Effective low-energy Hamiltonians for interacting nanostructures
Michael Kinza, Jutta Ortloff, Carsten Honerkamp

TL;DR
This paper develops a functional renormalization group approach to derive low-energy Hamiltonians for interacting trigonal graphene nanodiscs, demonstrating the robustness of zero-energy state degeneracy and analyzing the effects of excited states.
Contribution
It introduces a systematic fRG method to derive effective low-energy Hamiltonians for nanostructures, including excited state effects, and confirms the robustness of zero-energy degeneracy.
Findings
Zero-energy state degeneracy remains robust against higher level influences.
The effective Hamiltonian captures interaction effects accurately.
Degeneracy is preserved for various nanodisc sizes and shapes.
Abstract
We present a functional renormalization group (fRG) treatment of trigonal graphene nanodiscs and composites thereof, modeled by finite-size Hubbard-like Hamiltonians with honeycomb lattice structure. At half filling, the noninteracting spectrum of these structures contains a certain number of half-filled states at the Fermi level. For the case of trigonal nanodiscs, including interactions between these degenerate states was argued to lead to a large ground state spin with potential spintronics applications. Here we perform a systematic fRG flow where the excited single-particle states are integrated out with a decreasing energy cutoff, yielding a renormalized low-energy Hamiltonian for the zero-energy states that includes effects of the excited levels. The numerical implementation corroborates the results obtained with a simpler Hartree-Fock treatment of the interaction effects within…
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