# Magnetic order in single crystals of Na3Co2SbO6 with a honeycomb arrangement of 3d$^7$ Co$^{2+}$ ions

## TL;DR

This study synthesizes and characterizes Na$_3$Co$_2$SbO$_6$ single crystals, revealing a monoclinic structure with anisotropic magnetic properties, a zigzag antiferromagnetic order below 5 K, and insights into its electronic ground state.

## Contribution

The paper provides detailed structural, magnetic, and theoretical analysis of Na$_3$Co$_2$SbO$_6$, highlighting its zigzag magnetic order and complex electronic interactions.

## Key findings

- Na$_3$Co$_2$SbO$_6$ has a monoclinic structure with layered Co$_2$SbO$_6$ sheets.
- The compound exhibits anisotropic magnetic susceptibility and a transition to antiferromagnetic order below 5 K.
- Neutron diffraction confirms zigzag magnetic order with moments aligned along the b-axis.

## Abstract

We have synthesized single crystals of Na$_3$Co$_2$SbO$_6$ and characterized the structure and magnetic order by measuring anisotropic magnetic properties, heat capacity, x-ray and neutron single crystal diffraction. Magnetic properties and specific heat of polycrystalline Na$_3$Co$_2$SbO$_6$ were also measured for comparison. Na$_3$Co$_2$SbO$_6$ crystallizes in a monoclinic structure (space group $C2/m$) with [Co$_2$SbO$_6$]$^{3-}$ layers separated by Na$^+$ ions. The temperature dependence of magnetic susceptibility shows significant anisotropic behavior in the whole temperature range 2\,K-350\,K investigated in this work. An effective moment of about 5.5\,$\mu_B$/Co$^{2+}$ from a Curie-Weiss fitting of the magnetic susceptibility is larger than the spin only value and signals significant orbital contribution. Na$_3$Co$_2$SbO$_6$ single crystal undergoes a transition into a long-range antiferromagnetically ordered state below $T_N$=5\,K. Neutron single crystal diffraction confirmed the zigzag magnetic structure with a propagation vector k\,=\,(0.5, 0.5, 0). The ordered moment is found to be 0.9\,$\mu_B$ at 4\,K and align along the crystallographic \textit{b}-axis. Density functional theory calculations suggest that the experimentally observed zigzag order is energetically competing with the Neel order. It is also found that the covalency between Co $d$ and O $p$ is quite strong and competes with the local spin-orbit coupling, suggesting a $J_{eff}$=1/2 ground state may not be realized in this compound.