Magnetic frustration in the cubic double perovskite Ba2NiIrO6

TL;DR

This study investigates the magnetic and electronic properties of Ba2NiIrO6, revealing the role of frustrated second-nearest-neighbor antiferromagnetic interactions in its antiferromagnetic ground state and clarifying the absence of $J_{eff}$ states.

Contribution

The paper combines theoretical calculations and simulations to elucidate the magnetic interactions and ground state structure of Ba2NiIrO6, highlighting the importance of long-range couplings and spin-orbit effects.

Findings

Strong 2NN AF couplings cause magnetic frustration.

The observed AF order is due to long-range interactions, not local $J_{eff}$ states.

Predicted AF transition temperature matches experimental data.

Abstract

Hybrid transition metal oxides continue to attract attention due to their multiple degrees of freedom ($e.g.$, lattice, charge, spin, and orbital) and versatile properties. Here we investigate the magnetic and electronic properties of the newly synthesized double perovskite Ba$_2$NiIrO$_6$, using crystal field theory, superexchange model analysis, density functional calculations, and parallel tempering Monte Carlo (PTMC) simulations. Our results indicate that Ba$_2$NiIrO$_6$ has the Ni$^{2+}$ ($t_{2g}^{6}e_{g}^{2}$)-Ir$^{6+}$ ($t_{2g}^{3}$) charge states. The first nearest-neighboring (1NN) Ni$^{2+}$-Ir$^{6+}$ ions prefer a ferromagnetic (FM) coupling as expected from the Goodenough-Kanamori-Anderson rules, which contradicts the experimental antiferromagnetic (AF) order in Ba$_2$NiIrO$_6$. We find that the strong 2NN AF couplings are frustrated in the fcc sublattices, and they play a major role in determining the observed AF ground state. We also prove that the $J_{\rm eff}$ = 3/2 and $J_{\rm eff}$ = 1/2 states induced by spin-orbit coupling, which would be manifested in low-dimensional (e.g., layered) iridates, are however not the case for cubic Ba$_2$NiIrO$_6$. Our PTMC simulations show that when the long-range (2NN and 3NN) AF interactions are included, an AF transition with $T_{\rm N}$ = 66 K would be obtained and it is well comparable with the experimental 51 K. Meanwhile, we propose a possible 2$\times$2$\times$2 noncollinear AF structure for Ba$_2$NiIrO$_6$.