Volume 2014, Issue 1 632434
Research Article
Open Access

Existence of Solutions for Two-Point Boundary Value Problem of Fractional Differential Equations at Resonance

Lei Hu

Corresponding Author

Lei Hu

Department of Mathematics, China University of Mining and Technology, Beijing 100083, China cumt.edu.cn

School of Science, Shandong Jiaotong University, Jinan, Shandong 250357, China sdjtu.edu.cn

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Shuqin Zhang

Shuqin Zhang

School of Science, Shandong Jiaotong University, Jinan, Shandong 250357, China sdjtu.edu.cn

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Ailing Shi

Ailing Shi

School of Science, Beijing University of Civil Engineering and Architecture, Beijing 100044, China bucea.edu.cn

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First published: 05 August 2014
Citations: 7
Academic Editor: Patricia J. Y. Wong

Abstract

We establish the existence results for two-point boundary value problem of fractional differential equations at resonance by means of the coincidence degree theory. Furthermore, a result on the uniqueness of solution is obtained. We give an example to demonstrate our results.

1. Introduction

Fractional differential equations have been studied extensively. It is caused both by the intensive development of the theory of fractional calculus itself and by the applications such as physics, chemistry, phenomena arising in engineering, economy, and science; see, for example, [15].

Recently, more and more authors have paid their attentions to the boundary value problems of fractional differential equations; see [621]. Moreover, there have been many works related to the existence of solutions for boundary value problems at resonance; see [1221]. It is considerable that there are many papers that have dealt with the solutions of multipoint boundary value problems of fractional differential equations at resonance (see, e.g., [12, 16]).

In [12], Bai and Zhang considered a three-point boundary value problem of fractional differential equations with nonlinear growth given by
(1)
where 1 < α ≤ 2, 0 < η, σ < 1 > 0, σηα−1 = 1, is Riemann-Liouville fractional derivative, and are given functions.
In [13], Hu et al. have studied a two-point boundary value problem for fractional differential equation at resonance
(2)
where 1 < α ≤ 2, is Caputo fractional derivative, and satisfies Carathéodory conditions.
As far as we know, there are few works on the existence of two-point boundary value problems of the fractional differential equations at resonance. Motivated by the works above, we discuss the existence and uniqueness of solutions for the following nonlinear fractional differential equation:
(3)
where 0 < t < 1, N − 1 < α < N, is Riemann-Liouville fractional derivative, and is continuous function.

More precisely, we use the coincidence degree theorem due to Mawhin [22]. The rest of this paper is organized as follows. In Section 2, we give some necessary notations, definitions, and lemmas. In Section 3, we study the existence of solutions of (3) by the coincidence degree theory. Finally, an example is given to illustrate our results in Section 4.

The two-point boundary value problem (3) happens to be at resonance in the sense that the associated linear homogeneous boundary value problem
(4)
has u(t) = c1tα−1 as a nontrivial solution.

2. Preliminaries

In this section, we present the necessary definitions and lemmas from fractional calculus theory. These definitions and properties can be found in the literature. For more details see [13].

Definition 1 (see [1].)The Riemann-Liouville fractional integral of order α > 0 of a function is given by

(5)
provided that the right-hand side is pointwise defined on (0, ).

Definition 2 (see [1].)The Riemann-Liouville fractional derivative of order α > 0 of a continuous function is given by

(6)
where n − 1 < αn, provided that the right-hand side is pointwise defined on (0, ).

Lemma 3 (see [1].)Let n − 1 < αn, uC(0,1) ⋂ L1(0,1); then

(7)
where , i = 1,2, …n.

Lemma 4 (see [1].)If α > 0, and D = d/dx. If the fractional derivatives and exist, then

(8)

Lemma 5 (see [1].)The relation

(9)
is valid in following cases β > 0, α + β > 0, and f(x) ∈ L1(a, b).

Now let us recall some notations about the coincidence degree continuation theorem.

Let Y, Z be real Banach spaces, let L : dom⁡LYZ be a Fredholm map of index zero, and let P : YY, Q : ZZ be continuous projectors such that kerL = ImP, ImL = kerQ, and Y = kerLkerP, Z = ImLImQ. It follows that L|dom⁡LkerP : dom⁡LkerPImL is invertible. We denote the inverse of this map by KP. If Ω is an open bounded subset of Y, the map N will be called L-compact on if is bounded and is compact.

