Research article

Existence of local and global solutions to fractional order fuzzy delay differential equation with non-instantaneous impulses

  • Received: 09 September 2021 Accepted: 01 November 2021 Published: 11 November 2021
  • MSC : 03B52, 34A07, 34A08, 34A37

  • The main concern of this manuscript is to examine some sufficient conditions under which the fractional order fuzzy delay differential system with the non-instantaneous impulsive condition has a unique solution. We also study the existence of a global solution for the considered system. Fuzzy set theory, Banach fixed point theorem and Non-linear functional analysis are the major tools to demonstrate our results. In last, an example is given to illustrate these analytical results.

    Citation: Anil Kumar, Muslim Malik, Mohammad Sajid, Dumitru Baleanu. Existence of local and global solutions to fractional order fuzzy delay differential equation with non-instantaneous impulses[J]. AIMS Mathematics, 2022, 7(2): 2348-2369. doi: 10.3934/math.2022133

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  • The main concern of this manuscript is to examine some sufficient conditions under which the fractional order fuzzy delay differential system with the non-instantaneous impulsive condition has a unique solution. We also study the existence of a global solution for the considered system. Fuzzy set theory, Banach fixed point theorem and Non-linear functional analysis are the major tools to demonstrate our results. In last, an example is given to illustrate these analytical results.



    The dynamics of many evolutionary processes are characterized by the fact that at a specific moment of time they experience a sudden change in their state, such as harvesting, natural disasters and shocks, etc. These processes are subject to short-term perturbations, whose time period is minimal in analogy with the whole evolution. In dynamical systems associated with such sudden changes, we assume these changes in the form of impulses. Therefore, impulsive differential equations have been developed to model these types of situations. In literature, there are two types of impulses, one is instantaneous and another one is non-instantaneous impulses. For more detail, one can see [1-4].

    The theory of fractional calculus deals with the integral and derivative of any arbitrary (real or complex) order. It was first proposed in the works by mathematicians Leibniz, Abel, L'Hopital, Riemann, Liouville [5,6]. Because of the nonlocality and inherent properties of numerous complex systems, fractional calculus is important to model many physical applications in dissimilar branches of science and engineering. Memory and hereditary are additionally significant properties of various materials and processes in biomechanics, electrical circuits, electrochemistry, biology, electromagnetic processes, control and porous media, which are widely recognized to be well predicted by using fractional differential operators [7-9]. In the existing literature, there are numerous definitions for fractional operators, for example, Riemann-Liouville, Grunwald-Letnikov, Hadamard, Caputo, Riesz-Caputo and so on.

    More recently, in 2015, Caputo and Fabrizio introduced a new fractional derivative known as Caputo-Fabrizio fractional derivative which is given by

    CFDςa+P(ξ)=M(ς)1ςξaexp[ς1ς(ξϑ)]P(ϑ)dϑ,

    where ςR is the order of the derivative[10,11]. A year after, Atangana and Baleanu proposed another definition of nonlocal derivatives with non-singular kernel relied on the Mittag-Leffler function

    ABCDςa+P(ξ)=B(ς)1ςξaEς[ς1ς(ξϑ)ς]P(ϑ)dϑ,

    where PCF(I)LF(I) is the fuzzy function and B(ς)=(1ς)+ςΓ(ς) is known as a normalization function which satisfies B(0)=B(1)=1 and 0<ς<1. This definition upheld the Caputo-Fabrizio's one relied on the exponential function. It expand the profundity of the connection between the Mittag-Leffler function and fractional calculus which leads to the significant applications such as thermal physics, population dynamics, control problems and so on [12-15].

    On the other hand, in many real applications there is some uncertainty that occurs in the system due to that the behaviour of the system is affected. Therefore, to overcome this type of issue, Zadeh [16] in 1965, presented the theory of fuzzy set by using the membership function. The theory of fuzzy set is a well-built tool for modelling the uncertainty, ambiguity and vague information such as particle system, medicine, quantum optics, civil engineering, computational biology, bioinformatics and hydraulic process [17-20] etc. Moreover, the nonlocal effects, as well as uncertainty behaviours, represent interesting phenomena and hence nowadays many researchers working on the fuzzy fractional operator which combine fractional calculus with the fuzzy set theory. In the last few decays, many authors established some results on the existence, uniqueness and stability of the solution for fuzzy differential equations of an integer as well as fractional order [21-28]. In particular, S. Seikkala [21], established the existence and uniqueness of the solution for a fuzzy initial value problem. In [25], authors investigated the existence and uniqueness of solution for the fractional fuzzy differential equation. In [26], authors examined the uniqueness of the solution for a nonlinear impulsive fuzzy integro-differential equation. In [27] authors examined the existence and uniqueness of a mild solution to a nonlinear fuzzy differential equation with time delay. Moreover, there are only a few papers that established the existence and uniqueness results for ABC fuzzy fractional differential equation [29,30]. For instance, in [30] authors considered the ABC fractional fuzzy differential equation and establish the existence and uniqueness of the solution. As per the author's knowledge, there is not a single paper that established the existence of local and global solutions for the ABC fractional fuzzy delay differential system with impulsive effects.

    Therefore, motivated by the above facts, in this paper, we will study the existence of local and global solution for fractional order fuzzy delay differential equation with non-instantaneous impulsive condition of the form

    ABC     0DςξP(ξ)=H(ξ,P(ξ),P(ξδ)),ξ(kj,ξj+1], j=0,1,,n,P(ξ)=hj(ξ,P(ξj)), ξ(ξj,kj],j=1,2,,n,P(ξ)=Ψ(ξ),ξ[δ,0], (1.1)

    where P is a state fuzzy function and ABC     0Dςξ is the ABC derivative of order ς(0,1). The points kj and ξj satisfies the sequence 0=k0=ξ0<ξ1<k1<ξ2<<ξn<kn<ξn+1=T<. H is the nonlinear function which is defined from (kj,ξj+1]×Kn×Kn into Kn, where Kn denotes the set of all upper semi continuous convex normal fuzzy number with bounded ι-level intervals and j=0,1,,n (which will be specified in Definition 2.9). The functions hj(ξ,P(ξj)) represent non-instantaneous impulses during the interval (ξj,kj], j=1,2,,n. P(ξj), P(ξ+j) represent the left and right limit of the state fuzzy function P at ξj. For δ>0, Ψ:[δ,0]Kn is a continuous function.

