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Research article Special Issues

Optimal harvesting strategy of a stochastic n-species marine food chain model driven by Lévy noises


  • Received: 24 May 2023 Revised: 30 June 2023 Accepted: 09 July 2023 Published: 19 July 2023
  • A stochastic n-species marine food chain model with harvesting and Lévy noises is proposed. First, the criterion on the asymptotic stability in distribution is established. Second, the criterion on the existence of optimal harvesting strategy (OHS) and the maximum of expectation of sustainable yield (MESY) are derived. Furthermore, the numerical simulations are presented to verify the theoretical results. Our results show that (i) noises intensity can easily affect the dynamics of marine populations, leading to the imbalances of marine ecology, (ii) the establishment of an optimal harvesting strategy should fully consider the impact of noises intensity for better managing and protecting marine resources.

    Citation: Nafeisha Tuerxun, Zhidong Teng. Optimal harvesting strategy of a stochastic n-species marine food chain model driven by Lévy noises[J]. Electronic Research Archive, 2023, 31(9): 5207-5225. doi: 10.3934/era.2023265

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  • A stochastic n-species marine food chain model with harvesting and Lévy noises is proposed. First, the criterion on the asymptotic stability in distribution is established. Second, the criterion on the existence of optimal harvesting strategy (OHS) and the maximum of expectation of sustainable yield (MESY) are derived. Furthermore, the numerical simulations are presented to verify the theoretical results. Our results show that (i) noises intensity can easily affect the dynamics of marine populations, leading to the imbalances of marine ecology, (ii) the establishment of an optimal harvesting strategy should fully consider the impact of noises intensity for better managing and protecting marine resources.



    The concepts of fractional calculus have gained widespread recognition as an important area within pure mathematics. The concepts within fractional calculus have been studied by numerous mathematicians, given their significance across various fields of knowledge, see [1,2,3,4]. Theoretical aspects of fractional differential equations have attracted considerable interest since the advent of fractional calculus. Owing to the nonlocal nature of fractional-order differential equations, researchers possess the flexibility to choose and apply the most suitable operator, thereby accurately representing complex real-world phenomena. However, there are numerous versions of integrals and derivatives of arbitrary fractional order, employing various types of operators, as detailed in[5,6,7,8,9,10,11].

    Fixed-point theorems serve as valuable tools for establishing both the existence and uniqueness of solutions to fractional differential equations. The methodology has been extensively studied by numerous mathematicians, and vast results have been published, see [12,13,14,15,16,17,18] and references therein. Furthermore, in the physical and life sciences, fractional calculus has widespread applicability across various domains, including image processing, complex systems, traffic flow, etc. Numerous researchers have studied many different kinds of initial and boundary value problems with various types of fractional operators, using techniques based on fixed-point theorems, [19,20,21,22,23,24,25,26].

    The concept of sequential fractional derivatives was first introduced in [27]. Since its inception, numerous researchers have made significant contributions to the advancement of this field. As a result, several research articles have been published. For more research insight, we refer to [28,29,30,31,32,33,34].

    Wang et al. [35], studied the turbulent flow model within the framework of the Caputo-Hadamard fractional derivatives of the form:

    {CHDτ1ψp(s)(CHDτ2u(s))+g(u(s),Iα1,α2u(s))=0,s[1,λ],u(1)=αu(λ),u(1)=u(1)=0,CHDτ2u(1)=0,2<τ2<3,0<τ1<1,α1,α2>0,λ2<α2λ4λ. (1.1)

    In [36], the authors discussed the existence and uniqueness of positive solutions for a class of Caputo fractional differential equations described by:

    {CDα1ψp(s)(CDα2u(s))+g(s,u(s))=0,s[0,1],u(0)=k,u(1)=mn=1φnRLIδnu(βn),mN,φn0,k>0,0<β1<β2<<βm<1,0<α1,α2<1,ψp(s)>2,δn>0. (1.2)

    In 2018, Tariboon et al. [37] considered the sequential Caputo and Hadamard fractional nonseparated boundary value problem given by:

    {CDα1(HDα2u)(s)=g(s,u(s)),s(a,b),0<α1,α2<1,c1u(a)+c2(HDα2u)(b)=0,c3u(a)+c4(HDα2u)(b)=0,andHDα2(CDα1u)(s)=g(s,u(s)),s(a,b),c1u(a)+c2(CDα1u)(b)=0,c3u(a)+c4(CDα1u)(b)=0,c1,c2,c3,c4R. (1.3)

    The investigation employed Banach and Krasnoselskii's fixed-point theorems, alongside Leray-Schauder's nonlinear alternative, to establish the existence and uniqueness of the results.

