Abstract

In this study we present ab initio density-functional theory calculations on stoichiometric, cation-doped, and strained $\mathrm{GaFeO}{}_{3}$. We start with a detailed discussion of the origin of the antiferromagnetic (AFM) superexchange in stoichiometric $\mathrm{GaFeO}{}_{3}$ and give a molecular orbital description of the exchange mechanism derived from our calculations. In addition, we study the properties of the Fe-O-Fe bonds for different geometries to underline the angle and distance dependence of the AFM coupling as formulated in the Goodenough-Kanamori rules. We describe the AFM ground state of $\mathrm{GaFeO}{}_{3}$ as a result of two intrinsic Fe-O-Fe chains that meander through the crystal along the $c$ direction. The magnetocrystalline anisotropy energies are calculated for the stoichiometric phase with and without inner cationic site disorder, and the presence of a sublattice-dependent anisotropy is examined. Furthermore, we perform our studies of ${\mathrm{Ga}}_{2\ensuremath{-}x}\mathrm{Fe}{}_{x}{\mathrm{O}}_{3}$ for varying Fe concentrations $\mathit{x}(0.0\ensuremath{\le}\mathit{x}\ensuremath{\le}2.0)$ where at a value of $\mathit{x}=0.0$ and $\mathit{x}=2.0$ it transforms into the isomorphic $\ensuremath{\varepsilon}\text{\ensuremath{-}}\mathrm{Ga}{}_{2}{\mathrm{O}}_{3}$ and $\ensuremath{\varepsilon}\text{\ensuremath{-}}\mathrm{Fe}{}_{2}{\mathrm{O}}_{3}$ phases, respectively. The effect of strain was also studied. Incorporating dopants and applying strain to the simulation cell changes the intrinsic geometry and thus the magnetic properties of gallium ferrite.

Highlights

  • GaFeO3 (GFO) is a multiferroic material showing both antiferromagnetic (AFM) and ferroelectric behavior in its ground state

  • Performing ab initio DFT calculations of the electronic and magnetic structure we examine the effects of strain, cation doping, and inner cationic site disorder on the AFM coupling strength

  • Since spin-orbit-related properties are influenced by geometry we compared the magnetocrystalline anisotropy energy (MAE) for simulation cells relaxed within the GGA+U or with the more realistic but computationally more elaborate HSE functional

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Summary

INTRODUCTION

GaFeO3 (GFO) is a multiferroic material showing both antiferromagnetic (AFM) and ferroelectric behavior in its ground state. Motivated by that we calculate the energetic difference and the contribution of the respective sublattices to the total MAE by including spin-orbit coupling in our calculations This is done for pure GaFeO3 and for the case of inner cationic site disorder. Strain evoked changes in the AFM coupling strength are examined, stretching and compressing the simulation cell in the a, b, and c directions while keeping the volume constant This is done for a doping concentration of 0.9 x 1.4 and the case of inner cationic site disorder. Performing ab initio DFT calculations of the electronic and magnetic structure we examine the effects of strain, cation doping, and inner cationic site disorder on the AFM coupling strength. Magnetic properties of GFO and may support the possibilities of tailoring the electronic and magnetic properties of GFO for a future application in electronic devices

COMPUTATIONAL DETAILS AND METHODS
AFM superexchange in GaFeO3
AFM superexchange in GFO
The instrinsic AFM chain in GFO
Magnetization density in GFO
Magnetocrystalline anisotropy energy in GFO
From ε-GO to GFO
Inner cationic site disorder in stoichiometric GFO
From GFO to ε-FO
THE EFFECT OF STRAIN
Strain on pristine GFO
Findings
CONCLUSION
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