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Existence and Ulam stability for fractional differential equations of mixed Caputo-Riemann derivatives

  • In this paper, we study the existence, uniqueness, and stability theorems of solutions for a differential equation of mixed Caputo-Riemann fractional derivatives with integral initial conditions in a Banach space. Our analysis is based on an application of the Shauder fixed point theorem with Ulam-Hyers and Ulam-Hyers-Rassias theorems. A couple of examples are presented to illustrate the obtained results.

    Citation: Shayma A. Murad, Zanyar A. Ameen. Existence and Ulam stability for fractional differential equations of mixed Caputo-Riemann derivatives[J]. AIMS Mathematics, 2022, 7(4): 6404-6419. doi: 10.3934/math.2022357

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  • In this paper, we study the existence, uniqueness, and stability theorems of solutions for a differential equation of mixed Caputo-Riemann fractional derivatives with integral initial conditions in a Banach space. Our analysis is based on an application of the Shauder fixed point theorem with Ulam-Hyers and Ulam-Hyers-Rassias theorems. A couple of examples are presented to illustrate the obtained results.



    The fractional differential equations have drawn much attention due to their applications in a number of fields such as physics, mechanics, chemistry, biology, economics, biophysics, etc, see [16,32]. Some physical phenomena such as the fractional oscillator equations and fractional Euler-Lagrange equations with mixed fractional derivatives can be found in [10,12,31]. Once a model of fractional differential equation for the real problem have been constructed, people faced the issue of how to solve this model. In many circumstances, finding the exact solution to the fractional differential equation is quite challenging. As a result, researchers must identify as many aspects of the problem's solution as possible. Is there a solution to the problem, for example? Is the solution unique if there is a one? Hence the study of existence and uniqueness solutions for fractional differential equations with initial and boundary conditions appealed many scientists and mathematicians [2,3,4,19,20,21,25,27,30]. Some existence results for fractional differential equations with integral boundary conditions can be found in [17,28,29]. Recently, the existence theorem for fractional differential equations involving mixed fractional derivatives have been studied by many authors [5,6,8]. More specifically, Abbas [1] proved the existence and uniqueness of solution for a boundary value problem of fractional differential equation of the form

    CDαy(t)=f(t,y(t),CDβy(t)),β>0,y(0)=λ1y(η),y(0)=0,y(0)=0,...,y(m2)(0)=0,y(1)=λ2y(η),

    where α(m1,m],m2, and CDα,CDβ are the Caputo fractional derivatives. Alghamdi et al.[7] studied new existence and uniqueness results for three-point boundary value problem of sequential fractional differential equations given by

    (CDβ+1+KCDβ)y(t)=f(t,y(t)),1<β<2,k>0,y(ε)=0,y(η)=0,y(ζ)=0,<ε<η<ζ<,

    where CDβ is Caputo fractional derivative. Song et al. [34] used the coincidence degree theory while proving the existence of solutions of the following nonlinear mixed fractional differential equation with the integral boundary value problem:

    CDα1Dβ0+y(t)=f(t,y(t),Dβ+10+y(t),Dβ0+y(t)),α(1,2],β(0,1],0<t<1,y(0)=y(0)=0,y(1)=10y(s)dA(t),

    where CDα1 and Dβ0+ are respectively the left Caputo fractional derivative and the right Riemann–Liouville fractional derivative. Sousa et al. [35] investigated the existence and uniqueness of mild and strong solutions of fractional semilinear evolution equations, by means of the Banach fixed point theorem and the Gronwall inequality. The notion of Ulam stability has been studied and expanded in many ways. There have been a number of articles published on this subject that have yielded a number of conclusions [11,23,24]. Ibrahim [18] examined Ulam stability for the Cauchy differential equation of fractional order in the unit disk. Chen et al. [13] studied the Ulam-Hyers stability of solutions for linear and nonlinear nabla fractional Caputo difference equations when 0<v1 on finite intervals. The linear case has the form

    vx(t)=λx(t)+f(t),x(a)=y(a),

    and the non-linear case has the form

    vx(t)=λx(t)+f(t,y(t)),x(a)=y(a).

