<?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">IJMNTA</journal-id><journal-title-group><journal-title>International Journal of Modern Nonlinear Theory and Application</journal-title></journal-title-group><issn pub-type="epub">2167-9479</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijmnta.2013.21A008</article-id><article-id pub-id-type="publisher-id">IJMNTA-29401</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Transitivity and Chaoticity in 1-D Cellular Automata
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>angyue</surname><given-names>Chen</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Guanrong</surname><given-names>Chen</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>Weifeng</surname><given-names>Jin</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Science, Hangzhou Dianzi University, Hangzhou, China</addr-line></aff><aff id="aff3"><addr-line>College of Pharmaceutical Sciences, Zhejiang Chinese Medical University, Hangzhou, China</addr-line></aff><aff id="aff2"><addr-line>Department of Electronic Engineering, City University of Hong Kong, Hong Kong, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>fychen@hdu.edu.cn(AC)</email>;<email>eegchen@cityu.edu.hk(GC)</email>;<email>jin.weifeng@hotmail.com(WJ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>29</day><month>03</month><year>2013</year></pub-date><volume>02</volume><issue>01</issue><fpage>69</fpage><lpage>73</lpage><history><date date-type="received"><day>November</day>	<month>22,</month>	<year>2012</year></date><date date-type="rev-recd"><day>December</day>	<month>30,</month>	<year>2012</year>	</date><date date-type="accepted"><day>January</day>	<month>14,</month>	<year>2013</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>
 
 
   
   Recent progress in symbolic dynamics of cellular automata (CA) shows that many CA exhibit rich and complicated Bernoulli-shift properties, such as positive topological entropy, topological transitivity and even mixing. Noticeably, some CA are only transitive, but not mixing on their subsystems. Yet, for one-dimensional CA, this paper proves that not only the shift transitivity guarantees the CA transitivity but also the CA with transitive non-trivial Bernoulli subshift of finite type have dense periodic points. It is concluded that, for one-dimensional CA, the transitivity implies chaos in the sense of Devaney on the non-trivial Bernoulli subshift of finite types. 
  
 
</p></abstract><kwd-group><kwd>Bernoulli Subshift of Finite Type; Cellular Automata; Devaney Chaos; Symbolic Dynamics; Topological Transitivity</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><sec id="s1_1"><title>1.1. Cellular Automata</title><p>Cellular automata (CA), formally introduced by von Neumann in the late 1940s and early 1950s, are a class of spatially and temporally discrete deterministic systems, characterized by local interactions and an inherently parallel form of evolution [<xref ref-type="bibr" rid="scirp.29401-ref1">1</xref>]. In the late 1960s, Conway proposed his now-famous Game of Life, which shows the great potential of CA in simulating complex systems [<xref ref-type="bibr" rid="scirp.29401-ref2">2</xref>]. In the 1980s, Wolfram focused on the analysis of dynamical systems and studied CA in detail [3,4]. In 2002, he introduced the monumental work A New Kind of Science [<xref ref-type="bibr" rid="scirp.29401-ref5">5</xref>]. In fact, mathematical theory of CA was firstly developed by Hedlund about two decades after Neumann’s seminal work [<xref ref-type="bibr" rid="scirp.29401-ref6">6</xref>]. Since 2002, Chua et al. provided a rigorous nonlinear dynamical approach to Wolfram’s empirical observations [7-10]. All elementary CA (ECA) rules are reorganized into four groups in terms of finite bit stings. There are 40 topologically-distinct period-<img src="1-2340062\dc2d2043-ce02-4b5e-9630-e23d544a2003.jpg" /> rules<img src="1-2340062\8e1e4961-db96-4cad-9f18-945eb2a91328.jpg" />, 30 topologically-distinct Bernoulli shift rules, 10 complex Bernoulli shift rules, and 8 hyper Bernoulli shift rules. Recently, the dynamical properties of Chua’s periodic rules and robust Bernoulli-shift rules with distinct parameters have been investigated from the viewpoint of symbolic dynamics [11-17].</p><p>By a theorem of Hedlund [<xref ref-type="bibr" rid="scirp.29401-ref6">6</xref>], a map <img src="1-2340062\3f4af1e5-1fde-40f4-a3c8-36ee1f807708.jpg" /> is an one-dimensional cellular automata (1-D CA) if and only if it is continuous and commutes with the shift map<img src="1-2340062\490f1a23-9af4-4bd9-85a2-cad76a524b6b.jpg" />. For any 1-D CA, there exists a radius <img src="1-2340062\7cbc72da-0789-4b04-ad1e-8881a4739610.jpg" /> and a local map <img src="1-2340062\981793cb-335f-485e-ad27-7f84f951297d.jpg" /> such that</p><p><img src="1-2340062\9f136182-db62-4303-bf52-c778d842b236.jpg" />where notetions will be precisely defined below. In particular, <img src="1-2340062\ccbe2b1e-ad51-4e62-bc10-8770c299267b.jpg" />is an ECA global map when <img src="1-2340062\1d8bf8be-3d0a-49bd-a3b8-a1587df93240.jpg" /> and <img src="1-2340062\a7a1f661-718c-4399-9ea5-4cac78506608.jpg" /> <img src="1-2340062\a1eb1064-0a65-47aa-853e-4cb0e31d28de.jpg" />. Each ECA can be expressed by a 3-bit Boolean function and coded by an integer<img src="1-2340062\6850904c-81bf-4b68-8ce2-83ea273432ef.jpg" />, which is the decimal notation of the output binary sequence of the Boolean function [5,7,18].