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Study of multi term delay fractional order impulsive differential equation using fixed point approach

  • This manuscript is devoted to investigate a class of multi terms delay fractional order impulsive differential equations. Our investigation includes existence theory along with Ulam type stability. By using classical fixed point theorems, we establish sufficient conditions for existence and uniqueness of solution to the proposed problem. We develop some appropriate conditions for different kinds of Ulam-Hyers stability results by using tools of nonlinear functional analysis. We demonstrate our results by an example.

    Citation: Amjad Ali, Kamal Shah, Dildar Ahmad, Ghaus Ur Rahman, Nabil Mlaiki, Thabet Abdeljawad. Study of multi term delay fractional order impulsive differential equation using fixed point approach[J]. AIMS Mathematics, 2022, 7(7): 11551-11580. doi: 10.3934/math.2022644

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  • This manuscript is devoted to investigate a class of multi terms delay fractional order impulsive differential equations. Our investigation includes existence theory along with Ulam type stability. By using classical fixed point theorems, we establish sufficient conditions for existence and uniqueness of solution to the proposed problem. We develop some appropriate conditions for different kinds of Ulam-Hyers stability results by using tools of nonlinear functional analysis. We demonstrate our results by an example.



    Fractional calculus has gotten considerable attention recently. Derivatives and integrals of non-integer order are increasingly using for different analysis of various problems. Fractional differential operators are global in nature and preserve greater degree of freedom. Therefore, researchers now give preference to use fractional order differential equations (FODEs) in mathematical modelings of various real world process and phenomenons over classical order differential equation. FODEs have multi-dimensional applications in the variety of fields of modern sciences, such as to control the phase difference in oscillators, to accomplish the high frequency oscillation and in electric engineering DC converter models are used to obtain good assessment of the power conversion efficiency. Recently various biological models have been investigated by using fractional order differential equations. In the mentioned study, researchers have established more good results than those already derived for ordinary differential equations. For some more applications of fractions derivatives, for theory and applications of FODEs see [1,2], for integro-FODEs, see [3]. For basic theory and applications we refer [4]. Some generalized type FODEs have been analyzed in [5,6]. Some engineering applications have been investigated in [7]. For real world applications by using FODEs, see [8]. Those differential equations which observe impulsive conditions at points of discontinuity of solution are known as impulsive differential equations. Impulsive differential equations are the tools used for modeling of those evolutionary and physical phenomena that containing sudden changes and discontinuous jumps. Therefore, the proposed types of impulsive differential equations play a significant role to models such phenomena, in this regards (see [9]). Some stability results about the said area has been studied in [10]. Also some conformable impulsive FODEs have been studied in [11]). In some circumstance physical problems depends on preceding states of problem and cannot be describes by current time. In order to avoid such circumstance, researches introduced an important class of differential equations (DEs) known as Delay Differential Equations (DDEs). There are verities of DDEs including proportional (pantograph), continuous and discrete type DDEs. The concern types of DEs are widely using to formulate various real world phenomena in different fields, such as dynamics, quantum mechanics [12], biology [13], and electrodynamics [14].

    Important aspects of mathematical analysis are existence theory and stability analysis. Researchers have used various tools of nonlinear analysis for investigating the existence and uniqueness of solution to various problems of FODEs. Various fixed point results and degrees theories have been developed to investigate the said area for existence of solutions. In same line stability analysis of FODEs has also been given proper attention recently. The mentioned analysis is important for developing various numerical methods. Stability results have been investigated by using various methods including exponential method, Mittag-Leffler method and Hyers-Ulam method (see some detail in [15]). Here, we remark that the Ulam's type stability analysis has given more attention recently. The aforementioned stability results have been derived for various problems of FODEs in last few years (for instance see [16]). Hyers and Ulam had been introduced the mentioned stability for the first time for functional equations in 1940 (see some detail [17]). Rassias [18] extended the mentioned stability analysis for linear equations. Also Jung [19] extended the Rassias stability results for functional equations in nonlinear analysis.

    Motivated from the mentioned work, researchers have been given much attention to investigate the aforesaid stability analysis for various dynamical problems (we refer few as [20,21]). For boundary value problems of FODEs, the mentioned stability has been studied very well (we refer few results as [22,23]). Furthermore, results related to existence theory of solutions to various problems of fractional order mathematical models of epidemiology have been investigated very well (for instance see [24]). The said results have been investigated for TB models in [27]. The Green functions theory using FODEs has been established in [25,26]. Also the mentioned analysis has been studied for those FODEs involving non-singular derivatives (for instance see [28]).

    The existence theory has been developed very well for FODEs in last few years. As an example the reader can look at the second order FODE with non local boundary condition on the independent variable [29]. Researchers have been used fixed point theory together with topological degree theory to develop necessary condition for existence of solution for various problems of fractional order differential equations. Furthermore, they have also derived various results related to Ulam type stability for said problems. Here we recall a suitable example which has been studied in [33] as

    cDηU(t)=F(t,U(t)),1<η2,t[0,1],Z1U(0)+Z2U(1)=P1(U),Z3U(0)+Z4U(1)=P2(U), (1.1)

    where Z1,Z2,Z3 and Z4 are members of the set of real numbers, which satisfy the condition given as: Z1+Z20 and Z3+Z40. The function F,P1 and P1 are continuous. The authors initially utilized the tools of fractional calculus as well as nonlinear analysis to transform the aforementioned FDE to corresponding integral equation and then used fixed theory to achieve their aims.

