Research article Special Issues

Study of implicit-impulsive differential equations involving Caputo-Fabrizio fractional derivative

  • This article is devoted to investigate a class of non-local initial value problem of implicit-impulsive fractional differential equations (IFDEs) with the participation of the Caputo-Fabrizio fractional derivative (CFFD). By means of Krasnoselskii's fixed-point theorem and Banach's contraction principle, the results of existence and uniqueness are obtained. Furthermore, we establish some results of Hyers-Ulam (H-U) and generalized Hyers-Ulam (g-H-U) stability. Finally, an example is provided to demonstrate our results.

    Citation: Thanin Sitthiwirattham, Rozi Gul, Kamal Shah, Ibrahim Mahariq, Jarunee Soontharanon, Khursheed J. Ansari. Study of implicit-impulsive differential equations involving Caputo-Fabrizio fractional derivative[J]. AIMS Mathematics, 2022, 7(3): 4017-4037. doi: 10.3934/math.2022222

    Related Papers:

    [1] Kamal Shah, Thabet Abdeljawad, Bahaaeldin Abdalla, Marwan S Abualrub . Utilizing fixed point approach to investigate piecewise equations with non-singular type derivative. AIMS Mathematics, 2022, 7(8): 14614-14630. doi: 10.3934/math.2022804
    [2] Zhoujin Cui . Solutions of some typical nonlinear differential equations with Caputo-Fabrizio fractional derivative. AIMS Mathematics, 2022, 7(8): 14139-14153. doi: 10.3934/math.2022779
    [3] Gulalai, Shabir Ahmad, Fathalla Ali Rihan, Aman Ullah, Qasem M. Al-Mdallal, Ali Akgül . Nonlinear analysis of a nonlinear modified KdV equation under Atangana Baleanu Caputo derivative. AIMS Mathematics, 2022, 7(5): 7847-7865. doi: 10.3934/math.2022439
    [4] Saïd Abbas, Mouffak Benchohra, Juan J. Nieto . Caputo-Fabrizio fractional differential equations with instantaneous impulses. AIMS Mathematics, 2021, 6(3): 2932-2946. doi: 10.3934/math.2021177
    [5] Sadia Arshad, Iram Saleem, Ali Akgül, Jianfei Huang, Yifa Tang, Sayed M Eldin . A novel numerical method for solving the Caputo-Fabrizio fractional differential equation. AIMS Mathematics, 2023, 8(4): 9535-9556. doi: 10.3934/math.2023481
    [6] Khalid K. Ali, K. R. Raslan, Amira Abd-Elall Ibrahim, Mohamed S. Mohamed . On study the fractional Caputo-Fabrizio integro differential equation including the fractional q-integral of the Riemann-Liouville type. AIMS Mathematics, 2023, 8(8): 18206-18222. doi: 10.3934/math.2023925
    [7] Murugesan Sivashankar, Sriramulu Sabarinathan, Vediyappan Govindan, Unai Fernandez-Gamiz, Samad Noeiaghdam . Stability analysis of COVID-19 outbreak using Caputo-Fabrizio fractional differential equation. AIMS Mathematics, 2023, 8(2): 2720-2735. doi: 10.3934/math.2023143
    [8] Kishor D. Kucche, Sagar T. Sutar, Kottakkaran Sooppy Nisar . Analysis of nonlinear implicit fractional differential equations with the Atangana-Baleanu derivative via measure of non-compactness. AIMS Mathematics, 2024, 9(10): 27058-27079. doi: 10.3934/math.20241316
    [9] H. H. G. Hashem, Hessah O. Alrashidi . Qualitative analysis of nonlinear implicit neutral differential equation of fractional order. AIMS Mathematics, 2021, 6(4): 3703-3719. doi: 10.3934/math.2021220
    [10] Ritu Agarwal, Mahaveer Prasad Yadav, Dumitru Baleanu, S. D. Purohit . Existence and uniqueness of miscible flow equation through porous media with a non singular fractional derivative. AIMS Mathematics, 2020, 5(2): 1062-1073. doi: 10.3934/math.2020074
  • This article is devoted to investigate a class of non-local initial value problem of implicit-impulsive fractional differential equations (IFDEs) with the participation of the Caputo-Fabrizio fractional derivative (CFFD). By means of Krasnoselskii's fixed-point theorem and Banach's contraction principle, the results of existence and uniqueness are obtained. Furthermore, we establish some results of Hyers-Ulam (H-U) and generalized Hyers-Ulam (g-H-U) stability. Finally, an example is provided to demonstrate our results.



    In recent decades, fractional differential equations have received great attention from the researchers in many applied fields such as physics, biology, chemistry and other fields of sciences and engineering [1,2,3,4,5,6,7,32]. Due to many applications, this area has been studied with different fractional derivatives such as Riemman-Liouvile, Caputo, Hilfer and Hadamard type fractional derivatives [8,9,10,11,12,30,31]. Further, the fractional time derivatives are importance reactive-transport, since solutes may interact immobile porous medium in highly non-linear ways, some of the investigator using fractional time derivatives for the solution of space-time fractional diffusion equations [41,42]. But now a days the researchers are studying a new type of fractional derivative which is called Caputo-Fabrizio fractional derivative. This fractional derivative is also known as a non-singular kernel or exponential kernel type derivative. In 2015, Caputo and Fabrizio together introduced this derivative [13]. Latter on, Caputo-Fabrizio derivatives was used by many researchers for modeling various problems in engineering sciences (look for example some articles [35,36]. Further, this type of derivative have many applications. Such as it is use an exponential decay kernel to a novel HIV/AIDS epidemic model that includes an anti-retrovirus treatment compartment [37], and also some researcher apply this new type of the fractional derivative for the dynamical system with both chaotic and non-chaotic behaviors [38], hyper-chaotic behaviors, optimal control and synchronization [39], nonstandard finite difference scheme and non-identical synchronization of a novel fractional chaotic system [40]. Furthermore, the researchers studied the aforementioned area looking for results of existence, uniqueness and stability. Some of the articles we refer to see the reader to earlier works [14,15,16,17,18].

