“…15,17 This is probably due to the high coercive electric field and dielectric loss of BFO relative to that of BKT. 5,13 Morozov et al have recently shown that the conductivity of BFO-BKT materials can be reduced by annealing in an inert atmosphere improving the electromechanical performance.…”
Ferroelectric BiFeO 3 has attractive properties such as high strain and polarization, but a wide range of applications of bulk BiFeO 3 are hindered due to high leakage currents and a high coercive electric field.Here, we report on the thermal behaviour of the electrical conductivity and thermopower of BiFeO 3 substituted with 10 and 20 mol% Bi 0.5 K 0.5 TiO 3 . A change from p-type to n-type conductivity in these semi-conducting materials was demonstrated by the change in the sign of the Seebeck coefficient and the change in the slope of the isothermal conductivity versus partial pressure of O. A minimum in the isothermal conductivity was observed at B10 À2 bar O 2 partial pressure for both solid solutions. The strong dependence of the conductivity on the partial pressure of O 2 was rationalized by a point defect model describing qualitatively the conductivity involving oxidation/reduction of Fe 3+ , the dominating oxidation state of Fe in stoichiometric BiFeO 3 . The ferroelectric to paraelectric phase transition of 80 and 90 mol% BiFeO 3 was observed at 648 AE 15 and 723 AE 15 1C respectively by differential thermal analysis and confirmed by dielectric spectroscopy and high temperature powder X-ray diffraction.
“…15,17 This is probably due to the high coercive electric field and dielectric loss of BFO relative to that of BKT. 5,13 Morozov et al have recently shown that the conductivity of BFO-BKT materials can be reduced by annealing in an inert atmosphere improving the electromechanical performance.…”
Ferroelectric BiFeO 3 has attractive properties such as high strain and polarization, but a wide range of applications of bulk BiFeO 3 are hindered due to high leakage currents and a high coercive electric field.Here, we report on the thermal behaviour of the electrical conductivity and thermopower of BiFeO 3 substituted with 10 and 20 mol% Bi 0.5 K 0.5 TiO 3 . A change from p-type to n-type conductivity in these semi-conducting materials was demonstrated by the change in the sign of the Seebeck coefficient and the change in the slope of the isothermal conductivity versus partial pressure of O. A minimum in the isothermal conductivity was observed at B10 À2 bar O 2 partial pressure for both solid solutions. The strong dependence of the conductivity on the partial pressure of O 2 was rationalized by a point defect model describing qualitatively the conductivity involving oxidation/reduction of Fe 3+ , the dominating oxidation state of Fe in stoichiometric BiFeO 3 . The ferroelectric to paraelectric phase transition of 80 and 90 mol% BiFeO 3 was observed at 648 AE 15 and 723 AE 15 1C respectively by differential thermal analysis and confirmed by dielectric spectroscopy and high temperature powder X-ray diffraction.
“…6 Owing to these limitations, application of pure bismuth ferrite in piezoelectric devices is challenging, but as a perovskite modifier it can be very prospective for compositional engineering. Recently, tailoring of BFO-related compositions for high-temperature electromechanical applications has been proposed for a wide range of solid solutions with lead-free Bi 0.5 K 0.5 TiO 3 (BFO-BKT), [7][8][9][10] and further along morphotropic phase boundary towards lead titanate (BFO-BKT-PT). 11,12 The understanding of the origins of the undesired conductivity in BFO has been a topic of several theoretical 13,14 and experimental [15][16][17] studies.…”
High electrical conductivity is one of the main obstacles for advances of bulk BiFeO3 ceramics in piezoelectric applications. Here, we demonstrate that the electrical conductivity of BiFeO3 can be lowered by compositional modification with Bi0.5K0.5TiO3 and further reduced by annealing in oxidizing or reducing atmospheres. These manipulations also allow for tailoring of other functional properties. In particular, we demonstrate that the electric field induced strain performance of bulk bismuth ferrite can be significantly improved by addition of 30% Bi0.5K0.5TiO3 and thermal annealing in an inert atmosphere.
“…The BiFeO 3 rich compositions, where x < 0.7 belong to the rhombohedral R3c phase as determined using laboratory X-rays and neutron diffraction. 26 Morozov and Matsuo determined the presence of a MPB at x ¼ 0.6 between the polar rhombohedral R3c phase and a psuedocubic phase which exists over a large compositional space between 0.25 < x < 0.6. The large electric-field induced strains reported in BF-KBT are proposed to be due to the presence of polar nano-regions (PNRs) that are easily switched by an applied electric field; 23,24 however, the PNRs return to a random order upon removal of the field and, hence, the electromechanical properties are dominated by electrostriction.…”
Article:Bennett, J, Bell, AJ, Stevenson, TJ et al.(1 more author) (2013) Tailoring the structure and piezoelectric properties of BiFeO3-(K0.5Bi0.5)TiO3-PbTiO3 ceramics for high temperature applications. Applied Physics Letters, 103 (15). 152901.
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