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Solvability of product of n-quadratic Hadamard-type fractional integral equations in Orlicz spaces

  • The current study demonstrated and studied the existence of monotonic solutions, as well as the uniqueness of the solutions for a general and abstract form of a product of n-quadratic fractional integral equations of Hadamard-type in Orlicz spaces Lφ. We utilized the analysis of the measure of non-compactness associated with Darbo's fixed-point theorem and fractional calculus to obtain the results.

    Citation: Saud Fahad Aldosary, Mohamed M. A. Metwali. Solvability of product of n-quadratic Hadamard-type fractional integral equations in Orlicz spaces[J]. AIMS Mathematics, 2024, 9(5): 11039-11050. doi: 10.3934/math.2024541

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  • The current study demonstrated and studied the existence of monotonic solutions, as well as the uniqueness of the solutions for a general and abstract form of a product of n-quadratic fractional integral equations of Hadamard-type in Orlicz spaces Lφ. We utilized the analysis of the measure of non-compactness associated with Darbo's fixed-point theorem and fractional calculus to obtain the results.



    The theory of fractional integral and differential equations has a fundamental role in several branches of science, such as economics, biology, engineering, physics, electrical circuits, electro-chemistry, earthquakes, fluid dynamics, traffic models, and viscoelasticity (cf. [1,2,3]).

    Hadamard fractional integral operators were defined by Hadamard in 1892 [4]. These operators have a kernel of logarithmic function of arbitrary order, which is not of convolution type. Consequently, they should be examined separately from the more well-known Caputo and Riemann-Liouville fractional operators. These types of operators have been studied by several researchers in numerous function spaces. (cf. [5,6,7]).

    The present work investigates and establishes the existence theorem as well as the uniqueness of the solution to a general and abstract form of a product of n-quadratic fractional integral equations of Hadamard-type in Orlicz spaces Lφ, which has the form

    y(s)=ni=1(hi(s)+G2i(y)(s)+G1i(y)(s)Γ(αi)s1(logsτ)αi1G3i(y)(τ)τdτ),s[1,e],0<αi<1, (1.1)

    in arbitrary Orlicz spaces Lφ, where Gji,j=1,2,3 are general operators.

    The theory of fractional calculus in Orlicz spaces was studied by O'Neill in 1965 [8], and, subsequently, several interesting articles were published on this topic (see, for example, [9,10,11]).

    Orlicz spaces Lφ are suitable spaces for studying operators with strong nonlinearities (e.g., exponential growth) rather than polynomial growth in Lebesgue spaces Lp,p1, (see [12,13]). These are motivated by some problems in statistical physics and mathematical physics (see [14,15]). In particular, the thermodynamics problem

    y(s)+Ia(s,u)ey(u)du=0,

    contains exponential nonlinearity (cf. [16]).

    Moreover, quadratic integral equations have been applied in astrophysics, radiative transfer theory, or neutron transport [17,18,19]. It should be noted that several kinds of quadratic integral equations have been investigated in Lp spaces [20,21,22] and in Lφ-spaces [12,13,23] using the measure of non-compactness analysis associated with Darbo's fixed-point hypothesis via different sets of assumptions.

    It is useful to study the product of two or more than two operators, as mentioned by Medveˇd and Brestovanská in [24,25]; however, they consider the Banach algebras of continuous functions, which have a different technique in the proof. Since Orlicz spaces are not Banach algebras, we use the methods given in [26,27] to obtain our results.

    In [26], the author proved some fixed point theorems and employed them in examining the solution of the equation

    y(s)=ni=1(gi(s)+saKi(s,τ,y(τ))dτ),

    in some types of ideal spaces like Lp,p>1 and Orlicz spaces Lφ(I),I=[a,b], where φ verifies the Δ2-condition.

    In [27], the existence theorems for the product of n-integral equations operating on n-distinct Orlicz spaces

    y(s)=ni=1(gi(s)+λihi(s,y(s))baKi(s,τ)fi(τ,y(τ))dτ),

    were discussed in Orlicz spaces Lφ([a,b]), for n2, when the function φ verifies the so-called Δ,Δ3, and Δ2-conditions.

