Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2012, Article ID 414320, 14 pages doi:10.1155/2012/414320 Research Article Mean Square Almost Periodic Solutions for Impulsive Stochastic Differential Equations with Delays Ruojun Zhang,1 Nan Ding,2, 3 and Linshan Wang1 1 School of Mathematical Sciences, Ocean University of China, Qingdao 266100, China College of Information Engineering, Ocean University of China, Qingdao 266100, China 3 Department of Mathematics, Chongqing Three Gorges University, Chongqing 404100, China 2 Correspondence should be addressed to Ruojun Zhang, zhangru1626@sina.com Received 28 December 2011; Revised 15 March 2012; Accepted 15 March 2012 Academic Editor: Zhiwei Gao Copyright q 2012 Ruojun Zhang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. We establish a result on existence and uniqueness on mean square almost periodic solutions for a class of impulsive stochastic differential equations with delays, which extends some earlier works reported in the literature. 1. Introduction Impulsive effects widely exist in many evolution processes of real-life phenomena in which states are changed abruptly at certain moments of time, involving such areas as population dynamics and automatic control 1–3. Because delay is ubiquitous in the dynamical system, impulsive differential equations with delays have received much interesting in recent years, intensively researched, some important results are obtained 4–9. And almost periodic solutions for abstract impulsive differential equations and for impulsive neural networks with delay have been discussed by G. T. Stamov and I. M. Stamova 10, and Stamov and Alzabut 11. However, besides delay and impulsive effects, stochastic effects likewise exist in real system. A lot of dynamic systems have variable structures subject to stochastic abrupt changes, which may result from abrupt phenomena such as stochastic failures and repairs of components, changes in the interconnections of subsystems, sudden environment changes, and so on 12–14. Moreover, differential descriptor systems also have abrupt changes 15, 16. Recently, a large number of stability criteria of stochastic system with delays have 2 Journal of Applied Mathematics been reported 17–19. Almost periodic solutions to some functional integro-differential stochastic evolution equations and to some stochastic differential equations have been studied by Bezandry and Diagana 20, and Bezandry 21. Huang and Yang investigated almost periodic solution for stochastic cellular neural networks with delays 22. Because it is not easy to deal with the case of coexistence of impulsive, delay and stochastic effects in a dynamical system, there are few results about this problems 23–25. To the best of our knowledge, there exists no result on the existence and uniqueness of mean square almost periodic solutions for impulsive stochastic differential equations with