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排斥相互作用下的最小嵌合体

Smallest Chimeras Under Repulsive Interactions.

作者信息

Saha Suman, Dana Syamal Kumar

机构信息

National Brain Research Centre, Gurugram, India.

National Institute of Technology, Durgapur, India.

出版信息

Front Netw Physiol. 2021 Dec 21;1:778597. doi: 10.3389/fnetp.2021.778597. eCollection 2021.

DOI:10.3389/fnetp.2021.778597
PMID:36925584
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10013064/
Abstract

We present an exemplary system of three identical oscillators in a ring interacting repulsively to show up chimera patterns. The dynamics of individual oscillators is governed by the superconducting Josephson junction. Surprisingly, the repulsive interactions can only establish a symmetry of complete synchrony in the ring, which is broken with increasing repulsive interactions when the junctions pass through serials of asynchronous states (periodic and chaotic) but finally emerge into chimera states. The chimera pattern first appears in chaotic rotational motion of the three junctions when two junctions evolve coherently, while the third junction is incoherent. For larger repulsive coupling, the junctions evolve into another chimera pattern in a periodic state when two junctions remain coherent in rotational motion and one junction transits to incoherent librational motion. This chimera pattern is sensitive to initial conditions in the sense that the chimera state flips to another pattern when two junctions switch to coherent librational motion and the third junction remains in rotational motion, but incoherent. The chimera patterns are detected by using partial and global error functions of the junctions, while the librational and rotational motions are identified by a libration index. All the collective states, complete synchrony, desynchronization, and two chimera patterns are delineated in a parameter plane of the ring of junctions, where the boundaries of complete synchrony are demarcated by using the master stability function.

摘要

我们展示了一个由三个相同的振荡器组成的环形系统,它们之间存在排斥相互作用,从而呈现出奇异子模式。单个振荡器的动力学由超导约瑟夫森结控制。令人惊讶的是,排斥相互作用只能在环中建立完全同步的对称性,当结经过一系列异步状态(周期性和混沌性)时,随着排斥相互作用的增加,这种对称性会被打破,但最终会出现奇异子状态。当两个结相干演化而第三个结不相干时,奇异子模式首先出现在三个结的混沌旋转运动中。对于更大的排斥耦合,当两个结在旋转运动中保持相干而一个结转变为不相干的平动时,结会在周期性状态下演化为另一种奇异子模式。这种奇异子模式对初始条件敏感,即当两个结切换到相干平动而第三个结保持旋转但不相干时,奇异子状态会翻转到另一种模式。通过使用结的局部和全局误差函数来检测奇异子模式,而通过平动指数来识别平动和旋转运动。在结环的参数平面中描绘了所有的集体状态,即完全同步、去同步以及两种奇异子模式,其中通过主稳定性函数划定了完全同步的边界。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8244/10013064/31d0259b3b56/fnetp-01-778597-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8244/10013064/5800be39e41e/fnetp-01-778597-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8244/10013064/77da348f7027/fnetp-01-778597-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8244/10013064/95b6aadf7f54/fnetp-01-778597-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8244/10013064/31d0259b3b56/fnetp-01-778597-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8244/10013064/5800be39e41e/fnetp-01-778597-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8244/10013064/77da348f7027/fnetp-01-778597-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8244/10013064/95b6aadf7f54/fnetp-01-778597-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8244/10013064/31d0259b3b56/fnetp-01-778597-g004.jpg

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