This paper investigates the existence and uniqueness of solutions for several two-point fractional BVPs, including hybrid fractional BVP, sequential fractional BVP and so on. Using the Banach contraction mapping theorem, some sharp conditions that depend on the length of the given interval are presented, which ensure the uniqueness of solutions for the considered BVPs. Illustrative examples are also constructed. The results obtained in this study are noteworthy extensions of earlier works.
Citation: Wei Zhang, Jinbo Ni. New sharp estimates of the interval length of the uniqueness results for several two-point fractional boundary value problems[J]. Electronic Research Archive, 2023, 31(3): 1253-1270. doi: 10.3934/era.2023064
[1] | Jinheng Liu, Kemei Zhang, Xue-Jun Xie . The existence of solutions of Hadamard fractional differential equations with integral and discrete boundary conditions on infinite interval. Electronic Research Archive, 2024, 32(4): 2286-2309. doi: 10.3934/era.2024104 |
[2] | Qingcong Song, Xinan Hao . Positive solutions for fractional iterative functional differential equation with a convection term. Electronic Research Archive, 2023, 31(4): 1863-1875. doi: 10.3934/era.2023096 |
[3] | Mustafa Aydin, Nazim I. Mahmudov, Hüseyin Aktuğlu, Erdem Baytunç, Mehmet S. Atamert . On a study of the representation of solutions of a $ \Psi $-Caputo fractional differential equations with a single delay. Electronic Research Archive, 2022, 30(3): 1016-1034. doi: 10.3934/era.2022053 |
[4] | Limin Guo, Weihua Wang, Cheng Li, Jingbo Zhao, Dandan Min . Existence results for a class of nonlinear singular $ p $-Laplacian Hadamard fractional differential equations. Electronic Research Archive, 2024, 32(2): 928-944. doi: 10.3934/era.2024045 |
[5] | Yumei Zou, Yujun Cui . Uniqueness criteria for initial value problem of conformable fractional differential equation. Electronic Research Archive, 2023, 31(7): 4077-4087. doi: 10.3934/era.2023207 |
[6] | Vo Van Au, Jagdev Singh, Anh Tuan Nguyen . Well-posedness results and blow-up for a semi-linear time fractional diffusion equation with variable coefficients. Electronic Research Archive, 2021, 29(6): 3581-3607. doi: 10.3934/era.2021052 |
[7] | Yihui Xu, Benoumran Telli, Mohammed Said Souid, Sina Etemad, Jiafa Xu, Shahram Rezapour . Stability on a boundary problem with RL-Fractional derivative in the sense of Atangana-Baleanu of variable-order. Electronic Research Archive, 2024, 32(1): 134-159. doi: 10.3934/era.2024007 |
[8] | Mufit San, Seyma Ramazan . A study for a higher order Riemann-Liouville fractional differential equation with weakly singularity. Electronic Research Archive, 2024, 32(5): 3092-3112. doi: 10.3934/era.2024141 |
[9] | Changjia Wang, Yuxi Duan . Well-posedness for heat conducting non-Newtonian micropolar fluid equations. Electronic Research Archive, 2024, 32(2): 897-914. doi: 10.3934/era.2024043 |
[10] | David Barilla, Martin Bohner, Giuseppe Caristi, Shapour Heidarkhani, Shahin Moradi . Existence results for a discrete fractional boundary value problem. Electronic Research Archive, 2025, 33(3): 1541-1565. doi: 10.3934/era.2025073 |
This paper investigates the existence and uniqueness of solutions for several two-point fractional BVPs, including hybrid fractional BVP, sequential fractional BVP and so on. Using the Banach contraction mapping theorem, some sharp conditions that depend on the length of the given interval are presented, which ensure the uniqueness of solutions for the considered BVPs. Illustrative examples are also constructed. The results obtained in this study are noteworthy extensions of earlier works.
Bailey, Shampine and Waltman analyzed the following classical two-point boundary value problems (BVPs) [1]:
{y″(t)+f(t,y(t))=0,t∈(a,b),y(a)=A,y(b)=B,and | (1.1) |
{y″(t)+f(t,y(t),y′(t))=0,t∈(a,b),y(a)=A,y(b)=B, | (1.2) |
where A,B∈R. The authors presented the following results.
Theorem 1.1. [1] Let f(t,y) be continuous on [a,b]×R and satisfy Lipschitz condition with Lipschitz constant K,
|f(t,y)−f(t,x)|≤K, |
for all (t,y),(t,x)∈[a,b]×R. Then BVP (1.1) has a unique solution whenever
b−a<2√2√K. | (1.3) |
Theorem 1.2. [1] Let f(t,y,y′) be continuous on [a,b]×R2 and satisfy Lipschitz condition with Lipschitz constants K and L,
|f(t,y,y′)−f(t,x,x′)|≤K|y−x|+L|y′−x′|, |
for all (t,y,y′),(t,x,x′)∈[a,b]×R2. Then BVP (1.2) has a unique solution if
K(b−a)28+L(b−a)2<1. | (1.4) |
Fractional calculus has risen in many fields of science and engineering over the past few decades. Numerous problems in physics, chemistry, biology, economics, signal and image processing, fluid dynamics, economics and control theory can be modeled in the form of fractional models, especially to describe processes with memory effects [2,3,4,5,6]. Consequently, solving fractional BVPs has always received considerable attention, and various interesting results dealing with the existence and uniqueness results for fractional differential equations involving a variety of boundary conditions have been established [7,8,9,10,11].
Recently, several scholars have proposed to extend the result of Theorem 1.1 by considering a fractional derivative. Additionally, based on different definitions of the fractional derivative, inequality (1.3) has been generalized to various forms. Examples include the Riemann-Liouville derivative [12], the Caputo fractional derivative [13], the Conformable fractional derivative [14], and the Hadamard fractional derivative [15]. For example, Ferreira [12] extended the result of Theorem 1.1 by using the Riemann-Liouville fractional derivative, that is, the following two-point fractional BVP was studied:
{Dαa+y(t)+f(t,y(t))=0,a<t<b,y(a)=0,y(b)=B, | (1.5) |
where 1<α≤2, Dαa+ is the Riemann-Liouville fractional derivative of order α. The following result was obtained.
