<?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">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2013.412220</article-id><article-id pub-id-type="publisher-id">AM-39801</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>
 
 
  Hybrid Adaptive Synchronization of Hyperchaotic Systems with Fully Unknown Parameters
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>Mossa Al-sawalha</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Mathematics Department, Faculty of Science, University of Ha’il, Ha’il, KSA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>sawalha_moh@yahoo.com</email></corresp></author-notes><pub-date pub-type="epub"><day>08</day><month>11</month><year>2013</year></pub-date><volume>04</volume><issue>12</issue><fpage>1621</fpage><lpage>1628</lpage><history><date date-type="received"><day>October</day>	<month>1,</month>	<year>2013</year></date><date date-type="rev-recd"><day>November</day>	<month>1,</month>	<year>2013</year>	</date><date date-type="accepted"><day>November</day>	<month>8,</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>
 
 
   In this paper, an adaptive control scheme is developed to study the hybrid synchronization behavior between two identical and different hyperchaotic systems with unknown parameters. This adaptive hybrid synchronization controller is designed based on Lyapunov stability theory and an analytic expression of the controller with its adaptive laws of parameters is shown. The adaptive hybrid synchronization between two identical systems (hyperchaotic Chen system) and different systems (hyperchaotic Lorenz and hyperchaotic <inline-formula><inline-graphic xlink:href="dit_0dbdfb0d-9220-43db-9979-987629460f91.png" xlink:type="simple"/></inline-formula> systems) are taken as two illustrative examples to show the effectiveness of the proposed method. Theoretical analysis and numerical simulations are shown to verify the results. 
 
</p></abstract><kwd-group><kwd>Hybrid Synchronization; Adaptive Control; Unknown Parameters; Hyperchaotic System</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Chaos is an omnipresent phenomenon. Scientists who understand its existence have been struggling to control chaos to our benefit. There is a great need to control the chaotic systems as chaos theory plays an important role in industrial applications particularly in chemical reactions, biological systems, information processing and secure communications [1-3]. Many scientists who are interested in this field have struggled to achieve the synchronization or anti-synchronization of different hyperchaotic systems. Therefore due to its complexity and applications, a wide variety of approaches have been proposed for the synchronization or anti-synchronization of hyperchaotic systems. The types of synchronization used so far include generalized active control [4-8], nonlinear control [9,10], and adaptive control [11-19].</p><p>The co-existence of synchronization and anti-synchronization, known as hybrid synchronization, has good application prospects in digital communications. Therefore it attracted a lot of attention in recent years. In hybrid synchronization scheme, one part of the system is anti-synchronized and the others are completely synchronized so that complete synchronization and anti-synchronization co-exist in the system. The co-existence of CS and AS may enhance security in communication and chaotic encryption schemes. Li [<xref ref-type="bibr" rid="scirp.39801-ref20">20</xref>] studied full state hybrid projective synchronization behavior in multiscroll chaotic systems in symmetrical coordinate subspace. Xie, Chen and Bolt [<xref ref-type="bibr" rid="scirp.39801-ref21">21</xref>], through numerical studies show that an arbitrary signal can be synchronized by hybrid chaotic system and then that particular signal can then be stored for password and message identification. They further identify potential applications in information storage, message identification and certain types of secure signal and image communications.