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Research article

Existence of solutions for Caputo fractional iterative equations under several boundary value conditions

  • Received: 29 July 2022 Revised: 22 September 2022 Accepted: 25 September 2022 Published: 29 September 2022
  • MSC : 34C25, 34B16, 37J40

  • In this paper, we investigate the existence and uniqueness of solutions for nonlinear quadratic iterative equations in the sense of the Caputo fractional derivative with different boundary conditions. Under a one-sided-Lipschitz condition on the nonlinear term, the existence and uniqueness of a solution for the boundary value problems of Caputo fractional iterative equations with arbitrary order is demonstrated by applying the Leray-Schauder fixed point theorem and topological degree theory, where the solution for the case of fractional order greater than 1 is monotonic. Then, the existence and uniqueness of a solution for the period and integral boundary value problems of Caputo fractional quadratic iterative equations in RN are also demonstrated. Furthermore, the well posedness of the control problem of a nonlinear iteration system with a disturbance is established by applying set-valued theory, and the existence of solutions for a neural network iterative system is guaranteed. As an application, an example is provided at the end.

    Citation: Cuiying Li, Rui Wu, Ranzhuo Ma. Existence of solutions for Caputo fractional iterative equations under several boundary value conditions[J]. AIMS Mathematics, 2023, 8(1): 317-339. doi: 10.3934/math.2023015

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  • In this paper, we investigate the existence and uniqueness of solutions for nonlinear quadratic iterative equations in the sense of the Caputo fractional derivative with different boundary conditions. Under a one-sided-Lipschitz condition on the nonlinear term, the existence and uniqueness of a solution for the boundary value problems of Caputo fractional iterative equations with arbitrary order is demonstrated by applying the Leray-Schauder fixed point theorem and topological degree theory, where the solution for the case of fractional order greater than 1 is monotonic. Then, the existence and uniqueness of a solution for the period and integral boundary value problems of Caputo fractional quadratic iterative equations in RN are also demonstrated. Furthermore, the well posedness of the control problem of a nonlinear iteration system with a disturbance is established by applying set-valued theory, and the existence of solutions for a neural network iterative system is guaranteed. As an application, an example is provided at the end.



    Boundary value and periodic problems for iterative differential equations have attracted significant interest in recent years. The investigation of iterative differential equations dates back to 1965, when Petuhov [1] first proposed the existence and uniqueness of solutions to the following equation:

    z=λz(z(t)),t[b,b],

    with z(0)=z(b)=k under the different ranges of parameters λ and k. In general, compared with ordinary differential equations, it is more difficult to deal with such iterative differential equations since the existence of iterative terms leads to considerable difficulties of analysis and the failure of some methods, such as the monotone method [2], the measure of noncompactness [3], the upper and lower solutions method [4], the coincidence degree theory [5,6], etc. However, the fixed point method is one of the most powerful and fruitful tools studying the boundary value or periodic problems of this kind of iterative differential equation. It is worth mentioning that Ke [7] considered the existence of a solution for the first order iterative differential equation

    z=f(z(z(t))),z(a)=a,

    where a is the end point of an interval. Recently, applying Schauder's fixed point theorem, Kaufmann [8] further investigated the boundary value problems of the second-order iterative differential equation

    z=f(t,z(t),z[2](t)),

    where z[2](t)=z(z(t)), with z(a)=a,z(b)=b or z(a)=b,z(b)=a. In [9], the authors studied a third-order differential equations with linear iterative source for which the existence and uniqueness of a periodic solution are established by using Banach's and Krasnoselskii's fixed point theorems. The same method is used to deal with a first-order iterative differential equations together with some properties of Green's functions in [10]. Periodic problems were investigated in [11,12,13] by Schauder's or Banach's fixed point theorem. In recent years, fractional calculus has attracted the attention of many mathematicians, as well as researchers in a number of other fields, such as engineering, chemistry and physics. It is recognized that the usage of fractional calculus in various modeling applications is quite outstanding in the process. The main reason for the broad application of fractional operators is the fact that, distinct from "integer" operators, these operators have a non-local behavior which enables us to trace the past impact of the involved phenomena [14,15,16,17,18]. Along with the recent advances in fractional differential equations, researchers have contributed many investigations that discuss the behaviors of solutions of different types of fractional differential equations [19,20,21,22,23,24,25]. In addition, since fractional derivatives and integrals have different forms, other types of fractional differential systems are also investigated in [26,27,28,29,30,31,32], to name a few. To the best of our knowledge, there are few results on boundary value problems for fractional iterative equations. It should be noted that, the rotational periodic problem of some Caputo-fractional iterative systems is investigated in [33]. The existence and uniqueness of solutions for fractional iterative equations was studied in [34], in which the nonlinear function satisfies the Lipschitz condition.

    In this paper, however, under weaker conditions of one-sided Lipschitz, we consider the existence and uniqueness for a fractional quadratic iterative differential equation with arbitrary order in the sense of Caputo. It is worth emphasizing that the solution we obtained the case of fractional order greater than 1 is monotonically continuous for the first time. Then, the existence and uniqueness for a fractional vector iterative differential equation in RN are established by the Leray-Schauder fixed point theorem and topological degree theory under periodic and integral boundary value conditions, respectively. Furthermore, applying set-value theory, we prove the existence of solutions for a fractional nonlinear control system with a disturbance. Eventually, motivated by [35], the existence of a solution for a fractional neural networks iterative system where neuron activations are continuous or discontinuous.

    The framework of the present paper is arranged as follows. Some basic definitions and auxiliary results on fractional calculus are provided in section 2. In section 3, the existence and uniqueness of solutions of Caputo-fractional quadratic iterative equations with arbitrary order are addressed by applying the Leray-Schauder fixed point theorem and topological degree theory. In section 4, the existence and uniqueness of periodic solutions of fractional vector iterative equations are established in RN. Then, the existence of an integral boundary value solution for this vector iterative equation follows in section 5. In section 6, the well-posed result for a nonlinear control system is studied by applying set-valued theory, followed the existence of solutions for a neural network iterative system in section 7 and the presentation of an example in section 8.

    In this section, let RN be N dimensional Euclid space, , be the inner product in RN, and be the norm of RN space. Let T=[0,b] and C(T;RN) denote the space composed of all continuous functions from T to RN, with norm C=maxtT. Some basic definitions and fundamental facts of fractional calculus which will be used later need to be provided in the sequel. For details, we refer interest readers to [16,17,18].

    Definition 2.1. Assume that g is a function defined on the interval [a,b]. The Caputo fractional integral of order α>0 of g is defined by

    Iαg(t)=1Γ(α)ta(ts)α1g(s)ds,t>a, (2.1)

    where Γ() is the Gamma function.

    Definition 2.2. Let g be a function defined on the interval [a,b]. Then, the Caputo fractional derivative of order α>0 of g is defined by

    CDαg(t)=1Γ(nα)ta(ts)nα1g(n)(s)ds,(n1α<n,t>a),

    where g(n)(t):=dngdtn, n=[α]+1, and [α] is defined as the maximum positive integer not exceeding the number α.

    Definition 2.3. If gCn[a,b], then

    IαCDαg(t)=g(t)n1k=0g(k)(a)k!tk,

    where α[n1,n),nN. In particular, if gC1[0,b] and α(0,1], then for any t[0,b],

    IαCDαg(t)=g(t)g(0).