    Asawasamrit et al. [38] studied the nonlocal boundary value problem involving the Hilfer fractional derivative of the form:

    {HDα1,α2u(s)=g(s,u(s)),s[a,b],1<α1<2,0α21,u(a)=0,u(b)=ki=1ciIα3u(ϑi),ciR,α30,ϑi[a,b]. (1.4)

    Jackson [39,40] initiated the idea of q-difference calculus. For more basic concepts of q-difference calculus, see [41,42]. Since then, numerous researchers have delved into the theoretical analysis of q-fractional-order differential equations, see [43,44,45,46,47,48].

    Allouch et al. [49] studied the q-difference equation with nonlinear integral boundary conditions of the form:

    {Dζqu(κ)=g(κ,u(κ)),κ[0,b],1<ζ<2,0<q<1,b>0,u(0)u(0)=b0g(ϑ,u(ϑ))dϑ,u(A)+u(b)=b0h(ϑ,u(ϑ))dϑ. (1.5)

    Measures of noncompactness and Mönch's fixed point theorems were utilized to derive the results.

    Inspired by recent publications, we propose a new type of separated boundary value problems and investigate its theoretical analysis. The problem under consideration takes the form of

    {HDα,βq(CDδqz)(t)=f(t,z(t)),t[0,T],z(0)+λ1CDγ+δ1qz(0)=0,z(T)+λ2CDγ+δ1qz(T)=0,0<α,δ,q<1,0β1,λ1,λ2R,T>0, (1.6)

    where CDδq() and HDα,βq(), respectively, are the Caputo and Hilfer fractional derivatives of orders δ,α, and type β such that γ=α+β(1α) with γ+δ>1, and f:[0,T]×RR is a continuous function.

    The existence and uniqueness of solutions to q sequential fractional-order boundary value problems have not been extensively studied. In our study, we introduce a new class of sequential q-Hilfer and q-Caputo fractional differential equations with separated boundary conditions and provide a comprehensive theoretical analysis.

    The novelty of our study lies in the fact that we consider a sequential fractional boundary value problem combining q-Hilfer and q-Caputo fractional derivative operators subjected to non-separated boundary conditions. To the best of our knowledge, this is the first paper to appear in the literature. The method used is standard, but its configuration in the Hilfer-Caputo sequential boundary value problem (1.6) is new. The results are new and significantly enrich the existing results in the literature on Hilfer boundary value problems.

    The rest of the paper is organized as follows: Section 2 revisits essential definitions, lemmas, and theorems. Section 3 focuses on establishing an integral equivalent form of the proposed problem, which enables us to prove the existence and uniqueness of results. In Section 4, two examples are presented. Section 5 provides the conclusion of the paper.

    The section includes prerequisite facts, definitions, and key lemmas that will assists in proving the main results. The space X=C([0,T],R) constitutes a Banach space comprising all continuous functions over [0,T] with

    z=supt[0,T]|z(t)|.

    Recall that for q(0,1) and g,hR, the following properties holds [42]:

    [g]q=qg1q1,

    and

    (gh)(0)q=1,(gh)(k)q=k1n=0(ghqn);kN.

    Moreover, for αR, we have

    (gh)(α)q=gαn=0(1(hg)qn1(hg)qn+α).

    The q analog gamma function is given by

    Γq(α)=(1q)(α1)q(1q)α1;αR{0,1,2,},

    such that Γq(α+1)=[α]qΓq(α).

    For u:[0,T]R and 0<q<1, the q-derivative of u is defined by

    Dqu(t)=u(t)u(qt)(1q)t;t0,Dqu(0)=limt0Dqu(t).

    Moreover, the higher-order q-derivative shows

    D0qu(t)=u(t),Dnqu(t)=Dq(Dn1qu)(t),nN.

    For setting Jt={tqn:nN,t0}{0}, the analog q-integral of a function u:JtR is of the form:

    Iqu(t)=t0u(ν)dqν=n=0t(1q)qnu(tqn),

    provided that the right-hand side converges. Note that Dq(Iqu)(t)=u(t), and if u is continuous at 0, then

    Iq(Dqu)(t)=u(t)u(0).

    Definition 2.1. [45] Let w:[0,T]R,ϑ[0,T], and α>0. The integral operator

    Iαqw(ϑ)=1Γq(α)ϑ0(ϑqν)(α1)qw(ν)dqν,

    is called the q-fractional-order integral in the Riemann-Liouville sense of order α>0 for the function w, and I0qw(ϑ)=w(ϑ).

