
In this paper, we investigate a class of boundary value problems involving Caputo fractional derivative CDαa of order α∈(2,3), and the usual derivative, of the form
(CDαax)(t)+p(t)x′(t)+q(t)x(t)=g(t),a≤t≤b,
for an unknown x with x(a)=x′(a)=x(b)=0, and p,q,g∈C2([a,b]). The proposed method uses certain integral inequalities, Banach's Contraction Principle and Krasnoselskii's Fixed Point Theorem to identify conditions that guarantee the existence and uniqueness of the solution (for the problem under study) and that allow the deduction of Ulam-Hyers and Ulam-Hyers-Rassias stabilities.
Citation: Luís P. Castro, Anabela S. Silva. On the solution and Ulam-Hyers-Rassias stability of a Caputo fractional boundary value problem[J]. Mathematical Biosciences and Engineering, 2022, 19(11): 10809-10825. doi: 10.3934/mbe.2022505
[1] | Kadda Maazouz, Rosana Rodríguez-López . Differential equations of arbitrary order under Caputo-Fabrizio derivative: some existence results and study of stability. Mathematical Biosciences and Engineering, 2022, 19(6): 6234-6251. doi: 10.3934/mbe.2022291 |
[2] | Zahra Eidinejad, Reza Saadati . Hyers-Ulam-Rassias-Kummer stability of the fractional integro-differential equations. Mathematical Biosciences and Engineering, 2022, 19(7): 6536-6550. doi: 10.3934/mbe.2022308 |
[3] | Noura Laksaci, Ahmed Boudaoui, Seham Mahyoub Al-Mekhlafi, Abdon Atangana . Mathematical analysis and numerical simulation for fractal-fractional cancer model. Mathematical Biosciences and Engineering, 2023, 20(10): 18083-18103. doi: 10.3934/mbe.2023803 |
[4] | George Maria Selvam, Jehad Alzabut, Vignesh Dhakshinamoorthy, Jagan Mohan Jonnalagadda, Kamaleldin Abodayeh . Existence and stability of nonlinear discrete fractional initial value problems with application to vibrating eardrum. Mathematical Biosciences and Engineering, 2021, 18(4): 3907-3921. doi: 10.3934/mbe.2021195 |
[5] | Saima Akter, Zhen Jin . A fractional order model of the COVID-19 outbreak in Bangladesh. Mathematical Biosciences and Engineering, 2023, 20(2): 2544-2565. doi: 10.3934/mbe.2023119 |
[6] | Guodong Li, Ying Zhang, Yajuan Guan, Wenjie Li . Stability analysis of multi-point boundary conditions for fractional differential equation with non-instantaneous integral impulse. Mathematical Biosciences and Engineering, 2023, 20(4): 7020-7041. doi: 10.3934/mbe.2023303 |
[7] | M. A. El-Shorbagy, Mati ur Rahman, Maryam Ahmed Alyami . On the analysis of the fractional model of COVID-19 under the piecewise global operators. Mathematical Biosciences and Engineering, 2023, 20(4): 6134-6173. doi: 10.3934/mbe.2023265 |
[8] | Jutarat Kongson, Chatthai Thaiprayoon, Apichat Neamvonk, Jehad Alzabut, Weerawat Sudsutad . Investigation of fractal-fractional HIV infection by evaluating the drug therapy effect in the Atangana-Baleanu sense. Mathematical Biosciences and Engineering, 2022, 19(11): 10762-10808. doi: 10.3934/mbe.2022504 |
[9] | Masumi Kondo, Masakazu Onitsuka . Ulam type stability for von Bertalanffy growth model with Allee effect. Mathematical Biosciences and Engineering, 2024, 21(3): 4698-4723. doi: 10.3934/mbe.2024206 |
[10] | Debao Yan . Existence results of fractional differential equations with nonlocal double-integral boundary conditions. Mathematical Biosciences and Engineering, 2023, 20(3): 4437-4454. doi: 10.3934/mbe.2023206 |
In this paper, we investigate a class of boundary value problems involving Caputo fractional derivative CDαa of order α∈(2,3), and the usual derivative, of the form
(CDαax)(t)+p(t)x′(t)+q(t)x(t)=g(t),a≤t≤b,
for an unknown x with x(a)=x′(a)=x(b)=0, and p,q,g∈C2([a,b]). The proposed method uses certain integral inequalities, Banach's Contraction Principle and Krasnoselskii's Fixed Point Theorem to identify conditions that guarantee the existence and uniqueness of the solution (for the problem under study) and that allow the deduction of Ulam-Hyers and Ulam-Hyers-Rassias stabilities.
In recent decades, fractional calculus has gained considerable popularity and importance. This is mainly due to its wide range of applications in different areas of engineering and other scientific fields such as biology, chemistry, economics, physics, image and signal processing, etc. (cf., for example, [1,2,3,4,5,6]). In fact, several studies have shown that fractional derivation allows different occurrences – such as complex long memory and hereditary properties of many processes – to be described in a much more satisfactory way when compared to models that consider only classical integer-order derivation (see, for example, [7,8]).
Within this scope, different aspects and properties of fractional boundary value problems (FBVP) have been studied, with special emphasis on the analysis of the existence and uniqueness of solutions, as well as on different types of stabilities (cf., for example, [9,10,11,12,13,14]).
