群作用下移位映射的动力学性质

IF 1 4区 物理与天体物理 Q3 PHYSICS, MATHEMATICAL Advances in Mathematical Physics Pub Date : 2022-12-22 DOI:10.1155/2022/5969042
Zhan-Huai Ji
{"title":"群作用下移位映射的动力学性质","authors":"Zhan-Huai Ji","doi":"10.1155/2022/5969042","DOIUrl":null,"url":null,"abstract":"<jats:p>Firstly, we introduced the concept of <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M1\">\n <mi>G</mi>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>Lipschitz tracking property, <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M2\">\n <mi>G</mi>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>asymptotic average tracking property, and <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M3\">\n <mi>G</mi>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>periodic tracking property. Secondly, we studied their dynamical properties and topological structure and obtained the following conclusions: (1) let <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M4\">\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <mi>X</mi>\n <mo>,</mo>\n <mi>d</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> be compact metric <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M5\">\n <mi>G</mi>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>space and the metric <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M6\">\n <mi>d</mi>\n </math>\n </jats:inline-formula> be invariant to <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M7\">\n <mi>G</mi>\n </math>\n </jats:inline-formula>. Then, <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M8\">\n <mi>σ</mi>\n </math>\n </jats:inline-formula> has <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M9\">\n <mover accent=\"true\">\n <mi>G</mi>\n <mo stretchy=\"true\">¯</mo>\n </mover>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>asymptotic average tracking property; (2) let <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M10\">\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <mi>X</mi>\n <mo>,</mo>\n <mi>d</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> be compact metric <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M11\">\n <mi>G</mi>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>space and the metric <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M12\">\n <mi>d</mi>\n </math>\n </jats:inline-formula> be invariant to <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M13\">\n <mi>G</mi>\n </math>\n </jats:inline-formula>. Then, <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M14\">\n <mi>σ</mi>\n </math>\n </jats:inline-formula> has <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M15\">\n <mover accent=\"true\">\n <mi>G</mi>\n <mo stretchy=\"true\">¯</mo>\n </mover>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>Lipschitz tracking property; (3) let <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M16\">\n <mfenced open=\"(\" close=\")\">\n <mrow>\n <mi>X</mi>\n <mo>,</mo>\n <mi>d</mi>\n </mrow>\n </mfenced>\n </math>\n </jats:inline-formula> be compact metric <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M17\">\n <mi>G</mi>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>space and the metric <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M18\">\n <mi>d</mi>\n </math>\n </jats:inline-formula> be invariant to <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M19\">\n <mi>G</mi>\n </math>\n </jats:inline-formula>. Then, <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M20\">\n <mi>σ</mi>\n </math>\n </jats:inline-formula> has <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M21\">\n <mover accent=\"true\">\n <mi>G</mi>\n <mo stretchy=\"true\">¯</mo>\n </mover>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>periodic tracking property. The above results make up for the lack of theory of <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M22\">\n <mi>G</mi>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>Lipschitz tracking property, <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M23\">\n <mi>G</mi>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>asymptotic average tracking property, and <jats:inline-formula>\n <math xmlns=\"http://www.w3.org/1998/Math/MathML\" id=\"M24\">\n <mi>G</mi>\n <mo>‐</mo>\n </math>\n </jats:inline-formula>periodic tracking property in infinite product space under group action.</jats:p>","PeriodicalId":49111,"journal":{"name":"Advances in Mathematical Physics","volume":null,"pages":null},"PeriodicalIF":1.0000,"publicationDate":"2022-12-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Dynamical Property of the Shift Map under Group Action\",\"authors\":\"Zhan-Huai Ji\",\"doi\":\"10.1155/2022/5969042\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<jats:p>Firstly, we introduced the concept of <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M1\\\">\\n <mi>G</mi>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>Lipschitz tracking property, <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M2\\\">\\n <mi>G</mi>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>asymptotic average tracking property, and <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M3\\\">\\n <mi>G</mi>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>periodic tracking property. Secondly, we studied their dynamical properties and topological structure and obtained the following conclusions: (1) let <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M4\\\">\\n <mfenced open=\\\"(\\\" close=\\\")\\\">\\n <mrow>\\n <mi>X</mi>\\n <mo>,</mo>\\n <mi>d</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> be compact metric <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M5\\\">\\n <mi>G</mi>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>space and the metric <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M6\\\">\\n <mi>d</mi>\\n </math>\\n </jats:inline-formula> be invariant to <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M7\\\">\\n <mi>G</mi>\\n </math>\\n </jats:inline-formula>. Then, <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M8\\\">\\n <mi>σ</mi>\\n </math>\\n </jats:inline-formula> has <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M9\\\">\\n <mover accent=\\\"true\\\">\\n <mi>G</mi>\\n <mo stretchy=\\\"true\\\">¯</mo>\\n </mover>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>asymptotic average tracking property; (2) let <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M10\\\">\\n <mfenced open=\\\"(\\\" close=\\\")\\\">\\n <mrow>\\n <mi>X</mi>\\n <mo>,</mo>\\n <mi>d</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> be compact metric <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M11\\\">\\n <mi>G</mi>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>space and the metric <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M12\\\">\\n <mi>d</mi>\\n </math>\\n </jats:inline-formula> be invariant to <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M13\\\">\\n <mi>G</mi>\\n </math>\\n </jats:inline-formula>. Then, <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M14\\\">\\n <mi>σ</mi>\\n </math>\\n </jats:inline-formula> has <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M15\\\">\\n <mover accent=\\\"true\\\">\\n <mi>G</mi>\\n <mo stretchy=\\\"true\\\">¯</mo>\\n </mover>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>Lipschitz tracking property; (3) let <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M16\\\">\\n <mfenced open=\\\"(\\\" close=\\\")\\\">\\n <mrow>\\n <mi>X</mi>\\n <mo>,</mo>\\n <mi>d</mi>\\n </mrow>\\n </mfenced>\\n </math>\\n </jats:inline-formula> be compact metric <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M17\\\">\\n <mi>G</mi>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>space and the metric <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M18\\\">\\n <mi>d</mi>\\n </math>\\n </jats:inline-formula> be invariant to <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M19\\\">\\n <mi>G</mi>\\n </math>\\n </jats:inline-formula>. Then, <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M20\\\">\\n <mi>σ</mi>\\n </math>\\n </jats:inline-formula> has <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M21\\\">\\n <mover accent=\\\"true\\\">\\n <mi>G</mi>\\n <mo stretchy=\\\"true\\\">¯</mo>\\n </mover>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>periodic tracking property. The above results make up for the lack of theory of <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M22\\\">\\n <mi>G</mi>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>Lipschitz tracking property, <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M23\\\">\\n <mi>G</mi>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>asymptotic average tracking property, and <jats:inline-formula>\\n <math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\" id=\\\"M24\\\">\\n <mi>G</mi>\\n <mo>‐</mo>\\n </math>\\n </jats:inline-formula>periodic tracking property in infinite product space under group action.</jats:p>\",\"PeriodicalId\":49111,\"journal\":{\"name\":\"Advances in Mathematical Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":1.0000,\"publicationDate\":\"2022-12-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advances in Mathematical Physics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1155/2022/5969042\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, MATHEMATICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advances in Mathematical Physics","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1155/2022/5969042","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, MATHEMATICAL","Score":null,"Total":0}
引用次数: 0