    Similarly, in [30] uniqueness and existence of solution have been studied by utilizing the tools of fixed point theory. Authors have investigated the following system of FODEs with anti periodic coupled with non local subsidiary conditions as

    αc1Dη1U(t)+αc2Dη2U(t)=H1(t,U(t),Y(t)),αc3Dη3Y(t)+αc4Dη4Y(t)=H2(t,U(t),Y(t)),U(0)+U(1)=nj=1κjY(βj),U(0)+U(1)=nj=1λjY(βj),Y(0)+Y(1)=nj=1κjU(βj),Y(0)+Y(1)=nj=1λjU(βj).

    The author have used standard Caputo derivative in the consider problem, where parameters α1,α2,α3,α4,κj,κj,λj and λj are real numbers for j=1,2,,m and 0<βj<1.

    Inspired from by the above discussion, in this research work, we take the following system by extending the problem (1.1) utilizing the concept of [30,31] as

    {pi=1σicDαiU(t)=H(t,U(t),U(λt)),α1(1,2]αi(0,1], fori=2,3,,p,t[0,τ],Δ(U(tk))=IkU(tk),Δ(U(tk))=IkU(tk),k=0,1,,m,a1U(0)+b1U(τ)=g1(U),a2U(0)+b2U(τ)=g2(U),al,blRforl=1,2. (1.2)

    In the consider problem (1.2), σiR for i=1,2,,p with σ10, and functions g1,g2:PC([0,τ]),R)R and non linear function H:[0,τ]×R×RR are continuous and τ>0 is real constant. Furthermore, impulsive operators Ik and Ik are also continuous. In this article, we use tools of fixed point theory and functional analysis to obtain the desired results. Results devoted to the existence and uniqueness of solution are derived by using Banach and Krasnoselskii's fixed point theorems. Also, the results devoted to stability analysis of Ulam type are established by using tools of nonlinear functional analysis. For verification of the obtain results, we give appropriate example.

    The rest of the paper is organized as follows: In Section 2, we recall some basic concepts of fractional calculus, while the main results, relying on Krasnoselski's fixed point theorem and Banach contraction principal are presented in Section 3. Section 4 is devoted to stability analysis of the proposed problem (1.2). Section 5 contains illustrative examples for the obtained results. In Section 6, we present conclusion of our findings.

    This section of research, is devoted to basic results, theorems and lemmas of FPT and non-linear analysis, which we need for investigation of the main work.

    In the present work, we use the following space and norm

    PC(J,R)=X={U:JR:UC(Jk),k=0,1,,m, and U(t+),U(t) exist,k=1,2,,m}

    with norm define as

    U=maxtJ{|U(t)| UPC(J,R):tJ},

    where

    J0=[0,t1],J1=(t1,t,2],J2=(t2,t3],,Jm=(tm,τ] and J=[0,τ].

    Definition 2.1. The integral of fractional order α of a function y(t)L[0,d] is denoted by Iαy(t), and defined as

    Iαy(t)=t0y(χ)Γ(α)(tχ)1αdχ.

    Definition 2.2. [32] Fractional order Caputo derivative for a function y(t)L1([0,d],R+) on the interval [0,d] is defined as

    cDαy(t)=t0yn(χ)Γ(nα)(tχ)α+1ndχ,

    where n=α and α is defined to be the smallest integer equal or greater than α.

    Lemma 2.1. [34] The relation between fractional order integral and derivative is given as

    Iα[cDαy(t)]=A1+A2t+A3t2+A4t3++Antn1+y(t),

    where AiR for i=1,2,,n.

    Definition 2.3. The mapping T:XY on norm linear spaces is continuous and complete, if for each bounded MX, ¯T(M)Y is compact.

    Definition 2.4. [35] Let F(X) be the collection of function (real valued) on (X,d) metric space, be equi-continuous xX, if for each ϵ>0, we can find δ>0, such that for every function fF(X) and x0X, we have |f(x0)f(x)|<ϵ, whenever d(x0x)<δ.

    Definition 2.5. [35] An operator T on (X,d) metric space into itself is Lipschitz, if c0, and d(T(x1),T(x2))cd(x2,x1), for each x2,x1X, where c is called Lipschitz constant and contraction, if 0<c<1.

    Definition 2.6. [35] An operator T from a metric space (X,d) into itself is contraction, if 0<c<1, such that d(T(x1),T(x2))cd(x1,x2),x1,x2X.

    Theorem 2.7. [35]every mapping(self contraction) T in complete (X,d) metric space has unique fixed point.

    Theorem 2.8. [36] Assume that H is a non empty, convex, bounded and closed convex bounded subset of a Banach space X. let J1 and J1 be two operator provide that J1U1+J2U2H whenever U,U2H, J1 is continuous and compact and J2 is contraction map. Then there is UH provide that, U=J1U+J2U.

