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1
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2942610744
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Spintronics: Fundamentals and applications
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DOI 10.1103/RevModPhys.76.323
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I. Zutic, J. Fabian, and S. Das Sarma, Rev. Mod. Phys. 76, 323 (2004). 10.1103/RevModPhys.76.323 (Pubitemid 39063520)
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(2004)
Reviews of Modern Physics
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, pp. 323-410
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Zutic, I.1
Fabian, J.2
Sarma, S.D.3
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4
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16344394810
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First-principles study of magnetization relaxation enhancement and spin transfer in thin magnetic films
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DOI 10.1103/PhysRevB.71.064420, 064420
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M. Zwierzycki, Y. Tserkovnyak, P. J. Kelly, A. Brataas, and G. E. W. Bauer, Phys. Rev. B 71, 064420 (2005). 10.1103/PhysRevB.71.064420 (Pubitemid 40467477)
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(2005)
Physical Review B - Condensed Matter and Materials Physics
, vol.71
, Issue.6
, pp. 0644201-06442011
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Zwierzycki, M.1
Tserkovnyak, Y.2
Kelly, P.J.3
Brataas, A.4
Bauer, G.E.W.5
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5
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77954904777
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10.1103/PhysRevB.81.094409
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B. Kardaz and B. Heinrich, Phys. Rev. B 81, 094409 (2010). 10.1103/PhysRevB.81.094409
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(2010)
Phys. Rev. B
, vol.81
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Kardaz, B.1
Heinrich, B.2
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10.1063/1.3551729
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A. Ghosh, J. F. Sierra, S. Auffret, U. Ebels, and W. E. Bailey, Appl. Phys. Lett. 98, 052508 (2011). 10.1063/1.3551729
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(2011)
Appl. Phys. Lett.
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Ghosh, A.1
Sierra, J.F.2
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Ebels, U.4
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J. Z. Sun, Phys. Rev. B 62, 570 (2000). 10.1103/PhysRevB.62.570
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Sun, J.Z.1
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10.1103/PhysRevB.78.014413
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K. Ando, Y. Kajiwara, S. Takahashi, S. Maekawa, K. Takemoto, M. Takatsu, and E. Saitoh, Phys. Rev. B 78, 014413 (2008). 10.1103/PhysRevB.78.014413
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(2008)
Phys. Rev. B
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Ando, K.1
Kajiwara, Y.2
Takahashi, S.3
Maekawa, S.4
Takemoto, K.5
Takatsu, M.6
Saitoh, E.7
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10.1103/PhysRevB.76.104409
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K. Carva and I. Turek, Phys. Rev. B 76, 104409 (2007). 10.1103/PhysRevB.76.104409
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Phys. Rev. B
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Carva, K.1
Turek, I.2
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10
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80555137201
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The general form of the SMC contains G r and G t , where G t = S - 1 mn t mn t mn and t mn () is the transmission matrix for u(down) electrons. However, in metallic junctions, G t sharply decreases to zero with the thickness of magnetic layers, and thus, G t can be safely neglected for thicker junctions.
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The general form of the SMC contains G r and G t, where G t = S-1 mn t mn t mn and t mn () is the transmission matrix for up (down) electrons. However, in metallic junctions, G t sharply decreases to zero with the thickness of magnetic layers, and thus, G t can be safely neglected for thicker junctions.
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12
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80555137202
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We set eight layers of Pt and Py in the S to ensure that the electronic structures away from the interface are similar to those for the bulk.
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We set eight layers of Pt and Py in the S to ensure that the electronic structures away from the interface are similar to those for the bulk.
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13
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0003499960
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(Kluwer, Boston).
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I. Turek, V. Drchal, J. Kudrnovsk, M. ob, P. Weinberger, Electronic Structure of Disordered Alloys, Surfaces and Interfaces (Kluwer, Boston, 1997).
