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Existence and stability analysis of a problem of the Caputo fractional derivative with mixed conditions

  • 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)=σγ0ϖ(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), 0z1,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)=bη0ϖ(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)=ϖ1γ0ϖ(s)ds,0<γ<1, (1.4)

    where ϖ0,ϖ1 are real constants, 1<ν+κ2, 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×EE,ψ:J×EE,N:J×J×EE, (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 :R+R. The Riemann-Liouville fractional integral of order κ of a function is given by

    Iκ0+(z)=1Γ(κ)z0(zs)κ1(s)(s)ds,zR+.

    Definition 2.2. [28] Let κ>0; the order κ Caputo fractional derivative of a function :R+R is defined by

    CaDκ0+(z)=1Γ(nκ)z0(zs)nκ1(n)(s)ds=Inκ0+(n)(z),zR+,

    where n=[κ]+1, and the right-hand side is point-wise defined on R+.

    Lemma 2.1. [25] For κ>0, iR, and the appropriate function (z)Cn1[0,), where (z) exists almost everywhere in any bounded interval of R+, we have

    (Iκ0+CaDκ0+)(z)=(z)n1i=0(i)(0)i!zi.

    Lemma 2.2. Let 1<ν+κ<2 and ϖ12γ2. Assume that ω,ψ and N are three continuous functions. If ϖC(J,E), then ϖ is a solution of (1.4) if and only if ϖ satisfies the integral equation

    ϖ(z)=z0(zs)ν+κ1Γ(ν+κ)(ω(s,ϖ(s))+s0N(s,τ,ϖ(τ))dτ)ds+z0(zs)κ1Γ(κ)ψ(s,ϖ(s))ds+ϖ0ψ(0,ϖ0)Γ(κ+1)zκ+zϖ1(1γ22ϖ1)[γ0(γτ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))+τ0N(τ,σ,ϖ(σ))dσ)dτ+γ0(γτ)κΓ(κ+1)ψ(τ,ϖ(τ))dτψ(0,ϖ0)Γ(κ+2)γκ+1+γϖ0]. (2.1)

    Proof. Assume that ϖC(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+ϖ0ψ(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))]dsψ(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(1γ22ϖ1)[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(1γ22ϖ1)[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)=I2νκ[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(zs)ν+κ1Γ(ν+κ)(ω(s,ϖ(s))+s0N(s,τ,ϖ(τ))dτ)ds+z0(zs)κ1Γ(κ)ψ(s,ϖ(s))ds+ϖ0ψ(0,ϖ0)Γ(κ+1)zκ+ϖ1z(1γ22ϖ1)[γϖ0ψ(0,ϖ0)Γ(κ+2)γκ+1]+ϖ1z(1γ22ϖ1)[γ0(γτ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))+τ0N(τ,σ,ϖ(σ))dσ)dτ+γ0(γτ)κΓ(κ+1)ψ(τ,ϖ(τ))dτ].

    Noting by

    Λ=μ1L+μ3L2+κ+ν(1+κ+ν2+κ+ν+|ϖ1|γν+κ+1|1γ22ϖ1|)+μ2L2+κ(2+κκ+1+|ϖ1|γκ+1|1γ22ϖ1|), (3.1)
    Λ1=|ϖ1|L|1γ22ϖ1|[2γν+κ+12+ν+κ+γκ+12+κ]. (3.2)
    δ=2Γ(ν+κ+1)+1Γ(κ+1)+|ϖ1||1γ22ϖ1|(2γν+κ+1Γ(ν+κ+2)+γκ+1Γ(κ+2)), (3.3)
    δ1=|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|), (3.4)
    δ2=1ν+κ+1+2ν+κ+2+1κ+1+|ϖ1||1γ22ϖ1|(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,ψC(J×R,R) and NC(J×J×R,R) are continuous functions. Assume that

    (H0) There exist functions f1,f2C(J,R+), f3C(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],ϖR. Also, assume that there exists a constant M>0 such that

    Mfg(M)δ2+δ1>1.

    Then problem (1.4) has at least one solution in J.

