<?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.2013.411A1006</article-id><article-id pub-id-type="publisher-id">AM-40118</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>
 
 
  Stabilization of Functional System with Markovian Switching
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>izhu</surname><given-names>Feng</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>Qiong</surname><given-names>Cai</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Mathematics and Computer Science, Jianghan University, Wuhan, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>fengliahu11@163.com(IF)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>16</day><month>10</month><year>2013</year></pub-date><volume>04</volume><issue>11</issue><fpage>37</fpage><lpage>43</lpage><history><date date-type="received"><day>October</day>	<month>14,</month>	<year>2013</year></date><date date-type="rev-recd"><day>November</day>	<month>14,</month>	<year>2013</year>	</date><date date-type="accepted"><day>November</day>	<month>21,</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>
 
 
   There are many papers related to stability, some on suppression or on stabilization are one type of them. Functional differential systems are common and important in practice. They are special situations of neutral differential systems and generalization of ordinary differential systems. We discussed conditions on suppression on functional system with Markovian switching in our previous work: “Suppression of Functional System with Markovian Switching”. Based on it, by slightly modifying and adding some conditions, we get this paper. In this paper, we will study a functional system whose coefficient satisfies the local Lipschitz condition and the one-sided polynomial growth condition under Markovian switching. By introducing two appropriate intensity Brownian noise, we find the potential explosion system stabilized. 
 
</p></abstract><kwd-group><kwd>Stochastic Functional System; Brownian Noise; Markovian Switching; Boundedness; Stabilization</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>There are many papers which discuss stability of systems. It is called a stabilization problem when we impose such conditions on a given unstable system to make it stable. There have been rich literatures on this topic, here we only mention [1-4]. It is talked about suppression of noise in [1,2]. It is showed similar stabilization phenomena in stochastic systems as those in deterministic systems in [3,4]. They all indicate clearly that different structures of environmental noise may have different effects on the deterministic system. On the other hand, there are also many papers related to stabilization of functional systems, such as [5-8]. [<xref ref-type="bibr" rid="scirp.40118-ref5">5</xref>] investigates a stochastic Lotka-Volterra system with infinite delay, whose initial data come from an admissible Banach space C, and show that its unique global positive solution has asymptotic boundedness property by using the exponential martingale inequality. [<xref ref-type="bibr" rid="scirp.40118-ref6">6</xref>] studies existence and uniqueness of the global positive solution of stochastic functional Kolmogorov-type system and its asymptotic bound properties and moment average boundedness in time under the traditionally diagonally dominant condition. [<xref ref-type="bibr" rid="scirp.40118-ref7">7</xref>] studies the same problems as [<xref ref-type="bibr" rid="scirp.40118-ref6">6</xref>] under some other conditions. [<xref ref-type="bibr" rid="scirp.40118-ref8">8</xref>] discusses stabilization of a given unstable nonlinear functional system by introducing two Brownian noise.