1990
DOI: 10.1007/bf01047768
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Transversality between invariant manifolds of periodic orbits for a class of monotone dynamical systems

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Cited by 21 publications
(26 citation statements)
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“…For the Neumann case ðNÞ; this property has been discovered independently by Henry [Hen85] and Angenent [Ang86]. For the S 1 -equivariant periodic case ðPÞ; the Morse-Smale property is established in Section 3 following Fusco and Oliva [FuOl90]. Loosely speaking it states that hyperbolicity of E,F,R alone is sufficient to imply transverse intersections of stable and unstable manifolds.…”
Section: Introductionmentioning
confidence: 90%
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“…For the Neumann case ðNÞ; this property has been discovered independently by Henry [Hen85] and Angenent [Ang86]. For the S 1 -equivariant periodic case ðPÞ; the Morse-Smale property is established in Section 3 following Fusco and Oliva [FuOl90]. Loosely speaking it states that hyperbolicity of E,F,R alone is sufficient to imply transverse intersections of stable and unstable manifolds.…”
Section: Introductionmentioning
confidence: 90%
“…Claim (b), (3.5) involves a decomposition of the Floquet eigenspaces, according to zero number z ¼ 2k; very similar to-but less explicit than-(3.11) above. See [AF88] and also [FuOl90] for details. The lap number cðvÞ ¼ zðv x Þ enters diacritically, because v t ¼ cv x is the Floquet eigenfunction of the trivial Floquet multiplier 1, and thus separates the strongly stable from the strongly unstable Floquet eigenspace.…”
Section: Article In Pressmentioning
confidence: 97%
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“…In the case when the linear system (1.3) is time-periodic in t, Smith [34] studied the Floquet theory by using an integer-valued Lyapunov function σ, first defined by Smillie [33] (see also similar forms by Mallet-Paret and Smith [17], Fusco and Oliva [8,9], and Mallet-Paret and Sell [16]), and related the values of σ to the Floquet multipliers of the linear periodic system. This function σ is not defined everywhere but only on an open and dense subset Λ of R n on which it is also continuous (see section 2).…”
Section: Introductionmentioning
confidence: 99%
“…For a generic perturbation R the associated parabolic flow Ψ t is a Morse-Smale flow [21]. The (finite) collection of rest points {u a } and periodic orbits {γ b } of Ψ t then yields a Morse decomposition of Inv(N ), and the Morse inequalities are…”
Section: Lemma 36 An Arbitrary Parabolic Flow On a Bounded Relative mentioning
confidence: 99%