<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2020.86075</article-id><article-id pub-id-type="publisher-id">JAMP-100623</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Some Chaotic Properties of a Kind of Coupled Map Lattices
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xiaofang</surname><given-names>Yang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tianxiu</surname><given-names>Lu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Guo</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Artificial Intelligence Key Laboratory of Sichuan Province, Zigong, China</addr-line></aff><aff id="aff1"><addr-line>Department of Mathematics and Statistics, Sichuan University of Science and Engineering, Zigong, China</addr-line></aff><pub-date pub-type="epub"><day>29</day><month>05</month><year>2020</year></pub-date><volume>08</volume><issue>06</issue><fpage>968</fpage><lpage>975</lpage><history><date date-type="received"><day>7,</day>	<month>May</month>	<year>2020</year></date><date date-type="rev-recd"><day>28,</day>	<month>May</month>	<year>2020</year>	</date><date date-type="accepted"><day>1,</day>	<month>June</month>	<year>2020</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p><html>
 <head></head>
 
  This paper is concerned with some chaotic properties of a kind of coupled map lattices, which is proposed by Kaneko. First, this research discussed the sensitivity, infinite sensitivity, transitivity, accessibility, densely Li-Yorke sensitivity and exact of coupled map lattices. Then, some sufficient conditions under which 
  <img src="Edit_c0fc315a-d176-4c9e-9e41-5cb6bc6d679d.bmp" alt="" /> is Kato chaotic, positive entropy chaotic and Ruelle-Takens chaos are obtained.
 
</html></p></abstract><kwd-group><kwd>Coupled Map Lattices</kwd><kwd> Sensitivity</kwd><kwd> Chaos</kwd><kwd> Accessibility</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In 1983, Kaneko [<xref ref-type="bibr" rid="scirp.100623-ref1">1</xref>] proposed coupled map lattices (Short for CMLs). Then, in biophysics, materials, chaos, image processing, CMLs are intensively discussed (Refer to literature [<xref ref-type="bibr" rid="scirp.100623-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.100623-ref8">8</xref>] and others). In 2005, the literature [<xref ref-type="bibr" rid="scirp.100623-ref9">9</xref>] showed that CMLs have some topology and ergodic properties. In 2010, Juan Lu [<xref ref-type="bibr" rid="scirp.100623-ref10">10</xref>] presented a definition of distributional chaos on a sequence (DCS) for CML systems and stated two different sufficient conditions for having DCS. In 2010, Juan Luis [<xref ref-type="bibr" rid="scirp.100623-ref11">11</xref>] proved that this CML system has positive topological entropy for zero coupling constant. In 2016, Risong Li [<xref ref-type="bibr" rid="scirp.100623-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.100623-ref13">13</xref>] had obtained some relevant conclusions for the zero coupling constant and proved that the system has three kinds of chaos. In this paper, the following CML from [<xref ref-type="bibr" rid="scirp.100623-ref14">14</xref>] is considered.