{ "id": "1907.09434", "version": "v1", "published": "2019-07-22T17:10:27.000Z", "updated": "2019-07-22T17:10:27.000Z", "title": "On the topology of nearly-integrable Hamiltonians at simple resonances", "authors": [ "L. Biasco", "L. Chierchia" ], "categories": [ "math.DS" ], "abstract": "We show that, in general, averaging at simple resonances a real--analytic, nearly--integrable Hamiltonian, one obtains a one--dimensional system with a cosine--like potential; ``in general'' means for a generic class of holomorphic perturbations and apart from a finite number of simple resonances with small Fourier modes; ``cosine--like'' means that the potential depends only on the resonant angle, with respect to which it is a Morse function with one maximum and one minimum. \\\\ Furthermore, the (full) transformed Hamiltonian is the sum of an effective one--dimen\\-sio\\-nal Hamiltonian (which is, in turn, the sum of the unperturbed Hamiltonian plus the cosine--like potential) and a perturbation, which is exponentially small with respect to the oscillation of the potential. \\\\ As a corollary, under the above hypotheses, if the unperturbed Hamiltonian is also strictly convex, the effective Hamiltonian at {\\sl any simple resonance} (apart a finite number of low--mode resonances) has the phase portrait of a pendulum. \\\\ The results presented in this paper are an essential step in the proof (in the ``mechanical'' case) of a conjecture by Arnold--Kozlov--Neishdadt (\\cite[Remark~6.8, p. 285]{AKN}), claiming that the measure of the ``non--torus set'' in general nearly--integrable Hamiltonian systems has the same size of the perturbation; compare \\cite{BClin}, \\cite{BC}.", "revisions": [ { "version": "v1", "updated": "2019-07-22T17:10:27.000Z" } ], "analyses": { "keywords": [ "simple resonance", "finite number", "cosine-like potential", "small fourier modes", "general nearly-integrable hamiltonian systems" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }