亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        A Devaney Chaotic System Which Is Neither Distributively nor Topologically Chaotic

        2013-08-27 01:41:22CHENZHIZHILIAOLIANDWANGWEI

        CHEN ZHI-ZHI,LIAO LIAND WANG WEI

        (1.Institute of Mathematics,Jilin University,Changchun,130012) (2.Institute of Statistics,Jilin University of Finance and Economics,Changchun,130017) (3.Institute of Applied Physics and Computational Mathematics,Beijing,100094)

        Communicated by Lei Feng-chun

        A Devaney Chaotic System Which Is Neither Distributively nor Topologically Chaotic

        CHEN ZHI-ZHI1,2,LIAO LI3AND WANG WEI1

        (1.Institute of Mathematics,Jilin University,Changchun,130012) (2.Institute of Statistics,Jilin University of Finance and Economics,Changchun,130017) (3.Institute of Applied Physics and Computational Mathematics,Beijing,100094)

        Communicated by Lei Feng-chun

        Weiss proved that Devaney chaos does not imply topological chaos and Oprocha pointed out that Devaney chaos does not imply distributional chaos.In this paper,by constructing a simple example which is Devaney chaotic but neither distributively nor topologically chaotic,we give a unif i ed proof for the results of Weiss and Oprocha.

        Devaney chaos,distributional chaos,topological entropy

        1 Introduction

        Devaney,distributional and topological chaos are a few of dif f erent versions of chaos.Let us f i rst recall their concrete def i nitions.

        Let(X,d)be a metric space,and f:X→X continuous(sometimes f is said to be a system).We call f Devaney chaotic,brief l y DevC,if it possesses the three properties as def i ned in[1]:

        (1)transitivity,i.e.,there exists a point x∈X such that the orbit orb(x,f)={x,f(x), f2(x),···}is dense in X;

        (2)periodic density,i.e.,the set of periodic points of f is dense in X;

        (3)sensitive dependence(on initial conditions).

        To determine if a map is chaotic,it is sufficient to consider whether it possesses the transitivity and the periodic density,since the properties(1)and(2)in the def i nition ofDevaney imply(3)for the case that f is inf i nite(see[2–3]).

        The notion of distributional chaos was given in[4](where,however,distributional chaos is called“strong chaos”).We call f distributively chaotic,brief l y DC,if there exists an uncountable set D?X such that any dif f erent points x,y∈D form a distributively chaotic pair,brief l y DC pair,i.e.,there exists an ε>0 such that

        and for any ε>0,

        where

        (#denotes the cardinality).

        The def i nition of topological entropy was introduced in[5].For more detail discussion we refer the readers to[6].In this note,the topological entropy of f is denoted by ent(f). f is said to be topologically chaotic,brief l y PTE,if ent(f)>0.

        Many researchers gave their attention to the relations among Devaney,distributional and topological chaos(see[7–13]).

        By the def i nitions,Devaney chaos is a global characteristic,but distributional and topological chaos are not.One can easily give an example which is either distributional or topological chaos but not Devaney chaos.However,the inverse implications are not so evident.In 1971,Weiss[7]found that the transitivity and the periodic density do not imply PTE,and he had proved essentially that DevC does not imply PTE.Recently,the conclusion of Weiss was restated in[8].To show that DevC does not imply DC,Oprocha[9]constructed a Devaney chaotic subshift without DC pairs where.However,he did not give a strict proof.

        In the present paper,by forming a simple example which is Devaney chaotic but neither distributively nor topologically chaotic,we give a unif i ed proof for the results of Weiss and Oprocha.

        2 Symbolic Space,Shift and Subshift

        Let S={0,1},Σ={x=x0x1···|xi∈S,i=0,1,2,···},and def i ne ρ:Σ×Σ→R as: for any x=x0x1···,y=y0y1···∈Σ,

        where i is the minimal integer such that xi/=yi.It is not difficult to check that ρ is a metric on Σ.(Σ,ρ)is compact(see[6])and called the one-sided symbolic space(with two symbols).Def i ne σ:Σ→Σ by

        σ is continuous(see[6])and is called the shift on Σ.If X?Σ is closed and σ(X)?X,we call(X,σ|X)or σ|Xa subshift of σ.