    This section of research work is committed, to integral representation and existence results for the consider class of multi-term fractional delay differential equations. The authors established the expression for integral representation of proposed problem. In order to obtain results for existence and stability analysis the authors used the tools of analysis and fixed point theory.

    This subsection of the research work, is devoted the integral representation of the consider model (1.2).

    Theorem 3.1. Assumed that Y(t)C(J,R), then the solution of multi-term impulsive fractional delay differential equation,

    {pi=1σicDαiU(t)=Y(t),α1(1,2]αi(0,1], fori=2,3,,p,t[0,τ],Δ(U(tk))=IkU(tk),Δ(U(tk))=IkU(tk),k=0,1,,m,a1U(0)+b1U(τ)=g1(U),a2U(0)+b2U(τ)=g2(U),al,blRforl=1,2, (3.1)

    is equivalent to the integral equation

    (3.2)

    Where gi(i=1,2):C(J,R)R are continuous function, al+bl0 for l=1,2 and α1αi1>0 for i=2,3,,p and

    D=σ1a1+b1g1(U)+b2σ1a2+b2(tτb1a1+b1)g2(U)b1a1+b1[σ1mj=1IjU(tj)+σ1m1j=1(tmtj)IjU(tj)+σ1mj=1(ttm)IjU(tj)]b2a2+b2(tτb1a1+b1)mj=11Γ(α11)tjtj1(tjX)α12Y(X)dX+b2a2+b2(tτb1a1+b1)mj=1pi=2σi1Γ(α1αi1)tjtj1(tjX)α1αi2U(X)dXb2a2+b2(tτb1a1+b1)1Γ(α11)τtm(τX)α12Y(X)dX+b2a2+b2(tτb1a1+b1)pi=2σi1Γ(α1αi1)τtm(τX)α1αi2U(X)dX+b1a1+b1[mj=11Γ(α1)tjtj1(tjX)α11Y(X)dXmj=1τtmΓ(α11)tjtj1(tjX)α12Y(X)dXm1j=1tmtjΓ(α11)tjtj1(t1X)α12Y(X)dX+mj=1pi=2σi1Γ(α1αi)tjtj1(tjX)α1αi1U(X)dX+mj=1pi=2σiτtmΓ(α1αi1)tjtj1(tjX)α1αi2U(X)dX1Γ(α1)τtm(τX)α11Y(X)dX+m1j=1pi=2σitmtjΓ(α1αi1)tjtj1(tjX)α1αi2U(X)dXpi=2σiτtm(τX)α1αi1Γ(α1αi)U(X)dX].

    Proof. Applying fractional order integral Iα1 on (3.1) and in-view of Lemma 2.1 for t[0,t1], we get

    σ1U(t)=C0+C1t+1Γ(α1)t0(tX)α11Y(X)dXpi=2σiΓ(α1αi)t0(tX)α1αi1U(X)dX. (3.3)

    By differentiating (3.3), we get

    σ1U(t)=C1+1Γ(α11)t0(tX)α12Y(X)dXpi=2σiΓ(α1αi1)t0(tX)α1αi2U(X)dX. (3.4)

    Similarly, for t(t1,t2], the system (3.1) become

    σ1U(t)=C01+C11(tt1)+1Γ(α1)tt1(tX)α11Y(X)dXpi=2tt1σi(tX)α1αi1Γ(α1αi)U(X)dX. (3.5)

    By differentiating (3.5), we get

    σ1U(t)=C11+1Γ(α1)tt1(tX)α11Y(X)dXpi=2σiΓ(α1αi)tt1(tX)α1αi1U(X)dX. (3.6)

    Now to compute σ1U(t1), σ1U(t1), σ1U(t+1) and σ1U(t+1) using (3.3)–(3.6), we obtain

    σ1U(t1)=C0+C1t1+1Γ(α1)t10(t1X)α11Y(X)dXpi=2t10σit1X)α1αi1Γ(α1αi)(U(X)dX,σ1U(t1)=C1+1Γ(α11)t10(t1X)α12Y(X)dXpi=2t10σi(t1X)α1αi2Γ(α1αi1)U(X)dX,σ1U(t+1)=C01,σ1U(t+1)=C11. (3.7)

    Using the impulsive condition

    Δ(U(t1))=U(t+1)U(t1)=I1U(t1),

    and

    Δ(U(t1))=U(t+1)U(t1)=I1U(t1),

    we get

    C01=σ1I1U(t1)+C0+C1t1+1Γ(α1)t10(t1X)α11Y(X)dXpi=2σi1Γ(α1αi)t10(t1X)α1αi1U(X)dX,C11=σ1I1U(t1)+C1+1Γ(α11)t10(t1X)α12Y(X)dXpi=2σi1Γ(α1αi1)t10(t1X)α1αi2U(X)dX. (3.8)

