Hindawi Publishing Corporation Abstract and Applied Analysis Volume 2008, Article ID 939062, 19 pages doi:10.1155/2008/939062 Research Article Existence of Periodic Solutions for Integrodifferential Impulsive Periodic System on Banach Space JinRong Wang,1 X. Xiang,2 and W. Wei2 1 2 College of Computer Science and Technology, Guizhou University, Guiyang, Guizhou 550025, China College of Science, Guizhou University, Guiyang, Guizhou 550025, China Correspondence should be addressed to JinRong Wang, wjr9668@126.com Received 5 July 2008; Accepted 28 October 2008 Recommended by Agacik Zafer This paper deals with a class of integrodifferential impulsive periodic systems on Banach space. Using impulsive periodic evolution operator given by us, the T0 -periodic PC-mild solution is introduced and suitable Poincaré operator is constructed. By virtue of the generalized new Gronwall lemma with impulse and B-norm, the estimate on the PC-mild solutions is derived. Showing the continuity and compactness of the Poincaré operator, we utilize Horn’s fixed point theorem to prove the existence of T0 -periodic PC-mild solutions when the PC-mild solutions are bounded and ultimate bounded. This extends the study of periodic solutions of integrodifferential periodic system without impulse to integrodifferential periodic system with impulse on general Banach spaces. At last, an example is given for demonstration. Copyright q 2008 JinRong Wang 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. 1. Introduction It is well known that impulsive periodic motion is a very important and special phenomenon not only in natural science but also in social science such as climate, food supplement, insecticide population, and sustainable development. Periodic system with applications on finite dimensional spaces has been extensively studied. Particularly, impulsive periodic systems on finite dimensional spaces are considered and some important results such as the existence and stability of periodic solution, the relationship between bounded solution and periodic solution, robustness by perturbation are obtained see 1–4. Since the end of the last century, many authors including us pay great attention to impulsive systems on infinite dimensional spaces. Ahmed investigated optimal control problems of a system governed by an impulsive system see 5–8. We also gave a series of results for semilinear integrodifferential, strongly nonlinear impulsive systems and 2 Abstract and Applied Analysis optimal control problems see 9–12. Particulary, Benchohra et al. give many interesting recent results for various classes of differential equations with impulses on finite and infinite dimensional Banach spaces see 13. Although, there are some papers on periodic solution for periodic system on infinite dimensional spaces see 14–24 and some results discussing integrodifferential system on finite Banach space and infinite Banach space see 19, 25, to our knowledge, integrodifferential impulsive periodic systems on infinite dimensional spaces with unbounded operator have not been extensively investigated. Recently, we discuss the impulsive periodic system and integrodifferential impulsive system on infinite dimensional spaces. For linear impulsive evolution operator is constructed and T0 -periodic P C-mild solution is introduced. Existence of periodic solutions and alternative theorem, criteria of Massera type, and asymptotical stability and robustness by perturbation