在kagome金属FeGe中竞争的巡回和局部自旋相互作用
Lebing Chen1, Xiaokun Teng1, Hengxin Tan2
1Department of Physics and Astronomy, Rice University, Houston, TX, 77005, USA.
Nature communications
|March 1, 2024
概括
二维卡戈梅金属FeGe表现出复杂的磁相. 中子散射揭示了与其双反铁磁结构相关的无间隙自旋激发,来自嵌套的费米表面和自旋密度波序.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子材料是一种量子材料.
- 磁力学 磁力学 是一种
背景情况:
- 二维卡戈梅金属具有几何挫折格子和类似的能量尺度,导致丰富的量子相.
- 甲基金属FeGe显示了连续的磁顺序:A型反铁磁 (AFM) 顺序,电荷密度波 (CDW) 阶段,以及双 AFM 结构.
研究的目的:
- 为了研究卡戈梅金属FeGe.Ge.中的自旋刺激的性质.
- 阐明磁性结构与电子性质之间的关系.
- 为了了解不相称的磁结构的起源.
主要方法:
- 中子散射实验被用来探测旋转激发.
- 密度函数理论 (DFT) 的计算用于理论分析.
- 对自旋波行为及其温度依赖性的分析.
主要成果:
- 在双 AFM 过渡温度以上观察到无间隙不相称的旋转激发.
- 这些刺激合并为与A型AFM顺序相关的间隙相称旋转波.
- 不相称的旋转刺激表现出关键的散射行为,与二次磁性相位过渡相一致.
结论:
- 在FeGe中,不相称的磁性结构来自于旅行电子的嵌套费米表面.
- 旋转密度波序的形成被确定为这些激发背后的机制.
- 中子散射为卡戈梅金属中的磁性秩序和电子结构的复杂相互作用提供了关键的见解.
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