    Proof. For r>0, let

    Br={zC([0,1],R):ϖr},

    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)=10τκ1(1τ)ν1dτ,
    10(1s)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(γτ)κ+ντκdτ=γ2κ+ν+1ν(κ+1,κ+ν+1),

    we obtain

    Fϖ(z)z0(zs)ν+κ1Γ(ν+κ)(f1(s)g1(ϖ(s))+s0f3(s)g3(ϖ(τ))dτ)ds+z0(zs)κ1Γ(κ)f2(s)g2(ϖ(s))ds+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]+|ϖ1||1γ22ϖ1|[γ0(γτ)κ+1Γ(κ+2)f2(τ)g2(ϖ(τ))dτ+γ0(γτ)ν+κ+1Γ(ν+κ+2)(f1(τ)g1(ϖ(τ))+τ0f3(τ)g3(ϖ(σ))dσ)dτ]fg(ϖ)[z0(zs)ν+κ1Γ(ν+κ)(1+s)ds+z0(zs)κ1Γ(κ)ds+|ϖ1||1γ22ϖ1|(γ0(γτ)κ+1Γ(κ+2)dτ+γ0(γτ)ν+κ+1Γ(ν+κ+2)(1+τ))dτ]+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]fg(ϖ)[1ν+κ+1+2ν+κ+2+1κ+1+|ϖ1||1γ22ϖ1|(γν+κ+1ν+κ+2+γκ+1κ+2+2γν+κ+2ν+κ+3)]+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|)=fg(ϖ)δ2+δ1<+. (3.6)

    Let z1,z2[0,1], with z1<z2, and ϖBr, in which Br is a bounded set of C([0,1],R). Then

    (Fϖ)(z2)(Fϖ)(z1)z2z1(z2s)ν+κ1Γ(ν+κ)(ω(s,ϖ(s))+s0N(s,τ,ϖ(τ))dτ)ds+z2z1(z2s)κ1Γ(κ)ψ(s,ϖ(s))ds+z10(z1s)ν+κ1(z2s)ν+κ1Γ(ν+κ)(ψ(s,ϖ(s))+s0N(s,τ,ϖ(τ))dτ)ds+z10(z1s)κ1(z2s)κ1Γ(κ)ψ(s,ϖ(s))ds+|ψ(0,ϖ0)|Γ(κ+1)(zκ2zκ1)+|ϖ1|(z2z1)|1γ22ϖ1|[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|+γ0(γτ)κΓ(κ+1)ψ(τ,ϖ(τ))dτ+γ0(γτ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))+τ0N(τ,σ,ϖ(σ))dσ)dτ].fg(ϖ)[2(z2z1)ν+κ+|zν+κ1zν+κ2|Γ(ν+κ+1)+2(z2z1)κ+|zκ1zκ2|Γ(κ+1)+(z2z1)|ϖ1||1γ22ϖ1|[γν+κ+1ν+κ+2+γκ+1κ+2+2γν+κ+2ν+κ+3]]+(zκ2zκ1)|ψ(0,ϖ0)|Γ(κ+1)+(z2z1)|ϖ1||1γ22ϖ1|)[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|].

    If (z2z1)0, then the RHS of (3.7) tends to zero independently of ϖBr. 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)|fg(ϖ)δ2+δ1,

    which implies

    ϖfg(ϖ)δ2+δ11.

    Then by (H2), M>0 where Mϖ. Define the set

    Y={ϖC([0,1],R)/  ϖ<M},

    so

    F:ˉYC([0,1],R),

    is completely continuous. By the choice of Y, there is no zY where

    ϖ=ϵFϖfor  ϵ(0,1),

    then owing to the nonlinear Leray-Schauder type, we find that F has a fixed point ϖˉY 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+ezz2+18ez)ϖ(z)+z0esz115(ϖ(s)+2e|ϖ(s)|)ds,ϖ(0)=1,ϖ(0)=6230ϖ(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+ezz2+18ez)ϖ(118+ezz2+18ez)ϖ,
    |ω(z,ϖ(z))||sinz|22+ez(ϖ1+ϖ+|cosϖ|)122+ez(1+ϖ),
    |N(z,s,ϖ(x))|esz115(ϖ+2eϖ)esz115(ϖ+2),

    with

    f1(z)=118+ezz2+18ez,f1=19,
    f2(z)=122+ez,f2=123,
    f3(z,s)=esz115,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]×EE,

    and

    N:[0,1]×[0,1]×EE,

    be continuous functions satisfying

    (H1)

