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Hindawi Publishing Corporation Advances in Difference Equations Volume 2011, Article ID 483816, 17 pages doi:10.1155/2011/483816 ResearchArticleNonlocalCauchyProblemforNonautonomousFractionalEvolutionEquationsFei Xiao Department of Mathematics, University of Science and Technology of China, Hefei, Anhui 230026, China Correspondence should be addressed to Fei Xiao, sheaf@mail.ustc.edu.cn Received 28 November 2010; Accepted 29 January 2011 Academic Editor: Toka Diagana Copyright q 2011 Fei Xiao. 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 investigate the mild solutions of a nonlocalCauchyproblemfornonautonomousfractionalevolutionequations d q ut/dt q −Atutft, K 1 ut, K 2 ut, ,K n ut,t∈ I 0,T, u0A −1 0guu 0 , in Banach spaces, where T>0, 0 <q<1. New results are obtained by using Sadovskii’s fixed point theorem and the Banach contraction mapping principle. An example is also given. 1. Introduction During the past decades, the fractional differential equations have been proved to be valuable tools in the investigation of many phenomena in engineering and physics; they attracted many researchers cf., e.g., 1–9. On the other hand, the autonomous and nonautonomousevolutionequations and related topics were studied in, for example, 6, 7, 10–20,andthe nonlocal C auchy problem was considered in, for example, 2, 5, 18, 21–26. In this paper, we consider the following nonlocalCauchyproblemfornonautonomousfractionalevolutionequations d q u t dt q −A t u t f t, K 1 u t , K 2 u t , , K n u t ,t∈ I 0,T , u 0 A −1 0 g u u 0 , 1.1 in Banach spaces, where 0 <q<1, g : CI; X → X.ThetermsK i ut, i 1, ,n are 2AdvancesinDifference Equations defined by K i u t t 0 k i t, s u s ds, 1.2 the positive functions k i t, s are continuous on D {t, s ∈ R 2 :0≤ s ≤ t ≤ T} and K ∗ i sup t∈0,T t 0 k i t, s ds < ∞. 1.3 Let us assume that u ∈ L0,T; X and At is a family linear closed operator defined in a Banach space X. The fractional order integral of the function u is understood here in the Riemann-Liouville sense, that is, I q u t 1 Γ q t 0 t − s q−1 u s ds. 1.4 In this paper, we denote that C is a positive constant and assume that a family of closed linear {At : t ∈ 0,T} satisfying A1 the domain DA of {At : t ∈ 0 ,T} is dense in the Banach space X and in- dependent of t, A2 the operator Atλ −1 exists in LX for any λ with Re λ ≤ 0and A t λ −1 ≤ C | λ 1 | ,t∈ 0,T . 1.5 A3 There exists constant γ ∈ 0, 1 and C such that A t 1 − A t 2 A −1 s ≤ C | t 1 − t 2 | γ ,t 1 ,t 2 ,s∈ 0,T . 1.6 Under condition A2,eachoperator−As, s ∈ 0,T generates an analytic semigroup exp−tAs, t>0, and there exists a constant C such that A n s exp −tA s ≤ C t n , 1.7 where n 0, 1, t>0, s ∈ 0,T11. We study the existence of mild solution of 1.1 and obtain the existence theorem based on the measures of noncompactness. An example is given to show an application of the abstract results. Advances in Difference Equations 3 2. Preliminaries Throughout this work, we set I 0,T.WedenotebyX a Banach space, LX the space of all linear and bounded operators on X,andCI, X the space of all X-valued continuous functions on I. Lemma 2.1 see 9. 