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纳米厚YIG薄膜中交换扭矩诱导的垂直驻波自旋波激发

Exchange-torque-induced excitation of perpendicular standing spin waves in nanometer-thick YIG films.

作者信息

Qin Huajun, Hämäläinen Sampo J, van Dijken Sebastiaan

机构信息

NanoSpin, Department of Applied Physics, Aalto University School of Science, P.O. Box 15100, FI-00076, Aalto, Finland.

出版信息

Sci Rep. 2018 Apr 10;8(1):5755. doi: 10.1038/s41598-018-23933-y.

Abstract

Spin waves in ferrimagnetic yttrium iron garnet (YIG) films with ultralow magnetic damping are relevant for magnon-based spintronics and low-power wave-like computing. The excitation frequency of spin waves in YIG is rather low in weak external magnetic fields because of its small saturation magnetization, which limits the potential of YIG films for high-frequency applications. Here, we demonstrate how exchange-coupling to a CoFeB film enables efficient excitation of high-frequency perpendicular standing spin waves (PSSWs) in nanometer-thick (80 nm and 295 nm) YIG films using uniform microwave magnetic fields. In the 295-nm-thick YIG film, we measure intense PSSW modes up to 10th order. Strong hybridization between the PSSW modes and the ferromagnetic resonance mode of CoFeB leads to characteristic anti-crossing behavior in broadband spin-wave spectra. We explain the excitation of PSSWs by exchange coupling between forced magnetization precessions in the YIG and CoFeB layers. If the amplitudes of these precessions are different, a dynamic exchange torque is generated, causing the emission of spin waves from the interface. PSSWs form when the wave vector of the spin waves matches a perpendicular confinement condition. PSSWs are not excited if exchange coupling between YIG and CoFeB is eliminated by a 10 nm Ta spacer layer. Micromagnetic simulations confirm the exchange-torque-driven mechanism.

摘要

具有超低磁阻尼的亚铁磁性钇铁石榴石(YIG)薄膜中的自旋波与基于磁振子的自旋电子学和低功耗波状计算相关。由于其饱和磁化强度较小,YIG中自旋波在弱外磁场中的激发频率相当低,这限制了YIG薄膜在高频应用中的潜力。在此,我们展示了与CoFeB薄膜的交换耦合如何利用均匀微波磁场在纳米厚(80纳米和295纳米)的YIG薄膜中实现高频垂直驻波自旋波(PSSW)的高效激发。在295纳米厚的YIG薄膜中,我们测量到了高达十阶的强烈PSSW模式。PSSW模式与CoFeB的铁磁共振模式之间的强杂化导致了宽带自旋波谱中的特征性反交叉行为。我们通过YIG和CoFeB层中受迫磁化进动之间的交换耦合来解释PSSW的激发。如果这些进动的幅度不同,就会产生动态交换转矩,导致自旋波从界面发射。当自旋波的波矢满足垂直限制条件时,PSSW就会形成。如果通过10纳米的Ta间隔层消除YIG和CoFeB之间的交换耦合,PSSW就不会被激发。微磁模拟证实了交换转矩驱动机制。

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