delays. Motivated by the above discussions, the main aim of this paper is to study the mean square almost periodic solutions for impulsive stochastic differential equations with delays. By employing stochastic analysis, delay differential inequality technique and fixed points theorem, we obtain some criteria to ensure the existence and uniqueness of mean square almost periodic solutions. The rest of this paper is organized as follows: in Section 2, we introduce a class of impulsive stochastic differential equations with delays, and the relating notations, definitions and lemmas which would be used later; in Section 3, a new sufficient condition is proposed to ensure the existence and uniqueness of mean square almost periodic solutions; in Section 4, an example is constructed to show the effectiveness of our results. Finally, a conclusion is given in Section 5. 2. Preliminaries Let R −∞, ∞, N {1, 2, 3, . . .}, and B {{tk } : t0 0 < t1 < t2 < · · · < tk < tk1 < · · · , limk → ∞ tk ∞} be the set of all sequence unbounded and strictly increasing. For x ∈ Rn and A ∈ Rn×n , let x be any vector norm, and denote the induced matrix norm and the matrix measure, respectively, by Ax , x/ 0 x A sup μA lim h→0 I hA − 1 . h 2.1 The norm and measure of vector and matrix are x maxi |xi |, A maxi nj1 |aij |, μA maxi {aii nj/ i |aij |}. Consider the following a class of Itô impulsive stochastic differential equations with delay dxt Axt Bft, xt Cgt, xt − h It dt σt, xtdωt, t ≥ 0, t / tk , − − − Δxt xtk − x tk Dk x tk Vk x tk βk , t tk , k ∈ N, xt φt, −h ≤ t ≤ 0, 2.2 where xt x1 t, . . . , xn tT is the solution process, A, B, C, Dk ∈ Rn×n are constant matrices, ft, x f1 t, x, . . . , fn t, xT , gt, x g1 t, x, . . . , gn t, xT , It I1 t, . . . , In tT , σt, x σij t, xn×n is the diffusion coefficient matrix, Vk x V1k x, . . . , Vnk xT is impulsive function, h > 0 is delay; tk ∈ B is impulsive time, βk β1k , . . . , βnk T is a constant vector, ωt ω1 t, . . . , ωn tT is an n-dimensional Brown motion defined on a complete Journal of Applied Mathematics 3 probability space Ω, F, P with a natural filtration {Ft }t≥0 generated by ωt, and denote by F the associated σ-algebra generated by ωt with the probability measure P. Moreover, Δ the initial conditions φt φ1 t, . . . , φn tT ∈ P CBFb 0 −h, 0, Rn P CBFb 0 . Denote by P CBFb 0 the family of all bounded F0 -measurable, P C−h, 0, Rn -valued random variable ζ, satisfying Eζ2 Esup−h≤θ≤0 ζθ2 < ∞, where P C−h, 0, Rn {ζ : −h, 0 → Rn is continuous}. E denotes the expectation of stochastic process. Let H, · be a Hilbert space and Ω, F, P be a complete probability space. Define L2 P, H to be the space of all H-value random variable Y such that 2 EY Ω Y 2 dP < ∞. 