Recently, initial-boundary-value problems with the Caputo fractional derivative for ordinary differential equations have been intensively studied. This paper studies a nonlinear integro-differential equation of fractional order, containing a composition of fractional derivatives with different origins and mixed conditions. The equation under consideration acts as a model equation of motion in a fractal medium. First, we use three fixed-point theorems to prove the existence and uniqueness results. Then, the Ulam stability criterion of the solution is given. The main results will be illustrated by a proposed example.
Citation: Naimi Abdellouahab, Keltum Bouhali, Loay Alkhalifa, Khaled Zennir. Existence and stability analysis of a problem of the Caputo fractional derivative with mixed conditions[J]. AIMS Mathematics, 2025, 10(3): 6805-6826. doi: 10.3934/math.2025312
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Recently, initial-boundary-value problems with the Caputo fractional derivative for ordinary differential equations have been intensively studied. This paper studies a nonlinear integro-differential equation of fractional order, containing a composition of fractional derivatives with different origins and mixed conditions. The equation under consideration acts as a model equation of motion in a fractal medium. First, we use three fixed-point theorems to prove the existence and uniqueness results. Then, the Ulam stability criterion of the solution is given. The main results will be illustrated by a proposed example.
The analytical apparatus of fractional integro-differentiation and the theory of fractional differential equations demonstrate high efficiency in the description and mathematical modeling of various physical and geophysical processes occurring in fractal environments. Using the concept of the effective rate of the change in the number of parameters of the modeled systems leads to differential equations that contain a composition of fractional differentiation operators of different origins; see [1,2,3]. More than 300 years ago, scientists used incorrect random orders to generalize ordinary differential equations and integrals using fractional differential equations. The origin of fractional calculus goes to Newton and Leibniz; see [4,5,6]. Fractional differential equations are useful for many models: physical, biological, genetic, and even economic phenomena. Several recent studies have been carried out by researchers to prove the existence and uniqueness of the solution for fractional differential equations with different conditions (boundary, initial, nonlocal, and integral conditions, etc.). For more details, the reader is referred to [7,8,9] and the references therein. For a more comprehensive and informative presentation and to illustrate the broad applicability of fractional calculus, we mention the work in [10] for fluid dynamics, mathematical biology [11,12], image denoising [13,14], and image super-resolution[15,16]. In ancient times, the study of the stability of solutions of fractional differential equations was slow, but recently many researchers have done it in different articles in several ways (asymptotically stable, Ulam stable, generalized Ulam stable, ...), see [17,18,19].
In [20], the system is governed by a Caputo fractional with a nonlocal initial condition
{CaDν0+ϖ(z)=h(ϖ(z))+ψ(z,ϖ(z))+∫z0N(z,s,ϖ(s))ds,ϖ(0)=σγ∫0ϖ(s)ds,0<γ<1, | (1.1) |
is considered. The authors investigated the existence and uniqueness of the solution using the Banach and Krasnoselskii fixed-point theorems.
In [21], using the Banach contraction mapping together with the Burton-Kirk fixed-point theorem, the authors obtained certain results on the existence and uniqueness of a solution for the problem with the Caputo fractional delay
{CaDα0+ϖ(z)=f(z,ϖz,CaDν0+ϖ), 0≤z≤1,ϖ(0)=0,ϖ′(0)=aIσ0+ϖ(η),bϖ(1)+cϖ′(1)=g(ϖ),ϖ(t)=ϕ(z), z∈[−τ,0], | (1.2) |
with appropriate conditions on the parameters of nonlocal and integral boundary value. In [22], the problem with the Riemann-Liouville fractional integral in the RHS of
{CaDν+κ0+ϖ(z)=ω(z,ϖ(z))+Iν0+ψ(z,ϖ(z))+∫z0N(z,s,ϖ(s))dsϖ(0)=b∫η0ϖ(z)dz,0<η<1, | (1.3) |
is considered. Using a combination of the Krasnoselskii and Banach fixed-point theorems, results on the existence and uniqueness are proved. In addition, some suitable conditions are provided that ensure the generalized Ulam stability of the system.
In light of these studies, we shall prove that the unique solution exists with the Ulam stability of the following system:
{CaDν+κ0+ϖ(z)=ω(z,ϖ(z))+CaDν0+ψ(z,ϖ(z))+∫z0N(z,s,ϖ(s))ds,ϖ(0)=ϖ0,ϖ′(0)=ϖ1γ∫0ϖ(s)ds,0<γ<1, | (1.4) |
where ϖ0,ϖ1 are real constants, 1<ν+κ≤2, the functional CaDκ0+ is the Caputo fractional derivative of order κ, and ω,ψ, and N are appropriate functions given by the following:
ω:J×E⟶E,ψ:J×E⟶E,N:J×J×E⟶E, | (1.5) |
where E is a Banach space. The existence and stability analysis for the problem (1.4) involving the Caputo fractional derivative with mixed conditions typically refers to studying the behavior and solutions of fractional differential equations (FDEs) under a specific boundary. The Caputo fractional derivative is one of the most commonly used definitions of fractional derivatives, particularly because of its useful properties in physical and engineering applications. Equation (1.4)1 is studied under mixed conditions (1.4)2 to extend the work in [22], where only the integral boundary condition was taken and the problem was with the Riemann-Liouville fractional integral in the RHS of the differential equation and the works [23,24], in which the authors used fractional integration in the equation with the initial condition, but here we used the fractional derivative instead with mixed conditions.