In the present work, we will focus on two important types of stabilities: the Ulam-Hyers and Ulam-Hyers-Rassias stabilities. In historical terms, it was Ulam who, as far back as 1940, questioned for the first time the stability of functional equations relating to group homomorphisms (cf. [15]). The question was initially answered the following year by Hyers in the context of Banach spaces for additive mappings (cf. [16]). This first result of Hyers was later generalized by T. Aoki [17] for additive mapping. Much later, in 1978, a generalization of the Ulam-Hyers stability was then proposed by Rassias [18], for linear mappings. In this case, the Cauchy differences were allowed to be unlimited, giving rise to the so-called Ulam-Hyers-Rassias stability. Since then, these types of stabilities, their properties and consequences, have attracted the attention of many mathematicians, as well as researchers from other more applied areas (cf. [10,12,19,20,21,22,23,24]). Note that if a system is stable in the Ulam-Hyers or Ulam-Hyers-Rassias sense, then significant properties hold around the exact solution. In this way, awareness of the existence of such types of stability constitutes an important tool in many applications in different areas, such as numerical analysis, optimization, biology or even economics (e.g., specially when determining an exact solution is sometimes quite difficult).
Taking into account [25], we address the study of the Ulam-Hyers and the Ulam-Hyers-Rassias stabilities for the following Caputo fractional boundary value problem (which also includes the usual derivative):
(CDαax)(t)+p(t)x′(t)+q(t)x(t)=g(t),a<t<b,2<α<3, | (1.1) |
with x(a)=x′(a)=x(b)=0, where p,q and g∈C2([a,b]).
To the best of our knowledge, there is no results dealing with the Ulam-Hyers and Ulam-Hyers-Rassias stabilities of such fractional boundary value problem (FBVP).
The paper is organized as follows: Section 2 contains the necessary definitions from fractional calculus and the fundamental tools that are used throughout the paper; in Section 3, we focus on questions about the existence of solutions for the FBVP (1.1), identifying conditions for the existence of solutions and also for there to be only one solution; in Section 4, we discuss the Ulam-Hyers and the Ulam-Hyers-Rassias stabilities and introduce conditions for their existence. Finally, examples are given in Section 5 to illustrate the theoretical results.
In this section, just to have as self-contained work as possible, with the consequent benefit of the reader in mind, we recall some useful definitions and properties of the theory of fractional calculus [6] and necessary results in our future proofs.
We denote by Cn([a,b]):=(Cn([a,b]),‖⋅‖Cn) the space of functions x which are n-times continuously differentiable on [a,b] endowed with the norm ‖x‖Cn=∑nk=0supt∈[a,b]|x(k)(t)|. It is well-known that Cn([a,b]) is a Banach space.
Definition 1. [8] The Riemann-Liouville fractional integral of order α∈R+ of a function u is defined by
Iαau(t)=1Γ(α)∫ta(t−s)α−1u(s)ds, |
provided the right-hand side is pointwise defined on (a,∞), and where Γ is the well-known Euler Gamma function (given by Γ(α)=∫∞0tα−1e−tdt,α>0).
Definition 2. [8] The Caputo fractional derivative of order α>0 of a continuous function u is given by
CDαau(t)=1Γ(n−α)∫tau(n)(s)(t−s)α−n+1ds |
provided that the right-hand side is pointwise defined on (a,∞), and where n∈N is such that n−1<α<n.
It is clear that if α∈N, then CDαau(t)=(ddt)αu(t).
Proposition 1. [8,Lemma 2.22] Let n−1<α<n, n∈N. If f∈Cn−1([a,b]) (or f∈ACn−1([a,b])), then the following relation holds true:
(IαaCDαaf)(t)=f(t)−n−1∑k=0f(k)(a)k!(t−a)k. | (2.1) |
As explained above, there are some classic and essential results that we will use in this work. We will recall them here, stating the Banach Contraction Principle, the Krasnoselski Fixed Point Theorem and the Arzelà-Ascoli Theorem.
Theorem 1. (Banach Contraction Principle) Let (X,d) be a generalized complete metric space, and consider a mapping T:X→X which is a strictly contractive operator, that is,
d(Tx,Ty)≤Ld(x,y),∀x,y∈X |
for some constant 0≤L<1. Then
(a) the mapping T has a unique fixed point x∗=Tx∗;
(b) the fixed point x∗ is globally attractive, in the sense that for any starting point x∈X, the following identity holds true:
limn→∞Tnx=x∗; |
(c) we have the following inequalities:
d(Tnx,x∗)≤Lnd(x,x∗),n≥0,x∈X;d(Tnx,x∗)≤11−Ld(Tnx,Tn+1x),n≥0,x∈X;d(x,x∗)≤11−Ld(x,Tx),x∈X. |
Theorem 2. [26] (Krasnoselskii's Fixed Point Theorem) Let M be a closed, bounded, convex and nonempty subset of a Banach space X. Let A and B be operators such that
(i) Ax+By∈M whenever x,y∈M;
(ii) A is compact and continuous;
(iii) B is a contraction mapping.
Then, there exists z∈M such that z=Az+Bz.
Theorem 3. (Arzelà-Ascoli) Let (X,d) be a compact metric space. A set of functions F in C(X) is relatively compact if and only if it is bounded and equicontinuous.
In this section, we derive the existence and uniqueness of solutions of the FBVP (1.1). To that purpose, let us introduce some notation and three important results about the solutions of the FBVP under study (see [25] for related techniques in this context).
Proposition 2. A function x∈C2([a,b]) is a solution of the boundary value problem (1.1) if and only if x satisfies the integral equation
x(t)=(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds−1Γ(α)∫ta(t−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds. |
Proof. From Proposition 1, we can reduce the equation in the problem (1.1) to the following equivalent integral equation:
x(t)=c0+c1(t−a)+c2(t−a)2−1Γ(α)∫ta(t−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds. |
Having in mind the boundary conditions, we conclude that c0=x(a)=0 and c1=x′(a)=0. Thus, using the condition x(b)=0, one also obtains
c2=1(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds. |
Consequently, we have that
x(t)=(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds−1Γ(α)∫ta(t−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds |
and the proof is complete.