2.3 It is then routine to check that L2 P, H is a Hilbert space when it is equipped with its natural norm · 2 defined by Y 2 Ω 1/2 < ∞, Y 2 dP 2.4 for each Y ∈ L2 P, H. Definition 2.1 see 25. For any φ ∈ P CBFb 0 , a function xt : −h, ∞ → L2 P, H is said to be solution of system 2.2 on −h, ∞ satisfying initial value condition, if the following conditions hold: i xt is absolutely continuous on each interval tk , tk1 ∈ 0, ∞, k ∈ N; ii for any tk ∈ 0, ∞, k ∈ N, xtk and xt−k exist and xtk xtk ; iii xt satisfies 2.2 for almost everywhere in −h, ∞ and at impulsive points t tk situated in 0, ∞, k ∈ N, may have discontinuity points of the first kind. Obviously, the solution defined by definition 1 is piecewise continuous. j j Definition 2.2 see 26. The set of sequences {tk }, tk tkj − tk , k ∈ N, j ∈ N, {tk } ∈ B is said to be uniformly almost periodic if for any ε > 0, there exists relatively dense set of ε-almost periods common for any sequences. Definition 2.3. A piecewise continuous function xt : −h, ∞ → L2 P, H with discontinuity points of first kind at t tk is said to be mean square almost periodic, if j i the set of sequence {tk } is uniformly almost periodic; ii for any ε > 0, there exists δ > 0, such that if the points t and t belong to one and the same interval of continuity of xt and satisfy the inequality |t − t | < δ, then Ext − xt 2 < ε; iii for any ε > 0, there exists a relatively dense set T such that if τ ∈ T , then Ext τ − xt2 < ε for all t ∈ −h, ∞ satisfying the condition |t − tk | > ε, k ∈ N. The collection of all functions xt : −h, ∞ → L2 P, H with discontinuity points of the first kind at t tk which are mean square almost periodic is denoted by 4 Journal of Applied Mathematics AP −h, ∞; L2 P, H, one can check that AP −h, ∞; L2 P, H is a Banach space when it is equipped with the norm: 1/2 . x∞ sup Ext2 2.5 t∈R Let B1 , · 1 and B2 , · 2 be Banach space and L2 P, B1 and L2 P, B2 be their corresponding L2 -space, respectively. Lemma 2.4 see 20. Let f : R × L2 P, B1 → L2 P, B2 , t, x → ft, x be mean square almost periodic in t ∈ R uniformly in x ∈ K, where K ⊂ L2 P, B1 is compact. Suppose that there exists Lf > 0 such that 2 2 Eft, x − ft, y2 ≤ Lf Ex − y1 2.6 for all x, y ∈ L2 P, B1 and for each t ∈ R. Then for any mean square almost periodic function ψt : R → L2 P, B1 , ft, ψt is mean square almost periodic. In this paper, we always assume that: 0 and the sequence {Dk }, k ∈ N, is almost periodic, where I ∈ Rn×n is A1 detI Dk / the identity matrix; j A2 the set of {tk } is uniformly almost periodic and θ infk {t1k } > 0. Recall 2, consider the following linear system of system2.2 ẋt Axt, t / tk , − Δxtk Dk x tk , k ∈ N, 2.7 that if Uk t, s is the Cauchy matrix for the system ẋt Axt, tk−1 ≤ t < tk , 2.8 then the Cauchy matrix for the system 2.7 is in the form ⎧ ⎪ Uk t, s, ⎪ ⎪ ⎪ ⎪ ⎪ ⎨U t, t I D U t , s, k1 k k k k Wt, s ⎪ i1 ⎪ ⎪ ⎪ ⎪ Uk1 t, tk I Dk Uj tj , tj1 I Di Ui ti , s, ⎪ ⎩ tk−1 ≤ s ≤ t < tk , tk−1 ≤ s < tk ≤ t < tk1 , ti−1 ≤ s < ti < tk ≤ t < tk1 . jk 2.9 As the special case of Lemma 1 in 10, we have the following lemma. Journal of Applied Mathematics 5 Lemma 