Our study is based on the three-fixed-point theorem, and the goal is to prove the existence and uniqueness results for the solution. In Section 2, some preliminary and integral equations are given. The generalized stability is shown in Section 3. It should be noted that this representation constitutes a generalization of recent results obtained in this research area. To illustrate our results, we conclude the article with examples.
In this section, we present the definitions of fractional integral, fractional Caputo derivative, and some auxiliary lemmas. We refer to [25,26,27,28] for essential preliminary concepts regarding fractional calculus and fixed-point theory.
Definition 2.1. [25] Let κ>0 and ℏ:R+⟶R. The Riemann-Liouville fractional integral of order κ of a function ℏ is given by
Iκ0+ℏ(z)=1Γ(κ)∫z0(z−s)κ−1(s)ℏ(s)ds,z∈R+. |
Definition 2.2. [28] Let κ>0; the order κ Caputo fractional derivative of a function ℏ:R+⟶R is defined by
CaDκ0+ℏ(z)=1Γ(n−κ)∫z0(z−s)n−κ−1ℏ(n)(s)ds=In−κ0+ℏ(n)(z),z∈R+, |
where n=[κ]+1, and the right-hand side is point-wise defined on R+.
Lemma 2.1. [25] For κ>0, i∈R, and the appropriate function ℏ(z)∈Cn−1[0,∞), where ℏ(z) exists almost everywhere in any bounded interval of R+, we have
(Iκ0+CaDκ0+ℏ)(z)=ℏ(z)−n−1∑i=0ℏ(i)(0)i!zi. |
Lemma 2.2. Let 1<ν+κ<2 and ϖ1≠2γ2. Assume that ω,ψ and N are three continuous functions. If ϖ∈C(J,E), then ϖ is a solution of (1.4) if and only if ϖ satisfies the integral equation
ϖ(z)=∫z0(z−s)ν+κ−1Γ(ν+κ)(ω(s,ϖ(s))+∫s0N(s,τ,ϖ(τ))dτ)ds+∫z0(z−s)κ−1Γ(κ)ψ(s,ϖ(s))ds+ϖ0−ψ(0,ϖ0)Γ(κ+1)zκ+zϖ1(1−γ22ϖ1)[∫γ0(γ−τ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))+∫τ0N(τ,σ,ϖ(σ))dσ)dτ+∫γ0(γ−τ)κΓ(κ+1)ψ(τ,ϖ(τ))dτ−ψ(0,ϖ0)Γ(κ+2)γκ+1+γϖ0]. | (2.1) |
Proof. Assume that ϖ∈C(J,E) is a solution of (1.4), and the goal is to prove that ϖ satisfies (2.1). By Lemma 2.1, we obtain
Iν+κ0+ CaDν+κ0+ϖ(z)=ϖ(z)−ϖ(0)−ϖ′(0)z. | (2.2) |
Then, by (1.4), Lemma 2.1, and Definition 2.1, we obtain
Iν+κ0+ CaDν+κ0+ϖ(z)=Iν+κ0+(ω(z,ϖ(z))+∫z0N(z,s,ϖ(s))ds+CaDν0+ψ(z,ϖ(z)))=Iν+κ0+(ω(z,ϖ(z))+∫z0N(z,s,ϖ(s))ds)+Iκ0+ψ(z,ϖ(z))−ψ(0,ϖ0)Γ(κ+1)zκ. | (2.3) |
Substituting (2.3) in (2.2) with the first condition in (1.4) yields:
ϖ(z)=Iν+κ0+(ω(z,ϖ(z))+∫z0N(z,s,ϖ(s))ds)+Iκ0+ψ(z,ϖ(z))−ψ(0,ϖ0)Γ(κ+1)zκ+ϖ0+ϖ′(0)z. | (2.4) |
But we have
ϖ′(0)ϖ1=∫γ0ϖ(s)ds=∫γ0[Iν+κ0+[ω(s,ϖ(s))+∫s0N(s,τ,ϖ(τ))dτ]+Iκ0+ψ(s,ϖ(s))+ϖ′(0)s+ϖ0−ψ(0,ϖ0)Γ(κ+1)sκ]ds=∫γ0[Iν+κ0+[ω(s,ϖ(s))+∫s0N(s,τ,ϖ(τ))dτ]+Iκ0+ψ(s,ϖ(s))]ds−ψ(0,ϖ0)Γ(κ+2)γκ+1+γϖ0+γ22ϖ′(0)=Iν+κ+10+[ω(γ,ϖ(γ))+∫γ0N(γ,τ,ϖ(τ))dτ]+Iκ+10+ψ(γ,ϖ(γ))−ψ(0,ϖ0)Γ(κ+2)γκ+1+γϖ0+γ22ϖ′(0). |
Then, we find
ϖ′(0)=ϖ1(1−γ22ϖ1)[Iν+κ+10+[ω(γ,ϖ(γ))+∫γ0N(γ,τ,ϖ(τ))dτ]+Iκ+10+ψ(γ,ϖ(γ))−ψ(0,ϖ0)Γ(κ+2)γκ+1+γϖ0]. |
Therefore, we obtain