    ω(z,ϖ(z))ω(z,v(z))L1ϖ(z)v(z),z[0,1],ϖ,vX,
    ψ(z,ϖ(z))ψ(z,v(z))L2ϖ(z)v(z),z[0,1],ϖ,vE,
    N(z,s,ϖ(s))N(z,s,v(s))L3ϖ(s)v(s),(z,s)G,ϖ,vX,

    hold where L1,L2,L30 with

    L=max{L1,L2,L3},

    and

    G={(z,s):0sx1}.

    (H2) μ1,μ2,μ3L([0,1],R+) such that

    ω(z,ϖ(z))μ1(z)ϖ(z),0z1,ϖE,
    ψ(z,ϖ(z))μ2(z)ϖ(z),0z1,ϖE,
    N(z,s,ϖ(s))μ3(z)ϖ(s),(z,s)G,ϖE.

    If Λ1 and LΛ11, then problem (1.4) has at least one solution on [0,1].

    Proof. Let ϖC(J,E), we define

    ϖ1=max{exϖ(z):z[0,1]},

    and consider the closed ball

    Br={ϖC(J,E):ϖ1r}.

    Then, the operators F1,F2 are defined on Br as

    F1ϖ(z)=z0(zs)ν+κ1Γ(ν+κ)(ω(s,ϖ(s))+s0N(s,τ,ϖ(τ))dτ)ds+z0(zs)κ1Γ(κ)ψ(s,ϖ(s))ds+ϖ0ψ(0,ϖ0)Γ(κ+1)zκ+ϖ1x(1γ22ϖ1)[γϖ0ψ(0,ϖ0)Γ(κ+2)γκ+1], (3.8)

    and

    F2ϖ(z)=ϖ1x(1γ22ϖ1)[γ0(γτ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))+τ0N(τ,σ,ϖ(σ))dσ)dτ+γ0(γτ)κΓ(κ+1)ψ(τ,ϖ(τ))dτ]. (3.9)

    For ϖ,vBr, z[0,1], by fixed rδ11Λ and by the assumption (H2), we find:

    ezF1ϖ(z)+F2v(z)1z0(zs)ν+κ1Γ(ν+κ)(μ1(s)ϖ(s)+s0μ3(s)ϖ(τ)dτ)ds+z0(zs)κ1Γ(κ)μ2(s)ϖ(s)ds+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]+|ϖ1||1γ22ϖ1|[γ0(γτ)κΓ(κ+1)μ2(τ)v(τ)dτ+γ0(γτ)ν+κΓ(ν+κ+1)(μ1(τ)v(τ)+τ0μ3(τ)v(σ)dσ)dτ]z0(zs)ν+κ1Γ(ν+κ)(μ1Lϖ1es+μ3Lϖ1(es1))ds+μ2Lϖ1z0(zs)κ1Γ(κ)esds+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|]+|ϖ1||1γ22ϖ1|[γ0(γτ)κΓ(κ+1)μ2Lv2eτdτ+γ0(γτ)ν+κΓ(ν+κ+1)(μ1Lv1eτ+μ3Lv3(eτ1))dτ].

    Therefore

    F1ϖ+F2v1zν+κν+κ+1(μ1Lϖ1+μ3Lϖ1)+zκκ+1μ2Lϖ1+ez[|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|)]+|ϖ1||1γ22ϖ1|[γκ+1κ+2μ2Lv1+γν+κ+1ν+κ+2(μ1Lv1+μ3Lv3)]r[μ1L+μ3L2+κ+ν(1+κ+ν2+κ+ν+|ϖ1|γν+κ+1|1γ22ϖ1|)+μ2L2+κ(2+κκ+1+|ϖ1|γκ+1|1γ22ϖ1|)]+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|)=rΛ+δ1r.

