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Research article

On Cauchy-type problems with weighted R-L fractional derivatives of a function with respect to another function and comparison theorems

  • Received: 18 January 2024 Revised: 23 March 2024 Accepted: 02 April 2024 Published: 18 April 2024
  • MSC : 26A33, 34A08, 34K37

  • The main aim of this paper is to study the Cauchy problem for nonlinear differential equations of fractional order containing the weighted Riemann-Liouville fractional derivative of a function with respect to another function. The equivalence of this problem and a nonlinear Volterra-type integral equation of the second kind have been presented. In addition, the existence and uniqueness of the solution to the considered Cauchy problem are proved using Banach's fixed point theorem and the method of successive approximations. Finally, we obtain a new estimate of the weighted Riemann-Liouville fractional derivative of a function with respect to functions at their extreme points. With the assistance of the estimate obtained, we develop the comparison theorems of fractional differential inequalities, strict as well as nonstrict, involving weighted Riemann-Liouville differential operators of a function with respect to functions of order δ, 0<δ<1.

    Citation: Iman Ben Othmane, Lamine Nisse, Thabet Abdeljawad. On Cauchy-type problems with weighted R-L fractional derivatives of a function with respect to another function and comparison theorems[J]. AIMS Mathematics, 2024, 9(6): 14106-14129. doi: 10.3934/math.2024686

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  • The main aim of this paper is to study the Cauchy problem for nonlinear differential equations of fractional order containing the weighted Riemann-Liouville fractional derivative of a function with respect to another function. The equivalence of this problem and a nonlinear Volterra-type integral equation of the second kind have been presented. In addition, the existence and uniqueness of the solution to the considered Cauchy problem are proved using Banach's fixed point theorem and the method of successive approximations. Finally, we obtain a new estimate of the weighted Riemann-Liouville fractional derivative of a function with respect to functions at their extreme points. With the assistance of the estimate obtained, we develop the comparison theorems of fractional differential inequalities, strict as well as nonstrict, involving weighted Riemann-Liouville differential operators of a function with respect to functions of order δ, 0<δ<1.



    Fractional calculus is a generalization of ordinary calculus that studies the integration and differentiation of real or complex orders. Even though it is ancient, this calculus has experienced a surge in popularity in recent decades because of the interesting results obtained when it was applied to model some real-world phenomena. The presence of numerous new fractional operators is what distinguishes fractional calculus. This feature enables scientists to enhance the development of models for real-world problems by selecting the operator that best fits the model they are studying. Numerous phenomena across diverse fields such as science, mathematics, engineering, bioengineering, and economics are more precisely elucidated through the application of fractional derivatives, as we refer the readers to [1,2,3,4].

    Recently, the theory concerning the existence and uniqueness of solutions for the Cauchy-type problems of fractional differential equations has been developing and is increasingly recognized as a valuable tool for modeling real-world problems across various domains, leading to a significantly richer theoretical framework compared to the theory of ordinary differential equations [5,6,7]. Applications for fractional differential equations are found in many scientific domains, including but not limited to engineering [8], chemistry [9], physics [10], and other fields [11,12].

    The complexity of applications is the main reason that prompted researchers to expand the definitions of fractional derivatives. This leads to the proposal of weighted fractional derivatives to generalize many known fractional operators (see [13,14,15]). In [16,17], Agrawal introduced generalized fractional derivatives known as weighted fractional derivatives and outlined some of their properties. Nevertheless, no details were provided regarding the spaces on which these operators are defined. In [18,19], weighted fractional operators are studied, and many fundamental properties of these operators are studied. In addition, some spaces in which these operators are defined are presented. Recent research has discussed the weighted fractional operators with their applications and studied the mathematical properties in [16,17,20,21], along with a study of the associated differential equations presented in [22,23,24]. There are two categories of nonlocal fractional derivatives: The classical ones characterized by singular kernels, such as the Riemann-Liouville and Caputo derivatives, and the more recently introduced ones with nonsingular kernels, such as the Atangana-Baleanu and Caputo-Fabrizio derivatives [25,26]. In recent publications [20,21], the authors introduced the weighted Caputo-Fabrizio fractional operators. Furthermore, they expanded the scope of their investigation to encompass the weighted Atangana-Baleanu fractional operators and a study of their properties.

    The comparison theorem is one of the basic theories of differential equations, playing an important role in the qualitative analysis of research. In [27,28,29], comparison theorems relative to fractional differential and integral inequalities involving Riemann-Liouville derivatives of order δ, 0<δ<1, were proved. In [30], the comparison results were presented for the Riemann-Liouville fractional differential equation of order δ, 0<δ<1. Notably, these results were presented without necessitating the Hölder continuity assumption [29], where the local Hölder continuity assumption is replaced with Cp-continuity of the functions involved in the Riemann-Liouville fractional differential equations; see [31,32] and references therein for further details.

    This paper's principal contribution lies in extending the methodology introduced by Chunhai Kou et al.[5] to tackle fractional Cauchy problems involving weighted Riemann-Liouville operators of a function with respect to another function. Our contributions include not only establishing the existence and uniqueness of solutions but also generalizing the comparison result for these problems introduced by V. Lakshmikantham et al.[29]. As it stands, there has been no initiation of work on comparison theorems for fractional differential equations that incorporate the weighted Riemann-Liouville derivative of a function with respect to another function of order δ, 0<δ<1. We have confidence that the obtained results will serve as a beneficial addition and extension to the current findings in the literature. In fact, the existence and uniqueness investigations in this work are necessary steps to proceed with proving the comparison theory of the considered weighted fractional system as an essential part of analyzing the qualitative theory of dynamic systems. The used kernel and weight require extra effort to analyze such a general system. Moreover, weighted fractional derivatives include a considerable class of fractional operators. For example, tempered fractional operators can be considered a particular case. Such a general type of fractional operator makes it easier to handle more complex real-world systems in modeling.

    The current work is as follows: Section 2 consists of preliminary definitions and results concerning the weighted fractional operators of a function with respect to another function. In Section 3, we outline our problem and discuss the equivalence between an initial value problem and a Volterra integral equation. In Section 4, we substantiate the existence and uniqueness theorem for the initial value problem discussed in the preceding section. Section 5 deals with the estimation of the weighted Riemann-Liouville derivative of a function with respect to another function at extreme points. Based on the obtained results, we derive comparison results for the weighted Riemann-Liouville fractional differential equations involving initial conditions. Lastly, we conclude with a summary, and we talk about future extensions for this work.

    In this section, we present some fundamental definitions of weighted fractional calculus of a function with respect to another function, lemmas, theorems, and propositions that are important and needed for our findings in this article (cf. [16,18,19]).

    Theorem 2.1. (Banach fixed point theorem [11]) Let (S,σ) be a nonempty, complete metric space, let 0λ<1, and let A:SS be the map such that, for every u,vS, the relation

    σ(Au,Av)λσ(u,v)(0λ<1), (2.1)

    holds. Then the operator A has a unique fixed point uS.

