2013
DOI: 10.24033/asens.2190
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KAM theory for the hamiltonian derivative wave equation

Abstract: We prove an infinite dimensional KAM theorem which implies the existence of Cantor families of small-amplitude, reducible, elliptic, analytic, invariant tori of Hamiltonian derivative wave equations.2000AMS subject classification: 37K55, 35L05.In the last years many progresses have been done concerning KAM theory for nonlinear Hamiltonian PDEs. The first existence results were given by Kuksin [18] and Wayne [29] for semilinear wave (NLW) and Schrödinger equations (NLS) in one space dimension (1d) under Dirich… Show more

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Cited by 107 publications
(192 citation statements)
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“…By (6.9), we know that if R σ,σ jj (0) = ∅ then we must have j + j ≤ 16|ω|| |. Indeed, if σ = σ , then 12) while, if σ = σ , one has (j + j )/2 ≤ (j 2 + j 2 ) ≤ 8|ω|| | see (6.9). Then, for τ > d + 2, we obtain the first of (6.6), by…”
Section: Proof Of Proposition 110mentioning
confidence: 99%
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“…By (6.9), we know that if R σ,σ jj (0) = ∅ then we must have j + j ≤ 16|ω|| |. Indeed, if σ = σ , then 12) while, if σ = σ , one has (j + j )/2 ≤ (j 2 + j 2 ) ≤ 8|ω|| | see (6.9). Then, for τ > d + 2, we obtain the first of (6.6), by…”
Section: Proof Of Proposition 110mentioning
confidence: 99%
“…If we consider the operator B acting on the quasi-periodic functions as (Bu)(ϕ, x) = u(ϕ + ωα(ϕ), x) and (B −1 u)(ϕ, x) := u(ϕ + ωα(ϕ), x), we have that 12) and ρ(ϕ) := B −1 (1+ω ·∂ ϕ α), that means that L + is the linear system (5.11) acting on quasi-periodic functions. By these arguments, we have simply that a curve u(t) in the phase space of functions of x, i.e.…”
Section: Proof Of Proposition 17mentioning
confidence: 99%
“…Suppose now that |k (1) |, |k (2) | ≤ N we wish to understand under which conditions on the α (i) , β (i) the expression (109) is not zero. For a monomial M := e i(k,x) y a z αzβ if Π (M ) = 0 we must have d H (M ) = 2 (plus further conditions).…”
Section: A Technical Lemmamentioning
confidence: 99%
“…and since ad(N ) −1 is diagonal (at least in complex coordinates) this definition can be given degree by degree, thus defining F 0 , F (1) , F (2) . Notice that even if we use complex coordinates F is always real.…”
Section: ≤2mentioning
confidence: 99%
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