    The structure of the manuscript is as follows: In Section 2, we have given the fundamental definitions and some important lemmas. In Section 3, we establish the local existence and uniqueness results for the solution. Section 4 is devoted to establishing the global solution for the considered system and in the last Section 5, an example is given to validate the obtained analytical results.

    In this section, we briefly describe some notations, fundamental definitions and important lemmas which are useful to prove the main results. CF(I=[0,T]) denote the set of all continuous fuzzy valued functions on I and LF(I) denote the set of all Lebesgue integrable fuzzy valued functions on I. Also we define PC(J;Kn) as: PC(J;Kn)={P:JKn:PCF([δ,0); Kn)  CF((ξj,ξj+1]; Kn), j=0,1,,n and there exists P(ξj) and P(ξ+j),j=1,2,,n, with P(ξj)=P(ξj)} for the space of piecewise continuous functions, where J=[δ,0)[0,T].

    Next, we define the definition of ABC derivative and integrals.

    Definition 2.1. [31] The Atangana-Baleanu fractional integral of order ς(0,1), is given by

    ABaIςP(ξ)=1ςB(ς)P(ξ)+ςB(ς)Γ(ς)ξa(ξϑ)(ς1)P(ϑ)dϑ,Pa,

    where PCF(I)LF(I) is the fuzzy function and B(ς)=(1ς)+ςΓ(ς) is known as the normalization function which satisfies B(0)=B(1)=1.

    Definition 2.2. [31] The Atangana-Baleanu fractional fuzzy derivative in Caputo sense is defined by

    ABCDςa+P(ξ)=B(ς)1ςξaEς[ς1ς(ξϑ)ς]P(ϑ)dϑ,

    where PCF(I)LF(I) is the fuzzy function and Eς is the Mittag-Leffler function.

    Definition 2.3. For ABC derivative, we have the following important properties of Laplace transformation

    1) L(ABCDςa+P(ξ))=B(ς)1ςsς1sς+ς1ς(sP(s)P(0)),

    2) L(ξς)=ςsς+1,

    3) L(Hn(ξ))=snL(H(ξ))sn1H(0)H(n1)(0),

    4) L(u(ξ)P(ξ))=L(u(ξ))L(P(ξ)).

    Now, we define some important definitions and lemmas which are often used.

    Definition 2.4. [32] Let ϰ and α be two nonempty bounded subsets of Rn then we define

    dH(ϰ,α)=max{supˆϰϰinfˆαα||ˆϰˆα||,supˆααinfˆϰϰ||ˆϰˆα||},

    where ||.|| denotes the usual Euclidean norm in Rn. Clearly, dH(ϰ,α)=dH(α,ϰ), i.e., it is symmetric on ϰ and α.

    Consequently, for any nonemptey subsets ϰ,α and Θ of Rn, we have

    (1) dH(ϰ,α)0 with dH(ϰ,α)=0 iff ϰ=α,

    (2) dH(ϰ,α)=dH(α,ϰ),

    (3) dH(ϰ,α)dH(ϰ,Θ)+dH(Θ,α).

    We denote Kn(Rn) for the family of all nonempty subset of Rn which are convex and compact. The scalar multiplication and addition in Kn(Rn) are defined as

    ϰ+α={ˆϰ+ˆα:ˆϰϰ and ˆαα},ϱϰ={ϱˆϰ:ˆϰϰ}

    for all ϱ0 and ϰ,αKn(Rn).

    Definition 2.5. [32] We define

    dH([z]ι,[y]ι)=max{d([z]ι,[y]ι),d([y]ι,[z]ι):ι(0,1]}, z,y,Kn.

    Clearly, (Kn(Rn),dH) forms a complete metric space.

    Definition 2.6. [32] The supremium metric d on Kn is defined by

    d(z,y)=sup{dH([z]ι,[y]ι):ι(0,1],  z,yKn}.

    Clearly, we can see that d is a metric in Kn and (Kn,d) forms a complete metric space.

    Suppose that J=[δ,T]R be a compact interval and PC(J;Kn) denotes tha space of all fuzzy functions which are piece-wise continuous from J to Kn. We define the metric H1 on PC(J;Kn) by

    H1(z,y)=sup{d(z(ξ),y(ξ)) : ξJ,  z,yPC(J;Kn)}.

    Clearly, (PC(J;Kn),H1) is a complete metric space.

    Definition 2.7. [33] A membership function ΩD:Ξ[0,1] of fuzzy set D satisfy the following:

    1) If ΩD(ρ)=1, then ρ is completely belongs to D,

    2) If 0<ΩD(ρ)<1, then ρ is partially belongs to D,

    3) If ΩD(ρ)=0, then ρD.

    Definition 2.8. [33] A fuzzy set D is said to be fuzzy number if it satisfy the following properties:

    1) D is normal, i.e.,  ρ0R with ΩD(ρ0)=1.

    2) D is fuzzy convex, i.e., ΩD(ξρ+(1ξ)ˆρ)min{ΩD(ρ),ΩD(ˆρ)},  ξ[0,1],ρ,ˆρRn.

    3) D is upper semi continuous on Rn, i.e.,  ϵ>0,  τ>0 such that ΩD(ρ)ΩD(ρ0)<ϵ,|ρρ0|<τ.

