Volume 2011, Issue 1 838639
Research Article
Open Access

3-Adic System and Chaos

Lidong Wang

Corresponding Author

Lidong Wang

School of Science, Dalian Nationalities University, Liaoning, Dalian 116600, China dlnu.edu.cn

School of Information and Computing Science, Beifang University of Nationality, Ningxia, Yinchuan 750021, China

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Yingnan Li

Yingnan Li

Department of Mathematics, Liaoning Normal University, Liaoning, Dalian 116029, China lnnu.edu.cn

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Li Liao

Li Liao

Institute of Applied Physics and Computational Mathematics, Beijing 100094, China iapcm.ac.cn

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First published: 30 November 2011
Academic Editor: James Buchanan

Abstract

Let (Z(3), τ) be a 3-adic system. we prove in (Z(3), τ) the existence of uncountable distributional chaotic set of A(τ), which is an almost periodic points set, and further come to a conclusion that τ is chaotic in the sense of Devaney and Wiggins.

1. Introduction

In 1975, Li and Yorke introduced in [1] a new definition of chaos for interval maps. The central point in their definition is the existence of a scrambled set. Later, it was observed that positive topological entropy of interval map implies the existence of a scrambled set [2]. Many sharpened results come into being in succession (see [311]). One can find in [3, 4, 12] equivalent conditions for f to be chaotic and in [13] or [14] a chaotic map with topological entropy zero, which showed that positive topological entropy and Li-Yorke chaos are not equivalent.

By the result, it became clear that the positive topological entropy is a much stronger notion than the definition of chaos in the sense of Li and Yorke. To remove this disadvantage, Zhou [15] introduced the notion of measure center and showed importantly dynamical properties of system on its measure center. To decide the concept of measure center, he defined weakly almost periodic point, too, showing that the closure of a set of weakly almost periodic points equals to its measure center and the set of weakly almost periodic points is a set of absolutely ergodic measure 1. These show that it is more significant to discuss problems on a set of weakly almost periodic points. On the other hand, one important extensions of Li-Yorke definition were developed by Schweizer and Smítal in [16]; this paper introduced the definition of distributional chaos and prove that this notion is equivalent to positive topological entropy for interval maps. And many scholars (such as Liao, Du, and Zhou, Wang) proved that the positive topological entropy of interval map is equivalent to the uncountable Li-Yorke chaotic set and the uncountable distributional chaotic set for A(f), W(f), and R(f). Meanwhile Liao showed that the equivalent characterization is no longer valid when f acts on more general compact metric spaces.

In this paper, we discuss the existence of uncountable distributional chaotic set of A(f) in 3-adic system.

The main results are stated as follows.

Main Theorem 1. Let (Z(3), τ) be a 3-adic system. Then

  • (1)

    A(τ) contains an uncountable distributional chaotic set of τ;

  • (2)

    τ is chaotic in the sense of Devaney;

  • (3)

    τ is chaotic in the sense of Wiggins.

2. Basic Definitions and Preparations

Throughout this paper, X will denote a compact metric space with metric d, I is the closed interval [0, 1].

For a continuous map f: XX, we denote the set of almost periodic points of f by A(f) and denote the topological entropy of f by ent(f), whose definitions are as usual; fn will denote the n-fold iteration of f.

For x, y in X, any real number t and positive integer n, let
()
where we use #(·) to denote the cardinality of a set. Let
()

Definition 2.1. Call x, yX a pair of points displaying distributional chaos, if

  • (1)

    F(f, x, y, t) = 0 for some t > 0;

  • (2)

    F(f, x, y, t) = 1 for any t > 0.

Definition 2.2. f is said to display distributional chaos, if there exists an uncountable set DX such that any two different points in D display distributional chaos.

Definition 2.3. Let X be a metric space and f : XX be a continuous map. The dynamical system (X, f) is called chaotic in the sense of Devaney, if

  • (1)

    (X, f) is transitive;

  • (2)

    the periodic points are dense in X;

  • (3)

    (X, f) is sensitive to initial conditions.

Definition 2.4. Let X be a metric space and f : XX be a continuous map. The dynamical system (X, f) is called chaotic in the sense of Wiggins, if there exists a compact invariant subset YX such that

  • (1)

    fY is sensitive to initial conditions;

  • (2)

    fY is transitive.

Definition 2.5. Let (X, f) and (Y, g) be dynamical systems; if there exists a homeomorphism h : XY such that hf = gh, then f and g are said to be topologically conjugate.

The notion of adic system is defined as follows.

Definition 2.6. Put

()
We use the sequence a = a1a2⋯ to denote simply the member in Z(3). Define ρ : Z(3) × Z(3) → R as follows: for any a, bZ(3), if a = a1a2⋯, b = b1b2⋯, then
()
It is not difficult to check that ρ is a metric on Z(3) and (Z(3), ρ) is a compact abelian group. Define τ : Z(3) → Z(3) by τ(a) = a + 1 for a = a1a2 ⋯ ∈Z(3); τ or (Z(3), τ) is called the 3-adic system. (see [17])

Call an invariant closed set AI  3-adic, if the restriction fA is topologically conjugate to the 3-adic system.

