Fig. 6: The weak density dependence at high temperature and strong density dependence at a low temperature of the resistivity close to charge neutrality seen in experiment42 is well captured within the Dirac theory of electron–(gauge) phonon scattering40.
From: Carrier transport theory for twisted bilayer graphene in the metallic regime
Experimental data (top squares) for resistivity at θ = 1.24∘ vs density at various temperatures (a) compared to the Dirac theory (bottom solid lines) of electron–phonon scattering (b).