In what follows, we will use the notation
μ:=maxt∈[a,b]{|p(t)|,|q(t)|},supt∈[a,b]|g(t)|:=β, | (3.1) |
M1:=(b−a)αΓ(α+1)+(b−a)α−1Γ(α)+(b−a)α−2Γ(α−1), | (3.2) |
M2:=(b−a)αΓ(α+1)+2(b−a)α−1Γ(α+1)+2(b−a)α−2Γ(α+1). | (3.3) |
Theorem 4. If μ(M1+M2)<1, then the FBVP (1.1) has at least one solution in C2([a,b]).
Proof. From Proposition 2, we know that x∈C2([a,b]) is a solution of the FBVP (1.1) if and only if
x(t)=(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds−1Γ(α)∫ta(t−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds. |
Let us choose a suitable constant R such R≥(M1+M2)β1−(M1+M2)μ and consider the set BR={x∈C2([a,b]):‖x‖C2≤R}. Then, BR is a nonempty bounded closed convex subset in C2([a,b]). Now, we will define operators P and Q, on BR, as follows:
(Px)(t):=−1Γ(α)∫ta(t−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds,(Qx)(t):=(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds, |
for each t∈[a,b].
For any x,y∈BR, t∈[a,b], one has
|(Px)(t)|≤1Γ(α)∫ta(t−s)α−1(|p(s)||x′(s)|+|q(s)||x(s)|)ds+1Γ(α)∫ta(t−s)α−1|g(s)|ds≤1Γ(α)∫ta(t−s)α−1μ(|x′(s)|+|x(s)|)ds+1Γ(α)∫ta(t−s)α−1|g(s)|ds≤1Γ(α)∫ta(t−s)α−1μ(|x′(s)|+|x(s)|+|x″(s)|)ds+1Γ(α)∫ta(t−s)α−1|g(s)|ds≤μ‖x‖C2Γ(α)∫ta(t−s)α−1ds+βΓ(α)∫ta(t−s)α−1ds≤(b−a)αΓ(α+1)(μR+β), |
|(Px)′(t)|≤α−1Γ(α)∫ta(t−s)α−2(|p(s)||x′(s)|+|q(s)||x(s)|)ds+α−1Γ(α)∫ta(t−s)α−2|g(s)|ds≤α−1Γ(α)∫ta(t−s)α−2μ(|x′(s)|+|x(s)|)ds+α−1Γ(α)∫ta(t−s)α−2|g(s)|ds≤α−1Γ(α)∫ta(t−s)α−2μ(|x′(s)|+|x(s)|+|x″(s)|)ds+α−1Γ(α)∫ta(t−s)α−2|g(s)|ds≤(b−a)α−1Γ(α)(μR+β), |
and
|(Px)″(t)|≤(α−1)(α−2)Γ(α)(∫ta(t−s)α−3(|p(s)||x′(s)|+|q(s)||x(s)|)ds+∫ta(t−s)α−3|g(s)|ds)≤(α−1)(α−2)Γ(α)(∫ta(t−s)α−3μ(|x′(s)|+|x(s)|)ds+∫ta(t−s)α−3|g(s)|ds)≤(α−1)(α−2)Γ(α)(∫ta(t−s)α−3μ(|x′(s)|+|x(s)|+|x″(s)|)ds+∫ta(t−s)α−3|g(s)|ds)≤(b−a)α−2Γ(α−1)(μR+β). |
Thus, we conclude that
‖Px‖C2=supt∈[a,b]|(Px)(t)|+supt∈[a,b]|(Px)′(t)|+supt∈[a,b]|(Px)″(t)|≤M1(μR+β). |
In the same way, we get
|(Qx)(t)|≤(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1(|p(s)||x′(s)|+|q(s)||x(s)|)ds+(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1|g(s)|ds≤1Γ(α)∫ba(b−s)α−1μ(|x′(s)|+|x(s)|)ds+1Γ(α)∫ba(b−s)α−1|g(s)|ds≤μ‖x‖C2Γ(α)∫ba(b−s)α−1ds+βΓ(α)∫ba(b−s)α−1ds≤(b−a)αΓ(α+1)(μR+β), |
|(Qx)′(t)|≤2|t−a|(b−a)2Γ(α)∫ba(b−s)α−1(|p(s)||x′(s)|+|q(s)||x(s)|)ds+2|t−a|(b−a)2Γ(α)∫ba(b−s)α−1|g(s)|ds≤2(b−a)Γ(α)∫ba(b−s)α−1μ(|x′(s)|+|x(s)|)ds+2(b−a)Γ(α)∫ba(b−s)α−1|g(s)|ds≤2(b−a)α−1Γ(α+1)(μR+β), |
and
|(Qx)″(t)|≤2(b−a)2Γ(α)∫ba(b−s)α−1(|p(s)||x′(s)|+|q(s)||x(s)|)ds+2(b−a)2Γ(α)∫ba(b−s)α−1|g(s)|ds≤2(b−a)α−2Γ(α+1)(μR+β). |
Thus, we conclude that
‖Qy‖C2=supt∈[a,b]|(Qy)(t)|+supt∈[a,b]|(Qy)′(t)|+supt∈[a,b]|(Qy)″(t)|≤M2(μR+β). |
It follows that, for R≥(M1+M2)β1−(M1+M2)μ,
‖Px+Qy‖C2≤‖Px‖C2+‖Qy‖C2≤(M1+M2)(μR+β)≤R, |
and we conclude that Px+Qy∈BR, for x,y∈BR.