Theorem 1.3. [12] Let f:[a,b]×R→R be continuous and satisfy the Lipschitz condition on [a,b]×R with Lipschitz constant K,
|f(t,x)−f(t,y)|≤K|x−y|, |
for all (t,x),(t,y)∈[a,b]×R. Then BVP (1.5) has a unique solution if
b−a<(Γ(α))1/αα(α+1)/αK1/α(α−1)(α−1)/α. |
Laadjal, Abdeljawad and Jarad [14] extended the result of Theorem 1.1 involving a conformable fractional derivative. The author investigated the following two-point fractional BVP:
{Taβu(t)+f(t,u(t))=0,t∈(a,b),u(a)=A,u(b)=B,A,B∈R, | (1.6) |
where 1<β≤2 and Taβ is the conformable fractional derivative of order β. The following result was obtained.
Theorem 1.4. [14] Let f:[a,b]×R→R be continuous and satisfy the Lipschitz condition on [a,b]×R with Lipschitz constant K,
|f(t,x)−f(t,y)|≤K|x−y|, |
for all (t,x),(t,y)∈[a,b]×R. Then BVP (1.6) has a unique solution if
b−a<β(2β−1)/(2β−1)β(β−1)β(β−1)K1/1ββ. |
However, no result exists in the literature that extends Theorem 1.2 to fractional differential equations. The main objective of this study is to bridge this gap. To this end, inspired by the above literature, the following fractional BVPs are considered.
Motivated by the above-mentioned works, the sharp estimate for the unique solution of the following two-point hybrid fractional BVP is investigated:
{Dαa+[x(t)f(t,x(t))]+g(t,x(t))=0,t∈(a,b),x(a)=0,x(b)=B, | (1.7) |
where 1<α≤2, Dαa+ is the Riemann-Liouville fractional derivative of order α, B∈R is a constant, f:[a,b]×R→R∖{0} and g:[a,b]×R→R are two continuous functions.
As a second problem, inspired by the above ideas and by [1], this paper aims to extend Theorem 1.2 by considering a fractional derivative. The sharp estimate for the unique solution of the following two-point fractional BVPs were studied with a non-linear term depending on the fractional derivative given by
{Dαa+y(t)+f(t,(t−a)2−αy(t),Dα−1a+y(t))=0,t∈(a,b),limt→a+(t−a)2−αy(t)=A,y(b)=B, | (1.8) |
and the sequential fractional BVP
{Dβa+CDγa+z(t)+g(t,z(t),(t−a)1−βCDγa+z(t))=0,t∈(a,b),z(a)=A,z(b)=B, | (1.9) |
where 1<α≤2, 0<γ,β≤1, 1<γ+β≤2, Dκa+ is the Riemann-Liouville fractional derivative of order κ=α,β, CDγa+ is the Caputo fractional derivative of order γ; A,B∈R are two constants, and f,g:[a,b]×R2→R are two continuous functions.
The following assumptions were considered throughout the present analysis:
(A1) There exist Lipschitz constants L1,L2, such that, for all (t,xi)∈[a,b]×R, (i=1,2),
|f(t,x1)−f(t,x2)|≤L1|x1−x2|,|g(t,x1)−g(t,x2)|≤L2|x1−x2|. |
(A2) There exist Lipschitz constants K,L, such that, for any (t,ui,vi)∈[a,b]×R2, (i=1,2),
|f(t,u1,v1)−f(t,u2,v2)|≤K|u1−u2|+L|v1−v2|. |
(A3) There exist Lipschitz constants P,Q, such that, for any (t,wi,zi)∈[a,b]×R2, (i=1,2),
|g(t,w1,z1)−g(t,w2,z2)|≤P|w1−w2|+Q|z1−z2|. |
Based on the above interpretation, the contribution of this work is summarized as follows:
∙ A new condition in terms of the end points of the given interval is presented, which ensures the uniqueness of the solution for a two-point hybrid fractional BVP and generalizes the result of Theorem 1.3.
∙ The sharp estimate for the unique solution of the two-point fractional BVPs with a non-linear term depending on a lower fractional order derivative is established, which extends the classical integer order results of Theorem 1.2.
∙ The sequential two-point fractional BVP is considered, providing a means to solve the open problem (30) proposed in [14].
The rest of the paper is organized as follows. In Section 2, some basic results related to the fractional calculus are given. In Section 3, by using the Banach contraction mapping theorem the estimate for the uniqueness results of the two-point fractional BVPs (1.7)–(1.9) are investigated. In Section 4, we present some examples which illustrate the efficiency of the main results. Finally, Section 5 addresses the conclusion of the work.
In this section, we recall some basic definitions and lemmas on fractional calculus, we refer the reader to [2].
Definition 2.1. [2] The Riemann-Liouville fractional integral of order α>0 for a function u:[a,b]→R is defined as
Iαa+u(t)=1Γ(α)∫ta(t−s)α−1u(s)ds,t∈[a,b]. |
Definition 2.2. [2] The Riemann-Liouville fractional derivative of order α>0 for a function u:[a,b]→R is defined as
Dαa+u(t)=1Γ(n−α)(ddt)n∫ta(t−s)n−α−1u(s)ds,t∈[a,b],n−1<α<n,n=[α]+1, |
where [α] denotes the integer part of the real number α.
Definition 2.3. [2] The Caputo fractional derivative of order α>0 for a (n−1)-times absolutely continuous function u:[a,b]→R is defined as
CDαa+u(t)=1Γ(n−α)∫ta(t−s)n−α−1u(n)(s)ds,t∈[a,b],n−1<α<n,n=[α]+1, |
where [α] denotes the integer part of the real number α.
