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Field dependence of the magnetic eigenmode frequencies in layered nanowires with ferromagnetic and antiferromagnetic ground states: experimental and theoretical study

机译:具有铁磁和反铁磁基态的层状纳米线中本征模式频率的磁场依赖性:实验和理论研究

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摘要

The magnetic field dependence of the magnetic eigenmode frequencies in 150 nm wide layered permalloy nanowires (NWs) has been studied by the Brillouin light scattering technique. The NWs have the following layering structure Py(30 nm)/Cu(10 nm)/Py(d)/Cu(10 nm)/Py(30 nm) with fixed thickness of the top and bottom stripe and differ by the thickness d of the middle Py stripe (with d = 15, 30, 60 nm). The magnetic field, applied along the length of the wires, has been swept from positive to negative saturation thus exploring both the ferromagnetic and the antiferromagnetic relative orientation of the magnetization in the middle stripe with respect to the outermost ones. In conjunction with the transition between the two different ground states, the mode frequencies undergo an abrupt variation. Moreover the mode frequencies in the antiferromagnetic state are relatively insensitive to the applied field strength. The experimental results (frequencies versus magnetic field strength) have been successfully interpreted by means of a microscopic (Hamiltonian-based) theory which incorporates both the exchange and dipole-dipole interactions as well as effects of single-ion anisotropy and an external magnetic field applied parallel to the NW axis. This model was extended to account for parallel and antiparallel magnetization orientations in the layered NWs, enabling us to also calculate the probability amplitude of each spin-wave eigenmode at any position in the trilayered NWs.
机译:通过布里渊光散射技术研究了150 nm宽的层状坡莫合金纳米线(NWs)中本征模频率的磁场依赖性。 NW具有以下分层结构Py(30 nm)/ Cu(10 nm)/ Py(d)/ Cu(10 nm)/ Py(30 nm),顶部和底部条纹的厚度固定,并且厚度d中间Py条纹的宽度(d = 15、30、60 nm)。沿着导线长度施加的磁场已从正饱和扫荡到负饱和,因此探索了中间条相对于最外面条的磁化强度的铁磁和反铁磁相对方向。结合两个不同基态之间的过渡,模式频率会发生突变。此外,处于反铁磁状态的模式频率对施加的场强相对不敏感。实验结果(频率与磁场强度)已通过微观(基于哈密顿理论)理论成功解释,该理论结合了交换和偶极-偶极相互作用以及单离子各向异性和施加的外部磁场的影响平行于NW轴。扩展了该模型,以考虑分层NW中平行和反平行的磁化方向,使我们能够计算三层NW中任意位置处每个自旋波本征模的概率振幅。

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