在奇拉非线性变磁体中的Spin Hall和Edelstein效应
Mengli Hu1, Oleg Janson1, Claudia Felser2
1Leibniz Institute for Solid State and Materials Research, IFW Dresden, Dresden, Germany.
Nature communications
|September 26, 2025
概括
新发现的性变磁体表现出独特的旋转纹理和运输现象,与传统的旋转电子学不同. 这项研究确定了这些材料中的新型多极顺序参数,用于先进的自旋电子应用.
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
- 这就是Spintronics.
背景情况:
- 变磁体是磁相,具有铁磁旋极化和反铁磁净磁化.
- 变磁的概念,最初是用于对线结构,现在包括非对线系统.
- 兰道理论与旋转空间对称度有助于识别对直线变磁体.
研究的目的:
- 扩展兰道理论对对线性替代磁体,以确定非对线性奇拉材料中的替代磁多极顺序参数.
- 探索非对线性反磁性和奇拉性之间的独特相互作用.
- 为了预测这些现象的实验特征在性变磁体中.
主要方法:
- 兰道理论的扩展,将非线性性替代磁体纳入.
- 玩具模型和第一原则计算的应用.
- 使用奇拉拓磁性材料Mn3IrSi.Si.的案例研究.
主要成果:
- 在非对线性性材料中识别变磁多极顺序参数.
- 空间奇异的多极元件的演示,由于变磁性-奇拉性相互作用.
- 预测非微不足道的费米表面旋转纹理和新型运输现象 (例如,大型旋转霍尔和埃德尔斯坦效应),即使没有旋转轨道合 (SOC).
结论:
- 与SOC驱动的效应相比,状变磁体具有从根本上不同的自旋电磁特性.
- 在Mn3IrSi中预测了巨大的旋转霍尔和埃德尔斯坦效应,此前在替代磁体中没有观察到.
- 这些发现为利用奇拉变磁特征的自旋电子应用开辟了新的途径.
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