    This implies that (F1u+F2v)Br. We use the estimations:

    esez1,eτez1,eτ1ez1,es1ez1.

    Now, we have to show that F2 is a contraction mapping. For ϖ,vE and 0z1, we have

    exF2ϖ(z)F2v(z)1|ϖ1||1γ22ϖ1|[γ0(γτ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))ω(τ,v(τ))+τ0N(τ,σ,ϖ(σ))N(τ,σ,v(σ))dσ)dτ+γ0(γτ)κΓ(κ+1)ψ(τ,ϖ(τ))ψ(τ,v(τ))dτ]|ϖ1|L|1γ22ϖ1|[γ0(γτ)ν+κΓ(ν+κ+1)(ϖv1eτ+ϖv1(eτ1))+γ0(γτ)κΓ(κ+1)ϖv1eτdτ].

    Thus

    F2ϖF2v1|ϖ1|L|1γ22ϖ1|[2γν+κ+12+ν+κ+γκ+12+κ]ϖv1.=LΛ1ϖv1.

    As long as LΛ11, then F2 is a contraction. Since the functions h,f, and K are continuous, we have the operator F1 is continuous. Also, F1BrBr, for ϖBr, i.e., F1 is uniformly bounded on Br as

    exF1ϖ(z)1z0(zs)ν+κ1Γ(ν+κ)(μ1Lϖ1es+μ3Lϖ1(es1))ds+μ2Lϖ1z0(zs)κΓ(κ)esds+|ψ(0,ϖ0)|Γ(κ+1)zκ+|ϖ0|+|ϖ1|x(1γ22|ϖ1|)[|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|].

    Therefore

    F1ϖ1r[μ1L+μ3Lν+κ+1+μ2L1+κ]+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|)=rΛ+δ1r.

    We will now show that ¯(F1Br) is equicontinuous. So, let us define

    ¯ω=sup(s,ϖ)[0,1]×Brω(s,u),¯ψ=sup(s,ϖ)[0,1]×Brψ(s,ϖ),¯N=sup(s,τ,ϖ)G×Brs0N(z,s,ϖ)dz. (3.10)

    For any ϖBr and for each z1,z2[0,1] with z1z2, we have

    (F1ϖ)(z2)(F1ϖ)(z1)¯ω+¯NΓ(ν+κ+1)[2|z2z1|ν+κ+|zν+κ1zν+κ2|]+¯ψΓ(κ+1)[2|z2z1|κ+|zκ1zν2|]+(zκ2zκ1)|ψ(0,ϖ0)|Γ(κ+1)+(z2z1)|ϖ1||1γ22ϖ1|)[|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 |z2z1|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)(7z2)245+CaD850+ϖ(z)2ln(z+1)86ϖ(z)+z02+e(s2+z2)93ϖ(s)dsϖ(0)=1,ϖ(0)=6230ϖ(s)ds, (3.12)

    Where

    ν=15,κ=85,ϖ0=1,ϖ1=6,γ=23.

    For ϖ,vE=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)=7z2245,μ2(z)=2ln(z+1)86,μ3(z)=2+e(s2+z2)93,

    yields

    μ1L=135,μ2L=143,μ3L=131,

    and

    L=131.

    Using the above data, we obtain

    Λ=0.2285,Λ1=7.6401,LΛ1=0.2465<1,δ1=13.1677.

    fixing rδ11Λ=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)Gz0N(z,s,0)ds. (3.16)

    For

    r1Mδ+δ11Lδ,

    fixed, let

    Dr1={zC([0,1],E):ϖr1}.

    By (H1), we have

    ω(z,ϖ(z))=ω(z,ϖ(z))ω(z,0)+ω(z,0)L1ϖ+M1,

    and

    ψ(z,ϖ(z))L2ϖ+M2, (3.17)

    and

    z0N(z,s,ϖ(s))L3ϖ+M3.

