Hopf bifurcation with tetrahedral and octahedral symmetry

TL;DR

This paper compares the bifurcation of periodic solutions in symmetric dynamical systems with tetrahedral and octahedral symmetry, analyzing how group representations influence possible bifurcations and solution types.

Contribution

It provides a detailed comparison of Hopf bifurcations under tetrahedral and octahedral symmetries, highlighting differences in spatial symmetries of solutions despite similar matrix groups.

Findings

Different spatial symmetries of bifurcating solutions are possible for the two groups.

Identification of which solutions guaranteed by the $H~\mathrm{mod}~K$ theorem are realizable via Hopf bifurcation.

Analysis of the impact of group representations on bifurcation types.

Abstract

In the study of the periodic solutions of a $\Gamma$-equivariant dynamical system, the $H~\mathrm{mod}~K$ theorem gives all possible periodic solutions, based on group-theoretical aspects. By contrast, the equivariant Hopf theorem guarantees the existence of families of small-amplitude periodic solutions bifurcating from the origin for each $\mathbf{C}$-axial subgroup of $\Gamma\times\mathbb{S}^1$. In this article we compare the bifurcation of periodic solutions for generic differential equations equivariant under the full group of symmetries of the tetrahedron and the group of rotational symmetries of the cube. The two groups are the image of inequivalent representations of the symmetric group $S_4$. The possible spatial symmetries of bifurcating solutions are different, even though the two groups yield the same group of matrices $\Gamma\times\mathbb{S}^1$. The same group of matrices occurs again as the extension $\Gamma\times\mathbb{S}^1$ when $\Gamma$ is the full group of symmetries of the cube. For these three groups, while characterizing the Hopf bifurcation, we identify which periodic solution types, whose existence is guaranteed by the $H~\mathrm{mod}~K$ theorem, are obtainable by Hopf bifurcation from the origin.