are established see 26–28. For integrodifferential impulsive system, existence of P C-mild solutions and optimal controls are presented see 9. Herein, we go on studying the following integrodifferential impulsive periodic system: t ẋt Axt f t, x, gt, s, xds , 0 Δxt Bk xt ck , t / τk , 1.1 t τk , on infinite dimensional Banach space X, where 0 τ0 < τ1 < τ2 < · · · < τk · · · , limk → ∞ τk ∞, τkδ τk T0 , Δxτk xτk − xτk− , k ∈ Z0 , T0 is a fixed positive number, and δ ∈ N denotes the number of impulsive points between 0 and T0 . The operator A is the infinitesimal generator of a C0 -semigroup {T t, t ≥ 0} on X, f is a measurable function from 0, ∞×X ×X to X and is T0 -periodic in t, g is a continuous function from 0, ∞ × 0, ∞ × X to X and is T0 -periodic in t and s and Bkδ Bk , ckδ ck . This paper is mainly concerned with the existence of periodic solutions for integrodifferential impulsive periodic system on infinite dimensional Banach space X. In this paper, we use Horn’s fixed point theorem to obtain the existence of periodic solutions for integrodifferential impulsive periodic system 1.1. First, by virtue of impulsive evolution operator corresponding to linear homogeneous impulsive system, we construct a new Poincaré operator P for integrodifferential impulsive periodic system 1.1, then overcome some difficulties to show the continuity and compactness of Poincaré operator P which are very important. By a new generalized Gronwall inequality with impulse and Bnorm given by us, the estimate of P C-mild solutions is established. Therefore, the existence of T0 -periodic P C-mild solutions for impulsive integrodifferential periodic system is shown. This extends the study of periodic solutions of integrodifferential periodic system without impulse to integrodifferential periodic system with impulse on general Banach spaces. This paper is organized as follows. In Section 2, some results of linear impulsive periodic system and properties of impulsive periodic evolution operator corresponding to homogeneous linear impulsive periodic system are recalled. In Section 3, the new generalized Gronwall inequality with impulse and B-norm is established and the existence of P C-mild solutions for integrodifferential impulsive system is presented. In Section 4, the T0 -periodic P C-mild solutions for integrodifferential impulsive periodic system 1.1 are introduced. We construct the suitable Poincaré operator P and give the relation between T0 -periodic P C-mild solution and the fixed point of the Poincaré operator P . After showing the continuity and JinRong Wang et al. 3 compactness of the Poincaré operator P , we can use Horn’s fixed point theorem to establish the existence of T0 -periodic P C-mild solutions for integrodifferential impulsive periodic system when the P C-mild solutions are bounded and ultimate bounded. At last, an example is given to demonstrate the applicability of our result. 2. Preliminaries In order to study the integrodifferential impulsive periodic system, we first recall some results about linear impulsive periodic system here. Let X be a Banach space. £X denotes the space of linear operators in X, and £b X denotes the space of bounded linear operators in X. {τ1 , . . . , τδ } ⊂ 0, T0 , £b X is the Banach space with the usual supremum norm. Define D where δ ∈ N denotes the number of impulsive points between 0 and T0 . We introduce x is continuous from P C0, T0 ; X ≡ {x : 0, T0 → X | x is continuous at t ∈ 0, T0 \ D, 1 left and has right-hand limits at t ∈ D} and P C 0, T0 ; X ≡ {x ∈ P C0, T0 ; X | ẋ ∈ P C0, T0 ; X}. Set xP C max sup xt 0, sup xt − 0 , t∈0,T0 t∈0,T0 xP C1 xP C ẋP C . 