Hindawi Publishing Corporation Advances in Difference Equations Volume 2011, Article ID 483816, 17 pages doi:10.1155/2011/483816 Research Article Nonlocal Cauchy Problem for Nonautonomous Fractional Evolution Equations Fei 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 nonlocal Cauchy problem for nonautonomous fractional evolution equations dq ut/dtq −Atut f t, K1 ut, K2 ut, . . . , Kn ut, t ∈ I 0, T, u0 A−1 0gu u0 , 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 nonautonomous evolution equations and related topics were studied in, for example, 6, 7, 10–20, and the nonlocal Cauchy problem was considered in, for example, 2, 5, 18, 21–26. In this paper, we consider the following nonlocal Cauchy problem for nonautonomous fractional evolution equations dq ut −Atut ft, K1 ut, K2 ut, . . . , Kn ut, dtq t ∈ I 0, T, 1.1 −1 u0 A 0gu u0 , in Banach spaces, where 0 < q < 1, g : CI; X → X. The terms Ki ut, i 1, . . . , n are 2 Advances in Difference Equations defined by t Ki ut ki t, susds, 1.2 0 the positive functions ki t, s are continuous on D {t, s ∈ R2 : 0 ≤ s ≤ t ≤ T} and Ki∗ sup t t∈0,T ki t, sds < ∞. 1.3 0 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, 1 I ut Γ q t q t − sq−1 usds. 1.4 0 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 independent of t, A2 the operator At λ−1 exists in LX for any λ with Re λ ≤ 0 and At λ−1 ≤ C , |λ 1| t ∈ 0, T. 1.5 A3 There exists constant γ ∈ 0, 1 and C such that At1 − At2 A−1 s ≤ C|t1 − t2 |γ , t1 , t2 , s ∈ 0, T. 1.6 Under condition A2, each operator −As, s ∈ 0, T generates an analytic semigroup exp−tAs, t > 0, and there exists a constant C such that n A s exp−tAs ≤ C , tn 1.7 where n 0, 1, t > 0, s ∈ 0, T 11. 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. We denote by X a Banach space, LX the space of all linear and bounded operators on X, and CI, X the space of all X-valued continuous functions on I. Lemma 2.1 see 9. 1 I q : L1 0, T → L1 0, T. 2 For g ∈ L1 0, T, we have t η 0 q−1 γ −1 t−η η−s gsds dη B q, γ t 0 t − sqγ −1 gsds, 2.1 0 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 αB 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, if A ⊆ B. 2 αA αAcl , where Acl denotes the closure of A. 3 αA 0 if and only if A is precompact. 4 αλA |λ|αA, λ ∈ R. 5 αA ∪ B max{αA, αB}. 6 αA B ≤ αA αB, where A B {x y : x ∈ A, y ∈ B}. 7 αA x0 αA, for any x0 ∈ X. For H ⊂ CI, X we define t Hsds t 0 usds : u ∈ H , 0 for t ∈ I, where Hs {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 αH supt∈I αHt. t t 2 α 0 Hsds ≤ 0 αHsds, for t ∈ I. 2.3 4 Advances in Difference Equations 1 1 Lemma 2.5 see 28. If {un }∞ n1 ⊂ L I, X and there exists a m· ∈ L I, R such that un t ≤ mt, a.e t ∈ I, 2.4 then α{un t}∞ n1 is integrable and t α ∞ ≤2 un sds 0 t 0 n1 α{un s}∞ n1 ds. 2.5 We need to use the following Sadovskii’s fixed point theorem. Definition 2.6 see 29. Let P be an operator