</p><p>Zhang and Lű [<xref ref-type="bibr" rid="scirp.39801-ref22">22</xref>] introduce a new type of hybrid synchronization called full state hybrid log projective synchronization and apply it to the Rossler systems and the hyperchaotic Lorenz system to numerically verify their results. Similarly Chen, Chen and Lin [<xref ref-type="bibr" rid="scirp.39801-ref23">23</xref>] achieve hybrid synchronization in Chin-Lee system using both linear and non-linear control schemes. Recently Sun et al. [<xref ref-type="bibr" rid="scirp.39801-ref24">24</xref>] analyze the hybrid synchronization of two coupled complex networks using linear feedback and adaptive feedback control methods. They derive a criterion for the hybrid synchronization of the two complex networks and show that under suitable conditions two complex networks can realize hybrid synchronization. More recently, Vaidyanathan and Rasappan [<xref ref-type="bibr" rid="scirp.39801-ref25">25</xref>] investigate the hybrid chaos synchronization of hyperchaotic Qi and Jia systems using active nonlinear control. The idea of the aforementioned type of hybrid synchronization of chaotic systems deals with systems with known parameters. However in practical engineering situations, parameters are probably unknown and may change from time to time. Therefore, there is a vital need to effectively hybridsynchronize two chaotic systems (identical and different) with unknown parameters. This is typically important in theoretical research as well as practical applications. Among the aforementioned methods, adaptive control [11-19] is an effective option for achieving the synchronization of chaotic systems with fully unknown parameters. Therefore motivated by this, we study the hybrid synchronization of two identical and two different hyperchaotic systems with fully unknown parameters. The rest of the paper is organized as follows. In Section 2, we present a novel adaptive hybrid synchronization scheme with a parameter update law and give a brief description of the systems. In Sections 3 and 4, we present the hyperchaos hybrid synchronization between two identical and different hyper chaotic systems via adaptive control. Conclusions are given in Section 5.</p></sec><sec id="s2"><title>2. Problem Formulation and Systems Description</title><p>In the first part of this section, we set up the problem and present novel adaptive hybrid synchronization scheme with parameter update law. By using Lyapunov stability theory we show the co-existence of hybrid synchronization between two systems described below. In the second part of this section we briefly describe the two systems used for further analysis.</p><sec id="s2_1"><title>2.1. Hybrid Synchronization of Chaotic Systems</title><p>Consider the master chaotic system in the form of</p><disp-formula id="scirp.39801-formula125437"><label>(1)</label><graphic position="anchor" xlink:href="6-7401913\de49d4b0-7b09-4dd8-b658-25702dd968ec.