Studies on multiferroic properties of single phasic Bi0.85Ho0.05Sm0.1FeO3 ceramics

Author:

Rajesh R.1,John Ethilton S.1,Ramachandran K.2,Giridharan N. V.3,Ramesh Kumar K.4,Vadla Samba Siva5

Affiliation:

1. Department of Physics, Velammal College of Engineering and Technology, Madurai 625 009, Tamilnadu, India

2. Department of Physics, Gandhigram Rural Institute Deemed University, Dindigul 624 302, Tamilnadu, India

3. Department of Physics, National Institute of Technology, Tiruchirappalli 620 015, Tamilnadu, India

4. Department of Physics, University of Johannesburg, P. O. Box 524, Auckland Park 2006, South Africa

5. Department of Physics, Indian Institute of Technology Madras, Chennai 600 053, Tamilnadu, India

Abstract

Single-phase polycrystalline Bi[Formula: see text]Ho[Formula: see text]Sm[Formula: see text]FeO3 ceramic is prepared by conventional solid state route. The co-doping of Sm and Ho (via Bi site) in BiFeO3 controls the formation of secondary phases. The Rietveld refinement analysis shows an increasing trend in tilt angle due to the rotation of FeO6 octohedra with respect to host BiFeO3. The remanent polarization and the magnetization of Bi[Formula: see text]Ho[Formula: see text]Sm[Formula: see text]FeO3 ceramic are found to be significantly improved than BiFeO3 and Bi[Formula: see text]Sm[Formula: see text]FeO3 at room-temperature. Considerable variations in the remanent polarization (0.18 to 0.11 [Formula: see text]C/cm2) on magnetic poling and a dielectric anomaly in the vicinity of the antiferromagnetic transition temperature are due to the intrinsic magnetoelectric coupling effect in Bi[Formula: see text]Ho[Formula: see text]Sm[Formula: see text]FeO3 ceramic. The dielectric permittivity increases with increase in applied magnetic field and the coupling coefficient of Bi[Formula: see text]Ho[Formula: see text]Sm[Formula: see text]FeO3 ceramic is found to be 0.91% at 4 kOe.

Publisher

World Scientific Pub Co Pte Lt

Subject

Condensed Matter Physics,Statistical and Nonlinear Physics

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