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)=n∏i=1(hi(s)+G2i(y)(s)+G1i(y)(s)Γ(αi)⋅∫s1(logsτ)αi−1G3i(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,p≥1, (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)=n∏i=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)=n∏i=1(gi(s)+λi⋅hi(s,y(s))⋅∫baKi(s,τ)fi(τ,y(τ))dτ), |
were discussed in Orlicz spaces Lφ([a,b]), for n≥2, 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(s−τ)α−1Γ(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)α−1G2(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)⋅∫s0τβ−1h2(τ,y(τ))(sβ−τβ)1−αdτ),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],e≈2.718. A function M:[0,∞)→[0,∞) points to a Young function if
M(τ)=∫τ0u(s)dt, forτ≥0, |
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)=supz≥0(yz−N(y)). Furthermore, if M is finite-valued with limτ→0M(τ)τ=0, limτ→∞M(τ)τ=∞, and M(τ)>0 if τ>0 (M(τ)=0⟺τ=0), then M is said to be an N-function.
The Orlicz space LM=LM(I) is the space of all measurable functions y:I→R with the Luxemburg norm
‖y‖M=infϵ>0{∫IM(y(τ)ϵ)dτ≤1}. |
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)α−1y(τ)τdτ,s>1,α>0, |
where Γ(α)=∫∞0e−ssα−1ds.
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(τα−1)dτ<∞,α∈(0,1). Moreover, suppose that φ is N-function, where
k(s)=1ϵ11−α∫sϵ11−α0M(τα−1)dτ∈Eφ |
for a.e. τ∈I and ϵ>0, then the operator Jα:LN→Lφ is continuous and verifying
‖Jαy‖φ≤2Γ(α)‖k‖φ‖y‖N. |
The following lemma characterizes the product of the operators in Lφ:
Lemma 2.2. ([32, Theorem 1]) Let n≥2. If φ and φi,i=1,⋯n are arbitrary N-functions, then the following conditions are equivalent:
(1) For every ui∈Lφi, ∏ni=1ui∈Lφ.
(2) There exists a constant K>0 s.t.
‖n∏i=1ui‖φ≤Kn∏i=1‖ui‖φi, |
for every ui∈Lφi,i=1,2,⋯n.
(3) There exists a constant C>0 s.t.
n∏i=1φ−1i(s)≤Cφ−1(s) |
for every s≥0.
(4) There exists a constant C>0 s.t. ∀si≥0,i=1,⋯n,
φ(∏ni=1siC)≤n∑i=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 Y⊂LM be a bounded set, and there is a family (Ωc)0≤c≤e−1⊂I s.t. meas Ωc=c for every c∈[1,e], and for every y∈Y,
y(s1)≥y(s2),(s1∈Ωc,s2∉Ωc). |
Thus, Y represents a compact in measure set in LM.
Definition 2.2. [23] Let ∅≠Y⊂LM be bounded, then
βH(Y)=inf{r>0:∃a finite subset Z of LM s.t.Y⊂Z+Br}, |
is called the Hausdorff measure of non-compactness (MNC), where Br={m∈LM:‖m‖M≤r}.
The measure of equi-integrability c of the set Y∈LM is given by
c(Y)=limϵ→0supmesD≤ϵsupy∈Y‖y⋅χD‖LM, |
where ϵ>0 and χD is the characteristic function of D⊂I (cf. [33] or [34]).
Lemma 2.4. [23,33] Let ∅≠Y⊂EM provide a bounded and compact in measure set, then we have
βH(Y)=c(Y). |
Rewrite Eq (1.1) as
y=B(y)=n∏i=1Bi(y)=n∏i=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(ταi−1)dτ<∞,αi∈(0,1), and consider the assumptions:
(N1) There exists a constant K>0 s.t. for every ui∈Lφi, and we have ‖∏ni=1ui‖φ≤K∏ni=1‖ui‖φi.
(N2) There exists a constant k1i>0 such that for every u1∈Lφ1i and u2∈Lφ2i, we get ‖u1u2‖φi≤k1i‖u1‖φ1i‖u2‖φ2i.