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401913\9d6a1c9b-da92-4974-9674-275718c99190.jpg" /> is the state vector, <img src="6-7401913\4ae3d0e4-4ab5-4595-8986-60e92266c5ce.jpg" />is the unknown constant parameter vector of the system, <img src="6-7401913\488642b0-9c38-41ec-b66b-e5e5a35322ef.jpg" />is an <img src="6-7401913\613446cc-f344-4275-8428-7cec312fdf1d.jpg" /> matrix, <img src="6-7401913\3941d8b0-ef2a-46a4-bbf3-cc78a14955ff.jpg" />is an <img src="6-7401913\1fa34b17-a5b6-4ddd-9edb-aed23e0254f1.jpg" /> matrix whose elements<img src="6-7401913\082dd0fc-5179-4514-997d-02f35f02fb30.jpg" />. The slave system is assumed by:</p><disp-formula id="scirp.39801-formula125438"><label>(2)</label><graphic position="anchor" xlink:href="6-7401913\c97c7eb9-fa88-4f10-9b01-f6b4e99a84ac.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401913\be5d9e27-3cdf-4416-aea1-205345fd32f0.jpg" /> is the state vector, <img src="6-7401913\5e77b277-8280-487f-bb44-e9eb3d1ef121.jpg" />is the unknown constant parameter vector of the system <img src="6-7401913\b5d57b61-8473-439d-90ce-356d2b1659f6.jpg" /> is an <img src="6-7401913\f031eb22-5e71-4a2f-b351-76c803a82761.jpg" /> matrix, <img src="6-7401913\3c9ce396-57aa-471d-afb7-56dc402fdc7b.jpg" />is an <img src="6-7401913\a46c772d-fbb2-4c34-bd49-bbdd6391abe1.jpg" /> matrix whose elements<img src="6-7401913\caf6d8de-7cf0-4626-bc5e-d701a4cfe688.jpg" />, and <img src="6-7401913\125de422-9abf-4523-b947-e16f5b2e7028.jpg" /> is control input vector. If we divide the master and the slave systems into two parts, then system (1) can be written as:</p><disp-formula id="scirp.39801-formula125439"><label>(3)</label><graphic position="anchor" xlink:href="6-7401913\bed471fd-8193-4d3d-92b9-5644072c4484.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.39801-formula125440"><label>(4)</label><graphic position="anchor" xlink:href="6-7401913\e8181e9e-e5c3-4a39-b630-9764ec0c89af.jpg"  xlink:type="simple"/></disp-formula><p>and the slave system (2) can be written as</p><disp-formula id="scirp.39801-formula125441"><label>(5)</label><graphic position="anchor" xlink:href="6-7401913\9f122747-c8c4-4d40-804c-6049d6e80baf.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.39801-formula125442"><label>(6)</label><graphic position="anchor" xlink:href="6-7401913\c818c84f-7e89-41cd-bb17-393dc3d07ffd.jpg"  xlink:type="simple"/></disp-formula><p>Let <img src="6-7401913\c9dca106-f862-41ce-9254-da04b7340ca6.jpg" /> and <img src="6-7401913\ae19502c-cf3d-45ed-9677-a0b57dade655.jpg" /> be the synchronization and the anti–synchronization error vector’s respectively. Our goal is to design a controller <img src="6-7401913\1cf0f3a7-7a4d-4a31-8745-a7e6f5458966.jpg" />such that the trajectory of the response system (5)-(6) with initial conditions <img src="6-7401913\89c1a844-eb7e-477f-a77e-1849e704441e.jpg" /> can asymptotically approach the drive system, (3)-(4), with initial condition <img src="6-7401913\ab6fe505-f467-4d81-af85-55efe67f18cd.jpg" />And finally implement the hybrid synchronization such that, <img src="6-7401913\c8a370e4-f349-4de4-ae7f-dd76cfffc970.jpg" />and the anti-synchronization such that</p><p><img src="6-7401913\abfbc3fe-7441-4b9a-bd93-71e987ba8373.jpg" /></p><p>where <img src="6-7401913\1e471974-a416-433e-9d3f-4da03df16893.jpg" /> is the Euclidean norm.