2010
DOI: 10.1103/physrevb.82.245416
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Thermoelectric transport of massive Dirac fermions in bilayer graphene

Abstract: Thermoelectric power ͑TEP͒ is measured in bilayer graphene for various temperatures and charge-carrier densities. At low temperatures, measured TEP well follows the semiclassical Mott formula with a hyperbolic dispersion relation. TEP for a high carrier density shows a linear temperature dependence, which demonstrates a weak electron-phonon interaction in the bilayer graphene. For a low carrier density, a deviation from the Mott relation is observed at high temperatures and is attributed to the low Fermi tempe… Show more

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Cited by 76 publications
(77 citation statements)
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References 34 publications
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“…Thermoelectric measurement 11 shows that the roomtemperature thermopower with a bias voltage can be enhanced by a factor of 4 compared to that of monolayer graphene or unbiased bilayer graphene, making it a more promising candidate for future thermoelectric applications. Theoretical calculations from the tight-binding models for monolayer and bilayer graphene 12,13 are in agreement with the experimental observations [1][2][3]11,14 .…”
supporting
confidence: 79%
“…Thermoelectric measurement 11 shows that the roomtemperature thermopower with a bias voltage can be enhanced by a factor of 4 compared to that of monolayer graphene or unbiased bilayer graphene, making it a more promising candidate for future thermoelectric applications. Theoretical calculations from the tight-binding models for monolayer and bilayer graphene 12,13 are in agreement with the experimental observations [1][2][3]11,14 .…”
supporting
confidence: 79%
“…In particular, its high mobility, which due to the weak electron-phonon interaction persists up to room temperature, can be orders of magnitude higher than in other 2D thermoelectric materials, such as semiconducting transition metal dichalcogenides (13)(14)(15)(16). Theoretical and experimental studies show that the Seebeck coefficient in graphene could reach values comparable to that in bulk semiconductors by decreasing the carrier density (17)(18)(19)(20)(21)(22)(23). The combination of graphene's large mobility and competitive Seebeck coefficient result in large power factor and large active cooling.…”
Section: ·Kmentioning
confidence: 99%
“…Graphene (monolayer [38,39] and bilayer [40]) exfoliated on a SiO 2 =Si substrate, for example, provides a significant thermoelectric response and the usual temperature dependence of S can be overcome on a SiC substrate [41]. Performance improvements have been achieved through O plasma treatment [42] and molecular decoration [43].…”
Section: Introductionmentioning
confidence: 99%