</p><p>x m + 1, n = ( 1 − ε ) f ( x m , n ) + ε f ( x m , n − 1 ) (1)</p><p>where x m , n ∈ I , m ∈ ℕ 0 = { 0,1,2, ⋯ } , n ∈ ℤ = { ⋯ , − 1,0,1, ⋯ } , I is a non-degenerate compact interval, f is a map on I, and ε ∈ [ 0,1 ] is a constant.</p><p>For t ∈ ℤ , let ℕ t = { t , t + 1, ⋯ } and Ω = { ( 0 , n ) : n ∈ ℤ } = { ⋯ , ( 0 , − 1 ) , ( 0 , 0 ) , ( 0 , 1 ) , ⋯ } . For any sequence ϕ = { ϕ 0, n } ∞ ∞ on Ω , by induction, one can obtain a double-indexed sequence x = { x m , n : m = 0 , 1 , 2 , ⋯ ; n = ⋯ , − 1 , 0 , 1 , ⋯ } , which is said to be a solution of the above system (1) with initial condition ϕ .</p><p>Let I be a subset of real number set, write</p><p>I ∞ ∞ = { { a n } n = − ∞ ∞ = ( ⋯ , a − 1 , a 0 , a 1 , ⋯ ) : a n ∈ I , n ∈ ℤ }</p><p>and</p><p>Δ ∞ ∞ = { ( ⋯ , a − 1 , a 0 , a 1 , ⋯ ) : a i = a j ∈ I , i , j ∈ ℤ }</p><p>which is called the diagonal set of I ∞ ∞ .</p><p>For arbitrary, two sequences x 1 = { x 1 , n } n = − ∞ ∞ , x 2 = { x 2 , n } n = − ∞ ∞ ∈ I ∞ ∞ , it is easy to prove that</p><p>d ( x 1 , x 2 ) = sup { | x 1 , n − x 2 , n | : n = ⋯ , − 1 , 0 , 1 , ⋯ } (2)</p><p>is a metric on I ∞ ∞ .</p><p>Let f : I ↦ I be a continuous map and x = { x m , n : m ∈ ℕ 0 , n ∈ ℤ } be a solution of the above system (1) with initial condition ϕ = { ϕ 0 , n } ∞ ∞ ∈ I ∞ ∞ .</p><p>Let</p><p>x m = { x m , n } n = − ∞ ∞ = ( ⋯ , x m , − 1 , x m , 0 , x m , 1 , ⋯ ) , ∀ m ∈ ℕ 0 ,</p><p>and</p><p>x m + 1 = { x m + 1 , n } n = − ∞ ∞ = ( ⋯ , x m + 1 , − 1 , x m + 1 , 0 , x m + 1 , 1 , ⋯ ) = F ( x m ) , ∀ m ∈ ℕ 0 ,</p><p>where x 0 = ϕ = { x 0 , n = ϕ 0 , n } n = − ∞ ∞ and</p><p>x m + 1, n = ( 1 − ε ) f ( x m , n ) + ε f ( x m , n − 1 ) , ∀ m ∈ ℕ 0 , n ∈ ℤ .</p><p>Then, one can see that the above system (1) is equivalent to the following system</p><p>x m + 1 = F ( x m ) , x m ∈ I ∞ ∞ , m = 0 , 1 , 2 , ⋯ (3)</p><p>For the above system (3), the map F is said to be induced by the system (1). Obviously, a double-indexed sequence { x m , n : m ∈ ℕ 0 , n ∈ ℤ } is a solution of the above system (1) if and only if the sequence { x m = { x m , n } n = − ∞ ∞ : m ∈ ℕ 0 } m = 0 ∞ is a solution of the above system (3).</p><p>Next section, the definitions of sensitive, infinite sensitive, transitive, accessibility, densely Li-Yorke sensitive and exact will be reviewed. And then, in section 3, it is proved that the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) satisfies three definitions of chaos (Kato chaotic, positive entropy chaotic and Ruelle-Takens chaos) under the conditions that f is chaos in these sense.