Consider the following functional equation:

()
where λ∈(0,1) is to be determined, x ∈ [0,1] and f3 is the 3-fold iteration of f.

By we denote the set of continuous solutions of (2.5) such that any f satisfies: (p1) there exists α ∈ (λ, 1) such that f(α) = 0; the restrictions f[λ,α] and f[α,1] are both once continuously differentiable, and f(x) ≥ 1 on [α, 1], f(x)<−2 on [λ, α]; (p2)f(λα) < f(λ).

The following Lemma can be concluded by in [18, Theorem  2.1].

Lemma 2.7. Let 0 <λ < 1, α ∈ (λ, 1). Let f0 : [λ, 1]→[0,1] be C1 on each of the interval [λ, α] and [α, 1], and satisfy

  • (1)

    f0(α) = 0;

  • (2)

    on [λ, α] and on [α, 1];

  • (3)

    there exists α0 ∈ (α, 1) such that f0(α0) = α and α < f0(1) < α0 < f0(λ) < 1;

  • (4)

    .

Then there exists a unique f with f|[λ,1] = f0. Conversely, if f0 is the restriction on [λ, 1] of some f, then it must satisfy (1)–(4).

Proposition 2.8. .

Proof. Let λ = 2/9, α = 1/2. Define f0 : [λ, 1]→[0,1] by

()

It is not difficult to check that f0 satisfies the condition (1)–(4) in Lemma 2.7. So .

We will be concerned in the notions of Hausdorff metric and Hausdorff dimension, whose definitions can be found in [19].

Lemma 2.9 (see [19], Theorem 8.3.)Let ϕ1, ϕ2, …, ϕm be contractions on Rn. Then there exists a unique nonempty compact set E such that

()
where
()
is a transformation of subsets of Rn. Furthermore, for any nonempty compact subset F of Rn, the iterates ϕk(F) converge to E in the Hausdorff metric as k.

Lemma 2.10 (see [19], Theorem 8.8.)Let be contractions on R for which the open set condition holds; that is, there is an open interval V such that

  • (1)

    ,

  • (2)

    ϕ1(V), ϕ2(V), …, ϕm(V) are pairwise disjoint.

Moreover, suppose that for each i, there exists ri, such that |ϕi(x) − ϕi(y)| ≤ ri|xy| for all . Then dimEt, where dim(·) denotes the Hausdorff dimension and t is defined by
()

Lemma 2.11 (see [20], Theorem 3.2, [21].)Let f : II be continuous. Then the followings are equivalent:

  • (1)

    ent(f) > 0;

  • (2)

    A(f) contains an uncountable distributional chaotic set of f.

Lemma 2.12 (see [21].)Let f : XX, g : YY be continuous, where X, Y are compact metric spaces. If there exists a continuous surjection h : XY such that gh = hf, then h(A(f)) = A(g).

Lemma 2.13 (see [22].)Let ent(f) = 0 and xI be recurrent but not periodic such that f(x) > x. Then the inequality fm(x) < fn(x) holds for all even m and all odd n.

Lemma 2.14 (see [23], Theorem 6.1.4.)Let f : II be an interval map. Then ent(f) > 0 if and only if there exists a closed invariant subset ∧⊂I such that f is chaotic in the sense of Devaney.

Lemma 2.15 (see [23], Theorem 6.2.4.)Let f : II be an interval map. If ent(f) > 0, then f is chaotic in the sense of Wiggins.

3. Proof of Main Theorem

In the sequel, we always suppose that f and f take the minimum at α ∈ (λ, 1).

Let I = [0,1], f+ = f|[α,1]. For i = 0,1, 2, define ϕi : II by ϕ2(x) = λx, , . Then ϕi is a contraction for every i = 0,1, 2. Let . By Lemma 2.9, there exists a unique nonempty compact set E with
()
For simplicity, we write for .

Step 1. Prove that for any xI, fϕ0(x) = ϕ1(x), fϕ1(x) = ϕ2(x), fϕ2(x) = ϕ0f(x).

Proof. Letting f act on both sides of the equality , we get immediately the first equality. A similar argument yields the second equality. To show the third equality, we write (2.5) as f(f(f(ϕ2(x)))) = λf(x). Since ϕ2(x) ∈ [0, λ], it follows from Lemma 2.7 that fϕ2(x) ∈ [α, 1] and f2ϕ2(x) ∈ [α, 1]. By this and definitions of ϕ0 and ϕ1, we get

()

Step 2. Prove that for any subsets and , there is an n > 0 such that .

Proof. If xI, i = 0,1, 2, then f3ϕi(x) = ϕif(x) by Step 1. Using this repeatedly, we get for any k > 0

()
If for each r = 1,2, …, k, we all have ir = jr, then from (3.3),
()
(nothing that f(I) = I). Thus the lemma holds for this special case. Assume that there exists some r, 1 ≤ rk, such that iq = jq for q < r, but irjr. Then by using (3.3) repeatedly, we know that or has the form , where lq = jq for q = 1, …, r. Continuing this procedure, we must get some n, such that .

