Infinite Orbit depth and length of Melnikov functions

Abstract

In this paper we study polynomial Hamiltonian systems $dF=0$ in the plane and their small perturbations: $dF+εω=0$. The first nonzero Melnikov function $M_μ=M_μ(F,γ,ω)$ of the Poincaré map along a loop $γ$ of $dF=0$ is given by an iterated integral. In a previous work (see arXiv 1703.03837), we bounded the length of the iterated integral $M_μ$ by a geometric number $k=k(F,γ)$ which we call orbit depth. We conjectured that the bound is optimal. Here, we give a simple example of a Hamiltonian system $F$ and its orbit $γ$ having infinite orbit depth. If our conjecture is true, for this example there should exist deformations $dF+εω$ with arbitrary high length first nonzero Melnikov function $M_μ$ along $γ$. We construct deformations $dF+εω=0$ whose first nonzero Melnikov function $M_μ$ is of length three and explain the difficulties in constructing deformations having high length first nonzero Melnikov functions $M_μ$.