2.1 It can be seen that a Banach space is endowed with the norm ·P C ·P C1 , P C0, T0 ; X P C1 0, T0 ; X. Firstly, we consider the homogeneous linear impulsive periodic system . x t Axt, Δxt Bk xt, t / τk , t τk . 2.2 We introduce the following assumption. Assumption H1. H1.1 A is the infinitesimal generator of a C0 -semigroup {T t, t ≥ 0} on X with domain DA. H1.2 There exists δ ∈ N such that τkδ τk T0 . H1.3 For each k ∈ Z0 , δ ∈ N, Bk ∈ £b X and Bkδ Bk . In order to study system 2.2, we need to consider the associated Cauchy problem . x t Axt, t ∈ 0, T0 \ D, Δx τk Bk x τk , k 1, 2, . . . , δ, 2.3 x0 x. If x ∈ DA and DA is an invariant subspace of Bk , using 29, Theorem 5.2.2, page 144, step by step, one can verify that the Cauchy problem 2.3 has a unique classical solution x ∈ P C1 0, T0 ; X represented by xt St, 0x where S·, ·: Δ t, θ ∈ 0, T0 × 0, T0 | 0 ≤ θ ≤ t ≤ T0 −→ £b X 2.4 4 Abstract and Applied Analysis given by ⎧ T t − θ, τk−1 ≤ θ ≤ t ≤ τk , ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ ⎪ τk−1 ≤ θ < τk < t ≤ τk1 , ⎪ ⎨T t − τk I Bk T τk − θ , St, θ ⎪ ⎪T t − τk I Bj T τj − τj−1 I Bi T τi − θ , ⎪ ⎪ ⎪ ⎪ θ<τj <t ⎪ ⎪ ⎩ τi−1 ≤ θ < τi ≤ · · · < τk < t ≤ τk1 . 2.5 The operator {St, θ, t, θ ∈ Δ} is called impulsive evolution operator associated with {Bk ; τk }∞ k1 . Now we introduce the P C-mild solution of Cauchy problem 2.3 and T0 -periodic P Cmild solution of the system 2.2. Definition 2.1. For every x ∈ X, the function x ∈ P C0, T0 ; X given by xt St, 0x is said to be the P C-mild solution of the Cauchy problem 2.3. Definition 2.2. A function x ∈ P C0, ∞; X is said to be a T0 -periodic P C-mild solution of system 2.2 if it is a P C-mild solution of Cauchy problem 2.3 corresponding to some x and xt T0 xt for t ≥ 0. The following lemma gives the properties of the impulsive evolution operator {St, θ, t, θ ∈ Δ} associated with {Bk ; τk }∞ k1 which are widely used in the sequel. Lemma 2.3 see 26, Lemma 1. Impulsive evolution operator {St, θ, t, θ ∈ Δ} has the following properties. 1 For 0 ≤ θ ≤ t ≤ T0 , St, θ ∈ £b X, that is, sup0≤θ≤t≤T0 St, θ ≤ MT0 , where MT0 > 0. 2 For 0 ≤ θ < r < t ≤ T0 , r / τk , St, θ St, rSr, θ. 3 For 0 ≤ θ ≤ t ≤ T0 and N ∈ Z0 , St NT0 , θ NT0 St, θ. 4 For 0 ≤ t ≤ T0 and N ∈ Z0 , SNT0 t, 0 St, 0ST0 , 0N . 5 If {T t, t > 0} is a compact semigroup in X, then St, θ is a compact operator for 0 ≤ θ < t ≤ T0 . Here, we note that system 2.2 has a T0 -periodic P C-mild solution x if and only if ST0 , 0 has a fixed point. The impulsive evolution operator {St, θ, t, θ ∈ Δ} can be used to reduce the existence of T0 -periodic P C-mild solutions for linear impulsive periodic system to the existence of fixed points for an operator equation. This implies that we can build up the new framework to study the periodic P C-mild solutions for integrodifferential impulsive periodic system on Banach space. Consider the nonhomogeneous linear impulsive periodic system ẋt Axt ft, t/ τk , Δxt Bk xt ck , t τk , 2.6 JinRong Wang et al. 5 and the associated Cauchy problem ẋt Axt ft, t ∈ 0, T0 \ D, Δx τk Bk x τk ck , k 1, 2, . . . , δ, 2.7 x0 x, where f ∈ L1 0, T0 ; X, ft T0 ft, and ckδ ck . Now we introduce the P C-mild solution of Cauchy problem 2.7 and T0 -periodic P Cmild solution of system 2.6. Definition 2.4. A function x ∈ P C0, T0 ; X, for finite interval 0, T0 , is said to be a P C-mild solution of the Cauchy problem 2.6 corresponding to the initial value x ∈ X and input f ∈ L1 0, T0 ; X if x is given by xt St, 0x t St, θfθdθ 0 S t, τk ck . 