Hindawi Publishing Corporation Discrete Dynamics in Nature and Society Volume 2009, Article ID 641368, 11 pages doi:10.1155/2009/641368 Research Article Existence Results for Second-Order Impulsive Neutral Functional Differential Equations with Nonlocal Conditions Meili Li and Chunhai Kou Department of Applied Mathematics, Donghua University, Shanghai 201620, China Correspondence should be addressed to Meili Li, stylml@dhu.edu.cn Received 2 September 2009; Accepted 26 October 2009 Recommended by Guang Zhang The existence of mild solutions for second-order impulsive semilinear neutral functional differential equations with nonlocal conditions in Banach spaces is investigated. The results are obtained by using fractional power of operators and Sadovskii’s fixed point theorem. Copyright q 2009 M. Li and C. Kou. 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. 1. Introduction The study of impulsive functional differential equations is linked to their utility in simulating processes and phenomena subject to short-time perturbations during their evolution. The perturbations are performed discretely and their duration is negligible in comparison with the total duration of the processes. That is why the perturbations are considered to take place “instantaneously” in the form of impulses. The theory of impulsive differential and functional differential equations has been extensively developed; see the monographs of Bainov and Simeonov 1, Lakshmikantham et al. 2, and Samoilenko and Perestyuk 3, where numerous properties of their solutions are studied, and detailed bibliographies are given. This paper is devoted to extending existing results to second-order differential equations. To be precise, in 4, the authors used Sadovsii’s fixed point theorem for a condensing map to establish existence results for first-order impulsive semilinear neutral functional differential inclusions with nonlocal conditions. Here, we obtain existence results for second-order semilinear impulsive differential equations with nonlocal conditions of the form d tk , x t − Ft, xh1 t Axt Gt, xh2 t, t ∈ J 0, b, t / dt − Δx|ttk Ik x tk , k 1, . . . , m, 2 Discrete Dynamics in Nature and Society Δx ttk I k x t−k , k 1, . . . , m, x 0 η, x0 gx x0 , 1.1 where A is the infinitesimal generator of a strongly continuous cosine family Ct, t ∈ R, of bounded linear operators in X. Also, 0 t0 < t1 < · · · < tm < tm1 b, Δx|ttk xtk − xt−k , Δx |ttk x tk − x t−k . Finally, F, G, g, Ik , I k k 1, . . . , m and h1 , h2 are given functions to be specified later. Other results on second order functional differential equations with and without impulsive effect can be founded in the monographs 5–8. This paper is organized as follows. In Section 2, we recall briefly some basic definitions and lemmas. The existence theorem for 1.1 and its proof are arranged in Section 3. Our approaches are based on Sadovskii’s fixed point theorem, and the theory of strongly continuous cosine families. 