M. Wanic , Z. Toklikishvili , S.K. Mishra , M. Trybus , L. Chotorlishvili
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引用次数: 0
摘要
在本研究中,我们研究了通过磁电耦合与铁电晶体耦合的磁性纳米盘的动力学。我们感兴趣的模型是非线性的,我们在弱非线性和强非线性的不同极限下探索问题。通过施加两个不同频率的电场,我们控制了铁电子系统的约束势形式,并实现了不同类型的动力学。我们证明,在双阱势的情况下,系统对磁电耦合更为敏感。特别是在强非线性情况下,任意小的磁电耦合值都会导致混乱动力学。从本质上讲,磁电耦合的作用类似于根据 KAM 定理破坏不变环的小扰动。我们证明了系统中的分岔是霍普夫类型的。我们观察到系统中磁电分形的形成。在弱非线性极限下,我们研究了参数非线性共振和通过磁电耦合增强磁振荡的问题。
Magnetoelectric fractals, Magnetoelectric parametric resonance and Hopf bifurcation
In the present work, we study the dynamics of the magnetic nanodisc coupled through a magnetoelectric coupling to a ferroelectric crystal. The model of our interest is nonlinear, and we explore the problem under different limits of weak and strong non-linearity. By applying two electric fields with different frequencies, we control the form of the confinement potential of a ferroelectric subsystem and realize different types of dynamics. We proved that the system is more sensitive to magnetoelectric coupling in the case of double-well potential. In particular, in the case of strong non-linearity, arbitrary small values of magnetoelectric coupling lead to chaotic dynamics. In essence, magnetoelectric coupling plays a role akin to the small perturbations destroying invariant tori according to the KAM theorem. We showed that bifurcations in the system are of Hopf’s type. We observed the formation of magnetoelectric fractals in the system. In the limit of weak non-linearity, we studied a problem of parametric nonlinear resonance and enhancement of magnetic oscillations through magnetoelectric coupling.