ϖ(z)=Iν+κ0+(ω(z,ϖ(z))+∫z0N(z,s,ϖ(s))ds)+Iκ0+ψ(z,ϖ(z))−ψ(0,ϖ0)Γ(κ+1)zκ+ϖ0+zϖ1(1−γ22ϖ1)[Iν+κ+10+[ω(γ,ϖ(γ))+∫γ0N(γ,τ,ϖ(τ))dτ]+Iκ+10+ψ(γ,ϖ(γ))−ψ(0,ϖ0)Γ(κ+2)γκ+1+γϖ0]. |
Finally, the integral equivalent Eq (2.1) is obtained. Conversely, using the integral Eq (2.4), which is equivalent to (2.1), we have
ϖ(z)=Iν+κ0+ω(z,ϖ(z))+∫zz0N(z,s,ϖ(s))ds+Iκ0+ψ(z,ϖ(z))−ψ(0,ϖ0)Γ(κ+1)zκ+ϖ0+ϖ′(0)z. |
Applying the inverse operator of the integral operator on both sides of (2.4) and using the properties of the Caputo derivative (linearity), then
CaDν+κ0+ϖ(z)=CaDν+κ0+{Iν+κ0+ω(z,ϖ(z))+∫zz0N(z,s,ϖ(s))ds+Iκ0+ψ(z,ϖ(z))−ψ(0,ϖ0)Γ(κ+1)zκ+ϖ0+ϖ′(0)z}=CaDν+κ0+Iν+κ0+ω(z,ϖ(z))+CaDν+κ0+∫zz0N(z,s,ϖ(s))ds+CaDν+κ0+Iκ0+ψ(z,ϖ(z))+CaDν+κ0+{−ψ(0,ϖ0)Γ(κ+1)zκ+ϖ0+ϖ′(0)z}. |
By the properties
CaDν+κ0+Iν+κ0+f(t)=f(t), |
and
CaDν+κ0+{−ψ(0,ϖ0)Γ(κ+1)zκ+ϖ0+ϖ′(0)z}=0, |
will lead to
CaDν+κ0+ϖ(z)=CaDν+κ0+Iν+κ0+ω(s,ϖ(s))+CaDν+κ0+Iκ+ν0+∫s0N(s,τ,ϖ(τ))dτ+CaDν+κ0+Iκ0+ψ(s,ϖ(s))+CaDν+κ0+(ϖ(0)+ϖ′(0)z)=ω(z,ϖ(z))+CaDν0+ψ(z,ϖ(z))+∫z0N(z,s,ϖ(s))ds, | (2.5) |
because
CaDν+κ0+(ϖ(0)+ϖ′(0)z)=I2−ν−κ[d2dx2(ϖ(0)+ϖ′(0)z)]=0, |
which means that ϖ verify (1.4).
For the other side of the proof, substituting z by 0 in (2.1) will make clear that the non-local condition in (1.4) matches. Thus, ϖ is a solution of (1.4). This concludes the proof.
We discuss the existence of a globally unique solution by using three fixed-point theorems in different directions. System (1.4) is transformed into a related fixed-point system as
ϖ=Fϖ, |
here the operator
F:C(J,E)⟶C(J,E), |
is given by:
Fϖ(z)=∫z0(z−s)ν+κ−1Γ(ν+κ)(ω(s,ϖ(s))+∫s0N(s,τ,ϖ(τ))dτ)ds+∫z0(z−s)κ−1Γ(κ)ψ(s,ϖ(s))ds+ϖ0−ψ(0,ϖ0)Γ(κ+1)zκ+ϖ1z(1−γ22ϖ1)[γϖ0−ψ(0,ϖ0)Γ(κ+2)γκ+1]+ϖ1z(1−γ22ϖ1)[∫γ0(γ−τ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))+∫τ0N(τ,σ,ϖ(σ))dσ)dτ+∫γ0(γ−τ)κΓ(κ+1)ψ(τ,ϖ(τ))dτ]. |
Noting by
Λ=‖μ1‖L∞+‖μ3‖L∞2+κ+ν(1+κ+ν2+κ+ν+|ϖ1|γν+κ+1|1−γ22ϖ1|)+‖μ2‖L∞2+κ(2+κκ+1+|ϖ1|γκ+1|1−γ22ϖ1|), | (3.1) |
Λ1=|ϖ1|L|1−γ22ϖ1|[2γν+κ+12+ν+κ+γκ+12+κ]. | (3.2) |
δ=2Γ(ν+κ+1)+1Γ(κ+1)+|ϖ1||1−γ22ϖ1|(2γν+κ+1Γ(ν+κ+2)+γκ+1Γ(κ+2)), | (3.3) |
δ1=|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|), | (3.4) |
δ2=1ν+κ+1+2ν+κ+2+1κ+1+|ϖ1||1−γ22ϖ1|(γν+κ+1ν+κ+2+γκ+1κ+2+2γν+κ+2ν+κ+3), | (3.5) |
where μ1, μ2, and μ3 will be defined in (H2).
Theorem 3.1. Assume ω,ψ∈C(J×R,R) and N∈C(J×J×R,R) are continuous functions. Assume that
(H0) There exist functions f1,f2∈C(J,R+), f3∈C(J×J,R+), with f=max{f1,f2,f3} and nondecreasing functions
g1,g2,g3:R+→R+, |
with g=max{g1,g2,g3} such that
|ω(z,ϖ(z))|≤f1(z)g1(‖ϖ‖), |
|ψ(z,ϖ(z))|≤f2(z)g2(‖ϖ‖), |
and
|N(z,s,ϖ(s))|≤f3(s)g3(‖ϖ‖), |
for all z∈[0,1],s∈[0,1],ϖ∈R. Also, assume that there exists a constant M>0 such that
M‖f‖g(M)δ2+δ1>1. |
Then problem (1.4) has at least one solution in J.
