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20044379203
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note
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For clarity, we have removed from the micrograph the shadow replicas, as these are not in electrical contact to the device and do not affect the system.
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24
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20044365053
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note
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F|, because the perpendicular component is rapidly averaged out by the large exchange energy in the ferromagnet.
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25
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0242500318
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For intermetallic scleand contacts, the Sharvin resistance has to be subtracted, see G. E. W Bauer, Y. Tserkovnyak, D. Huertas-Hernando, and A. Brataas, Phys. Rev. B 67, 094421 (2003).
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Bauer, G.E.W.1
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Huertas-Hernando, D.3
Brataas, A.4
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26
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0034261159
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Hernando, D.H.1
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Bauer, G.E.W.4
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2342559756
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G. E. W. Bauer, A. Brataas, Y. Tserkovnyak, B. I. Halperin, M. Zwierzycki, and P. J. Kelly, Phys. Rev. Lett. 92, 126601 (2004).
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Zwierzycki, M.5
Kelly, P.J.6
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29
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20044367274
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note
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2≥PG, see Ref. 11.
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31
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33749406012
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Phys. Rev. Lett. 57, 1761 (1986).
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Phys. Rev. Lett.
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32
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20044362382
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note
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Note that the tunnel barriers of the narrowest electrodes have higher resistance than the other two: this is due to a small misalignment during metal deposition. The resistances of largest electrodes are equal and so are those of the narrowest ones, though.
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33
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20044375359
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In the equivalent configuration (in the sense of the reciprocity theorem, with current and voltage probes interchanged, and magnetizations reversed), a spin accumulation is present, but it is not detected because the voltage electrodes are parallel to each other.
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34
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20044383555
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The interpretation we gave in Ref. 9 of the difference between antiparallel and anomalous signals as caused by the spin current is not correct.
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|