</p></sec><sec id="s1_2"><title>1.2. Definition of Chaos</title><p>Let <img src="1-2340062\0cda53a0-583b-4aad-a08f-7295fc2f3b49.jpg" /> be a metric space and<img src="1-2340062\ca46e4fd-6b6c-41da-847a-5350317ffc19.jpg" />: <img src="1-2340062\dfc18f78-74ae-4e73-9d77-8ec51ed092aa.jpg" />be a continuous map. <img src="1-2340062\b9331180-e05c-41db-8fd5-a8ff8f30fe21.jpg" />is said to be topologically transitive or simply transitive if, for any non-empty open subsets <img src="1-2340062\c836b21c-3dcb-4a81-be72-5e59519d3a30.jpg" /> and <img src="1-2340062\ca57be40-aa6a-4a7d-9703-29c14418f888.jpg" /> of <img src="1-2340062\0a87e02c-bfd4-4f18-8de1-21ee73ecbabf.jpg" /> there exists a natural number <img src="1-2340062\3cba1ed5-8b16-4812-bebb-0d9ea1fbe8d1.jpg" /> such that<img src="1-2340062\f8f53e46-6602-41ce-bebe-c25224fdc41c.jpg" />; <img src="1-2340062\af452fff-ca23-4211-b4b2-6345695699cf.jpg" />is topologically mixing or simply mixing if there exists a natural number <img src="1-2340062\268ff9d8-981b-4959-a098-a47b6a69166b.jpg" /> such that <img src="1-2340062\54c4e5a5-6067-4277-a12e-152363ddf312.jpg" /> for all<img src="1-2340062\106b5fbf-9616-4d87-93f1-5f699454e1e1.jpg" />; <img src="1-2340062\81f52dcd-3c31-4ced-8fd3-0928b2f901af.jpg" />is sensitive to initial conditions (or simply sensitive) if there exists a <img src="1-2340062\ac712786-6b24-4ecc-9106-7942599b0c86.jpg" /> such that, for <img src="1-2340062\bf9cceaf-d4ee-4d1c-a665-1007604d42b8.jpg" /> and for any neighborhood <img src="1-2340062\09e64088-1c76-4f47-87f6-50fe2c05d398.jpg" /> of<img src="1-2340062\f7b88bfb-86b8-49f6-b994-ce9ccb98de24.jpg" />, there exists a <img src="1-2340062\ada33e9d-23b6-4f72-a7ba-fc17cd70a5fb.jpg" /> and a natural number <img src="1-2340062\8184e196-f681-48a1-93a5-5984de21034d.jpg" /> such that<img src="1-2340062\145bc569-4864-415a-96ad-378c99e06ba0.jpg" />, where <img src="1-2340062\3ab790ad-fb69-4105-90eb-d93a7d9695b3.jpg" /> is a distance defined on<img src="1-2340062\619e8ad0-6c2b-4b20-be77-9f6365f2b183.jpg" />.</p><p>Let <img src="1-2340062\9ded9153-9f46-4668-bf79-5e1ad3209876.jpg" /> be the set of periodic points of<img src="1-2340062\9a974c49-98a9-4c95-8994-eb06be7bdb3e.jpg" />. <img src="1-2340062\6cfe2a31-292f-45a9-b1b0-c2040aea9523.jpg" />is said to be a dense subset of <img src="1-2340062\08d92411-c3ce-4059-897e-4da48eef410c.jpg" /> if, for any <img src="1-2340062\e86bb4e3-7173-40f4-9a7c-e469417832d5.jpg" /> and any constant<img src="1-2340062\2ee164d9-f4fa-41b7-9b3b-77a597e4f0b7.jpg" />, there exists a <img src="1-2340062\18d7f2c2-71d4-4db5-969a-2a94d5252add.jpg" /> such that<img src="1-2340062\ebcdec26-1674-4cda-8b38-e7342efa0df4.jpg" />.</p><p>Definition 1. <img src="1-2340062\3feeb24d-edf8-4339-b841-7e40a2f2ab79.jpg" />is chaotic on <img src="1-2340062\4cda2c2f-423a-4161-82c8-8563f050cddd.jpg" /> in the sense of Devaney if (1)<img src="1-2340062\0c0b4426-609e-4ea8-92f0-afdf69e50b9c.jpg" /> is transitive, (2) <img src="1-2340062\9634235e-2ab4-428a-9a9f-0ba267ab6188.jpg" />is a dense subset of<img src="1-2340062\039df630-a045-49f6-943f-746ba6dcfe70.jpg" />, (3)<img src="1-2340062\f1661d8b-2b0c-4547-bbcd-4cb8a6059711.jpg" /> is sensitive [<xref ref-type="bibr" rid="scirp.29401-ref19">19</xref>].</p><p>It has been proved that additive 1-D CA are chaotic [<xref ref-type="bibr" rid="scirp.29401-ref20">20</xref>]. For general dynamical systems, it has been proved that (1) and (2) together imply (3) [<xref ref-type="bibr" rid="scirp.29401-ref21">21</xref>], and for 1-D CA, (1) implies (3) [<xref ref-type="bibr" rid="scirp.29401-ref22">22</xref>]. In the next section of this paper, it will be proved that, for 1-D CA with Bernoulli subshift of finite type (BSFT), (1) also implies (2).</p></sec><sec id="s1_3"><title>1.3. Symbolic Dynamical Systems and SFT</title><p>For a finite alphabet<img src="1-2340062\8c3aa628-cce1-4a4a-a1cc-429cc8e2904f.jpg" />, a word over <img src="1-2340062\92c70ed5-edba-4423-90fb-e0962d1d04f8.jpg" /> is a finite sequence <img src="1-2340062\bcbe343f-fad6-4278-b8ef-f86de0428e80.jpg" /> of elements of<img src="1-2340062\6abc2fd8-6477-4139-8091-a861ef3d1335.jpg" />. Denote by <img src="1-2340062\57c4c998-37d0-48c1-a114-fdbf67b1316c.jpg" /> the set of all words of length<img src="1-2340062\89300799-46b7-4650-8cf2-e6bbb026f87d.jpg" />. If <img src="1-2340062\8a3f5ad2-64ac-4372-a9dc-76481f8a58bf.jpg" /> is a finite or infinite word and <img src="1-2340062\abc3bba7-3539-4ee0-9eb3-289342ceb025.jpg" /> is an interval of integers on which <img src="1-2340062\873b091f-c5bc-4343-ba17-d240f0e79d78.jpg" /> is defined, then denote</p><p><img src="1-2340062\6d131de5-f62c-460e-aec3-7184540d046d.jpg" />. Moreover, <img src="1-2340062\dc14a1b6-11d5-4d0a-9645-6cf4fee8048b.jpg" />is said to be a subword of<img src="1-2340062\511b9701-909e-4924-8153-47e61adb5b50.jpg" />, denoted as<img src="1-2340062\e2478810-9dd1-4954-a5f0-f75563fc8101.jpg" />, if <img src="1-2340062\9f51f5e8-1f5b-40fc-b4fb-d3487a581d25.jpg" /> for some interval<img src="1-2340062\2cc8403c-ed24-4da4-b129-0bfb5d705f3d.jpg" />, where <img src="1-2340062\62945d90-ddd5-43c9-b08e-47b210afc475.jpg" /> is the set of all integers. The set of bi-infinite configurations is denoted by<img src="1-2340062\2e99b0cf-3f02-4dd9-a23c-e1a9e53a857e.jpg" />, and a distance <img src="1-2340062\2a49775d-f84b-4e42-95bb-8a217abf7c8e.jpg" /> on<img src="1-2340062\6e205e20-7fd0-43f2-843a-84aa90f07378.jpg" />is defined by</p><p><img src="1-2340062\6aa5e71a-c702-4cea-bb8e-282a0a64a6a7.jpg" /></p><p>where<img src="1-2340062\e456e0d6-9bbe-4fc4-b80e-0b58922dac07.jpg" />,</p><p><img src="1-2340062\e205ee47-4960-4a79-a8be-ebbe52a620f9.jpg" />, and <img src="1-2340062\b4d53d44-8856-49fc-b532-3131b0505df5.jpg" /> if <img src="1-2340062\0782cde8-7195-4068-a686-17985fe86e06.jpg" />, or <img src="1-2340062\5ffde7f1-f055-4cb7-b7f2-831a36403ee4.jpg" /> otherwise. It is known that <img src="1-2340062\c200b3fd-199a-4d23-ae01-ea9108457262.jpg" /> is a compact, perfect and totally disconnected metric space [<xref ref-type="bibr" rid="scirp.29401-ref23">23</xref>].