Proof. For r>0, let
Br={z∈C([0,1],R):‖ϖ‖≤r}, |
where r>0, be a bounded set in C([0,1],R). We shall prove that F maps bounded sets into bounded sets in C([0,1],R). By using the assumption (H1) and some computations (The beta function and its properties together with the gamma function)
(κ,ν)=∫10τκ−1(1−τ)ν−1dτ, |
∫10(1−s)κ+νsκds=ν(κ+1,κ+ν). |
The well-known Beta function and Gamma function are related as
(z,w)=Γ(z)Γ(w)Γ(z+w), |
and
∫γ0(γ−τ)κ+ντκdτ=γ2κ+ν+1ν(κ+1,κ+ν+1), |
we obtain
‖Fϖ(z)‖≤∫z0(z−s)ν+κ−1Γ(ν+κ)(f1(s)g1(‖ϖ(s)‖)+∫s0f3(s)g3(‖ϖ(τ)‖)dτ)ds+∫z0(z−s)κ−1Γ(κ)f2(s)g2(‖ϖ(s)‖)ds+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]+|ϖ1||1−γ22ϖ1|[∫γ0(γ−τ)κ+1Γ(κ+2)f2(τ)g2(‖ϖ(τ)‖)dτ+∫γ0(γ−τ)ν+κ+1Γ(ν+κ+2)(f1(τ)g1(‖ϖ(τ)‖)+∫τ0f3(τ)g3(‖ϖ(σ)‖)dσ)dτ]≤‖f‖g(‖ϖ‖)[∫z0(z−s)ν+κ−1Γ(ν+κ)(1+s)ds+∫z0(z−s)κ−1Γ(κ)ds+|ϖ1||1−γ22ϖ1|(∫γ0(γ−τ)κ+1Γ(κ+2)dτ+∫γ0(γ−τ)ν+κ+1Γ(ν+κ+2)(1+τ))dτ]+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]≤‖f‖g(‖ϖ‖)[1ν+κ+1+2ν+κ+2+1κ+1+|ϖ1||1−γ22ϖ1|(γν+κ+1ν+κ+2+γκ+1κ+2+2γν+κ+2ν+κ+3)]+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|)=‖f‖g(‖ϖ‖)δ2+δ1<+∞. | (3.6) |
Let z1,z2∈[0,1], with z1<z2, and ϖ∈Br, in which Br is a bounded set of C([0,1],R). Then
‖(Fϖ)(z2)−(Fϖ)(z1)‖≤∫z2z1(z2−s)ν+κ−1Γ(ν+κ)(‖ω(s,ϖ(s))‖+∫s0‖N(s,τ,ϖ(τ))‖dτ)ds+∫z2z1(z2−s)κ−1Γ(κ)‖ψ(s,ϖ(s))‖ds+∫z10(z1−s)ν+κ−1−(z2−s)ν+κ−1Γ(ν+κ)(‖ψ(s,ϖ(s))‖+∫s0‖N(s,τ,ϖ(τ))‖dτ)ds+∫z10(z1−s)κ−1−(z2−s)κ−1Γ(κ)‖ψ(s,ϖ(s))‖ds+|ψ(0,ϖ0)|Γ(κ+1)(zκ2−zκ1)+|ϖ1|(z2−z1)|1−γ22ϖ1|[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|+∫γ0(γ−τ)κΓ(κ+1)ψ(τ,ϖ(τ))dτ+∫γ0(γ−τ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))+∫τ0N(τ,σ,ϖ(σ))dσ)dτ].≤‖f‖g(‖ϖ‖)[2(z2−z1)ν+κ+|zν+κ1−zν+κ2|Γ(ν+κ+1)+2(z2−z1)κ+|zκ1−zκ2|Γ(κ+1)+(z2−z1)|ϖ1||1−γ22ϖ1|[γν+κ+1ν+κ+2+γκ+1κ+2+2γν+κ+2ν+κ+3]]+(zκ2−zκ1)|ψ(0,ϖ0)|Γ(κ+1)+(z2−z1)|ϖ1||1−γ22ϖ1|)[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]. |
If (z2−z1)⟶0, then the RHS of (3.7) tends to zero independently of ϖ∈Br. Therefore,
‖Fϖ(z2)−Fϖ(z1)‖⟶0, |
so F maps bounded sets into equi-continuous sets of C.
Owing to the Arzela-Ascoli theorem, we find
F:C([0,1],R)⟶C([0,1],R), |
is completely continuous.
Applying the Leray-Schauder nonlinear alternative when we show the boundedness of the set of all solutions to
ϖ=ϵFϖfor0<ϵ<1. |
Let ϖ be a solution of (1.4). Thus, by (3.6) we obtain
|ϖ(z)|≤‖f‖g(‖ϖ‖)δ2+δ1, |
which implies
‖ϖ‖‖f‖g(‖ϖ‖)δ2+δ1≤1. |
Then by (H2), ∃M>0 where M≠‖ϖ‖. Define the set
Y={ϖ∈C([0,1],R)/ ‖ϖ‖<M}, |
so
F:ˉY⟶C([0,1],R), |
is completely continuous. By the choice of Y, there is no z∈∂Y where
ϖ=ϵFϖfor ϵ∈(0,1), |
then owing to the nonlinear Leray-Schauder type, we find that F has a fixed point ϖ∈ˉY which is exactly the solution of the IVP (1.4).