    Using (3.8) in (3.5), we obtain

    On the same fashion, for t(tk,tk+1], (3.1) becomes

    σ1U(t)=C0+tC1+σ1kj=1IjU(tj)+σ1k1j=1(tktj)IjU(tj)+σ1kj=1(ttk)IjU(tj)+σ1kj=11Γ(α1)tjtj1(tjX)α11Y(X)dX+kj=1ttkΓ(α11)tjtj1(tjX)α12Y(X)dX+k1j=1tktjΓ(α11)tjtj1(t1X)α12Y(X)dXkj=1pi=2σi1Γ(α1αi)tjtj1(tjX)α1αi1U(X)dXkj=1pi=2σi(ttk)Γ(α1αi1)tjtj1(tjX)α1αi2U(X)dX+1Γ(α1)ttk(tX)α11Y(X)dXk1j=1pi=2σi(tktj)Γ(α1αi1)tjtj1(tjX)α1αi2U(X)dXpi=2σiΓ(α1αi)ttk(tX)α1αi1U(X)dX. (3.9)

    By using the boundary conditions involve in (3.1), we obtain

    C1=b2a2+b2[mj=1tjtj1(tjX)α12Γ(α11)Y(X)dXmj=1pi=2tjtj1σi(tjX)α1αi2Γ(α1αi1)U(X)dXpi=2τtmσi(τX)α1αi2Γ(α1αi1)U(X)dX+1Γ(α11)τtm(τX)α12Y(X)dX]+σ1a2+b2g2(U) (3.10)

    and

    (3.11)

    One can obtain the desired integral form of solution (3.2), by using (3.10) and (3.11) in (3.9) and (3.3).

    Corollary 3.1. In view of Theorem 3.1 the solution of the given multi-terms fractional delay differential equation (1.2) is given by

    (3.12)

    Where (gi(i=1,2):C(J,R)R) are continuous functions, al+bl0 for l=1,2 and α1αi1>0 for i=2,3,,p and

    In this subsection of the research work, we represent the desired solution for MIFDDE (1.2), in the form of operator equation and provides some assumptions for investigation of existence results for proposed problem.

    Lets define T:XX, such that

    (3.13)

    We consider the following assumptions, which we needs for further correspondence in this work. (H1) For U1,U2X, there exist LF1,LF20, i.e

    |H(t,U1(t),U2(λt))H(t,U2(λt),U2(t))|LF1||U1U2||+LF2||U1U2||. (3.14)

    (H2) For U1,U2X, there exist Lgi>0, for i = 1, 2, such that

    |gi(U1)gi(U2)|Lgi||U1U2||. (3.15)

    (H3) For U1,U2X, there exist LI>0, such that

    |IkU1(t)IkU2(t)|LI||U1U2||. (3.16)

    (H4) For U1,U2X, there exist LI>0, such that

    |IkU1(t)IkU2(t)|LI||U1U2||. (3.17)

    (H5) For any UX, there exist BF:C(J,R+) such that

    |H(t,U(t),U(λt))|BF(t). (3.18)

    (H6) For any UX, there exist Bgi:C(J,R+) for i=1,2, such that

    |gi(U)|Bgi(t). (3.19)

    (H7) For any UX, there exist BI:C(J,R+), such that

    |IkU(t)|BI(t). (3.20)

    (H8) For any UX, there exist BI:C(J,R+), such that

    |IkU(t)|BI(t). (3.21)

    For computational convenience, we introduce the following notation:

    BI=(|b1||a1+b1|+1)m. (3.22)
    BI=(|b1||a1+b1|+1)τ(2m1). (3.23)
    Bg2=|b2||a2+b2|suptJ{|tτb1a1+b1|}. (3.24)
    (3.25)
    BC=pi=2|σi|τα1αi|σ1|Γ(α1αi)(m+1α1αi+2m1)+|b2||σ1||a2+b2|suptJ{|tτb1a1+b1|}pi=2(m+1)|σi|Γ(α1αi)τα1αi1+|b1||σ1||a1+b1|pi=2|σi|1Γ(α1αi)τα1αi(m+1α1αi+2m1)). (3.26)
    L=BILI+BILI+Lg1|a1+b1|+Bg2Lg2+BLFLF+BC. (3.27)
    Ld=BLFLF+BC. (3.28)
    BLR=BLFτα1|σ1|Γ(α1+1). (3.29)

    Theorem 3.2. Consider (H1)(H4) holds and L<1, then problem (1.2) has at most one fixed point, where L is defined by (3.27).

    Proof. Consider that U,UX and tJk where k = 1, 2…, m.