1 I q : L 1 0,T → L 1 0,T. 2 For g ∈ L 1 0,T,wehave t 0 η 0 t − η q−1 η − s γ−1 g s ds dη B q, γ t 0 t − s qγ−1 g s ds, 2.1 where Bq, γ is a Beta function. Definition 2.2. Let B be a bounded set of seminormed linear space Y. The Kuratowski’s measure of noncompactness for brevity, α-measure of B is defined as α B inf d>0:B has a finite cover by sets of diameter ≤ d . 2.2 From the definition, we can get some properties of α-measure immediately, see 27. Lemma 2.3 see 27. Let A and B be bounded sets of X.Then 1 αA ≤ αB,ifA ⊆ B. 2 αAαA cl ,whereA cl denotes the closure of A. 3 αA0 if and only if A is precompact. 4 αλA|λ|αA, λ ∈ R. 5 αA ∪ Bmax{αA,αB}. 6 αA B ≤ αAαB,whereA B {x y : x ∈ A, y ∈ B}. 7 αA x 0 αA, for any x 0 ∈ X. For H ⊂ CI, X we define t 0 H s ds t 0 u s ds : u ∈ H , 2.3 for t ∈ I,whereHs{us ∈ X : u ∈ H}. The following lemma will be needed. Lemma 2.4 see 27. If H ⊂ CI,X is a bounded, equicontinuous set, then 1 αHsup t∈I αHt. 2 α t 0 Hsds ≤ t 0 αHsds,fort ∈ I. 4AdvancesinDifference Equations Lemma 2.5 see 28. If {u n } ∞ n1 ⊂ L 1 I, X and there exists a m· ∈ L 1 I, R such that u n t ≤ m t , a.e t ∈ I, 2.4 then α{u n t} ∞ n1 is integrable and α t 0 u n s ds ∞ n1 ≤ 2 t 0 α { u n s } ∞ n1 ds. 2.5 We need to use the following Sadovskii’s fixed point theorem. Definition 2.6 see 29.LetP be an operator in Banach space X.IfP is continuous and takes bounded, sets into bounded sets, and αPH <αH for every bounded set H of X with αH > 0, then P is said to be a condensing operator on X. Lemma 2.7 Sadovskii’s fixed point theorem 29. Let P be a condensing o perator on Banach space X.IfP B ⊆ B for a convex, closed, and bounded set B of X,thenP has a fixed point in B. According to 4, a mild solution of 1.1 can be defined as follows. Definition 2.8. Afunctionu ∈ CI, X satisfying the equation u t A −1 0 g u u 0 t 0 ψ t − η, η U η A 0 A −1 0 g u u 0 dη t 0 ψ t − η, η f η, K 1 u η , K 2 u η , , K n u η dη t 0 η 0 ψ t − η, η ϕ η, s f s, K 1 u s , K 2 u s , , K n u s ds dη, 2.6 is called a mild solution of 1.1,where ψ t, s q ∞ 0 θt q−1 ξ q θ exp −t q θA s dθ, 2.7 and ξ q is a probability density function defined on 0, ∞ such that its Laplace transform is given by ∞ 0 e −σx ξ q σ dσ ∞ j0 −x j Γ 1 qj ,q∈ 0, 1 ,x>0, ϕ t, τ ∞ k1 ϕ k t, τ , 2.8 Advances in Difference Equations 5 where ϕ 1 t, τ A t − A τ ψ t − τ, τ , ϕ k1 t, τ t τ ϕ k t, s ϕ 1 s, τ ds, k 1, 2 , U t −A t A −1 0 − t 0 ϕ t, s A s A −1 0 ds. 2.9 To our purpose, the following conclusions will be needed. For the proofs refer to 4. Lemma 2.9 see 4. The operator-valued functions ψt − η, η and Atψt − η, η are continuous in uniform topology in the variables t, η,where0 ≤ η ≤ t − ε, 0 ≤ t ≤ T, for any ε>0. Clearly, ψ t − η, η ≤ C t − η q−1 . 