2.8 0≤τk <t Definition 2.5. A function x ∈ P C0, ∞; X is said to be a T0 -periodic P C-mild solution of system 2.6 if it is a P C-mild solution of Cauchy problem 2.7 corresponding to some x and xt T0 xt for t ≥ 0. 3. The generalized Gronwall inequality and existence of solutions In order to derive an estimate of the P C-mild solutions, we introduce the following generalized Gronwall inequality with impulse and B-norm. Lemma 3.1. Let x ∈ P C0, ∞, X and let it satisfy the following inequality: xt ≤ a b t xθλ1 dθ c 0 t 0 λ2 xθ dθ, B 3.1 where a, b, c ≥ 0, 0 ≤ λ1 , λ2 ≤ 1 are constants, and xθ B max sup xξ 0, sup xξ − 0 . 0≤ξ≤θ 3.2 0≤ξ≤θ Then one has xt ≤ a 1ebct . 3.3 Proof. i For 0 ≤ λ1 , λ2 < 1, let λ max{λ1 , λ2 } ∈ 0, 1 and yt ⎧ ⎨1, xt ≤ 1, ⎩xt, xt > 1. 3.4 6 Abstract and Applied Analysis Then xt ≤ yt ≤ a 1 b t yθλ dθ c t 0 0 λ yθ dθ, B ∀t ∈ 0, T0 , 3.5 Using 3.5, we obtain λ yt ≤ a 1 b c B t 0 λ yθ dθ. B 3.6 Define t λ yθ dθ, 3.7 λ u̇t b cyt B , t / τk , u0 a 1, u τk 0 u τk . 3.8 ut a 1 b c 0 B then we get Since yt λB ≤ ut, we then have u̇t ≤ b cut, t / τk , u0 a 1, u τk 0 u τk . 3.9 For t ∈ τk , τk1 , by 3.9, we obtain ut ≤ u τk 0 ebct−τk u τk ebct−τk , 3.10 ut ≤ a 1ebct , 3.11 xt ≤ yt B ≤ a 1ebct . 3.12 further, thus, ii For λ1 λ2 1, we only need to define u1 t a b c t 0 xθ dθ. B 3.13 JinRong Wang et al. 7 Similar to the proof in i, one can obtain xt ≤ xt B ≤ aebct . 3.14 Combining i and ii, one can complete the proof. Now, we consider the following integrodifferential impulsive periodic system: t ẋt Axt f t, x, gt, s, xds , t / τk , 0 Δxt Bk xt ck , 3.15 t τk , and the associated Cauchy problem t ẋt Axt f t, x, gt, s, xds , t ∈ 0, T0 \ D, 0 Δx τk Bk x τk ck , k 1, 2, . . . , δ, 3.16 x0 x. By virtue of the expression of the P C-mild solution of the Cauchy problem 2.7, we can introduce the P C-mild solution of the Cauchy problem 3.16. Definition 3.2. A function x ∈ P C0, T0 ; X is said to be a P C-mild solution of the Cauchy problem 3.16 corresponding to the initial value x ∈ X if x satisfies the following integral equation: xt St, 0x S t θ St, θf θ, xθ, gθ, s, xsds dθ 0 t, τk ck , 0 for t ∈ 0, T0 . 3.17 0≤τk <t Now, we introduce the T0 -periodic P C-mild solution of system 3.15. Definition 3.3. A function x ∈ P C0, ∞; X is said to be a T0 -periodic P C-mild solution of system 3.15 if it is a P C-mild solution of Cauchy problem 3.16 corresponding to some x and xt T0 xt for t ≥ 0. Assumption H2. H2.1 f : 0, ∞ × X × X → X is measurable for t ≥ 0, and for any x1 , x2 , y1 , y2 ∈ X satisfying x1 , x2 , y1 , y2 ≤ ρ there exists a positive constant Lf ρ > 0 such that f t, x1 , y1 − f t, x2 , y2 ≤ Lf ρ x1 − x2 y1 − y2 . 3.18 8 Abstract and Applied Analysis H2.2 There exists a positive constant Mf > 0 such that ft, x, y ≤ Mf 1 x y, ∀x, y ∈ X. 3.19 H2.3 ft, x, y is T0 -periodic in t, that is, f t T0 , x, y ft, x, y, t ≥ 0. 3.20 H2.4 g : 0, ∞ × 0, ∞ × X → X is continuous for t ≥ s ≥ 0 and for any x, y ∈ X satisfying x, y ≤ ρ there exists a positive constant Lg ρ > 0 such that gt, s, x − gt, s, y ≤ Lg ρx − y. 3.21 H2.5 There exists a positive constant Mg > 0 such that gt, s, x ≤ Mg 1 x, ∀x ∈ X. 3.22 H2.6 gt, s, x are T0 -periodic in t and s, that is, g t T0 , s T0 , x gt, s, x, t ≥ s ≥ 0, T0 gt, s, xds 0, t ≥ s ≥ 0. 