<?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.2013.410192</article-id><article-id pub-id-type="publisher-id">AM-37486</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>
 
 
  Matrix Measure with Application in Quantized Synchronization Analysis of Complex Networks with Delayed Time via the General Intermittent Control
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>unli</surname><given-names>Zhang</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>Department of Mathematics, Heze University, Heze, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>qunli-zhang@126.com</email></corresp></author-notes><pub-date pub-type="epub"><day>25</day><month>09</month><year>2013</year></pub-date><volume>04</volume><issue>10</issue><fpage>1417</fpage><lpage>1426</lpage><history><date date-type="received"><day>July</day>	<month>19,</month>	<year>2013</year></date><date date-type="rev-recd"><day>August</day>	<month>19,</month>	<year>2013</year>	</date><date date-type="accepted"><day>August</day>	<month>26,</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>
 
 
   This paper concerned with the quantized synchronization analysis problem. The scope of state vectors of dynamic systems, based on the matrix measure, is estimated. By using the general intermittent control, some simple yet generic criteria are derived ensuring the exponential stability of dynamic systems. Then, both the general intermittent networked controller and the quantized parameters can be designed, which guarantee that the nodes of the complex network are synchronized. Finally, simulation examples are given to illustrate the effectiveness and feasibility of the proposed method. 
 
</p></abstract><kwd-group><kwd>Matrix Measure; The General Intermittent Control; Exponential Stability; Quantized Synchronization; Complex Networks</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Since its origins in the work of Fujisaka and Yamada [1- 3], Afraimovich, Verichev, and Rabinovich [<xref ref-type="bibr" rid="scirp.37486-ref4">4</xref>], and Pecora and Carrol [<xref ref-type="bibr" rid="scirp.37486-ref5">5</xref>], the study of synchronization of chaotic systems [6-19] is of great practical significance and has received great interest in recent years. In the above literatures, the approach applied to stability analysis is basically the Lyapunov’s method. As we all know, the construction of a proper Lyapunov function usually becomes very skillful, and the Lyapunov’s method does not specifically describe the convergence rate near the equilibrium point of the system. Hence, there is little compatibility among all of the stability criteria obtained so far.</p><p>The concept named the matrix measur [20-25] has been applied to the investigation of the existence, uniqueness or stability analysis of the equilibrium. Intermittent control [26-29] has been used for a variety of purposes in engineering fields such as manufacturing, transportation, air-quality control and communication. A wide variety of synchronization or stabilization using the periodically intermittent control method has been studied (see [27- 32]). Compared with continuous control methods [7-14], intermittent control is more efficient when the system output is measured intermittently rather than continuously. All of intermittent control and impulsive control are belong to switch control. But the intermittent control is different from the impulsive control, because impulsive control is activated only at some isolated moments, namely it is of zero duation, while intermittent control has a nonzero control width.