in Banach space X. If P is continuous and takes bounded, sets into bounded sets, and αP H < 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 operator on Banach space X. If P B ⊆ B for a convex, closed, and bounded set B of X, then P has a fixed point in B. According to 4, a mild solution of 1.1 can be defined as follows. Definition 2.8. A function u ∈ CI, X satisfying the equation ut A−1 0gu u0 t ψ t − η, η U η A0 A−1 0gu u0 dη 0 t ψ t − η, η f η, K1 u η , K2 u η , . . . , Kn u η dη 0 t η 0 2.6 ψ t − η, η ϕ η, s fs, K1 us, K2 us, . . . , Kn usds dη, 0 is called a mild solution of 1.1, where ψt, s q ∞ θtq−1 ξq θ exp−tq θAsdθ, 2.7 0 and ξq is a probability density function defined on 0, ∞ such that its Laplace transform is given by ∞ 0 e−σx ξq σdσ ∞ −xj , j0 Γ 1 qj ϕt, τ ∞ k1 q ∈ 0, 1, x > 0, ϕk t, τ, 2.8 Advances in Difference Equations 5 where ϕ1 t, τ At − Aτψt − τ, τ, ϕk1 t, τ t ϕk t, sϕ1 s, τds, k 1, 2 . . . , τ −1 Ut −AtA 0 − t 2.9 ϕt, sAsA−1 0ds. 0 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, where 0 ≤ η ≤ t − ε, 0 ≤ t ≤ T, for any ε > 0. Clearly, ψ t − η, η ≤ C t − η q−1 . 2.10 ϕ t, η ≤ C t − η γ −1 . 2.11 Moreover, we have Remark 2.10. From the proof of Theorem 2.5 in 4, we can see 1 Ut ≤ C Ctγ . t 2 For t ∈ I, 0 ψt − η, ηUηdη is uniformly continuous in the norm of LX and t 1 tγ B q, γ 1 : Mt. ψ t − η, η U η dη ≤ C2 tq 0 q 2.12 3. Existence of Solution Assume that B1 f : I × X × X × · · · × X → X satisfies f·, v1 , v2 , . . . , vn : I → X is measurable for all vi ∈ 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· ∈ Lp I, R p > 1/q > 1 and a continuous nondecreasing function ω : 0, ∞ → 0, ∞ such that n ft, v1 , v2 , . . . , vn ≤ μtω vi , i1 and set Tp,q max{T q−1/p , T q }. t, v1 , v2 , . . . , vn ∈ I × X × X × · · · × X, 3.1 6 Advances in Difference Equations B2 For any bounded sets D, D1 , D2 , . . . , Dn ⊂ X, and 0 ≤ τ ≤ s ≤ t ≤ T, α gD ≤ βtαD, α ψt − s, sfs, D1 , D2 , . . . , Dn ≤ β1 t, sαD1 β2 t, sαD2 · · · βn t, sαDn , 3.2 α ψt − s, sϕs, τfτ, D1 , D2 , . . . , Dn ≤ ζ1 t, s, ταD1 ζ2 t, s, ταD2 · · · ζn t, s, ταDn , where βt is a nonnegative function, and supt∈I βt : β < ∞, t sup t s sup t∈I 0 βi t, sds : βi < ∞, i 1, 2, . . . , n, 0 t∈I 3.3 ζj t, s, τdτ ds : ζj < ∞, j 1, 2, . . . , n. 0 B3 g : CI; X → X is continuous and there exists −1 0 < α1 < C MT , α2 ≥ 0 3.4 such that gu ≤ α1 u α2 . 3.5 B4 The functions μ and ω satisfy the following condition: n γ ωτ ∗ C 1 CB q, γ Tp,q Ωp,q Ki μ Lp lim inf < 1 − α1 C MT , τ →∞ τ i1 3.6 where Ωp,q p − 1/pq − 1p−1/p , and Tp,q max{Tp,q , Tp,qγ }. γ Theorem 3.1. Suppose that (B1)–(B4) are satisfied, and if C MTβ 4Σni1 βi 2ζi Ki∗ < 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 −1 Fut A 0gu u0 t ψ t − η, η U η A0 A−1 0gu u0 dη 0 t ψ t − η, η f η, K1 u η , K2 u η , . . . , Kn u η dη 0 t η 0 ψ t − η, η ϕ η, s fs, K1 us, K2 us, . . . , Kn usds dη, t ∈ I. 0 3.7 Then we proceed in five steps. Step 1. We show that F is continuous. Let ui be a sequence that ui → u as i → ∞. Since f satisfies B1, we have ft, K1 ui t, K2 ui t, . . . , Kn ui t −→ ft, K1 ut, K2 ut, . . . , Kn ut, as i −→ ∞. 