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Induced magnetization and power loss for a periodically driven system of ferromagnetic nanoparticles with randomly oriented easy axes

机译:具有随机取向易轴的铁磁纳米粒子周期性驱动系统的感应磁化和功率损耗

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We study the effect of an elliptically polarized magnetic field on a system of noninteracting, single-domain ferromagnetic nanoparticles characterized by a uniform distribution of easy axis directions. Our main goal is to determine the average magnetization of this system and the power loss in it. In order to calculate these quantities analytically, we develop a general perturbation theory for the Landau-Lifshitz-Gilbert (LLG) equation and find its steady-state solution for small magnetic field amplitudes. On this basis, we derive the second-order expressions for the average magnetization and power loss, investigate their dependence on the magnetic field frequency, and analyze the role of subharmonic resonances resulting from the nonlinear nature of the LLG equation. For arbitrary amplitudes, the frequency dependence of these quantities is obtained from the numerical solution of this equation. The impact of transitions between different regimes of regular and chaotic dynamics of magnetization, which can be induced in nanoparticles by changing the magnetic field frequency, is examined in detail.
机译:我们研究了椭圆极化磁场对以互作用轴方向均匀分布为特征的非相互作用单畴铁磁纳米粒子系统的影响。我们的主要目标是确定该系统的平均磁化强度和其中的功率损耗。为了分析性地计算这些量,我们针对Landau-Lifshitz-Gilbert(LLG)方程开发了一种通用摄动理论,并针对较小的磁场振幅找到了其稳态解。在此基础上,我们推导了平均磁化强度和功率损耗的二阶表达式,研究了它们对磁场频率的依赖性,并分析了由LLG方程的非线性性质导致的次谐波共振的作用。对于任意振幅,这些量的频率相关性可从该方程的数值解获得。详细研究了通过改变磁场频率可以在纳米颗粒中引起的不同规律的磁化动力学和混沌动力学之间的过渡所产生的影响。

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