磁性补偿点的不均电流驱动的形成和移位在变宽纳米级铁磁铁中
Maksim E Stebliy1, Michail A Bazrov1, Zhimba Zh Namsaraev1
1Laboratory of Spin-Orbitronics, Institute of High Technologies and Advanced Materials, Far Eastern Federal University, Vladivostok 690950, Russia.
ACS applied materials & interfaces
|August 18, 2023
概括
局部加热在铁磁材料中产生补偿状态,以便有效地切换磁化. 这一突破通过控制旋转纹理和域壁来实现先进的旋转电子和旋转轨道电子设备.
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
- 纳米技术 纳米技术
背景情况:
- 铁磁纳米结构提供高效的电流诱导磁化切换和稳定的旋转纹理 (例如, skyrmions).
- 这些属性通常与磁性或角动量补偿状态有关.
- 螺旋电子和螺旋轨道电子应用需要对这些状态进行精确的控制.
研究的目的:
- 用非均的朱尔加热来实验证明对补偿状态的局部实现.
- 为了研究局部加热对铁磁材料磁化切换的影响.
- 探索工程先进的纳米设备的潜力.
主要方法:
- 使用由W/Co76Tb24/Ru薄膜制成的可变宽度电流导体.
- 应用电流脉冲来诱导不均的朱尔加热并创建局部补偿温度.
- 观察共主导和Tb主导区域的共存及其对旋转轨道扭矩的反应.
主要成果:
- 局部加热补偿区域的位置显示出对当前脉冲振幅的线性依赖.
- 相反方向的旋转轨道扭矩的同时共存导致局部磁化切换.
- 尼尔域壁的位置靠近补偿点,但由于旋转电流的影响而变化.
结论:
- 不均的朱尔加热提供了一种有效的方法,可以在当地实现铁磁体中的补偿状态.
- 这种方法可以实现受控的局部磁化切换,并为旋转电子和旋转轨道电子设备工程提供新的途径.
- 这些发现为具有增强功能的新型纳米电子设备铺平了道路.
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