2000
DOI: 10.5565/publmat_44100_08
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Bifurcations of limit cycles from cubic Hamiltonian systems with a center and a homoclinic saddle-loop

Abstract: It is proved in this paper that the maximum number of limit cycles of systemis equal to two in the finite plane, where k >, 0 < | | 1, |α| + |β| + |γ| = 0. This is partial answer to the seventh question in [2], posed by Arnold.

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Cited by 6 publications
(2 citation statements)
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“…Obviously, system ð1:1Þ E is the perturbations of Hamiltonian vector field, whose Hamiltonian has the form H nþ1 ¼ y 2 2 þ P nþ1 ðxÞ; where P nþ1 ðxÞ is a polynomial in x of degree n þ 1: Many results can be found for n ¼ 1; 2; 3; see [12][13][14][15][16] for example. For nX5; there are few results.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…Obviously, system ð1:1Þ E is the perturbations of Hamiltonian vector field, whose Hamiltonian has the form H nþ1 ¼ y 2 2 þ P nþ1 ðxÞ; where P nþ1 ðxÞ is a polynomial in x of degree n þ 1: Many results can be found for n ¼ 1; 2; 3; see [12][13][14][15][16] for example. For nX5; there are few results.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…Clearly, a homoclinic loop can be either stable or unstable. A nonisolated homoclinic loop may appear as the boundary curve of period annuli [4,6,22]. In many cases a nonisolated homoclinic loop can generate an isolated loop under perturbations on a codimension one surfaces in the parameter space.…”
Section: Introductionmentioning
confidence: 99%