Abstract

BiFeO3 is an interesting material due to its multiferroic properties. It attracts attention due to its potential applications in spintronics and in microelectronics for data storage, among others. Single-phase bulk material from BiFeO3 is difficult to synthesize. The kinetics of perovskite phase formation most often leads to the presence of impurity phases. It has been shown that low levels of replacement of Bi with rare earth ions lead to stabilization of the perovskite phase. In the present work, Rietveld refinement of the crystal structure based on powder X-ray diffraction patterns was applied to study the influence of partial substitution of Bi by rare-earth (RE) elements with different ionic radii on structural and morphological properties of the ferrite phase. Substitution by large RE ions was found to preserve the rhombohedral symmetry of BiFeO3, whereas substitution by smaller RE ions led to the coexistence of two polymorphic perovskite phases with rhombohedral R3c and orthorhombic Pnma symmetries. The unit cell parameters as well as the interatomic distances and angles, not only around the A cation but also around the iron ions, were influenced by the substitution. The mean crystallite and particle size decreased with the decrease of ionic radius of substituting RE ion.

Highlights

  • Rietveld refinement of the crystal structure based on powder

  • X-ray diffraction patterns was applied to study the influence of partial substitution of bismuth by rare earth elements with different ionic radii, on structural and microstructural properties of the perovskite phase

  • The morphology of the compounds was studied by scanning electron microscopy (SEM)

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Summary

Introduction

BiFeO3 belongs to a class of perovskite structure and is one of the most studied compounds due to its unique electrical and magnetic properties. It shows a ferroelectric arrangement at 830 ◦ C, which is thought to originate from the stereochemical activity of. The G-type antiferromagnetic arrangement below 370 ◦ C describes the magnetic structure of BiFeO3. The phase is multiferroic at room temperature and is considered a promising material for various applications in electronics and data storage [1,2,3]. The crystal structure of nonsubstituted BiFeO3 can be described as corner shared trigonally distorted FeO6 octahedra with mutual tilting.

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