Research article Special Issues

Solutions and anti-periodic solutions for impulsive differential equations and inclusions containing Atangana-Baleanu fractional derivative of order ζ(1,2) in infinite dimensional Banach spaces

  • In this paper, we improved recent results on the existence of solutions for nonlinear fractional boundary value problems containing the Atangana-Baleanu fractional derivative of order ζ(1,2). We also derived the exact relations between these fractional boundary value problems and the corresponding fractional integral equations in infinite dimensional Banach spaces. We showed that the continuity assumption on the nonlinear term of these equations is insufficient, give the derived expression for the solution, and present two results about the existence and uniqueness of the solution. We examined the case of impulsive impact and provide some sufficiency conditions for the existence and uniqueness of the solution in these cases. We also demonstrated the existence and uniqueness of anti-periodic solution for the studied problems and considered the problem when the right-hand side was a multivalued function. Examples were given to illustrate the obtained results.

    Citation: Muneerah Al Nuwairan, Ahmed Gamal Ibrahim. Solutions and anti-periodic solutions for impulsive differential equations and inclusions containing Atangana-Baleanu fractional derivative of order ζ(1,2) in infinite dimensional Banach spaces[J]. AIMS Mathematics, 2024, 9(4): 10386-10415. doi: 10.3934/math.2024508

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  • In this paper, we improved recent results on the existence of solutions for nonlinear fractional boundary value problems containing the Atangana-Baleanu fractional derivative of order ζ(1,2). We also derived the exact relations between these fractional boundary value problems and the corresponding fractional integral equations in infinite dimensional Banach spaces. We showed that the continuity assumption on the nonlinear term of these equations is insufficient, give the derived expression for the solution, and present two results about the existence and uniqueness of the solution. We examined the case of impulsive impact and provide some sufficiency conditions for the existence and uniqueness of the solution in these cases. We also demonstrated the existence and uniqueness of anti-periodic solution for the studied problems and considered the problem when the right-hand side was a multivalued function. Examples were given to illustrate the obtained results.



    It has been recognized that the dynamics of complex real-world problems are better described using fractional calculus. Fractional calculus has many applications in engineering [2,3,4,5,6,7], in environmental, and biological studies [8,9,10,11,12]. As an extension to Newtonian derivatives, researchers have proposed different concepts of fractional derivatives and integrals, each of which generalizes the concept of differentiation and integration of integer order. The best known fractional operators are those of Riemann-Liouville and Caputo. These operators use a singular kernel. The problems arising from the presence of singular kernel were overcome by introducing fractional operators with non singular kernels. Caputo et al. [13] proposed a definition based on the exponential function. Atangana and Baleanu [14] generalized the Caputo fractional operators using kernels based on the Mittag-Leffler function.

    Although Atangana and Baleanu's derivative is not the left inverse of the corresponding Atangana and Baleanu's integral (Lemma 1 and Remark 2 below), there are many applications of Atangana and Baleanu's fractional derivative to differential equations [15,16,17,18,19]. Many researchers obtained results regarding the existence of solutions for fractional differential equations and inclusions involving Atangana and Baleanu derivative in finite dimensional spaces [20,21,22,23,24]. Recently, Al Nuwairan et al. [25] investigated the existence of solutions for non-local impulsive differential equations and inclusions with Atangana and Baleanu derivative of order ζ(0,1) in infinite dimensional spaces.

    Impulsive differential equations and impulsive differential inclusions have been an object of interest with wide applications to physics, biology, engineering, medicine, industry, and technology. The impulsive differential equations provide appropriate models for processes that change their state rapidly and cannot be modeled using the ordinary differential equations. An example of such a process is the motion of an elastic ball bouncing vertically on a surface. The moments of the impulses are the times when the ball touches the surface and rapidly changes its velocity. For some applications of impulsive differential equations, we see [27]. Xu et al. [28] studied the exponential stability of stochastic nonlinear delay systems subject to multiple periodic impulses. For further results on the existence of solutions or mild solutions for impulsive differential equations and inclusions, we refer to [29,30,31,32,33].

    Kaslik et al. [34] showed that unlike the integer order derivative, the fractional-order derivative of a periodic function cannot be a function with the same period. This implies the non-existence of periodic solutions for a wide class of fractional-order differential systems on bounded intervals. Thus, much attention has been devoted to the study of anti-periodic solutions or S-asymptotically w-periodic solution. Fractional differential equations with anti-periodic conditions have been applied to the study of blood flow, chemical engineering, underground water flow, and population dynamics. The anti-periodic solutions to various fractional differential equations and inclusions are investigated by several authors [36,37,38,39,40] and papers cited therein. Very recently, Abdeljawad et al. [41] proposed a higher-order extension of Atangana–Baleanu fractional operators. For more recent results on fractional differential equations, we refer the reader to [42,43,44].

    Notation 1.1. Throughout this paper, we use the following notation:

    ● For b>0, let J=[0,b]R. Let m be a natural number, 0km,Nk={k,k+1,,m},0=ι0<ι1≤<ι2ι3<ιm+1=b be a partition of J, J0=[0,ι1], and Jk=(ιk,ιk+1],kN1.

    E is a reflexive real Banach space, z0,z1 are elements of E.

    AC(J,E) is the Banach space of absolutely continuous functions from J to E.

    H1((a,b),E) is the Sobolev space {zL2((a,b),E):zL2((a,b),E)}.

    PC(J,E) is the Banach space defined as

    PC(J,E)={z:JE,zH1(Jk,E):z(ι+k)andz(ιk)exist withz(ιk)=z(ιk)},kN1}.

    The norm on PC(J,E) is given by ||z||PC(J,E)=sup{||z(ι)||:ιJ}.

    PCH1(J,E)={zPC(J,E):z|JkH1((ιk,ιk+1),E),kN1}.

    PCH2(J,E)={zPC(J,E):z|JkH1((ιk,ιk+1),E),kN1}. The spaces PCH1(J,E) and PCH2(J,E) are Banach spaces endowed with the norms

    ||z||PCHt(J,E)=max{||z|Jk||Hs(Jk,E):kN1}, t=1,2.

    Recently, it was shown in [20,21,23] that the following fractional differential equation:

    {ABCDζ0,ιz(ι)=w(ι), ιJ,z(0)=z0,z(b)=z1 (1.1)

    is equivalent to the fractional integral equation:

    z(ι)=z0+ι(z1z0)bι(2ζ)bM(ζ1)b0w(s)dsι(ζ1)bM(ζ1)Γ(ζ)b0(bs)ζ1w(s)ds+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds, (1.2)

    where ζ(1,2) and ABCDζ0,ι is the Atangana-Baleanu fractional derivative in the Caputo sense of order ζ with lower limit at 0,w:JR is continuous function satisfying w(0)=0 and z0,z1 are fixed points. We claim that the assumption of continuity of w is not enough as it does not assure that the function z in Eq (1.2) satisfies zH1((0,b)). Thus, it does not guarantee that z has Atangana-Baleanu fractional derivative of order ζ. Without differentiability, z would not be a solution for Eq (1.1).

    In this paper, we provide

    (1) A more precise result regarding the relation between the fractional differential equation (1.1) and the fractional integral equation (1.2) in a real Banach space E (Lemma 3.1).

    (2) Two results (Theorems 3.1 and 3.2) concerning the existence and uniqueness of solutions for the following boundary value problem containing Atangana-Baleanu fractional derivative

    {ABCDζ0,ιz(ι)=f(ι,z(ι)), ιJ,1<ζ<2,z(0)=z0,z(b)=z1, (1.3)

    where f(0,z(0))=0.

    (3) A formula (given in Lemma 4.1) for the relation between the boundary value problem

    {ABCDζ0,ιz(ι)=w(ι), ιJ,z(a)=z0,z(a)=z1

    and the integral equation

    z(ι)=z0+(ιa)[z12ζM(ζ1)w(a)ζ1M(ζ1)Γ(ζ1)a0(as)ζ2w(s)ds]2ζM(ζ1)a0w(s)dsζ1M(ζ1)Γ(ζ)a0(as)ζ1w(s)ds+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds,   ιJ.