    Next, the following lemmas given here are of significant completing the proof of the main results.

    Lemma 2.1. ([36])Let α>0 and β(t) be locally integrable on [a,b], where β(t) is a nondecreasing and nonnegative function. Assume that h is a nonnegative, nondecreasing and continuous function, and U is a nonnegative continuous function satisfying

    U(t)β(t)+h(t)ta(ts)α1U(s)ds.

    Then, it holds that

    U(t)β(t)Eα(h(t)Γ(α)tα),

    where Eα is the single parameter Mittag-Leffler function given by Eα(x)=k=0xkΓ(kα+1).

    Now, we introduce several inequalities on the fractional derivative which will be used later.

    Lemma 2.2. ([37])Let U:TRN be a continuous differentiable function, and ARN×N is a positive definite matrix. Then, it holds that

    12CDα[U(t)AU(t)]U(t)ACDαU(t),

    for any α(0,1].

    Lemma 2.3. ([38])Assume that U:RR+ is a continuous function such that

    CDαU(t)ωU(t),α(0,1],

    where ω>0 is a constant. Then, the following estimate holds:

    U(t)U(0)Eα(ωtα),t0.

    Lemma 2.4. ([39]) Suppose that W is a Banach space, the set CW is nonempty and convex with 0C, and G:CC is an upper semicontinuous multifunction with compact convex value, which maps bounded sets to relatively compact sets. Then, one of the following statements is true:

    (i) Ξ={zC:zϵG(z),ϵ(0,1)} is an unbounded set;

    (ii) The multifunction G() has a fixed point, i.e., there exists zC such that zG(z).

    Let Eα,γ(x):=k=0xkΓ(αk+γ) be the two parameter (α,γ)-Mittag-Leffler function for xR. For notational convenience, set MA=maxtTEα(Atα), ˆMA=maxtTEα,α(Atα).

    This subsection investigates the existence and uniqueness of solutions of the Caputo-fractional quadratic iterative equation represented as follows:

    CDαz(t)=f(t,z(t),z[2](t)),a<t<b, (3.1)

    where z[2](t)=z(z(t)) for any α>0. In order to obtain our desired results, the following hypothesis on the nonlinear function f is needed:

    (H1) f[a,b]×R×RR is a continuous function such that

    (ⅰ) there exists a function θ1L+[a,b] such that |f(t,μ,η)|θ1(t), for all t[a,b], μ,ηR;

    (ⅱ) there exists a constant W>0, for any (t1,u1,v1),(t2,u2,v2)[a,b]×R×R, such that

    [f(t1,u1,v1)f(t2,u2,v2)](u1u2)W|u1u2|2.

    Theorem 3.1. Let 0<α<1, z(a)=a and b>(θ1Γ(α)α)11α. If hypothesis (H1) holds, then the Caputo-fractional quadratic iterative equation (3.1) admits a unique solution.

    Proof. Following Proposition 2.1, Eq (3.1) is equivalent to the following integral equation:

    z(t)z(a)=1Γ(α)ta(ts)α1f(s,z(s),z[2](s))ds.

    Define the operator T1:C[a,b]C[a,b] by

    T1(z(t)):=z(a)+1Γ(α)ta(ts)α1f(s,z(s),z[2](s))ds,t[a,b].

    Now, we divide the proof into two steps.

    First step. We claim the existence of a solution for Eq (3.1).

    From the definition of the operator T1 and the assumption (H1)(ⅰ), we can deduce

    |T1(z(t))||a|+1Γ(α)ta(ts)α1|f(s,z(s),z[2](s))|ds|a|+θ1Γ(α)ta(ts)α1ds|a|+θ1αΓ(α)(ba)αb,

    which means that T1 is uniformly bounded in C[a,b]. Now, we show the equicontinuity of T1. For any t,t+δ[a,b] and δ>0, it follows that

    |T1(z(t+δ))T1(z(t))|=|1Γ(α)t+δa(t+δs)α1f(s,z(s),z[2](s))ds1Γ(α)ta(ts)α1f(s,z(s),z[2](s))ds|1Γ(α)t+δt(t+δs)α1f(s,z(s),z[2](s))ds+ta[(t+δs)α1(ts)α1]f(s,z(s),z[2](s))dsθ1Γ(α)|t+δt(t+δs)α1ds|+|ta(t+δs)α1(ts)α1ds|2θ1αΓ(α)δα+θ1αΓ(α)|(t+δa)α(ta)α|.

    Let δ0, and then |T1(z(t+δ))T1(z(t))|0. Applying the Arzela-Ascoli theorem, it is easy to find that the operator T1:ΩΩ is completely continuous where

    Ω:={uC[a,b]:uC<b+1}.

    Then, the existence of a solution for the system (3.1) is transformed into the fixed point problem of T1, i.e., z=T1(z). For this, let Qλ(z):=zλT1(z) with λ[0,1], and then the definition of Ω implies that pQ(Ω). Thus, for any λ[0,1], we have

    deg(Qλ,Ω,p)=deg(Q1,Ω,p)=deg(IT1,Ω,p)=deg(Q0,Ω,p)=deg(I,Ω,p)=10,

    where I is the identity map. Consequently, T1 has a fixed point in Ω, i.e. z=T1(z), which leads to the existence of a solution for the system (3.1).

    Second step. We show the uniqueness of a solution for the system (3.1).

    Assume z1(t),z2(t) are two solutions of system (3.1) with the same initial value. Then, for all t[a,b], we can deduce from (3.1) that

    CDα(z1(t)z2(t))=f(t,z1(t),z[2]1(t))f(t,z2(t),z[2]2(t)),

    which, with multiplying by z1(t)z2(t), leads to

    CDα|z1(t)z2(t)|212(z1(t)z2(t))CDα(z1(t)z2(t))12[f(t,z1(t),z[2]1(t))f(t,z2(t),z[2]2(t))](z1(t)z2(t)). (3.2)

    Integrate on both sides with Proposition 2.1 and apply (H1)(ⅱ) to get

    |z1(t)z2(t)|212Γ(α)ta(ts)α1[(f(s,z1(s),z[2]1(s))f(s,z2(s),z[2]2(s)))(z1(s)z2(s))]dsW2Γ(α)ta(ts)α1|z1(s)z2(s)|2ds,t[a,b],

    which, by using Lemma 2.1, yields

    |z1(t)z2(t)|2=0,

    for any t[a,b]. This gives z1z2, and therefore, a unique solution for system (3.1) is guaranteed.

    Now, we consider the case 1<α<2 for system (3.1), and then the hypothesis on the nonlinear function f needs to be improved as follows:

    (H2) f[a,b]×R×RR is a continuous function such that

    (ⅰ) there exist two constants N,Q>0 such that N<f(t,μ,η)<Q for all (t,μ,η)[a,b]×R2;

    (ⅱ) there exist two constants M,F>0 such that

    [f(t1,u1,v1)f(t2,u2,v2)](u1u2)M|u1u2|2+F|v1v2|2

    for any (t,u1,v1),(t,u2,v2)[a,b]×R2.

    Theorem 3.2. Let 1<α<2, z(a)=a and z(b)=b. Suppose that ba+(Γ(α)ααN+Q)1α1 is satisfied, and (H2) holds. Then Eq (3.1) admits a unique solution which is monotonically increasing and continuous.

