Abstract

Let D(t0,ε) be the splitting distance of the stable and unstable manifold of a time-periodic second order equation. We expand D(t0,ε) as a formal power series in ε asD(t0,ε)=E0(t0)+εE1(t0)+⋯+εnEn(t0)+⋯. In this paper we derive an explicit integral formula for E1(t0). We also evaluate E1(t0) to prove the existence of homoclinic tangles for an equation to which the Poincaré/Melnikov method fails to apply.

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