    The author in [28] demonstrated and proved some basic theorems for the Riemann-Liouville fractional integral operator and investigated the existence theorems in Lφ-spaces for the equation

    y(s)=y(s)+G(y)(s)s0(sτ)α1Γ(α)f(τ,y(τ))dτ,0<α<1,s[0,d].

    In [29], some basic theorems were demonstrated and proved for the Hadamard fractional order integral operator, and the existence theorems were also investigated for the equation:

    y(s)=G3(y)(s)+G1(y)(s)Γ(α)s1(logsτ)α1G2(y)(τ)τdτ,0<α<1,s[1,e],

    in Orlicz spaces Lφ.

    Basic theorems for the Erdélyi-Kober fractional order integral operator can be found, both demonstrated and proved, in [30], where the existence theorems were also investigated for the following equation:

    y(s)=g(s)+f1(s,y(s))+f2(s,βh1(s,y(s))Γ(α)s0τβ1h2(τ,y(τ))(sβτβ)1αdτ),s[0,d],

    where 0<α<1 and β>0 in both Lp and Lφ spaces.

    This paper is motivated by studying monotonic solutions for a general and abstract form of a product of n-quadratic fractional integral equations of Hadamard-type in Orlicz spaces Lφ. We provide two existence theorems, namely (the existence and the uniqueness of) the solutions for Eq (1.1). The measure of non-compactness and Darbo's fixed point theorem are our main tools for examining the obtained results.

    Let R+=[0,)R=(,) and I=[1,e],e2.718. A function M:[0,)[0,) points to a Young function if

    M(τ)=τ0u(s)dt,  forτ0,

    where u:[0,)[0,) is a left-continuous-increasing function and is neither equal to infinite, nor zero on R+. The functions N and M are referred to the complementary Young functions, if M(y)=supz0(yzN(y)). Furthermore, if M is finite-valued with limτ0M(τ)τ=0, limτM(τ)τ=, and M(τ)>0 if τ>0 (M(τ)=0τ=0), then M is said to be an N-function.

    The Orlicz space LM=LM(I) is the space of all measurable functions y:IR with the Luxemburg norm

    yM=infϵ>0{IM(y(τ)ϵ)dτ1}.

    Let EM=EM(I) contain the set of all bounded functions of LM and have absolutely continuous norms.

    Definition 2.1. [31] The Hadamard-type fractional integral of an integrable function y of order α>0 is given by

    Jαy(s)=1Γ(α)s1(logsτ)α1y(τ)τdτ,s>1,α>0,

    where Γ(α)=0essα1ds.

    Proposition 2.1. [5] The operator Jα maps a.e. nondecreasing and nonnegative functions to functions of similar types.

    Lemma 2.1. [29] Assume, that M and N are complementary N-functions with s0M(τα1)dτ<,α(0,1). Moreover, suppose that φ is N-function, where

    k(s)=1ϵ11αsϵ11α0M(τα1)dτEφ

    for a.e. τI and ϵ>0, then the operator Jα:LNLφ is continuous and verifying

    Jαyφ2Γ(α)kφyN.

    The following lemma characterizes the product of the operators in Lφ:

    Lemma 2.2. ([32, Theorem 1]) Let n2. If φ and φi,i=1,n are arbitrary N-functions, then the following conditions are equivalent:

    (1) For every uiLφi, ni=1uiLφ.

    (2) There exists a constant K>0 s.t.

    ni=1uiφKni=1uiφi,

    for every uiLφi,i=1,2,n.

    (3) There exists a constant C>0 s.t.

    ni=1φ1i(s)Cφ1(s)

    for every s0.

    (4) There exists a constant C>0 s.t. si0,i=1,n,

    φ(ni=1siC)ni=1φi(si).

    Let S=S(I) refer to all Lebesgue measurable functions on the interval I. The set S concerning the metric

    d(y,z)=infϵ>0[ϵ+meas{τ:|y(τ)z(τ)|ϵ}]

    becomes a complete space, where "meas" points to the Lebesgue measure in R. The convergence w.r. to d is identical to the convergence in measure on I (cf. Proposition 2.14 in [34]). We call the compactness in S by "compactness in measure".

    Lemma 2.3. [23] Let YLM be a bounded set, and there is a family (Ωc)0ce1I s.t. meas Ωc=c for every c[1,e], and for every yY,

    y(s1)y(s2),(s1Ωc,s2Ωc).

    Thus, Y represents a compact in measure set in LM.

    Definition 2.2. [23] Let YLM be bounded, then

    βH(Y)=inf{r>0:a finite subset Z of LM s.t.YZ+Br},

    is called the Hausdorff measure of non-compactness (MNC), where Br={mLM:mMr}.

    The measure of equi-integrability c of the set YLM is given by

    c(Y)=limϵ0supmesDϵsupyYyχDLM,

    where ϵ>0 and χD is the characteristic function of DI (cf. [33] or [34]).

    Lemma 2.4. [23,33] Let YEM provide a bounded and compact in measure set, then we have

    βH(Y)=c(Y).

    Rewrite Eq (1.1) as

    y=B(y)=ni=1Bi(y)=ni=1(hi+G2i(y)+Ui(y)),

    where

    Ui(y)=G1i(y)Ai(y),Ai(y)=JαiiG3i(y),

    s.t. Jαii is as in Definition 2.1 and Gji(y) are general operators that act on some different Orlicz spaces for j=1,2,3 and i=1,,n.

    Next, we discuss the existence of Lφ solutions for Eq (1.1).

    For i=1,,n, suppose that φ,φi,φ1i,φ2i are N-functions and that Ni,Mi are complementary N-functions with s0Mi(ταi1)dτ<,αi(0,1), and consider the assumptions:

    (N1) There exists a constant K>0 s.t. for every uiLφi, and we have ni=1uiφKni=1uiφi.

    (N2) There exists a constant k1i>0 such that for every u1Lφ1i and u2Lφ2i, we get u1u2φik1iu1φ1iu2φ2i.

    (N3) The functions hiEφi are a.e. nondecreasing on the interval I.

    (N4) G1i:LφLφ1i take continuously EφEφ1i, the operators G2i:LφLφi take continuously EφEφi, and the operators G3i:LφLNi take continuously EφENi.

    (N5) There exist positive functions g1iLφ1i,g2iLφi,g3iLNi s.t. for sI, |Gji(y)(s)|gji(s)yφ; and Gji,j=1,2,3, takes the set of all a.e. nondecreasing functions to functions of similar properties. Moreover, suppose that for any yEφ, we have G1i(y)Eφ1i,G2i(y)Eφi, and G3i(y)ENi.

    (N6) Assume that ki(s)=1ϵ11αisϵ11αi0Mi(ταi1)dτEφ2i for ϵ>0 and sI.

    (N7) Suppose that r>0 and Li>0 verify

    mi=1Li=Kni=1(hiφi+g2iφir+2k1ikiφ2iΓ(αi)g1iφ1ig3iNir2)r (3.1)

    and

    ni=1(g2iφi+2k1ikiφ2irΓ(αi)g1iφ1ig3iNi)<1rnK.

    Theorem 3.1. Let the assumptions (N1)–(N7) be verified, then there exists a solution yEφ of (1.1) that is a.e. nondecreasing on I.

    Proof. Ⅰ. In what follows, put i=1,,n. First, Lemma 2.1 implies that each Jαi:LNiLφ2i is continuous. By assumption (N4), we have that the operators G1i:EφEφ1i,G2i:EφEφi, and G3i:EφENi are continuous, then Ai=JαiiG3i:EφEφ2i are continuous. By assumption (N2) and the Hölder inequality, we get that Ui=G1iAi:EφEφi, and they are continuous. By using assumptions (N3), we have the operators Bi:EφEφi. Finally, assumption (N1) and the Hölder inequality give us that B=ni=1Bi:EφEφ is continuous.

    Ⅱ. We shall establish the ball Br(Eφ)={yLφ:yφr}, where r is defined in assumption (N7).

    Let yBr(Eφ), and by recalling Lemma 2.1, we have

    Bi(y)φihiφi+G2i(y)φi+Uiyφihiφi+g2iyφφi+G1i(y)Ai(y)φihiφi+g2iφiyφ+k1iG1i(y)φ1iAi(y)φ2ihiφi+g2iφiyφ+k1ig1iyφφ1iJαiiG3i(y)φ2ihiφi+g2iφiyφ+k1ig1iφ1iyφ2Γ(αi)kiφ2ig3iyφNihiφi+g2iφiyφ+k1ig1iφ1iyφ2Γ(αi)kiφ2ig3iNiyφhiφi+g2iφiyφ+2k1ikiφ2iΓ(αi)g1iφ1ig3iNiy2φhiφi+g2iφir+2k1ikiφ2iΓ(αi)g1iφ1ig3iNir2.