    4) D is compactly supported, i.e., cl{ρRn;ΩD(ρ)>0} is compact.

    Definition 2.9. [34] The ι - level set of fuzzy set D is defined by

    [D]ι={ρ|ρΞ,ΩD(ρ)ι},ι(0,1],

    and for ι=0, we have

    [D]0=cl{ρ|ρΞ,ΩD(ρ)0}.

    Definition 2.10. [34] A fuzzy number gR is called positive if for two arbitrary fuzzy number g1,g2, it holds 0<g1<g2 for the support ψg=[g1,g2] of g, i.e., ψg is in the positive real line. Similarly, g is called negative if g1g2<0 and zero if g10g2.

    Lemma 2.1. [35] If g,hKn, then for ι(0,1],

    [g+h]ι=[gιa+hιa,gιb+hιb].[g×h]ι=[min{hιihιj},max{hιihιj}],i,j=a,b.[gh]ι=[gιahιb,gιbhιa].

    Definition 2.11. [35] We define the fuzzy integral as follows

    [ba[P(ξ)dξ]]ι=[baPιq(ξ)dξ,baPιr(ξ)dξ], a,bI,

    provided that the right side Lebesgue integrals in the above equation are exists. Also, the fuzzy integral is a fuzzy number.

    Lemma 2.2. [30] If y(ξ)CF(I)LF(I), 0<ς<1, then the unique solution of following problem

    ABC     0Dςξy(ξ)=u(ξ),

    is given by

    y(ξ)=1ςB(ς)u(ξ)+ςB(ς)Γ(ς)ξ0u(τ)(ξτ)ς1dτ.

    Lemma 2.3. A function PPC(J;Kn) is the solution of the considered system (1.1) if H(0,P(0),P(δ))=0 holds and solution is given by

    P(ξ)={Ψ(ξ),ξ[δ,0),Ψ(0)+1ςB(ς)H(ξ,P(ξ),P(ξδ))+ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ, ξ[0,ξ1],hj(ξ,P(ξj)),ξ(ξj,kj],j=1,2,,n,hj(kj,P(ξj))+ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ+1ςB(ς)H(ξ,P(ξ),P(ξδ)),ξ(kj,ξj+1],j=1,2,,n. (2.1)

    Proof. From Lemma 2.2, for any ξ[0,ξ1], we have

    P(ξ)=Ψ(0)+1ςB(ς)H(ξ,P(ξ),P(ξδ))+ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ.

    Now, for any ξ(ξ1,k1],

    P(ξ)=h1(k1,P(ξ1)).

    Also, for any ξ(k1,ξ2],

    P(ξ)=P(ξ)+ςB(ς)Γ(ς)ξk1(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ+1ςB(ς)H(ξ,P(ξ),P(ξδ)),=h1(k1,P(ξ1))+ςB(ς)Γ(ς)ξk1(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ+1ςB(ς)H(ξ,P(ξ),P(ξδ)).

    Now, for any ξ(ξ2,k2],

    P(ξ)=h2(k2,P(ξ2)).

    Also, for any ξ(k2,ξ3],

    P(ξ)=P(ξ2)+ςB(ς)Γ(ς)ξk2(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ+1ςB(ς)H(ξ,P(ξ),P(ξδ)),=h2(k2,P(ξ2))+ςB(ς)Γ(ς)ξk2(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ+1ςB(ς)H(ξ,P(ξ),P(ξδ)).

    By using the similar process, we will get for ξ(kj,ξj+1],

    P(ξ)=hj(kj,P(ξj))+ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ+1ςB(ς)H(ξ,P(ξ),P(ξδ)),

    which has the form (2.1). Hence, the result follows. For more detail on solution, please see [36].

    In this section, we state and prove the existence and uniqueness of local solution to the system (1.1). For this purpose, the following assumptions are required:

    (B1) The function H:(kj,ξj+1]×Kn×KnKn, j=0,1,,n, is continuous and there exists positive constant MH1 and MH2 such that

    dH([H(ξ,η1,η2)]ι,[H(ξ,γ1,γ2)]ι)MH1dH([η1]ι,[γ1]ι)+MH2dH([η2]ι,[γ2]ι),  η1,γ1,η2,γ2Kn.

    (B2) The functions hj:(ξj,kj]×KnKn, j=1,2,,n, are continuous and there exists a positive constants Mhj<1 such that

    dH([hj(ξ,η1)]ι,[hj(ξ,γ1)]ι)MhjdH([η1]ι,[γ1)]ι),  η1,γ1Kn,ξ(ξj,kj].

    For the convenience, we use the following notations throughout the manuscript L=max1jn{L1,L2j}, where L1=(1ςB(ς)(MH1+MH2)+ςB(ς)Γ(ς)(MH1+MH2)Tς) and L2j=(Mhj+1ςB(ς)(MH1+MH2)+ςB(ς)Γ(ς)(MH1+MH2)Tς), j=1,2,,n.

    Theorem 3.1. If the assumptions (B1) and (B2) are satisfied then the problem (1.1) has a unique local solution on J.

    Proof. For each ηPC(J;Kn), we define an operator Λ:PC(J;Kn)PC(J;Kn) such that

    (Λη)(ξ)={Ψ(ξ),ξ[δ,0),Ψ(0)+1ςB(ς)H(ξ,η(ξ),η(ξδ))+ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ,ξ[0,ξ1],hj(ξ,η(ξj)), ξ(ξj,kj],j=1,2,,n,hj(kj,η(ξj))+1ςB(ς)H(ξ,η(ξ),η(ξδ))+ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ,ξ(kj,ξj+1],j=1,2,,n.

    Here, we need to show that the operator Λ has a fixed point, which is the solution of our considered system (1.1). The proof of this theorem is divided into the following cases:

    Case 1: For ξ[δ,0), η,γPC(J;Kn),

    (Λη)(ξ)=Ψ(ξ),(Λγ)(ξ)=Ψ(ξ).

