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Effects of La-doping on microstructure, dielectric and piezoelectric properties of Ba0.85Ca0.15Ti0.90Zr0.10O3 lead-free ceramics
Effects of La-doping on microstructure, dielectric and piezoelectric properties of Ba0.85Ca0.15Ti0.90Zr0.10O3 lead-free ceramics
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Effects of La-doping on microstructure, dielectric and piezoelectric properties of Ba0.85Ca0.15Ti0.90Zr0.10O3 lead-free ceramics
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Effects of La-doping on microstructure, dielectric and piezoelectric properties of Ba0.85Ca0.15Ti0.90Zr0.10O3 lead-free ceramics
Effects of La-doping on microstructure, dielectric and piezoelectric properties of Ba0.85Ca0.15Ti0.90Zr0.10O3 lead-free ceramics

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Effects of La-doping on microstructure, dielectric and piezoelectric properties of Ba0.85Ca0.15Ti0.90Zr0.10O3 lead-free ceramics
Effects of La-doping on microstructure, dielectric and piezoelectric properties of Ba0.85Ca0.15Ti0.90Zr0.10O3 lead-free ceramics
Journal Article

Effects of La-doping on microstructure, dielectric and piezoelectric properties of Ba0.85Ca0.15Ti0.90Zr0.10O3 lead-free ceramics

2013
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Overview
Lead-free (Ba 0.85 Ca 0.15 ) 1−x La 2/3x Ti 0.90 Zr 0.10 O 3  + 1 mol% MnO 2 ceramics have been prepared an ordinary sintering technique and the effects of La-doping on the microstructure, dielectric and piezoelectric properties of Ba 0.85 Ca 0.15 Ti 0.90 Zr 0.10 O 3 were studied. All the ceramics possess a pure perovskite structure, indicating that La ions are incorporated into Ba 0.85 Ca 0.15 Ti 0.90 Zr 0.10 O 3 lattices to form a lead-free solid solution. The ceramics are transformed from coexistence of orthorhombic and tetragonal phases to pseudocubic phase with the doping level of La increasing. After the doping of La, grain growth is inhibited, ferroelectric-paraelectric phase transition temperature ( T C ) is decreased and the degree of diffuse phase transition is increased. The ferroelectricity of the ceramics is weakened after the addition of La. Unlike donor-doped lead zirconate titanate ceramics, the piezoelectric properties of the ceramics are degraded after the partial substitution of La 3+ for (Ba 0.85 Ca 0.15 ) 2+ because of the weakness or disappearance of coexistence of orthorhombic and tetragonal phases near room temperature. The (Ba 0.85 Ca 0.15 ) 1−x La 2/3x Ti 0.90 Zr 0.10 O 3  + 1 mol% MnO 2 ceramic with x = 0 exhibit the optimum piezoelectric properties: d 33  = 277 pC/N and k p  = 30.3 %, respectively.