    (4) A formula for the solutions to the following impulsive boundary value problem involving Atangana-Baleanu fractional derivative of order ζ(1,2):

    {ABCDζ0,ιu(ι)=f(ι,z(ι)),ιJ{ι1,ι2,,ιm}, z(0)=z0, z(0)=z1,z(ι+i)=z(ιi)+Ii(z(ιi)), iN1,z(ι+i)=z(ιi)+¯Ii(z(ιi)), iN1, (1.4)

    where f(0,z(0))=0, and Ii,¯Ii:EE are continuous functions (Lemma 4.2). We also establish two results concerning the existence and uniqueness of the solution of (1.4) (Theorems 4.1 and 4.2).

    (5) The sufficient conditions for the existence of anti-periodic solution to the following impulsive differential equation involving Atangana-Baleanu fractional derivative of order ζ(1,2)

    {ABCDζ0,ιz(ι)=f(ι,z(ι)),ιJ{ι1,ι2,,ιm}, z(0)=z(b), z(0)=z(b),z(ι+i)=z(ιi)+Ii(z(ιi)), iN1,z(ι+i)=z(ιi)+¯Ii(z(ιi)), iN1, (1.5)

    where f(0,z(0))=0, (Theorem 5.1).

    (6) The sufficient conditions for the existence of solutions to the impulsive differential inclusion

    {ABCDζ0,ιz(ι)F(ι,z(ι)),ιJ{ι1,ι2,,ιm}, z(0)=z0, z(0)=z1,z(ι+i)=z(ιi)+Ii(z(ιi)), iN1,z(ι+i)=z(ιi)+¯Ii(z(ιi)), iN1, (1.6)

    where F is a multi-valued function satisfying F(0,z0)={0} (Theorem 6.1).

    Remark 1.1. Previously, the authors in [29] had investigated problems (1.3) and (1.4) with the Atangana-Belearn derivative replaced with Caputo's. Also in [29,40] problems (1.5) and (1.6) were studied using Caputo derivative without impulses. Saha et al. [42] established the existence of solutions for problem (1.1) in finite dimensional spaces with the boundary conditions z(0)=z0,ABCD0,ιz(b)=z1. Indeed, the vast majority of published research on the existence of solutions to differential equations involving Atangana-Baleanu fractional derivative are restricted to finite-dimensional spaces [20,21,22,23,24,45]. Up to the authors knowledge, there has been no published research on anti-periodic solutions.

    The contribution of this paper can be summarized as follows:

    (1) In Lemma 3, we obtained a precise relationship between the fractional differential Equation (1.1) and the corresponding integral Equation (1.2). We showed in detail that the continuity assumption on the nonlinear term, used earlier, e.g., Theorem 3.6 in [21] and Lemma 2 in [23], is insufficient and should be replaced with the requirement that w lies in the space H1((a,b),E).

    (2) As to our knowledge, Theorem 5.1 showing the existence of an anti-periodic solution for the impulsive fractional differential equation (1.5), with Attange-Baleanu fractional derivative of order ζ(1,2), has not previously appeared in literature.

    (3) To our knowledge, there has been no published results on the existence of solutions for impulsive differential equations containing Atangana-Baleanu fractional derivative of order ζ(1,2), or on the existence of anti-periodic solutions for differential equations containing Atangana-Baleanu fractional derivative.

    The paper is organized as follows. In the second section, we recall the basic facts and concepts needed for the following sections. In Section 3, we present two existence and uniqueness results for the solution to problem (1.3). Section 4 studies the existence and uniqueness of solutions to problem (1.4), and Section 5 is devoted to showing the existence of solutions to problem (1.5). In Section 6, we prove the existence of solutions for problem (1.6). Three examples are given in the last section to illustrate the obtained results.

    Definition 2.1. [14,19] Let a<b be two real numbers, and ζ(0,1). The Atangana-Baleanu fractional derivative for a function zH1((a,b),E) in the Caputo sense and in the Riemann-Liouville sense of order ζ with lower limit at a are defined by

    ABCDζa,ιz(ι)=M(ζ)1ζιaz(x)Eζ(ζ(ιx)ζ1ζ)dx,   ιJ,

    and

    ABRDζa,ιz(ι)=M(ζ)1ζ ddιιaz(x)Eζ(ζ(ιx)ζ1ζ)dx,  ιJ,

    where M(ζ)>0 is a normalized function satisfying M(0)=M(1)=1, and Eζ=Eζ,1 is the Mittag-Leffler function given by:

    Eζ,β(μ)=k=0μkΓ(ζk+β),  βR, μC.

    Definition 2.2. [14,19] Let a<b be two real numbers, and ζ(0,1). The Atangana-Baleanu fractional integral for a function zH1((a,b),E) of order ζ with lower limit at a is given by

    ABIζa,ιz(ι)=1ζM(ζ)z(ι)+ζM(ζ)Γ(ζ)ιaz(x)(ιx)ζ1dx, ιJ.

    The following lemma was proved in [14,19] for E=R. It can be generalized to a Banach space E with little changes in the proof.

    Lemma 2.1. Let zH1((a,b),E), ζ(0,1) and ιJ.

    i. ABRDζa,ι(ABIζa,ιz(ι))=z(ι) and ABIζa,ι(ABRIζa,ιz(ι))=z(ι).

    ii. ABCDζa,ι(ABIζa,ιz(ι))=z(ι)z(a)Eζ(ζ(ιa)ζ1ζ).

    iii. ABCIζa,ι(ABCIζa,ιz(ι))=z(ι)z(a).

    iv. ABRDζa,ιz(ι)=ABCDζ0,ιz(ι)+M(ζ)1ζz(a)Eζ(ζ(ιa)ζ1ζ).

    v. ABRDζa,ιc=cEζ(ζ1ζ(ιa)ζ),ABCDζa,ιc=0, for a constant c.

    Remark 2.1. Note that the second assertion of Lemma 2.1 implies that ABCDζa,ι(ABIζa,ιz(ι))z(ι), unless z(a)=0. Thus, we can not drop the assumption that f(0,z(0))=0 in problems (1.3)–(1.5) and that F(0,z0)=0 in problem (1.6).

    Definition 2.3. [14,19] Let ζ(n,n+1),nN and z:[a,b]E  with z(n)H1((a,b),E). The left Atangana-Baleanu fractional derivative of z, in the Caputo sense and in the Riemann-Liouville sense of order ζ with lower limit at a are defined by

    ABCDζa,ιz(ι)=ABCDζna,ιz(n)(ι)=M(ζ1)1(ζn)ιaz(n+1)(x)E(ζn)((ζn)(ιx)(ζn)1(ζn))dx,

    and

    ABRDζa,ιz(ι)=ABRDζna,ιz(n)(ι)=M(ζn)1(ζn)ddιιaz(n)(x)E(ζn)((ζn)(ιx)(ζn)1(ζn))dx.

    Definition 2.4. [14,19] Let ζ(n,n+1),nN and z:[a,b]E with z(n)H1((a,b),E). The left Atangana-Baleanu fractional integral for z, of order ζ with lower limit at a, is defined by

    ABIζa,ιz(ι)=Ina,ιABIζna,ιz(ι).

    As in [20,22], one can prove the following lemma.

    Lemma 2.2. Let ζ(1,2) and z:JE with zH1((a,b),E). For any ι[a,b],

    (1) ABRDζa,ι(ABIζa,ιz(ι))=z(ι).

    (2) ABCDζa,ι(ABIζa,ιz(ι))=ABCDζ1a,ι(ddι(I(ABIζ10,ιz(ι))))=ABCDζ1a,ι(ABIζ10,ιz(ι))=z(ι)z(a)Eζ1((ζ1)(ιa)ζ12ζ).

