Minimal conductivity in graphene: interaction corrections and ultraviolet anomaly
arXiv:0709.4245 · doi:10.1209/0295-5075/83/17005
Abstract
Conductivity of a disorder-free intrinsic graphene is studied to the first order in the long-range Coulomb interaction and is found to be σ=σ_0(1+0.01 g), where 'g' is the dimensionless ("fine structure") coupling constant. The calculations are performed using three different methods: i) electron polarization function, ii) Kubo formula for the conductivity, iii) quantum transport equation. Surprisingly, these methods yield different results unless a proper ultraviolet cut-off procedure is implemented, which requires that the interaction potential in the effective Dirac Hamiltonian is cut-off at small distances (large momenta).
5 pages, 1 figure; Reply to the Comment by I.F. Herbut, V. Juricic, O. Vafek, and M.J. Case, "Comment on "Minimal conductivity in graphene: Interaction corrections and ultraviolet anomaly" by Mishchenko E. G.", arXiv:0809.0725, is added in Appendix
References in corpus (6)
- Electric Field Effect in Atomically Thin Carbon Films
- Unconventional Integer Quantum Hall effect in graphene
- Coulomb interaction, ripples, and the minimal conductivity of graphene
- Effect of electron-electron interactions on the conductivity of clean graphene
- Landauer conductance and twisted boundary conditions for Dirac fermions in two space dimensions
- Notes on the minimal longitudinal dc conductivity of perfect bilayer graphene