        Call A a word,if it is a f i nite arrangement of the elements in S.If A=a0···an-1,where ai∈S for i=0,1,···,n-1,then n is said to be the length of A,denoted by|A|=n.Let B=b0···bm-1be another word.Denote

        Then AB is also a word.Furthermore,if A0,A1,···are all words,then A0A1···is an element in Σ.We use An(n may be∞)to denote the word arranged by n A's.We say that A occurs in B,denoted by A?B,if there is an i≥0 such that

        A word A occurs in a point x∈Σ if it occurs in some initial word of x.For any x∈Σ, i≥0 and n>0,we use Qn(A)to denote the number of subwords of length n occurring in the word A,and for any W?Σ,

        For any x∈Σ,i≥0 and n>0,x[i,i+n]denotes the word xi···xi+n. We give the following lemma(for the proof see[6]).

        Lemma 2.1Let(X,σ|X)be a subshift.Then

        3 The Main Results and Their Proofs

        Example 3.1Let q1=1,p1=1∞.For each i≥1,def i ne inductively

        Put

        Lemma 3.1For each i>0,there exist inf i nite sequences〈Aj〉and〈Bj〉of words satisfying

        (P1)Aj∈Pi,Bj∈i,and

        for any j≥1 such that u=A1B1A2B2···,which is called an i-representation of u. Proof.For given i>0,by the def i nition,there exist f i nite sequencesandof words satisfying(P1)such that

        where Aj∈Pi(1≤j≤k),Bj∈i(1≤j≤k-1).It follows by induction that for any l≥i+1 and any m>0,may be written as the form(3.1).In particular, where k≥1 and for each(1≤j≤k),Aj∈Pi,Bj∈i.Since every qlis an initial word of u by the def i nition,we see that for given i>0 there must exist inf i nite sequences〈Aj〉and〈Bj〉of words satisfying(P1)such that To complete the proof of the lemma,it suffices to show that the inf i nite sequences〈Aj〉and〈Bj〉also satisfy(P2).

        Notice that rewriting u cannot contract any gap of zeros.It follows that for any j≥1, if t=maxthenandby the def i nition of u. We then have

        Whatever happens,the sequences〈Aj〉and〈Bj〉satisfy(P2).

        In the sequel,X always denotes the space which is def i ned in Example 3.1.Put

        Lemma 3.2Let x=x0x1···∈X.If x∈E,then for any ε>0,

        (B0denotes nothing,if lt-1=0).Thus for each t,by(P2),one has

        Lemma 3.3Let x=x0x1···∈X.If x∈F,then there exists an l≥0 such that σl(x) is a periodic point not to be 0∞.

        Proof.By the hypotheses,there exists an i>0 such that for each k≥i,0kdoes not occur in x.Let

        Then 0≤j≤i-1(we prescribe that n0=0).There exists an l≥0 such that xl=1 and 0kdoes not occur infor all k>j.Since x?u,it follows that for any n>l withand,there exists an m>0 such that.Letting n→∞gives

        The lemma then follows(noting that for any j≥0,by the def i nition,pj+1is a periodic point not to be).

        Theorem 3.1σ|X is a Devaney chaotic system without a DC pair.

        Proof.It is evident from the def i nition that σ|X is transitive and has a dense set of periodic points.So σ|X is Devaney chaotic.It remains to show that σ|X contains no DC pairs.For this we let x,y∈X and ε>0 be given.We prove successively for three possible cases that {x,y}is not a DC pair.

        Case 1.{x,y}?E.

        In this case,noting that if bothandare less thanthen

        we have

        Thus,by Lemma 3.2,

        Hence

        Case 2.{x,y}?F.

        By Lemma 3.3,we know that x and y are both eventually periodic points.So for any,if σl(x)=σl(y)for some l≥0,then

        if for all l≥0,σl(x)/=σl(y),then there must exist some ε>0 such that

        Case 3.One point is in E and another in F.

        We may assume that x∈F,y∈E.By Lemma 3.3,there exists a δ>0 such that for all i≥0,

        Since

        it follows that for any i≥0,

        Thus we have

        provided that

        Then for each n,

        By Lemma 3.2,

        Whatever happens,{x,y}is not a DC pair by the def i nition.

        Theorem 3.2ent(σ|X)=0,i.e.,σ|X is not topologically chaotic.

