Hindawi Publishing Corporation Advances in Mathematical Physics Volume 2013, Article ID 823961, 9 pages http://dx.doi.org/10.1155/2013/823961 Research Article On a Multipoint Boundary Value Problem for a Fractional Order Differential Inclusion on an Infinite Interval Nemat Nyamoradi,1 Dumitru Baleanu,2,3,4 and Ravi P. Agarwal5,6 1 Department of Mathematics, Faculty of Sciences, Razi University, Kermanshah 67149, Iran Department of Mathematics and Computer Sciences, Faculty of Art and Sciences, Cankaya University, 06530 Ankara, Turkey 3 Institute of Space Sciences, P.O. BOX MG-23, 76900 Magurele, Bucharest, Romania 4 Department of Chemical and Materials Engineering, Faculty of Engineering, King Abdulaziz University, P.O. Box 80204, Jeddah 21589, Saudi Arabia 5 Department of Mathematics, Texas A & M University-Kingsville, 700 University Boulevard, Kingsville, USA 6 Department of Mathematics, King Abdulaziz University, P.O. Box 80204, Jeddah 21589, Saudi Arabia 2 Correspondence should be addressed to Dumitru Baleanu; dumitru@cankaya.edu.tr Received 12 January 2013; Accepted 22 January 2013 Academic Editor: JoseΜ Tenreiro Machado Copyright © 2013 Nemat Nyamoradi 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 investigate the existence of solutions for the following multipoint boundary value problem of a fractional order differential π−2 inclusion π·0πΌ+ π’(π‘) + πΉ(π‘, π’(π‘), π’σΈ (π‘)) ∋ 0, 0 < π‘ < +∞, π’(0) = π’σΈ (0) = 0, π·πΌ−1 π’(+∞) − ∑π=1 π½π π’(ππ ) = 0, where π·0πΌ+ is the standard π−2 Riemann-Liouville fractional derivative, 2 < πΌ < 3, 0 < π1 < π2 < ⋅ ⋅ ⋅ < ππ−2 < +∞, satisfies 0 < ∑π=1 π½π πππΌ−1 < Γ(πΌ), and πΉ : [0, +∞) × R × R → P(R) is a set-valued map. Several results are obtained by using suitable fixed point theorems when the right hand side has convex or nonconvex values. 1. Introduction In this paper, we will consider the existence of solutions for the following multipoint boundary value problem of a fractional order differential inclusion π·0πΌ+ π’ (π‘) + πΉ (π‘, π’ (π‘) , π’σΈ (π‘)) ∋ 0, π’ (0) = π’σΈ (0) = 0, 0 < π‘ < +∞, π−2 π·πΌ−1 π’ (+∞) − ∑ π½π π’ (ππ ) = 0, (1) π=1 π·0πΌ+ is the standard Riemann-Liouville fractional where derivative, 2 < πΌ < 3, 0 < π1 < π2 < ⋅ ⋅ ⋅ < ππ−2 < +∞, πΌ−1 satisfies 0 < ∑π−2 < Γ(πΌ), and πΉ : [0, +∞) × R × R → π=1 π½π ππ P(R) is a set-valued map. The present paper is motivated by a recent paper of Liang and Zhang [1], where it is considered problem (1) with πΉ single valued, and several existence results are provided. Fractional differential equations have been of great interest recently. This is because of both the intensive development of the theory of fractional calculus itself and the applications of such constructions in various scientific fields such as physics, mechanics, chemistry, and engineering. For details, see [2–4] and the references therein. The existence of solutions of initial value problems for fractional order differential equations has been studied in the literature [5–17] and the references therein. The study of fractional differential inclusions was initiated by El-Sayed and Ibrahim [18]. Also, recently, several qualitative results for fractional differential inclusions were obtained in [19–23] and the references therein. The aim here is to establish existence results for problem (1) when the right hand side is convex as well as nonconvex valued. In the first result (Theorem 21), we consider the case when the right hand side has convex values and prove an existence result via nonlinear alternative for Kakutani maps. In the second result (Theorem 25), we will use the fixed point theorem for contraction multivalued maps according to Covitz and Nadler. The paper is organized as follows. 2 Advances in Mathematical Physics In Section 2 we recall some preliminary facts that we need in the sequel, and in Section 3 we prove our main results. Finally, in Section 4, an example is given to demonstrate the application of one of our main results. that is, for every sequence {π₯π }π∈N ⊂ π and {π¦π }π∈N ⊂ π, if when π → ∞, π₯π → π₯∗ , π¦π → π¦∗ , and π¦π ∈ π(π₯π ), then π¦∗ ∈ π(π₯∗ ). Conversely, if π is completely continuous and has a closed graph, then it is upper semicontinuous. 