Drift in phase space: a new variational mechanism with optimal diffusion time

dc.creatorBerti, Massimiliano
dc.creatorBiasco, Luca
dc.creatorBolle, Philippe
dc.date2002-05-29
dc.date.accessioned2026-07-07T04:48:47Z
dc.date.available2026-07-07T04:48:47Z
dc.descriptionWe consider non-isochronous, nearly integrable, a-priori unstable Hamiltonian systems with a (trigonometric polynomial) $O(μ)$-perturbation which does not preserve the unperturbed tori. We prove the existence of Arnold diffusion with diffusion time $ T_d = O((1/ μ) \log (1/ μ))$ by a variational method which does not require the existence of ``transition chains of tori'' provided by KAM theory. We also prove that our estimate of the diffusion time $T_d $ is optimal as a consequence of a general stability result derived from classical perturbation theory.
dc.description34 pages
dc.identifierhttps://arxiv.org/abs/math/0205307
dc.identifierhttp://arxiv.org/abs/math/0205307
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/64180
dc.subjectFunctional Analysis
dc.subjectDynamical Systems
dc.subject37J40, 37J45
dc.titleDrift in phase space: a new variational mechanism with optimal diffusion time
dc.typetext

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