# Two-dimensional ${J}_{\rm eff}$ = 1/2 antiferromagnetic insulator unraveled from interlayer exchange coupling in artificial perovskite iridate superlattices

## TL;DR

This study investigates how varying interlayer exchange coupling in artificial iridate superlattices influences their magnetic and electronic properties, revealing a switchable interlayer exchange and the realization of a two-dimensional antiferromagnetic insulator.

## Contribution

It demonstrates control over interlayer exchange coupling in iridate superlattices, leading to switchable magnetic interactions and the realization of a two-dimensional ${J}_{
m eff}$ = 1/2 antiferromagnetic insulator.

## Key findings

- Stronger insulating behavior in samples with more SrTiO$_3$ layers.
- Interlayer exchange coupling sign can be switched by layer number.
- Achieved a stable two-dimensional antiferromagnetic phase.

## Abstract

We report an experimental investigation of the two-dimensional ${J}_{\rm eff}$ = 1/2 antiferromagnetic Mott insulator by varying the interlayer exchange coupling in [(SrIrO$_3$)$_1$, (SrTiO$_3$)$_m$] ($m$ = 1, 2 and 3) superlattices. Although all samples exhibited an insulating ground state with long-range magnetic order, temperature-dependent resistivity measurements showed a stronger insulating behavior in the $m$ = 2 and $m$ = 3 samples than the $m$ = 1 sample which displayed a clear kink at the magnetic transition. This difference indicates that the blocking effect of the excessive SrTiO$_3$ layer enhances the effective electron-electron correlation and strengthens the Mott phase. The significant reduction of the Neel temperature from 150 K for $m$ = 1 to 40 K for $m$ = 2 demonstrates that the long-range order stability in the former is boosted by a substantial interlayer exchange coupling. Resonant x-ray magnetic scattering revealed that the interlayer exchange coupling has a switchable sign, depending on the SrTiO$_3$ layer number $m$, for maintaining canting-induced weak ferromagnetism. The nearly unaltered transition temperature between the $m$ = 2 and the $m$ = 3 demonstrated that we have realized a two-dimensional antiferromagnet at finite temperatures with diminishing interlayer exchange coupling.