2. Preliminaries Definition 2.1 see 9. A one-parameter family Ct, t ∈ R, of bounded linear operators in the Banach space X is called a strongly continuous cosine family if and only if i Cs t Cs − t 2CsCt for all s, t ∈ R; ii C0 I; iii Ctx is strongly continuous in t on R for each fixed x ∈ X. We define the associated sine family St, t ∈ R, by Stx t Csxds, x ∈ X, t ∈ R. 2.1 0 We make the following assumption on A: H1 A is the infinitesimal generator of a strongly continuous cosine family Ct, t ∈ R, of bounded linear operators from X into itself. The infinitesimal generator of a strongly continuous cosine family Ct, t ∈ R is the operator A : X → X defined by d2 Ax 2 Ctx , dt t0 x ∈ DA, 2.2 Discrete Dynamics in Nature and Society 3 where DA x ∈ X : Ctx is twice continuously differentiable in t . 2.3 We define E x ∈ X : Ctx is once continuously differentiable in t . 2.4 Lemma 2.2 see 9. If Ct, t ∈ R, be a strongly continuous cosine family in X, then i there exist constants K ≥ 1 and ω ≥ 0 so that Ct ≤ Keω|t| , for all t ∈ R, and t2 ω|s| St1 − St2 ≤ K e ds, t1 ∀t1 , t2 ∈ R; 2.5 ii if x ∈ E, then Stx ∈ DA and d/dtCtx AStx. It is proved in 10 that for 0 ≤ α ≤ 1, the fractional powers −Aα exist as close linear operator in X, D−Aα ⊂ D−Aβ , for 0 ≤ β ≤ α ≤ 1, and −Aα −Aβ −Aαβ for 0 ≤ α β ≤ 1. We assume in addition the following assumption: H2 for 0 ≤ α ≤ 1, −Aα maps onto X and is 1 − 1, so that D−Aα is a Banach space when endowed with the form xα −Aα x, x ∈ D−Aα . We denote this Banach space by Xα . Denote J0 0, t1 , Jk tk , tk1 , k 1, 2, . . . , m. We define the following classes of functions: P CJ, Xα {x : J → Xα : xk ∈ CJk , Xα , k 0, 1, . . . , m and there exist xtk , xt−k , k 1, . . . , m with xtk xt−k }: P C1 J, Xα {x ∈ P CJ, Xα : xk ∈ CJk , Xα , k 0, 1, . . . , m and there exist x tk , x t−k , k 1, . . . , m with x tk x t−k }, where xk and xk represent the restriction of x and x to Jk , respectively, k 0, . . . , m, and xk Jk sups∈Jk xk sα . Obviously, P CJ, Xα is a Banach space with the norm xP C max{xk Jk , k 0, . . . , m}, and P C1 J, Xα is also a Banach space with the norm xP C1 max{xP C , x P C }. Definition 2.3. A function x· ∈ P C1 J, Xα is said to be a mild solution of 1.1 if i x0 gx x0 , x 0 η; ii Δx|ttk Ik xt−k , k 1, . . . , m; iii Δx |ttk I k xt−k , k 1, . . . , m; 4 Discrete Dynamics in Nature and Society iv the restriction of x· to the interval Jk k 0, . . . , m is continuous and the following integral equation is verified: xt Ct x0 − gx St η − F0, xh1 0 t Ct − sFs, xh1 sds 0 St − sGs, xh2 sds 0 t Ct − tk Ik x t−k 2.6 0<tk <t St − tk I k x t−k , t ∈ J. 0<tk <t For 1.1, we assume that the following hypotheses are satisfied: for some α ∈ 0, 1, H3 there exists a constant β ∈ 0, 1 such that F : J × Xα → Xβ is a continuous function, and −Aβ F : J × Xα → Xα satisfies the Lipschitz condition, that is, there exists a constant L > 0 such that −Aβ Ft1 , x1 − −Aβ Ft2 , x2 ≤ L|t1 − t2 | x1 − x2 α , α 2.7 for any 0 ≤ t1 , t2 ≤ b, x1 , x2 ∈ Xα . Moreover, there exists a constant L1 > 0 such that the inequality −Aβ Ft, x ≤ L1 xα 1 α 2.8 holds for any x ∈ Xα ; H4 the function G : J × Xα → X satisfies the following conditions: i for each t ∈ J, the function Gt, · : Xα → X is continuous, and for each x ∈ Xα , the function G·, x : J → X is strongly measurable, ii for each positive number l ∈ N, there is a positive function wl ∈ L1 J such that sup Gt, x ≤ wl t a.e. on J, xα ≤l 1 lim inf l→∞ l b wl sds γ < ∞, 2.9 0 where xα sup xsα ; 0≤s≤b H5 hi ∈ CJ, J, i 1, 2. g : P C1 J, Xα → Xα is continuous and satisfies that 2.10 Discrete Dynamics in Nature and Society 5 i there exist positive constants L2 and L2 such that gu ≤ L2 u 1 L PC 2 α ∀u ∈ P C1 J, Xα , 2.11 ii g is a completely continuous map; H6 Ik , I k ∈ CXα , Xα , k 1, . . . , m are all bounded, that is, there exist constants dk , dk , k 1, . . . , m, such that Ik xα ≤ dk , I k xα ≤ dk , for x ∈ Xα ; H7 Ct, t ∈ J, is completely continuous. 3. Main Result Theorem 3.1. Let x0 ∈ Xα . If the hypotheses H1 –H7 are satisfied, then 1.1 has a mild solution provided that L0 : 2M0 LMb < 1, 3.1 M L2 2M0 bL1 bγ < 1, 3.2 where M sup{Ct : t ∈ J}, M sup C t : t ∈ J , M0 −A−β . 3.3 Proof. Consider the space B P C1 J, Xα with morm xP C1 max{xP C , x P C }. We should now show that the operator P defined by P xt Ct x0 − gx St η − F0, xh1 0 t Ct − sFs, xh1 sds 0 t 0 St − sGs, xh2 sds Ct − tk Ik x t−k St − tk I k x t−k 0<tk <t 0<tk <t 3.4 has a fixed point. This fixed point is then a solution of 2.6. For each positive number l, let Bl {x ∈ B : xtα ≤ l, t ∈ J}. Then for each l, Bl is clearly a bounded close convex set in B. We claim that there exists a positive integer l such that P Bl ⊆ Bl . If it is not true, then for each positive integer l, there is a function xl · ∈ Bl , but 6 Discrete Dynamics in Nature and Society ∈ Bl , that is, P xl tα > l for some tl ∈ J, where tl denotes t is dependent on l. P xl · / However, on the other hand, we have l < P xl tα Ct x0 − gxl St η − F0, xl h1 0 t Ct − sFs, xl h1 sds 0 t St − sGs, xl h2 sds 0 − − Ct − tk Ik xl tk St − tk I k xl tk <t 0<t <t 0<tk α k ≤ Ct x0 − gxl α St η − −A−β −Aβ F0, xl h1 0 α t −β β Ct − s−A −A Fs, xl h1 sds 0 3.5 α t St − sGs, xl h2 sds 0 α − Ct − tk Ik xl t− − t xl tk I St k k k α 0<tk <t α 0<tk <t ≤ M x0 α L2 l L2 Mb ηα M0 L1 l 1 MM0 bL1 l 1 Mb b wl sds M 0 m m dk M b − tk dk . k1 k1 Dividing on both sides by l and taking the lower limits as l → ∞, we get ML2 2M0 bL1 bγ ≥ 1. This is a contradiction with the formula 3.2. Hence for some positive integer l, P Bl ⊆ Bl . Next we will show that the operator P has a fixed point on Bl , which implies that 1.1 has a mild solution. For this purpose, we decompose P as P P1 P2 , where the operators P1 , P2 are defined on Bl , respectively, by P1 xt t Ct − sFs, xh1 sds − StF0, xh1 0, 0 P2 xt Ct x0 − gx Stη t St − sGs, xh2 sds 0 Ct − tk Ik x t−k St − tk I k x t−k , 0<tk <t 0<tk <t 3.6 Discrete Dynamics in Nature and Society 7 for t ∈ J, and we will verify that P1 is a contraction while P2 is a completely continuous operator. To prove that P1 is a contraction, we take x1 , x2 ∈ Bl arbitrarily. Then for each t ∈ J and by condition H3 , we have that t P1 x1 t − P1 x2 tα ≤ Ct − sFs, x1 h1 s − Fs, x2 h1 sds 0 α StF0, x1 h1 0 − F0, x2 h1 0α t Ct − s−A−β −Aβ Fs, x1 h1 s − Fs, x2 h1 sds 0 α St−A−β −Aβ F0, x1 h1 0 − F0, x2 h1 0 α ≤ 2M0 LMb sup x1 s − x2 sα 0≤s≤b L0 sup x1 s − x2 sα . 0≤s≤b 3.7 Thus P1 x1 − P1 x2 α ≤ L0 x1 − x2 α . Therefore, by assumption 0 < L0 < 1 see 3.1, we see that P1 is a contraction. To prove that P2 is completely continuous, firstly we prove that P2 is continuous on Bl . Let xn → x∗ , xn ∈ Bl , then by H4 i, we have Gs, xn h2 s → Gs, x∗ h2 s, n → ∞. Since Gs, xn h2 s − Gs, x∗ h2 s ≤ 2wl s, by the dominated convergence theorem, we have P2 xn − P2 x∗ P C t supCt gx∗ − gxn St − sGs, xn h2 s − Gs, x∗ h2 sds 0 t∈J − − − − Ct−tk Ik xn tk −Ik x∗ tk St−tk I k xn tk −I k x∗ tk <t 0<t <t 0<tk ≤ Mgx∗ − gxn α m k1 k b 0 St − sGs, xn h2 s − Gs, x∗ h2 sα ds MIk xn t−k − Ik x∗ t−k α α 8 Discrete Dynamics in Nature and Society m Mb − tk I k xn t−k − I k x∗ t−k −→ 0 α k1 as n −→ ∞, P2 xn − P2 x∗ PC t supC t gx∗ − gxn Ct − sGs, xn h2 s − Gs, x∗ h2 sds 0 t∈J C t − tk Ik xn t−k − Ik x∗ t−k 0<tk <t − − Ct − tk I k xn tk − I k x∗ tk <t 0<tk α ≤ M gx∗ − gxn α m k1 m b 0 Ct − sGs, xn h2 s − Gs, x∗ h2 sα ds M Ik xn t−k − Ik x∗ t−k α MI k xn t−k − I k x∗ t−k −→ 0 as n −→ ∞. α k1 3.8 Thus, P2 is continuous. Next, we prove that {P2 x : x ∈ Bl } is a family of equicontinuous functions. Let τ1 , τ2 ∈ J, τ1 < τ2 . Then for each t ∈ J, we have P2 xτ2 − P2 xτ1 α ≤ Cτ2 − Cτ1 x0 − gx α Sτ2 η − Sτ1 ηα τ1 τ2 Sτ2 − s − Sτ1 − sGs, xh2 sds Sτ2 − sGs, xh2 sds τ1 0 α α − − Cτ2 − tk Ik x tk Cτ2 − tk − Cτ1 − tk Ik x tk 0<t <τ τ ≤t <τ k 1 α 1 k 2 − − Sτ2 − tk I k x tk Sτ2 − tk − Sτ1 − tk I k x tk 0<t <τ τ ≤t <τ k 1 α 1 k 2 α α Discrete Dynamics in Nature and Society 9 ≤ Cτ2 − Cτ1 x0 − gx α Sτ2 η − Sτ1 ηα τ1 0 τ2 Sτ2 − s − Sτ1 − sGs, xh2 sα ds Sτ2 − sGs, xh2 sds τ1 α Cτ2 − tk − Cτ1 − tk dk Cτ2 − tk dk τ1 ≤tk <τ2 0<tk <τ1 Sτ2 − tk − Sτ1 − tk dk Sτ2 − tk dk , τ1 ≤tk <τ2 0<tk <τ1 3.9 and similarly P2 x τ2 − P2 x τ1 α ≤ C τ2 − C τ1 x0 − gx α S τ2 − S τ1 ηα τ1 τ2 Cτ2 − s − Cτ1 − sGs, xh2 sds Cτ2 − sGs, xh2 sds 0 τ α 1 α − − C τ2 − tk Ik x tk C τ2 − tk − C τ1 − tk Ik x tk 0<t <τ τ ≤t <τ k 1 α 1 α 1 k 2 − − S τ2 − tk I k x tk S τ2 − tk − S τ1 − tk I k x tk 0<t <τ τ ≤t <τ k 1 k 2 α α ≤ C τ2 − C τ1 x0 − gx α S τ2 − S τ1 ηα τ1 τ2 Cτ2 − s − Cτ1 − sGs, xh2 sα ds Cτ2 − sGs, xh2 sds 0 τ1 C τ2 − tk − C τ1 − tk dk C τ2 − tk dk 0<tk <τ1 α τ1 ≤tk <τ2 S τ2 − tk − S τ1 − tk dk S τ2 − tk dk . 0<tk <τ1 τ1 ≤tk <τ2 3.10 The right-hand sides are independent of x ∈ Bl and tend to zero as τ2 − τ1 → 0, since Ct, St, C t, S t are uniformly continuous for t ∈ J and the compactness of Ct, St for t > 0 implies the continuity in the uniform operator topology. The compactness of St follows from that of Ct and Lemma 2.2. This shows that P2 maps Bl into a family of equicontinuous functions. It remains to prove that V t {P2 xt : x ∈ Bl } is relatively compact in X. 10 Discrete Dynamics in Nature and Society Obviously, by condition H5 ii, V 0 is relatively compact in B. Let 0 < t ≤ b be fixed and 0 < < t. For x ∈ Bl , we define ccP2, xt Ct x0 − gx Stη t− St − sGs, xh2 sds 0 Ct − tk Ik x t−k St − tk I k x t−k . 