</p></sec><sec id="s2"><title>2. Preliminaries</title><p>After T. Y. Li and J. A. Yorke [<xref ref-type="bibr" rid="scirp.100623-ref15">15</xref>] first put forward the mathematical definition of “chaos”, many other definitions of chaos appeared later. For example, sensitivity, infinite sensitivity, transitivity, accessibility, densely Li-Yorke sensitivity, Kato chaotic, positive entropy chaotic, Ruelle-Takens chaos, and so on.</p><p>Definition 1. Let ( X , ρ ) be a metric space and f : X ↦ X be a continuous function. f is said to be</p><p>1) transitive if for any nonempty open subsets U 1 , U 2 ⊂ Y , f n ( U 1 ) ∩ U 2 ≠ ∅ for some integer n ∈ ℕ (see [<xref ref-type="bibr" rid="scirp.100623-ref16">16</xref>]).</p><p>2) sensitive if there exist η &gt; 0 such that for any x ∈ X and ε &gt; 0 , there exists y ∈ B ( x , ε ) and n ∈ ℕ such that ρ ( f n ( x ) , f n ( y ) ) (see [<xref ref-type="bibr" rid="scirp.100623-ref17">17</xref>]).</p><p>3) infinitely sensitive if there exist η &gt; 0 such that for any x ∈ X and ε &gt; 0 , there exists y ∈ B ( x , ε ) and n ∈ ℕ such that lim sup n → ∞ ρ ( f n ( x ) , f n ( y ) ) ≥ η (see [<xref ref-type="bibr" rid="scirp.100623-ref17">17</xref>]).</p><p>4) accessible if for any ε &gt; 0 and any two nonempty open subsets U 1 , U 2 ⊂ X , there are two points x ∈ U 1 and y ∈ U 2 such that ρ ( f n ( x ) , f n ( y ) ) &lt; ε for some integer n &gt; 0 (see [<xref ref-type="bibr" rid="scirp.100623-ref16">16</xref>]).</p><p>5) exact if for any open subset U ⊂ X , there is m ∈ ℕ such that f m ( U ) = X (see [<xref ref-type="bibr" rid="scirp.100623-ref18">18</xref>]).</p><p>Remark 1. [<xref ref-type="bibr" rid="scirp.100623-ref19">19</xref>] There is another equivalent definition of transitivity. f : X ↦ X is said to be transitivity, if there is an x 0 ∈ X such that O r b f ( x 0 ) &#175; = X . Where, O r b f ( x 0 ) &#175; = { f n ( x 0 ) | n = 0 , 1 , 2 , ⋯ } is called the orbit of the point x 0 .</p><p>Definition 2. 1) A dynamic system ( X , f ) (or the map f : X → X ) is Li-Yorke sensitive, if for any x ∈ X has x ∈ Q δ ( f ) for some δ &gt; 0 .</p><p>2) A dynamic system ( X , f ) (or the map f : X → X ) is densely Li-Yorke sensitive if Q δ ( f ) is dense in X for some δ &gt; 0 . Among them,</p><p>Q δ ( f ) = { x ∈ X : ∀ ε &gt; 0 , ∃ y ∈ B ( x , ε )   such   that   ( x , y ) ∈ L Y ρ ( f , δ ) }</p><p>L Y ρ ( f , δ ) = { ( x , y ) ∈ X &#215; X : lim sup n → ∞ ρ ( f n ( x ) , f n ( y ) ) &gt; δ                                   and   lim inf n → ∞ ρ ( f n ( x ) , f n ( y ) ) = 0 }</p><p>Definition 3. 1) A dynamic system ( X , f ) (or the map f : X → X ) is Kato chaotic if it is sensitive and accessible (see [<xref ref-type="bibr" rid="scirp.100623-ref20">20</xref>]).</p><p>2) A dynamic system ( X , f ) (or the map f : X → X ) is chaotic in the sense of Ruelle and Takens (short for R-T chaotic) if it is transitive and sensitive (see [<xref ref-type="bibr" rid="scirp.100623-ref21">21</xref>]).