在非对线反铁磁铁中,电流驱动的快速磁性八极域壁运动在非对线反铁磁铁中
Mingxing Wu1,2, Taishi Chen1,3,4, Takuya Nomoto5
1The Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba, 277-8581, Japan.
Nature communications
|June 11, 2024
概括
研究人员使用电流在抗铁磁体 (AFM) 中展示了快速的磁性八极域壁运动. 在控制AFM方面取得的这一突破为新型自旋电子设备提供了潜力.
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:
- 抗铁磁铁 (AFM) 提供诸如太赫兹旋转动力学和域墙应用的最小迷路场等优势.
- 由于其不敏感的磁电反应,控制设备中的AFM具有挑战性.
- 非线性性AFM,如Mn3X,允许检测和操纵磁性八极管域状态.
研究的目的:
- 为了证明电流驱动的磁性八极管域壁 (MODW) 运动在Mn3X.
- 研究MODWs在这些材料中的动态和移动性.
- 将旋转扭矩理论扩展到非对线磁系统.
主要方法:
- 使用磁光克尔效应显微镜观察MODW运动.
- 将受控电流密度应用于Mn3Ge样本.
- 开发了用于旋转扭矩驱动的域壁动态的理论模型.
主要成果:
- 在Mn3Ge中实现了快速的Neel-like MODW运动,达到750 m/s的速度.
- 观察到高 MODW 流动性与低临界电流密度 (7.56 × 10^10 A m^-2).
- 在不需要外部磁场的情况下证明了运动.
结论:
- 电流驱动的MODW运动是可行的,并且在非对线性性反铁磁体中非常高效.
- 这项研究为基于反铁磁域壁的自旋电子应用开辟了新的途径.
- 这些发现为利用AFM独特特性开发新型设备概念铺平了道路.
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