    |T(U(t))T(U(t))|1|σ1|[|σ1|kj=1LI||U1U2||+|σ1|k1j=1(tktj)LI||U1U2||+|σ1|kj=1suptJ{|ttk|}LI||U1U2||+|σ1|kj=11Γ(α1)tjtj1(tjX)α11(LF1||U1U2||+LF2||U1U2||)dX+kj=1|ttk|Γ(α11)tjtj1(tjX)α12(LF1||U1U2||+LF2||U1U2||)dX+k1j=1tktjΓ(α11)tjtj1(t1X)α12(LF1||U1U2||+LF2||U1U2||)dX+(kj=1pi=2tjtj1|σi|(tjX)α1αi1Γ(α1αi)+|σi||ttk|Γ(α1αi1)tjtj1(tjX)α1αi2)||UU||dX+k1j=1pi=2|σi|(tktj)Γ(α1αi1)tjtj1(tjX)α1αi2||UU||dX+suptJ{pi=2ttk|σi|(tX)α1αi1Γ(α1αi)||UU||dX}+suptJ{1Γ(α1)ttk(tX)α11(LF1||U1U2||+LF2||U1U2||)dX}]+1|a1+b1||g1(U)g1(U)|+|b2||a2+b2||tτb1a1+b1||g2(U)g2(U)|+|b1||a1+b1|[mj=1LI||U1U2||+m1j=1(tmtj)LI||U1U2||+mj=1suptJ{|ttm|}LI||U1U2||]+|b2||σ1||a2+b2|suptJ{|tτb1a1+b1|}[mj=11Γ(α11)tjtj1(tjX)α12(LF1||U1U2||
    +LF2||U1U2||)dX+mj=1pi=2|σi|1Γ(α1αi1)tjtj1(tjX)α1αi2||UU||dX+1Γ(α11)τtm(τX)α12(LF1||U1U2||+LF2||U1U2||)dX+pi=2|σi|1Γ(α1αi1)τtm(τX)α1αi2||UU||dX]+|b1||σ1||a1+b1|[mj=11Γ(α1)tjtj1(tjX)α11(LF1||U1U2||+LF2||U1U2||)dX+mj=1τtmΓ(α11)tjtj1(tjX)α12(LF1||U1U2||+LF2||U1U2||)dX+m1j=1tmtjΓ(α11)tjtj1(t1X)α12(LF1||U1U2||+LF2||U1U2||)dX+mj=1pi=2|σi|1Γ(α1αi)tjtj1(tjX)α1αi1||UU||dX+mj=1pi=2|σi|τtmΓ(α1αi1)tjtj1(tjX)α1αi2||UU||dX+1Γ(α1)τtm(τX)α11(LF1||U1U2||+LF2||U1U2||)dX+m1j=1pi=2|σi|tmtjΓ(α1αi1)tjtj1(tjX)α1αi2||UU||dX+pi=2|σi|1Γ(α1αi)τtm(τX)α1αi1||UU||dX]. (3.30)

    Let us assume LF=LF1+LF2 and evaluate the integral involve in (3.30), we have

    (3.31)

    It is quite clearly that tj1tjτ, hence by using the aforementioned inequality equation (3.31) can be express as

    |T(U(t))T(U(t))|||U1U2|||σ1|[LI|σ1|m+LI|σ1|τ(2m1)+LFτα1Γ(α1)(|σ1|m+1α1+2m1)+pi=2|σi|τα1αiΓ(α1αi)(m+1α1αi+2m1)]+Lg1||UU|||a1+b1|+|b2|Lg2||UU|||a2+b2|suptJ{|tτb1a1+b1|}+|b1|||UU|||a1+b1|(mLI+(2m1)τLI)+|b2||σ1||a2+b2|suptJ{|tτb1a1+b1|}[(m+1)τα11Γ(α1)LF+pi=2(m+1)|σi|Γ(α1αi)τα1αi1]+|b1|||UU|||σ1||a1+b1|[τα1Γ(α1)(m+1α1+(2m1))LF+pi=2|σi|1Γ(α1αi)τα1αi(m+1α1αi+2m1))]. (3.32)

    By rearranging term containing LI, LI, Lg1, Lg2 and LF in Eq (3.32), we obtain

    (3.33)

    Now using (3.22)–(3.27) in (3.33), we have

    |T(U(t))T(U(t))|||U1U2||[BILI+BILI+Lg1|a1+b1|+Bg2Lg2+BLFLF+BC]LUU.

    Therefore, by Banach contraction principal the mapping T has fixed point. Thus, the consider problem (1.2) has solution, which is unique.

    Theorem 3.3. The consider problem (1.2) has at least one solution, if (H1) and (H5)(H8) holds and Ld<1, where Ld is defined in (3.28).

    Proof. In order to prove existence of at least one solution, we define operator T1,T2:PC(J,R)PC(J,R) given by

    and

    Moreover, we construct a ball H={U(t)PC(J,R):UR}, with positive radius R chosen as

    R1(1BC)(BIBI(t)+BI||BI(t)||+||Bg1(t)|||a1+b1|+Bg2||Bg2(t)||+BLF||BF(t)||).

    Step 1: We claim that T1U1(t)+T2U2(t)HPC(J,R) for every U1(t),U2(t)HPC(J,R).

