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Rotational periodic solutions for fractional iterative systems

  • In this paper, we devoted to deal with the rotational periodic problem of some fractional iterative systems in the sense of Caputo fractional derivative. Under one sided-Lipschtiz condition on nonlinear term, the existence and uniqueness of solution for a fractional iterative equation is proved by applying the Leray-Schauder fixed point theorem and topological degree theory. Furthermore, the well posedness for a nonlinear control system with iteration term and a multivalued disturbance is established by using set-valued theory. The existence of solutions for a iterative neural network system is demonstrated at the end.

    Citation: Rui Wu, Yi Cheng, Ravi P. Agarwal. Rotational periodic solutions for fractional iterative systems[J]. AIMS Mathematics, 2021, 6(10): 11233-11245. doi: 10.3934/math.2021651

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  • In this paper, we devoted to deal with the rotational periodic problem of some fractional iterative systems in the sense of Caputo fractional derivative. Under one sided-Lipschtiz condition on nonlinear term, the existence and uniqueness of solution for a fractional iterative equation is proved by applying the Leray-Schauder fixed point theorem and topological degree theory. Furthermore, the well posedness for a nonlinear control system with iteration term and a multivalued disturbance is established by using set-valued theory. The existence of solutions for a iterative neural network system is demonstrated at the end.



    The research on iterative differential equations can be traced back to 1965, Petuhov studied a periodic boundary value problem of second-order differential iterative equation

    x=λx[2](t),x(0)=x(T)=αR,

    with x[2](t)=x(x(t)) in [1], where the author obtained the existence and uniqueness of solution of the equation when the parameters λ and α were in different ranges. Compared with ordinary differential equations, the appearance of iteration terms brings certain difficulties to study this type of iterative differential equations, and the fixed point theory is a common method to deal with such problems. Recently, Kaufmann considered the boundary value problem of a class of second-order differential iterative equations in [2], and used the Schauder fixed point theorem to show the existence of solution. In [3,4,5,6], researchers use different fixed point theories, including Krasnoselskii fixed point theorem, Schauder fixed point theorem, etc., to investigate the existence and uniqueness of periodic solutions or quasi-periodic solutions of several types of iterative differential equations.

    In recent years, fractional differential equations has aroused the interest of many mathematicians and researchers in the fields of engineering, chemistry, and physics, etc. However, there are few results on boundary value and periodic problems of fractional iterative differential equations. It is worth noting that when the nonlinear function satisfies the Lipschitz condition, Ibrahim [7] extended some results of integer order to fractional iterative differential equations. However, to the best of the authors' knowledge, there is no report about vector iterative equations in RN including integer order, since one-dimensional iterative differential systems were handled in previous works.

    In this paper, we first consider the following rotational periodic boundary value problem (RPBVP) of fractional differential system:

    {CDαx(t)+Ax(t)=f(t,x(t),x[2]+(t)),tI:=[0,b],x(b)=Qx(0), (1.1)

    where CDα denotes the Caputo fractional derivative with α(0,1), A:RNRN is a linear operator, f:I×RN×RNRN is a measurable function, and QO(n), where O(n) denotes the group of orthogonal matrix. When Q-rotating periodic are in different ranges, different solutions are derived, such as periodic solutions if we let Q=EN, where EN represents the identity matrix in RN, anti-periodic solutions if we let Q=EN, subharmonic solutions if we let Qk=EN for some kZ, and quasi-periodic solutions if we let Q=diag(W(θ1),,W(θk)) for N=2k with kZ, or Q=diag(W(θ1),,W(θk),±1) for N=2k+1, where W(θi)=(cosθisinθisinθicosθi) and θi[0,2π](i=1,2,,k).

    The first objective of this work is to prove that the RPBVP (1.1) has a unique rotational periodic solution by using topology-degree theory and the Leray-Schauder fixed point theorem. It is worth noting that the solution x is called rotational periodic solution if x satisfies x(t+T)=Qx(t) for all tR. Recently, more attention has been paid to the rotational periodic solutions of differential equations. The existence of rotating periodic solutions for second-order differential equations are demonstrated in [8,9] by using the coincidence degree method. The existence of rotating periodic solutions for second-order Hamiltonian system is investigated in [10] via the technique of penalized functionals and Morse theory, where the resonance condition at infinity is satisfied. Applying the homotopy continuation method, the rotating periodic problems of second order differential equation is considered in [11], where the nonlinearity satisfies the Hartman-type condition. The interested readers are referred to see [12,13] for physical investigation on the rotational periodic.

