Transverse Spin-Orbit Force in the Spin Hall Effect in Ballistic Semiconductor Wires

Details Transverse Spin-Orbit Force in the Spin Hall Effect in Ballistic Semiconductor Wires Transverse Spin-Orbit Force in the Spin Hall Effect in Ballistic Semiconductor Wires

2005-03-17

arxiv.org/abs/cond-mat/0503415v2

Phys. Rev. B 72, 075335 (2005)

Physics

Condensed Matter

Mesoscale and Nanoscale Physics

5 pages, 4 color EPS figures; 2 new figures and expanded discussion on the sign of spin Hall quantities. To appear in Phys. Re

Scientific paper

10.1103/PhysRevB.72.075335

We introduce the spin and momentum dependent {\em force operator} which is defined by the Hamiltonian of a {\em clean} semiconductor quantum wire with homogeneous Rashba spin-orbit (SO) coupling attached to two ideal (i.e., free of spin and charge interactions) leads. Its expectation value in the spin-polarized electronic wave packet injected through the leads explains why the center of the packet gets deflected in the transverse direction. Moreover, the corresponding {\em spin density} will be dragged along the transverse direction to generate an out-of-plane spin accumulation of opposite signs on the lateral edges of the wire, as expected in the phenomenology of the spin Hall effect, when spin-$\uparrow$ and spin-$\downarrow$ polarized packets (mimicking the injection of conventional unpolarized charge current) propagate simultaneously through the wire. We also demonstrate that spin coherence of the injected spin-polarized wave packet will gradually diminish (thereby diminishing the ``force'') along the SO coupled wire due to the entanglement of spin and orbital degrees of freedom of a single electron, even in the absence of any impurity scattering.

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