</p><p>For a map<img src="1-2340062\fb18f944-7710-4f01-bb35-1a3de422770f.jpg" />, a set <img src="1-2340062\0c63487a-7104-4870-9043-c1de08c4a6e9.jpg" /> is said to be <img src="1-2340062\e3424718-ef85-4977-bca4-a401d4d20e0f.jpg" /> if<img src="1-2340062\bfc6d2f1-2653-4b38-b568-ddebdb9e5927.jpg" />. If <img src="1-2340062\c406eff8-562b-4faa-8a25-c9cedc1ab045.jpg" /> is closed and</p><p><img src="1-2340062\be2f4df0-c886-406c-9363-ad74854efe3e.jpg" />then <img src="1-2340062\711a6d0e-2c28-41f9-be41-814d63391367.jpg" /> is called a subsystem of the dynamical system<img src="1-2340062\68d76152-b77a-4c67-b303-c9e022b87869.jpg" />. For example, let <img src="1-2340062\49a00f00-3ec8-4915-ac63-04cc0b1c3024.jpg" /> be a set of some words of length <img src="1-2340062\a361d1e9-fc69-4c64-ab6d-d977d0482084.jpg" /> over<img src="1-2340062\b8862366-1333-44d8-8d67-be23259de71f.jpg" />, and <img src="1-2340062\063331af-9e3a-4242-9ffd-b41ffafbf0d7.jpg" /> be the set of the bi-infinite configurations consisting of all the words in<img src="1-2340062\e3d4c58e-98d0-4eb9-9277-bf160855aa2e.jpg" />. Then, <img src="1-2340062\ce5b3bf7-6aba-4cce-8d55-8ad88de8cbf2.jpg" />is a subsystem of</p><p><img src="1-2340062\c8ba41a2-897c-42dc-b84e-ff53ae95db01.jpg" />, where <img src="1-2340062\1bdc0d48-7b6d-4219-a413-d4d5f4716ed9.jpg" /> is the left shift <img src="1-2340062\8a2ae16c-4213-47ce-b1b6-a07f14fc598e.jpg" /> (or the right shift<img src="1-2340062\d28df955-8831-4d09-b216-6425168ce539.jpg" />) defined on<img src="1-2340062\031a36b5-adb4-4ad3-a64d-ea9dd8c161ee.jpg" />, and <img src="1-2340062\7e9eea58-7e32-443c-b2a4-23504aedcd13.jpg" /> is called the determinative block system of<img src="1-2340062\eeb7e93e-cc86-455c-ae5a-252be4a8280e.jpg" />. The subsystem<img src="1-2340062\489c1783-581d-4733-b38e-2d23084f650f.jpg" />, or simply <img src="1-2340062\b2ce1851-079b-410d-936a-80b2a154e2ba.jpg" /> is called a subshift of finite type (SFT) with respect to<img src="1-2340062\528cfa9b-7804-4710-ac24-d1b10beb4cf0.jpg" />.</p><p>Furthermore, <img src="1-2340062\011f6d86-0d2c-47bc-912a-ae0fa19e0ae0.jpg" />can be described by a finite directed graph, <img src="1-2340062\88d42de5-975c-4f30-a946-cbe827f51888.jpg" />, where each vertex is labeled by a word in<img src="1-2340062\4d9f5530-c5d7-4bb2-a151-2e3e75f3283e.jpg" />, and <img src="1-2340062\927ad4ad-41b9-481a-bf60-85d6d3c5bbfb.jpg" /> is the set of edges connecting the vertices in<img src="1-2340062\7c49f47c-982f-408f-980c-4f22e6af1f22.jpg" />. Two vertices <img src="1-2340062\6dc16ebd-b590-4d86-a568-4b4a2c9030aa.jpg" /> and <img src="1-2340062\81d963be-251c-45bc-b294-6b03f656ffca.jpg" /> are connected by an edge <img src="1-2340062\945ed3c2-d3b2-4aed-a0f9-7383fddc5a86.jpg" /> if and only if<img src="1-2340062\446b5e9f-5c24-4424-b1b4-58948a7d7124.jpg" />. One can think of each element of <img src="1-2340062\487d2fde-65a6-468f-bd10-d9819695dd67.jpg" /> as a bi-infinite path on the graph<img src="1-2340062\842244bf-4897-481d-9b79-413a0116729a.jpg" />. Whereas a directed graph corresponds to a square transition matrix <img src="1-2340062\f7e632c1-e2bd-457f-80e9-2d7d9119f73f.jpg" /> with <img src="1-2340062\6de14e1c-ba47-4c2a-8db8-356dffb4bd5b.jpg" /> if and only if there is an edge from vertex <img src="1-2340062\ee852ca7-03fb-4e2d-a74d-966732e18c97.jpg" /> to vertex<img src="1-2340062\e7bcfefc-21eb-4b6b-a289-d4f0323d89d3.jpg" />, where <img src="1-2340062\721bb867-8488-44b0-85c7-40f2767d2762.jpg" /> is the number of elements in<img src="1-2340062\36e75241-2433-47c3-8ece-38c480db5df3.jpg" />, and <img src="1-2340062\1e60fabf-dff0-45f0-a32f-3adbeec4e295.jpg" /> (or<img src="1-2340062\31f6d3f2-fbbb-48ea-895c-72afa5762529.jpg" />) is the code of the corresponding vertex in<img src="1-2340062\2a7420d8-cb71-4ce7-9516-ad7b518aa1cf.jpg" />,<img src="1-2340062\8f7f6c15-40df-4d26-9fe4-ede29c1d5527.jpg" />. Thus, <img src="1-2340062\456ca098-6ddd-4131-b2ea-768d02b775d8.jpg" />is precisely defined by the transition matrix<img src="1-2340062\0324dd1e-d2f3-4654-a653-9457addafd40.jpg" />.