Abstract

The definitions of Devaney chaos (DevC), exact Devaney chaos (EDevC), mixing Devaney chaos (MDevC), and weak mixing Devaney chaos (WMDevC) are extended to topological spaces. This paper proves that these chaotic properties are all preserved under topological conjugation. Besides, an example is given to show that the Li-Yorke chaos is not preserved under topological conjugation if the domain is extended to a general metric space.

1. Introduction and Preliminaries

The existence of chaotic behavior in deterministic systems has attracted researchers for many years. In engineering applications such as biological engineering, imaging, encryption, and chaos control, chaoticity of a system is an important subject for investigation. The complexity of a topological dynamical system is intensively discussed since the term chaos is introduced by Li and Yorke [1] in 1975. However, the definition of chaos in the sense of Li-Yorke is inconveniently in research of engineering applications. In 1989, Devaney [2] stated another known definition of chaos called “Devaney chaos” today. A map is said to be chaotic in the sense of Devaney (or DevC for short) on a close set if is transitive on , the set of periodic points of is dense in , and has sensitive dependence on initial conditions.

In 1992, Banks et al. [3] proved that if is transitive and has dense periodic points, then has sensitive dependence on initial conditions, where is a metric space which has no isolated point. This causes that Devaney chaos is preserved under topological conjugation on general infinite metric spaces. If sensitivity is replaced by some other dynamical properties, such as weakly mixing (WMix), mixing (Mix), or exact, then we obtain stronger notions of chaos comparing with the original one (see [47]), which are called Weak Mixing Devaney chaos (WMDevC), Mixing Devaney chaos (MDevC), and Exact Devaney chaos (EDevC), respectively.

From [7], on metric spaces, implications immediately follow from their definitions. Since an invertible map may not be topologically exact, then MDevC does not imply EDevC. In [8], Carnnrl gave a dynamical system which is WMix but not Mix on a compact metric space. And an example in [9] is constructed to show that there exists a DevC map that is not WMDevC. Hence, the inverse of (1) is not proper.

This paper extends the definitions of DevC, WMDevC, MDevC, and EDevC to topological spaces and proves that topological conjugation preserves these chaotic properties. Moreover, we use an example to show that Li-Yorke chaos is not preserved under topological conjugation on metric spaces.

Throughout this paper, let The open neighborhood system of a point is denoted by . The set of periods and periodic points of a continuous self-map are denoted by and , respectively.

Definition 1 (see [10]). A map is called a homeomorphism if it is one-to-one and onto, and both and are continuous.

Definition 2 (see [10]). Let and be two topological spaces and let and be two continuous maps. Maps and are said to be (topologically) conjugate if there exists a homeomorphism such that , where “” denotes composition of two maps. For short, we call and   -conjugate maps.

Some more results related to topological conjugation may be found in [1012].

2. Devaney Chaoticity

Throughout this section, and are two -conjugate maps defined on two topological spaces and , where is a homeomorphism.

Definition 3. The map is exact if, for every nonempty open set , there exists some such that . The map is (topological) transitive (resp., mixing) if for any two nonempty open sets , there exists some such that (resp., for all ). The map is weak mixing if is transitive on .

Definition 4. (1) The map is chaotic in the sense of Devaney if is transitive on and the set of periodic points of is dense in .
(2) The map exhibits exact Devaney chaos (resp., mixing Devaney chaos and weakly mixing Devaney chaos) if is exact (resp., mixing and weakly mixing) and chaotic in the sense of Devaney. Devaney chaos, exact Devaney chaos, mixing Devaney chaos, and weak mixing Devaney chaos are briefly denoted by DevC, EDevC, MDevC, and WMDevC, respectively.

Similarly, from these definitions, we have these implications that (1) is right and its inverse is not proper on topological spaces.

Proposition 5. The map is exact if and only if is exact.

