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Volumn 139, Issue 1, 2006, Pages 31-34

Theory of spin transfer phenomena in magnetic metals and semiconductors

Author keywords

A. Magnetic metals; D. Non equilibrium; D. Spin transport

Indexed keywords

CHARGE TRANSFER; ELECTRONS; FERROMAGNETIC MATERIALS; MAGNETIC PROPERTIES; MAGNETIZATION;

EID: 33745236829     PISSN: 00381098     EISSN: None     Source Type: Journal    
DOI: 10.1016/j.ssc.2006.05.004     Document Type: Article
Times cited : (35)

References (53)
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  • 33
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    • Scattering formulations of transport in ferromagnetic systems will in general require the consistent evaluation of scalar and spin exchange fields using an approach similar to that developed by
    • Scattering formulations of transport in ferromagnetic systems will in general require the consistent evaluation of scalar and spin exchange fields using an approach similar to that developed by. Taylor J., Guo H., and Wang J. Phys. Rev. B 63 (2001) 245407
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    • For examples of successful applications of scattering formulations to investigate ferromagnetic transport effects see:
    • For examples of successful applications of scattering formulations to investigate ferromagnetic transport effects see:. Bauer G.E.W., et al. J. Appl. Phys. 75 (1994) 6704
    • (1994) J. Appl. Phys. , vol.75 , pp. 6704
    • Bauer, G.E.W.1
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    • The association between magnetization dynamics and spatial structure and spin-currents has been discussed previously in a number of contexts. See, for example
    • The association between magnetization dynamics and spatial structure and spin-currents has been discussed previously in a number of contexts. See, for example,. Tserkovnyak Y., Brataas A., and Bauer G.E.W. Phys. Rev. Lett. 88 (2002) 117601
    • (2002) Phys. Rev. Lett. , vol.88 , pp. 117601
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    • See for example, Interscience Publishers, New York
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    • note
    • The transport orbitals will also, in general, contribute to the total spin-density component in the direction of the magnetization. This effect alters the exchange field along the magnetization direction and does not produce a spin torque.
  • 48
  • 53
    • 33745286325 scopus 로고    scopus 로고
    • note
    • S O = ({ λ, over(p, →) } × over(z, ̂)) · over(s, →), where the symbol {·,·} denotes the operator anticonmutator.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.