Lemma 2.1. [2,7] Let α>0. If u∈C(a,b)∩L1(a,b), then
Iαa+Dαa+u(t)=u(t)−c1(t−a)α−1−c2(t−a)α−2−⋯−cn(t−a)α−n, |
for some constants ci∈R,i=1,2,⋯,n, and n=[α]+1.
Lemma 2.2. [2] Let α>0. If x,CDαa+x∈L([a,b],R), then
Iαa+CDαa+x(t)=x(t)−c0−c1(t−a)−⋯−cn−1(t−a)n−1, |
for some constants ci∈R, i=0,1,⋯,n−1, and n=[α]+1.
Lemma 2.3. [2,7] Let α,β>0, n=[α]+1. Then,
Iαa+(t−a)β−1=Γ(β)Γ(β+α)(t−a)α+β−1,t>a; | (2.1) |
Dαa+(t−a)β−1=Γ(β)Γ(β−α)(t−a)β−α−1,t>a; | (2.2) |
Dαa+(t−a)α−j=0,t>a,j=1,2,⋯,n; | (2.3) |
CDαa+(t−a)β−1=Γ(β)Γ(β−α)(t−a)β−α−1,t>a; | (2.4) |
CDαa+(t−a)k=0,t>a,k=0,1,2,⋯,n−1,andCDαa+1=0. | (2.5) |
Lemma 2.4. [2] Let α>β>0, u(t)∈C(a,b). Then,
Iαa+Iβa+u(t)=Iα+βa+u(t),Dαa+Iαa+x(t)=u(t)=CDαa+Iαa+u(t), | (2.6) |
Dβa+Iαa+u(t)=Iα−βa+u(t). | (2.7) |
Define Banach space X of continuous functions on [a,b] with the norm ||x||∞=maxt∈[a,b]|x(t)|. Let α,β,γ∈R, 1<α≤2, 0<γ,β≤1, 1<γ+β≤2 be fixed and I=[a,b]. For any y:(a,b]→R and z:[a,b]→R, we define functions yα:I→R and ˙zβ:I→R by
yα(t)={(t−a)2−αy(t),ift∈(a,b],limt→a+(t−a)2−αy(t),ift=a,˙zβ(t)={(t−a)1−βCDγa+z(t),ift∈(a,b],limt→a+(t−a)1−βCDγa+z(t),ift=a, |
given that the right-hand limits are exist. Define spaces
Y:={y:(a,b]→R|yα,Dα−1a+y∈C[a,b]},Z:={z:[a,b]→R|z,˙zβ(t)∈C[a,b]}. |
It is not difficult to show that Y and Z are two Banach spaces equipped with the norms
||y||α=maxt∈[a,b](K|yα|+L|Dα−1a+y|),||z||β=maxt∈[a,b](P|z|+Q|˙zβ|), |
respectively.
Lemma 3.1. Assume that f and g are continuous functions. Then, a function x∈C[a,b] is a solution of Eq (1.7) if and only if x(t) satisfies
x(t)=f(t,x(t))∫baG(t,s)g(s,x(s))ds+B(t−a)α−1f(t,x(t))(b−a)α−1f(b,x(b)), | (3.1) |
where
G(t,s)=1Γ(α){(t−a)α−1(b−a)α−1(b−s)α−1−(t−s)α−1,a≤s≤t≤b,(t−a)α−1(b−a)α−1(b−s)α−1,a≤t≤s≤b. | (3.2) |
Proof. According to Lemma 2.1, applying operator Iαa+ on both sides of Eq (1.7) yields
x(t)f(t,x(t))=−Iαa+g(t,x(t))+c1(t−a)α−1+c2(t−a)α−2, |
where c1,c2∈R are arbitrary constants. Therefore,
x(t)=f(t,x(t))[−Iαa+g(t,x(t))+c1(t−a)α−1+c2(t−a)α−2]. |
Using boundary condition x(a)=0, we get c2=0. Then,
x(t)=f(t,x(t))[−Iαa+g(t,x(t))+c1(t−a)α−1]. | (3.3) |
From boundary condition x(b)=B, it follows that
Bf(b,x(b))=−Iαa+g(t,x(t))|t=b+c1(b−a)α−1, |
that is,
c1=B(b−a)α−1f(b,x(b))+Iαa+g(t,x(t))|t=b(b−a)α−1. |
Substituting the value of c1 in Eq (3.3) yields
x(t)=f(t,x(t))(−1Γ(α)∫ta(t−s)α−1g(s,x(s))ds+(t−a)α−1Γ(α)(b−a)α−1∫ba(b−s)α−1g(s,x(s))ds)+B(t−a)α−1f(t,x(t))(b−a)α−1f(b,x(b))=f(t,x(t))∫baG(t,s)g(s,x(s))ds+B(t−a)α−1f(t,x(t))(b−a)α−1f(b,x(b)). |
Conversely, by direct computation, it can be established that (3.1) satisfies problem (1.7). This completes the proof.
