2013
DOI: 10.1103/physrevb.88.125431
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Electron delocalization in gate-tunable gapless silicene

Abstract: The application of a perpendicular electric field can drive silicene into a gapless state, characterized by two nearly fully spin-polarized Dirac cones owing to both relatively large spin-orbital interactions and inversion symmetry breaking. Here we argue that since inter-valley scattering from non-magnetic impurities is highly suppressed by time reversal symmetry, the physics should be effectively single-Dirac-cone like. Through numerical calculations, we demonstrate that there is no significant backscatterin… Show more

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Cited by 15 publications
(10 citation statements)
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“…[40] However, in the calculations, the intervalley scattering can be neglected because of a slight impact on the transport properties in our considered system. [41,42] We find that the tunneling transmission is asymmetric with respect to the in-plane momentum k y for P configuration but symmetric about k y for AP configuration. The interplay of massive electrons with spin-orbit coupling in silicene results in a spin-valley dependent gap.…”
Section: Introductionmentioning
confidence: 74%
“…[40] However, in the calculations, the intervalley scattering can be neglected because of a slight impact on the transport properties in our considered system. [41,42] We find that the tunneling transmission is asymmetric with respect to the in-plane momentum k y for P configuration but symmetric about k y for AP configuration. The interplay of massive electrons with spin-orbit coupling in silicene results in a spin-valley dependent gap.…”
Section: Introductionmentioning
confidence: 74%
“…After that, σ int xy grows remarkably to a considerable but non-quantized value ∼ 0.35 e 2 h at W ∼ 10, before the localization (σ int xy ∼ 0) at strong disorder W = 15. Such an emergence of nonzero σ int xy under increasing disorder is not rare in systems without particle-hole symmetry, and can be attributed to disorder induced band inversion [30,31,36,56]. The nonquantization of σ int xy suggests that the system is in the metallic state, similar to that before the appearance of topological Anderson insulator [31,35,36].…”
Section: Topologically Trivial Phasementioning
confidence: 94%
“…Such an emergence of nonzero σ int xy under increasing disorder is not rare in systems without particle-hole symmetry, and can be attributed to disorder induced band inversion [30,31,36,56]. The nonquantization of σ int xy suggests that the system is in the metallic state, similar to that before the appearance of topological Anderson insulator [31,35,36]. However, since a stable energy gap or mobility gap cannot be formed before another disorder induced band inversion into a trivial Anderson insulator at strong disorder [29][30][31], this system cannot develop into a topological Anderson insulator with a quantized topological invariant (Chern number here).…”
Section: Topologically Trivial Phasementioning
confidence: 99%
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“…It is clear that the numerical calculations should be supported by a simple but adequate model presenting the exact analytic solutions. The theory of the modification of the spectrum of graphene caused by an increase in the concentration of point impurities was developed in works [5][6][7], where the possibility of the metal-dielectric transition was predicted, and the dominant role of a quasigap filled by localized states in the scattering by pairs and triples of impurity centers was indicated.…”
Section: Introductionmentioning
confidence: 99%