    (3) ABIζa,ι(ABCDζa,ιz(ι))=z(ι)c0c1(ιa).

    We end this section by listing some assumptions that are used later.

    Assumptions 2.1. Let f:J×EE be a function, we assume the following:

    - (A1): For any δ>0 there is Lδ >0 such that for any x,yE with ||x||δ, ||y||δ and any s,ιJ, we have

    ||f(ι,x)f(s,y)|||sι|+Lδ ||xy||.

    - (A2): There is σ>0 such that for any x,yE, we have

    ||f(ι,x)f(ι,y)||σ||xy||,ιJ.

    - (A3): For every iN1, the functions Ii,¯Ii:EE are continuous, compact and there exist positive constants hi¯hi (i=1,2,..,m) such that

    Ii(x)hix,xE.and¯Ii(x)¯hix,xE. (2.1)

    - (A4): For every iN1, there exists positive constants δiηi, such that

    Ii(x)Ii(y)δixy,xE, (2.2)

    and

    ¯Ii(x)¯Ii(y)ηixy,xE. (2.3)

    In this section, we stat and prove the relationship between the fractional differential Equation (1.1) and the fractional integral Equation (1.2) in a reflexive Banach space E.

    Lemma 3.1. Let ζ(1,2).

    (1) If w:JE is continuous and z:JE is a solution to Eq (1.1), then z satisfies the integral equation (1.2).

    (2) If wH1((0,b),E) with w(0)=0 and z satisfies Eq (1.2), then zH1((0,b),E) and z is a solution to Eq (1.1).

    Proof.

    (1) By applying ABIζ0,ι to both sides of Eq (1.1) and using the definition of ABIζ0,ι, the third assertion of Lemma 2.2, and Definition (2.4), we obtain that for any ι[0,b]

    z(ι)=c0+ιc1+ABIζ0,ιw(ι)=c0+ιc1+I0,ι( ABIζ10,ιw(ι))=c0+ιc1+I0,ι[1(ζ1)M(ζ1)w(ι)+ζ1M(ζ1)Iζ10,ιw(ι)]=c0+ιc1+ι02ζM(ζ1)w(s)ds+ζ1M(ζ1)Iζ0,ιw(ι)=c0+ιc1+ι02ζM(ζ1)w(s)ds+ζ1M(ζ1)Γ(ζ)ι0w(s)(ιs)ζ1ds. (3.1)

    From the boundary conditions z(0)=z0 and z(b)=z1, it follows that c0=z0 and

    z1=z0+bc1+b02ζM(ζ1)w(s)ds+ζ1M(ζ1)Γ(ζ)b0w(s)(bs)ζ1ds,

    i.e.,

    c1=z1bz0bb02ζbM(ζ1)w(s)dsζ1bM(ζ1)Γ(ζ)b0w(s)(bs)ζ1ds. (3.2)

    Substituting the values of c0 and c1 into (3.1), we obtain

    z(ι)=ιz1+z0(bι)bι(2ζ)bM(ζ1)b0w(s)dsι(ζ1)bM(ζ1)Γ(ζ)b0w(s)(bs)ζ1ds.+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0w(s)(ιs)ζ1ds.

    (2) Assume that wH1((0,b),E) with w(0)=0, and that Eq (1.2) holds. Clearly z(0)=z0 and z(b)=z1. Moreover,

    z(ι)=c0+ιc1+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0w(s)(ιs)ζ1ds, (3.3)

    where c0=z0 and c1 is given by (3.2). Since ζ>1, Eq (3.3) gives us that

    z(ι)=c1+2ζM(ζ1)w(ι)+ζ1M(ζ1)I ζ10,ιw(ι), for   a.e.  ιJ, (3.4)

    where I ζ10,ι is the Riemann-Liouville fractional integral of order ζ1. Since wH1(J,E), ζ1(0,1), and E is reflexive, w has a Bochner integrable derivative w almost everywhere, and

    w(s)=w(0)+s0w(x)dx,  sw.

    This implies that

    I ζ10,ιw(ι)=1Γ(ζ1)ι0(ιs)ζ2w(s)ds=1Γ(ζ1)ι0(ιs)ζ2[s0w(x)dx]ds,

    i.e., I ζ10,ιw(ι) is the primitive of a Bochner integrable function, hence is absolutely continuous. Thus Eq (3.4) is valid for every ιJ. Moreover,

    z(2)(ι)=2ζM(ζ1)w(ι)+ζ1M(ζ1)ddι(I ζ1w(ι)),

    giving us that zH1((0,b),E). Equation (3.2) implies

    z(ι)=c0+ιc1+ABIζ0,ιw(ι), ιJ.

    Finally, by the second assertion of Lemma 2.2,

    ABCDζ0,ιz(ι)=ABCDζ0,ι ABIζ0,ιw(ι)=w(ι)w(0)Eζ1((ζ1)ιζ12ζ)=w(ι), ιJ.

    Remark 3.1. Note that

    (1) The first assertion of Lemma 3.1 has been proved in Lemma 2 in [23] for the case where E=R.

    (2) The solution formula of problem (1.1) does not follow from the first assertion of Lemma 3.1, nor from Lemma 2 in [23].

    (3) The assumption w(0)=0 cannot be omitted in the second assertion of Lemma 3.1 since

    ABCDζ0,ι ABIζ0,ιw(ι)=w(ι)w(0)Eζ1((ζ1)ιζ12ζ)w(ι).

    (4) If w is continuous and not in H1((0,b),E), then Eq (3.4) does not imply the existence of z(2). Therefore, without the assumption wH1((0,b),E), there is no guarantee that ABCDζ0,ιz(ι) exists.

    (5) Lemma 3.1 gives a more accurate statement of Lemma 2 in [23] and generalizes it to the infinite dimensional case.

    The results in Lemma 3.1 can be summarized as follows.

    Lemma 3.2. Let wH1((0,b),E) with w(0)=0. A function z:JE is a solution of problem (1.1) if and only if

    z(ι)=z0+ι(z1z0)bι(2ζ)bM(ζ1)b0w(s)dsι(ζ1)bM(ζ1)Γ(ζ)b0(bs)ζ1w(s)ds+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds. (3.5)

    Theorem 3.1. Let f:J×EE be a function. If (A1) holds, then problem $ (1.3) has a unique solution provided that f(0,z0)=0 and there is r>0 such that

    ||z0||+||z1||+2(b+rLr+||f(0,0)||)[b(2ζ)M(ζ1)+(ζ1)bζM(ζ1)Γ(ζ)]<r. (3.6)

    Proof. Define T:C(J,E)C(J,E) by

    T(z)(ι)=z0+ι(z1z0)bι(2ζ)bM(ζ1)b0f(s,z(s))dsι(ζ1)bM(ζ1)Γ(ζ)b0(bs)ζ1f(s,z(s))ds+2ζM(ζ1)ι0f(s,z(s))ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1f(s,z(s))ds. (3.7)

    Using the Schauder fixed point theorem, we will show that T has a unique fixed point. Set B0={zC(J,E):zC(J,E)r}.

    ● Step 1: T(B0)B0. Let zB0. It follows that from (A1) 

    ||f(ι,z(ι))||||f(ι,z(ι))f(0,0)||+||f(0,0)||b+Lr||z(ι)||+||f(0,0)||b+rLr+||f(0,0)||,  ιJ. (3.8)

    From (3.6)–(3.8), one has

    ||T(z)(ι)||||z0(1ιb)+ιbz1||+2(b+rLr+||f(0,0)||)[b(2ζ)M(ζ1)+(ζ1)bζM(ζ1)Γ(ζ)]||z0||+||z1||+2(b+rLr+||f(0,0)||)[b(2ζ)M(ζ1)+(ζ1)bζM(ζ1)Γ(ζ)]<r,

    showing that T(B0)B0.