</p><p>Many practical systems may experience abrupt changes in their structure and parameters caused by phenomena such as component failures or repairs, changing subsystem interconnections, and abrupt environmental disturbances. The hybrid systems have been used to desribe such situations. Along the trajectories of the Markovian jump system, the mode switches from one value to another in a random way are governed by a Markov process with discrete state space. [9,10] studied the stability of a jump system. Feng et al. [<xref ref-type="bibr" rid="scirp.40118-ref11">11</xref>] systematically studied stochastic stability properties of jump linear systems and the relationship among various moment and sample path stability properties. Shen and Wang [<xref ref-type="bibr" rid="scirp.40118-ref12">12</xref>] presented new exponential stability results for recurrent neural networks with Markovian switching. Wang et al. [<xref ref-type="bibr" rid="scirp.40118-ref13">13</xref>] dealt with the problem of state estimation for a class of delayed neural networks with Markovian jumping parameters without the traditional monotonicity and smoothness assumptions on the activation function.</p><p>Taking both the environmental noise and jump into account, the system under consideration becomes a stochastic differential system with Markovian switching (SDSwMS), which has received a lot of attention (see [14-24]) recently. [<xref ref-type="bibr" rid="scirp.40118-ref17">17</xref>] provided some useful conditions on the exponential stability for general nonlinear SDSwMSs, which was improved by himself in Mao et al. [<xref ref-type="bibr" rid="scirp.40118-ref19">19</xref>]. Yuan and Lygeros [<xref ref-type="bibr" rid="scirp.40118-ref20">20</xref>] investigated almost sure exponential stability for a class of switching diffusion processes. [<xref ref-type="bibr" rid="scirp.40118-ref25">25</xref>] discusses the asymptotic stability and exponential stability of SDSwMSs, whose coefficients are assumed to satisfy the local Lipschitz condition and the polynomial growth condition.</p><p>Motivated by [25,26] and some other literatures, we will investigate suppression and stabilization by noise of functional differential system with Markov chains, whose coefficient satisfies the local Lipschitz condition and the one-sided polynomial growth condition. For a given unstable functional system with Markovian switching</p><disp-formula id="scirp.40118-formula125416"><label>(1)</label><graphic position="anchor" xlink:href="6-7401907\8e3fe029-ff20-423a-b7a6-d3cda77571fc.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="6-7401907\63e91da3-a90c-41bc-8a24-d23f47f5d06b.jpg" /></p><p><img src="6-7401907\2256f173-d820-4f7c-9d84-90ad209c797e.jpg" /></p><p><img src="6-7401907\4e8a63b1-0ada-4a33-880c-cd1b0479973a.jpg" />is defined by<img src="6-7401907\c2deae7a-6eec-4dfe-a082-e561858cd3a9.jpg" />, by introducing two independent scalar Brownian noise under some conditions, we get a stochastic functional system which admits a unique global positive solution. Furthermore, choosing appropriate intensity noise, we can get an exponential stable stochastic functional system</p><disp-formula id="scirp.40118-formula125417"><label>(2)</label><graphic position="anchor" xlink:href="6-7401907\844d0b42-b212-444e-a2e3-10bc84573423.jpg"  