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
“…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.…”
In this paper we consider a class of fully nonlinear forced and reversible Schrödinger equations and prove existence and stability of quasi-periodic solutions. We use a Nash-Moser algorithm together with a reducibility theorem on the linearized operator in a neighborhood of zero. Due to the presence of the highest order derivatives in the non-linearity the classic KAM-reducibility argument fails and one needs to use a wider class of changes of variables such has diffeomorphisms of the torus and pseudo-differential operators. This procedure automtically produces a change of variables, well defined on the phase space of the equation, which diagonalizes the operator linearized at the solution. This gives the linear stability.
“…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.…”
In this paper we consider a class of fully nonlinear forced and reversible Schrödinger equations and prove existence and stability of quasi-periodic solutions. We use a Nash-Moser algorithm together with a reducibility theorem on the linearized operator in a neighborhood of zero. Due to the presence of the highest order derivatives in the non-linearity the classic KAM-reducibility argument fails and one needs to use a wider class of changes of variables such has diffeomorphisms of the torus and pseudo-differential operators. This procedure automtically produces a change of variables, well defined on the phase space of the equation, which diagonalizes the operator linearized at the solution. This gives the linear stability.
“…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%
“…, (2) ), γ −1 X P T p := Θ . We require that 9 note that the condition LM < 4 is added only in order to simplify notations, any ε 2 , r, K independent constat would be acceptable.…”
Abstract. We prove, by applying a KAM algorithm, existence of large families of stable and unstable quasi periodic solutions for the NLS in any number of independent frequencies. The main tools are the existence of a non-degenerate integrable normal form proved in [18] and [20] and a suitable generalization of the quasi-Töplitz functions introduced in [24]
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