</p><p>Proposition 1. A dynamic system ( X , f ) (or the map f : X → X ) is Li-Yorke sensitive if and only if P δ ( f ) &#175; = X for some δ &gt; 0 . Among them,</p><p>P δ ( f ) = { x ∈ X : ∀ ε &gt; 0, ∃ y ∈ B ( x , ε ) , ∃ n ∈ ℕ   such   that   ρ ( f n ( x ) , f n ( y ) ) &gt; δ }</p><p>Proposition 2. [<xref ref-type="bibr" rid="scirp.100623-ref17">17</xref>] A dynamical system ( X , f ) is infinitely sensitive if and only is it is sensitive.</p><p>Proposition 3. [<xref ref-type="bibr" rid="scirp.100623-ref22">22</xref>] A dynamical system ( X , f ) is dense Li-Yorke sensitivity, then it is Topological mixing (or its topological entropy is positive).</p></sec><sec id="s3"><title>3. Main Results</title><p>In this section, let X = I . The metric ρ in I is defined by ρ ( a , b ) = | a − b |     ( ∀ a , b ∈ I ) . The metric d in I ∞ ∞ is defined by (2).</p><p>Theorem 1. If f is transitive, then the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is transitive.</p><p>Proof. Since f is transitive, then there exist a ∈ I satisfying O r b f ( a ) &#175; = I . Then for any b ∈ I and any ε &gt; 0 , B ( b , ε ) ∩ O r b f ( a ) ≠ ∅ . That is, there exists a k 0 &gt; 0 such that ρ ( f k 0 ( a ) , b ) = | f k 0 ( a ) − b | &lt; ε . Take x 0 = ( ⋯ , a , a , a , ⋯ ) ∈ Δ ∞ ∞ . It is easy to see, for any k ∈ ℕ , F k ( x 0 ) = { f k ( a ) } n = − ∞ ∞ . Then, O r b F ( x 0 ) = { f k ( a ) } n = − ∞ ∞ | k ∈ ℕ . For any y = ( ⋯ , b , b , b , ⋯ ) ∈ Δ ∞ ∞ and above k 0 &gt; 0 ,</p><p>d ( F k 0 ( x 0 ) , y ) = sup { | f k 0 ( a ) − b | : n ∈ ℕ } = | f k 0 ( a ) − b | &lt; ε .</p><p>So, B ( y , ε ) ∩ O r b F ( x 0 ) ≠ ∅ .</p><p>Thus, the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is transitive.</p><p>Theorem 2. If f is sensitive, then the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is sensitive.</p><p>Proof. Take Δ ∞ ∞ = { ( ⋯ , x − 1 , x 0 , x 0 , ⋯ ) : x n = a ∈ I , n ∈ ℤ } ⊂ I ∞ ∞ , ∀ x = { ⋯ , a , a , a , ⋯ } , y = { ⋯ , b , b , b , ⋯ } ∈ Δ ∞ ∞ , x ≠ y . It is easy to know that, for ∀ k ∈ ℕ ,</p><p>F k ( x ) = { f k ( a ) } n = − ∞ ∞ , F k ( y ) = { f k ( b ) } n = − ∞ ∞ .</p><p>So, for ∀ k ∈ ℕ ,</p><p>d ( F k ( x ) , F k ( y ) ) = d ( { f k ( a ) } n = − ∞ ∞ , { f k ( b ) } n = − ∞ ∞ ) = sup { | f k ( a ) − f k ( b ) | , k = ⋯ , − 1 , 0 , 1 , ⋯ } = | f k ( a ) − f k ( b ) | .</p><p>Since f is Sensitive, so there exists a ε 0 &gt; 0 such that for any p ∈ I and any δ &gt; 0 , there exists a q p , δ ∈ B ( p , δ ) and n p , δ ∈ ℕ such that | f n p , δ ( p ) , f n p , δ ( q p , δ ) | &gt; ε 0 . So for any fixed x = ( ⋯ , p , p , p , ⋯ ) ∈ Δ ∞ ∞ and any δ &gt; 0 , taking y = ( ⋯ , q p , δ , q p , δ , q p , δ , ⋯ ) ∈ Δ ∞ ∞ , one has that,</p><p>d ( x , y ) = sup { ⋯ , | p − q p , δ | , | p − q p , δ | , | p − q p , δ | , ⋯ } = | p − q p , δ | &lt; δ ,</p><p>that is y ∈ B ( x , δ ) . And because</p><p>d ( F n p , δ ( x ) , F n p , δ ( y ) ) = | f n p , δ ( p ) − f n p , δ ( q p , δ ) | &gt; ε 0 ,</p><p>so F | Δ ∞ ∞ is sensitive.</p><p>Corollary 1. If f is chaotic in the sense of Ruelle and Takens, then the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is chaotic in the sense of Ruelle and Takens.