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# Nonlinear fractional differential equations with nonlocal fractional integro-differential boundary conditions

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Department of Mathematics, Faculty of Science, King Abdulaziz University, P.O. Box 80203, Jeddah, 21589, Saudi Arabia

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Boundary Value Problems 2012, 2012:124  doi:10.1186/1687-2770-2012-124

 Received: 23 July 2012 Accepted: 4 October 2012 Published: 24 October 2012

This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

### Abstract

We study the existence of solutions for a class of nonlinear Caputo-type fractional boundary value problems with nonlocal fractional integro-differential boundary conditions. We apply some fixed point principles and Leray-Schauder degree theory to obtain the main results. Some examples are discussed for the illustration of the main work.

MSC: 34A08, 34A12, 34B15.

##### Keywords:
fractional differential equations; fractional boundary conditions; separated boundary conditions; fixed point theorems

### 1 Introduction

Nonlocal boundary value problems of fractional differential equations have been extensively studied in the recent years. In fact, the subject of fractional calculus has been quite attractive and exciting due to its applications in the modeling of many physical and engineering problems. For theoretical and practical development of the subject, we refer to the books [1-5]. Some recent results on fractional boundary value problems can be found in [6-14] and references therein. In [11], the authors studied a boundary value problem of fractional differential equations with fractional separated boundary conditions.

In this article, motivated by [11], we consider a fractional boundary value problem with fractional integro-differential boundary conditions given by

{ D α c x ( t ) = f ( t , x ( t ) ) , 1 < α 2 , t [ 0 , 1 ] , α 1 x ( 0 ) + β 1 ( c D p x ( 0 ) ) = γ 1 0 η ( η s ) α 2 Γ ( α 1 ) x ( s ) d s , 0 < p < 1 , α 2 x ( 1 ) + β 2 ( c D p x ( 1 ) ) = γ 2 0 σ ( σ s ) α 2 Γ ( α 1 ) x ( s ) d s , 0 < η , σ < 1 , (1.1)

where D α c denotes the Caputo fractional derivative of order α, f is a given continuous function, and α i , β i , γ i ( i = 1 , 2 ) are suitably chosen real constants.

The main aim of the present study is to obtain some existence results for the problem (1.1). As a first step, we transform the given problem to a fixed point problem and show the existence of fixed points for the transformed problem which in turn correspond to the solutions of the actual problem. The methods used to prove the existence results are standard; however, their exposition in the framework of the problem (1.1) is new.

### 2 Preliminaries

Let us recall some basic definitions of fractional calculus [1,2].

Definition 2.1 For ( n 1 ) -times absolutely continuous function g : [ 0 , ) R , the Caputo derivative of fractional order q is defined as

D q c g ( t ) = 1 Γ ( n q ) 0 t ( t s ) n q 1 g ( n ) ( s ) d s , n 1 < q < n , n = [ q ] + 1 ,

where [ q ] denotes the integer part of the real number q.

Definition 2.2 The Riemann-Liouville fractional integral of order q is defined as

I q g ( t ) = 1 Γ ( q ) 0 t g ( s ) ( t s ) 1 q d s , q > 0 ,

provided the integral exists.

To define the solution of the boundary value problem (1.1), we need the following lemma, which deals with a linear variant of the problem (1.1).

Lemma 2.3For a given y C ( [ 0 , 1 ] , R ) , the unique solution of the linear fractional boundary value problem

{ D α c x ( t ) = y ( t ) , 1 < α 2 , α 1 x ( 0 ) + β 1 ( c D p x ( 0 ) ) = γ 1 0 η ( η s ) α 2 Γ ( α 1 ) x ( s ) d s , 0 < p < 1 , α 2 x ( 1 ) + β 2 ( c D p x ( 1 ) ) = γ 2 0 σ ( σ s ) α 2 Γ ( α 1 ) x ( s ) d s , 0 < η , σ < 1 (2.1)

