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3
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0033576696
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R. Fiederling, M. Keim, G. Reusher, W. Ossau, G. Schmidt, A. Waag, and L. Molemkamp, Nature (London)402, 787 (1999).
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(1999)
Nature (London)
, vol.402
, pp. 787
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Fiederling, R.1
Keim, M.2
Reusher, G.3
Ossau, W.4
Schmidt, G.5
Waag, A.6
Molemkamp, L.7
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4
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0033576573
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Y. Ohno, D K. Young, B. Beschoten, F. Matsukura, H. Ohno, and D D. Awschalom, Nature (London)402, 790 (1999).
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(1999)
Nature (London)
, vol.402
, pp. 790
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Ohno, Y.1
Young, D.K.2
Beschoten, B.3
Matsukura, F.4
Ohno, H.5
Awschalom, D.D.6
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5
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0009906761
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G. Schmidt, D. Ferrand, L W. Molemkamp, A T. Filip, and B J. Van Wees, Phys. Rev. B62, 4790 (2000).
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(2000)
Phys. Rev. B
, vol.62
, pp. 4790
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Schmidt, G.1
Ferrand, D.2
Molemkamp, L.W.3
Filip, A.T.4
Van Wees, B.J.5
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12
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68949093158
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A. Barthelemy, A. Fert, and F. Petroff, edited by K.H.J. Buschow (Elsevier Science, Amsterdam, 1999), 12
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A. Barthelemy, A. Fert, and F. Petroff, Handbook of Magnetic Materials, edited by K.H.J. Buschow (Elsevier Science, Amsterdam, 1999), Vol. 12.
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20
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85038955232
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The resistivity and spin diffusion length (SDL) data we refer to in Sec. II to estimate (formula presented) and (formula presented) have been obtained at low temperature (LT) where most CPP-GMR experiments have been performed. Some CPP-GMR measurements have also been performed as a function of temperature on multilayered nanowires. The resistivity increases and the SDL decreases as a function of T, so that their product, changes only weakly, by 11% between LT and RT in Co for example (Ref. This is also consistent with Eq. (14) and the Yafet mechanism of spin relaxation in which (formula presented) is temperature independent. The weak temperature dependence of (formula presented) (or (formula presented) justifies the use of LT data at any temperature
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The resistivity and spin diffusion length (SDL) data we refer to in Sec. II to estimate (formula presented) and (formula presented) have been obtained at low temperature (LT) where most CPP-GMR experiments have been performed. Some CPP-GMR measurements have also been performed as a function of temperature on multilayered nanowires. The resistivity increases and the SDL decreases as a function of T, so that their product r changes only weakly, by 11% between LT and RT in Co for example (Ref. 20). This is also consistent with Eq. (14) and the Yafet mechanism of spin relaxation in which (formula presented) is temperature independent. The weak temperature dependence of (formula presented) (or (formula presented) justifies the use of LT data at any temperature.
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21
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0347334707
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L. Piraux, S. Dubois, A. Fert, and L. Belliard, Eur. Phys. J. B4, 413 (1998).
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(1998)
Eur. Phys. J. B
, vol.4
, pp. 413
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Piraux, L.1
Dubois, S.2
Fert, A.3
Belliard, L.4
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24
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85038939035
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Schmidt, in Ref., find that, for a given metal resistivity, a value of the spin asymmetry coefficient (formula presented) very close to 1 (case of an ideal half-metallic ferromagnet) can restore a significant SP of the current injected into the SC. This is also shown by our Eq. (20) if one reminds that (formula presented) is proportional to (formula presented), that is to the resistivity of the bulk metal divided by (formula presented)
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Schmidt et al. in Ref. 5 find that, for a given metal resistivity, a value of the spin asymmetry coefficient (formula presented) very close to 1 (case of an ideal half-metallic ferromagnet) can restore a significant SP of the current injected into the SC. This is also shown by our Eq. (20) if one reminds that (formula presented) is proportional to (formula presented), that is to the resistivity of the bulk metal divided by (formula presented).
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