2. Preliminaries For the convenience of the reader, we present here the following nonlinear alternative of the Leray-Schauder type and its consequences. In this section, we present some notations and preliminary lemmas that will be used in the proof of the main result. Let (π, π) be a metric space with the corresponding norm β ⋅ β and let πΌ = [0, +∞). We denote by L(πΌ) the π-algebra of all Lebesgue measurable subsets of πΌ, by B(π) the family of all nonempty subsets of π, and by P(π) the family of all Borel subsets of π. If π΄ ⊂ πΌ then ππ΄ : πΌ → {0, 1} denotes the characteristic function of π΄. For any subset π΄ ⊂ π, we denote by π΄ the closure of π΄. Recall that the Pompeiu-Hausdorff distance of the closed subsets π΄, π΅ ⊂ π is defined by the following: ππ» (π΄, π΅) = max {π∗ (π΄, π΅) , π∗ (π΅, π΄)} , π∗ (π΄, π΅) = sup {π (π, π΅) , π ∈ π΄} , (2) where π(π₯, π΅) = inf π¦∈π΅ π(π₯, π¦). Define (i) π has a fixed point in π or (ii) there is a π’ ∈ ππ and π ∈ (0, 1) with π’ ∈ ππ(π’). Definition 3. The multifunction π : π → P(π) is said to be lower semicontinuous if for any closed subset πΆ ⊂ π, the subset {π ∈ π : π(π ) ⊂ πΆ} is closed. If πΉ : [0, +∞) × R × R → P(R) is a set-valued map with compact values and π₯ ∈ πΆ([0, +∞), R), we define P (π) = {π ⊂ π : π =ΜΈ 0} , Pπ (π) = {π ∈ P (π) : π bounded} , Pππ (π) = {π ∈ P (π) : π closed} , Theorem 2 (nonlinear alternative for Kakutani maps [25]). Let π be a Banach space, πΆ a closed convex subset of π, π an open subset of πΆ, and 0 ∈ π. Suppose that π : π → Pππ,πV (πΆ) is an upper semicontinuous compact map; here Pππ,πV (πΆ) denotes the family of nonempty, compact convex subsets of πΆ. Then, either (3) Pππ (π) = {π ∈ P (π) : π compact} , PπV (π) = {π ∈ P (π) : π convex} . Also, we denote by πΆ(πΌ, π) the Banach space of all continuous functions π₯ : [0, +∞) → π endowed with the norm |π₯|π = supπ‘∈[0,+∞) |π₯(π‘)| and by πΏ1 ([0, +∞), π) the Banach space of all (Bochner) integrable functions π₯ : [0, +∞) → π endowed with the norm |π₯|1 = ∫[0,+∞) |π₯(π‘)|ππ‘. Let (π, π1 ) and (π, π2 ) be two metric spaces. If π : π → P(π) is a set-valued map, then a point π₯ ∈ π is called a fixed point for π if π₯ ∈ π(π₯). π is said to be bounded on bounded sets if π(π΅) := ∪π₯∈π΅ π(π₯) is a bounded subset of π for all bounded sets π΅ in π. π is said to be compact if π(π΅) is relatively compact for any bounded sets π΅ in π. π is said to be totally compact if π(π) is a compact subset of π. π is said to be upper semicontinuous if for any open set π· ⊂ π, the set {π₯ ∈ π : π(π₯) ⊂ π·} is open in π. π is called completely continuous if it is upper semicontinuous and, for every bounded subset π΄ ⊂ π, π(π΄) is relatively compact. It is well known that a compact set-valued map π with nonempty compact values is upper semicontinuous if and only if π has a closed graph. We define the graph of π to be the set Gr(π) = {(π₯, π¦) ∈ π × π, π¦ = π(π₯)} and recall a useful result regarding connection between closed graphs and upper semicontinuity. Lemma 1 (see [24, Proposition 1.2]). If π : π → Pππ (π) is upper semicontinuous, then Gr(π) is a closed subset of π × π, ππΉ (π₯) := {π ∈ πΏ1 ([0, +∞) , R) : π (π‘) ∈ πΉ (π‘, π₯ (π‘) , π₯σΈ (π‘)) a.e. [0, +∞)} . (4) Then, πΉ is of a lower semicontinuous type if ππΉ (⋅) is a lower semicontinuous with closed and decomposable values. Theorem 4 (see [26]). Let π be a separable metric space and πΊ : π → P(πΏ1 ([0, +∞), R)) be a lower semicontinuous setvalued map with closed decomposable values. Then πΊ has a continuous selection (i.e., there exists a continuous mapping π : π → πΏ1 ([0, +∞), R) such that π(π ) ∈ πΊ(π ) for all π ∈ π). Definition 5. Consider the following. (i) A set-valued map πΊ : [0, +∞) → P(R) with nonempty compact convex values is said to be measurable if for