    Muniyappan and Rajan [26] discussed Hyers-Ulam and Hyers-Ulam-Rassias stability for the following fractional differential equation with boundary condition

    Dαy(t)=f(t,y(t)),0<α1,ay(0)+by(T)=c,

    where Dα is Caputo fractional derivative of order α. Dai et al. [14] researched the Ulam–Hyers and Ulam–Hyers–Rassias stability of nonlinear fractional differential equations with integral boundary condition which has the form

    y(t)+CDα0+y(t))=f(t,y(t)),0<α<1,t[0,1],y(1)=Iβ0+y(η)=1Γ(β)η0(ηs)β1y(s)ds,β>0,

    where Dα is Caputo derivative and Iβ0+(.) is the Riemann–Liouville fractional integral.

    In this paper, we consider the nonlinear fractional differential equations wich has the form

    RDβ(CDαy(t)+λCDα1y(t))=f(t,y(t)),J=[0,1],λ0, (1.1)

    with initial conditions

    y(0)=0,y(0)=10y(s)ds, and y(0)=1Γ(β)10(1s)β1y(s)ds, (1.2)

    where f:J×RR, 1<α2,0<β1, CDα is the Caputo fractional derivative, and RDβ is the Riemann fractional derivative. New existence and uniqueness results are obtained by driving the corresponding Green's function of problem (1.1) and (1.2) with the help of the Schauder theorem and Banach contraction principle. Furthermore, the Ulam–Hyers and Ulam–Hyers–Rassias stability for Eq (1.1) is briefly described. Finally, some examples are given to demonstrate the application of our main results.

    Let us give some definitions and lemmas that are basic and needed at various places in this work.

    Definition 2.1. [9] Let f be a function which is defined almost everywhere (a.e.) on [a,b], If α>0, then:

    baIαf=baf(s)(bs)α1Γ(α)ds,

    provided that this integral (Lebesgue) exists.

    Definition 2.2. [22] The Riemann-Liouville fractional derivative oforder α>0 for a function function f:[0,)R, is defined as

    RLDαf(t)=1Γ(nα)dndtnt0(ts)nα1f(s)ds,n1<αn,

    where n=[α]+1,[α] denotes the integer part of the real number α.

    Definition 2.3. [32] For a continuous function f:[0,)R, the Caputo derivative of fractional order α is defined as

    CDαf(t)=1Γ(nα)t0(ts)nα1f(n)(s)ds,n1<αn,

    provided that f(n) exists, where n=[α]+1,[α] denotes the integer part of the real number α.

    Lemma 2.4. [32] Let f(t)L1[a,b] and α,β0. Then

    IαIβf(t)=Iα+βf(t)=IβIαf(t)(a.e)on[a,b].

    Moreover, if f(t)C[a,b], then the above identity is true for all t[a,b].

    Lemma 2.5. [9] Let α>0, n be the smallest integer n>α and let f(t)L(a,b). If taDα1f exists and is absolutely continuous on [a,b], then a+aDαif=ki exists for i=1,2,...,n; taDαf exists a.e. on [a,b], is in L(a,b) and

    taIαsaDαf(s)=f(t)ni=1ki(ta)αiΓ(αi+1)a.e.onatb.

    Furthermore, the inequality holds everywhere on (a,b], if in addition, f(t) is continuous on (a,b].

    Lemma 2.6. [22] Let α>0. If we assume yC(0,1)L1(0,1), then the Caputo fractional differential equation

    Dαy(t)=0

    has the solution

    y(t)=c0+c1t+c2t2+...+cn1tn1,

    where ciR,i=0,1,2,...,n1, and n=[α]+1.

    Lemma 2.7. [22] Let yC(0,1)L1(0,1) with fractional derivative of order α>0 that belongs to C(0,1)L1(0,1). Then

    IαCDαy(t)=y(t)+c0+c1t+c2t2+...+cn1tn1,

    for ciR,i=0,1,2,...,n1, where n is the smallest integer greater than or equal to α.

    Lemma 2.8. [9,32] Let α, βR, β>1. If t>a, then

    taIα(sa)βΓ(β+1)={(ta)α+βΓ(α+β+1),α+βnegative integer,0,α+β=negative integer.

    Definition 2.9. [32] The two-parametric Mittag-Leffler function is defined as

    Eα,β(t)=k=0tkΓ(kα+β),α,β,tC,Re(α)>0,Re(β)>0.

    Theorem 2.10. [15] (Arzela-Ascoli Theorem). If X is compact and fC(X), then f totally is bounded if and only if f is bounded and equicontinuous.

