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note
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Coherences in the distribution function are the off-diagonal elements of statistical density matrix; here, we are interested in those induced by currents across noncollinear magnetic structures at the Fermi surface.
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19
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A realistic evaluation of the transmission coefficient, Eq. (14), is being undertaken by using spin-polarized single-electron states for a Cu/Co interface; I. Mertig (private communication).
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Mertig, I.1
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In the situation envisaged in Figs. 3(c) and 3(d) of M. D. Stiles and A. Zangwill, J. Appl. Phys. 91, 6812 (2002), we see that the transverse components of the spin fluxes are annihilated on opposite sides of the normal spacer layer between two noncollinear magnetic layers.
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