    Hence,

    H1((Λη),(Λγ))=0.

    Case 2: For ξ[0,ξ1], η,γPC(J;Kn),

    (Λη)(ξ)=Ψ(0)+1ςB(ς)H(ξ,η(ξ),η(ξδ))+ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ,(Λγ)(ξ)=Ψ(0)+1ςB(ς)H(ξ,γ(ξ),γ(ξδ))+ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,γ(ϑ),γ(ϑδ))dϑ.

    Therefore,

    dH([Λη(ξ)]ι,[Λγ(ξ)]ι)=dH([Ψ(0)+1ςB(ς)H(ξ,η(ξ),η(ξδ))+ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ]ι,[Ψ(0)+1ςB(ς)H(ξ,γ(ξ),γ(ξδ))+ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,γ(ϑ),γ(ϑδ))dϑ]ι)=dH([Ψ(0)]ι+[1ςB(ς)H(ξ,η(ξ),η(ξδ))]ι+[ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ]ι,[Ψ(0)]ι+[1ςB(ς)H(ξ,γ(ξ),γ(ξδ))]ι+[ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,γ(ϑ),γ(ϑδ))dϑ]ι)=dH([1ςB(ς)H(ξ,η(ξ),η(ξδ))]ι+[ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ]ι,[1ςB(ς)H(ξ,γ(ξ),γ(ξδ))]ι+[ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,γ(ϑ),γ(ϑδ))dϑ]ι)dH([1ςB(ς)H(ξ,η(ξ),η(ξδ))]ι,[1ςB(ς)H(ξ,γ(ξ),γ(ξδ))]ι)+dH([ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ]ι, [ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,γ(ϑ),γ(ϑδ))dϑ]ι)1ςB(ς)MH1dH([η(ξ)]ι,[γ(ξ)]ι)+1ςB(ς)MH2dH([η(ξδ)]ι,[γ(ξδ)]ι)+ςB(ς)Γ(ς)ξ0|(ξϑ)ς1|(MH1dH([η(ϑ)]ι,[γ(ϑ)]ι)+MH2dH([η(ϑδ)]ι,[γ(ϑδ)]ι))dϑ.

    Therefore,

    d[Λη(ξ),Λγ(ξ)]=supι(0,1]dH([Λη(ξ)]ι,[Λγ(ξ)]ι)=supι(0,1](1ςB(ς)MH1dH([η(ξ)]ι,[γ(ξ)]ι)+1ςB(ς)MH2dH([η(ξδ)]ι,[γ(ξδ)]ι)+ςB(ς)Γ(ς)ξ0|(ξϑ)ς1|(MH1dH([η(ϑ)]ι,[γ(ϑ)]ι)+MH2dH([η(ϑδ)]ι,[γ(ϑδ)]ι))dϑ)1ςB(ς)MH1supι(0,1]dH([η(ξ)]ι,[γ(ξ)]ι)+1ςB(ς)MH2supι(0,1]dH([η(ξδ)]ι,[γ(ξδ)]ι)+ςB(ς)Γ(ς)ξ0|(ξϑ)ς1|(MH1supι(0,1]dH([η(ϑ)]ι,[γ(ϑ)]ι)+MH2supι(0,1]dH([η(ϑδ)]ι,[γ(ϑδ)]ι))dϑ1ςB(ς)MH1d(η(ξ),γ(ξ))+1ςB(ς)MH2d(η(ξδ),γ(ξδ))+ςB(ς)Γ(ς)ξ0|(ξϑ)ς1|(MH1d(η(ϑ),γ(ϑ))+MH2d(η(ϑδ),γ(ϑδ)))dϑ.

    Thus,

    H1((Λη),(Λγ))=supξ[0,ξ1]d[Λη(ξ),Λγ(ξ)]=supξ[0,ξ1](1ςB(ς)MH1d(η(ξ),γ(ξ))+1ςB(ς)MH2d(η(ξδ),γ(ξδ))+ςB(ς)Γ(ς)ξ0|(ξϑ)ς1|(MH1d(η(ϑ),γ(ϑ))+MH2d(η(ϑδ),γ(ϑδ)))dϑ)1ςB(ς)MH1supξ[0,ξ1]d(η(ξ),γ(ξ))+1ςB(ς)MH2supξ[0,ξ1]d(η(ξδ),γ(ξδ))+ςB(ς)Γ(ς)ξ0|(ξϑ)ς1|(MH1supξ[0,ξ1]d(η(ϑ),γ(ϑ))+ MH2supξ[0,ξ1]d(η(ϑδ),γ(ϑδ)))dϑ1ςB(ς)MH1H1(η,γ)+1ςB(ς)MH2H1(η,γ)+ςB(ς)Γ(ς)(MH1+MH2)H1(η,γ)ξ0|(ξϑ)ς1|dϑL1H1(η,γ).

    Case 3: For ξ(ξj,kj], j=1,2,,n and η,γPC(J;Kn),

    (Λη)(ξ)=hj(ξ,η(ξj)),(Λγ)(ξ)=hj(ξ,γ(ξj)).

    Therefore,

    dH([Λη(ξ)]ι,[Λγ(ξ)]ι)=dH([hj(ξ,η(ξj))]ι,[hj(ξ,γ(ξj)]ι)MhjdH([η(ξj)]ι,[γ(ξj)]ι).

    Thus,

    d[Λη(ξ),Λγ(ξ)]=supι(0,1]dH([Λη(ξ)]ι,[Λγ(ξ)]ι)Mhjd(η(ξj),γ(ξj)).

    Hence,

    H1((Λη),(Λγ))=supξ[ξj,kj]d[Λη(ξ),Λγ(ξ)]H1((Λη),(Λγ))MhjH1(η,γ).