    On the other hand, impulsive differential equations (IDEs) have played an important role in the modeling of phenomena, chiefly in the description of dynamics to sudden changes as well as other phenomena such as crops, diseases, etc. The said differential systems have been used to designate the model since the previous century. For the fundamentals theory on IDEs the reader can consult the monographs of Burton and Simeonov [19], Lakshmikantham et al. [20], Benchohra et al. [21]. Recently, impulsive FDEs are increasingly used to constitute an impulsive control theory. This theory is used to model some physical phenomena. The said area has become a very important direction in IDEs theory. Further numerous applications of IDEs to problems arising in satellite orbital transfer [24], ecosystem management [25], electrical engineering [26], etc. Here refer for further applications on IDEs [28,29,33]. When reviewing the existence literature, we see that very rarely it has been investigated IFDEs with the participation of the CFFD. For instance recently author [22] investigated the following problem of IDE with CFFD as

    {CF0Dωru(r)=f(r,u(r)),rJ,rrk,Δu(rk)=Ik(u(rk)),k=1,2,3,...,n,u(0)=u0, (1.1)

    where CF0Dωr represent CFFD of order ω, J=[0,T], u0R, the given function f:J×RR, Ik:RR are continuous. Where Δu(rk) represent change of right and left hand limit of the discontinuity points rk, it is define as Δu(rk)=u(r+k)u(rk).

    Inspired by the research work as mentioned above, we intend to work on implicit-IFDEs involving CFFD of the form:

    {CF0Dωru(r)=g(r,u(r), CF0Dωru(r)), rJ,rrk,Δu(rk)=Ik(u(rk)),k=1,2,3,...,n,u(0)=f(u), (1.2)

    where CF0Dωr represents the CFFD of order 0<ω<1, g:J×R×RR,Ik:RR and f:RR are continuous function. Where Δu(rk) represent change of right and left hand limit of the discontinuity points rk, it is define as Δu(rk)=u(r+k)u(rk). By using Krasnoselskii's and Banach fixed point theorems, we establish the existence theory for the considered problem. Also we develop some results for Hyers-Ulam (H-U) and generalized (G-H-U) stability. Pertinent example is given to verify our results. Further keeping in mind that right hand side of problem (1.2) vanish at r=0 as suggested in [43].

    In this article, we use a new type of fractional derivative with non-singular kernel involving non-local initial condition and implicit functions is proposed. The introduced fractional derivative includes as a special case Caputo-Fabrizio fractional derivative, and also study the implicit-FDEs with using impulsive condition for the solution of existence, uniqueness and stability results. Next take two counter examples to verify the necessary results.

    In section 2, some basics preliminaries on fractional calculus are presented. In section 3, We develop a results and discussion of implicit-IFDEs using an arbitrary non-singular kernel, such as Caputo-Fabrizio fractional derivative. In section 4, we will investigate the stability results of Hyers-Ulam and generalize Hyers-Ulam stability for the proposed problem of implicit-IFDEs. In section 5, take some counter examples and its graphs to verify the necessary results. In the last section 6, take concluding remarks of our article.

    In this part of our article, we need to provide some basic results and definitions of fractional calculus. We derived our main results through using these basic results.

    Definition 1. [27] For 0<ω<1,uH1(0,a). The CFFD for a function u of order ω is defined as

    CF0Dωru(r)=(2ω)M(ω)2(1ω)r0exp(ω1ω(rθ))u(θ)dθ, (2.1)

    where M(ω) is a normalization constant depending on ω.

    Definition 2. [27] For 0<ω<1, the fractional integral for a function u is given by

    CF0Iωru(r)=2(1ω)(2ω)M(ω)u(r)+2ω(2ω)M(ω)r0u(θ)dθ. (2.2)

    When ω=1, then we get first order classical integral using Remark 1. This convergent has been proved in [34].

    Remark 1. [22] Note that according to the previous definition, the fractional integral of a function u with order 0<ω<1 is an average between function u and its integral of one. Imposing

    2(1ω)(2ω)M(ω)+2ω(2ω)M(ω)=1,

    it can be concluded that

    M(ω)=22ω,0ω1.

    Lemma 1. [22] The unique solution of the given initial value problem

    {CF0Dωru(r)=y(r),0<ω<1,u(0)=u0R, (2.3)

    is given by

    u(r)=u0+2(1ω)(2ω)M(ω)(y(r)y(0))+2ω(2ω)M(ω)r0y(θ)dθ,

    where

    Gω=2(1ω)(2ω)M(ω)=1ω,Qω=2ω(2ω)M(ω)=ω.

    Let C(J,R) be the space of all continuous functions defined on the interval J endowed with the usual supremum norm, that as:

    uC=suprJu(r).

    Let the set of functions

    X=PC(J,R)={u:JRuC((rk,rk+1],R)},k=0,1,2,3,...,m

    and there exist u(r+k) and u(rk),k=1,2,3,4,...,m. The given set is Banach space with the norm is defined as:

    uPC=maxrJ|u(r)|.

    Theorem 1. [23] Let Y be non empty, convex and closed subset of X. Consider two operators T, S such that

    1) T(y1)+S(y2)Y, for all y1,y2Y.

    2) T is contraction operator.

    3) S is continuous and compact.

    then there exists at least one solution yX such that T(y)+S(y)=y.

    The present section of our paper is reserved to investigate the existence and uniqueness for the solution of the implicit-IFDEs by Krasnoselskii's and Banach fixed point theorems.

    Lemma 2. Suppose 0<ω<1 and τ:JR be continuous. A function uX is the solution of the given impulsive problem:

    {CF0Dωru(r)=τ(r),0<ω<1,rJ,rrk,Δu(rk)=Ik(u(rk)),k=1,2,3,...,n,u(0)=f(u). (3.1)

    If and only if it satisfies

    u(r)={f(u)+Gω[τ(r)τ(0)]+Qωr0τ(η)dη,forr[0,r1],f(u)+Gω[τ(r)τ(0)]+I1(u(r1))+Qωr10τ(η)dη+Qωr0τ(η)dη,forr[r1,r2],f(u)+Gω[τ(r)τ(0)]+I1(u(r1))+I2(u(r2))+Qωr10τ(η)dη+Qωr20τ(η)dη+Qωr0τ(η)dη,forr[r2,r3],...,f(u)+Gω[τ(r)τ(0)]+ki=1Ii(u(ri))+Qωki=1ri0τ(η)dη+Qωr0τ(η)dη,forr[rk,rk+1],wherek=1,2,...,m. (3.2)

    Proof. Suppose u(r) satisfies (3.1). If r[0,r1], then

    CF0Dωru(r)=τ(r),r(0,r1]withu(0)=f(u).

    Using Lemma 1, we get

    u(r)=f(u)+Gω[τ(r)τ(0)]+Qωr0τ(η)dη. (3.3)

    Now applying impulsive condition u(r1), one has

    u(r1)=f(u)+Gω[τ(r1)τ(0)]+Qωr10τ(η)dη. (3.4)

    Again if r[r1,r2], then

    CFr1Dωru(r)=τ(r),r(r1,r2]withu(r+1)=u(r1)+I1(u(r1)).

    Again using Lemma 1, we can obtain

    u(r)=u(r+1)+Gω[τ(r)τ(r1)]+Qωr0τ(η)dη=u(r1)+I1(u(r1))+Gω[τ(r)τ(r1)]+Qωr0τ(η)dη.