    Furthermore, if Ai(iN) is the sequence of operators defined by

    A1=AandAi=AAi1(iN{1}), (2.2)

    then, for any u0S, the sequence {Aiu0}i=1 converges to the above fixed point u.

    Definition 2.1. [11] Assume that κ(t,z) is defined on the (,r]×Ω(ΩR). κ(t,z) is said to satisfy Lipschitzian condition with respect to the second variable, if for all t(,r] and for any z1,z2Ω one has

    |κ(t,z1)κ(t,z2)|L|z1z2|, (2.3)

    where L>0 does not depend on t[,r].

    Let D=[,r](0<r<) be a finite interval and ϱ be a parameter such that m1ϱ<m. The space of continuous functions κ on D is denoted by C[,r] and the associated norm is defined by [33]

    κC[,r]=maxt[,r]|κ(t)|,

    and

    ACm[,r]={κ:[,r]R such that κ(m1)AC[,r]},

    be the space of m times absolutely continuous differentiable functions.

    The weighted space Cϱ,θ[,r] of functions κ on (,r] is defined by

    Cϱ,θ[,r]={κ:(,r]R;(θ(t)θ())ϱκ(t)C[,r]},

    having norm

    κCϱ,θ[,r]=(θ(t)θ())ϱκ(t)C[,r]=maxt[,r]|(θ(t)θ())ϱκ(t)|.

    The weighted space Cmϱ,θ[,r] of functions κ on (,r] is defined by

    Cmϱ,θ[,r]={κ:[,r]R;κ(t)Cm1[,r];κ(m)(t)Cϱ,θ[,r]},

    along with the norm

    κCmϱ,θ[,r]=m1i=0κ(i)C[,r]+κ(m)Cϱ,θ[,r].

    The above space satisfies the following properties:

    (1) C0ϱ,θ[,r]=Cϱ,θ[,r], for m=0.

    (2) For m1ϱ1<ϱ2<m, Cϱ1,θ[,r]Cϱ2,θ[,r].

    The space ACmπ[,r] is defined by [18]

    ACmπ[,r]={κ:[,r]R such that κ(m1)πAC[,r]}

    where AC[,r] is the set of absolute continuous functions on the interval [,r], and

    κ(m)π(t)=1π(t)(Dtθ(t))(m)(π(t)κ(t)),m=0,1,2,...

    The space χpπ(,r), 1p is defined by [18]

    χpπ(,r)={κ:[,r]R;κ is measurable functionr|π(t)κ(t)|pθ(t)dt<},

    along with the norm

    κχpπ=(r|π(t)κ(t)|pθ(t)dt)1p,1p.

    It should be noted that

    fχpπ(,r)π(t)κ(t)(θ(t))1pLp(,r),

    where θ is a differential strictly increasing function and π(t)0 be a weight function on [,r].

    Definition 2.2. [16,18,19] Let θ:[,r]R be a strictly increasing C1 function, so that θ>0 everywhere, and let πL(,r) be a weight function, κX1π(,r). The π-weighted Riemann-Liouville fractional integral of order δ>0 of a function κ(t) with respect to another function θ(t), is defined by

    (δ,θ(t)+,π(t)κ)(t)=1π(t)Γ(α)t(θ(t)θ(s))δ1π(s)θ(s)κ(s)ds,t(,r). (2.4)

    Here, Γ(α)=0sα1esds,Re(α)>0 is the Gamma function extending the factorial notation.

    Definition 2.3. [16,18,19] Let mN. The π-weighted derivatives of integer order m of a function κ with respact to another function θ is defined as

    (Dm,θ(t)π(t)κ)(t)=1π(t)[(ϑtθ(t))m(π(t)κ(t))](t), (2.5)

    where ϑt=ddt, and the first-order operator D1,θ(t)π(t) is defined by

    (D1,θ(t)π(t)κ)(t)=1π(t)[(ϑtθ(t))(π(t)κ(t))](t). (2.6)

    Definition 2.4. [16,18,19] Let κACmπ,θ[,r]. Then, the π-weighted Riemann-Liouville fractional derivative of order δ>0 of the function κ with respect to another function θ is defined as

    (Dδ,θ(t)+,π(t)κ)(t)=(Dm,θ(t)π(t)mδ,θ(t)+,π(t)κ)(t)=Dm,θ(t)π(t)π(t)Γ(mδ)t(θ(t)θ(s))mδ1π(s)θ(s)κ(s)ds, (2.7)

    where m=[δ]+1 so that m1<δ<m, [δ] being the integer part of δ.

    Property 2.2. [16,18,19]

    1) For δ>0 and μ>0, we have

    (δ,θ(t)+,π(t)[(θ(t)θ())μ1π(t)])(t)=Γ(μ)Γ(μ+δ)π(t)(θ(t)θ())μ+δ1. (2.8)

    2) For δ<m(mN) and μ>0, we have

    (Dδ,θ(t)+,π(t)[(θ(t)θ())μ1π(t)])(t)=Γ(μ)Γ(μδ)π(t)(θ(t)θ())μδ1. (2.9)

    On the other hand, for i=1,2,,[δ]+1, we have

    (Dδ,θ(t)+,π(t)[(θ(t)θ())δiπ(t)])(t)=0. (2.10)

    Theorem 2.3. [16,18,19] Let κχpπ(,r), 1p, δ>0 and μ>0. Then,

    (δ,θ(t)+,π(t)μ,θ(t)+,π(t)κ)(t)=(δ+μ,θ(t)+,π(t)κ)(t). (2.11)

    Property 2.4. [16,18,19] Let δ>μ>0 and κχpπ(,r), 1p<. Then,

    (Dμ,θ(t)+,π(t)δ,θ(t)+,π(t)κ)(t)=(δμ,θ(t)+,π(t)κ)(t), (2.12)

    where m=[δ]+1.

    Theorem 2.5. [16,18,19] Let δ>0. Then, we have

    (Dδ,θ(t)+,π(t)δ,θ(t)+,π(t)κ)(t)=κ(t). (2.13)

    Lemma 2.6. [16,18,19] Let δ>0, m=[δ], κχpπ(,r) and δ,θ(t)+,π(t)κACmπ[,r]. Then

    (δ,θ(t)+,θ(t)Dδ,θ(t)π(t)k)(t)=κ(t)π1(t)mi=1(θ(t)θ())δiΓ(δi+1)(mδ,θ(t)+,π(t)κ)mi(+), (2.14)

    where

    (mδ,θ(t)+,π(t)κ)i(+)=(ϑtθ(t))i(π(t)mδ,θ(t)+,π(t)κ)(+),i=0,1,,m. (2.15)

    In particular, if 0<δ<1, then

    (δ,θ(t)+,π(t)Dδ,θ(t)π(t)κ)(t)=κ(t)π(+)(1δ,θ(t)+,π(t)κ)(+)Γ(δ)(θ(t)θ())δ1π1(t). (2.16)

    Let D=[,r] be a finite interval and ϱ be a parameter such that m1<ϱm, then

    1) The weighted space Cπϱ,θ[a,b] of functions κ with respect to θ and weighted π on [,r] is defined by

    Cπϱ,θ[,r]={κ:(,r]R;(θ(t)θ())ϱπ(t)κ(t)C[,r]}, (3.1)

    having norm

    κCπϱ,θ[,r]=(θ(t)θ())ϱπ(t)κ(t)C[,r].

