2014
DOI: 10.4236/jmp.2014.510100
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Quantum Field Theory of Graphene with Dynamical Partial Symmetry Breaking

Abstract: The quantum field theory approach has been proposed for the description of graphene electronic properties. It generalizes massless Dirac fermion model and is based on the Dirac-Hartree-Fock self-consistent field approximation and assumption on antiferromagnetic ordering of graphene lattice. The developed approach allows asymmetric charged carriers in single layer graphene with partially degenerated Dirac cones.

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Cited by 6 publications
(9 citation statements)
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“…Let us consider the screening in true two-dimensional (2D) semimetals. As known, [15][16][17] free charge carriers at the Fermi level in these materials are absent.…”
Section: Screening Depending On Charge State Of Mixed-valence Complexesmentioning
confidence: 99%
“…Let us consider the screening in true two-dimensional (2D) semimetals. As known, [15][16][17] free charge carriers at the Fermi level in these materials are absent.…”
Section: Screening Depending On Charge State Of Mixed-valence Complexesmentioning
confidence: 99%
“…Let a wavevector k m1, m2 , satisfying either the quantization conditions (II.3) or (II.4), be associated with the reduced wavevector q m1,m2 as the difference between k m1,m2 and the nearest Dirac point (valley) K(K ) of Brillouin zone. The Hamiltonian ĤD is obtained within the quasirelativistic Dirac-Hartree-Fock selfconsistent field approach (see [26,27]). It is a highenergy k • p-Hamiltonian in a q 4 approximation for the quasirelativistic quantum exchange that the latter is series expanded in the vicinity of the Dirac point K( K ) on the absolute value of the difference q = p − K of the quasiparticle momentum p and K( K ) up to the terms of O(q 4 ) inclusively.…”
Section: A "Folding Zone" Approximationmentioning
confidence: 99%
“…Then, the emergence of unfolding leads to replica appearance, and further splitting of these replicas gives the octagonal symmetry of the problem, as one can see in Figure 3. Hyperbolic points (saddle points) are located between nodes and at the apex of the Dirac cone (Van-Hove singularities) as one can see in Figure 2a,b [3,[48][49][50]. Therefore, a fractal-like set of Fermi arcs which are shown in Figure 4, is formed in the absence of damping in the system.…”
Section: Harmonic Analysis Of the Problemmentioning
confidence: 99%
“…In Section 2, we propose a semimetal model with coupling between pseudospin and valley currents and prove the pseudo-helicity conservation law. In Section 3, we briefly introduce the approach [3,[35][36][37] and use it in a simple tight-binding approximation to obtain the system of equations for a Majorana secondary quantized field. In Section 4, we support the statement that the squared equation for the constructed field is of the Klein-Gordon-Fock type for different model exchange operators.…”
Section: Introductionmentioning
confidence: 99%
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