</p><p>Remarkably, a <img src="1-2340062\ad5c6241-83c6-432c-856d-1bfb166e5f97.jpg" /> square matrix <img src="1-2340062\fc169662-cebb-4778-a987-3dd6a1861515.jpg" /> is irreducible if, for any<img src="1-2340062\d5d7865d-9f8f-4257-be33-40d8266228de.jpg" />, there exists an <img src="1-2340062\2ea67732-4716-4b23-9d5f-a578fd2d511e.jpg" /> such that<img src="1-2340062\3114463f-c488-4800-ae91-a25c4f1df23a.jpg" />; aperiodic if there exists an <img src="1-2340062\eb71da4e-5966-425d-8db4-d7c77913caaf.jpg" /> such that <img src="1-2340062\3735863a-27ea-4b95-bad0-0b640ad20f90.jpg" /> for all<img src="1-2340062\8c7258a0-4be4-4f8b-9e57-d69b3b1dada0.jpg" />, where <img src="1-2340062\43f213f5-945f-46ad-b84b-b1b1ae206393.jpg" /> is the <img src="1-2340062\1189461d-d98e-4eb8-8581-cbe2d695514b.jpg" /> entry of the power matrix</p><p><img src="1-2340062\63edb98b-87f0-44dc-bd52-e75c8a083692.jpg" />. If <img src="1-2340062\9865f578-d19d-4931-a11a-d3ad2ab653f0.jpg" /> is an SFT of<img src="1-2340062\da331413-b630-42be-b1ef-787de2d8ffe1.jpg" />, then it is transitive if and only if <img src="1-2340062\58b1d3a7-6f1f-42a1-9e65-dbc607e6d562.jpg" /> is irreducible; it is mixing if and only if <img src="1-2340062\4228d71b-d103-44f5-9a4c-75155c406821.jpg" /> is aperiodic. Equivalently, <img src="1-2340062\d0dfe5f2-1ccb-48c1-843f-08a3b0388dd4.jpg" />is irreducible if and only if for every ordered pair of vertices <img src="1-2340062\d747386d-453e-4cb4-a0df-3ed8dea47e17.jpg" /> and <img src="1-2340062\1da779aa-f481-4240-b146-928bf33b7659.jpg" /> there is a path in <img src="1-2340062\673473df-7656-47da-a641-c58e2688b651.jpg" /> starting at <img src="1-2340062\d38f2466-1466-4760-ad3f-1779dabfb9f6.jpg" /> and ending at <img src="1-2340062\0d467aab-9740-494c-accb-fc187038bb27.jpg" /> [23,24].</p></sec></sec><sec id="s2"><title>2. Transitivity and Chaoticity</title><p>In this section, it is proved that, for any 1-D CA restricted on its Bernoulli-shift subsystem, the shift transitivity implies the CA transitivity, and transitive nontrivial Bernoulli subshift of finite type (BSFT) has dense periodic points. Consequently, for 1-D CA, transitivity implies chaos in the sense of Devaney on the non-trivial BSFT.</p><sec id="s2_1"><title>2.1. Shift Transitivity Implies CA Transitivity</title><p>Definition 2. A closed invariant subset <img src="1-2340062\0ef516d3-7cfb-428c-9003-ea7613897fbf.jpg" /> of a 1-D CA <img src="1-2340062\f9c900b9-998a-4ac3-9faf-f4b22c2f8e8d.jpg" /> is called a Bernoulli-shift subsystem if there exists an integer pair <img src="1-2340062\5af3fb8a-8899-49c1-a7d4-b5fa27ecf657.jpg" /> with <img src="1-2340062\19486b1d-e3bf-45a1-8cad-7b042876f0ec.jpg" /> such that<img src="1-2340062\88732f10-5c14-4b94-ad5d-f2b40f373994.jpg" />, where <img src="1-2340062\c9def522-bfb8-4054-a795-fc1affb81df8.jpg" /> is the radius of the local map <img src="1-2340062\59fb0171-1883-44eb-817c-b81abdc4d709.jpg" /> of the CA <img src="1-2340062\f6413e01-a70e-4288-abbc-046cd6e794b5.jpg" /> and <img src="1-2340062\29f977b6-7bb6-4356-87a3-059368e740f1.jpg" /> is the left (or right) shift map.</p><p>For simplicity, only consider <img src="1-2340062\5b27fa17-b9b7-4ea3-bc0a-cffa14c3c9a9.jpg" /> as the left shift in the following discussion.</p><p>Proposition 1. If <img src="1-2340062\787f0656-8525-4c12-8d73-442c18b09cf6.jpg" /> is a Bernoulli-shift subsystem of a 1-D CA <img src="1-2340062\1209f7a8-ecde-40ce-a0b1-c44ffc06a7ac.jpg" /> with<img src="1-2340062\6f67fb04-cdf4-4ddb-b5e9-364ea8d2e3d1.jpg" />then there exists a <img src="1-2340062\1ec85228-bead-4a76-8db1-026c52a3ef2d.jpg" />-sequence set <img src="1-2340062\6d4a290e-eded-4415-a74d-b2a9195a43ff.jpg" /> such that</p><p><img src="1-2340062\3a467a78-7d6e-453c-8559-6dc7ef72c8b6.jpg" />.</p><p>Proof: If <img src="1-2340062\732acdf8-d8b5-423e-bbe8-28f393b16906.jpg" /> is the local map of<img src="1-2340062\c740edab-a8ae-4f7d-9640-439c74d6ed7b.jpg" />, then one can get the <img src="1-2340062\6a74276c-1c68-426e-99b3-216064f52425.jpg" /> times iteration of <img src="1-2340062\63458b5e-f1b9-457b-a8e2-f318a36e3590.jpg" /> <img src="1-2340062\7822b13d-acd4-4279-9806-827f22deed49.jpg" /> Thus, <img src="1-2340062\2521dffb-3e96-4341-9974-402dc24c4110.jpg" />, if and only if</p><p><img src="1-2340062\d609a20c-4d4b-4143-bf1d-8e808d6ce3c5.jpg" />for all<img src="1-2340062\bdf2094f-3d7b-4485-8858-de814137bb66.jpg" />. Let</p><p><img src="1-2340062\bea9c226-7443-475a-88de-2136d03430e3.jpg" /></p><p>and</p><p><img src="1-2340062\bc4f3e5a-d7cc-4710-8f30-ca6212fb04f4.jpg" />where <img src="1-2340062\5248589b-ebd9-48d4-ae95-f552d815fe5e.jpg" /> is a finite set since <img src="1-2340062\1fd34020-5699-4d79-b473-6d2d3bf1db09.jpg" /> Then, it follows that<img src="1-2340062\bd7ce77c-2fa8-44e7-af4d-7ef1393243d2.jpg" />.<img src="1-2340062\85d1a880-f009-4ea8-8f5d-405b4154a632.jpg" /></p><p>Definition 3. The Bernoulli-shift subsystem <img src="1-2340062\d5ae4b17-b845-4158-81bf-ca6ae637cd6f.jpg" /> in Proposition 1 is called the Bernoulli subshift of finite type (BSFT), and <img src="1-2340062\5877d327-f734-4855-bf65-25ec3d14bb93.jpg" /> is called the determinative block system of<img src="1-2340062\e15d06d6-5191-43e1-9fbf-40e860cbd3ca.jpg" />. If BSFT is an infinite set, then it is said to be non-trivial.</p><p>Based on Definitions 1, 3 and Proposition 1, an obvious result is the following proposition.</p><p>Proposition 2. Consider two BSFTs, <img src="1-2340062\a8a192ba-f328-45e3-95b0-d403cbd85340.jpg" />and<img src="1-2340062\d451482c-b482-446b-a064-b7ea90f27ea8.jpg" />, of a 1-D CA <img src="1-2340062\67747123-4263-4b1d-9826-03501276877c.jpg" /> with</p><p><img src="1-2340062\1b70888d-3b3a-4b1c-be6e-fa52bd7c0fb5.jpg" />.</p><p>Then, <img src="1-2340062\db5424dd-d78a-484f-8967-157c155ca828.jpg" />if and only if<img src="1-2340062\610b1ebd-1b82-4cef-8141-f1b3ce178fdc.jpg" />.