(N3) The functions hi∈Eφi are a.e. nondecreasing on the interval I.
(N4) G1i:Lφ→Lφ1i take continuously Eφ→Eφ1i, the operators G2i:Lφ→Lφi take continuously Eφ→Eφi, and the operators G3i:Lφ→LNi take continuously Eφ→ENi.
(N5) There exist positive functions g1i∈Lφ1i,g2i∈Lφi,g3i∈LNi s.t. for s∈I, |Gji(y)(s)|≤gji(s)‖y‖φ; 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 y∈Eφ, we have G1i(y)∈Eφ1i,G2i(y)∈Eφi, and G3i(y)∈ENi.
(N6) Assume that ki(s)=1ϵ11−αi∫sϵ11−αi0Mi(ταi−1)dτ∈Eφ2i for ϵ>0 and s∈I.
(N7) Suppose that ∃r>0 and Li>0 verify
m∏i=1Li=Kn∏i=1(‖hi‖φi+‖g2i‖φi⋅r+2k1i‖ki‖φ2iΓ(αi)‖g1i‖φ1i‖g3i‖Ni⋅r2)≤r | (3.1) |
and
n∏i=1(‖g2i‖φi+2k1i‖ki‖φ2i⋅rΓ(αi)‖g1i‖φ1i‖g3i‖Ni)<1rnK. |
Theorem 3.1. Let the assumptions (N1)–(N7) be verified, then there exists a solution y∈Eφ 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:LNi→Lφ2i is continuous. By assumption (N4), we have that the operators G1i:Eφ→Eφ1i,G2i:Eφ→Eφi, and G3i:Eφ→ENi are continuous, then Ai=JαiiG3i:Eφ→Eφ2i are continuous. By assumption (N2) and the Hölder inequality, we get that Ui=G1i⋅Ai:Eφ→Eφi, and they are continuous. By using assumptions (N3), we have the operators Bi:Eφ→Eφi. Finally, assumption (N1) and the Hölder inequality give us that B=∏ni=1Bi:Eφ→Eφ is continuous.
Ⅱ. We shall establish the ball Br(Eφ)={y∈Lφ:‖y‖φ≤r}, where r is defined in assumption (N7).
Let y∈Br(Eφ), and by recalling Lemma 2.1, we have
‖Bi(y)‖φi≤‖hi‖φi+‖G2i(y)‖φi+‖Uiy‖φi≤‖hi‖φi+‖g2i⋅‖y‖φ‖φi+‖G1i(y)⋅Ai(y)‖φi≤‖hi‖φi+‖g2i‖φi‖y‖φ+k1i‖G1i(y)‖φ1i⋅‖Ai(y)‖φ2i≤‖hi‖φi+‖g2i‖φi‖y‖φ+k1i‖g1i⋅‖y‖φ‖φ1i⋅‖JαiiG3i(y)‖φ2i≤‖hi‖φi+‖g2i‖φi‖y‖φ+k1i‖g1i‖φ1i‖y‖φ2Γ(αi)‖ki‖φ2i‖g3i⋅‖y‖φ‖Ni≤‖hi‖φi+‖g2i‖φi‖y‖φ+k1i‖g1i‖φ1i‖y‖φ2Γ(αi)‖ki‖φ2i‖g3i‖Ni‖y‖φ≤‖hi‖φi+‖g2i‖φi‖y‖φ+2k1i‖ki‖φ2iΓ(αi)‖g1i‖φ1i‖g3i‖Ni‖y‖2φ≤‖hi‖φi+‖g2i‖φi⋅r+2k1i‖ki‖φ2iΓ(αi)‖g1i‖φ1i‖g3i‖Ni⋅r2. |
Therefore, utilizing assumption (N1), we have
‖B(y)‖φ≤Kn∏i=1‖Bi(y)‖φi≤Kn∏i=1(‖hi‖φi+‖g2i‖φi⋅r+2k1i‖ki‖φ2iΓ(αi)‖g1i‖φ1i‖g3i‖Ni⋅r2)≤r. |
By using assumption (N7), we have that B:Br(Eφ)→Eφ is continuous.
