Spin accumulation without spin current
arXiv:2112.11043 · doi:10.1103/PhysRevB.105.L201202
Abstract
The spin Hall (SH) effect is a phenomenon in which the spin current flows perpendicular to an applied electric field and causes the spin accumulation at the boundaries. However, in the presence of spin-orbit couplings, the spin current is not well defined. Here, we calculate the spin response to an electric-field gradient, which naturally appears at the boundaries. We derive a generic formula using the Bloch wave functions and the phenomenological relaxation time. We also calculate the response for the uniform Rashba model with -function nonmagnetic disorder within the first-order Born approximation and corresponding vertex corrections. We find the nonzero spin accumulation, although the SH conductivity exactly vanishes.
6 pages, 2 figures, Supplemental Material is available in the source
References in corpus (14)
- Dissipationless Quantum Spin Current at Room Temperature
- Direct electronic measurement of the spin Hall effect
- Quantum Spin Hall Effect and Enhanced Magnetic Response by Spin-Orbit Coupling
- Spin current and polarization in impure 2D electron systems with spin-orbit coupling
- On A Proper Definition of Spin Current
- Can Non-Equilibrium Spin Hall Accumulation be Induced in Ballistic Nanostructures?
- Spin-Hall effect in a disordered 2D electron-system
- Sign Changes of Intrinsic Spin Hall Effect in Semiconductors and Simple Metals: First-Principles Calculations
- Imaging mesoscopic spin Hall flow: Spatial distribution of local spin currents and spin densities in and out of multiterminal spin-orbit coupled semiconductor nanostructures
- Onsager Relations in Coupled Electric, Thermoelectric and Spin Transport: The Ten-Fold Way
- Quasiclassical approach to the spin-Hall effect in the two-dimensional electron gas
- Spin Hall effect of conserved current: Conditions for a nonzero spin Hall current
- Theory of conserved spin current and its application to two dimensional hole gas
- Mesoscopic Spin-Hall Effect in 2D electron systems with smooth boundaries