2014
DOI: 10.1088/2053-1583/1/3/035002
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Effect of C-face 4H-SiC(0001) deposition on thermopower of single and multilayer graphene in AA, AB and ABC stacking

Abstract: The Seebeck coefficient in multilayer graphene is investigated within the density-functional theory, using the semiclassical Boltzmann equations and interpolating the bands in a maximally-localized Wannier functions basis set. We compare various graphene stackings (AA, AB and ABC) both freestanding and deposited on a 4H-SiC(0001) C-terminated substrate. We find that the presence of the SiC substrate can significantly affect the thermopower properties of graphene layers, depending on the stacking, providing a p… Show more

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Cited by 8 publications
(8 citation statements)
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“…The thermoelectric parameters at the low-energy parts of the F-impurity bands are low, since in that region, the impurity bands touch the valence band manifold. For the spindown channel of the F-doped graphene, we observe the Seebeck-coefficient and the ZT-efficiency extrema similar to these obtaned for the pure graphene close to the band crossing at the Fermi level near the K-point [37]. Less pronounced features of the same shape in the thermopower curve are visible below -1.2 eV for the spin-up…”
Section: A Free-standing Doped Graphene Monolayersupporting
confidence: 67%
See 1 more Smart Citation
“…The thermoelectric parameters at the low-energy parts of the F-impurity bands are low, since in that region, the impurity bands touch the valence band manifold. For the spindown channel of the F-doped graphene, we observe the Seebeck-coefficient and the ZT-efficiency extrema similar to these obtaned for the pure graphene close to the band crossing at the Fermi level near the K-point [37]. Less pronounced features of the same shape in the thermopower curve are visible below -1.2 eV for the spin-up…”
Section: A Free-standing Doped Graphene Monolayersupporting
confidence: 67%
“…4, together with the band structures of H-and F-doped systems. In the case of hydrogen doping, the majority spin-bands close to the K-point are similar to the bands of bilayer graphene in the AB stacking or graphite [32,37] -with the difference that here the parabolic bands touch each other below the Fermi level, and the minority spin-bands open the gap close to the K-point. In the case of fluorine doping, the band gap opens at the K-point in both spin channels.…”
Section: A Free-standing Doped Graphene Monolayermentioning
confidence: 79%
“…The behaviors of the Seebeck coefficients are comparable to the results reported by Wierzbowska et al although the graphs look somewhat different due to different scaling of the x-axis [43]. show Raman modes that are used to identify ABA-and ABC-stacked domains in TLG [28,29,32,34].…”
Section: Theoretical Calculationssupporting
confidence: 81%
“…The thermopower of biased and unbiased multilayer graphene was studied in the Slonczewski-WeisMcClure model, where the effect of impurity scattering was treated in the self-consistent Born approximation 10 . The classic and spin Seebeck effects in single as well as in multilayer graphene on the SiC substrate were also investigated within ab-initio methods, 11,12 and by nonequilibrium molecular-dynamics simulations.…”
Section: Introductionmentioning
confidence: 99%