is given by

x ( t ) = 0 t ( t s ) α 1 Γ ( α ) y ( s ) d s + μ 1 ( t ) 0 η ( η s ) 2 α 2 Γ ( 2 α 1 ) y ( s ) d s + μ 2 ( t ) { γ 2 0 σ ( σ s ) 2 α 2 Γ ( 2 α 1 ) y ( s ) d s β 2 0 1 ( 1 s ) α p 1 Γ ( α p ) y ( s ) d s α 2 0 1 ( 1 s ) α 1 Γ ( α ) y ( s ) d s } , (2.2)

where

μ 1 ( t ) = γ 1 ( Δ 1 Δ 2 t ) , μ 2 ( t ) = γ 1 Δ 3 + Δ 4 t , Δ 1 = 1 Δ ( α 2 γ 2 σ α Γ ( α + 1 ) + β 2 Γ ( 2 p ) ) , Δ 2 = 1 Δ ( α 2 γ 2 σ α 1 Γ ( α ) ) , Δ 3 = η α Δ Γ ( α + 1 ) , Δ 4 = 1 Δ ( α 1 γ 1 η α 1 Γ ( α ) ) , Δ = ( α 1 γ 1 η α 1 Γ ( α ) ) ( α 2 γ 2 σ α Γ ( α + 1 ) + β 2 Γ ( 2 p ) ) + γ 1 η α Γ ( α + 1 ) ( α 2 γ 2 σ α 1 Γ ( α ) ) 0 . (2.3)

Proof It is well known [2] that the solution of the fractional differential equation in (2.1) can be written as

x ( t ) = 0 t ( t s ) α 1 Γ ( α ) y ( s ) d s + c 0 + c 1 t . (2.4)

Using D p c b = 0 (b is a constant), D p c t = t 1 p Γ ( 2 p ) , D p c I q y ( t ) = I q p y ( t ) , (2.4) gives

D p c x ( t ) = 0 t ( t s ) α p 1 Γ ( α p ) y ( s ) d s c 1 t 1 p Γ ( 2 p ) . (2.5)

Using the integral boundary conditions of the problem (2.1) together with (2.3), (2.4), and (2.5) yields

c 0 = 1 Δ { γ 1 ( α 2 γ 2 σ α Γ ( α + 1 ) + β 2 Γ ( 2 p ) ) 0 η ( η s ) 2 α 2 Γ ( 2 α 1 ) y ( s ) d s + γ 1 η α Γ ( α + 1 ) ( γ 2 0 σ ( σ s ) 2 α 2 Γ ( 2 α 1 ) y ( s ) d s β 2 0 1 ( 1 s ) α p 1 Γ ( α p ) y ( s ) d s α 2 0 1 ( 1 s ) α 1 Γ ( α ) y ( s ) d s ) } , c 1 = 1 Δ { γ 1 ( α 2 γ 2 σ α 1 Γ ( α ) ) 0 η ( η s ) 2 α 2 Γ ( 2 α 1 ) y ( s ) d s + ( α 1 γ 1 η α 1 Γ ( α ) ) ( γ 2 0 σ ( σ s ) 2 α 2 Γ ( 2 α 1 ) y ( s ) d s β 2 0 1 ( 1 s ) α p 1 Γ ( α p ) y ( s ) d s α 2 0 1 ( 1 s ) α 1 Γ ( α ) y ( s ) d s ) } .

Substituting the values of c 0 , c 1 in (2.4), we get (2.2). This completes the proof. □

Remark 2.4 Notice that the solution (2.2) is independent of the parameter β 1 , which distinguishes the present work from the one containing the fractional differential equation of (2.1) with the boundary conditions of the form:

α 1 x ( 0 ) + β 1 x ( 0 ) = γ 1 0 η ( η s ) α 2 Γ ( α 1 ) x ( s ) d s , α 2 x ( 1 ) + β 2 x ( 1 ) = γ 2 0 σ ( σ s ) α 2 Γ ( α 1 ) x ( s ) d s . (2.6)

In case β 1 = 0 = β 2 , the boundary conditions in (2.1) coincide with (2.6) and consequently the corresponding solutions become identical.

### 3 Main results

Let C = C ( [ 0 , 1 ] , R ) denote the Banach space of all continuous functions from [ 0 , 1 ] into ℝ endowed with the usual supremum norm.

