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Phase Transition and Electrical Properties of Ba 0.7 Ca 0.3 TiO 3 – BiFeO 3 Ceramics
Author(s) -
Li CaiXia,
Yang Bin,
Zhang ShanTao,
Wu FengMin,
Cao WenWu
Publication year - 2012
Publication title -
journal of the american ceramic society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.9
H-Index - 196
eISSN - 1551-2916
pISSN - 0002-7820
DOI - 10.1111/j.1551-2916.2012.05398.x
Subject(s) - materials science , ferroelectricity , tetragonal crystal system , orthorhombic crystal system , phase transition , dielectric , piezoelectricity , hysteresis , piezoelectric coefficient , electric field , condensed matter physics , ceramic , analytical chemistry (journal) , mineralogy , crystal structure , crystallography , composite material , chemistry , optoelectronics , physics , chromatography , quantum mechanics
Lead‐free piezoelectric ceramics of (1 −  x ) Ba 0.70 Ca 0.30 TiO 3 – x BiFeO 3 [(1 −  x ) BCT – x BF , x  =   0–0.065] have been prepared and investigated. The ceramics with x  ≤   0.06 have diphasic tetragonal and orthorhombic crystal structures, whereas tetragonal phase is suppressed by the introduction of BF . As a result, the composition with x  =   0.065 is found to have diphasic pseudocubic and orthorhombic phases. Significantly composition‐dependent grain size is observed. With increasing x from 0 to 0.065, the ferroelectric‐paraelectric phase transition temperature decreases monotonically from 128°C to 50°C, accompanied by enhanced ferroelectric relaxor behavior, as indicated by the widened diffused phase transition temperature. The room temperature polarization–electric field ( P–E ) hysteresis loops and strain–electric field ( S–E ) curves indicate that the ferroelectricity enhances slightly and reaches the maximum near x  =   0.05, and then weakens with increasing x . On the other hand, the piezoelectric coefficient ( d 33 ) and electromechanical coupling coefficient ( k p ) decrease simultaneously with increasing x , whereas the mechanical quality factor ( Q m ) reaches the maximum near x  =   0.05. The structure‐property relationship is discussed intensively. Our results may be helpful for further understanding and designing BaTiO 3 ‐related lead‐free ferroelectric/piezoelectric materials.

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