    Proof. Similar to (3.2), by Proposition 2.1, the solution of (3.1) is equivalent to

    z(t)=z(a)+z(a)(ta)+1Γ(α)ta(ts)α1f(s,z(s),z[2](s))ds. (3.3)

    Due to z(a)=a,z(b)=b, it follows from (3.3) that

    b=a+z(a)(ba)+1Γ(α)ba(bs)α1f(s,z(s),z[2](s))ds,

    which implies that

    z(a)=11Γ(α)(ba)ba(bs)α1f(s,z(s),z[2](s))ds.

    Now, substitute z(a) into (3.3), and use Green's function to turn problem (3.3) into the following integral equation:

    z(t)=a+tataΓ(α)(ba)ba(bs)α1f(s,z(s),z[2](s))ds+1Γ(α)ta(ts)α1f(s,z(s),z[2](s))ds=t+1Γ(α)(ba)ba(at)(bs)α1f(s,z(s),z[2](s))ds+1Γ(α)(ba)ta(ba)(ts)α1f(s,z(s),z[2](s))ds=t+1Γ(α)(ba)baG(t,s)f(s,z(s),z[2](s))ds, (3.4)

    where

     G(t,s)=1Γ(α)(ba){(at)(bs)α1+(ba)(ts)α1,astb,(at)(bs)α1,atsb.

    Similar to the proof of Theorem 3.1, define the operator T2:C[a,b]C[a,b], by

    T2(z(t)):=t+1Γ(α)(ba)baG(t,s)f(s,z(s),z[2](s))ds.

    First step. The existence of a solution to the problem (3.3).

    In light of the definition of T2, we can derive from (H2)(ⅰ) that

    d(T2(z(t)))dt=11Γ(α)(ba)ba(bs)α1f(s,z(s),z[2](s))ds+α1Γ(α)(ba)ta(ba)(ts)α2f(s,z(s),z[2](s))ds1QΓ(α)(ba)ba(bs)α1dsN(α1)Γ(α)ta(ts)α2ds1(αN+Q)(ba)α1αΓ(α),

    and

    d(T2(z(t)))dt=11Γ(α)(ba)ba(bs)α1f(s,z(s),z[2](s))ds+α1Γ(α)(ba)ta(ba)(ts)α2f(s,z(s),z[2](s))ds1+NΓ(α)(ba)ba(bs)α1ds+Q(α1)Γ(α)ta(ts)α2ds1+(N+αQ)(ba)α1αΓ(α).

    Notice that ba+(Γ(α)ααN+Q)1α1, and then (N+αQ)(ba)α1αΓ(α), which gives d(T2(z(t)))dt>0, d(T2(z(t)))dt<2 for any t[a,b]. Consequently, T2 is bounded and monotone increasing. Since T2(z(a))=a,T2(z(b))=b, then we have aT2(z(t))b, for all t[a,b]. The application of Schauder's theorem yields that there exists at least one fixed point of T2 such that z=T2(z), i.e., z is the solution of system (3.1).

    Second step. The uniqueness of the solution of Eq (3.1).

    Let z1,z2 be two solutions to Eq (3.1) with same initial data, and then it follows from (T2(zi(t)))<2(i=1,2), (3.4) and (H2)(ⅱ) that

    |z1(t)z2(t)|2=baG(t,s)[f(s,z1(s),z[2]1(s))f(s,z2(s),z[2]2(s))][z1(s)z2(s)]dsbaG(t,s)(M|z1(s)z2(s)|2+F|z[2]1(s)z[2]2(s)|2)ds(M+2F)baG(t,s)|z1(s)z2(s)|2ds,

    which together with Lemma 2.1 yields

    |z1(t)z2(t)|2=0,

    for any t[a,b]. Hence, z1z2, i.e., the uniqueness of the solution is proved, which completes the proof of Theorem 3.2.

    Theorem 3.3. Let n1<α<n (n3), z(a)=a, z(b)=b, and z(i)(a)=ξi>0(i=1,2,,n1) with ξ1>N(ba)α1Γ(α). Assume that the hypothesis (H2) is fulfilled, and then there is a unique solution of system (3.1) which is monotone.

    Proof. Integrating on both sides of system (3.1) and applying Proposition 2.1 gives

    z(t)=n1k=0z(k)(a)k!(ta)k+1Γ(α)ta(ts)α1f(s,z(s),z[2](s))ds. (3.5)

    Define the operator T3:C[a,b]C[a,b], by

    T3(z(t)):=n1k=0z(k)(a)k!(ta)k+1Γ(α)ta(ts)α1f(s,z(s),z[2](s))ds.

    First step. We establish the existence of a solution for Eq (3.1).

    The derivation rule, (H2)(ⅰ) and the boundary value condition in (3.1) show that

    d(T3(z(t)))dt=ξ1++ξn1(n2)!(ta)n2+α1Γ(α)ta(ts)α2f(s,z(s),z[2](s))dsξ1(α1)NΓ(α)ta(ts)α2dsξ1N(ba)α1Γ(α)>0, (3.6)

    for any t[a,b]. Also, we can find

    d(T3(z(t)))dt=ξ1++ξn1(n2)!(ta)n2+α1Γ(α)ta(ts)α2f(s,z(s),z[2](s))dsξ1++ξn1(n2)!(ba)n2+(α1)QΓ(α)ta(ts)α2dsC:=n1i=1ξi(i1)!(ba)i1+Q(ba)α1Γ(α). (3.7)

    Therefore, T3(z(t)) is a bounded and monotone increasing function. By taking T3(z(a))=a, T3(z(b))=b into account, one has aT3(z(t))b for all t[a,b]. Thanks to Schauder's theorem, we can conclude that z is a fixed point of T3. Therefore, z is the solution of Eq (3.1).

    Second step. We claim the uniqueness of a solution of Eq (3.1).

    Assume that z1,z2Cn1[a,b] are two solutions of (3.1) with the same initial data. Similar to (3.2), and from assumption (H2)(ⅱ), (3.5) and (3.7), one obtains that

    |z1(t)z2(t)|2=1Γ(α)ta(ts)α1f(s,z1(s),z[2]1)f(s,z2(s),z[2]2),z1(s)z2(s)dsta(ts)α1(M|z1(t)z2(t)|2+F|z[2]1(s)z[2]2(s)|2)dsM+CFΓ(α)ta(ts)α1|z1(s)z2(s)|2ds,

    where

    C=n1i=1ξi(i1)!(ba)i1+Q(ba)α1Γ(α). (3.8)

    Lemma 2.1 and z1(0)=z2(0) show z1(t)=z2(t) for any t[a,b], and then z1z2. The proof of Theorem 3.3 is completed.

    Consider the following boundary value periodic problem of the fractional iterative vector differential equation

    CDαz(t)+Bz(t)=f(t,z(t),z[2](t))+g(t),tT:=[0,b],z(0)=z(b), (4.1)

    where α(0,1), z[2](t)=(z1(z),z2(z),,zn(z))RN for any tT, the linear operator B:RNRN is positive definite, f:T×RN×RNRN is a continuous function, and gL(T;RN). Throughout this section, we assume that b is greater than some constant M11α to be determined later.

    We need the following assumptions:

    (H3) The linear operator B:RNRN is bounded and positive definite, that is, for any zRN, there exists a constant ξR+, such that Az,zξz2.