</p></sec><sec id="s2_2"><title>2.2. Adaptive Hybrid Synchronization Controller Design</title><p>Theorem: If the nonlinear control <img src="6-7401913\ffb9945a-9663-4d84-a5b5-c9b47cf29a1a.jpg" /> is selected as:</p><p><img src="6-7401913\389dc2f9-3450-4ed8-8c8e-725eecde4172.jpg" /></p><p>and adaptive laws of parameters are taken as:</p><p><img src="6-7401913\c1010057-d9de-4b70-8d17-7f42d353cc8a.jpg" /></p><p>then the response system (5)-(6) can synchronize and anti-synchronize the drive system (3)-(4) globally and asymptotically, where <img src="6-7401913\65fd1469-dc44-4963-93e4-57d26d35d949.jpg" /> and <img src="6-7401913\a0b98a98-d1bf-4479-bab7-fbc7933d89f9.jpg" /> are respecttively, estimations of the unknown parameters <img src="6-7401913\8849d9a8-f0c3-4099-883f-32baffb19b7d.jpg" /> and <img src="6-7401913\c2c420b0-d266-4c52-99bc-77713e7d4b4b.jpg" /></p><p>Proof: From Equations (3)-(6), we get the error dynamical systems as follows:</p><disp-formula id="scirp.39801-formula125443"><label>(7)</label><graphic position="anchor" xlink:href="6-7401913\d5113215-bba3-4fff-bdbf-ff791b1a948e.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.39801-formula125444"><label>(8)</label><graphic position="anchor" xlink:href="6-7401913\9495451c-c9dc-4b07-a9a4-214ee533f871.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.39801-formula125445"><label>(9)</label><graphic position="anchor" xlink:href="6-7401913\4e6c4764-ace6-49bd-bdfa-b5088cb9c5c8.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401913\f8d920c3-0fa7-42d5-8773-3656161491e8.jpg" /></p><p>Let <img src="6-7401913\8fd67910-d3c3-41c3-bef4-7ef390850888.jpg" /> and <img src="6-7401913\2faeeb31-1332-4ce2-a4ee-e57173643489.jpg" />.</p><p>If a Lyapunov function candidate is chosen as</p><disp-formula id="scirp.39801-formula125446"><label>(10)</label><graphic position="anchor" xlink:href="6-7401913\7fa9946c-088f-4032-a485-d26558bb6052.jpg"  xlink:type="simple"/></disp-formula><p>The time derivative of V along the error dynamical system is given by:</p><disp-formula id="scirp.39801-formula125447"><label>(11)</label><graphic position="anchor" xlink:href="6-7401913\f5f5ef29-0512-4bed-8c77-09c1785b8640.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.39801-formula125448"><label>(12)</label><graphic position="anchor" xlink:href="6-7401913\5354da4c-d1de-418f-a3d7-6620a1e02088.jpg"  xlink:type="simple"/></disp-formula><p>Since <img src="6-7401913\86418ca8-bc11-41d6-9474-58640ff687ec.jpg" /> is positive definite, and <img src="6-7401913\1f88c767-7b3d-494d-b799-a8331de684cd.jpg" /> is negative semi-definite, it follows that from the fact that</p><p><img src="6-7401913\93335a39-b2a3-4ad5-9cdd-ab60250e8976.jpg" /></p><p>It can easily be seen that <img src="6-7401913\50f5e8bb-b545-4c0e-9e0c-cd1443afe5f3.jpg" />From Equation (9) have<img src="6-7401913\13fe03fb-6db5-45e4-a5b8-f3e9352b6dbe.jpg" />. Thus, by Barbalat’s lemma, we have <img src="6-7401913\68ba5bdf-6f89-4bb7-82e2-f267c888ec55.jpg" /> Thus the response system (2) can be synchronized and anti-synchronized the drive system (1) globally and asymptotically. This completes the proof.</p></sec><sec id="s2_3"><title>2.3. Systems Description</title><p>The hyperchaotic Chen system [26,27] is given by:</p><disp-formula id="scirp.39801-formula125449"><label>(13)</label><graphic position="anchor" xlink:href="6-7401913\f08cc056-1443-4242-83c6-c4ce59459566.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401913\58d1ad35-d2f6-401f-8500-27bede79db15.jpg" /> and <img src="6-7401913\97b6312f-0395-4653-8769-e1386ef999e5.jpg" /> are state variables, and <img src="6-7401913\b41025e6-6a05-4a6f-8890-879a2b7f31e5.jpg" />, and <img src="6-7401913\98707593-a92e-49ef-9fc4-effda5bcab6d.jpg" />are real constants. When <img src="6-7401913\425f147b-dea3-400c-894f-0f8f173ec223.jpg" /> system (13) is chaotic, when <img src="6-7401913\0fa1efce-f721-4206-b7c1-fe09d6e7badf.jpg" />, system (13) is hyperchaotic.