any π₯ ∈ R the function π‘ → π(π₯, πΊ(π‘)) is measurable. (ii) A set-valued map πΉ : [0, +∞) × R × R → P(R) is said to be CaratheΜodory if π‘ → πΉ(π‘, π₯, π¦) is measurable for all π₯, π¦ ∈ R and (π₯, π¦) → πΉ(π‘, π₯, π¦) is upper semicontinuous for almost all π‘ ∈ [0, +∞). (iii) πΉ is said to be πΏ1 -CaratheΜodory if for any π > 0 there exists βπ ∈ πΏ1 ([0, +∞), R) such that sup{|V| : V ∈ πΉ(π‘, π₯, π¦)} ≤ βπ (π‘) a.e. [0, +∞); ∀π₯, π¦ ∈ R. Finally, the following results are easily deduced from the theoretical limit set properties. Advances in Mathematical Physics 3 Lemma 6 (see [27, Lemma 1.1.9]). Let {πΎπ }π∈N ⊂ πΎ ⊂ π be a sequence of subsets where πΎ is a compact subset of a separable Banach space π. Then, co (lim supπΎπ ) = β co ( β πΎπ ) , π→∞ π>0 (5) π≥π Definition 13 (see [31]). The Riemann-Liouville fractional derivative of order πΌ > 0, π − 1 < πΌ < π, π ∈ N is defined as π·0πΌ+ π (π‘) = π π π‘ 1 ( ) ∫ (π‘ − π )π−πΌ−1 π (π ) ππ , Γ (π − πΌ) ππ‘ 0 (9) where co(π΄) refers to the closure of the convex hull of π΄. where the function π(π‘) has absolutely continuous derivatives up to order (π − 1). Lemma 7 (see [27, Lemma 1.4.13]). Let π and π be two metric spaces. If πΊ : π → Pππ (π) is an upper semicontinuous, then, for each π₯0 ∈ π, Lemma 14 (see [31]). The equality π·0+ πΌ0+ π(π‘) = π(π‘), πΎ > 0 holds for π ∈ πΏ1 (0, 1). lim sup πΊ (π₯) = πΊ (π₯0 ) . Lemma 15 (see [31]). Let πΌ > 0 and π’ ∈ πΆ(0, 1) ∩ πΏ1 (0, 1). Then, the differential equation π₯ → π₯0 (6) Definition 8. Let π be a Banach space. A sequence {π₯π }π∈N ⊂ πΏ1 ([π, π], π) is said to be semicompact if (a) it is integrably bounded; that is, there exists π ∈ πΏ1 ([π, π], R+ ) such that σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨π₯π (π‘)σ΅¨σ΅¨σ΅¨πΈ ≤ π (π‘) , for a.e. π‘ ∈ [π, π] and every π ∈ N, (7) (b) the image sequence {π₯π (π‘)}π∈N is relatively compact in πΈ for a.e. π‘ ∈ [π, π]. The following important result follows from the DunfordPettis theorem (see [28, Proposition 4.2.1]). Lemma 9. Every semicompact sequence πΏ1 ([π, π], π) is weakly compact in πΏ1 ([π, π], π). When the nonlinearity takes convex values, Mazur’s Lemma, 1933, may be useful. Lemma 10 (see [29, Theorem 21.4]). Let πΈ be a normed space and {π₯π }π∈N ⊂ πΈ a sequence weakly converging to a limit π₯ ∈ πΈ. Then, there exists a sequence of convex combinations π¦π = π ∑π π=1 πΌππ π₯π with πΌππ > 0 for π = 1, 2, . . . , π and ∑π=1 πΌππ = 1 which converges strongly to π₯. Lemma 11 (see [30]). Let π be defined as before and π ⊂ π. Then π is relatively compact in π if the following conditions hold: (a) π is uniformly bounded in π; (b) the functions from π are equicontinuous on any compact interval of [0, +∞); (c) the functions from π are equiconvergent; that is, for any given π > 0, there exists a π = π(π) > 0 such that |π(π‘) − π(+∞)| < π, for any π‘ > π, π ∈ π. Definition 12 (see [6]). The Riemann-Liouville fractional integral operator of order πΌ > 0, of function π ∈ πΏ1 (R+ ), is defined as πΌ0πΌ+ π (π‘) = π‘ 1 ∫ (π‘ − π )πΌ−1 π (π ) ππ , Γ (πΌ) 0 where Γ(⋅) is the Euler gamma function. (8) πΎ πΎ π·0πΌ+ π’ (π‘) = 0 (10) has a unique solution π’(π‘) = π1 π‘πΌ−1 +π2 π‘πΌ−2 +⋅ ⋅ ⋅+ππ π‘πΌ−π , ππ ∈ R, π = 1, . . . , π, where π − 1 < πΌ < π. Lemma 16 (see [31]). Let πΌ > 0. Then, the following equality holds for π’ ∈ πΏ1 (0, 1), π·0πΌ+ π’ ∈ πΏ1 (0, 1): πΌ0πΌ+ π·0πΌ+ π’ (π‘) = π’ (π‘) + π1 π‘πΌ−1 + π2 π‘πΌ−2 + ⋅ ⋅ ⋅ + ππ π‘πΌ−π , (11) ππ ∈ R, π = 1, . . . , π, where π − 1 < πΌ ≤ π. By π΄πΆ1 ([0, +∞), R) we denote the space of continuous real-valued functions whose first derivative exists and it is absolutely continuous on [0, +∞). In this paper, we will use the following space πΈ to the study (1) which is denoted by |π’ (π‘)| , πΌ−1 1 0≤π‘<+∞ + π‘ πΈ = {π’ ∈ π΄πΆ1 ([0, +∞) , R) : sup (12) σ΅¨σ΅¨ σΈ σ΅¨σ΅¨ σ΅¨σ΅¨π’ (π‘)σ΅¨σ΅¨ sup σ΅¨ πΌ−1σ΅¨ < +∞} . 