Lemma 3.2. Assume that f is a continuous function. Then, a function y∈Y is a solution of Eq (1.8) if and only if y(t) satisfies the integral equations
y(t)=∫baG(t,s)f(s,(s−a)2−αy(s),Dα−1a+y(s))ds+(t−a)α−1(b−a)α−1[B−A(b−a)α−2]+A(t−a)α−2, | (3.4) |
and
Dα−1a+y(t)=Γ(α)[B−A(b−a)α−2](b−a)α−1+∫baH(t,s)f(s,(s−a)2−αy(s),Dα−1a+y(s))ds, | (3.5) |
where G(t,s) defined the same as in (3.2),
G(t,s)=1Γ(α){(t−a)α−1(b−a)α−1(b−s)α−1−(t−s)α−1,a≤s≤t≤b,(t−a)α−1(b−a)α−1(b−s)α−1,a≤t≤s≤b, |
and
H(t,s)=1(b−a)α−1{(b−s)α−1−(b−a)α−1,a≤s≤t≤b,(b−s)α−1,a≤t≤s≤b. | (3.6) |
Proof. In view of Lemma 2.1, a general solution of the fractional equation in (1.8) is given by
y(t)=−Iαa+f(t,(t−a)2−αy(t),Dα−1a+y(t))+c0(t−a)α−1+c1(t−a)α−2, | (3.7) |
where c0,c1∈R are arbitrary constants. From the first boundary condition limt→a+(t−a)2−αy(t)=A, we obtain c1=A, which yields
y(t)=−Iαa+f(t,(t−a)2−αy(t),Dα−1a+y(t))+c0(t−a)α−1+A(t−a)α−2. | (3.8) |
From y(b)=B and by using (3.8), we derive
c0=1(b−a)α−1[Iαa+f(t,(t−a)2−αy(t),Dα−1a+y(t))|t=b+B−A(b−a)α−2]. |
Substituting the value of c0 in (3.8) yields solution (3.4),
y(t)=−Iαa+f(t,(t−a)2−αy(t),Dα−1a+y(t))+A(t−a)α−2+(t−a)α−1(b−a)α−1[Iαa+f(t,(t−a)2−αy(t),Dα−1a+y(t))|t=b+B−A(b−a)α−2]=∫baG(t,s)f(s,(s−a)2−αy(s),Dα−1a+y(s))ds+(t−a)α−1(b−a)α−1[B−A(b−a)α−2]+A(t−a)α−2. |
The converse follows by direct computation. On the other hand, according to (2.2), (2.3) and (2.7), taking the (α−1)-th Riemann-Liouville fractional derivative on the both sides of (3.4) yields (3.5),
Dα−1a+y(t)=−Dα−1a+Iαa+f(t,(t−a)2−αy(t),Dα−1a+y(t))+A[Dα−1a+(t−a)α−2]+Dα−1a+(t−a)α−1(b−a)α−1[Iαa+f(t,(t−a)2−αy(t),Dα−1a+y(t))|t=b+B−A(b−a)α−2]=−∫taf(s,(s−a)2−αy(s),Dα−1a+y(s))ds+Γ(α)(b−a)α−1[B−A(b−a)α−2]+1(b−a)α−1[∫ba(b−s)α−1f(s,(s−a)2−αy(s),Dα−1a+y(s))ds]=Γ(α)[B−A(b−a)α−2](b−a)α−1+∫baH(t,s)f(s,(s−a)2−αy(s),Dα−1a+y(s))ds. |
This proves the lemma.
Lemma 3.3. Assume that g is a continuous function. Then, a function z∈Y is a solution of equation (1.9) if and only if z(t) satisfies the integral equations
z(t)=∫baG(t,s)g(s,z(s),(s−a)1−βCDγa+z(s))ds+(t−a)γ+β−1(b−a)γ+β−1(B−A)+A, | (3.9) |
and
CDγa+z(t)=(B−A)Γ(γ+β)(b−a)γ+β−1Γ(β)(t−a)β−1+∫baH(t,s)g(s,z(s),(s−a)1−βCDγa+z(s))ds, | (3.10) |
where kernel functions G(t,s) and H(t,s) are defined as
G(t,s)=1Γ(γ+β){(t−a)γ+β−1(b−a)γ+β−1(b−s)γ+β−1−(t−s)γ+β−1,a≤s≤t≤b,(t−a)γ+β−1(b−a)γ+β−1(b−s)γ+β−1,a≤t≤s≤b, | (3.11) |
and
H(t,s)=1Γ(β){(t−a)β−1(b−a)γ+β−1(b−s)γ+β−1−(t−s)β−1,a≤s≤t≤b,(t−a)β−1(b−a)γ+β−1(b−s)γ+β−1,a≤t≤s≤b. | (3.12) |
Proof. Applying operators Iβa+ and Iγa+ on the fractional equation in (1.9) and then using Lemmas 2.1–2.4 yields
z(t)=−Iγ+βa+g(t,z(t),(t−a)1−βCDγa+z(t))+Γ(β)Γ(γ+β)c0(t−a)γ+β−1+c1, | (3.13) |
where c0,c1∈R are arbitrary constants. Applying the boundary conditions z(a)=A,z(b)=B in (3.13) yields
c1=A,c0=Γ(γ+β)(b−a)γ+β−1Γ(β)[B−A+Iγ+βa+g(t,z(t),(t−a)1−βCDγa+z(t))|t=b]. |
Substituting the above values into (3.13), the solution given by (3.9) is obtained. The converse of the lemma can be obtained by direct computation. On the other hand, by Lemma 2.3 and Lemma 2.4, taking the γ-th Caputo fractional derivative on both sides of (3.9) yields (3.10). The proof is completed.
Lemma 3.4. The Green's functions G(t,s), H(t,s), G(t,s) and H(t,s) given by Lemmas 3.1–3.3, respectively, satisfy the following properties:
(i) G(t,s), H(t,s), G(t,s) and H(t,s) are continuous functions in [a,b]×[a,b];
(ii) G(t,s) and G(t,s) are two nonnegative functions in [a,b]×[a,b];
(iii) ∫baG(t,s)ds≤(α−1)α−1Γ(α)αα+1(b−a)α, for any t∈[a,b];
(iv) ∫ba(t−a)2−αG(t,s)ds≤(b−a)24Γ(α+1), for any t∈[a,b];
(v) ∫ba|H(t,s)|ds≤1α(b−a), for any t∈[a,b];
(vi) ∫baG(t,s)ds≤(γ+β−1)γ+β−1Γ(γ+β)(γ+β)γ+β+1(b−a)γ+β, for any t∈[a,b];
(vii) ∫ba(t−a)1−β|H(t,s)|ds≤max{β,γ}(b−a)(γ+β)Γ(β+1), for any t∈[a,b].
