Interactions and phase transitions on graphene's honeycomb lattice
arXiv:cond-mat/0606195 · doi:10.1103/PhysRevLett.97.146401
Abstract
The low-energy theory of interacting electrons on graphene's two-dimensional honeycomb lattice is derived and discussed. In particular, the Hubbard model in the large-N limit is shown to have a semi-metal - antiferromagnetic insulator quantum critical point in the universality class of the Gross-Neveu model. The same equivalence is conjectured to hold in the physical case N=2, and its consequences for various physical quantities are examined. The effects of the long-range Coulomb interaction and of the magnetic field are discussed.
four pages, one figure; few typos corrected, references added
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Cited by in corpus (45)
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- Topological Mott Insulators
- AC conductivity of graphene: from tight-binding model to 2+1-dimensional quantum electrodynamics
- Is graphene in vacuum an insulator?
- Theory of interacting electrons on the honeycomb lattice
- Density waves and Cooper pairing on the honeycomb lattice
- Gauge field induced by ripples in graphene
- Quantum critical point in graphene approached in the limit of infinitely strong Coulomb interaction
- Coulomb interaction, ripples, and the minimal conductivity of graphene
- Inverse magnetic catalysis in dense holographic matter
- Lattice field theory simulations of graphene
- Theory of integer quantum Hall effect in graphene
- Quantum Critical Behaviour in a Graphene-like Model
- BCS-BEC crossover on the two-dimensional honeycomb lattice
- Unconventional superconductivity on honeycomb lattice: the theory of Kekule order parameter
- Supercritical Coulomb center and excitonic instability in graphene
- Coulomb interaction in graphene: Relaxation rates and transport
- SO(3) symmetry between Neel and ferromagnetic order parameters for graphene in a magnetic field
- SU(2) gauge theory of the Hubbard model and application to the honeycomb lattice
- Renormalization group approach to 2D Coulomb interacting Dirac fermions with random gauge potential
- Conductivity of interacting massless Dirac particles in graphene: Collisionless regime
- UV fixed-point structure of the three-dimensional Thirring model
- Dynamics in the quantum Hall effect and the phase diagram of graphene
- Chiral asymmetry of the Fermi surface in dense relativistic matter in a magnetic field
- Edge states, mass and spin gaps, and quantum Hall effect in graphene
- Effect of electron-electron interaction on the Fermi surface topology of doped graphene
- Renormalization group flow of quartic perturbations in graphene: Strong coupling and large-N limits
- Pseudo-magnetic catalysis of the time-reversal symmetry breaking in graphene
- Dynamical Mean Field Study of The Dirac Liquid
- Spin-flip excitations, spin waves, and magneto-excitons in graphene Landau levels at integer filling factors
- Zero-energy states and fragmentation of spin in the easy-plane antiferromagnet on a honeycomb lattice
- Edge states on graphene ribbon in magnetic field: interplay between Dirac and ferromagnetic-like gaps
- Lattice gauge theory model for graphene
- Quantum critical scaling in magnetic field near the Dirac point in graphene
- Toward theory of quantum Hall effect in graphene
- Sensory Organ like Response of Zigzag Edge Graphene Nanoribbons
- Tomonaga-Luttinger liquid parameters of magnetic waveguides in graphene
- Magnetic field induced semimetal-to-canted-antiferromagnet transition on the honeycomb lattice
- Gap generation for Dirac fermions on Lobachevsky plane in a magnetic field
- Quantum Hall plateau transition in the lowest Landau level of disordered graphene
- Properties of A Class of Topological Phase Transition
- Estimates of Effective Hubbard Model Parameters for C20 isomers
- Competition between excitonic gap generation and disorder scattering in graphene
- Explanation for the isotropy of the Dirac cone in graphene
- Charge density wave in graphene: magnetic-field-induced Peierls instability