</p><p>The hyperchaotic Lorenz system [28,29] is described by</p><disp-formula id="scirp.39801-formula125450"><label>(14)</label><graphic position="anchor" xlink:href="6-7401913\7f48228b-e5cf-4a3f-be5b-c70960f55fe0.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="6-7401913\a8f78af4-0698-4a33-b1f2-9c9f2b45c3ae.jpg" />, and <img src="6-7401913\0143d9f1-bd44-4094-94d1-0746b112dd6a.jpg" />are state variables, <img src="6-7401913\c28671c5-ec86-4ef2-a038-b1d6960db52f.jpg" />and <img src="6-7401913\a8ad35a5-2bf0-407c-8345-12b494cff183.jpg" /> are real constants. When <img src="6-7401913\b07d5d8d-f13c-42a8-97e3-ddb4df7b5849.jpg" /> and <img src="6-7401913\34206d61-1013-441b-b5f3-3b3836b2aa37.jpg" /> system (14) has hyperchaotic attractor.</p><p>The hyperchaotic Lű system [<xref ref-type="bibr" rid="scirp.39801-ref30">30</xref>] is described by:</p><disp-formula id="scirp.39801-formula125451"><label>(15)</label><graphic position="anchor" xlink:href="6-7401913\791e6392-8c37-4691-a6ea-83ca06d7c5e3.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401913\0e296fb6-6d74-4f04-8aca-564dcacf6847.jpg" /> and <img src="6-7401913\05d3cbdb-ef35-4bdb-863f-709068e91753.jpg" /> are state variables, <img src="6-7401913\ce930899-c1dc-4593-9b0f-a9778714e8d0.jpg" />and <img src="6-7401913\fcdcdc19-9503-4809-964c-8337a3756cfc.jpg" /> are real constants. When <img src="6-7401913\2ffc9811-d799-4aec-b4ef-a8480f7ab10a.jpg" /> system (15) has hyperchaotic attractor.</p></sec></sec><sec id="s3"><title>3. Adaptive Hybrid Synchronization of Two Identical Hyperchaotic Systems with Unknown Parameters</title><p>In order to observe the efficacy of our proposed method, we used two hyperchaotic Chen systems where the master system is denoted with the subscript 1 and the response system having identical equations denoted by the subscript 2. The two systems are defined below.</p><disp-formula id="scirp.39801-formula125452"><label>(16)</label><graphic position="anchor" xlink:href="6-7401913\66d7c8a1-bc83-423e-aa62-53c5bd1c217d.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.39801-formula125453"><label>(17)</label><graphic position="anchor" xlink:href="6-7401913\bcffc975-abcd-40ff-845a-23bb5320b081.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401913\de0dbcb5-9f52-4810-a004-2566c9547ab8.jpg" /> are four control functions to be designed. For the hybrid synchronization, we define the state errors between the response system that is to be controlled and the controlling drive system as <img src="6-7401913\3804f79d-0c70-44bb-aeca-e03f8342cd5f.jpg" /><img src="6-7401913\3a417e3a-ef64-4a91-bfd3-6a15a10ac0d2.jpg" /><img src="6-7401913\fdf2ea3c-40cd-4a75-9923-9a84b9fe3bb7.jpg" />. The error system is given by</p><disp-formula id="scirp.39801-formula125454"><label>(18)</label><graphic position="anchor" xlink:href="6-7401913\859f2d98-943f-416d-aa1f-e939d64d1099.jpg"  xlink:type="simple"/></disp-formula><p>Now our goal is to find proper control functions <img src="6-7401913\72f6b816-6a14-4d92-97e3-b0c14ebb333c.jpg" /> and parameter update rule, such that system (17) globally hybrid synchronizes system (16) asymptotically. i.e., <img src="6-7401913\aa0cf9d4-17b9-4575-adc2-a90e7d1a103c.jpg" />where</p><p><img src="6-7401913\12d7979b-0096-475b-a520-84c908612df5.jpg" />If the two systems are without controls <img src="6-7401913\ccbd9f3f-56dd-41d7-95b2-efdc9cae696a.jpg" /> and the initial condition is:</p><p><img src="6-7401913\3132fcb8-52fd-487e-9a09-aef3ac187b6d.jpg" /></p><p>then the trajectories of the two systems will quickly separate each other and become irrelevant. However, when appropriate controls are applied the two systems will approach hybrid synchronization for any initial conditions. We shall propose the following adaptive control law for system (17).