3.8 Then Fui t − Fut t −1 ≤ A 0 gui − gu ψ t − η, η U η gui − gudη 0 t ψ t − η, η f η, K1 ui η , K2 ui η , . . . , Kn ui η 0 −f η, K1 u η , K2 u η , . . . , Kn u η dη t η 0 3.9 ψ t − η, η ϕ η, s fs, K1 ui s, K2 ui s, . . . , Kn ui s 0 −fs, K1 us, K2 us, . . . , Kn us ds dη. According to the condition A2, 2.12, and the continuity of g, we have −1 A 0gui − gu −→ 0, t 0 as i −→ ∞; ψ t − η, η U η gui − gudη −→ 0, 3.10 as i −→ ∞. 8 Advances in Difference Equations Noting that ui → u in CI, X, there exists ε > 0 such that ui − u ≤ ε for i sufficiently large. Therefore, we have ft, K1 ui t, K2 ui t, . . . , Kn ui t − ft, K1 ut, K2 ut, . . . , Kn ut ⎡ ⎛ ⎤ ⎞ n n ≤ μt⎣ω⎝ Kj ui t⎠ ω Kj u t⎦ j1 j1 3.11 ⎡ ⎛ ⎞ ⎛ ⎞⎤ n n ≤ μt⎣ω⎝ Kj∗ u ε⎠ ω⎝ Kj∗ u ⎠⎦. j1 j1 Using 2.10 and by means of the Lebesgue dominated convergence theorem, we obtain t ψ t − η, η f η, K1 ui η , K2 ui η , . . . , Kn ui η 0 −f η, K1 u η , K2 u η , . . . , Kn u η dη ≤C t q−1 f η, K1 ui η , K2 ui η , . . . , Kn ui η t−η 3.12 0 −f η, K1 u η , K2 u η , . . . , Kn u η dη, −→ 0, as i −→ ∞. Similarly, by 2.10 and 2.11, we have t η 0 0 ψ t − η, η ϕ η, s × fs, K1 ui t, K2 ui t, . . . , Kn ui t −fs, K1 us, K2 us, . . . , Kn us ds dη t η q−1 γ −1 2 t−η η−s ≤C 0 3.13 0 × fs, K1 ui t, K2 ui t, . . . , Kn ui t −fs, K1 us, K2 us, . . . , Kn usds dη −→ 0, as i −→ ∞. Therefore, we deduce that lim Fui − Fu 0. i→∞ 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 Br {u ∈ CI, X : u ≤ r}. Now, for u ∈ Br , by B1, we can see ⎛ ⎞ n ∗ ft, K1 ut, K2 ut, . . . , Kn ut ≤ μtω⎝ K r ⎠. j 3.15 j1 Based on 2.12, we denote that St : StA0u0 ≤ C t 2 q t 0 ψt − η, ηUηdη, we have 1 γ t B q, γ 1 A0u0 Mt A0u0 . q 3.16 Then for any u ∈ Br , by A2, 2.10, 2.11, and Lemma 2.1, we have Fut ≤ A−1 0gu u0 Stgu StA0u0 t ψ t − η, η f η, K1 u η , K2 u η , . . . , Kn u η dη 0 t η 0 ψ t − η, η ϕ η, s fs, K1 us, K2 us, . . . , Kn usds dη 0 ≤ C Mt gu u0 Mt A0u0 C t 0 C ⎛ ⎞ n q−1 ∗ t−η μ η ω⎝ Kj r ⎠dη j1 t η 2 0 0 ⎛ ⎞ n q−1 γ −1 ∗ μsω⎝ Kj r ⎠ds dη t−η η−s j1 ≤ α1 C Mt u α2 C Mt u0 Mt A0u0 t q−1 qγ −1 t 2 M1 C t−η t−η μ η dη C B q, γ μ η dη , 0 0 3.17 where M1 ω nj1 Kj∗ r. By means of the Hölder inequality, we have t 0 q−1 μ η dη tpq−1/p Mp,q μLp ≤ Tp,q Ωp,q μLp , t−η t 0 γ q−1 μ η dη ≤ Tp,qγ Ωp,qγ μLp . t−η 3.18 10 Advances in Difference Equations Thus Fut ≤ α1 C MT r α2 C MT u0 MT A0u0 γ M1 Ωp,q Tp,q C C2 B q, γ μLp : r!. 3.19 This means FBr ⊂ Br! . Step 3. We show that there exists m ∈ N such that FBm ⊂ Bm . Suppose the contrary, that for every m ∈ N, there exists um ∈ Bm and tm ∈ I, such that Fum tm > m. However, on the other hand ⎛ ⎞ n ft, K1 um t, K2 um t, . . . , Kn um t ≤ μtω⎝ K ∗ m⎠, j 3.20 j1 we have m < Fum tm ≤ α1 C MT um α2 C MT u0 t m q−1 tm qγ −1 2 tm − η tm − η MT A0u0 M1 C μ η dη C B q, γ μ η dη 0 0 ≤ α1 C MT um α2 C MT u0 γ MT A0u0 M1 Ωp,q Tp,q C C2 B q, γ μLp ≤ α1 C MT m α2 C MT u0 γ MT A0u0 M1 Ωp,q Tp,q C C2 B q, γ μLp . 