Abstract:Abstract. We consider families of one and a half degrees of freedom rapidly forced Hamiltonian system which are perturbations of one degree of freedom Hamiltonians having a homoclinic connection. We derive the inner equation for this class of Hamiltonian system which is expressed as the Hamiltonian-Jacobi equation of one a half degrees of freedom Hamiltonian. The inner equation depends on a parameter not necessarily small.We prove the existence of special solutions of the inner equation with a given behavior a… Show more
We study the problem of exponentially small splitting of separatrices of one degree of freedom classical Hamiltonian systems with a non-autonomous perturbation fast and periodic in time. We provide a result valid for general systems which are algebraic or trigonometric polynomials in the state variables. It consists on obtaining a rigorous proof of the asymptotic formula for the measure of the splitting. We obtain that the splitting has the asymptotic behavior K ε β e −a/ε , identifying the constants K , β, a in terms of the system features. We consider several cases. In some cases, assuming the perturbation is small enough, the values of K , β coincide with the classical Melnikov approach. We identify the limit size of the perturbation for which this theory holds true. However for the limit cases, which appear naturally both in averaging and bifurcation theories, we encounter that, generically, K and β are not well predicted by Melnikov theory.
We study the problem of exponentially small splitting of separatrices of one degree of freedom classical Hamiltonian systems with a non-autonomous perturbation fast and periodic in time. We provide a result valid for general systems which are algebraic or trigonometric polynomials in the state variables. It consists on obtaining a rigorous proof of the asymptotic formula for the measure of the splitting. We obtain that the splitting has the asymptotic behavior K ε β e −a/ε , identifying the constants K , β, a in terms of the system features. We consider several cases. In some cases, assuming the perturbation is small enough, the values of K , β coincide with the classical Melnikov approach. We identify the limit size of the perturbation for which this theory holds true. However for the limit cases, which appear naturally both in averaging and bifurcation theories, we encounter that, generically, K and β are not well predicted by Melnikov theory.
“…In fact, in [3] the asymptotic expression for I n is proved only when I n has the form I n = +∞ −∞ e i αt (s + t) − −1 dt with ∈ Q, but it is immediate that the result also holds in this case. The estimation for J n also needs an extra argument to be done from the results in [3].…”
Section: Asymptotic Expression For the Difference φmentioning
confidence: 99%
“…In this section we will recover Theorem 1.2 from Theorem 1.5. We will need a technical lemma, analogous to Lemma 2.6, which was proved in [3].…”
Section: Asymptotic Expression For the Difference φmentioning
confidence: 99%
“…Introduction. We consider the family of autonomous differential equations in C 3 given by dφ dτ = −ηφ − (α + cη) i φ + εF 1 (φ, ϕ, η) dϕ dτ = −ηϕ + (α + cη) i ϕ + εF 2 (φ, ϕ, η) (1.1)…”
Abstract. A classical problem in the study of the (conservative) unfoldings of the so called Hopf-zero bifurcation, is the computation of the splitting of a heteroclinic connection which exists in the symmetric normal form along the z-axis. In this paper we derive the inner system associated to this singular problem, which is independent on the unfolding parameter. We prove the existence of two solutions of this system related with the stable and unstable manifolds of the unfolding, and we give an asymptotic formula for their difference. We check that the results in this work agree with the ones obtained in the regular case by the authors.
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