    Furthermore, we consider a fractional nonlinear control system of the following form:

    {CDαx(t)+Ax(t)f(t,x(t),x[2]+(t))+U(t)+d(t,x),tIU(t)F(t,x)x(b)=Qx(0) (1.2)

    where A,Q, f are present as in RPBVP (1.1), U:IRN is a control input, F:I×RN2RN{} is a multifunction of observation data, and d:I×RN2RN{} is a multivalued disturbance function. Motivated by [14,15], we use the techniques of functional analysis and set-value theory to get the existence of solutions for RPBVP (1.2).

    It is well known that dynamic neural networks systems are widely used in combinatorial optimization, associative memory, image and signal processing, pattern recognition and other fields. It should be mentioned that the existence and stability of solution for a fractional neural networks is studied in [16], where neuron activation functions are required to be continuous. Inspired by this, we also consider the fractional neural networks where neuron activations are discontinuous, and establish the existence of equilibrium point of this system at the end.

    The remainder of this paper is organized as follows. some basic definitions and auxiliary results corresponding to the fractional calculus are introduced in section 2. In section 3, the existence and uniqueness of solution for RPBVP (1.1) is provided by applying the Leray-Schauder fixed point theorem and topological degree theory. In section 4, the well posedness for a nonlinear control system (1.2) is established by using set-valued theory, followed up the existence of solution for a iterative neural network system in section 5.

    Let I:=[0,b], where b is greater than a constant given later. Let RN be an N-dimensional Euclid space, where the inner product and norm of RN are denoted by , and , respectively. Let C([0,b];RN) denote the space composed of all continuous functions from [0,b] to RN with xC=maxtIx(t),xC([0,b];RN). Let denote the norm of L[0,b]. For the basic properties of fractional calculus, we refer the readers to see [17,18,19].

    Definition 2.1. The fractional integral of order α>0 of a function y is defined as

    CIαy(t)=1Γ(α)t0(tτ)α1y(τ)dτ,t>0,

    where Γ() is the Gamma function.

    Definition 2.2. The fractional derivative of order α in the sense of Caputo for a function yCn[0,b] is defined as

    CDαy(t)=1Γ(nα)t0(tτ)nα1y(n)(τ)dτ,t>0,

    where α(n1,n),nN.

    A property regarding the Caputo fractional derivative is given as follows:

    Proposition 2.1. If yCn[0,T], then

    CIαCDαy(t)=y(t)n1k=0y(k)(0)k!tk,

    where α(n1,n),nN. In particular, if yC1[0,T] and α(0,1), then

    CIαCDαy(t)=y(t)y(0).

    Now, we state the fractional Gronwall's inequality which will be used later.

    Lemma 2.1. [20] Suppose that the nonnegative integrable function m(t) is defined on I, the nonnegative function p(t) is non-decreasing on I, and the nonnegative integrable function Y(t) satisfies

    Y(t)m(t)+p(t)t0(ts)α1Y(s)ds,tI,α>0.

    Then

    Y(t)m(t)Eα[Γ(α)p(t)tα],

    where Eα(w):=k=0wkΓ(αk+1),wR, is called the single parameter Mittag-Leffler function.

    Several inequalities on fractional derivative are given in the following.

    Lemma 2.2. [21] Assume that Y:IRN is a continuous differentiable function, and the matrix PRN×N is a positive definite. Then we have

    12CDα[YT(t)PY(t)]YT(t)PCDαY(t),

    for any α(0,1).

    Lemma 2.3. [22] Suppose W:RR+ is a continuous function satisfying

    CDαW(t)ωW(t),α(0,1),

    where ω is a positive constant. Then the following inequality holds:

    W(t)W(0)Eα(ωtα),t0.

    We present Leray-Schauder alternative theorem which plays an crucial role in our proofs.

    Lemma 2.4. [23] Assume that X is a Banach space, the set QX is nonempty and convex with 0Q, and G:QQ is an upper semicontinuous multifunction which has compact convex value and maps bounded sets to relatively compact sets, then one of the following arguments is valid:

    (i) Γ={xQ:zβG(z),β(0,1)} is an unbounded set;

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

    Let Eα,β(w):=k=0wkΓ(αk+β),wR be the two parameter Mittag-Leffler function. For notational convenience, set Mα=maxtIEα(Atα), ˆMα=maxtIEα,α(Atα), ME=(QEα(Abα)1. Throughout the article, we assume b>M11α with M:=(MEMα+1)ˆMαMλα, where Mλ is a positive constant.