Let us show that P is a contraction. For every x,y∈BR, we have
‖Px−Py‖C2=supt∈[a,b]|(Px)(t)−(Py)(t)|+supt∈[a,b]|(Px)′(t)−(Py)′(t)|+supt∈[a,b]|(Px)″(t)−(Py)″(t)|≤M1μ‖x−y‖C2. |
Since M1μ<1, we conclude that P is a contraction.
Since c(t−a)2(b−a)2∈C2([a,b]) for any c∈R, we have that Qx∈C2([a,b]). Moreover, for any bounded subset BR of C2([a,b]) and x∈BR, we have that
‖Qx‖C2≤M2(μR+β) |
which shows that the operator Q is uniformly bounded on BR.
Let us prove that Q is a compact operator on BR. Take t1,t2∈[a,b] with t2≥t1. One has
|(Qx)(t2)−(Qx)(t1)|=|(t2−a)2−(t1−a)2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds|≤(t2−a)2−(t1−a)2Γ(α+1)(μR+β)(b−a)α−2. |
It is seen that |(Qx)(t2)−(Qx)(t1)|→0 as t2→t1. Also, we have
|(Qx)′(t2)−(Qx)′(t1)|=|2(t2−a)−2(t1−a)(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds|≤2(t2−a)−2(t1−a)Γ(α+1)(μR+β)(b−a)α−2. |
Again, we have that |(Qx)′(t2)−(Qx)′(t1)|→0 as t2→t1. Finally, we observe that
|(Qx)″(t2)−(Qx)″(t1)|=0. |
Thus, we conclude that QBR is equicontinuous. By Arzelà-Ascoli Theorem, QBR is compact for each bounded subset BR⊂C2([a,b]), and thus, Q is compact.
Applying Krasnoselskii's Fixed Point Theorem to the operators P and Q, we conclude that there exists at least one x∈BR such that x=Px+Qx which is the solution of the FBVP (1.1) and the proof is complete.
Theorem 5. If the following condition holds
μ(M1+M2)<1, | (3.4) |
then the FBVP (1.1) has a unique solution in x∈C2([a,b]).
Proof. From Theorem 4, since μ(M1+M2)<1, the FBVP (1.1) has at least one solution. Let us define the operator T:C2([a,b])→C2([a,b]) by
(Tx)(t):=(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds−1Γ(α)∫ta(t−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds. | (3.5) |
By the Banach Contraction Principle, we will prove that T has a unique fixed point.
Let BR={x∈C2([a,b]):‖x‖C2≤R} and choose R such that
R≥(M1+M2)β1−(M1+M2)μ. |
We have
‖Tx‖C2=supt∈[a,b]|(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds−1Γ(α)∫ta(t−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds|+supt∈[a,b]|2(t−a)(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds−α−1Γ(α)∫ta(t−s)α−2(p(s)x′(s)+q(s)x(s)−g(s))ds|+supt∈[a,b]|2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)x′(s)+q(s)x(s)−g(s))ds−(α−1)(α−2)Γ(α)∫ta(t−s)α−3(p(s)x′(s)+q(s)x(s)−g(s))ds|≤(M1+M2)(μR+β). |
Thus, ‖Tx‖C2≤R, i.e., TBR⊂BR. Moreover, since p,q,g∈C2([a,b]), we conclude that Tx∈C2([a,b]) for any x∈C2([a,b]), which proves that T maps C2([a,b]) into itself.
Let us prove that T is strictly contractive. Consider x,y∈C2([a,b]). It follows that
‖Tx−Ty‖C2=supt∈[a,b]|(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)(x′(s)−y′(s))+q(s)(x(s)−y(s)))ds−1Γ(α)∫ta(t−s)α−1(p(s)(x′(s)−y′(s))+q(s)(x(s)−y(s)))ds|+supt∈[a,b]|2(t−a)(b−a)2Γ(α)∫ba(b−s)α−1(p(s)(x′(s)−y′(s))+q(s)(x(s)−y(s))ds−α−1Γ(α)∫ta(t−s)α−2(p(s)(x′(s)−y′(s))+q(s)(x(s)−y(s)))ds|+supt∈[a,b]|2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)(x′(s)−y′(s))+q(s)(x(s)−y(s)))ds−(α−1)(α−2)Γ(α)∫ta(t−s)α−3(p(s)(x′(s)−y′(s))+q(s)(x(s)−y(s)))ds|≤1Γ(α)∫ba(b−s)α−1(|p(s)||x′(s)−y′(s)|+|q(s)||x(s)−y(s)|)ds+1Γ(α)∫ba(b−s)α−1(|p(s)|x′(s)−y′(s)|+|q(s)||x(s)−y(s)|)ds+2(b−a)Γ(α)∫ba(b−s)α−1(|p(s)||x′(s)−y′(s)|+|q(s)||x(s)−y(s)|)ds+α−1Γ(α)∫ba(b−s)α−2(|p(s)||x′(s)−y′(s)|+|q(s)||x(s)−y(s)|)ds+2(b−a)2Γ(α)∫ba(b−s)α−1(|p(s)||x′(s)−y′(s)|+|q(s)||x(s)−y(s)|)ds+(α−1)(α−2)Γ(α)∫ba(b−s)α−3(|p(s)||x′(s)−y′(s)|+|q(s)||x(s)−y(s)|)ds≤μΓ(α)∫ba(b−s)α−1(|x(s)−y(s)|+|x′(s)−y′(s)|+|x″(s)−y″(s)|)ds+μΓ(α)∫ba(b−s)α−1(|x(s)−y(s)|+|x′(s)−y′(s)|+|x″(s)−y″(s)|)ds+2μ(b−a)Γ(α)∫ba(b−s)α−1(|x(s)−y(s)|+|x′(s)−y′(s)|+|x″(s)−y″(s)|)ds+μ(α−1)Γ(α)∫ba(b−s)α−2(|x(s)−y(s)|+|x′(s)−y′(s)|+|x″(s)−y″(s)|)ds+2μ(b−a)2Γ(α)∫ba(b−s)α−1(|x(s)−y(s)|+|x′(s)−y′(s)|+|x″(s)−y″(s)|)ds+μ(α−1)(α−2)Γ(α)∫ba(b−s)α−3(|x(s)−y(s)|+|x′(s)−y′(s)|+|x″(s)−y″(s)|)ds≤μ(2(b−a)αΓ(α+1)+2(b−a)α−1Γ(α+1)+(b−a)α−1Γ(α)+2(b−a)α−2Γ(α+1)+(b−a)α−2Γ(α−1))‖x−y‖C2=μ(M1+M2)‖x−y‖C2. | (3.6) |
Since by hypothesis μ(M1+M2)<1, we conclude that T is strictly contractive.
