
handle: 11585/725366 , 2158/1438824
Summary: We consider a singularly perturbed system where the fast dynamics of the unperturbed problem exhibits a trajectory homoclinic to a critical point. We assume that the slow time system is \(1\)-dimensional and it admits a unique critical point, which undergoes to a bifurcation as a second parameter varies: transcritical, saddle-node, or pitchfork. In this setting Battelli and Palmer proved the existence of a unique trajectory \((\tilde{x}(t,\varepsilon,\lambda),\tilde{y}(t,\varepsilon,\lambda))\) homoclinic to the slow manifold. The purpose of this paper is to construct curves which divide the \(2\)-dimensional parameters space in different areas where \((\tilde{x}(t,\varepsilon,\lambda),\tilde{y}(t,\varepsilon,\lambda))\) is either homoclinic, heteroclinic, or unbounded. We derive explicit formulas for the tangents of these curves. The results are illustrated by some examples.
Bifurcation theory for ordinary differential equations, Bifurcations of singular points in dynamical systems, QA Mathematics / matematika, Homoclinic and heteroclinic solutions to ordinary differential equations, transcritical bifurcation, Singular perturbation; homoclinic trajectory; transcritical bifurcation; saddle-node bifurcation, homoclinic trajectory, QA1-939, Singular perturbations for ordinary differential equations, Invariant manifolds for ordinary differential equations, singular perturbation, Mathematics, saddle-node bifurcation
Bifurcation theory for ordinary differential equations, Bifurcations of singular points in dynamical systems, QA Mathematics / matematika, Homoclinic and heteroclinic solutions to ordinary differential equations, transcritical bifurcation, Singular perturbation; homoclinic trajectory; transcritical bifurcation; saddle-node bifurcation, homoclinic trajectory, QA1-939, Singular perturbations for ordinary differential equations, Invariant manifolds for ordinary differential equations, singular perturbation, Mathematics, saddle-node bifurcation
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