Hexagon-singlet solid ansatz for the spin-1 kagome antiferromagnet

TL;DR

This paper investigates hexagon-singlet solid states as potential spin liquid candidates for the spin-1 kagome antiferromagnet, revealing their exponential decay of correlations, lack of topological order, and their use in variational studies showing a trimerized ground state.

Contribution

It introduces a tensor network representation of HSS states and demonstrates their properties and effectiveness in variational calculations for the kagome antiferromagnet.

Findings

HSS states have exponentially decaying correlations.

HSS states lack intrinsic topological order.

Trimerized valence bond crystal has lower energy than symmetric HSS states.

Abstract

We perform a systematic investigation on the hexagon-singlet solid (HSS) states, which are a class of spin liquid candidates for the spin-1 kagome antiferromagnet. With the Schwinger boson representation, we show that all HSS states have exponentially decaying correlations and can be interpreted as a (special) subset of the resonating Affleck-Kennedy-Lieb-Tasaki (AKLT) loop states. We provide a compact tensor network representation of the HSS states, with which we are able to calculate physical observables efficiently. We find that the HSS states have vanishing topological entanglement entropy, suggesting the absence of intrinsic topological order. We also employ the HSS states to perform a variational study of the spin-1 kagome Heisenberg antiferromagnetic model. When we use a restricted HSS ansatz preserving lattice symmetry, the best variational energy per site is found to be $e_0 = -1.3600$. In contrast, when allowing lattice symmetry breaking, we find a trimerized simplex valence bond crystal with a lower energy, $e_0=-1.3871$.