2016
DOI: 10.1088/0022-3727/49/10/105305
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Spin polarisation using gate voltage through a Rashba barrier in graphene

Abstract: Gate-tunable spin-resolved scattering through a Rashba spin–orbit (SO) coupling graphene barrier is considered theoretically by using a mode-matching method. In this structure, we investigate the dependence of the tunnelling transmission probability on the spin orientation of the incident electron. It is found that the difference of the transmission probability for opposite spin orientations exhibits considerable incident-angle-dependent features when both gate voltage and Rashba SO coupling in the barrier reg… Show more

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Cited by 3 publications
(3 citation statements)
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“…This achievement is in agreement with the result of Ref. [27] in which the transmission probability is larger for lower gate voltages. The mentioned change in the spin orientation by the RSOC is useful in the applications that use a gate voltage for the spin filtration.…”
Section: Resultssupporting
confidence: 93%
See 1 more Smart Citation
“…This achievement is in agreement with the result of Ref. [27] in which the transmission probability is larger for lower gate voltages. The mentioned change in the spin orientation by the RSOC is useful in the applications that use a gate voltage for the spin filtration.…”
Section: Resultssupporting
confidence: 93%
“…It found that the sign of the spin polarization can switch from positive to negative by adjusting the electric potential at any RSOC. [27] There also exist technological applications of the grephene in spintronic devices. The graphene nanostrips can be used as digital memory devices in which the spin-polarized states can be treated as switchable quantum bits through the applied voltage.…”
Section: Introductionmentioning
confidence: 99%
“…In analogy with the differential spin transmission for spintronics [56][57][58][59][60], we define the differential valley transmission P T = (TKK +T KK )−(T K K +T K K ) T that describes the difference of transmission for the K and K states through the scattering region with the total transmission T = T KK + T KK + T K K + T K K . In fig.…”
Section: (A) the Low-energy Effective Hamiltonianmentioning
confidence: 99%