0≤π‘<+∞ 1 + π‘ From [32], we know that πΈ is a Banach space equipped with the norm σ΅¨σ΅¨ σΈ σ΅¨σ΅¨ σ΅¨σ΅¨π’ (π‘)σ΅¨σ΅¨ |π’ (π‘)| (13) , sup σ΅¨ πΌ−1σ΅¨ } . βπ’β = max { sup πΌ−1 0≤π‘<+∞ 1 + π‘ 0≤π‘<+∞ 1 + π‘ In what follows, πΌ = [0, +∞), πΌ ∈ (2, 3), and Δ = πΌ−1 . Next, we need the following technical result ∑π−2 π=1 π½π ππ proved in [1]. Lemma 17 (see [1]). For any β ∈ πΏ1 ([0, +∞), R), the problem π·0πΌ+ π’ (π‘) + β (π‘) = 0, 0 < π‘ < ∞, 2 < πΌ < 3, π−2 π’ (0) = π’σΈ (0) = 0, π·πΌ−1 π’ (+∞) = ∑ π½π π’ (ππ ) , (14) π=1 has a unique solution π’(π‘) that π’ (π‘) = ∫ +∞ 0 πΊ (π‘, π ) β (π ) ππ , (15) 4 Advances in Mathematical Physics where πΊ (π‘, π ) = πΊ1 (π‘, π ) + πΊ2 (π‘, π ) , πΊ1 (π‘, π ) = π‘πΌ−1 − (π‘ − π )πΌ−1 , 1 { πΌ−1 Γ (πΌ) π‘ , πΊ2 (π‘, π ) = (16) 0 ≤ π ≤ π‘ < +∞, (17) 0 ≤ π‘ ≤ π < +∞, πΌ−1 ∑π−2 π=1 π½π π‘ πΊ (π , π ) . Γ (πΌ) − Δ 1 π (18) Note that πΊ(π‘, π ) > 0, ∀π‘, π ∈ [0, +∞), (e.g., Lemma 3.2 in [1]) and from the definition of πΊ1 (π‘, π ), we have the following (e.g., Remark 3.1 in [1]): πΊ1 (π‘, π ) 1 , ≤ 1 + π‘πΌ−1 Γ (πΌ) πΊ (π‘, π ) ≤ πΏ1 1 + π‘πΌ−1 (19) for (π‘, π ) ∈ [0, +∞) × [0, +∞) , ∑π−2 π½ ππΌ−1 1 (1 + π=1 π π−2 ) . Γ (πΌ) (Γ (πΌ) − Δ) (20) for (π‘, π ) ∈ [0, +∞) × [0, +∞) , (21) where ∑π−2 π½ ππΌ−1 2 (πΌ − 1) πΏ2 = (1 + π=1 π π−2 ) . Γ (πΌ) (Γ (πΌ) − Δ) π +∞ max {πΏ 1 , πΏ 2 } π (π) ∫0 π (π ) ππ > 1. (25) Then, problem (1) has at least one solution. π’ (π‘) ∈ ∫ +∞ πΊ (π‘, π ) πΉ (π , π’ (π ) , π’σΈ (π )) ππ , π‘ ∈ πΌ, (26) where πΊ(π‘, π ) is defined by (16) and (17). Consider the setvalued map, π : πΈ → P(π) is defined by π (π’) := {V ∈ π; V (π‘) = ∫ +∞ 0 πΊ (π‘, π ) π (π ) ππ , π ∈ ππΉ (π’)} . (27) (22) We show that π satisfies the hypotheses of Theorem 2. Lemma 18. The function πΊ(π‘, π ) defined by (16) satisfies πΌ−1 ∑π−2 πΊ (π‘, π ) π=1 π½π ππ . lim = π‘ → +∞ 1 + π‘πΌ−1 Γ (πΌ) (Γ (πΌ) − Δ) (H2) There exists a constant π > 0 such that 0 Also, one can get ππΊ (π‘, π ) /ππ‘ ≤ πΏ2 1 + π‘πΌ−1 (H1) There exists a continuous nondecreasing function π : [0, +∞) → (0, +∞) and π ∈ πΏ1 ([0, +∞), R+ ) such that βπΉ(π‘, π₯, π¦)βP := sup{|V(π‘)/(1 + π‘πΌ−1 )| : V ∈ πΉ(π‘, π₯, π¦)} ≤ π(π‘)π(βπ₯β), for a.e. π‘ ∈ πΌ and each π₯, π¦ ∈ R. Proof. Let π = πΈ and consider π > 0 as in (25). It is obvious that the existence of solutions to problem (1) is reduced to the existence of the solutions of the integral inclusion where πΏ1 = Theorem 21. The CaratheΜodory multivalued map πΉ : πΌ × R × R → P(R) has nonempty, compact, convex values and satisfies the following. (23) By calculation, it is easy to prove that Lemma 18 holds. So, we omit its proof here. 3. Main Results Now we are able to present the existence results for problem (1). Claim 1. We show that π(π’) ⊂ π is convex for any π’ ∈ π. If V1 , V2 ∈ π(π’), then, there exist π1 , π2 ∈ ππΉ (π’) such that for any π‘ ∈ πΌ one has Vπ (π‘) = ∫ 0 Lemma 19 (see [32]). Let π = {π’ ∈ πΈ | βπ’β < π}(π > 0), π1 = {π’(π‘)/(1 + π‘πΌ−1 ) : π’ ∈ π}. If π1 is equicontinuous on any compact interval of [0, +∞) and equiconvergent at infinity, then π is relatively compact on πΈ. Definition 20. π1 is called equiconvergent at infinity if and only if for all π > 0, there exists V(π) > 0 such that for all π’ ∈ π1 , π‘1 , π‘2 ≥ V, it holds σ΅¨σ΅¨ π’ (π‘ ) π’ (π‘2 ) σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ 1 σ΅¨ σ΅¨σ΅¨ (24) − σ΅¨σ΅¨ 1 + π‘πΌ−1 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨ < π. σ΅¨ 1 2 σ΅¨ πΊ (π‘, π ) ππ (π ) ππ , π = 1, 2. (28) Let 0 ≤ π ≤ 1. Then, for any π‘ ∈ πΌ, we have (πV1 + (1 − π) V2 ) (π‘) =∫ 3.1. The Upper Semicontinuous Case. To obtain the complete continuity of existence solutions operator, the following lemma is still needed. +∞ +∞ 0 πΊ (π‘, π ) [ππ1 (π ) + (1 − π) π2 (π )] ππ . (29) The values of πΉ are convex; thus, ππΉ (π’) is a convex set and hence πV1 + (1 − π)V2 ∈ π(π’). Claim 2. We show that π is bounded on bounded sets of π. Let π΅ be any bounded subset of π. Then, there exists π > 0 such that βπ’β ≤ π for all π’ ∈ π΅. If V ∈ π(π’), then there exists +∞ π ∈ ππΉ (π’) such that V(π‘) = ∫0 πΊ(π‘, π )π(π )ππ . One may write the following for any π‘ ∈ πΌ: σ΅¨σ΅¨ V (π‘) σ΅¨σ΅¨ σ΅¨ +∞ σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ πΊ (π‘, π ) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ π (π )σ΅¨σ΅¨σ΅¨ ππ ≤ ∫ σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨ πΌ−1 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘πΌ−1 σ΅¨σ΅¨ σ΅¨ 1 + π‘ 0 σ΅¨ σ΅¨ ≤ πΏ1 ∫ +∞ 0 σ΅¨ σ΅¨ π (π ) π (βπ’β) ππ ≤ πΏ 1 σ΅¨σ΅¨σ΅¨πσ΅¨σ΅¨σ΅¨1 π (π) . (30) Advances in Mathematical Physics 5 On the other hand, σ΅¨σ΅¨ σΈ σ΅¨ +∞ ππΊ (π‘, π ) /ππ‘ σ΅¨σ΅¨ V (π‘) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨ π (π ) ππ σ΅¨σ΅¨ 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨ ≤ ∫0 1 + π‘πΌ−1 σ΅¨ σ΅¨ ≤ πΏ2 ∫ +∞ 0 π (π ) π (βπ’β) ππ (31) σ΅¨ σ΅¨ ≤ πΏ 2 σ΅¨σ΅¨σ΅¨πσ΅¨σ΅¨σ΅¨1 π (π) , On the other hand, we get +∞ σ΅¨σ΅¨ πΊ (π‘ , π ) πΊ (π‘ , π ) σ΅¨σ΅¨σ΅¨ σ΅¨ ∫ σ΅¨σ΅¨σ΅¨σ΅¨ 1 1πΌ−1 − 1 2πΌ−1 σ΅¨σ΅¨σ΅¨σ΅¨ π (π ) π (βπ’β) ππ 1 + π‘1 σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘1 0 π‘1 π‘2 +∞ σ΅¨σ΅¨ πΊ (π‘ , π ) πΊ (π‘ , π ) σ΅¨σ΅¨σ΅¨ σ΅¨ ≤ (∫ + ∫ + ∫ ) σ΅¨σ΅¨σ΅¨σ΅¨ 1 1πΌ−1 − 1 2πΌ−1 σ΅¨σ΅¨σ΅¨σ΅¨ 1 + π‘1 σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘1 π‘2 0 π‘1 × π (π ) π (βπ’β) ππ π‘1 ≤ π (π) ∫ (π‘2πΌ−1 − π‘1πΌ−1 ) + ((π‘2 − π ) 1+ 0 πΌ−1 − (π‘1 − π ) πΌ−1 ) π‘1πΌ−1 × π (π ) ππ and therefore σ΅¨σ΅¨ V (π‘) σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨ VσΈ (π‘) σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨} βVβ = max {σ΅¨σ΅¨σ΅¨ σ΅¨, σ΅¨σ΅¨ 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨σ΅¨ 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨σ΅¨ π‘∈πΌ + π (π) ∫ π‘2 πΌ−1 (π‘2πΌ−1 − π‘1πΌ−1 ) + (π‘2 − π ) 1 + π‘1πΌ−1 π‘1 (32) σ΅¨ σ΅¨ ≤ max {πΏ 1 , πΏ 2 } σ΅¨σ΅¨σ΅¨πσ΅¨σ΅¨σ΅¨1 π (π) , + π (π) ∫ +∞ (π‘2πΌ−1 − π‘1πΌ−1 ) 1 + π‘1πΌ−1 π‘2 π (π ) ππ π (π ) ππ σ³¨→ 0 uniformly as π‘1 σ³¨→ π‘2 . (34) for all V ∈ π(π’); that is, π(π΅) is bounded. Claim 3. We show that π maps bounded the sets into equicontinuous sets. Let π΅ be any bounded subset of π as before and V ∈ π(π’) for some π’ ∈ π΅. Then, there exists π ∈ ππΉ (π’) +∞ such that V(π‘) = ∫0 πΊ(π‘, π )π(π )ππ . So, for any π0 ∈ (0, +∞) and π‘1 , π‘2 ∈ [0, π0 ], without loss of generality, we may assume that π‘2 > π‘1 and one can get the following: σ΅¨σ΅¨ V (π‘ ) V (π‘2 ) σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ 1 σ΅¨ σ΅¨σ΅¨ − σ΅¨σ΅¨ 1 + π‘πΌ−1 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨ σ΅¨ 1 2 σ΅¨ +∞ σ΅¨σ΅¨ πΊ (π‘ , π ) πΊ (π‘ , π ) σ΅¨σ΅¨σ΅¨ σ΅¨ ≤ ∫ σ΅¨σ΅¨σ΅¨σ΅¨ 1 1πΌ−1 − 1 2πΌ−1 σ΅¨σ΅¨σ΅¨σ΅¨ π (π ) ππ 1 + π‘2 σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘1 0 +∞ 0 σ΅¨σ΅¨ πΊ (π‘ , π ) πΊ (π‘ , π ) σ΅¨σ΅¨ σ΅¨ σ΅¨ ≤ ∫ σ΅¨σ΅¨σ΅¨σ΅¨ 1 1πΌ−1 − 1 2πΌ−1 σ΅¨σ΅¨σ΅¨σ΅¨ π (π ) π (βπ’β) ππ 1 + π‘1 σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘1 0 +∞ σ΅¨σ΅¨ πΊ (π‘ , π ) πΊ (π‘ , π ) σ΅¨σ΅¨σ΅¨ σ΅¨ + ∫ σ΅¨σ΅¨σ΅¨σ΅¨ 1 2πΌ−1 − 1 2πΌ−1 σ΅¨σ΅¨σ΅¨σ΅¨ π (π ) π (βπ’β) ππ 1 + π‘2 σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘1 0 σ΅¨σ΅¨ π‘πΌ−1 π‘2πΌ−1 σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ 1 σ΅¨σ΅¨ σ΅¨σ΅¨ + − Γ (Γ (πΌ) − Δ σ΅¨σ΅¨σ΅¨ 1 + π‘1πΌ−1 1 + π‘2πΌ−1 σ΅¨σ΅¨σ΅¨ ∑π−2 π=1 ×∫ +∞ 0 πΌ−1 π½π ππ−2 π (π ) π (βπ’β) ππ . uniformly as π‘1 σ³¨→ π‘2 . From (34) and (35), we have σ΅¨σ΅¨σ΅¨ V (π‘1 ) V (π‘2 ) σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ³¨→ 0 uniformly as π‘1 σ³¨→ π‘2 . (36) − σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘1πΌ−1 1 + π‘2πΌ−1 σ΅¨σ΅¨σ΅¨ Similar to (36), one can get σ΅¨σ΅¨ VσΈ (π‘ ) VσΈ (π‘2 ) σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ 1 σ΅¨ σ΅¨σ΅¨ − σ΅¨σ΅¨ 1 + π‘πΌ−1 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨ σ³¨→ 0 uniformly as π‘1 σ³¨→ π‘2 . (37) σ΅¨ 1 2 σ΅¨ Therefore, π(π΅) is an equicontinuous set in π. ∫ πΊ1 (ππ , π ) π (π ) ππ +∞ (35) Claim 4. We show that π is equiconvergent at ∞. Let V ∈ π(π’) for some π’ ∈ π΅. Then, there exists π ∈ ππΉ (π’) such that V(π‘) = +∞ ∫0 πΊ(π‘, π )π(π )ππ . So, we have the following: ∑π−2 π½ σ΅¨σ΅¨σ΅¨ π‘πΌ−1 π‘πΌ−1 σ΅¨σ΅¨σ΅¨ + π=1 π σ΅¨σ΅¨σ΅¨σ΅¨ 1 πΌ−1 − 2 πΌ−1 σ΅¨σ΅¨σ΅¨σ΅¨ Γ (πΌ) − Δ σ΅¨σ΅¨ 1 + π‘1 