</p><p><img src="6-7401913\cb61ed5f-e893-4325-9bdc-32b7a7ec908c.jpg" /></p><p>where <img src="6-7401913\8f3fdd0d-9392-423e-950b-154ce7fb4367.jpg" /> are the estimates of <img src="6-7401913\910273fa-21f7-43e0-b77b-4d42da7b790e.jpg" /> respectively. Now, let us choose a controller <img src="6-7401913\238d733e-0764-474f-abcc-2f46c138eece.jpg" /> and parameters update law <img src="6-7401913\beb182aa-50c3-437e-93d2-02042ebaf130.jpg" /> as follows:</p><disp-formula id="scirp.39801-formula125455"><label>(19)</label><graphic position="anchor" xlink:href="6-7401913\b7781f65-df3c-4235-81a2-6cc3e7120e31.jpg"  xlink:type="simple"/></disp-formula><p>and the parameter update rule.</p><p>Consider the following Lyapunov function</p><disp-formula id="scirp.39801-formula125456"><label>(20)</label><graphic position="anchor" xlink:href="6-7401913\cdc80c27-0e02-4a0b-8fa6-72709f42f0d1.jpg"  xlink:type="simple"/></disp-formula><p>Consider the following Lyapunov function</p><p><img src="6-7401913\7463bb66-c408-437a-a3e1-1767093702a5.jpg" /></p><p>Then the time derivative of <img src="6-7401913\41561514-dfd8-44a1-a999-653fbbb63ed4.jpg" /> along the trajectories of Equation (18) is:</p><disp-formula id="scirp.39801-formula125457"><label>(21)</label><graphic position="anchor" xlink:href="6-7401913\0fbd3f36-f7a0-4610-ba56-cf101a6cc6af.jpg"  xlink:type="simple"/></disp-formula><p>Since <img src="6-7401913\f3abbae7-7057-4ce9-837f-0da078bad9fc.jpg" /> is positive definite function and <img src="6-7401913\6ae99137-addb-4861-982d-543666b8adaf.jpg" />is negative definite function, it translates to <img src="6-7401913\8dee5adc-6bd2-403b-b910-09151411d175.jpg" /> based on the Lyapunov stability theorem [<xref ref-type="bibr" rid="scirp.39801-ref31">31</xref>]. Therefore, the hyperchaotic Chen response system (17) is hybrid synchronized with hyperchaotic Chen drive system (16) with fully uncertain parameters under the adaptive controller (19) and the parameters update law (20).</p>Numerical Simulations<p>To verify and demonstrate the effectiveness of the proposed method, we discuss the simulation results for hyperchaotic Chen system. In the numerical simulations, the fourth-order Runge-Kutta method is used to solve the systems with time step size 0.001. For these numerical simulations, we used the initial conditions, <img src="6-7401913\f22611c6-af40-4413-ac9e-35a428e23fb7.jpg" /> and <img src="6-7401913\60edb0dc-fa58-474b-af3a-8926432407f0.jpg" />. Hence, the error system has the initial values <img src="6-7401913\2b1dec65-f99f-44c9-aac9-bddcfe78645d.jpg" /> and <img src="6-7401913\4ef85eb4-ccd5-4c6b-b520-80833db55666.jpg" />The unknown parameters are chosen as <img src="6-7401913\9b0dd89a-226c-4c2a-b915-95d43d5cafcc.jpg" /> and <img src="6-7401913\726ef6a7-6cfc-409a-943f-d3ce7bf8022b.jpg" /> such that the hyperchaotic Chen system exhibits chaotic behavior. Hybrid synchronization of systems (16) and (17) via adaptive control laws (Equations (19) and (20)) with the initial estimated parameters <img src="6-7401913\6deac727-3763-4e1f-a986-9c981de391ec.jpg" /> and <img src="6-7401913\be227946-3b9b-46ff-b6eb-45924c987f77.jpg" /> are shown in Figures 1 and 2. Figures 1(a) and (d) display state trajectories of drive system (16) and the response system (17). <xref ref-type="fig" rid="fig2">Figure 2</xref>(a) displays the hybrid synchronization errors between system (16) and (17). <xref ref-type="fig" rid="fig2">Figure 2</xref>(b) Shows that the estimates <img