2017
DOI: 10.1016/j.geomphys.2016.05.014
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Monodromy of Hamiltonian systems with complexity 1 torus actions

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Cited by 12 publications
(43 citation statements)
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“…Part of this computation has been given in [13], with the exception of an overall "sign" of the monodromy vector (which depends on a careful choice of orientations and was outside the scope of [13]). In this case π 1 (R) is isomorphic to the free product Z * Z and is generated by two closed paths: one path [γ 1 ] encircling the thread C 0 23 and one path [γ 2 ] encircling the thread C 0 13 . The threads C 0 23 and C 0 13 are oriented so that they start at infinity and point to the origin.…”
Section: Case δmentioning
confidence: 99%
“…Part of this computation has been given in [13], with the exception of an overall "sign" of the monodromy vector (which depends on a careful choice of orientations and was outside the scope of [13]). In this case π 1 (R) is isomorphic to the free product Z * Z and is generated by two closed paths: one path [γ 1 ] encircling the thread C 0 23 and one path [γ 2 ] encircling the thread C 0 13 . The threads C 0 23 and C 0 13 are oriented so that they start at infinity and point to the origin.…”
Section: Case δmentioning
confidence: 99%
“…We note that the present work is closely related to the works [29,39], which demonstrate how one can compute monodromy by focusing on the circle action and without using Morse theory. However, the idea of computing monodromy through energy hyper-surfaces and their Chern numbers can also be applied when we do not have a detailed knowledge of the singularities of the system; see Remark 3.5.…”
Section: Introductionmentioning
confidence: 65%
“…For this reason, it cannot be directly generalized to systems with many degrees of freedom. An approach that admits such a generalization was developed in [29,39]; we shall recall it in the next section.…”
Section: Remark 35 (Generalization)mentioning
confidence: 99%
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