Existence of Solutions for Two-Point Boundary Value Problem of Fractional Differential Equations at Resonance
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, [1–5].
Recently, more and more authors have paid their attentions to the boundary value problems of fractional differential equations; see [6–21]. Moreover, there have been many works related to the existence of solutions for boundary value problems at resonance; see [12–21]. 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]).
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.
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 [1–3].
Definition 1 (see [1].)The Riemann-Liouville fractional integral of order α > 0 of a function is given by
Definition 2 (see [1].)The Riemann-Liouville fractional derivative of order α > 0 of a continuous function is given by
Lemma 3 (see [1].)Let n − 1 < α ≤ n, u ∈ C(0,1) ⋂ L1(0,1); then
Lemma 4 (see [1].)If α > 0, and D = d/dx. If the fractional derivatives and exist, then
Lemma 5 (see [1].)The relation
Now let us recall some notations about the coincidence degree continuation theorem.
Let Y, Z be real Banach spaces, let L : domL ⊂ Y → Z be a Fredholm map of index zero, and let P : Y → Y, Q : Z → Z be continuous projectors such that kerL = ImP, ImL = kerQ, and Y = kerL ⊕ kerP, Z = ImL ⊕ ImQ. It follows that L|domL∩kerP : domL∩kerP → ImL 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)
Lx ≠ λNx for each (x, λ) ∈ [(domL∖kerL)∩∂Ω] × (0,1);
- (2)
Nx ∉ ImL for each x ∈ kerL∩∂Ω;
- (3)
deg(JQN|kerL, Ω∩kerL, 0) ≠ 0, where Q : Z → Z is a continuous projection as above with ImL = kerQ and J : ImQ → kerL is any isomorphism.
3. Main Results
In this section, we will prove the existence results for (3).
Lemma 7. The mapping L : dom(L) ⊂ E is a Fredholm operator of index zero.
Proof. It is clear that
Thus, we conclude that
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 u ∈ Im(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 define KP : ImL → domL∩kerP by .
Lemma 8. Assume Ω ⊂ Y is an open bounded subset such that domL ⋂ Y ≠ ∅; 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 |(I − Q)N(u(t))| ≤ r, for all , t ∈ [0,1].
For 0 ≤ t1 ≤ t2 ≤ 1, u ∈ Ω, we have
- (H1)
There exist functions φ, ψi ∈ L1[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 u ∈ Ω1, λ ≠ 0 and Lu = λNu. By (12), Lu = λNu ∈ Im(L) = Ker(Q); that is,
Again for u ∈ Ω1, (I − P)u ∈ dom(L)∖Ker(L) and LPu = 0. From (29), we have
Lemma 10. Ω2 = {u ∈ Ker(L) : Nu ∈ Im(L)} is bounded.
Proof. Let u ∈ Ker(L), so we have u = c1tα−1, . For Nu ∈ Im(L) = Ker(Q),
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
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)
Lu ≠ λNu, for every u ∈ [(domL∖KerL) ⋂ ∂Ω]×(0,1);
- (2)
Nu ∉ ImL for every u ∈ KerL ⋂ ∂Ω;
- (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)
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)
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 ui ∈ Y, i = 1,2 are two solutions of (3); then
4. Example
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).