    The above space satisfies the following properties:

    i) Cπϱ,θ[,r]=C[,r], for ϱ=0 and π(t)=1.

    ii) For π(t)=1, Cπϱ,θ[,r]=Cϱ,θ[,r].

    2) The weighted space Cm,πϱ,θ[,r] of functions κ with respect to θ and weighted π on [,r] is defined by

    Cm,πϱ,θ[,r]={κ:[,r]R;(πκ)(t)Cm1[,r];(Dm,θ(t)π(t)κ)(t)Cπϱ,θ[,r]}, (3.2)

    where

    (Dm,θ(t)π(t)κ)(t)=1π(t)(ϑtθ(t))m(π(t)κ(t)),ϑt=ddt, (3.3)

    along with the norm

    κCm,πϱ,θ[,r]=m1i=0(πκ)(i)C[,r]+Dm,θ(t)π(t)κCπϱ,θ[,r].

    The above space satisfies the following properties:

    p1) C0,πϱ,θ[,r]=Cπϱ,θ[,r], for m=0.

    p2) Cπϱ,θ[,r]=Cϱ,θ[,r] and Cm,πϱ,θ[,r]=Cmϱ,θ[,r], for π(t)=1.

    3) For m1<δm(mN), we denote by Cδ,πϱ,θ[,r]

    Cδ,πϱ,θ[,r]={z(t)Cπϱ,θ[,r]:(Dδ,θ(t)+,π(t)z)(t)Cπϱ,θ[,r]}. (3.4)

    4) The space Cπ[,r] of functions κ with respect to weighted π on [,r] is defined by

    Cπ[,r]={κ:(,r]R;π(t)κ(t)C[,r]}. (3.5)

    We will study the existence and uniqueness of a Cauchy-type problem with a π-weighted Riemann-Liouville fractional derivative of a function with respect to another function

    (Dδ,θ(t)+,π(t)z)(t)=κ(t,z(t))(δ>0,t>), (3.6)

    with initial conditions

    (πDδk,θ(t)+π(t)z)(+)=rk,rkR(k=1,...,m=[δ]). (3.7)

    From the above initial condition and by Definition 2.4, it is clear that

    (πDδk,θ(t)+,π(t)z)(t)=(mδ,θ(t)+,π(t)z)mk(t)=(ϑtθ(t))mk(πmδ,θ(t)+,π(t)z)(t), (3.8)

    where, (δ,θ+,π(t)z(t)) is the π-weighted Riemann-Liouville fractional integration operator of order δ defined by (2.4).

    The notation (Dδk,θ(t)+,π(t)z)(+) means that the limit is taken at almost all points of the right-sided neighborhood (,+ε)(ε>0) of a as follows:

    (πDδk,θ(t)+,π(t)z)(+)=π(+)limt+(Dδk,θ(t)+,π(t)z)(t)(1km1), (3.9)
    (πDδm,θ(t)+,π(t)z)(+)=π(+)limt+(mδ,θ(t)+,π(t)z)(t),(δm). (3.10)

    The nonlinear Volterra integral equation of the second kind corresponding to the problems (3.6)(3.7) takes the form

    z(t)=1π(t)mj=1rjΓ(δj+1)(θ(t)θ())δj+1π(t)Γ(δ)t(θ(t)θ(s))δ1π(s)θ(s)κ(s,z(s))ds. (3.11)

    In particular, if 0<δ<1, the problems (3.6)(3.7) takes the form

    {(Dδ,θ(t)+,π(t)z)(t)=κ(t,z(t)),(0<δ<1),(π1δ,θ(t)+,π(t)z)(+)=rrR.} (3.12)

    and this problem can be rewritten as a weighted Cauchy type problem

    {(Dδ,θ(t)+,π(t)z)(t)=κ(t,z(t)),(0<δ<1),limt+(θ(t)θ())1δπ(t)z(t)]=CCR.} (3.13)

    The corresponding integral equation to the problem (3.12) has the form:

    Z(t)=r(θ(t)θ())δ1Γ(δ)π(t)+1π(t)Γ(δ)t(θ(t)θ(s))δ1π(s)θ(s)κ(s,z(s))ds. (3.14)

    In this section, we give conditions for a unique solution z(t) to the Cauchy type problems (3.6)(3.7) in the space Cδ,πmδ,θ[,r].

    First, we prove that the Cauchy type problems (3.6)(3.7) and the nonlinear Volterra integral equation (3.11) are equivalent in the space Cπmδ,θ[,r], in the sense that, if z(t)Cπmδ,θ[,r] satisfies one of these relations, then it also satisfies the other one. For that, we need the following lemmas:

    Lemma 3.1. If ϱR(0ϱ<1), then the π-weighted Riemann-Liouville fractional integral operator δ,θ(t)+,π(t) with δR(δ>0) is bounded from Cπϱ,θ[,r] into Cπϱ,θ[,r], and

    δ,θ(t)+,π(t)κCπϱ,θ[,r](θ(r)θ())δΓ(1ϱ)Γ(1+δϱ)κCπϱ,θ[,r]. (3.15)

    Proof. Using the definition of the weighted fractional integral (2.4) and property 2.2, for any κCπϱ,θ[,r] and t[,r], we obtain

    |(θ(t)θ())ϱπ(t)δ,θ(t)+,π(t)κ(t)|=|(θ(t)θ())ϱ1Γ(δ)t(θ(t)θ(s))δ1θ(s)π(s)κ(s)ds||(θ(t)θ())ϱ||Γ(δ)|t|(θ(t)θ(s))δ1(θ(s)θ())ϱθ(s)|×|(θ(s)θ())ϱκ(s)π(s)|dsπ(t)(θ(t)θ())ϱκCπϱ,θ[,r](δ,θ(t)+,π(t)(π1(t)(θ(t)θ())ϱ))(t)=(θ(t)θ())δΓ(1ϱ)Γ(1+δϱ)κCπϱ,θ[,r].

    Now, by the definition of the weighted space Cπϱ,[,r] defined by (3.1), we have

    δ,θ(t)+,π(t)κCπϱ,θ[,r]=(θ(t)θ())ϱπ(t)δ,θ(t)+,π(t)κ(t)C[,r](θ(r)θ())δΓ(1ϱ)Γ(1+δϱ)κCπϱ,θ[,r].

    Hence, the proof of this lemma is complete.

    Lemma 3.2. Let δ>0, μ>0, and 0ϱ<1. The following assertions are then true:

    a) If κ(t)Cπϱ,θ[,r], then the relation (2.11) holds any point t(,r].

    b) If κ(t)Cπϱ,θ(t)[,r], then the equality (2.13) holds any point t(,r].

    c) Let δ>μ>0. If κ(t)Cπϱ,θ[,r], then the relation (2.12) holds at any point t(,r].

    d) Let m=[δ]+1. Also, let (mδ,θ(t)+,π(t)κ)(t) be the weighted fractional integral (2.4) of order mδ.