xlink:type="simple"/></disp-formula><p>on<img src="6-7401907\3e4af0c9-5ffe-4796-8a4e-528ed9665470.jpg" />, where <img src="6-7401907\aa1ddf62-0175-432f-b526-cea7da634e40.jpg" /> is a scalar Brownian motion, and</p><p><img src="6-7401907\9c6890de-1720-4184-9778-14daa9f853fd.jpg" /></p><p><img src="6-7401907\9840e453-df88-4d5a-832e-b400ee6bcbe1.jpg" /></p><p><img src="6-7401907\51f290c0-ad61-419a-aa35-83abae5e5455.jpg" /></p><p>In the next section we will give some necessary notations and lemmas. In Section 3, we will give the main results of this paper.</p></sec><sec id="s2"><title>2. Preliminaries</title><p>Throughout this paper, unless otherwise specified, let <img src="6-7401907\14dc29c6-83e3-43f0-825c-fcd9a4b634f8.jpg" /> be the Euclidean norm in<img src="6-7401907\70acf6ec-aa1e-466e-8a18-5af68401cfc6.jpg" />. If <img src="6-7401907\3ea56d3e-8e4b-473e-91df-2daefe7acc67.jpg" /> is a vector or matrix, its transpose is denoted by<img src="6-7401907\d121e2a7-a93a-480d-a0fe-fd1e3a5d8cb5.jpg" />. If <img src="6-7401907\38d2e1b9-4902-45d6-924a-a75a9a269054.jpg" /> is a matrixits trace norm is denoted by<img src="6-7401907\902b3f72-d088-4cd9-a302-5d24ad541f3d.jpg" />. Denote the inner product of <img src="6-7401907\f97d334d-b873-4414-89ac-467f798df28b.jpg" /> by <img src="6-7401907\512cc7a0-7af3-48db-b813-a27e5676ddd2.jpg" /> or<img src="6-7401907\18979f0d-be42-4c3b-afdb-56694774df00.jpg" />. Let <img src="6-7401907\7434adb6-b890-4533-a906-44539e5f841a.jpg" /> be positive integers. Let <img src="6-7401907\3c1dd369-2969-467d-a366-e56ccc22662f.jpg" /> denote the maximum of <img src="6-7401907\085f05e3-ad3f-4d18-b99f-dfb4e0da2d0d.jpg" /> and<img src="6-7401907\22b35425-617f-4a57-903f-e2111ddb8d47.jpg" />, while <img src="6-7401907\c561736d-4835-4a00-a2c4-4b65a7dc7e8e.jpg" /> the minimum of <img src="6-7401907\80c42da1-e253-4067-8766-a9b314da7308.jpg" /> and<img src="6-7401907\f37e41fb-424b-4bf1-a872-88d0dc223419.jpg" />. Let <img src="6-7401907\86833397-3ce4-4904-a2d9-97d70332fbfb.jpg" /> <img src="6-7401907\dbc5ced4-342c-4abf-a3e8-225b15d83c90.jpg" />. Denote by <img src="6-7401907\50f26d0e-8a32-4c04-897a-0c926a231021.jpg" />the family of continuous functions from <img src="6-7401907\a9211688-8bcd-4af2-8f60-7008daf0d90d.jpg" /> to R<sup>n</sup> with the norm<img src="6-7401907\b3e76555-82fc-4c17-a7ef-54452981887b.jpg" />which forms a Banach space. Let <img src="6-7401907\b7e4dd78-17ff-424d-841a-6c950ea857bd.jpg" /> and<img src="6-7401907\6e0e1c86-4200-4747-bdb0-98ea3359fc84.jpg" />. Let <img src="6-7401907\c51e72e3-d24f-4829-83bb-f78f3215cff9.jpg" /> denote the family of functions <img src="6-7401907\66fa2501-c107-47ae-992f-8cfcab177bdf.jpg" /> on <img src="6-7401907\8a16b55f-b887-4640-a994-88d56ce00f58.jpg" /> which are continuously twice differentiable in <img src="6-7401907\9da2fb28-74e7-427d-b79b-0beb0a4da381.jpg" /> and once in<img src="6-7401907\99bd72ba-1ab6-4a50-a108-7b5b2f1378a8.jpg" />.