无机材料学报 ›› 2012, Vol. 27 ›› Issue (11): 1228-1232.DOI: 10.3724/SP.J.1077.2012.12325

• 研究快报 • 上一篇    

铁酸镧掺杂对铌酸钾钠基陶瓷介电和铁电性能的影响

程花蕾, 杜红亮, 周万城, 罗 发, 朱冬梅   

  1. (西北工业大学 材料科学与工程学院, 凝固技术国家重点实验室, 西安 710072)
  • 收稿日期:2012-05-18 修回日期:2012-06-06 出版日期:2012-11-20 网络出版日期:2012-10-25
  • 基金资助:

    Doctorate Foundation of Northwestern Polytechnical University (CX201108); National Natural Science Foundation of China (51072165); State Key Laboratory of Solidification Processing in NWPU (KP200901)

Effects of LaFeO3 Additions on the Dielectric and Ferroelectric Properties of (K0.5Na0.5)NbO3 Ceramics

CHENG Hua-Lei, DU Hong-Liang, ZHOU Wan-Cheng, LUO Fa, ZHU Dong-Mei   

  1. (State Key Laboratory of Solidification Processing, School of Materials Science and Engineering, Northwestern Polytechnical University, Xi’an 710072, China)
  • Received:2012-05-18 Revised:2012-06-06 Published:2012-11-20 Online:2012-10-25
  • Supported by:

    Doctorate Foundation of Northwestern Polytechnical University (CX201108); National Natural Science Foundation of China (51072165); State Key Laboratory of Solidification Processing in NWPU (KP200901)

摘要: 用传统固相反应法制备了(K0.5Na0.5)NbO3(KNN)和0.98(K0.5Na0.5)NbO3-0.02LaFeO3(0.98KNN-0.02LF)无铅陶瓷, 并对其介电、铁电性质以及相结构进行了研究. KNN陶瓷是正交相, 0.98KNN-0.02LF陶瓷是伪立方相结构. 介电研究表明: 0.98KNN-0.02LF 陶瓷的介温曲线与KNN陶瓷相比较出现两点异常: (i)正交相–四方相相变温度(TO-T)和四方 相–立方相相变温度(TT-C)均降低; (ii)最高介电常数温度Tm附近的相变温度宽化. 并且, 0.98KNN-0.02LF陶瓷在0~400℃内显示了相对比较平坦的介电常数, 介电常数达到2000, 介电损耗低于4%. 电滞回线变“窄”进一步证明了0.98KNN-0.02LF陶瓷的弛豫性.

关键词: 铌酸钾钠, 介电性能, 铁电性能, 弛豫性质, 无铅陶瓷

Abstract: Pure (K0.5Na0.5)NbO3 and 0.98(K0.5Na0.5)NbO3-0.02LaFeO3 ceramics (abbreviated as KNN and 0.98KNN-0.02LF, respectively) were prepared by a solid state reaction approach, and their crystal structure, dielectric and ferroelectric properties were investigated. Pure KNN and 0.98KNN-0.02LF ceramics are the orthorhombic structure and pseudo-cubic perovskite structure, respectively. Dielectric measurements revealed that the dielectric permittivity curves of 0.98KNN-0.02LF ceramics present two anomalies compared with pure KNN: (i) The orthorhombic- tetragonal transition (TO-T) and the tetragonal-cubic transition (TT-C) shifts to lower temperatures. (ii) The phase transition temperature range around the temperature of the maximum dielectric permittivity (Tm) becomes more and more broad. In addition, 0.98KNN-0.02LF ceramics exhibited a very stable temperature dependence of dielectric permittivity with permittivity maximum near 2000 and dielectric loss less than 4% in the temperature range of 0–400℃. The relaxation behavior of the 0.98KNN-0.02LF ceramics is interpreted in terms of polar nanoregions (PNRs) caused by cations disorder. The P-E hysteresis loops further confirms the relaxor behavior in 0.98KNN-0.02LF ceramics.

Key words: (K0.5Na0.5)NbO3, dielectric properties, ferroelectric properties, relaxor properties, lead-free ceramics

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