    Further using (3.4), we get

    u(r)=f(u)+Gω[τ(r1)τ(0)]+Qωr10τ(η)dη+I1(u(r1))+Gω[τ(r)τ(r1)]+Qωr0τ(η)dη.

    Upon further simplification, we have

    u(r)=f(u)+Gω[τ(r)τ(0)]+I1(u(r1))+Qωr10τ(η)dη+Qωr0τ(η)dη. (3.5)

    Again using impulsive condition u(r2) in (3.5), we obtain

    u(r2)=f(u)+Gω[τ(r2)τ(0)]+I1(u(r1))+Qωr10τ(η)dη+Qωr20τ(η)dη. (3.6)

    If r[r2,r3], then

    CFr2Dωru(r)=τ(r),r(r2,r3]withu(r+2)=u(r2)+I2(u(r2)).

    Again using Lemma 1, we can obtain

    u(r)=u(r+2)+Gω[τ(r)τ(r2)]+Qωr0τ(η)dη=u(r2)+I2(u(r2))+Gω[τ(r)τ(r2)]+Qωr0τ(η)dη.

    By using (3.6), we get

    u(r)=f(u)+Gω[τ(r2)τ(0)]+I1(u(r1))+Qωr10τ(η)dη+Qωr20τ(η)dη+I2(u(r2))+Gω[τ(r)τ(r2)]+Qωr0τ(η)dη.

    Further simplify, we get

    u(r)=f(u)+Gω[τ(r)τ(0)]+I1(u(r1))+I2(u(r2))+Qωr10τ(η)dη+Qωr20τ(η)dη+Qωr0τ(η)dη.

    Furthermore, continue this process we obtain for r[rk,rk+1] as

    u(r)=f(u)+Gω[τ(r)τ(0)]+ki=1Ii(u(ri))+Qωki=1ri0τ(η)dη+Qωr0τ(η)dη,wherek=1,2,...,m.

    Similarly, if u(r) satisfies (3.2), then we can prove that u(r) is the solution of (3.1). This complete the proof.

    Corollary 1. In view of Lemma 2, the solution of the said problem (1.2) is given by

    u(r)={f(u)+Gω[g(r,u(r), CF0Dωru(r))g(0,u(0), CF0Dωru(0))]+Qωr0g(η,u(η), CF0Dωηu(η))dη,forr[0,r1],f(u)+Gω[g(r,u(r), CF0Dωru(r))g(0,u(0), CF0Dωru(0))]+I1(u(r1))+Qωr10g(η,u(η), CF0Dωηu(η))dη+Qωr0g(η,u(η), CF0Dωηu(η))dη,forr[r1,r2],f(u)+Gω[g(r,u(r), CF0Dωru(r))g(0,u(0), CF0Dωru(0))]+I1(u(r1))+I2(u(r2))+Qωr10g(η,u(η), CF0Dωηu(η))dη+Qωr20g(η,u(η), CF0Dωηu(η))dη+Qωr0g(η,u(η), CF0Dωηu(η))dη,forr[r2,r3],...,f(u)+Gω[g(r,u(r), CF0Dωru(r))g(0,u(0), CF0Dωru(0))]+ki=1Ii(u(ri))+Qωki=1ri0g(η,u(η), CF0Dωηu(η))dη+Qωr0g(η,u(η), CF0Dωηu(η))dη,forr[rk,rk+1].

    For the sake of simplicity, we use g(r,u(r), CF0Dωru(r))=δu(r) and g(r,ˉu(r), CF0Dωrˉu(r))=ˉδu(r) also at r=0, we use δu(0)=δ0. Further, for qualitative results, we need to transform the proposed problem (1.2) to fixed point problem, we need to define an operator T:XX defined as:

    Tu(r)=f(u)+Gω[δu(r)δ0]+ki=1Ii(u(ri))+Qωki=1ri0δu(η)dη+Qωr0δu(η)dη. (3.7)

    First of all we introduce some hypothesis which are needed:

    (H1) The function g:J×R×RR is continuous.

    (H2) There exist positive constants Cg>0 and 0<Cg<1, such that

    |g(r,u(r),δu(r))g(r,ˉu(r),ˉδu(r))|Cg|u(r)ˉu(r)|+Cg|δu(r)ˉδu(r)|.

    (H3) The function Ik:RR are continuous and there exists positive constant 0<Lk<1 with nk=1Lk<1, such that

    nk=1|Ik(u(r))Ik(ˉu(r))|nk=1Lk|u(r)ˉu(r)|,

    for all u,ˉuR, k=1,2,3,...,n. Further we use nk=1Lk=LI throughout the paper.

    (H4) The function f:RR is continuous and there exists constant 0<Kf<1, such that

    |f(u)f(ˉu)|Kf|uˉu|.

    Theorem 2. Under the hypothesis H1H4, the impulsive problem (1.2) has a unique solution if

    [Kf+LI+(Gω+(n+1)Qω)TCg1Cg]<1.

    Proof. Suppose for each rJ and any u(r),ˉu(r)X, we have in view of (3.7)

    |Tu(r)Tˉu(r)||f(u)f(ˉu)|+Gω|δu(r)ˉδu(r)|+nk=1|Ik(u(r))Ik(ˉu(r))|+Qωnk=1rk0|δu(η)ˉδu(η)|dη+Qωr0|δu(η)ˉδu(r)(η)|dη, (3.8)

    where δu(r)=g(r,u(r),δu(r)), so

    |δu(r)ˉδu(r)(r)|=|g(r,u(r),δu(r))g(r,ˉu(r),ˉδu(r))|Cg|u(r)ˉu(r)|+Cg|δu(r)ˉδu(r)|.

    Continuing the above process, so we obtain

    |δu(r)ˉδu(r)|Cg1Cg|u(r)ˉu(r)|. (3.9)

    Using the hypothesis (H3), (H4) and (3.9) in Eq (3.8), we get

    |Tu(r)Tˉu(r)|Kf|uˉu|+Gω(Cg1Cg)|uˉu|+nk=1Lk|uˉu|+Qω(Cg1Cg)nk=1rk0|uˉu|dη+Qω(Cg1Cg)r0|uˉu|dη.

    Taking maximum on both side, we get

    maxrJ|Tu(r)Tˉu(r)|KfmaxrJ|u(r)ˉu(r)|+Gω(Cg1Cg)maxrJ|u(r)ˉu(r)|+nk=1LkmaxrJ|u(r)ˉu(r)|+Qω(Cg1Cg)nk=1maxrJrk0|u(r)ˉu(r)|dη+Qω(Cg1Cg)maxrJr0|u(r)ˉu(r)|dη.
    TuTˉuPC[Kf+Gω(Cg1Cg)+LI+nTQω(Cg1Cg)+TQω(Cg1Cg)]uˉuPC,[Kf+LI+(Gω+(n+1)TQω)Cg1Cg]uˉuPC.

