Abstract:We consider di erentiable maps having an invariant torus with normal behavior having a central part. We p r o ve the existence and regularity of pseudostable manifolds and regularity with respect to parameters. Then we p r o ve a l a m bda lemma in this setting for C 2 maps.
“…Using the symmetry of H r , introducing I i = −I i for i < 0, we have the pseudo-orbit {(I i , θ i ), |i| ≤ N } ⊂ H r . Using standard shadowing results in [FM00,FM03] (changing slightly I i to obtain an irrational frequency of the inner map, if necessary ) or newer results like the corollary 3.5 of [GLS14], there exists a trajectory of the system such that for some T , I 0 ≤ −I * and I(T ) ≥ I * . If a 10 < 0, changing H r to H l all the previous reasoning applies.…”
In this work we illustrate the Arnold diffusion in a concrete example-the a priori unstable Hamiltonian system of 2 + 1/2 degrees of freedom H(p, q, I, ϕ, s) = p 2 /2 + cos q − 1 + I 2 /2+h(q, ϕ, s; ε)-proving that for any small periodic perturbation of the form h(q, ϕ, s; ε) = ε cos q (a00 + a10 cos ϕ + a01 cos s) (a10a01 = 0) there is global instability for the action. For the proof we apply a geometrical mechanism based in the so-called Scattering map.This work has the following structure: In a first stage, for a more restricted case (I * ∼ π/2µ, µ = a10/a01), we use only one scattering map, with a special property: the existence of simple paths of diffusion called highways. Later, in the general case we combine a scattering map with the inner map (inner dynamics) to prove the more general result (the existence of the instability for any µ). The bifurcations of the scattering map are also studied as a function of µ. Finally, we give an estimate for the time of diffusion, and we show that this time is primarily the time spent under the scattering map.
MSC2010 numbers: 37J40
“…Using the symmetry of H r , introducing I i = −I i for i < 0, we have the pseudo-orbit {(I i , θ i ), |i| ≤ N } ⊂ H r . Using standard shadowing results in [FM00,FM03] (changing slightly I i to obtain an irrational frequency of the inner map, if necessary ) or newer results like the corollary 3.5 of [GLS14], there exists a trajectory of the system such that for some T , I 0 ≤ −I * and I(T ) ≥ I * . If a 10 < 0, changing H r to H l all the previous reasoning applies.…”
In this work we illustrate the Arnold diffusion in a concrete example-the a priori unstable Hamiltonian system of 2 + 1/2 degrees of freedom H(p, q, I, ϕ, s) = p 2 /2 + cos q − 1 + I 2 /2+h(q, ϕ, s; ε)-proving that for any small periodic perturbation of the form h(q, ϕ, s; ε) = ε cos q (a00 + a10 cos ϕ + a01 cos s) (a10a01 = 0) there is global instability for the action. For the proof we apply a geometrical mechanism based in the so-called Scattering map.This work has the following structure: In a first stage, for a more restricted case (I * ∼ π/2µ, µ = a10/a01), we use only one scattering map, with a special property: the existence of simple paths of diffusion called highways. Later, in the general case we combine a scattering map with the inner map (inner dynamics) to prove the more general result (the existence of the instability for any µ). The bifurcations of the scattering map are also studied as a function of µ. Finally, we give an estimate for the time of diffusion, and we show that this time is primarily the time spent under the scattering map.
MSC2010 numbers: 37J40
“…This follows by applying the λ-lemma for partially hyperbolic tori of Fontich and Martin [12] to C 0 and C 1 . It follows from this lemma that for all ǫ > 0, there exists a positive integer K ′ such that for all…”
Section: Our Main Results Is the Followingmentioning
confidence: 99%
“…Theorem 4 implies that the λ-lemma proven in Theorem 3 applies to the three degreeof-freedom Hamiltonian systems defined by (12).…”
Abstract. Let N be a smooth manifold and f : N → N be a C ℓ , ℓ ≥ 2 diffeomorphism. Let M be a normally hyperbolic invariant manifold, not necessarily compact. We prove an analogue of the λ-lemma in this case.
“…After enough iterations of F , one can obtain some estimate of closeness to W u . The novelty of [14] is that they also track the tangent space at every point in S and off W s . This is necessary in order to obtain the claim of the lemma.…”
Abstract. In this article, we prove the existence of Arnold diffusion for an interesting specific system -discrete nonlinear Schrödinger equation. The proof is for the 5-dimensional case with or without resonance. In higher dimensions, the problem is open. Progresses are made by establishing a complete set of Melnikov-Arnold integrals in higher and infinite dimensions. The openness lies at the concrete computation of these Melnikov-Arnold integrals. New machineries introduced here into the topic of Arnold diffusion are the Darboux transformation and isospectral theory of integrable systems.
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