Example 3.1. Let the next fractional integro-differential system
CaD1270+ϖ(z)=sinz22+ez(|u(z)|1+‖ϖ‖+cos(ϖ(z)))+CaD870+(cosz18+e−zz2+18e−z)ϖ(z)+∫z0es−z−115(ϖ(s)+2e−|ϖ(s)|)ds,ϖ(0)=1,ϖ′(0)=623∫0ϖ(s)ds, | (3.7) |
where
ν=47,κ=87,ϖ0=1,ϖ1=6,γ=23. |
Clearly
δ1=2.7868,δ2=4.6248, |
|ψ(z,ϖ(z))|≤(|cosz|18+e−zz2+18e−z)‖ϖ‖≤(118+e−zz2+18e−z)‖ϖ‖, |
|ω(z,ϖ(z))|≤|sinz|22+ez(‖ϖ‖1+‖ϖ‖+|cosϖ|)≤122+ez(1+‖ϖ‖), |
|N(z,s,ϖ(x))|≤es−z−115(‖ϖ‖+2e−‖ϖ‖)≤es−z−115(‖ϖ‖+2), |
with
f1(z)=118+e−zz2+18e−z,‖f1‖=19, |
f2(z)=122+ez,‖f2‖=123, |
f3(z,s)=es−z−115,‖f3‖=115, |
g1(‖ϖ‖)=‖ϖ‖,g2(‖ϖ‖)=‖ϖ‖+2,g3(‖ϖ‖)=2+‖ϖ‖. |
f=max{19,123,115}=19, |
g=max{‖ϖ‖, ‖ϖ‖+1, ‖ϖ‖+2}=‖ϖ‖+2. |
Since all the conditions of Theorem3.1 are satisfied, the problem (3.8) has at least one solution on [0,1].
Theorem 3.2. Let
ω,ψ:[0,1]×E⟶E, |
and
N:[0,1]×[0,1]×E⟶E, |
be continuous functions satisfying
(H1)
‖ω(z,ϖ(z))−ω(z,v∗(z))‖≤L1‖ϖ(z)−v∗(z)‖,z∈[0,1],ϖ,v∗∈X, |
‖ψ(z,ϖ(z))−ψ(z,v∗(z))‖≤L2‖ϖ(z)−v∗(z)‖,z∈[0,1],ϖ,v∗∈E, |
‖N(z,s,ϖ(s))−N(z,s,v∗(s))‖≤L3‖ϖ(s)−v∗(s)‖,(z,s)∈G,ϖ,v∗∈X, |
hold where L1,L2,L3≥0 with
L=max{L1,L2,L3}, |
and
G={(z,s):0≤s≤x≤1}. |
(H2) ∃μ∗1,μ2,μ3∈L∞([0,1],R+) such that
‖ω(z,ϖ(z))‖≤μ∗1(z)‖ϖ(z)‖,0≤z≤1,ϖ∈E, |
‖ψ(z,ϖ(z))‖≤μ2(z)‖ϖ(z)‖,0≤z≤1,ϖ∈E, |
‖N(z,s,ϖ(s))‖≤μ3(z)‖ϖ(s)‖,(z,s)∈G,ϖ∈E. |
If Λ≤1 and LΛ1≤1, then problem (1.4) has at least one solution on [0,1].
Proof. Let ϖ∈C(J,E), we define
‖ϖ‖1=max{e−x‖ϖ(z)‖:z∈[0,1]}, |
and consider the closed ball
Br={ϖ∈C(J,E):‖ϖ‖1≤r}. |
Then, the operators F1,F2 are defined on Br as
F1ϖ(z)=∫z0(z−s)ν+κ−1Γ(ν+κ)(ω(s,ϖ(s))+∫s0N(s,τ,ϖ(τ))dτ)ds+∫z0(z−s)κ−1Γ(κ)ψ(s,ϖ(s))ds+ϖ0−ψ(0,ϖ0)Γ(κ+1)zκ+ϖ1x(1−γ22ϖ1)[γϖ0−ψ(0,ϖ0)Γ(κ+2)γκ+1], | (3.8) |
and
F2ϖ(z)=ϖ1x(1−γ22ϖ1)[∫γ0(γ−τ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))+∫τ0N(τ,σ,ϖ(σ))dσ)dτ+∫γ0(γ−τ)κΓ(κ+1)ψ(τ,ϖ(τ))dτ]. | (3.9) |
For ϖ,v∗∈Br, z∈[0,1], by fixed r≥δ11−Λ and by the assumption (H2), we find:
ez‖F1ϖ(z)+F2v∗(z)‖1≤∫z0(z−s)ν+κ−1Γ(ν+κ)(μ1(s)‖ϖ(s)‖+∫s0μ3(s)‖ϖ(τ)‖dτ)ds+∫z0(z−s)κ−1Γ(κ)μ2(s)‖ϖ(s)‖ds+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]+|ϖ1||1−γ22ϖ1|[∫γ0(γ−τ)κΓ(κ+1)μ2(τ)‖v∗(τ)‖dτ+∫γ0(γ−τ)ν+κΓ(ν+κ+1)(μ1(τ)‖v∗(τ)‖+∫τ0μ3(τ)‖v∗(σ)‖dσ)dτ]≤∫z0(z−s)ν+κ−1Γ(ν+κ)(‖μ1‖L∞‖ϖ‖1es+‖μ3‖L∞‖ϖ‖1(es−1))ds+‖μ2‖L∞‖ϖ‖1∫z0(z−s)κ−1Γ(κ)esds+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]+|ϖ1||1−γ22ϖ1|[∫γ0(γ−τ)κΓ(κ+1)‖μ2‖L∞‖v∗‖2eτdτ+∫γ0(γ−τ)ν+κΓ(ν+κ+1)(‖μ1‖L∞‖v∗‖1eτ+‖μ3‖L∞‖v∗‖3(eτ−1))dτ]. |
Therefore
‖F1ϖ+F2v∗‖1≤zν+κν+κ+1(‖μ1‖L∞‖ϖ‖1+‖μ3‖L∞‖ϖ‖1)+zκκ+1‖μ2‖L∞‖ϖ‖1+e−z[|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|)]+|ϖ1||1−γ22ϖ1|[γκ+1κ+2‖μ2‖L∞‖v∗‖1+γν+κ+1ν+κ+2(‖μ1‖L∞‖v∗‖1+‖μ3‖L∞‖v∗‖3)]≤r[‖μ1‖L∞+‖μ3‖L∞2+κ+ν(1+κ+ν2+κ+ν+|ϖ1|γν+κ+1|1−γ22ϖ1|)+‖μ2‖L∞2+κ(2+κκ+1+|ϖ1|γκ+1|1−γ22ϖ1|)]+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|)=rΛ+δ1≤r. |
