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Bifurcations in dynamical systems with interior symmetry

机译:具有内部对称性的动力系统中的分叉

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We propose a definition of interior symmetry in the context of general dynamical systems. This concept appeared originally in the theory of coupled cell networks, as a generalization of the idea of symmetry of a network. The notion of interior symmetry introduced here can be seen as a special form of forced symmetry breaking of an equivariant system of differential equations. Indeed, we show that a dynamical system with interior symmetry can be written as the sum of an equivariant system and a 'perturbation term' which completely breaks the symmetry. Nonetheless, the resulting dynamical system still retains an important feature common to systems with symmetry, namely, the existence of flow-invariant subspaces. We define interior symmetry breaking bifurcations in analogy with the definition of symmetry breaking bifurcation from equivariant bifurcation theory and study the codimension one steady-state and Hopf bifurcations. Our main result is the full analogues of the well-known Equivariant Branching Lemma and the Equivariant Hopf Theorem from the bifurcation theory of equivariant dynamical systems in the context of interior symmetry breaking bifurcations.
机译:我们提出了在一般动力系统中内部对称性的定义。这个概念最初出现在耦合单元网络的理论中,作为网络对称性思想的概括。此处介绍的内部对称性概念可以看作是微分方程等变系统强迫对称性破坏的一种特殊形式。实际上,我们证明了具有内部对称性的动力学系统可以写成等变系统和“扰动项”的总和,该扰动项完全破坏了对称性。尽管如此,最终的动力学系统仍然保留了对称系统所共有的重要特征,即存在流量不变子空间。我们用等变分叉理论定义了对称对称分叉的内部对称分叉,并研究了稳态的一维稳态和霍普夫分叉的余维。我们的主要结果是在内部对称打破分叉的背景下,根据等变动力系统的分叉理论,我们熟知的等价分支引理和等价Hopf定理的完全相似。

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