2.5. Assume that (A1), (A2) and the following condition hold. For the Cauchy matrix Wt, s of system 2.7, there exist positive constants M and λ such that Wt, s ≤ Me−λt−s , t ≥ s, t, s ∈ R. 2.10 Then for any ε > 0, t ≥ s, t, s ∈ R, |t − tk | > ε, |s − tk | > ε, k ∈ N, there must be exist a relatively dense set T of ε-almost periodic of the matrix A and a positive constant Γ such that for τ ∈ T , it follows: Wt τ, s τ − Wt, s ≤ εΓe−λ/2t−s . 2.11 Lemma 2.6 see 6. Let Wt, s be the Cauchy matrix of the linear system 2.7. Given a constant η ≥ I Dk for all k ∈ N, if η ≥ 1 and θ infk {t1k } > 0, then Wt, s ≤ ηeμAln η/θt−s , t ≥ s. 2.12 Introduce the following conditions: A3 The functions f, g : R × L2 P, H → L2 P, H are mean square almost periodic in t ∈ R uniformly in x ∈ Θ, where Θ ⊂ L2 P, H is compact, and f0, 0 g0, 0 0. Moreover, there exist Lf , Lg > 0 such that 2 2 Eft, x − ft, y ≤ Lf Ex − y , 2 2 Egt, x − gt, y ≤ Lg Ex − y , 2.13 for all stochastic processes x, y ∈ L2 P, H and t ∈ R. A4 The function σ : R × L2 P, H → L2 P, H is mean square almost periodic in t ∈ R uniformly in x ∈ Θ , where Θ ⊂ L2 P, H is compact, and σ0, 0 0. Moreover, there exists Lσ > 0 such that 2 2 Eσt, x − σ t, y ≤ Lσ Ex − y , 2.14 for all stochastic processes x, y ∈ L2 P, H and t ∈ R. A5 The function Ii t : R → R is almost periodic in the sense of Bohr, {βk }k∈N is almost periodic sequence and there exists a constant γ0 > 0, such that max maxβk , supIt ≤ γ0 . k t 2.15 6 Journal of Applied Mathematics A6 The sequence of functions Vk x : L2 P, H → L2 P, H is mean square almost periodic uniformly with respect to x ∈ Θ , where Θ ⊂ L2 P, H is compact. Moreover, there exists LV > 0 such that 2 2 EVk x − Vk y ≤ LV Ex − y 2.16 for all stochastic processes x, y ∈ L2 P, H. Lemma 2.7 see 26. If conditions (A1)–(A6) are satisfied, then for each ε > 0, there exists ε1 , 0 < ε1 < ε and relatively dense sets T of real numbers and Q of integral numbers, such that i Eft τ, y − ft, y2 < ε, Egt τ, y − gt, y2 < ε, t ∈ R, τ ∈ T , |t − tk | > ε, k ∈ N, y ∈ L2 P, H; ii Eσt τ, y − σt, y2 < ε, t ∈ R, τ ∈ T, |t − tk | > ε, k ∈ N, y ∈ L2 P, H; iii It τ − It2 < ε, t ∈ R, τ ∈ T, |t − tk | > ε; iv EVkq y − Vk y2 < ε, q ∈ Q, k ∈ N; v βkq − βk 2 < ε, q ∈ Q, k ∈ N; vi tkq − τ2 < ε1 , q ∈ Q, τ ∈ T, k ∈ N. Lemma 2.8 see 26. Let condition (A2) holds. Then for each p > 0, there exists a positive integer N such that on each interval of length p, there are no more than N elements of the sequence {tk }, that is, is, t ≤ Nt − s N, 2.17 where is, t is the number of points tk in the interval s, t. 3. Main Results Theorem 3.1. Assume that (A1)–(A6) hold, then there exists a unique mean square almost periodic solution of system 2.2 if the following conditions are satisfied: There exists a constant η ≥ 1, such that I Dk ≤ η, k ∈ N and μA ln η Δ −λ < 0. θ 3.1 Furthermore, ρ 6η 2 L2 2 N2 L2V σ B2 L2f C2 L2g 2 2 2λ λ 1 − e−λ < 1. 