异常格子收缩和新出现的拓相在二替代的Sm2Ir2O7中
Prachi Telang1, Abhisek Bandyopadhyay2, Carlo Meneghini3
1Department of Physics, Indian Institute of Science Education and Research Pune, Dr. Homi Bhabha Road, Pashan, Pune 411008, Pune, MH, 411008, INDIA.
在Sm$_2$Ir$_2$O$_7$中替换 (Bi) 为 (Sm) 会导致异常格子收缩,并将材料转移到拓相. 这种过渡表明在韦尔半金属到二次金属带接触边界的量子临界点.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 材料科学 材料科学 材料科学
- 固态化学 固态化学
背景情况:
- 像Sm$_2$Ir$_2$O$_7$这样的火氧化物以异国情调的电子特性而闻名.
- 调节材料的组成可以改变电子相和晶格结构.
研究的目的:
- 为了研究在Sm$_2$Ir$_2$O$_7$中替换Bi为Sm对其晶体结构和电子特性的影响.
- 探索拓相的出现,特别是韦尔和二次带接触 (QBT),作为生物度的函数.
主要方法:
- 用于结构分析的同步粉X射线衍射 (XRD).
- 对于电子和局部结构的X射线近边缘精细结构 (XANES) 和扩展的X射线吸收精细结构 (EXAFS).
- 电阻,磁感应和热容量测量以探测电子行为.
主要成果:
- 观察到一个异常的晶格收缩,高达10%的Bi替代,随后是遵守维加德定律的扩张.
- 电阻测量显示了从1/T行为 (韦尔阶段) 过渡到-lnT依赖 (QBT阶段) 随着Bi含量增加.
- 中间组合表现出 $\rm 1/T^{1/4}$ 的缩放,表明接近量子临界点.
结论:
- 在Sm$_2$Ir$_2$O$_7$中石的替代导致结构异常和从韦尔半金属到QBT拓相的相变.
- 观察到的现象与这些拓相的边界处的潜在量子临界点有关.
- 这项研究突出了通过组合工程在火 iridates的拓电子状态的可调性.
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