Abstract
Planar spin transport in disordered ultrathin magnetic bilayers comprising a ferromagnet and a normal metal (typically used for spin pumping, spin Seebeck and spin-orbit torque experiments) is investigated theoretically. Using a tight-binding model that puts the extrinsic spin Hall effect and spin swapping on equal footing, we show that the nature of spin-orbit coupled transport dramatically depends on the ratio between the layer thickness d and the mean free path λ. While the spin Hall effect dominates in the diffusive limit (d≫λ), spin swapping dominates in the Knudsen regime (d≲λ). A remarkable consequence is that spin swapping induces a substantial fieldlike torque in the Knudsen regime.
Original language | English (US) |
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Journal | Physical Review Letters |
Volume | 117 |
Issue number | 3 |
DOIs | |
State | Published - Jul 12 2016 |
Bibliographical note
KAUST Repository Item: Exported on 2020-10-01Acknowledgements: A. M. acknowledges the inspiring discussions with
T. Valet and H. B. M. S. thanks S. Feki and B. Hadri for
their valuable technical support. This work was supported
by the King Abdullah University of Science and
Technology (KAUST).