{"title":"Global Phase Portraits of Uniform Isochronous Centers System of Degree Six with Polynomial Commutator","authors":"Li-na Guo, Ai-yong Chen, Shuai-feng Zhao","doi":"10.1007/s10255-024-1081-z","DOIUrl":null,"url":null,"abstract":"<div><p>This paper studies the global phase portraits of uniform isochronous centers system of degree six with polynomial commutator. Such systems have the form <span>\\(\\dot x = - y + xf(x,\\,y),\\,\\,\\dot y = x + yf(x,\\,y)\\)</span>, where <i>f</i>(<i>x, y</i>) = <i>a</i><sub>1</sub><i>x</i> + <i>a</i><sub>2</sub><i>xy</i> + <i>a</i><sub>3</sub><i>xy</i><sup>2</sup> + <i>a</i><sub>4</sub><i>xy</i><sup>3</sup> + <i>a</i><sub>5</sub><i>xy</i><sup>4</sup> = <i>xσ</i>(<i>y</i>), and any zero of 1 + <i>a</i><sub>1</sub><i>y</i> + <i>a</i><sub>2</sub><i>y</i><sup>2</sup> + <i>a</i><sub>3</sub><i>y</i><sup>3</sup> + <i>a</i><sub>4</sub><i>y</i><sup>4</sup> + <i>a</i><sub>5</sub><i>y</i><sup>5</sup>, <span>\\(y = \\bar y\\)</span> is an invariant straight line. At last, all global phase portraits are drawn on the Poincaré disk.</p></div>","PeriodicalId":0,"journal":{"name":"","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-06-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s10255-024-1081-z.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"","FirstCategoryId":"100","ListUrlMain":"https://link.springer.com/article/10.1007/s10255-024-1081-z","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
This paper studies the global phase portraits of uniform isochronous centers system of degree six with polynomial commutator. Such systems have the form \(\dot x = - y + xf(x,\,y),\,\,\dot y = x + yf(x,\,y)\), where f(x, y) = a1x + a2xy + a3xy2 + a4xy3 + a5xy4 = xσ(y), and any zero of 1 + a1y + a2y2 + a3y3 + a4y4 + a5y5, \(y = \bar y\) is an invariant straight line. At last, all global phase portraits are drawn on the Poincaré disk.