Ⅲ. Let Qr⊂Br(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 y∈Qr, 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:Qr→Qr is continuous.
Ⅴ. We will demonstrate that B is a contraction w.r. to the MNC. Suppose that ∅≠Y⊂Qr. For y∈Y and for a set D⊂I,ϵ>0, measD≤ϵ. By assumption (N4), we have
‖G1i(y)⋅χD‖φ1i≤‖G1i(y⋅χD)‖φ1i≤‖g1i⋅‖y⋅χD‖φ‖φ1i≤‖g1i‖φ1i‖y⋅χD‖φ |
and, similarly,
‖G2i(y)⋅χD‖φi≤‖g2i‖φi‖y⋅χD‖φ, |
then we have
‖Bi(y)⋅χD‖φi≤‖hi⋅χD‖φi+‖G2i(y)⋅χD‖φi+‖Ui(y)⋅χD‖φi≤‖hi⋅χD‖φi+‖G2i(y⋅χD)‖φi+‖G1i(y)⋅Ai(y)⋅χD‖φi≤‖hi⋅χD‖φi+‖g2i‖φi‖y⋅χD‖φ+k1i‖G1i(y)⋅χD‖φ1i⋅‖Ai(y)⋅χD‖φ2i≤‖hi⋅χD‖φi+‖g2i‖φi‖y⋅χD‖φ+k1i‖G1i(y⋅χD)‖φ1i⋅‖Ai(y)‖φ2i≤‖hi⋅χD‖φi+‖g2i‖φi‖y⋅χD‖φ+2k1iΓ(αi)‖g1i‖φ1i‖y⋅χD‖φ‖ki‖φ2i‖G3i(y)‖Ni≤‖hi⋅χD‖φi+‖g2i‖φi‖y⋅χD‖φ+2k1iΓ(αi)‖g1i‖φ1i‖y⋅χD‖φ‖ki‖φ2i‖g3i‖Ni‖y‖φ≤‖hi⋅χD‖φi+‖g2i‖φi‖y⋅χD‖φ+2k1i‖ki‖φ2i⋅rΓ(αi)‖g1i‖φ1i‖g3i‖Ni‖y⋅χD‖φ. |
Therefore,
‖B(y)⋅χD‖φ≤Kn∏i=1‖Bi(y)⋅χD‖φi≤Kn∏i=1(‖hi⋅χD‖φi+‖g2i‖φi‖y⋅χD‖φ+2k1i‖ki‖φ2i⋅rΓ(αi)‖g1i‖φ1i‖g3i‖Ni‖y⋅χD‖φ). |
Since hi∈Eφi, we obtain
limε→0{supmeasD≤ε[supy∈Y{‖hi⋅χD‖φi}]}=0. |
From the definition of c(y), we have
c(B(Y))≤rnKn∏i=1(‖g2i‖φi+2k1i‖ki‖φ2i⋅rΓ(αi)‖g1i‖φ1i‖g3i‖Ni)c(Y), |
where ‖y⋅χD‖nφ=‖y⋅χD‖n−1φ‖y⋅χD‖φ≤rn‖y⋅χD‖φ.
Since ∅≠Y⊂Qr is a bounded and compact in measure subset of Eφ, we can employ Lemma 2.4 to get
βH(B(Y))≤rnKn∏i=1(‖g2i‖φi+2k1i‖ki‖φ2i⋅rΓ(αi)‖g1i‖φ1i‖g3i‖Ni)⋅βH(Y). |
Since ∏ni=1(‖g2i‖φi+2k1i‖ki‖φ2i⋅rΓ(αi)‖g1i‖φ1i‖g3i‖Ni)<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)={y∈Lφ:‖y‖φ≤1}. 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=n∑j=1[K(‖g2j‖φj+4k1j⋅r‖kj‖φ2jΓ(αj)‖g1j‖φij‖g3j‖Nj)⋅n∏i=1,i≠jLi]<1, |
where r and Li are defined in assumption (N7), then Eq (1.1) has a unique solution y∈Lφ in Qr.
