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Research article

Li-Yorke chaotic property of cookie-cutter systems

  • Received: 25 January 2022 Revised: 07 April 2022 Accepted: 11 April 2022 Published: 10 May 2022
  • MSC : 11K55, 34C28

  • In this paper, we investigate mean Li-Yorke chaos along some sequence and Li-Yorke chaos for cookie-cutter systems. By applying bounded distortion and a locally α-H¨older condition, we show that the cookie-cutter set contains a mean Li-Yorke scrambled set along some sequence in which the Hausdorff dimension equals the Hausdorff dimension of the cookie-cutter set. That is to say, a cookie-cutter system is mean Li-Yorke chaotic along some sequence. Meanwhile, we proved that every mean Li-Yorke scrambled set is also a scrambled set; hence a cookie-cutter system is also Li-Yorke chaotic.

    Citation: Alqahtani Bushra Abdulshakoor M, Weibin Liu. Li-Yorke chaotic property of cookie-cutter systems[J]. AIMS Mathematics, 2022, 7(7): 13192-13207. doi: 10.3934/math.2022727

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  • In this paper, we investigate mean Li-Yorke chaos along some sequence and Li-Yorke chaos for cookie-cutter systems. By applying bounded distortion and a locally α-H¨older condition, we show that the cookie-cutter set contains a mean Li-Yorke scrambled set along some sequence in which the Hausdorff dimension equals the Hausdorff dimension of the cookie-cutter set. That is to say, a cookie-cutter system is mean Li-Yorke chaotic along some sequence. Meanwhile, we proved that every mean Li-Yorke scrambled set is also a scrambled set; hence a cookie-cutter system is also Li-Yorke chaotic.



    The chaotic property is a characterization of the asymptotic behaviors between different orbits in the dynamical system. Until now, many versions of chaos have been studied, such as Devaney chaos [10], Li-Yorke chaos [22], distributional chaos [34] and mean Li-Yorke chaos [11]. These types of chaos are closely connected. Blanchard, Glasner, Kolyada and Maass [5] proved that positive entropy implied Li-Yorke chaos for a surjective continuous map. Huang and Ye [18] showed that Devaney chaos implies Li-Yorke chaos. Wang, Huang and Huan [36] introduced distributional chaos in a sequence, and showed that a continuous map of an interval is Li-Yorke chaotic if and only if it is distributively chaotic in a sequence. Downarowicz [11] observed that mean Li-Yorke chaos is equivalent to the DC2 chaos and proved that positive topological entropy implies mean Li-Yorke chaos. Liu, Wang and Chu [28] proved that Devaney chaos is stronger than distributional chaos in a sequence. Garcia-Ramos and Jin [16] found a new condition that implies mean Li-Yorke chaos. Cánovas [9] considered that {fn}n=1 is a sequence of continuous interval maps that converges uniformly to a continuous map f, and showed that the chaoticity of f implied that the chaoticity of {fn}n=1. Mangang [30] studied the mean equicontinuity, sensitivity, expansiveness and distality of the product dynamical systems. The reader can refer to [6,12,13,17,19,21,33,35,37], which are related to Li-Yorke chaos.

    Throughout this paper, we focus on Li-Yorke chaos and mean Li-Yorke chaos. Let us recall the definition of the scrambled set and mean Li-Yorke scrambled set.

    Let (X,ρ) be a metric space and f:XX be a self-map. The pair (X,f) is called a topological dynamical system.

    Definition 1.1. [22] Let (X,ρ) be a metric space. For two points x,yX, (x,y) is a scrambled pair for the map f:XX, if

    lim supnρ(fn(x),fn(y))>0andlim infnρ(fn(x),fn(y))=0.

    A subset SX, containing at least two points, is a scrambled set of f, if for any x,yS where xy, (x,y) is a scrambled pair for f. If a scrambled set S for f is uncountable, we say that f is chaotic in the sense of Li-Yorke.

    Definition 1.2. A subset M of X is called a mean Li-Yorke scrambled set if any two distinct points x,y in M satisfy

    lim infn1nnj=1ρ(fj(x),fj(y))=0andlim supn1nnj=1ρ(fj(x),fj(y))>0.

    A system (X,f) is said to be mean Li-Yorke chaotic, if it contains an uncountable mean Li-Yorke scrambled set.

    The sequence version of mean Li-Yorke chaos was introduced in [20].