src="6-7401913\dae4a277-17ca-4bed-864a-17bf7611c769.jpg" /> and <img src="6-7401913\8772c642-632f-4240-8347-5076ce5f2851.jpg" /> of the unknown parameters converges to <img src="6-7401913\be8956cc-5745-478b-b2a7-4628dd64d138.jpg" /> and <img src="6-7401913\f598a050-09d5-433e-9530-eec1f7d80b87.jpg" /> as <img src="6-7401913\2a7aed89-7598-4b10-86ff-4a81ddfdbc04.jpg" /></p></sec><sec id="s4"><title>4. Adaptive Hybrid Synchronization between Two Different Hyperchaotic Systems</title><p>In order to observe the hybrid synchronization behavior between hyperchaotic Lorenz system (15) and hyperchaotic Lű system (14), we assume that hyperchaotic Lorenz system with four unknown parameters is the drive system and hyperchaotic Lű system with four unknown parameters is the response system. The drive and response systems are defined as follows:</p><p><img src="6-7401913\7d6efc5a-fdf1-4af2-bed2-05c001442048.jpg" /></p><p>and</p><disp-formula id="scirp.39801-formula125458"><label>(23)</label><graphic position="anchor" xlink:href="6-7401913\e74acc10-8981-4719-88ac-4e1e403d3c90.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401913\75329b71-8e57-411f-97a9-3bfb23368405.jpg" /> are four control functions to be designed. For the hybrid synchronization, we define the state errors between the response system that is to be controlled and the controlling drive system as <img src="6-7401913\8977b5ca-6c0b-41d8-8225-dea757379389.jpg" /></p><p>The error system is given by</p><disp-formula id="scirp.39801-formula125459"><label>(24)</label><graphic position="anchor" xlink:href="6-7401913\15284c52-f84a-460c-9c1e-5cbf17270910.jpg"  xlink:type="simple"/></disp-formula><p>Now our goal is to find proper control functions <img src="6-7401913\19e1d5d1-6f50-405e-a11d-2338b41f7b67.jpg" /> and parameter update rule, such that system (17) globally hybrid synchronizes system (16) asymptotically. i.e. <img src="6-7401913\f80373e0-4e5f-4ae8-aa23-5f1f552aa7e6.jpg" />where</p><p><img src="6-7401913\092b2f94-b41f-40e8-8a94-31f1e998c7c5.jpg" />. If the two systems are without controls <img src="6-7401913\52647541-f8b4-47ff-9efb-678aaaa82a3a.jpg" /> and the initial condition is</p><p><img src="6-7401913\9818b67f-f8ec-4127-8522-c367e6b57fcc.jpg" /></p><p>then the trajectories of the two systems will quickly separate each other and become irrelevant. However, when appropriate controls are applied the two systems will approach hybrid synchronization for any initial conditions. We shall propose the following adaptive control law for system (23). We define the parameters error <img src="6-7401913\5a15f11d-71b8-45ef-aeac-f52f344fc193.jpg" /> and</p><p><img src="6-7401913\3dac5fb5-b83d-4a94-958a-05deb34c4923.jpg" />where</p><p><img src="6-7401913\9d8884d5-dc2b-412b-9f79-5be6e587c613.jpg" />and <img src="6-7401913\dc3c33de-2213-40a8-8c58-cb924e119ff9.jpg" /> are the estimates of <img src="6-7401913\bca6b8c9-8a2e-4337-8257-7618dcb196ce.jpg" /> and <img src="6-7401913\5b812263-79cb-4e63-9788-b59d15b11f86.jpg" /> respectively. Now, let us choose a controller <img src="6-7401913\6c021b03-b594-4d60-9b69-facb14bfc0b6.jpg" /> and parameters update law <img src="6-7401913\f04c245b-cbca-435d-a8b1-157f90f5891e.jpg" /> as follows:</p><disp-formula id="scirp.39801-formula125460"><label>(25)</label><graphic position="anchor" xlink:href="6-7401913\66e48cc4-27ae-45d1-a0a0-545f1819d433.jpg"  xlink:type="simple"/></disp-formula><p>and the parameter update rule</p><disp-formula id="scirp.39801-formula125461"><label>(26)</label><graphic position="anchor" xlink:href="6-7401913\f4646418-1ca6-4bc4-ad72-a470552ab5b4.jpg"  