{ "id": "1212.1150", "version": "v2", "published": "2012-12-05T20:28:09.000Z", "updated": "2013-01-28T14:39:05.000Z", "title": "A strong form of Arnold diffusion for two and a half degrees of freedom", "authors": [ "Vadim Kaloshin", "Ke Zhang" ], "comment": "207 pages, 21 figures. This paper includes and supercedes arXiv:1202.1032. arXiv admin note: text overlap with arXiv:math/0412300 by other authors", "categories": [ "math.DS" ], "abstract": "In the present paper we prove a strong form of Arnold diffusion. Let $\\T^2$ be the two torus and $B^2$ be the unit ball around the origin in $\\R^2$. Fix $\\rho>0$. Our main result says that for a \"generic\" time-periodic perturbation of an integrable system of two degrees of freedom $H_\\epsilon = H_0 + \\epsilon H_1(\\theta, p, t)$ with a strictly convex $H_0$, there exists a $\\rho$-dense orbit $(\\theta_{\\epsilon},p_{\\epsilon},t)(t)$ in $\\T^2 \\times B^2 \\times \\T$, namely, a $\\rho$-neighbourhood of the orbit contains $\\T^2 \\times B^2 \\times \\T$. Our proof is a combination of geometric and variational methods. The fundamental elements of the construction are usage of crumpled normally hyperbolic invariant cylinders from [13], flower and simple normally hyperbolic invariant manifolds from [47] as well as their kissing property at a strong double resonance. This allows us to build a \"connected\" net of 3-dimensional normally hyperbolic invariant manifolds. To construct diffusing orbits along this net we employ a version of Mather variational method [54] equipped with weak KAM theory [34], proposed by Bernard in [9].", "revisions": [ { "version": "v2", "updated": "2013-01-28T14:39:05.000Z" } ], "analyses": { "subjects": [ "37J40", "37J45", "37J50", "37D10" ], "keywords": [ "arnold diffusion", "strong form", "half degrees", "normally hyperbolic invariant cylinders", "variational method" ], "note": { "typesetting": "TeX", "pages": 207, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2012arXiv1212.1150K" } } }