3.23 0 H2.7 For each k ∈ Z0 and ck ∈ X there exists δ ∈ N such that ckδ ck . It is not difficult to verify the following results. Lemma 3.4. Under the assumptions [H2.4] and [H2.5], one has the following properties: · 1 0 g·, s, xsds : P C0, T0 ; X → P C0, T0 ; X; 2 for all x1 , x2 ∈ P C0, T0 ; X and x1 P C0,T0 ;X , x2 P C0,T0 ;X ≤ ρ, t t g t, s, x1 s ds − g t, s, x2 s ds ≤ Lg ρT0 x1 − x2 ; t t B 0 3.24 0 3 for x ∈ P C0, T0 ; X, t gt, s, xsds ≤ Mg T0 1 xt . B 0 Now we present the existence of P C-mild solution for system 3.16. 3.25 JinRong Wang et al. 9 Theorem 3.5. Assumptions [H1.1], [H2.1], [H2.2], [H2.4], and [H2.5] hold, and for each k ∈ Z0 , Bk ∈ £b X, ck ∈ Xare fixed. Then system 3.16 has a unique P C-mild solution given by xt, x St, 0x t θ St, θf θ, xθ, 0 0 gθ, s, xsds dθ S t, τk ck . 3.26 0≤τk <t Proof. A similar result is given by Wei et al. in 9. Thus, we only sketch the proof here. In order to make the process clear we divide it into three steps. Step 1. We consider the following general integrodifferential equation without impulse ẋt Axt f t, x, t gt, s, xds , t ∈ s, τ, 3.27 0 xs x ∈ X. In order to obtain the local existence of mild solution for system 3.27, we only need to set up the framework for using the contraction mapping theorem. Consider the ball given by B x ∈ C s, t1 ; X | xt − x ≤ 1, s ≤ t ≤ t1 , 3.28 where t1 would be chosen and xt ≤ 1 x ρ, s ≤ t ≤ t1 . B ⊆ Cs, t1 , X is a closed convex set. Define a map Q on B given by Qxt T tx t θ T t − θf θ, xθ, gθ, s, xsds dθ. s 3.29 0 Under the assumptions H1.1, H2.1, H2.2, H2.4, H2.5, and Lemma 3.1, one can verify that map Q is a contraction map on B with chosen t1 > 0. This means that system 3.27 has a unique mild solution x ∈ Cs, t1 ; X given by xt T tx t s θ T t − θf θ, xθ, gθ, s, xsds dθ on s, t1 . 3.30 0 Again, using Lemma 3.1, we can obtain the a priori estimate of the mild solutions for system 3.27 and present the global existence of mild solutions. 10 Abstract and Applied Analysis Step 2. For t ∈ τk , τk1 , consider the Cauchy problem ẋt Axt f t, x, t gt, s, xds , t ∈ τk , τk1 , 0 x τk xk ≡ I Bk x τk ck ∈ X. 3.31 By Step 1, Cauchy problem 3.31 also has a unique P C-mild solution: xt T t − τk xk t θ T t − θf θ, xθ, gθ, s, xsds dθ. τk 3.32 0 Step 3. Combining all solutions on τk , τk1 k 1, . . . , δ, one can obtain the P C-mild solution of the Cauchy problem 3.16 given by xt, x St, 0x t 0 θ St, θf θ, xθ, gθ, s, xsds dθ S t, τk ck . 0 3.33 0≤τk <t This completes the proof. 4. Poincaré operator and existence of periodic solutions To establish the periodic solutions for the system 3.15, we define a Poincaré operator from X to X as follows: P x x T0 , x S T0 , 0 x T0 θ S T0 , θ f θ, xθ, x, 0 0 gθ, s, xs, xds dθ S T0 , τk ck , 0≤τk <T0 4.1 where x·, xdenotes the P C-mild solution of the Cauchy problem 3.16 corresponding to the initial value x0 x, then examine whether P has a fixed point. We first note that a fixed point of the Poincaré operator P gives rise to a periodic solution. Lemma 4.1. System 3.15 has a T0 -periodic P C-mild solution if and only if P has a fixed point. Proof. Suppose x· x· T0 , then x0 xT0 P x0. This implies that x0 is a fixed point of P . On the other hand, if P x0 x0 , x0 ∈ X, then for the P C-mild solution x·, x0 of the Cauchy problem 3.16 corresponding to the initial value x0 x0 , we can define y· x· T0 , x0 , then y0 xT0 , x0 P x0 x0 . Now, for t > 0, we can use the properties JinRong Wang