<?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">IJCNS</journal-id><journal-title-group><journal-title>International Journal of Communications, Network and System Sciences</journal-title></journal-title-group><issn pub-type="epub">1913-3715</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijcns.2012.512085</article-id><article-id pub-id-type="publisher-id">IJCNS-25435</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject></subj-group></article-categories><title-group><article-title>
 
 
  Periodic Solutions of Cohen-Grossberg-Type BAM Neural Networks with Time-Varying Delays
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>iming</surname><given-names>Liu</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>Shaoning</surname><given-names>Li</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>College of Mathematics and Information Science, Shaanxi Normal University, Xi’an, China</addr-line></aff><aff id="aff1"><addr-line>Institute of Applied Mathematics, Shijiazhuang Mechanical Engineering College, Shijiazhuang, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>lqmmath@yahoo.com.cn(IL)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>14</day><month>12</month><year>2012</year></pub-date><volume>05</volume><issue>12</issue><fpage>810</fpage><lpage>814</lpage><history><date date-type="received"><day>September</day>	<month>12,</month>	<year>2012</year></date><date date-type="rev-recd"><day>October</day>	<month>25,</month>	<year>2012</year>	</date><date date-type="accepted"><day>November</day>	<month>6,</month>	<year>2012</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>
 
 
  Sufficient conditions to guarantee the existence and global exponential stability of periodic solutions of a Cohen-Grossberg-type BAM neural network are established by suitable mathematical transformation.
 
</p></abstract><kwd-group><kwd>Cohen-Grossberg Neural Networks; BAM Neural Networks; Periodic Solution; Delay; Global Stability</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Many important results on the existence and global exponential stability of equilibria of neural networks with time delays have been widely investigated and successfully applied to signal processing system. However, the research of neural networks involves not only the dynamic analysis of equilibrium point but also that of periodic oscillatory solution. In practice, the dynamic behavior of periodic oscillatory solution is very important in learning theory [1,2], which is motivated by the fact that learning usually requires repetition, some important results for periodic solutions of Hopfield neural networks or Cohen-Grossberg neural networks with delays have been obtained in Refs. [3-15].</p><p>The objective of this paper is to study the existence and global exponential stability of periodic solutios of a class of Cohen-Grossberg-type BAM neural networks (CGBAMNNs) with time-varying delays by suitable mathematical transformation.</p><p>The rest of this paper is organized as follows: preliminaries are given in Section 2. Sufficient conditions which guarantee the existence and global exponential stability of periodic solutions for the CGBAMNNs are established Section 3. An example is given in Section 4 to demonstrate the main results.