    Case 4: For ξ(kj,ξj+1], j=1,2,,n and η,γPC(J;Kn),

    (Λη)(ξ)=hj(kj,η(ξj))+1ςB(ς)H(ξ,η(ξ),η(ξδ))+ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ,(Λγ)(ξ)=hj(kj,γ(ξj))+1ςB(ς)H(ξ,γ(ξ),γ(ξδ))+ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,γ(ϑ),γ(ϑδ))dϑ.

    Therefore,

    dH([Λη(ξ)]ι,[Λγ(ξ)]ι) =dH([hj(kj,η(ξj))+1ςB(ς)H(ξ,η(ξ),η(ξδ))+ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ]ι,[hj(kj,γ(ξj))+1ςB(ς)H(ξ,γ(ξ),γ(ξδ))+ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,γ(ϑ),γ(ϑδ))dϑ]ι) =dH([hj(kj,η(ξj))]ι+[1ςB(ς)H(ξ,η(ξ),η(ξδ))]ι+[ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ]ι, [hj(kj,γ(ξj))]ι+[1ςB(ς)H(ξ,γ(ξ),γ(ξδ))]ι+[ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,γ(ϑ),γ(ϑδ))dϑ]ι) dH([hj(kj,η(ξj))]ι,[hj(kj,γ(ξj))]ι)+ dH([1ςB(ς)H(ξ,η(ξ),η(ξδ))]ι,[1ςB(ς)H(ξ,γ(ξ),γ(ξδ))]ι)+ dH([ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,η(ϑ),η(ϑδ))dϑ]ι,[ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,γ(ϑ),γ(ϑδ))dϑ]ι) dH([hj(kj,η(ξj))]ι,[hj(kj,γ(ξj))]ι)+1ςB(ς)dH([H(ξ,η(ξ),η(ξδ))]ι,[H(ξ,γ(ξ),γ(ξδ))]ι)+ςB(ς)Γ(ς)ξkj|(ξϑ)ς1|dH([H(ϑ,η(ϑ),η(ϑδ))]ι,[H(ϑ,γ(ϑ),γ(ϑδ))]ι)dϑ MhjdH([η(ξj)]ι,[γ(ξj)]ι)+1ςB(ς)MH1dH([η(ξ)]ι,[γ(ξ)]ι)+1ςB(ς)MH2dH([η(ξδ)]ι,[γ(ξδ)]ι)+ςB(ς)Γ(ς)ξkj|(ξϑ)ς1|(MH1dH([η(ϑ)]ι,[γ(ϑ)]ι)+MH2dH([η(ϑδ)]ι,[γ(ϑδ)]ι))dϑ.

    Therefore,

    d[Λη(ξ),Λγ(ξ)]=supι(0,1]dH([Λη(ξ)]ι,[Λγ(ξ)]ι)Mhjsupι(0,1]dH([η(ξj)]ι,[γ(ξj)]ι)+1ςB(ς)MH1supι(0,1]dH([η(ξ)]ι,[γ(ξ)]ι)+1ςB(ς)MH2supι(0,1]dH([η(ξδ)]ι,[γ(ξδ)]ι)+ςB(ς)Γ(ς)ξkj|(ξϑ)ς1|(MH1supι(0,1]dH([η(ϑ)]ι,[γ(ϑ)]ι)+MH2supι(0,1]dH([η(ϑδ)]ι,[γ(ϑδ)]ι))dϑMhjd(η(ξj),γ(ξj))+1ςB(ς)MH1d(η(ξ),γ(ξ))+1ςB(ς)MH2d(η(ξδ),γ(ξδ))+ςB(ς)Γ(ς)ξkj|(ξϑ)ς1|(MH1d(η(ϑ),γ(ϑ))+MH2d(η(ϑδ),γ(ϑδ)))dϑ.

    Hence,

    H1((Λη),(Λγ))=supξ[kj,ξj+1]d[Λη(ξ),Λγ(ξ)]=supξ[kj,ξj+1](Mhjd(η(ξj),γ(ξj))+1ςB(ς)MH1d(η(ξ),γ(ξ))+1ςB(ς)MH2d(η(ξδ),γ(ξδ))+ςB(ς)Γ(ς)ξkj|(ξϑ)ς1|(MH1d(η(ϑ),γ(ϑ))+MH2d(η(ϑδ),γ(ϑδ)))dϑ)=Mhjsupξ[kj,ξj+1]d(η(ξj),γ(ξj))+1ςB(ς)MH1supξ[kj,ξj+1]d(η(ξ),γ(ξ))+1ςB(ς)MH2supξ[kj,ξj+1]d(η(ξδ),γ(ξδ))+ςB(ς)Γ(ς)ξkj|(ξϑ)ς1|(MH1supξ[kj,ξj+1]d(η(ϑ),γ(ϑ))+MH2supξ[kj,ξj+1]d(η(ϑδ),γ(ϑδ)))dϑMhjH1(η,γ)+1ςB(ς)MH1H1(η,γ)+1ςB(ς)MH2H1(η,γ)+ςB(ς)Γ(ς)(MH1+MH2)H1(η,γ)ξkj|(ξϑ)ς1|dϑMhjH1(η,γ)+1ςB(ς)(MH1+MH2)H1(η,γ)+ςB(ς)Γ(ς)(MH1+MH2)H1(η,γ)Tς(Mhj+1ςB(ς)(MH1+MH2)+ςB(ς)Γ(ς)(MH1+MH2)Tς)H1(η,γ)L2jH1(η,γ).

    From the above four cases, we conclude that

    H1((Λη),(Λγ))=supξJd[Λη(ξ),Λγ(ξ)]LH1(η,γ). (3.1)

    Thus, for sufficiently small T, Λ is a strict contraction mapping and hence by Banach fixed point theorem Λ has a unique fixed point which is the solution of system (1.1). The Theorem 3.1 is existence of local solution because our mapping Λ:PC(J:Kn)PC(J:Kn) is not strict contraction for all values of T. In Eq (3.1), we can see that a constant L<1 if T is sufficiently small. Thus, we can say that our solution exists locally.

