在3D铁磁铁磁铁中超快速去磁化的合原子自旋晶格模拟
M Pankratova1, I P Miranda2, D Thonig3,4
1Department of Physics and Astronomy, Uppsala University, Box 516, 75120, Uppsala, Sweden. maryna.pankratova@physics.uu.se.
Scientific reports
|April 7, 2024
概括
铁 (Fe) 和 (Co) 的超快速去磁化受到格子缓的影响,而不是明确的自旋格子合. 模拟证实了激光流动和去磁化之间的线性关系,与实验一致.
科学领域:
- 材料科学 材料科学 材料科学
- 凝聚物质物理学 凝聚物质物理学
- 计算物理 计算物理
背景情况:
- 尽管进行了广泛的研究,但晶格相互作用在超快去磁化中的作用仍然不清楚.
- 了解这些过程对于开发先进的磁性材料和技术至关重要.
研究的目的:
- 调查显式和隐式格子效应对bcc Fe和fcc Co.中的激光诱导超快去磁化的影响.
- 为了比较Fe和Co与Ni的去磁化动态,分析相似之处和差异.
主要方法:
- 原子自旋和格子动力学模拟采用热保三温度模型.
- 使用来自电子结构理论的参数,具有多种格子动态阻尼术语.
- 基于Langevin的模拟方法与实验趋势进行了验证.
主要成果:
- 显式自旋格子合显示对Fe和Co的去磁化影响很小.
- 格子阻尼显著影响了详细的磁化动态.
- 在所有模拟元素的激光流动和最大去磁状态之间观察到线性相关性.
- 脱磁幅度在Ni中最大,在Co中最小,与实验结果一致.
结论:
- 在超快速去磁化中,格子阻尼起着至关重要的作用,而在Fe和Co中,明确的自旋格子合不那么重要.
- 模拟模型准确地复制了对超快磁化动态的实验观测结果.
- 在Ni,Fe和Co的脱磁幅度中发现的趋势为材料设计提供了宝贵的见解.
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