2018
DOI: 10.48550/arxiv.1806.10289
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Josephson effect in silicene-based SNS Josephson junction: Andreev reflection and free energy

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Cited by 7 publications
(10 citation statements)
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“…For the low-energy Dirac-Hamilatonian of silicene in tight-binding model, it reads [3,4,5,6,7] H(t) = v F (ητ x P x (t) + τ y P y (t)) + ηλ SOC τ z σ z + aλ R 2 ητ z (P y σ x − P x σ y )…”
Section: Model Of Silicene In Optical Systemmentioning
confidence: 99%
“…For the low-energy Dirac-Hamilatonian of silicene in tight-binding model, it reads [3,4,5,6,7] H(t) = v F (ητ x P x (t) + τ y P y (t)) + ηλ SOC τ z σ z + aλ R 2 ητ z (P y σ x − P x σ y )…”
Section: Model Of Silicene In Optical Systemmentioning
confidence: 99%
“…While for the two-dimension Dirac system with nonzero Dirac-mass (we here take the monolayer silicene and MoS 2 as example), the β-term (i.e., the pseudospin index-dependent term) is also needed for the Berry curvature and the related anomalous effects [17]. For silicene in low-energy Dirac tight-binding model, the Hamiltonian of silicene reads which reads [17,2,21,22,23,3,4]…”
Section: Modelsmentioning
confidence: 99%
“…We at first intruduce the low-energy Dirac-Hamilatonian of silicene in tight-binding model, which reads [8,1,3,5,7,2]…”
Section: Modelmentioning
confidence: 99%
“…The many-body effect (many-electron effect) is also related to the retarded polarization function as well as the dielectric function, thus in the following computation, we define ω = ω + i0 + for simplicity. The self-energy effect in the many-electron system is generally important for the system with quasi-one-dimension band, like the graphene, silicene, and genmanene in the M − K region [3,4,1,5,6,7,8] or the black phosphorus in the M − Y region [9]. The ignorance of the electron-interaction effect also leads to the ignorance of the self-energy and the related excitonic effect and the Coulomb potential.…”
Section: Introductionmentioning
confidence: 99%