1 + π‘2 σ΅¨σ΅¨ ×∫ Similar to (34), we have +∞ σ΅¨σ΅¨ πΊ (π‘ , π ) πΊ (π‘ , π ) σ΅¨σ΅¨σ΅¨ σ΅¨ ∫ σ΅¨σ΅¨σ΅¨σ΅¨ 1 2πΌ−1 − 1 2πΌ−1 σ΅¨σ΅¨σ΅¨σ΅¨ π (π ) π (βπ’β) ππ σ³¨→ 0 1 + π‘2 σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘1 0 (33) +∞ 0 +∞ π (π ) ππ ≤ π (π) ∫ 0 π (π ) ππ < +∞, σ΅¨σ΅¨ V (π‘) σ΅¨σ΅¨ +∞ 1 σ΅¨ σ΅¨σ΅¨ = lim lim σ΅¨σ΅¨σ΅¨ πΊ (π‘, π ) π (π ) ππ ∫ σ΅¨ π‘ → +∞ σ΅¨σ΅¨ 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨ π‘ → +∞ 1 + π‘πΌ−1 0 = πΌ−1 +∞ ∑π−2 π=1 π½π ππ ∫ π (π ) ππ Γ (πΌ) (Γ (πΌ) − Δ) 0 − ∑π−2 π=1 π½π Γ (πΌ) (Γ (πΌ) − Δ) ππ × ∫ (ππ − π ) 0 πΌ−1 π (π ) ππ < ∞, (38) 6 Advances in Mathematical Physics and, similarly, one has σ΅¨σ΅¨ σΈ σ΅¨ σ΅¨ V (π‘) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ < ∞. lim σ΅¨σ΅¨σ΅¨σ΅¨ π‘ → +∞ σ΅¨ 1 + π‘πΌ−1 σ΅¨σ΅¨ σ΅¨ σ΅¨ (39) Therefore, π(π΅) is equiconvergent at infinity. Therefore, with Lemma 11, Lemma 19 and Claims 2–4, we conclude that π is completely continuous. Claim 5. π is upper semicontinuous. To this end, it is sufficient to show that π has a closed graph. Let Vπ ∈ π(π’π ) such that Vπ → V and π’π → π’, as π → +∞. Then, there exists π > 0 such that βπ’π β ≤ π. We will prove that V ∈ π(π’) means that there exists ππ ∈ ππΉ (π’π ) such that, for a.e. π‘ ∈ πΌ, we have +∞ Vπ (π‘) = ∫0 πΊ(π‘, π )ππ (π )ππ . Then, we need to show that V ∈ π(π’). Condition (H1) implies that ππ (π‘) ∈ π(π‘)π(π)π΅1 (0). Then, {ππ }π∈N is integrably bounded in πΏ1 (πΌ, R). Since πΉ has compact values, we deduce that {ππ }π is semicompact. By Lemma 9, there exists a subsequence, still denoted as {ππ }π∈N , which converges weakly to some limit π ∈ πΏ1 (πΌ, R). Moreover, the mapping Γ : πΏ1 (πΌ, R) → π = πΈ defined by Γ (π) (π‘) = ∫ +∞ 0 πΊ (π‘, π ) π (π ) ππ (40) is a continuous linear operator. Then, it remains continuous if these spaces are endowed with their weak topologies [29, 33]. Moreover, for a.e. π‘ ∈ πΌ, π’π (π‘) converges to π’(π‘). Then, we have +∞ V (π‘) = ∫ 0 πΊ (π‘, π ) π (π ) ππ . (41) It remains to prove that π ∈ πΉ(π‘, π’(π‘), π’σΈ (π‘)), a.e. π‘ ∈ πΌ. Mazur’s Lemma (see Lemma 10) yields the existence of πΌππ ≥ 0, π = π π, . . . , π(π) such that ∑π(π) π=1 πΌπ = 1 and the sequence of convex π(π) π combinations ππ (⋅) = ∑π=1 πΌπ ππ (⋅) converges strongly to π in πΏ1 . Using Lemma 6, we obtain that V (π‘) ∈ β {ππ (π‘)}, a.e. π‘ ∈ πΌ π≥1 π≥1 (42) ⊂ β co {β πΉ (π‘, π’π (π‘) , π’πσΈ (π‘))} ×∫ +∞ 0 (44) π (π ) ππ . Consequently, βπ’β +∞ max {πΏ 1 , πΏ 2 } π (βπ’β) ∫0 π (π ) ππ ≤ 1. (45) In view of (H2), there exists π such that βπ’β =ΜΈ π. Let us consider the following: π := {π’ ∈ π΄πΆ1 ([0, +∞) , R) : βπ’β < π} . (46) Note that the operator π : π → P(π΄πΆ1 ([0, +∞)) is upper semicontinuous and completely continuous. From the choice of π, there is no π’ ∈ ππ such that π’ = ππ(π’) for some π ∈ (0, 1). Consequently, by the nonlinear alternative of the Leray-Schauder type (Theorem 2), we deduce that π has a fixed point π’ ∈ π which is a solution of the problem (1). This completes the proof. 3.2. The Lipschitz Case. Now we prove the existence of solutions for the problem (1) with a nonconvex-valued right hand side by applying a fixed point theorem for multivalued maps according to Covitz and Nadler [34]. (a) πΎ-Lipschitz if and only if there exists πΎ > 0 such that ππ»(π(π₯), π(π¦)) ≤ πΎπ(π₯, π¦) for each π₯, π¦ ∈ π; Lemma 23 (Covitz-Nadler, [34]). Let (π, π) be a complete metric space. If π : π → Pππ (π) is a contraction, then πΉππ₯π =ΜΈ 0. = co (lim supπΉ (π‘, π’π (π‘) , π’πσΈ (π‘))) . π → +∞ However, the fact that the multivalued π₯ → πΉ(⋅, π₯, π₯σΈ ) is upper semicontinuous and has compact values, together with Lemma 7, implies that π → +∞ ≤ max {πΏ 1 , πΏ 2 } π (βπ’β) (b) a contraction if and only if it is πΎ-Lipschitz with πΎ < 1. π≥1 lim sup πΉ (π‘, π’π (π‘) , π’πσΈ (π‘)) = πΉ (π‘, π’ (π‘) , π’σΈ (π‘)) , Claim 6. A priori bounds on solutions. Let π’ be a solution of (1). Then, there exists π ∈ πΏ1 ([0, +∞), R) with π ∈ ππΉ (π’) +∞ such that π’(π‘) = ∫0 πΊ(π‘, π )π(π )ππ . In view