3.21 Dividing both sides by m and taking the lower limit as m → ∞, we obtain n γ wm ≥ 1 − α1 C MT C 1 CB q, γ Tp,q Ωp,q Kj∗ μLp lim inf m→∞ m j1 3.22 which contradicts B4. Step 4. Denote −1 Fut A 0gu u0 t 0 ψ t − η, η U η A0 A−1 0gu u0 dη Gut, 3.23 Advances in Difference Equations 11 where Gut t ψ t − η, η f η, K1 u η , K2 u η , . . . , Kn u η dη 0 t η 0 ψ t − η, η ϕ η, s fs, K1 us, K2 us, . . . , Kn usds dη. 3.24 0 We show that Gu· is equicontinuous. Let 0 < t2 < t1 < T and u ∈ Bm . Then Gut1 − Gut2 ≤ I1 I2 I3 I4 , 3.25 where I1 t2 ψ t1 − η, η − ψ t2 − η, η f η, K1 u η , K2 u η , . . . , Kn u η dη, 0 I2 t1 ψ t1 − η, η f η, K1 u η , K2 u η , . . . , Kn u η dη, t2 I3 t2 η 0 0 I4 ψ t1 − η, η − ψ t2 − η, η ϕ η, s fs, K1 us, K2 us, . . . , Kn usds dη, t1 η ψ t1 − η, η ϕ η, s fs, K1 us, K2 us, . . . , Kn usds dη. 0 t2 3.26 It follows from Lemma 2.9, B1, and 3.20 that I1 , I3 → 0, as t2 → t1 . For I2 , from 2.10, 3.20, and B1, we have I2 t1 ψ t1 − η, η f η, K1 u η , K2 u η , . . . , Kn u η dη t2 ≤ CM1 t1 q−1 μ η dη −→ 0, t1 − η 3.27 as t2 −→ t1 . t2 Similarly, by 2.10, 2.11, B1, and Lemma 2.1, we have I4 t1 η t2 ψ t1 − η, η ϕ η, s fs, K1 us, K2 us, . . . , Kn usds dη 0 ≤ C2 M1 t1 t2 q−1 t1 − η η 0 γ −1 η−s μsds dη −→ 0, 3.28 as t2 −→ t1 . 12 Advances in Difference Equations Step 5. We show that αFH < αH for every bounded set H ⊂ Bm . For any ε > 0, we can take a sequence {hv }∞ v1 ⊂ H such that αH ≤ 2α{hv } ε, 3.29 cf. 30. So it follows from Lemmas 2.3–2.5, 2.9, 2 in Remark 2.10, and B2 that αFH ≤ Cα gH MTα gH 2αG{hv } ε ≤ Cα gH MTα gH t 2 sup α ψ t − η, η f η, K1 hv η , K2 hv η , . . . , Kn hv η dη 0 t∈I t η 0 ψ t − η, η ϕ η, s 0 ×fs, K1 hv s, K2 hv s, . . . , Kn hv sds dη ε ≤ CβαH MTβαH t dη 4 sup α ψ t − η, η f η, K1 hv η , K2 hv η , . . . , Kn hv η 0 t∈I t η 8 sup t∈I 0 α ψ t − η, η ϕ η, s fs, K1 hv s, K2 hv s, . . . , Kn hv s 0 t n ∗ βi t, η Ki α{hv }dη ε ≤ CβαH MTβαH 4 sup t∈I 0 i1 t η n ∗ ζi t, η, s Ki α{hv }ds dη ε 8 sup t∈I 0 0 i1 ≤ CβαH MTβαH C MT β 4 n n ∗ ∗ 4 βi Ki 8 ζi Ki α{hv } ε n i1 βi 2ζi Ki∗ i1 αH ε. i1 3.30 Since ε is arbitrary, we can obtain αFH ≤ C MT β 4 Σni1 βi 2ζi Ki∗ αH < αH. 3.31 Advances in Difference Equations 13 In summary, we have proven that F has a fixed point u ! ∈ Bm . Consequently, 1.1 has at least one mild solution. Our next result is based on the Banach’s fixed point theorem. G1 There exists a positive function l· ∈ L1 I, R and a constant μ > 0 such that gu − gu∗ ≤ μ u − u∗ , ft, v1 , v2 , . . . , vn − ft, w1 , w2 , . . . , wn n ≤ lt vi − wi , vi , wi ∈ X 2 , i 1, 2, . . . , n. 3.32 i1 G2 There exists a constant 0 < δ < 1 such that the function