    Hence the constant given as

    [Kf+LI+(Gω+(n+1)TQω)Cg1Cg]<1.

    Therefore, the operator T is contraction, so the operator has a unique fixed point, therefore the said problem (1.2) has a unique solution.

    Next second main result is based on the Krasnoselskii's fixed-point theorem. For this results we need some hypothesis which is given below.

    (H5) There exist some positive constants Pg,Qg,Rg>0 and 0<Qg<1, such that

    |g(r,u(r),δu(r))|Pg+Qg|u(r)|+Rg|δu(r)|,

    for each rJ and u(r),δu(r)R.

    (H6) There exists positive constant Kf>0, such that

    |f(u)|Kf|u(r)|,

    for u(r)R.

    Theorem 3. Under the hypothesis (H2)(H6) are satisfied, then the implicit-impulsive problem (1.2) has at least one solution if

    0<(Kf+GωCg1Cg+LI)<1.

    Proof. For the proof of this theorem, we need to define two operators from (3.7), we have

    T1u(r)=f(u)+Gω[δu(r)δ0]+ki=1Ii(u(ri))

    and

    T2u(r)=Qωki=1ri0δ(η)dη+Qωr0δ(η)dη.

    Let us define a set for a real number q>0 as H={u(r)X:uPCq}, we need to show the operator T1, is contraction. For this suppose u(r),ˉu(r)X, we have

    |T1u(r)T1ˉu(r)||f(u)f(ˉu)|+Gω|δu(r)ˉδu(r)|+nk=1|Ik(u(r))Ik(ˉu(r))|.

    Using hypothesis (H3), (H4) and (3.9), then taking maximum on both side, we get

    maxrJ|T1u(r)T1ˉu(r)|KfmaxrJ|u(r)ˉu(r)|+GωCg1CgmaxrJ|u(r)ˉu(r)|+nk=1LkCg1CgmaxrJ|u(r)ˉu(r)|.
    T1uT1ˉuPC(Kf+GωCg1Cg+LI)uˉuPC.

    Here the given constant is

    (Kf+GωCg1Cg+LI)<1.

    Hence the operator T1 is contraction. Next we need to prove that the operator T2 is compact and continuous, for this u(r)X, we have

    |T2u(r)|Qωnk=1rk0|δ(η)|dη+Qωr0|δ(η)|dη, (3.10)

    where

    |δu(r)|=|g(r,u(r),δu(r))|Pg+Qg|u(r)|+Rg|δu(r)|.

    Upon further simplification, we have

    |δu(r)|Pg1Rg+(Qg1Rg)|u(r)|. (3.11)

    Using (3.11) in (3.10) and then taking maximum, we get

    maxrJ|T2u(r)|nQω[Pg1Rg+(Qg1Rg)]maxrJ(rk|u(r)|)+Qω[Pg1Rg+(Qg1Rg)]maxrJ(r|u(r)|).
    T2uPC(n+1)QωT[Pg1Rg+(Qg1Rg)]uPC,T2uPCA,

    where

    A=(n+1)QωT[Pg1Rg+(Qg1Rg)]q.

    Hence the operator T2 is bounded. Further suppose r1<r2 in J, we have

    |T2u(r2)T2u(r1)|=|Qωnk=1rk0δ(η)dη+Qωr20δ(η)dηQωnk=1rk0δ(η)dηQωr10δ(η)dη|,Qωr20|δ(η)|dη+Qω0r1|δ(η)|dη. (3.12)

    Using (3.11) in (3.12), we get

    |T2u(r2)T2u(r1)|Qω[Pg1Rg+(Qg1Rg)|u(r)|](r2r1).

    Taking maximum on right hand side, we have

    |T2u(r2)T2u(r1)|Qω[Pg1Rg+(Qg1Rg)maxrJ|u(r)|](r2r1)Qω[Pg1Rg+(Qg1Rg)uPC](r2r1).

    Further

    |T2u(r2)T2u(r1)|Qω[Pg1Rg+(Qg1Rg)q](r2r1). (3.13)

    Obviously, from (3.13), we look that if r1r2, then the right hand side of the Eq (3.13) goes to zero, so |T2u(r2)T2u(r1)|0 as if r1r2. Hence we observe that the right-hand side of (3.13) goes to zero uniformly. Therefore, the operator T2 is equicontinuou. Therefore the operator T2 is compact by Arzelá-Ascoli theorem. Hence in view of Krasnoselskii theorem, we conclude that (1.2) has at least one solution.

    In this part of our article, we will investigate the stability of H-U and g-U-H stability for the problem of implicit-IFDEs.

    Definition 3. H-U stable

    The said implicit-impulsive problem (1.2), is H-U stable if any ϵ>0 for the given inequality

    |CF0Dωru(r)g(r,u(r),CF0Dωru(r))|ϵ,rJ.

    Then, there exists unique solution ˉu(r) with a constant Z such that

    |u(r)ˉu(r)|Zϵ,rJ.

    Definition 4. Generalized H-U stable Our implicit-impulsive problem is g-H-U stable if there exists non-decreasing function ϕ:(0,T)(0,), such that

    |u(r)ˉu(r)|Zϕ(ϵ),rJ.

    With ϕ(0)=0,ϕ(T)=0.

    Also we discuss important remark here which is used in this section as:

    Remark 2. Suppose there exists a function Ψ(r), which is depend on uX with Ψ(0)=0,Ψ(T)=0 such that

    (1) |Ψ(r)|ϵ,rJ,

    (2) CF0Dωru(r)=g(r,u(r),CF0Dωru(r))+Ψ(r),rJ.

    Lemma 3. The solution of given proposed problem

    {CF0Dωru(r)=g(r,u(r),CF0Dωru(r))+Ψ(r),0<ω<1,rJ=[0,T],rrk,Δu(rk)=Ik(u(rk)),k=1,2,3,...,n,u(0)=f(u),

    is

    u(r)=f(u)+Gω[δu(r)δ0]+Gω[Ψ(r)Ψ(0)]+nk=1Ik(u(rk))+Qωnk=1rk0δ(η)dη+Qωnk=1rk0Ψ(η)dη+Qωr0δ(η)dη+Qωr0Ψ(η)dη,rJ,wherek=1,2,3,...,n. (4.1)

    where δu(r)=g(r,u(r),CF0Dωru(r)) and Ψ(0)=0. Further, from the solution (4.1), we get

    |u(r)[f(u)+Gω[δu(r)δ0]+ki=1Ii(u(ri))+Qωki=1ri0δ(η)dη+Qωr0δ(η)dη]|(Gω+QωT(n+1))ϵ. (4.2)

    Proof. The solution of (4.1) can be easily obtained through using Lemma 2. Although from the solution it is clear to become result (4.2), by using Remark 2.

