Short range Coulomb correlations render massive Dirac fermions massless
arXiv:1112.3616 · doi:10.1209/0295-5075/98/27009
Abstract
Tight binding electrons on a honeycomb lattice are described by an effective Dirac theory at low energies. Lowering symmetry by an alternate ionic potential () generates a single-particle gap in the spectrum. We employ the dynamical mean field theory (DMFT) technique, to study the effect of on-site electron correlation () on massive Dirac fermions. For a fixed mass parameter , we find that beyond a critical value massive Dirac fermions become massless. Further increasing beyond , there will be another phase transition to the Mott insulating state. Therefore the competition between the single-particle gap parameter, , and the Hubbard restores the semi-metallic nature of the parent Hamiltonian. The width of the intermediate semi-metallic regime shrinks by increasing the ionic potential. However, at small values of , there is a wide interval of values for which the system remains semi-metal.
4 pages, 5 figures
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