In view of Lemma 2.3, we define an operator F : C C by

( F x ) ( t ) = 0 t ( t s ) α 1 Γ ( α ) f ( s , x ( s ) ) d s + μ 1 ( t ) 0 η ( η s ) 2 α 2 Γ ( 2 α 1 ) f ( s , x ( s ) ) d s + μ 2 ( t ) { γ 2 0 σ ( σ s ) 2 α 2 Γ ( 2 α 1 ) f ( s , x ( s ) ) d s β 2 0 1 ( 1 s ) α p 1 Γ ( α p ) f ( s , x ( s ) ) d s α 2 0 1 ( 1 s ) α 1 Γ ( α ) f ( s , x ( s ) ) d s } . (3.1)

Observe that the problem (1.1) has solutions if and only if the operator equation F x = x has fixed points.

In the sequel, we use the following notation:

ω = max t [ 0 , 1 ] { t α Γ ( α + 1 ) + | μ 1 ( t ) | η 2 α 1 Γ ( 2 α ) + | μ 2 ( t ) | ( | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | Γ ( α p + 1 ) + | α 2 | Γ ( α + 1 ) ) } = 1 + | α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) , (3.2)

where μ ˜ 1 = | γ 1 | ( | Δ 1 | + | Δ 2 | ) , μ ˜ 2 = | γ 1 Δ 3 | + | Δ 4 | with Δ i ( i = 1 , 2 , 3 , 4 ) given by (2.3).

Our first result is based on the Leray-Schauder nonlinear alternative [15].

Lemma 3.1 (Nonlinear alternative for single valued maps)

LetEbe a Banach space, Ca closed, convex subset ofE, Uan open subset ofC, and 0 U . Suppose that F : U ¯ C is a continuous, compact (that is, F ( U ¯ ) is a relatively compact subset ofC) map. Then either

(i) Fhas a fixed point in U ¯ , or

(ii) there is a u U (the boundary ofUinC) and λ ( 0 , 1 ) with u = λ F ( u ) .

Theorem 3.2Let f : [ 0 , 1 ] × R R be a jointly continuous function. Assume that:

( A 1 ) there exist a function p C ( [ 0 , 1 ] , R + ) and a nondecreasing function ψ : R + R + such that | f ( t , x ) | p ( t ) ψ ( x ) , ( t , x ) [ 0 , 1 ] × R ;

( A 2 ) there exists a constant M > 0 such that

M ψ ( M ) { 1 + | α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) } p > 1 .

Then the boundary value problem (1.1) has at least one solution on [ 0 , 1 ] .

Proof Consider the operator F : C C defined by (3.1). We show that Fmaps bounded sets into bounded sets in C ( [ 0 , 1 ] , R ) . For a positive number r, let B r = { x C ( [ 0 , 1 ] , R ) : x r } be a bounded set in C ( [ 0 , 1 ] , R ) . Then

F x sup t [ 0 , 1 ] { 0 t ( t s ) α 1 Γ ( α ) | f ( s , x ( s ) ) | d s + | μ 1 ( t ) | 0 η ( η s ) 2 α 2 Γ ( 2 α 1 ) | f ( s , x ( s ) ) | d s + | μ 2 ( t ) | ( | γ 2 | 0 σ ( σ s ) 2 α 2 Γ ( 2 α 1 ) | f ( s , x ( s ) ) | d s + | β 2 | 0 1 ( 1 s ) α p 1 Γ ( α p ) | f ( s , x ( s ) ) | d s + | α 2 | 0 1 ( 1 s ) α 1 Γ ( α ) | f ( s , x ( s ) ) | d s ) } ψ ( r ) { 1 + | α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) } p .