    Definition 1.3. Let B={b1<b2<} be a strictly increasing sequence of N. According to [20], a subset M of X is called a mean Li-Yorke scrambled set along the sequence B if any two distinct points x,y in M satisfy

    lim infn1nnj=1ρ(fbj(x),fbj(y))=0andlim supn1nnj=1ρ(fbj(x),fbj(y))>0. (1.1)

    If the set M is uncountable, then we say that the system (X,f) is mean Li-Yorke chaotic along the sequence B.

    The definitions of Li-Yorke chaos, and mean Li-Yorke chaos only require that the cardinality of the chaotic set is uncountable, so a natural further question is how 'large' the size of a scrambled set can be. There are three approaches to analyze the size: topological, measure-theoretic and dimension-theoretic. In [7], Blanchard, Huang and Snoha studied the topological size of scrambled sets extensively; see also the references therein. In [2], Balibrea and Lˊopez surveyed the Lebesgue measure of scrambled sets for continuous maps on the interval. In [8], Bruin and Lˊopez studied the Lebesgue measure of scrambled sets for C2 and C3 multimodal interval maps f with non-flat critical points. In [39], Xiong proved that there exists a scrambled set of the full Hausdorff dimension for the symbolic dynamics with finite symbols. Recently, the second author and his coauthors [25,27] constructed a Li-Yorke chaotic set with full Hausdorff dimension for continued fractions and the β-transformation. Xiao [38] constructed a mean Li-Yorke chaotic set along a polynomial sequence with full Hausdorff dimension for the β-transformation. In 2021, the second author and his coauthor [26] studied the mean Li-Yorke chaotic property for continued fractions, and constructed a mean Li-Yorke chaotic set with full Hausdorff dimension for a sequence with some mild conditions.

    Both continued fractions and the β-transformations are interval mappings, which are defined on the unit [0,1). An interesting question is as follows: what about the dynamical system defined on a fractal set? For example, is a 3-adic transformation on the classical middle-third Cantor set Li-Yorke chaotic? that is to say, does the classic middle-third Cantor set contain an uncountable scrambled set?

    Motivated by the ideas and results above, we focus on the size of the scrambled set for cookie-cutter sets from the dimensional sense. We first recall the definition of the cookie-cutter mappings, which was defined and studied by Bedford [4].

    Definition 1.4. A mapping f is called a cookie-cutter map if there exists a finite collection of disjoint closed intervals I1,I2,,IqI=[0,1], such that

    (1). f is defined in qj=1Ij, the restriction of f on each Ij is 1 to 1 and surjective, the corresponding branch inverse is denoted by ϕj=(f|Ij)1:IIj;

    (2). f is differentiable becoming the H¨older continuous derivative f, i.e. there exist constants c>0 and r(0,1] such that |f(x)f(y)|c|xy|r for any x,yIj, 1jq;

    (3). f is bounded expanding in the sense that

    1<b:=infx|f(x)|supx|f(x)|:=B<+.

    The cookie-cutter set associated with f is

    C={x[0,1]:fn1(x)qj=1Ij,n1}=+k=0fk(I),

    where f0 denotes identity mapping.

    In [32], Nakata gave a method of the approximation of Hausdorff dimensions of generalized cookie-cutter Cantor sets using the thermodynamic formalism. In [23], Liang, Yu and Ren proved the existence of self-similar measures, conformal measures and Gibbs measures on cookie-cutter sets and analysed the dimension spectrum of each of these measures. Barral and Seuret [3] computed the singularity spectrum of the inverse measure of Gibbs measures on cookie-cutter sets. Baker [1] proposed a new multifractal zeta function and showed that under certain conditions the abscissa of convergence yields the Hausdorff multifractal spectrum for a class of measures supported on cookie-cutter sets. In [29], Ma, Rao and Wen defined the cookie-cutter-like sets by the limit sets of a sequence of classical cookie-cutter mappings, and they calculated the dimensions, Hausdorff and packing measures of the cookie-cutter-like sets. Liu [24] proved that for the Cookie-cutter-like dynamic system with unbounded expansion, the properties such as bounded variation and bounded distortion, the existence of a Gibbs-like measure still holds. Recently, Fan, Liao and Wu [15] studied the multifractal spectrum of some multiple ergodic averages in linear Cookie-Cutter dynamical systems.

