arXiv Analytics

Sign in

arXiv:1212.1991 [cond-mat.mes-hall]AbstractReferencesReviewsResources

Optical Hall conductivity in bulk and nanostructured graphene beyond the Dirac approximation

Jesper Goor Pedersen, Mikkel H. Brynildsen, Horia D. Cornean, Thomas Garm Pedersen

Published 2012-12-10Version 1

We present a perturbative method for calculating the optical Hall conductivity in a tight-binding framework based on the Kubo formalism. The method involves diagonalization only of the Hamiltonian in absence of the magnetic field, and thus avoids the computational problems usually arising due to the huge magnetic unit cells required to maintain translational invariance in presence of a Peierls phase. A recipe for applying the method to numerical calculations of the magneto-optical response is presented. We apply the formalism to the case of ordinary and gapped graphene in a next-nearest neighbour tight-binding model as well as graphene antidot lattices. In both case, we find unique signatures in the Hall response, that are not captured in continuum (Dirac) approximations. These include a non-zero optical Hall conductivity even when the chemical potential is at the Dirac point energy. Numerical results suggest that this effect should be measurable in experiments.

Comments: 7 pages, 4 figures, accepted in Physical Review B
Journal: Phys. Rev. B 86, 235438 (2012)
Categories: cond-mat.mes-hall
Related articles: Most relevant | Search more
arXiv:1404.6899 [cond-mat.mes-hall] (Published 2014-04-28, updated 2014-04-29)
Electronic and optical properties of graphene antidot lattices: Comparison of Dirac and tight-binding models
arXiv:0901.0840 [cond-mat.mes-hall] (Published 2009-01-07, updated 2009-09-16)
Weak Localization and Transport Gap in Graphene Antidot Lattices
arXiv:0903.0918 [cond-mat.mes-hall] (Published 2009-03-05, updated 2009-07-16)
Character of electronic states in graphene antidot lattices: Flat bands and spatial localization