    Therefore, utilizing assumption (N1), we have

    B(y)φKni=1Bi(y)φiKni=1(hiφi+g2iφir+2k1ikiφ2iΓ(αi)g1iφ1ig3iNir2)r.

    By using assumption (N7), we have that B:Br(Eφ)Eφ is continuous.

    Ⅲ. Let QrBr(Eφ) contain the a.e. nondecreasing functions of I. The set Qr is a closed, nonempty, bounded, and convex set in Lφ; see [23]. Furthermore, Qr is compact in measure (thanks to Lemma 2.3).

    Ⅳ. Next, we discuss the monotonicity for the operator B. Take yQr, then y is a.e. nondecreasing on I. By assumption (N5), the operators Gji(y),j=1,2,3 are a.e. nondecreasing on I, by Proposition, 2.1 the operator Ai is of the same type, then the operators Ui(y)=G1i(y)Ai(y) are a.e. nondecreasing on I, and by using assumption (N3), we have that B:QrQr is continuous.

    Ⅴ. We will demonstrate that B is a contraction w.r. to the MNC. Suppose that YQr. For yY and for a set DI,ϵ>0, measDϵ. By assumption (N4), we have

    G1i(y)χDφ1iG1i(yχD)φ1ig1iyχDφφ1ig1iφ1iyχDφ

    and, similarly,

    G2i(y)χDφig2iφiyχDφ,

    then we have

    Bi(y)χDφihiχDφi+G2i(y)χDφi+Ui(y)χDφihiχDφi+G2i(yχD)φi+G1i(y)Ai(y)χDφihiχDφi+g2iφiyχDφ+k1iG1i(y)χDφ1iAi(y)χDφ2ihiχDφi+g2iφiyχDφ+k1iG1i(yχD)φ1iAi(y)φ2ihiχDφi+g2iφiyχDφ+2k1iΓ(αi)g1iφ1iyχDφkiφ2iG3i(y)NihiχDφi+g2iφiyχDφ+2k1iΓ(αi)g1iφ1iyχDφkiφ2ig3iNiyφhiχDφi+g2iφiyχDφ+2k1ikiφ2irΓ(αi)g1iφ1ig3iNiyχDφ.

    Therefore,

    B(y)χDφKni=1Bi(y)χDφiKni=1(hiχDφi+g2iφiyχDφ+2k1ikiφ2irΓ(αi)g1iφ1ig3iNiyχDφ).

    Since hiEφi, we obtain

    limε0{supmeasDε[supyY{hiχDφi}]}=0.

    From the definition of c(y), we have

    c(B(Y))rnKni=1(g2iφi+2k1ikiφ2irΓ(αi)g1iφ1ig3iNi)c(Y),

    where yχDnφ=yχDn1φyχDφrnyχDφ.

    Since YQr is a bounded and compact in measure subset of Eφ, we can employ Lemma 2.4 to get

    βH(B(Y))rnKni=1(g2iφi+2k1ikiφ2irΓ(αi)g1iφ1ig3iNi)βH(Y).

    Since ni=1(g2iφi+2k1ikiφ2irΓ(αi)g1iφ1ig3iNi)<1rnK, we have finished (cf. [26]).

    Remark 3.1. If the N-functions Ni,i=1,,n verify the Δ-condition, then Theorem 3.1 is valid on the unite balls B1(Eφ)={yLφ:yφ1}. Furthermore, if they verify the Δ3 or Δ2-conditions, then Theorem 3.1 is valid on the whole Eφ (cf. [13,23]).

    Now, we discuss the uniqueness of Eq (1.1).

    Theorem 3.2. Let assumption (N1)–(N7) be verified. If

    C=nj=1[K(g2jφj+4k1jrkjφ2jΓ(αj)g1jφijg3jNj)ni=1,ijLi]<1,

    where r and Li are defined in assumption (N7), then Eq (1.1) has a unique solution yLφ in Qr.