    If κ(t)Cωϱ,θ[,r] and (mδ,θ(t)+,π(t)κ)(t)Cm,πϱ,θ[,r], then the relation (2.14) holds at any point t(,r].

    In particular, when 0<δ<1 and (1δ,θ(t)+,π(t)κ)(t)C1,πϱ,θ[,r], the equality (2.16) is valid.

    Proof. As the proof is similar to the proofs in [18], we deleted it.

    Lemma 3.3. Let 0<<r<, δ>0 and m1ϱ<m with mN and κCπϱ,θ[,r].

    If δ>ϱ and π(t)>0, for all t[,r], then δ,θ(t)+,π(t)κ is continuous on [,r] and

    (δ,θ(t)+,π(t)κ)()=limt+(δ,θ(t)+,π(t)κ)(t)=0. (3.16)

    Proof. Since κCπϱ,θ[,r], then (θ(t)θ())ϱπ(t)κ(t) is continuous on [,r] and hence

    |(θ(t)θ())ϱπ(t)κ(t)|<C,

    where t[,r] and C>0 is a constant.

    Therefore,

    |(ϱ,θ(t)+,π(t)κ)(t)|<C(δ,θ(t)+,π(t)(π1(t)(θ(t)θ())ϱ))(t),

    and by Property 2.2, we can write

    |(δ,θ(t)+,π(t)κ)(t)|<CΓ(1ϱ)Γ(δϱ+1)(π1(t)(θ(t)θ())δϱ)). (3.17)

    As δ>ϱ, the right-hand side of (3.17) goes to zero when t+, we obtain the result.

    Theorem 3.4. Let δ>0, m=[δ]. Let B be an open set in R and let κ:(,r]×BR be a function such that κ(t,z(t))Cπmδ,θ[,r] for any z(t)Cπmδ,θ[,r]. If z(t)Cπmδ,θ[,r], then z(t) satisfies the relations (3.6)(3.7) if, and only if, z(t) satisfies the Volterra integral equation (3.11).

    Proof. First, we prove the necessity. Let z(t)Cπmδ,θ[,r] satisfy the relations (3.6)(3.7). By hypothesis, κ(t,z)Cπmδ,θ[,r] and it follows from (3.6) that

    (Dδ,θ(t)+,π(t)z)(t)Cπmδ,θ[,r].

    According to (2.7)

    (Dδ,θ(t)+,π(t)z)(t)=(Dm,θ(t)π(t)mδ,θ(t)+,π(t)z)(t),m=[δ], (3.18)

    and hence, by Lemma 3.1, we have

    (mδ,θ(t)+,π(t)z)(t)Cm,π(t)mδ,θ(t)[,r].

    Thus, we can apply Lemma 3.2 (d), and, in accordance with (2.14), we have

    (δ,θ(t)+,π(t)Dδπ(t)z)(t)=z(t)mj=1(θ(t)ψ())δjπ1(t)Γ(δj+1)(mδ,θ(t)+,π(t)z)mj(+), (3.19)

    where

    (mδ,θ(t)+,π(t)z)mj(+)=(ϑtθ(t))mj(π(t)mδ,θ(t)+,π(t)z)(+),ϑt=ddt.

    By (3.7) and (3.9), we rewrite (3.19) in the form

    (δ,θ(t)+,π(t)Dδπ(t)z)(t)=z(t)mj=1(θ(t)θ())δjπ1(t)Γ(δj+1)(πDδj,θ(t)+,π(t)t)(+)=z(t)mj=1rjΓ(δj+1)(θ(t)θ())δjπ1(t). (3.20)

    By Lemma 3.1, the integral (δ,θ(t)+,π(t)κ(t,z(t)))(t)Cπmδ,θ[,r] exists on [,r]. Applying the operator δ,θ(t)+,π(t) to both sides of (3.6) and using (3.20), we obtain Eq (3.11), and hence necessity is proved.

    Now, we prove sufficiency. Let z(t)Cπmδ,θ[,r] satisfy the Eq (3.11). Applying the operator Dδ,θ(t)+π(t) to both sides of (3.11), we have

    (Dδ,θ(t)+,π(t)z)(t)=mj=1rjΓ(δj+1)(Dδ,θ+,π(t)(π1(t)(θ(t)θ())δj))(t)+(Dδ,θ(t)+,π(t)δ,θ(t)+,π(t)κ(t,z(t)))(t).

    From here, in accordance with the formula (2.10) and Lemma 3.2 (b), we arrive at Eq (3.6).

    Now, we show that the relation in (3.7) also holds. For this, we apply the operators Dδk+,π(t)(k=1,...,m) to both sides of (3.11).

    If 1km1, then, in accordance with (2.9) and Lemma 3.2(c), we have

    (Dδk,θ(t)+,π(t)z)(t)=mj=1rjΓ(δj+1)(Dδk,θ(t)+,π(t)((θ(t)θ())δjπ1(t)))(t)+(Dδk,θ(t)+,π(t)δ,θ(t)+,π(t)κ(t,z(t)))(t)=mj=1rjΓ(kj+1)(θ(t)θ())kjπ1(t)+(k,θ(t)+,π(t)κ(t,(t)))(t).

    Hence,

    (Dδk,θ(t)+,π(t)z)(t)=mj=1rj(kj)!(θ(t)θ())kjπ1(t)+π1(t)(k1)!t(θ(t)θ(s))k1π(s)κ(s,z(s))θ(s)ds. (3.21)

    If k=m, then, in accordance with (3.10), (2.8) and, Lemma 3.2 (a), and using Lemma 3.3, similarly to (3.21), we obtain

    (Dδm,θ(t)+,π(t)z)(t)=mj=1rjΓ(δj+1)(mδ,θ(t)+,π(t)((θ(t)θ())δjπ1(t)))(t)+(mδ,θ(t)+,π(t)δ,θ(t)+πκ(t,z(t)))(t)=mj=1rjΓ(mj+1)(θ(t)θ())mjπ1(t)+(m,θ(t)+π(t)κ(t,z(t)))(t).

    Therefore,

    (Dδm,θ(t)+,π(t)(t))(t)=mj=1rj(mj)!(θ(t)θ())mjπ1(t)+π1(t)(m1)!t(θ(t)θ(s))m1π(s)κ(s,z(s))ψ(s)ds. (3.22)

    Multiplying (3.21), (3.22) by π(t) and taking the limit as t0+ above, we obtain (3.7). Thus, sufficiency is proven, and the proof is completed.

    Corollary 3.5. Let 0<δ<1, let B be an open set in R and let κ:(,r]×BR be a function such that κ(t,z(t))Cπ1δ,θ[,r] for any z(t)Cπ1δ,θ[,r]. If z(t)Cπ1δ,θ[,r], then z(t) satisfies the relations in (3.12) if, and only if, z(t) satisfies the integral equation (3.14).