</p><p>But it should be mentioned that the influence caused by quantization has not been considered in their results. It is well known that in modern networked systems, quantization is an indispensable step that aims at saving limited bandwidth and energy consumption [<xref ref-type="bibr" rid="scirp.37486-ref33">33</xref>]. Quantization cannot be avoided in the digital control setting, and it is indeed a natural way to be inserted into the control design complexity constraints of the controller and communication constraints of the channels which connect the controller and the plant [<xref ref-type="bibr" rid="scirp.37486-ref34">34</xref>]. The important application of quantization in real world can be found in humanmachine interaction, for instance, see [35-37]. Therefore, it is essential and important to investigate the exponential quantized synchronization problem of networks with mixed delays by periodically intermittent control.</p><p>Our interest focuses on the class of commonly intermittent controller with time duration, where the control is activated in certain nonzero time intervals, and is off in other time intervals. A special case of such a control law is of the form</p><p><img src="9-7401737\80378a64-f53b-40ef-8c26-22364fcd6d95.jpg" /></p><p>where <img src="9-7401737\89954c5e-43e1-45cb-8316-95fce2864ba4.jpg" /> denotes the control strength, <img src="9-7401737\da41672b-abbd-400f-ab53-95e215f99fce.jpg" />denotes the switching width, and T denotes the control period. The general intermittent controller</p><p><img src="9-7401737\3a06bd26-4c1c-47fd-a703-2cd67e96184a.jpg" /></p><p>where <img src="9-7401737\952978e6-7206-4906-8036-263a8956abc6.jpg" /> is a strictly monotone increasing function on<img src="9-7401737\366cf7a8-5f28-422c-b235-1bbc9846e3f2.jpg" />, has been studied (see [<xref ref-type="bibr" rid="scirp.37486-ref38">38</xref>]).</p><p>Moreover, a logarithmic quantizer <img src="9-7401737\2340a65e-3c7f-4812-aec5-02b52139d4d0.jpg" /> has quantization levels give by</p><p><img src="9-7401737\9e915512-90c3-4796-b1a0-37b85b465d83.jpg" />where the quantization densitie is<img src="9-7401737\aae5be03-3252-468f-85c5-4fa12f1d2bb1.jpg" />, and the scaling parameter is<img src="9-7401737\0999ec02-7c19-4985-b6d0-854d229a659b.jpg" />. Then, the quantizer <img src="9-7401737\788e6325-c3ea-49a7-a0c3-ebe6e8bbd456.jpg" /> is defined as follow</p><disp-formula id="scirp.37486-formula152010"><label>(1)</label><graphic position="anchor" xlink:href="9-7401737\e9b0db6c-3bee-431f-a95a-d5d347d736be.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="9-7401737\382cc099-1689-4864-9afb-3bbc39fb21d3.jpg" />. Based on (1), it is obvious that<img src="9-7401737\bca115ee-312c-44ad-b1a4-196f706dd459.jpg" />and the quantization synchronization error <img src="9-7401737\ae356dda-cb06-4ebe-af2e-4440426132b4.jpg" /> (see [39-43]).</p><p>In this paper, based on matrix measure and Gronwall inequality, the general intermittent controller</p><p><img src="9-7401737\fe7476aa-0405-40e3-8e2e-192ded28faa1.jpg" /></p><p>where <img src="9-7401737\1b7e2f56-7145-44fc-bd69-deed67afafa5.jpg" /> is a strictly monotone increasing function on<img src="9-7401737\d4ecfcb4-7735-4d2d-ad88-ff90b5c7d2ca.jpg" />,</p><p><img src="9-7401737\438ff2ee-fe7e-449d-aed8-e40424170df4.jpg" /></p><p>where <img src="9-7401737\5c42a80c-5e6f-4861-8026-b2f66902a2dd.jpg" /> is a strictly monotone decreasing function on<img src="9-7401737\ecc60ed1-25a0-4df9-ab63-05d0cff55cbe.jpg" />, is designed. Then the sufficient yet generic criteria for synchronization of complex networks with and without delayed item are obtained.