Strain dependent conductivity in biased bilayer graphene
arXiv:1404.1655 · doi:10.1103/PhysRevB.90.235403
Abstract
Intrinsic bilayer graphene is a gapless semimetal. Under the application of a bias field it becomes a semiconductor with a direct band gap that is proportional to the applied field. Under a layer-asymmetric strain (where the upper layer undergoes compression and lower layer tension or visa-versa) we find that the band gap of a biased bilayer graphene ribbon becomes indirect and, for higher strains, becomes negative returning the material its original semimetal state. As a result, the conductivity of the ribbon increases and can be almost an order of magnitude larger that of the intrinsic unbiased material - a change that can be induced with a strain of only ~2-3%. The conductivity is proportional to the applied strain and the magnitude of the effect is tunable with the bias field. Such layer-asymmetric strains can be achieved by bending, with forces on the order of ~1nN resulting in a layer-asymmetric strain of ~1%. This new electromechanical effect has a wide potential for application in the areas of nano-force microscopy and pressure sensing on the atomic scale.
Updated to journal version with new title and revised figures. 8 pages, 6 figures
References in corpus (10)
- Electric Field Effect in Atomically Thin Carbon Films
- The electronic properties of graphene
- Energy Band Gap Engineering of Graphene Nanoribbons
- Uniaxial Strain in Graphene by Raman Spectroscopy: G peak splitting, Gruneisen Parameters and Sample Orientation
- A tight-binding approach to uniaxial strain in graphene
- The electronic properties of bilayer graphene
- Strained bilayer graphene: Band structure topology and Landau level spectrum
- Electron pumping in graphene mechanical resonators
- Multilayer graphene under vertical electric field
- Large displacement strain theory and its application to graphene