在ZrO2纳米晶体中,铁弹性保护的可逆的形到单临床类相位过渡
Xinyan Li1,2, Zhuohui Liu1,2, Ang Gao3
1Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, China.
Nature materials
|April 8, 2024
概括
铁电化氧化物由于相位过渡而降解. 这项研究表明,铁弹性切换保护ZrO2纳米晶体的可逆相变,但拉伸应变可以导致不可逆转的铁电损失.
科学领域:
- 材料科学 材料科学 材料科学
- 凝聚物质物理学 凝聚物质物理学
- 纳米技术纳米技术
背景情况:
- 纳米尺度化物氧化物中的铁电是兼容器件的关键.
- 转移稳定的极极 (O) 阶段可以降解为非极极单临床 (M) 阶段.
研究的目的:
- 研究ZrO2纳米晶体中O-M相变的可逆性.
- 了解控制铁电降解的原子尺度机制.
主要方法:
- 在现场原子尺度可视化相位过渡.
- 分析马氏体转化路径.
- 应变工程和表征.
主要成果:
- 通过铁电-铁弹性切换识别了一条可逆的剪切变形路径 (O到单临床类型的M').
- 发现M'状态中累积的拉伸应变可以不可逆转地固定铁弹性域.
- 确定了导致铁电降解的关键拉伸应变值.
结论:
- 铁弹性切换在化氧化物中相变的可逆性中起着至关重要的作用.
- 拉力应变是限制元稳定铁电相稳定的关键因素.
- 结果为先进的电子应用提供了氧化物薄膜中稳定铁电的见解.
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