    Theorem 2.11. [15] (Schauder fixed point theorem). Let X be a Banach space and let MX be nonempty, convex, and closed. If T:MM is compact, then T has a fixed point

    Theorem 2.12. [36] (Contraction mapping principle). Let M be a Banach space. If T:MM is a contraction, thenT has a unique fixed point in M.

    For the definitions of Ulam-Hyers stable and Ulam-Hyers-Rassias stable see [33].

    Definition 2.13. The Eq (1.1) is Ulam-Hyers stable if there exists a real number cf>0 such that for each ε>0 and for each solution zC1(J,R) of the inequality

    |RDβ(cDαz(t)+λcDα1z(t))f(t,z(t))|ε,tJ, (2.1)

    there exists a solution yC1(J,R) of Eq (1.1) with

    |z(t)y(t)|cfε,tJ.

    Definition 2.14. The Eq (1.1) is Ulam-Hyers-Rassias stable with respect to φC(J,R+) if there exists a real number cf>0 such that for each ε>0 and for each solution zC1(J,R) of the inequality

    |RDβ(cDαz(t)+λcDα1z(t))f(t,z(t))|εφ(t),tJ, (2.2)

    there exists a solution yC1(J,R) of Eq (1.1) with

    |z(t)y(t)|cfεφ(t),tJ.

    Lemma 2.15. Let fC[0,1], yC1[0,1], then the initial value problem (1.1) and (1.2) has a solution

    y(t)=10G(t,s)f(s,y(s))ds, (2.3)

    where G(t,s) is the Green's function described by

    G(t,s)={eλ(ts)Γ(α+β1)s0(sτ)α+β2dτ+[tα+β1E1,α+β(λt)(m1(1s)β1Γ(β)m2)+m1m2λ(1eλt)(Ω4(1s)β1Γ(β)Ω1)]s0eλ(sτ)(Ω4m2Ω1m1)τ0(τr)α+β2Γ(α+β1)drdτ,if0st,[tα+β1E1,α+β(λt)(m1(1s)β1Γ(β)m2)+m1m2λ(1eλt)(Ω4(1s)β1Γ(β)Ω1)]s0eλ(sτ)(Ω4m2Ω1m1)τ0(τr)α+β2Γ(α+β1)drdτ,ifts1.

    where

    Ω1=1Γ(β)10(1s)β1s0eλ(sτ)τα+β2Γ(α+β1)dτds,Ω2=1Γ(β)10(1s)β1s0eλ(sτ)Γ(α+β1)τ0(τr)α+β2f(r,y(r))drdτds,Ω3=10s0eλ(sτ)Γ(α+β1)τ0(τr)α+β2f(r,y(r))drdτds,Ω4=10s0eλ(sτ)τα+β2Γ(α+β1)dτds,D1=1Γ(β)10(1s)β1eλsds1Γ(β+1)λ2,D2=(λ2λeλ+1),m2=λ2D2,m1=λD1,

    Proof. By applying the Lemma 2.5 and 2.7, we may reduce Eq (1.1) to an equivalent equation

    y(t)+λt0y(s)ds=t0Iα+βf(t,y(t))+c1tα+β1Γ(α+β)+k0+k1t. (2.4)

    Operate both sides of Eq (2.4) by operator D, we get

    Dy(t)+λy(t)=t0Iα+β1f(t,y(t))+c1tα+β2Γ(α+β1)+k1. (2.5)

    Then the solution of Eq (2.5) is

    y(t)=eλty(0)+t0eλ(ts)saIα+β1f(s,y(s))ds+c1t0eλ(ts)sα+β2Γ(α+β1)ds+k1λ(1eλt). (2.6)

    Using the initial conditions (1.2), we find that

    c1=(Ω2m1Ω3m2)(Ω4m2Ω1m1) and k1=m1m2(Ω2Ω4Ω3Ω1)(Ω4m2Ω1m1).

    Substituting the values of c1 and k1 in Eq (2.6), we have

    y(t)=t0eλ(ts)saIα+β1f(s,y(s))ds+(Ω2m1Ω3m2)(Ω4m2Ω1m1)t0eλ(ts)sα+β2Γ(α+β1)ds+m1m2(Ω2Ω4Ω3Ω1)λ(Ω4m2Ω1m1)(1eλt),=10G(t,s)f(s,y(s))ds.

    The converse of the lemma follows from a direct computation. Hence, the proof is completed.