    Theorem 4. Under the Lemma 3, solution of the said implicit-impulsive problem (1.2), is H-U and g-H-U stable if

    Z=(Gω+QωT(n+1))1(Kf+LI+(Gω+(n+1)TQω)Cg1Cg)<1.

    Proof. Suppose u(r)X be any solution of the mentioned problem (1.2) and ˉu(r)X be unique solution of the said problem, then we need to consider

    |u(r)ˉu(r)|=|u(r)[f(ˉu)+Gω[ˉδu(r)δ0]+nk=1Ik(ˉu(rk))+Qωnk=1rk0ˉδ(η)dη+Qωr0ˉδ(η)dη]|,=|u(r)[f(u)+Gω[δu(r)δ0]+ki=1Ii(u(ri))+Qωnk=1rk0δ(η)dη+Qωr0δ(η)dη]+[f(u)+Gω[δu(r)δ0]+nk=1Ik(u(rk))+Qωnk=1rk0δ(η)dη+Qωr0δ(η)dη][f(ˉu)+Gω[ˉδu(r)δ0]+nk=1Ik(ˉu(rk))+Qωnk=1rk0ˉδ(η)dη+Qωr0ˉδ(η)dη]|
    |u(r)ˉu(r)||u(r)[f(u)+Gω[δu(r)δ0]+nk=1Ik(u(rk))+Qωnk=1rk0δ(η)dη+Qωr0δ(η)dη]|+|f(u)f(ˉu)|+Gω|δu(r)ˉδu(r)|+nk=1|Ik(u(rk))Ik(ˉu(rk))|+Qωnk=1rk0|δ(η)ˉδ(η)|dη+Qωr0|δ(η)ˉδ(η)|dη].

    Using (4.2), (3.9) and hypothesis H3,H4 and then taking maximum on both side, we get

    |u(r)ˉu(r)|(Gω+QωT(n+1))ϵ+(Kf+GωCg1Cg+LI+nQωCg1Cgrk+QωCg1Cgr)|u(r)ˉu(r)|.
    maxrJ|u(r)ˉu(r)|(Gω+QωT(n+1))ϵ+maxrJ(Kf+GωCg1Cg+LI+nQωCg1Cgrk+QωCg1Cgr)maxrJ|u(r)ˉu(r)|.

    Upon further simplification

    uˉuPC(Gω+QωT(n+1))ϵ+(Kf+LI+(Gω+(n+1)TQω)Cg1Cg)uˉuPC.

    Hence from the above inequality, we get

    uˉuPC(Gω+QωT(n+1))ϵ1(Kf+LI+(Gω+(n+1)TQω)Cg1Cg),

    which gives

    uˉuPCZϵ. (4.3)

    Therefore, solution is H-U stable. And there exists non-decreasing function ϕX. Then from Eq (4.3), we can be write as

    uˉuPCZϕ(ϵ),

    with ϕ(0)=ϕ(T)=0. Therefore, solution of the implicit-impulsive problem (1.2) is g-H-U stable.

    In this section, we study counter example to verify our results.

    Example 1. Considered the implicit-IFDEs problem

    {CF0D15ru(r)=r225+sin(u(r))+sin(CF0D15ru(r))47+r2,r[0,1],Δu(13)=eu(13)55,u(0)=cos|u|15. (5.1)

    Here ω=15 and CF0D15ru(r)=δu(r), we can set

    g(r,u(r),δu(r))=r225+sin(u(r))+sin(δu(r))47+r2,whereu(r)X,δu(r)R,
    I1(u(13))=eu(13)55,

    and

    f(u)=cos|u|15.

    Clearly f and g are continuous functions. Now for u(r),ˉu(r)X,δu(r),ˉδu(r)R and r[0,1]. Now, we consider

    |g(r,u(r),δu(r))g(r,ˉu(r),ˉδu(r))||sin(u(r))+sin(ˉu(r))|47+r2+|sin(δu(r))+sin(ˉδu(r))|47+r2,147+r2(|u(r)ˉu(r)|+|δu(r)ˉδu(r)|).

    Applying maximum on both side, so we get

    maxr[0,1]|g(r,u(r),δu(r))g(r,ˉu(r),ˉδu(r))|148(uˉu+δˉδ).

    Which satisfy hypothesis H2, we have

    Cg=Cg=148.

    Now next we set for u(r),ˉu(r)X, we have

    |I1(u(13))I1(ˉu(13))|=|eu(13)55eˉu(13)55|155(|u(13)ˉu(13)|)155(uˉuPC).

    Hence, hypothesis H3, is satisfied, so L=155. Next we consider a function f(u)=cos|u|15, for u,ˉuR, we have

    |f(u)f(ˉu)|=|cos|u|15cos|ˉu|15|115|uˉu|.

    Therefore, H4, is satisfied, so Kf=115. Further, we need to verify the condition of the theorems, for this we know that ω=15 and Gω=45,Qω=15, we have the condition of theorem 2 is

    [Kf+LI+(Gω+(n+1)Qω)Cg1Cg]=[115+155+(45+2×15)1481148]=8567755=0.11038<1.

    Therefore, the condition of Theorem 2, is satisfied, hence the mentioned implicit-impulsive problem (5.1) has a unique solution. Further, we need to verify the condition of the theorem 3, we have

    0<(Kf+GωCg1Cg+LI)=7907755<1.

    Also the condition of Theorem 3, holds, so the solution of the said problem (5.1), is at least one solution. In the last, we need to verify the stability results, for this, we verify the condition of the Theorem 4, we have

    Z=02698<1.

    Therefore, condition of the Theorem 4, is satisfied, hence the solution of the problem (5.1), has H-U and g- H-U stable.

    Remark 3. Here we consider the given Example 1 and provide the graphical presentation in Figure 1. We present graphical presentation of solution at different values of fractional order ω=0.45,0.65.0.85 and at the given values of impulsive points r1=14, r2=12, r3=34.

    Figure 1.  Graphical presentation for different fractional order and given impulsive points of Example 1.

    From Figure 1, we see the stability behavior for different fractional order.

    Example 2. Take another implicit-IFDEs problem

    {CF0D17ru(r)=r315+cos(u(r))35+cos(CF0D17ru(r))25+r,r[0,1],Δu(15)=eu(15)35,u(0)=sin(|u|)25. (5.2)

    Here ω=17 and CF0D17ru(r)=δu(r), we can set

    g(r,u(r),δu(r))=r315+cos(u(r))35+cos(CF0D17ru(r))25+r,whereu(r)X,δu(r)R,
    I1(u(15))=eu(15)35,

    and

    f(u)=sin(|u|)25.