</p><p>Let <img src="6-7401907\d3f1aa5d-10ac-41d7-8d3a-9ef2b2b196d2.jpg" /> be a complete probability space with a filtration <img src="6-7401907\d8ba5bea-75e0-4a46-b85c-6bb4a9bc9c48.jpg" /> satisfying the usual conditions (i.e. it is increasing and right continuous while <img src="6-7401907\080ad2a5-8e2c-4391-9ac4-aeaebfdf6f8d.jpg" /> contains all <img src="6-7401907\69323400-9e48-4d35-9004-e58de5a71423.jpg" />-null sets). Let <img src="6-7401907\9fac2050-8bbb-4df2-9659-630ab2aa1a6c.jpg" /> denote the family of <img src="6-7401907\01c64f01-29db-4f4b-b44f-9a8959d60758.jpg" />-valued <img src="6-7401907\aec34707-2236-47a2-8d33-6b2767cdd14c.jpg" />-measurable random variables <img src="6-7401907\6c8957fe-1a3d-4c1b-96fa-6727848dc1bb.jpg" /> with<img src="6-7401907\3a8f9ea4-5571-454f-9a95-da92f4f132d4.jpg" />. Denote the family of R<sup>n</sup>-valued bounded <img src="6-7401907\3515d55e-a941-479d-9fb4-99116a7ee74f.jpg" />-measurable random variables by<img src="6-7401907\54ca08c2-1ee0-4df4-b990-8a5d5e155b35.jpg" />. If <img src="6-7401907\9b54d38a-03d5-431c-a699-098e1a473972.jpg" /> is an R<sup>n</sup>-valued process on<img src="6-7401907\92ab3957-2f0b-4a9d-a16c-5d6bc6e6068d.jpg" />, let</p><p><img src="6-7401907\08bfd76d-3c6f-4415-b5b0-f9b1c506fcb8.jpg" />.</p><p>If <img src="6-7401907\1088c64e-38d5-4683-83fe-dc0b169045c9.jpg" /> is a continuous local martingale, denote the quadratic variation of <img src="6-7401907\0c9747d7-e534-4396-b395-68596d615ee5.jpg" /> by<img src="6-7401907\b7a4335f-0929-446c-ba14-2b928ae8b3a8.jpg" />. Let</p><p><img src="6-7401907\f9395a03-aaf7-49cf-a2a1-140f665a4549.jpg" /></p><p>be independent scalar Brownian motion defined on the probability space. Let <img src="6-7401907\101f1dee-a2bd-419d-88fc-38c0c2ca1243.jpg" /> be a right-continuous Markov chain on the probability space taking values in a definite state space <img src="6-7401907\883c9f28-4065-4c69-82b1-74c8d1be1bb0.jpg" /> with the generator <img src="6-7401907\9dff827f-d72e-44da-b9ee-3a11079384ff.jpg" /> given by</p><p><img src="6-7401907\07eed1a2-f66b-4cec-8f0f-35114b980498.jpg" /></p><p>where <img src="6-7401907\20013344-c92d-4047-a148-e77ed167383b.jpg" /> <img src="6-7401907\6e6563db-5930-4e6e-bd70-f71fcf67541f.jpg" /> is the transition rate from <img src="6-7401907\0c2057ec-ebd4-4e6e-8b72-e63f8b5a5f56.jpg" /> to <img src="6-7401907\21aed3c6-a1f1-4afd-b162-835b53d8a20f.jpg" /> and <img src="6-7401907\cd38ae9e-cbe3-4627-81df-182efe72e146.jpg" /> if <img src="6-7401907\1153032f-bd08-4ec5-a765-d952c819e768.jpg" /> while<img src="6-7401907\97030430-87a6-4ec3-b6e7-b741bd48e485.jpg" />. We assume that the Markov chain <img src="6-7401907\4b173f15-8ed1-40fe-ab14-a69d07802e8d.jpg" /> is independent of the Brownian motion<img src="6-7401907\cabe51f3-4e4b-4778-bad3-b340565fb7b9.jpg" />. For any initial value <img src="6-7401907\36f184ba-1936-4f2b-9a92-d424ae4986eb.jpg" />denote the solution of the corresponding initial value problem by <img src="6-7401907\b920c0c6-ae3a-4025-96c6-b276b6b54a16.jpg" /> or simply <img src="6-7401907\e645f46e-5724-433c-a721-fc22c9586967.jpg" /> on<img src="6-7401907\90791566-e814-4e6b-b34d-0b768d1b5119.jpg" />.</p><p>In order to obtain the main results, we need the following assumptions.</p><p>(H<sub>1</sub>) There are some nonnegative constants <img src="6-7401907\170213c0-19d4-4d8e-be2b-532575e8468f.jpg" /> such that</p><disp-formula id="scirp.40118-formula125418"><label>(3)</label><graphic position="anchor" xlink:href="6-7401907\66188c84-701d-44e5-9d9a-1d11dfb07cde.jpg"  xlink:type="simple"/></disp-formula><p>for all<img src="6-7401907\6aaba37c-1bbe-4180-a4e6-fd481f225c12.jpg" />, where <img src="6-7401907\8fb1e2a9-4877-4b80-9958-4cc1f85019c3.jpg" /> is a probability measure on <img src="6-7401907\4b07a837-919e-4042-a4e1-cacd5bbeb41f.jpg" /> and <img src="6-7401907\9a6de463-4e37-4709-97c8-9dd5578897c0.jpg" /> means some functions satisfying<img src="6-7401907\f47caf5f-f334-472a-ba03-eccf0ee0ae92.jpg" />.