    In this section, we prove the existence and uniqueness of solution for the problem (1.1) and (1.2) in the Banach space C by applying Banach contraction principle and Schauder fixed point theorem.

    Let C([0,1],R) denote the Banach space of all continuous functions from [0,1] into R with the norm defined by

    y=sup{|y(t)|,t[0,1]}.

    To prove the main results, we need the following assumptions:

    (H1) There exists a positive constants γ1,γ2 such that |f(t,y(t))|γ1+γ2|y(t)|, for each tJ and all yR.

    (H2) There exists a positive constant k such that |f(t,x(t))f(t,y(t))|k|x(t)y(t)|,

    for each tJ and all x,yR.

    (H3) There exists an increasing function φC(J,R+) and there exists νφ>0 such that for any tJ, we have

    t0eλ(ts)sα+β2Γ(α+β1)φ(s)dsνφφ(t).

    For convenience, we define the following notations:

    μ=k(1eλ)λΓ(α+β)(1+m1(1eλ)(λ+2m2Λ2)λ2Γ(α+β1)Γ(β+1)+m2Λ2λΓ(α+β1)),ζ1=|m1E1,α+2β+1(λ)m2E1,α+β+2(λ)m2E1,α+β+1(λ)m1E1,α+2β(λ)|,ζ2=m1m2λ|E1,α+β+1(λ)E1,α+2β+1(λ)E1,α+2β(λ)E1,α+β+2(λ)m2E1,α+β+1(λ)m1E1,α+2β(λ)|,ζ3=tα+β|E1,α+β+1(λt)|+ζ1tα+β1|E1,α+β(λt)|+ζ2|1eλt|,Λ1=|E1,α+β+1(λ)|+ζ1|E1,α+β(λ)|+ζ2(1eλ).

    The existence result can be obtained by the Schauder fixed point theorem.

    Theorem 3.1. Assume f:J×RR is continuous and satisfies (H1). Then the problem (1.1) and (1.2) has a solution.

    Proof. Consider an operator T defined on C(J) by

    (Ty)(t)=suptJ10G(t,s)f(s,y(s))ds.

    By the continuity of the functions G(t,s) and f(t,y(t)), we have TyC(J) for any yC(J). We define the set Br={y(t)C(J,R):yr} and choose rγ1Λ1(1γ2Λ1). First, we have to show that TBrBr, for yBr. Now, consider

    ||(Ty)(t)||=suptJ10|G(t,s)||f(s,y(s))|ds.

    Then

    ||(Ty)(t)||(γ1+γ2r)suptJ10|G(t,s)|ds,

    and so

    ||(Ty)(t)||(γ1+γ2r)(tα+β|E1,α+β+1(λt)|+tα+β1|E1,α+β(λt)||m1E1,α+2β+1(λ)m2E1,α+β+2(λ)m2E1,α+β+1(λ)m1E1,α+2β(λ)|+m1m2λ|E1,α+β+1(λ)E1,α+2β+1(λ)E1,α+2β(λ)E1,α+β+2(λ)m2E1,α+β+1(λ)m1E1,α+2β(λ)|(1eλt)).

    Therefore, we have

    ||(Ty)(t)||(γ1+γ2r)(|E1,α+β+1(λ)|+|E1,α+β(λ)||m1E1,α+2β+1(λ)m2E1,α+β+2(λ)m2E1,α+β+1(λ)m1E1,α+2β(λ)|+m1m2λ|E1,α+β+1(λ)E1,α+2β+1(λ)E1,α+2β(λ)E1,α+β+2(λ)m2E1,α+β+1(λ)m1E1,α+2β(λ)|(1eλ)),

    which implies that

    ||(Ty)(t)||(γ1+γ2r)Λ1r.

    Hence, TBrBr.

    Next, we need to prove that T is a completely continuous operator. For this purpose we fix,

    Q=suptJ|f(s,y(s))|, where yBr, and t,τJ with t<τ. Then

    T(y)(t)T(y)(τ)QsuptJ10|G(t,s)G(τ,s)|ds.