    Clearly f and g are continuous functions. For u(r),ˉu(r)X,δu(r),ˉδu(r)R and r[0,1]. Consider,

    |g(r,u(r),δu(r))g(r,ˉu(r),ˉδu(r))||cos(u(r))+cos(ˉu(r))|35+|cos(δu(r))+cos(ˉδu(r))|25+r,135(|u(r)ˉu(r)|)+125+r(|δu(r)ˉδu(r)|).

    Taking maximum on both side, we get

    maxr[0,1]|g(r,u(r),δu(r))g(r,ˉu(r),ˉδu(r))|135(uˉu)+125(δˉδ).

    One can see that the hypothesis H2 is satisfy, we have

    Cg=135andCg=125.

    Next consider for u(r),ˉu(r)X, we have

    |I1(u(15))I1(ˉu(15))|=|eu(15)35eˉu(15)35|135(|u(15)ˉu(15)|)135(uˉu).

    Hence, the hypothesis H3, is satisfied, where LI=135.

    Next we consider a function f(u)=sin(|u|)25, for u,ˉuR, we have

    |f(u)f(ˉu)|=|sin(|u|)25sin(|ˉu|)25|125|uˉu|.

    Here Kf=125, so the hypothesis H3, is satisfied.

    Moreover, we need to verify the sufficient conditions of the theorems. For this we have ω=17 and Gω=67,Qω=17. First we have to verify the condition of the Theorem 2, is

    [Kf+LI+(Gω+(n+1)Qω)Cg1Cg]=[125+135+(67+2×17)1351135]=161525=0.3067<1.

    One can see that condition of the Theorem 2, is satisfied. Therefore, the implicit-impulsive problem (5.2) has a unique solution.

    Further, verify condition of the Theorem 3, we have

    0<(Kf+GωCg1Cg+LI)=73700<1.

    Also holds condition of the Theorem 3, hence solution of the said problem (5.2), is at least one solution. In the last, we need to verify the stability results, for this, we have to verify condition of the Theorem 4, we get

    Z=0792<1.

    Therefore, condition of the Theorem 4, is satisfied, hence the solution of the problem (5.2), has H-U and g-H-U stable.

    Remark 4. Here we consider the given Example 2 and provide the graphical presentation in Figure 2. We present graphical presentation of solution at different values of fractional order ω=0.25,0.45.0.99 and at the given values of impulsive points r1=14, r2=12, r3=34. From Figure 2, we see the stability behavior for different fractional order.

    Figure 2.  Graphical presentation for different fractional order and given impulsive points of Example 2.

    We have in fact obtained some conditions necessary for the solution of existence, uniqueness and stability of the said implicit-impulsive FDEs with involving CFFD. we obtain this conditions using the fixed point theorem as Krasnoselskii's and Banach contraction principle. In this article, we have used Banach's contraction theorem for the uniqueness of solution and Krasnoselskii's fixed point theorem for the existence of the solution for the said problem (1.2). Also we have studied this problem for the stability of H-U and g-H-U stable. All the results have been demonstrated by a proper example. We have also presented the solution through graph by taking different fractional order and impulsive points using RKM methods.

    The authors extend their appreciation to the Deanship of Scientific Research at King Khalid University for funding this work through research groups program under Grant number R.G.P.1/195/42. This research was funded by King Mongkut's University of Technology North Bangkok. Contract no.KMUTNB-62-KNOW-022.

    No conflict of interest exist.