    Consider the following fractional iterative vector differential equations

    CDαx(t)+Ax(t)=f(t,x(t),x[2]+(t)),tI,x(b)=Qx(0), (3.1)

    where x[2]+(t)=(x1(x),x2(x),,xn(x)), A:RNRN is a linear operator, f:I×RN×RNRN is a Carathéodory function. The required assumptions are given below.

    H(A):A:RNRN is a bounded, linear positive definite operator, that is, for any yRN, there exists a constant cR+ such that Ay,ycy2.

    H(f):f:I×RN×RNRN is a Carathéodory function such that

    (i) for any v,uRN, there exists a nonnegative function λL[0,b] with λMλ2, such that f(t,v,u)λ(t),t[0,b];

    (ii) for any tI, and v1,v2,u1,u2RN, there exists a nonnegative function μL[0,b], such that

    f(t,v1,u1)f(t,v2,u2),v1v2μ(t)v1v22,

    where μ<c, c is the positive constant provided in assumption H(A).

    Theorem 3.1. Assume that H(A) and H(f) hold, then the fractional iterative differential system (3.1) has a unique solution.

    Proof. It is easy to verify that the problem (3.1) is equivalent to the following integral iterative equation [24]

    x(t)=Eα(Atα)x(0)+t0(tτ)α1Eα,α(A(tτ)α)f(τ,x(τ),x[2]+(τ))dτ,tI. (3.2)

    Define an operator T1:C([0,b];RN)C([0,b];RN) by

    T1x(t)=Eα(Atα)x(0)+t0(tτ)α1Eα,α(A(tτ)α)f(τ,x(τ),x[2]+(τ))dτ. (3.3)

    We divide the proof process into three steps.

    Step 1. The priori boundedness of the solutions for problem (3.1).

    Invoke the definition of operator T1 and the hypothesis H(f)(i), to deduce

    T1xCx(0)Eα(Atα)C+maxtIEα,α(Atα)maxtIt0(ts)α1|f(s,x(s),x[2](s))|dsx(0)Mα+λˆMαmaxtIt0(ts)α1dsx(0)Mα+λˆMααbα, (3.4)

    where Mα=maxtIEα(Atα), ˆMα=maxtIEα,α(Atα), for any tI. Now, we estimate the initial value x(0). In Eq (3.2), taking t=b, we have

    x(b)=Eα(Abα)x(0)+b0(bτ)α1Eα,α(A(bτ)α)f(τ,x(τ),x[2]+(τ))dτ.

    Since x(b)=Qx(0) and hypothesis H(A), it is easy to check that the determinant |QEα(Abα)|0, so

    x(0)=(QEα(Abα))1b0(bτ)α1Eα,α(A(bτ)α)f(τ,x(τ),x[2]+(τ))dτ.

    From the hypothesis H(f)(i), in a similar fashion as (3.4), we derive directly that

    x(0)MEˆMαλbαα, (3.5)

    where ME=(QEα(Abα))1. Substitute (3.5) into (3.4) to obtain

    T1xC(MEMα+1)ˆMαλαbαMbα, (3.6)

    where M=(MEMα+1)ˆMαMλα. Due to b>M11α, one has T1xCMbα<b.

    Step 2. The existence of the solution to problem (3.1).

    To begin with, we show that T1xC([0,b];RN) for any xC([0,b];RN). For any t,t+δ[0,b], and δ>0, it follows from (3.3) that

    |T1x(t+δ)T1x(t)|t+δ0(t+δs)α1Eα,α(A(t+δs)α)f(s,x(s),x[2](s))dst0(ts)α1Eα,α(A(ts)α)f(s,x(s),x[2](s))ds+[Eα(A(t+δ)α)Eα(Atα)]x(0)λˆMα|t+δ0(t+δs)α1ds+t0(t+δs)α1(ts)α1ds|+[Eα(A(t+δ)α)Eα(Atα)]x(0)2λˆMααδα+2λˆMαα|(t+δa)α(ta)α|+[Eα(A(t+δ)α)Eα(At)α]x(0).

    When δ0, we have |T1x(t+δ)T1x(t)|0, therefore T1xC([0,b];RN). Taking xnxC([0,b];RN) where xn(t):=(x1n(t),x2n(t),,xnn(t))RN and x(t):=(x1(t),x2(t),,xn(t))RN for t[0,b], we arrive at xin(x)xi(x) for each i=1,2,,n, which together with the continuity of (s,v)f(t,s,v), yields |T1xnT1x|0. Hence, T1:C([0,b];RN)C([0,b];RN) is continuous. According to the prior estimation (Step.1) and applying Arzela-Ascoli theorem, we obtain that the operator T1:ΩΩ is completely continuous, where

    Ω={uC([0,b];RN):uCb+1}.