    Next, we will establish the existence and uniqueness of a solution for the Cauchy-type problems (3.6)(3.7) in the space Cδ,ωϱ,θ[,r], as defined in (3.4), utilizing the Banach fixed point theorem. This requires the following lemmas:

    Lemma 3.6. Let λ[0,), <n<r, κCπλ,θ[,n] and κCπ[n,r]. Then κCπλ,θ[,r] and

    κCπλ,θ[,r]max{κCπλ,θ[,n],(θ(r)ψ())λκCπ[n,r]}, (3.23)

    where the space Cπ[,r] is the same as defined in (3.5).

    Proof. Since κCπλ,θ[,n] and κCπ[n,r], then we obtain

    κCπ(,r]andκCπλ,θ[,r].

    Now, we prove the estimate. Because κCπλ,θ[,r], there exists t[,r] such that

    κCπλ,θ[,r]=|(θ(t)θ())λπ(t)κ(t)|. (3.24)

    Assume that t[,n], then we have

    κCπλ,θ[,r]κCπλ,θ[,n].

    Similarly, if we suppose that t[n,r], then we have

    κCπλ,θ[,r](θ(r)θ())λκCπ[n,r].

    Now, we can write this result

    κCπλ,θ[,r]max{κCπλ,θ[,n],(θ(r)θ())λκCπ[n,r]}.

    The proof of this lemma is complete.

    Lemma 3.7. The weighted fractional integration operator δ,θ(t)+,π(t) of order δ(δ>0) is a mapping from Cπ[,r] to Cπ[,r], and

    δ,θ(t)+,π(t)κCπ[,r](θ(r)ψ())λδΓ(δ)κCπ[,r], (3.25)

    where κCπ[,r].

    Proof. we prove the estimate in (3.25) as follows:

    |π(t)δ,θ(t)+,π(t)κ(t)|=|1Γ(δ)t(θ(t)θ(s))δ1θ(s)π(s)κ(s)ds|πκC[,r]Γ(δ)t(θ(t)θ(s))δ1θ(s)ds=(θ(t)θ())λδΓ(δ)κCπ[,r].

    Therefore,

    δ,θ(t)+,π(t)κCπ[,r](θ(r)θ())λδΓ(δ)κCπ[,r].

    Hence, the proof of this lemma is complete.

    Theorem 3.8. Let δ>0 and m=[δ]. Let B be an open set in R and let κ:(,r]×BR be a function such that κ(t,z(t))Cπmδ,θ[,r] for any z(t)Cπmδ,θ[,r] and the Lipschitzian condition (2.3) holds.

    Then there exists a unique solution z(t) to the Cauchy type problems (3.6)(3.7) in the space Cπmδ,θ[,r].

    Proof. Step1. First we prove the existence of a unique solution z(t)Cπmδ,θ[,r]. According to the previous Theorem 3.4, it is sufficient to prove the existence of a unique solution z(t)Cπmδ,θ[,r] to the nonlinear Volterra integral equation (3.11), which, mainly based on Theorem 2.1(Banach fixed point theorem).

    Divide the interval [,r] into M subdivisions [,t1],[t1,t2],...,[tM1,r] such that <t1<t2<...<tM1<r.

    I) Choose t1(,r] such that the following estimate holds

    ξ1=L(θ(t1)θ())δΓ(δm+1)Γ(2δm+1)<1, (3.26)

    where L is the Lipschitzian constant. Now we prove that there exists a unique solution z(t)Cωmδ,θ[,t1] to (3.11) on the interval (,t1]. To do this, we apply the Banach fixed point theorem (Theorem 2.1) for the space Cπmδ,θ[,r], which is the complete metric space equipped with the distance given by

    σ(z1,z2)=z1z2Cπmδ,θ[,t1]=maxt[,t1]|(θ(t)θ())mδπ(t)[z1(t)z2(t)]|.

    For any z(t)Cπmδ,θ[,t1], we define the operator A by expressing the integral equation (3.11) as follows:

    z(t)=(Az)(t),
    (Az)(t)=z0(t)+1Γ(δ)π(t)t(θ(t)θ(s))δ1θ(s)ω(s)κ(s,z(s))ds, (3.27)

    with

    z0(t)=1π(t)mj=1rjΓ(δj+1)(θ(t)θ())δj. (3.28)

    Applying the Banach contraction mapping, we shall prove that A has a unique fixed point.

    Firstly, we have to show that:

    I1) If z(t)Cπmδ,θ[,t1], then (Az)(t)Cπmδ,θ[,t1].

    I2) For any z1,z2Cπmδ,θ[,t1] the following estimate holds:

    Az1Az2Cπmδ,θ[,t1]ξ1z1z2Cπmδ,θ[,t1],ξ1=L(θ(t1)θ())δΓ(δm+1)Γ(2δm+1). (3.29)

    It is evident from Eq (3.28) that z0(t)Cπmδ,θ[,t1]. Since κ(t,z(t))Cπmδ,θ[,t1] for any z(t)Cπmδ,θ[,t1], then, by Lemma 3.1, the integral in the right-hand side of (3.27) also belongs to Cπmδ,θ[,t1]. The above implies that (Az)(t)Cπmδ,θ[,t1].

    Let z1,z2Cπmδ,θ[,t1]. Using (3.27), (2.3) and hance by Lemma 3.1, we obtain

    Az1Az2Cπmδ,θ[,t1]=δ,θ(t)+,π(t)(κ(t,z1(t))κ(t,z2(t)))Cπmδ,θ[,t1](θ(t1)θ())δΓ(δm+1)Γ(2δm+1)κ(t,z1(t))κ(t,z2(t))Cπmδ,θ[,t1]L(θ(t1)θ())δΓ(δm+1)Γ(2δm+1)z1z2Cπmδ,θ[,t1]=ξ1z1z2Cπmδ,θ[,t1].

    This results in obtaining the estimate (3.29). By (3.26), 0<ξ1<1, and therefore by using the Banach fixed point theorem, there exists a unique solution z(t)Cπmδ,θ[,t1] to (3.11) on the interval [,t1]. This solution z(t) is a limit of a convergent sequence (Aiz0)(t):

    limiAiz0zCπmδ,θ[,t1]=0, (3.30)

    where z0(t) is any function in Cπmδ,θ[,t1], and

    (Aiz0)(t)=z0(t)+1Γ(δ)π(t)t(θ(t)θ(s))δ1θ(s)π(s)κ(s,(Ai1z0)(s))ds,(iN).

    If we denote zi(t)=(Aiz0)(t), (iN), then it is clear that

    limmzizCπmδ,θ[,t1]=0. (3.31)

    If there exists at least one rk0 in the initial condition (3.7), then we can choose z0(t)=z0(t), where z0(t) is defined by (3.28).

    E) Next, we prove the existence of a unique solution zCπ[t1,r] to (3.11) on the interval [t1,r].

