Abstract

In this paper we consider the persistence of lower dimensional tori of a class of analytic perturbed Hamiltonian system, H =hw(x), Ii + 1 W0 (u 2 + v 2 ) + P(q, I, z, ¯ z;x) and prove that if the frequencies (w0,W0) satisfy some non-resonance condition and the Brouwer degree of the frequency mapping w(x) at w0 is nonzero, then there exists an invariant lower dimensional invariant torus, whose frequencies are a small dilation of w0.

Highlights

  • In this paper we consider small perturbations of an analytic Hamiltonian in a normal form N=v2), on a phase space (θ, I, z, z) ∈ P = Tn × Rn × R × R, where Tn is the usual n-dimensional torus and the tangential frequencies ω(ξ) = (ω1, . . . , ωn) are parameters dependent on ξ ∈ D ⊂ Rn with D a bounded connected open domain.The associated symplectic form is n∑ dθj ∧ dIj + du ∧ dv. j=1X

  • For each ξ ∈ D, there exists an invariant n-dimensional torus Tn × {0} × {0} ⊂ R2n × R2 with tangential frequencies ω(ξ), which has an elliptic fixed point in the normal uv-space with normal frequency Ω0. These tori are called lower dimensional invariant tori, split from resonant ones lying in the resonance zone constituted by both stochastic trajectories and regular orbits

  • In the case of Rüssmann’s non-degeneracy, generally speaking, we cannot expect any more information on the persistence of both maximal and lower dimensional invariant tori with a given Diophantine frequency vector without adding any other extra condition to the Hamiltonian, since the image of the frequency map may be on a sub-manifold

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Summary

Introduction

Prove that if the frequencies (ω0, Ω0) satisfy some non-resonance condition and the Brouwer degree of the frequency mapping ω(ξ) at ω0 is nonzero, there exists an invariant lower dimensional invariant torus, whose frequencies are a small dilation of ω0. In the case of Rüssmann’s non-degeneracy, generally speaking, we cannot expect any more information on the persistence of both maximal and lower dimensional invariant tori with a given Diophantine frequency vector without adding any other extra condition to the Hamiltonian, since the image of the frequency map may be on a sub-manifold.

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