Next, we show that Fmaps bounded sets into equicontinuous sets of C ( [ 0 , 1 ] , R ) . Let t , t [ 0 , 1 ] with t < t and x B r , where B r is a bounded set of C ( [ 0 , 1 ] , R ) . Then we obtain

| ( F x ) ( t ) ( F x ) ( t ) | = | 1 Γ ( q ) 0 t ( t s ) q 1 f ( s , x ( s ) ) d s 1 Γ ( q ) 0 t ( t s ) q 1 f ( s , x ( s ) ) d s γ 1 Δ 2 ( t t ) 0 η ( η s ) 2 α 2 Γ ( 2 α 1 ) f ( s , x ( s ) ) d s + Δ 4 ( t t ) { γ 2 0 σ ( σ s ) 2 α 2 Γ ( 2 α 1 ) f ( s , x ( s ) ) d s β 2 0 1 ( 1 s ) α p 1 Γ ( α p ) f ( s , x ( s ) ) d s α 2 0 1 ( 1 s ) α 1 Γ ( α ) f ( s , x ( s ) ) d s } | 1 Γ ( q ) 0 t | ( t s ) q 1 ( t s ) q 1 | ψ ( r ) p ( s ) d s + 1 Γ ( q ) t t | t s | q 1 ψ ( r ) p ( s ) d s + | γ 1 Δ 2 ( t t ) | 0 η | η s | 2 α 2 Γ ( 2 α 1 ) ψ ( r ) p ( s ) d s + | Δ 4 ( t t ) | { | γ 2 | 0 σ | σ s | 2 α 2 Γ ( 2 α 1 ) ψ ( r ) p ( s ) d s | β 2 | 0 1 | 1 s | α p 1 Γ ( α p ) ψ ( r ) p ( s ) d s | α 2 | 0 1 | 1 s | α 1 Γ ( α ) ψ ( r ) p ( s ) d s } .

Obviously, the right-hand side of the above inequality tends to zero independently of x B r as t t 0 . As ℱ satisfies the above assumptions, therefore, it follows by the Arzelá-Ascoli theorem that F : C ( [ 0 , 1 ] , R ) C ( [ 0 , 1 ] , R ) is completely continuous.

Let x be a solution. Then for t [ 0 , 1 ] , using the computations in proving that ℱ is bounded, we have

| x ( t ) | = | λ ( F x ) ( t ) | ψ ( x ) { 1 + | α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) } p .

Consequently, we have

x ψ ( x ) { 1 + | α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) } p 1 .

In view of ( A 2 ), there exists M such that x M . Let us set

U = { x C ( [ 0 , 1 ] , R ) : x < M + 1 } .

Note that the operator F : U ¯ C ( [ 0 , 1 ] , R ) is continuous and completely continuous. From the choice of U, there is no x U such that x = λ F ( x ) for some λ ( 0 , 1 ) . Consequently, by the nonlinear alternative of Leray-Schauder type (Lemma 3.1), we deduce that ℱ has a fixed point x U ¯ which is a solution of the problem (1.1). This completes the proof. □

In the special case when p ( t ) = 1 and ψ ( | x | ) = κ | x | + N (κ and N are suitable constants) in the statement of Theorem 3.2, we have the following corollary.

Corollary 3.3Let f : [ 0 , 1 ] × R R be a continuous function. Assume that there exist constants 0 κ < 1 / ω , whereωis given by (3.2) and N > 0 such that | f ( t , x ) | κ | x | + N for all t [ 0 , 1 ] , x C [ 0 , 1 ] . Then the boundary value problem (1.1) has at least one solution.

Next, we prove an existence and uniqueness result by means of Banach’s contraction mapping principle.

Theorem 3.4Suppose that f : [ 0 , 1 ] × R R is a continuous function and satisfies the following assumption:

( A 3 ) | f ( t , x ) f ( t , y ) | L | x y | , t [ 0 , 1 ] , L > 0 , x , y R .

Then the boundary value problem (1.1) has a unique solution provided

ω < 1 / L , (3.3)

whereωis given by (3.2).