    Now for the proof of desired results, consider

    ||T1U1(t)+T2U2(t)||kj=1||BI(t)||+k1j=1(tktj)||BI(t)||+kj=1suptJ{|ttk|}||BI(t)||+1|a1+b1|||Bg1(t)||+|b2||a2+b2||tτb1a1+b1|||Bg2(t)||+|b1||a1+b1|[mj=1||BI(t)||+m1j=1(tmtj)||BI(t)||+mj=1suptJ{|ttm|}||BI(t)||]+1|σ1|[|σ1|kj=11Γ(α1)tjtj1(tjX)α11||BF(t)||dX+kj=1|ttk|Γ(α11)tjtj1(tjX)α12||BF(t)||dX+k1j=1tktjΓ(α11)tjtj1(t1X)α12||BF(t)||dX+kj=1pi=2|σi|1Γ(α1αi)tjtj1(tjX)α1αi1RdX+kj=1pi=2|σi||ttk|Γ(α1αi1)tjtj1(tjX)α1αi2RdX+k1j=1pi=2|σi|tktjΓ(α1αi1)tjtj1(tjX)α1αi2RdX+suptJ{1Γ(α1)ttk(tX)α11||BF(t)||dX}+suptJ{pi=2|σi|1Γ(α1αi)ttk(tX)α1αi1RdX}]+|b2||σ1||a2+b2|suptJ{|tτb1a1+b1|}[mj=1tjtj1(tjX)α12Γ(α11)||BF(t)||dX+τtm(τX)α12Γ(α11)||BF(t)||dX+mj=1pi=2|σi|1Γ(α1αi1)tjtj1(tjX)α1αi2RdX+pi=2|σi|1Γ(α1αi1)τtm(τX)α1αi2RdX]+|b1||σ1||a1+b1|[mj=11Γ(α1)tjtj1(tjX)α11||BF(t)||dX+mj=1τtmΓ(α11)tjtj1(tjX)α12||BF(t)||dX+m1j=1tmtjΓ(α11)tjtj1(t1X)α12||BF(t)||dX+mj=1pi=2|σi|1Γ(α1αi)tjtj1(tjX)α1αi1RdX+mj=1pi=2|σi|τtmΓ(α1αi1)tjtj1(tjX)α1αi2RdX+1Γ(α1)τtm(τX)α11||BF(t)||dX+m1j=1pi=2|σi|tmtjΓ(α1αi1)tjtj1(tjX)α1αi2RdX+pi=2|σi|1Γ(α1αi)τtm(τX)α1αi1RdX]. (3.34)

    By using (H5)(H8), and evaluating the integral in (3.34), we obtain

    By rearranging term containing LI, LI, Lg1, Lg2, and LF in (3.34), we obtain

    ||T1U1(t)+T2U2(t)||(|b1||a1+b1|+1)m||BI(t)||+(|b1||a1+b1|+1)τ(2m1)||BI(t)||+||Bg1(t)|||a1+b1|+|b2||a2+b2|suptJ{|tτb1a1+b1|}||Bg2(t)||+{τα1|σ1|Γ(α1)(|σ1|m+1α1+2m1)+|b2||σ1||a2+b2|suptJ{|tτb1a1+b1|}(m+1)τα11Γ(α1)+|b1||σ1||a1+b1|τα1Γ(α1)(m+1α1+(2m1))}||BF(t)||+R{pi=2τα1αiΓ(α1αi)(m+1α1αi+2m1)+|b2||σ1||a2+b2|suptJ{|tτb1a1+b1|}pi=2(m+1)|σi|Γ(α1αi)τα1αi1+|b1||σ1||a1+b1|pi=2|σi|1Γ(α1αi)τα1αi(m+1α1αi+2m1))}. (3.35)

    By using (3.22)–(3.26) in (3.35), we obtain

    Hence it show that T1U1(t)+T2U2(t)HPC(J,R).

    Step 2: Here we claim that F1 is uniformly bounded for confirmation, we proceed as

    (3.36)

    As we clearly see that ttmτ. So substitute τ instead of ttm in (3.36), then we obtain

    (3.37)

    Using (3.22)–(3.24) in (3.37), we obtain

    ||T1U1(t)+T2U2(t)||BI||BI(t)||+BI||BI(t)||+||Bg1(t)|||a1+b1|+Bg2||Bg2(t)||.

    Hence T1 is uniformly bounded.

    Step 3: Suppose Un(t) is a sequence in H which converge to UH for the continuity of T1 we have to prove F1(Un(t))T1(U(t)). For the proof we precede as

    ||T1Un(t)T1U(t)||kj=1|IjUn(tj)IjU(tj)|+k1j=1(tktj)|IjUn(tj)IjU(tj)|+kj=1suptJ{|ttk|}|IjUn(tj)IjU(tj)|]+1|a1+b1||g1(Un)g1(U)|+|b2||a2+b2|suptJ{|tτb1a1+b1|}|g2(Un)g2(U)|+|b1||a1+b1|[mj=1|IjUn(tj)IjU(tj)|+m1j=1(tmtj)|IjUn(tj)IjU(tj)|+mj=1suptJ{|ttm|}|IjUn(tj)IjU(tj)|].

    Hence clearly from the continuity of g1,g2,Ij and Ij, we get that T1 is continuous.

    Step 4: To prove T1 is equi-continuous. Consider

    clearly as t1t2 we have ||T1U(t2)T1U(t1)||=0. Hence T1 is equi-continuous.

    Step 5: To prove T2 is contraction, one can get help from Theorem 3.2 and obtain the following expression,

    ||T2U1(t)T2U2(t)||||U1U2||[{τα1(|σ1|m+1α1+2m1)+|b2||a2+b2|suptJ{|tτb1a1+b1|}(m+1)τα11|σ1|Γ(α1)+|b1||σ1||a1+b1|τα1Γ(α1)(m+1α1+(2m1))}LF+{pi=2τα1αiΓ(α1αi)(m+1α1αi+2m1)+|b2||σ1||a2+b2|suptJ{|tτb1a1+b1|}pi=2(m+1)|σi|Γ(α1αi)τα1αi1+|b1|||UU|||σ1||a1+b1|pi=2|σi|1Γ(α1αi)τα1αi(m+1α1αi+2m1))}]. (3.38)

    By using (3.25), (3.26) and (3.28) in (3.38), we obtain

    ||T2U1(t)T2U2(t)||||U1U2||[BLFLF+BC],Ld||UU||.