        Proof.For given i>0,let A be a word of length|qi|.From Lemma 3.1 we may observe any i-representation of u,from which we see that A?u if and only iffor some 1≤j≤i and some 0≤m≤2|qi|.Since for 1≤j≤i,0≤m≤2|qi|,it follows that

        From Theorems 3.1 and 3.2,we obtain

        Corollary 3.1There is a Devaney chaotic system which is neither Distributively chaotic nor topologically chaotic.

        This is a unif i ed statement for some known results.

        AcknowledgmentThe authors would like to thank Professors Piotr Oprocha and Wen Huang for of f ering us valuable references.

        [1]Devaney R L.An Introduction to Chaotic Dynamical Systems.Redwood City:Addison-Wesley,1989.

        [2]Banks J,Brooks J,Cairns G,Stacey P.On the def i nition of chaos.Amer.Math.Monthly, 1992,99:332–334.

        [3]Silverman S.On maps with dense orbits and the def i nition of chaos.Rocky Mountain J.Math., 1992,22:353–375.

        [4]Schweitzer B,Smˊ?tal J.Measures of chaos and spectral decomposition of dynamical systems of the interval.Trans.Amer.Math.Soc.,1994,344:737–754.

        [5]Adler R,Konheim A,McAndrew J.Topological entropy.Trans.Amer.Math.Soc.,1965,114: 309–319.

        [6]Walters P.An Introduction to Ergodic Theory.New York:Springer-Verlag,1982.

        [7]Weiss B.Topological transtivity and ergodic measures.Math.Systems Theory,1971,5:71–75.

        [8]Blanchard F,Huang W.Entropy sets,weakly mixing sets and entropy capacity.Discrete Contin.Dynam.Syst.,2008,20:277–313.

        [9]Oprocha P.Relations between distributional and Devaney chaos.Chaos,2006,16:033112.

        [10]Forti G L,Paganoni L,Smˊ?tal J.Dynamics of homeomorphisms on minimal sets generated by triangular mappings.Bull.Austral.Math.Soc.,1999,59:1–20.

        [11]Smˊ?tal J,?Stefˊankovˊa M.Distributional chaos for triangular maps.Chaos Solitons Fractals, 2004,21:1125–1128.

        [12]Liao G F,Fan Q J.Minimal subshifts which display Schweizer-Smˊ?tal chaos and have zero topological entropy.Sci.China Ser.A,1998,41:33–38.

        [13]Pikula R.On some notions of chaos in dimension zero.Colloq.Math.,2007,107:167–177.

        tion:54H20,58F03,58F08

        A

        1674-5647(2013)02-0148-07

        Received date:Sept.30,2011.

        2013 Jilin's universities science and technology project during the 12th f i ve-year plan,and the f i nancial special funds for projects of higher education of Jilin province.

        E-mail address:chenzz77@163.com(Chen Z Z).

        无码伊人久久大香线蕉| 西西大胆午夜人体视频| 曰本极品少妇videossexhd| 欧美日韩性高爱潮视频| 日本一本二本三本道久久久| 丝袜美腿av在线观看| 日本黄网站三级三级三级| 国产精品密播放国产免费看| 国产三级在线看完整版| 不卡一本av天堂专区| 精品国内在视频线2019| 北条麻妃毛片在线视频| 亚洲中文字幕无线乱码va| 亚洲一区二区三区偷拍女| 中文字幕av一区二区三区人妻少妇| 亚洲av成人一区二区三区av| 日本第一区二区三区视频| 精品三级国产一区二区三| 国模无码一区二区三区| 国产精品美女| 亚洲天堂色婷婷一区二区| 免费国产自拍在线观看| 国产精品无码av天天爽| 国产免费播放一区二区| 免费国产不卡在线观看| 日韩人妻少妇一区二区三区| 无码一区二区三区老色鬼| 完整在线视频免费黄片| 国产女优一区在线观看| 少妇高潮惨叫久久久久久电影| 亚洲国产一区二区在线| 国产精品亚洲一区二区三区正片| 国产农村妇女精品一区| 台湾无码av一区二区三区| 精品国偷自产在线不卡短视频| 国产在线观看黄片视频免费 | 伊人久久大香线蕉av色| 亚洲熟妇av乱码在线观看| 毛片av中文字幕一区二区| av素人中文字幕在线观看| 国产真实伦在线观看|