    (H4) f:T×RN×RNRN is a continuous function satisfying

    (ⅰ) for any x,yRN, there exists a function θL+(T), such that f(t,x,y)θ(t) for any tT;

    (ⅱ) for any tT, (u1,v1), (u2,v2)RN×RN, there exists a function μL+(T), such that

    f(t,u1,v1)f(t,u2,v2),u1u2μ(t)u1u22,

    where μ<ξ, and ξ is a constant in (H3).

    Theorem 4.1. If assumptions (H3),(H4) hold, then the fractional iterative differential system (4.1) has a unique solution.

    Proof. In view of Corollary 7.1 in [40], problem (4.1) is equivalent to the following integral iterative equation:

    z(t)=Eα(Atα)z(0)+t0(tτ)α1Eα,α(A((tτ)α))[f(τ,z(τ),z[2](τ))+g(τ)]dτ. (4.2)

    Then, it suffices to show the existence of a solution for problem (4.2). For this, the operator T4: C(T;RN)C(T;RN) is defined by

    T4(z(t)):=Eα(Atα)z(0)+t0(tτ)α1Eα,α(A((tτ)α))[f(τ,z(τ),z[2](τ))+g(τ)]dτ. (4.3)

    First, we show a priori boundedness of the solution. From the definition of operator T4 and the assumption (H4)(ⅰ), it can be deduced that

    T4(z(t))z(0)maxsTEα(Asα)+maxsTEα,α(Asα)Γ(α)t0(ts)α1[f(τ,z(τ),z[2](τ))+g(τ)]dsz(0)MA+(θ+g)ˆMAΓ(α)t0(ts)α1dsz(0)MA+(θ+g)ˆMAαΓ(α)bα, (4.4)

    where

    MA=maxsTEα(Asα),ˆMA=maxsTEα,α(Asα).

    Now, let us estimate the initial value z(0). Let t=b in Eq (4.2), and then it follows that

    z(b)=Eα(Abα)z(0)+ba(bτ)α1Eα,α(A(bτ)α)[f(τ,z(τ),z[2](τ))+g(τ)]dτ. (4.5)

    Invoking z(0)=z(b) and the assumption (H3), it is easy to see the determinant EEα(Abα)0, where E represents the identity matrix. Thus, we have from (4.4)

    z(0)=(EEα(Abα))1ba(bτ)α1Eα,α(A(bτ)α)[f(τ,z(τ),z[2](τ))+g(τ)]dτ.

    By means of hypothesis H4(ⅰ) and similar to estimate (4.4), one can show

    z(0)MEˆMA(θ+g)bααΓ(α), (4.6)

    where

    ME=(EEα(Abα))1.

    Substitute estimate (4.6) into estimate (4.4) to obtain

    T4(z(t))(MEMA+1)ˆMA(θ+g)αΓ(α)bα,tT.

    Let M:=(MEMA+1)ˆMA(θ+g)αΓ(α). From b>M11α, we therefore have

    T4(z(t))Mbα<b,tT. (4.7)

    Second, it will be shown that the existence of the solution is obtained. For this, we shall prove that the nonlinear operator T4 is completely continuous. For any zC(T;RN), we claim T4(z(t))C(T;RN). For all t,t+δ[0,b] and δ>0, from (4.2) one can show

    T4(z(t+δ))T4(z(t))1Γ(α)t+δ0(t+δs)α1Eα,α(A(t+δτ)α)f(s,z(s),z[2](s))ds1Γ(α)t0(ts)α1Eα,α(A(t+τ)α)f(s,z(s),z[2](s))ds+[Eα(A(t+δ)α)Eα(Atα)]z(0)+t+δ0(t+δs)α1Eα,α(A(t+δs)α)g(s)dst0(ts)α1Eα,α(A(ts)α)g(s)ds(θ+g)ˆMAΓ(α)|t+δ0(t+δs)α1ds+t0(t+δs)α1(ts)α1ds|+[Eα(A(t+δ)α)Eα(Atα)]z(0)2(θ+g)ˆMAαΓ(α)δα+2(θ+g)ˆMAαΓ(α)(t+δa)α(ta)α+[Eα(A(t+δ)α)Eα(Atα)]z(0). (4.8)

    As δ0, it is easy to get that

    T4(z(t+δ))T4(z(t))0.

    Therefore, T4(z(t))C(T;RN). Taking znz in C(T;RN), we can deduce T4(zn)T4(z)0, so T4: C(T;RN)C(T;RN) is continuous. According to the above prior estimate, by applying the Arzela-Ascoli theorem, it is easy to find that the operator T4: ΩΩ is completely continuous, where

    Ω:={uC(T;RN):uCb+1}.

    Thus, to get the existence of the solution, it suffices to show the fixed point problem of T4. Define the mapping Hε(z)=zεT4(z), where ε[0,1]. Take pH(Ω), and then for any ε[0,1], we get

    deg(Hε,Ω,p)=deg(H1,Ω,p)=deg(IT4,Ω,p)=deg(H0,Ω,p)=deg(I,Ω,p)0.

    So, T4 has a fixed point on Ω, i.e., z=T4(z), which leads to the existence of the solution.

    Finally, we will establish the uniqueness of the solution of differential iterative system (4.1). If z1,z2C(T;RN) are the two solutions to problem (4.1) with the same initial data, and take the difference between the two solutions and take the inner product with z1z2 to get

    z1(t)z2(t),CDα(z1(t)z2(t))+z1(t)z2(t),A(z1(t)z2(t))=z1(t)z2(t),f(t,z1(t),z[2]1(t))f(t,z2(t),z[2]2(t)).

    Based on the assumptions (H3) and (H4)(ⅱ), and using Lemma 2.2, we can derive

    CDαz1(t)z2(t)22z1(t)z2(t),CDα(z1(t)z2(t))2μ(t)z1(t)z2(t)22ξz1(t)z2(t)2. (4.9)

    Let S(t)=z1(t)z2(t)2, and inequality (4.9) can be simplified as

    CDαS(t)2(μ(t)ξ)S(t),

    which, by applying Lemma 2.3, presents

    S(t)S(0)Eα(2(μξ)tα),t[0,b]. (4.10)

    Take t=b in (4.10) to obtain

    S(b)S(0)Eα(2(μξ)bα). (4.11)

    Boundary condition z(b)=z(0) shows S(b)=S(0). Hence, we find from (4.11) that

    S(0){1Eα[2(μξ)bα]}0.

    From the monotonicity of Mittag-Leffler function Eα(t) (α(0,1)) and μ<ξ, it holds that

    Eα[(2(μξ)bα)]<1.

    Due to

    S(0)=z1(0)z2(0)20,

    one gets S(0)=0, which with (4.10) implies S(t)0. This means z1z2, so the uniqueness of the solution follows.

    Consider the following integral boundary value problem of Caputo-fractional quadratic iterative differential equations:

    CDαz(t)+Az(t)=f(t,z(t),z[2](t))+g(t),tT:=[0,b],z(0)=1λbb0z(s)ds, (5.1)

    where z[2](t)=(z1(z),z2(z),,zn(z)), λ>1, linear operator A:RNRN is positive definite satisfying (H3), f:T×RN×RNRN is a Carathéodory function satisfying (H4), and gL(T). Throughout this section, we assume that b>M11α with

    M:=(λ1)(MEMA+1)ˆMA(θ+g)λαΓ(α).