</p><p>This paper is organized as follows. In Section 2, some necessary background materials are presented. In Section 3, the state vectors scope estimated via matrix measure are formulated. Section 4 deals with the quantized synchronization. The theoretical results are applied to complex networks, and numerical simulations of delayed neural network systems are shown in this section. Finally, some concluding remarks are given in Section 5.</p></sec><sec id="s2"><title>2. Preliminaries</title><p>Let <img src="9-7401737\b3acc8a5-6cc6-4741-992b-3945f25e0b41.jpg" /> be a Banach space endowed with the l<sup>2</sup>-norm</p><p><img src="9-7401737\b93a8a7f-9add-405a-8c76-90c23c74c642.jpg" />, i.e.<img src="9-7401737\e178e7bc-9d86-46ba-87ab-4be6715455ad.jpg" />, where <img src="9-7401737\858e2568-1ce6-4d66-bcdd-8d1b365de703.jpg" /> is inner product, and <img src="9-7401737\8ca04ec7-4910-4ec6-b6a9-56ec090f7190.jpg" /> be a open subset of<img src="9-7401737\92b7d686-a7e6-48fa-89b4-dfc040f848e9.jpg" />. We consider the following system:</p><disp-formula id="scirp.37486-formula152011"><label>(2)</label><graphic position="anchor" xlink:href="9-7401737\84fa919d-2488-43a5-97f2-c269d063231c.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="9-7401737\b23ab607-ced9-4c43-a70e-d340da284213.jpg" /> are nonlinear operators defined on<img src="9-7401737\05076e99-7fda-4ebf-80b2-aa988107d70e.jpg" />, and <img src="9-7401737\2062230d-7767-4ae7-be58-e397519eaadc.jpg" /> <img src="9-7401737\533ba11a-e9a4-4722-9198-b2c95329afbc.jpg" />, and <img src="9-7401737\86271b26-e991-4e56-a7ed-5d61f4868c36.jpg" /> is a time-delayed positive constant, and<img src="9-7401737\2209f54b-80e9-4636-a128-08853251be6e.jpg" />.</p><p>Definition 1 [12,26,28,44] System (2) is called to be exponentially stable on a neighborhood <img src="9-7401737\85220d8a-183a-48cb-81fc-06454e3f35a4.jpg" /> of the equilibrium point, if there exist constants<img src="9-7401737\f853720c-20b1-4625-b3e1-03dfc5243b99.jpg" />, such that</p><p><img src="9-7401737\9bfb01e6-cf24-42e1-ae36-05b2d110a896.jpg" /></p><p>where <img src="9-7401737\b1b06f48-9c7a-41b7-a58a-a763d520d8ff.jpg" /> is any solution of (2) initiated from <img src="9-7401737\1eb8ef3d-91e7-4b58-a8ab-94f930824d9b.jpg" />.</p><p>Definition 2 [20-25] Suppose that <img src="9-7401737\785ab66f-0ba4-4ece-9578-766075541227.jpg" /> is a matrix. Let <img src="9-7401737\d5206dbd-f66e-455c-a196-96433ff899c1.jpg" /> be the matrix measure of <img src="9-7401737\00a72583-bd37-4fd7-afef-d511554e9d50.jpg" /> defined as</p><p><img src="9-7401737\88715c36-6dfb-4089-a302-1995aa9264e5.jpg" />where <img src="9-7401737\f99e4b0f-fdd3-4242-920a-e7d0c6ce95cb.jpg" /> is the identity matrix.</p><p>Lemma [20-25] The matrix measure <img src="9-7401737\29d718b6-049c-4d7f-aa83-c39aac9c4cdf.jpg" /> is well defined for the l<sup>2</sup>-norm<img src="9-7401737\0946ca41-c405-41f0-bc1b-42e8c6eec05f.jpg" />, the induced matrix measure is given by</p><p><img src="9-7401737\92b25dc4-d7f0-4c08-bc9f-4de3797bb2c2.jpg" /></p><p>where <img src="9-7401737\30931349-5579-4f58-a65e-502b843bcc27.jpg" /> denotes all eigenvalues of the matrix<img src="9-7401737\20822d4b-4228-433a-8c79-9ffe10c09be6.jpg" />.</p></sec><sec id="s3"><title>3. Estimating the Scope of the State Vectors</title><p>We consider the following system:</p><disp-formula id="scirp.37486-formula152012"><label>(3)</label><graphic position="anchor" xlink:href="9-7401737\f55ceb5d-dede-40d7-b188-3fdfe0062aed.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.37486-formula152013"><label>(4)</label><graphic position="anchor" xlink:href="9-7401737\090f5d38-332a-4fcd-ada9-469cd6aea9cc.