This implies that (F1u+F2v)∈Br. We use the estimations:
esez≤1,eτez≤1,eτ−1ez≤1,es−1ez≤1. |
Now, we have to show that F2 is a contraction mapping. For ϖ,v∗∈E and 0≤z≤1, we have
ex‖F2ϖ(z)−F2v∗(z)‖1≤|ϖ1||1−γ22ϖ1|[∫γ0(γ−τ)ν+κΓ(ν+κ+1)(‖ω(τ,ϖ(τ))−ω(τ,v∗(τ))‖+∫τ0‖N(τ,σ,ϖ(σ))−N(τ,σ,v∗(σ))‖dσ)dτ+∫γ0(γ−τ)κΓ(κ+1)‖ψ(τ,ϖ(τ))−ψ(τ,v∗(τ))‖dτ]≤|ϖ1|L|1−γ22ϖ1|[∫γ0(γ−τ)ν+κΓ(ν+κ+1)(‖ϖ−v∗‖1eτ+‖ϖ−v∗‖1(eτ−1))+∫γ0(γ−τ)κΓ(κ+1)‖ϖ−v∗‖1eτdτ]. |
Thus
‖F2ϖ−F2v∗‖1≤|ϖ1|L|1−γ22ϖ1|[2γν+κ+12+ν+κ+γκ+12+κ]‖ϖ−v∗‖1.=LΛ1‖ϖ−v∗‖1. |
As long as LΛ1≤1, then F2 is a contraction. Since the functions h,f, and K are continuous, we have the operator F1 is continuous. Also, F1Br⊂Br, for ϖ∈Br, i.e., F1 is uniformly bounded on Br as
ex‖F1ϖ(z)‖1≤∫z0(z−s)ν+κ−1Γ(ν+κ)(‖μ1‖L∞‖ϖ‖1es+‖μ3‖L∞‖ϖ‖1(es−1))ds+‖μ2‖L∞‖ϖ‖1∫z0(z−s)κΓ(κ)esds+|ψ(0,ϖ0)|Γ(κ+1)zκ+|ϖ0|+|ϖ1|x(1−γ22|ϖ1|)[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]. |
Therefore
‖F1ϖ‖1≤r[‖μ1‖L∞+‖μ3‖L∞ν+κ+1+‖μ2‖L∞1+κ]+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|)=rΛ+δ1≤r. |
We will now show that ¯(F1Br) is equicontinuous. So, let us define
¯ω=sup(s,ϖ)∈[0,1]×Br‖ω(s,u)‖,¯ψ=sup(s,ϖ)∈[0,1]×Br‖ψ(s,ϖ)‖,¯N=sup(s,τ,ϖ)∈G×Br∫s0‖N(z,s,ϖ)‖dz. | (3.10) |
For any ϖ∈Br and for each z1,z2∈[0,1] with z1≤z2, we have
‖(F1ϖ)(z2)−(F1ϖ)(z1)‖≤¯ω+¯NΓ(ν+κ+1)[2|z2−z1|ν+κ+|zν+κ1−zν+κ2|]+¯ψΓ(κ+1)[2|z2−z1|κ+|zκ1−zν2|]+(zκ2−zκ1)|ψ(0,ϖ0)|Γ(κ+1)+(z2−z1)|ϖ1||1−γ22ϖ1|)[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]. | (3.11) |
The right hand side of (3.11) is independent of ϖ and tends to 0 when |z2−z1|⟶0, which means that
|F1ϖ(z2)−F1ϖ(z1)|⟶0, |
this implies that ¯F1Br is equicontinuous, then F1 is relatively compact on Br. So, owing to the Arzela-Ascoli theorem, F1 is compact on Br, and then, all conditions of Theorem 3.2 are fulfilled. Then, the operator F1+F2 has a fixed point on Br. Therefore, problem (1.4) has at least one solution on [0,1].
Example 3.2. Consider the following fractional integro-differential problem.
{CaD950+ϖ(z)=ϖ(z)(7−z2)245+CaD850+ϖ(z)−2−ln(z+1)86ϖ(z)+∫z02+e−(s2+z2)93ϖ(s)dsϖ(0)=1,ϖ′(0)=623∫0ϖ(s)ds, | (3.12) |
Where
ν=15,κ=85,ϖ0=1,ϖ1=6,γ=23. |
For ϖ,v∗∈E=R+ and z∈[0,1], we obtain
L1=8245,L2=2+ln(2)86,L3=131,ψ(0,ϖ0)=ψ(0,1)=135, |
μ1(z)=7−z2245,μ2(z)=2−ln(z+1)86,μ3(z)=2+e−(s2+z2)93, |
yields
‖μ1‖L∞=135,‖μ2‖L∞=143,‖μ3‖L∞=131, |
and
L=131. |
Using the above data, we obtain
Λ=0.2285,Λ1=7.6401,LΛ1=0.2465<1,δ1=13.1677. |
fixing r≥δ11−Λ=17.0673 then, problem (3.12) has at least one solution on [0,1] by Theorem3.2
Theorem 3.3. Let (H1) hold. If LΛ<1, then (1.4) has a unique solution in [0,1].
