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Nonstoichiometric BiFe{sub 0.9}Ti{sub 0.05}O{sub 3} multiferroic ceramics with ultrahigh electrical resistivity

Journal Article · · Journal of Applied Physics
DOI:https://doi.org/10.1063/1.3506526· OSTI ID:21476612
;  [1]; ; ;  [2]
  1. Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education and School of Physics and Technology, Wuhan University, Wuhan 430072 (China)
  2. Department of Applied Physics and Materials Research Centre, Hong Kong Polytechnic University (Hong Kong)
BiFeO{sub 3}, BiFe{sub 0.9}Ti{sub 0.1}O{sub 3}, and BiFe{sub 0.9}Ti{sub 0.05}O{sub 3} ceramics of relatively high perovskite phase content were prepared for a comparison study. While both BiFe{sub 0.9}Ti{sub 0.1}O{sub 3} and BiFe{sub 0.9}Ti{sub 0.05}O{sub 3} exhibit similarly improved weak ferromagnetism over BiFeO{sub 3}, there exists a major difference in the x-ray diffraction patterns of BiFe{sub 0.9}Ti{sub 0.1}O{sub 3} and BiFe{sub 0.9}Ti{sub 0.05}O{sub 3}, and the leakage current of BiFe{sub 0.9}Ti{sub 0.05}O{sub 3} is decreased by five orders of magnitude from that of BiFe{sub 0.9}Ti{sub 0.1}O{sub 3}. With an ultrahigh electrical resistivity, over 1x10{sup 14} {Omega} cm, BiFe{sub 0.9}Ti{sub 0.05}O{sub 3} ceramic displays an especially low dielectric loss, 0.015 at 100 Hz, a remanent polarization P{sub r} of 0.23 {mu}C/cm{sup 2} and a remanent magnetization M{sub r} of 0.13 emu/g at room temperature. It is proposed that the Fe-deficiency in BiFe{sub 0.9}Ti{sub 0.05}O{sub 3} decreases the amount of Fe{sup 2+} and leads to the ultrahigh electrical resistivity. Nonstoichiometric compositions should receive more attention for developing high quality BiFeO{sub 3} multiferroic materials.
OSTI ID:
21476612
Journal Information:
Journal of Applied Physics, Journal Name: Journal of Applied Physics Journal Issue: 9 Vol. 108; ISSN JAPIAU; ISSN 0021-8979
Country of Publication:
United States
Language:
English