Imaging the N\'eel vector switching in the monolayer antiferromagnet MnPSe$_3$ with strain-controlled Ising order

TL;DR

This study visualizes and manipulates Neel vector switching in monolayer MnPSe$_3$ using strain-controlled Ising order, revealing new insights into 2D antiferromagnetic spintronics and phase transition behavior.

Contribution

It demonstrates direct imaging of Neel vector switching in monolayer MnPSe$_3$ and elucidates the strain-induced transition from XY to Ising universality class.

Findings

Detected long-range Neel AFM order in monolayer MnPSe$_3$

Strain enables arbitrary rotation of Neel vectors in-plane

AFM domain walls are highly mobile after thermal cycling

Abstract

The family of monolayer two-dimensional (2D) materials hosts a wide range of interesting phenomena, including superconductivity, charge density waves, topological states and ferromagnetism, but direct evidence for antiferromagnetism in the monolayer has been lacking. Nevertheless, antiferromagnets have attracted enormous interest recently in spintronics due to the absence of stray fields and their terahertz resonant frequency. Despite the great advantages of antiferromagnetic spintronics, controlling and detecting N\'eel vectors have been limited in bulk materials. In this work, we developed a sensitive second harmonic generation (SHG) microscope and detected long-range N\'eel antiferromagnetic (AFM) order and N\'eel vector switching down to the monolayer in MnPSe$_3$. Temperature-dependent SHG measurement in repetitive thermal cooling surprisingly collapses into two curves, which correspond to the switching of an Ising type N\'eel vector reversed by the time-reversal operation, instead of a six-state clock ground state expected from the threefold rotation symmetry in the structure. We imaged the spatial distribution of the N\'eel vectors across samples and rotated them by an arbitrary angle irrespective of the lattice in the sample plane by applying strain. By studying both a Landau theory and a microscopic model that couples strain to nearest-neighbor exchange, we conclude that the phase transition of the XY model in the presence of strain falls into the Ising universality class instead of the XY one, which could explain the extreme strain tunability. Finally, we found that the 180{\deg} AFM domain walls are highly mobile down to the monolayer after thermal cycles, paving the way for future control of the antiferromagnetic domains by strain or external fields on demand for ultra-compact 2D AFM terahertz spintronics.