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="9-7401737\27ae2fdf-cc98-4e9b-8fb4-47da0305bec7.jpg" /> are nonlinear operators defined on<img src="9-7401737\1e8418ed-ea59-4110-b8d6-b648e77ecebe.jpg" />, and <img src="9-7401737\3f9b029e-7e1c-4151-af04-8740aac68475.jpg" /> <img src="9-7401737\c8250812-56f0-4df4-8974-ac8ac196e850.jpg" />, and <img src="9-7401737\b3bcc908-d956-494d-99a7-0d46b085d7ce.jpg" /> is a timedelayed positive constant, and <img src="9-7401737\5029f392-3886-4e3a-b168-20de6d5c3039.jpg" />.</p><p>Theorem 1 For any <img src="9-7401737\6bf0200c-ca1a-419e-be57-25f9a1ac0778.jpg" /> in the system (3), (4), if the operator <img src="9-7401737\534e35c1-54af-4c00-a9af-cf11f755904b.jpg" /> satisfies</p><disp-formula id="scirp.37486-formula152014"><label>, (5)</label><graphic position="anchor" xlink:href="9-7401737\94cfa0fe-7f39-4ed3-bb2e-c45db52cb830.jpg"  xlink:type="simple"/></disp-formula><p><img src="9-7401737\3ba283ca-ed82-4363-afae-5ef8847d3832.jpg" />is bound, where <img src="9-7401737\c0748ea1-ca0d-415d-80e4-5f66b89a0214.jpg" /> is a positive constant. The solutions <img src="9-7401737\21b787f2-58f8-41ab-b380-9956787df6a5.jpg" /> initiated from <img src="9-7401737\f91eec80-d3a3-4eca-a1de-529eeba693d5.jpg" /> <img src="9-7401737\eba20481-2d5f-4d55-b909-cedbfbda0043.jpg" /> <img src="9-7401737\e0deaf71-5e1f-4d9a-a25e-e8f2f6e9bf43.jpg" /> of the system (3) and (4) satisfy</p><p><img src="9-7401737\482ee954-9ea8-40cd-aae1-eb11c02b1a5e.jpg" /></p><p>where <img src="9-7401737\8b0e8d58-aa26-44fd-8d50-8048f6c5cc31.jpg" /></p><p><img src="9-7401737\6116d9f0-36d8-43a5-a996-ba0fc65b3f19.jpg" /></p><p>Proof Under the initial conditions <img src="9-7401737\89d4d1dd-dcb9-4b28-b3e6-ba9e75d57494.jpg" /> <img src="9-7401737\bdba52e6-985a-43ff-a456-49a3d1f7731a.jpg" /> we have</p><p><img src="9-7401737\74c89295-ddfa-4a3a-b94e-951c5dfbff56.jpg" /></p><p>for any<img src="9-7401737\d7b4022e-6d19-40bf-8afb-5fffbdfe7f2f.jpg" />.</p><p>Let <img src="9-7401737\f4669d47-fa78-486c-a868-dea6681da952.jpg" /></p><p><img src="9-7401737\ea0f9e0a-1465-49ba-9c18-17a9e358eb8e.jpg" /></p><p>then</p><p><img src="9-7401737\5ed4239d-7797-4962-85d8-714b6b4ae3c5.jpg" /></p><p><img src="9-7401737\f4973b82-952c-4419-9698-a485ecd3dbcb.jpg" /></p><p>Using Cauchy-Bunyakovsky Inequality and condition (5), we obtain</p><p><img src="9-7401737\c9ca7195-5f5a-4a97-9c23-3c875f40c01a.jpg" /></p><p>So</p><p><img src="9-7401737\f06f6638-fa24-4eb9-b797-f45ebb3894d9.jpg" /></p><p><img src="9-7401737\645da873-12ce-4f61-bfb4-182cad067a44.jpg" /></p><p>Namely</p><p><img src="9-7401737\ae304bb0-8236-44c5-ae3e-63c00f18697e.jpg" /></p><p>Using the Gronwall inequality [45,46], we have</p><p><img src="9-7401737\21ff5d68-381e-4e8a-92a2-4870227db8c5.jpg" />that is</p><p><img src="9-7401737\4703b110-565b-4e5d-a593-3dba242d56f2.jpg" /></p></sec><sec id="s4"><title>4. Synchronization via the General Intermittent Control and Examples</title><p>Consider a delayed complex dynamical network consisting of <img src="9-7401737\67853d6a-bd38-4716-b349-af4b6e021fc1.jpg" /> linearly coupled nonidentical nodes described by</p><disp-formula id="scirp.37486-formula152015"><label>(6)</label><graphic position="anchor" xlink:href="9-7401737\982e03f1-02c2-4cc7-b487-e0b0161d4e69.