</p></sec><sec id="s2"><title>2. Preliminaries</title><p>Consider the following periodic CGNNs with timevarying delays (see Equation (1)):</p><p>For<img src="3-23610\345c1644-702d-4f94-86aa-98a8e76d17b2.jpg" />, <img src="3-23610\6a2756fb-6991-48e3-9298-63fc1bc6e86d.jpg" />and<img src="3-23610\5538171b-3d65-453d-86c3-a844461f7abc.jpg" />. <img src="3-23610\b209332a-cb18-4b70-9091-620941be7173.jpg" />denote the state variables of the ith neuron, <img src="3-23610\81ab7b3f-b7e7-4751-bc15-f9cc3f2a2ff1.jpg" />denote the signal functions of the jth neuron at time t; <sub>&#160;<img src="3-23610\5a8cb8d3-e7c8-4a65-9329-754c8bc74bae.jpg" /></sub>denote inputs of the ith neuron at time t; <img src="3-23610\3d344a90-810c-4fb1-b101-c61cd6093bfc.jpg" />represent amplification functions; <img src="3-23610\68554a87-0618-491f-9b2b-0c2b81069273.jpg" />are appropriately behaved functions; <img src="3-23610\cfd1b2c7-d030-412a-9f3e-1016c02ba3c5.jpg" />and <img src="3-23610\9f8f7b7f-72ec-4afb-a290-5608c136d8c2.jpg" /> and are connection weights of the neural networks, respectively; <img src="3-23610\e402246c-bb39-413b-a9d3-abf35a76d95d.jpg" />are positive constants which correspond to the neuronal gains associated with the neuronal activations; <img src="3-23610\e3f8d5c5-dbe8-4527-be01-d76c81009f45.jpg" />correspond to the finite speed of the axonal signal transmission at time t and there exist constants <img src="3-23610\0feb9cd8-5b58-4357-8d02-85a354984e55.jpg" />such that<img src="3-23610\57983393-ff1e-4326-a6fb-a1f80f178269.jpg" />, <img src="3-23610\0b154a56-78dc-4550-ac2d-01f635c8419e.jpg" />and <img src="3-23610\a14e4c23-13cf-4541-8fcd-019cadb1c117.jpg" /> are all continuously periodic functions on [0, +∞) with common period T &gt; 0.</p><p>Throughout this paper, we assume for system (1) that</p><p>(H<sub>1</sub>) Amplification functions <img src="3-23610\b4781a31-1b41-4739-acc2-a6289b1872dc.jpg" /> are continuous and there exist constants <img src="3-23610\bad6c263-d5e5-4662-8ac8-5f67e1b6cfaa.jpg" />such that <img src="3-23610\596e7d1b-2f0a-4e3f-92c9-13acb596869f.jpg" /> for<img src="3-23610\33f50340-be95-41b5-ad22-a2cb57fc213d.jpg" />.</p><p>(H<sub>2</sub>) <img src="3-23610\1c988f34-b316-4e07-ab86-db91b2d0b06d.jpg" />are T-periodic about the first argument and there exist continuous T-periodic functions <img src="3-23610\a32f82c9-2da8-45b6-99e7-860ab43bfe21.jpg" /> such that</p><p><img src="3-23610\97527273-3b88-441c-9b91-4275a1a0e711.jpg" />.</p><p>(H<sub>3</sub>) For activation functions<img src="3-23610\06f95f24-3b25-480c-94aa-86eab9b3c1e0.jpg" />, there exist positive constants <img src="3-23610\799e73c0-f25a-42c0-b5dd-2105f99c31da.jpg" /> such that</p><disp-formula id="scirp.25435-formula79434"><label>(1)</label><graphic position="anchor" xlink:href="3-23610\7a403c3d-e2b3-4f23-90b1-c933435103e8.jpg"  xlink:type="simple"/></disp-formula><p><img src="3-23610\3407954c-00fb-480c-875c-53978dea829e.jpg" /></p><p>For any continuous function <img src="3-23610\6ba0aa0c-a961-4b4a-9f49-df9b1722e7a0.jpg" /> on<img src="3-23610\bd7b7c27-b80a-45f8-96af-85bfef74bea1.jpg" />, <img src="3-23610\7b42d5f9-3b33-4fa7-9762-8be9ab315de0.jpg" /></p><p>and <img src="3-23610\4542b8c3-8b8d-4b9e-afd7-aeee832cbf64.jpg" /> denote <img src="3-23610\681cb8d3-eaf0-4d88-ae0b-be01c0f2a63f.jpg" /> and<img src="3-23610\10e960bd-677a-4a39-92c3-978a9a23b47a.jpg" />respectively.</p><p>For any</p><p><img src="3-23610\884f3164-5de2-4034-959f-327d605ac310.jpg" />define</p><p><img src="3-23610\50927c6b-c20f-4db9-a879-0089444b9806.jpg" />and for any</p><p><img src="3-23610\ca12f87b-f841-42e4-b808-2c9b8282cad4.jpg" />,</p><p><img src="3-23610\21bd8b9e-7bde-452f-9344-5a8b3e685f95.jpg" />define</p><p><img src="3-23610\919aaf37-c7a9-4cb5-b200-ef1e743cb7b7.jpg" /></p><p>in which</p><p><img src="3-23610\c8065c43-080d-4122-aff9-e3a94afe93ba.jpg" />.</p><p>Denote</p><p><img src="3-23610\3861993b-a48b-4eed-87af-6169f2d87a05.jpg" /></p><p>is continuous on<img src="3-23610\3dc4eb3e-459a-464e-a8b0-647839b4ace1.jpg" />.