2D完全补偿铁磁体中的超快旋转动力学:一个时间依赖的Ab Initio研究
Shuo Li1, Ran Wang1, Thomas Frauenheim1,2
1Institute for Advanced Study, Chengdu University, Chengdu 610106, China.
The journal of physical chemistry letters
|October 17, 2025
概括
完全补偿的铁磁体 (CFiM) 在激光激发时表现出暂时的净磁化. 这项研究揭示了用于自旋电子应用的2D Janus CFiM中的超快自旋动力学机制.
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
- 量子化学 是一个量子化学.
背景情况:
- 完全补偿的铁磁体 (CFiM) 提供零净磁化和高旋转极化,这对于旋转电子学至关重要.
- 贾努斯材料具有破碎的反向对称性,使其具有独特的电子和磁性质.
研究的目的:
- 在2D Janus NiICl双层中研究超快激光诱导的自旋动力学.
- 阐明CFiMs中短暂磁化背后的机制.
主要方法:
- 实时的时间依赖密度函数理论 (rt-TDDFT) 模拟.
- 分析超快激光诱导的去磁化和旋转转移.
主要成果:
- 观察到在50 fs以内不对称的中间层去磁化.
- 确定了不对称的电荷积累和光学诱导的旋转转移 (OISTR) 作为关键机制.
- 证明了由于不对称的层间相互作用造成的过渡性铁磁状态的形成.
结论:
- 2D Janus CFiMs的内在不对称性在激光照射下驱动超快自旋动力学.
- 不对称的层间相互作用是暂时磁化的原因.
- 这项研究提供了对2D CFiMs中用于先进的自旋电子设备的超快自旋动力学规则的微观机制的洞察.
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