Proof. Let y and z be any two different solutions of Eq (1.1), then we obtain
|y−z|=|n∏i=1Bi(y)−n∏i=1Bi(z)|≤|n∏i=1Bi(y)−B1(z)n∏i=2Bi(y)|+|B1(z)n∏i=2Bi(y)−B1(z)B2(z)n∏i=3Bi(y)|+⋯+|Bn(y)n−1∏i=1Bi(z)−n∏i=1Bi(z)|≤|B1(y)−B1(z)|⋅n∏i=2|Bi(y)|+|B1(z)|⋅|B2(y)−B2(z)|⋅n∏i=3|Bi(y)|+⋯+|Bn(y)−Bn(z)|⋅n−1∏i=1|Bi(z)|. |
Therefore,
‖y−z‖φ≤K‖B1(y)−B1(z)‖φ1n∏i=2‖Bi(y)‖φi+K‖B1(z)‖φ1‖B2(y)−B2(z)‖φ2n∏i=3‖Bi(y)‖φi+...+K‖Bn(y)−Bn(z)‖φnn−1∏i=1‖Bi(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)‖φj≤‖G2j(y)−G2j(z)‖φj+‖G1j(y)Aj(y)−G1j(z)Aj(z)‖φj≤‖g2j⋅‖y‖φ−g2j⋅‖z‖φ‖φj+‖G1j(y)Aj(y)−G1j(z)Aj(y)‖φj+‖G1j(z)Aj(y)−G1j(z)Aj(z)‖φj≤‖g2j⋅|‖y‖φ−‖z‖φ|‖φj+k1j‖G1j(y)−G1j(z)‖φ1j‖Aj(y)‖φ2j+k1j‖G1j(z)‖φ1j‖Aj(y)−Aj(z)‖φ2j≤‖g2j‖φj‖y−z‖φ+k1j‖g1j⋅|‖y‖φ−‖z‖φ|‖φ1j‖JαjjG3j(y)‖φ2j+k1j‖g1j⋅‖z‖φ‖φ1j‖JαjjG3j(y)−JαjjG3j(z)‖φ2j≤‖g2j‖φj‖y−z‖φ+k1j‖g1j‖φ1j‖y−z‖φ2Γ(αi)‖kj‖φ2j‖g3j‖Nj‖y‖φ+k1j‖g1j‖φ1j⋅‖z‖φ2Γ(αj)‖kj‖φ2j‖g3j‖Nj‖y−z‖φ≤(‖g2j‖φj+4k1j⋅r‖kj‖φ2jΓ(αj)‖g1j‖φ1j‖g3j‖Nj)‖y−z‖φ. | (3.3) |
By substituting from (3.1) and (3.3) in (3.2), we obtain
‖y−z‖φ≤[K(‖g21‖φ1+4k11⋅r‖k1‖φ21Γ(α1)‖g11‖φ11‖g31‖N1)n∏i=2Li+KL1(‖g22‖φ2+4k12⋅r‖k2‖φ22Γ(α2)‖g12‖φ12‖g32‖N2)n∏i=3Li+...+K(‖g2n‖φn+4k1n⋅r‖kn‖φ2nΓ(αn)‖g1n‖φ1n‖g3n‖Nn)n−1∏i=1Li]‖y−z‖φ=C⋅‖y−z‖φ. |
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:LNi→Lφ2i,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(ταi−1)dτ=∫s0τ2αi−2dτ=s2αi−12αi−1. |
Moreover,
∫e1φ2i(ki(s))dτ=∫e1(es2αi−12αi−1−s2αi−12αi−1−1)ds<∞. |
Thus for y∈LNi, we get that Jαii:LNi→Lφ2i 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)=n∏i=1(hi(s)+g2i(s)⋅y(s)+g1i(s)⋅y(s)∫s1(logsτ)αi−1g3i(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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