在 Nd-doped Bi1.1Sb0.9STe2的拓绝缘体单晶中出现异常的霍尔效应
Lei Chen1, Weiyao Zhao2, Kaijian Xing3
1School of Physics and Materials Science, Guangzhou University, Guangzhou 510006, China. zrk@ustc.edu.
Physical chemistry chemical physics : PCCP
|January 4, 2024
概括
在拓绝缘器中使用稀土元素的兴奋剂使铁磁排序成为可能,为量子异常霍尔效应研究铺平了道路. 这项研究探讨了Nd-doped Bi$_{1.1}$Sb$_{0.9}$STe$_{2}$用于先进的量子运输和旋转子应用.
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
- 量子现象是一种量子现象.
背景情况:
- 拓绝缘体具有独特的表面状态,由对称性保护.
- 量子异常霍尔效应 (QAHE) 是在磁拓绝缘体中观察到的关键现象.
- 实现强大的磁性排序对于实现QAHE至关重要.
研究的目的:
- 在散装绝缘型拓绝缘体单晶体中引入铁磁排序.
- 为了研究被杂的拓绝缘体的电子传输特性.
- 探索量子运输和自旋电子学的潜在应用.
主要方法:
- 用稀土元素 (Nd) 的单晶生物化.
- 磁性排序及其温度依赖性的特征.
- 测量电子传输特性,包括舒布尼科夫-德哈斯振荡.
主要成果:
- 在成功地将Nd化为Bi$_{1.1}$Sb$_{0.9}$STe$_{2}$后,铁磁性约为100K左右.
- 在铁磁体制中观察到由拓表面状态主导的电子运输.
- 在低温下检测到Shubnikov-de Haas振荡,呈现出非碎的Berry阶段.
结论:
- Nd-doped Bi$_{1.1}$Sb$_{0.9}$STe$_{2}$单晶为研究磁拓绝缘体提供了一个有前途的平台.
- 观察到的现象支持量子运输研究和旋转器件应用的潜力.
- 这些兴奋剂材料的远程磁性排序是它们独特电子性质的关键.
更多相关视频
05:39Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
9.6K
09:06Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
Published on: March 24, 2019
8.1K
相关概念视频
Imperfections in Crystal Structure: Stoichiometric Point Defects
Schottky defects arise when some lattice points in a crystal, such as those in NaCl, remain unoccupied, creating lattice vacancies without disturbing the overall electrical neutrality of the crystal. This defect is common in ionic crystals where the positive and negative ions are similar in size, as seen in sodium chloride and cesium chloride. The presence of Schottky defects enables the crystal to conduct electricity to a small extent through an ionic mechanism. Electric fields cause nearby...
The Hall Effect
Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