et al. 11 2, 3, and 4 of Lemma 2.3 and assumptions H1.2, H1.3, H2.3, H2.6, and H2.7to arrive at yt x t T0 , x0 S t T0 , T0 S T0 , 0 x0 T0 θ S t T0 , T0 S T0 , θ f θ, x θ, x0 , g θ, s, x s, x0 ds dθ 0 0 S t T0 , T0 S T0 , τk ck 0≤τk <T0 tT0 T0 θ S t T0 , θ f θ, x θ, x0 , g θ, s, x s, x0 ds dθ S t T0 ≤τkδ <tT0 T0 , τkδ St, 0 S T0 , 0 x0 T0 0 ckδ θ S T0 , θ f θ, x θ, x0 , g θ, s, x s, x0 ds dθ 0 t 0 S T0 , τk ckδ 0≤τk <T0 0 S t T0 , θ T0 f θ T0 , x θ T0 , x0 , S t T0 , τkδ ckδ θT0 g θ T0 , s, x s, x0 ds dθ 0 T0 ≤τkδ <tT0 St, 0x T0 t θT0 S t T0 , θ T0 f θ T0 , x θ T0 , x0 , g θ T0 , s, x s, x0 ds dθ 0 S t T0 ≤τkδ <tT0 T0 , τkδ T0 ckδ St, 0x T0 t θ St, θf θ, x θ T0 , x0 , g θ T0 , s T0 , x s T0 , x0 ds dθ 0 S t T0 ≤τkδ <tT0 St, 0y0 S t T0 , τkδ t, τk ckδ θ St, θf θ, yθ, y0, gθ, s, ys, y0ds dθ 0 0 0 ck 0≤τk <t St, 0y0 t θ St, θf θ, yθ, y0, gθ, s, ys, y0ds dθ 0 S t, τk ck . 0≤τk <t 0 4.2 12 Abstract and Applied Analysis This implies that y·, y0 is a P C-mild solution of Cauchy problem 3.16 with initial value y0 x0 . Thus the uniqueness implies that x·, x0 y·, y0 x· T0 , x0 , so that x·, x0 is a T0 -periodic. Second, we show that the Poincaré operator P defined by 4.1 is a continuous operator. Lemma 4.2. Assumptions [H1.1], [H2.1], [H2.2], [H2.4], and [H2.5] hold. Then the operator P is a continuous operator of x on X. Proof. Let x, y ∈ Ξ ⊂ X, where Ξ is a bounded subset of X. Suppose x·, x and x·, y are the P C-mild solutions of Cauchy problem 3.16 corresponding to the initial value x and y ∈ X, respectively, given by xt, x St, 0x t 0 xt, y St, 0y t 0 θ St, θf θ, xθ, x, gθ, s, xs, xds dθ S T0 , τk ck ; 0 0≤τ <t 0 0≤τk <t k θ St, θf θ, xθ, y, gθ, s, xs, yds dθ S T0 , τk ck . 4.3 Thus, by assumption H2.2, property 1 of Lemma 2.3, and property 3 of Lemma 3.4, we obtain ck xt, x ≤ MT0 x 1 Mg T0 MT0 Mf T0 MT0 0≤τk <T0 MT0 Mf t xθ, xdθ MT0 Mf Mg T0 0 t 0 xθ,x dθ B 4.4 t t ≤ a0 MT0 Mf xθ, xdθ MT0 Mf Mg T0 xθ,x B dθ, 0 0 ck xt, y ≤ MT0 y 1 Mg T0 MT0 Mf T0 MT0 0≤τk <T0 MT0 Mf t 0 ≤ b0 MT0 Mf xθ, ydθ MT0 Mf Mg T0 t t 0 xθ, ydθ MT0 Mf Mg T0 0 xθ,y dθ B t 0 4.5 xθ,y dθ. B By Lemma 3.1, one can verify that there exist constants M1∗ and M2∗ > 0 such that xt, x ≤ M1∗ , xt, y ≤ M2∗ . 4.6 Let ρ max{M1∗ , M2∗ } > 0, then x·, x, x·, y ≤ ρ which imply that they are locally bounded. JinRong Wang et al. 13 By assumption H2.1, property 1 of Lemma 2.3, and property 2 of Lemma 3.4, we obtain xt, x − xt, y ≤ St, 0x − y θ t f θ, xθ, x, gθ, s, xs, xds St, θ 0 − f θ, xθ, y, 0 θ 0 gθ, s, xs, yds dθ 4.7 ≤ MT0 x − y MT0 Lf ρ t xθ, x − xθ, ydθ MT0 Lf ρLg ρT0 0 t 0 xθ,x − xθ,y dθ. B By Lemma 3.1 again, one can verify that there exists a constant M3∗ > 0 such that xt, x − xt, y ≤ M3∗ MT0 x − y ≡ Lx − y, ∀t ∈ 0, T0 , 4.8 which implies that P x − P y x T0 , x − x T0 , y ≤ Lx − y. 4.9 Hence, P is a continuous operator of x on X. In the sequel, we need to prove the compactness of operator P , so we make the following assumption. Assumption H3 The semigroup {T t, t > 0} is a compact semigroup on X. Now, we are ready to prove the compactness of operator P defined by 4.1. Lemma 4.3. Assumptions [H1.1], [H2.1], [H2.2], [H2.4], [H2.5], and [H3] hold. Then the operator P is a compact operator. Proof. We only need to verify that P takes a bounded set into a precompact set in X. Let Γ be a bounded subset of X. Define K P Γ {P x ∈ X | x ∈ Γ}. For 0 < ε ≤ T0 , define Kε Pε Γ S T0 , T0 − ε x T0 − ε, x | x ∈ Γ . 