    Lemma 2.1. [45] For 0α< and σ(1,+). If w(ϑ)=(ϑa)(σ), then

    Iαqw(ϑ)=Γq(σ+1)Γq(α+σ+1)(ϑa)(α+σ)q;0<a<ϑ<T,

    also

    (Iαq1)(ϑ)=1Γq(α+1)(ϑa)(α)q.

    Definition 2.2. [50] Let w:[0,T]R,ϑ[0,T],0<α<1. The derivative operator

    RLDαqw(ϑ)=1Γq(1α)Dqϑ0(ϑqν)(α)qw(ν)dqν,

    is called the q-fractional-order derivative in Riemann-Liouville sense of order α for the function w.

    Definition 2.3. [50] Let wC1q([0,T],R),ϑ[0,T],0<α<1. The derivative operator

    CDαqw(ϑ)=1Γq(1α)ϑ0(ϑqν)(α)qDqw(ν)dqν, (2.1)

    is called the q-fractional-order derivative in the Caputo sense of order α.

    Lemma 2.2. [50] Let w:[0,T]R and α,σ0. Thus

    (i).Iαq(Iσqw)(t)=Iα+σqw(t),(ii).CDαq(Iαqw)(t)=w(t).

    Definition 2.4. [51] Let wC1q([0,T]R) and 0<α<1,0β1. The operator

    HDα,βqw(ϑ)=Iβ(1α)q[Dq(I(1β)(1α)qw)](ϑ), (2.2)

    is called q-Hilfer fractional derivative of order α with a parameter β. Note that HDα,βq can be written as

    HDα,βqw=Iβ(1α)qDq(I(1β)(1α)qw)=Iβ(1α)qDq(I1γqw),γ=α+β(1α).

    Lemma 2.3. [50] Suppose that 0<α<1. Then we have

    Iαq(RLDαqw)(ϑ)=w(ϑ)1Γq(α)ϑα1(I1αqw)(0),

    and moreover,

    Iαq(CDαqw)(ϑ)=w(ϑ)+k,kR.

    Remark 2.1. Note that if β=0, from problem (1.6), we have

    {RLDαq(CDδqz)(t)=f(t,z(t)),t[0,T],z(0)+λ1CDα+δ1qz(0)=0,z(T)+λ2CDα+δ1qz(T)=0,

    and if β=1, we have

    {CDαq(CDδqz)(t)=f(t,z(t)),t[0,T],z(0)+λ1CDδqz(0)=0,z(T)+λ2CDδqz(T)=0,

    which are the q sequential Riemann-Liouville and Caputo derivatives with separated boundary conditions.

    In this part, we begin by employing techniques from Lemma 2.3 to establish an integral equation associated with problem (1.6). To this end, we introduce the lemma, addressing a linear variant of problem (1.6), which serves as the fundamental tool for transforming the problem into a fixed-point problem.

    Lemma 3.1. Let 0<α,δ<1, 0β1, γ=α+β(1α), λ1,λ2R and 0<q<1 and

    Q=T(γ+δ1)+(λ2λ1)Γq(γ+δ)0.

    Suppose gC([0,T],R). If zC2q([0,T],R), then, the linear problem

    {HDα,βq(CDδqz)(t)=g(t),t[0,T],z(0)+λ1CDγ+δ1qz(0)=0,z(T)+λ2CDγ+δ1qz(T)=0, (3.1)

    is equivalent to the integral equation:

    z(t)=λ1Γq(γ+δ)t(γ+δ1)Q[1Γq(α+δ)T0(Tqν)(α+δ1)qg(ν)dqν+λ2Γq(αγ+1)T0(Tqν)(αγ)qg(ν)dqν]+1Γq(α+δ)t0(tqν)(α+δ1)qg(ν)dqν,t[0,T]. (3.2)

    Proof. Suppose zC2q([0,T],R) satisfies problem (3.1), then, we show that z is satisfies the integral (3.2). Since

    HDα,βq()=Iβ(1α)qDqIq(1β)(1α)()=Iβ(1α)qDqI1γq(), (3.3)

    then, make use of Eq (3.3), the first equation of (3.1) can be simplified as

    Iβ(1α)qDqI1γq(CDδqz)(t)=g(t). (3.4)

    Taking Iαq to both sides of Eq (3.4) and utilize the techniques in Lemma 2.3, yields

    CDδqz(t)=AΓq(γ)t(γ1)+1Γq(α)t0(tqν)(α1)qg(ν)dqν,AR,(A constant). (3.5)

    Also, taking Iδq to both sides of Eq (3.5) and utilize the techniques in Lemma 2.3, we get

    z(t)=B+AΓq(γ+δ)t(γ+δ1)+1Γq(α+δ)t0(tqν)(α+δ1)qg(ν)dqν, (3.6)

    where BR is an arbitrary constant. Applying the operator CDγ+δ1q to both sides of Eq (3.6), yields

    CDγ+δ1qz(t)=A+1Γq(αγ+1)t0(tqν)(αγ)qg(ν)dqν. (3.7)

    Thus, from the condition z(0)+λ1CDγ+δ1qz(0)=0, Eqs (3.6) and (3.7), we get

    z(0)+λ1CDγ+δ1qz(0)=λ1A+B=0B=λ1A. (3.8)

    From z(T)+λ2CDγ+δ1qz(T)=0, Eqs (3.6) and (3.7), we obtain

    0=B+λ2A+AΓq(γ+δ)T(γ+δ1)+λ2Γq(αγ+1)T0(Tqν)(αγ)qg(ν)dqν+1Γq(α+δ)T0(Tqν)(α+δ1)qg(ν)dqν. (3.9)

    Upon simplification and substituting B=λ1A in Eq (3.9), we get

    B=λ1Γq(γ+δ)Q[1Γq(α+δ)T0(Tqν)(α+δ1)qg(ν)dqν+λ2Γq(αγ+1)T0(Tqν)(αγ)qg(ν)dqν],

    and

    A=Γq(γ+δ)Q[1Γq(α+δ)T0(Tqν)(α+δ1)qg(ν)dqν+λ2Γq(αγ+1)T0(Tqν)(αγ)qg(ν)dqν].

    To explore the numerical behavior of the integral solution of the proposed problem (1.6), we vary the fractional-orders associated with the problem. The following parameters, α,β, and δ, respectively, were considered. The respective graphical analysis are shown in Figures 1 and 2, respectively. Figures 1a1c illustrate the behavior of the solution of the integral (3.2) when varying the fraction-order α. Moreover, the corresponding 3D plots is displayed in Figures 2a2c, respectively.

    Figure 1.  Solution of the integral Eq (3.2) for values of α,β and δ for the function g(t)=t2+2t+1 and t[0,1].
    Figure 2.  3D plots for the solution of (3.2) for the function g(t)=t2+2t+1 and t[0,1].

    By employing Krasnoselskii's fixed-point theorem and Leray-Schauder's nonlinear alternative, in this subsection, we will present the proof of the existence results of (1.6).

    Lemma 3.2. (Krasnoselskii's fixed point theorem) [52] Let MX be closed, bounded, convex, and nonempty. Suppose F1,F2 be operators such that:

    (i) F1z+F2z1M whenever z,z1M;

    (ii) F2 is a contraction mapping;

    (iii) F1 is compact and continuous.

    Then there exists wM such that w=F1w+F2w.

    Theorem 3.1. Let 0<α,δ<1, 0β1, and γ=α+β(1α). Suppose that the function f:[0,T]×RR is continuous and satisfies:

    (H1) There exists L>0,(constant) such that

    |f(t,z)f(t,z1)|L|zz1|,fort[0,T],andz,z1R.

    (H2) |f(t,z)|Ψ(t),(t,z)[0,T]×R and ΨC([0,T],R+);

    Then there exists at least one solution of the quantum Hilfer and Caputo separated boundary value problem (1.6) on [0,T], provided that

    L(ΔT(α+δ)Γq(α+δ+1))<1, (3.10)

    where

    Δ=|λ1|Γq(γ+δ)+T(γ+δ1)|Q|[T(α+δ)Γq(α+δ+1)+|λ2|T(αγ+1)Γq(αγ+2)]+T(α+δ)Γq(α+δ+1). (3.11)

    Proof. Now, from equation 3.2, define F:XX by

    (Fz)(t)=λ1Γq(γ+δ)t(γ+δ1)Q[1Γq(α+δ)T0(Tqν)(α+δ1)qf(ν,z(ν))dqν+λ2Γq(αγ+1)T0(Tqν)(αγ)qf(ν,z(ν))dqν]+1Γq(α+δ)t0(tqν)(α+δ1)qf(ν,z(ν))dqν,t[0,T].

    Suppose supt[0,T]Ψ(t)=Ψ and σΨΔ such that Bσ={xX:zσ}. Now, we set

    F1z(t)=1Γq(α+δ)t0(tqν)(α+δ1)qf(ν,z(ν))dqν,t[0,T],

    and

    F2z(t)=λ1Γq(γ+δ)t(γ+δ1)Q[1Γq(α+δ)T0(Tqν)(α+δ1)qf(ν,z(ν))dqν+λ2Γq(αγ+1)T0(Tqν)(αγ)qf(ν,z(ν))dqν],t[0,T].