3.2 Proof. Let D {ϕt ∈ L2 P, H : ϕt ϕ1 t, . . . , ϕn tT } ⊂ AP −h, ∞; L2 P, H satisfy2 ing the equality Eϕ2 < K, where K 2η2 γ02 1/λ N/1 − e−λ > 0. Journal of Applied Mathematics 7 Set xt Wt, 0φ0 t Wt, s Bfs, xs Cgs, xs − h Is ds 0 Wt, tk Vk xtk βk t 3.3 Wt, sσs, xsdωs, t ≥ 0. 0 0≤tk <t where φ0 x0, it is easy to see that xt given by 3.3 is the solution of system 2.2 according to 2 and Lemma 2.2 in 27. By Lemma 2.6 and the conditions of Theorem, we have Wt, s ≤ ηe−λt−s , t ≥ s, t, s ∈ R. 3.4 For zt ∈ D, we define the operator L in the following way Lzt t 0 Wt, s Bfs, zs Cgs, zs − h Is ds Wt, tk Vk ztk βk t 3.5 Wt, sσs, zsdωs. 0 0≤tk <t Define subset D∗ ⊂ D, D∗ {z ∈ D : Ez − z0 2 ≤ ρK/1 − ρ}, and z0 Isds 0≤tk <t Wt, tk βk . We have 2 2 t Ez0 ≤ 2E Wt, sIsds 2E Wt, tk βk 0 0≤t <t k 2 t 2 −λt−s −λt−tk ≤2 ηe supIsds 2 ηe max βk t 0 Wt, s 2 0 ≤ 2η2 γ02 s N 1 λ 1 − e−λ 2 0≤tk <t 3.6 k K. Then for ∀z ∈ D∗ , from the definition of D∗ and 3.6, since a b2 ≤ 2a2 2b2 , we have Ez2 Ez − z0 z0 2 ≤ 2E z − z0 2 z0 2 ≤2 ρK K 1−ρ 2K . 1−ρ 3.7 8 Journal of Applied Mathematics For ∀z ∈ D∗ , we have t Lz − z0 Wt, s Bfs, zs Cgs, zs − h ds 0 t Wt, tk Vk ztk Wt, sσs, zsdωs. 0 0≤t <t 3.8 k Since a b c2 ≤ 3a2 3b2 3c2 , it follows 2 ELz − z0 ≤ 3E t 2 Wt, sBfs, zs Cgs, zs − hds 0 2 t 2 3E Wt, tk Vk ztk 3E Wt, sσs, zsdωs . 0≤t <t 0 k 3.9 For first term of the right-hand side, using 3.7, A3 and Cauchy-Schwarz inequality, we have t E 2 Wt, sBfs, zs Cgs, zs − hds 0 ≤η 2 t e 0 ≤ η2 t 0 −λt−s t 2 −λt−s ds · e · EBfs, zs Cgs, zs − h ds 0 t 3.10 2 2 2 2 2 2 −λt−s −λt−s e ds · e · 2B Lf Ezs 2C Lg Ezs − h ds 0 2K 2 2 2 2 2 . ≤ η2 · L L C B g f 1 − ρ λ2 As to the second term, using 3.7, A6 and Cauchy-Schwarz inequality, we can write 2 E Wt, tk Vk ztk 0≤t <t k 2 2 −λt−tk −λt−tk · ≤η e e EVk ztk 0≤tk <t ≤ η2 e−λt−tk 0≤tk <t 0≤tk <t · e−λt−tk L2V Eztk 2 0≤tk <t 2K N2 2 . L · ≤η · 1 − ρ V 1 − e−λ 2 2 3.11 Journal of Applied Mathematics 9 As far as last term is concerned, using 3.7, A4, and the Itô isometry theorem, we obtain t E 2 Wt, sσs, zsdωs ≤ t 0 0 ≤η 2 Wt, s2 Eσs, zs2 ds t 0 e−2λt−s L2σ Ezs2 ds 2K L2σ · . ≤η · 1 − ρ 2λ 3.12 2 Thus, by combining 3.9–3.12, it follows that ρK L2σ N2 2K 2 2 2 2 2 2 ELz − z0 ≤ 3η · . LV B Lf C Lg 2 2 1−ρ λ 2λ 1−ρ 1 − e−λ 2 2 3.13 By Lemmas 2.5 and 2.6, one can obtain Wt τ, s τ − Wt, s ≤ εΓe−λ/2t−s . 3.14 Let τ ∈ T, q ∈ Q, where the sets T and Q are determined in Lemma 2.7, and we assume that 0 < ε < 1, then Lzt τ − Lzt t Wt τ, s τ − Wt, s Bfs τ, zs τ Cgs τ, zs τ − h Is τ ds 0 t Wt, s Bfs τ, zs τ Cgs τ, zs τ − h Is τ 0 − Bfs, zs Cgs, zs − h Is ds W t τ, tkq − Wt, tk Vkq z tkq βkq 0≤tk <t Wt, tk Vkq z tkq − Vk ztk βkq − βk 0≤tk <t t Wt τ, s τ − Wt, sσs τ, zs τdωs Wt, sσs τ, zs τ − σs, zsdωs. 0 0 t 3.15 10 Journal of Applied Mathematics Therefore, we have ELzt τ − Lzt2 t ≤ 3E Wt τ, s τ−Wt, s Bfsτ, zs τCgs τ, zsτ −h Is τ ds 0 t Wt, s Bfs τ, zs τCgs τ, zs τ − hIs τ 0 2 − Bfs, zs Cgs, zs −h Is ds 3E W t τ, tkq − Wt, tk Vkq z tkq βkq 0≤t <t k 2 Wt, tk Vkq z tkq − Vk ztk βkq − βk <t 0≤tk t 3E Wt τ, s τ − Wt, sσs τ, zs τdωs 0 2 t Wt, sσs τ, zs τ − σs, zsdωs . 