Interaction of static charges in graphene within Monte-Carlo simulation
arXiv:1306.2544 · doi:10.1103/PhysRevB.89.195401
Abstract
The study of the interaction potential between static charges within Monte-Carlo simulation of graphene is carried out. The numerical simulations are performed in the effective lattice field theory with noncompact -dimensional Abelian lattice gauge fields and -dimensional staggered lattice fermions. It is shown that for all considered temperatures the interaction can be well described by the Debye screened potential created by two-dimensional electron-hole excitations. At low temperatures Debye mass plays a role of order parameter of the insulator-semimetal phase transition. In the semimetal phase at high temperature graphene reveals the properties of weakly interacting two-dimensional plasma of fermions excitations.
8 pages, 7 figures
References in corpus (9)
- Electric Field Effect in Atomically Thin Carbon Films
- The electronic properties of graphene
- Is graphene in vacuum an insulator?
- Lattice field theory simulations of graphene
- Monte-Carlo study of the semimetal-insulator phase transition in monolayer graphene with realistic inter-electron interaction potential
- Quantum Critical Behaviour in a Graphene-like Model
- Monte-Carlo study of the electron transport properties of monolayer graphene within the tight-binding model
- Atomic Structures of Graphene, Benzene and Methane with Bond Lengths as Sums of the Single, Double and Resonance Bond Radii of Carbon
- Numerical study of the conductivity of graphene monolayer within the effective field theory approach
Cited by in corpus (6)
- Many-body effects in graphene beyond the Dirac model with Coulomb interaction
- Quantum Monte Carlo study of static potential in graphene
- Absence of inhomogeneous chiral phases in 2+1-dimensional four-fermion and Yukawa models
- Numerical simulation of graphene in external magnetic field
- Spatially oscillating correlation functions in -dimensional four-fermion models: The mixing of scalar and vector modes at finite density
- Lattice field theory simulations of Dirac semimetals