Proof. It is obvious that (i) is true. For (ii), in view of the definition of G(t,s), let
G1(t,s)=1Γ(α)(t−a)α−1(b−a)α−1(b−s)α−1−(t−s)α−1,a≤s≤t≤b,G2(t,s)=1Γ(α)(t−a)α−1(b−a)α−1(b−s)α−1,a≤t≤s≤b. |
Then, we can easily obtain that
G2(t,s)≥0,(t,s)∈[a,b]×[a,b]. |
Differentiating G1(t,s) with respect to s for every fixed t∈[a,b],
∂G1(t,s)∂s=α−1Γ(α)[−(t−a)α−1(b−a)α−1(b−s)α−2+(t−s)α−2]=α−1Γ(α)(t−s)α−2[1−(t−ab−a)α−1(t−sb−s)2−α]≥0, |
that is, G1(t,s) is increasing with respect to s∈[a,t] for any fixed t∈[a,b]. Therefore,
G1(t,s)≥G1(t,a)=0,t∈[a,b]. |
Thus, we have derived that G(t,s) ia nonnegative in [a,b]×[a,b]. Let α=β+γ, then we can also get G(t,s) is nonnegative in [a,b]×[a,b]. For (iii) and (iv), by the expression for the function G(t,s), we obtain
∫baG(t,s)ds=1Γ(α){∫ta[(t−a)α−1(b−a)α−1(b−s)α−1−(t−s)α−1]ds+∫bt(t−a)α−1(b−a)α−1(b−s)α−1ds}=1Γ(α){1α[−(t−a)α−1(b−a)α−1(b−s)α+(t−s)α]|s=ts=a−1α(t−a)α−1(b−a)α−1(b−s)α|s=bs=t}=1αΓ(α)(t−a)α−1(b−t). |
It follows that
∫ba(t−a)2−αG(t,s)ds=(t−a)2−α∫baG(t,s)ds=1αΓ(α)(t−a)(b−t). |
Define
g(t)=(t−a)(b−t),t∈[a,b], |
and
˜g(t)=(t−a)α−1(b−t),t∈[a,b]. |
Differentiating the functions g(t) and ˜g(t) on (a,b), we immediately find that g(t) and ˜g(t) are achieved their maximum at the following points, respectively,
t∗=a+b2,˜t=1α[a+(α−1)b]. |
This yields,
maxt∈[a,b]g(t)=14(b−a)2,maxt∈[a,b]˜g(t)=(α−1)α−1(b−a)ααα, |
which completes the proof of (iii) and (iv). Let α=β+γ, then property (vi) can be obtained directly from (iii). We will now show that properties (v) and (vii) are true. First, for (v), in view of the definition of H(t,s), we have
∫ba|H(t,s)|ds=1(b−a)α−1[∫ta((b−a)α−1−(b−s)α−1)ds+∫bt(b−s)α−1ds]=1(b−a)α−1[(b−a)α−1(t−a)+2α(b−t)α−1α(b−a)α]. |
Define
h(t)=(b−a)α−1(t−a)+2α(b−t)α−1α(b−a)α,t∈[a,b]. |
Then,
h(a)=1α(b−a)α≥h(b)=(b−a)α−1α(b−a)α>0. |
Taking the second-order derivative of function h(t) on (a,b), we obtain
h″(t)=2(α−1)(b−t)α−2≥0,t∈[a,b]. |
Therefore, h(t) is convex on (a,b). Hence,
maxt∈[a,b]h(t)=maxt∈[a,b]{h(a),h(b)}=h(a)=1α(b−a)α. |
This completes the proof of (v). Finally, for (vii), for a≤s≤t≤b, we can derive that
(b−s)γ+β−1(t−a)β−1−(b−a)γ+β−1(t−s)β−1=(b−a)γ+β−1(t−s)β−1[(b−sb−a)γ+β−1(t−st−a)1−β−1]≤0. |
Hence, it follows from the definition of H(t,s) that
∫ba|H(t,s)|ds=1Γ(β)∫ta[(t−s)β−1−(t−a)β−1(b−a)γ+β−1(b−s)γ+β−1]ds+1Γ(β)∫bt(t−a)β−1(b−a)γ+β−1(b−s)γ+β−1ds=1(γ+β)Γ(β)(t−a)β−1(b−a)γ+β−1[2(b−t)γ+β−(b−a)γ+β]+1Γ(β+1)(t−a)β. |
Consequently,
∫ba(t−a)1−β|H(t,s)|ds=2(b−t)γ+β−(b−a)γ+β(b−a)γ+β−1(γ+β)Γ(β)+(t−a)Γ(β+1). |
Define
h(t)=2(b−t)γ+β−(b−a)γ+β(b−a)γ+β−1(γ+β)Γ(β)+(t−a)Γ(β+1),t∈[a,b]. |
Then,
h(a)=β(b−a)(γ+β)Γ(β+1)>0,h(b)=γ(b−a)(γ+β)Γ(β+1)>0. |
Taking the second derivative of function h(t) on (a,b) leads to
h″(t)=(γ+β−1)2(b−t)γ+β−2(b−a)γ+β−1Γ(β)≥0,t∈(a,b). |
This implies that h(t) is convex on (a,b). Therefore,
maxt∈[a,b]h(t)=max{h(a),h(b)}=max{β,γ}(b−a)(γ+β)Γ(β+1). |
The proof is completed.
Based on Lemmas 3.1 to 3.3, operators T1:X→X, T2:Y→Y and T3:Z→Z are defined as
T1x(t)=f(t,x(t))∫baG(t,s)g(s,x(s))ds+B(t−a)α−1f(t,x(t))(b−a)α−1f(b,x(b)),x(t)∈X,T2y(t)=∫baG(t,s)f(s,(s−a)2−αy(s),Dα−1a+y(s))ds+(t−a)α−1(b−a)α−1[B−A(b−a)α−2]+A(t−a)α−2,y(t)∈Y,T3z(t)=∫baG(t,s)g(s,z(s),(s−a)1−βCDγa+z(s))ds+(t−a)γ+β−1(b−a)γ+β−1(B−A)+A,z(t)∈Z. |
Theorem 3.1. Assume that f,g:[a,b]×R→R are continuous functions and satisfy condition (A1). Let
M1=supt∈[a,b]|f(t,x(t))|,m1=inft∈[a,b]|f(t,x(t))|,M2=supt∈[a,b]|g(t,x(t))|. |
If
b−a<{αα+1[m21−BL1(m1+M1)]Γ(α)m21(M2L1+M1L2)(α−1)α−1}1/1αα, | (3.14) |
then problem (1.7) has a unique solution.