    ● Step 2: T(B0) is equicontinuous. Let zB0 and ι,ι+λJ. Using (3.7), we obtain

    T(z)(ι+λ)T(z)(ι)λ(z1z0)b+λ(2ζ)(b+rLr+||f(0,0)||)M(ζ1)+λ(ζ1)(b+rLr+||f(0,0)||)bζζM(ζ1)Γ(ζ)+λ(2ζ)(b+rLr+||f(0,0)||)M(ζ1)+(ζ1)(b+rLr+||f(0,0)||)M(ζ1)Γ(ζ)[ι+λ0(ι+λs)ζ1(ιs)ζ1)ds].

    Since ζ1 >0,T(z)(ι+λ)T(z)(ι)0 when λ0, independently of z, proving the assertion.

    ● Step 3: For n1, let Bn=¯convT(Bn1), and B=n0Bn.

    Let B,Bn be as defined above, then the set B is a non empty compact subset of C(J,E). It follows from Step 1, that BnBn1, n1. By Cantor intersection property [47], it is enough to show that

    limnχC(J,E)(Bn)=0, (3.9)

    where χC(J,E) is the Hausdorff measure of noncompactness on C(J,E) [48].

    Let n1 be a fixed natural number and ε>0. By Lemma 3 in [49], there exists a sequence (zk), k1 in Bn1 such that

    χC(J,E)(Bn)=χC(J,E)T(Bn1)2χC(J,E){T(zk):k1}+ε. (3.10)

    Since Bn is equicontinuous, inequality (3.10) becomes

    χC(J,E)(Bn)2maxι JχE{T(zk)(ι):k1}+ε. (3.11)

    Let ιJ be fixed. In view of (3.8)

    ||f(ι,zm(ι))f(ι,zn(ι))||Lr ||zm(ι)zn(ι)||,n,mN.

    It follows that

    χE{f(ι,zk(ι)):k1}LrχE{zk(ι):k1}. (3.12)

    We also have that

    T(zk)(ι)=z0+ι(z1z0)bι(2ζ)bM(ζ1)b0f(s,zk(s))ds(ζ1)bM(ζ1)Γ(ζ)b0(bs)ζ1f(s,zk(s))ds+2ζM(ζ1)ι0f(s,zk(s))ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1f(s,zk(s))ds. (3.13)

    Since ζ>1, Eqs (3.12) and (3.13) give

    χ{T(zk)(ι):k1}b0χE{zk(s):k1}ds[2(2ζ)LrM(ζ1)+2bζ1(ζ1)LrM(ζ1)Γ(ζ)]b[2(2ζ)LrM(ζ1)+2bζ1(ζ1)LrM(ζ1)Γ(ζ)]χC(J,E)(Bn1). (3.14)

    Using (3.11) and (3.14), we obtain that

    χC(J,E)(Bn)4bLr[2ζM(ζ1)+bζ1(ζ1)M(ζ1)Γ(ζ)]χC(J,E)(Bn1),nN.

    This inequality yields that

    χC(J,E)(Bn)χC(T,E)(B0)4bLr[2ζM(ζ1)+bζ1(ζ1)M(ζ1)Γ(ζ)]n1. (3.15)

    The inequality in (3.6) implies that 4bLr[(2ζ)M(ζ1)+bζ(ζ1)M(ζ1)Γ(ζ)]<1, and thus, (3.15) implies (3.9).

    ● Step 4: The function T|B:BB is continuous. Assume that znz in B. Note that for n1 and ιJ, we have

    T(zn)(ι)=z0+ι(z1z0)bι(2ζ)bM(ζ1)b0f(s,zn(s))ds,ι(ζ1)bM(ζ1)Γ(ζ)b0(bs)ζ1f(s,zn(s))ds+2ζM(ζ1)ι0f(s,zn(s))ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1f(s,zn(s))ds.

    Using (A1),ζ>1, the inequality (3.8), and the Lebesgue dominated convergence theorem, we obtain that T(zn)T(z).

    It follows from Steps (1) to (4) and Schauder's fixed point theorem that there is zB such that z=T(z). That is,

    z(ι)=z0+ι(z1z0)bι(2ζ)bM(ζ1)b0w(s)dsι(ζ1)bM(ζ1)Γ(ζ)b0(bs)ζ1w(s)Bs+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds,

    where w(ι)=f(ι,z(ι)), ιJ.

    Next, we show that this function z is a solution for problem (1.3). By Lemma 3.1, it is sufficient to show that wH1(J,E). Since ζ>1, then

    z(t)=2ζM(ζ1)w(t)+ζ1M(ζ1)Iζ10,tw(t),tJ.

    From (A1),w is absolutely continuous, and since E is reflexive, the function tIζ10,tw(t) is absolutely continuous. Hence wH1(J,E).

    To show the uniqueness of the solution, let z,vC(J,E) be two solutions for problem (1.3) and ιJ.  Since z,v are solutions, it follows from (A1) that

    ||T(z)(ι)T(v)(ι)||(2ζ)M(ζ1)b0||f(s,z(s))f(s,v(s)))||+bζ1(ζ1)M(ζ1)Γ(ζ)b0||f(s,z(s))f(s,v(s))||ds+2ζM(ζ1)ι0||f(s,z(s))f(s,v(s))||ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1||f(s,z(s))f(s,v(s))||dsLr(2ζ)M(ζ1)b0||z(s))v(s)||ds+Lrbζ1(ζ1)M(ζ1)Γ(ζ)b0||z(s))v(s)||ds+Lr(2ζ)M(ζ1)ι0||z(s))v(s)||ds+Lr(ζ1)M(ζ1)Γ(ζ)ι0(ιs)ζ1||z(s))v(s)||ds.

    Hence,

    ||z(ι)v(ι)||Lr(2ζ)bM(ζ1)||zv||+Lrbζ(ζ1)M(ζ1)Γ(ζ)||zv||+Lr(2ζ)bM(ζ1)||zv||+Lr(ζ1)bζM(ζ1)Γ(ζ)||zv||||zv||[2Lr(2ζ)bM(ζ1)+2Lr(ζ1)bζM(ζ1)Γ(ζ)].

    Since ι is arbitrary, it follows that

    ||zv||C(J,E)||zv||C(J,E)[2Lr(2ζ)bM(ζ1)+2Lr(ζ1)bζM(ζ1)Γ(ζ)].

    Inequality (3.6) implies 2Lr(2ζ)bM(ζ1)+2Lr(ζ1)bζM(ζ1)Γ(ζ)<1, consequently, ||zv||C(J,E)=0, and z=v.

    In the following, another existence and uniqueness result for solutions of problem (1.3) is obtained. Replacing the assumption (A1) by (A2) simplifies the inequality (3.6) enabling us to use the Banach fixed point theorem for contraction mappings instead of the Schauder fixed point.

    Theorem 3.2. Let f:J×EE. If (A2) is satisfied, then problem (1.3) has a unique solution provided that f(0,z0)=0 and

    2bσ(2ζ)M(ζ1)+2bζ(ζ1)σM(ζ1)Γ(ζ)<1. (3.16)

    Proof. Consider the function  T:C(J,E)C(J,E) defined by (3.7). Let z,vC(J,E). For any ιJ,

    ||T(z)(ι)T(v)(ι)||(2ζ)M(ζ1)b0||f(s,z(s))f(s,z(s))||ds+bζ1(ζ1)M(ζ1)Γ(ζ)b0||f(s,z(s))f(s,z(s))||ds+2ζM(ζ1)ι0||f(s,z(s))f(s,z(s))||ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1||f(s,z(s))f(s,z(s))||ds.

    Since ζ>1, this inequality together with (A2) imply that

    ||T(z)(ι)T(v)(ι)||2σ(2ζ)M(ζ1)b0||z(s)v(s))||ds+2bζ1(ζ1)σM(ζ1)Γ(ζ)b0||z(s)v(s))||ds[2bσ(2ζ)M(ζ1)+2bζ(ζ1)σM(ζ1)Γ(ζ)]||zv||ds.

