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由平均场密度和低通滤波器引起的对称性破缺动力学

Symmetry breaking dynamics induced by mean-field density and low-pass filter.

作者信息

Ponrasu K, Singh Uday, Sathiyadevi K, Senthilkumar D V, Chandrasekar V K

机构信息

Centre for Nonlinear Science & Engineering, School of Electrical & Electronics Engineering, SASTRA Deemed University, Thanjavur 613401, Tamil Nadu, India.

School of Physics, Indian Institute of Science Education and Research, Thiruvananthapuram 695551, Kerala, India.

出版信息

Chaos. 2020 May;30(5):053120. doi: 10.1063/1.5142234.

Abstract

The phenomenon of spontaneous symmetry breaking facilitates the onset of a plethora of nontrivial dynamical states/patterns in a wide variety of dynamical systems. Spontaneous symmetry breaking results in amplitude and phase variations in a coupled identical oscillator due to the breaking of the prevailing permutational/translational symmetry of the coupled system. Nevertheless, the role and the competing interaction of the low-pass filter and the mean-field density parameter on the symmetry breaking dynamical states are unclear and yet to be explored explicitly. The effect of low pass filtering along with the mean-field parameter is explored in conjugately coupled Stuart-Landau oscillators. The dynamical transitions are examined via bifurcation analysis. We show the emergence of a spontaneous symmetry breaking (asymmetric) oscillatory state, which coexists with a nontrivial amplitude death state. Through the basin of attraction, the multi-stable nature of the spontaneous symmetry breaking state is examined, which reveals that the asymmetric distribution of the initial state favors the spontaneous symmetry breaking dynamics, while the symmetric distribution of initial states gives rise to the nontrivial amplitude death state. In addition, the trade-off between the cut-off frequency of the low-pass filter along with the mean-field density induces and enhances the symmetry breaking dynamical states. Global dynamical transitions are discussed as a function of various system parameters. Analytical stability curves corresponding to the nontrivial amplitude death and oscillation death states are deduced.

摘要

自发对称性破缺现象促进了各种动力系统中大量非平凡动力学状态/模式的出现。由于耦合系统中主导的置换/平移对称性被打破,自发对称性破缺会导致耦合的相同振子出现幅度和相位变化。然而,低通滤波器和平均场密度参数在对称性破缺动力学状态中的作用以及它们之间的竞争相互作用尚不清楚,有待进一步明确探索。本文在共轭耦合的斯图尔特 - 兰道振子中研究了低通滤波与平均场参数的影响。通过分岔分析研究了动力学转变。我们展示了一种自发对称性破缺(不对称)振荡状态的出现,它与一种非平凡的振幅死亡状态共存。通过吸引域,研究了自发对称性破缺状态的多稳态性质,结果表明初始状态的不对称分布有利于自发对称性破缺动力学,而初始状态的对称分布会导致非平凡的振幅死亡状态。此外,低通滤波器的截止频率与平均场密度之间的权衡会诱导并增强对称性破缺动力学状态。讨论了作为各种系统参数函数的全局动力学转变。推导了对应于非平凡振幅死亡和振荡死亡状态的解析稳定性曲线。

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