</p><p>Proof. According to Theorem 1, Theorem 2 and the definition of R-T chaos, the conclusion is obvious.</p><p>According to Proposition 2 and Theorem 2, the following Corollary is hold.</p><p>Corollary 2. If f is infinitely sensitive, then the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is sensitive.</p><p>In fact, there is a stronger conclusion.</p><p>Theorem 3. If f is infinitely sensitive, then the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is infinitely sensitive.</p><p>Proof. Since f is infinitely sensitive, then there exists a δ &gt; 0 such that for any a ∈ I and any ε , there exists b a , ε ∈ B ( a , ε ) and n a , ε ∈ ℕ such that lim sup n a , ε → ∞ ρ ( f n a , ε ( a ) , f n a , ε ( b a , ε ) ) ≥ δ . So for any fixed x = ( ⋯ , a , a , a , ⋯ ) ∈ Δ ∞ ∞ , and any ε &gt; 0 , taking x = ( ⋯ , b a , ε , b a , ε , b a , ε , ⋯ ) ∈ Δ ∞ ∞ , one has that</p><p>d ( x , y ) = sup { ⋯ , | a − b a , ε | , | a − b a , ε | , | a − b a , ε | , ⋯ } = | a − b a , ε | &lt; ε ,</p><p>that is y ∈ B ( x , ε ) . And because</p><p>lim sup n a , ε d ( F n a , ε ( x ) , F n a , ε ( y ) ) = lim sup n a , ε → ∞ d ( f n a , ε ( a ) , f n a , ε ( b a , ε ) ) ≥ δ .</p><p>So F | Δ ∞ ∞ is infinitely sensitive.</p><p>Theorem 4. If f is accessible, then the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is accessible.</p><p>Proof. For any open subset</p><p>( Δ 1 ) ∞ ∞ = { ( ⋯ , x − 1 , x 0 , x 1 , ⋯ ) , x n = a ∈ U 1 ⊂ I , n ∈ ℤ } ⊂ I ∞ ∞</p><p>and</p><p>( Δ 2 ) ∞ ∞ = { ( ⋯ , y − 1 , y 0 , y 1 , ⋯ ) , y n = b ∈ U 2 ⊂ I , n ∈ ℤ } ⊂ I ∞ ∞ ,</p><p>since f is accessible, then, for the above U 1 , U 2 ⊂ I , there exist a ∈ U 1 , b ∈ U 2 such that</p><p>ρ ( f k ( a ) , f k ( b ) ) = | f k ( a ) − f k ( b ) | &lt; ε</p><p>for some k &gt; 0 . Take</p><p>x = ( ⋯ , a , a , a , ⋯ ) ∈ ( Δ 1 ) ∞ ∞ , y = ( ⋯ , b , b , b , ⋯ ) ∈ ( Δ 2 ) ∞ ∞ ,</p><p>then</p><p>d ( F k ( x ) , F k ( y ) ) = | f k ( a ) , f k ( b ) | &lt; ε .</p><p>So, the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is accessible.</p><p>Corollary 3. If f is Kato chaotic, then the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is Kato chaotic.</p><p>Proof. According to Theorem 2 and Theorem 4, the conclusion is obvious.</p><p>Theorem 5. If f is exact, then the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is exact.</p><p>Proof. Since f is exact, for any open subset D ⊂ I , there exist m ∈ ℕ such that f m ( D ) = I . That is, for any a ∈ D , there exists an m &gt; 0 such that B ( f m ( a ) , ε ) ∩ I ≠ ∅ for any ε &gt; 0 . So there is a b ∈ X such that ρ ( f m ( a ) , ε ) = | f m ( a ) − b | &lt; ε .</p><p>Take ( Δ * ) ∞ ∞ is arbitrary open subset of Δ ∞ ∞ , and x 0 = ( ⋯ , a , a , a , ⋯ ) ∈ ( Δ * ) ∞ ∞ . Clearly, for any k ∈ ℕ , F k ( x 0 ) = { f k ( a ) } n = − ∞ ∞ . For any y 0 = ( ⋯ , b , b , b , ⋯ ) ∈ Δ ∞ ∞ , d ( F m ( x 0 ) , y 0 ) = | f m ( a ) − b | &lt; ε . That is to say, there exist an m ∈ ℕ , F m ( ( Δ * ) ∞ ∞ ) = Δ ∞ ∞ . So, the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is exact.