
The authors consider the problem of bifurcation of periodic solutions in singular systems of differential equations \[ \varepsilon\dot{u}=f(u)+\varepsilon g(t,u,\varepsilon)\quad u\in\mathbb{R}^n, \] where \(g(t+2,u,\varepsilon)=g(t,u,\varepsilon)\) and \(\dot{u}=f(u)\) has an orbit \(\gamma(t)\) homoclinic to a hyperbolic equilibrium point \(p\). By using a functional analytic approach and the Lyapunov-Schmidt method they obtain a bifurcation function which tends, as \(\varepsilon\to0+\), to the Melnikov function. They show that if a certain Melnikov condition is satisfied then the system has a unique periodic solution of period \(2m\), for any \(m\geq1\), \(m\in\mathbb{N}\), and \(\varepsilon\) sufficiently small.
Bifurcation theory for ordinary differential equations, singular system of differential equations, Melnikov function, Singular perturbations for ordinary differential equations, Homoclinic and heteroclinic solutions to ordinary differential equations, Periodic solutions to ordinary differential equations, homoclinic, Analysis
Bifurcation theory for ordinary differential equations, singular system of differential equations, Melnikov function, Singular perturbations for ordinary differential equations, Homoclinic and heteroclinic solutions to ordinary differential equations, Periodic solutions to ordinary differential equations, homoclinic, Analysis
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