    Therefore,

    T(y)(t)T(y)(τ)Q(|tα+βE1,α+β+1(λt)τα+βE1,α+β+1(λτ)|+|tα+β1E1,α+β(λt)τα+β1E1,α+β(λτ)||m1E1,α+2β+1(λ)m2E1,α+β+2(λ)m2E1,α+β+1(λ)m1E1,α+2β(λ)|+m1m2λ|E1,α+β+1(λ)E1,α+2β+1(λ)E1,α+2β(λ)E1,α+β+2(λ)m2E1,α+β+1(λ)m1E1,α+2β(λ)||eλteλτ|),

    and so

    T(y)(t)T(y)(τ)Q(|tα+βE1,α+β+1(λt)τα+βE1,α+β+1(λτ)|+ζ1|tα+β1E1,α+β(λt)τα+β1E1,α+β(λτ)|+ζ2|eλteλτ|).

    Let tτ, the right-hand side of the above inequality tends to zero. Thus, T is uniformly bounded and equicontinuous. Therefore by th Arzela-Ascoli implies that T is completely continuous. Hence, by Schauder's fixed point theorem, the problem (1.1) and (1.2) has a solution on C(J,R). Now, we use the contraction principle mapping to investigate uniqueness results for (1.1) and (1.2).

    Theorem 3.2. Suppose that (H2) holds. If

    k(1eλ)λΓ(α+β)(1+m1(1eλ)(λ+2m2Λ2)λ2Γ(α+β1)Γ(β+1)+m2Λ2λΓ(α+β1))<1, (3.1)

    where Λ2=(λ+eλ1)λ, then the problem (1.1) and (1.2) has a unique solution.

    Proof. Let x,yC(J,R). Then

    ||T(x)(t)T(y)(t)||suptJ10|G(t,s)||f(s,x(s))f(s,y(s))|ds,

    and so

    ||T(x)(t)T(y)(t)||ksuptJ10|G(t,s)||x(s)y(s)|ds.

    Therefore,

    ||T(x)(t)T(y)(t)||k||x(t)y(t)||(|t0eλ(ts)s0(sτ)α+β2Γ(α+β1)dτds|+t0eλ(ts)sα+β2Γ(α+β1)ds(|m110(1s)β1Γ(β)s0eλ(sτ)τ0(τr)α+β2Γ(α+β1)drdτds|+|m210s0eλ(sτ)τ0(τr)α+β2Γ(α+β1)drdτds|)+m1m2λ(1eλt)[|Ω410(1s)β1Γ(β)s0eλ(sτ)τ0(τr)α+β2Γ(α+β1)drdτds|+|Ω110s0eλ(sτ)τ0(τr)α+β2Γ(α+β1)drdτds|]).

    Then

    ||T(x)(t)T(y)(t)||k(1eλ)λΓ(α+β)(1+m1(1eλ)(λ+2m2Λ2)λ2Γ(α+β1)Γ(β+1)+m2Λ2λΓ(α+β1))||x(t)y(t)||,

    Hence

    ||T(x)(t)T(y)(t)||kμ||x(t)y(t)||.

    Using the condition (3.1), we conclude that T is a contraction mapping. Hence Banach contraction principle guarantees that T has a fixed point which is the unique solution of the problem (1.1) and (1.2). The proof is complete.

    In this section, we study Ulam-Hyers and Ulam-Hyers-Rassias stability of our problem (1.1) and (1.2).

    Theorem 4.1. Assume that f:J×RR is a continuous function and (H2) holds with kμ<1. Then the problem (1.1) and (1.2) is Ulam-Hyers stable.

    Proof. Let z(t)C(J,R) be a solution of the inequality (2.1), and there exists a solution yC(J,R) of Eq (1.1). Then, we have

    y(t)=10G(t,s)f(s,y(s))ds.

    From inequality (2.1), for each tJ, we get

    |z(t)10G(t,s)f(s,z(s))ds|εtα+β1E1,α+β(λt)εE1,α+β(λ), (4.1)

    by (H2), for each tJ, we obtain

    |z(t)y(t)||z(t)10G(t,s)f(s,z(s))ds|+k10G(t,s)|z(s)y(s)|ds.

    Then from Eq (4.1) we conclude that

    |z(t)y(t)|εE1,α+β(λ)1kμ,1kμ0.

    If cf=E1,α+β(λ)1kμ, then inequality

    |z(t)y(t)|cfε,tJ

    holds. Thus the problem (1.1) and (1.2) is Ulam-Hyers stable.

    Theorem 4.2. Assume that f:J×RR is a continuous function and (H2), (H3) holds with kμ<1. Then the problem (1.1) and (1.2) is Ulam-Hyers-Rassias stable.