Λ : I → R defined by n n q ∗ 2 ∗ Λt μ C MT C Ki Γ q I lt C Ki Γ q Γ γ I qγ lt ≤ δ, i1 i1 t ∈ I. 3.33 Theorem 3.2. Assume that (G1), (G2) are satisfied, then 1.1 has a unique mild solution. Proof. Let F be defined as in Theorem 3.1. For any u, u∗ ∈ CI, X, we have ft, K1 ut, K2 ut, . . . , Kn ut − ft, K1 u∗ t, K2 u∗ t, . . . , Kn u∗ t n ∗ ≤ lt Ki ut − Ki u t i1 3.34 n ≤ lt Ki∗ u − u∗ . i1 Thus, from A2, 2.10, 2.11, Lemma 2.1, we have Fut − Fu∗ t t ≤ μC u − u∗ μ ψ t − η, η U η u − u∗ dη t 0 ψ t − η, η f η, K1 u η , K2 u η , . . . , Kn u η 0 −f η, K1 u∗ η , K2 u∗ η , . . . , Kn u∗ η dη t η 0 0 ψ t − η, η ϕ η, s fs, Kus, Hus − fs, Ku∗ s, Hu∗ sds dη 14 Advances in Difference Equations t n q−1 ∗ t−η Ki l η dη ≤ u − u μ C MT C ∗ C 2 n Ki∗ i1 0 i1 t η 0 q−1 γ −1 t−η η−s lsds dη 0 n n q qγ ∗ 2 ∗ μ C MT C Ki Γ q I lt C Ki Γ q Γ γ I lt u − u∗ i1 i1 Λt u − u∗ . 3.35 We get Fu − Fu∗ ≤ δ u − u∗ . 3.36 By the Banach contraction mapping principle, F has a unique fixed point, which is a mild solution of 1.1. 4. An Example To illustrate the usefulness of our main result, we consider the following fractional differential equation: ∂2 tn ∂q ut, ξ bt, ξ 2 ut, ξ q ∂t n ∂ξ t t − sus, ξds 0 tn n t e−ts us, ξds, ut, 0 ut, 1 0, u0, ξ − ξ y 0 0 ξ ∈ 0, 1, 0 4.1 "u" " " b−1 0, x sin" "dx dy, λ where 0 < q < 1, 0 ≤ t ≤ 1, λ > C M1, n ∈ N, bt, ξ is continuous function and is uniformly Hölder continuous in t, that is, there exist C > 0 and γ ∈ 0, 1 such that bt1 , ξ − bt2 , ξ ≤ C|t1 − t2 |γ , 0 ≤ t1 ≤ t2 ≤ 1. 4.2 Let X L2 0, 1, R and define At by # $ DAt H 2 0, 1 ∩ H01 0, 1 H 2 0, 1 : z0 z1 0 , −Atz bt, ξz . Then −As generates an analytic semigroup exp−tAs. 4.3 Advances in Difference Equations 15 For t ∈ 0, 1, ξ ∈ 0, 1, we set utξ ut, ξ, "u" " " gu sin" ", λ A−1 0gu − ξ y 0 tn ft, K1 ut, K2 utξ n 0 "u" " " b−1 0, x sin" "dx dy, λ t tn t − sus, ξds n 0 t 4.4 e−ts us, ξds, 0 where K1 utξ t t − sus, ξds, 0 K2 utξ t e−ts us, ξds, 0 K1∗ 4.5 t 1 sup t − sds < < ∞, 2 0 t∈I K2∗ sup t∈I t e−ts ds 0 1 < ∞. 4 Moreover, we can get gu ≤ 1 u , λ 1 α gD ≤ αD λ 4.6 for any D ⊂ X. Then the above equation 4.1 can be written in the abstract form as 1.1. On the other hand, n ft, Kut, Hutξ ≤ t K1 ut, ξ K2 ut, ξ n tn ∗ K1 u K2∗ u n μtω K1∗ u K2∗ u , ≤ 4.7 16 Advances in Difference Equations where μt tn , ωz z/n satisfying B1. For any u1 , u2 ∈ X, ψt − s, sfs, K1 u1 s, K2 u1 sξ − ψt − s, sfs, K1 u2 s, K2 u2 sξ ≤ Csn t − sq−1 K1 u1 sξ − K1 u2 sξ K2 u1 sξ − K2 u2 sξ . n 4.8 Therefore, for any bounded sets D1 , D2 ⊂ X, we have Csn α ψt − s, sfs, D1 , D2 ≤ t − sq−1 αD1 αD2 . n 4.9 Moreover, C sup n t∈0,1 t t − sq−1 sn ds 0 C C sup tnq B q, n 1 B q, n 1 : β1 β2 . n t∈0,1 n 4.10 Similarly, we obtain C2 α ψt − s, sϕs, τfτ, D1 , D2 ≤ t − sq−1 s − τγ −1 τ n αD1 αD2 , n t s C2 C2 sup B q, γ B q γ, n 1 : ζ1 ζ2 . t − sq−1 s − τγ −1 τ n dτ ds ≤ n t∈0,1 0 0 n Suppose further that 4.11 1 3/4nC1 CBq, γ p − 1/pq − 1p−1/p μ Lp < 1 − C M1/λ, 2 1/λC M1 3β1 2ζ1 < 1. Then 4.1 has a mild solution by Theorem 3.1. References 1 R. P. Agarwal, M. Belmekki, and M. Benchohra, “A survey on semilinear differential equations and inclusions involving Riemann-Liouville fractional derivative,” Advances in Difference Equations, vol. 2009, Article ID 981728, 47 pages, 2009. 