    Proof. Let y and z be any two different solutions of Eq (1.1), then we obtain

    |yz|=|ni=1Bi(y)ni=1Bi(z)||ni=1Bi(y)B1(z)ni=2Bi(y)|+|B1(z)ni=2Bi(y)B1(z)B2(z)ni=3Bi(y)|++|Bn(y)n1i=1Bi(z)ni=1Bi(z)||B1(y)B1(z)|ni=2|Bi(y)|+|B1(z)||B2(y)B2(z)|ni=3|Bi(y)|++|Bn(y)Bn(z)|n1i=1|Bi(z)|.

    Therefore,

    yzφKB1(y)B1(z)φ1ni=2Bi(y)φi+KB1(z)φ1B2(y)B2(z)φ2ni=3Bi(y)φi+...+KBn(y)Bn(z)φnn1i=1Bi(z)φi. (3.2)

    To calculate the above inequality, we need the following estimation. For j=1,,n, and by using Lemma 2.1, we have

    Bj(y)Bj(z)φjG2j(y)G2j(z)φj+G1j(y)Aj(y)G1j(z)Aj(z)φjg2jyφg2jzφφj+G1j(y)Aj(y)G1j(z)Aj(y)φj+G1j(z)Aj(y)G1j(z)Aj(z)φjg2j|yφzφ|φj+k1jG1j(y)G1j(z)φ1jAj(y)φ2j+k1jG1j(z)φ1jAj(y)Aj(z)φ2jg2jφjyzφ+k1jg1j|yφzφ|φ1jJαjjG3j(y)φ2j+k1jg1jzφφ1jJαjjG3j(y)JαjjG3j(z)φ2jg2jφjyzφ+k1jg1jφ1jyzφ2Γ(αi)kjφ2jg3jNjyφ+k1jg1jφ1jzφ2Γ(αj)kjφ2jg3jNjyzφ(g2jφj+4k1jrkjφ2jΓ(αj)g1jφ1jg3jNj)yzφ. (3.3)

    By substituting from (3.1) and (3.3) in (3.2), we obtain

    yzφ[K(g21φ1+4k11rk1φ21Γ(α1)g11φ11g31N1)ni=2Li+KL1(g22φ2+4k12rk2φ22Γ(α2)g12φ12g32N2)ni=3Li+...+K(g2nφn+4k1nrknφ2nΓ(αn)g1nφ1ng3nNn)n1i=1Li]yzφ=Cyzφ.

    Since C<1, we get y=z (a.e.), and we have finished.

    We need to provide some examples to demonstrate our results.

    Example 4.1. Put the N-functions Mi(u)=Ni(u)=u2 and φ2i(u)=exp|u||u|1. We shall show that Jαii:LNiLφ2i,i=1,,n are continuous, and Lemma 2.1 is verified.

    Indeed: For s[1,e] and any αi(0,1), we have

    ki(s)=s0Mi(ταi1)dτ=s0τ2αi2dτ=s2αi12αi1.

    Moreover,

    e1φ2i(ki(s))dτ=e1(es2αi12αi1s2αi12αi11)ds<.

    Thus for yLNi, we get that Jαii:LNiLφ2i is continuous.

    Remark 4.1. For more details and information about the acting and continuity assumptions of Gi(y)=gi(s)y(s), (see our assumption (N5) and [15, Theorem 18.2]).

    Example 4.2. Let Gji(y)(s)=gi(s)y(s),j=1,2,3, and i=1,n, then we have

    y(s)=ni=1(hi(s)+g2i(s)y(s)+g1i(s)y(s)s1(logsτ)αi1g3i(τ)y(τ)τdτ),αi(0,1),s[1,e],

    which provides a special case of Eq (1.1).

    The current study demonstrates and studies two existence theorems, namely, (the existence and the uniqueness) the monotonic solutions for a general and abstract form of a product of n-quadratic Hadamard-type fractional integral equations in Orlicz spaces Lφ. The measure of non-compactness associated with Darbo's fixed-point theorem and fractional calculus are the main tools used to obtain our results in Lφ-spaces. For the upcoming work in this direction, we will look for some numerical solutions for similar problems in different function spaces.

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

    This study is supported via funding from Prince Sattam bin Abdulaziz University project number (PSAU/2024/R/1445).

    The authors declare that there are no conflicts of interest regarding the publication of this article.



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