<?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">OALibJ</journal-id><journal-title-group><journal-title>Open Access Library Journal</journal-title></journal-title-group><issn pub-type="epub">2333-9705</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/oalib.1102856</article-id><article-id pub-id-type="publisher-id">OALibJ-69516</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Business&amp;Economics</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Earth&amp;Environmental Sciences</subject><subject> Engineering</subject><subject> Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject><subject> Social Sciences&amp;Humanities</subject></subj-group></article-categories><title-group><article-title>
 
 
  Chaos Anti-Synchronization between Chen System and Genesio System
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xianyong</surname><given-names>Wu</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>Hao</surname><given-names>Wu</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>Zhengrong</surname><given-names>Yan</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>Yuehua</surname><given-names>Huang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>College of Electrical Engineering &amp;amp; New Energy, China Three Gorges University, Yichang, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>420372724@qq.com(XW)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>31</day><month>07</month><year>2016</year></pub-date><volume>03</volume><issue>07</issue><fpage>1</fpage><lpage>5</lpage><history><date date-type="received"><day>27</day>	<month>June</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>10</month>	<year>July</year>	</date><date date-type="accepted"><day>14</day>	<month>July</month>	<year>2016</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>
 
 
   
   In this paper, anti-synchronization of two different chaotic systems is investigated. On the basis of Lyapunov theory, adaptive control scheme is proposed when system parameters are unknown or uncertain; sufficient conditions for the stability of the error dynamics are derived, where the controllers are designed by using the sum of the state variables in chaotic systems. Numerical simulations are performed for the Chen system and Genesio system to demonstrate the effectiveness of the proposed control strategy. 
  
