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A New Phase Boundary in (Bi 1/2 Na 1/2 )TiO 3 −BaTiO 3 Revealed via a Novel Method of Electron Diffraction Analysis
Author(s) -
Ma Cheng,
Guo Hanzheng,
Tan Xiaoli
Publication year - 2013
Publication title -
advanced functional materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 6.069
H-Index - 322
eISSN - 1616-3028
pISSN - 1616-301X
DOI - 10.1002/adfm.201300640
Subject(s) - materials science , phase boundary , poling , crystallite , phase (matter) , piezoelectricity , perovskite (structure) , electron diffraction , diffraction , phase diagram , condensed matter physics , octahedron , crystallography , ferroelectricity , crystal structure , optics , dielectric , composite material , optoelectronics , physics , metallurgy , chemistry , quantum mechanics
A new phase boundary is revealed in (1– x )(Bi 1/2 Na 1/2 )TiO 3 − x BaTiO 3 , the most extensively studied lead‐free piezoelectric solid solution. This discovery results from a novel method of electron diffraction analysis, which allows the precise determination of oxygen octahedra tilting in multi‐domain perovskite ferroelectrics. The study using this method supports the recently proposed Cc symmetry for pure (Bi 1/2 Na 1/2 )TiO 3 , and, more importantly, indicates the crystal structure evolves into the R3c symmetry with the addition of BaTiO 3 , forming a Cc / R3c phase boundary at x = 3–4%. In the poling field E pol versus composition x phase diagram for polycrystalline ceramics, this phase boundary exists with E pol below 5.5 kV mm −1 ; the Cc phase is transformed to the R3c phase during poling at higher fields. The results reported here provide the microstructural origin for the previously unexplained strain behavior and clarify the low‐BaTiO 3 ‐content phase relationship in this popular lead‐free piezoelectric system.

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