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Regular and Stochastic Nonlinear Dynamics of Magnetization in an Exchange-Coupled Multilayer Structure

机译:交换耦合多层结构中磁化的规则和随机非线性动力学

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Various oscillating systems with both stochastic and regular dynamical regimes have attracted wide attention in recent years [1]. Among the most studied of such systems are magnetically ordered structures whose dynamics is associated with the precession motion of magnetization and is generally described by the Lan-dau-Lifshitz nonlinear equations [2, 3]. Of great interest today are multilayer exchange-coupled structures, where giant rnagnetoresistive and magnetooptical effects have been discovered [4-6]. The existence of static and dynamical bistable states characteristic of a magnetic subsystem is substantial for the practical use of such structures [7, 8]. The behavior of the magnetic subsystem near these states determines the features of the self-organization of magnetization, which proceeds in external magnetic fields [9]. In this work, we analyze dynamical regimes of the magnetization of a multilayer nanostructure with an antiferromagnetic interlayer exchange coupling that permits the realization of various equilibrium states [10]. We show that there are narrow frequency bands where self-sustained oscillations transform to stochastic oscillations of magnetization.
机译:近年来,具有随机和规则动力学机制的各种振荡系统引起了广泛的关注[1]。在这类系统中,最受研究的是磁有序结构,其动力学与磁化的进动运动有关,通常用Lan-dau-Lifshitz非线性方程式描述[2,3]。今天,人们非常感兴趣的是多层交换耦合结构,其中已经发现了巨大的磁阻效应和磁光效应[4-6]。磁性子系统的静态和动态双稳态特性的存在对于此类结构的实际使用是至关重要的[7、8]。磁性子系统在这些状态附近的行为决定了在外部磁场中进行的磁化自组织的特征[9]。在这项工作中,我们分析了具有反铁磁层间交换耦合的多层纳米结构的磁化动力学机制,该耦合允许实现各种平衡态[10]。我们表明,在狭窄的频带中,自持振荡转换为磁化的随机振荡。

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