</p><p>Theorem 1. Let <img src="1-2340062\1ac792c1-111f-4543-bb35-92a32bb4e5e1.jpg" /> be a BSFT of a 1-D CA <img src="1-2340062\15c14baa-fb5b-4c04-908b-d24aaa35f254.jpg" /> with <img src="1-2340062\747a5978-5fe3-4e6a-bcfc-907d0fe9240d.jpg" /> If the shift <img src="1-2340062\a9c0bd9a-2e4f-412f-96ce-056c8ad4717f.jpg" /> is transitive, then <img src="1-2340062\45bbd97f-87ac-4e5a-94b9-df3012deebfa.jpg" /> is also transitive.</p><p>Proof: Since the transitivity of <img src="1-2340062\f22700aa-b664-4f39-a0d4-1b89eb1db786.jpg" /> on <img src="1-2340062\cc6923f8-14ca-48fb-9eb3-8eb87d49e6ea.jpg" /> is equivalent to the existence of a <img src="1-2340062\e0a43a1b-28ab-4447-98dd-baa7dd4b6d7b.jpg" /> such that</p><p><img src="1-2340062\b3a7fd5e-39ff-4d3a-8361-70d75ed2d240.jpg" />where</p><p><img src="1-2340062\975ee916-cb67-4a56-8f5b-1e085ebab242.jpg" /></p><p>is the orbit of <img src="1-2340062\aeeba531-b039-49e5-bc58-83b7161c209c.jpg" /> starting from <img src="1-2340062\459cda2d-3b86-4380-8b15-7f3e1e997d89.jpg" /> and <img src="1-2340062\34427034-29f0-4c30-a557-b888aa9cea4e.jpg" /> is its closure [14,15]. It can be verified that for any <img src="1-2340062\b302855c-1274-4ad9-83d9-c3a877409cd2.jpg" /> <img src="1-2340062\dd948874-2096-44c1-96a6-78c3afe11846.jpg" />, there exists at least an <img src="1-2340062\460f3c48-786e-4905-86b0-de857f4752fa.jpg" /> such that</p><p><img src="1-2340062\a0e957d0-bed2-4b50-a85e-e7bef986779f.jpg" />.</p><p>Conversely, for any<img src="1-2340062\41a1b1b7-a429-4b6f-9670-917015ddc6c0.jpg" />, the <img src="1-2340062\0f33a2e7-0d1a-4c35-af8b-441e22c4f957.jpg" /> <img src="1-2340062\a9809ca4-ea57-4fbd-aa5e-a14330355f0c.jpg" />.</p><p>For the <img src="1-2340062\a8349f6a-d09d-4631-959f-fad4f655c311.jpg" /> above, consider the orbit</p><p><img src="1-2340062\ccee9128-75f5-4c51-8734-6d6a620248bc.jpg" /></p><p>and let<img src="1-2340062\65b005f0-b42d-4da9-bfa5-0c1b238aa924.jpg" />. It is clear that <img src="1-2340062\9afe562a-1291-4b76-9947-f18ed034884e.jpg" /> is closed and<img src="1-2340062\a64a03cc-1a8d-47f1-910d-e99dd63059cd.jpg" />. Because <img src="1-2340062\f13f5536-9f5c-4125-89a9-494d091b2ca4.jpg" /> is <img src="1-2340062\8e4a4be9-9a05-40ca-bd1b-14ab53dd08bb.jpg" />-invariant and closed, one has <img src="1-2340062\2148e7d6-4306-41b2-a7c0-20221ed2cf8e.jpg" /> and<img src="1-2340062\0e0426a7-49d1-4a12-8c08-e0a6ae72368c.jpg" />. Obviously, <img src="1-2340062\56c10641-ce3f-46a9-a813-0f22fe071480.jpg" /></p><p>is transitive on<img src="1-2340062\a316c6dc-eece-4943-a683-fe09083c4aa1.jpg" />.</p><p>Let <img src="1-2340062\9031f279-bf5e-4695-bfdf-36619b1df2bf.jpg" /> denote the determinative block system of<img src="1-2340062\023bdd0f-a357-4f33-98b3-0b43ea2516d8.jpg" />. On one hand, based on Proposition 2 and<img src="1-2340062\5ff5269f-bf34-42a0-9be6-60a7ddd49df3.jpg" />, one has<img src="1-2340062\3d8d0a11-68b8-4edf-afc5-5bc5ae913121.jpg" />. On the other hand, since<img src="1-2340062\9aa54594-4f9a-4558-bc6b-fffe8a83e0cc.jpg" />, it follows that<img src="1-2340062\30dce874-58d7-4fbe-b93b-1c5b2d7f2ec6.jpg" />, but the <img src="1-2340062\c33dd05d-6d46-4ec0-a791-0043d982fda4.jpg" />-sequence set consisting of <img src="1-2340062\2d7b643a-46f7-4452-aa74-e26a71d79b12.jpg" /> is<img src="1-2340062\b146ea2d-b865-4ab7-b659-5611e85e0304.jpg" />. This implies</p><p><img src="1-2340062\44ffebe9-6439-4970-b8ba-d4b048562384.jpg" />and<img src="1-2340062\84f3f221-5cc1-49d0-b2c0-aa7ada63bfc5.jpg" />. Thus, <img src="1-2340062\09dc68ea-7313-4980-a491-32c08f834195.jpg" />, i.e., <img src="1-2340062\419b9523-b7df-416e-b98c-d3d3d50d5db1.jpg" />is transitive on<img src="1-2340062\f9a96bf9-3150-4813-bc2f-bd540885fff5.jpg" />.<img src="1-2340062\18f908e5-2898-4cd6-8283-f3b051020bec.jpg" /></p><sec id="s2_1_1"><title>Remark 1.</title><p>1) Theorem 1 gives a convenient method to check if a CA <img src="1-2340062\95831ca9-b87a-4eee-a23d-87a46a5d0268.jpg" /> is transitive on a BSFT, since <img src="1-2340062\c1201e53-9a49-4b44-9a61-f8df8c6ab29c.jpg" /> is transitive on SFT if and only if the transition matrix corresponding to the SFT is irreducible [23,24].</p><p>2) Theorem 1 shows that the shift transitivity implies the CA transitivity on the BSFT, but the inverse implication may not be correct, with a counter example of ECA<img src="1-2340062\fc0c9a0b-66dd-4fd4-84b9-491dec591296.jpg" />. One has<img src="1-2340062\e4177c3a-911d-4aea-afab-16fe05b6814b.jpg" />, where <img src="1-2340062\a5f8af96-f85a-4d21-bd5e-164dcd213dce.jpg" /></p><p>and<img src="1-2340062\790ca111-d998-458b-b46f-917efc5d2aa6.jpg" />, <img src="1-2340062\0a79ba8c-5c8f-4688-9f33-3e0fd32f7e9d.jpg" />, so <img src="1-2340062\a28853fa-5c91-45d2-933a-28b11e2aaf68.jpg" /> contains two points. It is clear that <img src="1-2340062\6de046b7-9bcf-46d9-9304-fb71f4475198.jpg" /> is transitive but <img src="1-2340062\1aa92424-d6a5-4a34-8e5b-baf782951ffb.jpg" /> is not. In case BSFT is an infinite set, whether the CA transitivity implies the shift transitivity on the BSFT is still an open problem.</p><p>3) When a BSFT <img src="1-2340062\0be5936d-9fec-4b6e-97a6-034798a15c6e.jpg" /> is a finite set on which <img src="1-2340062\c2a00498-04cc-4891-a956-26eb11f27c74.jpg" /> is transitive, then it is a set of <img src="1-2340062\e27613c8-4061-4de0-b0ef-59e684a09bb6.jpg" /> points, <img src="1-2340062\ede7161e-4237-4ca5-bbfd-8a91a1d99a25.jpg" /> for some <img src="1-2340062\f65a12c9-1058-4633-9ee9-aafea33751f5.jpg" /> and <img src="1-2340062\4f2f2718-a0c3-47b2-9f4d-dd554a4a84ff.jpg" />, it is said that <img src="1-2340062\b5d7437e-6f64-48e9-b485-8007dd7f6269.jpg" /> is trivial.