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Numerical Analysis of Electromagnetic Wave Instability in Nonlinear Ferrite Structures Using Bifurcation Points of the Nonlinear Maxwell√c??s Operator

机译:非线性Maxwell√智能术分岔点的非线性铁氧体结构中电磁波不稳定性的数值分析

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A new approach, based on the bifurcation theory [1], to develop mathematical models of nonlinear electromagnetic waves or oscillations in waveguiding (WGS) and resonator structures (RS), containing a strongly nonlinear bounded gyromagnetic medium, is proposed. The physical meaning of the bifurcation points of the nonlinear Maxwell's operator is that these are the values of the parameters at which qualitative modifications of nonlinear processes occur, caused by instabilities, such as the onset or breakdown of self-oscillations, the transition from periodic to chaotic behavior. The rigorous statement of a nonlinear boundary problem for waveguiding structures, containing a nonlinear gyromagnetic medium, requires to solve the full set of non-linear Maxwell's equations complemented by the equation of motion of the magnetization vector in a ferromagnet [2]. Earlier theories of the instability of magnetostatic or spin waves were developed using an approximate analysis based on the equation of motion of the magnetization for 1-D ferrite structures [3].
机译:一种新的方法,基于所述分岔理论[1],开发非线性电磁波或振荡的数学模型中的波导(WGS)和谐振器结构(RS),其包含强非线性有界旋磁介质,提出了。非线性麦克斯韦操作者的分叉点的物理意义是,这些都是在该非线性过程的定性修饰发生的参数,由不稳定性的值,例如发作或自振荡的击穿,从周期性的,以过渡混沌行为。用于波导结构,含有一个非线性旋磁介质中的非线性边界问题的严格声明,需要解决的全套非线性麦克斯韦方程由磁化矢量的运动在一个铁磁体[2]方程补充的。静或自旋波的不稳定性的早期的理论是使用基于所述磁化的运动的1-d铁氧体结构[3]方程式的近似分析开发的。

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