在室温性磁铁中进行非互惠的传输
Daisuke Nakamura1, Mu-Kun Lee2, Kosuke Karube1
1RIKEN Center for Emergent Matter Science (CEMS), Wako 351-0198, Japan.
Science advances
|July 4, 2025
概括
奇拉磁体由于时间逆向对称性被打破而表现出非互惠的传输. 这项研究确定了旋转波动散射和带不对称性作为Co8Zn9Mn3中的关键机制,将它们在磁相中的贡献分开.
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
- 这就是Spintronics.
背景情况:
- 带有时间逆向对称性破裂的状磁铁表现出非互换传输,这是一个电子流被纠正的现象.
- 现有的理论提出了诸如旋转波动散射和带不对称等机制,但在单一材料内缺乏明确的识别.
研究的目的:
- 为了研究和区分在奇拉磁体Co8Zn9Mn3.3中对非互惠传输的贡献.
- 为各种磁相和温度的识别机制提供全面的理论描述.
主要方法:
- 在Co8Zn9Mn3的磁相图上对非相互传输现象的实验研究.
- 使用理论计算来分离和识别非相互电阻的基本机制.
主要成果:
- 观察到非相互传输的明显的场和温度依赖性,这表明了多种促成因素.
- 成功地将非相互电阻分为归因于旋转波动诱导的性散射和带不对称的组件.
结论:
- Co8Zn9Mn3 作为理解复杂的非互惠运输的模型系统.
- 这项研究澄清了旋转波动和带不对称性在奇拉磁体中的作用,进步了对旋转电子现象的理解.
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