在f电子金属中统一的高压相变序列:oF16→oF8在中的过渡
C V Storm1, S E Finnegan1, J D McHardy1
1The University of Edinburgh, SUPA, School of Physics and Astronomy, and Centre for Science at Extreme Conditions, Peter Guthrie Tait Road, Edinburgh EH9 3FD, United Kingdom.
Physical review letters
|October 12, 2025
概括
在极端压力下, (Tb) 从独特的16原子正方形结构 (oF16) 转变为8原子正方形结构 (oF8). 这一发现结合了之前分开的在压力下兰化物相位过渡序列.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学是一种材料科学.
- 高压物理学的高压物理
背景情况:
- 兰化物元素在压缩下表现出复杂的结构相变.
- 最近的研究发现了两个不同的过渡序列:低Z (Nd,Sm) 与oF8和高Z (Gd,Tb,Dy,Ho) 具有独特的oF16结构.
- 没有观察到任何单一的兰坦化物元素同时表现出oF8和oF16结构.
研究的目的:
- 在高压下研究 (Tb) 的结构演变.
- 要确定Tb是否在oF16和oF8结构之间呈现过渡.
- 为了统一理解压力下的兰化物相位过渡.
主要方法:
- 在高压中对高达308GPa的 (Tb) 进行高压衍射研究.
- 理论计算以确认结构阶段的能量有利性.
- 结构阶段过渡及其序列的分析.
主要成果:
- 观察到 (Tb) 在234 GPa时从oF16结构过渡到oF8结构.
- 在Tb的oF8阶段保持稳定,至少达到308GPa.
- 理论结果证实了oF8阶段在280 GPa以上变得能量有利.
结论:
- 在Tb中观察到的oF16→oF8过渡连接了之前识别的两种兰化物相位过渡序列.
- 这一发现表明,在压力下,类元素的通用过渡路径 (oF16→oF8→oC4→tI2).
- 这项研究统一了对整个兰坦化物系列的高压结构行为的理解.
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