Proof With r M ω / ( 1 L ω ) , we define B r = { x F : x r } , where M = sup t [ 0 , 1 ] | f ( t , 0 ) | < and ω is given by (3.2). Then we show that F B r B r . For x B r , we have

F x = sup t [ 0 , 1 ] | ( F x ) ( t ) | sup t [ 0 , 1 ] { 0 t ( t s ) α 1 Γ ( α ) | f ( s , x ( s ) ) | d s + | μ 1 ( t ) | 0 η ( η s ) 2 α 2 Γ ( 2 α 1 ) | f ( s , x ( s ) ) | d s + | μ 2 ( t ) | ( | γ 2 | 0 σ ( σ s ) 2 α 2 Γ ( 2 α 1 ) | f ( s , x ( s ) ) | d s + | β 2 | 0 1 ( 1 s ) α p 1 Γ ( α p ) | f ( s , x ( s ) ) | d s + | α 2 | 0 1 ( 1 s ) α 1 Γ ( α ) | f ( s , x ( s ) ) | d s ) } .

Using | f ( s , x ( s ) ) | | f ( s , x ( s ) ) f ( s , 0 ) | + | f ( s , 0 ) | L x + M L r + M , the above expression yields

F x ( L r + M ) sup t [ 0 , 1 ] { 0 t ( t s ) α 1 Γ ( α ) d s + | μ 1 ( t ) | 0 η ( η s ) 2 α 2 Γ ( 2 α 1 ) d s + | μ 2 ( t ) | ( | γ 2 | 0 σ ( σ s ) 2 α 2 Γ ( 2 α 1 ) d s + | β 2 | 0 1 ( 1 s ) α p 1 Γ ( α p ) d s + | α 2 | 0 1 ( 1 s ) α 1 Γ ( α ) d s ) } ( L r + M ) { 1 + | α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) } = ( L r + M ) ω r ,

where we used (3.2). Now, for x , y C and for each t [ 0 , 1 ] , we obtain

( F x ) ( t ) ( F y ) ( t ) sup t [ 0 , 1 ] { 0 t ( t s ) α 1 Γ ( α ) | f ( s , x ( s ) ) f ( s , y ( s ) ) | d s + | μ 1 ( t ) | 0 η ( η s ) 2 α 2 Γ ( 2 α 1 ) | f ( s , x ( s ) ) f ( s , y ( s ) ) | d s + | μ 2 ( t ) | ( | γ 2 | 0 σ ( σ s ) 2 α 2 Γ ( 2 α 1 ) | f ( s , x ( s ) ) f ( s , y ( s ) ) | d s + | β 2 | 0 1 ( 1 s ) α p 1 Γ ( α p ) | f ( s , x ( s ) ) f ( s , y ( s ) ) | d s + | α 2 | 0 1 ( 1 s ) α 1 Γ ( α ) | f ( s , x ( s ) ) f ( s , y ( s ) ) | d s ) } L { 1 + | α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) } x y = L ω x y .

Note that ω depends only on the parameters involved in the problem. As L ω < 1 , therefore, ℱ is a contraction. Hence, by Banach’s contraction mapping principle, the problem (1.1) has a unique solution on [ 0 , 1 ] . □

Now, we prove the existence of solutions of (1.1) by applying Krasnoselskii’s fixed point theorem [16].

Theorem 3.5 (Krasnoselskii’s fixed point theorem)

LetMbe a closed, bounded, convex, and nonempty subset of a Banach spaceX. LetA, Bbe the operators such that (i) A x + B y M whenever x , y M ; (ii) Ais compact and continuous; (iii) Bis a contraction mapping. Then there exists z M such that z = A z + B z .

Theorem 3.6Let f : [ 0 , 1 ] × R R be a jointly continuous function satisfying the assumption ( A 3 ). In addition we assume that:

( A 4 ) | f ( t , x ) | μ ( t ) , ( t , x ) [ 0 , 1 ] × R , and μ C ( [ 0 , 1 ] , R + ) .

