KAM for the nonlinear wave equation on the circle: a normal form theorem
Moudhaffar Bouthelja

TL;DR
This paper proves a KAM theorem for infinite-dimensional Hamiltonian systems with multiple eigenvalues, demonstrating the persistence of invariant tori under small perturbations in the context of nonlinear wave equations on the circle.
Contribution
It extends KAM theory to infinite-dimensional systems with multiple eigenvalues, providing conditions for the persistence of invariant tori in nonlinear wave equations.
Findings
Invariant tori persist under small perturbations.
Conditions for non-resonance of frequencies are established.
The theorem applies to Hamiltonian normal forms with block-diagonal matrices.
Abstract
In this paper we prove a KAM theorem in infinite dimension which treats the case of multiple eigenvalues (or frequencies) of finite order. More precisely, we consider a Hamiltonian normal form in infinite dimension:\begin{equation} \nonumberh(\rho)=\omega(\rho).r + \frac{1}{2} \langle \zeta,A(\rho)\zeta \rangle,\end{equation}where , and is a subset of . We assume that the infinite matrix satisfies , where and is a bloc diagonal matrix. We assume that the size of each bloc of is the multiplicity of the corresponding eigenvalue in .In this context, if we start from a torus, then the solution of the associated Hamiltonian system remains on that torus.…
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