</p></sec><sec id="s2_1_2"><title>Remark 2.</title><p>Recall two claims proved in [<xref ref-type="bibr" rid="scirp.29401-ref22">22</xref>]: 1) transitive 1-D CA is always sensitive; 2) a 1-D CA <img src="1-2340062\7fff1374-0ae2-4f5a-ad18-d3f3b434af05.jpg" /> is transitive but not sensitive on a SFT <img src="1-2340062\7d3c9993-45eb-47f0-91bc-ce724e486f16.jpg" /> if and only if <img src="1-2340062\c8defba4-fbf3-4a91-bf5a-c032397ce8bd.jpg" /> for some <img src="1-2340062\01d50a0d-0f28-4f32-9a8e-44d61c510748.jpg" /> and<img src="1-2340062\61cd4082-af03-4dc8-a0bd-236fec6f494a.jpg" />. It is easy to be verified that <img src="1-2340062\b7afcfc2-45ec-4165-abec-293525d1a302.jpg" /> and they are common multiples of <img src="1-2340062\bdd3d1a3-0a6e-4e55-9303-f9219f8c89cd.jpg" /> and<img src="1-2340062\31abd7fe-7443-4113-aad5-7351d85e0991.jpg" />.</p></sec></sec><sec id="s2_2"><title>2.2. Transitivity Implies Density of Periodic Points</title><p>Theorem 2 Let <img src="1-2340062\7aed6741-4707-4bb2-8950-b4fdf89f3e32.jpg" /> be a BSFT of a 1-D CA <img src="1-2340062\3159dfa7-d338-4fc3-a112-245a4f6f1a7a.jpg" /> with<img src="1-2340062\d0dd1fe1-8b93-4910-846f-476e8091c581.jpg" />. If the shift <img src="1-2340062\5b6151b1-4d39-4412-9fcd-0a6876c0048e.jpg" /> is transitive, then the set of periodic points of <img src="1-2340062\0601c965-1f34-47ff-85cf-761008009e0e.jpg" /></p><p><img src="1-2340062\26bc6262-c426-4590-abd0-598f29ad97ce.jpg" />is dense in<img src="1-2340062\dbd06d95-c3b7-4314-b228-c0cfc68a8a62.jpg" />.</p><p>Proof: Let <img src="1-2340062\7c25ae35-5451-47f1-809b-468a554a7e6e.jpg" /> be the BSFT, and <img src="1-2340062\55e372ba-5d5d-4551-b8bf-905bf0c178a1.jpg" /> be its determinative block system. For any <img src="1-2340062\d3eb668d-22f0-492e-988f-1503712f7350.jpg" /> and<img src="1-2340062\f80be537-8676-4c38-82bf-4eebf4e05a5f.jpg" />, there exists a positive integer <img src="1-2340062\a975133f-709c-449c-8057-d901905357c1.jpg" /> such that</p><p><img src="1-2340062\57ed6a6f-6f94-40e0-befa-2dc810d23267.jpg" />and for</p><p><img src="1-2340062\088f6bcb-7a51-4c4c-8da1-944508a2584c.jpg" />it follows that</p><p><img src="1-2340062\11248453-28d6-4d2e-bb7b-c779f47bfd79.jpg" />.</p><p>Since <img src="1-2340062\c5162503-1050-476e-a30d-7fec2d7b7090.jpg" /> is transitive on <img src="1-2340062\5e2be247-8f78-4f08-ad5e-640e40bf19f9.jpg" /> there exists a path from</p><p><img src="1-2340062\286533c9-05d5-43c6-8bb3-951c0feda12f.jpg" />to <img src="1-2340062\fa35cc92-1d57-4adf-89ab-ce43c2997645.jpg" /> in the graph</p><p><img src="1-2340062\3e49694b-b9b3-4686-9a9e-05753163e327.jpg" />. Let</p><p><img src="1-2340062\f74668c6-36f3-42ca-b367-386553cfa3fe.jpg" /></p><p>be the sequence corresponding to this path. Then, its any <img src="1-2340062\8486185e-106d-4903-a052-2420ce187c7a.jpg" />-subsequences belong to<img src="1-2340062\5a012f11-23e8-47b9-b88e-c604e31bc108.jpg" />.</p><p>Now, construct a cyclic configuration</p><p><img src="1-2340062\b22c09f3-479c-4f58-8819-b8009e4dc153.jpg" />where</p><p><img src="1-2340062\e461fe92-7ac1-4872-86d6-3840aed48b2b.jpg" />.</p><p>Obviously, <img src="1-2340062\25f2ad62-22e1-4404-a2ba-e67e3a98f3e6.jpg" />and<img src="1-2340062\a90fca65-4b02-48e1-bd7b-d6b07e959d11.jpg" />, where <img src="1-2340062\0783a780-563a-454f-9cbe-05957b561a94.jpg" /></p><p>is the length of<img src="1-2340062\e4dd47fb-414c-453d-91a1-132fad8e90b7.jpg" />. Thus, <img src="1-2340062\9693e8f2-17cc-4bf1-808c-84afe6ae3bcf.jpg" />and<img src="1-2340062\758bb3f3-6cd9-4607-9716-21595c646cf3.jpg" />, i.e., <img src="1-2340062\4671183b-0bbe-4012-abf8-5f0102cb4f24.jpg" />and<img src="1-2340062\b0c9e9cb-1995-4ed9-ad2e-e7fc8c06f65b.jpg" />.</p><p>Therefore, the sets of periodic points <img src="1-2340062\61e74869-4217-4083-9284-1b0fcdfa5d6f.jpg" /> is dense in<img src="1-2340062\cda35052-ec70-4a85-b48a-b4e181be7e53.jpg" />.<img src="1-2340062\e5330dc1-1f16-481e-a86e-c9fe07a12c0e.jpg" /></p><p>By Theorem 2 and some results in [<xref ref-type="bibr" rid="scirp.29401-ref21">21</xref>], the following two theorems are obtained.</p><p>Theorem 3. If <img src="1-2340062\2ca69cbb-64d9-4a93-abdb-32cbf689213a.jpg" /> is transitive on a non-trivial BSFT of a 1-D CA<img src="1-2340062\1486b647-612a-4e24-96d5-73049219e435.jpg" />, then <img src="1-2340062\aa1dea29-facc-4553-a0ea-f35e67fd7afb.jpg" /> is sensitive on the BSFT.</p><p>Theorem 4. A 1-D CA <img src="1-2340062\ff666037-8839-47b7-a99e-77a4f78ce855.jpg" /> is chaotic in the sense of Devaney on its transitive non-trivial BSFT.