0 3.16 We first evaluate the first term of the right hand side t E Wt τ, s τ − Wt, s Bfs τ, zs τ Cgs τ, zs τ − h Is τ ds 0 t Wt, s Bfs τ, zs τ Cgs τ, zs τ − h Is τ 0 ≤ 2E t 0 2 − Bfs, zs Cgs, zs −h Is ds Wt τ, s τ − Wt, s 2 × Bfs τ, zs τ Cgs τ, zs τ − h Is τ ds 2E t Wt, sB fs τ, zs τ − fs, zs 0 2 C gs τ, zs τ − h − gs, zs − h Is τ − Is ds ≤ c1 ε, 3.17 where c1 96η2 /λ2 B2 L2f · K/1 − ρ 1 C2 L2g · K/1 − ρ 1 γ02 1. Journal of Applied Mathematics 11 For the second term, we can estimate that E W t τ, tkq − Wt, tk Vkq z tkq βkq 0≤t <t k 2 Wt, tk Vkq z tkq − Vk ztk βkq − βk 0≤tk <t 2 Wt τ, tkq − Wt, tk Vkq ztkq βkq ≤ 2E 0≤t <t k 2 2E Wt, tk Vkq ztkq − Vk ztk βkq − βk 0≤t <t 3.18 k ≤ c2 ε, where c2 8η2 N 2 /1 − e−λ L2V · K/1 − ρ 1 γ02 1. For the last term, using A4 and Itô isometry identity, we have t E Wt τ, s τ − Wt, sσs τ, zs τdωs 0 2 t Wt, sσs τ, zs τ − σs, zsdωs 0 2 t ≤ 2E Wt τ, s τ − Wt, s, σs τ, zs τdωs 0 2 t 2E Wt, sσs τ, zs τ − σs, zsdωs 0 t ≤ 2E Wt τ, s τ − Wt, s2 σs τ, zs τ2 ds 0 2E t 3.19 Wt, s2 σs τ, zs τ − σs, zs2 ds 0 ≤ c3 ε, where c3 2/λΓ2 L2σ K/1 − ρ 1. Combining 3.17, 3.18 and 3.19, it follows that ELzt τ − Lzt2 ≤ c0 ε, where c0 3c1 c2 c3 . So, Lz ∈ D∗ , that is L is self-mapping from D∗ to D∗ by 3.13 and 3.20. Secondly, we will show L is contracting operator in D∗ . 3.20 12 Journal of Applied Mathematics For ∀x, y ∈ D∗ , t Lx − Ly Wt, sB fs, xs − f s, ys 0 C gs, xs − h − g s, ys − h ds Wt, tk Vk xtk − Vk ytk 3.21 0≤tk <t Wt, s σs, xs − σ s, ys dωs. 0 t By a minor modification of the proof of 3.13, we can obtain 2 ELx − Ly 2 L2σ N2 2 2 2 2 2 2 2 sup Ext − yt ≤ 6η LV B Lf C Lg 2 2 2λ λ t 1 − e−λ 2 ρ x − y ∞, 3.22 and therefore, Lx − Ly∞ ≤ ρx − y∞ , it follows that L is contracting operator in D∗ , so there exists a unique mean square almost periodic solution of 2.2 by the fixed points theorem. 4. Example Consider the following impulsive stochastic differential equation with delay ⎡ dxi t ⎣ai xi t 2 ⎤ 2 bij fj xj t cij gj xj t − 0.1 Ii t⎦dt j1 j1 0.5xi tdωi t, t ≥ 0, t / tk , − − Δxt xtk − x tk Dk x tk Vk x t−k βk , xt φt, 4.1 t tk , k ∈ N, −h ≤ t ≤ 0, where tk k, k ∈ N, fxt sin x1 t, sin x2 tT , gxt−0.1 cos x1 t−0.1, cos x2 t− 0.1T , Vik 0.01 sin x1 t, 0.01 cos x2 tT , βk 0.1, It 0.1, 0.1T , γ0 0.1, for convenience, we can choose −2 0 A , 0 −3 −0.1 0 B , 0 −0.1 0.2 0 C , 0 −0.2 −0.5 0 . Dk 0 −0.5 4.2 Then μA −2, I Dk 1/2, B 0.1, C 0.2, Lf Lg 1, LV 0.01, Lσ 0.5. Choose θ infk {t1k } 0.01, η 1, N 6. By simple calculation, we have λ −μA . . . ln η/θ 2, ρ 0.8139 < 1, K 1.107, ρK/1 − ρ 4.841. Journal of Applied Mathematics 13 Let D∗ {z ∈ D : Ez − z0 2 ≤ 4.841}, so, by Theorem 3.1, system 4.1 has a unique mean square almost periodic solution in D∗ . Remark 4.1. 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