在形磁体中的巨型和负磁电阻在不平衡的博尔兹曼方程方法中
Raz Rivlis1, Andrei Zadorozhnyi2, Yuri Dahnovsky1
1Department of Physics and Astronomy/3905, University of Wyoming, 1000 E. University Avenue, Laramie, WY 82071, United States of America.
Journal of physics. Condensed matter : an Institute of Physics journal
|September 27, 2024
概括
圆形直磁体中的磁传输显示出显著的自旋依赖磁电阻和霍尔效应. 这些由电子度变化驱动的特性表明,在基于旋转的电子设备中存在潜在的应用.
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
背景情况:
- 圆形的直磁体表现出复杂的磁性排序.
- 了解自旋依赖的运输现象对于自旋电子学至关重要.
研究的目的:
- 研究圆形海磁体晶体中的磁传输特性.
- 分析自旋依赖磁电阻和霍尔效应.
- 探索旋转开关装置中的潜在应用.
主要方法:
- 使用非平衡的博尔兹曼方程方法.
- 模拟了自旋向上和自旋向下电子传输.
- 分析了磁场和温度的影响.
主要成果:
- 由于载体密度增加,观察到自旋电子的负磁电阻.
- 发现了由载体枯竭引起的自转下方电子的巨大磁阻.
- 识别了巨大的霍尔电阻和消失的霍尔电流,用于在关键场中的自转下方电子.
- 发现了霍尔常数在磁场增加时自旋升电子的显著下降.
结论:
- 圆形直磁体表现出独特的自旋依赖的运输行为.
- 观察到的巨型磁阻和霍尔效应与载体密度调制有关.
- 这些材料对开发先进的旋转切换器件充满希望.
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