</p><p>Then <img src="3-23610\dfdd8181-78f5-4fa2-9b7a-1951f6c90ee6.jpg" /> is a Banach space with respect to<img src="3-23610\c973fcb8-5bec-411c-8873-a3e53e457c62.jpg" />.</p><p>The initial conditions of system (1) are given by</p><disp-formula id="scirp.25435-formula79435"><label>(2)</label><graphic position="anchor" xlink:href="3-23610\c883856a-aa27-4ed5-b1de-49418d95b6d8.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="3-23610\8b9a6390-2059-4128-9bf1-164e24489c14.jpg" />.</p><p>Le <img src="3-23610\e588a370-31ba-45ce-baf0-719572470718.jpg" /> denotes any solution of the system (1) with initial value<img src="3-23610\689ef5cd-89a4-418b-affb-cc3e6550b431.jpg" />.</p><p>Definition 1. An solution <img src="3-23610\7df8b470-b460-48dd-aac7-574a021e6bd0.jpg" /> of system (1) is said to be globally exponentially stable, for any solutions <img src="3-23610\fcaf1108-29b9-4a38-81e6-f674180bcb6e.jpg" /> of the system (1), if there exist positive constant <img src="3-23610\ac39fb6e-c4b2-411d-90e5-31b768aabf12.jpg" /> and <img src="3-23610\7fb5e543-d428-4961-8200-a4209ef26c24.jpg" /> such that</p><disp-formula id="scirp.25435-formula79436"><label>(3)</label><graphic position="anchor" xlink:href="3-23610\c9200ac1-e2dd-4d4d-acf1-f40b23ac4617.jpg"  xlink:type="simple"/></disp-formula><p>Lemma 1. Under assumptions (H<sub>1</sub>)-(H<sub>3</sub>), system (1) has a T-periodic solution which is globally exponentially stable, if the following conditions hold.</p><p>(H<sub>4</sub>) Assume that there exist constants <img src="3-23610\e413abcc-c21a-4be6-b51f-4e4140c55281.jpg" /> such that<img src="3-23610\41f687a8-3c59-445b-be1e-bc22a9572728.jpg" />,<img src="3-23610\d39b14c0-062d-4135-ad28-24f0b3539f7e.jpg" />.</p><p>(H<sub>5</sub>) <img src="3-23610\efb42050-a317-43d4-83f6-718d0e2d004a.jpg" />is a nonsingular M-matrix, where</p><disp-formula id="scirp.25435-formula79437"><graphic  xlink:href="3-23610\8720255a-23d1-4988-9160-c6dbe8746a04.jpg"  xlink:type="simple"/></disp-formula><p>Proof. If<img src="3-23610\a4dd926a-8edb-402c-aaee-dfec58d5f677.jpg" />, the model (2.1) in [<xref ref-type="bibr" rid="scirp.25435-ref14">14</xref>] reduces to the system (1), we know that Lemma 1 holds from Theorem 3.1 with r = 1 in [<xref ref-type="bibr" rid="scirp.25435-ref14">14</xref>].</p></sec><sec id="s3"><title>3. Periodic Solutions of CGBAMNNs with Time Varying Delays</title><p>Consider the following CGBAMNNs with time-varying delays:</p><disp-formula id="scirp.25435-formula79438"><label>(4)</label><graphic position="anchor" xlink:href="3-23610\714d1b23-d45b-41ce-93e8-18c8d6924c43.jpg"  xlink:type="simple"/></disp-formula><p>for<img src="3-23610\b239a1c9-f1a8-4308-8849-7a28d1445e59.jpg" />, <img src="3-23610\93882539-85f8-4c3f-be12-3f3d0684ef32.jpg" />and <img src="3-23610\e292267e-0fef-43d5-a5ba-35db83a42eb1.jpg" /><img src="3-23610\9107ab39-4370-490e-a624-70452c92d2d7.jpg" /> and <img src="3-23610\b2cd9982-051d-4bdd-b18a-c88c65fafeb9.jpg" /> denote the state variables, <img src="3-23610\3de5f5b7-d6b0-4f56-82a3-66b455c6c15e.jpg" />and <img src="3-23610\a0937231-2b2d-4c36-aa02-71940e299501.jpg" /> denote the signal functions, <img src="3-23610\d930f2b7-9d9b-455f-ae81-034c5ecfb616.jpg" />and <img src="3-23610\01b224ae-0ff6-49f1-a5cb-c89acddb696d.jpg" /> denote inputs;<sub> <img src="3-23610\079495e2-137f-4699-b8a2-26796fd5b442.jpg" /></sub>and <img src="3-23610\0adc2f03-6198-4046-b647-21a40f6b6e15.jpg" /> represent amplification functions; <img src="3-23610\82dad6f1-d2ff-427c-83e5-205a57190b64.jpg" />and <img src="3-23610\f1a115eb-a616-41bb-8605-4730587a7194.jpg" /> are appropriately behaved functions;<img src="3-23610\a8fdee6b-2966-47a7-a1af-41c242e01679.jpg" />, <img