2017
DOI: 10.1016/j.jde.2017.08.067
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On the existence of connecting orbits for critical values of the energy

Abstract: We consider an open connected set Ω and a smooth potential U which is positive in Ω and vanishes on ∂Ω. We study the existence of orbits of the mechanical systemthat connect different components of ∂Ω and lie on the zero level of the energy. We allow that ∂Ω contains a finite number of critical points of U . The case of symmetric potential is also considered.

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Cited by 8 publications
(7 citation statements)
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“…The first existence proofs of a heteroclinic connection in the vector case were given by Rabinowitz [15] and by Sternberg [18,17]. For more recent developments on the heteroclinic connection problem we refer to [6,3,5,14,19,8,9,4]. The aforementioned works provide sufficient conditions for the existence of heteroclinic orbits, in various settings.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…The first existence proofs of a heteroclinic connection in the vector case were given by Rabinowitz [15] and by Sternberg [18,17]. For more recent developments on the heteroclinic connection problem we refer to [6,3,5,14,19,8,9,4]. The aforementioned works provide sufficient conditions for the existence of heteroclinic orbits, in various settings.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…In particular, such systems admit infinitely many periodic orbits and homoclinics to the Lyapunoff orbit near the critical energy level containing a saddle-center equilibrium. Motivated by the Allen-Cahn equation, Fusco-Gronchi-Novaga [12,13] use variational methods to study the existence of periodic motions of kinetic plus potential Hamiltonians.…”
Section: Applicationsmentioning
confidence: 99%
“…Remark 1. The assumptions on W imply (see for example [14], [22] and [12]) the existence of a Lipschitz continuous map u H : R → R m that satisfies lim t→±∞ u(t) = a ± ,…”
Section: The Finite Dimensional Casementioning
confidence: 99%
“…Then Theorem 5.5 in [1] or Corollary 1.5 in [12] yields the existence of a brake orbit u δ that oscillates between Γ − and Γ + and whose period T δ diverges to +∞ as δ → 0 + . Even though the condition (1.3) can be relaxed by allowing Γ ± to contain hyperbolic critical points of W [12], the extension of this approach to the infinite dimensional setting requires new ideas to overcome the difficulties related to the formulation of a condition analogous to To avoid these pathologies the idea is to minimize on a set of T -periodic maps. But we can not expect that u δ is a minimizer in the class of maps of period T = T δ .…”
Section: Introductionmentioning
confidence: 99%