Theorem 6. Let L be a Fredholm operator of index zero and N be L-compact on . Suppose that the following conditions are satisfied:

  • (1)

    LxλNx for each (x, λ) ∈ [(dom⁡LkerL)∩Ω] × (0,1);

  • (2)

    NxImL for each xkerLΩ;

  • (3)

    deg⁡(JQN|kerL, ΩkerL, 0) ≠ 0, where Q : ZZ is a continuous projection as above with ImL = kerQ and J : ImQkerL is any isomorphism.

Then the equation Lx = Nx has at least one solution in .

3. Main Results

In this section, we will prove the existence results for (3).

We use the Banach space E = C[0,1] with the norm ∥u = max⁡0≤t≤1|u(t)|. For α > 0, N = [α] + 1, we define a linear space
(10)
By means of the functional analysis theory, we can prove that X is a Banach space with the norm .
Define L to be the linear operator from dom⁡(L) ⋂ X to E with and
(11)
We define N : XE by
(12)
Then the problem (3) can be written by Lu = Nu.

Lemma 7. The mapping L : dom⁡(L) ⊂ E is a Fredholm operator of index zero.

Proof. It is clear that

(13)
Let xImL, so there exists a function u ∈ dom⁡L which satisfies Lu = x. By (11) and Lemma 3, we have
(14)
By , we can obtain c2 = ⋯ = cN = 0. Hence
(15)
Then, we have
(16)
Taking into account , we obtain
(17)
On the other hand, suppose x satisfy . Let , we can easily prove u(t) ∈ dom⁡(L).

Thus, we conclude that

(18)
Consider the linear operators Q : EE defined by
(19)
Take x(t) ∈ E; then
(20)
We can see Q2 = Q.

For x(t) ∈ E in the type x(t) = x(t) − Qx(t) + Qx(t), obviously, x(t) − Qx(t) ∈ Ker⁡(Q) = Im⁡(L) and Qx(t) ∈ Im⁡(Q). That is to say, E = Im⁡(L) + Im⁡(Q). If uIm⁡(L) ⋂ Im⁡(Q), we have u = c1; then . As a result c1 = 0, and we get E = Im⁡(L) ⊕ Im⁡(Q).

Note that Ind L = dim⁡ kerL − codim ImL = 0. Then L is a Fredholm mapping of index zero.

We can define the operators P : XX, where
(21)
For uX,
(22)
So we have P2 = P.
Note that
(23)
Since u = uPu + Pu, it is easy to say that uPu ∈ Ker⁡(P) and Pu ∈ Ker⁡(L). So we have X = Ker⁡(P) + Ker⁡(L). If u ∈ Ker⁡(L) ⋂ Ker⁡(P), then u = c1tα−1. We can derive c1 = 0 from . Then
(24)
For uX,
(25)
where .

We define KP : ImL → dom⁡LkerP by .

For xIm⁡(L), we have
(26)
For u ∈ dom⁡(L) ⋂ Ker⁡(P), we have . And for u ∈ dom⁡(L), the coefficients c1, …, cN in the expressions
(27)
are all equal to zero. Thus, we obtain
(28)
This shows that . Again for each xIm⁡(L),
(29)
where .

Lemma 8. Assume ΩY is an open bounded subset such that dom⁡LY; then map N is L-compact on

Proof. By the continuity of f, we can get that and are bounded. So, in view of the Arzela-Ascoli theorem, we need only to prove that is equicontinuous. From the continuity of f, there exists a constant r > 0, such that |(IQ)N(u(t))| ≤ r, for all , t ∈ [0,1].

For 0 ≤ t1t2 ≤ 1, uΩ, we have

(30)
Furthermore, we have
(31)
where i = 1,2, …, N − 1. Since tα and ti are uniformly continuous on [0,1], we can get that is compact. The proof is completed.

To obtain our main results, we need the following conditions.
  • (H1)

    There exist functions φ, ψiL1[0,1], i = 1, N, such that for all , t ∈ [0,1],

    (32)

  • (H2)

    There exists a constant A > 0 such that for every , if |x2| > A for all t ∈ [0,1], then

    (33)

  • (H3)

    There exists a constant D > 0 such that, for each ci, i = 1,2 satisfying min⁡{|c1|, |c2|} > D. We have either at least one of the following:

    (34)

  • or

    (35)

  • (H4)

    , where , i = 1,2, …, N.

Lemma 9. Ω1 = {u ∈ dom⁡(L)∖Ker⁡(L)∣Lu = λNu, λ ∈ [0,1]} is bounded.