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="9-7401737\5a7a3769-6619-4e08-beb2-c9afbf92594f.jpg" /> is the state vector of the ith node, <img src="9-7401737\02eb5569-62b1-40d8-8247-1d4970d5ab8f.jpg" />are nonlinear vector functions, <img src="9-7401737\eccf519e-47da-42c1-b17e-cbfb8f9c8cf3.jpg" />is the control input of the ith node, and <img src="9-7401737\33731cb5-d39b-4bd4-8797-fa6458b34a84.jpg" /> is the coupling figuration matrix representing the coupling strength and the topological structure of the complex networks, in which <img src="9-7401737\a29c8296-1cb8-4e97-9616-60130bbde172.jpg" /> if there is connection from node i to node <img src="9-7401737\d8e9a4d2-7315-40e2-aed4-5a2f9e486811.jpg" /> <img src="9-7401737\28628c2c-7934-45ae-9375-7fd93463ff60.jpg" />, and is zero, otherwise, and the constraint</p><p><img src="9-7401737\adb81fe2-1fe9-4505-9d62-3d7470fd3b5e.jpg" /><img src="9-7401737\312067fb-862f-475e-8bf0-cdf548bfce76.jpg" />, is set.</p><p>A complex network is said to achieve asymptotical synchronization if</p><disp-formula id="scirp.37486-formula152016"><label>, (7)</label><graphic position="anchor" xlink:href="9-7401737\64f708a1-6e95-4858-bd90-ee3f4779be20.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="9-7401737\787a3229-34a2-46c1-a0c1-c0124df2277e.jpg" /> is a solution of a real target node, satisfying</p><p><img src="9-7401737\ce8224a4-e315-49e7-ac0e-4018342aca67.jpg" />.</p><p>For our synchronization scheme, let us define error vector and control input <img src="9-7401737\51e4e6b5-8eb1-497b-93a0-bc1e0821315f.jpg" /> as follows, respectively:</p><p><img src="9-7401737\c287a632-5800-498e-be73-3c8739521661.jpg" />When <img src="9-7401737\38f252f3-9858-4d0d-8b0a-424d6c718144.jpg" /> is a strictly monotone increasing function on n with <img src="9-7401737\ca66bd79-f527-4443-a916-14c1346482ce.jpg" /></p><disp-formula id="scirp.37486-formula152017"><label>(8)</label><graphic position="anchor" xlink:href="9-7401737\ba78bcfd-86ab-445c-b76b-e9f0b01a6f45.jpg"  xlink:type="simple"/></disp-formula><p>When <img src="9-7401737\bc2f1520-9601-4c55-9beb-a3739b462d78.jpg" /> is a strictly monotone decreasing function on n with <img src="9-7401737\611598a7-0c4d-459b-9ea5-be3f83e683ce.jpg" /> <img src="9-7401737\3b980c23-0374-49de-9f00-081a6e2a5994.jpg" /></p><disp-formula id="scirp.37486-formula152018"><label>(9)</label><graphic position="anchor" xlink:href="9-7401737\35a77833-bdde-4b77-b5b1-829cc70fe9e6.jpg"  xlink:type="simple"/></disp-formula><p>In this work, the goal is to design suitable function <img src="9-7401737\2fa09f05-9c13-4677-af47-385dd3baeedb.jpg" /> and parameters<img src="9-7401737\8f9e8aed-560d-4786-a55b-f9e5e3434a55.jpg" />, <img src="9-7401737\421b65b2-7d41-40b0-8498-f479568bf2fb.jpg" />and <img src="9-7401737\ac88f2b7-4e38-440b-a4dd-4a3f64d30f6e.jpg" /> satisfying the condition (7). The error system follows from the expression (6), (8) and (9)</p><disp-formula id="scirp.37486-formula152019"><label>(10)</label><graphic position="anchor" xlink:href="9-7401737\532c1ae7-b338-4766-8abb-0a7f62fdaa3b.jpg"  xlink:type="simple"/></disp-formula><p>When <img src="9-7401737\a12adee6-373d-40ba-9c6b-7227169e62e7.jpg" /> is a strictly monotone increasing function on <img src="9-7401737\8aff0589-f132-49d0-8cdf-befd7fa724cf.jpg" /> with <img src="9-7401737\6450ab1e-ffca-4bba-abbb-ae6964ada638.jpg" /> <img src="9-7401737\37e0bd35-33bb-4a8f-894f-20a766efa6b3.jpg" /> we obtain the following result:</p><p>Theorem 2 Suppose that the operator <img src="9-7401737\ff82c16e-fcb3-417e-add8-cf0c8b3dabb7.jpg" /> in the network (6) satisfies condition (5), and <img src="9-7401737\c1dca08e-67b4-4705-a508-3816ead2f6b8.jpg" /> is defined as Definition 2,</p><p><img src="9-7401737\298f8bd6-cde4-48fc-935d-270c6dbc8342.jpg" /></p><p><img src="9-7401737\3be786b3-ae7d-4cfe-8db7-d78df1238d99.jpg" />where the constant</p><p><img src="9-7401737\00db86b9-3d5b-40b7-b9ec-785644798487.jpg" /></p><p><img src="9-7401737\43bf7928-f28d-4b86-acfd-9a90632dc793.jpg" /></p><p><img