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Volumn 64, Issue 12, 2001, Pages

Rashba Hamiltonian and electron transport

Author keywords

[No Author keywords available]

Indexed keywords

ACCELERATION; ARTICLE; ELECTRIC CONDUCTIVITY; ELECTRON TRANSPORT; MAGNETISM; SEMICONDUCTOR;

EID: 0035883686     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.64.121202     Document Type: Article
Times cited : (209)

References (13)
  • 2
    • 0000696553 scopus 로고
    • Fiz. Tverd. Tela (S.-Peterburg), 1224 (1960)
    • E I. Rashba, Fiz. Tverd. Tela (S.-Peterburg) 2, 1224 (1960) [Sov. Phys. Solid State2, 1109 (1960)];
    • (1960) Sov. Phys. Solid State , vol.2 , pp. 1109
    • Rashba, E.I.1
  • 3
    • 0002902816 scopus 로고
    • Pis’ma Zh. Éksp. Teor. Fiz., 66 (1984)
    • Yu. A. Bychkov and E.I Rashba, Pis’ma Zh. Éksp. Teor. Fiz. 39, 66 (1984) [JETP Lett.39, 78 (1984)].
    • (1984) JETP Lett. , vol.39 , pp. 78
    • Yu, A.1
  • 5
    • 85038288813 scopus 로고    scopus 로고
    • This argument holds also in the presence of stray fields from the ferromagnet which rotate invariantly with the magnetization
    • This argument holds also in the presence of stray fields from the ferromagnet which rotate invariantly with the magnetization.
  • 7
    • 0034905910 scopus 로고    scopus 로고
    • There is some uncertainty as to whether the experimental data on (formula presented) might suffer from an interfering effect; see, e.g., and, (R)
    • There is some uncertainty as to whether the experimental data on (formula presented) might suffer from an interfering effect; see, e.g., A C H. Rowe, J. Nehls, R A. Stradling, and R S. Ferguson, Phys. Rev. B63, 201307(R) (2001).
    • (2001) Phys. Rev. B , vol.63 , pp. 201307
    • Rowe, A.C.H.1    Nehls, J.2    Stradling, R.A.3    Ferguson, R.S.4
  • 8
    • 85038293501 scopus 로고    scopus 로고
    • Note that even in the limit of (formula presented) the eigenstates (3) are linear combinations of spin-up and spin-down states. Pure spin eigenstates could be obtained in this limit by including a Zeeman spin splitting Δ in the Hamiltonian which in the end is allowed to vanish
    • Note that even in the limit of (formula presented) the eigenstates (3) are linear combinations of spin-up and spin-down states. Pure spin eigenstates could be obtained in this limit by including a Zeeman spin splitting Δ in the Hamiltonian which in the end is allowed to vanish.


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