</p><p>(H<sub>2</sub>) For every integer<img src="6-7401907\7c10d608-746c-4f13-9795-a35255b3d092.jpg" />, there is a <img src="6-7401907\89e95e16-48d5-4622-96d8-962d6a9321da.jpg" /> such that</p><disp-formula id="scirp.40118-formula125419"><label>(4)</label><graphic position="anchor" xlink:href="6-7401907\dda5bf40-f88b-4f0c-9280-f01358ac1f19.jpg"  xlink:type="simple"/></disp-formula><p>for all <img src="6-7401907\33df4a0a-3a78-4158-a164-e23b40e22b02.jpg" /> with<img src="6-7401907\31363593-3b03-4a8d-a765-35002ee7c921.jpg" />.</p><p>(H<sub>3</sub>) There are some nonnegative constants <img src="6-7401907\fd69476b-ae9d-490b-821e-78fae70e6d0b.jpg" /> <img src="6-7401907\61016759-4d06-479a-9635-f0b944811da3.jpg" /> and probability measure <img src="6-7401907\771cdabb-15aa-440b-99ae-af2de66e2a26.jpg" /> such that for any <img src="6-7401907\82dbb42e-bdfd-4a06-a8b7-e39c473fa0e3.jpg" /> satisfying<img src="6-7401907\435a5e68-79c6-4bce-9240-a3209042bd52.jpg" />,</p><disp-formula id="scirp.40118-formula125420"><label>(5)</label><graphic position="anchor" xlink:href="6-7401907\a2e699c8-2c79-4981-b7eb-83791a45a8f1.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40118-formula125421"><label>(6)</label><graphic position="anchor" xlink:href="6-7401907\299e35e5-e5a0-4f75-8c69-3a5b9787896a.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40118-formula125422"><label>(7)</label><graphic position="anchor" xlink:href="6-7401907\32f6f672-010b-4852-8e30-504d73e2afa0.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40118-formula125423"><label>. (8)</label><graphic position="anchor" xlink:href="6-7401907\f1853d18-1168-444f-8bad-a627f295d1f7.jpg"  xlink:type="simple"/></disp-formula><p>Definition 1: The irreducibility of the Markov chain means that the Markov chain has a unique stationary (probability) distribution <img src="6-7401907\d108300a-05ff-4185-b2b1-9aceb744fc2e.jpg" /> which can be determined by solving the following linear equation</p><disp-formula id="scirp.40118-formula125424"><label>(9)</label><graphic position="anchor" xlink:href="6-7401907\3e92ec04-cc21-48c7-9fa0-8ad7eed2bc1d.jpg"  xlink:type="simple"/></disp-formula><p>subject to</p><disp-formula id="scirp.40118-formula125425"><label>(10)</label><graphic position="anchor" xlink:href="6-7401907\70adb863-01f2-4935-9bcc-e71c1ef60aa8.jpg"  xlink:type="simple"/></disp-formula><p>Lemma 1: [<xref ref-type="bibr" rid="scirp.40118-ref27">27</xref>] Let (H<sub>2</sub>) hold, for any initial value<img src="6-7401907\411c0733-917b-4b13-97b9-09ccf9c33e80.jpg" />, system (2) has a unique maximal local strong solution on<img src="6-7401907\d6f402e3-c0b1-476a-ad5e-164e8dd4d92c.jpg" />, where <img src="6-7401907\59eac1fe-3aa0-43e5-a4bb-00a05c992bb3.jpg" /> is the explosion time.</p></sec><sec id="s3"><title>3. Main Results</title><p>Similar to the proof of Theorem 1 in [<xref ref-type="bibr" rid="scirp.40118-ref28">28</xref>], we slightly modify the condition on the coefficient of (1) and obtain the following theorem.</p><p>Theorem 1: Let (H<sub>1</sub>) - (H<sub>3</sub>) hold, for any initial value<img src="6-7401907\dd191ab9-6247-4493-870f-f9517ec84ff9.jpg" />, if <img src="6-7401907\dcbf7abd-aeb6-40da-b2c2-a2789ac746a5.jpg" />and<img src="6-7401907\ee8155f1-bfc0-4709-9600-b0f7e2162529.jpg" />then there exists a unique global solution <img src="6-7401907\bb738479-7005-4b7b-815a-a847d2398214.jpg" /> of system (2) on all <img src="6-7401907\cf8bb1e3-4619-4ed5-9c76-728fe443129e.jpg" /> a.s.