By Banach Contraction Principle, T has a unique fixed point in C2([a,b]) which is the unique solution of the FBVP (1.1).
In this section, we analyse the Ulam-Hyers and the Ulam-Hyers-Rassias stabilities of FBVP (1.1). To that purpose, let us first present the definitions of those notions in the sense of our FBVP.
Definition 3. The FBVP (1.1) is Ulam-Hyers stable if there exists a real constant k>0 such that, for each ϵ>0 and for each solution y∈C2([a,b]) of the inequality problem
{|(CDαay)(t)+p(t)y′(t)+q(t)y(t)−g(t)|≤ϵ,t∈[a,b],y′(a)=y(a)=y(b)=0, |
there exists a solution x∈C2([a,b]) of the problem (1.1) such that
‖y−x‖C2≤kϵ. |
Definition 4. The FBVP (1.1) is Ulam-Hyers-Rassias stable with respect to φ:[a,b]→R+ if there exists a real constant kφ>0 such that, for each ϵ>0 and for each solution y∈C2([a,b]) of the inequality problem
{|(CDαay)(t)+p(t)y′(t)+q(t)y(t)−g(t)|≤ϵφ(t),t∈[a,b],y′(a)=y(a)=y(b)=0, |
there exists a solution x∈C2([a,b]) of the problem (1.1) with
‖y−x‖C2≤kφϵφ(t),t∈[a,b]. |
In the next theorem, we present sufficient conditions upon which the FBVP (1.1) is Ulam-Hyers stable.
Theorem 6. Suppose that μ(M1+M2)<1. Let x(t) be the solution of the FBVP (1.1) and y(t) be such that y(a)=y′(a)=y(b)=0 and
|(CDαay)(t)+p(t)y′(t)+q(t)y(t)−g(t)|≤ϵ,t∈[a,b], | (4.1) |
where ϵ>0. Then, there exists a constant k>0 such that
‖y−x‖C2≤kϵ, |
which means that the FBVP (1.1) is Ulam-Hyers stable.
Proof. By Theorems 4 and 5, the solution of the FBVP (1.1) exists and is unique. Let x(t) be that unique solution of the FBVP (1.1) and suppose y(t) satisfies inequality (Eq 4.1). It follows that y∈C2([a,b]) is a solution of inequality (Eq 4.1) if and only if there exists a function h∈C2([a,b]), which depends on y such that
(i) |h(t)|≤ϵ, t∈[a,b], ϵ>0,
(ii) h(t)=(CDαay)(t)+p(t)y′(t)+q(t)y(t)−g(t), t∈[a,b],
(iii) y(a)=y′(a)=y(b)=0.
Computing the α-order Riemann-Liouville fractional integral of each member in (ii), according to Proposition 1, we obtain
y(t)−y(a)−y′(a)(t−a)−y″(a)2(t−a)2+(Iαa(py′))(t)+(Iαa(qy))(t)−(Iαa(g−h))(t)=0 |
Since y(a)=y′(a)=0, we have
y(t)=d1(t−a)2−1Γ(α)∫ta(t−s)α−1(p(s)y′(s)+q(s)y(s)−g(s)−h(s))ds |
where d1=y″(a)2.
Moreover, attending that y(b)=0, we have
d1=1(b−a)2Γ(α)∫ba(b−s)α−1(p(s)y′(s)+q(s)y(s)−g(s)−h(s))ds |
and we conclude that
y(t)=(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)y′(s)+q(s)y(s)−g(s)−h(s))ds−1Γ(α)∫ta(t−s)α−1(p(s)y′(s)+q(s)y(s)−g(s)−h(s))ds. |
Recalling the operator T, defined in (3.5), from (3.6) we already know that under the present conditions T is a contraction and that
‖Tx−Ty‖C2≤μ(M1+M2)‖x−y‖C2. |
Thus, from Theorem 1, we have
‖x−y‖C2≤11−μ(M1+M2)‖Ty−y‖C2. | (4.2) |
Moreover, we have that
‖Ty−y‖C2=supt∈[a,b]|(Ty)(t)−y(t)|+supt∈[a,b]|(Ty)′(t)−y′(t)|+supt∈[a,b]|(Ty)″(t)−y″(t)|=supt∈[a,b]|(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1h(s)ds−1Γ(α)∫ta(t−s)α−1h(s)ds|+supt∈[a,b]|2(t−a)(b−a)2Γ(α)∫ba(b−s)α−1h(s)ds−α−1Γ(α)∫ta(t−s)α−2h(s)ds|+supt∈[a,b]|2(b−a)2Γ(α)∫ba(b−s)α−1h(s)ds−(α−1)(α−2)Γ(α)∫ta(t−s)α−3h(s)ds|≤1Γ(α)∫ba(b−s)α−1|h(s)|ds+1Γ(α)∫ba(b−s)α−1|h(s)|ds+2(b−a)Γ(α)∫ba(b−s)α−1|h(s)|ds+α−1Γ(α)∫ba(b−s)α−2|h(s)|ds+2(b−a)2Γ(α)∫ba(b−s)α−1|h(s)|ds+(α−1)(α−2)Γ(α)∫ba(b−s)α−3|h(s)|ds≤ϵ(2(b−a)αΓ(α+1)+2(b−a)α−1Γ(α+1)+(b−a)α−1Γ(α)+2(b−a)α−2Γ(α+1)+(b−a)α−1Γ(α−1))=(M1+M2)ϵ. |
Therefore, taking also (4.2) into account, we obtain
‖x−y‖C2≤M1+M21−μ(M1+M2)ϵ |
and we conclude that the FBVP (1.1) is Ulam-Hyers stable.
