Asymmetry gap in the electronic band structure of bilayer graphene
arXiv:cond-mat/0608221 · doi:10.1103/PhysRevB.74.161403
Abstract
A tight binding model is used to calculate the band structure of bilayer graphene in the presence of a potential difference between the layers that opens a gap $Î$ between the conduction and valence bands. In particular, a self consistent Hartree approximation is used to describe imperfect screening of an external gate, employed primarily to control the density $n$ of electrons on the bilayer, resulting in a potential difference between the layers and a density dependent gap $Î(n)$. We discuss the influence of a finite asymmetry gap $Î(0)$ at zero excess density, caused by the screening of an additional transverse electric field, on observations of the quantum Hall effect.
4 pages, 3 eps figures