    Moreover, if we consider the interval [t1,r], we can express Eq (3.11) in the following manner:

    z(t)=z01(t)+1π(t)Γ(δ)tt1(θ(t)θ(s))δ1π(s)θ(s)f(s,z(s))ds, (3.32)

    where z01(t) is defined by

    z01(t)=mj=1rjΓ(δj+1)(θ(t)θ())δjπ1(t)+1π(t)Γ(δ)t1(θ(t)θ(s))δ1π(s)θ(s)κ(s,z(s))ds,

    is a known function.

    We note that z01(t)Cπ[t1,r]. Because, z0(t)Cπ[t1,r]. Also, by hypothesis κ(t,z(t))Cπmδ,θ[,r] for any z(t)Cπmδ,θ[,r], then, κ(t,z(t))Cπ[t1,r], therefore, we can apply Lemma 3.7, we have δ,θ(t)+,π(t)κ(t,z(t))Cπ[t1,r]. Thus, z01(t)Cπ[t1,r].

    We consider the interval [t1,t2], where t2=t1+ε1 and ε1>0 are such that t2(t1,r]. We also use Banach fixed point theorem for the space Cπ[t1,t2], where t2 satisfies

    ξ2=L(θ(t2)θ(t1))δδΓ(δ)<1. (3.33)

    The space Cπ[t1,t2] is a complete metric space, with the distance given by

    δ(z1,z2)=z1z2Cπ[t1,t2]=maxt[t1,t2]|π(t)[z1(t)z2(t)]|.

    Also, we can rewrite the integral equation (3.32) in the form:

    z(t)=(Az)(t),

    where A is the operator given by

    (Az)(t)=z01(t)+1Γ(δ)π(t)tt1(θ(t)θ(s))δ1θ(s)π(s)κ(s,z(s))ds. (3.34)

    To apply Theorem 2.1, we have to prove the following:

    E1) If z(t)Cπ[t1,t2], then (Az)(t)Cπ[t1,t2].

    E2) For any z1,z2Cπ[t1,t2] the following estimate holds:

    Az1Az2Cπ[t1,t2]ξ2z1z2Cπ[t1,t2],ξ2=L(θ(t2)θ(t1))δδΓ(δ). (3.35)

    Similarly, by hypothesis κ(t,z(t))Cπmδ,θ[,r] for any z(t)Cπmδ,θ[,r], then, by Lemma 3.7, the integral in the right-hand side of (3.34) also belongs to Cπ[t1,t2], and hence (Az)(t)Cπ[t1,t2]. Now, we prove the estimate in (3.35), using the Lipschitz condition and applying Lemma 3.7, we find

    Az1Az2Cπ[t1,t2]=δ,θ(t)+,π(t)(κ(t,z1(t))κ(t,z2(t)))Cπ[t1,t2](ψ(t2)ψ(t1))δδΓ(δ)κ(t,z1(t))κ(t,z2(t))Cπ[t1,t2]L(θ(t2)θ(t1))δδΓ(δ)z1z2Cπ[t1,t2]=ξ2z1z2Cπ[t1,t2],

    which yields the estimate (3.35). This, together with our assumption 0<ξ2<1, shows that A is a contraction and therefore from Theorem 2.1, there exists a unique solution z1(t)Cπ[t1,t2] to (3.11) on the interval [t1,t2]. Further, Theorem 2.1 guarantees that this solution z1(t) is the limit of the convergent sequence (Aiz01)(t):

    limiAiz01z1Cπ[t1,t2]=0, (3.36)

    where z01(t) is any function in Cπ[t1,t2].

    If z0(t)0 on [t1,t2], then we can take z01(t)=z0(t) with z0(t) defined by (3.28). The last relation can be rewritten in the form

    limiziz1Cπ[t1,t2]=0, (3.37)

    where

    zi(t)=(Aiz01)(t)=z01(t)+1π(t)Γ(δ)tt1(θ(t)θ(s))δ1π(s)θ(s)κ(s,(Ai1z01)(s))ds,(iN). (3.38)

    E3) Next, if t2r, we consider the interval [t2,t3], where t3=t2+ε2,ε2>0, such that t3r and

    ξ3=L(θ(t3)θ(t2))δδΓ(δ)<1.

    By using the same arguments as above, we conclude that there exists a unique solution z2(t)Cπ[t2,t3] to (3.11) on the interval [t2,t3]. If t3r, repeating the above process, then we find that there exists a unique solution z(t) to (3.11), z(t)=zk(t), and zk(t)Cπ[tk1,tk] for k=1,...,M, where a=t0<t1<...<tM=r and

    ξk=L(θ(tk)θ(tk1))δδΓ(δ)<1.

    Consequently, there exists a unique solution z(t)Cπ[t1,r] to (3.11) on the interval [t1,r]. Using Lemma 3.6, we can conclude that there exists a unique solution z(t)Cπmδ,θ[,r] to the Volterra integral equation (3.11) on the whole interval [,r]. Therefore, z(t)Cπmδ,θ[,r] is the unique solution to the Cauchy-type problems (3.6)(3.7).

    Step 2. Finally, it remains to show that such a unique solution is actually in Cδ,πmδ,θ[,r]. By (3.4), it is sufficient to prove that (Dδ,θ(t)+,π(t)z)(t)Cπmδ,θ[,r]. By the above proof, the solution z(t)Cπmδ,θ[,r] is a limit of the sequence zi(t), where zi(t)=(Aiz0)(t)Cπmδ,θ[,r]:

    limizizCπmδ,θ[,r]=0, (3.39)

    with the choice of certain z0 on each [,t1],...,[tM1,r].

    If z0(t)0, then we can take z0(t)=z0(t). Hence, by using (3.6) and (2.3), we have

    Dδ,θ(t)+,π(t)ziDδ,θ(t)+,π(t)zCπmδ,θ[,r]=κ(t,zi(t))κ(t,z(t))Cπmδ,θ[,r]Lziz(t)Cπmδ,θ[,r]. (3.40)

    In virtue of (3.39) and (3.40), it can be said that

    limiDδ,θ+,π(t)ziDδ,θ+,π(t)zCπmδ,θ[,r]=0.

    By hypothesis, (Dδ,θ(t)+,π(t)zi)(t)=κ(t,zi1(t)) and κ(t,z(t))Cπmδ,θ[,r] for any z(t)Cπmδ,θ[,r], we have (Dδ,θ(t)+,π(t)zi)(t)Cπmδ,θ[,r]. Hence (Dδ,θ(t)+,π(t)z)(t)Cπmδ,θ[,r]. Consequently, z(t)Cπmδ,θ[,r] is the unique solution to the problems (3.6)(3.7). The proof is complete.

    Corollary 3.9. Let 0<δ<1, let B be an open set in R and let κ:(,r]×BR be a function such that κ(t,z(t))Cπ1δ,θ[,r] for any z(t)Cπ1δ,θ[,r] and (2.3) holds. Then there exists a unique solution z(t) to the Cauchy type problem (3.12) in the space Cδ,π1δ,θ[,r].

    When 0<δ<1, the result of Corollary 3.9 remains true for the following weighted Cauchy type problem (3.13) with CR:

    (Dδ,θ(t)+,π(t)z)(t)=κ(t,z(t));limt+[(θ(t)θ())1δπ(t)z(t)]=C,(0<δ<1). (3.41)

    Its proof is based on the following lemma assertion:

    Lemma 3.10. Let 0<δ<1 and let z(t)Cπ1δ,θ[,r].

