Abstract
Abstract
The in-plane phonon-drag thermopower S
g, diffusion thermopower S
d and the power factor PF are theoretically investigated in a twisted bilayer graphene (tBLG) as a function of twist angle θ, temperature T and electron density n
s in the region of low T (1–20 K). As θ approaches magic angle θ
m, the S
g and S
d are found to be strongly enhanced, which is manifestation of great suppression of effective Fermi velocity v
F
* of electrons in moiré flat band near θ
m. This enhancement decreases with increasing θ and T. In the Bloch–Grüneisen (BG) regime, it is found that S
g ∼ v
F
*−2, T
3 and n
s
−1/2. As T increases, the exponent δ in S
g ∼ T
δ
, changes from 3 to nearly zero and a maximum S
g value of ∼10 mV K−1 at ∼20 K is estimated. S
g is found to be larger (smaller) for smaller n
s in low (high) temperature region. On the other hand, S
d, taken to be governed by Mott formula with S
d ∼ v
F
*−1, T and n
s
−1/2 and S
d ≪ S
g for T > ∼2 K. The power factor PF is also shown to be strongly θ dependent and is very much enhanced. Consequently, possibility of a giant figure of merit is discussed. In tBLG, θ acts as a strong tuning parameter of both S
g and S
d and PF in addition to T and n
s. Our results are qualitatively compared with the measured out-of-plane thermopower in tBLG.
Subject
Condensed Matter Physics,General Materials Science
Cited by
7 articles.
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