English

Lagrange Stability for Reversible Duffing Equations with Quasi-Periodic Coefficients

Dynamical Systems 2026-07-19 v1

Abstract

We consider x¨+f(x,ωt)x˙+g(x,ωt)=0, \ddot x+f(x,\omega t)\dot x+g(x,\omega t)=0, where f(x,θ)=j=0maj(θ)x2j+1,g(x,θ)=x2n+1+j=0n1bj(θ)x2j+1. f(x,\theta)=\sum_{j=0}^{m}a_j(\theta)x^{2j+1},\qquad g(x,\theta)=x^{2n+1}+\sum_{j=0}^{n-1}b_j(\theta)x^{2j+1}. The coefficient functions are real analytic and even on the torus and the frequency vector ω\omega is Diophantine. If n2(m+1)n\geq2(m+1), we construct codimension-one reversible KAM tori accumulating at infinity and prove that all solutions are bounded. The main point is a finite normal-form procedure. After the reversible polynomial reduction, a logarithmic Fourier cut-off is introduced. At the vv-th step a truncated homological equation is solved on a non-resonant action interval and the new error satisfies an explicit finite-step recurrence. Thus an arbitrarily small negative power of the large action is reached after finitely many steps. Finally, the Largrangian stability and the existence of quasi-periodic solutions are proved by the reversible KAM theorem.

Keywords

Cite

@article{arxiv.2607.17068,
  title  = {Lagrange Stability for Reversible Duffing Equations with Quasi-Periodic Coefficients},
  author = {Huining Xue},
  journal= {arXiv preprint arXiv:2607.17068},
  year   = {2026}
}