xlink:type="simple"/></disp-formula><p>Consider the following Lyapunov function</p><p><img src="6-7401913\50b0db9d-f567-4317-98fd-3d75022189b9.jpg" /></p><p>Then the time derivative of <img src="6-7401913\4a524bae-12e9-4477-90bd-c372b6733870.jpg" /> along the trajectories of Equation (24) is</p><disp-formula id="scirp.39801-formula125462"><label>(27)</label><graphic position="anchor" xlink:href="6-7401913\8b1f0782-9044-42d3-b2d0-abf684fcbfbc.jpg"  xlink:type="simple"/></disp-formula><p>Since <img src="6-7401913\665f0fdd-f7ca-4098-a73a-30c1f26fe318.jpg" /> is positive definite function and <img src="6-7401913\02d8aad6-4c25-4e9e-affa-6d2c8abcf01b.jpg" /> is negative definite function, it translates to <img src="6-7401913\4d3d4341-da49-4993-867a-d27fb4682197.jpg" /> based on the Lyapunov stability theorem [<xref ref-type="bibr" rid="scirp.39801-ref31">31</xref>]. Therefore, the hyperchaotic Lű response system (14) is hybrid synchronized the hyperchaotic Lorenz drive system (15) with fully uncertain parameters under the adaptive controller (25) and the parameters update law (26).</p>Numerical Simulations<p>To verify and demonstrate the effectiveness of the proposed method, we discuss the simulation result for the hybrid synchronization between hyperchaotic Lorenz</p><p>system and hyperchaotic Lű system. In the numerical simulations, the fourth-order Runge-Kutta method is used to solve the systems with time step size 0.001. For this numerical simulation, we assume that the initial condition, <img src="6-7401913\f7ae5ca8-cec7-4f65-9cfc-b3e0bda96ecb.jpg" />and <img src="6-7401913\e549f12f-7100-40d0-b600-6c03709c4f23.jpg" /> is employed. Hence the error system has the initial values <img src="6-7401913\fd26913c-8d8f-4808-a889-67f9c3a0a1ae.jpg" /> and<img src="6-7401913\3e6d26ed-7d78-4f42-9625-f3fa257e24e7.jpg" />. The unknown parameters are chosen as</p><p><img src="6-7401913\6669ea9f-e610-42de-8a47-dd7944aac36b.jpg" />and</p><p><img src="6-7401913\4a4c27b9-fb2f-4572-8c14-2b60ca57996c.jpg" />in simulations so that both the systems exhibits a hyperchaotic behavior. Hybrid synchronization of and (26) with the initial estimated parameters</p><p><img src="6-7401913\9ea6216d-763e-4d16-a664-e7e97ff71ce5.jpg" />and <img src="6-7401913\4c3700a7-2e79-43b4-81a3-d7a63650cdf5.jpg" /> are shown in Figures 3 and 4. <xref ref-type="fig" rid="fig3">Figure 3</xref> displays state trajectories of drive system (22) and the response system (23). <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) displays the hybrid synchronization errors between system (22) and (23). Figures 3(b) and (c) show that the estimates <img src="6-7401913\3af8e4aa-635e-4054-b315-24e8a33ce389.jpg" />and <img src="6-7401913\89b6b50b-bfb2-4f8f-a149-11ea2ced0edf.jpg" /> of the unknown parameters converges to <img src="6-7401913\88fff78d-f33e-4c00-a3d7-99726b565838.jpg" /> and</p><p><img src="6-7401913\d0754d54-2f02-4df0-bfbd-3467af74fa66.jpg" />as<img src="6-7401913\3fb96417-8f32-4cea-8d11-875b3b7004be.jpg" />.</p></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, we discussed the problem of adaptive hybrid synchronization of hyperchaotic systems with fully unknown parameters. On the basis of the Lyapunov stability theory and the adaptive control theory, a new adaptive hybrid synchronization control law and a novel parameter estimation update law are proposed to achieve hybrid synchronization between the two identical and different hyperchaotic systems with uncertain parameters. This shows that our proposed method has strong robustness. 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