Proof. For uΩ1, λ ≠ 0 and Lu = λNu. By (12), Lu = λNuIm⁡(L) = Ker⁡(Q); that is,

(36)
By the integral mean value theorem, there exits a constant t0 ∈ [0,1] such that
(37)
Form (H2), we can get .

Again for uΩ1, (IP)u ∈ dom⁡(L)∖Ker⁡(L) and LPu = 0. From (29), we have

(38)
Now by Lemma 4
(39)
That is,
(40)
From (25) and (38), we have
(41)
Furthermore, it follows from (40) and (H1) that
(42)
By the definition ∥uX and (H4), it is easy to see that and ∥u are bounded. So, Ω1 is bounded.

Lemma 10. Ω2 = {u ∈ Ker⁡(L) : NuIm⁡(L)} is bounded.

Proof. Let u ∈ Ker⁡(L), so we have u = c1tα−1, . For NuIm⁡(L) = Ker⁡(Q),

(43)
By the integral mean value theorem, there exits a constant t1 ∈ [0,1] such that
(44)
From (H2), it follows that |c1| ≤ A/Γ(α). Hence, Ω2 is bounded.

Lemma 11. Ω3 = {u ∈ Ker⁡(L) : λu + (1 − λ)QNu = 0,  λ ∈ [0,1]} is bounded.

Proof. Let u ∈ Ker⁡(L), so we have u = c1tα−1, . If λ = 0, then |c1| ≤ D. If λ = 1, we have c1 = 0.

If λ ≠ 0 and λ ≠ 1, then

(45)
It follows that
(46)
Then we get
(47)
which, together with (H3), implies |c1| ≤ D. Here, Ω3 is bounded.

Remark 12. If the other parts of (H3) hold, then the set is bounded.

Theorem 13. Suppose (H1)–(H4) hold; then the problem (3) has at least one solution in Y.

Proof. Let Ω be a bounded open set of Y, such that . It follows from Lemma 8, N is L-compact on Ω. By Lemmas 9, 10, and 11, we get the following:

  • (1)

    LuλNu, for every u ∈ [(dom⁡L∖Ker⁡L) ⋂ Ω]×(0,1);

  • (2)

    NuImL for every u ∈ Ker⁡LΩ;

  • (3)

    let H(u, λ) = ±λIu + (1 − λ)JQNu, where I is the identical operator. Via the homotopy property of degree, we obtain that

    (48)

Applying Theorem 6, we conclude that Lu = Nu has at least one solution in .

Under the stronger conditions imposed on f, we can prove the uniqueness of solutions to the (3) studied above.

Theorem 14. Suppose the conditions (H1) in the theorem are replaced by the following conditions.

  • (H1)′

    There exist positive constants ai, i = 0,1, …, N − 1, such that, for all (x1, x2, …, xN), , one has

    (49)

  • (H1)′′

    There exist constants li, i = 1,2, …, N − 1, such that for all (x1, x2, …, xN), , one has

    (50)

Then, the BVP (3) has a unique solution, provided that
(51)

Proof. Let yi = 0, i = 1,2, …, N, and φ1 = |f(t, 0, …, 0)|; then the condition (H1) is satisfied. According to Theorem 13, BVP (3) has at least one solution. Suppose uiY, i = 1,2 are two solutions of (3); then

(52)
Note that u = u1u2, so u satisfy the equation
(53)
According to Im⁡(L) = Ker⁡(Q), we have
(54)
By the integral mean value theorem, there exists η ∈ [0,1], such that
(55)
By (H1)′′, we have
(56)
We can have
(57)
Thus, we can obtain
(58)
According to (25), (38), and (58), we have
(59)
From the definition of ∥uX and the assumption (51), we have ∥u∥ = 0, so that u1 = u2.

4. Example

Let us consider the following boundary value problems:
(60)
Corresponding to the problem (3), we have that α = 2.5 and
(61)
Moreover,
(62)
We can get that the condition (H1) holds; that is, φ = (12 + 5π)/10, ψ1 = ψ3 = 0, and ψ2 = 1/9. Taking A = 25, D = 19, we can calculate that (H2)–(H4) hold.

Hence, by Theorem 13, we obtain that (60) has at least one solution.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Authors’ Contribution

All authors typed, read, and approved the final paper.

Acknowledgments

Research was supported by the National Natural Science Foundation of China (11371364) and 2013 Science and Technology Research Project of Beijing Municipal Education Commission (KM201310016001).

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