Effect of Rhombohedral to Orthorhombic Transition on Magnetic and Dielectric Properties of La and Ti co-substituted BiFeO3

TL;DR

This study investigates how La and Ti co-substitution in BiFeO3 induces a structural phase transition from rhombohedral to orthorhombic, significantly affecting its magnetic and dielectric properties, with potential implications for multifunctional device applications.

Contribution

It demonstrates the suppression of impurity phases and the structural transition caused by La and Ti co-substitution, revealing their effects on magnetic and dielectric enhancements in BiFeO3.

Findings

Remnant magnetization increases up to 10% co-substitution

Structural transition breaks spin cycloid structure

Dielectric constant significantly enhanced at x=0.100

Abstract

Polycrystalline La and Ti co-substituted ceramics were synthesized by the tartaric acid modified sol-gel technique. It was observed that the co-substitution of La & Ti at Bi & Fe sites in BiFeO3 suppress the impurity phase formation which is a common problem in bismuth ferrite. The quantitative crystallographic phase analysis was performed with the help of FULLPROF program which suggests the existence of compositional driven crystal structure transition from rhombohederal (space group R3c) to the orthorhombic (space group Pbnm). The changes in the phonon frequencies as well as line widths of A1 mode in Raman spectra reveal the lattice distortion which tends to modify the crystal structure. The structural transition breaks the spin cycloid structure in co-substituted BiFeO3 nanoparticles which leads to canting of the antiferromagnetic spin structure. Hence, the remnant magnetization increases up to 10 % of co-substitution and becomes 22 times that of BiFeO3. However, it decreases for higher co-substitution percentage due to significant contribution from the collinear antiferromagnetic ordering in the orthorhombic crystal symmetry. The co-substitution significantly enhanced the dielectric constant (maximum in x = 0.100) as well as frequency independent region for dielectric constant and dielectric loss.