    First step: We shall prove that TDrDr. Let t[0,1] and ϖDr, we have

    (Fϖ)(z)z0(zs)ν+κ1Γ(ν+κ)(ω(s,ϖ(s))+s0N(s,τ,ϖ(τ))dτ)ds+z0(zs)κ1Γ(κ)ψ(s,ϖ(s))ds+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|[γ0(γτ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))+τ0N(τ,λ,ϖ(λ))dλ)dτ+γ0(γτ)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||1γ22ϖ1|(γν+κ+1ν+κ+2+γκ+1κ+2+2γν+κ+2ν+κ+3)]+|ψ(0,ϖ0)|Γ(κ+1)+|ϖ0|+|ϖ1||1γ22ϖ1|(|ψ(0,ϖ0)|Γ(κ+2)γκ+1+γ|ϖ0|)=(Lr1+M)δ2+δ1r1.

    Hence, FDr1Dr1.

    Second step: We prove now that F:Dr1Dr is a contraction. By (H1), let z[0,1] and ϖ,vDr1, we have

    (Fϖ)(z)(Fv)(z)z0(zs)ν+κ1Γ(ν+κ)[ω(s,ϖ(s))ω(s,v(s))+s0N(s,τ,ϖ(τ))N(s,τ,v(τ))dτ]ds+z0(zs)κ1Γ(κ)ψ(s,ϖ(s))ψ(s,v(s))ds+|ϖ1||1γ22ϖ1|[γ0(γτ)ν+κΓ(ν+κ+1)(ω(τ,ϖ(τ))ω(τ,v(τ))+τ0N(τ,σ,ϖ(σ))N(τ,σ,v(σ))dσ)dτ+γ0(γτ)κΓ(κ+1)ψ(τ,ϖ(τ))ψ(τ,v(τ))dτ]dτL[1ν+κ+1+2ν+κ+2+1κ+1+|ϖ1||1γ22ϖ1|(γν+κ+1ν+κ+2+γκ+1κ+2+2γν+κ+2ν+κ+3)]ϖv=Lδ2ϖv.

    Since Lδ2<1, we have F is a contraction. All conditions of Banach's fixed point theorem are satisfied, then ϖC(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)=6230ϖ(s)ds,0<γ<1, (3.18)

    where

    ν=κ=67,ϖ0=1,ϖ1=6,γ=23.

    Taking ϖ,vE=R+ and z[0,1], and

    ω(z,ϖ(z))=ϖ(z)(1x2)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)=7.6450ϖ(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,vE=R+, 0z1, and

    ω(z,ϖ(z))=3ϖ(z)+(|cos(zπ)|+x2)22+1466|ϖ|,M1=111,L1=1033,ψ(z,ϖ(z))=5|ϖ|+(4z1)23z+246ϖ(z),M2=323,L2=623,N(z,s,ϖ(s))=7(s+z)+e14(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

    Qvϵ, (4.1)

    We say that problem (1.4) is Ulam-Hyers stable if there exists β>0 and solution ϖC([0,1],E) of (1.4) satisfying

    ϖvβϵ, (4.2)

    here ϵ>0 depending on ϵ.

    Definition 4.2. Let gC(R+,R+) and solution v of (1.4), there exists a solution ϖC([0,1],E) of (1.4) where

    ϖ(z)v(z)g(ϵ),0x1. (4.3)

    Then (1.4) is said to be stable in the generalized Ulam-Hyers sense.

    Definition 4.3. Let ϵ>0 and θC([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),0x1, (4.4)

    and β>0 and a solution vC([0,1],E) of (1.4) where

    ϖ(z)v(z)βϵθ(z),0x1, (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 ϖC([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)+QvLδϖv+ϵ, (4.6)

    because Lδ<1 and ϵ>0, we obtain

    ϖvϵ1Lδ.

    Let ϵ=ϵ1Lδ be fixed and β=1, we obtain the Ulam-Hyers stability requirements. Besides, the generalized Ulam-Hyers stability is followed by taking

    g(ϵ)=ϵ1Lδ.

    Theorem 4.2. Let (H1) holds with L<δ1, and θC([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(zϵθ(z),0z1,

    where ϵ=ϵ1Lδ.

    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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