src="3-23610\fb41bc2a-e1ac-4b70-8baf-1011544ebdbf.jpg" />, <img src="3-23610\edff4109-a45a-4939-b427-8799d022e734.jpg" />and <img src="3-23610\7c810329-1ccb-4d4d-be7b-dd8993b215c4.jpg" /> are the connection weights and<img src="3-23610\054f9188-e5d5-4b17-a77b-ae45cd6e2e36.jpg" />, <img src="3-23610\4fa49528-9379-4099-b168-5169f138277f.jpg" />are positive constants, which correspond to the neuronal gains associated with the neuronal activations; Time delays <img src="3-23610\d3a4bcb8-0274-480f-8a43-c0738f7b1cda.jpg" /> and <img src="3-23610\0f9c4c77-fe86-4951-b98c-ff57dc333911.jpg" /> correspond to the finite speed of the axonal signal transmission at time t and there exist constants <img src="3-23610\29cb56bb-458c-4455-aed8-9cf999d54111.jpg" /> and <img src="3-23610\5d5a1c3c-3b21-4d32-93b9-89e1a0fc11cb.jpg" /> such that<img src="3-23610\83c83b69-cb8b-471f-ba3f-453a2e6b8a01.jpg" />,<img src="3-23610\292e10d1-fde0-4f5d-92b4-8f88b16180c5.jpg" />;<img src="3-23610\dfc5e50e-0d4b-41d8-87ab-46f0f308ad1e.jpg" />, <img src="3-23610\84b701ba-a8a2-47d1-bd9f-27b7c63d593f.jpg" />, <img src="3-23610\8c22356f-7320-4001-9204-6716356bfcb8.jpg" />, <img src="3-23610\604a3350-887a-424a-9d5d-dcc11b91156f.jpg" />, <img src="3-23610\56c9842a-4188-4739-9380-fd78007db2c3.jpg" />, <img src="3-23610\fb9f97b1-9277-4aa7-87b1-31382d9d64f2.jpg" />, <img src="3-23610\5db29986-93c1-4588-809c-1b6830f885c4.jpg" />and <img src="3-23610\def2c2e0-e546-43c8-8580-0ef1f04df638.jpg" /> are all continuously periodic functions on <img src="3-23610\ed2c45d2-c914-403c-8e37-081bfb3f77cd.jpg" /> with common period<img src="3-23610\32989819-a195-4d50-b44a-e8882cad111a.jpg" />.</p><p>Throughout this paper, we assume for system (4) that</p><p>(H<sub>6</sub>) Amplification functions <img src="3-23610\0449ffb6-4409-4a64-b6bc-c773e27e28bf.jpg" /> and <img src="3-23610\fbc26c0a-d57a-4f0a-bd07-71017354da03.jpg" /> are continuous and there exist positive constants <img src="3-23610\0fee7aea-343a-436e-802b-c0530479770d.jpg" /> and <img src="3-23610\de766d5f-bbc2-42eb-a6c6-c0796997cd68.jpg" /> such that<img src="3-23610\ba2fe55a-9684-470e-a7a7-db868cced7b1.jpg" />, <img src="3-23610\ad04c466-d438-41a5-bed8-17526f089173.jpg" />,<img src="3-23610\92530a03-b33a-4590-a4e0-c129b5a2c098.jpg" />.<sub> </sub></p><p>(H<sub>7</sub>)<img src="3-23610\90f4fe06-6093-4ba4-a1bc-e472d1cbc666.jpg" />, <img src="3-23610\ad9b8584-52fd-49fe-b63b-b5a4ed4c6c5c.jpg" />are T-periodic about the first argument and there exist continuous T-periodic functions <img src="3-23610\82235c74-6ebc-4a7b-9c1c-9c44502cd594.jpg" /> and <img src="3-23610\554477d8-da6d-409f-8e79-0235c32fd8d8.jpg" /> such that</p><p><img src="3-23610\8fd4cf5f-b9fe-4d84-8535-3143263a833d.jpg" /></p><p>(H<sub>8</sub>) For activation functions<img src="3-23610\0111c0d4-125a-4217-ae13-7603980de772.jpg" /> and<img src="3-23610\1e8658e9-612f-470f-9404-9f15468c42b1.jpg" />, there exist constants <img src="3-23610\9946800d-46c6-44a4-a0ab-a7a8f98a0979.jpg" /> and <img src="3-23610\989528f9-1ee4-4b3d-800b-42f301c5e85a.jpg" /> such that</p><disp-formula id="scirp.25435-formula79439"><graphic  xlink:href="3-23610\b0f36520-745d-4829-a044-d2a8f7e2372a.jpg"  xlink:type="simple"/></disp-formula><p>The initial conditions of system (4) are given by <sub></sub></p><p><img src="3-23610\47928345-168d-4219-b66f-53f731a67f1e.jpg" /></p><p>where</p><p><img src="3-23610\8a49a519-e6a5-4eec-9198-3b83980c06ae.jpg" />,</p><p><img src="3-23610\7a9c5321-c277-4e8b-8ce6-89ce7654af4e.jpg" /></p><p>Theorem 1. Under assumptions (H<sub>6</sub>)-(H<sub>10</sub>), system (4) has a T-periodic solution which is globally exponentially stable, if the following condition holds.