</p><p>Similarly to that in [<xref ref-type="bibr" rid="scirp.40118-ref28">28</xref>], we define the stopping time</p><disp-formula id="scirp.40118-formula125426"><label>(11)</label><graphic position="anchor" xlink:href="6-7401907\7802b234-625b-4bb5-933e-a5a4b599c969.jpg"  xlink:type="simple"/></disp-formula><p>and a C<sup>2</sup>-function<img src="6-7401907\08759a07-df70-49be-b835-e790c3e0bd02.jpg" />, for any<img src="6-7401907\4e722ab4-3440-4973-80bf-6296f227f860.jpg" />.</p><p>Using the It&#244; formula and the Young inequality, for any<img src="6-7401907\24e7eb1f-2802-440d-bdec-e81ea5128aeb.jpg" />, by (H<sub>1</sub>) and (H<sub>3</sub>), we get</p><disp-formula id="scirp.40118-formula125427"><label>(12)</label><graphic position="anchor" xlink:href="6-7401907\9de3c93b-9923-4942-ba6e-8e2da2eaba65.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.40118-formula125428"><label>(13)</label><graphic position="anchor" xlink:href="6-7401907\98413ee1-3fbc-4d76-98a2-a7bf3666fc07.jpg"  xlink:type="simple"/></disp-formula><p>These results will be used in the following.</p><sec id="s3_1"><title>3.1. Boundedness</title><p>Theorem 2: Let (H<sub>1</sub>) - (H<sub>3</sub>) hold, for any initial value <img src="6-7401907\70bb1e9d-fc6c-4731-9b4f-7a40f44dd1ce.jpg" /> and<img src="6-7401907\b2ee2cf6-c1a0-4d96-8483-aca7f98d1c14.jpg" />, if <img src="6-7401907\83e29558-841a-435b-95ae-8652c7abe7ae.jpg" /> and<img src="6-7401907\1609f5d9-ff9f-4e2c-af59-9403a5045746.jpg" />, then there exists a constant <img src="6-7401907\9a5df001-5a5a-44d6-9e15-f9ecb682dc18.jpg" /> such that the global solution <img src="6-7401907\81157d39-dab5-4e1c-9167-704b6831c7fe.jpg" /> of system (2) has the property that</p><disp-formula id="scirp.40118-formula125429"><label>(14)</label><graphic position="anchor" xlink:href="6-7401907\dbe39ced-9f30-4dd3-ad4a-d14d84290905.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401907\27d64b21-6f3d-4bf9-9d3c-2c4eec23e4bd.jpg" /> is dependent on <img src="6-7401907\dddcfee1-598c-4e5f-9ec3-43192c25338f.jpg" /> and independent of the initial value<img src="6-7401907\0cfb9f82-72a5-421e-9eec-7350a5786026.jpg" />, that is, <img src="6-7401907\e1a157a8-7030-45f2-88cd-8b462fd365cd.jpg" />is bounded in moment.</p><p>Proof: For any<img src="6-7401907\411103d8-e532-4329-8e9c-77374c3830af.jpg" />, applying the It&#244; formula to <img src="6-7401907\c6249c56-87c0-4d91-b515-80fd93d39b9b.jpg" /> yields</p><p><img src="6-7401907\c8d537ca-809d-4e48-bc34-b7678b7f4b86.jpg" /></p><p>By (12) and (13), we have</p><p><img src="6-7401907\96ac4ace-89c8-48e6-bc6c-7f29e478ca4e.jpg" /></p><p>By the boundedness of polynomial functions, there exists a constant <img src="6-7401907\b89c13dc-1df3-44d3-bd2a-b006d832b57e.jpg" /> such that <img src="6-7401907\13539f6f-6da4-4891-93d3-a68817474baf.jpg" />which implies</p><p><img src="6-7401907\66b200ef-2687-453d-9253-a93167ee6f5e.jpg" /></p><p>Then</p><p><img src="6-7401907\d08283ed-9e45-4c99-a1d3-06a2c076a8e7.jpg" /></p><p>That is, the global solution <img src="6-7401907\ed81ddb6-430f-435f-993e-2ecfcc241ac2.jpg" /> of system (2) is bounded in <img src="6-7401907\4b4730d6-7a8f-4cf6-aea8-a7f760356526.jpg" />-th moment for any<img src="6-7401907\8b065c76-98e7-4eb6-bc4f-ad300168b79a.jpg" />.