2 A. Anguraj, P. Karthikeyan, and G. M. N’Guérékata, “Nonlocal Cauchy problem for some fractional abstract integro-differential equations in Banach spaces,” Communications in Mathematical Analysis, vol. 6, no. 1, pp. 31–35, 2009. 3 M. M. El-Borai, “Some probability densities and fundamental solutions of fractional evolution equations,” Chaos, Solitons and Fractals, vol. 14, no. 3, pp. 433–440, 2002. 4 M. M. El-Borai, “The fundamental solutions for fractional evolution equations of parabolic type,” Journal of Applied Mathematics and Stochastic Analysis, no. 3, pp. 197–211, 2004. 5 F. Li, “Mild solutions for fractional differential equations with nonlocal conditions,” Advances in Difference Equations, vol. 2010, Article ID 287861, 9 pages, 2010. 6 F. Li, “Solvability of nonautonomous fractional integrodifferential equations with infinite delay,” Advances in Difference Equations, vol. 2011, Article ID 806729, 18 pages, 2011. Advances in Difference Equations 17 7 J. Liang and T.-J. Xiao, “Solutions to nonautonomous abstract functional equations with infinite delay,” Taiwanese Journal of Mathematics, vol. 10, no. 1, pp. 163–172, 2006. 8 G. M. Mophou, “Existence and uniqueness of mild solutions to impulsive fractional differential equations,” Nonlinear Analysis: Theory, Methods & Applications, vol. 72, no. 3-4, pp. 1604–1615, 2010. 9 S. G. Samko, A. A. Kilbas, and O. I. Marichev, Fractional Integrals and Derivatives: Theory and Applications, Gordon and Breach Science, New York, NY, USA, 1993. 10 T. Diagana, “Pseudo-almost automorphic solutions to some classes of nonautonomous partial evolution equations,” Differential Equations & Applications, vol. 1, no. 4, pp. 561–582, 2009. 11 E. Hille and R. S. Phillips, Functional Analysis and Semi-Groups, vol. 31 of American Mathematical Society Colloquium Publications, American Mathematical Society, Providence, RI, USA, 1957. 12 K. Josić and R. Rosenbaum, “Unstable solutions of nonautonomous linear differential equations,” SIAM Review, vol. 50, no. 3, pp. 570–584, 2008. 13 M. Kunze, L. Lorenzi, and A. Lunardi, “Nonautonomous Kolmogorov parabolic equations with unbounded coefficients,” Transactions of the American Mathematical Society, vol. 362, no. 1, pp. 169–198, 2010. 14 J. Liang, R. Nagel, and T.-J. Xiao, “Approximation theorems for the propagators of higher order abstract Cauchy problems,” Transactions of the American Mathematical Society, vol. 360, no. 4, pp. 1723– 1739, 2008. 