博彩评级网-博彩网

專 欄

首 頁

專 欄

學術報告(Kawamura Shinzo 教授,2019.9.16)

學術舉辦時間 2019年9月16日 10:00—11:00 學術舉辦地點 廣州大學理學實驗樓314
主講人 Kawamura Shinzo (河村新蔵) 主題 Chaos on symbolic dynamical systems

數學學院學術講座  (2019054)

 

 

 

報告人: Kawamura Shinzo (河村新蔵)

單位: 日本山形大學(Yamagata University

職務: 教授

報告時間: 2019916 上午10:00—11:00

報告地點: 廣州大學理學實驗樓314

 

TitleChaos on symbolic dynamical systems

 

ABSTRACTChaos theory is a branch of mathematics focusing on the behavior of dynamical systems that are highly sensitive to initial conditions. ”Chaos” is an interdisciplinary theory stating within the apparent randomness of chaotic complex systems such as f(z)=z^2+C and the deterministic nonlinear system which can result in large differences in a later state, e.g. a butterfly flapping its wings in Brazil can cause a hurricane in Texas.

 

Nowadays, in common usage, ”chaos” means ”a state of disorder”. However, in chaos theory, the term is defined more precisely. Although no universally accepted mathematical definition of chaos exists, a commonly used definition originally formulated by Robert L. Devaney for a continuous map f:X—>X on some metric space X as follows [2]: the dynamical system Σ=(X,f) is said to be chaotic if has the following three properties called chaotic properties.

(1) The set of all periodic points of is dense in X. (2) is topologically transitive. (3) has sensitive dependence on initial conditions.

 

We here note that five mathematicians [1] show that if a dynamical system (X; f) satisfies Properties (1) and (2) and the cardinal number of is infinite, then Property (3) automatically holds. Namely two topological properties implies a property of metric space. It was a surprising result.

 

Now, we restrict the compact metric space to the compact metric Cantor space Σ_n consisting of all infinite sequences of integers between 1 and n, and the function to the backward shiftσ_n. It is well-known that the dynamical system (Σ_n,σ_n) is chaotic in the sense of Devaney. In this talk, we consider a kind of dynamical systems (Σ_A,σ_A) associated with n×n matrix with all entries belonging to {0,1}, whereΣ_A is a compact and σ-invarinat subset ofΣ_n andσ_A is the restriction of σ toΣ_A. We show a necessary and sufficient condition for the dynamical system (Σ_A,σ_A) to be chaotic in term of the propery of the following matrix [3]: A+A^2+…+A^n

[1] J. Banks, J. Brooks, G. Cairns, G. Davis and P. Stacey, On Devaney’s definition of Chaos, Amer. Math. Monthly, 99(1992), 332-334.

[2] R. L. Devaney, An intorodunction to chaotic dynamical systems, Second Edition, Addision-Wesley, Redwood City, 1989

[3] S. Kawamura, H.Takaegara and A.Uchiyam, Chaotic conditions of dubshift on symbolic dynamical systems, preprint.

 

報告人簡介:河村新蔵,日本山形大學數理科學部教授。1983年畢業于北海道大學,獲得博士學位。1974—2014間,日本山形大學講師,副教授,教授。1988Wales 大學(United Kingdom)留學,2012-至今,北京林業大學客座教授。

主要研究內容:泛函分析,代數算子,模糊理論,動力系統等,分別在Tohoku Math.J.J.Math.Soc.Japan,Proc.Amer.Math.Soc.Math. Scand等學術雜志上發表學術論文60余篇。

 

 

上一條:2019年引智講壇之五十 下一條: 化學化工講壇第五十五、五十六、五十七講

郵編:510006        郵箱:webmaster@gzhu.edu.cn

通訊地址:廣州市大學城外環西路230號


移動網站

  • 官方微博

  • 官方微信

廣州大學版權所有     COPYRIGHT?1999-2021      粵ICP備 05008855號

大发888信誉最新娱乐| 百乐门娱乐城注册| E世博百家乐官网的玩法技巧和规则 | 罗盘24层| 德晋百家乐的玩法技巧和规则| 百家乐官网里和的作用| 百家乐百家乐视频| 大发888游戏备用网址| 百家乐官网赌场软件| 澳门百家乐游戏官网| 百家乐官网园小区户型图 | 百家乐官网智能软件| 百家乐筹码桌| 百家乐官网庄闲机率| 百家乐博彩优惠论坛| 台北市| 免费百家乐娱乐城| 333娱乐场| 真人百家乐技巧| 六合彩开码| 百家乐官网论坛bocaila| 鸿运国际| 百家乐游戏平台排名| 彩票| 百家乐剁手| 鄂托克前旗| 百家乐一般的庄闲比例是多少| 百家乐官网长龙怎么预判| 58百家乐的玩法技巧和规则 | 百家乐官网论坛| 在线赌博平台| 权威百家乐信誉网站| 百家乐官网智能分析软| 百家乐稳赢投资法| 百家乐官网做庄家必赢诀窍| 网上百家乐作| 百家乐官网平注法口诀技巧| 靖江市| 百家乐娱乐网77scs| 百家乐官网凯时娱乐网| 明升娱乐城开户|