Then the problem (1.1) has at least one solution on [ 0 , 1 ] if

| α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) < 1 . (3.4)

Proof Letting sup t [ 0 , 1 ] | μ ( t ) | = μ , we choose a real number r ¯ satisfying the inequality

r ¯ μ [ 1 + | α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) ] ,

and consider B r ¯ = { x C : x r ¯ } . We define the operators P and Q on B r ¯ as

( P x ) ( t ) = 0 t ( t s ) α 1 Γ ( α ) f ( s , x ( s ) ) d s , ( Q x ) ( t ) = μ 1 ( t ) 0 η ( η s ) 2 α 2 Γ ( 2 α 1 ) f ( s , x ( s ) ) d s + μ 2 ( t ) ( γ 2 0 σ ( σ s ) 2 α 2 Γ ( 2 α 1 ) f ( s , x ( s ) ) d s β 2 0 1 ( 1 s ) α p 1 Γ ( α p ) f ( s , x ( s ) ) d s α 2 0 1 ( 1 s ) α 1 Γ ( α ) f ( s , x ( s ) ) d s ) .

For x , y B r ¯ , we find that

P x + Q y μ [ 1 + | α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) ] r ¯ .

Thus, P x + Q y B r ¯ . It follows from the assumption ( A 3 ) together with (3.4) that Q is a contraction mapping. Continuity of f implies that the operator P is continuous. Also, P is uniformly bounded on B r ¯ as

P x μ Γ ( q + 1 ) .

Now, we prove the compactness of the operator P .

In view of ( A 1 ), we define sup ( t , x ) [ 0 , 1 ] × B r ¯ | f ( t , x ) | = f ¯ , and consequently, for t 1 , t 2 [ 0 , 1 ] , we have

| ( P x ) ( t 1 ) ( P x ) ( t 2 ) | = | 1 Γ ( q ) 0 t 1 [ ( t 2 s ) q 1 ( t 1 s ) q 1 ] f ( s , x ( s ) ) d s + t 1 t 2 ( t 2 s ) q 1 f ( s , x ( s ) ) d s | f ¯ Γ ( q + 1 ) [ 2 ( | t 2 t 1 | ) q + | t 1 q t 2 q | ] ,

which is independent of x. Thus, P is equicontinuous. Hence, by the Arzelá-Ascoli theorem, P is compact on B r ¯ . Thus, all the assumptions of Theorem 3.5 are satisfied. So, the conclusion of Theorem 3.5 implies that the boundary value problem (1.1) has at least one solution on [ 0 , 1 ] . □

### 4 Examples

Example 4.1 Consider the following boundary value problem:

{ D 3 / 2 c x ( t ) = 1 ( 12 π ) sin ( 2 π x ) + | x | 1 + | x | + 1 30 | x | + t 2 + 2 , t [ 0 , 1 ] , x ( 0 ) + 3 ( c D 1 / 3 x ( 0 ) ) = 0 1 / 4 ( 1 / 4 s ) 1 / 2 Γ ( 1 / 2 ) x ( s ) d s , x ( 1 ) + 2 ( c D 1 / 3 x ( 1 ) ) = 3 0 3 / 4 ( 3 / 4 s ) 1 / 2 Γ ( 1 / 2 ) x ( s ) d s . (4.1)

Here, α = 3 / 2 , p = 1 / 3 , α 1 = 1 , β 1 = 3 , γ 1 = 1 , η = 1 / 4 , α 2 = 1 , β 2 = 2 , γ 2 = 3 , σ = 3 / 4 , and

ω = 1 + | α 2 | μ ˜ 2 Γ ( α + 1 ) + μ ˜ 1 η 2 α 1 + μ ˜ 2 | γ 2 | σ 2 α 1 Γ ( 2 α ) + | β 2 | μ ˜ 2 Γ ( α p + 1 ) 3.578386 .

Clearly,

| f ( t , x ) | = | 1 ( 12 π ) sin ( 2 π x ) + | x | 1 + | x | + 1 30 | x | + t 2 + 2 | 1 5 | x | + 4 .

Clearly, N = 4 and

κ = 1 5 < 1 ω = 1 3.578386 .

Thus, all the conditions of Corollary 3.3 are satisfied and consequently the problem (4.1) has at least one solution.