    Thus, the existence of solutions for the differential iterative system (3.1) can be transformed into a fixed point problem of T1. Define the mapping hε(x)=xεT1(x) for xC([0,b];RN), where ε[0,1]. Let ph(Ω), for any ε[0,1], this allows us to get

    deg(hε,Ω,p)=deg(h1,Ω,p)=deg(IET1,Ω,p)=deg(h0,Ω,p)=deg(IE,Ω,p)=10,

    where IE is the identity map. Therefore, T1 has a fixed point on Ω, namely x=T1x, so the existence of the solution x for differential iterative system (3.1) follows.

    Step 3. The uniqueness of the solution for problem (3.1).

    Suppose that x1,x2C([0,b];RN) are two solutions of the problem (3.1). Substitute x1 and x2 into (3.1) respectively, then take a difference and the inner product with x1x2, to obtain

    x1(t)x2(t),CDα(x1(t)x2(t))+x1(t)x2(t),A(x1(t)x2(t))=x1(t)x2(t),f(t,x1(t),x[2]1+(t))f(t,x2(t),x[2]2+(t)).

    By virtue of the hypotheses H(A) and H(f)(ii), invoking Lemma 2.2, one gets

    Dαx1(t)x2(t)22x1(t)x2(t),Dα(x1(t)x2(t))2μ(t)x1x222cx1x22.

    Set U(t)=x1(t)x2(t)2 for brevity, the above estimate can be simplified as

    CDαU(t)2(μ(t)c)U(t).

    Apply Lemma 2.3 to present

    U(t)U(0)Eα(2(μc)tα),tI. (3.7)

    Taking t=b in (3.7), one obtains

    U(b)U(0)Eα((2μc)bα). (3.8)

    Since boundary condition xi(b)=Qxi(0)(i=1,2), one can find

    U(b)=x1(b)x2(b)2=Qx1(0)Qx2(0)2=Q(x1(0)x2(0)),Q(x1(0)x2(0))=(x1(0)x2(0))TQTQ(x1(0)x2(0))=x1(0)x2(0)2=U(0). (3.9)

    Hence, it follows from (3.8) that

    U(0){1Eα[2(μc)bα]}0.

    Due to the monotonicity of Mittag-Leffler function Eα(t)(t0) and μ<c, we can conclude that Eα[2(μc)bα]<1. Because U(0)=x1(0)x2(0)20, we can derive U(0)=0. From (3.7), we have U(t)0, and then U(t)0, that is, x1x2, so the iterative differential equations (3.1) admits a unique solution, which our desired result follows.

    In this section, consider the following nonlinear iterative control with a multivalued disturbance:

    {CDαx(t)+Ax(t)f(t,x(t),x[2]+(t))+U(t)+d(t,x),tI,U(t)F(t,x),x(b)=Qx(0), (4.1)

    where A,Q f are present as in RPBVP (3.1), U:IRN is a control input, F:I×RN2RN{} is a multifunction of observation data, and d:I×RN2RN{} is a multivalued disturbance function. The hypotheses on F and d are given as follows:

    H(F):F:I×RN2RN{} is a multivalued mapping with closed convex value such that

    (i) (t,w)F(t,w) is graph measurable for every (t,w)I×RN;

    (ii) for almost all tI, wF(t,w) has a closed graph;

    (iii) for every wRN and all tI, there exists a nonnegative function λ1L[0,b] such that

    |F|=sup{f;fF}λ1(t),

    with λ1<14Mλ.

    H(d)d:I×RN2RN{} is a multivalued mapping with closed convex value such that

    (i) xRN,td(t,x) is measurable;

    (ii) tI,xd(t,x) is upper semicontinuity;

    (iii) for all xRN and tI,|d(t,x)|14Mλ.

    Theorem 4.1. If the assumptions H(A),H(f), H(F) and H(d) are satisfied, then the problem (4.1) admits at least one solution xC([0,b];RN).

    Proof. First, introduce a closed convex subset K in L(I;RN) defined by

    K:={uL(I;RN);uMλ2}.

