Journal of the American Ceramic Society · 2015 · 15 citations · 28 references
Natural SciencesMaterials EngineeringMaterials ScienceCeramic MaterialsCeramicsSolid State PhysicsDefects In CeramicsElectrical Properties Of CeramicsFerroelectric CeramicsPiezoelectric ActuatorsPiezoelectric CeramicsPiezoelectric MaterialsCeramic Actuator MaterialsElectrical CeramicsHysteresisM ValueMultilayer ActuatorsMultilayer Piezoelectric ActuatorsMultilayer Piezoelectric CeramicsPolarization
In this study, 1.0 mol% CuO‐added (Na x K 1− x )NbO 3 ( CN x K 1− x N) ceramics with 0.0 ≤ x ≤ 0.5 were sintered at a relatively low temperature of 960°C. A large Q m value (≥1750) was obtained for the specimens with x ≤ 0.2 owing to the hardening effect of Cu 2+ ions, indicating that a large number of Cu 2+ ions had replaced Nb 5+ ions in these ceramics. The double polarization versus electric field ( P – E ) hysteresis loop was observed for the specimens with x ≤ 0.2, and was explained by the defect polarization ( P d ) formed between Cu 2+ ions and O 2− vacancies. These specimens also exhibited a sprout‐shaped strain versus electric field ( S – E ) curves with a large strain of 0.14%–0.15% at 8.0 kV/mm because of the internal bias field produced by P d . For the CN 0.2 K 0.8 N ceramic, a double P – E hysteresis loop was maintained at 125°C without remnant polarization. Moreover, this ceramic showed a large strain of 0.175% after 10 4 cycles when a high electric field of 8.0 kV/mm was continuously applied to the specimens during each cycles. Therefore, CN 0.2 K 0.8 N is a useful lead‐free piezoelectric ceramic for multilayer actuators.
28