Abstract Consider an analytic Hamiltonian system near its analytic invariant torus $$\mathcal T_0$$ carrying zero frequency. We assume that the Birkhoff normal form of the Hamiltonian at $$\mathcal T_0$$ is convergent and has a particular form: it is an analytic function of its non-degenerate quadratic part. We prove that in this case there is an analytic canonical transformation—not just a formal power series—bringing the Hamiltonian into its Birkhoff normal form.
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Lyapunov unstable elliptic equilibria
A new diffusion mechanism from the neighborhood of elliptic equilibria for Hamiltonian flows in three or more degrees of freedom is introduced. We thus obtain explicit real entire Hamiltonians on R 2 d \mathbb {R}^{2d} , d ≥ 4 d\geq 4 , that have a Lyapunov unstable elliptic equilibrium with an arbitrary chosen frequency vector whose coordinates are not all of the same sign. For non-resonant frequency vectors, our examples all have divergent Birkhoff normal form at the equilibrium. On R 4 \mathbb {R}^4 , we give explicit examples of real entire Hamiltonians having an equilibrium with an arbitrary chosen non-resonant frequency vector and a divergent Birkhoff normal form.
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- Award ID(s):
- 2101464
- PAR ID:
- 10351439
- Date Published:
- Journal Name:
- Journal of the American Mathematical Society
- ISSN:
- 0894-0347
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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