src="9-7401737\6215e890-bc7d-4360-bb26-251610644c39.jpg" /></p><p><img src="9-7401737\9efb95a9-1a9e-4da9-a359-888a042e3c72.jpg" /><img src="9-7401737\6055e00a-fbbe-462c-b24f-19b111cc84ea.jpg" /><img src="9-7401737\0af2fc40-7e3c-4772-818b-389e9e61e4b9.jpg" />satisfies <img src="9-7401737\b44ed94e-3ab8-47e3-aa2f-d61f2d18cd10.jpg" /></p><p>Then the synchronization of network (6) is achieved if the parameters<img src="9-7401737\bf966e82-4577-4349-8416-e054752981f7.jpg" />, <img src="9-7401737\4081537a-88ff-4a92-b41a-fd0be2365fc1.jpg" />, <img src="9-7401737\29db6320-d080-4a80-93b0-be90182c70b7.jpg" />, <img src="9-7401737\0c51f732-d0d2-4cd7-9395-0feab251b671.jpg" />and <img src="9-7401737\0cf277c3-c881-4afb-9b84-a9842dd75ea0.jpg" /> satisfy</p><disp-formula id="scirp.37486-formula152020"><label>(11)</label><graphic position="anchor" xlink:href="9-7401737\c7324b29-45e1-4190-af6a-9a3e39cf5221.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="9-7401737\a57c7e6f-e518-4c3a-bbaa-897eb623f57f.jpg" /> is the inverse function of the function <img src="9-7401737\4708527b-85f8-49d9-b87f-9643daca6357.jpg" /></p><p>Proof From Theorem 1, the following conclusion is valid:</p><disp-formula id="scirp.37486-formula152021"><label>(12)</label><graphic position="anchor" xlink:href="9-7401737\2c448be9-859d-48c2-8f9f-64cbb1579a02.jpg"  xlink:type="simple"/></disp-formula><p>for any<img src="9-7401737\5a70890f-7046-4d46-aefb-10c1b548ac2e.jpg" />;</p><disp-formula id="scirp.37486-formula152022"><label>(13)</label><graphic position="anchor" xlink:href="9-7401737\6d6d998a-a671-4d58-96fc-6815839ab7dd.jpg"  xlink:type="simple"/></disp-formula><p>for any<img src="9-7401737\f8a1e263-565a-40bd-9be8-a7e5a3357aa7.jpg" />.</p><p>In the following, we use mathematical induction to prove, for any nonnegative integer<img src="9-7401737\558e72e5-7853-4d4c-8b41-ae4f6da557e1.jpg" />,</p><disp-formula id="scirp.37486-formula152023"><label>(14)</label><graphic position="anchor" xlink:href="9-7401737\d21396f5-e7e5-491c-97ce-9e5451dbd9a4.jpg"  xlink:type="simple"/></disp-formula><p>1) For<img src="9-7401737\97e99d82-7631-465b-8a20-a09013a9c030.jpg" />, from (12) and (13), we can see that</p><p>a) For<img src="9-7401737\2e280862-1160-4479-a51d-516a963a1163.jpg" />,</p><p><img src="9-7401737\154e4651-1ba6-48f6-a4dc-bc310baaef3f.jpg" /></p><p><img src="9-7401737\44e525ca-9835-4ba3-bcdf-e09cb8753d7e.jpg" /></p><p>b) For<img src="9-7401737\45165f33-23de-4b34-863a-903fd899fec5.jpg" />,</p><p><img src="9-7401737\1b409013-27cb-433a-aa39-9ec6ab4da847.jpg" /></p><p>So (14) is true for<img src="9-7401737\c9963d16-0cae-4d20-ad1e-bb4d1c44bb89.jpg" />.</p><p>2) Assume that (14) is true for all<img src="9-7401737\64082f81-d089-488c-ad10-31b38f555cf6.jpg" />, that is</p><p><img src="9-7401737\e50a1d38-2137-44eb-a37e-8a8f35fed6c1.jpg" /></p><p><img src="9-7401737\8862e5f4-b469-49c5-b8d8-a224de6fc25d.jpg" /></p><p><img src="9-7401737\44023419-7375-4315-96f3-8c4a6738db4a.jpg" /></p><p>We will prove (14) is also true when<img src="9-7401737\7d2aa05e-4879-468d-bb36-747e509862e1.jpg" />. From (12) and (13), it is easy to see that</p><p><img src="9-7401737\4527c464-a912-4422-ba0d-27dca775f05b.jpg" /></p><p><img src="9-7401737\856f29c5-c8b3-4130-8153-cea4a132cf1a.jpg" /></p><p>Then, for<img src="9-7401737\1f1dc02b-23dd-4c14-a6c9-5d2a813503e0.jpg" />, we have</p><p><img src="9-7401737\635a1c2c-53c2-4786-9d4f-92921472c2ae.jpg" /></p><p><img src="9-7401737\94f48bb9-6aa9-4bd0-a158-b38846cd9a4a.jpg" /></p><p>and also, for<img src="9-7401737\017ab616-b281-4a57-a26b-8d21ee9011a9.jpg" />, it follows from above results that</p><p><img src="9-7401737\1dcefd42-9c4b-4dde-bb52-addc1c7acfef.jpg" /></p><p>From above discussion, we can see that the (14) is always correct for any nonnegative integer<img src="9-7401737\48b737be-b37c-4e63-ba05-686a79f26420.jpg" />.