Proof. Let
M=max{M1,M2,M3}, | (3.13) |
where M1,M2,M3>0 and
M1=supz∈[0,1]‖ω(z,0)‖, | (3.14) |
M2=supz∈[0,1]‖ψ(z,0)‖, | (3.15) |
M3=sup(z,s)∈G‖∫z0N(z,s,0)ds‖. | (3.16) |
For
r1≥Mδ+δ11−Lδ, |
fixed, let
Dr1={z∈C([0,1],E):‖ϖ‖≤r1}. |
By (H1), we have
‖ω(z,ϖ(z))‖=‖ω(z,ϖ(z))−ω(z,0)+ω(z,0)‖≤L1‖ϖ‖+M1, |
and
‖ψ(z,ϖ(z))‖≤L2‖ϖ‖+M2, | (3.17) |
and
‖∫z0N(z,s,ϖ(s))‖≤L3‖ϖ‖+M3. |
First step: We shall prove that TDr⊂Dr. Let t∈[0,1] and ϖ∈Dr, we have
‖(Fϖ)(z)‖≤∫z0(z−s)ν+κ−1Γ(ν+κ)(‖ω(s,ϖ(s))‖+∫s0‖N(s,τ,ϖ(τ))‖dτ)ds+∫z0(z−s)κ−1Γ(κ)‖ψ(s,ϖ(s))‖ds+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|[∫γ0(γ−τ)ν+κΓ(ν+κ+1)(‖ω(τ,ϖ(τ))‖+∫τ0‖N(τ,λ,ϖ(λ))‖dλ)dτ+∫γ0(γ−τ)κΓ(κ+1)‖ψ(τ,ϖ(τ))‖dτ+|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]≤(Lr+M)[1ν+κ+1+2ν+κ+2+1κ+1+|ϖ1||1−γ22ϖ1|(γν+κ+1ν+κ+2+γκ+1κ+2+2γν+κ+2ν+κ+3)]+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1−γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|)=(Lr1+M)δ2+δ1≤r1. |
Hence, FDr1⊂Dr1.
Second step: We prove now that F:Dr1⟶Dr is a contraction. By (H1), let z∈[0,1] and ∀ϖ,v∗∈Dr1, we have
‖(Fϖ)(z)−(Fv∗)(z)‖≤∫z0(z−s)ν+κ−1Γ(ν+κ)[‖ω(s,ϖ(s))−ω(s,v∗(s))‖+∫s0‖N(s,τ,ϖ(τ))−N(s,τ,v∗(τ))‖dτ]ds+∫z0(z−s)κ−1Γ(κ)‖ψ(s,ϖ(s))−ψ(s,v∗(s))‖ds+|ϖ1||1−γ22ϖ1|[∫γ0(γ−τ)ν+κΓ(ν+κ+1)(‖ω(τ,ϖ(τ))−ω(τ,v∗(τ))‖+∫τ0‖N(τ,σ,ϖ(σ))−N(τ,σ,v∗(σ))‖dσ)dτ+∫γ0(γ−τ)κΓ(κ+1)‖ψ(τ,ϖ(τ))−ψ(τ,v∗(τ))‖dτ]dτ≤L[1ν+κ+1+2ν+κ+2+1κ+1+|ϖ1||1−γ22ϖ1|(γν+κ+1ν+κ+2+γκ+1κ+2+2γν+κ+2ν+κ+3)]‖ϖ−v∗‖=Lδ2‖ϖ−v∗‖. |
Since Lδ2<1, we have F is a contraction. All conditions of Banach's fixed point theorem are satisfied, then ∃ϖ∈C(J,E) such that Fϖ=ϖ, which is considered as a unique solution of (1.4) in C(J,E).
Example 3.3. Consider the following fractional integro-differential problem:
{CaD1270+ϖ(z)=ω(z,ϖ(z))+CaD670+ψ(z,ϖ(z))+∫z0N(z,s,ϖ(s))ds,ϖ(0)=1,ϖ′(0)=623∫0ϖ(s)ds,0<γ<1, | (3.18) |
where
ν=κ=67,ϖ0=1,ϖ1=6,γ=23. |
Taking ϖ,v∗∈E=R+ and z∈[0,1], and
ω(z,ϖ(z))=ϖ(z)−(1−x2)13+1439|ϖ|, | (3.19) |
M1=113, L1=439,ψ(z,ϖ(z))=|ϖ|+5(z+1)17+134ϖ(z), | (3.20) |
M2=517,L2=334, | (3.21) |
N(z,s,ϖ(s))=4e−(s+z)19+257|ϖ|,M3=419,L3=257. | (3.22) |
Thus,
ψ(0,ϖ0)=ψ(0,1)=4217, andL=max{L1,L2,L3}=434. |
δ2=13.1677,Lδ2=0.4743<1,δ1=9.0338. |
Then, there exists a unique solution for the problem (3.18) on [0,1] by application of Theorem 3.3
Example 3.4. Consider the following fractional integro-differential problem:
{CaD1780+ϖ(z)=ω(z,ϖ(z))+CaD580+ψ(z,ϖ(z))+∫z0N(z,s,ϖ(s))ds,ϖ(0)=16,ϖ′(0)=7.645∫0ϖ(s)ds,0<γ<1, | (3.23) |
where
ν=128, κ=58,ϖ0=16,ϖ1=77.6,γ=45. |
To illustrate our result in Theorem 3.3, let ϖ,v∗∈E=R+, 0≤z≤1, and
ω(z,ϖ(z))=3ϖ(z)+(|cos(zπ)|+x2)22+1466|ϖ|,M1=111,L1=1033,ψ(z,ϖ(z))=5|ϖ|+(4z−1)23−z+246ϖ(z),M2=323,L2=623,N(z,s,ϖ(s))=7(s+z)+e−14(s+z)37+974|ϖ|,M3=1423,L3=974. |
Thus,
ψ(0,ϖ0)=ψ(0,1)=1046, andL=max{L1,L2,L3}=1033. |
δ2=2.3621,Lδ2=0.757<1,δ1=60.5888. |
then, there exists a unique solution for the problem (3.23) on [0,1] by application of Theorem 3.3.
