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The relative contribution of ferroelastic and ferroelectric texture to the character of a hard PZT ceramic.

机译:铁弹性和铁电织构对硬质PZT陶瓷性能的相对贡献。

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摘要

The development of ferroelastic (90°) texture in addition to ferroelectric (180°) texture is essential to maximizing the piezoelectric properties of many hard tetragonal PZTs, including Piezoetechnologies K270. Ferroelastic texture results from motion of domain walls that is dependent on an individual crystals orientation. Increases in ferroelastic texture raises the maximum net polarization that can be achieved by changes in ferroelectric texture. By studying a hard PZT poled under various temperature conditions, insight was gained into factors affecting the development of ferroelastic texture and how ferroelastic texture contributes to piezoelectric properties. Depinning proved to be the major barrier to preventing ferroelastic domain wall motion where strain based domain interactions and polar defect complexes on the domain level appear to be the dominant factors. Insight into the affect of increased domain texture on the relationship between the increasing magnitude of the remnant polarization (|Pr|) and the magnitude of the coercive field (|EC|) was gained by plotting |EC| vs. |Pr| as a function of poling time for a variety of poling temperatures. At low |Pr| values, |EC| increased rapidly as a function of increases in |Pr| regardless of the poling temperature. This relationship was characteristic of samples poled at 25 °C where increases in ferroelastic texture were largely suppressed. Because increases in polarization were still observable changes in ferroelectric texture most responsible for the polarization increase and like play a strong role in the initial |EC| vs. |Pr| relationship. As |Pr| increased beyond 5 to 8 iC/cm2, the slope of |EC| vs. |Pr| decreased where the reduction in slope increased with poling temperature. This only occurred in samples poled at elevated temperatures where ferroelastic texture was know to ultimately develop during the poling process, leading to the suggestion that the change in slope was due to increases in combined ferroelectric and ferroelastic texture. Lastly, it was found that electric field induced increases in ferroelectric texture by poling at 25 °C occurs while ferroelastic domain wall motion is largely suppressed. This change in ferroelectric texture severely hinders the rate at which subsequent ferroelastic domain wall motion can be induced during poling at elevated temperatures below TC, suggesting that hard PZT samples should be preheated to the poling temperature before poling begins.
机译:除铁电(180°)织构外,铁弹性(90°)织构的发展对于最大限度地提高许多硬四方PZT(包括Piezoetechnologies K270)的压电性能至关重要。铁弹性织构是由于畴壁的运动而产生的,而畴壁的运动取决于单个晶体的取向。铁弹性织构的增加提高了最大的净极化,这可以通过改变铁电织构来实现。通过研究在不同温度条件下极化的硬质PZT,可以洞悉影响铁弹性织构发展的因素以及铁弹性织构如何有助于压电性能。事实证明,去钉化是阻止铁弹性畴壁运动的主要障碍,其中基于应变的畴相互作用和畴水平上的极性缺陷复合物似乎是主要因素。通过绘制| EC |,可以了解增加的畴纹理对剩余极化强度(| Pr |)的增加与矫顽场强度(| EC |)之间的关系的影响。与| Pr |对于各种极化温度,它是极化时间的函数。低| Pr |值,| EC | | Pr |的增加迅速增加不管极化温度如何。这种关系是在25°C极化的样品的特征,在该样品中铁弹性织构的增加被大大抑制了。因为极化仍是可观察到的,铁电织构的变化仍然是可观察到的,而这种变化是导致极化增加的最主要原因,并且在初始| EC |中起着重要的作用。与| Pr |关系。作为| Pr |增加到5至8 iC / cm2以上,| EC |的斜率与| Pr |坡度的降低随极化温度的增加而降低。这仅在极化后的样品中发生,已知在极化过程中铁弹性组织最终会发展,这表明斜率的变化是由于铁电和铁弹性组织的增加所致。最后,发现在25℃下通过极化产生的电场诱导的铁电织构的增加在很大程度上抑制铁弹性畴壁运动的同时发生。铁电织构的这种变化严重阻碍了在低于TC的高温下极化过程中随后的铁弹性畴壁运动的诱导速率,这表明在极化开始之前应将硬质PZT样品预热到极化温度。

著录项

  • 作者

    Key, Thomas Stallings.;

  • 作者单位

    Purdue University.;

  • 授予单位 Purdue University.;
  • 学科 Engineering Materials Science.
  • 学位 Ph.D.
  • 年度 2007
  • 页码 95 p.
  • 总页数 95
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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