Volume 98, Number 2, April 2012
|Number of page(s)||5|
|Section||Condensed Matter: Electronic Structure, Electrical, Magnetic and Optical Properties|
|Published online||27 April 2012|
Short-range Coulomb correlations render massive Dirac fermions massless
Department of Science, Tarbiat Modares University - Tehran, Iran
2 Department of Physics, Sharif University of Technology - Tehran 11155-9161, Iran
3 School of Physics, Institute for Research in Fundamental Sciences (IPM) - Tehran 19395-5531, Iran
Accepted: 27 March 2012
Tight-binding electrons on a honeycomb lattice are described by an effective Dirac theory at low energies. Lowering symmetry by an alternate ionic potential (Δ) 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 (U) on massive Dirac fermions. For a fixed mass parameter Δ, we find that beyond a critical value Uc1(Δ) massive Dirac fermions become massless. Further increasing U beyond Uc2(Δ), there will be another phase transition to the Mott insulating state. Therefore, the competition between the single-particle gap parameter, Δ, and the Hubbard U 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 Δ, there is a wide interval of U values for which the system remains semi-metal. The implication of this result for graphene is that in contrast to a single-particle picture, the on-site Coulomb repulsion makes the Dirac cone spectrum robust against small values of the symmetry breaking parameter Δ.
PACS: 73.22.Pr – Electronic structure of graphene / 71.30.+h – Metal-insulator transitions and other electronic transitions
© EPLA, 2012
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