    Thus all assumption of Krasnoselskii's fixed point theorem are satisfied. So the problem (1.2) has at least one solution.

    The authors motivated by the literature [10,29] and present some specific findings for the stability analysis of the proposed problem (1.2).

    Definition 4.1. The solution U(t) of proposed problem will be Ulam-Hyres (UH) stable, if for unique solution U(t) one can find B1>0, such that for each solution UPC(J,R) of the following differential inequality and ϵ>0

    {|pi=1σicDαiU(t)f(t,U(t),U(λt))|ϵ,t[0,τ]|Δ(U(tk))IkU(tk)|ϵ,k=1,2,,m,|Δ(U(tk))IkU(tk)|ϵ,k=1,2,,m, (4.1)

    and a unique solution UPC(J,R) of the given problem (1.2), such that |UU|B1ϵ and solution will be generalized Ulam-Hyers (GUH) stable, if there exist a positive function K:(0,)(0,) with K(0)=0, such that |UU|B1K(t).

    Definition 4.2. The solution of consider problem is UH Rassias stable, with respect to continuous function χX and a positive constant ψ>0 if we have B2 (positive constant) >0, and ϵ>0, for each solution UPC(J,R) of the following differential inequality

    {|pi=1σicDαiU(t)f(t,U(t),U(λt))|χ(t)ϵ,t[0,τ]|Δ(U(tk))IkU(tk)|ψϵ,k=1,2,,m,|Δ(U(tk))IkU(tk)|ψϵ,k=1,2,,m, (4.2)

    and a unique solution UPC(J,R) of the given problem (1.2), such that |UU|B2(χ(t)+ψ)ϵ.

    Definition 4.3. The solution of consider problem is GUH Rassias stable, with respect to continuous function χX and a positive constant ψ>0 if we have B2(positive constant) >0, for each solution UPC(J,R) of the following differential inequality

    {|pi=1σicDαiU(t)f(t,U(t),U(λt))|χ(t),t[0,τ]|Δ(U(tk))IkU(tk)|ψ,k=1,2,,m,|Δ(U(tk))IkU(tk)|ψ,k=1,2,,m. (4.3)

    and a unique solution UPC(J,R) of the given problem (1.2), such that |UU|B2χ(t)ϵ.

    Remark 1. The solution of the inequality (4.1) is UPC(J,R), iff one can find a function ζPC(J,R), and a sequence ζk,k=1,2,,m. Depend on U, such that

    {(i)ζ(t)ϵ,ζkϵwherek=1,2,3,,m,tJ(ii)pi=1σicDαiU(t)=f(t,U(t),U(λt))+ζ(t),t[0,τ](iii)Δ(U(tk))=IkU(tk)+ζk,k=1,,m,(iv)Δ(U(tk))=IkU(tk)+ζk,k=1,,m. (4.4)

    Remark 2. Let UPC(J,R) be the solution of (4.2), iff one can find a function ζPC(J,R), and a sequence ζk,k=1,2,,m. Depend on U, such that

    {(i)ζ(t)χ(t)ϵ,ζkψϵwherek=1,2,3,,m,tJ(ii)pi=1σicDαiU(t)=f(t,U(t),U(λt))+ζ(t),t[0,τ](iii)Δ(U(tk))=IkU(tk)+ζk,k=1,,m,(iv)Δ(U(tk))=IkU(tk)+ζk,k=1,,m. (4.5)

    Remark 3. Let UPC(J,R) be the solution of (4.3), iff one can find a function ξPC(J,R), and a sequence ζk,k=1,2,,m. Depend on U, such that

    {(i)ζ(t)χ(t),ζkψwherek=1,2,3,,m,tJ(ii)pi=1σicDαiU(t)=f(t,U(t),U(λt))+ζ(t),t[0,τ](iii)Δ(U(tk))=IkU(tk)+ζk,k=1,,m,(iv)Δ(U(tk))=IkU(tk)+ζk,k=1,,m. (4.6)

    Lemma 4.1. Consider UPC(J,R) is solution of FDDE,

    (4.7)

    satisfy the following relation,

    |U(t)TU(t)|(BI+BI+BLF)ϵ.

    Proof. In light of Theorem 3.1, the solution of (4.7), is given as

    (4.8)

    By taking absolute on (4.8) and using Remark 1, we get

    By using (3.22), (3.23) and (3.25), we obtain

    |U(t)TU(t)|(BI+BI+BLF)ϵ.

    Which prove the required result.

    Theorem 4.4. Under the assumptions (H1H4), the problem (1.2) is UH as well as GUH stable, if L<1, where L is defined in (3.27).