 
</p></abstract><kwd-group><kwd>Chaotic System</kwd><kwd> Anti-Synchronization</kwd><kwd> Adaptive Control</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Since the pioneering work by Pecora and Carroll [<xref ref-type="bibr" rid="scirp.69516-ref1">1</xref>] , chaos synchronization, a very active topic in nonlinear science, has received increasing attention. The concept of synchronization has been extended in scope, for example to generalized synchronization [<xref ref-type="bibr" rid="scirp.69516-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.69516-ref4">4</xref>] , phase synchronization [<xref ref-type="bibr" rid="scirp.69516-ref5">5</xref>] , lag synchronization [<xref ref-type="bibr" rid="scirp.69516-ref6">6</xref>] , and even anti-phase synchronization (APS) [<xref ref-type="bibr" rid="scirp.69516-ref7">7</xref>] - [<xref ref-type="bibr" rid="scirp.69516-ref9">9</xref>] . APS can also be interpreted as anti-synchronization (AS), which is a phenomenon in which the state variables of the synchronized systems have the same amplitude as but opposite signs to those of the driving system. Therefore, the sums of two signals are expected to converge to zero when AS appears. Recently, Singh and Roy generalized active control to AS for two systems [<xref ref-type="bibr" rid="scirp.69516-ref10">10</xref>] . However, it seems that there are fewer previous results on AS between two different systems with unknown parameters using adaptive control. In this paper, we will focus on the AS of two different systems. Adaptive control methods will be employed; a sufficient condition for anti-synchronization is derived rigorously. Numerical simulations on Chen system and Genesio system are performed, which demonstrate the effectiveness and feasibility of the proposed control technique.</p><p>The layout of the rest of the paper is as follows. Section 2 describes the systems and their mathematical models; in Section 3, adaptive anti-synchronization between Chen and Genesio systems is presented; numerical simulation results are given for illustration and verification. Finally, conclusions are drawn in Section 4.</p></sec><sec id="s2"><title>2. Systems Description and Mathematical Models</title><p>Consider nonlinear chaotic system as follows.</p><disp-formula id="scirp.69516-formula398"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69516x6.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x7.png" xlink:type="simple"/></inline-formula> are differentiable functions, the first equation in (1) is the drive system, and the second one is the response system, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x8.png" xlink:type="simple"/></inline-formula>is the control input. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x9.png" xlink:type="simple"/></inline-formula> be the anti-synchro- nization error, our goal is to design controllers <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x10.png" xlink:type="simple"/></inline-formula> such that the trajectory of the response system with initial conditions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x11.png" xlink:type="simple"/></inline-formula> can asymptotically approach the drive system with initial conditions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x12.png" xlink:type="simple"/></inline-formula> reversely and implement anti-synchronization finally, in the sense that</p><disp-formula id="scirp.69516-formula399"><graphic  xlink:href="http://html.scirp.org/file/69516x13.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x14.png" xlink:type="simple"/></inline-formula> is the Euclidean norm.</p><p>The Genesio system, proposed by Genesio and Tesi [<xref ref-type="bibr" rid="scirp.69516-ref11">11</xref>] , is one of paradigms of chaos since it captures many features of chaotic systems. It includes a simple square part and three simple ordinary differential equations that depend on three negative real parameters. The dynamic equations of the system is given by</p><disp-formula id="scirp.69516-formula400"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69516x15.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x16.png" xlink:type="simple"/></inline-formula> are state variables, when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x17.png" xlink:type="simple"/></inline-formula> system (2) is chaotic.</p><p>Chen system is described by</p><disp-formula id="scirp.69516-formula401"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69516x18.png"  xlink:type="simple"/></disp-formula><p>When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x19.png" xlink:type="simple"/></inline-formula>, system (3) is chaotic.</p><p>In the next section, we will study chaos anti-synchronization between Chen and Genesio systems with known or unknown parameters using adaptive control.</p></sec><sec id="s3"><title>3. Adaptive Anti-Synchronization between Chen and Genesio System with Unknown Parameters</title><p>We assume that Genesio system (2) is the drive system, and the controlled Chen system (4) is the response system.</p><disp-formula id="scirp.69516-formula402"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69516x20.png"  xlink:type="simple"/></disp-formula><p>We add (2) from Equation (4) and yield</p><disp-formula id="scirp.69516-formula403"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69516x21.png"  xlink:type="simple"/></disp-formula><p>Our goal is to find the proper controllers <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x22.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x23.png" xlink:type="simple"/></inline-formula> and parameter update laws, such that system (4) globally anti-synchronizes system (2) asymptotically. i.e.</p><disp-formula id="scirp.69516-formula404"><graphic  xlink:href="http://html.scirp.org/file/69516x24.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x25.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem: If the controllers are chosen as</p><disp-formula id="scirp.69516-formula405"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69516x26.png"  xlink:type="simple"/></disp-formula><p>and the update laws of parameters are chosen as</p><disp-formula id="scirp.69516-formula406"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69516x27.png"  xlink:type="simple"/></disp-formula><p>Then system (4) globally anti-synchronizes system (2) asymptotically, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x28.png" xlink:type="simple"/></inline-formula> are positive constants, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x29.png" xlink:type="simple"/></inline-formula>are estimate values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x30.png" xlink:type="simple"/></inline-formula>, respectively.</p><p>Proof: Applying control laws (6) to (5) yields the resulting error dynamics as follows.</p><disp-formula id="scirp.69516-formula407"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69516x31.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x32.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x33.png" xlink:type="simple"/></inline-formula>.</p><p>Consider the following Lyapunov function</p><disp-formula id="scirp.69516-formula408"><graphic  xlink:href="http://html.scirp.org/file/69516x34.png"  xlink:type="simple"/></disp-formula><p>The time derivative of V along the solution of error dynamical system (8) gives that</p><disp-formula id="scirp.69516-formula409"><graphic  xlink:href="http://html.scirp.org/file/69516x35.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x36.png" xlink:type="simple"/></inline-formula></p><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x37.png" xlink:type="simple"/></inline-formula> is positive definite and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x38.png" xlink:type="simple"/></inline-formula> is negative semi-definite in the neighborhood of zero solution of system (5), it follows that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x39.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x40.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x41.png" xlink:type="simple"/></inline-formula> from (8), we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x42.png" xlink:type="simple"/></inline-formula> since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x43.png" xlink:type="simple"/></inline-formula>, we obtain</p><disp-formula id="scirp.69516-formula410"><graphic  xlink:href="http://html.scirp.org/file/69516x44.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x45.png" xlink:type="simple"/></inline-formula> is the minimal eigenvalue of the positive definite matrix P. Thus, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x46.png" xlink:type="simple"/></inline-formula>by Barbalat’s lemma, we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x47.png" xlink:type="simple"/></inline-formula> Therefore, response system (4) can globally anti-synchronize drive system (2) asymptotically. This completes the proof.</p><p>In simulation, Fourth order Runge-Kutta integration method is used to solve the systems of differential Equations (2) and (4) with the controllers (6) and the parameter update laws (7). We select the parameters of Genesio system as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x48.png" xlink:type="simple"/></inline-formula> and the parameters of Chen system as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x49.png" xlink:type="simple"/></inline-formula> respectively, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x50.png" xlink:type="simple"/></inline-formula> The initial values of drive and response systems are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x51.png" xlink:type="simple"/></inline-formula></p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x52.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x53.png" xlink:type="simple"/></inline-formula> respectively, while the initial errors of system (5) are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x54.png" xlink:type="simple"/></inline-formula> and the initial values of estimate parameters are<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x55.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x56.png" xlink:type="simple"/></inline-formula>The anti-synchronization errors between Chen system and Genesio system are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, the estimate values of parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x57.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69516x58.png" xlink:type="simple"/></inline-formula> are shown in <xref ref-type="fig" rid="fig2">Figure 2</xref> and <xref ref-type="fig" rid="fig3">Figure 3</xref>, respectively. Obviously, the anti-synchronization errors converge asymptotically to zero and two different systems are indeed achieved chaos anti-synchronization. Furthermore, the estimates of parameter converge to their true values.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Anti-synchronization errors between Chen and Genesio systems via adaptive control</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/69516x59.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Estimate values of parameters a, b, c of drive system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/69516x60.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Estimate values of parameters a<sub>1</sub>, b<sub>1</sub>, c<sub>1</sub> of response system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/69516x61.png"/></fig></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper, chaos anti-synchronization between two different chaotic systems with different structures using adaptive control is presented. Chen system and Genesio system are taken as an illustrative example to verify the effectiveness of the proposed methods.</p></sec><sec id="s5"><title>Cite this paper</title><p>Xianyong Wu,Hao Wu,Zhengrong Yan,Yuehua Huang, (2016) Chaos Anti-Synchronization between Chen System and Genesio System. Open Access Library Journal,03,1-5. doi: 10.4236/oalib.1102856</p></sec></body><back><ref-list><title>References</title><ref id="scirp.69516-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Pecora, L.M. and Carroll, T.L. (1990) Synchronization in Chaotic Systems. Physical Review Letters, 64, 821-824. http://dx.doi.org/10.1103/PhysRevLett.64.821</mixed-citation></ref><ref id="scirp.69516-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Kocarev, L. and Parlitz, U. 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