4.10 14 Abstract and Applied Analysis Next, we show that Kε is precompact in X. In fact, for x ∈ Γ fixed, we have x T0 − ε, x ≤ S T0 − ε, 0 x 0 T0 −ε θ S T0 − ε, θ f θ, xθ, x, gθ, s, xs, xds dθ 0≤τk <T0 −ε 0 S T0 − ε, τ ck k ≤ MT0 x MT0 Mf T0 1 Mg T0 MT0 Mf ck MT Mf Mg T0 0 MT0 T0 0 0≤τk <T0 T0 4.11 xθ, xdθ 0 xθ,x dθ B ck . ≤ MT0 x MT0 Mf T0 1 Mg T0 1 Mg T0 MT0 Mf T0 ρ MT0 0≤τk <T0 This implies that the set {xT0 − ε, x | x ∈ Γ} is totally bounded. By virtue of the compactness of {T t, t > 0} and property 5 of Lemma 2.3, ST0 , T0 − ε is a compact operator. Thus, Kε is precompact in X. On the other hand, for arbitrary x ∈ Γ, T0 −ε Pε x S T0 , 0 x 0≤τk <T0 −ε S θ S T0 , θ f θ, xθ, x, gθ, s, xs, xds dθ 0 T0 , τk 0 4.12 ck . Thus, combined with 4.1, we have Pε x − P x θ T0 −ε ≤ S T , θ f θ, xθ, x, gθ, s, xs, xds dθ 0 0 − T0 0 0 θ S T0 , θ f θ, xθ, x, gθ, s, xs, xds dθ 0 S T0 , τk ck − S T0 , τk ck 0≤τ <T −ε 0≤τ <T k ≤ T0 T0 −ε 0 k 4.13 0 θ S T0 , θ f θ, xθ, x, gθ, s, xs, xds dθ MT 0 0 ≤ MT0 Mf 1 Mg T0 1 ρε MT0 T0 −ε≤τk <T0 ck . T0 −ε≤τk <T0 ck JinRong Wang et al. 15 It is showing that the set K can be approximated to an arbitrary degree of accuracy by a precompact set Kε . Hence K itself is a precompact set in X, that is, P takes a bounded set into a precompact set in X. As a result, P is a compact operator. After showing the continuity and compactness of operator P , we can follow and derive periodic P C-mild solutions for system 3.15. In the sequel, we define the following definitions. The following definitions are standard, we state them here for convenient references. Note that the uniform boundedness and uniform ultimate boundedness are not required to obtain the periodic P C-mild solutions here, so we only define the locally boundedness and ultimate boundedness. Definition 4.4. One says that P C-mild solutions of Cauchy problem 3.16 are bounded if for each B1 > 0, there is a B2 > 0 such that x ≤ B1 implies xt, x ≤ B2 for t ≥ 0. Definition 4.5. One says that P C-mild solutions of Cauchy problem 3.16 are locally bounded if for each B1 > 0 and k0 > 0, there is a B2 > 0 such that x ≤ B1 implies xt, x ≤ B2 for 0 ≤ t ≤ k0 . Definition 4.6. One says that P C-mild solutions of Cauchy problem 3.16 are ultimate bounded if there is a bound B > 0 such that for each B3 > 0, there is a k > 0, such that x ≤ B3 and t ≥ k imply xt, x ≤ B. We also need the following results as a reference. Lemma 4.7 see 21, Theorem 3.1. Local boundedness and ultimate boundedness imply boundedness and ultimate boundedness. Lemma 4.8 Horn’s fixed point theorem 20, Lemma 3.1. Let E0 ⊂ E1 ⊂ E2 be convex subsets of Banach space X, with E0 and E2 compact subsets and E1 open relative to E2 . Let P : E2 → X be a continuous map such that for some integer m, one has P j E1 ⊂ E2 , 1 ≤ j ≤ m − 1, P j E1 ⊂ E0 , m ≤ j ≤ 2m − 1, 4.14 then P has a fixed point in E0 . With these preparations, we can prove our main result in this paper. Theorem 4.9. Let assumptions [H1], [H2], and [H3] hold. If the P C-mild solutions of Cauchy problem 3.16 are ultimate bounded, then system 3.15 has a T0 -periodic P C-mild solution. Proof. By Theorem 3.5, 4.4 in Lemma 4.2, and Definition 4.5, the Cauchy problem 3.16 corresponding to the initial value x0 x has a P C-mild solution x·, x which is locally bounded. From ultimate boundedness and Lemma 4.7, x·, x is bounded. Next, let B > 0 be the bound in the definition of ultimate boundedness. Then by boundedness, there is a B1 > B such that x ≤ B implies xt, x ≤ B1 for t ≥ 0. Furthermore, there is a B2 > B1 such that x ≤ B1 implies xt, x ≤ B2 for t ≥ 0. Now, using ultimate boundedness again, there is a positive integer m such that x ≤ B1 implies xt, x ≤ B for t ≥ m − 2T0 . 