</p></sec><sec id="s2_3"><title>2.3. An Example of Transitive ECA Rule</title><p>Rule 26 is a member of Wolfram’s class IV and Chua’s hyper Bernoulli-shift rules, which defines many subsystems with rich and complex dynamics. This rule’s local map is <img src="1-2340062\a6c97b39-6956-4c3b-8151-a44146c82a93.jpg" /> and</p><p><img src="1-2340062\aaf236a6-4bf3-4935-9498-40d65a16feff.jpg" />for all other triples<img src="1-2340062\516483af-8320-40d1-b0b3-b1dfbf711f9c.jpg" />, and the corresponding global map is denoted by <img src="1-2340062\78ebf7f3-6aab-48a4-8500-479841459821.jpg" /></p><p>Proposition 3 There exists a BSFT of<img src="1-2340062\afdabfa6-dab1-4915-b78e-bbda429aaa2f.jpg" />,</p><p><img src="1-2340062\a1f461e9-5a87-4291-ac6c-6999c87e23e4.jpg" /></p><p>such that<img src="1-2340062\cb4efbdc-9da6-45b0-a4af-347f713f6006.jpg" />, where <img src="1-2340062\34cf9eaa-2804-4254-a73d-05ee020b0de8.jpg" /> and</p><p><img src="1-2340062\04595378-6f28-4267-a52c-b00a0f67ef0f.jpg" /></p><p>Proof: Firstly, <img src="1-2340062\bfaf5f80-c527-48a5-8d1a-3d62115b22a7.jpg" />is a closed set because <img src="1-2340062\45f8141c-cf2f-4d63-a02f-bb2102eb72f8.jpg" /> is an open set. Then, it can be easily verified that <img src="1-2340062\dcf1c2f5-23c5-462b-acd1-aab4bbafc953.jpg" /> for any <img src="1-2340062\9a2245e8-e581-4a6b-8fe2-fed706d2af3b.jpg" /> and <img src="1-2340062\52f776cf-b7ec-4976-a6a5-f1977e4ed659.jpg" /> for any</p><p><img src="1-2340062\2577838d-3cdd-4b40-bdee-26433049ebfb.jpg" />. This implies that</p><p><img src="1-2340062\7a4a3bbf-4658-4c5e-9bf0-713f142af016.jpg" />for<img src="1-2340062\c60e29da-9ac4-4df5-839e-6fbc94e92e1d.jpg" />.<img src="1-2340062\cb62d82f-ea4c-4449-8499-94b93fc03eb4.jpg" /></p><p>It is clear that the transition matrix corresponding to <img src="1-2340062\362f0d1c-150e-4554-bbc0-d8eb4bf9b571.jpg" /> is</p><p><img src="1-2340062\1409e8ae-222a-420c-8fad-995e2c75b6da.jpg" /></p><p>Proposition 4. The transition matrix <img src="1-2340062\d0282ab3-3e92-4f9f-a2d5-476f5aa561c3.jpg" /> is irreducible, so <img src="1-2340062\83f9d126-6d7e-4dbd-b679-744e88ca64ee.jpg" /> is transitive on<img src="1-2340062\f84d5466-8dca-4eb4-b851-18beb22e0b12.jpg" />.</p><p>Proof: Let<img src="1-2340062\b3dac136-3ce8-41b9-8175-a443523191d3.jpg" />, where <img src="1-2340062\4c0c59d0-3cb8-42ca-815a-bf6a0ddc4f96.jpg" /> is the identity matrix, and let <img src="1-2340062\5943f123-c85e-4e53-90e7-99d704455929.jpg" /> denote the elements of the power matrix<img src="1-2340062\94a5f6d0-e6f9-41b6-9e0c-58a67dccea4d.jpg" />. It can be easily verified that <img src="1-2340062\b6748eae-e044-438c-872f-c354932e4343.jpg" /> for all<img src="1-2340062\e3653511-b492-4852-9591-7ecb465a03ac.jpg" />, so <img src="1-2340062\cdc20607-d2dc-408a-8d02-cba182c990d2.jpg" /> is aperiodic. Recall that a matrix <img src="1-2340062\c3289046-7211-4d86-a203-6c4d7f6c75fa.jpg" /> is irreducible if and only if <img src="1-2340062\fa020eaa-6c01-470a-a96c-c1e611317215.jpg" /> is aperiodic [23,24]. Hence, <img src="1-2340062\a675e390-4da7-4abe-9576-ae1186d67daf.jpg" />is irreducible and so <img src="1-2340062\6b729f1e-8e0d-45eb-9ba8-d16398e309f8.jpg" /> is transitive on<img src="1-2340062\ebb09889-02da-413d-9061-a5e1380db531.jpg" />.<img src="1-2340062\ee43c8c0-3ba4-4dbc-8887-4bbdf7eea2aa.jpg" /></p><p>Theorem 5 <img src="1-2340062\490d94ef-c8b7-4f32-b24b-b36445e01e67.jpg" /> is chaotic in the sense of Devaney on<img src="1-2340062\037083bb-2171-4814-acec-4d19e3737f63.jpg" />.</p></sec></sec><sec id="s3"><title>3. Conclusion</title><p>As a particular class of dynamical systems, CA have been widely used for modeling and simulating many physical phenomena. Despite their apparent simplicity, 1-D CA can display rich and complex evolutions, but many properties of their temporal evolutions are undecidable [25,26]. Although checking the transitivity based on its definition is very difficult [<xref ref-type="bibr" rid="scirp.29401-ref27">27</xref>], and it alone is not sufficient for chaos to exist in general dynamical systems, this work has rigorously proved that the shift transitivity implies the CA transitivity, and the CA with transitive non-trivial BSFT are chaotic in the sense of Devaney, partly answer the open question whether Devaney chaos in 1-D CA is equivalent to transitivity [<xref ref-type="bibr" rid="scirp.29401-ref28">28</xref>].</p></sec><sec id="s4"><title>4. Acknowledgments</title><p>This research was jointly supported by the NSFC (Grants No. 11171084 and No. 60872093), the Hong Kong Research Grants Council (Grant No. CityU1117/10) and Foundation of Zhejiang Chinese Medical University (Grant No. 17211076).</p></sec><sec id="s5"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.29401-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">J. von Neumann, “Theory of Self-Reproducing Automata,” University of Illinois Press, Urbana and London, 1966.</mixed-citation></ref><ref id="scirp.29401-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">M. Gardner, “The Fantastic Combinations of John Conway’s New Solitaire Game Life,” Scientific American, Vol. 223, No. 4, 1970, pp. 120-123.  
doi:10.1038/scientificamerican1070-120</mixed-citation></ref><ref id="scirp.29401-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">S. Wolfram, “Computation Theory of Cellular Automata,” Communications in Mathematical Physics, Vol. 96, No. 1, 1984, pp. 15-57. doi:10.1007/BF01217347</mixed-citation></ref><ref id="scirp.29401-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">S. Wolfram, “Theory and Application of Cellular Automata,” Word Scientific, Singapore Cty, 1986.</mixed-citation></ref><ref id="scirp.29401-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">S. Wolfram, “A New Kind of Science,” Wolfram Media, Inc., Champaign, 2002.</mixed-citation></ref><ref id="scirp.29401-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">G. A. Hedlund, “Endomorphisms and Automorphism of the Shift Dynamical System,” Mathematical System Theory, Vol. 3, No. 4, 1969, pp. 320-375.  
