{ "id": "1406.0208", "version": "v1", "published": "2014-06-01T21:26:37.000Z", "updated": "2014-06-01T21:26:37.000Z", "title": "Cubic perturbations of elliptic Hamiltonian vector fields of degree three", "authors": [ "Lubomir Gavrilov", "Iliya D. Iliev" ], "categories": [ "math.DS" ], "abstract": "The purpose of the present paper is to study the limit cycles of one-parameter perturbed plane Hamiltonian vector field $X_\\varepsilon$ $$ X_\\varepsilon : \\left\\{ \\begin{array}{llr} \\dot{x}=\\;\\; H_y+\\varepsilon f(x,y)\\\\ \\dot{y}=-H_x+\\varepsilon g(x,y), \\end{array} \\;\\;\\;\\;\\; H~=\\frac{1}{2} y^2~+U(x) \\right. $$ which bifurcate from the period annuli of $X_0$ for sufficiently small $\\varepsilon$. Here $U$ is a univariate polynomial of degree four without symmetry, and $f, g$ are arbitrary cubic polynomials in two variables. We take a period annulus and parameterize the related displacement map $d(h,\\varepsilon)$ by the Hamiltonian value $h$ and by the small parameter $\\varepsilon$. Let $M_k(h)$ be the $k$-th coefficient in its expansion with respect to $\\varepsilon$. We establish the general form of $M_k$ and study its zeroes. We deduce that the period annuli of $X_0$ can produce for sufficiently small $\\varepsilon$, at most 5, 7 or 8 zeroes in the interior eight-loop case, the saddle-loop case, and the exterior eight-loop case respectively. In the interior eight-loop case the bound is exact, while in the saddle-loop case we provide examples of Hamiltonian fields which produce 6 small-amplitude limit cycles. Polynomial perturbations of $X_0$ of higher degrees are also studied.", "revisions": [ { "version": "v1", "updated": "2014-06-01T21:26:37.000Z" } ], "analyses": { "subjects": [ "34C07" ], "keywords": [ "elliptic hamiltonian vector fields", "cubic perturbations", "period annulus", "interior eight-loop case", "perturbed plane hamiltonian vector field" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2014arXiv1406.0208G" } } }