In the next theorem, we present sufficient conditions for the FBVP (1.1) to be Ulam-Hyers-Rassias stable.
Theorem 7. Assume that μ(M1+M2)<1. Let x(t) be the solution of the FBVP (1.1) and y(t) be such that y(a)=y′(a)=y(b)=0 and
|(CDαay)(t)+p(t)y′(t)+q(t)y(t)−g(t)|≤ϵφ(t),t∈[a,b] | (4.3) |
where ϵ>0 and φ:[a,b]→R+ satisfies the property
(Iτaφ)(b)≤φ(t),t∈[a,b],τ=α,α−1,α−2,α∈(2,3). | (4.4) |
Then, there exists a constant kφ>0 such that
‖y−x‖C2≤kφϵφ(t),t∈[a,b], |
which means that the FBVP (1.1) is Ulam-Hyers-Rassias stable.
Proof. By Theorems 4 and 5, the solution of the FBVP (1.1) exists and is unique. Let x(t) be the unique solution of the FBVP (1.1) and suppose that y(t) satisfies inequality (Eq 4.3). It follows that y∈C2([a,b]) is a solution of inequality (Eq 4.3) if and only if there exists a function f∈C2([a,b]) depending on y and such that
(i) |f(t)|≤ϵφ(t), t∈[a,b], ϵ>0,
(ii) f(t)=(CDαay)(t)+p(t)y′(t)+q(t)y(t)−g(t), t∈[a,b],
(iii) y(a)=y′(a)=y(b)=0.
Using (ii), we can proceed similarly as in the proof of the previous theorem and obtain
y(t)=(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1(p(s)y′(s)+q(s)y(s)−g(s)−f(s))ds−1Γ(α)∫ta(t−s)α−1(p(s)y′(s)+q(s)y(s)−g(s)−f(s))ds. |
Recalling the operator T, defined in (3.5), having into account condition (4.4), we have
‖Ty−y‖C2=supt∈[a,b]|(Ty)(t)−y(t)|+supt∈[a,b]|(Ty)′(t)−y′(t)|+supt∈[a,b]|(Ty)″(t)−y″(t)|=supt∈[a,b]|(t−a)2(b−a)2Γ(α)∫ba(b−s)α−1f(s)ds−1Γ(α)∫ta(t−s)α−1f(s)ds|+supt∈[a,b]|2(t−a)(b−a)2Γ(α)∫ba(b−s)α−1f(s)ds−α−1Γ(α)∫ta(t−s)α−2f(s)ds|+supt∈[a,b]|2(b−a)2Γ(α)∫ba(b−s)α−1f(s)ds−(α−1)(α−2)Γ(α)∫ta(t−s)α−3f(s)ds|≤1Γ(α)∫ba(b−s)α−1|f(s)|ds+1Γ(α)∫ba(b−s)α−1|f(s)|ds+2(b−a)Γ(α)∫ba(b−s)α−1|f(s)|ds+α−1Γ(α)∫ba(b−s)α−2|f(s)|ds+2(b−a)2Γ(α)∫ba(b−s)α−1|f(s)|ds+(α−1)(α−2)Γ(α)∫ba(b−s)α−3|f(s)|ds≤1Γ(α)∫ba(b−s)α−1ϵφ(s)ds+1Γ(α)∫ba(b−s)α−1ϵφ(s)ds+2(b−a)Γ(α)∫ba(b−s)α−1ϵφ(s)ds+α−1Γ(α)∫ba(b−s)α−2ϵφ(s)ds+2(b−a)2Γ(α)∫ba(b−s)α−1ϵφ(s)ds+(α−1)(α−2)Γ(α)∫ba(b−s)α−3ϵφ(s)ds≤ϵ(φ(t)+φ(t)+2b−aφ(t)+φ(t)+2(b−a)2φ(t)+φ(t)),t∈[a,b]≤4(b−a)2+2(b−a)+2(b−a)2ϵφ(t),t∈[a,b]. |
From the proof of Theorem 5 (cf. (3.6)), we have that the operator T is a contraction with
‖Tx−Ty‖C2≤μ(M1+M2)‖x−y‖C2. |
Thus, using Banach Contraction Principle (Theorem 1), we obtain that
‖x−y‖C2≤4(b−a)2+2(b−a)+2(b−a)21−μ(M1+M2)ϵφ(t),t∈[a,b]. |
Taking
kφ=4(b−a)2+2(b−a)+2(b−a)21−μ(M1+M2), |
we have ‖x−y‖C2≤kφϵφ(t), t∈[a,b], and so we conclude that the FBVP (1.1) is Ulam-Hyers-Rassias stable.