    [1] J. T. Machado, V. Kiryakova, F. Mainardi, Recent history of fractional calculus, Commun. Nonlinear Sci., 16 (2011), 1140–1153.
    [2] R. Metzler, K. Joseph, Boundary value problems for fractional diffusion equations, Phys. A, 278 (2000), 107–125.
    [3] K. B. Oldham, Fractional differential equations in electrochemistry, Adv. Eng. Softw., 41 (2010), 9–12. https://doi.org/10.1016/j.advengsoft.2008.12.012 doi: 10.1016/j.advengsoft.2008.12.012
    [4] F. A. Rihan, Numerical modeling of fractional-order biological systems, Abstr. Appl. Anal., 2013 (2013), 1–11. https://doi.org/10.1155/2013/816803 doi: 10.1155/2013/816803
    [5] J. Sabatier, O. P. Agrawal, J. A. T. Machado, Advances in fractional Calculus, Dordrecht, Springer, 2007.
    [6] V. E. Tarasov, Fractional dynamics: Application of fractional Calculus to dynamics of particles, Fields and Media, Springer, Heidelberg, Higher Education Press, Beijing, 2010.
    [7] M. D. Ortigueira, Fractional Calculus for scientists and engineers: Lecture notes in electrical engineering, 84, Springer, Dordrecht, 2011.
    [8] J. Hristov, Derivatives with non-singular kernels from the Caputo-Fabrizio definition and beyond: Appraising analysis with emphasis on diffusion models, Front. Fract. Calc., 1 (2017), 270–342.
    [9] M. I. Abbas, On the Hamdard and Riemann-Liouville fractional neutral functional integro-differential equations with finite delay, J. Pseudo-Differ. Oper., 10 (2019), 1–10.
    [10] M. I. Abbas, Ulam stability of fractional impulsive differential equations with Riemann-Liouville integral boundary conditions, J. Contemp. Math. Anal., 50 (2015), 209–219. https://doi.org/10.3103/S1068362315050015 doi: 10.3103/S1068362315050015
    [11] A. Atangana, B. S. T. Alkahtani, New model of groundwater flowing within a confine aquifer: application of Caputo-Fabrizio derivative, Arabian J. Geo., 9 (2016), 1–6. https://doi.org/10.1007/s12517-015-2060-8 doi: 10.1007/s12517-015-2060-8
    [12] A. A. Kilbas, M. Saigo, RK. Saxena, Generalized Mittag-Leffler function and generalized fractional calculus operators, Integr. Transf. Spec. F., (2004), 31–49. https://doi.org/10.1080/10652460310001600717
    [13] M. Caputo, M. Fabrizio, A new definition of fractional derivative of without singular kernel, Prog. Fract. Differ. Appl., 1 (2015), 73–85.
    [14] T. Abdeljawad, D. Baleanu, Monotonicity results for fractional difference operators with discrete exponential kernels, Adv. Differ. Equ., 2017 (2017), 1–9. https://doi.org/10.1186/s13662-017-1126-1 doi: 10.1186/s13662-017-1126-1
    [15] R. A. Khan, K. Shah, Existence and uniqueness of solutions to fractional order multi-point boundary value problems, Commun. Appl. Anal., 19 (2015), 515–526.
    [16] D. H. Hyers, On the stability of the linear functional equation, Proc. Natl. Acad. Sci., 27 (1941), 222–224. https://doi.org/10.1073/pnas.27.4.222 doi: 10.1073/pnas.27.4.222
    [17] S. M. Jung, On the Hyers-Ulam stability of the functional equations that have the quadratic property, J. Math. Anal. Appl., 222 (1998), 126–137. https://doi.org/10.1006/jmaa.1998.5916 doi: 10.1006/jmaa.1998.5916
    [18] S. M. Jung, Hyers-Ulam stability of linear differential equations of first order Ⅱ, Appl. Math. Lett., 19 (2006), 854–858. https://doi.org/10.1016/j.aml.2005.11.004 doi: 10.1016/j.aml.2005.11.004
    [19] D. D. Bajnov, P. S. Simeonov, Systems with impulse effect stability, theory and applications. Ellis Horwood Series in mathematics and its applications, Halsted Press, New York, 1989.
    [20] M. Benchohra, J. Henderson, S. Ntouyas, Impulsive diferential equations and inclusions: Contemporary mathematics and its applications, Hindawi Publishing Corporation, New York, 2006. https://doi.org/10.1155/9789775945501
    [21] V. Lakshmikantham, D. D. Bainov, P. S. Simeonov, Theory of impulsive differential equations, World Scientific, Singapore, 1989. https://doi.org/10.1142/0906
    [22] A. Atangana, D. Baleanu, Caputo-Fabrizio derivative applied to groundwater flow within confined aquifer, J. Eng. Mech., 143 (2017), D4016005. https://doi.org/10.1061/(ASCE)EM.1943-7889.0001091 doi: 10.1061/(ASCE)EM.1943-7889.0001091
    [23] T. A. Burton, T. Furumochi, Krasnoselskii's fixed point theorem and stability, Nonlinear Anal.-Theor., 49 (2002), 445–54. https://doi.org/10.1016/S0362-546X(01)00111-0 doi: 10.1016/S0362-546X(01)00111-0
    [24] J. E. Prussing, L. J. Wellnitz, W. G. Heckathorn, Optimal impulsive time-fixed direct-ascent interception, J. Guid. Control Dynam., 12 (1989), 487–494. https://doi.org/10.2514/3.20436 doi: 10.2514/3.20436
    [25] X. Liu, K. Rohlf, Impulsive control of a Lotka-Volterra system, J. Math. Cont. Inf., 15 (1998), 269–284. https://doi.org/10.1093/imamci/15.3.269 doi: 10.1093/imamci/15.3.269
    [26] T. Yang, L. Chua, Impulsive stabilization for control and synchronization of chaotic systems: Theory and application to secure communication, IEEE T. Circuits-I, 44 (1997), 976–988. https://doi.org/10.1109/81.633887 doi: 10.1109/81.633887
    [27] J. Losada, J. J. Nieto, Properties of a new fractional derivative without singular kernel, Prog. Fract. Differ. Appl., 1 (2015), 87–92.
    [28] K. Liu, J. Wang, Y. Zhou, D. O'Regan, Hyers-Ulam stability and existence of solutions for fractional differential equations with Mittag-Leffler kernel, Chaos, Soliton. Fract., 132 (2020), 109534. https://doi.org/10.1016/j.chaos.2019.109534 doi: 10.1016/j.chaos.2019.109534
    [29] J. Sheng, W. Jiang, D. Pang, S. Wang, Controllability of nonlinear fractional dynamical systems with a Mittag-Leffler kernel, Mathematics, 8 (2020), 2139. https://doi.org/10.3390/math8122139 doi: 10.3390/math8122139
    [30] D. Aimene, D. Baleanu, D. Seba, Controllability of semilinear impulsive Atangana-Baleanu fractional differential equations with delay, Chaos, Soliton. Fract., 128 (2019), 51–57. https://doi.org/10.1016/j.chaos.2019.07.027 doi: 10.1016/j.chaos.2019.07.027
    [31] D. Kumar, J. Singh, D. Baleanu, On the analysis of vibration equation involving a fractional derivative with Mittag-Leffler law, Math. Method. Appl. Sci., 43 (2020), 443–457. https://doi.org/10.1002/mma.5903 doi: 10.1002/mma.5903
    [32] A. Atangana, Non validity of index law in fractional calculus: A fractional differential operator with Markovian and non-Markovian properties, Physica A: Stat. Mech. Appl., 505 (2018), 688–706. https://doi.org/10.1016/j.physa.2018.03.056 doi: 10.1016/j.physa.2018.03.056
    [33] A. Atangana, J. F. Gomez-Aguilar, Existence and data dependence theorems for solutions of an ABC-fractional order impulsive system, Chaos Soliton. Fract., 131 (2020), 109477. https://doi.org/10.1016/j.chaos.2019.109477 doi: 10.1016/j.chaos.2019.109477
    [34] Eiman, K. Shah, M. Sarwar, D. Baleanu, Study on Krasnoselskii's fixed point theorem for Caputo-Fabrizio fractional differential equations, Adv. Differ. Equ., 2020 (2020), 1–9. https://doi.org/10.1186/s13662-020-02624-x doi: 10.1186/s13662-020-02624-x
    [35] K. M. Owolabi, A. Shikonogo, Fractal fractional operator method on HER2+ and breast cancer dynamics, Appl. Comput. Math., 7 (2021), 1–19. https://doi.org/10.1007/s40819-021-01030-5 doi: 10.1007/s40819-021-01030-5
    [36] K. M. Owolabi, Analysis and numerical simulation of cross-reaction systems with the Caputo-Fabrizio and Riezs operators, Numer. Meth. Part. D. E., 2021 (2021), 1–23.
    [37] E. J. Moore, S. Sirisubtawee, S. Koonprasert, A Caputo-Fabrizio fractional differential equation model for HIV/AIDS with treatment compartment, Adv. Differ. Equ., 2019 (2019), 200. https://doi.org/10.1186/s13662-019-2138-9 doi: 10.1186/s13662-019-2138-9
    [38] D. Baleanu, S. S. Sajjadi, A. Jajarmi, Z. Defterli, On a nonlinear dynomical system with both chaotic and nonchaotic behaviors: A new fractional analysis and control, Adv. Differ. Equ., 2021 (2021), 234. https://doi.org/10.1186/s13662-021-03393-x doi: 10.1186/s13662-021-03393-x
    [39] D. Baleanu, S. S. Sajjadi, J. H. Asad, A. Jajarmi, E. Estiri, Hyperchaotic behaviors, optimal control and synchronization of a nonautonomous cardiac conduction System, Adv. Differ. Equ., 2021 (2021), 175. https://doi.org/10.1186/s13662-021-03320-0 doi: 10.1186/s13662-021-03320-0
    [40] D. Baleanu, S. Zibaei, M. Namjoo, A. Jajarmi, A nonstandard finite difference scheme for the modeling and nonidentical synchronization of a noval fractional chaotic system, Adv. Differ. Equ., 2021 (2021), 308. https://doi.org/10.1186/s13662-021-03454-1 doi: 10.1186/s13662-021-03454-1
    [41] M. M. Meerschaert, A. B. David, H. P. Scheffler, B. Baeumer, Stochastic solution of space-time fractional diffusion equations, Phys. Rev. E, 65 (2002), 041103. https://doi.org/10.1103/PhysRevE.65.041103 doi: 10.1103/PhysRevE.65.041103
    [42] R. Schumer, A. B. David, M. M. Meerschaert, B. Baeumer, Fractal mobile/immobile solute transport, Water Resour. Res., 39 (2003), 1296.
    [43] X. Zheng, H. Wang, H. Fu, Well-posedness of fractional differential equations with variable-order Caputo-Fabrizio derivative, Chaos Soliton. Fract., 138 (2020), 109966. https://doi.org/10.1016/j.chaos.2020.109966 doi: 10.1016/j.chaos.2020.109966
  • This article has been cited by:

