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Three-magnon processes in magnetic nanoelements: Quantization and localized mode effects

机译:磁性纳米元素中的三磁子过程:量化和局部模式效应

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Three-magnon effects are known to be important for nonlinear processes in magnetic thin films. In such a process, for example, the uniform mode at a frequency ω can decay into two modes at a lower frequency ω/2. In magnetic nanoelements, there are additional concerns which do not occur in films. First, in small elements, the excitation wave vectors become a set of discrete values. This limits the availability of final states. Second, localized modes are important in nanoelements. Our study is based on micromagnetic calculations using the Landau-Lifshitz equations. We use an oscillating magnetic field at frequency to to drive the system and to study the response over a wide range of frequencies and for a wide set of input powers. In nanoelements, the typical response occurs not exactly at ω/2 but for several frequencies which are symmetrically spaced around ω/2. This is explained by the two considerations introduced above. We study the response both as a function of the amplitude of the driving field and as a function of the driving frequency. In this way, we can study the system response both at resonance and outside of resonance.
机译:已知三磁振效应对于磁性薄膜的非线性过程很重要。在这样的过程中,例如,频率为ω的均匀模式可衰减为频率为ω/ 2的两个模式。在磁性纳米元素中,存在薄膜中不存在的其他问题。首先,在小元件中,激发波矢量成为一组离散值。这限制了最终状态的可用性。其次,局部模式在纳米元素中很重要。我们的研究基于使用Landau-Lifshitz方程进行的微磁计算。我们使用频率上的振荡磁场来驱动系统,并研究在很宽的频率范围内以及对于广泛的输入功率的响应。在纳米元素中,典型的响应不完全在ω/ 2处发生,而是针对在ω/ 2附近对称间隔的几个频率。上面介绍的两个注意事项对此进行了解释。我们研究响应既是驱动场振幅的函数,也是驱动频率的函数。这样,我们可以研究共振时和共振外的系统响应。

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