    Theorem 5.1. If the assumptions (H3) and (H4) are fulfilled, then the fractional quadratic iterative differential system (5.1) admits a unique solution.

    Proof. Similar to Theorem 4.1, it is sufficient to investigate the following integral iterative equation:

    z(t)=Eα(Atα)z(0)+t0(tτ)α1Eα,α(A(tτ)α)[f(τ,z(τ),z[2](τ))+g(τ)]dτ,tT.

    Due to z(0)=1λbb0z(s)ds, define an operator O1:C(T;RN)C(T;RN) by

    O1z(t)=Eα(Atα)λbb0z(s)ds+t0(tτ)α1Eα,α(A(tτ)α)[f(τ,z(τ),z[2](τ))+g(τ)]dτ.

    Then, the integral boundary value problem of Eq (5.1) can be transformed into a fixed point problem:

    z=O1z. (5.2)

    The proof process is divided into three steps.

    Step 1. The a priori boundedness of the solutions for problem (5.1).

    Let z be the solution of operator equation z=O1z. Apply the hypothesis (H4)(ⅰ), to deduce

    z(t)1λmaxtTz(t)Eα(Atα)+maxtTEα,α(Atα)t0(ts)α1|f(s,z(s),z[2](s))|ds+maxtTEα,α(Atα)t0(ts)α1|g(s)|ds1λzCMA+(g+θ)ˆMAt0(ts)α1ds, (5.3)

    where

    MA=maxtTEα(Atα),ˆMA=maxtTEα,α(Atα)

    for any tT. Due to the monotonicity of Mittag-Leffler function Eα(t)(t0) and because A is positive definite, it is easy to get MA<1. It follows from (5.3) that

    zCλλ1(g+θ)ˆMAΓ(α)αbα. (5.4)

    Notice

    M=λλ1(g+θ)ˆMAΓ(α)α

    and b>M11α, and then (5.6) yields

    zCb. (5.5)

    Step 2. The existence of the solution for problem (5.1).

    To begin with, we claim that O1zC(T;RN) for any zC(T;RN). For any t,t+δT, and δ>0, it follows from (5.2) that

    |O1z(t+δ)O1z(t)|t+δ0(t+δs)α1Eα,α(A(t+δs)α)f(s,z(s),z[2](s))dst0(ts)α1Eα,α(A(ts)α)f(s,z(s),z[2](s))ds+t+δ0(t+δs)α1Eα,α(A(t+δs)α)g(s)dst0(ts)α1Eα,α(A(ts)α)g(s)ds+[Eα(A(t+δ)α)Eα(Atα)]z(0)(θ+g)ˆMA|t+δ0(t+δs)α1ds+t0(t+δs)α1(ts)α1ds|+[Eα(A(t+δ)α)Eα(Atα)]z(0)2(θ+g)ˆMAαδα+2(θ+g)ˆMAα|(t+δa)α(ta)α|+[Eα(A(t+δ)α)Eα(At)α]z(0).

    As δ0, one has |O1z(t+δ)O1z(t)|0, and therefore O1zC(T;RN). Taking znz in C(T;RN), we have zin(z)zi(z) for each i=1,2,,n, which together with the continuity of (s,v)f(t,s,v), yields |O1znO1z|0. Thus, O1:C(T;RN)C(T;RN) is continuous. By taking the prior estimation (Step 1) into account and applying the Arzela-Ascoli theorem, it holds that the operator O1:ΩΩ is completely continuous, where

    Ω={zC(T;RN):zCb+1}.

    Hence, the existence of solutions for the differential iterative system (5.1) can be transformed into a fixed point problem of O1. Define the mapping Hε(z)=zεO1(z) for zC(T;RN), with ε[0,1]. Let pHε(Ω), for any ε[0,1], and this leads to

    deg(Hε,Ω,p)=deg(H1,Ω,p)=deg(IO1,Ω,p)=deg(H0,Ω,p)=deg(I,Ω,p)=10.

    Therefore, the operator O1 has a fixed point on Ω, i.e., z=O1z, so the existence of the solution z for differential system (5.1) follows.

    Step 3. The uniqueness of the solution for problem (5.1).

    Let z1,z2C(T;RN) be two solutions of problem (5.1). Substitute z1 and z2 into (5.1), respectively, and then take a difference and the inner product with z1z2 to get

    z1(t)z2(t),CDα(z1(t)z2(t))+z1(t)z2(t),A(z1(t)z2(t))=z1(t)z2(t),f(t,z1(t),z[2]1(t))f(t,z2(t),z[2]2(t)). (5.6)

    By means of the hypotheses (H3) and (H4)(ⅱ), applying Lemma 2.2, it results that

    Dαz1(t)z2(t)22z1(t)z2(t),Dα(z1(t)z2(t))2μ(t)z1(t)z2(t)22ξz1(t)z2(t)2.

    Let Q(t):=z1(t)z2(t)2 for brevity, and the above inequality can be simplified as

    CDαQ(t)2(μ(t)ξ)Q(t).

    Invoke Lemma 2.3 to show

    Q(t)Q(0)Eα(2(μξ)tα),tT. (5.7)

    In light of z1(0)z2(0)=1λbb0[z1(t)z2(t)]dt in (5.7), one obtains

    z1(t)z2(t)2C1λbb0[z1(t)z2(t)]2dtEα((2μξ)bα), (5.8)

    which leads to

    z1(t)z2(t)2C(1Eα((2μξ)tα)λ)0, (5.9)

    with λ>1. Since the Mittag-Leffler function Eα(t)(t0) is monotonically decreasing, and μ<ξ, we can conclude that z1z2, so the iterative differential equation (5.1) has a unique solution, which yields our desired result.

    The aim of this section is to study the following Control problem for an iterative differential system with a disturbance:

    {CDαz(t)+Az(t)=f(t,z(t),z[2](t))+u(t)+d(t),tT:=[0,b],u(t)U(t,x),z(0)=1λbb0z(s)ds, (6.1)

    where A, f are shown as in (5.1), u:TRN is a control input, U:T×RN2RN{} is a multifunction of observation value, and dL(T) is a disturbance function. The hypothesis on U is presented as follows.

    H(U):U:T×RN2RN{} is a multivalued function with closed, convex value such that

    (ⅰ) (t,y)U(t,y) is graph measurable for every (t,y)T×RN;

    (ⅱ) for almost all tT, yU(t,y) has a closed graph;

    (ⅲ) for every yRN and all tT, there exists a function ΦL+(T) such that

    |U|=sup{u;uU}Φ(t).

    In this section, we assume that b>M11α with

    M:=(λ1)(MEMA+1)ˆMA(θ+Φ+d)λαΓ(α).

    Theorem 6.1. If the assumptions (H3),(H4) and H(U) hold, then the problem (6.1) admits at least one solution zC(T;RN).

    Proof. We first construct a closed convex subset K in L(T;RN) given by

    K:={hL(T;RN);hΦ+d}.