    Let "dimH" denote the Hausdorff dimension and Hs denote the s-dimensional Hausdorff measure. Let C(X) denote the continuous functions defined on X, and P() denote the pressure function on C(X). The Hausdorff dimensions of a cookie-cutter set is given by the pressure function P().

    Theorem 1.5. [4] Suppose that C is the cookie-cutter set associatedwith f on [0,1].Then 0<Hβ(C)<+ and dimHC=β, where β is a unique real number withP(βlog|f(x)|)=0.

    The main aim of this paper is to demonstrate the Hausdorff dimensions of scrambled sets and the mean Li-Yorke scrambled set along B in cookie-cutter sets. Let'[]' denote the integer part.

    Theorem 1.6. Let G(x)=emxm+em1xm1++e1x+e0a polynomial with a degree m3 and em>0. LetB={b1<b2<}{[G(n)]:n1}be a sequence of positive integers.Let C be the cookie-cutter set associated with f on [0,1].Then there exists a meanLi-Yorke scrambled set along B in Cfor which the Hausdorff dimension equals to dimHC.

    Corollary 1.7. Let C be the cookie-cutter set associated with f on [0,1].Then there exists a scrambled set in Cfor which the Hausdorff dimension equals to dimHC.In particular, every cookie-cutter system is chaotic in the sense of Li-Yorke.

    The rest of the paper is organized as follows. In Section 2, we collect and establish some elementary properties of the Hausdorff dimension, pressure function and cookie-cutter sets that will be used later. Section 3 is devoted to proving Theorem 1.6 and Corollary 1.7. In Section 4, Theorem 1.6 is applied to a linear example and a non-linear one. Finally, the authors' conclusions are given in Section 5.

    Let A={1,2,,q} with q2. Denote the symbolic space of one-sided infinite sequences over A by

    AN={u=(u1,u2,):uiA,iN}.

    The symbol ui is called the i-th coordinate of u.

    We assign the discrete topology to A and the product topology to AN. For u,vAN, the distance d is defined by

    d(u,v)=qi,wherei=inf{j0:uj+1vj+1}.

    Denote by An the set of all n-letter words and A for the set of all finite words over A. For any u, vA, uv denotes the concatenation of u and v. For two finite words u and v, u is called the prefix of v if there exists a finite word w such that uw=v. The finite word u is called the prefix of vAN if there exists an infinite sequence wAN such that uw=v. Both of them denote uv. The symbol "||" means the diameter, the length and the absolute value with respect to a set, a word, and a real number respectively. For i,jN with i<j, we write (u|ji)=(ui,ui+1,,uj).

    The shift map σ:ANAN is defined by

    (σ(u))i=ui+1,iN.

    Let E be a subset of R; a finite or countable collection of subsets {Ui}i1 of R is called a δ-cover of a set ER if Ei1Ui and |Ui|<δ for all i1. For s0, δ0, define

    Hsδ(E)=inf{i1|Ui|s:{Ui}i1isaδcoverofE}.

    The s-dimensional Hausdorff measure of E is defined as

    Hs(E)=limδ0Hsδ(E).

    There exists a number dimHE, called the Hausdorff dimension of E, such that

    Hs(E)={ifs<dimHE,0ifs>dimHE.

    Thus

    dimHE=inf{s:Hs(E)=0}=sup{s:Hs(E)=}.

    The basics on the Hausdorff dimension can be found in [14], to which we refer the reader.

    Let α be a positive real number. We say that a map F:XR (XR) satisfies the local α-H¨older condition if there exists a real number r>0 and a constant c>0 such that, for any x,yX with |xy|<r,

    |F(x)F(y)|c|xy|α.

    The following well-known lemma can be easily deduced from the definitions of the Hausdorff dimension and the local α-H¨older condition. One can refer to [31] for more details.

    Lemma 2.1. Let X be a metric space and s, α>0 be real numbers.If a mapF:XR satisfiesthe local α-H¨older condition, then Hs(F(X))csHsα(X), where c is the constant in the definition of thelocally α-H¨older condition. Moreover, αdimH(F(X))dimH(X).

    Let f:XX and φ:XR be a continuous function. Denote

    Snφ(x)=n1i=0φ(fi(x))

    for xX. We define the pressure function P:C(X)R by

    P(φ)=limn1nlogxF(fn)eSnφ(x)

    where F(fn) denotes the set of fixed points of fn.

