The C1 persistence of heteroclinic repellers in Rn

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Abstract

In this paper, we show that if f is a C1-map from Rn into itself and has heteroclinic repellers, then g also has heteroclinic repellers with fgC1 being small enough and exhibits Devaney's chaos. The results demonstrate C1 structural stability of heteroclinic repellers in Euclidean spaces. In the end, we give some examples to illustrate our theoretical results.

Introduction

Research on chaotic behaviors in dynamics has attracted more and more attentions due to their potential applications in various fields (see [1], [3], [5], [7], [8], [14], [17]). Although chaotic phenomenon had previously been observed in various fields, the term “chaos” has first been introduced by Li and Yorke in 1975, where they obtained that “period three implies chaos”. When the study of chaos theory was in its infancy, Marotto generalized the work of Li and Yorke to multidimensional discrete systems and presented that snap-back repellers implies chaos [15]. Further, Blanco demonstrated that a snap-back repeller implies positive topological entropy in [2]. Later, Devaney outlined an explicit definition of chaos in 1989 [9].

From the viewpoint of differential dynamical systems, it is natural to ask whether a dynamical system with some property P still has the property P under any small perturbations. In [16], Marotto showed that the discrete system with a snap-back repeller under delayed perturbations still has chaotic behaviors. In 2009, Li et al. showed the persistence of snap-back repellers for any small C1 perturbations [10]. Chen et al. studyed the structural stability of snap-back repellers in Banach space [6]. In 2016, Chen and Li provides a sufficient condition for any small C1 perturbation of a high-dimensional difference equation to have symbolic embedding [4].

In this paper, we consider the following differential dynamical systems:x(n+1)=f(x(n)),n=1,2,, where f is a continuous map from Rn into itself. We show the persistence of the systems with heteroclinic repellers under any small C1 perturbation. We obtain that the following main result:

Theorem 3.1

Let f:RnRn be a continuously differentiable map. Suppose that f has heteroclinic repellers z1(0),z2(0),,zk(0)(k2). Then g also has heteroclinic repellers for any g with gfC1 being small enough and there exist a positive integer n and a Cantor invariant set Λ such that (gn,Λ) is topologically conjugate to the symbolic dynamical system (σ,Σ2+). Therefore g is chaotic in the sense of Devaney.

This paper is organized as follows: In Section 2, we first recall the definitions of heteroclinic repellers. Some important lemmas in the sequel are given. The main results in the paper are presented in Section 3. At the end, we give some examples to illustrate the theoretical results.

Section snippets

Definitions and lemmas

For the sake of brevity, some basic definitions and lemmas are introduced. The following definition of heteroclinic repellers for Rk was given by Lin & Chen in [13], and was extended to complete metric spaces by Li et al. in [11], [12].

Definition 2.1

[13]

Let f:RnRn be a continuous differential map. The k2 fixed points x1,x2,,xk of f are called heteroclinical repellers if the following three conditions hold:

  • (1)

    for every 1ik, xi is an expanding fixed point of f;

  • (2)

    there exist a point zi in an expanding

The persistence of heteroclinic repellers in Rn

In this section, we consider the structural stability of heteroclinic repellers under the C1-perturbation in Euclidean spaces.

Theorem 3.1

Let f:RnRn be a continuous differential map. Suppose that f has heteroclinic repellers z1(0),z2(0),,zk(0)(k2). Then g also has heteroclinic repellers for any g with gfC1 being small enough and there exist a positive integer n and a Cantor invariant set Λ such that (gn,Λ) is topologically conjugate to the symbolic dynamical system (σ,Σ2+). Therefore g is chaotic in

Examples

In this section, we will give some examples to illustrate our results and applications.

Example 4.1

Consider the one-dimensional map f(x)=x3+3x. Through a directing calculation, we have the following points:

  • (1)

    f has fixed points x1=2,x2=0,x3=2, |f(0)|=3>1,|f(±2)|=3>1; that is, f has three expanding fixed points,

  • (2)

    f is expanding in intervals (2,233),(63,63),(233,2),

  • (3)

    f(3)=0,f(0.5176)2,f2(1.81262)2.

So f has heteroclinic repellers x1,x2,x3. Thus for any C1-map h from Rn into itself, there exists a ε0

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Supported in part by the National Natural Science Foundation of P.R. China (11671410) and the Natural Science Foundation of Guangdong Province (2017A030313037, 2018A0303130120).

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