</p><p>Theorem 3: Let (H<sub>1</sub>) - (H<sub>3</sub>) hold, if</p><p><img src="6-7401907\51b0e00e-d25f-4a38-9230-7631b31830b1.jpg" />and<img src="6-7401907\f9de4f42-b795-4e22-899f-79dbff355f09.jpg" /></p><p>then for any initial value <img src="6-7401907\6b8eb127-3c83-4796-abaa-f6cfde110f67.jpg" /> and<img src="6-7401907\44113204-8d01-4b4d-8d2d-21b7e4923a02.jpg" />, the solution <img src="6-7401907\499f7f92-a0a3-4383-97a4-50e34710d1b8.jpg" /> of system (2) has the property that</p><disp-formula id="scirp.40118-formula125430"><label>(15)</label><graphic position="anchor" xlink:href="6-7401907\293e3875-72a9-4d49-a2ae-b61818fc7fb4.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="6-7401907\1c687703-07e1-4534-a7c9-5f8321cf0bb8.jpg" /></p><disp-formula id="scirp.40118-formula125431"><label>(16)</label><graphic position="anchor" xlink:href="6-7401907\53b12045-b282-45c5-8d18-cef7e5fc9671.jpg"  xlink:type="simple"/></disp-formula><p>Proof: By Theorem 1, there a.s. exists a unique global solution <img src="6-7401907\32d73cc6-0402-4445-9d9d-cb6b4449b0c0.jpg" /> to system (2) on <img src="6-7401907\6a2cd649-5018-4f3a-947e-70358ff6db25.jpg" /> a.s. Let<img src="6-7401907\8a434c44-4cd8-45ed-a88d-d1b433de81dc.jpg" />, by the It&#244; formula, we have</p><p><img src="6-7401907\5a486e99-39d8-449f-bbc3-c32eb54cb09f.jpg" /></p><p>where</p><p><img src="6-7401907\5a4d5606-437f-49c2-9e83-b3f3b987c06d.jpg" /></p><p>By (H<sub>1</sub>) and (H<sub>3</sub>), we have</p><p><img src="6-7401907\1b2035e9-f958-4e15-a3c0-f1d1e9c5f764.jpg" /></p><p>Let <img src="6-7401907\d88b4855-b3c7-4db5-8dc7-253dc24260b3.jpg" /> be the same stopping time as defined in the proof of Theorem 1. By (13) and (14), we have</p><p><img src="6-7401907\cef09e58-d5cf-4b39-9d78-e0922437310a.jpg" /></p><p>Then as<img src="6-7401907\47788969-cc3c-4f63-9513-e9a6380d08f7.jpg" />, we have</p><p><img src="6-7401907\8b268d7b-a4cc-4d4b-904d-a0440778e917.jpg" /></p><p>That is,</p><disp-formula id="scirp.40118-formula125432"><label>(17)</label><graphic position="anchor" xlink:href="6-7401907\864f5c47-807f-4676-818d-fbfae1c41791.jpg"  xlink:type="simple"/></disp-formula><p>By the ergodic and irreducibility property of the Markov chain, we have</p><p><img src="6-7401907\8594d6a9-037d-449f-8968-0b4ea5de601e.jpg" /></p><p>Hence,</p><p><img src="6-7401907\d3afef38-d090-4f55-8d60-13e37c8df079.jpg" /></p><p>as required.</p></sec><sec id="s3_2"><title>3.2. Stabilization of Noise</title><p>The following lemma can be obtained by slightly modifying the proof of Mao [<xref ref-type="bibr" rid="scirp.40118-ref2">2</xref>].</p><p>Lemma 2: Let (H<sub>1</sub>) - (H<sub>3</sub>) hold, for any initial value <img src="6-7401907\3c0cea0d-bf63-41a7-8f5a-1f2957ada5d7.jpg" /> with<img src="6-7401907\cb9ec5af-7d01-4929-96aa-20b7eec23a06.jpg" />, the global solution of system (2) has the property that</p><disp-formula id="scirp.40118-formula125433"><label>(18)</label><graphic position="anchor" xlink:href="6-7401907\a17c88ad-a085-4ea5-9eed-4d7ba78ff4be.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401907\50f10891-69e7-4289-ba69-378418578230.jpg" /> is the explosion time.</p><p>Theorem 4: Let (H<sub>1</sub>) - (H<sub>3</sub>) hold, assume that</p><p><img src="6-7401907\3bf3bd4c-5031-41df-8dfc-aab78c692ed7.jpg" />and<img src="6-7401907\e5c86a43-753a-4db2-8b88-55d81a0487f6.jpg" />.</p><p>If</p><disp-formula id="scirp.40118-formula125434"><label>(19)</label><graphic position="anchor" xlink:href="6-7401907\7fd8d7d7-8317-4a06-b0ee-7f42975caac1.