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Homoclinic solutions for second order differential equations generated by impulses. (English) Zbl 1257.34032

The purpose of the paper is to study the existence of homoclinic solutions of the following system of second-order impulsive differential equations \[ \begin{cases}\ddot u(t)+\nabla V(t,u(t))=f(t),\quad t\in(s_{k-1},s_{k}),\\ \Delta \dot u(s_{k})=g_{k}(u(s_{k})), \end{cases}\tag{1} \] where \(k\in\mathbb Z\), \(u\in\mathbb R^n\), \(\Delta\dot u(s_k)=\dot u(s_k^+)-\dot u(s_k^-)\) with \(\dot u(s_k^{\pm})=\lim_{t\to s_k^{\pm}}\dot u(t)\), \(f\in C(\mathbb R,\mathbb R^n)\), \(\nabla V(t,u)=\text{grad}_uV(t,u)\), \(g_k(u)=\text{grad}_uG_k(u)\), \(G_k\in C^1(\mathbb R^n,\mathbb R^n)\). It is assumed that there exist an \(m\in\mathbb N\) and \(T\in\mathbb R^+\) such that \(0=s_0<s_1<\dots <s_m=T\), \(s_{k+m}=s_k+T\) and \(g_{k+m}=g_k\) for all \(k\in\mathbb Z\) (that is, \(g_k\) is \(m\)-periodic in \(k\)). As usual, a solution \(u(t)\) of (1) is called homoclinic (to 0) if \(\lim_{t\to\pm\infty}u(t)=0\) and \(\lim_{t\to\pm\infty}\dot u(t^{\pm})=0\).
In [X. Han and H. Zhang, J. Comput. Appl. Math. 235, No. 5, 1531–1541 (2011; Zbl 1211.34008); H. Zhang and Z. Li, Nonlinear Anal., Real World Appl. 12, No. 1, 39–51 (2011; Zbl 1225.34019)], it was shown that under appropriate conditions, the system (1) possesses at least one nontrivial homoclinic solution generated by impulses when \(f\equiv 0\). In the present paper, the existence of homoclinic solutions of (1) via critical point theory is estsblished under weaker assumptions on \(V\) and \(g\). The work not only generalizes the known results, but also provides certain new methods and techniques.

MSC:

34C37 Homoclinic and heteroclinic solutions to ordinary differential equations
34A37 Ordinary differential equations with impulses
58E05 Abstract critical point theory (Morse theory, Lyusternik-Shnirel’man theory, etc.) in infinite-dimensional spaces
70H05 Hamilton’s equations