Effective models for strong electronic correlations at graphene edges
arXiv:1305.0559 · doi:10.1103/PhysRevB.87.245431
Abstract
We describe a method for deriving effective low-energy theories of electronic interactions at graphene edges. Our method is applicable to general edges of honeycomb lattices (zigzag, chiral, and even disordered) as long as localized low-energy states (edge states) are present. The central characteristic of the effective theories is a dramatically reduced number of degrees of freedom. As a consequence, the solution of the effective theory by exact diagonalization is feasible for reasonably large ribbon sizes. The quality of the involved approximations is critically assessed by comparing the correlation functions obtained from the effective theory with numerically exact quantum Monte-Carlo calculations. We discuss effective theories of two levels: a relatively complicated fermionic edge state theory and a further reduced Heisenberg spin model. The latter theory paves the way to an efficient description of the magnetic features in long and structurally disordered graphene edges beyond the mean-field approximation.
13 pages, 9 figures
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Cited by in corpus (12)
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- Ultra long spin decoherence times in graphene quantum dots with a small number of nuclear spins
- Quantum phase transitions in effective spin-ladder models for graphene zigzag nanoribbons
- Topological edge states of a graphene zigzag nanoribbon with spontaneous edge magnetism
- Effect of long-range interaction on graphene edge magnetism
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