    Then, for any z,z1Bσ, we get

    |(F1z)(t)+(F2z1)(t)|supt[0,T]{1Γq(α+δ)t0(tqν)(α+δ1)qf(ν,z(ν))dqν+λ1Γq(γ+δ)tγ+δ1Q[1Γq(α+δ)T0(Tqν)(α+δ1)qf(ν,z1(ν))dqν+λ2Γq(αγ+1)T0(Tqν)(αγ)qf(ν,z1(ν))dqν]}Ψ(T(α+δ)Γq(α+δ+1)+|λ1|Γq(γ+δ)+T(γ+δ1)|Q|(T(α+δ)Γq(α+δ+1)+|λ2|T(αγ+1)Γq(αγ+2)))ΨΔσ.

    Hence F1z+F2z1σ, which shows that F1z+F2z1Bσ. Therefore, the condition (i) of Lemma 3.2 is satisfied.

    To show condition (ii) of Lemma 3.2, we proceed as follows, for any z,z1C([0,T],R), gives

    |(F2z)(t)(F2z1)(t)||λ1|Γq(γ+δ)+t(γ+δ1)|Q|[1Γq(α+δ)T0(Tqν)(α+δ1)q|f(ν,z(ν))dqνf(ν,z1(ν))dqν|+|λ2|Γq(αγ+1)T0(Tqν)(αγ)q|f(ν,z(ν))dqνf(ν,z1(ν))dqν|ν]L(|λ1|Γq(γ+δ)+T(γ+δ1)|Q|(T(α+δ)Γq(α+δ+1)+|λ2|T(αγ+1)Γq(αγ+2)))zz1=L(ΔT(α+δ)Γq(α+δ+1))zz1.

    Consequently, (F2z)(F2z1)L(ΔT(α+δ)Γq(α+δ+1))zz1, and hence, by (3.10), F2 is a contraction. Hence, condition (ii) of Lemma 3.2 is satisfied.

    Moreover, since fC([0,T],R), the operator F1 is continuous and it is uniformly bounded, as

    F1zT(α+δ)Γq(α+δ+1)Ψ.

    Set sup(t,z)[0,T]×Bσ|f(t,z)|=ˆf. Then

    |(F1z)(t2)(F1z)(t1)|=1Γq(α+δ)|t10[(t2qν)(α+δ1)q(t1qν)(α+δ1)]f(ν,z(ν))dqν+t2t1(t2qν)(α+δ1)qf(ν,z(ν))dqν|ˆfΓq(α+δ+1)[2(t2t1)(α+δ)q+|t(α+δ)2t(α+δ)1|],

    0. as t2t10, independently of z. Hence, as a consequence of the Arzelá-Ascoli theorem, this shows that F1 is compact on Bσ.

    Therefore, since all the assumptions of Lemma 3.2 are satisfied, we conclude that there exists at least one solution of quantum Hilfer and Caputo separated boundary value problem (1.6) on [0,T].

    The next existence result relies on Leray-Schauder's nonlinear alternative.

    Lemma 3.3. (Leray-Schauder's Nonlinear Alternative) [53] Let CX be closed and convex of X, UC be open, and 0U. Suppose F:ˉUC is a continuous and compact map. Then either

    (i) F has a fixed point in ˉU or

    (ii) zU and ω(0,1) with z=ωF(z).

    Theorem 3.2. Suppose that the function f:[0,T]×RR is continuous and satisfies:

    (H3) there exists a function Λ:[0,)(0,) continuous and nondecreasing and a function GC([0,T],R+) such that

    |f(t,z)|G(t)Λ(z)for each(t,z)[0,T]×R;

    (H4) There exists C>0(constant) such that

    1<CΛ(C)GΔ.

    Then, there exists at least one solution of problem (1.6) on [0,T].

    Proof. Firstly, we show that F maps a bounded set into bounded sets in X. For any k>0, let Bk={zX:zk} be a bounded set in X. Then, for t[0,T] yields

    |(Fz)(t)|supt[0,T]{1Γq(α+δ)t0(tqν)(α+δ1)qf(ν,z(ν))dqν+λ1Γq(γ+δ)tγ+δ1Q[1Γq(α+δ)T0(Tqν)(α+δ1)qf(ν,z(ν))dqν+λ2Γq(αγ+1)T0(Tqν)(αγ)qf(ν,z(ν))dqν]}Λ(z)G{T(α+δ)Γq(α+δ+1)+|λ1|Γq(γ+δ)+T(γ+δ1)|Q|(T(α+δ)Γq(α+δ+1)+|λ2|T(αγ+1)Γq(αγ+2))}Λ(z)GΔ, (3.12)

    which implies that

    FzΛ(z)GΔ.

