Eur. Phys. J. B 75, 451-460 (2010)
https://doi.org/10.1140/epjb/e2010-00170-x

On the room temperature multiferroic BiFeO₃: magnetic, dielectric and thermal properties

¹ Experimental Physics V, Center for Electronic Correlations and Magnetism, University of Augsburg, 86159 Augsburg, Germany
² School of Materials Science and Engineering, University of Science and Technology, 100083, Beijing, P.R. China
³ Experimentelle Physik IV, Universität Würzburg, 97074 Würzburg, Germany
⁴ General Physics Institute of the Russian Academy of Sciences, 119991 Moscow, Russia

Corresponding author: ^a peter.lunkenheimer@physik.uni-augsburg.de

Received: 2 October 2009
Revised: 23 March 2010
Published online: 4 June 2010

Abstract

Magnetic dc susceptibility between 1.5 and 800 K, ac susceptibility and magnetization, thermodynamic properties, temperature dependence of radio and audio-wave dielectric constants and conductivity, contact-free dielectric constants at mm-wavelengths, as well as ferroelectric polarization are reported for single crystalline BiFeO₃. A well developed anomaly in the magnetic susceptibility signals the onset of antiferromagnetic order close to 635 K. Beside this anomaly no further indications of phase or glass transitions are indicated in the magnetic dc and ac susceptibilities down to the lowest temperatures. The heat capacity has been measured from 2 K up to room temperature and significant contributions from magnon excitations have been detected. From the low-temperature heat capacity an anisotropy gap of the magnon modes of the order of 6 meV has been determined. The dielectric constants measured in standard two-point configuration are dominated by Maxwell-Wagner like effects for temperatures T > 300 K and frequencies below 1 MHz. At lower temperatures the temperature dependence of the dielectric constant and loss reveals no anomalies outside the experimental errors, indicating neither phase transitions nor strong spin phonon coupling. The temperature dependence of the dielectric constant was measured contact free at microwave frequencies. At room temperature the dielectric constant has an intrinsic value of 53. The loss is substantial and strongly frequency dependent indicating the predominance of hopping conductivity. Finally, in small thin samples we were able to measure the ferroelectric polarization between 10 and 200 K. The saturation polarization is of the order of 40 μC/cm², comparable to reports in literature.