{"title":"可逆小马蹄形图的非对称鞍节点对","authors":"Y. Yamaguchi, K. Tanikawa","doi":"10.1143/PTP.128.15","DOIUrl":null,"url":null,"abstract":"In the reversible Smale horseshoe, we introduce a new symbol sequence other than the conventional one made of symbols 0 and 1. This system is based on subregionsE,F,S ,a ndD of resonance regions of rotation number between 0 and 1/2. We call E(p/q),F(p/q),S(p/q), and D(p/q )f or 0 <p /q <1/2, and E(1/2) and S(1/2) blocks. These blocks play the role of symbols. Thus, the number of symbols is infinite. In the system, space is divided finer and time is divided coarser. Given a periodic orbit, we want to know the origin of the orbit, that is, how the orbit has been bifurcated. In this paper, we look for the pair component of saddle-node pairs. We propose a procedure to find the pair component for a given nonsymmetric periodic orbit of the general type. If it turns out that there is no pair component, we suggest that the periodic orbit has been born through equiperiod bifurcation or period-doubling bifurcation. Subject Index: 030","PeriodicalId":49658,"journal":{"name":"Progress of Theoretical Physics","volume":"128 1","pages":"15-30"},"PeriodicalIF":0.0000,"publicationDate":"2012-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1143/PTP.128.15","citationCount":"0","resultStr":"{\"title\":\"Nonsymmetric Saddle-Node Pairs for the Reversible Smale Horseshoe Map\",\"authors\":\"Y. Yamaguchi, K. Tanikawa\",\"doi\":\"10.1143/PTP.128.15\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In the reversible Smale horseshoe, we introduce a new symbol sequence other than the conventional one made of symbols 0 and 1. This system is based on subregionsE,F,S ,a ndD of resonance regions of rotation number between 0 and 1/2. We call E(p/q),F(p/q),S(p/q), and D(p/q )f or 0 <p /q <1/2, and E(1/2) and S(1/2) blocks. These blocks play the role of symbols. Thus, the number of symbols is infinite. In the system, space is divided finer and time is divided coarser. Given a periodic orbit, we want to know the origin of the orbit, that is, how the orbit has been bifurcated. In this paper, we look for the pair component of saddle-node pairs. We propose a procedure to find the pair component for a given nonsymmetric periodic orbit of the general type. If it turns out that there is no pair component, we suggest that the periodic orbit has been born through equiperiod bifurcation or period-doubling bifurcation. Subject Index: 030\",\"PeriodicalId\":49658,\"journal\":{\"name\":\"Progress of Theoretical Physics\",\"volume\":\"128 1\",\"pages\":\"15-30\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2012-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1143/PTP.128.15\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Progress of Theoretical Physics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1143/PTP.128.15\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Progress of Theoretical Physics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1143/PTP.128.15","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
在可逆小马蹄铁中,我们引入了一个新的符号序列,而不是由符号0和1组成的符号序列。该系统是基于旋转数在0到1/2之间的共振区域的子区域se,F,S,a和dd。我们称之为E (p / q), F (p / q), S (p / q), D (p / q) F或0 < p / q < 1/2, E(1/2)和S(1/2)块。这些积木起到了符号的作用。因此,符号的数量是无限的。在这个系统中,空间划分得更精细,时间划分得更粗糙。给定一个周期轨道,我们想知道轨道的起源,也就是说,轨道是如何分叉的。在本文中,我们寻找鞍节点对的对分量。对于给定的一般型非对称周期轨道,我们提出了一种求轨道对分量的方法。如果不存在对分量,我们认为周期轨道是通过等周期分岔或倍周期分岔产生的。主题索引:030
Nonsymmetric Saddle-Node Pairs for the Reversible Smale Horseshoe Map
In the reversible Smale horseshoe, we introduce a new symbol sequence other than the conventional one made of symbols 0 and 1. This system is based on subregionsE,F,S ,a ndD of resonance regions of rotation number between 0 and 1/2. We call E(p/q),F(p/q),S(p/q), and D(p/q )f or 0