Proof. For x1(t),x2(t)∈X, using condition (A1), Lemma 3.4 (iii) and together with (3.1), yields
|Tx1(t)−Tx2(t)|≤|B(t−a)α−1f(t,x1(t))(b−a)α−1f(b,x1(b))−B(t−a)α−1f(t,x2(t))(b−a)α−1f(b,x2(b))|+|f(t,x1(t))∫baG(t,s)g(s,x1(s))ds−f(t,x2(t))∫baG(t,s)g(s,x2(s))ds|≤B(t−a)α−1(b−a)α−1(|f(t,x1(t))f(b,x1(b))−f(t,x2(t))f(b,x1(b))|+|f(t,x2(t))f(b,x1(b))−f(t,x2(t))f(b,x2(b))|)+|f(t,x1(t))∫baG(t,s)g(s,x1(s))ds−f(t,x2(t))∫baG(t,s)g(s,x1(s))ds|+|f(t,x2(t))∫baG(t,s)g(s,x1(s))ds−f(t,x2(t))∫baG(t,s)g(s,x2(s))ds|≤B(t−a)α−1(b−a)α−1|f(b,x1(b))||f(t,x1(t))−f(t,x2(t))|+B(t−a)α−1|f(t,x2(t))|(b−a)α−1|f(b,x1(b))||f(b,x2(b))||f(b,x2(b))−f(b,x1(b))|+|f(t,x1(t))−f(t,x2(t))|∫baG(t,s)|g(s,x1(s))|ds+∫baG(t,s)|g(s,x1(s))−g(s,x2(s))|ds|f(t,x2(t))|≤(Bm1+BM1m21)L1|x1−x2|+(M2L1+M1L2)(α−1)α−1(b−a)αΓ(α)αα+1|x1−x2| |
≤[BL1(m1+M1)m21+(M2L1+M1L2)(α−1)α−1(b−a)αΓ(α)αα+1]||x1−x2||∞. |
Therefore, we conclude from (3.14) that operator T1 is a contraction mapping. Hence problem (1.7) has a unique solution.
As special cases of Theorem 3.1, we have the following corollary:
Corollary 3.1. Let g(t,x) be continuous on [a,b]×R and satisfy Lipschitz condition
|g(t,x1)−g(t,x2)|≤K|x1−x2|,foranyx1,x2∈R,K>0. |
Then the BVP
{Dαa+x(t)+g(t,x(t))=0,t∈(a,b),1<α≤2,x(a)=0,x(b)=B,B∈R, |
has a unique solution whenever
b−a<[Γ(α)αα+1K(α−1)α−1]1/1αα. | (3.15) |
Proof. By Theorem 3.1, let f(t,x)≡1, (t,x)∈[a,b]×R, and L2=K. Then,
M1=supt∈[a,b]|f(t,x(t))|=inft∈[a,b]|f(t,x(t))|=m1=1,L1=0. |
Substituting the above values into (3.14), the desired result (3.15) is obtained. As such, our results match the results of Theorem 2.3 in [12].
Theorem 3.2. Let f(t,(t−a)2−αy(t),Dα−1a+y(t)) be continuous on [a,b]×R2 and satisfy condition (A2). If
K(b−a)24Γ(α+1)+Lα(b−a)<1, | (3.16) |
then problem (1.8) has a unique solution.
Proof. To see when T2 is contracting, we again from
(t−a)2−α|T2y1(t)−T2y2(t)|≤∫ba(t−a)2−αG(t,s)|f(s,(s−a)2−αy1(s),Dα−1a+y1(s))−f(s,(s−a)2−αy2(s),Dα−1a+y2(s))|ds, |
and from (3.5)
|Dα−1a+T2y1(t)−Dα−1a+T2y2(t)|≤∫ba|H(t,s)||f(s,(s−a)2−αy1(s),Dα−1a+y1(s))−f(s,(s−a)2−αy2(s),Dα−1a+y2(s))|ds. |
Using Lipschitz condition (A2) and Lemma 3.4 (iv), (v),
(t−a)2−α|T2y1(t)−T2y2(t)|≤∫ba(t−a)2−αG(t,s)(K(s−a)2−α|y1(s)−y2(s)|+L|Dα−1a+y1(s)−Dα−1a+y2(s)|)ds≤||y1−y2||α∫ba(t−a)2−αG(t,s)ds≤(b−a)24Γ(α+1)||y1−y2||α, |
and
|Dα−1a+T2y1(t)−Dα−1a+T2y2(t)|≤∫ba|H(t,s)|(K(s−a)2−α|y1(s)−y2(s)|+L|Dα−1a+y1(s)−Dα−1a+y2(s)|)ds≤||y1−y2||α∫ba|H(t,s)|ds≤1α(b−a)||y1−y2||α. |
Together these imply
||T2y1−T2y2||α≤[K(b−a)24Γ(α+1)+Lα(b−a)]||y1−y2||α. |
It follows from (3.16) that operator T2 is a contraction mapping. Hence, problem (1.8) has a unique solution.
Remark 3.1. Let α→2. Then, Theorem 3.2 can be reduced to Theorem 1.2.
Theorem 3.3. Let g(t,z(t),(t−a)1−βCDγa+z(t)) be continuous on [a,b]×R2 and satisfy condition (A3). If
P(γ+β−1)γ+β−1(b−a)γ+βΓ(γ+β)(γ+β)γ+β+1+Qmax{β,γ}(b−a)(γ+β)Γ(β+1)<1, | (3.17) |
then problem (1.9) has a unique solution.
