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用太赫兹频率脉冲对铁磁/反铁磁双层膜中的磁化反转进行模拟。

Simulations of magnetization reversal in FM/AFM bilayers with THz frequency pulses.

作者信息

Hirst Joel, Ruta Sergiu, Jackson Jerome, Ostler Thomas

机构信息

Materials & Engineering Research Institute, Sheffield Hallam University, Howard Street, Sheffield, S1 1WB, UK.

The Department of Engineering and Mathematics, Sheffield Hallam University, Howard Street, Sheffield, S1 1WB, UK.

出版信息

Sci Rep. 2023 Jul 28;13(1):12270. doi: 10.1038/s41598-023-39175-6.

Abstract

It is widely known that antiferromagnets (AFMs) display a high frequency response in the terahertz (THz) range, which opens up the possibility for ultrafast control of their magnetization for next generation data storage and processing applications. However, because the magnetization of the different sublattices cancel, their state is notoriously difficult to read. One way to overcome this is to couple AFMs to ferromagnets-whose state is trivially read via magneto-resistance sensors. Here we present conditions, using theoretical modelling, that it is possible to switch the magnetization of an AFM/FM bilayer using THz frequency pulses with moderate field amplitude and short durations, achievable in experiments. Consistent switching is observed in the phase diagrams for an order of magnitude increase in the interface coupling and a tripling in the thickness of the FM layer. We demonstrate a range of reversal paths that arise due to the combination of precession in the materials and the THz-induced fields. Our analysis demonstrates that the AFM drives the switching and results in a much higher frequency dynamics in the FM due to the exchange coupling at the interface. The switching is shown to be robust over a broad range of temperatures relevant for device applications.

摘要

众所周知,反铁磁体(AFM)在太赫兹(THz)范围内表现出高频响应,这为下一代数据存储和处理应用中对其磁化强度进行超快控制开辟了可能性。然而,由于不同亚晶格的磁化强度相互抵消,其状态极难读取。克服这一问题的一种方法是将反铁磁体与铁磁体耦合,铁磁体的状态可通过磁阻传感器轻松读取。在此,我们通过理论建模给出条件,即使用具有适度场振幅和短持续时间的太赫兹频率脉冲,在实验中是可以实现切换反铁磁体/铁磁体(AFM/FM)双层的磁化强度的。在相图中观察到,当界面耦合增加一个数量级且铁磁层厚度增加两倍时,会出现一致的切换。我们展示了一系列由于材料中的进动和太赫兹诱导场的组合而产生的反转路径。我们的分析表明,由于界面处的交换耦合,反铁磁体驱动了切换,并导致铁磁体中出现更高频率的动力学。结果表明,在与器件应用相关的广泛温度范围内,这种切换具有鲁棒性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/f81a/10382508/24f8e1f194f5/41598_2023_39175_Fig1_HTML.jpg

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