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.40118-formula125435"><label>(20)</label><graphic position="anchor" xlink:href="6-7401907\843a046c-e776-4742-acb5-426a3b6c5aed.jpg"  xlink:type="simple"/></disp-formula><p>then for any initial value<img src="6-7401907\923eca73-789d-4899-8122-a65026b80b7b.jpg" />, satisfying<img src="6-7401907\c7e4779f-7f65-4ffc-9412-0aeb67c7d0a5.jpg" />, the global solution of system (2) has the property that</p><disp-formula id="scirp.40118-formula125436"><label>(21)</label><graphic position="anchor" xlink:href="6-7401907\92035c5b-3c28-41ff-8846-a1e7be21c8bd.jpg"  xlink:type="simple"/></disp-formula><p>That is, the solution to system (2) is a.s. exponentially stable.</p><p>Proof: By Lemma 2 and Theorem 1, <img src="6-7401907\bf353922-fd02-4ec0-a9e3-172aaa7c61c1.jpg" /> a.s. Thus, applying the It&#244; formula to <img src="6-7401907\5bf8ac3b-8a9d-410a-b2a4-b3555b89bf4e.jpg" /> yields</p><p><img src="6-7401907\032aa77a-28fe-47f2-9a66-30f74c113aa4.jpg" /></p><p>where <img src="6-7401907\8dbb6915-c87e-47eb-abf3-c05506c0d147.jpg" /> is an identity matrix and</p><p><img src="6-7401907\27880232-de1c-4366-ba48-dc803bf53358.jpg" /></p><p>Clearly <img src="6-7401907\e21c2333-fcc3-4b24-90d4-5cfb87d8f4f7.jpg" /> and <img src="6-7401907\5db4f5a6-c262-41b8-802f-7296896a4fd3.jpg" /> are continuous local martingales with the quadratic variation</p><p><img src="6-7401907\1415133b-c1d5-43bc-b7e2-f0aee842d6fc.jpg" /></p><p>By (H<sub>3</sub>),</p><p><img src="6-7401907\73e10e48-06fd-4140-a2b7-514739ee4ea0.jpg" /></p><p>Applying the strong law of large number,</p><p><img src="6-7401907\a87aaf79-2281-4b61-81ec-c20f56e450fa.jpg" /></p><p>For any <img src="6-7401907\ef317a26-3dd9-4e70-a759-184c46432f8d.jpg" /> and each integer<img src="6-7401907\c4d900f9-9056-443d-a0a9-7c55815ec211.jpg" />, by the exponential martingale inequality,</p><p><img src="6-7401907\4564f4f9-e765-4ddc-ad90-1cfef9085619.jpg" /></p><p>Since<img src="6-7401907\375dd322-67d7-4381-95ca-75497bdf7741.jpg" />, by the Borel-Cantelli lemma, there exists an <img src="6-7401907\5711ca3c-fbb1-42c0-b1ff-6369b538b5f9.jpg" /> with <img src="6-7401907\2ff91b32-d85c-429e-b9d5-0794bb51f85f.jpg" /> such that for any<img src="6-7401907\8d1cd9b9-e385-426a-aea3-38bbad3a6c7d.jpg" />, when<img src="6-7401907\4cf4e8c8-533a-44fe-acee-b3dff711b108.jpg" />,</p><p><img src="6-7401907\a81b1db1-7a48-4675-971f-b8ebabcd2b82.jpg" /></p><p>From (H<sub>1</sub>) and (H<sub>3</sub>),</p><p><img src="6-7401907\2c6a77bf-585b-4639-a015-1a9534213b1e.jpg" /></p><p>where</p><p><img src="6-7401907\2b714d2a-28b9-49ba-98fe-14a9fa10c428.jpg" /></p><p>By the definition of <img src="6-7401907\50fa91c1-a97d-4f6c-9d8f-038553b374e4.jpg" /> in (20),</p><p><img src="6-7401907\f4c7d750-e6c6-455a-84ef-48f84fb4428a.jpg" /></p><p>Applying the strong law of large number to the Brownian motion,</p><p><img src="6-7401907\bd846da7-c4ff-47b9-9d41-f78c49a2f683.jpg" /></p><p>which implies</p><p><img src="6-7401907\d16e3593-2f50-403a-a9d6-b7f334a44c58.jpg" /></p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper, we study a stochastic functional system with Markovian switching. Motivated by [25,26] and other literatures, we introduce two appropriate intensity Brownian noise to perturb the system so as to suppress its potential explosion and stabilize it. Based on [<xref ref-type="bibr" rid="scirp.40118-ref28">28</xref>], we just slightly modify some conditions on its coefficients and add some contents, then we get some new conclusions about boundedness and stabilization of the system.</p></sec><sec id="s5"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.40118-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">X. Mao, G. Marion and E. 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