    In this subsection, we collect and establish some elementary properties on cookie-cutter sets. the reader can refer to [4] for more details.

    Since I1,I2,,Iq are disjoint closed intervals, as according to Definition 1.4, we can define a mapping π from {1,2,,q}N to C by

    π(a1,a2,,an,)=n>0ϕu1ϕu2ϕun(I)

    for any (a1,a2,,an,){1,2,,q}N. It can be verified that the mapping π is a continuous bijection.

    For w=u1u2un{1,2,,q}n, define the basic interval of the order n corresponding to w by

    I(w)=I(u1u2un)=ϕu1ϕu2ϕun(I).

    For example, when n=1, I(i)=ϕi(I)=Ii for 1iq.

    The following diagram is commutative, that is, fπ=πσ. Since π is bijective, the equation π1f=σπ1 also holds.

    Remark 2.2. (1). Since I1,I2,,Iq are disjoint closed intervals, as according to Definition 1.4, the distance of between two intervals ρ(Ii,Ij)>0 for any 1ijq; then, denote ρmin=min1ijqρ(Ii,Ij).

    (2). According to the condition (3) of Definition 1.4, the map f is monotonous on each Ij(1jq).

    (3). For any n and any w{1,2,,q}n, |I(w)|1bn.

    The following lemmas are useful for proving Theorem 1.6.

    Lemma 2.3. [14]Let C be a cookie-cutter set andρmin=min1ijqρ(Ii,Ij).For any w{1,2,,q}, there existsa constant d1 such that

    ρmind1|I(w)|ρ(I(wi),I(wj))|I(w)|,

    for any 1ijq.

    Lemma 2.4. [14](bounded distortion)Let C be a cookie-cutter set associated with f on [0,1].There exists a constant K1>0 such that for any N1 andany x,yI(w), w{1,2,,q},

    K11|(fN)(x)||(fN)(y)|K1.

    The idea of proving Theorem 1.6 is to construct a mean Li-Yorke scrambled set in the symbolic space {1,,q}N, then project such set onto the unit interval [0,1] where the projection is a mean Li-Yorke scrambled set along B, and finally calculate the Hausdorff dimension of the projection set.

    Actually, the idea for constructing a mean Li-Yorke scrambled set was inspired by [28]. In the following, we write Σq={1,2,,q}N.

    We define a positive integer sequence {ck}k1 such that c1=1 and c2=2c1 for any k2 and

    c2k1=c1+c2++c2k2

    and

    c2k=2c1+c2++c2k2+c2k1.

    Let

    J1={jN:2k1i=1ci<j2ki=1ciforsomek1}

    and

    J2={jN:2ki=1ci<j2k+1i=1ciforsomek1}.

    For u=(u1,u2,)Σq, and denote (1j)=(111j), we set a sequence of finite words {Vj(u)}j1 as follows.

    Vj(u)={u1ifj=1,1jifjJ1,u1u2ujifjJ2.

    Recall that B={bj}j1, (v|ji)=(vi,vi+1,,vj) and |v|ji|=ji+1. For u=(u1,u2,)Σq, we define a mapping g:ΣqΣq by

    g(u)=(u|b11,V1(u),u|b2|V1(u)|b1+1,V2(u),,Vn1(u),u|bnn1i=1|Vi(u)|bn1n2i=1|Vi(u)|+1,Vn(u),)

    Denote W1(u)=u|b11, and Wn(u)=u|bnn1i=1|Vi(u)|bn1n2i=1|Vi(u)|+1 for any n2. The mapping g:ΣqΣq can be written as:

    g(u)=(W1(u),V1(u),W2(u),V2(u),,Vn1(u),Wn(u),Vn(u),).

    Remark 3.1. (1). The mapping g is continuous and injective.

    (2). For jJ1, σbj(g(u))=(1j,Wj+1(u),Vj+1(u),).

    (3). For jJ2, σbj(g(u))=(u1u2uj,Wj+1(u),Vj+1(u),).

    Remark 3.2. (1). When j+, the length of the finite word 1j tends to infinity which can guarantee the equality of (1.1).

    (2). For u,vΣq with uv, there exists k1 such that ukvk. For jJ2 and j+, uk and vk appear infinitely in Vj(u) and Vj(u) which can guarantee the inequality of (1.1).

