...
首页> 外文期刊>Journal of Applied Physics >Statistical electric field and switching time distributions in PZT 1Nb2Sr ceramics: Crystal- and microstructure effects
【24h】

Statistical electric field and switching time distributions in PZT 1Nb2Sr ceramics: Crystal- and microstructure effects

机译:PZT 1Nb2Sr陶瓷的统计电场和转换时间分布:晶体和微观结构的影响

获取原文
获取原文并翻译 | 示例
           

摘要

Dispersive polarization response of ferroelectric PZT ceramics is analyzed assuming the inhomogeneous field mechanism of polarization switching. In terms of this model, the local polarization switching proceeds according to the Kolmogorov-Avrami-Ishibashi scenario with the switching time determined by the local electric field. As a result, the total polarization reversal is dominated by the statistical distribution of the local field magnitudes. Microscopic parameters of this model (the high-field switching time and the activation field) as well as the statistical field and consequent switching time distributions due to disorder at a mesoscopic scale can be directly determined from a set of experiments measuring the time dependence of the total polarization switching, when applying electric fields of different magnitudes. PZT 1Nb2Sr ceramics with Zr/Ti ratios 51.5/48.5, 52.25/47.75, and 60/40 with four different grain sizes each were analyzed following this approach. Pronounced differences of field and switching time distributions were found depending on the Zr/Ti ratios. Varying grain size also affects polarization reversal parameters, but in another way. The field distributions remain almost constant with grain size whereas switching times and activation field tend to decrease with increasing grain size. The quantitative changes of the latter parameters with grain size are very different depending on composition. The origin of the effects on the field and switching time distributions are related to differences in structural and microstructural characteristics of the materials and are discussed with respect to the hysteresis loops observed under bipolar electrical cycling.
机译:假定极化转换的场机制不均匀,分析了铁电PZT陶瓷的色散极化响应。根据该模型,局部极化切换根据Kolmogorov-Avrami-Ishibashi场景进行,切换时间由局部电场确定。结果,总极化反转由局部场大小的统计分布决定。该模型的微观参数(高场切换时间和激活场)以及统计场和由介观尺度引起的无序状态导致的切换时间分布可以直接从一组测量时间依赖性的实验中确定。当施加不同大小的电场时,总极化切换。按照该方法分析了Zr / Ti比为51.5 / 48.5、52.25 / 47.75和60/40的PZT 1Nb2Sr陶瓷,每种陶瓷具有四种不同的晶粒尺寸。根据Zr / Ti比,发现了场和切换时间分布的明显差异。晶粒尺寸的变化也会影响极化反转参数,但这是另一种方式。场分布随晶粒尺寸几乎保持恒定,而开关时间和激活场往往随晶粒尺寸的增加而减小。后者参数随晶粒尺寸的定量变化取决于组成。对磁场和转换时间分布的影响的起因与材料的结构和微观结构特征的差异有关,并针对双极性电循环下观察到的磁滞回线进行了讨论。

著录项

  • 来源
    《Journal of Applied Physics》 |2014年第1期|1-13|共13页
  • 作者单位

    Institut für Materialwissenschaft, Technische Universität Darmstadt, Alarich-Weiss-Straße 2, 64287 Darmstadt, Germany|c|;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号