    1. Gemeda Tolessa Lubo, Gemechis File Duressa, Lishan Liu, Redefined cubic B-spine finite element method for the generalized diffusion equation with delay, 2022, 9, 2768-4830, 10.1080/27684830.2022.2095092
    2. Shorog Aljoudi, Existence and uniqueness results for coupled system of fractional differential equations with exponential kernel derivatives, 2022, 8, 2473-6988, 590, 10.3934/math.2023027
    3. Meng Liu, Liangzhou Chen, Xiao-Bao Shu, The existence of positive solutions for φ-Hilfer fractional differential equation with random impulses and boundary value conditions, 2023, 1745-5030, 1, 10.1080/17455030.2023.2176695
    4. Mohammad Alshammari, Naveed Iqbal, Wael W. Mohammed, Thongchai Botmart, The solution of fractional-order system of KdV equations with exponential-decay kernel, 2022, 38, 22113797, 105615, 10.1016/j.rinp.2022.105615
    5. Meiling Song, Zhiguo Luo, Ibrahim Mahariq, Ulam–Hyers Stability for a Class of Hilfer-Type Fractional Stochastic Differential Equations, 2022, 2022, 1563-5147, 1, 10.1155/2022/9844295
    6. Osama Moaaz, Ahmed E. Abouelregal, Multi-fractional-differential operators for a thermo-elastic magnetic response in an unbounded solid with a spherical hole via the DPL model, 2022, 8, 2473-6988, 5588, 10.3934/math.2023282
    7. Ahmed E. Abouelregal, Taher A. Nofal, Fahad Alsharari, A thermodynamic two-temperature model with distinct fractional derivative operators for an infinite body with a cylindrical cavity and varying properties, 2022, 24680133, 10.1016/j.joes.2022.05.001
    8. Noufe H. Aljahdaly, Ali Akgül, Rasool Shah, Ibrahim Mahariq, Jeevan Kafle, A. Ghareeb, A Comparative Analysis of the Fractional-Order Coupled Korteweg–De Vries Equations with the Mittag–Leffler Law, 2022, 2022, 2314-4785, 1, 10.1155/2022/8876149
    9. Mesfin Mekuria Woldaregay, Lishan Liu, Solving singularly perturbed delay differential equations via fitted mesh and exact difference method, 2022, 9, 2768-4830, 10.1080/27684830.2022.2109301
    10. Ahmed E. Abouelregal, A comparative study of a thermoelastic problem for an infinite rigid cylinder with thermal properties using a new heat conduction model including fractional operators without non-singular kernels, 2022, 92, 0939-1533, 3141, 10.1007/s00419-022-02228-9
    11. Reham R. Mostafa, Fatma A. Hashim, Noha E. El-Attar, Ahmed M. Khedr, Empowering African vultures optimizer using Archimedes optimization algorithm for maximum efficiency for global optimization and feature selection, 2024, 15, 1868-6478, 1701, 10.1007/s12530-024-09585-6
    12. Linjun Wang, Aiqing She, Youxiang Xie, The dynamics analysis of Gompertz virus disease model under impulsive control, 2023, 13, 2045-2322, 10.1038/s41598-023-37205-x
    13. Panjaiyan Karthikeyann, Sadhasivam Poornima, Kulandhaivel Karthikeyan, Chanon Promsakon, Thanin Sitthiwirattham, Chang Phang, On Implicit Atangana–Baleanu–Caputo Fractional Integro-Differential Equations with Delay and Impulses, 2024, 2024, 2314-4785, 1, 10.1155/2024/5531984
    14. Velusamy Kavitha, Ravi Deepa , Balakrishnan Ganesh Priya , Seenith Sivasundaram , Mani Mallika Arjunan , EXISTENCE, STABILITY AND NUMERICAL ANALYSIS OF A FRACTIONAL NEUTRAL IMPLICIT DELAY DIFFERENTIAL SYSTEM WITH AN EXPONENTIAL KERNEL, 2024, 16, 20665997, 182, 10.56082/annalsarscimath.2024.2.182
    15. Noorah Mshary, Hamdy M. Ahmed, Ahmed S. Ghanem, Existence and controllability of nonlinear evolution equation involving Hilfer fractional derivative with noise and impulsive effect via Rosenblatt process and Poisson jumps, 2024, 9, 2473-6988, 9746, 10.3934/math.2024477
    16. Stanislaus Jasmin Swetha, Velusamy Kavitha , Mani Mallika Arjunan , Dumitru Baleanu , ON THE INITIAL VALUE PROBLEMS FOR NEUTRAL INTEGRO-DIFFERENTIAL SYSTEM WITHIN EXPONENTIAL KERNEL, 2024, 16, 20665997, 5, 10.56082/annalsarscimath.2024.1.5
    17. Yong Zhang, Xiaoting Liu, Dawei Lei, Maosheng Yin, HongGuang Sun, Zhilin Guo, Hongbin Zhan, Modeling Hydrologically Mediated Hot Moments of Transient Anomalous Diffusion in Aquifers Using an Impulsive Fractional‐Derivative Equation, 2024, 60, 0043-1397, 10.1029/2023WR036089
    18. Shiferaw Geremew Kebede, Assia Guezane Lakoud, Haider Ebrahim Yesuf, Solution analysis for non-linear fractional differential equations, 2024, 10, 2297-4687, 10.3389/fams.2024.1499179
  • Reader Comments
  • © 2022 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(2697) PDF downloads(124) Cited by(18)

Figures and Tables

Figures(2)

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog