2017
DOI: 10.1088/1361-648x/aa7735
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The influence of anisotropic Rashba spin–orbit coupling on current-induced spin polarization in graphene

Abstract: Abstract. We consider a disordered graphene layer with anisotropic Rashba spin-orbit coupling subjected to a longitudinal electric field. Using the linear response theory we calculate current-induced spin polarization including in-plane normal and parallel components with respect to the electric field direction. Unlike the case of isotropic Rashba spin-orbit where the normal component of spin polarization is linear in terms of Fermi energy around the Dirac point, anisotropic Rashba spin-orbit can result in non… Show more

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Cited by 5 publications
(5 citation statements)
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References 86 publications
(147 reference statements)
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“…The breaking of both mirror and hexagonal symmetries can lead to the anisotropic Rashba SOC, effects of which on the energy spectrum of the two-dimensional electron gas [53], metallic surface states [54] or electrons in graphene sheet [55] have been investigated. The spin polarization can be influenced by the anisotropic Rashba SOC and there is a Lifshitz transition.…”
Section: Discussionmentioning
confidence: 99%
“…The breaking of both mirror and hexagonal symmetries can lead to the anisotropic Rashba SOC, effects of which on the energy spectrum of the two-dimensional electron gas [53], metallic surface states [54] or electrons in graphene sheet [55] have been investigated. The spin polarization can be influenced by the anisotropic Rashba SOC and there is a Lifshitz transition.…”
Section: Discussionmentioning
confidence: 99%
“…The breaking of both mirror and hexagonal symmetries can lead to the anisotropic Rashba SOC, effects of which on the energy spectrum of the two-dimensional electron gas 54 , metallic surface states 55 or electrons in graphene sheet 56 have been investigated. The spin po-larization can be influenced by the anisotropic Rashba SOC and there is a Lifshitz transition.…”
Section: Discussionmentioning
confidence: 99%
“…where k c = π/a is the wave vector cutoff, sgn(x) is the Sign function, and γ b = n i u 2 0 / 4v 2 F is the impurity parameter. In the gap region, |µ| < ∆, due to the absence of states, the self-energies take exponentially small values [34,35]. Generally, the self-energies (19) can be written as…”
Section: Pointlike Impuritiesmentioning
confidence: 99%