2.10 Moreover, we have ϕ t, η ≤ C t − η γ−1 . 2.11 Remark 2.10. From the proof of Theorem 2.5 in 4,wecansee 1 Ut≤C Ct γ . 2 For t ∈ I, t 0 ψt − η, ηUηdη is uniformly continuous in the norm of LX and t 0 ψ t − η, η U η dη ≤ C 2 t q 1 q t γ B q, γ 1 : M t . 2.12 3. Existence of Solution Assume that B1 f : I × X × X ×···×X → X satisfies f·,v 1 ,v 2 , ,v n : I → X is measurable for all v i ∈ X, i 1, 2, ,n and ft, ·, ·, ,· : X × X ×···×X → X is continuous for a.e t ∈ I, and there exist a positive function μ· ∈ L p I, R p>1/q > 1 and a continuous nondecreasing function ω : 0 , ∞ → 0, ∞ such that f t, v 1 ,v 2 , ,v n ≤ μ t ω n i1 v i , t, v 1 ,v 2 , ,v n ∈ I × X × X ×···×X, 3.1 and set T p,q max{T q−1/p ,T q }. 6AdvancesinDifference Equations B2 For any bounded sets D, D 1 ,D 2 , ,D n ⊂ X,and0≤ τ ≤ s ≤ t ≤ T, α g D ≤ β t α D , α ψ t − s, s f s, D 1 ,D 2 , ,D n ≤ β 1 t, s α D 1 β 2 t, s α D 2 ··· β n t, s α D n , α ψ t − s, s ϕ s, τ f τ, D 1 ,D 2 , ,D n ≤ ζ 1 t, s, τ α D 1 ζ 2 t, s, τ α D 2 ··· ζ n t, s, τ α D n , 3.2 where βt is a nonnegative function, and sup t∈I βt : β<∞, sup t∈I t 0 β i t, s ds : β i < ∞,i 1, 2, ,n, sup t∈I t 0 s 0 ζ j t, s, τ dτ ds : ζ j < ∞,j 1, 2, ,n. 3.3 B3 g : CI; X → X is continuous and there exists 0 <α 1 < C M T −1 ,α 2 ≥ 0 3.4 such that g u ≤ α 1 u α 2 . 3.5 B4 The functions μ and ω satisfy the following c ondition: C 1 CB q, γ T γ p,q Ω p,q n i1 K ∗ i μ L p lim inf τ →∞ ω τ τ < 1 − α 1 C M T , 3.6 where Ω p,q p − 1/pq − 1 p−1/p ,andT γ p,q max{T p,q ,T p,qγ }. Theorem 3.1. Suppose that (B1)–(B4) are satisfied, and if C MTβ 4Σ n i1 β i 2ζ i K ∗ i < 1, then 1.1 has a mild solution on 0,T. Advances in Difference Equations 7 Proof. Define the operator F : CI; X → CI; X by F u t A −1 0 g u u 0 t 0 ψ t − η, η U η A 0 A −1 0 g u u 0 dη t 0 ψ t − η, η f η, K 1 u η , K 2 u η , , K n u η dη t 0 η 0 ψ t − η, η ϕ η, s f s, K 1 u s , K 2 u s , , K n u s ds dη, t ∈ I. 3.7 Then we proceed in five steps. Step 1. We show that F is continuous. Let u i be a sequence that u i → u as i →∞.Sincef satisfies B1,wehave f t, K 1 u i t , K 2 u i t , , K n u i t −→ f t, K 1 u t , K 2 u t , , K n u t , as i −→ ∞ . 3.8 Then F u i t − F u t ≤ A −1 0 g u i − g u t 0 ψ t − η, η U η g u i − g u dη t 0 ψ t − η, η f η, K 1 u i η , K 2 u i η , , K n u i η −f η, K 1 u η , K 2 u η , , K n u η dη t 0 η 0 ψ t − η, η ϕ η, s f s, K 1 u i s , K 2 u i s , , K n u i s −f s, K 1 u s , K 2 u s , , K n u s ds dη. 3.9 According to the condition A2, 2.12, and the continuity of g,wehave A −1 0 g u i − g u −→ 0, as i −→ ∞ ; t 0 ψ t − η, η U η g u i − g u dη −→ 0, as i −→ ∞ . 3.10 8AdvancesinDifference Equations Noting that u i → u in CI,X,thereexistsε>0suchthatu i − u≤ε for i sufficiently large. Therefore, we have f t, K 1 u i t , K 2 u i t , , K n u i t − f t, K 1 u t , K 2 u t , , K n u t ≤ μ t ⎡ ⎣ ω ⎛ ⎝ n j1 K j u i t ⎞ ⎠ ω n j1 K j u t ⎤ ⎦ ≤ μ t ⎡ ⎣ ω ⎛ ⎝ n j1 K ∗ j u ε ⎞ ⎠ ω ⎛ ⎝ n j1 K ∗ j u ⎞ ⎠ ⎤ ⎦ . 