    S1) If there exists a limit

    limt+[(θ(t)θ())1δπ(t)z(t)]=C,CR, (3.42)

    then there also exists a limit

    (π1δ,θ(t)+,π(t)z)(+)=limt+(π1δ,θ(t)+,π(t)z)(t)=CΓ(δ). (3.43)

    S2) If there exists a limit

    limt+(π1δ,θ(t)+,π(t)z)(t)=r,rR (3.44)

    and if there exists the limit limt+[(θ(t)θ())1δπ(t)z(t)], then

    limt+[(θ(t)θ())1δπ(t)z(t)]=rΓ(δ). (3.45)

    Proof. Choose an arbitrary ε>0. According to (3.42), there exists η=η(ε)>0 such that

    |(θ(t)θ())1δπ(t)z(t)C|<εΓ(δ). (3.46)

    For <t<+η.By using (2.8), we have

    Γ(δ)=(π1δ,θ(t)+,π(t)(π1(t)(θ(t)θ())δ1))(t),0<δ<1. (3.47)

    Using this equality and (2.4), we obtain

    |(ω1δ,θ(t)+,π(t)z)(t)CΓ(δ)|=|(π1δ,θ(t)+,π(t)z)(t)C(π1δ,θ(t)+,π(t)(π1(t)(θ(t)θ())δ1))(t)|1Γ(1δ)t(θ(t)θ(s))δθ(s)|π(s)z(s)C(θ(s)θ())δ1|ds1Γ(1δ)t(θ(t)θ(s))δθ(s)(θ(s)θ())δ1|(θ(s)θ())1δπ(s)z(s)C|ds.

    Now, by making use of (3.46) and the formula (3.47), we have

    |(π1δ,θ(t)+,π(t)z)(t)CΓ(δ)|επ(t)Γ(δ)(1δ,θ(t)+,π(t)(π1(t)(θ(t)θ())δ1))(t)=ε, (3.48)

    which proves the assertion (S1) of Lemma 3.10.

    Assume that the limit in (3.45) is equal to C :

    limt+[(θ(t)θ())1δπ(t)z(t)]=C.

    Consequently, based on (S1), we have

    (π1δ,θ(t)+,π(t)z)(+)=limt+(π1δ,θ(t)+,π(t)z)(t)=CΓ(δ),

    and hence, by (3.44), C=rΓ(δ), which proves (3.45).

    Now, by Corollary 3.9 and Lemma 3.10, we deduce the existence and uniqueness result for the weighted Cauchy type problem (3.41).

    Theorem 3.11. Let 0<δ<1, let B be an open set in R and let κ:(,r]×BR be a function such that κ(t,z(t))Cπ1δ,θ[,r] for any z(t)Cπ1δ,θ[,r] and the Lipschitzian condition (2.3) holds.

    Then there exists a unique solution z(t) to the weighted Cauchy type problem (3.41) in the space Cδ,π1δ,θ[,r].

    Proof. If z(t) fulfills the conditions (3.41), then, according to Lemma 3.10 (S1), z(t) also satisfies the conditions (3.12) with r=CΓ(δ):

    (Dδ,θ(t)+,π(t)z)(t)=κ(t,z(t))(0<δ<1),(π1δ,θ(t)+,π(t)z)(+)=CΓ(δ)R. (3.49)

    By Corollary 3.9, there exists a unique solution z(t)Cδ,π1δ,θ[,r] to this problem. Furthermore, by Lemma 3.10 (S2), z(t) is also a unique solution to the weighted Cauchy problem (3.41).

    We consider the initial value problem (IVP) for the fractional differential equation given by

    Dδ,θ(t)π(t)z=κ(t,z(t)),z(t0)=z0=z(t)π(t)(θ(t)θ(t0))1δ|t=t0,t0tH,H>0, (3.50)

    κC([t0,H]×R,R), Dδ,θ(t)π(t))z is the weighted Riemann Liouville fractional derivative of order δ of z, such that 0<δ<1.

    Definition 3.1. Let 0<δ<1 and β=1δ. We denote by Cπβ,θ([,r],R), the function space

    Cπβ,θ([t0,H],R)={zCπ((t0,H],R),(θ(t)θ(t0))βπ(t)z(t)C([t0,H],R)}. (3.51)

    Definition 3.2. (Locally Hölder continuous with respect to θ)

    Let κ be a real function. We say that κ is locally Hölder continuous with respect to θ at a point t1, with exponent ϑ(0,1], if there exist a real number N>0, such that for all h>0, small enough, we have

    |κ(t1)κ(t)|N|θ(t1)θ(t)|ϑt]t1h,t1+h[dom(κ),h>0, (3.52)

    where θ is a strictly increasing C1 function.

    A function κ is simply said to be locally Hölder continuous with respect to θ, if it is locally Hölder continuous with respect to θ at all points in dom(κ).

    Lemma 3.12. Let 0<δ,β<1, let θC1 is a strictly increasing function and π(t)0 for t[,r]. Consider the function

    m(t)=(θ(t)θ())β1π(t)Eδ,β[μ(θ(t)θ())δ],

    where Eδ,μ(.) is the Mttag-Leffler function with two parameters. Then,

    Dδ,θ+πm(t)=μm(t). (3.53)

    Proof. Using the definition of the Mittag Leffler function and Property 2.2, we have

    Dδ,θ(t)+,π(t)m(t)=Dδ,θ(t)+,π(t)[(θ(t)θ())β1π(t)Eδ,β[μ(θ(t)θ())δ]]=Dδ,θ(t)+,π(t)[(θ(t)θ())β1π(t)i=0μi(θ(t)θ())δiΓ(δi+β)]=i=0μiΓ(δi+β)Dδ,θ(t)+,π(t)[(θ(t)θ())δi+β1π(t)]=μ(θ(t)θ())β1π(t)i=1μi1(θ(t)θ())δ(i1)Γ(δ(i1)+β)=μm(t).

    This completes the proof of the lemma.

    Lemma 3.13. Let GCπβ,θ([t0,H],R), such that π is a positive function in L((t0,H)). Assume that G is locally Hölder continuous with respect to θ at t(t0, H] and exponent ϑ>1β. If t satisfies

    G(t)=0andG(t)0fort0tt, (3.54)

    then it follows that

    Dδ,θ(t)π(t)G(t)0, (3.55)

    where 0<δ<1 and β=1δ.

    Proof. From (2.6), it is clear that

    D1,θ(t)π(t)[K(t)π(t)]=1θ(t)π(t)dK(t)dt. (3.56)

    Thus, according to (2.7), we find that

    (Dδ,θ(t)+,π(t)G)(t)=(D1,θ(t)π(t)1δ,θ(t)+,π(t)G)(t)=D1,θ(t)π(t)[1Γ(β)π(t)tt0(θ(t)θ(s))β1θ(s)π(s)G(s)ds]=1Γ(β)π(t)θ(t)ddttt0(θ(t)θ(s))β1θ(s)π(s)G(s)ds,

    we set, K(t)=tt0(θ(t)θ(s))β1θ(s)π(s)G(s)ds.