    Thus,

    ||T(z)T(v)||[2bσ(2ζ)M(ζ1)+2bζ(ζ1)σM(ζ1)Γ(ζ)]||zv||.

    Using (3.16), we obtain that T is contraction, and hence has a unique fixed point.

    The following lemmas will be used for deriving an existence result for solutions of problem (1.4).

    Lemma 4.1.

    (1) If w:JE is continuous ,a[0,b),z:JE be such that zH1((0,b),E) and

    {ABCD ζ0,ιz(ι)=w(ι),ιJ,z(a)=z0, z(a)=z1, (4.1)

    then for any ιJ,

    z(ι)=z0+(ιa)[z12ζM(ζ1)w(a)ζ1M(ζ1)Γ(ζ1)a0(as)ζ2w(s)ds]2ζM(ζ1)a0w(s)dsζ1M(ζ1)Γ(ζ)a0(as)ζ1w(s)ds+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds. (4.2)

    (2) If a[0,b),w:JE be continuous with w(0)=0 and z:JE are such that (4.2) holds, then zH1((0,b),E) and z is a solution for (4.1).

    Proof.

    (1) Apply ABIζ0,ι on both side of the equation ABCD ζ0,ιz(ι)=w(ι);ι[0,b]. As in the proof of first assertion of Lemma 3.1, we obtain for any ι[0,b]

    z(ι)=c0+ιc1+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds.

    Using the boundary conditions z(a)=z0,z(a)=z1, we obtain

    c0=z0ac12ζM(ζ1)a0w(s)dsζ1M(ζ1)Γ(ζ)a0(as)ζ1w(s)ds, (4.3)

    and

    z1=c1+2ζM(ζ1)w(a)+ζ1M(ζ1)Γ(ζ1)a0(as)ζ2w(s)ds.

    This gives that

    c1=z12ζM(ζ1)w(a)ζ1M(ζ1)Γ(ζ1)a0(as)ζ2w(s)ds. (4.4)

    From (4.3) and (4.4), we obtain

    c0=z0a[z12ζM(ζ1)w(a)ζ1M(ζ1)Γ(ζ1)a0(as)ζ2w(s)ds]2ζM(ζ1)a0w(s)dsζ1M(ζ1)Γ(ζ)a0(as)ζ1w(s)ds. (4.5)

    Substituting the values of c0 and c1into z(ι), we obtain

    z(ι)=z0a[z12ζM(ζ1)w(a)ζ1M(ζ1)Γ(ζ1)a0(as)ζ2w(s)ds]2ζM(ζ1)a0w(s)dsζ1M(ζ1)Γ(ζ)a0(as)ζ1w(s)ds+ι[z12ζM(ζ1)w(a)ζ1M(ζ1)Γ(ζ1)a0(as)ζ2w(s)ds]+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds=z0+(ιa)[z12ζM(ζ1)w(a)ζ1M(ζ1)Γ(ζ1)a0(as)ζ2w(s)ds]2ζM(ζ1)a0w(s)dsζ1M(ζ1)Γ(ζ)a0(as)ζ1w(s)ds+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds.

    Hence, Eq (4.2) is verified.

    (2) Suppose that w:JE be continuous function with w(a)=0 and Eq (4.2) holds. Clearly z(a)=z0 and z(a)=z1. As in the proof of second assertion of Lemma 3.1, we can show that zH1((0,b),E). For any ι[a,b], we have

    ABCDζ0,ιz(ι)=ABCDζ10,ιz(ι)=ABCDζ10,ι(z1ζ1M(ζ1)Γ(ζ1)a0(as)ζ2w(s)ds+2ζM(ζ1)w(ι)+ζ1M(ζ1)Γ(ζ1)ι0(ιs)ζ2w(s)ds)(ι)=ABCDζ10,ι(2ζM(ζ1)w(ι)+ζ1M(ζ1)Γ(ζ1)ι0(ιs)ζ2w(s)ds)(ι)=ABCDζ10,ι( ABI1ζ0,ιw(ι))=w(ι)w(0)E1ζ((1ζ)ι(1ζ)2ζ)=w(ι).

    Remark 4.1. Following the same method, used in the above proof, a generalization of Theorem 4 in [21] can be derived for any Banach space.

    Lemma 4.2. If wPCH1(J,E) with w(0)=0 and z:JE be a function satisfying

    z(ι)=z0+ιz1+ki=1Ii(z(ιi))+ki=1(ιιi)¯Ii(z(ιi))+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds, where ιJk,kN0, (4.6)

    then z PCH2(J, E) and satisfies the impulsive fractional differential equation:

    {ABCD ζ0,ιz(ι)=w(ι), ιJ{ι1,ι2,,ιm}, z(0)=z0, z(0)=z1,z(ι+i)=z(ιi)+Ii(z(ιi)),   iN1,z(ι+i)=z(ιi)+¯Ii(z(ιi)),  iN1. (4.7)

    Note that for k=0, in Eq (4.6), the sum ki=1 is an empty sum and conventionally, equals zero.

    Proof. For any ιJ0,

    z(ι)=z0+ιz1+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0w(s)(ιs)ζ1ds. (4.8)

    Clearly, z(0)=z0, z(0)=z1. Since wPCH1(J,E) and w(0)=0, it follows by the second statement of Lemma 4.1, that z is a solution for the fractional differential equation:

    {ABCD ζ0,ιz(ι)=w(ι), ιJ0, z(0)=z0, z(0)=z1.

    Let us define a function v on J1=(ι1,ι2] by:

    v(ι)=z(ι1)+I1(z(ι1))+(ιι1)[z(ι1)+¯I1(z(ι1))2ζM(ζ1)w(ι1)ζ1M(ζ1)Γ(ζ1)ι10(ι1s)ζ2w(s)ds]2ζM(ζ1)ι10w(s)dsζ1M(ζ1)Γ(ζ)ι10(ι1s)ζ1w(s)ds+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds. (4.9)

    From the second assertion of Lemma 4.1, v is a solution for the fractional differential equation:

    {ABCD ζ0,ιz(ι)=w(ι), ιJ1, z(ι+1)=z(ι1)+I1(z(ι1)),z(ι+1)=z(1)(ι1)+¯I1(z(ι1)). (4.10)

    Let ιJ1. We show that, v(ι)=z(ι). From Eq (4.8), it follows that

    z(ι1)=z0+ι1z1+2ζM(ζ1)ι10w(s)ds+ζ1M(ζ1)Γ(ζ)ι10(ι1s)ζ1w(s)ds

    and

    z(ι1)=z1+2ζM(ζ1)w(ι1)+ζ1M(ζ1)Γ(ζ1)ι10(ι1s)ζ2w(s)ds.

    By substituting the values of z(ι1) and  z(ι1) into Eq (4.9), we obtain

    v(ι)=z0+ι1z1+2ζM(ζ1)ι10w(s)ds+ζ1M(ζ1)Γ(ζ)ι10w(s)(ι1s)ζ1ds+I1(z(ι1))+(ιι1)[z1+2ζM(ζ1)w(ι1)+ζ1M(ζ1)Γ(ζ1)ι10(ι1s)ζ2w(s)ds+¯I1(z(ι1))2ζM(ζ1)w(ι1)ζ1M(ζ1)Γ(ζ1)ι10(as)ζ2w(s)ds]2ζM(ζ1)ι10w(s)dsζ1M(ζ1)Γ(ζ)ι10(as)ζ1w(s)ds+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds=z0+ιz1+I1(z(ι1))+(ιι1)¯I1(z(ι1))+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds. (4.11)

    Therefore, v(ι)=z(ι),ιJ1. Since

    z(ι+1)z(ι1)=I1(z(ι1)),  and   z(ι+1)z(ι1)=¯I1(z(ι1)),

    then z is a solution for the fractional differential equation (4.10). By repeating the above steps for Jk;kN2, the proof follows.

    Definition 4.1. A function zPCH2(J,E) is said to be a solution for problem (1.4) if it has left Atangana-Baleanu fractional derivative of order ζ on each Jk, kN1 and satisfies Eq (4.6).

