$S = 1$ pyrochlore magnets with competing anisotropies: A tale of two Coulomb phases, $Z_2$ flux confinement and $XY$-like transitions

TL;DR

This paper explores the rich low-temperature phases of $S=1$ pyrochlore magnets with competing anisotropies, revealing transitions between Coulomb liquids with different flux confinement properties and a paramagnetic phase, characterized by pinch-point singularities.

Contribution

It introduces a theoretical framework describing three distinct low-temperature phases in $S=1$ pyrochlore magnets with competing anisotropies, including Coulomb liquids with $Z_2$ flux confinement and an XY-like transition.

Findings

Identification of two Coulomb liquid phases with different flux confinement properties.

Prediction of a flux-deconfinement to flux-confinement transition at $T_{c_2} \\approx 1.57|rac{\mu}{J}|$.

Observation of an XY-like transition at $T_{c_1} \\approx 0.98 |rac{\mu}{J}|$.

Abstract

We argue that the low-temperature physics of $S=1$ pyrochlore magnets with a predominantly Ising-like easy-axis exchange coupling $J$ that favors the local tetrahedral body diagonals, and a comparably large easy-plane single-ion anisotropy $\Delta =J + \mu$ ($|\mu| \ll J$) that favors the plane perpendicular to these local axes will exhibit interesting new phenomena due to the competition between $J$ and $\Delta$. In the $T/J \rightarrow 0$ limit, we find three low temperature phases as a function of $\mu/T$: a short-range correlated paramagnetic phase, and two topologically-distinct Coulomb liquids separated by a $Z_2$ flux confinement transition. Both Coulomb liquids are described at long-wavelengths by a fluctuating divergence-free polarization field and have characteristic pinch-point singularities in their structure factor. In one Coulomb phase, the flux of this polarization field is confined to {\em even} integers, while it takes on all integer values in the other Coulomb phase. Experimental realizations with $|\mu| \ll J$ and negative are predicted to exhibit signatures of a transition from a flux-deconfined Coulomb phase to the flux-confined Coulomb phase as they are cooled below $T_{c_2} \approx 1.57|\mu|$, while realizations with positive $\mu \ll J$ will show signatures of a transition from a flux-deconfined Coulomb liquid to a short-range correlated paramagnet via a continuous $XY$-like transition at $T_{c_1} \approx 0.98 \mu$.