Electric-field induced magnetic-anisotropy transformation to achieve spontaneous valley polarization

TL;DR

This paper proposes a method to achieve spontaneous valley polarization in 2D materials by electric-field-induced magnetic anisotropy transformation, demonstrated through first-principles calculations on a VSi2P4 monolayer.

Contribution

It introduces a novel approach to control valley polarization via electric fields by transforming magnetic anisotropy in a specific monolayer material.

Findings

Electric field induces transition of magnetic anisotropy from in-plane to out-of-plane.

Out-of-plane magnetization favors spontaneous valley polarization.

VSi2P4 exhibits ferromagnetic and ferrovalley properties under certain electric fields.

Abstract

Valleytronics has been widely investigated for providing new degrees of freedom to future information coding and processing. Here, it is proposed that valley polarization can be achieved by electric field induced magnetic anisotropy (MA) transformation. Through the first-principle calculations, our idea is illustrated by a concrete example of $\mathrm{VSi_2P_4}$ monolayer. The increasing electric field can induce a transition of MA from in-plane to out-of-plane by changing magnetic anisotropy energy (MAE) from negative to positive value, which is mainly due to increasing magnetocrystalline anisotropy (MCA) energy. The out-of-plane magnetization is in favour of spontaneous valley polarization in $\mathrm{VSi_2P_4}$. Within considered electric field range, $\mathrm{VSi_2P_4}$ is always ferromagnetic (FM) ground state. In a certain range of electric field, the coexistence of semiconductor and out-of-plane magnetization makes $\mathrm{VSi_2P_4}$ become a true ferrovalley (FV) material. The anomalous valley Hall effect (AVHE) can be observed under in-plane and out-of-plane electrical field in $\mathrm{VSi_2P_4}$. Our works pave the way to design the ferrovalley material by electric field.