On the nature of steady states of spin distributions in the presence of spin-orbit interactions

Abstract

In the presence of spin-orbit interactions, the steady state established for spin distributions in an electric field is qualitatively different from the steady state for charge distributions. This is primarily because the steady state established for spin distributions involves spin precession due to spin-orbit coupling. We demonstrate in this work that the spin density matrix in an external electric field acquires two corrections with different dependencies on the characteristic momentum scattering time. One part is associated with conserved spins, diverges in the clean limit and is responsible for the establishment of a steady-state spin density in electric fields. Another part is associated with precessing spins, is finite in the clean limit and is responsible for the establishment of spin currents in electric fields. Scattering between these distributions has important consequences for spin dynamics and spin-related effects in general, and explains some recent puzzling observations, which are captured by our unified theory.

10 pages, 1 figure

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Cited by in corpus (7)

• Ballistic spin transport in the presence of interfaces with strong spin-orbit coupling
• An electrically driven spin qubit based on valley mixing
• Current-induced spin polarization at the surface of metallic films: a theorem and an ab initio calculation
• Weak momentum scattering and the conductivity of graphene
• A generalized Stoner criterion and versatile spin ordering in two-dimensional spin-orbit coupled electron systems
• Spin transfer torques due to the bulk states of topological insulators
• Boltzmann approach to the spin Hall effect revisited and electric field modified collision integrals