English

On invariant tori in some reversible systems

Dynamical Systems 2021-10-22 v2

Abstract

In the present paper, we consider the following reversible system \begin{equation*} \begin{cases} \dot{x}=\omega_0+f(x,y),\\ \dot{y}=g(x,y), \end{cases} \end{equation*} where xTdx\in\mathbf{T}^{d}, y0Rdy\backsim0\in \mathbf{R}^{d}, ω0\omega_0 is Diophantine, f(x,y)=O(y)f(x,y)=O(y), g(x,y)=O(y2)g(x,y)=O(y^2) and ff, gg are reversible with respect to the involution G: (x,y)(x,y)(x,y)\mapsto(-x,y), that is, f(x,y)=f(x,y)f(-x,y)=f(x,y), g(x,y)=g(x,y)g(-x,y)=-g(x,y). We study the accumulation of an analytic invariant torus Γ0\Gamma_0 of the reversible system with Diophantine frequency ω0\omega_0 by other invariant tori. We will prove that if the Birkhoff normal form around Γ0\Gamma_0 is 0-degenerate, then Γ0\Gamma_0 is accumulated by other analytic invariant tori, the Lebesgue measure of the union of these tori being positive and the density of the union of these tori at Γ0\Gamma_0 being one. We will also prove that if the Birkhoff normal form around Γ0\Gamma_0 is jj-degenerate (1jd11\leq j\leq d-1) and condition (1.6) is satisfied, then through Γ0\Gamma_0 there passes an analytic subvariety of dimension d+jd+j foliated into analytic invariant tori with frequency vector ω0\omega_0. If the Birkhoff normal form around Γ0\Gamma_0 is d1d-1-degenerate, we will prove a stronger result, that is, a full neighborhood of Γ0\Gamma_0 is foliated into analytic invariant tori with frequency vectors proportional to ω0\omega_0.

Cite

@article{arxiv.2010.11402,
  title  = {On invariant tori in some reversible systems},
  author = {Lu Chen},
  journal= {arXiv preprint arXiv:2010.11402},
  year   = {2021}
}
R2 v1 2026-06-23T19:32:26.497Z