    Proof. Let z(t)C(J,R) be a solution of the inequality (2.2), and there exists a solution yC(J,R) of Eq (1.1). From inequality (2.2), for each tJ, we have

    |z(t)10G(t,s)f(s,z(s))ds|εt0eλ(ts)sα+β2Γ(α+β1)φ(s)dsενφφ(t), (4.2)

    by using the hypothesis (H2), for each tJ, we get

    |z(t)y(t)||z(t)10G(t,s)f(s,z(s))ds|+k10G(t,s)|z(s)y(s)|ds.

    Then the use of Eq (4.2) implies that

    |z(t)y(t)|ενφφ(t)1kμ,1kμ0.

    Set cf=νφ1kμ. The inequality

    |z(t)y(t)|cfεφ(t),tJ,

    holds. The problem (1.1) and (1.2) is Ulam-Hyers-Rassias stable.

    In this section, we give two examples to illustrate the usefulness of our main results.

    Example 5.1. Consider the following fractional initial value problem:

    {D0.2(D1.2y(t)+D0.2y(t))=t4siny(t),tJ,y[0,1],y(0)=0,y(0)=10y(s)ds,andy(0)=1Γ(β)10(1s)β1y(s)ds. (5.1)

    Here, α=1.2, β=0.2, and λ=1. By Lipschitz condition, we obtain k=0.25. To estimate the contraction mapping, apply Theorem 3.2 to get kμ=0.1499975<1. This proves the problem (5.1) has a unique solution.

    By Theorem 4.1, we have

    |z(t)y(t)|εE1,1.4(λ)1kμ, where E1,1.4(λ)1kμ=0.6795687>0,

    which shows the problem (5.1) is Ulam-Hyers stable.

    Now, to analyze the behavior of the operator T, one can see that |f(t,y(t))|0.2103677 and |Ty(t)|0.2103677ζ3, (see Figure 1).

    Figure 1.  The behavior of the operator T for tJ.

    Example 5.2. Consider the following fractional initial value problem:

    {D12(D32y(t)+D12y(t))=5(6+t2)1(1+|y(t)|),tJ,y(0)=0,y(0)=10y(s)ds,andy(0)=1Γ(β)10(1s)β1y(s)ds. (5.2)

    Here, α=1.5,β=0.5,λ=1, and k=56. By a direct calculation, one can obtain that

    kμ=0.298856<1. Then by Theorem 3.2, the problem (5.2) has a unique solution.

    Furthermore, by Theorem 4.1, the problem (5.2) is Ulam-Hyers stable with

    |z(t)y(t)|εE1,2(λ)1kμ, where cf=E1,2(λ)1kμ=0.9015562621>0.

    Now, to illustrate the obtained results for Ulam-Hyers and Ulam-Hyers-Rassias stability, we consider the following cases:

    CaseI: We start by computing the value of p(t)=|z(t)y(t)| for y=1. From the Eq (2.1), we have

    |RD12(cD32y(t)+λcD12y(t))56+t211+y(t)|=0.8333ε.

    Therefor, by Theorem 4.1, the problem (5.2) has a solution z satisfying

    |z(t)y(t)|εtα+β1E1,α+β(λt)1kμ0.83333tE1,2(t)1kμ,( see Figure 2).
    Figure 2.  The value of p(t) for tJ.

    CaseII: We estimate the value p(t) for y=1 and φ(t)=t, from the Eq (2.2), we obtain ε=0.83333. By Theorem 4.2, the problem (5.2) is Ulam-Hyers-Rassias stable with

    |z(t)y(t)|ενφφ(t)1kμ0.83333t2E1,3(t)0.7011437,( see Figure   3).
    Figure 3.  The value of p(t) for tJ.

    Now, we estimate the value p(t) for y=1 when the function φ(t)=et. The problem (5.2) is Ulam-Hyers-Rassias stable with

    |z(t)y(t)|εtα+β(eλteλt)2(1kμ)λΓ(α+β1),( see Figure   4).
    Figure 4.  The value of p(t) for tJ.

    In this research, we examined the solution of nonlinear fractional differential equations with integral initial conditions. By means of the Shauder fixed point theorem and contraction mapping principle, we proved the existence and uniqueness of solutions for a nonlinear problem. In addition, the Hyers-Ulam and Hyers-Ulam-Rassias stability of the problem (1.1) and (1.2) are studied. Lastly, we presented several examples to demonstrate the use of our main theorems.

    The authors declare no conflict of interest.



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