    To show the existence of global solution, we need the Gronwall's inequality:

    Lemma 4.1. [37] (Gronwall's inequality) Let F(ξ,k)0 be a continuous function on 0k<ξT. If, there are positive constant a,b,ς such that

    F(ξ,k)a+bξk(ξκ)ς1F(κ,k)dκ, for 0k<ξT,

    then there is a constant C such that F(ξ,k)C for 0k<ξT.

    For the convenience, we set the following notations

    C1=max1jn{a1,c1j,a2j}, C2=max1jn{b1,b2j},

    C3=maxδξT{C1exp(C2Tδ|(ξϑ)ς1|dϑ)},

    a1=(1L3A1+1L31ςB(ς)K(T)+1L3ςB(ς)Γ(ς)K(T)Tς), L3=(11ςB(ς)2K(T)), A1=d(Ψ(0),0),

    c1j=11Mhj, a2j=(1L4j1ςB(ς)K(T)+1L4jςB(ς)Γ(ς)K(T)(T)ς), b1=(1L3ςB(ς)Γ(ς)2K(T)),

    L4j=(1Mhj1ςB(ς)2K(T)), b2j=(1L4jςB(ς)Γ(ς)2K(T)), j=1,2,,n.

    Theorem 4.1. Let the function H:(kj,ξj+1]×Kn×KnKn satisfies the assumptions (B1) and (B2) and there exists a real valued function K(ξ) which is continuous and non decreasing such that

    dH([H(ξ,η1,η2)]ι,[0]ι)K(ξ)(1+dH([η1]ι,[0]ι)+dH([η2]ι,[0]ι)),  η1, η2Kn.

    Then, the Eq (1.1) has a unique solution P which exists for all ξ[δ,T].

    Proof. By Theorem 3.1, we can continue the solution of system (1.1) as long as P stays bounded. Therefore, we need to show that if P exists on [δ,T), then it is bounded as ξT. Also, the solution of system (1.1) is given by

    P(ξ)={Ψ(ξ),ξ[δ,0),Ψ(0)+1ςB(ς)H(ξ,P(ξ),P(ξδ))+ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ,ξ[0,ξ1],hj(ξ,P(ξj)), ξ(ξj,kj],j=1,2,,n,hj(kj,P(ξj))+ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ+1ςB(ς)H(ξ,P(ξ),P(ξδ)),ξ(kj,ξj+1],j=1,2,,n.

    The proof of this theorem is divided into following four cases:

    Case 1: For ξ[δ,0), we have P(ξ)=Ψ(ξ).

    In this case, we get

    H1(P,0)0.

    Case 2: For ξ[0,ξ1],

    P(ξ)=Ψ(0)+1ςB(ς)H(ξ,P(ξ),P(ξδ))+ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ.

    Now, we have

    dH([P(ξ)]ι,[0]ι)=dH([Ψ(0)+1ςB(ς)H(ξ,P(ξ),P(ξδ))+ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ]ι,[0]ι)=dH([Ψ(0)]ι+[1ςB(ς)H(ξ,P(ξ),P(ξδ))]ι+[ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ]ι,[0]ι)=dH([Ψ(0)]ι,[0]ι)+dH([1ςB(ς)H(ξ,P(ξ),P(ξδ))]ι,[0]ι)+dH([ςB(ς)Γ(ς)ξ0(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ]ι,[0]ι)dH([Ψ(0)]ι,[0]ι)+1ςB(ς)dH([H(ξ,P(ξ),P(ξδ))]ι,[0]ι)+ςB(ς)Γ(ς)ξ0|(ξϑ)ς1|dH([H(ϑ,P(ϑ),P(ϑδ))]ι,[0]ι)dϑdH([Ψ(0)]ι,[0]ι)+1ςB(ς)K(T)(1+dH([P(ξ)]ι,[0]ι)+dH([P(ξδ)]ι,[0]ι))+ςB(ς)Γ(ς)ξ0|(ξϑ)ς1|K(T)(1+dH([P(ϑ)]ι,[0]ι)+dH([P(ϑδ)]ι,[0]ι))dϑ.

    Therefore,

    d[P(ξ),0]=supι(0,1]dH([P(ξ)]ι,[0]ι)A1+1ςB(ς)K(T)(1+d(P(ξ),0)+d(P(ξδ),0))+ςB(ς)Γ(ς)ξ0|(ξϑ)ς1|K(T)(1+d(P(ϑ),0)+d(P(ϑδ),0))dϑ.

    Thus,

    H1(P,0)=supξ[0,ξ1]d(P(ξ),0)A1+1ςB(ς)K(T)(1+2H1(P,0))+ςB(ς)Γ(ς)ξ0|(ξϑ)ς1|K(T)(1+2H1(P,0))dϑA1+1ςB(ς)K(T)+1ςB(ς)2K(ξ)H1(P,0)+ςB(ς)Γ(ς)K(T)ξ0|(ξϑ)ς1|dϑ+ςB(ς)Γ(ς)2K(T)ξ0|(ξϑ)ς1|H1(P,0)dϑ(11ςB(ς)2K(ξ))H1(P,0)A1+1ςB(ς)K(T)+ςB(ς)Γ(ς)K(T)Tς+ςB(ς)Γ(ς)2K(T)ξ0|(ξϑ)ς1|H1(P,0)dϑH1(P,0)1L3A1+1L31ςB(ς)K(T)+1L3ςB(ς)Γ(ς)K(T)Tς+1L3ςB(ς)Γ(ς)2K(T)ξ0|(ξϑ)ς1|H1(P,0)dϑa1+b1ξ0|(ξϑ)ς1|H1(P,0)dϑ.