</p><p>In [<xref ref-type="bibr" rid="scirp.100623-ref23">23</xref>] we had proved that, f is Li-Yorke sensitive implies that the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is Li-Yorke sensitive. Inspired by this, the following conclusion can be drawing.</p><p>Theorem 6. If f is densely Li-Yorke sensitive, then the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is densely Li-Yorke sensitive.</p><p>Proof. Since f is densely Li-Yorke sensitive, then for any a ∈ Q δ ( f ) and any ε &gt; 0 . Then there exists a b ∈ B ( a , ε ) such that ( a , b ) ∈ L Y ρ ( f , δ ) . Take x * = { x n = a } n = − ∞ ∞ , y * = { y n = b } n = − ∞ ∞ . One has that</p><p>lim sup n → ∞ d ( F n ( x * ) , F n ( y * ) ) = lim sup n → ∞ d ( f n ( a ) , f n ( b ) ) &gt; δ</p><p>and</p><p>lim inf n → ∞ d ( F n ( x * ) , F n ( y * ) ) = lim inf n → ∞ d ( f n ( a ) , f n ( b ) ) = 0</p><p>Thus there is an x * ∈ Q δ ( F ) .</p><p>Any fixed x ∈ Δ ∞ ∞ , write x = ( ⋯ , x m , − 1 , x m ,0 , x m ,1 , ⋯ ) , where x m , p = x m , p + 1 , p ∈ ℤ . Because f : I ↦ I is densely Li-Yorke sensitive, then for any ε &gt; 0 and the above x m ,0 , B ( x m ,0 , ε ) ∩ Q δ ( f ) ≠ ∅ . Take a ∈ B ( x m ,0 , ε ) ∩ Q δ ( f ) , then</p><p>d ( x , x * ) = sup { | x m , p − a | } = | x m , p − a | &lt; ε .</p><p>So x * ∈ B ( x , ε ) . This suggests that Q δ ( F ) &#175; = Δ ∞ ∞ .</p><p>So, the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) is densely Li-Yorke sensitive.</p><p>According to Proposition 3 and Theorem 6 the following is right.</p><p>Corollary 4. If f is dense Li-Yorke sensitivity, then the system ( Δ ∞ ∞ , d , F | Δ ∞ ∞ ) it is Topological mixing (or its topological entropy is positive).</p></sec><sec id="s4"><title>4. Conclusion</title><p>Inspired by the literature [<xref ref-type="bibr" rid="scirp.100623-ref23">23</xref>], this paper further studies the chaoticity of coupled map lattices. Some sufficient conditions of sensitivity, accessibility and transitivity are obtained. However, the study of coupled map lattices is still a hot topic. Based on the conclusions of this paper and others, one can consider some questions, such as the form of CMLs, the measurement of CMLs, and discuss the chaos of CMLs in other systems, which are worthy of studying.</p></sec><sec id="s5"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s6"><title>Cite this paper</title><p>Yang, X.F., Lu, T.X. and Liu, G. (2020) Some Chaotic Properties of a Kind of Coupled Map Lattices. Journal of Applied Mathematics and Physics, 8, 968-975. https://doi.org/10.4236/jamp.2020.86075</p></sec></body><back><ref-list><title>References</title><ref id="scirp.100623-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Kaneko, K. (1983) Theory and Application of Coupled Map Lattices. 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