2005
DOI: 10.1070/rd2005v010n04abeh000321
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Abstract: The Kowalevski top in two constant fields is known as the unique profound example of an integrable Hamiltonian system with three degrees of freedom not reducible to a family of systems in fewer dimensions. As the first approach to topological analysis of this system we find the critical set of the integral map; this set consists of the trajectories with number of frequencies less than three. We obtain the equations of the bifurcation diagram in R 3 . A correspondence to the Appelrot classes in the classical Ko… Show more

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Cited by 30 publications
(36 citation statements)
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“…It is easily shown that X & O and X is the two-dimensional invariant submanifold of the flow (1) consisting of the pendulum motions found in Kharlamov (2005) a ¼ aðe 1 cos h À e 2 sin hÞ; b ¼ AEbðe 1 sin h þ e 2 cos hÞ;…”
Section: Partial Integralsmentioning
confidence: 99%
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“…It is easily shown that X & O and X is the two-dimensional invariant submanifold of the flow (1) consisting of the pendulum motions found in Kharlamov (2005) a ¼ aðe 1 cos h À e 2 sin hÞ; b ¼ AEbðe 1 sin h þ e 2 cos hÞ;…”
Section: Partial Integralsmentioning
confidence: 99%
“…It is natural to study the invariant submanifolds in P 6 such that the induced system has only two degrees of freedom. It is proved in Kharlamov (2005) …”
Section: Introductionmentioning
confidence: 96%
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“…Чтобы сформулировать описание критического множества отображения момента в случае Ковалевской -Соколова, напомним понятие критической подсистемы [38,20,39]. Рассмот-рим неприводимую интегрируемую систему с тремя степенями свободы с инволютивным набором интегралов, который обозначим так же, как и в нашей задаче, через H, L, K. Предположим, для простоты, что в ней отсутствуют фокусные особенности ранга 1.…”
Section: критическое множество и типы критических точекunclassified