    Due to Theorem 5.1, it is straightforward to derive that the iterative equation

    {CDαz(t)f(t,z(t),z[2](t))+Az(t)=h(t),tT,z(0)=1λbb0z(s)ds, (6.2)

    admits a unique solution zhC(T;RN) for every hK. An operator

    O2:D(O2)C(T;RN)L(T;RN),

    is defined by

    O2z=Dαzf(t,z(t),z[2](t))+Az,zD(O2), (6.3)

    where

    D(O2):={zC(T;RN),z(0)=1λbb0z(s)ds}.

    Since O2:D(O2)K(L(T;RN)) is a one-to-one mapping, it results that O12:KD(O2) exists. Now, we claim that the operator

    O12:KD(O2),

    is completely continuous. For this, we will claim that O12:KD(O2) is continuous. Let hmh in K as m, and it remains to prove that zm=O12(hm)z=O12(h) in D(O2)(C(T;RN)). Replacing z with zm in (6.2) and subtracting (6.2) implies

    CDα(zm(t)z(t))+A(zm(t)z(t))=f(t,zm(t),z[2]m(t))f(t,z(t),z[2](t))+hm(t)h(t).

    Then, take the inner product with zmz on the above equation and apply Lemma 2.2 to obtain

    12CDαzmz2zm(t)z(t),CDα(zm(t)z(t))z1(t)z2(t),f(t,z1(t),z[2]1(t))f(t,z2(t),z[2]2(t))zm(t)z(t),A(zm(t)z(t))zm(t)z(t),hm(t)h(t). (6.4)

    Now, integrating in time and invoking Proposition 2.1 yields

    12zmz21Γ(α)t0(tτ)α1zm(τ)z(τ),f(t,zm(τ),z[2]m(τ))f(t,z(τ),z[2](τ)dτ1Γ(α)t0(tτ)α1zm(τ)z(τ),A(zm(τ)z(τ))dτ1Γ(α)t0(tτ)α1zm(τ)z(τ),hm(τ)h(τ)dτ+12zm(0)z(0)2. (6.5)

    Similar to the a priori estimate of the solution of Theorem 5.1, it is easy to verify that zmCb, which together with zmC(T;RN) and the Arzela-Ascoli theorem reveals that there exists a subsequence zm (still denoted by itself) such that zmˆz in D(O2) as m. By passing the limit in (6.5), this enables us to obtain

    12ˆzz2ˆz(0)z(0)21Γ(α)t0(tτ)α1ˆz(τ)z(τ),A(ˆz(τ)z(τ))dτ+1Γ(α)t0(tτ)α1ˆz(τ)z(τ),f(τ,ˆz(τ),ˆz[2](τ))f(τ,z(τ),z[2](τ))dτ. (6.6)

    Analogous to the analysis of (5.6), set Y=ˆzz2, and then we can conclude that Y(t)0, i.e., ˆzz in D(O2). This implies the continuity of operator O12. In view of the a priori estimate of the solution, it is easy to deduce that O12(K) is a bounded set in C(T;RN). Invoking the Arzela-Ascoli theorem, O12(K)L(T;RN) is relatively compact. As a result, O12:KL(T;RN) is completely continuous.

    Now, a multivalued Nemitsky operator N:L(T;RN)2L(T;RN) corresponding to U(t,z) is defined by

    N(z)={uL(T;RN);u(t)U(t,z),a.e.tT}.

    From hypothesis H(U), it holds that the multivalued Nemitsky operator N() is nonempty, closed convex value and upper hemicontinuous (Theorem 3.2, [41]). Thus, we can find that O12N:KL(T;RN) is an upper hemicontinuous multifunction with closed, convex value, which maps a bounded set into a relatively compact set. Then, the control problem for a iterative differential system (6.1) is turned into the following fixed points problem:

    zO12N(z). (6.7)

    For this aim, via Lemma 2.4, it remains to show that the set

    Ξ:={zL(T;RN):zϵO12N(z),ϵ(0,1)}

    is bounded. Let zΞ, and then O2(zϵ)N(z), which gives

    CDαzϵf(t,z(t)ϵ,z[2]ϵ(t)ϵ)+Azϵ=h(t)+d(t), (6.8)

    where h(t)U(z,t) for all tT. Similar to (5.2), Eq (6.8) can be rewritten as

    z(t)=Eα(Atα)z(0)+ϵt0(tτ)α1Eα,α(A(tτ)α)f(τ,z(τ)ϵ,z[2]ϵ(τ)ϵ)dτ+ϵt0(tτ)α1Eα,α(A(tτ)α)(h(τ)+d(τ))dτ. (6.9)

    Likewise as in (5.3) and by taking (H4)(ⅱ) into account, it results from (6.9) that

    zCz(0)MA+(θ+Φ+d)ˆMAmaxtIt0(ts)α1dsz(0)MA+(θ+Φ+d)ˆMAαbα. (6.10)

    Similar to the estimate (5.3), it holds that z(t) is uniformly bounded for any tT. Thanks to Lemma 2.4, there exists zD(O2), such that zO12N(z). It is obvious that z is the solution of problem (5.1). This proof is thus complete.

    Consider the fractional iterative neural network system described as follows:

    Dαz(t)+Bz(t)=F(z(t),z[2](t))+I(t),tT=[0,b],z(0)=1λbb0z(s)ds, (7.1)

    where B=diag(d1,d2,,dN) is a diagonal matrix with di>0(i=1,2,,N), z:TRN denotes the vector element of the neuron system, IL(T;RN) is the mapping of neuron inputs, and F:RN×RNRN stands for the neuron input-output continuous activation function such that

    (ⅰ) For any x,yRN, there exists a function ˆωL+(T) such that F(x,y)ˆω(t),tT;

    (ⅱ) For any x1,x2,y1,y2RN, there exists a function ˆμL+(T) such that

    F(x1,y1)F(x2,y2),x1x2ˆμ(t)x1x22,

    where ˆμ<min{di:i=1,2,,N}, for almost all tT.

    The initial value problem of the differential system (7.1) without iteration was discussed in [35], where the existence and uniqueness of the solution were demonstrated. Here, however, considering the iterative term and the integral boundary value condition, the existence of a unique integral boundary value solution to system (7.1) is guaranteed by using our results. Let b>M11α with

    M:=(MEMA+1)ˆMA(ˆω+I)αΓ(α).

    It is easy to show that all assumptions of Theorem 5.1 hold, and then the existence result for system (7.1) is provided as follows.

    Theorem 7.1. If the above assumptions are fulfilled, problem (7.1) admits a unique integral boundary value solution.

    It should be noted that the fractional system (7.1) without iteration was considered in Song et al. [35], where input function I(t) is assumed to be continuous. Automatically, a question is whether the fractional iteration system (7.1) has a solution, provided that I(t)=(I1(t),,IN(t)) is discontinuous. The following work is to deal with this question. For this, it is assumed that IiΛ(i=1,2,,N) are nondecreasing monotone, bounded mappings, where Λ:RR denotes the class of functions which have a finite number of jumping discontinuities in the closed interval. If only isolated jump discontinuities for any Ii(i=1,2,,N) appear, then we can deduce

    Y(I(t)):=([I1_,¯I1],[I2_,¯I2],,[IN_,¯IN])

    with

    Ii_Ii¯Ii,Ii_=lim_εtiIi(ε),¯Ii=¯limεtiIi(ε)(i=1,2,,N).