0<tk <t 3.11 0<tk <t Since Ct, St are compact operators, the set V t {P2, xt : x ∈ Bl } is relatively compact in B for every , 0 < < t. Moreover, for every x ∈ Bl , we have t t St − sGs, xh2 sds ≤ P2 xt − P2, xtα St − swl sds, t− t− α t t P2 x t − P2, x t Ct − sGs, xh ≤ sds Ct − swl sds. 2 α t− t− α 3.12 Therefore, there are relatively compact sets arbitrarily close to the set V t. Hence, the set V t is relatively compact in B. Thus, by Arzela-Ascoli theorem, P2 is a completely continuous operator. Those arguments enable us to conclude that P P1 P2 is a condensing map on Bl , and by the fixed point theorem of Sadovskii, there exists a fixed point x· for P on Bl . Therefore, the nonlocal Cauchy problem with impulsive effect 1.1 has a mild solution. The proof is completed. Acknowledgments The work of the M. Li is supported by NNSF of China no. 10971139. The work of C. Kou is supported by NNSF of China nos. 10701023 and 10971221. The authors would like to thank the anonymous referee for his/her remarks about the evaluation of the original version of the manuscript. References 1 D. D. Bainov and P. S. Simeonov, Systems with Impulse Effect, Stability, Theory and Applications, John Wiley & Sons, New York, NY, USA, 1989. 2 V. Lakshmikantham, D. D. Bainov, and P. S. Simeonov, Theory of Impulsive Differential Equations, vol. 6 of Series in Modern Applied Mathematics, World Scientific, Singapore, 1989. 3 A. M. Samoilenko and N. A. Perestyuk, Impulsive Differential Equations, vol. 14 of World Scientific Series on Nonlinear Science. Series A: Monographs and Treatises, World Scientific, Singapore, 1995. 4 X. Fu and Y. Cao, “Existence for neutral impulsive differential inclusions with nonlocal conditions,” Nonlinear Analysis: Theory, Methods & Applications, vol. 68, no. 12, pp. 3707–3718, 2008. 5 K. Balachandran, J. Y. Park, and S. Marshal Anthoni, “Controllability of second order semilinear Volterra integrodifferential systems in Banach spaces,” Bulletin of the Korean Mathematical Society, vol. 36, no. 1, pp. 1–13, 1999. Discrete Dynamics in Nature and Society 11 6 M. Benchohra, J. Henderson, and S. K. Ntouyas, “Existence results for impulsive multivalued semilinear neutral functional differential inclusions in Banach spaces,” Journal of Mathematical Analysis and Applications, vol. 263, no. 2, pp. 763–780, 2001. 7 H. R. Henrı́quez and M. Eduardo Hernández, “Approximate controllability of second-order distributed implicit functional systems,” Nonlinear Analysis: Theory, Methods & Applications, vol. 70, no. 2, pp. 1023–1039, 2009. 8 R. Sakthivel, N. I. Mahmudov, and J. H. Kim, “On controllability of second order nonlinear impulsive differential systems,” Nonlinear Analysis: Theory, Methods & Applications, vol. 71, no. 1-2, pp. 45–52, 2009. 9 C. C. Travis and G. F. Webb, “Cosine families and abstract nonlinear second order differential equations,” Acta Mathematica Academiae Scientiarum Hungaricae, vol. 32, no. 1-2, pp. 75–96, 1978. 10 H. O. Fattorini, “Ordinary differential equations in linear topological spaces. I,” Journal of Differential Equations, vol. 5, pp. 72–105, 1969.