    In the following theorem, we provide an existence result for problem (1.4).

    Theorem 4.1. Let f:J×EE with f(0,z0)=0 and Ii,¯Ii:EE (iN1) be functions. If both Assumptions (A1) and (A3) are satisfied, then problem (1.4) has a unique solution provided that f(0,z0)=0, and there is r>0 such that

    ||z0||+b(||z1||+rhm(1+b)+(b+rLr +||f(0,0)||)[(2ζ)bM(ζ1)+(ζ1)bζM(ζ1)Γ(ζ+1)]<r, (4.12)

    where h=max{mi=1himi=1¯hi}.

    Proof. Using Schauder's fixed point theorem, we show that the function R:PC(J,E)PC(J,E) given by

    R(z)(ι)=z0+ιz1+ki=1Ii(z(ιi))+ki=1(ιιi)¯Ii(z(ιi))+2ζM(ζ1)ι0f(s,z(s))ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1f(s,z(s))ds, where  ιJk,kN0, (4.13)

    has a fixed point. Set B0={zPC(J,E):zPC(J,E)r}. The remainder of the proof is similar to the steps used in proving Theorem (3.1), so we give it in outline.

    ● Step 1: Let zB0 and ιJk, k=0,1,2,..,m. Using (2.1), (3.8), (4.12), and (4.13), we obtain that for ιJk,k=1,2,..,m,

    ||R(z)(ι)||||z0||+b||z1||+rmh(1+b)+(b+rLr +||f(0,0)||)[(2ζ)bM(ζ1)+(ζ1)bζM(ζ1)Γ(ζ+1)]<r

    from which we deduce that R(B0)B0.

    ● Step 2: Let Z=R(B0). We claim that Z is equicontinuous on every Jk,kN0={0,1,2,..,m}. Let kN0 be fixed, zB0 and ι,ι+λJk. Using (4.13), we get

    R(z)(ι+λ)R(z)(ι)λ(||z1||+2ζM(ζ1)||f(0,z0)||)+λ(2ζ)M(ζ1)(b+rLr +||f(0,0)||)+(ζ1)(b+rLr +||f(0,0)||)M(ζ1)Γ(ζ)ι0[(ι+λs)ζ1(ιs)ζ1]ds.

    Since ζ1 >0, we have R(z)(ι+λ)R(z)(ι)0 \ as λ0,\ independently of z.

    ● Step 3: We show that B=n1Bn is non-empty and compact in PC(J,E), where Bn=¯conv(R(Bn1)),n1. By Step 1, it follows that Bn,n1 is a decreasing sequence of non-empty, closed convex and bounded subsets of PC(J,E), and hence it is sufficient to show that

    limnχPC(J,E)(Bn)=0, (4.14)

    where χPC(J,E) is the Hausdorff measure of noncompactness on PC(J,E).

    Let n1 be a fixed natural number and ε>0. In view of Lemma 3 in [49], there exists a sequence (zk),k1 in Bn1 such that

    χPC(J,E)(Bn)=χPC(J,E)R(Bn1)2χPC(J,E){R(zk):k1}+ε=2maxi=0,1,...,m χi{R(zk)|¯Ji:k1}+ε,

    where χi is the Hausdorff measure of noncompactness on C(¯Ji,E). Since R(Bn1) is equicontinuous, the above inequality becomes

    χPC(J,E)(Bn) 2maxi=0,1,...,msupι¯Jiχ{R(zk)(ι):k1}+ε, (4.15)

    where χ is the the Hausdorff measure of noncompactness on E. Since Ii,¯Ii,i=0,..,m, are compact, we have

    mi=1χ{Ii(zk(ιi)):k1}=mi=1χ{(ιιi)(¯Ii(zk(ιi)):k1}=0.

    Thus, as in (3.12)

    χ{R(zk)(ι):k1}χC(J,E)(Bn1)Lr(2ζM(ζ1)+(ζ1)bζM(ζ1)Γ(ζ)),

    from which,

    χPC(J,E)(Bn)χPC(J,E)(B0)[Lr(2ζM(ζ1)+(ζ1)bζM(ζ1)Γ(ζ))]n1.

    Inequality (4.12) insures that Lr(2ζM(ζ1)+(ζ1)bζM(ζ1)Γ(ζ))<1, and Eq (4.14) follows.

    ● Step 4: The function R|B:BB is continuous. Let znz in B and yn=R(zn). The proof follows from the continuity of both Ii,¯Iii=0,1,2,..,m, by following the same arguments in Step 4 of the proof of Theorem (3.1).

    As a result of Steps (1) to (4) and Schauder's fixed point theorem, there is zBPC(J,E) such that z=R(z).

    To show the uniqueness of the solution, let z and v be two solutions for problem (1.4). For ιJ0, we have

    ||z(ι)v(ι)||Lr(2ζ)bM(ζ1)supsJ0||z(s)v(s)||+Lrbζ(ζ1)M(ζ1)Γ(ζ)supsJ0||z(s)v(s)||supsJ0||z(s)v(s)||[Lr(2ζ)bM(ζ1)+Lr(ζ1)bζM(ζ1)Γ(ζ)].

    Thus,

    supsJ0||z(s)v(s)||supsJ0||z(s)v(s)||[Lr(2ζ)bM(ζ1)+Lr(ζ1)bζM(ζ1)Γ(ζ)].

    The inequality (4.12) gives

    Lr(2ζ)bM(ζ1)+Lr(ζ1)bζM(ζ1)Γ(ζ)<1.

    Thus, supsJ0||z(s)v(s)||=0, and hence z(s)=v(s),sJ0.

    Assume that ιJ1. Because z(ι1)=v(ι1), it yields that,

    ||z(ι)v(ι)||||I1(z(ι1))I1(v(ι1))||+(ιι1)||¯I1(z(ι1))¯I1(v(ι1))||+Lr(2ζ)bM(ζ1)supsJ0||z(s)v(s)||+Lrbζ(ζ1)M(ζ1)Γ(ζ)supsJ0||z(s)v(s)||=Lr(2ζ)bM(ζ1)supsJ0||z(s)v(s)||+Lrbζ(ζ1)M(ζ1)Γ(ζ)supsJ0||z(s)v(s)||supsJ0||z(s)v(s)||[Lr(2ζ)bM(ζ1)+Lr(ζ1)bζM(ζ1)Γ(ζ)].

    As above, we obtain that z(ι)=v(ι), ιJ1. By continuing in the same manner, we show that z=v.

    Next, we show that replacing the Assumptions (A1), and (A3) in Theorem 4.1 by (A2), and (A4) simplifies (4.12). In fact this enable us to apply Banach fixed point theorem for contraction mappings instead of Schauder fixed point.

    Theorem 4.2. Let f:J×EE such that f(0,z0)=0 and Ii, ¯Ii:EE\ (iN1) be functions. If Assumptions (A2) and (A4) are satisfied, then problem (1.4) has a unique solution provided that

    mi=1(δi+bηi)+σ(2ζ)bM(ζ1)+σ(ζ1)bζM(ζ1)Γ(ζ+1)<1. (4.16)

    Proof. Let R:PC(J,E)PC(J,E), be function given by Eq (4.13), and z,vPC(J,E). For each ιJk;kN1, we have

    ||R(z)(ι)R(v)(ι)||[mi=1δi+bηi)+σ(2ζ)bM(ζ1)+σ(ζ1)bζM(ζ1)Γ(ζ+1)]||zv||PC(J,E).

    Thus, R is contraction. By applying Banach fixed point theorem, we obtain that R has a unique fixed point, and such point is a solution for problem (1.4).

    To obtain the sufficient conditions for the existence of anti-periodic solution for problem (1.5), we consider the following problem:

    {ABCD ζ0,ιz(ι)=w(ι), ιJ{ι1,ι2,,ιm}, z(0)=z(b), z(0)=z(b),z(ι+i)=z(ιi)+Ii(z(ιi)), iN1,z(ι+i)=z(ιi)+¯Ii(z(ιi)), iN1. (5.1)

    Note that problem (5.1) can be obtained from (4.7) by setting z0=z(b) and z1=z(b) . Therefore, the solution of (5.1) is given by Eq (4.6) after substituting the values of z0 and z1.

    Lemma 5.1. Let wPCH1(J,E) with w(0)=0. The solution function of problem (5.1) is given by Eq (4.6), where z0,z1 are given as follows:

    z0=b(2ζ)4M(ζ1)w(b)+b(ζ1)4M(ζ1)Γ(ζ1)b0(bs)ζ2w(s)ds.12mi=1Ii(z(ιi))14mi=1(b2ιi)¯Ii(z(ιi))122ζM(ζ1)b0w(s)ds12ζ1M(ζ1)Γ(ζ)b0(bs)ζ1w(s)ds, (5.2)

    and

    z1=12[mi=1¯Ii(z(ιi))+2ζM(ζ1)w(b)+ζ1M(ζ1)Γ(ζ1)b0(bs)ζ2w(s)ds]. (5.3)

    Proof. Using Eq (4.6) and the boundary conditions z(0)=z(b), z(0)=z(b), we obtain

    z1=z1mi=1¯Ii(z(ιi))2ζM(ζ1)w(b)ζ1M(ζ1)Γ(ζ1)b0(bs)ζ2w(s)ds.

    So, Eq (5.3) is verified. Moreover,

    z0=[z0+bz1+mi=1Ii(z(ιi))+mi=1(bιi)¯Ii(z(ιi))+2ζM(ζ1)b0w(s)ds+ζ1M(ζ1)Γ(ζ)b0(bs)ζ1w(s)ds],

    i.e.,

    z0=12[bz1+mi=1Ii(z(ιi))+mi=1(bιi)¯Ii(z(ιi))+2ζM(ζ1)b0w(s)ds+ζ1M(ζ1)Γ(ζ)b0(bs)ζ1w(s)ds].

    This equation along with Eq (5.3) lead to

    z0=b(2ζ)4M(ζ1)w(b)+b(ζ1)4M(ζ1)Γ(ζ1)b0(bs)ζ2w(s)ds.12mi=1Ii(z(ιi))14mi=1(b2ιi)¯Ii(z(ιi))122ζM(ζ1)b0w(s)ds12ζ1M(ζ1)Γ(ζ)b0(bs)ζ1w(s)ds].

    By substituting the values of z0 and z1 into Eq (4.6), we obtain the following

    Corollary 5.1. Let wPCH1(J,E) with w(0)=0. The solution of system in (5.1) is given by:

    z(ι)=(b4ι2)2ζM(ζ1)w(b)+(b4ι2)b0(bs)ζ2w(s)ds122ζM(ζ1)b0w(s)ds12ζ1M(ζ1)Γ(ζ)b0(bs)ζ1w(s)ds12mi=1Ii(z(ιi))b4mi=1¯Ii(z(ιi))12mi=1(ιιi)¯Ii(z(ιi))+ki=1Ii(z(ιi))+ki=1(ιιi)¯Ii(z(ιi))+2ζM(ζ1)ι0w(s)ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1w(s)ds, where ιJk,kN0. (5.4)

    As a result of Corollary 5.1, we state the following definition.

    Definition 5.1. A function zPCH2(J,E) is said to be a solution for problem (1.5) if it has left Atangana-Baleanu fractional derivative of order ζ on each Jk, where kN0, and satisfies the integral equation:

    z(ι)=(b4ι2)2ζM(ζ1)f(b,z(b))+(b4ι2)b0(bs)ζ2f(s,z(s))ds122ζM(ζ1)b0f(s,z(s))ds12ζ1M(ζ1)Γ(ζ)b0(bs)ζ1f(s,z(s))ds12mi=1Ii(z(ιi))b4mi=1¯Ii(z(ιi))12mi=1(ιιi)¯Ii(z(ιi))+ki=1Ii(z(ιi))+ki=1(ιιi)¯Ii(z(ιi))+2ζM(ζ1)ι0f(s,z(s))ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1f(s,z(s))ds, where  ιJk,kN0. (5.5)

    Theorem 5.1. Under the assumptions of Theorem 4.2, problem (1.5) has a unique solution provided that

    [σb2+σbζ2(ζ1)+2σb(2ζ)M(ζ1)+3σbζ2ζ1M(ζ1)Γ(ζ+1)32mi=1δi+7b4mi=1ηi]<1. (5.6)

    Proof. Consider the function R:PC(J,E)PC(J,E) defined as:

    R(z)(ι)=(b4ι2)2ζM(ζ1)f(b,z(b))+(b4ι2)b0(bs)ζ2f(s,z(s))ds122ζM(ζ1)b0f(s,z(s))ds12ζ1M(ζ1)Γ(ζ)b0(bs)ζ1f(s,z(s))ds12mi=1Ii(z(ιi))b4mi=1¯Ii(z(ιi))12mi=1(ιιi)¯Ii(z(ιi))+ki=1Ii(z(ιi))+ki=1(ιιi)¯Ii(z(ιi))+2ζM(ζ1)ι0f(s,z(s))ds+ζ1M(ζ1)Γ(ζ)ι0(ιs)ζ1f(s,z(s))ds,where ιJk,kN0. (5.7)

    Let z,vPC(J,E), ιJk,kN1. By the assumptions (A2), (A4), and above equality, we have

    ||R(z)(ι)R(v)(ι)||[σb2+σbζ2(ζ1)+σb22ζM(ζ1)+σbζ2ζ1M(ζ1)Γ(ζ+1)+32mi=1δi+b4mi=1ηi+3b2mi=1ηi+σb(2ζ)M(ζ1)+σbζ(ζ1)M(ζ1)Γ(ζ+1)]||zv||=[σb2+σbζ2(ζ1)+2σb(2ζ)M(ζ1)+3σbζ2ζ1M(ζ1)Γ(ζ+1)+32mi=1δi+7b4mi=1ηi]||zv||.

    This equation along with (5.6) shows that R is a contraction. Therefore, problem (1.5) has a unique solution.

    Definition 6.1. Let Λ and Δ be two normed spaces. A multi-valued function G:Λ2E with non-empty closed, bounded and convex values is called ρ-Lipschitz if

    h(G(x)G(y))ρ ||xy||Λ,x,yΛ,

    where h is the Hausdorff distance.

    For information about the multi-valued functions, we refer the reader to [50].

    Lemma 6.1. ([51], Theorem 7) Let (Ω,,μ) be a σ finite measure space and (T,d) be a metric space. If G:T2Lp(Ω,Rn),p[1,) is a ρ-Lipschitz multi-valued function with non-empty, closed, convex, bounded and decomposable values, then there is single-valued function f:T2Lp(Ω,Rn) such that f(t)G(t),a.e, and ||f(z)f(v)||ξG ρ||zv||Lp(Ω,Rn), z,vT, where ξG  is a positive real number.

    In the following theorem, we provide sufficient conditions for the existence of solutions of problem (1.6).

    Theorem 6.1. Let F:J×L2(J,R)2L2(J,R) be an ρ-Lipschitz multi-valued function with non-empty, closed, convex, bounded and decomposable values, and Ii, ¯Ii: L2(J,R)L2(J,R),iN1 be functions such that

    Ii(x)Ii(y)δixy,xL2(J,R),iN1,

    and

    ¯Ii(x)¯Ii(y)ηixy,xL2(J,R),iN1,

    where δiηi, are positive real numbers, then problem (1.6) has a solution provided that F(0,z0)={0} and

    ki=1(δi+ηi)+ξF ρ(2ζ)bM(ζ1)+σ(ζ1)bζM(ζ1)Γ(ζ+1)<1. (6.1)

    Proof. Let E=L2(J,R). The set T=J×E is a complete metric space, where d((ι1,x1),(ι2,x2))=|ι1ι2|+||x1x2||E. By Lemma 6.1, there exists f: J×EE satisfying f(ι,x)F(ι,x),a.e., and

    ||f(ι,x)f(s,y)||ξF ρ(|ιs|+||xy||E), (ι,x),(s,y)T.

