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note
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As proposed by Tatara and Kohno (Ref.), there are other possible contributions to the current-driving force, which is proportional to the DW resistance RDW, Fj =en RDW I Ly Lz, where n a-3 is the electron density (a is the lattice constant), and I= ja Ly Lz is the current. It easy to verify that, if both contributions are taken into account, the current-driving force can be expressed as Fj =-2 μ0 Ms Ly Lz cJ′ / (γ0 Δ), where cJ′ μB (ξP+ R) / (e Ms) and R =Δ e2 n RDW Ly Lz is the dimensionless DW resistivity. This additional term (proportional to R) will be omitted unless the contrary is said.
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