    Moreover, for t1,t2[0,T] with t1<t2 and zBk, we obtain

    |(Fz)(t2)(Fz)(t1)||tγ+δ12tγ+δ11||Q|[1Γq(α+δ)T0(Tqν)(α+δ1)q|f(ν,z(ν))|dqν+|λ2|Γq(αγ+1)T0(Tqν)(αγ)q|f(ν,z(ν))|dqν]+1Γq(α+δ)|t10[(t2qν)(α+δ1)q(t1qν)(α+δ1)]|f(ν,z(ν))|dqν+t2t1(t2qν)(α+δ1)q|f(ν,z(ν))|dqν||tγ+δ12tγ+δ11||Q|Λ(k)[1Γq(α+δ)T0(Tqν)(α+δ1)qg(ν)dqν+|λ2|Γq(αγ+1)T0(Tqν)(αγ)qg(ν)dqν]+1Γq(α+δ)Λ(k)|t10[(t2qν)(α+δ1)q(t1qν)(α+δ1)]g(ν)dqν+t2t1(t2qν)(α+δ1)qg(ν)dqν|GΛ(k)|tγ+δ12tγ+δ11||Q|{T(α+δ)Γq(α+δ+1)+|λ2|T(αγ+1)Γq(αγ+2)}+GΛ(k)Γq(α+δ+1)[2(t2t1)(α+δ)q+|t(α+δ)2t(α+δ)1|],0ast2t10.

    This proves the equicontinuity of the set F(Bk), and by the Arzelá-Ascoli theorem, it is relatively compact. Thus, F:XX is completely continuous.

    Now, for t[0,T], as in step 1, yields

    |z(t)|GΛ(z)Δ,

    which gives

    zGΛ(z)Δ1.

    By (H4) C such that Cz. Let

    U={zX:z<C}.

    Then, F:ˉUC is both continuous and completely continuous. From U, there exists no zˉU such that z=ωF(z) for any ω(0,1). Thus, as a consequence of Lemma 3.3, we conclude that F has a fixed point zˉU which is a solution of problem (1.6).

    We proceed to establish the uniqueness of problem (1.6) using the Banach contraction principle [54].

    Theorem 3.3. Let 0<α,δ<1, 0β1, and γ=α+β(1α). Suppose that f:[0,T]×RR fulfills the assumption (H1). If

    LΔ<1, (3.13)

    where Δ is defined by (3.11), then, there exists a unique solution of problem (1.6) on [0,T].

    Proof. To do so, problem (1.6) can be viewed as a fixed-point problem, z=Fz, where F is defined as in (3.1). Next, we show that F has a unique fixed point. Indeed, let supt[0,T]|f(t,0)|=K< and KΔ1LΔk. First, we show that FBkBk, where Bk={zX:zk}. Given zBk, gives

    |(Fz)(t)|supt[0,T]{1Γq(α+δ)t0(tqν)(α+δ1)q|f(ν,z(ν))|dqν+λ1Γq(γ+δ)t(γ+δ1)Q[1Γq(α+δ)T0(Tqν)(α+δ1)q|f(ν,z(ν))|dqν+λ2Γq(αγ+1)T0(Tqν)(αγ)q|f(ν,z(ν))|dqν]}1Γq(α+δ)T0(Tqν)(α+δ1)q(|f(ν,z(ν))f(ν,0)|+|f(ν,0)|)dqν+|λ1|Γq(γ+δ)+T(γ+δ1)|Q|×[1Γq(α+δ)T0(Tqν)(α+δ1)q(|f(ν,z(ν))f(ν,0)|+|f(ν,0)|)f(ν,z(ν))dqν+|λ2|Γq(αγ+1)T0(Tqν)(αγ)q(|f(ν,z(ν))f(ν,0)|+|f(ν,0)|)dqν](Lz+K){1Γq(α+δ)T0(Tqν)(α+δ1)qdqν+|λ1|Γq(γ+δ)+T(γ+δ1)|Q|[1Γq(α+δ)T0(Tqν)(α+δ1)qdqν+|λ2|Γq(αγ+1)T0(Tqν)(αγ)qdqν]},(Lz+K){T(α+δ)Γq(α+δ+1)+|λ1|Γq(γ+δ)+T(γ+δ1)|Q|(T(α+δ)Γq(α+δ+1)+|λ2|T(αγ+1)Γq(αγ+2))}(Lk+K)Δk,

    and hence (Fz)k, which means that FBkBk.