Proof. This result will follow from the Banach contraction mapping theorem if we can show that operator T3 is a contraction mapping. In fact, for any z1(t),z2(t)∈Z, we have
|T3z1(t)−T3z2(t)|≤∫baG(t,s)|g(s,z1(s),(s−a)1−βCDγa+z1(s))−g(s,z2(s),(s−a)1−βCDγa+z2(s))|ds, |
and in view of (3.10),
|(t−a)1−βCDγa+T3z1(t)−(t−a)1−βCDγa+T3z2(t)|≤∫ba(t−a)1−β|H(t,s)||g(s,z1(s),(s−a)1−βCDγa+z1(s))−g(s,z2(s),(s−a)1−βCDγa+z2(s))|ds. |
Using Lipschitz condition (A3) and Lemma 3.4 (vi), (vii),
|T3z1(t)−T3z2(t)|≤∫baG(t,s)P|z1(s)−z2(s)|+Q(s−a)1−β|CDγa+z1(s)−CDγa+z2(s)|ds≤||z1−z2||β∫baG(t,s)ds≤(γ+β−1)γ+β−1(b−a)γ+βΓ(γ+β)(γ+β)γ+β+1||z1−z2||β, |
and
(t−a)1−β|CDγa+T3z1(t)−CDγa+T3z2(t)|≤∫ba(t−a)1−β|H(t,s)|P|z1(s)−z2(s)|+Q(s−a)1−β|CDγa+z1(s)−CDγa+z2(s)|ds≤||z1−z2||β∫ba(t−a)1−β|H(t,s)|ds≤max{β,γ}(b−a)(γ+β)Γ(β+1)||z1−z2||β, |
which, by taking the norm for t∈[a,b], implies that
||T3z1−T3z2||β≤[P(γ+β−1)γ+β−1(b−a)γ+βΓ(γ+β)(γ+β)γ+β+1+Qmax{β,γ}(b−a)(γ+β)Γ(β+1)]||z1−z2||β. |
From (3.17) we conclude that operator T3 is a contraction mapping. Thus, problem (1.9) has a unique solution.
Remark 3.2. Let γ,β→1. Then Theorem 3.3 can be reduced to Theorem 1.2.
Example 4.1. Consider the following two-point fractional BVP
{D4/31+[x(t)(6t/5)+(cosx(t))/10]+lnt5sinx(t)=0,t∈(1,2),x(1)=0,x(2)=1. | (4.1) |
Corresponding to BVP (1.7), here
α=4/3,a=B=1,b=2, |
f(t,x(t))=6t/5+cosx(t)/10,g(t,x(t))=((lnt)/5)sinx(t). |
Obviously, we have
|f(t,x)−f(t,y)|≤(1/10)|cosx−cosy|≤(1/10)|x−y|,forx,y∈R,|g(t,x)−g(t,y)|≤((lnt)/5)|sinx−siny|≤((ln2)/5)|x−y|,forx,y∈R. |
It is easy to find that L1=1/10,L2=M2=(ln2)/5,M1=2.5,m1=1.1. Thus,
BL1(m1+M1)m21+(M2L1+M1L2)(α−1)α−1(b−a)αΓ(α)αα+1≈0.4405<1. |
Clearly, all assumptions of Theorem 3.1 are satisfied. Therefore, BVP (4.1) has a unique solution on [1,2].
Example 4.2. Consider the following two-point fractional BVP
{D3/3220+y(t)+34√πsint1/122y(t)+34sinD1/1220+y(t)+52=0,t∈(0,1),limt→0+t1/122y(t)=y(1)=0, | (4.2) |
Corresponding to BVP (1.8), here
α=32,a=A=B=0,b=1, |
f(t,(t−a)2−αy(t),Dα−1a+y(t))=34√πsint1/122y(t)+34sinD1/1220+y(t)+52, |
Clearly,
|f(t,(t−a)2−αy1(t),Dα−1a+y1(t))−f(t,(t−a)2−αy2(t),Dα−1a+y2(t))|≤34√πt1/122|y1(t)−y2(t)|+34|Dα−1a+y1(t)−Dα−1a+y2(t)|. |
Choosing K=34√π,L=34 and consequently, we obtain
K(b−a)24Γ(α+1)+Lα(b−a)=3√π16Γ(5/522)+12=34<1. |
Thus, all the conditions of Theorem 3.2 are satisfied. Hence, BVP (4.2) has a unique solution on [0,1].
Example 4.3. Consider the following two-point fractional BVP
{D1/1220+CD3/3440+z(t)+et1+t+310sinz(t)+25⋅|t1/122CD3/3440+z(t)|1+|t1/122CD3/3440+z(t)|=0,t∈(0,2),z(0)=z(2)=0, | (4.3) |
Corresponding to BVP (1.9), here
β=12,γ=34,a=A=B=0,b=2, |
g(t,z(t),(t−a)1−βCDγa+z(t))=et1+t+310sinz(t)+25⋅|t1/122CD3/3440+z(t)|1+|t1/122CD3/3440+z(t)|. |
Clearly,
|g(t,z1(t),(t−a)1−βCDγa+z1(t))−g(t,z2(t),(t−a)1−βCDγa+z2(t))|≤310|z1(t)−z2(t)|+25t1/122|CD3/3440+z1(t)−CD3/3440+z2(t)|. |
Taking P=310,Q=25, we can find that
P(γ+β−1)γ+β−1(b−a)γ+βΓ(γ+β)(γ+β)γ+β+1+Qmax{β,γ}(b−a)(γ+β)Γ(β+1)=310⋅(1/144)1/14425/544(5/544)9/944Γ(5/544)+25⋅3/322(5/544)Γ(3/322)≈0.9628<1. |
Thus, the hypotheses of Theorem 3.3 are satisfied. Therefore, the BVP (4.3) has a unique solution on [0,2].