    Let M:=g(Σq). Recall that the mapping π from {1,2,,q}N to C is

    π(a1,a2,,an,)=n>0ϕu1ϕu2ϕun(I)

    for any (a1,a2,,an,)Σq, and that the equation fπ=πσ holds.

    The following lemma indicates π(M) is a mean Li-Yorke scrambled set of f on C.

    Lemma 3.3. The set π(M) is a mean Li-Yorkescrambled set along B of f on C.

    Proof. For any u,vM with uv, we shall show that (π(u),π(v)) is a mean Li-Yorke scrambled pair for f.

    Since the map π is continuous and satisfies fπ=πσ, we obtain

    |fbjπ(u)fbjπ(v)|=|π(σbj(u))π(σbj(v))|.

    (1). Lowerlimits. Taking n=2ki=1ci, since |π(σbj(u))π(σbj(v))|1 for 1jnc2k, we get

    nj=1|π(σbj(u))π(σbj(v))|nc2k+nj=nc2k+1|π(σbj(u))π(σbj(v))|.

    By Remark 2.2(3) and Remark 3.1(2),

    nj=nc2k+1|π(σbj(u))π(σbj(v))|nj=nc2k+1|I(1j)|nj=nc2k+1bj1b1.

    Therefore

    1nnj=1|fbjπ(u)fbjπ(v)|nc2k+1b1n.

    Note that c2k=22k1i=1ci and n=2ki=1ci; taking the lim inf gives

    lim infn1nnj=1|fbjπ(u)fbjπ(v)|=0.

    (2). Upperlimits.

    For any u,vM with uv, there exists ξηΣq satisying g(ξ)=u and g(η)=v. Since the mapping g is injective, it follows that ξη. Let t1 be the least positive integer such that ξtηt and ξi=ηi for any 1it1.

    For k>t large enough, taking n=2k+1i=1ci, we obtain

    nj=1|π(σbj(u))π(σbj(v))|nj=nc2k+1+1|π(σbj(u))π(σbj(v))|

    By Remark 3.1(3), for jJ2,

    σbj(u)=σbj(g(ξ))=(ξ1ξ2ξj,Wj+1(ξ),Vj+1(ξ),)

    and

    σbj(v)=σbj(g(η))=(η1η2ηj,Wj+1(η),Vj+1(η),).

    When nc2k+1+1jn, it follows that jJ2 and j>t. By the definition of g, the distinct symbols ξt and ηt appear infinitely often in the same location of g(ξ) and g(η) respectively. Hence

    nj=nc2k+1+1|π(σbj(u))π(σbj(v))|nj=nc2k+1+1ht=c2k+1ht,

    where ht=ρ(I(ξ1ξ2ξt),I(η1η2ηt))ρmind1|I(ξ1ξ2ξt1)|. Therefore

    1nnj=1|fbjπ(u)fbjπ(v)|c2k+1htn.

    Note that c2k+1=2ki=1ci and n=2k+1i=1ci=2c2k+1, taking the lim sup gives

    lim supn1nnj=1|fbjπ(u)fbjπ(v)|=ht2>0.

    Note that π(M)C, so we have dimHπ(M)dimHC.

    Consider a mapping h:π(M)C defined by

    h(a)=πg1π1(a),

    for aπ(M). Since π is continuous and bijective from Σq to C and the mapping g is continuous and bijective from Σq to M, the mapping h is a continuous bijection on π(M).

    Proposition 3.4. We have dimHπ(M)dimHC.

    By Lemma 2.1, Proposition 3.4 is the corollary of the following lemma.

    Lemma 3.5. For any ϵ>0, the mapping h satisfies the local 11+ϵ-H¨older condition.

    Before proving Lemma 3.5, we make use of a kind of symbolic space described as follows:

    For any n1, we can check that

    π(M)=n1(u1,u2,,un)AnI(u1,u2,,un),

    where

    An={(u1,u2,,un){1,,q}n:(u1,,un)=(x1,,xn),(x1,x2,)M}.

    For any n1, let t(n) be the sum of the length of all of the inserted pieces before the element in the position of n for any g(u)M, that is,

    t(n)={0if1nb1,nb1ifb1+1nb1+|V1(u)|,kj=1|Vj(u)|ifbk+|Vk(u)|+1nbk+1forsomek1,k1j=1|Vj(u)|+nbkifbk+1nbk+|Vk(u)|forsomek2.