In, Steps 3, 5, and 6, we always suppose that the notation E is as in (3.1).

Step 3. Prove that

()

Proof. Since ϕ(I) ⊂ I, we have ϕk+1(I) = ϕkϕ(I) ⊂ ϕk(I) for any k > 0. So from Lemma 2.9 we get

()

Step 4. Prove that for any k > 0, is an invariant set of f, that is, f(ϕk(I)) ⊂ ϕk(I).

Proof. Note that each has the form ϕ22⋯2 or or . Then, by using Step 1 repeatedly, we have

()
Thus by f(I) ⊂ I, we have . Moreover,
()

Step 5. Prove that the restriction f|E is topologically conjugate to τ, where τ is the 3-adic system as defined in Section 1.

Proof. By the definition of ϕ, we have with this union disjoint. Then transforming by ,

()
again with a disjoint union. Thus the sets (with k arbitrary) form a net in the sense that any pair of sets from the collection are either disjoint or such that one is included in the other. It follows from Step 3 that for any a = a1a2 ⋯ ∈Z(3), if let
()
then ϕa(I) ⊂ E is nonempty, and if xE, then there exists a unique aZ(3) with xϕa(I).

We now define a map H of E onto Z(3) by setting H(x) = a if xϕa(I). Then H is well defined. It is easy to see that for each i = 0,1, 2, the contraction ratio of ϕiλ, so the contraction ratio of . It follows that diam converges to zero uniformly for ir ∈ {0,1, 2} as k (where diam denotes diameter). Thus ϕa(I) is a single point for each aZ(3). And so H is injective. Moreover the map H is continuous. Let δk > 0 be the least distance between any two of the 3k interval . If xϕα(I), yϕβ(I), and |xy| < δ, then ρ(α, β) < 3k. Finally, since f(ϕa(I)) = ϕτ(a)(I) by (3.7), we have Hf(x) = τH(x) for each xE.

Step 6. Prove that if f has an n-adic set and the n is not a power of 2, then ent(f) > 0.

Proof. Write n = k · 2m, where k ≥ 3 is odd and m ≥ 0 is an integer. Let A be the n-adic set of f and p = min A. There exists a homeomorphism H : AZ(n) such that for xA, τH(x) = Hf(x). We may assume without loss of generality that H(p) = a = 0a2a3⋯. Put

()
Then VZ(n) is an open neighborhood of the sequence a. There exists an ε > 0, such that for any qA, if qp < ε, there H(q) ∈ V. Note that for and furthermore , we have that there exists an l ≥ 0 such that
()
Let . Since we easily see that H(fs(p)) = τs(H(p)) ∈ V if and only if n divides s, it follows that , since n can not divide 2lm. And so . In particular, g(p) > p. By the same argument, we also have . In particular, g2(p) > p. Since , from (3.12), , that is, . Thus we have for the odd kl,
()
Note that a is current and nonperiodic for , and so is p for g. By Lemma 2.13 we get ent(g) > 0. Moreover ent(f) > 0.

Finally, we prove that A(τ) contains an uncountable distributional chaotic set of τ. By Step 5, the restriction fE is topologically conjugate to τ. Thus there is a homeomorphism h : Z(3) → E such that for any xZ(3),

()

According to Lemma 2.11, there is an uncountable set ∧⊂A(f), which is distributional chaotic. By Lemma 2.12 for any y ∈ ∧, there exists xA(τ) such that h(x) = y. Let

()
Then D is an uncountable set.

To complete the proof, it suffices to show that D is a distributional chaotic set for τ.

First of all, we prove that for any x1, x2D, if F(f, h(x1), h(x2), t) = 0 for some t > 0, then F(τ, x1, x2, s) = 0 for some s > 0.

For given  t > 0, by uniform continuity of h, there exists s > 0, such that for any p, qD, |h(p) − h(q)| < t, provided ρ(p, q) < s. Since we easily see that hτi = fih, it follows that if ρ(τi(x1), τi(x2)) < s, then

()
This implies
()
for any n ≥ 0. Thus by the definition of F, we immediately have the following result:
()

Secondly, we prove that if F*(f, h(x1), h(x2), s) = 1 for all s > 0, then F*(τ, x1, x2, t) = 1 for all t > 0. Since h is homeomorphism, h−1 : EZ(n) is a surjective continuous map. By the first proof, we have

()
which gives
()
By (3.18), (3.20), and the arbitrariness of x1 and x2, we conclude that D is an uncountable distributional chaotic set of τ.

The proofs of (2) and (3) of the Main Theorem are obvious.

Acknowledgments

This work is supported by the major basic research fund of Department of Education of Liaoning Province no. 2009A141 and the NSFC no. 10971245 and the independent fund of central universities no. 10010101.

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