Consider the following FBVP:
{(CD520x)(t)+15cos(t)x′(t)+16sin(t)x(t)=t2,t∈[0,34]x(0)=x′(0)=x(34)=0. | (5.1) |
In the notation of (1.1), we have in here p(t)=15cos(t), q(t)=16sin(t), g(t)=t2∈C2([0,34]) and α=52. Moreover, considering the notations (3.1)–(3.3), we realize that
μ=15,M1<5815√π,M2<83√π. |
Thus,
μ(M1+M2)<9875√π<1 |
and we conclude that the FBVP (5.1) has a unique solution and it is Ulam-Hyers stable.
Consider now φ(t)=−0,1t2+2. For any t∈[0,34], one has
I520φ(t)<φ(t),I320φ(t)<φ(t),I120φ(t)<φ(t),t∈[0,34] |
(see Figure 1).
Therefore, from Theorem 7, we conclude that the FBVP (5.1) is Ulam-Hyers-Rassias stable with respect to φ.
Fractional calculus has gained considerable popularity and importance during the last few decades, mainly due to its attractive applications in various areas of science and engineering. In particular, fractional boundary value problems have been used in the fields of physics, biology, chemistry, economics, electromagnetic theory, image and signal processing. In fact, boundary problems involving fractional differential equations model certain situations – such as the study of heredity and memory problems – better than integer-order differential equations. Given the difficulty in obtaining exact explicit solutions for such problems, it becomes important to study their eventual different types of stability, in particular, the Ulam-Hyers and Ulam-Hyers-Rassias stabilities.
In this article, we analyzed a class of fractional boundary value problems involving Caputo's fractional derivative as well as the usual (integer) derivative. Using several Functional Analysis techniques (including, for example, Krasnoselskii's Fixed Point Theorem), we obtained sufficient conditions to guarantee the existence of solutions to this class of problems and we also obtained conditions for the uniqueness of these solutions. Finally, we establish – in the form of sufficient conditions – the Ulam-Hyers and Ulam-Hyers-Rassias stabilities. At the end, a concrete example was given to illustrate the obtained theoretical results.
The authors thank the Referees for their constructive comments and recommendations which helped to improve the readability and quality of the paper.
This work is supported by the Center for Research and Development in Mathematics and Applications (CIDMA) through the Portuguese Foundation for Science and Technology (FCT - Fundação para a Ciência e a Tecnologia), reference UIDB/04106/2020.
Additionally, A. Silva is also funded by national funds (OE), through FCT, I.P., in the scope of the framework contract foreseen in the numbers 4, 5 and 6 of the article 23, of the Decree-Law 57/2016, of August 29, changed by Law 57/2017, of July 19.
The authors declare there is no conflict of interest.
[1] | K. Diethelm, A. D. Freed, On the solution of nonlinear fractional order differential equations used in the modeling of viscoplasticity, in Scientific Computing in Chemical Engineering II-Computational Fluid Dynamics, Reaction Engineering and Molecular Properties (eds. F. Keil, W. Mackens, H. Voss and J. Werther), Springer, Heidelberg, (1999), 217–224. https://doi.org/10.1007/978-3-642-60185-9_24 |
[2] |
W. G. Glockle, T. F. Nonnenmacher, A fractional calculus approach of self-similar protein dynamics, Biophys. J., 68 (1995), 46–53. https://doi.org/10.1016/S0006-3495(95)80157-8 doi: 10.1016/S0006-3495(95)80157-8
![]() |
[3] | R. Hilfer, Applications of Fractional Calculus in Physics, World Scientific, Singapore, 2000. |
[4] |
F. Metzler, W. Schick, H. G. Kilian, T. F. Nonnenmacher, Relaxation in filled polymers: A fractional calculus approach, J. Chem. Phys., 103 (1995), 7180–7186. https://doi.org/10.1063/1.470346 doi: 10.1063/1.470346
![]() |
[5] | I. Podlubny, Fractional Differential Equations, Academic Press, San Diego, 1999. |
[6] | S. G. Samko, A. A. Kilbas, O. I. Marichev, Fractional Integrals and Derivatives-Theory and Applications, Gordon and Breach Science Publishers, Amsterdam, 1993. |
[7] |
A. Jajarmi, A. Yusuf, D. Baleanu, M. Inc, A new fractional HRSV model and its optimal control: a non-singular operator approach, Phys. A, 547 (2020), 1–11. https://doi.org/10.1016/j.physa.2019.123860 doi: 10.1016/j.physa.2019.123860
![]() |
[8] | A. A. Kilbas, H. M. Srivastava, J. J. Trujillo, Theory and Applications of Fractional Differential Equations, Elsevier, Amsterdam, 2016. |
[9] |
M. Ahmad, A. Zada, J. Alzabut, Hyers–Ulam stability of coupled system of fractional differential equations of Hilfer–Hadamard type, Demonstr. Math., 52 (2019), 283–295. https://doi.org/10.1515/dema-2019-0024 doi: 10.1515/dema-2019-0024
![]() |
[10] |
Y. Guo, X. Shu, Y. Li, F. Xu, The existence and Hyers–Ulam stability of solution for an impulsive Riemann–Liouville fractional neutral functional stochastic differential equation with infinite delay of order 1<β<2, Boundary Value Probl., 59 (2019), 1–18. https://doi.org/10.1186/s13661-019-1172-6 doi: 10.1186/s13661-019-1172-6