</p><p>When <img src="9-7401737\1707448c-c3fc-4ff2-82be-63d9a06e569d.jpg" /> is a strictly monotone increasing function on <img src="9-7401737\04d10469-4543-4bc5-ae4f-6ceba83dd900.jpg" /> and<img src="9-7401737\1b9ce86b-ecf7-448d-95e0-d99d6050c613.jpg" />, it is easy to obtain <img src="9-7401737\69629041-0179-48b2-9939-fb9597a423fb.jpg" /></p><p><img src="9-7401737\ce36bcc8-b223-43fb-8f99-059d5a5cf424.jpg" /></p><p>When <img src="9-7401737\710bbb87-bee7-4674-9f74-261c1c7c2812.jpg" /> is a strictly monotone increasing function on <img src="9-7401737\7cd54de9-2ca0-4aca-9bb8-a8f16fba1ce5.jpg" /> and<img src="9-7401737\088f32b3-3ad6-4172-a2d6-b297e09659f8.jpg" />, it follows that</p><p><img src="9-7401737\d1fba637-3b7a-428c-abd4-15636ebe8827.jpg" /></p><p><img src="9-7401737\6eb272cf-f4f2-4f93-a81c-457834a0c010.jpg" /></p><p><img src="9-7401737\f1ba9bad-bce7-42cf-a350-da7c95246e55.jpg" /></p><p>then</p><p><img src="9-7401737\f1964521-f62b-4621-aa49-358fe7ad882e.jpg" /></p><p>Therefore</p><p><img src="9-7401737\df99cb27-adc7-4dbb-8cd4-46c453488da2.jpg" /></p><p>when <img src="9-7401737\b6408bf1-8143-4766-a40f-8d38ad5a2500.jpg" /> <img src="9-7401737\978cf4aa-31a2-4d38-a3f1-ba0a19e05e07.jpg" /> <img src="9-7401737\8e0f93fd-04c4-4347-8bf5-ab7c9d6f2e48.jpg" /> is obtained under the condition (11). So the synchronization of the network (6) is achieved.</p><p>When <img src="9-7401737\8f89c7c2-b309-48c8-bab0-2c5074bd3e02.jpg" /> is a strictly monotone decreasing function on <img src="9-7401737\69939505-3757-4c59-b6c5-abf56ca234b2.jpg" /> with<img src="9-7401737\f7fe5f90-af3b-48e2-a487-8877a380bac7.jpg" />, we obtain the following result:</p><p>Theorem 3 Suppose that the operator <img src="9-7401737\f3084862-86ad-4603-985b-9b6e0a2a3f32.jpg" /> in the network (6) satisfies condition (5), and <img src="9-7401737\aefa73dc-29f3-443c-88fd-d9bd4b8a1a9f.jpg" /> is defined as Definition 2, <img src="9-7401737\377ad263-677b-4461-85ec-fc30a9f0a023.jpg" /> <img src="9-7401737\f449012b-c21c-4915-b1dd-0d0e90e2cdd0.jpg" /> <img src="9-7401737\5ba3b2ff-d90b-4ef3-83a6-941d0770b0f5.jpg" /> <img src="9-7401737\43331de0-ac89-417d-9837-12b51d36a6ae.jpg" /></p><p>where the constant</p><p><img src="9-7401737\d285dcd9-bb15-42b5-b08b-96edfa35f326.jpg" /></p><p><img src="9-7401737\f19f90ac-adbb-4e6e-a6c4-cfe0b310b52e.jpg" />are the same as Theorem 2. So the synchronization of networks (6) is achieved if the parameters<img src="9-7401737\645519c6-9d52-4da3-8fcf-1d9524a20ad2.jpg" />, and <img src="9-7401737\e67bad10-a7c3-4502-9ea3-f5d373a10e42.jpg" /> satisfy</p><disp-formula id="scirp.37486-formula152024"><label>(15)</label><graphic position="anchor" xlink:href="9-7401737\2559e455-938c-49ed-8d23-3885692bb621.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="9-7401737\96460c78-3b22-4031-9501-47f67da29eb1.jpg" /> is the inverse function of the function <img src="9-7401737\e9ea6a83-f79d-4c3c-a06b-3f65b322791d.jpg" /></p><p>Proof From Theorem 1, the following conclusion is valid:</p><disp-formula id="scirp.37486-formula152025"><label>(16)</label><graphic position="anchor" xlink:href="9-7401737\9f34d4b2-5f3d-45b7-bbaf-b2cb65ac7b00.jpg"  xlink:type="simple"/></disp-formula><p>for any<img src="9-7401737\ff777755-af53-4844-b880-1d847a4e29e5.jpg" />;</p><disp-formula id="scirp.37486-formula152026"><label>(17)</label><graphic position="anchor" xlink:href="9-7401737\be4703b6-72c2-4df5-8fad-14a574cc055d.jpg"  xlink:type="simple"/></disp-formula><p>for any<img src="9-7401737\6dac0f17-d777-41c2-a561-909e92235208.jpg" />.