3.11 Using 2.10 and by means of the Lebesgue dominated convergence theorem, we obtain t 0 ψ t − η, η f η, K 1 u i η , K 2 u i η , , K n u i η −f η, K 1 u η , K 2 u η , , K n u η dη ≤ C t 0 t − η q−1 f η, K 1 u i η , K 2 u i η , , K n u i η −f η, K 1 u η , K 2 u η , , K n u η dη, −→ 0, as i −→ ∞ . 3.12 Similarly, by 2.10 and 2.11,wehave t 0 η 0 ψ t − η, η ϕ η, s × f s, K 1 u i t , K 2 u i t , , K n u i t −f s, K 1 u s , K 2 u s , , K n u s ds dη ≤ C 2 t 0 η 0 t − η q−1 η − s γ−1 × f s, K 1 u i t , K 2 u i t , , K n u i t −f s, K 1 u s , K 2 u s , , K n u s ds dη −→ 0, as i −→ ∞ . 3.13 Therefore, we deduce that lim i →∞ F u i − F u 0. 3.14 Advances in Difference Equations 9 Step 2. We show that F maps bounded sets of CI, X into bounded sets in CI, X. For any r>0, we set B r {u ∈ CI, X : u≤r}. Now, for u ∈ B r ,byB1,wecansee f t, K 1 u t , K 2 u t , , K n u t ≤ μ t ω ⎛ ⎝ n j1 K ∗ j r ⎞ ⎠ . 3.15 Based on 2.12,wedenotethatSt : t 0 ψt − η, ηUηdη,wehave S t A 0 u 0 ≤ C 2 t q 1 q t γ B q, γ 1 A 0 u 0 M t A 0 u 0 . 3.16 Then for any u ∈ B r ,byA2, 2.10, 2.11,andLemma 2.1,wehave Fu t ≤ A −1 0 g u u 0 S t g u S t A 0 u 0 t 0 ψ t − η, η f η, K 1 u η , K 2 u η , , K n u η dη t 0 η 0 ψ t − η, η ϕ η, s f s, K 1 u s , K 2 u s , , K n u s ds dη ≤ C Mt g u u 0 Mt A 0 u 0 C t 0 t − η q−1 μ η ω ⎛ ⎝ n j1 K ∗ j r ⎞ ⎠ dη C 2 t 0 η 0 t − η q−1 η − s γ−1 μ s ω ⎛ ⎝ n j1 K ∗ j r ⎞ ⎠ ds dη ≤ α 1 C Mt u α 2 C M t u 0 Mt A 0 u 0 M 1 C t 0 t − η q−1 μ η dη C 2 B q, γ t 0 t − η qγ−1 μ η dη , 3.17 where M 1 ω n j1 K ∗ j r. By means of the H ¨ older inequality, we have t 0 t − η q−1 μ η dη t pq−1/p M p,q μ L p ≤ T p,q Ω p,q μ L p , t 0 t − η γq−1 μ η dη ≤ T p,qγ Ω p,qγ μ L p . 3.18 10 Advances in Difference Equations Thus Fu t ≤ α 1 C M T r α 2 C M T u 0 M T A 0 u 0 M 1 Ω p,q T γ p,q C C 2 B q, γ μ L p : r. 3.19 This means FB r ⊂ B r . Step 3. We show that there exists m ∈ N such that FB m ⊂ B m . Suppose the contrary, that for every m ∈ N,thereexistsu m ∈ B m and t m ∈ I,suchthat Fu m t m >m. However, on the other hand f t, K 1 u m t , K 2 u m t , , K n u m t ≤ μ t ω ⎛ ⎝ n j1 K ∗ j m ⎞ ⎠ , 3.20 we have m< Fu m t m ≤ α 1 C M T u m α 2 C M T u 0 M T A 0 u 0 M 1 C t m 0 t m − η q−1 μ η dη C 2 B q, γ t m 0 t m − η qγ−1 μ η dη ≤ α 1 C M T u m α 2 C M T u 0 M T A 0 u 0 M 1 Ω p,q T γ p,q C C 2 B q, γ μ L p ≤ α 1 C M T m α 2 C M T u 0 M T A 0 u 0 M 1 Ω p,q T γ p,q C C 2 B q, γ μ L p . 3.21 Dividing both sides by m and taking the lower limit as m →∞,weobtain C 1 CB q, γ T γ p,q Ω p,q n j1 K ∗ j μ L p lim inf m →∞ w m m ≥ 1 − α 1 C M T 3.22 which contradicts B4. Step 4. 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We investigate the mild solutions of a nonlocal Cauchy problem for nonautonomous fractional evolution equations d q ut/dt q −Atutft, K 1 ut, K 2 ut,. example, 2, 5, 18, 21–26. In this paper, we consider the following nonlocal Cauchy problem for nonautonomous fractional evolution equations d q u t dt q −A t u t f t, K 1 u t , K 2 u t ,