Bifurcations on a Five-Parameter Family of Planar Vector Field
Tóm tắt
In this paper we consider a five-parameter family of planar vector fields
$${X_{\mu}: \, \begin{array}{ll} \frac{dx}{dt} = y,\\ \frac{dy}{dt} = x^4+\mu_3x^2+\mu_2x+\mu_1 +y(\mu_4+\mu_5x\\ \quad+\,c(\mu )x^2+x^3h(x,\mu))+y^2Q(x,y,\mu), \end{array}}$$
where μ = (μ
1, μ
2, μ
3, μ
4, μ
5), which is a small parameter vector, and c(0) ≠ 0. The family X
μ
represents the generic unfolding of a class of nilpotent cusp of codimension five. We discuss the local bifurcations of X
μ, which exhibits numerous kinds of bifurcation phenomena including Bogdanov-Takens bifurcations of codimension four in Li and Rousseau (J. Differ. Eq. 79, 132–167, 1989) and Dumortier and Fiddelaers (In: Global analysis of dynamical systems, 2001), and Bogdanov-Takens bifurcations of codimension three in Dumortier et al. (Ergodic Theory Dynam. Syst. 7, 375–413, 1987) and Dumortier et al. (Bifurcations of planar vector fields. Nilpotent singularities and Abelian integrals, 1991). After making some rescalings, we obtain the truncated systems of X
μ
. For a truncated system, all possible bifurcation sets and related phase portraits are obtained. When the truncated system is a Hamiltonian system, the bifurcation diagram and the related phase portraits are given too. Hopf bifurcations are studied for another truncated system. And it shows that the system has the Hopf bifurcations of codimension at most three, and at most three limit cycles occur in the small neighborhood of the Hopf singularity.
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