Proof. Necessity. Given any nonempty open set in , take . Clearly, is a nonempty open set in . Since is exact, there exists an such that . Noting that and are -conjugate maps and that is a homeomorphism, it follows that This implies that is exact.
Similarly to the proof of necessity, the sufficiency follows immediately.

Proposition 6. The map is mixing if and only if is mixing.

Proof. Necessity. Given any two nonempty open sets , it is clear that and are two nonempty open sets in . Since is mixing, there exists such that This implies that Thus, is mixing.
Sufficiency can be proved similarly.

Proposition 7. The map is weakly mixing if and only if is weakly mixing.

Proof. Necessity. For any two nonempty open sets , according to the construction of product topology, it follows that there exist nonempty open sets , , , such that and . Since is weakly mixing, there exists such that This implies that Thus, is weak mixing.
Sufficiency can be proved similarly.

Theorem 8 (see [3]). The map is DevC on if and only if is DevC on .

Proof. Necessity. Similarly to the proof of Proposition 6, it can be verified that is transitive on , as is transitive. According to the definition of periodic points, it is not difficult to check that Applying this, one has This implies that .
Summing up the above discussion, it follows that is chaotic in the sense of Devaney.
Sufficiency can be proved similarly.

Applying Propositions 5, 6, and 7 and Theorem 8, the following results are straightforward.

Theorem 9. The map is EDevC if and only if is EDevC.

Theorem 10. The map is MDevC if and only if is MDevC.

Theorem 11. The map is WMDevC if and only if is WMDevC.

Remark 12. According to the results obtained in this section, it is easy to see that DevC, EDevC, MDevC, and WMDevC are all preserved under topological conjugation on metric spaces. The next section will show that this does not hold for the Li-Yorke chaos.

3. Li-Yorke Chaoticity

First, we give the definition of Li-Yorke chaos.

Definition 13 (see [13]). Let be a metric space. A continuous map is called to be chaotic in the sense of Li-Yorke if , and there exists an uncountable set such that(i) (, );(ii) ();(iii) ().

Next, we construct -map and -map and prove that they are topologically conjugative and that -map is Li-Yorke chaotic, but -map is not.

-map. Let . Define : as follows:

It is easy to see that is a metric on . Define as follows: when ; for every nature number ,

-map. Let . Define , where, for each pair , Then is a metric on . Define such that for each .

Since both and are discrete metrics on , -map and -map are both continuous.

Proposition 14. -map and -map are topologically conjugate.

Proof. Define as for any . It is easy to see that the map is a homeomorphism and that holds for any .

Proposition 15. -map is Li-Yorke chaotic.

Proof. According to the definition of -map, one has , and again for any , there exists such that and for any . This implies that
Take . Now we assert that satisfies (i), (ii), and (iii) of Definition 13.(i)For any with , we have That is, .(ii)Consider (iii)For any and any , it is easy to see that there exists a such that and that for any . Then, for any , .So, We thus conclude that -map is chaotic in the sense of Li-Yorke.

Proposition 16. -map is not Li-Yorke chaotic.

Proof. For any , with , it is clear that for any , . Then, This implies that -map is not Li-Yorke chaotic.

The following theorem holds obviously by Propositions 14, 15, and 16.

Theorem 17. For a continuous self-map which is defined on a metric space, Li-Yorke’s chaoticity is not preserved under topological conjugation.

Remark 18. Section 2 discusses some notions of “chaos” which can be defined on topological spaces and Section 3 studies Li-Yorke chaos on metric spaces. There are some other problems for further research; For example, could Li-Yorke chaos be extended to topological spaces? According to Section 3, we can conclude that even if Li-Yorke chaos may be extended to topological spaces, topological conjugation does not preserve it.

Acknowledgments

This work was financially supported by the Scientific Research Fund of Sichuan Provincial Education Department (12ZA098) and Artificial Intelligence of Key Laboratory of Sichuan Province (2012RYY04).