    Consider the following for a small η>0:

    K(t)K(tη)=tηt0[(θ(t)θ(s))β1(θ(tη)θ(s))β1]θ(s)π(s)G(s)ds+ttη(θ(t)θ(s))β1θ(s)π(s)G(s)ds.=Δ1+Δ2.

    Since t0stη and β1<0, then from (3.54), we obtain

    [(θ(t)θ(s))β1(θ(tη)θ(s))β1]<0andG(s)0.

    Thus implying that Δ10. Therefore,

    K(t)K(tη)ttη(θ(t)θ(s))β1θ(s)π(s)G(s)ds=Δ2.

    Since G(t) is locally Hölder continuous with respect to θ and exponent ϑ, there exists a real number N(t)>0 such that for tηst+η

    N(t)(θ(t)θ(s))ϑG(t)G(s)N(t)(θ(t)θ(s))ϑ,

    where 0<ϑ<1 is such that ϑ>1β. Knowing that π is a positive function, then by (3.54) we have

    Δ2N(t)πLttη(θ(t)θ(s))β1+ϑθ(s)ds=N(t)πL(θ(t)θ(tη))β+ϑβ+ϑ.

    Hence, for sufficiently small η>0

    K(t)K(tη)ηN(t)πLβ+ϑ(θ(t)θ(tη)η)β+ϑηβ+ϑ1.

    Letting η0, we obtain ddtG(t)0, which implies Dδ,θ(t)π(t)G(t)0, and the proof is complete.

    Theorem 3.14. Let Y,ZCπβ,θ([t0,H],R), such that π is a positive function in L((t0,H)) and θC1 be a strictly increasing function on [t0,H], κC([t0,H]×R,R). Assume that Y,Z are locally Hölder continuous with respect to θ for respectively an exponent ϑ1 and ϑ2 in ]0,1] such that min{ϑ1,ϑ2}+β>1 and

    (D1) Dδ,θ(t)π(t)Y(t)κ(t,Y(t)),

    (D2) Dδ,θ(t)π(t)Z(t)κ(t,Z(t)), t0<tH,

    one of the inequalities (D1) or (D2) being strict. Then

    Y0<Z0, (3.57)

    where Y0=Y(t)π(t)(θ(t)θ(t0))1δ|t=t0 and Z0=Z(t)π(t)(θ(t)θ(t0))1δ|t=t0, implies

    Y(t)<Z(t),t0tH. (3.58)

    Proof. Assume that the conclusion (3.58) is not true. Then, since Y0<Z0 and Y(t)π(t)(θ(t)θ(t0))1δ, Z(t)π(t)(θ(t)θ(t0))1δ are continuous functions, there exists a ξ such that t0<ξH

    Y(ξ)=Z(ξ)andY(t)<Z(t)t0t<ξ. (3.59)

    Define G(t)=Y(t)Z(t), t[t0,H]. Then, we find that G(ξ)=0 and G(t)<0t0t<ξ, with GCπβ,θ([t0,H],R). Hence by Lemma 3.13, we obtain

    Dδ,θ(t)π(t)G(ξ)0.

    This gives

    Dδ,θ(t)π(t)Y(ξ)Dδ,θ(t)π(t)Z(ξ).

    Suppose that the inequality (D2) is strict, then we have

    κ(ξ,Y(ξ))Dδ,θ(t)π(t)Y(ξ)Dδ,θ(t)π(t)Z(ξ)>κ(ξ,Z(ξ)),

    which is a contradiction with Y(ξ)=Z(ξ). Hence, the conclusion (3.58) is valid and the proof is complete.

    The next result is for non-strict fractional differential inequalities, which demand a Lipschitz-type condition.

    Theorem 3.15. Assume that the condition of Theorem 3.14 holds with non-strict inequalities (D1) and (D2). Further, assume that κ satisfies the Lipschitz condition

    κ(t,U)κ(t,V)ρ(UV),UVandρ>0. (3.60)

    Then, Y0Z0, implies

    Y(t)Z(t),t0tH. (3.61)

    Proof. For small h, we define

    Zh(t)=Z(t)+hΛ(t), (3.62)

    where Λ(t)=π1(t)(θ(t)θ(t0))δ1Eδ,δ[2ρ(θ(t)θ(t0))δ], with ZhCπβ,θ([t0,H],R).

    It follows from this

    Zh(t)π(t)(θ(t)θ(t0))1δ|t=t0=Z(t)θ(t)(θ(t)θ(t0))1δ|t=t0+hΛ(t)π(t)(θ(t)θ(t0))1δ|t=t0.

    So, we obtain, Z0h=Z0+hΛ0. This leads to

    Z0h>Z0Y0andZh(t)>Z(t). (3.63)

    Next, by applying the Lipschitz condition (3.60) and Lemma 3.12 (with μ=2ρ,β=δ and =t0), we deduce

    Dδ,θ(t)π(t)Zh(t)=Dδ,θ(t)π(t)Z(t)+hDδ,θ(t)π(t)Λ(t)κ(t,Z(t))+2hρΛ(t)>κ(t,Zh(t)ρhΛ(t)+2hρΛ(t)>κ(t,Zh(t)),t0<tH.

    Therefore,

    Dδ,θ(t)π(t)Zh(t)>κ(t,Zh(t)),t0tH.

    In this case, we have made use of the fact that Λ(t) is the linear weighted weighted Riemann-Liouville fractional differential equation

    Dδ,θ(t)π(t)Λ(t)=2ρΛ(t),t0<t1HΛ(t)π(t)(θ(t)θ(t0))1δ|t=t0=Λ0>0.

    Utilizing (3.63), we can apply Theorem 3.14 to Y(t) and Zh(t). As a result, we have

    Y(t)<Zh(t),t[t0,H],ε>0. (3.64)

    By taking the limit as h0, in the above inequality and using (3.62), we deduce that

    Y(t)Z(t),t[t0,H].

    Hence, then the proof is complete.

    In this paper, we establish the equivalence between a nonlinear initial value problem and a Volterra integral equation. Furthermore, we discussed the existence and uniqueness of the solution for this initial value problem, along with specifying the space in which this solution exists. Finally, we obtained estimates on the weighted Riemann-Liouville fractional derivatives at extreme points, which were used to develop the comparison results. This work has opened new horizons for us to expand the theory of comparison for the weighted Caputo fractional operators with respect to another function. Our forthcoming focus will be directed towards these intriguing aspects in the near future.

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

    The author, T. Abdeljawad, would like to thank Prince Sultan University for the support through the TAS research lab. The first author would like to thank Professor T. Abdeljawad for his hospitality at the TAS. research lab. at Prince Sultan University where the work on this article was undertaken, as well as the Operator Theory and PDE Laboratory at the University of El-Oued for its support during this research work.

    All authors declare no conflicts of interest in this paper.



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