We show the Ulam stability of (1.4), using integration v∗(z)=Fv∗(z).
Let us define the non-linear continuous operator
Q:C([0,1],E)⟶C([0,1],E), |
as follows
Qv∗(z)=CaDν+κv∗(z)−CaDν0+ω(z,v∗(z))−ψ(z,v∗(z))−∫z0N(z,s,v∗(s))ds. |
Definition 4.1. Let ϵ>0 and v be a solution of (1.4), where
‖Qv∗‖≤ϵ, | (4.1) |
We say that problem (1.4) is Ulam-Hyers stable if there exists β>0 and solution ϖ∈C([0,1],E) of (1.4) satisfying
‖ϖ−v∗‖≤βϵ∗, | (4.2) |
here ϵ∗>0 depending on ϵ.
Definition 4.2. Let g∈C(R+,R+) and solution v of (1.4), there exists a solution ϖ∈C([0,1],E) of (1.4) where
‖ϖ(z)−v∗(z)‖≤g(ϵ),0≤x≤1. | (4.3) |
Then (1.4) is said to be stable in the generalized Ulam-Hyers sense.
Definition 4.3. Let ϵ>0 and θ∈C([0,1],R+). Let v be a solution of (1.4); we say that the system (1.4) is stable in the Ulam-Hyers-Rassias sense with respect to θ if
‖Qv∗(z)‖≤ϵθ(z),0≤x≤1, | (4.4) |
and ∃β>0 and a solution v∈C([0,1],E) of (1.4) where
‖ϖ(z)−v∗(z)‖≤βϵ∗θ(z),0≤x≤1, | (4.5) |
here ϵ∗>0 depending on ϵ.
Theorem 4.1. Let (H1) in Theorem 3.1 hold with Lδ<1. The (1.4) is both Ulam-Hyers and generalized Ulam-Hyers stable.
Proof. Let ϖ∈C([0,1],E) be a solution of (1.4), satisfying (2.1) in the sense of Theorem 3.3, and any solution v∗ satisfying (4.1). Then, we obtain:
‖v∗(z)−ϖ(z)‖=‖v∗(z)−Fv∗(z)+Fv∗(z)−ϖ(z)‖=‖v∗(z)−Fv∗(z)+Fv∗(z)−Fϖ(z)‖≤‖Fv∗(z)−Fϖ(z)‖+‖Fv∗(z)−Id(v∗(z))‖≤‖Fv∗(z)−Fϖ(z)‖+‖Qv∗‖≤Lδ‖ϖ−v∗‖+ϵ, | (4.6) |
because Lδ<1 and ϵ>0, we obtain
‖ϖ−v∗‖≤ϵ1−Lδ. |
Let ϵ∗=ϵ1−Lδ be fixed and β=1, we obtain the Ulam-Hyers stability requirements. Besides, the generalized Ulam-Hyers stability is followed by taking
g(ϵ)=ϵ1−Lδ. |
Theorem 4.2. Let (H1) holds with L<δ−1, and ∃θ∈C([0,1],R+) satisfy (4.4). Then (1.4) is Ulam-Hyers-Rassias stable with respect to θ.
Proof. As in the proof of Theorem 4.1, we have
‖ϖ(z)−v∗(z‖≤ϵ∗θ(z),0≤z≤1, |
where ϵ∗=ϵ1−Lδ.
This article delves into the study of a fractional-order non-linear integro-differential equation, featuring a composition of fractional derivatives with distinct origins and mixed conditions. This equation serves as a model for the motion of a system within a fractal medium. The paper utilizes three fixed-point theorems to establish the existence and uniqueness of a solution. Subsequently, it presents the Ulam stability criterion for the obtained solution. Finally, a proposed example is provided to illustrate the main results. Complete studies are made in which our contributions extend the work in [22]. The problem of the fractional Caputo derivative (in the RHS and LHS of the differential equation) with mixed conditions is considered in (1.4) to improve the model (1.3), where only the integral boundary condition was taken, and the problem was with the Riemann-Liouville fractional integral in the RHS of the differential equation. This problem can be studied by a generalized Caputo derivative with changing conditions, especially when the derivative comes in the psi Caputo derivative; then study it with different origins and suitable mixed conditions.
All authors contributed equally to this work. All authors have read and approved the final version of the manuscript for publication.
The authors declare that they have not used Artificial Intelligence (AI) tools in the creation of this article.
The Researchers would like to thank the Deanship of Graduate Studies and Scientific Research at Qassim University for financial support (QU-APC-2025).
The authors declare that they have no conflict of interest.
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