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(1997)
Electronic Structure of Disordered Alloys, Surfaces and Interfaces
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Turek, I.1
Drchal, V.2
Kudrnovsk, J.3
Ob, M.4
Weinberger, P.5
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14
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5444237332
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10.1088/0022-3719/5/13/012
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U. von Barth and L. Hedin, J. Phys. C 5, 1629 (1972). 10.1088/0022-3719/5/13/012
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(1972)
J. Phys. C
, vol.5
, pp. 1629
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Von Barth, U.1
Hedin, L.2
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15
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79959922970
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10.1088/0953-8984/23/25/254210
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B. Glaubitz, S. Buschhorn, F. Brssing, R. Abrudan, and H. Zabel, J. Phys.: Condens. Matter 23, 254210 (2011). 10.1088/0953-8984/23/25/254210
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(2011)
J. Phys.: Condens. Matter
, vol.23
, pp. 254210
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Glaubitz, B.1
Buschhorn, S.2
Brssing, F.3
Abrudan, R.4
Zabel, H.5
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16
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80555142199
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We have checked the effect of the lattice constant mismatch for Pt and Py by using the lateral supercell sizes of Pt (9 9) and Py (10 10), and found that the real part of SMC generally decreases at most about 10. However, the main conclusions in this paper are unaffected.
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We have checked the effect of the lattice constant mismatch for Pt and Py by using the lateral supercell sizes of Pt (9 9) and Py (10 10), and found that the real part of SMC generally decreases at most about 10. However, the main conclusions in this paper are unaffected.
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17
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0035109245
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10.1103/PhysRevB.63.064407
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K. Xia, P. J. Kelly, G. E. W. Bauer, I. Turek, J. Kudrnovsky, and V. Drchal, Phys. Rev. B 63, 064407 (2001); 10.1103/PhysRevB.63.064407
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(2001)
Phys. Rev. B
, vol.63
, pp. 064407
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Xia, K.1
Kelly, P.J.2
Bauer, G.E.W.3
Turek, I.4
Kudrnovsky, J.5
Drchal, V.6
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18
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33244493966
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First-principles scattering matrices for spin transport
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DOI 10.1103/PhysRevB.73.064420, 064420
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K. Xia, M. Zwierzycki, M. Talanana, P. J. Kelly, and G. E. W. Bauer, Phys. Rev. B 73, 064420 (2006). 10.1103/PhysRevB.73.064420 (Pubitemid 43279546)
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(2006)
Physical Review B - Condensed Matter and Materials Physics
, vol.73
, Issue.6
, pp. 1-21
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Xia, K.1
Zwierzycki, M.2
Talanana, M.3
Kelly, P.J.4
Bauer, G.E.W.5
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19
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34547793139
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Thermal spin-transfer torque in magnetoelectronic devices
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DOI 10.1103/PhysRevLett.99.066603
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M. Hatami, G. E. W. Bauer, Q. Zhang, and P. J. Kelly, Phys. Rev. Lett. 99, 066603 (2007); 10.1103/PhysRevLett.99.066603 (Pubitemid 47230764)
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(2007)
Physical Review Letters
, vol.99
, Issue.6
, pp. 066603
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Hatami, M.1
Bauer, G.E.W.2
Zhang, Q.3
Kelly, P.J.4
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20
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67449089711
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10.1103/PhysRevB.79.174426
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M. Hatami, G. E. W. Bauer, Q. Zhang, and P. J. Kelly, Phys. Rev. B 79, 174426 (2009). 10.1103/PhysRevB.79.174426
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(2009)
Phys. Rev. B
, vol.79
, pp. 174426
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Hatami, M.1
Bauer, G.E.W.2
Zhang, Q.3
Kelly, P.J.4
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21
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80555137203
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We have checked the lateral supercell size (N) dependence on the SMC uto N 14 14, and found that the SMC is already converged for N 6 6. Therefore, we have adopted N 6 6 for calculations of the SMC presented here.
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We have checked the lateral supercell size (N) dependence on the SMC up to N 14 14, and found that the SMC is already converged for N 6 6. Therefore, we have adopted N 6 6 for calculations of the SMC presented here.
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22
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80555135127
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A vacuum barrier is adopted as an insulating buffer layer where we use empty spheres to populate the vaccum sites.
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A vacuum barrier is adopted as an insulating buffer layer where we use empty spheres to populate the vaccum sites.
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