English

KAM theorem for reversible mapping of low smoothness with application

Dynamical Systems 2019-10-21 v1

Abstract

Assume the mapping A:{x1=x+ω+y+f(x,y),y1=y+g(x,y),(x,y)Td×B(r0)A:\left\{ \begin{array}{ll} x_{1}=x+\omega+y+f(x,y), y_{1}=y+g(x,y), \end{array} \right. (x, y)\in \mathbb{T}^{d}\times B(r_{0}) is reversible with respect to G:(x,y)(x,y),G: (x, y)\mapsto (-x, y), and fC(Td×B(r0))ε0,gC+d(Td×B(r0))ε0,| f | _{C^{\ell}(\mathbb{T}^{d}\times B(r_{0}))}\leq \varepsilon_{0}, | g |_{C^{\ell+d}(\mathbb{T}^{d}\times B(r_{0}))}\leq \varepsilon_{0}, where B(r0):={yr0:  yRd},B(r_{0}):=\{|y|\le r_0:\; y\in\mathbb R^d\}, =2d+1+μ\ell=2d+1+\mu with 0<μ1.0<\mu\ll 1. Then when ε0=ε0(d)>0\varepsilon_{0}=\varepsilon_{0}(d)>0 is small enough and ω\omega is Diophantine, the map AA possesses an invariantS torus with rotational frequency ω.\omega. As an application of the obtained theorem, the Lagrange stability is proved for a class of reversible Duffing equation with finite smooth perturbation.

Keywords

Cite

@article{arxiv.1910.08214,
  title  = {KAM theorem for reversible mapping of low smoothness with application},
  author = {Jing Li and Jiangang Qi and Xiaoping Yuan},
  journal= {arXiv preprint arXiv:1910.08214},
  year   = {2019}
}
R2 v1 2026-06-23T11:47:25.551Z