    Hence, in this case, the iteration problem (7.1) can be rewritten as the following iteration differential inclusion:

    \begin{eqnarray} D^{\alpha}z(t)+Bz(t)\in {\mathcal F}(z(t), z^{[2]}(t)) +{\mathcal Y}({ I}(t)). \end{eqnarray} (7.2)

    Here, {\mathcal Y}({ I}(t)) can be handled as a multivalued control item of problem (6.1). Then, the argument is similar to that of Theorem 6.1, and we can conclude the following result.

    Theorem 7.2. If the given assumptions are satisfied, then the solution set of iteration differential system (7.2) is nonempty.

    As an application of the previous results, we introduce an example. Let us consider the boundary value problem of the following iterative differential equation:

    \begin{eqnarray} \left\{\begin{array}{l}{^{C}{\mathcal D}^{\frac{3}{2}} z(t) = \cos(t)[\frac{1}{\sqrt{1+z^2(t)}}+\sin (z^{[2]}(t))]}, \; \; t\in T: = [0, b], \\ z(0) = 0, \; z(b) = b. \\ \end{array}\right. \end{eqnarray} (8.1)

    From (3.1), it is easy to see that \alpha = \frac{3}{2} and

    f(t, z(t), z^{[2]}(t)) = \cos(t)[\frac{1}{\sqrt{1+z^2(t)}}+\sin (z^{[2]}(t))].

    Then we can directly calculate -2\leq f(t, s, w)\leq 2 for any (t, s, w)\in T\times \mathbb{R}\times \mathbb{R}, so the condition ( H_2 )(ⅰ) holds. For any (s_1, w_1), (s_2, w_2)\in \mathbb{R}\times \mathbb{R} and t\in T , it is easy to deduce that

    \begin{eqnarray} \label{e8.3} |f(t, s_1, w_1)-|f(t, s_2, w_2)|&\leq& |\cos(t)|\left[|\frac{1}{\sqrt{1+s_1^2}}-\frac{1}{\sqrt{1+s_2^2}}|+|\sin w_1-\sin w_2|\right]\\ &\leq& |s_1-s_2|+|w_1-w_2|, \end{eqnarray}

    which yields

    \begin{eqnarray} \label{e8.2} [f(t, s_1, w_1)-|f(t, s_2, w_2)][s_1-s_2]&\leq& |s_1-s_2|^2+|w_1-w_2||s_1-s_2|\\ &\leq& \frac{3}{2}|s_1-s_2|+\frac{1}{2}|w_1-w_2|. \end{eqnarray}

    This implies that the condition ( H_2 )(ⅱ) holds. Assume b < (\frac{3\Gamma(\frac{3}{2})}{10})^2 , and then apply Theorem 3.2 to conclude that Eq (8.1) admits a unique solution which is monotonically increasing continuous.

    In this article, we established the existence and uniqueness of solutions for nonlinear quadratic iterative equations in the sense of the Caputo fractional derivative with several boundary conditions by using several fixed point theorems, and we finally applied it to a neural network iterative system and a control problem of a nonlinear iteration system with a disturbance. Furthermore, when the fractional order of the differential system is greater than 1, it was shown for the first time that the solution for a nonlinear quadratic iterative equation is monotonic. Since different definitions of the fractional integral lead to different fractional order differential systems, the method applied in this article can also be applied to systems of many other fractional order iterative differential equations.

    The authors are indebted to Professor Yi Cheng for his encouragement and helpful discussion. This work were partially supported by the Natural Science Foundation of Liaoning Province and of Jilin Province (No. 2020-MS-290, 20200201274JC), Jilin Provincial Department of Education Science and Technology Research Project (No. JJKH20221261KJ) and School Research Project of Bohai University. The authors are grateful to referees for their constructive comments on the first version of our paper.

    The authors declare that there are no conflicts of interest.