doi:10.1007/BF01691062</mixed-citation></ref><ref id="scirp.29401-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">L. O. Chua, V. I. Sbitnev and S. Yoon, “A Nonlinear Dynamics Perspective of Wolfram’s New Kind of Science, Part IV: From Bernoulli-Shift to 1/f Spectrum,” International Journal of Bifurcation and Chaos, Vol. 15, No. 4, 2005, pp. 1045-1183. doi:10.1142/S0218127405012995</mixed-citation></ref><ref id="scirp.29401-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">L. O. Chua, V. I. Sbitnev and S. Yoon, “A Nonlinear Dynamics Perspective of Wolfram’s New Kind of Scienc, Part VI: From Time-Reversible Attractors to the Arrows of Time,” International Journal of Bifurcation and Chaos, Vol. 16, No. 5, 2006, pp. 1097-1373.  
doi:10.1142/S0218127406015544</mixed-citation></ref><ref id="scirp.29401-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">L. O. Chua, J. B. Guan, I. S. Valery and J. Shin, “A Nonlinear Dynamics Perspective of Wolfram’s New Kind of Science, Part VII: Isle of Eden,” International Journal of Bifurcation and Chaos, Vol. 17, No. 9, 2007, pp. 2839-3012. doi:10.1142/S0218127407019068</mixed-citation></ref><ref id="scirp.29401-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">L. O. Chua, K. Karacs, V. I. Sbitnev, J. B. Guan and J. Shin, “A Nonlinear Dynamics Perspective of Wolfram’s New Kind of Science, Part VIII: More Isles of Eden,” International Journal of Bifurcation and Chaos, Vol. 17, No. 11, 2007, pp. 3741-3894.  
doi:10.1142/S0218127407019901</mixed-citation></ref><ref id="scirp.29401-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">F. Y. Chen, W. F. Jin, G. R. Chen, F. F. Chen and L. Chen, “Chaos of Elementary Cellular Automata Rule 42 of Wolfram’s Class II,” Chaos, Vol. 19, No. 013140, 2009, pp. 1-6.</mixed-citation></ref><ref id="scirp.29401-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">W. F. Jin, F. Y. Chen, G. R. Chen, L. Chen and F. F. Chen, “Extending the Symbolic Dynamics of Chua’s Bernoulli-Shift Rule 56,” Journal of Cellular Automata, Vol. 5, No. 1-2, 2010, pp. 121-138.</mixed-citation></ref><ref id="scirp.29401-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">W. F. Jin, F. Y. Chen, G. R. Chen, L. Chen and F. F. Chen, “Complex Symbolic Dynamics of Chua’s Period-2 Rule 37,” Journal of Cellular Automata, Vol. 5, No. 4-5, 2010, pp. 315-331.</mixed-citation></ref><ref id="scirp.29401-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">F. F. Chen and F. Y. Chen, “Complex Dynamics of Cellular Automata Rule 119,” Physica A, Vol. 388, No. 6, 2009, pp. 984-990. doi:10.1016/j.physa.2008.12.002</mixed-citation></ref><ref id="scirp.29401-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">F. F. Chen, F. Y. Chen, G. R. Chen, W. F. Jin and L. Chen, “Symbolics Dynamics of Elementary Cellular Automata Rule 88,” Nonlinear Dynamics, Vol. 58, No. 1-2, 2009, pp. 431-442. doi:10.1007/s11071-009-9490-3</mixed-citation></ref><ref id="scirp.29401-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">L. Chen, F. Y. Chen, W. F. Jin, F. F. Chen and G. R. Chen, “Some Nonrobust Bernolli-Shift Rules,” International Journal of Bifurcation and Chaos, Vol. 19, No. 10, 2009, pp. 3407-3415. doi:10.1142/S0218127409024840</mixed-citation></ref><ref id="scirp.29401-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">F. Y. Chen, L. Shi, G. R. Chen and W. F. Jin, “Chaos and Gliders in Periodic Cellular Automaton Rule 62,” Journal of Cellular Automata, Vol. 7, No. 4, 2012, pp. 287-302.</mixed-citation></ref><ref id="scirp.29401-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">J. B. Guan, S. W. Shen, C. B. Tang and F. Y. Chen, “Extending Chua’s Global Equivalence Theorem on Wolfram’s New Kind of Science,” International Journal of Bifurcation and Chaos, Vol. 17, No. 12, 2007, pp. 4245-4259. doi:10.1142/S0218127407019925</mixed-citation></ref><ref id="scirp.29401-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">R. L. Devaney, “An Introduction to Chaotic Dynamical Systems,” Addison-Wesley, Hazard, 1989.</mixed-citation></ref><ref id="scirp.29401-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">P. Favati, G. Lotti and L. Margara, “Additive One-Dimensional Cellular Automata Are Chaotic According to Devaney’s Definition of Chaos,” Theoretical Computer Science, Vol. 174, No. 1-2, 1997, pp. 157-170. 
doi:10.1016/S0304-3975(95)00022-4</mixed-citation></ref><ref id="scirp.29401-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">J. Banks, J. Brooks, G. Cairns, G. Davis and P. Stacey, “On the Devaney’s Definition of Chaos,” The American Mathematical Monthly, Vol. 99, No. 4, 1992, pp. 332-334.  
doi:10.2307/2324899</mixed-citation></ref><ref id="scirp.29401-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">B. Codenotti and L. Margara, “Transitive Cellular Automata Are Sensitive,” The American Mathematical Monthly, Vol. 103, No. 1, 1996, pp. 58-62. doi:10.2307/2975215</mixed-citation></ref><ref id="scirp.29401-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">B. Kitchens, “Symbolic Dynamics: One-Sided, Two-Sided and Countable State Markov Shifts,” Springer-Verlag, Berlin, 1998.</mixed-citation></ref><ref id="scirp.29401-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Z. L. Zhou, “Symbolic Dynamics,” Shanghai Scientific and Technological Education Publishing House, Shanghai, 1997.</mixed-citation></ref><ref id="scirp.29401-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">J. Banks, “Regular Periodic Decompositions for Topologically Transitive Maps,” Ergodic Theory and Dynamical Systems, Vol. 17, No. 3, 1997, pp. 505-529. 
doi:10.1017/S0143385797069885</mixed-citation></ref><ref id="scirp.29401-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">K. Culik, L. P. Hurd and S. Yu, “Computation Theoretic Aspects of Cellular Automata,” Physica D, Vol. 45, No. 1-3, 1990, pp. 357-378.  
doi:10.1016/0167-2789(90)90194-T</mixed-citation></ref><ref id="scirp.29401-ref27"><label>27</label><mixed-citation publication-type="other" xlink:type="simple">T. K. S. Moothathu, “Homogeneity of Surjective Cellular Automata,” Discrete Continuous Dynamic Systems, Vol. 13, No. 1, 2005, pp. 195-202.</mixed-citation></ref><ref id="scirp.29401-ref28"><label>28</label><mixed-citation publication-type="other" xlink:type="simple">J. Kari, “Theory of Cellular Automata: A Survey,” Theoretical Computer Science, Vol. 334, No. 1, 2005, pp. 3-33. doi:10.1016/j.tcs.2004.11.021</mixed-citation></ref></ref-list></back></article>