    Since

    t(bk+1)=kj=1|Vj(u)|=kj=1j=k(k+1)2,

    according to the condition of Theorem 1.6, G(x)=emxm+em1xm1++e0 is a polynomial with degree m3 and B={b1<b2<}{[G(n)]:n1}; thus, we have limkt(bk+1)bk=0.

    For any n>1, there exists l1 such that bln<bl+1; thus, t(n)nt(bl+1)bl, which implies limnt(n)n=0.

    For any finite word (u1,u2,,un), let ¯(u1,u2,,un) be the finite word by eliminating the finite words {Vj(u)}j1. Then

    ¯(u1,u2,,un){1,2,,q}nt(n).

    The word ¯(u1,u2,,un) has different cases for n and t(n), that is,

    ¯(u1,u2,,un)=¯(u|n1)={(u|n1)if1nb1,(u|b11)ifb1+1nb1+|V1(u)|,(u|nkj=1|Vj(u)|1)ifbk+|Vk(u)|+1nbk+1forsomek1,(u|bkk1j=1|Vj(u)|1)ifbk+1nbk+|Vk(u)|forsomek2.

    For any u=(u1,u2,),v=(v1,v2,)M and uv, there exists n1 such that (u1,,un)=(v1,,vn) and un+1vn+1.

    Lemma 3.6. We have |π(u)π(v)|ρmind1|I(u1,,un)|where d1 is defined in Lemma 2.3.

    Proof. Applying Lemma 2.3, we immediately obtain the conclusion.

    Proof of Lemma 3.5:

    According to Lagrange's mean value theorem, for any n and any finite word (u1,,un), there exist ξI(u1,,un) and ηI¯(u1,,un) such that

    (fn)(ξ)|I(u1,,un)|=1

    and

    (fnt(n))(η)|I¯(u1,,un)|=1.

    Recall that uv means that u is the prefix of v. By the form of g(u),

    g(u)=(W1(u),V1(u),W2(u),V2(u),,Wn(u),Vn(u),)

    for any n>1; thus, we can find the maximum integer n0, where n02n+1, satisfying

    (W1(u),V1(u),,Wn0(u),Vn0(u))g(u)|n1

    and

    g(u)|n1(W1(u),V1(u),,Wn0+1(u),Vn0+1(u)).

    We denote the location of the finite word Wi(u) (1in0+1) by [N2i2,N2i1] and

    R=[1,n]n0+1i=1[N2i2,N2i1].

    Let ϵ>0; then, by limnt(n)n=0, there exists K=K(ϵ) such that

    Bt(n)Kn0+11<b(nt(n))ϵ

    for any nK, where b is the lower bound and B is the upper bound in Definition 1.4, and K1 is defined as Lemma 2.4.

    For any (u1,u2,,un)An with nK,

    |I(u1,u2,,un)|=1(fn)(ξ)=1n1k=0f(fk(ξ))1Bt(n)10kn1,kRf(fk(ξ))=1Bt(n)11kn0+1(fN2k1N2k2+1)(fN2k2(ξ))=1Bt(n)(fnt(n))(η)|I¯(u1,,un)|1kn0+1(fN2k1N2k2+1)(fN2k2(ξ))1Bt(n)1Kn0+11|I¯(u1,,un)|1b(nt(n))ϵ|I¯(u1,,un)||I¯(u1,,un)|1+ϵ

    where the first inequality holds according to the condition (3) of Definition 1.4, the second inequality holds by Lemma 2.4, and the last inequality holds according to (3) of Remark 2.2.

    Let r<ρmind1min(u1,,uK)AK|I(u1,,uK)|. For any π(v)(π(u)r,π(u)+r), there exists n such that (u1,,un)=(v1,,vn) and un+1vn+1; then

    |h(π(u))h(π(v))|=|πg1π1(π(u))πg1π1(π(v))||I¯(u1,,un)||I(u1,,un)|11+ϵ(ρmind1)11+ϵ|π(u)π(v)|11+ϵ

    where the last inequality holds by Lemma 3.6.

    Proof of Theorem 1.6: Proposition 3.4 implies that dimHπ(M)=dimHC.

    The following lemma indicates that every mean Li-Yorke scrambled set along B is a scrambled set. Hence Corollary 1.7 is proved by Theorem 1.6 and Lemma 3.7.

