hall effect originally
predicted to be universal in a 2D electron gas -- independent of the
strength of spin-orbit coupling -- turned out to be destroyed by an
arbitrarily small disorder in any steady state of an infinite 2DEG. Is it
possible to have non-vanishing spin-Hall effect in case of a mesoscopic
system with the size less that the mean free path and to which extent will
the effect be really universal? We find that the net spin polarization
across the edge of the conductor is second order in spin-orbit coupling
constant independent of the form of the boundary potential.
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