摘要

首先,我们引入了G‐Lipschitz跟踪性质、G‐渐近平均跟踪性质的概念,和G周期跟踪特性。其次研究了它们的动力学性质和拓扑结构,得到以下结论:(1)设X,d是紧致度量G‐空间,并且度量d对G那么,σ具有G′‐渐近平均跟踪性质;(2) 设X,d是紧致度量G‐空间,并且度量d对G那么,σ具有G‐Lipschitz跟踪性质;(3) 设X,d是紧致度量G‐空间,并且度量d对G那么,σ具有G′-周期跟踪性质。上述结果弥补了G‐Lipschitz跟踪性质、G‐渐近平均跟踪性质、,以及群作用下无穷乘积空间中的G-周期跟踪性质。
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Dynamical Property of the Shift Map under Group Action
Firstly, we introduced the concept of G Lipschitz tracking property, G asymptotic average tracking property, and G periodic tracking property. Secondly, we studied their dynamical properties and topological structure and obtained the following conclusions: (1) let X , d be compact metric G space and the metric d be invariant to G . Then, σ has G ¯ asymptotic average tracking property; (2) let X , d be compact metric G space and the metric d be invariant to G . Then, σ has G ¯ Lipschitz tracking property; (3) let X , d be compact metric G space and the metric d be invariant to G . Then, σ has G ¯ periodic tracking property. The above results make up for the lack of theory of G Lipschitz tracking property, G asymptotic average tracking property, and G periodic tracking property in infinite product space under group action.
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来源期刊
Advances in Mathematical Physics
Advances in Mathematical Physics 数学-应用数学
CiteScore
2.40
自引率
8.30%
发文量
151
审稿时长
>12 weeks
期刊介绍: Advances in Mathematical Physics publishes papers that seek to understand mathematical basis of physical phenomena, and solve problems in physics via mathematical approaches. The journal welcomes submissions from mathematical physicists, theoretical physicists, and mathematicians alike. As well as original research, Advances in Mathematical Physics also publishes focused review articles that examine the state of the art, identify emerging trends, and suggest future directions for developing fields.
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