    By applying Theorem (4.2), the following fractional boundary problem

    {ABCDζ0,ιz(ι)=f(ι,z(ι)),ιJ{ι1,ι2,,ιm}, z(0)=z0, z(0)=z1,z(ι+i)=z(ιi)+Ki(z(ιi)), i=1,2,,m,z(ι+i)=z(ιi)+¯Ki(z(ιi)), i=1,2,,m.

    has a solution. Since f(ι,x)F(ι,x) a.e, we have ABCDζ0,ιz(ι)F(ι,z(ι)) a.e. for  ιJ{ι1,ι2,,ιm} which completes the proof.

    Example 6.1. Let E =L2[0,π], ζ(1,2),  J=[0,1] and z0:[0,π]R be the zero function. Define f:J×EE by

    f(w,ς)(η)=sinwπ+λς2(η); wJ, ςE, η[0,π], (6.2)

    where λ>0. Thus, f(0,z0)(η)=0;η[0,π]. For any ς1,ς2E=L2[0,π] and any w1,w2J, we have

    ||f(w1,ς1)f(w2,ς2)||L2[0,π]=(π01π|(sinw1sinw2)+λ2(ς21(η)ς22(η))|2dη)12(π01π|sinw1sinw2|2dη)12+λ(π0|ς21(η)ς22(η)|2dη)12|sinw1sinw2|+λ(π0|(ς1(η))+ς2(η)) (ς1(η))ς2(η))|2dη)12|w1w2|+λ|<ς1+ς2,ς1ς2>||w1w2|+λ||ς1+ς2|| ||ς1ς2|||w1w2|+λ(||ς1||+||ς2||) ||ς1ς2||.

    Thus, (A1) is satisfied with Lδ=2λδ. By applying Theorem 3.1, we have that if there is r>0 such that

    ||z1||+2(1+2λr2)[(2ζ)M(ζ1)+(ζ1)M(ζ1)Γ(ζ)]<r, (6.3)

    then there is a unique function z:[0,1]L2[0,π] satisfying the boundary value problem

    {ABCDζ0,ιz(ι)(s)=sinιπ+ς2(s),  ιJ, ςE, s[0,π],z(0)=z0,z(1)=z1, (6.4)

    (see relation (3.6)).

    The inequality (6.3) is equivalent to

    4λωr2r+||z1||+2ω<0, (6.5)

    where ω=(2ζ)M(ζ1)+(ζ1)M(ζ1)Γ(ζ).

    If 16 λ ω(||z1||+2ω)<1, then the equation 4ωλr2r+||z1||+2ω=0 has two positive solutions, namely

    r1=1116λω(||z1||+2ω)8ω  and  r2=1+116λω(||z1||+2ω)8ω.

    Therefore, (6.5) will be satisfied for r(r1,r2). Thus, inequality (6.3) has a solution provided the following inequality

    16 λ ω(||z1||+2ω)<1 (6.6)

    holds. The last inequality will hold if we choose λ sufficiently small.

    Example 6.2. Let E =L2[0,π], ζ(1,2),  J=[0,1]. Define f:J×EE by:

    f(w,ς)(η):=sinwπ+σsinς(η); wJ, ςE, η[0,π], (6.7)

    where, σ>0. Let z0:[0,π]R, be the zero function and z1L2[0,π] be a fixed function. Note that f(0,z0)(η)=0, η[0,π]. For every ς1,ς2E=L2[0,π]  and every w1,w2J, we have

    ||f(w,ς1)f(w,ς2)||L2[0,π]=σ(π0|sinς1(η)sinς2(η)|2dη)12σ(π0|ς1(η)ς2(η)|2dη)12=σ||ς1ς2||L2[0,π]σ||ς1ς2||L2[0,π].

    Thus, (A2) is satisfied. By applying Theorem 3.2, there is a unique z:[0,1]L2[0,π] such that zH1((0,1),L2[0,π]) and z satisfies the boundary value problem:

    {ABCDζ0,ιz(ι)(η)=sinιπ+υsin(z(ι)η), ι[0,1],η[0,π],z(0)=z0,z(1)=z1, (6.8)

    provided the following condition is satisfied

    2σ(2ζ)M(ζ1)+2(ζ1)σM(ζ1)Γ(ζ)<1. (6.9)

    The last inequality holds by choosing σ sufficiently small.

    Example 6.3. Let E,ζ,J,f as be in Example 6.2, ι0=0,ι1 =12  and ι2=1. Define I1(x)=λ ProjK(x), ¯I1(x)=λ ProjZ(x),xE, where λ>0, K and Z are convex and compact subset of L2[0,π] and λ>0. Then, (A2) is satisfied. Also, (2.2) and (2.3) are verified with δ1=η1=λ. By applying Theorem 4.2, the problem

    {(ABCDζ0,ιz(ι))(η)=sinιπ+υsin(z(ι)η), ι[0,1]{0,12},η[0,π],z(0)=z0, z(0)=z1,z(ι+1)=z(ι1)+I1(z(ι1)),z(ι+1)=z(ι1)+¯I1(z(ι1)), (6.10)

    has a solution provided that

    2λ+σ(2ζ)M(ζ1)+σ(ζ1)M(ζ1)Γ(ζ+1)<1. (6.11)

    This inequality will hold by choosing σ and λ sufficiently small.

    In a similar manner, many examples of the application of Theorems 5.1 and 6.1 can be provided.

    The relationships between some boundary value problems involving the Atangana-Baleanu fractional derivative (AB) of order ζ(1,2) and the corresponding fractional integral equations were obtained in infinite dimensional Banach spaces with or without impulses. We showed that the continuity assumption on the nonlinear term is insufficient and must be replaced by membership in the space H1((a,b),E). The sufficient conditions for the existence of solutions for differential equations and inclusions involving AB fractional derivative in the presences of instantaneous impulses in infinite dimensional Banach spaces were established. Additionally, the sufficient conditions for the existence and uniqueness of solutions and anti-periodic solutions for differential equations and inclusions containing AB fractional derivative of order ζ(1,2) in the presences of instantaneous impulses in infinite dimensional Banach spaces were obtained.

    The major contributions of this work can be summarized as follows:

    (1) A modified formula for relationship between the solution of problem (1.1) and the corresponding integral equation (1.2) is derived.

    (2) A new class of boundary value for differential equations and inclusions containing AB derivative with instantaneous impulses in infinite dimensional Banach spaces were formulated with and without impulsive effects.

    (3) The existence/uniqueness of solutions and anti-periodic solutions for the considered problems and the corresponding inclusions were proved.

    We provide methods to deal with differential equations and differential inclusions in infinite dimensional Banach spaces. i.e., to extend the results in [19,20,21,22,23,24,45,46] to infinite dimensional spaces. The methods used in this paper can help researchers to generalize many of the results cited above in the presence of impulsive effects, infinite dimensional Banach spaces, and when the right hand side of the equation is a multi-valued function. We suggest the following topics for future research

    ● Study the existence of S-asymptotically w-periodic solutions for problems (1.3) and (1.4).

    ● Extend the recent work by Saha et al.[42] to infinite dimensional Branch spaces.

    ● Generalize the present work to the case where the Atangana and Baleanu's derivative is replaced by the Atangana and Baleanu's derivative with respect to another function.

    The authors declare that they have not used Artificial Intelligence (AI) tools in the creation of this article.

    The authors acknowledge the Deanship of Scientific Research at King Faisal University for the financial support.

    This work was supported by the Deanship of Scientific Research, Vice Presidency for Graduate Studies and Scientific Research, King Faisal University, Saudi Arabia [Grant No. GRANT3812].

    The authors declare no conflicts of interest.



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