16 Abstract and Applied Analysis Define y·, y0 x· T0 , x, then y0 xT0 , x P x. From 4.2 in Lemma 4.1, we obtain P y0 yT0 , y0 x2T0 , x. Thus, P 2 x P P x P y0 x2T0 , x. Suppose there exists integer m − 1 such that P m−1 x xm − 1T0 , x. By induction we arrive at P m x P m−1 P x P m−1 y0 ym − 1T0 , y0 x mT0 , x . 4.15 Thus, we obtain j−1 P x xj − 1T0 , x < B2 , j 1, 2, . . . , m − 1, x < B1 ; j−1 P x xj − 1T0 , x < B, j ≥ m, x < B1 . 4.16 It comes from Lemma 4.3 that P x xT0 , x on X is compact. Now let H x ∈ X : x < B2 , E2 cl.convP H, W x ∈ X : x < B1 , E1 W ∩ E2 , G x ∈ X : x < B , E0 cl.convP G, 4.17 where convY is the convex hull of the set Y defined by convY { ni1 λi yi | n ≥ 1, yi ∈ n Y, λi ≥ 0, i1 λi 1}, and cl. denotes the closure. Then we see that E0 ⊂ E1 ⊂ E2 are convex subsets of X with E0 , E2 compact subsets and E1 open relative to E2 , and from 4.16 one has P j E1 ⊂ P j W P P j−1 W ⊂ P H ⊂ E2 , P E1 ⊂ P W P P j j j−1 W ⊂ P G ⊂ E0 , j 1, 2, . . . , m − 1; j m, m 1, . . . , 2m − 1. 4.18 We see that P : E2 → X is a continuous map continuous from Lemma 4.2. Consequently, from Horn’s fixed point theorem, we know that the operator P has a fixed point x0 ∈ E0 ⊂ X. By Lemma 4.1, we know that the P C-mild solution x·, x0 of the Cauchy problem 3.16 corresponding to the initial value x0 x0 is just T0 -periodic. Therefore, x·, x0 is a T0 periodic P C-mild solution of system 3.15. This proves the theorem. At last, an example is given to illustrate our theory. Consider the following problem: ∂ xt, y Δxt, y xt, y ∂t y ∈ Ω, t 1 sint − s 3x2 s, y 2ds, 0 t ≥ s, t, s ∈ 0, 2π \ 3 1 π, π, π , 2 2 JinRong Wang et al. 17 ⎧ ⎪ ⎪ ⎨0.05Ixτi , y, − Δxτi , y xτi , y − xτi , y −0.05Ixτi , y, ⎪ ⎪ ⎩0.05Ixτ , y, i xt, y|y∈∂Ω 0, i 1, i i 2, y ∈ Ω, τi π, i 1, 2, 3, 2 i 3, t > 0, x0, y x2π, y, 4.19 where Ω ⊂ R3 is a bounded domain and ∂Ω ∈ C3 . Define X L2 Ω, DA H 2 Ω ∩ H01 Ω, and Ax −∂2 x/∂y12 ∂2 x/∂y22 ∂2 x/∂y32 for x ∈ DA. Then, A generates a compact semigroup {T t, t ≥ 0} on L2 Ω. Define t · x·y x·, y, sin·y sin·, y, f·, x·, 0 g·, s, xdsy x·y 0 1 sin· − s 3x2 · 2dsy, and ⎧ ⎪ ⎪ ⎪0.05I, ⎨ Bi −0.05I, ⎪ ⎪ ⎪ ⎩0.05I, i 1, i 2, 4.20 i 3. Thus problem 4.19 can be rewritten as t 3 1 π, π, π , gt, s, xds , t ≥ s, t, s ∈ 0, 2π \ 2 2 0 i i π Bi x π , i 1, 2, 3, Δx 2 2 ẋt Axt f t, x, 4.21 x0 x2π. If the P C-mild solutions of Cauchy problem 4.21 are ultimate bounded, then all the assumptions in Theorem 4.9 are met, and our results can be used to system 4.19, that is, problem 4.19 has a 2π-periodic P C-mild solution x2π ·, y ∈ P C2π 0 ∞; L2 Ω, where P C2π 0, ∞; L2 Ω ≡ {x ∈ P C0, ∞; L2 Ω | xt xt 2π, t ≥ 0}. 4.22 Acknowledgments This work is supported by Natural Science Foundation of Guizhou Province Education Department no. 2007008 and Guizhou Province no. 20052001. This work is also supported by the undergraduate carve out project of Department of Guiyang Science and Technology 2008 no. 15-2. References 1 D. Baı̆nov and P. Simeonov, Impulsive Differential Equations: Periodic Solutions and Applications, vol. 66 of Pitman Monographs and Surveys in Pure and Applied Mathematics, Longman Scientific & Technical, Harlow, UK, 1993. 18 Abstract and Applied Analysis 2 V. Lakshmikantham, D. D. Baı̆nov, and P. S. 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