无机材料学报 ›› 2016, Vol. 31 ›› Issue (8): 850-854.DOI: 10.15541/jim20160038

• • 上一篇    下一篇

Ba(Ti0.96Sn0.04)O3陶瓷的物性研究

武燕庆, 张家良, 刘大康, 孙丹丹   

  1. (山东大学 物理学院, 晶体材料国家重点实验室, 济南 250100)
  • 收稿日期:2016-01-25 修回日期:2016-03-22 出版日期:2016-08-20 网络出版日期:2016-07-20
  • 作者简介:武燕庆(1986–), 女, 博士研究生. E-mail: wq20061010@126.com
  • 基金资助:
    国家自然科学基金重点项目(51172128);高等教育博士点基金(2013131110006)

Physical Properties of Ba(Ti0.96Sn0.04)O3 Ceramics

WU Yan-Qing, ZHANG Jia-Liang, LIU Da-Kang, SUN Dan-Dan   

  1. (School of physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, China)
  • Received:2016-01-25 Revised:2016-03-22 Published:2016-08-20 Online:2016-07-20
  • About author:WU Yan-Qing. E-mail: wq20061010@126.com
  • Supported by:
    National Natural Science Foundation of China (51172128 );Specialized Research Fund for the Doctoral Program of Higher Education (2013131110006)

摘要:

采用传统固相反应法制备了Ba(Ti0.96Sn0.04)O3无铅压电陶瓷, 对其压电性能、介电性能、铁电性能和微观结构等进行了研究。研究发现, 原料以及制备工艺对Ba(Ti0.96Sn0.04)O3陶瓷的压电性质具有较大的影响。与BaTiO3陶瓷相比, Ba(Ti0.96Sn0.04)O3陶瓷的正交-四方相变温度TO-T得到了一定的提高, 并且TO-T附近的热滞只有1.8℃。陶瓷的微观形貌呈现出较为复杂的畴结构, 主要以90°平行带状畴为主, 偶尔有少量不同构型的180°畴。电滞回线呈现为理想的近似矩形饱和形状的曲线, 剩余极化强度Pr为18.9 μC/cm2, 矫顽场Ec为 2.5 kV/cm。此外, 非180°畴的翻转是引起陶瓷逆压电常数d33*的主要因素, 其值可达550 pm/V。

关键词: Ba(Ti0.96Sn0.04)O3, 压电性能, 介电性能, 铁电性能, 微观结构

Abstract:

The Ba(Ti0.96Sn0.04)O3 ceramics were prepared through solid-state reaction route. Piezoelectric property, dielectric property, ferroelectric property, and microstructure were investigated. It is found that raw material and processing technique can largely affect the piezoelectric property of the Ba(Ti0.96Sn0.04)O3 ceramics. By comparing with the physical property of pure BaTiO3 ceramics, Sn doping significantly increases the transition temperature from orthorhombic phase to tetragonal phase (TO-T) of the Ba(Ti0.96Sn0.04)O3 ceramic to 36.9℃, while the thermal hysteresis at about TO-T is only 1.8℃. Its microstructure shows complicated domain, mainly composed of simple 90° parallel stripes with a few of different 180° configurations. P-E curve shows ideal square-like and saturated form with remanent polarization Pr of 18.9 μC/cm2 and coercive field Ec of 2.5 kV/cm. In addition, it is the non-180°-domain switching that leads large converse piezoelectric constant d33*, (up to 550 pm/V).

Key words: Ba(Ti0.96Sn0.04)O3, piezoelectric property, dielectric property, ferroelectric property, microstructure

中图分类号: