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
[1] | Muneerah Al Nuwairan, Ahmed Gamal Ibrahim . Nonlocal impulsive differential equations and inclusions involving Atangana-Baleanu fractional derivative in infinite dimensional spaces. AIMS Mathematics, 2023, 8(5): 11752-11780. doi: 10.3934/math.2023595 |
[2] | Muneerah AL Nuwairan, Ahmed Gamal Ibrahim . The weighted generalized Atangana-Baleanu fractional derivative in banach spaces- definition and applications. AIMS Mathematics, 2024, 9(12): 36293-36335. doi: 10.3934/math.20241722 |
[3] | Zainab Alsheekhhussain, Ahmed Gamal Ibrahim, Rabie A. Ramadan . Existence of $ S $-asymptotically $ \omega $-periodic solutions for non-instantaneous impulsive semilinear differential equations and inclusions of fractional order $ 1 < \alpha < 2 $. AIMS Mathematics, 2023, 8(1): 76-101. doi: 10.3934/math.2023004 |
[4] | A.G. Ibrahim, A.A. Elmandouh . Existence and stability of solutions of $ \psi $-Hilfer fractional functional differential inclusions with non-instantaneous impulses. AIMS Mathematics, 2021, 6(10): 10802-10832. doi: 10.3934/math.2021628 |
[5] | Velusamy Kavitha, Mani Mallika Arjunan, Dumitru Baleanu . Non-instantaneous impulsive fractional-order delay differential systems with Mittag-Leffler kernel. AIMS Mathematics, 2022, 7(5): 9353-9372. doi: 10.3934/math.2022519 |
[6] | Mohamed I. Abbas, Maria Alessandra Ragusa . Nonlinear fractional differential inclusions with non-singular Mittag-Leffler kernel. AIMS Mathematics, 2022, 7(11): 20328-20340. doi: 10.3934/math.20221113 |
[7] | Lulu Ren, JinRong Wang, Michal Fečkan . Periodic mild solutions of impulsive fractional evolution equations. AIMS Mathematics, 2020, 5(1): 497-506. doi: 10.3934/math.2020033 |
[8] | Thabet Abdeljawad, Pshtiwan Othman Mohammed, Hari Mohan Srivastava, Eman Al-Sarairah, Artion Kashuri, Kamsing Nonlaopon . Some novel existence and uniqueness results for the Hilfer fractional integro-differential equations with non-instantaneous impulsive multi-point boundary conditions and their application. AIMS Mathematics, 2023, 8(2): 3469-3483. doi: 10.3934/math.2023177 |
[9] | Ahmed Salem, Kholoud N. Alharbi . Fractional infinite time-delay evolution equations with non-instantaneous impulsive. AIMS Mathematics, 2023, 8(6): 12943-12963. doi: 10.3934/math.2023652 |
[10] | Ravi Agarwal, Snezhana Hristova, Donal O'Regan . Integral presentations of the solution of a boundary value problem for impulsive fractional integro-differential equations with Riemann-Liouville derivatives. AIMS Mathematics, 2022, 7(2): 2973-2988. doi: 10.3934/math.2022164 |
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, 0≤k≤m,Nk={k,k+1,…,m},0=ι0<ι1≤<ι2≤ι3⋯<ιm+1=b be a partition of J, J0=[0,ι1], and Jk=(ιk,ιk+1],k∈N1.
● 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 {z∈L2((a,b),E):z′∈L2((a,b),E)}.
● PC(J,E) is the Banach space defined as
PC(J,E)={z:J→E,z∈H1(Jk,E):z(ι+k)andz(ι−k)exist withz(ιk)=z(ι−k)},∀k∈N1}.
The norm on PC(J,E) is given by ||z||PC(J,E)=sup{||z(ι)||:ι∈J}.
● PCH1(J,E)={z∈PC(J,E):z|Jk∈H1((ιk,ιk+1),E),∀k∈N1}.
● PCH2(J,E)={z∈PC(J,E):z′|Jk∈H1((ιk,ιk+1),E),∀k∈N1}. 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):k∈N1}, t=1,2. |
Recently, it was shown in [20,21,23] that the following fractional differential equation:
{ABCDζ0,ιz(ι)=w(ι), ι∈J,z(0)=z0,z(b)=z1 | (1.1) |
is equivalent to the fractional integral equation:
z(ι)=z0+ι(z1−z0)b−ι(2−ζ)bM(ζ−1)∫b0w(s)ds−ι(ζ−1)bM(ζ−1)Γ(ζ)∫b0(b−s)ζ−1w(s)ds+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(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:J→R 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 z′∈H1((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)), ι∈J,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), ι∈J,z(a)=z0,z′(a)=z1 |
and the integral equation
z(ι)=z0+(ι−a)[z1−2−ζM(ζ−1)w(a)−ζ−1M(ζ−1)Γ(ζ−1)∫a0(a−s)ζ−2w(s)ds]−2−ζM(ζ−1)∫a0w(s)ds−ζ−1M(ζ−1)Γ(ζ)∫a0(a−s)ζ−1w(s)ds+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds, ι∈J. |
(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)),ι∈J−{ι1,ι2,…,ιm}, z(0)=z0, z′(0)=z1,z(ι+i)=z(ι−i)+Ii(z(ι−i)), i∈N1,z′(ι+i)=z′(ι−i)+¯Ii(z(ι−i)), i∈N1, | (1.4) |
where f(0,z(0))=0, and Ii,¯Ii:E→E 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)),ι∈J−{ι1,ι2,…,ιm}, z(0)=−z(b), z′(0)=−z′(b),z(ι+i)=z(ι−i)+Ii(z(ι−i)), i∈N1,z′(ι+i)=z′(ι−i)+¯Ii(z(ι−i)), i∈N1, | (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)),ι∈J−{ι1,ι2,…,ιm}, z(0)=z0, z′(0)=z1,z(ι+i)=z(ι−i)+Ii(z(ι−i)), i∈N1,z′(ι+i)=z′(ι−i)+¯Ii(z(ι−i)), i∈N1, | (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 z∈H1((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)1−ζ∫ιaz′(x)Eζ(−ζ(ι−x)ζ1−ζ)dx, ι∈J, |
and
ABRDζa,ιz(ι)=M(ζ)1−ζ ddι∫ιaz(x)Eζ(−ζ(ι−x)ζ1−ζ)dx, ι∈J, |
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), β∈R, μ∈C. |
Definition 2.2. [14,19] Let a<b be two real numbers, and ζ∈(0,1). The Atangana-Baleanu fractional integral for a function z∈H1((a,b),E) of order ζ with lower limit at a is given by
ABIζa,ιz(ι)=1−ζM(ζ)z(ι)+ζM(ζ)Γ(ζ)∫ιaz(x)(ι−x)ζ−1dx, ι∈J. |
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 z∈H1((a,b),E), ζ∈(0,1) and ι∈J.
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(ι−a)ζ1−ζ).
iii. ABCIζa,ι(ABCIζa,ιz(ι))=z(ι)−z(a).
iv. ABRDζa,ιz(ι)=ABCDζ0,ιz(ι)+M(ζ)1−ζz(a)Eζ(−ζ(ι−a)ζ1−ζ).
v. ABRDζa,ιc=cEζ(−ζ1−ζ(ι−a)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),n∈N 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)=ABCDζ−na,ιz(n)(ι)=M(ζ−1)1−(ζ−n)∫ιaz(n+1)(x)E(ζ−n)(−(ζ−n)(ι−x)(ζ−n)1−(ζ−n))dx, |
and
ABRDζa,ιz(ι)=ABRDζ−na,ιz(n)(ι)=M(ζ−n)1−(ζ−n)ddι∫ιaz(n)(x)E(ζ−n)(−(ζ−n)(ι−x)(ζ−n)1−(ζ−n))dx. |
Definition 2.4. [14,19] Let ζ∈(n,n+1),n∈N 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,ιABIζ−na,ιz(ι). |
As in [20,22], one can prove the following lemma.
Lemma 2.2. Let ζ∈(1,2) and z:J→E with z′∈H1((a,b),E). For any ι∈[a,b],
(1) ABRDζa,ι(ABIζa,ιz(ι))=z(ι).
(2) ABCDζa,ι(ABIζa,ιz(ι))=ABCDζ−1a,ι(ddι(I(ABIζ−10,ιz(ι))))=ABCDζ−1a,ι(ABIζ−10,ιz(ι))=z(ι)−z(a)Eζ−1(−(ζ−1)(ι−a)ζ−12−ζ).
(3) ABIζa,ι(ABCDζa,ιz(ι))=z(ι)−c0−c1(ι−a).
We end this section by listing some assumptions that are used later.
Assumptions 2.1. Let f:J×E→E be a function, we assume the following:
- (A1): For any δ>0 there is Lδ >0 such that for any x,y∈E with ||x||≤δ, ||y||≤δ and any s,ι∈J, we have
||f(ι,x)−f(s,y)||≤|s−ι|+Lδ ||x−y||. |
- (A2): There is σ>0 such that for any x,y∈E, we have
||f(ι,x)−f(ι,y)||≤σ||x−y||,∀ι∈J. |
- (A3): For every i∈N1, the functions Ii,¯Ii:E→E are continuous, compact and there exist positive constants hi¯hi (i=1,2,..,m) such that
Ii(x)≤hix,∀x∈E.and¯Ii(x)≤¯hix,∀x∈E. | (2.1) |
- (A4): For every i∈N1, there exists positive constants δiηi, such that
‖Ii(x)−Ii(y)‖≤δi‖x−y‖,∀x∈E, | (2.2) |
and
‖¯Ii(x)−¯Ii(y)‖≤ηi‖x−y‖,∀x∈E. | (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:J→E is continuous and z:J→E is a solution to Eq (1.1), then z satisfies the integral equation (1.2).
(2) If w∈H1((0,b),E) with w(0)=0 and z satisfies Eq (1.2), then z′∈H1((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( ABIζ−10,ιw(ι))=c0+ιc1+I0,ι[1−(ζ−1)M(ζ−1)w(ι)+ζ−1M(ζ−1)Iζ−10,ιw(ι)]=c0+ιc1+∫ι02−ζM(ζ−1)w(s)ds+ζ−1M(ζ−1)Iζ0,ιw(ι)=c0+ιc1+∫ι02−ζM(ζ−1)w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0w(s)(ι−s)ζ−1ds. | (3.1) |
From the boundary conditions z(0)=z0 and z(b)=z1, it follows that c0=z0 and
z1=z0+bc1+∫b02−ζM(ζ−1)w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫b0w(s)(b−s)ζ−1ds, |
i.e.,
c1=z1b−z0b−∫b02−ζbM(ζ−1)w(s)ds−ζ−1bM(ζ−1)Γ(ζ)∫b0w(s)(b−s)ζ−1ds. | (3.2) |
Substituting the values of c0 and c1 into (3.1), we obtain
z(ι)=ιz1+z0(b−ι)b−ι(2−ζ)bM(ζ−1)∫b0w(s)ds−ι(ζ−1)bM(ζ−1)Γ(ζ)∫b0w(s)(b−s)ζ−1ds.+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0w(s)(ι−s)ζ−1ds. |
(2) Assume that w∈H1((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+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0w(s)(ι−s)ζ−1ds, | (3.3) |
where c0=z0 and c1 is given by (3.2). Since ζ>1, Eq (3.3) gives us that
z′(ι)=c1+2−ζM(ζ−1)w(ι)+ζ−1M(ζ−1)I ζ−10,ιw(ι), for a.e. ι∈J, | (3.4) |
where I ζ−10,ι is the Riemann-Liouville fractional integral of order ζ−1. Since w∈H1(J,E), ζ−1∈(0,1), and E is reflexive, w has a Bochner integrable derivative w′ almost everywhere, and
w(s)=w(0)+∫s0w′(x)dx, ∀s∈w. |
This implies that
I ζ−10,ιw(ι)=1Γ(ζ−1)∫ι0(ι−s)ζ−2w(s)ds=1Γ(ζ−1)∫ι0(ι−s)ζ−2[∫s0w′(x)dx]ds, |
i.e., I ζ−10,ιw(ι) is the primitive of a Bochner integrable function, hence is absolutely continuous. Thus Eq (3.4) is valid for every ι∈J. Moreover,
z(2)(ι)=2−ζM(ζ−1)w′(ι)+ζ−1M(ζ−1)ddι(I ζ−1w(ι)), |
giving us that z′∈H1((0,b),E). Equation (3.2) implies
z(ι)=c0+ιc1+ABIζ0,ιw(ι), ι∈J. |
Finally, by the second assertion of Lemma 2.2,
ABCDζ0,ιz(ι)=ABCDζ0,ι ABIζ0,ιw(ι)=w(ι)−w(0)Eζ−1(−(ζ−1)ιζ−12−ζ)=w(ι), ι∈J.
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)Eζ−1(−(ζ−1)ιζ−12−ζ)≠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 w∈H1((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 w∈H1((0,b),E) with w(0)=0. A function z:J→E is a solution of problem (1.1) if and only if
z(ι)=z0+ι(z1−z0)b−ι(2−ζ)bM(ζ−1)∫b0w(s)ds−ι(ζ−1)bM(ζ−1)Γ(ζ)∫b0(b−s)ζ−1w(s)ds+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds. | (3.5) |
Theorem 3.1. Let f:J×E→E 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(2−ζ)M(ζ−1)+(ζ−1)bζM(ζ−1)Γ(ζ)]<r. | (3.6) |
Proof. Define T:C(J,E)→C(J,E) by
T(z)(ι)=z0+ι(z1−z0)b−ι(2−ζ)bM(ζ−1)∫b0f(s,z(s))ds−ι(ζ−1)bM(ζ−1)Γ(ζ)∫b0(b−s)ζ−1f(s,z(s))ds+2−ζM(ζ−1)∫ι0f(s,z(s))ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1f(s,z(s))ds. | (3.7) |
Using the Schauder fixed point theorem, we will show that T has a unique fixed point. Set B0={z∈C(J,E):‖z‖C(J,E)≤r}.
● Step 1: T(B0)⊆B0. Let z∈B0. 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)||, ∀ ι∈J. | (3.8) |
From (3.6)–(3.8), one has
||T(z)(ι)||≤||z0(1−ιb)+ιbz1||+2(b+rLr+||f(0,0)||)[b(2−ζ)M(ζ−1)+(ζ−1)bζM(ζ−1)Γ(ζ)]≤||z0||+||z1||+2(b+rLr+||f(0,0)||)[b(2−ζ)M(ζ−1)+(ζ−1)bζM(ζ−1)Γ(ζ)]<r, |
showing that T(B0)⊆B0.
● Step 2: T(B0) is equicontinuous. Let z∈B0 and ι,ι+λ∈J. Using (3.7), we obtain
‖T(z)(ι+λ)−T(z)(ι)‖≤‖λ(z1−z0)b‖+λ(2−ζ)(b+rLr+||f(0,0)||)M(ζ−1)+λ(ζ−1)(b+rLr+||f(0,0)||)bζζM(ζ−1)Γ(ζ)+λ(2−ζ)(b+rLr+||f(0,0)||)M(ζ−1)+(ζ−1)(b+rLr+||f(0,0)||)M(ζ−1)Γ(ζ)[∫ι+λ0(ι+λ−s)ζ−1−(ι−s)ζ−1)ds]. |
Since ζ−1 >0,‖T(z)(ι+λ)−T(z)(ι)‖→0 when λ→0, independently of z, proving the assertion.
● Step 3: For n≥1, let Bn=¯convT(Bn−1), and B=∩n≥0Bn.
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 Bn⊆Bn−1, n≥1. By Cantor intersection property [47], it is enough to show that
limn→∞χC(J,E)(Bn)=0, | (3.9) |
where χC(J,E) is the Hausdorff measure of noncompactness on C(J,E) [48].
Let n≥1 be a fixed natural number and ε>0. By Lemma 3 in [49], there exists a sequence (zk), k≥1 in Bn−1 such that
χC(J,E)(Bn)=χC(J,E)T(Bn−1)≤2χC(J,E){T(zk):k≥1}+ε. | (3.10) |
Since Bn is equicontinuous, inequality (3.10) becomes
χC(J,E)(Bn)≤2maxι ∈JχE{T(zk)(ι):k≥1}+ε. | (3.11) |
Let ι∈J be fixed. In view of (3.8)
||f(ι,zm(ι))−f(ι,zn(ι))||≤Lr ||zm(ι)−zn(ι)||,∀n,m∈N. |
It follows that
χE{f(ι,zk(ι)):k≥1}≤LrχE{zk(ι):k≥1}. | (3.12) |
We also have that
T(zk)(ι)=z0+ι(z1−z0)b−ι(2−ζ)bM(ζ−1)∫b0f(s,zk(s))ds−(ζ−1)bM(ζ−1)Γ(ζ)∫b0(b−s)ζ−1f(s,zk(s))ds+2−ζM(ζ−1)∫ι0f(s,zk(s))ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1f(s,zk(s))ds. | (3.13) |
Since ζ>1, Eqs (3.12) and (3.13) give
χ{T(zk)(ι):k≥1}≤∫b0χE{zk(s):k≥1}ds[2(2−ζ)LrM(ζ−1)+2bζ−1(ζ−1)LrM(ζ−1)Γ(ζ)]≤b[2(2−ζ)LrM(ζ−1)+2bζ−1(ζ−1)LrM(ζ−1)Γ(ζ)]χC(J,E)(Bn−1). | (3.14) |
Using (3.11) and (3.14), we obtain that
χC(J,E)(Bn)≤4bLr[2−ζM(ζ−1)+bζ−1(ζ−1)M(ζ−1)Γ(ζ)]χC(J,E)(Bn−1),∀n∈N. |
This inequality yields that
χC(J,E)(Bn)≤χC(T,E)(B0)4bLr[2−ζM(ζ−1)+bζ−1(ζ−1)M(ζ−1)Γ(ζ)]n−1. | (3.15) |
The inequality in (3.6) implies that 4bLr[(2−ζ)M(ζ−1)+bζ(ζ−1)M(ζ−1)Γ(ζ)]<1, and thus, (3.15) implies (3.9).
● Step 4: The function T|B:B→B is continuous. Assume that zn→z in B. Note that for n≥1 and ι∈J, we have
T(zn)(ι)=z0+ι(z1−z0)b−ι(2−ζ)bM(ζ−1)∫b0f(s,zn(s))ds,−ι(ζ−1)bM(ζ−1)Γ(ζ)∫b0(b−s)ζ−1f(s,zn(s))ds+2−ζM(ζ−1)∫ι0f(s,zn(s))ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1f(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 z∈B such that z=T(z). That is,
z(ι)=z0+ι(z1−z0)b−ι(2−ζ)bM(ζ−1)∫b0w(s)ds−ι(ζ−1)bM(ζ−1)Γ(ζ)∫b0(b−s)ζ−1w(s)Bs+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds, |
where w(ι)=f(ι,z(ι)), ι∈J.
Next, we show that this function z is a solution for problem (1.3). By Lemma 3.1, it is sufficient to show that w∈H1(J,E). Since ζ>1, then
z′(t)=2−ζM(ζ−1)w(t)+ζ−1M(ζ−1)Iζ−10,tw(t),t∈J. |
From (A1),w is absolutely continuous, and since E is reflexive, the function t→Iζ−10,tw(t) is absolutely continuous. Hence w∈H1(J,E).
To show the uniqueness of the solution, let z,v∈C(J,E) be two solutions for problem (1.3) and ι∈J. Since z,v are solutions, it follows from (A1) that
||T(z)(ι)−T(v)(ι)||≤(2−ζ)M(ζ−1)∫b0||f(s,z(s))−f(s,v(s)))||+bζ−1(ζ−1)M(ζ−1)Γ(ζ)∫b0||f(s,z(s))−f(s,v(s))||ds+2−ζM(ζ−1)∫ι0||f(s,z(s))−f(s,v(s))||ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1||f(s,z(s))−f(s,v(s))||ds≤Lr(2−ζ)M(ζ−1)∫b0||z(s))−v(s)||ds+Lrbζ−1(ζ−1)M(ζ−1)Γ(ζ)∫b0||z(s))−v(s)||ds+Lr(2−ζ)M(ζ−1)∫ι0||z(s))−v(s)||ds+Lr(ζ−1)M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1||z(s))−v(s)||ds. |
Hence,
||z(ι)−v(ι)||≤Lr(2−ζ)bM(ζ−1)||z−v||+Lrbζ(ζ−1)M(ζ−1)Γ(ζ)||z−v||+Lr(2−ζ)bM(ζ−1)||z−v||+Lr(ζ−1)bζM(ζ−1)Γ(ζ)||z−v||≤||z−v||[2Lr(2−ζ)bM(ζ−1)+2Lr(ζ−1)bζM(ζ−1)Γ(ζ)]. |
Since ι is arbitrary, it follows that
||z−v||C(J,E)≤||z−v||C(J,E)[2Lr(2−ζ)bM(ζ−1)+2Lr(ζ−1)bζM(ζ−1)Γ(ζ)]. |
Inequality (3.6) implies 2Lr(2−ζ)bM(ζ−1)+2Lr(ζ−1)bζM(ζ−1)Γ(ζ)<1, consequently, ||z−v||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×E→E. If (A2) is satisfied, then problem (1.3) has a unique solution provided that f(0,z0)=0 and
2bσ(2−ζ)M(ζ−1)+2bζ(ζ−1)σM(ζ−1)Γ(ζ)<1. | (3.16) |
Proof. Consider the function T:C(J,E)→C(J,E) defined by (3.7). Let z,v∈C(J,E). For any ι∈J,
||T(z)(ι)−T(v)(ι)||≤(2−ζ)M(ζ−1)∫b0||f(s,z(s))−f(s,z(s))||ds+bζ−1(ζ−1)M(ζ−1)Γ(ζ)∫b0||f(s,z(s))−f(s,z(s))||ds+2−ζM(ζ−1)∫ι0||f(s,z(s))−f(s,z(s))||ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1||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(2−ζ)M(ζ−1)∫b0||z(s)−v(s))||ds+2bζ−1(ζ−1)σM(ζ−1)Γ(ζ)∫b0||z(s)−v(s))||ds≤[2bσ(2−ζ)M(ζ−1)+2bζ(ζ−1)σM(ζ−1)Γ(ζ)]||z−v||ds. |
Thus,
||T(z)−T(v)||≤[2bσ(2−ζ)M(ζ−1)+2bζ(ζ−1)σM(ζ−1)Γ(ζ)]||z−v||. |
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:J→E is continuous ,a∈[0,b),z:J→E be such that z′∈H1((0,b),E) and
{ABCD ζ0,ιz(ι)=w(ι),ι∈J,z(a)=z0, z′(a)=z1, | (4.1) |
then for any ι∈J,
z(ι)=z0+(ι−a)[z1−2−ζM(ζ−1)w(a)−ζ−1M(ζ−1)Γ(ζ−1)∫a0(a−s)ζ−2w(s)ds]−2−ζM(ζ−1)∫a0w(s)ds−ζ−1M(ζ−1)Γ(ζ)∫a0(a−s)ζ−1w(s)ds+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds. | (4.2) |
(2) If a∈[0,b),w:J→E be continuous with w(0)=0 and z:J→E are such that (4.2) holds, then z′∈H1((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+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds. |
Using the boundary conditions z(a)=z0,z′(a)=z1, we obtain
c0=z0−ac1−2−ζM(ζ−1)∫a0w(s)ds−ζ−1M(ζ−1)Γ(ζ)∫a0(a−s)ζ−1w(s)ds, | (4.3) |
and
z1=c1+2−ζM(ζ−1)w(a)+ζ−1M(ζ−1)Γ(ζ−1)∫a0(a−s)ζ−2w(s)ds. |
This gives that
c1=z1−2−ζM(ζ−1)w(a)−ζ−1M(ζ−1)Γ(ζ−1)∫a0(a−s)ζ−2w(s)ds. | (4.4) |
From (4.3) and (4.4), we obtain
c0=z0−a[z1−2−ζM(ζ−1)w(a)−ζ−1M(ζ−1)Γ(ζ−1)∫a0(a−s)ζ−2w(s)ds]−2−ζM(ζ−1)∫a0w(s)ds−ζ−1M(ζ−1)Γ(ζ)∫a0(a−s)ζ−1w(s)ds. | (4.5) |
Substituting the values of c0 and c1into z(ι), we obtain
z(ι)=z0−a[z1−2−ζM(ζ−1)w(a)−ζ−1M(ζ−1)Γ(ζ−1)∫a0(a−s)ζ−2w(s)ds]−2−ζM(ζ−1)∫a0w(s)ds−ζ−1M(ζ−1)Γ(ζ)∫a0(a−s)ζ−1w(s)ds+ι[z1−2−ζM(ζ−1)w(a)−ζ−1M(ζ−1)Γ(ζ−1)∫a0(a−s)ζ−2w(s)ds]+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds=z0+(ι−a)[z1−2−ζM(ζ−1)w(a)−ζ−1M(ζ−1)Γ(ζ−1)∫a0(a−s)ζ−2w(s)ds]−2−ζM(ζ−1)∫a0w(s)ds−ζ−1M(ζ−1)Γ(ζ)∫a0(a−s)ζ−1w(s)ds+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds. |
Hence, Eq (4.2) is verified.
(2) Suppose that w:J→E 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 z′∈H1((0,b),E). For any ι∈[a,b], we have
ABCDζ0,ιz(ι)=ABCDζ−10,ιz′(ι)=ABCDζ−10,ι(z1−ζ−1M(ζ−1)Γ(ζ−1)∫a0(a−s)ζ−2w(s)ds+2−ζM(ζ−1)w(ι)+ζ−1M(ζ−1)Γ(ζ−1)∫ι0(ι−s)ζ−2w(s)ds)(ι)=ABCDζ−10,ι(2−ζM(ζ−1)w(ι)+ζ−1M(ζ−1)Γ(ζ−1)∫ι0(ι−s)ζ−2w(s)ds)(ι)=ABCDζ−10,ι( ABI1−ζ0,ιw(ι))=w(ι)−w(0)E1−ζ(−(1−ζ)ι(1−ζ)2−ζ)=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 w∈PCH1(J,E) with w(0)=0 and z:J→E be a function satisfying
z(ι)=z0+ιz1+k∑i=1Ii(z(ι−i))+k∑i=1(ι−ιi)¯Ii(z(ι−i))+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds, where ι∈Jk,k∈N0, | (4.6) |
then z ∈PCH2(J, E) and satisfies the impulsive fractional differential equation:
{ABCD ζ0,ιz(ι)=w(ι), ι∈J−{ι1,ι2,…,ιm}, z(0)=z0, z′(0)=z1,z(ι+i)=z(ι−i)+Ii(z(ιi)), i∈N1,z′(ι+i)=z′(ι−i)+¯Ii(z(ιi)), i∈N1. | (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 ι∈J0,
z(ι)=z0+ιz1+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0w(s)(ι−s)ζ−1ds. | (4.8) |
Clearly, z(0)=z0, z′(0)=z1. Since w∈PCH1(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), ι∈J0, z(0)=z0, z′(0)=z1. |
Let us define a function v on J1=(ι1,ι2] by:
v(ι)=z(ι−1)+I1(z(ι−1))+(ι−ι1)[z′(ι−1)+¯I1(z(ι1))−2−ζM(ζ−1)w(ι1)−ζ−1M(ζ−1)Γ(ζ−1)∫ι10(ι1−s)ζ−2w(s)ds]−2−ζM(ζ−1)∫ι10w(s)ds−ζ−1M(ζ−1)Γ(ζ)∫ι10(ι1−s)ζ−1w(s)ds+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(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), ι∈J1, z(ι+1)=z(ι−1)+I1(z(ι−1)),z′(ι+1)=z(1)(ι−1)+¯I1(z(ι−1)). | (4.10) |
Let ι∈J1. We show that, v(ι)=z(ι). From Eq (4.8), it follows that
z(ι−1)=z0+ι1z1+2−ζM(ζ−1)∫ι10w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι10(ι1−s)ζ−1w(s)ds |
and
z′(ι−1)=z1+2−ζM(ζ−1)w(ι1)+ζ−1M(ζ−1)Γ(ζ−1)∫ι10(ι1−s)ζ−2w(s)ds. |
By substituting the values of z(ι−1) and z′(ι−1) into Eq (4.9), we obtain
v(ι)=z0+ι1z1+2−ζM(ζ−1)∫ι10w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι10w(s)(ι1−s)ζ−1ds+I1(z(ι−1))+(ι−ι1)[z1+2−ζM(ζ−1)w(ι1)+ζ−1M(ζ−1)Γ(ζ−1)∫ι10(ι1−s)ζ−2w(s)ds+¯I1(z(ι−1))−2−ζM(ζ−1)w(ι1)−ζ−1M(ζ−1)Γ(ζ−1)∫ι10(a−s)ζ−2w(s)ds]−2−ζM(ζ−1)∫ι10w(s)ds−ζ−1M(ζ−1)Γ(ζ)∫ι10(a−s)ζ−1w(s)ds+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds=z0+ιz1+I1(z(ι−1))+(ι−ι1)¯I1(z(ι−1))+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds. | (4.11) |
Therefore, v(ι)=z(ι),∀ι∈J1. Since
z(ι+1)−z(ι−1)=I1(z(ι−1)), and z′(ι+1)−z′(ι−1)=¯I1(z(ι−1)), |
then z is a solution for the fractional differential equation (4.10). By repeating the above steps for Jk;k∈N2, the proof follows.
Definition 4.1. A function z∈PCH2(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, k∈N1 and satisfies Eq (4.6).
In the following theorem, we provide an existence result for problem (1.4).
Theorem 4.1. Let f:J×E→E with f(0,z0)=0 and Ii,¯Ii:E→E (i∈N1) 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)||)[(2−ζ)bM(ζ−1)+(ζ−1)bζM(ζ−1)Γ(ζ+1)]<r, | (4.12) |
where h=max{∑mi=1hi∑mi=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+k∑i=1Ii(z(ι−i))+k∑i=1(ι−ιi)¯Ii(z(ι−i))+2−ζM(ζ−1)∫ι0f(s,z(s))ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1f(s,z(s))ds, where ι∈Jk,k∈N0, | (4.13) |
has a fixed point. Set B0={z∈PC(J,E):‖z‖PC(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 z∈B0 and ι∈Jk, k=0,1,2,..,m. Using (2.1), (3.8), (4.12), and (4.13), we obtain that for ι∈Jk,k=1,2,..,m,
||R(z)(ι)||≤||z0||+b||z1||+rmh(1+b)+(b+rLr +||f(0,0)||)[(2−ζ)bM(ζ−1)+(ζ−1)bζM(ζ−1)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,k∈N0={0,1,2,..,m}. Let k∈N0 be fixed, z∈B0 and ι,ι+λ∈Jk. Using (4.13), we get
‖R(z)(ι+λ)−R(z)(ι)‖≤λ(||z1||+2−ζM(ζ−1)||f(0,z0)||)+λ(2−ζ)M(ζ−1)(b+rLr +||f(0,0)||)+(ζ−1)(b+rLr +||f(0,0)||)M(ζ−1)Γ(ζ)∫ι0[(ι+λ−s)ζ−1−(ι−s)ζ−1]ds. |
Since ζ−1 >0, we have ‖R(z)(ι+λ)−R(z)(ι)‖→0 \ as λ→0,\ independently of z.
● Step 3: We show that B=∩n≥1Bn is non-empty and compact in PC(J,E), where Bn=¯conv(R(Bn−1)),∀n≥1. By Step 1, it follows that Bn,n≥1 is a decreasing sequence of non-empty, closed convex and bounded subsets of PC(J,E), and hence it is sufficient to show that
limn→∞χPC(J,E)(Bn)=0, | (4.14) |
where χPC(J,E) is the Hausdorff measure of noncompactness on PC(J,E).
Let n≥1 be a fixed natural number and ε>0. In view of Lemma 3 in [49], there exists a sequence (zk),k≥1 in Bn−1 such that
χPC(J,E)(Bn)=χPC(J,E)R(Bn−1)≤2χPC(J,E){R(zk):k≥1}+ε=2maxi=0,1,...,m χi{R(zk)|¯Ji:k≥1}+ε, |
where χi is the Hausdorff measure of noncompactness on C(¯Ji,E). Since R(Bn−1) is equicontinuous, the above inequality becomes
χPC(J,E)(Bn)≤ 2maxi=0,1,...,msupι∈¯Jiχ{R(zk)(ι):k≥1}+ε, | (4.15) |
where χ is the the Hausdorff measure of noncompactness on E. Since Ii,¯Ii,i=0,..,m, are compact, we have
m∑i=1χ{Ii(zk(ι−i)):k≥1}=m∑i=1χ{(ι−ιi)(¯Ii(zk(ι−i)):k≥1}=0. |
Thus, as in (3.12)
χ{R(zk)(ι):k≥1}≤χC(J,E)(Bn−1)Lr(2−ζM(ζ−1)+(ζ−1)bζM(ζ−1)Γ(ζ)), |
from which,
χPC(J,E)(Bn)≤χPC(J,E)(B0)[Lr(2−ζM(ζ−1)+(ζ−1)bζM(ζ−1)Γ(ζ))]n−1. |
Inequality (4.12) insures that Lr(2−ζM(ζ−1)+(ζ−1)bζM(ζ−1)Γ(ζ))<1, and Eq (4.14) follows.
● Step 4: The function R|B:B→B is continuous. Let zn→z 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 z∈B⊆PC(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 ι∈J0, we have
||z(ι)−v(ι)||≤Lr(2−ζ)bM(ζ−1)sups∈J0||z(s)−v(s)||+Lrbζ(ζ−1)M(ζ−1)Γ(ζ)sups∈J0||z(s)−v(s)||≤sups∈J0||z(s)−v(s)||[Lr(2−ζ)bM(ζ−1)+Lr(ζ−1)bζM(ζ−1)Γ(ζ)]. |
Thus,
sups∈J0||z(s)−v(s)||≤sups∈J0||z(s)−v(s)||[Lr(2−ζ)bM(ζ−1)+Lr(ζ−1)bζM(ζ−1)Γ(ζ)]. |
The inequality (4.12) gives
Lr(2−ζ)bM(ζ−1)+Lr(ζ−1)bζM(ζ−1)Γ(ζ)<1. |
Thus, sups∈J0||z(s)−v(s)||=0, and hence z(s)=v(s),∀s∈J0.
Assume that ι∈J1. Because z(ι−1)=v(ι−1), it yields that,
||z(ι)−v(ι)||≤||I1(z(ι−1))−I1(v(ι−1))||+(ι−ι1)||¯I1(z(ι−1))−¯I1(v(ι−1))||+Lr(2−ζ)bM(ζ−1)sups∈J0||z(s)−v(s)||+Lrbζ(ζ−1)M(ζ−1)Γ(ζ)sups∈J0||z(s)−v(s)||=Lr(2−ζ)bM(ζ−1)sups∈J0||z(s)−v(s)||+Lrbζ(ζ−1)M(ζ−1)Γ(ζ)sups∈J0||z(s)−v(s)||≤sups∈J0||z(s)−v(s)||[Lr(2−ζ)bM(ζ−1)+Lr(ζ−1)bζM(ζ−1)Γ(ζ)]. |
As above, we obtain that z(ι)=v(ι),∀ ι∈J1. 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×E→E such that f(0,z0)=0 and Ii, ¯Ii:E→E\ (i∈N1) be functions. If Assumptions (A2) and (A4) are satisfied, then problem (1.4) has a unique solution provided that
m∑i=1(δi+bηi)+σ(2−ζ)bM(ζ−1)+σ(ζ−1)bζM(ζ−1)Γ(ζ+1)<1. | (4.16) |
Proof. Let R:PC(J,E)→PC(J,E), be function given by Eq (4.13), and z,v∈PC(J,E). For each ι∈Jk;k∈N1, we have
||R(z)(ι)−R(v)(ι)||≤[m∑i=1δi+bηi)+σ(2−ζ)bM(ζ−1)+σ(ζ−1)bζM(ζ−1)Γ(ζ+1)]||z−v||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), ι∈J−{ι1,ι2,…,ιm}, z(0)=−z(b), z′(0)=−z′(b),z(ι+i)=z(ι−i)+Ii(z(ιi)), i∈N1,z′(ι+i)=z′(ι−i)+¯Ii(z(ιi)), i∈N1. | (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 w∈PCH1(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(2−ζ)4M(ζ−1)w(b)+b(ζ−1)4M(ζ−1)Γ(ζ−1)∫b0(b−s)ζ−2w(s)ds.−12m∑i=1Ii(z(ι−i))−14m∑i=1(b−2ιi)¯Ii(z(ι−i))−122−ζM(ζ−1)∫b0w(s)ds−12ζ−1M(ζ−1)Γ(ζ)∫b0(b−s)ζ−1w(s)ds, | (5.2) |
and
z1=−12[m∑i=1¯Ii(z(ι−i))+2−ζM(ζ−1)w(b)+ζ−1M(ζ−1)Γ(ζ−1)∫b0(b−s)ζ−2w(s)ds]. | (5.3) |
Proof. Using Eq (4.6) and the boundary conditions z(0)=−z(b), z′(0)=−z′(b), we obtain
z1=−z1−m∑i=1¯Ii(z(ι−i))−2−ζM(ζ−1)w(b)−ζ−1M(ζ−1)Γ(ζ−1)∫b0(b−s)ζ−2w(s)ds. |
So, Eq (5.3) is verified. Moreover,
z0=−[z0+bz1+m∑i=1Ii(z(ι−i))+m∑i=1(b−ιi)¯Ii(z(ι−i))+2−ζM(ζ−1)∫b0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫b0(b−s)ζ−1w(s)ds], |
i.e.,
z0=−12[bz1+m∑i=1Ii(z(ι−i))+m∑i=1(b−ιi)¯Ii(z(ι−i))+2−ζM(ζ−1)∫b0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫b0(b−s)ζ−1w(s)ds]. |
This equation along with Eq (5.3) lead to
z0=b(2−ζ)4M(ζ−1)w(b)+b(ζ−1)4M(ζ−1)Γ(ζ−1)∫b0(b−s)ζ−2w(s)ds.−12m∑i=1Ii(z(ι−i))−14m∑i=1(b−2ιi)¯Ii(z(ι−i))−122−ζM(ζ−1)∫b0w(s)ds−12ζ−1M(ζ−1)Γ(ζ)∫b0(b−s)ζ−1w(s)ds]. |
By substituting the values of z0 and z1 into Eq (4.6), we obtain the following
Corollary 5.1. Let w∈PCH1(J,E) with w(0)=0. The solution of system in (5.1) is given by:
z(ι)=(b4−ι2)2−ζM(ζ−1)w(b)+(b4−ι2)∫b0(b−s)ζ−2w(s)ds−122−ζM(ζ−1)∫b0w(s)ds−12ζ−1M(ζ−1)Γ(ζ)∫b0(b−s)ζ−1w(s)ds−12m∑i=1Ii(z(ι−i))−b4m∑i=1¯Ii(z(ι−i))−12m∑i=1(ι−ιi)¯Ii(z(ι−i))+k∑i=1Ii(z(ι−i))+k∑i=1(ι−ιi)¯Ii(z(ι−i))+2−ζM(ζ−1)∫ι0w(s)ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1w(s)ds, where ι∈Jk,k∈N0. | (5.4) |
As a result of Corollary 5.1, we state the following definition.
Definition 5.1. A function z∈PCH2(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 k∈N0, and satisfies the integral equation:
z(ι)=(b4−ι2)2−ζM(ζ−1)f(b,z(b))+(b4−ι2)∫b0(b−s)ζ−2f(s,z(s))ds−122−ζM(ζ−1)∫b0f(s,z(s))ds−12ζ−1M(ζ−1)Γ(ζ)∫b0(b−s)ζ−1f(s,z(s))ds−12m∑i=1Ii(z(ι−i))−b4m∑i=1¯Ii(z(ι−i))−12m∑i=1(ι−ιi)¯Ii(z(ι−i))+k∑i=1Ii(z(ι−i))+k∑i=1(ι−ιi)¯Ii(z(ι−i))+2−ζM(ζ−1)∫ι0f(s,z(s))ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1f(s,z(s))ds, where ι∈Jk,k∈N0. | (5.5) |
Theorem 5.1. Under the assumptions of Theorem 4.2, problem (1.5) has a unique solution provided that
[σb2+σbζ2(ζ−1)+2σb(2−ζ)M(ζ−1)+3σbζ2ζ−1M(ζ−1)Γ(ζ+1)32m∑i=1δi+7b4m∑i=1ηi]<1. | (5.6) |
Proof. Consider the function R:PC(J,E)→PC(J,E) defined as:
R(z)(ι)=(b4−ι2)2−ζM(ζ−1)f(b,z(b))+(b4−ι2)∫b0(b−s)ζ−2f(s,z(s))ds−122−ζM(ζ−1)∫b0f(s,z(s))ds−12ζ−1M(ζ−1)Γ(ζ)∫b0(b−s)ζ−1f(s,z(s))ds−12m∑i=1Ii(z(ι−i))−b4m∑i=1¯Ii(z(ι−i))−12m∑i=1(ι−ιi)¯Ii(z(ι−i))+k∑i=1Ii(z(ι−i))+k∑i=1(ι−ιi)¯Ii(z(ι−i))+2−ζM(ζ−1)∫ι0f(s,z(s))ds+ζ−1M(ζ−1)Γ(ζ)∫ι0(ι−s)ζ−1f(s,z(s))ds,where ι∈Jk,k∈N0. | (5.7) |
Let z,v∈PC(J,E), ι∈Jk,k∈N1. By the assumptions (A2), (A4), and above equality, we have
||R(z)(ι)−R(v)(ι)||≤[σb2+σbζ2(ζ−1)+σb22−ζM(ζ−1)+σbζ2ζ−1M(ζ−1)Γ(ζ+1)+32m∑i=1δi+b4m∑i=1ηi+3b2m∑i=1ηi+σb(2−ζ)M(ζ−1)+σbζ(ζ−1)M(ζ−1)Γ(ζ+1)]||z−v||=[σb2+σbζ2(ζ−1)+2σb(2−ζ)M(ζ−1)+3σbζ2ζ−1M(ζ−1)Γ(ζ+1)+32m∑i=1δi+7b4m∑i=1ηi]||z−v||. |
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:Λ→2E with non-empty closed, bounded and convex values is called ρ-Lipschitz if
h(G(x)−G(y))≤ρ ||x−y||Λ,∀x,y∈Λ, |
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:T→2Lp(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:T→2Lp(Ω,Rn) such that f(t)∈G(t),a.e, and ||f(z)−f(v)||≤ξG ρ||z−v||Lp(Ω,Rn), ∀z,v∈T, 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),i∈N1 be functions such that
‖Ii(x)−Ii(y)‖≤δi‖x−y‖,∀x∈L2(J,R),∀i∈N1, |
and
‖¯Ii(x)−¯Ii(y)‖≤ηi‖x−y‖,∀x∈L2(J,R),∀i∈N1, |
where δiηi, are positive real numbers, then problem (1.6) has a solution provided that F(0,z0)={0} and
k∑i=1(δi+ηi)+ξF ρ(2−ζ)bM(ζ−1)+σ(ζ−1)bζM(ζ−1)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))=|ι1−ι2|+||x1−x2||E. By Lemma 6.1, there exists f: J×E→E satisfying f(ι,x)∈F(ι,x),a.e., and
||f(ι,x)−f(s,y)||≤ξF ρ(|ι−s|+||x−y||E), ∀(ι,x),(s,y)∈T. |
By applying Theorem (4.2), the following fractional boundary problem
{ABCDζ0,ιz(ι)=f(ι,z(ι)),ι∈J−{ι1,ι2,…,ιm}, z(0)=z0, z′(0)=z1,z(ι+i)=z(ι−i)+Ki(z(ι−i)), i=1,2,…,m,z′(ι+i)=z′(ι−i)+¯Ki(z(ι−i)), 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 ι∈J−{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×E→E by
f(w,ς)(η)=sinw√π+λς2(η); w∈J, ς∈E, η∈[0,π], | (6.2) |
where λ>0. Thus, f(0,z0)(η)=0;∀η∈[0,π]. For any ς1,ς2∈E=L2[0,π] and any w1,w2∈J, we have
||f(w1,ς1)−f(w2,ς2)||L2[0,π]=(∫π01√π|(sinw1−sinw2)+λ2(ς21(η)−ς22(η))|2dη)12≤(∫π01√π|sinw1−sinw2|2dη)12+λ(∫π0|ς21(η)−ς22(η)|2dη)12≤|sinw1−sinw2|+λ(∫π0|(ς1(η))+ς2(η)) (ς1(η))−ς2(η))|2dη)12≤|w1−w2|+λ|<ς1+ς2,ς1−ς2>|≤|w1−w2|+λ||ς1+ς2|| ||ς1−ς2||≤|w1−w2|+λ(||ς1||+||ς2||) ||ς1−ς2||. |
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)[(2−ζ)M(ζ−1)+(ζ−1)M(ζ−1)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)=sinι√π+ς2(s), ι∈J, ς∈E, s∈[0,π],z(0)=z0,z(1)=z1, | (6.4) |
(see relation (3.6)).
The inequality (6.3) is equivalent to
4λωr2−r+||z1||+2ω<0, | (6.5) |
where ω=(2−ζ)M(ζ−1)+(ζ−1)M(ζ−1)Γ(ζ).
If 16 λ ω(||z1||+2ω)<1, then the equation 4ωλr2−r+||z1||+2ω=0 has two positive solutions, namely
r1=1−√1−16λω(||z1||+2ω)8ω and r2=1+√1−16λω(||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×E→E by:
f(w,ς)(η):=sinw√π+σsinς(η); w∈J, ς∈E, η∈[0,π], | (6.7) |
where, σ>0. Let z0:[0,π]→R, be the zero function and z1∈L2[0,π] be a fixed function. Note that f(0,z0)(η)=0, ∀η∈[0,π]. For every ς1,ς2∈E=L2[0,π] and every w1,w2∈J, we have
||f(w,ς1)−f(w,ς2)||L2[0,π]=σ(∫π0|sinς1(η)−sinς2(η)|2dη)12≤σ(∫π0|ς1(η)−ς2(η)|2dη)12=σ||ς1−ς2||L2[0,π]≤σ||ς1−ς2||L2[0,π]. |
Thus, (A2) is satisfied. By applying Theorem 3.2, there is a unique z:[0,1]→L2[0,π] such that z′∈H1((0,1),L2[0,π]) and z satisfies the boundary value problem:
{ABCDζ0,ιz(ι)(η)=sinι√π+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(2−ζ)M(ζ−1)+2(ζ−1)σM(ζ−1)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),∀x∈E, 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)=sinι√π+υsin(z(ι)η), ι∈[0,1]−{0,12},η∈[0,π],z(0)=z0, z′(0)=z1,z(ι+1)=z(ι−1)+I1(z(ι−1)),z′(ι+1)=z′(ι−1)+¯I1(z(ι−1)), | (6.10) |
has a solution provided that
2λ+σ(2−ζ)M(ζ−1)+σ(ζ−1)M(ζ−1)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.
[1] | V. E. Tarasov, Applications in physics, part A, In: Handbook of fractional calculus with applications, De Gruyter, 4 (2019). https://doi.org/10.1515/9783110571707 |
[2] | D. Baleanu, A. M. Lopes, Applications in engineering, life and social sciences, part A, In: Handbook of fractional calculus with applications, De Gruyter, 7 (2019). https://doi.org/10.1515/9783110571905 |
[3] | B. F. Martínez-Salgado, R. Rosas-Sampayo, A. Torres-Hernández, C. Fuentes, Application of fractional calculus to oil industry, In: Fractal analysis applications in physics, engineering and technology, 2017. https://doi.org/10.5772/intechopen.68571 |
[4] |
G. U. Varieschi, Applications of fractional calculus to Newtonian Mechanics, J. Appl. Math. Phys., 6 (2018), 1247–1257. https://doi.org/10.4236/jamp.2018.66105 doi: 10.4236/jamp.2018.66105
![]() |
[5] | J. F. Douglas, Some applications of fractional calculus to polymer science, In: Advances in chemical physics, 102 (1997). https://doi.org/10.1002/9780470141618.ch3 |
[6] |
M. Al Nuwairan, Bifurcation and analytical solutions of the space-fractional stochastic schrödinger equation with white noise, Fractal Fract., 7 (2023), 157. https://doi.org/10.3390/fractalfract7020157 doi: 10.3390/fractalfract7020157
![]() |
[7] | A. A. Kilbas, H. M. Srivastava, J. J. Trujillo, Theory and applications of fractional differential equations, In: North-Holland mathematics studies, Elsevier, 2006. |
[8] |
A. Aldhafeeri, M. Al Nuwairan, Bifurcation of some novel wave solutions for modified nonlinear Schrödinger equation with time M-fractional derivative, Mathematics, 11 (2023), 1219. https://doi.org/10.3390/math11051219 doi: 10.3390/math11051219
![]() |
[9] |
M. Almulhim, M. Al Nuwairan, Bifurcation of traveling wave solution of Sakovich equation with beta fractional derivative, Fractal Fract., 7 (2023), 372. https://doi.org/10.3390/fractalfract7050372 doi: 10.3390/fractalfract7050372
![]() |
[10] |
M. Arfan, K. Shah, T. Abdeljawad, N. Mlaiki, A. Ullah, A Caputo power law model predicting the spread of the COVID-19 outbreak in Pakistan, Alex. Eng. J., 60 (2021), 447–456. https://doi.org/10.1016/j.aej.2020.09.011 doi: 10.1016/j.aej.2020.09.011
![]() |
[11] |
S. Ahmad, A. Ullah, Q. M. Al-Mdallal, H. Khan, K. Shah, A. Khan, Fractional order mathematical modeling of COVID-19 transmission, Chaos Soliton Fract., 139 (2020), 110256. https://doi.org/10.1016/j.chaos.2020.110256 doi: 10.1016/j.chaos.2020.110256
![]() |
[12] |
A. I. K. Butt, M. Imran, S. Batool, M. Al Nuwairan, Theoretical analysis of a COVID-19 CF-fractional model to optimally control the spread of pandemic, Symmetry, 15 (2023), 380. https://doi.org/10.3390/sym15020380 doi: 10.3390/sym15020380
![]() |
[13] | M. Caputo, M. Fabrizio, A new definition of fractional derivative without singular kernel, Prog. Fract. Differ. Appl., 1 (2015), 73–85. |
[14] |
A. Atangana, D. Baleanu, New fractional derivative with non-local and non-singular kernel: Theory and application to heat transfer model, Therm. Sci., 20 (2016), 763–769. https://doi.org/10.2298/TSCI160111018A doi: 10.2298/TSCI160111018A
![]() |
[15] |
K. A. Abro, A. Atangana, A comparative analysis of electromechanical model of piezoelectric actuator through Caputo-Fabrizio and Atangana-Baleanu fractional derivatives, Math. Meth. Appl. Sci., 43 (2020), 9681–9691. https://doi.org/10.1002/mma.6638 doi: 10.1002/mma.6638
![]() |
[16] |
B. Ghanbari, A. Atangana, A new application of fractional Atangana-Baleanu derivatives: Designing ABC-fractional masks in image processing, Physica A, 542 (2020), 123516. https://doi.org/10.1016/j.physa.2019.123516 doi: 10.1016/j.physa.2019.123516
![]() |
[17] |
M. A. Khan, A. Atangana, Modeling the dynamics of novel coronavirus (2019-nCov) with fractional derivative, Alex. Eng. J., 59 (2020), 2379–2389. https://doi.org/10.1016/j.aej.2020.02.033 doi: 10.1016/j.aej.2020.02.033
![]() |
[18] |
D. Baleanu, M. Inc, A. Yusuf, A. Aliyu, Optimal system, nonlinear self-adjointness and conservation law for generalized shallow water wave equation, Open Phys., 16 (2018), 364–370. https://doi.org/10.1515/phys-2018-0049 doi: 10.1515/phys-2018-0049
![]() |
[19] |
T. Abdeljawad, D. Baleanu, Integration by parts and its applications of a new nonlocal fractional derivative with Mittag-Leffler nonsingular kernel, J. Nonlinear Sci. Appl., 10 (2017), 1098–1107. http://dx.doi.org/10.22436/jnsa.010.03.20 doi: 10.22436/jnsa.010.03.20
![]() |
[20] |
T. Abdeljawad, A Lyapunov type inequality for fractional operators with nonsingular Mittag-Leffler kernel, J. Inequal. Appl., 2017 (2017), 130. https://doi.org/10.1186/s13660-017-1400-5 doi: 10.1186/s13660-017-1400-5
![]() |
[21] |
M. S. Abdo, T. Abdeljawad, S. M. Ali, K. Shah, On fractional boundary value problems involving fractional derivatives with Mittag-Leffler kernel and nonlinear integral conditions, Adv. Differ. Equ., 2021 (2021), 37. https://doi.org/10.1186/s13662-020-03196-6 doi: 10.1186/s13662-020-03196-6
![]() |
[22] |
F. Jarad, T. Abdeljawad, Z. Hammouch, On a class of ordinary differential equations in the frame of Atangana-Baleanu fractional derivative, Chaos Soliton Fract., 117 (2018), 16–20. https://doi.org/10.1016/j.chaos.2018.10.006 doi: 10.1016/j.chaos.2018.10.006
![]() |
[23] |
Asma, S. Shabbir, K. Shah, T. Abdeljawad, Stability analysis for a class of implicit fractional differential equations involving Atangana-Baleanu fractional derivative, Adv. Differ. Equ., 2021 (2021), 395. https://doi.org/10.1186/s13662-021-03551-1 doi: 10.1186/s13662-021-03551-1
![]() |
[24] | A. Devi, A. Kumar, Existence and uniqueness results for integro fractional differential equations with Atangana-Baleanu fractional derivative, J. Math. Ext., 15 (2021). |
[25] |
M. Al Nuwairan, A. G. Ibrahim, Nonlocal impulsive differential equations and inclusions involving Atangana-Baleanu fractional derivative in infinite dimensional spaces, AIMS Mathematics, 8 (2023), 11752–11780. https://doi.org/10.3934/math.2023595 doi: 10.3934/math.2023595
![]() |
[26] |
X. Liu, G. Ballinger, Boundedness for impulsive delay differential equations and applications in populations growth models, Nonlinear Anal. Theor., 53 (2003), 1041–1062. https://doi.org/10.1016/S0362-546X(03)00041-5 doi: 10.1016/S0362-546X(03)00041-5
![]() |
[27] | K. Church, Applications of impulsive differential equations to the control of malaria outbreaks and introduction to impulse extension equations: A general framework to study the validity of ordinary differential equation models with discontinuities in state, University of Ottawa, 2014. https://doi.org/10.20381/RUOR-6771 |
[28] | H. F. Xu, Q. X. Zhu, W. X. Zheng, Exponential stability of stochastic nonlinear delay systems subject to multiple periodic impulses, IEEE Trans. Autom. Control, 2023. https://doi.org/10.1109/TAC.2023.3335005 |
[29] |
A. G. Ibrahim, Differential equations and inclusions of fractional order with impulse effect in Banach spaces, Bull. Malays. Math. Sci. Soc., 43 (2020), 69–109. https://doi.org/10.1007/s40840-018-0665-2 doi: 10.1007/s40840-018-0665-2
![]() |
[30] | J. R. Wang, A. G. Ibrahim, D. O'Regan, Nonemptyness and compactness of the solution set for fractional evolution inclusions with non-instantaneous impulses, Electron. J. Differ. Eq., 2019 (2019), 1–17. |
[31] |
J. R. Wang, A. G. Ibrahim, D. O'Regan, A. A. Elmandouh, Nonlocal fractional semilinear differential inclusions with noninstantaneous impulses of order α∈(1,2), Int. J. Nonlinear Sci. Numer. Simul., 22 (2021), 593–605. https://doi.org/10.1515/ijnsns-2019-0179 doi: 10.1515/ijnsns-2019-0179
![]() |
[32] |
R. Agarwal, S. Hristova, D. O'Regan, Noninstantaneous impulses in Caputo fractional differential equations and practical stability via Lyapunov functions, J. Franklin Inst., 354 (2017), 3097–3119. https://doi.org/10.1016/j.jfranklin.2017.02.002 doi: 10.1016/j.jfranklin.2017.02.002
![]() |
[33] |
K. Liu, Stability analysis for (w,c)-periodic non-instantaneous impulsive differential equations, AIMS Mathematics, 7 (2022), 1758–1774. https://doi.org/10.3934/math.2022101 doi: 10.3934/math.2022101
![]() |
[34] |
E. Kaslik, S. Sivasundaram, Non-existence of periodic solutions in fractional-order dynamical systems and a remarkable difference between integer and fractional-order derivatives of periodic functions, Nonlinear Anal. Real World Appl., 13 (2012), 1489–1497. https://doi.org/10.1016/j.nonrwa.2011.11.013 doi: 10.1016/j.nonrwa.2011.11.013
![]() |
[35] |
Y. Alruwaily, S. Aljoudi, L. Almaghamsi, A. Ben Makhlouf, N. Alghamdi, Existence and uniqueness results for different orders coupled system of fractional integro-differential equations with anti-periodic nonlocal integral boundary conditions, Symmetry, 15 (2023), 182. https://doi.org/10.3390/sym15010182 doi: 10.3390/sym15010182
![]() |
[36] |
R. P. Agarwal, B. Ahmad, A. Alsaedi, Fractional-order differential equations with anti-periodic boundary conditions: A survey, Bound. Value Probl., 2017 (2017), 173. https://doi.org/10.1186/s13661-017-0902-x doi: 10.1186/s13661-017-0902-x
![]() |
[37] |
B. Ahmad, Y. Alruwaily, A. Alsaedi, J. J. Nieto, Fractional integro-differential equations with dual anti-periodic boundary conditions, Differ. Integral Equ., 33 (2020), 181–206. https://doi.org/10.57262/die/1584756018 doi: 10.57262/die/1584756018
![]() |
[38] |
B. Ahmad, V. Otero-Espinar, Existence of solutions for fractional differential inclusions with antiperiodic boundary conditions, Bound. Value Probl., 2009 (2009), 625347. https://doi.org/10.1155/2009/625347 doi: 10.1155/2009/625347
![]() |
[39] |
A. G. Ibrahim, Fractional differential inclusions with anti-periodic boundary conditions in Banach spaces, Electron. J. Qual. Theory Differ. Equ., 65 (2014), 1–32. https://doi.org/10.14232/ejqtde.2014.1.65 doi: 10.14232/ejqtde.2014.1.65
![]() |
[40] |
J. R. Wang, A. G. Ibrahim, M. Feckan, Differential inclusions of arbitrary fractional order with anti-periodic conditions in Banach spaces, Electron. J. Qual. Theory Differ. Equ., 34 (2016), 1–22. https://doi.org/10.14232/ejqtde.2016.1.34 doi: 10.14232/ejqtde.2016.1.34
![]() |
[41] |
T. Abdeljawad, S. T. M. Thabet, T. Kedim, M. I. Ayari, A. Khan, A higher-order extension of Atangana-Baleanu fractional operators with respect to another function and a Gronwall-type inequality, Bound. Value Probl., 2023 (2023), 49. https://doi.org/10.1186/s13661-023-01736-z doi: 10.1186/s13661-023-01736-z
![]() |
[42] |
K. K. Saha, N. Sukavanam, S. Pan, Existence and uniqueness of solutions to fractional differential equations with fractional boundary conditions, Alex. Eng. J., 72 (2023), 147–155. https://doi.org/10.1016/j.aej.2023.03.076 doi: 10.1016/j.aej.2023.03.076
![]() |
[43] |
K. Diethelm, V. Kiryakova, Y. Luchko, J. A. Tenreiro Machado, V. E. Tarasov, Trends, directions for further research, and some open problems of fractional calculus, Nonlinear Dyn., 107 (2022), 3245–3270. https://doi.org/10.1007/s11071-021-07158-9 doi: 10.1007/s11071-021-07158-9
![]() |
[44] |
W. Saleh, A. Lakhdari, A. Kilicman, A. Frioui, B. Meftah, Some new fractional Hermite-Hadamard type inequalities for functions with co-ordinated extended (s,m)-prequasiinvex mixed partial derivatives, Alex. Eng. J., 72 (2023), 261–267. https://doi.org/10.1016/j.aej.2023.03.080 doi: 10.1016/j.aej.2023.03.080
![]() |
[45] |
M. I. Syam, M. Al-Refai, Fractional differential equations with Atangana-Baleanu fractional derivative: Analysis and applications, Chaos Soliton Fract., 2 (2019), 100013. https://doi.org/10.1016/j.csfx.2019.100013 doi: 10.1016/j.csfx.2019.100013
![]() |
[46] |
S. T. Sutar, K. D. Kucche, Existence and data dependence results for fractional differential equations involving Atangana-Baleanu derivative, Rend. Circ. Mat. Palermo II Ser., 71 (2022), 647–663. https://doi.org/10.1007/s12215-021-00622-w doi: 10.1007/s12215-021-00622-w
![]() |
[47] |
T. Cardinali, P. Rubbioni, Impulsive mild solution for semilinear differential inclusions with nonlocal conditions in Banach spaces, Nonlinear Anal. Theor., 75 (2012), 871–879. https://doi.org/10.1016/j.na.2011.09.023 doi: 10.1016/j.na.2011.09.023
![]() |
[48] | M. I. Kamenskii, V. V. Obukhowskii, P. Zecca, Condensing multivalued maps and semilinear differential inclusions in Banach spaces, De Gruyter, 2001. https://doi.org/10.1515/9783110870893 |
[49] | D. Bothe, Multivalued perturbation of m-accerative differential inclusions, Israel J. Math. 108 (1998), 109–138. https://doi.org/10.1007/BF02783044 |
[50] | S. Hu, N. S. Papageorgiou, Handbook of multivalued analysis, In: Mathematics and its applications, New York: Springer, 1997. |
[51] | C. Rom, On Lipschitz selections of multifunctions with decomposable values, Bulletin Polish Acad. Sci. Math., 57 (2009), 121–127. |
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