</p><p>(H<sub>9</sub>) Assume that there exist constants <img src="3-23610\cfedf1be-9815-4ff3-b785-88fa58472f01.jpg" /><sup> &#160;</sup>and <img src="3-23610\e47e6156-82e8-4b7d-be94-be1abbcd69b1.jpg" /> such that <img src="3-23610\19686803-0c3c-40d0-8e32-8ffefd748e20.jpg" /> and <img src="3-23610\ffcb6f5f-cda7-48a9-ac2f-57ef24ead319.jpg" /> hold for<img src="3-23610\b86eabd1-4adf-4cff-9539-131318d7bb76.jpg" />.<sub></sub></p><p>(H<sub>10</sub>) The following<img src="3-23610\a9d8ccb2-6af9-4bef-bde9-bac1230f8bf4.jpg" />is a nonsingular M-matrix, and</p><disp-formula id="scirp.25435-formula79440"><label>(5)</label><graphic position="anchor" xlink:href="3-23610\8910ce6e-f6b8-4b72-b017-3b9797420357.jpg"  xlink:type="simple"/></disp-formula><p>in which</p><p><img src="3-23610\664d12e3-5073-4230-9821-1345e8f6f417.jpg" /></p><p>Proof. Let</p><disp-formula id="scirp.25435-formula79441"><label>(6)</label><graphic position="anchor" xlink:href="3-23610\b06c6cd1-00ef-4f65-bba5-f0e504b68152.jpg"  xlink:type="simple"/></disp-formula><p>It follows that system (4) can be rewrote as</p><disp-formula id="scirp.25435-formula79442"><label>(7)</label><graphic position="anchor" xlink:href="3-23610\2a25dddc-363c-4993-805c-1885e70cbac6.jpg"  xlink:type="simple"/></disp-formula><p>for<img src="3-23610\d53e9a24-2620-4a1a-9c28-348b28816793.jpg" />.</p><p>Initial conditions are given by</p><disp-formula id="scirp.25435-formula79443"><label>(8)</label><graphic position="anchor" xlink:href="3-23610\7c3e8193-7bbe-41e5-90c5-e3eec510543c.jpg"  xlink:type="simple"/></disp-formula><p>Hence system (7) is a special case of system (1) in mathematical form in which there are n+m neurons and connection weights <img src="3-23610\4c29b30e-670d-4773-a89c-d5d2424f4541.jpg" /> for <img src="3-23610\7c6ab11a-db46-452f-bfc7-1216cad9a936.jpg" /> and<img src="3-23610\3e5814bd-153c-4615-8513-557741d1bc2b.jpg" />. Under conditions (H<sub>6</sub>)-(H<sub>10</sub>), from Lemma 1, we obtain that system (7) has a T-periodic solution which is globally exponentially stable, if the following matrix <img src="3-23610\a0be0fab-23b5-4ccd-9172-6e5e0d2112d6.jpg" /> is a M-matrix, and</p><disp-formula id="scirp.25435-formula79444"><label>(9)</label><graphic position="anchor" xlink:href="3-23610\35b48366-14e3-4079-bf81-fac131839abf.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="3-23610\fd2ddcf1-b46c-446e-8d5e-6f2abadb2adf.jpg" /></p><p><img src="3-23610\037bb95c-8661-4f86-97bd-1bb1ef269285.jpg" /></p><p>in which <img src="3-23610\484cee18-1ece-41ff-82ca-1348da042281.jpg" /></p><p>Then, we know from (6) and (9) that Theorem 1 holds.</p></sec><sec id="s4"><title>4. An Example</title><p>Consider the following CGBAMNNs with time delays:</p><disp-formula id="scirp.25435-formula79445"><label>(10)</label><graphic position="anchor" xlink:href="3-23610\79aa7d4d-bf17-464e-8c7e-224a52631df6.jpg"  xlink:type="simple"/></disp-formula><p>It is easy to verify system (10) satisfies (H<sub>6</sub>)-(H<sub>9</sub>). In addition, system (10) satisfies (H<sub>10</sub>) because</p><p><img src="3-23610\646c6e07-7d0c-4eac-a714-e25971bd6521.jpg" /></p><p>is a nonsingular M-matrix. According to Theorem 1, system (10) has a 2-periodic solution which is globally exponentially stable. <xref ref-type="fig" rid="fig1">Figure 1</xref> shows the dynamic behaveiors of system (10) with initial conditions (0.8, 0.9).</p><p>Remark 1 The results in [3,15] have more restrictions than the results in this paper because conditions for the results in [3,15] are relevant to amplification functions. 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