Example 4.2 Consider the following fractional boundary value problem:

{ D 3 / 2 c x ( t ) = L 2 ( x + tan 1 x ) + t ( t + 3 ) t 4 + 2 , t [ 0 , 1 ] , x ( 0 ) + 3 ( c D 1 / 3 x ( 0 ) ) = 0 1 / 4 ( 1 / 4 s ) 1 / 2 Γ ( 1 / 2 ) x ( s ) d s , x ( 1 ) + 2 ( c D 1 / 3 x ( 1 ) ) = 3 0 3 / 4 ( 3 / 4 s ) 1 / 2 Γ ( 1 / 2 ) x ( s ) d s , (4.2)

where α, p, α i , β i , γ i , ( i = 1 , 2 ) η, σ are the same as given in (4.1) and f ( t , x ) = L 2 ( x + tan 1 x ) + t ( t + 3 ) t 4 + 2 . Clearly, | f ( t , x ) f ( t , y ) | L | x y | and thus, for L < 1 / ω = 1 / 3.578386 , all the conditions of Theorem 3.4 are satisfied. Hence, the boundary value problem (4.2) has a unique solution on [ 0 , 1 ] .

### Competing interests

The authors declare that they have no competing interests.

### Authors’ contributions

Each of the authors, BA and AA contributed to each part of this work equally and read and approved the final version of the manuscript.

### Acknowledgements

The authors thank the reviewers for their useful comments that led to the improvement of the original manuscript. This research was partially supported by the Deanship of Scientific Research (DSR), King Abdulaziz University, Jeddah, Saudi Arabia.

### References

1. Podlubny, I: Fractional Differential Equations, Academic Press, San Diego (1999)

2. Kilbas, AA, Srivastava, HM, Trujillo, JJ: Theory and Applications of Fractional Differential Equations, Elsevier, Amsterdam (2006)

3. Magin, RL: Fractional Calculus in Bioengineering, Begell House, Redding (2006)

4. Sabatier J, Agrawal OP, Machado JAT (eds.): Advances in Fractional Calculus: Theoretical Developments and Applications in Physics and Engineering, Springer, Dordrecht (2007)

5. Baleanu, D, Diethelm, K, Scalas, E, Trujillo, JJ: Fractional Calculus Models and Numerical Methods, World Scientific, Boston (2012)

6. Agarwal, RP, Belmekki, M, Benchohra, M: A survey on semilinear differential equations and inclusions involving Riemann-Liouville fractional derivative. Adv. Differ. Equ.. 2009, (2009) Article ID 981728

7. Baleanu, D, Mustafa, OG, Agarwal, RP: An existence result for a superlinear fractional differential equation. Appl. Math. Lett.. 23, 1129–1132 (2010). Publisher Full Text

8. Hernandez, E, O’Regan, D, Balachandran, K: On recent developments in the theory of abstract differential equations with fractional derivatives. Nonlinear Anal.. 73(10), 3462–3471 (2010). Publisher Full Text

9. Ahmad, B, Ntouyas, SK: A four-point nonlocal integral boundary value problem for fractional differential equations of arbitrary order. Electron. J. Qual. Theory Differ. Equ.. 2011, (2011) Article ID 22

10. Ahmad, B, Nieto, JJ: Riemann-Liouville fractional integro-differential equations with fractional nonlocal integral boundary conditions. Bound. Value Probl.. 2011, (2011) Article ID 36

11. Ahmad, B, Ntouyas, SK: A note on fractional differential equations with fractional separated boundary conditions. Abstr. Appl. Anal.. 2012, (2012) Article ID 818703

12. Aghajani, A, Jalilian, Y, Trujillo, JJ: On the existence of solutions of fractional integro-differential equations. Fract. Calc. Appl. Anal.. 15(2), 44–69 (2012)

13. Ahmad, B, Ntouyas, SK: Existence results for nonlocal boundary value problems for fractional differential equations and inclusions with strip conditions. Bound. Value Probl.. 2012, (2012) Article ID 55

14. Ahmad, B, Nieto, JJ: Anti-periodic fractional boundary value problem with nonlinear term depending on lower order derivative. Fract. Calc. Appl. Anal.. 15, 451–462 (2012)

15. Granas, A, Dugundji, J: Fixed Point Theory, Springer, New York (2005)

16. Krasnoselskii, MA: Two remarks on the method of successive approximations. Usp. Mat. Nauk. 10, 123–127 (1955)