of (H1), and using the computations in Claim 2 above, for each π‘ ∈ [0, +∞), we obtain σ΅¨σ΅¨ π’ (π‘) σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨ π’σΈ (π‘) σ΅¨σ΅¨σ΅¨ +∞ σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨} ≤ max {πΏ , πΏ } ∫ π (π ) ππ , {σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅¨ 1 2 σ΅¨σ΅¨ 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨ 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨ 0 Definition 22. A multivalued operator π : π → Pππ (π) is called the following: ⊂ β co {ππ (π‘) , π ≥ π} π≥1 πΉ(π‘, π’(π‘), π’σΈ (π‘)), a.e. π‘ ∈ πΌ. Thus, V ∈ π(π’), proving that π has a closed graph. Finally, with Lemma 1 and the compactness of π, we conclude that π is upper semicontinuous. a.e. π‘ ∈ πΌ. (43) This along with (42) yields that π(π‘) ∈ coπΉ(π‘, π’(π‘), π’σΈ (π‘)). Finally, πΉ(⋅, ⋅, ⋅) has closed, convex values; hence, π(π‘) ∈ Definition 24. A measurable multivalued function πΉ : [0, +∞) → P(π) is said to be integrably bounded if there exists a function π ∈ πΏ1 ([0, +∞), π) such that for all V ∈ πΉ(π‘), βVβ ≤ π(π‘) for a.e. π‘ ∈ [0, +∞). Theorem 25. Assume that the following condition holds: (H4) πΉ : πΌ × R × R → Pππ (R) such that πΉ(⋅, π₯, π¦) : [0, +∞) → Pππ (R) is measurable for each π₯, π¦ ∈ R; Advances in Mathematical Physics 7 (H5) There exist π1 , π2 : [0, +∞) → [0, +∞) which are not identical zero on any closed subinterval of [0, +∞), and ∫ +∞ 0 (1 + π πΌ−1 ) ππ (π ) ππ < +∞, π = 1, 2, (48) for all π₯1 , π₯2 , π¦1 , and π¦2 ∈ R with π(0, πΉ(π‘, 0, 0)) ≤ π1 (π‘) + π2 (π‘) for almost all π‘ ∈ [0, +∞). Then, the boundary value problem (1) has at least one solution on πΌ = [0, +∞) if 0 (1 + π πΌ−1 ) (π1 (π ) + π2 (π )) ππ ) < 1. (49) Proof. We transform problem (1) into a fixed point problem. Consider the set-valued map π : π΄πΆ1 [0, +∞) → P(π΄πΆ1 [0, +∞)) defined at the beginning of the proof of Theorem 21. It is clear that the fixed point of π are solutions of the problem (1). Note that since the set-valued map πΉ(⋅, π’(⋅)) is measurable with the measurable selection theorem (e.g., Theorem III. 6 in [35]) it admits a measurable selection π : πΌ → R. Moreover, since πΉ is integrably bounded, π ∈ πΏ1 ([0, +∞), R). Therefore, ππΉ (π’) =ΜΈ 0. We will prove that π fulfills the assumptions of CovitzNadler contraction principle (Lemma 23). First, we note that since ππΉ (π’) =ΜΈ 0, π(π’) =ΜΈ 0 for any π’ ∈ 1 π΄πΆ ([0, +∞), R). Second, we prove that π(π’) is closed for any π’ ∈ 1 π΄πΆ ([0, +∞), R). Let {π’π }π≥0 ∈ π(π’) such that π’π → π’0 in π΄πΆ1 ([0, +∞), R). Then π’0 ∈ π΄πΆ1 ([0, +∞), R) and there exists ππ ∈ ππΉ (π’) such that π’π (π‘) = ∫ +∞ 0 πΊ (π‘, π ) ππ (π ) ππ . (50) Since πΉ has compact values, we may pass onto a subsequence (if necessary) to obtain that ππ converges to π ∈ πΏ1 (([0, +∞), R)) in πΏ1 (([0, +∞), R)). In particular, π ∈ ππΉ (π’), and for any π‘ ∈ [0, +∞) we have π’π (π‘) σ³¨→ π’0 (π‘) = ∫ +∞ 0 πΊ (π‘, π ) π (π ) ππ , +∞ 0 πΊ (π‘, π ) π1 (π ) ππ , σ΅¨ σ΅¨ ππ» (πΉ (π‘, π₯1 , π₯1σΈ ) , πΉ (π‘, π₯2 , π₯2σΈ )) ≤ π1 (π‘) σ΅¨σ΅¨σ΅¨π₯1 − π₯2 σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ + π2 (π‘) σ΅¨σ΅¨σ΅¨σ΅¨π₯1σΈ − π₯2σΈ σ΅¨σ΅¨σ΅¨σ΅¨ , (53) σ΅¨ σΈ σ΅¨ σ΅¨ σ΅¨ σ΅¨σ΅¨ σΈ σ΅¨ σ΅¨σ΅¨π1 (π‘) − π2 (π‘)σ΅¨σ΅¨σ΅¨ ≤ π1 (π‘) σ΅¨σ΅¨σ΅¨π₯1 − π₯2 σ΅¨σ΅¨σ΅¨ + π2 (π‘) σ΅¨σ΅¨σ΅¨σ΅¨π₯1 − π₯2 σ΅¨σ΅¨σ΅¨σ΅¨ . +∞ V2 (π‘) = ∫ 0 πΊ (π‘, π ) π2 (π ) ππ , π‘ ∈ [0, +∞) , (56) and one can get σ΅¨σ΅¨ V (π‘) V2 (π‘) σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ 1 − σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘πΌ−1 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨ ≤∫ +∞ πΊ (π‘, π ) σ΅¨σ΅¨ σ΅¨ σ΅¨π (π ) − π1 (π )σ΅¨σ΅¨σ΅¨ ππ 1 + π‘πΌ−1 σ΅¨ 1 0 ≤ πΏ1 ∫ +∞ 0 ≤ πΏ1 ∫ +∞ 0 σ΅¨ σ΅¨ σ΅¨ σ΅¨ [π1 (π ) σ΅¨σ΅¨σ΅¨π₯1 (π )−π₯2 (π )σ΅¨σ΅¨σ΅¨ +π2 (π ) σ΅¨σ΅¨σ΅¨σ΅¨π₯1σΈ (π )−π₯2σΈ (π )σ΅¨σ΅¨σ΅¨σ΅¨] ππ σ΅¨σ΅¨ π₯ (π ) − π₯ (π ) σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨ 2 (1 + π πΌ−1 ) [π1 (π ) σ΅¨σ΅¨σ΅¨ 1 σ΅¨ σ΅¨σ΅¨ 1 + π πΌ−1 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨σ΅¨ π₯σΈ (π ) − π₯2σΈ (π ) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨] ππ + π2 (π ) σ΅¨σ΅¨σ΅¨σ΅¨ 1 σ΅¨ σ΅¨σ΅¨ 1 + π πΌ−1 σ΅¨σ΅¨σ΅¨ σ΅© σ΅© ≤ max {πΏ 1 , πΏ 2 } σ΅©σ΅©σ΅©π₯1 − π₯2 σ΅©σ΅©σ΅© ∫ +∞ 0 (1+π πΌ−1 ) (π1 (π )+π2 (π )) ππ . (57) Similarly, we have σ΅¨σ΅¨ VσΈ (π‘) V2σΈ (π‘) σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ 1 σ΅©σ΅© σ΅©σ΅© σ΅¨σ΅¨ σ΅¨ − σ΅¨σ΅¨ 1 + π‘πΌ−1 1 + π‘πΌ−1 σ΅¨σ΅¨σ΅¨ ≤ max {πΏ 1 , πΏ 2 } σ΅©σ΅©π₯1 − π₯2 σ΅©σ΅© σ΅¨ σ΅¨ ×∫ +∞ (1 + π πΌ−1 ) (π1 (π ) + π2 (π )) ππ . (58) Therefore, σ΅© σ΅© σ΅©σ΅© σ΅© σ΅©σ΅©V1 − V2 σ΅©σ΅©σ΅© ≤ max {πΏ 1 , πΏ 2 } σ΅©σ΅©σ΅©π₯1 − π₯2 σ΅©σ΅©σ΅© +∞ (52) (55) Define 0 π‘ ∈ [0, +∞) . (54) hence π» has nonempty closed values. Moreover, since π» is measurable (e.g., Proposition III. 4 in [35]), there exists π2 which is a measurable selection of π». It follows that π2 ∈ ππΉ (π’2 ) and for any π‘ ∈ [0, +∞), (51) that is, π’0 ∈ π(π’) and π(π’) is closed. Next we show that π is a contraction on π΄πΆ1 ([0, +∞), R). Let π’1 , π’2 ∈ π΄πΆ1 ([0, +∞), R) and V1 ∈ π(π’1 ). Then there exist π1 ∈ ππΉ (π’1 ) such that V1 (π‘) = ∫ σ΅¨ σ΅¨ σ΅¨ σ΅¨ ∩ {π’ ∈ R; σ΅¨σ΅¨σ΅¨π1 (π‘) − π’σ΅¨σ΅¨σ΅¨ ≤ π1 (π‘) σ΅¨σ΅¨σ΅¨π₯1 − π₯2 σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ +π2 (π‘) σ΅¨σ΅¨σ΅¨σ΅¨π₯1σΈ − π₯2σΈ σ΅¨σ΅¨σ΅¨σ΅¨} , π‘ ∈ [0, +∞) . By (H5), we have σ΅¨ σ΅¨ ππ» (πΉ (π‘, π₯1 , π¦1 ) , πΉ (π‘, π₯2 , π¦2 )) ≤ π1 (π‘) σ΅¨σ΅¨σ΅¨π₯1 − π₯2 σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ + π2 (π‘) σ΅¨σ΅¨σ΅¨π¦1 − π¦2 σ΅¨σ΅¨σ΅¨ +∞ π» (π‘) := πΉ (π‘, π’2 (π‘) , π’2σΈ (π‘)) (47) such that for almost all π‘ ∈ [0, +∞), max {πΏ 1 , πΏ 2 } (∫ Consider the set-valued map ×∫ 0 (1 + π πΌ−1 ) (π1 (π ) + π2 (π )) ππ . (59) 8 Advances in Mathematical Physics From an analogous reasoning by interchanging the roles of π’1 and π’2 , it follows that σ΅© σ΅© ππ» (π (π’1 ) , π (π’2 )) ≤ max {πΏ 1 , πΏ 2 } σ΅©σ΅©σ΅©π₯1 − π₯2 σ΅©σ΅©σ΅© ×∫ +∞ 0 (1 + π πΌ−1 ) (π1 (π ) + π2 (π )) ππ . 4. Application Consider the fractional boundary value problem, σΈ π·05/2 + π’ (π‘) + πΉ (π‘, π’ (π‘) , π’ (π‘)) ∋ 0, 0 < π‘ < +∞, 1 1 1 π’ (0) = π’σΈ (0) = 0, π·3/2 π’ (+∞) − π’ ( ) − π’ (1) = 0. 8 8 4 (61) Here π = 4, πΌ = 5/2, π½1 = 1/8, π½2 = 1/4, π1 = 1/8, and π2 = 1, and πΉ : πΌ × R × R → P(R) is a multivalued map given by 3/2 πΉ (π‘, π₯, π¦) = [π (1 + π‘ σ΅¨5 σ΅¨σ΅¨ σ΅¨σ΅¨π₯ + π¦σ΅¨σ΅¨σ΅¨ ) (σ΅¨ + 9) , σ΅¨σ΅¨π₯ + π¦σ΅¨σ΅¨σ΅¨5 + 5 σ΅¨ σ΅¨ σ΅¨3 σ΅¨σ΅¨ σ΅¨π₯ + π¦σ΅¨σ΅¨ 2π−π‘ (1 + π‘3/2 ) ( σ΅¨ σ΅¨ σ΅¨3 σ΅¨ + 1)] . σ΅¨σ΅¨π₯ + π¦σ΅¨σ΅¨ + 3 σ΅¨ σ΅¨ (62) For V ∈ πΉ, we have σ΅¨5 σ΅¨σ΅¨ σ΅¨σ΅¨ V (π‘) σ΅¨σ΅¨ σ΅¨σ΅¨π₯ + π¦σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ −π‘ + 9) , σ΅¨ ≤ max (π ( σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘3/2 σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨π₯ + π¦σ΅¨σ΅¨σ΅¨5 + 5 σ΅¨ σ΅¨ σ΅¨3 σ΅¨σ΅¨ σ΅¨π₯ + π¦σ΅¨σ΅¨ 2π−π‘ ( σ΅¨ σ΅¨ σ΅¨3 σ΅¨ + 1)) σ΅¨σ΅¨π₯ + π¦σ΅¨σ΅¨ + 3 σ΅¨ σ΅¨ ≤ 10π−π‘ , (63) π₯, π¦ ∈ R. Thus, σ΅¨σ΅¨ V (π‘) σ΅¨σ΅¨ σ΅© σ΅¨ σ΅¨σ΅¨ σ΅©σ΅© σ΅¨ : V ∈ πΉ (π‘, π₯, π¦)} σ΅©σ΅©πΉ(π‘, π₯, π¦)σ΅©σ΅©σ΅©P := sup {σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ 1 + π‘3/2 σ΅¨σ΅¨σ΅¨ −π‘ ≤ 10π = π (π‘) π (βπ₯β) , (64) π₯, π¦ ∈ R, with π(π‘) = π−π‘ , π(βπ₯β) = 10. Also, by direct calculation, we can obtain that πΏ 1 = 1.01529 and πΏ 2 = 3.045869. Further, by using the following condition: π The authors thank the referees for their careful reading of this paper and useful suggestions. This paper was funded by King Abdulaziz University, under Grant no. (130-1-1433/HiCi). The authors, therefore, acknowledge technical and financial support of KAU. (60) Since π is a contraction, it follows by the Lemma 23 that π admits a fixed point which is a solution to problem (1). −π‘ Acknowledgments +∞ max {πΏ 1 , πΏ 2 } π (π) ∫0 π (π ) ππ > 1, (65) we find that π > 30.45869. Clearly, all the conditions of Theorem 21 are satisfied. So, there exists at least one solution of problem (1) on πΌ. References [1] S. Liang and J. 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