    Subsequently, for t[0,T] and any z,z1C([0,T],R), we get

    |(Fz)(t)(Fz1)(t)|1Γq(α+δ)t0(tqν)(α+δ1)q|f(ν,z(ν))f(ν,z1(ν))|dqν+|λ1|Γq(γ+δ)+t(γ+δ1)|Q|[1Γq(α+δ)T0(Tqν)(α+δ1)q|f(ν,z(ν))f(ν,z1(ν))|dqν+|λ2|Γq(αγ+1)T0(Tqν)(αγ)q|f(ν,z(ν))f(ν,z1(ν))|dqν]Lzz1(|λ1|Γq(γ+δ)+T(γ+δ1)|Q|[T(α+δ)Γq(α+δ+1)+|λ2|T(αγ+1)Γq(αγ+2)]+T(α+δ)Γq(α+δ+1))=LΔzz1.

    Therefore, (Fz)(Fz1)LΔzz1, and hence, by (3.13), F is a contraction, and hence, problem (1.6) has a unique solution on [0,T].

    Case Ⅰ. If λ1=λ2=0, problem (1.6) reduces to sequential q-Hilfer problems of the form:

    {HDα,βq(CDδqz)(t)=f(t,z(t)),t[0,T],z(0)=0,z(T)=0. (3.14)

    Corollary 3.1. Let 0<α,δ<1, 0β1, and γ=α+β(1α). Suppose f:[0,T]×RR is a continuous function. If zC2q([0,T],R), then z satisfies the problem (3.14) if and only if z satisfies the integral equation:

    z(t)=1Γq(α+δ)t0(tqν)(α+δ1)qf(ν,z(ν))dqνt(γ+δ1)T(γ+δ1)1Γq(α+δ)T0(Tqν)(α+δ1)qf(ν,z(ν))dqν. (3.15)

    Case Ⅱ. If λ1=λ2=1, problem (1.6) reduces to sequential q-Hilfer problems of the form:

    {HDα,βq(CDδqz)(t)=f(t,z(t)),t[0,T],z(0)+CDγ+δ1qz(0)=0,z(T)+CDγ+δ1qz(T)=0. (3.16)

    Corollary 3.2. Let 0<α,δ<1, 0β1, and γ=α+β(1α). Suppose f:[0,T]×RR is a continuous function. If zC2q([0,T],R), then z satisfies the problem (3.16) if and only if z satisfies the integral equation:

    z(t)=Γq(γ+δ)t(γ+δ1)T(γ+δ1)[1Γq(α+δ)T0(Tqν)(α+δ1)qf(ν,z(ν))dqν+1Γq(αγ+1)T0(Tqν)(αγ)qf(ν,z(ν))dqν]+1Γq(α+δ)t0(tqν)(α+δ1)qf(ν,z(ν))dqν. (3.17)

    Case Ⅲ. Let β=1, then γ=1, and problem (1.6) reduces to the sequential q-Caputo fractional-order differential equation given by

    {CDαq(CDδqz)(t)=f(t,z(t)),t[0,T],z(0)+λ1CDδqz(0)=0,z(T)+λ2CDδqz(T)=0. (3.18)

    Corollary 3.3. Let 0<α,δ<1 be orders of fractional derivative and 0<q<1 be quantum number. Suppose f:[0,T]×RR is a continuous function. If zC2q([0,T],R), then z satisfies the problem (3.18) if and only if z satisfies the integral equation:

    z(t)=λ1Γq(δ+1)tδT(δ)+(λ2λ1)Γq(δ+1)[1Γq(α+δ)T0(Tqν)(α+δ1)qf(ν,z(ν))dqν+λ2Γq(α)T0(Tqν)(α1)qf(ν,z(ν))dqν]+1Γq(α+δ)t0(tqν)(α+δ1)qf(ν,z(ν))dqν. (3.19)

    Case Ⅳ. Let β=0, then γ=α, and problem (1.6) reduces to the sequential q-Riemann and Caputo fractional-order differential equation given by

    {RLDαq(CDδqz)(t)=f(t,z(t)),t[0,T],z(0)+λ1CDα+δ1qz(0)=0,z(T)+λ2CDα+δ1qz(T)=0. (3.20)

    Corollary 3.4. Let 0<α,δ<1, and f:[0,T]×RR is a continuous function. If zC([0,T],R), then z satisfies the problem (3.20) if and only if z satisfies the integral equation:

    z(t)=λ1Γq(α+δ)t(α+δ1)Q[1Γq(α+δ)T0(Tqν)(α+δ1)qf(ν,z(ν))dqν+λ2T0f(ν,z(ν))dqν]+1Γq(α+δ)t0(tqν)(α+δ1)qf(ν,z(ν))dqν, (3.21)

    where Q=T(α+δ1)+(λ2λ1)Γq(α+δ).