15 A. Pazy, Semigroups of Linear Operators and Applications to Partial Differential Equations, vol. 44 of Applied Mathematical Sciences, Springer, New York, NY, USA, 1983. 16 T.-J. Xiao and J. Liang, The Cauchy Problem for Higher-Order Abstract Differential Equations, vol. 1701 of Lecture Notes in Mathematics, Springer, Berlin, Germany, 1998. 17 T.-J. Xiao and J. Liang, “Approximations of Laplace transforms and integrated semigroups,” Journal of Functional Analysis, vol. 172, no. 1, pp. 202–220, 2000. 18 T.-J. Xiao and J. Liang, “Existence of classical solutions to nonautonomous nonlocal parabolic problems,” Nonlinear Analysis: Theory, Methods and Applications, vol. 63, no. 5–7, pp. e225–e232, 2005. 19 T.-J. Xiao and J. Liang, “Second order differential operators with Feller-Wentzell type boundary conditions,” Journal of Functional Analysis, vol. 254, no. 6, pp. 1467–1486, 2008. 20 T.-J. Xiao, J. Liang, and J. van Casteren, “Time dependent Desch-Schappacher type perturbations of Volterra integral equations,” Integral Equations and Operator Theory, vol. 44, no. 4, pp. 494–506, 2002. 21 L. Byszewski and V. Lakshmikantham, “Theorem about the existence and uniqueness of a solution of a nonlocal abstract Cauchy problem in a Banach space,” Applicable Analysis, vol. 40, no. 1, pp. 11–19, 1991. 22 Z. Fan, “Impulsive problems for semilinear differential equations with nonlocal conditions,” Nonlinear Analysis: Theory, Methods & Applications, vol. 72, no. 2, pp. 1104–1109, 2010. 23 J. Liang and T.-J. Xiao, “Semilinear integrodifferential equations with nonlocal initial conditions,” Computers & Mathematics with Applications, vol. 47, no. 6-7, pp. 863–875, 2004. 24 J. Liang, J. H. Liu, and T.-J. Xiao, “Nonlocal problems for integrodifferential equations,” Dynamics of Continuous, Discrete & Impulsive Systems. Series A, vol. 15, no. 6, pp. 815–824, 2008. 25 J. Liang, J. van Casteren, and T.-J. Xiao, “Nonlocal Cauchy problems for semilinear evolution equations,” Nonlinear Analysis: Theory, Methods & Applications, vol. 50, no. 2, pp. 173–189, 2002. 26 H. Liu and J.-C. Chang, “Existence for a class of partial differential equations with nonlocal conditions,” Nonlinear Analysis: Theory, Methods & Applications, vol. 70, no. 9, pp. 3076–3083, 2009. 27 J. Banaś and K. Goebel, Measures of Noncompactness in Banach Spaces, vol. 60 of Lecture Notes in Pure and Applied Mathematics, Marcel Dekker, New York, NY, USA, 1980. 28 H.-P. Heinz, “On the behaviour of measures of noncompactness with respect to differentiation and integration of vector-valued functions,” Nonlinear Analysis: Theory, Methods & Applications, vol. 7, no. 12, pp. 1351–1371, 1983. 29 B. Sadovskii, “On a fixed point principle,” Functional Analysis and Its Applications, vol. 2, pp. 151–153, 1967. 30 D. Bothe, “Multivalued perturbations of m-accretive differential inclusions,” Israel Journal of Mathematics, vol. 108, pp. 109–138, 1998.