    According to Theorem 3.1, it is straightforward to deduce that the following equation

    {CDαx(t)f(t,x(t),x[2]+(t))+Ax(t)=g(t),tI,x(b)=Qx(0), (4.2)

    has a unique solution xgC([0,b];RN) for each gK. Define an operator

    L:D(L)C([0,b];RN)L([0,b];RN),

    by

    Lx=Dαxf(t,x(t),x[2]+(t))+Ax,xD(L), (4.3)

    where D(L):={xC([0,b];RN),x(b)=Qx(0)}. Since L:D(L)K(L([0,T];RN)) is a one-to-one mapping, then it holds that L1:KD(L) exists. Now, we show that the operator

    L1:KD(L)

    is completely continuous. For this, we will claim that L1:KD(L) is continuous. Assume gmg in K as m, it remains to show that xm=L1(gm)x=L1(g) in D(L)(C([0,b];RN)). Replace x with xm in (4.2), then subtract (4.2) to get

    CDα(xm(t)x(t))+A(xm(t)x(t))=gm(t)g(t)+f(t,xm(t),x[2]m+(t))f(t,x(t),x[2]+(t)).

    Taking the inner product with xmx on the both side of above equation and using Lemma 2.2, implies

    12CDαxmx2xm(t)x(t),CDα(xm(t)x(t))x1(t)x2(t),f(t,x1(t),x[2]1+(t))f(t,x2(t),x[2]2+(t))xm(t)x(t),A(xm(t)x(t))xm(t)x(t),gm(t)g(t). (4.4)

    Now integrate in time, invoking Proposition 2.1, to derive

    12xmx21Γ(α)t0(tτ)α1xm(τ)x(τ),f(t,xm(τ),x[2]m+(τ))f(t,x(τ),x[2]+(τ)dτ1Γ(α)t0(tτ)α1xm(τ)x(τ),A(xm(τ)x(τ))dτ1Γ(α)t0(tτ)α1xm(τ)x(τ),gm(τ)g(τ)dτ+12xm(0)x(0)2. (4.5)

    Analogous the priori estimate of the solution to those of Theorem 3.1, one can find that xmCb, which with xmC([0,b];RN) and Arzela-Ascoli theorem together, implies that there exists a subsequence xm (still denoted by itself) such that xmˆx in D(L) as m. Taking the limit in (4.5), this allow us to get

    12ˆxx2ˆx(0)x(0)21Γ(α)t0(tτ)α1ˆx(τ)x(τ),A(ˆx(τ)x(τ))dτ+1Γ(α)t0(tτ)α1ˆx(τ)x(τ),f(τ,ˆx(τ),ˆx[2]+(τ))f(τ,x(τ),x[2]+(τ))dτ. (4.6)

    Analogous analysis to (3.7), set Y=ˆxx2, then it follows from (4.6) that

    YY(0)+1Γ(α)t0(tτ)α12(μ(τ)c)Y(τ)dτ, (4.7)

    which together with Lemma 2.1 leads to

    Y(t)Y(0)Eα(2(μc)tα),tI. (4.8)

    Arguing as in (3.8), we can conclude that Y(t)0, i.e., ˆxx in D(L). This gives the continuity of operator L1. In light of a priori estimate of the solution, it is easy to verify that L1(K) is a bounded set in C([0,b];RN). Thanks to Arzela-Ascoli theorem, L1(K)L([0,b];RN) is relatively compact. Therefore, L1:KL([0,b];RN) is completely continuous.

    Define a multivalued Nemitsky operator N:L([0,b];RN)2L([0,b];RN) in terms of F(t,x) and d(t,x) given by

    N(x)={vL([0,b];RN);v(t)F(t,x)+d(t,x),a.e.t[0,b]}.

    Thanks to hypotheses H(F) and H(d), it results that the multivalued Nemitsky operator N() is nonempty, closed, convex value, and upper hemicontinuous (Theorem 3.2, [25]). So we can see that L1N:KL([0,T];RN) is a upper hemicontinuous multifunction with closed, convex value, and map a bounded set into a relatively compact set. Now consider the following fixed points problem

    xL1N(x). (4.9)

    For this, by using Lemma 2.4, it remains to show that the set Ω:={xL([0,b];RN):xξL1N(x),ξ(0,1)} is bounded. Let xΩ, then L(xξ)N(x), which gives

    CDαxξf(t,x(t)ξ,x[2]+(t)ξ)+Axξ=g1(t)+g2(t), (4.10)

    where g1(t)F(x,t) and g2(t)d(x,t) for all tI. Likewise as in (3.2), the Eq (4.10) can be rewritten as

    x(t)=Eα(Atα)x(0)+ξt0(tτ)α1Eα,α(A(tτ)α)f(τ,x(τ)ξ,x[2]+(τ)ξ)dτ+ξt0(tτ)α1Eα,α(A(tτ)α)(g1(τ)+g2(τ))dτ. (4.11)