In this article, we discussed the uniqueness results for several two-point fractional BVPs. By using the Banach contraction mapping theorem, we obtained the sharp conditions in terms of the end-points of the given interval which ensures the uniqueness of solutions for these fractional BVPs. This seems to have something in common with studying of the Lyapunov inequality for BVPs. In terms of methods, both of them are converted the BVPs into the equivalent integral equations with corresponding Green's functions. By estimating the upper bound of Green's function, the existence of solutions to BVPs is finally characterized. The difference is that Lyapunov inequality directly estimates the upper bound of the Green's function G(t,s) on the interval [a,b]×[a,b], while this paper estimates the upper bound of ∫baG(t,s)ds for any t∈[a,b]. Our work is an extension of the classical results of Theorem 1.1 and Theorem 1.2. It is also an extension and supplement to some recent work [10,11,12,13,14]. Compared with the paper [10,11,12,13,14], we discuss the BVP where the nonlinear term of the differential equation has the fractional derivative of unknown function, and obtain new interesting results. Based on the this study, in the forthcoming paper, we will investigate the sharp estimate for the unique solution of the two-point Ψ-Hilfer fractional hybird-Sturm-Liouville equations.
The authors wish to express their sincere appreciation to the editor and the anonymous referees for their valuable comments and suggestions. This research is supported by Anhui Provincial Natural Science Foundation (2208085QA05), National Natural Science Foundation of China (11601007) and the Key Program of the University Natural Science Research Fund of Anhui Province (KJ2020A0291).
The authors declare that there is no conflict of interest.
[1] | P. B. Bailey, L. F. Shampine, P. E. Waltman, Nonlinear Two Point Boundary Value Problems, Academic Press, New York, 1968. https://doi.org/10.1090/S0002-9904-1969-12263-9 |
[2] | A. A. Kilbas, H. M. Srivastava, J. J. Trujillo, Theory and Applications of Fractional Differential Equations, Elsevier, 2006. |
[3] | H. Sheng, Y. Chen, T. Qiu, Fractional Processes and Fractional-Order Signal Processing, Springer, London, 2012. https://doi.org/10.1007/978-1-4471-2233-3 |
[4] | H. A. Fallahgoul, S. M. Focardi, F. J. Fabozzi, 2-Fractional Calculus, in Fractional Calculus and Fractional Processes with Applications to Financial Economics, Academic Press, London, (2017), 12–22. https://doi.org/10.1016/B978-0-12-804248-9.50002-4 |
[5] |
I. Uddin, C. Garodia, T. Abdeljawad, N. Mlaiki, Convergence analysis of a novel iteration process with application to a fractional differential equation, Adv. Contin. Discrete Models, 16 (2022), 20. https://doi.org/10.1186/s13662-022-03690-z doi: 10.1186/s13662-022-03690-z
![]() |
[6] |
S. Khatoon, I. Uddin, D. Baleanu, Approximation of fixed point and its application to fractional differential equation, J. Appl. Math. Comput., 66 (2021), 507–525. https://doi.org/10.1007/s12190-020-01445-1 doi: 10.1007/s12190-020-01445-1
![]() |
[7] |
Z. Bai, H. Lü, Positive solutions for boundary value problem of nonlinear fractional differential equation, J. Math. Anal. Appl., 311 (2005), 495–505. https://doi.org/10.1016/j.jmaa.2005.02.052 doi: 10.1016/j.jmaa.2005.02.052
![]() |
[8] |
B. Ahmad, S. K. Ntouyas, J. Tariboon, A nonlocal hybrid boundary value problem of Caputo fractional integro-differential equations, Acta Math. Sci., 36 (2016), 1631–1640. https://doi.org/10.1016/S0252-9602(16)30095-9 doi: 10.1016/S0252-9602(16)30095-9
![]() |
[9] |
X. Zhang, Z. Shao, Q. Zhong, Multiple positive solutions for higher-order fractional integral boundary value problems with singularity on space variable, Fract. Calc. Appl. Anal., 25 (2022), 1507–1526. https://doi.org/10.1007/s13540-022-00073-9 doi: 10.1007/s13540-022-00073-9
![]() |
[10] |
A. Cabada, T. Kisela, Existence of positive periodic solutions of some nonlinear fractional differential equations, Commun. Nonlinear Sci. Numer. Simul., 50 (2017), 51–67. https://doi.org/10.1016/j.cnsns.2017.02.010 doi: 10.1016/j.cnsns.2017.02.010
![]() |
[11] |
R. A. C. Ferreira, Two-point fractional boundary value problems, J. Integral Equations Appl., 33 (2021), 229–236. https://doi.org/10.1216/jie.2021.33.229 doi: 10.1216/jie.2021.33.229
![]() |
[12] | R. A. C. Ferreira, Existence and uniqueness of solutions for two-point fractional boundary value problems, Electron. J. Diff. Equations, 2016 (2016), 202. Available from: http://ejde.math.unt.edu |
[13] |
R. A. C. Ferreira, Note on a uniqueness result for a two-point fractional boundary value problem, Appl. Math. Lett., 90 (2019), 75–78. https://doi.org/10.1016/j.aml.2018.10.020 doi: 10.1016/j.aml.2018.10.020
![]() |
[14] | Z. Laadjal, T. Abdeljawad, F. Jarad, Sharp estimates of the unique solution for two-point fractional boundary value problems with conformable derivative, Numer. Methods Partial Diff. Equations, (2021). https://doi.org/10.1002/num.22760 |
[15] | Z. Laadjal, N. Adjeroud, Sharp estimates for the unique solution of the Hadamard-type two-point fractional boundary value problems, Appl. Math. E-Notes, 21 (2021), 275–281. Available from: http://www.math.nthu.edu.tw/~amen/ |
1. | Zaid Laadjal, Thabet Abdeljawad, Fahd Jarad, Some results for two classes of two-point local fractional proportional boundary value problems, 2023, 37, 0354-5180, 7199, 10.2298/FIL2321199L |