    Lemma 3.7. Let (X,ρ) be a metric space and f:XX be aself-map. Suppose that M isa mean Li-Yorke scrambled set along some sequenceBN; then, M is a scrambled set of f.

    Proof.

    For any x,yM with xy, that is, x and y satisfy the condition (1.1), the proof is divided into two parts.

    (1). Suppose that

    lim supnρ(fn(x),fn(y))=0.

    Thus

    limnρ(fn(x),fn(y))=0,

    that is, we have

    limnρ(fbn(x),fbn(y))=0,

    and

    limn1nnj=1ρ(fbj(x),fbj(y))=0.

    Therefore

    lim supn1nnj=1ρ(fbj(x),fbj(y))=0.

    This is a contradiction. So lim supnρ(fn(x),fn(y))>0.

    (2). Given

    lim infnρ(fn(x),fn(y))>0,

    there exist a constant δ>0 and an integer N>1 such that, for any nN, we have

    ρ(fn(x),fn(y))>δ.

    Therefore,

    1nnj=1ρ(fbj(x),fbj(y))(nN)δn,

    which implies that

    lim infn1nnj=1ρ(fbj(x),fbj(y))>δ>0.

    This is also a contradiction. Hence, lim infnρ(fn(x),fn(y))=0.

    Combining (1) and (2), we know that M is a scrambled set of f.

    In this section, we give a linear example and a non-linear one by applying Theorem 1.6.

    Firstly, we recall the classical middle-third Cantor set C as follows.

    Let I=[0,1], I0=[0,1/3] and I2=[2/3,1]. Define the mapping f:I0I2I by

    f(x)={3x,xI0,3x2,xI2,

    where '' denotes the disjoint union. We can check that C1/3=+k=0fk(I) is a cookie-cutter set.

    On the symbolic space {0,2}N, we can define the projection mapping π:{0,2}N[0,1] by

    π(x1,x2,)=+i=1xi3i

    for (x1,x2,){0,2}N. The middle-third Cantor set can also be described by the projection mapping π, that is,

    C1/3=π({0,2}N)={x[0,1):x=+i=1xi3i,xi{0,2},i1}.

    It is well known that dimHC1/3=log2log3; thus, applying Theorem 1.6, the middle-third Cantor set contains a scrambled set for which the Hausdorff dimension is log2log3.

    The example in Section 4.1 is piecewise linear. Here, we give a non-linear one that is from [14].

    Let I=[0,1]. Define the mappings ϕ1 and ϕ2 from I to I as

    ϕ1(x)=13x+110x2,ϕ2(x)=13x+23110x2.

    Then

    f(x)={ϕ11(x),xϕ1(I),ϕ12(x),xϕ2(I).

    We can check that C=+k=0fk(I) is a cookie-cutter set. By Theorem 1.5, dimHC is the unique solution of P(βlog|f(x)|)=0.

    Applying Theorem 1.6, we see that the above cookie-cutter set contains a scrambled set for which the Hausdorff dimension equals to dimHC.

    In this paper, we demonstrated the Li-Yorke chaos of the cookie-cutter sets. In fact, according to the definitions of scrambled sets and mean Li-Yorke scrambled sets along the sequence B, mean Li-Yorke chaos along the sequence B is stronger than Li-Yorke chaos. Downarowicz [11] observed that mean Li-Yorke chaos is equivalent to the DC2 chaos and proved that positive topological entropy implies mean Li-Yorke chaos for a continuous interval map. A natural question is below.

    Question 5.1. Is every cookie-cutter system mean Li-Yorke chaotic?

    In this paper, we demonstrated mean Li-Yorke chaos along some sequence and Li-Yorke chaos for cookie-cutter system. For a given polynomial sequence B, by constructing a mean Li-Yorke scrambled set along B, we prove that the cookie-cutter set contains a mean Li-Yorke scrambled set along B for which the Hausdorff dimension equals the Hausdorff dimension of the cookie-cutter set. That is to say, cookie-cutter system is mean Li-Yorke chaotic along B. Meanwhile, we proved that every mean Li-Yorke scrambled set is also a scrambled set, hence, cookie-cutter system is also Li-Yorke chaotic.

    This work was supported by the Scientific Research Project of Guangzhou Municipal Colleges and Universities grant no.202032802, and Science and Technology Projects in Guangzhou grant no.202102021152.

    The authors declare no conflict of interest.



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