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Conductivity of interacting massless Dirac particles in graphene: Collisionless regime

Vladimir Juričić, Oskar Vafek, and Igor F. Herbut
Phys. Rev. B 82, 235402 – Published 1 December 2010

Abstract

We provide detailed calculation of the ac conductivity in the case of 1/r Coulomb interacting massless Dirac particles in graphene in the collisionless limit when ωT. The analysis of the electron self-energy, current vertex function, and polarization function, which enter into the calculation of physical quantities including the ac conductivity, is carried out by checking the Ward-Takahashi identities associated with the electrical charge conservation and making sure that they are satisfied at each step. We adopt a variant of the dimensional regularization of Veltman and ’t Hooft by taking the spatial dimension D=2ϵ for ϵ>0. The procedure adopted here yields a result for the conductivity correction which, while explicitly preserving charge conservation laws, is nevertheless different from the results reported previously in literature.

  • Received 16 September 2010

DOI:https://doi.org/10.1103/PhysRevB.82.235402

©2010 American Physical Society

Authors & Affiliations

Vladimir Juričić1,2, Oskar Vafek3, and Igor F. Herbut4

  • 1Instituut-Lorentz for Theoretical Physics, Universiteit Leiden, P.O. Box 9506, 2300 RA Leiden, The Netherlands
  • 2Max-Planck-Institute for Solid State Research, Heisenbergstr. 1, D-70569 Stuttgart, Germany
  • 3National High Magnetic Field Laboratory and Department of Physics, Florida State University, Tallahasse, Florida 32306, USA
  • 4Department of Physics, Simon Fraser University, Burnaby, British Columbia, Canada V5A 1S6

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Issue

Vol. 82, Iss. 23 — 15 December 2010

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