Abstract

A pressing need in low energy spintronics is two-dimensional (2D) ferromagnets with Curie temperature above the liquid-nitrogen temperature (77 K), and sizeable magnetic anisotropy. We studied Mn3Br8 monolayer which is obtained via inducing Mn vacancy at 1/4 population in MnBr2 monolayer. Such defective configuration is designed to change the coordination structure of the Mn-d5 and achieve ferromagnetism with sizeable magnetic anisotropy energy (MAE). Our calculations show that Mn3Br8 monolayer is a ferromagnetic (FM) half-metal with Curie temperature of 130 K, large MAE of − 2.33 meV per formula unit, and atomic magnetic moment of 13/3μB for the Mn atom. Additionally, Mn3Br8 monolayer maintains to be FM under small biaxial strain, whose Curie temperature under 5% compressive strain is 160 K. Additionally, both biaxial strain and carrier doping make the MAE increases, which mainly contributed by the magneto-crystalline anisotropy energy (MCE). Our designed defective structure of MnBr2 monolayer provides a simple but effective way to achieve ferromagnetism with large MAE in 2D materials.

Highlights

  • Spintronics, exploiting the electron spin and the associated magnetic moment, has attracted extensive attention during the past few decades [1], because of its unique advantages over charge-based devices

  • ­MnBr2 monolayer is antiferromagnetic with 0.25 meV magnetic anisotropy energy (MAE) along the perpendicular direction to the plane based on the first-principles calculations [16]; ­Mn2+ ions are in the d­ 5 high-spin state with magnetic moment of 5μB [16, 26]

  • Our results show that ­Mn3Br8 monolayer maintains to be FM with Curie temperature increasing under small biaxial strain

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Summary

Introduction

Spintronics, exploiting the electron spin and the associated magnetic moment, has attracted extensive attention during the past few decades [1], because of its unique advantages over charge-based devices. The first two 2D ferromagnets with atomic-thickness was achieved in 2017, that is monolayer ­CrI3 [2] and bilayer ­Cr2Ge2Te6 [3]. ­MnBr2 monolayer is antiferromagnetic with 0.25 meV MAE along the perpendicular direction to the plane based on the first-principles calculations [16]; ­Mn2+ ions are in the d­ 5 high-spin state with magnetic moment of 5μB [16, 26]. These results imply the potentials of M­ nBr2 as monolayer ferromagnet with large magnetic moment. The key problem is how to convert the AFM coupling between Mn ions into FM coupling

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