    Case 3: Similarly, for ξ(ξj,kj], j=1,2,,n and P(ξ)=hj(ξ,P(ξj)),

    dH([P(ξ)]ι,[0]ι)=dH([hj(ξ,P(ξj))]ι,[0]ι)MhjdH([P(ξj)]ι,[0]ι).

    Therefore,

    d[P(ξ),0]=supι(0,1]dH([P(ξ)]ι,[0]ι)Mhjd(P(ξj),0).

    Thus,

    H1(P,0)=sup[ξj,kj]d[P(ξ),0]H1(P,0)MhjH1(P,0)H1(P,0)11Mhj,H1(P,0)c1j.

    Case 4: For ξ(kj,ξj+1], j=1,2,,n, we have

    P(ξ)=hj(kj,P(ξj))+1ςB(ς)H(ξ,P(ξ),P(ξδ))+ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ.

    Now, we have

    dH([P(ξ)]ι,[0]ι)=dH([hj(kj,P(ξj))+1ςB(ς)H(ξ,P(ξ),P(ξδ))+ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ]ι,[0]ι)=dH([hj(kj,P(ξj))]ι+[1ςB(ς)H(ξ,P(ξ),P(ξδ))]ι +[ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ]ι,[0]ι)dH([hj(kj,P(ξj))]ι,[0]ι)+dH([1ςB(ς)H(ξ,P(ξ),P(ξδ))]ι,[0]ι)+ dH([ςB(ς)Γ(ς)ξkj(ξϑ)ς1H(ϑ,P(ϑ),P(ϑδ))dϑ]ι,[0]ι)dH([hj(kj,P(ξj))]ι,[0]ι)+1ςB(ς)dH([H(ξ,P(ξ),P(ξδ))]ι,[0]ι)+ςB(ς)Γ(ς)ξkj|(ξϑ)ς1|dH([H(ϑ,P(ϑ),P(ϑδ))]ι,[0]ι)dϑMhjdH([P(ξj)]ι,[0]ι)+1ςB(ς)K(T)(1+dH([P(ξ)]ι,[0]ι)+dH([P(ξδ)]ι,[0]ι))+ςB(ς)Γ(ς)ξkj|(ξϑ)ς1|K(T)(1+dH([P(ϑ)]ι,[0]ι)+dH([P(ϑδ)]ι,[0]ι))dϑ.

    Therefore,

    d[P(ξ),0]=supι(0,1]dH([P(ξ)]ι,[0]ι)Mhjd(P(ξj),0)+1ςB(ς)K(T)(1+d(P(ξ),0)+d(P(ξδ),0))+ςB(ς)Γ(ς)ξkj|(ξϑ)ς1|K(T)(1+d(P(ϑ),0)+d(P(ϑδ),0))dϑ.

    Thus,

    H1(P,0)=supξ[kj,ξj+1]d[P(ξ),0]MhjH1(P,0)+1ςB(ς)K(T)(1+2H1(P,0))+ςB(ς)Γ(ς)ξkj|(ξϑ)ς1|K(T)(1+2H1(P,0))dϑMhjH1(P,0)+1ςB(ς)K(T)+1ςB(ς)2K(ξ)H1(P,0))+ςB(ς)Γ(ς)K(T)ξkj|(ξϑ)ς1|dϑ+ςB(ς)Γ(ς)2K(T)ξkj|(ξϑ)ς1|H1(P,0))dϑL4jH1(P,0)1ςB(ς)K(T)+ςB(ς)Γ(ς)K(T)(T)ς+ςB(ς)Γ(ς)2K(T)ξkj|(ξϑ)ς1|H1(P,0))dϑH1(P,0)1L4j1ςB(ς)K(T)+1L4jςB(ς)Γ(ς)K(T)(T)ς+1L4jςB(ς)Γ(ς)2K(T)ξkj|(ξϑ)ς1|H1(P,0))dϑa2j+b2jξkj|(ξϑ)ς1|H1(P,0)dϑ.

    From the above four cases, we conclude that, for ξ[δ,T]

    H1(P,0)C1+C2Tδ|(ξϑ)ς1|H1(P,0)dϑ.

    So that,

    H1(P,0)C1exp{C2Tδ|(ξϑ)ς1|dϑ}C3.

    Thus, H1(P,0)=PC3. Hence, from Lemma 4.1, P is bounded. Therefore, we can extend our solution to the whole interval [δ,T]. Thus, our solution is global. For more details, please see[37]).

    Remark 5. By using the above argument, we can prove that the system (1.1) has atleast one solution under the following weak assumptions

    (A1) Function H:(kj,ξj+1]×Kn×KnKn, j=0,1,,n, is continuous and there exists a positive constant MH>0 such that

    |H(ξ,η1,η2)|MH(1+|η1|+|η2|), ξ(kj,ξj+1], η1, η2Kn.

    (A2) Functions hj:(ξj,kj]×KnKn, j=1,2,,n are continuous and there exists a positive constants Mj>0 such that

    |hj(ξ,η1)|Mj(1+|η1|),  ξ(ξj,kj], η1Kn.

    We consider the following retarded fractional differential system with non-instantaneous impulsive condition

    ABC     0D12ξP(ξ)=ˉ2ξP2(ξ)+ˉ2ξ2P2(ξ12),ξ(0,1](1.5,2],P(ξ)=sin(jξ)ejξP(ξj), ξ(1,1.5],j=1,P(ξ)=Ψ(ξ)=ξ+1, ξ[12,0]. (6.1)

    Here, we have ς=12, ξ[12,2], 0=k0<ξ1=1<k1=1.5<ξ2=2=T, H(ξ,P(ξ),P(ξδ))=ˉ2ξP2(ξ)+ˉ2ξ2P2(ξ12) and impulsive function hj(ξ,P(ξj))=sin(jξ)ejξP(ξj), j=1.

