# Theory of partial quantum disorder in the stuffed honeycomb Heisenberg antiferromagnet

## TL;DR

This paper develops an effective model to explain the partial quantum disorder observed in a stuffed honeycomb antiferromagnet, revealing a transition from planar ferromagnetic to stripe-ordered phases influenced by quantum fluctuations.

## Contribution

It derives a novel effective triangular-lattice XXZ model capturing the partial disorder phenomenon and identifies a critical spin value close to 1/2 where quantum fluctuations destabilize magnetic order.

## Key findings

- Effective model predicts transition at S_c=0.646
- Quantum fluctuations destabilize order near S=1/2
- Partial disorder state explained by frustrated interactions

## Abstract

Recent numerical results [Gonzalez $\textit{et al.}$, Phys. Rev. Lett. $\textbf{122}$, 017201 (2019); Shimada $\textit{et al.}$, J. Phys. Conf. Ser. $\textbf{969}$, 012126 (2018)] point to the existence of a partial-disorder ground state for a spin-1/2 antiferromagnet on the stuffed honeycomb lattice, with 2/3 of the local moments ordering in an antiferromagnetic N\'eel pattern, while the remaining 1/3 of the sites display short-range correlations only, akin to a quantum spin liquid. We derive an effective model for this disordered subsystem, by integrating out fluctuations of the ordered local moments, which yield couplings in a formal $1/S$ expansion, with $S$ being the spin amplitude. The result is an effective triangular-lattice XXZ model, with planar ferromagnetic order for large $S$ and a stripe-ordered Ising ground state for small $S$, the latter being the result of frustrated Ising interactions. Within the semiclassical analysis, the transition point between the two orders is located at $S_c=0.646$, being very close to the relevant case $S=1/2$. Near $S=S_c$ quantum fluctuations tend to destabilize magnetic order. We conjecture that this applies to $S=1/2$, thus explaining the observed partial-disorder state.