    The same arguments as in (3.4) and by taking into account H(F)(iii) and H(d)(iii), it follows from (4.11) that

    xCx(0)Mα+(λ+λ1+Mλ4)ˆMαmaxtIt0(ts)α1dsx(0)Mα+MλˆMααbα. (4.12)

    Similar to the estimate x(0) of (3.4), it holds that

    x(0)MEˆMαMλbαα, (4.13)

    which with (4.12) together gives that x(t) is uniformly bounded in I. Invoking Lemma 2.4, there exists xD(L), such that xL1N(x). Obviously, x is the solution of problem (3.1). This proof is thus complete.

    Consider the fractional iterative neural network model (FINN) described as follows:

    Dαx(t)+ˆAx(t)=g(x(t),x[2]+(t))+I(t),tI, (5.1)

    where x:[0,b]RN is the vector of neuron system; ˆA=diag(k1,k2,,kN) is a constant diagonal matrix with ki>0(i=1,2,,N); g:RN×RNRN represents the neuron input-output continuous activation function satisfying the following assumptions:

    (i) For any u,vRN, there exists a nonnegative function ˆλL[0,b] with ˆλMλ2, such that g(u,v)ˆλ(t),t[0,b];

    (ii) For any u1,u2,v1,v2RN, there exists a nonnegative function ˆμL[0,b], such that

    g(u1,v1)g(u2,v2),u1u2ˆμ(t)u1u22,

    where ˆμ<min{ki:i=1,2,,N}; the mapping of neuron inputs I:[0,b]RN is continuous with IC12Mλ.

    The initial value problem of this system (5.1) without iteration was studied in [16], where the existence and uniqueness of equilibrium point was established. Here however considering the iterative term and the rotating periodic boundary value condition, we guarantee the existence of a unique rotational periodic boundary value solution to system (5.1) by using our results. It is easy to check that all assumptions of Theorem 3.1 holds, so the following result for system (5.1) is present.

    Theorem 5.1. Under the above assumptions, the problem (5.1) has a unique rotational periodic boundary value solution.

    It should be pointed out that the system (5.1) without iteration was examined in Song et al. [16] where input function I(t) is continuous. Naturally, a question is whether the system (5.1) has a solution if I(t)=(I1(t),,IN(t)) is discontinuous. The following work is to answer this question. For this, we further hypothesize that IjΦ,(j=1,2,,N) are nondecreasing monotone bounded, where Φ:RR represents the class of functions which have at most finite jumping discontinuities in every closed interval. If there are only isolated jump discontinuities for any Ij(j=1,2,,N), then we deduce

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

    where Ij_Ij¯Ij,Ij_=lim_εtjIj(ε),¯Ij=¯limεtjIj(ε)(j=1,2,,N). Hence, in this way, the problem (5.1) can be rewritten as the following differential inclusion:

    Dαx(t)+ˆAx(t)g(x(t),x[2]+(t))+R(I(t)). (5.2)

    Here R(I(t)) can be treated as a multivalued disturbance item of problem (4.1). Then similar to the argument of theorem 4.1, we can conclude the following theorem.

    Theorem 5.2. Under the given assumptions, then the solution set of problem (5.2) is nonempty.

    The rotational periodic problems of some fractional iterative systems in the sense of Caputo fractional derivative are investigated in this paper. First we use the Leray-Schauder fixed point theorem and topological degree theory to establish the existence and uniqueness of solution for a fractional iterative equation with one sided-Lipschtiz condition on nonlinear term. Furthermore, applying set-valued theory, the well posedness of a nonlinear control system with iteration term and a multivalued disturbance is completed. Finally, to reflect the application of fractional iterative systems, the existence of solutions for a iterative neural network system is demonstrated. Our future concerns are to examine the stability for these fractional iterative systems which is still an open problem.

    This work were partially supported by Natural Science Foundation of Liaoning Province and of Jilin Province (No. 2020-MS-290, 20200201274JC), Liaoning Natural Fund Guidance Plan (No. 2019-ZD-0508) and Young Science and Technology Talents "Nursery Seedling" Project of Liaoning Provincial Department of Education (No. LQ2019008). Authors are grateful to referees for their constructive comments on the first version of our paper.

    The authors declare that there are no conflict of interest.



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