![]() |
[11] | C. Yang, C. Zhai, Uniqueness of positive solutions for a fractional differential equation via a fixed point theorem of a sum operator, Electron. J. Differ. Equations, 70 (2012), 1–8. Available from: https://www.researchgate.net/publication/265759303. |
[12] | A. Zada, J. Alzabut, H. Waheed, P. Loan-Lucian, Ulam–Hyers stability of impulsive integro-differential equations with Riemann-Liouville boundary conditions, Adv. Differ. Equations, 2020 (2020). https://doi.org/10.1186/s13662-020-2534-1 |
[13] |
X. Zhao, C. Chai, W. Ge, Positive solutions for fractional four-point boundary value problems, Commun. Nonlinear Sci. Numer. Simul., 16 (2011), 3665–3672. https://doi.org/10.1016/j.cnsns.2011.01.002 doi: 10.1016/j.cnsns.2011.01.002
![]() |
[14] |
C. Zhai, L. Xu, Properties of positive solutions to a class of four-point boundary value problem of Caputo fractional differential equations with a parameter, Commun. Nonlinear Sci. Numer. Simul., 19 (2014), 2820–2827. https://doi.org/10.1016/j.cnsns.2014.01.003 doi: 10.1016/j.cnsns.2014.01.003
![]() |
[15] | S. M. Ulam, Problems in Modern Mathematics, John Wiley & Sons, New York, 1940. |
[16] |
D. H. Hyers, On the stability of the linear functional equation, Proc. Natl. Acad. Sci. U.S.A., 27 (1941), 222–224. https://doi.org/10.1073/pnas.27.4.222 doi: 10.1073/pnas.27.4.222
![]() |
[17] |
T. Aoki, On the stability of the linear transformation in Banach spaces, J. Math. Soc. Jpn., 2 (1950), 64–66. https://doi.org/10.2969/jmsj/00210064 doi: 10.2969/jmsj/00210064
![]() |
[18] |
T. M. Rassias, On the stability of the linear mapping in Banach spaces, Proc. Am. Math. Soc., 72 (1978), 297–300. https://doi.org/10.1090/S0002-9939-1978-0507327-1 doi: 10.1090/S0002-9939-1978-0507327-1
![]() |
[19] |
M. Akkouchi, Stability of certain functional equations via a fixed point of Ćirić, Filomat, 25 (2011), 121–127. https://doi.org/10.2298/FIL1102121A doi: 10.2298/FIL1102121A
![]() |
[20] |
S. András, A. Mészáros, Ulam-Hyers stability of dynamic equations on time scales via Picard operators, Appl. Math. Comput., 219 (2013), 4853–4864. https://doi.org/10.1016/j.amc.2012.10.115 doi: 10.1016/j.amc.2012.10.115
![]() |
[21] |
R. Bellman, The stability of solutions of linear differential equations, Duke Math. J., 10 (1943), 643–647. https://doi.org/10.1215/S0012-7094-43-01059-2 doi: 10.1215/S0012-7094-43-01059-2
![]() |
[22] |
L. P. Castro, R. C. Guerra, Hyers-Ulam-Rassias stability of Volterra integral equations within weighted spaces, Lib. Math., 33 (2013), 21–35. http://doi.org/10.14510/lm-ns.v33i2.50 doi: 10.14510/lm-ns.v33i2.50
![]() |
[23] |
L. P. Castro, A. M. Simões, Different types of Hyers-Ulam-Rassias stabilities for a class of integro-differential equations, Filomat, 31 (2017), 5379–5390. https://doi.org/10.2298/FIL1717379C doi: 10.2298/FIL1717379C
![]() |
[24] |
L. P. Castro, A. M. Simões, Hyers-Ulam-Rassias stability of nonlinear integral equations through the Bielecki metric, Math. Methods Appl. Sci., 41 (2018), 7367–7383. https://doi.org/10.1002/mma.4857 doi: 10.1002/mma.4857
![]() |
[25] |
E. Pourhadi, M. Mursaleen, A new fractional boundary value problem and Lyapunov-type inequality, J. Math. Inequal., 15 (2021), 81–93. https://doi.org/10.7153/JMI-2021-15-08 doi: 10.7153/JMI-2021-15-08
![]() |
[26] | M. A. Krasnoselskii, Two remarks on the method of successive approximations (in Russian), Usp. Mat. Nauk, 10 (1955), 123–127. |
1. | Luís P. Castro, Anabela S. Silva, On the Existence and Stability of Solutions for a Class of Fractional Riemann–Liouville Initial Value Problems, 2023, 11, 2227-7390, 297, 10.3390/math11020297 | |
2. | Poovarasan R, Pushpendra Kumar, V. Govindaraj, Marina Murillo-Arcila, The existence, uniqueness, and stability results for a nonlinear coupled system using ψ-Caputo fractional derivatives, 2023, 2023, 1687-2770, 10.1186/s13661-023-01769-4 | |
3. | Naoufel Hatime, Ali El Mfadel, M.’hamed Elomari, Said Melliani, EXISTENCE AND STABILITY OF SOLUTIONS FOR NONLINEAR FRACTIONAL DIFFERENTIAL EQUATIONS INVOLVING THE GRÖNWALL-FREDHOLM-TYPE INEQUALITY, 2024, 1072-3374, 10.1007/s10958-024-07202-0 | |
4. | Ragheb Mghames, Yahia Awad, Karim Amin, Hussein Falih, Rabab Hamad, A Complex Delay Differential Equations Model for Acute Lymphoblastic Leukemia, 2024, 21, 2224-2902, 363, 10.37394/23208.2024.21.37 | |
5. | Karim Amin, Yahia Awad, Ragheb Mghames, Samia Mrad, Analysis of Stability in a Delay Differential Equation Model for Malaria InfectionWith Treatment, 2024, 22, 2224-2902, 110, 10.37394/23208.2025.22.13 | |
6. | R. Poovarasan, Mohammad Esmael Samei, V. Govindaraj, Analysis of existence, uniqueness, and stability for nonlinear fractional boundary value problems with novel integral boundary conditions, 2025, 1598-5865, 10.1007/s12190-025-02378-3 |