    Proof. For any solution UPC(J,R), and unique solution U of the the given problem (1.2), then

    ||U(t)U(t)||=||U(t)TU(t)||=||U(t)TU+TUTU||,||U(t)TU||+||TUTU||.

    Using Theorem 3.2 and Lemma 4.1 we have

    ||U(t)U(t)||LUϵ+L||U(t)U(t)||,||U(t)U(t)||L||U(t)U(t)||LUϵ,||U(t)U(t)||LU1Lϵ.

    Let B1=LU1L, then the solution of the consider problem (1.2) is UH stable further set K(ϵ)=ϵ then the consider problem (1.2) is GUH stable.

    To prove the next stability result we need the following assumption given as (H9). For any non decreasing function χPC(J,R+) there exist a positive constant G, such that

    1Γ(α1)ttk(tX)α11χ(X)dXGχ(t).

    Lemma 4.2. If assumption (H9) holds then for any solution xPC(J,R) the muti-term fractional delay differential equation

    {pi=1σicDαiU(t)=f(t,U(t),U(λt))+ζ(t),α1(1,2]αi(0,1], fori=2,3,,p,t[0,τ]Δ(U(tk))=IkU(tk),Δ(U(tk))=IkU(tk),k=0,1,,m,a1U(0)+b1U(τ)=g1(U),a2U(0)+b2U(τ)=g2(U),al,blRforl=1,2 (4.9)

    satisfy the following relation,

    |U(t)TU(t)|(BI+BI+BLR)Aϵ+Gσ1χ(t)ϵ.

    Proof. We omit the proof as it is straightforward and may be derived like Lemma 4.1.

    Theorem 4.5. Under the assumption (H1H4) and H9, the problem (1.2) is UHR stable and GUHR stable, if L<1.

    Proof. For any solution UPC(J,R), and unique solution U of the the given problem (1.2), then

    ||U(t)U(t)||=||U(t)TU(t)||=||U(t)TU+TUTU||||U(t)TU||+||TUdTU||.

    Using Theorem 3.2 and Lemma 4.2, we have

    ||U(t)U(t)||(BI+BI+BLR)Aϵ+G|σ1|χ(t)ϵ+L||U(t)U(t)||,||U(t)U(t)||L||U(t)U(t)||(BI+BI+BLR)Aϵ+G|σ1|χ(t)ϵ,||U(t)U(t)||(BI+BI+BLR)A+G|σ1|χ(t)1Lϵ.

    Let B1=max(BI+BI+BLR,G|σ1|)1L, then the solution of the consider problem (1.2) is UHR stable further set ϵ=1 then the consider problem (1.2) is GUHR stable.

    Here we present an example to demonstrate our results.

    Example 1. Consider the following multi-term impulsive fractional delay differential equation

    {pi=11010i9cD41+2iU(t)=L(3t3+44et+55t)2(2|U(t)|cos(t)+|U(t)|t3|U(t6)|sec(t)+|U(t8)|cosh(t)),t[0,1],t14,LR+Δ(U(14))=IkU(14)=|U(14)|32+|U(14)|,Δ(U(14))=IkU(14)=|U(14)|54+|U(14)|,8U(0)+U(1)=g1(U)=|U|100+|U|,6U(0)+U(1)=g2(U)=142+|U|, (5.1)

    here

    p=5,m=1,a1=8,b1=b2=1,a2=6,τ=1,τ=1,
    α1=4/3,αi=41+2i,σ1=10,σi=1010i9.
    |H(t,U(t),U(t6))f(t,U1(t),U(t6)|L(3t3+44et+55t)2(|2|U1(t)|cos(t)+|U1(t)|2|U2(t)|cos(t)+|U2(t)||+|t3|U1(t6)|sec(t)+|U1(t8)|t3|U2(t6)|sec(t)+|U2(t8)||)L442(2cos(t)|U1(t)U2(t)|+t3sec(t)|U1(t)U2(t)|).

    Hence, we obtain LF=L442(2cos(1)+1), and similarly by simple computation, one can calculate,

    Lg1=1100,Lg2=11764,LI=132,andLI=154.

    Hence, we can calculate that L<1 if G<24.608599. Now as a consequence of Theorem 3.2, we conclude that example 1, has unique solution.

    Set χ(t)=(4t1)2, and ψ=3tJ. since

    1Γ(43)t14(tX)431(4X1)2dX=32Γ(133)(t14)10326.3103(4t1)2

    condition H9 is satisfied with G=26.3103. Hence all assumption of Theorem 4.5 are satisfied so as a conclusion the solution of problem 1.2 is UHR and GUHR stable. Moreover problem (1.2) is UH and GUH stable due to Theorem 4.4.

    In this research work we have established a detailed analysis about existence theory of at least one solution to a class of multi term impulsive FODEs. The required theory has been established by using Krasnoselskii's fixed-point theorem and Banach contraction principle. Also keeping in mind the importance of stability, we have developed some results regarding different kinds of Ulam stability including HU, GHU, HUR and GHUR. The obtained analysis has been demonstrated by using pertinent examples.

    Authors Kamal Shah, Nabil Mlaiki and Thabet Abdeljawad would like to thank Prince Sultan University for paying the APC and support through research Lab TAS.

    No conflict of interest exists.



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