    [1] V. R. Petuhov, On a boundary value problem, Trudy Sem. Teor. Differ. Uravneniis Otklon. Arg. Univ. Družby Narodov Patrisa Limum, 3 (1965), 252–255.
    [2] C. Derbazi, Z. Baitiche, M. S. Abdo, K. Shah, B. Abdalla, T. Abdeljawad, Extremal solutions of generalized Caputo-type fractional-order boundary value problems using monotone iterative method, Fractal Fract., 6 (2008), 146. https://doi.org/10.3390/fractalfract6030146 doi: 10.3390/fractalfract6030146
    [3] A. Aghajani, E. Pourhadi, J. J. Trujillo, Application of measure of noncompactness to a Cauchy problem for fractional differential equations in Banach spaces, Fract. Calc. Appl. Anal., 16 (2013), 962–977. https://doi.org/10.2478/s13540-013-0059-y doi: 10.2478/s13540-013-0059-y
    [4] A. Boutiara, M. Benbachir, J. Alzabut, M. E. Samei, Monotone iterative and upper-lower solution techniques for solving the nonlinear \Psi-Caputo fractional boundary value problem, Fractal Fract., 5 (2021), 194. https://doi.org/10.3390/fractalfract5040194 doi: 10.3390/fractalfract5040194
    [5] Z. Baitiche, K. Guerbati, M. Benchohra, Y. Zhou, Solvability of fractional multi-point BVP with nonlinear growth at resonance, J. Contemp. Math. Anal., 55 (2020), 126–142. https://doi.org/10.3103/S1068362320020041 doi: 10.3103/S1068362320020041
    [6] M. Benchohra, S. Bouriah, J. J. Nieto, Existence of periodic solutions for nonlinear implicit Hadamard's fractional differential equations, RACSAM, 112 (2018), 25–35. https://doi.org/10.1007/s13398-016-0359-2 doi: 10.1007/s13398-016-0359-2
    [7] K. Wang, On the equation x'(t) = f(x(x(t))), Funkcial. Ekvac., 33 (1990), 405–425.
    [8] E. R. Kaufmann, Existence and uniqueness of solutions for a second-order iterative boundary-value problem, Electron. J. Differ. Equ., 150 (2018), 1–6.
    [9] A. Bouakkaz, A. Ardjouni, R. Khemis, A. Djoudi, Periodic solutions of a class of third-order functional differential equations with iterative source terms, Bol. Soc. Mat. Mex., 26 (2020), 443–458. https://doi.org/10.1007/s40590-019-00267-x doi: 10.1007/s40590-019-00267-x
    [10] E. Egri, I. A. Rus, First order iterative functional-differential equation with parameter, Stud. Univ. Babes-Bolyai Math., 52 (2007), 67–80.
    [11] H. Y. Zhao, J. Liu, Periodic solutions of an iterative functional differential equation with variable coefficients, Math. Methods Appl. Sci., 1 (2016), 286–292. https://doi.org/10.1002/mma.3991 doi: 10.1002/mma.3991
    [12] H. Y. Zhao, M. Fečkan, Periodic solutions for a class of differential equation with delays depending on state, Math. Commun., 23 (2018), 29–42.
    [13] A. Bouakkaz, A. Ardjouni, A. Djoudi, Periodic solutions for a second order nonlinear functional differential equation with iterative terms by schauder's fixed point theorem, Acta Math. Univ. Comen., 87 (2018), 223–235.
    [14] J. Sabatier, O. P. Agrawal, J. A. T. Machado, Advances in fractional calculus: Theoretical developments and applications in physics and engineering, Springer Dordrecht, 2007. https://doi.org/10.1007/978-1-4020-6042-7
    [15] V. E. Tarasov, Fractional dynamics, Nonlinear Physical Science Springer Berlin, Heidelberg, 2010. https://doi.org/10.1007/978-3-642-14003-7
    [16] K. S. Miller, B. Ross, An introduction to the fractional calculus and fractional differential equations, Wiley, 1993.
    [17] I. Podlubny, Fractional differential equations: An introduction to fractional derivatives, fractional differential equations, to methods of their solution and some of their applications, San Diego: Academic Press, 1998.
    [18] S. Samko, A. Kilbas, O. Marichev, Fractional integrals and derivatives-theory and applications gordon and breach, Gordon and Breach Science Publishers, 1993.
    [19] J. Alzabut, J. Viji, V. Muthulakshmi, W. Sudsutad, Oscillatory behavior of a type of generalized proportional fractional differential equations with forcing and damping terms, Mathematics, 8 (2020), 1037. https://doi.org/10.3390/math8061037 doi: 10.3390/math8061037
    [20] X. Lin, Z. Zhao, Iterative technique for a third-order differential equation with three-point nonlinear boundary value conditions, Electron. J. Qual. Theory Differ. Equ., 2016 (2016), 1–10. https://doi.org/10.14232/ejqtde.2016.1.12 doi: 10.14232/ejqtde.2016.1.12
    [21] Y. Zhou, Fractional evolution equations and inclusions: Analysis and control, Elsevier, 2016.
    [22] Y. Cheng, K. Jin, R. P. Agarwal, Rotating periodic integrable solutions for second-order differential systems with nonresonance condition, Turk. J. Math., 45 (2021), 233–243. https://doi.org/10.3906/mat-2005-63 doi: 10.3906/mat-2005-63
    [23] Y. Cheng, S. Gao, R. P. Agarwal, Rotational periodic boundary value problem for a fractional nonlinear differential equation, Math. Method. Appl. Sci., 2020, 1–15. https://doi.org/10.1002/mma.6860 doi: 10.1002/mma.6860
    [24] Y. Belgaid, M. Helal, A. Lakmeche, E. Venturino, A mathematical study of a coronavirus model with the Caputo fractional-order derivative, Fractal Fract., 5 (2021), 87. https://doi.org/10.3390/fractalfract5030087 doi: 10.3390/fractalfract5030087
    [25] S. Gao, R. Wu, C. Li, The existence and uniqueness of solution to sequential fractional differential equation with affine periodic boundary value conditions, Symmetry, 14 (2022), 1389. https://doi.org/10.3390/sym14071389 doi: 10.3390/sym14071389
    [26] A. Das, B. Hazarika, S. K. Panda, V. Vijayakumar, An existence result for an infinite system of implicit fractional integral equations via generalized Darbo's fixed point theorem, Comput. Appl. Math., 40 (2021), 143. https://doi.org/10.1007/s40314-021-01537-z doi: 10.1007/s40314-021-01537-z
    [27] T. Abdeljawad, E. Karapinar, S. K. Panda, N. Mlaiki, Solutions of boundary value problems on extended-Branciari b-distance, J. Inequal. Appl., 2020 (2020), 103. https://doi.org/10.1186/s13660-020-02373-1 doi: 10.1186/s13660-020-02373-1
    [28] S. K. Panda, C. Ravichandran, B. Hazarika, Results on system of Atangana-Baleanu fractional order Willis aneurysm and nonlinear singularly perturbed boundary value problems, Chaos Solitons Fract., 142 (2021), 110390. https://doi.org/10.1016/j.chaos.2020.110390 doi: 10.1016/j.chaos.2020.110390
    [29] S. K. Panda, T. Abdeljawad, C. Ravichandran, Novel fixed point approach to Atangana-Baleanu fractional and L^{p}-Fredholm integral equations, Alex. Eng. J., 59 (2020), 1959–1970. https://doi.org/10.1016/j.aej.2019.12.027 doi: 10.1016/j.aej.2019.12.027
    [30] M. M. Matar, A. A. Lubbad, J. Alzabut, On p-Laplacian boundary value problem involving Caputo-Katugampula fractional derivatives, Math. Methods Appl. Sci., 51 (2020), 1485–1526. https://doi.org/10.1002/mma.6534 doi: 10.1002/mma.6534
    [31] K. D. Kucche, A. D. Mali, On the nonlinear \Psi-Hilfer fractional differential equations, Comput. Appl. Math., 41 (2019), 86. https://doi.org/10.1007/s40314-022-01800-x doi: 10.1007/s40314-022-01800-x
    [32] M. E. Samei, R. Ghaffari, S. W. Yao, M. K. A. Kaabar, F. Martínez, M. Inc, Existence of solutions for a singular fractional q-differential equations under Riemann-Liouville integral boundary condition, Symmetry, 13 (2021), 1235. https://doi.org/10.3390/sym13071235 doi: 10.3390/sym13071235
    [33] R. Wu, Y. Cheng, R. P. Agarwal, Rotational periodic solutions for fractional iterative systems, AIMS Math., 6 (2021), 11233–11245. https://doi.org/10.3934/math.2021651 doi: 10.3934/math.2021651
    [34] R. W. Ibrahim, A. Kilicman, F. H. Damag, Existence and uniqueness for a class of iterative fractional differential equations, Adv. Differ. Equ., 2015 (2015), 78. https://doi.org/10.1186/s13662-015-0421-y doi: 10.1186/s13662-015-0421-y
    [35] K. Song, H. Wu, L. Wang, Lur'e-Postnikov Lyapunov function approach to global robust mittag-leffler stability of fractional-order neural networks, Adv. Differ. Equ., 2017 (2017), 232. https://doi.org/10.1186/s13662-017-1298-8 doi: 10.1186/s13662-017-1298-8
    [36] H. Ye, J. Gao, Y. Ding, A generalized gronwall inequality and its application to a fractional differential equation, J. Math. Anal. Appl., 328 (2007), 1075–1081. https://doi.org/10.1016/j.jmaa.2006.05.061 doi: 10.1016/j.jmaa.2006.05.061
    [37] H. Wu, L. Wang, Y. Wang, P. Niu, B. Fang, Global mittag-leffler projective synchronization for fractional-order neural networks: An LMI-based approach, Adv. Differ. Equ., 2016 (2016), 132. https://doi.org/10.1186/s13662-016-0857-8 doi: 10.1186/s13662-016-0857-8
    [38] J. Chen, Z. Zeng, P. Jiang, Global Mittag-leffler stability and synchronization of memristor-based fractional-order neural networks, Neural Networks, 51 (2014), 1–8. https://doi.org/10.1016/j.neunet.2013.11.016 doi: 10.1016/j.neunet.2013.11.016
    [39] A. Granas, J. Dugundji, Fixed point theory, Springer, 2003. https://doi.org/10.1007/978-0-387-21593-8
    [40] K. Diethelm, The analysis of fractional differential equations, An application-oriented exposition using differential operators of Caputo type, Springer Berlin, Heidelberg, 2010. https://doi.org/10.1007/978-3-642-14574-2
    [41] Y. Cheng, F. Cong, H. Hua, Anti-periodic solutions for nonlinear evolution equations, Adv. Differ. Equ., 2012 (2012), 165. https://doi.org/10.1186/1687-1847-2012-165 doi: 10.1186/1687-1847-2012-165
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