Electronic structure of turbostratic graphene

S. Shallcross; S. Sharma; E. Kandelaki; O. A. Pankratov

doi:10.1103/PhysRevB.81.165105

paper

Electronic structure of turbostratic graphene

arXiv:0910.5811 · doi:10.1103/PhysRevB.81.165105

Abstract

We explore the rotational degree of freedom between graphene layers via the simple prototype of the graphene twist bilayer, i.e., two layers rotated by some angle $θ$ . It is shown that, due to the weak interaction between graphene layers, many features of this system can be understood by interference conditions between the quantum states of the two layers, mathematically expressed as Diophantine problems. Based on this general analysis we demonstrate that while the Dirac cones from each layer are always effectively degenerate, the Fermi velocity $v_{F}$ of the Dirac cones decreases as $θ \to 0^{\circ}$ ; the form we derive for $v_{F} (θ)$ agrees with that found via a continuum approximation in Phys. Rev. Lett., 99:256802, 2007. From tight binding calculations for structures with $1.4 7^{\circ} \leq θ < 3 0^{\circ}$ we find agreement with this formula for $θ ≳ 5^{\circ}$ . In contrast, for $θ ≲ 5^{\circ}$ this formula breaks down and the Dirac bands become strongly warped as the limit $θ \to 0$ is approached. For an ideal system of twisted layers the limit as $θ \to 0^{\circ}$ is singular as for $θ > 0$ the Dirac point is fourfold degenerate, while at $θ = 0$ one has the twofold degeneracy of the $A B$ stacked bilayer. Interestingly, in this limit the electronic properties are in an essential way determined \emph{globally}, in contrast to the 'nearsightedness' [W. Kohn. Phys. Rev. Lett., 76:3168, 1996.] of electronic structure generally found in condensed matter.

Article as to be published in Phys. Rev B. Main changes: K-point mapping tables fixed, several changes to presentation.

Electronic structure of turbostratic graphene

Abstract

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