</p><p>From (16) and (17), imitating Theorem 2,we can prove</p><p><img src="9-7401737\edd08959-ab68-4099-a4c3-e1e1b25ed683.jpg" /></p><p>where</p><p><img src="9-7401737\379b8014-40ed-4cc5-a956-8c063867cfa8.jpg" />,</p><p><img src="9-7401737\32d6d29c-6152-4be7-8cad-8921e5dc6db0.jpg" />,</p><p><img src="9-7401737\5dd8e40c-d685-496e-b445-0efed2b329a5.jpg" />,</p><p><img src="9-7401737\f0e2dac2-4960-4007-9f70-8430021d0b85.jpg" />.</p><p>when <img src="9-7401737\3d39bc62-643b-4a4f-a2ea-4b82314eac4b.jpg" /> is obtained under the condition (15). So the synchronization of network (6) is achieved.</p><p>Corollary 1 Supposing that <img src="9-7401737\bdfba004-24ef-4839-a243-40ea65a25f6c.jpg" /> <img src="9-7401737\7066d1d1-e60b-43ca-a001-169bb2d3fd18.jpg" /> <img src="9-7401737\5a6dce63-01d6-4ccc-9eb1-216ba698e8f3.jpg" />, and the rest of restricted conditions are invariable. Then the synchronization of the network (6) is achieved if the parameters<img src="9-7401737\79e9b445-d0da-4aa5-ba0c-6e0180c9f25a.jpg" />, <img src="9-7401737\7cf7e7fc-70fa-4e7e-a1a6-f01cff44e3ac.jpg" />and <img src="9-7401737\9b6ba004-1908-412a-a3b6-cefe8a5ee9a7.jpg" /> satisfy</p><p><img src="9-7401737\1b452867-af6c-4dbb-9327-02131ebe07ff.jpg" /></p><p>Corollary 2 when we add normally distributed white noise randn (size(t)), the result similar to Theorem 2 and Theorem 3 is obtained if the condition (11) or (12) , respectively, is satisfied.</p><p>In the simulations of following examples, we always choose <img src="9-7401737\62a32a5c-8383-4ffd-9405-a6bee0843cf7.jpg" /> the matrix</p><p><img src="9-7401737\62fcbe15-5d73-4c63-9396-8dbe68f07a9d.jpg" />.</p><p>Let the initial condition be</p><p><img src="9-7401737\9582802c-a1c5-4fe6-a461-73ab8517fda3.jpg" /></p><p>Example 1 Consider a delayed system [<xref ref-type="bibr" rid="scirp.37486-ref47">47</xref>]:</p><disp-formula id="scirp.37486-formula152027"><label>(18)</label><graphic position="anchor" xlink:href="9-7401737\b52879bb-6c1b-437f-8c01-26c09e1bd4e7.jpg"  xlink:type="simple"/></disp-formula><p>The function<img src="9-7401737\2b14158d-b076-4bb3-b77e-53a6710a7a24.jpg" />, <img src="9-7401737\08371498-64cf-4899-b150-419ca8b625a8.jpg" /><img src="9-7401737\1f4880e3-5cd3-4c56-b999-ac892fd499c7.jpg" />which are the strictly monotone increasing or decreasing function on<img src="9-7401737\e8251c45-921d-4691-b6a2-6c2dd6d6d496.jpg" />, respectively, then they can be clearly seen that the synchronization of network (6), which is composed of system (18), is realized in Figures 1-4 (Excited by parameter white-noise), respectively.</p></sec><sec id="s5"><title>5. Conclusion</title><p>Approaches for quantized synchronization of complex networks with delayed time via general intermittent which uses the nonlinear operator named the matrix measure have been presented in this paper. Strong properties of global and exponential synchronization have been achieved in a finite number of steps. Numerical simulations have verified the effectiveness of the method.</p></sec><sec id="s6"><title>REFERENCES</title></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.37486-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">H. Fujisaka and T. Yamada, “Stability Theory of Syn     chronized Motion in a Coupled-Oscillator System,” Pro     gress of Theoretical Physics, Vol. 69, No. 1, 1983, pp. 32-47. http://dx.doi.org/10.1143/PTP.69.32</mixed-citation></ref><ref id="scirp.37486-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">H. Fujisaka and T. 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