Inducing topological order in a honeycomb lattice
T. Pereg-Barnea, G. Refael

TL;DR
This paper proposes a method to induce topological insulator phases in a honeycomb lattice by coupling it to a metallic environment, using long-range interactions controlled by the metal's Fermi wave vector, with potential realization in cold-atom systems.
Contribution
It introduces a novel approach to generate topological order in honeycomb lattices via metallic environment-induced interactions without spin-orbit coupling.
Findings
Fermi wave vector kF controls the phase of the honeycomb lattice.
Tuning parameters can realize topological insulator and quantum Hall states.
Parameter estimates suggest feasibility in cold-atom experiments.
Abstract
We explore the possibility of inducing a topological insulator phase in a honeycomb lattice lacking spin-orbit interaction using a metallic (or Fermi gas) environment. The lattice and the metallic environment interact through a density-density interaction without particle tunneling, and integrating out the metallic environment produces a honeycomb sheet with in-plane oscillating long-ranged interactions. We find the ground state of the interacting system in a variational mean-field method and show that the Fermi wave vector, kF, of the metal determines which phase occurs in the honeycomb lattice sheet. This is analogous to the Ruderman-Kittel-Kasuya-Yosida (RKKY) mechanism in which the metal's kF determines the interaction profile as a function of the distance. Tuning kF and the interaction strength may lead to a variety of ordered phases, including a topological insulator and anomalous…
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