    Case Ⅴ. If q=1, then problem (1.6) reduces to the sequential Hilfer and Caputo boundary value problem of the form:

    {HDα,β(CDδz)(t)=f(t,z(t)),t[0,T],z(0)+λ1CDγ+δ1z(0)=0,z(T)+λ2CDγ+δ1z(T)=0. (3.22)

    Corollary 3.5. Let 0<α,δ<1, 0β1, and γ=α+β(1α). Suppose f:[0,T]×RR is a continuous function. If zC2([0,T],R), then z satisfies the problem (3.22) if and only if z satisfies the integral equation:

    z(t)=λ1Γ(γ+δ)tγ+δ1Q[1Γ(α+δ)T0(Tν)α+δ1f(ν,z(ν))dν+λ2Γ(αγ+1)T0(Tν)αγf(ν,z(ν))dν]+1Γ(α+δ)t0(tν)α+δ1f(ν,z(ν))dν. (3.23)

    Example 4.1. Consider the sequential fractional differential equation involving q-Hilfer and q-Caputo fractional derivatives:

    {HD35,2512(CD4512z)(t)=f(t,z(t)),t[0,97],z(0)+1123CD142512z(0)=0,z(97)+1329CD142512z(97)=0. (4.1)

    Now, we choose constants as α=3/5, β=2/5, δ=4/5, q=1/2, T=9/7, λ1=11/23, λ2=13/29. Then we compute γ=19/25, which yields γ+δ1=14/25. These information can be used to find that Q1.123420003, Δ3.821919331, and Δ(T(α+δ)/Γq(α+δ))2.578777897.

    Case (i). Let the nonlinear bounded function f(t,z) be presented by

    f(t,z)=h(t)+|z|p+|z|, (4.2)

    where h:[0,9/7]R, and p is a positive constant.

    Thus,

    |f(t,z)||h(t)|+1:=Ψ(t).

    and

    |f(t,z)f(t,z1)|1p|zz1|,

    for all t[0,9/7] and z,z1R. Therefore, conditions (H1) and (H2) in Theorem 3.1 are satisfied with L=1/p. Thus, from Theorem 3.1, we say that problem (4.1) with (4.2) has at least one solution on [0,9/7] if p>2.578777897. In addition, the unique solution of problem (4.1) with (4.2), can be guaranteed if p>3.821919331 by applying the result in Theorem 3.3.

    Case (ii). If the nonlinear, unbounded function f(t,z) is expressed as

    f(t,z)=12(t2+4)(z2+2|z|1+|z|)+34, (4.3)

    then it is easy to check that condition (H1) is fulfilled by inequality

    |f(t,z)f(t,z1)|14|zz1|,

    with L=1/4, which leads to

    LΔ0.9554798328<1.

    Hence, problem (4.1) with (4.3) has a unique solution on [0,9/7].

    Example 4.2. Consider the sequential boundary value differential equations in the frame of q-Hilfer and q-Caputo fractional derivatives given by:

    {HD57,3423(CD6723z)(t)=1t+2(z2024(t)4(1+z2022(t))+1t+3),t[0,89],z(0)+1731CD111423z(0)=0,z(89)+1937CD111423z(89)=0. (4.4)

    Here α=5/7, β=3/4, γ=13/14 (by computing), q=2/3, δ=6/7, T=8/9, λ1=17/31, λ2=19/37, and γ+δ1=11/14. From all constants, we have Q0.8787426597 and Δ2.500884518.

    Now, we see that the nonlinear non-Lipschitzian function f(t,z) shown in the right-side of the first equation in (4.4), is bounded by

    |f(t,z)|=|1t+2(z2024(t)4(1+z2022(t))+1t+3)|1t+2(14z2+13).

    Choosing G(t)=1/(t+2) and Λ(u)=(1/4)u2+(1/3), we have G=1/2, and we can find that C(0.492701921,2.706166297) satisfying (H4). Thus, by applying Theorem 3.2, we say that problem (4.4) has at least one solution on [0,8/9].

    Since the appearance of fractional operators, many research articles have been dedicated to improving and generalizing those operators. This paper investigates the existence and uniqueness of the results of a sequential boundary value problem in the setting of q-Hilfer and q-Caputo fractional derivatives with separated boundary conditions. The proposed problem is new and can be visualized as a generalization of Hilfer, q-Caputo, Caputo, q-Riemann-Liouville, and Riemann-Liouville fractional differential equations.

    All authors contributed equally and significantly to writing this article. All authors read and approved the final manuscript.

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

    The first author was supported by King Mongkut's University of Technology North Bangkok with contract no. KMUTNB-Post-67-08. This research budget was allocated by National Science, Research and Innovation Fund (NSRF) and King Mongkut's University of Technology North Bangkok with Contract no. KMUTNB-FF-67-B-02.

    The authors declare no conflict of interest.



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