    The ι-level of fuzzy number ˉ2 is [2]ι=[ι+1,3ι],  ι[0,1]. Then, the ι-level set of H(ξ,P(ξ),P(ξδ)) is

    [H(ξ,P(ξ),P(ξδ))]ι=[ˉ2ξP2(ξ)+ˉ2P2(ξ12)]ι=ξ[(ι+1)(Pιq(ξ))2,(3ι)(Pιr(ξ))2]+ξ2[(ι+1)(Pιq(ξ12))2,(3ι)(Pιr(ξ12))2].

    Now, we have

    dH([H(ξ,η(ξ),η(ξδ))]ι,[H(ξ,γ(ξ),γ(ξδ))]ι)=dH{((ι+1)ξ(ηιq(ξ))2,(3ι)ξ(ηιr(ξ))2+ξ2(ι+1)(ηιq(ξ12))2,ξ2(3ι)(ηιr(ξ12))2),((ι+1)ξ(γιq(ξ))2,(3ι)ξ(γιr(ξ))2+ξ2(ι+1)(γιq)(ξ12))2,ξ2(3ι)(γιr(ξ12))2)}=dH(ξ[(ι+1)(ηιq(ξ))2,(3ι)(ηιr(ξ))2],ξ[(ι+1)(γιq(ξ))2,(3ι)(γιr(ξ))2])+dH([ξ2(ι+1)(ηιq(ξ12))2,ξ2(3ι)(ηιr(ξ12))2],[ξ2(ι+1)(γιq(ξ12))2,ξ2(3ι)(γιr(ξ12))2])max{|(ι+1)ξ(ηιq(ξ))2(ι+1)ξ(γιq(ξ))2|,|(3ι)ξ(ηιr(ξ))2(3ι)ξ(γιr(ξ))2|}+max{|(ι+1)ξ2(ηιq(ξ12))2ξ2(ι+1)(γιq(ξ12))2|,|(3ι)ξ2(ηιr(ξ12))2ξ2(3ι)(γιr(ξ12))2|}max{(ι+1)ξ|(ηιq(ξ))2(γιq(ξ))2|,(3ι)ξ|(ηιr(ξ))2(γιr(ξ))2|}+max{(ι+1)ξ2|(ηιq(ξ12))2(γιq(ξ12))2|,(3ι)ξ2|(ηιr(ξ12))2(γιr(ξ12))2|}T(3ι)max{|ηιq(ξ)γιq(ξ)||ηιq(ξ)+γιq(ξ)|,|ηιr(ξ)γιr(ξ)||ηιr(ξ)+γιr(ξ)|}+T2(3ι)max{|ηιq(ξ12)γιq(ξ12)||ηιq(ξ12)+γιq(ξ12)|,|ηιr(ξ12)γιr(ξ12)||ηιr(ξ12)+γιr(ξ12)|}(3ι)Tmax12ξ2{|ηιq(ξ)+γιq(ξ)|} dH([η(ξ)]ι,[γ(ξ)]ι)+T2(3ι)max12ξ2{|ηιr(ξ12)+γιr(ξ12)|}dH([η(ξ12)]ι,[γ(ξ12)]ι)c1 dH([η(ξ)]ι,[γ(ξ)]ι)+c2dH([η(ξ12)]ι,[γ(ξ12)]ι),

    where c1=(3ι)Tmax12ξ2{|ηιq(ξ)+γιq(ξ)|}, c2=(3ι)T2max12ξ2{|ηιr(ξ12)+γιr(ξ12)|} satisfies the condition (B1).

    Now, the ι-level set of fuzzy number ˉ1 is [ˉ1]ι=[ι,2ι],  ι[0,1] and ι-level set of impulsive function hj(ξ,P(ξj)) is

    [hj(ξ,P(ξj))]ι=[sin(jξ)ejξP(ξj)]ι=sin(jξ)ejξ[(ι,2ι)[P(ξj)]ι]=sin(jξ)ejξ[ιPιq(ξj),(2ι)Pιr(ξj)].

    Therefore,

    dH([hj(ξ,η(ξj))]ι,[hj(ξ,γ(ξj))]ι)=dH(sin(jξ)ejξ[ιηιq(ξj),(2ι)ηιr(ξj)],sin(jξ)ejξ[ιγιq(ξj),(2ι)γιr(ξj)])=dH(sin(jξ)ejξ[ιηιq(ξj),(2ι)ηιr(ξj)],sin(jξ)ejξ[ιγιq(ξj),(2ι)γιr(ξj)])max{ιsin(jξ)ejξ|ηιq(ξj)γιq(ξj)|,(2ι)sin(jξ)ejξ|ηιr(ξj)γιr(ξj)|}(2ι)sin(jT)ejTmax{|ηιq(ξj)γιq(ξj)|,|ηιr(ξj)γιr(ξj)|}(2ι)sin(jT)ejTdH([η(ξj)]ι,[γ(ξj)]ι)c3dH([η(ξj)]ι,[γ(ξj)]ι),

    where c3=(2ι)sin(jT)ejT, j=1, satisfies the condition (B2).

    Thus, all the conditions of Theorem 3.1 are fulfilled. Hence, system (5.1) has a unique fuzzy solution.

    In this work, we have considered the fractional order fuzzy delay differential system with non-instantaneous impulses. The main aim of this work is to establish the existence of local and global solutions to the considered system. In Section 3, we have studied the existence of a local solution and in Section 4, we have extended the local solution of Section 3 to a global solution. Fuzzy set theory, Banach fixed point theorem and non-linear function analysis are the major tools to establish these results. In Section 5, an example is given to validate obtained outcomes.

    The researchers would like to thank the Deanship of Scientific Research, Qassim University for funding the publication of this project. We are also thankful to the associate editor and anonymous reviewers for their constructive comments and suggestions which help us to improve the manuscript.

    The authors declare no conflict of interest.



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