2010
DOI: 10.1007/s10884-010-9176-z
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Stability of Equilibrium Solutions of Autonomous and Periodic Hamiltonian Systems with n-Degrees of Freedom in the Case of Single Resonance

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Cited by 15 publications
(14 citation statements)
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“…The Lie normal form of the Hamiltonian function H in (2) was characterized in [7] according to the generators of the module M ω . In fact, we have: • If M ω = k 1 Z + · · · + k s Z = {0}, we have that H m = H m (r, k 1 · ϕ, .…”
Section: Definitionmentioning
confidence: 99%
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“…The Lie normal form of the Hamiltonian function H in (2) was characterized in [7] according to the generators of the module M ω . In fact, we have: • If M ω = k 1 Z + · · · + k s Z = {0}, we have that H m = H m (r, k 1 · ϕ, .…”
Section: Definitionmentioning
confidence: 99%
“…For single third and four order resonances we can cite [2] and [10] for the autonomous case, while the periodic case was considered in [20]. In [7] it was considered the case of a single resonance in the general case where the matrix of the linearized system is diagonalizable. Here, the authors improve and generalize several results existing in the literature.…”
Section: Definitionmentioning
confidence: 99%
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“…In the case of resonance, i.e., ω is a rational number, the above result cannot be applied directly. For this case, there also are many results, see [2], [3], [7], [8], [22], [23], [24] and the references therein. For example, Mansilla [7] obtained some sufficient conditions for stability and instability of the trivial solution by using Moser's twist theorem and Liapunov theorem, respectively.…”
Section: Introductionmentioning
confidence: 99%
“…More recent papers on Lie stable and unstable systems are due to dos Santos and coworkers [33,34,35] where the authors establish several criteria dealing with Lie stable equilibria in cases of resonances. They also treat instability using suitable Chetaev functions [24].…”
mentioning
confidence: 99%