Abstract

We study the mobility of Dirac fermions in monolayer graphene on a GaAs substrate, limited by the combined action of the extrinsic potential of piezoelectric surface acoustical phonons of GaAs (PA) and of the intrinsic deformation potential of acoustical phonons in graphene (DA). In the high-temperature ($T$) regime, the momentum relaxation rate exhibits the same linear dependence on $T$ but different dependencies on the carrier density $n$, corresponding to the mobility $\ensuremath{\mu}\ensuremath{\propto}1/\sqrt{n}$ and $1/n$, respectively for the PA and DA scattering mechanisms. In the low-$T$ Bloch-Gr\"uneisen regime, the mobility shows the same square-root density dependence $\ensuremath{\mu}\ensuremath{\propto}\sqrt{n}$, but different temperature dependencies $\ensuremath{\mu}\ensuremath{\propto}{T}^{\ensuremath{-}3}$ and ${T}^{\ensuremath{-}4}$, respectively for PA and DA phonon scattering.

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